pythia8-8.1.80.orig/0000755000175000017500000000000012217616062012334 5ustar sunsunpythia8-8.1.80.orig/Makefile.msc0000644000175000017500000001210212217346233014551 0ustar sunsun# Makefile.msc for Pythia8 on Win32/NMAKE # Author: Bertrand Bellenot, 02/05/2007, 04/11/2009 !IF "$(CFG)" == "" CFG = Win32 Release !MESSAGE No configuration specified. Defaulting to Win32 Release. !ENDIF !IF "$(CFG)" != "Win32 Release" && "$(CFG)" != "Win32 Debug" !MESSAGE Invalid configuration "$(CFG)" specified. !MESSAGE You can specify a configuration when running NMAKE !MESSAGE by defining the macro CFG on the command line. For example: !MESSAGE !MESSAGE NMAKE /f "Makefile.msc" CFG="Win32 Debug" !MESSAGE !MESSAGE Possible choices for configuration are: !MESSAGE !MESSAGE "Win32 Release" (based on "Win32 (x86) Static Library") !MESSAGE "Win32 Debug" (based on "Win32 (x86) Static Library") !MESSAGE !ERROR An invalid configuration is specified. !ENDIF !IF "$(OS)" == "Windows_NT" NULL= !ELSE NULL=nul !ENDIF OutPutOpt = -out: # Win32 system with Microsoft Visual C/C++ !include CC = $(cc) CXX = $(cc) CXXFLAGS = -EHsc -nologo -GR -DWIN32 -W3 -FIiso646.h \ -DVISUAL_CPLUSPLUS -D_WINDOWS -Iinclude LD = $(link) !IF "$(CFG)" == "Win32 Release" CXXOPT = -O2 -MD -DNDEBUG LDOPT = OUTDIR = ./Release !ELSEIF "$(CFG)" == "Win32 Debug" CXXOPT = -Z7 -MDd LDOPT = OUTDIR = ./Debug !ENDIF # Check if nmake version is 8.xx or 9.xx !if ([nmake /? 2>&1 | findstr /c:"Version 8\." > nul ] == 0) || \ ([nmake /? 2>&1 | findstr /c:"Version 9\." > nul ] == 0) MT_EXE = mt -nologo -manifest $@.manifest -outputresource:$@;1 MT_DLL = mt -nologo -manifest $@.manifest -outputresource:$@;2 EXTRAFLAGS = -D_CRT_SECURE_NO_DEPRECATE !else MT_EXE = MT_DLL = EXTRAFLAGS = -G5 !endif ####### Files SRCDIR = src DUMDIR = lhapdfdummy INCDIR = include LIBDIR = lib LIBRARY = libPythia8 LIBDLL = $(LIBDIR)/$(LIBRARY).dll LIBLIB = $(LIBDIR)/$(LIBRARY).lib LDFLAGS = -lib /nologo /out:$(LIBLIB) OBJS = $(OUTDIR)/Analysis.obj \ $(OUTDIR)/Basics.obj \ $(OUTDIR)/BeamParticle.obj \ $(OUTDIR)/BeamRemnants.obj \ $(OUTDIR)/BeamShape.obj \ $(OUTDIR)/BoseEinstein.obj \ $(OUTDIR)/Event.obj \ $(OUTDIR)/FragmentationFlavZpT.obj \ $(OUTDIR)/FragmentationSystems.obj \ $(OUTDIR)/HadronLevel.obj \ $(OUTDIR)/HadronScatter.obj \ $(OUTDIR)/HelicityBasics.obj \ $(OUTDIR)/HelicityMatrixElements.obj \ $(OUTDIR)/HiddenValleyFragmentation.obj \ $(OUTDIR)/History.obj \ $(OUTDIR)/Info.obj \ $(OUTDIR)/LesHouches.obj \ $(OUTDIR)/MergingHooks.obj \ $(OUTDIR)/MiniStringFragmentation.obj \ $(OUTDIR)/MultipartonInteractions.obj \ $(OUTDIR)/ParticleData.obj \ $(OUTDIR)/ParticleDecays.obj \ $(OUTDIR)/PartonDistributions.obj \ $(OUTDIR)/PartonLevel.obj \ $(OUTDIR)/PartonSystems.obj \ $(OUTDIR)/PhaseSpace.obj \ $(OUTDIR)/ProcessContainer.obj \ $(OUTDIR)/ProcessLevel.obj \ $(OUTDIR)/Pythia.obj \ $(OUTDIR)/PythiaStdlib.obj \ $(OUTDIR)/ResonanceDecays.obj \ $(OUTDIR)/ResonanceWidths.obj \ $(OUTDIR)/RHadrons.obj \ $(OUTDIR)/Settings.obj \ $(OUTDIR)/SigmaCompositeness.obj \ $(OUTDIR)/SigmaEW.obj \ $(OUTDIR)/SigmaExtraDim.obj \ $(OUTDIR)/SigmaGeneric.obj \ $(OUTDIR)/SigmaHiggs.obj \ $(OUTDIR)/SigmaLeftRightSym.obj \ $(OUTDIR)/SigmaLeptoquark.obj \ $(OUTDIR)/SigmaNewGaugeBosons.obj \ $(OUTDIR)/SigmaOnia.obj \ $(OUTDIR)/SigmaProcess.obj \ $(OUTDIR)/SigmaQCD.obj \ $(OUTDIR)/SigmaSUSY.obj \ $(OUTDIR)/SigmaTotal.obj \ $(OUTDIR)/SLHAinterface.obj \ $(OUTDIR)/SpaceShower.obj \ $(OUTDIR)/StandardModel.obj \ $(OUTDIR)/StringFragmentation.obj \ $(OUTDIR)/SusyCouplings.obj \ $(OUTDIR)/SusyLesHouches.obj \ $(OUTDIR)/SusyResonanceWidths.obj \ $(OUTDIR)/TauDecays.obj \ $(OUTDIR)/TimeShower.obj \ $(OUTDIR)/UserHooks.obj \ # If you link to HepMC you also need HepMCInterface # $(OUTDIR)/HepMCInterface.obj \ # If you link to LHAPDF you don't want the last line $(OUTDIR)/LHAPDFDummy.obj LIBS : $(OUTDIR) $(LIBDIR) $(BINDIR) $(LIBLIB) .PHONY: $(LIBS) all all: $(LIBS) "$(OUTDIR)" : @if not exist "$(OUTDIR)/$(NULL)" mkdir "$(OUTDIR)" "$(LIBDIR)" : @if not exist "$(LIBDIR)/$(NULL)" mkdir "$(LIBDIR)" $(LIBLIB) : $(OBJS) $(LD) $(LDFLAGS) $(LDOPT) @<< $(OBJS) << .SUFFIXES: .h .cc .obj {$(INCDIR)}.h{$(OUTDIR)}.obj: $(CXX) $(CXXFLAGS) $(EXTRAFLAGS) $(CXXOPT) /Fo"$(OUTDIR)/" -c $(SRCDIR)\$(@B).cc {$(SRCDIR)}.cc{$(OUTDIR)}.obj: $(CXX) $(CXXFLAGS) $(EXTRAFLAGS) $(CXXOPT) /Fo"$(OUTDIR)/" -c $< {$(DUMDIR)}.cc{$(OUTDIR)}.obj: $(CXX) $(CXXFLAGS) $(EXTRAFLAGS) $(CXXOPT) /Fo"$(OUTDIR)/" -c $< clean: -@erase /q /s *.obj >nul 2>&1 -@rmdir /q /s Debug >nul 2>&1 -@rmdir /q /s Release >nul 2>&1 distclean: clean -@erase /q "$(LIBDIR)\*.*" >nul 2>&1 -@rmdir /q /s lib >nul 2>&1 pythia8-8.1.80.orig/rootexamples/0000755000175000017500000000000012217346244015060 5ustar sunsunpythia8-8.1.80.orig/rootexamples/tree.cc0000644000175000017500000000273312217346244016333 0ustar sunsun// File: tree.cc // This is a simple test program. // Modified by Rene Brun and Axcel Naumann to put the Pythia::event // into a TTree. // Copyright (C) 2013 Torbjorn Sjostrand // Header file to access Pythia 8 program elements. #include "Pythia8/Pythia.h" // ROOT, for saving Pythia events as trees in a file. #include "TTree.h" #include "TFile.h" using namespace Pythia8; int main() { // Create Pythia instance and set it up to generate hard QCD processes // above pTHat = 20 GeV for pp collisions at 14 TeV. Pythia pythia; pythia.readString("HardQCD:all = on"); pythia.readString("PhaseSpace:pTHatMin = 20."); pythia.readString("Beams:eCM = 14000."); pythia.init(); // Set up the ROOT TFile and TTree. TFile *file = TFile::Open("pytree.root","recreate"); Event *event = &pythia.event; TTree *T = new TTree("T","ev1 Tree"); T->Branch("event",&event); // Begin event loop. Generate event; skip if generation aborted. for (int iEvent = 0; iEvent < 100; ++iEvent) { if (!pythia.next()) continue; // Fill the pythia event into the TTree. // Warning: the files will rapidly become large if all events // are saved. In some cases it may be convenient to do some // processing of events and only save those that appear // interesting for future analyses. T->Fill(); // End event loop. } // Statistics on event generation. pythia.stat(); // Write tree. T->Print(); T->Write(); delete file; // Done. return 0; } pythia8-8.1.80.orig/rootexamples/Makefile0000644000175000017500000000421512217346244016522 0ustar sunsun###################################################################### # Makefile for building Pythia's ROOT examples. # Axel Naumann, 2011-03-03 ###################################################################### # Need this to get SHAREDSUFFIX (e.g. dylib or so) -include ../config.mk # A few variables used in this Makefile: EX := hist tree EXE := $(addsuffix .exe,$(EX)) PYTHIA8 ?= $(PWD)/.. STATICLIB := $(PYTHIA8)/lib/archive/libpythia8.a SHAREDLIB := $(PYTHIA8)/lib/libpythia8.$(SHAREDSUFFIX) DICTCXXFLAGS := -I$(PYTHIA8)/include ROOTCXXFLAGS := $(DICTCXXFLAGS) $(shell root-config --cflags) # Libraries to include if GZIP support is enabled ifeq (x$(ENABLEGZIP),xyes) LIBGZIP=-L$(BOOSTLIBLOCATION) -lboost_iostreams -L$(ZLIBLOCATION) -lz endif # LDFLAGS1 for static library, LDFLAGS2 for shared library LDFLAGS1 := $(shell root-config --ldflags --glibs) \ -L$(PYTHIA8)/lib/archive -lpythia8 -llhapdfdummy $(LIBGZIP) LDFLAGS2 := $(shell root-config --ldflags --glibs) \ -L$(PYTHIA8)/lib -lpythia8 -llhapdfdummy $(LIBGZIP) # Default target; make examples (but not shared dictionary) all: $(EX) # Rule to build hist example. Needs static PYTHIA 8 library hist: $(STATICLIB) hist.cc $(CXX) $(ROOTCXXFLAGS) $@.cc -o $@.exe $(LDFLAGS1) # Rule to build tree example. Needs dictionary to be built and # static PYTHIA 8 library tree: $(STATICLIB) tree.cc rootcint -f treeDict.cc -c $(DICTCXXFLAGS) pythiaROOT.h pythiaLinkdef.h $(CXX) $(ROOTCXXFLAGS) treeDict.cc $@.cc -o $@.exe $(LDFLAGS1) # Rule to build full dictionary dict: $(SHAREDLIB) rootcint -f pythiaDict.cc -c $(DICTCXXFLAGS) \ -DPYTHIA8_COMPLETE_ROOT_DICTIONARY \ pythiaROOT.h pythiaLinkdef.h $(CXX) -shared -fPIC -o pythiaDict.$(SHAREDSUFFIX) pythiaDict.cc \ -DPYTHIA8_COMPLETE_ROOT_DICTIONARY \ $(ROOTCXXFLAGS) $(LDFLAGS2) # Error messages if PYTHIA libraries don't exist $(STATICLIB): @echo "Error: PYTHIA 8 archive library must be built" @false $(SHAREDLIB): @echo "Error: PYTHIA 8 shared library must be built" @false # Clean up clean: rm -f $(EXE) hist.root pythiaDict.* \ treeDict.cc treeDict.h pytree.root pythia8-8.1.80.orig/rootexamples/pythiaROOT.h0000644000175000017500000000020612217346244017231 0ustar sunsun#ifdef PYTHIA8_COMPLETE_ROOT_DICTIONARY #include "Pythia8/Pythia.h" #else #include "Pythia8/Event.h" #endif using namespace Pythia8; pythia8-8.1.80.orig/rootexamples/hist.cc0000644000175000017500000000373012217346244016341 0ustar sunsun// File: hist.cc // This is a simple test program. // It studies the charged multiplicity distribution at the LHC. // Modified by Rene Brun, Axel Naumann and Bernhard Meirose // to use ROOT for histogramming. // Copyright (C) 2013 Torbjorn Sjostrand // Stdlib header file for input and output. #include // Header file to access Pythia 8 program elements. #include "Pythia8/Pythia.h" // ROOT, for histogramming. #include "TH1.h" // ROOT, for interactive graphics. #include "TVirtualPad.h" #include "TApplication.h" // ROOT, for saving file. #include "TFile.h" using namespace Pythia8; int main(int argc, char* argv[]) { // Create the ROOT application environment. TApplication theApp("hist", &argc, argv); // Create Pythia instance and set it up to generate hard QCD processes // above pTHat = 20 GeV for pp collisions at 14 TeV. Pythia pythia; pythia.readString("HardQCD:all = on"); pythia.readString("PhaseSpace:pTHatMin = 20."); pythia.readString("Beams:eCM = 14000."); pythia.init(); // Create file on which histogram(s) can be saved. TFile* outFile = new TFile("hist.root", "RECREATE"); // Book histogram. TH1F *mult = new TH1F("mult","charged multiplicity", 100, -0.5, 799.5); // Begin event loop. Generate event; skip if generation aborted. for (int iEvent = 0; iEvent < 100; ++iEvent) { if (!pythia.next()) continue; // Find number of all final charged particles. int nCharged = 0; for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].isFinal() && pythia.event[i].isCharged()) ++nCharged; // Fill charged multiplicity in histogram. End event loop. mult->Fill( nCharged ); } // Statistics on event generation. pythia.stat(); // Show histogram. Possibility to close it. mult->Draw(); std::cout << "\nDouble click on the histogram window to quit.\n"; gPad->WaitPrimitive(); // Save histogram on file and close file. mult->Write(); delete outFile; // Done. return 0; } pythia8-8.1.80.orig/rootexamples/pythiaLinkdef.h0000644000175000017500000000424512217346244020031 0ustar sunsun#ifdef __CINT__ #pragma link off all globals; #pragma link off all classes; #pragma link off all functions; #pragma link C++ namespace Pythia8; #pragma link C++ class Pythia8::Event+; #pragma link C++ class Pythia8::Particle+; #pragma link C++ class Pythia8::Junction+; #pragma link C++ class Pythia8::Vec4+; #ifdef PYTHIA8_COMPLETE_ROOT_DICTIONARY // For tree.cc, none of the following (generator-internal) // classes is needed. Thus excluded from the default Linkdef.h. #pragma link C++ class Pythia8::ParticleData+; #pragma link C++ class Pythia8::ParticleDataEntry+; #pragma link C++ class Pythia8::DecayChannel+; #pragma link C++ class Pythia8::Pythia+; #pragma link C++ class Pythia8::CoupSM+; #pragma link C++ class Pythia8::Couplings+; #pragma link C++ class Pythia8::InBeam+; #pragma link C++ class Pythia8::InPair+; #pragma link C++ class Pythia8::AlphaStrong+; #pragma link C++ class Pythia8::AlphaEM+; #pragma link C++ class Pythia8::Info+; #pragma link C++ class Pythia8::Rndm+; #pragma link C++ class Pythia8::RndmEngine+; #pragma link C++ class Pythia8::Settings+; #pragma link C++ class Pythia8::ResonanceTop+; #pragma link C++ class Pythia8::ResonanceGeneric+; #pragma link C++ class Pythia8::ResonanceGmZ+; #pragma link C++ class Pythia8::ResonanceW+; #pragma link C++ class Pythia8::ResonanceFour+; #pragma link C++ class Pythia8::ResonanceH+; #pragma link C++ class Pythia8::ResonanceHchg+; #pragma link C++ class Pythia8::ResonanceZprime+; #pragma link C++ class Pythia8::ResonanceWprime+; #pragma link C++ class Pythia8::ResonanceRhorizontal+; #pragma link C++ class Pythia8::ResonanceExcited+; #pragma link C++ class Pythia8::ResonanceGraviton+; #pragma link C++ class Pythia8::ResonanceLeptoquark+; #pragma link C++ class Pythia8::ResonanceNuRight+; #pragma link C++ class Pythia8::ResonanceZRight+; #pragma link C++ class Pythia8::ResonanceWRight+; #pragma link C++ class Pythia8::ResonanceHchgchgLeft+; #pragma link C++ class Pythia8::ResonanceHchgchgRight+; #pragma link C++ class Pythia8::ResonanceWidths+; #pragma link C++ class Pythia8::SigmaProcess+; #pragma link C++ class std::vector+; #pragma link C++ class std::pair+; #endif #endif pythia8-8.1.80.orig/rootexamples/README0000644000175000017500000000406612217346244015746 0ustar sunsunThis directory contains files contributed by Rene Brun and Axel Naumann, with further input from Bernhard Meirose, which illustrate how ROOT commands can be used inside PYTHIA code. You should read the "ROOT usage" page in the manual to understand the function of the files, and how to set up the environment in which they can be used. The practical steps to be taken, assuming you use the bash shell, are: 1) Add to your ".bashrc" file (in your home directory) the following lines: ######################################################## # Root path and libraries: source /Path_to_ROOT/root/bin/thisroot.sh # Pythia 8 path and libraries: export PYTHIA8=/Path_to_Pythia8/pythia81xx/ export LD_LIBRARY_PATH=$PYTHIA8/lib:$LD_LIBRARY_PATH ######################################################## where xx is the Pythia 8.1 subversion. As usual type "source .bashrc" after the changes. 2) Before compilation, configure Pythia 8 if you want to use shared libraries: ./configure --enable-shared 3) "make hist" builds an application for histogramming Pythia output (alternatively "make" builds and runs all examples). 4) "./hist" runs the example showing the Pythia output histogram in Root format. 5) You can correspondingly try the "tree" program, which illustrates how Pythia event records can be saved by Root. Needless to say, files can become quite large when many events are generated. 6) When upgrading to a new Pythia subversion, and you want to use a shared library, you should re-generate pythiaDict.cxx to reflect the new classes: cd NewPythiaVersion/rootexamples make dict and use the generated pythiaDict.h and pythiaDict.cxx for building your program. 7) For FastJet use, add the following lines to the Makefile: CXXFLAGS += -I/Path_to_FastJet/include -L$(PYTHIA8)/lib -lpythia8 -llhapdfdummy -L/Path_to_FastJet/lib -lfastjet where "Path_to_FastJet" is the directory where FastJet was installed. Finally, add to your ".bashrc" file the following line: export LD_LIBRARY_PATH=//Path_to_FastJet/lib:LD_LIBRARY_PATH and type "source .bashrc" after the changes. pythia8-8.1.80.orig/lhapdfdummy/0000755000175000017500000000000012217346232014645 5ustar sunsunpythia8-8.1.80.orig/lhapdfdummy/LHAPDFDummy.cc0000644000175000017500000000126612217346232017133 0ustar sunsun// LHAPDFDummy.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Dummy routines to link when LHAPDF not linked. extern "C" { void initpdfsetm_(int& nSet, const char*, int) {nSet = -1;} void initpdfsetbynamem_(int& nSet, const char*, int) {nSet = -1;} void initpdfm_(int& nSet, int&) {nSet = -1;} void evolvepdfm_(int& nSet, double&, double&, double*) {nSet = -1;} void evolvepdfphotonm_(int& nSet, double&, double&, double*, double&) {nSet = -1;} void setlhaparm_(const char*, int) {} } pythia8-8.1.80.orig/htmldoc/0000755000175000017500000000000012217357500013765 5ustar sunsunpythia8-8.1.80.orig/htmldoc/MatchingAndMerging.html0000644000175000017500000002036512217615312020345 0ustar sunsun Matching and Merging

Matching and Merging

Starting from a Born-level leading-order (LO) process, higher orders can be included in various ways. The three basic approaches would be
  • A formal order-by-order perturbative calculation, in each order higher including graphs both with one particle more in the final state and with one loop more in the intermediate state. This is accurate to the order of the calculation, but gives no hint of event structures beyond that, with more particles in the final state. Today next-to-leading order (NLO) is standard, while next-to-next-to-leading order (NNLO) is coming. This approach thus is limited to few orders, and also breaks down in soft and collinear regions, which makes it unsuitable for matching to hadronization.
  • Real emissions to several higher orders, but neglecting the virtual/loop corrections that should go with it at any given order. Thereby it is possible to allow for topologies with a large and varying number of partons, at the prize of not being accurate to any particular order. The approach also opens up for doublecounting, and as above breaks down in soft and colliner regions.
  • The parton shower provides an approximation to higher orders, both real and virtual contributions for the emission of arbitrarily many particles. As such it is less accurate than either of the two above, at least for topologies of well separated partons, but it contains a physically sensible behaviour in the soft and collinear limits, and therefore matches well onto the hadronization stage.
Given the pros and cons, much of the effort in recent years has involved the development of different prescriptions to combine the methods above in various ways.

The common traits of all combination methods are that matrix elements are used to describe the production of hard and well separated particles, and parton showers for the production of soft or collinear particles. What differs between the various approaches that have been proposed are which matrix elements are being used, how doublecounting is avoided, and how the transition from the hard to the soft regime is handled. These combination methods are typically referred to as "matching" or "merging" algorithms. There is some confusion about the distinction between the two terms, and so we leave it to the inventor/implementor of a particular scheme to choose and motivate the name given to that scheme.

PYTHIA comes with methods, to be described next, that implement or support several different kind of algorithms. The field is open-ended, however: any external program can feed in Les Houches events that PYTHIA subsequently showers, adds multiparton interactions to, and hadronizes. These events afterwards can be reweighted and combined in any desired way. The maximum pT of the shower evolution is set by the Les Houches scale, on the one hand, and by the values of the SpaceShower:pTmaxMatch, TimeShower:pTmaxMatch and other parton-shower settings, on the other. Typically it is not possible to achieve perfect matching this way, given that the PYTHIA pT evolution variables are not likely to agree with the variables used for cuts in the external program. Often one can get close enough with simple means but, for an improved matching, User Hooks can be inserted to control the steps taken on the way, e.g. to veto those parton shower branchings that would doublecount emissions included in the matrix elements.

Zooming in from the "anything goes" perspective, the list of relevent approaches actively supported is as follows.

  • For many/most resonance decays the first branching in the shower is merged with first-order matrix elements [Ben87, Nor01]. This means that the emission rate is accurate to NLO, similarly to the POWHEG strategy (see below), but built into the timelike showers. The angular orientation of the event after the first emission is only handled by the parton shower kinematics, however. Needless to say, this formalism is precisely what is tested by Z^0 decays at LEP1, and it is known to do a pretty good job there.
  • Also the spacelike showers contain a correction to first-order matrix elements, but only for the one-body-final-state processes q qbar -> gamma^*/Z^0/W^+-/h^0/H^0/A0/Z'0/W'+-/R0 [Miu99] and g g -> h^0/H^0/A0, and only to leading order. That is, it is equivalent to the POWHEG formalism for the real emission, but the prefactor "cross section normalization" is LO rather than NLO. Therefore this framework is less relevant, and has been superseded the following ones.
  • The POWHEG strategy [Nas04] provides a cross section accurate to NLO. The hardest emission is constructed with unit probability, based on the ratio of the real-emission matrix element to the Born-level cross section, and with a Sudakov factor derived from this ratio, i.e. the philosophy introduced in [Ben87].
    While POWHEG is a generic strategy, the POWHEG BOX [Ali] is an explicit framework, within which several processes are available. Potential emissions are ordered in a transverse-momentum-related variable. The LHA scale variable encodes this value for each event, and thereby sets the upper limit for subsequent shower emissions. There is a mismatch between the POWHEG BOX and the PYTHIA pT variables, however, which gives imperfections in the transition region [Cor10]. The proposed solution is to allow showers to cover the full phase space, but then veto emissions in the region already covered by the POWHEG BOX evolution. The code required for this can be found in examples/main31. While fairly general, the code would have to be modified to accommodate a different pT scale definition in the POWHEG BOX.
  • The other traditional approach for NLO calculations is the MC@NLO one [Fri02]. In it the shower emission probability, without its Sudakov factor, is subtracted from the real-emission matrix element to regularize divergences. It therefore requires a analytic knowledge of the way the shower populates phase space. Currently there is no MC@NLO implementation for PYTHIA 8, but one is in preparation by Paolo Torrielli and Stefano Frixione, for the aMC@NLO program [Fre11]. The global-recoil option of the PYTHIA final-state shower has been constructed in anticipation of its use for the above-mentioned subtraction.
  • Multi-jet merging in the CKKW-L approach [Lon01] is directly available. Its implementation, relevant parameters and test programs are documented on a separate page.
  • Multi-jet matching in the MLM approach [Man02, Man07] is also available, either based on the ALPGEN or on the Madgraph variant, and with input events either from ALPGEN or from Madgraph. For details see separate page.
  • Unitarised matrix element + parton shower merging (UMEPS) is directly available. Its implementation, relevant parameters and test programs are documented on a separate page.
  • Next-to-leading order multi-jet merging (in the NL3 and UNLOPS approaches) is directly available. Its implementation, relevant parameters and test programs are documented on a separate page.
pythia8-8.1.80.orig/htmldoc/NewGaugeBosonProcesses.html0000644000175000017500000003734312217615311021254 0ustar sunsun New-Gauge-Boson Processes

New-Gauge-Boson Processes

This page contains the production of new Z'^0 and W'^+- gauge bosons, e.g. within the context of a new U(1) or SU(2) gauge group, and also a (rather speculative) horizontal gauge boson R^0. Left-right-symmetry scenarios also contain new gauge bosons, but are described separately.

Z'^0

This group only contains one subprocess, with the full gamma^*/Z^0/Z'^0 interference structure for couplings to fermion pairs. It is possible to pick only a subset, e.g, only the pure Z'^0 piece. No higher-order processes are available explicitly, but the ISR showers contain automatic matching to the Z'^0 + 1 jet matrix elements, as for the corresponding gamma^*/Z^0 process.

flag  NewGaugeBoson:ffbar2gmZZprime   (default = off)
Scattering f fbar ->Z'^0. Code 3001.

mode  Zprime:gmZmode   (default = 0; minimum = 0; maximum = 6)
Choice of full gamma^*/Z^0/Z'^0 structure or not in the above process. Note that, with the Z'^0 part switched off, this process is reduced to what already exists among electroweak processes, so those options are here only for crosschecks.
option 0 : full gamma^*/Z^0/Z'^0 structure, with interference included.
option 1 : only pure gamma^* contribution.
option 2 : only pure Z^0 contribution.
option 3 : only pure Z'^0 contribution.
option 4 : only the gamma^*/Z^0 contribution, including interference.
option 5 : only the gamma^*/Z'^0 contribution, including interference.
option 6 : only the Z^0/Z'^0 contribution, including interference.
Note: irrespective of the option used, the particle produced will always be assigned code 32 for Z'^0, and open decay channels is purely dictated by what is set for the Z'^0.

The couplings of the Z'^0 to quarks and leptons can either be assumed universal, i.e. generation-independent, or not. In the former case eight numbers parametrize the vector and axial couplings of down-type quarks, up-type quarks, leptons and neutrinos, respectively. Depending on your assumed neutrino nature you may want to restrict your freedom in that sector, but no limitations are enforced by the program. The default corresponds to the same couplings as that of the Standard Model Z^0, with axial couplings a_f = +-1 and vector couplings v_f = a_f - 4 e_f sin^2(theta_W), with sin^2(theta_W) = 0.23. Without universality the same eight numbers have to be set separately also for the second and the third generation. The choice of fixed axial and vector couplings implies a resonance width that increases linearly with the Z'^0 mass.

By a suitable choice of the parameters, it is possible to simulate just about any imaginable Z'^0 scenario, with full interference effects in cross sections and decay angular distributions and generation-dependent couplings; the default values should mainly be viewed as placeholders. The conversion from the coupling conventions in a set of different Z'^0 models in the literature to those used in PYTHIA is described by C. Ciobanu et al.

flag  Zprime:universality   (default = on)
If on then you need only set the first-generation couplings below, and these are automatically also used for the second and third generation. If off, then couplings can be chosen separately for each generation.

Here are the couplings always valid for the first generation, and normally also for the second and third by trivial analogy:

parm  Zprime:vd   (default = -0.693)
vector coupling of d quarks.

parm  Zprime:ad   (default = -1.)
axial coupling of d quarks.

parm  Zprime:vu   (default = 0.387)
vector coupling of u quarks.

parm  Zprime:au   (default = 1.)
axial coupling of u quarks.

parm  Zprime:ve   (default = -0.08)
vector coupling of e leptons.

parm  Zprime:ae   (default = -1.)
axial coupling of e leptons.

parm  Zprime:vnue   (default = 1.)
vector coupling of nu_e neutrinos.

parm  Zprime:anue   (default = 1.)
axial coupling of nu_e neutrinos.

Here are the further couplings that are specific for a scenario with Zprime:universality switched off:

parm  Zprime:vs   (default = -0.693)
vector coupling of s quarks.

parm  Zprime:as   (default = -1.)
axial coupling of s quarks.

parm  Zprime:vc   (default = 0.387)
vector coupling of c quarks.

parm  Zprime:ac   (default = 1.)
axial coupling of c quarks.

parm  Zprime:vmu   (default = -0.08)
vector coupling of mu leptons.

parm  Zprime:amu   (default = -1.)
axial coupling of mu leptons.

parm  Zprime:vnumu   (default = 1.)
vector coupling of nu_mu neutrinos.

parm  Zprime:anumu   (default = 1.)
axial coupling of nu_mu neutrinos.

parm  Zprime:vb   (default = -0.693)
vector coupling of b quarks.

parm  Zprime:ab   (default = -1.)
axial coupling of b quarks.

parm  Zprime:vt   (default = 0.387)
vector coupling of t quarks.

parm  Zprime:at   (default = 1.)
axial coupling of t quarks.

parm  Zprime:vtau   (default = -0.08)
vector coupling of tau leptons.

parm  Zprime:atau   (default = -1.)
axial coupling of tau leptons.

parm  Zprime:vnutau   (default = 1.)
vector coupling of nu_tau neutrinos.

parm  Zprime:anutau   (default = 1.)
axial coupling of nu_tau neutrinos.

The coupling to the decay channel Z'^0 -> W^+ W^- is more model-dependent. By default it is therefore off, but can be switched on as follows. Furthermore, we have left some amount of freedom in the choice of decay angular correlations in this channel, but obviously alternative shapes could be imagined.

parm  Zprime:coup2WW   (default = 0.; minimum = 0.)
the coupling Z'^0 -> W^+ W^- is taken to be this number times m_W^2 / m_Z'^2 times the Z^0 -> W^+ W^- coupling. Thus a unit value corresponds to the Z^0 -> W^+ W^- coupling, scaled down by a factor m_W^2 / m_Z'^2, and gives a Z'^0 partial width into this channel that again increases linearly. If you cancel this behaviour, by letting Zprime:coup2WW be proportional to m_Z'^2 / m_W^2, you instead obtain a partial width that goes like the fifth power of the Z'^0 mass. These two extremes correspond to the "extended gauge model" and the "reference model", respectively, of [Alt89]. Note that this channel only includes the pure Z' part, while f fbar -> gamma^*/Z^*0 -> W^+ W^- is available as a separate electroweak process.

parm  Zprime:anglesWW   (default = 0.; minimum = 0.; maximum = 1.)
in the decay chain Z'^0 -> W^+ W^- ->f_1 fbar_2 f_3 fbar_4 the decay angular distributions is taken to be a mixture of two possible shapes. This parameter gives the fraction that is distributed as in Higgs h^0 -> W^+ W^- (longitudinal bosons), with the remainder (by default all) is taken to be the same as for Z^0 -> W^+ W^- (a mixture of transverse and longitudinal bosons).

A massive Z'^0 is also likely to decay into Higgs bosons and potentially into other now unknown particles. Such possibilities clearly are quite model-dependent, and have not been included for now.

W'^+-

The W'^+- implementation is less ambitious than the Z'^0. Specifically, while indirect detection of a Z'^0 through its interference contribution is a possible discovery channel in lepton colliders, there is no equally compelling case for W^+-/W'^+- interference effects being of importance for discovery, and such interference has therefore not been implemented for now. Related to this, a Z'^0 could appear on its own in a new U(1) group, while W'^+- would have to sit in a SU(2) group and thus have a Z'^0 partner that is likely to be found first. Only one process is implemented but, like for the W^+-, the ISR showers contain automatic matching to the W'^+- + 1 jet matrix elements.

flag  NewGaugeBoson:ffbar2Wprime   (default = off)
Scattering f fbar' -> W'^+-. Code 3021.

The couplings of the W'^+- are here assumed universal, i.e. the same for all generations. One may set vector and axial couplings freely, separately for the q qbar' and the l nu_l decay channels. The defaults correspond to the V - A structure and normalization of the Standard Model W^+-, but can be changed to simulate a wide selection of models. One limitation is that, for simplicity, the same Cabibbo--Kobayashi--Maskawa quark mixing matrix is assumed as for the standard W^+-. Depending on your assumed neutrino nature you may want to restrict your freedom in the lepton sector, but no limitations are enforced by the program.

parm  Wprime:vq   (default = 1.)
vector coupling of quarks.

parm  Wprime:aq   (default = -1.)
axial coupling of quarks.

parm  Wprime:vl   (default = 1.)
vector coupling of leptons.

parm  Wprime:al   (default = -1.)
axial coupling of leptons.

The coupling to the decay channel W'^+- -> W^+- Z^0 is more model-dependent, like for Z'^0 -> W^+ W^- described above. By default it is therefore off, but can be switched on as follows. Furthermore, we have left some amount of freedom in the choice of decay angular correlations in this channel, but obviously alternative shapes could be imagined.

parm  Wprime:coup2WZ   (default = 0.; minimum = 0.)
the coupling W'^0 -> W^+- Z^0 is taken to be this number times m_W^2 / m_W'^2 times the W^+- -> W^+- Z^0 coupling. Thus a unit value corresponds to the W^+- -> W^+- Z^0 coupling, scaled down by a factor m_W^2 / m_W'^2, and gives a W'^+- partial width into this channel that increases linearly with the W'^+- mass. If you cancel this behaviour, by letting Wprime:coup2WZ be proportional to m_W'^2 / m_W^2, you instead obtain a partial width that goes like the fifth power of the W'^+- mass. These two extremes correspond to the "extended gauge model" and the "reference model", respectively, of [Alt89].

parm  Wprime:anglesWZ   (default = 0.; minimum = 0.; maximum = 1.)
in the decay chain W'^+- -> W^+- Z^0 ->f_1 fbar_2 f_3 fbar_4 the decay angular distributions is taken to be a mixture of two possible shapes. This parameter gives the fraction that is distributed as in Higgs H^+- -> W^+- Z^0 (longitudinal bosons), with the remainder (by default all) is taken to be the same as for W^+- -> W^+- Z^0 (a mixture of transverse and longitudinal bosons).

A massive W'^+- is also likely to decay into Higgs bosons and potentially into other now unknown particles. Such possibilities clearly are quite model-dependent, and have not been included for now.

R^0

The R^0 boson (particle code 41) represents one possible scenario for a horizontal gauge boson, i.e. a gauge boson that couples between the generations, inducing processes like s dbar -> R^0 -> mu^- e^+. Experimental limits on flavour-changing neutral currents forces such a boson to be fairly heavy. In spite of being neutral the antiparticle is distinct from the particle: one carries a net positive generation number and the other a negative one. This particular model has no new parameters beyond the R^0 mass. Decays are assumed isotropic. For further details see [Ben85].

flag  NewGaugeBoson:ffbar2R0   (default = off)
Scattering f_1 fbar_2 -> R^0 -> f_3 fbar_4, where f_1 and fbar_2 are separated by +- one generation and similarly for f_3 and fbar_4. Thus possible final states are e.g. d sbar, u cbar s bbar, c tbar, e- mu+ and mu- tau+. Code 3041. pythia8-8.1.80.orig/htmldoc/Histograms.html0000644000175000017500000003134412217615312016776 0ustar sunsun Histograms

Histograms

The Hist class gives a simple implementation of one-dimensional histograms, useful for quick-and-dirty testing, without the need to link to more sophisticated packages. For this reason it is used in many of the sample main programs found in the examples subdirectory.

Basic principles

We here provide a simple overview of what is involved. As a first step you need to declare a histogram, with name, title, number of bins and x range (from, to).
   Hist ZpT( "Z0 pT spectrum", 100, 0., 100.);
Alternatively you can first declare it and later define it:
   Hist ZpT;
   ZpT.book( "Z0 pT spectrum", 100, 0., 100.);
Once declared, its contents can be added by repeated calls to fill,
   ZpT.fill( 22.7, 1.); 
where the first argument is the x value and the second the weight. Since the weight defaults to 1 the last argument could have been omitted in this case.

A set of overloaded operators have been defined, so that histograms can be added, subtracted, divided or multiplied by each other. Then the contents are modified accordingly bin by bin. Thus the relative deviation between two histograms data and theory can be found as

  diff = (data - theory) / (data + theory);
assuming that diff, data and theory have been booked with the same number of bins and x range. That responsibility rests on the user; some checks are made for compatibility, but not enough to catch all possible mistakes.

Also overloaded operations with double real numbers are available. Again these four operations are defined bin by bin, i.e. the corresponding amount is added to, subtracted from, multiplied by or divided by each bin. The double number can come before or after the histograms, with obvious results. Thus the inverse of a histogram result is given by 1. / result. The two kind of operations can be combined, e.g.

  allpT = ZpT + 2. * WpT
Finally, also the +=, -+, *=, /= are overloaded, with the right-hand side being either a histogram or a real number.

Output format

A histogram can be printed by making use of the overloaded << operator, e.g.:

   cout << ZpT;
The printout format is inspired by the old HBOOK one. To understand how to read this format, consider the simplified example
                                    
        3.50*10^ 2  9                     
        3.00*10^ 2  X   7               
        2.50*10^ 2  X  1X               
        2.00*10^ 2  X6 XX                
        1.50*10^ 2  XX5XX                 
        1.00*10^ 2  XXXXX                
        0.50*10^ 2  XXXXX        

          Contents 
            *10^ 2  31122
            *10^ 1  47208
            *10^ 0  79373

          Low edge  -- 
            *10^ 1  10001 
            *10^ 0  05050
The key feature is that the Contents and Low edge have to be read vertically. For instance, the first bin has the contents 3 * 10^2 + 4 * 10^1 + 7 * 10^0 = 347. Correspondingly, the other bins have contents 179, 123, 207 and 283. The first bin stretches from -(1 * 10^1 + 0 * 10^0) = -10 to the beginning of the second bin, at -(0 * 10^1 + 5 * 10^0) = -5.

The visual representation above the contents give a simple impression of the shape. An X means that the contents are filled up to this level, a digit in the topmost row the fraction to which the last level is filled. So the 9 of the first column indicates this bin is filled 9/10 of the way from 3.00*10^2 = 300 to 3.50*10^2 = 350, i.e. somewhere close to 345, or more precisely in the range 342.5 to 347.5.

The printout also provides some other information, such as the number of entries, i.e. how many times the histogram has been filled, the total weight inside the histogram, the total weight in underflow and overflow, and the mean value and root-mean-square width (disregarding underflow and overflow). The mean and width assumes that all the contents is in the middle of the respective bin. This is especially relevant when you plot a integer quantity, such as a multiplicity. Then it makes sense to book with limits that are half-integers, e.g.

   Hist multMPI( "number of multiparton interactions", 20, -0.5, 19.5);
so that the bins are centered at 0, 1, 2, ..., respectively. This also avoids ambiguities which bin gets to be filled if entries are exactly at the border between two bins. Also note that the fill( xValue) method automatically performs a cast to double precision where necessary, i.e. xValue can be an integer.

The methods

We here collect a more complete and formal overview of the methods.

Hist::Hist()  
declare a histogram, but does not define it.

Hist::Hist(string title, int numberOfBins, double xMin, double xMax)  
declare and define a histogram, where
argument title : is a string with the title of the histogram at output,
argument numberOfBins : is the number of bin the x range will be subdivided into, limited to be at most 1000,
argument xMin : is the lower edge of the histogram,
argument xMax : is the upper edge of the histogram.

Hist::Hist(const Hist& h)  
creates an identical copy of the histogram in the argument, including bin contents.

Hist::Hist(string title, const Hist& h)  
creates an identical copy of the histogram in the argument, including bin contents, except that a new title is provided as first argument.

Hist& Hist::operator=(const Hist& h)  
copies all properties of the histogram in the argument, except that the original histogram title is retained.

void Hist::book(string title, int numberOfBins, double xMin, double xMax)  
define a histogram that previously was only declared; see above for the meaning of the arguments.

void Hist::name(string title)  
change the title of a histogram, but keep other properties unchanged.

void Hist::null()  
reset bin contents, but keep other histogram properties unchanged.

void Hist::fill(double xValue, double weight)  
fill the histogram, where
argument xValue : is the x position where the filling should occur, and
argument weight (default = 1.) : is the amount of weight to be added at this x value.

friend ostream& operator<<(ostream& os, const Hist& h)  
appends a simple histogram printout (see above for format) to the ostream, while leaving the histogram object itself unchanged. At most 100 columns are allowed to be displayed. If the number of bins is larger than 100 then the contents of adjacent bins are added to give the value in each column. (Two by two up to 200 bins, three by three up to 300, and so on, with the very last column possibly summing fewer rows than the others.)

void Hist::table(ostream& os = cout)  
void Hist::table(string fileName)  
print a two-column table, where the first column gives the center of each bin and the second one the corresponding bin contents. The desired output stream or file name can be provided as argument. The former is more flexible (e.g., it allows easy append to an existing file), whereas the latter is simpler for the case that each histogram should be a file of its own. The table may be useful for plotting e.g. with Gnuplot.

friend void table(const Hist& h1, const Hist& h2, ostream& os = cout)  
friend void table(const Hist& h1, const Hist& h2, string fileName)  
print a three-column table, where the first column gives the center of each bin and the second and third ones the corresponding bin contents of the two histograms. Only works if the two histograms have the same x axis (within a tiny tolerance), else nothing will be done.

double Hist::getBinContent(int iBin)  
return the value in bin iBin, ranging from 1 through numberOfBins, with 0 for underflow and numberOfBins + 1 for overflow.

int Hist::getEntries()  
return the number of entries, i.e. the number of time that fill(...) has been called.

bool Hist::sameSize(const Hist& h)  
checks that the number of bins and upper and lower limits are the same as in the histogram in the argument.

void Hist::takeLog(bool tenLog = true)  
by default take 10-logarithm of current contents bin by bin. With optional argument false instead take e-logarithm of contents bin by bin. If to be used, then right before the histogram is output.

void Hist::takeSqrt()  
take square root of current contents bin by bin, with negative contents set to zero.

Hist& Hist::operator+=(const Hist& h)  
Hist& Hist::operator-=(const Hist& h)  
adds or subtracts the current histogram by the contents of the histogram in the argument if sameSize(...) is true, else does nothing.

Hist& Hist::operator*=(const Hist& h)  
Hist& Hist::operator/=(const Hist& h)  
multiplies or divides the current histogram by the contents of the histogram in the argument if sameSize(...) is true, else does nothing.

Hist& Hist::operator+=(double f)  
Hist& Hist::operator-=(double f)  
adds or subtracts each bin content by the common offset f.

Hist& Hist::operator*=(double f)  
Hist& Hist::operator*=(double f)  
multiplies or divides each bin content by the common factor f.

friend Hist operator+(double f, const Hist& h1)  
friend Hist operator+(const Hist& h1, double f)  
friend Hist operator+(const Hist& h1, const Hist h2)  
add a constant to a histogram or two histograms to each other, bin by bin.

friend Hist operator-(double f, const Hist& h1)  
friend Hist operator-(const Hist& h1, double f)  
friend Hist operator-(const Hist& h1, const Hist h2)  
subtract a histogram from a constant, a constant from a histogram, or two histograms from each other, bin by bin.

friend Hist operator*(double f, const Hist& h1)  
friend Hist operator*(const Hist& h1, double f)  
friend Hist operator*(const Hist& h1, const Hist h2)  
multiply a constant by a histogram or two histograms by each other, bin by bin.

friend Hist operator/(double f, const Hist& h1)  
friend Hist operator/(const Hist& h1, double f)  
friend Hist operator/(const Hist& h1, const Hist h2)  
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Ϙ=&OCW*#oa&rl 'ᔖrk5Ǡ5{CW4٢_ kk)WPnmZWW9<`'!?Ah MW@e./P, T‚A4~9fsBNd9Ṵ")&Y[5H 8N+}M)݁0*&oZ-Ӻ}P :N^*Fmqf`sR>@95]qҨ 6,Çh;l4 @_LYՆ Vo3qa>=`\ej@2 p^${_;6Aj$dԠ>ѨzSMwiP}W/nM Տlbw+;U)˔siQ:P*G|VWTC 7iw$mJr(+WUR\pv%@1#ȗ-%\Y|?NE׷AĪ7k]Q)d^Eݏ ?gՓ.LC!C`'/ݲhcXQ0Y葶ɚ JX-s6#G zhjIΙ&t]ow5G3X,b4kR *dIU>(fh` bs1U|,1' )ThH5߿s\}xmcAJ? b ^\[EyӋj;niOe#qfCX79ߏ8{9-] tl:M1/8dl0 lԫZ2C  7=g ֻ|%R~O oj> endobj 20 0 obj <>stream xcd`ab`ddv44f!CyПڳ%L1wfFF7hʢ gMCKKsԢ<Ē 'G!8?93RO1'G!X!(8,5bs~nAiIjo~JjQ5/##F~.B=g6d/\3}Fr}=====]YY ݝ-'L};_Ÿ /6mi쫸.sq\2d endstream endobj 187 0 obj 283 endobj 18 0 obj <> endobj 17 0 obj <>stream xR HTHPLJ+CMR10c=4.FKZCopyright (C) 1997 American Mathematical Society. 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QCD Processes

This section is subdivided into soft and hard QCD processes, with open charm and bottom production set aside as a special part of the latter, and three-jet topologies as a special subset. Kindly note that there is a considerable amount of overlap between the soft and hard process classes, so that you are likely to double-count if you include both in a run.

Soft QCD processes

As a rule, the processes in this class should not be mixed with the simulation of other processes. All by themselves, they are intended to represent the total cross section of hadron collisions, with the exception of the "rare processes" that one wishes to study separately. In particular, jet physics at all scales occurs as part of the minimum-bias description.

We here use the "minimum bias" expression as a shorthand for inelastic, nondiffractive events. Strictly speaking, "minimum bias" represents an experimental procedure of accepting "everything", with some non-universal cuts to exclude elastic and diffractive topologies. In practice, the experimental minimum-bias sample may then contain some contamination of what is in PYTHIA classified as diffractive, especially (high-mass) double diffractive.

Some options to modify these cross sections are found on the Total Cross Sections page.

flag  SoftQCD:all   (default = off)
Common switch for the group of all soft QCD processes, as listed separately in the following.

flag  SoftQCD:nonDiffractive   (default = off)
The inelastic nondiffrative part of the total cross section, i.e. what would often be called the "minimum-bias component". The formalism is based on an eikonalized description of all the hard QCD processes, so includes them in combination with low-pT events. Code 101.
Since the current description is handled by the multiparton-interactions machinery as part of the parton-level processing, no hard process at all is defined at the process-level part of the event generation. Fortunately, in this case a special codeSub() method provides information on the first, i.e. hardest, subprocess selected by the multiparton-interactions machinery.
Note: this flag was precviously named SoftQCD:minBias, since it is almost equivalent to the minimum-bias component of the total cross section. It has invited some confusion, however, since "minimum-bias" usually refers to the experimental procedure, while "(inelastic) non-diffractive" better relates to the way events are generated in the program code. (Although also what separates diffractive from nondiffractive physics can be a matter of definition.) For backwards compatibility the SoftQCD:minBias name can be used as an alternative to SoftQCD:nonDiffractive for some time yet.

flag  SoftQCD:elastic   (default = off)
Elastic scattering A B -> A B. Code 102. It is possible to include Coulomb corrections, but by default this is off.

flag  SoftQCD:singleDiffractive   (default = off)
Single diffractive scattering A B -> X B and A B -> A X. See page on Diffraction for details. Codes 103 and 104.

flag  SoftQCD:doubleDiffractive   (default = off)
Double diffractive scattering A B -> X_1 X_2. See page on Diffraction for details. Code 105.

flag  SoftQCD:centralDiffractive   (default = off)
Central diffractive scattering A B -> A X B (a.k.a. double-Pomeron exchange, DPE). See pages on Total Cross Sections and on Diffraction for details. In particular note the SigmaTotal:zeroAXB flag, which is off in most tunes, and that therefore would need to be reset to on after the selection of a tune (even the default one). Code 106.

flag  SoftQCD:inelastic   (default = off)
All of the above processes, except for elastic. Codes 101, 103, 104, 105 and 106.

Hard QCD processes

This group contains the processes for QCD jet production above some minimum pT threshold. The pT_min cut cannot be put too low, or else unreasonably large jet cross sections will be obtained. This is because the divergent perturbative QCD cross section is used in this process group, without any regularization modifications. An eikonalized description, intended to be valid at all pT, is instead included as part of the multiparton-interactions framework, specifically in SoftQCD:nonDiffractive above.
Warning 1: you must remember to set the PhaseSpace:pTHatMin value if you use any of these processes; there is no sensible default.
Warning 2: you must not mix processes from the SoftQCD and HardQCD process groups, since this is likely to lead to double-counting.

flag  HardQCD:all   (default = off)
Common switch for the group of all hard QCD processes, as listed separately in the following.

flag  HardQCD:gg2gg   (default = off)
Scatterings g g -> g g. Code 111.

flag  HardQCD:gg2qqbar   (default = off)
Scatterings g g -> q qbar, where q by default is a light quark (u, d, s) (see below). Code 112.

flag  HardQCD:qg2qg   (default = off)
Scatterings q g -> q g and qbar g -> qbar g. Code 113.

flag  HardQCD:qq2qq   (default = off)
Scatterings q q' -> q q', q qbar' -> q qbar', qbar qbar' -> qbar qbar', where q' and q may agree, but the outgoing flavours equals the incoming ones Code 114.

flag  HardQCD:qqbar2gg   (default = off)
Scatterings q qbar -> g g. Code 115.

flag  HardQCD:qqbar2qqbarNew   (default = off)
Scatterings q qbar -> q' qbar', where q' by default is a light quark (u, d, s) (see below). Code 116.

mode  HardQCD:nQuarkNew   (default = 3; minimum = 0; maximum = 5)
Number of allowed outgoing new quark flavours in the above g g -> q qbar and q qbar -> q' qbar' processes, where quarks are treated as massless in the matrix-element expressions (but correctly in the phase space). It is thus assumed that c cbar and b bbar are added separately with masses taken into account, using the processes below. A change to 4 would also include c cbar in the massless approximation, etc. In order to avoid double-counting the processes below should then not be used simultaneously.

Hard QCD processes: heavy-flavour subset

These processes form a natural part of the above class, but can also be generated separately. Formally the heavy-quark mass makes these matrix elements finite in the pT -> 0 limit, but at high energies one may still question the validity of the expressions at low pT values, like for the other hard-QCD processes. Also as above, an eikonalized description, intended to be valid at all pT, is included as part of the multiparton-interactions framework.
Note that the processes below only represent the "tip of the iceberg" of charm and bottom production at high energies, where flavour excitation and shower branchings provide major additional sources. All these sources come together in the descriptions offered by SoftQCD:nonDiffractive and HardQCD:all.

flag  HardQCD:gg2ccbar   (default = off)
Scatterings g g -> c cbar. Code 121.

flag  HardQCD:qqbar2ccbar   (default = off)
Scatterings q qbar -> c cbar. Code 122.

flag  HardQCD:hardccbar   (default = off)
Sum of the previous two event types. Codes 121 and 122.

flag  HardQCD:gg2bbbar   (default = off)
Scatterings g g -> b bbar. Code 123.

flag  HardQCD:qqbar2bbbar   (default = off)
Scatterings q qbar -> b bbar. Code 124.

flag  HardQCD:hardbbbar   (default = off)
Sum of the previous two event types. Codes 123 and 124.

Hard QCD three-parton processes

Three-parton final states are generated by showers off two-parton processes. Topologies then cannot be specified beforehand, beyond what is provided by the two-parton hard process. For some checks it may be convenient to have access to the dedicated three-parton final states, which is what this set of processes allows. Cross sections have been taken from [Ber81].
Note that the processes in this section are not affected by the HardQCD:all switch. In fact, it would be double-counting to include both the HardQCD:all and the HardQCD:3parton processes in a run or study.
Warning: this section is still incomplete, e.g. the selection of colour flow is very simple, and so it should only be used with caution.

flag  HardQCD:3parton   (default = off)
Common switch for the group of all hard QCD processes with three partons in the final state, as listed separately in the following.

flag  HardQCD:gg2ggg   (default = off)
Scatterings g g -> g g g. Code 131.

flag  HardQCD:qqbar2ggg   (default = off)
Scatterings q qbar -> g g g. Code 132.

flag  HardQCD:qg2qgg   (default = off)
Scatterings q g -> q g g and qbar g -> qbar g g. Code 133.

flag  HardQCD:qq2qqgDiff   (default = off)
Scatterings q q' -> q q' g, q qbar' -> q qbar' g, and qbar qbar' -> qbar qbar' g. Code 134.

flag  HardQCD:qq2qqgSame   (default = off)
Scatterings q q -> q q g and qbar qbar -> qbar qbar g (q qbar -> q qbar g scatterings are considered separately below, see HardQCD:qqbar2qqbargSame). Code 135.

flag  HardQCD:qqbar2qqbargDiff   (default = off)
Scatterings q qbar -> q' qbar' g, where q' by default is a light quark (u, d, s) (see HardQCD:nQuarkNew above). Code 136.

flag  HardQCD:qqbar2qqbargSame   (default = off)
Scatterings q qbar -> q qbar g. Code 137.

flag  HardQCD:gg2qqbarg   (default = off)
Scatterings g g -> q qbar g, where q by default is a light quark (u, d, s) (see HardQCD:nQuarkNew above). Code 138.

flag  HardQCD:qg2qqqbarDiff   (default = off)
Scatterings q g -> q q' qbar' and qbar g -> qbar qbar' q', where q' by default is a light quark (u, d, s) (see HardQCD:nQuarkNew above). Code 139.

flag  HardQCD:qg2qqqbarSame   (default = off)
Scatterings q g -> q q qbar and qbar g -> qbar qbar q. Code 140. pythia8-8.1.80.orig/htmldoc/Diffraction.html0000644000175000017500000005257712217615311017120 0ustar sunsun Diffraction

Diffraction

Introduction

Diffraction is not well understood, and several alternative approaches have been proposed. Here we follow a fairly conventional Pomeron-based one, in the Ingelman-Schlein spirit [Ing85], but integrated to make full use of the standard PYTHIA machinery for multiparton interactions, parton showers and hadronization [Nav10,Cor10a]. This is the approach pioneered in the PomPyt program by Ingelman and collaborators [Ing97].

For ease of use (and of modelling), the Pomeron-specific parts of the generation are subdivided into three sets of parameters that are rather independent of each other:
(i) the total, elastic and diffractive cross sections are parametrized as functions of the CM energy, or can be set by the user to the desired values, see the Total Cross Sections page;
(ii) once it has been decided to have a diffractive process, a Pomeron flux parametrization is used to pick the mass of the diffractive system(s) and the t of the exchanged Pomeron, see below;
(iii) a diffractive system of a given mass is classified either as low-mass unresolved, which gives a simple low-pT string topology, or as high-mass resolved, for which the full machinery of multiparton interactions and parton showers are applied, making use of Pomeron PDFs.
The parameters related to multiparton interactions, parton showers and hadronization are kept the same as for normal nondiffractive events, with only one exception. This may be questioned, especially for the multiparton interactions, but we do not believe that there are currently enough good diffractive data that would allow detailed separate tunes.

The above subdivision may not represent the way "physics comes about". For instance, the total diffractive cross section can be viewed as a convolution of a Pomeron flux with a Pomeron-proton total cross section. Since neither of the two is known from first principles there will be a significant amount of ambiguity in the flux factor. The picture is further complicated by the fact that the possibility of simultaneous further multiparton interactions ("cut Pomerons") will screen the rate of diffractive systems. In the end, our set of parameters refers to the effective description that emerges out of these effects, rather than to the underlying "bare" parameters.

In the event record the diffractive system in the case of an excited proton is denoted p_diffr, code 9902210, whereas a central diffractive system is denoted rho_diffr, code 9900110. Apart from representing the correct charge and baryon numbers, no deeper meaning should be attributed to the names.

Pomeron flux

As already mentioned above, the total diffractive cross section is fixed by a default energy-dependent parametrization or by the user, see the Total Cross Sections page. Therefore we do not attribute any significance to the absolute normalization of the Pomeron flux. The choice of Pomeron flux model still will decide on the mass spectrum of diffractive states and the t spectrum of the Pomeron exchange.

mode  Diffraction:PomFlux   (default = 1; minimum = 1; maximum = 5)
Parametrization of the Pomeron flux f_Pom/p( x_Pom, t).
option 1 : Schuler and Sjöstrand [Sch94]: based on a critical Pomeron, giving a mass spectrum roughly like dm^2/m^2; a mass-dependent exponential t slope that reduces the rate of low-mass states; partly compensated by a very-low-mass (resonance region) enhancement. Is currently the only one that contains a separate t spectrum for double diffraction (along with MBR) and separate parameters for pion beams.
option 2 : Bruni and Ingelman [Bru93]: also a critical Pomeron giving close to dm^2/m^2, with a t distribution the sum of two exponentials. The original model only covers single diffraction, but is here expanded by analogy to double and central diffraction.
option 3 : a conventional Pomeron description, in the RapGap manual [Jun95] attributed to Berger et al. and Streng [Ber87a], but there (and here) with values updated to a supercritical Pomeron with epsilon > 0 (see below), which gives a stronger peaking towards low-mass diffractive states, and with a mass-dependent (the alpha' below) exponential t slope. The original model only covers single diffraction, but is here expanded by analogy to double and central diffraction.
option 4 : a conventional Pomeron description, attributed to Donnachie and Landshoff [Don84], again with supercritical Pomeron, with the same two parameters as option 3 above, but this time with a power-law t distribution. The original model only covers single diffraction, but is here expanded by analogy to double and central diffraction.
option 5 : the MBR (Minimum Bias Rockefeller) simulation of (anti)proton-proton interactions [Cie12]. The event generation follows a renormalized-Regge-theory model, successfully tested using CDF data. The simulation includes single and double diffraction, as well as the central diffractive (double-Pomeron exchange) process (106). Only p p, pbar p and p pbar beam combinations are allowed for this option. Several parameters of this model are listed below.

In options 3 and 4 above, the Pomeron Regge trajectory is parametrized as
alpha(t) = 1 + epsilon + alpha' t
The epsilon and alpha' parameters can be set separately:

parm  Diffraction:PomFluxEpsilon   (default = 0.085; minimum = 0.02; maximum = 0.15)
The Pomeron trajectory intercept epsilon above. For technical reasons epsilon > 0 is necessary in the current implementation.

parm  Diffraction:PomFluxAlphaPrime   (default = 0.25; minimum = 0.1; maximum = 0.4)
The Pomeron trajectory slope alpha' above.

When option 5 is selected, the following parameters of the MBR model [Cie12] are used:

parm  Diffraction:MBRepsilon   (default = 0.104; minimum = 0.02; maximum = 0.15)

parm  Diffraction:MBRalpha   (default = 0.25; minimum = 0.1; maximum = 0.4)
the parameters of the Pomeron trajectory.

parm  Diffraction:MBRbeta0   (default = 6.566; minimum = 0.0; maximum = 10.0)

parm  Diffraction:MBRsigma0   (default = 2.82; minimum = 0.0; maximum = 5.0)
the Pomeron-proton coupling, and the total Pomeron-proton cross section.

parm  Diffraction:MBRm2Min   (default = 1.5; minimum = 0.0; maximum = 3.0)
the lowest value of the mass squared of the dissociated system.

parm  Diffraction:MBRdyminSDflux   (default = 2.3; minimum = 0.0; maximum = 5.0)

parm  Diffraction:MBRdyminDDflux   (default = 2.3; minimum = 0.0; maximum = 5.0)

parm  Diffraction:MBRdyminCDflux   (default = 2.3; minimum = 0.0; maximum = 5.0)
the minimum width of the rapidity gap used in the calculation of Ngap(s) (flux renormalization).

parm  Diffraction:MBRdyminSD   (default = 2.0; minimum = 0.0; maximum = 5.0)

parm  Diffraction:MBRdyminDD   (default = 2.0; minimum = 0.0; maximum = 5.0)

parm  Diffraction:MBRdyminCD   (default = 2.0; minimum = 0.0; maximum = 5.0)
the minimum width of the rapidity gap used in the calculation of cross sections, i.e. the parameter dy_S, which suppresses the cross section at low dy (non-diffractive region).

parm  Diffraction:MBRdyminSigSD   (default = 0.5; minimum = 0.001; maximum = 5.0)

parm  Diffraction:MBRdyminSigDD   (default = 0.5; minimum = 0.001; maximum = 5.0)

parm  Diffraction:MBRdyminSigCD   (default = 0.5; minimum = 0.001; maximum = 5.0)
the parameter sigma_S, used for the cross section suppression at low dy (non-diffractive region).

Separation into low and high masses

Preferably one would want to have a perturbative picture of the dynamics of Pomeron-proton collisions, like multiparton interactions provide for proton-proton ones. However, while PYTHIA by default will only allow collisions with a CM energy above 10 GeV, the mass spectrum of diffractive systems will stretch to down to the order of 1.2 GeV. It would not be feasible to attempt a perturbative description there. Therefore we do offer a simpler low-mass description, with only longitudinally stretched strings, with a gradual switch-over to the perturbative picture for higher masses. The probability for the latter picture is parametrized as
P_pert = P_max ( 1 - exp( (m_diffr - m_min) / m_width ) )
which vanishes for the diffractive system mass m_diffr < m_min, and is 1 - 1/e = 0.632 for m_diffr = m_min + m_width, assuming P_max = 1.

parm  Diffraction:mMinPert   (default = 10.; minimum = 5.)
The abovementioned threshold mass m_min for phasing in a perturbative treatment. If you put this parameter to be bigger than the CM energy then there will be no perturbative description at all, but only the older low-pt description.

parm  Diffraction:mWidthPert   (default = 10.; minimum = 0.)
The abovementioned threshold width m_width.

parm  Diffraction:probMaxPert   (default = 1.; minimum = 0.; maximum = 1.)
The abovementioned maximum probability P_max.. Would normally be assumed to be unity, but a somewhat lower value could be used to represent a small nonperturbative component also at high diffractive masses.

Low-mass diffraction

When an incoming hadron beam is diffractively excited, it is modeled as if either a valence quark or a gluon is kicked out from the hadron. In the former case this produces a simple string to the leftover remnant, in the latter it gives a hairpin arrangement where a string is stretched from one quark in the remnant, via the gluon, back to the rest of the remnant. The latter ought to dominate at higher mass of the diffractive system. Therefore an approximate behaviour like
P_q / P_g = N / m^p
is assumed.

parm  Diffraction:pickQuarkNorm   (default = 5.0; minimum = 0.)
The abovementioned normalization N for the relative quark rate in diffractive systems.

parm  Diffraction:pickQuarkPower   (default = 1.0)
The abovementioned mass-dependence power p for the relative quark rate in diffractive systems.

When a gluon is kicked out from the hadron, the longitudinal momentum sharing between the the two remnant partons is determined by the same parameters as above. It is plausible that the primordial kT may be lower than in perturbative processes, however:

parm  Diffraction:primKTwidth   (default = 0.5; minimum = 0.)
The width of Gaussian distributions in p_x and p_y separately that is assigned as a primordial kT to the two beam remnants when a gluon is kicked out of a diffractive system.

parm  Diffraction:largeMassSuppress   (default = 2.; minimum = 0.)
The choice of longitudinal and transverse structure of a diffractive beam remnant for a kicked-out gluon implies a remnant mass m_rem distribution (i.e. quark plus diquark invariant mass for a baryon beam) that knows no bounds. A suppression like (1 - m_rem^2 / m_diff^2)^p is therefore introduced, where p is the diffLargeMassSuppress parameter.

High-mass diffraction

The perturbative description need to use parton densities of the Pomeron. The options are described in the page on PDF Selection. The standard perturbative multiparton interactions framework then provides cross sections for parton-parton interactions. In order to turn these cross section into probabilities one also needs an ansatz for the Pomeron-proton total cross section. In the literature one often finds low numbers for this, of the order of 2 mb. These, if taken at face value, would give way too much activity per event. There are ways to tame this, e.g. by a larger pT0 than in the normal pp framework. Actually, there are many reasons to use a completely different set of parameters for MPI in diffraction than in pp collisions, especially with respect to the impact-parameter picture, see below. A lower number in some frameworks could alternatively be regarded as a consequence of screening, with a larger "bare" number.

For now, however, an attempt at the most general solution would carry too far, and instead we patch up the problem by using a larger Pomeron-proton total cross section, such that average activity makes more sense. This should be viewed as the main tunable parameter in the description of high-mass diffraction. It is to be fitted to diffractive event-shape data such as the average charged multiplicity. It would be very closely tied to the choice of Pomeron PDF; we remind that some of these add up to less than unit momentum sum in the Pomeron, a choice that also affect the value one ends up with. Furthermore, like with hadronic cross sections, it is quite plausible that the Pomeron-proton cross section increases with energy, so we have allowed for a power-like dependence on the diffractive mass.

parm  Diffraction:sigmaRefPomP   (default = 10.; minimum = 2.; maximum = 40.)
The assumed Pomeron-proton effective cross section, as used for multiparton interactions in diffractive systems. If this cross section is made to depend on the mass of the diffractive system then the above value refers to the cross section at the reference scale, and
sigma_PomP(m) = sigma_PomP(m_ref) * (m / m_ref)^p
where m is the mass of the diffractive system, m_ref is the reference mass scale Diffraction:mRefPomP below and p is the mass-dependence power Diffraction:mPowPomP. Note that a larger cross section value gives less MPI activity per event. There is no point in making the cross section too big, however, since then pT0 will be adjusted downwards to ensure that the integrated perturbative cross section stays above this assumed total cross section. (The requirement of at least one perturbative interaction per event.)

parm  Diffraction:mRefPomP   (default = 100.0; minimum = 1.)
The mRef reference mass scale introduced above.

parm  Diffraction:mPowPomP   (default = 0.0; minimum = 0.0; maximum = 0.5)
The p mass rescaling pace introduced above.

Also note that, even for a fixed CM energy of events, the diffractive subsystem will range from the abovementioned threshold mass m_min to the full CM energy, with a variation of parameters such as pT0 along this mass range. Therefore multiparton interactions are initialized for a few different diffractive masses, currently five, and all relevant parameters are interpolated between them to obtain the behaviour at a specific diffractive mass. Furthermore, A B ->X B and A B ->A X are initialized separately, to allow for different beams or PDF's on the two sides. These two aspects mean that initialization of MPI is appreciably slower when perturbative high-mass diffraction is allowed.

Diffraction tends to be peripheral, i.e. occur at intermediate impact parameter for the two protons. That aspect is implicit in the selection of diffractive cross section. For the simulation of the Pomeron-proton subcollision it is the impact-parameter distribution of that particular subsystem that should rather be modeled. That is, it also involves the transverse coordinate space of a Pomeron wavefunction. The outcome of the convolution therefore could be a different shape than for nondiffractive events. For simplicity we allow the same kind of options as for nondiffractive events, except that the bProfile = 4 option for now is not implemented.

mode  Diffraction:bProfile   (default = 1; minimum = 0; maximum = 3)
Choice of impact parameter profile for the incoming hadron beams.
option 0 : no impact parameter dependence at all.
option 1 : a simple Gaussian matter distribution; no free parameters.
option 2 : a double Gaussian matter distribution, with the two free parameters coreRadius and coreFraction.
option 3 : an overlap function, i.e. the convolution of the matter distributions of the two incoming hadrons, of the form exp(- b^expPow), where expPow is a free parameter.

parm  Diffraction:coreRadius   (default = 0.4; minimum = 0.1; maximum = 1.)
When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a radius that is a factor coreRadius smaller than the rest.

parm  Diffraction:coreFraction   (default = 0.5; minimum = 0.; maximum = 1.)
When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a fraction coreFraction of the matter content of the hadron.

parm  Diffraction:expPow   (default = 1.; minimum = 0.4; maximum = 10.)
When bProfile = 3 it gives the power of the assumed overlap shape exp(- b^expPow). Default corresponds to a simple exponential drop, which is not too dissimilar from the overlap obtained with the standard double Gaussian parameters. For expPow = 2 we reduce to the simple Gaussian, bProfile = 1, and for expPow -> infinity to no impact parameter dependence at all, bProfile = 0. For small expPow the program becomes slow and unstable, so the min limit must be respected. pythia8-8.1.80.orig/htmldoc/EventRecord.html0000644000175000017500000006175612217615312017110 0ustar sunsun The Event Record

The Event Record

A Pythia instance contains two members of the Event class. The one called process provides a brief summary of the main steps of the hard process, while the one called event contains the full history. The user would normally interact mainly with the second one, so we will exemplify primarily with that one.

The Event class to first approximation is a vector of Particles, so that it can expand to fit the current event size. The index operator is overloaded, so that e.g. event[i] corresponds to the i'th particle of the object event. Thus event[i].id() returns the identity of the i'th particle, and so on. Therefore the methods of the Particle class are at least as essential as those of the Event class itself.

As used inside PYTHIA, some conventions are imposed on the structure of the event record. Entry 0 of the vector<Particle> is used to represent the event as a whole, with its total four-momentum and invariant mass, but does not form part of the event history. Lines 1 and 2 contains the two incoming beams, and only from here on history tracing works as could be expected. That way unassigned mother and daughter indices can be put 0 without ambiguity. Depending on the task at hand, a loop may therefore start at index 1 rather than 0 without any loss. Specifically, for translation to other event record formats such as HepMC [Dob01], where the first index is 1, the Pythia entry 0 definitely ought to be skipped in order to minimize the danger of indexing errors.

In the following we will list the methods available. Only a few of them have a function to fill in normal user code.

Basic output methods

Some methods are available to read out information on the current event record:

Particle& Event::operator[](int i)  
const Particle& Event::operator[](int i)  
returns a (const) reference to the i'th particle in the event record, which can be used to get (or set) all the properties of this particle.

Particle& Event::front()  
Particle& Event::at(int i)  
Particle& Event::back()  
returns a reference to the zeroth, i'th or last particle in the event record, as an alternative to the methods above.

int Event::size()  
The event size, i.e. the size of the vector<Particle>. Thus valid particles, to be accessed by the above indexing operator, are stored in the range 0 <= i < size(). See comment above about the (ir)relevance of entry 0.

void Event::list()  
void Event::list(ostream& os)  
void Event::list(bool showScaleAndVertex, bool showMothersAndDaughters = false)  
void Event::list(bool showScaleAndVertex, bool showMothersAndDaughters, ostream& os)  
Provide a listing of the whole event, i.e. of the vector<Particle>. The methods with fewer arguments call the final one with the respective default values, and are non-inlined so they can be used in a debugger. The basic identity code, status, mother, daughter, colour, four-momentum and mass data are always given, but the methods can also be called with a few optional arguments for further information:
argument showScaleAndVertex (default = false) : optionally give a second line for each particle, with the production scale (in GeV), the particle polarization (dimensionless), the production vertex (in mm or mm/c) and the invariant lifetime (also in mm/c).
argument showMothersAndDaughters (default = false) : gives a list of all daughters and mothers of a particle, as defined by the motherList(i) and daughterList(i) methods described below. It is mainly intended for debug purposes.
argument os (default = cout) : a reference to the ostream object to which the event listing will be directed.

Each Particle has two mother and two daughter indices. These may be used to encode zero, one, two or more mothers/daughters, depending on the combination of values and status code, according to well-defined rules. The two methods below can do this job easier for you.

vector<int> Event::motherList(int i)  
returns a vector of all the mother indices of the particle at index i. This list is empty for entries 0, 1 and 2, i.e. the "system" in line 0 is not counted as part of the history. Normally the list contains one or two mothers, but it can also be more, e.g. in string fragmentation the whole fragmenting system is counted as mothers to the primary hadrons. Many particles may have the same motherList. Mothers are listed in ascending order.

vector<int> Event::daughterList(int i)  
returns a vector of all the daughter indices of the particle at index i. This list is empty for a particle that did not decay (or, if the evolution is stopped early enough, a parton that did not branch), while otherwise it can contain a list of varying length, from one to many. For the two incoming beam particles, all shower initiators and beam remnants are counted as daughters, with the one in slot 0 being the one leading up to the hardest interaction. The "system" in line 0 does not have any daughters, i.e. is not counted as part of the history. Many partons may have the same daughterList. Daughters are listed in ascending order.

int Event::statusHepMC(int i)  
returns the status code according to the HepMC conventions agreed in February 2009. This convention does not preserve the full information provided by the internal PYTHIA status code, as obtained by Particle::status(), but comes reasonably close. The allowed output values are:

  • 0 : an empty entry, with no meaningful information and therefore to be skipped unconditionally (should not occur in PYTHIA);
  • 1 : a final-state particle, i.e. a particle that is not decayed further by the generator (may also include unstable particles that are to be decayed later, as part of the detector simulation);
  • 2 : a decayed Standard Model hadron or tau or mu lepton, excepting virtual intermediate states thereof (i.e. the particle must undergo a normal decay, not e.g. a shower branching);
  • 3 : a documentation entry (not used in PYTHIA);
  • 4 : an incoming beam particle;
  • 11 - 200 : an intermediate (decayed/branched/...) particle that does not fulfill the criteria of status code 2, with a generator-dependent classification of its nature; in PYTHIA the absolute value of the normal status code is used.

Further output methods

The above methods are the main ones that a normal user would make frequent use of. There are some further methods that also could come in handy, in the exploration of the history of an event, but where the outcome is not always obvious if one is not familiar with the detailed structure of an event record.

int Event::iTopCopy(int i)  
int Event::iBotCopy(int i)  
are used to trace carbon copies of the particle at index i up to its top mother or down to its bottom daughter. If there are no such carbon copies, i itself will be returned. A carbon copy is when the "same" particle appears several times in the event record, but with changed momentum owing to recoil effects.

int Event::iTopCopyId(int i)  
int Event::iBotCopyId(int i)  
also trace top mother and bottom daughter, but do not require carbon copies, only that one can find an unbroken chain, of mothers or daughters, with the same flavour id code. When it encounters ambiguities, say a g -> g g branching or a u u -> u u hard scattering, it will stop the tracing and return the current position. It can be confused by nontrivial flavour changes, e.g. a hard process u d -> d u by W^+- exchange will give the wrong answer. These methods therefore are of limited use for common particles, in particular for the gluon, but should work well for "rare" particles.

vector<int> Event::sisterList(int i)  
returns a vector of all the sister indices of the particle at index i, i.e. all the daughters of the first mother, except the particle itself.

vector<int> Event::sisterListTopBot(int i,bool widenSearch = true)  
returns a vector of all the sister indices of the particle at index i, tracking up and back down through carbon copies if required. That is, the particle is first traced up with iTopCopy() before its mother is found, and then all the particles in the daughterList() of this mother are traced down with iBotCopy(), omitting the original particle itself. Any non-final particles are removed from the list. Should this make the list empty the search criterion is widened so that all final daughters are allowed, not only carbon-copy ones. That is, starting from the top mother, all its daughters are found, except for the traced-up one, and then all their daughters, and so on. This can produce quite extensive and rather useless output, notably when tracing parton showers. A second argument false inhibits the second step, and increases the risk that an empty list is returned. A typical example of this is for ISR cascades, e.g. e -> e gamma where the photon may not have any obvious sister in the final state if the bottom copy of the photon is an electron that annihilates and thus is not part of the final state.

bool Event::isAncestor(int i, int iAncestor)  
traces the particle i upwards through mother, grandmother, and so on, until either iAncestor is found or the top of the record is reached. Normally one unique mother is required, as is the case e.g. in decay chains or in parton showers, so that e.g. the tracing through a hard scattering would not work. For hadronization, first-rank hadrons are identified with the respective string endpoint quark, which may be useful e.g. for b physics, while higher-rank hadrons give false. Currently also ministrings that collapsed to one single hadron and junction topologies give false.

One data member in an Event object is used to keep track of the largest col() or acol() colour tag set so far, so that new ones do not clash.

mode  Event:startColTag   (default = 100; minimum = 0; maximum = 1000)
This sets the initial colour tag value used, so that the first one assigned is startColTag + 1, etc. The Les Houches accord [Boo01] suggests this number to be 500, but 100 works equally well.

void Event::initColTag(int colTag = 0)  
forces the current colour tag value to be the larger of the input colTag and the above Event:startColTag values.

int Event::lastColTag()  
returns the current maximum colour tag.

int Event::nextColTag()  
increases the current maximum colour tag by one and returns this new value. This method is used whenever a new colour tag is needed.

Many event properties are accessible via the Info class, see here. Since they are used directly in the event generation, a few are stored directly in the Event class, however.

void Event::scale( double scaleIn)  
double Event::scale()  
set or get the scale (in GeV) of the hardest process in the event. Matches the function of the scale variable in the Les Houches Accord.

void Event::scaleSecond( double scaleSecondIn)  
double Event::scaleSecond()  
set or get the scale (in GeV) of a second hard process in the event, in those cases where such a one has been requested.

Constructors and modifications of the event record

Although you would not normally need to create your own Event instance, there may be times where that could be convenient. The typical example would be if you want to create a new event record that is the sum of a few different ones, e.g. if you want to simulate pileup events. There may also be cases where you want to add one or a few particles to an existing event record.

Event::Event(int capacity = 100)  
creates an empty event record, but with a reserved size capacity for the Particle vector.

Event& Event::operator=(const Event& oldEvent)  
copies the input event record.

Event& Event::operator+=(const Event& addEvent)  
appends an event to an existing one. For the appended particles mother, daughter and colour tags are shifted to make a consistent record. The zeroth particle of the appended event is not copied, but the zeroth particle of the combined event is updated to the full energy-momentum content.

void Event::init(string headerIn = "", ParticleData* particleDataPtrIn = 0, int startColTagIn = 100)  
initializes colour, the pointer to the particle database, and the header specification used for the event listing. We remind that a Pythia object contains two event records process and event. Thus one may e.g. call either pythia.process.list() or pythia.event.list(). To distinguish those two rapidly at visual inspection, the "Pythia Event Listing" header is printed out differently, in one case adding "(hard process)" and in the other "(complete event)". When += is used to append an event, the modified event is printed with "(combination of several events)" as a reminder.

void Event::clear()  
empties event record. Specifically the Particle vector size is reset to zero.

void Event::reset()  
empties the event record, as clear() above, but then fills the zero entry of the Particle vector with the pseudoparticle used to represent the event as a whole. At this point the pseudoparticle is not assigned any momentum or mass.

void Event::popBack(int n = 1)  
removes the last n particle entries; must be a positive number. History (and other) information of remaning entries is untouched, and so may be internally inconsistent.

void Event::remove(int iFirst, int iLast)  
removes particles in the range between indices iFirst and iLast, including the endpoints. History (and other) information of remaning entries is untouched, and so may be internally inconsistent.

bool Event::undoDecay(int i)  
removes the decay chain of the particle i and thus restores it to its undecayed state. It is only intended for "normal" particle decay chains, and will return false in other cases, notably if the particle is coloured. The procedure would not work if non-local momentum shifts have been performed, such as with a Bose-Einstein shift procedure (or for a dipole shower recoiler). The history information of the remaining particles, many of which may have new indices, is updated to be internally consistent.

int Event::append(Particle entryIn)  
appends a particle to the bottom of the event record and returns the index of this position.

int Event::append(int id, int status, int mother1, int mother2, int daughter1, int daughter2, int col, int acol, double px, double py, double pz, double e, double m = 0., double scale = 0., double pol = 9.)  
appends a particle to the bottom of the event record and returns the index of this position; see here for the meaning of the various particle properties.

int Event::append(int id, int status, int mother1, int mother2, int daughter1, int daughter2, int col, int acol, Vec4 p, double m = 0., double scale = 0., double pol = 9.)  
appends a particle to the bottom of the event record and returns the index of this position, as above but with four-momentum as a Vec4.

int Event::append(int id, int status, int col, int acol, double px, double py, double pz, double e, double m = 0., double scale = 0., double pol = 9.)  
int Event::append(int id, int status, int col, int acol, Vec4 p, double m = 0., double scale = 0., double pol = 9.)  
appends a particle to the bottom of the event record and returns the index of this position, as above but with vanishing (i.e. zero) mother and daughter indices.

int Event::setEvtPtr(int iSet = -1)  
send in the this pointer of the current Event itself to the particle iSet, by default the most recently appended particle. Also generates a pointer to the ParticleDataEntry object of the identity code of the particle.

int Event::copy(int iCopy, int newStatus = 0)  
copies the existing particle in entry iCopy to the bottom of the event record and returns the index of this position. By default, i.e. with newStatus = 0, everything is copied precisely as it is, which means that history information has to be modified further by hand to make sense. With a positive newStatus, the new copy is set up to be the daughter of the old, with status code newStatus, while the status code of iCopy is negated. With a negative newStatus, the new copy is instead set up to be the mother of iCopy. An attempt to copy an out-of-range entry will return -1.

void Event::restorePtrs()  
each particle in the event record has a pointer to the event itself and another to the particle species it belongs to. The latter pointer is automatically set/changed whenever the particle identity is set/changed by one of the normal methods. Of course the pointer values are specific to the memory locations of the current run, and so it has no sense to save them if events are written to file. Should you use some persistency scheme that bypasses the normal methods when the event is read back in, you can use restorePtrs() afterwards to set these pointers appropriately.

A few methods exist to rotate and boost events. These derive from the Vec4 methods, and affect both the momentum and the vertex (position) components of all particles.

void Event::rot(double theta, double phi)  
rotate all particles in the event by this polar and azimuthal angle (expressed in radians).

void Event::bst(double betaX, double betaY, double betaZ)  
void Event::bst(double betaX, double betaY, double betaZ, double gamma)  
void Event::bst(const Vec4& vec)  
boost all particles in the event by this three-vector. Optionally you may provide the gamma value as a fourth argument, which may help avoid roundoff errors for big boosts. You may alternatively supply a Vec4 four-vector, in which case the boost vector becomes beta = p/E.

void Event::rotbst(const RotBstMatrix& M)  
rotate and boost by the combined action encoded in the RotBstMatrix M.

The Junction Class

The event record also contains a vector of junctions, which often is empty or else contains only a very few per event. Methods are available to add further junctions or query the current junction list. This is only for the expert user, however, and is not discussed further here, but only the main points.

A junction stores the properties associated with a baryon number that is fully resolved, i.e. where three different colour indices are involved. There are two main applications,

  1. baryon beams, where at least two valence quarks are kicked out, and so the motion of the baryon number is nontrivial;
  2. baryon-number violating processes, e.g. in SUSY with broken R-parity.
Information on junctions is set, partly in the process generation, partly in the beam remnants machinery, and used by the fragmentation routines, but the normal user does not have to know the details.

For each junction, information is stored on the kind of junction, and on the three (anti)colour indices that are involved in the junction. The possibilities foreseen are:

  • kind = 1 : incoming colourless particle to three outgoing colours (e.g. baryon beam remnant or neutralino -> q q q);
  • kind = 2 : incoming colourless particle to three outgoing anticolours;
  • kind = 3 : one incoming anticolour (stored first) and two outgoing colours (e.g. antisquark decaying to two quarks, or gluino decay to three quarks);
  • kind = 4 : one incoming colour (stored first) and two outgoing anticolours (e.g. squark decaying to two antiquarks, or gluino decaying to three antiquarks);
  • kind = 5 : two incoming anticolours (stored first) and one outgoing colour (e.g. resonant squark production through RPV);
  • kind = 6 : two incoming colours (stored first) and one outgoing anticolour (e.g. resonant antisquark production through RPV);
The odd (even) kind codes corresponds to a +1 (-1) change in baryon number across the junction.

The kind and colour information in the list of junctions can be set or read with methods of the Event class, but are not of common interest and so not described here.

A listing of current junctions can be obtained with the listJunctions() method.

Subsystems

Separate from the event record as such, but closely tied to it is the PartonSystems class, which mainly stores the parton indices of incoming and outgoing partons, classified by collision subsystem. Such information is needed to interleave multiparton interactions, initial-state showers and final-state showers, and append beam remnants. It could also be used in other places. It is intended to be accessed only by experts, such as implementors of new showering models. pythia8-8.1.80.orig/htmldoc/ProgramFiles.html0000644000175000017500000003705412217615311017253 0ustar sunsun Program Files

Program Files

The code is subdivided into a set of files, mainly by physics task. Each file typically contains one main class, but often with a few related helper classes that are not used elsewhere in the program. Normally the files come in pairs.
  • A header file, .h in the include subdirectory, where the public interface of the class is declared, and inline methods are defined.
  • A source code file, .cc in the src subdirectory, where most of the methods are implemented.
During compilation, related dependency files, .d, and compiled code, .o are created in the tmp subdirectory.

In part the .xml documentation files in the xmldoc subdirectory have matching names, but the match is broken by the desire to group topics more by user interaction than internal operation. On these pages the function of the different code files is summarized. Currently, each .xml file is also translated into an .html one in the htmldoc subdirectory, to allow easy viewing of the contents in a web browser, and an .php one in phpdoc, for more sophisticated interactivity if that subdirectory is installed on a web server.

Here is the current list of files, ordered alphabetically, with a brief description of contents.

file  Analysis  
contains routines to analyze events. Currently it can do sphericity, thrust, Lund/Jade/Durham jet clustering, cone-jet finding, and the kT, anti-kT and Cambridge/Aachen algorithms for hadron colliders.

file  Basics  
contains some basic facilities of general use: a random number generator Rndm, a four-vector class Vec4, and a histogram class Hist.

file  BeamParticle  
contains information on all partons extracted from one of the two beams. Defines modified parton distributions accordingly during the showering and multiparton interactions processing, thereby extending on the one-particle-inclusive distributions defined by the previous class. Finds the internal structure for a beam remnant.

file  BeamRemnants  
adds primordial kT to the set of hard subsystems, and combines these subsystems with the two beam remnants to provide the overall energy-momentum picture. Also ties together all the colour lines into consistent singlets.

file  BeamShape  
generates momentum spread of beams, and spread of collision vertex position.

file  BoseEinstein  
provides a simple method to impose Bose-Einstein correlations on pairs of identical mesons.

file  Event  
contains the event record, which basically is a vector of particles. This file also contains the Particle class, used by Event. Pythia uses two Event objects, one for the process-level record (process) and one for the complete event (event).

file  FragmentationFlavZpT  
contains the classes for describing the fragmentation steps in flavour and in longitudinal and transverse momentum.

file  FragmentationSystems  
defines some containers of parton systems, for use in the fragmentation routines.

file  HadronLevel  
turns the parton-level event above into a set of outgoing particles, by applying string fragmentation (with special treatment for low-mass systems) and secondary decays, and optionally Bose-Einstein corrections.

file  HelicityBasics  
basic classes for the handling of helicities in tau lepton decays.

file  HelicityMatrixElements  
helicity-dependent decay matrix elements for the tau lepton.

file  HiddenValleyFragmentation  
hadronization in models with a hidden sector that contains an unbroken SU(N), which gives confinement. The model and code is largely derived from the normal fragmentation classes.

file  History  
methods to reconstruct the imagined shower history of a matrix-element-generated multiparton configuration, as part of the CKKW-L matrix element merging.

file  Info  
is a simple container that gives access to some information on the nature of the current process, such as Mandelstam variables. Also contains a small database for errors and warnings encountered during program execution.

file  LesHouches  
gives the possibility to feed in parton configurations for the subsequent event generation. One base class is defined, with containers for initialization and event information, that can be read from Pythia. Derived classes allow for a few different cases.

file  LHAFortran  
is a header file only, for a class derived from the above LesHouches one, to be used for runtime interfacing to Fortran programs, such as PYTHIA 6.

file  LHAPDFInterface  
is a header file only, with interfaces to the key LHAPDF routines, as needed for a runtime interface. There is a file lhapdfdummy/LHAPDFdummy.cc with matching dummy implementations, however. This file is used to build a separate liblhapdfdummy library, to be linked when the LHAPDF library is not used, so as to avoid problems with undefined references.

file  MergingHooks  
intercede in the normal shower evolution to construct the relevant Sudakov form factor suppressions as part of the CKKW-L matrix element merging.

file  MiniStringFragmentation  
performs string fragmentation in cases where the colour singlet subsystem mass is so small that one or at most two primary hadrons should be produced from it.

file  MultipartonInteractions  
performs multiparton interactions.

file  ParticleData  
contains a database of all necessary particle data (masses, names, ..) and decay channels.

file  ParticleDecays  
performs the decays of all normal unstable hadrons and leptons, i.e. in mass up to and including b bbar systems. It is not intended for decays of electroweak resonances, like Z^0.

file  PartonDistributions  
contains parton distribution functions for the proton and electron. Currently very simple, with only two p parametrizations and one e ditto available, but it is possible to link in external sets.

file  PartonLevel  
turns the (hard) process above into a complete set of partons, by adding initial- and final-state radiation, multiparton interactions, and beam remnants.

file  PartonSystems  
keeps track of which partons belong to which partonic subsystem, i.e. one of the multiparton (semi)hard interactions with associated showers.

file  PhaseSpace  
selects a point in phase space for the hard-process generation, optimized separately for each process to give improved Monte Carlo efficiency.

file  ProcessContainer  
packages the information on a given subprocess, combining the phase-space selection and cross-section evaluation machineries with some statistics information. Also sets up the list of processes to be studied in a run.

file  ProcessLevel  
handles the generation of the (hard) process that sets the character of the event. This involves either using internally implemented processes or linking to Les Houches information. The latter can be by runtime interfaces or by reading in a file. This step also includes resonance decays.

file  Pythia  
is the main class, that administrates the whole event generation process by making use of all the others classes. Objects of most other classes reside (directly or indirectly) inside Pythia, so only a Pythia object needs to be explicitly instantiated and addressed by the user.

file  Pythia8ToHepMC  
contains an interface to convert the PYTHIA 8 event record into the HepMC format. The Pythia8ToHepMC.cc file is located in the subdirectory pythia8tohepmc and is used to build a separate libpythia8tohepmc library.

file  PythiaComplex  
is only a .h file, containing a typedef for double precision complex numbers.

file  PythiaStdlib  
contains most of the Stdlib headers used in PYTHIA 8, with using directives. It defines M_PI if this is not already done. Also a few simple inline methods: pow2(x), pow3(x), pow4(x), pow5(x) and pow6(x) for small integer powers, and sqrtpos(x) where a max(0., x) ensures that one does not take the square root of a negative number. Also non-inlined GammaReal(x) for the Gamma function value of a real argument.

file  ResonanceDecays  
decays resonances as part of the hard-process stage, in many cases (but not all) including angular correlations between the decay products.

file  ResonanceWidths  
encodes some properties of resonances, in particular the dynamic calculation of widths.

file  RHadrons  
handles the production and decay of hadrons formed by long-lived gluinos, stops or sbottoms.

file  Settings  
contains a database of all flags, modes, parameters and words that determine the performance of the generator. Initial values are obtained from the contents of the .xml files, but these values can then be changed by the user.

file  SigmaCompositeness  
contains the cross sections and matrix elements for production of some particles in compositeness scenarios, specifically excited fermions.

file  SigmaEW  
contains the cross sections and matrix elements for electroweak processes involving photons, Z^0's and W^+-'s.

file  SigmaExtraDim  
contains the cross sections and matrix elements for processes in scenarios involving extra dimensions.

file  SigmaGeneric  
contains the cross sections and matrix elements for some generic processes, to be used as building blocks for a few BSM scenarios.

file  SigmaHiggs  
contains the cross sections and matrix elements for Higgs production.

file  SigmaLeftRightSym  
contains the cross sections and matrix elements for particle production in left-right-symmetry scenarios, specifically righthanded Z and W bosons and doubly-charged Higgs bosons.

file  SigmaLeptoquark  
contains the cross sections and matrix elements for leptoquark production.

file  SigmaNewGaugeBosons  
contains the cross sections and matrix elements for a Z'^0, a W^+- and a horizontal gauge boson R^0.

file  SigmaOnia  
contains the cross sections and matrix elements for charmonium and bottomonium production.

file  SigmaProcess  
contains the base class and derived classes for the evaluation of different matrix elements. Also keeps track of allowed incoming parton configurations and their cross sections, including parton densities. In order to keep this file from becoming too big, actual cross sections are found in several separate files of derived classes: SigmaQCD, SigmaEW, SigmaOnia, SigmaHiggs, SigmaSUSY, SigmaNewGaugeBosons, SigmaLeftRightSym, SigmaLeptoquark, SigmaCompositeness, SigmaExtraDim and SigmaGeneric.

file  SigmaQCD  
contains the cross sections and matrix elements for soft and hard QCD processes.

file  SigmaSUSY  
contains the cross sections and matrix elements for Supersymmetric processes.

file  SigmaTotal  
contains parametrizations of total, elastic and diffractive hadronic cross sections.

file  SpaceShower  
performs spacelike initial-state transverse-momentum-ordered shower evolution.

file  StandardModel  
contains the running alpha_strong, with Lambda matching at flavour thresholds, the running alpha_em, CKM mixing matrices, and a few other parameters such as sin^2(theta_W).

file  StringFragmentation  
performs string fragmentation of a given set of partons.

file  SusyCouplings  
stores the various couplings used for SUSY cross sections and decays, as calculated from input e.g. based on the SUSY Les Houches Accord.

file  SusyLesHouches  
contains information on SUSY parameters and particle data as specified by the SUSY Les Houches Accord.

file  TauDecays  
the main routines for handling tau lepton decays with helicity information.

file  TimeShower  
performs timelike final-state transverse-momentum-ordered shower evolution.

file  UserHooks  
Provides a way for a user to study the event at a few intermediate stages of evolution, to reject the event as a whole or to modify its cross-section weight. pythia8-8.1.80.orig/htmldoc/EventInformation.html0000644000175000017500000007524712217615312020157 0ustar sunsun Event Information

Event Information

The Info class collects various one-of-a-kind information, some relevant for all events and others for the current event. An object info is a public member of the Pythia class, so if you e.g. have declared Pythia pythia, the Info methods can be accessed by pythia.info.method(). Most of this is information that could also be obtained e.g. from the event record, but is here more directly available. It is primarily intended for processes generated internally in PYTHIA, but many of the methods would work also for events fed in via the Les Houches Accord.

List information

void Info::list()  
a listing of most of the information set for the current event.

The beams

int Info::idA()  
int Info::idB()  
the identities of the two beam particles.

double Info::pzA()  
double Info::pzB()  
the longitudinal momenta of the two beam particles.

double Info::eA()  
double Info::eB()  
the energies of the two beam particles.

double Info::mA()  
double Info::mB()  
the masses of the two beam particles.

double Info::eCM()  
double Info::s()  
the CM energy and its square for the two beams.

Initialization

bool Info::tooLowPTmin()  
normally false, but true if the proposed pTmin scale was too low in timelike or spacelike showers, or in multiparton interactions. In the former case the pTmin is raised to some minimal value, in the latter the initialization fails (it is impossible to obtain a minijet cross section bigger than the nondiffractive one by reducing pTmin).

The event type

string Info::name()  
int Info::code()  
the name and code of the process that occurred.

int Info::nFinal()  
the number of final-state partons in the hard process.

bool Info::isResolved()  
are beam particles resolved, i.e. were PDF's used for the process?

bool Info::isDiffractiveA()  
bool Info::isDiffractiveB()  
is either beam diffractively excited?

bool Info::isDiffractiveC()  
is there central diffraction (a.k.a. double Pomeron exchange)?

bool Info::isNonDiffractive()  
is the process the SoftQCD:nonDiffractive one, i.e. corresponding to the full inelastic nondiffractive part of the total cross section. (Note that a hard process, say Z^0 production, normally is nondiffractive, but this is not what we aim at here, and so the method would return false, unless the Z^0 had been generated as part of the MPI machinery for the SoftQCD:nonDiffractive component.)

bool Info::isMinBias()  
the same as above, retained for backwards compatibility, but to be removed in PYTHIA 8.2.

bool Info::isLHA()  
has the process been generated from external Les Houches Accord information?

bool Info::atEndOfFile()  
true if a linked Les Houches class refuses to return any further events, presumably because it has reached the end of the file from which events have been read in.

bool Info::hasSub()  
does the process have a subprocess classification? Currently only true for nondiffractive and Les Houches events, where it allows the hardest collision to be identified.

string Info::nameSub()  
int Info::codeSub()  
int Info::nFinalSub()  
the name, code and number of final-state partons in the subprocess that occurred when hasSub() is true. For a minimum-bias event the code would always be 101, while codeSub() would vary depending on the actual hardest interaction, e.g. 111 for g g -> g g. For a Les Houches event the code would always be 9999, while codeSub() would be the external user-defined classification code. The methods below would also provide information for such particular subcollisions.

Hard process initiators

The methods in this sections refer to the two initial partons of the hard 2 -> n process (diffraction excluded; see below).

int Info::id1()  
int Info::id2()  
the identities of the two partons coming in to the hard process.

double Info::x1()  
double Info::x2()  
x fractions of the two partons coming in to the hard process.

double Info::y()  
double Info::tau()  
rapidity and scaled mass-squared of the hard-process subsystem, as defined by the above x values.

bool Info::isValence1()  
bool Info::isValence2()  
true if the two hard incoming partons have been picked to belong to the valence piece of the parton-density distribution, else false. Should be interpreted with caution. Information is not set if you switch off parton-level processing.

Hard process parton densities and scales

The methods in this section refer to the partons for which parton densities have been defined, in order to calculate the cross section of the hard process (diffraction excluded; see below).

These partons would normally agree with the ones above, the initiators of the 2 -> n process, but it does not have to be so. Currently the one counterexample is POWHEG events [Ali10]. Here the original hard process could be 2 -> (n-1). The NLO machinery at times would add an initial-state branching to give a 2 -> n process with a changed initial state. In that case the values in this section refer to the original 2 -> (n-1) state and the initiator ones above to the complete2 -> n process. The Info::list() printout will contain a warning in such cases.

For external events in the Les Houches format, the pdf information is obtained from the optional #pdf line. When this information is absent, the parton identities and x values agree with the initiator ones above, while the pdf values are unknown and therefore set to vanish. The alpha_s and alpha_em values are part of the compulsory information. The factorization and renormalization scales are both equated with the one compulsory scale value in the Les Houches standard, except when a #pdf line provides the factorization scale separately. If alpha_s, alpha_em or the compulsory scale value are negative at input then new values are defined as for internal processes.

int Info::id1pdf()  
int Info::id2pdf()  
the identities of the two partons for which parton density values are defined.

double Info::x1pdf()  
double Info::x2pdf()  
x fractions of the two partons for which parton density values are defined.

double Info::pdf1()  
double Info::pdf2()  
parton densities x*f(x,Q^2) evaluated for the two incoming partons; could be used e.g. for reweighting purposes in conjunction with the idpdf, xpdf and QFac methods. Events obtained from external programs or files may not contain this information and, if so, 0 is returned.

double Info::QFac()  
double Info::Q2Fac()  
the Q or Q^2 factorization scale at which the densities were evaluated.

double Info::alphaS()  
double Info::alphaEM()  
the alpha_strong and alpha_electromagnetic values used for the hard process.

double Info::QRen()  
double Info::Q2Ren()  
the Q or Q^2 renormalization scale at which alpha_strong and alpha_electromagnetic were evaluated.

double Info::scalup()  
returns the stored SCALUP value for Les Houches events, and else zero. It may agree with both the QFac() and QRen() values, as explained above. However, to repeat, should the input SCALUP scale be negative, separate positive factorization and renormalization scales are calculated and set as for internally generated events. Furthermore, when PDF info is supplied for the Les Houches event, the factorization scale is set by this PDF info (scalePDF), which can disagree with SCALUP.

Hard process kinematics

The methods in this section provide info on the kinematics of the hard processes, with special emphasis on 2 -> 2 (diffraction excluded; see below).

double Info::mHat()  
double Info::sHat()  
the invariant mass and its square for the hard process.

double Info::tHat()  
double Info::uHat()  
the remaining two Mandelstam variables; only defined for 2 -> 2 processes.

double Info::pTHat()  
double Info::pT2Hat()  
transverse momentum and its square in the rest frame of a 2 -> 2 processes.

double Info::m3Hat()  
double Info::m4Hat()  
the masses of the two outgoing particles in a 2 -> 2 processes.

double Info::thetaHat()  
double Info::phiHat()  
the polar and azimuthal scattering angles in the rest frame of a 2 -> 2 process.

Diffraction

Information on the primary elastic or diffractive process (A B -> A B, X1 B, A X2, X1 X2, A X B) can be obtained with the methods in the "Hard process kinematics" section above. The variables here obviously are s, t, u, ... rather than sHat, tHat, uHat, ..., but the method names remain to avoid unnecessary duplication. Most other methods are irrelevant for a primary elastic/diffractive process.

Central diffraction A B -> A X B is a 2 -> 3 process, and therefore most of the 2 -> 2 variables are no longer relevant. The tHat() and uHat() methods instead return the two t values at the A -> A and B -> B vertices, and pTHat() the average transverse momentum of the three outgoing "particles", while thetaHat() and phiHat() are undefined.

While the primary interaction does not contain a hard process, the diffractive subsystems can contain them, but need not. Specifically, double diffraction can contain two separate hard subprocesses, which breaks the methods above. Most of them have been expanded with an optional argument to address properties of diffractive subsystems. This argument can take four values:

  • 0 : default argument, used for normal nondiffractive events or the primary elastic/diffractive process (see above);
  • 1 : the X1 system in single diffraction A B -> X1 B or double diffraction A B -> X1 X2;
  • 2 : the X2 system in single diffraction A B -> A X2 or double diffraction A B -> X1 X2;
  • 3 : the X system in central diffraction A B -> A X B.
The argument is defined for all of the methods in the three sections above, "Hard process initiators", "Hard process parton densities and scales" and "Hard process kinematics", with the exception of the isValence methods. Also the four final methods of "The event type" section, the ...Sub() methods, take this argument. But recall that they will only provide meaningful answers, firstly if there is a system of the requested type, and secondly if there is a hard subprocess in this system. A simple check for this is that id1() has to be nonvanishing. The methods below this section do not currently provide information specific to diffractive subsystems, e.g. the MPI information is not bookkept in such cases.

Event weight and activity

double Info::weight()  
weight assigned to the current event. Is normally 1 and thus uninteresting. However, there are several cases where one may have nontrivial event weights. These weights must the be used e.g. when filling histograms.
(i) In the PhaseSpace:increaseMaximum = off default strategy, an event with a differential cross-section above the assumed one (in a given phase-space point) is assigned a weight correspondingly above unity. This should happen only very rarely, if at all, and so could normally be disregarded.
(ii) The User Hooks class offers the possibility to bias the selection of phase space points, which means that events come with a compensating weight, stored here.
(iii) For Les Houches events some strategies allow negative weights, which then after unweighting lead to events with weight -1. There are also Les Houches strategies where no unweighting is done, so events come with a weight. Specifically, for strategies +4 and -4, the event weight is in units of pb. (Internally in mb, but converted at output.)

double Info::weightSum()  
Sum of weights accumulated during the run. For unweighted events this agrees with the number of generated events. In order to obtain histograms normalized "per event", at the end of a run, histogram contents should be divided by this weight. (And additionally divided by the bin width.) Normalization to cross section also required multiplication by sigmaGen() below.

int Info::lhaStrategy()  
normally 0, but if Les Houches events are input then it gives the event weighting strategy, see Les Houches Accord.

int Info::nISR()  
int Info::nFSRinProc()  
int Info::nFSRinRes()  
the number of emissions in the initial-state showering, in the final-state showering excluding resonance decays, and in the final-state showering inside resonance decays, respectively.

double Info::pTmaxMPI()  
double Info::pTmaxISR()  
double Info::pTmaxFSR()  
Maximum pT scales set for MPI, ISR and FSR, given the process type and scale choice for the hard interactions. The actual evolution will run down from these scales.

double Info::pTnow()  
The current pT scale in the combined MPI, ISR and FSR evolution. Useful for classification in user hooks, but not once the event has been evolved.

double Info::mergingWeight()  
combined leading-order merging weight assigned to the current event, if tree-level multi-jet merging (i.e. CKKW-L or UMEPS merging) is attempted. If tree-level multi-jet merging is performed, all histograms should be filled with this weight, as discussed in CKKW-L Merging and UMEPS Merging.

double Info::mergingWeightNLO()  
combined NLO merging weight assigned to the current event, if NLO multi-jet merging (i.e. NL3 or UNLOPS merging) is attempted. If NLO multi-jet merging is performed, all histograms should be filled with this weight, as discussed in NLO Merging .

Multiparton interactions

As already noted, these methods do not make sense for diffractive topologies, and should not be used there. Partly this is physics, but mainly it is for technical reasons, e.g. that double diffraction involves two separate systems that would have to be bookkept as such.

double Info::a0MPI()  
The value of a0 when an x-dependent matter profile is used, MultipartonInteractions:bProfile = 4.

double Info::bMPI()  
The impact parameter b assumed for the current collision when multiparton interactions are simulated. Is not expressed in any physical size (like fm), but only rescaled so that the average should be unity for minimum-bias events (meaning less than that for events with hard processes).

double Info::enhanceMPI()  
The choice of impact parameter implies an enhancement or depletion of the rate of subsequent interactions, as given by this number. Again the average is normalized be unity for minimum-bias events (meaning more than that for events with hard processes).

int Info::nMPI()  
The number of hard interactions in the current event. Is 0 for elastic and diffractive events, and else at least 1, with more possible from multiparton interactions.

int Info::codeMPI(int i)  
double Info::pTMPI(int i)  
the process code and transverse momentum of the i'th subprocess, with i in the range from 0 to nMPI() - 1. The values for subprocess 0 is redundant with information already provided above.

int Info::iAMPI(int i)  
int Info::iBMPI(int i)  
are normally zero. However, if the i'th subprocess is a rescattering, i.e. either or both incoming partons come from the outgoing state of previous scatterings, they give the position in the event record of the outgoing-state parton that rescatters. iAMPI and iBMPI then denote partons coming from the first or second beam, respectively.

double Info::eMPI(int i)  
The enhancement or depletion of the rate of the i'th subprocess. Is primarily of interest for the MultipartonInteractions:bProfile = 4 option, where the size of the proton depends on the x values of the colliding partons. Note that eMPI(0) = enhanceMPI().

Cross sections

Here are the currently available methods related to the event sample as a whole, for the default value i = 0, and otherwise for the specific process code provided as argument. This is the number obtained with Info::code(), while the further subdivision given by Info::codeSub() is not bookkept. While continuously updated during the run, it is recommended only to study these properties at the end of the event generation, when the full statistics is available. The individual process results are not available if a second hard process has been chosen, but can be gleaned from the pythia.stat() output.

long Info::nTried(int i = 0)  
long Info::nSelected(int i = 0)  
long Info::nAccepted(int i = 0)  
the total number of tried phase-space points, selected hard processes and finally accepted events, summed over all allowed processes (i = 0) or for the given process. The first number is only intended for a study of the phase-space selection efficiency. The last two numbers usually only disagree if the user introduces some veto during the event-generation process; then the former is the number of acceptable events found by PYTHIA and the latter the number that also were approved by the user. If you set a second hard process there may also be a mismatch.

double Info::sigmaGen(int i = 0)  
double Info::sigmaErr(int i = 0)  
the estimated cross section and its estimated error, summed over all allowed processes (i = 0) or for the given process, in units of mb. The numbers refer to the accepted event sample above, i.e. after any user veto.

Loop counters

Mainly for internal/debug purposes, a number of loop counters from various parts of the program are stored in the Info class, so that one can keep track of how the event generation is progressing. This may be especially useful in the context of the User Hooks facility.

int Info::getCounter(int i)  
the method that gives you access to the value of the various loop counters.
argument i : the counter number you want to access:
argumentoption 0 - 9 : counters that refer to the run as a whole, i.e. are set 0 at the beginning of the run and then only can increase.
argumentoption 0 : the number of successful constructor calls for the Pythia class (can only be 0 or 1).
argumentoption 1 : the number of times a Pythia::init(...) call has been begun.
argumentoption 2 : the number of times a Pythia::init(...) call has been completed successfully.
argumentoption 3 : the number of times a Pythia::next() call has been begun.
argumentoption 4 : the number of times a Pythia::next() call has been completed successfully.
argumentoption 10 - 19 : counters that refer to each individual event, and are reset and updated in the top-level Pythia::next() method.
argumentoption 10 : the number of times the selection of a new hard process has been begun. Normally this should only happen once, unless a user veto is set to abort the current process and try a new one.
argumentoption 11 : the number of times the selection of a new hard process has been completed successfully.
argumentoption 12 : as 11, but additionally the process should survive any user veto and go on to the parton- and hadron-level stages.
argumentoption 13 : as 11, but additionally the process should survive the parton- and hadron-level stage and any user cuts.
argumentoption 14 : the number of times the loop over parton- and hadron-level processing has begun for a hard process. Is reset each time counter 12 above is reached.
argumentoption 15 : the number of times the above loop has successfully completed the parton-level step.
argumentoption 16 : the number of times the above loop has successfully completed the checks and user vetoes after the parton-level step.
argumentoption 17 : the number of times the above loop has successfully completed the hadron-level step.
argumentoption 18 : the number of times the above loop has successfully completed the checks and user vetoes after the hadron-level step.
argumentoption 20 - 39 : counters that refer to a local part of the individual event, and are reset at the beginning of this part.
argumentoption 20 : the current system being processed in PartonLevel::next(). Is almost always 1, but for double diffraction the two diffractive systems are 1 and 2, respectively.
argumentoption 21 : the number of times the processing of the current system (see above) has begun.
argumentoption 22 : the number of times a step has begun in the combined MPI/ISR/FSR evolution downwards in pT for the current system.
argumentoption 23 : the number of times MPI has been selected for the downwards step above.
argumentoption 24 : the number of times ISR has been selected for the downwards step above.
argumentoption 25 : the number of times FSR has been selected for the downwards step above.
argumentoption 26 : the number of times MPI has been accepted as the downwards step above, after the vetoes.
argumentoption 27 : the number of times ISR has been accepted as the downwards step above, after the vetoes.
argumentoption 28 : the number of times FSR has been accepted as the downwards step above, after the vetoes.
argumentoption 29 : the number of times a step has begun in the separate (optional) FSR evolution downwards in pT for the current system.
argumentoption 30 : the number of times FSR has been selected for the downwards step above.
argumentoption 31 : the number of times FSR has been accepted as the downwards step above, after the vetoes.
argumentoption 40 - 49 : counters that are unused (currently), and that therefore are free to use, with the help of the two methods below.

void Info::setCounter(int i, int value = 0)  
set the above counters to a given value. Only to be used by you for the unassigned counters 40 - 49.
argument i : the counter number, see above.
argument value (default = 0) : set the counter to this number; normally the default value is what you want.

void Info::addCounter(int i, int value = 0)  
increase the above counters by a given amount. Only to be used by you for the unassigned counters 40 - 49.
argument i : the counter number, see above.
argument value (default = 1) : increase the counter by this amount; normally the default value is what you want.

Parton shower history

The following methods are mainly intended for internal use, e.g. for matrix-element matching.

void Info::hasHistory(bool hasHistoryIn)  
bool Info::hasHistory()  
set/get knowledge whether the likely shower history of an event has been traced.

void Info::zNowISR(bool zNowIn)  
double Info::zNowISR()  
set/get value of z in latest ISR branching.

void Info::pT2NowISR(bool pT2NowIn)  
double Info::pT2NowISR()  
set/get value of pT^2 in latest ISR branching.

Header information

A simple string key/value store, mainly intended for accessing information that is stored in the header block of Les Houches Event (LHE) files. In principle, any LHAup derived class can set this header information, which can then be read out later. Although the naming convention is arbitrary, in practice, it is dictated by the XML-like format of LHE files, see Les Houches Accord for more details.

string Info::header(string key)  
return the header named key

vector <string> Info::headerKeys()  
return a vector of all header key names

void Info::setHeader(string key, string val)  
set the header named key with the contents of val pythia8-8.1.80.orig/htmldoc/AdvancedUsage.html0000644000175000017500000002570712217615312017356 0ustar sunsun Advanced Usage

Advanced Usage

On this page we collect information on a number of classes that the normal user would not encounter. There are cases where the information is essential, however, for instance to implement your own showers.

The subsystems

One aspect that complicates administration is that an event can contain several subsystems, each consisting of one MPI and its associated ISR and FSR. To first approximation these systems are assumed to evolve independently, but to second they are connected by the interleaved evolution, and potentially by rescattering effects. The partons of a given subsystem therefore do not have to be stored consecutively.

The PartonSystems class is primarily used to keep track of the current positions of all partons belonging to each system, represented by the index iPos for a parton stored in the event-record slot event[iPos]. With "all" we mean the currently defined two incoming partons, or none for a resonance decay, and the current set of outgoing partons, but with all ISR and FSR intermediate-state partons omitted. That is, it stores all partons that could be subject to some action in the next step of the combined MPI/ISR/FSR/BR description. As a special case, an outgoing parton is stored even if it undergoes a rescattering, and thus no longer belongs to the final state proper.

The partonSystems instance of PartonSystems class is a public member of the Pythia top-level class, but is also available as a pointer partonSystemsPtr in various PartonLevel classes, e.g. inside the current instances of the TimeShower and SpaceShower classes.

A number of PartonSystems methods can be used to set or get information on the subsystems:

  • clear() resets all the contents in preparation for the next event.
  • addSys() add a new (initially empty) subsystem to the current list and return its index iSys in the list, where index 0 is the hardest subcollision and so on.
  • sizeSys() the number of separate subsystems.
  • setInA(iSys, iPos), setInB(iSys, iPos) store position iPos of the incoming parton from beam A or beam B to the iSys'th subcollision. These values are 0 initially, and should so remain if there are no beams, such as in resonance decays.
  • addOut(iSys, iPos) store position iPos of a new outgoing parton in the iSys'th subcollision, by appending it at the end of the current vector, with beginning in slot 0.
  • setOut(iSys, iMem, iPos) store position iPos in the iMem'th slot in the vector of outgoing partons in the iSys'th subcollision. Here iMem must be in the range already constructed by addOut calls.
  • replace(iSys, iPosOld, iPosNew) replace the existing incoming or outgoing parton position iPosOld by iPosNew in the iSys'th subcollision.
  • setSHat(iSys, sHat) set the invariant squared mass sHat of the iSys'th subcollision.
  • hasInAB(iSys) true if an incoming parton has been set for beam A or beam B (and hence should have been set for both) in the iSys'th subcollision, else false.
  • getInA(iSys), getInB(iSys) the position iPos of the incoming parton from beam A or beam B to the iSys'th subcollision.
  • sizeOut(iSys) the number of outgoing partons in the iSys'th subcollision.
  • getOut(iSys, iMem) the position iPos of an outgoing parton in the iSys'th subcollision, with the iMem range limited by sizeOut(iSys). These partons are not guaranteed to appear in any particular order.
  • sizeAll(iSys) the total number of incoming and outgoing partons in the iSys'th subcollision.
  • getAll(iSys, iMem) the position iPos of an incoming or outgoing parton in the iSys'th subcollision. In case there are beams it gives same as getInA(iSys) and getInB(iSys) for indices 0 and 1, and thereafter agrees with getOut(iSys, iMem) offset two positions. If there are no beams it is identical with getOut(iSys, iMem).
  • getSHat(iSys) the invariant squared mass sHat of the iSys'th subcollision.
  • list() print a listing of all the system information, except for the sHat values.

New systems are created from the hard process and by the MPI, not from any of the other components. Both FSR and ISR modify the position of partons, however. Since an FSR or ISR branching typically implies a new state with one more parton than before, an outgoing parton must be added to the system. Furthermore, in a branching, several existing partons may also be moved to new slots, including the incoming beam ones. In a FSR 1 -> 2 branching it is irrelevant which parton position you let overwrite the existing slot and which is added to the end of the system.

The system information must be kept up-to-date. Both the MPI, ISR, FSR and BR descriptions make extensive use of the existing information. As an example, the introduction of primordial kT in the beam remnants will fail if the information on which final-state partons belong to which system is out-of-date. The introduction of rescattering as part of the MPI framework adds further complications, where an outgoing parton of one subsystem may be the incoming one of another system. This part of the code is still under development.

Currently the system information is kept throughout the continued history of the event. Specifically, resonance decays create new systems, appended to the existing ones. This could be useful during the hadronization stage, to collect the partons that belong to a resonance with preserved mass when a small string collapses to one particle, but is not yet used for that.

The beams

The different subsystems are tied together by them sharing the same initial beam particles, and thereby being restricted by energy-momentum and flavour conservation issues. The information stored in the two beam particles, here called beamA and beamB, is therefore as crucial to keep correct as the above subsystem list.

Both beam objects are of the BeamParticle class. Each such object contains a vector with the partons extracted from it. The number of such partons, beamX.size() (X = A or B), of course is the same as the above number of subsystems in the event record. (The two diverge at the BR step, where further beam remnants are added to the beams without corresponding to new subsystems.) The individual partons are accessed by an overloaded indexing operator to a vector of ResolvedParton objects. The iPos() property corresponds to the iPos one above, i.e. providing the position in the main event record of a parton. In particular, beamA[iSys].iPos() = partonSystemsPtr->getInA(iSys) and beamB[iSys].iPos() = partonSystemsPtr->getInB(iSys). Whereas thus the indices of the two incoming partons to a subsystem are stored in two places, the ones of the outgoing partons only appear in the system part of the PartonSystems class.

Just as the subsystems in PartonSystems must be updated, so must the information in the two BeamParticle's, e.g. with methodsbeamX[iSys].iPos( iPosIn) when an incoming parton is replaced by a new one in line iPosIn. Furthermore the new parton identity should be set by beamX[iSys].id( idIn) and the new x energy-momentum fraction by beamX[iSys].x( xIn). The three can be combined in one go by beamX[iSys].update( iPosIn, idIn, xIn).

To be specific, it is assumed that, at each step, the two incoming partons are moving along the +-z axis and are massless. Since the event is constructed in the c.m. frame of the incoming beams this implies that x = 2 E / E_cm. If the x values are not defined accordingly or not kept up-to-date the BR treatment will not conserve energy-momentum.

In return, the BeamParticle objects give access to some useful methods. The beamX.xf( id, x, Q2) returns the standard PDF weight x f_id(x, Q^2). More interestingly, beamX.xfISR( iSys, id, x, Q2) returns the modified weight required when several subsystems have to share the energy and flavours. Thus iSys is added as an extra argument, and the momentum already assigned to the other subsystems is not available for evolution, i.e. the maximal x is correspondingly smaller than unity. Also flavour issues are handled in a similar spirit.

An additional complication is that a parton can be either valence or sea, and in the latter case the BR treatment also distinguishes companion quarks, i.e. quark-antiquark pairs that are assumed to come from the same original g -> q qbar branching, whether perturbative or not. This can be queried either with the beamX[iSys].companion() method, for detailed information, or with the beamX[iSys].isValence(), beamX[iSys].isUnmatched() and beamX[iSys].isCompanion() methods for yes/no answers whether a parton is valence, unmatched sea or matched sea. This choice should affect the ISR evolution; e.g., a valence quark cannot be constructed back to come from a gluon.

To keep this info up-to-date, the beamX.pickValSeaComp() method should be called whenever a parton of a new flavour has been picked in the ISR backwards evolution, but not if the flavour has not been changed, since then one should not be allowed to switch back and forth between the same quark being considered as valence or as sea. Since the pickValSeaComp() method makes use of the current parton-density values, it should be preceded by a call to beamX.xfISR( iSys, id, x, Q2), where the values in the call are the now finally accepted ones for the newly-found mother. (Such a call is likely to have been made before, during the evolution, but is not likely to be the most recent one, i.e. still in memory, and therefore had better be redone.) pythia8-8.1.80.orig/htmldoc/ExternalDecays.html0000644000175000017500000000642412217615312017572 0ustar sunsun External Decays

External Decays

DecayHandler is a base class for the external handling of decays. It is intended for normal particle decays, primarily B mesons and tau, and cannot be used to redirect decays of heavy resonances like t or Z^0. The user-written derived class is called if a pointer to it has been given with the pythia.decayPtr() method, where it also is specified which particles it will be called for. This particle information is accessible with the doExternalDecay() method.

There is only one pure virtual method in DecayHandler, to do the decay:

virtual bool DecayHandler::decay(vector<int>& idProd, vector<double>& mProd, vector<Vec4>& pProd, int iDec, const Event& event)  
where
argument idProd : is a list of particle PDG identity codes,
argument mProd : is a list of their respective masses (in GeV), and
argument pProd : is a list of their respective four-momenta.

At input, these vectors each have size one, so that idProd[0], mProd[0] and pProd[0] contain information on the particle that is to be decayed. At output, the vectors should have increased by the addition of all the decay products. Even if initially defined in the rest frame of the mother, the products should have been boosted so that their four-momenta add up to the pProd[0] of the decaying particle.

Should it be of interest to know the prehistory of the decaying particle, e.g. to set some helicity information affecting the decay angular distribution, the full event record is available read-only, with info in which slot iDec the decaying particle is stored.

The routine should return true if it managed the decay and false otherwise, in which case Pythia will try to do the decay itself. This e.g. means you can choose to do some decay channels yourself, and leave others to Pythia. To avoid double-counting, the channels you want to handle should be switched off in the Pythia particle database. In the beginning of the external decay method you should then return false with a probability given by the sum of the branching ratios for those channels you do not want to handle yourself.

Note that the decay vertex is always set by Pythia, and that B-Bbar oscillations have already been taken into account, if they were switched on. Thus idProd[0] may be the opposite of event[iDec].id(), where the latter provides the code at production.

A sample test program is available in main17.cc, providing a simple example of how to use this facility. pythia8-8.1.80.orig/htmldoc/UMEPSMerging.html0000644000175000017500000002306512217615312017061 0ustar sunsun UMEPS Merging

Unitarised Matrix Element + Parton Shower Merging

Pythia offers the possibility to use the unitarised matrix element + parton shower merging scheme, as presented in [Lon12]. Unitarised ME+PS merging (UMEPS) allows for a consistent inclusion of tree-level multi-parton matrix elements into Pythia, and prevents potential changes in the inclusive production cross section. This makes it theoretically more appealing than CKKW-L merging. As in CKKW-L, UMEPS merging requires the user to supply Les Houches Event File input.

UMEPS is different from other tree-level merging schemes in that it contains events with negative weights. These are generated by constructing parts of no-emission probabilities by reweighted higher-multiplicity samples [Lon12]. The main philosophy of UMEPS is "subtract what you add", meaning that in order to ensure the stability of the inclusive cross section, one has to counter the inclusion of additional tree-level matrix elements by "subtraction terms".

The scheme closely reflects how unitarity is achieved in a non-merged shower, and indeed explicitly enforces the cancellations that are implicitly happening in a non-merged shower. This makes very low merging scale values possible.

The usage of UMEPS is illustrated in the sample main program main86.cc, together with the input file main86.cmnd.

Unitarised merging is heavily indebted to CKKW-L merging, and shares many settings with CKKW-L. In particular,

         The hard process (Merging:Process)needs to be defined exactly as in CKKW-L (see Defining the hard process in the CKKW-L documentation).

         The merging scale value (Merging:TMS) has to be set.

         The maximal number of additional partons Merging:nJetMax has to be set.

UMEPS further shares the switches listed under the sections "Matrix element merging and HepMC output for RIVET" and "Further variables" in the CKKW-L documentation with CKKW-L merging. Also, all MergingHooks routines that allow for user interference in CKKW-L merging are also usable for UMEPS -- with the exception of a user-defined merging scale. Currently, UMEPS is only implemented for a merging scale defined by the minimal Pythia evolution pT value between sets of radiator, emitted and recoiler partons. This is no fundamental limitation of the method, and will possibly be lifted in the future. Since this merging scale definition is not completely obvious, UMEPS also shares the Merging:enforceCutOnLHE switch with CKKW-L. In this way, it is possible to use LHE files that are regularised only with weak cuts as input, while the merging machinery imposes the stronger merging scale cut automatically. This means that no merging scale implementation is required from the user side, but also means that it is the user's responsibility to ensure that the cuts used for generating input LHE files are always looser than the cut given by the merging scale value Merging:TMS.


UMEPS merging with main86.cc

The UMEPS procedure is illustrated in the sample main program main86.cc (with the input card main86.cmnd). This program produces HepMC events [Dob01], that can be histogrammed (e.g. using RIVET [Buc10]), or used as input for a detector simulation. If the user is not familiar with HepMC analysis tools, it is possible to instead use Pythia's histogramming routines. For this, remove the lines referring to HepMC, and histogram events as illustrated (for CKKW-L) for the histogram histPTFirstSum in main84.cc, i.e. using weight*normhepmc as weight.

In principle, no changes to main86.cc are necessary. Instead, all settings can be transferred to main86.cc through an input file. The input LHE files are also part of the (command line) input of main86.cc. Note that the sample program assumes that LHE file names are of the form name_tree_#nAdditionalJets.lhe. If you want to e.g. use the LHE files that are shipped with the Pythia distribution, you can execute main86.exe with the command

./main86.exe ./main86.cmnd ./w_production ./myhepmc.hepmc

Since main86.cc is currently the "front-end" for UMEPS merging, we will briefly discuss this sample program in the following.

Inputs

In its current form, main86.cc uses separate tree-level LHE files for different numbers of additional partons as input. If e.g. UMEPS merging for W-boson + up to two additional partons is to be performed, three LHE files (for W+zero, W+one, W+two partons) are required. The configurations in the input files should be regularised with inclusive (i.e. weak) cuts. The actual "merging scale cut" will be handled internally. If e.g. Merging:TMS = 15 is the desired merging scale value, it is acceptable to regularise the matrix element calculation for Higgs+jets events at the LHC with the loose cuts pTjet = 5 GeV, ΔRjetA jetB = 0.01 and QjetA jetB = 5 GeV.

All input settings are handed to main86.cc in the form of an input file. This input file has to contain

         The number of desired events (Main:numberOfEvents)

         The hard process (Merging:Process)

         The merging scale value (Merging:TMS)

         The maximal number of additional partons (Merging:nJetMax).

Other settings are of course allowed. However, please refrain from adding switches that are used to invoke other merging schemes (e.g. Merging:doKTMerging) into the input file, since this can cause problems.

Program flow

The sample program starts by estimating the cross section for samples with different jet multiplicities. For this, the switch Merging:doXSectionEstimate is invoked together with the merging scale definition of Merging:doUMEPSTree, which corresponds to the minimal Pythia evolution pT value. We will come back to the latter switch below. All showering, multiparton interactions and hadronisation is, for speed reasons, switched off when estimating the cross section, since the hard cross section estimate would not be influenced by the event evolution anyway.

After the hard cross sections are known (including the application of the merging scale cut), the first part of the UMEPS events is generated by using the following switch.

flag  Merging:doUMEPSTree   (default = off)
Reweight events according to the UMEPS prescription for tree-level configurations.

The weight generated by the UMEPS procedure can be accessed by using the function double Info::mergingWeight(). When printing (or histogramming) merged events, this weight, multiplied with the estimated cross section for the current sample, should be used as event weight (or to fill histogram bins).

After this first part is complete, the outcome is an addition of reweighted tree-level samples. To restore the inclusive cross section (i.e. that the cross section after merging corresponds to the cross section of the hard process, without any additional jets), it is necessary to subtract samples. Parton shower unitarity leads to the conclusion that "resolved" and "unresolved" corrections always cancel between states that contain an additional resolved jet, and states in which we "integrate over" the phase space of the additional jet. main86.cc makes this cancellation explicit by producing (correctly weighted) counter events by switching on

flag  Merging:doUMEPSSubt   (default = off)
Reweight events according to the UMEPS prescription of reweighted, integrated configurations. Please note that, in order for this to work smoothly, the switch Merging:doUMEPSTree has to be turned off.

The integration is achieved internally, and the number of desired integrations (which is always one for UMEPS counter events) is set by

mode  Merging:nRecluster   (default = 0; minimum = 0)
Number of hard partons to integrate out in the UMEPS procedure.

Again, the weight generated by the UMEPS procedure can be accessed by using the function double Info::mergingWeight(). This weight, multiplied with the cross section of the current sample, and multiplied by -1, should then be used as event weight (or to fill histogram bins).

Before returning, main86.cc prints the merged cross section after UMEPS merging. pythia8-8.1.80.orig/htmldoc/JetMatching.html0000644000175000017500000007065712217615312017065 0ustar sunsun Jet Matching

Jet Matching

This manual page describes the parton-jet matching interfaces for PYTHIA8. In this approach, usually referred to as MLM matching [Man02, Man07], the final jets after parton-shower evolution and jet clustering are matched to the original partons. The event is accepted if a reasonable match is found, and rejected if not. The rejection step in an approximate way introduces a Sudakov form factor on to the hard processes. Notably the parton shower should not generate an emission that would doublecount hard activity already included in the matrix-element description. Within this general ansatz, different technical solutions can be adopted. We provide two alternatives, one based on the algorithm used in ALPGEN [Man03], and another on the one used in Madgraph [Alw11], both reimplemented from scratch here. The main points of these two algorithms are outlined further down on this page.

We also allow for two alternative sources of external events, one in the ALPGEN native format and one in the Madgraph LHEF-based one. All four combinations of input format and matching style are implemented. In the following it is therefore important to keep the two aspects apart, whenever the ALPGEN and Madgraph labels are used.

Currently all the files of interest are located in the examples/ subdirectory:

  • JetMatching.h contains the machinery for the parton-jet matching, in the two JetMatchingAlpgen and JetMatchingMadgraph classes.
  • GeneratorInput.h contains three classes for the reading of ALPGEN event and parameter files, and one for the reading of Madgraph parameters.
  • CombineMatchingInput.h contains three classes that combine the reading of events with the matching of them.
  • main32.cc, main32.cmnd : a sample main program and card file showing the usage of the previous files/classes.

Event input source

External sources of partons are used in the parton-jet matching process. The source of the partons has been separated from the implementation of the matching algorithm. By default, PYTHIA8 contains a machinery to process Les Houches Event Files (LHEFs) as described on the Les Houches Accord and Beam Parameters pages. Madgraph5 adheres to this format, but also contains some further non-standardized information that can be used. The parsing of the native ALPGEN file format is described on the Alpgen Event Interface page.

Commonly, the source of external partons also contains information about how a particular type of matching algorithm should be employed. This information is handled by the AlpgenPar class for ALPGEN files, and MadgraphPar for LHEFs. The user can choose to set default matching parameters using the Alpgen:setMLM flag for ALPGEN files. For LHEFs, instead, the setting of default parameters is controlled with the JetMatching:setMad flag:

flag  JetMatching:setMad   (default = on)
When enabled, the merging parameters are set according to the values in the LHEF header. Specifically, the header must set the ickkw, xqcut, maxjetflavor and alpsfact values, and ickkw must be nonzero. Note that these labels are Madgraph-specific. For other programs with LHEF output, or for Madgraph files lacking this information, these parameters should be set by the user (or one can rely on the default values). The following parameters (described below) must then be specified:

  • JetMatching:doMerge = ickkw,
  • JetMatching:qCut = xqcut,
  • JetMatching:nQmatch = maxjetflavor,
  • JetMatching:clFact = alpsfact.
With this flag on, the values from the LHEF for these parameters take precedence over other values.

Jet Matching parameters

A class JetMatching, derived from UserHooks, is used to define the basic structure of a parton-jet matching algorithm. Two versions are implemented here, based on the FORTRAN code provided by the ALPGEN and Madgraph packages, respectively: JetMatchingAlpgen and JetMatchingMadgraph. The matching parameters are defined with the JetMatching:* keyword.

Scheme and Usage

flag  JetMatching:merge   (default = off)
Master switch to activate parton-jet matching. When off, all external events are accepted (unless they are rejected due to weighting or event processing problems).

mode  JetMatching:scheme   (default = 1; minimum = 1; maximum = 2)
The parton-jet MLM-style matching scheme.
option 1 : The one inspired by the Madgraph matching code, here implemented in the JetMatchingMadgraph class.
option 2 : The one inspired by the ALPGEN matching code, here implemented in the JetMatchingAlpgen class.

Jet algorithm

The choice of jet algorithm and associated parameters can be adjusted with the settings below. The PYTHIA8 internal CellJet and SlowJet routines are used for jet finding. See the Event Analysis page for more details.

mode  JetMatching:jetAlgorithm   (default = 1; minimum = 1; maximum = 2)
The choice of jet algorithm to use when merging against hard partons. Currently, only SlowJet with the kT algorithm (and useStandardR = false) is supported for Madgraph-style matching, while there is full freedom for the ALPGEN-style matching.
option 1 : The CellJet cone algorithm.
option 2 : The SlowJet clustering algorithm.

mode  JetMatching:slowJetPower   (default = -1; minimum = -1; maximum = 1)
The power to use in the SlowJet algorithm.
option -1 : The anti-kT algorithm.
option 0 : The Cambridge/Aachen algorithm.
option 1 : The kT algorithm.

mode  JetMatching:nEta   (default = 100; minimum = 50)
Specific to the CellJet algorithm, the number of bins in pseudorapidity.

mode  JetMatching:nPhi   (default = 60; minimum = 30)
Specific to the CellJet algorithm, the number of bins in phi.

parm  JetMatching:eTseed   (default = 1.5; minimum = 0.0)
Specific to the CellJet algorithm, the minimum eT for a cell to be acceptable as the trial center of a jet.

parm  JetMatching:eTthreshold   (default = 0.1)
Specific to the CellJet algorithm, cells with eT < eTthreshold are completely neglected by the jet algorithm.

Merging parameters

The following options are the three main parameters for the merging procedure. Although here they are in principle free parameters, they should be heavily influenced by the hard process generation cuts. These values can be set automatically based on the information in the ALPGEN file or LHEF.

parm  JetMatching:eTjetMin   (default = 20.0; minimum = 5.0)
For the CellJet algorithm, this gives the minimum transverse energy inside a cone for a jet to be accepted. For the SlowJet algorithm, this is instead the minimum transverse momentum required for a cluster to be accepted as a jet. For Madgraph-style matching, this parameter should match the qCut parameter described later.

parm  JetMatching:coneRadius   (default = 0.7; minimum = 0.1)
For the CellJet algorithm, this gives the size of the cone in (eta, phi) space drawn around the geometric center of the jet. For the SlowJet algorithm, this gives the R parameter.

parm  JetMatching:etaJetMax   (default = 2.5; minimum = 0.1)
For both jet algorithms, this defines the maximum pseudorapidity that the detector is assumed to cover. In this context, however, it is tied to the phase space region in which partons have been generated. For the Alpgen-style matching, particles within etaJetMax + coneRadius are passed to the jet algorithm, with only jets within etaJetMax retained in the merging. For the Madgraph-style matching, only particles within etaJetMax are used.

Exclusive mode

The following settings determine whether clustered jets which do not match an original hard parton are allowed. They are typically permitted in the highest jet multiplicity sample, where the parton shower may produce extra hard jets, without risk of double counting. Any extra jet produced by the shower must be softer than any matched light jet, or else the event is vetoed.

mode  JetMatching:exclusive   (default = 2; minimum = 0; maximum = 2)
Exclusive or inclusive merging.
option 0 : The merging is run in inclusive mode. All partons must match jets, but additional jets are allowed, provided they are not harder than the matched jets.
option 1 : The merging is run in exclusive mode. All partons must match jets, and no additional jets are allowed.
option 2 : If nJet < nJetMax, then the merging is run in exclusive mode, otherwise it is run in inclusive mode. For Madgraph-style matching, this is checked on an event-by-event basis, which is useful when an LHEF contains a "soup" of partonic multiplicities. If nJetMax < 0 or nJet < 0, then the algorithm defaults to exclusive mode.

mode  JetMatching:nJet   (default = -1; minimum = -1)
When JetMatching:exclusive = 2, nJet indicates the minimum number of additional light jets in the incoming process. This value may be set automatically.

mode  JetMatching:nJetMax   (default = -1; minimum = -1)
When JetMatching:exclusive = 2, nJetMax is used to indicate the maximum number of jets that will be matched.

Jet matching

The following parameters control the criteria for matching a clustered jet to a hard parton.

mode  JetMatching:jetAllow   (default = 1; minimum = 1; maximum = 2)
Controls which particles are clustered by the jet algorithm.
option 1 : This option explicitly disallows top quarks, leptons and photons. All other particle types are passed to the jet algorithm.
option 2 : No extra particles are disallowed.

Alpgen-specific parameters

mode  JetMatching:jetMatch   (default = 1; minimum = 1; maximum = 2)
Criteria for matching a clustered jet to a parton.
option 1 : This option can be used with both the CellJet and SlowJet algorithms. The delta R between each parton and jet is taken, and the minimal value compared against coneMatchLight * coneRadius for light jets or coneMatchHeavy * coneRadiusHeavy for heavy jets. Note that by default coneRadiusHeavy = coneRadius, see below. If below this value, the parton and jet are considered to match. With CellJet, the delta R measure is in (eta, phi), while with SlowJet it is in (y, phi).
option 2 : This option can only be used with the SlowJet algorithm. The hard partons are inserted into the parton level event as "ghost" particles, but at the correct (y, phi) position. If this particle is then clustered into a jet, it is considered a match.

parm  JetMatching:coneMatchLight   (default = 1.5; minimum = 0.1)
The coneMatchLight parameter used when JetMatching:jetMatch = 1.

parm  JetMatching:coneRadiusHeavy   (default = -1.0)
The coneRadiusHeavy parameter used when JetMatching:jetMatch = 1. When assigned a negative value, the value of JetMatching:coneRadius is used.

parm  JetMatching:coneMatchHeavy   (default = 1.0; minimum = 0.1)
The coneMatchHeavy parameter used when JetMatching:jetMatch = 1.

Madgraph-specific parameters

parm  JetMatching:qCut   (default = 10.0; minimum = 0.0)
kT scale for merging shower products into jets.

mode  JetMatching:nQmatch   (default = 5; minimum = 3; maximum = 6)
Controls the treatment of heavy quarks.
option 5 : All quarks (except top) are treated as light quarks for matching.
option 4 : Bottom quarks are treated separately. Currently, they are unmatched.

parm  JetMatching:clFact   (default = 1.0)
The clFact parameter determines how jet-to parton matching is done. A match is defined as a squared cluster scale that equals:
|clFact| * qCut for inclusive mode,
|clFact| * max(qCut,min(pT(parton))) for exclusive mode, clFact ≥ 0, or
|clFact| * min(kT(parton)) for exclusive mode, clFact < 0.

Alpgen-style parton-jet matching and merging

This section describes the Alpgen-style MLM merging algorithm for PYTHIA8. The most common reference to the algorithm is [Man02]. In many respects, however, the implementation provided in the ALPGEN package should be considered the official description of the MLM merging procedure. Although designed primarily to work with events generated with ALPGEN, it can in principle also be used with events from a different source. This should not be done without thought, however, and it is up to the user to understand the details of the algorithm and the implications of using a different hard process generator.

First, either the CellJet or SlowJet jet algorithm is chosen. Both of these algorithms have an R and an etaMax parameter. In addition, CellJet has an eTmin and SlowJet has a pTmin parameter. These are the primary three parameters of the merging procedure, and in practice are set dependent on the cuts applied to the matrix element (ME) generation. We stress that the merging procedure is not tied to the geometry of a specific physical detector, but only to the match between the original partons and the resulting jets, using standard jet algorithms in the phase space region where partons have been generated.

ME samples with different jet multiplicities are run through the event generator, and the generation interrupted after parton showers have been applied, but before resonance decays and beam remnants have been processed. Note in particular that top quarks will not yet be decayed, which may lead to slight differences with the PYTHIA 6 interface included with the ALPGEN package. In what follows, the hardness measure of jets/partons is taken to be eT when CellJet is used and pT when SlowJet is used. The hard system (ignoring all MPI systems) is then analysed:

  • The particles in the original matrix element process are sorted into light partons, heavy partons and other particles. For backwards compatibility, a light parton is defined as the set (d, u, s, c, b, g) with zero mass. A heavy parton is defined as the set (c, b, t) with non-zero mass.
  • All particles not originating from the heavy partons or other particles are passed to the jet algorithm and clustered.
  • Clustered jets are matched to the light partons in the original ME process. There are two different methods which can be used:
    • Method 1: The following is done for each parton, in order of decreasing hardness. The delta R between the parton and all jets is calculated and the smallest value taken. If this is less than the jet R parameter, possibly multiplied by a constant, the jet and parton are considered to match, and the jet is removed from further consideration. Note that for CellJet the delta R measure is in (eta, phi), while for SlowJet, it is in (y, phi).
    • Method 2: This method is only possible when using the SlowJet algorithm. Before the clustering is performed, extremely soft "ghost" particles are added to the event at the (y, phi) coordinates of the original matrix element partons. If such a particle is clustered into a jet, the parton and jet are considered to match. The idea of "ghost" particles was originally introduced by FastJet as a way to measure jet areas [Cac06] and should not affect clustering with an infrared-safe jet algorithm.
  • If there is a light ME parton remaining which has not been matched to a jet, then the event is vetoed. If all ME partons have been matched to a jet, but there are still some extra jets remaining, then two options are possible:
    • Exclusive mode: the event is vetoed. This is typically used when there are ME samples with higher jet multiplicities, which would fill in the extra jets.
    • Inclusive mode: the event is retained if the extra jets are softer than the softest matched jet. This is typically used when there is no ME sample with higher jet multiplicity, so the parton shower should be allowed to give extra jets.
  • All particles originating from the heavy partons are passed to the jet algorithm and clustered.
  • The clustered jets are again matched to the original partons, but there is no requirement for a match to be present; all matched jets are immediately discarded. The matching procedure is much the same as for light partons, but with two differences when delta R matching is used. First, a different R parameter than that used by the jet algorithm may optionally be given. Second, all jets that are within the given radius of the parton are matched, not just the one with the smallest delta R measure. If there are still extra jets remaining then in exclusive mode the event is immediately vetoed, while in inclusive mode the event is retained if the extra jets are softer than the softest light matched jet.

Some different options are provided, specified further above in the parameters section. These are set so that, by default, the algorithm closely follows the official MLM interface provided in the ALPGEN package.

All vetoing of events is done through the usual User Hooks machinery, and is therefore already taken into account in the cross section. In the output from Pythia::stat(), the difference between the "Selected" and "Accepted" columns gives the number of events that have not survived the vetoing procedure. It is still the responsibility of the user to add together the results from runs with different jet multiplicities. In the simplest case, when ALPGEN input is used and the hard process parameters are used to guide the merging procedure, it is enough to set the JetMatching:nJetMax parameter.

Madgraph-style parton-jet Merging and Matching

This section describes the Madgraph-style parton-jet matching algorithm for PYTHIA8.

First, the kT jet algorithm is applied using the PYTHIA8 SlowJet implementation. The useStandardR = false is used, ie. the (delta R)^2 separation is defined as 2 (cosh(delta y) - cos(delta phi)) rather than the more common (delta y)^2 + delta phi)^2. The R, etaMax, and a pTmin parameters are specified. By default, R = 1 and pTmin = qCut . It is not recommended to change these. These should match the algorithm parameters used in the Madgraph Matrix Element (ME) generation.

ME samples with different jet multiplicities are run through the event generator, and the generation is interrupted after parton showers have been applied, but before resonance decays and beam remnants have been processed. In what follows, the hardness measure of jets/partons is taken to be kT relative to qCut. The hard system (ignoring all MPI systems) is analyzed:

  • The hard partons in the original matrix element process, provided by the LHEF, are sorted into light partons, heavy partons and other particles. A heavy parton is defined by the JetMatching:nQmatch or by the maxjetflavor value in the LHEF. nQmatch refers to the absolute value of the quark PDG identity code.
  • All partons arising from the parton shower are sorted based on their motherhood. A showered parton arising from a heavy parton or "other" parton classified in the previous step is not passed to the jet algorithm. All other partons are clustered into light jets.
  • It is checked whether there are "too few" or "too many" light jets. If the number of light jets is less than the number of light partons defined by nQmatch, the event is vetoed. If the number is larger, the event is vetoed only in exclusive mode (defined below).
  • In exclusive mode, the number of jets matches the number of light partons. In inclusive mode, the jets are re-clustered until the number of jets equals the number of light partons. Next, each light hard parton is clustered, one at a time, with the jets until a match is found. A match is defined as a squared cluster scale that equals:
    • |clFact| * qCut for inclusive mode,
    • |clFact| * max(qCut,min(pT(parton))) for exclusive mode, clFact ≥ 0, or
    • |clFact| * min(kT(parton)) for exclusive mode, clFact < 0.
    If no match is found, the event is vetoed. When a parton matches a jet, the jet is removed from the collection, and the process continues. The process terminates when all partons are matched to a jet, or a parton is unmatched.
  • All particles originating from the heavy partons are not used.
In exclusive mode, it is expected that ME samples with higher parton multiplicity are available to fill the phase space above qCut. The inclusive mode is when there are no such samples, and the parton shower is used to fill the phase space.

Some different options are provided, specified further above. These are set so that, by default, the algorithm closely follows the FORTRAN interface ME2Pythia provided in the Madgraph package.

All vetoing of events is done through the usual User Hooks machinery, and is therefore already taken into account in the cross section. In the output from Pythia::stat(), the difference between the "Selected" and "Accepted" columns gives the number of events that have not survived the vetoing procedure. It is still the responsibility of the user to add together the results from runs with different jet multiplicities. In the simplest case, when the hard process parameters are used to guide the merging procedure, events will be matched in the exclusive mode.

A note on combining UserHooks

As have been noted above, the matching is implemented using classes derived from the UserHooks class, thereby gaining access to the event generation process at the relevant locations. For native ALPGEN files, which do not adhere to the Les Houches standards, it is also necessary to intervene with a UserHooks-derived AlpgenHooks to handle the extraction and setting of relevant extra information.

One must then combine multiple UserHooks classes, such that the functionality of both is present. A prerequisite is that the different UserHooks classes should be declared with virtual inheritance, e.g.

  class JetMatching : virtual public UserHooks
Without this option, when combining two UserHooks-derived classes, two copies of the base UserHooks class would be created, leading to ambiguities.

The two first classes in CombineMatchingInput.h combine ALPGEN input with the two different matching schemes, e.g. for the first

class JetMatchingAlpgenInputAlpgen : public AlpgenHooks, 
  public JetMatchingAlpgen {
public:
  // Constructor and destructor.
  JetMatchingAlpgenInputAlpgen(Pythia& pythia) : AlpgenHooks(pythia), 
    JetMatchingAlpgen() { }
  ~JetMatchingAlpgenInputAlpgen() {}
  // Initialisation.
  virtual bool initAfterBeams() {
    if (!AlpgenHooks::initAfterBeams()) return false;
    if (!JetMatchingAlpgen::initAfterBeams()) return false;
    return true;
  }
  // Process level vetos.
  virtual bool canVetoProcessLevel() { 
    return JetMatchingAlpgen::canVetoProcessLevel();    
  }
  ....
};
This class inherits from both AlpgenHooks and JetMatchingAlpgen. Any functions which are present in both classes should be overridden with a function that calls the different parent methods in the desired order. In the above example, the only shared methods are the constructor and initAfterBeams(). pythia8-8.1.80.orig/htmldoc/ResonanceDecays.html0000644000175000017500000004405612217615311017727 0ustar sunsun Resonance Decays

Resonance Decays

The ResonanceDecays class performs the sequential decays of all resonances formed in the hard process. Note the important distinction between "resonances" and other "particles" made in PYTHIA.
  • The list of resonances contains gamma^*/Z^0, W^+-, top, the Higgs, and essentially all new particles of Beyond-the-Standard-Model physics: further Higgs bosons, sfermions, gauginos, techniparticles, and so on. The partial widths to different decay channels are perturbatively calculable, given the parameters of the respective model, and branching ratios may be allowed to vary across a (reasonably broad) resonance peak. Usually resonances are short-lived, and therefore it makes sense to consider their decays immediately after the primary hard process has been set up. Furthermore, in several cases the decay angular distributions are encoded as part of the specific process, e.g. the W decays differently in f fbar -> W^+-, f fbar -> W^+ W^- and h^0 -> W^+ W^- . All of these particles are (in PYTHIA) only produced as part of the hard process itself, i.e. they are not produced in showers or hadronization processes. Therefore the restriction to specific decay channels can be consistently taken into account as a corresponding reduction in the cross section of a process. Finally, note that all of these resonances have an on-shell mass above 20 GeV, with the exception of some hypothetical weakly interacting and stable particles such as the gravitino.
  • The other particles include normal hadrons and the Standard-Model leptons, including the tau^+-. These can be produced in the normal hadronization and decay description, which involve unknown nonperturbative parameters and multistep chains that cannot be predicted beforehand: a hard process like g g -> g g can develop a shower with a g -> b bbar branching, where the b hadronizes to a B^0bar that oscillates to a B^0 that decays to a tau^+. Therefore any change of branching ratios - most of which are determined from data rather than from first principles anyway - will not be taken into account in the cross section of a process. Exceptions exist, but most particles in this class are made to decay isotropically. Finally, note that all of these particles have a mass below 20 GeV.
There is one ambiguous case in this classification, namely the photon. The gamma^*/Z^0 combination contains a low-mass peak when produced in a hard process. On the other hand, photons can participate in shower evolution, and therefore a photon originally assumed massless can be assigned an arbitrarily high mass when it is allowed to branch into a fermion pair. In some cases this could lead to double-counting, e.g. between processes such as f fbar -> (gamma^*/Z^0) (gamma^*/Z^0), f fbar -> (gamma^*/Z^0) gamma and f fbar -> gamma gamma. Here it make sense to limit the lower mass allowed for the gamma^*/Z^0 combination, in 23:mMin, to be the same as the upper limit allowed for an off-shell photon in the shower evolution, in TimeShower:mMaxGamma. By default this matching is done at 10 GeV.

In spite of the above-mentioned differences, the resonances and the other particles are all stored in one common particle data table, so as to offer a uniform interface to setting and getting properties such as name, mass, charge and decay modes, also for the particle properties in the event record. Some methods are specific to resonances, however, in particular for the calculation of partial widths and thereby of branching ratio. For resonances these can be calculated dynamically, set up at initialization for the nominal mass and then updated to the current mass when these are picked according to a Breit-Wigner resonance shape.

Resonance Decays and Cross Sections

As already hinted above, you have the possibility to set the allowed decay channels of resonances, see Particle Data Scheme description. For instance, if you study the process q qbar -> H^0 Z^0 you could specify that the Z^0 should decay only to lepton pairs, the H^0 only to W^+ W^-, the W^+ only to a muon and a neutrino, while the W^- can decay to anything. Unfortunately there are limits to the flexibility: you cannot set a resonance to have different properties in different places of a process, e.g. if instead H^0 -> Z^0 Z^0 in the above process then the three Z^0's would all obey the same rules.

The restrictions on the allowed final states of a process is directly reflected in the cross section of it. That is, if some final states are excluded then the cross section is reduced accordingly. Such restrictions are built up recursively in cases of sequential decay chains. The restrictions are also reflected in the compositions of those events that actually do get to be generated. For instance, the relative rates of H^0 -> W^+ W^- and H^0 -> Z^0 Z^0 are shifted when the allowed sets of W^+- and Z^0 decay channels are changed.

We remind that only those particles that Pythia treat as resonances enjoy this property, and only those that are considered as part of the hard process and its associated resonance decays.

There is one key restriction on resonances:

parm  ResonanceWidths:minWidth   (default = 1e-20; minimum = 1e-30)
Minimal allowed width of a resonance, in GeV. If the width falls below this number the resonance is considered stable and will not be allowed to decay. This is mainly intended as a technical parameter, to avoid disasters in cases where no open decay channels exists at all. It could be used for real-life decisions as well, however, but then typically would have to be much bigger than the default value. Special caution would be needed if coloured resonance particles were made stable, since the program would not necessarily know how to hadronize them, and therefore fail at that stage.

In spite of this technical parameter choice, it is possible to set a lifetime for a resonance, and thereby to obtain displaced vertices. If a resonance is allowed to decay it will do so, irrespective of the location of the decay vertex. This is unlike normal particle decays, where it is possible to define some region around the primary vertex within which all decays should happen, with particles leaving that region considered stable. The logic is that resonances as a rule are too short-lived for secondary vertices, so if you pick a scenario with a long-lived but unstable resonance it is because you want to study secondary vertices. How to interface those decays to a detector simulation program then is another story, to be solved separately. Do note that a special treatment is needed for coloured long-lived resonances, that form R-hadrons, and where charge and flavour may change between the production and decay vertices.

Special properties and methods for resonances

The method ParticleData::isResonance(id) allows you to query whether a given particle species is considered a resonance or not. You can also change the default value of this flag in the normal way, e.g. pythia.readString("id:isResonance = true").

An option with a forced width can be set with the id:doForceWidth flag as above, and queried with ParticleData::doForceWidth(id). It is by default off, and should normally so remain. If switched on then the width stored in id:mWidth is strictly used to describe the Breit-Wigner of the resonance. This is unlike the normal behaviour of standard resonances such as the Z^0, W^+-, t or h^0, which have explicit decay-widths formulae encoded, in classes derived from the ResonanceWidths base class. These formulae are used, e.g., to derive all the Higgs partial widths as a function of the Higgs mass you choose, and at initialization overwrites the existing total width value. The reason for forcing the width to another value specified by you would normally more have to do with experimental issues than with physics ones, e.g. how sensitive your detector would be to changes in the Higgs width by a factor of two. A warning is that such a rescaling could modify the cross section of a process correspondingly for some processes, while leaving it (essentially) unchanged for others (as would seem most logical), depending on how these were encoded. A further warning is that, if you use this facility for Z^0 or Z'^0 with gamma^*/Z^0 or gamma^*/Z^0/Z'^0 interference on, then also the handling of this interference is questionable. So, if you need to use the width-rescaling option, be extremely cautious.

If a resonance does not have a class of its own, with hardcoded equations for all relevant partial widths, then a simpler object will be created at initialization. This object will take the total width and branching ratios as is (with the optional variations explained in the next section), and thus the rescaling approach brings no further freedom.

Mainly for internal usage, the ParticleData contain some special methods that are only meaningful for resonances:

  • resInit(...) to initialize a resonance, possibly including a recalculation of the nominal width to match the nominal mass;
  • resWidth(...) to calculate the partial and total widths at the currently selected mass;
  • resWidthOpen(...) to calculate the partial and total widths of those channels left open by user switches, at the currently selected mass;
  • resWidthStore(...) to calculate the partial and total widths of those channels left open by user switches, at the currently selected mass, and store those as input for a subsequent selection of decay channel;
  • resOpenFrac(...) to return the fraction of the total width that is open by the decay channel selection made by users (based on the choice of onMode for the various decay channels, recursively calculated for sequential decays);
  • resWidthRescaleFactor(...) returns the factor by which the internally calculated PYTHIA width has to be rescaled to give the user-enforced width;
  • resWidthChan(...) to return the width for one particular channel (currently only used for Higgs decays, to obtain instate coupling from outstate width).
These methods actually provide an interface to the classes derived from the ResonanceWidths base class, to describe various resonances.

Modes for Matrix Element Processing

The meMode() value for a decay mode is used to specify nonisotropic decays or the conversion of a parton list into a set of hadrons in some channels of normal particles. For resonances it can also take a third function, namely to describe how the branching ratios and widths of a resonance should be rescaled as a function of the current mass of the decaying resonance. The rules are especially useful when new channels are added to an existing particle, or a completely new resonance added.
  • 0 : channels for which hardcoded partial-width expressions are expected to exist in the derived class of the respective resonance. Should no such code exist then the partial width defaults to zero.
  • 1 - 99 : same as 0, but normally not used for resonances.
  • 100 : calculate the partial width of the channel from its stored branching ratio times the stored total width. This value remains unchanged when the resonance fluctuates in mass. Specifically there are no threshold corrections. That is, if the resonance fluctuates down in mass, to below the nominal threshold, it is assumed that one of the daughters could also fluctuate down to keep the channel open. (If not, there may be problems later on.)
  • 101 : calculate the partial width of the channel from its stored branching ratio times the stored total width. Multiply by a step threshold, i.e. the channel is switched off when the sum of the daughter on-shell masses is above the current mother mass.
  • 102 : calculate the partial width of the channel from its stored branching ratio times the stored total width. Multiply by a smooth threshold factor beta = sqrt( (1 - m_1^2/m_2 - m_2^2/m^2)^2 - 4 m_1^2 m_2^2/m^4) for two-body decays and sqrt(1 - Sum_i m_i / m) for multibody ones. The former correctly encodes the size of the phase space but misses out on any nontrivial matrix-element behaviour, while the latter obviously is a very crude simplification of the correct phase-space expression. Specifically, it is thereby assumed that the stored branching ratio and total width did not take into account such a factor.
  • 103 : use the same kind of behaviour and threshold factor as for 102 above, but assume that such a threshold factor has been used when the default branching ratio and total width were calculated, so that one should additionally divide by the on-shell threshold factor. Specifically, this will give back the stored branching ratios for on-shell mass, unlike the 102 option. To avoid division by zero, or in general unreasonably big rescaling factors, a lower limit minThreshold (see below) on the value of the on-shell threshold factor is imposed. (In cases where a big rescaling is intentional, code 102 would be more appropriate.)

parm  ResonanceWidths:minThreshold   (default = 0.1; minimum = 0.01)
Used uniquely for meMode = 103 to set the minimal value assumed for the threshold factor, sqrt( (1 - m_1^2/m_2 - m_2^2/m^2)^2 - 4 m_1^2 m_2^2/m^4) for two-body decays and sqrt(1 - Sum_i m_i / m) for multibody ones. Thus the inverse of this number sets an upper limit for how much the partial width of a channel can increase from the on-shell value to the value for asymptotically large resonance masses. Is mainly intended as a safety measure, to avoid unintentionally large rescalings.

All of these meMode's may coexist for the same resonance. This would be the case e.g. if you want to add a few new channels to an already existing resonance, where the old partial widths come hardcoded while the new ones are read in from an external file. The typical example would be an MSSM Higgs sector, where partial widths to SM particles are already encoded, meMode = 0, while decay rates to sparticles are read in from some external calculation and maybe would be best approximated by using meMode = 103. Indeed the default particle table in PYTHIA uses 103 for all channels that are expected to be provided by external input.

Some further clarification may be useful. At initialization the existing total width and on-shell branching ratios will be updated. For channels with meMode < 100 the originally stored branching ratios are irrelevant, since the existing code will anyway be used to calculate the partial widths from scratch. For channels with meMode = 100 or bigger, instead the stored branching ratio is used together with the originally stored total width to define the correct on-shell partial width. The sum of partial widths then gives the new total width, and from there new branching ratios are defined.

In these operations the original sum of branching ratios need not be normalized to unity. For instance, you may at input have a stored total width of 1 GeV and a sum of branching ratios of 2. After initialization the width will then have been changed to 2 GeV and the sum of branching ratios rescaled to unity. This might happen e.g. if you add a few channels to an existing resonance, without changing the branching ratios of the existing channels or the total width of the resonance.

In order to simulate the Breit-Wigner shape correctly, it is important that all channels that contribute to the total width are included in the above operations. This must be kept separate from the issue of which channels you want to have switched on for a particular study, to be considered next.

In the event-generation process, when an off-shell resonance mass has been selected, the width and branching ratios are re-evaluated for this new mass. At this stage also the effects of restrictions on allowed decay modes are taken into account, as set by the onMode switch for each separate decay channel. Thus a channel may be on or off, with different choices of open channels between the particle and its antiparticle. In addition, even when a channel is on, the decay may be into another resonance with its selection of allowed channels. It is these kinds of restrictions that lead to the Gamma_out possibly being smaller than Gamma_tot. As a reminder, the Breit-Wigner for decays behaves like Gamma_out / ((s - m^2)^2 + s * Gamma_tot^2), where the width in the numerator is only to those channels being studied, but the one in the denominator to all channels of the particle. These ever-changing numbers are not directly visible to the user, but are only stored in a work area. pythia8-8.1.80.orig/htmldoc/ROOTusage.html0000644000175000017500000002266012217615312016467 0ustar sunsun ROOT usage

ROOT usage

Many PYTHIA users wish to use ROOT to produce histograms, or even to run PYTHIA as a plugin to ROOT. This is possible. It is not a task supported by the PYTHIA team, however. All issues involving ROOT usage should be directed to the ROOT team, or to the local support team of your collaboration. Below some helpful hints have been collected. The text is based on contributions by Rene Brun, Andreas Morsch and Axel Naumann. Another example may be found in the VINCIA add-on program for parton showers, but this should also work for a PYTHIA standalone run.

Note that in all that follows, a Linux-type system with a Bash shell and GNU Make is assumed. In particular, for Mac OS X, the LD_LIBRARY_PATH should be replaced with DYLD_LIBRARY_PATH and the extension for shared libraries .so should be replaced with .dylib.


Standalone usage

One can perform the generation and analysis of events in a completely standalone fashion, and only use ROOT to process the completed events. Some example programs are provided in the rootexamples directory, with details provided below and in the README file. The examples assume that you have already compiled the PYTHIA library, ROOT is installed, and that all paths have been setup correctly (e.g. PATH and LD_LIBRARY_PATH). If these paths are not already set, ROOT typically comes with a shell script to set these paths, which can be run with
    source /path_to_ROOT_installation/bin/thisroot.sh

Histogramming with ROOT

An example of histogramming with ROOT is provided in rootexamples/hist.cc. It may be compiled and run with the following commands
    make hist
    ./hist.exe
After PYTHIA has run, a ROOT histogram of the charged multiplicity in the events will be shown. This is now stored in the hist.root file.

Storing PYTHIA events in ROOT trees

Instead of only generating histograms, it is possible to store entire PYTHIA events in ROOT trees. The tree example in the rootexamples subdirectory provides an example of this and is comprised of the following files
  • tree.cc is the main example program showing how PYTHIA events can be stored in ROOT trees.
  • pythiaLinkdef.h is used by Makefile to generate the dictionary for all PYTHIA classes involved in the IO, as needed for the example.
  • pythiaROOT.h is a small include declaring the Pythia8 namespace as default.

The example may be compiled and run with
    make tree
    ./tree.exe
After the example has run, the pytree.root file will now be present containing the PYTHIA events. Note that files can become quite large when many events are generated.


PYTHIA as a plugin to ROOT

In more ROOT-centric applications, PYTHIA can be run as a ROOT plug-in. This requires a version of ROOT that has been installed from source. The reason is that the interfaces depend on PYTHIA header files that are not distributed with ROOT. Installing ROOT is not more difficult than the PYTHIA installation, and some guidelines are provided below.

Installation

To be run as a plugin, PYTHIA must be compiled as a shared library. This is achieved by running the PYTHIA configure script with the --enable-shared option before make is run.

Define an environment variable for the path to your PYTHIA installation directory
    export PYTHIA8=path_to_PYTHIA8_installation
Before compiling ROOT, configure ROOT by running the configure command including the following options
    --enable-pythia8
    --with-pythia8-incdir=$PYTHIA8/include
    --with-pythia8-libdir=$PYTHIA8/lib
In case ROOT has already been compiled before, it will only recompile the PYTHIA module and build the library libEGPythia8.

Interfaces

When running PYTHIA as a plugin, the exact interface structure becomes very relevant. ROOT provides two simple interfaces (wrappers) for PYTHIA 8. The code for these interfaces are located in
    path_to_ROOT_source/montecarlo/pythia8

The two interfaces are
  • TPythia8 is an implementation of the TGenerator interface for PYTHIA 8.
    It allows you to use PYTHIA within a ROOT macro or as a plug-in for a general-purpose particle generator based on this interface. The main methods of the interface are
    • GenerateEvent() which triggers the generation of the next event, and
    • ImportParticles(TClonesArray* particles) which copies the native PYTHIA stack into a TClonesArray of TParticles.
    In addition, some methods that are directly related to corresponding PYTHIA methods are implemented
    • ReadString(const char* string) -> readString(...)
    • ReadConfigFile(const char* string) -> readFile(...)
    • Initialize(int idAin, int idBin, double ecms) -> init(...)
    • EventListing() -> event.list()
    • PrintStatistic() -> statistics()
    These methods provide already the basic PYTHIA functionality interactively from the ROOT command line. However, this does not mean that the usage of PYTHIA from within ROOT is restricted to these methods. In compiled code, one can always obtain a pointer to the Pythia instance e.g.
        TPythia8        *tp = new TPythia8();
        Pythia8::Pythia *p  = tp->Pythia8();
    giving access to the full PYTHIA functionality. To access this functionality in the CINT interpreter see the "Advanced usage" section below.
  • TPythia8Decayer is an implementation of the TVirtualMCDecayer interface.
    It allows you to use PYTHIA as a plug-in decayer for simulation frameworks based on the Virtual Monte Carlo (VMC) interface classes. The main methods of the interface are
    • TPythia8Decayer::Init() for initialisation,
    • TPythia8Decayer::Decay(Int_t pdg, TLorentzVector* p) to decay a particle with PDG code pdg and 4-momentum p, and
    • ImportParticles(TClonesArray* particles) to retrieve the decay products as TParticles in the TClonesArray particles.

An example

A basic example for generating minimum-bias events with PYTHIA 8 inside a ROOT macro, and filling some histograms with the kinematics of the final-state particles is provided in either of the locations below
    /path_to_ROOT_source/tutorials/pythia/pythia8.C
    /path_to_ROOT_installation/share/doc/root/tutorials/pythia/pythia8.C

Note that before executing this script
  • the environment variables PYTHIA8 and PYTHIA8DATA must be setup correctly e.g.
        export PYTHIA8=/path_to_PYTHIA_installation
        export PYTHIA8DATA=$PYTHIA8/xmldoc
      
  • your LD_LIBRARY_PATH must contain the location of the PYTHIA 8 shared library, e.g.
        export LD_LIBRARY_PATH=$LD_LIBRARY_PATH:path_to_PYTHIA8_installation/lib
      
The script can then be run with ROOT
    root pythia8.C
After execution, ROOT will display some histograms from the event generation.

Advanced usage

To access the full PYTHIA functionality from the CINT interpreter, a ROOT dictionary must be created. An example of creating this dictionary is contained in the rootexamples directory. The pythiaDict.so library may be created by running
    make dict
This may then be loaded in ROOT giving full access to the full PYTHIA 8 functionality, e.g. in an interactive session
    gSystem->Load("path_to_PYTHIA8_installation/rootexamples/pythiaDict");
    Pythia8::Pythia *p = new Pythia8::Pythia();
    p->readString("SoftQCD:nonDiffractive = on");
pythia8-8.1.80.orig/htmldoc/FourVectors.html0000644000175000017500000004077112217615312017143 0ustar sunsun Four-Vectors

Four-Vectors

The Vec4 class gives a simple implementation of four-vectors. The member function names are based on the assumption that these represent four-momentum vectors. Thus one can get or set p_x, p_y, p_z and e, but not x, y, z or t. This is only a matter of naming, however; a Vec4 can equally well be used to store a space-time four-vector.

The Particle object contains a Vec4 p that stores the particle four-momentum, and another Vec4 vProd for the production vertex. For the latter the input/output method names are adapted to the space-time character rather than the normal energy-momentum one. Thus a user would not normally access the Vec4 classes directly, but only via the methods of the Particle class, see Particle Properties.

Nevertheless you are free to use the PYTHIA four-vectors, e.g. as part of some simple analysis code based directly on the PYTHIA output, say to define the four-vector sum of a set of particles. But note that this class was never set up to allow complete generality, only to provide the operations that are of use inside PYTHIA. There is no separate class for three-vectors, since such can easily be represented by four-vectors where the fourth component is not used.

Four-vectors have the expected functionality: they can be created, copied, added, multiplied, rotated, boosted, and manipulated in other ways. Operator overloading is implemented where reasonable. Properties can be read out, not only the components themselves but also for derived quantities such as absolute momentum and direction angles.

Constructors and basic operators

A few methods are available to create or copy a four-vector:

Vec4::Vec4(double x = 0., double y = 0., double z = 0., double t = 0.)  
creates a four-vector, by default with all components set to 0.

Vec4::Vec4(const Vec4& v)  
creates a four-vector copy of the input four-vector.

Vec4& Vec4::operator=(const Vec4& v)  
copies the input four-vector.

Vec4& Vec4::operator=(double value)  
gives a four-vector with all components set to value.

Member methods for input

The values stored in a four-vector can be modified in a few different ways:

void Vec4::reset()  
sets all components to 0.

void Vec4::p(double pxIn, double pyIn, double pzIn, double eIn)  
sets all components to their input values.

void Vec4::p(Vec4 pIn)  
sets all components equal to those of the input four-vector.

void Vec4::px(double pxIn)  
void Vec4::py(double pyIn)  
void Vec4::pz(double pzIn)  
void Vec4::e(double eIn)  
sets the respective component to the input value.

Member methods for output

A number of methods provides output of basic or derived quantities:

double Vec4::px()  
double Vec4::py()  
double Vec4::pz()  
double Vec4::e()  
gets the respective component.

double Vec4::mCalc()  
double Vec4::m2Calc()  
the (squared) mass, calculated from the four-vectors. If m^2 < 0 the mass is given with a minus sign, -sqrt(-m^2). Note the possible loss of precision in the calculation of E^2 - p^2; for particles the correct mass is stored separately to avoid such problems.

double Vec4::pT()  
double Vec4::pT2()  
the (squared) transverse momentum.

double Vec4::pAbs()  
double Vec4::pAbs2()  
the (squared) absolute momentum.

double Vec4::eT()  
double Vec4::eT2()  
the (squared) transverse energy, eT = e * sin(theta) = e * pT / pAbs.

double Vec4::theta()  
the polar angle, in the range 0 through pi.

double Vec4::phi()  
the azimuthal angle, in the range -pi through pi.

double Vec4::thetaXZ()  
the angle in the xz plane, in the range -pi through pi, with 0 along the +z axis.

double Vec4::pPos()  
double Vec4::pNeg()  
the combinations E+-p_z.

double Vec4::rap()  
double Vec4::eta()  
true rapidity y and pseudorapidity eta.

Friend methods for output

There are also some friend methods that take one, two or three four-vectors as argument. Several of them only use the three-vector part of the four-vector.

friend ostream& operator<<(ostream&, const Vec4& v)  
writes out the values of the four components of a Vec4 and, within brackets, a fifth component being the invariant length of the four-vector, as provided by mCalc() above, and it all ended with a newline.

friend double m(const Vec4& v1, const Vec4& v2)  
friend double m2(const Vec4& v1, const Vec4& v2)  
the (squared) invariant mass.

friend double dot3(const Vec4& v1, const Vec4& v2)  
the three-product.

friend double cross3(const Vec4& v1, const Vec4& v2)  
the cross-product.

friend double theta(const Vec4& v1, const Vec4& v2)  
friend double costheta(const Vec4& v1, const Vec4& v2)  
the (cosine) of the opening angle between the vectors, in the range 0 through pi.

friend double phi(const Vec4& v1, const Vec4& v2)  
friend double cosphi(const Vec4& v1, const Vec4& v2)  
the (cosine) of the azimuthal angle between the vectors around the z axis, in the range 0 through pi.

friend double phi(const Vec4& v1, const Vec4& v2, const Vec4& v3)  
friend double cosphi(const Vec4& v1, const Vec4& v2, const Vec4& v3)  
the (cosine) of the azimuthal angle between the first two vectors around the direction of the third, in the range 0 through pi.

friend double RRapPhi(const Vec4& v1, const Vec4& v2)  
friend double REtaPhi(const Vec4& v1, const Vec4& v2)  
the R distance measure, in (y, phi) or (eta, phi) cylindrical coordinates, i.e. R^2 = (y_1 - y_2)^2 + (phi_1 - phi_2)^2 and equivalent.

Operations with four-vectors

Of course one should be able to add, subtract and scale four-vectors, and more:

Vec4 Vec4::operator-()  
return a vector with flipped sign for all components, while leaving the original vector unchanged.

Vec4& Vec4::operator+=(const Vec4& v)  
add a four-vector to an existing one.

Vec4& Vec4::operator-=(const Vec4& v)  
subtract a four-vector from an existing one.

Vec4& Vec4::operator*=(double f)  
multiply all four-vector components by a real number.

Vec4& Vec4::operator/=(double f)  
divide all four-vector components by a real number.

friend Vec4 operator+(const Vec4& v1, const Vec4& v2)  
add two four-vectors.

friend Vec4 operator-(const Vec4& v1, const Vec4& v2)  
subtract two four-vectors.

friend Vec4 operator*(double f, const Vec4& v)  
friend Vec4 operator*(const Vec4& v, double f)  
multiply a four-vector by a real number.

friend Vec4 operator/(const Vec4& v, double f)  
divide a four-vector by a real number.

friend double operator*(const Vec4& v1, const Vec4 v2)  
four-vector product.

There are also a few related operations that are normal member methods:

void Vec4::rescale3(double f)  
multiply the three-vector components by f, but keep the fourth component unchanged.

void Vec4::rescale4(double f)  
multiply all four-vector components by f.

void Vec4::flip3()  
flip the sign of the three-vector components, but keep the fourth component unchanged.

void Vec4::flip4()  
flip the sign of all four-vector components.

Rotations and boosts

A common task is to rotate or boost four-vectors. In case only one four-vector is affected the operation may be performed directly on it. However, in case many particles are affected, the helper class RotBstMatrix can be used to speed up operations.

void Vec4::rot(double theta, double phi)  
rotate the three-momentum with the polar angle theta and the azimuthal angle phi.

void Vec4::rotaxis(double phi, double nx, double ny, double nz)  
rotate the three-momentum with the azimuthal angle phi around the direction defined by the (n_x, n_y, n_z) three-vector.

void Vec4::rotaxis(double phi, Vec4& n)  
rotate the three-momentum with the azimuthal angle phi around the direction defined by the three-vector part of n.

void Vec4::bst(double betaX, double betaY, double betaZ)  
boost the four-momentum by beta = (beta_x, beta_y, beta_z).

void Vec4::bst(double betaX, double betaY, double betaZ,double gamma)  
boost the four-momentum by beta = (beta_x, beta_y, beta_z), where the gamma = 1/sqrt(1 - beta^2) is also input to allow better precision when beta is close to unity.

void Vec4::bst(const Vec4& p)  
boost the four-momentum by beta = (p_x/E, p_y/E, p_z/E).

void Vec4::bst(const Vec4& p, double m)  
boost the four-momentum by beta = (p_x/E, p_y/E, p_z/E), where the gamma = E/m is also calculated from input to allow better precision when beta is close to unity.

void Vec4::bstback(const Vec4& p)  
boost the four-momentum by beta = (-p_x/E, -p_y/E, -p_z/E).

void Vec4::bstback(const Vec4& p, double m)  
boost the four-momentum by beta = (-p_x/E, -p_y/E, -p_z/E), where the gamma = E/m is also calculated from input to allow better precision when beta is close to unity.

void Vec4::rotbst(const RotBstMatrix& M)  
perform a combined rotation and boost; see below for a description of the RotBstMatrix.

For a longer sequence of rotations and boosts, and where several Vec4 are to be rotated and boosted in the same way, a more efficient approach is to define a RotBstMatrix, which forms a separate auxiliary class. You can build up this 4-by-4 matrix by successive calls to the methods of the class, such that the matrix encodes the full sequence of operations. The order in which you do these calls must agree with the imagined order in which the rotations/boosts should be applied to a four-momentum, since in general the operations do not commute.

RotBstMatrix::RotBstMatrix()  
creates a diagonal unit matrix, i.e. one that leaves a four-vector unchanged.

RotBstMatrix::RotBstMatrix(const RotBstMatrix& Min)  
creates a copy of the input matrix.

RotBstMatrix& RotBstMatrix::operator=(const RotBstMatrix4& Min)  
copies the input matrix.

void RotBstMatrix::rot(double theta = 0., double phi = 0.)  
rotate by this polar and azimuthal angle.

void RotBstMatrix::rot(const Vec4& p)  
rotate so that a vector originally along the +z axis becomes parallel with p. More specifically, rotate by -phi, theta and phi, with angles defined by p.

void RotBstMatrix::bst(double betaX = 0., double betaY = 0., double betaZ = 0.)  
boost by this beta vector.

void RotBstMatrix::bst(const Vec4&)  
void RotBstMatrix::bstback(const Vec4&)  
boost with a beta = p/E or beta = -p/E, respectively.

void RotBstMatrix::bst(const Vec4& p1, const Vec4& p2)  
boost so that p_1 is transformed to p_2. It is assumed that the two vectors obey p_1^2 = p_2^2.

void RotBstMatrix::toCMframe(const Vec4& p1, const Vec4& p2)  
boost and rotate to the rest frame of p_1 and p_2, with p_1 along the +z axis.

void RotBstMatrix::fromCMframe(const Vec4& p1, const Vec4& p2)  
rotate and boost from the rest frame of p_1 and p_2, with p_1 along the +z axis, to the actual frame of p_1 and p_2, i.e. the inverse of the above.

void RotBstMatrix::rotbst(const RotBstMatrix& Min);  
combine the current matrix with another one.

void RotBstMatrix::invert()  
invert the matrix, which corresponds to an opposite sequence and sign of rotations and boosts.

void RotBstMatrix::reset()  
reset to no rotation/boost; i.e. the default at creation.

double RotBstMatrix::deviation()  
crude estimate how much a matrix deviates from the unit matrix: the sum of the absolute values of all non-diagonal matrix elements plus the sum of the absolute deviation of the diagonal matrix elements from unity.

friend ostream& operator<<(ostream&, const RotBstMatrix& M)  
writes out the values of the sixteen components of a RotBstMatrix, on four consecutive lines and ended with a newline. pythia8-8.1.80.orig/htmldoc/PhaseSpaceCuts.html0000644000175000017500000004337212217615311017534 0ustar sunsun Phase Space Cuts

Phase Space Cuts

PhaseSpace is base class for all hard-process phase-space generators, either generic 2 -> 1 or 2 -> 2 ones, or specialized ones like for elastic and diffractive scattering.

In it, it is possible to constrain the kinematics of most processes. (Exceptions are "soft physics", i.e. minimum bias, elastic and diffractive processes. The Coulomb singularity for elastic scatterings, if simulated, is handled separately.) These constraints apply in the rest frame of the hard subprocess, and topologies normally would be changed e.g. by subsequent showering activity. The cross section of a process is adjusted to only correspond to the allowed phase space.

The more particles in the final state, the more cuts could be applied. Here we have tried to remain with the useful minimum, however. More generic possibilities could be handled by the user hooks facility.

Cuts in all processes

parm  PhaseSpace:mHatMin   (default = 4.; minimum = 0.)
The minimum invariant mass.

parm  PhaseSpace:mHatMax   (default = -1.)
The maximum invariant mass. A value below mHatMin means there is no upper limit.

Cuts in 2 -> 1 processes

When a resonance id is produced, the mMin(id) and mMax(id) methods restrict the allowed mass range of this resonance. Therefore the allowed range is chosen to be the overlap of this range and the mHatMin to mHatMax range above. Most resonances by default have no upper mass limit, so effects mainly concern the lower limit. Should there be no overlap between the two ranges then the process will be switched off.

Cuts in 2 -> 2 processes

parm  PhaseSpace:pTHatMin   (default = 0.; minimum = 0.)
The minimum invariant pT.

parm  PhaseSpace:pTHatMax   (default = -1.)
The maximum invariant pT. A value below pTHatMin means there is no upper limit.

parm  PhaseSpace:pTHatMinDiverge   (default = 1.; minimum = 0.5)
Extra pT cut to avoid the divergences of some processes in the limit pT -> 0. Specifically, if either or both produced particles have a mass below pTHatMinDiverge then pT is limited from below by the larger of pTHatMin and pTHatMinDiverge.

flag  PhaseSpace:useBreitWigners   (default = on)
Allows masses to be selected according to Breit-Wigner shapes in 2 -> 2 processes, whenever particles have been declared with a nonvanishing width above the threshold below. In those cases also the limits below will be used for the mass selection. For 2 -> 1 processes the Breit-Wigner shape is part of the cross section itself, and therefore always included.

parm  PhaseSpace:minWidthBreitWigners   (default = 0.01; minimum = 1e-6)
The minimum width a resonance must have for the mass to be dynamically selected according to a Breit-Wigner shape, within the limits set below. Only applies when useBreitWigners is on; else the nominal mass value is always used.

For a particle with a Breit-Wigner shape selected, according to the rules above and to the rules of the particle species itself, the mMin(id) and mMax(id) methods restrict the allowed mass range of the particle, just like for the 2 -> 1 processes.

Cuts in 2 -> 3 processes

There are two main classes of 2 -> 3 processes. One is the processes such as WW/ZZ-fusion Higgs production, i.e. q q -> q q H, where there are no special singularities associated with two partons in the final state being collinear, or even for pT -> 0. For this class, no further cuts have been introduced than those already available for 2 -> 2 processes. Specifically, for now all three are restricted exactly the same way by pTHatMin and pTHatMax. As above, Breit-Wigner mass ranges can be restricted.

The other 2 -> 3 event class is QCD processes, such as g g -> g g g. Here the soft and collinear singularities play a major role, and the phase space generation and cuts have been adapted to this. For this class, an alternative set of cuts is used, as outlined in the following. First of all the three outgoing partons are ordered in falling pT, i.e. pT_3 > pT_4 > pT_5 (where the labeling 3, 4, 5 of the outgoing partons is random, i.e. unrelated to the order specified in the process name). The allowed ranges of pT_3 and pT_5 can be specified, but obviously pT_3max >= pT_5max and pT_3min >= pT_5min. The pT_4 is not constrained explicitly, but is constructed from the vector sum of pT_3 and pT_5, subject to the constraint that it has to lie between the two in magnitude. While the pT cuts take care of singularities collinear with the incoming beams, it is also necessary to handle final-state singularities, when two outgoing partons become collinear. This is done by requiring a minimal separation in R, where R^2 = (Delta eta)^2 + (Delta phi)^2. Finally, a note about efficiency. The QCD 2 -> 3 phase space is not set up to explicitly include mHat as one of the basic variables. Such a cut is only done after a phase space point is already selected, which means that a narrow mass choice will slow down the program appreciably. Also narrow pT_3 and pT_5 bins are likely to give inefficient generation, if it gives rise to significant indirect restrictions on pT_4.

parm  PhaseSpace:pTHat3Min   (default = 10.; minimum = 0.)
The minimum invariant pT of the highest-pT parton in QCD 2 -> 3 processes.

parm  PhaseSpace:pTHat3Max   (default = -1.)
The maximum invariant pT of the highest-pT parton in QCD 2 -> 3 processes A value below pTHat3Min means there is no upper limit.

parm  PhaseSpace:pTHat5Min   (default = 10.; minimum = 0.)
The minimum invariant pT of the lowest-pT parton in QCD 2 -> 3 processes.

parm  PhaseSpace:pTHat5Max   (default = -1.)
The maximum invariant pT of the lowest-pT parton in QCD 2 -> 3 processes A value below pTHat5Min means there is no upper limit.

parm  PhaseSpace:RsepMin   (default = 1.)
The minimum separation R in (eta, phi) space between any two outgoing partons in QCD 2 -> 3 processes.

Cuts for a second hard process

If you use the machinery that allows the generation of a specified second hard process then, by default, the same phase space cuts will be used for it as listed above. Optionally, however, you may use a second set of cuts, as described here. In this context "first" and "second" is merely a technical distinction; you are welcome e.g. to pick pT ranges such that the second interaction always has a larger pT than the first.

flag  PhaseSpace:sameForSecond   (default = on)
By default use the same cuts for a second hard process as for the first. If off then instead use the mass and pT cuts below, where relevant. (The other cuts above still remain the same.)

parm  PhaseSpace:mHatMinSecond   (default = 4.; minimum = 0.)
The minimum invariant mass for a second interaction, if separate.

parm  PhaseSpace:mHatMaxSecond   (default = -1.)
The maximum invariant mass for a second interaction, if separate. A value below mHatMin means there is no upper limit.

parm  PhaseSpace:pTHatMinSecond   (default = 0.; minimum = 0.)
The minimum invariant pT for a second interaction, if separate.

parm  PhaseSpace:pTHatMaxSecond   (default = -1.)
The maximum invariant pT for a second interaction, if separate. A value below pTHatMin means there is no upper limit.

Generation strategy and documentation

During the initialization stage a simplified function is found, that is intended to be above the true cross-section behaviour over the whole of phase space. It is chosen to be easily integrable and invertible. That way a trial phase space point can be selected according this simple function, and then be accepted by the ratio of true to the simple function. For a good efficiency the ratio should be close to unity, yet never above it. This constrains the absolute normalization of the simple function. The initial search may fail to find the phase space point where the true-to-simple ratio is maximal, however. This then can lead to subsequent maximum violations, where the ratio is above unity. Two alternative strategies are implemented to handle such situations, see below.

flag  PhaseSpace:showSearch   (default = off)
Possibility to print information on the search for phase-space coefficients that (in a multichannel approach) provides an analytical upper envelope of the differential cross section, and the corresponding upper estimate of the cross section. Of interest for crosschecks by expert users only.

flag  PhaseSpace:showViolation   (default = off)
Possibility to print information whenever the assumed maximum differential cross section of a process is violated, i.e. when the initial maximization procedure did not find the true maximum. Also, should negative cross sections occur, print whenever a more negative value is encountered.

flag  PhaseSpace:increaseMaximum   (default = off)
Strategy for handling cases where a larger cross section is obtained during the event generation than was assumed at initialization, i.e. when a violation occurs.
off:each event comes with a weight, which normally is unity (as a consequence of the acceptance/rejection step), and is found in Info::weight(). For events which exceed the maximum instead the true-to-simple ratio is stored as event weight, which then is above unity. If the user so wishes this weight can then be carried along when event properties are histogrammed. Since normally such violations should be rare and not too much above unity one could expect most users to ignore such issues be default. Should maximum violations turn out to be frequent (visible in the Pythia::statistics() output) the option exists to use the information.
on:the maximum is increased whenever it is exceeded. Thus events generated after this point will be "correctly" distributed, while ones generated previously obviously then have had too high a relative weight. If violations occur early on and/or are small this strategy should do a good job of correcting to the desired phase-space distribution. This strategy may be more convenient for the normal user, who would not wish to worry about event weights. It does have the disadvantage that the raised maximum introduces an extra amount of "history memory" to the generation sequence, so that it becomes less easy to save-and-restore the random-number state for debugging purposes.

Reweighting of 2 -> 2 processes

Events normally come with unit weight, i.e. are distributed across the allowed phase space region according to the appropriate differential cross sections. Sometimes it may be convenient to have an uneven distribution of events. The classical example here is that many cross sections drop off with transverse momentum pT, such that few events are generated at large pT scales. If one wants to plot the pT cross section, and all that comes with it, the statistical error will then degrade with increasing pT where fewer events end up.

One solution is to split the full pT range into several separate subranges, where the events of each subsample obtains a different overall normalization. Specifically, if you generate a comparable number of events in each pT bin, such that larger pT bins are oversampled, these bins come with a correspondingly reduced overall weight, that needs to be taken into account when the bins are combined. The other is to have a continuously increasing oversampling of events at larger pT scales, which is compensated by a continuously decreasing weight for the event.

Both of these solutions are supported. Specifically, for 2 -> 2 processes, the pTHat scale offers a convenient classification of the event. (Of course, two events starting out from the same pTHat scale will experience different parton shower evolutions, etc., and may therefore look quite different at the end.) The two cuts PhaseSpace:pTHatMin and PhaseSpace:pTHatMax therefore offers a way to slice a pT range into subranges, see e.g. main08.cc. Alternatively the User Hooks machinery offers the possibility for you to define your own reweighting of phase space sampling, with a corresponding event weight, with UserHooks::canBiasSelection and related methods.

As a simplified option, we here offer the possibility to bias the 2 -> 2 sampling by a power of pTHat, then with events having a weight the inverse of this. This fast track will only work under a number of strict conditions, implemented to reduce the risk of abuse. (Whereas a UserHooks setup can be more flexible.) Specifically it will work if only high-pT 2 -> 2 processes already implemented in PYTHIA are requested, notably the HardQCD ones. That is, you cannot mix with 2 -> 1 or 2 -> 3 processes, nor with external processes (notably Les Houches input) or SoftQCD ones, and you cannot use the option to define a second hard process in the same event. Furthermore you have to be careful about the choice of PhaseSpace:pTHatMin, since a pTHat = 0 event would come with an infinite weight.

flag  PhaseSpace:bias2Selection   (default = off)
Possibility to switch on a biased phase space sampling, with compensatingly weighted events, for 2 -> 2 processes. Can only be used under the specific conditions explained in the paragraph above; under other conditions the initialization will abort.

parm  PhaseSpace:bias2SelectionPow   (default = 4.; minimum = 0.; maximum = 10.)
If the above flag is on, then a 2 -> 2 process at a scale pTHat will be oversampled in phase space by an amount (pTHat/pTRef)^pow, where you set the power pow here. Events are assigned a compensating weight the inverse of this, i.e. Info::weight() will return (pTRef/pTHat)^pow. This weight should then be used in the histogramming of event properties. The final overall normalization also involves the Info::weightSum() value.

parm  PhaseSpace:bias2SelectionRef   (default = 10.; minimum = 1.)
The reference scale pTRef introduced above, such that events with this pTHat obtain unit weight in the reweighting procedure. The value of this parameter has no impact on the final result of the reweighting procedure, but is only there for convenience, i.e. to give "reasonably-sized" weights. pythia8-8.1.80.orig/htmldoc/ParticleDataScheme.html0000644000175000017500000020630012217615311020333 0ustar sunsun The Particle Data Scheme

The Particle Data Scheme

The particle data scheme may take somewhat longer to understand than the settings one. In particular the set of methods to access information is rather more varied, to allow better functionality for advanced usage. However, PYTHIA does come with a sensible default set of particle properties and decay tables. Thus there is no need to learn any of the methods on this page to get going. Only when you perceive a specific need does it make sense to learn the basics.

The central section on this page is the Operation one. The preceding sections are there mainly to introduce the basic structure and the set of properties that can be accessed. The subsequent sections provide a complete listing of the existing public methods, which most users probably will have little interaction with.

Databases

The management of particle data is based on three classes:
  • ParticleData, which is the top-level class, with methods that can be used to interrogate all particle data. It contains a map of PDG particle identity numbers [Yao06] onto the relevant ParticleDataEntry objects,
  • ParticleDataEntry, which stores the relevant information on an individual particle species, and
  • DecayChannel, which stores info on one particular decay mode of a particle.
The objects of these classes together form a database that is continuously being used as the program has to assign particle masses, select decay modes, etc.

Each Pythia object has a public member particleData of the ParticleData class. Therefore you access the particle data methods as pythia.particleData.command(argument), assuming that pythia is an instance of the Pythia class. Further, for some of the most frequent user tasks, Pythia methods have been defined, so that pythia.command(argument) would work, see further below.

A fundamental difference between the particle data classes and the settings ones is that the former are accessed regularly during the event generation process, as a new particle is produced and its mass need to be set, e.g., while the latter are mainly/only used at the initialization stage. Nevertheless, it is not a good idea to change data in either of them in mid-run, since this may lead to inconsistencies.

Stored properties for particles

The main properties stored for each particle are as follows. Different ways to set and get these properties will be described further down.
  • name: a character string with the name of the particle. Particle and antiparticle names are stored separately, with void returned when no antiparticle exists.
  • spinType: the spin type, of the form 2 s + 1, with special code 0 for entries of unknown or indeterminate spin.
  • chargeType: three times the charge (to make it an integer).
  • colType: the colour type, with 0 uncoloured, 1 triplet, -1 antitriplet and 2 octet. (A preliminary implementation of colour sextets, available since version 8.150, further uses 3 for a sextet and -3 for an antisextet.)
  • m0: the nominal mass m_0 (in GeV).
  • mWidth: the width Gamma of the Breit-Wigner distribution (in GeV).
  • mMin: the lower limit of the allowed mass range generated by the Breit-Wigner (in GeV). Has no meaning for particles without width, and would typically be 0 there.
  • mMax: the upper limit of the allowed mass range generated by the Breit-Wigner (in GeV). If mMax < mMin then no upper limit is imposed. Has no meaning for particles without width, and would typically be 0 there.
  • tau0: the nominal proper lifetime tau_0 (in mm/c).
  • isResonance: a flag telling whether a particle species is considered as a resonance or not. Here "resonance" is used as shorthand for any massive particle where the decay process should be counted as part of the hard process itself, and thus be performed before showers and other event aspects are added. Restrictions on allowed decay channels is also directly reflected in the cross section of simulated processes, while those of normal hadrons and other light particles are not. In practice, it is reserved for states above the b bbar bound systems in mass, i.e. for W, Z, t, Higgs states, supersymmetric states and (most?) other states in any new theory. All particles with m0 above 20 GeV are by default initialized to be considered as resonances.
  • mayDecay: a flag telling whether a particle species may decay or not, offering the main user switch. Whether a given particle of this kind then actually will decay also depends on it having allowed decay channels, and on other flags for particle decays (or resonance decays). All particles with tau0 below 1000 mm are by default initialized to allow decays.
  • doExternalDecays: a flag telling whether a particle should be handled by an external decay package or not, with the latter default. Can be manipulated as described on this page, but should normally not be. Instead the Pythia::decayPtr(...) method should be provided with the list of relevant particles.
  • isVisible: a flag telling whether a particle species is to be considered as visible in a detector or not, as used e.g. in analysis routines. By default this includes neutrinos and a few BSM particles (gravitino, sneutrinos, neutralinos) that have neither strong nor electromagnetic charge, and are not made up of constituents that have it. The value of this flag is only relevant if a particle is long-lived enough actually to make it to a detector.
  • doForceWidth: a flag valid only for resonances where PYTHIA contains code to calculate the width of the resonance from encoded matrix-element expressions, i.e. the Z^0, W^+-, t, h^0, and a few more. The normal behaviour (false) is then that the width is calculated from the mass, but it is possible to force the resonance to retain the nominal width. Branching ratios and the running of the total width are unaffected.

Stored properties for decays

An unstable particle has a decay table consisting of one or more decay channel. The following properties are stored for each such channel. Again different ways to set and get these properties will be described further down.
  • onMode: integer code for use or not of channel,
    0 if a channel is off,
    1 if on,
    2 if on for a particle but off for an antiparticle,
    3 if on for an antiparticle but off for a particle.
    If a particle is its own antiparticle then 2 is on and 3 off but, of course, for such particles it is much simpler and safer to use only 1 and 0.
    The 2 and 3 options can be used e.g. to encode CP violation in B decays, or to let the W's in a q qbar -> W^+ W^- process decay in different channels.
  • bRatio: the branching ratio of the channel (with some reservations for resonances, see meMode below).
  • meMode: the mode of processing this channel, possibly with matrix elements; see the particle decays and resonance decays descriptions for the list of possibilities. Notably the default code 0 for a particle means pure phase space decays according to the given branching ratios, while for a resonance it means that code exists for the dynamic calculations of partial widths and thereby branching ratios as a function of the resonance mass (which is done e.g. at initialization based on the mass set by the user). Then codes 1 - 99 are reserved for various matrix-element-improved ordinary particle decays, and 100 - 103 for resonances where the partial width of a given channel is calculated from the total width and the stored branching ratio. Thus, to enforce a new branching ratio for a resonance channel (with its own partial-width calculation code) it is not sufficient only to change the bRatio but also to set e.g. meMode = 100.
  • multiplicity: the number of decay products of the channel. Can be at most 8.
  • product(i): the identity code of the decay products, where i runs between 0 and multiplicity - 1. Trailing positions are filled with 0.

Operation

The normal flow of the particle data operations is:
  1. When a Pythia object pythia is created, the pythia.particleData member is asked to scan the ParticleData.xml file.

    All lines beginning with <particle are scanned for information on a particle species, and all lines beginning with <channel are assumed to contain a decay channel of the enclosing particle. In both cases XML syntax is used, with attributes used to identify the stored properties, and with omitted properties defaulting back to 0 where meaningful. The particle and channel information may be split over several lines, up to the > endtoken. The format of a <particle tag is:

        <particle id="..." name="..." antiName="..." spinType="..." chargeType="..." colType="..." 
           m0="..." mWidth="..." mMin="..." mMax="..." tau0="...">
        </particle>
    
    where the fields are the properties already introduced above. Note that isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth are not set here, but are provided with default values by the rules described above. Once initialized, also these latter properties can be changed, see below.
    The format of a <channel> tag is:
        <channel onMode="..." bRatio="..." meMode="..." products="..." />
    
    again see properties above. The products are given as a blank-separated list of id codes.
    Important: the values in the .xml file should not be changed, except by the PYTHIA authors. Any changes should be done with the help of the methods described below.
  2. Between the creation of the Pythia object and the init call for it, you may use the methods of the ParticleData class to modify some of the default values. Several different approaches can be chosen for this.

    a) Inside your main program you can directly set values with

        pythia.readString(string);
    
    where both the variable name and the value are contained inside the character string, separated by blanks and/or a =, e.g.
        pythia.readString("111:mayDecay = off"); 
    
    switches off the decays of the pi^0.
    The particle id (> 0) and the property to be changed must be given, separated by a colon.
    The allowed properties are: name, antiName, spinType, chargeType, colType, m0, mWidth, mMin, mMax, tau0, isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth. All of these names are case-insensitive. Names that do not match an existing variable are ignored.
    Strings beginning with a non-alphanumeric character, like # or !, are assumed to be comments and are not processed at all. For bool values, the following notation may be used interchangeably: true = on = yes = ok = 1, while everything else gives false (including but not limited to false, off, no and 0).

    Particle data often comes in sets of closely related information. Therefore some properties expect the value to consist of several numbers. These can then be separated by blanks (or by commas). A simple example is names, which expects both the name and antiname to be given. A more interesting one is the all property,

      
        id:all = name antiName spinType chargeType colType m0 mWidth mMin mMax tau0
    
    where all the current information on the particle itself is replaced, but any decay channels are kept unchanged. Using new instead of all also removes any previous decay channels. If the string contains fewer fields than expected the trailing properties are set to vanish ("void", 0 or 0.). Note that such a truncated string should not be followed by a comment, since this comment would then be read in as if it contained the missing properties. The truncation can be done anywhere, specifically a string with only id:new defines a new "empty" particle. As before, isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth are (re)set to their default values, and would have to be changed separately if required.

    A further command is rescaleBR, which rescales each of the existing branching ratios with a common factor, such that their new sum is the provided value. This may be a first step towards adding new decay channels, see further below.

    Alternatively the id code may be followed by another integer, which then gives the decay channel number. This then has to be followed by the property specific to this channel, either onMode, bRatio, meMode or products. In the latter case all the products of the channel should be given:

        id:channel:products =  product1 product2 ....  
    
    The line will be scanned until the end of the line, or until a non-number word is encountered, or until the maximum allowed number of eight products is encountered, whichever happens first. (Thus the multiplicity of a decay channel need not be input; it is automatically calculated from the products list.) It is also possible to replace all the properties of a channel in a similar way:
        id:channel:all = onMode bRatio meMode product1 product2 ....  
    
    To add a new channel at the end, use
        id:addChannel = onMode bRatio meMode product1 product2 ....
    

    It is currently not possible to remove a channel selectively, but setting its branching ratio vanishing is as effective. If you want to remove all existing channels and force decays into one new channel you can use

        id:oneChannel = onMode bRatio meMode product1 product2 ....
    
    A first oneChannel command could be followed by several subsequent addChannel ones, to build up a completely new decay table for an existing particle.

    When adding new channels or changing branching ratios in general, note that, once a particle is to be decayed, the sum of branching ratios is always rescaled to unity. Beforehand, rescaleBR may be used to rescale an existing branching ratio by the given factor.

    There are a few commands that will study all the decay channels of the given particle, to switch them on or off as desired. The

        id:onMode = onMode
    
    will set the onMode property of all channels to the desired value. The
     
        id:offIfAny   = product1 product2 .... 
        id:onIfAny    = product1 product2 .... 
        id:onPosIfAny = product1 product2 .... 
        id:onNegIfAny = product1 product2 .... 
    
    will set the onMode 0, 1, 2 or 3, respectively, for all channels which contain any of the enumerated products, where the matching to these products is done without distinction of particles and antiparticles. Note that "Pos" and "Neg" are slightly misleading since it refers to the particle and antiparticle of the id species rather than charge, but should still be simpler to remember and understand than alternative notations. Correspondingly
     
        id:offIfAll   = product1 product2 .... 
        id:onIfAll    = product1 product2 .... 
        id:onPosIfAll = product1 product2 .... 
        id:onNegIfAll = product1 product2 .... 
    
    will set the onMode 0, 1, 2 or 3, respectively, for all channels which contain all of the enumerated products, again without distinction of particles and antiparticles. If the same product appears twice in the list it must also appear twice in the decay channel, and so on. The decay channel is allowed to contain further particles, beyond the product list. By contrast,
     
        id:offIfMatch   = product1 product2 .... 
        id:onIfMatch    = product1 product2 .... 
        id:onPosIfMatch = product1 product2 .... 
        id:onPosIfMatch = product1 product2 .... 
    
    requires the decay-channel multiplicity to agree with that of the product list, but otherwise works as the onIfAll/offIfAll methods.

    Note that the action of several of the commands depends on the order in which they are executed, as one would logically expect. For instance, id:oneChannel removes all decay channels of id and thus all previous changes in this decay table, while subsequent additions or changes would still take effect. Another example would be that 23:onMode = off followed by 23:onIfAny = 1 2 3 4 5 would let the Z^0 decay to quarks, while no decays would be allowed if the order were to be reversed.

    b) The Pythia readString(string) method actually does not do changes itself, but sends on the string either to the ParticleData class or to the Settings one, depending on whether the string begins with a digit or a letter. If desired, it is possible to communicate directly with the corresponding ParticleData method:

        pythia.particleData.readString("111:mayDecay = off"); 
        pythia.particleData.readString("15:2:products = 16 -211"); 
    
    In this case, changes intended for Settings would not be understood.

    c) Underlying this are commands for all the individual properties in the ParticleData class, one for each. These are further described below. Thus, an example now reads

        pythia.particleData.mayDecay(111, false);
    
    Boolean values should here be given as true or false.

    d) A simpler and more useful way is to collect all your changes in a separate file, with one line per change, e.g.

        111:mayDecay = off
    
    The file can be read by the
        pythia.readFile(fileName); 
    
    method, where fileName is a string, e.g. pythia.readFile("main.cmnd") (or an istream instead of a fileName). Each line is processed as described for the string in 2a). This file can freely mix commands to the Settings and ParticleData classes.
  3. A routine reInit(fileName) is provided, and can be used to zero the particle data table and reinitialize it from scratch. Such a call might be useful if several subruns are to be made with widely different particle data - normally the maps are only built from scratch once, namely when the Pythia() object is created. Also, there is no other possibility to restore the default values, unlike for the settings.

  4. You may at any time obtain a listing of all the particle data by calling

        pythia.particleData.listAll();
    
    The listing is by increasing id number. It shows the basic quantities introduced above. Some are abbreviated in the header to fit on the lines: spn = spinType, chg = chargeType, col = colType, res = isResonance, dec = mayDecay && canDecay (the latter checks that decay channels have been defined), ext = doExternalDecay, vis = isVisible and wid = doForceWidth.
    To list only those particles that were changed (one way or another, the listing will not tell what property or decay channel was changed), instead use
        pythia.particleData.listChanged();
    
    (This info is based on a further hasChanged flag of a particle or a channel, set true whenever any of the changing methods are used. It is possible to manipulate this value, but this is not recommended.) By default the internal initialization of the widths of resonances such as gamma^*/Z^0, W^+-, t/tbar, H^0 do not count as changes; if you want to list also those changes instead call listChanged(true).
    To list only one particle, give its id code as argument to the list(...) function.. To list a restricted set of particles, give in their id codes to list(...) as a vector<int>.
  5. For wholesale changes of particle properties all available data can be written out, edited, and then read back in again. These methods are mainly intended for expert users. You can choose between two alternative syntaxes.

    a) XML syntax, using the <particle and <channel lines already described. You use the method particleData.listXML(fileName) to produce such an XML file and particleData.readXML(fileName) to read it back in after editing.

    b) Fixed/free format, using exactly the same information as illustrated for the <particle and <channel lines above, but now without any tags. This means that all information fields must be provided (if there is no antiparticle then write void), in the correct order (while the order is irrelevant with XML syntax), and all on one line. Information is written out in properly lined-up columns, but the reading is done using free format, so fields need only be separated by at least one blank. Each new particle is supposed to be separated by (at least) one blank line, whereas no blank lines are allowed between the particle line and the subsequent decay channel lines, if any. You use the method particleData.listFF(fileName) to produce such a fixed/free file and particleData.readFF(fileName) to read it back in after editing.

    As an alternative to the readXML and readFF methods you can also use the particleData.reInit(fileName, xmlFormat) method, where xmlFormat = true (default) corresponds to reading an XML file and xmlFormat = false to a fixed/free format one.

    To check that the new particle and decay tables makes sense, you can use the particleData.checkTable() method, either directly or by switching it on among the standard error checks.

The public methods

In the following we present briefly the public methods in the three classes used to build up the particle database. The order is top-down, i.e from the full table of all particles to a single particle to a single channel. Note that these methods usually are less elegant and safe than the input methods outlined above. If you use any of these methods, it is likely to be the ones in the full database, i.e. the first ones to be covered in the following.

For convenience, we have grouped related input and output methods together. It should be obvious from the context which is which: the input is of type void and has an extra last argument, namely is the input value, while the output method returns a quantity of the expected type.

The ParticleData methods

ParticleData::ParticleData()  
the constructor has no arguments and does not do anything. Internal.

void ParticleData::initPtr(Info* infoPtr,Settings* settingsPtrIn, Rndm* rndmPtrIn, CoupSM* coupSMPtrIn)  
initialize pointers to a few other classes. Internal.

bool ParticleData::init(string startFile = "../xmldoc/ParticleData.xml")  
read in an XML-style file with particle data and initialize the particle data tables accordingly. This command is executed in the Pythia constructor, i.e. is mainly for internal use.
argument startFile (default = ../xmldoc/ParticleData.xml) : the name of the data file to be read. When called from the Pythia constructor the directory is provided by the PYTHIA8DATA environment variable, if set, else by the argument of this constructor, which has the default value "../xmldoc".

bool ParticleData::reInit(string startFile,bool xmlFormat = true)  
overwrite the existing database by reading from the specified file. Unlike init above this method is not called by the Pythia constructor, but is entirely intended for users who want to replace the existing particle data with their own.
argument startFile : the path and name of file to be read.
argument xmlFormat : if true read the same kind of XML-style file as used by init, if not use an alternative "free format" file (i.e. without any XML tags, but with well-defined rules specifying in which order properties are stored).

void ParticleData::initWidths(vector<ResonanceWidths*> resonancePtrs)  
initialize Breit-Wigner shape parameters for all particles, and the detailed handling of resonances, i.e. particles with perturbatively calculable partial widths, which can be used to obtain a mass-dependent Breit-Wigner and a dynamic choice of decay channels. Called from Pythia::init().

bool ParticleData::readXML(string inFile, bool reset = true)  
void ParticleData::listXML(string outFile)  
read in XML-style data from a file or write it out to a file. For the former one can also decide whether to reset all particles to scratch, or only overwrite those particles in the file. The former method is used by init and reInit above.

bool ParticleData::readFF(string inFile, bool reset = true)  
void ParticleData::listFF(string outFile)  
read in free-format-style data from a file or write it out to a file. For the former one can also decide whether to reset all particles to scratch, or only overwrite those particles in the file. The former method is used by reInit above.

bool ParticleData::readString(string line, bool warn = true, ostream& os = cout)  
read in a string and interpret is as a new or changed particle data. The possibilities are extensively described above. It is normally used indirectly, via Pythia::readString(...) and Pythia::readFile(...).
argument line : the string to be interpreted as an instruction.
argument warn (default = true) : write a warning message or not whenever the instruction does not make sense, e.g. if the particle does not exist in the database.
argument os (default = cout) : stream for error printout.
Note: the method returns false if it fails to make sense out of the input string.

void ParticleData::listAll(ostream& os = cout)  
void ParticleData::listChanged(ostream& os = cout)  
void ParticleData::listChangedAndRes(ostream& os = cout)  
void ParticleData::list(bool changedOnly = false, bool changedRes = true, ostream& os = cout)  
methods intended to present a listing of particle data in a readable format. The first three are special cases of the fourth. The first lists all particle data, the second only data for those particles that were changed after the original creation of the particle data table. Resonances are a special case since they can get their data changed by being linked to an object that does the calculation of branching ratios. The second method does not count such resonances as changed, whereas the third does and thus lists all resonances.

void ParticleData::list(int idList, ostream& os = cout)  
void ParticleData::list(vector<int> idList, ostream& os = cout)  
list particle data for one single particle, with the identity code as input, or for a set of particles, with an input vector of identity codes.

void ParticleData::checkTable(ostream& os = cout)  
void ParticleData::checkTable(int verbosity,ostream& os = cout)  
check that the particle decay table makes sense, especially for decays.
argument verbosity : level of checks. 0 is only minimal, e.g. if a particle has no open decay channels. 1, which is the level of the first method, provides warning if any individual channel is closed, except for resonances. 2 also prints the branching-ratio-averaged threshold mass. 11 and 12 are like 1 and 2, but also include resonances in the detailed checks.

void ParticleData::addParticle(int id, string name = " ", int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0., double tau0 = 0.)  
void ParticleData::addParticle(int id, string name, string antiName, int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0., double tau0 = 0.)  
add a particle to the decay table; in the first form a particle which is its own antiparticle, in the second where a separate antiparticle exists.

void ParticleData::setAll(int id, string name, string antiName, int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0.,double tau0 = 0.)  
change all the properties of the particle associated with a given identity code.

bool ParticleData::isParticle(int id)  
query whether the particle data table contains the particle of the identity code.

int ParticleData::nextId(int id)  
return the identity code of the sequentially next particle stored in table.

bool ParticleData::hasAnti(int id)  
bool whether a distinct antiparticle exists or not. Is true if an antiparticle name has been set (and is different from void).

void ParticleData::name(int id, string name)  
void ParticleData::antiName(int id, string antiName)  
void ParticleData::names(int id, string name, string antiName)  
string ParticleData::name(int id)  
particle and antiparticle names are stored separately, the sign of id determines which of the two is returned, with void used to indicate the absence of an antiparticle.

void ParticleData::spinType(int id, int spinType)  
int ParticleData::spinType(int id)  
the spin type, of the form 2 s + 1, with special code 0 for entries of unknown or indeterminate spin.

void ParticleData::chargeType(int id, int chargeType)  
int ParticleData::chargeType(int id)  
three times the charge (to make it an integer), taking into account the sign of id.

double ParticleData::charge(int id)  
the electrical charge of a particle, equal to chargeType(id)/3.

void ParticleData::colType(int id, int colType)  
int ParticleData::colType(int id)  
the colour type, with 0 uncoloured, 1 triplet, -1 antitriplet and 2 octet, taking into account the sign of id.

void ParticleData::m0(int id, double m0)  
double ParticleData::m0(int id)  
the nominal mass m_0 (in GeV).

void ParticleData::mWidth(int id, double mWidth)  
double ParticleData::mWidth(int id)  
the width Gamma of the Breit-Wigner distribution (in GeV).

void ParticleData::mMin(int id, double mMin)  
double ParticleData::mMin(int id)  
the lower limit of the allowed mass range generated by the Breit-Wigner (in GeV). Has no meaning for particles without width, and would typically be 0 there.

void ParticleData::mMax(int id, double mMax)  
double ParticleData::mMax(int id)  
the upper limit of the allowed mass range generated by the Breit-Wigner (in GeV). If mMax < mMin then no upper limit is imposed. Has no meaning for particles without width, and would typically be 0 there.

double ParticleData::m0Min(int id)  
similar to mMin() above, except that for particles with no width the m0(id) value is returned.

double ParticleData::m0Max(int id)  
similar to mMax() above, except that for particles with no width the m0(id) value is returned.

void ParticleData::tau0(int id, double tau0)  
double ParticleData::tau0(int id)  
the nominal proper lifetime tau_0 (in mm/c).

void ParticleData::isResonance(int id, bool isResonance)  
bool ParticleData::isResonance(int id)  
a flag telling whether a particle species are considered as a resonance or not. Here "resonance" is used as shorthand for any massive particle where the decay process should be counted as part of the hard process itself, and thus be performed before showers and other event aspects are added. Restrictions on allowed decay channels is also directly reflected in the cross section of simulated processes, while those of normal hadrons and other light particles are not. In practice, it is reserved for states above the b bbar bound systems in mass, i.e. for W, Z, t, Higgs states, supersymmetric states and (most?) other states in any new theory. All particles with m0 above 20 GeV are by default initialized to be considered as resonances.

void ParticleData::mayDecay(int id, bool mayDecay)  
bool ParticleData::mayDecay(int id)  
a flag telling whether a particle species may decay or not, offering the main user switch. Whether a given particle of this kind then actually will decay also depends on it having allowed decay channels, and on other flags for particle decays (or resonance decays). All particles with tau0 below 1000 mm are by default initialized to allow decays.

void ParticleData::doExternalDecays(int id, bool doExternalDecays)  
bool ParticleData::doExternalDecay(int id)  
a flag telling whether a particle should be handled by an external decay package or not, with the latter default. Can be manipulated as described on this page, but should normally not be. Instead the pythia.decayPtr method should be provided with the list of relevant particles.

void ParticleData::isVisible(int id, bool isVisible)  
bool ParticleData::isVisible(int id)  
a flag telling whether a particle species is to be considered as visible in a detector or not, as used e.g. in analysis routines. By default this includes neutrinos and a few BSM particles (gravitino, sneutrinos, neutralinos) that have neither strong nor electromagnetic charge, and are not made up of constituents that have it. The value of this flag is only relevant if a particle is long-lived enough actually to make it to a detector.

void ParticleData::doForceWidth(int id, bool doForceWidth)  
bool ParticleData::doForceWidth(int id)  
a flag valid only for resonances where PYTHIA contains code to calculate the width of the resonance from encoded matrix-element expressions, i.e. the Z^0, W^+-, t, h^0, and a few more. The normal behaviour (false) is then that the width is calculated from the mass, but it is possible to force the resonance to retain the nominal width. Branching ratios and the running of the total width are unaffected.

void ParticleData::hasChanged(int id, bool hasChanged)  
bool ParticleData::hasChanged(int id)  
keep track of whether the data for a particle has been changed in any respect between initialization and the current status. Is used e.g. by the listChanged method to determine which particles to list.

bool ParticleData::useBreitWigner(int id)  
tells whether a particle will have a Breit-Wigner mass distribution or not. Is determined by an internal logic based on the particle width and on the value of the ParticleData:modeBreitWigner switch.

double ParticleData::constituentMass(int id)  
is the constituent mass for a quark, hardcoded as m_u = m_d = 0.325, m_s = 0.50, m_c = 1.60 and m_b = 5.0 GeV, for a diquark the sum of quark constituent masses, and for everything else the same as the ordinary mass.

double ParticleData::mSel(int id)  
returns a mass distributed according to a truncated Breit-Wigner, with parameters as described here. Is equal to m0(id) for particles without width.

double ParticleData::mRun(int id, double mH)  
calculate the running mass of species id when probed at a hard mass scale of mH. Only applied to obtain the running quark masses; for all other particle the normal fixed mass is used.

bool ParticleData::canDecay(int id)  
true for a particle with at least one decay channel defined.

bool ParticleData::isLepton(int id)  
true for a lepton or an antilepton (including neutrinos).

bool ParticleData::isQuark(int id)  
true for a quark or an antiquark.

bool ParticleData::isGluon(int id)  
true for a gluon.

bool ParticleData::isDiquark(int id)  
true for a diquark or antidiquark.

bool ParticleData::isParton()  
true for a gluon, a quark or antiquark up to the b (but excluding top), and a diquark or antidiquark consisting of quarks up to the b.

bool ParticleData::isHadron(int id)  
true for a hadron (made up out of normal quarks and gluons, i.e. not for R-hadrons and other exotic states).

bool ParticleData::isMeson(int id)  
true for a meson.

bool ParticleData::isBaryon(int id)  
true for a baryon or antibaryon.

bool ParticleData::isOctetHadron(int id)  
true for an intermediate hadron-like state with a colour octet charge as used in the colour octet model for onia production.

int ParticleData::heaviestQuark(int id)  
extracts the heaviest quark or antiquark, i.e. one with largest id number, for a hadron.

int ParticleData::baryonNumberType(int id)  
is 1 for a quark, 2 for a diquark, 3 for a baryon, the same with a minus sign for antiparticles, and else zero.

void ParticleData::rescaleBR(int id, double newSumBR = 1.)  
rescales all partial branching ratios by a common factor, such that the sum afterward becomes newSumBR.

void setResonancePtr(int id, ResonanceWidths* resonancePtr)  
set a pointer for a particle kind to a ResonanceWidths object. This is done, from inside ParticleData::initWidths, only for resonances, i.e. for particles such as Z^0, W^+-, top, Higgs, and new unstable states beyond the Standard Model. The presence of such an object will allow a more dynamic calculation of partial and total widths, as illustrated by the following methods.

void ParticleData::resInit(int id)  
initialize the treatment of a resonance.

double ParticleData::resWidth(int id, double mHat, int idInFlav = 0, bool openOnly = false, bool setBR = false)  
calculate the total with for a resonance of a given current mass, optionally including coupling to incoming flavour state (consider the gamma*/Z^0 combination), optionally excluding decay channels that have been closed by the user, and optionally storing the results in the normal decay table.

double ParticleData::resWidthOpen(int id, double mHat, int idInFlav = 0)  
special case of resWidth, where only open channels are included, but results are not stored in the normal decay table.

double ParticleData::resWidthStore(int id, double mHat, int idInFlav = 0)  
special case of resWidth, where only open channels are included, and results are stored in the normal decay table.

double ParticleData::resOpenFrac(int id1, int id2 = 0, int id3 = 0)  
calculate the fraction of the full branching ratio that is left open by the user choice of allowed decay channels. Can be applied to a final state with up to three resonances. Since the procedure is multiplicative, it would be easy to generalize also to more.

double ParticleData::resWidthRescaleFactor(int id)  
the factor used to rescale all partial widths in case the total width is being forced to a specific value by the user.

double ParticleData::resWidthChan(int id,double mHat, int idAbs1 = 0, int idAbs2 = 0)  
special case to calculate one final-state width; currently only used for Higgs decay to q qbar, g g or gamma gamma.

ParticleDataEntry* ParticleData::particleDataEntryPtr(int id)  
returns a pointer to the ParticleDataEntry object. The methods in the next section can then be used to manipulate this object.

The ParticleDataEntry methods

Most of the methods that can be applied to a single ParticleDataEntry object are almost identical with those used above for the ParticleData, except that the id argument is no longer needed to find the right entry in the table. By and large, this makes direct access to the ParticleDataEntry methods superfluous. There are a few methods that are unique to each class, however. Furthermore, to avoid some naming ambiguities, many methods that set values begin with set.

ParticleDataEntry::ParticleDataEntry(int id = 0, string name = " ", int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0., double tau0 = 0.)  
ParticleDataEntry::ParticleDataEntry(int id, string name, string antiName, int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0., double tau0 = 0.)  
there are two alternative constructors, that both expect the properties of a particle as input. The first assumes that there is only one particle, the latter that there is a particle-antiparticle pair (but if the antiparticle name is void one reverts back to the particle-only case).

ParticleDataEntry::~ParticleDataEntry  
the destructor is needed to delete any ResonanceWidths objects that have been created and linked to the respective particle.

void ParticleDataEntry::setDefaults()  
initialize some particle flags with default values, e.g. whether a particle is a resonance, may decay, or is visible. Is called from the constructors and from setAll.

void ParticleDataEntry::initPtr(ParticleData* particleDataPtrIn)  
initialize pointer back to the whole database (so that masses of decay products can be accessed, e.g.).

void ParticleDataEntry::setAll( string name, string antiName, int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0.,double tau0 = 0.)  
change all the properties of the particle associated with a given identity code.

int ParticleDataEntry::id()  
the PDG identity code.

bool ParticleDataEntry::hasAnti()  
tell whether a separate antiparticle exists.

void ParticleDataEntry::setName(string name)  
void ParticleDataEntry::setAntiName(string antiName)  
void ParticleDataEntry::setNames(string name,string antiName)  
string ParticleDataEntry::name(int id = 1)  
set or get the particle or antiparticle name. Only the sign of id is needed to distinguish particle/antiparticle.

void ParticleDataEntry::setSpinType(int spinType)  
int ParticleDataEntry::spinType()  
set or get the particle spin type, i.e. 2 s + 1, or 0 in some special cases.

void ParticleDataEntry::setChargeType(int chargeType)  
int ParticleDataEntry::chargeType(int id = 1)  
double ParticleDataEntry::charge(int id = 1)  
set or get the particle charge type, i.e. three times the charge, or the charge itself. Only the sign of id is needed to distinguish particle/antiparticle.

void ParticleDataEntry::setColType(int colType)  
int ParticleDataEntry::colType(int id = 1)  
set or get the particle colour type, 0 for singlet, 1 for triplet, -1 for antitriplet, 2 for octet. Only the sign of id is needed to distinguish particle/antiparticle.

void ParticleDataEntry::setM0(double m0)  
double ParticleDataEntry::m0()  
the nominal mass m_0 (in GeV).

void ParticleDataEntry::setMWidth(double mWidth)  
double ParticleDataEntry::mWidth()  
the width Gamma of the Breit-Wigner distribution (in GeV).

void ParticleDataEntry::setMMin(double mMin)  
double ParticleDataEntry::mMin()  
the lower limit of the allowed mass range generated by the Breit-Wigner (in GeV). Has no meaning for particles without width, and would typically be 0 there.

void ParticleDataEntry::setMMax(double mMax)  
double ParticleDataEntry::mMax()  
the upper limit of the allowed mass range generated by the Breit-Wigner (in GeV). If mMax < mMin then no upper limit is imposed. Has no meaning for particles without width, and would typically be 0 there.

double ParticleDataEntry::m0Min()  
similar to mMin() above, except that for particles with no width the m0(id) value is returned.

double ParticleDataEntry::m0Max()  
similar to mMax() above, except that for particles with no width the m0(id) value is returned.

void ParticleDataEntry::setTau0(double tau0)  
double ParticleDataEntry::tau0()  
the nominal proper lifetime tau_0 (in mm/c).

void ParticleDataEntry::setIsResonance(bool isResonance)  
bool ParticleDataEntry::isResonance()  
a flag telling whether a particle species are considered as a resonance or not. Here "resonance" is used as shorthand for any massive particle where the decay process should be counted as part of the hard process itself, and thus be performed before showers and other event aspects are added. Restrictions on allowed decay channels is also directly reflected in the cross section of simulated processes, while those of normal hadrons and other light particles are not. In practice, it is reserved for states above the b bbar bound systems in mass, i.e. for W, Z, t, Higgs states, supersymmetric states and (most?) other states in any new theory. All particles with m0 above 20 GeV are by default initialized to be considered as resonances.

void ParticleDataEntry::setMayDecay(bool mayDecay)  
bool ParticleDataEntry::mayDecay()  
a flag telling whether a particle species may decay or not, offering the main user switch. Whether a given particle of this kind then actually will decay also depends on it having allowed decay channels, and on other flags for particle decays (or resonance decays). All particles with tau0 below 1000 mm are by default initialized to allow decays.

void ParticleDataEntry::setDoExternalDecays(bool doExternalDecays)  
bool ParticleDataEntry::doExternalDecay()  
a flag telling whether a particle should be handled by an external decay package or not, with the latter default. Can be manipulated as described on this page, but should normally not be. Instead the pythia.decayPtr method should be provided with the list of relevant particles.

void ParticleDataEntry::setIsVisible(bool isVisible)  
bool ParticleDataEntry::isVisible()  
a flag telling whether a particle species is to be considered as visible in a detector or not, as used e.g. in analysis routines. By default this includes neutrinos and a few BSM particles (gravitino, sneutrinos, neutralinos) that have neither strong nor electromagnetic charge, and are not made up of constituents that have it. The value of this flag is only relevant if a particle is long-lived enough actually to make it to a detector.

void ParticleDataEntry::setDoForceWidth(bool doForceWidth)  
bool ParticleDataEntry::doForceWidth()  
a flag valid only for resonances where PYTHIA contains code to calculate the width of the resonance from encoded matrix-element expressions, i.e. the Z^0, W^+-, t, h^0, and a few more. The normal behaviour (false) is then that the width is calculated from the mass, but it is possible to force the resonance to retain the nominal width. Branching ratios and the running of the total width are unaffected.

void ParticleDataEntry::setHasChanged(bool hasChanged)  

void ParticleDataEntry::hasChanged(bool hasChanged)  
keep track of whether the data for a particle has been changed in any respect between initialization and the current status. Is used e.g. by the ParticleData::listChanged method to determine which particles to list.

void ParticleDataEntry::initBWmass()  
Prepare the Breit-Wigner mass selection by precalculating frequently-used expressions.

double ParticleDataEntry::constituentMass()  
is the constituent mass for a quark, hardcoded as m_u = m_d = 0.325, m_s = 0.50, m_c = 1.60 and m_b = 5.0 GeV, for a diquark the sum of quark constituent masses, and for everything else the same as the ordinary mass.

double ParticleDataEntry::mSel()  
give the mass of a particle, either at the nominal value or picked according to a (linear or quadratic) Breit-Wigner.

double ParticleDataEntry::mRun(double mH)  
calculate the running quark mass at a hard scale mH. For other particles the on-shell mass is given.

bool ParticleDataEntry::useBreitWigner()  
tells whether a particle will have a Breit-Wigner mass distribution or not. Is determined by an internal logic based on the particle width and on the value of the ParticleData:modeBreitWigner switch.

bool ParticleDataEntry::canDecay(int id)  
true for a particle with at least one decay channel defined.

bool ParticleDataEntry::isLepton()  
true for a lepton or an antilepton (including neutrinos).

bool ParticleDataEntry::isQuark()  
true for a quark or an antiquark.

bool ParticleDataEntry::isGluon()  
true for a gluon.

bool ParticleDataEntry::isDiquark()  
true for a diquark or antidiquark.

bool ParticleDataEntry::isParton()  
true for a gluon, a quark or antiquark up to the b (but excluding top), and a diquark or antidiquark consisting of quarks up to the b.

bool ParticleDataEntry::isHadron()  
true for a hadron (made up out of normal quarks and gluons, i.e. not for R-hadrons and other exotic states).

bool ParticleDataEntry::isMeson()  
true for a meson.

bool ParticleDataEntry::isBaryon()  
true for a baryon or antibaryon.

bool ParticleDataEntry::isOctetHadron()  
true for an intermediate hadron-like state with a colour octet charge as used in the colour octet model for onia production.

int ParticleDataEntry::heaviestQuark(int id)  
extracts the heaviest quark or antiquark, i.e. one with largest id number, for a hadron. Only the sign of the input argument is relevant.

int ParticleDataEntry::baryonNumberType(int id)  
is 1 for a quark, 2 for a diquark, 3 for a baryon, the same with a minus sign for antiparticles, and else zero. Only the sign of the input argument is relevant.

void ParticleDataEntry::clearChannels()  
resets to an empty decay table.

void ParticleDataEntry::addChannel(int onMode = 0, double bRatio = 0., int meMode = 0, int prod0 = 0, int prod1 = 0,int prod2 = 0, int prod3 = 0, int prod4 = 0, int prod5 = 0, int prod6 = 0, int prod7 = 0,)  
adds a decay channel with up to 8 products.

int ParticleDataEntry::sizeChannels()  
returns the number of decay channels for a particle.

DecayChannel& ParticleDataEntry::channel(int i)  
const DecayChannel& ParticleDataEntry::channel(int i)  
gain access to a specified channel in the decay table.

void ParticleDataEntry::rescaleBR(double newSumBR = 1.)  
rescales all partial branching ratios by a common factor, such that the sum afterward becomes newSumBR.

bool ParticleDataEntry::preparePick(int idSgn, double mHat = 0., int idInFlav = 0)  
prepare to pick a decay channel.

DecayChannel& ParticleDataEntry::pickChannel()  
pick a decay channel according to branching ratios from preparePick.

void ParticleDataEntry::setResonancePtr(ResonanceWidths* resonancePtr)  
ResonanceWidths* ParticleDataEntry::getResonancePtr()  
set or get a pointer to an object that can be used for dynamic calculation of partial and total resonance widths. Here a resonance is a particle such as top, Z^0, W^+-, Higgs, and new unstable states beyond the Standard Model.

void ParticleDataEntry::resInit(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, CoupSM* coupSMPtrIn)  
initialize the treatment of a resonance.

double ParticleDataEntry::resWidth(int idSgn,double mHat, int idInFlav = 0, bool openOnly = false, bool setBR = false)  
calculate the total with for a resonance of a given current mass, optionally including coupling to incoming flavour state (consider the gamma*/Z^0 combination), optionally excluding decay channels that have been closed by the user, and optionally storing the results in the normal decay table. For the first argument only the sign is relevant.

double ParticleDataEntry::resWidthOpen(int idSgn,double mHat, int idInFlav = 0)  
special case of resWidth, where only open channels are included, but results are not stored in the normal decay table.

double ParticleDataEntry::resWidthStore(int idSgn,double mHat, int idInFlav = 0)  
special case of resWidth, where only open channels are included, and results are stored in the normal decay table.

double ParticleDataEntry::resOpenFrac(int idSgn)  
calculate the fraction of the full branching ratio that is left open by the user choice of allowed decay channels.

double ParticleDataEntry::resWidthRescaleFactor()  
the factor used to rescale all partial widths in case the total width is being forced to a specific value by the user.

double ParticleDataEntry::resWidthChan(double mHat, int idAbs1 = 0, int idAbs2 = 0)  
special case to calculate one final-state width; currently only used for Higgs decay to q qbar, g g or gamma gamma.

The DecayChannel methods

The properties stored in an individual decay channel can be set or get by the methods in this section.

DecayChannel::DecayChannel(int onMode = 0, double bRatio = 0., int meMode = 0, int prod0 = 0, int prod1 = 0, int prod2 = 0, int prod3 = 0, int prod4 = 0, int prod5 = 0, int prod6 = 0, int prod7 = 0)  
the constructor for a decay channel. Internal.

void DecayChannel::onMode(int onMode)  
int DecayChannel::onMode()  
set or get the onMode of a decay channel,
0 if a channel is off,
1 if on,
2 if on for a particle but off for an antiparticle,
3 if on for an antiparticle but off for a particle.
If a particle is its own antiparticle then 2 is on and 3 off but, of course, for such particles it is much simpler and safer to use only 1 and 0.
The 2 and 3 options can be used e.g. to encode CP violation in B decays, or to let the W's in a q qbar -> W^+ W^- process decay in different channels.

void DecayChannel::bRatio(double bRatio, bool countAsChanged = true)  
double DecayChannel::bRatio()  
set or get the branching ratio of the channel. Second argument only for internal use.

void DecayChannel::rescaleBR(double fac)  
multiply the current branching ratio by fac.

void DecayChannel::meMode(int meMode)  
int DecayChannel::meMode()  
set or get the mode of processing this channel, possibly with matrix elements (see the particle decays and resonance decays descriptions).

void DecayChannel::multiplicity(int multiplicity)  
int DecayChannel::multiplicity()  
set or get the number of decay products in a channel, at most 8. (Is normally not to be set by hand, since it is automatically updated whenever the products list is changed.)

void DecayChannel::product(int i, int product)  
int DecayChannel::product(int i)  
set or get a list of the decay products, 8 products 0 <= i < 8, with trailing unused ones set to 0.

void DecayChannel::setHasChanged(bool hasChanged)  
bool DecayChannel::hasChanged()  
used for internal purposes, to know which decay modes have been changed.

bool DecayChannel::contains(int id1)  
bool DecayChannel::contains(int id1, int id2)  
bool DecayChannel::contains(int id1, int id2, int id3)  
find if the decay product list contains the one, two or three particle identities provided. If the same code is repeated then so must it be in the products list. Matching also requires correct sign.

void DecayChannel::currentBR(double currentBR)  
double DecayChannel::currentBR()  
set or get the current branching ratio, taking into account on/off switches and dynamic width for resonances. For internal use.

void DecayChannel::onShellWidth(double onShellWidth)  
double DecayChannel::onShellWidth()  
set or get the current partial width of the channel; intended for resonances where the widths are recalculated based on the current resonance mass. For internal use.

void DecayChannel::onShellWidthFactor(double factor)  
multiply the current partial width by factor.

void DecayChannel::openSec(int idSgn, double openSecIn)  
double DecayChannel::openSec(nt idSgn)  
set or get the fraction of secondary open widths, separately for positive and negative particles. For internal use. pythia8-8.1.80.orig/htmldoc/RandomNumberSeed.html0000644000175000017500000000277412217615311020054 0ustar sunsun Random-Number Seed

Random-Number Seed

The seed of the random number generator can be set as follows:

flag  Random:setSeed   (default = off)
Indicates whether a user-set seed should be used every time the Pythia::init routine is called. If off, the random number generator is initialized with its default seed at the beginning of the run, and never again. If on, each new Pythia::init call (should several be made in the same run) results in the random number being re-initialized, thereby possibly starting over with the same sequence, if you do not watch out.

mode  Random:seed   (default = -1; maximum = 900000000)
The seed to be used, if setSeed is on.
A negative value gives the default seed,
a value 0 gives a random seed based on the time, and
a value between 1 and 900,000,000 a unique different random number sequence.

For more on random numbers see here. This includes methods to save and restore the state of the generator, and some preprogrammed methods to generate non-uniform random numbers. pythia8-8.1.80.orig/htmldoc/RandomNumbers.html0000644000175000017500000001305712217615312017433 0ustar sunsun Random Numbers

Random Numbers

This page describes the random-number generator in PYTHIA and how it can be replaced by an external one.

Internal random numbers

The Rndm class generates random numbers, using the Marsaglia-Zaman-Tsang algorithm [Mar90].

Random numbers R uniformly distributed in 0 < R < 1 are obtained with

   Rndm::flat();
There are also methods to generate according to an exponential, to x * exp(-x), to a Gaussian, or picked among a set of possibilities, which make use of flat().

If the random number generator is not initialized before, it will be so the first time it is asked to generate a random number, and then with the default seed, 19780503. This means that, by default, all runs will use identically the same random number sequence. This is convenient for debugging purposes, but dangerous if you intend to run several "identical" jobs to boost statistics. You can initialize, or reinitialize, with your own choice of seed with a

   Rndm::init(seed);
Here values 0 < seed < 900 000 000 gives so many different random number sequences, while seed = 0 will call the Stdlib time(0) function to provide a "random" seed, and seed < 0 will revert back to the default seed.

The Pythia class defines a flag and a mode, that allows the seed to be set in the Pythia::init call. That would be the standard way for a user to pick the random number sequence in a run.

External random numbers

RndmEngine is a base class for the external handling of random-number generation. The user-written derived class is called if a pointer to it has been handed in with the pythia.rndmEnginePtr() method. Since the default Marsaglia-Zaman-Tsang algorithm is quite good, chances are that any replacement would be a step down, but this may still be required by consistency with other program elements in big experimental frameworks.

There is only one pure virtual method in RndmEngine, to generate one random number flat in the range between 0 and 1:

  virtual double flat() = 0;
Note that methods for initialization are not provided in the base class, in part since input parameters may be specific to the generator used, in part since initialization can as well be taken care of externally to the Pythia code.

An example illustrating how to run with an external random number generator is provided in main23.cc.

The methods

We here collect a more complete and formal overview of the methods.

Rndm::Rndm()  
construct a random number generator, but does not initialize it.

Rndm::Rndm(int seed)  
construct a random number generator, and initialize it for the given seed number.

bool Rndm::rndmEnginePtr( RndmEngine* rndmPtr)  
pass in pointer for external random number generation.

void Rndm::init(int seed = 0)  
initialize, or reinitialize, the random number generator for the given seed number. Not necessary if the seed was already set in the constructor.

double Rndm::flat()  
generate next random number uniformly between 0 and 1.

double Rndm::exp()  
generate random numbers according to exp(-x).

double Rndm::xexp()  
generate random numbers according to x exp(-x).

double Rndm::gauss()  
generate random numbers according to exp(-x^2/2).

pair<double, double> Rndm::gauss2()  
generate a pair of random numbers according to exp( -(x^2 + y^2) / 2). Is faster than two calls to gauss().

int Rndm::pick(const vector& prob)  
pick one option among vector of (positive) probabilities.

bool Rndm::dumpState(string fileName)  
save the current state of the random number generator to a binary file. This involves two integers and 100 double-precision numbers. Intended for debug purposes. Note that binary files may be platform-dependent and thus not transportable.

bool Rndm::readState(string fileName)  
set the state of the random number generator by reading in a binary file saved by the above command. Comments as above.

virtual double RndmEngine::flat()  
if you want to construct an external random number generator (or generator interface) then you must implement this method in your class derived from the RndmEningen base class, to give a random number between 0 and 1. pythia8-8.1.80.orig/htmldoc/SUSYProcesses.html0000644000175000017500000004275212217615311017354 0ustar sunsun SUSY Processes

SUSY

Here is collected processes involving supersymmetric particle production, with the exception of the (extended) Higgs sector. Since the number of separate but closely related processes is so big, there will not be switches for each separate process but only for a reasonable set of subgroups. However, the general switches SUSY:idA and SUSY:idB,valternatively vectors SUSY:idVecA and SUSY:idVecB, may be used in conjunction with any of these groups to provide some additional flexibility to concentrate on processes involving only specific (s)particle final states, see below.

Most of the SUSY implementation in PYTHIA 8 has been written by N. Desai and is documented in [Des11]. Please give due credit to external contributions to PYTHIA 8, such as this one, by including the original work in your list of references when using this implementation. The cross section formulae are mostly taken from [Boz07] and [Fuk11].

Since the implementation of SUSY processes was only recently completed [Des11], case-by-case validations against other codes are still recommended. A set of default validations have already been carried out by the authors, comparing to the PYTHIA 6 SUSY implementation and to the XSUSY code, using an sps1a spectrum. Explicit validations of the non-trivial SLHA2-specific extensions have generally not been carried out yet, with the exception of the R-parity violating single-sparticle production cross sections. Please report the results of any user validations you may carry out to the authors.


Important Note on SLHA: In order to simulate SUSY processes it is required to read in the couplings and masses relevant for the scenario to be studied. This is done with the help of the SUSY Les Houches Accord (SLHA), including the SLHA2 extensions and generalizations. (Internally, the SLHA2 conventions are used. SLHA1 spectra are automatically translated into SLHA2 notation during initialization.) The reading of a relevant SLHA file must be set up, as described on the SLHA page. Attempting to generate SUSY processes without a properly initialized SLHA spectrum is strongly discouraged and may lead to unexpected results. Always check for warnings and errors reported by the SLHA reader during the initialization stage.

SUSY Processes


Note 1: Decays of SUSY particles are described separately below.
Note 2: One special possibility is that the gluino or some squark(s) are sufficiently long-lived to hadronize. See the R-hadrons page for further details.
Note 3: lepton- and photon-initial states are not yet available. Only quark/gluon-initiated 2 -> 2 and 2 -> 1 (RPV) processes have been implemented.
Note 4: cross sections will be correctly folded with open branching fractions of cascade decays, but at present any difference between particle and antiparticle decay tables is not taken into account. This possibility will be included in a future update.

flag  SUSY:all   (default = off)
Common switch for production of supersymmetric particles, i.e. particles with R-parity -1.

mode  SUSY:idA   (default = 0; minimum = 0)
Option to limit the sum over possible outgoing states in SUSY 2 -> 2 processes to ones including a specific particle identity code. The default corresponds to summing over all possible indices. A non-zero value of SUSY:idA selects only processes that contain the state corresponding to that particular particle identity code in the fundamental 2 -> 2 scattering process (summed over particle/antiparticle). It is the user's responsibility to ensure that (a subset of) the processes to be simulated actually include this particle at the 2 -> 2 level; thus, asking for the lightest neutralino (code 1000021) to be present in a squark-squark production process will give no match.

mode  SUSY:idB   (default = 0; minimum = 0)
As for SUSY:idA, but requires an additional particle with PDG code SUSY:idB to be present in the 2 -> 2 process. Thus, using SUSY:idA and SUSY:idB a specific subprocess can be selected. Again only the absolute sign is used, i.e. the summation over particle and antiparticle is retained. Also the order of SUSY:idA and SUSY:idB is irrelevant; since both possible orderings are checked for a match with the two outgoing particles. (Although not recommended, should SUSY:idA be zero and SUSY:idB nonzero a match is searched for just like in the normal case with SUSY:idA nonzero and SUSY:idB zero.)

mvec  SUSY:idVecA   (default = 0; minimum = 0)
As for SUSY:idA, but as a vector of PDG codes. (Character-string input of such vectors should be as a comma-separated list, without any blanks.) Thus, it selects only processes that have a final-state particle corresponding to one of the identity codes in this vector. Note that, to activate this, SUSY:idA must be equal to zero; if not then the match to SUSY:idA takes precedence.

mvec  SUSY:idVecB   (default = 0; minimum = 0)
As for SUSY:idB, but as a vector of PDG codes. (Character-string input of such vectors should be as a comma-separated list, without any blanks.) As above, to activate this, SUSY:idB must be equal to zero; if not then the match to SUSY:idB takes precedence. For the matching, either of SUSY:idA and SUSY:idVecA may be combined with either of SUSY:idB and SUSY:idVecB. As above one of the two outgoing SUSY particles must match one of the particles in SUSY:id(Vec)A and the other one of the particles in SUSY:id(Vec)B when both are nonzero.

mode  SUSY:sin2thetaWMode   (default = 2; minimum = 1; maximum = 3)
The value of sin2(thetaW) should be taken from
option 1 : SM value, defined at M_Z, taken from PYTHIA's StandardModel:sin2thetaW parameter.
option 2 : SUSY value, defined at M_SUSY, derived from the running gauge couplings in BLOCK GAUGE in the SLHA file. Note: if no such block is present in the input file, this option will default back to option 1 above, i.e., the SM value.
option 3 : Pole value, defined by 1 - M_W^2/M_Z^2, using the pole masses stored in the SLHA BLOCK MASS, or, alternatively, PYTHIA's internal pole masses if no such block is present.

Gluino Pair Production

flag  SUSY:gg2gluinogluino   (default = off)
Pair production of gluinos by gluon-gluon initial states.

flag  SUSY:qqbar2gluinogluino   (default = off)
Pair production of gluinos by quark-antiquark annihilation and t-channel squark exchange. The cross section expression follows [Fuk11] and include the possibility of non-minimal flavour violation through misalignment of quarks with squarks. Only the MFV case has been explicitly validated.

Associated Squark-Gluino Production

flag  SUSY:qg2squarkgluino   (default = off)
Associated production of a squark with a gluino. The cross section expression follows [Fuk11] and include the possibility of non-minimal flavour violation through misalignment of quarks with squarks. Only the MFV case has been explicitly validated.

Squark Pair Production

flag  SUSY:gg2squarkantisquark   (default = off)
Pair production of a scalar quark together with a scalar antiquark by gluon annihilation via s-channel gluon exchange, t- and u-channel squark exchange, and the direct 4-point coupling. The cross section expression follows [Boz07]. Only the MFV case has been explicitly validated.

flag  SUSY:qqbar2squarkantisquark   (default = off)
Pair production of a scalar quark together with a scalar antiquark by quark-antiquark annihilation. For same-isospin ~q~q* production (i.e., ~u~u*, ~u~c*, ...), the s-channel gluon, photon, and Z and t-channel gluino contributions have so far been implemented (i.e., the t-channel neutralino contributions are neglected). For opposite-isospin ~q~q* production (~u~d*, ~u~s*, ...), the s-channel W and t-channel gluino contributions have been implemented (i.e., the t-channel neutralino contributions are neglected). The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated. (Note to PYTHIA 6 users: in older PYTHIA 6 versions, a bug caused the ~t1~t2* cross to be overcounted by a factor of 2. Starting from version 6.4.24, that generator now agrees with the implementation here.)

flag  SUSY:qqbar2squarkantisquark:onlyQCD   (default = off)
When switched on this flag switches off all but the s-channel gluon contribution in the calculation of same-isospin squark-antisquark production cross sections. Intended for reference only. For the most accurate physics simulation, leave this flag in the off position.

flag  SUSY:qq2squarksquark   (default = off)
Pair production of scalar quarks (squark-squark and its charge conjugate process; for squark-antisquark production see above) by t- and u-channel gluino, neutralino, and chargino exchange. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated. (Note to PYTHIA 6 users: PYTHIA 6 only included the gluino exchange contribution, which typically dominates due to the size of the strong coupling; for counterchecks, the flag SUSY:qq2squarksquark:onlyQCD below can be switched on to eliminate the chargino and neutralino contributions.)

flag  SUSY:qq2squarksquark:onlyQCD   (default = off)
When switched on this flag causes the t- or u-channel neutralino and chargino contributions to be ignored in the calculation of squark pair production cross sections. Intended for reference only. For the most accurate physics simulation, leave this flag in the off position.

Neutralino and Chargino Pair Production

flag  SUSY:qqbar2chi0chi0   (default = off)
Pair production of neutralinos by quark-antiquark annihilation. With four neutralino species this gives ten separate processes, codes 1201 - 1210. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated.

flag  SUSY:qqbar2chi+-chi0   (default = off)
Associated chargino-neutralino production by quark-antiquark annihilation. With four neutralino species, two chargino ones, and maintaining charge conjugate processes separate, this gives 16 separate processes, codes 1221 - 1236. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated.

flag  SUSY:qqbar2chi+chi-   (default = off)
Pair production of charginos by quark-antiquark annihilation. With two chargino species and maintaining mutually charge conjugate processes separate, this gives four separate processes, codes 1241 - 1244. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated.

Associated Neutralino/Chargino + Squark/Gluino Production

flag  SUSY:qg2chi0squark   (default = off)
Pair production of neutralinos from quark-gluon initial states. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated.

flag  SUSY:qg2chi+-squark   (default = off)
Associated chargino-squark production from quark-gluon initial states. annihilation. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated.

flag  SUSY:qqbar2chi0gluino   (default = off)
Associated neutralino-gluino production by quark-antiquark annihilation. The cross section expressions follow [Fuk11]. Only the MFV case has been explicitly validated.

flag  SUSY:qqbar2chi+-gluino   (default = off)
Associated chargino-gluino production by quark-antiquark annihilation. The cross section expressions follow [Fuk11]. Only the MFV case has been explicitly validated. (Note to PYTHIA 6 users: small differences between this implementation and PYTHIA 6 arise due to slightly different treatments of the weak mixing angle, which is fixed in PYTHIA 6, while it is computed from the SLHA input in PYTHIA 8; see SUSY:sin2thetaWMode above.)

Slepton Production

flag  SUSY:qqbar2sleptonantislepton   (default = off)
Pair production of slepton-antislepton via s-channel W, Z and gamma exchange. Includes both charged sleptons and sneutrinos but right handed sneutrinos currently not supported.

R-parity violating squark production

flag  SUSY:qq2antisquark   (default = off)
Resonant squark production via R-parity violating UDD couplings. The couplings must be input using the SLHA2 structure.

Decays of SUSY Particles

Based on the parameters read in from the SLHA, PYTHIA 8 will normally compute the decay modes of SUSY particles automatically, using the SusyResonanceDecays class(es). Essentially all tree-level 2-body decays in the MSSM have been implemented this way, excepting so far only those involving Higgs bosons (either in the in- or out-state) or gravitinos. Available channels so far include:
  • ~q → q + ~chi
  • ~q → ~q + W/Z
  • ~q → q + q (RPV UDD)
  • ~q → l + q (RPV LQD)
  • ~g → ~q + q
  • ~chi → ~chi + Z/W
  • ~chi → ~q + q
  • ~chi → ~l/~nu + l/nu
  • ~chi0 → q + q + q (RPV UDD)
  • ~l/~nu → l/nu + ~chi
  • ~l/~nu → ~l/~nu + W/Z
All channels are still undergoing validation, so this implementation should be considered preliminary. Still missing but to be included in a forthcoming update are: 3-body decays of charginos (via RPV), and 2-body decays of squarks and gauginos with Higgs as one of the decay products. Some 3-body decays have been implemented with Matrix Element weighting. In particular, those for a neutralino to a lighter neutralino and a fermion pair can be enabled.

flag  SUSYResonance:3BodyMatrixElement   (default = off)
When "on", the spin-averaged, squared matrix element is used to sample the phase space for resonance decay. Currently, only possible for a heavy neutralino decay to a light neutralino and a fermion-antifermion pair. pythia8-8.1.80.orig/htmldoc/ImplementNewShowers.html0000644000175000017500000006656312217615312020650 0ustar sunsun Implement New Showers

Implement New Showers

In case you want to replace the PYTHIA initial- and final-state showers by your own, it is possible but not trivial. The point is that multiparton interactions (MPI), initial-state radiation (ISR) and final-state radiation (FSR) in general appear in one single interleaved sequence of decreasing pT values. Therefore shower replacements would have to be able to play the game by such rules, as we will outline further below. Of course, this still leaves the field open exactly how to define what to mean by pT, how to handle recoil effects, how the colour flow is affected, and so on, so there is certainly room for alternative showers. A first example of a shower implemented within the PYTHIA context is VINCIA, which however so far only handles FSR.

For the moment we assume you want to keep the MPI part of the story unchanged, and make use of the existing beam-remnants (BR) machinery. If you want to replace both MPI, ISR, FSR and BR then you had better replace the whole PartonLevel module of the code. If, in addition, you want to produce your own hard processes, then you only need the hadron-level standalone part of the machinery.

In order to write replacement codes for ISR and/or FSR it is useful to be aware of which information has to be shared between the different components, and which input/output structure is required of the relevant methods. For details, nothing beats studying the existing code. However, here we provide an overview, that should serve as a useful introduction.

It should be noted that we here primarily address the problem in its full generality, with interleaved MPI, ISR and FSR. There exists an option TimeShower:interleave = off where only MPI and ISR would be interleaved and FSR be considered after these two, but still before BR. Most of the aspects described here would apply also for that case. By contrast, resonance decays are only considered after all the four above components, and timelike showers in those decays would never be interleaved with anything else, so are much simpler to administrate.

Therefore the pythia.setShowerPtr( timesDecPtr, timesPtr, spacePtr) method allows two separate pointers to be set to instances of derived TimeShower classes. The first is only required to handle decays, say of Z^0 or Upsilon, with no dependence on beam remnants or ISR. The second, as well as spacePtr, has to handle the interleaved evolution of MPI, ISR and FSR. Therefore you are free to implement only the first, and let the PYTHIA default showers take care of the latter two. But, if you wanted to, you could also set timesDecPtr = 0 and only provide a timesPtr, or only a spacePtr. If your timelike shower does both cases, the first two pointers can agree. The only tiny point to take into account then is that init( beamAPtr, beamBPtr) is called twice, a first time to timesDecPtr with beam pointers 0, and a second time to timesPtr with nonvanishing beam pointers.

The event record and associated information

Obviously the main place for sharing information is the event record, specifically the Event event member of Pythia, passed around as a reference. It is assumed you already studied how it works, so here we only draw attention to a few aspects of special relevance.

One basic principle is that existing partons should not be overwritten. Instead new partons should be created, even when a parton only receives a slightly shifted momentum and for the rest stays the same. Such "carbon copies" by final-state branchings should be denoted by both daughter indices of the original parton pointing to the copy, and both mother indices of the copy to the original. If the copy instead is intended to represent an earlier step, e.g. in ISR backwards evolution, the role of mothers and daughters is interchanged. The event.copy( iCopy, newStatus) routine can take care of this tedious task; the sign of newStatus tells the program which case to assume.

To make the event record legible it is essential that the status codes are selected appropriately to represent the reason why each new parton is added to the record. Also remember to change the status of a parton to be negative whenever an existing parton is replaced by a set of new daughter partons.

Another important parton property is scale(), which does not appear in the normal event listing, but only if you use the extended Event:listScaleAndVertex = on option. This property is supposed to represent the production scale (in GeV) of a parton. In the current FSR and ISR algorithms it is used to restrict from above the allowed pT values for branchings of this particular parton. Beam remnants and other partons that should not radiate are assigned scale 0.

Auxiliary to the event record proper is the PartonSystems class, that keep track of which partons belong together in the same scattering subsystem. This information must be kept up-to-date during the shower evolution.

For initial-state showers it is also necessary to keep track of the partonic content extracted from the beams. This information is stored in the BeamParticle class.

The TimeShower interface

If you want to replace the TimeShower class this would involve replacing the virtual methods among the following ones.

TimeShower::TimeShower()  
The constructor does not need to do anything.

virtual TimeShower::~TimeShower()  
The destructor does not need to do anything.

void TimeShower::initPtr(Info* infoPtr, Settings* settingsPtr, ParticleData* particleDataPtr, Rndm* rndmPtr, CoupSM* coupSMPtr, PartonSystems* partonSystemsPtr, UserHooks* userHooksPtr)  
This method only imports pointers to standard facilities, and is not virtual.

virtual void TimeShower::init( BeamParticle* beamAPtrIn = 0, BeamParticle* beamBPtrIn = 0)  
You have to store your local copy of the pointers to these objects, since they have to be used during the generation, as explained above. The pointers could be zero; e.g. a local copy of TimeShower is created to handle showers in decays such as Upsilon -> q qbar from inside the ParticleDecays class. This is also the place to do initialization of whatever parameters you plan to use, e.g. by reading in them from a user-accessible database like the Settings one.

virtual bool TimeShower::limitPTmax( Event& event, double Q2Fac = 0., double Q2Ren = 0.)  
The question is whether the FSR should be allowed to occur at larger scales than the hard process it surrounds. This is process-dependent, as illustrated below for the the analogous SpaeShower::limitPTmax(...) method, although the two kinds of radiation need not have to be modeled identically. The TimeShower:pTmaxMatch switch allows you to force the behaviour among three options, but you may replace by your own logic.
The internal PYTHIA implementation also allows intermediate options, where emissions can go up to the kinematical limit but be dampened above the factorization or renormalization scale. Therefore the (square of the) latter two are provided as optional input parameters.

double TimeShower::enhancePTmax()  
Relative to the default pT_max evolution scale of the process, it may still be convenient to vary the matching slightly for the hardest interaction in an event, to probe the sensitivity to such details. The base-class implementation returns the value of the TimeShower:pTmaxFudge parameter.

virtual int TimeShower::shower( int iBeg, int iEnd, Event& event, double pTmax, int nBranchMax = 0)  
This is an all-in-one call for shower evolution, and as such cannot be used for the normal interleaved evolution, where only the routines below are used. It also cannot be used in resonance decays that form part of the hard process, since there the user hooks insert a potential veto step. Currently this routine is therefore only used in the hadron-level decays, e.g. Upsilon -> g g g.
iBeg and iEnd is the position of the first and last parton of a separate system, typically produced by a resonance decay. Such a system only evolves in isolation, and in particular does not relate to the beams.
The pTmax value sets the maximum scale for evolution, but normally you would restrict that further for each individual parton based on its respective scale value.
The nBranchMax value, if positive, gives the maximum number of allowed branchings in the call, as useful for matching studies.
The routine is expected to return the number of FSR branchings that were generated, but only for non-critical statistics purposes.
Since the real action typically is delegated to the routines below, it may well be that the existing code need not be replaced.

virtual int TimeShower::showerQED( int iBeg, int iEnd, Event& event, double pTmax)  
This is a further simplified version of the shower method above. Currently it only handles the emission of photons in the decay of a hadron into a pair of leptons, either a charged lepton-antilepton or a lepton-neutrino pair. It is properly matched to the matrix element in the decay via a virtual photon or W^+-, respectively. It is called as part of such decays if ParticleDecays:allowPhotonRadiation = on, which is not the default value.

double TimeShower::pTLastInShower()  
Can be used to return the pT evolution scale of the last branching in the cascade generated with the above shower(...) method. Is to be set in the internal pTLastInShower variable, and should be 0 if there were no branchings. Can be useful for matching studies.

virtual void TimeShower::prepareGlobal( Event& event)  
This method resets some counters and extracts the locations of outgoing partons, in preparation of using the optional global recoil scheme. Unlike prepare(...) below it is only called once during the parton-level evolution, since it only relates to the hardest interaction. Is probably of no use to most people.

virtual void TimeShower::prepare( int iSys, Event& event, bool limitPTmaxIn = true, double pTfirstTrialIn = 1e9)  
This method is called immediately after a new interaction (or the products of a resonance decay) has been added, and should then be used to prepare the subsystem of partons for subsequent evolution. In the current code this involves identifying all colour and charge dipole ends: the position of radiating and recoiling partons, maximum pT scales, possible higher-order matrix elements matchings to apply, and so on.
The iSys parameter specifies which parton system is to be prepared. It is used to extract the set of partons to be treated, with rules as described in the above section on subsystems. Specifically, the first two partons represent the incoming state, or are 0 for resonance decays unrelated to the beams, while the rest are not required to be in any particular order.
The limitPTmaxIn switch conveys the choice made on maximum scale for the dipole-ends evolution associated with the hard interaction of the event (while scales for subsequent MPIs by default are set to respect pT ordering). If true then this scale is set by the user choice options, see the TimeShower::limitPTmax method above, while if false emissions are allowed to go up to the kinematical limit. For the two-hard-interactions scenario, the two class variables dopTlimit1 and dopTlimit2 instead convey the choice made.
The pTfirstTrialIn parameter is tentatively used in the new weak-shower part of the code. It is related to the option to shift the weak-shower evolution scale up by (some factor times) the gauge boson mass, without this backfiring on the QCD/QED evolution. Still under evolution, and normally not used.

virtual void TimeShower::rescatterUpdate( int iSys, Event& event)  
This method is called immediately after rescattering in the description of multiparton interactions. Thus the information on one or several systems is out-of-date, while that of the others is unchanged. We do not provide the details here, since we presume few implementors of new showers will want to touch the technicalities involved in obtaining a description of rescattering.

virtual void TimeShower::update( int iSys, Event& event)  
This method is called immediately after a spacelike branching in the iSys'th subsystem. Thus the information for that system is out-of-date, while that of the others is unchanged. If you want, you are free to throw away all information for the affected subsystem and call prepare( iSys, event) to create new one. Alternatively you may choose only to update the information that has changed.

virtual double TimeShower::pTnext( Event& event, double pTbegAll, double pTendAll, bool isFirstTrialIn = false)  
This is the main driver routine for the downwards evolution. A new pT is to be selected based on the current information set up by the routines above, and along with that a branching parton or dipole. The pTbegAll scale is the maximum scale allowed, from which the downwards evolution should be begun (usually respecting the maximum scale of each individual parton). If no emission is found above pTendAll (and above the respective shower cutoff scales) then 0. should be returned and no emissions will be allowed. Both scales can vary from one event to the next: if a scale has already been selected for MPI or ISR it makes no sense to look for a scale smaller than that from FSR, since it would not be able to compete, so pTendAll is set correspondingly. As it happens, FSR is tried before ISR and MPI in the interleaved evolution, but this is an implementation detail that could well change.
Typically the implementation of this routine would be to set up a loop over all possible radiating objects (dipoles, dipole ends, ...), for each pick its possible branching scale and then pick the one with largest scale as possible winner. At this stage no branching should actually be carried out, since MPI, ISR and FSR still have to be compared to assign the winner.
The isFirstTrialIn is true only for the very first emission, and can then optionally be used to switch the weak-shower evolution scale up by (some factor times) the gauge boson mass.

virtual bool TimeShower::branch( Event& event, bool isInterleaved = false)  
This method will be called once FSR has won the competition with MPI and ISR to do the next branching. The candidate branching found in the previous step should here be carried out in full. The pre-branching partons should get a negative status code and new replacement ones added to the end of the event record. Also the subsystem information should be updated, and possibly also the beams.
Should some problem be encountered in this procedure, e.g. if some not-previously-considered kinematics requirement fails, it is allowed to return false to indicate that no branching could be carried out.
Normally the optional isInterleaved argument would not be of interest. It can be used to separate resonance decays, false, from the interleaved evolution together with MPI and ISR, true. More precisely, it separates calls to the timesDecPtr and the timesPtr instances.

virtual bool TimeShower::rescatterPropogateRecoil( Event& event, Vec4& pNew)  
This method is only called if rescattering is switched on in the description of multiparton interactions. It then propagates a recoil from a timelike branching to internal lines that connect systems. As for rescatterUpdate above, this is not likely to be of interest to most implementors of new showers.

int TimeShower::system()  
This method is not virtual. If a branching is constructed by the previous routine this tiny method should be able to return the number of the selected subsystem iSysSel where it occurred, so that the spacelike shower can be told which system to update, if necessary. Therefore iSysSel must be set in branch (or already in pTnext).

virtual void TimeShower::list( ostream& os = cout)  
This method is not at all required. In the current implementation it outputs a list of all the dipole ends, with information on the respective dipole. The routine is not called anywhere in the public code, but has been inserted at various places during the development/debug phase.

The SpaceShower interface

If you want to replace the SpaceShower class this would involve replacing the virtual methods in the following. You will find that much of the story reminds of TimeShower above, and actually some cut-and-paste of text is involved. In some respects the description is simpler, since there are no special cases for resonance decays and non-interleaved evolution. Thus there is no correspondence to the TimeShower::shower(...) routine.

SpaceShower::SpaceShower()  
The constructor does not need to do anything.

virtual SpaceShower::~SpaceShower()  
Also the destructor does not need to do anything.

void SpaceShower::initPtr(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, CoupSM* coupSMPtrIn, PartonSystems* partonSystemsPtrIn, UserHooks* userHooksPtrIn, MergingHooks* mergingHooksPtrIn = 0)  
This method only imports pointers to standard facilities, and is not virtual.

virtual void SpaceShower::init(BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn)  
You have to store your local copy of the pointers to these objects, since they have to be used during the generation, as explained above. This is also the place to do initialization of whatever parameters you plan to use, e.g. by reading in them from a user-accessible database like the Settings one.

virtual bool SpaceShower::limitPTmax( Event& event, double Q2Fac = 0., double Q2Ren = 0.)  
The question is whether the ISR should be allowed to occur at larger scales than the hard process it surrounds. This is process-dependent. For instance, if the hard process is Z^0 production we know that ISR should be allowed to go right up to the kinematical limit. If it is a 2 -> 2 QCD process the ISR should not exceed the scale of the hard process, since if so one would double-count. The SpaceShower:pTmaxMatch switch allows you to force the behaviour, or else to program your own logic. The current default implementation limits pT whenever the final state contains a quark (except top), gluon or photon, since then the danger of double-counting is there. You may replace by your own logic, or leave as is.
The internal PYTHIA implementation also allows intermediate options, where emissions can go up to the kinematical limit but be dampened above the factorization or renormalization scale. Therefore the (square of the) latter two are provided as optional input parameters.

virtual double SpaceShower::enhancePTmax()  
When the above method limits pT_max to the scale of the process, it may still be convenient to vary the matching slightly for the hardest interaction in an event, to probe the sensitivity to such details. The base-class implementation returns the value of the SpaceShower:pTmaxFudge parameter.

virtual void SpaceShower::prepare( int iSys, Event& event, bool limitPTmaxIn = true, double pTfirstTrialIn = 1e9)  
This method is called immediately after a new interaction has been added, and should then be used to prepare the subsystem of partons for subsequent evolution. In the current code this involves identifying the colour and charge dipole ends: the position of radiating and recoiling partons, maximum pT scales, and possible higher-order matrix elements matchings to apply. Depending on what you have in mind you may choose to store slightly different quantities. You have to use the subsystem information described above to find the positions of the two incoming partons (and the outgoing ones) of the system, and from there the scales at which they were produced.
The limitPTmax input agrees with the output of the previous method for the hardest process, and is always true for subsequent MPI, since there an unlimited pT for sure would lead to double-counting.
The pTfirstTrialIn parameter is tentatively used in the new weak-shower part of the code. It is related to the option to shift the weak-shower evolution scale up by (some factor times) the gauge boson mass, without this backfiring on the QCD/QED evolution. Still under evolution, and normally not used.

virtual void SpaceShower::update( int iSys, Event& event)  
This method is called immediately after a timelike branching in the iSys'th subsystem. Thus the information for that system may be out-of-date, and to be updated. For the standard PYTHIA showers this routine does not need to do anything, but that may be different in another implementation.

virtual double SpaceShower::pTnext( Event& event, double pTbegAll, double pTendAll, int nRadIn = -1, bool isFirstTrial = false)  
This is the main driver routine for the downwards evolution. A new pT is to be selected based on the current information set up by the routines above, and along with that a branching parton or dipole. The pTbegAll scale is the maximum scale allowed, from which the downwards evolution should be begun (usually respecting the maximum scale of each individual parton). If no emission is found above pTendAll (and above the respective shower cutoff scales) then 0. should be returned and no emissions will be allowed. Both scales can vary from one event to the next: if a scale has already been selected for MPI or ISR it makes no sense to look for a scale smaller than that from FSR, since it would not be able to compete, so pTendAll is set correspondingly. As it happens, FSR is tried before ISR and MPI in the interleaved evolution, but this is an implementation detail that could well change.
Typically the implementation of this routine would be to set up a loop over all possible radiating objects (dipoles, dipole ends, ...), for each pick its possible branching scale and then pick the one with largest scale as possible winner. At this stage no branching should actually be carried out, since MPI, ISR and FSR still have to be compared to assign the winner.
The input nRadIn provides the total number of ISR and FSR emissions already generated in the event, and so allows a special treatment for the very first emission, if desired.
The isFirstTrialIn is true only for the very first emission, and can then optionally be used to switch the weak-shower evolution scale up by (some factor times) the gauge boson mass.

virtual bool SpaceShower::branch( Event& event)  
This method will be called once ISR has won the competition with MPI and FSR to do the next branching. The candidate branching found in the previous step should here be carried out in full. The pre-branching partons should get a negative status code and new replacement ones added to the end of the event record. Also the subsystem information should be updated, and possibly also the beams.
Should some problem be encountered in this procedure, e.g. if some not-previously-considered kinematics requirement fails, it is allowed to return false to indicate that no branching could be carried out. Also a complete restart of the parton-level description may be necessary, see doRestart() below.

int SpaceShower::system()  
This method is not virtual. If a branching is constructed by the previous routine this tiny method should be able to return the number of the selected subsystem iSysSel where it occurred, so that the spacelike shower can be told which system to update, if necessary. Therefore iSysSel must be set in branch (or already in pTnext).

bool SpaceShower::doRestart()  
This method is not virtual. If branch(...) above fails to construct a branching, and the conditions are such that the whole parton-level description should be restarted, then it should return true, else not. Currently only the rescattering description can give this kind of failures, and so the internal rescatterFail boolean must be set true when this should happen, and else false.

virtual void SpaceShower::list( ostream& os = cout)  
This method is not at all required. In the current implementation it outputs a list of all the dipole ends, with information on the respective dipole. The routine is not called anywhere in the public code, but has been inserted at various places during the development/debug phase. pythia8-8.1.80.orig/htmldoc/ParticleProperties.html0000644000175000017500000010744412217615312020503 0ustar sunsun Particle Properties

Particle Properties

A Particle corresponds to one entry/slot in the event record. Its properties therefore is a mix of ones belonging to a particle-as-such, like its identity code or four-momentum, and ones related to the event-as-a-whole, like which mother it has.

What is stored for each particle is

  • the identity code,
  • the status code,
  • two mother indices,
  • two daughter indices,
  • a colour and an anticolour index,
  • the four-momentum and mass,
  • the scale at which the particle was produced (optional),
  • the polarization/spin/helicity of the particle (optional),
  • the production vertex and proper lifetime (optional),
  • a pointer to the particle kind in the particle data table, and
  • a pointer to the event the particle belongs to.
From these, a number of further quantities may be derived.

Basic output methods

The following member functions can be used to extract the most important information:

int Particle::id()  
the identity of a particle, according to the PDG particle codes [Yao06].

int Particle::status()  
status code. The status code includes information on how a particle was produced, i.e. where in the program execution it was inserted into the event record, and why. It also tells whether the particle is still present or not. It does not tell how a particle disappeared, whether by a decay, a shower branching, a hadronization process, or whatever, but this is implicit in the status code of its daughter(s). The basic scheme is:

  • status = +- (10 * i + j)
  • + : still remaining particles
  • - : decayed/branched/fragmented/... and not remaining
  • i = 1 - 9 : stage of event generation inside PYTHIA
  • i = 10 -19 : reserved for future expansion
  • i >= 20 : free for add-on programs
  • j = 1 - 9 : further specification
In detail, the list of used or foreseen status codes is:
  • 11 - 19 : beam particles
    • 11 : the event as a whole
    • 12 : incoming beam
    • 13 : incoming beam-inside-beam (e.g. gamma inside e)
    • 14 : outgoing elastically scattered
    • 15 : outgoing diffractively scattered
  • 21 - 29 : particles of the hardest subprocess
    • 21 : incoming
    • 22 : intermediate (intended to have preserved mass)
    • 23 : outgoing
  • 31 - 39 : particles of subsequent subprocesses
    • 31 : incoming
    • 32 : intermediate (intended to have preserved mass)
    • 33 : outgoing
    • 34 : incoming that has already scattered
  • 41 - 49 : particles produced by initial-state-showers
    • 41 : incoming on spacelike main branch
    • 42 : incoming copy of recoiler
    • 43 : outgoing produced by a branching
    • 44 : outgoing shifted by a branching
    • 45 : incoming rescattered parton, with changed kinematics owing to ISR in the mother system (cf. status 34)
    • 46 : incoming copy of recoiler when this is a rescattered parton (cf. status 42)
    • 47 : a W or Z gauge boson produced in the shower evolution
  • 51 - 59 : particles produced by final-state-showers
    • 51 : outgoing produced by parton branching
    • 52 : outgoing copy of recoiler, with changed momentum
    • 53 : copy of recoiler when this is incoming parton, with changed momentum
    • 54 : copy of a recoiler, when in the initial state of a different system from the radiator
    • 55 : copy of a recoiler, when in the final state of a different system from the radiator
    • 56 : a W or Z gauge boson produced in the shower evolution
  • 61 - 69 : particles produced by beam-remnant treatment
    • 61 : incoming subprocess particle with primordial kT included
    • 62 : outgoing subprocess particle with primordial kT included
    • 63 : outgoing beam remnant
  • 71 - 79 : partons in preparation of hadronization process
    • 71 : copied partons to collect into contiguous colour singlet
    • 72 : copied recoiling singlet when ministring collapses to one hadron and momentum has to be reshuffled
    • 73 : combination of very nearby partons into one
    • 74 : combination of two junction quarks (+ nearby gluons) to a diquark
    • 75 : gluons split to decouple a junction-antijunction pair
    • 76 : partons with momentum shuffled to decouple a junction-antijunction pair
    • 77 : temporary opposing parton when fragmenting first two strings in to junction (should disappear again)
    • 78 : temporary combined diquark end when fragmenting last string in to junction (should disappear again)
  • 81 - 89 : primary hadrons produced by hadronization process
    • 81 : from ministring into one hadron
    • 82 : from ministring into two hadrons
    • 83, 84 : from normal string (the difference between the two is technical, whether fragmented off from the top of the string system or from the bottom, useful for debug only)
    • 85, 86 : primary produced hadrons in junction fragmentation of the first two string legs in to the junction, in order of treatment
  • 91 - 99 : particles produced in decay process, or by Bose-Einstein effects
    • 91 : normal decay products
    • 92 : decay products after oscillation B0 <-> B0bar or B_s0 <-> B_s0bar
    • 93, 94 : decay handled by external program, normally or with oscillation
    • 99 : particles with momenta shifted by Bose-Einstein effects (not a proper decay, but bookkept as an 1 -> 1 such, happening after decays of short-lived resonances but before decays of longer-lived particles)
  • 101 - 109 : particles in the handling of R-hadron production and decay, i.e. long-lived (or stable) particles containing a very heavy flavour
    • 101 : when a string system contains two such long-lived particles, the system is split up by the production of a new q-qbar pair (bookkept as decay chains that seemingly need not conserve flavour etc., but do when considered together)
    • 102 : partons rearranged from the long-lived particle end to prepare for fragmentation from this end
    • 103 : intermediate "half-R-hadron" formed when a colour octet particle (like the gluino) has been fragmented on one side, but not yet on the other
    • 104 : an R-hadron
    • 105 : partons or particles formed together with the R-hadron during the fragmentation treatment
    • 106 : subdivision of an R-hadron into its flavour content, with momentum split accordingly, in preparation of the decay of the heavy new particle, if it is unstable
    • 107 : two temporary leftover gluons joined into one in the formation of a gluino-gluon R-hadron.
  • 111 - 199 : reserved for future expansion
  • 201 - : free to be used by anybody

int Particle::mother1()  
int Particle::mother2()  
the indices in the event record where the first and last mothers are stored, if any. There are five allowed combinations of mother1 and mother2:

  1. mother1 = mother2 = 0: for lines 0 - 2, where line 0 represents the event as a whole, and 1 and 2 the two incoming beam particles;
  2. mother1 = mother2 > 0: the particle is a "carbon copy" of its mother, but with changed momentum as a "recoil" effect, e.g. in a shower;
  3. mother1 > 0, mother2 = 0: the "normal" mother case, where it is meaningful to speak of one single mother to several products, in a shower or decay;
  4. mother1 < mother2, both > 0, for abs(status) = 81 - 86: primary hadrons produced from the fragmentation of a string spanning the range from mother1 to mother2, so that all partons in this range should be considered mothers; and analogously for abs(status) = 101 - 106, the formation of R-hadrons;
  5. mother1 < mother2, both > 0, except case 4: particles with two truly different mothers, in particular the particles emerging from a hard 2 -> n interaction.

Note 1: in backwards evolution of initial-state showers, the mother may well appear below the daughter in the event record.
Note 2: the motherList() method below returns a vector of all the mothers, providing a uniform representation for all five cases.

int Particle::daughter1()  
int Particle::daughter2()  
the indices in the event record where the first and last daughters are stored, if any. There are five allowed combinations of daughter1 and daughter2:

  1. daughter1 = daughter2 = 0: there are no daughters (so far);
  2. daughter1 = daughter2 > 0: the particle has a "carbon copy" as its sole daughter, but with changed momentum as a "recoil" effect, e.g. in a shower;
  3. daughter1 > 0, daughter2 = 0: each of the incoming beams has only (at most) one daughter, namely the initiator parton of the hardest interaction; further, in a 2 -> 1 hard interaction, like q qbar -> Z^0, or in a clustering of two nearby partons, the initial partons only have this one daughter;
  4. daughter1 < daughter2, both > 0: the particle has a range of decay products from daughter1 to daughter2;
  5. daughter2 < daughter1, both > 0: the particle has two separately stored decay products (e.g. in backwards evolution of initial-state showers).

Note 1: in backwards evolution of initial-state showers, the daughters may well appear below the mother in the event record.
Note 2: the mother-daughter relation normally is reciprocal, but not always. An example is hadron beams (indices 1 and 2), where each beam remnant and the initiator of each multiparton interaction has the respective beam as mother, but the beam itself only has the initiator of the hardest interaction as daughter.
Note 3: the daughterList() method below returns a vector of all the daughters, providing a uniform representation for all five cases. With this method, also all the daughters of the beams are caught, with the initiators of the basic process given first, while the rest are in no guaranteed order (since they are found by a scanning of the event record for particles with the beam as mother, with no further information).

int Particle::col()  
int Particle::acol()  
the colour and anticolour tags, Les Houches Accord [Boo01] style (starting from tag 101 by default, see below).
Note: in the preliminary implementation of colour sextets (exotic BSM particles) that exists since PYTHIA 8.150, a negative anticolour tag is interpreted as an additional positive colour tag, and vice versa.

double Particle::px()  
double Particle::py()  
double Particle::pz()  
double Particle::e()  
the particle four-momentum components.

Vec4 Particle::p()  
the particle four-momentum vector, with components as above.

double Particle::m()  
the particle mass, stored with a minus sign (times the absolute value) for spacelike virtual particles.

double Particle::scale()  
the scale at which a parton was produced, which can be used to restrict its radiation to lower scales in subsequent steps of the shower evolution. Note that scale is linear in momenta, not quadratic (i.e. Q, not Q^2).

double Particle::pol()  
the polarization/spin/helicity of a particle. Currently Pythia does not use this variable for any internal operations, so its meaning is not uniquely defined. The LHA standard sets SPINUP to be the cosine of the angle between the spin vector and the 3-momentum of the decaying particle in the lab frame, i.e. restricted to be between +1 and -1. A more convenient choice could be the same quantity in the rest frame of the particle production, either the hard subprocess or the mother particle of a decay. Unknown or unpolarized particles should be assigned the value 9.

double Particle::xProd()  
double Particle::yProd()  
double Particle::zProd()  
double Particle::tProd()  
the production vertex coordinates, in mm or mm/c.

Vec4 Particle::vProd()  
The production vertex four-vector. Note that the components of a Vec4 are named px(), py(), pz() and e() which of course then should be reinterpreted as above.

double Particle::tau()  
the proper lifetime, in mm/c. It is assigned for all hadrons with positive nominal tau, tau_0 > 0, because it can be used by PYTHIA to decide whether a particle should or should not be allowed to decay, e.g. based on the decay vertex distance to the primary interaction vertex.

Input methods

The same method names as above are also overloaded in versions that set values. These have an input argument of the same type as the respective output above, and are of type void.

There are also a few alternative methods for input:

void Particle::statusPos()  
void Particle::statusNeg()  
sets the status sign positive or negative, without changing the absolute value.

void Particle::statusCode(int code)  
changes the absolute value but retains the original sign.

void Particle::mothers(int mother1, int mother2)  
sets both mothers in one go.

void Particle::daughters(int daughter1, int daughter2)  
sets both daughters in one go.

void Particle::cols(int col, int acol)  
sets both colour and anticolour in one go.

void Particle::p(double px, double py, double pz, double e)  
sets the four-momentum components in one go.

void Particle::vProd(double xProd, double yProd, double zProd, double tProd)  
sets the production vertex components in one go.

Further output methods

In addition, a number of derived quantities can easily be obtained, but cannot be set, such as:

int Particle::idAbs()  
the absolute value of the particle identity code.

int Particle::statusAbs()  
the absolute value of the status code.

bool Particle::isFinal()  
true for a remaining particle, i.e. one with positive status code, else false. Thus, after an event has been fully generated, it separates the final-state particles from intermediate-stage ones. (If used earlier in the generation process, a particle then considered final may well decay later.)

bool Particle::isRescatteredIncoming()  
true for particles with a status code -34, -45, -46 or -54, else false. This singles out partons that have been created in a previous scattering but here are bookkept as belonging to the incoming state of another scattering.

bool Particle::hasVertex()  
production vertex has been set; if false then production at the origin is assumed.

double Particle::m2()  
squared mass, which can be negative for spacelike partons.

double Particle::mCalc()  
double Particle::m2Calc()  
(squared) mass calculated from the four-momentum; should agree with m(), m2() up to roundoff. Negative for spacelike virtualities.

double Particle::eCalc()  
energy calculated from the mass and three-momentum; should agree with e() up to roundoff. For spacelike partons a positive-energy solution is picked. This need not be the correct one, so it is recommended not to use the method in such cases.

double Particle::pT()  
double Particle::pT2()  
(squared) transverse momentum.

double Particle::mT()  
double Particle::mT2()  
(squared) transverse mass. If m_T^2 is negative, which can happen for a spacelike parton, then mT() returns -sqrt(-m_T^2), by analogy with the negative sign used to store spacelike masses.

double Particle::pAbs()  
double Particle::pAbs2()  
(squared) three-momentum size.

double Particle::eT()  
double Particle::eT2()  
(squared) transverse energy, eT = e * sin(theta) = e * pT / pAbs.

double Particle::theta()  
double Particle::phi()  
polar and azimuthal angle.

double Particle::thetaXZ()  
angle in the (p_x, p_z) plane, between -pi and +pi, with 0 along the +z axis

double Particle::pPos()  
double Particle::pNeg()  
E +- p_z.

double Particle::y()  
double Particle::eta()  
rapidity and pseudorapidity.

double Particle::xDec()  
double Particle::yDec()  
double Particle::zDec()  
double Particle::tDec()  
Vec4 Particle::vDec()  
the decay vertex coordinates, in mm or mm/c. This decay vertex is calculated from the production vertex, the proper lifetime and the four-momentum assuming no magnetic field or other detector interference. It can be used to decide whether a decay should be performed or not, and thus is defined also for particles which PYTHIA did not let decay.

Not part of the Particle class proper, but obviously tightly linked, are the two methods

double m(const Particle& pp1, const Particle& pp2)  
double m2(const Particle& pp1, const Particle& pp2)  
the (squared) invariant mass of two particles.

Properties of the particle species

Each Particle contains a pointer to the respective ParticleDataEntry object in the particle data tables. This gives access to properties of the particle species as such. It is there mainly for convenience, and should be thrown if an event is written to disk, to avoid any problems of object persistency. Should an event later be read back in, the pointer will be recreated from the id code if the normal input methods are used. (Use the Event::restorePtrs() method if your persistency scheme bypasses the normal methods.) This pointer is used by the following member functions:

string Particle::name()  
the name of the particle.

string Particle::nameWithStatus()  
as above, but for negative-status particles the name is given in brackets to emphasize that they are intermediaries.

int Particle::spinType()  
2 *spin + 1 when defined, else 0.

double Particle::charge()  
int Particle::chargeType()  
charge, and three times it to make an integer.

bool Particle::isCharged()  
bool Particle::isNeutral()  
charge different from or equal to 0.

int Particle::colType()  
0 for colour singlets, 1 for triplets, -1 for antitriplets and 2 for octets. (A preliminary implementation of colour sextets also exists, using 3 for sextets and -3 for antisextets.)

double Particle::m0()  
the nominal mass of the particle, according to the data tables.

double Particle::mWidth()  
double Particle::mMin()  
double Particle::mMax()  
the width of the particle, and the minimum and maximum allowed mass value for particles with a width, according to the data tables.

double Particle::mSel()  
the mass of the particle, picked according to a Breit-Wigner distribution for particles with width. It is different each time called, and is therefore only used once per particle to set its mass m().

double Particle::constituentMass()  
will give the constituent masses for quarks and diquarks, else the same masses as with m0().

double Particle::tau0()  
the nominal lifetime tau_0 > 0, in mm/c, of the particle species. It is used to assign the actual lifetime tau.

bool Particle::mayDecay()  
flag whether particle has been declared unstable or not, offering the main user switch to select which particle species to decay.

bool Particle::canDecay()  
flag whether decay modes have been declared for a particle, so that it could be decayed, should that be requested.

bool Particle::doExternalDecay()  
particles that are decayed by an external program.

bool Particle::isResonance()  
particles where the decay is to be treated as part of the hard process, typically with nominal mass above 20 GeV (W^+-, Z^0, t, ...).

bool Particle::isVisible()  
particles with strong or electric charge, or composed of ones having it, which thereby should be considered visible in a normal detector.

bool Particle::isLepton()  
true for a lepton or an antilepton (including neutrinos).

bool Particle::isQuark()  
true for a quark or an antiquark.

bool Particle::isGluon()  
true for a gluon.

bool Particle::isDiquark()  
true for a diquark or an antidiquark.

bool Particle::isParton()  
true for a gluon, a quark or antiquark up to the b (but excluding top), and a diquark or antidiquark consisting of quarks up to the b.

bool Particle::isHadron()  
true for a hadron (made up out of normal quarks and gluons, i.e. not for R-hadrons and other exotic states).

ParticleDataEntry& particleDataEntry()  
a reference to the ParticleDataEntry.

Methods that may access the event the particle belongs to

A particle can be created on its own. When inserted into an event record, it obtains a pointer to that event-as-a-whole. It is then possible to use methods that do not make sense for a particle in isolation. These methods are listed below. Whenever the pointer to the event is not defined, these will return an appropriate "null" value, this being -1 for an integer, false for a bool, and empty for a vector, unless otherwise specified.

void Particle::index()  
the index of the particle itself in the event record.

int Particle::statusHepMC()  
returns the status code according to the HepMC conventions agreed in February 2009. This convention does not preserve the full information provided by the internal PYTHIA status code, as obtained by Particle::status(), but comes reasonably close. The allowed output values are:

  • 0 : an empty entry, with no meaningful information and therefore to be skipped unconditionally;
  • 1 : a final-state particle, i.e. a particle that is not decayed further by the generator (may also include unstable particles that are to be decayed later, as part of the detector simulation);
  • 2 : a decayed Standard Model hadron or tau or mu lepton, excepting virtual intermediate states thereof (i.e. the particle must undergo a normal decay, not e.g. a shower branching);
  • 3 : a documentation entry (not used in PYTHIA);
  • 4 : an incoming beam particle;
  • 11 - 200 : an intermediate (decayed/branched/...) particle that does not fulfill the criteria of status code 2, with a generator-dependent classification of its nature; in PYTHIA the absolute value of the normal status code is used.

Note: for a particle without a properly set pointer to its event, codes 1 and 4 can still be inferred from its status code, while everythg else is assigned code 0.

int Particle::iTopCopy()  
int Particle::iBotCopy()  
are used to trace carbon copies of the particle up to its top mother or down to its bottom daughter. If there are no such carbon copies, the index of the particle itself will be returned. A carbon copy is when the "same" particle appears several times in the event record, but with changed momentum owing to recoil effects.

int Particle::iTopCopyId()  
int Particle::iBotCopyId()  
also trace top mother and bottom daughter, but do not require carbon copies, only that one can find an unbroken chain, of mothers or daughters, with the same flavour id code. When it encounters ambiguities, say a g -> g g branching or a u u -> u u hard scattering, it will stop the tracing and return the current position. It can be confused by nontrivial flavour changes, e.g. a hard process u d -> d u by W^+- exchange will give the wrong answer. These methods therefore are of limited use for common particles, in particular for the gluon, but should work well for "rare" particles.

vector<int> Particle::sisterList(bool traceTopBot = false)  
returns a vector of all the sister indices of the particle, i.e. all the daughters of the first mother, except the particle itself. If the argument traceTopBot = true the particle is first traced up with iTopCopy() before its mother is found, and then all the particles in the daughterList() of this mother are traced down with iBotCopy(), omitting the original particle itself. The method is not meaningful for the 0 entry, with status code -11, and there returns an empty list.

bool Particle::isAncestor(int iAncestor)  
traces the particle upwards through mother, grandmother, and so on, until either iAncestor is found or the top of the record is reached. Normally one unique mother is required, as is the case e.g. in decay chains or in parton showers, so that e.g. the tracing through a hard scattering would not work. For hadronization, first-rank hadrons are identified with the respective string endpoint quark, which may be useful e.g. for b physics, while higher-rank hadrons give false. Currently also ministrings that collapsed to one single hadron and junction topologies give false.

bool Particle::undoDecay()  
removes the decay chain of the particle and thus restores it to its undecayed state. It is only intended for "normal" particle decay chains, and will return false in other cases, notably if the particle is coloured. The procedure would not work if non-local momentum shifts have been performed, such as with a Bose-Einstein shift procedure (or for a dipole shower recoiler). As the decay products are erased from the event record, mother and daughter indices are updated to retain a correct history for the remaining particles.

Methods that perform operations

There are some further methods, some of them inherited from Vec4, to modify the properties of a particle. They are of little interest to the normal user.

void Particle::rescale3(double fac)  
multiply the three-momentum components by fac.

void Particle::rescale4(double fac)  
multiply the four-momentum components by fac.

void Particle::rescale5(double fac)  
multiply the four-momentum components and the mass by fac.

void Particle::rot(double theta, double phi)  
rotate three-momentum and production vertex by these polar and azimuthal angles.

void Particle::bst(double betaX, double betaY, double betaZ)  
boost four-momentum and production vertex by this three-vector.

void Particle::bst(double betaX, double betaY, double betaZ, double gamma)  
as above, but also input the gamma value, to reduce roundoff errors.

void Particle::bst(const Vec4& pBst)  
boost four-momentum and production vertex by beta = (px/e, py/e, pz/e).

void Particle::bst(const Vec4& pBst, double mBst)  
as above, but also use gamma> = e/m to reduce roundoff errors.

void Particle::bstback(const Vec4& pBst)  
void Particle::bstback(const Vec4& pBst, double mBst)  
as above, but with sign of boost flipped.

void Particle::rotbst(const RotBstMatrix& M)  
combined rotation and boost of the four-momentum and production vertex.

void Particle::offsetHistory( int minMother, int addMother, int minDaughter, int addDaughter))  
add a positive offset to the mother and daughter indices, i.e. if mother1 is above minMother then addMother is added to it, same with mother2, if daughter1 is above minDaughter then addDaughter is added to it, same with daughter2.

void Particle::offsetCol( int addCol)  
add a positive offset to colour indices, i.e. if col is positive then addCol is added to it, same with acol.

Constructors and operators

Normally a user would not need to create new particles. However, if necessary, the following constructors and methods may be of interest.

Particle::Particle()  
constructs an empty particle, i.e. where all properties have been set 0 or equivalent.

Particle::Particle(int id, int status = 0, int mother1 = 0, int mother2 = 0, int daughter1 = 0, int daughter2 = 0, int col = 0, int acol = 0, double px = 0., double py = 0., double pz = 0., double e = 0., double m = 0., double scale = 0., double pol = 9.)  
constructs a particle with the input properties provided, and non-provided ones set 0 (9 for pol).

Particle::Particle(int id, int status, int mother1, int mother2, int daughter1, int daughter2, int col, int acol, Vec4 p, double m = 0., double scale = 0., double pol = 9.)  
constructs a particle with the input properties provided, and non-provided ones set 0 (9 for pol).

Particle::Particle(const Particle& pt)  
constructs an particle that is a copy of the input one.

Particle& Particle::operator=(const Particle& pt)  
copies the input particle.

void Particle::setEvtPtr(Event* evtPtr)  
sets the pointer to the Event object the particle belongs to. This method is automatically called when a particle is appended to an event record. Also calls setPDEPtr below.

void Particle::setPDEPtr(ParticleDataEntry* pdePtr = 0)  
sets the pointer to the ParticleDataEntry object of the particle, based on its current id code. If the particle belongs to an event there is no need to provide the input argument. As explained above, a valid ParticleDataEntry pointer is needed for the methods that provide information generic to the particle species. pythia8-8.1.80.orig/htmldoc/ExtraDimensionalProcesses.html0000644000175000017500000007220612217615311022014 0ustar sunsun Extra-Dimensional Processes

Extra-Dimensional Processes

Scenarios with extra dimensions (ED) allow a multitude of processes. Currently three different categories of processes are implemented. The first involves the production of excited Kaluza Klein states within so-called Randall-Sundrum (RS) scenarios, the second is related to resonance production in TeV-1 sized extra dimensions and the third relates to phenomena from large extra dimensions (LED). Due to the close relation between the LED model and a so-called unparticle model, similar unparticle processes are also kept in this section.

Randall-Sundrum Resonances, production processes

The graviton (G*) and gluon (KKgluon*) resonance states are assigned PDG code 5100039 and 5100021 respectively. The G* processes are described in [Bij01] and the KKgluon* process in [Ask11]. Decays into fermion and boson pairs are handled with the correct angular distributions, while subsequent decays are handled isotropically.

There are two lowest-order processes that together normally should be sufficient for a simulation of G^* production.

flag  ExtraDimensionsG*:all   (default = off)
Common switch for the group of lowest-order G^* production processes, i.e. the two ones below.

flag  ExtraDimensionsG*:gg2G*   (default = off)
Scatterings g g -> G^*. Code 5001.

flag  ExtraDimensionsG*:ffbar2G*   (default = off)
Scatterings f fbar -> G^*. Code 5002.

In addition there are three first-order processes included. These are of less interest, but can be used for dedicated studies of the high-pT tail of G^* production. As usual, it would be double counting to include the lowest-order and first-order processes simultaneously. Therefore the latter ones are not included with the ExtraDimensionsG*:all = on option. In this set of processes all decay angles are assumed isotropic.

flag  ExtraDimensionsG*:gg2G*g   (default = off)
Scatterings g g -> G^* g. Code 5003.

flag  ExtraDimensionsG*:qg2G*q   (default = off)
Scatterings q g -> G^* q. Code 5004.

flag  ExtraDimensionsG*:qqbar2G*g   (default = off)
Scatterings q qbar -> G^* g. Code 5005.

There is also one process for the production of a gluon resonance.

flag  ExtraDimensionsG*:qqbar2KKgluon*   (default = off)
Scatterings q qbar -> g^*/KKgluon^*. Code 5006.

Randall-Sundrum Resonances, parameters

In the above scenario the main free parameters are the masses, which are set as usual. In addition there are the following coupling parameters. The coupling kappaMG follows the conventions in [Bij01], where as the flavour dependent couplings follow the conventions used in [Dav01].

flag  ExtraDimensionsG*:SMinBulk   (default = off)
Parameter to choose between the two scenarios: off, SM on the TeV brane (common kappaMG coupling); on, SM in the ED bulk (flavour dependent couplings). This parameter is only relevant for the lowest-order graviton (G*) processes, where as the first-order processes corresponds to the off scenario.

flag  ExtraDimensionsG*:VLVL   (default = on)
Parameter to specify Z/W coupling scenario: off, usual Z/W boson couplings; on, coupling only to longitudinal Z/W bosons. In both cases the GZZ and GWW values are used and this parameter is only relevant when SMinBulk = on. The formulas for longitudinal bosons should be appropriate up to O(m_V/E_V) corrections.

parm  ExtraDimensionsG*:kappaMG   (default = 0.054; minimum = 0.0)
dimensionless coupling, which enters quadratically in all partial widths of the G^*. Is kappa m_G* = sqrt(2) x_1 k / Mbar_Pl, where x_1 = 3.83 is the first zero of the J_1 Bessel function and Mbar_Pl is the modified Planck mass.

parm  ExtraDimensionsG*:Gll   (default = 0.0; minimum = 0.0)
Coupling between graviton and leptons.

parm  ExtraDimensionsG*:Gqq   (default = 0.0; minimum = 0.0)
Coupling between graviton and light quarks.

parm  ExtraDimensionsG*:Gbb   (default = 0.0; minimum = 0.0)
Coupling between graviton and bottom quark.

parm  ExtraDimensionsG*:Gtt   (default = 0.001; minimum = 0.0)
Coupling between graviton and top quark.

parm  ExtraDimensionsG*:Ggg   (default = 0.000013; minimum = 0.0)
Coupling between graviton and gluon.

parm  ExtraDimensionsG*:Ggmgm   (default = 0.000013; minimum = 0.0)
Coupling between graviton and gamma.

parm  ExtraDimensionsG*:GZZ   (default = 0.001; minimum = 0.0)
Coupling between graviton and Z boson.

parm  ExtraDimensionsG*:GWW   (default = 0.001; minimum = 0.0)
Coupling between graviton and W boson.

parm  ExtraDimensionsG*:Ghh   (default = 0.001; minimum = 0.0)
Coupling between graviton and Higgs bosons.

parm  ExtraDimensionsG*:KKgqR   (default = -0.2)
Coupling between KK-gluon and a right-handed light quark.

parm  ExtraDimensionsG*:KKgqL   (default = -0.2)
Coupling between KK-gluon and a left-handed light quark.

parm  ExtraDimensionsG*:KKgbR   (default = -0.2)
Coupling between KK-gluon and a right-handed bottom quark.

parm  ExtraDimensionsG*:KKgbL   (default = 1.0)
Coupling between KK-gluon and a left-handed bottom quark.

parm  ExtraDimensionsG*:KKgtR   (default = 4.0)
Coupling between KK-gluon and a right-handed top quark.

parm  ExtraDimensionsG*:KKgtL   (default = 1.0)
Coupling between KK-gluon and a left-handed top quark.

mode  ExtraDimensionsG*:KKintMode   (default = 0; minimum = 0; maximum = 2)
Choice of full g^*/KK-gluon^* structure or not in relevant processes.
option 0 : full g^*/KK-gluon^* structure, with interference included.
option 1 : only pure gluon_{SM} contribution.
option 2 : only pure gluon_{KK} contribution.

TeV^-1 Sized Extra Dimension, production processes

This section contains a processes involving the production of electroweak KK gauge bosons, i.e. gamma_{KK}/Z_{KK}, in one TeV^-1 sized extra dimension. The process is described in [Bel10] and allows for individual final states to be specified.

flag  ExtraDimensionsTEV:ffbar2ddbar   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> d dbar , Code 5061.

flag  ExtraDimensionsTEV:ffbar2uubar   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> u ubar , Code 5062.

flag  ExtraDimensionsTEV:ffbar2ssbar   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> s sbar , Code 5063.

flag  ExtraDimensionsTEV:ffbar2ccbar   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> c cbar , Code 5064.

flag  ExtraDimensionsTEV:ffbar2bbbar   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> b bbar , Code 5065.

flag  ExtraDimensionsTEV:ffbar2ttbar   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> t tbar , Code 5066.

flag  ExtraDimensionsTEV:ffbar2e+e-   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> e+ e- , Code 5071.

flag  ExtraDimensionsTEV:ffbar2nuenuebar   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> nue nuebar , Code 5072.

flag  ExtraDimensionsTEV:ffbar2mu+mu-   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> mu+ mu- , Code 5073.

flag  ExtraDimensionsTEV:ffbar2numunumubar   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> numu numubar , Code 5074.

flag  ExtraDimensionsTEV:ffbar2tau+tau-   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> tau+ tau- , Code 5075.

flag  ExtraDimensionsTEV:ffbar2nutaunutaubar   (default = off)
Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> nutau nutaubar , Code 5076.

TeV^-1 Sized Extra Dimension, parameters

Irrespective of the parameter options used, the particle produced, gamma_{KK}/Z_{KK}, will always be assigned code 5000023.

mode  ExtraDimensionsTEV:gmZmode   (default = 3; minimum = 0; maximum = 5)
Choice of full gamma_{KK}/Z_{KK} structure or not in relevant processes.
option 0 : full gamma_{SM}/Z_{SM} structure, with interference included.
option 1 : only pure gamma_{SM} contribution.
option 2 : only pure Z_{SM} contribution.
option 3 : full gamma_{KK}/Z_{KK} structure, with interference included.
option 4 : only pure gamma_{KK} contribution, with SM interference included.
option 5 : only pure Z_{KK} contribution, with SM interference included.

parm  ExtraDimensionsTEV:nMax   (default = 10; minimum = 1; maximum = 100)
The number of included KK excitations.

parm  ExtraDimensionsTEV:mStar   (default = 4000.0; minimum = 1000.0)
The KK mass m^*, given by the inverse of the single extra dimension radius.

Large Extra Dimensions, production processes

The LED graviton, where the KK-modes normally are summed and do not give rise to phenomena individually, is assigned PDG code 5000039. The graviton emission and virtual graviton exchange processes use the same implementation as the corresponding unparticle processes, which are all described in [Ask10]. It is also possible to generate monojet events from scalar graviton emission as described in [Azu05], by turning on the option GravScalar.

Note: As discussed in [Ask09], for the graviton or unparticle emission processes the underlying Breit-Wigner mass distribution should be matched to the graviton mass spectrum in order to achieve an optimal MC efficiency.

The following lowest order graviton emission processes are available.

flag  ExtraDimensionsLED:monojet   (default = off)
Common switch for the group of lowest-order G jet emission processes, i.e. the three ones below.

flag  ExtraDimensionsLED:gg2Gg   (default = off)
Scatterings g g -> G g. Code 5021.

flag  ExtraDimensionsLED:qg2Gq   (default = off)
Scatterings q g -> G q. Code 5022.

flag  ExtraDimensionsLED:qqbar2Gg   (default = off)
Scatterings q qbar -> G g. Code 5023.

flag  ExtraDimensionsLED:ffbar2GZ   (default = off)
Scatterings f fbar -> G Z. Code 5024.

flag  ExtraDimensionsLED:ffbar2Ggamma   (default = off)
Scatterings f fbar -> G gamma. This process corresponds to the photon limit of the G Z process, as described in [Ask09]. Code 5025.

The following LED processes with virtual graviton exchange are available.

flag  ExtraDimensionsLED:ffbar2gammagamma   (default = off)
Scatterings f fbar -> (LED G*) -> gamma gamma. If the graviton contribution is zero, the results corresponds to the SM contribution, i.e. equivalent to PromptPhoton:ffbar2gammagamma. Code 5026.

flag  ExtraDimensionsLED:gg2gammagamma   (default = off)
Scatterings g g -> (LED G*) -> gamma gamma. Code 5027.

flag  ExtraDimensionsLED:ffbar2llbar   (default = off)
Scatterings f fbar -> (LED G*) -> l l , where l is a charged lepton. If the graviton contribution is zero, the results corresponds to the SM contribution, i.e. similar to WeakSingleBoson:ffbar2gmZ. Does not include t-channel amplitude relevant for e^+e^- to e^+e^- and no K-factor is used. Code 5028.

flag  ExtraDimensionsLED:gg2llbar   (default = off)
Scatterings g g -> (LED G*) -> l l. Code 5029.

Dijet production including graviton exchange is also available, using the same effective theory approach as the LED G exchange processes above or including more detailed amplitudes in accordance with [Fra11]. In case of the latter, the value of LambdaT is used as the value of the cut-off scale Lambda. For this reason the dijet processes only relates to the LED model and no unparticle versions are available. The processes are grouped together like their HardQCD equivalents and should therefore converge to the same results in the limit of an insignificant graviton contribution.

Warning: These LED dijets processes are still being validated.

flag  ExtraDimensionsLED:dijets   (default = off)
Common switch for the group of lowest-order jet jet production processes with graviton exchange, i.e. the six ones below.

flag  ExtraDimensionsLED:gg2DJgg   (default = off)
Scatterings g g -> (LED G*) -> g g. Code 5030.

flag  ExtraDimensionsLED:gg2DJqqbar   (default = off)
Scatterings g g -> (LED G*) -> q qbar. Number of outgoing flavours specified by nQuarkNew parameter below. Code 5031.

flag  ExtraDimensionsLED:qg2DJqg   (default = off)
Scatterings q g -> (LED G*) -> q g and qbar g -> (LED G*) -> qbar g. Code 5032.

flag  ExtraDimensionsLED:qq2DJqq   (default = off)
Scatterings q q(bar)' -> (LED G*) -> q q(bar)'. Including q and qbar of same or different flavours, but the outgoing flavours equals the incoming ones. Code 5033.

flag  ExtraDimensionsLED:qqbar2DJgg   (default = off)
Scatterings q qbar -> (LED G*) -> g g. Code 5034.

flag  ExtraDimensionsLED:qqbar2DJqqbarNew   (default = off)
Scatterings q qbar -> (LED G*) -> q' qbar'. Number of outgoing flavours specified by nQuarkNew parameter below. Code 5035.

Large Extra Dimensions, parameters

flag  ExtraDimensionsLED:GravScalar   (default = off)
Allow the monojet processes to produce scalar graviton emission instead of the default tensor one. The scalar option is according to the processes described in [Azu05] and includes two coupling constants below.

mode  ExtraDimensionsLED:n   (default = 2; minimum = 1)
Number of extra dimensions.

parm  ExtraDimensionsLED:MD   (default = 2000.; minimum = 100.0)
Fundamental scale of gravity in D = 4 + n dimensions.

parm  ExtraDimensionsLED:LambdaT   (default = 2000.; minimum = 100.0)
Ultraviolet cutoff parameter for the virtual graviton exchange processes.

mode  ExtraDimensionsLED:NegInt   (default = 0; minimum = 0; maximum = 1)
Allows to change sign of the interference terms in the graviton exchange processes, common in connection to using the Hewett convention [Hew99].
option 0 : 1
option 1 : -1

mode  ExtraDimensionsLED:CutOffMode   (default = 0; minimum = 0; maximum = 3)
Options for when the hard scale of the process (e.g. sHat) approaches or exceed the scale of validity of the low energy effective theory (e.g. M_D). Note: Option 1 only concerns the graviton emission processes and the form factor is currently not available for the scalar graviton processes.
option 0 : Do nothing, i.e. all values of sHat contribute.
option 1 : Truncate contributing sHat region ([Ask09]).
option 2 : Form factor, using mu = renormScale2 .
option 3 : Form factor, using mu = E_jet.

parm  ExtraDimensionsLED:t   (default = 1.; minimum = 0.001)
Form factor parameter.

parm  ExtraDimensionsLED:g   (default = 1.0; minimum = 0.0)
Coupling related to scalar graviton emission.

parm  ExtraDimensionsLED:c   (default = 1.0; minimum = 0.0)
Coupling related to scalar graviton emission.

mode  ExtraDimensionsLED:nQuarkNew   (default = 3; minimum = 0; maximum = 5)
Number of allowed outgoing new quark flavours in the above q qbar -> (LED G*) -> q' qbar' and g g -> (LED G*) -> q' qbar' processes. Similar to HardQCD:nQuarkNew for the QCD processes.

mode  ExtraDimensionsLED:opMode   (default = 0; minimum = 0; maximum = 1)
Options to specify S function for LED dijet amplitudes.
option 0 : Use detailed amplitude, as described in [Fra11].
option 1 : Use conventional LambdaT parametrization, like the other LED processes.

Unparticles, production processes

As mentioned above, the similar unparticle and graviton processes share the same implementations. The unparticle processes, however, only use the dedicated unparticle parameters below. The unparticle is also assigned the PDG code 5000039 and is therefore called Graviton in the event record. The graviton and unparticle emission as well as virtual graviton and unparticle exchange processes are described in [Ask10].

Note: As discussed in [Ask09], for the graviton or unparticle emission processes the underlying Breit-Wigner mass distribution should be matched to the graviton mass spectrum in order to achieve an optimal MC efficiency.

The following unparticle emission processes are available.

flag  ExtraDimensionsUnpart:monojet   (default = off)
Common switch for the group of lowest-order U jet emission processes, i.e. the three ones below.

flag  ExtraDimensionsUnpart:gg2Ug   (default = off)
Scatterings g g -> U g. Code 5045.

flag  ExtraDimensionsUnpart:qg2Uq   (default = off)
Scatterings q g -> U q. Code 5046.

flag  ExtraDimensionsUnpart:qqbar2Ug   (default = off)
Scatterings q qbar -> U g. Code 5047.

flag  ExtraDimensionsUnpart:ffbar2UZ   (default = off)
Scatterings f fbar -> U Z. Code 5041.

flag  ExtraDimensionsUnpart:ffbar2Ugamma   (default = off)
Scatterings f fbar -> U gamma. This process corresponds to the photon limit of the U Z process, as described in [Ask09]. Code 5042.

The following processes with virtual unparticle exchange are available.

flag  ExtraDimensionsUnpart:ffbar2gammagamma   (default = off)
Scatterings f fbar -> (U*) -> gamma gamma. If the unparticle contribution is zero in the spin-2 case, the results corresponds to the SM contribution, i.e. equivalent to PromptPhoton:ffbar2gammagamma. Code 5043.

flag  ExtraDimensionsUnpart:gg2gammagamma   (default = off)
Scatterings g g -> (U*) -> gamma gamma. Code 5044.

flag  ExtraDimensionsUnpart:ffbar2llbar   (default = off)
Scatterings f fbar -> (U*) -> l lbar , where l is a charged lepton. If the unparticle contribution is zero, the results corresponds to the SM contribution, i.e. similar to WeakSingleBoson:ffbar2gmZ. Does not include t-channel amplitude relevant for e^+e^- to e^+e^- and no K-factor is used. Code 5048.

flag  ExtraDimensionsUnpart:gg2llbar   (default = off)
Scatterings g g -> (U*) -> l lbar. Code 5049.

Unparticles, parameters

mode  ExtraDimensionsUnpart:spinU   (default = 2; minimum = 0; maximum = 2)
Unparticle spin.

parm  ExtraDimensionsUnpart:dU   (default = 1.4; minimum = 1.0)
Scale dimension parameter.

parm  ExtraDimensionsUnpart:LambdaU   (default = 2000.; minimum = 100.0)
Unparticle renormalization scale.

parm  ExtraDimensionsUnpart:lambda   (default = 1.0; minimum = 0.0)
Unparticle coupling to the SM fields.

parm  ExtraDimensionsUnpart:ratio   (default = 1.0; minimum = 1.0; maximum = 1.0)
Ratio, lambda'/lambda, between the two possible coupling constants of the spin-2 ME. Warning: A ratio value different from one give rise to an IR divergence which makes the event generation very slow, so this values is fixed to ratio = 1 for the moment.

mode  ExtraDimensionsUnpart:CutOffMode   (default = 0; minimum = 0; maximum = 1)
Options for when the hard scale of the process (e.g. sHat) approaches or exceed the scale of validity of the low energy effective theory (Lambda_U). This mode only concerns the unparticle emission processes.
option 0 : Do nothing, i.e. all values of sHat contribute.
option 1 : Truncate contributing sHat region ([Ask09]).

mode  ExtraDimensionsUnpart:gXX   (default = 0; minimum = 0; maximum = 2)
Chiral unparticle couplings, gXX = gLL = gRR. Only relevant for lepton production from spin-1 unparticle exchange.
option 0 : 1
option 1 : -1
option 2 : 0

mode  ExtraDimensionsUnpart:gXY   (default = 0; minimum = 0; maximum = 2)
Chiral unparticle couplings, gXY = gLR = gRL. Only relevant for lepton production from spin-1 unparticle exchange.
option 0 : 1
option 1 : -1
option 2 : 0 pythia8-8.1.80.orig/htmldoc/LesHouchesAccord.html0000644000175000017500000011511112217615312020027 0ustar sunsun Les Houches Accord

Les Houches Accord

The Les Houches Accord (LHA) for user processes [Boo01] is the standard way to input parton-level information from a matrix-elements-based generator into PYTHIA. The conventions for which information should be stored has been defined in a Fortran context, as two commonblocks. Here a C++ equivalent is defined, as a single class.

The LHAup class is a base class, containing reading and printout functions, plus two pure virtual functions, one to set initialization information and one to set information on each new event. Derived classes have to provide these two virtual functions to do the actual work. The existing derived classes are for reading information from a Les Houches Event File (LHEF), from the respective Fortran commonblocks, or from PYTHIA 8 itself.

You are free to write your own derived classes, using the rules and methods to be described below. Normally, pointers to objects of such derived classes should be handed in with the Pythia::init( LHAup*) method. However, with the LHEF format a filename can replace the pointer, see further below.

Let us now describe the methods at your disposal to do the job.

LHAup::LHAup( int strategy = 3)  
the base class constructor takes the choice of mixing/weighting strategy as optional input argument, and calls setStrategy, see below. It also reserves some space for processes and particles.

virtual LHAup::~LHAup()  
the destructor does not need to do anything.

void LHAup::setPtr(Info* infoPtr)  
this method only sets the pointer that allows some information to be accessed, and is automatically called by Pythia::init(...).

Initialization

The LHAup class stores information equivalent to the /HEPRUP/ commonblock, as required to initialize the event generation chain. The main difference is that the vector container now allows a flexible number of subprocesses to be defined. For the rest, names have been modified, since the 6-character-limit does not apply, and variables have been regrouped for clarity, but nothing fundamental is changed.

virtual bool LHAup::setInit()  
this pure virtual method has to be implemented in the derived class, to set relevant information when called. It should return false if it fails to set the info.

Inside setInit(), such information can be set by the following methods:

void LHAup::setBeamA( int identity, double energy, int pdfGroup, int pdfSet)  
void LHAup::setBeamB( int identity, double energy, int pdfGroup, int pdfSet)  
sets the properties of the first and second incoming beam, respectively (cf. the Fortran IDBMUP(1), EBMUP(i), PDFGUP(i), PDFSUP(i), with i 1 or 2). The parton distribution information defaults to zero. These numbers can be used to tell which PDF sets were used when the hard process was generated, while the normal PDF Selection is used for the further event generation in PYTHIA.

void LHAup::setStrategy( int strategy)  
sets the event weighting and cross section strategy. The default, provided in the class constructor, is 3, which is the natural value e.g. for an LHEF.
argument strategy : chosen strategy (cf. IDWTUP; see [Sjo06] section 9.9.1 for extensive comments).
argumentoption 1 : events come with non-negative weight, given in units of pb, with an average that converges towards the cross section of the process. PYTHIA is in charge of the event mixing, i.e. for each new try decides which process should be generated, and then decides whether is should be kept, based on a comparison with xMax. Accepted events therefore have unit weight.
argumentoption -1 : as option 1, except that cross sections can now be negative and events after unweighting have weight +-1. You can use Info::weight() to find the weight of the current event. A correct event mixing requires that a process that can take both signs should be split in two, one limited to positive or zero and the other to negative or zero values, with xMax chosen appropriately for the two.
argumentoption 2 : events come with non-negative weight, in unspecified units, but such that xMax can be used to unweight the events to unit weight. Again PYTHIA is in charge of the event mixing. The total cross section of a process is stored in xSec.
argumentoption -2 : as option 2, except that cross sections can now be negative and events after unweighting have weight +-1. As for option -1 processes with indeterminate sign should be split in two.
argumentoption 3 : events come with unit weight, and are thus accepted as is. The total cross section of the process is stored in xSec.
argumentoption -3 : as option 3, except that events now come with weight +-1. Unlike options -1 and -2 processes with indeterminate sign need not be split in two, unless you intend to mix with internal PYTHIA processes (see below).
argumentoption 4 : events come with non-negative weight, given in units of pb, with an average that converges towards the cross section of the process, like for option 1. No attempt is made to unweight the events, however, but all are generated in full, and retain their original weight. For consistency with normal PYTHIA units, the weight stored in Info::weight() has been converted to mb, however.
argumentoption -4 : as option 4, except that events now can come either with positive or negative weights.
Note 1: if several processes have already been mixed and stored in a common event file, either LHEF or some private format, it would be problematical to read back events in a different order. Since it is then not feasible to let PYTHIA pick the next process type, strategies +-1 and +-2 would not work. Instead strategy 3 would be the recommended choice, or -3 if negative-weight events are required.
Note 2: it is possible to switch on internally implemented processes and have PYTHIA mix these with LHA ones according to their relative cross sections for strategies +-1, +-2 and 3. It does not work for strategy -3 unless the positive and negative sectors of the cross sections are in separate subprocesses (as must always be the case for -1 and -2), since otherwise the overall mixture of PYTHIA and LHA processes will be off. Mixing is not possible for strategies +-4, since the weighting procedure is not specified by the standard. (For instance, the intention may be to have events biased towards larger pT values in some particular functional form.)

void LHAup::addProcess( int idProcess, double xSec, double xErr, double xMax)  
sets info on an allowed process (cf. LPRUP, XSECUP, XERRUP, XMAXUP). Each new call will append one more entry to the list of processes. The choice of strategy determines which quantities are mandatory: xSec for strategies +-2 and +-3, xErr never, and xMax for strategies +-1 and +-2.
Note: PYTHIA does not make active use of the (optional) xErr values, but calculates a statistical cross section error based on the spread of event-to-event weights. This should work fine for strategy options +-1, but not for the others. Specifically, for options +-2 and +-3 the weight spread may well vanish, and anyway is likely to be an underestimate of the true error. If the author of the LHA input information does provide error information you may use that - this information is displayed at initialization. If not, then a relative error decreasing like 1/sqrt(n_acc), where n_acc is the number of accepted events, should offer a reasonable estimate.

void LHAup::setXSec( int i, double xSec)  
update the xSec value of the i'th process added with addProcess method (i.e. i runs from 0 through sizeProc() - 1, see below).

void LHAup::setXErr( int i, double xErr)  
update the xErr value of the i'th process added with addProcess method.

void LHAup::setXMax( int i, double xMax)  
update the xMax value of the i'th process added with addProcess method.

void LHAup::setInfoHeader(string &key, string &val)  
set the header key to have value val. This is a wrapper function to the Info::setHeader function that should be used in any classes derived from LHAup.

Information is handed back by the following methods (that normally you would not need to touch):

int LHAup::idBeamA()  
int LHAup::idBeamB()  
double LHAup::eBeamA()  
double LHAup::eBeamB()  
int LHAup::pdfGroupBeamA()  
int LHAup::pdfGroupBeamB()  
int LHAup::pdfSetBeamA()  
int LHAup::pdfSetBeamB()  
for the beam properties.

int LHAup::strategy()  
for the strategy choice.

int LHAup::sizeProc()  
for the number of subprocesses.

int LHAup::idProcess(i)  
double LHAup::xSec(i)  
double LHAup::xErr(i)  
double LHAup::xMax(i)  
for process i in the range 0 <= i < sizeProc().

double LHAup::xSecSum()  
double LHAup::xErrSum()  
the sum of the cross sections and errors (the latter added quadratically). Note that cross section errors are only meaningful for strategies +-3.

void LHAup::listInit(ostream& os = cout)  
prints the above initialization information. This method is automatically called from Pythia::init(...), so would normally not need to be called directly by the user.

Event input

The LHAup class also stores information equivalent to the /HEPEUP/ commonblock, as required to hand in the next parton-level configuration for complete event generation. The main difference is that the vector container now allows a flexible number of partons to be defined. For the rest, names have been modified, since the 6-character-limit does not apply, and variables have been regrouped for clarity, but nothing fundamental is changed.

The LHA standard is based on Fortran arrays beginning with index 1, and mother information is defined accordingly. In order to be compatible with this convention, the zeroth line of the C++ particle array is kept empty, so that index 1 also here corresponds to the first particle. One small incompatibility is that the sizePart() method returns the full size of the particle array, including the empty zeroth line, and thus is one larger than the true number of particles (NUP).

virtual bool LHAup::setEvent(int idProcess = 0, double mRecalculate = -1.)  
this pure virtual method has to be implemented in the derived class, to set relevant information when called. For strategy options +-1 and +-2 the input idProcess value specifies which process that should be generated, while idProcess is irrelevant for strategies +-3 and +-4. The mRecalculate input alllows an optional recalculation of the mass from the four-momentum, see LesHouches::mRecalculate below. The method should return false if it fails to set the info, i.e. normally that the supply of events in a file is exhausted. If so, no event is generated, and Pythia::next() returns false. You can then interrogate Info::atEndOfFile() to confirm that indeed the failure is caused in this method, and decide to break out of the event generation loop.

Inside a normal setEvent(...) call, information can be set by the following methods:

void LHAup::setProcess( int idProcess, double weight, double scale, double alphaQED, double alphaQCD)  
tells which kind of process occurred, with what weight, at what scale, and which alpha_EM and alpha_strong were used (cf. IDPRUP, XWTGUP, SCALUP, AQEDUP, AQCDUP). This method also resets the size of the particle list, and adds the empty zeroth line, so it has to be called before the addParticle method below.

void LHAup::addParticle( int id, int status, int mother1, int mother2, int colourTag1, int colourTag2, double p_x, double p_y, double p_z, double e, double m, double tau, double spin, double scale)  
gives the properties of the next particle handed in (cf. IDUP, ISTUP, MOTHUP(1,..), MOTHUP(2,..), ICOLUP(1,..), ICOLUP(2,..), PUP(J,..), VTIMUP, SPINUP; while scale is a new optional property, see further below) .

Information is handed back by the following methods:

int LHAup::idProcess()  
process number.

double LHAup::weight()  
Note that the weight stored in Info::weight() as a rule is not the same as the above weight(): the method here gives the value before unweighting while the one in info gives the one after unweighting and thus normally is 1 or -1. Only with strategy options +-3 and +-4 would the value in info be the same as here, except for a conversion from pb to mb for +-4.

double LHAup::scale()  
double LHAup::alphaQED()  
double LHAup::alphaQCD()  
scale and couplings at that scale.

int LHAup::sizePart()  
the size of the particle array, which is one larger than the number of particles in the event, since the zeroth entry is kept empty (see above).

int LHAup::id(int i)  
int LHAup::status(int i)  
int LHAup::mother1(int i)  
int LHAup::mother2(int i)  
int LHAup::col1(int i)  
int LHAup::col2(int i)  
double LHAup::px(int i)  
double LHAup::py(int i)  
double LHAup::pz(int i)  
double LHAup::e(int i)  
double LHAup::m(int i)  
double LHAup::tau(int i)  
double LHAup::spin(int i)  
double LHAup::scale(int i)  
for particle i in the range 0 <= i < sizePart(). (But again note that i = 0 is an empty line, so the true range begins at 1.)

From the information in the event record it is possible to set the flavour and x values of the initiators

void LHAup::setIdX(int id1, int id2, double x1, double x2)  

This information is returned by the methods

int LHAup::id1()  
int LHAup::id2()  
double LHAup::x1()  
double LHAup::x2()  

In the LHEF description [Alw06] an extension to include information on the parton densities of the colliding partons is suggested. This optional further information can be set by

void LHAup::setPdf( int id1pdf, int id2pdf, double x1pdf, double x2pdf, double scalePDF, double pdf1, double pdf2, bool pdfIsSet)  
which gives the flavours , the x and the Q scale (in GeV) at which the parton densities x*f_i(x, Q) have been evaluated. The last argument is normally true.

This information is returned by the methods

bool LHAup::pdfIsSet()  
int LHAup::id1pdf()  
int LHAup::id2pdf()  
double LHAup::x1pdf()  
double LHAup::x2pdf()  
double LHAup::scalePDF()  
double LHAup::pdf1()  
double LHAup::pdf2()  
where the first one tells whether this optional information has been set for the current event. (setPdf(...) must be called after the setProcess(...) call of the event for this to work.) Note that the flavour and x values usually but not always agree with those obtained by the same methods without pdf in their names, see explanation in the Event Information description.

As a further, currently completely non-standard feature, it is also possible to read in the separate scale values of all final particles. Currently such information should appear as a line begun by a single hashtag character (#) and then sequentially the scale value of all particles with status 1. Such scale values could be used e.g. to restrict the maximum scale for shower evolutions for each parton separately. This information is returned by the method double LHAup::scale(int i). When no such information has been read from the LHEF, the scale defaults to -1.

void LHAup::listEvent(ostream& os = cout)  
prints the above information for the current event. In cases where the LHAup object is not available to the user, the Pythia::LHAeventList(ostream& os = cout) method can be used, which is a wrapper for the above.

virtual bool LHAup::skipEvent(int nSkip)  
skip ahead nSkip events in the Les Houches generation sequence, without doing anything further with them. Mainly intended for debug purposes, e.g. when an event at a known location in a Les Houches Event File is causing problems. Will return false if operation fails, specifically if the end of an LHEF has been reached. The implementation in the base class simply executes setEvent() the requested number of times. The derived LHAupLHEF class (see below) only uses the setNewEventLHEF(...) part of its setEvent() method, and other derived classes could choose other shortcuts.

The LHA expects the decay of resonances to be included as part of the hard process, i.e. if unstable particles are produced in a process then their decays are also described. This includes Z^0, W^+-, H^0 and other short-lived particles in models beyond the Standard Model. Should this not be the case then PYTHIA will perform the decays of all resonances it knows how to do, in the same way as for internal processes. Note that you will be on slippery ground if you then restrict the decay of these resonances to specific allowed channels since, if this is not what was intended, you will obtain the wrong cross section and potentially the wrong mix of different event types. (Since the original intention is unknown, the cross section will not be corrected for the fraction of open channels, i.e. the procedure used for internal processes is not applied in this case.)

Even if PYTHIA can select resonance decay modes according to its internal tables, there is normally no way for it to know which decay angular correlations should exist in the simulated process. Therefore almost all decays are isotropic. The exceptions are Higgs and top decays, in the decay chains H -> WW/ZZ -> f fbar f' fbar' and t -> b W -> b f fbar, where the process-independent correlations implemented for internal processes are used. If part of the decay chain has already been set, however (e.g. H -> WW/ZZ or t -> b W), then decay is still isotropic.

There is one setting available for event input.

mode  LesHouches:setLifetime   (default = 1; minimum = 0; maximum = 2)
handling of the decay time information stored in VTIMUP when the Les Houches event record is stored into the PYTHIA process one. The reason is that some matrix-element generators (like POWHEG) do not set decay times, so that it is up to PYTHIA to make that selection. This is particularly important for the tau lepton.
option 0 : all decay times are taken from the Les Houches input.
option 1 : the decay time of tau leptons is generated like for internal PYTHIA taus, whereas all other decay times are taken from the Les Houches input.
option 2 : all decay times are generated by PYTHIA, thus completely disregarding the Les Houches values. This option could go wrong in BSM scenarios with long-lived particles, if PYTHIA has not been provided with the information to select those lifetimes correctly.

There is also one parameter that can be used to modify the setting of event information, if implemented in the derived class. It is prompted by an unforeseen choice made in some programs (like CalcHEP) of storing the nominal mass of a particle species rather than the mass of the current member of that species. This is likely to induce energy-momentum nonconservation when the event is further processed.

parm  LesHouches:mRecalculate   (default = -1.)
Does not have any effect by default, or more generally when it is negative. If it is positive then all particles with an input mass above this value will have the mass recalculated and reset from the four-momentum, m^2 = E^2 - p^2. Obviously such a step is problematic numerically for light particles, so it should only be used for the programs and particles where it is needed. Thus the value ought to be at least 10 GeV, so that only massive particles like W^+-, Z^0 and t are affected.

An interface to Les Houches Event Files

The LHEF standard [Alw06] specifies a format where a single file packs initialization and event information. This has become the most frequently used procedure to process external parton-level events in Pythia. Therefore a special Pythia::init(fileName) initialization option exists, where the LHEF name is provided as input. Internally this name is then used to create an instance of the derived class LHAupLHEF, which can do the job of reading an LHEF.

The LHEF reader can also read in and store header blocks. By default this option is switched on, but may be controlled through the Beams:readLHEFheaders flag if necessary. The information can later be read out through the Info class for further processing. Due to the non-standard nature of the information in these blocks they are stored whole, and PYTHIA itself makes no further attempt to process their meaning.

Because Les Houches Event files tend not to adhere strictly to XML conventions, to consistently read in header information, certain choices must be made. The primary goal is to make as much information available as possible. First, information sitting directly in the <header> block is stored under the key "base". Second, the tags starting and ending each sub block must be on their own line. Finally, the contents of comment blocks, <!-- -->, are still stored. The header keys are formed hierarchically from the names of the header blocks. This behaviour is illustrated in the following example:

  <header>
    BaseA
    <hblock1>
      1A
      <hblock11>
        11A <hblock111>
        </hblock111> 11B
      </hblock11>
      1B
    </hblock1>
    <hblock2>
      2A
      <!-- 2B -->
    </hblock2>
    BaseB
  </header>
which would lead to the following information being stored in the Info class:
Key Value
base BaseA
BaseB
hblock1 1A
1B
hblock1.hblock11 11A <hblock111>
</hblock111> 11B
hblock2 2A
<!-- 2B -->

Normally the LHEF would be in uncompressed format, and thus human-readable if opened in a text editor. A possibility to read gzipped files has been added, based on the Boost and zlib libraries, which therefore have to be linked appropriately in order for this option to work. See the README file in the main directory for details on how to do this.

An example how to generate events from an LHEF is found in main11.cc. Note the use of Info::atEndOfFile() to find out when the whole LHEF has been processed.

To allow the sequential use of several event files the Pythia::init(...) method has an optional second argument: Pythia::init(fileName, bool skipInit = false). If called with this argument true then there will be no initialization, except that the existing LHAupLHEF class instance will be deleted and replaced by ones pointing to the new file. It is assumed (but never checked) that the initialization information is identical, and that the new file simply contains further events of exactly the same kind as the previous one. An example of this possibility, and the option to mix with internal processes, is found in main12.cc. A variant, based on input in a command file, is given in main13.cc.

In C++, real numbers are printed with an 'E' to denote the exponent part, e.g. 1.23E+04, and are read in accordingly. Other languages may use other letters, e.g. Fortran allows either 'E' or 'D'. A file using the latter convention would not be readable by the standard routines. In case you have such an "incorrectly formatted" file, a conversion to a new corrected file could be done e.g. using sed, as a one-line command

  sed -e 's/\([0-9]\.\{0,1\}\)[dD]\([+-]\{0,1\}[0-9]\)/\1E\2/g' old.lhe > new.lhe
This replaces a 'd' or 'D' with an 'E' only when it occurs in the combination
(digit) ('.' or absent) ('d' or 'D') ('+', '-' or absent) (digit)
It will work on all parts of the file, also inside a <header>...</header> block. For conversion only inside the <init>...</init> and <event>...</event> blocks, create a file convert.sed containing
  /<init>/,/<\/init>/bconv
  /<event>/,/<\/event>/bconv
  b
  :conv
  s/\([0-9]\.\{0,1\}\)[dD]\([+-]\{0,1\}[0-9]\)/\1E\2/g
and run it with
  sed -f convert.sed old.lhe > new.lhe

The workhorses of the LHAupLHEF class are three methods found in the base class, so as to allow them to be reused in other contexts. Specifically, it allows derived classes where one parton-level configuration can be reused several times, e.g. in the context of matrix-element-to-parton-shower matching (example in preparation). Also two small utility routines.

bool LHAup::setInitLHEF(ifstream& is, bool readHeaders = false)  
read in and set all required initialization information from the specified stream. With second argument true it will also read and store header information, as described above. Return false if it fails.

bool LHAup::setNewEventLHEF(ifstream& is)  
read in event information from the specified stream into a staging area where it can be reused by setOldEventLHEF.

bool LHAup::setOldEventLHEF()  
store the event information from the staging area into the normal location. Thus a single setNewEventLHEF call can be followed by several setOldEventLHEF ones, so as to process the same configuration several times. This method currently only returns true, i.e. any errors should be caught by the preceding setNewEventLHEF call.

bool LHAup::fileFound()  
always returns true in the base class, but in LHAupLHEF it returns false if the LHEF provided in the constructor is not found and opened correctly.

void LHAup::setInfoHeader(const string &key, const string &val)  
is used to send header information on to the Info class.

A few other methods, most of them derived from the base class, streamlines file opening and closing, e.g. if several LHE files are to be read consecutively, without the need for a complete reinitialization. This presupposes that the events are of the same kind, only split e.g. to limit file sizes.

bool LHAup::newEventFile(const char* fileIn)  
close current event input file/stream and open a new one, to continue reading events of the same kind as before.

istream* LHAup::openFile(const char *fn, ifstream &ifs)  
void LHAup::closeFile(istream *&is, ifstream &ifs)  
open and close a file, also gzip files, where an intermediate decompression layer is needed.

void LHAupLHEF::closeAllFiles()  
close main event file (LHEF) and, if present, separate header file.

A runtime Fortran interface

The runtime Fortran interface requires linking to an external Fortran code. In order to avoid problems with unresolved external references when this interface is not used, the code has been put in a separate LHAFortran.h file, that is not included in any of the other library files. Instead it should be included in the user-supplied main program, together with the implementation of two methods below that call the Fortran program to do its part of the job.

The LHAupFortran class derives from LHAup. It reads initialization and event information from the LHA standard Fortran commonblocks, assuming these commonblocks behave like two extern "C" struct named heprup_ and hepeup_. (Note the final underscore, to match how the gcc compiler internally names Fortran files.)

The instantiation does not require any arguments.

The user has to supply implementations of the fillHepRup() and fillHepEup() methods, that is to do the actual calling of the external Fortran routines that fill the HEPRUP and HEPEUP commonblocks. The translation of this information to the C++ structure is provided by the existing setInit() and setEvent() code.

Up to and including version 8.125 the LHAupFortran class was used to construct a runtime interface to PYTHIA 6.4. This was convenient in the early days of PYTHIA 8 evolution, when this program did not yet contain hard-process generation, and the LHEF standard did not yet exist. Nowadays it is more of a bother, since a full cross-platform support leads to many possible combinations. Therefore this support has been removed, but can still be recuperated from previous code versions, in a reduced form up to version 8.176.

Methods for LHEF output

The main objective of the LHAup class is to feed information from an external program into PYTHIA. It can be used to export information as well, however. Specifically, there are four routines in the base class that can be called to write a Les Houches Event File. These should be called in sequence in order to build up the proper file structure.

bool LHAup::openLHEF(string filename)  
Opens a file with the filename indicated, and writes a header plus a brief comment with date and time information.

bool LHAup::initLHEF()  
Writes initialization information to the file above. Such information should already have been set with the methods described in the "Initialization" section above.

bool LHAup::eventLHEF(bool verbose = true)  
Writes event information to the file above. Such information should already have been set with the methods described in the "Event input" section above. This call should be repeated once for each event to be stored. By default the event information is lined up in columns. To save space, the alternative verbose = false only leaves a single blank between the information fields.

bool LHAup::closeLHEF(bool updateInit = false)  
Writes the closing tag and closes the file. Optionally, if updateInit = true, this routine will reopen the file from the beginning, rewrite the same header as openLHEF() did, and then call initLHEF() again to overwrite the old information. This is especially geared towards programs, such as PYTHIA itself, where the cross section information is not available at the beginning of the run, but only is obtained by Monte Carlo integration in parallel with the event generation itself. Then the setXSec( i, xSec), setXErr( i, xSec) and setXMax( i, xSec) can be used to update the relevant information before closeLHEF is called.
Warning: overwriting the beginning of a file without upsetting anything is a delicate operation. It only works when the new lines require exactly as much space as the old ones did. Thus, if you add another process in between, the file will be corrupted.

PYTHIA 8 output to an LHEF

The above methods could be used by any program to write an LHEF. For PYTHIA 8 to do this, a derived class already exists, LHAupFromPYTHIA8. In order for it to do its job, it must gain access to the information produced by PYTHIA, specifically the process event record and the generic information stored in info. Therefore, if you are working with an instance pythia of the Pythia class, you have to instantiate LHAupFromPYTHIA8 with pointers to the process and info objects of pythia:
LHAupFromPYTHIA8 myLHA(&pythia.process, &pythia.info);

The method setInit() should be called to store the pythia initialization information in the LHA object, and setEvent() to store event information. Furthermore, updateSigma() can be used at the end of the run to update cross-section information, cf. closeLHEF(true) above. An example how the generation, translation and writing methods should be ordered is found in main20.cc.

Currently there are some limitations, that could be overcome if necessary. Firstly, you may mix many processes in the same run, but the cross-section information stored in info only refers to the sum of them all, and therefore they are all classified as a common process 9999. Secondly, you should generate your events in the CM frame of the collision, since this is the assumed frame of stored Les Houches events, and no boosts have been implemented for the case that Pythia::process is not in this frame.

The LHEF standard is the agreed format to store the particles of a hard process, as input to generators, whereas output of final states is normally handled using the HepMC standard. It is possible to use LHEF also here, however. It requires that the above initialization is replaced by
LHAupFromPYTHIA8 myLHA(&pythia.event, &pythia.info);
i.e. that process is replaced by event. In addition, the PartonLevel:all = off command found in main20.cc obviously must be removed if one wants to obtain complete events. pythia8-8.1.80.orig/htmldoc/ASecondHardProcess.html0000644000175000017500000004637112217615311020335 0ustar sunsun A Second Hard Process

A Second Hard Process

When you have selected a set of hard processes for hadron beams, the multiparton interactions framework can add further interactions to build up a realistic underlying event. These further interactions can come from a wide variety of processes, and will occasionally be quite hard. They do represent a realistic random mix, however, which means one cannot predetermine what will happen. Occasionally there may be cases where one wants to specify also the second hard interaction rather precisely. The options on this page allow you to do precisely that.

flag  SecondHard:generate   (default = off)
Generate two hard scatterings in a collision between hadron beams. The hardest process can be any combination of internal processes, available in the normal process selection machinery, or external input. Here you must further specify which set of processes to allow for the second hard one, see the following.

Process Selection

In principle the whole process selection allowed for the first process could be repeated for the second one. However, this would probably be overkill. Therefore here a more limited set of prepackaged process collections are made available, that can then be further combined at will. Since the description is almost completely symmetric between the first and the second process, you always have the possibility to pick one of the two processes according to the complete list of possibilities.

Here comes the list of allowed sets of processes, to combine at will:

flag  SecondHard:TwoJets   (default = off)
Standard QCD 2 -> 2 processes involving gluons and d, u, s, c, b quarks.

flag  SecondHard:PhotonAndJet   (default = off)
A prompt photon recoiling against a quark or gluon jet.

flag  SecondHard:TwoPhotons   (default = off)
Two prompt photons recoiling against each other.

flag  SecondHard:Charmonium   (default = off)
Production of charmonium via colour singlet and colour octet channels.

flag  SecondHard:Bottomonium   (default = off)
Production of bottomonium via colour singlet and colour octet channels.

flag  SecondHard:SingleGmZ   (default = off)
Scattering q qbar -> gamma^*/Z^0, with full interference between the gamma^* and Z^0.

flag  SecondHard:SingleW   (default = off)
Scattering q qbar' -> W^+-.

flag  SecondHard:GmZAndJet   (default = off)
Scattering q qbar -> gamma^*/Z^0 g and q g -> gamma^*/Z^0 q.

flag  SecondHard:WAndJet   (default = off)
Scattering q qbar' -> W^+- g and q g -> W^+- q'.

flag  SecondHard:TopPair   (default = off)
Production of a top pair, either via QCD processes or via an intermediate gamma^*/Z^0 resonance.

flag  SecondHard:SingleTop   (default = off)
Production of a single top, either via a t- or an s-channel W^+- resonance.

A further process collection comes with a warning flag:

flag  SecondHard:TwoBJets   (default = off)
The q qbar -> b bbar and g g -> b bbar processes. These are already included in the TwoJets sample above, so it would be double-counting to include both, but we assume there may be cases where the b subsample will be of special interest. This subsample does not include flavour-excitation or gluon-splitting contributions to the b rate, however, so, depending on the topology if interest, it may or may not be a good approximation.

Cuts and scales

The second hard process obeys exactly the same selection rules for phase space cuts and couplings and scales as the first one does. Specifically, a pTmin cut for 2 -> 2 processes would apply to the first and the second hard process alike, and ballpark half of the time the second could be generated with a larger pT than the first. (Exact numbers depending on the relative shape of the two cross sections.) That is, first and second is only used as an administrative distinction between the two, not as a physics ordering one.

Optionally it is possible to pick the mass and pT phase space cuts separately for the second hard interaction. The main application presumably would be to allow a second process that is softer than the first, but still hard. But one is also free to make the second process harder than the first, if desired. So long as the two pT (or mass) ranges overlap the ordering will not be the same in all events, however.

Cross-section calculation

As an introduction, a brief reminder of Poissonian statistics. Assume a stochastic process in time, for now not necessarily a high-energy physics one, where the probability for an event to occur at any given time is independent of what happens at other times. Then the probability for n events to occur in a finite time interval is
P_n = <n>^n exp(-<n>) / n!
where <n> is the average number of events. If this number is small we can approximate exp(-<n>) = 1 , so that P_1 = <n> and P_2 = <n>^2 / 2 = P_1^2 / 2.

Now further assume that the events actually are of two different kinds a and b, occurring independently of each other, such that <n> = <n_a> + <n_b>. It then follows that the probability of having one event of type a (or b) and nothing else is P_1a = <n_a> (or P_1b = <n_b>). From
P_2 = (<n_a> + <n_b>)^2 / 2 = (P_1a + P_1b)^2 / 2 = (P_1a^2 + 2 P_1a P_1b + P_1b^2) / 2
it is easy to read off that the probability to have exactly two events of kind a and none of b is P_2aa = P_1a^2 / 2 whereas that of having one a and one b is P_2ab = P_1a P_1b. Note that the former, with two identical events, contains a factor 1/2 while the latter, with two different ones, does not. If viewed in a time-ordered sense, the difference is that the latter can be obtained two ways, either first an a and then a b or else first a b and then an a.

To translate this language into cross-sections for high-energy events, we assume that interactions can occur at different pT values independently of each other inside inelastic nondiffractive (sometimes equated with "minbias") events. Then the above probabilities translate into P_n = sigma_n / sigma_ND where sigma_ND is the total nondiffractive cross section. Again we want to assume that exp(-<n>) is close to unity, i.e. that the total hard cross section above pTmin is much smaller than sigma_ND. The hard cross section is dominated by QCD jet production, and a reasonable precaution is to require a pTmin of at least 20 GeV at LHC energies. (For 2 -> 1 processes such as q qbar -> gamma^*/Z^0 (-> f fbar) one can instead make a similar cut on mass.) Then the generic equation P_2 = P_1^2 / 2 translates into sigma_2/sigma_ND = (sigma_1 / sigma_ND)^2 / 2 or sigma_2 = sigma_1^2 / (2 sigma_ND).

Again different processes a, b, c, ... contribute, and by the same reasoning we obtain sigma_2aa = sigma_1a^2 / (2 sigma_ND), sigma_2ab = sigma_1a sigma_1b / sigma_ND, and so on.

There is one important correction to this picture: all collisions do no occur under equal conditions. Some are more central in impact parameter, others more peripheral. This leads to a further element of variability: central collisions are likely to have more activity than the average, peripheral less. Integrated over impact parameter standard cross sections are recovered, but correlations are affected by a "trigger bias" effect: if you select for events with a hard process you favour events at small impact parameter which have above-average activity, and therefore also increased chance for further interactions. (In PYTHIA this is the origin of the "pedestal effect", i.e. that events with a hard interaction have more underlying activity than the level found in minimum-bias events.) When you specify a matter overlap profile in the multiparton-interactions scenario, such an enhancement/depletion factor f_impact is chosen event-by-event and can be averaged during the course of the run. As an example, the double Gaussian form used in Tune A gives approximately <f_impact> = 2.5. The above equations therefore have to be modified to sigma_2aa = <f_impact> sigma_1a^2 / (2 sigma_ND), sigma_2ab = <f_impact> sigma_1a sigma_1b / sigma_ND. Experimentalists often instead use the notation sigma_2ab = sigma_1a sigma_1b / sigma_eff, from which we see that PYTHIA "predicts" sigma_eff = sigma_ND / <f_impact>. When the generation of multiparton interactions is switched off it is not possible to calculate <f_impact> and therefore it is set to unity.

When this recipe is to be applied to calculate actual cross sections, it is useful to distinguish three cases, depending on which set of processes are selected to study for the first and second interaction.

(1) The processes a for the first interaction and b for the second one have no overlap at all. For instance, the first could be TwoJets and the second TwoPhotons. In that case, the two interactions can be selected independently, and cross sections tabulated for each separate subprocess in the two above classes. At the end of the run, the cross sections in a should be multiplied by <f_impact> sigma_1b / sigma_ND to bring them to the correct overall level, and those in b by <f_impact> sigma_1a / sigma_ND.

(2) Exactly the same processes a are selected for the first and second interaction. In that case it works as above, with a = b, and it is only necessary to multiply by an additional factor 1/2. A compensating factor of 2 is automatically obtained for picking two different subprocesses, e.g. if TwoJets is selected for both interactions, then the combination of the two subprocesses q qbar -> g g and g g -> g g can trivially be obtained two ways.

(3) The list of subprocesses partly but not completely overlap. For instance, the first process is allowed to contain a or c and the second b or c, where there is no overlap between a and b. Then, when an independent selection for the first and second interaction both pick one of the subprocesses in c, half of those events have to be thrown, and the stored cross section reduced accordingly. Considering the four possible combinations of first and second process, this gives a
sigma'_1 = sigma_1a + sigma_1c * (sigma_2b + sigma_2c/2) / (sigma_2b + sigma_2c)
with the factor 1/2 for the sigma_1c sigma_2c term. At the end of the day, this sigma'_1 should be multiplied by the normalization factor
f_1norm = <f_impact> (sigma_2b + sigma_2c) / sigma_ND
here without a factor 1/2 (or else it would have been double-counted). This gives the correct
(sigma_2b + sigma_2c) * sigma'_1 = sigma_1a * sigma_2b + sigma_1a * sigma_2c + sigma_1c * sigma_2b + sigma_1c * sigma_2c/2
The second interaction can be handled in exact analogy.

For the considerations above it is assumed that the phase space cuts are the same for the two processes. It is possible to set the mass and transverse momentum cuts differently, however. This changes nothing for processes that already are different. For two collisions of the same type it is partly a matter of interpretation what is intended. If we consider the case of the same process in two non-overlapping phase space regions, most likely we want to consider them as separate processes, in the sense that we expect a factor 2 relative to Poissonian statistics from either of the two hardest processes populating either of the two phase space regions. In total we are therefore lead to adopt the same strategy as in case (3) above: only in the overlapping part of the two allowed phase space regions could two processes be identical and thus appear with a 1/2 factor, elsewhere the two processes are never identical and do not include the 1/2 factor. We reiterate, however, that the case of partly but not completely overlapping phase space regions for one and the same process is tricky, and not to be used without prior deliberation.

The listing obtained with the pythia.statistics() already contain these corrections factors, i.e. cross sections are for the occurrence of two interactions of the specified kinds. There is not a full tabulation of the matrix of all the possible combinations of a specific first process together with a specific second one (but the information is there for the user to do that, if desired). Instead pythia.statistics() shows this matrix projected onto the set of processes and associated cross sections for the first and the second interaction, respectively. Up to statistical fluctuations, these two sections of the pythia.statistics() listing both add up to the same total cross section for the event sample.

There is a further special feature to be noted for this listing, and that is the difference between the number of "selected" events and the number of "accepted" ones. Here is how that comes about. Originally the first and second process are selected completely independently. The generation (in)efficiency is reflected in the different number of initially tried events for the first and second process, leading to the same number of selected events. While acceptable on their own, the combination of the two processes may be unacceptable, however. It may be that the two processes added together use more energy-momentum than kinematically allowed, or, even if not, are disfavoured when the PYTHIA approach to provide correlated parton densities is applied. Alternatively, referring to case (3) above, it may be because half of the events should be thrown for identical processes. Taken together, it is these effects that reduced the event number from "selected" to "accepted". (A further reduction may occur if a user hook rejects some events.)

It is allowed to use external Les Houches Accord input for the hardest process, and then pick an internal one for the second hardest. In this case PYTHIA does not have access to your thinking concerning the external process, and cannot know whether it overlaps with the internal or not. (External events q qbar' -> e+ nu_e could agree with the internal W ones, or be a W' resonance in a BSM scenario, to give one example.) Therefore the combined cross section is always based on the scenario (1) above. Corrections for correlated parton densities are included also in this case, however. That is, an external event that takes a large fraction of the incoming beam momenta stands a fair chance of being rejected when it has to be combined with another hard process. For this reason the "selected" and "accepted" event numbers are likely to disagree.

In the cross section calculation above, the sigma'_1 cross sections are based on the number of accepted events, while the f_1norm factor is evaluated based on the cross sections for selected events. That way the suppression by correlations between the two processes does not get to be double-counted.

The pythia.statistics() listing contains two final lines, indicating the summed cross sections sigma_1sum and sigma_2sum for the first and second set of processes, at the "selected" stage above, plus information on the sigma_ND and <f_impact> used. The total cross section generated is related to this by
<f_impact> * (sigma_1sum * sigma_2sum / sigma_ND) * (n_accepted / n_selected)
with an additional factor of 1/2 for case 2 above.

The error quoted for the cross section of a process is a combination in quadrature of the error on this process alone with the error on the normalization factor, including the error on <f_impact>. As always it is a purely statistical one and of course hides considerably bigger systematic uncertainties.

Event information

Normally the process event record only contains the hardest interaction, but in this case also the second hardest is stored there. If both of them are 2 -> 2 ones, the first would be stored in lines 3 - 6 and the second in 7 - 10. For both, status codes 21 - 29 would be used, as for a hardest process. Any resonance decay chains would occur after the two main processes, to allow normal parsing. The beams in 1 and 2 only appear in one copy. This structure is echoed in the full event event record.

Most of the properties accessible by the pythia.info methods refer to the first process, whether that happens to be the hardest or not. The code and pT scale of the second process are accessible by the info.codeMPI(1) and info.pTMPI(1), however.

The sigmaGen() and sigmaErr() methods provide the cross section and its error for the event sample as a whole, combining the information from the two hard processes as described above. In particular, the former should be used to give the weight of the generated event sample. The statistical error estimate is somewhat cruder and gives a larger value than the subprocess-by-subprocess one employed in pythia.statistics(), but this number is anyway less relevant, since systematical errors are likely to dominate. pythia8-8.1.80.orig/htmldoc/MainProgramSettings.html0000644000175000017500000003722012217615311020611 0ustar sunsun Main-Program and Related Settings

Main-Program and Related Settings

Introduction

The main program is up to the user to write. However, sample main programs are provided. In one such class of programs, key settings of the run are read in from a "cards file". For experimental collaborations this is actually the most common way to run a program like PYTHIA. The commands in such a file may be of two types
(a) instructions directly to Pythia, like which processes to generate, and
(b) instructions to the main program for what it should do, like how many events to generate, and how many events should be listed.
In principle these two kinds could be kept completely separate. However, to make life simpler, a number of useful main-program settings are defined on this page, so that they are recognized by the Settings machinery. They can thus be put among the other cards without distinction. It is up to you to decide which ones, if any, you actually want to use when you write your main program.

To further reduce the necessary amount of main-program code, some of the tasks that you can steer from your main program can also be done internally. This in particular relates to some information printing. To give an example, the Main:numberToList mode can be used by you in your main program to decide to list a few of the generated events, whereas Next:numberListEvent is used internally in a pythia.next() call to do such a listing automatically. Ultimately, in both cases, a pythia.event.list() call is the one that generates the listing, explicitly in the main program in the former case, implicitly called from pythia.next() in the latter.

The settings names on this page thus fall into four main groups

  • Init:... denote actions that automatically may be taken during the pythia.init() call.
  • Next:... denote actions that automatically may be taken during the pythia.next() call.
  • Stat:... denote actions that automatically may be taken during the pythia.stat() call.
  • Main:... denote actions that you yourself have the freedom to make use of in your main program.
The use of several of the Main:... options is deprecated in favour of the other possibilities.

The Main:... options works like this. Once you have used the pythia.readFile(fileName) method to read in the cards file, where the values have been set, you can interrogate the Settings database to make the values available in your main program. A slight complication is that you need to use a different Settings method for each of the four possible return types that you want to extract. To save some typing the same method names are found directly in the Pythia class, and just send on to the Settings ones to do the job, e.g.

  bool   showCS = pythia.flag("Main:showChangedSettings");
  int    nEvent = pythia.mode("Main:numberOfEvents");
  double spare1 = pythia.parm("Main:spareParm1");
  string file   = pythia.word("Main:allSettingsFile"); 

Main-program settings

The settings in this section must be under the control of the user, i.e. there are no internal equivalents.

mode  Main:numberOfEvents   (default = 1000; minimum = 0)
The number of events to be generated.

mode  Main:timesAllowErrors   (default = 10)
Allow this many times that pythia.next() returns false, i.e. that an event is flawed, before aborting the run.

Initialization settings

flag  Init:showProcesses   (default = on)
Print a list of all processes that will be simulated, with their estimated cross section maxima, as used for the subsequent Monte Carlo selection. Also print corresponding Les Houches initialization data, where relevant.

flag  Init:showMultipartonInteractions   (default = on)
Print initialization information for the multiparton interactions machinery.

flag  Init:showChangedSettings   (default = on)
Print a list of the changed flag/mode/parameter/word settings.

flag  Init:showAllSettings   (default = off)
Print a list of all flag/mode/parameter/word settings. Warning: this will be a long list.

flag  Init:showChangedParticleData   (default = on)
Print a list of particle and decay data for those particles that were changed (one way or another).

flag  Init:showChangedResonanceData   (default = off)
In the previous listing also include the resonances that are initialized at the beginning of a run and thus get new particle data, even if these may well agree with the default ones. Warning: this will be a rather long list.

flag  Init:showAllParticleData   (default = off)
Print a list of all particle and decay data. Warning: this will be a long list.

mode  Init:showOneParticleData   (default = 0; minimum = 0)
Print particle and decay data for the particle with this particular identity code. Default means that no particle is printed.

flag  Main:showChangedSettings   (default = on)
Deprecated. Print a list of the changed flag/mode/parameter/word settings.

flag  Main:showAllSettings   (default = off)
Deprecated. Print a list of all flag/mode/parameter/word settings. Warning: this will be a long list.

flag  Main:showChangedParticleData   (default = off)
Deprecated. Print a list of particle and decay data for those particles that were changed (one way or another).

flag  Main:showChangedResonanceData   (default = off)
Deprecated. In the previous listing also include the resonances that are initialized at the beginning of a run and thus get new particle data, even if these may well agree with the default ones. Warning: this will be a rather long list.

flag  Main:showAllParticleData   (default = off)
Deprecated. Print a list of all particle and decay data. Warning: this will be a long list.

mode  Main:showOneParticleData   (default = 0; minimum = 0)
Deprecated. Print particle and decay data for the particle with this particular identity code. Default means that no particle is printed.

flag  Main:writeChangedSettings   (default = off)
Write a file with the changed flag/mode/parameter/word settings, in a format appropriate to be read in at the beginning of a new run, using the pythia.readFile(fileName) method.

word  Main:changedSettingsFile   (default = currentSettings.cmnd)
The name of the file to which the changed flag/mode/parameter/word settings are written if Main:writeChangedSettings is on.

flag  Main:writeAllSettings   (default = off)
Write a file with all flag/mode/parameter/word settings, in a format appropriate to be read in at the beginning of a new run, using the pythia.readFile(fileName) method.

word  Main:allSettingsFile   (default = allSettings.cmnd)
The name of the file to which a flag/mode/parameter/word settings are written if Main:writeAllSettings is on.

Event-generation settings

mode  Next:numberCount   (default = 1000; minimum = 0)
Print a line telling how many events have been generated so far, once every numberCount events. If set zero then no lines are ever printed.

mode  Next:numberShowLHA   (default = 1; minimum = 0)
The number of events to list the Les Houches input information for, where relevant.

mode  Next:numberShowInfo   (default = 1; minimum = 0)
The number of events to list the Info information for, where relevant.

mode  Next:numberShowProcess   (default = 1; minimum = 0)
The number of events to list the process record for, where relevant.

mode  Next:numberShowEvent   (default = 1; minimum = 0)
The number of events to list the event record for, where relevant.

flag  Next:showScaleAndVertex   (default = off)
In addition to the normal information in the listing of the process and event records, a second line per particle provides information on the production scale, particle polarization and production vertex.

flag  Next:showMothersAndDaughters   (default = off)
In addition to the normal information in the listing of the process and event records, further lines list all the mothers and daughters of each particle.

mode  Main:numberToList   (default = 2; minimum = 0)
Deprecated. The number of events to list.

mode  Main:timesToShow   (default = 50; minimum = 0)
Deprecated. Print the number of events generated so far, this many times, i.e. once every numberOfEvents/numberToShow events.

Statistics

flag  Stat:showProcessLevel   (default = on)
Print the available statistics on number of generated events and cross sections, where relevant.

flag  Stat:showPartonLevel   (default = off)
Print the available statistics on number and types of multiparton interactions, where relevant.

flag  Stat:showErrors   (default = on)
Print the available statistics on number and types of aborts, errors and warnings.

flag  Stat:reset   (default = off)
Reset the statistics of the above three kinds. The default is that all stored statistics information is unaffected by the pythia.stat() call. Counters are automatically reset in each new pythia.init() call, however, so the only time the reset option makes a difference is if stat() is called several times in a (sub)run.

flag  Main:showAllStatistics   (default = off)
Print all available statistics or only the minimal set at the end of the run.

Subruns

You can use subruns to carry out several tasks in the same run. In that case you will need repeated instances of the first setting below in your command file, and could additionally use the second and third as well.

mode  Main:subrun   (default = -999; minimum = 0)
The number of the current subrun, a non-negative integer, put as first line in a section of lines to be read for this particular subrun.

flag  Main:LHEFskipInit   (default = off)
If you read several Les Houches Event Files that you want to see considered as one single combined event sample you can set this flag on after the first subrun to skip (most of) the (re-)initialization step.

mode  Main:numberOfSubruns   (default = 0)
The number of subruns you intend to use in your current run. Unlike the two settings above, Pythia itself will not interpret this number, but you could e.g. have a loop in your main program to loop over subruns from 0 through numberOfSubruns - 1.

Spares

For currently unforeseen purposes, a few dummy settings are made available here. The user can set the desired value in a "cards file" and then use that value in the main program as desired.

flag  Main:spareFlag1   (default = off)

flag  Main:spareFlag2   (default = off)

flag  Main:spareFlag3   (default = off)

mode  Main:spareMode1   (default = 0)

mode  Main:spareMode2   (default = 0)

mode  Main:spareMode3   (default = 0)

parm  Main:spareParm1   (default = 0.)

parm  Main:spareParm2   (default = 0.)

parm  Main:spareParm3   (default = 0.)

word  Main:spareWord1   (default = void)

word  Main:spareWord2   (default = void)

word  Main:spareWord3   (default = void)
pythia8-8.1.80.orig/htmldoc/HadronScattering.html0000644000175000017500000001125412217615311020112 0ustar sunsun Hadron Scattering

Hadron Scattering

A simple hadron scattering model. It is intended to take into account that the overlap of multiple strings at low transverse dimensions is likely to lead to some collective effects, not unlike those observed in heavy-ion collisions, even if not quite as pronounced. Specifically, it is assumed that the hadrons produced can scatter against each other on the way out, before the fragmenting system has had time to expand enough that the hadrons get free. Thereby heavier particles are shifted to higher transverse momenta, at the expense of the lighter ones.
Warning: This is still at an experimental level, and should not be used unless you know what you are doing.

flag  HadronScatter:scatter   (default = off)
Master flag for hadron scattering.

flag  HadronScatter:afterDecay   (default = off)
Perform hadron scattering before or after first round of decays, involving very short-lived particles like the rho. The default is to perform scattering directly after the string fragmentation, before any decays.

flag  HadronScatter:allowDecayProd   (default = off)
Allow two hadrons with same parent hadron to scatter.

flag  HadronScatter:scatterRepeat   (default = off)
Allow hadrons which have already scattered to scatter again. Even if switched on, the same pair can not scatter off each other twice.

Hadron selection

mode  HadronScatter:hadronSelect   (default = 0; minimum = 0; maximum = 0)
Probability that a hadron is soft enough to scatter. (A high-pT hadron presumably being part of a jet, and thus produced away from the high-particle-density region at small transverse dimensions.)
option 0 : P = N exp(-pT^2 / 2 / sigma^2) / ( (1 - k) exp(-pT^2 / 2 / sigma^2) + k pT0^p / (pT0^2 + pT^2)^(p/2), with sigma = 2 StringPT:sigma and pT0 the same as that used in MultipartonInteractions.

parm  HadronScatter:N   (default = 1.0; minimum = 0.01; maximum = 1.0)
N parameter as above.

parm  HadronScatter:k   (default = 1.0; minimum = 0.01; maximum = 1.0)
k parameter as above.

parm  HadronScatter:p   (default = 6; minimum = 2; maximum = 30)
p parameter as above.

Scattering probability

mode  HadronScatter:scatterProb   (default = 0; minimum = 0; maximum = 2)
Probability for a pair of hadrons to scatter.
option 0 : All hadrons scatter with probability j max(0, 1 - dR^2 / rMax^2). Angular distribution is picked flat in cos(theta).
option 1 : As option 0, above, but only pi-pi, pi-K and pi-p scatterings are considered.
option 2 : Only pi-pi, pi-K and pi-p scatterings are considered, with probability given by (1 - exp(-j sigEl)) max(0, 1 - dR^2 / rMax^2). The elastic cross sections and angular distributions are taken from the partial-wave distributions.

parm  HadronScatter:j   (default = 0.5; minimum = 0.0; maximum = 10.0)
j parameter as above.

parm  HadronScatter:rMax   (default = 0.5; minimum = 0.1; maximum = 2.0)
rMax parameter as above.

flag  HadronScatter:tile   (default = off)
Use tiling in (eta, phi) to reduce number of pairwise tests. pythia8-8.1.80.orig/htmldoc/CouplingsAndScales.html0000644000175000017500000003520312217615311020374 0ustar sunsun Couplings and Scales

Couplings and Scales

Here is collected some possibilities to modify the scale choices of couplings and parton densities for all internally implemented hard processes. This is based on them all being derived from the SigmaProcess base class. The matrix-element coding is also used by the multiparton-interactions machinery, but there with a separate choice of alpha_strong(M_Z^2) value and running, and separate PDF scale choices. Also, in 2 -> 2 and 2 -> 3 processes where resonances are produced, their couplings and thereby their Breit-Wigner shapes are always evaluated with the resonance mass as scale, irrespective of the choices below.

Couplings and K factor

The size of QCD cross sections is mainly determined by

parm  SigmaProcess:alphaSvalue   (default = 0.1265; minimum = 0.06; maximum = 0.25)
The alpha_strong value at scale M_Z^2.

The actual value is then regulated by the running to the Q^2 renormalization scale, at which alpha_strong is evaluated

mode  SigmaProcess:alphaSorder   (default = 1; minimum = 0; maximum = 2)
Order at which alpha_strong runs,
option 0 : zeroth order, i.e. alpha_strong is kept fixed.
option 1 : first order, which is the normal value.
option 2 : second order. Since other parts of the code do not go to second order there is no strong reason to use this option, but there is also nothing wrong with it.

QED interactions are regulated by the alpha_electromagnetic value at the Q^2 renormalization scale of an interaction.

mode  SigmaProcess:alphaEMorder   (default = 1; minimum = -1; maximum = 1)
The running of alpha_em used in hard processes.
option 1 : first-order running, constrained to agree with StandardModel:alphaEMmZ at the Z^0 mass.
option 0 : zeroth order, i.e. alpha_em is kept fixed at its value at vanishing momentum transfer.
option -1 : zeroth order, i.e. alpha_em is kept fixed, but at StandardModel:alphaEMmZ, i.e. its value at the Z^0 mass.

In addition there is the possibility of a global rescaling of cross sections (which could not easily be accommodated by a changed alpha_strong, since alpha_strong runs)

parm  SigmaProcess:Kfactor   (default = 1.0; minimum = 0.5; maximum = 4.0)
Multiply almost all cross sections by this common fix factor. Excluded are only unresolved processes, where cross sections are better set directly, and multiparton interactions, which have a separate K factor of their own. This degree of freedom is primarily intended for hadron colliders, and should not normally be used for e^+e^- annihilation processes.

Renormalization scales

The Q^2 renormalization scale can be chosen among a few different alternatives, separately for 2 -> 1, 2 -> 2 and two different kinds of 2 -> 3 processes. In addition a common multiplicative factor may be imposed.

mode  SigmaProcess:renormScale1   (default = 1; minimum = 1; maximum = 2)
The Q^2 renormalization scale for 2 -> 1 processes. The same options also apply for those 2 -> 2 and 2 -> 3 processes that have been specially marked as proceeding only through an s-channel resonance, by the isSChannel() virtual method of SigmaProcess.
option 1 : the squared invariant mass, i.e. sHat.
option 2 : fix scale set in SigmaProcess:renormFixScale below.

mode  SigmaProcess:renormScale2   (default = 2; minimum = 1; maximum = 5)
The Q^2 renormalization scale for 2 -> 2 processes.
option 1 : the smaller of the squared transverse masses of the two outgoing particles, i.e. min(mT_3^2, mT_4^2) = pT^2 + min(m_3^2, m_4^2).
option 2 : the geometric mean of the squared transverse masses of the two outgoing particles, i.e. mT_3 * mT_4 = sqrt((pT^2 + m_3^2) * (pT^2 + m_4^2)).
option 3 : the arithmetic mean of the squared transverse masses of the two outgoing particles, i.e. (mT_3^2 + mT_4^2) / 2 = pT^2 + 0.5 * (m_3^2 + m_4^2). Useful for comparisons with PYTHIA 6, where this is the default.
option 4 : squared invariant mass of the system, i.e. sHat. Useful for processes dominated by s-channel exchange.
option 5 : fix scale set in SigmaProcess:renormFixScale below.

mode  SigmaProcess:renormScale3   (default = 3; minimum = 1; maximum = 6)
The Q^2 renormalization scale for "normal" 2 -> 3 processes, i.e excepting the vector-boson-fusion processes below. Here it is assumed that particle masses in the final state either match or are heavier than that of any t-channel propagator particle. (Currently only g g / q qbar -> H^0 Q Qbar processes are implemented, where the "match" criterion holds.)
option 1 : the smaller of the squared transverse masses of the three outgoing particles, i.e. min(mT_3^2, mT_4^2, mT_5^2).
option 2 : the geometric mean of the two smallest squared transverse masses of the three outgoing particles, i.e. sqrt( mT_3^2 * mT_4^2 * mT_5^2 / max(mT_3^2, mT_4^2, mT_5^2) ).
option 3 : the geometric mean of the squared transverse masses of the three outgoing particles, i.e. (mT_3^2 * mT_4^2 * mT_5^2)^(1/3).
option 4 : the arithmetic mean of the squared transverse masses of the three outgoing particles, i.e. (mT_3^2 + mT_4^2 + mT_5^2)/3.
option 5 : squared invariant mass of the system, i.e. sHat.
option 6 : fix scale set in SigmaProcess:renormFixScale below.

mode  SigmaProcess:renormScale3VV   (default = 3; minimum = 1; maximum = 6)
The Q^2 renormalization scale for 2 -> 3 vector-boson-fusion processes, i.e. f_1 f_2 -> H^0 f_3 f_4 with Z^0 or W^+- t-channel propagators. Here the transverse masses of the outgoing fermions do not reflect the virtualities of the exchanged bosons. A better estimate is obtained by replacing the final-state fermion masses by the vector-boson ones in the definition of transverse masses. We denote these combinations mT_Vi^2 = m_V^2 + pT_i^2.
option 1 : the squared mass m_V^2 of the exchanged vector boson.
option 2 : the geometric mean of the two propagator virtuality estimates, i.e. sqrt(mT_V3^2 * mT_V4^2).
option 3 : the geometric mean of the three relevant squared transverse masses, i.e. (mT_V3^2 * mT_V4^2 * mT_H^2)^(1/3).
option 4 : the arithmetic mean of the three relevant squared transverse masses, i.e. (mT_V3^2 + mT_V4^2 + mT_H^2)/3.
option 5 : squared invariant mass of the system, i.e. sHat.
option 6 : fix scale set in SigmaProcess:renormFixScale below.

parm  SigmaProcess:renormMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
The Q^2 renormalization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes is multiplied by this factor relative to the scale described above (except for the options with a fix scale). Should be use sparingly for 2 -> 1 processes.

parm  SigmaProcess:renormFixScale   (default = 10000.; minimum = 1.)
A fix Q^2 value used as renormalization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes in some of the options above.

Factorization scales

Corresponding options exist for the Q^2 factorization scale used as argument in PDF's. Again there is a choice of form for 2 -> 1, 2 -> 2 and 2 -> 3 processes separately. For simplicity we have let the numbering of options agree, for each event class separately, between normalization and factorization scales, and the description has therefore been slightly shortened. The default values are not necessarily the same, however.

mode  SigmaProcess:factorScale1   (default = 1; minimum = 1; maximum = 2)
The Q^2 factorization scale for 2 -> 1 processes. The same options also apply for those 2 -> 2 and 2 -> 3 processes that have been specially marked as proceeding only through an s-channel resonance.
option 1 : the squared invariant mass, i.e. sHat.
option 2 : fix scale set in SigmaProcess:factorFixScale below.

mode  SigmaProcess:factorScale2   (default = 1; minimum = 1; maximum = 5)
The Q^2 factorization scale for 2 -> 2 processes.
option 1 : the smaller of the squared transverse masses of the two outgoing particles.
option 2 : the geometric mean of the squared transverse masses of the two outgoing particles.
option 3 : the arithmetic mean of the squared transverse masses of the two outgoing particles. Useful for comparisons with PYTHIA 6, where this is the default.
option 4 : squared invariant mass of the system, i.e. sHat. Useful for processes dominated by s-channel exchange.
option 5 : fix scale set in SigmaProcess:factorFixScale below.

mode  SigmaProcess:factorScale3   (default = 2; minimum = 1; maximum = 6)
The Q^2 factorization scale for "normal" 2 -> 3 processes, i.e excepting the vector-boson-fusion processes below.
option 1 : the smaller of the squared transverse masses of the three outgoing particles.
option 2 : the geometric mean of the two smallest squared transverse masses of the three outgoing particles.
option 3 : the geometric mean of the squared transverse masses of the three outgoing particles.
option 4 : the arithmetic mean of the squared transverse masses of the three outgoing particles.
option 5 : squared invariant mass of the system, i.e. sHat.
option 6 : fix scale set in SigmaProcess:factorFixScale below.

mode  SigmaProcess:factorScale3VV   (default = 2; minimum = 1; maximum = 6)
The Q^2 factorization scale for 2 -> 3 vector-boson-fusion processes, i.e. f_1 f_2 -> H^0 f_3 f_4 with Z^0 or W^+- t-channel propagators. Here we again introduce the combinations mT_Vi^2 = m_V^2 + pT_i^2 as replacements for the normal squared transverse masses of the two outgoing quarks.
option 1 : the squared mass m_V^2 of the exchanged vector boson.
option 2 : the geometric mean of the two propagator virtuality estimates.
option 3 : the geometric mean of the three relevant squared transverse masses.
option 4 : the arithmetic mean of the three relevant squared transverse masses.
option 5 : squared invariant mass of the system, i.e. sHat.
option 6 : fix scale set in SigmaProcess:factorFixScale below.

parm  SigmaProcess:factorMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
The Q^2 factorization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes is multiplied by this factor relative to the scale described above (except for the options with a fix scale). Should be use sparingly for 2 -> 1 processes.

parm  SigmaProcess:factorFixScale   (default = 10000.; minimum = 1.)
A fix Q^2 value used as factorization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes in some of the options above. pythia8-8.1.80.orig/htmldoc/UserHooks.html0000644000175000017500000013540412217615312016602 0ustar sunsun User Hooks

User Hooks

Sometimes it may be convenient to step in during the generation process: to modify the built-in cross sections, to veto undesirable events or simply to collect statistics at various stages of the evolution. There is a base class UserHooks that gives you this access at a few selected places. This class in itself does nothing; the idea is that you should write your own derived class for your task. One simple derived class (SuppressSmallPT) comes with the program, mainly as illustration, and the main10.cc program provides a complete (toy) example how a derived class could be set up and used.

There are six sets of routines, that give you different kinds of freedom. They are, in no particular order:
(i) Ones that give you access to the event record in between the process-level and parton-level steps, or in between the parton-level and hadron-level ones. You can study the event record and decide whether to veto this event.
(ii) Ones that allow you to set a scale at which the combined parton-level MPI+ISR+FSR downwards evolution in pT is temporarily interrupted, so the event can be studied and either vetoed or allowed to continue the evolution.
(iii) Ones that allow you to to study the event after the first few ISR/FSR emissions, or first few MPI, so the event can be vetoed or allowed to continue the evolution.
(iv) Ones that allow you to study the latest initial- or final-state emission and veto that emission, without vetoing the event as a whole.
(v) Ones that give you access to the properties of the trial hard process, so that you can modify the internal Pythia cross section, alternatively the phase space sampling, by your own correction factors.
(vi) Ones that allow you to reject the decay sequence of resonances at the process level.
(vii) Ones that let you set the scale of shower evolution, specifically for matching in resonance decays.
They are described further in the following numbered subsections.

All the possibilities above can be combined freely and also be combined with the standard flags. An event would then survive only if it survived each of the possible veto methods. There are no hidden interdependencies in this game, but of course some combinations may not be particularly meaningful. For instance, if you set PartonLevel:all = off then the doVetoPT(...) and doVetoPartonLevel(...) locations in the code are not even reached, so they would never be called.

The effect of the vetoes of types (i), (ii) and (iii) can be studied in the output of the Pythia::statistics() method. The "Selected" column represents the number of events that were found acceptable by the internal Pythia machinery, whereas the "Accepted" one are the events that also survived the user cuts. The cross section is based on the latter number, and so is reduced by the amount associated by the vetoed events. Also type (v) modifies the cross section, while types (iv), (vi) and (vii) do not.

A warning. When you program your own derived class, do remember that you must exactly match the arguments of the base-class methods you overload. If not, your methods will be considered as completely new ones, and compile without any warnings, but not be used inside Pythia. So, at the debug stage, do insert some suitable print statements to check that the new methods are called (and do what they should).

The basic components

For a derived UserHooks class to be called during the execution, a pointer to an object of this class should be handed in with the
Pythia::setUserHooksPtr( UserHooks*)
method. The first step therefore is to construct your own derived class, of course. This must contain a constructor and a destructor. The initPtr method comes "for free", and is set up without any intervention from you.

UserHooks::UserHooks()  
virtual UserHooks::~UserHooks()  
The constructor and destructor do not need to do anything.

void UserHooks::initPtr( Info* infoPtr, Settings* settingsPtr, ParticleData* particleDataPtr, Rndm* rndmPtr, BeamParticle* beamAPtr, BeamParticle* beamBPtr, BeamParticle* beamPomAPtr, BeamParticle* beamPomBPtr, CoupSM* coupSMPtr, PartonSystems* partonSystemsPtr, SigmaTotal* sigmaTotPtr)  
this (non-virtual) method is automatically called during the initialization stage to set several useful pointers, and to set up the workEvent below. The corresponding objects can later be used to extract some useful information.
Info: general event and run information, including some loop counters.
Settings: the settings used to determine the character of the run.
ParticleData: the particle data used in the event record (including workEvent below).
Rndm: the random number generator, that you could also use in your code.
BeamParticle: the beamAPtr and beamBPtr beam particles contain info on partons extracted from the two incoming beams, on the PDFs used, and more. In cases when diffraction is simulated, also special Pomeron beams beamPomAPtr and beamPomBPtr are introduced, for the Pomerons residing inside the respective proton.
CoupSM: Standard Model couplings.
PartonSystems: the list of partons that belong to each individual subcollision system.
SigmaTotal: total/elastic/diffractive cross section parametrizations.

Next you overload the desired methods listed in the sections below. These often come in pairs or triplets, where the first must return true for the last method to be called. This latter method typically hands you a reference to the event record, which you then can use to decide whether or not to veto. Often the event record can be quite lengthy and difficult to overview. The following methods and data member can then come in handy.

void UserHooks::omitResonanceDecays(const Event& process, bool finalOnly = false)  
is a protected method that you can make use of in your own methods to extract a simplified list of the hard process, where all resonance decay chains are omitted. Intended for the can/doVetoProcessLevel routines. Note that the normal process-level generation does include resonance decays. That is, if a top quark is produced in the hard process, then also decays such as t -> b W+, W+ -> u dbar will be generated and stored in process. The omitResonanceDecays routine will take the input process and copy it to workEvent (see below), minus the resonance decay chains. All particles produced in the hard process, such as the top, will be considered final-state ones, with positive status and no daughters, just as it is before resonances are allowed to decay.
(In the PartonLevel routines, these decay chains will initially not be copied from process to event. Instead the combined MPI, ISR and FSR evolution is done with the top above as final particle. Only afterwards will the resonance decay chains be copied over, with kinematics changes reflecting those of the top, and showers in the decays carried out.)
For the default finalOnly = false the beam particles and incoming partons are retained, so the event looks like a normal event record up to the point of resonance decays, with a normal history setup.
With finalOnly = true only the final-state partons are retained in the list. It therefore becomes similar in functionality to the subEvent method below, with the difference that subEvent counts the decay products of the resonances as the final state, whereas here the resonances themselves are the final state. Since the history has been removed in this option, mother1() and mother2() return 0, while daughter1() and daughter2() both return the index of the same parton in the original event record.

void UserHooks::subEvent(const Event& event, bool isHardest = true)  
is a protected method that you can make use of in your own methods to extract a brief list of the current partons of interest, with all irrelevant ones omitted. It is primarily intended to track the evolution at the parton level, notably the shower evolution of the hardest (i.e. first) interaction.
For the default isHardest = true only the outgoing partons from the hardest interaction (including the partons added to it by ISR and FSR) are extracted, as relevant e.g. for doVetoPT( iPos, event) with iPos = 0 - 4. With isHardest = false instead the outgoing partons of the latest "subprocess" are extracted, as relevant when iPos = 5, where it corresponds to the outgoing partons in the currently considered decay.
The method also works at the process level, but there simply extracts all final-state partons in the event, and thus offers no extra functionality.
The result is stored in workEvent below. Since the history has been removed, mother1() and mother2() return 0, while daughter1() and daughter2() both return the index of the same parton in the original event record (event; possibly process), so that you can trace the full history, if of interest.

Event UserHooks::workEvent  
This protected class member contains the outcome of the above omitResonanceDecays(...) and subEvent(...) methods. Alternatively you can use it for whatever temporary purposes you wish. You are free to use standard operations, e.g. to boost the event to its rest frame before analysis, or remove particles that should not be analyzed. The workEvent can also be sent on to a jet clustering algorithm.

(i) Interrupt between the main generation levels

virtual bool UserHooks::initAfterBeams()  
This routine is called by Pythia::init(), after the beams have been set up, but before any other initialisation. Therefore, at this stage, it is still possible to modify settings (apart from Beams:*) and particle data. This is mainly intended to be used in conjunction with Les Houches Event files, where headers are read in during beam initialisation, see the header functions in the Info class. In the base class this method returns true. By returning false, PYTHIA initialisation will be aborted.

virtual bool UserHooks::canVetoProcessLevel()  
In the base class this method returns false. If you redefine it to return true then the method doVetoProcessLevel(...) will be called immediately after a hard process (and associated resonance decays) has been selected and stored in the process event record.
At this stage, the process record typically contains the two beams in slots 1 and 2, the two incoming partons to the hard process in slots 3 and 4, the N (usually 1, 2 or 3) primary produced particles in slots 5 through 4 + N, and thereafter recursively the resonance decay chains, if any. Use the method omitResonanceDecays(...) if you want to skip these decay chains. There are exceptions to this structure, for soft QCD processes (where the partonic process may not yet have been selected at this stage), and when a second hard process has been requested (where two hard processes are bookkept). In general it is useful to begin the development work by listing a few process records, to clarify what the structure is for the cases of interest.

virtual bool UserHooks::doVetoProcessLevel(Event& process)  
can optionally be called, as described above. You can study the process event record of the hard process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next().
Warning: Normally you should not modify the process event record. However, for some matrix-element-matching procedures it may become unavoidable. If so, be very careful, since there are many pitfalls. Only to give one example: if you modify the incoming partons then also the information stored in the beam particles may need to be modified.
Note: the above veto is different from setting the flag PartonLevel:all = off. Also in the latter case the event generation will stop after the process level, but an event generated up to this point is considered perfectly acceptable. It can be studied and it contributes to the cross section. That is, PartonLevel:all = off is intended for simple studies of hard processes, where one can save a lot of time by not generating the rest of the story. By contrast, the doVetoProcessLevel() method allows you to throw away uninteresting events at an early stage to save time, but those events that do survive the veto are allowed to develop into complete final states (unless flags have been set otherwise).

virtual bool UserHooks::canVetoPartonLevel()  
In the base class this method returns false. If you redefine it to return true then the method doVetoPartonLevel(...) will be called immediately after the parton level has been generated and stored in the event event record. Thus showers, multiparton interactions and beam remnants have been set up, but hadronization and decays have not yet been performed. This is already a fairly complete event, possibly with quite a complex parton-level history. Therefore it is usually only meaningful to study the hardest interaction, e.g. using subEvent(...) introduced above, or fairly generic properties, such as the parton-level jet structure.

virtual bool UserHooks::doVetoPartonLevel(const Event& event)  
can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next().
Note: the above veto is different from setting the flag HadronLevel:all = off. Also in the latter case the event generation will stop after the parton level, but an event generated up to this point is considered perfectly acceptable. It can be studied and it contributes to the cross section. That is, HadronLevel:all = off is intended for simple studies of complete partonic states, where one can save time by not generating the complete hadronic final state. By contrast, the doVetoPartonLevel() method allows you to throw away uninteresting events to save time that way, but those events that do survive the veto are allowed to develop into complete final states (unless flags have been set otherwise).

virtual bool UserHooks::canVetoPartonLevelEarly()  
is very similar to canVetoPartonLevel() above, except that the chance to veto appears somewhat earlier in the generation chain, after showers and multiparton interactions, but before the beam remnants and resonance decays have been added. It is therefore somewhat more convenient for many matrix element strategies, where the primordial kT added along with the beam remnants should not be included.

virtual bool UserHooks::doVetoPartonLevelEarly(const Event& event)  
is very similar to doVetoPartonLevel(...) above, but the veto can be done earlier, as described for canVetoPartonLevelEarly().

(ii) Interrupt during the parton-level evolution, at a pT scale

During the parton-level evolution, multiparton interactions (MPI), initial-state radiation (ISR) and final-state radiation (FSR) are normally evolved downwards in one interleaved evolution sequence of decreasing pT values. For some applications, e.g matrix-element-matching approaches, it may be convenient to stop the evolution temporarily when the "hard" emissions have been considered, but before continuing with the more time-consuming soft activity. Based on these hard partons one can make a decision whether the event at all falls in the intended event class, e.g. has the "right" number of parton-level jets. If yes then, as for the methods above, the evolution will continue all the way up to a complete event. Also as above, if no, then the event will not be considered in the final cross section.

Recall that the new or modified partons resulting from a MPI, ISR or FSR step are always appended to the end of the then-current event record. Previously existing partons are not touched, except for the status, mother and daughter values, which are updated to reflect the modified history. It is therefore straightforward to find the partons associated with the most recent occurrence.
An MPI results in four new partons being appended, two incoming and two outgoing ones.
An ISR results in the whole affected system being copied down, with one of the two incoming partons being replaced by a new one, and one more outgoing parton.
An FSR results in three new partons, two that come from the branching and one that takes the recoil.
The story becomes more messy when rescattering is allowed as part of the MPI machinery. Then there will not only be a new system, as outlined above, but additionally some existing systems will undergo cascade effects, and be copied down with changed kinematics.

In this subsection we outline the possibility to interrupt at a given pT scale, in the next to interrupt after a given number of emissions.

virtual bool UserHooks::canVetoPT()  
In the base class this method returns false. If you redefine it to return true then the method doVetoPT(...) will interrupt the downward evolution at scaleVetoPT().

virtual double UserHooks::scaleVetoPT()  
In the base class this method returns 0. You should redefine it to return the pT scale at which you want to study the event.

virtual bool UserHooks::doVetoPT(int iPos, const Event& event)  
can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next().
argument iPos : is the position/status when the routine is called, information that can help you decide your course of action:
argumentoption 0 : when no MPI, ISR or FSR occurred above the veto scale;
argumentoption 1 : when inside the interleaved MPI + ISR + FSR evolution, after an MPI process;
argumentoption 2 : when inside the interleaved MPI + ISR + FSR evolution, after an ISR emission;
argumentoption 3 : when inside the interleaved MPI + ISR + FSR evolution, after an FSR emission;
argumentoption 4 : for the optional case where FSR is deferred from the interleaved evolution and only considered separately afterward (then alternative 3 would never occur);
argumentoption 5 : is for subsequent resonance decays, and is called once for each decaying resonance in a chain such as t -> b W, W -> u dbar.
argument event : the event record contains a list of all partons generated so far, also including intermediate ones not part of the "current final state", and also those from further multiparton interactions. This may not be desirable for comparisons with matrix-element calculations. You may want to make use of the subEvent(...) method below to obtain a simplified event record workEvent.

(iii) Interrupt during the parton-level evolution, after a step

These options are closely related to the ones above in section (ii), so we do not repeat the introduction, nor the possibilities to study the event record, also by using subEvent(...) and workEvent. What is different is that the methods in this section give access to the event as it looks like after each of the first few steps in the downwards evolution, irrespective of the pT scales of these branchings. Furthermore, it is here assumed that the focus normally is on the hardest subprocess, so that ISR/FSR emissions associated with additional MPI's are not considered. For MPI studies, however, a separate simpler alternative is offered to consider the event after a given number of interactions.

virtual bool UserHooks::canVetoStep()  
In the base class this method returns false. If you redefine it to return true then the method doVetoStep(...) will interrupt the downward ISR and FSR evolution the first numberVetoStep() times.

virtual int UserHooks::numberVetoStep()  
Returns the number of steps n each of ISR and FSR, for the hardest interaction, that you want to be able to study. That is, the method will be called after the first n ISR emissions, irrespective of the number of FSR ones at the time, and after the first n FSR emissions, irrespective of the number of ISR ones. The number of steps defaults to the first one only, but you are free to pick another value. Note that double diffraction is handled as two separate Pomeron-proton collisions, and thus has two sequences of emissions.

virtual bool UserHooks::doVetoStep(int iPos, int nISR, int nFSR, const Event& event)  
can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next().
argument iPos : is the position/status when the routine is called, information that can help you decide your course of action. Agrees with options 2 - 5 of the doVetoPT(...) routine above, while options 0 and 1 are not relevant here.
argument nISR : is the number of ISR emissions in the hardest process so far. For resonance decays, iPos = 5, it is 0.
argument nFSR : is the number of FSR emissions in the hardest process so far. For resonance decays, iPos = 5, it is the number of emissions in the currently studied system.
argument event : the event record contains a list of all partons generated so far, also including intermediate ones not part of the "current final state", and also those from further multiparton interactions. This may not be desirable for comparisons with matrix-element calculations. You may want to make use of the subEvent(...) method above to obtain a simplified event record.

virtual bool UserHooks::canVetoMPIStep()  
In the base class this method returns false. If you redefine it to return true then the method doVetoMPIStep(...) will interrupt the downward MPI evolution the first numberVetoMPIStep() times.

virtual int UserHooks::numberVetoMPIStep()  
Returns the number of steps in the MPI evolution that you want to be able to study, right after each new step has been taken and the subcollision has been added to the event record. The number of steps defaults to the first one only, but you are free to pick another value. Note that the hardest interaction of an events counts as the first multiparton interaction. For most hard processes it thus at the first step offers nothing not available with the VetoProcessLevel functionality above. For the minimum-bias and diffractive systems the hardest interaction is not selected at the process level, however, so there a check after the first multiparton interaction offers new functionality. Note that double diffraction is handled as two separate Pomeron-proton collisions, and thus has two sequences of interactions. Also, if you have set up a second hard process then a check is made after these first two, and the first interaction coming from the MPI machinery would have sequence number 3.

virtual bool UserHooks::doVetoMPIStep(int nMPI,const Event& event)  
can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next().
argument nMPI : is the number of MPI subprocesses has occurred so far.
argument event : the event record contains a list of all partons generated so far, also including intermediate ones not part of the "current final state", e.g. leftovers from the ISR and FSR evolution of previously generated systems. The most recently added one has not had time to radiate, of course.

(iv) Veto emissions

The methods in this group are intended to allow the veto of an emission in ISR, FSR or MPI, without affecting the evolution in any other way. If an emission is vetoed, the event record is "rolled back" to the way it was before the emission occurred, and the evolution in pT is continued downwards from the rejected value. The decision can be based on full knowledge of the kinematics of the shower branching or MPI.

To identify where shower emissions originated, the ISR/FSR veto routines are passed the system from which the radiation occurred, according to the Parton Systems class (see Advanced Usage). Note, however, that inside the veto routines only the event record has been updated; all other information, including the Parton Systems, reflects the event before the shower branching or MPI has taken place.

virtual bool UserHooks::canVetoISREmission()  
In the base class this method returns false. If you redefine it to return true then the method doVetoISREmission(...) will interrupt the initial-state shower immediately after each emission and allow that emission to be vetoed.

virtual bool UserHooks::doVetoISREmission( int sizeOld, const Event& event, int iSys)  
can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the emission, true, or not, false. If you veto, then the latest emission is removed from the event record. In either case the evolution of the shower will continue from the point where it was left off.
argument sizeOld : is the size of the event record before the latest emission was added to it. It will also become the new size if the emission is vetoed.
argument event : the event record contains a list of all partons generated so far. Of special interest are the ones associated with the most recent emission, which are stored in entries from sizeOld through event.size() - 1 inclusive. If you veto the emission these entries will be removed, and the history info in the remaining partons will be restored to a state as if the emission had never occurred.
argument iSys : the system where the radiation occurs, according to Parton Systems.

virtual bool UserHooks::canVetoFSREmission()  
In the base class this method returns false. If you redefine it to return true then the method doVetoFSREmission(...) will interrupt the final-state shower immediately after each emission and allow that emission to be vetoed.

virtual bool UserHooks::doVetoFSREmission( int sizeOld, const Event& event, int iSys, bool inResonance = false)  
can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the emission, true, or not, false. If you veto, then the latest emission is removed from the event record. In either case the evolution of the shower will continue from the point where it was left off.
argument sizeOld : is the size of the event record before the latest emission was added to it. It will also become the new size if the emission is vetoed.
argument event : the event record contains a list of all partons generated so far. Of special interest are the ones associated with the most recent emission, which are stored in entries from sizeOld through event.size() - 1 inclusive. If you veto the emission these entries will be removed, and the history info in the remaining partons will be restored to a state as if the emission had never occurred.
argument iSys : the system where the radiation occurs, according to Parton Systems.
argument inResonance : true if the emission takes place in a resonance decay, subsequent to the hard process.

virtual bool UserHooks::canVetoMPIEmission()  
In the base class this method returns false. If you redefine it to return true then the method doVetoMPIEmission(...) will interrupt the MPI machinery immediately after each multiparton interaction and allow it to be vetoed.

virtual bool UserHooks::doVetoMPIEmission( int sizeOld, const Event& event)  
can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the MPI, true, or not, false. If you veto, then the latest MPI is removed from the event record. In either case the interleaved evolution will continue from the point where it was left off.
argument sizeOld : is the size of the event record before the latest MPI was added to it. It will also become the new size if the MPI is vetoed.
argument event : the event record contains a list of all partons generated so far. Of special interest are the ones associated with the most recent MPI, which are stored in entries from sizeOld through event.size() - 1 inclusive. If you veto the MPI these entries will be removed.

(v) Modify cross-sections or phase space sampling

This section addresses two related but different topics. In both cases the sampling of events in phase space is modified, so that some regions are more populated while others are depleted. In the first case, this is assumed to be because the physical cross section should be modified relative to the built-in Pythia form. Therefore not only the relative population of phase space is changed, but also the integrated cross section of the process. In the second case the repopulation is only to be viewed as a technical trick to sample some phase-space regions better, so as to reduce the statistical error. There each event instead obtains a compensating weight, the inverse of the differential cross section reweighting factor, in such a way that the integrated cross section is unchanged. Below these two cases are considered separately, but note that they share many points.

virtual bool UserHooks::canModifySigma()  
In the base class this method returns false. If you redefine it to return true then the method multiplySigmaBy(...) will allow you to modify the cross section weight assigned to the current event.

virtual double UserHooks::multiplySigmaBy(const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool inEvent)  
when called this method should provide the factor by which you want to see the cross section weight of the current event modified. If you return unity then the normal cross section is obtained. Note that, unlike the methods above, these modifications do not lead to a difference between the number of "selected" events and the number of "accepted" ones, since the modifications occur already before the "selected" level. The integrated cross section of a process is modified, of course. Note that the cross section is only modifiable for normal hard processes. It does not affect the cross section in further multiparton interactions, nor in elastic/diffractive/minimum-bias events.
argument sigmaProcessPtr, phaseSpacePtr : : what makes this routine somewhat tricky to write is that the hard-process event has not yet been constructed, so one is restricted to use the information available in the phase-space and cross-section objects currently being accessed. Which of their methods are applicable depends on the process, in particular the number of final-state particles. The multiplySigmaBy code in UserHooks.cc contains explicit instructions about which methods provide meaningful information, and so offers a convenient starting point.
argument inEvent : : this flag is true when the method is called from within the event-generation machinery and false when it is called at the initialization stage of the run, when the cross section is explored to find a maximum for later Monte Carlo usage. Cross-section modifications should be independent of this flag, for consistency, but if multiplySigmaBy(...) is used to collect statistics on the original kinematics distributions before cuts, then it is important to be able to exclude the initialization stage from comparisons.

One derived class is supplied as an example how this facility can be used to reweight cross sections in the same spirit as is done with QCD cross sections for the minimum-bias/underlying-event description:

class  SuppressSmallPT : public UserHooks  
suppress small-pT production for 2 -> 2 processes only, while leaving other processes unaffected. The basic suppression factor is pT^4 / ((k*pT0)^2 + pT^2)^2, where pT refers to the current hard subprocess and pT0 is the same energy-dependent dampening scale as used for multiparton interactions. This class contains canModifySigma() and multiplySigmaBy() methods that overload the base class ones.

SuppressSmallPT::SuppressSmallPT( double pT0timesMPI = 1., int numberAlphaS = 0, bool useSameAlphaSasMPI = true)  
The optional arguments of the constructor provides further variability.
argument pT0timesMPI : corresponds to the additional factor k in the above formula. It is by default equal to 1 but can be used to explore deviations from the expected value.
argument numberAlphaS : if this number n is bigger than the default 0, the corresponding number of alpha_strong factors is also reweighted from the normal renormalization scale to a modified one, i.e. a further suppression factor ( alpha_s((k*pT0)^2 + Q^2_ren) / alpha_s(Q^2_ren) )^n is introduced.
argument useSameAlphaSasMPI : regulates which kind of new alpha_strong value is evaluated for the numerator in the above expression. It is by default the same as set for multiparton interactions (i.e. same starting value at M_Z and same order of running), but if false instead the one for hard subprocesses. The denominator alpha_s(Q^2_ren) is always the value used for the "original", unweighted cross section.

The second main case of the current section involves three methods, as follows.

virtual bool UserHooks::canBiasSelection()  
In the base class this method returns false. If you redefine it to return true then the method biasSelectionBy(...) will allow you to modify the phase space sampling, with a compensating event weight, such that the cross section is unchanged. You cannot combine this kind of reweighting with the selection of a second hard process.

virtual double UserHooks::biasSelectionBy(const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool inEvent)  
when called this method should provide the factor by which you want to see the phase space sampling of the current event modified. Events are assigned a weight being the inverse of this, such that the integrated cross section of a process is unchanged. Note that the selection is only modifiable for normal hard processes. It does not affect the selection in further multiparton interactions, nor in elastic/diffractive/minimum-bias events.
argument sigmaProcessPtr, phaseSpacePtr : : what makes this routine somewhat tricky to write is that the hard-process event has not yet been constructed, so one is restricted to use the information available in the phase-space and cross-section objects currently being accessed. Which of their methods are applicable depends on the process, in particular the number of final-state particles. The biasSelectionBy code in UserHooks.cc contains explicit instructions about which methods provide meaningful information, and so offers a convenient starting point.
argument inEvent : : this flag is true when the method is called from within the event-generation machinery and false when it is called at the initialization stage of the run, when the cross section is explored to find a maximum for later Monte Carlo usage. Cross-section modifications should be independent of this flag, for consistency, but if biasSelectionBy(...) is used to collect statistics on the original kinematics distributions before cuts, then it is important to be able to exclude the initialization stage from comparisons.

virtual double UserHooks::biasedSelectionWeight()  
Returns the weight you should assign to the event, to use e.g. when you histogram results. It is the exact inverse of the weight you used to modify the phase-space sampling, a weight that must be stored in the selBias member variable, such that this routine can return 1/selBias. The weight is also returned by the Info::weight() method, which may be more convenient to use.

(vi) Reject the decay sequence of resonances

Resonance decays are performed already at the process level, as an integrated second step of the hard process itself. One reason is that the matrix element of many processes encode nontrivial decay angular distributions. Another is to have equivalence with Les Houches input, where resonance decays typically are provided from the onset. The methods in this section allow you to veto that decay sequence and try a new one. Unlike the veto of the whole process-level step, in point (i), the first step of the hard process is retained, i.e. where the resonances are produced. For this reason the cross section is not affected here but, depending on context, you may want to introduce your own counters to check how often a new set of decay modes and kinematics is selected, and correct accordingly.

The main method below is applied after all decays. For the production of a t tbar pair this typically means after four decays, namely those of the t, the tbar, the W+ and the W-. If Les Houches events are processed, the rollback is to the level of the originally read events. For top, that might mean either to the tops, or to the W bosons, or no rollback at all, depending on how the process generation was set up.

virtual bool UserHooks::canVetoResonanceDecays()  
In the base class this method returns false. If you redefine it to return true then the method doVetoResonanceDecays(...) will be called immediately after the resonance decays have been selected and stored in the process event record, as described above for canVetoProcessLevel().

virtual bool UserHooks::doVetoResonanceDecays(Event& process)  
can optionally be called, as described above. You can study the process event record of the hard process. Based on that you can decide whether to reject the sequence of resonance decays that was not already fixed by the production step of the hard process (which can vary depending on how a process has been set up, see above). If you veto, then a new resonance decay sequence is selected, but the production step remains unchanged. The cross section remains unaffected by this veto, for better or worse.
Warning: Normally you should not modify the process event record. However, as an extreme measure, parts or the complete decay chain could be overwritten. If so, be very careful.

(vii) Modify scale in shower evolution

The choice of maximum shower scale in resonance decays is normally not a big issue, since the shower here is expected to cover the full phase space. In some special cases a matching scheme is intended, where hard radiation is covered by matrix elements, and only softer by showers. The below two methods support such an approach. Note that the two methods are not used in the TimeShower class itself, but when showers are called from the PartonLevel generation. Thus user calls directly to TimeShower are not affected.

virtual bool UserHooks::canSetResonanceScale()  
In the base class this method returns false. If you redefine it to return true then the method scaleResonance(...) will set the initial scale of downwards shower evolution.

virtual double UserHooks::scaleResonance( int iRes, const Event& event)  
can optionally be called, as described above. You should return the maximum scale, in GeV, from which the shower evolution will begin. The base class method returns 0, i.e. gives no shower evolution at all. You can study, but not modify, the event event record of the partonic process to check which resonance is decaying, and into what.
argument iRes : is the location in the event record of the resonance that decayed to the particles that now will shower.
argument event : the event record contains a list of all partons generated so far, specifically the decaying resonance and its immediate decay products. pythia8-8.1.80.orig/htmldoc/EventAnalysis.html0000644000175000017500000012661712217615312017453 0ustar sunsun Event Analysis

Event Analysis

Introduction

The routines in this section are intended to be used to analyze event properties. As such they are not part of the main event generation chain, but can be used in comparisons between Monte Carlo events and real data. They are rather free-standing, but assume that input is provided in the PYTHIA 8 Event format, and use a few basic facilities such as four-vectors. Their ordering is mainly by history; for current LHC applications the final one, SlowJet, is of special interest.

In addition to the methods presented here, there is also the possibility to make use of external jet finders .

Sphericity

The standard sphericity tensor is
S^{ab} = (sum_i p_i^a p_i^b) / (sum_i p_i^2)
where the sum i runs over the particles in the event, a, b = x, y, z, and p without such an index is the absolute size of the three-momentum . This tensor can be diagonalized to find eigenvalues and eigenvectors.

The above tensor can be generalized by introducing a power r, such that
S^{ab} = (sum_i p_i^a p_i^b p_i^{r-2}) / (sum_i p_i^r)
In particular, r = 1 gives a linear dependence on momenta and thus a collinear safe definition, unlike sphericity.

To do sphericity analyses you have to set up a Sphericity instance, and then feed in events to it, one at a time. The results for the latest event are available as output from a few methods.

Sphericity::Sphericity(double power = 2., int select = 2)  
create a sphericity analysis object, where
argument power (default = 2.) : is the power r defined above, i.e.
argumentoption 2. : gives Sphericity, and
argumentoption 1. : gives the linear form.
argument select (default = 2) : tells which particles are analyzed,
argumentoption 1 : all final-state particles,
argumentoption 2 : all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and
argumentoption 3 : only charged final-state particles.

bool Sphericity::analyze( const Event& event, ostream& os = cout)  
perform a sphericity analysis, where
argument event : is an object of the Event class, most likely the pythia.event one.
argument os (default = cout) : is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
If the routine returns false the analysis failed, e.g. if too few particles are present to analyze.

After the analysis has been performed, a few methods are available to return the result of the analysis of the latest event:

double Sphericity::sphericity()  
gives the sphericity (or equivalent if r is not 2),

double Sphericity::aplanarity()  
gives the aplanarity (with the same comment),

double Sphericity::eigenValue(int i)  
gives one of the three eigenvalues for i = 1, 2 or 3, in descending order,

Vec4 Sphericity::eventAxis(i)  
gives the matching normalized eigenvector, as a Vec4 with vanishing time/energy component.

void Sphericity::list(ostream& os = cout)  
provides a listing of the above information.

There is also one method that returns information accumulated for all the events analyzed so far.

int Sphericity::nError()  
tells the number of times analyze(...) failed to analyze events, i.e. returned false.

Thrust

Thrust is obtained by varying the thrust axis so that the longitudinal momentum component projected onto it is maximized, and thrust itself is then defined as the sum of absolute longitudinal momenta divided by the sum of absolute momenta. The major axis is found correspondingly in the plane transverse to thrust, and the minor one is then defined to be transverse to both. Oblateness is the difference between the major and the minor values.

The calculation of thrust is more computer-time-intensive than e.g. linear sphericity, introduced above, and has no specific advantages except historical precedent. In the PYTHIA 6 implementation the search was sped up at the price of then not being guaranteed to hit the absolute maximum. The current implementation studies all possibilities, but at the price of being slower, with time consumption for an event with n particles growing like n^3.

To do thrust analyses you have to set up a Thrust instance, and then feed in events to it, one at a time. The results for the latest event are available as output from a few methods.

Thrust::Thrust(int select = 2)  
create a thrust analysis object, where
argument select (default = 2) : tells which particles are analyzed,
argumentoption 1 : all final-state particles,
argumentoption 2 : all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and
argumentoption 3 : only charged final-state particles.

bool Thrust::analyze( const Event& event, ostream& os = cout)  
perform a thrust analysis, where
argument event : is an object of the Event class, most likely the pythia.event one.
argument os (default = cout) : is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
If the routine returns false the analysis failed, e.g. if too few particles are present to analyze.

After the analysis has been performed, a few methods are available to return the result of the analysis of the latest event:

double Thrust::thrust()  
double Thrust::tMajor()  
double Thrust::tMinor()  
double Thrust::oblateness()  
gives the thrust, major, minor and oblateness values, respectively,

Vec4 Thrust::eventAxis(int i)  
gives the matching normalized event-axis vectors, for i = 1, 2 or 3 corresponding to thrust, major or minor, as a Vec4 with vanishing time/energy component.

void Thrust::list(ostream& os = cout)  
provides a listing of the above information.

There is also one method that returns information accumulated for all the events analyzed so far.

int Thrust::nError()  
tells the number of times analyze(...) failed to analyze events, i.e. returned false.

ClusterJet

ClusterJet (a.k.a. LUCLUS and PYCLUS) is a clustering algorithm of the type used for analyses of e^+e^- events, see the PYTHIA 6 manual. All visible particles in the events are clustered into jets. A few options are available for some well-known distance measures. Cutoff distances can either be given in terms of a scaled quadratic quantity like y = pT^2/E^2 or an unscaled linear one like pT.

Note that we have deliberately chosen not to include the e^+e^- equivalents of the Cambridge/Aachen and anti-kRT algorithms. These tend to be good at clustering the densely populated (in angle) cores of jets, but less successful for the sparsely populated transverse regions, where many jets may come to consist of a single low-momentum particle. In hadron collisions such jets could easily be disregarded, while in e^+e^- annihilation all particles derive back from the hard process.

To do jet finding analyses you have to set up a ClusterJet instance, and then feed in events to it, one at a time. The results for the latest event are available as output from a few methods.

ClusterJet::ClusterJet(string measure = "Lund", int select = 2, int massSet = 2, bool precluster = false, bool reassign = false)  
create a ClusterJet instance, where
argument measure (default = "Lund") : distance measure, to be provided as a character string (actually, only the first character is necessary)
argumentoption "Lund" : the Lund pT distance,
argumentoption "JADE" : the JADE mass distance, and
argumentoption "Durham" : the Durham kT measure.
argument select (default = 2) : tells which particles are analyzed,
argumentoption 1 : all final-state particles,
argumentoption 2 : all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and
argumentoption 3 : only charged final-state particles.
argument massSet (default = 2) : masses assumed for the particles used in the analysis
argumentoption 0 : all massless,
argumentoption 1 : photons are massless while all others are assigned the pi+- mass, and
argumentoption 2 : all given their correct masses.
argument precluster (default = false) : perform or not a early preclustering step, where nearby particles are lumped together so as to speed up the subsequent normal clustering.
argument reassign (default = false) : reassign all particles to the nearest jet each time after two jets have been joined.

ClusterJet::analyze( const Event& event, double yScale, double pTscale, int nJetMin = 1, int nJetMax = 0, ostream& os = cout)  
performs a jet finding analysis, where
argument event : is an object of the Event class, most likely the pythia.event one.
argument yScale : is the cutoff joining scale, below which jets are joined. Is given in quadratic dimensionless quantities. Either yScale or pTscale must be set nonvanishing, and the larger of the two dictates the actual value.
argument pTscale : is the cutoff joining scale, below which jets are joined. Is given in linear quantities, such as pT or m depending on the measure used, but always in units of GeV. Either yScale or pTscale must be set nonvanishing, and the larger of the two dictates the actual value.
argument nJetMin (default = 1) : the minimum number of jets to be reconstructed. If used, it can override the yScale and pTscale values.
argument nJetMax (default = 0) : the maximum number of jets to be reconstructed. Is not used if below nJetMin. If used, it can override the yScale and pTscale values. Thus e.g. nJetMin = nJetMax = 3 can be used to reconstruct exactly 3 jets.
argument os (default = cout) : is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
If the routine returns false the analysis failed, e.g. because the number of particles was smaller than the minimum number of jets requested.

After the analysis has been performed, a few ClusterJet class methods are available to return the result of the analysis:

int ClusterJet::size()  
gives the number of jets found, with jets numbered 0 through size() - 1.

Vec4 ClusterJet::p(int i)  
gives a Vec4 corresponding to the four-momentum defined by the sum of all the contributing particles to the i'th jet.

int ClusterJet::mult(int i)  
the number of particles that have been clustered into the i'th jet.

int ClusterJet::jetAssignment(int i)  
gives the index of the jet that the particle i of the event record belongs to,

void ClusterJet::list(ostream& os = cout)  
provides a listing of the reconstructed jets.

int ClusterJet::distanceSize()  
the number of most recent clustering scales that have been stored for readout with the next method. Normally this would be five, but less if fewer clustering steps occurred.

double ClusterJet::distance(int i)  
clustering scales, with distance(0) being the most recent one, i.e. normally the highest, up to distance(4) being the fifth most recent. That is, with n being the final number of jets, ClusterJet::size(), the scales at which n+1 jets become n, n+2 become n+1, and so on till n+5 become n+4. Nonexisting clustering scales are returned as zero. The physical interpretation of a scale is as provided by the respective distance measure (Lund, JADE, Durham).

There is also one method that returns information accumulated for all the events analyzed so far.

int ClusterJet::nError()  
tells the number of times analyze(...) failed to analyze events, i.e. returned false.

CellJet

CellJet (a.k.a. PYCELL) is a simple cone jet finder in the UA1 spirit, see the PYTHIA 6 manual. It works in an (eta, phi, eT) space, where eta is pseudorapidity, phi azimuthal angle and eT transverse energy. It will draw cones in R = sqrt(Delta-eta^2 + Delta-phi^2) around seed cells. If the total eT inside the cone exceeds the threshold, a jet is formed, and the cells are removed from further analysis. There are no split or merge procedures, so later-found jets may be missing some of the edge regions already used up by previous ones. Not all particles in the event are assigned to jets; leftovers may be viewed as belonging to beam remnants or the underlying event. It is not used by any experimental collaboration, but is closely related to the more recent and better theoretically motivated anti-kT algorithm [Cac08].

To do jet finding analyses you have to set up a CellJet instance, and then feed in events to it, one at a time. Especially note that, if you want to use the options where energies are smeared in order so emulate detector imperfections, you must hand in an external random number generator, preferably the one residing in the Pythia class. The results for the latest event are available as output from a few methods.

CellJet::CellJet(double etaMax = 5., int nEta = 50, int nPhi = 32, int select = 2, int smear = 0, double resolution = 0.5, double upperCut = 2., double threshold = 0., Rndm* rndmPtr = 0)  
create a CellJet instance, where
argument etaMax (default = 5.) : the maximum +-pseudorapidity that the detector is assumed to cover.
argument nEta (default = 50) : the number of equal-sized bins that the +-etaMax range is assumed to be divided into.
argument nPhi (default = 32) : the number of equal-sized bins that the phi range +-pi is assumed to be divided into.
argument select (default = 2) : tells which particles are analyzed,
argumentoption 1 : all final-state particles,
argumentoption 2 : all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and
argumentoption 3 : only charged final-state particles.
argument smear (default = 0) : strategy to smear the actual eT bin by bin,
argumentoption 0 : no smearing,
argumentoption 1 : smear the eT according to a Gaussian with width resolution * sqrt(eT), with the Gaussian truncated at 0 and upperCut * eT,
argumentoption 2 : smear the e = eT * cosh(eta) according to a Gaussian with width resolution * sqrt(e), with the Gaussian truncated at 0 and upperCut * e.
argument resolution (default = 0.5) : see above.
argument upperCut (default = 2.) : see above.
argument threshold (default = 0 GeV) : completely neglect all bins with an eT < threshold.
argument rndmPtr (default = 0) : the random-number generator used to select the smearing described above. Must be handed in for smearing to be possible. If your Pythia class instance is named pythia, then &pythia.rndm would be the logical choice.

bool CellJet::analyze( const Event& event, double eTjetMin = 20., double coneRadius = 0.7, double eTseed = 1.5, ostream& os = cout)  
performs a jet finding analysis, where
argument event : is an object of the Event class, most likely the pythia.event one.
argument eTjetMin (default = 20. GeV) : is the minimum transverse energy inside a cone for this to be accepted as a jet.
argument coneRadius (default = 0.7) : is the size of the cone in (eta, phi) space drawn around the geometric center of the jet.
argument eTseed (default = 1.5 GeV) : the minimum eT in a cell for this to be acceptable as the trial center of a jet.
argument os (default = cout) : is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
If the routine returns false the analysis failed, but currently this is not foreseen ever to happen.

After the analysis has been performed, a few CellJet class methods are available to return the result of the analysis:

int CellJet::size()  
gives the number of jets found, with jets numbered 0 through size() - 1,

double CellJet::eT(i)  
gives the eT of the i'th jet, where jets have been ordered with decreasing eT values,

double CellJet::etaCenter(int i)  
double CellJet::phiCenter(int i)  
gives the eta and phi coordinates of the geometrical center of the i'th jet,

double CellJet::etaWeighted(int i)  
double CellJet::phiWeighted(int i)  
gives the eta and phi coordinates of the eT-weighted center of the i'th jet,

int CellJet::multiplicity(int i)  
gives the number of particles clustered into the i'th jet,

Vec4 CellJet::pMassless(int i)  
gives a Vec4 corresponding to the four-momentum defined by the eT and the weighted center of the i'th jet,

Vec4 CellJet::pMassive(int i)  
gives a Vec4 corresponding to the four-momentum defined by the sum of all the contributing cells to the i'th jet, where each cell contributes a four-momentum as if all the eT is deposited in the center of the cell,

double CellJet::m(int i)  
gives the invariant mass of the i'th jet, defined by the pMassive above,

void CellJet::list()  
provides a listing of the above information (except pMassless, for reasons of space).

There is also one method that returns information accumulated for all the events analyzed so far.

int CellJet::nError()  
tells the number of times analyze(...) failed to analyze events, i.e. returned false.

SlowJet

SlowJet is a simple program for doing jet finding according to either of the kT, anti-kT, and Cambridge/Aachen algorithms, in a cylindrical coordinate frame. The name is obviously an homage to the FastJet program [Cac06, Cac12]. That package contains many more algorithms, with many more options, and, above all, is much faster. Therefore SlowJet is not so much intended for massive processing of data or Monte Carlo files as for simple first tests. Nevertheless, within the advertised capabilities of SlowJet, it has been checked to find identically the same jets as FastJet. The time consumption typically is around or below that to generate an LHC pp event in the first place, so is not prohibitive. But the time rises rapidly for large multiplicities, so obviously SlowJet can not be used for tricks like distributing a dense grid of pseudoparticles to be able to define jet areas, like FastJet can, and also not for events with much pileup or other noise.

The recent introduction of fjcore, containing the core functionality of FastJet in a very much smaller package, has changed the conditions. It now is possible (even encouraged by the authors) to distribute the two fjcore files as part of the PYTHIA package. Therefore the SlowJet class doubles as a convenient front end to fjcore, managing the conversion back and forth between PYTHIA and FastJet variables. Some applications may still benefit from using the native codes, but the default now is to let SlowJet call on fjcore for the jet finding.

The first step is to decide which particles should be included in the analysis, and with what four-momenta. The SlowJet constructor allows to pick a maximum pseudorapidity defined by the extent of the assumed detector, to pick among some standard options of which particles to analyze, and to allow for some standard mass assumptions, like that all charged particles have the pion mass. Obviously this is only a restricted set of possibilities.

Full flexibility can be obtained by deriving from the base class SlowJetHook to write your own include method. This will be presented with one final-state particle at a time, and should return true for those particles that should be analyzed. It is also possible to return modified four-momenta and masses, to take into account detector smearing effects or particle identity misassignments, but you must respect E^2 - p^2 = m^2.

Alternatively you can modify the event record itself, or a copy of it (if you want to keep the original intact). For instance, only final particles are considered in the analysis, i.e. particles with positive status code, so negative status code should then be assigned to those particles that you do not want to see analyzed. Again four-momenta and masses can be modified, subject to E^2 - p^2 = m^2.

The jet reconstructions is then based on sequential recombination with progressive removal, using the E recombination scheme. To be more specific, the algorithm works as follows.

  1. Each particle to be analyzed defines an original cluster. It has a well-defined four-momentum and mass at input. From this information the triplet (pT, y, phi) is calculated, i.e. the transverse momentum, rapidity and azimuthal angle of the cluster.
  2. Define distance measures of all clusters i to the beam
    d_iB = pT_i^2p
    and of all pairs (i,j) relative to each other
    d_ij = min( pT_i^2p, pT_j^2p) DeltaR_ij^2 / R^2
    where
    DeltaR_ij^2 = (y_i - y_j)^2 + (phi_i - phi_j)^2.
    The jet algorithm is determined by the user-selected p value, where p = -1 corresponds to the anti-kT one, p = 0 to the Cambridge/Aachen one and p = 1 to the kT one. Also R is chosen by the user, to give an approximate measure of the size of jets. However, note that jets need not have a circular shape in (y, phi) space, so R can not straight off be interpreted as a jet radius.
  3. Find the smallest of all d_iB and d_ij.
  4. If this is a d_iB then cluster i is removed from the clusters list and instead added to the jets list. Optionally, a pTjetMin requirement is imposed, where only clusters with pT > pTjetMin are added to the jets list. If so, some of the analyzed particles will not be part of any final jet.
  5. If instead the smallest measure is a d_ij then the four-momenta of the i and j clusters are added to define a single new cluster. Convert this four-momentum to a new (pT, y, phi) triplet and update the list of d_iB and d_ij.
  6. Return to step 3 until no clusters remain.

To do jet finding analyses you first have to set up a SlowJet instance, where the arguments of the constructor specifies the details of the subsequent analyses. Thereafter you can feed in events to it, one at a time, and have them analyzed by the analyze method. Information on the resulting jets can be extracted by a few different methods. The minimal procedure only requires one call per event to do the analysis. We will begin by presenting it, and only afterwards some extensions.

SlowJet::SlowJet(int power, double R, double pTjetMin = 0.,double etaMax = 25., int select = 2, int massSet = 2, SlowJetHook* sjHookPtr = 0, bool useFJcore = true, bool useStandardR = true)  
create a SlowJet instance, where
argument power : tells (half) the power of the transverse-momentum dependence of the distance measure,
argumentoption -1 : the anti-kT algorithm,
argumentoption 0 : the Cambridge/Aachen algorithm, and
argumentoption 1 : the kT algorithm.
argument R : the R size parameter, which is crudely related to the radius of the jet cone in (y, phi) space around the center of the jet.
argument pTjetMin (default = 0.0 GeV) : the minimum transverse momentum required for a cluster to become a jet. By default all clusters become jets, and therefore all analyzed particles are assigned to a jet. For comparisons with perturbative QCD, however, it is only meaningful to consider jets with a significant pT.
argument etaMax (default = 25.) : the maximum +-pseudorapidity that the detector is assumed to cover. If you pick a value above 20 there is assumed to be full coverage (obviously only meaningful for theoretical studies).
argument select (default = 2) : tells which particles are analyzed,
argumentoption 1 : all final-state particles,
argumentoption 2 : all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and
argumentoption 3 : only charged final-state particles.
argument massSet (default = 2) : masses assumed for the particles used in the analysis
argumentoption 0 : all massless,
argumentoption 1 : photons are massless while all others are assigned the pi+- mass, and
argumentoption 2 : all given their correct masses.
argument sjHookPtr (default = 0) : gives the possibility to send in your own selection routine for which particles should be part of the analysis; see further below on the SlowJetHook class. If this pointer is sent in nonzero, etaMax and massSet are disregarded, and select only gives the basic selection, to which the user can add further requirements.
argument useFJcore (default = true) : choice of code used for finding the jets. Does not affect the outcome of the analysis, but only the speed, and some more specialized options.
argumentoption true : use the fjcore package of FastJet 3.0.5.
argumentoption false : use the native SlowJet implementation, which gives a slower jet finding, but allows some extra options of step-by-step jet joining.
argument useStandardR (default = true) : definition of R distance between two jets. This switch is only meaningful for useFJcore = false; within the fjcore package the standard option below is always used.
argumentoption true : standard, as described above, DeltaR_ij^2 = (y_i - y_j)^2 + (phi_i - phi_j)^2.
argumentoption false : alternative, DeltaR_ij^2 = 2 (cosh(y_i - y_j) - cos(phi_i - phi_j)), which corresponds to the rim of the "deformed cone" giving a constant invariant mass between the two partons considered (for fixed masses and transverse momenta).

bool SlowJet::analyze( const Event& event)  
performs a jet finding analysis, where
argument event : is an object of the Event class, most likely the pythia.event one.
If the routine returns false the analysis failed, but currently this is not foreseen ever to happen.

After the analysis has been performed, a few SlowJet class methods are available to return the result of the analysis:

int SlowJet::sizeOrig()  
gives the original number of particles (and thus clusters) that the analysis starts with.

int SlowJet::sizeJet()  
gives the number of jets found, with jets numbered 0 through sizeJet() - 1, and ordered in terms of decreasing transverse momentum values w.r.t. the beam axis,

double SlowJet::pT(i)  
gives the transverse momentum pT of the i'th jet,

double SlowJet::y(int i)  
double SlowJet::phi(int i)  
gives the rapidity y and azimuthal angle phi of the center of the i'th jet (defined by the vector sum of constituent four-momenta),

Vec4 SlowJet::p(int i)  
double SlowJet::m(int i)  
gives a Vec4 corresponding to the four-momentum sum of the particles assigned to the i'th jet, and the invariant mass of this four-vector,

int SlowJet::multiplicity(int i)  
gives the number of particles clustered into the i'th jet,

vector<int> SlowJet::constituents(int i)  
gives a list of the indices of the particles that have been clustered into the i'th jet,

int SlowJet::jetAssignment(int i)  
gives the index of the jet that the particle i of the event record belongs to, or -1 if there is no jet containing particle i,

void SlowJet::removeJet(int i)  
removes the i'th jet,

void SlowJet::list()  
provides a listing of the basic jet information from above.

These are the basic methods. For more sophisticated usage it is possible to trace the clustering, one step at a time. It requires the native jet finding code, useFJcore = false in the constructor. If so, the setup method should be used to read in the event and find the initial smallest distance. Each subsequent doStep will then do one cluster joining and find the new smallest distance. You can therefore interrogate which clusters will be joined next before the joining actually is performed. Alternatively you can take several steps in one go, or take steps down to a predetermined number of jets plus remaining clusters.

bool SlowJet::setup( const Event& event)  
selects the particles to be analyzed, calculates initial distances, and finds the initial smallest distance.
argument event : is an object of the Event class, most likely the pythia.event one.
If the routine returns false the setup failed, but currently this is not foreseen ever to happen.

bool SlowJet::doStep()  
do the next step of the clustering. This can either be that two clusters are joined to one, or that a cluster is promoted to a jet (which is discarded if its pT value is below pTjetMin).
The routine will only return false if there are no clusters left, or if useFJcore = true.

bool SlowJet::doNSteps(int nStep)  
calls the doStep() method nStep times, if possible. Will return false if the list of clusters is emptied before then. The stored jet information is still perfectly fine; it is only the number of steps that is wrong. Will also return false if useFJcore = true.

bool SlowJet::stopAtN(int nStop)  
calls the doStep() method until a total of nStop jet and cluster objects remain. Will return false if this is not possible, specifically if the number of objects already is smaller than nStop when the method is called. The stored jet and cluster information is still perfectly fine; it only does not have the expected multiplicity. Will also return false if useFJcore = true.

int SlowJet::sizeAll()  
gives the total current number of jets and clusters. The jets are numbered 0 through sizeJet() - 1, while the clusters are numbered sizeJet() through sizeAll() - 1. (Internally jets and clusters are represented by two separate arrays, but are here presented in one flat range.) Note that the jets are ordered in decreasing pT, while the clusters are not ordered. When useFJcore = true there are no intermediate steps, and thus the number of clusters is zero (after jet finding).

With this extension, the methods double pT(int i), double y(int i), double phi(int i), Vec4 p(int i), double m(int i) and int multiplicity(int i) can be used as before. Furthermore, list() generalizes

void SlowJet::list(bool listAll = false, ostream& os = cout)  
provides a listing of the above information.
argument listAll : lists both jets and clusters if true, else only jets.

Three further methods can be used to check what will happen next.

int SlowJet::iNext()  
int SlowJet::jNext()  
double SlowJet::dNext()  
if the next step is to join two clusters, then the methods give the (i,j, d_ij) values, if instead to promote a cluster to a jet then (i, -1, d_iB). If no clusters remain then (-1, -1, 0.). Note that the cluster numbers are offset as described above, i.e. they begin at sizeJet(), which of course easily could be subtracted off. Also note that the jet and cluster lists are (moderately) reshuffled in each new step. When useFJcore = true there are no intermediate steps, and thus these methods do not return meaningul information.

Finally, and separately, the SlowJetHook class can be used for a more smart selection of which particles to include in the analysis. For instance, isolated and/or high-pT muons, electrons and photons should presumably be identified separately at an early stage, and then not clustered to jets.

Technically, it works like with User Hooks. That is, PYTHIA contains the base class. You write a derived class. In the main program you create an instance of this class, and hand it in to SlowJet; in this case already as part of the constructor.

The following methods should be defined in your derived class.

SlowJetHook::SlowJetHook()  
virtual SlowJetHook::~SlowJetHook()  
the constructor and destructor need not do anything, and if so you need not write your own destructor.

virtual bool SlowJetHook::include(int iSel, const Event& event, Vec4& pSel, double& mSel)  
is the main method that you will need to write. It will be called once for each final-state particle in an event, subject to the value of the select switch in the SlowJet constructor. The value select = 2 may be convenient since then you do not need to remove e.g. neutrinos yourself, but use select = 1 for full control. The method should then return true if you want to see particle included in the jet clustering, and false if not.
argument iSel : is the index in the event record of the currently studied particle.
argument event : is an object of the Event class, most likely the pythia.event one, where the currently studied particle is found.
argument pSel : is at input the four-momentum of the currently studied particle. You can change the values, e.g. to take into account energy smearing in the detector, to define the initial cluster value, without corrupting the event record itself.
argument mSel : is at input the mass of the currently studied particle. You can change the value, e.g. to take into account particle misidentification, to define the initial cluster value, without corrupting the event record itself. Note that the changes of pSel and mSel must be coordinated such that E^2 - p^2 = m^2 holds.

It is also possible to define further methods of your own. One such could e.g. be called directly in the main program before the analyze method is called, to identify and bookkeep some event properties you may not want to reanalyze for each individual particle. pythia8-8.1.80.orig/htmldoc/FlavourSelection.html0000644000175000017500000004447712217615311020154 0ustar sunsun Flavour Selection

Flavour Selection

The StringFlav class handles the choice of a new flavour in the fragmentation process, and the production of a new hadron from a set of input flavours. It is mainly used by the string fragmentation machinery (including ministrings), but also e.g. in some particle decays and for some beam-remnant cases. The basic concepts are in agreement with [And83]. The baryon-sector implementation is based on the MSTJ(12)=3 option of PYTHIA 6, i.e. new SU(6) weights scheme with at most one popcorn meson.

The relative production rates of different particle species is influenced by the parameters below. Some have only an impact on one specific quantity, but most directly or indirectly have consequences for many observables. Therefore the values to use have to be viewed in the context of a complete tune.

New flavours

The main parameters of the selection of a new flavour are

parm  StringFlav:probStoUD   (default = 0.19; minimum = 0.0; maximum = 1.0)
the suppression of s quark production relative to ordinary u or d one.

parm  StringFlav:probQQtoQ   (default = 0.09; minimum = 0.0; maximum = 1.0)
the suppression of diquark production relative to quark production, i.e. of baryon relative to meson production.

parm  StringFlav:probSQtoQQ   (default = 1.00; minimum = 0.0; maximum = 1.0)
the suppression of strange diquark production relative to light diquark production, over and above the one already given by probStoU.

parm  StringFlav:probQQ1toQQ0   (default = 0.027; minimum = 0.0; maximum = 1.0)
the suppression of spin 1 diquark production relative to spin 0 one, apart from the factor of 3 enhancement of spin 1 from counting the number of states.

Standard-meson production

The bulk of the particle production corresponds to the lowest-lying pseudoscalar and vector multiplets. Their production rates are determined by the parameters in this section.

For a given set of flavours, produced according to the probabilities outlined above, the ratio of vector-to-pseudocalar meson production is described by the parameters below. The maximum allowed rate for each case has been set according to spin-counting rules, but we expect the real rates to be lower, especially for lighter mesons, owing to the vector-pseudoscalar mass splitting.

parm  StringFlav:mesonUDvector   (default = 0.62; minimum = 0.; maximum = 3.)
the relative production ratio vector/pseudoscalar for light (u, d) mesons.

parm  StringFlav:mesonSvector   (default = 0.725; minimum = 0.; maximum = 3.)
the relative production ratio vector/pseudoscalar for strange mesons.

parm  StringFlav:mesonCvector   (default = 1.06; minimum = 0.; maximum = 3.)
the relative production ratio vector/pseudoscalar for charm mesons.

parm  StringFlav:mesonBvector   (default = 3.0; minimum = 0.; maximum = 3.)
the relative production ratio vector/pseudoscalar for bottom mesons.

Inside each light-quark meson nonet, an octet-singlet mixing angle describes the mixing of the two flavour-diagonal isoscalar = 0 states. (For terminology and details see [Yao06], chapter 14 on the quark model.) This angle is needed to specify the probability for such a q qbar state to project onto a specific meson. More transparent formulae are obtained by introducing the angle alpha = theta + 54.7 degrees:
f = (uubar + ddbar)/sqrt(2) * sin(alpha) + ssbar * cos(alpha)
f' = (uubar + ddbar)/sqrt(2) * cos(alpha) - ssbar * sin(alpha)

parm  StringFlav:thetaPS   (default = -15.; minimum = -90.; maximum = 90.)
gives the mixing angle theta_PS in the pseudoscalar meson sector (which is rather poorly determined), expressed in degrees. Here f is associated with eta' and f' with eta. (This standard but counterintuitive choice is fixed up in the code by replacing alpha -> 90^0 - alpha so that eta <-> eta'; relative signs do not matter since we are interested in probabilities only.)

parm  StringFlav:thetaV   (default = 36.; minimum = -90.; maximum = 90.)
gives the mixing angle theta_V in the vector meson sector (which is somewhat better determined), expressed in degrees. Here f is associated with omega and f' with phi.

Further, the simple model overestimates the production of eta and, in particular, eta' mesons, which can be rectified by

parm  StringFlav:etaSup   (default = 0.63; minimum = 0.; maximum = 1.)
the additional suppression of eta production, multiplying the normal production probability. Thus 0 means no eta at all are produced, while 1 means full rate.

parm  StringFlav:etaPrimeSup   (default = 0.12; minimum = 0.; maximum = 1.)
the additional suppression of eta' production, multiplying the normal production probability. Thus 0 means no eta' at all are produced, while 1 means full rate.

Excited-meson production

Several excited mesons, ie. with radial or orbital excitations, have been observed at non-negligible production rates. Extrapolated to all states a fair fraction of all particle production might proceed through such states. There are big uncertainties, however, since these excited mesons in many cases are extremely poorly known. This also means that the modeling of their production and decay is very primitive, and even that the inclusion of the production of such states may lead to a degraded agreement with data. Currently the default is that all such production is switched off.

Parameters are provided to switch them on. By demand, this machinery has been made more flexible than in the past. Therefore one parameter is provided for each combination of heaviest flavour (u/d, s, c or b) and multiplet produced. In each case the production rate is normalized to that of the lowest-lying pseudoscalar of the same flavour content, as for the vector-meson rates introduced above. The multiplets available are the four obtained for one unit of orbital angular momentum, in the nonrelativistic classification. Using J to denote the sum of quark spin S and orbital angular momentum L, i.e. what would normally be called the spin of the meson, one has:

  • a pseudovector multiplet with L=1, S=0, J=1;
  • a scalar multiplet with L=1, S=1, J=0;
  • a pseudovector multiplet with L=1, S=1, J=1;
  • a tensor multiplet with L=1, S=1, J=2.
The maximum allowed rate for each case has been set according to spin-counting rules, but we expect the real rates to be significantly lower, owing to mass suppression.

parm  StringFlav:mesonUDL1S0J1   (default = 0.0; minimum = 0.; maximum = 3.)
the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for light (u, d) mesons.

parm  StringFlav:mesonUDL1S1J0   (default = 0.0; minimum = 0.; maximum = 1.)
the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for light (u, d) mesons.

parm  StringFlav:mesonUDL1S1J1   (default = 0.0; minimum = 0.; maximum = 3.)
the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for light (u, d) mesons.

parm  StringFlav:mesonUDL1S1J2   (default = 0.0; minimum = 0.; maximum = 5.)
the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for light (u, d) mesons.

parm  StringFlav:mesonSL1S0J1   (default = 0.0; minimum = 0.; maximum = 3.)
the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for strange mesons.

parm  StringFlav:mesonSL1S1J0   (default = 0.0; minimum = 0.; maximum = 1.)
the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for strange mesons.

parm  StringFlav:mesonSL1S1J1   (default = 0.0; minimum = 0.; maximum = 3.)
the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for strange mesons.

parm  StringFlav:mesonSL1S1J2   (default = 0.0; minimum = 0.; maximum = 5.)
the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for strange mesons.

parm  StringFlav:mesonCL1S0J1   (default = 0.0; minimum = 0.; maximum = 3.)
the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for charm mesons.

parm  StringFlav:mesonCL1S1J0   (default = 0.0; minimum = 0.; maximum = 1.)
the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for charm mesons.

parm  StringFlav:mesonCL1S1J1   (default = 0.0; minimum = 0.; maximum = 3.)
the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for charm mesons.

parm  StringFlav:mesonCL1S1J2   (default = 0.0; minimum = 0.; maximum = 5.)
the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for charm mesons.

parm  StringFlav:mesonBL1S0J1   (default = 0.0; minimum = 0.; maximum = 3.)
the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for bottom mesons.

parm  StringFlav:mesonBL1S1J0   (default = 0.0; minimum = 0.; maximum = 1.)
the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for bottom mesons.

parm  StringFlav:mesonBL1S1J1   (default = 0.0; minimum = 0.; maximum = 3.)
the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for bottom mesons.

parm  StringFlav:mesonBL1S1J2   (default = 0.0; minimum = 0.; maximum = 5.)
the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for bottom mesons.

In addition, an octet-singlet mixing angle is needed for each multiplet, as for the pseudoscalar and vector multiplets above. Only for the tensor multiplet does any determination exist; for the other multiplets default has been chose so that ssbar does not mix with the light quarks, and so that the ssbar state is the heavier of the two.

parm  StringFlav:thetaL1S0J1   (default = 35.3; minimum = -90.; maximum = 90.)
gives the mixing angle theta in the (L=1,S=0,J=1) pseudovector meson sector, expressed in degrees.

parm  StringFlav:thetaL1S1J0   (default = 35.3; minimum = -90.; maximum = 90.)
gives the mixing angle theta in the (L=1,S=1,J=0) scalar meson sector, expressed in degrees.

parm  StringFlav:thetaL1S1J1   (default = 35.3; minimum = -90.; maximum = 90.)
gives the mixing angle theta in the (L=1,S=1,J=1) pseudovector meson sector, expressed in degrees.

parm  StringFlav:thetaL1S1J2   (default = 28.0; minimum = -90.; maximum = 90.)
gives the mixing angle theta in the (L=1,S=1,J=2) tensor meson sector, expressed in degrees.

Baryon production

The relative rate of baryon production is mainly given by the quark and diquark production parameters above, plus SU(6) Clebsch-Gordans. The one modifiable parameter related to these coefficients is

parm  StringFlav:decupletSup   (default = 1.0; minimum = 0.0; maximum = 1.0)
the suppression, relative to default SU(6) factors, of decuplet baryon production. Default corresponds to no suppression, while 0 corresponds to no decuplet production at all.

In addition, if popcorn production is allowed, wherein a set of mesons (M) may be produced in between the baryon (B) and the antibaryon (Bbar), a set of further parameters is introduced. Currently only the simplest scenario is implemented, wherein at most one intermediate meson may be produced.

parm  StringFlav:popcornRate   (default = 0.5; minimum = 0.; maximum = 2.0)
gives the relative rates of B Bbar and B M Bbar production, roughly as
Prob(B M Bbar) / (Prob(B Bbar) + Prob(B M Bbar)) = popcornRate / (0.5 + popcornRate)
(the complete expression depends on all the quark and diquark production parameters and is therefore not so useful).

parm  StringFlav:popcornSpair   (default = 0.5; minimum = 0.; maximum = 1.0)
extra suppression for having an s sbar pair shared between the B and Bbar in a B M Bbar configuration.

parm  StringFlav:popcornSmeson   (default = 0.5; minimum = 0.; maximum = 1.0)
extra suppression for having a strange meson M in a B M Bbar configuration.

Finally, there are some indications that leading-baryon production may be further suppressed. A proper description should probably be based on a suppression of early production times [Ede97], but we here only implement a simpler version where production near the end of a string, as defined by rank, is suppressed. The more detailed studies suggest that leading c and b baryon production will be less suppressed, so we leave it open to set light- and heavy-baryon suppression separately.

flag  StringFlav:suppressLeadingB   (default = off)
Suppress leading-baryon production.
option off : No suppression.
option on : Suppress the production of a diquark in the string breaking closest to a quark end of a string, by either of the factors below. This suppresses the production of first-rank baryons by the same amount. Indirectly also the second-rank and, if popcorn production is switched on, third-rank (anti)baryon production is affected.

parm  StringFlav:lightLeadingBSup   (default = 0.5; minimum = 0.; maximum = 1.0)
extra suppression of leading-baryon production for a light-quark jet, i.e. d, u or s, when suppressLeadingB = on. Thus 0 means no leading-baryon production at all, while 1 means full rate.

parm  StringFlav:heavyLeadingBSup   (default = 0.9; minimum = 0.; maximum = 1.0)
extra suppression of leading-baryon production for a heavy-quark jet, i.e. c or b, when suppressLeadingB = on. Thus 0 means no leading-baryon production at all, while 1 means full rate. pythia8-8.1.80.orig/htmldoc/Glossary.html0000644000175000017500000000600612217615312016456 0ustar sunsun Glossary

Glossary

BR
Beam Remnants; not much used since it may be confused with Branching Ratio
BSM
Beyond-the-Standard-Model physics, as a generic term for anything not contained within the SM
FSR
Final-State Radiation, implemented in terms of timelike showers
LHA
Les Houches Accord for user processes, describing which process-level information should be stored to allow further showering and hadronization of "skeleton" hard processes
LHAPDF
Les Houches Accord Parton Distribution Functions, originally a standard format for defining PDF's and later a library with such PDF's
LHEF
Les Houches Event File(s), a file format for storing LHA process and event information
ISR
Initial-State Radiation, implemented in terms of spacelike showers
MPI
Multiparton Interactions, i.e. several (more or less) independent parton-parton subcollisions as part of a hadron-hadron event (previously called MI for multiple interactions)
MSSM
Minimal Supersymmetric extension of the Standard Model
PDF
Parton Distribution Function (alternatively Parton Density Function)
PDG code
a scheme for assigning unique integers, particle identity codes, to known and hypothetical particles; code rules and tables are published in the RPP (see below).
pileup
several hadron-hadron collisions in a bunch crossing; not to be confused with MPI
RPP
Review of Particle Physics, the biannual review by the ParticleData Group (PDG) from which many Standard-Model parameter values and much particle data has been taken (but, given the poor data on many hadron resonances, a lot of extra (guess)work is needed)
setting
collectively used to denote all the boolean flag, integer mode, double-precision parm and string word variables that can be set by the user to steer the behaviour of a run; normally particle data are considered separately but clearly are closely related
SLHA
SUSY Les Houches Accord for interchange of mass and coupling information in SUSY scenarios, via a well-defined file format
SM
the Standard Model of particle physics
SUSY
SUperSYmmetry
units
Normal PYTHIA input, internal operations and output is based on a set of standard units, such as:
GeV for all energies, momenta and masses, always with c = 1;
mm for all distances and mm/c for all times, so that again they match for c = 1;
mb for all cross sections (but input or output via the Les Houches Accord takes into account that the unit there is pb)
pythia8-8.1.80.orig/htmldoc/SampleMainPrograms.html0000644000175000017500000003727712217615311020431 0ustar sunsun Sample Main Programs

Sample Main Programs

Descriptions of available classes, methods and settings are all very good and useful. Ultimately they are necessary for you to be able to fine-tune your runs to the task at hand. To get going, however, nothing helps like having explicit examples to study. This is what is provided in the examples subdirectory, along with instructions how they should be run:
  • main00.cc : does not exist, but it has been defined in the Makefile, so this name could be used for a simple first test run.
  • main01.cc : a simple study of the charged multiplicity for jet events at the LHC. (Brief example fitting on one slide.)
  • main02.cc : a simple study of the pT spectrum of Z bosons at the Tevatron. (Brief example fitting on one slide.)
  • main03.cc : a simple study of several different kinds of events, with the choice to be made in the main03.cmnd "cards file".
  • main04.cc : tests of cross sections, multiplicities and average transverse momenta for elastic, diffractive and nondiffractive topologies, using main04.cmnd to pick processes.
  • main05.cc : generation of QCD jet events at the LHC, with jet analysis using the SlowJet inclusive anti-kT sequential-recombination finder and the CellJet cone-jet finder.
  • main06.cc : generation of LEP1 hadronic events, i.e. e^+e^- -> gamma*/Z^0 -> q qbar, with charged multiplicity, sphericity, thrust and jet analysis.
  • main07.cc : set up a fictitious production process to a generic resonance, where you easily can compose your own list of (two-body) decay modes to a variety of final states. Also traces decay chains down to truly stable particles: gamma, e+-, p/pbar and neutrinos. Suitable for astroparticle applications, like neutralino pair annihilation, where cross sections are calculated separately in another program.
  • main08.cc : generation of the QCD jet cross section biased towards higher pT values, by two different techniques. Firstly, by splitting the run into subruns, each in its own pT bin, and adding the results properly reweighted. Two suboptions, with limits set either in the main program or by subrun specification in the main08.cmnd file. Secondly, by a continuous reweighting with a pT^4 bias in the selection, compensated by a 1/pT^4 event weight. Also inclusion of soft processes is illustrated, with subruns and weighted events.
  • main09.cc : generation of two predetermined hard interactions in each event.
  • main10.cc : illustration how userHooks can be used interact directly with the event-generation process.
  • main11.cc : a study of top events, fed in from the Les Houches Event File ttbar.lhe, here generated by PYTHIA 6.4. This file currently only contains 100 events so as not to make the distributed PYTHIA package too big, and so serves mainly as a demonstration of the principles involved.
  • main12.cc : a more sophisticated variant of main11.cc, where two Les Houches Event Files (ttbar.lhe and ttbar2.lhe) successively are used as input. Also illustrating some other aspects, like the capability to mix in internally generated events.
  • main13.cc : a streamlined version of main12.cc, where two Les Houches Event Files (ttbar.lhe and ttbar2.lhe) successively are used as input in main13.cmnd file.
  • main14.cc : a systematic comparison of several cross section values with their corresponding values in PYTHIA 6.4, the latter available as a table in the code.
  • main15.cc : loop over several tries, either to redo B decays only or to redo the complete hadronization chain of an event. Since much of the generation process is only made once this is a way to increase efficiency.
  • main16.cc : put all user analysis code into a class of its own, separate from the main program; provide the "cards file" name as a command-line argument. Also exemplifies how Higgs mass, width and branching ratios can be set by hand.
  • main17.cc : shows (a) how to use UserHooks to regularize onium cross section for pT -> 0, and (b) how decays could be handled externally.
  • main18.cc : shows how to write an event filter class, where you keep a vector of pointers to the subset of particles you want to study further. The event record itself remains unchanged.
  • main19.cc : use several instances of Pythia, one for signal events and others for a variable number of pileup and "beam-gas" events, combined into one common event record.
  • main20.cc : shows how PYTHIA 8 can write a Les Houches Event File, using facilities potentially useful also for other programs to write an LHEF.
  • main21.cc : an example how a single particle or various parton-level configurations can be input directly for hadronization, without being tied to the full process-generation machinery, e.g. to study the hadronization of junction topologies. Can also be used for single-resonance decays, with showers.
  • main22.cc : shows how an external resonance can be implemented as a new class derived from a PYTHIA base class, and be used in an external process, both of them handed in for generation as with normal internal classes.
  • main23.cc : shows how an external beam momentum spread and vertex location generator can be implemented as a new class derived from a PYTHIA base class, and then handed in for internal use. Also how to use an external random-number generator and an external parton distribution set.
  • main24.cc : tests of internally implemented cross sections for Supersymmetric particle production, with SUSY spectrum defined in cmssm.spc and settings in main24.cmnd. For illustration, an alternative example spectrum is also available, sps1aWithDecays.spc, which contains a decay table in SLHA format.
  • main25.cc : input RPV-SUSY events from an LHEF file that contains an SLHA spectrum inside its header. The event file, main25.lhe, contains a sample events that illustrate how to arrange color tags in the presence of the color-space epsilon tensors that accompany baryon number violating event topologies.
  • main26.cc : test program for processes in scenarios with large extra dimensions or unparticles.
  • main27.cc : production of Kaluza-Klein gamma/Z states in TeV-sized extra dimensions.
  • main28.cc : production of long-lived R-hadrons, that are forced to decay at a separate vertices and possibly with changed momenta.
  • main31.cc : exemplifies an improved matching of parton showers to LHEF-style input based on the POWHEG approach. The main31.cmnd allows to switch between several different matching options. It also allows to select input process, in this case either for the POWHEG-hvq program applied to top pair production [Cor10] or for QCD 2+3-jet events. The small samples of input events are stored in the powheg-hvq.lhe and powheg-dijets.lhe files, respectively.
  • main32.cc : exemplifies MLM merging, either in the ALPGEN variant or in the Madgraph one, and with input events either from ALPGEN or from Madgraph, with relevant control cards stored in main32.cmnd. See Jet Matching for further details. Traditionally the ALPGEN output is split into one file with events and another with parameters and cross sections (unlike in LHEF). Here a sample of W + 3 jets events is stored in main32.unw and the parameters to go with it in main32_unw.par. Madgraph events are taken from the w+_production_lhc_2.lhe file in this case.
  • main41.cc : similar to main01, except that the event record is output in the HepMC event record format. Requires that HepMC is properly linked. Note that the hepmcout41.dat output file can become quite big; so no example is included in this distribution.
  • main42.cc : a streamlined version for the generation of events that are then stored in HepMC format, without any event analysis. That is, all physics studies will have to be done afterwards. The name of the input "cards file" (e.g. main42.cmnd) and output HepMC event file (e.g. hepmcout42.dat) are to be provided as command-line arguments. Requires that HepMC is properly linked. Note that the HepMC output file can become quite big; so no example is included in this distribution.
  • main46.cc : illustrates how to write a ProMC file with PYTHIA events. Note that this example cannot (yet) be built by the PYTHIA Makefile, but a relevant Makefile is available on the ProMC webpage http://atlaswww.hep.anl.gov/asc/promc/.
  • main51.cc : a test of the shape of parton densities, as a check prior to using a given PDF set in a generator. Requires that LHAPDF is properly linked.
  • main52.cc : compares the charged multiplicity distribution, and a few other minimum-bias physics aspects, between default PYTHIA PDF and another one. Requires that LHAPDF is properly linked.
  • main53.cc : tests the possibility to do backwards evolution from an incoming photon at the hard interaction. Requires that you link to a LHAPDF set that includes the photon PDF.
  • main61.cc : a streamlined version for the generation of events that are then stored in HepMC format, without any event analysis. That is, just like main42.cc, with the difference that main61.cc can be used in conjunction with LHAPDF. The name of the input "cards file" (e.g. main61.cmnd) and output HepMC event file (e.g. hepmcout61.dat) are to be provided as command-line arguments. Requires that HepMC and LHAPDF are properly linked. Note that the HepMC output file can become quite big; so no example is included in this distribution.
  • main62.cc : a further extension of main61.cc, where subruns are used to process several consecutive LHEF, as in main13.cc, with information stored e.g in main62.cmnd. Other comments as for main61.cc.
  • main71.cc : an example how the FastJet jet finding package can be linked to allow an analysis of the final state, in this case for a study of W + jet production.
  • main72.cc : a comparison of SlowJet and FastJet jet finding, showing that they find the same jets if run under identical conditions, in this case for QCD jets.
  • main81.cc : do CKKW-L merging with a merging scale defined in kT. Input is provided by the main81.cmnd file and the three data files w+_production_lhc_0.lhe, w+_production_lhc_1.lhe and w+_production_lhc_2.lhe.
  • main82.cc : do CKKW-L merging with a user-defined merging scale function. Input is provided by the main82.cmnd file and the three data files w+_production_lhc_0.lhe, w+_production_lhc_1.lhe and w+_production_lhc_2.lhe.
  • main83.cc : as main82.cc but with an additional cut on the lowest multiplicity allowed for the reclustered state. The same input as for main82.cc can be used.
  • main84.cc : do CKKW-L merging with output in such a way that it can be used in subsequent RIVET analyses. Input is provided by the main84.cmnd file and the three data files w+_production_lhc_0.lhe, w+_production_lhc_1.lhe and w+_production_lhc_2.lhe.
  • main85.cc : do CKKW-L merging, with HepMC event output. Input settings are provided by the main85.cmnd file. This example program allows the use of input Les Houches events that are regularised with only very minimal cuts, and on which Pythia itself should enforce the more restrictive merging scale cut. The example program can be used with the input files w_production_tree_0.lhe, w_production_tree_1.lhe and w_production_tree_2.lhe.
  • main86.cc : do unitarised ME+PS (UMEPS) merging, with HepMC event output. Input settings are provided by the main86.cmnd file. This example program allows the consistent use of input Les Houches events that are regularised with only very minimal cuts, similar to main85.cc. The example program can be used with the input files w_production_tree_0.lhe, w_production_tree_1.lhe and w_production_tree_2.lhe. The program will produce positively and negatively weighted events. See UMEPS Merging for further details.
  • main87.cc : do NL3 NLO merging, with inclusive NLO input, and with HepMC event output. Input settings are provided by the main87.cmnd file. This example program allows the consistent use of input Les Houches events that are regularised with only very minimal cuts, similar to main85.cc. The example program can be used with the tree-level input files w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and the inclusive POWHEG input files w_production_powheg_0.lhe, w_production_powheg_1.lhe. The program will produce positively and negatively weighted events. See NLO Merging (NL3 section) for further details.
  • main88.cc : do unitarised NLO+PS (UNLOPS) merging, with inclusive NLO input, and with HepMC event output. Input settings are provided by the main88.cmnd file. This example program allows the consistent use of input Les Houches events that are regularised with only very minimal cuts, similar to main85.cc. The example program can be used with the tree-level input files w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and the inclusive POWHEG input files w_production_powheg_0.lhe, w_production_powheg_1.lhe. The program will produce positively and negatively weighted events. See NLO Merging (UNLOPS section) for further details.
In addition two main program illustrating the use of ROOT are available in the rootexamples subdirectory:
  • hist.cc : shows how ROOT can be used for histogramming in a program that for the rest is structured like a normal PYTHIA run.
  • tree.cc : shows how PYTHIA events can be stored as ROOT trees.
This subdirectory also contains a special Makefile and related documentation. pythia8-8.1.80.orig/htmldoc/SettingsScheme.html0000644000175000017500000005145712217615311017611 0ustar sunsun The Settings Scheme

The Settings Scheme

The Settings class keeps track of all the flags, modes, parameters and words used during the event generation. As such, it serves all the Pythia program elements from one central repository. Accessing it allows the user to modify the generator behaviour.

Each Pythia object has a public member settings of the Settings class. Therefore you access the settings methods as pythia.settings.command(argument), assuming that pythia is an instance of the Pythia class. Further, for the most frequent user tasks, Pythia methods have been defined, so that pythia.command(argument) would work, see further below.

The central section on this page is the Operation one. The preceding concepts section is there mainly to introduce the basic structure and the set of properties that can be accessed. The subsequent sections provide a complete listing of the existing public methods, which most users probably will have little interaction with.

Concepts

We distinguish six kinds of user-modifiable variables, by the way they have to be stored:
  1. Flags are on/off switches, and are stored as bool.
  2. Modes corresponds to a finite enumeration of separate options, and are stored as int.
  3. Parameters take a continuum of values, and are stored as double. The shorthand notation parm is used in the C++ code and XML tags.
  4. Words are simple character strings and are stored as string. No blanks or double quotation marks (") may appear inside a word, the former to simplify parsing of an input file and the latter not to cause conflicts with XML attribute delimiters. Currently the main application is to store file names.
  5. Vectors of modes take a variable length, and are stored as vector<int>. The shorthand notation mvec is used in the C++ code and XML tags. When the vector is input as a string, all the values have to be given as a comma-separated list with no blanks, to simplify parsing.
  6. Vectors of parameters take a variable length and for each element a continuum of values, and are stored as vector<double>. The shorthand notation pvec is used in the C++ code and XML tag. When the vector is input as a string, all the values have to be given as a comma-separated list with no blanks, to simplify parsing.
Note that all shorthands have been chosen four letters long.

In general, each variable stored in Settings is associated with four kinds of information:

  • The variable name, of the form class:name (or file:name, usually these agree), e.g. TimeShower:pTmin. The class/file part usually identifies the .xml file where the variable is defined, and the part of the program where it is used, but such a connection cannot be strictly upheld, since e.g. the same variable may be used in a few different cases (even if most of them are not).
  • The default value, set in the original declaration, and intended to represent a reasonable choice.
  • The current value, which differs from the default when the user so requests.
  • An allowed range of values, represented by meaningful minimum and maximum values. This has no sense for a flag or a word (and is not used there), is usually rather well-defined for a mode or mvec, but less so for a parm or pvec. Often the allowed range exaggerates the degree of our current knowledge, so as not to restrict too much what the user can do. One may choose not to set the lower or upper limit, in which case the range is open-ended.

Technically, the Settings class is implemented with the help of six separate maps, one for each kind of variable, with the variable name used as key.

Operation

The normal flow of setting values is:

  1. When a Pythia object pythia is created, the member pythia.settings is asked to scan the files listed in the Index.xml file in the xmldoc subdirectory.

    In all of the files scanned, lines beginning with <flag, <mode, <parm, <word, <mvec or <pvec are identified, and the information on such a line is used to define a new flag, mode, parameter, word, or vector of modes or parameters. To exemplify, consider a line

    <parm name="TimeShower:pTmin" default="0.5" min="0.1" max="2.0">
    
    which appears in the TimeShower.xml file, and there defines a parameter TimeShower:pTmin with default value 0.5 GeV and allowed variation in the range 0.1 - 2.0 GeV. The min and max values are optional.
    Important: the values in the .xml files should not be changed, except by the PYTHIA authors. Any changes should be done with the help of the methods described below.
  2. Between the creation of the Pythia object and the init call for it, you may use several alternative methods to modify some of the default values. The same variable can be changed several times. If so, it is the last read value that counts. The two special Tune:ee and Tune:pp modes and the Print:quiet flag are expanded to change several settings in one go, but these obey the same ordering rules.

    a) Inside your main program you can directly set values with

        pythia.readString(string) 
    
    where both the variable name and the value are contained inside the character string, separated by blanks and/or a =, e.g.
        pythia.readString("TimeShower:pTmin = 1.0"); 
    
    The match of the name to the database is case-insensitive. Names that do not match an existing variable are ignored. A warning is printed, however. Strings beginning with a non-alphanumeric character, like # or !, are assumed to be comments and are not processed at all. Values below the minimum or above the maximum are set at the respective border. For bool values, the following notation may be used interchangeably: true = on = yes = ok = 1, while everything else gives false (including but not limited to false, off, no and 0).

    b) The Pythia readString(string) method actually does not do changes itself, but sends on the string either to the Settings class or to ParticleData. The former holds if the string begins with a letter, the latter if it begins with a digit. If desired, it is possible to communicate directly with the corresponding Settings method:

        pythia.settings.readString("TimeShower:pTmin = 1.0"); 
    
    In this case, changes intended for ParticleData would not be understood.

    c) Underlying the settings.readString(string) method are the settings-type-sensitive commands in the Settings, that are split by names containing flag, mode, parm or word. Thus, the example now reads

        pythia.settings.parm("TimeShower:pTmin", 1.0); 
    
    Such a form could be convenient e.g. if a parameter is calculated at the beginning of the main program, and thus is available as a variable rather than as a character string. Note that Boolean values must here be given as true or false i.e. there is less flexibility than with the previous methods.

    At the same level, there are several different methods available. These are included in the full description below, but normally the user should have no need for them.

    d) A simpler and more useful way is to collect all your changes in a separate file, with one line per change, e.g.

        TimeShower:pTmin = 1.0
    
    Each line is read in as a string and processed with the methods already introduced. The file can be read by the
        pythia.readFile(fileName); 
    
    method (or an istream instead of a fileName). The file can freely mix commands to the Settings and ParticleData classes, and so is preferable. Lines with settings are handled by calls to the pythia.settings.readString(string) method.
  3. In the pythia.init(...) call, many of the various other program elements are initialized, making use of the current values in the database. Once initialized, the common Settings database is likely not consulted again by these routines. It is therefore not productive to do further changes in mid-run: at best nothing changes, at worst you may set up inconsistencies.

    A routine reInit(fileName) is provided, and can be used to zero all the maps and reinitialize them from scratch. Such a call might be useful if several subruns are to be made with widely different parameter sets - normally the maps are only built from scratch once, namely when the Pythia() object is created. A more economical alternative is offered by resetAll(), however, which sets all variables back to their default values.

  4. You may at any time obtain a listing of all variables in the database by calling
        pythia.settings.listAll();
    
    The listing is strictly alphabetical, which at least means that names from the same file are kept together, but otherwise may not be so well-structured: important and unimportant ones will appear mixed. A more relevant alternative is
        pythia.settings.listChanged();
    
    where you will only get those variables that differ from their defaults. Or you can use
        pythia.settings.list("string");
    
    where only those variables with names that contain the string (case-insensitive match) are listed. Thus, with a string shower, the shower-related variables would be shown.
  5. The above listings are in a tabular form that cannot be read back in. Assuming you want to save all changed settings (maybe because you read in changes from several files), you can do that by calling
        pythia.settings.writeFile(fileName);
    
    This file could then directly be read in by readFile(fileName) in a subsequent (identical) run. Some variants of this command are listed below.

Methods

The complete list of methods and arguments is as follows. Most of the ones of interest to the user have already been mentioned above. Others can be used, but the same functionality is better achieved by higher-level routines. Some are part of the internal machinery, and should not be touched by user.

Note that there is no Settings::readFile(...) method. The intention is that you should use Pythia::readFile(...). It parses and decides which individual lines should be sent on to Settings::readString(...).

Settings::Settings()  
the constructor, which takes no arguments. Internal.

bool Settings::initPtr(Info* infoPtrIn)  
initialize pointer to error-message database. Internal.

bool Settings::init(string startFile = "../xmldoc/Index.xml", bool append = false, ostream& os = cout)  
read in the settings database.
argument startFile (default = "../xmldoc/Index.xml") : read in the settings from all the files listed in this file, and assumed to be located in the same subdirectory.
argument append (default = false) : By default nothing is done if the method has already been called once. If true the further settings read in are added to the current database.
argument os (default = cout) : stream for error printout.
Note: The method returns false if it fails.

bool Settings::reInit(string startFile = "../xmldoc/Index.xml", ostream& os = cout)  
overwrite the existing database.
argument startFile (default = "../xmldoc/Index.xml") : read in the settings from all the files listed in this file, and assumed to be located in the same subdirectory.
argument os (default = cout) : stream for error printout.
Note: The method returns false if it fails.

bool Settings::readString(string line, bool warn = true, ostream& os = cout)  
read in a string, and change the relevant quantity in the database. It is normally used indirectly, via Pythia::readString(...) and Pythia::readFile(...).
argument line : the string to be interpreted as an instruction.
argument warn (default = true) : write a warning message or not whenever the instruction does not make sense, e.g. if the variable does not exist in the databases.
argument os (default = cout) : stream for error printout.
Note: the method returns false if it fails to make sense out of the input string.

bool Settings::writeFile(string toFile, bool writeAll = false)  
bool Settings::writeFile(ostream& os = cout, bool writeAll = false)  
write current settings to a file or to an ostream.
argument toFile, os : file or stream on which settings are written.
argument writeAll (default = false) : normally only settings that have been changed are written, but if true then all settings are output.
Note: the method returns false if it fails.

void Settings::listAll(ostream& os = cout)  
void Settings::listChanged(ostream& os = cout)  
void Settings::list(string match, ostream& os = cout)  
list all or changed settings, or a group of them.
argument match : list all those settings where the name contains the match (sub)string (case-insensitive).
argument os (default = cout) : output stream for the listing.

void Settings::resetAll()  
reset all current values to their defaults.

bool Settings::isFlag(string key)  
bool Settings::isMode(string key)  
bool Settings::isParm(string key)  
bool Settings::isWord(string key)  
bool Settings::isMVec(string key)  
bool Settings::isPVec(string key)  
return true if an entry of the given name and kind exists, else false.

void Settings::addFlag(string key, bool default)  
void Settings::addMode(string key, int default, bool hasMin, bool hasMax, int min, int max)  
void Settings::addParm(string key, double default, bool hasMin, bool hasMax, double min, double max)  
void Settings::addWord(string key, string default)  
void Settings::addMVec(string key, vector<int> default, bool hasMin, bool hasMax, int min, int max)  
void Settings::addPVec(string key, vector<double> default, bool hasMin, bool hasMax, double min, double max)  
add an entry of the respective kind to the database. The name and default value(s) always has to be supplied, for Mode, Parm, MVec and PVec additionally if lower and/or upper limits are to be imposed and, if so, what those limit are.

bool Settings::flag(string key)  
int Settings::mode(string key)  
double Settings::parm(string key)  
string Settings::word(string key)  
vector<int> Settings::mvec(string key)  
vector<double> Settings::pvec(string key)  
return the current value(s) of the respective setting. If the name does not exist in the database, a value false, 0, 0., " ", or a vector of length 1 and value 0 or 0., respectively, is returned.

bool Settings::flagDefault(string key)  
int Settings::modeDefault(string key)  
double Settings::parmDefault(string key)  
string Settings::wordDefault(string key)  
vector<int> Settings::mvecDefault(string key)  
vector<double> Settings::pvecDefault(string key)  
return the default value(s) of the respective setting. If the name does not exist in the database, a value false, 0, 0., " ", or a vector of length 1 and value 0 or 0., respectively, is returned.

map Settings::getFlagMap(string match)  
map Settings::getModeMap(string match)  
map Settings::getParmMap(string match)  
map Settings::getWordMap(string match)  
map Settings::getMVecMap(string match)  
map Settings::getPVecMap(string match)  
return a map of all settings of the respective type that contain the string "match" in its name.

void Settings::flag(string key, bool now)  
void Settings::mode(string key, int now)  
void Settings::parm(string key, double now)  
void Settings::word(string key, string now)  
void Settings::mvec(string key, vector<int> now)  
void Settings::pvec(string key, vector<double> now)  
change the current value(s) of the respective setting to the provided new value(s). If lower or upper limits have been set, input values outside the allowed range are reinterpreted as being a the nearest limit.

void Settings::forceMode(string key, int now)  
void Settings::forceParm(string key, double now)  
void Settings::forceMVec(string key, vector<int> now)  
void Settings::forcePVec(string key, vector<double> now)  
as above, but do not check lower and upper limits, so that the current value(s) can be put outside the intended borders.

void Settings::resetFlag(string key)  
void Settings::resetMode(string key)  
void Settings::resetParm(string key)  
void Settings::resetWord(string key)  
void Settings::resetMVec(string key)  
void Settings::resetPVec(string key)  
reset the current value to the default one. pythia8-8.1.80.orig/htmldoc/SemiInternalResonances.html0000644000175000017500000002727112217615312021275 0ustar sunsun Semi-Internal Resonances

Semi-Internal Resonances

The introduction of a new semi-internal process may also involve a new particle, not currently implemented in PYTHIA. Often it is then enough to use the standard machinery to introduce a new particle (id:all = ...) and new decay channels (id:addChannel = ...). By default this only allows you to define a fixed total width and fixed branching ratios. Using meMode values 100 or bigger provides the possibility of a very simple threshold behaviour.

If you want to have complete freedom, however, there are two ways to go. One is that you make the resonance decay part of the hard process itself, either using the Les Houches interface or a semi-internal process. The other is for you to create a new ResonanceWidths object, where you write the code needed for a calculation of the partial width of a particular channel.

Here we will explain what is involved in setting up a resonance. Should you actually go ahead with this, it is strongly recommended to use an existing resonance as a template, to get the correct structure. There also exists a sample main program, main22.cc, that illustrates how you could combine a new process and a new resonance.

There are three steps involved in implementing a new resonance:
1) providing the standard particle information, as already outlined above (id:all = ..., id:addChannel = ...), except that now branching ratios need not be specified, since they anyway will be overwritten by the dynamically calculated values.
2) writing the class that calculates the partial widths.
3) handing in a pointer to an instance of this class to PYTHIA.
We consider the latter two aspects in turn.

The ResonanceWidths Class

The resonance-width calculation has to be encoded in a new class. The relevant code could either be put before the main program in the same file, or be stored separately, e.g. in a matched pair of .h and .cc files. The latter may be more convenient, in particular if the calculations are lengthy, or likely to be used in many different runs, but of course requires that these additional files are correctly compiled and linked.

The class has to be derived from the ResonanceWidths base class. It can implement a number of methods. The constructor and the calcWidth ones are always needed, while others are for convenience. Much of the administrative machinery is handled by methods in the base class.

Thus, in particular, you must implement expressions for all possible final states, whether switched on in the current run or not, since all contribute to the total width needed in the denominator of the Breit-Wigner expression. Then the methods in the base class take care of selecting only allowed channels where that is required, and also of including effects of closed channels in secondary decays. These methods can be accessed indirectly via the res... methods of the normal particle database.

A constructor for the derived class obviously must be available. Here you are quite free to allow a list of arguments, to set the parameters of your model. The constructor must call the base-class initBasic(idResIn) method, where the argument idResIn is the PDG-style identity code you have chosen for the new resonance. When you create several related resonances as instances of the same class you would naturally make idResIn an argument of the constructor; for the PYTHIA classes this convention is used also in cases when it is not needed.
The initBasic(...) method will hook up the ResonanceWidths object with the corresponding entry in the generic particle database, i.e. with the normal particle information you set up in point 1) above. It will store, in base-class member variables, a number of quantities that you later may find useful:
idRes : the identity code you provide;
hasAntiRes : whether there is an antiparticle;
mRes : resonance mass;
GammaRes resonance width;
m2Res : the squared mass;
GamMRat : the ratio of width to mass.

A destructor is only needed if you plan to delete the resonance before the natural end of the run, and require some special behaviour at that point. If you call such a destructor you will leave a pointer dangling inside the Pythia object you gave it in to, if that still exists.

void ResonanceWidths::initConstants()  
is called once during initialization, and can then be used to set up further parameters specific to this particle species, such as couplings, and perform calculations that need not be repeated for each new event, thereby saving time. This method needs not be implemented.

void ResonanceWidths::calcPreFac(bool calledFromInit = false)  
is called once a mass has been chosen for the resonance, but before a specific final state is considered. This routine can therefore be used to perform calculations that otherwise might have to be repeated over and over again in calcWidth below. It is optional whether you want to use this method, however, or put everything in calcWidth().
The optional argument will have the value true when the resonance is initialized, and then be false throughout the event generation, should you wish to make a distinction. In PYTHIA such a distinction is made for gamma^*/Z^0 and gamma^*/Z^0/Z'^0, owing to the necessity of a special description of interference effects, but not for other resonances.
In addition to the base-class member variables already described above, mHat contains the current mass of the resonance. At initialization this agrees with the nominal mass mRes, but during the run it will not (in general).

void ResonanceWidths::calcWidth(bool calledFromInit = false)  
is the key method for width calculations and returns a partial width value, as further described below. It is called for a specific final state, typically in a loop over all allowed final states, subsequent to the calcPreFac(...) call above. Information on the final state is stored in a number of base-class variables, for you to use in your calculations:
iChannel : the channel number in the list of possible decay channels;
mult : the number of decay products;
id1, id2, id3 : the identity code of up to the first three decay products, arranged in descending order of the absolute value of the identity code;
id1Abs, id2Abs, id3Abs : the absolute value of the above three identity codes;
mHat : the current resonance mass, which is the same as in the latest calcPreFac(...) call;
mf1, mf2, mf3 : masses of the above decay products;
mr1, mr2, mr3 : squared ratio of the product masses to the resonance mass;
ps : is only meaningful for two-body decays, where it gives the phase-space factor ps = sqrt( (1. - mr1 - mr2)^2 - 4. * mr1 * mr2 );
In two-body decays the third slot is zero for the above properties. Should there be more than three particles in the decay, you would have to take care of the subsequent products yourself, e.g. using
particlePtr->decay[iChannel].product(j);
to extract the j'th decay products (with j = 0 for the first, etc.). Currently we are not aware of any such examples.
The base class also contains methods for alpha_em and alpha_strong evaluation, and can access many standard-model couplings; see the existing code for examples.
The result of your calculation should be stored in
widNow : the partial width of the current channel, expressed in GeV.

double ResonanceWidths::widthChan( double mHat, int idAbs1, int idAbs2)  
is not normally used. In PYTHIA the only exception is Higgs decays, where it is used to define the width (except for colour factors) associated with a specific incoming/outgoing state. It allows the results of some loop expressions to be pretabulated.

bool ResonanceWidths::allowCalc()  
can normally be left dummy (and then always returns true) but can optionally be used to determine whether to force dynamical width calculation to be switched off (return false). An example is provided by the SUSYResonanceWidths class, in which the implementation of this method checks for the existence of SLHA decay tables for the particular resonance in question, and checks if those tables should be given precedence over the internal width calculation.

bool ResonanceWidths::initBSM()  
can normally be left dummy, but for advanced implementations it provides a possibility to initialize data members of the derived class at a very early stage during initialization, before any of the other members are called. An example is provided by the SUSYResonanceWidths class, in which an internal pointer to a derived Couplings class must be (re)set before any of the other methods are used. A return value of false can be used to signal that this initialization step failed.

Access to resonance widths

Once you have implemented a class, it is straightforward to make use of it in a run. Assume you have written a new class MyResonance, which inherits from ResonanceWidths. You then create an instance of this class and hand it in to a pythia object with
      ResonanceWidths* myResonance = new MyResonance();
      pythia.setResonancePtr( myResonance); 
If you have several resonances you can repeat the procedure any number of times. When pythia.init(...) is called these resonances are initialized along with all the internal resonances, and treated in exactly the same manner. See also the Program Flow description.

If the code should be of good quality and general usefulness, it would be simple to include it as a permanently available process in the standard program distribution. The final step of that integration ought to be left for the PYTHIA authors, but basically all that is needed is to add one line in ParticleData::initResonances, where one creates an instance of the resonance in the same way as for the resonances already there. In addition, the particle data and decay table for the new resonance has to be added to the permanent particle database, and the code itself to include/ResonanceWidths.h and src/ResonanceWidths.cc. pythia8-8.1.80.orig/htmldoc/BeamShape.html0000644000175000017500000000712712217615312016505 0ustar sunsun Beam Shape

Beam Shape

The Beam Parameters page explains how you can set a momentum spread of the two incoming beams, and a spread and offset for the location of the interaction vertex. The spread is based on a simple parametrization in terms of independent Gaussians, however, which is likely to be too primitive for realistic applications.

It is therefore possible to define your own class, derived from the BeamShape base class, and hand it in to Pythia with the pythia.setBeamShapePtr( BeamShape*) method. Below we describe what such a class has to do. An explicit toy example is shown in main23.cc.

The BeamShape base class has a very simple structure. It only has two main virtual methods. The first, init(), is used for initialization. The second, pick(), selects beam momentum and production vertex in the current event.

BeamShape::BeamShape()  
virtual BeamShape::~BeamShape()  
the constructor and destructor do not need to do anything.

virtual void BeamShape::init( Settings& settings, Rndm* rndmPtrIn)  
the base-class method simply reads in the relevant values stored in the Settings data base, and saves a pointer to the random-number generator. You are free to write your own derived initialization routine, or use the existing one. In the latter case you can then give your own modified interpretation to the beam spread parameters defined there.
The two flags Beams:allowMomentumSpread and Beams:allowVertexSpread should not be tampered with, however. These are checked elsewhere to determine whether the beam shape should be set or not, whereas the other momentum-spread and vertex-spread parameters are local to this class.

virtual void BeamShape::pick()  
this method is the key one to supply in the derived class. Here you are free to pick whatever parametrization you desire for beam momenta and vertex position, including correlations between the two. At the end of the day, you should set a few protected double numbers:
deltaPxA, deltaPyA, deltaPzA for the three-momentum shift of the first incoming beam, relative to the nominal values;
deltaPxB, deltaPyB, deltaPzB for the three-momentum shift of the second incoming beam, relative to the nominal values;
vertexX, vertexY, vertexZ, vertexT for the production-vertex position and time.
As usual, momentum is given in GeV, and space and time in mm, with c = 1.

Vec4 BeamShape::deltaPA()  
Vec4 BeamShape::deltaPB()  
read out the three-momentum shifts for beams A and B that were set by pick(). The energy components are put to zero at this stage, since they are most conveniently calculated after the original and the shift three-momenta have been added.

Vec4 BeamShape::vertex()  
read out the production-vertex position and time that were set by pick(). pythia8-8.1.80.orig/htmldoc/ErrorChecks.html0000644000175000017500000001147612217615312017074 0ustar sunsun Error Checks

Error Checks

There is a few settings related to error checking during program execution. Many other checks are performed as well, but do not have any specific setting related to themselves.

flag  Check:abortIfVeto   (default = off)
There are a few ways in which an event can be vetoed, the most common being a User Hooks test. Normally this will simply mean that the next parton-level configuration is selected inside the Pythia::next() routine, without any need for a user intervention. With this option switched on, however, Pythia::next() will return false. It is then up to the user to decide what to do next.

flag  Check:particleData   (default = off)
Check the particle data tables for potential problems during initialization. This includes inconsistent use of charge in particle names, inconsistent setup of mass, mass range, width and lifetime, sum of branching ratios not unity (allowed but discouraged) or charge not conserved in a decay channel. Warnings should be viewed as reasons to check further, but need not indicate a true problem, and also not all problems may be caught. The pythia.particleData.checkTable(level) method, used for these checks, may also be called directly.

mode  Check:levelParticleData   (default = 1)
The level of verbosity and checks of particle data, if switched on.
option 0 : minimal amount of checks, e.g. that no channels open.
option 1 : further warning if individual channels closed, except for resonances.
option 2 : also print branching-ratio-averaged threshold mass except for resonances.
option 11 : as 1, but include resonances in detailed checks.
option 12 : as 2, but include resonances in detailed checks.

flag  Check:event   (default = on)
When an event has been successfully generated, check that the final event record in event does not contain any unphysical particles, or nonconserved charge or energy-momentum. If this check fails, then pythia.next() obtains the value false, i.e. the event is counted as aborted.

flag  Check:history   (default = on)
When Check:event = on and the event is checked as above, further checks are made that all mother and daughter pointers are consistently set. Specifically that all daughters in the daughterlist (or motherList) have the particle in their respective motherList (or daughterlist). This operation takes a bit more time than the other error tests (of the order of 10% of what it takes to generate the event in the first place), and so could be switched off to save time.

mode  Check:nErrList   (default = 0)
The number of erroneous events, in the above check, for which event listing and other detailed information will be printed. After that, only the normal error messages will be issued. Error counters are always updated, and accumulated numbers can be shown with pythia.statistics() at the end of the run.

parm  Check:epTolErr   (default = 1e-4)
Maximum allowed summed deviation of E, p_x, p_y and p_z between the incoming beams and the final state, as a fraction of the initial energy, above which the event is counted as aborted. (Unfortunately roundoff errors do not scale linearly with the energy, and also have a very long tail. So while most events at lower energies may be correct to better than 1e-10, at LHC it does not have to signal any fundamental bug if also the default tolerance above is violated occasionally.)

parm  Check:epTolWarn   (default = 1e-6)
A check on the same summed deviation as above, but counted as a warning rather than an error, and not leading to the event being classified as aborted. pythia8-8.1.80.orig/htmldoc/PartonDistributions.html0000644000175000017500000001474412217615312020711 0ustar sunsun Parton Distributions

Parton Distributions

The parton distributions file contains the PDF class. PDF is the base class, from which specific PDF classes are derived.

The choice of which PDF to use is made by settings in the Pythia class, see here. These settings also allow to access all the proton PDF's available in the LHAPDF library [Wha05]. Thus there is no need for a normal user to study the PDF class. The structure must only be understood when interfacing new PDF's, e.g. ones not yet found in LHAPDF.

The PDF base class

PDF defines the interface that all PDF classes should respect. The constructor requires the incoming beam species to be given: even if used for a proton PDF, one needs to know whether the beam is actually an antiproton. This is one of the reasons why Pythia always defines two PDF objects in an event, one for each beam.

Once a PDF object has been constructed, call it pdf, the main method is pdf.xf( id, x, Q2), which returns x*f_id(x, Q2), properly taking into account whether the beam is an antiparticle or not.

Whenever the xf member is called with a new flavour, x or Q^2, the xfUpdate member is called to do the actual updating. This routine may either update that particular flavour or all flavours at this (x, Q^2) point. (In the latter case the saved id value idSav should be set to 9.) The choice is to be made by the producer of a given set, based on what he/she deems most effective, given that sometimes only one flavour need be evaluated, and about equally often all flavours are needed at the same x and Q^2. Anyway, the latest value is always kept in memory. This is the other reason why Pythia has one separate PDF object for each beam, so that values at different x can be kept in memory.

Two further public methods are xfVal( id, x, Q2) and xfSea( id, x, Q2). These are simple variants whereby the quark distributions can be subdivided into a valence and a sea part. If these are not directly accessible in the parametrization, one can make the simplified choices u_sea = ubar_sea, u_val = u_tot - u_sea, and correspondingly for d. (Positivity will always be guaranteed at output.) The xfUpdate method should also take care of updating this information.

A method setExtrapolate(bool) allows you to switch between freezing parametrizations at the x and Q^2 boundaries (false) or extrapolating them outside the boundaries (true). This method is only implemented for the LHAPDF class below. If you implement a new PDF you are free to use this method, but it would be smarter to hardcode the desired limiting behaviour.

Derived classes

There is only one pure virtual method, xfUpdate, that therefore must be implemented in any derived class. A reasonable number of such classes come with the program:

For protons:

  • LHAPDFinterface provides an interface to the LHAPDF library[Wha05].
  • GRV94L gives the GRV 94 L parametrization [Glu95].
  • CTEQ5L gives the CTEQ 5 L parametrization [Lai00].
  • MSTWpdf gives the four distributions of the MRST/MSTW group that have been implemented.
  • CTEQ6pdf gives the six distributions of the CTEQ/CT group that have been implemented.
  • NNPDF gives four distributions from the NNPDF 2.3 QCD+QED sets that have been implemented.
The current default is CTEQ 5L, which has been used in most studies to date.

For charged pions:

  • GRVpiL gives the GRV 1992 pi+ parametrization.

For Pomerons (used to describe diffraction):

  • PomFix gives a simple but flexible Q2-independent parametrization.
  • PomH1FitAB gives the H1 2006 Fit A and Fit B parametrizations.
  • PomH1Jets gives the H1 2007 Jets parametrization.

For charged leptons (e, mu, tau):

  • Lepton gives a QED parametrization [Kle89]. In QED there are not so many ambiguities, so here one set should be enough. On the other hand, there is the problem that the lepton-inside-lepton pdf is integrably divergent for x -> 1, which gives numerical problems. Like in PYTHIA 6, the pdf is therefore made to vanish for x > 1 - 10^{-10}, and scaled up in the range 1 - 10^{-7} < x < 1 - 10^{-10} in such a way that the total area under the pdf is preserved.
  • LeptonPoint gives the trivial distribution of a pointlike (i.e. unresolved) charged lepton.

For neutrinos:

  • NeutrinoPoint is the only method, so there is no choice. Analogously to LeptonPoint it gives the distribution of a pointlike (i.e. unresolved) neutrino. A difference, however, is that neutrinos always are lefthanded, so there is no need to average over incoming spin states. Since the PYTHIA formalism assumes unpolarized beams, and thus implicitly includes a 1/2 for incoming fermions, the NeutrinoPoint PDF is normalized to 2 rather than 1 to compensate for this.

There is another method, isSetup(), that returns the base-class boolean variable isSet. This variable is initially true, but could be set false if the setup procedure of a PDF failed, e.g. if the user has chosen an unknown PDF set.

The MRST/MSTW, CTEQ/CT, NNPDF and H1 PDF routines are based on the interpolation in (x, Q) grids. The grid files are stored in the xmldoc subdirectory, like settings and particle data. 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Onia Processes

Production of J/psi or Upsilon, directly and via chi states and the colour-octet mechanism. In each process the square-bracketed expression specifies the state in spectroscopic notation, (2S+1) L J, followed by (1) for colour-singlet states and (8) for colour-octet ditto.

The original Fortran code for these processes has been contributed by Stefan Wolf [unpublished]. For the C++ version only the unpolarized expressions are retained, since the theoretical predictions of the colour-octet model anyway do not agree with the experimental observations. Furthermore, the polarization effects are modest, so isotropic decay is not a bad starting point. Such an event sample can afterwards be reweighted at will by the user, to test various assumptions.

The description of final-state radiation is in this case based on some further model assumptions.

Most of the processes below are divergent in the limit pT -> 0, and therefore a pTmin scale should be set. Comparisons with data indicate that this divergence can be tamed the same way as for the normal QCD 2 -> 2 cross sections [Bar06,Kra08], which makes sense, since they are all dominated by the same kind of t-channel gluon exchange. It is therefore possible to use the SuppressSmallPT user hook to impose a reweighting that cancels the low-pT divergence.

An eikonalized description of these processes is included in the multiparton-interactions framework. Here the low-pT dampening is automatic, and additionally the framework is more consistent (e.g. with respect to energy-momentum constraints and the impact-parameter description) for events where the onium production is not the hardest subprocess, as would often be the case in the low-pT limit.

Charmonium

flag  Charmonium:all   (default = off)
Common switch for the group of charmonium production.

flag  Charmonium:gg2QQbar[3S1(1)]g   (default = off)
g g -> ccbar[3S1(1)] g. Code 401.

flag  Charmonium:gg2QQbar[3P0(1)]g   (default = off)
g g -> ccbar[3P0(1)] g. Code 402.

flag  Charmonium:gg2QQbar[3P1(1)]g   (default = off)
g g -> ccbar[3P1(1)] g. Code 403.

flag  Charmonium:gg2QQbar[3P2(1)]g   (default = off)
g g -> ccbar[3P2(1)] g. Code 404.

flag  Charmonium:qg2QQbar[3P0(1)]q   (default = off)
q g -> ccbar[3P0(1)] q. Code 405.

flag  Charmonium:qg2QQbar[3P1(1)]q   (default = off)
q g -> ccbar[3P1(1)] q. Code 406.

flag  Charmonium:qg2QQbar[3P2(1)]q   (default = off)
q g -> ccbar[3P2(1)] q. Code 407.

flag  Charmonium:qqbar2QQbar[3P0(1)]g   (default = off)
q qbar -> ccbar[3P0(1)] g. Code 408.

flag  Charmonium:qqbar2QQbar[3P1(1)]g   (default = off)
q qbar -> ccbar[3P1(1)] g. Code 409.

flag  Charmonium:qqbar2QQbar[3P2(1)]g   (default = off)
q qbar -> ccbar[3P2(1)] g. Code 410.

flag  Charmonium:gg2QQbar[3S1(8)]g   (default = off)
g g -> ccbar[3S1(8)] g. Code 411.

flag  Charmonium:gg2QQbar[1S0(8)]g   (default = off)
g g -> ccbar[3S1(8)] g. Code 412.

flag  Charmonium:gg2QQbar[3PJ(8)]g   (default = off)
g g -> ccbar[3S1(8)] g. Code 413.

flag  Charmonium:qg2QQbar[3S1(8)]q   (default = off)
q g -> ccbar[3S1(8)] q. Code 414.

flag  Charmonium:qg2QQbar[1S0(8)]q   (default = off)
q g -> ccbar[3S1(8)] q. Code 415.

flag  Charmonium:qg2QQbar[3PJ(8)]q   (default = off)
q g -> ccbar[3S1(8)] q. Code 416.

flag  Charmonium:qqbar2QQbar[3S1(8)]g   (default = off)
q qbar -> ccbar[3S1(8)] g. Code 417.

flag  Charmonium:qqbar2QQbar[1S0(8)]g   (default = off)
q qbar -> ccbar[3S1(8)] g. Code 418.

flag  Charmonium:qqbar2QQbar[3PJ(8)]g   (default = off)
q qbar -> ccbar[3S1(8)] g. Code 419.

Bottomonium

flag  Bottomonium:all   (default = off)
Common switch for the group of charmonium production.

flag  Bottomonium:gg2QQbar[3S1(1)]g   (default = off)
g g -> bbbar[3S1(1)] g. Code 501.

flag  Bottomonium:gg2QQbar[3P0(1)]g   (default = off)
g g -> bbbar[3P0(1)] g. Code 502.

flag  Bottomonium:gg2QQbar[3P1(1)]g   (default = off)
g g -> bbbar[3P1(1)] g. Code 503.

flag  Bottomonium:gg2QQbar[3P2(1)]g   (default = off)
g g -> bbbar[3P2(1)] g. Code 504.

flag  Bottomonium:qg2QQbar[3P0(1)]q   (default = off)
q g -> bbbar[3P0(1)] q. Code 505.

flag  Bottomonium:qg2QQbar[3P1(1)]q   (default = off)
q g -> bbbar[3P1(1)] q. Code 506.

flag  Bottomonium:qg2QQbar[3P2(1)]q   (default = off)
q g -> bbbar[3P2(1)] q. Code 507.

flag  Bottomonium:qqbar2QQbar[3P0(1)]g   (default = off)
q qbar -> bbbar[3P0(1)] g. Code 508.

flag  Bottomonium:qqbar2QQbar[3P1(1)]g   (default = off)
q qbar -> bbbar[3P1(1)] g. Code 509.

flag  Bottomonium:qqbar2QQbar[3P2(1)]g   (default = off)
q qbar -> bbbar[3P2(1)] g. Code 510.

flag  Bottomonium:gg2QQbar[3S1(8)]g   (default = off)
g g -> bbbar[3S1(8)] g. Code 511.

flag  Bottomonium:gg2QQbar[1S0(8)]g   (default = off)
g g -> bbbar[3S1(8)] g. Code 512.

flag  Bottomonium:gg2QQbar[3PJ(8)]g   (default = off)
g g -> bbbar[3S1(8)] g. Code 513.

flag  Bottomonium:qg2QQbar[3S1(8)]q   (default = off)
q g -> bbbar[3S1(8)] q. Code 514.

flag  Bottomonium:qg2QQbar[1S0(8)]q   (default = off)
q g -> bbbar[3S1(8)] q. Code 515.

flag  Bottomonium:qg2QQbar[3PJ(8)]q   (default = off)
q g -> bbbar[3S1(8)] q. Code 516.

flag  Bottomonium:qqbar2QQbar[3S1(8)]g   (default = off)
q qbar -> bbbar[3S1(8)] g. Code 517.

flag  Bottomonium:qqbar2QQbar[1S0(8)]g   (default = off)
q qbar -> bbbar[3S1(8)] g. Code 518.

flag  Bottomonium:qqbar2QQbar[3PJ(8)]g   (default = off)
q qbar -> bbbar[3S1(8)] g. Code 519.

Onium matrix elements

The implementation of charmonium and bottomonium production, including the colour-octet production mechanism, requires information on NRQCD matrix elements for the various wavefunctions involved. Default values for these are encoded in the following ten variables. They are taken from [Nas00]; see also [Bar06].

parm  Charmonium:OJpsi3S11   (default = 1.16; minimum = 0.0)
<O(J/psi)[3S1(1)]>.

parm  Charmonium:OJpsi3S18   (default = 0.0119; minimum = 0.0)
<O(J/psi)[3S1(8)]>.

parm  Charmonium:OJpsi1S08   (default = 0.01; minimum = 0.0)
<O(J/psi)[1S0(8)]>.

parm  Charmonium:OJpsi3P08   (default = 0.01; minimum = 0.0)
<O(J/psi)[3P0(8)]>/m_c^2.

parm  Charmonium:Ochic03P01   (default = 0.05; minimum = 0.0)
<O(chi_c0)[3P0(8)]>/m_c^2.

parm  Bottomonium:OUpsilon3S11   (default = 9.28; minimum = 0.0)
<O(Upsilon)[3S1(1)]>.

parm  Bottomonium:OUpsilon3S18   (default = 0.15; minimum = 0.0)
<O(Upsilon)[3S1(8)]>.

parm  Bottomonium:OUpsilon1S08   (default = 0.02; minimum = 0.0)
<O(Upsilon)[1S0(8)]>.

parm  Bottomonium:OUpsilon3P08   (default = 0.02; minimum = 0.0)
<O(Upsilon)[3P0(8)]>/m_b^2.

parm  Bottomonium:Ochib03P01   (default = 0.085; minimum = 0.0)
<O(chi_b0)[3P0(8)]>/m_b^2. pythia8-8.1.80.orig/htmldoc/ElectroweakProcesses.html0000644000175000017500000002717712217615311021022 0ustar sunsun Electroweak Processes

Electroweak Processes

This page contains processes involving Prompt-photon, gamma^*/Z^0 and W^+- production, plus a few with t-channel boson exchange.

Prompt photon processes

This group collects the processes where one or two photons are produced by the hard process. Additional sources of photons include parton showers and hadron decays. A pT cut is required to stay away from the unphysical low-pT region. An eikonalized description, intended to be valid at all pT, is included as part of the multiparton-interactions framework.

flag  PromptPhoton:all   (default = off)
Common switch for the group of all prompt photon processes, as listed separately in the following.

flag  PromptPhoton:qg2qgamma   (default = off)
Scattering q g -> q gamma. Code 201.

flag  PromptPhoton:qqbar2ggamma   (default = off)
Scattering q qbar -> g gamma. Code 202.

flag  PromptPhoton:gg2ggamma   (default = off)
Scattering g g -> g gamma.
Note: This is a box graph. The full quark-mass dependence in the loop leads to very complicated expressions. The current implementation is based on assuming five massless quarks (see below), and thus is questionable at small (pT < m_b) or large (pT > m_t) transverse momenta. Code 203.

flag  PromptPhoton:ffbar2gammagamma   (default = off)
Scattering q qbar -> gamma gamma. Code 204.

flag  PromptPhoton:gg2gammagamma   (default = off)
Scattering g g -> gamma gamma.
Note: This is a box graph. The full quark-mass dependence in the loop leads to very complicated expressions. The current implementation is based on assuming five massless quarks (see below), and thus is questionable at small (pT < m_b) or large (pT > m_t) transverse momenta. Code 205.

mode  PromptPhoton:nQuarkLoop   (default = 5; minimum = 3; maximum = 6)
Number of quark flavours included in the box graphs responsible for g g -> g gamma and g g-> gamma gamma processes. Owing to the complexity if the massive expressions, quarks are treated as massless. The default value should be applicable in the range of transverse momenta above the b mass but below the t one.

Weak boson processes

Under this heading we group processes involving the production of a single electroweak gauge boson, i.e. a gamma^*/Z^0 or a W^+-, or a pair of them, or one of them in combination with a parton. Since the three sets are partly conflicting, each is associated with its own group flag. In addition, t-channel exchange of such a boson between two fermions form a separate group.

There is one flag that can be used to influence the gamma^*/Z^0 structure in all the processes below where it is produced, unless otherwise stated.

mode  WeakZ0:gmZmode   (default = 0; minimum = 0; maximum = 2)
Choice of full gamma^*/Z^0 structure or not in relevant processes.
option 0 : full gamma^*/Z^0 structure, with interference included.
option 1 : only pure gamma^* contribution.
option 2 : only pure Z^0 contribution.
Note: irrespective of the option used, the particle produced will always be assigned code 23 for Z^0, and open decay channels is purely dictated by what is set for the Z^0.

Boson exchange

The two processes in this subgroup is included as part of the multiparton-interactions framework.

flag  WeakBosonExchange:all   (default = off)
Common switch for the group of gamma^*/Z^0 or W^+- exchange between two fermions.

flag  WeakBosonExchange:ff2ff(t:gmZ)   (default = off)
Scattering f f' -> f f' via gamma^*/Z^0 t-channel exchange, with full interference between the gamma^* and Z^0. Code 211.

flag  WeakBosonExchange:ff2ff(t:W)   (default = off)
Scattering f_1 f_2 -> f_3 f_4 via W^+- t-channel exchange. Code 212.

Single boson

flag  WeakSingleBoson:all   (default = off)
Common switch for the group of a single gamma^*/Z^0 or W^+- production.

flag  WeakSingleBoson:ffbar2gmZ   (default = off)
Scattering f fbar -> gamma^*/Z^0, with full interference between the gamma^* and Z^0. Code 221.

flag  WeakSingleBoson:ffbar2W   (default = off)
Scattering f fbar' -> W^+-. Code 222.

flag  WeakSingleBoson:ffbar2ffbar(s:gm)   (default = off)
Scattering f fbar -> gamma^* -> f' fbar'. Subset of process 221, but written as a 2 -> 2 process, so that pT can be used as ordering variable, e.g. in multiparton interactions. Hardcoded for the final state being either of the five quark flavours or three lepton ones. Not included in the WeakSingleBoson:all set, but included in the multiparton-interactions framework. Code 223.

Boson pair

Note that, in the decay of the two vector bosons produced by an f fbar -> V V process, the full four-fermion correlations from the leading-order f fbar -> V V -> 4f matrix elements are included [Gun86] (with some extensions by the authors). The matrix elements are provided in the double-resonant approach, i.e. excludes graph like f fbar -> V -> f fbar -> f fbar V -> 4f.

flag  WeakDoubleBoson:all   (default = off)
Common switch for the group of pair production of gamma^*/Z^0 and W^+-.

flag  WeakDoubleBoson:ffbar2gmZgmZ   (default = off)
Scattering f fbar' -> gamma^*/Z^0 gamma^*/Z^0. Code 231.

flag  WeakDoubleBoson:ffbar2ZW   (default = off)
Scattering f fbar' -> Z^0 W^+-. Note that here the gamma^* contribution is not (currently) included. Code 232.

flag  WeakDoubleBoson:ffbar2WW   (default = off)
Scattering f fbar -> W^+ W^-. Code 233.

Boson and parton

flag  WeakBosonAndParton:all   (default = off)
Common switch for the group of production of a single electroweak gauge boson, i.e. a gamma^*/Z^0 or a W^+-, in association with a parton, i.e. a quark, gluon, photon or lepton. These processes give first-order corrections to the ones in the WeakSingleBoson class, and both sets cannot be used simultaneously without unphysical double-counting. The current class should only be used to study the high-pT tail of the gauge-boson production processes (for LHC applications at least pT > 20 GeV), while the ones in WeakSingleBoson should be used for inclusive production.

flag  WeakBosonAndParton:qqbar2gmZg   (default = off)
Scattering q qbar -> gamma^*/Z^0 g. Code 241.

flag  WeakBosonAndParton:qg2gmZq   (default = off)
Scattering q g -> gamma^*/Z^0 q . Code 242.

flag  WeakBosonAndParton:ffbar2gmZgm   (default = off)
Scattering f fbar -> gamma^*/Z^0 gamma. Code 243.

flag  WeakBosonAndParton:fgm2gmZf   (default = off)
Scattering f gamma -> gamma^*/Z^0 f. Code 244.

flag  WeakBosonAndParton:qqbar2Wg   (default = off)
Scattering q qbar -> W^+- g. Code 251.

flag  WeakBosonAndParton:qg2Wq   (default = off)
Scattering q g -> W^+- q. Code 252.

flag  WeakBosonAndParton:ffbar2Wgm   (default = off)
Scattering f fbar -> W^+- gamma. Code 253.

flag  WeakBosonAndParton:fgm2Wf   (default = off)
Scattering f gamma -> W^+- f. Code 254.

Photon Collision Processes

A few electroweak two-photon production processes are available. To use them, photon PDFs have to be defined for the incoming beam particles. For proton beams an appropriate set would be MRST QED 2004 [Mar05], available in the LHAPDF library.

flag  PhotonCollision:all   (default = off)
Common switch for the group of six processes presented below.

flag  PhotonCollision:gmgm2qqbar   (default = off)
Scatterings gamma gamma -> q qbar, where q is a light quark (u, d, s) . Code 261.

flag  PhotonCollision:gmgm2ccbar   (default = off)
Scattering gamma gamma -> c cbar. Code 262.

flag  PhotonCollision:gmgm2bbbar   (default = off)
Scattering gamma gamma -> b bbar. Code 263.

flag  PhotonCollision:gmgm2ee   (default = off)
Scattering gamma gamma -> e+ e-. Code 264.

flag  PhotonCollision:gmgm2mumu   (default = off)
Scattering gamma gamma -> mu+ mu-. Code 265.

flag  PhotonCollision:gmgm2tautau   (default = off)
Scattering gamma gamma -> tau+ tau-. Code 266. pythia8-8.1.80.orig/htmldoc/PDFSelection.html0000644000175000017500000005717112217615311017142 0ustar sunsun PDF Selection

PDF Selection

This page contains five subsections. The first deals with how to pick the parton distribution set for protons, including from LHAPDF, to be used for all proton and antiproton beams. The second is a special option that allows a separate PDF set to be used for the hard process only, while the first choice would still apply to everything else. The third and fourth give access to pion and Pomeron PDF's, respectively, the latter being used to describe diffractive systems. The fifth gives the possibility to switch off the lepton "parton density". More information on PDF classes is found here.

Parton densities for protons

The selection of parton densities is made once and then is propagated through the program. It is essential to make an informed choice, for several reasons [Kas10]:
Warning 1: the choice of PDF set affects a number of properties of events. A change of PDF therefore requires a complete retuning e.g. of the multiparton-interactions model for minimum-bias and underlying events.
Warning 2: People often underestimate the differences between different sets on the market. The sets for the same order are constructed to behave more or less similarly at large x and Q^2, while the multiparton interactions are dominated by the behaviour in the region of small x and Q^2. A good PDF parametrization ought to be sensible down to x = 10^-6 (x = 10^-7) and Q^2 = 1 GeV^2 for Tevatron (LHC) applications. Unfortunately there are distributions on the market that completely derail in that region. The main51.cc and main52.cc programs in the examples subdirectory provide some examples of absolutely minimal sanity checks before a new PDF set is put in production.
Warning 3: NLO and LO sets tend to have quite different behaviours, e.g. NLO ones have less gluons at small x, which then is compensated by positive corrections in the NLO matrix elements. Therefore do not blindly assume that an NLO tune has to be better than an LO one when combined with the LO matrix elements in PYTHIA. There are explicit examples where such thinking can lead you down the wrong alley, especially if you study low-pT physics. In the list below you should therefore be extra cautious when using set 6 or set 9.

The simplest option is to pick one of the distributions available internally:

mode  PDF:pSet   (default = 2; minimum = 1; maximum = 16)
Parton densities to be used for proton beams (and, by implication, antiproton ones):
option 1 : GRV 94L, LO alpha_s(M_Z) = 0.128 (this set is out of date, but retained for historical comparisons).
option 2 : CTEQ 5L, LO alpha_s(M_Z) = 0.127 (this set is also out of date, but not badly so, and many tunes are based on it).
option 3 : MRST LO* (2007), NLO alpha_s(M_Z) = 0.12032.
option 4 : MRST LO** (2008), NLO alpha_s(M_Z) = 0.11517.
option 5 : MSTW 2008 LO (central member), LO alpha_s(M_Z) = 0.13939.
option 6 : MSTW 2008 NLO (central member), NLO alpha_s(M_Z) = 0.12018 (NLO, see Warning 3 above).
option 7 : CTEQ6L, NLO alpha_s(M_Z) = 0.1180.
option 8 : CTEQ6L1, LO alpha_s(M_Z) = 0.1298.
option 9 : CTEQ66.00 (NLO, central member), NLO alpha_s(M_Z) = 0.1180 (NLO, see Warning 3 above).
option 10 : CT09MC1, LO alpha_s(M_Z) = 0.1300.
option 11 : CT09MC2, NLO alpha_s(M_Z) = 0.1180.
option 12 : CT09MCS, NLO alpha_s(M_Z) = 0.1180.
option 13 : NNPDF2.3 QCD+QED LO alpha_s(M_Z) = 0.130.
option 14 : NNPDF2.3 QCD+QED LO alpha_s(M_Z) = 0.119.
option 15 : NNPDF2.3 QCD+QED NLO alpha_s(M_Z) = 0.119.
option 16 : NNPDF2.3 QCD+QED NNLO alpha_s(M_Z) = 0.119.
Note: the alpha_s(M_Z) values and the order of the running in the description above is purely informative, and does not affect any other parts of the program. Instead you have the freedom to set alpha_s(M_Z) value and running separately for hard processes (including resonance decays), multiparton interactions, initial-state radiation, and final-state radiation.

This is a reasonably complete list of recent LO fits, both ones within the normal LO context and ones with modifications for better matching to event generators. In addition two older sets are included for backwards reference (most studies to date are based on CTEQ 5L). If you link to the LHAPDF library [Wha05] you get access to a much wider selection.
Warning 1: owing to previous problems with the behaviour of PDF's beyond the x and Q^2 boundaries of a set, you should only use LHAPDF version 5.3.0 or later.
Warning 2: the behaviour of the LHAPDF sets need not be identical with the implementation found in PYTHIA. Specifically we are aware of the following points that may influence a comparison.
(a) CTEQ 5L in PYTHIA is the parametrization, in LHAPDF the grid interpolation.
(b) MRST LO* and LO** in PYTHIA is based on an updated edition, where one makes use of the expanded MSTW grid format, while LHAPDF is based on the original smaller grid.
(c) The CTEQ 6 and CT09MC sets in PYTHIA are frozen at the boundaries of the grid, by recommendation of the authors, while LHAPDF also offers an option with a smooth extrapolation outside the grid boundaries.

flag  PDF:useLHAPDF   (default = off)
If off then the choice of proton PDF is based on PDF:pSet above. If on then it is instead based on the choice of PDF:LHAPDFset and PDF:LHAPDFmember below.
Note: in order for this option to work you must have compiled PYTHIA appropriately and have set the LHAPATH environment variable to provide the data-files directory of your local LHAPDF installation. See the README file in the examples directory for further instructions.

word  PDF:LHAPDFset   (default = MRST2004FF4lo.LHgrid)
Name of proton PDF set from LHAPDF to be used. You have to choose from the list of available sets. Examples of some fairly recent ones (but still less recent than found above) would be cteq61.LHpdf, cteq61.LHgrid, cteq6l.LHpdf, cteq6ll.LHpdf, MRST2004nlo.LHpdf, MRST2004nlo.LHgrid, MRST2004nnlo.LHgrid and MRST2004FF3lo.LHgrid. If you pick a LHpdf set it will require some calculation the first time it is called.
Technical note: if you provide a name beginning with a slash (/) it is assumed you want to provide the full file path and then initPDFsetM(name) is called, else the correct path is assumed already set and initPDFsetByNameM(name) is called.

mode  PDF:LHAPDFmember   (default = 0; minimum = 0)
Further choice of a specific member from the set picked above. Member 0 should normally correspond to the central value, with higher values corresponding to different error PDF's somewhat off in different directions. You have to check from set to set which options are open.
Note: you can only use one member in a run, so if you want to sweep over many members you either have to do many separate runs or, as a simplification, save the pdf weights at the hard scattering and do an offline reweighting of events.

flag  PDF:extrapolateLHAPDF   (default = off)
Parton densities have a guaranteed range of validity in x and Q^2, and what should be done beyond that range usually is not explained by the authors of PDF sets. Nevertheless these boundaries very often are exceeded, e.g. minimum-bias studies at LHC may sample x values down to 10^-8, while many PDF sets stop already at 10^-5. The default behaviour is then that the PDF's are frozen at the boundary, i.e. xf(x,Q^2) is fixed at its value at x_min for all values x < x_min, and so on. This is a conservative approach. Alternatively, if you switch on extrapolation, then parametrizations will be extended beyond the boundaries, by some prescription. In some cases this will provide a more realistic answer, in others complete rubbish. Another problem is that some of the PDF-set codes will write a warning message anytime the limits are exceeded, thus swamping your output file. Therefore you should study a set seriously before you run it with this switch on.

If you want to use PDF's not found in LHAPDF, or you want to interface LHAPDF another way, you have full freedom to use the more generic interface options.

Parton densities for protons in the hard process

The above options provides a PDF set that will be used everywhere: for the hard process, the parton showers and the multiparton interactions alike. As already mentioned, therefore a change of PDF should be accompanied by a complete retuning of the whole MPI framework, and maybe more. There are cases where one may want to explore different PDF options for the hard process, but would not want to touch the rest. If several different sets are to be compared, a simple reweighting based on the originally used flavour, x, Q^2 and PDF values may offer the best route. The options in this section allow a choice of the PDF set for the hard process alone, while the choice made in the previous section would still be used for everything else. The hardest interaction of the minimum-bias process is part of the multiparton-interactions framework and so does not count as a hard process here.

Of course it is inconsistent to use different PDF's in different parts of an event, but if the x and Q^2 ranges mainly accessed by the components are rather different then the contradiction would not be too glaring. Furthermore, since standard PDF's are one-particle-inclusive we anyway have to 'invent' our own PDF modifications to handle configurations where more than one parton is kicked out of the proton [Sjo04].

The PDF choices that can be made are the same as above, so we do not repeat the detailed discussion.

flag  PDF:useHard   (default = off)
If on then select a separate PDF set for the hard process, using the variables below. If off then use the same PDF set for everything, as already chosen above.

mode  PDF:pHardSet   (default = 2; minimum = 1; maximum = 16)
Parton densities to be used for proton beams (and, by implication, antiproton ones):
option 1 : GRV 94L, LO alpha_s(M_Z) = 0.128 (out of date).
option 2 : CTEQ 5L, LO alpha_s(M_Z) = 0.127 (slightly out of date; many tunes are based on it).
option 3 : MRST LO* (2007), NLO alpha_s(M_Z) = 0.12032.
option 4 : MRST LO** (2008), NLO alpha_s(M_Z) = 0.11517.
option 5 : MSTW 2008 LO (central member), LO alpha_s(M_Z) = 0.13939.
option 6 : MSTW 2008 NLO (central member), LO alpha_s(M_Z) = 0.12018.
option 7 : CTEQ6L, NLO alpha_s(M_Z) = 0.1180.
option 8 : CTEQ6L1, LO alpha_s(M_Z) = 0.1298.
option 9 : CTEQ66.00 (NLO, central member), NLO alpha_s(M_Z) = 0.1180.
option 10 : CT09MC1, LO alpha_s(M_Z) = 0.1300.
option 11 : CT09MC2, NLO alpha_s(M_Z) = 0.1180.
option 12 : CT09MCS, NLO alpha_s(M_Z) = 0.1180.
option 13 : NNPDF2.3 QCD+QED LO alpha_s(M_Z) = 0.130.
option 14 : NNPDF2.3 QCD+QED LO alpha_s(M_Z) = 0.119.
option 15 : NNPDF2.3 QCD+QED NLO alpha_s(M_Z) = 0.119.
option 16 : NNPDF2.3 QCD+QED NNLO alpha_s(M_Z) = 0.119.

flag  PDF:useHardLHAPDF   (default = off)
If off then the choice of proton PDF is based on hardpPDFset above. If on then it is instead based on the choice of hardLHAPDFset and hardLHAPDFmember below. Note that if you want to use LHAPDF here, and you also use LHAPDF for the "normal" PDF set, then LHAPDF must have been compiled so as to handle (at least) two concurrent sets, with the configure statement --with-max-num-pdfsets=2.

word  PDF:hardLHAPDFset   (default = MRST2004FF4lo.LHgrid)
Name of proton PDF set from LHAPDF to be used.

mode  PDF:hardLHAPDFmember   (default = 0; minimum = 0)
Further choice of a specific member from the set picked above.

Note that there is no separate equivalent of the PDF:extrapolateLHAPDF flag specifically for the hard PDF. Since LHAPDF only has one global flag for extrapolation or not, the choice for the normal PDF's also applies to the hard ones.

Parton densities for pions

The parton densities of the pion are considerably less well known than those of the proton. There are only rather few sets on the market, and none particularly recent. Only one comes built-in, but others can be accessed from LHAPDF. Input parametrizations are for the pi+. >From this the pi- is obtained by charge conjugation and the pi0 from averaging (half the pions have d dbar valence quark content, half u ubar.

Much of the switches are taken over from the proton case, with obvious modifications; therefore the description is briefer. Currently we have not seen the need to allow separate parton densities for hard processes. When using LHAPDF the PDF:extrapolateLHAPDF switch of the proton also applies to pions.

mode  PDF:piSet   (default = 1; minimum = 1; maximum = 1)
Internal parton densities that can be used for pion beams, currently with only one choice.
option 1 : GRV 92 L.

flag  PDF:piUseLHAPDF   (default = off)
If off then the choice of proton PDF is based on PDF:piSet above. If on then it is instead based on the choice of PDF:piLHAPDFset and PDF:piLHAPDFmember below.

word  PDF:piLHAPDFset   (default = OWPI.LHgrid)
Name of pion PDF set from LHAPDF to be used. You have to choose from the list of available sets.

mode  PDF:piLHAPDFmember   (default = 0; minimum = 0)
Further choice of a specific member from the set picked above.

Parton densities for Pomerons

The Pomeron is introduced in the description of diffractive events, i.e. a diffractive system is viewed as a Pomeron-proton collision at a reduced CM energy. Here the PDF's are even less well known. Most experimental parametrizations are NLO, which makes them less well suited for Monte Carlo applications. Furthermore note that the momentum sum is arbitrarily normalized to a non-unity value.

mode  PDF:PomSet   (default = 6; minimum = 1; maximum = 6)
Parton densities that can be used for Pomeron beams.
option 1 : Q^2-independent parametrizations xf(x) = N_ab x^a (1 - x)^b, where N_ab ensures unit momentum sum. The a and b parameters can be set separately for the gluon and the quark distributions. The momentum fraction of gluons and quarks can be freely mixed, and production of s quarks can be suppressed relative to that of d and u ones, with antiquarks as likely as quarks. See further below how to set the six parameters of this approach.
option 2 : pi0 distributions, as specified in the section above.
option 3 : the H1 2006 Fit A NLO Q^2-dependent parametrization, based on a tune to their data [H1P06], rescaled by the factor PomRescale below.
option 4 : the H1 2006 Fit B NLO Q^2-dependent parametrization, based on a tune to their data [H1P06], rescaled by the factor PomRescale below.
option 5 : the H1 2007 Jets NLO Q^2-dependent parametrization, based on a tune to their data [H1P07], rescaled by the factor PomRescale below.
option 6 : the H1 2006 Fit B LO Q^2-dependent parametrization, based on a tune to their data [H1P06], rescaled by the factor PomRescale below.

parm  PDF:PomGluonA   (default = 0.; minimum = -0.5; maximum = 2.)
the parameter a in the ansatz xg(x) = N_ab x^a (1 - x)^b for option 1 above.

parm  PDF:PomGluonB   (default = 3.; minimum = 0.; maximum = 10.)
the parameter b in the ansatz xg(x) = N_ab x^a (1 - x)^b for option 1 above.

parm  PDF:PomQuarkA   (default = 0.; minimum = -0.5; maximum = 2.)
the parameter a in the ansatz xq(x) = N_ab x^a (1 - x)^b for option 1 above.

parm  PDF:PomQuarkB   (default = 3.; minimum = 0.; maximum = 10.)
the parameter b in the ansatz xq(x) = N_ab x^a (1 - x)^b for option 1 above.

parm  PDF:PomQuarkFrac   (default = 0.2; minimum = 0.; maximum = 1.)
the fraction of the Pomeron momentum carried by quarks for option 1 above, with the rest carried by gluons.

parm  PDF:PomStrangeSupp   (default = 0.5; minimum = 0.; maximum = 1.)
the suppression of the s quark density relative to that of the d and u ones for option 1 above.

parm  PDF:PomRescale   (default = 1.0; minimum = 0.5; maximum = 5.0)
Rescale the four H1 fits above by this uniform factor, e.g. to bring up their momentum sum to around unity. By default all three have a momentum sum of order 0.5, suggesting that a factor around 2.0 should be used. You can use examples/main51.cc to get a more precise value. Note that also other parameters in the diffraction framework may need to be retuned when this parameter is changed.

Parton densities for leptons

For electrons/muons/taus there is no need to choose between different parametrizations, since only one implementation is available, and should be rather uncontroversial (apart from some technical details). However, insofar as e.g. e^+ e^- data often are corrected back to a world without any initial-state photon radiation, it is useful to have a corresponding option available here.

flag  PDF:lepton   (default = on)
Use parton densities for lepton beams or not. If off the colliding leptons carry the full beam energy, if on part of the energy is radiated away by initial-state photons. In the latter case the initial-state showers will generate the angles and energies of the set of photons that go with the collision. In addition one collinear photon per beam carries any leftover amount of energy not described by shower emissions. If the initial-state showers are switched off these collinear photons will carry the full radiated energy.

Neutrinos are always taken pointlike. Do note that the phase space selection machinery currently does not allow one resolved and one unresolved beam. For lepton-neutrino collisions to work you must therefore set PDF:lepton = off.

Incoming parton selection

There is one useful degree of freedom to restrict the set of incoming quark flavours for hard processes. It does not change the PDF's as such, only which quarks are allowed to contribute to the hard-process cross sections. Note that separate but similarly named modes are available for multiparton interactions and spacelike showers.

mode  PDFinProcess:nQuarkIn   (default = 5; minimum = 0; maximum = 5)
Number of allowed incoming quark flavours in the beams; a change to 4 would thus exclude b and bbar as incoming partons, etc. pythia8-8.1.80.orig/htmldoc/LeftRightSymmetryProcesses.html0000644000175000017500000002002212217615311022175 0ustar sunsun Left-Right-Symmetry Processes

Left-Right-Symmetry Processes

At current energies, the world is left-handed, i.e. the Standard Model contains an SU(2)_L group. Left-right symmetry at some larger scale implies the need for an SU(2)_R group. Thus the particle content is expanded by right-handed Z_R^0 and W_R^+- and right-handed neutrinos. The Higgs fields have to be in a triplet representation, leading to doubly-charged Higgs particles, one set for each of the two SU(2) groups. Also the number of neutral and singly-charged Higgs states is increased relative to the Standard Model, but a search for the lowest-lying states of this kind is no different from e.g. the freedom already accorded by the MSSM Higgs scenarios.

PYTHIA implements the scenario of [Hui97].

The W_R^+- has been implemented as a simple copy of the ordinary W^+-, with the exception that it couples to right-handed neutrinos instead of the ordinary left-handed ones. Thus the standard CKM matrix is used in the quark sector, and the same vector and axial coupling strengths, leaving only the mass as free parameter. The Z_R^0 implementation (without interference with the photon or the ordinary Z^0) allows decays both to left- and right-handed neutrinos, as well as other fermions, according to one specific model ansatz. Obviously both the W_R^+- and the Z_R^0 descriptions are likely to be simplifications, but provide a starting point.

For the doubly-charged Higgs bosons, the main decay modes implemented are H_L^++ -> W_L^+ W_L^+, l_i^+ l_j^+ (i, j generation indices) and H_R^++ -> W_R^+ W_R^+, l_i^+ l_j^+.

The right-handed neutrinos can be allowed to decay further. Assuming them to have a mass below that of W_R^+-, they decay to three-body states via a virtual W_R^+-, nu_Rl -> l+- f fbar', where both lepton charges are allowed owing to the Majorana character of the neutrinos. If there is a significant mass splitting, also sequential decays nu_Rl -> l+- l'-+ nu'_Rl are allowed. Currently the decays are isotropic in phase space. If the neutrino masses are close to or above the W_R^ ones, this description has to be substituted by a sequential decay via a real W_R^ (not implemented, but actually simpler to do than the one here).

Production processes

A few different production processes have been implemented, which normally would not overlap and therefore could be run together.

flag  LeftRightSymmmetry:all   (default = off)
Common switch for the group of implemented processes within a left-right-symmetric scenario.

flag  LeftRightSymmmetry:ffbar2ZR   (default = off)
Scatterings f fbar -> Z_R^0. Code 3101.

flag  LeftRightSymmmetry:ffbar2WR   (default = off)
Scatterings W_R^+. Code 3102.

flag  LeftRightSymmmetry:ll2HL   (default = off)
Scatterings l_i l_j -> H_L^--. Code 3121.

flag  LeftRightSymmmetry:lgm2HLe   (default = off)
Scatterings l_i gamma -> H_L^-- e^+. Code 3122.

flag  LeftRightSymmmetry:lgm2HLmu   (default = off)
Scatterings l_i gamma -> H_L^-- mu^+. Code 3123.

flag  LeftRightSymmmetry:lgm2HLtau   (default = off)
Scatterings l_i gamma -> H_L^-- tau^+. Code 3124.

flag  LeftRightSymmmetry:ff2HLff   (default = off)
Scatterings f_1 f_2 -> H_L^-- f_3 f_4 via WW fusion. Code 3125.

flag  LeftRightSymmmetry:ffbar2HLHL   (default = off)
Scatterings f fbar -> H_L^++ H_L^--. Code 3126.

flag  LeftRightSymmmetry:ll2HR   (default = off)
Scatterings l_i l_j -> H_R^--. Code 3141.

flag  LeftRightSymmmetry:lgm2HRe   (default = off)
Scatterings l_i gamma -> H_R^-- e^+. Code 3142.

flag  LeftRightSymmmetry:lgm2HRmu   (default = off)
Scatterings l_i gamma -> H_R^-- mu^+. Code 3143.

flag  LeftRightSymmmetry:lgm2HRtau   (default = off)
Scatterings l_i gamma -> H_R^-- tau^+. Code 3144.

flag  LeftRightSymmmetry:ff2HRff   (default = off)
Scatterings f_1 f_2 -> H_R^-- f_3 f_4 via WW fusion. Code 3145.

flag  LeftRightSymmmetry:ffbar2HRHR   (default = off)
Scatterings f fbar -> H_R^++ H_L^--. Code 3146.

Parameters

The basic couplings of the model are

parm  LeftRightSymmmetry:gL   (default = 0.64; minimum = 0.0)
lefthanded coupling g_L = e / sin(theta).

parm  LeftRightSymmmetry:gR   (default = 0.64; minimum = 0.0)
righthanded coupling g_R, assumed the same as g_L.

parm  LeftRightSymmmetry:vL   (default = 5.; minimum = 0.0)
vacuum expectation value v_L (in GeV) for the left-triplet.

The corresponding vacuum expectation value v_R is assumed given by v_R = sqrt(2) M_WR / g_R and is not stored explicitly.

The Yukawa couplings of a lepton pair to a H^--, assumed the same for H_L^-- and H_R^--, is described by a symmetric 3-by-3 matrix. The default matrix is dominated by the diagonal elements and especially by the tau tau one.

parm  LeftRightSymmmetry:coupHee   (default = 0.1; minimum = 0.0)
Yukawa coupling for H^-- -> e- e-.

parm  LeftRightSymmmetry:coupHmue   (default = 0.01; minimum = 0.0)
Yukawa coupling for H^-- -> mu- e-.

parm  LeftRightSymmmetry:coupHmumu   (default = 0.1; minimum = 0.0)
Yukawa coupling for H^-- -> mu- mu-.

parm  LeftRightSymmmetry:coupHtaue   (default = 0.01; minimum = 0.0)
Yukawa coupling for H^-- -> tau- e-.

parm  LeftRightSymmmetry:coupHtaumu   (default = 0.01; minimum = 0.0)
Yukawa coupling for H^-- -> tau- mu-.

parm  LeftRightSymmmetry:coupHtautau   (default = 0.3; minimum = 0.0)
Yukawa coupling for H^-- -> tau- tau-. pythia8-8.1.80.orig/htmldoc/ProcessSelection.html0000644000175000017500000001337712217615311020147 0ustar sunsun Process Selection

Process Selection

There is no way PYTHIA could contain all processes of interest, neither in terms of potential physics topics nor in terms of high-multiplicity final states. What exists is a reasonably complete setup of all 2 -> 1 and 2 -> 2 processes within the Standard Model, plus some examples of processes beyond that, again for low multiplicities. Combined with the PYTHIA parton showers, this should be enough to get a flying start in the study of many physics scenarios. Other processes could be fed in via the Les Houches Accord or be implemented as a Semi-Internal Process. In the latter case the existing processes would act as obvious templates.

By default all processes are switched off. You should switch on those you want to simulate. This may be done at two (occasionally three) levels, either for each individual process or for a group of processes. That is, a process is going to be generated either if its own flag or its group flag is on. There is no built-in construction to switch on a group and then switch off a few of its members.

Each process is assigned an integer code. This code is not used in the internal administration of events (so having the same code for two completely different processes would not be a problem), but only intended to allow a simpler user separation of different processes. Also the process name is available, as a string.

To ease navigation, the list of processes has been split into several separate pages, by main topic. The classification is hopefully intuitive, but by no means unambiguous. For instance, essentially all processes involve QCD, so the "QCD processes" are the ones that only involve QCD. (And also that is not completely true, once one includes all that may happen in multiparton interactions.) On these separate pages also appear the settings that are completely local to that particular process class, but not the ones that have a broader usage.

QCD Processes

QCD processes fall in two main categories: soft and hard. The soft ones contain elastic, diffractive and "minimum-bias" events, together covering the total cross section. Hard processes are the normal 2 -> 2 ones, including charm and bottom production.
Reserved code range: 101 - 199.

Electroweak Processes

Prompt-photon, gamma^*/Z^0 and W^+- production, plus a few processes with t-channel boson exchange.
Reserved code range: 201 - 299.

Onia Processes

Colour singlet and octet production of charmonium and bottomonium.
Reserved code range: 401 - 499 for charmonium and 501 - 599 for bottomonium.

Top Processes

Top production, singly or doubly.
Reserved code range: 601 - 699.

Fourth-Generation Processes

Production of hypothetical fourth-generation fermions.
Reserved code range: 801 - 899.

Higgs Processes

Higgs production, within or beyond the Standard Model. See section on Left-Right-Symmetry processes for doubly charged Higgs bosons.
Reserved code range: 901 - 999 for a Standard Model Higgs and 1001 - 1199 for MSSM Higgs bosons.

SUSY Processes

Production of supersymmetric particles, currently barely begun.
Reserved code range: 1001 - 2999. (Whereof 1001 - 1199 for Higgs bosons; see above.)

New-Gauge-Boson Processes

Production of new gauge bosons such as Z' and W'.
Reserved code range: 3001 - 3099.

Left-Right-Symmetry Processes

Production of righthanded Z_R and W_R bosons and of doubly charged Higgs bosons.
Reserved code range: 3101 - 3199.

Leptoquark Processes

Production of a simple scalar leptoquark state.
Reserved code range: 3201 - 3299.

Compositeness Processes

Production of excited fermion states and contact-interaction modification to interactions between fermions (excluding technicolor; see below).
Reserved code range: 4001 - 4099.

Technicolor Processes

Production of technicolor particles and modifications of QCD processes by technicolor interactions. Does not exist yet.
Reserved code range: 4101 - 4199.

Hidden Valley Processes

A scenario for the pair production of new particles with couplings under a new gauge group, with invisible gauge bosons. Radiation of these gauge bosons is included in the standard final-state parton shower.
Reserved code range: 4901 - 4999.

Extra-Dimensional Processes

A vast area, here represented by the production of a Randall-Sundrum excited graviton state and a Kaluza-Klein gluon, a Kaluza-Klein tower of gamma/Z^0 excitations in one TeV^- sized extra dimension, several Large Extra Dimension processes, and a few related Unparticle processes.
Reserved code range: 5001 - 5099. pythia8-8.1.80.orig/htmldoc/HadronLevelStandalone.html0000644000175000017500000002755112217615312021077 0ustar sunsun Hadron-Level Standalone

Hadron-Level Standalone

The Les Houches Accord allows external process-level configurations to be fed in, for subsequent parton-level and hadron-level generation to be handled internally by PYTHIA. There is no correspondingly standardized interface if you have external events that have also been generated through the parton-level stage, so that only the hadron-level remains to be handled. A non-standard way to achieve this exists, however, and can be useful both for real applications and for various tests of the hadronization model on its own.

The key trick is to set the flag ProcessLevel:all = off. When pythia.next() is called it then does not try to generate a hard process. Since there are no beams, it is also not possible to perform the normal PartonLevel step. (It is still possible to generate final-state radiation, but this is not automatic. It would have to be done by hand, using the pythia.forceTimeShower(...) method, before pythia.next() is called.) Thus only the HadronLevel methods are called, to take the current content of the event record stored in pythia.event as a starting point for any hadronization and decays that are allowed by the normal parameters of this step. Often the input would consist solely of partons grouped into colour singlets, but also (colour-singlet) particles are allowed.

To set up all the parameters, a pythia.init() call has to be used, without any arguments. In brief, the structure of the main program therefore should be something like

  Pythia pythia;                               // Declare generator.
  Event& event = pythia.event                  // Convenient shorthand.
  pythia.readString("ProcessLevel:all = off"); // The trick!
  pythia.init();                               // Initialization.
  for (int iEvent = 0; iEvent < nEvent; ++iEvent) {
    // Insert filling of event here!
    pythia.next();                             // Do the hadron level.
  }
Of course this should be supplemented by analysis of events, error checks, and so on, as for a normal PYTHIA run. The unique aspect is how to fill the event inside the loop, before pythia.next() is called.

Input configuration

To set up a new configuration the first step is to throw away the current one, with event.reset(). This routine will also reserve the zeroth entry in the even record to represent the event as a whole.

With the event.append(...) methods a new entry is added at the bottom of the current record, i.e. the first time it is called entry number 1 is filled, and so on. The append method basically exists in four variants, either without or with history information, and with four-momentum provided either as a Vec4 four-vector or as four individual components:

  append( id, status, col, acol, p, m)
  append( id, status, col, acol, px, py, pz, e, m)
  append( id, status, mother1, mother2, daughter1, daughter2, col, acol, p, m)
  append( id, status, mother1, mother2, daughter1, daughter2, col, acol, px, py, pz, e, m)
The methods return the index at which the entry has been stored, but normally you would not use this feature.

You can find descriptions of the input variables here. The PDG particle code id and the Les Houches Accord colour col and anticolour acol tags must be set correctly. The four-momentum and mass have to be provided in units of GeV; if you omit the mass it defaults to 0.

Outgoing particles that should hadronize should be given status code 23. Often this is the only status code you need. You could e.g. also fill in incoming partons with -21 and intermediate ones with -22, if you so wish. Usually the choice of status codes is not crucial, so long as you recall that positive numbers correspond to particles that are still around, while negative numbers denote ones that already hadronized or decayed. However, so as not to run into contradictions with the internal PYTHIA checks (when Check:event = on), or with external formats such as HepMC, we do recommend the above codes. When pythia.next() is called the positive-status particles that hadronize/decay get the sign of the status code flipped to negative but the absolute value is retained. The new particles are added with normal PYTHIA status codes.

For normal hadronization/decays in pythia.next() the history encoded in the mother and daughter indices is not used. Therefore the first two append methods, which set all these indices vanishing, should suffice. The subsequent hadronization/decays will still be properly documented.

The exception is when you want to include junctions in your string topology, i.e. have three string pieces meet. Then you must insert in your event record the (decayed) particle that is the reason for the presence of a junction, e.g. a baryon beam remnant from which several valence quarks have been kicked out, or a neutralino that underwent a baryon-number-violating decay. This particle must have as daughters the three partons that together carry the baryon number.

The sample program in main21.cc illustrates how you can work with this facility, both for simple parton configurations and for more complicated ones with junctions.

As an alternative to setting up a topology with the methods above, a Les Houches Event File (LHEF) can also provide the configurations. Since no beams or processes are defined, only the <event>....</event> blocks need to be present, one for each event, so strictly it is not a true LHEF. You need to select Beams:frameType = 4, provide the file name in Beams:LHEF and, as above, set ProcessLevel:all = off. Needless to say, an externally linked LHAup class works as well as an LHEF, with Beams:frameType = 5.

The event information to store in the LHEF, or provide by the LHAup, is essentially the same as above. The only difference is in status codes: outgoing particles should have 1 instead of 23, and intermediate resonances 2 instead of -22. Incoming partons, if any, are -1 instead of -21.

Extensions to resonance decays

With the above scheme, pythia.next() will generate hadronization, i.e. string fragmentation and subsequent decays of normal unstable particles. It will not decay resonances, i.e. W, Z, top, Higgs, SUSY and other massive particles.

If the decay products are already provided, of course those products will be hadronized, but without any of the showers that one would expect in Z^0 -> q qbar, say. That is, the presence of a decayed resonance in the event record can be nice for documentation purposes, but otherwise it plays no role. It is possible to change this behaviour with the following flag.

flag  Standalone:allowResDec   (default = off)
If off, then resonances are stable if final-state particles, and irrelevant if intermediate particles. If on, then resonances are decayed, sequentially if necessary. After each decay step a parton shower is applied, and subsequent decay kinematics is shifted by the recoil of such branchings. If the decay chain and kinematics of the resonance is provided at input, this information is used, otherwise it is generated internally according to built-in branching ratios etc.

The input configuration has to follow the rules described above, with ProcessLevel:all = off. (Terminology not quite consistent, since resonance decays normally is part of the process-level step.) It is possible to combine several resonances, and other coloured or uncoloured particles into the same event.

Final-state radiation is applied to each step of the decay sequence by default, but can be switched off with PartonLevel:FSR = off or PartonLevel:FSRinResonances.

Repeated hadronization or decay

An alternative approach is possible with the pythia.forceHadronLevel() routine. This method does a call to the HadronLevel methods, irrespective of the value of the HadronLevel:all flag. If you hadronize externally generated events it is equivalent to a pythia.next() call with ProcessLevel:all = off.

This method truly sticks to the hadron level, and thus cannot handle resonance decays. You therefore must not mix it with the Standalone:allowResDec = on framework.

The similarity of names indicates that pythia.forceTimeShower( int iBeg, int iEnd, double pTmax, int nBranchMax = 0) is intended to belong to the same set of work-by-hand methods. Here iBeg and iEnd give the range of partons that should be allowed to shower, pTmax the maximum pT scale of emissions, and a nonzero nBranchMax a maximum number of allowed branchings. Additionally, a scale has to be set for each parton that should shower, which requires an additional final argument to the append methods above. This scale limits the maximum pT allowed for each parton, in addition to the global pTmax. When not set the scale defaults to 0, meaning no radiation for that parton.

The real application instead is for repeated hadronization of the same PYTHIA process- and parton-level event. This may for some studies help to save time, given that these two first step are more time-consuming than the hadronization one.

For repeated hadronization you should first generate an event as usual, but with HadronLevel:all = off. This event you can save in a temporary copy, e.g. Event savedEvent = pythia.event. Inside a loop you copy back with pythia.event = savedEvent, and call pythia.forceHadronLevel() to obtain a new hadronization history.

A more limited form of repetition is if you want to decay a given kind of particle repeatedly, without having to generate the rest of the event anew. This could be the case e.g. in B physics applications. Then you can use the pythia.moreDecays() method, which decays all particles in the event record that have not been decayed but should have been done so. The pythia.particleData.mayDecay( id, false/true) method may be used to switch off/on the decays of a particle species id, so that it is not decayed in the pythia.next() call but only inside a loop over a number of tries.

Between each loop the newly produced decay products must be removed and the decayed particle status restored to undecayed. The former is simple, since the new products are appended to the end of the event record: event.saveSize() saves the initial size of the event record, and event.restoreSize() can later be used repeatedly to restore this original size, which means that the new particles at the end are thrown away. The latter is more complicated, and requires the user to identify the positions of all particles of the species and restore a positive status code with event[i].statusPos().

The main15.cc program illustrates both these methods, i.e. either repeated hadronization or repeated decay of PYTHIA events. pythia8-8.1.80.orig/htmldoc/CKKWLMerging.html0000644000175000017500000016341112217615312017043 0ustar sunsun CKKW-L Merging

CKKW-L Merging

CKKW-L merging [Lon01] allows for a consistent merging of parton showers with matrix elements to include multiple well-separated partons. The algorithm implemented in PYTHIA is described in [Lon11]. To perform matrix element merging, the user has to supply LHE files [Alw07] for the hard process and the corresponding process with up to N additional jets.

The usage of the merging procedure is illustrated in a few example main programs (main81.cc, main82.cc, main83.cc, main84.cc and main85.cc, together with the input files main81.cmnd, main82.cmnd, main84.cmnd and main85.cmnd). These examples should of course only serve as an illustration, and as such will not make use of the merging in all possible ways. For full generality, the example programs link to LHAPDF, FastJet and HepMC. Of course the user is welcome to remove these dependencies. To remove the FastJet dependence, the functions calculating example observables have to be deleted. Removing the LHAPDF dependence requires changing the cmnd input files to choose an inbuilt PDF, as outlined in the PDF documentation. The HepMC dependence can be removed by erasing the code allowing for HepMC output.

Please note that a detailed tutorial on merging in Pythia is available from http://home.thep.lu.se/~torbjorn/pythia8/mergingworksheet8160.pdf.

Three very short LHE files (w+_production_lhc_0.lhe, w+_production_lhc_1.lhe, w+_production_lhc_2.lhe) are included in the distribution. These files are not intended for physics studies, but only serve as input for the example main programs. For realistic studies, the user has to supply LHE files.

In the generation of LHE files, the value of the factorisation scale used in the PDFs is not important, since the cross section will be multiplied by ratios of PDFs to adjust to the PYTHIA starting scales. The same is true for the renormalisation scale (and starting value αs(MZ)) used to evaluate αs. Coupling and scale choices by the user will be transferred to the merging routines.

Multi-jet events can suffer from infrared divergences in the calculation. Sensible matrix element generator (MEG) outputs should not contain phase space points in which the calculation is ill-defined, meaning infrared regions need to be removed by cuts. This is most conveniently done by disallowing the MEG to produce partons below a minimal parton-parton separation in a certain jet algorithm. Using dedicated cuts to regularise MEG output is of course possible as well. Any regularisation criterion defines the matrix element region: The parts of phase space in which the fixed order calculation is considered valid and preferable to the parton shower. Matrix element merging is combining MEG events in the matrix element region with parton shower events in regions outside the regularisation cut (often called parton shower region). Because the regularisation cut defines a boundary between the matrix element and parton shower regions, i.e. the regions to be merged into one inclusive sample, it is usually called merging scale . Since many different cut choices may regularise the MEG calculation, many different merging scale definitions are possible. A few standard choices are listed below, as well as documentation on how to use a user-defined cut criterion. In combining matrix element and parton shower regions, the CKKW-L prescription tries to minimise the dependence on the merging scale. This can only be achieved if the combination of MEG events and parton shower populates the whole phase space. Additional cuts on the partons in the LHEF generation should hence be avoided as much as possible, meaning that the merging scale cut should always pose a more stringent cut than all other cuts on the partons. Of course, if the hard process itself is divergent, cuts need to be made. However, this should be chosen in such a way as to not exclude regions that will be available to the matrix elements with additional jets. An example is QCD di-jet production with additional jets: Say the 2 -> 2 process is regularised with a pTmin cut of pTminCut = 100 GeV, and the 2 - >3 sample is regularised with a kTmin-cut of kTminCut = 50 GeV. This would mean that when reclustering the emission in the 2 -> 3 sample, we could end up with a pT value pTminNow of the 2 -> 2 configuration with pTminCut > pTminNow, which is excluded in the 2 -> 2 sample. Thus, the 2 -> 3 sample will include a Sudakov factor not included in the 2 -> 2 sample, resulting in merging scale dependencies. Such dependencies can be avoided if the additional cuts on the hard process are minimal.

Of course, additional cuts on electroweak particles are allowed. These should be the same for all samples with 0 <= n <= N additional partons.

If it is not possible to generate LHE files with minimal cuts, the user can choose to use the MergingHooks structures in order to decide how much influence to attribute to parton shower histories in which the reclustered lowest multiplicity process does not pass the matrix element cuts. This is described below.

When generating LHE files, we advise against putting unstable particles (e.g. massive gauge bosons) in the final state. Rather, specify a resonance by its decay products, e.g. if Les Houches events for the pp → Z + jets → e+e- + jets process are desired, generate the matrix element events with the Z decay included. From a physical point of view, on-shell final massive gauge bosons should not be considered part of a hard process, since only the boson decay products will be detectable. Furthermore, non-narrow-width approximation contributions are not present if the ME generator only produces on-shell bosons. Interference effects between different production channels for the decay products would also be neglected. These points seem an unnecessary restriction on the accuracy of the ME calculation. In addition, there is a technical reason for this strategy. Since some matrix element generators choose to put additional information on intermediate bosons into Les Houches events, depending on if they pass a certain criterion (e.g. being close to the mass shell), without exact knowledge of this criterion, the only feasible way of bookkeeping the hard process is by identifying outgoing decay products.

Despite these considerations, (massive) gauge bosons in the final state are allowed in the hard process definition. This is useful particularly for Higgs physics, when different decays of the Higgs boson need to be simulated after the LHEF generation.

For all merging purposes, processes with different charge of outgoing leptons are considered different processes. That means e.g. that e+νe+ jets and e-ν̄e + jets are considered independent processes. If the user wishes to generate distributions including effects of more than one process, merged samples for all independent processes should be generated separately and added afterwards. Alternatively, to combine simple processes, combined LHE files can be used in conjunction with flexible containers (see below).

When the matrix element merging is used to produce HepMC [Dob01] files to be analysed with RIVET [Buc10], special care needs to taken in how the cross section is read by RIVET (see below).

To specify the merging conditions, additionally information on the merging scale value and the functional definition of the merging scale is needed. A few standard definitions of merging scales are available. We hope this makes the user interface less cumbersome.

Different choices intrinsic to the CKKW-L merging procedure might be relevant for the user as well. The base class MergingHooks gives the user the opportunity to define the functional form of the merging scale. In the following, the usage of the merging machinery to consistently include LHE files with additional jets into PYTHIA will be discussed.


Merging scale definitions

The quickest way to include processes with additional jets is to produce LHE files with one of the standard ways to define the merging scale. Three standard ways to define a merging scale (minimal kT, minimal evolution pT and by three cuts) are implemented. All of these prescriptions are equivalent - different definitions have only been introduced for the convenience of users, who might be limited by which cuts can be used in the generation of LHE files. Below, we describe how to switch on and use these different merging scale definitions.

Merging with merging scale defined in kT:

flag  Merging:doKTMerging   (default = off)
If the additional jets in the LHE files have been regulated by a kT cut, the user can supply the merging scale definition by setting this flag to on. kT here and below means cutting on Durham kT for e+e- collisions, and cutting on longitudinally invariant kT for hadronic collisions. Please note that this particular merging scale definition will check kT between all pairs of u,d,c,s,b,g partons.

Currently, the name longitudinally invariant kT is used for a few jet recombination algorithms with slightly different jet measures. A specific form can be chosen by setting the switch

mode  Merging:ktType   (default = 1; minimum = 1; maximum = 3)
Precise functional definition of longitudinally invariant kT. For e+e- collisions, Durham kT is always defined by the square root of min{ 2*min[ Ei2, Ej2] * [ 1 - cosθij] }, so that this switch will have no effect.
option 1 : Longitudinally invariant kT is defined by the square root of the minimum of minimal jet kinematic pT (pTkin,min2 = min{ pT,i2 } ) and pTlon,min2 = min{ min[ pT,i2, pT,j2] * [ (Δyij)2 + (Δφij)2 ] / D2 } , i.e. kT = min{ √pTkin,min2, √pTlon,min2 } for hadronic collisions. Note that the true rapidity of partons is used.
option 2 : Longitudinally invariant kT is defined by the square root of the minimum of minimal jet kinematic pT (pTkin,min2 = min{ pT,i2 } ) and pTlon,min2 = min{ min[ pT,i2, pT,j2] * [ (Δηij)2 + (Δφij)2 ] / D2 }, i.e. kT = min{ √pTkin,min2, √pTlon,min2 } for hadronic collisions. Note that the pseudorapidity of partons is used.
option 3 : Longitudinally invariant kT is defined by the square root of the minimum of minimal jet kinematic pT (pTkin,min2 = min{ pT,i2 } ) and pTlon,min2 = min{ min[ pT,i2, pT,j2] * [ cosh(Δηij) - cos(Δφij) ] / D2 } , i.e. kT = min{ √pTkin,min2 , √pTlon,min2 } for hadronic collisions.

mode  Merging:nJetMax   (default = 0; minimum = 0)
Maximal number of additional jets in the matrix element

parm  Merging:TMS   (default = 0.0)
The value of the merging scale. The name is inspired by the scale in evolution equations, which is often called 't', and the suffix 'MS' stands for merging scale. In the particular case of kT-merging, this would be the value of the kT-cut in GeV. For any merging scale definition, this input is considered the actual value of the merging scale.

word  Merging:Process   (default = void)
The string specifying the hard core process, in MG4/ME notation.

If e.g. W + jets merging should be performed, set this to pp>e+ve (without white spaces or quotation marks). This string may contain resonances in the MG/ME notation, e.g. for merging pp→Z W+→q q̄ e+νe + jets, the string pp>(z>jj)(w+>e+ve) would be applicable.

A lot more flexible hard process definitions are possible. To not dwell too much on these details here, we will come back to the process string at the end of this section.

flag  Merging:doMGMerging   (default = off)
Even easier, but highly non-general, is to perform the merging with MadGraph/MadEvent-produced LHE files, with a merging scale defined by a kT cut. For this, set this switch to on. The merging scale value will be read from the +1 jet LHE file by searching for the string ktdurham, and extracting the value from value = ktdurham. Also, the hard process will be read from the +0 jet LHE file, from the line containing the string @1 (the tag specifying the first process in the MadGraph process card). For this to work, PYTHIA should be initialised on LHE files called NameOfYourLesHouchesFile_0.lhe (+0 jet sample) and NameOfYourLesHouchesFile_1.lhe (+1 jet sample) and the same naming convention for LHE files with two or more additional jets. Since for this option, the merging scale value is read from the LHEF, no merging scale value needs to be supplied by setting Merging:TMS . Also, the hard process is read from LHEF, the input Merging::Process does not have to be defined. However, the maximal number of merged jets still has to be supplied by setting Merging:nJetMax.

Merging with merging scale defined in Pythia evolution pT:

If the LHE file has been regularised by cutting on the minimal Pythia evolution pT in the state, this can also be used as a merging scale right away. For this, change the switch

flag  Merging:doPTLundMerging   (default = off)
The merging scale is then defined by finding the minimal Pythia evolution pT between sets of radiator, emitted and recoiler partons. For this particular merging scale definition, u,d,c,s,b,g are considered partons. The Pythia evolution pT of a single three-parton set is defined by

pTevol = zijk(1-zijk) Qij2 for FSR, where i is the radiating parton, j is the emitted parton and k is the recoiler, and Qij2 = (pi + pj)2 , and zijk = xi,jk / (xi,jk + xj,ik) with xi,jk = 2 pi (pi + pj + pk) / (pi + pj + pk)2

pTevol = (1-zijk) Qij2 for ISR, where i is the radiating parton, j is the emitted parton and k is the second initial state parton, and Qij2 = -(pi - pj)2 , and zijk = (pi - pj + pk)2 / (pi + pk)2 .

When using this option, the merging scale is defined by the minimum pTevol for all combinations of three partons in the event, irrespective of flavour or colour-connections. The merging scale value will be read from the Merging:TMS parameter, so that this needs to be set just as in the case of the kT-merging prescription. Of course you will also need to set Merging:Process and the maximal number of additional matrix element jets Merging:nJetMax.

Merging with merging scale defined by a combination of cuts:

It is possible to regularise QCD divergences in a LHE file by applying cuts to the kinematical pT of jets (pTi), combined with a cut on ΔRij between jets and a cut on invariant mass Qij of jet pairs. The combination of these standard cuts can also serve as a merging scale. For this, use this setting

flag  Merging:doCutBasedMerging   (default = off)
This switch will use cuts on (pTi), ΔRij and Qij to define when parton shower emissions are allowed. Please note for this particular merging scale definition, only light jets (u,d,c,s,g) are checked.

The values of the cuts will then be read from

parm  Merging:QijMS   (default = 0.0)
The value of the invariant mass cut Qij of pairs of final state partons used in the matrix element generation.

parm  Merging:pTiMS   (default = 0.0)
The value of the minimal transverse momentum cut pTi on final state partons, as used in the matrix element generation.

parm  Merging:dRijMS   (default = 0.0)
The value of the minimal ΔRij separation between pairs of final state partons used in the matrix element generation, where ΔRij2 = (Δyij)2 + (Δφij)2.

With knowledge of these values, and Merging:doCutBasedMerging, Pythia will use these cuts as a separation between matrix element phase space and parton shower region. If e.g. the Les Houches Events have been generated with the cuts ΔRij = 0.1 , pTi= 20 GeV and Qij = 40 GeV, set Merging:QijMS=40., Merging:pTjMS=20., Merging:dRijMS=0.1 to perform a cut-based merging. Of course you will also need to set Merging:Process and the maximal number of additional matrix element jets Merging:nJetMax.

Les Houches events outside the matrix element region

Before continuing, we would like to point out that in general, the user should make sure that the events in the Les Houches file are actually calculated using the regularisation cut definition and value(s) supplied to Pythia as merging scale definition and value(s). However, if LH files with a large number of events and loose merging scale cuts are available, it might be useful to choose a higher merging scale value, e.g. for merging scale variations as part of uncertainty assessments. If CKKW-L merging is enabled, Pythia will by default check if events read from Les Houches file are in the matrix element region as defined by the merging scale definition and merging scale value. Events outside the matrix element region will be discarded. This will lead to warnings of the form "Les Houches Event fails merging scale cut. Cut by rejecting event". These warnings should, in this case, rather be regarded as information. To change the default behaviour, use the flag

flag  Merging:enforceCutOnLHE   (default = on)
This will check if the events read from LHE file are in the matrix element region as defined by the merging scale definition and value(s). If on, LHE input outside the matrix element region will be rejected. If off, every event is assumed to pass the merging scale cut.

Defining the hard process

To perform CKKW-L matrix element merging, the user has to decide on a hard process, and communicate this choice to Pythia. This is done by setting the input Merging:Process

For single processes in the Standard Model or the MSSM, MG4/ME notation is applicable. However, for some purposes, using a single simple process string is not satisfactory. Mixed W+ and W- events in a single LHE file is a common example. For this case, it would of course be perfectly allowed to perform twice, once for W+ production and once for W- production, and then add the results. Nevertheless, it seems reasonable to alleviate difficulties by allowing for less restrictive hard process definitions. Two generalisations of the process tag are available: Containers and user-defined particle tags. The syntax of these settings is described below.

In case you want multiple processes in a LHE file to be treated on equal footing (e.g. W+ + jets and W- + jets), you should use flexible containers do specify the hard process. So far, we allow the use of the containers LEPTONS, NEUTRINOS, BQUARKS. If you use these containers, the hard process definition is relatively flexible, meaning that Pythia will attempt a merging of QCD jets for each event in the LHE file, and assume that all particles matching one of the containers are products of the hard process. This is best explained by examples. If you want to have both pp → e+ νe + jets and pp → e- ν̄e + jets events in a single file, you can set Merging:Process=pp>LEPTONS,NEUTRINOS as hard process (note that for readability, you are allowed to use commata to separate container names). Combining e.g. the processes pp → e+ νe and pp → μ+ νμ is possible with the hard process definition pp>LEPTONS,NEUTRINOS.

For maximal flexibility, the definition of the hard process by these containers does not mean that each Les Houches event needs to contain particles to match each container. It is enough if one container is matched. This means that with the string pp>LEPTONS,NEUTRINOS, you can immediately process pp → e+ e- events mixed with pp → e+ νe events, since particles matching at least one container can be found in both cases. Another example for the usage of containers is mixing pp → e+ νe and pp → tt̄ → e+ νe e- ν̄e bb̄. This can be accommodated by the hard process string Merging:Process=pp>LEPTONS,NEUTRINOS,BQUARKS.

There is however a conceptual limitation to containers: The hard process definition is necessary to ensure that when constructing lower multiplicity states (that will be used to calculate the correct merging weight), the structure of the hard process will be preserved. If e.g. we want the hard process to be pp → Z → bb̄ , we should ensure that the lowest multiplicity state contains a colour-singlet bb̄-pair. When reconstructing intermediate lower multiplicity states from multi-jet matrix elements, we should thus always be able to find at least one bb̄-pair. By mixing different processes in a LHE file, this requirement might already be violated at the level of Les Houches events. Flexible containers cannot give strong conditions which flavours should be preserved in the construction of the hard process. In order to avoid non-sensible results, it is hence assumed that all particles matching any of the containers will be part of the lowest multiplicity process. This implies that if you decide to use the BQUARKS container, all b-quarks in the LHE file will be interpreted as hard process particles, and never as additional radiation.

Another way to specify the hard process particles is to explicitly define the particle names and identifiers. This is necessary if the matrix element merging in Pythia does not contain the particles of interest. To make sure that the hard process is still treated correctly, it is possible to define particles in the process string. If you e.g. want the hard process to contain a particle "zeta~" with PDG identifier "12345", produced in proton collisions, you have to include a user-defined particle tag by setting the process string to pp>{zeta~,12345}. The user-defined particle is enclosed in curly brackets, with syntax {particle_name,particle_identifier}, where "particle_name" and "particle_identifier" are the particle name and particle identifier used for this particle in the input LHE file. User-defined particles are only allowed in the final state. You are free to fix user-defined particles with more common ones, as long as user-defined particles are put before more common particles in the process string. This means that if you e.g. wanted the hard process to contain a graviton in association with a positron and an electron-neutrino, you have to define the hard process as pp>{G,39}e+ve.

Below you can find a list of particles predefined in the merging. If you wish to include a hard process with different final state particles, you may use the "curly bracket notation" outlined above.

The set of incoming particles us limited to: e- (electron), e+ (positron), mu- (muon), mu+ (antimuon), p (proton, container to hold all initial state coloured particles), p~ (identical to p container).

The following intermediate particles are allowed: a (photon), z (Z boson), w- (W- boson), w+ (W+ boson), h (scalar Higgs boson), W (container to hold both W- and W+ boson), t (top quark), t~ (anti-top), dl, dl~, ul, ul~, sl, sl~, cl, cl~, b1, b1~, t1, t1~, dr, dr~, ur, ur~, sr, sr~, cr, cr~, b2, b2~, t2, t2~ (all MSSM squarks).

We have pre-defined the outgoing particles: e+, e-, ve~, ve, mu+, mu-, vm~, vm, ta+, ta-, vt~, vt (all SM leptons and neutrinos), j~ (container to hold all final state coloured particles), j (container to hold all final state coloured particles), NEUTRINOS (container to hold all final state neutrinos and anti-neutrinos), LEPTONS (container to hold all final state leptons and anti-leptons), BQUARKS (container to hold final state b-quarks), d~, d, u~, u, s~, s, c~, c, b~, b, t~, t (all SM quarks), a, z, w-, w+ (all SM electro-weak bosons), h (scalar Higgs boson), W (container to hold both W- and W+ boson), n1 (MSSM neutralino), dl~, dl, ul~, ul, sl~, sl, cl~, cl, b1~, b1, t1~, t1, dr~, dr, ur~, ur, sr~, sr, cr~, cr, b2~, b2, t2~, t2 (all MSSM squarks). Other outgoing particles are possible if you use the "curly bracket notation" described earlier.


Histogramming the events

After the event has been processed, histograms for observables of interest need to be filled. In order to achieve good statistical accuracy for all jet multiplicities and all subprocesses contributing to one jet multiplicity, generally a fixed number of unit-weighted events is read from each Les Houches Event file. To then arrive at the correct prediction, for each of these events, histogram bins should be filled with the corresponding cross section, or weighted with unit weight and normalised at the end to the generated cross section for each jet multiplicity separately.

Still another, even more important, event weight that has to applied on an event-by-event basis is the CKKW-L-weight. This corrective weight is the main outcome of the merging procedure and includes the correct no-emission probabilities, PDF weights and αs factors. This means that the merging implementation will generate weighted events. The CKKW-L-weight can be accessed by the following function:

double Info::mergingWeight()  
Returns the CKKW-L weight for the current event.

Note that to avoid confusion, this function does not include the the weight of a phase space point (given by Info::weight()). This weight will differ from unity when reading in weighted Les Houches events. In this case, the full weight with which to fill histogram bins is Info::mergingWeight() * Info::weight().

Finally, to arrive at a correct relative normalisation of the contributions from different number of additional jets in the matrix element, each histogram should be rescaled with the accepted cross section given by Info::sigmaGen(). The accepted cross section includes the effect of vetoes generating Sudakov form factors for the matrix elements, and is in general only known after the run.

This final step can of course be skipped if the accepted cross section had been estimated before the histogramming run, and histogram bins had instead been filled with the weight Info::mergingWeight() * σest(number of additional jets in current ME sample). This is the way HepMC events should be weighted to produce correct relative weights of events (see below, and particularly examine the example programs main84.cc and main85.cc).

Examples how to use these options are given in main81.cc (kT merging), main84.cc (automatic MG/ME merging for RIVET usage), and main85.cc (HepMC output for RIVET usage).


Merging with user-defined merging scale function

For all other merging scale definitions, the procedure is slightly more complicated, since the user has to write a small piece of code defining the merging scale. To allow for a user defined procedure, set the input

flag  Merging:doUserMerging   (default = off)
General user defined merging on/off.

Then, set the Merging:nJetMax, Merging:TMS and Merging:Process input as before.

Since during execution, PYTHIA needs to evaluate the merging scale with the definition of the user, the user interface is designed in a way similar to the UserHooks strategy. The class controlling the merging scale definition is called MergingHooks.

Initialisation

To initialise the merging with user-defined merging scale, we should construct a class derived from MergingHooks, with a constructor and destructor

MergingHooks::MergingHooks()  

virtual MergingHooks::~MergingHooks()  
The constructor and destructor do not need to do anything.

For the class to be called during execution, a pointer to an object of the class should be handed in with the
Pythia::setMergingHooksPtr( MergingHooks*) method. An examples of this procedure are given in main82.cc.

Defining a merging scale

Then, in the spirit of the UserHooks class, the user needs to supply the process to be merged by defining a methods to evaluate the merging scale variable.

virtual double MergingHooks::tmsDefinition(const Event& event)  
This method will have to calculate the value of the merging scale defined in some variable from the input event record. An example of such a function is given in main82.cc.

The base class MergingHooks contains many functions giving information on the hard process, to make the definition of the merging scale as easy as possible:

int MergingHooks::nMaxJets()  
Return the maximum number of additional jets to be merged.

int MergingHooks::nHardOutPartons()  
Returns the number of outgoing partons in the hard core process.

int MergingHooks::nHardOutLeptons()  
Returns the number of outgoing leptons in the hard core process.

int MergingHooks::nHardInPartons()  
Returns the number of incoming partons in the hard core process.

int MergingHooks::nHardInLeptons()  
Returns the number of incoming leptons in the hard core process.

int MergingHooks::nResInCurrent()  
The number of resonances in the hard process reconstructed from the current event. If e.g. the ME configuration was pp -> (w+->e+ve)(z -> mu+mu-)jj, and the ME generator put both intermediate bosons into the LHE file, this will return 2.

double MergingHooks::tms()  
Returns the value used as the merging scale.

Filling output histograms for the event then proceeds along the lines described above in "Histogramming the events".

The full procedure is outlined in main82.cc. Special care needs to be taken when the output is stored in the form of HepMC files for RIVET usage.

Defining a cut on lowest jet multiplicity events

It can sometimes happen that when generating LHE files, a fairly restrictive cut has been used when generating the lowest multiplicity matrix element configurations. Then, it can happen that states that are (in the generation of a parton shower history) constructed by reclustering from higher multiplicity configurations, do not pass this matrix element cut.

Consider as an example pure QCD dijet merging, when up to one additional jet should be merged. Three-jet matrix element configurations for which the reclustered two-jet state does not pass the cuts applied to the two-jet matrix element would never have been produced by showering the two-jet matrix element. This means that the three-jet matrix element includes regions of phase space that would never have been populated by the parton shower. Thus, since the matrix element phase space is larger than the shower phase space, merging scale dependencies are expected. A priori, this is not troublesome, since the aim of matrix element merging is to include regions of phase space outside the range of the parton shower approximation into the shower. An example is the inclusion of configurations with only unordered histories.

Clearly, if the parton shower phase space is very constrained by applying stringent cuts to the two-jet matrix element, merging scale dependencies can become sizable, as was e.g. seen in [Lon11] when forcing shower emissions to be ordered both in the evolution variable and in rapidity. To influence the effect of large phase space differences for shower emissions and matrix element configurations due to LHEF generation cuts, the user has to write a small piece of code overwriting method

virtual double MergingHooks::dampenIfFailCuts(const Event&event)  
multiplicity reclustered state as an input Event. From this input event, the user can then check if matrix element cuts are fulfilled. The return value will be internally multiplied to the CKKW-L weight of the current event. Thus, if the user wishes to suppress contributions not passing particular cuts, a number smaller than unity can be returned.

Note that this method gives the user access to the lowest multiplicity state, which ( e.g. in the case of incomplete histories) does not have to be a 2 → 2 configuration. Also, changing the weight of the current event by hand is of course a major intervention in the algorithm, and should be considered very carefully. Generally, if this facility would have to be used extensively, it is certainly preferable to be less restrictive when applying additional, non-merging-scale-related cuts to the matrix element.

An example how to force a cut on lowest multiplicity reclustered states for pure QCD matrix element configurations is given by main83.cc (to be used with e.g. main82.cmnd).

Influencing the construction of all possible histories

Even more powerful - and dangerous - is influencing the construction of histories directly. This should only be attempted by expert users. If you believe manipulations completely unavoidable, we advise you to take great care when redefining the following functions.

virtual bool MergingHooks::canCutOnRecState()  
In the base class this method returns false. If you redefine it to return true then the method doCutOnRecState(...) will be called for each reclustered state encountered in the generation of all possible histories of the matrix element state.

virtual bool MergingHooks::doCutOnRecState(const Event&event)  
This routine will be supplied internally with every possible reclustered event that can be reached by reclustering any number of partons in the matrix element input state. The new, reclustered, states can then be analysed. If the method returns false, the history to which the state belongs will be treated as if it were unordered, i.e. this path will only be chosen if no other histories are available. In this way, the number of histories not fulfilling the user criterion will be minimised.

Clearly, these methods are highly intrusive. It could e.g. happen that no history is allowed, which would make merging impossible. One example where this method could be useful is if cuts on the core 2 -> 2 processes have to be checked, and the method MergingHooks::dampenIfFailCuts(const Event& event) is not sufficiently effective.

Defining the hard process matrix element

The MergingHooks class also allows the expert user to define the matrix element of the hard process, by defining the method

virtual double MergingHooks::hardProcessME(const Event&inEvent)  
This routine will be supplied internally with the reconstructed lowest-multiplicity event. From this, it is possible to calculate the squared matrix element of the hard process, by using the information stored in the event record. The function should return a double value that corresponds to the matrix element at the phase space point given by the input event record. This number will then be multiplied to the product of splitting functions that define the probability of the current path of the parton shower history. In this way, the hard process configuration can be taken into account when choosing the parton shower history, which is, internally, used to generate the "merging weight".

The inclusion of the hard process matrix element into the choice of histories becomes relevant when the hard process matrix element has very strong phase space dependencies. QCD dijet cross sections for example strongly depend on the transverse momentum of the jets. So far, the authors have not encountered any changes upon inclusion of the full hard process matrix element, even for the QCD dijet case.


Matrix element merging and HepMC output for RIVET

Examples how to produce matrix element merged events to be analysed with RIVET are given by main84.cc and main85.cc.

The main issue is that the output of separate RIVET runs can not in general be combined. To perform a matrix element merging, we however need to runs over different LHE files. The solution to this problem (so far) is to only perform one RIVET run for all matrix elements, i.e. print the events for all ME parton multiplicities, with the correct weights, to a single HepMC file. Since the correct weight includes the cross section of the different samples after Sudakov vetoes --- which is not a priori known --- the cross sections have to be estimated in a test run, before the actual production run is performed. Finally, the cross section of the last event in the HepMC file has to be taken as the full merged cross section sigma_merge = Sum_{i=0}^N Sum_{j=0}*^{nEvents} sigma_est(i)*wckkwl(j).

This procedure is outlined in main84.cc. Input LHE files with only very inclusive cuts pose further difficulties. For such files (which were already addressed under the heading Les Houches events outside the matrix element region), the cross section after the merging scale cut is not known before the cut is performed. Using Pythia's UserHooks facilities, it is possible to produce a valid estimate of the cross section after cuts. This however entails a careful cut definition by the user, which might become cumbersome for some in-built merging scale definitions. A reasonable alternative is using the switch

flag  Merging:doXSectionEstimate   (default = off)
If on, estimate cross section after merging scale cut. This switch has to be used in conjunction with a merging scale definition (e.g. Merging:doPTLundMerging = on). Then, this merging scale definition will be used as a cut on the input events. After the requested number of Monte Carlo events, the cross section after the cut can be extracted by inferring the Info::sigmaGen() method, and the number of accepted events by using Info::nAccepted()

This switch also relies on knowledge on how many partons a LHE file should contain. This is important for real-emission kinematics in the case of NLO merging. The number of (additional) partons in a LHE file can be set with

mode  Merging:nRequested   (default = -1; minimum = -1)
Exact number of additional jets requested for a particular LHE file. If a file should for example only contain W+ g g events, this switch should be set to "2" for this LHE file. For NLO merging schemes (see NLO Merging), this number has to be set.

The usage of these switches to obtain the necessary cross section estimate is illustrated in main85.cc. The example main85.cc program is intended as a "front-end" for CKKW-L merging in Pythia8, so we will discuss the program briefly. main85.cc should be used together with an input file (like main85.cmnd). The executable should be invoked with three arguments: the input file, the "name" of the input LHE files, and the name of the output HepMC event file. To use the LHE files that are shipped with the Pythia distribution, a valid usage would be

./main85.exe ./main85.cmnd ./w_production ./myhepmc.hepmc

If you want to use other input LHE files, note that main85.cc assumes the naming convention name_tree_#nAdditionalJets.lhe. All settings can be included though the input file, so that main85.cc does not have to be changed explicitly. main85.cc first switches off showers, multiparton interactions and hadronisation, and estimates the cross sections (after enforcing the merging scale cut) of samples for different numbers of additional jets. Then, showers, MPI and hadronisation are switched on again, and the CKKW-L merging procedure is performed. Events will be read in a decreasing sequence of jet multiplicities, which also means that e.g. events with two additional partons in the LHE file will be printed to the HepMC file before events with one additional parton.


Further variables

For more advanced manipulations of the merging machinery, all parameter changes that were investigated in [Lon11] are supplied. Please check [Lon11] for a detailed discussion of the switches.

These switches allow enthusiastic users to perform a systematic assessment of the merging prescription. Apart from this, we advise the non-expert user to keep the default values.

mode  Merging:nQuarksMerge   (default = 5; minimum = 2; maximum = 5)
This switch controls which quarks flavours (labelled by PDG id's) are considered additional partons. If e.g. set to 4, then u-, d-, c- and s-quarks will be merged, while b-quarks will not be considered in the merging (corresponding to a 4-flavour merging scheme). We advise caution when changing this number. In particular, please ensure that the allowed flavour for additional partons in the input LHE file does not exceed this value, since unnecessary double-counting might occur otherwise.

flag  Merging:includeMassive   (default = on)
If on, use the correct massive evolution variable and massive splitting kernels in the reconstruction and picking of parton shower histories of the matrix element. If off, reconstruct evolution scales, kinematics and splitting kernels as if all partons were massless.

flag  Merging:enforceStrongOrdering   (default = off)
If on, preferably pick parton shower histories of the matrix element which have strongly ordered consecutive splittings, i.e. paths in which consecutive reclustered evolution scales are separated by a user-defined factor.

parm  Merging:scaleSeparationFactor   (default = 1.0; minimum = 1.0; maximum = 10.0)
The factor by which scales should differ to be classified as strongly ordered.

flag  Merging:orderInRapidity   (default = off)
If on, preferably pick parton shower histories of the matrix element with consecutive splittings ordered in rapidity and pT.

flag  Merging:pickByFullP   (default = on)
If on, pick parton shower histories of the matrix element by the full shower splitting kernels, including potential ME corrections and Jacobians from joined evolution measures.

flag  Merging:pickByPoPT2   (default = off)
If on, pick parton shower histories of the matrix element by the shower splitting kernels divided by the evolution pT.

flag  Merging:pickBySumPT   (default = off)
If on, exclusively pick parton shower histories of the matrix element for which have the smallest sum of scalar evolution pT for consecutive splittings has been calculated.

flag  Merging:includeRedundant   (default = off)
If on, then also include PDF ratios and αs factors in the splitting probabilities used for picking a parton shower history of the matrix element, when picking histories by the full shower splitting probability. As argued in [Lon11], this should not be done since a reweighting with PDF ratios and αs factors will be performed. However, it can give useful insight in how sensitive the results are to the prescription on how to choose PS histories.

parm  Merging:nonJoinedNorm   (default = 1.0; minimum = 0.0; maximum = 10.0)
Normalisation factor with which to multiply splitting probability for splittings without joined evolution equation.

parm  Merging:fsrInRecNorm   (default = 1.0; minimum = 0.0; maximum = 10.0)
Normalisation factor with which to multiply splitting probability for final state splittings with an initial state recoiler.

parm  Merging:aCollFSR   (default = 1.0; minimum = 0.0; maximum = 10.0)
Factor with which to multiply the scalar pT of a final state splitting, when choosing the history by the smallest sum of scalar pT. Default value taken from Herwig++ [Tul09].

parm  Merging:aCollISR   (default = 0.9; minimum = 0.0; maximum = 10.0)
Factor with which to multiply the scalar pT of an initial state splitting, when choosing the history by the smallest sum of scalar pT. Default value taken from Herwig++ [Tul09].

mode  Merging:unorderedScalePrescrip   (default = 0; minimum = 0; maximum = 1)
When the parton shower history of the matrix element contains a sequence of splittings which are not ordered in evolution pT (called an unordered history), this sequence is interpreted as a combined emission. Then, a decision on which starting scale for trial emissions off reconstructed states in this sequence of unordered splittings has to be made. Two options are available:
option 0 : Use larger of the two reconstructed (unordered) scales as starting scale.
option 1 : Use smaller of the two reconstructed (unordered) scales as starting scale.

mode  Merging:unorderedASscalePrescrip   (default = 1; minimum = 0; maximum = 1)
Prescription which scale to use to evaluate αs weight for splittings in a sequence of splittings which are not ordered in evolution pT.
option 0 : Use the combined splitting scale as argument in αs, for both splittings.
option 1 : Use the true reconstructed scale as as argument in αs, for each splitting separately.

mode  Merging:unorderedPDFscalePrescrip   (default = 0; minimum = 0; maximum = 1)
Prescription which scale to use to evaluate ratios of parton distributions for splittings in a sequence of splittings which are not ordered in evolution pT.
option 0 : Use the combined splitting scale as argument in PDF ratios, for both splittings.
option 1 : Use the true reconstructed scale as argument in PDF ratios, for each splitting separately.

mode  Merging:incompleteScalePrescrip   (default = 0; minimum = 0; maximum = 2)
When no complete parton shower history (i.e. starting from a 2 → 2 process) for a matrix element with additional jets can be found, such a configuration is said to have an incomplete history. Since in incomplete histories, not all shower starting scales are determined by clusterings, a prescription for setting the starting scale of trial showers in incomplete histories is needed. Three options are provided.
option 0 : Use factorisation scale as shower starting scale for incomplete histories.
option 1 : Use sHat as shower starting scale for incomplete histories.
option 2 : Use s as shower starting scale for incomplete histories.

flag  Merging:allowColourShuffling   (default = off)
If on, this will allow the algorithm to swap one colour index in the state, when trying to find all possible clusterings, if no clustering has been found, but more clusterings had been requested. In this way, some incomplete histories can be avoided. Generally, we advise the non-expert user to not touch this switch, because a slight change in the colour structure can change the radiation pattern. To however study the sensitivity of the predictions on these effects, allowing for colour reshuffling can be useful.

flag  Merging:usePythiaQRenHard   (default = on)
If on, this will allow the algorithm to use a dynamical renormalisation scale to evaluate the strong couplings of the core hard process in dijet and prompt photon events. This means that the value of αs used as coupling of the hard process in the matrix element generation will be replaced with a running coupling evaluated at the geometric mean of the squared transverse masses of the two outgoing particles, as is the default prescription in Pythia.

flag  Merging:usePythiaQFacHard   (default = on)
If on, this will allow the algorithm to use a dynamical factorisation scale to evaluate parton distributions associated with the hadronic cross section of the core hard process in dijet and prompt photon events. In the calculation of PDF ratios as part of the CKKW-L weight of an event, parton distributions that should be evaluated at the scale of the core 2 - >2 process will be evaluated using the dynamical factorisation scale Pythia would attribute to this process. This means that the hard process factorisation scale is set to the smaller of the squared transverse masses of the two outgoing particles.

flag  Merging:mayRemoveDecayProducts   (default = off)
Remove products of resonances in the hard process, in case Pythia generates decay products before merging. This makes merging possible even for an indeterminate final state, if Pythia itself has produced the decay products. The merging methods will instead be invoked on the "non-decayed" event, thus removing the limitation to only one decay channel when performing the merging. This switch is necessary e.g. for slepton pair production in association with additional QCD jets, if the input LHE file contains the resonant sleptons, and Pythia decides on a decay according to the branching fractions read from SLHA input.

flag  Merging:allowSQCDClustering   (default = off)
Allow clustering of gluon emission off squarks.

flag  Merging:allowWClustering   (default = off)
Allow clustering of W boson, if interpreted as a final state emission. This switch should not be used until electro-weak showers become available. pythia8-8.1.80.orig/htmldoc/Bibliography.html0000644000175000017500000002741212217615312017272 0ustar sunsun Bibliography

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pythia8-8.1.80.orig/htmldoc/UpdateHistory.html0000644000175000017500000035361312217615312017470 0ustar sunsun Update History

Update History

These update notes describe major updates relative to the baseline PYTHIA 8.100 version. However, they are less extensive than the corresponding update notes for PYTHIA 6. On the other hand, whereas the PYTHIA 6 manual is a static document, the PYTHIA 8 html/php pages are kept up to date for each subversion.

Important note:version 8.160 does introduce some elements of backwards incompatibility. Specifically, "multiple interactions", abbreviated MI, has been renamed "multiparton interactions", MPI. This affects many parts of the code and documentation. Also some features are deprecated, although remaining until the end of the 8.1xx version series.

Main news by version

  • 8.105: 24 February 2008
    • New option to initialize with arbitrary beam directions
      pythia.init( idA, idB, pxA, pyA, pzA, pxB, pyB, pzB)
    • Added capability to set beam energy spread and beam vertex.
      Warning: as a consequence, the old Beams group of settings has been moved to BeamRemnants, and Beams is now instead used for machine beam parameters. Therefore also some Main settings of this character have been regrouped, as follows:
      8.100 setting has been moved to
      Main:idA Beams:idA
      Main:idB Beams:idB
      Main:inCMframe (Beams:frameType)
      Main:eCM Beams:eCM
      Main:eA Beams:eA
      Main:eB Beams:eB
      Main:LHEF Beams:LHEF
    • The forceHadronLevel() method introduced for standalone hadronization.
    • main15.cc illustrated how either full hadronization or only decays of some particles can be looped over for the rest of the event retained.
    • The LHAevnt and LHAinit classes have been joined into a new LHAup one, with new options that allow the writing of a Les Houches Event File.
    • The SusyLesHouches class updated to handle SLHA version 2.
    • Updated HepMC conversion routine.
    • The static ErrorMsg class has been removed and its functionality moved into the non-static Info class, in the renamed Info file.
    • Further reduction of the use of static, with related code changes. This should allow to have several almost independent Pythia instances. Some static classes still remain, however, notably for random number generation and particle properties.
    • Limited capability to use two different Pythia instances for signal + pileup event generation, see main19.cc for an example.
    • In the Event class the = and =+ methods have been overloaded to allow the copying or appending of event records. Illustrated in main19.cc.
    • The html and php page formatting improved with cascading style sheets.
    • Several minor improvements and new options, including updated configure scripts.
  • 8.108: 1 May 2008
    • Correction in the event record, so that the beam particles in line 1 and 2 do not have any mother according to the motherList method. Previously the "system" entry in line 0 was counted as their mother, which gave rise to an unexpected extra vertex in the conversion to the HepMC format.
    • Support for HepMC version 1 is removed, to simplify the code and reflect the evolution of the field.
    • Status codes are stored in HepMC only as 1 for existing and 2 for decayed or fragmented particles (whereas previously the original PYTHIA codes were used for the latter).
    • Parton densities are stored in HepMC as xf(x,Q^2) rather than the f(x,Q^2) used in (some) previous versions.
    • The SusyLesHouches class has been updated so that reading is fully compatible with the SLHA2 standard.
    • Improved handling of the Higgs width, relevant for massive and thereby broad resonance shapes.
    • The matrix elements for neutralino pair production have now been completed and checked.
    • Ensure that alpha_strong does not blow up, by introducing a minimal scale somewhat above Lambda_3 (roughly where alpha_strong = 10).
    • New methods isValence1() and isValence2() in the Info class.
    • Protection against division by zero in calculation of decay vertex (for zero-mass gluons with zero lifetime, where there should be no displacement).
    • A new compilation option -Wshadow is introduced and code is rewritten at all places where this option gave warnings.
    • Minor library correction to allow compilation with gcc 4.3.0.
  • 8.114: 22 October 2008
    • New rescattering description operational (but still experimental) for the case that FSR is not interleaved, but saved until after MPI, ISR and beam remnants have been handled. This involves much new code in several classes.
    • A new class PartonSystems is introduced to keep track of which partons in the event record belong to which subcollision system, plus some further information on each subsystem. It takes over functionality previously found as part of the Event class, but leaves room for future growth.
    • Add optional model, wherein an increased pT0 turnoff scale for MPI and ISR is used for above-average active events, i.e. events that already have several MPI's or ISR emissions.
    • Freeze GRV 94L distribution at small Q^2 to avoid blowup.
    • The pythia.readFile(...) method can now alternatively take an istream as argument instead of a filename.
    • Minor bug correction in PartonLevel.cc; the bug could (rarely) give a segmentation fault.
  • 8.120: 10 March 2009
    • New rescattering description further developed, but not yet recommended for normal usage.
    • Include new processes for Large Extra Dimensions and Unparticles, contributed by Stefan Ask. New test program main28.cc illustrates.
    • Include further SUSY processes: neutralino-chargino and chargino-chargino pairs. The processes should be valid also in the case of non-minimal flavour violation and/or CP violation. Expanded machinery to keep track of SUSY parameters.
    • Include backwards evolution of incoming photon as part of the SpaceShower initial-state radiation description. This allows you to simulate hard collisions where one of the incoming partons is a photon. New test program main43.cc illustrates.
    • Allow separate mass and transverse momentum cuts when two hard subprocesses are generated in the same event.
    • The default value for the border between short- and long-lived particles has been changed from 1 mm to 10 mm, to better conform with LHC standards, see here. The default is still to let all unstable particles decay.
    • New ISR matrix-element correction to f -> f gamma in single W production.
    • New method Event::statusHepMC returns the status code according to the HepMC conventions agreed in February 2009. The interface to HepMC now writes out status according to this convention.
    • Add capability to link to FastJet, with expanded configure script and Makefile, and with main61.cc as new example.
    • Update of Makefile.msc, with added support for latest Visual C++ Express edition and use of regexp to check nmake version.
    • Update of LHAFortran.h and Pythia6Interface.h, to make the interface to Fortran routines work also under Windows. (Thanks to Anton Karneyeu.)
    • Updated and expanded worksheet.
    • The manual pages in the xmldoc directory, and thereby also those of the htmldoc and phpdoc directories, have been significantly updated and expanded. In particular, in many places the class of each method is explicitly shown, as well as the type of the return value and of the arguments. This upgrade is not yet completed, but already covers the more relevant sections.
    • The unary minus operator in the Vec4() returns a reference to a four-vector with all components negated, but leaves the original four-vector unchanged. Previously the four-vector itself was flipped.
    • The pPlus() and pMinus() methods of a four-vector and an event-record particle are renamed pPos() and pNeg(), respectively.
    • Include a further loop in ProcessLevel, so that a new process is generated in case of failures of a less severe nature.
    • Introduce warning message for unexpected meMode in ResonanceWidths.
    • Les Houches event reading framework has been rearranged for more flexibility. Some bugs corrected. Specifically, when scale is not set (scale = -1. in the Les Houches standard), PYTHIA did not attempt to set this scale itself, which typically lead to there not being any ISR or FSR. Now the rules for normal 1-, 2- and 3-body final states are applied, with a trivial extension of the 3-body rules for higher multiplicities.
    • Correct bug in the handling of parton densities, whereby it was not possible to switch to a new set, once a first initialization had been done.
    • Correct bugs when several Pythia::init initialization calls are made in the same run, specifically in the case that pointers to external processes have been handed in.
    • Changes in main03.cmnd and main04.cmnd so that some nonstandard options are commented out rather than active. Related comments inserted also in some other .cmnd files, but there without any change in program execution.
    • A few further minor bug fixes.
    • Update year to 2009.
  • 8.125: 16 June 2009
    • Hadronization and timelike-shower parameter default values updated according to a tune to LEP1 data by Hendrik Hoeth, using the Rivet + Professor framework.
    • Many further SUSY production processes. SLHA readin expanded to cover also masses and decay modes. Example main22.cc updated, while main33.cc now superfluous and removed.
    • Also further processes for extra dimensions.
    • Stefan Ask joins as coauthor.
    • The TimeShower::shower(...) method has gained a new argument, that forces the shower evolution to stop after a given number of branchings. A new method TimeShower::pTLastInShower() permits the last evolution pT to be read out. These extensions can be useful for matching studies.
    • New optional argument isInterleaved added to TimeShower::branch(...). Is false by default, but true when called from the parton level for interleaved evolution of several parton systems, optionally also with ISR and MPI.
    • New methods UserHooks::canSetResonanceScale() and UserHooks:scaleResonance(...) allows an optional user choice of the maximum shower scale in resonance decays.
    • A new method SpaceShower::doRestart() has been added, to help distinguish cases when a SpaceShower::branch(...) failure forces a complete restart of the evolution from ones where only the intended current branching has been vetoed.
    • When multiparton interactions are initialized, it is now possible to reduce both pT0 and pTmin if necessary to find a valid solution where sigma_jet > sigma_nondiffractive. Previously only the former would be reduced, which could lead to infinite loops if too large a pTmin was used. Thanks to Sami Kama for pointing out the problem.
    • The rescattering machinery is now essentially completed, and can be used also by others than the authors. For now, however, it can only be recommended for dedicated studies, not e.g. for generic tunes.
    • Timelike and spacelike showers, and beam remnant handling, are modified to handle rescattering partons. Specifically, a new machinery is introduced to trace the recoils from the combination of rescattering with showers and primordial kT. Can assign space- or timelike virtualities to intermediate particles to have energy and momentum conserved locally. This affects the PartonLevel, MultipartonInteractions, TimeShower, SpaceShower and BeamRemnants classes. Further details to appear in the upcoming article on rescattering. (Another change is a reversal to pre-8.114 order for non-interleaved FSR, wherein also FSR is treated before beam remnants are attached.)
    • Four new status codes introduced, as part of the rescattering description:
      45 : incoming rescattered parton, with changed kinematics owing to ISR in the mother system (cf. status 34);
      46 : incoming copy of recoiler when this is a rescattered parton (cf. status 42);
      54 : copy of a recoiler, when in the initial state of a different system from the radiator;
      55 : copy of a recoiler, when in the final state of a different system from the radiator.
    • New method Info::tooLowPTmin() can tell whether the pTmin scales for showers or multiparton interactions are too low.
    • Pion beams allowed, both pi^+, pi^- and pi^0. New machinery for the latter, where the valence flavour content is chosen to be either d dbar or u ubar for each new event. One internal pion PDF implemented, with others from LHAPDF.
    • Treatment of Pomeron-proton collisions begun.
    • Phase-space handling of hard processes and multiparton interactions slightly expanded to better allow for harder PDF's than proton ones, e.g. for Pomerons.
    • The program documentation has been expanded with an alphabetical index of all methods that are described on the webpages, see the Program Methods page. Also other sections of the documentation have been updated and expanded, including the worksheet.
    • Several list methods have been made const. For the listing of events two new methods have been added, Event::list() and Event::list(bool showScaleAndVertex, bool showMothersAndDaughters = false), that correspond to special cases of the general method.
    • A new method Pythia::LHAeventSkip(int nSkip) permits a skip-ahead of the reading of external Les Houches Events, without the necessity to generate the intervening nSkip events in full. Makes use of the new LHAup::skipEvent(int nSkip) method to perform the operations. Mainly intended for debug purposes.
    • The ClusterJet jet finder now saves the last five clustering scales. Also a minor bug fix. Thanks to Nils Lavesson for this contribution.
    • The Particle::m2() method now returns a negative number when the stored mass m is negative, as used to indicate spacelike virtualities. Also the Particle::eCalc(), Particle::mT() and Particle::mT2() methods have been modified.
    • The << method to print our a four-vector has been expanded with a fifth number, the invariant length, with a minus sign for spacelike vectors, and provided within brackets to allow a simple visual distinction.
    • New methods Rndm::dumpState(string fileName) and Rndm::readState(string fileName) allows to write or read the state of the random number generator to or from a binary file.
    • New method double GammaReal(double x) returns the value of the Gamma function for arbitrary real argument. Some cross sections for extra-dimensional processes rewritten to make use of it.
    • New example program main29.cc shows how to set up a fictitious process of a heavy system decaying to two particles or partons, with decays traced to stable particles, as relevant for astroparticle applications.
    • Main programs that illustrate the HepMC interface have been updated to use version 2.04, including units and excluding deprecated output formats.
    • The main32.cc example extended also to handle Les Houches Event Files.
    • The Makefile has been modified so that "make clean" only removes the current compilation and library files, while "make distclean" gives a more extensive reset and cleanup. Thanks to Nils Lavesson for this contribution. Some other minor Makefile corrections.
    • Several main programs that use the Main:timesToShow mode have been corrected so as not to crash if this is set to zero. Also some other cosmetics changes in main programs that do not affect the running.
    • Bug correction, in that previously a veto with user hooks was not propagated from parton showers inside resonance decays.
    • Minor bug fix in TimeShower for kinematics with unequal beam-particle masses.
    • Bug fix so that PartonLevel:MPI = off also works for minimum-bias events.
    • Minor bug fix in the impact-parameter selection of multiparton interactions. Thanks to Sami Kama for pointing it out.
    • String fragmentation for junction topology protected against numerical instability in boost.
    • Bug correction in the handling of particle decays to partons, where the scale of the partons was set before the partons had been added to some arrays, leading to indexation out of bounds. Thanks to Vladislav Burylov for discovering this bug.
    • Bug correction in the handling of particles with inhibited decay, where the decay vertex would be too far displaced, which could lead to infinite loop. Thanks to Sami Kama for debugging this.
    • Check to avoid infinite loop in matrix-element handling of two-body decays.
    • Bug correction to avoid infinite loops in Dalitz decay treatment. Some changes in the decay handling logic to allow a new try when the decay of a particle fails.
    • Minor correction, so the pointer to the Info class is set also for user-written classes derived from LHAup.
    • Correction for typo in the matrix element of the Sigma3ff2HchgchgfftWW class, for doubly charged Higgs production. Thanks to Merlin Kole for spotting it.
    • Updated colour bookkeeping in junction-antijunction annihilation avoids later problems in Pythia::check().
    • Minor updates of the Makefile.msc file to work with Visual Studio 2008. Thanks to David Bailey for these modifications.
    • Ensure that nInit in the BeamParticle class is set also for unresolved lepton beams.
    • The VetoEvolution class, derived from UserHooks, is obsolete and has been removed.
  • 8.130: 15 September 2009
    • New machinery that allows multiparton interactions inside diffractive systems. Also new optional Pomeron flux factors and Pomeron PDFs. New page on diffraction added, where further details are collected. Still not tuned, so to be used with caution.
    • Make Peter Skands' "Tune 1" parameters for ISR and MPI default. The older simpler tune is still available as an option, see Tune:pp.
    • New possible choices for a second hard process: charmonium, bottomonium, top pair and single top.
    • New code for pair production of generic colour-triplet scalar, fermion or vector. Largely written by Johan Bijnens, partly recycling existing code.
    • Add user hooks possibility to veto event after a given number of multiparton interactions.
    • Add instructions how PYTHIA 8 can be used from inside ROOT. Thanks to Andreas Morsch for providing the text and Rene Brun for a simple example.
    • The main21.cc example extended with an option for a single-particle gun.
    • Improvements and bug fixes in rescattering framework.
    • New method Hist::table(string fileName) provides a more direct way to print a two-column table of histogram contents into a file than the current Hist::table(ostream& os = cout).
    • Modify reading of external files so that a line only consisting of control characters counts as empty, the same way as a line only consisting of blanks already did. This includes carriage return, tabs and a few more, the ones represented by \n \t \v \b \r \f \a. Applies to Les Houches Event files, settings files and particle data files.
    • Fix it so that the read-in of a Les Houches Event File for the hardest process can be combined with the facility to select a specified second hard process.
    • New empty base class method LHAup::fileFound() allows the derived class LHAupLHEF to signal more clearly that a failed initialization is caused by a failure to open the desired file.
    • Check that a pointer to an LHAup object has been set in Pythia::LHAeventList() and Pythia::LHAeventSkip(...) calls.
    • Updated configure and Makefile, e.g. to build shared libraries on Mac OS X.
    • The options with a direct link to hard-process generation in PYTHIA 6 has been removed. It is hardly ever used but complicates the build structure. (Owing to its usefulness for some debug work, it was reinstated in a limited form in version 8.135. Thus main51.cc now contains the complete interface, previously in separate files, and commented-out lines in examples/Makefile suggest how PYTHIA 6 could be linked.)
    • New argument to Info::errorMsg(...) allows to show all error messages of a specific kind rather than only the first one, e.g. for initialization.
    • Correction in decay table of righthanded Majorana neutrinos. Thanks to Arnaud Ferrari and Vladimir Savinov.
    • Correction in expressions in the manual for H^+- couplings to an h^0, H^0 or A^0 and a W^+-. Thanks to Rikard Enberg.
    • Fix for accessing uninitialized memory, caused by accessing the daughters of the incoming beams before these daughters actually existed. Thanks to David Bailey and Sami Kama.
    • Uninitialized photon PDF inside the proton could give crazy results for processes with incoming photons. Thanks to Adam Davison.
    • Bug fix such that finite lifetimes can be set also for particles produced in the hard process. To exemplify, the bug affected tau leptons produced in Z^0 and W^+- decays. Thanks to Troels Petersen.
    • Bug fix in TimeShower, that beamOffset could remain uninitialized. Thanks to Sami Kama.
    • Minor correction to resonance decays: fail if the allowed mass range of a Breit-Wigner resonance is a small fraction of the total area under the resonance curve.
    • Correction when all three valence quarks were kicked out from a proton and could give false messages that beam momentum had been used up.
    • Clarify status codes needed for hadron-level standalone runs in order to avoid error messages, and modify the main21.cc example accordingly.
    • Minor corrections in the processes for extra dimensions.
    • Some other minor additions to existing facilities and minor bug fixes.
  • 8.135: 10 January 2010
    • All usage of static member methods inside Pythia8 has now been eliminated. This simplifies for you to have several simultaneous Pythia instances that are run with different conditions. The three main classes affected by this are the Settings and ParticleData databases and the Rndm random-number generator. You can no longer address the methods of these classes directly, but have to address them via the settings, particleData and rndm instances in the respective Pythia object. Also some other smaller pieces of code are affected, e.g. Standard Model and SUSY couplings (the latter in new files).
      Note 1: The documentation has been updated accordingly on these webpages, but the "A Brief Introduction to PYTHIA 8.1" still refers to the old behaviour of version 8.100.
      Note 2: the interface to the external LHAPDF library remains static, since LHAPDF is written in Fortran and thus by definition static.
      Note 3: if you want to have momentum smearing in CellJet you now need to send in a pointer to a random-number generator.
    • Ten new proton PDF sets are made available internally: MRST LO* (2007), MRST LO** (2008), MSTW 2008 LO (central member), MSTW 2008 NLO (central member), CTEQ6L, CTEQ6L1, CTEQ6.6 (NLO, central member), CT09MC1, CT09MC2, and CT09MCS, see PDF Selection. The Pomeron PDF data files have been renamed for consistency. Thanks to Tomas Kasemets for help with this [Kas10].
    • New parameters TimeShower:pTmaxFudgeMPI and SpaceShower:pTmaxFudgeMPI introduced, to give the same functionality for multiparton interactions that TimeShower:pTmaxFudge and SpaceShower:pTmaxFudge do for the hardest.
    • A few extensions of the UserHooks framework. New methods UserHooks:canVetoISREmission() and UserHooks::doVetoISREmission(...) allows the latest initial-state emission to be studied before being finalized, with the possibility to veto it. Similarly Userhooks:canVetoFSREmission() and UserHooks::doVetoFSREmission(...) can be used to veto the latest final-state emission.
    • A number of loop counters have been introduced in the Info class, that offers some further information on the progress of the event generation, for use e.g. in conjunction with the UserHooks facility.
    • The Pythia::initTunes(...) method is made public, so that it can be called before the normal call from Pythia::init(...). That way it is possible to start out from a given tune and change a few of the parameters.
    • Bug corrected in LHAFortran.h for hard-process input from Fortran commonblock. This did not work properly when the input was used in combination with a second hard process generated internally. Thanks to Mikhail Kirsanov and Roberto Chierici.
    • Insertion of missing initialization of isInit in the Settings and ParticleData constructors, and nInit for BeamParticle. Thanks to Leif Lönnblad.
    • Updated Makefile.msc for Windows users.
    • Fix of some non-optimal use of booleans, that give warnings on a Windows compiler. Thanks to Anton Karneyeu.
    • New options for the SUSY Les Houches Accord such that, by default, particle and decay data are not overwritten for known Standard Model particles (including Z^0, W^+- and t, but excluding the Higgs).
    • Bug fix in SusyLesHouches, where the reading of SLHA information embedded in an LHEF would not stop at the end of the header section.
    • Bug correction for undefined secondary widths where decay products together are heavier than the mother. Also unit default secondary width values in the DecayChannel constructor.
    • Documentation updated, including change of current year to 2010.
  • 8.140: 16 July 2010
    • Four new draft tunes available.
    • Introduction of a new scenario for production of Hidden-Valley particles, and interleaved showering in the QCD and HV sectors, see the new Hidden Valleys description. A longer physics writeup is available [Car10].
    • Implementation of 2 -> 3 phase space selection intended for QCD processes with massless partons. A new set of matching phase space cut parameters. The ten different QCD 2 -> 3 processes have been implemented making use of this new possibility, so far without a complete handling of possible colour flows, however.
    • New processes have been added for contact interactions in q q -> q q and q qbar -> q qbar scattering.
    • A process has been added for TeV^-1 Sized Extra Dimensions, which involves the electroweak KK gauge bosons, i.e. gamma_{KK}/Z_{KK}, in one TeV^-1 sized extra dimension; see main30.cc for an example. This scenario is described in [Bel10]. Thanks to Noam Hod and coworkers for contributing this code.
    • In the Randall-Sundrum extra-dimensional scenario a new option has been added where SM fields can exist in the bulk rather than only on a brane. (Still under development.) Furthermore production of a Kaluza-Klein gluon state has been added, and the main28.cc test program extended.
    • The scenario for monojets in Large Extra Dimensions has been expanded with an alternative for scalar graviton exchange instead of tensor one.
    • New parameters for maximum scale of timelike showers, TimeShower:pTmaxMatch, and the dampening of hard radiation, TimeShower:pTdampMatch and TimeShower:pTdampFudge, by analogy with corresponding ones for spacelike showers. Also new method TimeShower:limitPTmax(...) to implement alternative procedures. For dipoles stretched to the beam the new switch TimeShower:dampenBeamRecoil allows to dampen radiation close to the beam direction, with a changed default behaviour.
    • Azimuthal anisotropies from coherence arguments have been introduced for the spacelike parton showers, see SpaceShower:phiIntAsym and SpaceShower:strengthIntAsym. Also azimuthal anisotropies from gluon polarization have been introduced for the spacelike parton showers, see SpaceShower:phiPolAsym, and updated for timelike parton showers, see TimeShower:phiPolAsym.
    • Improvements for the matching to POWHEG LHEF-style input illustrated by the new main71.cc example. See also [Cor10].
    • A set of new processes gamma gamma -> f fbar, with f quarks or leptons. Code for equivalent photon flux around an unresolved proton, with more to come. Thanks to Oystein Alvestad.
    • A new option has been included to dampen the growth of the diffractive cross sections, see Total Cross Sections.
    • A new method virtual int SigmaProcess::idSChannel() has been introduced. If overloaded to return a nonzero value then a 2 -> n process will appear listed as a 2 -> 1 -> n one. That is, an intermediate resonance with the requested identity will be inserted in the event record, even without appearing in the calculation of the matrix element proper. Thanks to Noam Hod for idea and code.
    • A new method SigmaProcess::convertM2() has been introduced to optionally allow the SigmaProcess::sigmaHat() to return the squared matrix element rather than d(sigmaHat)/d(tHat) for 2 -> 2 processes. Furthermore kinematics is stored in the new mME and pME vectors for alternative cross section encodings.
    • Different encoding of the f fbar -> Z W cross section, contributed by Merlin Kole, based on the cross section of Brown, Sahdev and Mikaelian. Gives a distinctly different cross section than the previous based on EHLQ (including their bug fix). In particular the problem with negative cross sections is now fixed.
    • Minor updates: pass xmlPath to new MSTW and CTEQ PDFs; reset beams earlier to give cleaner documentation.
    • The H1 Fit B LO parametrization to the Pomeron PDF has been included, and made new default for Pomerons. Thanks to Paul Newman for providing the data files.
    • Three changes, in principle unrelated, but with the common objective to make the generation of a given event depend only on the values determined during the initialization stage and on the state of the random-number generator when the event is begun. The new default should ensure a reproducible stop-and-restart behaviour, convenient for debug purposes. Thanks to Michael Schmelling for stressing the desire for such a behaviour.
      (i) Introduction of a new option PhaseSpace:increaseMaximum that allows to switch between two strategies for handling the (hopefully rare) cases when the assumed maximum of the cross section function is exceeded during the event generation, with a changed default behaviour. In the old default the maximum could be increased if it was exceeded during the run, thereby introducing a memory of the previously generated events.
      (ii) Updated handling of random numbers with Gaussian distributions. The gauss() method now only generates one value at a time. Instead the new gauss2() method returns a pair of Gauss numbers, with related time savings. In the old approach one Gaussian number could be buffered, which introduced a memory.
      (iii) Minor bug fix in MiniStringFragmentation, where the popcorn baryon state was not reset for each new system, again giving a (flawed) memory.
    • New directory rootexample with a simple code example how to use ROOT for histogramming in PYTHIA runs. See ROOT Usage for details. Thanks to Rene Brun.
    • In the HepMCinterface the checks for unhadronized quarks and gluons are not performed if hadronization has been switched off.
    • The UserHooks::initPtr(...) has been expanded so that pointers to more classes (beam particles, random number, couplings, etc.) are sent in, thereby increasing the scope of possible user-written code. Also, the UserHooks::doVetoProcessLevel(Event& process) now allows the process event record to be modified, even if it is not recommended. The new Info::pTnow() method returns the current pT scale of the combined MPI, ISR and FSR evolution, which can be useful for some user hooks decisions.
    • Histograms of the Hist class can now be booked with up to 1000 bins, instead of the previous maximum 100. All bins can be written to file, but the line-printer style printing will join nearby bins so at most 100 are printed, as before.
    • Updated configure and Makefile to allow 64-bit compilation and more options. Thanks to Mikhail Kirsanov, Rene Brun and Fons Rademakers.
    • Bug fix in ProcessLevel for colour flow checks of junctions. Enables the decay of a neutralino to three quarks, e.g. Thanks to Nils-Erik Bomark.
    • Bug fixes in TimeShower, where recoil partners in resonance decays of coloured particles, and recoil partners in QED dipoles when beams are not allowed to take a recoil, might not be correctly identified.
    • Bug fix in SpaceShower: when used with a fixed alpha_strong, the threshold enhancement factor of g -> Q Qbar became undefined. Thanks to Stefan Prestel.
    • Bug fix in initialization of resonance widths, where the minWidth parameter could be used uninitialized, occasionally resulting in strange initialization problems when kinematics needs to force at least one resonance to be off-shell.
    • Minor updates of main06.cc, main10.cc and main23.cc.
    • Bug fix in mother pointer of multiparton interactions in diffractive systems.
  • 8.142: 15 August 2010
    • The strategy for setting up tune values has been changed. Previously the Tune:ee and Tune:pp settings were only interpreted during the Pythia::init(...) stage. Now they are interpreted as soon as they are read. Specifically this means that it is possible to override any of the tune parameters by putting new commands below Tune:ee and Tune:pp in the Pythia::readFile(...) configuration file or in the list of Pythia::readString(...) commands.
      As a consequence of this change, the public Pythia::initTunes(...) method has been replaced by two private Settings::initTuneEE(...) and Settings::initTunePP(...) methods.
      If Tune:ee or Tune:pp are nonvanishing by default, then the corresponding tune variables are set also from the Pythia constructor, before any user changes are possible. Currently this is not relevant.
    • Bug fix in the setup of the Tune:pp = 5 and = 6 options, which meant that diffractive cross sections were not reduced as advertised.
    • The default value of MultipartonInteractions:pT0Ref has been slightly reduced so as to give a somewhat improved default description. It is not intended as a replacement for the specific tunes, however.
    • Some comparisons between tunes and data, obtained with the Rivet package, have been posted on http://home.thep.lu.se/~richard/pythia81/. Further improvements can be expected from future Professor-based tunes. The current set of 2C, 2M, 3C and 3M "draft tunes" have deliberately been chosen different also to explore a range of possibilities. One not visible in the plots is the fraction of single and double diffractive events in the inelastic cross section. This is 32% in 2C and 2M, while it was reduced to 21% in 3C and 3M, and a recent ATLAS study (ATLAS-CONF-2010-048) would suggest 28+-4%.
    • Minor changes in TimeShower and SpaceShower, as protection if the c or b masses are set small.
    • Bug fix in SpaceShower, for case when phi angle selection is biased to take into account interference effects.
    • The SigmaProcess::convertM2() method now has been implemented also for 2 -> 1 processes, so that it is possible to provide the squared matrix element instead of sigmaHat for semi-internal processes. A fixed-width Breit-Wigner is also inserted, since the matrix element is supposed not to include it.
    • New method SigmaProcess::setupForME() does an extended conversion from the internal kinematics to an almost equivalent one, better adapted to the mass conventions of matrix-element calculation programs, such as massive incoming b quarks. New flags allow to determine whether the c, b, mu and tau should be considered massless or not in the calculations.
    • Two new friend methods table of the Hist class allow to print a table with three columns, the first for the (common!) x values and the other two for the respective histogram values. A new method takeSqrt for the square root of histogram bin contents.
  • 8.145: 10 November 2010
    • Couplings is defined in StandardModel.h as a derived class of coupSM and has only one extra flag: isSUSY to check presence of extra couplings.Changed all pointers CoupSM* to Couplings* and removed explicit references to CoupSUSY*. The coupSUSY object is only initialised if SUSY couplings are present. The new pointer couplingsPtr points either to only SM couplings or SM+SUSY couplings based on SLHA data.
    • New files SusyResonanceWidths.h/cc contains the SusyResonanceWidths class, which inherits from ResonanceWidths but typecasts the couplingsPtr to (CoupSUSY*) coupSUSYPtr. This is the base class for all SUSY resonances. It contains the ResonanceSquark class for all squark decays. A new flag SLHA:useDecayTable to check if internal widths should be overwritten by those read in via SLHA.
    • Added new functionality to SusyLesHouches for read-in of generic user blocks in the SLHA format, along with methods to extract parameters from them with typecasting controlled by the user. Intended for use with user-written semi-internal processes.
    • Added Sigma1qq2antisquark cross section.
    • Some new flags and modes in the SUSY and SLHA series offer further functionality.
    • Several further changes as a consequence of the upgrade of the SUSY machinery.
    • Bug/typo fixes in rotation matrices for SUSY couplings and for the processes qqbar2squarkantisquark, qq2squarksquark and more.
    • Improved handling of colour junctions. Added new example program main72.cc, to illustrate read-in of color junction structures via LHEF (main72.lhe). The example used is SUSY with RPV.
    • New Tune 4C introduced as Tune:pp = 5. The more crude (non-)tunes 3C and 3M are removed.
    • New methods Settings::getFlagMap(...), Settings::getModeMap(...), Settings::getParmMap(...) and Settings::getWordMap(...) allows to return a map of all settings of the respective type that contain a specific string in its name.
    • Improved description of excited g^*/KK-gluon^* production in the Sigma1qqbar2KKgluonStar and ResonanceKKgluon classes.
    • Possibility added to let Hidden-Valley gamma_v have a nonzero mass and decay by mixing with the ordinary photon. Still experimental.
    • Minor bug fix in handling of three-body phase space.
    • Minor correction in Sigma2ffbar2TEVffbar class.
    • Bug fix for decays of W' to a pair of heavy fermions when gV != gA. Thanks to M. Chizhov, see arXiv:0705.3944.
    • Restore the older EHLQ-based encoding of the f fbar -> Z W cross section, which was changed in version 8.140, since comparisons with Madgraph gives much better agreement with it than with the expression of Brown, Sahdev and Mikaelian.
    • The HepMCInterface now also stores colour flow information for coloured particles.
    • Pointer to Couplings made available for particle decays.
    • Minor update in main61.cc for more elegant usage of FastJet, as suggested by Gregory Soyez.
  • 8.150: 20 April 2011
    • Tune 4C is made default. It is based on first comparisons with LHC data [Cor10a], and has also been checked independently [Buc11] to give reasonable agreement with many distributions.
    • The description of tau lepton decays has been significantly enhanced, to include helicity information related to the production process and hadronic currents fitted to data. A complete writeup is in preparation, while a summary can be found in [Ilt12]. A new flag is introduced to revert to the old behaviour, for cross-checks, see Particle Decays. The new tau decay machinery is on by default.
    • A new option MultipartonInteractions:bProfile = 4 has been introduced for the impact-parameter profile of protons in the Multiparton Interactions framework, wherein low-x partons are spread over a larger area than high-x ones, see [Cor11]. A new method Info::eMPI(i) gives back the enhancement factor related to the i'th interaction. The impact-parameter profile can now be selected separately for diffraction, but without a bProfile = 4 option.
    • The possibility of "hadronization" in the Hidden Valley sector has been added as a new option HiddenValley:fragment = on. This is based on a copy of the standard string fragmentation framework, but with the option of a completely separate "flavour" sector, and separately tunable longitudinal fragmentation functions and transverse momenta. For now only a simple flavour scenario is provided, where flavour-diagonal mesons can decay back into the normal visible sector while off-diagonal ones remain hidden. A writeup of the model is in preparation [Car11]. Also some further Hidden Valley options have been added.
    • Included possibility in TimeShower for QCD dipoles to have an adjustable normalization factor, via the new bool isFlexible and double flexFactor properties of class TimeDipoleEnd. This flexibility is used to treat radiation off colour topologies with epsilon tensors, in particular colour junctions which have all their partons in the final state. (An example is the BNV-SUSY decay ~chi0→uds.) For such topologies, the new treatment in PYTHIA 8 is that a half-strength dipole is spanned between all combinations of final-state quarks. For junctions with an incoming (anti)colour line (such as in the BNV-SUSY decay ~t*→cb), a full-strength dipole is instead spanned between the two daughters, with no radiation from the decaying object (in its CM). As will be described in a forthcoming paper with N. Desai, this should give the closest possible correspondence to the radiation patterns exhibited by higher-order matrix elements for this type of process.
    • Corrected harmless bugs in ProcessLevel::findJunctions which caused junctions of types 3 and 4 (i.e., junctions with 1 incoming color tag) to sometimes be incorrectly classified as types 1 and 2 (with all color tags outgoing), respectively. Since the parity (even/odd) of the junction kind was still correct, however, this did not cause any problems at the hadronization stage.
    • The junction-finder in ProcessLevel::findJunctions has been made more stable, and the following ordering of the color tags returned by Event::endColJunction(iJun, iLeg) is now enforced: for junction kinds 3 and 4 (one tag incoming), iLeg = 0 will return the incoming tag, while for kinds 5 and 6 (two tags incoming), iLeg = 0 and iLeg = 1 will return the incoming tags. Apart from this ordering, the color tags are ordered in ascending color tag number.
    • Declarations of friend functions moved to sit outside the class it befriends. Thanks to Axel Naumann for pointing out the incorrect previous construction.
    • The rootexample subdirectory becomes rootexamples as the old example is split into two, with improved documentation to clarify usage. Thanks to Axel Naumann and Bernhard Meirose for the new code.
    • In the Les Houches Event File machinery, input type has been changed from ifstream to istream for more flexibility.
    • R-hadron handling is largely implemented, see the R-hadrons page, although some aspects still need polishing. A new class RHadrons takes care of the hadronization and decay. Particle data have been added for R-hadrons containing a gluino, stop or sbottom, but could alternatively be used for other long-lived coloured particles. Thanks to Bernhard Meirose for support.
    • Calculations of SUSY decay widths included by N. Desai, contained in the new source files SusyResonanceWidth.cc and .h. Validation and addition of more modes is still in progress, so this implementation should be considered preliminary for now. For a list of available modes, see the SUSY Processes page.
    • A first implementation of the SLHA-based QNUMBERS interface for defining new exotic particles has been included. See [Alw07] and the SUSY Les Houches Accord page.
    • Read-in of LHEF events containing Baryon Number Violating vertices has been included, using colour junctions, see the Event Record page. The advanced shower model taking into account the full colour structure of such events, developed by N. Desai and described above, is turned on by default in such events. Several test cases were used to validate this implementation, but it is possible that problems could still exist for some cases. Feedback is welcome. Thanks to the MadGraph authors for providing several test cases.
    • Some first steps taken to allow events containing colour sextets, e.g., from semi-internal processes or LHEF interfaces, and/or from SLHA DECAY tables. New colType codes 3 and -3 are introduced to describe sextets and antisextets, respectively. The state of the current implementation is that hard processes containing such states can be read in and decays generated (via DECAY tables). Parton showers can be added, but the sextets themselves do not, as yet, shower, and any undecayed sextets remaining at the hadronization stage would lead to unpredictable problems if hadronization is switched on. Thanks to J. Alwall for help with testing this implementation.
    • The functionality of the SLHA SUSY/BSM interface (see the SUSY Les Houches page) has been extended so that copies of all BLOCKs are now stored internally as strings, regardless of whether they correspond to "official" SLHA blocks or not. Their contents can subsequently be queried by a set of new templated member functions of the class SusyLesHouches. Available query functions so far include
      template <class T> bool getEntry(string, T&);,
      template <class T> bool getEntry(string, int, T&);,
      template <class T> bool getEntry(string, int, int, T&); , and
      template <class T> bool getEntry(string, int, int, int, T&);,
      where the type of the argument used in the call determines how to read the block entries. Thus, if an LHEF, SLHA, or other card file is read in by PYTHIA, the contents of any BLOCK in that file can subsequently be queried run-time using these functions. This is used, e.g., in the new interface between MADGRAPH 5 and PYTHIA 8. Thanks to the MADGRAPH team, and to J. Alwall in particular, for help and debug on this new implementation.
  • 8.153: 10 August 2011
    • The setup of tunes has been modified, see the Tunes page for details. Specifically the Tune:ee and Tune:pp modes have acquired a new option -1 for a forced restore to the default values of all settings used in the respective kind of tunes.
    • The code for handling multiparton interactions in the scenario with an x-dependent width of the Gaussian matter profile [Cor11], has been improved and updated. Tune 4Cx, which is based on this option, has been added as a further tune option.
    • A possibility to bias the phase-space selection has been added, whereby some phase space regions can be oversampled, which is compensated by assigning a weight to each event. A new set of methods have been added to the UserHooks class to allow users to program how to bias the selection.
    • New options added so that matrix-element corrections can be switched off after the first branching in ISR or FSR.
    • Some new Info methods have been added to store information on latest ISR branching. The SpaceShower class has also been corrected so that the latest z = 1/2 when not defined by history. This avoids undefined values for azimuthal asymmetries. Thanks to Stefan Prestel for finding and sorting out this problem.
    • The Pythia::forceHadronLevel() method now takes an argument that optionally means that existing junction information is not overwritten. Thanks to Leif Lönnblad for pointing out the usefulness of this.
    • For particle decays to a varying number of hadrons the multiplicity increase with mass has been somewhat reduced, and especially for meMode = 23 a separate even slower increase has been introduced.
    • New possibility to force the tau polarization.
    • Bug fix for the special case in which events containing SUSY particles are generated without proper initialization of SUSY decays. This can happen, e.g., if events containing SUSY particles are read in via external LHEF files, if those files do not contain readable SLHA spectra in their headers. In this case, a failed attempt to generate sparticle decays with ill-defined couplings previously led to crashes. The program now reverts to the old behaviour, based on static decay tables, in such cases, with the default being to decay all sparticles to gravitino + particle. An error message stating that the full SUSY treatment has been switched off and why is also issued. Thanks to N. Desai for this fix.
    • The R-hadron machinery has been completed.
    • Minor change in timelike showers: gluons which fall below the pTmin cutoff by the correction for mass effects are now eliminated, while previously they were kept. This reduces the number of gluons somewhat, but has no significant effects on the hadronic final state. (Prompted by R-hadron studies, where big mass effects else give bothersome low-energy gluons.)
    • Corrected typos in two of the Upsilon wave function matrix elements, Bottomonium:OUpsilon3P08 and Bottomonium:Ochib03P01. Thanks to Beate Heinemann for pointing it out.
    • Implemented f* decay angle in f f -> f f* processes, and fixed some bugs for the same process. Thanks to Piyali Banerjee for tests.
    • Introduce possibility to separate production channels for TeV-sized extra dimensions, and a small code correction. Thanks to Noam Hod for code contribution.
    • Bug fix for neutrino beams: since neutrinos are always lefthanded there should be a factor 2 in the cross section, relative to charged leptons, from the non-need to average over incoming spin states. This is now fixed by introducing a new PDF class NeutrinoPoint for (unresolved) neutrinos, with normalization 2 rather than 1 for charged leptons. Thanks to Ryosuke Sato.
    • Bug fix for some (rarely used) particle settings, which could not be changed by users because they were read too early. Thanks to Andrew Altheimer and Gustaaf Brooijmans.
    • Bug fix in handling of tau decays, where setting of decay vertices could write outside memory. Thanks to Steven Schramm.
    • Minor expansion of the BeamParticle constructor.
    • Minor bug fix in CTEQ 6L for uninitialized variables.
    • Minor bug fix in fragmentation flavour combination to hadron.
    • Some updates of the documentation, including new pages on MadGraph 5 as a generator for semi-internal processes (thanks to Johan Alwall) and on RIVET interfacing.
    • Minor improvements of ROOT- and HepMC-related code and documentation.
    • Some cleanup of code.
  • 8.157: 10 November 2011
      Stefan Prestel joins as new member of the PYTHIA author team. He is mainly working on matching/merging issues, and has contributed the CKKW-L machinery mentioned below.
    • Merging capabilities according to the CKKW-L scheme [Lon11] have been added, see the new Matrix Element Merging page. It involves new classes to reconstruct and select how a matrix-element-generated partonic configuration could have been obtained by the PYTHIA evolution, and to perform trial showers (using a new copy of the normal parton-level machinery) that introduce the appropriate Sudakov suppression factors. New examples to illustrate various common tasks are found in main81.cc, main82.cc, main83.cc and main84.cc.
    • The main71.cc program is now generalised for reading in arbitrary POWHEG LHE files, to implement a smooth matching between NLO matrix elements and the PYTHIA parton showers. Cuts are made on both ISR and FSR emissions, while previously only ISR was covered. The key assumptions are the pT definitions used for ISR and FSR, but several further options are available, as documented in the main71.cmnd file. Work is still ongoing to pick the best default options.
    • Several expansions of the UserHooks class. For both doVetoFSREmission and doVetoISREmission a new argument iSys labels the system within which the radiation occurs. For doVetoFSREmission a further argument inResonance distinguishes FSR in resonance decays from that in the hard process itself. New methods canVetoMPIEmission and doVetoMPIEmission have been added to veto multiparton interactions in the same way as FSR and ISR. In biasSelectionBy at times incorrect values for inEvent has been corrected. Also some systematization of the use of const.
    • A new model for hadron scattering is introduced, still at an early stage and therefore more intended for internal development than for the normal user. The basic idea is that a high-energy pp collision involves the fragmentation of multiparton strings that overlap in space (and time). Also the produced hadrons therefore initially overlap, and there is a strong likelihood that hadrons can scatter against each other until the system has expanded sufficiently. This can e.g. increase the transverse momentum of heavier hadrons at the expense of lighter ones.
    • A new jet finder SlowJet offers simple access to the inclusive kT, anti-kT, and Cambridge/Aachen algorithms in a cylindrical coordinate frame. The jet reconstruction is then based on sequential recombination with progressive removal, using the E recombination scheme. The minimalistic SlowJet code is much slower than FastJet [Cac06], and contains less options, but reconstructs the same jets if run under identical conditions. For details see the Event Analysis page.
    • Starting in gcc 4.6, it is possible to switch off specific warnings around specific blocks of code. Although version 4.6 is some way off from being commonly found, this option has now been introduced to switch off -Wshadow warnings in HepMCInterface.cc. For other compilers, or earlier versions of gcc, the old behaviour is retained.
    • Support for reading in gzipped LHEFs has been added in the LesHouches and SusyLesHouches classes. This also affects configure and Makefiles. Unless explicitly enabled, it should not affect anything. If enabled, it relies on the Boost and zlib libraries to function, so paths to these must be set appropriately, see the README file for details. The Boost header files can give very many shadow warnings, so -Wshadow is disabled if gzip support is enabled, as described above.
    • Introduce use of the HEPMC_HAS_UNITS environment variable in the HepMCInterface.cc and main32.cc codes to automatically check whether GeV and mm can be set as relevant units. If yes, then it is set in main32.cc. If no, a conversion from GeV to MeV is done explicitly in HepMCInterface.cc. Note that, for early HepMC versions, this means a change of behaviour. Thanks to Andy Buckley.
    • A new method Info::lhaStrategy() returns the Les Houches event weighting strategy where relevant, and 0 where not. For the strategies +-4 the event weight and sum, Info::weight() and Info::weightSum(), is now in units of pb at output, as it should be at input. (While internally mb is used.)
    • New flag Check:abortIfVeto allows the user to resume control over execution in case of a veto in the event generation process.
    • New method Event::at(i) returns reference to i'th particle in the event record.
    • Introduce the Fermi constant as one of the Standard Model parameters.
    • Included automatic pre-initialization of SLHA blocks MASS and SMINPUTS using PYTHIA's SM parameters and particle data table values.
    • SUSY: added sleptons (and sneutrinos) as resonances. Corrected 2-body decay widths of gluinos, squarks and gauginos. Added sleptonic decay modes to gaugino decays. Implemented 2-body decays of sleptons (and sneutrinos) into sleptons/leptons/gauginos. Corrected slepton couplings (they now look exactly like squark couplings, using a 6x6 slepton mixing matrix).
    • New parameter Diffraction:probMaxPert introduce to give more flexibility in transition from a nonperturbative to a perturbative description of a diffractive system.
    • Bug corrected in SigmaEW.cc, for the process WeakSingleBoson:ffbar2ffbar(s:gm). Previously, all outgoing quark flavours in this process were erroneously assigned ID code 5 (b quarks). This has now been corrected so the proper ratios are obtained, with u : c : d : s : b = 4 : 4 : 1 : 1 : 1, according to the squared quark charges.
    • Changes in FragmentationSystems and StringFragmentation to reject systems with three or more interconnected junctions. This may happen in baryon-number-violating scenarios in pp collisions, if both of the beam baryon junctions are resolved and get connected via an antijunction created by a hard-process BNV vertex. In principle, this could be addressed by an extension of the existing junction fragmentation framework. However, since it happens rarely, for the time being an error message is printed and the fragmentation restarted.
    • Change in Event::copy to safeguard against attempting to copy out-of-range entries. An attempt to copy a non-existing entry will now return -1.
    • Bug fix in the machinery for the user to force the setting of tau polarization.
    • Bug fix in the initial search for a maximum of the process cross section (only affecting rare cases).
    • Corrected angular decay distributions for two compositeness processes, Sigma2qq2qStarq and Sigma2qqbar2lStarlbar.
    • Extra check in HiddenValleyFragmentation to make sure that pointers which have not been assigned with new are not deleted.
    • Some further minor changes.
  • 8.160: 23 January 2012
    • The older term "multiple interactions" has been replaced by the new standard "multiparton interactions" one, and correspondingly the abbreviation MI by MPI. This affects everything: settings, class and method names, documentation, etc. It therefore becomes necessary to rewrite user code. However, so as to keep the immediate effort at a reasonable level, the old settings names are kept as aliases. Thus PartonLevel:MI and PartonLevel:MPI are equivalent, and similarly MultipleInteractions:pT0Ref and MultipartonInteractions:pT0Ref. Should you be using methods such as double Info::pTMI(int i) you need to edit the code, however. All the example/main* files have been updated accordingly.
    • A new option Beams:frameType = 5 has been added for the case where an external generator should provide LHA process information. The new Pythia::setLHAupPtr(...) method should then be used to link in this generator. The new switch Beams:newLHEFsameInit can be used to tell that a new LHEF should be used, but without the need for a new initialization. With these two changes, all the different ways of initializing can be covered by the Pythia::init() call with no arguments. The various init(...)options with arguments are deprecated and will be removed for PYTHIA 8.2.
    • The Pythia::stat() method, with no arguments, replaces Pythia::statistics(...), although the latter remains as a deprecated alternative.
    • New settings Init:..., Next:..., and Stat:... can be used to steer some details of the operation of the Pythia::init(), Pythia::next() and Pythia::stat(), respectively. In particular it affects the amount of printout at the various stages of operation. See here for further details. This change involves several code changes, but in documentation rather than physics. Most of the Main:... settings are deprecated as a consequence.
    • The sample main programs in the examples subdirectory have been updated. This includes a change to the new favoured methods and settings outlined above, plus some update of the physics contents. Some of the examples have been combined, some others have been added (e.g. for R-hadrons), and as a consequence some renumbering has been made. See the modified list of sample main programs for the new status. In particular note that (the new) main61.cc allows streamlined input and output in HepMC, like main42.cc (previously main32.cc), but additionally links to LHAPDF.
    • The examples/configure script has new optional argument --with-pythia8. It can be used to set the new PYTHIA8LOCATION environment variable, which then is used in examples/Makefile to give the path to the PYTHIA library. Thereby it becomes possible to relocate (parts of) the examples directory and still obtain the correct path. Thanks to Mikhail Kirsanov.
    • Polarization information has been included as a new Particle property, that can be set by void pol(double polIn) and obtained by double pol(). Default value is 9., in agreement with the Les Houches standard. Event listings have been expanded to optionally display this information. Currently polarization is not used internally.
    • The matrix element merging machinery has been modified as follows.
      - Improved handling of the hard process, so that MadGraph5-produced LHE files do not produce problems (sometimes, the choices of MG4 on what to put into a LHEF have changed in MG5).
      - Improved handling of colour for easier handling of states with many quarks (the code has been tested for states with up to 5 q qbar pairs and some gluons).
      - Improved checking which clusterings are allowed. Now, clusterings should immediately be rejected if they lead to unphysical states, without the need to explicitly construct these states. This was needed to get t tbar production, VBF and some simple SUSY processes running with reasonable generality.
      - Improved handling of incomplete histories. Now there is an additional switch allowing code to try to swap some colours when fewer clusterings than requested have been found.
    • Updates in the handling of graviton resonances in scenarios with extra dimensions.
      - Now all G decays have correct angular distribution, which was not the case before for W/Z decays.
      - Added the possibility for G to only couple to longitudinal W/Z bosons, which affects both the width and angular distributions.
      - Added decays to Higgs pairs, G -> hh.
    • Bug fix in the findJunctions() function in ProcessLevel.cc. Changes introduced in version 8.145 (to allow for junctions in baryon-number-violating processes) did not correctly handle the remapping of color tags that can be applied when adding beam remnants to events with multiparton interactions. A simpler and more stable algorithm is now applied for the simplest cases, with the more complex one only invoked for cases such as BNV, which are normally considered before remnants are added, hence avoiding this particular problem. Also some other changes in the handling of junction, including a safeguard to reject systems with three or more interconnected junctions.
    • Bug fix and updates to the SLHA interface. Possibility of infinite loop during ProcessLevel::initSLHA corrected. Modifications to SusyLesHouches to allow interpretation of SLHA1 spectra with R-parity violation. Rather than reject spectra that do not conform fully to the SLHA2 standard for RPV, the interface will now first look for SLHA1 mixing matrices and attempt to translate those into SLHA2 ones if possible. In this case, warnings that the expected SLHA2 blocks were not found will be printed. It is up to the user to check that the derived SLHA2 information is correct. Corresponding additions to SusyCouplings.cc to extract mixing-matrix information from the relevant SLHA2 RPV blocks when RPV is switched on.
    • Updated SLHA example main24.cmnd to use new example spectrum, cmssm.spc, corresponding to CMSSM point 10.1.1, obtained with SOFTSUSY 3.3.0. Thanks to B. Allanach for providing the new spectrum file.
    • A new include/FastJet3.h header file simplifies interfacing of FastJet to Pythia. For details see documentation in the file itself. Thanks to Gavin Salam for this contribution.
    • The handling of diffraction has been made more flexible. Specifically the "total" Pomeron-proton cross section can now be made to depend on the mass of the diffractive system. This does not affect the diffractive cross section in pp collisions, which is set separately, but is used in the MPI machinery to affect the average number of interactions per Pomeron-proton collision. Furthermore, the allowed range for some parameters has been expanded. Thanks to Robert Ciesielski.
    • New method Pythia::forceTimeShower(...) can be used to generate a single final-state cascade from a set of partons, without any knowledge of prior history. This is mainly intended for toy studies. The meaning of the ProcessLevel:all switch has been modified so that this parton-level function is available, but not any others at this level.
    • ATLAS tune A2 now included. Thanks to Deepak Kar for providing it.
    • Change in the handling of recoils of timelike showers in resonance decays, in cases of coloured resonances such as t -> b W. In the first step the W always acts as recoiler to the b, but in subsequent step previously the W remained as recoiler to one dipole, while now all QCD-radiating partons recoil against another coloured parton. The old behaviour could give a (small) unphysical spike of radiation collinear with the colourless recoiler in the subsequent emissions (while the pattern of the first was and remains correct). The old behaviour can be recovered for checks, see TimeShower:recoilToColoured. Thanks to Yevgeny Kats for pointing out this issue (previously noted for Pythia 6 by several persons).
    • Bug fixes for rootexamples/Makefile and restoration of some deleted information in rootexamples/README. Thanks to Axel Naumann and Bernhard Meirose.
    • Bug fix, so that displaced vertices are possible in resonance decay chains. Thanks to Daniel Blackburn and Andy Buckley for pointing this out.
    • Bug fix for Info counter 2.
    • Bug fix so that sextet quarks now are read in correctly from Les Houches Event files; previously the (anti)colours were set to 0.
    • Year updated to 2012 in copyright statements etc.
    • Reformatting to reduce the number of code lines with more than 79 characters.
    • Pythia::initSLHA() moved from public to private.
    • Remove warning message when tau polarization is set by hand.
    • Several minor changes to reduce the number of warnings issued by the clang compiler. The origin of some warnings remains unclear so those remain to track down (could also be compiler bugs; note that we discuss warnings, not errors). Thanks to Randy MacLeod for bringing this up.
    • The worksheet has been updated to be in step with Pythia 8.160.
    • Several other minor corrections in the code and documentation.
  • 8.162: 12 March 2012
    • A new option allows for several partons to share the recoil in final-state radiation, seeTimelike Showers. It is mainly intended to be used in the context of matching to matrix elements, and so only to be used in the first few branchings.
    • Several new processes for LED dijet production, see Extra Dimensions.
    • Small update of the Sigma2ffbar2LEDllbar and Sigma2ffbar2LEDgammagamma LED processes.
    • New Sigma2QCffbar2llbar contact interaction process.
    • Inclusion of a new method in the matrix-element merging framework to influence the construction of histories, e.g. to already in the construction of histories disallow paths that fail the 2 -> 2 cuts.
    • Further minor updates of the matrix-element merging code, mainly for improved clarity.
    • Minor bug fix in the handling of beam and event information fed in from an LHAup instance.
    • Minor bug fix for potential crashes from uninitialized variables for the merging machinery when merging is not used.
    • Updated History class for matrix element merging, also avoiding some compiler warnings.
    • Bug fixes in the handling of correlated mass choices in resonance decays, such as H -> Z^*0 Z^*0.
    • Bug fix when the process-level execution is switched off, where Info::isResolved() could be called before its value was initialized. Thanks to Christian Pulvermacher for finding this.
    • Corrected matrix-element expression for mass selection in A^0 -> Z^*0 Z^*0 and A^0 -> W^*+ W^*-.
    • SM Higgs mass updated to 125 GeV and default width and branching ratios modified accordingly. Minor technical improvements of width calculation.
    • The usage of nested classes has been removed from SusyLesHouches, since it could give compilation errors on some platforms. The new class names begin with LH and all classes have been put inside the Pythia8 namespace.
    • Minor Makefile updates. Thanks to Mikhail Kirsanov.
    • Minor changes to avoid some clang compiler warnings on the Mac OS X platform.
  • 8.163: 27 March 2012
    • New methods in the Info class, id1pdf(), id2pdf(), x1pdf() and x2pdf(), to denote the partons for which parton distribution values have been defined. Previously this was assumed to agree with the incoming partons to the hard process, the same methods without the pdf qualifier. However, now the POWHEG approach offers a counterexample. Also the reading and handling of Les Houches (and other) events, and the interface to HepMC, has been modified accordingly.
    • The decay of Higgs and top resonances read in from Les Houches Event files is now performed with angular correlations as for internal processes. LHE files should normally contain all process-specific resonance decay chains and, if not, decays are made isotropic. The H -> WW/ZZ -> f fbar f' fbar' and t -> b W -> b f fbar correlations are process-independent, however, and thus can be handled internally. If part of the decay chain has already been set, e.g. H -> WW/Z> or t -> b W, then the subsequent decays are still isotropic.
    • Updated instructions how to link to HepMC, in README.HepMC.
    • Bug fix in the turn-on of resolved diffraction for low CM energies. Thanks to Erwin Visser.
    • Bug fix in the handling of string junctions at very high energies, caused by numerical errors. Thanks to Erwin Visser.
    • Some other small changes, mainly aesthetics.
  • 8.165: 8 May 2012
    • The MBR (Minimum Bias Rockefeller) model for single, double and central diffraction [Cie12] is included as new option Diffraction:PomFlux = 5. It is specifically intended for p p and pbar p interactions, and is currently the only option that also supports central diffraction. Thus the basic machinery for Central Diffraction (a.k.a. Double Pomeron Exchange) has now been implemented. See examples/main04.cc for an example. Thanks to Robert Ciesielski for contributing the new code.
    • For a tau lepton in an external process, by default the SPINUP number in the Les Houches Accord now is interpreted as giving the tau helicity, and is used for its decay.
    • A tau coming from a W now defaults to being purely lefthanded when neither of the existing matrix elements apply.
    • Decay mode t -> H+ b included as an option.
    • Four ATLAS tunes have been implemented as options for Tune:pp: A2-minbias-mstw2008lo, AU2-cteq6l1, AU2-mstw2008lo, and AU2-ct10. The new flag Tune:preferLHAPDF can be used to switch between the LHAPDF and the internal implementation of a PDF set, in cases where both are available.
    • Reorder libraries in examples/Makefile, specifically move LIBGZIP so that it is properly linked when used. Thanks to Erik Schnetter.
    • Minor modification so that LHAPDF can be used for PDFs in the hard process, with one of the built-in PDFs for the rest, even if LHAPDF is compiled so as to handle only one concurrent PDF set.
    • Bug fix, that ParticleDecays:mixB = off did not switch off B0 - B0bar and Bs0 - Bs0bar mixing. Thanks to James Catmore.
    • Bug fix for the handling of gluon polarization of initial-state radiation, where an anisotropic azimuthal distribution was inadvertently generated in some 2 -> 1 processes. The update also includes always setting the second daughter zero for the two partons coming in to a hard 2 -> 1 process. Thanks to Antonio Policicchio.
    • Bug fix, that the setting of the number of user hooks MPI steps did not use UserHooks::canVetoMPIStep() properly.
    • Some other small changes, mainly documentation and aesthetics.
  • 8.170: 21 September 2012
    • Streamline default behaviour and options for choice of GeV or MeV for output to the HepMC event format, see HepMC Interface. Also set the mass of HepMC particles explicitly, rather than having it calculated implicitly. Thanks to James Monk and Andy Buckley.
    • The tau decay machinery has been further augmented with matrix elements and form factors for a variety of decay modes, such that all modes with a branching ratio above 0.1% are fully modeled. Several new classes and methods have been added to this end, Also, a tau pair coming from a Z^0 decay is now handled by assuming the Z^0 to be unpolarized when neither of the existing matrix elements apply. Taus coming from B baryons are handed as for B mesons.
    • Flavour violating decays have been added to the squark, gluino, neutralino and chargino decay tables.
    • Extend the UserHooks::subEvent(...) method so that it also works passably at the process level. Also new option for UserHooks::omitResonanceDecays(...).
    • New methods UserHooks::canVetoPartonLevelEarly() and UserHooks::doVetoPartonLevelEarly( const Event&) are intended to be used the same way as the existing ones without Early in their names, but allow veto right after the ISR + FSR + MPI evolution, before beam remnants are added and resonance decays are considered.
    • Central diffraction now available for all PomFlux options, not only the MBR model. This has been constructed by analogy with the respective assumptions made for single diffraction, but includes some arbitrariness. Therefore the cross section is left easily rescaleable and, for backwards compatibility with tunes that does not contain it, easily possible to switch off, see the relevant section.
    • Reading of ALPGEN parameter and event files has been added, see ALPGEN and MLM Merging.
    • MLM matching has been added, as a first step for ALPGEN events, see ALPGEN and MLM Merging.
    • The CKKW-L merging machinery has been upgraded in a number of respects.
      - More thorough treatment of pp>bb~e+e-veve~ with additional b-jets.
      - Corrected hard mu_r and mu_f choices for dijet and prompt photon.
      - More ways to define a hard process, e.g. with the LEPTONS and NEUTRINO tags. The merging will understand LHE files for mixed processes (e.g. W+ and W- production together).
      - More merging scale definitions.
      - More freedom to generate all possible histories.
      - Internal check (and cut) on Les Houches events in Pythia::mergeProcess if merging scale value of the events is below the value given to Pythia by setting Merging::TMS.
    • It now works to have R-parity violating decays of R-hadrons, i.e. baryon number violation in a vertex displaced from the primary one.
    • The documentation of diffractive processes by the Info methods has been expanded and corrected. This also include the list() method.
    • Particle masses and widths have been updated to agree with the 2012 RPP values [Ber12]. Thanks to Piotr Zyla for data file and James Catmore for program to update the PYTHIA tables from this input.
    • New methods jetAssignment and removeJet added to the SlowJet class.
    • Introduce angular correlation in decay chain H -> gamma Z0 -> gamma f fbar. Thanks to Tim Barklow and Michael Peskin.
    • Introduce simple way to bias the selection of 2 -> 2 processes towards larger pT values, with a compensatingly decreasing event weight, see Phase Space Cuts. Only offers a subset of the possibilities allowed by UserHooks, but simpler to use. The main08.cc program has been expanded to illustrate this possibility, and also expanded to include low-pT subsamples.
    • The two remaining non-NLO tunes from [ATL12] are now included.
    • The Info methods nTried, nSelected, nAccepted, sigmaGen and SigmaErr now takes the code of an individual process as an optional argument.
    • It is now possible to generate resonance decays, followed by showers and hadronization, without having them associated with any specific process. This is part of an expanded Hadron-Level Standalone machinery, as before triggered by ProcessLevel = off, but additionally requiring Standalone:allowResDec = on. Input can either be directly into the event event record or via a (simplified) Les Houches Event File.
    • New configure script options --installdir, --prefix and --datadir can be used to set the location(s) to which the library, header and data directories will be copied by a make install subsequent to the make. Thanks to Mikhail Kirsanov.
    • Fix charge in antiparticle name when particle read in from SLHA file. Thanks to Johan Alwall.
    • Pointers now only compared with == and != (not e.g. > 0), to avoid warnings in gcc 4.7.
    • New check that version number of the code matches that of the XML files. If not, no events can be generated. Thanks to James Monk for suggestion.
    • New check that mother and daughter indices have been set to give a consistent event history. Can be switched on/off with the new Check:history flag.
    • A new method LHAup::newEventFile has been added to switch to reading in events from another LHE file without having to reinitialize the whole class. Lower-level routines like openFile and closeFile have been added to handle correct order of operations also when an intermediate gzip decompression step is involved.
    • LHAup::eventLHEF() can now be called with an optional argument false, to make event files somewhat smaller by reducing the amount of blanks.
    • A new mode Beams:nSkipLHEFatInit introduced to skip ahead the first few events in a Les Houches Event File (cf. the LHAup::skipEvent(nSkip) method).
    • Introduce a new pair of user hooks that can be used to reject the sequence of hard-process resonance decays, without rejecting the production of the primary resonances.
    • The possibility of separate multiplicative prefactors to the renormalization and factorization default pT^2 scale has been introduced for both timelike and spacelike showers.
    • Bug fixes in history information for R-hadron production, which also fixes HepMC conversion in this case.
    • Bug corrected in SigmaSusy.cc, for chargino+neutralino production. Indexing error for incoming quark states in the process Sigma2qqbar2charchi0, resulted in incorrect CKM factors.
    • Corrected a bug in SusyLesHouches.cc, for NMSSM spectra. The unitarity check on the neutralino mixing matrix was faulty, leading to erroneous messages about unitarity violations and SUSY being switched off.
    • Bug fixes in the handling of resolved and unresolved diffractive events. Thanks to Robert Ciesielski for debug.
    • Do not set up FSR dipoles for 2 -> 1 processes.
    • Check that some channel open for resonance decays. Also further check whether resonance decay treatment should be invoked.
    • Bug fix in reading of particle names from SLHA input.
    • Change mass, width and decay mode(s) of D*_s(10431). Thanks to Michal Petran.
    • Bug fix in leptoquark production (lepton sign in q g -> LQ l).
    • New argument added to SpaceShower::reassignBeamPtrs for diffractive event processing, as already available for TimeShower.
    • Do not write warnings in SpaceShower for weights above unity if the evolution scale is below 1 GeV^2.
    • Add default values for member variables in some constructors, and some related changes for AlphaStrong code.
    • Warn if negative-energy parton in hadronization.
    • The MPI pT values assumed in the beam remnant setting of primordial kT and colour reconnection probability were incorrect for diffractive events.
    • The arrays with MPI information were not reset when parton or hadron level fails and a new try is made. Only affected few events.
    • MPI statistics can not yet be accumulated for diffractive events, and therefore the relevant routine is no longer called.
    • Bug fix in the double parton scattering suppression from energy-momentum conservation.
    • Outgoing proton masses were not set in the event record for elastic scattering (but kinematics handling was correct).
    • Bug fixes in the identification and documentation of junctions, previously leading to some unnecessarily rejected events. Also other improvements leading to fewer errors.
    • Slightly increased values for FragmentationSystems:mJoin and StringFragmentation::FACSTOPMASS to reduce failure rate, without noticeably affecting event properties.
    • The Les Houches cross section error is now taken into account in the final Pythia error for strategies +-3. New methods LHAup::xSecSum() and LHAup::xErrSum() provide the necessary information.
    • When a tau pair comes from a massless photon, in dipole shower evolution, for the decay description the mother photon is reassigned to have the sum of the tau momenta.
    • Minor change in initialization sequence for user hooks, to allow for more flexibility.
    • Do not print warnings when multiparton interaction weights are only slightly above unity.
    • Do not write warnings for three known particles that are so close to threshold that widths are switched off to avoid trouble.
    • Some minor typographical changes.
  • 8.175: 18 February 2013
    • Richard Corke and Stefan Ask leave as active authors, and have new e-mail addresses.
    • Jesper Roy Christiansen and Philip Ilten join as new authors.
    • A severe bug found and corrected in the handling of junction fragmentation. For some string topologies it could lead to parts of partonic systems mainly aligned along the beam axis to obtain an effective tilt, thereby giving rise to a pair of opposing jets that should not be there. The bug was an unfortunate side consequence of the improvement of junction handling introduced in version 8.170, and do not affect versions prior to that. To the largest extent possible, it is recommended to avoid this version. Potential errors are likely to be most relevant for processes at low pT, whereas processes that already have a large scale proportionately are less affected. Sincere apologies, and thanks to Hannes Jung for discovering it.
    • The initialization is aborted when the user tries to change the value of a non-existing variable in the Settings or ParticleData databases, and it becomes impossible to generate events. This may be rather brutal, as opposed to the former policy of ignoring such commands (except for a warning), but avoids that the user wastes time on a run that is likely not to give the wanted results. Thanks to Gavin Salam for stressing this point.
    • Major updates of the merging code. CKKW-L code is made more flexible, and now includes additional options to facilitate merging of additional jets in MSSM processes. Unitarised ME+PS merging (UMEPS) is introduced as a new merging scheme for tree-level input. An example main program for UMEPS is added. UMEPS is documented in the new section UMEPS Merging. NLO merging methods are now functional. Two NLO merging schemes are implemented: NL3 and unitarised NLO+PS merging (UNLOPS), both of which are illustrated with example main programs. NLO merging is documented in NLO Merging.
    • The machinery for the MLM-style matching of jets has been expanded to cover input either from ALPGEN, as before, or from Madgraph (or other LHEF input), and expanded to cover either a matching algorithm based on the one in ALPGEN or the one in Madgraph. See Jet Matching for details.
    • Neutrons and antineutrons are now allowed as incoming beam particles. The neutron PDF is derived from the chosen proton PDF by simple isospin conjugation, and total/elastic/diffractive cross sections are assumed the same as for protons.
    • Update in Pythia.cc, to allow user to override SLHA mass values by hand, controlled by the new flag SLHA:allowUserOverride. This was motivated by people wanting to be able to read in a base SLHA spectrum and then quickly scan over particular mass values manually. Corresponding documentation update in SUSYLesHouchesAccord.xml.
    • Updates to the ResonanceWidths and SUSYResonanceWidths classes, to merge common initialization steps into the base class. Corresponding documentation update in SemiInternalResonances.xml. Also some cosmetic changes in SUSYResonanceWidths to improve conformity with CODINGSTYLE rules.
    • The SlowJet jet finder is updated with an option for an alternative R separation based on cosh(Delta y)-cos(Delta phi).
    • Statistics information on the separate subprocesses among the Les Houches external input is improved.
    • The sophisticated tau decay machinery has been expanded so that it can also handle production of taus in hypothetical lepton-number-violating processes, such as H0 -> tau+ mu-.
    • Branching ratios for most light hadrons, and the tau lepton, have been updated to agree with the 2012 Review of Particle Physics [Ber12], by Anil Pratap Singh.
    • Photon radiation can now be included in leptonic two-body decays of hadrons by setting the new switch ParticleDecays:allowPhotonRadiation = on. The lower shower cutoff TimeShower:pTminChgL has been reduced so as to let the simulated photon spectrum extend to lower energies.
    • A new switch MultipartonInteractions:bSelScale has been introduced, to determine the relevant mass or pT scale of an event for the selection of impact parameter in the MPI framework. In spite of a changed default behaviour (the old being option 3), practical consequences are small for most processes.
    • The new UserHooks::retryPartonLevel() method can be overloaded, so that the same hard process is reused for a new try on the parton level, rather than being rejected completely. Thanks to Christian Bauer for suggestion.
    • A new method Event::undoDecay(int i) can be used to remove the daughters of a particle, and further descendents. Does not work for removing the daughters of a parton.
    • The interface to HepMC has been updated. In particular the support for old version has been removed, thereby allowing significant simplifications. The list of methods to set and get the behaviour of the conversion routine has also been updated. The set_event_scale method now stores the renormalization scale (rather than the pT stored previously). The examples main41, main42, main61, main62 and main84 have been updated accordingly.
    • Four new methods to interrogate the default values of the four different kinds of settings.
    • The Vec4 class has been expanded with methods to return true rapidity or pseudorapidity, and the R distance in (y, phi) or (eta, phi) cylindrical coordinates. Thanks to Andy Buckley.
    • The copy and = constructors of the Pythia class are made private so that compilers will block use of them. Thanks to Andy Buckley.
    • New option of the Pythia constructor, to omit the banner printout where necessary. Also new master switch Print:quiet to switch off most runtime program messages. Thanks to Andy Buckley.
    • Updates in the machinery that restores all affected values to their defaults before setting a new tune.
    • A new Vect class has been introduced for the Settings database. It can be used to store a vector of double-precision real values.
    • Three new groupings of existing QCD processes: SoftQCD:inelastic, HardQCD:hardccbar and HardQCD:hardbbbar.
    • New possibility to set the a and b parameters of the Lund fragmentation function separately for heavy flavour. Especially the b is expected to be universal, but Aurelien Martens and Eli Ben-Haim have found improved fits by relaxing this condition, so we formalize this possibility without recommeding it.
    • Method Pythia::getPDFPtr is made public so it can be used also outside the Pythia class to access PDF sets. Internally the PDF bookkeeping is modified to allow for the simultaneous handling of several PDF sets. Thanks to Mathias Ritzmann for providing code changes.
    • It is now possible to read the separate scale values of all outgoing particles, if this info is stored as a single line in an LHEF, begun by a single hashtag character. This is currently nonstandard and may evolve.
    • Some improvements to the install targets code in the Makefile and error detection in examples/configure. Thanks to Mikhail Kirsanov.
    • The CC and FC global environment variables can be set to specify the C++ and Fortran 77/90 compilers, otherwise set in configure and examples/configure. Thanks to Mikhail Kirsanov.
    • Check of shell choice in configure removed. Thanks to Andy Buckley.
    • Minor modifications in the Makefile and text for Root examples, relevant if shared libraries are used.
    • Previously the whole std namespace has been made available in PythiaStdlib.h. Now this behaviour has been replaced by the already-existing alternative, where only a part of std is made available, and only inside the Pythia8 namespace. Thus user code does not become reliant on the choices in PYTHIA. Some related smaller code rearrangements. Thanks to Andy Buckley.
    • When the "second hard" machinery is used to set two hard processes, the old behaviour for the SpaceShower:pTmaxMatch = 0 and TimeShower:pTmaxMatch = 0 options was to use the combined final state of the two processes to decide what pT_max scale to use. This could have unexpected consequences. Now each process is analyzed separately, and therefore has a separate scale. Also for MultipartonInteractions:pTmaxMatch = 0 the two interactions now are analyzed separately. It is then enough that one of them should limit pT_max of subsequent MPI's for such a restriction to be imposed. Thanks to Monika Jindal for discovering this bug.
    • The TimeShower:pTdampMatch option had no effect if switched on, since some code was missing. The manual description of it and the more relevant SpaceShower:pTdampMatch has been updated.
    • One minor bug fix and some corrections to make the code compile on Windows/VisualC++-2010. A simple error function parametrization has been added to PhaseSpace.h and SigmaTotal.h, to be uncommented in case erf(x) is not available by default. Thanks to Guy Barrand for providing the information.
    • Break a closed dependency loop between ParticleData.h and ResonanceWidths.h. Thanks to Andreas Schaelicke and Andy Buckley.
    • In the examples/mainXX.cc programs, class instances that have been created with a new are explicitly deleted at the end of the run. Useful if trying to track memory leaks.
    • Bug fix for R-parity violating decays of R-hadrons, to treat the special case of sequential resonance decays after the RPV one. Thanks to Mariangela Lisanti for pointing out this bug.
    • Changed the maximum allowed value for Tune:pp. Thanks to Yevgeny Kats.
    • Bug fix in the z-value weight for QED ISR emissions.
    • Some destructors moved for improved consistency.
    • Constants DEBUG renamed DBSUSY in the SusyCouplings and SusyResonanceWidths classes to avoid confusion. Thanks to Guy Barrand.
    • Many typos corrected and some other minor improvements of the online documentation.
    • The year has been updated to 2013 in files.
  • 8.176: 18 April 2013
    • Introduce weak shower, whereby W^+- and Z^0 gauge bosons can be produced interleaved with ordinary QCD and QED emissions. Currently only available for final-state radiation, and off by default, see Timelike Showers. A new status code 56 denotes W^+- and Z^0 gauge bosons produced by the FSR parton showers.
    • The gauge bosons produced by showers decay at the end of the parton-level step. New identity codes 93 for a Zcopy and 94 for a Wcopy can be used to set the decay modes of shower-produced gauge bosons separately from hard-process ones, but do not appear in event listings.
    • The Particle class has been updated with a pointer to the mother Event class, replacing the previous pointer to the ParticleData class. Thereby several old methods in the Event class can obtain new equivalents for the Particle one. That is, a call event.method(i) instead can be written event[i].method(). The duplicated methods are statusHepMC, iTopCopy, iBotCopy, iTopCopyId, iBotCopyId, motherList, daughterList, sisterList, isAncestor and undoDecay. Omitted is sisterListTopBot, while sisterList obtains an optional argument. A new method index is introduced. The now redundant Event class methods will be removed in PYTHIA version 8.2. Thanks to Andy Buckley for suggestion.
    • The initialization of SUSY couplings and particle data has been moved from the Pythia and ProcessLevel classes to a new dedicated SLHAinterface class.
    • Some SUSY 3-body decays have been implemented with Matrix Element weighting.
    • New method Info::scalup() returns the Les Houches SCALUP variable. This method is now used instead of QFac() in main31.cc, to set maximal scale for shower radiation in case that the event contains no POWHEG emission, and thereby sidesteps a potential bug when PDF information is provided in the Les Houches Event File. Also some default values have been changed in main31.cmnd. Thanks to James Monk.
    • New parameter LesHouches:mRecalculate can be used to prompt the recalculation of a particle mass from its four-momentum. This may be required for Les Houches input events where the nominal mass of the particle species is stored in the mass slot, rather than the actual mass of the current particle, as foreseen.
    • Extra checks that tracing of junctions in particular and partonic colour singlets in general are only performed when the event record contains coloured unhadronized partons. Thanks to James Catmore.
    • Minor correction related to GZIP support. Thanks to James Monk.
    • Recalculate the phase space of diffractive processes for each event when variable beam energies are allowed. Thanks to Oldrich Kepka for finding the bug.
    • Fix a bug whereby a gluon in diffractive systems would obtain a light-quark mass.
    • The Pythia::check() method can also check that each particle obeys E^2 - p^2 = m^2 (within numerical precision). Speed up the checks on mother-daughter history by streamlining the handling of simple cases.
  • 8.180: 22 September 2013
    • Nishita Desai joins as new author.
    • All the header files include/*.h have been moved to include/Pythia8/*.h to better comply with conventions in other libraries (* = generic name). Thus also all code lines #include "*.h" that refer to PYTHIA files have been changed to #include "Pythia8/*.h". Thanks to Andy Buckley for suggestion.
    • The class that converts PYTHIA events to the HepMC format is renamed from I_Pythia8 to Pythia8ToHepMC, the files where the class resides from HepMCInterface.h/.cc to Pythia8ToHepMC.h/.cc, and the subdirectory of the .cc file from hepmcinterface to pythia8tohepmc. This clarifies the role of the class and avoids potential future name clashes with other interfaces. Makefiles and example main runs have been modified accordingly. Thanks to Andy Buckley.
    • The configure/Makefile step has been extended such that a bin/pythia8-config script is constructed, to simplify subsequent linking of PYTHIA 8 and other libraries to your main program. See the README file for further instructions, the new "Compling programs against PYTHIA 8" section. Thanks to Andy Buckley for code and text.
    • The "minbias" event class has been renamed into the (inelastic) "nondiffractive" one, since the "minbias" denomination should be reserved for an experimental procedure. Needless to say, also the separation into diffraction or not could be made by experimental procedures, but here it is more generally accepted that there is an underlying theoretical description that takes precedence in cases of conflict. Thus the SoftQCD:minBias flag has been remaned SoftQCD:nonDiffractive, and the Info::isMinBias() method has been renamed Info::isNonDiffractive(). The old names have been retained as alternatives for now. Thanks to Andy Buckley.
    • Four PDF sets have been added from the NNPDF2.3 QCD+QED family: the central sets for LO with alpha_s(M_Z) = 0.130, LO with alpha_s(M_Z) = 0.119, NLO with alpha_s(M_Z) = 0.119, and NNLO with alpha_s(M_Z) = 0.119. Thanks to Juan Rojo and Stefano Carrazza for providing the code.
    • The fjcore version 3.0.5 code from FastJet has been included with the PYTHIA distribution. SlowJet now by default becomes a front end to fjcore, but the old behaviour is retained as an option. The new approach is faster, but the older one still offers a few extra possibilities. Note that the new useFJcore argument to the SlowJet constructor has been included as a new last-but-one argument, since the last one is likely to be used much more infrequently and logically depends on the value set for useFJcore. Thanks to Matteo Cacciari, Gavin Salam and Gregory Soyez for making the fjcore code freely distributable.
    • New method constituents(i) in FastJet returns a vector with the indices of the particles belonging to the i'th jet.
    • The global recoil option for final-state showers has been extended with a few more options to improve possibility for matching to output from other programs, such as aMC@NLO.
    • Further extensions of the weak-showering machinery, but still experimental. Now also includes W/Z emission in the initial state.
    • Introduce new qqbar option for SigmaProcess::inFlux() and update documentation.
    • Improve the description of meMode for resonances and illustrate how to force specific Higgs branching ratios in main16.cmnd.
    • Added two previously missing SUSY processes for associated production of a gluino with a neutralino or chargino: SUSY:qqbar2chi0gluino and SUSY:qqbar2chi+-gluino, using the cross section expressions in [Fuk11]. Validated against PYTHIA 6 and XSUSY.
    • Added direct slepton production from q qbar annihilation, SUSY:qqbar2sleptonantislepton. Validated against PYTHIA 6.
    • Corrected some slepton and squark EW couplings in SusyCouplings.
    • Generalized the cross section formulae for SUSY:qg2squarkgluino to the case of non-minimal flavor violation, using the expressions in [Fuk11]. Validated against PYTHIA 6 and XSUSY. The new implementation is compatible with both SLHA2 and SLHA1, whereas the older was only compatible with SLHA1.
    • Generalized the cross section formulae for SUSY:qqbar2gluinogluino to the case of non-minimal flavour violation, using the expressions in [Fuk11]. (Also corrected a factor 2 in that paper on the color factor for st and su interference terms.) The new implementation is compatible with both SLHA2 and SLHA1, whereas the older was only compatible with SLHA1.
    • Changed the default meMode for SLHA DECAY modes to 100, to allow off-shell decays. Enabled the user to choose a different meMode if desired, via a new mode, SLHA:meMode. If values different from 100 are selected (e.g., 103), modes that are extremely far off shell (defined as needing a fluctuation of more than 100 times the root-sum-square of the widths of the mother and daughter particles) will still default back to 100, though the user may of course still switch them off if so desired. Added documentation about this in SusyLesHouchesAccord.xml. Deleted the parameter SLHA:minDecayDeltaM, which would prevent the possibility of off-shell decays unless set to a large negative value.
    • Added calculation of decay lengths to SLHA DECAY modes.
    • Updated documentation of SUSY processes and SLHA-related parameters. Additional reference to the new cross sections included in the bibliography.
    • Allow six-flavour running of alpha_s above the top threshold, and implement option with CMW rescaling of the Lambda values, for use in coherent showers.
    • The merging code has been updated, with corrected handling of massive partons. This amends problems in tt̄, and makes clusterings of massive emissions W, Z, ~g possible. The bookkeeping for the hard process has been upgraded to accommodate more general BSM processes. The treatment of incomplete histories has been upgraded, so that histories which allow for at least one clustering will be used in the unitarisation. Also, states that do not allow for any clustering will not be subject to the (internal, optional) cut on the input events any longer, to guarantee full phase space coverage. This is important for processes for which a non-negligible fraction of states lead to incomplete histories, e.g. tt̄W production. Further, functionality for reclustering FSR off SUSY particles has been added. A new setting allows more easily to switch between 4-flavour and 5-flavour merging schemes.
    • The main85.cc - main88.cc have obtained support for zipped LHE input files, and have nicer printing of the inclusive cross section at the end.
    • Introduced new mode LesHouches:setLifetime so that the lifetime information in Les Houches input can be replaced by the standard PYTHIA selection procedure. By default this is applied to tau leptons, since some matrix-element generators do not set this lifetime. Thanks to James Monk and Thorsten Kuhl.
    • A new examples/main46.cc illustrates how to write a ProMC file with PYTHIA events. Thanks to Sergei Chekanov.
    • The Vect class has been renamed PVec and a new MVec class has been introduced along the same lines, see the Settings database. They can be used to store a vector of double-precision real or integer values, respectively, i.e. of parms or modes, hence the names. Thanks to Abram Krislock.
    • Two new vectors of integers SUSY:idVecA and SUSY:idVecB have been introduced to allow a more flexible selection of final states in SUSY processes, see the SUSY process selection page. The selection machinery has been expanded to cope. Thanks to Abram Krislock.
    • New switch PartonLevel:earlyResDec to give first simple option where resonances are allowed ro decay before colour reconnection and beam remnants are added.
    • Renamed the mass(...) methods to mSel(...) in the Particle, ParticleData and ParticleDataEntry classes, to avoid users mistaking Particle::mass() for Particle::m().
    • Fixed a missing (unused) argument in some derived classes when the mRecalculate parameter was introduced in Les Houches code in version 8.176.
    • Removed several unused class variables from header files, based on new compiler information.
    • Fixed a bug in Sigma2ffbar2HposHneg, where int(...) was used instead of abs.(...). Thanks to Vittorio Zecca.
    • Fixed missing re-initialization of Breit-Wigner mass generation parameters for externally set new resonance widths. Thanks to Vittorio Zecca.
    • Fixed several places where division by zero or adressing of arrays out-of-bounds could occur. While some were trivial, others revealed underlying errors, notably in the handling of some SUSY processes and resonances. New checks against unphysical SLHA input have been implemented. Also some bug fixes in the new weak-shower ISR component, the sphericity analysis, the event undo-decay option, and more. Thanks to Vittorio Zecca.
    • Bug fix in the tau decay description for decay chains like H0 -> A0 A0 -> 4 tau, caused by an erroneous assignment of the number of spin states. Thanks to Brock Tweedie.
    • Add setting of some TimeShower variables that might remain uninitialized. Thanks to Christian Pulvermacher.
    • Extra check in TimeShower for incoming massive particles, where a recalculation of kinematics to an equivalent massless case could give a slightly negative effective dipole mass (with endpoint masses subtracted). Thanks to Paolo Torrielli.
    • Updated manual on how to implement new showers, mainly detailing new optional method arguments. Thanks to Mathias Ritzmann.
    • Corrected bug in SigmaSUSY which caused flavour violating slepton production (for R-parity conserving cases too).
    • Corrected bug in SusyCouplings where tan(beta) was not read from LHA file for RPV spectrum.
    • Modified the contact interaction term normalization of the f fbar -> l lbar process to agree with the one used in PYTHIA 6. Documentation of the ContactInteractions:Lambda updated to reflect this. Thanks to Daniel Hayden.
    • Introduced copy constroctor for the Event class.
    • Reset the Higgs mass range when its mass is changed in examples/main14.cc.
    • Remove obsolete examples/main91.cc and associated Makefile code.
    • Catch cases where junction topologies are sent to the ministring machinery, which is not set up to handle it, and therefore could give segmentation faults. Very rare.
pythia8-8.1.80.orig/htmldoc/pythia.css0000644000175000017500000000230312217346217015776 0ustar sunsuna:link {color:#bb4444;text-decoration:none;} a:visited {color:#bb4444;text-decoration:none;} a:active {color:#ff0000; text-decoration:underline;} a:hover {color:#ff0000; text-decoration:underline;} body, td, div, span { font-size:16px; font-family:arial,verdana,geneva,helvetica; color:#000000; line-height:1.25; } h1 { font-size:40px; font-family:verdana,verdana,helvetica; font-weight:normal; color:#000000; } h2 { font-size:24px; font-family:arial,helvetica; font-weight:normal; color:#000000; } h3 { font-size:20px; font-family:verdana,geneva,arial,helvetica; font-weight:normal; color:#000000; } h4 { font-size:18px; font-family:verdana,arial,helvetica; font-weight:normal; color:#000000; } code { color:#0000bb; } pre { color:#0000bb; margin-top:0.25em; margin-bottom:0.25em; } strong { color:#0000bb; } input { font-size:16px; font-family:arial,verdana,geneva,helvetica; color:#bb00ff; } i, dt { color:#006600; } p { margin-bottom:0.5em; } li { margin-top:0.5em; margin-bottom:0.5em; } ul, ol { margin-top:0.5em; margin-bottom:0.5em; } pythia8-8.1.80.orig/htmldoc/Welcome.html0000644000175000017500000000106712217615311016247 0ustar sunsun PYTHIA 8 online manual pythia8-8.1.80.orig/htmldoc/ProgramClasses.html0000644000175000017500000001505212217615311017600 0ustar sunsun Program Classes

Program Classes

The complete PYTHIA 8 package contains a multitude of classes. There is no reason to describe all of them, with all of their methods, since most should not be touched by a normal user. Nevertheless some of the crucial ones are described in detail, as a help not only to advanced users but also to developers. We here provide a quick reference (still incomplete) which classes you can find described where on these pages. Normally you have to scroll down to find the details, since the top of the page contains information of more general interest.

Class Reference Comment
BeamShape Beam Shape vertex and beam momentum spread
CellJet Event Analysis jet cone clustering analysis, intended for hadron collider topologies
ClusterJet Event Analysis jet clustering analysis, intended for e^+e^- collider topologies
CoupSM Standard Model Parameters couplings and mixing matrices
CoupSUSY SUSY Les Houches Accord compute and store SUSY couplings, using input from SusyLesHouches
DecayChannel Particle Data Scheme the properties of a single decay channel of particle species
Event Event Record the complete event record
HepMC::Pythia8ToHepMC HepMC Interface convert a PYTHIA event record to the HepMC format
Hist Histograms a primitive built-in histogramming package
Info Event Information various one-of-a-kind information on the current event
LHAPDFInterface Parton Distributions use PDF sets from the LHAPDF library
LHAup Les Houches Accord base class for Les Houches external hard-event input
Particle Particle Properties the properties of a particle in the event record
ParticleData Particle Data Scheme the database of particle species properties
ParticleDataEntry Particle Data Scheme the properties of a particle species
PDF Parton Distributions base class for all PDFs
Pythia Program Flow the top-level class, that drives the generation process
ResonanceWidths Semi-Internal Resonances base class for all resonance-width treatment
Rndm RandomNumbers a primitive built-in histogramming package
RotBstMatrix Four-Vectors rotation and boosts of four-vectors
Settings Settings Scheme the database that regulates the behaviour of the program
SigmaProcess Semi-Internal Processes base class for all hard-process cross sections
SlowJet Event Analysis simple jet clustering using the kT, anti-kT or Cambridge/Aachen algorithms.
SpaceShower Implement New Showers spacelike, i..e. initial-state showers
Sphericity Event Analysis sphericity analysis of events
SusyLesHouches SUSY Les Houches Accord reading in of SLHA information
Thrust Event Analysis thrust analysis of events
TimeShower Implement New Showers timelike, i..e. final-state showers
UserHooks User Hooks get access to some steps of the generation process
Vec4 Four-Vectors four-vectors

You can also access an extensive list of the public methods in these classes, which compensates for the brevity of the current page. pythia8-8.1.80.orig/htmldoc/Fragmentation.html0000644000175000017500000004371412217615311017457 0ustar sunsun Fragmentation

Fragmentation

Fragmentation in PYTHIA is based on the Lund string model [And83, Sjo84]. Several different aspects are involved in the physics description, which here therefore is split accordingly. This also, at least partly, reflect the set of classes involved in the fragmentation machinery.

The variables collected here have a very wide span of usefulness. Some would be central in any hadronization tuning exercise, others should not be touched except by experts.

The fragmentation flavour-choice machinery is also used in a few other places of the program, notably particle decays, and is thus described on the separate Flavour Selection page.

Fragmentation functions

The StringZ class handles the choice of longitudinal lightcone fraction z according to one of two possible shape sets.

The Lund symmetric fragmentation function [And83] is the only alternative for light quarks. It is of the form
f(z) = (1/z) * (1-z)^a * exp(-b m_T^2 / z)
with the two main free parameters a and b to be tuned to data. They are stored in

parm  StringZ:aLund   (default = 0.3; minimum = 0.0; maximum = 2.0)
The a parameter of the Lund symmetric fragmentation function.

parm  StringZ:bLund   (default = 0.8; minimum = 0.2; maximum = 2.0)
The b parameter of the Lund symmetric fragmentation function.

In principle, each flavour can have a different a. Then, for going from an old flavour i to a new j one the shape is
f(z) = (1/z) * z^{a_i} * ((1-z)/z)^{a_j} * exp(-b * m_T^2 / z)
This is only implemented for diquarks relative to normal quarks:

parm  StringZ:aExtraDiquark   (default = 0.5; minimum = 0.0; maximum = 2.0)
allows a larger a for diquarks, with total a = aLund + aExtraDiquark.

Finally, the Bowler modification [Bow81] introduces an extra factor
1/z^{r_Q * b * m_Q^2}
for heavy quarks. To keep some flexibility, a multiplicative factor r_Q is introduced, which ought to be unity (provided that quark masses were uniquely defined) but can be set in

parm  StringZ:rFactC   (default = 1.0; minimum = 0.0; maximum = 2.0)
r_c, i.e. the above parameter for c quarks.

parm  StringZ:rFactB   (default = 0.67; minimum = 0.0; maximum = 2.0)
r_b, i.e. the above parameter for b quarks.

parm  StringZ:rFactH   (default = 1.0; minimum = 0.0; maximum = 2.0)
r_h, i.e. the above parameter for heavier hypothetical quarks, or in general any new coloured particle long-lived enough to hadronize.

Within the string framework, the b parameter is universal, i.e. common for all flavours. Nevertheless, for fits to experimental data, better agreement can be obtained if both a_Q and b_Q can be set freely in a general expression
f(z) = 1/z^{1 + r_Q * b_Q * m_Q^2} * (1-z)^a_Q * exp(-b_Q m_T^2 / z)
The below switches and values can be used to achieve this. They should be used with caution and constitute clear deviations from the Lund philosophy.

flag  StringZ:useNonstandardC   (default = off)
use the above nonstandard Lund ansatz for c quarks.

flag  StringZ:useNonstandardB   (default = off)
use the above nonstandard Lund ansatz for b quarks.

flag  StringZ:useNonstandardH   (default = off)
use the above nonstandard Lund ansatz for hypothetical heavier quarks.

parm  StringZ:aNonstandardC   (default = 0.3; minimum = 0.0; maximum = 2.0)
The a parameter in the nonstandard Lund ansatz for c quarks.

parm  StringZ:aNonstandardB   (default = 0.3; minimum = 0.0; maximum = 2.0)
The a parameter in the nonstandard Lund ansatz for b quarks.

parm  StringZ:aNonstandardH   (default = 0.3; minimum = 0.0; maximum = 2.0)
The a parameter in the nonstandard Lund ansatz for hypothetical heavier quarks.

parm  StringZ:bNonstandardC   (default = 0.8; minimum = 0.2; maximum = 2.0)
The b parameter in the nonstandard Lund ansatz for c quarks.

parm  StringZ:bNonstandardB   (default = 0.8; minimum = 0.2; maximum = 2.0)
The b parameter in the nonstandard Lund ansatz for b quarks.

parm  StringZ:bNonstandardH   (default = 0.8; minimum = 0.2; maximum = 2.0)
The b parameter in the nonstandard Lund ansatz for hypothetical heavier quarks.

As another nonstandard alternative, it is possible to switch over to the Peterson/SLAC formula [Pet83]
f(z) = 1 / ( z * (1 - 1/z - epsilon/(1-z))^2 )
for charm, bottom and heavier (defined as above) by the three flags

flag  StringZ:usePetersonC   (default = off)
use Peterson for c quarks.

flag  StringZ:usePetersonB   (default = off)
use Peterson for b quarks.

flag  StringZ:usePetersonH   (default = off)
use Peterson for hypothetical heavier quarks.

When switched on, the corresponding epsilon values are chosen to be

parm  StringZ:epsilonC   (default = 0.05; minimum = 0.01; maximum = 0.25)
epsilon_c, i.e. the above parameter for c quarks.

parm  StringZ:epsilonB   (default = 0.005; minimum = 0.001; maximum = 0.025)
epsilon_b, i.e. the above parameter for b quarks.

parm  StringZ:epsilonH   (default = 0.005; minimum = 0.0001; maximum = 0.25)
epsilon_h, i.e. the above parameter for hypothetical heavier quarks, normalized to the case where m_h = m_b. The actually used parameter is then epsilon = epsilon_h * (m_b^2 / m_h^2). This allows a sensible scaling to a particle with an unknown higher mass without the need for a user intervention.

Fragmentation pT

The StringPT class handles the choice of fragmentation pT. At each string breaking the quark and antiquark of the pair are supposed to receive opposite and compensating pT kicks according to a Gaussian distribution in p_x and p_y separately. Call sigma_q the width of the p_x and p_y distributions separately, i.e.
d(Prob) = exp( -(p_x^2 + p_y^2) / 2 sigma_q^2).
Then the total squared width is
<pT^2> = <p_x^2> + <p_y^2> = 2 sigma_q^2 = sigma^2.
It is this latter number that is stored in

parm  StringPT:sigma   (default = 0.304; minimum = 0.0; maximum = 1.0)
the width sigma in the fragmentation process.

Since a normal hadron receives pT contributions for two string breakings, it has a <p_x^2>_had = <p_y^2>_had = sigma^2, and thus <pT^2>_had = 2 sigma^2.

Some studies on isolated particles at LEP has indicated the need for a slightly enhanced rate in the high-pT tail of the above distribution. This would have to be reviewed in the context of a complete retune of parton showers and hadronization, but for the moment we stay with the current recipe, to boost the above pT by a factor enhancedWidth for a small fraction enhancedFraction of the breakups, where

parm  StringPT:enhancedFraction   (default = 0.01; minimum = 0.0; maximum = 1.)
enhancedFraction,the fraction of string breaks with enhanced width.

parm  StringPT:enhancedWidth   (default = 2.0; minimum = 1.0; maximum = 10.0)
enhancedWidth,the enhancement of the width in this fraction.

Jet joining procedure

String fragmentation is carried out iteratively from both string ends inwards, which means that the two chains of hadrons have to be joined up somewhere in the middle of the event. This joining is described by parameters that in principle follows from the standard fragmentation parameters, but in a way too complicated to parametrize. The dependence is rather mild, however, so for a sensible range of variation the parameters in this section should not be touched.

parm  StringFragmentation:stopMass   (default = 1.0; minimum = 0.0; maximum = 2.0)
Is used to define a W_min = m_q1 + m_q2 + stopMass, where m_q1 and m_q2 are the masses of the two current endpoint quarks or diquarks.

parm  StringFragmentation:stopNewFlav   (default = 2.0; minimum = 0.0; maximum = 2.0)
Add to W_min an amount stopNewFlav * m_q_last, where q_last is the last q qbar pair produced between the final two hadrons.

parm  StringFragmentation:stopSmear   (default = 0.2; minimum = 0.0; maximum = 0.5)
The W_min above is then smeared uniformly in the range W_min_smeared = W_min * [ 1 - stopSmear, 1 + stopSmear ].

This W_min_smeared is then compared with the current remaining W_transverse to determine if there is energy left for further particle production. If not, i.e. if W_transverse < W_min_smeared, the final two particles are produced from what is currently left, if possible. (If not, the fragmentation process is started over.)

Simplifying systems

There are a few situations when it is meaningful to simplify the original task, one way or another.

parm  HadronLevel:mStringMin   (default = 1.; minimum = 0.5; maximum = 1.5)
Decides whether a partonic system should be considered as a normal string or a ministring, the latter only producing one or two primary hadrons. The system mass should be above mStringMin plus the sum of quark/diquark constituent masses for a normal string description, else the ministring scenario is used.

parm  FragmentationSystems:mJoin   (default = 0.3; minimum = 0.2; maximum = 1.)
When two colour-connected partons are very nearby, with at least one being a gluon, they can be joined into one, to avoid technical problems of very small string regions. The requirement for joining is that the invariant mass of the pair is below mJoin, where a gluon only counts with half its momentum, i.e. with its contribution to the string region under consideration. (Note that, for technical reasons, the 0.2 GeV lower limit is de facto hardcoded.)

parm  FragmentationSystems:mJoinJunction   (default = 1.0; minimum = 0.5; maximum = 2.)
When the invariant mass of two of the quarks in a three-quark junction string system becomes too small, the system is simplified to a quark-diquark simple string. The requirement for this simplification is that the diquark mass, minus the two quark masses, falls below mJoinJunction. Gluons on the string between the junction and the respective quark, if any, are counted as part of the quark four-momentum. Those on the two combined legs are clustered with the diquark when it is formed.

Ministrings

The MiniStringFragmentation machinery is only used when a string system has so small invariant mass that normal string fragmentation is difficult/impossible. Instead one or two particles are produced, in the former case shuffling energy-momentum relative to another colour singlet system in the event, while preserving the invariant mass of that system. With one exception parameters are the same as defined for normal string fragmentation, to the extent that they are at all applicable in this case. A discussion of the relevant physics is found in [Nor00]. The current implementation does not completely abide to the scheme presented there, however, but has in part been simplified. (In part for greater clarity, in part since the class is not quite finished yet.)

mode  MiniStringFragmentation:nTry   (default = 2; minimum = 1; maximum = 10)
Whenever the machinery is called, first this many attempts are made to pick two hadrons that the system fragments to. If the hadrons are too massive the attempt will fail, but a new subsequent try could involve other flavour and hadrons and thus still succeed. After nTry attempts, instead an attempt is made to produce a single hadron from the system. Should also this fail, some further attempts at obtaining two hadrons will be made before eventually giving up.

Junction treatment

A junction topology corresponds to an Y arrangement of strings i.e. where three string pieces have to be joined up in a junction. Such topologies can arise if several valence quarks are kicked out from a proton beam, or in baryon-number-violating SUSY decays. Special attention is necessary to handle the region just around the junction, where the baryon number topologically is located. The junction fragmentation scheme is described in [Sjo03]. The parameters in this section should not be touched except by experts.

parm  StringFragmentation:eNormJunction   (default = 2.0; minimum = 0.5; maximum = 10)
Used to find the effective rest frame of the junction, which is complicated when the three string legs may contain additional gluons between the junction and the endpoint. To this end, a pull is defined as a weighed sum of the momenta on each leg, where the weight is exp(- eSum / eNormJunction), with eSum the summed energy of all partons closer to the junction than the currently considered one (in the junction rest frame). Should in principle be (close to) sqrt((1 + a) / b), with a and b the parameters of the Lund symmetric fragmentation function.

parm  StringFragmentation:eBothLeftJunction   (default = 1.0; minimum = 0.5)
Retry (up to 10 times) when the first two considered strings in to a junction both have a remaining energy (in the junction rest frame) above this number.

parm  StringFragmentation:eMaxLeftJunction   (default = 10.0; minimum = 0.)
Retry (up to 10 times) when the first two considered strings in to a junction has a highest remaining energy (in the junction rest frame) above a random energy evenly distributed between eBothLeftJunction and eBothLeftJunction + eMaxLeftJunction (drawn anew for each test).

parm  StringFragmentation:eMinLeftJunction   (default = 0.2; minimum = 0.)
Retry (up to 10 times) when the invariant mass-squared of the final leg and the leftover momentum of the first two treated legs falls below eMinLeftJunction times the energy of the final leg (in the junction rest frame). pythia8-8.1.80.orig/htmldoc/HiggsProcesses.html0000644000175000017500000012673112217615311017612 0ustar sunsun Higgs Processes

Higgs Processes

This page documents Higgs production within and beyond the Standard Model (SM and BSM for short). This includes several different processes and, for the BSM scenarios, a large set of parameters that would only be fixed within a more specific framework such as MSSM. Three choices can be made irrespective of the particular model:

flag  Higgs:cubicWidth   (default = off)
The partial width of a Higgs particle to a pair of gauge bosons, W^+ W^- or Z^0 Z^0, depends cubically on the Higgs mass. When selecting the Higgs according to a Breit-Wigner, so that the actual mass mHat does not agree with the nominal m_Higgs one, an ambiguity arises which of the two to use [Sey95]. The default is to use a linear dependence on mHat, i.e. a width proportional to m_Higgs^2 * mHat, while on gives a mHat^3 dependence. This does not affect the widths to fermions, which only depend linearly on mHat. This flag is used both for SM and BSM Higgs bosons.

flag  Higgs:runningLoopMass   (default = on)
The partial width of a Higgs particle to a pair of gluons or photons, or a gamma Z^0 pair, proceeds in part through quark loops, mainly b and t. There is some ambiguity what kind of masses to use. Default is running MSbar ones, but alternatively fixed pole masses are allowed (as was standard in PYTHIA 6), which typically gives a noticeably higher cross section for these channels. (For a decay to a pair of fermions, such as top, the running mass is used for couplings and the fixed one for phase space.)

flag  Higgs:clipWings   (default = on)
The Breit-Wigner shape of a Higgs is nontrivial, owing to the rapid width variation with the mass of a Higgs. This implies that a Higgs of low nominal mass may still acquire a non-negligible high-end tail. The validity of the calculation may be questioned in these wings. With this option on, the Higgs:wingsFac value is used to cut away the wings.
Warning: with this option on, the allowed mass range is shrunk, but never widened. This can lead to inconsistencies if a run consists of several subruns with different Higgs masses. The id:mMin and id:mMax values should therefore be reset (e.g. to the defaults 50. and 0.) when id:m0 is changed.

parm  Higgs:wingsFac   (default = 50.; minimum = 0.)
With Higgs:clipWings on, all Higgs masses which deviate from the nominal one by more than Higgs:wingsFac times the nominal width are forbidden. This is achieved by setting the mMin and mMax values of the Higgs states at initialization. These changes never allow a wider range than already set by the user, alternatively by the current default values, see warning above.

Standard-Model Higgs, basic processes

This section provides the standard set of processes that can be run together to provide a reasonably complete overview of possible production channels for a single SM Higgs. The main parameter is the choice of Higgs mass, which can be set in the normal ParticleData database; thereafter the properties within the SM are essentially fixed.

flag  HiggsSM:all   (default = off)
Common switch for the group of Higgs production within the Standard Model.

flag  HiggsSM:ffbar2H   (default = off)
Scattering f fbar -> H^0, where f sums over available flavours except top. Related to the mass-dependent Higgs point coupling to fermions, so at hadron colliders the bottom contribution will dominate. Code 901.

flag  HiggsSM:gg2H   (default = off)
Scattering g g -> H^0 via loop contributions primarily from top. Code 902.

flag  HiggsSM:gmgm2H   (default = off)
Scattering gamma gamma -> H^0 via loop contributions primarily from top and W. Code 903.

flag  HiggsSM:ffbar2HZ   (default = off)
Scattering f fbar -> H^0 Z^0 via s-channel Z^0 exchange. Code 904.

flag  HiggsSM:ffbar2HW   (default = off)
Scattering f fbar -> H^0 W^+- via s-channel W^+- exchange. Code 905.

flag  HiggsSM:ff2Hff(t:ZZ)   (default = off)
Scattering f f' -> H^0 f f' via Z^0 Z^0 fusion. Code 906.

flag  HiggsSM:ff2Hff(t:WW)   (default = off)
Scattering f_1 f_2 -> H^0 f_3 f_4 via W^+ W^- fusion. Code 907.

flag  HiggsSM:gg2Httbar   (default = off)
Scattering g g -> H^0 t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 908.

flag  HiggsSM:qqbar2Httbar   (default = off)
Scattering q qbar -> H^0 t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 909.

Standard-Model Higgs, further processes

A number of further production processes has been implemented, that are specializations of some of the above ones to the high-pT region. The sets therefore could not be used simultaneously without unphysical double-counting, as further explained below. They are not switched on by the HiggsSM:all flag, but have to be switched on for each separate process after due consideration.

The first three processes in this section are related to the Higgs point coupling to fermions, and so primarily are of interest for b quarks. It is here useful to begin by reminding that a process like b bbar -> H^0 implies that a b/bbar is taken from each incoming hadron, leaving behind its respective antiparticle. The initial-state showers will then add one g -> b bbar branching on either side, so that effectively the process becomes g g -> H0 b bbar. This would be the same basic process as the g g -> H^0 t tbar one used for top. The difference is that (a) no PDF's are defined for top and (b) the shower approach would not be good enough to provide sensible kinematics for the H^0 t tbar subsystem. By contrast, owing to the b being much lighter than the Higgs, multiple gluon emissions must be resummed for b, as is done by PDF's and showers, in order to obtain a sensible description of the total production rate, when the b quarks predominantly are produced at small pT values.

flag  HiggsSM:qg2Hq   (default = off)
Scattering q g -> H^0 q. This process gives first-order corrections to the f fbar -> H^0 one above, and should only be used to study the high-pT tail, while f fbar -> H^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> H^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 911.

flag  HiggsSM:gg2Hbbbar   (default = off)
Scattering g g -> H^0 b bbar. This process is yet one order higher of the b bbar -> H^0 and b g -> H^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 912.

flag  HiggsSM:qqbar2Hbbbar   (default = off)
Scattering q qbar -> H^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 913.

The second set of processes are predominantly first-order corrections to the g g -> H^0 process, again dominated by the top loop. We here only provide the kinematical expressions obtained in the limit that the top quark goes to infinity, but scaled to the finite-top-mass coupling in g g -> H^0. (Complete loop expressions are available e.g. in PYTHIA 6.4 but are very lengthy.) This provides a reasonably accurate description for "intermediate" pT values, but fails when the pT scale approaches the top mass.

flag  HiggsSM:gg2Hg(l:t)   (default = off)
Scattering g g -> H^0 g via loop contributions primarily from top. Code 914.

flag  HiggsSM:qg2Hq(l:t)   (default = off)
Scattering q g -> H^0 q via loop contributions primarily from top. Not to be confused with the HiggsSM:qg2Hq process above, with its direct fermion-to-Higgs coupling. Code 915.

flag  HiggsSM:qqbar2Hg(l:t)   (default = off)
Scattering q qbar -> H^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> H^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 916.

Beyond-the-Standard-Model Higgs, introduction

Further Higgs multiplets arise in a number of scenarios. We here concentrate on the MSSM scenario with two Higgs doublets, but with flexibility enough that also other two-Higgs-doublet scenarios could be represented by a suitable choice of parameters. Conventionally the Higgs states are labeled h^0, H^0, A^0 and H^+-. If the scalar and pseudocalar states mix the resulting states are labeled H_1^0, H_2^0, H_3^0. In process names and parameter explanations both notations will be used, but for settings labels we have adapted the shorthand hybrid notation H1 for h^0(H_1^0), H2 for H^0(H_2^0) and A3 for A^0(H_3^0). (Recall that the Settings database does not distinguish upper- and lowercase characters, so that the user has one thing less to worry about, but here it causes problems with h^0 vs. H^0.) We leave the issue of mass ordering between H^0 and A^0 open, and thereby also that of H_2^0 and H_3^0.

flag  Higgs:useBSM   (default = off)
Master switch to initialize and use the two-Higgs-doublet states. If off, only the above SM Higgs processes can be used, with couplings as predicted in the SM. If on, only the below BSM Higgs processes can be used, with couplings that can be set freely, also found further down on this page.

Beyond-the-Standard-Model Higgs, basic processes

This section provides the standard set of processes that can be run together to provide a reasonably complete overview of possible production channels for a single neutral Higgs state in a two-doublet scenarios such as MSSM. The list of processes for neutral states closely mimics the one found for the SM Higgs. Some of the processes vanish for a pure pseudoscalar A^0, but are kept for flexibility in cases of mixing with the scalar h^0 and H^0 states, or for use in the context of non-MSSM models. This should work well to represent e.g. that a small admixture of the "wrong" parity would allow a process such as q qbar -> A^0 Z^0, which otherwise is forbidden. However, note that the loop integrals e.g. for g g -> h^0/H^0/A^0 are hardcoded to be for scalars for the former two particles and for a pseudoscalar for the latter one, so absolute rates would not be correctly represented in the case of large scalar/pseudoscalar mixing.

flag  HiggsBSM:all   (default = off)
Common switch for the group of Higgs production beyond the Standard Model, as listed below.

1) h^0(H_1^0) processes

flag  HiggsBSM:allH1   (default = off)
Common switch for the group of h^0(H_1^0) production processes.

flag  HiggsBSM:ffbar2H1   (default = off)
Scattering f fbar -> h^0(H_1^0), where f sums over available flavours except top. Code 1001.

flag  HiggsBSM:gg2H1   (default = off)
Scattering g g -> h^0(H_1^0) via loop contributions primarily from top. Code 1002.

flag  HiggsBSM:gmgm2H1   (default = off)
Scattering gamma gamma -> h^0(H_1^0) via loop contributions primarily from top and W. Code 1003.

flag  HiggsBSM:ffbar2H1Z   (default = off)
Scattering f fbar -> h^0(H_1^0) Z^0 via s-channel Z^0 exchange. Code 1004.

flag  HiggsBSM:ffbar2H1W   (default = off)
Scattering f fbar -> h^0(H_1^0) W^+- via s-channel W^+- exchange. Code 1005.

flag  HiggsBSM:ff2H1ff(t:ZZ)   (default = off)
Scattering f f' -> h^0(H_1^0) f f' via Z^0 Z^0 fusion. Code 1006.

flag  HiggsBSM:ff2H1ff(t:WW)   (default = off)
Scattering f_1 f_2 -> h^0(H_1^0) f_3 f_4 via W^+ W^- fusion. Code 1007.

flag  HiggsBSM:gg2H1ttbar   (default = off)
Scattering g g -> h^0(H_1^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1008.

flag  HiggsBSM:qqbar2H1ttbar   (default = off)
Scattering q qbar -> h^0(H_1^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1009.

2) H^0(H_2^0) processes

flag  HiggsBSM:allH2   (default = off)
Common switch for the group of H^0(H_2^0) production processes.

flag  HiggsBSM:ffbar2H2   (default = off)
Scattering f fbar -> H^0(H_2^0), where f sums over available flavours except top. Code 1021.

flag  HiggsBSM:gg2H2   (default = off)
Scattering g g -> H^0(H_2^0) via loop contributions primarily from top. Code 1022.

flag  HiggsBSM:gmgm2H2   (default = off)
Scattering gamma gamma -> H^0(H_2^0) via loop contributions primarily from top and W. Code 1023.

flag  HiggsBSM:ffbar2H2Z   (default = off)
Scattering f fbar -> H^0(H_2^0) Z^0 via s-channel Z^0 exchange. Code 1024.

flag  HiggsBSM:ffbar2H2W   (default = off)
Scattering f fbar -> H^0(H_2^0) W^+- via s-channel W^+- exchange. Code 1025.

flag  HiggsBSM:ff2H2ff(t:ZZ)   (default = off)
Scattering f f' -> H^0(H_2^0) f f' via Z^0 Z^0 fusion. Code 1026.

flag  HiggsBSM:ff2H2ff(t:WW)   (default = off)
Scattering f_1 f_2 -> H^0(H_2^0) f_3 f_4 via W^+ W^- fusion. Code 1027.

flag  HiggsBSM:gg2H2ttbar   (default = off)
Scattering g g -> H^0(H_2^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1028.

flag  HiggsBSM:qqbar2H2ttbar   (default = off)
Scattering q qbar -> H^0(H_2^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1029.

3) A^0(H_3^0) processes

flag  HiggsBSM:allA3   (default = off)
Common switch for the group of A^0(H_3^0) production processes.

flag  HiggsBSM:ffbar2A3   (default = off)
Scattering f fbar -> A^0(H_3^0), where f sums over available flavours except top. Code 1041.

flag  HiggsBSM:gg2A3   (default = off)
Scattering g g -> A^0(A_3^0) via loop contributions primarily from top. Code 1042.

flag  HiggsBSM:gmgm2A3   (default = off)
Scattering gamma gamma -> A^0(A_3^0) via loop contributions primarily from top and W. Code 1043.

flag  HiggsBSM:ffbar2A3Z   (default = off)
Scattering f fbar -> A^0(A_3^0) Z^0 via s-channel Z^0 exchange. Code 1044.

flag  HiggsBSM:ffbar2A3W   (default = off)
Scattering f fbar -> A^0(A_3^0) W^+- via s-channel W^+- exchange. Code 1045.

flag  HiggsBSM:ff2A3ff(t:ZZ)   (default = off)
Scattering f f' -> A^0(A_3^0) f f' via Z^0 Z^0 fusion. Code 1046.

flag  HiggsBSM:ff2A3ff(t:WW)   (default = off)
Scattering f_1 f_2 -> A^0(A_3^0) f_3 f_4 via W^+ W^- fusion. Code 1047.

flag  HiggsBSM:gg2A3ttbar   (default = off)
Scattering g g -> A^0(A_3^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1048.

flag  HiggsBSM:qqbar2A3ttbar   (default = off)
Scattering q qbar -> A^0(A_3^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1049.

4) H+- processes

flag  HiggsBSM:allH+-   (default = off)
Common switch for the group of H^+- production processes.

flag  HiggsBSM:ffbar2H+-   (default = off)
Scattering f fbar' -> H^+-, where f, fbar' sums over available incoming flavours. Since couplings are assumed generation-diagonal, in practice this means c sbar -> H^+ and s cbar -> H^-. Code 1061.

flag  HiggsBSM:bg2H+-t   (default = off)
Scattering b g -> H^+ tbar. At hadron colliders this is the dominant process for single-charged-Higgs production. Code 1062.

5) Higgs-pair processes

flag  HiggsBSM:allHpair   (default = off)
Common switch for the group of Higgs pair-production processes.

flag  HiggsBSM:ffbar2A3H1   (default = off)
Scattering f fbar -> A^0(H_3) h^0(H_1). Code 1081.

flag  HiggsBSM:ffbar2A3H2   (default = off)
Scattering f fbar -> A^0(H_3) H^0(H_2). Code 1082.

flag  HiggsBSM:ffbar2H+-H1   (default = off)
Scattering f fbar -> H^+- h^0(H_1). Code 1083.

flag  HiggsBSM:ffbar2H+-H2   (default = off)
Scattering f fbar -> H^+- H^0(H_2). Code 1084.

flag  HiggsBSM:ffbar2H+H-   (default = off)
Scattering f fbar -> H+ H-. Code 1085.

Beyond-the-Standard-Model Higgs, further processes

This section mimics the above section on "Standard-Model Higgs, further processes", i.e. it contains higher-order corrections to the processes already listed. The two sets therefore could not be used simultaneously without unphysical double-counting. They are not controlled by any group flag, but have to be switched on for each separate process after due consideration. We refer to the standard-model description for a set of further comments on the processes.

1) h^0(H_1^0) processes

flag  HiggsBSM:qg2H1q   (default = off)
Scattering q g -> h^0 q. This process gives first-order corrections to the f fbar -> h^0 one above, and should only be used to study the high-pT tail, while f fbar -> h^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> h^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 1011.

flag  HiggsBSM:gg2H1bbbar   (default = off)
Scattering g g -> h^0 b bbar. This process is yet one order higher of the b bbar -> h^0 and b g -> h^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1012.

flag  HiggsBSM:qqbar2H1bbbar   (default = off)
Scattering q qbar -> h^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1013.

flag  HiggsBSM:gg2H1g(l:t)   (default = off)
Scattering g g -> h^0 g via loop contributions primarily from top. Code 1014.

flag  HiggsBSM:qg2H1q(l:t)   (default = off)
Scattering q g -> h^0 q via loop contributions primarily from top. Not to be confused with the HiggsBSM:qg2H1q process above, with its direct fermion-to-Higgs coupling. Code 1015.

flag  HiggsBSM:qqbar2H1g(l:t)   (default = off)
Scattering q qbar -> h^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> h^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 1016.

2) H^0(H_2^0) processes

flag  HiggsBSM:qg2H2q   (default = off)
Scattering q g -> H^0 q. This process gives first-order corrections to the f fbar -> H^0 one above, and should only be used to study the high-pT tail, while f fbar -> H^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> H^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 1031.

flag  HiggsBSM:gg2H2bbbar   (default = off)
Scattering g g -> H^0 b bbar. This process is yet one order higher of the b bbar -> H^0 and b g -> H^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1032.

flag  HiggsBSM:qqbar2H2bbbar   (default = off)
Scattering q qbar -> H^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1033.

flag  HiggsBSM:gg2H2g(l:t)   (default = off)
Scattering g g -> H^0 g via loop contributions primarily from top. Code 1034.

flag  HiggsBSM:qg2H2q(l:t)   (default = off)
Scattering q g -> H^0 q via loop contributions primarily from top. Not to be confused with the HiggsBSM:qg2H1q process above, with its direct fermion-to-Higgs coupling. Code 1035.

flag  HiggsBSM:qqbar2H2g(l:t)   (default = off)
Scattering q qbar -> H^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> H^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 1036.

3) A^0(H_3^0) processes

flag  HiggsBSM:qg2A3q   (default = off)
Scattering q g -> A^0 q. This process gives first-order corrections to the f fbar -> A^0 one above, and should only be used to study the high-pT tail, while f fbar -> A^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> A^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 1051.

flag  HiggsBSM:gg2A3bbbar   (default = off)
Scattering g g -> A^0 b bbar. This process is yet one order higher of the b bbar -> A^0 and b g -> A^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1052.

flag  HiggsBSM:qqbar2A3bbbar   (default = off)
Scattering q qbar -> A^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1053.

flag  HiggsBSM:gg2A3g(l:t)   (default = off)
Scattering g g -> A^0 g via loop contributions primarily from top. Code 1054.

flag  HiggsBSM:qg2A3q(l:t)   (default = off)
Scattering q g -> A^0 q via loop contributions primarily from top. Not to be confused with the HiggsBSM:qg2H1q process above, with its direct fermion-to-Higgs coupling. Code 1055.

flag  HiggsBSM:qqbar2A3g(l:t)   (default = off)
Scattering q qbar -> A^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> A^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 1056.

Parameters for Beyond-the-Standard-Model Higgs production and decay

This section offers a big flexibility to set couplings of the various Higgs states to fermions and gauge bosons, and also to each other. The intention is that, for scenarios like MSSM, you should use standard input from the SUSY Les Houches Accord, rather than having to set it all yourself. In other cases, however, the freedom is there for you to use. Kindly note that some of the internal calculations of partial widths from the parameters provided do not include mixing between the scalar and pseudoscalar states.

Masses would be set in the ParticleData database, while couplings are set below. When possible, the couplings of the Higgs states are normalized to the corresponding coupling within the SM. When not, their values within the MSSM are indicated, from which it should be straightforward to understand what to use instead. The exception is some couplings that vanish also in the MSSM, where the normalization has been defined in close analogy with nonvanishing ones. Some parameter names are asymmetric but crossing can always be used, i.e. the coupling for A^0 -> H^0 Z^0 obviously is also valid for H^0 -> A^0 Z^0 and Z^0 -> H^0 A^0. Note that couplings usually appear quadratically in matrix elements.

parm  HiggsH1:coup2d   (default = 1.)
The h^0(H_1^0) coupling to down-type quarks.

parm  HiggsH1:coup2u   (default = 1.)
The h^0(H_1^0) coupling to up-type quarks.

parm  HiggsH1:coup2l   (default = 1.)
The h^0(H_1^0) coupling to (charged) leptons.

parm  HiggsH1:coup2Z   (default = 1.)
The h^0(H_1^0) coupling to Z^0.

parm  HiggsH1:coup2W   (default = 1.)
The h^0(H_1^0) coupling to W^+-.

parm  HiggsH1:coup2Hchg   (default = 0.)
The h^0(H_1^0) coupling to H^+- (in loops). Is sin(beta - alpha) + cos(2 beta) sin(beta + alpha) / (2 cos^2theta_W) in the MSSM.

parm  HiggsH2:coup2d   (default = 1.)
The H^0(H_2^0) coupling to down-type quarks.

parm  HiggsH2:coup2u   (default = 1.)
The H^0(H_2^0) coupling to up-type quarks.

parm  HiggsH2:coup2l   (default = 1.)
The H^0(H_2^0) coupling to (charged) leptons.

parm  HiggsH2:coup2Z   (default = 1.)
The H^0(H_2^0) coupling to Z^0.

parm  HiggsH2:coup2W   (default = 1.)
The H^0(H_2^0) coupling to W^+-.

parm  HiggsH2:coup2Hchg   (default = 0.)
The H^0(H_2^0) coupling to H^+- (in loops). Is cos(beta - alpha) + cos(2 beta) cos(beta + alpha) / (2 cos^2theta_W) in the MSSM.

parm  HiggsH2:coup2H1H1   (default = 1.)
The H^0(H_2^0) coupling to a h^0(H_1^0) pair. Is cos(2 alpha) cos(beta + alpha) - 2 sin(2 alpha) sin(beta + alpha) in the MSSM.

parm  HiggsH2:coup2A3A3   (default = 1.)
The H^0(H_2^0) coupling to an A^0(H_3^0) pair. Is cos(2 beta) cos(beta + alpha) in the MSSM.

parm  HiggsH2:coup2H1Z   (default = 0.)
The H^0(H_2^0) coupling to a h^0(H_1^0) Z^0 pair. Vanishes in the MSSM.

parm  HiggsH2:coup2A3H1   (default = 0.)
The H^0(H_2^0) coupling to an A^0(H_3^0) h^0(H_1^0) pair. Vanishes in the MSSM.

parm  HiggsH2:coup2HchgW   (default = 0.)
The H^0(H_2^0) coupling to a H^+- W-+ pair. Is sin(beta - alpha) in the MSSM.

parm  HiggsA3:coup2d   (default = 1.)
The A^0(H_3^0) coupling to down-type quarks.

parm  HiggsA3:coup2u   (default = 1.)
The A^0(H_3^0) coupling to up-type quarks.

parm  HiggsA3:coup2l   (default = 1.)
The A^0(H_3^0) coupling to (charged) leptons.

parm  HiggsA3:coup2H1Z   (default = 1.)
The A^0(H_3^0) coupling to a h^0(H_1^0) Z^0 pair. Is cos(beta - alpha) in the MSSM.

parm  HiggsA3:coup2H2Z   (default = 1.)
The A^0(H_3^0) coupling to a H^0(H_2^0) Z^0 pair. Is sin(beta - alpha) in the MSSM.

parm  HiggsA3:coup2Z   (default = 0.)
The A^0(H_3^0) coupling to Z^0. Vanishes in the MSSM.

parm  HiggsA3:coup2W   (default = 0.)
The A^0(H_3^0) coupling to W^+-. Vanishes in the MSSM.

parm  HiggsA3:coup2H1H1   (default = 0.)
The A^0(H_3^0) coupling to a h^0(H_1^0) pair. Vanishes in the MSSM.

parm  HiggsA3:coup2Hchg   (default = 0.)
The A^0(H_3^0) coupling to H^+-. Vanishes in the MSSM.

parm  HiggsA3:coup2HchgW   (default = 1.)
The A^0(H_3^0) coupling to a H^+- W-+ pair. Is 1 in the MSSM.

parm  HiggsHchg:tanBeta   (default = 5.)
The tan(beta) value, which leads to an enhancement of the H^+- coupling to down-type fermions and suppression to up-type ones. The same angle also appears in many other places, but this particular parameter is only used for the charged-Higgs case.

parm  HiggsHchg:coup2H1W   (default = 1.)
The H^+- coupling to a h^0(H_1^0) W^+- pair. Is cos(beta - alpha) in the MSSM.

parm  HiggsHchg:coup2H2W   (default = 0.)
The H^+- coupling to a H^0(H_2^0) W^+- pair. Is sin(beta - alpha) in the MSSM.

Another set of parameters are not used in the production stage but exclusively for the description of angular distributions in decays.

mode  HiggsH1:parity   (default = 1; minimum = 0; maximum = 3)
possibility to modify angular decay correlations in the decay of a h^0(H_1) decay Z^0 Z^0 or W^+ W^- to four fermions. Currently it does not affect the partial width of the channels, which is only based on the above parameters.
option 0 : isotropic decays.
option 1 : assuming the h^0(H_1) is a pure scalar (CP-even), as in the MSSM.
option 2 : assuming the h^0(H_1) is a pure pseudoscalar (CP-odd).
option 3 : assuming the h^0(H_1) is a mixture of the two, including the CP-violating interference term. The parameter eta, see below, sets the strength of the CP-odd admixture, with the interference term being proportional to eta and the CP-odd one to eta^2.

parm  HiggsH1:etaParity   (default = 0.)
The eta value of CP-violation in the HiggsSM:parity = 3 option.

mode  HiggsH2:parity   (default = 1; minimum = 0; maximum = 3)
possibility to modify angular decay correlations in the decay of a H^0(H_2) decay Z^0 Z^0 or W^+ W^- to four fermions. Currently it does not affect the partial width of the channels, which is only based on the above parameters.
option 0 : isotropic decays.
option 1 : assuming the H^0(H_2) is a pure scalar (CP-even), as in the MSSM.
option 2 : assuming the H^0(H_2) is a pure pseudoscalar (CP-odd).
option 3 : assuming the H^0(H_2) is a mixture of the two, including the CP-violating interference term. The parameter eta, see below, sets the strength of the CP-odd admixture, with the interference term being proportional to eta and the CP-odd one to eta^2.

parm  HiggsH2:etaParity   (default = 0.)
The eta value of CP-violation in the HiggsSM:parity = 3 option.

mode  HiggsA3:parity   (default = 2; minimum = 0; maximum = 3)
possibility to modify angular decay correlations in the decay of a A^0(H_3) decay Z^0 Z^0 or W^+ W^- to four fermions. Currently it does not affect the partial width of the channels, which is only based on the above parameters.
option 0 : isotropic decays.
option 1 : assuming the A^0(H_3) is a pure scalar (CP-even).
option 2 : assuming the A^0(H_3) is a pure pseudoscalar (CP-odd), as in the MSSM.
option 3 : assuming the A^0(H_3) is a mixture of the two, including the CP-violating interference term. The parameter eta, see below, sets the strength of the CP-odd admixture, with the interference term being proportional to eta and the CP-odd one to eta^2.

parm  HiggsA3:etaParity   (default = 0.)
The eta value of CP-violation in the HiggsSM:parity = 3 option. pythia8-8.1.80.orig/htmldoc/pythia32.gif0000644000175000017500000000337512217346217016132 0ustar sunsunGIF89a         #!($,#)+* 4 10 8 6! 1%6"=#A!C" =& <&@)>, A*I(G* F.I,M0K2I5 F7O5L7S4^3X8]7V<X=[;f9a;V@[?Z?]@_>b@`?g?g@aDhD gDfE!mDfHmEpFmHhJrDkHtEfMsItJqLrMEzJyJJ!vQ~MyO!xRI"vQ!|PsT"NQT SL"{V&R&VWU'V!ST(U#ZZ#T$UZV'\&X,Y [&ZV)Z$_\*a$e] _ ]&['_&Y(aZ#`-]"e!`^[*cc$a$a1c0g`,d+ia&e&f d h&^)a*f"f)f/k#b1e+j$gg&m,k2g3l-o&m'i(k5l/m"p#t)n*p0u#j2i-n3o'p3p s-m.u u(s(q/p*s*u,v&yt/y.z(|/0v,y,|%{'%~..|2z2Ʉ*͂+̂2Ӂ-|1߀)Ӈ0ׅ14ޅ4ԍ,܉4ފ.03234.//1.2214-5-./003!Created with The GIMP!,  Hp Bbl}UÂQc*S>Np?,qكYdGQ're9pO֗:^0l@]m@={Ny색#b| `n*0DF=<QN p!` -*9Q28fń `*MpB><Խ2 H43O#07xb?Î=c*)xQc:0 I0~D093.DP-k4;ُ4@,HL0~rs;鼃9=0spHqd1D7s=x (B=fۉ3@ZX*@M9픣9J% Bc>DC SNTFP9m SUSY Les Houches Accord

SUSY Les Houches Accord

The PYTHIA 8 program does not contain an internal spectrum calculator (a.k.a. RGE package) to provide supersymmetric couplings, mixing angles, masses and branching ratios. Thus the SUSY Les Houches Accord (SLHA) [Ska04][All08] is the only way of inputting SUSY models, and SUSY processes (see the SUSYProcesses page) cannot be run unless such an input has taken place.

The SLHA input format can also be extended for use with more general BSM models, beyond SUSY. Information specific to how to use the SLHA interface for generic BSM models is collected below, under Using SLHA for generic BSM Models, with more elaborate explanations and examples in [Des11].

Most of the SUSY implementation in PYTHIA 8 is compatible with both the SLHA1 [Ska04] and SLHA2 [All08] conventions (with some limitations for the NMSSM in the latter case). Internally, PYTHIA 8 uses the SLHA2 conventions and translates SLHA1 input to these when necessary. See the section on SUSY Processes and [Des11] for more information. Note that PYTHIA assumes that a spectrum is either fully SHLA1 or fully SLHA2 compliant. Mixing of the two standards is discouraged, as this can lead to ambiguities and inconsistencies.

When reading LHEF files, Pythia automatically looks for SLHA information between <slha>...</slha> tags in the header of such files. When running Pythia without LHEF input (or if reading an LHEF file that does not contain SLHA information in the header), a separate file containing SLHA information may be specified using SLHA:file (see below).

Normally the LHEF would be in uncompressed format, and thus human-readable if opened in a text editor. A possibility to read gzipped files has been added, based on the Boost and zlib libraries, which therefore have to be linked appropriately in order for this option to work. See the README file in the main directory for details on how to do this.

Finally, the SLHA input capability can of course also be used to input SLHA-formatted MASS and DECAY tables for other particles, such as the Higgs boson, furnishing a less sophisticated but more universal complement to the standard PYTHIA 8-specific methods for inputting such information (for the latter, see the section on Particle Data and the scheme to modify it). This may at times not be desirable, so a few options can be used to curb the right of SLHA to overwrite particle data. Conversely, it is sometimes useful to allow the user to modify eg a mass parameter relative to its value in the SLHA spectrum. This is normally not permitted (the SLHA spectrum is normally self-consistent and should not be modified), but an option for allowing it is provided.

The reading-in of information from SLHA or LHEF files is handled by the SusyLesHouches class, while the subsequent calculation of derived quantities of direct application to SUSY processes is done in the CoupSUSY, SigmaSUSY, and SUSYResonanceWidths classes.

Sanity Checks

As an aid for basic validation, some checks and ranges are imposed on SLHA input during initialization, as follows:
  • Several parameters (SLHA:keepSM, minMassSM, and SLHA:allowUserOverride) provide some safety against unintentionally overwriting PYTHIA's Standard-Model information. These parameters can be altered to hand over more or less control to the SLHA interface. In particular, a lot of mass and decay-table information may be included by default in some SLHA files, without it being the explicit intention of the user to overwrite the corresponding PYTHIA information. The default values of the SLHA safety parameters have been chosen so as to eliminate at least the most obvious causes of Garbage In Garbage Out. (E.g., there is usually no reason to modify the masses of well-measured SM particles, like the W and Z bosons, nor to replace their sophisticated internal decay treatments by the simplified isotropic treatment used for SLHA DECAY tables.)
  • For SLHA SUSY spectra, the interface checks the mass-ordering of the Higgs, Neutralino, and Chargino sectors, and the unitarity/orthogonality of the mixing matrices. It also performs some additional self-consistency checks on whether the correct SLHA BLOCKs for the given SUSY model have been included, and whether all required entries have been defined.
  • If MASS or DECAY information for a particle has been changed by SLHA input, the following sanity checks will be carried out. The particle will be declared stable unless there is at least one on-shell decay channel open (regardless of the presence of any DECAY information). In particular, massless particles will always be declared stable. A lower cutoff is imposed on the Breit-Wigner shape of the particle, requiring its mass to remain above the sum of masses for the lightest decay channel. Subject to that constraint, the lower cutoff will normally be placed at 5 times the width (so that the default gives a decent sampling of the shape), but the user is allowed to use the mMin parameter to choose a larger sampling range if so desired (still subject to the on-shell constraint).
  • For each decay channel in an SLHA DECAY table, PYTHIA will checks the available phase space. If the channel is on shell (sum of daughter masses is less than mass of decaying particle), then the threshold dependence is given by SLHA:meMode. If the channel is off shell, then an meMode of 100 is always used. As a further protection against GIGO, if the channel appears to be physically impossible (defined as requiring fluctuations of more than more than 100 times the effective combined widths), it is switched of and a warning message is printed.
  • DECAY table branching fractions are always interpreted as positive. However, a negative sign for one or more channels can be given, and will then be interpreted to mean that the corresponding channel(s) should be switched off for the current run. This furnishes a simple way to switch SLHA DECAY channels on and off while preserving the sum of branching fractions equal to unity.
Note that these sanity checks will not catch all possible cases of Garbage In Garbage Out, so human verification of the input files is always a good idea, as is taking a look at any warnings or error messages printed by the SLHA interface during initialization. It is ultimately up to the user to ensure that sensible input is being given.

SLHA Switches and Parameters

mode  SLHA:readFrom   (default = 1; minimum = 0; maximum = 2)
Controls from where SLHA information is read.
option 0 : is not read at all. Useful when SUSY is not simulated and normal particle properties should not be overwritten.
option 1 : read in from the <slha>...</slha> block of a LHEF, if such a file is read during initialization, and else from the SLHA:file below.
option 2 : read in from the SLHA:file below.

word  SLHA:file   (default = void)
Name of an SLHA (or LHEF) file containing the SUSY/BSM model definition, spectra, and (optionally) decay tables. Default void signals that no such file has been assigned.

flag  SLHA:keepSM   (default = on)
Some programs write SLHA output also for SM particles where normally one would not want to have masses and decay modes changed unwittingly. Therefore, by default, known SM particles are ignored in SLHA files. To be more specific, particle data for identity codes in the ranges 1 - 24 and 81 - 999,999 are ignored. Notably this includes Z^0, W^+- and t. The SM Higgs is modified by the SLHA input, as is other codes in the range 25 - 80 and 1,000,000 - . If you switch off this flag then also SM particles are modified by SLHA input.

parm  SLHA:minMassSM   (default = 100.0)
This parameter provides an alternative possibility to ignore SLHA input for all particles with identity codes below 1,000,000 (which mainly means SM particle, but also includes e.g. the Higgs bosons in two-Higgs-doublet scenarios) whose default masses in PYTHIA lie below some threshold value, given by this parameter. The default value of 100.0 allows SLHA input to modify the top quark, but not, e.g., the Z^0 and W^+- bosons.

flag  SLHA:allowUserOverride   (default = off)
Flag to set whether the user is allowed to modify the parameters read from an SLHA spectrum. Is normally kept off to preserve the internal self-consistency of SLHA spectra. If this flag is switched on, the mass values read from the SLHA block MASS are allowed to be modified by the user, using PYTHIA's standard readString and related methods.

SLHA DECAY Tables

In addition to SUSY spectra, the SLHA also defines a set of conventions for decay tables. These are not restricted to SUSY models, but can be used for arbitrary particles, either in combination with or independently of the SUSY parts of the Accord. The settings in this section control whether and how PYTHIA will make use of such tables. See also the comments under sanity checks above.
Note: the PYTHIA SLHA interface is limited to at most 1→8 decays.

flag  SLHA:useDecayTable   (default = on)
Switch to choose whether to read in SLHA DECAY tables or not. If this switch is set to off, PYTHIA will ignore any decay tables found in the SLHA file, and all decay widths will be calculated internally by PYTHIA. If switched on, SLHA decay tables will be read in, and will then supersede PYTHIA's internal calculations, with PYTHIA only computing the decays for particles for which no SLHA decay table is found. (To set a particle stable, you may either omit an SLHA DECAY table for it and then use PYTHIA's internal id:MayDecay switch for that particle, or you may include an SLHA DECAY table for it, with the width set explicitly to zero.)

mode  SLHA:meMode   (default = 100; minimum = 100; maximum = 103)
This value specifies how threshold, off-shell, and phase-space weighting effects for SLHA decay channels should be treated, using the same numbering scheme as for resonances. The default (100) is to use the branching fraction given in the SLHA DECAY tables without any modifications. The corresponding partial widths remain unchanged when the resonance fluctuates in mass. Specifically there are no threshold corrections. That is, if the resonance fluctuates down in mass, to below the nominal threshold for some decay mode, it is assumed that one of the daughters could also fluctuate down to keep the channel open. (If not, there may be problems later on.) Alternative options (with values 101+) documented under resonances allow for some flexibility to apply threshold factors expressing the closing of the on-shell phase space when the daughter masses approach or exceed the parent one. Note that modes that are extremely far off shell (defined as needing a fluctuation of more than 100 times the root-sum-square of the widths of the mother and daughter particles) will always be assigned meMode = 100 and should be switched off by hand if so desired. It is up to the user to ensure that the final behaviour is consistent with what is desired (and/or to apply suitable post facto reweightings). Plotting the generator-level resonance and decay-product mass distributions (and e.g., mass differences), effective branching fractions, etc, may be of assistance to validate the behaviour of the program.

Internal SLHA Variables

mode  SLHA:verbose   (default = 1; minimum = 0; maximum = 3)
Controls amount of text output written by the SLHA interface, with a value of 0 corresponding to the most quiet mode. The following variables are used internally by PYTHIA as local copies of SLHA information. User changes will generally have no effect, since these variables will be reset by the SLHA reader during initialization.

flag  SLHA:NMSSM   (default = off)
Corresponds to SLHA block MODSEL entry 3.

Using SLHA for generic BSM Models

Using the QNUMBERS extension [Alw07], the SLHA can also be used to define new particles, with arbitrary quantum numbers. This already serves as a useful way to introduce new particles and can be combined with MASS and DECAY tables in the usual way, to generate isotropically distributed decays or even chains of such decays. (If you want something better than isotropic, sorry, you'll have to do some actual work ...)

A more advanced further option is to make use of the possibility in the SLHA to include user-defined blocks with arbitrary names and contents. Obviously, standalone PYTHIA 8 does not know what to do with such information. However, it does not throw it away either, but instead stores the contents of user blocks as strings, which can be read back later, with the user having full control over the format used to read the individual entries.

The contents of both standard and user-defined SLHA blocks can be accessed in any class inheriting from PYTHIA 8's SigmaProcess class (i.e., in particular, from any semi-internal process written by a user), through its SLHA pointer, slhaPtr, by using the following methods:
bool slhaPtr->getEntry(string blockName, double& val);
bool slhaPtr->getEntry(string blockName, int indx, double& val);
bool slhaPtr->getEntry(string blockName, int indx, int jndx, double& val);
bool slhaPtr->getEntry(string blockName, int indx, int jndx, int kndx, double& val);

This particular example assumes that the user wants to read the entries (without index, indexed, matrix-indexed, or 3-tensor-indexed, respectively) in the user-defined block blockName, and that it should be interpreted as a double. The last argument is templated, and hence if anything other than a double is desired to be read, the user has only to give the last argument a different type. If anything went wrong (i.e., the block doesn't exist, or it doesn't have an entry with that index, or that entry can't be read as a double), the method returns false; true otherwise. This effectively allows to input completely arbitrary parameters using the SLHA machinery, with the user having full control over names and conventions. Of course, it is then the user's responsibility to ensure complete consistency between the names and conventions used in the SLHA input, and those assumed in any user-written semi-internal process code.

Note that PYTHIA 8 always initializes at least the SLHA blocks MASS and SMINPUTS, starting from its internal SM parameters and particle data table values (updated to take into account user modifications). These blocks can therefore be accessed using the slhaPtr->getEntry() methods even in the absence of SLHA input. Note: in the SMINPUTS block, PYTHIA outputs physically correct (i.e., measured) values of GF, m_Z, and alpha_EM(m_Z). However, if one attempts to compute, e.g., the W mass, at one loop from these quantities, a value of 79 GeV results, with a corresponding value for the weak mixing angle. We advise to instead take the physically measured W mass from block MASS, and recompute the EW parameters as best suited for the application at hand.

pythia8-8.1.80.orig/htmldoc/NLOMerging.html0000644000175000017500000012210612217615312016614 0ustar sunsun NLO Merging

NLO Merging

Pythia offers two NLO merging approaches. Both of these methods have been presented in [Lon13]. The goal of NLO merging is to extend tree-level multi-jet merging methods to next-to-leading order accuracy in QCD, for every available jet multiplicity. If for example NLO calculations for Higgs + 0 jet, Higgs + 1 jet and Higgs + 2 jets were available, NLO merging allows to simultaneously describe 0-, 1- and 2-jet observables with NLO accuracy. Further jets can, depending on additional tree-level input, be described by additional tree-level matrix elements. In the example, it would be possible to achieve NLO accuracy for 0-, 1- and 2-jet observables, tree-level accuracy for 3-, 4- and 5-jet configurations, and use the parton shower approximation for events with more than five jets.

The two NLO merging methods implemented in Pythia are called NL3 (for Nils Lavesson + Leif Lönnblad) and UNLOPS (for unitarised NLO+PS merging). Both of these schemes require Les Houches Event File input that is generated by tree-level or NLO matrix element generators. Currently, Pythia requires NLO input generated within the POWHEG framework. The generation of sensible input will be discussed below. The two NLO merging methods are illustrated in the sample main programs main87.cc (introducing NL3 ) and main88.cc (introducing UNLOPS). Before describing these programs, we would like to outline the differences between the two approaches.

NL3 is a generalisation of CKKW-L tree-level merging. The main idea of NL3 is to start from CKKW-L-reweighted multi-jet merging, and replace the αsn+0- and αsn+1-terms by the NLO result of POWHEG. This "replacement" means that we subtract the αsn+0- and αsn+1-terms from the CKKW-L-reweighted tree-level samples, and add another sample -- the POWHEG input. All "higher orders" are unchanged w.r.t. CKKW-L. We have implemented the "inclusive" scheme of [Lon13] in Pythia. This means that the POWHEG input will contain contributions for hard, resolved real emission jets, which are already taken care of by higher-multiplicity samples in CKKW-L. Thus, explicit phase space subtractions are also included. The sample program main87.cc, together with the input file main87.cmnd, illustrates the procedure.

UNLOPS is a generalisation of the UMEPS multi-jet merging scheme. Since UMEPS is already slightly more complicated than CKKW-L, this makes UNLOPS more complicated than NL3. The basic idea however remains the same: Start from a tree-level merging scheme (in this case UMEPS), remove all undesirable αsn+0- and αsn+1-terms from this result, and add back the "correct" description via POWHEG input samples. Again, since the "inclusive" scheme of [Lon13] was implemented in Pythia, it is necessary to handle explicit phase space subtractions. Similar to UMEPS, UNLOPS further ensures that the lowest-multiplicity cross section is given by the NLO result. This means that the UMEPS philosophy of "subtract what you add" needs to be extended to multi-leg NLO inputs.

UNLOPS is a theoretically more appealing definition of NLO merging than NL3, and should thus be considered the preferred choice. However, we believe it valuable to include both methods into Pythia, so that the variation of NLO merged results due to different NLO merging schemes can be studied in situ. Furthermore, NLO merging can be outlined more pedagogically when starting from NL3. The two NLO merging methods share parts of code with CKKW-L and UMEPS, and correspondingly share many input settings with these schemes. In particular,

         The hard process (Merging:Process) needs to be defined exactly as in CKKW-L (see Defining the hard process in the CKKW-L documentation).

         The merging scale value (Merging:TMS) has to be set.

         The maximal number of additional partons in tree-level events (Merging:nJetMax) has to be set.

All settings listed under the sections "Matrix element merging and HepMC output for RIVET" and "Further variables" in the CKKW-L documentation can be accessed in NLO merging as well. Furthermore, the Merging:nRecluster switch (see the UMEPS documentation) is important. Also, all MergingHooks routines that allow for user interference in CKKW-L merging are also usable for NLO merging -- with the exception of a user-defined merging scale. The NLO merging schemes currently implemented in Pythia do not allow for a merging scale definition that differs from the parton shower evolution variable. Since this merging scale definition is not completely obvious, the NLO merging schemes also share the Merging:enforceCutOnLHE switch with CKKW-L. In this way, it is possible to use LHE files that are regularised only with weak cuts as input, while the merging machinery imposes the stronger merging scale cut automatically. This means that no merging scale implementation is required from the user side, but also means that it is the user's responsibility to ensure that the cuts used for generating input LHE files are always looser than the cut given by the merging scale value Merging:TMS. This will lead to warnings of the form "Les Houches Event fails merging scale cut. Cut by rejecting event". These warning should rather be regarded as information. An example of inclusive matrix element generation cuts would be pTjet = 5 GeV, ΔRjetA jetB = 0.01 and QjetA jetB = 5 GeV, if NLO merging with a desired merging scale value of Merging:TMS = 15 is attempted for Higgs + jets events at the LHC.

In the following, we will first describe the generation of NLO input samples, and list input settings for NLO merging in Pythia. Then, we will examine the sample main programs main87.cc and main88.cc, which implement NL3 and UNLOPS merging, respectively.


Inputs for NLO merging

The NLO merging schemes in Pythia currently require Les Houches Event File input. To perform a merging with up to M additional partons described by tree-level matrix elements, and with up to N ≤ M-1 additional partons at NLO accuracy, the user needs to supply

         LHE files for 0... M additional partons, taken from a tree-level matrix element generator, and

         LHE files for 0... N additional partons, taken from a POWHEG NLO generator.

All input files need to be regularised, if they contain additional partons. Large files with fairly inclusive (i.e. loose) cuts are recommended. The input LHE files should further be generated with fixed renormalisation and factorisation scales. (In the POWHEG-BOX program, this means using the settings runningscales 0, btlscalereal 1, btlscalect 1, ckkwscalup 0. Some older processes in the POWHEG-BOX program need the input runningscale 0 instead of runningscales 0.)

When attempting NLO merging, the following Pythia settings are relevant.

mode  Merging:nJetMaxNLO   (default = 0; minimum = 0)
The maximal number of additional jets for which NLO event samples are supplied by the user.

parm  Merging:muFac   (default = -1.0)
The fixed factorisation scale used in the hard process cross section, as needed to generate the leading-order weight, in case the factorisation scale cannot be inferred from Les Houches event input. (This is the case for files that have been generated with the POWHEG-BOX program, since this program prints the transverse momentum scale of the real emission into the LH events.). If the value is not set, the SCALUP variable of the current LH event will be used instead. If wimpy showers (see Timelike Showers and Spacelike Showers) are used together with multi-jet merging, then this scale further sets the parton shower starting scale (μQ) for the core hard process.

parm  Merging:muRen   (default = -1.0)
The fixed renormalisation scale used in the hard process cross section, as needed to generate the leading-order weight, in case the renormalisation scale cannot be inferred from Les Houches event input. (As mentioned above, this is the case for files generated with the POWHEG-BOX program.) If the value is not set, the SCALUP variable of the current LH event will be used instead.

parm  Merging:muFacInME   (default = -1.0)
The fixed factorisation scale used in the matrix element calculation. This information is needed if factorisation scale variations in NLO merged results are attempted. Depending on the matrix element generator, it might not be possible to infer the factorisation scale from Les Houches event input, and thus, setting an explicit value is required. (As mentioned above, this is the case for files generated with the POWHEG-BOX program.) If the value is not set, the SCALUP variable of the current LH event will be used instead.

parm  Merging:muRenInME   (default = -1.0)
The fixed renormalisation scale used in the matrix element calculation. This information is needed if renormalisation scale variations in NLO merged results are attempted, for the same reason as factorisation scales might be required. (As mentioned above, this is the case for files generated with the POWHEG-BOX program.) If the value is not set, the SCALUP variable of the current LH event will be used instead.

All further settings will be discussed while examining the sample main programs.


NL3 merging with main87.cc

NL3-style NLO merging in Pythia is illustrated by the sample main program main87.cc. This program works together with an input file (e.g. main87.cmnd) for Pythia settings, and requires LHE input files that follow the naming convention name_tree_#nAdditionalJets.lhe (tree-level samples) and name_powheg_#nAdditionalJets.lhe (POWHEG NLO samples). main87.cc produces HepMC event output [Dob01], which can be used for analysis (e.g. using RIVET [Buc10]), or as input for detector simulations. For users not familiar with HepMC output, it is of course possible remove the HepMC code in the sample program, and use Pythia's histogramming routines instead. Histograms should then be filled as indicated for the histPTFirstSum histograms in main84.cc, i.e. using weightNLO*normhepmc.

If the user only wants to change the number of requested events (Main:numberOfEvents), the hard process (Merging:Process), the merging scale value (Merging:TMS) and the maximal number of additional tree-level or NLO-accuracte jets (Merging:nJetMax and Merging:nJetMaxNLO, respectively), and HepMC output is desired, then there is no need to change the main87.cc code. The input LHE files are also part of the (command line) input for main87.exe. The default settings in main87.cmnd are intended to work with the (very short) sample LHEF inputs (w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and w_production_powheg_0.lhe, w_production_powheg_1.lhe). For these input files, the main87.exe executable can be run with the command

./main87.exe main87.cmnd w_production myhepmc.hepmc

to produce a file myhepmc.hepmc of NLO merged HepMC event output. All mandatory Pythia input settngs have been outlined earlier. Please refrain from adding input switches than invoke any other merging scheme (e.g. e.g. Merging:doKTMerging) into the input file that you want to use in conjunction with main87.cc.

In the following, we will explain main87.cc in depth. Users who are willing to accept the default choices do not need to know all details, but are still encouraged to read further.

Program flow

main87.cc can be divided into four steps:

         1. Estimate the cross section for tree-level and NLO samples after the merging scale cut.

         2. Produce reweighted tree-level events, which do not contain αs0- and αs1-terms.

         3. Add POWHEG NLO events.

         4. Subtract phase space points with an extra (real-emission) jet above the merging scale from the POWHEG result, since such configurations have already been taken into account by processing other samples.

The first step is necessary to produce the correct weights for HepMC output events. The estimation of tree-level cross sections after the merging scale cut is generated by invoking the switch Merging:doXSectionEstimate together with Merging:doNL3Tree. In this configuration, the latter switch will only act to define the merging scale. After the tree-level cross sections have been estimated, main87.cc estimates the NLO cross sections after application of the merging scale cut, by inferring Merging:doXSectionEstimate together with Merging:doNL3Loop. Again, in this configuration, the latter switch only acts as the merging scale definition. When generating the estimates, all showering, multiparton interactions and hadronisation is turned off to not unnecessarily waste processor time. For all estimates, is further mandatory to set the value of Merging:nRequested to the jet multiplicity of the current event sample (e.g. to "2" for a sample containing W + 2 jet events). This is necessary in order to correctly apply the merging scale cut. POWHEG NLO input files for W + 1 jet e.g. contain W + 1 jet and W + 2 jet (i.e. real emission) kinematics. However, the merging scale cut aims at regularising the "underlying Born" configuration (i.e. the W + 1 states in our example). Setting Merging:nRequested = 1 for the W + 1 jet POWHEG sample ensures that even for real-emission (W + 2 jet) kinematics, the merging scale cut is applied to W + 1 jet states.

After the cross section estimation step, main87.cc proceeds to perform the actual merging. Before explaining this part, we would like to make some comments about K-factors.

main87.cc is prepared to use fixed K-factors to rescale the weight of tree-level events. This rescaling does not affect the NLO accuracy of the method, and was investigated in [Lon13]. By default, main87.cc does not use K-factors. However, if the user wants to include K-factors, this can be done by using the following input settings.

parm  Merging:kFactor0j   (default = 1.0)
The k-Factor used to rescale the tree-level (i.e. CKKW-L or UMEPS) part of zero-jet tree-level events.

parm  Merging:kFactor1j   (default = 1.0)
The k-Factor used to rescale the tree-level (i.e. CKKW-L or UMEPS) part of one-jet tree-level events.

parm  Merging:kFactor2j   (default = 1.0)
The k-Factor used to rescale the tree-level (i.e. CKKW-L or UMEPS) part of two-jet tree-level events.

If the variables k0, k1, k2 in main87.cc are set to non-unity values, K-factors will be applied. The K-factor of highest jet multiplicity will then be used to also rescale tree-level samples with a number of additional jets beyond the number of the highest-multiplicity real-emission sample. If we, for example, attempt an NLO merging of W+0 jet and W+1 jet at NLO accuracy, and with W+≤4 jets at tree-level accuracy, then Merging:kFactor2j is used to rescale the W+2 jet, W+3 jets and W+4 jets tree-level samples. We recommend to not include a K-factor rescaling of the tree-level samples.

Let us turn to the production of NLO merged events. The first step in the procedure is to generate reweighted tree-level samples. This is implemented by using the following switch.

flag  Merging:doNL3Tree   (default = off)
This switch will allow the generation of the weight that should be applied to tree-level events in the NL3 merging scheme. Please note that, in order for this to work smoothly, the switch Merging:doNL3Loop and the switch Merging:doNL3Subt have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

The weight of tree-level events can be accessed by calling the function double Info::mergingWeightNLO(). When printing (or histogramming) NLO merged events, this weight, multiplied with the estimated cross section of the current event sample, should be used as event weight (or weight of histogram bins). For Merging:doNL3Tree = on, the weight double Info::mergingWeightNLO() contains the CKKW-L weight, subtracted, if necessary, by αs0- and αs1-terms. This weight can become negative. As an example, imagine we attempt an NLO merging of W + 0 jet and W + 1 jet at NLO accuracy, and with W + 2 jets at tree-level accuracy. This weight will then be

  Info::mergingWeightNLO() = CKKW-L-weight for zero jets - αs0-terms - αs1-terms for events in the zero-jet sample,

  Info::mergingWeightNLO() = CKKW-L-weight for one jet - αs0-terms - αs1-terms for events in the one-jet sample, and

  Info::mergingWeightNLO() = CKKW-L-weight for two jets for events in the two-jet sample.

After the tree-level events have been reweighted, main87.cc will move on to process the POWHEG NLO input. This is done by switching to the following flag.

flag  Merging:doNL3Loop   (default = off)
This switch will allow the processing of POWHEG NLO events in the NL3 merging scheme. Please note that, in order for this to work smoothly, the switch Merging:doNL3Tree and the switch Merging:doNL3Subt have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

Also in this case, the NLO merging weight of the events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doNL3Loop = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in [Lon13]). After the processing of POWHEG NLO events, main87.cc continues by generating explicit phase space subtractions. This is facilitated by the following switch.

flag  Merging:doNL3Subt   (default = off)
This switch will allow the processing of tree-level events, to produce explicit phase space subtractions in the NL3 merging scheme. Please note that, in order for this to work smoothly, the switch Merging:doNL3Tree and the switch Merging:doNL3Loop have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested. Furthermore, it is necessary to set the value of Merging:nRecluster to one.

These contributions are necessary because we have implemented the "inclusive scheme" of [Lon13] in Pythia. The benefit of this scheme is the user does not have to intrusively change the POWHEG-BOX program to implement very particular cuts. Let us explain this comment with an example (a more detailed explanation of the idea is given in Appendix A.2 of [Lon13]). When generating W + 0 jet events with the POWHEG-BOX program, the output LHE files will contain W + 1 jet real emission events. Some of these events will contain a jet above the merging scale. However, in NLO merging methods, such configurations have already been included by a separate W + 1 jet sample. Thus, to avoid counting such events twice, we have to remove the configurations from the POWHEG-BOX output. We choose to remove such events by explicit subtraction.

As always, the NLO merging weight of the events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doNL3Subt = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in [Lon13]).

After these steps, all necessary events for NL3 merging have been produced. main87.cc finishes by returning the NL3-merged total cross section.


UNLOPS merging with main88.cc

UNLOPS-style NLO merging in Pythia is illustrated by the sample main program main88.cc, which relies on an input file (e.g. main88.cmnd) for Pythia settings. As for all merging methods in Pythia, main88.cc requires LHE input files. To use main88.cc without any changes, these input files should follow the naming convention name_tree_#nAdditionalJets.lhe (for tree-level samples) and name_powheg_#nAdditionalJets.lhe (for POWHEG NLO samples). main88.cc produces HepMC event output, which can e.g. be analysed with RIVET, or used as input for detector simulations. For users not familiar with HepMC output, it is of course possible remove the HepMC code in the sample program, and use Pythia's histogramming routines instead. Histograms should then be filled as indicated for the histPTFirstSum histograms in main84.cc, i.e. using weightNLO*normhepmc.

As for NL3, it is not necessary to change main88.cc if the user is only interested in changing standard settings. Thus, if the user only wants to change the number of requested events (Main:numberOfEvents), the hard process (Merging:Process), the merging scale value (Merging:TMS) and the maximal number of additional tree-level or NLO-accuracte jets (Merging:nJetMax and Merging:nJetMaxNLO, respectively), and HepMC output is desired, then there is no need to change the main88.cc code. The input LHE files are also part of the (command line) input for main88.exe. The default settings in main88.cmnd are intended to work with the (very short) sample LHEF inputs (w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and w_production_powheg_0.lhe, w_production_powheg_1.lhe). For these input files, the main88.exe executable can be run with the command

./main88.exe main88.cmnd w_production myhepmc.hepmc

to produce a file myhepmc.hepmc of UNLOPS merged HepMC event output. Please refrain from adding input switches than invoke any other merging scheme (e.g. Merging:doKTMerging) into the input file that you want to use in conjunction with main88.cc.

In the following, we will explain main88.cc in depth. To not be overly repetitive, we will at times refer to the relevant parts in the discussion of main87.cc. Users who are willing to accept the default choices do not need to know all details, but are still encouraged to read further.

Program flow

main88.cc can be divided into five steps:

         1. Estimate the cross section for tree-level and NLO samples after the merging scale cut.

         2. Produce reweighted tree-level events, which do not contain αs0- and αs1-terms.

         3. Add POWHEG NLO events.

         4. Subtract integrated, reweighted tree-level events, to ensure that the inclusive NLO cross section remains intact upon inclusion of multi-jet tree-level events.

         5. Subtract integrated POWHEG NLO events, to ensure that the inclusive NLO cross section remains intact upon inclusion of multi-jet tree-level events.

The estimation of cross sections after the application of the merging scale cut is nearly identical to the first step in main87.cc, and we refer to the first paragraph of the "Program flow" discussion for main87.cc for details. For main88.cc, the flags Merging:doUNLOPSTree or Merging:doUNLOPSLoop supply the merging scale definition used in the cross section estimation.

After the cross section estimation step, main88.cc proceeds to perform the actual NLO merging. The discussion of K-factors given in the NL3 section (i.e. of Merging:kFactor0j, Merging:kFactor1j and Merging:kFactor2j) also applies to main88.cc. Although UNLOPS is considerably more stable than NL3 upon changing the K-factors, we do not recommend the use of K-factors.

The production of UNLOPS-merged events with main88.cc starts by generating reweighted tree-level events. The processing of tree-level events can be invoked by setting the following flag.

flag  Merging:doUNLOPSTree   (default = off)
This switch will allow the generation of the weight that should be applied to tree-level events in the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSLoop, Merging:doUNLOPSSubt and Merging:doUNLOPSSubtNLO have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

The weight of tree-level events is returned by the function double Info::mergingWeightNLO(). When printing (or histogramming) NLO merged events, this weight, multiplied with the estimated cross section of the current event sample, should be used as event weight (or weight of histogram bins). For Merging:doUNLOPSTree = on, the weight double Info::mergingWeightNLO() contains the UMEPS weight, subtracted, if necessary, by αs0- and αs1-terms. This weight can become negative. As an example, assume that we attempt an UNLOPS merging of W + 0 jet and W + 1 jet at NLO accuracy, and with W + 2 jets at tree-level accuracy. This weight will then be

  Info::mergingWeightNLO() = UMEPS-weight for one jet - αs0-terms - αs1-terms for events in the one-jet sample, and

  Info::mergingWeightNLO() = UMEPS-weight for two jets for events in the two-jet sample.

After reweighted tree-level events have been generated, main88.cc processes the POWHEG NLO input files. This is facilitated by the following switch.

flag  Merging:doUNLOPSLoop   (default = off)
This switch will allow the processing of POWHEG NLO events in the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSTree, Merging:doUNLOPSSubt and Merging:doUNLOPSSubtNLO have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

The NLO merging weight of the events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doUNLOPSLoop = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in [Lon13]).

After processing the POWHEG NLO events, main88.cc continues by generating the reweighted subtraction terms of UMEPS. This part is implemented by setting the following flag.

flag  Merging:doUNLOPSSubt   (default = off)
This switch will allow the processing of tree-level events, to produce UMEPS subtraction terms for the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSTree, Merging:doUNLOPSLoop and Merging:doUNLOPSSubtNLO have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested. Furthermore, it is necessary to set the value of Merging:nRecluster to one.

By using this switch, main88.cc ensures that the inclusive cross section is preserved. At variance with UMEPS however, the event weight contains the UMEPS weight, subtracted, if necessary, by αs+0- and αs1-terms. Otherwise, αsn+0- and αsn+1-terms of the UMEPS procedure would be introduced, although our goal is to describe all αsn+0- and αsn+1-terms by n-jet POWHEG input. The weight of these integrated, subtractive tree-level events is, as always, returned by the function double Info::mergingWeightNLO(). When printing (or histogramming) NLO merged events, this weight, multiplied with the estimated cross section of the current event sample, and with -1, should be used as event weight (or weight of histogram bins). As for the case of tree-level events in UNLOPS, this weight can become negative. For the example given before, i.e. attempting an UNLOPS merging of W + 0 jet and W + 1 jet at NLO accuracy, and with W + 2 jets at tree-level accuracy, this weight will be

  Info::mergingWeightNLO() = UMEPS-weight for the integrated one-jet sample - αs0-terms - αs1-terms for events in the integrated one-jet sample, and

  Info::mergingWeightNLO() = UMEPS-weight for the integrated two-jet sample for events in the integrated two-jet sample.

This choice of weights already incorporates the fact that we have implemented the "inclusive scheme" of [Lon13], meaning that the "explicit phase space subtractions" of NL3 are (partially) included though these weights.

To ensure that the NLO inclusive cross section is unchanged, UNLOPS further requires the introduction of another sample. If POWHEG NLO events with one or more jets are included, it is necessary to subtract these samples in an integrated form. In main88.cc, this is done by setting the following flag.

flag  Merging:doUNLOPSSubtNLO   (default = off)
This switch will allow the processing of POWHEG NLO events, to produce NLO subtraction terms for the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSTree, Merging:doUNLOPSLoop and Merging:doUNLOPSSubt have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested. Furthermore, it is necessary to set the value of Merging:nRecluster to one.

This sample also provides some "explicit phase space subtractions" of NL3, which are necessary because we implemented the "inclusive scheme" of [Lon13]. Let us again look at the example of UNLOPS merging of W + 0 jet and W + 1 jet at NLO accuracy. The integrated W + 1 jet NLO events, which are produced by the setting Merging:doUNLOPSSubtNLO = on, contain a tree-level part. This part will exactly cancel the real-emission events with one jet above the merging scale in the W + 0 jet NLO events.

The NLO merging weight of these "integrated" events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doUNLOPSSubtNLO = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in [Lon13]).

After these five steps (estimation of cross sections, tree-level processing, POWHEG processing, integrated tree-level processing, integrated POWHEG processing) we have produced a UNLOPS-merged HepMC event file. main88.cc finishes by returning the UNLOPS-merged total cross section.


NLO merging and "exclusive" NLO inputs

Currently, both sample main programs for NLO merging (main87.cc and main88.cc) are intended for "inclusive" POWHEG input. Inclusive input means that all real emission phase space points are included in the POWHEG output files. In order to avoid double counting with higher-multiplicity matrix elements, it is then necessary remove phase space points with too many jets from the real-emission configurations. This can be done by introducing explicit phase space subtractions. Another way of removing the undesired configurations is by implementing a cut in the NLO generator. This is not a completely trivial task, since it is necessary to ensure numerical stability and the correct cancellation of (finite) dipole regularisation terms. One way of producing such exclusive NLO output is by setting the (tree-level) real-emission matrix element in the NLO generator to zero if the real-emission phase space point contains too many jets above the merging scale. This will however not be numerically stable for too low merging scale values.

We should be very clear that using exclusive NLO input is not recommended, since it requires hacking the NLO generator. Only for the expert user, we briefly summarise the necessary changes for using exclusive NLO input.

For the moment, assume that the NLO input has been produced in an "exclusive" way. This input can then be processed by some trivial changes in main87.cc: estimate the cross section for tree-level and NLO samples after the merging scale cut, still using inclusive NLO samples, remove the last part of main87.cc, i.e. the part that produces explicit phase space subtractions, and use the exclusive NLO files as input files for the processing of "POWHEG NLO files".

The changes to main88.cc (implementing UNLOPS) are slightly more complicated. This is the case because the weights of integrated tree-level samples change when using exclusive input, as can be seen in Appendix D in [Lon13]. The correct weights can be produced by Pythia by using the following flag.

flag  Merging:doUNLOPSTilde   (default = off)
This flag allows the UNLOPS machinery to produce the event weights if exclusive NLO input is used for the merging. This flag should be set to "on" directly after the cross section estimates have been produced.

Then, it is necessary to add code for processing another sample to main88.cc, since when using exclusive inputs, it is also necessary to enforce two integrations on tree-level events (the "↑"-contributions in Appendix D of [Lon13]). This can be achieved by adding the following code at the end of main88.cc.

  cout << endl << endl << endl;
  cout << "Shower subtractive events" << endl;

  // Switch on processing of counter-events.
  pythia.settings.flag("Merging:doUNLOPSTree",false);
  pythia.settings.flag("Merging:doUNLOPSLoop",false);
  pythia.settings.flag("Merging:doUNLOPSSubt",true);
  pythia.settings.flag("Merging:doUNLOPSSubtNLO",false);
  pythia.settings.mode("Merging:nRecluster",2);

  nMaxCT         = nMaxNLO+1;
  njetcounterCT  = nMaxCT;
  iPathSubt      = iPath + "_tree";

  while(njetcounterCT >= 2){

    // From njet, choose LHE file
    stringstream in;
    in   << "_" << njetcounterCT << ".lhe";
    string LHEfile = iPathSubt + in.str();

    cout << endl << endl << endl
         << "Start subtractive treatment for " << njetcounterCT << " jets\n"
         << "Recluster at least 2 times" << endl;

    pythia.readString("Beams:frameType = 4"); 
    pythia.settings.word("Beams:LHEF", LHEfile);  
    pythia.settings.mode("Merging:nRequested", njetcounterCT);
    pythia.init();
    // Remember position in vector of cross section estimates.
    int iNow = sizeLO-1-njetcounterCT;

    // Start generation loop
    for( int iEvent=0; iEvent < nEvent; ++iEvent ){

      // Generate next event
      if( !pythia.next() ) {
        if( pythia.info.atEndOfFile() ) break;
        else continue;
      }

      // Get event weight(s).
      double weightNLO  = pythia.info.mergingWeightNLO();
      double evtweight  = pythia.info.weight();
      weightNLO        *= evtweight;
      // Do not print zero-weight events.
      if ( weightNLO == 0. ) continue; 

      // Construct new empty HepMC event.
      HepMC::GenEvent* hepmcevt = new HepMC::GenEvent();
      // Get correct cross section from previous estimate.
      double normhepmc = -1*xsecLO[iNow] / nAcceptLO[iNow];
      // Set hepmc event weight.
      hepmcevt->weights().push_back(weightNLO*normhepmc);
      // Fill HepMC event.
      ToHepMC.fill_next_event( pythia, hepmcevt );
      // Add the weight of the current event to the cross section.
      sigmaTotal += weightNLO*normhepmc;
      errorTotal += pow2(weightNLO*normhepmc);
      // Report cross section to hepmc.
      HepMC::GenCrossSection xsec;
      xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 );
      hepmcevt->set_cross_section( xsec );
      // Write the HepMC event to file. Done with it.
      ascii_io << hepmcevt;
      delete hepmcevt;

    } // end loop over events to generate

    // print cross section, errors
    pythia.stat();

    // Restart with ME of a reduced the number of jets
    if( njetcounterCT > 2 )
      njetcounterCT--;
    else
      break;

  }
pythia8-8.1.80.orig/htmldoc/ParticleData.html0000644000175000017500000244376612217615312017234 0ustar sunsun Particle Data

Particle Data

The structure and operation of the particle data table is described here. That page also describes how default data properties can be changed. The current page provides the actual default values.

Main settings

Apart from the data itself, the particle data table only contains a few aspects that are available to change:

mode  ParticleData:modeBreitWigner   (default = 4; minimum = 0; maximum = 4)
Selection of particle masses when the mSel(id) is called to provide a new mass:
option 0 : mass is fixed at the nominal m_0 value.
option 1 : particles registered as having a mass width are given a mass in the range m_min < m < m_max, according to a truncated nonrelativistic Breit-Wigner, i.e. linear in m.
option 2 : as above, except that the width is made mass-dependent: Gamma = Gamma_0 * sqrt( (m^2 - m_thr^2) / (m_0^2 - m_thr^2) ) where m is the current mass, m_0 the nominal one and m_thr is the mass threshold, given by the sum of the nominal masses of the decay products. In order to decouple production and decay the threshold is defined as the branching-ratio-weighted average over all allowed decay channels.
option 3 : particles registered as having a mass width are given a mass in the range m_min < m < m_max, according to a truncated relativistic Breit-Wigner, i.e. quadratic in m.
option 4 : as 3, but the width is modified as for 2, and the current mass is used for its phase-space prefactor, i.e. m_0 Gamma_0 -> m Gamma(m).
Note: this mode only applies to normal hadronic resonances like the rho. The more massive states of the isResonance() type, like Z^0 or top, are considered separately.

parm  ParticleData:maxEnhanceBW   (default = 2.5; minimum = 1.; maximum = 5.)
The modifications in options 2 and 4 above enhance the large-mass tail of the Breit-Wigner distributions (the mass spectrum develops a dm/m divergence). However, we expect form factors to dampen this tail at masses some distance above the nominal one, so cut off the rise by requiring the actual Breit-Wigner weight not to be more than a factor maxEnhanceBW above the one obtained with options 1 or 3, respectively. This also opens up for a simpler technical handling of mass selection in options 2 and 4, by using standard hit-and-miss Monte Carlo.

Since running masses are only calculated for the six quark flavours, e.g. to obtain couplings to the Higgs boson(s), there is not an entry in the normal tables for each particles, but only the six MSbar mass values below, used as starting point for the running. In addition you can pick an alpha_s(M_Z), which is converted into a first-order five-flavour Lambda that is used to determine the rate of the running. (Without any match to four flavours below m_b; if desired, this can be fixed by slightly shifted default mass values, since the routines never should be called below the m_b scale anyway.)

parm  ParticleData:mdRun   (default = 0.006; minimum = 0.003; maximum = 0.008)
the d quark MSbar mass at 2 GeV scale.

parm  ParticleData:muRun   (default = 0.003; minimum = 0.001; maximum = 0.006)
the u quark MSbar mass at 2 GeV scale.

parm  ParticleData:msRun   (default = 0.095; minimum = 0.060; maximum = 0.150)
the s quark MSbar mass at 2 GeV scale.

parm  ParticleData:mcRun   (default = 1.25; minimum = 1.00; maximum = 1.50)
the c quark MSbar mass at the mass scale itself.

parm  ParticleData:mbRun   (default = 4.20; minimum = 4.00; maximum = 4.50)
the b quark MSbar mass at the mass scale itself.

parm  ParticleData:mtRun   (default = 165.0; minimum = 150.0; maximum = 175.0)
the t quark MSbar mass at the mass scale itself.

parm  ParticleData:alphaSvalueMRun   (default = 0.125; minimum = 0.10; maximum = 0.20)
the alpha_s(M_Z) value used to define the rate at which MSbar masses run.

Comments on the data

Much of the current data has been updated based on the 2012 Review of Particle Physics [Ber12], while some is still based on the 2006 RPP [Yao06]. All known particle masses, widths and lifetimes have been set accordingly, while most not-yet-measured particles are kept at their values from PYTHIA 6. Decay channels and their branching ratios remain a major worry: many particles do not have one single solidly measured branching ratio, and many further do not have known branching ratios that add up to (the neighbourhood of) unity.

Uncertainties are especially big for the scalar, pseudovector and tensor L = 1 multiplets available in PYTHIA. We note that some distributions become better described when these multiplets are included in the generation, while others become worse. It is tempting to associate this lackluster performance with the primitive knowledge. Not even the multiplets themselves are particularly well known. It used to be that the a_0(980) and f_0(980) were considered to be members of the scalar multiplet. Nowadays they are commonly assumed to be either four-quark states or of some other exotic character. This means that the PYTHIA 8 PDG particle codes have been changed for these particles, relative to what was used in PYTHIA 6 based on previous PDG editions. Specifically their numbers are now in the 9000000 series, and they have been replaced in the scalar multiplet by a_0(1450) and f_0(1370).

For charm and bottom mesons the jungle of partial measurements makes it very difficult to construct fully consistent sets of decay channels. This part of the program has not yet been brought up to date to the 2006 RPP. Instead the LHCb decay tables (for EvtGen, but without using the EvtGen matrix-element machinery) and the DELPHI tune for PYTHIA 6 is being used. (This also includes a few non-c/b hadrons that only occur in the c/b decay tables.) This has the advantage that many tests have been made for consistency, but the disadvantage that it is not always in agreement with the latest measurements of some specific decay channels. The decays based on the LHCb tables (with some modifications) are 411, 421, 431, 441, 445, 511, 521, 531, 541, 3124, 4122, 4124, 5122, 10441, 10443, 13122, 14122, 20443, 23122, 30313, 30323, 30443, 33122, 100113, 100213, 100441, 100443, 100553, 9000111, 9000211. Correspondingly the decays based on the DELPHI tables are 415, 425, 435, 515, 525, 535, 4132, 4232, 4332, 5132, 5232 and 5332.

The data itself

Here comes the default particle data used in the program. Do not touch. The meaning of the various properties and the format used are explained here and the meMode codes here.

particle: id="0" name="void" spinType="0" chargeType="0" colType="0" m0="0.00000"

particle: id="1" name="d" antiName="dbar" spinType="2" chargeType="-1" colType="1" m0="0.33000"

particle: id="2" name="u" antiName="ubar" spinType="2" chargeType="2" colType="1" m0="0.33000"

particle: id="3" name="s" antiName="sbar" spinType="2" chargeType="-1" colType="1" m0="0.50000"

particle: id="4" name="c" antiName="cbar" spinType="2" chargeType="2" colType="1" m0="1.50000"

particle: id="5" name="b" antiName="bbar" spinType="2" chargeType="-1" colType="1" m0="4.80000"

particle: id="6" name="t" antiName="tbar" spinType="2" chargeType="2" colType="1" m0="171.00000" mWidth="1.40000" mMin="86.00000" mMax="0.00000"
channel: onMode="1" bRatio="0.0000300" products="24 1"
channel: onMode="1" bRatio="0.0017650" products="24 3"
channel: onMode="1" bRatio="0.9982050" products="24 5"
channel: onMode="0" bRatio="0.0000000" products="37 5"

particle: id="7" name="b'" antiName="b'bar" spinType="2" chargeType="-1" colType="1" m0="400.00000"
channel: onMode="1" bRatio="0.0000000" products="-24 2"
channel: onMode="1" bRatio="0.0000000" products="-24 4"
channel: onMode="1" bRatio="0.0000000" products="-24 6"
channel: onMode="1" bRatio="1.0000000" products="-24 8"

particle: id="8" name="t'" antiName="t'bar" spinType="2" chargeType="2" colType="1" m0="400.00000"
channel: onMode="1" bRatio="0.0000000" products="24 1"
channel: onMode="1" bRatio="0.0000000" products="24 3"
channel: onMode="1" bRatio="0.0000000" products="24 5"
channel: onMode="1" bRatio="1.0000000" products="24 7"

particle: id="11" name="e-" antiName="e+" spinType="2" chargeType="-3" colType="0" m0="5.110e-04"

particle: id="12" name="nu_e" antiName="nu_ebar" spinType="2" chargeType="0" colType="0" m0="0.00000"

particle: id="13" name="mu-" antiName="mu+" spinType="2" chargeType="-3" colType="0" m0="0.10566" tau0="6.58654e+05"
channel: onMode="1" bRatio="1.0000000" meMode="22" products="-12 11 14"

particle: id="14" name="nu_mu" antiName="nu_mubar" spinType="2" chargeType="0" colType="0" m0="0.00000"

particle: id="15" name="tau-" antiName="tau+" spinType="2" chargeType="-3" colType="0" m0="1.77682" tau0="8.71100e-02"
channel: onMode="1" bRatio="0.1076825" meMode="1521" products="16 -211"
channel: onMode="1" bRatio="0.0069601" meMode="1521" products="16 -321"
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channel: onMode="1" bRatio="0.0001631" meMode="0" products="16 -211 -211 211 221"
channel: onMode="1" bRatio="0.0001491" meMode="0" products="16 111 111 -211 221"
channel: onMode="1" bRatio="0.0001392" meMode="0" products="16 111 111 -211 223"
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channel: onMode="1" bRatio="0.0004077" meMode="0" products="16 223 -321"
channel: onMode="1" bRatio="0.0004773" meMode="0" products="16 111 111 111 -321"
channel: onMode="1" bRatio="0.0003052" meMode="0" products="16 111 -211 211 -321"
channel: onMode="1" bRatio="0.0002784" meMode="0" products="16 221 -323"
channel: onMode="1" bRatio="0.0002366" meMode="0" products="16 111 111 -211 -311"
channel: onMode="1" bRatio="0.0002237" meMode="0" products="16 -211 -211 211 -311"
channel: onMode="1" bRatio="0.0002953" meMode="0" products="16 111 -211 -311 311"
channel: onMode="1" bRatio="0.0000590" meMode="0" products="16 111 -211 -321 321"

particle: id="16" name="nu_tau" antiName="nu_taubar" spinType="2" chargeType="0" colType="0" m0="0.00000"

particle: id="17" name="tau'-" antiName="tau'+" spinType="2" chargeType="-3" colType="0" m0="400.00000"
channel: onMode="1" bRatio="1.0000000" products="-24 18"

particle: id="18" name="nu'_tau" antiName="nu'_taubar" spinType="2" chargeType="0" colType="0" m0="400.00000"
channel: onMode="1" bRatio="1.0000000" products="24 17"

particle: id="21" name="g" spinType="3" chargeType="0" colType="2" m0="0.00000"

particle: id="22" name="gamma" spinType="3" chargeType="0" colType="0" m0="0.00000"

particle: id="23" name="Z0" spinType="3" chargeType="0" colType="0" m0="91.18760" mWidth="2.49520" mMin="10.00000" mMax="0.00000"
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channel: onMode="1" bRatio="0.1539840" products="3 -3"
channel: onMode="1" bRatio="0.1192590" products="4 -4"
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channel: onMode="1" bRatio="0.0668060" products="12 -12"
channel: onMode="1" bRatio="0.0335760" products="13 -13"
channel: onMode="1" bRatio="0.0668060" products="14 -14"
channel: onMode="1" bRatio="0.0335000" products="15 -15"
channel: onMode="1" bRatio="0.0668060" products="16 -16"

particle: id="24" name="W+" antiName="W-" spinType="3" chargeType="3" colType="0" m0="80.38500" mWidth="2.08500" mMin="10.00000" mMax="0.00000"
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channel: onMode="1" bRatio="0.0165020" products="-3 2"
channel: onMode="1" bRatio="0.3206150" products="-3 4"
channel: onMode="1" bRatio="0.0000100" products="-5 2"
channel: onMode="1" bRatio="0.0005910" products="-5 4"
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channel: onMode="1" bRatio="0.1081660" products="-13 14"
channel: onMode="1" bRatio="0.1080870" products="-15 16"

particle: id="25" name="h0(H_1)" spinType="1" chargeType="0" colType="0" m0="125.00000" mWidth="0.00374" mMin="50.00000" mMax="0.00000"
channel: onMode="1" bRatio="0.0000009" products="1 -1"
channel: onMode="1" bRatio="0.0000002" products="2 -2"
channel: onMode="1" bRatio="0.0002361" products="3 -3"
channel: onMode="1" bRatio="0.0335602" products="4 -4"
channel: onMode="1" bRatio="0.5876728" products="5 -5"
channel: onMode="1" bRatio="0.0000000" products="6 -6"
channel: onMode="1" bRatio="0.0000000" products="11 -11"
channel: onMode="1" bRatio="0.0002445" products="13 -13"
channel: onMode="1" bRatio="0.0690800" products="15 -15"
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channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000002 2000002"
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channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000004 -2000004"
channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000004 2000004"
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channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000005 -2000005"
channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000005 -2000005"
channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000005 2000005"
channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000006 -1000006"
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channel: onMode="1" bRatio="1.0000000" products="553 21" pythia8-8.1.80.orig/htmldoc/MultipartonInteractions.html0000644000175000017500000007213412217615311021560 0ustar sunsun Multiparton Interactions

Multiparton Interactions

The starting point for the multiparton interactions physics scenario in PYTHIA is provided by [Sjo87]. Recent developments have included a more careful study of flavour and colour correlations, junction topologies and the relationship to beam remnants [Sjo04], interleaving with initial-state radiation [Sjo05], making use of transverse-momentum-ordered initial- and final-state showers, with the extension to fully interleaved evolution covered in [Cor10a]. A framework to handle rescattering is described in [Cor09].

A big unsolved issue is how the colour of all these subsystems is correlated. For sure there is a correlation coming from the colour singlet nature of the incoming beams, but in addition final-state colour rearrangements may change the picture. Indeed such extra effects appear necessary to describe data, e.g. on <pT>(n_ch). A simple implementation of colour rearrangement is found as part of the beam remnants description.

Main variables

Matching to hard process

The maximum pT to be allowed for multiparton interactions is related to the nature of the hard process itself. It involves a delicate balance between not double-counting and not leaving any gaps in the coverage. The best procedure may depend on information only the user has: how the events were generated and mixed (e.g. with Les Houches Accord external input), and how they are intended to be used. Therefore a few options are available, with a sensible default behaviour.

mode  MultipartonInteractions:pTmaxMatch   (default = 0; minimum = 0; maximum = 2)
Way in which the maximum scale for multiparton interactions is set to match the scale of the hard process itself.
option 0 : (i) if the final state of the hard process (not counting subsequent resonance decays) contains only quarks (u, d, s, c, b), gluons and photons then pT_max is chosen to be the factorization scale for internal processes and the scale value for Les Houches input; (ii) if not, interactions are allowed to go all the way up to the kinematical limit. The reasoning is that the former kind of processes are generated by the multiparton-interactions machinery and so would double-count hard processes if allowed to overlap the same pT range, while no such danger exists in the latter case.
option 1 : always use the factorization scale for an internal process and the scale value for Les Houches input, i.e. the lower value. This should avoid double-counting, but may leave out some interactions that ought to have been simulated.
option 2 : always allow multiparton interactions up to the kinematical limit. This will simulate all possible event topologies, but may lead to double-counting.
Note: If a "second hard" process is present, the two are analyzed separately for the default 0 option. It is enough that one of them only consists of quarks, gluons and photons to restrict the pT range. The maximum for MPI is then set by the hard interaction with lowest scale.

Cross-section parameters

The rate of interactions is determined by

parm  MultipartonInteractions:alphaSvalue   (default = 0.127; minimum = 0.06; maximum = 0.25)
The value of alpha_strong at m_Z. Default value is picked equal to the one used in CTEQ 5L.

The actual value is then regulated by the running to the scale pT^2, at which it is evaluated

mode  MultipartonInteractions:alphaSorder   (default = 1; minimum = 0; maximum = 2)
The order at which alpha_strong runs at scales away from m_Z.
option 0 : zeroth order, i.e. alpha_strong is kept fixed.
option 1 : first order, which is the normal value.
option 2 : second order. Since other parts of the code do not go to second order there is no strong reason to use this option, but there is also nothing wrong with it.

QED interactions are regulated by the alpha_electromagnetic value at the pT^2 scale of an interaction.

mode  MultipartonInteractions:alphaEMorder   (default = 1; minimum = -1; maximum = 1)
The running of alpha_em used in hard processes.
option 1 : first-order running, constrained to agree with StandardModel:alphaEMmZ at the Z^0 mass.
option 0 : zeroth order, i.e. alpha_em is kept fixed at its value at vanishing momentum transfer.
option -1 : zeroth order, i.e. alpha_em is kept fixed, but at StandardModel:alphaEMmZ, i.e. its value at the Z^0 mass.

Note that the choices of alpha_strong and alpha_em made here override the ones implemented in the normal process machinery, but only for the interactions generated by the MultipartonInteractions class.

In addition there is the possibility of a global rescaling of cross sections (which could not easily be accommodated by a changed alpha_strong, since alpha_strong runs)

parm  MultipartonInteractions:Kfactor   (default = 1.0; minimum = 0.5; maximum = 4.0)
Multiply all cross sections by this fix factor.

The processes used to generate multiparton interactions form a subset of the standard library of hard processes. The input is slightly different from the standard hard-process machinery, however, since incoming flavours, the alpha_strong value and most of the kinematics are already fixed when the process is called. It is possible to regulate the set of processes that are included in the multiparton-interactions framework.

mode  MultipartonInteractions:processLevel   (default = 3; minimum = 0; maximum = 3)
Set of processes included in the machinery.
option 0 : only the simplest 2 -> 2 QCD processes between quarks and gluons, giving no new flavours, i.e. dominated by t-channel gluon exchange.
option 1 : also 2 -> 2 QCD processes giving new flavours (including charm and bottom), i.e. proceeding through s-channel gluon exchange.
option 2 : also 2 -> 2 processes involving one or two photons in the final state, s-channel gamma boson exchange and t-channel gamma/Z^0/W^+- boson exchange.
option 3 : also charmonium and bottomonium production, via colour singlet and colour octet channels.

Cross-section regularization

There are two complementary ways of regularizing the small-pT divergence, a sharp cutoff and a smooth dampening. These can be combined as desired, but it makes sense to coordinate with how the same issue is handled in spacelike showers. Actually, by default, the parameters defined here are used also for the spacelike showers, but this can be overridden.

Regularization of the divergence of the QCD cross section for pT -> 0 is obtained by a factor pT^4 / (pT0^2 + pT^2)^2, and by using an alpha_s(pT0^2 + pT^2). An energy dependence of the pT0 choice is introduced by two further parameters, so that pT0Ref is the pT0 value for the reference CM energy, pT0Ref = pT0(ecmRef).
Warning: if a large pT0 is picked for multiparton interactions, such that the integrated interaction cross section is below the nondiffractive inelastic one, this pT0 will automatically be scaled down to cope.

The actual pT0 parameter used at a given CM energy scale, ecmNow, is obtained as
pT0 = pT0(ecmNow) = pT0Ref * (ecmNow / ecmRef)^ecmPow
where pT0Ref, ecmRef and ecmPow are the three parameters below.

parm  MultipartonInteractions:pT0Ref   (default = 2.15; minimum = 0.5; maximum = 10.0)
The pT0Ref scale in the above formula.
Note: pT0Ref is one of the key parameters in a complete PYTHIA tune. Its value is intimately tied to a number of other choices, such as that of colour flow description, so unfortunately it is difficult to give an independent meaning to pT0Ref.

parm  MultipartonInteractions:ecmRef   (default = 1800.0; minimum = 1.)
The ecmRef reference energy scale introduced above.

parm  MultipartonInteractions:ecmPow   (default = 0.24; minimum = 0.0; maximum = 0.5)
The ecmPow energy rescaling pace introduced above.

Alternatively, or in combination, a sharp cut can be used.

parm  MultipartonInteractions:pTmin   (default = 0.2; minimum = 0.1; maximum = 10.0)
Lower cutoff in pT, below which no further interactions are allowed. Normally pT0 above would be used to provide the main regularization of the cross section for pT -> 0, in which case pTmin is used mainly for technical reasons. It is possible, however, to set pT0Ref = 0 and use pTmin to provide a step-function regularization, or to combine them in intermediate approaches. Currently pTmin is taken to be energy-independent.

Gösta Gustafson has proposed (private communication, unpublished) that the amount of screening, as encapsulated in the pT0 parameter, fluctuates from one event to the next. Specifically, high-activity event are more likely to lead to interactions at large pT scales, but the high activity simultaneously leads to a larger screening of interactions at smaller pT. Such a scenario can approximately be simulated by scaling up the pT0 by a factor sqrt(n), where n is the number of interactions considered so far, including the current one. That is, for the first interaction the dampening factor is pT^4 / (pT0^2 + pT^2)^2, for the second pT^4 / (2 pT0^2 + pT^2)^2, for the third pT^4 / (3 pT0^2 + pT^2)^2, and so on. Optionally the scheme may also be applied to ISR emissions. For simplicity the same alpha_s(pT0^2 + pT^2) is used throughout. Note that, in this scenario the pT0 scale must be lower than in the normal case to begin with, since it later is increased back up. Also note that the idea with this scenario is to propose an alternative to colour reconnection to understand the rise of <pT>(n_ch), so that the amount of colour reconnection should be reduced.

mode  MultipartonInteractions:enhanceScreening   (default = 0; minimum = 0; maximum = 2)
Choice to activate the above screening scenario, i.e. an increasing effective pT0 for consecutive interactions.
option 0 : No activity-dependent screening, i.e. pT0 is fixed.
option 1 : The pT0 scale is increased as a function of the number of MPI's, as explained above. ISR is not affected, but note that, if SpaceShower:samePTasMPI is on, then MultipartonInteractions:pT0Ref is used also for ISR, which may or may not be desirable.
option 2 : Both MPI and ISR influence and are influenced by the screening. That is, the dampening is reduced based on the total number of MPI and ISR steps considered so far, including the current one. This dampening is implemented both for MPI and for ISR emissions, for the latter provided that SpaceShower:samePTasMPI is on (default).

Impact-parameter dependence

The choice of impact-parameter dependence is regulated by several parameters. The ones listed here refer to nondiffractive topologies only, while their equivalents for diffractive events are put in the Diffraction description. Note that there is currently no bProfile = 4 option for diffraction. Other parameters are assumed to agree between diffractive and nondiffractive topologies.

mode  MultipartonInteractions:bProfile   (default = 1; minimum = 0; maximum = 4)
Choice of impact parameter profile for the incoming hadron beams.
option 0 : no impact parameter dependence at all.
option 1 : a simple Gaussian matter distribution; no free parameters.
option 2 : a double Gaussian matter distribution, with the two free parameters coreRadius and coreFraction.
option 3 : an overlap function, i.e. the convolution of the matter distributions of the two incoming hadrons, of the form exp(- b^expPow), where expPow is a free parameter.
option 4 : a Gaussian matter distribution with a width that varies according to the selected x value of an interaction, 1. + a1 log (1 / x), where a1 is a free parameter. Note that once b has been selected for the hard process, it remains fixed for the remainder of the evolution.

parm  MultipartonInteractions:coreRadius   (default = 0.4; minimum = 0.1; maximum = 1.)
When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a radius that is a factor coreRadius smaller than the rest.

parm  MultipartonInteractions:coreFraction   (default = 0.5; minimum = 0.; maximum = 1.)
When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a fraction coreFraction of the matter content of the hadron.

parm  MultipartonInteractions:expPow   (default = 1.; minimum = 0.4; maximum = 10.)
When bProfile = 3 it gives the power of the assumed overlap shape exp(- b^expPow). Default corresponds to a simple exponential drop, which is not too dissimilar from the overlap obtained with the standard double Gaussian parameters. For expPow = 2 we reduce to the simple Gaussian, bProfile = 1, and for expPow -> infinity to no impact parameter dependence at all, bProfile = 0. For small expPow the program becomes slow and unstable, so the min limit must be respected.

parm  MultipartonInteractions:a1   (default = 0.15; minimum = 0.; maximum = 2.)
When bProfile = 4, this gives the a1 constant in the Gaussian width. When a1 = 0., this reduces back to the single Gaussian case.

mode  MultipartonInteractions:bSelScale   (default = 1; minimum = 1; maximum = 3)
The selection of impact parameter is related to the scale of the hard process: the harder this scale is, the more central the collision. In practice this centrality saturates quickly, however, and beyond a scale of roughly 20 GeV very little changes. (The relevant quantity is that the QCD jet cross section above the scale should be a tiny fraction of the total cross section.) In 2 -> 1 and 2 -> 2 processes traditional scale choices work fine, but ambiguities arise for higher multiplicities, in particular when the scale is used for matching between the multiparton matrix elements and parton showers. Then the event scale may be chosen as that of a very low-pT parton, i.e. suggesting a peripheral collision, while the much harder other partons instead would favour a central collision. Therefore the default here is to override whatever scale value have been read in from an LHEF, say. Notice that the scale used here is decoupled from the maximum scale for MPIs (MultipartonInteractions:pTmaxMatch).
option 1 : Use the mass for a 2 -> 1 process. For 2 -> n, n > 1 processes order the particles in falling mmT = m + mT and then let the scale be (mmT_1 + mmT_2)/2 + mmT_3/3 + mmT_4/4 + ... + mmT_n/n. This is constructed always to be above m1, and to assign decreasing importance to softer particles that are less likely to be associated with the hard process.
option 2 : Use the scale parameter of the event.
option 3 : use the same scale as chosen by the rules for MultipartonInteractions:pTmaxMatch.

Rescattering

It is possible that a parton may rescatter, i.e. undergo a further interaction subsequent to the first one. The machinery to model this kind of physics has only recently become fully operational [Cor09], and is therefore not yet so well explored.

The rescattering framework has ties with other parts of the program, notably with the beam remnants.

flag  MultipartonInteractions:allowRescatter   (default = off)
Switch to allow rescattering of partons; on/off = true/false.
Note: the rescattering framework has not yet been implemented for the MultipartonInteractions:bProfile = 4 option, and can therefore not be switched on in that case. Warning: use with caution since machinery is still not so well tested.

flag  MultipartonInteractions:allowDoubleRescatter   (default = off)
Switch to allow rescattering of partons, where both incoming partons have already rescattered; on/off = true/false. Is only used if MultipartonInteractions:allowRescatter is switched on.
Warning: currently there is no complete implementation that combines it with shower evolution, so you must use PartonLevel:ISR = off and PartonLevel:FSR = off. If not, a warning will be issued and double rescattering will not be simulated. The rate also comes out to be much lower than for single rescattering, so to first approximation it can be neglected.

mode  MultipartonInteractions:rescatterMode   (default = 0; minimum = 0; maximum = 4)
Selection of which partons rescatter against unscattered partons from the incoming beams A and B, based on their rapidity value y in the collision rest frame. Here ySep is shorthand for MultipartonInteractions:ySepRescatter and deltaY for MultipartonInteractions:deltaYRescatter, defined below. The description is symmetric between the two beams, so only one case is described below.
option 0 : only scattered partons with y > 0 can collide with unscattered partons from beam B.
option 1 : only scattered partons with y > ySep can collide with unscattered partons from beam B.
option 2 : the probability for a scattered parton to be considered as a potential rescatterer against unscattered partons in beam B increases linearly from zero at y = ySep - deltaY to unity at y = ySep + deltaY.
option 3 : the probability for a scattered parton to be considered as a potential rescatterer against unscattered partons in beam B increases with y according to (1/2) * (1 + tanh( (y - ySep) / deltaY)).
option 4 : all partons are potential rescatterers against both beams.

parm  MultipartonInteractions:ySepRescatter   (default = 0.)
used for some of the MultipartonInteractions:rescatterMode options above, as the rapidity for which a scattered parton has a 50% probability to be considered as a potential rescatterer. A ySep > 0 generally implies that some central partons cannot rescatter at all, while a ySep < 0 instead allows central partons to scatter against either beam.

parm  MultipartonInteractions:deltaYRescatter   (default = 1.; minimum = 0.1)
used for some of the MultipartonInteractions:rescatterMode options above, as the width of the rapidity transition region, where the probability rises from zero to unity that a scattered parton is considered as a potential rescatterer.

Further variables

These should normally not be touched. Their only function is for cross-checks.

mode  MultipartonInteractions:nQuarkIn   (default = 5; minimum = 0; maximum = 5)
Number of allowed incoming quark flavours in the beams; a change to 4 would thus exclude b and bbar as incoming partons, etc.

mode  MultipartonInteractions:nSample   (default = 1000; minimum = 100)
The allowed pT range is split (unevenly) into 100 bins, and in each of these the interaction cross section is evaluated in nSample random phase space points. The full integral is used at initialization, and the differential one during the run as a "Sudakov form factor" for the choice of the hardest interaction. A larger number implies increased accuracy of the calculations.

Technical notes

Relative to the articles mentioned above, not much has happened. The main news is a technical one, that the phase space of the 2 -> 2 (massless) QCD processes is now sampled in dy_3 dy_4 dpT^2, where y_3 and y_4 are the rapidities of the two produced partons. One can show that
(dx_1 / x_1) * (dx_2 / x_2) * d(tHat) = dy_3 * dy_4 * dpT^2
Furthermore, since cross sections are dominated by the "Rutherford" one of t-channel gluon exchange, which is enhanced by a factor of 9/4 for each incoming gluon, effective structure functions are defined as
F(x, pT2) = (9/4) * xg(x, pT2) + sum_i xq_i(x, pT2)
With this technical shift of factors 9/4 from cross sections to parton densities, a common upper estimate of
d(sigmaHat)/d(pT2) < pi * alpha_strong^2 / pT^4
is obtained.

In fact this estimate can be reduced by a factor of 1/2 for the following reason: for any configuration (y_3, y_4, pT2) also one with (y_4, y_3, pT2) lies in the phase space. Not both of those can enjoy being enhanced by the tHat -> 0 singularity of
d(sigmaHat) propto 1/tHat^2.
Or if they are, which is possible with identical partons like q q -> q q and g g -> g g, each singularity comes with half the strength. So, when integrating/averaging over the two configurations, the estimated d(sigmaHat)/d(pT2) drops. Actually, it drops even further, since the naive estimate above is based on
(4 /9) * (1 + (uHat/sHat)^2) < 8/9 < 1
The 8/9 value would be approached for tHat -> 0, which implies sHat >> pT2 and thus a heavy parton-distribution penalty, while parton distributions are largest for tHat = uHat = -sHat/2, where the above expression evaluates to 5/9. A fudge factor is therefore introduced to go the final step, so it can easily be modified when further non-Rutherford processes are added, or should parton distributions change significantly.

At initialization, it is assumed that
d(sigma)/d(pT2) < d(sigmaHat)/d(pT2) * F(x_T, pT2) * F(x_T, pT2) * (2 y_max(pT))^2
where the first factor is the upper estimate as above, the second two the parton density sum evaluated at y_3 = y_ 4 = 0 so that x_1 = x_2 = x_T = 2 pT / E_cm, where the product is expected to be maximal, and the final is the phase space for -y_max < y_{3,4} < y_max. The right-hand side expression is scanned logarithmically in y, and a N is determined such that it always is below N/pT^4.

To describe the dampening of the cross section at pT -> 0 by colour screening, the actual cross section is multiplied by a regularization factor (pT^2 / (pT^2 + pT0^2))^2, and the alpha_s is evaluated at a scale pT^2 + pT0^2, where pT0 is a free parameter of the order of 2 - 4 GeV. Since pT0 can be energy-dependent, an ansatz
pT0(ecm) = pT0Ref * (ecm/ecmRef)^ecmPow
is used, where ecm is the current CM frame energy, ecmRef is an arbitrary reference energy where pT0Ref is defined, and ecmPow gives the energy rescaling pace. For technical reasons, also an absolute lower pT scale pTmin, by default 0.2 GeV, is introduced. In principle, it is possible to recover older scenarios with a sharp pT cutoff by setting pT0 = 0 and letting pTmin be a larger number.

The above scanning strategy is then slightly modified: instead of an upper estimate N/pT^4 one of the form N/(pT^2 + r * pT0^2)^2 is used. At first glance, r = 1 would seem to be fixed by the form of the regularization procedure, but this does not take into account the nontrivial dependence on alpha_s, parton distributions and phase space. A better Monte Carlo efficiency is obtained for r somewhat below unity, and currently r = 0.25 is hardcoded. In the generation a trial pT2 is then selected according to
d(Prob)/d(pT2) = (1/sigma_ND) * N/(pT^2 + r * pT0^2)^2 * ("Sudakov")
For the trial pT2, a y_3 and a y_4 are then selected, and incoming flavours according to the respective F(x_i, pT2), and then the cross section is evaluated for this flavour combination. The ratio of trial/upper estimate gives the probability of survival.

Actually, to profit from the factor 1/2 mentioned above, the cross section for the combination with y_3 and y_4 interchanged is also tried, which corresponds to exchanging tHat and uHat, and the average formed, while the final kinematics is given by the relative importance of the two.

Furthermore, since large y values are disfavoured by dropping PDF's, a factor
WT_y = (1 - (y_3/y_max)^2) * (1 - (y_4/y_max)^2)
is evaluated, and used as a survival probability before the more time-consuming PDF+ME evaluation, with surviving events given a compensating weight 1/WT_y.

An impact-parameter dependence is also allowed. Based on the hard pT scale of the first interaction, and enhancement/depletion factor is picked, which multiplies the rate of subsequent interactions.

Parton densities are rescaled and modified to take into account the energy-momentum and flavours kicked out by already-considered interactions. pythia8-8.1.80.orig/htmldoc/TimelikeShowers.html0000644000175000017500000012535012217615311017774 0ustar sunsun Timelike Showers

Timelike Showers

The PYTHIA algorithm for timelike final-state showers is based on the article [Sjo05], where a transverse-momentum-ordered evolution scheme is introduced, with the extension to fully interleaved evolution covered in [Cor10a]. This algorithm is influenced by the previous mass-ordered algorithm in PYTHIA [Ben87] and by the dipole-emission formulation in Ariadne [Gus86]. From the mass-ordered algorithm it inherits a merging procedure for first-order gluon-emission matrix elements in essentially all two-body decays in the standard model and its minimal supersymmetric extension [Nor01].

The normal user is not expected to call TimeShower directly, but only have it called from Pythia. Some of the parameters below, in particular TimeShower:alphaSvalue, would be of interest for a tuning exercise, however.

Main variables

Often the maximum scale of the FSR shower evolution is understood from the context. For instance, in a resonance decay half the resonance mass sets an absolute upper limit. For a hard process in a hadronic collision the choice is not as unique. Here the factorization scale has been chosen as the maximum evolution scale. This would be the pT for a 2 -> 2 process, supplemented by mass terms for massive outgoing particles. For some special applications we do allow an alternative.

mode  TimeShower:pTmaxMatch   (default = 1; minimum = 0; maximum = 2)
Way in which the maximum shower evolution scale is set to match the scale of the hard process itself.
option 0 : (i) if the final state of the hard process (not counting subsequent resonance decays) contains at least one quark (u, d, s, c ,b), gluon or photon then pT_max is chosen to be the factorization scale for internal processes and the scale value for Les Houches input; (ii) if not, emissions are allowed to go all the way up to the kinematical limit (i.e. to half the dipole mass). This option agrees with the corresponding one for spacelike showers. There the reasoning is that in the former set of processes the ISR emission of yet another quark, gluon or photon could lead to double-counting, while no such danger exists in the latter case. The argument is less compelling for timelike showers, but could be a reasonable starting point.
option 1 : always use the factorization scale for an internal process and the scale value for Les Houches input, i.e. the lower value. This should avoid double-counting, but may leave out some emissions that ought to have been simulated. (Also known as wimpy showers.)
option 2 : always allow emissions up to the kinematical limit (i.e. to half the dipole mass). This will simulate all possible event topologies, but may lead to double-counting. (Also known as power showers.)
Note 1: as enumerated in the text, these options take effect both for internal and external processes. Whether a particular option makes sense depends on the context. For instance, if events for the same basic process to different orders are to be matched, then option 1 would be a reasonable first guess. But in more sophisticated descriptions option 2 could be combined with UserHook vetoes on emissions that would lead to double-counting, using more flexible phase space boundaries. Option 0, finally, may be most realistic when only Born-level processes are involved, possibly in combination with a nonzero TimeShower:pTdampMatch.
Note 2: These options only apply to the hard interaction. If a "second hard" process is present, the two are analyzed and set separately for the default 0 option, while both are affected the same way for non-default options 1 and 2. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of each process itself. The options also assume that you use interleaved evolution, so that FSR is in direct competition with ISR for the hardest emission. If you already generated a number of ISR partons at low pT, it would not make sense to have a later FSR shower up to the kinematical limit for all of them.
Note 3: Recall that resonance decays are not affected by this mode, but that showers there are always set to fill the full phase space, often with built-in matrix-element-matching that give a NLO accuracy. A modification of this behaviour would require you to work with UserHooks.

parm  TimeShower:pTmaxFudge   (default = 1.0; minimum = 0.25; maximum = 2.0)
In cases where the above pTmaxMatch rules would imply that pT_max = pT_factorization, pTmaxFudge introduces a multiplicative factor f such that instead pT_max = f * pT_factorization. Only applies to the hardest interaction in an event, and a "second hard" if there is such a one, cf. below. It is strongly suggested that f = 1, but variations around this default can be useful to test this assumption.
Note:Scales for resonance decays are not affected, but can be set separately by user hooks.

parm  TimeShower:pTmaxFudgeMPI   (default = 1.0; minimum = 0.25; maximum = 2.0)
A multiplicative factor f such that pT_max = f * pT_factorization, as above, but here for the non-hardest interactions (when multiparton interactions are allowed).

mode  TimeShower:pTdampMatch   (default = 0; minimum = 0; maximum = 2)
These options only take effect when a process is allowed to radiate up to the kinematical limit by the above pTmaxMatch choice, and no matrix-element corrections are available. Then, in many processes, the fall-off in pT will be too slow by one factor of pT^2. That is, while showers have an approximate dpT^2/pT^2 shape, often it should become more like dpT^2/pT^4 at pT values above the scale of the hard process. This argument is more obvious and relevant for ISR, where emissions could go the the kinematical limit, whereas they are constrained by the respective dipole mass for FSR. Nevertheless this matching option is offered for FSR to have a (semi-)symmetric description. Note that a dampening factor is applied to all dipoles in the final state of the hard process, which is somewhat different from the ISR implementation.
option 0 : emissions go up to the kinematical limit, with no special dampening.
option 1 : emissions go up to the kinematical limit, but dampened by a factor k^2 Q^2_fac/(pT^2 + k^2 Q^2_fac), where Q_fac is the factorization scale and k is a multiplicative fudge factor stored in pTdampFudge below.
option 2 : emissions go up to the kinematical limit, but dampened by a factor k^2 Q^2_ren/(pT^2 + k^2 Q^2_ren), where Q_ren is the renormalization scale and k is a multiplicative fudge factor stored in pTdampFudge below.
Note: These options only apply to the hard interaction. Specifically, a "second hard" interaction would not be affected. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of the process itself.

parm  TimeShower:pTdampFudge   (default = 1.0; minimum = 0.25; maximum = 4.0)
In cases 1 and 2 above, where a dampening is imposed at around the factorization or renormalization scale, respectively, this allows the pT scale of dampening of radiation by a half to be shifted by this factor relative to the default Q_fac or Q_ren. This number ought to be in the neighbourhood of unity, but variations away from this value could do better in some processes.

The amount of QCD radiation in the shower is determined by

parm  TimeShower:alphaSvalue   (default = 0.1383; minimum = 0.06; maximum = 0.25)
The alpha_strong value at scale M_Z^2. The default value corresponds to a crude tuning to LEP data, to be improved.

The actual value is then regulated by the running to the scale pT^2, at which the shower evaluates alpha_strong.

mode  TimeShower:alphaSorder   (default = 1; minimum = 0; maximum = 2)
Order at which alpha_strong runs,
option 0 : zeroth order, i.e. alpha_strong is kept fixed.
option 1 : first order, which is the normal value.
option 2 : second order. Since other parts of the code do not go to second order there is no strong reason to use this option, but there is also nothing wrong with it.

The CMW rescaling of Lambda_QCD (see the section on StandardModelParameters) can be applied to the alpha_strong values used for timelike showers. Note that tunes using this option need lower values of alpha_strong(m_Z^2) than tunes that do not.

flag  TimeShower:alphaSuseCMW   (default = false)

option false : Do not apply the CMW rescaling.
option true : Apply the CMW rescaling, increasing Lambda_QCD for timelike showers by a factor roughly 1.6.

QED radiation is regulated by the alpha_electromagnetic value at the pT^2 scale of a branching.

mode  TimeShower:alphaEMorder   (default = 1; minimum = -1; maximum = 1)
The running of alpha_em.
option 1 : first-order running, constrained to agree with StandardModel:alphaEMmZ at the Z^0 mass.
option 0 : zeroth order, i.e. alpha_em is kept fixed at its value at vanishing momentum transfer.
option -1 : zeroth order, i.e. alpha_em is kept fixed, but at StandardModel:alphaEMmZ, i.e. its value at the Z^0 mass.

The natural scale for couplings, and PDFs for dipoles stretching out to the beam remnants, is pT^2. To explore uncertainties it is possibly to vary around this value, however, in analogy with what can be done for hard processes.

parm  TimeShower:renormMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
The default pT^2 renormalization scale is multiplied by this prefactor. For QCD this is equivalent to a change of Lambda^2 in the opposite direction, i.e. to a change of alpha_strong(M_Z^2) (except that flavour thresholds remain at fixed scales).

parm  TimeShower:factorMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
The default pT^2 factorization scale is multiplied by this prefactor.

The rate of radiation if divergent in the pT -> 0 limit. Here, however, perturbation theory is expected to break down. Therefore an effective pT_min cutoff parameter is introduced, below which no emissions are allowed. The cutoff may be different for QCD and QED radiation off quarks, and is mainly a technical parameter for QED radiation off leptons.

parm  TimeShower:pTmin   (default = 0.4; minimum = 0.1; maximum = 2.0)
Parton shower cut-off pT for QCD emissions.

parm  TimeShower:pTminChgQ   (default = 0.4; minimum = 0.1; maximum = 2.0)
Parton shower cut-off pT for photon coupling to coloured particle.

parm  TimeShower:pTminChgL   (default = 1e-6; minimum = 1e-10; maximum = 2.0)
Parton shower cut-off pT for pure QED branchings. Assumed smaller than (or equal to) pTminChgQ.

Shower branchings gamma -> f fbar, where f is a quark or lepton, in part compete with the hard processes involving gamma^*/Z^0 production. In order to avoid overlap it makes sense to correlate the maximum gamma mass allowed in showers with the minimum gamma^*/Z^0 mass allowed in hard processes. In addition, the shower contribution only contains the pure gamma^* contribution, i.e. not the Z^0 part, so the mass spectrum above 50 GeV or so would not be well described.

parm  TimeShower:mMaxGamma   (default = 10.0; minimum = 0.001; maximum = 5000.0)
Maximum invariant mass allowed for the created fermion pair in a gamma -> f fbar branching in the shower.

Interleaved evolution

Multiparton interactions (MPI) and initial-state showers (ISR) are always interleaved, as follows. Starting from the hard interaction, the complete event is constructed by a set of steps. In each step the pT scale of the previous step is used as starting scale for a downwards evolution. The MPI and ISR components each make their respective Monte Carlo choices for the next lower pT value. The one with larger pT is allowed to carry out its proposed action, thereby modifying the conditions for the next steps. This is relevant since the two components compete for the energy contained in the beam remnants: both an interaction and an emission take away some of the energy, leaving less for the future. The end result is a combined chain of decreasing pT values, where ones associated with new interactions and ones with new emissions are interleaved.

There is no corresponding requirement for final-state radiation (FSR) to be interleaved. Such an FSR emission does not compete directly for beam energy (but see below), and also can be viewed as occurring after the other two components in some kind of time sense. Interleaving is allowed, however, since it can be argued that a high-pT FSR occurs on shorter time scales than a low-pT MPI, say. Backwards evolution of ISR is also an example that physical time is not the only possible ordering principle, but that one can work with conditional probabilities: given the partonic picture at a specific pT resolution scale, what possibilities are open for a modified picture at a slightly lower pT scale, either by MPI, ISR or FSR? Complete interleaving of the three components also offers advantages if one aims at matching to higher-order matrix elements above some given scale.

flag  TimeShower:interleave   (default = on)
If on, final-state emissions are interleaved in the same decreasing-pT chain as multiparton interactions and initial-state emissions. If off, final-state emissions are only addressed after the multiparton interactions and initial-state radiation have been considered.

As an aside, it should be noted that such interleaving does not affect showering in resonance decays, such as a Z^0. These decays are only introduced after the production process has been considered in full, and the subsequent FSR is carried out inside the resonance, with preserved resonance mass.

One aspect of FSR for a hard process in hadron collisions is that often colour dipoles are formed between a scattered parton and a beam remnant, or rather the hole left behind by an incoming partons. If such holes are allowed as dipole ends and take the recoil when the scattered parton undergoes a branching then this translates into the need to take some amount of remnant energy also in the case of FSR, i.e. the roles of ISR and FSR are not completely decoupled. The energy taken away is bookkept by increasing the x value assigned to the incoming scattering parton, and a reweighting factor x_new f(x_new, pT^2) / x_old f(x_old, pT^2) in the emission probability ensures that not unphysically large x_new values are reached. Usually such x changes are small, and they can be viewed as a higher-order effect beyond the accuracy of the leading-log initial-state showers.

This choice is not unique, however. As an alternative, if nothing else useful for cross-checks, one could imagine that the FSR is completely decoupled from the ISR and beam remnants.

flag  TimeShower:allowBeamRecoil   (default = on)
If on, the final-state shower is allowed to borrow energy from the beam remnants as described above, thereby changing the mass of the scattering subsystem. If off, the partons in the scattering subsystem are constrained to borrow energy from each other, such that the total four-momentum of the system is preserved. This flag has no effect on resonance decays, where the shower always preserves the resonance mass, cf. the comment above about showers for resonances never being interleaved.

flag  TimeShower:dampenBeamRecoil   (default = on)
When beam recoil is allowed there is still some ambiguity how far into the beam end of the dipole that emission should be allowed. It is dampened in the beam region, but probably not enough. When on an additional suppression factor 4 pT2_hard / (4 pT2_hard + m2) is multiplied on to the emission probability. Here pT_hard is the transverse momentum of the radiating parton and m the off-shell mass it acquires by the branching, m2 = pT2/(z(1-z)). Note that m2 = 4 pT2_hard is the kinematical limit for a scattering at 90 degrees without beam recoil.

Global recoil

The final-state algorithm is based on dipole-style recoils, where one single parton takes the full recoil of a branching. This is unlike the initial-state algorithm, where the complete already-existing final state shares the recoil of each new emission. As an alternative, also the final-state algorithm contains an option where the recoil is shared between all partons in the final state. Thus the radiation pattern is unrelated to colour correlations. This is especially convenient for some matching algorithms, like MC@NLO, where a full analytic knowledge of the shower radiation pattern is needed to avoid double-counting. (The pT-ordered shower is described in [Sjo05], and the corrections for massive radiator and recoiler in [Nor01].)

Technically, the radiation pattern is most conveniently represented in the rest frame of the final state of the hard subprocess. Then, for each parton at a time, the rest of the final state can be viewed as a single effective parton. This "parton" has a fixed invariant mass during the emission process, and takes the recoil without any changed direction of motion. The momenta of the individual new recoilers are then obtained by a simple common boost of the original ones.

This alternative approach will miss out on the colour coherence phenomena. Specifically, with the whole subcollision mass as "dipole" mass, the phase space for subsequent emissions is larger than for the normal dipole algorithm. The phase space difference grows as more and more gluons are created, and thus leads to a way too steep multiplication of soft gluons. Therefore the main application is for the first one or few emissions of the shower, where a potential overestimate of the emission rate is to be corrected for anyway, by matching to the relevant matrix elements. Thereafter, subsequent emissions should be handled as before, i.e. with dipoles spanned between nearby partons. Furthermore, only the first (hardest) subcollision is handled with global recoils, since subsequent MPI's would not be subject to matrix element corrections anyway.

In order for the mid-shower switch from global to local recoils to work, colours are traced and bookkept just as for normal showers; it is only that this information is not used in those steps where a global recoil is requested. (Thus, e.g., a gluon is still bookkept as one colour and one anticolour dipole end, with half the charge each, but with global recoil those two ends radiate identically.)

flag  TimeShower:globalRecoil   (default = off)
Alternative approach as above, where all final-state particles share the recoil of an emission.
If off, then use the standard dipole-recoil approach.
If on, use the alternative global recoil, but only for the first interaction, and only while the number of particles in the final state is at most TimeShower:nMaxGlobalRecoil before the branching.

mode  TimeShower:nMaxGlobalRecoil   (default = 2; minimum = 1)
Represents the maximum number of particles in the final state for which the next final-state emission can be performed with the global recoil strategy. This number counts all particles, whether they are allowed to radiate or not, e.g. also Z^0. Also partons created by initial-state radiation emissions counts towards this sum, as part of the interleaved evolution. Without interleaved evolution this option would not make sense, since then a varying and large number of partons could already have been created by the initial-state radiation before the first final-state one, and then there is not likely to be any matrix elements available for matching.

Two variations of the scheme outlined above are also available, (motivated by comparative studies within aMC@NLO). These studies indicate that global recoils should be used as sparsely as possible, in order to retain desirable features of the radiation pattern produced with the local recoil prescription.

mode  TimeShower:globalRecoilMode   (default = 0; minimum = 0; maximum = 2)
Choice which splittings are produced with the global recoil approach.
option 0 : Global recoil mode as outlined above, i.e. using global recoils until the number of final state particles exceeds TimeShower:nMaxGlobalRecoil.
option 1 : Global recoil only for the first branching of final state legs that have an ancestor in the hard process, and if the maximal number of branchings generated according to the global recoil scheme (see TimeShower:nMaxGlobalBranch below) has not yet been reached.
option 2 : Global recoil only if the first branching in the whole evolution is a timelike splitting of a parton in an event with Born-like kinematics (i.e.\ an S-event). The impact of global recoils should be minimal in this case. This option is only sensible for interleaved evolution.

mode  TimeShower:nMaxGlobalBranch   (default = -1)
The maximum number of splittings in the final state for which the next final-state emission can be performed with the global recoil strategy. This number has to be set if TimeShower:globalRecoilMode = 1 or TimeShower:globalRecoilMode = 2

mode  TimeShower:nPartonsInBorn   (default = -1)
The number of partons for Born-like phase space points. This number needs to be set if a different treatment of S-events (with Born-like kinematics) and H-events (with real-emission kinematics) is desired. This number has to be set if TimeShower:globalRecoilMode = 2.

flag  TimeShower:limitPTmaxGlobal   (default = off)
If on, limit the maximal pT produced in branchings in the global recoil scheme exactly as in the default (local) scheme. This means that the mass of the splitting dipole will set an upper bound for the pT of an emission. To be more explicit, this disallows emissions with pT larger than min{μstart 2, mD2/4}, with mD 2 = (√ (pr +ps)2 -m0,s)2 - m0,r2 , where the shower starting scale is μstart (i.e. SCALUP when reading LHE files, and Info.QFac() otherwise), r the radiating parton, and s the recoiling particle that would have been used in the local recoil scheme. This option is only used if wimpy showers are enabled.

The global-recoil machinery does not work well with rescattering in the MPI machinery, since then the recoiling system is not uniquely defined. MultipartonInteractions:allowRescatter = off by default, so this is not a main issue. If both options are switched on, rescattering will only be allowed to kick in after the global recoil has ceased to be active, i.e. once the nMaxGlobalRecoil limit has been exceeded. This should not be a major conflict, since rescattering is mainly of interest at later stages of the downwards pT evolution.

Further, it is strongly recommended to set TimeShower:MEcorrections = off (not default!), i.e. not to correct the emission probability to the internal matrix elements. The internal ME options do not cover any cases relevant for a multibody recoiler anyway, so no guarantees are given what prescription would come to be used. Instead, without ME corrections, a process-independent emission rate is obtained, and user hooks can provide the desired process-specific rejection factors.

Radiation off octet onium states

In the current implementation, charmonium and bottomonium production can proceed either through colour singlet or colour octet mechanisms, both of them implemented in terms of 2 -> 2 hard processes such as g g -> (onium) g. In the former case the state does not radiate and the onium therefore is produced in isolation, up to normal underlying-event activity. In the latter case the situation is not so clear, but it is sensible to assume that a shower can evolve. (Assuming, of course, that the transverse momentum of the onium state is sufficiently high that radiation is of relevance.)

There could be two parts to such a shower. Firstly a gluon (or even a quark, though less likely) produced in a hard 2 -> 2 process can undergo showering into many gluons, whereof one branches into the heavy-quark pair. Secondly, once the pair has been produced, each quark can radiate further gluons. This latter kind of emission could easily break up a semibound quark pair, but might also create a new semibound state where before an unbound pair existed, and to some approximation these two effects should balance in the onium production rate. The showering "off an onium state" as implemented here therefore should not be viewed as an accurate description of the emission history step by step, but rather as an effective approach to ensure that the octet onium produced "in the hard process" is embedded in a realistic amount of jet activity. Of course both the isolated singlet and embedded octet are likely to be extremes, but hopefully the mix of the two will strike a reasonable balance. However, it is possible that some part of the octet production occurs in channels where it should not be accompanied by (hard) radiation. Therefore reducing the fraction of octet onium states allowed to radiate is a valid variation to explore uncertainties.

If an octet onium state is chosen to radiate, the simulation of branchings is based on the assumption that the full radiation is provided by an incoherent sum of radiation off the quark and off the antiquark of the onium state. Thus the splitting kernel is taken to be the normal q -> q g one, multiplied by a factor of two. Obviously this is a simplification of a more complex picture, averaging over factors pulling in different directions. Firstly, radiation off a gluon ought to be enhanced by a factor 9/4 relative to a quark rather than the 2 now used, but this is a minor difference. Secondly, our use of the q -> q g branching kernel is roughly equivalent to always following the harder gluon in a g -> g g branching. This could give us a bias towards producing too hard onia. A soft gluon would have little phase space to branch into a heavy-quark pair however, so the bias may not be as big as it would seem at first glance. Thirdly, once the gluon has branched into a quark pair, each quark carries roughly only half of the onium energy. The maximum energy per emitted gluon should then be roughly half the onium energy rather than the full, as it is now. Thereby the energy of radiated gluons is exaggerated, i.e. onia become too soft. So the second and the third points tend to cancel each other.

Finally, note that the lower cutoff scale of the shower evolution depends on the onium mass rather than on the quark mass, as it should be. Gluons below the octet-onium scale should only be part of the octet-to-singlet transition.

parm  TimeShower:octetOniumFraction   (default = 1.; minimum = 0.; maximum = 1.)
Allow colour-octet charmonium and bottomonium states to radiate gluons. 0 means that no octet-onium states radiate, 1 that all do, with possibility to interpolate between these two extremes.

parm  TimeShower:octetOniumColFac   (default = 2.; minimum = 0.; maximum = 4.)
The colour factor used used in the splitting kernel for those octet onium states that are allowed to radiate, normalized to the q -> q g splitting kernel. Thus the default corresponds to twice the radiation off a quark. The physically preferred range would be between 1 and 9/4.

Weak showers

The emission of W^+- and Z^0 gauge bosons off fermions is intended to become an integrated part of the initial- and final-state radiation frameworks, and is fully interleaved with QCD and QED emissions. Currently it is under development, and off by default. Another restriction is that there is no simulation of the full gamma^*/Z^0 interference: at low masses the QED shower involves a pure gamma^* component, whereas the weak shower generates a pure Z^0.

Most events will not contain a W^+-/Z^0 emission at all, and in a shower framework it is not straightforward to force such emissions to happen without biasing the event sample in some respect. An option is available to enhance the emission rate artificially, but it is then the responsibility of the user to correct the cross section accordingly, and not to pick an enhancement so big that the probability for more than one emission is non-negligible. (It is not enough to assign an event weight 1/e^n where e is the enhancement factor and n is the number of emitted gauge bosons. This still misses to account for the change in phase space for late emissions by the effect of earlier ones, or equivalently for the unwanted change in the Sudakov form factor. See [Lon12a] for a detailed discussion and possible solutions.)

Another enhancement probability is to only allow some specific W^+-/Z^0 decay modes. By default the shower is inclusive, since it should describe all that can happen with unit probability. This also holds even if the W^+- and Z^0 produced in the hard process have been restricted to specific decay channels. The trick that allows this is that two new "aliases" have been produced, a Zcopy with identity code 93 and a Wcopy with code 94. These copies are used specifically to bookkeep decay channels open for W^+-/Z^0 bosons produced in the shower. For the rest they are invisible, i.e. you will not find them in event listings. The separation into two sets of gauge bosons then also allows the selection of specific decay modes for 93 and 94, i.e. for only the gauge bosons produced in the shower. As above it is here up to the user to reweight the event to compensate for the bias introduced, and to watch out for possible complications. In this case there is no kinematics bias, but one would miss out on topologies where a not-selected decay channel could be part of the background to the selected one, notably when more than one gauge boson is produced.

Note that the common theme is that a bias leads to an event-specific weight, since each event is unique. It also means that the cross-section information obtained e.g. by Pythia::stat() is misleading, since it has not been corrected for such weights. This is different from biases in a predetermined hard process, where the net reduction in cross section can be calculated once and for all at initialization, and events generated with unit weight thereafter.

Special for the weak showers is that couplings are different for left- and righthanded fermions. With incoming unpolarized beams this should average out, at least so long as only one weak emission occurs. In the case of several weak emissions off the same fermion the correlation between them will carry a memory of the fermion helicity. Such a memory is retained for the affected dipole end, and is reflected in the Particle::pol() property, it being +1 (-1) for fermions considered righthanded (lefthanded), and 0 for the bulk where no choice has been made.

The FSR shower emission is always matched to the matrix element for emission off a f fbar weak dipole. (Emission rates are normalized to the invariant mass of the dipole at the time of the weak emission, i.e. discounting the energy lost by previous QCD/QED emissions.) Also the angular distribution in the subsequent V = W^+-/Z^0 decay is matched to the matrix element expression for f fbar -> f fbar V -> f fbar f' fbar'. Afterwards the f' fbar' system undergoes showers and hadronization just like any W^+-/Z^0 decay products would.

A few special switches are available for the weak framework, several mainly intended for tryout purposes, as follows.

flag  TimeShower:weakShower   (default = off)
Allow a weak shower, yes or no.

mode  TimeShower:weakShowerMode   (default = 0; minimum = 0; maximum = 2)
Determine which branchings are allowed.
option 0 : both W^+- and Z^0 branchings.
option 1 : only W^+- branchings.
option 2 : only Z^0 branchings.

parm  TimeShower:pTminWeak   (default = 1.0; minimum = 0.1; maximum = 2.0)
Parton shower cut-off pT for weak branchings.

parm  TimeShower:weakShowerEnhancement   (default = 1.; minimum = 1.; maximum = 1000.)
Enhancement factor for the weak shower. This is used to increase the statistics of weak shower emissions. Remember afterwards to correct for the additional weak emissions (i.e. divide the rate of weak emissions by the same factor).

flag  TimeShower:singleWeakEmission   (default = off)
This parameter allows to stop the weak shower after a single emission.
If on, only a single weak emission is allowed.
If off, an unlimited number of weak emissions possible.

parm  TimeShower:extraScaleTerm   (default = 0.; minimum = 0.; maximum = 2.)
The normal showers uses pT^2 as ordering variable, but for massive particles it could be preferred to use pT^2 + M^2 instead. This parameter allows to use pT^2 + k * M^2 for weak showers, thus k = 0 is the standard ordering and is used as default.

flag  TimeShower:dopTDampMass   (default = on)
Add an extra dampening to the weak shower to lower the production of low-pT W/Z's. The dampening is given by (pT^2 + 0.25 M^2)/ (pT^2 + M^2), where M^2 is the squared mass of the W/Z.

Further variables

There are several possibilities you can use to switch on or off selected branching types in the shower, or in other respects simplify the shower. These should normally not be touched. Their main function is for cross-checks.

flag  TimeShower:QCDshower   (default = on)
Allow a QCD shower, i.e. branchings q -> q g, g -> g g and g -> q qbar; on/off = true/false.

mode  TimeShower:nGluonToQuark   (default = 5; minimum = 0; maximum = 5)
Number of allowed quark flavours in g -> q qbar branchings (phase space permitting). A change to 4 would exclude g -> b bbar, etc.

flag  TimeShower:QEDshowerByQ   (default = on)
Allow quarks to radiate photons, i.e. branchings q -> q gamma; on/off = true/false.

flag  TimeShower:QEDshowerByL   (default = on)
Allow leptons to radiate photons, i.e. branchings l -> l gamma; on/off = true/false.

flag  TimeShower:QEDshowerByGamma   (default = on)
Allow photons to branch into lepton or quark pairs, i.e. branchings gamma -> l+ l- and gamma -> q qbar; on/off = true/false.

mode  TimeShower:nGammaToQuark   (default = 5; minimum = 0; maximum = 5)
Number of allowed quark flavours in gamma -> q qbar branchings (phase space permitting). A change to 4 would exclude g -> b bbar, etc.

mode  TimeShower:nGammaToLepton   (default = 3; minimum = 0; maximum = 3)
Number of allowed lepton flavours in gamma -> l+ l- branchings (phase space permitting). A change to 2 would exclude gamma -> tau+ tau-, and a change to 1 also gamma -> mu+ mu-.

flag  TimeShower:MEcorrections   (default = on)
Use of matrix element corrections where available; on/off = true/false.

flag  TimeShower:MEafterFirst   (default = on)
Use of matrix element corrections also after the first emission, for dipole ends of the same system that did not yet radiate. Only has a meaning if MEcorrections above is switched on.

flag  TimeShower:phiPolAsym   (default = on)
Azimuthal asymmetry induced by gluon polarization; on/off = true/false.

flag  TimeShower:recoilToColoured   (default = on)
In the decays of coloured resonances, say t -> b W, it is not possible to set up dipoles with matched colours. Originally the b radiator therefore has W as recoiler, and that choice is unique. Once a gluon has been radiated, however, it is possible either to have the unmatched colour (inherited by the gluon) still recoiling against the W (off), or else let it recoil against the b also for this dipole (on). Before version 8.160 the former was the only possibility, which could give unphysical radiation patterns. It is kept as an option to check backwards compatibility. The same issue exists for QED radiation, but obviously is less significant. Consider the example W -> e nu, where originally the nu takes the recoil. In the old (off) scheme the nu would remain recoiler, while in the new (on) instead each newly emitted photon becomes the new recoiler. pythia8-8.1.80.orig/htmldoc/MasterSwitches.html0000644000175000017500000002315012217615311017616 0ustar sunsun Master Switches

Master Switches

Sometimes it may be convenient to omit certain aspects of the event generation chain. This cannot be motivated in a full-blown production run, but can often be convenient for own understanding and for debug purposes. The flags on this page allow just that.

The event generation is subdivided into three levels: the process level, the parton level and the hadron level, and flags are grouped accordingly.

Process Level

The ProcessLevel class administrates the initial step of the event generation, wherein the basic process is selected. Currently this is done either using some of the internal processes, or with Les Houches Accord input.

There could not be a complete event without an initial process, so it would not be a normal action to switch off this step. Furthermore, without a process set, it is also not possible to carry out the tasks on the parton level. It is still possible, however, to hadronize a parton-level configuration provided by some external program.

flag  ProcessLevel:all   (default = on)
If off, do not attempt to carry out any generation at all on the process level. For the parton level only final-state radiation is possible, using the Pythia::forceTimeShower(...) method. Do allow parton configurations stored in the event record to hadronize and hadrons to decay, however, as set by the HadronLevel switches. Further details are found here.

For ProcessLevel:all = on one part of the event generation on this level may be switched off individually:

flag  ProcessLevel:resonanceDecays   (default = on)
Master switch to allow resonance decays; on/off = true/false. Normal hadrons and leptons do not count as resonances, so this is aimed specifically towards Z^0, W^+-, t, h^0 and similar objects beyond the Standard Model. Do not use this option if you may produce coloured resonances and intend to allow hadronization, since currently the program would not know how to handle this.

It is possible to stop the generation immediately after the basic process has been selected, see PartonLevel:all below.

PartonLevel

The PartonLevel class administrates the middle step of the event generation, i.e. the evolution from an input (hard) process from ProcessLevel, containing a few partons only, to a complete parton-level configuration to be handed on to HadronLevel. This step involves the application of initial- and final-state radiation, multiparton interactions and the structure of beam remnants.

flag  PartonLevel:all   (default = on)
If off then stop the generation after the hard process has been generated, but before the parton-level and hadron-level steps. The process record is filled, but the event one is then not.

For PartonLevel:all = on some parts of the event generation on this level may be switched off individually:

flag  PartonLevel:MPI   (default = on)
Master switch for multiparton interactions; on/off = true/false. Further options are found here.

flag  PartonLevel:ISR   (default = on)
Master switch for initial-state radiation; on/off = true/false. Further options are found here.

flag  PartonLevel:FSR   (default = on)
Master switch for final-state radiation; on/off = true/false. Further options are found here. If you leave this switch on, the following two switches allow more detailed control to switch off only parts of the showers.

flag  PartonLevel:FSRinProcess   (default = on)
Switch for final-state radiation in association with the hard process itself; on/off = true/false. In addition PartonLevel:FSR must be on for these emissions to occur.

flag  PartonLevel:FSRinResonances   (default = on)
Master switch for final-state radiation in any resonance decays subsequent to the hard process itself; on/off = true/false. In addition PartonLevel:FSR must be on for these emissions to occur.

flag  PartonLevel:earlyResDec   (default = off)
If on then do resonance decays early, before beam handling including colour reconnection. If off then decays are done afterwards, and so are unaffected by colour reconnection. The early-decay option is still primitive, for some first studies. Eventually the choice should be made individually for each resonance based on lifetime (and the environment).

Switching off all the above MPI/ISR/FSR switches is not equivalent to setting PartonLevel:all = off. In the former case a minimal skeleton of parton-level operations are carried out, such as tying together the scattered partons with the beam remnants into colour singlets, and storing this information in the event record. It is therefore possible to go on and hadronize the event, if desired. In the latter case no operations at all are carried out on the parton level, and therefore it is also not possible to go on to the hadron level.

flag  PartonLevel:Remnants   (default = on)
Master switch for addition of beam remnants; on/off = true/false. Only intended for very special applications, and cannot be used to generate complete events. Specifically, unlike the other switches above, the program will complain and possibly crash unlike you also set HadronLevel:all = off and Check:event = off.

It is possible to stop the generation immediately after the parton level has been set up, see HadronLevel:all below.

HadronLevel

The HadronLevel class administrates the final step of the event generation, wherein the partonic configuration from PartonLevel is hadronized, including string fragmentation and secondary decays.

Most of the code in this class itself deals with subdividing the partonic content of the event into separate colour singlets, that can be treated individually by the string fragmentation machinery. When a junction and an antijunction are directly connected, it also breaks the string between the two, so that the topology can be reduced back to two separate one-junction systems, while still preserving the expected particle flow in the junction-junction string region(s).

flag  HadronLevel:all   (default = on)
If off then stop the generation after the hard process and parton-level activity has been generated, but before the hadron-level steps.

For HadronLevel:all = on some parts of the event generation on this level may be switched off individually:

flag  HadronLevel:Hadronize   (default = on)
Master switch for hadronization; on/off = true/false. Further options are found here.

flag  HadronLevel:Decay   (default = on)
Master switch for decays; on/off = true/false. Further options are found here.

flag  HadronLevel:BoseEinstein   (default = off)
Master switch for the simulation of Bose-Einstein effects; on/off = true/false. Further options are found here.

Printing

flag  Print:quiet   (default = off)
Can be set on to avoid the printing during program execution, to the largest extent possible. This flag acts by setting the relevant values for Init:showProcesses, Init:showMultipartonInteractions, Init:showChangedSettings, Init:showAllSettings, Init:showChangedParticleData, Init:showChangedResonanceData, Init:showAllParticleData, Init:showOneParticleData, Next:numberCount, Next:numberShowLHA, Next:numberShowInfo, Next:numberShowProcess, and Next:numberShowEvent. The change is to off or 0 for Print:quiet = off, and restores to the respective default value for = on. Those changes take effect immediately, so individual settings can be changed afterwards. pythia8-8.1.80.orig/htmldoc/GUIDELINES0000644000175000017500000001105212217346214015337 0ustar sunsun MCNET GUIDELINES for Event Generator Authors and Users PREAMBLE This generator has been developed as part of an academic research project and is the result of many years of work by the authors. Proper academic recognition is a requirement for its continued development. The components of the program have been developed to work together as a coherent physics framework. We believe that the creation of separately maintained forks or piecewise distribution of individual parts would diminish their scientific value. The authors are convinced that software development in a scientific context requires full availability of all source code, to further progress and to allow local modifications to meet the specific requirements of the individual user. Therefore we have decided to release this program under the GNU General Public License (GPL) version 2. This ensures that the source code will be available to you and grants you the freedom to use and modify the program. You can redistribute your modified versions as long as you retain the GPL and respect existing copyright notices (see the file 'COPYING' for details). By using the GPL, we entrust you with considerable freedom and expect you to use it wisely, since the GPL does not address the issues in the first two paragraphs. To remedy this shortcoming, we have formulated the following guidelines relevant for the distribution and usage of event generator software in an academic setting. GUIDELINES 1) The integrity of the program should be respected. ------------------------------------------------- 1.1) Suspected bugs and proposed fixes should be reported back to the original authors to be considered for inclusion in the standard distribution. No independently developed and maintained forks should be created as long as the original authors actively work on the program. 1.2) The program should normally be redistributed in its entirety. When there are special reasons, an agreement should be sought with the original authors to redistribute only specific parts. This should be arranged such that the redistributed parts remain updated in step with the standard distribution. 1.3) Any changes in the code must be clearly marked in the source (reason, author, date) and documented. If any modified version is redistributed it should be stated at the point of distribution (download link) that it has been modified and why. 1.4) If a significant part of the code is used by another program, this should be clearly specified in that program's documentation and stated at its point of distribution. 1.5) Copyright information and references may not be removed. Copyright-related program messages may not be altered and must be printed even if only a part of the program is used. Adding further messages specifying any modifications is encouraged. 2) The program and its physics should be properly cited when used for academic publications ------------------------------------------------------------------ 2.1) The main software reference as designated by the program authors should always be cited. 2.2) In addition, the original literature on which the program is based should be cited to the extent that it is of relevance for a study, applying the same threshold criteria as for other literature. 2.3) When several programs are combined, they should all be mentioned, commensurate with their importance for the physics study at hand. 2.4) To make published results reproducible, the exact versions of the codes that were used and any relevant program and parameter modifications should be spelled out. POSTSCRIPT The copyright license of the software is the GPL v2 alone, therefore the above guidelines are not legally binding. However, we reserve the right to criticize offenders. The guidelines should always be combined with common sense, for interpretation and for issues not covered. Enquiries regarding the guidelines and related issues are encouraged and should be directed to the authors of the program. Please note that the program, including all its code and documentation, is intended for academic use and is delivered "as is" to be used at your own risk, without any guarantees. ---------------------------------------------------------------------- These guidelines were edited by Nils Lavesson and David Grellscheid for the MCnet collaboration, which has approved and agreed to respect them. MCnet is a Marie Curie Research Training Network funded under Framework Programme 6 contract MRTN-CT-2006-035606. pythia8-8.1.80.orig/htmldoc/MadGraph5Processes.html0000644000175000017500000001324512217615312020315 0ustar sunsun MadGraph 5 Processes

MadGraph 5 Processes

By far the easiest way to implement new processes into PYTHIA 8 is by using the matrix-element generator MadGraph 5. This program has an option to output the results of a matrix-element calculation as a set of PYTHIA 8 C++ classes (plus further auxiliary code), that can then be linked and used as semi-internal processes, meaning they are handled identically with normal internal ones. This way, MadGraph 5 can be used to implement processes from any model that can be written in terms of a Lagrangian. Any 2 -> 1, 2 -> 2 and 2 -> 3 processes can be implemented, the limit being set by the absence of efficient phase space generator algorithms for higher multiplicities in PYTHIA. Features such as s-channel resonances are automatically implemented in the process classes. Besides the process library and necessary model files, also an example main program is generated for each set of processes, which can be easily modified to perform the desired analyses.

In order to create a PYTHIA 8 process library with MadGraph 5, first download the MadGraph 5 package from https://launchpad.net/madgraph5, and untar the package. You can then specify the location of your pythia81xx directory in the file input/mg5_configuration.txt:
pythia8_path = ./pythia81xx
The location can be either relative (to the directory MadGraph5_v_x_x_x/.) or absolute.

For any model that is already implemented in the MadGraph 5 package, you can directly use the model. Start the MadGraph 5 interface bin/mg5, and do:

import model model_name  
generate your_process_in_mg5_syntax 
add process your_next_process_in_mg5_syntax 
...  
output pythia8 [path_to_pythia81xx_directory]

For examples of MG5 process syntax, please see http://madgraph.phys.ucl.ac.be/EXAMPLES/example_mg5.html or type help generate. If you specified the path to the pythia81xx directory in the mg5_configuration file, you do not need to enter it in the output command.

If your preferred model is found on the FeynRules model wiki page, http://feynrules.irmp.ucl.ac.be/wiki/ModelDatabaseMainPage, download the UFO (Universal FeynRules Output) tar file for the model, untar in the models/ directory, and use as above.

If you want to implement a new model which has not yet been implemented, you can do this either using the Mathematica package FeynRules (see http://feynrules.irmp.ucl.ac.be/) or directly edit the UFO model files of the most similar model in the models/ directory.

The resulting output from the output pythia8 command is:

  • A process directory Processes_modelname with the model information and the files needed for all processes defined for this model, placed in the pythia81xx main directory. The model files are Parameters_modelname.h/cc and HelAmps_modelname.h/cc, and the process files for each process class (with the same mass, spin and color of the initial/final state particles) are called Sigma_modelname_processname.h/cc. The directory also contains a makefile and a model parameter file param_card_modelname.dat.
  • An example main program in the directory examples/ (in the pythia81xx main directory) called main_modelname_N.cc and a corresponding makefile Makefile_modelname_N. This main program links in the process classes in the process directory described above. To run the example main program, just go to the examples/ directory and run
    make -f Makefile_modelname_N
    or run launch directly inside the MadGraph 5 command line interface.

Note that in order for PYTHIA 8 to be able to automatically decay any new particles, it is necessary to specify the branching ratios of the particles in the param_card file, see [Ska04,Alw07] for details.

For further technical details, please see the MadGraph 5 release paper [Alw11] and the semi-internal processes page.

Of course, as with MadGraph 4, MadGraph 5 can also output files of parton-level events according to the LHEF standard, that can be read in and processed further by PYTHIA 8. The advantage is that then the MadGraph 5 phase space generator can be used, which opens up for processes with more than three particles in the final state. The disadvantages are that it is less easy to mix and match with existing PYTHIA processes, and that one needs to regenerate and store large LHEF files for different kinematics cuts or parameter values.

Please cite the MadGraph 5 release paper [Alw11] if you use MadGraph 5 to generate process libraries for PYTHIA 8. pythia8-8.1.80.orig/htmldoc/RHadrons.html0000644000175000017500000002012512217615311016370 0ustar sunsun R-hadrons

R-hadrons

When a coloured SUSY particle is longer-lived than typical hadronization scales, i.e. around c*tau > 1 fm, or equivalently width Gamma < 0.2 GeV, it will have time to hadronize into a colour singlet hadronic state, a R-hadron. Currently a set of such R-hadrons have been implemented for the case of a long-lived gluino, stop or sbottom. Needless to say, the normal case would be that only one of them will be long-lived enough to form R-hadrons.

For simplicity all gluino-mesons are assumed to have light-flavour spin 1, since those are the lightest and favoured by spin-state counting. Further, all gluino-baryons are bookkept as having light-flavour spin 3/2, and flavours are listed in descending order. This is more for convenience of notation, however, since the normal baryon octet e.g. has no uuu = "p++" state. When a diquark is extracted, a mixture of spin 0 and spin 1 is allowed. Names and codes are essentially in agreement with the PDG conventions, e.g.
1000993 R0(~g g) (or gluinoball)
1009213 R+(~g u dbar) (or gluino-rho+)
1092214 R+(~g uud) (or gluino-Delta+)
For internal bookkeeping of momenta, the code 1009002, Rtemp(~g q), is used to denote the intermediate state formed when only one of the two string pieces attached to the gluino has broken.

For the stop- and sbottom-hadrons the spin counting is simpler, since it is entirely given by the constituent quark or diquark spin. Again names and codes follow PDG conventions, e.g.
1000612 R+(~t dbar)
1006211 R+(~t ud0)

The spin and electromagnetic charge of the new particle plays only a minor role in the hadronization process, that can be neglected to first approximation. Therefore it is possible to use the same R-hadrons framework instead for other BSM scenarios with long-lived coloured particles, e.g. with massive extra-dimensions copies of gluons and quarks, or with leptoquarks. This can be regulated by the switches below. Note that the codes and names of the R-hadrons is not changed when the heavy particle involved is switched, for reasons of administrative simplicity. R-hadron mass spectra and other relevant particle data is automatically updated to reflect the change, however.

flag  RHadrons:allow   (default = off)
Allows the gluino, stop and sbottom to hadronize if their respective widths are below the limit RHadrons:maxWidth.

parm  RHadrons:maxWidth   (default = 0.2; minimum = 0.0; maximum = 1.0)
The maximum width of the gluino for which it is possible to form R-hadrons, provided that RHadrons:allow is on.

mode  RHadrons:idGluino   (default = 1000021)
The gluino identity code. For other scenarios than SUSY this code could be changed to represent another long-lived uncharged colour octet particle, that then would be treated in the same spirit. Could be set to 0 to forbid any gluino R-hadron formation even when the above two criteria, RHadrons:allow and RHadrons:maxWidth, are met.

mode  RHadrons:idStop   (default = 1000006)
The lightest stop identity code. For other scenarios than SUSY this code could be changed to represent another long-lived charge 2/3 colour triplet particle, that then would be treated in the same spirit. As above it could be set to 0 to forbid any stop R-hadron formation.

mode  RHadrons:idSbottom   (default = 1000005)
The lightest sbottom identity code. For other scenarios than SUSY this code could be changed to represent another long-lived charge -1/3 colour triplet particle, that then would be treated in the same spirit. As above it could be set to 0 to forbid any sbottom R-hadron formation.

flag  RHadrons:allowDecay   (default = on)
Allows the R-hadrons to decay or not. If the gluino/stop/sbottom is stable or too long-lived to decay inside the detector this switch has no real function, since then no decays will be performed anyway. If the sparticle is so short-lived that it decays before reaching the beam pipe then having the decay on is the logical choice. So the interesting region is when the decays happens after the R-hadron has passed through part of the detector, and changed its momentum and quite possibly its flavour content before it is to decay. Then normal decays should be switched off, and the R-hadron tracked through matter by a program like GEANT [Kra04,Mac07]. After that, the new R-hadron info can be overwritten into the event record and the Pythia::forceRHadronDecay() method can be called to force this modified R-hadron to decay.

flag  RHadrons:setMasses   (default = on)
Use simple mass formulae to construct all available R-hadron masses based on the currently initialized gluino/squark masses and the constituent masses of the other partons in the hadron. If you switch this off, it is your responsibility to set each of the R-hadron masses on your own, and set them in an internally consistent way. If you mess up on this you may generate accordingly crazy results. Specifically, it is to be assumed that none of the R-hadrons has a mass below its constituent sparticle, i.e. that the light degrees of freedom and the additional confinement gluon field gives a net positive contribution to the R-hadron mass.

parm  RHadrons:probGluinoball   (default = 0.1; minimum = 0.0; maximum = 1.0)
The fraction of produced gluino R-hadrons that are contain a "valence" gluon, with the rest containing a meson or baryon quark flavour content.

parm  RHadrons:mOffsetCloud   (default = 0.2; minimum = 0.0)
Extra mass (in GeV) added to each of the one or two extra constituent masses in an R-hadron, to calculate the mass of a R-hadron. The same offset is also used when the R-hadron momentum and mass is split between the squark or gluino and the one or two light (di)quarks, one for a squark and two for a gluino. Thus once or twice this amount represents a part of the nominal squark or gluino mass that will not decay weakly, since it is taken to correspond to the cloud of gluons that surround the squark or gluino.

parm  RHadrons:mCollapse   (default = 1.0; minimum = 0.0)
A colour singlet system with an invariant mass less than this amount, above the R-hadron mass with the given flavour content, is assumed to collapse to this single R-hadron, whereas a full fragmentation handling is applied above this mass.

parm  RHadrons:diquarkSpin1   (default = 0.5; minimum = 0.0; maximum = 1.0)
Probability that a diquark extracted from the flavour code of a gluino R-hadron should be assigned spin 1, with the rest being spin 0. Does not apply for two identical quarks, where spin 1 is only possibility. Note that gluino R-hadron codes for simplicity are assigned as if spin is 1 always, and so give no guidance. For stop and sbottom the diquark spin is preserved in the particle code, so there is no corresponding issue. pythia8-8.1.80.orig/htmldoc/pythia99.gif0000644000175000017500000000535312217346217016145 0ustar sunsunGIF89acd3̙3f33f333!,cdI8E^ aa@blrEN;0D;UB9OIr+2(s8tGNT@BB='}t^\B{=yZWDWDi9=e){5Vn'WQ=,,iq_6*Ƅ,NĔ:a|uTXҚ w-*1VTNזn> ! RC2Rk? AX6qJL)woU?Ҙ`J Ґ2>[EUCApCDME Ϊg""ةXrYZW.|H72 RE+@w2F!mh*Z],Z7ǰ݇dIjBs@j8׃=FEZ3tődZ`((-Q &A7 X"bo^vFr#PꅖIdOi ":_VK\ ~uLj?.,N|n8T-h̀%S ^B 80L.cF7ǼdGY guD[<^:OQZ&ICKLE!0^q(fυF!Pdɋ3$0wJsDk o)/-dz0:%~R2XT,VY藆6Ox*b+YbKcAdw1˼!i`%,699mhG#"[NM-@dyCjLqO`&'|5IY̫M{,@ҷ"8B*لd%d jwG @'͚(̕H\v3a/YDS"\L.ƌW"wxՒwYUN>Bs 9iQަǪv` &c>W`mG]5c ^%p Ɲ$+z9e(MjҰ_ 2:qpƩ}^bS`0NRqFoVEa #K[@kMTz_RW2j dkAL$r;qd4pr+1W$?@ v)M>2'ҵUHTSAaѸ.I9b7[Y \~8<=Gy4!ռ!.xP/)X0Qzk'8׎ Y'RJ蔤Yroߤx%8lf몥r7@(Yv2ݖ#0A&Qi(,e/y3 ժR>Ba  @^'s^X` w[m&&ԼO Kds_ +$Á]C`SB@9;a&aPL }E1Gwv.ƪi)p1c,^Nk?]0&.mE!&b)^B>+-E'&f*;?YE$8C0·FY!t炢 #%.mUSpAӘ֙"C~{BQia|E144|cH`ڈBn}SD 1zѡc8+A7~~-0VgpFO=`,wytpx 2V p9SP*QbC]Vxp6|G``u&A1Q́-hc9($NE8C3FXOX[cuQHkWx.YYY; pythia8-8.1.80.orig/htmldoc/COPYING0000644000175000017500000004310312217346212015017 0ustar sunsun GNU GENERAL PUBLIC LICENSE Version 2, June 1991 Copyright (C) 1989, 1991 Free Software Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA Everyone is permitted to copy and distribute verbatim copies of this license document, but changing it is not allowed. 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Here is a sample; alter the names: Yoyodyne, Inc., hereby disclaims all copyright interest in the program `Gnomovision' (which makes passes at compilers) written by James Hacker. , 1 April 1989 Ty Coon, President of Vice This General Public License does not permit incorporating your program into proprietary programs. If your program is a subroutine library, you may consider it more useful to permit linking proprietary applications with the library. If this is what you want to do, use the GNU Lesser General Public License instead of this License. pythia8-8.1.80.orig/htmldoc/BeamRemnants.html0000644000175000017500000004024112217615311017225 0ustar sunsun Beam Remnants

Beam Remnants

Introduction

The BeamParticle class contains information on all partons extracted from a beam (so far). As each consecutive multiparton interaction defines its respective incoming parton to the hard scattering a new slot is added to the list. This information is modified when the backwards evolution of the spacelike shower defines a new initiator parton. It is used, both for the multiparton interactions and the spacelike showers, to define rescaled parton densities based on the x and flavours already extracted, and to distinguish between valence, sea and companion quarks. Once the perturbative evolution is finished, further beam remnants are added to obtain a consistent set of flavours. The current physics framework is further described in [Sjo04].

The introduction of rescattering in the multiparton interactions framework further complicates the processing of events. Specifically, when combined with showers, the momentum of an individual parton is no longer uniquely associated with one single subcollision. Nevertheless the parton is classified with one system, owing to the technical and administrative complications of more complete classifications. Therefore the addition of primordial kT to the subsystem initiator partons does not automatically guarantee overall pT conservation. Various tricks are used to minimize the mismatch, with a brute force shift of all parton pT's as a final step.

Much of the above information is stored in a vector of ResolvedParton objects, which each contains flavour and momentum information, as well as valence/companion information and more. The BeamParticle method list() shows the contents of this vector, mainly for debug purposes.

The BeamRemnants class takes over for the final step of adding primordial kT to the initiators and remnants, assigning the relative longitudinal momentum sharing among the remnants, and constructing the overall kinematics and colour flow. This step couples the two sides of an event, and could therefore not be covered in the BeamParticle class, which only considers one beam at a time.

The methods of these classes are not intended for general use, and so are not described here.

In addition to the parameters described on this page, note that the choice of parton densities is made in the Pythia class. Then pointers to the pdf's are handed on to BeamParticle at initialization, for all subsequent usage.

Primordial kT

The primordial kT of initiators of hard-scattering subsystems are selected according to Gaussian distributions in p_x and p_y separately. The widths of these distributions are chosen to be dependent on the hard scale of the central process and on the mass of the whole subsystem defined by the two initiators:
sigma = (sigma_soft * Q_half + sigma_hard * Q) / (Q_half + Q) * m / (m_half + m)
Here Q is the hard-process renormalization scale for the hardest process and the pT scale for subsequent multiparton interactions, m the mass of the system, and sigma_soft, sigma_hard, Q_half and m_half parameters defined below. Furthermore each separately defined beam remnant has a distribution of width sigma_remn, independently of kinematical variables.

flag  BeamRemnants:primordialKT   (default = on)
Allow or not selection of primordial kT according to the parameter values below.

parm  BeamRemnants:primordialKTsoft   (default = 0.5; minimum = 0.)
The width sigma_soft in the above equation, assigned as a primordial kT to initiators in the soft-interaction limit.

parm  BeamRemnants:primordialKThard   (default = 2.0; minimum = 0.)
The width sigma_hard in the above equation, assigned as a primordial kT to initiators in the hard-interaction limit.

parm  BeamRemnants:halfScaleForKT   (default = 1.; minimum = 0.)
The scale Q_half in the equation above, defining the half-way point between hard and soft interactions.

parm  BeamRemnants:halfMassForKT   (default = 1.; minimum = 0.)
The scale m_half in the equation above, defining the half-way point between low-mass and high-mass subsystems. (Kinematics construction can easily fail if a system is assigned a primordial kT value higher than its mass, so the mass-dampening is intended to reduce some troubles later on.)

parm  BeamRemnants:primordialKTremnant   (default = 0.4; minimum = 0.)
The width sigma_remn, assigned as a primordial kT to beam-remnant partons.

A net kT imbalance is obtained from the vector sum of the primordial kT values of all initiators and all beam remnants. This quantity is compensated by a shift shared equally between all partons, except that the dampening factor m / (m_half + m) is again used to suppress the role of small-mass systems.

Note that the current sigma definition implies that <pT^2> = <p_x^2>+ <p_y^2> = 2 sigma^2. It thus cannot be compared directly with the sigma of nonperturbative hadronization, where each quark-antiquark breakup corresponds to <pT^2> = sigma^2 and only for hadrons it holds that <pT^2> = 2 sigma^2. The comparison is further complicated by the reduction of primordial kT values by the overall compensation mechanism.

flag  BeamRemnants:rescatterRestoreY   (default = off)
Is only relevant when rescattering is switched on in the multiparton interactions scenario. For a normal interaction the rapidity and mass of a system is preserved when primordial kT is introduced, by appropriate modification of the incoming parton momenta. Kinematics construction is more complicated for a rescattering, and two options are offered. Differences between these can be used to explore systematic uncertainties in the rescattering framework.
The default behaviour is to keep the incoming rescattered parton as is, but to modify the unrescattered incoming parton so as to preserve the invariant mass of the system. Thereby the rapidity of the rescattering is modified.
The alternative is to retain the rapidity (and mass) of the rescattered system when primordial kT is introduced. This is made at the expense of a modified longitudinal momentum of the incoming rescattered parton, so that it does not agree with the momentum it ought to have had by the kinematics of the previous interaction.
For a double rescattering, when both incoming partons have already scattered, there is no obvious way to retain the invariant mass of the system in the first approach, so the second is always used.

Colour flow

The colour flows in the separate subprocesses defined in the multiparton-interactions scenario are tied together via the assignment of colour flow in the beam remnant. This is not an unambiguous procedure, but currently no parameters are directly associated with it. However, a simple "minimal" procedure of colour flow only via the beam remnants does not result in a scenario in agreement with data, notably not a sufficiently steep rise of <pT>(n_ch). The true origin of this behaviour and the correct mechanism to reproduce it remains one of the big unsolved issues at the borderline between perturbative and nonperturbative QCD. As a simple attempt, an additional step is introduced, wherein the gluons of a lower-pT system are merged with the ones in a higher-pT one.

flag  BeamRemnants:reconnectColours   (default = on)
Allow or not a system to be merged with another one.

parm  BeamRemnants:reconnectRange   (default = 10.0; minimum = 0.; maximum = 10.)
A system with a hard scale pT can be merged with one of a harder scale with a probability that is pT0_Rec^2 / (pT0_Rec^2 + pT^2), where pT0_Rec is reconnectRange times pT0, the latter being the same energy-dependent dampening parameter as used for multiparton interactions. Thus it is easy to merge a low-pT system with any other, but difficult to merge two high-pT ones with each other.

The procedure is used iteratively. Thus first the reconnection probability P = pT0_Rec^2 / (pT0_Rec^2 + pT^2) of the lowest-pT system is found, and gives the probability for merger with the second-lowest one. If not merged, it is tested with the third-lowest one, and so on. For the m'th higher system the reconnection probability thus becomes (1 - P)^(m-1) P. That is, there is no explicit dependence on the higher pT scale, but implicitly there is via the survival probability of not already having been merged with a lower-pT system. Also note that the total reconnection probability for the lowest-pT system in an event with n systems becomes 1 - (1 - P)^(n-1). Once the fate of the lowest-pT system has been decided, the second-lowest is considered with respect to the ones above it, then the third-lowest, and so on.

Once it has been decided which systems should be joined, the actual merging is carried out in the opposite direction. That is, first the hardest system is studied, and all colour dipoles in it are found (including to the beam remnants, as defined by the holes of the incoming partons). Next each softer system to be merged is studied in turn. Its gluons are, in decreasing pT order, inserted on the colour dipole i,j that gives the smallest (p_g p_i)(p_g p_j)/(p_i p_j), i.e. minimizes the "disturbance" on the existing dipole, in terms of pT^2 or Lambda measure (string length). The insertion of the gluon means that the old dipole is replaced by two new ones. Also the (rather few) quark-antiquark pairs that can be traced back to a gluon splitting are treated in close analogy with the gluon case. Quark lines that attach directly to the beam remnants cannot be merged but are left behind.

The joining procedure can be viewed as a more sophisticated variant of the one introduced already in [Sjo87]. Clearly it is ad hoc. It hopefully captures some elements of truth. The lower pT scale a system has the larger its spatial extent and therefore the larger its overlap with other systems. It could be argued that one should classify individual initial-state partons by pT rather than the system as a whole. However, for final-state radiation, a soft gluon radiated off a hard parton is actually produced at late times and therefore probably less likely to reconnect. In the balance, a classification by system pT scale appears sensible as a first try.

Note that the reconnection is carried out before resonance decays are considered. Colour inside a resonance therefore is not reconnected. This is a deliberate choice, but certainly open to discussion and extensions at a later stage, as is the rest of this procedure.

Further variables

mode  BeamRemnants:maxValQuark   (default = 3; minimum = 0; maximum = 5)
The maximum valence quark kind allowed in acceptable incoming beams, for which multiparton interactions are simulated. Default is that hadrons may contain u, d and s quarks, but not c and b ones, since sensible kinematics has not really been worked out for the latter.

mode  BeamRemnants:companionPower   (default = 4; minimum = 0; maximum = 4)
When a sea quark has been found, a companion antisea quark ought to be nearby in x. The shape of this distribution can be derived from the gluon mother distribution convoluted with the g -> q qbar splitting kernel. In practice, simple solutions are only feasible if the gluon shape is assumed to be of the form g(x) ~ (1 - x)^p / x, where p is an integer power, the parameter above. Allowed values correspond to the cases programmed.
Since the whole framework is approximate anyway, this should be good enough. Note that companions typically are found at small Q^2, if at all, so the form is supposed to represent g(x) at small Q^2 scales, close to the lower cutoff for multiparton interactions.

When assigning relative momentum fractions to beam-remnant partons, valence quarks are chosen according to a distribution like (1 - x)^power / sqrt(x). This power is given below for quarks in mesons, and separately for u and d quarks in the proton, based on the approximate shape of low-Q^2 parton densities. The power for other baryons is derived from the proton ones, by an appropriate mixing. The x of a diquark is chosen as the sum of its two constituent x values, and can thus be above unity. (A common rescaling of all remnant partons and particles will fix that.) An additional enhancement of the diquark momentum is obtained by its x value being rescaled by the valenceDiqEnhance factor.

parm  BeamRemnants:valencePowerMeson   (default = 0.8; minimum = 0.)
The abovementioned power for valence quarks in mesons.

parm  BeamRemnants:valencePowerUinP   (default = 3.5; minimum = 0.)
The abovementioned power for valence u quarks in protons.

parm  BeamRemnants:valencePowerDinP   (default = 2.0; minimum = 0.)
The abovementioned power for valence d quarks in protons.

parm  BeamRemnants:valenceDiqEnhance   (default = 2.0; minimum = 0.5; maximum = 10.)
Enhancement factor for valence diquarks in baryons, relative to the simple sum of the two constituent quarks.

flag  BeamRemnants:allowJunction   (default = on)
The off option is intended for debug purposes only, as follows. When more than one valence quark is kicked out of a baryon beam, as part of the multiparton interactions scenario, the subsequent hadronization is described in terms of a junction string topology. This description involves a number of technical complications that may make the program more unstable. As an alternative, by switching this option off, junction configurations are rejected (which gives an error message that the remnant flavour setup failed), and the multiparton interactions and showers are redone until a junction-free topology is found. pythia8-8.1.80.orig/htmldoc/Index.html0000644000175000017500000001517712217615311015732 0ustar sunsun Index Pythia logo

PYTHIA 8 Index

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A Second Hard Process
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  --   CKKW-L Merging
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Separate documents

Brief Introduction
Worksheet pythia8-8.1.80.orig/htmldoc/FourthGenerationProcesses.html0000644000175000017500000001763212217615311022033 0ustar sunsun Fourth-Generation Processes

Fourth-Generation Processes

A fourth generation can be accommodated within the Standard Model, without the introduction of any new concepts. Many experimental constraints exist, but it has not been fully excluded. Therefore we offer a simple implementation, along the lines of the top. It could also be useful as a template for studies of other new particles with similar characteristics.

The fourth generation are given names as in the third, but with a prime, i.e. b' with PDG code 7, t' with code 8, tau' with code 17, and nu'_tau with code 18. Most important for you is to assign a mass hierarchy, to decide which fermions can decay into which. The current implementation assumes that mass splittings are big enough that fourth-generation fermions can decay to third-generation ones by the emission of an on-shell W. To this end, the standard three-generation CKM mixing matrix has been extended to include a fourth generation, see below. Since no mixing has been implemented in the neutrino sector it would be assumed that the lighter of tau' and nu'_tau is stable. No decay modes have been implemented that go beyond the Standard Model, so modifications would be needed if e.g. also SUSY is included in the game.

Production processes

1) b' processes

Different ways to produce b' quarks, singly or in pairs. For a b' t' pair see section 3 below.

flag  FourthBottom:all   (default = off)
Common switch for the group of b' production. Also includes the process f fbar' -> t' b'bar in section 3 below.

flag  FourthBottom:gg2bPrimebPrimebar   (default = off)
Scatterings g g -> b' b'bar. Code 801.

flag  FourthBottom:qqbar2bPrimebPrimebar   (default = off)
Scatterings q qbar -> b' b'bar by gluon exchange. Code 802.

flag  FourthBottom:qq2bPrimeq(t:W)   (default = off)
Scatterings q q' -> b' q'' by t-channel exchange of a W^+- boson. Code 803.

flag  FourthBottom:ffbar2bPrimebPrimebar(s:gmZ)   (default = off)
Scatterings f fbar -> b' b'bar by s-channel exchange of a gamma^*/Z^0 boson. Code 804.

flag  FourthBottom:ffbar2bPrimeqbar(s:W)   (default = off)
Scatterings f fbar' -> b' qbar'' by s-channel exchange of a W^+- boson. Here q'' is either u or c. Code 805.

flag  FourthBottom:ffbar2bPrimetbar(s:W)   (default = off)
Scatterings f fbar' -> b' tbar by s-channel exchange of a W^+- boson. Code 806.

2) t' processes

Different ways to produce t' quarks, singly or in pairs. For a b' t' pair see section 3 below.

flag  FourthTop:all   (default = off)
Common switch for the group of t' production. Also includes the process f fbar' -> t' b'bar in section 3 below.

flag  FourthTop:gg2tPrimetPrimebar   (default = off)
Scatterings g g -> t' t'bar. Code 821.

flag  FourthTop:qqbar2tPrimetPrimebar   (default = off)
Scatterings q qbar -> t' t'bar by gluon exchange. Code 822.

flag  FourthTop:qq2tPrimeq(t:W)   (default = off)
Scatterings q q' -> t' q'' by t-channel exchange of a W^+- boson. Code 823.

flag  FourthTop:ffbar2tPrimetPrimebar(s:gmZ)   (default = off)
Scatterings f fbar -> t' t'bar by s-channel exchange of a gamma^*/Z^0 boson. Code 824.

flag  FourthTop:ffbar2tPrimeqbar(s:W)   (default = off)
Scatterings f fbar' -> t' qbar'' by s-channel exchange of a W^+- boson. Code 825.

3) Pair-processes with different flavours

Different ways to produce two different fourth-generation fermions.

flag  FourthPair:ffbar2tPrimebPrimebar(s:W)   (default = off)
Scatterings f fbar' -> t' b'bar by s-channel exchange of a W^+- boson. Code 841.

flag  FourthPair:ffbar2tauPrimenuPrimebar(s:W)   (default = off)
Scatterings f fbar' -> tau' nu'_taubar by s-channel exchange of a W^+- boson. Code 842.

Missing in this list is scatterings q q' -> t' b' by t-channel exchange of a W^+- boson, since currently the matrix element for such processes have not been implemented for two massive particles in the final state. Since this process would involve two CKM-suppressed vertices it ought to be small.

Parameters

The Cabibbo-Kobayashi-Maskawa matrix is extended by seven further values. So as not to mess up the Standard Model, the normal 3 * 3 matrix is kept unitary, and so the new off-diagonal elements lead to a slight breaking of this. For exploratory studies this should be good enough; more detailed 4 * 4 tunes to data would only make sense the day there are evidence for the existence of a fourth generation.

parm  FourthGeneration:VubPrime   (default = 0.001; minimum = 0.0; maximum = 1.0)
The V_ub' matrix element in the 4 * 4 CKM matrix.

parm  FourthGeneration:VcbPrime   (default = 0.01; minimum = 0.0; maximum = 1.0)
The V_cb' matrix element in the 4 * 4 CKM matrix.

parm  FourthGeneration:VtbPrime   (default = 0.1; minimum = 0.0; maximum = 1.0)
The V_tb' matrix element in the 4 * 4 CKM matrix.

parm  FourthGeneration:VtPrimed   (default = 0.001; minimum = 0.0; maximum = 1.0)
The V_t'd matrix element in the 4 * 4 CKM matrix.

parm  FourthGeneration:VtPrimes   (default = 0.01; minimum = 0.0; maximum = 1.0)
The V_t's matrix element in the 4 * 4 CKM matrix.

parm  FourthGeneration:VtPrimeb   (default = 0.1; minimum = 0.0; maximum = 1.0)
The V_t'b matrix element in the 4 * 4 CKM matrix.

parm  FourthGeneration:VtPrimebPrime   (default = 0.99; minimum = 0.0; maximum = 1.0)
The V_t'b' matrix element in the 4 * 4 CKM matrix. pythia8-8.1.80.orig/htmldoc/ParticleDecays.html0000644000175000017500000004461512217615311017556 0ustar sunsun Particle Decays

Particle Decays

The ParticleDecays class performs the sequential decays of all unstable hadrons produced in the string fragmentation stage, i.e. up to and including b hadrons and their decay products, such as the tau lepton. It is not to be used for the decay of more massive resonances, such as top, Z^0 or SUSY, where decays must be performed already at the ProcessLevel of the event generation.

The decay description essentially copies the one present in PYTHIA since many years, but with some improvements, e.g. in the decay tables and the number of decay models available. Recently a more sophisticated handling of tau decays has also been introduced. Some issues may need further polishing.

Variables determining whether a particle decays

Before a particle is actually decayed, a number of checks are made.

(i) Decay modes must have been defined for the particle kind; tested by the canDecay() method of Event (and ParticleData).

(ii) The main switch for allowing this particle kind to decay must be on; tested by the mayDecay() method of Event (and ParticleData).

(iii) Particles may be requested to have a nominal proper lifetime tau0 below a threshold.

flag  ParticleDecays:limitTau0   (default = off)
When on, only particles with tau0 < tau0Max are decayed.

parm  ParticleDecays:tau0Max   (default = 10.; minimum = 0.)
The above tau0Max, expressed in mm/c.

(iv) Particles may be requested to have an actual proper lifetime tau below a threshold.

flag  ParticleDecays:limitTau   (default = off)
When on, only particles with tau < tauMax are decayed.

parm  ParticleDecays:tauMax   (default = 10.; minimum = 0.)
The above tauMax, expressed in mm/c.
In order for this and the subsequent tests to work, a tau is selected and stored for each particle, whether in the end it decays or not. (If each test would use a different temporary tau it would lead to inconsistencies.)

(v) Particles may be requested to decay within a given distance of the origin.

flag  ParticleDecays:limitRadius   (default = off)
When on, only particles with a decay within a radius r < rMax are decayed. There is assumed to be no magnetic field or other detector effects.

parm  ParticleDecays:rMax   (default = 10.; minimum = 0.)
The above rMax, expressed in mm.

(vi) Particles may be requested to decay within a given cylindrical volume around the origin.

flag  ParticleDecays:limitCylinder   (default = off)
When on, only particles with a decay within a volume limited by rho = sqrt(x^2 + y^2) < xyMax and |z| < zMax are decayed. There is assumed to be no magnetic field or other detector effects.

parm  ParticleDecays:xyMax   (default = 10.; minimum = 0.)
The above xyMax, expressed in mm.

parm  ParticleDecays:zMax   (default = 10.; minimum = 0.)
The above zMax, expressed in mm.

Mixing

flag  ParticleDecays:mixB   (default = on)
Allow or not B^0 - B^0bar and B_s^0 - B_s^0bar mixing.

parm  ParticleDecays:xBdMix   (default = 0.776; minimum = 0.74; maximum = 0.81)
The mixing parameter x_d = Delta(m_B^0)/Gamma_B^0 in the B^0 - B^0bar system. (Default from RPP2006.)

parm  ParticleDecays:xBsMix   (default = 26.05; minimum = 22.0; maximum = 30.0)
The mixing parameter x_s = Delta(m_B_s^0)/Gamma_B_s^0 in the B_s^0 - B_s^0bar system. (Delta-m from CDF hep-ex-0609040, Gamma from RPP2006.)

Tau decays

A new machinery has been introduced to handle tau lepton decays, with helicity information related to the production process and with the form of the hadronic current fitted to data. It is largely based on the corresponding Herwig++ implementation [Gre07], with some input from Tauola [Jad90]. A complete writeup is in preparation, but meanwhile a short summary can be found at [Ilt12].

For taus in external processes, interfaced with Les Houches Accord information available, e.g. via Les Houches Event Files (LHEF), the new machinery interprets the SPINUP number for tau leptons as giving their helicity, and decays them accordingly. The only exceptions are when a specific polarization is forced by the user (see below), which then overrides the SPINUP value, or when SPINUP has the special value 9 (unpolarized). In the latter case, PYTHIA defaults back to attempting to determine the helicity structure from the production process, in the same way as for internal processes.

This new machinery is on by default, but it is possible to revert to the simpler old decay handling, e.g. to study differences. Furthermore the spin tracing framework does not yet cover all possibilities; notably it cannot handle taus coming from SUSY decay chains (except via LHEF), so it makes sense to switch off the new machinery in such instances, for speed reasons if nothing else. In case only one tau mother species is undefined, the polarization involved can be set by hand.

mode  ParticleDecays:sophisticatedTau   (default = 1; minimum = 0; maximum = 3)
Choice of tau decay model.
option 0 : old decay model, with isotropic decays. When reading LHEF files, the SPINUP digit will be ignored.
option 1 : sophisticated decays where tau polarization is calculated from the tau production mechanism. When reading LHEF files, the SPINUP digit will be used.
option 2 : sophisticated decays as above, but additionally tau polarization is set to ParticleDecaus:tauPolarization for taus produced from ParticleDecays:tauMother. When reading LHEF files, this overrides the SPINUP digit.
option 3 : sophisticated decays where tau polarization is set to ParticleDecaus:tauPolarization for all tau decays. When reading LHEF files, this overrides the SPINUP digit.
Note: options 2 and 3, to force a specific tau polarization, only affect the decay of the tau. The angular distribution of the tau itself, given by its production, is not modified by these options. If you want, e.g., a righthanded W, or a SUSY decay chain, the kinematics should be handled by the corresponding cross section class(es), supplemented by the resonance decay one(s). The options here could then still be used to ensure the correct polarization at the tau decay stage.

parm  ParticleDecays:tauPolarization   (default = 0; minimum = -1.; maximum = 1.)
Polarization of the tau when mode 2 or 3 of ParticleDecays:sophisticatedTau is selected.

mode  ParticleDecays:tauMother   (default = 0; minimum = 0)
Mother of the tau for forced polarization when mode 2 of ParticleDecays:sophisticatedTau is selected. You should give the positive identity code; to the extent an antiparticle exists it will automatically obtain the inverse polarization.

QED radiation

So far PYTHIA does not have any generic machinery for handling QED radiation in normal particle decays. In order to include this, a program like Photos [Bar94, Dav10] could be used as an afterburner. In a few cases, however, the existing shower machinery can be used also here: for two-body decays to a lepton pair (l^+ l^- or l^+- nu_l). Such decays are mediated by gamma^*/Z^0/W^+- exchange, for which PYTHIA does have an existing machinery that can be applied, including first-order matrix-element corrections for the first (hardest) photon emission.

flag  ParticleDecays:allowPhotonRadiation   (default = off)
Allow or not photon radiations in decays to a lepton pair, see above.
Note: The current default is to have radiation switched off, in order to avoid double-counting of emissions if you link to an external QED-radiation program, as is the norm in many collaborations.

Other variables

parm  ParticleDecays:mSafety   (default = 0.0005; minimum = 0.; maximum = 0.01)
Minimum mass difference required between the decaying mother mass and the sum of the daughter masses, kept as a safety margin to avoid numerical problems in the decay generation.

parm  ParticleDecays:sigmaSoft   (default = 0.5; minimum = 0.2; maximum = 2.)
In semileptonic decays to more than one hadron, such as B -> nu l D pi, decay products after the first three are dampened in momentum by an explicit weight factor exp(-p^2/sigmaSoft^2), where p is the three-momentum in the rest frame of the decaying particle. This takes into account that such further particles come from the fragmentation of the spectator parton and thus should be soft.

When a decay mode is defined in terms of a partonic content, a random multiplicity (and a random flavour set) of hadrons is to be picked, especially for some charm and bottom decays. This is done according to a Poissonian distribution, for n_p normal particles and n_q quarks the average value is chosen as
n_p/ 2 + n_q/4 + multIncrease * ln ( mDiff / multRefMass)
with mDiff the difference between the decaying particle mass and the sum of the normal-particle masses and the constituent quark masses. For gluon systems multGoffset offers and optional additional term to the multiplicity. The lowest possible multiplicity is n_p + n_q/2 (but at least 2) and the highest possible 10. If the picked hadrons have a summed mass above that of the mother a new try is made, including a new multiplicity. These constraints imply that the actual average multiplicity does not quite agree with the formula above.

parm  ParticleDecays:multIncrease   (default = 4.; minimum = 2.; maximum = 6.)
The above multIncrease parameter, except for meMode = 23.

parm  ParticleDecays:multIncreaseWeak   (default = 2.5; minimum = 1.; maximum = 4.)
The above multIncrease parameter, specifically for meMode = 23. Here the weak decay implies that only the virtual W mass should contribute to the production of new particles, rather than the full meson mass.

parm  ParticleDecays:multRefMass   (default = 0.7; minimum = 0.2; maximum = 2.0)
The above multRefMass parameter.

parm  ParticleDecays:multGoffset   (default = 0.5; minimum = 0.0; maximum = 2.0)
The above multGoffset parameter.

parm  ParticleDecays:colRearrange   (default = 0.5; minimum = 0.; maximum = 1.0)
When a decay is given as a list of four partons to be turned into hadrons (primarily for modes 41 - 80) it is assumed that they are listed in pairs, as a first and a second colour singlet, which could give rise to separate sets of hadrons. Here colRearrange is the probability that this original assignment is not respected, and default corresponds to no memory of this original colour topology.

flag  ParticleDecays:FSRinDecays   (default = true)
When a particle decays to q qbar, g g, g g g or gamma g g, with meMode > 90, allow or not a shower to develop from it, before the partonic system is hadronized. (The typical example is Upsilon decay.) In addition, some variables defined for string fragmentation and for flavour production are used also here.

Modes for Matrix Element Processing

Some decays can be treated better than what pure phase space allows, by reweighting with appropriate matrix elements. In others a partonic content has to be converted to a set of hadrons. The presence of such corrections is signaled by a nonvanishing meMode() value for a decay mode in the particle data table. The list of allowed possibilities almost agrees with the PYTHIA 6 ones, but several obsolete choices have been removed, a few new introduced, and most have been moved for better consistency. Here is the list of currently allowed meMode() codes:
  • 0 : pure phase space of produced particles ("default"); input of partons is allowed and then the partonic content is converted into the minimal number of hadrons (i.e. one per parton pair, but at least two particles in total)
  • 1 : omega and phi -> pi+ pi- pi0
  • 2 : polarization in V -> PS + PS (V = vector, PS = pseudoscalar), when V is produced by PS -> PS + V or PS -> gamma + V
  • 11 : Dalitz decay into one particle, in addition to the lepton pair (also allowed to specify a quark-antiquark pair that should collapse to a single hadron)
  • 12 : Dalitz decay into two or more particles in addition to the lepton pair
  • 13 : double Dalitz decay into two lepton pairs
  • 21 : decay to phase space, but weight up neutrino_tau spectrum in tau decay
  • 22 : weak decay; if there is a quark spectator system it collapses to one hadron; for leptonic/semileptonic decays the V-A matrix element is used, for hadronic decays simple phase space
  • 23 : as 22, but require at least three particles in decay
  • 31 : decays of type B -> gamma X, very primitive simulation where X is given in terms of its flavour content, the X multiplicity is picked according to a geometrical distribution with average number 2, and the photon energy spectrum is weighted up relative to pure phase space
  • 42 - 50 : turn partons into a random number of hadrons, picked according to a Poissonian with average value as described above, but at least code - 40 and at most 10, and then distribute then in pure phase space; make a new try with another multiplicity if the sum of daughter masses exceed the mother one
  • 52 - 60 : as 42 - 50, with multiplicity between code - 50 and 10, but avoid already explicitly listed non-partonic channels
  • 62 - 70 : as 42 - 50, but fixed multiplicity code - 60
  • 72 - 80 : as 42 - 50, but fixed multiplicity code - 70, and avoid already explicitly listed non-partonic channels
  • 91 : decay to q qbar or g g, which should shower and hadronize
  • 92 : decay onium to g g g or g g gamma (with matrix element), which should shower and hadronize
  • 100 - : reserved for the description of partial widths of resonances
Three special decay product identity codes are defined.
  • 81: remnant flavour. Used for weak decays of c and b hadrons, where the c or b quark decays and the other quarks are considered as a spectator remnant in this decay. In practice only used for baryons with multiple c and b quarks, which presumably would never be used, but have simple (copied) just-in-case decay tables. Assumed to be last decay product.
  • 82: random flavour, picked by the standard fragmentation flavour machinery, used to start a sequence of hadrons, for matrix element codes in 41 - 80. Assumed to be first decay product, with -82 as second and last. Where multiplicity is free to be picked it is selected as for normal quarkonic systems. Currently unused.
  • 83: as for 82, with matched pair 83, -83 of decay products. The difference is that here the pair is supposed to come from a closed gluon loop (e.g. eta_c -> g g) and so have a somewhat higher average multiplicity than the simple string assumed for 82, see the ParticleDecays:multGoffset parameter above.
pythia8-8.1.80.orig/htmldoc/HepMCInterface.html0000644000175000017500000002007212217615312017427 0ustar sunsun HepMC Interface

HepMC Interface

An interface to the HepMC [Dob01] standard event record format has been provided by M. Kirsanov. To use it, the relevant libraries need to be linked, as explained in the README and README.HepMC files. Only version 2.06 (or later) of HepMC is supported as of 1 January 2013, by agreement with the LHC experimental community.

The (simple) procedure to translate PYTHIA 8 events into HepMC ones is illustrated in the main41.cc, main42.cc main61.cc and main62.cc main programs. At the core is a call to the

HepMC::Pythia8ToHepMC::fill_next_event( pythia, hepmcevt, ievnum = -1) 
which takes a reference of the generator object and uses it, on the one hand, to read out and convert the event record in pythia.event and, on the other hand, to extract and store parton-density (PDF), cross section and other information for the hard subprocess from pythia.info. There is also an alternative form that does not requires access to the full pythia object, but only the event record, at the expense of a reduced information storage, see below.

While PYTHIA always stores momenta in units of GeV, with c = 1, HepMC nowadays can be built either for MeV or GeV as default, a choice that can then be overridden on an event-by-event basis, see e.g. the main41.cc code. When filling the HepMC event record, PYTHIA will convert to the unit specified for the current HepMC event record.

Also for length units there are choices, and again the PYTHIA interface will convert to the units set for the HepMC event record. Here the mm choice of PYTHIA seems to be shared by most other programs, and is HepMC default.

The status code is now based on the new standard introduced for HepMC 2.05, see the Event::statusHepMC(...) conversion routine for details.

The current values from pythia.info.sigmaGen() and pythia.info.sigmaErr() are stored for each event, multiplied by 10^9 to convert from mb to pb. Note that PYTHIA improves its accuracy by Monte Carlo integration in the course of the run, so the values associated with the last generated event should be the most accurate ones. If events also come with a dimensional weight, like in some Les Houches strategies, this weight is in units of pb.

The public methods

Here comes a complete list of all public methods of the Pythia8ToHepMC class in the HepMC (not Pythia8!) namespace.

Pythia8ToHepMC::Pythia8ToHepMC()  
virtual Pythia8ToHepMC::~Pythia8ToHepMC()  
the constructor and destructor take no arguments.

bool Pythia8ToHepMC::fill_next_event( Pythia8::Pythia& pythia, GenEvent* evt, int ievnum = -1)  
convert a Pythia event to a HepMC one. Will return true if succeeded.
argument pythia : the input Pythia generator object, from which both the event and other information can be obtained.
argument evt : the output GenEvt event, in its standard form.
argument iev : set the event number of the current event. If negative then the internal event number is used, which is incremented by one for each new event.

bool Pythia8ToHepMC::fill_next_event( Pythia8::Event& pyev, GenEvent* evt, int ievnum = -1, Pythia8::Info* pyinfo = 0, Pythia8::Settings* pyset = 0)  
convert a Pythia event to a HepMC one. Will return true if succeeded.
argument pyev : the input Pythia event that is to be converted to HepMC format.
argument evt : the output GenEvt event, in its standard form.
argument iev : set the event number of the current event. If negative then the internal event number is used, which is incremented by one for each new event.
argument pyinfo : pointer to the Pythia Info object, which is used to extract PFD values, and process and cross section information. Without such a pointer this information therefore cannot be stored, i.e. it is equivalent to the three set_store methods below being set false.
argument pyset : pointer to the Pythia Settings object, which is used to decide whether hadronization is carried out, and therefore whether to warn about unhadronized partons. Without such a pointer the set_free_parton_warnings method below uniquely controls the behaviour.

The following paired methods can be used to set and get the status of some switches that modify the behaviour of the conversion routine. The set methods have the same default input values as the internal initialization ones, so that a call without an argument (re)stores the default.

void Pythia8ToHepMC::set_print_inconsistency(bool b = true)  
bool Pythia8ToHepMC::print_inconsistency()  
print a warning line, on cerr, when inconsistent mother and daughter information is encountered.

void Pythia8ToHepMC::set_free_parton_warnings(bool b = true)  
bool Pythia8ToHepMC::free_parton_warnings()  
check and print a warning line when unhadronized gluons or quarks are encountered in the event record. Does not apply when Pythia hadronization is switched off. Default is to do this check.

void Pythia8ToHepMC::set_crash_on_problem(bool b = false)  
bool Pythia8ToHepMC::crash_on_problem()  
if problems (like the free partons above) are encountered then the run is interrupted by an exit(1) command. Default is not to crash.

void Pythia8ToHepMC::set_convert_gluon_to_0(bool b = false)  
bool Pythia8ToHepMC::convert_gluon_to_0()  
the normal gluon identity code 21 is used also when parton density information is stored, unless this optional argument is set true to have gluons represented by a 0. This choice does not affect the normal event record, where a gluon is always 21.

void Pythia8ToHepMC::set_store_pdf(bool b = true)  
bool Pythia8ToHepMC::store_pdf()  
for each event store information on the two incoming flavours, their x values and common factorization scale, and the values of the two parton distributions, xf(x,Q).

void Pythia8ToHepMC::set_store_proc(bool b = true)  
bool Pythia8ToHepMC::store_proc()  
for each event store information on the Pythia process code, the renormalization scale, and alpha_em and alpha_s values used for the hard process.

void Pythia8ToHepMC::set_store_xsec(bool b = true)  
bool Pythia8ToHepMC::store_xsec()  
for each event store information on the Pythia cross section and its error, in pb, and the event weight. If events also come with a dimensional weight, like in some Les Houches strategies, this weight is in units of pb. pythia8-8.1.80.orig/htmldoc/Frontpage.html0000644000175000017500000001537512217615311016610 0ustar sunsun Front

PYTHIA 8

Welcome to PYTHIA - The Lund Monte Carlo!

PYTHIA 8 is the successor to PYTHIA 6, rewritten from scratch in C++. With the release of PYTHIA 8.1 it now becomes the official "current" PYTHIA version, although PYTHIA 6.4 will be supported in parallel with it for some time to come. Specifically, the new version has not yet been enough tested and tuned for it to have reached the same level of reliability as the older one. This testing will only happen if people begin to work with the program, however, which is why we encourage a gradual transition to the new version, starting now. There are some new physics features in PYTHIA 8.1, that would make use of it more attractive, but also some topics still missing, where 6.4 would have to be used. Further, many obsolete features will not be carried over, so for some backwards compatibility studies again 6.4 would be the choice.

Documentation

On these webpages you will find the up-to-date manual for PYTHIA 8.1. Use the left-hand index to navigate this documentation of program elements, especially of all possible program settings. All parameters are provided with sensible default values, however, so you need only change those of relevance to your particular study, such as choice of beams, processes and phase space cuts. The pages also contain a fairly extensive survey of all methods available to the user, e.g. to study the produced events. What is lacking on these webpages is an overview, on the one hand, and an in-depth physics description, on the other.

The overview can be found in the attached PDF file
A Brief Introduction to PYTHIA 8.1
T. Sjöstrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 852 [arXiv:0710.3820].
You are strongly recommended to read this summary when you start out to learn how to use PYTHIA 8.1. Note that some details have changed since the 8.100 version described there.

For the physics description we refer to the complete
PYTHIA 6.4 Physics and Manual
T. Sjöstrand, S. Mrenna and P. Skands, JHEP05 (2006) 026,
which in detail describes the physics (largely) implemented also in PYTHIA 8, and also provides a more extensive bibliography than found here.

When you use PYTHIA 8.1, you should therefore cite both, e.g. like
T. Sjöstrand, S. Mrenna and P. Skands, JHEP05 (2006) 026, Comput. Phys. Comm. 178 (2008) 852.

Furthermore, a separate
PYTHIA 8 Worksheet,
also an attached PDF file, offers a practical introduction to using the generator. It has been developed for and used at a few summer schools, with minor variations, but is also suited for self-study.

Authors

Torbjörn Sjöstrand
Department of Astronomy and Theoretical Physics, Lund University, Sölvegatan 14A, SE-223 62 Lund, Sweden
phone: + 46 - 46 - 222 48 16, e-mail: torbjorn@thep.lu.se

Jesper Roy Christiansen
Department of Astronomy and Theoretical Physics, Lund University, Sölvegatan 14A, SE-223 62 Lund, Sweden
e-mail: Jesper.Roy.Christiansen@thep.lu.se

Nishita Desai
Department of Physics and Astronomy, University College London, Gower Street, London, WC1E 6BT, United Kingdom
e-mail: Nishita.Desai@cern.ch

Philip Ilten
School of Physics, University College Dublin, Belfield, Dublin 4, Ireland
e-mail: philten@cern.ch

Stephen Mrenna
Computing Division, Simulations Group, Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA
phone: + 1 - 630 - 840 - 2556, e-mail: mrenna@fnal.gov

Stefan Prestel
Theory Group, DESY, Notkestrasse 85, D-22607 Hamburg, Germany
phone: + 49 - 40 - 8998-4250, e-mail: stefan.prestel@thep.lu.se

Peter Skands
Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland
phone: + 41 - 22 - 767 2447, e-mail: peter.skands@cern.ch

Former authors

Stefan Ask, e-mail: ask.stefan@gmail.com

Richard Corke, e-mail: r.corke@errno.net

Further contributions

Makefiles, configure scripts and HepMC interface by Mikhail Kirsanov.
Conversion of XML files to PHP ones by Ben Lloyd.
Simple Makefile for Win32/NMAKE by Bertrand Bellenot.
Extended Higgs sector partly implemented by Marc Montull.
Parts of charm and bottom decay tables courtesy DELPHI and LHCb collaborations.
Tunes and comparisons with data, based on Rivet and Professor, by Hendrik Hoeth.
Text and code on the use of ROOT in conjunction with PYTHIA by Rene Brun, Andreas Morsch and Axel Naumann.
Code and data for MRST/MSTW PDFs by Robert Thorne and Graeme Watt.
Code and data for the CTEQ/CT PDFs by Joey Huston and colleagues.
Help with implementing new proton PDFs by Tomas Kasemets.
Code and data for Pomeron PDFs by H1 collaboration and especially Paul Newman.
Help with implementing new Pomeron fluxes and PDFs by Sparsh Navin.
The new Hidden Valley code developed together with Lisa Carloni.
Code for a Kaluza-Klein electroweak gauge boson provided by Noam Hod and Mark Sutton.
Code for equivalent photon flux around an unresolved proton by Oystein Alvestad.
The MBR diffractive model and central diffraction by Robert Ciesielski.
2012 branching ratios for most light hadrons, and the tau lepton, by Anil Pratap Singh.
The pythia8-config script has been contributed by Andy Buckley, along with many other helpful suggestions.
Code and data for several of the NNPDF2.3 QCD+QED sets provided by Juan Rojo and Stefano Carrazza.
The fjcore code from FastJet provided by Matteo Cacciari, Gavin Salam and Gregory Soyez.
Note: in several cases modifications have been made to the original code, in order to integrate it with PYTHIA. In these cases the blame for any mistakes has to rest with the regular authors.

Licence

PYTHIA 8 is licensed under the GNU General Public Licence version 2.
Please respect the MCnet Guidelines for Event Generator Authors and Users.

The program and the documentation is Copyright © 2013 Torbjörn Sjöstrand pythia8-8.1.80.orig/htmldoc/SaveSettings.html0000644000175000017500000001243012217615311017267 0ustar sunsun Save Settings

Save Settings

The information on this webpage is only valid if you access the PHP dynamic webpages via a web browser, and does not apply to the static HTML equivalents. With PHP, all of the settings in the PYTHIA program are represented by radio buttons or fill-in boxes, that makes it easy for you to construct a file with your desired changes. This file can then be read into PYTHIA by your main program to steer the whole run.

Basic instructions

The functionality of the PHP option is described in the following.

  • To begin with, you must specify a (temporary) file name in the box above. If the filename already exists on the server, you will be requested to pick a new name.
  • Once you have Submitted your filename, you can browse through the pages and make your selections. The values currently selected when you load the page are the default values.
  • When you have finished making your changes to a particular page, you must click on Save Settings at the bottom of the page. This will write the changes to your temporary file. If you make a mistake, just repeat the procedure for that category again.

  • When you have finished all the changes you need, return to this page and click Finish File.
  • You will then get up a link, that you are asked to right-click with your mouse (or equivalent).
  • In the menu that appears, pick the option Save Link As (or equivalent).
  • You will now get up a file browser, for you to pick and Save the location and file name (the latter by default the same as the temporary file name).
  • At any time, if you click the RESET button, your temporary file will be erased and you can start anew.
  • Before you use a file, be sure to check it visually to confirm that you saved what you intended to. Minor corrections are easily made in a text editor.

Supplementary notes

The documentation files exist in three versions.

  1. As a set of .xml files, in the xmldoc/ subdirectory. These are the master copies that no user ever should touch, but that are used to generate the variants below.
  2. As a set of .html files, in the htmldoc/ subdirectory. You can open your own locally installed copy of the Welcome.html file in your web browser and thereafter navigate among all the pages. You can learn which parameters are free to be changed, but not change anything, except by brute-force cut-and-paste to a file of your own.
  3. As a set of .php files, in the phpdoc/ subdirectory. For these files to provide the functionality described above they have to accessed via a webserver. The one where you have your homepage should work fine. Alternatively you can use pages already available on another server.

A few further comments about the operation of the PHP option:

  • To set up the PHP files on your webserver, you have to install the whole phpdoc/ subdirectory there. In addition to the .php code this includes a few more files, plus a subdirectory named files where the temporary files are stored. This subdirectory must have public write access to work (chmod a+w files if not).
  • The "temporary" files stored in files actually remain unless the RESET button is used. The good news is that this makes it possible to recover a file that otherwise might be lost. The bad news is that the files directory may need to be cleaned up from time to time. (But typically the files are pretty small, so this should not be a major problem.)
  • When you click the Save Settings button on the bottom of a page all changed settings are written on the temporary file in the format
    name-of-flag/mode/parameter/word = value
    
    with one variable per line. Thereafter all the settings on the page are restored to their default values.
  • You can return to a page to do some further changes and save those. If you change the same parameter twice, it is the last value that counts. (Both values are stored in the file, with the more recent lower down, and then PYTHIA does the changes sequentially.) However remember that unchanged values are not stored, so if you want to restore some default value it may be simpler to edit the file afterwards.
  • The changeable flags/modes/parameters/words are mainly in the "Setup Run Tasks" section of the index, but a few (less frequently used ones) can also be found lower down, in the "Study Output" and "Link to Other Programs" pages.

  • It is not (yet) possible to modify particle data within the PHP-based setup approach. This is a more difficult task, since e.g. the modifications one may want to do in a decay table can be quite interrelated. pythia8-8.1.80.orig/htmldoc/BoseEinsteinEffects.html0000644000175000017500000001374412217615311020550 0ustar sunsun Bose-Einstein Effects

    Bose-Einstein Effects

    The BoseEinstein class performs shifts of momenta of identical particles to provide a crude estimate of Bose-Einstein effects. The algorithm is the BE_32 one described in [Lon95], with a Gaussian parametrization of the enhancement. We emphasize that this approach is not based on any first-principles quantum mechanical description of interference phenomena; such approaches anyway have many problems to contend with. Instead a cruder but more robust approach is adopted, wherein BE effects are introduced after the event has already been generated, with the exception of the decays of long-lived particles. The trick is that momenta of identical particles are shifted relative to each other so as to provide an enhancement of pairs closely separated, which is compensated by a depletion of pairs in an intermediate region of separation.

    More precisely, the intended target form of the BE correlations in BE_32 is
    f_2(Q) = (1 + lambda * exp(-Q^2 R^2)) * (1 + alpha * lambda * exp(-Q^2 R^2/9) * (1 - exp(-Q^2 R^2/4)))
    where Q^2 = (p_1 + p_2)^2 - (m_1 + m_2)^2. Here the strength lambda and effective radius R are the two main parameters. The first factor of the equation is implemented by pulling pairs of identical hadrons closer to each other. This is done in such a way that three-momentum is conserved, but at the price of a small but non-negligible negative shift in the energy of the event. The second factor compensates this by pushing particles apart. The negative alpha parameter is determined iteratively, separately for each event, so as to restore energy conservation. The effective radius parameter is here R/3, i.e. effects extend further out in Q. Without the dampening (1 - exp(-Q^2 R^2/4)) in the second factor the value at the origin would become f_2(0) = (1 + lambda) * (1 + alpha * lambda), with it the desired value f_2(0) = (1 + lambda) is restored. The end result can be viewed as a poor man's rendering of a rapidly dampened oscillatory behaviour in Q.

    Further details can be found in [Lon95]. For instance, the target is implemented under the assumption that the initial distribution in Q can be well approximated by pure phase space at small values, and implicitly generates higher-order effects by the way the algorithm is implemented. The algorithm is applied after the decay of short-lived resonances such as the rho, but before the decay of longer-lived particles.

    This algorithm is known to do a reasonable job of describing BE phenomena at LEP. It has not been tested against data for hadron colliders, to the best of our knowledge, so one should exercise some judgment before using it. Therefore by default the master switch HadronLevel:BoseEinstein is off. Furthermore, the implementation found here is not (yet) as sophisticated as the one used at LEP2, in that no provision is made for particles from separate colour singlet systems, such as W's and Z's, interfering only at a reduced rate.

    Warning: The algorithm will create a new copy of each particle with shifted momentum by BE effects, with status code 99, while the original particle with the original momentum at the same time will be marked as decayed. This means that if you e.g. search for all pi+- in an event you will often obtain the same particle twice. One way to protect yourself from unwanted doublecounting is to use only particles with a positive status code, i.e. ones for which event[i].isFinal() is true.

    Main parameters

    flag  BoseEinstein:Pion   (default = on)
    Include effects or not for identical pi^+, pi^- and pi^0.

    flag  BoseEinstein:Kaon   (default = on)
    Include effects or not for identical K^+, K^-, K_S^0 and K_L^0.

    flag  BoseEinstein:Eta   (default = on)
    Include effects or not for identical eta and eta'.

    parm  BoseEinstein:lambda   (default = 1.; minimum = 0.; maximum = 2.)
    The strength parameter for Bose-Einstein effects. On physical grounds it should not be above unity, but imperfections in the formalism used may require that nevertheless.

    parm  BoseEinstein:QRef   (default = 0.2; minimum = 0.05; maximum = 1.)
    The size parameter of the region in Q space over which Bose-Einstein effects are significant. Can be thought of as the inverse of an effective distance in normal space, R = hbar / QRef, with R as used in the above equation. That is, f_2(Q) = (1 + lambda * exp(-(Q/QRef)^2)) * (...).

    parm  BoseEinstein:widthSep   (default = 0.02; minimum = 0.001; maximum = 1.)
    Particle species with a width above this value (in GeV) are assumed to be so short-lived that they decay before Bose-Einstein effects are considered, while otherwise they do not. In the former case the decay products thus can obtain shifted momenta, in the latter not. The default has been picked such that both rho and K^* decay products would be modified. pythia8-8.1.80.orig/htmldoc/AlpgenEventInterface.html0000644000175000017500000003020012217615312020675 0ustar sunsun ALPGEN Event Interface

    ALPGEN Event Interface

    This manual page describes the ALPGEN [Man03] event interface for PYTHIA8. While future versions of ALPGEN will be able to write out events in LHEF format, previous versions always output events in an ALPGEN native format (a combination of a ".unw" and a "_unw.par" file). The ALPGEN component of this code contains a reader for this native format (for unweighted events), as well as parameter reading for both ALPGEN native and LHE file formats. The reader was designed to work together with an implementation of the ALPGEN-style parton-jet matching JetMatchingAlpgen described on the Jet Matching page. However, it will also work with a implementation of the Madgraph-style [Alw11] parton-jet matching JetMatchingMadgraph also described on the Jet Matching page. A sensible choice of JetMatching parameters is needed when using ALPGEN files with Madgraph-style matching and vice versa.

    It should be noted that all the functionality described here is provided through external routines, and therefore the presence of these features is dependent on the main program being used. This structure allows for the easy extensibility of the merging scheme. The files of interest are located in the examples/ subdirectory:

    • GeneratorInput.h : provides three classes for the reading of ALPGEN event and parameter files. LHAupAlpgen is an LHAup derived class for reading in ALPGEN native format event files. AlpgenPar is a class for the parsing of ALPGEN parameter files, making the information available through a simple interface. AlpgenHooks is a UserHooks derived class that provides the Alpgen:* options, described below. Further technical details of these classes are given at the end of this manual page.
    • main32.cc, main32.cmnd : a sample main program and card file showing the usage of previous file and an MLM UserHooks class. In combination, it reads in a sample ALPGEN (or Madgraph) event file while performing the MLM merging procedure as implemented in ALPGEN (or as in Madgraph). Some commented-out sets of options are provided in the card file, which can be activated to try different merging setups.
    • main32.unw, main32_unw.par : an ALPGEN format event and parameter file containing 100 W + 3 jet events. It is not feasible to package large event files with the PYTHIA distribution, but this sample is enough to show the different components in action.

    ALPGEN main options

    These following options are provided by the AlpgenHooks class, which must be loaded for this functionality to be present

    ALPGEN event files that have been written out in LHEF format should be read in through the normal LHEF machinery (see Beam Parameters). Files in ALPGEN's native format, instead, may be processed using the Alpgen:file option below. When using this option, the ALPGEN parameter file is stored in the PYTHIA Info object under the key AlpgenPar, see the "Header information" section of the Event Information manual page for more details. Processes not implemented by the PYTHIA 6 interface supplied with ALPGEN are also not implemented here.

    When reading in ALPGEN native event files, some momenta are shifted by the file reader to ensure energy-momentum conservation. The magnitude of these shifts should be small (around the MeV level in the worst case) and warnings will be produced if they are above a set threshold. A large number of warnings may signify unexpected behaviour and should potentially be investigated. It is also known that certain event classes, for example an event with both light and heavy b quarks may give rise to these warnings.

    The ALPGEN file reader supports the reading of the event and parameter files in gzip format with file extensions ".unw.gz" and "_unw.par.gz" respectively. This requires the use of external libraries, however, and the README file in the main directory contains instructions on how to enable this.

    All other Alpgen:* options apply to both LHE and native file formats, and include options to guide the MLM merging procedure based on the parameters that are read in with the events file.

    word  Alpgen:file   (default = void)
    This option is used to read in ALPGEN format event files. Using this option overrides any previously set beam options inside PYTHIA. The path to the files, not including any file extension, should be provided e.g. for input files input_unw.par and input.unw, the value input should be used.

    flag  Alpgen:setMasses   (default = on)
    When switched on, any particle masses provided by ALPGEN are set in the PYTHIA particle database.

    flag  Alpgen:setMLM   (default = on)
    When switched on, the merging parameters (see below) are set according to the ALPGEN hard process cuts:

    • JetMatching:eTjetMin = min(ptjmin + 5., 1.2 * ptjmin),
    • JetMatching:coneRadius = drjmin,
    • JetMatching:etaJetMax = etajmax.
    where the ptjmin, drjmin and etajmax are the incoming ALPGEN parameters. Note that any existing values of these parameters are overwritten.

    flag  Alpgen:setNjet   (default = on)
    When switched on, the JetMatching:nJet parameter (see below) is set to the incoming njet ALPGEN parameter. Note that any existing value of this parameter is overwritten.

    Class information

    Some more technical information about the different classes is given below. For clarity, some limited information on certain private methods is provided.

    LHAupAlpgen

    This class is derived from the LHAup base class, and uses the standard machinery to pass initialisation and event data to PYTHIA. These standard functions are not documented here. The complete parameter file is stored in the PYTHIA Info object, if given, under the key AlpgenPar.

    LHAupAlpgen::LHAupAlpgen(const char *baseFNin, Info *infoPtrIn = NULL)  
    The constructor for the class takes the base filename for the ALPGEN format files (without file extensions) and optionally a pointer to a PYTHIA Info class, used for warning/error message printing and for storing the ALPGEN parameter file. The event and parameter files are opened immediately, with the AlpgenPar class, described below, used to parse the parameter file.

    bool LHAupAlpgen::addResonances()  
    This is a private method used when an event is read in. The information read from the event file does not always contain a complete listing of all particles and four-momenta, and so various details must be reconstructed. Exactly which details are filled in can vary based on the ALPGEN process in question.

    bool LHAupAlpgen::rescaleMomenta()  
    This is another private method used when an event is read in. It shuffles and rescales momenta in an event to ensure energy-momentum conservation. First, pT is made to balance by splitting any imbalance between all outgoing particles with their energies also scaled. Second, the e/pZ of the two incoming particles are scaled to balance the outgoing particles. Finally, any intermediate resonances are recalculated from their decay products.

    AlpgenPar

    This class parses an ALPGEN parameter file and makes the information available through a simple interface. The information is stored internally in key/value (string/double) format. All lines prior to:
      ************** run parameters 
    are ignored, and in the general case, a line e.g.
      10   3.00000000000000        ! njets
    would be stored with key "njets" and value "3.0". The following lines are special cases where the line may be split or the key translated:
      3 ! hard process code
      0.000   4.700 174.300  80.419  91.188 120.000 ! mc,mb,mt,mw,mz,mh
      912.905 0.0914176   ! Crosssection +- error (pb)
      100 29787.4  ! unwtd events, lum (pb-1) Njob= 2
    
    In the first line, the key "hard process code" is translated to "hpc". In the second, the mass values are split and each given an entry in the internal store. In the third, the cross section and cross section error are stored under the keys "xsecup" and "xerrup" respectively. Finally, the number of events and luminosity are stored under the keys "nevent" and "lum" respectively. In the event that a duplicate key is present, with differing values, the stored value is overwritten and a warning given.

    AlpgenPar::AlpgenPar(Info *infoPtrIn = NULL)  
    The constructor does nothing except for store the PYTHIA Info pointer, if given. This is used for warning/error message printing.

    bool AlpgenPar::parse(const string paramStr)  
    This method parses an ALPGEN parameter file. The parameter file is passed as a single string, mainly intended to be read out from the PYTHIA Info object using the header information methods.

    bool AlpgenPar::haveParam(const string &paramIn)  
    Method to check if a parameter with key paramIn is present. Returns true if present, else false.

    double AlpgenPar::getParam(const string &paramIn)  
    int AlpgenPar::getParamAsInt(const string &paramIn)  
    Return the parameter with key paramIn as a double or integer. The presence of a parameter should have already been checked using the haveParam() function above. If the parameter is not present, 0 is returned.

    void AlpgenPar::void printParams()  
    Method to print a list of stored parameters.

    AlpgenHooks

    This UserHooks derived class provides all the Alpgen:* options. It is provided as a UserHooks class such that the code works regardless of whether ALPGEN native or LHE file formats are used. It is declared with virtual inheritance so that it may be combine with other UserHooks classes, see the "Combining UserHooks" section below.

    AlpgenHooks(Pythia &pythia)  
    The constructor takes a PYTHIA object as input, so that the beam parameter settings can be overridden if the Alpgen:file option is given. If this is the case, an LHAupAlpgen instance is automatically created and passed to PYTHIA.

    bool initAfterBeams()  
    This is the only UserHooks method that is overridden. It is called directly after PYTHIA has initialised the beams, and therefore the header information should be present in the PYTHIA Info object. The AlpgenPar class is used to parse ALPGEN parameters, if present, which are then used to set further PYTHIA settings. pythia8-8.1.80.orig/htmldoc/BeamParameters.html0000644000175000017500000003505712217615311017552 0ustar sunsun Beam Parameters

    Beam Parameters

    The settings on this page relate to the beam identities and energies, to a beam momentum spread and to a beam interaction spot. As always, momenta and energies are to be given in units of GeV, and of space and time in mm.

    Incoming beams

    There are two ways to set the identities and energies of the two incoming beam particles. One is to use the init() method with no arguments. Then the settings variables below will be read and used. The alternative is to call init(...) with arguments that provide this information. Then you need not use the variables below (although it would still be possible). Note that, if nothing is done, you will default to LHC at 14 TeV.

    Currently the beam particles must be either a hadron pair or a lepton pair. In the former category p p and pbar p combinations dominate, but it is also possible to combine with pi^+, pi^- and pi^0. In the latter e^+ e^- and mu^+ mu^- would be the most useful combinations, but also others should work if combined with an appropriate hard process.

    mode  Beams:idA   (default = 2212)
    The PDG id code for the first incoming particle. Allowed codes include
    2212 = p, -2212 = pbar,
    2112 = n, -2112 = nbar,
    211 = pi^+, -211 = pi^-, 111 = pi^0,
    990 = Pomeron (used in diffractive machinery; here mainly for debug purposes),
    11 = e^-, -11 = e^+,
    13 = mu^-, -13 = mu^+,
    and a few more leptons/neutrinos in a few combinations.

    mode  Beams:idB   (default = 2212)
    The PDG id code for the second incoming particle.

    mode  Beams:frameType   (default = 1; minimum = 1; maximum = 5)
    Choice of frame for the two colliding particles. For options 1 - 3 the beam identities are specified above, while they are obtained by the Les Houches information for options 4 and 5.
    option 1 : the beams are colliding in their CM frame, and therefore only the CM energy needs to be provided, see Beams:eCM below.
    option 2 : the beams are back-to-back, but with different energies, see Beams:eA and Beams:eB below. This option could also be used for fixed-target configurations.
    option 3 : the beams are not back-to-back, and therefore the three-momentum of each incoming particle needs to be specified, see Beams:pxA through Beams:pzB below.
    option 4 : the beam and event information is stored in a Les Houches Event File, see Beams:LHEF below.
    option 5 : the beam and event information is obtained by a pointer to an LHAup class instance.

    parm  Beams:eCM   (default = 14000.; minimum = 10.)
    Collision CM energy, to be set if Beams:frameType = 1.

    parm  Beams:eA   (default = 7000.; minimum = 0.)
    The energy of the first incoming particle, moving in the +z direction, to be set if Beams:frameType = 2. If the particle energy is smaller than its mass it is assumed to be at rest.

    parm  Beams:eB   (default = 7000.; minimum = 0.)
    The energy of the second incoming particle, moving in the -z direction, to be set if Beams:frameType = 2. If the particle energy is smaller than its mass it is assumed to be at rest.

    parm  Beams:pxA   (default = 0.)
    The p_x component of the first incoming particle, to be set if Beams:frameType = 3.

    parm  Beams:pyA   (default = 0.)
    The p_y component of the first incoming particle, to be set if Beams:frameType = 3.

    parm  Beams:pzA   (default = 7000.)
    The p_z component of the first incoming particle, to be set if Beams:frameType = 3.

    parm  Beams:pxB   (default = 0.)
    The p_x component of the second incoming particle, to be set if Beams:frameType = 3.

    parm  Beams:pyB   (default = 0.)
    The p_y component of the second incoming particle, to be set if Beams:frameType = 3.

    parm  Beams:pzB   (default = -7000.)
    The p_z component of the second incoming particle, to be set if Beams:frameType = 3.

    word  Beams:LHEF   (default = void)
    The name of a Les Houches Event File, to be set if Beams:frameType = 4.

    word  Beams:LHEFheader   (default = void)
    As some information in a Les Houches Event File init block is only known at the end of generation, some programs choose to output this as a separate file. If Beams:LHEFheader is given, information up till the end of the init block is read from this file, with the events themselves read as usual from the file given in Beams:LHEF.

    flag  Beams:newLHEFsameInit   (default = off)
    Allow to begin reading events from a new LHEF or or a new LHAup instance without a completely new initialization. Only useful when Beams:frameType = 4 or 5.

    flag  Beams:readLHEFheaders   (default = on)
    Read in LHEF header blocks and store them in the Info class. See also LHAupLHEF for more information.

    mode  Beams:nSkipLHEFatInit   (default = 0)
    Skip the first nSkip events of the input stream (cf. the LHAup::skipEvent(nSkip) method). Only used when Beams:frameType = 4 or 5.

    Beam momentum spread

    This framework currently is intended for a modest beam spread, such as experienced at hadron colliders. Thus it can be safely assumed that the physics does not change over the CM energy range probed, so that the parameters of the physics initialization at the nominal energy can be used as is. Currently it can not be used for the more extensive energy spread expected at linear e^+ e^- colliders. Also, any attempt to combine it with external Les Houches input of parton-level events is at own risk.

    On this page you can set the momentum spread according to a simple Gaussian distribution. If you instead want a more sophisticated parametrization, you can write and link your own BeamShape class.

    flag  Beams:allowMomentumSpread   (default = off)
    Allow the beam momenta to be smeared around their initialization nominal values.

    parm  Beams:sigmaPxA   (default = 0.; minimum = 0.)
    The width of a Gaussian distribution of the p_x spread of the first incoming particle.

    parm  Beams:sigmaPyA   (default = 0.; minimum = 0.)
    The width of a Gaussian distribution of the p_y spread of the first incoming particle.

    parm  Beams:sigmaPzA   (default = 0.; minimum = 0.)
    The width of a Gaussian distribution of the p_z spread of the first incoming particle.

    parm  Beams:maxDevA   (default = 5.; minimum = 0.)
    The triply Gaussian distribution (p_x, p_y, p_z) is restricted to a maximal total deviation from the nominal values (p_x0, p_y0, p_z0) for the first incoming particle, like
    (p_x - p_x0)^2/sigma_px^2 + (p_y - p_y0)^2/sigma_py^2 + (p_z - p_z0)^2/sigma_pz^2 < maxDev^2
    (Note the absence of a factor 2 in the denominator, unlike the Gaussians used to pick (p_x, p_y, p_z).)

    parm  Beams:sigmaPxB   (default = 0.; minimum = 0.)
    The width of a Gaussian distribution of the p_x spread of the second incoming particle.

    parm  Beams:sigmaPyB   (default = 0.; minimum = 0.)
    The width of a Gaussian distribution of the p_y spread of the second incoming particle.

    parm  Beams:sigmaPzB   (default = 0.; minimum = 0.)
    The width of a Gaussian distribution of the p_z spread of the second incoming particle.

    parm  Beams:maxDevB   (default = 5.; minimum = 0.)
    The triply Gaussian distribution (p_x, p_y, p_z) is restricted to a maximal total deviation from the nominal values (p_x0, p_y0, p_z0), for the second incoming particle, like
    (p_x - p_x0)^2/sigma_px^2 + (p_y - p_y0)^2/sigma_py^2 + (p_z - p_z0)^2/sigma_pz^2 < maxDev^2
    (Note the absence of a factor 2 in the denominator, unlike the Gaussians used to pick (p_x, p_y, p_z).)

    Beam interaction vertex

    On this page you can set the spread of the interaction vertex according to a simple Gaussian distribution. If you instead want a more sophisticated parametrization, you can write and link your own BeamShape class.

    flag  Beams:allowVertexSpread   (default = off)
    Allow the interaction vertex of the two colliding beams to be smeared. If off, then the vertex is set to be the origin.

    parm  Beams:sigmaVertexX   (default = 0.; minimum = 0.)
    The width of a Gaussian distribution of the x location of the interaction vertex.

    parm  Beams:sigmaVertexY   (default = 0.; minimum = 0.)
    The width of a Gaussian distribution of the y location of the interaction vertex.

    parm  Beams:sigmaVertexZ   (default = 0.; minimum = 0.)
    The width of a Gaussian distribution of the z location of the interaction vertex.

    parm  Beams:maxDevVertex   (default = 5.; minimum = 0.)
    The triply Gaussian distribution of interaction vertex position (x, y, z) is restricted to a maximal total deviation from the origin, like
    x^2/sigma_x^2 + y^2/sigma_y^2 + z^2/sigma_z^2 < maxDevVertex^2
    (Note the absence of a factor 2 in the denominator, unlike the Gaussians used to pick (x, y, z).)

    parm  Beams:sigmaTime   (default = 0.; minimum = 0.)
    The width of a Gaussian distribution of the collision time (in units of mm/c). Note that, if the above space parametrization is viewed as the effect of two incoming beams along the +-z axis, with each beam having a Gaussian spread, then the spread of the time would also become a Gaussian with the same width as the z one (times the velocity of the beams, which we expect is close to unity). For flexibility we have not enforced any such relation, however.

    parm  Beams:maxDevTime   (default = 5.; minimum = 0.)
    The collision time is restricted to be in the range |t| < sigma_t * maxDevTime.

    The distributions above are all centered at the origin. It is also possible to shift the above distributions to be centered around another nominal position. You must have Beams:allowVertexSpread = on to use this possibility.

    parm  Beams:offsetVertexX   (default = 0.)
    The x location of the interaction vertex is centered at this value.

    parm  Beams:offsetVertexY   (default = 0.)
    The y location of the interaction vertex is centered at this value.

    parm  Beams:offsetVertexZ   (default = 0.)
    The z location of the interaction vertex is centered at this value.

    parm  Beams:offsetTime   (default = 0.)
    The time t of the interaction vertex is centered at this value. pythia8-8.1.80.orig/htmldoc/SemiInternalProcesses.html0000644000175000017500000007614112217615312021143 0ustar sunsun Semi-Internal Processes

    Semi-Internal Processes

    Normally users are expected to implement new processes via the Les Houches Accord. Then you do all flavour, colour and phase-space selection externally, before your process-level events are input for further processing by PYTHIA. However, it is also possible to implement a new process in exactly the same way as the internal PYTHIA ones, thus making use of the internal phase space selection machinery to sample an externally provided cross-section expression. The MadGraph 5 program [Alw11] allows you to do exactly that, i.e. it can be used to generate C++ code that can be linked into the existing PYTHIA framework, see here.

    Should you decide to go ahead on your own, this page gives a brief summary how to do that. If you additionally want to introduce a new resonance species, with its own internal width calculations, you will find further instructions here. It is strongly recommended to shop around for a similar process that has already been implemented, and to use that existing code as a template. Look for processes with the same combinations of incoming flavours and colour flows, rather than the shape of the cross section itself. With a reasonable such match the task should be of medium difficulty, without it more demanding.

    PYTHIA is rather good at handling the phase space of 2 -> 1 and 2 -> 2 processes, is more primitive for 2 -> 3 ones and does not at all address higher multiplicities. This limits the set of processes that you can implement in this framework. The produced particles may be resonances, however, so it is possible to end up with bigger "final" multiplicities through sequential decays, and to include further matrix-element weighting in those decays.

    There are three steps involved in implementing a process:

    1. making use of the PYTHIA-provided kinematics information to calculate the relevant cross section,
    2. writing a new class, where the matrix elements are implemented, including information on incoming and outgoing flavours and colours, and
    3. making the process available.
    We consider these aspects in turn. An example where it all comes together is found in main22.cc.

    The Cross Section Calculation

    The key method for the cross section calculation is SigmaProcess::sigmaHat(), described below. At the point when it is called, the kinematics has already been set up, and from these phase space variables the differential cross section is to be calculated.

    For a 2 -> 1 process, the returned value should be sigmaHat(sHat), where mH (= mHat), sH (= sHat) and sH2 (= sHat^2) are available to be used. Incoming partons are massless. Overload the convertM2() method below if you instead plan to return |M|^2.

    For a 2 -> 2 process, instead d(sigmaHat)/d(tHat) should be returned, based on provided mH, sH, sH2, tH, tH2, uH, uH2, m3, s3, m4, s4 and pT2 values (s3 = m3*m3 etc.). Incoming partons are massless. Overload the convertM2() method below if you instead plan to return |M|^2.

    For a 2 -> 3 process, instead |M|^2 should be returned, with normalization such that |M|^2 / (2 sHat) integrated over the three-body phase space gives the cross section. Here no standard set of Mandelstam-style variables exists. Instead the obvious ones, mH, sH, m3, s3, m4, s4, m5, s5, are complemented by the four-vectors p3cm, p4cm, p5cm, from which further invariants may be calculated. The four-vectors are defined in the CM frame of the subcollision, with massless incoming partons along the +-z axis.

    In either case, alpha_s and alpha_em have already been calculated, and are stored in alpS and alpEM. Also other standard variables may be used, like CoupEW::sin2thetaW(), and related flavour-dependent vector and axial couplings in CoupEW and CKM combinations in VCKM.

    In case some of the final-state particles are resonances, their squared masses have already been selected according to a Breit-Wigner with a linearly running width Gamma(m) = Gamma(m_0) * m / m_0. More precisely, the mass spectrum is weighted according to w_BW(m^2) d(m^2), where
    w_BW(m^2) = (1/pi) * (m * Gamma(m)) / ( (m^2 - m_0^2)^2 + (m * Gamma(m))^2 ) .
    If you would like to have another expression, the above weights are stored in runBW3, runBW4 and runBW5, respectively. If you divide out one of these factors, you just remain with a phase space selection d(m^2) for this particle, and can multiply on your desired shape factor instead. Unfortunately, the Monte Carlo efficiency will drop if your new mass distribution differs dramatically from the input one. Therefore it does make sense to adjust the database value of the width to be slightly (but not too much) broader than the distribution you have in mind. Also note that, already by default, the wings of the Breit-Wigner are oversampled (with a compensating lower internal weight) by partly sampling like (a + b/m^2 + c/m^4) d(m^2), where the last term is only used for gamma^*/Z^0.

    As alternative to the kinematics variables defined above, also the two arrays mME[5] and pME[5], for masses and four-momenta, respectively, can be used for cross-section calculations. Here indices 0 and 1 are the two incoming beams, and 2 and onwards the outgoing particles. Note that this differs by one step from the normal internal labeling, where slot 0 is left empty. The four-momenta are defined in the rest frame of the subcollision, with the incoming partons along the +-z direction. The kinematics need not agree with the "correct" one stored in the event record, for three reasons.
    1) Gauge invariance forces matrix-element calculations to use the same masses for incoming as outgoing legs of a particle species, say b quarks. Therefore the kinematics of the two incoming partons is recalculated, relative to the normal event record, to put the partons on the mass shell. (Note that initial masses is a technical issue, not the correct physics picture: the incoming partons are likely to be spacelike virtual rather than on the mass shell.)
    2) In principle each fermion flavour has to be treated separately, owing to a different mass. However, in many cases fermions can be assumed massless, which speeds up the calculations, and further gains occur if then different flavours can use the same cross-section expression. In MadGraph the default is that fermions up to and including the c quark and the mu lepton are considered massless, while the b quark and the tau lepton are considered massive. This can be modified however, and below we provide four flags that can be used to consider the "borderline" fermions either as massless or as massive when matrix elements are evaluated, to match the assumptions made for the matrix elements themselves.
    3) For 2 -> 2 and 2 -> 3 processes of massive identical particles (or antiparticles) in the final state, such as t tbar or W^+ W^-, the kinematics is here adjusted so that the two or three particles have the same mass, formed as a suitable average of the actual Breit-Wigner-distributed masses. This allows the evaluation of matrix-element expressions that only have meaning if the two/three have the same mass.
    Thus the mass array mME[5] and the four-momentum array pME[5] present values both for initial- and final-state particles based on these mass principles suited for matrix-element input. Note that these variables therefore differ from the kinematics stored in the event record proper, where incoming fermions are always massless and outgoing resonances have independent Breit-Wigner mass distributions.
    The conversion from the normal to the special kinematics is done by calling the setupForME() method. This you have to do yourself in the SigmaHat() member of your derived class. Alternatively it could be done in SigmaKin(), i.e. before the loop over incoming flavours, but then these would be considered massless. The identity of final-state particles is obtained from the id3Mass(), id4Mass() and id5Mass() methods. Should the conversion to mME[5] and pME[5] not work, setupForME() will return false, and then the cross section should be put zero.

    flag  SigmaProcess:cMassiveME   (default = off)
    Let the c quark be massive or not in the kinematics set up for external matrix-element evaluation.

    flag  SigmaProcess:bMassiveME   (default = on)
    Let the b quark be massive or not in the kinematics set up for external matrix-element evaluation.

    flag  SigmaProcess:muMassiveME   (default = off)
    Let the mu lepton be massive or not in the kinematics set up for external matrix-element evaluation.

    flag  SigmaProcess:tauMassiveME   (default = on)
    Let the tau lepton be massive or not in the kinematics set up for external matrix-element evaluation.

    The Cross Section Class

    The matrix-element information has to be encoded in a new class. The relevant code could either be put before the main program in the same file, or be stored separately, e.g. in a matched pair of .h and .cc files. The latter may be more convenient, in particular if the cross sections are lengthy, or if you intend to build up your own little process library, but of course requires that these additional files are correctly compiled and linked.

    The class has to be derived either from Sigma1Process, for 2 -> 1 processes, from Sigma2Process, for 2 -> 2 ones, or from Sigma3Process, for 2 -> 3 ones. (The Sigma0Process class is used for elastic, diffractive and minimum-bias events, and is not recommended for use beyond that.) These are in their turn derived from the SigmaProcess base class.

    The class can implement a number of methods. Some of these are compulsory, others strongly recommended, and the rest are to be used only when the need arises to override the default behaviour. The methods are:

    A constructor for the derived class obviously must be available. Here you are quite free to allow a list of arguments, to set the parameters of your model, or even to create a set of closely related but distinct processes. For instance, g g -> Q Qbar, Q = c or b, is only coded once, and then the constructor takes the quark code (4 or 5) as argument, to allow the proper amount of differentiation.

    A destructor is only needed if you plan to delete the process before the natural end of the run, and require some special behaviour at that point. If you call such a destructor you will leave a pointer dangling inside the Pythia object you gave it in to, if that still exists.

    void SigmaProcess::initProc()  
    is called once during initialization, and can then be used to set up parameters, such as masses and couplings, and perform calculations that need not be repeated for each new event, thereby saving time. This method needs not be implemented, since in principle all calculations can be done in sigmaHat below.

    void SigmaProcess::sigmaKin()  
    is called once a kinematical configuration has been determined, but before the two incoming flavours are known. This routine can therefore be used to perform calculations that otherwise might have to be repeated over and over again in sigmaHat below. For instance a flavour-independent cross section calculation for a q g initial state would be repeated 20 times in sigmaHat, five times for the five quark flavours allowed in the incoming beams, times twice to include antiquarks, times twice since the (anti)quark could be in either of the two beams. You could therefore calculate the result once only and store it as a private data member of the class. It is optional whether you want to use this method, however, or put everything in sigmaHat.

    double SigmaProcess::sigmaHat()  
    is the key method for cross section calculations and returns a cross section value, as described in the previous section. It is called when also a preliminary set of incoming flavours has been picked, in addition to the kinematical ones already available for sigmaKin. Typically sigmaHat is called inside a loop over all allowed incoming flavour combinations, stored in id1 and id2, with fixed kinematics, as already illustrated above. The sum over the different flavour combinations provides the total cross section, while their relative size is used to make a selection of a specific incoming state.

    bool SigmaProcess::setupForME()  
    to be called by the user from inside sigmaHat() (or possibly sigmaKin()) to setup alternative kinematics in the mME[5] and pME[5] arrays, better suited for matrix-element calculations. See the end of the previous section for a more detailed description. Should the method return false then the conversion did not work, and sigmaHat() (or sigmaKin()) should be set to vanish.

    void SigmaProcess::setIdColAcol()  
    is called only once an initial state and a kinematical configuration has been picked. This routine must set the complete flavour information and the colour flow of the process. This may involve further random choices, between different possible final-state flavours or between possible competing colour flows. Private data members of the class may be used to retain some information from the previous steps above.
    When this routine is called the two incoming flavours have already been selected and are available in id1 and id2, whereas the one, two or three outgoing ones either are fixed for a given process or can be determined from the instate (e.g. whether a W^+ or W^- was produced). There is also a standard method in VCKM to pick a final flavour from an initial one with CKM mixing. Once you have figured out the value of id3 and, the case being, id4 and id5, you store these values permanently by a call setId( id1, id2, id3, id4, id5), where the last two may be omitted if irrelevant.
    Correspondingly, the colours are stored with setColAcol( col1, acol1, col2, acol2, col3, acol3, col4, acol4, col5, acol5), where the final ones may be omitted if irrelevant. Les Houches style colour tags are used, but starting with number 1 (and later shifted by the currently requested offset). The input is grouped particle by particle, with the colour index before the anticolour one. You may need to select colour flow dynamically, depending on the kinematics, when several distinct possibilities exist. Trivial operations, like swapping colours and anticolours, can be done with existing methods.
    When the id3Mass() and id4Mass() methods have been used, the order of the outgoing particles may be inconsistent with the way the tHat and uHat variables have been defined. A typical example would be a process like q g -> q' W with tHat defined between incoming and outgoing quark, but where id3Mass() = 24 and so the process is to be stored as q g -> W q'. One should then put the variable swapTU = true in setIdColAcol() for each event where the tHat and uHat variables should be swapped before the event kinematics is reconstructed. This variable is automatically restored to false for each new event.

    double SigmaProcess::weightDecayFlav( Event& process)  
    is called to allow a reweighting of the simultaneous flavour choices of resonance decay products. Is currently only used for the q qbar -> gamma*/Z^0 gamma*/Z^0 process, and will likely not be of interest for you.

    double SigmaProcess::weightDecay( Event& process, int iResBeg, int iResEnd)  
    is called when the basic process has one or several resonances, after each set of related resonances in process[i], iResBeg <= i <= iResEnd, has been allowed to decay. The calculated weight, to be normalized to the range between 0 and 1, is used to decide whether to accept the decay(s) or try for a new decay configuration. The base-class version of this method returns unity, i.e. gives isotropic decays by default. This method may be called repeatedly for a single event. For instance, in q qbar -> H^0 Z^0 with H^0 -> W^+ W^-, a first call would be made after the H^0 and Z^0 decays, and then depend only on the Z^0 decay angles since the H^0 decays isotropically. The second call would be after the W^+ W^- decays and then involve correlations between the four daughter fermions.

    string SigmaProcess::name()  
    returns the name of the process, as you want it to be shown in listings.

    int SigmaProcess::code()  
    returns an integer identifier of the process. This has no internal function, but is only intended as a service for the user to rapidly (and hopefully uniquely) identify which process occurred in a given event. Numbers below 10000 are reserved for internal PYTHIA use.

    string SigmaProcess::inFlux()  
    this string specifies the combinations of incoming partons that are allowed for the process under consideration, and thereby which incoming flavours id1 and id2 the sigmaHat() calls will be looped over. It is always possible to pick a wider flavour selection than strictly required and then put to zero cross sections in the superfluous channels, but of course this may cost some extra execution time. Currently allowed options are:
    * gg: two gluons.
    * qg: one (anti)quark and one gluon.
    * qq: any combination of two quarks, two antiquarks or a quark and an antiquark.
    * qqbar: any combination of a quark and an antiquark; a subset of the qq option.
    * qqbarSame: a quark and its antiquark; a subset of the qqbar option.
    * ff: any combination of two fermions, two antifermions or a fermion and an antifermion; is the same as qq for hadron beams but also allows processes to work with lepton beams.
    * ffbar: any combination of a fermion and an antifermion; is the same as qqbar for hadron beams but also allows processes to work with lepton beams.
    * ffbarSame: a fermion and its antifermion; is the same as qqbarSame for hadron beams but also allows processes to work with lepton beams.
    * ffbarChg: a fermion and an antifermion that combine to give charge +-1.
    * fgm: a fermion and a photon (gamma).
    * ggm: a gluon and a photon.
    * gmgm: two photons.

    bool SigmaProcess::convert2mb()  
    it is assumed that cross sections normally come in dimensions such that they, when integrated over the relevant phase space, obtain the dimension GeV^-2, and therefore need to be converted to mb. If the cross section is already encoded as mb then convert2mb() should be overloaded to instead return false.

    bool SigmaProcess::convertM2()  
    it is assumed that 2 -> 1 cross sections are encoded as sigmaHat(sHat), and 2 -> 2 ones as d(sigmaHat)/d(tHat) in the SigmaProcess::sigmaHat() methods. If convertM2() is overloaded to instead return true then the return value is instead assumed to be the squared matrix element |M|^2, and SigmaProcess::sigmaHatWrap(...) converts to sigmaHat(sHat) or d(sigmaHat)/d(tHat), respectively. This switch has no effect on 2 -> 3 processes, where |M|^2 is the only allowed input anyway.

    int SigmaProcess::id3Mass()  
    int SigmaProcess::id4Mass()  
    int SigmaProcess::id5Mass()  
    are the one, two or three final-state flavours, where masses are to be selected before the matrix elements are evaluated. Only the absolute value should be given. For massless particles, like gluons and photons, one need not give anything, i.e. one defaults to 0. The same goes for normal light quarks, where masses presumably are not implemented in the matrix elements. Later on, these quarks can still (automatically) obtain constituent masses, once a u, d or s flavour has been selected.

    int SigmaProcess::resonanceA()  
    int SigmaProcess::resonanceB()  
    are the codes of up to two s-channel resonances contributing to the matrix elements. These are used by the program to improve the phase-space selection efficiency, by partly sampling according to the relevant Breit-Wigner distributions. Massless resonances (the gluon and photon) need not be specified.

    bool SigmaProcess::isSChannel()  
    normally the choice of renormalization and factorization scales in 2 -> 2 and 2 -> 3 processes is based on the assumption that t- and u-channel exchanges dominates the cross section. In cases such as f fbar -> gamma* -> f' fbar' a 2 -> 2 process actually ought to be given scales as a 2 -> 1 one, in the sense that it proceeds entirely through an s-channel resonance. This can be achieved if you override the default false to return true. See further the page on couplings and scales.

    int SigmaProcess::idSChannel()  
    normally no intermediate state is shown in the event record for 2 -> 2 and 2 -> 3 processes. However, in case that idSChannel is overloaded to return a nonzero value, an intermediate particle with that identity code is inserted into the event record, to make it a 2 -> 1 -> 2 or 2 -> 1 -> 3 process. Thus if both isSChannel and idSChannel are overloaded, a process will behave and look like it proceeded through a resonance. The one difference is that the implementation of the matrix element is not based on the division into a production and a decay of an intermediate resonance, but is directly describing the transition from the initial to the final state.

    int SigmaProcess::isQCD3body()  
    there are two different 3-body phase-space selection machineries, of which the non-QCD one is default. If you overload this method instead the QCD-inspired machinery will be used. The differences between these two is related to which phase space cuts can be set, and also that the QCD machinery assumes (almost) massless outgoing partons.

    int SigmaProcess::idTchan1()  
    int SigmaProcess::idTchan2()  
    the non-QCD 2 -> 3 phase space selection machinery is rather primitive, as already mentioned. The efficiency can be improved in processes that proceed though t-channel exchanges, such as q qbar' -> H^0 q qbar' via Z^0 Z^0 fusion, if the identity of the t-channel-exchanged particles on the two side of the event are provided. Only the absolute value is of interest.

    double SigmaProcess::tChanFracPow1()  
    double SigmaProcess::tChanFracPow2()  
    in the above kind of 2 -> 3 phase-space selection, the sampling of pT^2 is done with one part flat, one part weighted like 1 / (pT^2 + m_R^2) and one part like 1 / (pT^2 + m_R^2)^2. The above values provide the relative amount put in the latter two channels, respectively, with the first obtaining the rest. Thus the sum of tChanFracPow1() and tChanFracPow2() must be below unity. The final results should be independent of these numbers, but the Monte Carlo efficiency may be quite low for a bad choice. Here m_R is the mass of the exchanged resonance specified by idTchan1() or idTchan2(). Note that the order of the final-state listing is important in the above q qbar' -> H^0 q qbar' example, i.e. the H^0 must be returned by id3Mass(), since it is actually the pT^2 of the latter two that are selected independently, with the first pT then fixed by transverse-momentum conservation.

    bool SigmaProcess::useMirrorWeight()  
    in 2 -> 3 processes the phase space selection used here involves a twofold ambiguity basically corresponding to a flipping of the positions of last two outgoing particles. These are assumed equally likely by default, false, but for processes proceeding entirely through t-channel exchange the Monte Carlo efficiency can be improved by making a preselection based on the relative propagator weights, true.

    int SigmaProcess::gmZmode()  
    allows a possibility to override the global mode WeakZ0:gmZmode for a specific process. The global mode normally is used to switch off parts of the gamma^*/Z^0 propagator for test purposes. The above local mode is useful for processes where a Z^0 really is that and nothing more, such as q qbar -> H^0 Z^0. The default value -1 returned by gmZmode() ensures that the global mode is used, while 0 gives full gamma^*/Z^0 interference, 1 gamma^* only and 2 Z^0 only.

    Access to a process

    Once you have implemented a class, it is straightforward to make use of it in a run. Assume you have written a new class MySigma, which inherits from Sigma1Process, Sigma2Process or Sigma3Process, which in their turn inherit from SigmaProcess. You then create an instance of this class and hand it in to a pythia object with
          SigmaProcess* mySigma = new MySigma();
          pythia.setSigmaPtr( mySigma); 
    
    If you have several processes you can repeat the procedure any number of times. When pythia.init(...) is called these processes are initialized along with any internal processes you may have switched on, and treated in exactly the same manner. The pythia.next() will therefore generate a mix of the different kinds of processes without distinction. See also the Program Flow description.

    If the code should be of good quality and general usefulness, it would be simple to include it as a permanently available process in the standard program distribution. The final step of that integration ought to be left for the PYTHIA authors, but here is a description of what is required.

    A flag has to be defined, that allows the process to be switched on; by default it should always be off. The name of the flag should be chosen of the type model:process. Here the model would be related to the general scenario considered, e.g. Compositeness, while process would specify instate and outstate, separated by a 2 (= to), e.g. ug2u*g. When several processes are implemented and "belong together" it is also useful to define a model:all switch that affects all the separate processes.

    The flags should normally be stored in the ProcessSelection.xml file or one of its daughters for a specific kind of processes. This is to make them easily found by users. You could create and use your own .xml file, so long as you then add that name to the list of files in the Index.xml file. (If not, the flags would never be created and the program would not work.)

    In the ProcessContainer.c file, the SetupContainers::init() method needs to be expanded to create instances of the processes switched on. This code is fairly repetitive, and should be easy to copy and modify from the code already there. The basic structure is
    (i) check whether a process is requested by the user and, if so,
    (ii) create an instance of the matrix-element class,
    (iii)create a container for the matrix element and its associated phase-space handling, and
    (iv) add the container to the existing process list.

    Two minor variations are possible. One is that a set of related processes are lumped inside the the same initial check, i.e. are switched on all together. The second is that the matrix-element constructor may take arguments, as specified by you (see above). If so, the same basic matrix element may be recycled for a set of related processes, e.g. one for a composite u and one for a composite d. Obviously these variations may be combined. pythia8-8.1.80.orig/htmldoc/Tunes.html0000644000175000017500000003667612217615312015771 0ustar sunsun Tunes

    Tunes

    Since some physics aspects cannot be derived from first principles, this program contains many parameters that represent a true uncertainty in our understanding of nature. Particularly afflicted are the areas of hadronization and multiparton interactions, which both involve nonperturbative QCD physics.

    Technically, PYTHIA parameters can be varied independently of each other, but the physical requirement of a sensible description of a set of data leads to correlations and anticorrelations between the parameters. Hence the need to produce tunes, not of one parameter at a time, but simultaneously for a group of them. A well-known (separate) such example is parton densities, where combined tunes to a wide range of data have been produced, that can then be obtained prepackaged.

    Given the many PYTHIA parameters to be tuned, it is convenient to divide the task into subtasks. Firstly, if we assume jet universality, hadronization and final-state parton showers should be tuned to e^+e^- annihilation data, notably from LEP1, since this offers the cleanest environment. Secondly, with such parameters fixed, hadron collider data should be studied to pin down multiparton interactions and other further aspects, such as initial-state radiation. Ideally this would be done separately for diffractive and non-diffractive events, although it is not possible to have a clean separation. (Thirdly would come anything else, such as physics with photon beams, which involve further parameters, but that is beyond the current scope.)

    The first step in this program has now been taken, with a tune to LEP1 data by Hendrik Hoeth, using the Rivet + Professor framework. Starting with version 8.125 it defines the default values for hadronization parameters and timelike showers.

    The situation is more complicated for hadronic interactions in general and multiparton interactions in particular, where PYTHIA 8 is more different from PYTHIA 6, and therefore more work is needed. Specifically, it is not possible to "port" a PYTHIA 6 tune to PYTHIA 8.

    A first simple tune, appropriately called "Tune 1", became default starting with version 8.127. It was noted, in particular by Hendrik Hoeth, that this tune had a tension between parameters needed to describe minimum-bias and underlying-event activity. Therefore some further physics features were introduced in the code itself [Cor10a], which were made default as of 8.140. This version also included two new tunes, 2C and 2M, based on the CTEQ 6L1 and the MRST LO** PDF sets, respectively. These have been made by hand, as a prequel to complete Professor-style tunings.

    The very first data to come out of the LHC showed a higher rapidity plateau than predicted for current PYTHIA 6 tunes, also for the lower energies. This may suggest some tension in the data. Two alternatives, 3C and 3M, were produced by a few brute-force changes of 2C and 2M. These were introduced in 8.140, but discontinued in 8.145 in favour of the new 4C tune, that is based on a more serious study of some early LHC data, see [Cor10a]. Following the comparative studies in [Buc11], which independently confirmed a reasonable agreement with LHC data, tune 4C was made the default as of 8.150. A variant is tune 4Cx, where the Gaussian matter profile has an x-dependent width [Cor11].

    Several ATLAS tunes have now been included, obtained with different PDFs and with different emphasis on minimum-bias and underlying-event data [ATL12]. These typically require LHAPDF to be linked, but this can be avoided in cases where the same PDF set is implemented internally.

    Central diffraction is a recent addition to the "soft QCD" process palette, and is thus not yet included in tunes; indeed its cross section is actively zeroed. You can switch it back on after you have selected your tune, with SigmaTotal:zeroAXB = off. But note that, since the total cross section is assumed unchanged, the nondiffractive cross section is reduced and thus also the MPI machinery affected, even if effects should not be big (for a small central diffractive cross section).

    Note that comparisons with data also require that other aspects agree, such as that decay chains are stopped at an agreed-on level. For instance, in the ATLAS tunes all particles with a lifetime above 10 mm are considered stable, ParticleDecays:limitTau0 = on, ParticleDecays:tau0Max = 10. We have chosen not to include this as part of the tune settings itself, since the tune as such could still be used with any other choice of stable and unstable particles.

    Further comparisons have been posted on the MCPLOTS pages. They have been produced with help of the Rivet package [Buc10].

    In the future we hope to see further PYTHIA 8 tunes appear. Like with parton distributions, there is likely to be several tunes, because different sets of data will pull in different directions, by imperfections in the model or in the data, and by differences in the chosen tuning strategies. We therefore propose to collect some of these tunes here, in a prepackaged form. Of course, in all cases it is a matter of setting values for parameters already defined elsewhere, so the tunes offer no new functionality, only a more convenient setup.

    You should be aware that the evolution of the program will not guarantee complete backwards compatibility between versions. Most obviously this concerns bug fixes. But also for some other major changes, like the introduction of the new diffractive machinery, the default behaviour of old tunes has been changed retroactively. (Which should be fine for diffraction, since previous tunes were not based on data strongly influenced by diffraction.)

    The setup of the tunes is special, in that the choice of a tune forces the change of several different flags, modes and parameters. Furthermore a design principle has been that it should be possible to start out from a tune and then change a few of its settings. This gives power and flexibility at the expense of requiring a more careful ordering of commands. We therefore here sketch the order in which operations are carried out.

    1. The constructor of a Pythia instance will read in all settings, and initialize them with their default values.
    2. At the end of this operation, the Tune:ee and Tune:pp modes (see further below) are checked. If either of them are positive the methods Settings::initTuneEE(...) and Settings::initTunePP(...), respectively, are called to overwrite the whole collection of settings in the relevant tune. Zero (or negative) means that nothing will be done.
    3. After the Pythia constructor all the relevant values for the default tune(s) have thus been set up.
    4. You as a user can now start to overwrite the values at will, using Pythia::readFile(...) to read a configuration file, or a list of Pythia::readString(...) commands, or the lower-level Settings methods. All changes are made in the order in which the commands are encountered during the execution. A given variable can be changed multiparton times, but it is the latest change that sets the current value.
    5. The two Tune:ee and Tune:pp modes can also be changed in exactly the same way as described for all other settings above. Unique for them, however, is that when one of them is encountered it also initiates a call to the initTuneEE(...) or initTunePP(...) method, respectively. In such cases all settings affected by the e^+e^- or pp/ppbar tune are first reset to the default values (the -1 options) and thereafter the relevant tune is set up.
    6. It is possible to mix commands of type 4 and 5 in any order; it is always the last change that counts. That is, any changes you have made to variables of a tune before a Tune:ee or Tune:pp command are overwritten by it, while variables you set after will overwrite the tune values. As a rule, therefore, you want to begin with the tune choice, and thereafter modify only a small part of its settings.
    7. Needless to say, the flexibility can lead to unwanted setups if you do not exercise some discipline. It is therefore recommended that you always check the listing obtained with Pythia::settings.listChanged() to confirm that the final set of changes is the intended one.

    mode  Tune:ee   (default = 0; minimum = -1; maximum = 3)
    Choice of tune to e^+e^- data, mainly for the hadronization and timelike-showering aspects of PYTHIA. You should study the Settings::initTuneEE(...) method to find exactly which are the settings for the respective tune.
    option -1 : reset all values that are affected by any of the e^+e^- tunes to the default values. This option can be used on its own, but is also automatically used as a first step for either of the positive tune values below, to undo the effect of previous tune settings.
    option 0 : no values are overwritten during the initial setup, step 2 above. Note that changing to 0 in the user code has no effect; if you want to restore the individual settings you should instead use -1.
    option 1 : the original PYTHIA 8 parameter set, based on some very old flavour studies (with JETSET around 1990) and a simple tune of alpha_strong to three-jet shapes to the new pT-ordered shower. These were the default values before version 8.125.
    option 2 : a tune by Marc Montull to the LEP 1 particle composition, as published in the RPP (August 2007). No related (re)tune to event shapes has been performed, however.
    option 3 : a tune to a wide selection of LEP1 data by Hendrik Hoeth within the Rivet + Professor framework, both to hadronization and timelike-shower parameters (June 2009). These are the default values starting from version 8.125, so currently there is no need for this option.

    flag  Tune:preferLHAPDF   (default = on)
    Tunes made by experimental collaborations typically use the LHAPDF package to obtain their PDF values, and so PYTHIA has to be linked accordingly. For PDFs implemented natively in PYTHIA it is possible to use the respective tunes, without having to link to LHAPDF, if you set Tune:preferLHAPDF = off before the Tune:pp choice.

    mode  Tune:pp   (default = 5; minimum = -1; maximum = 13)
    Choice of tune to pp/ppbar data, mainly for the initial-state-radiation, multiparton-interactions and beam-remnants aspects of PYTHIA. Note that the previous crude (non-)tunes 3C and 3M are removed as of 8.145, superseded by the 4C tune. You should study the Settings::initTunePP(...) method to find exactly which are the settings for the respective tune.
    option -1 : reset all values that are affected by any of the pp/ppbar tunes to the default values. This option can be used on its own, but is also automatically used as a first step for either of the positive tune values below, to undo the effect of previous tune settings.
    option 0 : no values are overwritten during the initial setup, step 2 above. Note that changing to 0 in the user code has no effect; if you want to restore the individual settings you should instead use -1.
    option 1 : default used up to version 8.126, based on some early and primitive comparisons with data.
    option 2 : "Tune 1", default in 8.127 - 8.139, based on some data comparisons by Peter Skands. Largely but not wholly overlaps with the default option 0.
    option 3 : "Tune 2C", introduced with 8.140 [Cor10a]. It uses the CTEQ 6L1 PDF, and is intended to give good agreement with much of the published CDF data.
    option 4 : "Tune 2M", introduced with 8.140 [Cor10a]. It is uses the MRST LO** PDF, which has a momentum sum somewhat above unity, which is compensated by a smaller alpha_s than in the previous tune. Again it is intended to give good agreement with much of the published CDF data.
    option 5 : "Tune 4C", new tune, introduced with 8.145 [Cor10a]. Starts out from tune 2C, but with a reduced cross section for diffraction, plus modified multiparton interactions parameters to give a higher and more rapidly increasing charged pseudorapidity plateau, for better agreement with some early key LHC numbers. See also the comparative study in [Buc11].
    option 6 : "Tune 4Cx", based on tune 4C, but using the x-dependent matter profile, MultipartonInteractions:bProfile = 4 and an increased MultipartonInteractions:pT0Ref [Cor11].
    option 7 : "ATLAS MB Tune A2-CTEQ6L1", a minimum-bias tune based on tune 4Cx, but without rapidity-ordered spacelike emissions [ATL12]. Uses CTEQ 6L1, by default from LHAPDF.
    option 8 : "ATLAS MB Tune A2-MSTW2008LO", as above, but uses MSTW 2008 LO, by default from LHAPDF.
    option 9 : "ATLAS UE Tune AU2-CTEQ6L1", an underlying-event tune based on tune 4Cx, but without rapidity-ordered spacelike emissions [ATL12]. Uses CTEQ 6L1, by default from LHAPDF.
    option 10 : "ATLAS UE Tune AU2-MSTW2008LO", as above, but uses MSTW 2008 LO, by default from LHAPDF.
    option 11 : "ATLAS UE Tune AU2-CT10", as above, but uses CT 10, which is not currently implemented in PYTHIA, so you must link LHAPDF.
    option 12 : "ATLAS UE Tune AU2-MRST2007LO*", as above, but uses MRST 2007 LO*, by default from LHAPDF.
    option 13 : "ATLAS UE Tune AU2-MRST2007LO**", as above, but uses MRST 2007 LO**, by default from LHAPDF. pythia8-8.1.80.orig/htmldoc/HiddenValleyProcesses.html0000644000175000017500000006157012217615311021120 0ustar sunsun Hidden Valley Processes

    Hidden Valley Processes

    This Hidden Valley (HV) scenario has been developed specifically to allow the study of visible consequences of radiation in a hidden sector, by recoil effect. A key aspect is therefore that the normal timelike showering machinery has been expanded with a third kind of radiation, in addition to the QCD and QED ones. These three kinds of radiation are fully interleaved, i.e. evolution occurs in a common pT-ordered sequence. The scenario is described in [Car10]. Furthermore hadronization in the hidden sector has been implemented. Three main scenarios for production into and decay out of the hidden sector can be compared, in each case either for an Abelian or a non-Abelian gauge group in the HV. For further details see [Car11].

    Particle content and properties

    For simplicity we assume that the HV contains an unbroken SU(N) gauge symmetry. This is used in the calculation of production cross sections. These could be rescaled by hand for other gauge groups.

    mode  HiddenValley:Ngauge   (default = 3; minimum = 1)
    is U(1) for Ngauge = 1, is SU(N) if Ngauge > 1. Note that pair production cross sections contains a factor of Ngauge for new particles in the fundamental representation of this group.

    A minimal HV particle content has been introduced. Firstly, there is a set of 12 particles that mirrors the Standard Model flavour structure, and is charged under both the SM and the HV symmetry groups. Each new particle couples flavour-diagonally to a corresponding SM state, and has the same SM charge and colour, but in addition is in the fundamental representation of the HV colour, as follows:
    Dv, identity 4900001, partner to the normal d quark;
    Uv, identity 4900002, partner to the normal u quark;
    Sv, identity 4900003, partner to the normal s quark;
    Cv, identity 4900004, partner to the normal c quark;
    Bv, identity 4900005, partner to the normal b quark;
    Tv, identity 4900006, partner to the normal t quark;
    Ev, identity 4900011, partner to the normal e lepton;
    nuEv, identity 4900012, partner to the normal nue neutrino;
    MUv, identity 4900013, partner to the normal mu lepton;
    nuMUv, identity 4900014, partner to the normal numu neutrino;
    TAUv, identity 4900015, partner to the normal tau lepton;
    nuTAUv, identity 4900016, partner to the normal nutau neutrino.
    Collectively we will refer to these states as Fv; note, however, that they need not be fermions themselves.

    In addition the model contains the HV gauge particle, either a HV-gluon or a HV-photon, but not both; see Ngauge above:
    gv, identity 4900021, is the massless gauge boson of the HV SU(N) group;
    gammav, identity 4900022, is the massless gauge boson of the HV U(1) group.

    Finally, for the basic HV scenario, there is a new massive particle with only HV charge sitting in the fundamental representation of the HV gauge group:
    qv, identity 4900101.

    The typical scenario would be for pair production of one of the states presented first above, e.g. g g -> Dv Dvbar. Such a Dv can radiate gluons and photons like an SM quark, but in addition HV-gluons or HV-photons in a similar fashion. Eventually the Dv will decay like Dv -> d + qv. The strength of this decay is not set as such, but is implicit in your choice of width for the Dv state. Thereafter the d and qv can radiate further within their respective sectors. The qv, gv or gammav are invisible, so their fate need not be considered further.

    While not part of the standard scenario, as an alternative there is also a kind of Z' resonance:
    Zv, identity 4900023, a boson that can couple both to pairs of Standard Model fermions and to qv qvbar pairs. Mass, total width and branching ratios can be set as convenient.
    This opens up for alternative processes l^+l^-, q qbar -> Zv -> qv qvbar.

    The possibility of a leakage back from the hidden sector will be considered in the Hadronization section below. For the U(1) case the gammav acquires a mass and can decay back to a Standard-Model fermion pair, while the qv remains invisible. The SU(N) alternative remains unbroken, so confinement holds and the gv is massless. A string like qv - gv - ... - gv - qvbar can break by the production of new qv - qvbar pairs, which will produce qv-qvbar mesons. It would be possible to build a rather sophisticated hidden sector by trivial extensions of the HV flavour content. For now, however, the qv can be duplicated in up to eight copies with the same properties except for the flavour charge. These are assigned codes 4900101 - 4900108. This gives a total of 64 possible lowest-lying mesons. We also include a duplication of that, into two multiplets, corresponding to the pseudoscalar and vector mesons of QCD. For now, again, these are assumed to have the same mass and other properties. Only the flavour-diagonal ones can decay back into the Standard-Model sector, however, while the rest remains in the hidden sector. It is therefore only necessary to distinguish a few states:
    pivDiag, identity 4900111, a flavour-diagonal HV-meson with spin 0 that can decay back into the Standard-Model sector;
    rhovDiag, identity 4900113, a flavour-diagonal HV-meson with spin 1 that can decay back into the Standard-Model sector;
    pivUp, identity 4900211, an off-diagonal HV-meson with spin 0 that is stable and invisible, with an antiparticle pivDn with identity -4900211; the particle is the one where the code of the flavour is larger than that of the antiflavour;
    rhovUp, identity 4900213, an off-diagonal HV-meson with spin 1 that is stable and invisible, with an antiparticle rhovDn with identity -4900213; again the particle is the one where the code of the flavour is larger than that of the antiflavour;
    ggv, identity 4900991, is only rarely used, to handle cases where it is kinematically impossible to produce an HV-meson on shell, and it therefore is assumed to de-excite by the emission of invisible gv-gv v-glueball bound states.

    Only the spin of the HV-gluon or HV-photon is determined unambiguously to be unity, for the others you can make your choice.

    mode  HiddenValley:spinFv   (default = 1; minimum = 0; maximum = 2)
    The spin of the HV partners of the SM fermions, e.g. Dv, Uv, Ev and nuEv.
    option 0 : spin 0.
    option 1 : spin 1/2.
    option 2 : spin 1.

    mode  HiddenValley:spinqv   (default = 0; minimum = 0; maximum = 1)
    The spin of qv when the Fv (the HV partners of the SM fermions) have spin 1/2. (While, if they have spin 0 or 1, the qv spin is fixed at 1/2.)
    option 0 : spin 0.
    option 1 : spin 1.

    parm  HiddenValley:kappa   (default = 1.)
    If the Fv have spin 1 then their production cross section depends on the presence of anomalous magnetic dipole moment, i.e. of a kappa different from unity. For other spins this parameter is not used.

    flag  HiddenValley:doKinMix   (default = off)
    allow kinematic mixing or not.

    parm  HiddenValley:kinMix   (default = 1.)
    strength of kinetic mixing.

    You should set the Fv and qv masses appropriately, with the latter smaller than the former two to allow decays. When U(1) hadronization is switched on, you need to set the gammav mass and decay modes. For SU(N) hadronization the HV-meson masses should be set to match the qv ones. The simplest is to assume that m_qv defines a constituent mass, so that m_HVmeson = 2 m_qv. The hvMesonDiag decay modes also need to be set.

    Production processes

    flag  HiddenValley:all   (default = off)
    Common switch for the group of all hard Hidden Valley processes, as listed separately in the following.

    flag  HiddenValley:gg2DvDvbar   (default = off)
    Pair production g g -> Dv Dvbar. Code 4901.

    flag  HiddenValley:gg2UvUvbar   (default = off)
    Pair production g g -> Uv Uvbar. Code 4902.

    flag  HiddenValley:gg2SvSvbar   (default = off)
    Pair production g g -> Sv Svbar. Code 4903.

    flag  HiddenValley:gg2CvCvbar   (default = off)
    Pair production g g -> Cv Cvbar. Code 4904.

    flag  HiddenValley:gg2BvBvbar   (default = off)
    Pair production g g -> Bv Bvbar. Code 4905.

    flag  HiddenValley:gg2TvTvbar   (default = off)
    Pair production g g -> Tv Tvbar. Code 4906.

    flag  HiddenValley:qqbar2DvDvbar   (default = off)
    Pair production q qbar -> Dv Dvbar via intermediate gluon. Code 4911.

    flag  HiddenValley:qqbar2UvUvbar   (default = off)
    Pair production q qbar -> Uv Uvbar via intermediate gluon. Code 4912.

    flag  HiddenValley:qqbar2SvSvbar   (default = off)
    Pair production q qbar -> Sv Svbar via intermediate gluon. Code 4913.

    flag  HiddenValley:qqbar2CvCvbar   (default = off)
    Pair production q qbar -> Cv Cvbar via intermediate gluon. Code 4914.

    flag  HiddenValley:qqbar2BvBvbar   (default = off)
    Pair production q qbar -> Bv Bvbar via intermediate gluon. Code 4915.

    flag  HiddenValley:qqbar2TvTvbar   (default = off)
    Pair production q qbar -> Tv Tvbar via intermediate gluon. Code 4916.

    flag  HiddenValley:ffbar2DvDvbar   (default = off)
    Pair production f fbar -> Dv Dvbar via intermediate gamma*/Z^*. Code 4921.

    flag  HiddenValley:ffbar2UvUvbar   (default = off)
    Pair production f fbar -> Uv Uvbar via intermediate gamma*/Z^*. Code 4922.

    flag  HiddenValley:ffbar2SvSvbar   (default = off)
    Pair production f fbar -> Sv Svbar via intermediate gamma*/Z^*. Code 4923.

    flag  HiddenValley:ffbar2CvCvbar   (default = off)
    Pair production f fbar -> Cv Cvbar via intermediate gamma*/Z^*. Code 4924.

    flag  HiddenValley:ffbar2BvBvbar   (default = off)
    Pair production f fbar -> Bv Bvbar via intermediate gamma*/Z^*. Code 4925.

    flag  HiddenValley:ffbar2TvTvbar   (default = off)
    Pair production f fbar -> Tv Tvbar via intermediate gamma*/Z^*. Code 4926.

    flag  HiddenValley:ffbar2EvEvbar   (default = off)
    Pair production f fbar -> Ev Evbar via intermediate gamma*/Z^*. Code 4931.

    flag  HiddenValley:ffbar2nuEvnuEvbar   (default = off)
    Pair production f fbar -> nuEv nuEvbar via intermediate gamma*/Z^*. Code 4932.

    flag  HiddenValley:ffbar2MUvMUvbar   (default = off)
    Pair production f fbar -> MUv MUvbar via intermediate gamma*/Z^*. Code 4933.

    flag  HiddenValley:ffbar2nuMUvnuMUvbar   (default = off)
    Pair production f fbar -> nuMUv nuMUvbar via intermediate gamma*/Z^*. Code 4934.

    flag  HiddenValley:ffbar2TAUvTAUvbar   (default = off)
    Pair production f fbar -> TAUv TAUvbar via intermediate gamma*/Z^*. Code 4935.

    flag  HiddenValley:ffbar2nuTAUvnuTAUvbar   (default = off)
    Pair production f fbar -> nuTAUv nuTAUvbar via intermediate gamma*/Z^*. Code 4936.

    flag  HiddenValley:ffbar2Zv   (default = off)
    Production f fbar -> Zv where Zv is a generic resonance that couples both SM fermion pairs and a qv qvbar pair. Not part of the framework of the above processes, but as an alternative. Code 4941.

    Timelike showers

    One key point of this HV scenario is that radiation off the HV-charged particles is allowed. This is done by the standard final-state showering machinery. (HV particles are not produced in initial-state radiation.) All the (anti)particles Fv and qv have one (negative) unit of HV charge. That is, radiation closely mimics the one in QCD. Both QCD, QED and HV radiation are interleaved in one common sequence of decreasing emission pT scales. Each radiation kind defines a set of dipoles, usually spanned between a radiating parton and its recoil partner, such that the invariant mass of the pair is not changed when a radiation occurs. This need not follow from trivial colour assignments, but is often obvious. For instance, in a decay Qv -> q + qv the QCD dipole is between the q and the hole after Qv, but qv becomes the recoiler should a radiation occur, while the role of q and qv is reversed for HV radiation.

    This also includes matrix-element corrections for a number of decay processes, with colour, spin and mass effects included [Nor01]. They were calculated within the context of the particle content of the MSSM, however, which does not include spin 1 particles with unit colour charge. In such cases spin 0 is assumed instead. By experience, the main effects come from mass and colour flow anyway, so this is not a bad approximation. (Furthermore the MSSM formulae allow for gamma_5 factors from wave functions or vertices; these are even less important.)

    An emitted gv can branch in its turn, gv -> gv + gv. This radiation may affect momenta in the visible sector by recoil effect, but this is a minor effect relative to the primary emission of the gv.

    flag  HiddenValley:FSR   (default = off)
    switch on final-state shower of gv or gammav in a HV production process.

    parm  HiddenValley:alphaFSR   (default = 0.1; minimum = 0.0)
    fixed alpha scale of gv/gammav emission; corresponds to alpha_strong of QCD or alpha_em of QED. For shower branchings such as Dv -> Dv + gv the coupling is multiplied by C_F = (N^2 - 1) / (2 * N) for an SU(N) group and for gv -> gv + gv by N.

    parm  HiddenValley:pTminFSR   (default = 0.4; minimum = 0.1)
    lowest allowed pT of emission. Chosen with same default as in normal QCD showers.

    Hadronization

    By default the HV particles with no Standard Model couplings are not visible. Their presence can only be deduced by the observation of missing (transverse) momentum in the event as a whole. In the current implementation it is possible to simulate two different scenarios where activity can leak back from the hidden sector.

    The first possibility is relevant for the U(1) scenario. The U(1) group may be broken, so that the gammav acquires a mass. Furthermore, the gammav may have a small mixing angle with the normal photon, or with some Z' state or other mediator, and may thus decay back into Standard Model particles. The qv still escapes undetected; recall that there is no confinement in the U(1) option.

    In order to enable this machinery two commands are necessary, 4900022:m0 = ... to set the gammav mass to the desired value, and 4900022:onMode = on to enable gammav decays. The default gammav decay table contains all Standard Model fermion-antifermion pairs, except top, with branching ratios in proportion to their coupling to the photon, whenever the production channel is allowed by kinematics. This table could easily be tailored to more specific models and needs. For instance, for a mass below 1 - 2 GeV, it would make sense to construct a table of exclusive hadronic decay channels rather than go the way via a hadronizing quark pair.

    The gammav are expected to decay so rapidly that no secondary vertex will be detectable. However, it is possible to set 4900022:tau0 to a finite lifetime (in mm) that will be used to create separated secondary vertices.

    The second, more interesting, possibility is relevant for the SU(N) scenarios. Here the gauge group remains unbroken, i.e. gv is massless, and the partons are confined. Like in QCD, the HV-partons can therefore be arranged in one single HV-colour-ordered chain, with a qv in one end, a qvbar in the other, and a varying number of gv in between. Each event will only contain (at most) one such string, (i) since perturbative branchings gv -> qv qvbar have been neglected, as is a reasonable approximation for QCD, and (ii) since HV-colours are assigned in the N_C -> infinity limit, just like in the handling of string fragmentation in QCD. The HV-string can then fragment by the nonperturbative creation of qv qvbar pairs, leading to the formation of HV-mesons along the string, each with its qv from one vertex and its qvbar from the neighbouring one.

    Since, so far, we have only assumed there to be one qv species, all produced qv qvbar HV-mesons are of the same flavour-diagonal species. Such an HV-meson can decay back to the normal sector, typically by whatever mediator particle allowed production in the first place. In this framework the full energy put into the HV sector will leak back to the normal one. To allow more flexibility, an ad hoc possibility of n_Flav different qv species is introduced. For now they are all assumed to have the same mass and other properties, but distinguished by some flavour-like property. Only the flavour-diagonal ones can decay, meaning that only a fraction (approximately) 1/n_Flav of the HV-energy leaks back, while the rest remains in the hidden sector.

    This scenario contains more parameters than the first one, for the U(1) group. They can be subdivided into two sets. One is related to particle properties, both for qv and for the two different kinds of HV-mesons, here labeled 4900111 and 4900113 for the diagonal ones, and +-4900211 and +-4900213 for the off-diagonal ones. It makes sense to set the HV-meson masses to be twice the qv one, as in a simple constituent mass context. Furthermore the hvMesonDiag decay modes need to be set up. Like with the gammav in the U(1) option, the default decay table is based on the branching ratios of an off-shell photon.

    The second set are fragmentation parameters that extend or replace the ones used in normal string fragmentation. Some of them are not encoded in the same way as normally, however, but rather scale as the qv mass is changed, so as to keep a sensible default behaviour. This does not mean that deviations from this set should not be explored, or that other scaling rules could be preferred within alternative scenarios. These parameters are as follows.

    flag  HiddenValley:fragment   (default = off)
    switch on string fragmentation of the HV partonic system. Only relevant for SU(N) scenarios.

    mode  HiddenValley:nFlav   (default = 1; minimum = 1; maximum = 8)
    number of different flavours assumed to exist in the hadronization description, leading to approximately 1/n_Flav of the produced HV-mesons being flavour-diagonal and capable to decay back to Standard Model particles.

    parm  HiddenValley:probVector   (default = 0.75; minimum = 0.; maximum = 1.)
    fraction of HV-mesons that are assigned spin 1 (vector), with the remainder spin 0 (pseudoscalar). Assuming the qv have spin 1/2 and the mass splitting is small, spin counting predicts that 3/4 of the mesons should have spin 1.

    parm  HiddenValley:aLund   (default = 0.3; minimum = 0.0; maximum = 2.0)
    The a parameter of the Lund symmetric fragmentation function. See the normal fragmentation function description for the shape of this function.

    parm  HiddenValley:bmqv2   (default = 0.8; minimum = 0.2; maximum = 2.0)
    The b parameter of the Lund symmetric fragmentation function, multiplied by the square of the qv mass. This scaling ensures that the fragmentation function keeps the same shape when the qv mass is changed (neglecting transverse momenta).

    parm  HiddenValley:rFactqv   (default = 1.0; minimum = 0.0; maximum = 2.0)
    r_qv, i.e. the Bowler correction factor to the Lund symmetric fragmentation function, which could be made weaker or stronger than its natural value.

    parm  HiddenValley:sigmamqv   (default = 0.5; minimum = 0.0)
    the width sigma of transverse momenta in the HV fragmentation process, normalized to the qv mass. This ensures that sigma scales proportionately to m_qv. See the normal fragmentation pT description for conventions for factors of 2. pythia8-8.1.80.orig/htmldoc/TotalCrossSections.html0000644000175000017500000002562512217615311020467 0ustar sunsun Total Cross Sections

    Total Cross Sections

    The SigmaTotal class returns the total, elastic, diffractive and nondiffractive cross sections in hadronic collisions, and also the slopes of the d(sigma)/dt distributions. Most of the parametrizations used are from [Sch94, Sch97] which borrows some of the total cross sections from [Don92]. If you use the MBR (Minimum Bias Rockefeller) model [Cie12], Diffraction:PomFlux = 5, this model contains its own parametrizations of all cross sections in p p and pbar p collisions.

    There are strong indications that the currently implemented diffractive cross section parametrizations, which should be in reasonable agreement with data at lower energies, overestimate the diffractive rate at larger values. If you wish to explore this (or other) aspect, it is possible to override the cross section values in two different ways. The first offers (almost) complete freedom, but needs to be defined separately for each CM energy, while the second introduces a simpler parametrized damping. The two cannot be combined. Furthermore the Coulomb term for elastic scattering, which by default is off, can be switched on.

    The allowed combinations of incoming particles are p + p, pbar + p, pi+ + p, pi- + p, pi0/rho0 + p, phi + p, J/psi + p, rho + rho, rho + phi, rho + J/psi, phi + phi, phi + J/psi, J/psi + J/psi. The strong emphasis on vector mesons is related to the description of gamma + p and gamma + gamma interactions in a Vector Dominance Model framework (which will not be available for some time to come, so this is a bit of overkill). Nevertheless, the sections below, with allowed variations, are mainly intended to make sense for p + p.

    Central diffraction

    Central diffraction (CD), a.k.a. double Pomeron exchange (DPE), was not part of the framework in [Sch94]. It has now been added for multiparticle states, i.e. excluding the resonance region below 1 GeV mass, as well as other exclusive states, but only for p p or pbar p. It uses the same proton-Pomeron vertex as in single diffraction, twice, to describe x_Pomeron and t spectra. This fixes the energy dependence, which has been integrated and parametrized. The absolute normalization has been left open, however. Furthermore, since CD has not been included in previous tunes to data, a special flag is available to reproduce the old behaviour (with due complications when one does not want to do this).

    parm  SigmaTotal:sigmaAXB2TeV   (default = 1.5; minimum = 0.)
    The CD cross section for p p and pbar p collisions, normalized to its value at 2 TeV CM energy, expressed in mb. The energy dependence is then parametrized, and behaves roughly like ln^1.5(s). Is used for the options Diffraction:PomFlux = 1 - 4, while the MBR model (= 5) has its own parametrization.

    flag  SigmaTotal:zeroAXB   (default = off)
    several existing tunes do not include CD. An inclusion of a nonvanishing CD cross section directly affects the nondiffractive phenomenology (even if not dramatically), and so this flag is used to switch off the CD cross section in such tunes. You can switch it back on after the selection of a tune, if you so wish. This option has no effect for the MBR model (Diffraction:PomFlux = 5), where the CD cross section has been included from the onset.

    Set cross sections

    flag  SigmaTotal:setOwn   (default = off)
    Allow a user to set own cross sections by hand; on/off = true/false.

    When SigmaTotal:setOwn = on, the user is expected to set values for the corresponding cross sections:

    parm  SigmaTotal:sigmaTot   (default = 80.; minimum = 0.)
    Total cross section in mb.

    parm  SigmaTotal:sigmaEl   (default = 20.; minimum = 0.)
    Elastic cross section in mb.

    parm  SigmaTotal:sigmaXB   (default = 8.; minimum = 0.)
    Single Diffractive cross section A + B -> X + B in mb.

    parm  SigmaTotal:sigmaAX   (default = 8.; minimum = 0.)
    Single Diffractive cross section A + B -> A + X in mb.

    parm  SigmaTotal:sigmaXX   (default = 4.; minimum = 0.)
    Double Diffractive cross section A + B -> X_1 + X_2 in mb.

    parm  SigmaTotal:sigmaAXB   (default = 1.; minimum = 0.)
    Central Diffractive cross section A + B -> A + X + B in mb.

    Note that the total cross section subtracted by the elastic and various diffractive ones gives the inelastic nondiffractive cross section, which therefore is not set separately. If this cross section evaluates to be negative the internal parametrizations are used instead of the ones here. However, since the nondiffractive inelastic cross section is what makes up the minimum-bias event class, and plays a major role in the description of multiparton interactions, it is important that a consistent set is used.

    Dampen diffractive cross sections

    As already noted, unitarization effects may dampen the rise of diffractive cross sections relative to the default parametrizations. The settings here allows one way to introduce a dampening, which is used in some of the existing tunes.

    flag  SigmaDiffractive:dampen   (default = no)
    Allow a user to dampen diffractive cross sections; on/off = true/false.

    When SigmaDiffractive:dampen = on, the three diffractive cross sections are damped so that they never can exceed the respective values below. Specifically, if the standard parametrization gives the cross section sigma_old(s) and a fixed sigma_max is set, the actual cross section becomes sigma_new(s) = sigma_old(s) * sigma_max / (sigma_old(s) + sigma_max). This reduces to sigma_old(s) at low energies and to sigma_max at high ones. Note that the asymptotic value is approached quite slowly, however.

    parm  SigmaDiffractive:maxXB   (default = 15.; minimum = 0.)
    The above sigma_max for A + B -> X + B in mb.

    parm  SigmaDiffractive:maxAX   (default = 15.; minimum = 0.)
    The above sigma_max for A + B -> A + X in mb.

    parm  SigmaDiffractive:maxXX   (default = 15.; minimum = 0.)
    The above sigma_max for A + B -> X_1 + X_2 in mb.

    parm  SigmaDiffractive:maxAXB   (default = 3.; minimum = 0.)
    The above sigma_max for A + B -> A + X + B in mb.

    As above, a reduced diffractive cross section automatically translates into an increased nondiffractive one, such that the total (and elastic) cross section remains fixed.

    Set elastic cross section

    In the above option the t slopes are based on the internal parametrizations. In addition there is no Coulomb-term contribution to the elastic (or total) cross section, which of course becomes infinite if this contribution is included. If you have switched on SigmaTotal:setOwn you can further switch on a machinery to include the Coulomb term, including interference with the conventional strong-interaction Pomeron one [Ber87]. Then the elastic cross section is no longer taken from SigmaTotal:sigmaEl but derived from the parameters below and SigmaTotal:sigmaTot, using the optical theorem. The machinery is only intended to be used for p p and pbar p collisions. The description of diffractive events, and especially their slopes, remains unchanged.

    flag  SigmaElastic:setOwn   (default = no)
    Allow a user to set parameters for the normalization and shape of the elastic cross section the by hand; yes/no = true/false.

    parm  SigmaElastic:bSlope   (default = 18.; minimum = 0.)
    the slope b of the strong-interaction term exp(bt), in units of GeV^-2.

    parm  SigmaElastic:rho   (default = 0.13; minimum = -1.; maximum = 1.)
    the ratio of the real to the imaginary parts of the nuclear scattering amplitude.

    parm  SigmaElastic:lambda   (default = 0.71; minimum = 0.1; maximum = 2.)
    the main parameter of the electric form factor G(t) = lambda^2 / (lambda + |t|)^2, in units of GeV^2.

    parm  SigmaElastic:tAbsMin   (default = 5e-5; minimum = 1e-10)
    since the Coulomb contribution is infinite a lower limit on |t| must be set to regularize the divergence, in units of GeV^2.

    parm  SigmaElastic:phaseConst   (default = 0.577)
    The Coulomb term is taken to contain a phase factor exp(+- i alpha phi(t)), with + for p p and - for pbar p, where phi(t) = - phaseConst - ln(-B t/2). This constant is model dependent [Cah82]. pythia8-8.1.80.orig/htmldoc/TopProcesses.html0000644000175000017500000000410512217615311017301 0ustar sunsun Top Processes

    Top Processes

    Different ways to produce top quarks, singly or in pairs.

    flag  Top:all   (default = off)
    Common switch for the group of top production.

    flag  Top:gg2ttbar   (default = off)
    Scatterings g g -> t tbar. Code 601.

    flag  Top:qqbar2ttbar   (default = off)
    Scatterings q qbar -> t tbar by gluon exchange. Code 602.

    flag  Top:qq2tq(t:W)   (default = off)
    Scatterings q q' -> t q'' by t-channel exchange of a W^+- boson. Code 603.

    flag  Top:ffbar2ttbar(s:gmZ)   (default = off)
    Scatterings f fbar -> t tbar by s-channel exchange of a gamma^*/Z^0 boson. Code 604.

    flag  Top:ffbar2tqbar(s:W)   (default = off)
    Scatterings f fbar' -> t q'' by s-channel exchange of a W^+- boson. Code 605.

    flag  Top:gmgm2ttbar   (default = off)
    Scatterings gamma gamma -> t tbar. Code 606.

    By default top always decays to a W and a down-type quark. It is possible to switch on the t -> H+ b decay mode. Note that its partial width is calculated using the tan(beta) value stored in HiggsHchg:tanBeta, so that it can be used without having to read in a SUSY parameter file. For the H+ to decay also Higgs:useBSM = on is necessary. pythia8-8.1.80.orig/htmldoc/LeptoquarkProcesses.html0000644000175000017500000000731012217615311020667 0ustar sunsun Leptoquark Processes

    Leptoquark Processes

    Leptoquarks arise in many scenarios, and can have widely different characteristics, with respect to spin, isospin am d flavour. The current implementation in no sense attempts to exhaust these possibilities, but only to encode one of the simplest possibilities, with a single scalar leptoquark, denoted LQ and assigned PDG code 42. The leptoquark is assumed to carry specific quark and lepton quantum numbers, by default u quark plus electron. These flavour numbers are conserved, i.e. a process such as u e^- -> LQ -> d nu_e is not allowed.

    Although only one leptoquark is implemented, its flavours may be changed arbitrarily to study the different possibilities. The flavours of the leptoquark are defined by the quark and lepton flavours in the decay mode list. Therefore, to change from the current u e^- to c mu^+, say, you only need a line
    pythia.readString("42:0:products = 4 -13");
    in your main program, or the equivalent in a command file. The former must always be a quark, while the latter could be a lepton or an antilepton; a charge-conjugate partner is automatically defined by the program. At initialization, the charge is recalculated as a function of the flavours defined; also the leptoquark name is redefined to be of the type LQ_q,l, where actual quark and lepton flavours are displayed.

    The leptoquark is likely to be fairly long-lived, in which case it could have time to fragment into a mesonic- or baryonic-type state, which would decay later on. Currently this possibility is not handled; therefore the leptoquark is always assumed to decay before fragmentation. For that reason the leptoquark can also not be put stable.

    Production processes

    Four production processes have been implemented, which normally would not overlap and therefore could be run together.

    flag  LeptoQuark:all   (default = off)
    Common switch for the group of lowest-order LQ production processes, i.e. the four ones below.

    flag  LeptoQuark:ql2LQ   (default = off)
    Scatterings q l -> LQ. Code 3201.

    flag  LeptoQuark:qg2LQl   (default = off)
    Scatterings q g -> LQ l. Code 3202.

    flag  LeptoQuark:gg2LQLQbar   (default = off)
    Scatterings g g -> LQ LQbar. Code 3203.

    flag  LeptoQuark:qqbar2LQLQbar   (default = off)
    Scatterings q qbar -> LQ LQbar. Code 3204.

    Parameters

    In the above scenario the main free parameters are the leptoquark flavour content, set as already described, and the LQ mass, set as usual. In addition there is one further parameter.

    parm  LeptoQuark:kCoup   (default = 1.0; minimum = 0.0)
    multiplicative factor in the LQ -> q l squared Yukawa coupling, and thereby in the LQ width and the q l -> LQ and other cross sections. Specifically, lambda^2/(4 pi) = k alpha_em, i.e. it corresponds to the $k$ factor of [Hew88]. pythia8-8.1.80.orig/htmldoc/EventStatistics.html0000644000175000017500000001425112217615312020010 0ustar sunsun Event Statistics

    Event Statistics

    At the end of the run you will want to write out the final statistics on number of events generated, the corresponding cross sections and the number of errors encountered. This is done either with the pythia.stat() method or the pythia.statistics() one, assuming pythia is an instance of the Pythia class.The former method is steered entirely by settings values, see here. The latter, deprecated one instead takes two arguments:

    void Pythia::statistics(bool all = false, bool reset = false)  
    write out statistics on cross sections and errors. This is based on calls to the methods below, for the two kinds of information.
    argument all : if true it allows a more extensive listing than the default one, see multiparton-interactions statistics below.
    argument reset : if true it implies that all counters, e.g on events generated and errors experienced, are reset to zero whenever the routine is called. The default instead is that all stored statistics information is unaffected by the call. Counters are automatically reset in each new Pythia::init() call, however, so the only time the reset option makes a difference is if statistics(...) is called several times in a (sub)run.

    Cross-section statistics

    The ProcessLevel::statistics() method cannot be accessed directly, but only via the Pythia::stat() and Pythia::statistics(...) calls above. When called it will loop over the list of existing processes, and for each write out name, code, the number of tried, selected and accepted events, the cross section and the estimated error on the latter. The three different event numbers are related to the Monte Carlo method used, whereby an initial upper estimate of the cross section is used to select a large number of trial phase-space points, whereof then not all survive. Rejections are normally done by the internal machinery, but can also be obtained by user hooks. Therefore:
    • tried events reflect the original number of phase-space points probed, as part of the upper estimate;
    • selected events correspond to those that survive the internal Monte-Carlo selection procedure;
    • accepted events are those that also survive the additional user cuts.
    In most runs there would be no user hooks implemented, and then the numbers of selected and of accepted events will agree. Aborted events (see below) usually appear in the selected statistics but not in the accepted one.

    For Les Houches events the total cross section will be correctly displayed; however the (optional) error value will not be used, so that the reported error will be smaller than the correct statistical ones, and often vanish completely. Furthermore, while the number of events is shown for each user process, the cross section is only for the sum of them.

    Error messages

    When Pythia is run, errors may occur, and give rise to warning messages. These may be of varying severity, as follows:
    • Abort means things went seriously wrong, and the initialization or event generation failed. In the former case it is not possible to generate events at all, in the latter the current event is flawed and should be skipped. In either case the respective method, Pythia::init() or Pythia::next(), then also returns the value false. There are occasions where an abort may be deliberate, such as when a file of Les Houches Events is read and the end of the file is reached.
    • Error normally is less severe. Typically the program will back up one step and try again. There are cases where this is not possible, in particular during the initialization and the generation of a hard process, and then the error may be followed by an abort as a direct consequence (with two separate messages).
    • Warning is even less severe. In some cases the program will try again, with good chances of success, in others no measure at all need to be taken.

    The error messages is handled by a small part of the Info class. It is handed any abort, error or warning messages during the event generation phase, and will store each distinct message, with a counter for how many times it is issued. Thus it is possible to limit the number of identical messages issued, currently hardcoded so that each kind of error message is only printed once (static const int TIMESTOPRINT = 1). This can be overridden by the calling routine, so that all messages of this kind are shown, which is particularly relevant for the initialization stage. The summary table printed by Pythia::statistics() provides a table with all the different messages issued, in alphabetical order, with the total number of times each was generated.

    Multiparton-interactions statistics

    If you call Pythia::statistics(true), i.e. with the first optional argument true, also statistics on multiparton interactions is printed, comprising a list of all allowed subprocesses with how many times each of them has been generated. For the nondiffractive process this also includes the hardest interaction, while else the hardest process is excluded from the statistics. (This is because the hardest process is of the same character and generated by the same machinery in the former case but not in the latter. Also, for the former case only, the standard statistics listing only lists nondiffractive as one single process, i.e. does not further specify the character of the hardest subprocess, so there is not any overlap between the two.) pythia8-8.1.80.orig/htmldoc/JetFinders.html0000644000175000017500000000513012217615312016705 0ustar sunsun Jet Finders

    Jet Finders

    Pythia comes with three built-in jet finders, ClusterJet for e^+e^- events and SlowJet and CellJetfor hadron collider ones. Especially the latter is not so well matched to the standards of its field, however. (But it is closely related to the anti-kT algorithm, so is also not completely disconnected [Cac08].)

    SlowJet can do jet finding according to the current-day kT, Cambridge/Aachen and anti-kT algorithms. It can be run in two modes. The original one is a native implementation which, as the name indicates, is rather slow. However, with the release of the fjcore code from FastJet [Cac06, Cac12], the default mode has become to use the fjcore methods. This is transparent to the user.

    FastJet

    SlowJet does not exhaust all the posssibilities of the fjcore code, so users are welcome to extend on the existing functionality by a direct usage of the fjcore methods.

    Missing from fjcore is a number of aspects, such as jet areas functionality, background estimation, access to other algorithms via plugins, interface to CGAL and tools such as filters and taggers. Therefore, for more sophisticated jet studies the complete FastJet package needs to be linked. This is foreseen in the configure file in the examples subdirectory, and the main71.cc and main72.cc programs contain examples how it can be used with Pythia events. (Even if these examples do not go beyond the functionality that SlowJet can offer.)

    The latter program makes use of the include/Pythia8/FastJet3.h header file, contributed by Gavin Salam. This allows simple input of a Pythia particle into a FastJet one, either retaining only the four-momentum or the full particle information. Thereby more sophisticated selectors become possible at the FastJet level. This code could be duplicated, with trivial modifications, to augment the fjcore package functionality in an identical manner, should the need arise. pythia8-8.1.80.orig/htmldoc/StandardModelParameters.html0000644000175000017500000003700012217615311021415 0ustar sunsun Standard-Model Parameters

    Standard-Model Parameters

    The strong coupling

    The AlphaStrong class is used to provide a first- or second-order running alpha_strong (or, trivially, a zeroth-order fixed one). Formulae are the standard ones found in [Yao06]. The second-order expression used, eq. (9.5), may be somewhat different in other approaches (with differences formally of higher order), so do not necessarily expect perfect agreement, especially not at small Q^2 scales. The starting alpha_strong value is defined at the M_Z mass scale. The Lambda values are matched at the c, b and t flavour thresholds, such that alpha_strong is continuous. For second-order matching an approximate iterative method is used.

    For backwards compatibility, the following global switch determines whether 5- or 6-flavour running will be used above the t threshold:

    mode  StandardModel:alphaSnfmax   (default = 6; minimum = 5; maximum = 6)

    option 5 : Use 5-flavour running for all scales above the b flavour threshold (old default).
    option 6 : Use 6-flavour running above the t threshold (new default).

    Since we allow alpha_strong to vary separately for hard processes, timelike showers, spacelike showers and multiparton interactions, all other relevant values are set in each of these classes. The default behaviour is everywhere first-order running.

    The alpha_strong calculation is initialized by init( value, order, nfmax), where value is the alpha_strong value at M_Z, order is the order of the running, 0, 1 or 2, and nfmax is the highest number of flavours to include in the running. Thereafter the value can be calculated by alphaS(scale2), where scale2 is the Q^2 scale in GeV^2.

    For applications inside shower programs, a second-order alpha_s value can be obtained as the product of the two functions alphaS1Ord(scale2) and alphaS2OrdCorr(scale2), where the first gives a simple first-order running (but with the second-order Lambda) and the second the correction factor, below unity, for the second-order terms. This allows a compact handling of evolution equations.

    Resummation arguments [Cat91] show that a set of universal QCD corrections can be absorbed in coherent parton showers by applying the so-called CMW rescaling of the MSbar value of Lambda_QCD. This can be accomplished via a fourth (optional) boolean argument to init( value, order, nfmax, useCMW), with default value useCMW = false. When set to true, the translation amounts to an N_F-dependent rescaling of Lambda_QCD, relative to its MSbar value, by a factor 1.661 for NF=3, 1.618 for NF=4, 1.569 for NF=5, and 1.513 for NF=6. When using this option, be aware that the original CMW arguments were derived using two-loop running and that the CMW rescaling may need be taken into account in the context of matrix-element matching. Note also that this option has only been made available for timelike and spacelike showers, not for hard processes.

    The electromagnetic coupling

    The AlphaEM class is used to generate a running alpha_em. The input StandardModel:alphaEMmZ value at the M_Z mass is matched to a low-energy behaviour with running starting at the electron mass threshold. The matching is done by fitting an effective running coefficient in the region between the light-quark threshold and the charm/tau threshold. This procedure is approximate, but good enough for our purposes.

    Since we allow alpha_em to vary separately for hard processes, timelike showers, spacelike showers and multiparton interactions, the choice between using a fixed or a running alpha_em can be made in each of these classes. The default behaviour is everywhere first-order running. The actual values assumed at zero momentum transfer and at M_Z are only set here, however.

    parm  StandardModel:alphaEM0   (default = 0.00729735; minimum = 0.0072973; maximum = 0.0072974)
    The alpha_em value at vanishing momentum transfer (and also below m_e).

    parm  StandardModel:alphaEMmZ   (default = 0.00781751; minimum = 0.00780; maximum = 0.00783)
    The alpha_em value at the M_Z mass scale. Default is taken from [Yao06].

    The alpha_em calculation is initialized by init(order), where order is the order of the running, 0 or 1, with -1 a special option to use the fix value provided at M_Z. Thereafter the value can be calculated by alphaEM(scale2), where scale2 is the Q^2 scale in GeV^2.

    The electroweak couplings

    There are two degrees of freedom that can be set, related to the electroweak mixing angle:

    parm  StandardModel:sin2thetaW   (default = 0.2312; minimum = 0.225; maximum = 0.240)
    The sine-squared of the weak mixing angle, as used in all Z^0 and W^+- masses and couplings, except for the vector couplings of fermions to the Z^0, see below. Default is the MSbar value from [Yao06].

    parm  StandardModel:sin2thetaWbar   (default = 0.2315; minimum = 0.225; maximum = 0.240)
    The sine-squared of the weak mixing angle, as used to derive the vector couplings of fermions to the Z^0, in the relation v_f = a_f - 4 e_f sin^2(theta_W)bar. Default is the effective-angle value from [Yao06].

    The Fermi constant is not much used in the currently coded matrix elements, since it is redundant, but it is available:

    parm  StandardModel:GF   (default = 1.16637e-5; minimum = 1.0e-5; maximum = 1.3e-5)
    The Fermi coupling constant, in units of GeV^-2.

    The quark weak-mixing matrix

    The absolute values of the Cabibbo-Kobayashi-Maskawa matrix elements are set by the following nine real values taken from [Yao06] - currently the CP-violating phase is not taken into account in this parametrization. It is up to the user to pick a consistent unitary set of new values whenever changes are made.

    parm  StandardModel:Vud   (default = 0.97383; minimum = 0.973; maximum = 0.975)
    The V_ud CKM matrix element.

    parm  StandardModel:Vus   (default = 0.2272; minimum = 0.224; maximum = 0.230)
    The V_us CKM matrix element.

    parm  StandardModel:Vub   (default = 0.00396; minimum = 0.0037; maximum = 0.0042)
    The V_ub CKM matrix element.

    parm  StandardModel:Vcd   (default = 0.2271; minimum = 0.224; maximum = 0.230)
    The V_cd CKM matrix element.

    parm  StandardModel:Vcs   (default = 0.97296; minimum = 0.972; maximum = 0.974)
    The V_cs CKM matrix element.

    parm  StandardModel:Vcb   (default = 0.04221; minimum = 0.0418; maximum = 0.0426)
    The V_cb CKM matrix element.

    parm  StandardModel:Vtd   (default = 0.00814; minimum = 0.006; maximum = 0.010)
    The V_td CKM matrix element.

    parm  StandardModel:Vts   (default = 0.04161; minimum = 0.039; maximum = 0.043)
    The V_ts CKM matrix element.

    parm  StandardModel:Vtb   (default = 0.9991; minimum = 0.99907; maximum = 0.9992)
    The V_tb CKM matrix element.

    The CoupSM class

    The Pythia class contains a public instance coupSM of the CoupSM class. This class contains one instance each of the AlphaStrong and AlphaEM classes, and additionally stores the weak couplings and the quark mixing matrix mentioned above. This class is used especially in the calculation of cross sections and resonance widths, but could also be used elsewhere. Specifically, as already mentioned, there are separate AlphaStrong and AlphaEM instances for timelike and spacelike showers and for multiparton interactions, while weak couplings and the quark mixing matrix are only stored here. With the exception of the first two methods below, which are for internal use, the subsequent ones could also be used externally.

    CoupSM::CoupSM()  
    the constructor does nothing. Internal.

    void CoupSM::init(Settings& settings, Rndm* rndmPtr)  
    this is where the AlphaStrong and AlphaEM instances are initialized, and weak couplings and the quark mixing matrix are read in and set. This is based on the values stored on this page and among the Couplings and Scales. Internal.

    double CoupSM::alphaS(double scale2)  
    the alpha_strong value at the quadratic scale scale2.

    double CoupSM::alphaS1Ord(double scale2)  
    a first-order overestimate of the full second-order alpha_strong value at the quadratic scale scale2.

    double CoupSM::alphaS2OrdCorr(double scale2)  
    a multiplicative correction factor, below unity, that brings the first-order overestimate above into agreement with the full second-order alpha_strong value at the quadratic scale scale2.

    double CoupSM::Lambda3()  
    double CoupSM::Lambda4()  
    double CoupSM::Lambda5()  
    the three-, four-, and five-flavour Lambda scale.

    double CoupSM::alphaEM(double scale2)  
    the alpha_em value at the quadratic scale scale2.

    double CoupSM::sin2thetaW()  
    double CoupSM::cos2thetaW()  
    the sine-squared and cosine-squared of the weak mixing angle, as used in the gauge-boson sector.

    double CoupSM::sin2thetaWbar()  
    the sine-squared of the weak mixing angle, as used to derive the vector couplings of fermions to the Z^0.

    double CoupSM::GF()  
    the Fermi constant of weak decays, in GeV^-2.

    double CoupSM::ef(int idAbs)  
    the electrical charge of a fermion, by the absolute sign of the PDF code, i.e. idAbs must be in the range between 1 and 18.

    double CoupSM::vf(int idAbs)  
    double CoupSM::af(int idAbs)  
    the vector and axial charges of a fermion, by the absolute sign of the PDF code (a_f = +-1, v_f = a_f - 4. * sin2thetaWbar * e_f).

    double CoupSM::t3f(int idAbs)  
    double CoupSM::lf(int idAbs)  
    double CoupSM::rf(int idAbs)  
    the weak isospin, left- and righthanded charges of a fermion, by the absolute sign of the PDF code (t^3_f = a_f/2, l_f = (v_f + a_f)/2, r_f = (v_f - a_f)/2; you may find other conventions in the literature that differ by a factor of 2).

    double CoupSM::ef2(int idAbs)  
    double CoupSM::vf2(int idAbs)  
    double CoupSM::af2(int idAbs)  
    double CoupSM::efvf(int idAbs)  
    double CoupSM::vf2af2(int idAbs)  
    common quadratic combinations of the above couplings: e_f^2, v_f^2, a_f^2, e_f * v_f, v_f^2 + a_f^2.

    double CoupSM::VCKMgen(int genU, int genD)  
    double CoupSM::V2CKMgen(int genU, int genD)  
    the CKM mixing element,or the square of it, for up-type generation index genU (1 = u, 2 = c, 3 = t, 4 = t') and down-type generation index genD (1 = d, 2 = s, 3 = b, 4 = b').

    double CoupSM::VCKMid(int id1, int id2)  
    double CoupSM::V2CKMid(int id1, int id2)  
    the CKM mixing element,or the square of it, for flavours id1 and id2, both in the range from -18 to +18. The sign is here not checked (so it can be used both for u + dbar -> W+ and u -> d + W+, say), but impossible flavour combinations evaluate to zero. The neutrino sector is numbered by flavor eigenstates, so there is no mixing in the lepton-neutrino system.

    double CoupSM::V2CKMsum(int id)  
    the sum of squared CKM mixing element that a given flavour can couple to, excluding the top quark and fourth generation. Is close to unity for the first two generations. Returns unity for the lepton-neutrino sector.

    int CoupSM::V2CKMpick(int id)  
    picks a random CKM partner quark or lepton (with the same sign as id) according to the respective squared elements, again excluding the top quark and fourth generation from the list of possibilities. Unambiguous choice for the lepton-neutrino sector. pythia8-8.1.80.orig/htmldoc/ProgramFlow.html0000644000175000017500000014563112217615311017121 0ustar sunsun Program Flow

    Program Flow

    Recall that, to first order, the event generation process can be subdivided into three stages:
    1. Initializaion.
    2. The event loop.
    3. Finishing.
    This is reflected in how the top-level Pythia class should be used in the user-supplied main program, further outlined in the following. Since the nature of the run is defined at the initialization stage, this is where most of the PYTHIA user code has to be written. So as not to confuse the reader unduly, the description of initialization options has been subdivided into what would normally be used and what is intended for more special applications.

    At the bottom of this webpage is a complete survey of all public Pythia methods and data members, in a more formal style than the task-oriented descriptions found in the preceding sections. This offers complementary information.

    Initialization - normal usage

    1. Already at the top of the main program file, you need to include the proper header file
          #include "Pythia8/Pythia.h"
      
      To simplify typing, it also makes sense to declare
          using namespace Pythia8; 
      
    2. The first step is to create a generator object, e.g. with
           Pythia pythia;
      
      It is this object that we will use from now on. Normally a run will only contain one Pythia object. (But you can use several Pythia objects, which then will be independent of each other.)
      By default all output from Pythia will be on the cout stream, but the list methods below do allow output to alternative streams or files.
    3. You next want to set up the character of the run. The pages under the "Setup Run Tasks" heading in the index describe all the options available (with some very few exceptions, found on the other pages). The default values and your modifications are stored in two databases, one for generic settings and one for particle data. Both of these are initialized with their default values by the Pythia constructor. The default values can then be changed, primarily by one of the two ways below, or by a combination of them.

      a) You can use the

          pythia.readString(string);
      
      method repeatedly to do a change of a property at a time. The information in the string is case-insensitive, but upper- and lowercase can be combined for clarity. The rules are that
      (i) if the first nonblank character of the string is a letter it is assumed to contain a setting, and is sent on to pythia.settings.readString(string);
      (ii) if instead the string begins with a digit it is assumed to contain particle data updates, and so sent on to pythia.particleData.readString(string);
      (iii) if none of the above, the string is assumed to be a comment, i.e. nothing will be done.
      In the former two cases, a warning is issued whenever a string cannot be recognized (maybe because of a spelling mistake).
      Some examples would be
          pythia.readString("TimeShower:pTmin = 1.0");
          pythia.readString("111:mayDecay = false");
      
      The readString(string) method is intended primarily for a few changes. It can also be useful if you want to construct a parser for input files that contain commands both to PYTHIA and to other libraries.

      b) You can read in a file containing a list of those variables you want to see changed, with a

          pythia.readFile(fileName);
      
      Each line in this file with be processes by the readString(string) method introduced above. You can thus freely mix comment lines and lines handed on to Settings or to ParticleData.
      This approach is better suited for more extensive changes than a direct usage of readString(string), and can also avoid having to recompile and relink your main program between runs.
      It is also possible to read input from an istream, by default cin, rather than from a file. This may be convenient if information is generated on-the-fly, within the same run.

      Changes are made sequentially in the order the commands are encountered during execution, meaning that if a parameter is changed several times it is the last one that counts. The two special Tune:ee and Tune:pp modes are expanded to change several settings in one go, but these obey the same ordering rules.

    4. Next comes the initialization stage, where all remaining details of the generation are to be specified. There is one standard method to use for this

      pythia.init();
      with no arguments will read all relevant information from the Settings and ParticleData databases. Specifically the setup of incoming beams and energies is governed by the the beam parameters from the Beams group of variables. If you don't change any of those you will default to proton-proton collisions at 14 TeV, i.e. the nominal LHC values.

      A few alternative forms are available, where the arguments of the init(...) call can be used to set the beam parameters. These alternatives are now deprecated, and will be removed for PYTHIA 8.2.

      a) pythia.init( idA, idB, eCM);
      lets you specify the identities and the CM energy of the two incoming beam particles, with A (B) assumed moving in the +z (-z) direction.

      b) pythia.init( idA, idB, eA, eB);
      is similar, but the two beam energies can be different, so the collisions do not occur in the CM frame. If one of the beam energies is below the particle mass you obtain a fixed-target topology.

      c) pythia.init( idA, idB, pxA, pyA, pzA, pxB, pyB, pzB);
      is similar, but here you provide the three-momenta (p_x, p_y, p_z) of the two incoming particles, to allow for arbitrary beam directions.

      d) pythia.init(fileName);
      assumes a file in the Les Houches Event File format is provided.

      e) pythia.init( LHAup*);
      assumes Les Houches Accord initialization and event information is available in an LHAup class object, and that a pointer to this object is handed in.

    5. If you want to have a list of the generator and particle data used, either only what has been changed or everything, you can use
          pythia.settings.listChanged();
          pythia.settings.listAll();
          pythia.particleData.listChanged(); 
          pythia.particleData.listAll(); 
      

    The event loop

    1. Inside the event generation loop you generate the next event using the next() method,
          pythia.next();
      
      This method takes no arguments; everything has already been specified. It does return a bool value, however, false when the generation failed. This can be a "programmed death" when the supply of input parton-level configurations on file is exhausted. It can alternatively signal a failure of Pythia to generate an event, or unphysical features in the event record at the end of the generation step. It makes sense to allow a few false values before a run is aborted, so long as the related faulty events are skipped.
    2. The generated event is now stored in the event object, of type Event, which is a public member of pythia. You therefore have access to all the tools described on the pages under the "Study Output" header in the index. For instance, an event can be listed with pythia.event.list(), the identity of the i'th particle is given by pythia.event[i].id(), and so on.
      The hard process - roughly the information normally stored in the Les Houches Accord event record - is available as a second object, process, also of type Event.
      A third useful public object is info, which offers a set of one-of-a kind pieces of information about the most recent event.

    Finishing

    1. At the end of the generation process, you can call
          pythia.stat(); 
      
      to get some run statistics, on cross sections and the number of errors and warnings encountered. The alternative pythia.statistics(...); is equivalent but deprecated.

    Advanced usage, mainly for initialization

    A) Necessary data are automatically loaded when you use the default PYTHIA installation directory structure and run the main programs in the examples subdirectory. However, in the general case, you must provide the path of the xmldoc directory, where default settings and particle data are found. This can be done in two ways.
    1. You can set the environment variable PYTHIA8DATA to contain the location of the xmldoc directory. In the csh and tcsh shells this could e.g. be
           setenv PYTHIA8DATA /home/myname/pythia81xx/xmldoc
      
      while in other shells it could be
           export PYTHIA8DATA=/home/myname/pythia81xx/xmldoc
      
      where xx is the subversion number.
      Recall that environment variables set locally are only defined in the current instance of the shell. The above lines should go into your .cshrc and .bashrc files, respectively, if you want a more permanent assignment.
    2. You can provide the path as argument to the Pythia constructor, e.g.
           Pythia pythia("/home/myname/pythia81xx/xmldoc");
      
    where again xx is the subversion number.
    When PYTHIA8DATA is set it takes precedence, else the path in the constructor is used, else one defaults to the ../xmldoc directory.

    B) You can override the default behaviour of PYTHIA not only by the settings and particle data, but also by replacing some of the PYTHIA standard routines by ones of your own. Of course, this is only possible if your routines fit into the general PYTHIA framework. Therefore they must be coded according to the the rules relevant in each case, as a derived class of a PYTHIA base class, and a pointer to such an object must be handed in by one of the methods below. These calls must be made before the pythia.init(...) call.

    1. If you are not satisfied with the list of parton density functions that are implemented internally or available via the LHAPDF interface (see the PDF Selection page), you can supply your own by a call to the setPDFPtr(...) method
            pythia.setPDFptr( pdfAPtr, pdfBPtr); 
      
      where pdfAPtr and pdfBPtr are pointers to two Pythia PDF objects. Note that pdfAPtr and pdfBPtr cannot point to the same object; even if the PDF set is the same, two copies are needed to keep track of two separate sets of x and density values.
      If you further wish to use separate PDF's for the hard process of an event than the ones being used for everything else, the extended form
            pythia.setPDFptr( pdfAPtr, pdfBPtr, pdfHardAPtr, pdfHardBPtr); 
      
      allows you to specify those separately, and then the first two sets would only be used for the showers and for multiparton interactions.
    2. If you want to link to an external generator that feeds in events in the LHA format, you can call the setLHAupPtr(...) method
            pythia.setLHAupPtr( lhaUpPtr);
      
      where the lhaUpPtr derives from the LHAup base class.
    3. If you want to perform some particle decays with an external generator, you can call the setDecayPtr(...) method
            pythia.setDecayPtr( decayHandlePtr, particles);
      
      where the decayHandlePtr derives from the DecayHandler base class and particles is a vector of particle codes to be handled.
    4. If you want to use an external random number generator, you can call the setRndmEnginePtr(...) method
            pythia.setRndmEnginePtr( rndmEnginePtr); 
      
      where rndmEnginePtr derives from the RndmEngine base class. The Pythia default random number generator is perfectly good, so this is only intended for consistency in bigger frameworks.
    5. If you want to interrupt the evolution at various stages, to interrogate the event and possibly veto it, or you want to reweight the cross section, you can use
            pythia.setUserHooksPtr( userHooksPtr); 
      
      where userHooksPtr derives from the UserHooks base class.
    6. If you want to use your own merging scale definition for matrix element + parton shower merging, you can call
            pythia.setMergingHooksPtr( mergingHooksPtr); 
      
      where mergingHooksPtr derives from the MergingHooks base class.
    7. If you want to use your own parametrization of beam momentum spread and interaction vertex, rather than the provided simple Gaussian parametrization (off by default), you can call
            pythia.setBeamShapePtr( beamShapePtr); 
      
      where beamShapePtr derives from the BeamShape base class.
    8. If you want to implement a cross section of your own, but still make use of the built-in phase space selection machinery, you can use
            pythia.setSigmaPtr( sigmaPtr);
      
      where sigmaPtr of type SigmaProcess* is an instance of a class derived from one of the Sigma1Process, Sigma2Process and Sigma3Process base classes in their turn derived from SigmaProcess. This call can be used repeatedly to hand in several different processes.
    9. If your cross section contains the production of a new resonance with known analytical expression for all the relevant partial widths, you can make this resonance available to the program with
            pythia.setResonancePtr( resonancePtr);
      
      where resonancePtr of type ResonanceWidths* is an instance of a class derived from the ResonanceWidths base class. In addition you need to add the particle to the normal particle and decay database. This procedure can be used repeatedly to hand in several different resonances.
    10. If you are a real expert and want to replace the PYTHIA initial- and final-state showers, you can use
            pythia.setShowerPtr( timesDecPtr, timesPtr, spacePtr);
      
      where timesDecPtr and timesPtr derive from the TimeShower base class, and spacePtr from SpaceShower.

    C) Some comments on collecting several tasks in the same run.

    1. PYTHIA has not been written for threadsafe execution on multicore processors. If you want to use all cores, the most efficient way presumably is to start correspondingly many jobs, with different random number seeds, and add the statistics at the end. However, note that several instances can be set up in the same main program, since instances are completely independent of each other, so each instance could be run inside a separate thread.
    2. In some cases it is convenient to use more than one Pythia object. The key example would be the simultaneous generation of signal and pileup events, see main19.cc. The two objects are then set up and initialized separately, and generate events completely independently of each other. It is only afterwards that the event records are combined into one single super-event per beam crossing.
    3. When time is not an issue, it may be that you want to perform several separate subruns sequentially inside a run, e.g. to combine results for several kinematical regions or to compare results for some different tunes of the underlying event. One way to go is to create (and destroy) one pythia object for each subrun, in which case they are completely separate. You can also use the same pythia object, only doing a new init(...) call for each subrun. In that case, the settings and particle databases remain as they were in the previous subrun, only affected by the specific changes you introduced in the meantime. You can put those changes in the main program, with pythia.readString(string), using your own logic to decide which ones to execute in which subrun. A corresponding possibility exists with pythia.readFile(fileName, subrun) (or an istream instead of a fileName), which as second argument can take a non-negative subrun number. Then only those sections of the file before any Main:subrun = ... line or with matching subrun number will be read. That is, the file could have a structure like
          ( lines always read, i.e. "default values" always (re)set )
          Main:subrun = 1
          ( lines only read with readFile(fileName, 1) )
          Main:subrun = 2
          ( lines only read with readFile(fileName, 2) )
      
      Both of these possibilities are illustrated in main08.cc.
    4. When working with Les Houches Event Files, it may well be that your intended input event sample is spread over several files, that you all want to turn into complete events in one and the same run. There is no problem with looping over several subruns, where each new subrun is initialized with a new file, with name set in Beams:LHEF. However, in that case you will do a complete re-initialization each time around. If you want to avoid this, note that the flag Beams:newLHEFsameInit = true can be set for the second and subsequent subruns. Then the new file will be simulated with the same initialization data as already set in a previous pythia.init() call. The burden rests on you to ensure that this is indeed correct, e.g. that the two event samples have not been generated for different beam energies. Also note that cross sections for processes will be based on the information in the first-read file, when the full initialization is performed.

    The Pythia Class

    Here follows the complete survey of all public Pythia methods and data members.

    Constructor and destructor

    Pythia::Pythia(string xmlDir = "../xmldoc",bool printBanner = true)  
    creates an instance of the Pythia event generators, and sets initial default values, notably for all settings and particle data. You may use several Pythia instances in the same run; only when you want to access external static libraries could this cause problems. (This includes in particular Fortran libraries such as LHAPDF.)
    argument xmlDir (default = ../xmldoc) : allows you to choose from which directory the default settings and particle data values are read in. If the PYTHIA8DATA environment variable has been set it takes precedence. Else this optional argument allows you to choose another directory location than the default one. Note that it is only the directory location you can change, its contents must be the ones of the xmldoc directory in the standard distribution.
    argument printBanner (default = true) : can be set false to stop the program from printing a banner. The banner contains useful information, so this option is only intended for runs with multiple Pythia instances, where output needs to be restricted.

    Pythia::~Pythia  
    the destructor deletes the objects created by the constructor.

    Set up run

    bool Pythia::readString(string line, bool warn = true)  
    reads in a single string, that is interpreted as an instruction to modify the value of a setting or particle data, as already described above.
    argument line : the string to be interpreted as an instruction.
    argument warn (default = true) : write a warning message or not whenever the instruction does not make sense, e.g. if the variable does not exist in the databases.
    Note: the method returns false if it fails to make sense out of the string.

    bool Pythia::readFile(string fileName, bool warn = true, int subrun = SUBRUNDEFAULT)  
    bool Pythia::readFile(string fileName, int subrun = SUBRUNDEFAULT)  
    bool Pythia::readFile(istream& inStream = cin, bool warn = true, int subrun = SUBRUNDEFAULT)  
    bool Pythia::readFile(istream& inStream = cin, int subrun = SUBRUNDEFAULT)  
    reads in a whole file, where each line is interpreted as an instruction to modify the value of a setting or particle data, cf. the above readString method. All four forms of the readFile command share code for actually reading a file.
    argument fileName : the file from which instructions are read.
    argument inStream : an istream from which instructions are read.
    argument warn (default = true) : write a warning message or not whenever the instruction does not make sense, e.g. if the variable does not exist in the databases. In the command forms where warn is omitted it is true.
    argument subrun : allows you have several optional sets of commands within the same file. Only those sections of the file before any Main:subrun = ... line or following such a line with matching subrun number will be read. The subrun number should not be negative; negative codes like SUBRUNDEFAULT corresponds to no specific subrun.
    Note: the method returns false if it fails to make sense out of any one line.

    bool Pythia::setPDFPtr( PDF* pdfAPtr, PDF* pdfBPtr, PDF* pdfHardAPtr = 0, PDF* pdfHardBPtr = 0)  
    offers the possibility to link in external PDF sets for usage inside the program. The rules for constructing your own class from the PDF base class are described here.
    argument pdfAPtr, pdfBPtr : pointers to two PDF-derived objects, one for each of the incoming beams. The two objects have to be instantiated by you in your program. Even if the two beam particles are the same (protons, say) two separate instances are required, since current information is cached in the objects. If both arguments are zero then any previous linkage to external PDF's is disconnected, see further Note 2 below.
    argument pdfHardAPtr, pdfHardBPtr (default = 0) : pointers to two further PDF-derived objects, one for each of the incoming beams. Normally only the first two arguments above would be used, and then the same PDF sets would be invoked everywhere. If you provide these two further pointers then two different sets of PDF's are used. This second set is then exclusively for the generation of the hard process from the process matrix elements library. The first set above is for everything else, notably parton showers and multiparton interactions.
    Note 1: The method returns false if the input is obviously incorrect, e.g. if two (nonzero) pointers agree.
    Note 2: If you want to combine several subruns you can call setPDFPtr with new arguments before each Pythia::init(...) call. To revert from external PDF's to the normal internal PDF selection you must call setPDFPtr(0, 0) before Pythia::init(...).

    bool Pythia::setLHAupPtr( LHAup* lhaUpPtrIn)  
    offers linkage to an external generator that feeds in events in the LHA format, see Les Houches Accord, assuming that Beams:frameType = 5 has been set.
    argument lhaUpPtrIn : pointer to a LHAup-derived object.
    Note: The method currently always returns true.

    bool Pythia::setDecayPtr( DecayHandler* decayHandlePtr, vector<int> handledParticles)  
    offers the possibility to link to an external program that can do some of the particle decays, instead of using the internal decay machinery. With particles we here mean the normal hadrons and leptons, not top quarks, electroweak bosons or new particles in BSM scenarios. The rules for constructing your own class from the DecayHandler base class are described here. Note that you can only provide one external object, but this object in its turn could very well hand on different particles to separate decay libraries.
    argument decayHandlePtr : pointer to a DecayHandler-derived object. This object must be instantiated by you in your program.
    argument handledParticles : vector with the PDG identity codes of the particles that should be handled by the external decay package. You should only give the particle (positive) codes; the respective antiparticle is always included as well.
    Note: The method currently always returns true.

    bool Pythia::setRndmEnginePtr( RndmEngine* rndmEnginePtr)  
    offers the possibility to link to an external random number generator. The rules for constructing your own class from the RndmEngine base class are described here.
    argument rndmEnginePtr : pointer to a RndmEngine-derived object. This object must be instantiated by you in your program.
    Note: The method returns true if the pointer is different from 0.

    bool Pythia::setUserHooksPtr( UserHooks* userHooksPtr)  
    offers the possibility to interact with the generation process at a few different specified points, e.g. to reject undesirable events at an early stage to save computer time. The rules for constructing your own class from the UserHooks base class are described here. You can only hand in one such pointer, but this may be to a class that implements several of the different allowed possibilities.
    argument userHooksPtr : pointer to a userHooks-derived object. This object must be instantiated by you in your program.
    Note: The method currently always returns true.

    bool Pythia::setBeamShapePtr( BeamShape* beamShapePtr)  
    offers the possibility to provide your own shape of the momentum and space-time spread of the incoming beams. The rules for constructing your own class from the BeamShape base class are described here.
    argument BeamShapePtr : pointer to a BeamShape-derived object. This object must be instantiated by you in your program.
    Note: The method currently always returns true.

    bool Pythia::setSigmaPtr( SigmaProcess* sigmaPtr)  
    offers the possibility to link your own implementation of a process and its cross section, to make it a part of the normal process generation machinery, without having to recompile the Pythia library itself. The rules for constructing your own class from the SigmaProcess base class are described here. You may call this routine repeatedly, to add as many new processes as you wish.
    argument sigmaPtr : pointer to a SigmaProcess-derived object. This object must be instantiated by you in your program.
    Note: The method currently always returns true.

    bool Pythia::setResonancePtr( ResonanceWidths* resonancePtr)  
    offers the possibility to link your own implementation of the calculation of partial resonance widths, to make it a part of the normal process generation machinery, without having to recompile the Pythia library itself. This allows the decay of new resonances to be handled internally, when combined with new particle data. Note that the decay of normal hadrons cannot be modeled here; this is for New Physics resonances. The rules for constructing your own class from the ResonanceWidths base class are described here. You may call this routine repeatedly, to add as many new resonances as you wish.
    argument resonancePtr : pointer to a ResonanceWidths-derived object. This object must be instantiated by you in your program.
    Note: The method currently always returns true.

    bool Pythia::setShowerPtr( TimeShower* timesDecPtr, TimeShower* timesPtr = 0, SpaceShower* spacePtr = 0)  
    offers the possibility to link your own parton shower routines as replacements for the default ones. This is much more complicated since the showers are so central and are so interlinked with other parts of the program. Therefore it is also possible to do the replacement in stages, from the more independent to the more intertwined. The rules for constructing your own classes from the TimeShower and SpaceShowerbase classes are described here. These objects must be instantiated by you in your program.
    argument timesDecPtr : pointer to a TimeShower-derived object for doing timelike shower evolution in resonance decays, e.g. of a Z^0. This is decoupled from beam remnants and parton distributions, and is therefore the simplest kind of shower to write. If you provide a value 0 then the internal shower routine will be used.
    argument timesPtr (default = 0) : pointer to a TimeShower-derived object for doing all other timelike shower evolution, which is normally interleaved with multiparton interactions and spacelike showers, introducing both further physics and further technical issues. If you retain the default value 0 then the internal shower routine will be used. You are allowed to use the same pointer as above for the timesDecPtr if the same shower can fulfill both tasks.
    argument spacePtr (default = 0) : pointer to a SpaceShower-derived object for doing all spacelike shower evolution, which is normally interleaved with multiparton interactions and timelike showers. If you retain the default value 0 then the internal shower routine will be used.
    Note: The method currently always returns true.

    Initialize

    At the initialization stage all the information provided above is processed, and the stage is set up for the subsequent generation of events. Currently several alternative forms of the init method are available for this stage, but only the first one is recommended.

    bool Pythia::init()  
    initialize for collisions, in any of the five separate possibilities below. In this option the beams are not specified by input arguments, but instead by the settings in the Beam Parameters section. This allows the beams to be specified in the same file as other run instructions. The default settings give pp collisions at 14 TeV.
    Note: The method returns false if the initialization fails. It is then not possible to generate any events.

    bool Pythia::init( int idA, int idB, double eCM)  
    initialize for collisions in the center-of-mass frame, with the beams moving in the +-z directions.
    argument idA, idB : particle identity code for the two incoming beams.
    argument eCM : the CM energy of the collisions.
    Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

    bool Pythia::init( int idA, int idB, double eA, double eB)  
    initialize for collisions with back-to-back beams, moving in the +-z directions, but with different energies.
    argument idA, idB : particle identity code for the two incoming beams.
    argument eA, eB : the energies of the two beams. If an energy is set to be below the mass of the respective beam particle that particle is taken to be at rest. This offers a simple possibility to simulate fixed-target collisions.
    Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

    bool Pythia::init( int idA, int idB, double pxA, double pyA, double pzA, double pxB, double pyB, double pzB)  
    initialize for collisions with arbitrary beam directions.
    argument idA, idB : particle identity code for the two incoming beams.
    argument pxA, pyA, pzA : the three-momentum vector (p_x, p_y, p_z) of the first incoming beam.
    argument pxB, pyB, pzB : the three-momentum vector (p_x, p_y, p_z) of the second incoming beam.
    Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

    bool Pythia::init( string LesHouchesEventFile, bool skipInit = false)  
    initialize for hard-process collisions fed in from an external file with events, written according to the Les Houches Event File standard.
    argument LesHouchesEventFile : the file name (including path, where required) where the events are stored, including relevant information on beam identities and energies.
    argument skipInit (default = false) : By default this method does a complete reinitialization of the generation process. If you set this argument to true then no reinitialization will occur, only the pointer to the event file is updated. This may come in handy if the full event sample is split across several files generated under the same conditions (except random numbers, of course). You then do the first initialization with the default, and all subsequent ones with true. Note that things may go wrong if the files are not created under the same conditions.
    Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

    bool Pythia::init( LHAup* lhaUpPtr)  
    initialize for hard-process collisions fed in from an external source of events, consistent with the Les Houches Accord standard. The rules for constructing your own class from the LHAup base class are described here. This class is also required to provide the beam parameters.
    argument lhaUpPtr : pointer to a LHAup-derived object. This object must be instantiated by you in your program.
    Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

    Generate events

    The next() method is the main one to generate events. In this section we also put a few other specialized methods that may be useful in some circumstances.

    bool Pythia::next()  
    generate the next event. No input parameters are required; all instructions have already been set up in the initialization stage.
    Note: The method returns false if the event generation fails. The event record is then not consistent and should not be studied. When reading in hard collisions from a Les Houches Event File the problem may be that the end of the file has been reached. This can be checked with the Info::atEndOfFile() method.

    int Pythia::forceTimeShower( int iBeg, int iEnd, double pTmax, int nBranchMax = 0)  
    perform a final-state shower evolution on partons in the event event record. This could be used for externally provided simple events, or even parts of events, for which a complete generation is not foreseen. Since the mother source of the parton system is not known, one cannot expect as good accuracy as in a normal generation. When two different timelike shower instances are set up, it is the one used for showering in resonance decays that is used here. The forceTimeShower method can be used in conjunction with the forceHadronLevel one below. Further comments are found here.
    argument iBeg, iEnd : the first and last entry of the event record to be affected by the call.
    argument pTmax : the maximum pT scale of emissions. Additionally, as always, the scale variable of each parton sets the maximum pT scale of branchings of this parton. Recall that this scale defaults to 0 if not set, so that no radiation can occur.
    argument nBranchMax (default = 0) : when positive, it sets the maximum number of branchings that are allowed to occur in the shower, i.e. the shower may stop evolving before reaching the lower cutoff. The argument has no effect when zero or negative, i.e. then the shower will continue to the lower cutoff.
    Note: The method returns the number of branchings that has been generated.

    bool Pythia::forceHadronLevel(bool findJunctions = true)  
    hadronize the existing event record, i.e. perform string fragmentation and particle decays. There are two main applications. Firstly, you can use the same parton-level content as a basis for repeated hadronization attempts, in schemes intended to save computer time. Secondly, you may have an external program that can simulate the full partonic level of the event - hard process, parton showers, multiparton interactions, beam remnants, colour flow, and so on - but not hadronization. Further details are found here.
    argument findJunctions (default = true) : normally this routine will search through the event record and try to figure out if any colour junctions are present. If so, the colour topology of such junctions must be sorted out. In tricky cases this might fail, and then hadronization will not work. A user who is aware of this and knows the intended colour flow can set up the junction information (if any) in the event record, and then call forceHadronLevel(false) so as not to have this information overwritten. (If the event record contains no unhadronized partons then no junction search will be performed in any case.)
    Note: The method returns false if the hadronization fails. The event record is then not consistent and should not be studied.

    bool Pythia::moreDecays()  
    perform decays of all particles in the event record that have not been decayed but should have been done so. This can be used e.g. for repeated decay attempts, in schemes intended to save computer time. Further details are found here.
    Note: The method returns false if the decays fail. The event record is then not consistent and should not be studied.

    bool Pythia::forceRHadronDecays()  
    perform decays of R-hadrons that were previously considered stable. This could be if an R-hadron is sufficiently long-lived that it may interact in the detector between production and decay, so that its four-momentum is changed. Further details are found here.
    Note: The method returns false if the decays fail. The event record is then not consistent and should not be studied.

    void Pythia::LHAeventList(ostream& os = cout)  
    list the Les Houches Accord information on the current event, see LHAup::listEvent(...). (Other listings are available via the class members below, so this listing is a special case that would not fit elsewhere.)
    argument os (default = cout) : output stream where the listing occurs.

    bool Pythia::LHAeventSkip(int nSkip)  
    skip ahead a number of events in the Les Houches generation sequence, without doing anything further with them, see LHAup::skipEvent(nSkip). Mainly intended for debug purposes, e.g. when an event at a known location in a Les Houches Event File is causing problems.
    argument nSkip : number of events to skip.
    Note: The method returns false if the operation fails, specifically if the end of a LHEF has been reached, cf. next() above.

    Finalize

    There is no required finalization step; you can stop generating events when and how you want. It is still recommended that you make it a routine to call the following method at the end. A second method provides a deprecated alternative.

    void Pythia::stat()  
    list statistics on the event generation, specifically total and partial cross sections and the number of different errors. For more details see here and for available options here.

    void Pythia::statistics(bool all = false, bool reset = false)  
    list statistics on the event generation, specifically total and partial cross sections and the number of different errors. For more details see here.
    argument all (default = false) : if true also statistics on multiparton interactions is shown, by default not.
    argument reset (default = false) : if true then all counters, e.g on events generated and errors experienced, are reset to zero whenever the routine is called. The default instead is that all stored statistics information is unaffected by the call. Counters are automatically reset in each new Pythia::init(...) call, however, so the only time the reset option makes a difference is if statistics(...) is called several times in a (sub)run.
    Note: Deprecated.

    Interrogate settings

    Normally settings are used in the setup and initialization stages to determine the character of a run, e.g. read from a file with the above-described Pythia::readFile(...) method. There is no strict need for a user to interact with the Settings database in any other way. However, as an option, some settings variables have been left free for the user to set in such a file, and then use in the main program to directly affect the performance of that program, see here. A typical example would be the number of events to generate. For such applications the following shortcuts to some Settings methods may be convenient.

    bool Pythia::flag(string key)  
    read in a boolean variable from the Settings database.
    argument key : the name of the variable to be read.

    int Pythia::mode(string key)  
    read in an integer variable from the Settings database.
    argument key : the name of the variable to be read.

    double Pythia::parm(string key)  
    read in a double-precision variable from the Settings database.
    argument key : the name of the variable to be read.

    string Pythia::word(string key)  
    read in a string variable from the Settings database.
    argument key : the name of the variable to be read.

    Get a PDF set

    Pythia contains an number of parton density sets internally, plus an interface to LHAPDF. With the method below, this machinery is also made available for external usage.

    PDF* getPDFPtr(int id, int sequence = 1)  
    get a pointer to a PDF object. Which PDF is returned depends on the PDF Selection settings.
    argument id : the identity code of the incoming particle.
    argument sequence : should normally be 1, but 2 can be used for protons to let the PDF selection be determined by the special settings for hard processes (PDF:useHard etc.).

    Data members

    The Pythia class contains a few public data members, several of which play a central role. We list them here, with links to the places where they are further described.

    Event Pythia::process  
    the hard-process event record, see here for further details.

    Event Pythia::event  
    the complete event record, see here for further details.

    Info Pythia::info  
    further information on the event-generation process, see here for further details.

    Settings Pythia::settings  
    the settings database, see here for further details.

    ParticleData Pythia::particleData  
    the particle properties and decay tables database, see here for further details.

    Rndm Pythia::rndm  
    the random number generator, see here and here for further details.

    CoupSM Pythia::coupSM  
    Standard Model couplings and mixing matrices, see here for further details.

    SusyLesHouches Pythia::slha  
    parameters and particle data in the context of supersymmetric models, see here for further details.

    PartonSystems Pythia::partonSystems  
    a grouping of the partons in the event record by subsystem, see here for further details. pythia8-8.1.80.orig/htmldoc/SpacelikeShowers.html0000644000175000017500000006066212217615311020135 0ustar sunsun Spacelike Showers

    Spacelike Showers

    The PYTHIA algorithm for spacelike initial-state showers is based on the article [Sjo05], where a transverse-momentum-ordered backwards evolution scheme is introduced, with the extension to fully interleaved evolution covered in [Cor10a]. This algorithm is a further development of the virtuality-ordered one presented in [Sj085], with matching to first-order matrix element for Z^0, W^+- and Higgs (in the m_t -> infinity limit) production as introduced in [Miu99].

    The normal user is not expected to call SpaceShower directly, but only have it called from Pythia, via PartonLevel. Some of the parameters below, in particular SpaceShower:alphaSvalue, would be of interest for a tuning exercise, however.

    Main variables

    The maximum pT to be allowed in the shower evolution is related to the nature of the hard process itself. It involves a delicate balance between not double-counting and not leaving any gaps in the coverage. The best procedure may depend on information only the user has: how the events were generated and mixed (e.g. with Les Houches Accord external input), and how they are intended to be used. Therefore a few options are available, with a sensible default behaviour.

    mode  SpaceShower:pTmaxMatch   (default = 0; minimum = 0; maximum = 2)
    Way in which the maximum shower evolution scale is set to match the scale of the hard process itself.
    option 0 : (i) if the final state of the hard process (not counting subsequent resonance decays) contains at least one quark (u, d, s, c ,b), gluon or photon then pT_max is chosen to be the factorization scale for internal processes and the scale value for Les Houches input; (ii) if not, emissions are allowed to go all the way up to the kinematical limit. The reasoning is that in the former set of processes the ISR emission of yet another quark, gluon or photon could lead to double-counting, while no such danger exists in the latter case.
    option 1 : always use the factorization scale for an internal process and the scale value for Les Houches input, i.e. the lower value. This should avoid double-counting, but may leave out some emissions that ought to have been simulated. (Also known as wimpy showers.)
    option 2 : always allow emissions up to the kinematical limit. This will simulate all possible event topologies, but may lead to double-counting. (Also known as power showers.)
    Note 1: Some processes contain matrix-element matching to the first emission; this is the case notably for single gamma^*/Z^0, W^+- and H^0 production. Then default and option 2 give the correct result, while option 1 should never be used.
    Note 2: as enumerated in the text, these options take effect both for internal and external processes. Whether a particular option makes sense depends on the context. For instance, if events for the same basic process to different orders are to be matched, then option 1 would be a reasonable first guess. But in more sophisticated descriptions option 2 could be combined with UserHooks vetoes on emissions that would lead to double-counting, using more flexible phase space boundaries. Option 0, finally, may be most realistic when only Born-level processes are involved, possibly in combination with a nonzero SpaceShower:pTdampMatch. The rules used for avoiding double-counting are not foolproof, however. As an example, for the t-channel process gamma gamma -> e^+ e^- its pT scale is the plausible upper shower limit, with only dampened emissions above it. But the initial state is not checked and, had only incoming quarks and gluons been taken into account, only the s-channel process q qbar -> gamma^*/Z^0 -> e^+ e^- would have been possible, where indeed the whole phase space should be populated. So this is erroneously used, giving too much emissions.
    Note 3: These options only apply to the hard interaction. If a "second hard" process is present, the two are analyzed and set separately for the default 0 option, while both are affected the same way for non-default options 1 and 2. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of each process itself.

    parm  SpaceShower:pTmaxFudge   (default = 1.0; minimum = 0.25; maximum = 2.0)
    In cases where the above pTmaxMatch rules would imply that pT_max = pT_factorization, pTmaxFudge introduces a multiplicative factor f such that instead pT_max = f * pT_factorization. Only applies to the hardest interaction in an event, and a "second hard" if there is such a one, cf. below. It is strongly suggested that f = 1, but variations around this default can be useful to test this assumption.

    parm  SpaceShower:pTmaxFudgeMPI   (default = 1.0; minimum = 0.25; maximum = 2.0)
    A multiplicative factor f such that pT_max = f * pT_factorization, as above, but here for the non-hardest interactions (when multiparton interactions are allowed).

    mode  SpaceShower:pTdampMatch   (default = 0; minimum = 0; maximum = 2)
    These options only take effect when a process is allowed to radiate up to the kinematical limit by the above pTmaxMatch choice, and no matrix-element corrections are available. Then, in many processes, the fall-off in pT will be too slow by one factor of pT^2. That is, while showers have an approximate dpT^2/pT^2 shape, often it should become more like dpT^2/pT^4 at pT values above the scale of the hard process. Whether this actually is the case depends on the particular process studied, e.g. if t-channel gluon exchange is likely to dominate. If so, the options below could provide a reasonable high-pT behaviour without requiring higher-order calculations.
    option 0 : emissions go up to the kinematical limit, with no special dampening.
    option 1 : emissions go up to the kinematical limit, but dampened by a factor k^2 Q^2_fac/(pT^2 + k^2 Q^2_fac), where Q_fac is the factorization scale and k is a multiplicative fudge factor stored in pTdampFudge below.
    option 2 : emissions go up to the kinematical limit, but dampened by a factor k^2 Q^2_ren/(pT^2 + k^2 Q^2_ren), where Q_ren is the renormalization scale and k is a multiplicative fudge factor stored in pTdampFudge below.
    Note: These options only apply to the hard interaction. Specifically, a "second hard" interaction would not be affected. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of the process itself.

    parm  SpaceShower:pTdampFudge   (default = 1.0; minimum = 0.25; maximum = 4.0)
    In cases 1 and 2 above, where a dampening is imposed at around the factorization or renormalization scale, respectively, this allows the pT scale of dampening of radiation by a half to be shifted by this factor relative to the default Q_fac or Q_ren. This number ought to be in the neighbourhood of unity, but variations away from this value could do better in some processes.

    The amount of QCD radiation in the shower is determined by

    parm  SpaceShower:alphaSvalue   (default = 0.137; minimum = 0.06; maximum = 0.25)
    The alpha_strong value at scale M_Z^2. Default value is picked equal to the one used in CTEQ 5L.

    The actual value is then regulated by the running to the scale pT^2, at which it is evaluated

    mode  SpaceShower:alphaSorder   (default = 1; minimum = 0; maximum = 2)
    Order at which alpha_strong runs,
    option 0 : zeroth order, i.e. alpha_strong is kept fixed.
    option 1 : first order, which is the normal value.
    option 2 : second order. Since other parts of the code do not go to second order there is no strong reason to use this option, but there is also nothing wrong with it.

    The CMW rescaling of Lambda_QCD (see the section on StandardModelParameters) can be applied to the alpha_strong values used for spacelike showers. Note that tunes using this option need lower values of alpha_strong(m_Z^2) than tunes that do not.

    flag  SpaceShower:alphaSuseCMW   (default = false)

    option false : Do not apply the CMW rescaling.
    option true : Apply the CMW rescaling, increasing Lambda_QCD for spacelike showers by a factor roughly 1.6.

    QED radiation is regulated by the alpha_electromagnetic value at the pT^2 scale of a branching.

    mode  SpaceShower:alphaEMorder   (default = 1; minimum = -1; maximum = 1)
    The running of alpha_em.
    option 1 : first-order running, constrained to agree with StandardModel:alphaEMmZ at the Z^0 mass.
    option 0 : zeroth order, i.e. alpha_em is kept fixed at its value at vanishing momentum transfer.
    option -1 : zeroth order, i.e. alpha_em is kept fixed, but at StandardModel:alphaEMmZ, i.e. its value at the Z^0 mass.

    The natural scale for couplings and PDFs is pT^2. To explore uncertainties it is possibly to vary around this value, however, in analogy with what can be done for hard processes.

    parm  SpaceShower:renormMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
    The default pT^2 renormalization scale is multiplied by this prefactor. For QCD this is equivalent to a change of Lambda^2 in the opposite direction, i.e. to a change of alpha_strong(M_Z^2) (except that flavour thresholds remain at fixed scales). Below, when pT^2 + pT_0^2 is used as scale, it is this whole expression that is multiplied by the prefactor.

    parm  SpaceShower:factorMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
    The default pT^2 factorization scale is multiplied by this prefactor.

    There are two complementary ways of regularizing the small-pT divergence, a sharp cutoff and a smooth dampening. These can be combined as desired but it makes sense to coordinate with how the same issue is handled in multiparton interactions.

    flag  SpaceShower:samePTasMPI   (default = off)
    Regularize the pT -> 0 divergence using the same sharp cutoff and smooth dampening parameters as used to describe multiparton interactions. That is, the MultipartonInteractions:pT0Ref, MultipartonInteractions:ecmRef, MultipartonInteractions:ecmPow and MultipartonInteractions:pTmin parameters are used to regularize all ISR QCD radiation, rather than the corresponding parameters below. This is a sensible physics ansatz, based on the assumption that colour screening effects influence both MPI and ISR in the same way. Photon radiation is regularized separately in either case.
    Warning: if a large pT0 is picked for multiparton interactions, such that the integrated interaction cross section is below the nondiffractive inelastic one, this pT0 will automatically be scaled down to cope. Information on such a rescaling does NOT propagate to SpaceShower, however.

    The actual pT0 parameter used at a given CM energy scale, ecmNow, is obtained as
    pT0 = pT0(ecmNow) = pT0Ref * (ecmNow / ecmRef)^ecmPow
    where pT0Ref, ecmRef and ecmPow are the three parameters below.

    parm  SpaceShower:pT0Ref   (default = 2.0; minimum = 0.5; maximum = 10.0)
    Regularization of the divergence of the QCD emission probability for pT -> 0 is obtained by a factor pT^2 / (pT0^2 + pT^2), and by using an alpha_s(pT0^2 + pT^2). An energy dependence of the pT0 choice is introduced by the next two parameters, so that pT0Ref is the pT0 value for the reference cm energy, pT0Ref = pT0(ecmRef).

    parm  SpaceShower:ecmRef   (default = 1800.0; minimum = 1.)
    The ecmRef reference energy scale introduced above.

    parm  SpaceShower:ecmPow   (default = 0.0; minimum = 0.; maximum = 0.5)
    The ecmPow energy rescaling pace introduced above.

    parm  SpaceShower:pTmin   (default = 0.2; minimum = 0.1; maximum = 10.0)
    Lower cutoff in pT, below which no further ISR branchings are allowed. Normally the pT0 above would be used to provide the main regularization of the branching rate for pT -> 0, in which case pTmin is used mainly for technical reasons. It is possible, however, to set pT0Ref = 0 and use pTmin to provide a step-function regularization, or to combine them in intermediate approaches. Currently pTmin is taken to be energy-independent.

    parm  SpaceShower:pTminChgQ   (default = 0.5; minimum = 0.01)
    Parton shower cut-off pT for photon coupling to a coloured particle.

    parm  SpaceShower:pTminChgL   (default = 0.0005; minimum = 0.0001)
    Parton shower cut-off mass for pure QED branchings. Assumed smaller than (or equal to) pTminChgQ.

    flag  SpaceShower:rapidityOrder   (default = off)
    Force emissions, after the first, to be ordered in rapidity, i.e. in terms of decreasing angles in a backwards-evolution sense. Could be used to probe sensitivity to unordered emissions. Only affects QCD emissions.

    Weak showers

    The description of W^+- and Z^0 gauge boson emission in ISR closely parallels that of such emissions in FSR. We therefore will not repeat the discussion here, but only report on the settings names, which again are similar to the FSR ones.

    flag  SpaceShower:weakShower   (default = off)
    Allow a weak shower, yes or no.

    mode  SpaceShower:weakShowerMode   (default = 0; minimum = 0; maximum = 2)
    Determine which branchings are allowed.
    option 0 : both W^+- and Z^0 branchings.
    option 1 : only W^+- branchings.
    option 2 : only Z^0 branchings.

    parm  SpaceShower:pTminWeak   (; minimum = 0.1; maximum = 2.0)
    Parton shower cut-off pT for weak branchings.

    parm  SpaceShower:weakShowerEnhancement   (default = 1.; minimum = 1.; maximum = 1000.)
    Enhancement factor for the weak shower. This is used to increase the statistics of weak shower emissions. Remember afterwards to correct for the additional weak emissions (i.e. divide the weak emissions by the same factor).

    flag  SpaceShower:singleWeakEmission   (default = off)
    This parameter allows to stop the weak shower after a single emission.
    on = only a single weak emission is allowed.
    off = unlimited number of weak emissions possible.

    parm  SpaceShower:extraScaleTerm   (default = 0.; minimum = 0.; maximum = 200.)
    The normal showers uses pT^2 as ordering variable, but for massive particles it could be preferred to use pT^2 + M^2 instead. This parameter allows to use pT^2 + k * M^2 for weak showers, thus k = 0 is the standard ordering and is used as default.

    flag  SpaceShower:dopTDampMass   (default = on)
    Add an extra dampening to the weak shower to lower the production of low-pT W/Z's. The dampening is given by (pT^2 + 0.25 M^2)/ (pT^2 + M^2), where M^2 is the squared mass of the W/Z.

    flag  SpaceShower:vetoWeakJets   (default = on)
    This flag will veto the 2nd emission on the same side of the process if it has too high "pT" if the primary process was weak production (code 221, 222, 223). This is too avoid doubling counting with dijet production followed by an emission of a W/Z boson. The pT definition used is the pT in the rest frame of the two emitted partons with respect to the incoming parton. This pT definition should be close to the pT definition of a dijet event.

    parm  SpaceShower:vetoWeakJetspTcut   (default = 20.0; minimum = 1.0; maximum = 1e9)
    This parameter determines the cut-off pT used for the veto of emissions for weak production. For more information see vetoWeakJets.

    Further variables

    These should normally not be touched. Their only function is for cross-checks.

    There are three flags you can use to switch on or off selected branchings in the shower:

    flag  SpaceShower:QCDshower   (default = on)
    Allow a QCD shower; on/off = true/false.

    flag  SpaceShower:QEDshowerByQ   (default = on)
    Allow quarks to radiate photons; on/off = true/false.

    flag  SpaceShower:QEDshowerByL   (default = on)
    Allow leptons to radiate photons; on/off = true/false.

    There are some further possibilities to modify the shower:

    flag  SpaceShower:MEcorrections   (default = on)
    Use of matrix element corrections; on/off = true/false.

    flag  SpaceShower:MEafterFirst   (default = on)
    Use of matrix element corrections also after the first emission, for dipole ends of the same system that did not yet radiate. Only has a meaning if MEcorrections above is switched on.

    flag  SpaceShower:phiPolAsym   (default = on)
    Azimuthal asymmetry induced by gluon polarization; on/off = true/false.

    flag  SpaceShower:phiIntAsym   (default = on)
    Azimuthal asymmetry induced by interference; on/off = true/false.

    parm  SpaceShower:strengthIntAsym   (default = 0.7; minimum = 0.; maximum = 0.9)
    Size of asymmetry induced by interference. Natural value of order 0.5; expression would blow up for a value of 1.

    mode  SpaceShower:nQuarkIn   (default = 5; minimum = 0; maximum = 5)
    Number of allowed quark flavours in g -> q qbar branchings, when kinematically allowed, and thereby also in incoming beams. Changing it to 4 would forbid g -> b bbar, etc.

    Technical notes

    Almost everything is equivalent to the algorithm in [1]. Minor changes are as follows.
    • It is now possible to have a second-order running alpha_s, in addition to fixed or first-order running.
    • The description of heavy flavour production in the threshold region has been modified, so as to be more forgiving about mismatches between the c/b masses used in Pythia relative to those used in a respective PDF parametrization. The basic idea is that, in the threshold region of a heavy quark Q, Q = c/b, the effect of subsequent Q -> Q g branchings is negligible. If so, then
      f_Q(x, pT2) = integral_mQ2^pT2 dpT'2/pT'2 * alpha_s(pT'2)/2pi * integral P(z) g(x', pT'2) delta(x - z x')
      so use this to select the pT2 of the g -> Q Qbar branching. In the old formalism the same kind of behaviour should be obtained, but by a cancellation of a 1/f_Q that diverges at the threshold and a Sudakov that vanishes.
      The strategy therefore is that, once pT2 < f * mQ2, with f a parameter of the order of 2, a pT2 is chosen like dpT2/pT2 between mQ2 and f * mQ2, a nd a z flat in the allowed range. Thereafter acceptance is based on the product of three factors, representing the running of alpha_strong, the splitting kernel (including the mass term) and the gluon density weight. At failure, a new pT2 is chosen in the same range, i.e. is not required to be lower since no Sudakov is involved.
    • The QED algorithm now allows for hadron beams with non-zero photon content. The backwards-evolution of a photon in a hadron is identical to that of a gluon, with CF -> eq^2 and CA -> 0. Note that this will only work in conjunction with parton distribution that explicitly include photons as part of the hadron structure (such as the MRST2004qed set). Since Pythia's internal sets do not allow for photon content in hadrons, it is thus necessary to use the LHAPDF interface to make use of this feature. The possibility of a fermion backwards-evolving to a photon has not yet been included, nor has photon backwards-evolution in lepton beams.
    pythia8-8.1.80.orig/htmldoc/CompositenessProcesses.html0000644000175000017500000002336012217615311021376 0ustar sunsun Compositeness Processes

    Compositeness Processes

    Compositeness scenarios may give rise to sharp resonances of excited quarks and leptons. An excited copy of the first generation is implemented, consisting of spin 1/2 particles. The possibility of contact interactions between SM fermions is also implemented in the context of 2 -> 2 quark or fermion-lepton scattering.

    Related to excited fermions, the current implementation contains gauge interaction production by quark-gluon fusion or lepton-photon fusion and contact interaction production by quark-quark or quark-antiquark scattering. For both the 2 -> 1 and 2 -> 2 processes a non-trivial angular dependence is included in the decay, however, only decays into gauge bosons are supported, i.e. not decays through contact interactions. In additions to the compositeness scale and couplings listed below, you are expected to change the excited-fermion masses in accordance with what is desired. See [Bau90] for conventions.

    The contact interactions are implemented according to [Eic83]. The processes include the SM contributions as well as interference. For this reason the processes below converge toward the SM equivalents when the contact interaction contributions are close to zero, e.g. HardQCD:qq2qq and HardQCD:qqbar2qqbarNew in the case of quark scattering.

    Excited fermions, production processes

    A few different production processes have been implemented, which normally would not overlap and therefore could be run together.

    flag  ExcitedFermion:all   (default = off)
    Common switch for the group of implemented processes that produce an excited fermion.

    flag  ExcitedFermion:dg2dStar   (default = off)
    Scatterings d g -> d^*. Code 4001.

    flag  ExcitedFermion:ug2uStar   (default = off)
    Scatterings u g -> u^*. Code 4002.

    flag  ExcitedFermion:sg2sStar   (default = off)
    Scatterings s g -> s^*. Code 4003.

    flag  ExcitedFermion:cg2cStar   (default = off)
    Scatterings c g -> c^*. Code 4004.

    flag  ExcitedFermion:bg2bStar   (default = off)
    Scatterings b g -> b^*. Code 4005.

    flag  ExcitedFermion:egm2eStar   (default = off)
    Scatterings e gamma -> e^*. Code 4011.

    flag  ExcitedFermion:mugm2muStar   (default = off)
    Scatterings mu gamma -> mu^*. Code 4013.

    flag  ExcitedFermion:taugm2tauStar   (default = off)
    Scatterings tau gamma -> tau^*. Code 4015.

    flag  ExcitedFermion:qq2dStarq   (default = off)
    Scatterings q q(bar) -> d^* q(bar). Code 4021.

    flag  ExcitedFermion:qq2uStarq   (default = off)
    Scatterings q q(bar) -> u^* q(bar). Code 4022.

    flag  ExcitedFermion:qq2sStarq   (default = off)
    Scatterings q q(bar) -> s^* q(bar). Code 4023.

    flag  ExcitedFermion:qq2cStarq   (default = off)
    Scatterings q q(bar) -> c^* q(bar). Code 4024.

    flag  ExcitedFermion:qq2bStarq   (default = off)
    Scatterings q q(bar) -> b^* q(bar). Code 4025.

    flag  ExcitedFermion:qqbar2eStare   (default = off)
    Scatterings q qbar -> e^*+- e^-+. Code 4031.

    flag  ExcitedFermion:qqbar2nueStarnue   (default = off)
    Scatterings q qbar -> nu_e^* nu_ebar. Code 4032.

    flag  ExcitedFermion:qqbar2muStarmu   (default = off)
    Scatterings q qbar -> mu^*+- mu^-+. Code 4033.

    flag  ExcitedFermion:qqbar2numuStarnumu   (default = off)
    Scatterings q qbar -> nu_mu^* nu_mubar. Code 4034.

    flag  ExcitedFermion:qqbar2tauStartau   (default = off)
    Scatterings q qbar -> tau^*+- tau^-+. Code 4035.

    flag  ExcitedFermion:qqbar2nutauStarnutau   (default = off)
    Scatterings q qbar -> nu_tau^* nu_taubar. Code 4036.

    Excited fermions, parameters

    The basic couplings of the model are

    parm  ExcitedFermion:Lambda   (default = 1000.; minimum = 100.)
    Compositeness scale Lambda in GeV.

    parm  ExcitedFermion:coupF   (default = 1.0; minimum = 0.0)
    Strength f of the SU(2) coupling.

    parm  ExcitedFermion:coupFprime   (default = 1.0; minimum = 0.0)
    Strength f' of the U(1) coupling.

    parm  ExcitedFermion:coupFcol   (default = 1.0; minimum = 0.0)
    Strength f_c of the SU(3) coupling.

    Contact interactions, production processes

    The processes including contact interactions are

    flag  ContactInteractions:QCqq2qq   (default = off)
    Scatterings q q -> q q including contact interactions. Code 4201.

    flag  ContactInteractions:QCqqbar2qqbar   (default = off)
    Scatterings q qbar -> q' qbar' including contact interactions. Code 4202.

    flag  ContactInteractions:QCffbar2eebar   (default = off)
    Scatterings f fbar -> e- e+ including contact interactions. Code 4203.

    flag  ContactInteractions:QCffbar2mumubar   (default = off)
    Scatterings f fbar -> mu- mu+ including contact interactions. Code 4204.

    flag  ContactInteractions:QCffbar2tautaubar   (default = off)
    Scatterings f fbar -> tau- tau+ including contact interactions. Code 4205.

    Contact interactions, parameters

    mode  ContactInteractions:nQuarkNew   (default = 3; minimum = 0; maximum = 5)
    Number of allowed outgoing new quark flavours in the above q qbar -> q' qbar' process. Similar to HardQCD:nQuarkNew for the QCD processes.

    parm  ContactInteractions:Lambda   (default = 1000.; minimum = 100.)
    Compositeness scale Lambda in GeV. Its overall normalization is largely a matter of convention. The choice made here for the q qbar -> l- l+ processes is such that the pure contact interaction part of the left-left interactions (i.e. disregarding gamma^*, Z^0 and interference terms) has the form d(sigmaHat)/d(tHat) = pi * uHat^2 / (3 * sHat^2 * Lambda^4). The corresponding part of the q qbar -> q' qbar' cross section is a factor 3 larger from colour.

    mode  ContactInteractions:etaLL   (default = 0; minimum = -1; maximum = 1)
    Helicity parameter.
    option 1 :
    option 0 :
    option -1 :

    mode  ContactInteractions:etaRR   (default = 0; minimum = -1; maximum = 1)
    Helicity parameter.
    option 1 :
    option 0 :
    option -1 :

    mode  ContactInteractions:etaLR   (default = 0; minimum = -1; maximum = 1)
    Helicity parameter.
    option 1 :
    option 0 :
    option -1 : pythia8-8.1.80.orig/htmldoc/ProgramMethods.html0000644000175000017500000043666312217615312017626 0ustar sunsun Program Methods

    Program Methods

    This is an alphabetical index of all methods that are documented elsewhere on these pages, beginning with the few methods that do not belong to a class. Many of them are only intended for experts, while undocumented ones are only for code authors.

    Return type Method name Documentation page
    AlpgenHooks(...) Alpgen Event Interface
    friend double cosphi(...) Four-Vectors
    friend double cosphi(...) Four-Vectors
    friend double costheta(...) Four-Vectors
    friend double cross3(...) Four-Vectors
    friend double dot3(...) Four-Vectors
    PDF* getPDFPtr(...) Program Flow
    bool initAfterBeams() Alpgen Event Interface
    friend double m(...) Four-Vectors
    double m(...) Particle Properties
    friend double m2(...) Four-Vectors
    double m2(...) Particle Properties
    friend ostream& operator<<(...) Four-Vectors
    friend ostream& operator<<(...) Four-Vectors
    friend Vec4 operator*(...) Four-Vectors
    friend Vec4 operator*(...) Four-Vectors
    friend double operator*(...) Four-Vectors
    friend Hist operator*(...) Histograms
    friend Hist operator*(...) Histograms
    friend Hist operator*(...) Histograms
    friend Vec4 operator+(...) Four-Vectors
    friend Hist operator+(...) Histograms
    friend Hist operator+(...) Histograms
    friend Hist operator+(...) Histograms
    friend Vec4 operator-(...) Four-Vectors
    friend Hist operator-(...) Histograms
    friend Hist operator-(...) Histograms
    friend Hist operator-(...) Histograms
    friend Vec4 operator/(...) Four-Vectors
    friend Hist operator/(...) Histograms
    friend Hist operator/(...) Histograms
    friend Hist operator/(...) Histograms
    friend ostream& operator<<(...) Histograms
    ParticleDataEntry& particleDataEntry() Particle Properties
    friend double phi(...) Four-Vectors
    friend double phi(...) Four-Vectors
    friend double REtaPhi(...) Four-Vectors
    friend double RRapPhi(...) Four-Vectors
    void setResonancePtr(...) Particle Data Scheme
    friend void table(...) Histograms
    friend void table(...) Histograms
    friend double theta(...) Four-Vectors
    AlpgenPar::AlpgenPar(...) Alpgen Event Interface
    double AlpgenPar::getParam(...) Alpgen Event Interface
    int AlpgenPar::getParamAsInt(...) Alpgen Event Interface
    bool AlpgenPar::haveParam(...) Alpgen Event Interface
    bool AlpgenPar::parse(...) Alpgen Event Interface
    BeamShape::BeamShape() Beam Shape
    Vec4 BeamShape::deltaPA() Beam Shape
    Vec4 BeamShape::deltaPB() Beam Shape
    virtual void BeamShape::init(...) Beam Shape
    virtual void BeamShape::pick() Beam Shape
    Vec4 BeamShape::vertex() Beam Shape
    virtual BeamShape::~BeamShape() Beam Shape
    bool CellJet::analyze(...) Event Analysis
    CellJet::CellJet(...) Event Analysis
    double CellJet::eT(...) Event Analysis
    double CellJet::etaCenter(...) Event Analysis
    double CellJet::etaWeighted(...) Event Analysis
    void CellJet::list() Event Analysis
    double CellJet::m(...) Event Analysis
    int CellJet::multiplicity(...) Event Analysis
    int CellJet::nError() Event Analysis
    double CellJet::phiCenter(...) Event Analysis
    double CellJet::phiWeighted(...) Event Analysis
    Vec4 CellJet::pMassive(...) Event Analysis
    Vec4 CellJet::pMassless(...) Event Analysis
    int CellJet::size() Event Analysis
    ClusterJet::analyze(...) Event Analysis
    ClusterJet::ClusterJet(...) Event Analysis
    double ClusterJet::distance(...) Event Analysis
    int ClusterJet::distanceSize() Event Analysis
    int ClusterJet::jetAssignment(...) Event Analysis
    void ClusterJet::list(...) Event Analysis
    int ClusterJet::mult(...) Event Analysis
    int ClusterJet::nError() Event Analysis
    Vec4 ClusterJet::p(...) Event Analysis
    int ClusterJet::size() Event Analysis
    double CoupSM::af(...) Standard Model Parameters
    double CoupSM::af2(...) Standard Model Parameters
    double CoupSM::alphaEM(...) Standard Model Parameters
    double CoupSM::alphaS(...) Standard Model Parameters
    double CoupSM::alphaS1Ord(...) Standard Model Parameters
    double CoupSM::alphaS2OrdCorr(...) Standard Model Parameters
    double CoupSM::cos2thetaW() Standard Model Parameters
    CoupSM::CoupSM() Standard Model Parameters
    double CoupSM::ef(...) Standard Model Parameters
    double CoupSM::ef2(...) Standard Model Parameters
    double CoupSM::efvf(...) Standard Model Parameters
    double CoupSM::GF() Standard Model Parameters
    void CoupSM::init(...) Standard Model Parameters
    double CoupSM::Lambda3() Standard Model Parameters
    double CoupSM::Lambda4() Standard Model Parameters
    double CoupSM::Lambda5() Standard Model Parameters
    double CoupSM::lf(...) Standard Model Parameters
    double CoupSM::rf(...) Standard Model Parameters
    double CoupSM::sin2thetaW() Standard Model Parameters
    double CoupSM::sin2thetaWbar() Standard Model Parameters
    double CoupSM::t3f(...) Standard Model Parameters
    double CoupSM::V2CKMgen(...) Standard Model Parameters
    double CoupSM::V2CKMid(...) Standard Model Parameters
    int CoupSM::V2CKMpick(...) Standard Model Parameters
    double CoupSM::V2CKMsum(...) Standard Model Parameters
    double CoupSM::VCKMgen(...) Standard Model Parameters
    double CoupSM::VCKMid(...) Standard Model Parameters
    double CoupSM::vf(...) Standard Model Parameters
    double CoupSM::vf2(...) Standard Model Parameters
    double CoupSM::vf2af2(...) Standard Model Parameters
    double DecayChannel::bRatio() Particle Data Scheme
    void DecayChannel::bRatio(...) Particle Data Scheme
    bool DecayChannel::contains(...) Particle Data Scheme
    bool DecayChannel::contains(...) Particle Data Scheme
    bool DecayChannel::contains(...) Particle Data Scheme
    double DecayChannel::currentBR() Particle Data Scheme
    void DecayChannel::currentBR(...) Particle Data Scheme
    DecayChannel::DecayChannel(...) Particle Data Scheme
    bool DecayChannel::hasChanged() Particle Data Scheme
    int DecayChannel::meMode() Particle Data Scheme
    void DecayChannel::meMode(...) Particle Data Scheme
    int DecayChannel::multiplicity() Particle Data Scheme
    void DecayChannel::multiplicity(...) Particle Data Scheme
    int DecayChannel::onMode() Particle Data Scheme
    void DecayChannel::onMode(...) Particle Data Scheme
    double DecayChannel::onShellWidth() Particle Data Scheme
    void DecayChannel::onShellWidth(...) Particle Data Scheme
    void DecayChannel::onShellWidthFactor(...) Particle Data Scheme
    void DecayChannel::openSec(...) Particle Data Scheme
    double DecayChannel::openSec(...) Particle Data Scheme
    void DecayChannel::product(...) Particle Data Scheme
    int DecayChannel::product(...) Particle Data Scheme
    void DecayChannel::rescaleBR(...) Particle Data Scheme
    void DecayChannel::setHasChanged(...) Particle Data Scheme
    virtual bool DecayHandler::decay(...) External Decays
    int Event::append(...) Event Record
    int Event::append(...) Event Record
    int Event::append(...) Event Record
    int Event::append(...) Event Record
    int Event::append(...) Event Record
    Particle& Event::at(...) Event Record
    Particle& Event::back() Event Record
    void Event::bst(...) Event Record
    void Event::bst(...) Event Record
    void Event::bst(...) Event Record
    void Event::clear() Event Record
    int Event::copy(...) Event Record
    vector<int> Event::daughterList(...) Event Record
    Event::Event(...) Event Record
    Particle& Event::front() Event Record
    int Event::iBotCopy(...) Event Record
    int Event::iBotCopyId(...) Event Record
    void Event::init(...) Event Record
    void Event::initColTag(...) Event Record
    bool Event::isAncestor(...) Event Record
    int Event::iTopCopy(...) Event Record
    int Event::iTopCopyId(...) Event Record
    int Event::lastColTag() Event Record
    void Event::list() Event Record
    void Event::list(...) Event Record
    void Event::list(...) Event Record
    void Event::list(...) Event Record
    vector<int> Event::motherList(...) Event Record
    int Event::nextColTag() Event Record
    Event& Event::operator+=(...) Event Record
    Event& Event::operator=(...) Event Record
    Particle& Event::operator[](...) Event Record
    const Particle& Event::operator[](...) Event Record
    void Event::popBack(...) Event Record
    void Event::remove(...) Event Record
    void Event::reset() Event Record
    void Event::restorePtrs() Event Record
    void Event::rot(...) Event Record
    void Event::rotbst(...) Event Record
    double Event::scale() Event Record
    void Event::scale(...) Event Record
    double Event::scaleSecond() Event Record
    void Event::scaleSecond(...) Event Record
    int Event::setEvtPtr(...) Event Record
    vector<int> Event::sisterList(...) Event Record
    vector<int> Event::sisterListTopBot(...) Event Record
    int Event::size() Event Record
    int Event::statusHepMC(...) Event Record
    bool Event::undoDecay(...) Event Record
    void Hist::book(...) Histograms
    void Hist::fill(...) Histograms
    double Hist::getBinContent(...) Histograms
    int Hist::getEntries() Histograms
    Hist::Hist() Histograms
    Hist::Hist(...) Histograms
    Hist::Hist(...) Histograms
    Hist::Hist(...) Histograms
    void Hist::name(...) Histograms
    void Hist::null() Histograms
    Hist& Hist::operator*=(...) Histograms
    Hist& Hist::operator*=(...) Histograms
    Hist& Hist::operator*=(...) Histograms
    Hist& Hist::operator+=(...) Histograms
    Hist& Hist::operator+=(...) Histograms
    Hist& Hist::operator-=(...) Histograms
    Hist& Hist::operator-=(...) Histograms
    Hist& Hist::operator/=(...) Histograms
    Hist& Hist::operator=(...) Histograms
    bool Hist::sameSize(...) Histograms
    void Hist::table(...) Histograms
    void Hist::table(...) Histograms
    void Hist::takeLog(...) Histograms
    void Hist::takeSqrt() Histograms
    double Info::a0MPI() Event Information
    void Info::addCounter(...) Event Information
    double Info::alphaEM() Event Information
    double Info::alphaS() Event Information
    bool Info::atEndOfFile() Event Information
    double Info::bMPI() Event Information
    int Info::code() Event Information
    int Info::codeMPI(...) Event Information
    int Info::codeSub() Event Information
    double Info::eA() Event Information
    double Info::eB() Event Information
    double Info::eCM() Event Information
    double Info::eMPI(...) Event Information
    double Info::enhanceMPI() Event Information
    int Info::getCounter(...) Event Information
    bool Info::hasHistory() Event Information
    void Info::hasHistory(...) Event Information
    bool Info::hasSub() Event Information
    string Info::header(...) Event Information
    vector <string> Info::headerKeys() Event Information
    int Info::iAMPI(...) Event Information
    int Info::iBMPI(...) Event Information
    int Info::id1() Event Information
    int Info::id1pdf() Event Information
    int Info::id2() Event Information
    int Info::id2pdf() Event Information
    int Info::idA() Event Information
    int Info::idB() Event Information
    bool Info::isDiffractiveA() Event Information
    bool Info::isDiffractiveB() Event Information
    bool Info::isDiffractiveC() Event Information
    bool Info::isLHA() Event Information
    bool Info::isMinBias() Event Information
    bool Info::isNonDiffractive() Event Information
    bool Info::isResolved() Event Information
    bool Info::isValence1() Event Information
    bool Info::isValence2() Event Information
    int Info::lhaStrategy() Event Information
    void Info::list() Event Information
    double Info::m3Hat() Event Information
    double Info::m4Hat() Event Information
    double Info::mA() Event Information
    double Info::mB() Event Information
    double Info::mergingWeight() Event Information
    double Info::mergingWeightNLO() Event Information
    double Info::mHat() Event Information
    long Info::nAccepted(...) Event Information
    string Info::name() Event Information
    string Info::nameSub() Event Information
    int Info::nFinal() Event Information
    int Info::nFinalSub() Event Information
    int Info::nFSRinProc() Event Information
    int Info::nFSRinRes() Event Information
    int Info::nISR() Event Information
    int Info::nMPI() Event Information
    long Info::nSelected(...) Event Information
    long Info::nTried(...) Event Information
    double Info::pdf1() Event Information
    double Info::pdf2() Event Information
    double Info::phiHat() Event Information
    double Info::pT2Hat() Event Information
    double Info::pT2NowISR() Event Information
    void Info::pT2NowISR(...) Event Information
    double Info::pTHat() Event Information
    double Info::pTmaxFSR() Event Information
    double Info::pTmaxISR() Event Information
    double Info::pTmaxMPI() Event Information
    double Info::pTMPI(...) Event Information
    double Info::pTnow() Event Information
    double Info::pzA() Event Information
    double Info::pzB() Event Information
    double Info::Q2Fac() Event Information
    double Info::Q2Ren() Event Information
    double Info::QFac() Event Information
    double Info::QRen() Event Information
    double Info::s() Event Information
    double Info::scalup() Event Information
    void Info::setCounter(...) Event Information
    void Info::setHeader(...) Event Information
    double Info::sHat() Event Information
    double Info::sigmaErr(...) Event Information
    double Info::sigmaGen(...) Event Information
    double Info::tau() Event Information
    double Info::tHat() Event Information
    double Info::thetaHat() Event Information
    bool Info::tooLowPTmin() Event Information
    double Info::uHat() Event Information
    double Info::weight() Event Information
    double Info::weightSum() Event Information
    double Info::x1() Event Information
    double Info::x1pdf() Event Information
    double Info::x2() Event Information
    double Info::x2pdf() Event Information
    double Info::y() Event Information
    double Info::zNowISR() Event Information
    void Info::zNowISR(...) Event Information
    void LHAup::addParticle(...) Les Houches Accord
    void LHAup::addProcess(...) Les Houches Accord
    double LHAup::alphaQCD() Les Houches Accord
    double LHAup::alphaQED() Les Houches Accord
    void LHAup::closeFile(...) Les Houches Accord
    bool LHAup::closeLHEF(...) Les Houches Accord
    int LHAup::col1(...) Les Houches Accord
    int LHAup::col2(...) Les Houches Accord
    double LHAup::e(...) Les Houches Accord
    double LHAup::eBeamA() Les Houches Accord
    double LHAup::eBeamB() Les Houches Accord
    bool LHAup::eventLHEF(...) Les Houches Accord
    bool LHAup::fileFound() Les Houches Accord
    int LHAup::id(...) Les Houches Accord
    int LHAup::id1() Les Houches Accord
    int LHAup::id1pdf() Les Houches Accord
    int LHAup::id2() Les Houches Accord
    int LHAup::id2pdf() Les Houches Accord
    int LHAup::idBeamA() Les Houches Accord
    int LHAup::idBeamB() Les Houches Accord
    int LHAup::idProcess() Les Houches Accord
    int LHAup::idProcess(...) Les Houches Accord
    bool LHAup::initLHEF() Les Houches Accord
    LHAup::LHAup(...) Les Houches Accord
    void LHAup::listEvent(...) Les Houches Accord
    void LHAup::listInit(...) Les Houches Accord
    double LHAup::m(...) Les Houches Accord
    int LHAup::mother1(...) Les Houches Accord
    int LHAup::mother2(...) Les Houches Accord
    bool LHAup::newEventFile(...) Les Houches Accord
    istream* LHAup::openFile(...) Les Houches Accord
    bool LHAup::openLHEF(...) Les Houches Accord
    double LHAup::pdf1() Les Houches Accord
    double LHAup::pdf2() Les Houches Accord
    int LHAup::pdfGroupBeamA() Les Houches Accord
    int LHAup::pdfGroupBeamB() Les Houches Accord
    bool LHAup::pdfIsSet() Les Houches Accord
    int LHAup::pdfSetBeamA() Les Houches Accord
    int LHAup::pdfSetBeamB() Les Houches Accord
    double LHAup::px(...) Les Houches Accord
    double LHAup::py(...) Les Houches Accord
    double LHAup::pz(...) Les Houches Accord
    double LHAup::scale() Les Houches Accord
    double LHAup::scale(...) Les Houches Accord
    double LHAup::scalePDF() Les Houches Accord
    void LHAup::setBeamA(...) Les Houches Accord
    void LHAup::setBeamB(...) Les Houches Accord
    virtual bool LHAup::setEvent(...) Les Houches Accord
    void LHAup::setIdX(...) Les Houches Accord
    void LHAup::setInfoHeader(...) Les Houches Accord
    void LHAup::setInfoHeader(...) Les Houches Accord
    virtual bool LHAup::setInit() Les Houches Accord
    bool LHAup::setInitLHEF(...) Les Houches Accord
    bool LHAup::setNewEventLHEF(...) Les Houches Accord
    bool LHAup::setOldEventLHEF() Les Houches Accord
    void LHAup::setPdf(...) Les Houches Accord
    void LHAup::setProcess(...) Les Houches Accord
    void LHAup::setPtr(...) Les Houches Accord
    void LHAup::setStrategy(...) Les Houches Accord
    void LHAup::setXErr(...) Les Houches Accord
    void LHAup::setXMax(...) Les Houches Accord
    void LHAup::setXSec(...) Les Houches Accord
    int LHAup::sizePart() Les Houches Accord
    int LHAup::sizeProc() Les Houches Accord
    virtual bool LHAup::skipEvent(...) Les Houches Accord
    double LHAup::spin(...) Les Houches Accord
    int LHAup::status(...) Les Houches Accord
    int LHAup::strategy() Les Houches Accord
    double LHAup::tau(...) Les Houches Accord
    double LHAup::weight() Les Houches Accord
    double LHAup::x1() Les Houches Accord
    double LHAup::x1pdf() Les Houches Accord
    double LHAup::x2() Les Houches Accord
    double LHAup::x2pdf() Les Houches Accord
    double LHAup::xErr(...) Les Houches Accord
    double LHAup::xErrSum() Les Houches Accord
    double LHAup::xMax(...) Les Houches Accord
    double LHAup::xSec(...) Les Houches Accord
    double LHAup::xSecSum() Les Houches Accord
    virtual LHAup::~LHAup() Les Houches Accord
    bool LHAupAlpgen::addResonances() Alpgen Event Interface
    LHAupAlpgen::LHAupAlpgen(...) Alpgen Event Interface
    bool LHAupAlpgen::rescaleMomenta() Alpgen Event Interface
    void LHAupLHEF::closeAllFiles() Les Houches Accord
    virtual bool MergingHooks::canCutOnRecState() C K K W L Merging
    virtual double MergingHooks::dampenIfFailCuts(...) C K K W L Merging
    virtual bool MergingHooks::doCutOnRecState(...) C K K W L Merging
    virtual double MergingHooks::hardProcessME(...) C K K W L Merging
    MergingHooks::MergingHooks() C K K W L Merging
    int MergingHooks::nHardInLeptons() C K K W L Merging
    int MergingHooks::nHardInPartons() C K K W L Merging
    int MergingHooks::nHardOutLeptons() C K K W L Merging
    int MergingHooks::nHardOutPartons() C K K W L Merging
    int MergingHooks::nMaxJets() C K K W L Merging
    int MergingHooks::nResInCurrent() C K K W L Merging
    double MergingHooks::tms() C K K W L Merging
    virtual double MergingHooks::tmsDefinition(...) C K K W L Merging
    virtual MergingHooks::~MergingHooks() C K K W L Merging
    int Particle::acol() Particle Properties
    void Particle::bst(...) Particle Properties
    void Particle::bst(...) Particle Properties
    void Particle::bst(...) Particle Properties
    void Particle::bst(...) Particle Properties
    void Particle::bstback(...) Particle Properties
    void Particle::bstback(...) Particle Properties
    bool Particle::canDecay() Particle Properties
    double Particle::charge() Particle Properties
    int Particle::chargeType() Particle Properties
    int Particle::col() Particle Properties
    void Particle::cols(...) Particle Properties
    int Particle::colType() Particle Properties
    double Particle::constituentMass() Particle Properties
    int Particle::daughter1() Particle Properties
    int Particle::daughter2() Particle Properties
    void Particle::daughters(...) Particle Properties
    bool Particle::doExternalDecay() Particle Properties
    double Particle::e() Particle Properties
    double Particle::eCalc() Particle Properties
    double Particle::eT() Particle Properties
    double Particle::eT2() Particle Properties
    double Particle::eta() Particle Properties
    bool Particle::hasVertex() Particle Properties
    int Particle::iBotCopy() Particle Properties
    int Particle::iBotCopyId() Particle Properties
    int Particle::id() Particle Properties
    int Particle::idAbs() Particle Properties
    void Particle::index() Particle Properties
    bool Particle::isAncestor(...) Particle Properties
    bool Particle::isCharged() Particle Properties
    bool Particle::isDiquark() Particle Properties
    bool Particle::isFinal() Particle Properties
    bool Particle::isGluon() Particle Properties
    bool Particle::isHadron() Particle Properties
    bool Particle::isLepton() Particle Properties
    bool Particle::isNeutral() Particle Properties
    bool Particle::isParton() Particle Properties
    bool Particle::isQuark() Particle Properties
    bool Particle::isRescatteredIncoming() Particle Properties
    bool Particle::isResonance() Particle Properties
    bool Particle::isVisible() Particle Properties
    int Particle::iTopCopy() Particle Properties
    int Particle::iTopCopyId() Particle Properties
    double Particle::m() Particle Properties
    double Particle::m0() Particle Properties
    double Particle::m2() Particle Properties
    double Particle::m2Calc() Particle Properties
    bool Particle::mayDecay() Particle Properties
    double Particle::mCalc() Particle Properties
    double Particle::mMax() Particle Properties
    double Particle::mMin() Particle Properties
    int Particle::mother1() Particle Properties
    int Particle::mother2() Particle Properties
    void Particle::mothers(...) Particle Properties
    double Particle::mSel() Particle Properties
    double Particle::mT() Particle Properties
    double Particle::mT2() Particle Properties
    double Particle::mWidth() Particle Properties
    string Particle::name() Particle Properties
    string Particle::nameWithStatus() Particle Properties
    void Particle::offsetCol(...) Particle Properties
    void Particle::offsetHistory(...)) Particle Properties
    Particle& Particle::operator=(...) Particle Properties
    Vec4 Particle::p() Particle Properties
    void Particle::p(...) Particle Properties
    double Particle::pAbs() Particle Properties
    double Particle::pAbs2() Particle Properties
    Particle::Particle() Particle Properties
    Particle::Particle(...) Particle Properties
    Particle::Particle(...) Particle Properties
    Particle::Particle(...) Particle Properties
    double Particle::phi() Particle Properties
    double Particle::pNeg() Particle Properties
    double Particle::pol() Particle Properties
    double Particle::pPos() Particle Properties
    double Particle::pT() Particle Properties
    double Particle::pT2() Particle Properties
    double Particle::px() Particle Properties
    double Particle::py() Particle Properties
    double Particle::pz() Particle Properties
    void Particle::rescale3(...) Particle Properties
    void Particle::rescale4(...) Particle Properties
    void Particle::rescale5(...) Particle Properties
    void Particle::rot(...) Particle Properties
    void Particle::rotbst(...) Particle Properties
    double Particle::scale() Particle Properties
    void Particle::setEvtPtr(...) Particle Properties
    void Particle::setPDEPtr(...) Particle Properties
    vector<int> Particle::sisterList(...) Particle Properties
    int Particle::spinType() Particle Properties
    int Particle::status() Particle Properties
    int Particle::statusAbs() Particle Properties
    void Particle::statusCode(...) Particle Properties
    int Particle::statusHepMC() Particle Properties
    void Particle::statusNeg() Particle Properties
    void Particle::statusPos() Particle Properties
    double Particle::tau() Particle Properties
    double Particle::tau0() Particle Properties
    double Particle::tDec() Particle Properties
    double Particle::theta() Particle Properties
    double Particle::thetaXZ() Particle Properties
    double Particle::tProd() Particle Properties
    bool Particle::undoDecay() Particle Properties
    Vec4 Particle::vDec() Particle Properties
    Vec4 Particle::vProd() Particle Properties
    void Particle::vProd(...) Particle Properties
    double Particle::xDec() Particle Properties
    double Particle::xProd() Particle Properties
    double Particle::y() Particle Properties
    double Particle::yDec() Particle Properties
    double Particle::yProd() Particle Properties
    double Particle::zDec() Particle Properties
    double Particle::zProd() Particle Properties
    void ParticleData::addParticle(...) Particle Data Scheme
    void ParticleData::addParticle(...) Particle Data Scheme
    void ParticleData::antiName(...) Particle Data Scheme
    int ParticleData::baryonNumberType(...) Particle Data Scheme
    bool ParticleData::canDecay(...) Particle Data Scheme
    double ParticleData::charge(...) Particle Data Scheme
    void ParticleData::chargeType(...) Particle Data Scheme
    int ParticleData::chargeType(...) Particle Data Scheme
    void ParticleData::checkTable(...) Particle Data Scheme
    void ParticleData::checkTable(...) Particle Data Scheme
    void ParticleData::colType(...) Particle Data Scheme
    int ParticleData::colType(...) Particle Data Scheme
    double ParticleData::constituentMass(...) Particle Data Scheme
    bool ParticleData::doExternalDecay(...) Particle Data Scheme
    void ParticleData::doExternalDecays(...) Particle Data Scheme
    void ParticleData::doForceWidth(...) Particle Data Scheme
    bool ParticleData::doForceWidth(...) Particle Data Scheme
    bool ParticleData::hasAnti(...) Particle Data Scheme
    void ParticleData::hasChanged(...) Particle Data Scheme
    bool ParticleData::hasChanged(...) Particle Data Scheme
    int ParticleData::heaviestQuark(...) Particle Data Scheme
    bool ParticleData::init(...) Particle Data Scheme
    void ParticleData::initPtr(...) Particle Data Scheme
    void ParticleData::initWidths(...) Particle Data Scheme
    bool ParticleData::isBaryon(...) Particle Data Scheme
    bool ParticleData::isDiquark(...) Particle Data Scheme
    bool ParticleData::isGluon(...) Particle Data Scheme
    bool ParticleData::isHadron(...) Particle Data Scheme
    bool ParticleData::isLepton(...) Particle Data Scheme
    bool ParticleData::isMeson(...) Particle Data Scheme
    bool ParticleData::isOctetHadron(...) Particle Data Scheme
    bool ParticleData::isParticle(...) Particle Data Scheme
    bool ParticleData::isParton() Particle Data Scheme
    bool ParticleData::isQuark(...) Particle Data Scheme
    void ParticleData::isResonance(...) Particle Data Scheme
    bool ParticleData::isResonance(...) Particle Data Scheme
    void ParticleData::isVisible(...) Particle Data Scheme
    bool ParticleData::isVisible(...) Particle Data Scheme
    void ParticleData::list(...) Particle Data Scheme
    void ParticleData::list(...) Particle Data Scheme
    void ParticleData::list(...) Particle Data Scheme
    void ParticleData::listAll(...) Particle Data Scheme
    void ParticleData::listChanged(...) Particle Data Scheme
    void ParticleData::listChangedAndRes(...) Particle Data Scheme
    void ParticleData::listFF(...) Particle Data Scheme
    void ParticleData::listXML(...) Particle Data Scheme
    void ParticleData::m0(...) Particle Data Scheme
    double ParticleData::m0(...) Particle Data Scheme
    double ParticleData::m0Max(...) Particle Data Scheme
    double ParticleData::m0Min(...) Particle Data Scheme
    void ParticleData::mayDecay(...) Particle Data Scheme
    bool ParticleData::mayDecay(...) Particle Data Scheme
    void ParticleData::mMax(...) Particle Data Scheme
    double ParticleData::mMax(...) Particle Data Scheme
    void ParticleData::mMin(...) Particle Data Scheme
    double ParticleData::mMin(...) Particle Data Scheme
    double ParticleData::mRun(...) Particle Data Scheme
    double ParticleData::mSel(...) Particle Data Scheme
    void ParticleData::mWidth(...) Particle Data Scheme
    double ParticleData::mWidth(...) Particle Data Scheme
    void ParticleData::name(...) Particle Data Scheme
    string ParticleData::name(...) Particle Data Scheme
    void ParticleData::names(...) Particle Data Scheme
    int ParticleData::nextId(...) Particle Data Scheme
    ParticleData::ParticleData() Particle Data Scheme
    ParticleDataEntry* ParticleData::particleDataEntryPtr(...) Particle Data Scheme
    bool ParticleData::readFF(...) Particle Data Scheme
    bool ParticleData::readString(...) Particle Data Scheme
    bool ParticleData::readXML(...) Particle Data Scheme
    bool ParticleData::reInit(...) Particle Data Scheme
    void ParticleData::rescaleBR(...) Particle Data Scheme
    void ParticleData::resInit(...) Particle Data Scheme
    double ParticleData::resOpenFrac(...) Particle Data Scheme
    double ParticleData::resWidth(...) Particle Data Scheme
    double ParticleData::resWidthChan(...) Particle Data Scheme
    double ParticleData::resWidthOpen(...) Particle Data Scheme
    double ParticleData::resWidthRescaleFactor(...) Particle Data Scheme
    double ParticleData::resWidthStore(...) Particle Data Scheme
    void ParticleData::setAll(...) Particle Data Scheme
    void ParticleData::spinType(...) Particle Data Scheme
    int ParticleData::spinType(...) Particle Data Scheme
    void ParticleData::tau0(...) Particle Data Scheme
    double ParticleData::tau0(...) Particle Data Scheme
    bool ParticleData::useBreitWigner(...) Particle Data Scheme
    void ParticleDataEntry::addChannel(...) Particle Data Scheme
    int ParticleDataEntry::baryonNumberType(...) Particle Data Scheme
    bool ParticleDataEntry::canDecay(...) Particle Data Scheme
    DecayChannel& ParticleDataEntry::channel(...) Particle Data Scheme
    const DecayChannel& ParticleDataEntry::channel(...) Particle Data Scheme
    double ParticleDataEntry::charge(...) Particle Data Scheme
    int ParticleDataEntry::chargeType(...) Particle Data Scheme
    void ParticleDataEntry::clearChannels() Particle Data Scheme
    int ParticleDataEntry::colType(...) Particle Data Scheme
    double ParticleDataEntry::constituentMass() Particle Data Scheme
    bool ParticleDataEntry::doExternalDecay() Particle Data Scheme
    bool ParticleDataEntry::doForceWidth() Particle Data Scheme
    ResonanceWidths* ParticleDataEntry::getResonancePtr() Particle Data Scheme
    bool ParticleDataEntry::hasAnti() Particle Data Scheme
    void ParticleDataEntry::hasChanged(...) Particle Data Scheme
    int ParticleDataEntry::heaviestQuark(...) Particle Data Scheme
    int ParticleDataEntry::id() Particle Data Scheme
    void ParticleDataEntry::initBWmass() Particle Data Scheme
    void ParticleDataEntry::initPtr(...) Particle Data Scheme
    bool ParticleDataEntry::isBaryon() Particle Data Scheme
    bool ParticleDataEntry::isDiquark() Particle Data Scheme
    bool ParticleDataEntry::isGluon() Particle Data Scheme
    bool ParticleDataEntry::isHadron() Particle Data Scheme
    bool ParticleDataEntry::isLepton() Particle Data Scheme
    bool ParticleDataEntry::isMeson() Particle Data Scheme
    bool ParticleDataEntry::isOctetHadron() Particle Data Scheme
    bool ParticleDataEntry::isParton() Particle Data Scheme
    bool ParticleDataEntry::isQuark() Particle Data Scheme
    bool ParticleDataEntry::isResonance() Particle Data Scheme
    bool ParticleDataEntry::isVisible() Particle Data Scheme
    double ParticleDataEntry::m0() Particle Data Scheme
    double ParticleDataEntry::m0Max() Particle Data Scheme
    double ParticleDataEntry::m0Min() Particle Data Scheme
    bool ParticleDataEntry::mayDecay() Particle Data Scheme
    double ParticleDataEntry::mMax() Particle Data Scheme
    double ParticleDataEntry::mMin() Particle Data Scheme
    double ParticleDataEntry::mRun(...) Particle Data Scheme
    double ParticleDataEntry::mSel() Particle Data Scheme
    double ParticleDataEntry::mWidth() Particle Data Scheme
    string ParticleDataEntry::name(...) Particle Data Scheme
    ParticleDataEntry::ParticleDataEntry(...) Particle Data Scheme
    ParticleDataEntry::ParticleDataEntry(...) Particle Data Scheme
    DecayChannel& ParticleDataEntry::pickChannel() Particle Data Scheme
    bool ParticleDataEntry::preparePick(...) Particle Data Scheme
    void ParticleDataEntry::rescaleBR(...) Particle Data Scheme
    void ParticleDataEntry::resInit(...) Particle Data Scheme
    double ParticleDataEntry::resOpenFrac(...) Particle Data Scheme
    double ParticleDataEntry::resWidth(...) Particle Data Scheme
    double ParticleDataEntry::resWidthChan(...) Particle Data Scheme
    double ParticleDataEntry::resWidthOpen(...) Particle Data Scheme
    double ParticleDataEntry::resWidthRescaleFactor() Particle Data Scheme
    double ParticleDataEntry::resWidthStore(...) Particle Data Scheme
    void ParticleDataEntry::setAll(...) Particle Data Scheme
    void ParticleDataEntry::setAntiName(...) Particle Data Scheme
    void ParticleDataEntry::setChargeType(...) Particle Data Scheme
    void ParticleDataEntry::setColType(...) Particle Data Scheme
    void ParticleDataEntry::setDefaults() Particle Data Scheme
    void ParticleDataEntry::setDoExternalDecays(...) Particle Data Scheme
    void ParticleDataEntry::setDoForceWidth(...) Particle Data Scheme
    void ParticleDataEntry::setHasChanged(...) Particle Data Scheme
    void ParticleDataEntry::setIsResonance(...) Particle Data Scheme
    void ParticleDataEntry::setIsVisible(...) Particle Data Scheme
    void ParticleDataEntry::setM0(...) Particle Data Scheme
    void ParticleDataEntry::setMayDecay(...) Particle Data Scheme
    void ParticleDataEntry::setMMax(...) Particle Data Scheme
    void ParticleDataEntry::setMMin(...) Particle Data Scheme
    void ParticleDataEntry::setMWidth(...) Particle Data Scheme
    void ParticleDataEntry::setName(...) Particle Data Scheme
    void ParticleDataEntry::setNames(...) Particle Data Scheme
    void ParticleDataEntry::setResonancePtr(...) Particle Data Scheme
    void ParticleDataEntry::setSpinType(...) Particle Data Scheme
    void ParticleDataEntry::setTau0(...) Particle Data Scheme
    int ParticleDataEntry::sizeChannels() Particle Data Scheme
    int ParticleDataEntry::spinType() Particle Data Scheme
    double ParticleDataEntry::tau0() Particle Data Scheme
    bool ParticleDataEntry::useBreitWigner() Particle Data Scheme
    ParticleDataEntry::~ParticleDataEntry Particle Data Scheme
    void AlpgenPar::void printParams() Alpgen Event Interface
    bool Pythia8ToHepMC::convert_gluon_to_0() HepMC Interface
    bool Pythia8ToHepMC::crash_on_problem() HepMC Interface
    bool Pythia8ToHepMC::fill_next_event(...) HepMC Interface
    bool Pythia8ToHepMC::fill_next_event(...) HepMC Interface
    bool Pythia8ToHepMC::free_parton_warnings() HepMC Interface
    bool Pythia8ToHepMC::print_inconsistency() HepMC Interface
    Pythia8ToHepMC::Pythia8ToHepMC() HepMC Interface
    void Pythia8ToHepMC::set_convert_gluon_to_0(...) HepMC Interface
    void Pythia8ToHepMC::set_crash_on_problem(...) HepMC Interface
    void Pythia8ToHepMC::set_free_parton_warnings(...) HepMC Interface
    void Pythia8ToHepMC::set_print_inconsistency(...) HepMC Interface
    void Pythia8ToHepMC::set_store_pdf(...) HepMC Interface
    void Pythia8ToHepMC::set_store_proc(...) HepMC Interface
    void Pythia8ToHepMC::set_store_xsec(...) HepMC Interface
    bool Pythia8ToHepMC::store_pdf() HepMC Interface
    bool Pythia8ToHepMC::store_proc() HepMC Interface
    bool Pythia8ToHepMC::store_xsec() HepMC Interface
    virtual Pythia8ToHepMC::~Pythia8ToHepMC() HepMC Interface
    CoupSM Pythia::coupSM Program Flow
    Event Pythia::event Program Flow
    bool Pythia::flag(...) Program Flow
    bool Pythia::forceHadronLevel(...) Program Flow
    bool Pythia::forceRHadronDecays() Program Flow
    int Pythia::forceTimeShower(...) Program Flow
    Info Pythia::info Program Flow
    bool Pythia::init() Program Flow
    bool Pythia::init(...) Program Flow
    bool Pythia::init(...) Program Flow
    bool Pythia::init(...) Program Flow
    bool Pythia::init(...) Program Flow
    bool Pythia::init(...) Program Flow
    void Pythia::LHAeventList(...) Program Flow
    bool Pythia::LHAeventSkip(...) Program Flow
    int Pythia::mode(...) Program Flow
    bool Pythia::moreDecays() Program Flow
    bool Pythia::next() Program Flow
    double Pythia::parm(...) Program Flow
    ParticleData Pythia::particleData Program Flow
    PartonSystems Pythia::partonSystems Program Flow
    Event Pythia::process Program Flow
    Pythia::Pythia(...) Program Flow
    bool Pythia::readFile(...) Program Flow
    bool Pythia::readFile(...) Program Flow
    bool Pythia::readFile(...) Program Flow
    bool Pythia::readFile(...) Program Flow
    bool Pythia::readString(...) Program Flow
    Rndm Pythia::rndm Program Flow
    bool Pythia::setBeamShapePtr(...) Program Flow
    bool Pythia::setDecayPtr(...) Program Flow
    bool Pythia::setLHAupPtr(...) Program Flow
    bool Pythia::setPDFPtr(...) Program Flow
    bool Pythia::setResonancePtr(...) Program Flow
    bool Pythia::setRndmEnginePtr(...) Program Flow
    bool Pythia::setShowerPtr(...) Program Flow
    bool Pythia::setSigmaPtr(...) Program Flow
    Settings Pythia::settings Program Flow
    bool Pythia::setUserHooksPtr(...) Program Flow
    SusyLesHouches Pythia::slha Program Flow
    void Pythia::stat() Program Flow
    void Pythia::statistics(...) Program Flow
    void Pythia::statistics(...) Event Statistics
    string Pythia::word(...) Program Flow
    Pythia::~Pythia Program Flow
    bool ResonanceWidths::allowCalc() Semi Internal Resonances
    void ResonanceWidths::calcPreFac(...) Semi Internal Resonances
    void ResonanceWidths::calcWidth(...) Semi Internal Resonances
    bool ResonanceWidths::initBSM() Semi Internal Resonances
    void ResonanceWidths::initConstants() Semi Internal Resonances
    double ResonanceWidths::widthChan(...) Semi Internal Resonances
    bool Rndm::dumpState(...) Random Numbers
    double Rndm::exp() Random Numbers
    double Rndm::flat() Random Numbers
    double Rndm::gauss() Random Numbers
    pair<double, double> Rndm::gauss2() Random Numbers
    void Rndm::init(...) Random Numbers
    int Rndm::pick(...) Random Numbers
    bool Rndm::readState(...) Random Numbers
    Rndm::Rndm() Random Numbers
    Rndm::Rndm(...) Random Numbers
    bool Rndm::rndmEnginePtr(...) Random Numbers
    double Rndm::xexp() Random Numbers
    virtual double RndmEngine::flat() Random Numbers
    void RotBstMatrix::bst(...) Four-Vectors
    void RotBstMatrix::bst(...) Four-Vectors
    void RotBstMatrix::bst(...) Four-Vectors
    void RotBstMatrix::bstback(...) Four-Vectors
    double RotBstMatrix::deviation() Four-Vectors
    void RotBstMatrix::fromCMframe(...) Four-Vectors
    void RotBstMatrix::invert() Four-Vectors
    RotBstMatrix& RotBstMatrix::operator=(...) Four-Vectors
    void RotBstMatrix::reset() Four-Vectors
    void RotBstMatrix::rot(...) Four-Vectors
    void RotBstMatrix::rot(...) Four-Vectors
    void RotBstMatrix::rotbst(...); Four-Vectors
    RotBstMatrix::RotBstMatrix() Four-Vectors
    RotBstMatrix::RotBstMatrix(...) Four-Vectors
    void RotBstMatrix::toCMframe(...) Four-Vectors
    void Settings::addFlag(...) Settings Scheme
    void Settings::addMode(...) Settings Scheme
    void Settings::addMVec(...) Settings Scheme
    void Settings::addParm(...) Settings Scheme
    void Settings::addPVec(...) Settings Scheme
    void Settings::addWord(...) Settings Scheme
    bool Settings::flag(...) Settings Scheme
    void Settings::flag(...) Settings Scheme
    bool Settings::flagDefault(...) Settings Scheme
    void Settings::forceMode(...) Settings Scheme
    void Settings::forceMVec(...) Settings Scheme
    void Settings::forceParm(...) Settings Scheme
    void Settings::forcePVec(...) Settings Scheme
    map Settings::getFlagMap(...) Settings Scheme
    map Settings::getModeMap(...) Settings Scheme
    map Settings::getMVecMap(...) Settings Scheme
    map Settings::getParmMap(...) Settings Scheme
    map Settings::getPVecMap(...) Settings Scheme
    map Settings::getWordMap(...) Settings Scheme
    bool Settings::init(...) Settings Scheme
    bool Settings::initPtr(...) Settings Scheme
    bool Settings::isFlag(...) Settings Scheme
    bool Settings::isMode(...) Settings Scheme
    bool Settings::isMVec(...) Settings Scheme
    bool Settings::isParm(...) Settings Scheme
    bool Settings::isPVec(...) Settings Scheme
    bool Settings::isWord(...) Settings Scheme
    void Settings::list(...) Settings Scheme
    void Settings::listAll(...) Settings Scheme
    void Settings::listChanged(...) Settings Scheme
    int Settings::mode(...) Settings Scheme
    void Settings::mode(...) Settings Scheme
    int Settings::modeDefault(...) Settings Scheme
    vector<int> Settings::mvec(...) Settings Scheme
    void Settings::mvec(...) Settings Scheme
    vector<int> Settings::mvecDefault(...) Settings Scheme
    double Settings::parm(...) Settings Scheme
    void Settings::parm(...) Settings Scheme
    double Settings::parmDefault(...) Settings Scheme
    vector<double> Settings::pvec(...) Settings Scheme
    void Settings::pvec(...) Settings Scheme
    vector<double> Settings::pvecDefault(...) Settings Scheme
    bool Settings::readString(...) Settings Scheme
    bool Settings::reInit(...) Settings Scheme
    void Settings::resetAll() Settings Scheme
    void Settings::resetFlag(...) Settings Scheme
    void Settings::resetMode(...) Settings Scheme
    void Settings::resetMVec(...) Settings Scheme
    void Settings::resetParm(...) Settings Scheme
    void Settings::resetPVec(...) Settings Scheme
    void Settings::resetWord(...) Settings Scheme
    Settings::Settings() Settings Scheme
    string Settings::word(...) Settings Scheme
    void Settings::word(...) Settings Scheme
    string Settings::wordDefault(...) Settings Scheme
    bool Settings::writeFile(...) Settings Scheme
    bool Settings::writeFile(...) Settings Scheme
    int SigmaProcess::code() Semi Internal Processes
    bool SigmaProcess::convert2mb() Semi Internal Processes
    bool SigmaProcess::convertM2() Semi Internal Processes
    int SigmaProcess::gmZmode() Semi Internal Processes
    int SigmaProcess::id3Mass() Semi Internal Processes
    int SigmaProcess::id4Mass() Semi Internal Processes
    int SigmaProcess::id5Mass() Semi Internal Processes
    int SigmaProcess::idSChannel() Semi Internal Processes
    int SigmaProcess::idTchan1() Semi Internal Processes
    int SigmaProcess::idTchan2() Semi Internal Processes
    string SigmaProcess::inFlux() Semi Internal Processes
    void SigmaProcess::initProc() Semi Internal Processes
    int SigmaProcess::isQCD3body() Semi Internal Processes
    bool SigmaProcess::isSChannel() Semi Internal Processes
    string SigmaProcess::name() Semi Internal Processes
    int SigmaProcess::resonanceA() Semi Internal Processes
    int SigmaProcess::resonanceB() Semi Internal Processes
    void SigmaProcess::setIdColAcol() Semi Internal Processes
    bool SigmaProcess::setupForME() Semi Internal Processes
    double SigmaProcess::sigmaHat() Semi Internal Processes
    void SigmaProcess::sigmaKin() Semi Internal Processes
    double SigmaProcess::tChanFracPow1() Semi Internal Processes
    double SigmaProcess::tChanFracPow2() Semi Internal Processes
    bool SigmaProcess::useMirrorWeight() Semi Internal Processes
    double SigmaProcess::weightDecay(...) Semi Internal Processes
    double SigmaProcess::weightDecayFlav(...) Semi Internal Processes
    bool SlowJet::analyze(...) Event Analysis
    vector<int> SlowJet::constituents(...) Event Analysis
    double SlowJet::dNext() Event Analysis
    bool SlowJet::doNSteps(...) Event Analysis
    bool SlowJet::doStep() Event Analysis
    int SlowJet::iNext() Event Analysis
    int SlowJet::jetAssignment(...) Event Analysis
    int SlowJet::jNext() Event Analysis
    void SlowJet::list() Event Analysis
    void SlowJet::list(...) Event Analysis
    double SlowJet::m(...) Event Analysis
    int SlowJet::multiplicity(...) Event Analysis
    Vec4 SlowJet::p(...) Event Analysis
    double SlowJet::phi(...) Event Analysis
    double SlowJet::pT(...) Event Analysis
    void SlowJet::removeJet(...) Event Analysis
    bool SlowJet::setup(...) Event Analysis
    int SlowJet::sizeAll() Event Analysis
    int SlowJet::sizeJet() Event Analysis
    int SlowJet::sizeOrig() Event Analysis
    SlowJet::SlowJet(...) Event Analysis
    bool SlowJet::stopAtN(...) Event Analysis
    double SlowJet::y(...) Event Analysis
    virtual bool SlowJetHook::include(...) Event Analysis
    SlowJetHook::SlowJetHook() Event Analysis
    virtual SlowJetHook::~SlowJetHook() Event Analysis
    virtual bool SpaceShower::branch(...) Implement New Showers
    bool SpaceShower::doRestart() Implement New Showers
    virtual double SpaceShower::enhancePTmax() Implement New Showers
    virtual void SpaceShower::init(...) Implement New Showers
    void SpaceShower::initPtr(...) Implement New Showers
    virtual bool SpaceShower::limitPTmax(...) Implement New Showers
    virtual void SpaceShower::list(...) Implement New Showers
    virtual void SpaceShower::prepare(...) Implement New Showers
    virtual double SpaceShower::pTnext(...) Implement New Showers
    SpaceShower::SpaceShower() Implement New Showers
    int SpaceShower::system() Implement New Showers
    virtual void SpaceShower::update(...) Implement New Showers
    virtual SpaceShower::~SpaceShower() Implement New Showers
    bool Sphericity::analyze(...) Event Analysis
    double Sphericity::aplanarity() Event Analysis
    double Sphericity::eigenValue(...) Event Analysis
    Vec4 Sphericity::eventAxis(...) Event Analysis
    void Sphericity::list(...) Event Analysis
    int Sphericity::nError() Event Analysis
    double Sphericity::sphericity() Event Analysis
    Sphericity::Sphericity(...) Event Analysis
    SuppressSmallPT::SuppressSmallPT(...) User Hooks
    bool Thrust::analyze(...) Event Analysis
    Vec4 Thrust::eventAxis(...) Event Analysis
    void Thrust::list(...) Event Analysis
    int Thrust::nError() Event Analysis
    double Thrust::oblateness() Event Analysis
    double Thrust::thrust() Event Analysis
    Thrust::Thrust(...) Event Analysis
    double Thrust::tMajor() Event Analysis
    double Thrust::tMinor() Event Analysis
    virtual bool TimeShower::branch(...) Implement New Showers
    double TimeShower::enhancePTmax() Implement New Showers
    virtual void TimeShower::init(...) Implement New Showers
    void TimeShower::initPtr(...) Implement New Showers
    virtual bool TimeShower::limitPTmax(...) Implement New Showers
    virtual void TimeShower::list(...) Implement New Showers
    virtual void TimeShower::prepare(...) Implement New Showers
    virtual void TimeShower::prepareGlobal(...) Implement New Showers
    double TimeShower::pTLastInShower() Implement New Showers
    virtual double TimeShower::pTnext(...) Implement New Showers
    virtual bool TimeShower::rescatterPropogateRecoil(...) Implement New Showers
    virtual void TimeShower::rescatterUpdate(...) Implement New Showers
    virtual int TimeShower::shower(...) Implement New Showers
    virtual int TimeShower::showerQED(...) Implement New Showers
    int TimeShower::system() Implement New Showers
    TimeShower::TimeShower() Implement New Showers
    virtual void TimeShower::update(...) Implement New Showers
    virtual TimeShower::~TimeShower() Implement New Showers
    virtual double UserHooks::biasedSelectionWeight() User Hooks
    virtual double UserHooks::biasSelectionBy(...) User Hooks
    virtual bool UserHooks::canBiasSelection() User Hooks
    virtual bool UserHooks::canModifySigma() User Hooks
    virtual bool UserHooks::canSetResonanceScale() User Hooks
    virtual bool UserHooks::canVetoFSREmission() User Hooks
    virtual bool UserHooks::canVetoISREmission() User Hooks
    virtual bool UserHooks::canVetoMPIEmission() User Hooks
    virtual bool UserHooks::canVetoMPIStep() User Hooks
    virtual bool UserHooks::canVetoPartonLevel() User Hooks
    virtual bool UserHooks::canVetoPartonLevelEarly() User Hooks
    virtual bool UserHooks::canVetoProcessLevel() User Hooks
    virtual bool UserHooks::canVetoPT() User Hooks
    virtual bool UserHooks::canVetoResonanceDecays() User Hooks
    virtual bool UserHooks::canVetoStep() User Hooks
    virtual bool UserHooks::doVetoFSREmission(...) User Hooks
    virtual bool UserHooks::doVetoISREmission(...) User Hooks
    virtual bool UserHooks::doVetoMPIEmission(...) User Hooks
    virtual bool UserHooks::doVetoMPIStep(...) User Hooks
    virtual bool UserHooks::doVetoPartonLevel(...) User Hooks
    virtual bool UserHooks::doVetoPartonLevelEarly(...) User Hooks
    virtual bool UserHooks::doVetoProcessLevel(...) User Hooks
    virtual bool UserHooks::doVetoPT(...) User Hooks
    virtual bool UserHooks::doVetoResonanceDecays(...) User Hooks
    virtual bool UserHooks::doVetoStep(...) User Hooks
    virtual bool UserHooks::initAfterBeams() User Hooks
    void UserHooks::initPtr(...) User Hooks
    virtual double UserHooks::multiplySigmaBy(...) User Hooks
    virtual int UserHooks::numberVetoMPIStep() User Hooks
    virtual int UserHooks::numberVetoStep() User Hooks
    void UserHooks::omitResonanceDecays(...) User Hooks
    virtual double UserHooks::scaleResonance(...) User Hooks
    virtual double UserHooks::scaleVetoPT() User Hooks
    void UserHooks::subEvent(...) User Hooks
    UserHooks::UserHooks() User Hooks
    Event UserHooks::workEvent User Hooks
    virtual UserHooks::~UserHooks() User Hooks
    void Vec4::bst(...) Four-Vectors
    void Vec4::bst(...) Four-Vectors
    void Vec4::bst(...) Four-Vectors
    void Vec4::bst(...) Four-Vectors
    void Vec4::bstback(...) Four-Vectors
    void Vec4::bstback(...) Four-Vectors
    double Vec4::e() Four-Vectors
    void Vec4::e(...) Four-Vectors
    double Vec4::eT() Four-Vectors
    double Vec4::eT2() Four-Vectors
    double Vec4::eta() Four-Vectors
    void Vec4::flip3() Four-Vectors
    void Vec4::flip4() Four-Vectors
    double Vec4::m2Calc() Four-Vectors
    double Vec4::mCalc() Four-Vectors
    Vec4& Vec4::operator*=(...) Four-Vectors
    Vec4& Vec4::operator+=(...) Four-Vectors
    Vec4 Vec4::operator-() Four-Vectors
    Vec4& Vec4::operator-=(...) Four-Vectors
    Vec4& Vec4::operator/=(...) Four-Vectors
    Vec4& Vec4::operator=(...) Four-Vectors
    Vec4& Vec4::operator=(...) Four-Vectors
    void Vec4::p(...) Four-Vectors
    void Vec4::p(...) Four-Vectors
    double Vec4::pAbs() Four-Vectors
    double Vec4::pAbs2() Four-Vectors
    double Vec4::phi() Four-Vectors
    double Vec4::pNeg() Four-Vectors
    double Vec4::pPos() Four-Vectors
    double Vec4::pT() Four-Vectors
    double Vec4::pT2() Four-Vectors
    double Vec4::px() Four-Vectors
    void Vec4::px(...) Four-Vectors
    double Vec4::py() Four-Vectors
    void Vec4::py(...) Four-Vectors
    double Vec4::pz() Four-Vectors
    void Vec4::pz(...) Four-Vectors
    double Vec4::rap() Four-Vectors
    void Vec4::rescale3(...) Four-Vectors
    void Vec4::rescale4(...) Four-Vectors
    void Vec4::reset() Four-Vectors
    void Vec4::rot(...) Four-Vectors
    void Vec4::rotaxis(...) Four-Vectors
    void Vec4::rotaxis(...) Four-Vectors
    void Vec4::rotbst(...) Four-Vectors
    double Vec4::theta() Four-Vectors
    double Vec4::thetaXZ() Four-Vectors
    Vec4::Vec4(...) Four-Vectors
    Vec4::Vec4(...) Four-Vectors
    pythia8-8.1.80.orig/htmldoc/RIVETusage.html0000644000175000017500000000565112217615312016576 0ustar sunsun RIVET usage

    RIVET usage

    RIVET is a toolkit for the validation of Monte Carlo event generators [Buc10]. It contains the results of many experimental analyses, so that generator output can easily be compared to data, as well as providing a framework to implement your own analyses. Although using PYTHIA with RIVET is not officially supported, some helpful hints are given below. The full RIVET manual is available online.

    Using PYTHIA with RIVET

    The following assumes that you already have RIVET installed. Instructions for this may be found here.

    Events are passed from PYTHIA to RIVET using the HepMC format. PYTHIA must be compiled with HepMC support, using the same version of HepMC used when compiling RIVET. This is setup through the PYTHIA configure script e.g.
      ./configure --with-hepmc=/path/to/HepMC --with-hepmcversion=HepMC.version.number
    
    The PYTHIA library itself does not need to be recompiled.

    The examples/main42.cc sample program can then be used to generate events in HepMC format (which examples/main61.cc and examples/main62.cc extends by allowing LHAPDF usage and subruns). When in the examples directory, the main program can be built and used as follows
      make main42
      ./main42 main42.cmnd main42.hepmc
    
    The first argument is the input file which provides the options for event generation, while the second is the output file where the HepMC events should be written.

    This HepMC file may now be read and processed by RIVET
      rivet --analysis=ANALYSIS_NAME main42.hepmc
    
    where ANALYSIS_NAME is a built-in RIVET analysis, or one you have created yourself. The output of RIVET is in the form of .aida files, containing the histograms for the analysis, which can be processed further with RIVET (see the RIVET documentation for more details).

    The above examples requires that (potentially large) HepMC events are stored to disk before being read by RIVET. It is possible, instead, to pass the events directly to RIVET as they are produced by using a FIFO pipe. This is done with the mkfifo command
      mkfifo my_fifo
      ./main42.exe main42.cmnd my_fifo &
      rivet --analysis=ANALYSIS_NAME my_fifo
    
    Note that main42 is run in the background. pythia8-8.1.80.orig/htmldoc/Version.html0000644000175000017500000000150612217615312016300 0ustar sunsun Version

    Version

    The settings on this page should not be changed by the ordinary user, but appear here for documentation purposes, and so that they can form part of the standard databases and be queried accordingly.

    parm  Pythia:versionNumber   (default = 8.180)
    Version and subversion number, with three significant decimals.

    mode  Pythia:versionDate   (default = 20130922)
    Last date of change of current (sub)version, in format yyyymmdd. pythia8-8.1.80.orig/Makefile0000644000175000017500000001650712217346232014004 0ustar sunsun# # Libraries Makefile. Some ideas from Geant4 Makefiles # # M. Kirsanov 07.04.2006 # Modified 18.11.2006 # 26.03.2008 CLHEP dependency removed # N. Lavesson 28.04.2009 clean/distclean separated # M. Kirsanov 21.07.2009 Mac-OSX flags added .PHONY: all install installit installmain installdata clean distclean SHELL = /bin/sh -include config.mk # flags: # #FFLAGSSHARED = -fPIC CFLAGSSHARED = -fPIC CXXFLAGSSHARED = -fPIC HEPMCERROR= ifneq (x$(HEPMCLOCATION),x) ifeq ($(wildcard $(HEPMCLOCATION)/include/HepMC/*.h),) HEPMCERROR= HepMC interface: ERROR, no HepMC headers found in ${HEPMCLOCATION}/include/HepMC endif endif # Location of directories. MYTMPDIR=tmp TOPDIR=$(shell \pwd) INCDIR=include SRCDIR=src LIBDIR=lib LIBDIRARCH=lib/archive BINDIR=bin # Location of libraries to be built. ifeq ($(SHAREDLIBS),yes) targets=$(LIBDIRARCH)/libpythia8.a targets+=$(LIBDIR)/libpythia8.$(SHAREDSUFFIX) targets+=$(LIBDIRARCH)/liblhapdfdummy.a targets+=$(LIBDIR)/liblhapdfdummy.$(SHAREDSUFFIX) else targets=$(LIBDIRARCH)/libpythia8.a targets+=$(LIBDIRARCH)/liblhapdfdummy.a endif ifneq (x$(HEPMCLOCATION),x) targets+=$(LIBDIRARCH)/libpythia8tohepmc.a ifeq ($(SHAREDLIBS),yes) targets+=$(LIBDIR)/libpythia8tohepmc.$(SHAREDSUFFIX) endif endif all: $(targets) config.mk # This default run of configure should only happen if configure # has not already been explicitly run. config.mk: ./configure # Main part: build Pythia8 library. $(MYTMPDIR)/%.o : $(SRCDIR)/%.cc @mkdir -p $(MYTMPDIR) $(CXX) $(CXXFLAGS) $(CXXFLAGSSHARED) -c -I$(INCDIR) $< -o $@ $(MYTMPDIR)/archive/%.o : $(SRCDIR)/%.cc @mkdir -p $(MYTMPDIR)/archive $(CXX) $(CXXFLAGS) -c -I$(INCDIR) $< -o $@ $(MYTMPDIR)/%.o : lhapdfdummy/%.cc @mkdir -p $(MYTMPDIR) $(CXX) $(CXXFLAGS) $(CXXFLAGSSHARED) -c -I$(INCDIR) $< -o $@ $(MYTMPDIR)/archive/%.o : lhapdfdummy/%.cc @mkdir -p $(MYTMPDIR)/archive $(CXX) $(CXXFLAGS) -c -I$(INCDIR) $< -o $@ # Creating the dependency files *.d # The compiler with option -M is used to build the dependency strings. They # are further edited with sed (stream editor). The first sed command adds the # dependency for the *.d files themselves, the second one is needed because # object files are put in the directory different from src. The last line # removes empty *.d files produced in case of error. ifeq ($(SHAREDLIBS),yes) $(MYTMPDIR)/%.d : $(SRCDIR)/%.cc @echo Making dependency for file $<; \ mkdir -p $(MYTMPDIR); \ $(CC) -M -I$(INCDIR) $< | \ sed 's,\($*\)\.o[ :]*,\1.o $@ : ,g' | \ sed 's/$*\.o/$(MYTMPDIR)\/$*.o/' > $@; \ [ -s $@ ] || rm -f $@ endif $(MYTMPDIR)/archive/%.d : $(SRCDIR)/%.cc @echo Making dependency for file $<; \ mkdir -p $(MYTMPDIR)/archive; \ $(CC) -M -I$(INCDIR) $< | \ sed 's,\($*\)\.o[ :]*,\1.o $@ : ,g' | \ sed 's/$*\.o/$(MYTMPDIR)\/archive\/$*.o/' > $@; \ [ -s $@ ] || rm -f $@ objects := $(patsubst $(SRCDIR)/%.cc,$(MYTMPDIR)/%.o,$(wildcard $(SRCDIR)/*.cc)) objectsarch := $(patsubst $(SRCDIR)/%.cc,$(MYTMPDIR)/archive/%.o,$(wildcard $(SRCDIR)/*.cc)) $(LIBDIR)/libpythia8.$(SHAREDSUFFIX): $(objects) @mkdir -p $(LIBDIR) $(CXX) $(LDFLAGSSHARED) -o $@ $(objects) $(LDFLAGLIBNAME),$(notdir $@) $(LIBDIRARCH)/libpythia8.a: $(objectsarch) @mkdir -p $(LIBDIRARCH) ar cru $@ $(objectsarch) objdum := $(patsubst lhapdfdummy/%.cc,$(MYTMPDIR)/%.o,$(wildcard lhapdfdummy/*.cc)) objdumarch := $(patsubst lhapdfdummy/%.cc,$(MYTMPDIR)/archive/%.o,$(wildcard lhapdfdummy/*.cc)) $(LIBDIR)/liblhapdfdummy.$(SHAREDSUFFIX): $(objdum) @mkdir -p $(LIBDIR) $(CXX) $(LDFLAGSSHARED) -o $@ $(objdum) $(LDFLAGLIBNAME),$(notdir $@) $(LIBDIRARCH)/liblhapdfdummy.a: $(objdumarch) @mkdir -p $(LIBDIRARCH) ar cru $@ $(objdumarch) deps := $(patsubst $(SRCDIR)/%.cc,$(MYTMPDIR)/%.d,$(wildcard $(SRCDIR)/*.cc)) depsarch := $(patsubst $(SRCDIR)/%.cc,$(MYTMPDIR)/archive/%.d,$(wildcard $(SRCDIR)/*.cc)) # The "if" below is needed in order to avoid producing the dependency files # when you want to just clean ifeq (,$(findstring clean, $(MAKECMDGOALS))) -include $(deps) -include $(depsarch) endif # Build HepMC interface part if HepMC location is set. ifneq (x$(HEPMCLOCATION),x) HEPMCINCLUDE=-I$(HEPMCLOCATION)/include ifeq (x$(HEPMCERROR),x) $(MYTMPDIR)/%.o : pythia8tohepmc/%.cc config.mk @mkdir -p $(MYTMPDIR) $(CXX) $(CXXFLAGS) $(CXXFLAGSSHARED) $(HEPMCVFLAG) -c -I$(INCDIR) $(HEPMCINCLUDE) $< -o $@ $(MYTMPDIR)/archive/%.o : pythia8tohepmc/%.cc config.mk @mkdir -p $(MYTMPDIR)/archive $(CXX) $(CXXFLAGS) $(HEPMCVFLAG) -c -I$(INCDIR) $(HEPMCINCLUDE) $< -o $@ $(MYTMPDIR)/%.d : pythia8tohepmc/%.cc @echo Making dependency for file $<; \ mkdir -p $(MYTMPDIR); \ $(CC) -M -I$(INCDIR) $(HEPMCINCLUDE) $< | \ sed 's,\($*\)\.o[ :]*,\1.o $@ : ,g' | \ sed 's/$*.o/$(MYTMPDIR)\/$*.o/' > $@; \ [ -s $@ ] || rm -f $@ $(MYTMPDIR)/archive/%.d : pythia8tohepmc/%.cc @echo Making dependency for file $<; \ mkdir -p $(MYTMPDIR)/archive; \ $(CC) -M -I$(INCDIR) $(HEPMCINCLUDE) $< | \ sed 's,\($*\)\.o[ :]*,\1.o $@ : ,g' | \ sed 's/$*.o/$(MYTMPDIR)\/archive\/$*.o/' > $@; \ [ -s $@ ] || rm -f $@ objectsI := $(patsubst pythia8tohepmc/%.cc,$(MYTMPDIR)/%.o,$(wildcard pythia8tohepmc/*.cc)) objectsIarch := $(patsubst pythia8tohepmc/%.cc,$(MYTMPDIR)/archive/%.o,$(wildcard pythia8tohepmc/*.cc)) $(LIBDIR)/libpythia8tohepmc.$(SHAREDSUFFIX) : $(objectsI) @mkdir -p $(LIBDIR) $(CXX) $(LDFLAGSSHARED) $(objectsI) -o $@ $(LDFLAGLIBNAME),$(notdir $@) $(LIBDIRARCH)/libpythia8tohepmc.a : $(objectsIarch) @mkdir -p $(LIBDIRARCH) ar cru $(LIBDIRARCH)/libpythia8tohepmc.a $(objectsIarch) depsI := $(patsubst pythia8tohepmc/%.cc,$(MYTMPDIR)/%.d,$(wildcard pythia8tohepmc/*.cc)) depsIarch := $(patsubst pythia8tohepmc/%.cc,$(MYTMPDIR)/archive/%.d,$(wildcard pythia8tohepmc/*.cc)) ifeq (,$(findstring clean, $(MAKECMDGOALS))) -include $(depsI) -include $(depsIarch) endif else $(LIBDIRARCH)/libpythia8tohepmc.a $(LIBDIR)/libpythia8tohepmc.$(SHAREDSUFFIX) : @echo $(HEPMCERROR) endif endif # Install targets: ifneq (x$(INSTALLDIR),x.) install: all mkdir -p $(INSTALLDIR) mkdir -p $(INSTALLDIR)/bin mkdir -p $(DATADIR) make installit installit: installmain installdata installmain: cp -r include $(INSTALLDIR)/. cp -r lib $(INSTALLDIR)/. cp -p config.mk $(INSTALLDIR)/. cp -p bin/pythia8-config $(INSTALLDIR)/bin/ ifneq ($(DATADIR),$(INSTALLDIR)) installdata: rm -rf $(DATADIR)/xmldoc rm -f $(INSTALLDIR)/xmldoc cp -r *doc $(DATADIR)/. ln -fs $(DATADIR)/xmldoc $(INSTALLDIR)/xmldoc else installdata: rm -rf $(INSTALLDIR)/xmldoc cp -r xmldoc $(INSTALLDIR)/. endif else install: all @echo "everything is already installed" endif # Clean up: remove (almost?) everything that cannot be recreated. clean: rm -rf $(MYTMPDIR) rm -rf $(LIBDIR) rm -rf $(BINDIR)/*.exe cd examples; rm -rf bin; rm -f *.exe; cd - cd rootexamples; rm -f *.exe; cd - distclean: clean rm -f config.mk rm -f *~; rm -f \#*; rm -rf $(BINDIR) cd $(SRCDIR); rm -f *~; rm -f \#*; cd - cd $(INCDIR)/Pythia8; rm -f *~; rm -f \#*; cd - cd xmldoc; rm -f *~; rm -f \#*; cd - cd htmldoc; rm -f *~; rm -f \#*; cd - cd phpdoc; rm -f *~; rm -f \#*; cd - cd pythia8tohepmc; rm -f *~; rm -f \#*; cd - cd lhapdfdummy; rm -f *~; rm -f \#*; cd - cd examples; rm -f *~; rm -f \#*; rm -f core*; rm -f config.*; cd - cd rootexamples; rm -f *~; rm -f \#*; rm -f core*; rm -f config.*; cd - pythia8-8.1.80.orig/xmldoc/0000755000175000017500000000000012217615455013627 5ustar sunsunpythia8-8.1.80.orig/xmldoc/Version.xml0000444000175000017500000000106512217615154015772 0ustar sunsun

    Version

    The settings on this page should not be changed by the ordinary user, but appear here for documentation purposes, and so that they can form part of the standard databases and be queried accordingly. Version and subversion number, with three significant decimals. Last date of change of current (sub)version, in format yyyymmdd. pythia8-8.1.80.orig/xmldoc/SampleMainPrograms.xml0000444000175000017500000003675512217346317020126 0ustar sunsun

    Sample Main Programs

    Descriptions of available classes, methods and settings are all very good and useful. Ultimately they are necessary for you to be able to fine-tune your runs to the task at hand. To get going, however, nothing helps like having explicit examples to study. This is what is provided in the examples subdirectory, along with instructions how they should be run:
    • main00.cc : does not exist, but it has been defined in the Makefile, so this name could be used for a simple first test run.
    • main01.cc : a simple study of the charged multiplicity for jet events at the LHC. (Brief example fitting on one slide.)
    • main02.cc : a simple study of the pT spectrum of Z bosons at the Tevatron. (Brief example fitting on one slide.)
    • main03.cc : a simple study of several different kinds of events, with the choice to be made in the main03.cmnd "cards file".
    • main04.cc : tests of cross sections, multiplicities and average transverse momenta for elastic, diffractive and nondiffractive topologies, using main04.cmnd to pick processes.
    • main05.cc : generation of QCD jet events at the LHC, with jet analysis using the SlowJet inclusive anti-kT sequential-recombination finder and the CellJet cone-jet finder.
    • main06.cc : generation of LEP1 hadronic events, i.e. e^+e^- -> gamma*/Z^0 -> q qbar, with charged multiplicity, sphericity, thrust and jet analysis.
    • main07.cc : set up a fictitious production process to a generic resonance, where you easily can compose your own list of (two-body) decay modes to a variety of final states. Also traces decay chains down to truly stable particles: gamma, e+-, p/pbar and neutrinos. Suitable for astroparticle applications, like neutralino pair annihilation, where cross sections are calculated separately in another program.
    • main08.cc : generation of the QCD jet cross section biased towards higher pT values, by two different techniques. Firstly, by splitting the run into subruns, each in its own pT bin, and adding the results properly reweighted. Two suboptions, with limits set either in the main program or by subrun specification in the main08.cmnd file. Secondly, by a continuous reweighting with a pT^4 bias in the selection, compensated by a 1/pT^4 event weight. Also inclusion of soft processes is illustrated, with subruns and weighted events.
    • main09.cc : generation of two predetermined hard interactions in each event.
    • main10.cc : illustration how userHooks can be used interact directly with the event-generation process.
    • main11.cc : a study of top events, fed in from the Les Houches Event File ttbar.lhe, here generated by PYTHIA 6.4. This file currently only contains 100 events so as not to make the distributed PYTHIA package too big, and so serves mainly as a demonstration of the principles involved.
    • main12.cc : a more sophisticated variant of main11.cc, where two Les Houches Event Files (ttbar.lhe and ttbar2.lhe) successively are used as input. Also illustrating some other aspects, like the capability to mix in internally generated events.
    • main13.cc : a streamlined version of main12.cc, where two Les Houches Event Files (ttbar.lhe and ttbar2.lhe) successively are used as input in main13.cmnd file.
    • main14.cc : a systematic comparison of several cross section values with their corresponding values in PYTHIA 6.4, the latter available as a table in the code.
    • main15.cc : loop over several tries, either to redo B decays only or to redo the complete hadronization chain of an event. Since much of the generation process is only made once this is a way to increase efficiency.
    • main16.cc : put all user analysis code into a class of its own, separate from the main program; provide the "cards file" name as a command-line argument. Also exemplifies how Higgs mass, width and branching ratios can be set by hand.
    • main17.cc : shows (a) how to use UserHooks to regularize onium cross section for pT -> 0, and (b) how decays could be handled externally.
    • main18.cc : shows how to write an event filter class, where you keep a vector of pointers to the subset of particles you want to study further. The event record itself remains unchanged.
    • main19.cc : use several instances of Pythia, one for signal events and others for a variable number of pileup and "beam-gas" events, combined into one common event record.
    • main20.cc : shows how PYTHIA 8 can write a Les Houches Event File, using facilities potentially useful also for other programs to write an LHEF.
    • main21.cc : an example how a single particle or various parton-level configurations can be input directly for hadronization, without being tied to the full process-generation machinery, e.g. to study the hadronization of junction topologies. Can also be used for single-resonance decays, with showers.
    • main22.cc : shows how an external resonance can be implemented as a new class derived from a PYTHIA base class, and be used in an external process, both of them handed in for generation as with normal internal classes.
    • main23.cc : shows how an external beam momentum spread and vertex location generator can be implemented as a new class derived from a PYTHIA base class, and then handed in for internal use. Also how to use an external random-number generator and an external parton distribution set.
    • main24.cc : tests of internally implemented cross sections for Supersymmetric particle production, with SUSY spectrum defined in cmssm.spc and settings in main24.cmnd. For illustration, an alternative example spectrum is also available, sps1aWithDecays.spc, which contains a decay table in SLHA format.
    • main25.cc : input RPV-SUSY events from an LHEF file that contains an SLHA spectrum inside its header. The event file, main25.lhe, contains a sample events that illustrate how to arrange color tags in the presence of the color-space epsilon tensors that accompany baryon number violating event topologies.
    • main26.cc : test program for processes in scenarios with large extra dimensions or unparticles.
    • main27.cc : production of Kaluza-Klein gamma/Z states in TeV-sized extra dimensions.
    • main28.cc : production of long-lived R-hadrons, that are forced to decay at a separate vertices and possibly with changed momenta.
    • main31.cc : exemplifies an improved matching of parton showers to LHEF-style input based on the POWHEG approach. The main31.cmnd allows to switch between several different matching options. It also allows to select input process, in this case either for the POWHEG-hvq program applied to top pair production Cor10 or for QCD 2+3-jet events. The small samples of input events are stored in the powheg-hvq.lhe and powheg-dijets.lhe files, respectively.
    • main32.cc : exemplifies MLM merging, either in the ALPGEN variant or in the Madgraph one, and with input events either from ALPGEN or from Madgraph, with relevant control cards stored in main32.cmnd. See Jet Matching for further details. Traditionally the ALPGEN output is split into one file with events and another with parameters and cross sections (unlike in LHEF). Here a sample of W + 3 jets events is stored in main32.unw and the parameters to go with it in main32_unw.par. Madgraph events are taken from the w+_production_lhc_2.lhe file in this case.
    • main41.cc : similar to main01, except that the event record is output in the HepMC event record format. Requires that HepMC is properly linked. Note that the hepmcout41.dat output file can become quite big; so no example is included in this distribution.
    • main42.cc : a streamlined version for the generation of events that are then stored in HepMC format, without any event analysis. That is, all physics studies will have to be done afterwards. The name of the input "cards file" (e.g. main42.cmnd) and output HepMC event file (e.g. hepmcout42.dat) are to be provided as command-line arguments. Requires that HepMC is properly linked. Note that the HepMC output file can become quite big; so no example is included in this distribution.
    • main46.cc : illustrates how to write a ProMC file with PYTHIA events. Note that this example cannot (yet) be built by the PYTHIA Makefile, but a relevant Makefile is available on the ProMC webpage http://atlaswww.hep.anl.gov/asc/promc/.
    • main51.cc : a test of the shape of parton densities, as a check prior to using a given PDF set in a generator. Requires that LHAPDF is properly linked.
    • main52.cc : compares the charged multiplicity distribution, and a few other minimum-bias physics aspects, between default PYTHIA PDF and another one. Requires that LHAPDF is properly linked.
    • main53.cc : tests the possibility to do backwards evolution from an incoming photon at the hard interaction. Requires that you link to a LHAPDF set that includes the photon PDF.
    • main61.cc : a streamlined version for the generation of events that are then stored in HepMC format, without any event analysis. That is, just like main42.cc, with the difference that main61.cc can be used in conjunction with LHAPDF. The name of the input "cards file" (e.g. main61.cmnd) and output HepMC event file (e.g. hepmcout61.dat) are to be provided as command-line arguments. Requires that HepMC and LHAPDF are properly linked. Note that the HepMC output file can become quite big; so no example is included in this distribution.
    • main62.cc : a further extension of main61.cc, where subruns are used to process several consecutive LHEF, as in main13.cc, with information stored e.g in main62.cmnd. Other comments as for main61.cc.
    • main71.cc : an example how the FastJet jet finding package can be linked to allow an analysis of the final state, in this case for a study of W + jet production.
    • main72.cc : a comparison of SlowJet and FastJet jet finding, showing that they find the same jets if run under identical conditions, in this case for QCD jets.
    • main81.cc : do CKKW-L merging with a merging scale defined in kT. Input is provided by the main81.cmnd file and the three data files w+_production_lhc_0.lhe, w+_production_lhc_1.lhe and w+_production_lhc_2.lhe.
    • main82.cc : do CKKW-L merging with a user-defined merging scale function. Input is provided by the main82.cmnd file and the three data files w+_production_lhc_0.lhe, w+_production_lhc_1.lhe and w+_production_lhc_2.lhe.
    • main83.cc : as main82.cc but with an additional cut on the lowest multiplicity allowed for the reclustered state. The same input as for main82.cc can be used.
    • main84.cc : do CKKW-L merging with output in such a way that it can be used in subsequent RIVET analyses. Input is provided by the main84.cmnd file and the three data files w+_production_lhc_0.lhe, w+_production_lhc_1.lhe and w+_production_lhc_2.lhe.
    • main85.cc : do CKKW-L merging, with HepMC event output. Input settings are provided by the main85.cmnd file. This example program allows the use of input Les Houches events that are regularised with only very minimal cuts, and on which Pythia itself should enforce the more restrictive merging scale cut. The example program can be used with the input files w_production_tree_0.lhe, w_production_tree_1.lhe and w_production_tree_2.lhe.
    • main86.cc : do unitarised ME+PS (UMEPS) merging, with HepMC event output. Input settings are provided by the main86.cmnd file. This example program allows the consistent use of input Les Houches events that are regularised with only very minimal cuts, similar to main85.cc. The example program can be used with the input files w_production_tree_0.lhe, w_production_tree_1.lhe and w_production_tree_2.lhe. The program will produce positively and negatively weighted events. See UMEPS Merging for further details.
    • main87.cc : do NL3 NLO merging, with inclusive NLO input, and with HepMC event output. Input settings are provided by the main87.cmnd file. This example program allows the consistent use of input Les Houches events that are regularised with only very minimal cuts, similar to main85.cc. The example program can be used with the tree-level input files w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and the inclusive POWHEG input files w_production_powheg_0.lhe, w_production_powheg_1.lhe. The program will produce positively and negatively weighted events. See NLO Merging (NL3 section) for further details.
    • main88.cc : do unitarised NLO+PS (UNLOPS) merging, with inclusive NLO input, and with HepMC event output. Input settings are provided by the main88.cmnd file. This example program allows the consistent use of input Les Houches events that are regularised with only very minimal cuts, similar to main85.cc. The example program can be used with the tree-level input files w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and the inclusive POWHEG input files w_production_powheg_0.lhe, w_production_powheg_1.lhe. The program will produce positively and negatively weighted events. See NLO Merging (UNLOPS section) for further details.
    In addition two main program illustrating the use of ROOT are available in the rootexamples subdirectory:
    • hist.cc : shows how ROOT can be used for histogramming in a program that for the rest is structured like a normal PYTHIA run.
    • tree.cc : shows how PYTHIA events can be stored as ROOT trees.
    This subdirectory also contains a special Makefile and related documentation.
    pythia8-8.1.80.orig/xmldoc/Frontpage.xml0000444000175000017500000001516212217346303016272 0ustar sunsun

    PYTHIA 8

    Welcome to PYTHIA - The Lund Monte Carlo!

    PYTHIA 8 is the successor to PYTHIA 6, rewritten from scratch in C++. With the release of PYTHIA 8.1 it now becomes the official "current" PYTHIA version, although PYTHIA 6.4 will be supported in parallel with it for some time to come. Specifically, the new version has not yet been enough tested and tuned for it to have reached the same level of reliability as the older one. This testing will only happen if people begin to work with the program, however, which is why we encourage a gradual transition to the new version, starting now. There are some new physics features in PYTHIA 8.1, that would make use of it more attractive, but also some topics still missing, where 6.4 would have to be used. Further, many obsolete features will not be carried over, so for some backwards compatibility studies again 6.4 would be the choice.

    Documentation

    On these webpages you will find the up-to-date manual for PYTHIA 8.1. Use the left-hand index to navigate this documentation of program elements, especially of all possible program settings. All parameters are provided with sensible default values, however, so you need only change those of relevance to your particular study, such as choice of beams, processes and phase space cuts. The pages also contain a fairly extensive survey of all methods available to the user, e.g. to study the produced events. What is lacking on these webpages is an overview, on the one hand, and an in-depth physics description, on the other.

    The overview can be found in the attached PDF file
    A Brief Introduction to PYTHIA 8.1
    T. Sjöstrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 852 [arXiv:0710.3820].
    You are strongly recommended to read this summary when you start out to learn how to use PYTHIA 8.1. Note that some details have changed since the 8.100 version described there.

    For the physics description we refer to the complete
    PYTHIA 6.4 Physics and Manual
    T. Sjöstrand, S. Mrenna and P. Skands, JHEP05 (2006) 026,
    which in detail describes the physics (largely) implemented also in PYTHIA 8, and also provides a more extensive bibliography than found here.

    When you use PYTHIA 8.1, you should therefore cite both, e.g. like
    T. Sjöstrand, S. Mrenna and P. Skands, JHEP05 (2006) 026, Comput. Phys. Comm. 178 (2008) 852.

    Furthermore, a separate
    PYTHIA 8 Worksheet,
    also an attached PDF file, offers a practical introduction to using the generator. It has been developed for and used at a few summer schools, with minor variations, but is also suited for self-study.

    Authors

    Torbjörn Sjöstrand
    Department of Astronomy and Theoretical Physics, Lund University, Sölvegatan 14A, SE-223 62 Lund, Sweden
    phone: + 46 - 46 - 222 48 16, e-mail: torbjorn@thep.lu.se

    Jesper Roy Christiansen
    Department of Astronomy and Theoretical Physics, Lund University, Sölvegatan 14A, SE-223 62 Lund, Sweden
    e-mail: Jesper.Roy.Christiansen@thep.lu.se

    Nishita Desai
    Department of Physics and Astronomy, University College London, Gower Street, London, WC1E 6BT, United Kingdom
    e-mail: Nishita.Desai@cern.ch

    Philip Ilten
    School of Physics, University College Dublin, Belfield, Dublin 4, Ireland
    e-mail: philten@cern.ch

    Stephen Mrenna
    Computing Division, Simulations Group, Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA
    phone: + 1 - 630 - 840 - 2556, e-mail: mrenna@fnal.gov

    Stefan Prestel
    Theory Group, DESY, Notkestrasse 85, D-22607 Hamburg, Germany
    phone: + 49 - 40 - 8998-4250, e-mail: stefan.prestel@thep.lu.se

    Peter Skands
    Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland
    phone: + 41 - 22 - 767 2447, e-mail: peter.skands@cern.ch

    Former authors

    Stefan Ask, e-mail: ask.stefan@gmail.com

    Richard Corke, e-mail: r.corke@errno.net

    Further contributions

    Makefiles, configure scripts and HepMC interface by Mikhail Kirsanov.
    Conversion of XML files to PHP ones by Ben Lloyd.
    Simple Makefile for Win32/NMAKE by Bertrand Bellenot.
    Extended Higgs sector partly implemented by Marc Montull.
    Parts of charm and bottom decay tables courtesy DELPHI and LHCb collaborations.
    Tunes and comparisons with data, based on Rivet and Professor, by Hendrik Hoeth.
    Text and code on the use of ROOT in conjunction with PYTHIA by Rene Brun, Andreas Morsch and Axel Naumann.
    Code and data for MRST/MSTW PDFs by Robert Thorne and Graeme Watt.
    Code and data for the CTEQ/CT PDFs by Joey Huston and colleagues.
    Help with implementing new proton PDFs by Tomas Kasemets.
    Code and data for Pomeron PDFs by H1 collaboration and especially Paul Newman.
    Help with implementing new Pomeron fluxes and PDFs by Sparsh Navin.
    The new Hidden Valley code developed together with Lisa Carloni.
    Code for a Kaluza-Klein electroweak gauge boson provided by Noam Hod and Mark Sutton.
    Code for equivalent photon flux around an unresolved proton by Oystein Alvestad.
    The MBR diffractive model and central diffraction by Robert Ciesielski.
    2012 branching ratios for most light hadrons, and the tau lepton, by Anil Pratap Singh.
    The pythia8-config script has been contributed by Andy Buckley, along with many other helpful suggestions.
    Code and data for several of the NNPDF2.3 QCD+QED sets provided by Juan Rojo and Stefano Carrazza.
    The fjcore code from FastJet provided by Matteo Cacciari, Gavin Salam and Gregory Soyez.
    Note: in several cases modifications have been made to the original code, in order to integrate it with PYTHIA. In these cases the blame for any mistakes has to rest with the regular authors.

    Licence

    PYTHIA 8 is licensed under the GNU General Public Licence version 2.
    Please respect the MCnet Guidelines for Event Generator Authors and Users.

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    MadGraph 5 Processes

    By far the easiest way to implement new processes into PYTHIA 8 is by using the matrix-element generator MadGraph 5. This program has an option to output the results of a matrix-element calculation as a set of PYTHIA 8 C++ classes (plus further auxiliary code), that can then be linked and used as semi-internal processes, meaning they are handled identically with normal internal ones. This way, MadGraph 5 can be used to implement processes from any model that can be written in terms of a Lagrangian. Any 2 -> 1, 2 -> 2 and 2 -> 3 processes can be implemented, the limit being set by the absence of efficient phase space generator algorithms for higher multiplicities in PYTHIA. Features such as s-channel resonances are automatically implemented in the process classes. Besides the process library and necessary model files, also an example main program is generated for each set of processes, which can be easily modified to perform the desired analyses.

    In order to create a PYTHIA 8 process library with MadGraph 5, first download the MadGraph 5 package from https://launchpad.net/madgraph5, and untar the package. You can then specify the location of your pythia81xx directory in the file input/mg5_configuration.txt:
    pythia8_path = ./pythia81xx
    The location can be either relative (to the directory MadGraph5_v_x_x_x/.) or absolute.

    For any model that is already implemented in the MadGraph 5 package, you can directly use the model. Start the MadGraph 5 interface bin/mg5, and do:

    import model model_name  
    generate your_process_in_mg5_syntax 
    add process your_next_process_in_mg5_syntax 
    ...  
    output pythia8 [path_to_pythia81xx_directory]
    

    For examples of MG5 process syntax, please see http://madgraph.phys.ucl.ac.be/EXAMPLES/example_mg5.html or type help generate. If you specified the path to the pythia81xx directory in the mg5_configuration file, you do not need to enter it in the output command.

    If your preferred model is found on the FeynRules model wiki page, http://feynrules.irmp.ucl.ac.be/wiki/ModelDatabaseMainPage, download the UFO (Universal FeynRules Output) tar file for the model, untar in the models/ directory, and use as above.

    If you want to implement a new model which has not yet been implemented, you can do this either using the Mathematica package FeynRules (see http://feynrules.irmp.ucl.ac.be/) or directly edit the UFO model files of the most similar model in the models/ directory.

    The resulting output from the output pythia8 command is:

    • A process directory Processes_modelname with the model information and the files needed for all processes defined for this model, placed in the pythia81xx main directory. The model files are Parameters_modelname.h/cc and HelAmps_modelname.h/cc, and the process files for each process class (with the same mass, spin and color of the initial/final state particles) are called Sigma_modelname_processname.h/cc. The directory also contains a makefile and a model parameter file param_card_modelname.dat.
    • An example main program in the directory examples/ (in the pythia81xx main directory) called main_modelname_N.cc and a corresponding makefile Makefile_modelname_N. This main program links in the process classes in the process directory described above. To run the example main program, just go to the examples/ directory and run
      make -f Makefile_modelname_N
      or run launch directly inside the MadGraph 5 command line interface.

    Note that in order for PYTHIA 8 to be able to automatically decay any new particles, it is necessary to specify the branching ratios of the particles in the param_card file, see Ska04,Alw07 for details.

    For further technical details, please see the MadGraph 5 release paper Alw11 and the semi-internal processes page.

    Of course, as with MadGraph 4, MadGraph 5 can also output files of parton-level events according to the LHEF standard, that can be read in and processed further by PYTHIA 8. The advantage is that then the MadGraph 5 phase space generator can be used, which opens up for processes with more than three particles in the final state. The disadvantages are that it is less easy to mix and match with existing PYTHIA processes, and that one needs to regenerate and store large LHEF files for different kinematics cuts or parameter values.

    Please cite the MadGraph 5 release paper Alw11 if you use MadGraph 5 to generate process libraries for PYTHIA 8. pythia8-8.1.80.orig/xmldoc/LesHouchesAccord.xml0000444000175000017500000011067012217346304017524 0ustar sunsun

    Les Houches Accord

    The Les Houches Accord (LHA) for user processes Boo01 is the standard way to input parton-level information from a matrix-elements-based generator into PYTHIA. The conventions for which information should be stored has been defined in a Fortran context, as two commonblocks. Here a C++ equivalent is defined, as a single class.

    The LHAup class is a base class, containing reading and printout functions, plus two pure virtual functions, one to set initialization information and one to set information on each new event. Derived classes have to provide these two virtual functions to do the actual work. The existing derived classes are for reading information from a Les Houches Event File (LHEF), from the respective Fortran commonblocks, or from PYTHIA 8 itself.

    You are free to write your own derived classes, using the rules and methods to be described below. Normally, pointers to objects of such derived classes should be handed in with the Pythia::init( LHAup*) method. However, with the LHEF format a filename can replace the pointer, see further below.

    Let us now describe the methods at your disposal to do the job. the base class constructor takes the choice of mixing/weighting strategy as optional input argument, and calls setStrategy, see below. It also reserves some space for processes and particles. the destructor does not need to do anything. this method only sets the pointer that allows some information to be accessed, and is automatically called by Pythia::init(...).

    Initialization

    The LHAup class stores information equivalent to the /HEPRUP/ commonblock, as required to initialize the event generation chain. The main difference is that the vector container now allows a flexible number of subprocesses to be defined. For the rest, names have been modified, since the 6-character-limit does not apply, and variables have been regrouped for clarity, but nothing fundamental is changed. this pure virtual method has to be implemented in the derived class, to set relevant information when called. It should return false if it fails to set the info.

    Inside setInit(), such information can be set by the following methods: sets the properties of the first and second incoming beam, respectively (cf. the Fortran IDBMUP(1), EBMUP(i), PDFGUP(i), PDFSUP(i), with i 1 or 2). The parton distribution information defaults to zero. These numbers can be used to tell which PDF sets were used when the hard process was generated, while the normal PDF Selection is used for the further event generation in PYTHIA. sets the event weighting and cross section strategy. The default, provided in the class constructor, is 3, which is the natural value e.g. for an LHEF. chosen strategy (cf. IDWTUP; see Sjo06 section 9.9.1 for extensive comments). events come with non-negative weight, given in units of pb, with an average that converges towards the cross section of the process. PYTHIA is in charge of the event mixing, i.e. for each new try decides which process should be generated, and then decides whether is should be kept, based on a comparison with xMax. Accepted events therefore have unit weight. as option 1, except that cross sections can now be negative and events after unweighting have weight +-1. You can use Info::weight() to find the weight of the current event. A correct event mixing requires that a process that can take both signs should be split in two, one limited to positive or zero and the other to negative or zero values, with xMax chosen appropriately for the two. events come with non-negative weight, in unspecified units, but such that xMax can be used to unweight the events to unit weight. Again PYTHIA is in charge of the event mixing. The total cross section of a process is stored in xSec. as option 2, except that cross sections can now be negative and events after unweighting have weight +-1. As for option -1 processes with indeterminate sign should be split in two. events come with unit weight, and are thus accepted as is. The total cross section of the process is stored in xSec. as option 3, except that events now come with weight +-1. Unlike options -1 and -2 processes with indeterminate sign need not be split in two, unless you intend to mix with internal PYTHIA processes (see below). events come with non-negative weight, given in units of pb, with an average that converges towards the cross section of the process, like for option 1. No attempt is made to unweight the events, however, but all are generated in full, and retain their original weight. For consistency with normal PYTHIA units, the weight stored in Info::weight() has been converted to mb, however. as option 4, except that events now can come either with positive or negative weights. Note 1: if several processes have already been mixed and stored in a common event file, either LHEF or some private format, it would be problematical to read back events in a different order. Since it is then not feasible to let PYTHIA pick the next process type, strategies +-1 and +-2 would not work. Instead strategy 3 would be the recommended choice, or -3 if negative-weight events are required. Note 2: it is possible to switch on internally implemented processes and have PYTHIA mix these with LHA ones according to their relative cross sections for strategies +-1, +-2 and 3. It does not work for strategy -3 unless the positive and negative sectors of the cross sections are in separate subprocesses (as must always be the case for -1 and -2), since otherwise the overall mixture of PYTHIA and LHA processes will be off. Mixing is not possible for strategies +-4, since the weighting procedure is not specified by the standard. (For instance, the intention may be to have events biased towards larger pT values in some particular functional form.) sets info on an allowed process (cf. LPRUP, XSECUP, XERRUP, XMAXUP). Each new call will append one more entry to the list of processes. The choice of strategy determines which quantities are mandatory: xSec for strategies +-2 and +-3, xErr never, and xMax for strategies +-1 and +-2. Note: PYTHIA does not make active use of the (optional) xErr values, but calculates a statistical cross section error based on the spread of event-to-event weights. This should work fine for strategy options +-1, but not for the others. Specifically, for options +-2 and +-3 the weight spread may well vanish, and anyway is likely to be an underestimate of the true error. If the author of the LHA input information does provide error information you may use that - this information is displayed at initialization. If not, then a relative error decreasing like 1/sqrt(n_acc), where n_acc is the number of accepted events, should offer a reasonable estimate. update the xSec value of the i'th process added with addProcess method (i.e. i runs from 0 through sizeProc() - 1, see below). update the xErr value of the i'th process added with addProcess method. update the xMax value of the i'th process added with addProcess method. set the header key to have value val. This is a wrapper function to the Info::setHeader function that should be used in any classes derived from LHAup.

    Information is handed back by the following methods (that normally you would not need to touch): for the beam properties. for the strategy choice. for the number of subprocesses. for process i in the range 0 <= i < sizeProc(). the sum of the cross sections and errors (the latter added quadratically). Note that cross section errors are only meaningful for strategies +-3. prints the above initialization information. This method is automatically called from Pythia::init(...), so would normally not need to be called directly by the user.

    Event input

    The LHAup class also stores information equivalent to the /HEPEUP/ commonblock, as required to hand in the next parton-level configuration for complete event generation. The main difference is that the vector container now allows a flexible number of partons to be defined. For the rest, names have been modified, since the 6-character-limit does not apply, and variables have been regrouped for clarity, but nothing fundamental is changed.

    The LHA standard is based on Fortran arrays beginning with index 1, and mother information is defined accordingly. In order to be compatible with this convention, the zeroth line of the C++ particle array is kept empty, so that index 1 also here corresponds to the first particle. One small incompatibility is that the sizePart() method returns the full size of the particle array, including the empty zeroth line, and thus is one larger than the true number of particles (NUP). this pure virtual method has to be implemented in the derived class, to set relevant information when called. For strategy options +-1 and +-2 the input idProcess value specifies which process that should be generated, while idProcess is irrelevant for strategies +-3 and +-4. The mRecalculate input alllows an optional recalculation of the mass from the four-momentum, see LesHouches::mRecalculate below. The method should return false if it fails to set the info, i.e. normally that the supply of events in a file is exhausted. If so, no event is generated, and Pythia::next() returns false. You can then interrogate Info::atEndOfFile() to confirm that indeed the failure is caused in this method, and decide to break out of the event generation loop.

    Inside a normal setEvent(...) call, information can be set by the following methods: tells which kind of process occurred, with what weight, at what scale, and which alpha_EM and alpha_strong were used (cf. IDPRUP, XWTGUP, SCALUP, AQEDUP, AQCDUP). This method also resets the size of the particle list, and adds the empty zeroth line, so it has to be called before the addParticle method below. gives the properties of the next particle handed in (cf. IDUP, ISTUP, MOTHUP(1,..), MOTHUP(2,..), ICOLUP(1,..), ICOLUP(2,..), PUP(J,..), VTIMUP, SPINUP; while scale is a new optional property, see further below) .

    Information is handed back by the following methods: process number. . Note that the weight stored in Info::weight() as a rule is not the same as the above weight(): the method here gives the value before unweighting while the one in info gives the one after unweighting and thus normally is 1 or -1. Only with strategy options +-3 and +-4 would the value in info be the same as here, except for a conversion from pb to mb for +-4. scale and couplings at that scale. the size of the particle array, which is one larger than the number of particles in the event, since the zeroth entry is kept empty (see above). for particle i in the range 0 <= i < sizePart(). (But again note that i = 0 is an empty line, so the true range begins at 1.)

    From the information in the event record it is possible to set the flavour and x values of the initiators

    This information is returned by the methods x values of the two initiators.

    In the LHEF description Alw06 an extension to include information on the parton densities of the colliding partons is suggested. This optional further information can be set by which gives the flavours , the x and the Q scale (in GeV) at which the parton densities x*f_i(x, Q) have been evaluated. The last argument is normally true.

    This information is returned by the methods where the first one tells whether this optional information has been set for the current event. (setPdf(...) must be called after the setProcess(...) call of the event for this to work.) Note that the flavour and x values usually but not always agree with those obtained by the same methods without pdf in their names, see explanation in the Event Information description.

    As a further, currently completely non-standard feature, it is also possible to read in the separate scale values of all final particles. Currently such information should appear as a line begun by a single hashtag character (#) and then sequentially the scale value of all particles with status 1. Such scale values could be used e.g. to restrict the maximum scale for shower evolutions for each parton separately. This information is returned by the method double LHAup::scale(int i). When no such information has been read from the LHEF, the scale defaults to -1.

    prints the above information for the current event. In cases where the LHAup object is not available to the user, the Pythia::LHAeventList(ostream& os = cout) method can be used, which is a wrapper for the above. skip ahead nSkip events in the Les Houches generation sequence, without doing anything further with them. Mainly intended for debug purposes, e.g. when an event at a known location in a Les Houches Event File is causing problems. Will return false if operation fails, specifically if the end of an LHEF has been reached. The implementation in the base class simply executes setEvent() the requested number of times. The derived LHAupLHEF class (see below) only uses the setNewEventLHEF(...) part of its setEvent() method, and other derived classes could choose other shortcuts.

    The LHA expects the decay of resonances to be included as part of the hard process, i.e. if unstable particles are produced in a process then their decays are also described. This includes Z^0, W^+-, H^0 and other short-lived particles in models beyond the Standard Model. Should this not be the case then PYTHIA will perform the decays of all resonances it knows how to do, in the same way as for internal processes. Note that you will be on slippery ground if you then restrict the decay of these resonances to specific allowed channels since, if this is not what was intended, you will obtain the wrong cross section and potentially the wrong mix of different event types. (Since the original intention is unknown, the cross section will not be corrected for the fraction of open channels, i.e. the procedure used for internal processes is not applied in this case.)

    Even if PYTHIA can select resonance decay modes according to its internal tables, there is normally no way for it to know which decay angular correlations should exist in the simulated process. Therefore almost all decays are isotropic. The exceptions are Higgs and top decays, in the decay chains H -> WW/ZZ -> f fbar f' fbar' and t -> b W -> b f fbar, where the process-independent correlations implemented for internal processes are used. If part of the decay chain has already been set, however (e.g. H -> WW/ZZ or t -> b W), then decay is still isotropic.

    There is one setting available for event input. handling of the decay time information stored in VTIMUP when the Les Houches event record is stored into the PYTHIA process one. The reason is that some matrix-element generators (like POWHEG) do not set decay times, so that it is up to PYTHIA to make that selection. This is particularly important for the tau lepton.

    There is also one parameter that can be used to modify the setting of event information, if implemented in the derived class. It is prompted by an unforeseen choice made in some programs (like CalcHEP) of storing the nominal mass of a particle species rather than the mass of the current member of that species. This is likely to induce energy-momentum nonconservation when the event is further processed. Does not have any effect by default, or more generally when it is negative. If it is positive then all particles with an input mass above this value will have the mass recalculated and reset from the four-momentum, m^2 = E^2 - p^2. Obviously such a step is problematic numerically for light particles, so it should only be used for the programs and particles where it is needed. Thus the value ought to be at least 10 GeV, so that only massive particles like W^+-, Z^0 and t are affected.

    An interface to Les Houches Event Files

    The LHEF standard Alw06 specifies a format where a single file packs initialization and event information. This has become the most frequently used procedure to process external parton-level events in Pythia. Therefore a special Pythia::init(fileName) initialization option exists, where the LHEF name is provided as input. Internally this name is then used to create an instance of the derived class LHAupLHEF, which can do the job of reading an LHEF.

    The LHEF reader can also read in and store header blocks. By default this option is switched on, but may be controlled through the Beams:readLHEFheaders flag if necessary. The information can later be read out through the Info class for further processing. Due to the non-standard nature of the information in these blocks they are stored whole, and PYTHIA itself makes no further attempt to process their meaning.

    Because Les Houches Event files tend not to adhere strictly to XML conventions, to consistently read in header information, certain choices must be made. The primary goal is to make as much information available as possible. First, information sitting directly in the <header> block is stored under the key "base". Second, the tags starting and ending each sub block must be on their own line. Finally, the contents of comment blocks, <!-- -->, are still stored. The header keys are formed hierarchically from the names of the header blocks. This behaviour is illustrated in the following example:

      <header>
        BaseA
        <hblock1>
          1A
          <hblock11>
            11A <hblock111>
            </hblock111> 11B
          </hblock11>
          1B
        </hblock1>
        <hblock2>
          2A
          <!-- 2B -->
        </hblock2>
        BaseB
      </header>
    
    which would lead to the following information being stored in the Info class:
    Key Value
    base BaseA
    BaseB
    hblock1 1A
    1B
    hblock1.hblock11 11A <hblock111>
    </hblock111> 11B
    hblock2 2A
    <!-- 2B -->

    Normally the LHEF would be in uncompressed format, and thus human-readable if opened in a text editor. A possibility to read gzipped files has been added, based on the Boost and zlib libraries, which therefore have to be linked appropriately in order for this option to work. See the README file in the main directory for details on how to do this.

    An example how to generate events from an LHEF is found in main11.cc. Note the use of Info::atEndOfFile() to find out when the whole LHEF has been processed.

    To allow the sequential use of several event files the Pythia::init(...) method has an optional second argument: Pythia::init(fileName, bool skipInit = false). If called with this argument true then there will be no initialization, except that the existing LHAupLHEF class instance will be deleted and replaced by ones pointing to the new file. It is assumed (but never checked) that the initialization information is identical, and that the new file simply contains further events of exactly the same kind as the previous one. An example of this possibility, and the option to mix with internal processes, is found in main12.cc. A variant, based on input in a command file, is given in main13.cc.

    In C++, real numbers are printed with an 'E' to denote the exponent part, e.g. 1.23E+04, and are read in accordingly. Other languages may use other letters, e.g. Fortran allows either 'E' or 'D'. A file using the latter convention would not be readable by the standard routines. In case you have such an "incorrectly formatted" file, a conversion to a new corrected file could be done e.g. using sed, as a one-line command

      sed -e 's/\([0-9]\.\{0,1\}\)[dD]\([+-]\{0,1\}[0-9]\)/\1E\2/g' old.lhe > new.lhe
    
    This replaces a 'd' or 'D' with an 'E' only when it occurs in the combination
    (digit) ('.' or absent) ('d' or 'D') ('+', '-' or absent) (digit)
    It will work on all parts of the file, also inside a <header>...</header> block. For conversion only inside the <init>...</init> and <event>...</event> blocks, create a file convert.sed containing
      /<init>/,/<\/init>/bconv
      /<event>/,/<\/event>/bconv
      b
      :conv
      s/\([0-9]\.\{0,1\}\)[dD]\([+-]\{0,1\}[0-9]\)/\1E\2/g
    
    and run it with
      sed -f convert.sed old.lhe > new.lhe
    

    The workhorses of the LHAupLHEF class are three methods found in the base class, so as to allow them to be reused in other contexts. Specifically, it allows derived classes where one parton-level configuration can be reused several times, e.g. in the context of matrix-element-to-parton-shower matching (example in preparation). Also two small utility routines. read in and set all required initialization information from the specified stream. With second argument true it will also read and store header information, as described above. Return false if it fails. read in event information from the specified stream into a staging area where it can be reused by setOldEventLHEF. store the event information from the staging area into the normal location. Thus a single setNewEventLHEF call can be followed by several setOldEventLHEF ones, so as to process the same configuration several times. This method currently only returns true, i.e. any errors should be caught by the preceding setNewEventLHEF call. always returns true in the base class, but in LHAupLHEF it returns false if the LHEF provided in the constructor is not found and opened correctly. is used to send header information on to the Info class.

    A few other methods, most of them derived from the base class, streamlines file opening and closing, e.g. if several LHE files are to be read consecutively, without the need for a complete reinitialization. This presupposes that the events are of the same kind, only split e.g. to limit file sizes. close current event input file/stream and open a new one, to continue reading events of the same kind as before. open and close a file, also gzip files, where an intermediate decompression layer is needed. close main event file (LHEF) and, if present, separate header file.

    A runtime Fortran interface

    The runtime Fortran interface requires linking to an external Fortran code. In order to avoid problems with unresolved external references when this interface is not used, the code has been put in a separate LHAFortran.h file, that is not included in any of the other library files. Instead it should be included in the user-supplied main program, together with the implementation of two methods below that call the Fortran program to do its part of the job.

    The LHAupFortran class derives from LHAup. It reads initialization and event information from the LHA standard Fortran commonblocks, assuming these commonblocks behave like two extern "C" struct named heprup_ and hepeup_. (Note the final underscore, to match how the gcc compiler internally names Fortran files.)

    The instantiation does not require any arguments.

    The user has to supply implementations of the fillHepRup() and fillHepEup() methods, that is to do the actual calling of the external Fortran routines that fill the HEPRUP and HEPEUP commonblocks. The translation of this information to the C++ structure is provided by the existing setInit() and setEvent() code.

    Up to and including version 8.125 the LHAupFortran class was used to construct a runtime interface to PYTHIA 6.4. This was convenient in the early days of PYTHIA 8 evolution, when this program did not yet contain hard-process generation, and the LHEF standard did not yet exist. Nowadays it is more of a bother, since a full cross-platform support leads to many possible combinations. Therefore this support has been removed, but can still be recuperated from previous code versions, in a reduced form up to version 8.176.

    Methods for LHEF output

    The main objective of the LHAup class is to feed information from an external program into PYTHIA. It can be used to export information as well, however. Specifically, there are four routines in the base class that can be called to write a Les Houches Event File. These should be called in sequence in order to build up the proper file structure. Opens a file with the filename indicated, and writes a header plus a brief comment with date and time information. Writes initialization information to the file above. Such information should already have been set with the methods described in the "Initialization" section above. Writes event information to the file above. Such information should already have been set with the methods described in the "Event input" section above. This call should be repeated once for each event to be stored. By default the event information is lined up in columns. To save space, the alternative verbose = false only leaves a single blank between the information fields. Writes the closing tag and closes the file. Optionally, if updateInit = true, this routine will reopen the file from the beginning, rewrite the same header as openLHEF() did, and then call initLHEF() again to overwrite the old information. This is especially geared towards programs, such as PYTHIA itself, where the cross section information is not available at the beginning of the run, but only is obtained by Monte Carlo integration in parallel with the event generation itself. Then the setXSec( i, xSec), setXErr( i, xSec) and setXMax( i, xSec) can be used to update the relevant information before closeLHEF is called. Warning: overwriting the beginning of a file without upsetting anything is a delicate operation. It only works when the new lines require exactly as much space as the old ones did. Thus, if you add another process in between, the file will be corrupted.

    PYTHIA 8 output to an LHEF

    The above methods could be used by any program to write an LHEF. For PYTHIA 8 to do this, a derived class already exists, LHAupFromPYTHIA8. In order for it to do its job, it must gain access to the information produced by PYTHIA, specifically the process event record and the generic information stored in info. Therefore, if you are working with an instance pythia of the Pythia class, you have to instantiate LHAupFromPYTHIA8 with pointers to the process and info objects of pythia:
    LHAupFromPYTHIA8 myLHA(&pythia.process, &pythia.info);

    The method setInit() should be called to store the pythia initialization information in the LHA object, and setEvent() to store event information. Furthermore, updateSigma() can be used at the end of the run to update cross-section information, cf. closeLHEF(true) above. An example how the generation, translation and writing methods should be ordered is found in main20.cc.

    Currently there are some limitations, that could be overcome if necessary. Firstly, you may mix many processes in the same run, but the cross-section information stored in info only refers to the sum of them all, and therefore they are all classified as a common process 9999. Secondly, you should generate your events in the CM frame of the collision, since this is the assumed frame of stored Les Houches events, and no boosts have been implemented for the case that Pythia::process is not in this frame.

    The LHEF standard is the agreed format to store the particles of a hard process, as input to generators, whereas output of final states is normally handled using the HepMC standard. It is possible to use LHEF also here, however. It requires that the above initialization is replaced by
    LHAupFromPYTHIA8 myLHA(&pythia.event, &pythia.info);
    i.e. that process is replaced by event. In addition, the PartonLevel:all = off command found in main20.cc obviously must be removed if one wants to obtain complete events. pythia8-8.1.80.orig/xmldoc/EventRecord.xml0000444000175000017500000005636112217346302016572 0ustar sunsun

    The Event Record

    A Pythia instance contains two members of the Event class. The one called process provides a brief summary of the main steps of the hard process, while the one called event contains the full history. The user would normally interact mainly with the second one, so we will exemplify primarily with that one.

    The Event class to first approximation is a vector of Particles, so that it can expand to fit the current event size. The index operator is overloaded, so that e.g. event[i] corresponds to the i'th particle of the object event. Thus event[i].id() returns the identity of the i'th particle, and so on. Therefore the methods of the Particle class are at least as essential as those of the Event class itself.

    As used inside PYTHIA, some conventions are imposed on the structure of the event record. Entry 0 of the vector<Particle> is used to represent the event as a whole, with its total four-momentum and invariant mass, but does not form part of the event history. Lines 1 and 2 contains the two incoming beams, and only from here on history tracing works as could be expected. That way unassigned mother and daughter indices can be put 0 without ambiguity. Depending on the task at hand, a loop may therefore start at index 1 rather than 0 without any loss. Specifically, for translation to other event record formats such as HepMC Dob01, where the first index is 1, the Pythia entry 0 definitely ought to be skipped in order to minimize the danger of indexing errors.

    In the following we will list the methods available. Only a few of them have a function to fill in normal user code.

    Basic output methods

    Some methods are available to read out information on the current event record: returns a (const) reference to the i'th particle in the event record, which can be used to get (or set) all the properties of this particle. returns a reference to the zeroth, i'th or last particle in the event record, as an alternative to the methods above. The event size, i.e. the size of the vector<Particle>. Thus valid particles, to be accessed by the above indexing operator, are stored in the range 0 <= i < size(). See comment above about the (ir)relevance of entry 0. Provide a listing of the whole event, i.e. of the vector<Particle>. The methods with fewer arguments call the final one with the respective default values, and are non-inlined so they can be used in a debugger. The basic identity code, status, mother, daughter, colour, four-momentum and mass data are always given, but the methods can also be called with a few optional arguments for further information: optionally give a second line for each particle, with the production scale (in GeV), the particle polarization (dimensionless), the production vertex (in mm or mm/c) and the invariant lifetime (also in mm/c). gives a list of all daughters and mothers of a particle, as defined by the motherList(i) and daughterList(i) methods described below. It is mainly intended for debug purposes. a reference to the ostream object to which the event listing will be directed.

    Each Particle has two mother and two daughter indices. These may be used to encode zero, one, two or more mothers/daughters, depending on the combination of values and status code, according to well-defined rules. The two methods below can do this job easier for you. returns a vector of all the mother indices of the particle at index i. This list is empty for entries 0, 1 and 2, i.e. the "system" in line 0 is not counted as part of the history. Normally the list contains one or two mothers, but it can also be more, e.g. in string fragmentation the whole fragmenting system is counted as mothers to the primary hadrons. Many particles may have the same motherList. Mothers are listed in ascending order. returns a vector of all the daughter indices of the particle at index i. This list is empty for a particle that did not decay (or, if the evolution is stopped early enough, a parton that did not branch), while otherwise it can contain a list of varying length, from one to many. For the two incoming beam particles, all shower initiators and beam remnants are counted as daughters, with the one in slot 0 being the one leading up to the hardest interaction. The "system" in line 0 does not have any daughters, i.e. is not counted as part of the history. Many partons may have the same daughterList. Daughters are listed in ascending order. returns the status code according to the HepMC conventions agreed in February 2009. This convention does not preserve the full information provided by the internal PYTHIA status code, as obtained by Particle::status(), but comes reasonably close. The allowed output values are:

    • 0 : an empty entry, with no meaningful information and therefore to be skipped unconditionally (should not occur in PYTHIA);
    • 1 : a final-state particle, i.e. a particle that is not decayed further by the generator (may also include unstable particles that are to be decayed later, as part of the detector simulation);
    • 2 : a decayed Standard Model hadron or tau or mu lepton, excepting virtual intermediate states thereof (i.e. the particle must undergo a normal decay, not e.g. a shower branching);
    • 3 : a documentation entry (not used in PYTHIA);
    • 4 : an incoming beam particle;
    • 11 - 200 : an intermediate (decayed/branched/...) particle that does not fulfill the criteria of status code 2, with a generator-dependent classification of its nature; in PYTHIA the absolute value of the normal status code is used.

    Further output methods

    The above methods are the main ones that a normal user would make frequent use of. There are some further methods that also could come in handy, in the exploration of the history of an event, but where the outcome is not always obvious if one is not familiar with the detailed structure of an event record. are used to trace carbon copies of the particle at index i up to its top mother or down to its bottom daughter. If there are no such carbon copies, i itself will be returned. A carbon copy is when the "same" particle appears several times in the event record, but with changed momentum owing to recoil effects. also trace top mother and bottom daughter, but do not require carbon copies, only that one can find an unbroken chain, of mothers or daughters, with the same flavour id code. When it encounters ambiguities, say a g -> g g branching or a u u -> u u hard scattering, it will stop the tracing and return the current position. It can be confused by nontrivial flavour changes, e.g. a hard process u d -> d u by W^+- exchange will give the wrong answer. These methods therefore are of limited use for common particles, in particular for the gluon, but should work well for "rare" particles. returns a vector of all the sister indices of the particle at index i, i.e. all the daughters of the first mother, except the particle itself. returns a vector of all the sister indices of the particle at index i, tracking up and back down through carbon copies if required. That is, the particle is first traced up with iTopCopy() before its mother is found, and then all the particles in the daughterList() of this mother are traced down with iBotCopy(), omitting the original particle itself. Any non-final particles are removed from the list. Should this make the list empty the search criterion is widened so that all final daughters are allowed, not only carbon-copy ones. That is, starting from the top mother, all its daughters are found, except for the traced-up one, and then all their daughters, and so on. This can produce quite extensive and rather useless output, notably when tracing parton showers. A second argument false inhibits the second step, and increases the risk that an empty list is returned. A typical example of this is for ISR cascades, e.g. e -> e gamma where the photon may not have any obvious sister in the final state if the bottom copy of the photon is an electron that annihilates and thus is not part of the final state. traces the particle i upwards through mother, grandmother, and so on, until either iAncestor is found or the top of the record is reached. Normally one unique mother is required, as is the case e.g. in decay chains or in parton showers, so that e.g. the tracing through a hard scattering would not work. For hadronization, first-rank hadrons are identified with the respective string endpoint quark, which may be useful e.g. for b physics, while higher-rank hadrons give false. Currently also ministrings that collapsed to one single hadron and junction topologies give false.

    One data member in an Event object is used to keep track of the largest col() or acol() colour tag set so far, so that new ones do not clash. This sets the initial colour tag value used, so that the first one assigned is startColTag + 1, etc. The Les Houches accord Boo01 suggests this number to be 500, but 100 works equally well. forces the current colour tag value to be the larger of the input colTag and the above Event:startColTag values. returns the current maximum colour tag. increases the current maximum colour tag by one and returns this new value. This method is used whenever a new colour tag is needed.

    Many event properties are accessible via the Info class, see here. Since they are used directly in the event generation, a few are stored directly in the Event class, however. set or get the scale (in GeV) of the hardest process in the event. Matches the function of the scale variable in the Les Houches Accord. set or get the scale (in GeV) of a second hard process in the event, in those cases where such a one has been requested.

    Constructors and modifications of the event record

    Although you would not normally need to create your own Event instance, there may be times where that could be convenient. The typical example would be if you want to create a new event record that is the sum of a few different ones, e.g. if you want to simulate pileup events. There may also be cases where you want to add one or a few particles to an existing event record. creates an empty event record, but with a reserved size capacity for the Particle vector. copies the input event record. appends an event to an existing one. For the appended particles mother, daughter and colour tags are shifted to make a consistent record. The zeroth particle of the appended event is not copied, but the zeroth particle of the combined event is updated to the full energy-momentum content. initializes colour, the pointer to the particle database, and the header specification used for the event listing. We remind that a Pythia object contains two event records process and event. Thus one may e.g. call either pythia.process.list() or pythia.event.list(). To distinguish those two rapidly at visual inspection, the "Pythia Event Listing" header is printed out differently, in one case adding "(hard process)" and in the other "(complete event)". When += is used to append an event, the modified event is printed with "(combination of several events)" as a reminder. empties event record. Specifically the Particle vector size is reset to zero. empties the event record, as clear() above, but then fills the zero entry of the Particle vector with the pseudoparticle used to represent the event as a whole. At this point the pseudoparticle is not assigned any momentum or mass. removes the last n particle entries; must be a positive number. History (and other) information of remaning entries is untouched, and so may be internally inconsistent. removes particles in the range between indices iFirst and iLast, including the endpoints. History (and other) information of remaning entries is untouched, and so may be internally inconsistent. removes the decay chain of the particle i and thus restores it to its undecayed state. It is only intended for "normal" particle decay chains, and will return false in other cases, notably if the particle is coloured. The procedure would not work if non-local momentum shifts have been performed, such as with a Bose-Einstein shift procedure (or for a dipole shower recoiler). The history information of the remaining particles, many of which may have new indices, is updated to be internally consistent. appends a particle to the bottom of the event record and returns the index of this position. appends a particle to the bottom of the event record and returns the index of this position; see here for the meaning of the various particle properties. appends a particle to the bottom of the event record and returns the index of this position, as above but with four-momentum as a Vec4. appends a particle to the bottom of the event record and returns the index of this position, as above but with vanishing (i.e. zero) mother and daughter indices. send in the this pointer of the current Event itself to the particle iSet, by default the most recently appended particle. Also generates a pointer to the ParticleDataEntry object of the identity code of the particle. copies the existing particle in entry iCopy to the bottom of the event record and returns the index of this position. By default, i.e. with newStatus = 0, everything is copied precisely as it is, which means that history information has to be modified further by hand to make sense. With a positive newStatus, the new copy is set up to be the daughter of the old, with status code newStatus, while the status code of iCopy is negated. With a negative newStatus, the new copy is instead set up to be the mother of iCopy. An attempt to copy an out-of-range entry will return -1. each particle in the event record has a pointer to the event itself and another to the particle species it belongs to. The latter pointer is automatically set/changed whenever the particle identity is set/changed by one of the normal methods. Of course the pointer values are specific to the memory locations of the current run, and so it has no sense to save them if events are written to file. Should you use some persistency scheme that bypasses the normal methods when the event is read back in, you can use restorePtrs() afterwards to set these pointers appropriately.

    A few methods exist to rotate and boost events. These derive from the Vec4 methods, and affect both the momentum and the vertex (position) components of all particles. rotate all particles in the event by this polar and azimuthal angle (expressed in radians). boost all particles in the event by this three-vector. Optionally you may provide the gamma value as a fourth argument, which may help avoid roundoff errors for big boosts. You may alternatively supply a Vec4 four-vector, in which case the boost vector becomes beta = p/E. rotate and boost by the combined action encoded in the RotBstMatrix M.

    The Junction Class

    The event record also contains a vector of junctions, which often is empty or else contains only a very few per event. Methods are available to add further junctions or query the current junction list. This is only for the expert user, however, and is not discussed further here, but only the main points.

    A junction stores the properties associated with a baryon number that is fully resolved, i.e. where three different colour indices are involved. There are two main applications,

    1. baryon beams, where at least two valence quarks are kicked out, and so the motion of the baryon number is nontrivial;
    2. baryon-number violating processes, e.g. in SUSY with broken R-parity.
    Information on junctions is set, partly in the process generation, partly in the beam remnants machinery, and used by the fragmentation routines, but the normal user does not have to know the details.

    For each junction, information is stored on the kind of junction, and on the three (anti)colour indices that are involved in the junction. The possibilities foreseen are:

    • kind = 1 : incoming colourless particle to three outgoing colours (e.g. baryon beam remnant or neutralino -> q q q);
    • kind = 2 : incoming colourless particle to three outgoing anticolours;
    • kind = 3 : one incoming anticolour (stored first) and two outgoing colours (e.g. antisquark decaying to two quarks, or gluino decay to three quarks);
    • kind = 4 : one incoming colour (stored first) and two outgoing anticolours (e.g. squark decaying to two antiquarks, or gluino decaying to three antiquarks);
    • kind = 5 : two incoming anticolours (stored first) and one outgoing colour (e.g. resonant squark production through RPV);
    • kind = 6 : two incoming colours (stored first) and one outgoing anticolour (e.g. resonant antisquark production through RPV);
    The odd (even) kind codes corresponds to a +1 (-1) change in baryon number across the junction.

    The kind and colour information in the list of junctions can be set or read with methods of the Event class, but are not of common interest and so not described here.

    A listing of current junctions can be obtained with the listJunctions() method.

    Subsystems

    Separate from the event record as such, but closely tied to it is the PartonSystems class, which mainly stores the parton indices of incoming and outgoing partons, classified by collision subsystem. Such information is needed to interleave multiparton interactions, initial-state showers and final-state showers, and append beam remnants. It could also be used in other places. It is intended to be accessed only by experts, such as implementors of new showering models.
    pythia8-8.1.80.orig/xmldoc/piN-SAID-WI08.dat0000444000175000017500000103205212217346315016247 0ustar sunsun# Pion-nucleon partial-wave data, GWU SAID WI08 solution # GWU SAID analyses: # FP84 - Phys. Rev. D32 1085 (1985) # SP06 - Phys. Rev. C74 045205 (2006) # WI08 - http://gwdac.phys.gwu.edu/analysis/pin_analysis.html # Notation for column headers is J,2I,2S # Entries in each column are Treal and Tim set eType Tlab set eUnit MeV set input Tr,Ti # Isospin = 1/2 Tlab 0,1,1 1,1,1 1,1,3 2,1,3 2,1,5 2.50 0.028 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 7.50 0.049 0.002 -0.001 0.000 -0.001 0.000 0.000 0.000 0.000 0.000 12.50 0.062 0.004 -0.003 0.000 -0.001 0.000 0.000 0.000 0.000 0.000 17.50 0.073 0.005 -0.004 0.000 -0.002 0.000 0.000 0.000 0.000 0.000 22.50 0.082 0.007 -0.006 0.000 -0.003 0.000 0.000 0.000 0.000 0.000 27.50 0.090 0.008 -0.007 0.000 -0.004 0.000 0.000 0.000 0.000 0.000 32.50 0.097 0.010 -0.009 0.000 -0.005 0.000 0.000 0.000 0.000 0.000 37.50 0.103 0.011 -0.010 0.000 -0.006 0.000 0.000 0.000 0.001 0.000 42.50 0.109 0.012 -0.012 0.000 -0.007 0.000 0.000 0.000 0.001 0.000 47.50 0.114 0.013 -0.013 0.000 -0.008 0.000 0.001 0.000 0.001 0.000 52.50 0.119 0.014 -0.014 0.000 -0.009 0.000 0.001 0.000 0.001 0.000 57.50 0.123 0.015 -0.015 0.000 -0.010 0.000 0.001 0.000 0.001 0.000 62.50 0.127 0.017 -0.016 0.000 -0.011 0.000 0.001 0.000 0.002 0.000 67.50 0.131 0.018 -0.017 0.000 -0.012 0.000 0.002 0.000 0.002 0.000 72.50 0.135 0.018 -0.017 0.000 -0.013 0.000 0.002 0.000 0.002 0.000 77.50 0.138 0.019 -0.018 0.000 -0.015 0.000 0.002 0.000 0.003 0.000 82.50 0.141 0.020 -0.018 0.000 -0.016 0.000 0.003 0.000 0.003 0.000 87.50 0.144 0.021 -0.018 0.000 -0.017 0.000 0.003 0.000 0.004 0.000 92.50 0.146 0.022 -0.017 0.000 -0.018 0.000 0.004 0.000 0.004 0.000 97.50 0.149 0.023 -0.017 0.000 -0.020 0.000 0.004 0.000 0.004 0.000 102.50 0.151 0.023 -0.016 0.000 -0.021 0.000 0.005 0.000 0.005 0.000 107.50 0.153 0.024 -0.015 0.000 -0.022 0.000 0.005 0.000 0.005 0.000 112.50 0.155 0.025 -0.014 0.000 -0.023 0.001 0.006 0.000 0.006 0.000 117.50 0.158 0.025 -0.013 0.000 -0.025 0.001 0.007 0.000 0.006 0.000 122.50 0.159 0.026 -0.011 0.000 -0.026 0.001 0.007 0.000 0.007 0.000 127.50 0.161 0.027 -0.009 0.000 -0.027 0.001 0.008 0.000 0.008 0.000 132.50 0.163 0.027 -0.007 0.000 -0.028 0.001 0.009 0.000 0.008 0.000 137.50 0.165 0.028 -0.004 0.000 -0.030 0.001 0.010 0.000 0.009 0.000 142.50 0.167 0.029 -0.002 0.000 -0.031 0.001 0.011 0.000 0.009 0.000 147.50 0.168 0.029 0.001 0.000 -0.032 0.001 0.012 0.000 0.010 0.000 152.50 0.170 0.030 0.005 0.000 -0.033 0.001 0.013 0.000 0.011 0.000 157.50 0.171 0.030 0.008 0.000 -0.035 0.001 0.014 0.000 0.011 0.000 162.50 0.173 0.031 0.012 0.000 -0.036 0.001 0.015 0.000 0.012 0.000 167.50 0.174 0.031 0.017 0.000 -0.037 0.001 0.016 0.000 0.012 0.000 172.50 0.176 0.032 0.021 0.001 -0.038 0.001 0.018 0.000 0.013 0.000 177.50 0.177 0.032 0.026 0.001 -0.039 0.002 0.019 0.000 0.014 0.000 182.50 0.178 0.033 0.031 0.001 -0.041 0.002 0.021 0.001 0.014 0.000 187.50 0.180 0.034 0.037 0.002 -0.042 0.002 0.022 0.001 0.015 0.000 192.50 0.181 0.034 0.043 0.002 -0.043 0.002 0.024 0.001 0.016 0.000 197.50 0.182 0.035 0.049 0.003 -0.044 0.002 0.025 0.001 0.016 0.000 202.50 0.183 0.035 0.056 0.004 -0.045 0.002 0.027 0.001 0.017 0.000 207.50 0.185 0.036 0.063 0.005 -0.046 0.002 0.029 0.002 0.018 0.000 212.50 0.186 0.036 0.071 0.006 -0.048 0.002 0.031 0.002 0.019 0.000 217.50 0.187 0.037 0.078 0.008 -0.049 0.002 0.032 0.002 0.019 0.000 222.50 0.188 0.038 0.087 0.010 -0.050 0.003 0.034 0.002 0.020 0.000 227.50 0.189 0.038 0.095 0.012 -0.051 0.003 0.036 0.003 0.021 0.000 232.50 0.191 0.039 0.104 0.014 -0.052 0.003 0.039 0.003 0.022 0.000 237.50 0.192 0.039 0.114 0.017 -0.053 0.003 0.041 0.003 0.022 0.001 242.50 0.193 0.040 0.123 0.020 -0.054 0.003 0.043 0.004 0.023 0.001 247.50 0.194 0.040 0.134 0.024 -0.055 0.003 0.045 0.004 0.024 0.001 252.50 0.195 0.041 0.144 0.028 -0.056 0.003 0.048 0.005 0.025 0.001 257.50 0.197 0.042 0.155 0.032 -0.057 0.003 0.050 0.005 0.025 0.001 262.50 0.198 0.042 0.166 0.037 -0.058 0.004 0.053 0.006 0.026 0.001 267.50 0.199 0.043 0.178 0.043 -0.059 0.004 0.055 0.006 0.027 0.001 272.50 0.201 0.044 0.189 0.050 -0.060 0.004 0.058 0.007 0.028 0.001 277.50 0.202 0.044 0.201 0.057 -0.061 0.004 0.061 0.007 0.028 0.001 282.50 0.203 0.045 0.213 0.065 -0.062 0.004 0.063 0.008 0.029 0.001 287.50 0.205 0.046 0.226 0.073 -0.063 0.004 0.066 0.009 0.030 0.001 292.50 0.206 0.047 0.238 0.083 -0.064 0.004 0.069 0.010 0.031 0.001 297.50 0.207 0.048 0.250 0.094 -0.065 0.004 0.073 0.010 0.032 0.001 302.50 0.209 0.048 0.263 0.105 -0.066 0.005 0.076 0.011 0.033 0.001 307.50 0.210 0.049 0.275 0.118 -0.066 0.005 0.079 0.012 0.033 0.001 312.50 0.212 0.050 0.286 0.132 -0.067 0.005 0.082 0.013 0.034 0.001 317.50 0.214 0.051 0.297 0.146 -0.068 0.005 0.086 0.015 0.035 0.001 322.50 0.215 0.052 0.308 0.162 -0.069 0.005 0.090 0.016 0.036 0.002 327.50 0.217 0.053 0.318 0.179 -0.070 0.005 0.093 0.017 0.037 0.002 332.50 0.219 0.054 0.327 0.197 -0.071 0.005 0.097 0.019 0.038 0.002 337.50 0.220 0.055 0.335 0.215 -0.071 0.006 0.101 0.020 0.039 0.002 342.50 0.222 0.056 0.342 0.235 -0.072 0.006 0.105 0.022 0.040 0.002 347.50 0.224 0.058 0.348 0.255 -0.073 0.006 0.109 0.023 0.040 0.002 352.50 0.226 0.059 0.352 0.275 -0.073 0.006 0.113 0.025 0.041 0.002 357.50 0.228 0.060 0.355 0.296 -0.074 0.006 0.118 0.027 0.042 0.002 362.50 0.230 0.062 0.356 0.318 -0.075 0.006 0.122 0.029 0.043 0.002 367.50 0.232 0.063 0.356 0.339 -0.075 0.007 0.127 0.032 0.044 0.003 372.50 0.235 0.065 0.355 0.360 -0.076 0.007 0.131 0.034 0.045 0.003 377.50 0.237 0.066 0.351 0.381 -0.077 0.007 0.136 0.037 0.046 0.003 382.50 0.239 0.068 0.347 0.401 -0.077 0.007 0.141 0.040 0.047 0.003 387.50 0.242 0.070 0.341 0.421 -0.078 0.007 0.146 0.043 0.048 0.003 392.50 0.244 0.072 0.334 0.439 -0.078 0.007 0.152 0.046 0.049 0.003 397.50 0.247 0.074 0.325 0.457 -0.079 0.007 0.157 0.050 0.051 0.004 402.50 0.250 0.076 0.316 0.474 -0.079 0.008 0.162 0.053 0.052 0.004 407.50 0.253 0.078 0.306 0.489 -0.080 0.008 0.168 0.057 0.053 0.004 412.50 0.256 0.080 0.296 0.504 -0.080 0.008 0.174 0.062 0.054 0.004 417.50 0.259 0.082 0.284 0.517 -0.081 0.008 0.180 0.066 0.055 0.004 422.50 0.262 0.085 0.273 0.529 -0.081 0.008 0.186 0.071 0.056 0.005 427.50 0.265 0.088 0.261 0.540 -0.081 0.008 0.192 0.076 0.057 0.005 432.50 0.268 0.091 0.249 0.550 -0.082 0.009 0.198 0.082 0.059 0.005 437.50 0.272 0.094 0.237 0.559 -0.082 0.009 0.204 0.088 0.060 0.005 442.50 0.276 0.097 0.225 0.567 -0.082 0.009 0.211 0.095 0.061 0.006 447.50 0.279 0.100 0.213 0.574 -0.083 0.009 0.217 0.102 0.062 0.006 452.50 0.283 0.104 0.202 0.580 -0.083 0.009 0.224 0.109 0.064 0.006 457.50 0.287 0.108 0.191 0.585 -0.083 0.009 0.231 0.117 0.065 0.007 462.50 0.292 0.112 0.180 0.590 -0.083 0.010 0.237 0.126 0.066 0.007 467.50 0.296 0.116 0.169 0.593 -0.083 0.010 0.244 0.135 0.068 0.007 472.50 0.301 0.121 0.159 0.596 -0.083 0.010 0.251 0.145 0.069 0.008 477.50 0.305 0.126 0.149 0.599 -0.084 0.010 0.258 0.156 0.071 0.008 482.50 0.310 0.131 0.139 0.601 -0.084 0.010 0.264 0.168 0.072 0.009 487.50 0.315 0.137 0.130 0.603 -0.084 0.011 0.270 0.180 0.074 0.009 492.50 0.321 0.143 0.121 0.604 -0.084 0.011 0.276 0.194 0.075 0.010 497.50 0.326 0.149 0.112 0.605 -0.084 0.011 0.282 0.208 0.077 0.010 502.50 0.332 0.157 0.104 0.606 -0.084 0.011 0.287 0.224 0.079 0.011 507.50 0.338 0.165 0.097 0.606 -0.083 0.012 0.292 0.240 0.080 0.011 512.50 0.345 0.173 0.089 0.606 -0.083 0.012 0.296 0.258 0.082 0.012 517.50 0.351 0.183 0.082 0.606 -0.083 0.012 0.299 0.277 0.084 0.013 522.50 0.358 0.193 0.075 0.605 -0.083 0.012 0.301 0.297 0.086 0.013 527.50 0.366 0.205 0.069 0.605 -0.083 0.013 0.302 0.318 0.088 0.014 532.50 0.373 0.218 0.063 0.604 -0.082 0.013 0.301 0.341 0.089 0.015 537.50 0.381 0.233 0.057 0.603 -0.082 0.013 0.299 0.364 0.091 0.016 542.50 0.390 0.251 0.052 0.602 -0.082 0.014 0.294 0.389 0.093 0.017 547.50 0.398 0.272 0.047 0.601 -0.081 0.014 0.287 0.414 0.095 0.018 552.50 0.407 0.299 0.042 0.600 -0.081 0.014 0.278 0.440 0.098 0.018 557.50 0.416 0.340 0.037 0.599 -0.081 0.015 0.266 0.466 0.100 0.020 562.50 0.381 0.385 0.032 0.597 -0.080 0.015 0.251 0.492 0.102 0.021 567.50 0.357 0.402 0.028 0.596 -0.080 0.015 0.232 0.517 0.104 0.022 572.50 0.334 0.417 0.024 0.595 -0.079 0.016 0.211 0.541 0.107 0.023 577.50 0.313 0.430 0.020 0.593 -0.078 0.016 0.186 0.564 0.109 0.024 582.50 0.290 0.441 0.017 0.592 -0.078 0.017 0.158 0.584 0.111 0.026 587.50 0.268 0.448 0.013 0.590 -0.077 0.017 0.128 0.602 0.114 0.027 592.50 0.246 0.453 0.010 0.589 -0.077 0.018 0.095 0.616 0.116 0.029 597.50 0.225 0.455 0.007 0.587 -0.076 0.018 0.060 0.626 0.119 0.030 602.50 0.205 0.454 0.004 0.585 -0.075 0.019 0.024 0.632 0.122 0.032 607.50 0.186 0.452 0.001 0.584 -0.074 0.020 -0.013 0.634 0.125 0.034 612.50 0.169 0.447 -0.002 0.582 -0.073 0.020 -0.049 0.631 0.127 0.036 617.50 0.154 0.441 -0.004 0.581 -0.073 0.021 -0.084 0.624 0.130 0.038 622.50 0.140 0.434 -0.006 0.579 -0.072 0.022 -0.117 0.614 0.133 0.040 627.50 0.128 0.427 -0.009 0.577 -0.071 0.022 -0.148 0.600 0.136 0.043 632.50 0.118 0.418 -0.011 0.576 -0.070 0.023 -0.177 0.584 0.140 0.045 637.50 0.110 0.410 -0.013 0.574 -0.069 0.024 -0.203 0.565 0.143 0.048 642.50 0.103 0.401 -0.015 0.573 -0.068 0.025 -0.226 0.544 0.146 0.051 647.50 0.098 0.392 -0.017 0.571 -0.067 0.026 -0.246 0.522 0.149 0.054 652.50 0.094 0.384 -0.018 0.570 -0.066 0.027 -0.263 0.499 0.153 0.057 657.50 0.091 0.376 -0.020 0.568 -0.064 0.028 -0.277 0.476 0.156 0.060 662.50 0.090 0.368 -0.022 0.566 -0.063 0.029 -0.288 0.453 0.159 0.064 667.50 0.089 0.361 -0.023 0.565 -0.062 0.030 -0.297 0.430 0.163 0.068 672.50 0.089 0.354 -0.024 0.563 -0.061 0.031 -0.303 0.408 0.166 0.072 677.50 0.090 0.348 -0.026 0.562 -0.060 0.032 -0.308 0.387 0.170 0.077 682.50 0.092 0.342 -0.027 0.560 -0.058 0.034 -0.311 0.366 0.174 0.081 687.50 0.095 0.337 -0.028 0.559 -0.057 0.035 -0.313 0.346 0.177 0.086 692.50 0.098 0.332 -0.029 0.557 -0.056 0.036 -0.313 0.328 0.181 0.092 697.50 0.102 0.328 -0.030 0.556 -0.055 0.038 -0.312 0.310 0.184 0.097 702.50 0.106 0.324 -0.031 0.554 -0.053 0.039 -0.310 0.293 0.188 0.103 707.50 0.111 0.320 -0.032 0.553 -0.052 0.041 -0.307 0.278 0.191 0.110 712.50 0.117 0.318 -0.033 0.552 -0.051 0.043 -0.304 0.263 0.194 0.117 717.50 0.123 0.316 -0.034 0.550 -0.050 0.045 -0.300 0.249 0.198 0.124 722.50 0.130 0.314 -0.034 0.549 -0.048 0.046 -0.295 0.236 0.200 0.131 727.50 0.138 0.313 -0.035 0.547 -0.047 0.048 -0.290 0.224 0.203 0.140 732.50 0.146 0.313 -0.036 0.546 -0.046 0.050 -0.285 0.212 0.206 0.148 737.50 0.155 0.313 -0.036 0.545 -0.045 0.052 -0.280 0.202 0.208 0.157 742.50 0.164 0.315 -0.037 0.543 -0.043 0.054 -0.274 0.192 0.210 0.167 747.50 0.174 0.317 -0.037 0.542 -0.042 0.056 -0.269 0.183 0.211 0.177 752.50 0.184 0.320 -0.038 0.541 -0.041 0.059 -0.263 0.174 0.212 0.187 757.50 0.196 0.325 -0.038 0.539 -0.040 0.061 -0.257 0.166 0.213 0.198 762.50 0.207 0.331 -0.038 0.538 -0.039 0.063 -0.251 0.159 0.213 0.209 767.50 0.219 0.338 -0.039 0.537 -0.038 0.066 -0.245 0.152 0.212 0.221 772.50 0.231 0.348 -0.039 0.535 -0.037 0.068 -0.239 0.145 0.210 0.233 777.50 0.244 0.359 -0.039 0.534 -0.036 0.071 -0.233 0.139 0.208 0.246 782.50 0.256 0.372 -0.039 0.533 -0.035 0.074 -0.227 0.134 0.204 0.258 787.50 0.267 0.388 -0.040 0.531 -0.034 0.076 -0.221 0.128 0.200 0.271 792.50 0.278 0.406 -0.040 0.530 -0.033 0.079 -0.216 0.124 0.195 0.284 797.50 0.287 0.426 -0.040 0.529 -0.033 0.082 -0.210 0.119 0.188 0.297 802.50 0.294 0.448 -0.040 0.528 -0.032 0.085 -0.204 0.115 0.181 0.309 807.50 0.298 0.472 -0.040 0.527 -0.031 0.087 -0.199 0.111 0.172 0.321 812.50 0.300 0.498 -0.040 0.525 -0.031 0.090 -0.193 0.107 0.163 0.333 817.50 0.299 0.524 -0.040 0.524 -0.031 0.093 -0.188 0.104 0.152 0.345 822.50 0.294 0.551 -0.040 0.523 -0.030 0.096 -0.183 0.101 0.141 0.355 827.50 0.285 0.577 -0.040 0.522 -0.030 0.099 -0.177 0.098 0.128 0.365 832.50 0.274 0.603 -0.040 0.521 -0.030 0.102 -0.172 0.096 0.115 0.373 837.50 0.259 0.626 -0.039 0.520 -0.030 0.105 -0.167 0.093 0.100 0.381 842.50 0.242 0.647 -0.039 0.519 -0.030 0.108 -0.162 0.091 0.086 0.388 847.50 0.223 0.666 -0.039 0.517 -0.030 0.111 -0.157 0.089 0.071 0.393 852.50 0.203 0.681 -0.039 0.516 -0.030 0.114 -0.153 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2587.50 -0.251 0.466 -0.075 0.587 -0.208 0.309 -0.033 0.341 -0.101 0.169 2592.50 -0.252 0.466 -0.076 0.587 -0.208 0.310 -0.033 0.341 -0.101 0.168 2597.50 -0.254 0.467 -0.077 0.588 -0.209 0.310 -0.033 0.342 -0.101 0.168 Tlab 3,1,5 3,1,7 4,1,7 4,1,9 5,1,9 2.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 7.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 12.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 17.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 22.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 27.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 32.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 37.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 42.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 47.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 52.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 57.50 0.000 0.000 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2437.50 -0.028 0.007 0.002 0.066 -0.024 0.007 0.019 0.042 -0.029 0.022 2442.50 -0.028 0.007 0.001 0.066 -0.025 0.007 0.019 0.042 -0.029 0.022 2447.50 -0.029 0.007 0.001 0.066 -0.025 0.007 0.019 0.043 -0.030 0.022 2452.50 -0.029 0.007 0.001 0.067 -0.025 0.008 0.019 0.043 -0.030 0.022 2457.50 -0.029 0.007 0.000 0.067 -0.025 0.008 0.019 0.044 -0.030 0.023 2462.50 -0.029 0.007 0.000 0.067 -0.025 0.008 0.019 0.044 -0.030 0.023 2467.50 -0.029 0.007 0.000 0.067 -0.025 0.008 0.019 0.044 -0.030 0.023 2472.50 -0.029 0.007 -0.001 0.068 -0.026 0.008 0.019 0.045 -0.031 0.023 2477.50 -0.029 0.007 -0.001 0.068 -0.026 0.008 0.019 0.045 -0.031 0.023 2482.50 -0.029 0.007 -0.001 0.068 -0.026 0.008 0.019 0.046 -0.031 0.024 2487.50 -0.029 0.007 -0.002 0.068 -0.026 0.008 0.019 0.046 -0.032 0.024 2492.50 -0.029 0.007 -0.002 0.068 -0.026 0.008 0.019 0.047 -0.032 0.024 2497.50 -0.029 0.007 -0.003 0.069 -0.026 0.008 0.019 0.047 -0.032 0.024 2502.50 -0.029 0.007 -0.003 0.069 -0.027 0.008 0.019 0.047 -0.032 0.024 2507.50 -0.030 0.007 -0.003 0.069 -0.027 0.008 0.019 0.048 -0.033 0.025 2512.50 -0.030 0.006 -0.004 0.069 -0.027 0.008 0.019 0.048 -0.033 0.025 2517.50 -0.030 0.006 -0.004 0.069 -0.027 0.008 0.019 0.049 -0.033 0.025 2522.50 -0.030 0.006 -0.004 0.070 -0.027 0.008 0.019 0.049 -0.033 0.025 2527.50 -0.030 0.006 -0.005 0.070 -0.027 0.008 0.019 0.050 -0.034 0.026 2532.50 -0.030 0.006 -0.005 0.070 -0.028 0.008 0.019 0.050 -0.034 0.026 2537.50 -0.030 0.006 -0.006 0.070 -0.028 0.008 0.019 0.051 -0.034 0.026 2542.50 -0.030 0.006 -0.006 0.070 -0.028 0.008 0.019 0.051 -0.034 0.026 2547.50 -0.030 0.006 -0.006 0.071 -0.028 0.008 0.019 0.052 -0.035 0.027 2552.50 -0.030 0.006 -0.007 0.071 -0.028 0.008 0.019 0.052 -0.035 0.027 2557.50 -0.030 0.006 -0.007 0.071 -0.028 0.008 0.019 0.052 -0.035 0.027 2562.50 -0.031 0.006 -0.008 0.071 -0.029 0.008 0.019 0.053 -0.035 0.027 2567.50 -0.031 0.006 -0.008 0.071 -0.029 0.008 0.019 0.053 -0.036 0.028 2572.50 -0.031 0.006 -0.008 0.072 -0.029 0.008 0.019 0.054 -0.036 0.028 2577.50 -0.031 0.006 -0.009 0.072 -0.029 0.008 0.019 0.054 -0.036 0.028 2582.50 -0.031 0.006 -0.009 0.072 -0.029 0.008 0.019 0.055 -0.036 0.028 2587.50 -0.031 0.006 -0.010 0.072 -0.029 0.008 0.019 0.055 -0.037 0.029 2592.50 -0.031 0.006 -0.010 0.072 -0.030 0.008 0.019 0.056 -0.037 0.029 2597.50 -0.031 0.006 -0.010 0.073 -0.030 0.008 0.019 0.056 -0.037 0.029 # Isospin = 3/2 Tlab 0,3,1 1,3,1 1,3,3 2,3,3 2,3,5 2.50 -0.013 0.000 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 7.50 -0.025 0.001 -0.001 0.000 0.005 0.000 0.000 0.000 0.000 0.000 12.50 -0.033 0.001 -0.002 0.000 0.011 0.000 0.000 0.000 0.000 0.000 17.50 -0.042 0.002 -0.003 0.000 0.018 0.000 0.000 0.000 0.000 0.000 22.50 -0.049 0.002 -0.005 0.000 0.027 0.001 0.000 0.000 0.000 0.000 27.50 -0.057 0.003 -0.006 0.000 0.037 0.001 0.000 0.000 0.000 0.000 32.50 -0.064 0.004 -0.008 0.000 0.049 0.002 0.000 0.000 0.000 0.000 37.50 -0.071 0.005 -0.009 0.000 0.062 0.004 0.000 0.000 0.000 0.000 42.50 -0.078 0.006 -0.011 0.000 0.076 0.006 0.000 0.000 0.000 0.000 47.50 -0.085 0.007 -0.013 0.000 0.091 0.008 0.000 0.000 0.000 0.000 52.50 -0.092 0.009 -0.015 0.000 0.109 0.012 0.000 0.000 -0.001 0.000 57.50 -0.099 0.010 -0.017 0.000 0.127 0.016 0.000 0.000 -0.001 0.000 62.50 -0.106 0.011 -0.019 0.000 0.147 0.022 0.001 0.000 -0.001 0.000 67.50 -0.112 0.013 -0.021 0.000 0.169 0.029 0.001 0.000 -0.001 0.000 72.50 -0.119 0.014 -0.024 0.001 0.192 0.038 0.001 0.000 -0.001 0.000 77.50 -0.125 0.016 -0.026 0.001 0.217 0.049 0.001 0.000 -0.001 0.000 82.50 -0.132 0.018 -0.028 0.001 0.243 0.063 0.001 0.000 -0.001 0.000 87.50 -0.138 0.019 -0.031 0.001 0.270 0.079 0.001 0.000 -0.002 0.000 92.50 -0.144 0.021 -0.033 0.001 0.298 0.099 0.001 0.000 -0.002 0.000 97.50 -0.151 0.023 -0.035 0.001 0.328 0.122 0.001 0.000 -0.002 0.000 102.50 -0.157 0.025 -0.038 0.001 0.357 0.150 0.001 0.000 -0.002 0.000 107.50 -0.163 0.027 -0.040 0.002 0.387 0.183 0.002 0.000 -0.003 0.000 112.50 -0.169 0.029 -0.043 0.002 0.415 0.221 0.002 0.000 -0.003 0.000 117.50 -0.174 0.031 -0.046 0.002 0.442 0.265 0.002 0.000 -0.003 0.000 122.50 -0.180 0.034 -0.048 0.002 0.465 0.316 0.002 0.000 -0.003 0.000 127.50 -0.186 0.036 -0.051 0.003 0.483 0.372 0.002 0.000 -0.004 0.000 132.50 -0.191 0.038 -0.053 0.003 0.496 0.434 0.002 0.000 -0.004 0.000 137.50 -0.197 0.040 -0.056 0.003 0.500 0.501 0.002 0.000 -0.004 0.000 142.50 -0.202 0.043 -0.059 0.003 0.495 0.571 0.003 0.000 -0.005 0.000 147.50 -0.207 0.045 -0.062 0.004 0.479 0.643 0.003 0.000 -0.005 0.000 152.50 -0.213 0.047 -0.064 0.004 0.452 0.714 0.003 0.000 -0.005 0.000 157.50 -0.218 0.050 -0.067 0.005 0.413 0.781 0.003 0.000 -0.005 0.000 162.50 -0.223 0.052 -0.070 0.005 0.364 0.842 0.003 0.000 -0.006 0.000 167.50 -0.228 0.055 -0.072 0.005 0.306 0.895 0.003 0.000 -0.006 0.000 172.50 -0.232 0.057 -0.075 0.006 0.241 0.938 0.003 0.000 -0.007 0.000 177.50 -0.237 0.060 -0.078 0.006 0.172 0.969 0.004 0.000 -0.007 0.000 182.50 -0.242 0.062 -0.081 0.007 0.102 0.989 0.004 0.000 -0.007 0.000 187.50 -0.246 0.065 -0.084 0.007 0.032 0.999 0.004 0.000 -0.008 0.000 192.50 -0.251 0.068 -0.086 0.008 -0.034 0.998 0.004 0.000 -0.008 0.000 197.50 -0.255 0.070 -0.089 0.008 -0.097 0.990 0.004 0.000 -0.008 0.000 202.50 -0.259 0.073 -0.092 0.009 -0.154 0.975 0.004 0.000 -0.009 0.000 207.50 -0.264 0.076 -0.095 0.009 -0.206 0.955 0.004 0.000 -0.009 0.000 212.50 -0.268 0.078 -0.098 0.010 -0.252 0.931 0.004 0.000 -0.009 0.000 217.50 -0.272 0.081 -0.100 0.011 -0.293 0.904 0.004 0.000 -0.010 0.000 222.50 -0.276 0.084 -0.103 0.011 -0.328 0.876 0.004 0.000 -0.010 0.000 227.50 -0.280 0.086 -0.106 0.012 -0.358 0.847 0.005 0.000 -0.011 0.000 232.50 -0.284 0.089 -0.109 0.013 -0.384 0.818 0.005 0.000 -0.011 0.000 237.50 -0.287 0.092 -0.111 0.013 -0.407 0.789 0.005 0.000 -0.011 0.000 242.50 -0.291 0.095 -0.114 0.014 -0.425 0.760 0.005 0.000 -0.012 0.000 247.50 -0.295 0.097 -0.117 0.015 -0.441 0.733 0.005 0.000 -0.012 0.000 252.50 -0.298 0.100 -0.120 0.016 -0.454 0.706 0.005 0.000 -0.013 0.000 257.50 -0.302 0.103 -0.122 0.017 -0.465 0.680 0.005 0.000 -0.013 0.000 262.50 -0.305 0.105 -0.125 0.018 -0.474 0.655 0.005 0.000 -0.013 0.000 267.50 -0.309 0.108 -0.128 0.018 -0.481 0.631 0.005 0.000 -0.014 0.000 272.50 -0.312 0.111 -0.130 0.019 -0.487 0.609 0.005 0.000 -0.014 0.000 277.50 -0.316 0.114 -0.133 0.020 -0.491 0.587 0.005 0.001 -0.015 0.000 282.50 -0.319 0.116 -0.136 0.021 -0.494 0.566 0.005 0.001 -0.015 0.000 287.50 -0.322 0.119 -0.138 0.022 -0.497 0.547 0.005 0.001 -0.016 0.000 292.50 -0.325 0.122 -0.141 0.023 -0.498 0.528 0.005 0.001 -0.016 0.000 297.50 -0.328 0.124 -0.143 0.024 -0.499 0.510 0.006 0.001 -0.016 0.000 302.50 -0.331 0.127 -0.146 0.025 -0.499 0.493 0.006 0.001 -0.017 0.000 307.50 -0.335 0.130 -0.148 0.026 -0.498 0.476 0.006 0.001 -0.017 0.000 312.50 -0.337 0.133 -0.151 0.027 -0.498 0.460 0.006 0.001 -0.018 0.000 317.50 -0.340 0.135 -0.153 0.029 -0.496 0.445 0.006 0.001 -0.018 0.000 322.50 -0.343 0.138 -0.156 0.030 -0.494 0.431 0.006 0.001 -0.019 0.000 327.50 -0.346 0.141 -0.158 0.031 -0.492 0.417 0.006 0.002 -0.019 0.000 332.50 -0.349 0.143 -0.161 0.032 -0.490 0.404 0.006 0.002 -0.019 0.000 337.50 -0.352 0.146 -0.163 0.033 -0.487 0.391 0.006 0.002 -0.020 0.000 342.50 -0.354 0.148 -0.166 0.035 -0.485 0.379 0.006 0.002 -0.020 0.000 347.50 -0.357 0.151 -0.168 0.036 -0.482 0.367 0.006 0.002 -0.021 0.001 352.50 -0.359 0.154 -0.170 0.037 -0.478 0.356 0.006 0.003 -0.021 0.001 357.50 -0.362 0.156 -0.173 0.039 -0.475 0.345 0.006 0.003 -0.021 0.001 362.50 -0.364 0.159 -0.175 0.040 -0.472 0.334 0.006 0.003 -0.022 0.001 367.50 -0.367 0.161 -0.177 0.042 -0.468 0.324 0.007 0.003 -0.022 0.001 372.50 -0.369 0.164 -0.180 0.043 -0.464 0.314 0.007 0.004 -0.023 0.001 377.50 -0.371 0.167 -0.182 0.044 -0.460 0.305 0.007 0.004 -0.023 0.001 382.50 -0.373 0.169 -0.184 0.046 -0.456 0.296 0.007 0.004 -0.023 0.001 387.50 -0.376 0.172 -0.187 0.048 -0.452 0.287 0.007 0.005 -0.024 0.001 392.50 -0.378 0.174 -0.189 0.049 -0.448 0.278 0.007 0.005 -0.024 0.001 397.50 -0.380 0.176 -0.191 0.051 -0.444 0.270 0.007 0.006 -0.025 0.001 402.50 -0.382 0.179 -0.194 0.052 -0.439 0.261 0.007 0.006 -0.025 0.001 407.50 -0.383 0.181 -0.196 0.054 -0.435 0.253 0.007 0.007 -0.025 0.001 412.50 -0.385 0.183 -0.198 0.056 -0.430 0.246 0.007 0.007 -0.026 0.001 417.50 -0.387 0.186 -0.201 0.057 -0.426 0.238 0.007 0.007 -0.026 0.001 422.50 -0.389 0.188 -0.203 0.059 -0.421 0.231 0.008 0.008 -0.027 0.001 427.50 -0.390 0.190 -0.205 0.061 -0.416 0.224 0.008 0.009 -0.027 0.001 432.50 -0.392 0.192 -0.208 0.062 -0.412 0.217 0.008 0.009 -0.027 0.001 437.50 -0.393 0.195 -0.210 0.064 -0.407 0.211 0.008 0.010 -0.028 0.001 442.50 -0.395 0.197 -0.212 0.066 -0.402 0.204 0.008 0.010 -0.028 0.001 447.50 -0.396 0.199 -0.215 0.067 -0.397 0.198 0.008 0.011 -0.029 0.001 452.50 -0.397 0.201 -0.217 0.069 -0.392 0.192 0.008 0.012 -0.029 0.001 457.50 -0.398 0.203 -0.219 0.071 -0.387 0.186 0.008 0.012 -0.029 0.001 462.50 -0.399 0.205 -0.222 0.072 -0.382 0.180 0.008 0.013 -0.030 0.001 467.50 -0.400 0.207 -0.224 0.074 -0.377 0.175 0.009 0.014 -0.030 0.001 472.50 -0.401 0.208 -0.226 0.076 -0.371 0.170 0.009 0.015 -0.030 0.001 477.50 -0.402 0.210 -0.229 0.077 -0.366 0.165 0.009 0.015 -0.031 0.001 482.50 -0.403 0.212 -0.231 0.079 -0.361 0.160 0.009 0.016 -0.031 0.001 487.50 -0.403 0.213 -0.233 0.081 -0.355 0.155 0.009 0.017 -0.031 0.002 492.50 -0.404 0.215 -0.236 0.082 -0.350 0.150 0.009 0.018 -0.032 0.002 497.50 -0.404 0.217 -0.238 0.084 -0.345 0.146 0.009 0.019 -0.032 0.002 502.50 -0.404 0.218 -0.241 0.085 -0.339 0.142 0.010 0.020 -0.032 0.002 507.50 -0.405 0.219 -0.243 0.087 -0.334 0.138 0.010 0.021 -0.033 0.002 512.50 -0.405 0.221 -0.245 0.089 -0.328 0.134 0.010 0.022 -0.033 0.002 517.50 -0.405 0.222 -0.248 0.090 -0.323 0.130 0.010 0.023 -0.033 0.002 522.50 -0.404 0.223 -0.250 0.092 -0.317 0.127 0.010 0.024 -0.034 0.002 527.50 -0.404 0.224 -0.252 0.093 -0.312 0.123 0.010 0.025 -0.034 0.002 532.50 -0.403 0.226 -0.255 0.095 -0.306 0.120 0.010 0.026 -0.034 0.002 537.50 -0.403 0.227 -0.257 0.096 -0.301 0.117 0.011 0.027 -0.035 0.002 542.50 -0.402 0.228 -0.259 0.098 -0.295 0.114 0.011 0.028 -0.035 0.002 547.50 -0.401 0.228 -0.261 0.099 -0.290 0.112 0.011 0.030 -0.035 0.002 552.50 -0.400 0.229 -0.264 0.100 -0.285 0.109 0.011 0.031 -0.036 0.002 557.50 -0.399 0.230 -0.266 0.102 -0.279 0.107 0.011 0.032 -0.036 0.002 562.50 -0.397 0.231 -0.268 0.103 -0.274 0.104 0.011 0.034 -0.036 0.002 567.50 -0.395 0.231 -0.270 0.105 -0.268 0.102 0.012 0.035 -0.036 0.002 572.50 -0.393 0.232 -0.273 0.106 -0.263 0.100 0.012 0.037 -0.037 0.002 577.50 -0.391 0.233 -0.275 0.107 -0.258 0.098 0.012 0.038 -0.037 0.002 582.50 -0.389 0.233 -0.277 0.108 -0.253 0.097 0.012 0.040 -0.037 0.003 587.50 -0.386 0.234 -0.279 0.110 -0.247 0.095 0.012 0.041 -0.037 0.003 592.50 -0.383 0.234 -0.281 0.111 -0.242 0.094 0.012 0.043 -0.038 0.003 597.50 -0.380 0.235 -0.283 0.112 -0.237 0.093 0.012 0.045 -0.038 0.003 602.50 -0.377 0.235 -0.286 0.113 -0.232 0.091 0.012 0.046 -0.038 0.003 607.50 -0.373 0.236 -0.288 0.114 -0.227 0.090 0.012 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0.003 0.242 -0.208 0.329 -0.017 0.171 2547.50 -0.046 0.489 -0.122 0.637 0.003 0.242 -0.208 0.330 -0.017 0.171 2552.50 -0.043 0.489 -0.120 0.638 0.003 0.242 -0.208 0.330 -0.017 0.172 2557.50 -0.039 0.488 -0.119 0.640 0.004 0.242 -0.208 0.331 -0.017 0.172 2562.50 -0.036 0.487 -0.118 0.641 0.004 0.241 -0.209 0.332 -0.017 0.172 2567.50 -0.033 0.486 -0.117 0.642 0.004 0.241 -0.209 0.333 -0.017 0.173 2572.50 -0.029 0.486 -0.116 0.643 0.004 0.241 -0.209 0.333 -0.018 0.173 2577.50 -0.026 0.485 -0.115 0.644 0.004 0.241 -0.209 0.334 -0.018 0.173 2582.50 -0.022 0.485 -0.114 0.645 0.004 0.240 -0.209 0.335 -0.018 0.173 2587.50 -0.019 0.484 -0.113 0.647 0.005 0.240 -0.209 0.336 -0.018 0.174 2592.50 -0.015 0.484 -0.112 0.648 0.005 0.240 -0.209 0.336 -0.018 0.174 2597.50 -0.012 0.483 -0.110 0.649 0.005 0.240 -0.209 0.337 -0.018 0.174 Tlab 3,3,5 3,3,7 4,3,7 4,3,9 5,3,9 2.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 7.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 12.50 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0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 92.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 97.50 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 0.000 102.50 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 107.50 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 112.50 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 117.50 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 122.50 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 127.50 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 132.50 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 137.50 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 142.50 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 147.50 0.000 0.000 0.001 0.000 0.000 0.000 0.000 0.000 0.000 0.000 152.50 0.000 0.000 0.002 0.000 0.000 0.000 0.000 0.000 0.000 0.000 157.50 0.000 0.000 0.002 0.000 0.000 0.000 0.000 0.000 0.000 0.000 162.50 0.000 0.000 0.002 0.000 0.000 0.000 0.000 0.000 0.000 0.000 167.50 0.000 0.000 0.002 0.000 0.000 0.000 0.000 0.000 0.000 0.000 172.50 0.000 0.000 0.002 0.000 0.000 0.000 0.000 0.000 0.000 0.000 177.50 0.000 0.000 0.002 0.000 0.000 0.000 0.000 0.000 0.000 0.000 182.50 0.000 0.000 0.003 0.000 0.000 0.000 0.000 0.000 0.000 0.000 187.50 0.000 0.000 0.003 0.000 0.000 0.000 0.000 0.000 0.000 0.000 192.50 0.000 0.000 0.003 0.000 0.000 0.000 0.000 0.000 0.000 0.000 197.50 0.000 0.000 0.003 0.000 0.000 0.000 0.000 0.000 0.000 0.000 202.50 0.000 0.000 0.003 0.000 0.000 0.000 0.000 0.000 0.000 0.000 207.50 0.000 0.000 0.004 0.000 0.000 0.000 0.000 0.000 0.000 0.000 212.50 0.000 0.000 0.004 0.000 0.000 0.000 0.000 0.000 0.000 0.000 217.50 0.000 0.000 0.004 0.000 0.000 0.000 0.000 0.000 0.000 0.000 222.50 0.000 0.000 0.004 0.000 0.000 0.000 0.000 0.000 0.000 0.000 227.50 0.000 0.000 0.005 0.000 0.000 0.000 0.000 0.000 0.000 0.000 232.50 0.000 0.000 0.005 0.000 0.000 0.000 0.000 0.000 0.000 0.000 237.50 0.000 0.000 0.005 0.000 0.000 0.000 0.000 0.000 0.000 0.000 242.50 -0.001 0.000 0.005 0.000 0.000 0.000 0.000 0.000 0.000 0.000 247.50 -0.001 0.000 0.006 0.000 0.000 0.000 0.000 0.000 0.000 0.000 252.50 -0.001 0.000 0.006 0.000 0.000 0.000 0.000 0.000 0.000 0.000 257.50 -0.001 0.000 0.006 0.000 0.000 0.000 0.000 0.000 0.000 0.000 262.50 -0.001 0.000 0.007 0.000 0.000 0.000 0.000 0.000 0.000 0.000 267.50 -0.001 0.000 0.007 0.000 0.000 0.000 0.000 0.000 0.000 0.000 272.50 -0.001 0.000 0.007 0.000 0.000 0.000 0.000 0.000 0.000 0.000 277.50 -0.001 0.000 0.008 0.000 0.000 0.000 0.000 0.000 0.000 0.000 282.50 -0.001 0.000 0.008 0.000 0.000 0.000 0.000 0.000 0.000 0.000 287.50 -0.001 0.000 0.008 0.000 0.000 0.000 0.000 0.000 0.000 0.000 292.50 -0.001 0.000 0.009 0.000 0.000 0.000 0.000 0.000 0.000 0.000 297.50 -0.001 0.000 0.009 0.000 0.000 0.000 0.000 0.000 0.000 0.000 302.50 -0.001 0.000 0.009 0.000 0.000 0.000 0.000 0.000 0.000 0.000 307.50 -0.001 0.000 0.010 0.000 0.000 0.000 0.000 0.000 0.000 0.000 312.50 -0.001 0.000 0.010 0.000 0.000 0.000 0.000 0.000 0.000 0.000 317.50 -0.001 0.000 0.011 0.000 0.000 0.000 0.000 0.000 0.000 0.000 322.50 -0.001 0.000 0.011 0.000 0.000 0.000 0.000 0.000 0.000 0.000 327.50 -0.001 0.000 0.011 0.000 0.000 0.000 0.000 0.000 0.000 0.000 332.50 -0.001 0.000 0.012 0.000 0.000 0.000 0.000 0.000 0.000 0.000 337.50 -0.002 0.000 0.012 0.000 0.000 0.000 0.000 0.000 0.000 0.000 342.50 -0.002 0.000 0.013 0.000 0.000 0.000 0.000 0.000 0.000 0.000 347.50 -0.002 0.000 0.013 0.000 0.000 0.000 0.000 0.000 0.000 0.000 352.50 -0.002 0.000 0.014 0.000 0.001 0.000 0.000 0.000 0.000 0.000 357.50 -0.002 0.000 0.014 0.000 0.001 0.000 0.000 0.000 0.000 0.000 362.50 -0.002 0.000 0.015 0.000 0.001 0.000 0.000 0.000 0.000 0.000 367.50 -0.002 0.000 0.015 0.000 0.001 0.000 0.000 0.000 0.000 0.000 372.50 -0.002 0.000 0.016 0.000 0.001 0.000 0.000 0.000 0.000 0.000 377.50 -0.002 0.000 0.016 0.000 0.001 0.000 0.000 0.000 0.000 0.000 382.50 -0.002 0.000 0.017 0.000 0.001 0.000 0.000 0.000 0.000 0.000 387.50 -0.002 0.000 0.017 0.000 0.001 0.000 0.000 0.000 0.000 0.000 392.50 -0.002 0.000 0.018 0.000 0.001 0.000 0.000 0.000 0.000 0.000 397.50 -0.002 0.000 0.018 0.000 0.001 0.000 0.000 0.000 0.000 0.000 402.50 -0.002 0.000 0.019 0.001 0.001 0.000 0.000 0.000 0.000 0.000 407.50 -0.003 0.000 0.019 0.001 0.001 0.000 0.000 0.000 0.000 0.000 412.50 -0.003 0.000 0.020 0.001 0.001 0.000 0.000 0.000 0.000 0.000 417.50 -0.003 0.000 0.020 0.001 0.001 0.000 0.000 0.000 0.000 0.000 422.50 -0.003 0.000 0.021 0.001 0.001 0.000 0.000 0.000 0.000 0.000 427.50 -0.003 0.001 0.022 0.001 0.001 0.000 0.000 0.000 0.000 0.000 432.50 -0.003 0.001 0.022 0.001 0.001 0.000 0.000 0.000 0.000 0.000 437.50 -0.003 0.001 0.023 0.001 0.001 0.000 0.000 0.000 0.000 0.000 442.50 -0.003 0.001 0.024 0.001 0.001 0.000 0.000 0.000 0.000 0.000 447.50 -0.003 0.001 0.024 0.001 0.001 0.000 0.000 0.000 0.000 0.000 452.50 -0.003 0.001 0.025 0.001 0.001 0.000 0.000 0.000 0.000 0.000 457.50 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0.000 0.000 532.50 -0.004 0.002 0.037 0.002 0.001 0.000 0.000 0.000 0.000 0.000 537.50 -0.004 0.002 0.038 0.002 0.001 0.000 0.000 0.000 0.000 0.000 542.50 -0.004 0.002 0.039 0.002 0.001 0.000 0.000 0.000 0.000 0.000 547.50 -0.004 0.002 0.039 0.003 0.001 0.000 0.000 0.000 0.000 0.000 552.50 -0.004 0.002 0.040 0.003 0.001 0.000 0.000 0.000 0.000 0.000 557.50 -0.004 0.002 0.041 0.003 0.001 0.000 0.000 0.000 0.000 0.000 562.50 -0.004 0.002 0.042 0.003 0.001 0.000 0.000 0.000 0.000 0.000 567.50 -0.004 0.003 0.043 0.003 0.001 0.000 0.000 0.000 0.000 0.000 572.50 -0.004 0.003 0.044 0.003 0.001 0.000 0.000 0.000 0.000 0.000 577.50 -0.004 0.003 0.045 0.003 0.001 0.000 0.000 0.000 0.000 0.000 582.50 -0.004 0.003 0.046 0.004 0.001 0.000 0.000 0.000 0.000 0.000 587.50 -0.004 0.003 0.047 0.004 0.001 0.000 0.000 0.000 0.000 0.000 592.50 -0.004 0.003 0.048 0.004 0.001 0.000 0.000 0.000 0.000 0.000 597.50 -0.004 0.003 0.049 0.004 0.001 0.000 0.001 0.000 -0.001 0.000 602.50 -0.004 0.004 0.050 0.004 0.001 0.000 0.001 0.000 -0.001 0.000 607.50 -0.004 0.004 0.051 0.004 0.001 0.000 0.001 0.000 -0.001 0.000 612.50 -0.004 0.004 0.052 0.005 0.001 0.000 0.001 0.000 -0.001 0.000 617.50 -0.004 0.004 0.053 0.005 0.001 0.000 0.001 0.000 -0.001 0.000 622.50 -0.004 0.004 0.054 0.005 0.001 0.000 0.001 0.000 -0.001 0.000 627.50 -0.004 0.004 0.056 0.005 0.001 0.000 0.001 0.000 -0.001 0.000 632.50 -0.004 0.005 0.057 0.006 0.001 0.000 0.001 0.000 -0.001 0.000 637.50 -0.004 0.005 0.058 0.006 0.001 0.000 0.001 0.000 -0.001 0.000 642.50 -0.004 0.005 0.059 0.006 0.001 0.000 0.001 0.000 -0.001 0.000 647.50 -0.004 0.005 0.060 0.006 0.001 0.000 0.001 0.000 -0.001 0.000 652.50 -0.004 0.005 0.061 0.007 0.001 0.000 0.001 0.000 -0.001 0.000 657.50 -0.004 0.006 0.063 0.007 0.001 0.000 0.001 0.000 -0.001 0.000 662.50 -0.004 0.006 0.064 0.007 0.001 0.000 0.001 0.000 -0.001 0.000 667.50 -0.004 0.006 0.065 0.008 0.001 0.000 0.001 0.000 -0.001 0.000 672.50 -0.003 0.006 0.067 0.008 0.001 0.000 0.001 0.000 -0.001 0.000 677.50 -0.003 0.007 0.068 0.008 0.001 0.000 0.001 0.000 -0.001 0.000 682.50 -0.003 0.007 0.069 0.009 0.001 0.001 0.001 0.000 -0.001 0.000 687.50 -0.003 0.007 0.071 0.009 0.001 0.001 0.001 0.000 -0.001 0.000 692.50 -0.003 0.007 0.072 0.009 0.001 0.001 0.001 0.000 -0.001 0.000 697.50 -0.003 0.008 0.073 0.010 0.001 0.001 0.001 0.000 -0.001 0.000 702.50 -0.003 0.008 0.075 0.010 0.001 0.001 0.001 0.000 -0.001 0.000 707.50 -0.003 0.008 0.076 0.010 0.001 0.001 0.002 0.000 -0.001 0.000 712.50 -0.003 0.009 0.078 0.011 0.001 0.001 0.002 0.000 -0.001 0.000 717.50 -0.002 0.009 0.079 0.011 0.001 0.001 0.002 0.000 -0.001 0.000 722.50 -0.002 0.009 0.081 0.012 0.001 0.001 0.002 0.000 -0.001 0.000 727.50 -0.002 0.010 0.082 0.012 0.001 0.001 0.002 0.000 -0.001 0.000 732.50 -0.002 0.010 0.084 0.013 0.001 0.001 0.002 0.000 -0.001 0.000 737.50 -0.002 0.010 0.085 0.013 0.001 0.001 0.002 0.001 -0.001 0.001 742.50 -0.002 0.011 0.087 0.014 0.001 0.001 0.002 0.001 -0.001 0.001 747.50 -0.001 0.011 0.089 0.014 0.001 0.001 0.002 0.001 -0.001 0.001 752.50 -0.001 0.012 0.090 0.015 0.001 0.001 0.002 0.001 -0.001 0.001 757.50 -0.001 0.012 0.092 0.016 0.001 0.001 0.002 0.001 -0.001 0.001 762.50 -0.001 0.013 0.094 0.016 0.001 0.001 0.002 0.001 -0.002 0.001 767.50 -0.001 0.013 0.096 0.017 0.001 0.001 0.002 0.001 -0.002 0.001 772.50 0.000 0.014 0.097 0.018 0.001 0.001 0.002 0.001 -0.002 0.001 777.50 0.000 0.014 0.099 0.018 0.001 0.001 0.003 0.001 -0.002 0.001 782.50 0.000 0.015 0.101 0.019 0.001 0.001 0.003 0.001 -0.002 0.001 787.50 0.000 0.015 0.103 0.020 0.001 0.001 0.003 0.001 -0.002 0.001 792.50 0.001 0.016 0.105 0.021 0.001 0.001 0.003 0.001 -0.002 0.001 797.50 0.001 0.016 0.107 0.021 0.001 0.001 0.003 0.001 -0.002 0.001 802.50 0.001 0.017 0.108 0.022 0.001 0.001 0.003 0.001 -0.002 0.001 807.50 0.002 0.017 0.110 0.023 0.001 0.001 0.003 0.001 -0.002 0.001 812.50 0.002 0.018 0.112 0.024 0.001 0.001 0.003 0.001 -0.002 0.001 817.50 0.002 0.019 0.114 0.025 0.001 0.001 0.003 0.001 -0.002 0.001 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    Particle Properties

    A Particle corresponds to one entry/slot in the event record. Its properties therefore is a mix of ones belonging to a particle-as-such, like its identity code or four-momentum, and ones related to the event-as-a-whole, like which mother it has.

    What is stored for each particle is

    • the identity code,
    • the status code,
    • two mother indices,
    • two daughter indices,
    • a colour and an anticolour index,
    • the four-momentum and mass,
    • the scale at which the particle was produced (optional),
    • the polarization/spin/helicity of the particle (optional),
    • the production vertex and proper lifetime (optional),
    • a pointer to the particle kind in the particle data table, and
    • a pointer to the event the particle belongs to.
    From these, a number of further quantities may be derived.

    Basic output methods

    The following member functions can be used to extract the most important information: the identity of a particle, according to the PDG particle codes Yao06. status code. The status code includes information on how a particle was produced, i.e. where in the program execution it was inserted into the event record, and why. It also tells whether the particle is still present or not. It does not tell how a particle disappeared, whether by a decay, a shower branching, a hadronization process, or whatever, but this is implicit in the status code of its daughter(s). The basic scheme is:
    • status = +- (10 * i + j)
    • + : still remaining particles
    • - : decayed/branched/fragmented/... and not remaining
    • i = 1 - 9 : stage of event generation inside PYTHIA
    • i = 10 -19 : reserved for future expansion
    • i >= 20 : free for add-on programs
    • j = 1 - 9 : further specification
    In detail, the list of used or foreseen status codes is:
    • 11 - 19 : beam particles
      • 11 : the event as a whole
      • 12 : incoming beam
      • 13 : incoming beam-inside-beam (e.g. gamma inside e)
      • 14 : outgoing elastically scattered
      • 15 : outgoing diffractively scattered
    • 21 - 29 : particles of the hardest subprocess
      • 21 : incoming
      • 22 : intermediate (intended to have preserved mass)
      • 23 : outgoing
    • 31 - 39 : particles of subsequent subprocesses
      • 31 : incoming
      • 32 : intermediate (intended to have preserved mass)
      • 33 : outgoing
      • 34 : incoming that has already scattered
    • 41 - 49 : particles produced by initial-state-showers
      • 41 : incoming on spacelike main branch
      • 42 : incoming copy of recoiler
      • 43 : outgoing produced by a branching
      • 44 : outgoing shifted by a branching
      • 45 : incoming rescattered parton, with changed kinematics owing to ISR in the mother system (cf. status 34)
      • 46 : incoming copy of recoiler when this is a rescattered parton (cf. status 42)
      • 47 : a W or Z gauge boson produced in the shower evolution
    • 51 - 59 : particles produced by final-state-showers
      • 51 : outgoing produced by parton branching
      • 52 : outgoing copy of recoiler, with changed momentum
      • 53 : copy of recoiler when this is incoming parton, with changed momentum
      • 54 : copy of a recoiler, when in the initial state of a different system from the radiator
      • 55 : copy of a recoiler, when in the final state of a different system from the radiator
      • 56 : a W or Z gauge boson produced in the shower evolution
    • 61 - 69 : particles produced by beam-remnant treatment
      • 61 : incoming subprocess particle with primordial kT included
      • 62 : outgoing subprocess particle with primordial kT included
      • 63 : outgoing beam remnant
    • 71 - 79 : partons in preparation of hadronization process
      • 71 : copied partons to collect into contiguous colour singlet
      • 72 : copied recoiling singlet when ministring collapses to one hadron and momentum has to be reshuffled
      • 73 : combination of very nearby partons into one
      • 74 : combination of two junction quarks (+ nearby gluons) to a diquark
      • 75 : gluons split to decouple a junction-antijunction pair
      • 76 : partons with momentum shuffled to decouple a junction-antijunction pair
      • 77 : temporary opposing parton when fragmenting first two strings in to junction (should disappear again)
      • 78 : temporary combined diquark end when fragmenting last string in to junction (should disappear again)
    • 81 - 89 : primary hadrons produced by hadronization process
      • 81 : from ministring into one hadron
      • 82 : from ministring into two hadrons
      • 83, 84 : from normal string (the difference between the two is technical, whether fragmented off from the top of the string system or from the bottom, useful for debug only)
      • 85, 86 : primary produced hadrons in junction fragmentation of the first two string legs in to the junction, in order of treatment
    • 91 - 99 : particles produced in decay process, or by Bose-Einstein effects
      • 91 : normal decay products
      • 92 : decay products after oscillation B0 <-> B0bar or B_s0 <-> B_s0bar
      • 93, 94 : decay handled by external program, normally or with oscillation
      • 99 : particles with momenta shifted by Bose-Einstein effects (not a proper decay, but bookkept as an 1 -> 1 such, happening after decays of short-lived resonances but before decays of longer-lived particles)
    • 101 - 109 : particles in the handling of R-hadron production and decay, i.e. long-lived (or stable) particles containing a very heavy flavour
      • 101 : when a string system contains two such long-lived particles, the system is split up by the production of a new q-qbar pair (bookkept as decay chains that seemingly need not conserve flavour etc., but do when considered together)
      • 102 : partons rearranged from the long-lived particle end to prepare for fragmentation from this end
      • 103 : intermediate "half-R-hadron" formed when a colour octet particle (like the gluino) has been fragmented on one side, but not yet on the other
      • 104 : an R-hadron
      • 105 : partons or particles formed together with the R-hadron during the fragmentation treatment
      • 106 : subdivision of an R-hadron into its flavour content, with momentum split accordingly, in preparation of the decay of the heavy new particle, if it is unstable
      • 107 : two temporary leftover gluons joined into one in the formation of a gluino-gluon R-hadron.
    • 111 - 199 : reserved for future expansion
    • 201 - : free to be used by anybody
    the indices in the event record where the first and last mothers are stored, if any. There are five allowed combinations of mother1 and mother2:
    1. mother1 = mother2 = 0: for lines 0 - 2, where line 0 represents the event as a whole, and 1 and 2 the two incoming beam particles;
    2. mother1 = mother2 > 0: the particle is a "carbon copy" of its mother, but with changed momentum as a "recoil" effect, e.g. in a shower;
    3. mother1 > 0, mother2 = 0: the "normal" mother case, where it is meaningful to speak of one single mother to several products, in a shower or decay;
    4. mother1 < mother2, both > 0, for abs(status) = 81 - 86: primary hadrons produced from the fragmentation of a string spanning the range from mother1 to mother2, so that all partons in this range should be considered mothers; and analogously for abs(status) = 101 - 106, the formation of R-hadrons;
    5. mother1 < mother2, both > 0, except case 4: particles with two truly different mothers, in particular the particles emerging from a hard 2 -> n interaction.
    Note 1: in backwards evolution of initial-state showers, the mother may well appear below the daughter in the event record. Note 2: the motherList() method below returns a vector of all the mothers, providing a uniform representation for all five cases.
    the indices in the event record where the first and last daughters are stored, if any. There are five allowed combinations of daughter1 and daughter2:
    1. daughter1 = daughter2 = 0: there are no daughters (so far);
    2. daughter1 = daughter2 > 0: the particle has a "carbon copy" as its sole daughter, but with changed momentum as a "recoil" effect, e.g. in a shower;
    3. daughter1 > 0, daughter2 = 0: each of the incoming beams has only (at most) one daughter, namely the initiator parton of the hardest interaction; further, in a 2 -> 1 hard interaction, like q qbar -> Z^0, or in a clustering of two nearby partons, the initial partons only have this one daughter;
    4. daughter1 < daughter2, both > 0: the particle has a range of decay products from daughter1 to daughter2;
    5. daughter2 < daughter1, both > 0: the particle has two separately stored decay products (e.g. in backwards evolution of initial-state showers).
    Note 1: in backwards evolution of initial-state showers, the daughters may well appear below the mother in the event record. Note 2: the mother-daughter relation normally is reciprocal, but not always. An example is hadron beams (indices 1 and 2), where each beam remnant and the initiator of each multiparton interaction has the respective beam as mother, but the beam itself only has the initiator of the hardest interaction as daughter. Note 3: the daughterList() method below returns a vector of all the daughters, providing a uniform representation for all five cases. With this method, also all the daughters of the beams are caught, with the initiators of the basic process given first, while the rest are in no guaranteed order (since they are found by a scanning of the event record for particles with the beam as mother, with no further information).
    the colour and anticolour tags, Les Houches Accord Boo01 style (starting from tag 101 by default, see below). Note: in the preliminary implementation of colour sextets (exotic BSM particles) that exists since PYTHIA 8.150, a negative anticolour tag is interpreted as an additional positive colour tag, and vice versa. the particle four-momentum components. the particle four-momentum vector, with components as above. the particle mass, stored with a minus sign (times the absolute value) for spacelike virtual particles. the scale at which a parton was produced, which can be used to restrict its radiation to lower scales in subsequent steps of the shower evolution. Note that scale is linear in momenta, not quadratic (i.e. Q, not Q^2). the polarization/spin/helicity of a particle. Currently Pythia does not use this variable for any internal operations, so its meaning is not uniquely defined. The LHA standard sets SPINUP to be the cosine of the angle between the spin vector and the 3-momentum of the decaying particle in the lab frame, i.e. restricted to be between +1 and -1. A more convenient choice could be the same quantity in the rest frame of the particle production, either the hard subprocess or the mother particle of a decay. Unknown or unpolarized particles should be assigned the value 9. the production vertex coordinates, in mm or mm/c. The production vertex four-vector. Note that the components of a Vec4 are named px(), py(), pz() and e() which of course then should be reinterpreted as above. the proper lifetime, in mm/c. It is assigned for all hadrons with positive nominal tau, tau_0 > 0, because it can be used by PYTHIA to decide whether a particle should or should not be allowed to decay, e.g. based on the decay vertex distance to the primary interaction vertex.

    Input methods

    The same method names as above are also overloaded in versions that set values. These have an input argument of the same type as the respective output above, and are of type void.

    There are also a few alternative methods for input: sets the status sign positive or negative, without changing the absolute value. changes the absolute value but retains the original sign. sets both mothers in one go. sets both daughters in one go. sets both colour and anticolour in one go. sets the four-momentum components in one go. sets the production vertex components in one go.

    Further output methods

    In addition, a number of derived quantities can easily be obtained, but cannot be set, such as: the absolute value of the particle identity code. the absolute value of the status code. true for a remaining particle, i.e. one with positive status code, else false. Thus, after an event has been fully generated, it separates the final-state particles from intermediate-stage ones. (If used earlier in the generation process, a particle then considered final may well decay later.) true for particles with a status code -34, -45, -46 or -54, else false. This singles out partons that have been created in a previous scattering but here are bookkept as belonging to the incoming state of another scattering. production vertex has been set; if false then production at the origin is assumed. squared mass, which can be negative for spacelike partons. (squared) mass calculated from the four-momentum; should agree with m(), m2() up to roundoff. Negative for spacelike virtualities. energy calculated from the mass and three-momentum; should agree with e() up to roundoff. For spacelike partons a positive-energy solution is picked. This need not be the correct one, so it is recommended not to use the method in such cases. (squared) transverse momentum. (squared) transverse mass. If m_T^2 is negative, which can happen for a spacelike parton, then mT() returns -sqrt(-m_T^2), by analogy with the negative sign used to store spacelike masses. (squared) three-momentum size. (squared) transverse energy, eT = e * sin(theta) = e * pT / pAbs. polar and azimuthal angle. angle in the (p_x, p_z) plane, between -pi and +pi, with 0 along the +z axis E +- p_z. rapidity and pseudorapidity. the decay vertex coordinates, in mm or mm/c. This decay vertex is calculated from the production vertex, the proper lifetime and the four-momentum assuming no magnetic field or other detector interference. It can be used to decide whether a decay should be performed or not, and thus is defined also for particles which PYTHIA did not let decay.

    Not part of the Particle class proper, but obviously tightly linked, are the two methods the (squared) invariant mass of two particles.

    Properties of the particle species

    Each Particle contains a pointer to the respective ParticleDataEntry object in the particle data tables. This gives access to properties of the particle species as such. It is there mainly for convenience, and should be thrown if an event is written to disk, to avoid any problems of object persistency. Should an event later be read back in, the pointer will be recreated from the id code if the normal input methods are used. (Use the Event::restorePtrs() method if your persistency scheme bypasses the normal methods.) This pointer is used by the following member functions: the name of the particle. as above, but for negative-status particles the name is given in brackets to emphasize that they are intermediaries. 2 *spin + 1 when defined, else 0. charge, and three times it to make an integer. charge different from or equal to 0. 0 for colour singlets, 1 for triplets, -1 for antitriplets and 2 for octets. (A preliminary implementation of colour sextets also exists, using 3 for sextets and -3 for antisextets.) the nominal mass of the particle, according to the data tables. the width of the particle, and the minimum and maximum allowed mass value for particles with a width, according to the data tables. the mass of the particle, picked according to a Breit-Wigner distribution for particles with width. It is different each time called, and is therefore only used once per particle to set its mass m(). will give the constituent masses for quarks and diquarks, else the same masses as with m0(). the nominal lifetime tau_0 > 0, in mm/c, of the particle species. It is used to assign the actual lifetime tau. flag whether particle has been declared unstable or not, offering the main user switch to select which particle species to decay. flag whether decay modes have been declared for a particle, so that it could be decayed, should that be requested. particles that are decayed by an external program. particles where the decay is to be treated as part of the hard process, typically with nominal mass above 20 GeV (W^+-, Z^0, t, ...). particles with strong or electric charge, or composed of ones having it, which thereby should be considered visible in a normal detector. true for a lepton or an antilepton (including neutrinos). true for a quark or an antiquark. true for a gluon. true for a diquark or an antidiquark. true for a gluon, a quark or antiquark up to the b (but excluding top), and a diquark or antidiquark consisting of quarks up to the b. true for a hadron (made up out of normal quarks and gluons, i.e. not for R-hadrons and other exotic states). a reference to the ParticleDataEntry.

    Methods that may access the event the particle belongs to

    A particle can be created on its own. When inserted into an event record, it obtains a pointer to that event-as-a-whole. It is then possible to use methods that do not make sense for a particle in isolation. These methods are listed below. Whenever the pointer to the event is not defined, these will return an appropriate "null" value, this being -1 for an integer, false for a bool, and empty for a vector, unless otherwise specified. the index of the particle itself in the event record. returns the status code according to the HepMC conventions agreed in February 2009. This convention does not preserve the full information provided by the internal PYTHIA status code, as obtained by Particle::status(), but comes reasonably close. The allowed output values are:
    • 0 : an empty entry, with no meaningful information and therefore to be skipped unconditionally;
    • 1 : a final-state particle, i.e. a particle that is not decayed further by the generator (may also include unstable particles that are to be decayed later, as part of the detector simulation);
    • 2 : a decayed Standard Model hadron or tau or mu lepton, excepting virtual intermediate states thereof (i.e. the particle must undergo a normal decay, not e.g. a shower branching);
    • 3 : a documentation entry (not used in PYTHIA);
    • 4 : an incoming beam particle;
    • 11 - 200 : an intermediate (decayed/branched/...) particle that does not fulfill the criteria of status code 2, with a generator-dependent classification of its nature; in PYTHIA the absolute value of the normal status code is used.
    Note: for a particle without a properly set pointer to its event, codes 1 and 4 can still be inferred from its status code, while everythg else is assigned code 0.
    are used to trace carbon copies of the particle up to its top mother or down to its bottom daughter. If there are no such carbon copies, the index of the particle itself will be returned. A carbon copy is when the "same" particle appears several times in the event record, but with changed momentum owing to recoil effects. also trace top mother and bottom daughter, but do not require carbon copies, only that one can find an unbroken chain, of mothers or daughters, with the same flavour id code. When it encounters ambiguities, say a g -> g g branching or a u u -> u u hard scattering, it will stop the tracing and return the current position. It can be confused by nontrivial flavour changes, e.g. a hard process u d -> d u by W^+- exchange will give the wrong answer. These methods therefore are of limited use for common particles, in particular for the gluon, but should work well for "rare" particles. returns a vector of all the sister indices of the particle, i.e. all the daughters of the first mother, except the particle itself. If the argument traceTopBot = true the particle is first traced up with iTopCopy() before its mother is found, and then all the particles in the daughterList() of this mother are traced down with iBotCopy(), omitting the original particle itself. The method is not meaningful for the 0 entry, with status code -11, and there returns an empty list. traces the particle upwards through mother, grandmother, and so on, until either iAncestor is found or the top of the record is reached. Normally one unique mother is required, as is the case e.g. in decay chains or in parton showers, so that e.g. the tracing through a hard scattering would not work. For hadronization, first-rank hadrons are identified with the respective string endpoint quark, which may be useful e.g. for b physics, while higher-rank hadrons give false. Currently also ministrings that collapsed to one single hadron and junction topologies give false. removes the decay chain of the particle and thus restores it to its undecayed state. It is only intended for "normal" particle decay chains, and will return false in other cases, notably if the particle is coloured. The procedure would not work if non-local momentum shifts have been performed, such as with a Bose-Einstein shift procedure (or for a dipole shower recoiler). As the decay products are erased from the event record, mother and daughter indices are updated to retain a correct history for the remaining particles.

    Methods that perform operations

    There are some further methods, some of them inherited from Vec4, to modify the properties of a particle. They are of little interest to the normal user. multiply the three-momentum components by fac. multiply the four-momentum components by fac. multiply the four-momentum components and the mass by fac. rotate three-momentum and production vertex by these polar and azimuthal angles. boost four-momentum and production vertex by this three-vector. as above, but also input the gamma value, to reduce roundoff errors. boost four-momentum and production vertex by beta = (px/e, py/e, pz/e). as above, but also use gamma> = e/m to reduce roundoff errors. as above, but with sign of boost flipped. combined rotation and boost of the four-momentum and production vertex. add a positive offset to the mother and daughter indices, i.e. if mother1 is above minMother then addMother is added to it, same with mother2, if daughter1 is above minDaughter then addDaughter is added to it, same with daughter2. add a positive offset to colour indices, i.e. if col is positive then addCol is added to it, same with acol.

    Constructors and operators

    Normally a user would not need to create new particles. However, if necessary, the following constructors and methods may be of interest. constructs an empty particle, i.e. where all properties have been set 0 or equivalent. constructs a particle with the input properties provided, and non-provided ones set 0 (9 for pol). constructs a particle with the input properties provided, and non-provided ones set 0 (9 for pol). constructs an particle that is a copy of the input one. copies the input particle. sets the pointer to the Event object the particle belongs to. This method is automatically called when a particle is appended to an event record. Also calls setPDEPtr below. sets the pointer to the ParticleDataEntry object of the particle, based on its current id code. If the particle belongs to an event there is no need to provide the input argument. As explained above, a valid ParticleDataEntry pointer is needed for the methods that provide information generic to the particle species.
    pythia8-8.1.80.orig/xmldoc/ParticleDecays.xml0000444000175000017500000003771412217346314017252 0ustar sunsun

    Particle Decays

    The ParticleDecays class performs the sequential decays of all unstable hadrons produced in the string fragmentation stage, i.e. up to and including b hadrons and their decay products, such as the tau lepton. It is not to be used for the decay of more massive resonances, such as top, Z^0 or SUSY, where decays must be performed already at the ProcessLevel of the event generation.

    The decay description essentially copies the one present in PYTHIA since many years, but with some improvements, e.g. in the decay tables and the number of decay models available. Recently a more sophisticated handling of tau decays has also been introduced. Some issues may need further polishing.

    Variables determining whether a particle decays

    Before a particle is actually decayed, a number of checks are made.

    (i) Decay modes must have been defined for the particle kind; tested by the canDecay() method of Event (and ParticleData).

    (ii) The main switch for allowing this particle kind to decay must be on; tested by the mayDecay() method of Event (and ParticleData).

    (iii) Particles may be requested to have a nominal proper lifetime tau0 below a threshold. When on, only particles with tau0 < tau0Max are decayed. The above tau0Max, expressed in mm/c.

    (iv) Particles may be requested to have an actual proper lifetime tau below a threshold. When on, only particles with tau < tauMax are decayed. The above tauMax, expressed in mm/c.
    In order for this and the subsequent tests to work, a tau is selected and stored for each particle, whether in the end it decays or not. (If each test would use a different temporary tau it would lead to inconsistencies.)

    (v) Particles may be requested to decay within a given distance of the origin. When on, only particles with a decay within a radius r < rMax are decayed. There is assumed to be no magnetic field or other detector effects. The above rMax, expressed in mm.

    (vi) Particles may be requested to decay within a given cylindrical volume around the origin. When on, only particles with a decay within a volume limited by rho = sqrt(x^2 + y^2) < xyMax and |z| < zMax are decayed. There is assumed to be no magnetic field or other detector effects. The above xyMax, expressed in mm. The above zMax, expressed in mm.

    Mixing

    Allow or not B^0 - B^0bar and B_s^0 - B_s^0bar mixing. The mixing parameter x_d = Delta(m_B^0)/Gamma_B^0 in the B^0 - B^0bar system. (Default from RPP2006.) The mixing parameter x_s = Delta(m_B_s^0)/Gamma_B_s^0 in the B_s^0 - B_s^0bar system. (Delta-m from CDF hep-ex-0609040, Gamma from RPP2006.)

    Tau decays

    A new machinery has been introduced to handle tau lepton decays, with helicity information related to the production process and with the form of the hadronic current fitted to data. It is largely based on the corresponding Herwig++ implementation Gre07, with some input from Tauola Jad90. A complete writeup is in preparation, but meanwhile a short summary can be found at Ilt12.

    For taus in external processes, interfaced with Les Houches Accord information available, e.g. via Les Houches Event Files (LHEF), the new machinery interprets the SPINUP number for tau leptons as giving their helicity, and decays them accordingly. The only exceptions are when a specific polarization is forced by the user (see below), which then overrides the SPINUP value, or when SPINUP has the special value 9 (unpolarized). In the latter case, PYTHIA defaults back to attempting to determine the helicity structure from the production process, in the same way as for internal processes.

    This new machinery is on by default, but it is possible to revert to the simpler old decay handling, e.g. to study differences. Furthermore the spin tracing framework does not yet cover all possibilities; notably it cannot handle taus coming from SUSY decay chains (except via LHEF), so it makes sense to switch off the new machinery in such instances, for speed reasons if nothing else. In case only one tau mother species is undefined, the polarization involved can be set by hand. Choice of tau decay model. Note: options 2 and 3, to force a specific tau polarization, only affect the decay of the tau. The angular distribution of the tau itself, given by its production, is not modified by these options. If you want, e.g., a righthanded W, or a SUSY decay chain, the kinematics should be handled by the corresponding cross section class(es), supplemented by the resonance decay one(s). The options here could then still be used to ensure the correct polarization at the tau decay stage. Polarization of the tau when mode 2 or 3 of ParticleDecays:sophisticatedTau is selected. Mother of the tau for forced polarization when mode 2 of ParticleDecays:sophisticatedTau is selected. You should give the positive identity code; to the extent an antiparticle exists it will automatically obtain the inverse polarization.

    QED radiation

    So far PYTHIA does not have any generic machinery for handling QED radiation in normal particle decays. In order to include this, a program like Photos Bar94, Dav10 could be used as an afterburner. In a few cases, however, the existing shower machinery can be used also here: for two-body decays to a lepton pair (l^+ l^- or l^+- nu_l). Such decays are mediated by gamma^*/Z^0/W^+- exchange, for which PYTHIA does have an existing machinery that can be applied, including first-order matrix-element corrections for the first (hardest) photon emission. Allow or not photon radiations in decays to a lepton pair, see above. Note: The current default is to have radiation switched off, in order to avoid double-counting of emissions if you link to an external QED-radiation program, as is the norm in many collaborations.

    Other variables

    Minimum mass difference required between the decaying mother mass and the sum of the daughter masses, kept as a safety margin to avoid numerical problems in the decay generation. In semileptonic decays to more than one hadron, such as B -> nu l D pi, decay products after the first three are dampened in momentum by an explicit weight factor exp(-p^2/sigmaSoft^2), where p is the three-momentum in the rest frame of the decaying particle. This takes into account that such further particles come from the fragmentation of the spectator parton and thus should be soft.

    When a decay mode is defined in terms of a partonic content, a random multiplicity (and a random flavour set) of hadrons is to be picked, especially for some charm and bottom decays. This is done according to a Poissonian distribution, for n_p normal particles and n_q quarks the average value is chosen as n_p/ 2 + n_q/4 + multIncrease * ln ( mDiff / multRefMass) with mDiff the difference between the decaying particle mass and the sum of the normal-particle masses and the constituent quark masses. For gluon systems multGoffset offers and optional additional term to the multiplicity. The lowest possible multiplicity is n_p + n_q/2 (but at least 2) and the highest possible 10. If the picked hadrons have a summed mass above that of the mother a new try is made, including a new multiplicity. These constraints imply that the actual average multiplicity does not quite agree with the formula above. The above multIncrease parameter, except for meMode = 23. The above multIncrease parameter, specifically for meMode = 23. Here the weak decay implies that only the virtual W mass should contribute to the production of new particles, rather than the full meson mass. The above multRefMass parameter. The above multGoffset parameter. When a decay is given as a list of four partons to be turned into hadrons (primarily for modes 41 - 80) it is assumed that they are listed in pairs, as a first and a second colour singlet, which could give rise to separate sets of hadrons. Here colRearrange is the probability that this original assignment is not respected, and default corresponds to no memory of this original colour topology. When a particle decays to q qbar, g g, g g g or gamma g g, with meMode > 90, allow or not a shower to develop from it, before the partonic system is hadronized. (The typical example is Upsilon decay.) In addition, some variables defined for string fragmentation and for flavour production are used also here.

    Modes for Matrix Element Processing

    Some decays can be treated better than what pure phase space allows, by reweighting with appropriate matrix elements. In others a partonic content has to be converted to a set of hadrons. The presence of such corrections is signaled by a nonvanishing meMode() value for a decay mode in the particle data table. The list of allowed possibilities almost agrees with the PYTHIA 6 ones, but several obsolete choices have been removed, a few new introduced, and most have been moved for better consistency. Here is the list of currently allowed meMode() codes:
    • 0 : pure phase space of produced particles ("default"); input of partons is allowed and then the partonic content is converted into the minimal number of hadrons (i.e. one per parton pair, but at least two particles in total)
    • 1 : omega and phi -> pi+ pi- pi0
    • 2 : polarization in V -> PS + PS (V = vector, PS = pseudoscalar), when V is produced by PS -> PS + V or PS -> gamma + V
    • 11 : Dalitz decay into one particle, in addition to the lepton pair (also allowed to specify a quark-antiquark pair that should collapse to a single hadron)
    • 12 : Dalitz decay into two or more particles in addition to the lepton pair
    • 13 : double Dalitz decay into two lepton pairs
    • 21 : decay to phase space, but weight up neutrino_tau spectrum in tau decay
    • 22 : weak decay; if there is a quark spectator system it collapses to one hadron; for leptonic/semileptonic decays the V-A matrix element is used, for hadronic decays simple phase space
    • 23 : as 22, but require at least three particles in decay
    • 31 : decays of type B -> gamma X, very primitive simulation where X is given in terms of its flavour content, the X multiplicity is picked according to a geometrical distribution with average number 2, and the photon energy spectrum is weighted up relative to pure phase space
    • 42 - 50 : turn partons into a random number of hadrons, picked according to a Poissonian with average value as described above, but at least code - 40 and at most 10, and then distribute then in pure phase space; make a new try with another multiplicity if the sum of daughter masses exceed the mother one
    • 52 - 60 : as 42 - 50, with multiplicity between code - 50 and 10, but avoid already explicitly listed non-partonic channels
    • 62 - 70 : as 42 - 50, but fixed multiplicity code - 60
    • 72 - 80 : as 42 - 50, but fixed multiplicity code - 70, and avoid already explicitly listed non-partonic channels
    • 91 : decay to q qbar or g g, which should shower and hadronize
    • 92 : decay onium to g g g or g g gamma (with matrix element), which should shower and hadronize
    • 100 - : reserved for the description of partial widths of resonances
    Three special decay product identity codes are defined.
    • 81: remnant flavour. Used for weak decays of c and b hadrons, where the c or b quark decays and the other quarks are considered as a spectator remnant in this decay. In practice only used for baryons with multiple c and b quarks, which presumably would never be used, but have simple (copied) just-in-case decay tables. Assumed to be last decay product.
    • 82: random flavour, picked by the standard fragmentation flavour machinery, used to start a sequence of hadrons, for matrix element codes in 41 - 80. Assumed to be first decay product, with -82 as second and last. Where multiplicity is free to be picked it is selected as for normal quarkonic systems. Currently unused.
    • 83: as for 82, with matched pair 83, -83 of decay products. The difference is that here the pair is supposed to come from a closed gluon loop (e.g. eta_c -> g g) and so have a somewhat higher average multiplicity than the simple string assumed for 82, see the ParticleDecays:multGoffset parameter above.
    pythia8-8.1.80.orig/xmldoc/TimelikeShowers.xml0000444000175000017500000011430412217346320017460 0ustar sunsun

    Timelike Showers

    The PYTHIA algorithm for timelike final-state showers is based on the article Sjo05, where a transverse-momentum-ordered evolution scheme is introduced, with the extension to fully interleaved evolution covered in Cor10a. This algorithm is influenced by the previous mass-ordered algorithm in PYTHIA Ben87 and by the dipole-emission formulation in Ariadne Gus86. From the mass-ordered algorithm it inherits a merging procedure for first-order gluon-emission matrix elements in essentially all two-body decays in the standard model and its minimal supersymmetric extension Nor01.

    The normal user is not expected to call TimeShower directly, but only have it called from Pythia. Some of the parameters below, in particular TimeShower:alphaSvalue, would be of interest for a tuning exercise, however.

    Main variables

    Often the maximum scale of the FSR shower evolution is understood from the context. For instance, in a resonance decay half the resonance mass sets an absolute upper limit. For a hard process in a hadronic collision the choice is not as unique. Here the factorization scale has been chosen as the maximum evolution scale. This would be the pT for a 2 -> 2 process, supplemented by mass terms for massive outgoing particles. For some special applications we do allow an alternative. Way in which the maximum shower evolution scale is set to match the scale of the hard process itself. Note 1: as enumerated in the text, these options take effect both for internal and external processes. Whether a particular option makes sense depends on the context. For instance, if events for the same basic process to different orders are to be matched, then option 1 would be a reasonable first guess. But in more sophisticated descriptions option 2 could be combined with UserHook vetoes on emissions that would lead to double-counting, using more flexible phase space boundaries. Option 0, finally, may be most realistic when only Born-level processes are involved, possibly in combination with a nonzero TimeShower:pTdampMatch. Note 2: These options only apply to the hard interaction. If a "second hard" process is present, the two are analyzed and set separately for the default 0 option, while both are affected the same way for non-default options 1 and 2. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of each process itself. The options also assume that you use interleaved evolution, so that FSR is in direct competition with ISR for the hardest emission. If you already generated a number of ISR partons at low pT, it would not make sense to have a later FSR shower up to the kinematical limit for all of them. Note 3: Recall that resonance decays are not affected by this mode, but that showers there are always set to fill the full phase space, often with built-in matrix-element-matching that give a NLO accuracy. A modification of this behaviour would require you to work with UserHooks. In cases where the above pTmaxMatch rules would imply that pT_max = pT_factorization, pTmaxFudge introduces a multiplicative factor f such that instead pT_max = f * pT_factorization. Only applies to the hardest interaction in an event, and a "second hard" if there is such a one, cf. below. It is strongly suggested that f = 1, but variations around this default can be useful to test this assumption. Note:Scales for resonance decays are not affected, but can be set separately by user hooks. A multiplicative factor f such that pT_max = f * pT_factorization, as above, but here for the non-hardest interactions (when multiparton interactions are allowed). These options only take effect when a process is allowed to radiate up to the kinematical limit by the above pTmaxMatch choice, and no matrix-element corrections are available. Then, in many processes, the fall-off in pT will be too slow by one factor of pT^2. That is, while showers have an approximate dpT^2/pT^2 shape, often it should become more like dpT^2/pT^4 at pT values above the scale of the hard process. This argument is more obvious and relevant for ISR, where emissions could go the the kinematical limit, whereas they are constrained by the respective dipole mass for FSR. Nevertheless this matching option is offered for FSR to have a (semi-)symmetric description. Note that a dampening factor is applied to all dipoles in the final state of the hard process, which is somewhat different from the ISR implementation. Note: These options only apply to the hard interaction. Specifically, a "second hard" interaction would not be affected. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of the process itself. In cases 1 and 2 above, where a dampening is imposed at around the factorization or renormalization scale, respectively, this allows the pT scale of dampening of radiation by a half to be shifted by this factor relative to the default Q_fac or Q_ren. This number ought to be in the neighbourhood of unity, but variations away from this value could do better in some processes.

    The amount of QCD radiation in the shower is determined by The alpha_strong value at scale M_Z^2. The default value corresponds to a crude tuning to LEP data, to be improved.

    The actual value is then regulated by the running to the scale pT^2, at which the shower evaluates alpha_strong. Order at which alpha_strong runs,

    The CMW rescaling of Lambda_QCD (see the section on StandardModelParameters) can be applied to the alpha_strong values used for timelike showers. Note that tunes using this option need lower values of alpha_strong(m_Z^2) than tunes that do not.

    QED radiation is regulated by the alpha_electromagnetic value at the pT^2 scale of a branching. The running of alpha_em.

    The natural scale for couplings, and PDFs for dipoles stretching out to the beam remnants, is pT^2. To explore uncertainties it is possibly to vary around this value, however, in analogy with what can be done for hard processes. The default pT^2 renormalization scale is multiplied by this prefactor. For QCD this is equivalent to a change of Lambda^2 in the opposite direction, i.e. to a change of alpha_strong(M_Z^2) (except that flavour thresholds remain at fixed scales). The default pT^2 factorization scale is multiplied by this prefactor.

    The rate of radiation if divergent in the pT -> 0 limit. Here, however, perturbation theory is expected to break down. Therefore an effective pT_min cutoff parameter is introduced, below which no emissions are allowed. The cutoff may be different for QCD and QED radiation off quarks, and is mainly a technical parameter for QED radiation off leptons. Parton shower cut-off pT for QCD emissions. Parton shower cut-off pT for photon coupling to coloured particle. Parton shower cut-off pT for pure QED branchings. Assumed smaller than (or equal to) pTminChgQ.

    Shower branchings gamma -> f fbar, where f is a quark or lepton, in part compete with the hard processes involving gamma^*/Z^0 production. In order to avoid overlap it makes sense to correlate the maximum gamma mass allowed in showers with the minimum gamma^*/Z^0 mass allowed in hard processes. In addition, the shower contribution only contains the pure gamma^* contribution, i.e. not the Z^0 part, so the mass spectrum above 50 GeV or so would not be well described. Maximum invariant mass allowed for the created fermion pair in a gamma -> f fbar branching in the shower.

    Interleaved evolution

    Multiparton interactions (MPI) and initial-state showers (ISR) are always interleaved, as follows. Starting from the hard interaction, the complete event is constructed by a set of steps. In each step the pT scale of the previous step is used as starting scale for a downwards evolution. The MPI and ISR components each make their respective Monte Carlo choices for the next lower pT value. The one with larger pT is allowed to carry out its proposed action, thereby modifying the conditions for the next steps. This is relevant since the two components compete for the energy contained in the beam remnants: both an interaction and an emission take away some of the energy, leaving less for the future. The end result is a combined chain of decreasing pT values, where ones associated with new interactions and ones with new emissions are interleaved.

    There is no corresponding requirement for final-state radiation (FSR) to be interleaved. Such an FSR emission does not compete directly for beam energy (but see below), and also can be viewed as occurring after the other two components in some kind of time sense. Interleaving is allowed, however, since it can be argued that a high-pT FSR occurs on shorter time scales than a low-pT MPI, say. Backwards evolution of ISR is also an example that physical time is not the only possible ordering principle, but that one can work with conditional probabilities: given the partonic picture at a specific pT resolution scale, what possibilities are open for a modified picture at a slightly lower pT scale, either by MPI, ISR or FSR? Complete interleaving of the three components also offers advantages if one aims at matching to higher-order matrix elements above some given scale. If on, final-state emissions are interleaved in the same decreasing-pT chain as multiparton interactions and initial-state emissions. If off, final-state emissions are only addressed after the multiparton interactions and initial-state radiation have been considered.

    As an aside, it should be noted that such interleaving does not affect showering in resonance decays, such as a Z^0. These decays are only introduced after the production process has been considered in full, and the subsequent FSR is carried out inside the resonance, with preserved resonance mass.

    One aspect of FSR for a hard process in hadron collisions is that often colour dipoles are formed between a scattered parton and a beam remnant, or rather the hole left behind by an incoming partons. If such holes are allowed as dipole ends and take the recoil when the scattered parton undergoes a branching then this translates into the need to take some amount of remnant energy also in the case of FSR, i.e. the roles of ISR and FSR are not completely decoupled. The energy taken away is bookkept by increasing the x value assigned to the incoming scattering parton, and a reweighting factor x_new f(x_new, pT^2) / x_old f(x_old, pT^2) in the emission probability ensures that not unphysically large x_new values are reached. Usually such x changes are small, and they can be viewed as a higher-order effect beyond the accuracy of the leading-log initial-state showers.

    This choice is not unique, however. As an alternative, if nothing else useful for cross-checks, one could imagine that the FSR is completely decoupled from the ISR and beam remnants. If on, the final-state shower is allowed to borrow energy from the beam remnants as described above, thereby changing the mass of the scattering subsystem. If off, the partons in the scattering subsystem are constrained to borrow energy from each other, such that the total four-momentum of the system is preserved. This flag has no effect on resonance decays, where the shower always preserves the resonance mass, cf. the comment above about showers for resonances never being interleaved. When beam recoil is allowed there is still some ambiguity how far into the beam end of the dipole that emission should be allowed. It is dampened in the beam region, but probably not enough. When on an additional suppression factor 4 pT2_hard / (4 pT2_hard + m2) is multiplied on to the emission probability. Here pT_hard is the transverse momentum of the radiating parton and m the off-shell mass it acquires by the branching, m2 = pT2/(z(1-z)). Note that m2 = 4 pT2_hard is the kinematical limit for a scattering at 90 degrees without beam recoil.

    Global recoil

    The final-state algorithm is based on dipole-style recoils, where one single parton takes the full recoil of a branching. This is unlike the initial-state algorithm, where the complete already-existing final state shares the recoil of each new emission. As an alternative, also the final-state algorithm contains an option where the recoil is shared between all partons in the final state. Thus the radiation pattern is unrelated to colour correlations. This is especially convenient for some matching algorithms, like MC@NLO, where a full analytic knowledge of the shower radiation pattern is needed to avoid double-counting. (The pT-ordered shower is described in Sjo05, and the corrections for massive radiator and recoiler in Nor01.)

    Technically, the radiation pattern is most conveniently represented in the rest frame of the final state of the hard subprocess. Then, for each parton at a time, the rest of the final state can be viewed as a single effective parton. This "parton" has a fixed invariant mass during the emission process, and takes the recoil without any changed direction of motion. The momenta of the individual new recoilers are then obtained by a simple common boost of the original ones.

    This alternative approach will miss out on the colour coherence phenomena. Specifically, with the whole subcollision mass as "dipole" mass, the phase space for subsequent emissions is larger than for the normal dipole algorithm. The phase space difference grows as more and more gluons are created, and thus leads to a way too steep multiplication of soft gluons. Therefore the main application is for the first one or few emissions of the shower, where a potential overestimate of the emission rate is to be corrected for anyway, by matching to the relevant matrix elements. Thereafter, subsequent emissions should be handled as before, i.e. with dipoles spanned between nearby partons. Furthermore, only the first (hardest) subcollision is handled with global recoils, since subsequent MPI's would not be subject to matrix element corrections anyway.

    In order for the mid-shower switch from global to local recoils to work, colours are traced and bookkept just as for normal showers; it is only that this information is not used in those steps where a global recoil is requested. (Thus, e.g., a gluon is still bookkept as one colour and one anticolour dipole end, with half the charge each, but with global recoil those two ends radiate identically.) Alternative approach as above, where all final-state particles share the recoil of an emission.
    If off, then use the standard dipole-recoil approach.
    If on, use the alternative global recoil, but only for the first interaction, and only while the number of particles in the final state is at most TimeShower:nMaxGlobalRecoil before the branching.
    Represents the maximum number of particles in the final state for which the next final-state emission can be performed with the global recoil strategy. This number counts all particles, whether they are allowed to radiate or not, e.g. also Z^0. Also partons created by initial-state radiation emissions counts towards this sum, as part of the interleaved evolution. Without interleaved evolution this option would not make sense, since then a varying and large number of partons could already have been created by the initial-state radiation before the first final-state one, and then there is not likely to be any matrix elements available for matching.

    Two variations of the scheme outlined above are also available, (motivated by comparative studies within aMC@NLO). These studies indicate that global recoils should be used as sparsely as possible, in order to retain desirable features of the radiation pattern produced with the local recoil prescription. Choice which splittings are produced with the global recoil approach. The maximum number of splittings in the final state for which the next final-state emission can be performed with the global recoil strategy. This number has to be set if TimeShower:globalRecoilMode = 1 or TimeShower:globalRecoilMode = 2 The number of partons for Born-like phase space points. This number needs to be set if a different treatment of S-events (with Born-like kinematics) and H-events (with real-emission kinematics) is desired. This number has to be set if TimeShower:globalRecoilMode = 2. If on, limit the maximal pT produced in branchings in the global recoil scheme exactly as in the default (local) scheme. This means that the mass of the splitting dipole will set an upper bound for the pT of an emission. To be more explicit, this disallows emissions with pT larger than min{μstart 2, mD2/4}, with mD 2 = (√ (pr +ps)2 -m0,s)2 - m0,r2 , where the shower starting scale is μstart (i.e. SCALUP when reading LHE files, and Info.QFac() otherwise), r the radiating parton, and s the recoiling particle that would have been used in the local recoil scheme. This option is only used if wimpy showers are enabled.

    The global-recoil machinery does not work well with rescattering in the MPI machinery, since then the recoiling system is not uniquely defined. MultipartonInteractions:allowRescatter = off by default, so this is not a main issue. If both options are switched on, rescattering will only be allowed to kick in after the global recoil has ceased to be active, i.e. once the nMaxGlobalRecoil limit has been exceeded. This should not be a major conflict, since rescattering is mainly of interest at later stages of the downwards pT evolution.

    Further, it is strongly recommended to set TimeShower:MEcorrections = off (not default!), i.e. not to correct the emission probability to the internal matrix elements. The internal ME options do not cover any cases relevant for a multibody recoiler anyway, so no guarantees are given what prescription would come to be used. Instead, without ME corrections, a process-independent emission rate is obtained, and user hooks can provide the desired process-specific rejection factors.

    Radiation off octet onium states

    In the current implementation, charmonium and bottomonium production can proceed either through colour singlet or colour octet mechanisms, both of them implemented in terms of 2 -> 2 hard processes such as g g -> (onium) g. In the former case the state does not radiate and the onium therefore is produced in isolation, up to normal underlying-event activity. In the latter case the situation is not so clear, but it is sensible to assume that a shower can evolve. (Assuming, of course, that the transverse momentum of the onium state is sufficiently high that radiation is of relevance.)

    There could be two parts to such a shower. Firstly a gluon (or even a quark, though less likely) produced in a hard 2 -> 2 process can undergo showering into many gluons, whereof one branches into the heavy-quark pair. Secondly, once the pair has been produced, each quark can radiate further gluons. This latter kind of emission could easily break up a semibound quark pair, but might also create a new semibound state where before an unbound pair existed, and to some approximation these two effects should balance in the onium production rate. The showering "off an onium state" as implemented here therefore should not be viewed as an accurate description of the emission history step by step, but rather as an effective approach to ensure that the octet onium produced "in the hard process" is embedded in a realistic amount of jet activity. Of course both the isolated singlet and embedded octet are likely to be extremes, but hopefully the mix of the two will strike a reasonable balance. However, it is possible that some part of the octet production occurs in channels where it should not be accompanied by (hard) radiation. Therefore reducing the fraction of octet onium states allowed to radiate is a valid variation to explore uncertainties.

    If an octet onium state is chosen to radiate, the simulation of branchings is based on the assumption that the full radiation is provided by an incoherent sum of radiation off the quark and off the antiquark of the onium state. Thus the splitting kernel is taken to be the normal q -> q g one, multiplied by a factor of two. Obviously this is a simplification of a more complex picture, averaging over factors pulling in different directions. Firstly, radiation off a gluon ought to be enhanced by a factor 9/4 relative to a quark rather than the 2 now used, but this is a minor difference. Secondly, our use of the q -> q g branching kernel is roughly equivalent to always following the harder gluon in a g -> g g branching. This could give us a bias towards producing too hard onia. A soft gluon would have little phase space to branch into a heavy-quark pair however, so the bias may not be as big as it would seem at first glance. Thirdly, once the gluon has branched into a quark pair, each quark carries roughly only half of the onium energy. The maximum energy per emitted gluon should then be roughly half the onium energy rather than the full, as it is now. Thereby the energy of radiated gluons is exaggerated, i.e. onia become too soft. So the second and the third points tend to cancel each other.

    Finally, note that the lower cutoff scale of the shower evolution depends on the onium mass rather than on the quark mass, as it should be. Gluons below the octet-onium scale should only be part of the octet-to-singlet transition. Allow colour-octet charmonium and bottomonium states to radiate gluons. 0 means that no octet-onium states radiate, 1 that all do, with possibility to interpolate between these two extremes. The colour factor used used in the splitting kernel for those octet onium states that are allowed to radiate, normalized to the q -> q g splitting kernel. Thus the default corresponds to twice the radiation off a quark. The physically preferred range would be between 1 and 9/4.

    Weak showers

    The emission of W^+- and Z^0 gauge bosons off fermions is intended to become an integrated part of the initial- and final-state radiation frameworks, and is fully interleaved with QCD and QED emissions. Currently it is under development, and off by default. Another restriction is that there is no simulation of the full gamma^*/Z^0 interference: at low masses the QED shower involves a pure gamma^* component, whereas the weak shower generates a pure Z^0.

    Most events will not contain a W^+-/Z^0 emission at all, and in a shower framework it is not straightforward to force such emissions to happen without biasing the event sample in some respect. An option is available to enhance the emission rate artificially, but it is then the responsibility of the user to correct the cross section accordingly, and not to pick an enhancement so big that the probability for more than one emission is non-negligible. (It is not enough to assign an event weight 1/e^n where e is the enhancement factor and n is the number of emitted gauge bosons. This still misses to account for the change in phase space for late emissions by the effect of earlier ones, or equivalently for the unwanted change in the Sudakov form factor. See Lon12a for a detailed discussion and possible solutions.)

    Another enhancement probability is to only allow some specific W^+-/Z^0 decay modes. By default the shower is inclusive, since it should describe all that can happen with unit probability. This also holds even if the W^+- and Z^0 produced in the hard process have been restricted to specific decay channels. The trick that allows this is that two new "aliases" have been produced, a Zcopy with identity code 93 and a Wcopy with code 94. These copies are used specifically to bookkeep decay channels open for W^+-/Z^0 bosons produced in the shower. For the rest they are invisible, i.e. you will not find them in event listings. The separation into two sets of gauge bosons then also allows the selection of specific decay modes for 93 and 94, i.e. for only the gauge bosons produced in the shower. As above it is here up to the user to reweight the event to compensate for the bias introduced, and to watch out for possible complications. In this case there is no kinematics bias, but one would miss out on topologies where a not-selected decay channel could be part of the background to the selected one, notably when more than one gauge boson is produced.

    Note that the common theme is that a bias leads to an event-specific weight, since each event is unique. It also means that the cross-section information obtained e.g. by Pythia::stat() is misleading, since it has not been corrected for such weights. This is different from biases in a predetermined hard process, where the net reduction in cross section can be calculated once and for all at initialization, and events generated with unit weight thereafter.

    Special for the weak showers is that couplings are different for left- and righthanded fermions. With incoming unpolarized beams this should average out, at least so long as only one weak emission occurs. In the case of several weak emissions off the same fermion the correlation between them will carry a memory of the fermion helicity. Such a memory is retained for the affected dipole end, and is reflected in the Particle::pol() property, it being +1 (-1) for fermions considered righthanded (lefthanded), and 0 for the bulk where no choice has been made.

    The FSR shower emission is always matched to the matrix element for emission off a f fbar weak dipole. (Emission rates are normalized to the invariant mass of the dipole at the time of the weak emission, i.e. discounting the energy lost by previous QCD/QED emissions.) Also the angular distribution in the subsequent V = W^+-/Z^0 decay is matched to the matrix element expression for f fbar -> f fbar V -> f fbar f' fbar'. Afterwards the f' fbar' system undergoes showers and hadronization just like any W^+-/Z^0 decay products would.

    A few special switches are available for the weak framework, several mainly intended for tryout purposes, as follows. Allow a weak shower, yes or no. Determine which branchings are allowed. Parton shower cut-off pT for weak branchings. Enhancement factor for the weak shower. This is used to increase the statistics of weak shower emissions. Remember afterwards to correct for the additional weak emissions (i.e. divide the rate of weak emissions by the same factor). This parameter allows to stop the weak shower after a single emission.
    If on, only a single weak emission is allowed.
    If off, an unlimited number of weak emissions possible.
    The normal showers uses pT^2 as ordering variable, but for massive particles it could be preferred to use pT^2 + M^2 instead. This parameter allows to use pT^2 + k * M^2 for weak showers, thus k = 0 is the standard ordering and is used as default. Add an extra dampening to the weak shower to lower the production of low-pT W/Z's. The dampening is given by (pT^2 + 0.25 M^2)/ (pT^2 + M^2), where M^2 is the squared mass of the W/Z.

    Further variables

    There are several possibilities you can use to switch on or off selected branching types in the shower, or in other respects simplify the shower. These should normally not be touched. Their main function is for cross-checks. Allow a QCD shower, i.e. branchings q -> q g, g -> g g and g -> q qbar; on/off = true/false. Number of allowed quark flavours in g -> q qbar branchings (phase space permitting). A change to 4 would exclude g -> b bbar, etc. Allow quarks to radiate photons, i.e. branchings q -> q gamma; on/off = true/false. Allow leptons to radiate photons, i.e. branchings l -> l gamma; on/off = true/false. Allow photons to branch into lepton or quark pairs, i.e. branchings gamma -> l+ l- and gamma -> q qbar; on/off = true/false. Number of allowed quark flavours in gamma -> q qbar branchings (phase space permitting). A change to 4 would exclude g -> b bbar, etc. Number of allowed lepton flavours in gamma -> l+ l- branchings (phase space permitting). A change to 2 would exclude gamma -> tau+ tau-, and a change to 1 also gamma -> mu+ mu-. Use of matrix element corrections where available; on/off = true/false. Use of matrix element corrections also after the first emission, for dipole ends of the same system that did not yet radiate. Only has a meaning if MEcorrections above is switched on. Azimuthal asymmetry induced by gluon polarization; on/off = true/false. In the decays of coloured resonances, say t -> b W, it is not possible to set up dipoles with matched colours. Originally the b radiator therefore has W as recoiler, and that choice is unique. Once a gluon has been radiated, however, it is possible either to have the unmatched colour (inherited by the gluon) still recoiling against the W (off), or else let it recoil against the b also for this dipole (on). Before version 8.160 the former was the only possibility, which could give unphysical radiation patterns. It is kept as an option to check backwards compatibility. The same issue exists for QED radiation, but obviously is less significant. Consider the example W -> e nu, where originally the nu takes the recoil. In the old (off) scheme the nu would remain recoiler, while in the new (on) instead each newly emitted photon becomes the new recoiler.
    pythia8-8.1.80.orig/xmldoc/ExternalDecays.xml0000444000175000017500000000602712217346302017257 0ustar sunsun

    External Decays

    DecayHandler is a base class for the external handling of decays. It is intended for normal particle decays, primarily B mesons and tau, and cannot be used to redirect decays of heavy resonances like t or Z^0. The user-written derived class is called if a pointer to it has been given with the pythia.decayPtr() method, where it also is specified which particles it will be called for. This particle information is accessible with the doExternalDecay() method.

    There is only one pure virtual method in DecayHandler, to do the decay: where is a list of particle PDG identity codes, is a list of their respective masses (in GeV), and is a list of their respective four-momenta.

    At input, these vectors each have size one, so that idProd[0], mProd[0] and pProd[0] contain information on the particle that is to be decayed. At output, the vectors should have increased by the addition of all the decay products. Even if initially defined in the rest frame of the mother, the products should have been boosted so that their four-momenta add up to the pProd[0] of the decaying particle.

    Should it be of interest to know the prehistory of the decaying particle, e.g. to set some helicity information affecting the decay angular distribution, the full event record is available read-only, with info in which slot iDec the decaying particle is stored.

    The routine should return true if it managed the decay and false otherwise, in which case Pythia will try to do the decay itself. This e.g. means you can choose to do some decay channels yourself, and leave others to Pythia. To avoid double-counting, the channels you want to handle should be switched off in the Pythia particle database. In the beginning of the external decay method you should then return false with a probability given by the sum of the branching ratios for those channels you do not want to handle yourself.

    Note that the decay vertex is always set by Pythia, and that B-Bbar oscillations have already been taken into account, if they were switched on. Thus idProd[0] may be the opposite of event[iDec].id(), where the latter provides the code at production.

    A sample test program is available in main17.cc, providing a simple example of how to use this facility. pythia8-8.1.80.orig/xmldoc/pomH1FitBlo.data0000444000175000017500000024634712217346315016560 0ustar sunsun -0.39548E-02 -0.10578E-02 0.21133E-02 0.67622E-02 0.12805E-01 0.20105E-01 0.28491E-01 0.37915E-01 0.47943E-01 0.58668E-01 0.69999E-01 0.81817E-01 0.94036E-01 0.10659E+00 0.11942E+00 0.13247E+00 0.14569E+00 0.15906E+00 0.17254E+00 0.18610E+00 0.19971E+00 0.21335E+00 0.22700E+00 0.24066E+00 0.25429E+00 0.26789E+00 0.28144E+00 0.29495E+00 0.30840E+00 0.32178E+00 -0.39521E-02 -0.10569E-02 0.21074E-02 0.67198E-02 0.12692E-01 0.19886E-01 0.28130E-01 0.37374E-01 0.47198E-01 0.57689E-01 0.68758E-01 0.80287E-01 0.92195E-01 0.10442E+00 0.11690E+00 0.12957E+00 0.14242E+00 0.15539E+00 0.16845E+00 0.18159E+00 0.19477E+00 0.20797E+00 0.22117E+00 0.23436E+00 0.24753E+00 0.26066E+00 0.27374E+00 0.28677E+00 0.29973E+00 0.31263E+00 -0.39493E-02 -0.10559E-02 0.21016E-02 0.66776E-02 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0.31754E+00 0.30843E+00 0.29926E+00 0.29017E+00 0.28124E+00 0.27254E+00 0.26408E+00 0.25591E+00 0.24803E+00 0.24045E+00 0.23318E+00 0.22624E+00 0.21953E+00 0.21309E+00 0.20694E+00 0.20106E+00 0.19542E+00 0.19002E+00 0.18484E+00 0.17988E+00 0.17512E+00 0.32738E+00 0.33692E+00 0.34509E+00 0.34678E+00 0.34390E+00 0.33796E+00 0.33011E+00 0.32102E+00 0.31147E+00 0.30157E+00 0.29160E+00 0.28174E+00 0.27209E+00 0.26272E+00 0.25368E+00 0.24496E+00 0.23660E+00 0.22861E+00 0.22096E+00 0.21365E+00 0.20674E+00 0.20006E+00 0.19369E+00 0.18764E+00 0.18186E+00 0.17635E+00 0.17110E+00 0.16607E+00 0.16127E+00 0.15668E+00 0.33220E+00 0.33804E+00 0.34258E+00 0.34115E+00 0.33562E+00 0.32747E+00 0.31778E+00 0.30723E+00 0.29642E+00 0.28550E+00 0.27473E+00 0.26422E+00 0.25407E+00 0.24433E+00 0.23500E+00 0.22608E+00 0.21759E+00 0.20952E+00 0.20185E+00 0.19457E+00 0.18771E+00 0.18112E+00 0.17486E+00 0.16894E+00 0.16331E+00 0.15797E+00 0.15289E+00 0.14805E+00 0.14344E+00 0.13905E+00 0.33717E+00 0.33915E+00 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0.10679E+00 0.10245E+00 0.98358E-01 0.94510E-01 0.90877E-01 0.35352E+00 0.34261E+00 0.33087E+00 0.31567E+00 0.29880E+00 0.28149E+00 0.26449E+00 0.24834E+00 0.23291E+00 0.21847E+00 0.20509E+00 0.19271E+00 0.18127E+00 0.17071E+00 0.16096E+00 0.15192E+00 0.14357E+00 0.13586E+00 0.12871E+00 0.12209E+00 0.11602E+00 0.11028E+00 0.10494E+00 0.99994E-01 0.95382E-01 0.91077E-01 0.87063E-01 0.83290E-01 0.79760E-01 0.76440E-01 0.35975E+00 0.34381E+00 0.32720E+00 0.30802E+00 0.28799E+00 0.26825E+00 0.24942E+00 0.23197E+00 0.21553E+00 0.20041E+00 0.18661E+00 0.17400E+00 0.16247E+00 0.15196E+00 0.14234E+00 0.13350E+00 0.12540E+00 0.11798E+00 0.11116E+00 0.10489E+00 0.99175E-01 0.93798E-01 0.88831E-01 0.84262E-01 0.80024E-01 0.76088E-01 0.72438E-01 0.69024E-01 0.65846E-01 0.62870E-01 0.36660E+00 0.34505E+00 0.32302E+00 0.29948E+00 0.27609E+00 0.25384E+00 0.23319E+00 0.21452E+00 0.19717E+00 0.18149E+00 0.16741E+00 0.15472E+00 0.14326E+00 0.13292E+00 0.12357E+00 0.11505E+00 0.10733E+00 0.10031E+00 0.93914E-01 0.88076E-01 0.82808E-01 0.77873E-01 0.73347E-01 0.69214E-01 0.65403E-01 0.61886E-01 0.58644E-01 0.55627E-01 0.52834E-01 0.50232E-01 0.37432E+00 0.34632E+00 0.31809E+00 0.28971E+00 0.26270E+00 0.23785E+00 0.21541E+00 0.19563E+00 0.17753E+00 0.16148E+00 0.14731E+00 0.13473E+00 0.12353E+00 0.11355E+00 0.10463E+00 0.96591E-01 0.89378E-01 0.82894E-01 0.77031E-01 0.71733E-01 0.66997E-01 0.62589E-01 0.58578E-01 0.54944E-01 0.51617E-01 0.48568E-01 0.45777E-01 0.43195E-01 0.40819E-01 0.38619E-01 0.38327E+00 0.34760E+00 0.31205E+00 0.27814E+00 0.24718E+00 0.21967E+00 0.19553E+00 0.17485E+00 0.15624E+00 0.14008E+00 0.12609E+00 0.11388E+00 0.10318E+00 0.93795E-01 0.85518E-01 0.78144E-01 0.71612E-01 0.65809E-01 0.60618E-01 0.55976E-01 0.51874E-01 0.48082E-01 0.44663E-01 0.41595E-01 0.38810E-01 0.36277E-01 0.33977E-01 0.31864E-01 0.29933E-01 0.28157E-01 0.39406E+00 0.34884E+00 0.30423E+00 0.26382E+00 0.22853E+00 0.19836E+00 0.17274E+00 0.15150E+00 0.13276E+00 0.11690E+00 0.10348E+00 0.92023E-01 0.82165E-01 0.73667E-01 0.66298E-01 0.59828E-01 0.54183E-01 0.49237E-01 0.44870E-01 0.41014E-01 0.37652E-01 0.34570E-01 0.31822E-01 0.29383E-01 0.27191E-01 0.25216E-01 0.23440E-01 0.21821E-01 0.20355E-01 0.19016E-01 0.40777E+00 0.34980E+00 0.29325E+00 0.24492E+00 0.20488E+00 0.17224E+00 0.14567E+00 0.12452E+00 0.10634E+00 0.91441E-01 0.79217E-01 0.69042E-01 0.60499E-01 0.53298E-01 0.47183E-01 0.41911E-01 0.37396E-01 0.33510E-01 0.30132E-01 0.27197E-01 0.24679E-01 0.22394E-01 0.20385E-01 0.18626E-01 0.17064E-01 0.15673E-01 0.14435E-01 0.13319E-01 0.12318E-01 0.11413E-01 0.42666E+00 0.34960E+00 0.27548E+00 0.21700E+00 0.17210E+00 0.13796E+00 0.11181E+00 0.92183E-01 0.75908E-01 0.63158E-01 0.53124E-01 0.45066E-01 0.38515E-01 0.33155E-01 0.28727E-01 0.24999E-01 0.21883E-01 0.19260E-01 0.17027E-01 0.15124E-01 0.13525E-01 0.12094E-01 0.10856E-01 0.97906E-02 0.88582E-02 0.80398E-02 0.73218E-02 0.66820E-02 0.61157E-02 0.56094E-02 0.46200E+00 0.34438E+00 0.23544E+00 0.16485E+00 0.11865E+00 0.87819E-01 0.66525E-01 0.51971E-01 0.40547E-01 0.32186E-01 0.25987E-01 0.21253E-01 0.17569E-01 0.14673E-01 0.12365E-01 0.10481E-01 0.89545E-02 0.77060E-02 0.66701E-02 0.58089E-02 0.51037E-02 0.44820E-02 0.39554E-02 0.35118E-02 0.31302E-02 0.28009E-02 0.25168E-02 0.22673E-02 0.20497E-02 0.18578E-02 0.67325E-01 0.49479E-01 0.33017E-01 0.22594E-01 0.15925E-01 0.11568E-01 0.86153E-02 0.66346E-02 0.50982E-02 0.39912E-02 0.31823E-02 0.25724E-02 0.21033E-02 0.17387E-02 0.14512E-02 0.12186E-02 0.10320E-02 0.88070E-03 0.75622E-03 0.65357E-03 0.57025E-03 0.49719E-03 0.43577E-03 0.38440E-03 0.34050E-03 0.30286E-03 0.27058E-03 0.24239E-03 0.21795E-03 0.19650E-03 pythia8-8.1.80.orig/xmldoc/ctq66.00.pds0000444000175000017500000141701612217346302015520 0ustar sunsunPDF Table for Fit #: p82a3 Ordr, Nfl, lambda Qmass 1, 2, 3, 4, 5, 6 2. 5. 0.2262 0.001 0.001 0.200 1.300 4.500 175.000 IPD0, IHDN, IKNL, NfMx, Nfval, KF, Nelmt 1 1 2 5 2 12 45300 NX, NT, JT, NG, NTL(NG+1) 150 24 1 2 24 (NTL(I), NTN(I), TLN(I), DTN(I), I =1, NG) 0 7 5.58779E-01 7.66540E-02 7 17 1.09536E+00 8.64425E-02 QINI, QMAX, (QV(I), TV(I), I =0, NT) 1.30000E+00 1.00000E+05 1.30000E+00 5.58779E-01 1.49431E+00 6.35433E-01 1.73684E+00 7.12087E-01 2.04307E+00 7.88741E-01 2.43457E+00 8.65395E-01 2.94191E+00 9.42049E-01 3.60899E+00 1.01870E+00 4.50000E+00 1.09536E+00 5.89476E+00 1.18180E+00 7.91236E+00 1.26824E+00 1.09066E+01 1.35468E+00 1.54759E+01 1.44113E+00 2.26644E+01 1.52757E+00 3.43551E+01 1.61401E+00 5.40692E+01 1.70045E+00 8.86525E+01 1.78690E+00 1.51992E+02 1.87334E+00 2.73584E+02 1.95978E+00 5.19288E+02 2.04622E+00 1.04437E+03 2.13267E+00 2.23717E+03 2.21911E+00 5.13351E+03 2.30555E+00 1.26969E+04 2.39199E+00 3.40794E+04 2.47844E+00 1.00000E+05 2.56488E+00 XMIN, XCR, (XV(I), I =1, NX) 1.00000E-08 2.00000E+00 1.00000E-08 1.21431E-08 1.47455E-08 1.79056E-08 2.17430E-08 2.64028E-08 3.20612E-08 3.89322E-08 4.72758E-08 5.74075E-08 6.97106E-08 8.46503E-08 1.02792E-07 1.24821E-07 1.51572E-07 1.84055E-07 2.23500E-07 2.71398E-07 3.29562E-07 4.00190E-07 4.85954E-07 5.90099E-07 7.16563E-07 8.70129E-07 1.05661E-06 1.28304E-06 1.55801E-06 1.89190E-06 2.29735E-06 2.78968E-06 3.38752E-06 4.11348E-06 4.99500E-06 6.06542E-06 7.36521E-06 8.94352E-06 1.08600E-05 1.31871E-05 1.60129E-05 1.94440E-05 2.36101E-05 2.86686E-05 3.48105E-05 4.22678E-05 5.13218E-05 6.23140E-05 7.56590E-05 9.18593E-05 1.11525E-04 1.35395E-04 1.64366E-04 1.99524E-04 2.42186E-04 2.93943E-04 3.56724E-04 4.32859E-04 5.25162E-04 6.37028E-04 7.72549E-04 9.36645E-04 1.13522E-03 1.37535E-03 1.66548E-03 2.01565E-03 2.43777E-03 2.94587E-03 3.55639E-03 4.28845E-03 5.16411E-03 6.20855E-03 7.45017E-03 8.92057E-03 1.06543E-02 1.26885E-02 1.50622E-02 1.78152E-02 2.09872E-02 2.46162E-02 2.87372E-02 3.33809E-02 3.85725E-02 4.43308E-02 5.06677E-02 5.75882E-02 6.50909E-02 7.31681E-02 8.18071E-02 9.09910E-02 1.00700E-01 1.10910E-01 1.21599E-01 1.32742E-01 1.44313E-01 1.56288E-01 1.68643E-01 1.81355E-01 1.94402E-01 2.07763E-01 2.21418E-01 2.35349E-01 2.49538E-01 2.63971E-01 2.78630E-01 2.93504E-01 3.08578E-01 3.23841E-01 3.39282E-01 3.54890E-01 3.70656E-01 3.86571E-01 4.02626E-01 4.18815E-01 4.35129E-01 4.51563E-01 4.68109E-01 4.84763E-01 5.01519E-01 5.18372E-01 5.35316E-01 5.52349E-01 5.69465E-01 5.86660E-01 6.03932E-01 6.21275E-01 6.38688E-01 6.56167E-01 6.73709E-01 6.91311E-01 7.08970E-01 7.26683E-01 7.44449E-01 7.62263E-01 7.80124E-01 7.98028E-01 8.15971E-01 8.33950E-01 8.51960E-01 8.69994E-01 8.88042E-01 9.06086E-01 9.24098E-01 9.42012E-01 9.59663E-01 9.76499E-01 9.90191E-01 9.96561E-01 9.98540E-01 9.99336E-01 9.99749E-01 1.00000E+00 Parton Distribution Table: 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 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    PDF Selection

    This page contains five subsections. The first deals with how to pick the parton distribution set for protons, including from LHAPDF, to be used for all proton and antiproton beams. The second is a special option that allows a separate PDF set to be used for the hard process only, while the first choice would still apply to everything else. The third and fourth give access to pion and Pomeron PDF's, respectively, the latter being used to describe diffractive systems. The fifth gives the possibility to switch off the lepton "parton density". More information on PDF classes is found here.

    Parton densities for protons

    The selection of parton densities is made once and then is propagated through the program. It is essential to make an informed choice, for several reasons Kas10: Warning 1: the choice of PDF set affects a number of properties of events. A change of PDF therefore requires a complete retuning e.g. of the multiparton-interactions model for minimum-bias and underlying events. Warning 2: People often underestimate the differences between different sets on the market. The sets for the same order are constructed to behave more or less similarly at large x and Q^2, while the multiparton interactions are dominated by the behaviour in the region of small x and Q^2. A good PDF parametrization ought to be sensible down to x = 10^-6 (x = 10^-7) and Q^2 = 1 GeV^2 for Tevatron (LHC) applications. Unfortunately there are distributions on the market that completely derail in that region. The main51.cc and main52.cc programs in the examples subdirectory provide some examples of absolutely minimal sanity checks before a new PDF set is put in production. Warning 3: NLO and LO sets tend to have quite different behaviours, e.g. NLO ones have less gluons at small x, which then is compensated by positive corrections in the NLO matrix elements. Therefore do not blindly assume that an NLO tune has to be better than an LO one when combined with the LO matrix elements in PYTHIA. There are explicit examples where such thinking can lead you down the wrong alley, especially if you study low-pT physics. In the list below you should therefore be extra cautious when using set 6 or set 9.

    The simplest option is to pick one of the distributions available internally: Parton densities to be used for proton beams (and, by implication, antiproton ones): Note: the alpha_s(M_Z) values and the order of the running in the description above is purely informative, and does not affect any other parts of the program. Instead you have the freedom to set alpha_s(M_Z) value and running separately for hard processes (including resonance decays), multiparton interactions, initial-state radiation, and final-state radiation.

    This is a reasonably complete list of recent LO fits, both ones within the normal LO context and ones with modifications for better matching to event generators. In addition two older sets are included for backwards reference (most studies to date are based on CTEQ 5L). If you link to the LHAPDF library Wha05 you get access to a much wider selection. Warning 1: owing to previous problems with the behaviour of PDF's beyond the x and Q^2 boundaries of a set, you should only use LHAPDF version 5.3.0 or later. Warning 2: the behaviour of the LHAPDF sets need not be identical with the implementation found in PYTHIA. Specifically we are aware of the following points that may influence a comparison.
    (a) CTEQ 5L in PYTHIA is the parametrization, in LHAPDF the grid interpolation.
    (b) MRST LO* and LO** in PYTHIA is based on an updated edition, where one makes use of the expanded MSTW grid format, while LHAPDF is based on the original smaller grid.
    (c) The CTEQ 6 and CT09MC sets in PYTHIA are frozen at the boundaries of the grid, by recommendation of the authors, while LHAPDF also offers an option with a smooth extrapolation outside the grid boundaries. If off then the choice of proton PDF is based on PDF:pSet above. If on then it is instead based on the choice of PDF:LHAPDFset and PDF:LHAPDFmember below. Note: in order for this option to work you must have compiled PYTHIA appropriately and have set the LHAPATH environment variable to provide the data-files directory of your local LHAPDF installation. See the README file in the examples directory for further instructions. Name of proton PDF set from LHAPDF to be used. You have to choose from the list of available sets. Examples of some fairly recent ones (but still less recent than found above) would be cteq61.LHpdf, cteq61.LHgrid, cteq6l.LHpdf, cteq6ll.LHpdf, MRST2004nlo.LHpdf, MRST2004nlo.LHgrid, MRST2004nnlo.LHgrid and MRST2004FF3lo.LHgrid. If you pick a LHpdf set it will require some calculation the first time it is called. Technical note: if you provide a name beginning with a slash (/) it is assumed you want to provide the full file path and then initPDFsetM(name) is called, else the correct path is assumed already set and initPDFsetByNameM(name) is called. Further choice of a specific member from the set picked above. Member 0 should normally correspond to the central value, with higher values corresponding to different error PDF's somewhat off in different directions. You have to check from set to set which options are open. Note: you can only use one member in a run, so if you want to sweep over many members you either have to do many separate runs or, as a simplification, save the pdf weights at the hard scattering and do an offline reweighting of events. Parton densities have a guaranteed range of validity in x and Q^2, and what should be done beyond that range usually is not explained by the authors of PDF sets. Nevertheless these boundaries very often are exceeded, e.g. minimum-bias studies at LHC may sample x values down to 10^-8, while many PDF sets stop already at 10^-5. The default behaviour is then that the PDF's are frozen at the boundary, i.e. xf(x,Q^2) is fixed at its value at x_min for all values x < x_min, and so on. This is a conservative approach. Alternatively, if you switch on extrapolation, then parametrizations will be extended beyond the boundaries, by some prescription. In some cases this will provide a more realistic answer, in others complete rubbish. Another problem is that some of the PDF-set codes will write a warning message anytime the limits are exceeded, thus swamping your output file. Therefore you should study a set seriously before you run it with this switch on.

    If you want to use PDF's not found in LHAPDF, or you want to interface LHAPDF another way, you have full freedom to use the more generic interface options.

    Parton densities for protons in the hard process

    The above options provides a PDF set that will be used everywhere: for the hard process, the parton showers and the multiparton interactions alike. As already mentioned, therefore a change of PDF should be accompanied by a complete retuning of the whole MPI framework, and maybe more. There are cases where one may want to explore different PDF options for the hard process, but would not want to touch the rest. If several different sets are to be compared, a simple reweighting based on the originally used flavour, x, Q^2 and PDF values may offer the best route. The options in this section allow a choice of the PDF set for the hard process alone, while the choice made in the previous section would still be used for everything else. The hardest interaction of the minimum-bias process is part of the multiparton-interactions framework and so does not count as a hard process here.

    Of course it is inconsistent to use different PDF's in different parts of an event, but if the x and Q^2 ranges mainly accessed by the components are rather different then the contradiction would not be too glaring. Furthermore, since standard PDF's are one-particle-inclusive we anyway have to 'invent' our own PDF modifications to handle configurations where more than one parton is kicked out of the proton Sjo04.

    The PDF choices that can be made are the same as above, so we do not repeat the detailed discussion. If on then select a separate PDF set for the hard process, using the variables below. If off then use the same PDF set for everything, as already chosen above. Parton densities to be used for proton beams (and, by implication, antiproton ones): If off then the choice of proton PDF is based on hardpPDFset above. If on then it is instead based on the choice of hardLHAPDFset and hardLHAPDFmember below. Note that if you want to use LHAPDF here, and you also use LHAPDF for the "normal" PDF set, then LHAPDF must have been compiled so as to handle (at least) two concurrent sets, with the configure statement --with-max-num-pdfsets=2. Name of proton PDF set from LHAPDF to be used. Further choice of a specific member from the set picked above.

    Note that there is no separate equivalent of the PDF:extrapolateLHAPDF flag specifically for the hard PDF. Since LHAPDF only has one global flag for extrapolation or not, the choice for the normal PDF's also applies to the hard ones.

    Parton densities for pions

    The parton densities of the pion are considerably less well known than those of the proton. There are only rather few sets on the market, and none particularly recent. Only one comes built-in, but others can be accessed from LHAPDF. Input parametrizations are for the pi+. >From this the pi- is obtained by charge conjugation and the pi0 from averaging (half the pions have d dbar valence quark content, half u ubar.

    Much of the switches are taken over from the proton case, with obvious modifications; therefore the description is briefer. Currently we have not seen the need to allow separate parton densities for hard processes. When using LHAPDF the PDF:extrapolateLHAPDF switch of the proton also applies to pions. Internal parton densities that can be used for pion beams, currently with only one choice. If off then the choice of proton PDF is based on PDF:piSet above. If on then it is instead based on the choice of PDF:piLHAPDFset and PDF:piLHAPDFmember below. Name of pion PDF set from LHAPDF to be used. You have to choose from the list of available sets. Further choice of a specific member from the set picked above.

    Parton densities for Pomerons

    The Pomeron is introduced in the description of diffractive events, i.e. a diffractive system is viewed as a Pomeron-proton collision at a reduced CM energy. Here the PDF's are even less well known. Most experimental parametrizations are NLO, which makes them less well suited for Monte Carlo applications. Furthermore note that the momentum sum is arbitrarily normalized to a non-unity value. Parton densities that can be used for Pomeron beams. the parameter a in the ansatz xg(x) = N_ab x^a (1 - x)^b for option 1 above. the parameter b in the ansatz xg(x) = N_ab x^a (1 - x)^b for option 1 above. the parameter a in the ansatz xq(x) = N_ab x^a (1 - x)^b for option 1 above. the parameter b in the ansatz xq(x) = N_ab x^a (1 - x)^b for option 1 above. the fraction of the Pomeron momentum carried by quarks for option 1 above, with the rest carried by gluons. the suppression of the s quark density relative to that of the d and u ones for option 1 above. Rescale the four H1 fits above by this uniform factor, e.g. to bring up their momentum sum to around unity. By default all three have a momentum sum of order 0.5, suggesting that a factor around 2.0 should be used. You can use examples/main51.cc to get a more precise value. Note that also other parameters in the diffraction framework may need to be retuned when this parameter is changed.

    Parton densities for leptons

    For electrons/muons/taus there is no need to choose between different parametrizations, since only one implementation is available, and should be rather uncontroversial (apart from some technical details). However, insofar as e.g. e^+ e^- data often are corrected back to a world without any initial-state photon radiation, it is useful to have a corresponding option available here. Use parton densities for lepton beams or not. If off the colliding leptons carry the full beam energy, if on part of the energy is radiated away by initial-state photons. In the latter case the initial-state showers will generate the angles and energies of the set of photons that go with the collision. In addition one collinear photon per beam carries any leftover amount of energy not described by shower emissions. If the initial-state showers are switched off these collinear photons will carry the full radiated energy.

    Neutrinos are always taken pointlike. Do note that the phase space selection machinery currently does not allow one resolved and one unresolved beam. For lepton-neutrino collisions to work you must therefore set PDF:lepton = off.

    Incoming parton selection

    There is one useful degree of freedom to restrict the set of incoming quark flavours for hard processes. It does not change the PDF's as such, only which quarks are allowed to contribute to the hard-process cross sections. Note that separate but similarly named modes are available for multiparton interactions and spacelike showers. Number of allowed incoming quark flavours in the beams; a change to 4 would thus exclude b and bbar as incoming partons, etc.
    pythia8-8.1.80.orig/xmldoc/mrstlostarstar.00.dat0000444000175000017500000121232312217346304017637 0ustar sunsun # Tue Oct 27 14:26:24 2009 # MSTW 2008 LO PDF grid for central fit. # distance(t),tolerance(T) = 0. 0. # mCharm = 1.43 # mBottom = 4.30 # alphaS(1GeV) = 0.40768 # alphaS(MZ) = 0.11517 # alphaSorder,alphaSnfmax = 0, 5 # nExtraFlavours = 0 xg xd xu xs xc xb xdv xuv xsv 1.2042E+01 1.3018E+00 1.3129E+00 6.4816E-01 0.0000E+00 0.0000E+00 5.5017E-03 1.6579E-02 0.0000E+00 1.8147E+01 1.3513E+00 1.3625E+00 7.0214E-01 -2.4286E-17 -2.4286E-17 5.5603E-03 1.6674E-02 0.0000E+00 2.3965E+01 1.4062E+00 1.4173E+00 7.6048E-01 -1.2924E-16 -1.2924E-16 5.6072E-03 1.6750E-02 -2.2204E-16 3.5512E+01 1.5303E+00 1.5415E+00 8.9026E-01 -5.5077E-16 -5.5077E-16 5.6849E-03 1.6875E-02 -1.1102E-15 3.5512E+01 1.5303E+00 1.5415E+00 8.9026E-01 2.9995E-07 -5.5077E-16 5.6849E-03 1.6875E-02 -1.1102E-15 4.3963E+01 1.6321E+00 1.6433E+00 9.9556E-01 1.1216E-01 -9.9920E-16 5.7339E-03 1.6953E-02 -1.9984E-15 5.5485E+01 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pythia8-8.1.80.orig/xmldoc/piK-Estabrooks.dat0000444000175000017500000000740612217346315017157 0ustar sunsun# Pion-kaon partial-wave data, analysis of Estabrooks et. al. # Nucl. Phys. B133 (1978) 490-524 # Notation for column headers is L,2I # Entries in each column are S_n = (1 - eta^2) and delta_L set eType Wcm set eUnit GeV set input Sn,delta set dUnit deg # Isospin 3/2 elastic Wcm 0,3 1,3 2,3 0.73 0.0 -10.0 0.0 0.0 0.0 0.0 0.82 0.0 -14.5 0.0 0.0 0.0 0.0 0.90 0.0 -16.5 0.0 0.0 0.0 0.0 0.94 0.0 -17.0 0.0 0.0 0.0 0.0 0.98 0.0 -18.0 0.0 0.0 0.0 0.0 1.02 0.0 -18.5 0.0 -0.8 0.0 -0.7 1.06 0.0 -18.2 0.0 -0.2 0.0 -0.6 1.10 0.0 -21.4 0.0 -0.9 0.0 -1.3 1.14 0.0 -21.1 0.0 -1.1 0.0 -1.2 1.18 0.0 -22.4 0.0 -0.6 0.0 -1.3 1.22 0.0 -23.5 0.0 -0.6 0.0 -1.5 1.26 0.0 -23.9 0.0 -0.6 0.0 -1.3 1.30 0.0 -23.8 0.0 -0.1 0.0 -1.7 1.34 0.0 -26.4 0.0 -0.7 0.0 -2.5 1.38 0.0 -25.0 0.0 -0.3 0.0 -1.5 1.44 0.0 -27.4 0.0 -1.2 0.0 -2.3 1.52 0.0 -26.7 0.0 -2.4 0.0 -1.5 1.60 0.0 -25.6 0.0 -2.1 0.0 -1.4 1.72 0.0 -22.8 0.0 -2.4 0.0 -0.5 # Isospin 1/2 elastic Wcm 0,1 1,1 2,1 3,1 0.730 0.0 21.0 0.0 6.0 0.0 0.0 0.0 0.0 0.780 0.0 27.2 0.0 10.0 0.0 0.0 0.0 0.0 0.820 0.0 40.7 0.0 14.0 0.0 0.0 0.0 0.0 0.845 0.0 36.8 0.0 23.9 0.0 0.0 0.0 0.0 0.855 0.0 40.4 0.0 28.3 0.0 0.0 0.0 0.0 0.865 0.0 38.0 0.0 39.5 0.0 0.0 0.0 0.0 0.875 0.0 38.1 0.0 49.6 0.0 0.0 0.0 0.0 0.885 0.0 39.1 0.0 70.6 0.0 0.0 0.0 0.0 0.895 0.0 39.6 0.0 96.2 0.0 0.0 0.0 0.0 0.905 0.0 34.7 0.0 108.3 0.0 0.0 0.0 0.0 0.915 0.0 33.5 0.0 122.4 0.0 0.0 0.0 0.0 0.925 0.0 37.2 0.0 134.6 0.0 0.0 0.0 0.0 0.935 0.0 40.9 0.0 140.4 0.0 0.0 0.0 0.0 0.945 0.0 42.8 0.0 147.4 0.0 0.0 0.0 0.0 0.955 0.0 46.9 0.0 150.9 0.0 0.0 0.0 0.0 0.980 0.0 48.4 0.0 157.0 0.0 0.0 0.0 0.0 1.020 0.0 53.9 0.0 162.9 0.0 0.0 0.0 0.0 1.060 0.0 57.8 0.0 165.2 0.0 0.0 0.0 0.0 1.100 0.0 60.2 0.0 167.5 0.0 0.0 0.0 0.0 #1.140 0.0 61.2 0.0 168.5 0.0 0.0 0.0 0.0 #1.180 0.0 66.3 0.0 173.0 0.0 0.0 0.0 0.0 #1.220 0.0 69.3 0.0 170.8 0.0 0.0 0.0 0.0 #1.260 0.0 71.7 0.0 166.7 0.0 0.0 0.0 0.0 #1.300 0.0 79.3 0.0 176.3 0.0 0.0 0.0 0.0 # Inelastic region data. Scattering amplitude: # a_J = |a_J| exp(i phi_L) # and column entries |a_J| and phi_J. set input mod,phi # Isospin 1/2 inelastic Wcm 0,1 1,1 2,1 3,1 1.14 0.87 73. 0.35 169. 0.01 0. 0.00 0. 1.18 0.93 78. 0.21 173. 0.09 5. 0.00 0. 1.22 0.96 81. 0.28 171. 0.04 2. 0.00 0. 1.26 0.98 83. 0.40 157. 0.01 1. 0.00 0. 1.30 1.01 99. 0.13 157. 0.35 14. 0.00 0. 1.34 1.05 104. 0.20 164. 0.40 22. 0.00 0. 1.38 1.06 109. 0.19 154. 0.75 39. 0.00 0. 1.42 1.00 126. 0.20 163. 1.02 74. 0.00 0. 1.46 0.84 142. 0.21 169. 1.02 115. 0.00 0. # Solution A 1.50 0.52 146. 0.30 209. 0.71 138. 0.08 8. 1.56 0.40 164. 0.32 222. 0.58 152. 0.12 34. 1.65 0.33 143. 0.22 177. 0.48 135. 0.29 30. 1.75 0.39 131. 0.23 160. 0.44 148. 0.43 70. 1.85 0.48 153. 0.28 189. 0.48 183. 0.43 127. ## Solution B ##1.50 0.63 161. 0.16 103. 0.58 138. 0.09 9. ##1.56 0.56 183. 0.22 114. 0.50 152. 0.11 26. ##1.65 0.27 190. 0.50 111. 0.30 141. 0.28 30. ##1.75 0.14 97. 0.53 144. 0.23 138. 0.43 70. ##1.85 0.36 122. 0.52 187. 0.33 165. 0.43 127. ## Solution C ##1.50 0.64 114. 0.17 75. 0.67 138. 0.09 7. ##1.56 0.59 122. 0.20 83. 0.48 152. 0.12 29. ##1.65 0.55 117. 0.20 98. 0.31 141. 0.28 30. ##1.75 0.56 127. 0.23 119. 0.29 139. 0.41 70. ##1.85 0.61 152. 0.30 115. 0.29 149. 0.43 127. ## Solution D ##1.50 0.45 127. 0.49 58. 0.64 138. 0.08 2. ##1.56 0.24 121. 0.60 70. 0.42 152. 0.11 17. ##1.65 0.23 92. 0.55 99. 0.12 174. 0.31 30. ##1.75 0.38 91. 0.51 132. 0.13 90. 0.42 70. ##1.85 0.58 123. 0.36 159. 0.27 113. 0.42 127. pythia8-8.1.80.orig/xmldoc/MasterSwitches.xml0000444000175000017500000002047512217346304017316 0ustar sunsun

    Master Switches

    Sometimes it may be convenient to omit certain aspects of the event generation chain. This cannot be motivated in a full-blown production run, but can often be convenient for own understanding and for debug purposes. The flags on this page allow just that.

    The event generation is subdivided into three levels: the process level, the parton level and the hadron level, and flags are grouped accordingly.

    Process Level

    The ProcessLevel class administrates the initial step of the event generation, wherein the basic process is selected. Currently this is done either using some of the internal processes, or with Les Houches Accord input.

    There could not be a complete event without an initial process, so it would not be a normal action to switch off this step. Furthermore, without a process set, it is also not possible to carry out the tasks on the parton level. It is still possible, however, to hadronize a parton-level configuration provided by some external program. If off, do not attempt to carry out any generation at all on the process level. For the parton level only final-state radiation is possible, using the Pythia::forceTimeShower(...) method. Do allow parton configurations stored in the event record to hadronize and hadrons to decay, however, as set by the HadronLevel switches. Further details are found here.

    For ProcessLevel:all = on one part of the event generation on this level may be switched off individually: Master switch to allow resonance decays; on/off = true/false. Normal hadrons and leptons do not count as resonances, so this is aimed specifically towards Z^0, W^+-, t, h^0 and similar objects beyond the Standard Model. Do not use this option if you may produce coloured resonances and intend to allow hadronization, since currently the program would not know how to handle this.

    It is possible to stop the generation immediately after the basic process has been selected, see PartonLevel:all below.

    PartonLevel

    The PartonLevel class administrates the middle step of the event generation, i.e. the evolution from an input (hard) process from ProcessLevel, containing a few partons only, to a complete parton-level configuration to be handed on to HadronLevel. This step involves the application of initial- and final-state radiation, multiparton interactions and the structure of beam remnants. If off then stop the generation after the hard process has been generated, but before the parton-level and hadron-level steps. The process record is filled, but the event one is then not.

    For PartonLevel:all = on some parts of the event generation on this level may be switched off individually: Master switch for multiparton interactions; on/off = true/false. Further options are found here. Master switch for initial-state radiation; on/off = true/false. Further options are found here. Master switch for final-state radiation; on/off = true/false. Further options are found here. If you leave this switch on, the following two switches allow more detailed control to switch off only parts of the showers. Switch for final-state radiation in association with the hard process itself; on/off = true/false. In addition PartonLevel:FSR must be on for these emissions to occur. Master switch for final-state radiation in any resonance decays subsequent to the hard process itself; on/off = true/false. In addition PartonLevel:FSR must be on for these emissions to occur. If on then do resonance decays early, before beam handling including colour reconnection. If off then decays are done afterwards, and so are unaffected by colour reconnection. The early-decay option is still primitive, for some first studies. Eventually the choice should be made individually for each resonance based on lifetime (and the environment).

    Switching off all the above MPI/ISR/FSR switches is not equivalent to setting PartonLevel:all = off. In the former case a minimal skeleton of parton-level operations are carried out, such as tying together the scattered partons with the beam remnants into colour singlets, and storing this information in the event record. It is therefore possible to go on and hadronize the event, if desired. In the latter case no operations at all are carried out on the parton level, and therefore it is also not possible to go on to the hadron level. Master switch for addition of beam remnants; on/off = true/false. Only intended for very special applications, and cannot be used to generate complete events. Specifically, unlike the other switches above, the program will complain and possibly crash unlike you also set HadronLevel:all = off and Check:event = off.

    It is possible to stop the generation immediately after the parton level has been set up, see HadronLevel:all below.

    HadronLevel

    The HadronLevel class administrates the final step of the event generation, wherein the partonic configuration from PartonLevel is hadronized, including string fragmentation and secondary decays.

    Most of the code in this class itself deals with subdividing the partonic content of the event into separate colour singlets, that can be treated individually by the string fragmentation machinery. When a junction and an antijunction are directly connected, it also breaks the string between the two, so that the topology can be reduced back to two separate one-junction systems, while still preserving the expected particle flow in the junction-junction string region(s). If off then stop the generation after the hard process and parton-level activity has been generated, but before the hadron-level steps.

    For HadronLevel:all = on some parts of the event generation on this level may be switched off individually: Master switch for hadronization; on/off = true/false. Further options are found here. Master switch for decays; on/off = true/false. Further options are found here. Master switch for the simulation of Bose-Einstein effects; on/off = true/false. Further options are found here.

    Printing

    Can be set on to avoid the printing during program execution, to the largest extent possible. This flag acts by setting the relevant values for Init:showProcesses, Init:showMultipartonInteractions, Init:showChangedSettings, Init:showAllSettings, Init:showChangedParticleData, Init:showChangedResonanceData, Init:showAllParticleData, Init:showOneParticleData, Next:numberCount, Next:numberShowLHA, Next:numberShowInfo, Next:numberShowProcess, and Next:numberShowEvent. The change is to off or 0 for Print:quiet = off, and restores to the respective default value for = on. Those changes take effect immediately, so individual settings can be changed afterwards.
    pythia8-8.1.80.orig/xmldoc/Welcome.xml0000444000175000017500000000067112217346320015736 0ustar sunsun pythia8-8.1.80.orig/xmldoc/NNPDF23_lo_as_0130_qed.grid0000444000175000017500000402636612217346310020167 0ustar sunsun 'Version' '5.8.9' 'Description:' 'NNPDF23_lo_as_0130_qed.grid' 'NNPDF2.3QED LO, arxiv:1308.0598' 'LO QCD + LO QED PDF set, alphas(MZ)=0.130' 'NNPDF Collaboration: R.D. Ball, V. Bertone,' 'S. Carrazza, L. Del Debbio, S. Forte,' 'A. Guffanti, N.P. Hartland, J. Rojo' 'This set has 100 member PDF' 'mem=0 --> average on replicas. ' 'Evolution - pol. interpolation on the LH grid.' 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    Total Cross Sections

    The SigmaTotal class returns the total, elastic, diffractive and nondiffractive cross sections in hadronic collisions, and also the slopes of the d(sigma)/dt distributions. Most of the parametrizations used are from Sch94, Sch97 which borrows some of the total cross sections from Don92. If you use the MBR (Minimum Bias Rockefeller) model Cie12, Diffraction:PomFlux = 5, this model contains its own parametrizations of all cross sections in p p and pbar p collisions.

    There are strong indications that the currently implemented diffractive cross section parametrizations, which should be in reasonable agreement with data at lower energies, overestimate the diffractive rate at larger values. If you wish to explore this (or other) aspect, it is possible to override the cross section values in two different ways. The first offers (almost) complete freedom, but needs to be defined separately for each CM energy, while the second introduces a simpler parametrized damping. The two cannot be combined. Furthermore the Coulomb term for elastic scattering, which by default is off, can be switched on.

    The allowed combinations of incoming particles are p + p, pbar + p, pi+ + p, pi- + p, pi0/rho0 + p, phi + p, J/psi + p, rho + rho, rho + phi, rho + J/psi, phi + phi, phi + J/psi, J/psi + J/psi. The strong emphasis on vector mesons is related to the description of gamma + p and gamma + gamma interactions in a Vector Dominance Model framework (which will not be available for some time to come, so this is a bit of overkill). Nevertheless, the sections below, with allowed variations, are mainly intended to make sense for p + p.

    Central diffraction

    Central diffraction (CD), a.k.a. double Pomeron exchange (DPE), was not part of the framework in Sch94. It has now been added for multiparticle states, i.e. excluding the resonance region below 1 GeV mass, as well as other exclusive states, but only for p p or pbar p. It uses the same proton-Pomeron vertex as in single diffraction, twice, to describe x_Pomeron and t spectra. This fixes the energy dependence, which has been integrated and parametrized. The absolute normalization has been left open, however. Furthermore, since CD has not been included in previous tunes to data, a special flag is available to reproduce the old behaviour (with due complications when one does not want to do this). The CD cross section for p p and pbar p collisions, normalized to its value at 2 TeV CM energy, expressed in mb. The energy dependence is then parametrized, and behaves roughly like ln^1.5(s). Is used for the options Diffraction:PomFlux = 1 - 4, while the MBR model (= 5) has its own parametrization. several existing tunes do not include CD. An inclusion of a nonvanishing CD cross section directly affects the nondiffractive phenomenology (even if not dramatically), and so this flag is used to switch off the CD cross section in such tunes. You can switch it back on after the selection of a tune, if you so wish. This option has no effect for the MBR model (Diffraction:PomFlux = 5), where the CD cross section has been included from the onset.

    Set cross sections

    Allow a user to set own cross sections by hand; on/off = true/false.

    When SigmaTotal:setOwn = on, the user is expected to set values for the corresponding cross sections: Total cross section in mb. Elastic cross section in mb. Single Diffractive cross section A + B -> X + B in mb. Single Diffractive cross section A + B -> A + X in mb. Double Diffractive cross section A + B -> X_1 + X_2 in mb. Central Diffractive cross section A + B -> A + X + B in mb.

    Note that the total cross section subtracted by the elastic and various diffractive ones gives the inelastic nondiffractive cross section, which therefore is not set separately. If this cross section evaluates to be negative the internal parametrizations are used instead of the ones here. However, since the nondiffractive inelastic cross section is what makes up the minimum-bias event class, and plays a major role in the description of multiparton interactions, it is important that a consistent set is used.

    Dampen diffractive cross sections

    As already noted, unitarization effects may dampen the rise of diffractive cross sections relative to the default parametrizations. The settings here allows one way to introduce a dampening, which is used in some of the existing tunes. Allow a user to dampen diffractive cross sections; on/off = true/false.

    When SigmaDiffractive:dampen = on, the three diffractive cross sections are damped so that they never can exceed the respective values below. Specifically, if the standard parametrization gives the cross section sigma_old(s) and a fixed sigma_max is set, the actual cross section becomes sigma_new(s) = sigma_old(s) * sigma_max / (sigma_old(s) + sigma_max). This reduces to sigma_old(s) at low energies and to sigma_max at high ones. Note that the asymptotic value is approached quite slowly, however. The above sigma_max for A + B -> X + B in mb. The above sigma_max for A + B -> A + X in mb. The above sigma_max for A + B -> X_1 + X_2 in mb. The above sigma_max for A + B -> A + X + B in mb.

    As above, a reduced diffractive cross section automatically translates into an increased nondiffractive one, such that the total (and elastic) cross section remains fixed.

    Set elastic cross section

    In the above option the t slopes are based on the internal parametrizations. In addition there is no Coulomb-term contribution to the elastic (or total) cross section, which of course becomes infinite if this contribution is included. If you have switched on SigmaTotal:setOwn you can further switch on a machinery to include the Coulomb term, including interference with the conventional strong-interaction Pomeron one Ber87. Then the elastic cross section is no longer taken from SigmaTotal:sigmaEl but derived from the parameters below and SigmaTotal:sigmaTot, using the optical theorem. The machinery is only intended to be used for p p and pbar p collisions. The description of diffractive events, and especially their slopes, remains unchanged. Allow a user to set parameters for the normalization and shape of the elastic cross section the by hand; yes/no = true/false. the slope b of the strong-interaction term exp(bt), in units of GeV^-2. the ratio of the real to the imaginary parts of the nuclear scattering amplitude. the main parameter of the electric form factor G(t) = lambda^2 / (lambda + |t|)^2, in units of GeV^2. since the Coulomb contribution is infinite a lower limit on |t| must be set to regularize the divergence, in units of GeV^2. The Coulomb term is taken to contain a phase factor exp(+- i alpha phi(t)), with + for p p and - for pbar p, where phi(t) = - phaseConst - ln(-B t/2). This constant is model dependent Cah82. pythia8-8.1.80.orig/xmldoc/Index.xml0000444000175000017500000001301712217346303015411 0ustar sunsun Pythia logo

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    pythia8-8.1.80.orig/xmldoc/FlavourSelection.xml0000444000175000017500000003406612217346302017634 0ustar sunsun

    Flavour Selection

    The StringFlav class handles the choice of a new flavour in the fragmentation process, and the production of a new hadron from a set of input flavours. It is mainly used by the string fragmentation machinery (including ministrings), but also e.g. in some particle decays and for some beam-remnant cases. The basic concepts are in agreement with And83. The baryon-sector implementation is based on the MSTJ(12)=3 option of PYTHIA 6, i.e. new SU(6) weights scheme with at most one popcorn meson.

    The relative production rates of different particle species is influenced by the parameters below. Some have only an impact on one specific quantity, but most directly or indirectly have consequences for many observables. Therefore the values to use have to be viewed in the context of a complete tune.

    New flavours

    The main parameters of the selection of a new flavour are the suppression of s quark production relative to ordinary u or d one. the suppression of diquark production relative to quark production, i.e. of baryon relative to meson production. the suppression of strange diquark production relative to light diquark production, over and above the one already given by probStoU. the suppression of spin 1 diquark production relative to spin 0 one, apart from the factor of 3 enhancement of spin 1 from counting the number of states.

    Standard-meson production

    The bulk of the particle production corresponds to the lowest-lying pseudoscalar and vector multiplets. Their production rates are determined by the parameters in this section.

    For a given set of flavours, produced according to the probabilities outlined above, the ratio of vector-to-pseudocalar meson production is described by the parameters below. The maximum allowed rate for each case has been set according to spin-counting rules, but we expect the real rates to be lower, especially for lighter mesons, owing to the vector-pseudoscalar mass splitting. the relative production ratio vector/pseudoscalar for light (u, d) mesons. the relative production ratio vector/pseudoscalar for strange mesons. the relative production ratio vector/pseudoscalar for charm mesons. the relative production ratio vector/pseudoscalar for bottom mesons.

    Inside each light-quark meson nonet, an octet-singlet mixing angle describes the mixing of the two flavour-diagonal isoscalar = 0 states. (For terminology and details see Yao06, chapter 14 on the quark model.) This angle is needed to specify the probability for such a q qbar state to project onto a specific meson. More transparent formulae are obtained by introducing the angle alpha = theta + 54.7 degrees: f = (uubar + ddbar)/sqrt(2) * sin(alpha) + ssbar * cos(alpha)
    f' = (uubar + ddbar)/sqrt(2) * cos(alpha) - ssbar * sin(alpha)
    gives the mixing angle theta_PS in the pseudoscalar meson sector (which is rather poorly determined), expressed in degrees. Here f is associated with eta' and f' with eta. (This standard but counterintuitive choice is fixed up in the code by replacing alpha -> 90^0 - alpha so that eta <-> eta'; relative signs do not matter since we are interested in probabilities only.) gives the mixing angle theta_V in the vector meson sector (which is somewhat better determined), expressed in degrees. Here f is associated with omega and f' with phi.

    Further, the simple model overestimates the production of eta and, in particular, eta' mesons, which can be rectified by the additional suppression of eta production, multiplying the normal production probability. Thus 0 means no eta at all are produced, while 1 means full rate. the additional suppression of eta' production, multiplying the normal production probability. Thus 0 means no eta' at all are produced, while 1 means full rate.

    Excited-meson production

    Several excited mesons, ie. with radial or orbital excitations, have been observed at non-negligible production rates. Extrapolated to all states a fair fraction of all particle production might proceed through such states. There are big uncertainties, however, since these excited mesons in many cases are extremely poorly known. This also means that the modeling of their production and decay is very primitive, and even that the inclusion of the production of such states may lead to a degraded agreement with data. Currently the default is that all such production is switched off.

    Parameters are provided to switch them on. By demand, this machinery has been made more flexible than in the past. Therefore one parameter is provided for each combination of heaviest flavour (u/d, s, c or b) and multiplet produced. In each case the production rate is normalized to that of the lowest-lying pseudoscalar of the same flavour content, as for the vector-meson rates introduced above. The multiplets available are the four obtained for one unit of orbital angular momentum, in the nonrelativistic classification. Using J to denote the sum of quark spin S and orbital angular momentum L, i.e. what would normally be called the spin of the meson, one has:

    • a pseudovector multiplet with L=1, S=0, J=1;
    • a scalar multiplet with L=1, S=1, J=0;
    • a pseudovector multiplet with L=1, S=1, J=1;
    • a tensor multiplet with L=1, S=1, J=2.
    The maximum allowed rate for each case has been set according to spin-counting rules, but we expect the real rates to be significantly lower, owing to mass suppression. the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for light (u, d) mesons. the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for light (u, d) mesons. the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for light (u, d) mesons. the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for light (u, d) mesons. the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for strange mesons. the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for strange mesons. the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for strange mesons. the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for strange mesons. the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for charm mesons. the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for charm mesons. the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for charm mesons. the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for charm mesons. the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for bottom mesons. the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for bottom mesons. the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for bottom mesons. the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for bottom mesons.

    In addition, an octet-singlet mixing angle is needed for each multiplet, as for the pseudoscalar and vector multiplets above. Only for the tensor multiplet does any determination exist; for the other multiplets default has been chose so that ssbar does not mix with the light quarks, and so that the ssbar state is the heavier of the two. gives the mixing angle theta in the (L=1,S=0,J=1) pseudovector meson sector, expressed in degrees. gives the mixing angle theta in the (L=1,S=1,J=0) scalar meson sector, expressed in degrees. gives the mixing angle theta in the (L=1,S=1,J=1) pseudovector meson sector, expressed in degrees. gives the mixing angle theta in the (L=1,S=1,J=2) tensor meson sector, expressed in degrees.

    Baryon production

    The relative rate of baryon production is mainly given by the quark and diquark production parameters above, plus SU(6) Clebsch-Gordans. The one modifiable parameter related to these coefficients is the suppression, relative to default SU(6) factors, of decuplet baryon production. Default corresponds to no suppression, while 0 corresponds to no decuplet production at all.

    In addition, if popcorn production is allowed, wherein a set of mesons (M) may be produced in between the baryon (B) and the antibaryon (Bbar), a set of further parameters is introduced. Currently only the simplest scenario is implemented, wherein at most one intermediate meson may be produced. gives the relative rates of B Bbar and B M Bbar production, roughly as Prob(B M Bbar) / (Prob(B Bbar) + Prob(B M Bbar)) = popcornRate / (0.5 + popcornRate) (the complete expression depends on all the quark and diquark production parameters and is therefore not so useful). extra suppression for having an s sbar pair shared between the B and Bbar in a B M Bbar configuration. extra suppression for having a strange meson M in a B M Bbar configuration.

    Finally, there are some indications that leading-baryon production may be further suppressed. A proper description should probably be based on a suppression of early production times Ede97, but we here only implement a simpler version where production near the end of a string, as defined by rank, is suppressed. The more detailed studies suggest that leading c and b baryon production will be less suppressed, so we leave it open to set light- and heavy-baryon suppression separately. Suppress leading-baryon production. extra suppression of leading-baryon production for a light-quark jet, i.e. d, u or s, when suppressLeadingB = on. Thus 0 means no leading-baryon production at all, while 1 means full rate. extra suppression of leading-baryon production for a heavy-quark jet, i.e. c or b, when suppressLeadingB = on. Thus 0 means no leading-baryon production at all, while 1 means full rate. pythia8-8.1.80.orig/xmldoc/pomH1JetsCharm.data0000444000175000017500000034714412217346316017257 0ustar sunsun-6.907755E+00-6.837980E+00-6.768205E+00-6.698429E+00-6.628654E+00-6.558879E+00 -6.489103E+00-6.419328E+00-6.349553E+00-6.279778E+00-6.210002E+00-6.140227E+00 -6.070452E+00-6.000676E+00-5.930901E+00-5.861126E+00-5.791350E+00-5.721575E+00 -5.651800E+00-5.582024E+00-5.512249E+00-5.442474E+00-5.372699E+00-5.302923E+00 -5.233148E+00-5.163373E+00-5.093597E+00-5.023822E+00-4.954047E+00-4.884271E+00 -4.814496E+00-4.744721E+00-4.674945E+00-4.605170E+00-4.535395E+00-4.465620E+00 -4.395844E+00-4.326069E+00-4.256294E+00-4.186518E+00-4.116743E+00-4.046968E+00 -3.977192E+00-3.907417E+00-3.837642E+00-3.767867E+00-3.698091E+00-3.628316E+00 -3.558541E+00-3.488765E+00-3.418990E+00-3.349215E+00-3.279439E+00-3.209664E+00 -3.139889E+00-3.070113E+00-3.000338E+00-2.930563E+00-2.860788E+00-2.791012E+00 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3.20000E+01 3.30000E+01 3.40000E+01 3.50000E+01 3.60000E+01 3.70000E+01 3.80000E+01 3.90000E+01 4.00000E+01 4.10000E+01 4.20000E+01 4.30000E+01 4.40000E+01 4.50000E+01 4.60000E+01 4.70000E+01 4.80000E+01 4.90000E+01 5.00000E+01 5.50000E+01 6.00000E+01 6.50000E+01 7.00000E+01 7.50000E+01 8.00000E+01 8.50000E+01 9.00000E+01 9.50000E+01 1.00000E+02 1.50000E+02 2.00000E+02 2.50000E+02 3.00000E+02 3.50000E+02 4.00000E+02 4.50000E+02 5.00000E+02 5.50000E+02 6.00000E+02 6.50000E+02 7.00000E+02 7.50000E+02 8.00000E+02 8.50000E+02 9.00000E+02 9.50000E+02 1.00000E+03 1.50000E+03 2.00000E+03 5.062582E-03 5.005623E-03 4.949315E-03 4.893533E-03 4.838280E-03 4.783619E-03 4.729459E-03 4.675563E-03 4.622113E-03 4.569084E-03 4.516439E-03 4.464239E-03 4.412994E-03 4.362850E-03 4.313742E-03 4.264649E-03 4.215443E-03 4.166185E-03 4.116884E-03 4.067468E-03 4.017656E-03 3.967730E-03 3.917819E-03 3.867592E-03 3.817324E-03 3.766709E-03 3.715875E-03 3.664476E-03 3.612878E-03 3.560694E-03 3.507438E-03 3.453261E-03 3.398207E-03 3.341806E-03 3.284160E-03 3.225704E-03 3.165521E-03 3.103743E-03 3.040676E-03 2.975686E-03 2.908873E-03 2.840012E-03 2.768637E-03 2.695201E-03 2.619938E-03 2.541750E-03 2.461780E-03 2.379242E-03 2.293936E-03 2.206042E-03 2.115887E-03 2.022565E-03 1.926535E-03 1.828667E-03 1.728318E-03 1.625842E-03 1.521745E-03 1.415742E-03 1.308600E-03 1.200689E-03 1.092031E-03 9.842690E-04 8.770966E-04 7.717425E-04 6.688289E-04 5.695036E-04 4.748561E-04 3.857490E-04 3.035092E-04 2.293066E-04 1.641917E-04 1.093240E-04 6.549575E-05 3.322056E-05 1.251652E-05 2.372415E-06 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 1.000000E-30 0.000000E+00 5.166661E-03 5.108391E-03 5.050847E-03 4.993855E-03 4.937402E-03 4.881562E-03 4.826183E-03 4.771198E-03 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8.193593E-03 7.314167E-03 6.484614E-03 5.708682E-03 4.981261E-03 4.304955E-03 3.684346E-03 3.113867E-03 2.597780E-03 2.134745E-03 1.725827E-03 1.367981E-03 1.060476E-03 8.018020E-04 5.885502E-04 4.162418E-04 2.809259E-04 1.765863E-04 9.825897E-05 4.173054E-05 7.873855E-06 0.000000E+00 2.034582E-01 1.997200E-01 1.960142E-01 1.923334E-01 1.886866E-01 1.850747E-01 1.814937E-01 1.779395E-01 1.744109E-01 1.709091E-01 1.674367E-01 1.639910E-01 1.605706E-01 1.571839E-01 1.538299E-01 1.505004E-01 1.472004E-01 1.439312E-01 1.406928E-01 1.374852E-01 1.343091E-01 1.311616E-01 1.280432E-01 1.249488E-01 1.218838E-01 1.188490E-01 1.158438E-01 1.128713E-01 1.099322E-01 1.070214E-01 1.041383E-01 1.012868E-01 9.846547E-02 9.566820E-02 9.290148E-02 9.016985E-02 8.746921E-02 8.480292E-02 8.216423E-02 7.955900E-02 7.698643E-02 7.445058E-02 7.194991E-02 6.947844E-02 6.704048E-02 6.463784E-02 6.227059E-02 5.993364E-02 5.763306E-02 5.537159E-02 5.314655E-02 5.095630E-02 4.880629E-02 4.668738E-02 4.460157E-02 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1.048332E-01 1.018026E-01 9.880851E-02 9.585409E-02 9.293311E-02 9.004917E-02 8.719371E-02 8.437437E-02 8.158952E-02 7.884328E-02 7.613581E-02 7.345963E-02 7.082035E-02 6.822160E-02 6.566118E-02 6.313275E-02 6.064224E-02 5.819278E-02 5.577944E-02 5.340356E-02 5.107497E-02 4.878645E-02 4.654073E-02 4.433586E-02 4.217395E-02 4.006012E-02 3.799058E-02 3.596758E-02 3.399047E-02 3.205515E-02 3.016483E-02 2.832153E-02 2.652890E-02 2.478285E-02 2.308823E-02 2.145147E-02 1.986241E-02 1.832912E-02 1.684969E-02 1.542524E-02 1.405811E-02 1.274709E-02 1.149422E-02 1.030371E-02 9.177679E-03 8.111670E-03 7.108955E-03 6.171206E-03 5.301975E-03 4.498640E-03 3.766178E-03 3.098644E-03 2.504641E-03 1.978282E-03 1.521513E-03 1.134841E-03 8.135911E-04 5.570422E-04 3.607560E-04 2.201465E-04 1.277803E-04 7.534864E-05 5.205349E-05 4.487114E-05 4.090512E-05 2.847866E-05 7.228384E-06 0.000000E+00 pythia8-8.1.80.orig/xmldoc/ProgramClasses.xml0000444000175000017500000001376012217346316017300 0ustar sunsun

    Program Classes

    The complete PYTHIA 8 package contains a multitude of classes. There is no reason to describe all of them, with all of their methods, since most should not be touched by a normal user. Nevertheless some of the crucial ones are described in detail, as a help not only to advanced users but also to developers. We here provide a quick reference (still incomplete) which classes you can find described where on these pages. Normally you have to scroll down to find the details, since the top of the page contains information of more general interest.

    Class Reference Comment
    BeamShape Beam Shape vertex and beam momentum spread
    CellJet Event Analysis jet cone clustering analysis, intended for hadron collider topologies
    ClusterJet Event Analysis jet clustering analysis, intended for e^+e^- collider topologies
    CoupSM Standard Model Parameters couplings and mixing matrices
    CoupSUSY SUSY Les Houches Accord compute and store SUSY couplings, using input from SusyLesHouches
    DecayChannel Particle Data Scheme the properties of a single decay channel of particle species
    Event Event Record the complete event record
    HepMC::Pythia8ToHepMC HepMC Interface convert a PYTHIA event record to the HepMC format
    Hist Histograms a primitive built-in histogramming package
    Info Event Information various one-of-a-kind information on the current event
    LHAPDFInterface Parton Distributions use PDF sets from the LHAPDF library
    LHAup Les Houches Accord base class for Les Houches external hard-event input
    Particle Particle Properties the properties of a particle in the event record
    ParticleData Particle Data Scheme the database of particle species properties
    ParticleDataEntry Particle Data Scheme the properties of a particle species
    PDF Parton Distributions base class for all PDFs
    Pythia Program Flow the top-level class, that drives the generation process
    ResonanceWidths Semi-Internal Resonances base class for all resonance-width treatment
    Rndm RandomNumbers a primitive built-in histogramming package
    RotBstMatrix Four-Vectors rotation and boosts of four-vectors
    Settings Settings Scheme the database that regulates the behaviour of the program
    SigmaProcess Semi-Internal Processes base class for all hard-process cross sections
    SlowJet Event Analysis simple jet clustering using the kT, anti-kT or Cambridge/Aachen algorithms.
    SpaceShower Implement New Showers spacelike, i..e. initial-state showers
    Sphericity Event Analysis sphericity analysis of events
    SusyLesHouches SUSY Les Houches Accord reading in of SLHA information
    Thrust Event Analysis thrust analysis of events
    TimeShower Implement New Showers timelike, i..e. final-state showers
    UserHooks User Hooks get access to some steps of the generation process
    Vec4 Four-Vectors four-vectors

    You can also access an extensive list of the public methods in these classes, which compensates for the brevity of the current page. pythia8-8.1.80.orig/xmldoc/mrstlostar.00.dat0000444000175000017500000120437112217346304016751 0ustar sunsun # Fri Oct 16 11:59:45 2009 # MSTW 2008 LO PDF grid for central fit. # distance(t),tolerance(T) = 0. 0. # mCharm = 1.43 # mBottom = 4.30 # alphaS(1GeV) = 0.49337 # alphaS(MZ) = 0.12032 # alphaSorder,alphaSnfmax = 0, 5 # nExtraFlavours = 0 xg xd xu xs xc xb xdv xuv xsv 8.0090E+00 1.3182E+00 1.3280E+00 6.5619E-01 0.0000E+00 0.0000E+00 5.8017E-03 1.5621E-02 0.0000E+00 1.3658E+01 1.3573E+00 1.3671E+00 7.0073E-01 0.0000E+00 0.0000E+00 5.8891E-03 1.5771E-02 0.0000E+00 1.9234E+01 1.4059E+00 1.4159E+00 7.5351E-01 0.0000E+00 0.0000E+00 5.9561E-03 1.5886E-02 0.0000E+00 3.0629E+01 1.5247E+00 1.5347E+00 8.7863E-01 0.0000E+00 0.0000E+00 6.0622E-03 1.6067E-02 0.0000E+00 3.0629E+01 1.5247E+00 1.5347E+00 8.7863E-01 2.9834E-07 0.0000E+00 6.0622E-03 1.6067E-02 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8.4857E-07 2.5465E-09 3.0727E-07 0.0000E+00 9.8533E-14 8.7957E-07 1.1591E-06 8.7724E-07 8.7543E-07 8.5477E-07 2.3294E-09 2.8184E-07 0.0000E+00 9.8533E-14 8.7694E-07 1.1331E-06 8.7481E-07 8.7311E-07 8.5366E-07 2.1288E-09 2.5828E-07 0.0000E+00 9.8533E-14 8.8104E-07 1.1160E-06 8.7909E-07 8.7749E-07 8.5919E-07 1.9475E-09 2.3691E-07 0.0000E+00 9.8533E-14 8.8404E-07 1.1004E-06 8.8225E-07 8.8074E-07 8.6349E-07 1.7887E-09 2.1815E-07 0.0000E+00 9.8533E-14 8.8066E-07 1.0807E-06 8.7900E-07 8.7757E-07 8.6126E-07 1.6499E-09 2.0171E-07 0.0000E+00 9.8533E-14 8.8354E-07 1.0683E-06 8.8202E-07 8.8067E-07 8.6527E-07 1.5204E-09 1.8632E-07 0.0000E+00 pythia8-8.1.80.orig/xmldoc/RIVETusage.xml0000444000175000017500000000537112217346317016271 0ustar sunsun

    RIVET usage

    RIVET is a toolkit for the validation of Monte Carlo event generators Buc10. It contains the results of many experimental analyses, so that generator output can easily be compared to data, as well as providing a framework to implement your own analyses. Although using PYTHIA with RIVET is not officially supported, some helpful hints are given below. The full RIVET manual is available online.

    Using PYTHIA with RIVET

    The following assumes that you already have RIVET installed. Instructions for this may be found here.

    Events are passed from PYTHIA to RIVET using the HepMC format. PYTHIA must be compiled with HepMC support, using the same version of HepMC used when compiling RIVET. This is setup through the PYTHIA configure script e.g.
      ./configure --with-hepmc=/path/to/HepMC --with-hepmcversion=HepMC.version.number
    
    The PYTHIA library itself does not need to be recompiled.

    The examples/main42.cc sample program can then be used to generate events in HepMC format (which examples/main61.cc and examples/main62.cc extends by allowing LHAPDF usage and subruns). When in the examples directory, the main program can be built and used as follows
      make main42
      ./main42 main42.cmnd main42.hepmc
    
    The first argument is the input file which provides the options for event generation, while the second is the output file where the HepMC events should be written.

    This HepMC file may now be read and processed by RIVET
      rivet --analysis=ANALYSIS_NAME main42.hepmc
    
    where ANALYSIS_NAME is a built-in RIVET analysis, or one you have created yourself. The output of RIVET is in the form of .aida files, containing the histograms for the analysis, which can be processed further with RIVET (see the RIVET documentation for more details).

    The above examples requires that (potentially large) HepMC events are stored to disk before being read by RIVET. It is possible, instead, to pass the events directly to RIVET as they are produced by using a FIFO pipe. This is done with the mkfifo command
      mkfifo my_fifo
      ./main42.exe main42.cmnd my_fifo &
      rivet --analysis=ANALYSIS_NAME my_fifo
    
    Note that main42 is run in the background.
    pythia8-8.1.80.orig/xmldoc/pipi-Froggatt.dat0000444000175000017500000001350712217346315017035 0ustar sunsun# Pion-pion partial-wave data, analysis of Froggatt and Petersen # Nucl. Phys. B129 (1977) 89-110 # Notation for column headers is L,2I set eType Wcm set eUnit GeV set input eta,delta set dUnit deg set norm 1 # Elastic region Wcm 0,0 0,4 1,2 2,0 2,4 3,2 0.30 1.00 7.1 1.00 -0.6 1.00 0.1 1.00 0.0 1.00 0.0 1.00 0.0 0.32 1.00 10.7 1.00 -1.2 1.00 0.4 1.00 0.0 1.00 0.0 1.00 0.0 0.34 1.00 14.0 1.00 -1.8 1.00 0.7 1.00 0.0 1.00 0.0 1.00 0.0 0.36 1.00 17.1 1.00 -2.4 1.00 1.0 1.00 0.0 1.00 0.0 1.00 0.0 0.38 1.00 20.2 1.00 -3.1 1.00 1.5 1.00 0.0 1.00 0.0 1.00 0.0 0.40 1.00 23.3 1.00 -3.7 1.00 2.0 1.00 0.0 1.00 0.0 1.00 0.0 0.42 1.00 26.4 1.00 -4.3 1.00 2.5 1.00 0.0 1.00 0.0 1.00 0.0 0.44 1.00 29.6 1.00 -5.0 1.00 3.2 1.00 0.0 1.00 0.0 1.00 0.0 0.46 1.00 32.7 1.00 -5.6 1.00 4.0 1.00 0.0 1.00 0.0 1.00 0.0 0.48 1.00 35.8 1.00 -6.2 1.00 4.9 1.00 0.0 1.00 0.0 1.00 0.0 0.50 1.00 39.0 1.00 -6.8 1.00 5.9 1.00 0.0 1.00 0.0 1.00 0.0 0.52 1.00 42.1 1.00 -7.4 1.00 7.1 1.00 0.0 1.00 0.0 1.00 0.0 0.54 1.00 45.1 1.00 -8.0 1.00 8.5 1.00 0.0 1.00 0.0 1.00 0.0 0.56 1.00 48.2 1.00 -8.6 1.00 10.1 1.00 0.0 1.00 0.0 1.00 0.0 0.58 1.00 51.2 1.00 -9.1 1.00 12.1 1.00 0.0 1.00 0.0 1.00 0.0 0.60 1.00 54.1 1.00 -9.6 1.00 14.4 1.00 0.0 1.00 0.0 1.00 0.0 0.62 1.00 57.0 1.00 -10.1 1.00 17.3 1.00 0.0 1.00 0.0 1.00 0.0 0.64 1.00 59.9 1.00 -10.6 1.00 20.9 1.00 0.0 1.00 0.0 1.00 0.0 0.66 1.00 62.7 1.00 -11.1 1.00 25.4 1.00 0.0 1.00 0.0 1.00 0.0 0.68 1.00 65.5 1.00 -11.5 1.00 31.2 1.00 0.0 1.00 0.0 1.00 0.0 0.70 1.00 68.3 1.00 -12.0 1.00 38.7 1.00 0.0 1.00 0.0 1.00 0.0 0.72 1.00 71.1 1.00 -12.4 1.00 48.4 1.00 0.0 1.00 0.0 1.00 0.0 0.74 1.00 73.9 1.00 -12.8 1.00 60.6 1.00 0.0 1.00 0.0 1.00 0.0 0.76 1.00 76.7 1.00 -13.2 1.00 74.9 1.00 0.0 1.00 0.0 1.00 0.0 0.78 1.00 79.6 1.00 -13.6 1.00 90.0 1.00 0.0 1.00 0.0 1.00 0.0 0.80 1.00 82.5 1.00 -13.9 1.00 103.8 1.00 0.0 1.00 0.0 1.00 0.0 0.82 1.00 85.6 1.00 -14.3 1.00 115.3 1.00 0.0 1.00 0.0 1.00 0.0 0.84 1.00 88.8 1.00 -14.6 1.00 124.3 1.00 0.0 1.00 0.0 1.00 0.0 0.86 1.00 92.4 1.00 -14.9 1.00 131.3 1.00 0.0 1.00 0.0 1.00 0.0 0.88 1.00 96.3 1.00 -15.2 1.00 136.7 1.00 0.0 1.00 0.0 1.00 0.0 0.90 1.00 100.8 1.00 -15.5 1.00 141.0 1.00 0.0 1.00 0.0 1.00 0.0 0.92 1.00 106.3 1.00 -15.8 1.00 144.5 1.00 0.0 1.00 0.0 1.00 0.0 0.94 1.00 113.6 1.00 -16.1 1.00 147.3 1.00 0.0 1.00 0.0 1.00 0.0 0.96 1.00 124,5 1.00 -16.4 1.00 149.7 1.00 0.0 1.00 0.0 1.00 0.0 0.98 1.00 146.9 1.00 -16.6 1.00 151.8 1.00 0.0 1.00 0.0 1.00 0.0 # Inelastic region 1.01 0.24 35.9 1.00 -17.4 0.90 156.4 0.88 15.1 1.00 -1.7 1.00 0.1 1.03 0.20 45.3 1.00 -17.6 0.85 158.2 0.85 16.9 1.00 -1.8 1.00 0.1 1.05 0.27 59.9 1.00 -17.8 0.90 159.8 0.94 17.5 1.00 -1.9 1.00 0.2 1.07 0.57 80.0 1.00 -18.0 0.85 160.6 0.88 18.4 1.00 -1.9 0.99 0.3 1.09 0.53 68.2 1.00 -18.3 0.88 163.0 0.93 22.1 1.00 -2.0 0.99 0.4 1.11 0.65 72.1 0.99 -18.5 0.88 164.4 0.93 26.4 1.00 -2.1 0.99 0.4 1.13 0.65 74.2 0.99 -18.7 0.85 167.1 0.91 29.7 1.00 -2.2 0.98 0.3 1.15 0.59 80.0 0.98 -19.0 0.83 168.5 0.88 31.7 1.00 -2.3 0.98 0.5 1.17 0.61 79.9 0.98 -19.2 0.84 169.4 0.87 38.7 1.00 -2.4 0.97 0.2 1.19 0.60 84.6 0.97 -19.5 0.83 169.0 0.82 43.5 1.00 -2.5 0.98 0.5 1.21 0.58 83.3 0.97 -19.8 0.81 169.3 0.80 53.6 1.00 -2.6 0.97 0.1 1.23 0.60 86.7 0.96 -20.0 0.84 168.8 0.74 62.3 0.99 -2.7 0.98 0.4 1.25 0.69 88.9 0.95 -20.3 0.85 168.9 0.74 75.0 0.99 -2.8 0.98 0.4 1.27 0.68 92.5 0.95 -20.6 0.89 170.7 0.70 87.7 0.99 -2.8 0.99 0.3 1.29 0.82 99.7 0.94 -20.9 0.90 171.1 0.59 101.2 0.99 -2.9 1.00 0.6 1.31 0.78 104.2 0.93 -21.1 0.81 174.5 0.72 112.8 0.99 -3.0 1.01 0.4 1.33 0.71 109.0 0.92 -21.4 0.74 176.7 0.75 122.2 0.99 -3.1 1.02 0.4 1.35 0.73 113.2 0.91 -21.7 0.69 0.6 0.71 132.7 0.98 -3.2 1.04 0.4 1.37 0.62 121.7 0.90 -22.0 0.69 3.1 0.77 137.6 0.98 -3.3 1.05 1.0 1.39 0.57 126.2 0.89 -22.3 0.65 4.9 0.80 143.1 0.98 -3.4 1.04 1.2 1.41 0.53 133.1 0.88 -22.6 0.60 5.6 0.81 147.1 0.98 -3.5 1.04 1.6 1.43 0.51 137.8 0.87 -22.9 0.53 5.8 0.82 150.3 0.98 -3.5 1.04 2.4 1.45 0.48 145.1 0.86 -23.3 0.49 5.7 0.81 153.8 0.97 -3.6 1.03 2.7 1.47 0.51 154.6 0.85 -23.6 0.48 5.0 0.82 157.7 0.97 -3.7 1.04 3.6 1.49 0.54 160.4 0.84 -23.9 0.44 4.2 0.82 159.8 0.97 -3.8 1.03 4.4 1.51 0.59 166.1 0.83 -24.2 0.41 3.1 0.82 161.7 0.97 -3.9 1.02 5.4 1.53 0.61 170.2 0.82 -24.5 0.37 0.6 0.80 163.6 0.96 -3.9 1.00 6.2 1.55 0.63 174.4 0.81 -24.9 0.33 177.7 0.77 165.2 0.96 -4.0 0.97 7.2 1.57 0.67 177.0 0.79 -25.2 0.27 176.9 0.69 167.6 0.96 -4.1 0.91 7.5 1.59 0.77 3.0 0.78 -25.5 0.29 169.3 0.79 168.4 0.96 -4.2 0.93 9.6 1.61 0.80 7.5 0.77 -25.8 0.30 162.9 0.77 169.9 0.95 -4.3 0.89 10.6 1.63 0.85 12.1 0.76 -26.2 0.33 157.7 0.76 171.8 0.95 -4.3 0.83 11.9 1.65 0.88 17.1 0.75 -26.5 0.40 154.2 0.77 173.2 0.95 -4.4 0.76 12.8 1.67 0.87 21.8 0.74 -26.9 0.49 153.2 0.74 175.4 0.95 -4.5 0.69 12.5 1.69 0.83 26.4 0.73 -27.2 0.59 154.3 0.75 177.3 0.94 -4.6 0.62 11.1 1.71 0.72 31.4 0.71 -27.6 0.68 155.9 0.61 178.6 0.94 -4.6 0.56 8.4 1.73 0.59 35.3 0.70 -27.9 0.75 158.4 0.59 179.0 0.94 -4.7 0.54 4.6 1.75 0.43 35.5 0.69 -28.3 0.80 161.5 0.55 179.2 0.93 -4.8 0.56 1.2 1.77 0.30 30.7 0.68 -28.6 0.82 164.2 0.51 178.3 0.93 -4.8 0.60 -0.8 1.79 0.21 21.6 0.67 -29.0 0.84 166.8 0.52 179.2 0.93 -4.9 0.65 -1.9 pythia8-8.1.80.orig/xmldoc/ParticleData.xml0000444000175000017500000224515612217346314016716 0ustar sunsun

    Particle Data

    The structure and operation of the particle data table is described here. That page also describes how default data properties can be changed. The current page provides the actual default values.

    Main settings

    Apart from the data itself, the particle data table only contains a few aspects that are available to change: Selection of particle masses when the mSel(id) is called to provide a new mass: Note: this mode only applies to normal hadronic resonances like the rho. The more massive states of the isResonance() type, like Z^0 or top, are considered separately. The modifications in options 2 and 4 above enhance the large-mass tail of the Breit-Wigner distributions (the mass spectrum develops a dm/m divergence). However, we expect form factors to dampen this tail at masses some distance above the nominal one, so cut off the rise by requiring the actual Breit-Wigner weight not to be more than a factor maxEnhanceBW above the one obtained with options 1 or 3, respectively. This also opens up for a simpler technical handling of mass selection in options 2 and 4, by using standard hit-and-miss Monte Carlo.

    Since running masses are only calculated for the six quark flavours, e.g. to obtain couplings to the Higgs boson(s), there is not an entry in the normal tables for each particles, but only the six MSbar mass values below, used as starting point for the running. In addition you can pick an alpha_s(M_Z), which is converted into a first-order five-flavour Lambda that is used to determine the rate of the running. (Without any match to four flavours below m_b; if desired, this can be fixed by slightly shifted default mass values, since the routines never should be called below the m_b scale anyway.) the d quark MSbar mass at 2 GeV scale. the u quark MSbar mass at 2 GeV scale. the s quark MSbar mass at 2 GeV scale. the c quark MSbar mass at the mass scale itself. the b quark MSbar mass at the mass scale itself. the t quark MSbar mass at the mass scale itself. the alpha_s(M_Z) value used to define the rate at which MSbar masses run.

    Comments on the data

    Much of the current data has been updated based on the 2012 Review of Particle Physics Ber12, while some is still based on the 2006 RPP Yao06. All known particle masses, widths and lifetimes have been set accordingly, while most not-yet-measured particles are kept at their values from PYTHIA 6. Decay channels and their branching ratios remain a major worry: many particles do not have one single solidly measured branching ratio, and many further do not have known branching ratios that add up to (the neighbourhood of) unity.

    Uncertainties are especially big for the scalar, pseudovector and tensor L = 1 multiplets available in PYTHIA. We note that some distributions become better described when these multiplets are included in the generation, while others become worse. It is tempting to associate this lackluster performance with the primitive knowledge. Not even the multiplets themselves are particularly well known. It used to be that the a_0(980) and f_0(980) were considered to be members of the scalar multiplet. Nowadays they are commonly assumed to be either four-quark states or of some other exotic character. This means that the PYTHIA 8 PDG particle codes have been changed for these particles, relative to what was used in PYTHIA 6 based on previous PDG editions. Specifically their numbers are now in the 9000000 series, and they have been replaced in the scalar multiplet by a_0(1450) and f_0(1370).

    For charm and bottom mesons the jungle of partial measurements makes it very difficult to construct fully consistent sets of decay channels. This part of the program has not yet been brought up to date to the 2006 RPP. Instead the LHCb decay tables (for EvtGen, but without using the EvtGen matrix-element machinery) and the DELPHI tune for PYTHIA 6 is being used. (This also includes a few non-c/b hadrons that only occur in the c/b decay tables.) This has the advantage that many tests have been made for consistency, but the disadvantage that it is not always in agreement with the latest measurements of some specific decay channels. The decays based on the LHCb tables (with some modifications) are 411, 421, 431, 441, 445, 511, 521, 531, 541, 3124, 4122, 4124, 5122, 10441, 10443, 13122, 14122, 20443, 23122, 30313, 30323, 30443, 33122, 100113, 100213, 100441, 100443, 100553, 9000111, 9000211. Correspondingly the decays based on the DELPHI tables are 415, 425, 435, 515, 525, 535, 4132, 4232, 4332, 5132, 5232 and 5332.

    The data itself

    Here comes the default particle data used in the program. Do not touch. The meaning of the various properties and the format used are explained here and the meMode codes here.
    pythia8-8.1.80.orig/xmldoc/PartonDistributions.xml0000444000175000017500000001426312217346315020377 0ustar sunsun

    Parton Distributions

    The parton distributions file contains the PDF class. PDF is the base class, from which specific PDF classes are derived.

    The choice of which PDF to use is made by settings in the Pythia class, see here. These settings also allow to access all the proton PDF's available in the LHAPDF library Wha05. Thus there is no need for a normal user to study the PDF class. The structure must only be understood when interfacing new PDF's, e.g. ones not yet found in LHAPDF.

    The PDF base class

    PDF defines the interface that all PDF classes should respect. The constructor requires the incoming beam species to be given: even if used for a proton PDF, one needs to know whether the beam is actually an antiproton. This is one of the reasons why Pythia always defines two PDF objects in an event, one for each beam.

    Once a PDF object has been constructed, call it pdf, the main method is pdf.xf( id, x, Q2), which returns x*f_id(x, Q2), properly taking into account whether the beam is an antiparticle or not.

    Whenever the xf member is called with a new flavour, x or Q^2, the xfUpdate member is called to do the actual updating. This routine may either update that particular flavour or all flavours at this (x, Q^2) point. (In the latter case the saved id value idSav should be set to 9.) The choice is to be made by the producer of a given set, based on what he/she deems most effective, given that sometimes only one flavour need be evaluated, and about equally often all flavours are needed at the same x and Q^2. Anyway, the latest value is always kept in memory. This is the other reason why Pythia has one separate PDF object for each beam, so that values at different x can be kept in memory.

    Two further public methods are xfVal( id, x, Q2) and xfSea( id, x, Q2). These are simple variants whereby the quark distributions can be subdivided into a valence and a sea part. If these are not directly accessible in the parametrization, one can make the simplified choices u_sea = ubar_sea, u_val = u_tot - u_sea, and correspondingly for d. (Positivity will always be guaranteed at output.) The xfUpdate method should also take care of updating this information.

    A method setExtrapolate(bool) allows you to switch between freezing parametrizations at the x and Q^2 boundaries (false) or extrapolating them outside the boundaries (true). This method is only implemented for the LHAPDF class below. If you implement a new PDF you are free to use this method, but it would be smarter to hardcode the desired limiting behaviour.

    Derived classes

    There is only one pure virtual method, xfUpdate, that therefore must be implemented in any derived class. A reasonable number of such classes come with the program:

    For protons:

    • LHAPDFinterface provides an interface to the LHAPDF libraryWha05.
    • GRV94L gives the GRV 94 L parametrization Glu95.
    • CTEQ5L gives the CTEQ 5 L parametrization Lai00.
    • MSTWpdf gives the four distributions of the MRST/MSTW group that have been implemented.
    • CTEQ6pdf gives the six distributions of the CTEQ/CT group that have been implemented.
    • NNPDF gives four distributions from the NNPDF 2.3 QCD+QED sets that have been implemented.
    The current default is CTEQ 5L, which has been used in most studies to date.

    For charged pions:

    • GRVpiL gives the GRV 1992 pi+ parametrization.

    For Pomerons (used to describe diffraction):

    • PomFix gives a simple but flexible Q2-independent parametrization.
    • PomH1FitAB gives the H1 2006 Fit A and Fit B parametrizations.
    • PomH1Jets gives the H1 2007 Jets parametrization.

    For charged leptons (e, mu, tau):

    • Lepton gives a QED parametrization Kle89. In QED there are not so many ambiguities, so here one set should be enough. On the other hand, there is the problem that the lepton-inside-lepton pdf is integrably divergent for x -> 1, which gives numerical problems. Like in PYTHIA 6, the pdf is therefore made to vanish for x > 1 - 10^{-10}, and scaled up in the range 1 - 10^{-7} < x < 1 - 10^{-10} in such a way that the total area under the pdf is preserved.
    • LeptonPoint gives the trivial distribution of a pointlike (i.e. unresolved) charged lepton.

    For neutrinos:

    • NeutrinoPoint is the only method, so there is no choice. Analogously to LeptonPoint it gives the distribution of a pointlike (i.e. unresolved) neutrino. A difference, however, is that neutrinos always are lefthanded, so there is no need to average over incoming spin states. Since the PYTHIA formalism assumes unpolarized beams, and thus implicitly includes a 1/2 for incoming fermions, the NeutrinoPoint PDF is normalized to 2 rather than 1 to compensate for this.

    There is another method, isSetup(), that returns the base-class boolean variable isSet. This variable is initially true, but could be set false if the setup procedure of a PDF failed, e.g. if the user has chosen an unknown PDF set.

    The MRST/MSTW, CTEQ/CT, NNPDF and H1 PDF routines are based on the interpolation in (x, Q) grids. The grid files are stored in the xmldoc subdirectory, like settings and particle data. Only PDF sets that will be used are read in during the initialization stage. pythia8-8.1.80.orig/xmldoc/BeamShape.xml0000444000175000017500000000642312217346277016204 0ustar sunsun

    Beam Shape

    The Beam Parameters page explains how you can set a momentum spread of the two incoming beams, and a spread and offset for the location of the interaction vertex. The spread is based on a simple parametrization in terms of independent Gaussians, however, which is likely to be too primitive for realistic applications.

    It is therefore possible to define your own class, derived from the BeamShape base class, and hand it in to Pythia with the pythia.setBeamShapePtr( BeamShape*) method. Below we describe what such a class has to do. An explicit toy example is shown in main23.cc.

    The BeamShape base class has a very simple structure. It only has two main virtual methods. The first, init(), is used for initialization. The second, pick(), selects beam momentum and production vertex in the current event. the constructor and destructor do not need to do anything. the base-class method simply reads in the relevant values stored in the Settings data base, and saves a pointer to the random-number generator. You are free to write your own derived initialization routine, or use the existing one. In the latter case you can then give your own modified interpretation to the beam spread parameters defined there.
    The two flags Beams:allowMomentumSpread and Beams:allowVertexSpread should not be tampered with, however. These are checked elsewhere to determine whether the beam shape should be set or not, whereas the other momentum-spread and vertex-spread parameters are local to this class.
    this method is the key one to supply in the derived class. Here you are free to pick whatever parametrization you desire for beam momenta and vertex position, including correlations between the two. At the end of the day, you should set a few protected double numbers:
    deltaPxA, deltaPyA, deltaPzA for the three-momentum shift of the first incoming beam, relative to the nominal values;
    deltaPxB, deltaPyB, deltaPzB for the three-momentum shift of the second incoming beam, relative to the nominal values;
    vertexX, vertexY, vertexZ, vertexT for the production-vertex position and time.
    As usual, momentum is given in GeV, and space and time in mm, with c = 1.
    read out the three-momentum shifts for beams A and B that were set by pick(). The energy components are put to zero at this stage, since they are most conveniently calculated after the original and the shift three-momenta have been added. read out the production-vertex position and time that were set by pick(). pythia8-8.1.80.orig/xmldoc/NNPDF23_nnlo_as_0119_qed.grid0000444000175000017500000403760012217346313020526 0ustar sunsun 'Version' '5.8.9' 'Description:' 'NNPDF23_nnlo_as_0119_qed.grid' 'NNPDF2.3QED NNLO, arxiv:1308.0598' 'NNLO QCD + LO QED PDF set, alphas(MZ)=0.119' 'NNPDF Collaboration: R.D. Ball, V. Bertone,' 'S. Carrazza, L. Del Debbio, S. Forte,' 'A. Guffanti, N.P. Hartland, J. Rojo' 'This set has 1 member PDF' 'mem=0 --> average on replicas.' 'Evolution: pol. interpolation on the LH grid.' 'Alphas:' 'Variable', 'nnlo', 'EvolCode' 1 , 91.2 , 1.41421356237309515e+00 , 4.75000000000000000e+00 , 1.75000000000000000e+02 'MinMax:' 0 , 1 1.00000000000000006e-09 , 1.00000000000000000e+00 , 2.00000000000000000e+00 , 1.00000000000000000e+08 'QCDparams:' 0 , 1 3.42206534270809215e-01 , 2.38999999999999990e-01 'Parameterlist:' 'list', 0 , 1 0.11899999999999999 'Evolution:' 'nnlo', 2.00000000000000000 , 1 , 5 'NNPDF20intqed' 0 , 1 100 1.00000000000000006e-09 1.45082877849593975e-09 2.10490414451202072e-09 3.05385550883341570e-09 4.43062145758388157e-09 6.42807311728432092e-09 9.32603346883219949e-09 1.35304777457980684e-08 1.96304065004027145e-08 2.84803586843580223e-08 4.13201240011533696e-08 5.99484250318940942e-08 8.69749002617783555e-08 1.26185688306602100e-07 1.83073828029536780e-07 2.65608778294668702e-07 3.85352859371053147e-07 5.59081018251222390e-07 8.11130830789687312e-07 1.17681195243499806e-06 1.70735264747069051e-06 2.47707635599171153e-06 3.59381366380462615e-06 5.21400828799968487e-06 7.56463327554629143e-06 1.09749876549305693e-05 1.59228279334109413e-05 2.31012970008315800e-05 3.35160265093884096e-05 4.86260158006535356e-05 7.05480231071864552e-05 1.02353102189902686e-04 1.48496826225446671e-04 2.15443469003188232e-04 3.12571584968823529e-04 4.53487850812858240e-04 6.57933224657568350e-04 9.54548456661834807e-04 1.38488637139387171e-03 2.00923300256504586e-03 2.91505306282517597e-03 4.22924287438949855e-03 6.13590727341317612e-03 8.90215085445039342e-03 1.29154966501488291e-02 1.87381742286038301e-02 2.71858824273294025e-02 3.94420605943765559e-02 5.72236765935022068e-02 8.16326530612244972e-02 1.00000000000000006e-01 1.18367346938775514e-01 1.36734693877551022e-01 1.55102040816326531e-01 1.73469387755102067e-01 1.91836734693877575e-01 2.10204081632653084e-01 2.28571428571428564e-01 2.46938775510204100e-01 2.65306122448979553e-01 2.83673469387755117e-01 3.02040816326530626e-01 3.20408163265306134e-01 3.38775510204081698e-01 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1.4761612e-03 2.7845438e-03 5.8819263e-05 1.0293347e-02 9.5318072e-03 7.3078892e-02 1.2665174e-01 3.1144749e-01 4.6100330e-03 2.7463369e-03 1.4638371e-03 1.9605747e-04 6.9569840e-03 2.2053970e-04 1.4694643e-03 2.7489550e-03 1.7874272e-05 1.0092780e-02 9.3139422e-03 7.0733927e-02 1.2446155e-01 3.0660905e-01 4.5226581e-03 2.7115172e-03 1.4573029e-03 2.1962756e-04 7.0576416e-03 2.4223452e-04 1.4620579e-03 2.7138218e-03 0.0000000e+00 9.8990123e-03 9.1046342e-03 6.8511481e-02 1.2234501e-01 3.0191793e-01 4.4382220e-03 2.6771273e-03 1.4500623e-03 2.4123057e-04 7.1587304e-03 2.6212559e-04 1.4540377e-03 2.6791698e-03 0.0000000e+00 9.7117299e-03 8.9034167e-03 6.6402991e-02 1.2029838e-01 2.9736719e-01 4.3565889e-03 2.6431935e-03 1.4422097e-03 2.6104117e-04 7.2602542e-03 2.8036414e-04 1.4454929e-03 2.6450154e-03 0.0000000e+00 9.5305901e-03 8.7098065e-03 6.4400628e-02 1.1831796e-01 2.9294982e-01 4.2776193e-03 2.6097378e-03 1.4338264e-03 2.7920875e-04 7.3622176e-03 2.9705559e-04 1.4364317e-03 2.6113270e-03 0.0000000e+00 9.3553154e-03 8.5234202e-03 6.2494966e-02 1.1640115e-01 2.8866123e-01 4.2011610e-03 2.5767225e-03 1.4249306e-03 2.9583625e-04 7.4646245e-03 3.1238898e-04 1.4270330e-03 2.5782168e-03 0.0000000e+00 9.1856761e-03 8.3439058e-03 6.0683739e-02 1.1454430e-01 2.8449426e-01 4.1271847e-03 2.5442698e-03 1.4156975e-03 3.1111678e-04 7.5674795e-03 3.2645248e-04 1.4173079e-03 2.5456442e-03 0.0000000e+00 9.0213840e-03 8.1708811e-03 5.8958854e-02 1.1274475e-01 2.8044401e-01 4.0555424e-03 2.5123339e-03 1.4061332e-03 3.2513078e-04 7.6707868e-03 3.3934553e-04 1.4072996e-03 2.5136178e-03 0.0000000e+00 8.8621932e-03 8.0040063e-03 5.7314763e-02 1.1099985e-01 2.7650542e-01 3.9861251e-03 2.4809215e-03 1.3962860e-03 3.3797984e-04 7.7745509e-03 3.5116158e-04 1.3970562e-03 2.4821313e-03 0.0000000e+00 8.7078847e-03 7.8429780e-03 5.5746354e-02 1.0930710e-01 2.7267373e-01 3.9188465e-03 2.4500327e-03 1.3862015e-03 3.4975997e-04 7.8787761e-03 3.6198682e-04 1.3866223e-03 2.4511933e-03 0.0000000e+00 8.5582424e-03 7.6875006e-03 5.4248917e-02 1.0766415e-01 2.6894444e-01 3.8536015e-03 2.4196722e-03 1.3759214e-03 3.6054878e-04 7.9834674e-03 3.7189762e-04 1.3760297e-03 2.4207989e-03 0.0000000e+00 8.4130593e-03 7.5373046e-03 5.2818104e-02 1.0606878e-01 2.6531334e-01 3.7903131e-03 2.3898439e-03 1.3654829e-03 3.7043006e-04 8.0886293e-03 3.8092347e-04 1.3652576e-03 2.3908907e-03 0.0000000e+00 8.2720883e-03 7.3920771e-03 5.1447577e-02 1.0451887e-01 2.6177636e-01 3.7288445e-03 2.3604810e-03 1.3548600e-03 3.7943082e-04 8.1942665e-03 3.8920832e-04 1.3544360e-03 2.3615707e-03 0.0000000e+00 8.1352606e-03 7.2516870e-03 5.0138078e-02 1.0301259e-01 2.5832983e-01 3.6692186e-03 2.3316908e-03 1.3441880e-03 3.8769438e-04 8.3003838e-03 3.9677330e-04 1.3435455e-03 2.3327816e-03 0.0000000e+00 8.0023519e-03 7.1158624e-03 4.8884010e-02 1.0154801e-01 2.5497012e-01 3.6113148e-03 2.3034199e-03 1.3334433e-03 3.9524285e-04 8.4069861e-03 4.0367214e-04 1.3326021e-03 2.3045171e-03 0.0000000e+00 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9.8481513e-04 8.2135257e-04 4.0998909e-04 7.0431593e-05 4.8993572e-03 7.5278693e-05 4.0924598e-04 8.1795998e-04 0.0000000e+00 3.2027163e-03 1.7508746e-03 2.1806387e-02 6.0707920e-02 1.7647382e-01 9.6895740e-04 8.0688362e-04 4.0558514e-04 7.4916167e-05 4.9503261e-03 7.9331422e-05 4.0469612e-04 8.0357681e-04 0.0000000e+00 3.1249543e-03 1.7038093e-03 2.1044455e-02 5.9478876e-02 1.7315326e-01 9.5355970e-04 7.9275187e-04 4.0109940e-04 7.8950787e-05 5.0015107e-03 8.3013735e-05 4.0015288e-04 7.8959893e-04 0.0000000e+00 3.0502659e-03 1.6587548e-03 2.0325877e-02 5.8294279e-02 1.6994428e-01 9.3867041e-04 7.7901655e-04 3.9662025e-04 8.2615631e-05 5.0529129e-03 8.6340486e-05 3.9559699e-04 7.7598734e-04 0.0000000e+00 2.9784555e-03 1.6155652e-03 1.9646250e-02 5.7151765e-02 1.6684128e-01 9.2423737e-04 7.6563994e-04 3.9212534e-04 8.5930428e-05 5.1045346e-03 8.9343588e-05 3.9103906e-04 7.6273021e-04 0.0000000e+00 2.9093621e-03 1.5741350e-03 1.9002777e-02 5.6049158e-02 1.6383908e-01 9.1023827e-04 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3.1044010e-02 1.0282395e-01 4.4177296e-04 2.8138657e-04 1.3220031e-04 2.6612693e-05 3.9731054e-03 2.7730067e-05 1.3149519e-04 2.7929380e-04 0.0000000e+00 9.5709077e-04 2.5702459e-04 7.7174418e-03 3.0344738e-02 1.0062591e-01 4.3765068e-04 2.7546806e-04 1.3021290e-04 2.7579777e-05 4.0007883e-03 2.8594798e-05 1.2950463e-04 2.7346966e-04 0.0000000e+00 9.3012340e-04 2.4785283e-04 7.4367613e-03 2.9672140e-02 9.8507037e-02 4.3355454e-04 2.6973725e-04 1.2824779e-04 2.8438579e-05 4.0285870e-03 2.9361760e-05 1.2754177e-04 2.6783291e-04 0.0000000e+00 9.0430302e-04 2.3911310e-04 7.1720604e-03 2.9024773e-02 9.6463239e-02 4.2949111e-04 2.6419018e-04 1.2631021e-04 2.9203242e-05 4.0565027e-03 3.0042882e-05 1.2560783e-04 2.6237616e-04 0.0000000e+00 8.7956815e-04 2.3078051e-04 6.9221392e-03 2.8401296e-02 9.4490692e-02 4.2546451e-04 2.5882075e-04 1.2440047e-04 2.9880942e-05 4.0845365e-03 3.0643110e-05 1.2370205e-04 2.5708954e-04 0.0000000e+00 8.5585590e-04 2.2283161e-04 6.6859066e-03 2.7800456e-02 9.2585823e-02 4.2147558e-04 2.5361794e-04 1.2252003e-04 3.0479109e-05 4.1126894e-03 3.1152830e-05 1.2180310e-04 2.5194411e-04 0.0000000e+00 8.3308563e-04 2.1521669e-04 6.4613291e-03 2.7221066e-02 9.0745272e-02 4.1750155e-04 2.4855255e-04 1.2064516e-04 3.0986841e-05 4.1409628e-03 3.1614327e-05 1.1995950e-04 2.4697976e-04 0.0000000e+00 8.1125096e-04 2.0796555e-04 6.2495054e-03 2.6662085e-02 8.8965954e-02 4.1359429e-04 2.4366714e-04 1.1882382e-04 3.1446637e-05 4.1693576e-03 3.2016187e-05 1.1814750e-04 2.4216799e-04 0.0000000e+00 7.9028064e-04 2.0103510e-04 6.0486438e-03 2.6122472e-02 8.7244926e-02 4.0972988e-04 2.3893018e-04 1.1703457e-04 3.1847774e-05 4.1978754e-03 3.2363754e-05 1.1636883e-04 2.3750309e-04 0.0000000e+00 7.7012697e-04 1.9440643e-04 5.8579886e-03 2.5601276e-02 8.5579441e-02 4.0591008e-04 2.3433728e-04 1.1527704e-04 3.2194347e-05 4.2265170e-03 3.2661618e-05 1.1462146e-04 2.3297728e-04 0.0000000e+00 7.5075080e-04 1.8806366e-04 5.6768480e-03 2.5097606e-02 8.3966919e-02 4.0213603e-04 2.2988290e-04 1.1355149e-04 3.2491769e-05 4.2552837e-03 3.2914424e-05 1.1290762e-04 2.2858658e-04 0.0000000e+00 7.3210848e-04 1.8199073e-04 5.5045877e-03 2.4610625e-02 8.2404938e-02 3.9840833e-04 2.2556015e-04 1.1185798e-04 3.2744436e-05 4.2841770e-03 0.0000000e+00 0.0000000e+00 1.4196881e-09 0.0000000e+00 5.5594862e-03 1.7244970e-03 1.2337831e-01 1.3664008e-01 4.1002599e-01 0.0000000e+00 1.4096659e-09 0.0000000e+00 0.0000000e+00 2.9250768e-03 0.0000000e+00 0.0000000e+00 5.1352779e-04 0.0000000e+00 4.8828720e-03 1.4854996e-03 1.0178461e-01 1.2281565e-01 3.7281660e-01 1.7660913e-05 5.0990828e-04 0.0000000e+00 0.0000000e+00 2.9465106e-03 0.0000000e+00 0.0000000e+00 5.2597032e-04 0.0000000e+00 4.3771610e-03 1.3107728e-03 8.7138629e-02 1.1217891e-01 3.4372593e-01 1.2473768e-04 5.2029772e-04 0.0000000e+00 0.0000000e+00 2.9677557e-03 0.0000000e+00 0.0000000e+00 5.2926857e-04 0.0000000e+00 3.9606026e-03 1.1684886e-03 7.5364917e-02 1.0327515e-01 3.1907221e-01 2.0673686e-04 5.2246444e-04 0.0000000e+00 0.0000000e+00 2.9890591e-03 0.0000000e+00 0.0000000e+00 5.2646492e-04 0.0000000e+00 3.6114624e-03 1.0503064e-03 6.5795708e-02 9.5706716e-02 2.9788244e-01 2.6997725e-04 5.1904843e-04 0.0000000e+00 0.0000000e+00 3.0104212e-03 0.0000000e+00 0.0000000e+00 5.1957293e-04 0.0000000e+00 3.3145415e-03 9.5052291e-04 5.7931658e-02 8.9188888e-02 2.7945061e-01 3.1899075e-04 5.1186865e-04 0.0000000e+00 0.0000000e+00 3.0318422e-03 0.0000000e+00 7.7477813e-11 5.1002998e-04 0.0000000e+00 3.0589333e-03 8.6516240e-04 5.1400119e-02 8.3512862e-02 2.6325251e-01 3.5716523e-04 5.0224830e-04 7.7312938e-11 0.0000000e+00 3.0533226e-03 0.0000000e+00 6.3883287e-05 4.9741136e-04 0.0000000e+00 2.8288430e-03 7.8798981e-04 4.5457879e-02 7.8372728e-02 2.4846926e-01 3.8686880e-04 4.8969956e-04 6.3747341e-05 0.0000000e+00 3.0748334e-03 0.0000000e+00 8.0650232e-05 4.8551712e-04 0.0000000e+00 2.6379029e-03 7.2507018e-04 4.0823280e-02 7.4038254e-02 2.3589423e-01 4.0970103e-04 4.7794288e-04 8.0144271e-05 0.0000000e+00 3.0963363e-03 0.0000000e+00 9.3590418e-05 4.7296733e-04 0.0000000e+00 2.4675044e-03 6.6916423e-04 3.6850613e-02 7.0134174e-02 2.2448898e-01 4.2760071e-04 4.6556962e-04 9.2808547e-05 0.0000000e+00 3.1179029e-03 0.0000000e+00 1.0349588e-04 4.5999180e-04 0.0000000e+00 2.3145101e-03 6.1913355e-04 3.3423309e-02 6.6599478e-02 2.1409572e-01 4.4142116e-04 4.5280135e-04 1.0251158e-04 0.0000000e+00 3.1395338e-03 0.0000000e+00 1.1105038e-04 4.4703942e-04 0.0000000e+00 2.1766573e-03 5.7432591e-04 3.0449017e-02 6.3384423e-02 2.0458424e-01 4.5212478e-04 4.4006572e-04 1.0991874e-04 0.0000000e+00 3.1612293e-03 0.0000000e+00 1.1669039e-04 4.3411124e-04 0.0000000e+00 2.0517479e-03 5.3388721e-04 2.7852871e-02 6.0447533e-02 1.9584567e-01 4.6013383e-04 4.2735296e-04 1.1545054e-04 0.0000000e+00 3.1829899e-03 0.0000000e+00 1.2086644e-04 4.2146874e-04 0.0000000e+00 1.9382543e-03 4.9737541e-04 2.5575766e-02 5.7754478e-02 1.8778878e-01 4.6607392e-04 4.1493004e-04 1.1954994e-04 0.0000000e+00 3.2048159e-03 0.0000000e+00 1.2381379e-04 4.0906549e-04 0.0000000e+00 1.8346305e-03 4.6419014e-04 2.3567724e-02 5.5276134e-02 1.8033601e-01 4.7020299e-04 4.0274439e-04 1.2244295e-04 0.0000000e+00 3.2267080e-03 0.0000000e+00 1.2583666e-04 3.9707016e-04 0.0000000e+00 1.7398013e-03 4.3402803e-04 2.1789904e-02 5.2988042e-02 1.7342148e-01 4.7294372e-04 3.9095964e-04 1.2443062e-04 0.0000000e+00 3.2486667e-03 0.0000000e+00 1.2705683e-04 3.8541061e-04 0.0000000e+00 1.6526606e-03 4.0644871e-04 2.0208000e-02 5.0869162e-02 1.6698844e-01 4.7444728e-04 3.7950607e-04 1.2563079e-04 0.0000000e+00 3.2706922e-03 0.0000000e+00 1.2768760e-04 3.7419479e-04 0.0000000e+00 1.5724303e-03 3.8123401e-04 1.8795828e-02 4.8901590e-02 1.6098807e-01 4.7500605e-04 3.6848946e-04 1.2625543e-04 0.0000000e+00 3.2927853e-03 0.0000000e+00 1.2782321e-04 3.6338765e-04 0.0000000e+00 1.4983317e-03 3.5809734e-04 1.7529946e-02 4.7069773e-02 1.5537790e-01 4.7474987e-04 3.5787539e-04 1.2638655e-04 0.0000000e+00 3.3149460e-03 0.0000000e+00 1.2752709e-04 3.5295904e-04 0.0000000e+00 1.4296891e-03 3.3677455e-04 1.6390275e-02 4.5360217e-02 1.5012087e-01 4.7377488e-04 3.4762860e-04 1.2609660e-04 0.0000000e+00 3.3371752e-03 0.0000000e+00 1.2693616e-04 3.4296494e-04 0.0000000e+00 1.3660119e-03 3.1714363e-04 1.5362077e-02 4.3761245e-02 1.4518462e-01 4.7227091e-04 3.3781520e-04 1.2551581e-04 0.0000000e+00 3.3594734e-03 0.0000000e+00 1.2608778e-04 3.3337164e-04 0.0000000e+00 1.3067860e-03 2.9901254e-04 1.4430928e-02 4.2262550e-02 1.4054054e-01 4.7029846e-04 3.2838417e-04 1.2468226e-04 0.0000000e+00 3.3818408e-03 0.0000000e+00 1.2500739e-04 3.2413093e-04 0.0000000e+00 1.2515500e-03 2.8219141e-04 1.3584282e-02 4.0855052e-02 1.3616339e-01 4.6790934e-04 3.1930366e-04 1.2362003e-04 0.0000000e+00 3.4042780e-03 0.0000000e+00 1.2378582e-04 3.1528852e-04 0.0000000e+00 1.1999974e-03 2.6661912e-04 1.2813596e-02 3.9530825e-02 1.3203080e-01 4.6522663e-04 3.1061687e-04 1.2241905e-04 0.0000000e+00 3.4267856e-03 0.0000000e+00 1.2243848e-04 3.0680515e-04 0.0000000e+00 1.1517669e-03 2.5215101e-04 1.2109573e-02 3.8282756e-02 1.2812283e-01 4.6228084e-04 3.0228094e-04 1.2109422e-04 0.0000000e+00 3.4493642e-03 0.0000000e+00 1.2099183e-04 2.9866660e-04 0.0000000e+00 1.1065636e-03 2.3868908e-04 1.1464774e-02 3.7104543e-02 1.2442166e-01 4.5911497e-04 2.9428141e-04 1.1966849e-04 0.0000000e+00 3.4720142e-03 2.2907245e-12 1.1944307e-04 2.9082812e-04 0.0000000e+00 1.0641062e-03 2.2611455e-04 1.0871902e-02 3.5990536e-02 1.2091128e-01 4.5574638e-04 2.8657662e-04 1.1814451e-04 2.2860257e-12 3.4947360e-03 3.5312090e-06 1.1778018e-04 2.8314581e-04 0.0000000e+00 1.0226257e-03 2.1458834e-04 1.0298429e-02 3.4918209e-02 1.1752109e-01 4.5260707e-04 2.7902412e-04 1.1650633e-04 3.5239656e-06 3.5173559e-03 5.9769273e-06 1.1618211e-04 2.7601465e-04 0.0000000e+00 9.8545211e-04 2.0378645e-04 9.7839779e-03 3.3926091e-02 1.1437528e-01 4.4908608e-04 2.7201637e-04 1.1493432e-04 5.9523798e-06 3.5397384e-03 8.1622619e-06 1.1454689e-04 2.6914154e-04 0.0000000e+00 9.5029747e-04 1.9364178e-04 9.3082811e-03 3.2981474e-02 1.1137173e-01 4.4545713e-04 2.6525909e-04 1.1332379e-04 8.1229785e-06 3.5622088e-03 1.0116644e-05 1.1288642e-04 2.6251741e-04 0.0000000e+00 9.1701411e-04 1.8410381e-04 8.8675950e-03 3.2081151e-02 1.0850127e-01 4.4174560e-04 2.5874800e-04 1.1168885e-04 1.0063200e-05 3.5847675e-03 1.1856507e-05 1.1118744e-04 2.5610700e-04 0.0000000e+00 8.8544833e-04 1.7510337e-04 8.4577022e-03 3.1222166e-02 1.0575543e-01 4.3794454e-04 2.5244423e-04 1.1001420e-04 1.1791232e-05 3.6074157e-03 1.3416660e-05 1.0950321e-04 2.4994900e-04 0.0000000e+00 8.5552189e-04 1.6664774e-04 8.0773680e-03 3.0401888e-02 1.0312654e-01 4.3411795e-04 2.4638906e-04 1.0835595e-04 1.3341304e-05 3.6301540e-03 1.4811216e-05 1.0781873e-04 2.4400860e-04 0.0000000e+00 8.2710223e-04 1.5867586e-04 7.7231750e-03 2.9617832e-02 1.0060746e-01 4.3025450e-04 2.4054770e-04 1.0669544e-04 1.4727237e-05 3.6529834e-03 1.6059579e-05 1.0614136e-04 2.3828242e-04 0.0000000e+00 8.0008969e-04 1.5115582e-04 7.3927962e-03 2.8867749e-02 9.8191632e-02 4.2636789e-04 2.3491344e-04 1.0504097e-04 1.5967550e-05 3.6759046e-03 1.7173462e-05 1.0447235e-04 2.3275554e-04 0.0000000e+00 7.7438866e-04 1.4405219e-04 7.0841536e-03 2.8149497e-02 9.5872841e-02 4.2246958e-04 2.2947800e-04 1.0339644e-04 1.7074869e-05 3.6989184e-03 1.8168858e-05 1.0281946e-04 2.2742344e-04 0.0000000e+00 7.4992008e-04 1.3734050e-04 6.7953860e-03 2.7461288e-02 9.3645853e-02 4.1856743e-04 2.2423301e-04 1.0176507e-04 1.8064196e-05 3.7220258e-03 1.9040998e-05 1.0115885e-04 2.2225100e-04 0.0000000e+00 7.2657861e-04 1.3096877e-04 6.5238813e-03 2.6801328e-02 9.1505472e-02 4.1464266e-04 2.1914423e-04 1.0012770e-04 1.8931942e-05 3.7452278e-03 1.9830588e-05 9.9541730e-05 2.1727887e-04 0.0000000e+00 7.0433724e-04 1.2495856e-04 6.2699408e-03 2.6167915e-02 8.9446596e-02 4.1075121e-04 2.1425223e-04 9.8531143e-05 1.9716430e-05 3.7685249e-03 2.0530933e-05 9.7945535e-05 2.1247597e-04 0.0000000e+00 6.8310790e-04 1.1926623e-04 6.0313534e-03 2.5559576e-02 8.7464931e-02 4.0687630e-04 2.0952676e-04 9.6956172e-05 2.0414196e-05 3.7919182e-03 2.1153023e-05 9.6372849e-05 2.0783528e-04 0.0000000e+00 6.6282823e-04 1.1386970e-04 5.8069005e-03 2.4974910e-02 8.5556339e-02 4.0302151e-04 2.0496149e-04 9.5405388e-05 2.1033525e-05 3.8154087e-03 2.1703716e-05 9.4826704e-05 2.0335096e-04 0.0000000e+00 6.4344356e-04 1.0875131e-04 5.5954815e-03 2.4412621e-02 8.3716977e-02 3.9919184e-04 2.0054791e-04 9.3878193e-05 2.1581470e-05 3.8389972e-03 2.2190071e-05 9.3305231e-05 1.9901585e-04 0.0000000e+00 6.2490174e-04 1.0389449e-04 5.3960989e-03 2.3871497e-02 8.1943256e-02 3.9538986e-04 1.9628078e-04 9.2376739e-05 2.2065036e-05 3.8626849e-03 2.2616642e-05 9.1810714e-05 1.9482134e-04 0.0000000e+00 6.0715170e-04 9.9281630e-05 5.2078483e-03 2.3350417e-02 8.0231827e-02 3.9162026e-04 1.9215392e-04 9.0902068e-05 2.2490634e-05 3.8864723e-03 2.2972459e-05 9.0320786e-05 1.9074119e-04 0.0000000e+00 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0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 0.0000000e+00 'End:' pythia8-8.1.80.orig/xmldoc/ct09mc2.pds0000444000175000017500000173562312217346301015526 0ustar sunsunPDF Table for Fit #: fl6msrv Ordr, Nfl, lambda Qmass 1, 2, 3, 4, 5, 6 2. 5. 0.2268 0.001 0.001 0.200 1.300 4.650 172.000 IPD0, IHDN, IKNL, NfMx, Nfval, KF, Nelmt 1 1 1 5 2 12 57300 NX, NT, JT, NG, NTL(NG+1) 190 24 1 2 24 (NTL(I), NTN(I), TLN(I), DTN(I), I =1, NG) 0 7 5.57275E-01 7.83026E-02 7 17 1.10539E+00 8.58403E-02 QINI, QMAX, (QV(I), TV(I), I =0, NT) 1.30000E+00 1.00000E+05 1.30000E+00 5.57275E-01 1.49866E+00 6.35577E-01 1.74779E+00 7.13880E-01 2.06404E+00 7.92182E-01 2.47076E+00 8.70485E-01 3.00126E+00 9.48788E-01 3.70389E+00 1.02709E+00 4.65000E+00 1.10539E+00 6.09576E+00 1.19123E+00 8.18731E+00 1.27707E+00 1.12911E+01 1.36291E+00 1.60268E+01 1.44875E+00 2.34741E+01 1.53459E+00 3.55786E+01 1.62043E+00 5.59725E+01 1.70627E+00 9.17063E+01 1.79212E+00 1.57052E+02 1.87796E+00 2.82247E+02 1.96380E+00 5.34606E+02 2.04964E+00 1.07227E+03 2.13548E+00 2.28911E+03 2.22132E+00 5.23059E+03 2.30716E+00 1.28707E+04 2.39300E+00 3.43324E+04 2.47884E+00 1.00000E+05 2.56468E+00 XMIN, XCR, (XV(I), I =1, NX) 1.00000E-08 1.50000E+00 1.00000E-08 1.17803E-08 1.38778E-08 1.63489E-08 1.92599E-08 2.26892E-08 2.67291E-08 3.14884E-08 3.70950E-08 4.36999E-08 5.14807E-08 6.06469E-08 7.14452E-08 8.41659E-08 9.91515E-08 1.16805E-07 1.37602E-07 1.62101E-07 1.90962E-07 2.24961E-07 2.65013E-07 3.12195E-07 3.67777E-07 4.33253E-07 5.10385E-07 6.01248E-07 7.08284E-07 8.34965E-07 9.83595E-07 1.15868E-06 1.36492E-06 1.60787E-06 1.89406E-06 2.23117E-06 2.62841E-06 3.09641E-06 3.64773E-06 4.29722E-06 5.06234E-06 5.96367E-06 7.02548E-06 8.27631E-06 9.74982E-06 1.14856E-05 1.35304E-05 1.59392E-05 1.87766E-05 2.21191E-05 2.60564E-05 3.06942E-05 3.61571E-05 4.25918E-05 5.01709E-05 5.90977E-05 6.96115E-05 8.19937E-05 9.65758E-05 1.13747E-04 1.33967E-04 1.57774E-04 1.85802E-04 2.18795E-04 2.57627E-04 3.03325E-04 3.57094E-04 4.20343E-04 4.94725E-04 5.82239E-04 6.85007E-04 8.05733E-04 9.47515E-04 1.11390E-03 1.30904E-03 1.53770E-03 1.80543E-03 2.11857E-03 2.48437E-03 2.91111E-03 3.40814E-03 3.98598E-03 4.65639E-03 5.43234E-03 6.32831E-03 7.35986E-03 8.54125E-03 9.89379E-03 1.14309E-02 1.31758E-02 1.51436E-02 1.73523E-02 1.98189E-02 2.25606E-02 2.55851E-02 2.89092E-02 3.25397E-02 3.64826E-02 4.07414E-02 4.53168E-02 5.02071E-02 5.54085E-02 6.09151E-02 6.67197E-02 7.28133E-02 7.91861E-02 8.58274E-02 9.27257E-02 9.98695E-02 1.07243E-01 1.14848E-01 1.22661E-01 1.30677E-01 1.38873E-01 1.47265E-01 1.55821E-01 1.64539E-01 1.73408E-01 1.82435E-01 1.91589E-01 2.00875E-01 2.10284E-01 2.19811E-01 2.29449E-01 2.39192E-01 2.49036E-01 2.58974E-01 2.69003E-01 2.79118E-01 2.89315E-01 2.99590E-01 3.09940E-01 3.20361E-01 3.30848E-01 3.41402E-01 3.52019E-01 3.62695E-01 3.73426E-01 3.84208E-01 3.95063E-01 4.05950E-01 4.16887E-01 4.27870E-01 4.38898E-01 4.49969E-01 4.61082E-01 4.72234E-01 4.83424E-01 4.94651E-01 5.05914E-01 5.17211E-01 5.28541E-01 5.39903E-01 5.51296E-01 5.62718E-01 5.74170E-01 5.85653E-01 5.97163E-01 6.08683E-01 6.20243E-01 6.31826E-01 6.43433E-01 6.55063E-01 6.66715E-01 6.78389E-01 6.90084E-01 7.01799E-01 7.13535E-01 7.25289E-01 7.37063E-01 7.48855E-01 7.60668E-01 7.72487E-01 7.84333E-01 7.96195E-01 8.08073E-01 8.19966E-01 8.31874E-01 8.43797E-01 8.55734E-01 8.67686E-01 8.79651E-01 8.91628E-01 9.03624E-01 9.15628E-01 9.27645E-01 9.39675E-01 9.51717E-01 9.63770E-01 9.75836E-01 9.87912E-01 1.00000E+00 Parton Distribution Table: 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 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    Leptoquark Processes

    Leptoquarks arise in many scenarios, and can have widely different characteristics, with respect to spin, isospin am d flavour. The current implementation in no sense attempts to exhaust these possibilities, but only to encode one of the simplest possibilities, with a single scalar leptoquark, denoted LQ and assigned PDG code 42. The leptoquark is assumed to carry specific quark and lepton quantum numbers, by default u quark plus electron. These flavour numbers are conserved, i.e. a process such as u e^- -> LQ -> d nu_e is not allowed.

    Although only one leptoquark is implemented, its flavours may be changed arbitrarily to study the different possibilities. The flavours of the leptoquark are defined by the quark and lepton flavours in the decay mode list. Therefore, to change from the current u e^- to c mu^+, say, you only need a line
    pythia.readString("42:0:products = 4 -13");
    in your main program, or the equivalent in a command file. The former must always be a quark, while the latter could be a lepton or an antilepton; a charge-conjugate partner is automatically defined by the program. At initialization, the charge is recalculated as a function of the flavours defined; also the leptoquark name is redefined to be of the type LQ_q,l, where actual quark and lepton flavours are displayed.

    The leptoquark is likely to be fairly long-lived, in which case it could have time to fragment into a mesonic- or baryonic-type state, which would decay later on. Currently this possibility is not handled; therefore the leptoquark is always assumed to decay before fragmentation. For that reason the leptoquark can also not be put stable.

    Production processes

    Four production processes have been implemented, which normally would not overlap and therefore could be run together. Common switch for the group of lowest-order LQ production processes, i.e. the four ones below. Scatterings q l -> LQ. Code 3201. Scatterings q g -> LQ l. Code 3202. Scatterings g g -> LQ LQbar. Code 3203. Scatterings q qbar -> LQ LQbar. Code 3204.

    Parameters

    In the above scenario the main free parameters are the leptoquark flavour content, set as already described, and the LQ mass, set as usual. In addition there is one further parameter. multiplicative factor in the LQ -> q l squared Yukawa coupling, and thereby in the LQ width and the q l -> LQ and other cross sections. Specifically, lambda^2/(4 pi) = k alpha_em, i.e. it corresponds to the $k$ factor of Hew88.
    pythia8-8.1.80.orig/xmldoc/NNPDF23_lo_as_0119_qed.grid0000444000175000017500000402636412217346307020202 0ustar sunsun 'Version' '5.8.9' 'Description:' 'NNPDF23_lo_as_0119_qed.grid' 'NNPDF2.3QED LO, arxiv:1308.0598' 'LO QCD + LO QED PDF set, alphas(MZ)=0.119' 'NNPDF Collaboration: R.D. Ball, V. Bertone,' 'S. Carrazza, L. Del Debbio, S. Forte,' 'A. Guffanti, N.P. Hartland, J. Rojo' 'This set has 1 member PDF' 'mem=0 --> average on replicas.' 'Evolution - pol. interpolation on the LH grid.' 'Alphas:' 'Variable','lo','EvolCode' 1 , 91.200000000000003 , 1.4142135623730951 , 4.7500000000000000 , 175.00000000000000 'MinMax:' 0 , 1 1.00000000000000006E-009 , 1.00000000000000000 , 2.0000000000000000 , 100000000.000000000 'QCDparams:' 0 , 1 0.1275 , 0.0931 'Parameterlist:' 'list', 0 , 1 0.11899999999999999 'Evolution:' 'lo', 2.0000000000000000 , 1.00000000000000000 ,5 'NNPDF20intqed' 0 , 1 100 1.00000000000000006E-009 1.45082877849593975E-009 2.10490414451202072E-009 3.05385550883341570E-009 4.43062145758388157E-009 6.42807311728432258E-009 9.32603346883219949E-009 1.35304777457980767E-008 1.96304065004027145E-008 2.84803586843580223E-008 4.13201240011533895E-008 5.99484250318941207E-008 8.69749002617783555E-008 1.26185688306602100E-007 1.83073828029536992E-007 2.65608778294668702E-007 3.85352859371053147E-007 5.59081018251222919E-007 8.11130830789687312E-007 1.17681195243499912E-006 1.70735264747069220E-006 2.47707635599171153E-006 3.59381366380462954E-006 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0.0000000E+00 0.0000000E+00 0.0000000E+00 0.0000000E+00 'End:' pythia8-8.1.80.orig/xmldoc/JetMatching.xml0000444000175000017500000006342012217346303016542 0ustar sunsun

    Jet Matching

    This manual page describes the parton-jet matching interfaces for PYTHIA8. In this approach, usually referred to as MLM matching Man02, Man07, the final jets after parton-shower evolution and jet clustering are matched to the original partons. The event is accepted if a reasonable match is found, and rejected if not. The rejection step in an approximate way introduces a Sudakov form factor on to the hard processes. Notably the parton shower should not generate an emission that would doublecount hard activity already included in the matrix-element description. Within this general ansatz, different technical solutions can be adopted. We provide two alternatives, one based on the algorithm used in ALPGEN Man03, and another on the one used in Madgraph Alw11, both reimplemented from scratch here. The main points of these two algorithms are outlined further down on this page.

    We also allow for two alternative sources of external events, one in the ALPGEN native format and one in the Madgraph LHEF-based one. All four combinations of input format and matching style are implemented. In the following it is therefore important to keep the two aspects apart, whenever the ALPGEN and Madgraph labels are used.

    Currently all the files of interest are located in the examples/ subdirectory:

    • JetMatching.h contains the machinery for the parton-jet matching, in the two JetMatchingAlpgen and JetMatchingMadgraph classes.
    • GeneratorInput.h contains three classes for the reading of ALPGEN event and parameter files, and one for the reading of Madgraph parameters.
    • CombineMatchingInput.h contains three classes that combine the reading of events with the matching of them.
    • main32.cc, main32.cmnd : a sample main program and card file showing the usage of the previous files/classes.

    Event input source

    External sources of partons are used in the parton-jet matching process. The source of the partons has been separated from the implementation of the matching algorithm. By default, PYTHIA8 contains a machinery to process Les Houches Event Files (LHEFs) as described on the Les Houches Accord and Beam Parameters pages. Madgraph5 adheres to this format, but also contains some further non-standardized information that can be used. The parsing of the native ALPGEN file format is described on the Alpgen Event Interface page.

    Commonly, the source of external partons also contains information about how a particular type of matching algorithm should be employed. This information is handled by the AlpgenPar class for ALPGEN files, and MadgraphPar for LHEFs. The user can choose to set default matching parameters using the Alpgen:setMLM flag for ALPGEN files. For LHEFs, instead, the setting of default parameters is controlled with the JetMatching:setMad flag: When enabled, the merging parameters are set according to the values in the LHEF header. Specifically, the header must set the ickkw, xqcut, maxjetflavor and alpsfact values, and ickkw must be nonzero. Note that these labels are Madgraph-specific. For other programs with LHEF output, or for Madgraph files lacking this information, these parameters should be set by the user (or one can rely on the default values). The following parameters (described below) must then be specified:

    • JetMatching:doMerge = ickkw,
    • JetMatching:qCut = xqcut,
    • JetMatching:nQmatch = maxjetflavor,
    • JetMatching:clFact = alpsfact.
    With this flag on, the values from the LHEF for these parameters take precedence over other values.

    Jet Matching parameters

    A class JetMatching, derived from UserHooks, is used to define the basic structure of a parton-jet matching algorithm. Two versions are implemented here, based on the FORTRAN code provided by the ALPGEN and Madgraph packages, respectively: JetMatchingAlpgen and JetMatchingMadgraph. The matching parameters are defined with the JetMatching:* keyword.

    Scheme and Usage

    Master switch to activate parton-jet matching. When off, all external events are accepted (unless they are rejected due to weighting or event processing problems). The parton-jet MLM-style matching scheme.

    Jet algorithm

    The choice of jet algorithm and associated parameters can be adjusted with the settings below. The PYTHIA8 internal CellJet and SlowJet routines are used for jet finding. See the Event Analysis page for more details. The choice of jet algorithm to use when merging against hard partons. Currently, only SlowJet with the kT algorithm (and useStandardR = false) is supported for Madgraph-style matching, while there is full freedom for the ALPGEN-style matching. The power to use in the SlowJet algorithm. Specific to the CellJet algorithm, the number of bins in pseudorapidity. Specific to the CellJet algorithm, the number of bins in phi. Specific to the CellJet algorithm, the minimum eT for a cell to be acceptable as the trial center of a jet. Specific to the CellJet algorithm, cells with eT < eTthreshold are completely neglected by the jet algorithm.

    Merging parameters

    The following options are the three main parameters for the merging procedure. Although here they are in principle free parameters, they should be heavily influenced by the hard process generation cuts. These values can be set automatically based on the information in the ALPGEN file or LHEF. For the CellJet algorithm, this gives the minimum transverse energy inside a cone for a jet to be accepted. For the SlowJet algorithm, this is instead the minimum transverse momentum required for a cluster to be accepted as a jet. For Madgraph-style matching, this parameter should match the qCut parameter described later. For the CellJet algorithm, this gives the size of the cone in (eta, phi) space drawn around the geometric center of the jet. For the SlowJet algorithm, this gives the R parameter. For both jet algorithms, this defines the maximum pseudorapidity that the detector is assumed to cover. In this context, however, it is tied to the phase space region in which partons have been generated. For the Alpgen-style matching, particles within etaJetMax + coneRadius are passed to the jet algorithm, with only jets within etaJetMax retained in the merging. For the Madgraph-style matching, only particles within etaJetMax are used.

    Exclusive mode

    The following settings determine whether clustered jets which do not match an original hard parton are allowed. They are typically permitted in the highest jet multiplicity sample, where the parton shower may produce extra hard jets, without risk of double counting. Any extra jet produced by the shower must be softer than any matched light jet, or else the event is vetoed. Exclusive or inclusive merging. When JetMatching:exclusive = 2, nJet indicates the minimum number of additional light jets in the incoming process. This value may be set automatically. When JetMatching:exclusive = 2, nJetMax is used to indicate the maximum number of jets that will be matched.

    Jet matching

    The following parameters control the criteria for matching a clustered jet to a hard parton. Controls which particles are clustered by the jet algorithm.

    Alpgen-specific parameters

    Criteria for matching a clustered jet to a parton. The coneMatchLight parameter used when JetMatching:jetMatch = 1. The coneRadiusHeavy parameter used when JetMatching:jetMatch = 1. When assigned a negative value, the value of JetMatching:coneRadius is used. The coneMatchHeavy parameter used when JetMatching:jetMatch = 1.

    Madgraph-specific parameters

    kT scale for merging shower products into jets. Controls the treatment of heavy quarks. The clFact parameter determines how jet-to parton matching is done. A match is defined as a squared cluster scale that equals:
    |clFact| * qCut for inclusive mode,
    |clFact| * max(qCut,min(pT(parton))) for exclusive mode, clFact ≥ 0, or
    |clFact| * min(kT(parton)) for exclusive mode, clFact < 0.

    Alpgen-style parton-jet matching and merging

    This section describes the Alpgen-style MLM merging algorithm for PYTHIA8. The most common reference to the algorithm is Man02. In many respects, however, the implementation provided in the ALPGEN package should be considered the official description of the MLM merging procedure. Although designed primarily to work with events generated with ALPGEN, it can in principle also be used with events from a different source. This should not be done without thought, however, and it is up to the user to understand the details of the algorithm and the implications of using a different hard process generator.

    First, either the CellJet or SlowJet jet algorithm is chosen. Both of these algorithms have an R and an etaMax parameter. In addition, CellJet has an eTmin and SlowJet has a pTmin parameter. These are the primary three parameters of the merging procedure, and in practice are set dependent on the cuts applied to the matrix element (ME) generation. We stress that the merging procedure is not tied to the geometry of a specific physical detector, but only to the match between the original partons and the resulting jets, using standard jet algorithms in the phase space region where partons have been generated.

    ME samples with different jet multiplicities are run through the event generator, and the generation interrupted after parton showers have been applied, but before resonance decays and beam remnants have been processed. Note in particular that top quarks will not yet be decayed, which may lead to slight differences with the PYTHIA 6 interface included with the ALPGEN package. In what follows, the hardness measure of jets/partons is taken to be eT when CellJet is used and pT when SlowJet is used. The hard system (ignoring all MPI systems) is then analysed:

    • The particles in the original matrix element process are sorted into light partons, heavy partons and other particles. For backwards compatibility, a light parton is defined as the set (d, u, s, c, b, g) with zero mass. A heavy parton is defined as the set (c, b, t) with non-zero mass.
    • All particles not originating from the heavy partons or other particles are passed to the jet algorithm and clustered.
    • Clustered jets are matched to the light partons in the original ME process. There are two different methods which can be used:
      • Method 1: The following is done for each parton, in order of decreasing hardness. The delta R between the parton and all jets is calculated and the smallest value taken. If this is less than the jet R parameter, possibly multiplied by a constant, the jet and parton are considered to match, and the jet is removed from further consideration. Note that for CellJet the delta R measure is in (eta, phi), while for SlowJet, it is in (y, phi).
      • Method 2: This method is only possible when using the SlowJet algorithm. Before the clustering is performed, extremely soft "ghost" particles are added to the event at the (y, phi) coordinates of the original matrix element partons. If such a particle is clustered into a jet, the parton and jet are considered to match. The idea of "ghost" particles was originally introduced by FastJet as a way to measure jet areas Cac06 and should not affect clustering with an infrared-safe jet algorithm.
    • If there is a light ME parton remaining which has not been matched to a jet, then the event is vetoed. If all ME partons have been matched to a jet, but there are still some extra jets remaining, then two options are possible:
      • Exclusive mode: the event is vetoed. This is typically used when there are ME samples with higher jet multiplicities, which would fill in the extra jets.
      • Inclusive mode: the event is retained if the extra jets are softer than the softest matched jet. This is typically used when there is no ME sample with higher jet multiplicity, so the parton shower should be allowed to give extra jets.
    • All particles originating from the heavy partons are passed to the jet algorithm and clustered.
    • The clustered jets are again matched to the original partons, but there is no requirement for a match to be present; all matched jets are immediately discarded. The matching procedure is much the same as for light partons, but with two differences when delta R matching is used. First, a different R parameter than that used by the jet algorithm may optionally be given. Second, all jets that are within the given radius of the parton are matched, not just the one with the smallest delta R measure. If there are still extra jets remaining then in exclusive mode the event is immediately vetoed, while in inclusive mode the event is retained if the extra jets are softer than the softest light matched jet.

    Some different options are provided, specified further above in the parameters section. These are set so that, by default, the algorithm closely follows the official MLM interface provided in the ALPGEN package.

    All vetoing of events is done through the usual User Hooks machinery, and is therefore already taken into account in the cross section. In the output from Pythia::stat(), the difference between the "Selected" and "Accepted" columns gives the number of events that have not survived the vetoing procedure. It is still the responsibility of the user to add together the results from runs with different jet multiplicities. In the simplest case, when ALPGEN input is used and the hard process parameters are used to guide the merging procedure, it is enough to set the JetMatching:nJetMax parameter.

    Madgraph-style parton-jet Merging and Matching

    This section describes the Madgraph-style parton-jet matching algorithm for PYTHIA8.

    First, the kT jet algorithm is applied using the PYTHIA8 SlowJet implementation. The useStandardR = false is used, ie. the (delta R)^2 separation is defined as 2 (cosh(delta y) - cos(delta phi)) rather than the more common (delta y)^2 + delta phi)^2. The R, etaMax, and a pTmin parameters are specified. By default, R = 1 and pTmin = qCut . It is not recommended to change these. These should match the algorithm parameters used in the Madgraph Matrix Element (ME) generation.

    ME samples with different jet multiplicities are run through the event generator, and the generation is interrupted after parton showers have been applied, but before resonance decays and beam remnants have been processed. In what follows, the hardness measure of jets/partons is taken to be kT relative to qCut. The hard system (ignoring all MPI systems) is analyzed:

    • The hard partons in the original matrix element process, provided by the LHEF, are sorted into light partons, heavy partons and other particles. A heavy parton is defined by the JetMatching:nQmatch or by the maxjetflavor value in the LHEF. nQmatch refers to the absolute value of the quark PDG identity code.
    • All partons arising from the parton shower are sorted based on their motherhood. A showered parton arising from a heavy parton or "other" parton classified in the previous step is not passed to the jet algorithm. All other partons are clustered into light jets.
    • It is checked whether there are "too few" or "too many" light jets. If the number of light jets is less than the number of light partons defined by nQmatch, the event is vetoed. If the number is larger, the event is vetoed only in exclusive mode (defined below).
    • In exclusive mode, the number of jets matches the number of light partons. In inclusive mode, the jets are re-clustered until the number of jets equals the number of light partons. Next, each light hard parton is clustered, one at a time, with the jets until a match is found. A match is defined as a squared cluster scale that equals:
      • |clFact| * qCut for inclusive mode,
      • |clFact| * max(qCut,min(pT(parton))) for exclusive mode, clFact ≥ 0, or
      • |clFact| * min(kT(parton)) for exclusive mode, clFact < 0.
      If no match is found, the event is vetoed. When a parton matches a jet, the jet is removed from the collection, and the process continues. The process terminates when all partons are matched to a jet, or a parton is unmatched.
    • All particles originating from the heavy partons are not used.
    In exclusive mode, it is expected that ME samples with higher parton multiplicity are available to fill the phase space above qCut. The inclusive mode is when there are no such samples, and the parton shower is used to fill the phase space.

    Some different options are provided, specified further above. These are set so that, by default, the algorithm closely follows the FORTRAN interface ME2Pythia provided in the Madgraph package.

    All vetoing of events is done through the usual User Hooks machinery, and is therefore already taken into account in the cross section. In the output from Pythia::stat(), the difference between the "Selected" and "Accepted" columns gives the number of events that have not survived the vetoing procedure. It is still the responsibility of the user to add together the results from runs with different jet multiplicities. In the simplest case, when the hard process parameters are used to guide the merging procedure, events will be matched in the exclusive mode.

    A note on combining UserHooks

    As have been noted above, the matching is implemented using classes derived from the UserHooks class, thereby gaining access to the event generation process at the relevant locations. For native ALPGEN files, which do not adhere to the Les Houches standards, it is also necessary to intervene with a UserHooks-derived AlpgenHooks to handle the extraction and setting of relevant extra information.

    One must then combine multiple UserHooks classes, such that the functionality of both is present. A prerequisite is that the different UserHooks classes should be declared with virtual inheritance, e.g.

      class JetMatching : virtual public UserHooks
    
    Without this option, when combining two UserHooks-derived classes, two copies of the base UserHooks class would be created, leading to ambiguities.

    The two first classes in CombineMatchingInput.h combine ALPGEN input with the two different matching schemes, e.g. for the first

    class JetMatchingAlpgenInputAlpgen : public AlpgenHooks, 
      public JetMatchingAlpgen {
    public:
      // Constructor and destructor.
      JetMatchingAlpgenInputAlpgen(Pythia& pythia) : AlpgenHooks(pythia), 
        JetMatchingAlpgen() { }
      ~JetMatchingAlpgenInputAlpgen() {}
      // Initialisation.
      virtual bool initAfterBeams() {
        if (!AlpgenHooks::initAfterBeams()) return false;
        if (!JetMatchingAlpgen::initAfterBeams()) return false;
        return true;
      }
      // Process level vetos.
      virtual bool canVetoProcessLevel() { 
        return JetMatchingAlpgen::canVetoProcessLevel();    
      }
      ....
    };
    
    This class inherits from both AlpgenHooks and JetMatchingAlpgen. Any functions which are present in both classes should be overridden with a function that calls the different parent methods in the desired order. In the above example, the only shared methods are the constructor and initAfterBeams().
    pythia8-8.1.80.orig/xmldoc/NewGaugeBosonProcesses.xml0000444000175000017500000003141612217346305020741 0ustar sunsun

    New-Gauge-Boson Processes

    This page contains the production of new Z'^0 and W'^+- gauge bosons, e.g. within the context of a new U(1) or SU(2) gauge group, and also a (rather speculative) horizontal gauge boson R^0. Left-right-symmetry scenarios also contain new gauge bosons, but are described separately.

    Z'^0

    This group only contains one subprocess, with the full gamma^*/Z^0/Z'^0 interference structure for couplings to fermion pairs. It is possible to pick only a subset, e.g, only the pure Z'^0 piece. No higher-order processes are available explicitly, but the ISR showers contain automatic matching to the Z'^0 + 1 jet matrix elements, as for the corresponding gamma^*/Z^0 process. Scattering f fbar ->Z'^0. Code 3001. Choice of full gamma^*/Z^0/Z'^0 structure or not in the above process. Note that, with the Z'^0 part switched off, this process is reduced to what already exists among electroweak processes, so those options are here only for crosschecks. Note: irrespective of the option used, the particle produced will always be assigned code 32 for Z'^0, and open decay channels is purely dictated by what is set for the Z'^0.

    The couplings of the Z'^0 to quarks and leptons can either be assumed universal, i.e. generation-independent, or not. In the former case eight numbers parametrize the vector and axial couplings of down-type quarks, up-type quarks, leptons and neutrinos, respectively. Depending on your assumed neutrino nature you may want to restrict your freedom in that sector, but no limitations are enforced by the program. The default corresponds to the same couplings as that of the Standard Model Z^0, with axial couplings a_f = +-1 and vector couplings v_f = a_f - 4 e_f sin^2(theta_W), with sin^2(theta_W) = 0.23. Without universality the same eight numbers have to be set separately also for the second and the third generation. The choice of fixed axial and vector couplings implies a resonance width that increases linearly with the Z'^0 mass.

    By a suitable choice of the parameters, it is possible to simulate just about any imaginable Z'^0 scenario, with full interference effects in cross sections and decay angular distributions and generation-dependent couplings; the default values should mainly be viewed as placeholders. The conversion from the coupling conventions in a set of different Z'^0 models in the literature to those used in PYTHIA is described by C. Ciobanu et al. If on then you need only set the first-generation couplings below, and these are automatically also used for the second and third generation. If off, then couplings can be chosen separately for each generation.

    Here are the couplings always valid for the first generation, and normally also for the second and third by trivial analogy: vector coupling of d quarks. axial coupling of d quarks. vector coupling of u quarks. axial coupling of u quarks. vector coupling of e leptons. axial coupling of e leptons. vector coupling of nu_e neutrinos. axial coupling of nu_e neutrinos.

    Here are the further couplings that are specific for a scenario with Zprime:universality switched off: vector coupling of s quarks. axial coupling of s quarks. vector coupling of c quarks. axial coupling of c quarks. vector coupling of mu leptons. axial coupling of mu leptons. vector coupling of nu_mu neutrinos. axial coupling of nu_mu neutrinos. vector coupling of b quarks. axial coupling of b quarks. vector coupling of t quarks. axial coupling of t quarks. vector coupling of tau leptons. axial coupling of tau leptons. vector coupling of nu_tau neutrinos. axial coupling of nu_tau neutrinos.

    The coupling to the decay channel Z'^0 -> W^+ W^- is more model-dependent. By default it is therefore off, but can be switched on as follows. Furthermore, we have left some amount of freedom in the choice of decay angular correlations in this channel, but obviously alternative shapes could be imagined. the coupling Z'^0 -> W^+ W^- is taken to be this number times m_W^2 / m_Z'^2 times the Z^0 -> W^+ W^- coupling. Thus a unit value corresponds to the Z^0 -> W^+ W^- coupling, scaled down by a factor m_W^2 / m_Z'^2, and gives a Z'^0 partial width into this channel that again increases linearly. If you cancel this behaviour, by letting Zprime:coup2WW be proportional to m_Z'^2 / m_W^2, you instead obtain a partial width that goes like the fifth power of the Z'^0 mass. These two extremes correspond to the "extended gauge model" and the "reference model", respectively, of Alt89. Note that this channel only includes the pure Z' part, while f fbar -> gamma^*/Z^*0 -> W^+ W^- is available as a separate electroweak process. in the decay chain Z'^0 -> W^+ W^- ->f_1 fbar_2 f_3 fbar_4 the decay angular distributions is taken to be a mixture of two possible shapes. This parameter gives the fraction that is distributed as in Higgs h^0 -> W^+ W^- (longitudinal bosons), with the remainder (by default all) is taken to be the same as for Z^0 -> W^+ W^- (a mixture of transverse and longitudinal bosons).

    A massive Z'^0 is also likely to decay into Higgs bosons and potentially into other now unknown particles. Such possibilities clearly are quite model-dependent, and have not been included for now.

    W'^+-

    The W'^+- implementation is less ambitious than the Z'^0. Specifically, while indirect detection of a Z'^0 through its interference contribution is a possible discovery channel in lepton colliders, there is no equally compelling case for W^+-/W'^+- interference effects being of importance for discovery, and such interference has therefore not been implemented for now. Related to this, a Z'^0 could appear on its own in a new U(1) group, while W'^+- would have to sit in a SU(2) group and thus have a Z'^0 partner that is likely to be found first. Only one process is implemented but, like for the W^+-, the ISR showers contain automatic matching to the W'^+- + 1 jet matrix elements. Scattering f fbar' -> W'^+-. Code 3021.

    The couplings of the W'^+- are here assumed universal, i.e. the same for all generations. One may set vector and axial couplings freely, separately for the q qbar' and the l nu_l decay channels. The defaults correspond to the V - A structure and normalization of the Standard Model W^+-, but can be changed to simulate a wide selection of models. One limitation is that, for simplicity, the same Cabibbo--Kobayashi--Maskawa quark mixing matrix is assumed as for the standard W^+-. Depending on your assumed neutrino nature you may want to restrict your freedom in the lepton sector, but no limitations are enforced by the program. vector coupling of quarks. axial coupling of quarks. vector coupling of leptons. axial coupling of leptons.

    The coupling to the decay channel W'^+- -> W^+- Z^0 is more model-dependent, like for Z'^0 -> W^+ W^- described above. By default it is therefore off, but can be switched on as follows. Furthermore, we have left some amount of freedom in the choice of decay angular correlations in this channel, but obviously alternative shapes could be imagined. the coupling W'^0 -> W^+- Z^0 is taken to be this number times m_W^2 / m_W'^2 times the W^+- -> W^+- Z^0 coupling. Thus a unit value corresponds to the W^+- -> W^+- Z^0 coupling, scaled down by a factor m_W^2 / m_W'^2, and gives a W'^+- partial width into this channel that increases linearly with the W'^+- mass. If you cancel this behaviour, by letting Wprime:coup2WZ be proportional to m_W'^2 / m_W^2, you instead obtain a partial width that goes like the fifth power of the W'^+- mass. These two extremes correspond to the "extended gauge model" and the "reference model", respectively, of Alt89. in the decay chain W'^+- -> W^+- Z^0 ->f_1 fbar_2 f_3 fbar_4 the decay angular distributions is taken to be a mixture of two possible shapes. This parameter gives the fraction that is distributed as in Higgs H^+- -> W^+- Z^0 (longitudinal bosons), with the remainder (by default all) is taken to be the same as for W^+- -> W^+- Z^0 (a mixture of transverse and longitudinal bosons).

    A massive W'^+- is also likely to decay into Higgs bosons and potentially into other now unknown particles. Such possibilities clearly are quite model-dependent, and have not been included for now.

    R^0

    The R^0 boson (particle code 41) represents one possible scenario for a horizontal gauge boson, i.e. a gauge boson that couples between the generations, inducing processes like s dbar -> R^0 -> mu^- e^+. Experimental limits on flavour-changing neutral currents forces such a boson to be fairly heavy. In spite of being neutral the antiparticle is distinct from the particle: one carries a net positive generation number and the other a negative one. This particular model has no new parameters beyond the R^0 mass. Decays are assumed isotropic. For further details see Ben85. Scattering f_1 fbar_2 -> R^0 -> f_3 fbar_4, where f_1 and fbar_2 are separated by +- one generation and similarly for f_3 and fbar_4. Thus possible final states are e.g. d sbar, u cbar s bbar, c tbar, e- mu+ and mu- tau+. Code 3041.
    pythia8-8.1.80.orig/xmldoc/ParticleDataScheme.xml0000444000175000017500000017434712217346314020044 0ustar sunsun

    The Particle Data Scheme

    The particle data scheme may take somewhat longer to understand than the settings one. In particular the set of methods to access information is rather more varied, to allow better functionality for advanced usage. However, PYTHIA does come with a sensible default set of particle properties and decay tables. Thus there is no need to learn any of the methods on this page to get going. Only when you perceive a specific need does it make sense to learn the basics.

    The central section on this page is the Operation one. The preceding sections are there mainly to introduce the basic structure and the set of properties that can be accessed. The subsequent sections provide a complete listing of the existing public methods, which most users probably will have little interaction with.

    Databases

    The management of particle data is based on three classes:
    • ParticleData, which is the top-level class, with methods that can be used to interrogate all particle data. It contains a map of PDG particle identity numbers Yao06 onto the relevant ParticleDataEntry objects,
    • ParticleDataEntry, which stores the relevant information on an individual particle species, and
    • DecayChannel, which stores info on one particular decay mode of a particle.
    The objects of these classes together form a database that is continuously being used as the program has to assign particle masses, select decay modes, etc.

    Each Pythia object has a public member particleData of the ParticleData class. Therefore you access the particle data methods as pythia.particleData.command(argument), assuming that pythia is an instance of the Pythia class. Further, for some of the most frequent user tasks, Pythia methods have been defined, so that pythia.command(argument) would work, see further below.

    A fundamental difference between the particle data classes and the settings ones is that the former are accessed regularly during the event generation process, as a new particle is produced and its mass need to be set, e.g., while the latter are mainly/only used at the initialization stage. Nevertheless, it is not a good idea to change data in either of them in mid-run, since this may lead to inconsistencies.

    Stored properties for particles

    The main properties stored for each particle are as follows. Different ways to set and get these properties will be described further down.
    • name: a character string with the name of the particle. Particle and antiparticle names are stored separately, with void returned when no antiparticle exists.
    • spinType: the spin type, of the form 2 s + 1, with special code 0 for entries of unknown or indeterminate spin.
    • chargeType: three times the charge (to make it an integer).
    • colType: the colour type, with 0 uncoloured, 1 triplet, -1 antitriplet and 2 octet. (A preliminary implementation of colour sextets, available since version 8.150, further uses 3 for a sextet and -3 for an antisextet.)
    • m0: the nominal mass m_0 (in GeV).
    • mWidth: the width Gamma of the Breit-Wigner distribution (in GeV).
    • mMin: the lower limit of the allowed mass range generated by the Breit-Wigner (in GeV). Has no meaning for particles without width, and would typically be 0 there.
    • mMax: the upper limit of the allowed mass range generated by the Breit-Wigner (in GeV). If mMax < mMin then no upper limit is imposed. Has no meaning for particles without width, and would typically be 0 there.
    • tau0: the nominal proper lifetime tau_0 (in mm/c).
    • isResonance: a flag telling whether a particle species is considered as a resonance or not. Here "resonance" is used as shorthand for any massive particle where the decay process should be counted as part of the hard process itself, and thus be performed before showers and other event aspects are added. Restrictions on allowed decay channels is also directly reflected in the cross section of simulated processes, while those of normal hadrons and other light particles are not. In practice, it is reserved for states above the b bbar bound systems in mass, i.e. for W, Z, t, Higgs states, supersymmetric states and (most?) other states in any new theory. All particles with m0 above 20 GeV are by default initialized to be considered as resonances.
    • mayDecay: a flag telling whether a particle species may decay or not, offering the main user switch. Whether a given particle of this kind then actually will decay also depends on it having allowed decay channels, and on other flags for particle decays (or resonance decays). All particles with tau0 below 1000 mm are by default initialized to allow decays.
    • doExternalDecays: a flag telling whether a particle should be handled by an external decay package or not, with the latter default. Can be manipulated as described on this page, but should normally not be. Instead the Pythia::decayPtr(...) method should be provided with the list of relevant particles.
    • isVisible: a flag telling whether a particle species is to be considered as visible in a detector or not, as used e.g. in analysis routines. By default this includes neutrinos and a few BSM particles (gravitino, sneutrinos, neutralinos) that have neither strong nor electromagnetic charge, and are not made up of constituents that have it. The value of this flag is only relevant if a particle is long-lived enough actually to make it to a detector.
    • doForceWidth: a flag valid only for resonances where PYTHIA contains code to calculate the width of the resonance from encoded matrix-element expressions, i.e. the Z^0, W^+-, t, h^0, and a few more. The normal behaviour (false) is then that the width is calculated from the mass, but it is possible to force the resonance to retain the nominal width. Branching ratios and the running of the total width are unaffected.

    Stored properties for decays

    An unstable particle has a decay table consisting of one or more decay channel. The following properties are stored for each such channel. Again different ways to set and get these properties will be described further down.
    • onMode: integer code for use or not of channel,
      0 if a channel is off,
      1 if on,
      2 if on for a particle but off for an antiparticle,
      3 if on for an antiparticle but off for a particle.
      If a particle is its own antiparticle then 2 is on and 3 off but, of course, for such particles it is much simpler and safer to use only 1 and 0.
      The 2 and 3 options can be used e.g. to encode CP violation in B decays, or to let the W's in a q qbar -> W^+ W^- process decay in different channels.
    • bRatio: the branching ratio of the channel (with some reservations for resonances, see meMode below).
    • meMode: the mode of processing this channel, possibly with matrix elements; see the particle decays and resonance decays descriptions for the list of possibilities. Notably the default code 0 for a particle means pure phase space decays according to the given branching ratios, while for a resonance it means that code exists for the dynamic calculations of partial widths and thereby branching ratios as a function of the resonance mass (which is done e.g. at initialization based on the mass set by the user). Then codes 1 - 99 are reserved for various matrix-element-improved ordinary particle decays, and 100 - 103 for resonances where the partial width of a given channel is calculated from the total width and the stored branching ratio. Thus, to enforce a new branching ratio for a resonance channel (with its own partial-width calculation code) it is not sufficient only to change the bRatio but also to set e.g. meMode = 100.
    • multiplicity: the number of decay products of the channel. Can be at most 8.
    • product(i): the identity code of the decay products, where i runs between 0 and multiplicity - 1. Trailing positions are filled with 0.

    Operation

    The normal flow of the particle data operations is:
    1. When a Pythia object pythia is created, the pythia.particleData member is asked to scan the ParticleData.xml file.

      All lines beginning with <particle are scanned for information on a particle species, and all lines beginning with <channel are assumed to contain a decay channel of the enclosing particle. In both cases XML syntax is used, with attributes used to identify the stored properties, and with omitted properties defaulting back to 0 where meaningful. The particle and channel information may be split over several lines, up to the > endtoken. The format of a <particle tag is:

          <particle id="..." name="..." antiName="..." spinType="..." chargeType="..." colType="..." 
             m0="..." mWidth="..." mMin="..." mMax="..." tau0="...">
          </particle>
      
      where the fields are the properties already introduced above. Note that isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth are not set here, but are provided with default values by the rules described above. Once initialized, also these latter properties can be changed, see below.
      The format of a <channel> tag is:
          <channel onMode="..." bRatio="..." meMode="..." products="..." />
      
      again see properties above. The products are given as a blank-separated list of id codes. Important: the values in the .xml file should not be changed, except by the PYTHIA authors. Any changes should be done with the help of the methods described below.
    2. Between the creation of the Pythia object and the init call for it, you may use the methods of the ParticleData class to modify some of the default values. Several different approaches can be chosen for this.

      a) Inside your main program you can directly set values with

          pythia.readString(string);
      
      where both the variable name and the value are contained inside the character string, separated by blanks and/or a =, e.g.
          pythia.readString("111:mayDecay = off"); 
      
      switches off the decays of the pi^0.
      The particle id (> 0) and the property to be changed must be given, separated by a colon.
      The allowed properties are: name, antiName, spinType, chargeType, colType, m0, mWidth, mMin, mMax, tau0, isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth. All of these names are case-insensitive. Names that do not match an existing variable are ignored.
      Strings beginning with a non-alphanumeric character, like # or !, are assumed to be comments and are not processed at all. For bool values, the following notation may be used interchangeably: true = on = yes = ok = 1, while everything else gives false (including but not limited to false, off, no and 0).

      Particle data often comes in sets of closely related information. Therefore some properties expect the value to consist of several numbers. These can then be separated by blanks (or by commas). A simple example is names, which expects both the name and antiname to be given. A more interesting one is the all property,

        
          id:all = name antiName spinType chargeType colType m0 mWidth mMin mMax tau0
      
      where all the current information on the particle itself is replaced, but any decay channels are kept unchanged. Using new instead of all also removes any previous decay channels. If the string contains fewer fields than expected the trailing properties are set to vanish ("void", 0 or 0.). Note that such a truncated string should not be followed by a comment, since this comment would then be read in as if it contained the missing properties. The truncation can be done anywhere, specifically a string with only id:new defines a new "empty" particle. As before, isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth are (re)set to their default values, and would have to be changed separately if required.

      A further command is rescaleBR, which rescales each of the existing branching ratios with a common factor, such that their new sum is the provided value. This may be a first step towards adding new decay channels, see further below.

      Alternatively the id code may be followed by another integer, which then gives the decay channel number. This then has to be followed by the property specific to this channel, either onMode, bRatio, meMode or products. In the latter case all the products of the channel should be given:

          id:channel:products =  product1 product2 ....  
      
      The line will be scanned until the end of the line, or until a non-number word is encountered, or until the maximum allowed number of eight products is encountered, whichever happens first. (Thus the multiplicity of a decay channel need not be input; it is automatically calculated from the products list.) It is also possible to replace all the properties of a channel in a similar way:
          id:channel:all = onMode bRatio meMode product1 product2 ....  
      
      To add a new channel at the end, use
          id:addChannel = onMode bRatio meMode product1 product2 ....
      

      It is currently not possible to remove a channel selectively, but setting its branching ratio vanishing is as effective. If you want to remove all existing channels and force decays into one new channel you can use

          id:oneChannel = onMode bRatio meMode product1 product2 ....
      
      A first oneChannel command could be followed by several subsequent addChannel ones, to build up a completely new decay table for an existing particle.

      When adding new channels or changing branching ratios in general, note that, once a particle is to be decayed, the sum of branching ratios is always rescaled to unity. Beforehand, rescaleBR may be used to rescale an existing branching ratio by the given factor.

      There are a few commands that will study all the decay channels of the given particle, to switch them on or off as desired. The

          id:onMode = onMode
      
      will set the onMode property of all channels to the desired value. The
       
          id:offIfAny   = product1 product2 .... 
          id:onIfAny    = product1 product2 .... 
          id:onPosIfAny = product1 product2 .... 
          id:onNegIfAny = product1 product2 .... 
      
      will set the onMode 0, 1, 2 or 3, respectively, for all channels which contain any of the enumerated products, where the matching to these products is done without distinction of particles and antiparticles. Note that "Pos" and "Neg" are slightly misleading since it refers to the particle and antiparticle of the id species rather than charge, but should still be simpler to remember and understand than alternative notations. Correspondingly
       
          id:offIfAll   = product1 product2 .... 
          id:onIfAll    = product1 product2 .... 
          id:onPosIfAll = product1 product2 .... 
          id:onNegIfAll = product1 product2 .... 
      
      will set the onMode 0, 1, 2 or 3, respectively, for all channels which contain all of the enumerated products, again without distinction of particles and antiparticles. If the same product appears twice in the list it must also appear twice in the decay channel, and so on. The decay channel is allowed to contain further particles, beyond the product list. By contrast,
       
          id:offIfMatch   = product1 product2 .... 
          id:onIfMatch    = product1 product2 .... 
          id:onPosIfMatch = product1 product2 .... 
          id:onPosIfMatch = product1 product2 .... 
      
      requires the decay-channel multiplicity to agree with that of the product list, but otherwise works as the onIfAll/offIfAll methods.

      Note that the action of several of the commands depends on the order in which they are executed, as one would logically expect. For instance, id:oneChannel removes all decay channels of id and thus all previous changes in this decay table, while subsequent additions or changes would still take effect. Another example would be that 23:onMode = off followed by 23:onIfAny = 1 2 3 4 5 would let the Z^0 decay to quarks, while no decays would be allowed if the order were to be reversed.

      b) The Pythia readString(string) method actually does not do changes itself, but sends on the string either to the ParticleData class or to the Settings one, depending on whether the string begins with a digit or a letter. If desired, it is possible to communicate directly with the corresponding ParticleData method:

          pythia.particleData.readString("111:mayDecay = off"); 
          pythia.particleData.readString("15:2:products = 16 -211"); 
      
      In this case, changes intended for Settings would not be understood.

      c) Underlying this are commands for all the individual properties in the ParticleData class, one for each. These are further described below. Thus, an example now reads

          pythia.particleData.mayDecay(111, false);
      
      Boolean values should here be given as true or false.

      d) A simpler and more useful way is to collect all your changes in a separate file, with one line per change, e.g.

          111:mayDecay = off
      
      The file can be read by the
          pythia.readFile(fileName); 
      
      method, where fileName is a string, e.g. pythia.readFile("main.cmnd") (or an istream instead of a fileName). Each line is processed as described for the string in 2a). This file can freely mix commands to the Settings and ParticleData classes.
    3. A routine reInit(fileName) is provided, and can be used to zero the particle data table and reinitialize it from scratch. Such a call might be useful if several subruns are to be made with widely different particle data - normally the maps are only built from scratch once, namely when the Pythia() object is created. Also, there is no other possibility to restore the default values, unlike for the settings.

    4. You may at any time obtain a listing of all the particle data by calling

          pythia.particleData.listAll();
      
      The listing is by increasing id number. It shows the basic quantities introduced above. Some are abbreviated in the header to fit on the lines: spn = spinType, chg = chargeType, col = colType, res = isResonance, dec = mayDecay && canDecay (the latter checks that decay channels have been defined), ext = doExternalDecay, vis = isVisible and wid = doForceWidth.
      To list only those particles that were changed (one way or another, the listing will not tell what property or decay channel was changed), instead use
          pythia.particleData.listChanged();
      
      (This info is based on a further hasChanged flag of a particle or a channel, set true whenever any of the changing methods are used. It is possible to manipulate this value, but this is not recommended.) By default the internal initialization of the widths of resonances such as gamma^*/Z^0, W^+-, t/tbar, H^0 do not count as changes; if you want to list also those changes instead call listChanged(true).
      To list only one particle, give its id code as argument to the list(...) function.. To list a restricted set of particles, give in their id codes to list(...) as a vector<int>.
    5. For wholesale changes of particle properties all available data can be written out, edited, and then read back in again. These methods are mainly intended for expert users. You can choose between two alternative syntaxes.

      a) XML syntax, using the <particle and <channel lines already described. You use the method particleData.listXML(fileName) to produce such an XML file and particleData.readXML(fileName) to read it back in after editing.

      b) Fixed/free format, using exactly the same information as illustrated for the <particle and <channel lines above, but now without any tags. This means that all information fields must be provided (if there is no antiparticle then write void), in the correct order (while the order is irrelevant with XML syntax), and all on one line. Information is written out in properly lined-up columns, but the reading is done using free format, so fields need only be separated by at least one blank. Each new particle is supposed to be separated by (at least) one blank line, whereas no blank lines are allowed between the particle line and the subsequent decay channel lines, if any. You use the method particleData.listFF(fileName) to produce such a fixed/free file and particleData.readFF(fileName) to read it back in after editing.

      As an alternative to the readXML and readFF methods you can also use the particleData.reInit(fileName, xmlFormat) method, where xmlFormat = true (default) corresponds to reading an XML file and xmlFormat = false to a fixed/free format one.

      To check that the new particle and decay tables makes sense, you can use the particleData.checkTable() method, either directly or by switching it on among the standard error checks.

    The public methods

    In the following we present briefly the public methods in the three classes used to build up the particle database. The order is top-down, i.e from the full table of all particles to a single particle to a single channel. Note that these methods usually are less elegant and safe than the input methods outlined above. If you use any of these methods, it is likely to be the ones in the full database, i.e. the first ones to be covered in the following.

    For convenience, we have grouped related input and output methods together. It should be obvious from the context which is which: the input is of type void and has an extra last argument, namely is the input value, while the output method returns a quantity of the expected type.

    The ParticleData methods

    the constructor has no arguments and does not do anything. Internal. initialize pointers to a few other classes. Internal. read in an XML-style file with particle data and initialize the particle data tables accordingly. This command is executed in the Pythia constructor, i.e. is mainly for internal use. the name of the data file to be read. When called from the Pythia constructor the directory is provided by the PYTHIA8DATA environment variable, if set, else by the argument of this constructor, which has the default value "../xmldoc". overwrite the existing database by reading from the specified file. Unlike init above this method is not called by the Pythia constructor, but is entirely intended for users who want to replace the existing particle data with their own. the path and name of file to be read. if true read the same kind of XML-style file as used by init, if not use an alternative "free format" file (i.e. without any XML tags, but with well-defined rules specifying in which order properties are stored). initialize Breit-Wigner shape parameters for all particles, and the detailed handling of resonances, i.e. particles with perturbatively calculable partial widths, which can be used to obtain a mass-dependent Breit-Wigner and a dynamic choice of decay channels. Called from Pythia::init(). read in XML-style data from a file or write it out to a file. For the former one can also decide whether to reset all particles to scratch, or only overwrite those particles in the file. The former method is used by init and reInit above. read in free-format-style data from a file or write it out to a file. For the former one can also decide whether to reset all particles to scratch, or only overwrite those particles in the file. The former method is used by reInit above. read in a string and interpret is as a new or changed particle data. The possibilities are extensively described above. It is normally used indirectly, via Pythia::readString(...) and Pythia::readFile(...). the string to be interpreted as an instruction. write a warning message or not whenever the instruction does not make sense, e.g. if the particle does not exist in the database. stream for error printout. Note: the method returns false if it fails to make sense out of the input string. methods intended to present a listing of particle data in a readable format. The first three are special cases of the fourth. The first lists all particle data, the second only data for those particles that were changed after the original creation of the particle data table. Resonances are a special case since they can get their data changed by being linked to an object that does the calculation of branching ratios. The second method does not count such resonances as changed, whereas the third does and thus lists all resonances. list particle data for one single particle, with the identity code as input, or for a set of particles, with an input vector of identity codes. check that the particle decay table makes sense, especially for decays. level of checks. 0 is only minimal, e.g. if a particle has no open decay channels. 1, which is the level of the first method, provides warning if any individual channel is closed, except for resonances. 2 also prints the branching-ratio-averaged threshold mass. 11 and 12 are like 1 and 2, but also include resonances in the detailed checks. add a particle to the decay table; in the first form a particle which is its own antiparticle, in the second where a separate antiparticle exists. change all the properties of the particle associated with a given identity code. query whether the particle data table contains the particle of the identity code. return the identity code of the sequentially next particle stored in table. bool whether a distinct antiparticle exists or not. Is true if an antiparticle name has been set (and is different from void). particle and antiparticle names are stored separately, the sign of id determines which of the two is returned, with void used to indicate the absence of an antiparticle. the spin type, of the form 2 s + 1, with special code 0 for entries of unknown or indeterminate spin. three times the charge (to make it an integer), taking into account the sign of id. the electrical charge of a particle, equal to chargeType(id)/3. the colour type, with 0 uncoloured, 1 triplet, -1 antitriplet and 2 octet, taking into account the sign of id. the nominal mass m_0 (in GeV). the width Gamma of the Breit-Wigner distribution (in GeV). the lower limit of the allowed mass range generated by the Breit-Wigner (in GeV). Has no meaning for particles without width, and would typically be 0 there. the upper limit of the allowed mass range generated by the Breit-Wigner (in GeV). If mMax < mMin then no upper limit is imposed. Has no meaning for particles without width, and would typically be 0 there. similar to mMin() above, except that for particles with no width the m0(id) value is returned. similar to mMax() above, except that for particles with no width the m0(id) value is returned. the nominal proper lifetime tau_0 (in mm/c). a flag telling whether a particle species are considered as a resonance or not. Here "resonance" is used as shorthand for any massive particle where the decay process should be counted as part of the hard process itself, and thus be performed before showers and other event aspects are added. Restrictions on allowed decay channels is also directly reflected in the cross section of simulated processes, while those of normal hadrons and other light particles are not. In practice, it is reserved for states above the b bbar bound systems in mass, i.e. for W, Z, t, Higgs states, supersymmetric states and (most?) other states in any new theory. All particles with m0 above 20 GeV are by default initialized to be considered as resonances. a flag telling whether a particle species may decay or not, offering the main user switch. Whether a given particle of this kind then actually will decay also depends on it having allowed decay channels, and on other flags for particle decays (or resonance decays). All particles with tau0 below 1000 mm are by default initialized to allow decays. a flag telling whether a particle should be handled by an external decay package or not, with the latter default. Can be manipulated as described on this page, but should normally not be. Instead the pythia.decayPtr method should be provided with the list of relevant particles. a flag telling whether a particle species is to be considered as visible in a detector or not, as used e.g. in analysis routines. By default this includes neutrinos and a few BSM particles (gravitino, sneutrinos, neutralinos) that have neither strong nor electromagnetic charge, and are not made up of constituents that have it. The value of this flag is only relevant if a particle is long-lived enough actually to make it to a detector. a flag valid only for resonances where PYTHIA contains code to calculate the width of the resonance from encoded matrix-element expressions, i.e. the Z^0, W^+-, t, h^0, and a few more. The normal behaviour (false) is then that the width is calculated from the mass, but it is possible to force the resonance to retain the nominal width. Branching ratios and the running of the total width are unaffected. keep track of whether the data for a particle has been changed in any respect between initialization and the current status. Is used e.g. by the listChanged method to determine which particles to list. tells whether a particle will have a Breit-Wigner mass distribution or not. Is determined by an internal logic based on the particle width and on the value of the ParticleData:modeBreitWigner switch. is the constituent mass for a quark, hardcoded as m_u = m_d = 0.325, m_s = 0.50, m_c = 1.60 and m_b = 5.0 GeV, for a diquark the sum of quark constituent masses, and for everything else the same as the ordinary mass. returns a mass distributed according to a truncated Breit-Wigner, with parameters as described here. Is equal to m0(id) for particles without width. calculate the running mass of species id when probed at a hard mass scale of mH. Only applied to obtain the running quark masses; for all other particle the normal fixed mass is used. true for a particle with at least one decay channel defined. true for a lepton or an antilepton (including neutrinos). true for a quark or an antiquark. true for a gluon. true for a diquark or antidiquark. true for a gluon, a quark or antiquark up to the b (but excluding top), and a diquark or antidiquark consisting of quarks up to the b. true for a hadron (made up out of normal quarks and gluons, i.e. not for R-hadrons and other exotic states). true for a meson. true for a baryon or antibaryon. true for an intermediate hadron-like state with a colour octet charge as used in the colour octet model for onia production. extracts the heaviest quark or antiquark, i.e. one with largest id number, for a hadron. is 1 for a quark, 2 for a diquark, 3 for a baryon, the same with a minus sign for antiparticles, and else zero. rescales all partial branching ratios by a common factor, such that the sum afterward becomes newSumBR. set a pointer for a particle kind to a ResonanceWidths object. This is done, from inside ParticleData::initWidths, only for resonances, i.e. for particles such as Z^0, W^+-, top, Higgs, and new unstable states beyond the Standard Model. The presence of such an object will allow a more dynamic calculation of partial and total widths, as illustrated by the following methods. initialize the treatment of a resonance. calculate the total with for a resonance of a given current mass, optionally including coupling to incoming flavour state (consider the gamma*/Z^0 combination), optionally excluding decay channels that have been closed by the user, and optionally storing the results in the normal decay table. special case of resWidth, where only open channels are included, but results are not stored in the normal decay table. special case of resWidth, where only open channels are included, and results are stored in the normal decay table. calculate the fraction of the full branching ratio that is left open by the user choice of allowed decay channels. Can be applied to a final state with up to three resonances. Since the procedure is multiplicative, it would be easy to generalize also to more. the factor used to rescale all partial widths in case the total width is being forced to a specific value by the user. special case to calculate one final-state width; currently only used for Higgs decay to q qbar, g g or gamma gamma. returns a pointer to the ParticleDataEntry object. The methods in the next section can then be used to manipulate this object.

    The ParticleDataEntry methods

    Most of the methods that can be applied to a single ParticleDataEntry object are almost identical with those used above for the ParticleData, except that the id argument is no longer needed to find the right entry in the table. By and large, this makes direct access to the ParticleDataEntry methods superfluous. There are a few methods that are unique to each class, however. Furthermore, to avoid some naming ambiguities, many methods that set values begin with set. there are two alternative constructors, that both expect the properties of a particle as input. The first assumes that there is only one particle, the latter that there is a particle-antiparticle pair (but if the antiparticle name is void one reverts back to the particle-only case). the destructor is needed to delete any ResonanceWidths objects that have been created and linked to the respective particle. initialize some particle flags with default values, e.g. whether a particle is a resonance, may decay, or is visible. Is called from the constructors and from setAll. initialize pointer back to the whole database (so that masses of decay products can be accessed, e.g.). change all the properties of the particle associated with a given identity code. the PDG identity code. tell whether a separate antiparticle exists. set or get the particle or antiparticle name. Only the sign of id is needed to distinguish particle/antiparticle. set or get the particle spin type, i.e. 2 s + 1, or 0 in some special cases. set or get the particle charge type, i.e. three times the charge, or the charge itself. Only the sign of id is needed to distinguish particle/antiparticle. set or get the particle colour type, 0 for singlet, 1 for triplet, -1 for antitriplet, 2 for octet. Only the sign of id is needed to distinguish particle/antiparticle. the nominal mass m_0 (in GeV). the width Gamma of the Breit-Wigner distribution (in GeV). the lower limit of the allowed mass range generated by the Breit-Wigner (in GeV). Has no meaning for particles without width, and would typically be 0 there. the upper limit of the allowed mass range generated by the Breit-Wigner (in GeV). If mMax < mMin then no upper limit is imposed. Has no meaning for particles without width, and would typically be 0 there. similar to mMin() above, except that for particles with no width the m0(id) value is returned. similar to mMax() above, except that for particles with no width the m0(id) value is returned. the nominal proper lifetime tau_0 (in mm/c). a flag telling whether a particle species are considered as a resonance or not. Here "resonance" is used as shorthand for any massive particle where the decay process should be counted as part of the hard process itself, and thus be performed before showers and other event aspects are added. Restrictions on allowed decay channels is also directly reflected in the cross section of simulated processes, while those of normal hadrons and other light particles are not. In practice, it is reserved for states above the b bbar bound systems in mass, i.e. for W, Z, t, Higgs states, supersymmetric states and (most?) other states in any new theory. All particles with m0 above 20 GeV are by default initialized to be considered as resonances. a flag telling whether a particle species may decay or not, offering the main user switch. Whether a given particle of this kind then actually will decay also depends on it having allowed decay channels, and on other flags for particle decays (or resonance decays). All particles with tau0 below 1000 mm are by default initialized to allow decays. a flag telling whether a particle should be handled by an external decay package or not, with the latter default. Can be manipulated as described on this page, but should normally not be. Instead the pythia.decayPtr method should be provided with the list of relevant particles. a flag telling whether a particle species is to be considered as visible in a detector or not, as used e.g. in analysis routines. By default this includes neutrinos and a few BSM particles (gravitino, sneutrinos, neutralinos) that have neither strong nor electromagnetic charge, and are not made up of constituents that have it. The value of this flag is only relevant if a particle is long-lived enough actually to make it to a detector. a flag valid only for resonances where PYTHIA contains code to calculate the width of the resonance from encoded matrix-element expressions, i.e. the Z^0, W^+-, t, h^0, and a few more. The normal behaviour (false) is then that the width is calculated from the mass, but it is possible to force the resonance to retain the nominal width. Branching ratios and the running of the total width are unaffected. keep track of whether the data for a particle has been changed in any respect between initialization and the current status. Is used e.g. by the ParticleData::listChanged method to determine which particles to list. Prepare the Breit-Wigner mass selection by precalculating frequently-used expressions. is the constituent mass for a quark, hardcoded as m_u = m_d = 0.325, m_s = 0.50, m_c = 1.60 and m_b = 5.0 GeV, for a diquark the sum of quark constituent masses, and for everything else the same as the ordinary mass. give the mass of a particle, either at the nominal value or picked according to a (linear or quadratic) Breit-Wigner. calculate the running quark mass at a hard scale mH. For other particles the on-shell mass is given. tells whether a particle will have a Breit-Wigner mass distribution or not. Is determined by an internal logic based on the particle width and on the value of the ParticleData:modeBreitWigner switch. true for a particle with at least one decay channel defined. true for a lepton or an antilepton (including neutrinos). true for a quark or an antiquark. true for a gluon. true for a diquark or antidiquark. true for a gluon, a quark or antiquark up to the b (but excluding top), and a diquark or antidiquark consisting of quarks up to the b. true for a hadron (made up out of normal quarks and gluons, i.e. not for R-hadrons and other exotic states). true for a meson. true for a baryon or antibaryon. true for an intermediate hadron-like state with a colour octet charge as used in the colour octet model for onia production. extracts the heaviest quark or antiquark, i.e. one with largest id number, for a hadron. Only the sign of the input argument is relevant. is 1 for a quark, 2 for a diquark, 3 for a baryon, the same with a minus sign for antiparticles, and else zero. Only the sign of the input argument is relevant. resets to an empty decay table. adds a decay channel with up to 8 products. returns the number of decay channels for a particle. gain access to a specified channel in the decay table. rescales all partial branching ratios by a common factor, such that the sum afterward becomes newSumBR. prepare to pick a decay channel. pick a decay channel according to branching ratios from preparePick. set or get a pointer to an object that can be used for dynamic calculation of partial and total resonance widths. Here a resonance is a particle such as top, Z^0, W^+-, Higgs, and new unstable states beyond the Standard Model. initialize the treatment of a resonance. calculate the total with for a resonance of a given current mass, optionally including coupling to incoming flavour state (consider the gamma*/Z^0 combination), optionally excluding decay channels that have been closed by the user, and optionally storing the results in the normal decay table. For the first argument only the sign is relevant. special case of resWidth, where only open channels are included, but results are not stored in the normal decay table. special case of resWidth, where only open channels are included, and results are stored in the normal decay table. calculate the fraction of the full branching ratio that is left open by the user choice of allowed decay channels. the factor used to rescale all partial widths in case the total width is being forced to a specific value by the user. special case to calculate one final-state width; currently only used for Higgs decay to q qbar, g g or gamma gamma.

    The DecayChannel methods

    The properties stored in an individual decay channel can be set or get by the methods in this section. the constructor for a decay channel. Internal. set or get the onMode of a decay channel,
    0 if a channel is off,
    1 if on,
    2 if on for a particle but off for an antiparticle,
    3 if on for an antiparticle but off for a particle.
    If a particle is its own antiparticle then 2 is on and 3 off but, of course, for such particles it is much simpler and safer to use only 1 and 0.
    The 2 and 3 options can be used e.g. to encode CP violation in B decays, or to let the W's in a q qbar -> W^+ W^- process decay in different channels.
    set or get the branching ratio of the channel. Second argument only for internal use. multiply the current branching ratio by fac. set or get the mode of processing this channel, possibly with matrix elements (see the particle decays and resonance decays descriptions). set or get the number of decay products in a channel, at most 8. (Is normally not to be set by hand, since it is automatically updated whenever the products list is changed.) set or get a list of the decay products, 8 products 0 <= i < 8, with trailing unused ones set to 0. used for internal purposes, to know which decay modes have been changed. find if the decay product list contains the one, two or three particle identities provided. If the same code is repeated then so must it be in the products list. Matching also requires correct sign. set or get the current branching ratio, taking into account on/off switches and dynamic width for resonances. For internal use. set or get the current partial width of the channel; intended for resonances where the widths are recalculated based on the current resonance mass. For internal use. multiply the current partial width by factor. set or get the fraction of secondary open widths, separately for positive and negative particles. For internal use.
    pythia8-8.1.80.orig/xmldoc/FourVectors.xml0000444000175000017500000003445412217346302016632 0ustar sunsun

    Four-Vectors

    The Vec4 class gives a simple implementation of four-vectors. The member function names are based on the assumption that these represent four-momentum vectors. Thus one can get or set p_x, p_y, p_z and e, but not x, y, z or t. This is only a matter of naming, however; a Vec4 can equally well be used to store a space-time four-vector.

    The Particle object contains a Vec4 p that stores the particle four-momentum, and another Vec4 vProd for the production vertex. For the latter the input/output method names are adapted to the space-time character rather than the normal energy-momentum one. Thus a user would not normally access the Vec4 classes directly, but only via the methods of the Particle class, see Particle Properties.

    Nevertheless you are free to use the PYTHIA four-vectors, e.g. as part of some simple analysis code based directly on the PYTHIA output, say to define the four-vector sum of a set of particles. But note that this class was never set up to allow complete generality, only to provide the operations that are of use inside PYTHIA. There is no separate class for three-vectors, since such can easily be represented by four-vectors where the fourth component is not used.

    Four-vectors have the expected functionality: they can be created, copied, added, multiplied, rotated, boosted, and manipulated in other ways. Operator overloading is implemented where reasonable. Properties can be read out, not only the components themselves but also for derived quantities such as absolute momentum and direction angles.

    Constructors and basic operators

    A few methods are available to create or copy a four-vector: creates a four-vector, by default with all components set to 0. creates a four-vector copy of the input four-vector. copies the input four-vector. gives a four-vector with all components set to value.

    Member methods for input

    The values stored in a four-vector can be modified in a few different ways: sets all components to 0. sets all components to their input values. sets all components equal to those of the input four-vector. sets the respective component to the input value.

    Member methods for output

    A number of methods provides output of basic or derived quantities: gets the respective component. the (squared) mass, calculated from the four-vectors. If m^2 < 0 the mass is given with a minus sign, -sqrt(-m^2). Note the possible loss of precision in the calculation of E^2 - p^2; for particles the correct mass is stored separately to avoid such problems. the (squared) transverse momentum. the (squared) absolute momentum. the (squared) transverse energy, eT = e * sin(theta) = e * pT / pAbs. the polar angle, in the range 0 through pi. the azimuthal angle, in the range -pi through pi. the angle in the xz plane, in the range -pi through pi, with 0 along the +z axis. the combinations E+-p_z. true rapidity y and pseudorapidity eta.

    Friend methods for output

    There are also some friend methods that take one, two or three four-vectors as argument. Several of them only use the three-vector part of the four-vector. writes out the values of the four components of a Vec4 and, within brackets, a fifth component being the invariant length of the four-vector, as provided by mCalc() above, and it all ended with a newline. the (squared) invariant mass. the three-product. the cross-product. the (cosine) of the opening angle between the vectors, in the range 0 through pi. the (cosine) of the azimuthal angle between the vectors around the z axis, in the range 0 through pi. the (cosine) of the azimuthal angle between the first two vectors around the direction of the third, in the range 0 through pi. the R distance measure, in (y, phi) or (eta, phi) cylindrical coordinates, i.e. R^2 = (y_1 - y_2)^2 + (phi_1 - phi_2)^2 and equivalent.

    Operations with four-vectors

    Of course one should be able to add, subtract and scale four-vectors, and more: return a vector with flipped sign for all components, while leaving the original vector unchanged. add a four-vector to an existing one. subtract a four-vector from an existing one. multiply all four-vector components by a real number. divide all four-vector components by a real number. add two four-vectors. subtract two four-vectors. multiply a four-vector by a real number. divide a four-vector by a real number. four-vector product.

    There are also a few related operations that are normal member methods: multiply the three-vector components by f, but keep the fourth component unchanged. multiply all four-vector components by f. flip the sign of the three-vector components, but keep the fourth component unchanged. flip the sign of all four-vector components.

    Rotations and boosts

    A common task is to rotate or boost four-vectors. In case only one four-vector is affected the operation may be performed directly on it. However, in case many particles are affected, the helper class RotBstMatrix can be used to speed up operations. rotate the three-momentum with the polar angle theta and the azimuthal angle phi. rotate the three-momentum with the azimuthal angle phi around the direction defined by the (n_x, n_y, n_z) three-vector. rotate the three-momentum with the azimuthal angle phi around the direction defined by the three-vector part of n. boost the four-momentum by beta = (beta_x, beta_y, beta_z). boost the four-momentum by beta = (beta_x, beta_y, beta_z), where the gamma = 1/sqrt(1 - beta^2) is also input to allow better precision when beta is close to unity. boost the four-momentum by beta = (p_x/E, p_y/E, p_z/E). boost the four-momentum by beta = (p_x/E, p_y/E, p_z/E), where the gamma = E/m is also calculated from input to allow better precision when beta is close to unity. boost the four-momentum by beta = (-p_x/E, -p_y/E, -p_z/E). boost the four-momentum by beta = (-p_x/E, -p_y/E, -p_z/E), where the gamma = E/m is also calculated from input to allow better precision when beta is close to unity. perform a combined rotation and boost; see below for a description of the RotBstMatrix.

    For a longer sequence of rotations and boosts, and where several Vec4 are to be rotated and boosted in the same way, a more efficient approach is to define a RotBstMatrix, which forms a separate auxiliary class. You can build up this 4-by-4 matrix by successive calls to the methods of the class, such that the matrix encodes the full sequence of operations. The order in which you do these calls must agree with the imagined order in which the rotations/boosts should be applied to a four-momentum, since in general the operations do not commute. creates a diagonal unit matrix, i.e. one that leaves a four-vector unchanged. creates a copy of the input matrix. copies the input matrix. rotate by this polar and azimuthal angle. rotate so that a vector originally along the +z axis becomes parallel with p. More specifically, rotate by -phi, theta and phi, with angles defined by p. boost by this beta vector. boost with a beta = p/E or beta = -p/E, respectively. boost so that p_1 is transformed to p_2. It is assumed that the two vectors obey p_1^2 = p_2^2. boost and rotate to the rest frame of p_1 and p_2, with p_1 along the +z axis. rotate and boost from the rest frame of p_1 and p_2, with p_1 along the +z axis, to the actual frame of p_1 and p_2, i.e. the inverse of the above. combine the current matrix with another one. invert the matrix, which corresponds to an opposite sequence and sign of rotations and boosts. reset to no rotation/boost; i.e. the default at creation. crude estimate how much a matrix deviates from the unit matrix: the sum of the absolute values of all non-diagonal matrix elements plus the sum of the absolute deviation of the diagonal matrix elements from unity. writes out the values of the sixteen components of a RotBstMatrix, on four consecutive lines and ended with a newline. pythia8-8.1.80.orig/xmldoc/pomH1JetsSinglet.data0000444000175000017500000034714412217346316017632 0ustar 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5.292930E-01 5.157822E-01 5.025489E-01 4.895899E-01 4.769018E-01 4.644815E-01 4.523260E-01 4.404325E-01 4.287985E-01 4.174213E-01 4.062989E-01 3.954292E-01 3.848102E-01 3.744404E-01 3.643184E-01 3.544432E-01 3.448138E-01 3.354297E-01 3.262907E-01 3.173968E-01 3.087482E-01 3.003459E-01 2.921908E-01 2.842844E-01 2.766285E-01 2.692252E-01 2.620770E-01 2.551869E-01 2.485583E-01 2.421946E-01 2.360998E-01 2.302781E-01 2.247340E-01 2.194719E-01 2.144964E-01 2.098120E-01 2.054229E-01 2.013327E-01 1.975447E-01 1.940607E-01 1.908815E-01 1.880059E-01 1.854305E-01 1.831487E-01 1.811503E-01 1.794204E-01 1.779385E-01 1.766768E-01 1.755993E-01 1.746594E-01 1.737984E-01 1.729425E-01 1.720005E-01 1.708602E-01 1.693844E-01 1.674073E-01 1.647287E-01 1.611092E-01 1.562640E-01 1.498573E-01 1.414968E-01 1.307312E-01 1.170536E-01 9.992231E-02 7.882832E-02 5.353126E-02 2.504557E-02 0.000000E+00 pythia8-8.1.80.orig/xmldoc/NNPDF23_nlo_as_0119_qed.grid0000444000175000017500000403757212217346312020357 0ustar sunsun 'Version' '5.8.9' 'Description:' 'NNPDF23_nlo_as_0119_qed.grid' 'NNPDF2.3QED NLO, arxiv:1308.0598' 'NLO QCD + LO QED PDF set, alphas(MZ)=0.119' 'NNPDF Collaboration: R.D. Ball, V. Bertone,' 'S. Carrazza, L. Del Debbio, S. Forte,' 'A. Guffanti, N.P. Hartland, J. Rojo' 'This set has 1 member PDF' 'mem=0 --> average on replicas.' 'Evolution: pol. interpolation on the LH grid.' 'Alphas:' 'Variable', 'nlo', 'EvolCode' 1 , 91.2 , 1.41421356237309515e+00 , 4.75000000000000000e+00 , 1.75000000000000000e+02 'MinMax:' 0 , 1 1.00000000000000006e-09 , 1.00000000000000000e+00 , 2.00000000000000000e+00 , 1.00000000000000000e+08 'QCDparams:' 0 , 1 3.42206534270809215e-01 , 2.38999999999999990e-01 'Parameterlist:' 'list', 0 , 1 0.11899999999999999 'Evolution:' 'nlo', 2.00000000000000000 , 1 , 5 'NNPDF20intqed' 0 , 1 100 1.00000000000000006e-09 1.45082877849593975e-09 2.10490414451202072e-09 3.05385550883341570e-09 4.43062145758388157e-09 6.42807311728432092e-09 9.32603346883219949e-09 1.35304777457980684e-08 1.96304065004027145e-08 2.84803586843580223e-08 4.13201240011533696e-08 5.99484250318940942e-08 8.69749002617783555e-08 1.26185688306602100e-07 1.83073828029536780e-07 2.65608778294668702e-07 3.85352859371053147e-07 5.59081018251222390e-07 8.11130830789687312e-07 1.17681195243499806e-06 1.70735264747069051e-06 2.47707635599171153e-06 3.59381366380462615e-06 5.21400828799968487e-06 7.56463327554629143e-06 1.09749876549305693e-05 1.59228279334109413e-05 2.31012970008315800e-05 3.35160265093884096e-05 4.86260158006535356e-05 7.05480231071864552e-05 1.02353102189902686e-04 1.48496826225446671e-04 2.15443469003188232e-04 3.12571584968823529e-04 4.53487850812858240e-04 6.57933224657568350e-04 9.54548456661834807e-04 1.38488637139387171e-03 2.00923300256504586e-03 2.91505306282517597e-03 4.22924287438949855e-03 6.13590727341317612e-03 8.90215085445039342e-03 1.29154966501488291e-02 1.87381742286038301e-02 2.71858824273294025e-02 3.94420605943765559e-02 5.72236765935022068e-02 8.16326530612244972e-02 1.00000000000000006e-01 1.18367346938775514e-01 1.36734693877551022e-01 1.55102040816326531e-01 1.73469387755102067e-01 1.91836734693877575e-01 2.10204081632653084e-01 2.28571428571428564e-01 2.46938775510204100e-01 2.65306122448979553e-01 2.83673469387755117e-01 3.02040816326530626e-01 3.20408163265306134e-01 3.38775510204081698e-01 3.57142857142857095e-01 3.75510204081632604e-01 3.93877551020408223e-01 4.12244897959183731e-01 4.30612244897959129e-01 4.48979591836734748e-01 4.67346938775510257e-01 4.85714285714285765e-01 5.04081632653061273e-01 5.22448979591836671e-01 5.40816326530612290e-01 5.59183673469387799e-01 5.77551020408163307e-01 5.95918367346938815e-01 6.14285714285714213e-01 6.32653061224489832e-01 6.51020408163265230e-01 6.69387755102040849e-01 6.87755102040816357e-01 7.06122448979591755e-01 7.24489795918367374e-01 7.42857142857142883e-01 7.61224489795918280e-01 7.79591836734693899e-01 7.97959183673469408e-01 8.16326530612244916e-01 8.34693877551020424e-01 8.53061224489795822e-01 8.71428571428571441e-01 8.89795918367346950e-01 9.08163265306122458e-01 9.26530612244897966e-01 9.44897959183673364e-01 9.63265306122449094e-01 9.81632653061224492e-01 1.00000000000000000e+00 50 2.00000000000000000e+00 2.00000000000000000e+00 2.87178440310906069e+00 4.12357282897023225e+00 5.92100606766051119e+00 8.50192643791078417e+00 1.22078498703863847e+01 1.75291564266362947e+01 2.51699790128365315e+01 3.61413765778231735e+01 5.18951207815418769e+01 7.45157992289464204e+01 1.06996655005447266e+02 1.53635662514742222e+02 2.20604249685582147e+02 3.16763921753315742e+02 4.54838844979415740e+02 6.53099550470012673e+02 9.37780551358661114e+02 1.34655178046540982e+03 1.93350320055964903e+03 2.77630216736432658e+03 3.98647063127737511e+03 5.72414209117735118e+03 8.21925098931160392e+03 1.18019583981718843e+04 1.69463400270060156e+04 2.43331174896693374e+04 3.49397336429263014e+04 5.01696910622703654e+04 7.20382681507140660e+04 1.03439187451104488e+05 1.48527522596178227e+05 2.13269511412066320e+05 3.06232028265931061e+05 4.39716181253277173e+05 6.31385035558919422e+05 9.06600848737282678e+05 1.30178108862458053e+06 1.86921731328720320e+06 2.68399456315980759e+06 3.85392686225592811e+06 5.53382352687481046e+06 7.94597404701851588e+06 1.14095621678685844e+07 1.63829013399941083e+07 2.35240802729348168e+07 3.37780434126498923e+07 4.85016291199942827e+07 6.96431110160899460e+07 1.00000000000000000e+08 0 0.0000000e+00 0.0000000e+00 3.9802768e-15 7.8675650e-01 1.0040492e+02 1.0040492e+02 9.7538076e+01 1.0040491e+02 1.0040491e+02 7.8675544e-01 3.9802768e-15 0.0000000e+00 0.0000000e+00 2.0905010e+00 0.0000000e+00 0.0000000e+00 3.8836657e+00 4.7482374e+00 1.0229158e+02 1.0229934e+02 2.0147784e+02 1.0229934e+02 1.0229158e+02 4.7482363e+00 3.8836657e+00 1.0243658e-14 0.0000000e+00 2.3181403e+00 0.0000000e+00 0.0000000e+00 8.4285956e+00 9.3617445e+00 1.0505544e+02 1.0507081e+02 3.1905224e+02 1.0507081e+02 1.0505544e+02 9.3617432e+00 8.4285956e+00 0.0000000e+00 0.0000000e+00 2.5074501e+00 0.0000000e+00 2.3320605e-15 1.3565249e+01 1.4559625e+01 1.0859235e+02 1.0861520e+02 4.5021081e+02 1.0861520e+02 1.0859235e+02 1.4559623e+01 1.3565249e+01 9.1926466e-16 0.0000000e+00 2.6973794e+00 0.0000000e+00 0.0000000e+00 1.9243862e+01 2.0293362e+01 1.1282050e+02 1.1285071e+02 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1.4102713e+02 1.4096161e+02 5.4304703e+01 5.3044352e+01 1.6851485e+01 0.0000000e+00 3.8500372e+00 0.0000000e+00 2.4894817e+01 6.0767913e+01 6.2061612e+01 1.4777267e+02 1.4784501e+02 1.7227208e+03 1.4784500e+02 1.4777267e+02 6.2061610e+01 6.0767913e+01 2.4894817e+01 0.0000000e+00 4.0444054e+00 0.0000000e+00 3.3370611e+01 6.8941803e+01 7.0266867e+01 1.5508318e+02 1.5516226e+02 1.9556553e+03 1.5516226e+02 1.5508319e+02 7.0266865e+01 6.8941803e+01 3.3370611e+01 0.0000000e+00 4.2394622e+00 0.0000000e+00 4.2276032e+01 7.7561431e+01 7.8916097e+01 1.6288385e+02 1.6296960e+02 2.2028917e+03 1.6296959e+02 1.6288385e+02 7.8916095e+01 7.7561431e+01 4.2276032e+01 0.0000000e+00 4.4352090e+00 0.0000000e+00 5.1608843e+01 8.6623037e+01 8.8005709e+01 1.7116696e+02 1.7125930e+02 2.4646374e+03 1.7125930e+02 1.7116696e+02 8.8005707e+01 8.6623037e+01 5.1608843e+01 0.0000000e+00 4.6316599e+00 0.0000000e+00 6.1367350e+01 9.6123621e+01 9.7532847e+01 1.7992589e+02 1.8002477e+02 2.7410900e+03 1.8002477e+02 1.7992589e+02 9.7532846e+01 9.6123621e+01 6.1367350e+01 0.0000000e+00 4.8288162e+00 0.0000000e+00 7.1550192e+01 1.0606065e+02 1.0749512e+02 1.8915501e+02 1.8926036e+02 3.0324310e+03 1.8926036e+02 1.8915501e+02 1.0749512e+02 1.0606065e+02 7.1550192e+01 0.0000000e+00 5.0266834e+00 0.0000000e+00 8.2156250e+01 1.1643200e+02 1.1789051e+02 1.9884943e+02 1.9896119e+02 3.3388263e+03 1.9896119e+02 1.9884943e+02 1.1789051e+02 1.1643200e+02 8.2156250e+01 0.0000000e+00 5.2252672e+00 0.0000000e+00 9.3184679e+01 1.2723593e+02 1.2871739e+02 2.0900501e+02 2.0912313e+02 3.6604285e+03 2.0912313e+02 2.0900501e+02 1.2871739e+02 1.2723593e+02 9.3184679e+01 0.0000000e+00 5.4245731e+00 0.0000000e+00 1.0463469e+02 1.3847086e+02 1.3997426e+02 2.1961798e+02 2.1974242e+02 3.9973709e+03 2.1974241e+02 2.1961799e+02 1.3997426e+02 1.3847086e+02 1.0463469e+02 0.0000000e+00 5.6246060e+00 0.0000000e+00 1.1650559e+02 1.5013537e+02 1.5165978e+02 2.3068502e+02 2.3081571e+02 4.3497707e+03 2.3081570e+02 2.3068502e+02 1.5165978e+02 1.5013537e+02 1.1650559e+02 0.0000000e+00 5.8253732e+00 0.0000000e+00 1.2879680e+02 1.6222827e+02 1.6377284e+02 2.4220318e+02 2.4234006e+02 4.7177305e+03 2.4234006e+02 2.4220318e+02 1.6377284e+02 1.6222827e+02 1.2879680e+02 0.0000000e+00 6.0268803e+00 0.0000000e+00 1.4150769e+02 1.7474836e+02 1.7631229e+02 2.5416969e+02 2.5431273e+02 5.1013350e+03 2.5431273e+02 2.5416970e+02 1.7631229e+02 1.7474836e+02 1.4150769e+02 0.0000000e+00 6.2291331e+00 0.0000000e+00 1.5463768e+02 1.8769454e+02 1.8927710e+02 2.6658207e+02 2.6673122e+02 5.5006538e+03 2.6673121e+02 2.6658207e+02 1.8927709e+02 1.8769454e+02 1.5463768e+02 0.0000000e+00 6.4321371e+00 0.0000000e+00 1.6818619e+02 2.0106578e+02 2.0266629e+02 2.7943805e+02 2.7959326e+02 5.9157441e+03 2.7959326e+02 2.7943805e+02 2.0266628e+02 2.0106578e+02 1.6818619e+02 0.0000000e+00 6.6358970e+00 0.0000000e+00 1.8215247e+02 2.1486088e+02 2.1647870e+02 2.9273518e+02 2.9289641e+02 6.3466413e+03 2.9289641e+02 2.9273518e+02 2.1647870e+02 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0.0000000e+00 0.0000000e+00 0.0000000e+00 'End:' pythia8-8.1.80.orig/xmldoc/HiggsProcesses.xml0000444000175000017500000010651112217346303017274 0ustar sunsun

    Higgs Processes

    This page documents Higgs production within and beyond the Standard Model (SM and BSM for short). This includes several different processes and, for the BSM scenarios, a large set of parameters that would only be fixed within a more specific framework such as MSSM. Three choices can be made irrespective of the particular model: The partial width of a Higgs particle to a pair of gauge bosons, W^+ W^- or Z^0 Z^0, depends cubically on the Higgs mass. When selecting the Higgs according to a Breit-Wigner, so that the actual mass mHat does not agree with the nominal m_Higgs one, an ambiguity arises which of the two to use Sey95. The default is to use a linear dependence on mHat, i.e. a width proportional to m_Higgs^2 * mHat, while on gives a mHat^3 dependence. This does not affect the widths to fermions, which only depend linearly on mHat. This flag is used both for SM and BSM Higgs bosons. The partial width of a Higgs particle to a pair of gluons or photons, or a gamma Z^0 pair, proceeds in part through quark loops, mainly b and t. There is some ambiguity what kind of masses to use. Default is running MSbar ones, but alternatively fixed pole masses are allowed (as was standard in PYTHIA 6), which typically gives a noticeably higher cross section for these channels. (For a decay to a pair of fermions, such as top, the running mass is used for couplings and the fixed one for phase space.) The Breit-Wigner shape of a Higgs is nontrivial, owing to the rapid width variation with the mass of a Higgs. This implies that a Higgs of low nominal mass may still acquire a non-negligible high-end tail. The validity of the calculation may be questioned in these wings. With this option on, the Higgs:wingsFac value is used to cut away the wings. Warning: with this option on, the allowed mass range is shrunk, but never widened. This can lead to inconsistencies if a run consists of several subruns with different Higgs masses. The id:mMin and id:mMax values should therefore be reset (e.g. to the defaults 50. and 0.) when id:m0 is changed. With Higgs:clipWings on, all Higgs masses which deviate from the nominal one by more than Higgs:wingsFac times the nominal width are forbidden. This is achieved by setting the mMin and mMax values of the Higgs states at initialization. These changes never allow a wider range than already set by the user, alternatively by the current default values, see warning above.

    Standard-Model Higgs, basic processes

    This section provides the standard set of processes that can be run together to provide a reasonably complete overview of possible production channels for a single SM Higgs. The main parameter is the choice of Higgs mass, which can be set in the normal ParticleData database; thereafter the properties within the SM are essentially fixed. Common switch for the group of Higgs production within the Standard Model. Scattering f fbar -> H^0, where f sums over available flavours except top. Related to the mass-dependent Higgs point coupling to fermions, so at hadron colliders the bottom contribution will dominate. Code 901. Scattering g g -> H^0 via loop contributions primarily from top. Code 902. Scattering gamma gamma -> H^0 via loop contributions primarily from top and W. Code 903. Scattering f fbar -> H^0 Z^0 via s-channel Z^0 exchange. Code 904. Scattering f fbar -> H^0 W^+- via s-channel W^+- exchange. Code 905. Scattering f f' -> H^0 f f' via Z^0 Z^0 fusion. Code 906. Scattering f_1 f_2 -> H^0 f_3 f_4 via W^+ W^- fusion. Code 907. Scattering g g -> H^0 t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 908. Scattering q qbar -> H^0 t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 909.

    Standard-Model Higgs, further processes

    A number of further production processes has been implemented, that are specializations of some of the above ones to the high-pT region. The sets therefore could not be used simultaneously without unphysical double-counting, as further explained below. They are not switched on by the HiggsSM:all flag, but have to be switched on for each separate process after due consideration.

    The first three processes in this section are related to the Higgs point coupling to fermions, and so primarily are of interest for b quarks. It is here useful to begin by reminding that a process like b bbar -> H^0 implies that a b/bbar is taken from each incoming hadron, leaving behind its respective antiparticle. The initial-state showers will then add one g -> b bbar branching on either side, so that effectively the process becomes g g -> H0 b bbar. This would be the same basic process as the g g -> H^0 t tbar one used for top. The difference is that (a) no PDF's are defined for top and (b) the shower approach would not be good enough to provide sensible kinematics for the H^0 t tbar subsystem. By contrast, owing to the b being much lighter than the Higgs, multiple gluon emissions must be resummed for b, as is done by PDF's and showers, in order to obtain a sensible description of the total production rate, when the b quarks predominantly are produced at small pT values. Scattering q g -> H^0 q. This process gives first-order corrections to the f fbar -> H^0 one above, and should only be used to study the high-pT tail, while f fbar -> H^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> H^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 911. Scattering g g -> H^0 b bbar. This process is yet one order higher of the b bbar -> H^0 and b g -> H^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 912. Scattering q qbar -> H^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 913.

    The second set of processes are predominantly first-order corrections to the g g -> H^0 process, again dominated by the top loop. We here only provide the kinematical expressions obtained in the limit that the top quark goes to infinity, but scaled to the finite-top-mass coupling in g g -> H^0. (Complete loop expressions are available e.g. in PYTHIA 6.4 but are very lengthy.) This provides a reasonably accurate description for "intermediate" pT values, but fails when the pT scale approaches the top mass. Scattering g g -> H^0 g via loop contributions primarily from top. Code 914. Scattering q g -> H^0 q via loop contributions primarily from top. Not to be confused with the HiggsSM:qg2Hq process above, with its direct fermion-to-Higgs coupling. Code 915. Scattering q qbar -> H^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> H^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 916.

    Beyond-the-Standard-Model Higgs, introduction

    Further Higgs multiplets arise in a number of scenarios. We here concentrate on the MSSM scenario with two Higgs doublets, but with flexibility enough that also other two-Higgs-doublet scenarios could be represented by a suitable choice of parameters. Conventionally the Higgs states are labeled h^0, H^0, A^0 and H^+-. If the scalar and pseudocalar states mix the resulting states are labeled H_1^0, H_2^0, H_3^0. In process names and parameter explanations both notations will be used, but for settings labels we have adapted the shorthand hybrid notation H1 for h^0(H_1^0), H2 for H^0(H_2^0) and A3 for A^0(H_3^0). (Recall that the Settings database does not distinguish upper- and lowercase characters, so that the user has one thing less to worry about, but here it causes problems with h^0 vs. H^0.) We leave the issue of mass ordering between H^0 and A^0 open, and thereby also that of H_2^0 and H_3^0. Master switch to initialize and use the two-Higgs-doublet states. If off, only the above SM Higgs processes can be used, with couplings as predicted in the SM. If on, only the below BSM Higgs processes can be used, with couplings that can be set freely, also found further down on this page.

    Beyond-the-Standard-Model Higgs, basic processes

    This section provides the standard set of processes that can be run together to provide a reasonably complete overview of possible production channels for a single neutral Higgs state in a two-doublet scenarios such as MSSM. The list of processes for neutral states closely mimics the one found for the SM Higgs. Some of the processes vanish for a pure pseudoscalar A^0, but are kept for flexibility in cases of mixing with the scalar h^0 and H^0 states, or for use in the context of non-MSSM models. This should work well to represent e.g. that a small admixture of the "wrong" parity would allow a process such as q qbar -> A^0 Z^0, which otherwise is forbidden. However, note that the loop integrals e.g. for g g -> h^0/H^0/A^0 are hardcoded to be for scalars for the former two particles and for a pseudoscalar for the latter one, so absolute rates would not be correctly represented in the case of large scalar/pseudoscalar mixing. Common switch for the group of Higgs production beyond the Standard Model, as listed below.

    1) h^0(H_1^0) processes

    Common switch for the group of h^0(H_1^0) production processes. Scattering f fbar -> h^0(H_1^0), where f sums over available flavours except top. Code 1001. Scattering g g -> h^0(H_1^0) via loop contributions primarily from top. Code 1002. Scattering gamma gamma -> h^0(H_1^0) via loop contributions primarily from top and W. Code 1003. Scattering f fbar -> h^0(H_1^0) Z^0 via s-channel Z^0 exchange. Code 1004. Scattering f fbar -> h^0(H_1^0) W^+- via s-channel W^+- exchange. Code 1005. Scattering f f' -> h^0(H_1^0) f f' via Z^0 Z^0 fusion. Code 1006. Scattering f_1 f_2 -> h^0(H_1^0) f_3 f_4 via W^+ W^- fusion. Code 1007. Scattering g g -> h^0(H_1^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1008. Scattering q qbar -> h^0(H_1^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1009.

    2) H^0(H_2^0) processes

    Common switch for the group of H^0(H_2^0) production processes. Scattering f fbar -> H^0(H_2^0), where f sums over available flavours except top. Code 1021. Scattering g g -> H^0(H_2^0) via loop contributions primarily from top. Code 1022. Scattering gamma gamma -> H^0(H_2^0) via loop contributions primarily from top and W. Code 1023. Scattering f fbar -> H^0(H_2^0) Z^0 via s-channel Z^0 exchange. Code 1024. Scattering f fbar -> H^0(H_2^0) W^+- via s-channel W^+- exchange. Code 1025. Scattering f f' -> H^0(H_2^0) f f' via Z^0 Z^0 fusion. Code 1026. Scattering f_1 f_2 -> H^0(H_2^0) f_3 f_4 via W^+ W^- fusion. Code 1027. Scattering g g -> H^0(H_2^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1028. Scattering q qbar -> H^0(H_2^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1029.

    3) A^0(H_3^0) processes

    Common switch for the group of A^0(H_3^0) production processes. Scattering f fbar -> A^0(H_3^0), where f sums over available flavours except top. Code 1041. Scattering g g -> A^0(A_3^0) via loop contributions primarily from top. Code 1042. Scattering gamma gamma -> A^0(A_3^0) via loop contributions primarily from top and W. Code 1043. Scattering f fbar -> A^0(A_3^0) Z^0 via s-channel Z^0 exchange. Code 1044. Scattering f fbar -> A^0(A_3^0) W^+- via s-channel W^+- exchange. Code 1045. Scattering f f' -> A^0(A_3^0) f f' via Z^0 Z^0 fusion. Code 1046. Scattering f_1 f_2 -> A^0(A_3^0) f_3 f_4 via W^+ W^- fusion. Code 1047. Scattering g g -> A^0(A_3^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1048. Scattering q qbar -> A^0(A_3^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1049.

    4) H+- processes

    Common switch for the group of H^+- production processes. Scattering f fbar' -> H^+-, where f, fbar' sums over available incoming flavours. Since couplings are assumed generation-diagonal, in practice this means c sbar -> H^+ and s cbar -> H^-. Code 1061. Scattering b g -> H^+ tbar. At hadron colliders this is the dominant process for single-charged-Higgs production. Code 1062.

    5) Higgs-pair processes

    Common switch for the group of Higgs pair-production processes. Scattering f fbar -> A^0(H_3) h^0(H_1). Code 1081. Scattering f fbar -> A^0(H_3) H^0(H_2). Code 1082. Scattering f fbar -> H^+- h^0(H_1). Code 1083. Scattering f fbar -> H^+- H^0(H_2). Code 1084. Scattering f fbar -> H+ H-. Code 1085.

    Beyond-the-Standard-Model Higgs, further processes

    This section mimics the above section on "Standard-Model Higgs, further processes", i.e. it contains higher-order corrections to the processes already listed. The two sets therefore could not be used simultaneously without unphysical double-counting. They are not controlled by any group flag, but have to be switched on for each separate process after due consideration. We refer to the standard-model description for a set of further comments on the processes.

    1) h^0(H_1^0) processes

    Scattering q g -> h^0 q. This process gives first-order corrections to the f fbar -> h^0 one above, and should only be used to study the high-pT tail, while f fbar -> h^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> h^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 1011. Scattering g g -> h^0 b bbar. This process is yet one order higher of the b bbar -> h^0 and b g -> h^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1012. Scattering q qbar -> h^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1013. Scattering g g -> h^0 g via loop contributions primarily from top. Code 1014. Scattering q g -> h^0 q via loop contributions primarily from top. Not to be confused with the HiggsBSM:qg2H1q process above, with its direct fermion-to-Higgs coupling. Code 1015. Scattering q qbar -> h^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> h^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 1016.

    2) H^0(H_2^0) processes

    Scattering q g -> H^0 q. This process gives first-order corrections to the f fbar -> H^0 one above, and should only be used to study the high-pT tail, while f fbar -> H^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> H^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 1031. Scattering g g -> H^0 b bbar. This process is yet one order higher of the b bbar -> H^0 and b g -> H^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1032. Scattering q qbar -> H^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1033. Scattering g g -> H^0 g via loop contributions primarily from top. Code 1034. Scattering q g -> H^0 q via loop contributions primarily from top. Not to be confused with the HiggsBSM:qg2H1q process above, with its direct fermion-to-Higgs coupling. Code 1035. Scattering q qbar -> H^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> H^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 1036.

    3) A^0(H_3^0) processes

    Scattering q g -> A^0 q. This process gives first-order corrections to the f fbar -> A^0 one above, and should only be used to study the high-pT tail, while f fbar -> A^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> A^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 1051. Scattering g g -> A^0 b bbar. This process is yet one order higher of the b bbar -> A^0 and b g -> A^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1052. Scattering q qbar -> A^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1053. Scattering g g -> A^0 g via loop contributions primarily from top. Code 1054. Scattering q g -> A^0 q via loop contributions primarily from top. Not to be confused with the HiggsBSM:qg2H1q process above, with its direct fermion-to-Higgs coupling. Code 1055. Scattering q qbar -> A^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> A^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 1056.

    Parameters for Beyond-the-Standard-Model Higgs production and decay

    This section offers a big flexibility to set couplings of the various Higgs states to fermions and gauge bosons, and also to each other. The intention is that, for scenarios like MSSM, you should use standard input from the SUSY Les Houches Accord, rather than having to set it all yourself. In other cases, however, the freedom is there for you to use. Kindly note that some of the internal calculations of partial widths from the parameters provided do not include mixing between the scalar and pseudoscalar states.

    Masses would be set in the ParticleData database, while couplings are set below. When possible, the couplings of the Higgs states are normalized to the corresponding coupling within the SM. When not, their values within the MSSM are indicated, from which it should be straightforward to understand what to use instead. The exception is some couplings that vanish also in the MSSM, where the normalization has been defined in close analogy with nonvanishing ones. Some parameter names are asymmetric but crossing can always be used, i.e. the coupling for A^0 -> H^0 Z^0 obviously is also valid for H^0 -> A^0 Z^0 and Z^0 -> H^0 A^0. Note that couplings usually appear quadratically in matrix elements. The h^0(H_1^0) coupling to down-type quarks. The h^0(H_1^0) coupling to up-type quarks. The h^0(H_1^0) coupling to (charged) leptons. The h^0(H_1^0) coupling to Z^0. The h^0(H_1^0) coupling to W^+-. The h^0(H_1^0) coupling to H^+- (in loops). Is sin(beta - alpha) + cos(2 beta) sin(beta + alpha) / (2 cos^2theta_W) in the MSSM. The H^0(H_2^0) coupling to down-type quarks. The H^0(H_2^0) coupling to up-type quarks. The H^0(H_2^0) coupling to (charged) leptons. The H^0(H_2^0) coupling to Z^0. The H^0(H_2^0) coupling to W^+-. The H^0(H_2^0) coupling to H^+- (in loops). Is cos(beta - alpha) + cos(2 beta) cos(beta + alpha) / (2 cos^2theta_W) in the MSSM. The H^0(H_2^0) coupling to a h^0(H_1^0) pair. Is cos(2 alpha) cos(beta + alpha) - 2 sin(2 alpha) sin(beta + alpha) in the MSSM. The H^0(H_2^0) coupling to an A^0(H_3^0) pair. Is cos(2 beta) cos(beta + alpha) in the MSSM. The H^0(H_2^0) coupling to a h^0(H_1^0) Z^0 pair. Vanishes in the MSSM. The H^0(H_2^0) coupling to an A^0(H_3^0) h^0(H_1^0) pair. Vanishes in the MSSM. The H^0(H_2^0) coupling to a H^+- W-+ pair. Is sin(beta - alpha) in the MSSM. The A^0(H_3^0) coupling to down-type quarks. The A^0(H_3^0) coupling to up-type quarks. The A^0(H_3^0) coupling to (charged) leptons. The A^0(H_3^0) coupling to a h^0(H_1^0) Z^0 pair. Is cos(beta - alpha) in the MSSM. The A^0(H_3^0) coupling to a H^0(H_2^0) Z^0 pair. Is sin(beta - alpha) in the MSSM. The A^0(H_3^0) coupling to Z^0. Vanishes in the MSSM. The A^0(H_3^0) coupling to W^+-. Vanishes in the MSSM. The A^0(H_3^0) coupling to a h^0(H_1^0) pair. Vanishes in the MSSM. The A^0(H_3^0) coupling to H^+-. Vanishes in the MSSM. The A^0(H_3^0) coupling to a H^+- W-+ pair. Is 1 in the MSSM. The tan(beta) value, which leads to an enhancement of the H^+- coupling to down-type fermions and suppression to up-type ones. The same angle also appears in many other places, but this particular parameter is only used for the charged-Higgs case. The H^+- coupling to a h^0(H_1^0) W^+- pair. Is cos(beta - alpha) in the MSSM. The H^+- coupling to a H^0(H_2^0) W^+- pair. Is sin(beta - alpha) in the MSSM.

    Another set of parameters are not used in the production stage but exclusively for the description of angular distributions in decays. possibility to modify angular decay correlations in the decay of a h^0(H_1) decay Z^0 Z^0 or W^+ W^- to four fermions. Currently it does not affect the partial width of the channels, which is only based on the above parameters. The eta value of CP-violation in the HiggsSM:parity = 3 option. possibility to modify angular decay correlations in the decay of a H^0(H_2) decay Z^0 Z^0 or W^+ W^- to four fermions. Currently it does not affect the partial width of the channels, which is only based on the above parameters. The eta value of CP-violation in the HiggsSM:parity = 3 option. possibility to modify angular decay correlations in the decay of a A^0(H_3) decay Z^0 Z^0 or W^+ W^- to four fermions. Currently it does not affect the partial width of the channels, which is only based on the above parameters. The eta value of CP-violation in the HiggsSM:parity = 3 option. pythia8-8.1.80.orig/xmldoc/ASecondHardProcess.xml0000444000175000017500000004433312217346277020033 0ustar sunsun

    A Second Hard Process

    When you have selected a set of hard processes for hadron beams, the multiparton interactions framework can add further interactions to build up a realistic underlying event. These further interactions can come from a wide variety of processes, and will occasionally be quite hard. They do represent a realistic random mix, however, which means one cannot predetermine what will happen. Occasionally there may be cases where one wants to specify also the second hard interaction rather precisely. The options on this page allow you to do precisely that. Generate two hard scatterings in a collision between hadron beams. The hardest process can be any combination of internal processes, available in the normal process selection machinery, or external input. Here you must further specify which set of processes to allow for the second hard one, see the following.

    Process Selection

    In principle the whole process selection allowed for the first process could be repeated for the second one. However, this would probably be overkill. Therefore here a more limited set of prepackaged process collections are made available, that can then be further combined at will. Since the description is almost completely symmetric between the first and the second process, you always have the possibility to pick one of the two processes according to the complete list of possibilities.

    Here comes the list of allowed sets of processes, to combine at will: Standard QCD 2 -> 2 processes involving gluons and d, u, s, c, b quarks. A prompt photon recoiling against a quark or gluon jet. Two prompt photons recoiling against each other. Production of charmonium via colour singlet and colour octet channels. Production of bottomonium via colour singlet and colour octet channels. Scattering q qbar -> gamma^*/Z^0, with full interference between the gamma^* and Z^0. Scattering q qbar' -> W^+-. Scattering q qbar -> gamma^*/Z^0 g and q g -> gamma^*/Z^0 q. Scattering q qbar' -> W^+- g and q g -> W^+- q'. Production of a top pair, either via QCD processes or via an intermediate gamma^*/Z^0 resonance. Production of a single top, either via a t- or an s-channel W^+- resonance.

    A further process collection comes with a warning flag: The q qbar -> b bbar and g g -> b bbar processes. These are already included in the TwoJets sample above, so it would be double-counting to include both, but we assume there may be cases where the b subsample will be of special interest. This subsample does not include flavour-excitation or gluon-splitting contributions to the b rate, however, so, depending on the topology if interest, it may or may not be a good approximation.

    Cuts and scales

    The second hard process obeys exactly the same selection rules for phase space cuts and couplings and scales as the first one does. Specifically, a pTmin cut for 2 -> 2 processes would apply to the first and the second hard process alike, and ballpark half of the time the second could be generated with a larger pT than the first. (Exact numbers depending on the relative shape of the two cross sections.) That is, first and second is only used as an administrative distinction between the two, not as a physics ordering one.

    Optionally it is possible to pick the mass and pT phase space cuts separately for the second hard interaction. The main application presumably would be to allow a second process that is softer than the first, but still hard. But one is also free to make the second process harder than the first, if desired. So long as the two pT (or mass) ranges overlap the ordering will not be the same in all events, however.

    Cross-section calculation

    As an introduction, a brief reminder of Poissonian statistics. Assume a stochastic process in time, for now not necessarily a high-energy physics one, where the probability for an event to occur at any given time is independent of what happens at other times. Then the probability for n events to occur in a finite time interval is P_n = <n>^n exp(-<n>) / n! where <n> is the average number of events. If this number is small we can approximate exp(-<n>) = 1 , so that P_1 = <n> and P_2 = <n>^2 / 2 = P_1^2 / 2.

    Now further assume that the events actually are of two different kinds a and b, occurring independently of each other, such that <n> = <n_a> + <n_b>. It then follows that the probability of having one event of type a (or b) and nothing else is P_1a = <n_a> (or P_1b = <n_b>). From P_2 = (<n_a> + <n_b>)^2 / 2 = (P_1a + P_1b)^2 / 2 = (P_1a^2 + 2 P_1a P_1b + P_1b^2) / 2 it is easy to read off that the probability to have exactly two events of kind a and none of b is P_2aa = P_1a^2 / 2 whereas that of having one a and one b is P_2ab = P_1a P_1b. Note that the former, with two identical events, contains a factor 1/2 while the latter, with two different ones, does not. If viewed in a time-ordered sense, the difference is that the latter can be obtained two ways, either first an a and then a b or else first a b and then an a.

    To translate this language into cross-sections for high-energy events, we assume that interactions can occur at different pT values independently of each other inside inelastic nondiffractive (sometimes equated with "minbias") events. Then the above probabilities translate into P_n = sigma_n / sigma_ND where sigma_ND is the total nondiffractive cross section. Again we want to assume that exp(-<n>) is close to unity, i.e. that the total hard cross section above pTmin is much smaller than sigma_ND. The hard cross section is dominated by QCD jet production, and a reasonable precaution is to require a pTmin of at least 20 GeV at LHC energies. (For 2 -> 1 processes such as q qbar -> gamma^*/Z^0 (-> f fbar) one can instead make a similar cut on mass.) Then the generic equation P_2 = P_1^2 / 2 translates into sigma_2/sigma_ND = (sigma_1 / sigma_ND)^2 / 2 or sigma_2 = sigma_1^2 / (2 sigma_ND).

    Again different processes a, b, c, ... contribute, and by the same reasoning we obtain sigma_2aa = sigma_1a^2 / (2 sigma_ND), sigma_2ab = sigma_1a sigma_1b / sigma_ND, and so on.

    There is one important correction to this picture: all collisions do no occur under equal conditions. Some are more central in impact parameter, others more peripheral. This leads to a further element of variability: central collisions are likely to have more activity than the average, peripheral less. Integrated over impact parameter standard cross sections are recovered, but correlations are affected by a "trigger bias" effect: if you select for events with a hard process you favour events at small impact parameter which have above-average activity, and therefore also increased chance for further interactions. (In PYTHIA this is the origin of the "pedestal effect", i.e. that events with a hard interaction have more underlying activity than the level found in minimum-bias events.) When you specify a matter overlap profile in the multiparton-interactions scenario, such an enhancement/depletion factor f_impact is chosen event-by-event and can be averaged during the course of the run. As an example, the double Gaussian form used in Tune A gives approximately <f_impact> = 2.5. The above equations therefore have to be modified to sigma_2aa = <f_impact> sigma_1a^2 / (2 sigma_ND), sigma_2ab = <f_impact> sigma_1a sigma_1b / sigma_ND. Experimentalists often instead use the notation sigma_2ab = sigma_1a sigma_1b / sigma_eff, from which we see that PYTHIA "predicts" sigma_eff = sigma_ND / <f_impact>. When the generation of multiparton interactions is switched off it is not possible to calculate <f_impact> and therefore it is set to unity.

    When this recipe is to be applied to calculate actual cross sections, it is useful to distinguish three cases, depending on which set of processes are selected to study for the first and second interaction.

    (1) The processes a for the first interaction and b for the second one have no overlap at all. For instance, the first could be TwoJets and the second TwoPhotons. In that case, the two interactions can be selected independently, and cross sections tabulated for each separate subprocess in the two above classes. At the end of the run, the cross sections in a should be multiplied by <f_impact> sigma_1b / sigma_ND to bring them to the correct overall level, and those in b by <f_impact> sigma_1a / sigma_ND.

    (2) Exactly the same processes a are selected for the first and second interaction. In that case it works as above, with a = b, and it is only necessary to multiply by an additional factor 1/2. A compensating factor of 2 is automatically obtained for picking two different subprocesses, e.g. if TwoJets is selected for both interactions, then the combination of the two subprocesses q qbar -> g g and g g -> g g can trivially be obtained two ways.

    (3) The list of subprocesses partly but not completely overlap. For instance, the first process is allowed to contain a or c and the second b or c, where there is no overlap between a and b. Then, when an independent selection for the first and second interaction both pick one of the subprocesses in c, half of those events have to be thrown, and the stored cross section reduced accordingly. Considering the four possible combinations of first and second process, this gives a sigma'_1 = sigma_1a + sigma_1c * (sigma_2b + sigma_2c/2) / (sigma_2b + sigma_2c) with the factor 1/2 for the sigma_1c sigma_2c term. At the end of the day, this sigma'_1 should be multiplied by the normalization factor f_1norm = <f_impact> (sigma_2b + sigma_2c) / sigma_ND here without a factor 1/2 (or else it would have been double-counted). This gives the correct (sigma_2b + sigma_2c) * sigma'_1 = sigma_1a * sigma_2b + sigma_1a * sigma_2c + sigma_1c * sigma_2b + sigma_1c * sigma_2c/2 The second interaction can be handled in exact analogy.

    For the considerations above it is assumed that the phase space cuts are the same for the two processes. It is possible to set the mass and transverse momentum cuts differently, however. This changes nothing for processes that already are different. For two collisions of the same type it is partly a matter of interpretation what is intended. If we consider the case of the same process in two non-overlapping phase space regions, most likely we want to consider them as separate processes, in the sense that we expect a factor 2 relative to Poissonian statistics from either of the two hardest processes populating either of the two phase space regions. In total we are therefore lead to adopt the same strategy as in case (3) above: only in the overlapping part of the two allowed phase space regions could two processes be identical and thus appear with a 1/2 factor, elsewhere the two processes are never identical and do not include the 1/2 factor. We reiterate, however, that the case of partly but not completely overlapping phase space regions for one and the same process is tricky, and not to be used without prior deliberation.

    The listing obtained with the pythia.statistics() already contain these corrections factors, i.e. cross sections are for the occurrence of two interactions of the specified kinds. There is not a full tabulation of the matrix of all the possible combinations of a specific first process together with a specific second one (but the information is there for the user to do that, if desired). Instead pythia.statistics() shows this matrix projected onto the set of processes and associated cross sections for the first and the second interaction, respectively. Up to statistical fluctuations, these two sections of the pythia.statistics() listing both add up to the same total cross section for the event sample.

    There is a further special feature to be noted for this listing, and that is the difference between the number of "selected" events and the number of "accepted" ones. Here is how that comes about. Originally the first and second process are selected completely independently. The generation (in)efficiency is reflected in the different number of initially tried events for the first and second process, leading to the same number of selected events. While acceptable on their own, the combination of the two processes may be unacceptable, however. It may be that the two processes added together use more energy-momentum than kinematically allowed, or, even if not, are disfavoured when the PYTHIA approach to provide correlated parton densities is applied. Alternatively, referring to case (3) above, it may be because half of the events should be thrown for identical processes. Taken together, it is these effects that reduced the event number from "selected" to "accepted". (A further reduction may occur if a user hook rejects some events.)

    It is allowed to use external Les Houches Accord input for the hardest process, and then pick an internal one for the second hardest. In this case PYTHIA does not have access to your thinking concerning the external process, and cannot know whether it overlaps with the internal or not. (External events q qbar' -> e+ nu_e could agree with the internal W ones, or be a W' resonance in a BSM scenario, to give one example.) Therefore the combined cross section is always based on the scenario (1) above. Corrections for correlated parton densities are included also in this case, however. That is, an external event that takes a large fraction of the incoming beam momenta stands a fair chance of being rejected when it has to be combined with another hard process. For this reason the "selected" and "accepted" event numbers are likely to disagree.

    In the cross section calculation above, the sigma'_1 cross sections are based on the number of accepted events, while the f_1norm factor is evaluated based on the cross sections for selected events. That way the suppression by correlations between the two processes does not get to be double-counted.

    The pythia.statistics() listing contains two final lines, indicating the summed cross sections sigma_1sum and sigma_2sum for the first and second set of processes, at the "selected" stage above, plus information on the sigma_ND and <f_impact> used. The total cross section generated is related to this by <f_impact> * (sigma_1sum * sigma_2sum / sigma_ND) * (n_accepted / n_selected) with an additional factor of 1/2 for case 2 above.

    The error quoted for the cross section of a process is a combination in quadrature of the error on this process alone with the error on the normalization factor, including the error on <f_impact>. As always it is a purely statistical one and of course hides considerably bigger systematic uncertainties.

    Event information

    Normally the process event record only contains the hardest interaction, but in this case also the second hardest is stored there. If both of them are 2 -> 2 ones, the first would be stored in lines 3 - 6 and the second in 7 - 10. For both, status codes 21 - 29 would be used, as for a hardest process. Any resonance decay chains would occur after the two main processes, to allow normal parsing. The beams in 1 and 2 only appear in one copy. This structure is echoed in the full event event record.

    Most of the properties accessible by the pythia.info methods refer to the first process, whether that happens to be the hardest or not. The code and pT scale of the second process are accessible by the info.codeMPI(1) and info.pTMPI(1), however.

    The sigmaGen() and sigmaErr() methods provide the cross section and its error for the event sample as a whole, combining the information from the two hard processes as described above. In particular, the former should be used to give the weight of the generated event sample. The statistical error estimate is somewhat cruder and gives a larger value than the subprocess-by-subprocess one employed in pythia.statistics(), but this number is anyway less relevant, since systematical errors are likely to dominate. pythia8-8.1.80.orig/xmldoc/JetFinders.xml0000444000175000017500000000457612217346303016411 0ustar sunsun

    Jet Finders

    Pythia comes with three built-in jet finders, ClusterJet for e^+e^- events and SlowJet and CellJetfor hadron collider ones. Especially the latter is not so well matched to the standards of its field, however. (But it is closely related to the anti-kT algorithm, so is also not completely disconnected Cac08.)

    SlowJet can do jet finding according to the current-day kT, Cambridge/Aachen and anti-kT algorithms. It can be run in two modes. The original one is a native implementation which, as the name indicates, is rather slow. However, with the release of the fjcore code from FastJet Cac06, Cac12, the default mode has become to use the fjcore methods. This is transparent to the user.

    FastJet

    SlowJet does not exhaust all the posssibilities of the fjcore code, so users are welcome to extend on the existing functionality by a direct usage of the fjcore methods.

    Missing from fjcore is a number of aspects, such as jet areas functionality, background estimation, access to other algorithms via plugins, interface to CGAL and tools such as filters and taggers. Therefore, for more sophisticated jet studies the complete FastJet package needs to be linked. This is foreseen in the configure file in the examples subdirectory, and the main71.cc and main72.cc programs contain examples how it can be used with Pythia events. (Even if these examples do not go beyond the functionality that SlowJet can offer.)

    The latter program makes use of the include/Pythia8/FastJet3.h header file, contributed by Gavin Salam. This allows simple input of a Pythia particle into a FastJet one, either retaining only the four-momentum or the full particle information. Thereby more sophisticated selectors become possible at the FastJet level. This code could be duplicated, with trivial modifications, to augment the fjcore package functionality in an identical manner, should the need arise. pythia8-8.1.80.orig/xmldoc/AlpgenEventInterface.xml0000444000175000017500000002631312217346277020410 0ustar sunsun

    ALPGEN Event Interface

    This manual page describes the ALPGEN Man03 event interface for PYTHIA8. While future versions of ALPGEN will be able to write out events in LHEF format, previous versions always output events in an ALPGEN native format (a combination of a ".unw" and a "_unw.par" file). The ALPGEN component of this code contains a reader for this native format (for unweighted events), as well as parameter reading for both ALPGEN native and LHE file formats. The reader was designed to work together with an implementation of the ALPGEN-style parton-jet matching JetMatchingAlpgen described on the Jet Matching page. However, it will also work with a implementation of the Madgraph-style Alw11 parton-jet matching JetMatchingMadgraph also described on the Jet Matching page. A sensible choice of JetMatching parameters is needed when using ALPGEN files with Madgraph-style matching and vice versa.

    It should be noted that all the functionality described here is provided through external routines, and therefore the presence of these features is dependent on the main program being used. This structure allows for the easy extensibility of the merging scheme. The files of interest are located in the examples/ subdirectory:

    • GeneratorInput.h : provides three classes for the reading of ALPGEN event and parameter files. LHAupAlpgen is an LHAup derived class for reading in ALPGEN native format event files. AlpgenPar is a class for the parsing of ALPGEN parameter files, making the information available through a simple interface. AlpgenHooks is a UserHooks derived class that provides the Alpgen:* options, described below. Further technical details of these classes are given at the end of this manual page.
    • main32.cc, main32.cmnd : a sample main program and card file showing the usage of previous file and an MLM UserHooks class. In combination, it reads in a sample ALPGEN (or Madgraph) event file while performing the MLM merging procedure as implemented in ALPGEN (or as in Madgraph). Some commented-out sets of options are provided in the card file, which can be activated to try different merging setups.
    • main32.unw, main32_unw.par : an ALPGEN format event and parameter file containing 100 W + 3 jet events. It is not feasible to package large event files with the PYTHIA distribution, but this sample is enough to show the different components in action.

    ALPGEN main options

    These following options are provided by the AlpgenHooks class, which must be loaded for this functionality to be present

    ALPGEN event files that have been written out in LHEF format should be read in through the normal LHEF machinery (see Beam Parameters). Files in ALPGEN's native format, instead, may be processed using the Alpgen:file option below. When using this option, the ALPGEN parameter file is stored in the PYTHIA Info object under the key AlpgenPar, see the "Header information" section of the Event Information manual page for more details. Processes not implemented by the PYTHIA 6 interface supplied with ALPGEN are also not implemented here.

    When reading in ALPGEN native event files, some momenta are shifted by the file reader to ensure energy-momentum conservation. The magnitude of these shifts should be small (around the MeV level in the worst case) and warnings will be produced if they are above a set threshold. A large number of warnings may signify unexpected behaviour and should potentially be investigated. It is also known that certain event classes, for example an event with both light and heavy b quarks may give rise to these warnings.

    The ALPGEN file reader supports the reading of the event and parameter files in gzip format with file extensions ".unw.gz" and "_unw.par.gz" respectively. This requires the use of external libraries, however, and the README file in the main directory contains instructions on how to enable this.

    All other Alpgen:* options apply to both LHE and native file formats, and include options to guide the MLM merging procedure based on the parameters that are read in with the events file. This option is used to read in ALPGEN format event files. Using this option overrides any previously set beam options inside PYTHIA. The path to the files, not including any file extension, should be provided e.g. for input files input_unw.par and input.unw, the value input should be used. When switched on, any particle masses provided by ALPGEN are set in the PYTHIA particle database. When switched on, the merging parameters (see below) are set according to the ALPGEN hard process cuts:

    • JetMatching:eTjetMin = min(ptjmin + 5., 1.2 * ptjmin),
    • JetMatching:coneRadius = drjmin,
    • JetMatching:etaJetMax = etajmax.
    where the ptjmin, drjmin and etajmax are the incoming ALPGEN parameters. Note that any existing values of these parameters are overwritten.
    When switched on, the JetMatching:nJet parameter (see below) is set to the incoming njet ALPGEN parameter. Note that any existing value of this parameter is overwritten.

    Class information

    Some more technical information about the different classes is given below. For clarity, some limited information on certain private methods is provided.

    LHAupAlpgen

    This class is derived from the LHAup base class, and uses the standard machinery to pass initialisation and event data to PYTHIA. These standard functions are not documented here. The complete parameter file is stored in the PYTHIA Info object, if given, under the key AlpgenPar. The constructor for the class takes the base filename for the ALPGEN format files (without file extensions) and optionally a pointer to a PYTHIA Info class, used for warning/error message printing and for storing the ALPGEN parameter file. The event and parameter files are opened immediately, with the AlpgenPar class, described below, used to parse the parameter file. This is a private method used when an event is read in. The information read from the event file does not always contain a complete listing of all particles and four-momenta, and so various details must be reconstructed. Exactly which details are filled in can vary based on the ALPGEN process in question. This is another private method used when an event is read in. It shuffles and rescales momenta in an event to ensure energy-momentum conservation. First, pT is made to balance by splitting any imbalance between all outgoing particles with their energies also scaled. Second, the e/pZ of the two incoming particles are scaled to balance the outgoing particles. Finally, any intermediate resonances are recalculated from their decay products.

    AlpgenPar

    This class parses an ALPGEN parameter file and makes the information available through a simple interface. The information is stored internally in key/value (string/double) format. All lines prior to:
      ************** run parameters 
    are ignored, and in the general case, a line e.g.
      10   3.00000000000000        ! njets
    would be stored with key "njets" and value "3.0". The following lines are special cases where the line may be split or the key translated:
      3 ! hard process code
      0.000   4.700 174.300  80.419  91.188 120.000 ! mc,mb,mt,mw,mz,mh
      912.905 0.0914176   ! Crosssection +- error (pb)
      100 29787.4  ! unwtd events, lum (pb-1) Njob= 2
    
    In the first line, the key "hard process code" is translated to "hpc". In the second, the mass values are split and each given an entry in the internal store. In the third, the cross section and cross section error are stored under the keys "xsecup" and "xerrup" respectively. Finally, the number of events and luminosity are stored under the keys "nevent" and "lum" respectively. In the event that a duplicate key is present, with differing values, the stored value is overwritten and a warning given. The constructor does nothing except for store the PYTHIA Info pointer, if given. This is used for warning/error message printing. This method parses an ALPGEN parameter file. The parameter file is passed as a single string, mainly intended to be read out from the PYTHIA Info object using the header information methods. Method to check if a parameter with key paramIn is present. Returns true if present, else false. Return the parameter with key paramIn as a double or integer. The presence of a parameter should have already been checked using the haveParam() function above. If the parameter is not present, 0 is returned. Method to print a list of stored parameters.

    AlpgenHooks

    This UserHooks derived class provides all the Alpgen:* options. It is provided as a UserHooks class such that the code works regardless of whether ALPGEN native or LHE file formats are used. It is declared with virtual inheritance so that it may be combine with other UserHooks classes, see the "Combining UserHooks" section below. The constructor takes a PYTHIA object as input, so that the beam parameter settings can be overridden if the Alpgen:file option is given. If this is the case, an LHAupAlpgen instance is automatically created and passed to PYTHIA. This is the only UserHooks method that is overridden. It is called directly after PYTHIA has initialised the beams, and therefore the header information should be present in the PYTHIA Info object. The AlpgenPar class is used to parse ALPGEN parameters, if present, which are then used to set further PYTHIA settings.
    pythia8-8.1.80.orig/xmldoc/ElectroweakProcesses.xml0000444000175000017500000002172212217346302020477 0ustar sunsun

    Electroweak Processes

    This page contains processes involving Prompt-photon, gamma^*/Z^0 and W^+- production, plus a few with t-channel boson exchange.

    Prompt photon processes

    This group collects the processes where one or two photons are produced by the hard process. Additional sources of photons include parton showers and hadron decays. A pT cut is required to stay away from the unphysical low-pT region. An eikonalized description, intended to be valid at all pT, is included as part of the multiparton-interactions framework. Common switch for the group of all prompt photon processes, as listed separately in the following. Scattering q g -> q gamma. Code 201. Scattering q qbar -> g gamma. Code 202. Scattering g g -> g gamma. Note: This is a box graph. The full quark-mass dependence in the loop leads to very complicated expressions. The current implementation is based on assuming five massless quarks (see below), and thus is questionable at small (pT < m_b) or large (pT > m_t) transverse momenta. Code 203. Scattering q qbar -> gamma gamma. Code 204. Scattering g g -> gamma gamma. Note: This is a box graph. The full quark-mass dependence in the loop leads to very complicated expressions. The current implementation is based on assuming five massless quarks (see below), and thus is questionable at small (pT < m_b) or large (pT > m_t) transverse momenta. Code 205. Number of quark flavours included in the box graphs responsible for g g -> g gamma and g g-> gamma gamma processes. Owing to the complexity if the massive expressions, quarks are treated as massless. The default value should be applicable in the range of transverse momenta above the b mass but below the t one.

    Weak boson processes

    Under this heading we group processes involving the production of a single electroweak gauge boson, i.e. a gamma^*/Z^0 or a W^+-, or a pair of them, or one of them in combination with a parton. Since the three sets are partly conflicting, each is associated with its own group flag. In addition, t-channel exchange of such a boson between two fermions form a separate group.

    There is one flag that can be used to influence the gamma^*/Z^0 structure in all the processes below where it is produced, unless otherwise stated. Choice of full gamma^*/Z^0 structure or not in relevant processes. Note: irrespective of the option used, the particle produced will always be assigned code 23 for Z^0, and open decay channels is purely dictated by what is set for the Z^0.

    Boson exchange

    The two processes in this subgroup is included as part of the multiparton-interactions framework. Common switch for the group of gamma^*/Z^0 or W^+- exchange between two fermions. Scattering f f' -> f f' via gamma^*/Z^0 t-channel exchange, with full interference between the gamma^* and Z^0. Code 211. Scattering f_1 f_2 -> f_3 f_4 via W^+- t-channel exchange. Code 212.

    Single boson

    Common switch for the group of a single gamma^*/Z^0 or W^+- production. Scattering f fbar -> gamma^*/Z^0, with full interference between the gamma^* and Z^0. Code 221. Scattering f fbar' -> W^+-. Code 222. Scattering f fbar -> gamma^* -> f' fbar'. Subset of process 221, but written as a 2 -> 2 process, so that pT can be used as ordering variable, e.g. in multiparton interactions. Hardcoded for the final state being either of the five quark flavours or three lepton ones. Not included in the WeakSingleBoson:all set, but included in the multiparton-interactions framework. Code 223.

    Boson pair

    Note that, in the decay of the two vector bosons produced by an f fbar -> V V process, the full four-fermion correlations from the leading-order f fbar -> V V -> 4f matrix elements are included Gun86 (with some extensions by the authors). The matrix elements are provided in the double-resonant approach, i.e. excludes graph like f fbar -> V -> f fbar -> f fbar V -> 4f. Common switch for the group of pair production of gamma^*/Z^0 and W^+-. Scattering f fbar' -> gamma^*/Z^0 gamma^*/Z^0. Code 231. Scattering f fbar' -> Z^0 W^+-. Note that here the gamma^* contribution is not (currently) included. Code 232. Scattering f fbar -> W^+ W^-. Code 233.

    Boson and parton

    Common switch for the group of production of a single electroweak gauge boson, i.e. a gamma^*/Z^0 or a W^+-, in association with a parton, i.e. a quark, gluon, photon or lepton. These processes give first-order corrections to the ones in the WeakSingleBoson class, and both sets cannot be used simultaneously without unphysical double-counting. The current class should only be used to study the high-pT tail of the gauge-boson production processes (for LHC applications at least pT > 20 GeV), while the ones in WeakSingleBoson should be used for inclusive production. Scattering q qbar -> gamma^*/Z^0 g. Code 241. Scattering q g -> gamma^*/Z^0 q . Code 242. Scattering f fbar -> gamma^*/Z^0 gamma. Code 243. Scattering f gamma -> gamma^*/Z^0 f. Code 244. Scattering q qbar -> W^+- g. Code 251. Scattering q g -> W^+- q. Code 252. Scattering f fbar -> W^+- gamma. Code 253. Scattering f gamma -> W^+- f. Code 254.

    Photon Collision Processes

    A few electroweak two-photon production processes are available. To use them, photon PDFs have to be defined for the incoming beam particles. For proton beams an appropriate set would be MRST QED 2004 Mar05, available in the LHAPDF library. Common switch for the group of six processes presented below. Scatterings gamma gamma -> q qbar, where q is a light quark (u, d, s) . Code 261. Scattering gamma gamma -> c cbar. Code 262. Scattering gamma gamma -> b bbar. Code 263. Scattering gamma gamma -> e+ e-. Code 264. Scattering gamma gamma -> mu+ mu-. Code 265. Scattering gamma gamma -> tau+ tau-. Code 266.
    pythia8-8.1.80.orig/xmldoc/SpacelikeShowers.xml0000444000175000017500000005125412217346317017627 0ustar sunsun

    Spacelike Showers

    The PYTHIA algorithm for spacelike initial-state showers is based on the article Sjo05, where a transverse-momentum-ordered backwards evolution scheme is introduced, with the extension to fully interleaved evolution covered in Cor10a. This algorithm is a further development of the virtuality-ordered one presented in Sj085, with matching to first-order matrix element for Z^0, W^+- and Higgs (in the m_t -> infinity limit) production as introduced in Miu99.

    The normal user is not expected to call SpaceShower directly, but only have it called from Pythia, via PartonLevel. Some of the parameters below, in particular SpaceShower:alphaSvalue, would be of interest for a tuning exercise, however.

    Main variables

    The maximum pT to be allowed in the shower evolution is related to the nature of the hard process itself. It involves a delicate balance between not double-counting and not leaving any gaps in the coverage. The best procedure may depend on information only the user has: how the events were generated and mixed (e.g. with Les Houches Accord external input), and how they are intended to be used. Therefore a few options are available, with a sensible default behaviour. Way in which the maximum shower evolution scale is set to match the scale of the hard process itself. Note 1: Some processes contain matrix-element matching to the first emission; this is the case notably for single gamma^*/Z^0, W^+- and H^0 production. Then default and option 2 give the correct result, while option 1 should never be used. Note 2: as enumerated in the text, these options take effect both for internal and external processes. Whether a particular option makes sense depends on the context. For instance, if events for the same basic process to different orders are to be matched, then option 1 would be a reasonable first guess. But in more sophisticated descriptions option 2 could be combined with UserHooks vetoes on emissions that would lead to double-counting, using more flexible phase space boundaries. Option 0, finally, may be most realistic when only Born-level processes are involved, possibly in combination with a nonzero SpaceShower:pTdampMatch. The rules used for avoiding double-counting are not foolproof, however. As an example, for the t-channel process gamma gamma -> e^+ e^- its pT scale is the plausible upper shower limit, with only dampened emissions above it. But the initial state is not checked and, had only incoming quarks and gluons been taken into account, only the s-channel process q qbar -> gamma^*/Z^0 -> e^+ e^- would have been possible, where indeed the whole phase space should be populated. So this is erroneously used, giving too much emissions. Note 3: These options only apply to the hard interaction. If a "second hard" process is present, the two are analyzed and set separately for the default 0 option, while both are affected the same way for non-default options 1 and 2. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of each process itself. In cases where the above pTmaxMatch rules would imply that pT_max = pT_factorization, pTmaxFudge introduces a multiplicative factor f such that instead pT_max = f * pT_factorization. Only applies to the hardest interaction in an event, and a "second hard" if there is such a one, cf. below. It is strongly suggested that f = 1, but variations around this default can be useful to test this assumption. A multiplicative factor f such that pT_max = f * pT_factorization, as above, but here for the non-hardest interactions (when multiparton interactions are allowed). These options only take effect when a process is allowed to radiate up to the kinematical limit by the above pTmaxMatch choice, and no matrix-element corrections are available. Then, in many processes, the fall-off in pT will be too slow by one factor of pT^2. That is, while showers have an approximate dpT^2/pT^2 shape, often it should become more like dpT^2/pT^4 at pT values above the scale of the hard process. Whether this actually is the case depends on the particular process studied, e.g. if t-channel gluon exchange is likely to dominate. If so, the options below could provide a reasonable high-pT behaviour without requiring higher-order calculations. Note: These options only apply to the hard interaction. Specifically, a "second hard" interaction would not be affected. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of the process itself. In cases 1 and 2 above, where a dampening is imposed at around the factorization or renormalization scale, respectively, this allows the pT scale of dampening of radiation by a half to be shifted by this factor relative to the default Q_fac or Q_ren. This number ought to be in the neighbourhood of unity, but variations away from this value could do better in some processes.

    The amount of QCD radiation in the shower is determined by The alpha_strong value at scale M_Z^2. Default value is picked equal to the one used in CTEQ 5L.

    The actual value is then regulated by the running to the scale pT^2, at which it is evaluated Order at which alpha_strong runs,

    The CMW rescaling of Lambda_QCD (see the section on StandardModelParameters) can be applied to the alpha_strong values used for spacelike showers. Note that tunes using this option need lower values of alpha_strong(m_Z^2) than tunes that do not.

    QED radiation is regulated by the alpha_electromagnetic value at the pT^2 scale of a branching. The running of alpha_em.

    The natural scale for couplings and PDFs is pT^2. To explore uncertainties it is possibly to vary around this value, however, in analogy with what can be done for hard processes. The default pT^2 renormalization scale is multiplied by this prefactor. For QCD this is equivalent to a change of Lambda^2 in the opposite direction, i.e. to a change of alpha_strong(M_Z^2) (except that flavour thresholds remain at fixed scales). Below, when pT^2 + pT_0^2 is used as scale, it is this whole expression that is multiplied by the prefactor. The default pT^2 factorization scale is multiplied by this prefactor.

    There are two complementary ways of regularizing the small-pT divergence, a sharp cutoff and a smooth dampening. These can be combined as desired but it makes sense to coordinate with how the same issue is handled in multiparton interactions. Regularize the pT -> 0 divergence using the same sharp cutoff and smooth dampening parameters as used to describe multiparton interactions. That is, the MultipartonInteractions:pT0Ref, MultipartonInteractions:ecmRef, MultipartonInteractions:ecmPow and MultipartonInteractions:pTmin parameters are used to regularize all ISR QCD radiation, rather than the corresponding parameters below. This is a sensible physics ansatz, based on the assumption that colour screening effects influence both MPI and ISR in the same way. Photon radiation is regularized separately in either case. Warning: if a large pT0 is picked for multiparton interactions, such that the integrated interaction cross section is below the nondiffractive inelastic one, this pT0 will automatically be scaled down to cope. Information on such a rescaling does NOT propagate to SpaceShower, however.

    The actual pT0 parameter used at a given CM energy scale, ecmNow, is obtained as pT0 = pT0(ecmNow) = pT0Ref * (ecmNow / ecmRef)^ecmPow where pT0Ref, ecmRef and ecmPow are the three parameters below. Regularization of the divergence of the QCD emission probability for pT -> 0 is obtained by a factor pT^2 / (pT0^2 + pT^2), and by using an alpha_s(pT0^2 + pT^2). An energy dependence of the pT0 choice is introduced by the next two parameters, so that pT0Ref is the pT0 value for the reference cm energy, pT0Ref = pT0(ecmRef). The ecmRef reference energy scale introduced above. The ecmPow energy rescaling pace introduced above. Lower cutoff in pT, below which no further ISR branchings are allowed. Normally the pT0 above would be used to provide the main regularization of the branching rate for pT -> 0, in which case pTmin is used mainly for technical reasons. It is possible, however, to set pT0Ref = 0 and use pTmin to provide a step-function regularization, or to combine them in intermediate approaches. Currently pTmin is taken to be energy-independent. Parton shower cut-off pT for photon coupling to a coloured particle. Parton shower cut-off mass for pure QED branchings. Assumed smaller than (or equal to) pTminChgQ. Force emissions, after the first, to be ordered in rapidity, i.e. in terms of decreasing angles in a backwards-evolution sense. Could be used to probe sensitivity to unordered emissions. Only affects QCD emissions.

    Weak showers

    The description of W^+- and Z^0 gauge boson emission in ISR closely parallels that of such emissions in FSR. We therefore will not repeat the discussion here, but only report on the settings names, which again are similar to the FSR ones. Allow a weak shower, yes or no. Determine which branchings are allowed. Parton shower cut-off pT for weak branchings. Enhancement factor for the weak shower. This is used to increase the statistics of weak shower emissions. Remember afterwards to correct for the additional weak emissions (i.e. divide the weak emissions by the same factor). This parameter allows to stop the weak shower after a single emission.
    on = only a single weak emission is allowed.
    off = unlimited number of weak emissions possible.
    The normal showers uses pT^2 as ordering variable, but for massive particles it could be preferred to use pT^2 + M^2 instead. This parameter allows to use pT^2 + k * M^2 for weak showers, thus k = 0 is the standard ordering and is used as default. Add an extra dampening to the weak shower to lower the production of low-pT W/Z's. The dampening is given by (pT^2 + 0.25 M^2)/ (pT^2 + M^2), where M^2 is the squared mass of the W/Z. This flag will veto the 2nd emission on the same side of the process if it has too high "pT" if the primary process was weak production (code 221, 222, 223). This is too avoid doubling counting with dijet production followed by an emission of a W/Z boson. The pT definition used is the pT in the rest frame of the two emitted partons with respect to the incoming parton. This pT definition should be close to the pT definition of a dijet event. This parameter determines the cut-off pT used for the veto of emissions for weak production. For more information see vetoWeakJets.

    Further variables

    These should normally not be touched. Their only function is for cross-checks.

    There are three flags you can use to switch on or off selected branchings in the shower: Allow a QCD shower; on/off = true/false. Allow quarks to radiate photons; on/off = true/false. Allow leptons to radiate photons; on/off = true/false.

    There are some further possibilities to modify the shower: Use of matrix element corrections; on/off = true/false. Use of matrix element corrections also after the first emission, for dipole ends of the same system that did not yet radiate. Only has a meaning if MEcorrections above is switched on. Azimuthal asymmetry induced by gluon polarization; on/off = true/false. Azimuthal asymmetry induced by interference; on/off = true/false. Size of asymmetry induced by interference. Natural value of order 0.5; expression would blow up for a value of 1. Number of allowed quark flavours in g -> q qbar branchings, when kinematically allowed, and thereby also in incoming beams. Changing it to 4 would forbid g -> b bbar, etc.

    Technical notes

    Almost everything is equivalent to the algorithm in [1]. Minor changes are as follows.
    • It is now possible to have a second-order running alpha_s, in addition to fixed or first-order running.
    • The description of heavy flavour production in the threshold region has been modified, so as to be more forgiving about mismatches between the c/b masses used in Pythia relative to those used in a respective PDF parametrization. The basic idea is that, in the threshold region of a heavy quark Q, Q = c/b, the effect of subsequent Q -> Q g branchings is negligible. If so, then f_Q(x, pT2) = integral_mQ2^pT2 dpT'2/pT'2 * alpha_s(pT'2)/2pi * integral P(z) g(x', pT'2) delta(x - z x') so use this to select the pT2 of the g -> Q Qbar branching. In the old formalism the same kind of behaviour should be obtained, but by a cancellation of a 1/f_Q that diverges at the threshold and a Sudakov that vanishes.
      The strategy therefore is that, once pT2 < f * mQ2, with f a parameter of the order of 2, a pT2 is chosen like dpT2/pT2 between mQ2 and f * mQ2, a nd a z flat in the allowed range. Thereafter acceptance is based on the product of three factors, representing the running of alpha_strong, the splitting kernel (including the mass term) and the gluon density weight. At failure, a new pT2 is chosen in the same range, i.e. is not required to be lower since no Sudakov is involved.
    • The QED algorithm now allows for hadron beams with non-zero photon content. The backwards-evolution of a photon in a hadron is identical to that of a gluon, with CF -> eq^2 and CA -> 0. Note that this will only work in conjunction with parton distribution that explicitly include photons as part of the hadron structure (such as the MRST2004qed set). Since Pythia's internal sets do not allow for photon content in hadrons, it is thus necessary to use the LHAPDF interface to make use of this feature. The possibility of a fermion backwards-evolving to a photon has not yet been included, nor has photon backwards-evolution in lepton beams.
    pythia8-8.1.80.orig/xmldoc/ct09mc1.pds0000444000175000017500000173562312217346300015524 0ustar sunsunPDF Table for Fit #: fl6msrv Ordr, Nfl, lambda Qmass 1, 2, 3, 4, 5, 6 1. 5. 0.1668 0.001 0.001 0.200 1.300 4.650 172.000 IPD0, IHDN, IKNL, NfMx, Nfval, KF, Nelmt 1 1 1 5 2 12 57300 NX, NT, JT, NG, NTL(NG+1) 190 24 1 2 24 (NTL(I), NTN(I), TLN(I), DTN(I), I =1, NG) 0 6 7.19603E-01 8.04674E-02 6 18 1.20241E+00 7.69817E-02 QINI, QMAX, (QV(I), TV(I), I =0, NT) 1.30000E+00 1.00000E+05 1.30000E+00 7.19603E-01 1.54410E+00 8.00071E-01 1.86068E+00 8.80538E-01 2.27748E+00 9.61006E-01 2.83526E+00 1.04147E+00 3.59503E+00 1.12194E+00 4.65000E+00 1.20241E+00 6.06898E+00 1.27939E+00 8.09160E+00 1.35637E+00 1.10395E+01 1.43335E+00 1.54405E+01 1.51033E+00 2.21836E+01 1.58732E+00 3.28092E+01 1.66430E+00 5.00682E+01 1.74128E+00 7.90344E+01 1.81826E+00 1.29400E+02 1.89524E+00 2.20389E+02 1.97222E+00 3.91696E+02 2.04921E+00 7.28945E+02 2.12619E+00 1.42569E+03 2.20317E+00 2.94218E+03 2.28015E+00 6.43417E+03 2.35713E+00 1.49799E+04 2.43411E+00 3.73160E+04 2.51110E+00 1.00000E+05 2.58808E+00 XMIN, XCR, (XV(I), I =1, NX) 1.00000E-08 1.50000E+00 1.00000E-08 1.17803E-08 1.38778E-08 1.63489E-08 1.92599E-08 2.26892E-08 2.67291E-08 3.14884E-08 3.70950E-08 4.36999E-08 5.14807E-08 6.06469E-08 7.14452E-08 8.41659E-08 9.91515E-08 1.16805E-07 1.37602E-07 1.62101E-07 1.90962E-07 2.24961E-07 2.65013E-07 3.12195E-07 3.67777E-07 4.33253E-07 5.10385E-07 6.01248E-07 7.08284E-07 8.34965E-07 9.83595E-07 1.15868E-06 1.36492E-06 1.60787E-06 1.89406E-06 2.23117E-06 2.62841E-06 3.09641E-06 3.64773E-06 4.29722E-06 5.06234E-06 5.96367E-06 7.02548E-06 8.27631E-06 9.74982E-06 1.14856E-05 1.35304E-05 1.59392E-05 1.87766E-05 2.21191E-05 2.60564E-05 3.06942E-05 3.61571E-05 4.25918E-05 5.01709E-05 5.90977E-05 6.96115E-05 8.19937E-05 9.65758E-05 1.13747E-04 1.33967E-04 1.57774E-04 1.85802E-04 2.18795E-04 2.57627E-04 3.03325E-04 3.57094E-04 4.20343E-04 4.94725E-04 5.82239E-04 6.85007E-04 8.05733E-04 9.47515E-04 1.11390E-03 1.30904E-03 1.53770E-03 1.80543E-03 2.11857E-03 2.48437E-03 2.91111E-03 3.40814E-03 3.98598E-03 4.65639E-03 5.43234E-03 6.32831E-03 7.35986E-03 8.54125E-03 9.89379E-03 1.14309E-02 1.31758E-02 1.51436E-02 1.73523E-02 1.98189E-02 2.25606E-02 2.55851E-02 2.89092E-02 3.25397E-02 3.64826E-02 4.07414E-02 4.53168E-02 5.02071E-02 5.54085E-02 6.09151E-02 6.67197E-02 7.28133E-02 7.91861E-02 8.58274E-02 9.27257E-02 9.98695E-02 1.07243E-01 1.14848E-01 1.22661E-01 1.30677E-01 1.38873E-01 1.47265E-01 1.55821E-01 1.64539E-01 1.73408E-01 1.82435E-01 1.91589E-01 2.00875E-01 2.10284E-01 2.19811E-01 2.29449E-01 2.39192E-01 2.49036E-01 2.58974E-01 2.69003E-01 2.79118E-01 2.89315E-01 2.99590E-01 3.09940E-01 3.20361E-01 3.30848E-01 3.41402E-01 3.52019E-01 3.62695E-01 3.73426E-01 3.84208E-01 3.95063E-01 4.05950E-01 4.16887E-01 4.27870E-01 4.38898E-01 4.49969E-01 4.61082E-01 4.72234E-01 4.83424E-01 4.94651E-01 5.05914E-01 5.17211E-01 5.28541E-01 5.39903E-01 5.51296E-01 5.62718E-01 5.74170E-01 5.85653E-01 5.97163E-01 6.08683E-01 6.20243E-01 6.31826E-01 6.43433E-01 6.55063E-01 6.66715E-01 6.78389E-01 6.90084E-01 7.01799E-01 7.13535E-01 7.25289E-01 7.37063E-01 7.48855E-01 7.60668E-01 7.72487E-01 7.84333E-01 7.96195E-01 8.08073E-01 8.19966E-01 8.31874E-01 8.43797E-01 8.55734E-01 8.67686E-01 8.79651E-01 8.91628E-01 9.03624E-01 9.15628E-01 9.27645E-01 9.39675E-01 9.51717E-01 9.63770E-01 9.75836E-01 9.87912E-01 1.00000E+00 Parton Distribution Table: 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 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    Multiparton Interactions

    The starting point for the multiparton interactions physics scenario in PYTHIA is provided by Sjo87. Recent developments have included a more careful study of flavour and colour correlations, junction topologies and the relationship to beam remnants Sjo04, interleaving with initial-state radiation Sjo05, making use of transverse-momentum-ordered initial- and final-state showers, with the extension to fully interleaved evolution covered in Cor10a. A framework to handle rescattering is described in Cor09.

    A big unsolved issue is how the colour of all these subsystems is correlated. For sure there is a correlation coming from the colour singlet nature of the incoming beams, but in addition final-state colour rearrangements may change the picture. Indeed such extra effects appear necessary to describe data, e.g. on <pT>(n_ch). A simple implementation of colour rearrangement is found as part of the beam remnants description.

    Main variables

    Matching to hard process

    The maximum pT to be allowed for multiparton interactions is related to the nature of the hard process itself. It involves a delicate balance between not double-counting and not leaving any gaps in the coverage. The best procedure may depend on information only the user has: how the events were generated and mixed (e.g. with Les Houches Accord external input), and how they are intended to be used. Therefore a few options are available, with a sensible default behaviour. Way in which the maximum scale for multiparton interactions is set to match the scale of the hard process itself. Note: If a "second hard" process is present, the two are analyzed separately for the default 0 option. It is enough that one of them only consists of quarks, gluons and photons to restrict the pT range. The maximum for MPI is then set by the hard interaction with lowest scale.

    Cross-section parameters

    The rate of interactions is determined by The value of alpha_strong at m_Z. Default value is picked equal to the one used in CTEQ 5L.

    The actual value is then regulated by the running to the scale pT^2, at which it is evaluated The order at which alpha_strong runs at scales away from m_Z.

    QED interactions are regulated by the alpha_electromagnetic value at the pT^2 scale of an interaction. The running of alpha_em used in hard processes.

    Note that the choices of alpha_strong and alpha_em made here override the ones implemented in the normal process machinery, but only for the interactions generated by the MultipartonInteractions class.

    In addition there is the possibility of a global rescaling of cross sections (which could not easily be accommodated by a changed alpha_strong, since alpha_strong runs) Multiply all cross sections by this fix factor.

    The processes used to generate multiparton interactions form a subset of the standard library of hard processes. The input is slightly different from the standard hard-process machinery, however, since incoming flavours, the alpha_strong value and most of the kinematics are already fixed when the process is called. It is possible to regulate the set of processes that are included in the multiparton-interactions framework. Set of processes included in the machinery.

    Cross-section regularization

    There are two complementary ways of regularizing the small-pT divergence, a sharp cutoff and a smooth dampening. These can be combined as desired, but it makes sense to coordinate with how the same issue is handled in spacelike showers. Actually, by default, the parameters defined here are used also for the spacelike showers, but this can be overridden.

    Regularization of the divergence of the QCD cross section for pT -> 0 is obtained by a factor pT^4 / (pT0^2 + pT^2)^2, and by using an alpha_s(pT0^2 + pT^2). An energy dependence of the pT0 choice is introduced by two further parameters, so that pT0Ref is the pT0 value for the reference CM energy, pT0Ref = pT0(ecmRef). Warning: if a large pT0 is picked for multiparton interactions, such that the integrated interaction cross section is below the nondiffractive inelastic one, this pT0 will automatically be scaled down to cope.

    The actual pT0 parameter used at a given CM energy scale, ecmNow, is obtained as pT0 = pT0(ecmNow) = pT0Ref * (ecmNow / ecmRef)^ecmPow where pT0Ref, ecmRef and ecmPow are the three parameters below. The pT0Ref scale in the above formula. Note: pT0Ref is one of the key parameters in a complete PYTHIA tune. Its value is intimately tied to a number of other choices, such as that of colour flow description, so unfortunately it is difficult to give an independent meaning to pT0Ref. The ecmRef reference energy scale introduced above. The ecmPow energy rescaling pace introduced above.

    Alternatively, or in combination, a sharp cut can be used. Lower cutoff in pT, below which no further interactions are allowed. Normally pT0 above would be used to provide the main regularization of the cross section for pT -> 0, in which case pTmin is used mainly for technical reasons. It is possible, however, to set pT0Ref = 0 and use pTmin to provide a step-function regularization, or to combine them in intermediate approaches. Currently pTmin is taken to be energy-independent.

    Gösta Gustafson has proposed (private communication, unpublished) that the amount of screening, as encapsulated in the pT0 parameter, fluctuates from one event to the next. Specifically, high-activity event are more likely to lead to interactions at large pT scales, but the high activity simultaneously leads to a larger screening of interactions at smaller pT. Such a scenario can approximately be simulated by scaling up the pT0 by a factor sqrt(n), where n is the number of interactions considered so far, including the current one. That is, for the first interaction the dampening factor is pT^4 / (pT0^2 + pT^2)^2, for the second pT^4 / (2 pT0^2 + pT^2)^2, for the third pT^4 / (3 pT0^2 + pT^2)^2, and so on. Optionally the scheme may also be applied to ISR emissions. For simplicity the same alpha_s(pT0^2 + pT^2) is used throughout. Note that, in this scenario the pT0 scale must be lower than in the normal case to begin with, since it later is increased back up. Also note that the idea with this scenario is to propose an alternative to colour reconnection to understand the rise of <pT>(n_ch), so that the amount of colour reconnection should be reduced. Choice to activate the above screening scenario, i.e. an increasing effective pT0 for consecutive interactions.

    Impact-parameter dependence

    The choice of impact-parameter dependence is regulated by several parameters. The ones listed here refer to nondiffractive topologies only, while their equivalents for diffractive events are put in the Diffraction description. Note that there is currently no bProfile = 4 option for diffraction. Other parameters are assumed to agree between diffractive and nondiffractive topologies. Choice of impact parameter profile for the incoming hadron beams. When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a radius that is a factor coreRadius smaller than the rest. When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a fraction coreFraction of the matter content of the hadron. When bProfile = 3 it gives the power of the assumed overlap shape exp(- b^expPow). Default corresponds to a simple exponential drop, which is not too dissimilar from the overlap obtained with the standard double Gaussian parameters. For expPow = 2 we reduce to the simple Gaussian, bProfile = 1, and for expPow -> infinity to no impact parameter dependence at all, bProfile = 0. For small expPow the program becomes slow and unstable, so the min limit must be respected. When bProfile = 4, this gives the a1 constant in the Gaussian width. When a1 = 0., this reduces back to the single Gaussian case. The selection of impact parameter is related to the scale of the hard process: the harder this scale is, the more central the collision. In practice this centrality saturates quickly, however, and beyond a scale of roughly 20 GeV very little changes. (The relevant quantity is that the QCD jet cross section above the scale should be a tiny fraction of the total cross section.) In 2 -> 1 and 2 -> 2 processes traditional scale choices work fine, but ambiguities arise for higher multiplicities, in particular when the scale is used for matching between the multiparton matrix elements and parton showers. Then the event scale may be chosen as that of a very low-pT parton, i.e. suggesting a peripheral collision, while the much harder other partons instead would favour a central collision. Therefore the default here is to override whatever scale value have been read in from an LHEF, say. Notice that the scale used here is decoupled from the maximum scale for MPIs (MultipartonInteractions:pTmaxMatch).

    Rescattering

    It is possible that a parton may rescatter, i.e. undergo a further interaction subsequent to the first one. The machinery to model this kind of physics has only recently become fully operational Cor09, and is therefore not yet so well explored.

    The rescattering framework has ties with other parts of the program, notably with the beam remnants. Switch to allow rescattering of partons; on/off = true/false.
    Note: the rescattering framework has not yet been implemented for the MultipartonInteractions:bProfile = 4 option, and can therefore not be switched on in that case. Warning: use with caution since machinery is still not so well tested.
    Switch to allow rescattering of partons, where both incoming partons have already rescattered; on/off = true/false. Is only used if MultipartonInteractions:allowRescatter is switched on.
    Warning: currently there is no complete implementation that combines it with shower evolution, so you must use PartonLevel:ISR = off and PartonLevel:FSR = off. If not, a warning will be issued and double rescattering will not be simulated. The rate also comes out to be much lower than for single rescattering, so to first approximation it can be neglected.
    Selection of which partons rescatter against unscattered partons from the incoming beams A and B, based on their rapidity value y in the collision rest frame. Here ySep is shorthand for MultipartonInteractions:ySepRescatter and deltaY for MultipartonInteractions:deltaYRescatter, defined below. The description is symmetric between the two beams, so only one case is described below. used for some of the MultipartonInteractions:rescatterMode options above, as the rapidity for which a scattered parton has a 50% probability to be considered as a potential rescatterer. A ySep > 0 generally implies that some central partons cannot rescatter at all, while a ySep < 0 instead allows central partons to scatter against either beam. used for some of the MultipartonInteractions:rescatterMode options above, as the width of the rapidity transition region, where the probability rises from zero to unity that a scattered parton is considered as a potential rescatterer.

    Further variables

    These should normally not be touched. Their only function is for cross-checks. Number of allowed incoming quark flavours in the beams; a change to 4 would thus exclude b and bbar as incoming partons, etc. The allowed pT range is split (unevenly) into 100 bins, and in each of these the interaction cross section is evaluated in nSample random phase space points. The full integral is used at initialization, and the differential one during the run as a "Sudakov form factor" for the choice of the hardest interaction. A larger number implies increased accuracy of the calculations.

    Technical notes

    Relative to the articles mentioned above, not much has happened. The main news is a technical one, that the phase space of the 2 -> 2 (massless) QCD processes is now sampled in dy_3 dy_4 dpT^2, where y_3 and y_4 are the rapidities of the two produced partons. One can show that (dx_1 / x_1) * (dx_2 / x_2) * d(tHat) = dy_3 * dy_4 * dpT^2 Furthermore, since cross sections are dominated by the "Rutherford" one of t-channel gluon exchange, which is enhanced by a factor of 9/4 for each incoming gluon, effective structure functions are defined as F(x, pT2) = (9/4) * xg(x, pT2) + sum_i xq_i(x, pT2) With this technical shift of factors 9/4 from cross sections to parton densities, a common upper estimate of d(sigmaHat)/d(pT2) < pi * alpha_strong^2 / pT^4 is obtained.

    In fact this estimate can be reduced by a factor of 1/2 for the following reason: for any configuration (y_3, y_4, pT2) also one with (y_4, y_3, pT2) lies in the phase space. Not both of those can enjoy being enhanced by the tHat -> 0 singularity of d(sigmaHat) propto 1/tHat^2. Or if they are, which is possible with identical partons like q q -> q q and g g -> g g, each singularity comes with half the strength. So, when integrating/averaging over the two configurations, the estimated d(sigmaHat)/d(pT2) drops. Actually, it drops even further, since the naive estimate above is based on (4 /9) * (1 + (uHat/sHat)^2) < 8/9 < 1 The 8/9 value would be approached for tHat -> 0, which implies sHat >> pT2 and thus a heavy parton-distribution penalty, while parton distributions are largest for tHat = uHat = -sHat/2, where the above expression evaluates to 5/9. A fudge factor is therefore introduced to go the final step, so it can easily be modified when further non-Rutherford processes are added, or should parton distributions change significantly.

    At initialization, it is assumed that d(sigma)/d(pT2) < d(sigmaHat)/d(pT2) * F(x_T, pT2) * F(x_T, pT2) * (2 y_max(pT))^2 where the first factor is the upper estimate as above, the second two the parton density sum evaluated at y_3 = y_ 4 = 0 so that x_1 = x_2 = x_T = 2 pT / E_cm, where the product is expected to be maximal, and the final is the phase space for -y_max < y_{3,4} < y_max. The right-hand side expression is scanned logarithmically in y, and a N is determined such that it always is below N/pT^4.

    To describe the dampening of the cross section at pT -> 0 by colour screening, the actual cross section is multiplied by a regularization factor (pT^2 / (pT^2 + pT0^2))^2, and the alpha_s is evaluated at a scale pT^2 + pT0^2, where pT0 is a free parameter of the order of 2 - 4 GeV. Since pT0 can be energy-dependent, an ansatz pT0(ecm) = pT0Ref * (ecm/ecmRef)^ecmPow is used, where ecm is the current CM frame energy, ecmRef is an arbitrary reference energy where pT0Ref is defined, and ecmPow gives the energy rescaling pace. For technical reasons, also an absolute lower pT scale pTmin, by default 0.2 GeV, is introduced. In principle, it is possible to recover older scenarios with a sharp pT cutoff by setting pT0 = 0 and letting pTmin be a larger number.

    The above scanning strategy is then slightly modified: instead of an upper estimate N/pT^4 one of the form N/(pT^2 + r * pT0^2)^2 is used. At first glance, r = 1 would seem to be fixed by the form of the regularization procedure, but this does not take into account the nontrivial dependence on alpha_s, parton distributions and phase space. A better Monte Carlo efficiency is obtained for r somewhat below unity, and currently r = 0.25 is hardcoded. In the generation a trial pT2 is then selected according to d(Prob)/d(pT2) = (1/sigma_ND) * N/(pT^2 + r * pT0^2)^2 * ("Sudakov") For the trial pT2, a y_3 and a y_4 are then selected, and incoming flavours according to the respective F(x_i, pT2), and then the cross section is evaluated for this flavour combination. The ratio of trial/upper estimate gives the probability of survival.

    Actually, to profit from the factor 1/2 mentioned above, the cross section for the combination with y_3 and y_4 interchanged is also tried, which corresponds to exchanging tHat and uHat, and the average formed, while the final kinematics is given by the relative importance of the two.

    Furthermore, since large y values are disfavoured by dropping PDF's, a factor WT_y = (1 - (y_3/y_max)^2) * (1 - (y_4/y_max)^2) is evaluated, and used as a survival probability before the more time-consuming PDF+ME evaluation, with surviving events given a compensating weight 1/WT_y.

    An impact-parameter dependence is also allowed. Based on the hard pT scale of the first interaction, and enhancement/depletion factor is picked, which multiplies the rate of subsequent interactions.

    Parton densities are rescaled and modified to take into account the energy-momentum and flavours kicked out by already-considered interactions. pythia8-8.1.80.orig/xmldoc/Tunes.xml0000444000175000017500000003423512217346320015444 0ustar sunsun

    Tunes

    Since some physics aspects cannot be derived from first principles, this program contains many parameters that represent a true uncertainty in our understanding of nature. Particularly afflicted are the areas of hadronization and multiparton interactions, which both involve nonperturbative QCD physics.

    Technically, PYTHIA parameters can be varied independently of each other, but the physical requirement of a sensible description of a set of data leads to correlations and anticorrelations between the parameters. Hence the need to produce tunes, not of one parameter at a time, but simultaneously for a group of them. A well-known (separate) such example is parton densities, where combined tunes to a wide range of data have been produced, that can then be obtained prepackaged.

    Given the many PYTHIA parameters to be tuned, it is convenient to divide the task into subtasks. Firstly, if we assume jet universality, hadronization and final-state parton showers should be tuned to e^+e^- annihilation data, notably from LEP1, since this offers the cleanest environment. Secondly, with such parameters fixed, hadron collider data should be studied to pin down multiparton interactions and other further aspects, such as initial-state radiation. Ideally this would be done separately for diffractive and non-diffractive events, although it is not possible to have a clean separation. (Thirdly would come anything else, such as physics with photon beams, which involve further parameters, but that is beyond the current scope.)

    The first step in this program has now been taken, with a tune to LEP1 data by Hendrik Hoeth, using the Rivet + Professor framework. Starting with version 8.125 it defines the default values for hadronization parameters and timelike showers.

    The situation is more complicated for hadronic interactions in general and multiparton interactions in particular, where PYTHIA 8 is more different from PYTHIA 6, and therefore more work is needed. Specifically, it is not possible to "port" a PYTHIA 6 tune to PYTHIA 8.

    A first simple tune, appropriately called "Tune 1", became default starting with version 8.127. It was noted, in particular by Hendrik Hoeth, that this tune had a tension between parameters needed to describe minimum-bias and underlying-event activity. Therefore some further physics features were introduced in the code itself Cor10a, which were made default as of 8.140. This version also included two new tunes, 2C and 2M, based on the CTEQ 6L1 and the MRST LO** PDF sets, respectively. These have been made by hand, as a prequel to complete Professor-style tunings.

    The very first data to come out of the LHC showed a higher rapidity plateau than predicted for current PYTHIA 6 tunes, also for the lower energies. This may suggest some tension in the data. Two alternatives, 3C and 3M, were produced by a few brute-force changes of 2C and 2M. These were introduced in 8.140, but discontinued in 8.145 in favour of the new 4C tune, that is based on a more serious study of some early LHC data, see Cor10a. Following the comparative studies in Buc11, which independently confirmed a reasonable agreement with LHC data, tune 4C was made the default as of 8.150. A variant is tune 4Cx, where the Gaussian matter profile has an x-dependent width Cor11.

    Several ATLAS tunes have now been included, obtained with different PDFs and with different emphasis on minimum-bias and underlying-event data ATL12. These typically require LHAPDF to be linked, but this can be avoided in cases where the same PDF set is implemented internally.

    Central diffraction is a recent addition to the "soft QCD" process palette, and is thus not yet included in tunes; indeed its cross section is actively zeroed. You can switch it back on after you have selected your tune, with SigmaTotal:zeroAXB = off. But note that, since the total cross section is assumed unchanged, the nondiffractive cross section is reduced and thus also the MPI machinery affected, even if effects should not be big (for a small central diffractive cross section).

    Note that comparisons with data also require that other aspects agree, such as that decay chains are stopped at an agreed-on level. For instance, in the ATLAS tunes all particles with a lifetime above 10 mm are considered stable, ParticleDecays:limitTau0 = on, ParticleDecays:tau0Max = 10. We have chosen not to include this as part of the tune settings itself, since the tune as such could still be used with any other choice of stable and unstable particles.

    Further comparisons have been posted on the MCPLOTS pages. They have been produced with help of the Rivet package Buc10.

    In the future we hope to see further PYTHIA 8 tunes appear. Like with parton distributions, there is likely to be several tunes, because different sets of data will pull in different directions, by imperfections in the model or in the data, and by differences in the chosen tuning strategies. We therefore propose to collect some of these tunes here, in a prepackaged form. Of course, in all cases it is a matter of setting values for parameters already defined elsewhere, so the tunes offer no new functionality, only a more convenient setup.

    You should be aware that the evolution of the program will not guarantee complete backwards compatibility between versions. Most obviously this concerns bug fixes. But also for some other major changes, like the introduction of the new diffractive machinery, the default behaviour of old tunes has been changed retroactively. (Which should be fine for diffraction, since previous tunes were not based on data strongly influenced by diffraction.)

    The setup of the tunes is special, in that the choice of a tune forces the change of several different flags, modes and parameters. Furthermore a design principle has been that it should be possible to start out from a tune and then change a few of its settings. This gives power and flexibility at the expense of requiring a more careful ordering of commands. We therefore here sketch the order in which operations are carried out.

    1. The constructor of a Pythia instance will read in all settings, and initialize them with their default values.
    2. At the end of this operation, the Tune:ee and Tune:pp modes (see further below) are checked. If either of them are positive the methods Settings::initTuneEE(...) and Settings::initTunePP(...), respectively, are called to overwrite the whole collection of settings in the relevant tune. Zero (or negative) means that nothing will be done.
    3. After the Pythia constructor all the relevant values for the default tune(s) have thus been set up.
    4. You as a user can now start to overwrite the values at will, using Pythia::readFile(...) to read a configuration file, or a list of Pythia::readString(...) commands, or the lower-level Settings methods. All changes are made in the order in which the commands are encountered during the execution. A given variable can be changed multiparton times, but it is the latest change that sets the current value.
    5. The two Tune:ee and Tune:pp modes can also be changed in exactly the same way as described for all other settings above. Unique for them, however, is that when one of them is encountered it also initiates a call to the initTuneEE(...) or initTunePP(...) method, respectively. In such cases all settings affected by the e^+e^- or pp/ppbar tune are first reset to the default values (the -1 options) and thereafter the relevant tune is set up.
    6. It is possible to mix commands of type 4 and 5 in any order; it is always the last change that counts. That is, any changes you have made to variables of a tune before a Tune:ee or Tune:pp command are overwritten by it, while variables you set after will overwrite the tune values. As a rule, therefore, you want to begin with the tune choice, and thereafter modify only a small part of its settings.
    7. Needless to say, the flexibility can lead to unwanted setups if you do not exercise some discipline. It is therefore recommended that you always check the listing obtained with Pythia::settings.listChanged() to confirm that the final set of changes is the intended one.
    Choice of tune to e^+e^- data, mainly for the hadronization and timelike-showering aspects of PYTHIA. You should study the Settings::initTuneEE(...) method to find exactly which are the settings for the respective tune. Tunes made by experimental collaborations typically use the LHAPDF package to obtain their PDF values, and so PYTHIA has to be linked accordingly. For PDFs implemented natively in PYTHIA it is possible to use the respective tunes, without having to link to LHAPDF, if you set Tune:preferLHAPDF = off before the Tune:pp choice. Choice of tune to pp/ppbar data, mainly for the initial-state-radiation, multiparton-interactions and beam-remnants aspects of PYTHIA. Note that the previous crude (non-)tunes 3C and 3M are removed as of 8.145, superseded by the 4C tune. You should study the Settings::initTunePP(...) method to find exactly which are the settings for the respective tune.
    pythia8-8.1.80.orig/xmldoc/RandomNumbers.xml0000444000175000017500000001167612217346317017134 0ustar sunsun

    Random Numbers

    This page describes the random-number generator in PYTHIA and how it can be replaced by an external one.

    Internal random numbers

    The Rndm class generates random numbers, using the Marsaglia-Zaman-Tsang algorithm Mar90.

    Random numbers R uniformly distributed in 0 < R < 1 are obtained with

       Rndm::flat();
    
    There are also methods to generate according to an exponential, to x * exp(-x), to a Gaussian, or picked among a set of possibilities, which make use of flat().

    If the random number generator is not initialized before, it will be so the first time it is asked to generate a random number, and then with the default seed, 19780503. This means that, by default, all runs will use identically the same random number sequence. This is convenient for debugging purposes, but dangerous if you intend to run several "identical" jobs to boost statistics. You can initialize, or reinitialize, with your own choice of seed with a

       Rndm::init(seed);
    
    Here values 0 < seed < 900 000 000 gives so many different random number sequences, while seed = 0 will call the Stdlib time(0) function to provide a "random" seed, and seed < 0 will revert back to the default seed.

    The Pythia class defines a flag and a mode, that allows the seed to be set in the Pythia::init call. That would be the standard way for a user to pick the random number sequence in a run.

    External random numbers

    RndmEngine is a base class for the external handling of random-number generation. The user-written derived class is called if a pointer to it has been handed in with the pythia.rndmEnginePtr() method. Since the default Marsaglia-Zaman-Tsang algorithm is quite good, chances are that any replacement would be a step down, but this may still be required by consistency with other program elements in big experimental frameworks.

    There is only one pure virtual method in RndmEngine, to generate one random number flat in the range between 0 and 1:

      virtual double flat() = 0;
    
    Note that methods for initialization are not provided in the base class, in part since input parameters may be specific to the generator used, in part since initialization can as well be taken care of externally to the Pythia code.

    An example illustrating how to run with an external random number generator is provided in main23.cc.

    The methods

    We here collect a more complete and formal overview of the methods. construct a random number generator, but does not initialize it. construct a random number generator, and initialize it for the given seed number. pass in pointer for external random number generation. initialize, or reinitialize, the random number generator for the given seed number. Not necessary if the seed was already set in the constructor. generate next random number uniformly between 0 and 1. generate random numbers according to exp(-x). generate random numbers according to x exp(-x). generate random numbers according to exp(-x^2/2). generate a pair of random numbers according to exp( -(x^2 + y^2) / 2). Is faster than two calls to gauss(). pick one option among vector of (positive) probabilities. save the current state of the random number generator to a binary file. This involves two integers and 100 double-precision numbers. Intended for debug purposes. Note that binary files may be platform-dependent and thus not transportable. set the state of the random number generator by reading in a binary file saved by the above command. Comments as above. if you want to construct an external random number generator (or generator interface) then you must implement this method in your class derived from the RndmEningen base class, to give a random number between 0 and 1.
    pythia8-8.1.80.orig/xmldoc/HadronLevelStandalone.xml0000444000175000017500000002717012217346303020563 0ustar sunsun

    Hadron-Level Standalone

    The Les Houches Accord allows external process-level configurations to be fed in, for subsequent parton-level and hadron-level generation to be handled internally by PYTHIA. There is no correspondingly standardized interface if you have external events that have also been generated through the parton-level stage, so that only the hadron-level remains to be handled. A non-standard way to achieve this exists, however, and can be useful both for real applications and for various tests of the hadronization model on its own.

    The key trick is to set the flag ProcessLevel:all = off. When pythia.next() is called it then does not try to generate a hard process. Since there are no beams, it is also not possible to perform the normal PartonLevel step. (It is still possible to generate final-state radiation, but this is not automatic. It would have to be done by hand, using the pythia.forceTimeShower(...) method, before pythia.next() is called.) Thus only the HadronLevel methods are called, to take the current content of the event record stored in pythia.event as a starting point for any hadronization and decays that are allowed by the normal parameters of this step. Often the input would consist solely of partons grouped into colour singlets, but also (colour-singlet) particles are allowed.

    To set up all the parameters, a pythia.init() call has to be used, without any arguments. In brief, the structure of the main program therefore should be something like

      Pythia pythia;                               // Declare generator.
      Event& event = pythia.event                  // Convenient shorthand.
      pythia.readString("ProcessLevel:all = off"); // The trick!
      pythia.init();                               // Initialization.
      for (int iEvent = 0; iEvent < nEvent; ++iEvent) {
        // Insert filling of event here!
        pythia.next();                             // Do the hadron level.
      }
    
    Of course this should be supplemented by analysis of events, error checks, and so on, as for a normal PYTHIA run. The unique aspect is how to fill the event inside the loop, before pythia.next() is called.

    Input configuration

    To set up a new configuration the first step is to throw away the current one, with event.reset(). This routine will also reserve the zeroth entry in the even record to represent the event as a whole.

    With the event.append(...) methods a new entry is added at the bottom of the current record, i.e. the first time it is called entry number 1 is filled, and so on. The append method basically exists in four variants, either without or with history information, and with four-momentum provided either as a Vec4 four-vector or as four individual components:

      append( id, status, col, acol, p, m)
      append( id, status, col, acol, px, py, pz, e, m)
      append( id, status, mother1, mother2, daughter1, daughter2, col, acol, p, m)
      append( id, status, mother1, mother2, daughter1, daughter2, col, acol, px, py, pz, e, m)
    
    The methods return the index at which the entry has been stored, but normally you would not use this feature.

    You can find descriptions of the input variables here. The PDG particle code id and the Les Houches Accord colour col and anticolour acol tags must be set correctly. The four-momentum and mass have to be provided in units of GeV; if you omit the mass it defaults to 0.

    Outgoing particles that should hadronize should be given status code 23. Often this is the only status code you need. You could e.g. also fill in incoming partons with -21 and intermediate ones with -22, if you so wish. Usually the choice of status codes is not crucial, so long as you recall that positive numbers correspond to particles that are still around, while negative numbers denote ones that already hadronized or decayed. However, so as not to run into contradictions with the internal PYTHIA checks (when Check:event = on), or with external formats such as HepMC, we do recommend the above codes. When pythia.next() is called the positive-status particles that hadronize/decay get the sign of the status code flipped to negative but the absolute value is retained. The new particles are added with normal PYTHIA status codes.

    For normal hadronization/decays in pythia.next() the history encoded in the mother and daughter indices is not used. Therefore the first two append methods, which set all these indices vanishing, should suffice. The subsequent hadronization/decays will still be properly documented.

    The exception is when you want to include junctions in your string topology, i.e. have three string pieces meet. Then you must insert in your event record the (decayed) particle that is the reason for the presence of a junction, e.g. a baryon beam remnant from which several valence quarks have been kicked out, or a neutralino that underwent a baryon-number-violating decay. This particle must have as daughters the three partons that together carry the baryon number.

    The sample program in main21.cc illustrates how you can work with this facility, both for simple parton configurations and for more complicated ones with junctions.

    As an alternative to setting up a topology with the methods above, a Les Houches Event File (LHEF) can also provide the configurations. Since no beams or processes are defined, only the <event>....</event> blocks need to be present, one for each event, so strictly it is not a true LHEF. You need to select Beams:frameType = 4, provide the file name in Beams:LHEF and, as above, set ProcessLevel:all = off. Needless to say, an externally linked LHAup class works as well as an LHEF, with Beams:frameType = 5.

    The event information to store in the LHEF, or provide by the LHAup, is essentially the same as above. The only difference is in status codes: outgoing particles should have 1 instead of 23, and intermediate resonances 2 instead of -22. Incoming partons, if any, are -1 instead of -21.

    Extensions to resonance decays

    With the above scheme, pythia.next() will generate hadronization, i.e. string fragmentation and subsequent decays of normal unstable particles. It will not decay resonances, i.e. W, Z, top, Higgs, SUSY and other massive particles.

    If the decay products are already provided, of course those products will be hadronized, but without any of the showers that one would expect in Z^0 -> q qbar, say. That is, the presence of a decayed resonance in the event record can be nice for documentation purposes, but otherwise it plays no role. It is possible to change this behaviour with the following flag. If off, then resonances are stable if final-state particles, and irrelevant if intermediate particles. If on, then resonances are decayed, sequentially if necessary. After each decay step a parton shower is applied, and subsequent decay kinematics is shifted by the recoil of such branchings. If the decay chain and kinematics of the resonance is provided at input, this information is used, otherwise it is generated internally according to built-in branching ratios etc.

    The input configuration has to follow the rules described above, with ProcessLevel:all = off. (Terminology not quite consistent, since resonance decays normally is part of the process-level step.) It is possible to combine several resonances, and other coloured or uncoloured particles into the same event.

    Final-state radiation is applied to each step of the decay sequence by default, but can be switched off with PartonLevel:FSR = off or PartonLevel:FSRinResonances.

    Repeated hadronization or decay

    An alternative approach is possible with the pythia.forceHadronLevel() routine. This method does a call to the HadronLevel methods, irrespective of the value of the HadronLevel:all flag. If you hadronize externally generated events it is equivalent to a pythia.next() call with ProcessLevel:all = off.

    This method truly sticks to the hadron level, and thus cannot handle resonance decays. You therefore must not mix it with the Standalone:allowResDec = on framework.

    The similarity of names indicates that pythia.forceTimeShower( int iBeg, int iEnd, double pTmax, int nBranchMax = 0) is intended to belong to the same set of work-by-hand methods. Here iBeg and iEnd give the range of partons that should be allowed to shower, pTmax the maximum pT scale of emissions, and a nonzero nBranchMax a maximum number of allowed branchings. Additionally, a scale has to be set for each parton that should shower, which requires an additional final argument to the append methods above. This scale limits the maximum pT allowed for each parton, in addition to the global pTmax. When not set the scale defaults to 0, meaning no radiation for that parton.

    The real application instead is for repeated hadronization of the same PYTHIA process- and parton-level event. This may for some studies help to save time, given that these two first step are more time-consuming than the hadronization one.

    For repeated hadronization you should first generate an event as usual, but with HadronLevel:all = off. This event you can save in a temporary copy, e.g. Event savedEvent = pythia.event. Inside a loop you copy back with pythia.event = savedEvent, and call pythia.forceHadronLevel() to obtain a new hadronization history.

    A more limited form of repetition is if you want to decay a given kind of particle repeatedly, without having to generate the rest of the event anew. This could be the case e.g. in B physics applications. Then you can use the pythia.moreDecays() method, which decays all particles in the event record that have not been decayed but should have been done so. The pythia.particleData.mayDecay( id, false/true) method may be used to switch off/on the decays of a particle species id, so that it is not decayed in the pythia.next() call but only inside a loop over a number of tries.

    Between each loop the newly produced decay products must be removed and the decayed particle status restored to undecayed. The former is simple, since the new products are appended to the end of the event record: event.saveSize() saves the initial size of the event record, and event.restoreSize() can later be used repeatedly to restore this original size, which means that the new particles at the end are thrown away. The latter is more complicated, and requires the user to identify the positions of all particles of the species and restore a positive status code with event[i].statusPos().

    The main15.cc program illustrates both these methods, i.e. either repeated hadronization or repeated decay of PYTHIA events. pythia8-8.1.80.orig/xmldoc/NLOMerging.xml0000444000175000017500000011642712217346305016316 0ustar sunsun

    NLO Merging

    Pythia offers two NLO merging approaches. Both of these methods have been presented in Lon13. The goal of NLO merging is to extend tree-level multi-jet merging methods to next-to-leading order accuracy in QCD, for every available jet multiplicity. If for example NLO calculations for Higgs + 0 jet, Higgs + 1 jet and Higgs + 2 jets were available, NLO merging allows to simultaneously describe 0-, 1- and 2-jet observables with NLO accuracy. Further jets can, depending on additional tree-level input, be described by additional tree-level matrix elements. In the example, it would be possible to achieve NLO accuracy for 0-, 1- and 2-jet observables, tree-level accuracy for 3-, 4- and 5-jet configurations, and use the parton shower approximation for events with more than five jets.

    The two NLO merging methods implemented in Pythia are called NL3 (for Nils Lavesson + Leif Lönnblad) and UNLOPS (for unitarised NLO+PS merging). Both of these schemes require Les Houches Event File input that is generated by tree-level or NLO matrix element generators. Currently, Pythia requires NLO input generated within the POWHEG framework. The generation of sensible input will be discussed below. The two NLO merging methods are illustrated in the sample main programs main87.cc (introducing NL3 ) and main88.cc (introducing UNLOPS). Before describing these programs, we would like to outline the differences between the two approaches.

    NL3 is a generalisation of CKKW-L tree-level merging. The main idea of NL3 is to start from CKKW-L-reweighted multi-jet merging, and replace the αsn+0- and αsn+1-terms by the NLO result of POWHEG. This "replacement" means that we subtract the αsn+0- and αsn+1-terms from the CKKW-L-reweighted tree-level samples, and add another sample -- the POWHEG input. All "higher orders" are unchanged w.r.t. CKKW-L. We have implemented the "inclusive" scheme of Lon13 in Pythia. This means that the POWHEG input will contain contributions for hard, resolved real emission jets, which are already taken care of by higher-multiplicity samples in CKKW-L. Thus, explicit phase space subtractions are also included. The sample program main87.cc, together with the input file main87.cmnd, illustrates the procedure.

    UNLOPS is a generalisation of the UMEPS multi-jet merging scheme. Since UMEPS is already slightly more complicated than CKKW-L, this makes UNLOPS more complicated than NL3. The basic idea however remains the same: Start from a tree-level merging scheme (in this case UMEPS), remove all undesirable αsn+0- and αsn+1-terms from this result, and add back the "correct" description via POWHEG input samples. Again, since the "inclusive" scheme of Lon13 was implemented in Pythia, it is necessary to handle explicit phase space subtractions. Similar to UMEPS, UNLOPS further ensures that the lowest-multiplicity cross section is given by the NLO result. This means that the UMEPS philosophy of "subtract what you add" needs to be extended to multi-leg NLO inputs.

    UNLOPS is a theoretically more appealing definition of NLO merging than NL3, and should thus be considered the preferred choice. However, we believe it valuable to include both methods into Pythia, so that the variation of NLO merged results due to different NLO merging schemes can be studied in situ. Furthermore, NLO merging can be outlined more pedagogically when starting from NL3. The two NLO merging methods share parts of code with CKKW-L and UMEPS, and correspondingly share many input settings with these schemes. In particular,

             The hard process (Merging:Process) needs to be defined exactly as in CKKW-L (see Defining the hard process in the CKKW-L documentation).

             The merging scale value (Merging:TMS) has to be set.

             The maximal number of additional partons in tree-level events (Merging:nJetMax) has to be set.

    All settings listed under the sections "Matrix element merging and HepMC output for RIVET" and "Further variables" in the CKKW-L documentation can be accessed in NLO merging as well. Furthermore, the Merging:nRecluster switch (see the UMEPS documentation) is important. Also, all MergingHooks routines that allow for user interference in CKKW-L merging are also usable for NLO merging -- with the exception of a user-defined merging scale. The NLO merging schemes currently implemented in Pythia do not allow for a merging scale definition that differs from the parton shower evolution variable. Since this merging scale definition is not completely obvious, the NLO merging schemes also share the Merging:enforceCutOnLHE switch with CKKW-L. In this way, it is possible to use LHE files that are regularised only with weak cuts as input, while the merging machinery imposes the stronger merging scale cut automatically. This means that no merging scale implementation is required from the user side, but also means that it is the user's responsibility to ensure that the cuts used for generating input LHE files are always looser than the cut given by the merging scale value Merging:TMS. This will lead to warnings of the form "Les Houches Event fails merging scale cut. Cut by rejecting event". These warning should rather be regarded as information. An example of inclusive matrix element generation cuts would be pTjet = 5 GeV, ΔRjetA jetB = 0.01 and QjetA jetB = 5 GeV, if NLO merging with a desired merging scale value of Merging:TMS = 15 is attempted for Higgs + jets events at the LHC.

    In the following, we will first describe the generation of NLO input samples, and list input settings for NLO merging in Pythia. Then, we will examine the sample main programs main87.cc and main88.cc, which implement NL3 and UNLOPS merging, respectively.


    Inputs for NLO merging

    The NLO merging schemes in Pythia currently require Les Houches Event File input. To perform a merging with up to M additional partons described by tree-level matrix elements, and with up to N ≤ M-1 additional partons at NLO accuracy, the user needs to supply

             LHE files for 0... M additional partons, taken from a tree-level matrix element generator, and

             LHE files for 0... N additional partons, taken from a POWHEG NLO generator.

    All input files need to be regularised, if they contain additional partons. Large files with fairly inclusive (i.e. loose) cuts are recommended. The input LHE files should further be generated with fixed renormalisation and factorisation scales. (In the POWHEG-BOX program, this means using the settings runningscales 0, btlscalereal 1, btlscalect 1, ckkwscalup 0. Some older processes in the POWHEG-BOX program need the input runningscale 0 instead of runningscales 0.)

    When attempting NLO merging, the following Pythia settings are relevant. The maximal number of additional jets for which NLO event samples are supplied by the user. The fixed factorisation scale used in the hard process cross section, as needed to generate the leading-order weight, in case the factorisation scale cannot be inferred from Les Houches event input. (This is the case for files that have been generated with the POWHEG-BOX program, since this program prints the transverse momentum scale of the real emission into the LH events.). If the value is not set, the SCALUP variable of the current LH event will be used instead. If wimpy showers (see Timelike Showers and Spacelike Showers) are used together with multi-jet merging, then this scale further sets the parton shower starting scale (μQ) for the core hard process. The fixed renormalisation scale used in the hard process cross section, as needed to generate the leading-order weight, in case the renormalisation scale cannot be inferred from Les Houches event input. (As mentioned above, this is the case for files generated with the POWHEG-BOX program.) If the value is not set, the SCALUP variable of the current LH event will be used instead. The fixed factorisation scale used in the matrix element calculation. This information is needed if factorisation scale variations in NLO merged results are attempted. Depending on the matrix element generator, it might not be possible to infer the factorisation scale from Les Houches event input, and thus, setting an explicit value is required. (As mentioned above, this is the case for files generated with the POWHEG-BOX program.) If the value is not set, the SCALUP variable of the current LH event will be used instead. The fixed renormalisation scale used in the matrix element calculation. This information is needed if renormalisation scale variations in NLO merged results are attempted, for the same reason as factorisation scales might be required. (As mentioned above, this is the case for files generated with the POWHEG-BOX program.) If the value is not set, the SCALUP variable of the current LH event will be used instead.

    All further settings will be discussed while examining the sample main programs.


    NL3 merging with main87.cc

    NL3-style NLO merging in Pythia is illustrated by the sample main program main87.cc. This program works together with an input file (e.g. main87.cmnd) for Pythia settings, and requires LHE input files that follow the naming convention name_tree_#nAdditionalJets.lhe (tree-level samples) and name_powheg_#nAdditionalJets.lhe (POWHEG NLO samples). main87.cc produces HepMC event output Dob01, which can be used for analysis (e.g. using RIVET Buc10), or as input for detector simulations. For users not familiar with HepMC output, it is of course possible remove the HepMC code in the sample program, and use Pythia's histogramming routines instead. Histograms should then be filled as indicated for the histPTFirstSum histograms in main84.cc, i.e. using weightNLO*normhepmc.

    If the user only wants to change the number of requested events (Main:numberOfEvents), the hard process (Merging:Process), the merging scale value (Merging:TMS) and the maximal number of additional tree-level or NLO-accuracte jets (Merging:nJetMax and Merging:nJetMaxNLO, respectively), and HepMC output is desired, then there is no need to change the main87.cc code. The input LHE files are also part of the (command line) input for main87.exe. The default settings in main87.cmnd are intended to work with the (very short) sample LHEF inputs (w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and w_production_powheg_0.lhe, w_production_powheg_1.lhe). For these input files, the main87.exe executable can be run with the command

    ./main87.exe main87.cmnd w_production myhepmc.hepmc

    to produce a file myhepmc.hepmc of NLO merged HepMC event output. All mandatory Pythia input settngs have been outlined earlier. Please refrain from adding input switches than invoke any other merging scheme (e.g. e.g. Merging:doKTMerging) into the input file that you want to use in conjunction with main87.cc.

    In the following, we will explain main87.cc in depth. Users who are willing to accept the default choices do not need to know all details, but are still encouraged to read further.

    Program flow

    main87.cc can be divided into four steps:

             1. Estimate the cross section for tree-level and NLO samples after the merging scale cut.

             2. Produce reweighted tree-level events, which do not contain αs0- and αs1-terms.

             3. Add POWHEG NLO events.

             4. Subtract phase space points with an extra (real-emission) jet above the merging scale from the POWHEG result, since such configurations have already been taken into account by processing other samples.

    The first step is necessary to produce the correct weights for HepMC output events. The estimation of tree-level cross sections after the merging scale cut is generated by invoking the switch Merging:doXSectionEstimate together with Merging:doNL3Tree. In this configuration, the latter switch will only act to define the merging scale. After the tree-level cross sections have been estimated, main87.cc estimates the NLO cross sections after application of the merging scale cut, by inferring Merging:doXSectionEstimate together with Merging:doNL3Loop. Again, in this configuration, the latter switch only acts as the merging scale definition. When generating the estimates, all showering, multiparton interactions and hadronisation is turned off to not unnecessarily waste processor time. For all estimates, is further mandatory to set the value of Merging:nRequested to the jet multiplicity of the current event sample (e.g. to "2" for a sample containing W + 2 jet events). This is necessary in order to correctly apply the merging scale cut. POWHEG NLO input files for W + 1 jet e.g. contain W + 1 jet and W + 2 jet (i.e. real emission) kinematics. However, the merging scale cut aims at regularising the "underlying Born" configuration (i.e. the W + 1 states in our example). Setting Merging:nRequested = 1 for the W + 1 jet POWHEG sample ensures that even for real-emission (W + 2 jet) kinematics, the merging scale cut is applied to W + 1 jet states.

    After the cross section estimation step, main87.cc proceeds to perform the actual merging. Before explaining this part, we would like to make some comments about K-factors.

    main87.cc is prepared to use fixed K-factors to rescale the weight of tree-level events. This rescaling does not affect the NLO accuracy of the method, and was investigated in Lon13. By default, main87.cc does not use K-factors. However, if the user wants to include K-factors, this can be done by using the following input settings. The k-Factor used to rescale the tree-level (i.e. CKKW-L or UMEPS) part of zero-jet tree-level events. The k-Factor used to rescale the tree-level (i.e. CKKW-L or UMEPS) part of one-jet tree-level events. The k-Factor used to rescale the tree-level (i.e. CKKW-L or UMEPS) part of two-jet tree-level events.

    If the variables k0, k1, k2 in main87.cc are set to non-unity values, K-factors will be applied. The K-factor of highest jet multiplicity will then be used to also rescale tree-level samples with a number of additional jets beyond the number of the highest-multiplicity real-emission sample. If we, for example, attempt an NLO merging of W+0 jet and W+1 jet at NLO accuracy, and with W+≤4 jets at tree-level accuracy, then Merging:kFactor2j is used to rescale the W+2 jet, W+3 jets and W+4 jets tree-level samples. We recommend to not include a K-factor rescaling of the tree-level samples.

    Let us turn to the production of NLO merged events. The first step in the procedure is to generate reweighted tree-level samples. This is implemented by using the following switch. This switch will allow the generation of the weight that should be applied to tree-level events in the NL3 merging scheme. Please note that, in order for this to work smoothly, the switch Merging:doNL3Loop and the switch Merging:doNL3Subt have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

    The weight of tree-level events can be accessed by calling the function double Info::mergingWeightNLO(). When printing (or histogramming) NLO merged events, this weight, multiplied with the estimated cross section of the current event sample, should be used as event weight (or weight of histogram bins). For Merging:doNL3Tree = on, the weight double Info::mergingWeightNLO() contains the CKKW-L weight, subtracted, if necessary, by αs0- and αs1-terms. This weight can become negative. As an example, imagine we attempt an NLO merging of W + 0 jet and W + 1 jet at NLO accuracy, and with W + 2 jets at tree-level accuracy. This weight will then be

      Info::mergingWeightNLO() = CKKW-L-weight for zero jets - αs0-terms - αs1-terms for events in the zero-jet sample,

      Info::mergingWeightNLO() = CKKW-L-weight for one jet - αs0-terms - αs1-terms for events in the one-jet sample, and

      Info::mergingWeightNLO() = CKKW-L-weight for two jets for events in the two-jet sample.

    After the tree-level events have been reweighted, main87.cc will move on to process the POWHEG NLO input. This is done by switching to the following flag. This switch will allow the processing of POWHEG NLO events in the NL3 merging scheme. Please note that, in order for this to work smoothly, the switch Merging:doNL3Tree and the switch Merging:doNL3Subt have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

    Also in this case, the NLO merging weight of the events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doNL3Loop = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in Lon13). After the processing of POWHEG NLO events, main87.cc continues by generating explicit phase space subtractions. This is facilitated by the following switch. This switch will allow the processing of tree-level events, to produce explicit phase space subtractions in the NL3 merging scheme. Please note that, in order for this to work smoothly, the switch Merging:doNL3Tree and the switch Merging:doNL3Loop have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested. Furthermore, it is necessary to set the value of Merging:nRecluster to one.

    These contributions are necessary because we have implemented the "inclusive scheme" of Lon13 in Pythia. The benefit of this scheme is the user does not have to intrusively change the POWHEG-BOX program to implement very particular cuts. Let us explain this comment with an example (a more detailed explanation of the idea is given in Appendix A.2 of Lon13). When generating W + 0 jet events with the POWHEG-BOX program, the output LHE files will contain W + 1 jet real emission events. Some of these events will contain a jet above the merging scale. However, in NLO merging methods, such configurations have already been included by a separate W + 1 jet sample. Thus, to avoid counting such events twice, we have to remove the configurations from the POWHEG-BOX output. We choose to remove such events by explicit subtraction.

    As always, the NLO merging weight of the events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doNL3Subt = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in Lon13).

    After these steps, all necessary events for NL3 merging have been produced. main87.cc finishes by returning the NL3-merged total cross section.


    UNLOPS merging with main88.cc

    UNLOPS-style NLO merging in Pythia is illustrated by the sample main program main88.cc, which relies on an input file (e.g. main88.cmnd) for Pythia settings. As for all merging methods in Pythia, main88.cc requires LHE input files. To use main88.cc without any changes, these input files should follow the naming convention name_tree_#nAdditionalJets.lhe (for tree-level samples) and name_powheg_#nAdditionalJets.lhe (for POWHEG NLO samples). main88.cc produces HepMC event output, which can e.g. be analysed with RIVET, or used as input for detector simulations. For users not familiar with HepMC output, it is of course possible remove the HepMC code in the sample program, and use Pythia's histogramming routines instead. Histograms should then be filled as indicated for the histPTFirstSum histograms in main84.cc, i.e. using weightNLO*normhepmc.

    As for NL3, it is not necessary to change main88.cc if the user is only interested in changing standard settings. Thus, if the user only wants to change the number of requested events (Main:numberOfEvents), the hard process (Merging:Process), the merging scale value (Merging:TMS) and the maximal number of additional tree-level or NLO-accuracte jets (Merging:nJetMax and Merging:nJetMaxNLO, respectively), and HepMC output is desired, then there is no need to change the main88.cc code. The input LHE files are also part of the (command line) input for main88.exe. The default settings in main88.cmnd are intended to work with the (very short) sample LHEF inputs (w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and w_production_powheg_0.lhe, w_production_powheg_1.lhe). For these input files, the main88.exe executable can be run with the command

    ./main88.exe main88.cmnd w_production myhepmc.hepmc

    to produce a file myhepmc.hepmc of UNLOPS merged HepMC event output. Please refrain from adding input switches than invoke any other merging scheme (e.g. Merging:doKTMerging) into the input file that you want to use in conjunction with main88.cc.

    In the following, we will explain main88.cc in depth. To not be overly repetitive, we will at times refer to the relevant parts in the discussion of main87.cc. Users who are willing to accept the default choices do not need to know all details, but are still encouraged to read further.

    Program flow

    main88.cc can be divided into five steps:

             1. Estimate the cross section for tree-level and NLO samples after the merging scale cut.

             2. Produce reweighted tree-level events, which do not contain αs0- and αs1-terms.

             3. Add POWHEG NLO events.

             4. Subtract integrated, reweighted tree-level events, to ensure that the inclusive NLO cross section remains intact upon inclusion of multi-jet tree-level events.

             5. Subtract integrated POWHEG NLO events, to ensure that the inclusive NLO cross section remains intact upon inclusion of multi-jet tree-level events.

    The estimation of cross sections after the application of the merging scale cut is nearly identical to the first step in main87.cc, and we refer to the first paragraph of the "Program flow" discussion for main87.cc for details. For main88.cc, the flags Merging:doUNLOPSTree or Merging:doUNLOPSLoop supply the merging scale definition used in the cross section estimation.

    After the cross section estimation step, main88.cc proceeds to perform the actual NLO merging. The discussion of K-factors given in the NL3 section (i.e. of Merging:kFactor0j, Merging:kFactor1j and Merging:kFactor2j) also applies to main88.cc. Although UNLOPS is considerably more stable than NL3 upon changing the K-factors, we do not recommend the use of K-factors.

    The production of UNLOPS-merged events with main88.cc starts by generating reweighted tree-level events. The processing of tree-level events can be invoked by setting the following flag. This switch will allow the generation of the weight that should be applied to tree-level events in the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSLoop, Merging:doUNLOPSSubt and Merging:doUNLOPSSubtNLO have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

    The weight of tree-level events is returned by the function double Info::mergingWeightNLO(). When printing (or histogramming) NLO merged events, this weight, multiplied with the estimated cross section of the current event sample, should be used as event weight (or weight of histogram bins). For Merging:doUNLOPSTree = on, the weight double Info::mergingWeightNLO() contains the UMEPS weight, subtracted, if necessary, by αs0- and αs1-terms. This weight can become negative. As an example, assume that we attempt an UNLOPS merging of W + 0 jet and W + 1 jet at NLO accuracy, and with W + 2 jets at tree-level accuracy. This weight will then be

      Info::mergingWeightNLO() = UMEPS-weight for one jet - αs0-terms - αs1-terms for events in the one-jet sample, and

      Info::mergingWeightNLO() = UMEPS-weight for two jets for events in the two-jet sample.

    After reweighted tree-level events have been generated, main88.cc processes the POWHEG NLO input files. This is facilitated by the following switch. This switch will allow the processing of POWHEG NLO events in the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSTree, Merging:doUNLOPSSubt and Merging:doUNLOPSSubtNLO have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

    The NLO merging weight of the events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doUNLOPSLoop = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in Lon13).

    After processing the POWHEG NLO events, main88.cc continues by generating the reweighted subtraction terms of UMEPS. This part is implemented by setting the following flag. This switch will allow the processing of tree-level events, to produce UMEPS subtraction terms for the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSTree, Merging:doUNLOPSLoop and Merging:doUNLOPSSubtNLO have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested. Furthermore, it is necessary to set the value of Merging:nRecluster to one.

    By using this switch, main88.cc ensures that the inclusive cross section is preserved. At variance with UMEPS however, the event weight contains the UMEPS weight, subtracted, if necessary, by αs+0- and αs1-terms. Otherwise, αsn+0- and αsn+1-terms of the UMEPS procedure would be introduced, although our goal is to describe all αsn+0- and αsn+1-terms by n-jet POWHEG input. The weight of these integrated, subtractive tree-level events is, as always, returned by the function double Info::mergingWeightNLO(). When printing (or histogramming) NLO merged events, this weight, multiplied with the estimated cross section of the current event sample, and with -1, should be used as event weight (or weight of histogram bins). As for the case of tree-level events in UNLOPS, this weight can become negative. For the example given before, i.e. attempting an UNLOPS merging of W + 0 jet and W + 1 jet at NLO accuracy, and with W + 2 jets at tree-level accuracy, this weight will be

      Info::mergingWeightNLO() = UMEPS-weight for the integrated one-jet sample - αs0-terms - αs1-terms for events in the integrated one-jet sample, and

      Info::mergingWeightNLO() = UMEPS-weight for the integrated two-jet sample for events in the integrated two-jet sample.

    This choice of weights already incorporates the fact that we have implemented the "inclusive scheme" of Lon13, meaning that the "explicit phase space subtractions" of NL3 are (partially) included though these weights.

    To ensure that the NLO inclusive cross section is unchanged, UNLOPS further requires the introduction of another sample. If POWHEG NLO events with one or more jets are included, it is necessary to subtract these samples in an integrated form. In main88.cc, this is done by setting the following flag. This switch will allow the processing of POWHEG NLO events, to produce NLO subtraction terms for the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSTree, Merging:doUNLOPSLoop and Merging:doUNLOPSSubt have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested. Furthermore, it is necessary to set the value of Merging:nRecluster to one.

    This sample also provides some "explicit phase space subtractions" of NL3, which are necessary because we implemented the "inclusive scheme" of Lon13. Let us again look at the example of UNLOPS merging of W + 0 jet and W + 1 jet at NLO accuracy. The integrated W + 1 jet NLO events, which are produced by the setting Merging:doUNLOPSSubtNLO = on, contain a tree-level part. This part will exactly cancel the real-emission events with one jet above the merging scale in the W + 0 jet NLO events.

    The NLO merging weight of these "integrated" events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doUNLOPSSubtNLO = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in Lon13).

    After these five steps (estimation of cross sections, tree-level processing, POWHEG processing, integrated tree-level processing, integrated POWHEG processing) we have produced a UNLOPS-merged HepMC event file. main88.cc finishes by returning the UNLOPS-merged total cross section.


    NLO merging and "exclusive" NLO inputs

    Currently, both sample main programs for NLO merging (main87.cc and main88.cc) are intended for "inclusive" POWHEG input. Inclusive input means that all real emission phase space points are included in the POWHEG output files. In order to avoid double counting with higher-multiplicity matrix elements, it is then necessary remove phase space points with too many jets from the real-emission configurations. This can be done by introducing explicit phase space subtractions. Another way of removing the undesired configurations is by implementing a cut in the NLO generator. This is not a completely trivial task, since it is necessary to ensure numerical stability and the correct cancellation of (finite) dipole regularisation terms. One way of producing such exclusive NLO output is by setting the (tree-level) real-emission matrix element in the NLO generator to zero if the real-emission phase space point contains too many jets above the merging scale. This will however not be numerically stable for too low merging scale values.

    We should be very clear that using exclusive NLO input is not recommended, since it requires hacking the NLO generator. Only for the expert user, we briefly summarise the necessary changes for using exclusive NLO input.

    For the moment, assume that the NLO input has been produced in an "exclusive" way. This input can then be processed by some trivial changes in main87.cc: estimate the cross section for tree-level and NLO samples after the merging scale cut, still using inclusive NLO samples, remove the last part of main87.cc, i.e. the part that produces explicit phase space subtractions, and use the exclusive NLO files as input files for the processing of "POWHEG NLO files".

    The changes to main88.cc (implementing UNLOPS) are slightly more complicated. This is the case because the weights of integrated tree-level samples change when using exclusive input, as can be seen in Appendix D in Lon13. The correct weights can be produced by Pythia by using the following flag. This flag allows the UNLOPS machinery to produce the event weights if exclusive NLO input is used for the merging. This flag should be set to "on" directly after the cross section estimates have been produced.

    Then, it is necessary to add code for processing another sample to main88.cc, since when using exclusive inputs, it is also necessary to enforce two integrations on tree-level events (the "↑"-contributions in Appendix D of Lon13). This can be achieved by adding the following code at the end of main88.cc.

      cout << endl << endl << endl;
      cout << "Shower subtractive events" << endl;
    
      // Switch on processing of counter-events.
      pythia.settings.flag("Merging:doUNLOPSTree",false);
      pythia.settings.flag("Merging:doUNLOPSLoop",false);
      pythia.settings.flag("Merging:doUNLOPSSubt",true);
      pythia.settings.flag("Merging:doUNLOPSSubtNLO",false);
      pythia.settings.mode("Merging:nRecluster",2);
    
      nMaxCT         = nMaxNLO+1;
      njetcounterCT  = nMaxCT;
      iPathSubt      = iPath + "_tree";
    
      while(njetcounterCT >= 2){
    
        // From njet, choose LHE file
        stringstream in;
        in   << "_" << njetcounterCT << ".lhe";
        string LHEfile = iPathSubt + in.str();
    
        cout << endl << endl << endl
             << "Start subtractive treatment for " << njetcounterCT << " jets\n"
             << "Recluster at least 2 times" << endl;
    
        pythia.readString("Beams:frameType = 4"); 
        pythia.settings.word("Beams:LHEF", LHEfile);  
        pythia.settings.mode("Merging:nRequested", njetcounterCT);
        pythia.init();
        // Remember position in vector of cross section estimates.
        int iNow = sizeLO-1-njetcounterCT;
    
        // Start generation loop
        for( int iEvent=0; iEvent < nEvent; ++iEvent ){
    
          // Generate next event
          if( !pythia.next() ) {
            if( pythia.info.atEndOfFile() ) break;
            else continue;
          }
    
          // Get event weight(s).
          double weightNLO  = pythia.info.mergingWeightNLO();
          double evtweight  = pythia.info.weight();
          weightNLO        *= evtweight;
          // Do not print zero-weight events.
          if ( weightNLO == 0. ) continue; 
    
          // Construct new empty HepMC event.
          HepMC::GenEvent* hepmcevt = new HepMC::GenEvent();
          // Get correct cross section from previous estimate.
          double normhepmc = -1*xsecLO[iNow] / nAcceptLO[iNow];
          // Set hepmc event weight.
          hepmcevt->weights().push_back(weightNLO*normhepmc);
          // Fill HepMC event.
          ToHepMC.fill_next_event( pythia, hepmcevt );
          // Add the weight of the current event to the cross section.
          sigmaTotal += weightNLO*normhepmc;
          errorTotal += pow2(weightNLO*normhepmc);
          // Report cross section to hepmc.
          HepMC::GenCrossSection xsec;
          xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 );
          hepmcevt->set_cross_section( xsec );
          // Write the HepMC event to file. Done with it.
          ascii_io << hepmcevt;
          delete hepmcevt;
    
        } // end loop over events to generate
    
        // print cross section, errors
        pythia.stat();
    
        // Restart with ME of a reduced the number of jets
        if( njetcounterCT > 2 )
          njetcounterCT--;
        else
          break;
    
      }
    
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0.39818e+00 0.27678e+00 0.19886e+00 0.14747e+00 0.11219e+00 0.88115e-01 0.69207e-01 0.55333e-01 0.45004e-01 0.37074e-01 0.30869e-01 0.25961e-01 0.22027e-01 0.18795e-01 0.16159e-01 0.13990e-01 0.12178e-01 0.10663e-01 0.94136e-02 0.83073e-02 0.72989e-02 0.62905e-02 0.52821e-02 0.42737e-02 0.32653e-02 0.22569e-02 0.12485e-02 0.24007e-03 0.10741e+00 0.82476e-01 0.57601e-01 0.39069e-01 0.27459e-01 0.19973e-01 0.14932e-01 0.11559e-01 0.89413e-02 0.70507e-02 0.56636e-02 0.46124e-02 0.37994e-02 0.31635e-02 0.26590e-02 0.22482e-02 0.19164e-02 0.16457e-02 0.14215e-02 0.12355e-02 0.10834e-02 0.94947e-03 0.82789e-03 0.70632e-03 0.58474e-03 0.46316e-03 0.34159e-03 0.22001e-03 0.98433e-04 -0.23143e-04 pythia8-8.1.80.orig/xmldoc/MatchingAndMerging.xml0000444000175000017500000001723612217346304020040 0ustar sunsun

    Matching and Merging

    Starting from a Born-level leading-order (LO) process, higher orders can be included in various ways. The three basic approaches would be
    • A formal order-by-order perturbative calculation, in each order higher including graphs both with one particle more in the final state and with one loop more in the intermediate state. This is accurate to the order of the calculation, but gives no hint of event structures beyond that, with more particles in the final state. Today next-to-leading order (NLO) is standard, while next-to-next-to-leading order (NNLO) is coming. This approach thus is limited to few orders, and also breaks down in soft and collinear regions, which makes it unsuitable for matching to hadronization.
    • Real emissions to several higher orders, but neglecting the virtual/loop corrections that should go with it at any given order. Thereby it is possible to allow for topologies with a large and varying number of partons, at the prize of not being accurate to any particular order. The approach also opens up for doublecounting, and as above breaks down in soft and colliner regions.
    • The parton shower provides an approximation to higher orders, both real and virtual contributions for the emission of arbitrarily many particles. As such it is less accurate than either of the two above, at least for topologies of well separated partons, but it contains a physically sensible behaviour in the soft and collinear limits, and therefore matches well onto the hadronization stage.
    Given the pros and cons, much of the effort in recent years has involved the development of different prescriptions to combine the methods above in various ways.

    The common traits of all combination methods are that matrix elements are used to describe the production of hard and well separated particles, and parton showers for the production of soft or collinear particles. What differs between the various approaches that have been proposed are which matrix elements are being used, how doublecounting is avoided, and how the transition from the hard to the soft regime is handled. These combination methods are typically referred to as "matching" or "merging" algorithms. There is some confusion about the distinction between the two terms, and so we leave it to the inventor/implementor of a particular scheme to choose and motivate the name given to that scheme.

    PYTHIA comes with methods, to be described next, that implement or support several different kind of algorithms. The field is open-ended, however: any external program can feed in Les Houches events that PYTHIA subsequently showers, adds multiparton interactions to, and hadronizes. These events afterwards can be reweighted and combined in any desired way. The maximum pT of the shower evolution is set by the Les Houches scale, on the one hand, and by the values of the SpaceShower:pTmaxMatch, TimeShower:pTmaxMatch and other parton-shower settings, on the other. Typically it is not possible to achieve perfect matching this way, given that the PYTHIA pT evolution variables are not likely to agree with the variables used for cuts in the external program. Often one can get close enough with simple means but, for an improved matching, User Hooks can be inserted to control the steps taken on the way, e.g. to veto those parton shower branchings that would doublecount emissions included in the matrix elements.

    Zooming in from the "anything goes" perspective, the list of relevent approaches actively supported is as follows.

    • For many/most resonance decays the first branching in the shower is merged with first-order matrix elements Ben87, Nor01. This means that the emission rate is accurate to NLO, similarly to the POWHEG strategy (see below), but built into the timelike showers. The angular orientation of the event after the first emission is only handled by the parton shower kinematics, however. Needless to say, this formalism is precisely what is tested by Z^0 decays at LEP1, and it is known to do a pretty good job there.
    • Also the spacelike showers contain a correction to first-order matrix elements, but only for the one-body-final-state processes q qbar -> gamma^*/Z^0/W^+-/h^0/H^0/A0/Z'0/W'+-/R0 Miu99 and g g -> h^0/H^0/A0, and only to leading order. That is, it is equivalent to the POWHEG formalism for the real emission, but the prefactor "cross section normalization" is LO rather than NLO. Therefore this framework is less relevant, and has been superseded the following ones.
    • The POWHEG strategy Nas04 provides a cross section accurate to NLO. The hardest emission is constructed with unit probability, based on the ratio of the real-emission matrix element to the Born-level cross section, and with a Sudakov factor derived from this ratio, i.e. the philosophy introduced in Ben87.
      While POWHEG is a generic strategy, the POWHEG BOX Ali is an explicit framework, within which several processes are available. Potential emissions are ordered in a transverse-momentum-related variable. The LHA scale variable encodes this value for each event, and thereby sets the upper limit for subsequent shower emissions. There is a mismatch between the POWHEG BOX and the PYTHIA pT variables, however, which gives imperfections in the transition region Cor10. The proposed solution is to allow showers to cover the full phase space, but then veto emissions in the region already covered by the POWHEG BOX evolution. The code required for this can be found in examples/main31. While fairly general, the code would have to be modified to accommodate a different pT scale definition in the POWHEG BOX.
    • The other traditional approach for NLO calculations is the MC@NLO one Fri02. In it the shower emission probability, without its Sudakov factor, is subtracted from the real-emission matrix element to regularize divergences. It therefore requires a analytic knowledge of the way the shower populates phase space. Currently there is no MC@NLO implementation for PYTHIA 8, but one is in preparation by Paolo Torrielli and Stefano Frixione, for the aMC@NLO program Fre11. The global-recoil option of the PYTHIA final-state shower has been constructed in anticipation of its use for the above-mentioned subtraction.
    • Multi-jet merging in the CKKW-L approach Lon01 is directly available. Its implementation, relevant parameters and test programs are documented on a separate page.
    • Multi-jet matching in the MLM approach Man02, Man07 is also available, either based on the ALPGEN or on the Madgraph variant, and with input events either from ALPGEN or from Madgraph. For details see separate page.
    • Unitarised matrix element + parton shower merging (UMEPS) is directly available. Its implementation, relevant parameters and test programs are documented on a separate page.
    • Next-to-leading order multi-jet merging (in the NL3 and UNLOPS approaches) is directly available. Its implementation, relevant parameters and test programs are documented on a separate page.
    pythia8-8.1.80.orig/xmldoc/PhaseSpaceCuts.xml0000444000175000017500000003743312217346315017230 0ustar sunsun

    Phase Space Cuts

    PhaseSpace is base class for all hard-process phase-space generators, either generic 2 -> 1 or 2 -> 2 ones, or specialized ones like for elastic and diffractive scattering.

    In it, it is possible to constrain the kinematics of most processes. (Exceptions are "soft physics", i.e. minimum bias, elastic and diffractive processes. The Coulomb singularity for elastic scatterings, if simulated, is handled separately.) These constraints apply in the rest frame of the hard subprocess, and topologies normally would be changed e.g. by subsequent showering activity. The cross section of a process is adjusted to only correspond to the allowed phase space.

    The more particles in the final state, the more cuts could be applied. Here we have tried to remain with the useful minimum, however. More generic possibilities could be handled by the user hooks facility.

    Cuts in all processes

    The minimum invariant mass. The maximum invariant mass. A value below mHatMin means there is no upper limit.

    Cuts in 2 -> 1 processes

    When a resonance id is produced, the mMin(id) and mMax(id) methods restrict the allowed mass range of this resonance. Therefore the allowed range is chosen to be the overlap of this range and the mHatMin to mHatMax range above. Most resonances by default have no upper mass limit, so effects mainly concern the lower limit. Should there be no overlap between the two ranges then the process will be switched off.

    Cuts in 2 -> 2 processes

    The minimum invariant pT. The maximum invariant pT. A value below pTHatMin means there is no upper limit. Extra pT cut to avoid the divergences of some processes in the limit pT -> 0. Specifically, if either or both produced particles have a mass below pTHatMinDiverge then pT is limited from below by the larger of pTHatMin and pTHatMinDiverge. Allows masses to be selected according to Breit-Wigner shapes in 2 -> 2 processes, whenever particles have been declared with a nonvanishing width above the threshold below. In those cases also the limits below will be used for the mass selection. For 2 -> 1 processes the Breit-Wigner shape is part of the cross section itself, and therefore always included. The minimum width a resonance must have for the mass to be dynamically selected according to a Breit-Wigner shape, within the limits set below. Only applies when useBreitWigners is on; else the nominal mass value is always used.

    For a particle with a Breit-Wigner shape selected, according to the rules above and to the rules of the particle species itself, the mMin(id) and mMax(id) methods restrict the allowed mass range of the particle, just like for the 2 -> 1 processes.

    Cuts in 2 -> 3 processes

    There are two main classes of 2 -> 3 processes. One is the processes such as WW/ZZ-fusion Higgs production, i.e. q q -> q q H, where there are no special singularities associated with two partons in the final state being collinear, or even for pT -> 0. For this class, no further cuts have been introduced than those already available for 2 -> 2 processes. Specifically, for now all three are restricted exactly the same way by pTHatMin and pTHatMax. As above, Breit-Wigner mass ranges can be restricted.

    The other 2 -> 3 event class is QCD processes, such as g g -> g g g. Here the soft and collinear singularities play a major role, and the phase space generation and cuts have been adapted to this. For this class, an alternative set of cuts is used, as outlined in the following. First of all the three outgoing partons are ordered in falling pT, i.e. pT_3 > pT_4 > pT_5 (where the labeling 3, 4, 5 of the outgoing partons is random, i.e. unrelated to the order specified in the process name). The allowed ranges of pT_3 and pT_5 can be specified, but obviously pT_3max >= pT_5max and pT_3min >= pT_5min. The pT_4 is not constrained explicitly, but is constructed from the vector sum of pT_3 and pT_5, subject to the constraint that it has to lie between the two in magnitude. While the pT cuts take care of singularities collinear with the incoming beams, it is also necessary to handle final-state singularities, when two outgoing partons become collinear. This is done by requiring a minimal separation in R, where R^2 = (Delta eta)^2 + (Delta phi)^2. Finally, a note about efficiency. The QCD 2 -> 3 phase space is not set up to explicitly include mHat as one of the basic variables. Such a cut is only done after a phase space point is already selected, which means that a narrow mass choice will slow down the program appreciably. Also narrow pT_3 and pT_5 bins are likely to give inefficient generation, if it gives rise to significant indirect restrictions on pT_4. The minimum invariant pT of the highest-pT parton in QCD 2 -> 3 processes. The maximum invariant pT of the highest-pT parton in QCD 2 -> 3 processes A value below pTHat3Min means there is no upper limit. The minimum invariant pT of the lowest-pT parton in QCD 2 -> 3 processes. The maximum invariant pT of the lowest-pT parton in QCD 2 -> 3 processes A value below pTHat5Min means there is no upper limit. The minimum separation R in (eta, phi) space between any two outgoing partons in QCD 2 -> 3 processes.

    Cuts for a second hard process

    If you use the machinery that allows the generation of a specified second hard process then, by default, the same phase space cuts will be used for it as listed above. Optionally, however, you may use a second set of cuts, as described here. In this context "first" and "second" is merely a technical distinction; you are welcome e.g. to pick pT ranges such that the second interaction always has a larger pT than the first. By default use the same cuts for a second hard process as for the first. If off then instead use the mass and pT cuts below, where relevant. (The other cuts above still remain the same.) The minimum invariant mass for a second interaction, if separate. The maximum invariant mass for a second interaction, if separate. A value below mHatMin means there is no upper limit. The minimum invariant pT for a second interaction, if separate. The maximum invariant pT for a second interaction, if separate. A value below pTHatMin means there is no upper limit.

    Generation strategy and documentation

    During the initialization stage a simplified function is found, that is intended to be above the true cross-section behaviour over the whole of phase space. It is chosen to be easily integrable and invertible. That way a trial phase space point can be selected according this simple function, and then be accepted by the ratio of true to the simple function. For a good efficiency the ratio should be close to unity, yet never above it. This constrains the absolute normalization of the simple function. The initial search may fail to find the phase space point where the true-to-simple ratio is maximal, however. This then can lead to subsequent maximum violations, where the ratio is above unity. Two alternative strategies are implemented to handle such situations, see below. Possibility to print information on the search for phase-space coefficients that (in a multichannel approach) provides an analytical upper envelope of the differential cross section, and the corresponding upper estimate of the cross section. Of interest for crosschecks by expert users only. Possibility to print information whenever the assumed maximum differential cross section of a process is violated, i.e. when the initial maximization procedure did not find the true maximum. Also, should negative cross sections occur, print whenever a more negative value is encountered. Strategy for handling cases where a larger cross section is obtained during the event generation than was assumed at initialization, i.e. when a violation occurs.
    off:each event comes with a weight, which normally is unity (as a consequence of the acceptance/rejection step), and is found in Info::weight(). For events which exceed the maximum instead the true-to-simple ratio is stored as event weight, which then is above unity. If the user so wishes this weight can then be carried along when event properties are histogrammed. Since normally such violations should be rare and not too much above unity one could expect most users to ignore such issues be default. Should maximum violations turn out to be frequent (visible in the Pythia::statistics() output) the option exists to use the information.
    on:the maximum is increased whenever it is exceeded. Thus events generated after this point will be "correctly" distributed, while ones generated previously obviously then have had too high a relative weight. If violations occur early on and/or are small this strategy should do a good job of correcting to the desired phase-space distribution. This strategy may be more convenient for the normal user, who would not wish to worry about event weights. It does have the disadvantage that the raised maximum introduces an extra amount of "history memory" to the generation sequence, so that it becomes less easy to save-and-restore the random-number state for debugging purposes.

    Reweighting of 2 -> 2 processes

    Events normally come with unit weight, i.e. are distributed across the allowed phase space region according to the appropriate differential cross sections. Sometimes it may be convenient to have an uneven distribution of events. The classical example here is that many cross sections drop off with transverse momentum pT, such that few events are generated at large pT scales. If one wants to plot the pT cross section, and all that comes with it, the statistical error will then degrade with increasing pT where fewer events end up.

    One solution is to split the full pT range into several separate subranges, where the events of each subsample obtains a different overall normalization. Specifically, if you generate a comparable number of events in each pT bin, such that larger pT bins are oversampled, these bins come with a correspondingly reduced overall weight, that needs to be taken into account when the bins are combined. The other is to have a continuously increasing oversampling of events at larger pT scales, which is compensated by a continuously decreasing weight for the event.

    Both of these solutions are supported. Specifically, for 2 -> 2 processes, the pTHat scale offers a convenient classification of the event. (Of course, two events starting out from the same pTHat scale will experience different parton shower evolutions, etc., and may therefore look quite different at the end.) The two cuts PhaseSpace:pTHatMin and PhaseSpace:pTHatMax therefore offers a way to slice a pT range into subranges, see e.g. main08.cc. Alternatively the User Hooks machinery offers the possibility for you to define your own reweighting of phase space sampling, with a corresponding event weight, with UserHooks::canBiasSelection and related methods.

    As a simplified option, we here offer the possibility to bias the 2 -> 2 sampling by a power of pTHat, then with events having a weight the inverse of this. This fast track will only work under a number of strict conditions, implemented to reduce the risk of abuse. (Whereas a UserHooks setup can be more flexible.) Specifically it will work if only high-pT 2 -> 2 processes already implemented in PYTHIA are requested, notably the HardQCD ones. That is, you cannot mix with 2 -> 1 or 2 -> 3 processes, nor with external processes (notably Les Houches input) or SoftQCD ones, and you cannot use the option to define a second hard process in the same event. Furthermore you have to be careful about the choice of PhaseSpace:pTHatMin, since a pTHat = 0 event would come with an infinite weight. Possibility to switch on a biased phase space sampling, with compensatingly weighted events, for 2 -> 2 processes. Can only be used under the specific conditions explained in the paragraph above; under other conditions the initialization will abort. If the above flag is on, then a 2 -> 2 process at a scale pTHat will be oversampled in phase space by an amount (pTHat/pTRef)^pow, where you set the power pow here. Events are assigned a compensating weight the inverse of this, i.e. Info::weight() will return (pTRef/pTHat)^pow. This weight should then be used in the histogramming of event properties. The final overall normalization also involves the Info::weightSum() value. The reference scale pTRef introduced above, such that events with this pTHat obtain unit weight in the reweighting procedure. The value of this parameter has no impact on the final result of the reweighting procedure, but is only there for convenience, i.e. to give "reasonably-sized" weights. pythia8-8.1.80.orig/xmldoc/QCDProcesses.xml0000444000175000017500000002574012217346316016652 0ustar sunsun

    QCD Processes

    This section is subdivided into soft and hard QCD processes, with open charm and bottom production set aside as a special part of the latter, and three-jet topologies as a special subset. Kindly note that there is a considerable amount of overlap between the soft and hard process classes, so that you are likely to double-count if you include both in a run.

    Soft QCD processes

    As a rule, the processes in this class should not be mixed with the simulation of other processes. All by themselves, they are intended to represent the total cross section of hadron collisions, with the exception of the "rare processes" that one wishes to study separately. In particular, jet physics at all scales occurs as part of the minimum-bias description.

    We here use the "minimum bias" expression as a shorthand for inelastic, nondiffractive events. Strictly speaking, "minimum bias" represents an experimental procedure of accepting "everything", with some non-universal cuts to exclude elastic and diffractive topologies. In practice, the experimental minimum-bias sample may then contain some contamination of what is in PYTHIA classified as diffractive, especially (high-mass) double diffractive.

    Some options to modify these cross sections are found on the Total Cross Sections page. Common switch for the group of all soft QCD processes, as listed separately in the following. The inelastic nondiffrative part of the total cross section, i.e. what would often be called the "minimum-bias component". The formalism is based on an eikonalized description of all the hard QCD processes, so includes them in combination with low-pT events. Code 101.
    Since the current description is handled by the multiparton-interactions machinery as part of the parton-level processing, no hard process at all is defined at the process-level part of the event generation. Fortunately, in this case a special codeSub() method provides information on the first, i.e. hardest, subprocess selected by the multiparton-interactions machinery. Note: this flag was precviously named SoftQCD:minBias, since it is almost equivalent to the minimum-bias component of the total cross section. It has invited some confusion, however, since "minimum-bias" usually refers to the experimental procedure, while "(inelastic) non-diffractive" better relates to the way events are generated in the program code. (Although also what separates diffractive from nondiffractive physics can be a matter of definition.) For backwards compatibility the SoftQCD:minBias name can be used as an alternative to SoftQCD:nonDiffractive for some time yet.
    Elastic scattering A B -> A B. Code 102. It is possible to include Coulomb corrections, but by default this is off. Single diffractive scattering A B -> X B and A B -> A X. See page on Diffraction for details. Codes 103 and 104. Double diffractive scattering A B -> X_1 X_2. See page on Diffraction for details. Code 105. Central diffractive scattering A B -> A X B (a.k.a. double-Pomeron exchange, DPE). See pages on Total Cross Sections and on Diffraction for details. In particular note the SigmaTotal:zeroAXB flag, which is off in most tunes, and that therefore would need to be reset to on after the selection of a tune (even the default one). Code 106. All of the above processes, except for elastic. Codes 101, 103, 104, 105 and 106.

    Hard QCD processes

    This group contains the processes for QCD jet production above some minimum pT threshold. The pT_min cut cannot be put too low, or else unreasonably large jet cross sections will be obtained. This is because the divergent perturbative QCD cross section is used in this process group, without any regularization modifications. An eikonalized description, intended to be valid at all pT, is instead included as part of the multiparton-interactions framework, specifically in SoftQCD:nonDiffractive above. Warning 1: you must remember to set the PhaseSpace:pTHatMin value if you use any of these processes; there is no sensible default. Warning 2: you must not mix processes from the SoftQCD and HardQCD process groups, since this is likely to lead to double-counting. Common switch for the group of all hard QCD processes, as listed separately in the following. Scatterings g g -> g g. Code 111. Scatterings g g -> q qbar, where q by default is a light quark (u, d, s) (see below). Code 112. Scatterings q g -> q g and qbar g -> qbar g. Code 113. Scatterings q q' -> q q', q qbar' -> q qbar', qbar qbar' -> qbar qbar', where q' and q may agree, but the outgoing flavours equals the incoming ones Code 114. Scatterings q qbar -> g g. Code 115. Scatterings q qbar -> q' qbar', where q' by default is a light quark (u, d, s) (see below). Code 116. Number of allowed outgoing new quark flavours in the above g g -> q qbar and q qbar -> q' qbar' processes, where quarks are treated as massless in the matrix-element expressions (but correctly in the phase space). It is thus assumed that c cbar and b bbar are added separately with masses taken into account, using the processes below. A change to 4 would also include c cbar in the massless approximation, etc. In order to avoid double-counting the processes below should then not be used simultaneously.

    Hard QCD processes: heavy-flavour subset

    These processes form a natural part of the above class, but can also be generated separately. Formally the heavy-quark mass makes these matrix elements finite in the pT -> 0 limit, but at high energies one may still question the validity of the expressions at low pT values, like for the other hard-QCD processes. Also as above, an eikonalized description, intended to be valid at all pT, is included as part of the multiparton-interactions framework.
    Note that the processes below only represent the "tip of the iceberg" of charm and bottom production at high energies, where flavour excitation and shower branchings provide major additional sources. All these sources come together in the descriptions offered by SoftQCD:nonDiffractive and HardQCD:all. Scatterings g g -> c cbar. Code 121. Scatterings q qbar -> c cbar. Code 122. Sum of the previous two event types. Codes 121 and 122. Scatterings g g -> b bbar. Code 123. Scatterings q qbar -> b bbar. Code 124. Sum of the previous two event types. Codes 123 and 124.

    Hard QCD three-parton processes

    Three-parton final states are generated by showers off two-parton processes. Topologies then cannot be specified beforehand, beyond what is provided by the two-parton hard process. For some checks it may be convenient to have access to the dedicated three-parton final states, which is what this set of processes allows. Cross sections have been taken from Ber81.
    Note that the processes in this section are not affected by the HardQCD:all switch. In fact, it would be double-counting to include both the HardQCD:all and the HardQCD:3parton processes in a run or study.
    Warning: this section is still incomplete, e.g. the selection of colour flow is very simple, and so it should only be used with caution. Common switch for the group of all hard QCD processes with three partons in the final state, as listed separately in the following. Scatterings g g -> g g g. Code 131. Scatterings q qbar -> g g g. Code 132. Scatterings q g -> q g g and qbar g -> qbar g g. Code 133. Scatterings q q' -> q q' g, q qbar' -> q qbar' g, and qbar qbar' -> qbar qbar' g. Code 134. Scatterings q q -> q q g and qbar qbar -> qbar qbar g (q qbar -> q qbar g scatterings are considered separately below, see HardQCD:qqbar2qqbargSame). Code 135. Scatterings q qbar -> q' qbar' g, where q' by default is a light quark (u, d, s) (see HardQCD:nQuarkNew above). Code 136. Scatterings q qbar -> q qbar g. Code 137. Scatterings g g -> q qbar g, where q by default is a light quark (u, d, s) (see HardQCD:nQuarkNew above). Code 138. Scatterings q g -> q q' qbar' and qbar g -> qbar qbar' q', where q' by default is a light quark (u, d, s) (see HardQCD:nQuarkNew above). Code 139. Scatterings q g -> q q qbar and qbar g -> qbar qbar q. Code 140.
    pythia8-8.1.80.orig/xmldoc/Diffraction.xml0000444000175000017500000004302212217346302016570 0ustar sunsun

    Diffraction

    Introduction

    Diffraction is not well understood, and several alternative approaches have been proposed. Here we follow a fairly conventional Pomeron-based one, in the Ingelman-Schlein spirit Ing85, but integrated to make full use of the standard PYTHIA machinery for multiparton interactions, parton showers and hadronization Nav10,Cor10a. This is the approach pioneered in the PomPyt program by Ingelman and collaborators Ing97.

    For ease of use (and of modelling), the Pomeron-specific parts of the generation are subdivided into three sets of parameters that are rather independent of each other:
    (i) the total, elastic and diffractive cross sections are parametrized as functions of the CM energy, or can be set by the user to the desired values, see the Total Cross Sections page;
    (ii) once it has been decided to have a diffractive process, a Pomeron flux parametrization is used to pick the mass of the diffractive system(s) and the t of the exchanged Pomeron, see below;
    (iii) a diffractive system of a given mass is classified either as low-mass unresolved, which gives a simple low-pT string topology, or as high-mass resolved, for which the full machinery of multiparton interactions and parton showers are applied, making use of Pomeron PDFs.
    The parameters related to multiparton interactions, parton showers and hadronization are kept the same as for normal nondiffractive events, with only one exception. This may be questioned, especially for the multiparton interactions, but we do not believe that there are currently enough good diffractive data that would allow detailed separate tunes.

    The above subdivision may not represent the way "physics comes about". For instance, the total diffractive cross section can be viewed as a convolution of a Pomeron flux with a Pomeron-proton total cross section. Since neither of the two is known from first principles there will be a significant amount of ambiguity in the flux factor. The picture is further complicated by the fact that the possibility of simultaneous further multiparton interactions ("cut Pomerons") will screen the rate of diffractive systems. In the end, our set of parameters refers to the effective description that emerges out of these effects, rather than to the underlying "bare" parameters.

    In the event record the diffractive system in the case of an excited proton is denoted p_diffr, code 9902210, whereas a central diffractive system is denoted rho_diffr, code 9900110. Apart from representing the correct charge and baryon numbers, no deeper meaning should be attributed to the names.

    Pomeron flux

    As already mentioned above, the total diffractive cross section is fixed by a default energy-dependent parametrization or by the user, see the Total Cross Sections page. Therefore we do not attribute any significance to the absolute normalization of the Pomeron flux. The choice of Pomeron flux model still will decide on the mass spectrum of diffractive states and the t spectrum of the Pomeron exchange. Parametrization of the Pomeron flux f_Pom/p( x_Pom, t).

    In options 3 and 4 above, the Pomeron Regge trajectory is parametrized as alpha(t) = 1 + epsilon + alpha' t The epsilon and alpha' parameters can be set separately: The Pomeron trajectory intercept epsilon above. For technical reasons epsilon > 0 is necessary in the current implementation. The Pomeron trajectory slope alpha' above.

    When option 5 is selected, the following parameters of the MBR model Cie12 are used: the parameters of the Pomeron trajectory. the Pomeron-proton coupling, and the total Pomeron-proton cross section. the lowest value of the mass squared of the dissociated system. the minimum width of the rapidity gap used in the calculation of Ngap(s) (flux renormalization). the minimum width of the rapidity gap used in the calculation of cross sections, i.e. the parameter dy_S, which suppresses the cross section at low dy (non-diffractive region). the parameter sigma_S, used for the cross section suppression at low dy (non-diffractive region).

    Separation into low and high masses

    Preferably one would want to have a perturbative picture of the dynamics of Pomeron-proton collisions, like multiparton interactions provide for proton-proton ones. However, while PYTHIA by default will only allow collisions with a CM energy above 10 GeV, the mass spectrum of diffractive systems will stretch to down to the order of 1.2 GeV. It would not be feasible to attempt a perturbative description there. Therefore we do offer a simpler low-mass description, with only longitudinally stretched strings, with a gradual switch-over to the perturbative picture for higher masses. The probability for the latter picture is parametrized as P_pert = P_max ( 1 - exp( (m_diffr - m_min) / m_width ) ) which vanishes for the diffractive system mass m_diffr < m_min, and is 1 - 1/e = 0.632 for m_diffr = m_min + m_width, assuming P_max = 1. The abovementioned threshold mass m_min for phasing in a perturbative treatment. If you put this parameter to be bigger than the CM energy then there will be no perturbative description at all, but only the older low-pt description. The abovementioned threshold width m_width. The abovementioned maximum probability P_max.. Would normally be assumed to be unity, but a somewhat lower value could be used to represent a small nonperturbative component also at high diffractive masses.

    Low-mass diffraction

    When an incoming hadron beam is diffractively excited, it is modeled as if either a valence quark or a gluon is kicked out from the hadron. In the former case this produces a simple string to the leftover remnant, in the latter it gives a hairpin arrangement where a string is stretched from one quark in the remnant, via the gluon, back to the rest of the remnant. The latter ought to dominate at higher mass of the diffractive system. Therefore an approximate behaviour like P_q / P_g = N / m^p is assumed. The abovementioned normalization N for the relative quark rate in diffractive systems. The abovementioned mass-dependence power p for the relative quark rate in diffractive systems.

    When a gluon is kicked out from the hadron, the longitudinal momentum sharing between the the two remnant partons is determined by the same parameters as above. It is plausible that the primordial kT may be lower than in perturbative processes, however: The width of Gaussian distributions in p_x and p_y separately that is assigned as a primordial kT to the two beam remnants when a gluon is kicked out of a diffractive system. The choice of longitudinal and transverse structure of a diffractive beam remnant for a kicked-out gluon implies a remnant mass m_rem distribution (i.e. quark plus diquark invariant mass for a baryon beam) that knows no bounds. A suppression like (1 - m_rem^2 / m_diff^2)^p is therefore introduced, where p is the diffLargeMassSuppress parameter.

    High-mass diffraction

    The perturbative description need to use parton densities of the Pomeron. The options are described in the page on PDF Selection. The standard perturbative multiparton interactions framework then provides cross sections for parton-parton interactions. In order to turn these cross section into probabilities one also needs an ansatz for the Pomeron-proton total cross section. In the literature one often finds low numbers for this, of the order of 2 mb. These, if taken at face value, would give way too much activity per event. There are ways to tame this, e.g. by a larger pT0 than in the normal pp framework. Actually, there are many reasons to use a completely different set of parameters for MPI in diffraction than in pp collisions, especially with respect to the impact-parameter picture, see below. A lower number in some frameworks could alternatively be regarded as a consequence of screening, with a larger "bare" number.

    For now, however, an attempt at the most general solution would carry too far, and instead we patch up the problem by using a larger Pomeron-proton total cross section, such that average activity makes more sense. This should be viewed as the main tunable parameter in the description of high-mass diffraction. It is to be fitted to diffractive event-shape data such as the average charged multiplicity. It would be very closely tied to the choice of Pomeron PDF; we remind that some of these add up to less than unit momentum sum in the Pomeron, a choice that also affect the value one ends up with. Furthermore, like with hadronic cross sections, it is quite plausible that the Pomeron-proton cross section increases with energy, so we have allowed for a power-like dependence on the diffractive mass. The assumed Pomeron-proton effective cross section, as used for multiparton interactions in diffractive systems. If this cross section is made to depend on the mass of the diffractive system then the above value refers to the cross section at the reference scale, and sigma_PomP(m) = sigma_PomP(m_ref) * (m / m_ref)^p where m is the mass of the diffractive system, m_ref is the reference mass scale Diffraction:mRefPomP below and p is the mass-dependence power Diffraction:mPowPomP. Note that a larger cross section value gives less MPI activity per event. There is no point in making the cross section too big, however, since then pT0 will be adjusted downwards to ensure that the integrated perturbative cross section stays above this assumed total cross section. (The requirement of at least one perturbative interaction per event.) The mRef reference mass scale introduced above. The p mass rescaling pace introduced above.

    Also note that, even for a fixed CM energy of events, the diffractive subsystem will range from the abovementioned threshold mass m_min to the full CM energy, with a variation of parameters such as pT0 along this mass range. Therefore multiparton interactions are initialized for a few different diffractive masses, currently five, and all relevant parameters are interpolated between them to obtain the behaviour at a specific diffractive mass. Furthermore, A B ->X B and A B ->A X are initialized separately, to allow for different beams or PDF's on the two sides. These two aspects mean that initialization of MPI is appreciably slower when perturbative high-mass diffraction is allowed.

    Diffraction tends to be peripheral, i.e. occur at intermediate impact parameter for the two protons. That aspect is implicit in the selection of diffractive cross section. For the simulation of the Pomeron-proton subcollision it is the impact-parameter distribution of that particular subsystem that should rather be modeled. That is, it also involves the transverse coordinate space of a Pomeron wavefunction. The outcome of the convolution therefore could be a different shape than for nondiffractive events. For simplicity we allow the same kind of options as for nondiffractive events, except that the bProfile = 4 option for now is not implemented. Choice of impact parameter profile for the incoming hadron beams. When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a radius that is a factor coreRadius smaller than the rest. When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a fraction coreFraction of the matter content of the hadron. When bProfile = 3 it gives the power of the assumed overlap shape exp(- b^expPow). Default corresponds to a simple exponential drop, which is not too dissimilar from the overlap obtained with the standard double Gaussian parameters. For expPow = 2 we reduce to the simple Gaussian, bProfile = 1, and for expPow -> infinity to no impact parameter dependence at all, bProfile = 0. For small expPow the program becomes slow and unstable, so the min limit must be respected. pythia8-8.1.80.orig/xmldoc/AdvancedUsage.xml0000444000175000017500000002550112217346277017047 0ustar sunsun

    Advanced Usage

    On this page we collect information on a number of classes that the normal user would not encounter. There are cases where the information is essential, however, for instance to implement your own showers.

    The subsystems

    One aspect that complicates administration is that an event can contain several subsystems, each consisting of one MPI and its associated ISR and FSR. To first approximation these systems are assumed to evolve independently, but to second they are connected by the interleaved evolution, and potentially by rescattering effects. The partons of a given subsystem therefore do not have to be stored consecutively.

    The PartonSystems class is primarily used to keep track of the current positions of all partons belonging to each system, represented by the index iPos for a parton stored in the event-record slot event[iPos]. With "all" we mean the currently defined two incoming partons, or none for a resonance decay, and the current set of outgoing partons, but with all ISR and FSR intermediate-state partons omitted. That is, it stores all partons that could be subject to some action in the next step of the combined MPI/ISR/FSR/BR description. As a special case, an outgoing parton is stored even if it undergoes a rescattering, and thus no longer belongs to the final state proper.

    The partonSystems instance of PartonSystems class is a public member of the Pythia top-level class, but is also available as a pointer partonSystemsPtr in various PartonLevel classes, e.g. inside the current instances of the TimeShower and SpaceShower classes.

    A number of PartonSystems methods can be used to set or get information on the subsystems:

    • clear() resets all the contents in preparation for the next event.
    • addSys() add a new (initially empty) subsystem to the current list and return its index iSys in the list, where index 0 is the hardest subcollision and so on.
    • sizeSys() the number of separate subsystems.
    • setInA(iSys, iPos), setInB(iSys, iPos) store position iPos of the incoming parton from beam A or beam B to the iSys'th subcollision. These values are 0 initially, and should so remain if there are no beams, such as in resonance decays.
    • addOut(iSys, iPos) store position iPos of a new outgoing parton in the iSys'th subcollision, by appending it at the end of the current vector, with beginning in slot 0.
    • setOut(iSys, iMem, iPos) store position iPos in the iMem'th slot in the vector of outgoing partons in the iSys'th subcollision. Here iMem must be in the range already constructed by addOut calls.
    • replace(iSys, iPosOld, iPosNew) replace the existing incoming or outgoing parton position iPosOld by iPosNew in the iSys'th subcollision.
    • setSHat(iSys, sHat) set the invariant squared mass sHat of the iSys'th subcollision.
    • hasInAB(iSys) true if an incoming parton has been set for beam A or beam B (and hence should have been set for both) in the iSys'th subcollision, else false.
    • getInA(iSys), getInB(iSys) the position iPos of the incoming parton from beam A or beam B to the iSys'th subcollision.
    • sizeOut(iSys) the number of outgoing partons in the iSys'th subcollision.
    • getOut(iSys, iMem) the position iPos of an outgoing parton in the iSys'th subcollision, with the iMem range limited by sizeOut(iSys). These partons are not guaranteed to appear in any particular order.
    • sizeAll(iSys) the total number of incoming and outgoing partons in the iSys'th subcollision.
    • getAll(iSys, iMem) the position iPos of an incoming or outgoing parton in the iSys'th subcollision. In case there are beams it gives same as getInA(iSys) and getInB(iSys) for indices 0 and 1, and thereafter agrees with getOut(iSys, iMem) offset two positions. If there are no beams it is identical with getOut(iSys, iMem).
    • getSHat(iSys) the invariant squared mass sHat of the iSys'th subcollision.
    • list() print a listing of all the system information, except for the sHat values.

    New systems are created from the hard process and by the MPI, not from any of the other components. Both FSR and ISR modify the position of partons, however. Since an FSR or ISR branching typically implies a new state with one more parton than before, an outgoing parton must be added to the system. Furthermore, in a branching, several existing partons may also be moved to new slots, including the incoming beam ones. In a FSR 1 -> 2 branching it is irrelevant which parton position you let overwrite the existing slot and which is added to the end of the system.

    The system information must be kept up-to-date. Both the MPI, ISR, FSR and BR descriptions make extensive use of the existing information. As an example, the introduction of primordial kT in the beam remnants will fail if the information on which final-state partons belong to which system is out-of-date. The introduction of rescattering as part of the MPI framework adds further complications, where an outgoing parton of one subsystem may be the incoming one of another system. This part of the code is still under development.

    Currently the system information is kept throughout the continued history of the event. Specifically, resonance decays create new systems, appended to the existing ones. This could be useful during the hadronization stage, to collect the partons that belong to a resonance with preserved mass when a small string collapses to one particle, but is not yet used for that.

    The beams

    The different subsystems are tied together by them sharing the same initial beam particles, and thereby being restricted by energy-momentum and flavour conservation issues. The information stored in the two beam particles, here called beamA and beamB, is therefore as crucial to keep correct as the above subsystem list.

    Both beam objects are of the BeamParticle class. Each such object contains a vector with the partons extracted from it. The number of such partons, beamX.size() (X = A or B), of course is the same as the above number of subsystems in the event record. (The two diverge at the BR step, where further beam remnants are added to the beams without corresponding to new subsystems.) The individual partons are accessed by an overloaded indexing operator to a vector of ResolvedParton objects. The iPos() property corresponds to the iPos one above, i.e. providing the position in the main event record of a parton. In particular, beamA[iSys].iPos() = partonSystemsPtr->getInA(iSys) and beamB[iSys].iPos() = partonSystemsPtr->getInB(iSys). Whereas thus the indices of the two incoming partons to a subsystem are stored in two places, the ones of the outgoing partons only appear in the system part of the PartonSystems class.

    Just as the subsystems in PartonSystems must be updated, so must the information in the two BeamParticle's, e.g. with methodsbeamX[iSys].iPos( iPosIn) when an incoming parton is replaced by a new one in line iPosIn. Furthermore the new parton identity should be set by beamX[iSys].id( idIn) and the new x energy-momentum fraction by beamX[iSys].x( xIn). The three can be combined in one go by beamX[iSys].update( iPosIn, idIn, xIn).

    To be specific, it is assumed that, at each step, the two incoming partons are moving along the +-z axis and are massless. Since the event is constructed in the c.m. frame of the incoming beams this implies that x = 2 E / E_cm. If the x values are not defined accordingly or not kept up-to-date the BR treatment will not conserve energy-momentum.

    In return, the BeamParticle objects give access to some useful methods. The beamX.xf( id, x, Q2) returns the standard PDF weight x f_id(x, Q^2). More interestingly, beamX.xfISR( iSys, id, x, Q2) returns the modified weight required when several subsystems have to share the energy and flavours. Thus iSys is added as an extra argument, and the momentum already assigned to the other subsystems is not available for evolution, i.e. the maximal x is correspondingly smaller than unity. Also flavour issues are handled in a similar spirit.

    An additional complication is that a parton can be either valence or sea, and in the latter case the BR treatment also distinguishes companion quarks, i.e. quark-antiquark pairs that are assumed to come from the same original g -> q qbar branching, whether perturbative or not. This can be queried either with the beamX[iSys].companion() method, for detailed information, or with the beamX[iSys].isValence(), beamX[iSys].isUnmatched() and beamX[iSys].isCompanion() methods for yes/no answers whether a parton is valence, unmatched sea or matched sea. This choice should affect the ISR evolution; e.g., a valence quark cannot be constructed back to come from a gluon.

    To keep this info up-to-date, the beamX.pickValSeaComp() method should be called whenever a parton of a new flavour has been picked in the ISR backwards evolution, but not if the flavour has not been changed, since then one should not be allowed to switch back and forth between the same quark being considered as valence or as sea. Since the pickValSeaComp() method makes use of the current parton-density values, it should be preceded by a call to beamX.xfISR( iSys, id, x, Q2), where the values in the call are the now finally accepted ones for the newly-found mother. (Such a call is likely to have been made before, during the evolution, but is not likely to be the most recent one, i.e. still in memory, and therefore had better be redone.) pythia8-8.1.80.orig/xmldoc/worksheet.tex0000444000175000017500000011251612217346320016360 0ustar sunsun\documentclass[12pt,a4paper]{article} %packages %\renewcommand{\familydefault}{phv} \usepackage{epsfig} \usepackage{axodraw} %define page size \setlength{\textheight}{233mm} \setlength{\topmargin}{14mm} \setlength{\headheight}{0mm} \setlength{\headsep}{0mm} \setlength{\footskip}{10mm} \setlength{\textwidth}{160mm} \setlength{\oddsidemargin}{0mm} \setlength{\evensidemargin}{0mm} \setlength{\parindent}{0mm} \setlength{\parskip}{0.35\baselineskip} %define math alphabets for teletype, roman, overline \newcommand{\ttt}[1]{\texttt{#1}} \newcommand{\tbl}[1]{{\color{blue}\texttt{#1}}} \newcommand{\trd}[1]{{\color{red}\texttt{#1}}} \newcommand{\tol}[1]{{\color{olive}\texttt{#1}}} \newcommand{\mrm}[1]{\mathrm{#1}} \newcommand{\mbf}[1]{\mathbf{#1}} \newcommand{\br}[1]{\overline{#1}} %some frequent math symbols \newcommand{\gtrsim}{\raisebox{-2mm}% {\hspace{1mm}$\stackrel{>}{\sim}$\hspace{1mm}}} \newcommand{\lessim}{\raisebox{-2mm}% {\hspace{1mm}$\stackrel{<}{\sim}$\hspace{1mm}}} %shorthands \newcommand{\as}{\alpha_{\mathrm{s}}} \newcommand{\aem}{\alpha_{\mathrm{em}}} \newcommand{\kT}{k_{\perp}} \newcommand{\pT}{p_{\perp}} \newcommand{\pTs}{p^2_{\perp}} \newcommand{\pTe}{\p_{\perp\mrm{evol}}} \newcommand{\pTse}{\p^2_{\perp\mrm{evol}}} \newcommand{\pTmin}{p_{\perp\mathrm{min}}} \newcommand{\pTsmim}{p^2_{\perp\mathrm{min}}} \newcommand{\pTmax}{p_{\perp\mathrm{max}}} \newcommand{\pTsmax}{p^2_{\perp\mathrm{max}}} \newcommand{\pTL}{p_{\perp\mathrm{L}}} \newcommand{\pTD}{p_{\perp\mathrm{D}}} \newcommand{\pTA}{p_{\perp\mathrm{A}}} \newcommand{\pTsL}{p^2_{\perp\mathrm{L}}} \newcommand{\pTsD}{p^2_{\perp\mathrm{D}}} \newcommand{\pTsA}{p^2_{\perp\mathrm{A}}} \newcommand{\pTo}{p_{\perp 0}} \newcommand{\shat}{\hat{s}} %roman names for particles in math mode \renewcommand{\a}{{\mathrm a}} \renewcommand{\b}{{\mathrm b}} \renewcommand{\c}{{\mathrm c}} \renewcommand{\d}{{\mathrm d}} \newcommand{\e}{{\mathrm e}} \newcommand{\f}{{\mathrm f}} \newcommand{\g}{{\mathrm g}} \newcommand{\hrm}{{\mathrm h}} \newcommand{\lrm}{{\mathrm l}} \newcommand{\n}{{\mathrm n}} \newcommand{\p}{{\mathrm p}} \newcommand{\q}{{\mathrm q}} \newcommand{\s}{{\mathrm s}} \renewcommand{\t}{{\mathrm t}} \renewcommand{\u}{{\mathrm u}} \newcommand{\A}{{\mathrm A}} \renewcommand{\B}{{\mathrm B}} \newcommand{\D}{{\mathrm D}} \newcommand{\F}{{\mathrm F}} \renewcommand{\H}{{\mathrm H}} \newcommand{\J}{{\mathrm J}} \newcommand{\K}{{\mathrm K}} \renewcommand{\L}{{\mathrm L}} \newcommand{\Q}{{\mathrm Q}} \newcommand{\R}{{\mathrm R}} \newcommand{\T}{{\mathrm T}} \newcommand{\W}{{\mathrm W}} \newcommand{\Z}{{\mathrm Z}} \newcommand{\bbar}{\overline{\mathrm b}} \newcommand{\cbar}{\overline{\mathrm c}} \newcommand{\dbar}{\overline{\mathrm d}} \newcommand{\fbar}{\overline{\mathrm f}} \newcommand{\pbar}{\overline{\mathrm p}} \newcommand{\qbar}{\overline{\mathrm q}} \newcommand{\rbar}{\overline{\mathrm{r}}} \newcommand{\sbar}{\overline{\mathrm s}} \newcommand{\tbar}{\overline{\mathrm t}} \newcommand{\ubar}{\overline{\mathrm u}} \newcommand{\Bbar}{\overline{\mathrm B}} \newcommand{\Fbar}{\overline{\mathrm F}} \newcommand{\Qbar}{\overline{\mathrm Q}} % %new list environments to replace itemize and enumerate \newenvironment{Itemize}{\begin{list}{$\bullet$}% {\setlength{\topsep}{0.4mm}\setlength{\partopsep}{0.4mm}% \setlength{\itemsep}{0.4mm}\setlength{\parsep}{0.4mm}}}% {\end{list}} \newcounter{enumct} \newenvironment{Enumerate}{\begin{list}{\arabic{enumct}.}% {\usecounter{enumct}\setlength{\topsep}{0.4mm}% \setlength{\partopsep}{0.4mm}\setlength{\itemsep}{0.4mm}% \setlength{\parsep}{0.4mm}}}{\end{list}} \begin{document} %set sloppy attitude to line breaks \sloppy \begin{flushright} For tutorials\\ at Summer Schools \end{flushright} \vspace{-20mm} \mbox{\epsfig{file=lejon2.eps,width=40mm}}% \hspace{30mm}% \raisebox{4mm}[0mm][0mm]{\epsfig{file=pythiapicture.eps,width=20mm}}\\[6mm] \begin{center} {\LARGE\bf PYTHIA 8 Worksheet}\\[10mm] {\large Torbj\"orn Sj\"ostrand, Richard Corke}\\[1mm] Department of Theoretical Physics, Lund University\\[4mm] {\large Peter Skands}\\[1mm] Theoretical Physics, CERN\\[15mm] \end{center} \section{Introduction} The objective of this exercise is to teach you the basics of how to use the \textsc{Pythia}~8.1 event generator to study various physics aspects. As you become more familiar you will better understand the tools at your disposal, and can develop your own style to use them. Within this first exercise it is not possible to describe the physics models used in the program; for this we refer to the \textsc{Pythia}~8.1 brief introduction \cite{pythiaeight}, to the full \textsc{Pythia}~6.4 physics description \cite{pythiasix}, and to all the further references found in them. \textsc{Pythia}~8 is, by today's standards, a small package. It is completely self-contained, and is therefore easy to install for standalone usage, e.g. if you want to have it on your own laptop, or if you want to explore physics or debug code without any danger of destructive interference between different libraries. Section 2 describes the installation procedure, which is what we will need for this introductory session. When you use \textsc{Pythia} you are expected to write the main program yourself, for maximal flexibility and power. Several examples of such main programs are included with the code, to illustrate common tasks and help getting started. Section 3 gives you a simple step-by-step recipe how to write a minimal main program, that can then gradually be expanded in different directions, e.g.\ as in Section 4. In Section 5 you will see how the parameters of a run can be read in from a file, so that the main program can be kept fixed. Many of the provided main programs therefore allow you to create executables that can be used for different physics studies without recompilation, but potentially at the cost of some flexibility. While \textsc{Pythia} can be run standalone, it can also be interfaced with a set of other libraries. One example is \textsc{HepMC}, which is the standard format used by experimentalists to store generated events. Since the \textsc{HepMC} library location is installation-dependent it is not possible to give a fool-proof linking procedure, but some hints are provided for the interested in Section 6. Finally, Section 7 gives some suggestions for the study of other possible physics topics, and Appendix A contains a brief summary of the event-record structure. \section{Installation} Denoting a generic \textsc{Pythia}~8 version \texttt{pythia81xx} (at the time of writing \texttt{xx} = 60), here is how to install \textsc{Pythia}~8 on a Linux/Unix/MacOSX system as a standalone package. \begin{Enumerate} \item In a browser, go to\\ \hspace*{10mm}\texttt{http://www.thep.lu.se/}$\sim$% \texttt{torbjorn/Pythia.html} \item Download the (current) program package\\ \hspace*{10mm}\texttt{pythia81xx.tgz}\\ to a directory of your choice (e.g. by right-clicking on the link). \item In a terminal window, \texttt{cd} to where \texttt{pythia81xx.tgz} was downloaded, and type\\ \hspace*{10mm}\texttt{tar xvfz pythia81xx.tgz}\\ This will create a new (sub)directory \texttt{pythia81xx} where all the \textsc{Pythia} source files are now ready and unpacked. \item Move to this directory (\texttt{cd pythia81xx}) and do a \texttt{make}. This will take $\sim$3 minutes (computer-dependent). The \textsc{Pythia}~8 libraries are now compiled and ready for physics. \item For test runs, \texttt{cd} to the \texttt{examples/} subdirectory. An \texttt{ls} reveals a list of programs, \texttt{mainNN}, with \texttt{NN} from \texttt{01} through \texttt{28} (and beyond). These example programs each illustrate an aspect of \textsc{Pythia}~8. For a list of what they do, see the ``Sample Main Programs'' page in the online manual (point 6 below).\\ Initially only use one or two of them to check that the installation works. Once you have worked your way though the introductory exercises in the next sections you can return and study the programs and their output in more detail.\\ To execute one of the test programs, do\\ \hspace*{10mm}\texttt{make mainNN}\\ \hspace*{10mm}\texttt{./mainNN.exe}\\ The output is now just written to the terminal, \texttt{stdout}. To save the output to a file instead, do \texttt{./mainNN.exe > mainNN.out}, after which you can study the test output at leisure by opening \texttt{mainNN.out}. See Appendix A for an explanation of the event record that is listed in several of the runs. \item If you use a web browser to open the file\\ \hspace*{10mm}\texttt{pythia81xx/htmldoc/Welcome.html}\\ you will gain access to the online manual, where all available methods and parameters are described. Use the left-column index to navigate among the topics, which are then displayed in the larger right-hand field. \end{Enumerate} \section{A ``Hello World'' program} We will now generate a single $\g \g \to \t \tbar$ event at the LHC, using \textsc{Pythia} standalone. Open a new file \texttt{mymain.cc} in the \texttt{examples} subdirectory with a text editor, e.g.\ Emacs. Then type the following lines (here with explanatory comments added): \begin{verbatim} // Headers and Namespaces. #include "Pythia.h" // Include Pythia headers. using namespace Pythia8; // Let Pythia8:: be implicit. int main() { // Begin main program. // Set up generation. Pythia pythia; // Declare Pythia object pythia.readString("Top:gg2ttbar = on"); // Switch on process. pythia.readString("Beams:eCM = 7000."); // 7 TeV CM energy. pythia.init(); // Initialize; incoming pp beams is default. // Generate event(s). pythia.next(); // Generate an(other) event. Fill event record. return 0; } // End main program with error-free return. \end{verbatim} Next you need to edit the \texttt{Makefile} (the one in the \texttt{examples} subdirectory) so it knows what to do with \texttt{mymain.cc}. The lines\\ \hspace*{10mm}\texttt{\# Create an executable for one of the normal test programs}\\ \hspace*{10mm}\texttt{main00 main01 main02 main03 ... main09 main10 main10}~\verb+\+ \\ and the three next enumerate the main programs that do not need any external libraries. Edit the last of these lines to include also \texttt{mymain}:\\ \hspace*{10mm}\texttt{ main31 ... main40 mymain:}~\verb+\+ Now it should work as before with the other examples:\\ \hspace*{10mm}\texttt{make mymain}\\ \hspace*{10mm}\texttt{./mymain.exe > mymain.out}\\ whereafter you can study \texttt{mymain.out}, especially the example of a complete event record (preceded by initialization information, and by kinematical-variable and hard-process listing for the same event). At this point you need to turn to Appendix A for a brief overview of the information stored in the event record. An important part of the event record is that many copies of the same particle may exist, but only those with a positive status code are still present in the final state. To exemplify, consider a top quark produced in the hard interaction, initially with positive status code. When later, a shower branching $\t \to \t \g$ occurs, the new $\t$ and $\g$ are added at the bottom of the then-current event record, but the old $\t$ is not removed. It is marked as decayed, however, by negating its status code. At any stage of the shower there is thus only one ``current'' copy of the top. After the shower, when the final top decays, $\t \to \b \W^+$, also that copy receives a negative status code. When you understand the basic principles, see if you can find several copies of the top quarks, and check the status codes to figure out why each new copy has been added. Also note how the mother/daughter indices tie together the various copies. \section{A first realistic analysis} We will now gradually expand the skeleton \texttt{mymain} program from above, towards what would be needed for a more realistic analysis setup. \begin{Itemize} \item Often, we wish to mix several processes together. To add the process $\q \qbar \to \t \tbar$ to the above example, just include a second \texttt{pythia.readString} call\\ \texttt{ \hspace*{10mm} pythia.readString("Top:qqbar2ttbar = on"); } \item Now we wish to generate more than one event. To do this, introduce a loop around \texttt{pythia.next()}, so the code now reads\\ \texttt{ \hspace*{10mm} for (int iEvent = 0; iEvent < 5; ++iEvent) \{ \\ \hspace*{15mm} pythia.next(); \\ \hspace*{10mm} \} } \\ Hereafter, we will call this the \textbf{event loop}. The program will now generate 5 events; each call to \texttt{pythia.next()} resets the event record and fills it with a new event. To list more of the events, you also need to add\\ \texttt{ \hspace*{10mm} pythia.readString("Next:numberShowEvent = 5"); }\\ along with the other \texttt{pythia.readString} commands. \item To obtain statistics on the number of events generated of the different kinds, and the estimated cross sections, add a \\ \hspace*{10mm}\texttt{pythia.stat();}\\ just before the end of the program. \item During the run you may receive problem messages. These come in three kinds: \begin{Itemize} \item a \textit{warning} is a minor problem that is automatically fixed by the program, at least approximately; \item an \textit{error} is a bigger problem, that is normally still automatically fixed by the program, by backing up and trying again; \item an \textit{abort} is such a major problem that the current event could not be completed; in such a rare case \texttt{pythia.next()} is \texttt{false} and the event should be skipped. \end{Itemize} Thus the user need only be on the lookout for aborts. During event generation, a problem message is printed only the first time it occurs. The above-mentioned \texttt{pythia.stat()} will then tell you how many times each problem was encountered over the entire run. \item Looking at the event listing for a few events at the beginning of each run is useful to make sure you are generating the right kind of events, at the right energies, etc. For real analyses, however, you need automated access to the event record. The Pythia event record provides many utilities to make this as simple and efficient as possible. To access all the particles in the event record, insert the following loop after \texttt{pythia.next()} (but fully enclosed by the \textbf{event loop}) \\ \texttt{ \hspace*{10mm} for (int i = 0; i < pythia.event.size(); ++i) \{ \\ \hspace*{15mm} cout << "i = " << i \\ \hspace*{26mm} << ", id = " << pythia.event[i].id() << endl; \\ \hspace*{10mm} \} \\ } which we will call the \textbf{particle loop}. Inside this loop, you can access the properties of each particle \texttt{pythia.event[i]}. For instance, the method \texttt{id()} returns the PDG identity code of a particle (see Appendix A). The \texttt{cout} statement, therefore, will give a list of the PDG code of every particle in the event record. \item As mentioned above, the event listing contains all partons and particles, traced through a number of intermediate steps. Eventually, the top will decay ($\t \to \W \b$), and by implication it is the last copy of this top in the event record that gives the ``final'' answer. You can obtain the location of this final top e.g. by a line just before the \textbf{particle loop} \\ \hspace*{10mm}\texttt{int iTop = 0;} \\ and a line inside the \textbf{particle loop} \\ \hspace*{10mm}\texttt{if (pythia.event[i].id() == 6) iTop = i;} \\ The value of \texttt{iTop} will be set every time a top is found in the event record. When the \textbf{particle loop} is complete, \texttt{iTop} will now point to the final top in the event record (which can be accessed as \texttt{pythia.event[iTop]}). \item In addition to the particle properties in the event listing, there are also methods that return many derived quantities for a particle, such as transverse momentum, \texttt{pythia.event[iTop].pT()}, and pseudorapidity, \texttt{pythia.event[iTop].eta()}. Use these methods to print out the values for the final top found above. \item We now want to generate more events, say 1000, to view the shape of these distributions. Inside \textsc{Pythia} is a very simple histogramming class, that can be used for rapid check/debug purposes. To book the histograms, insert before the \textbf{event loop} \\ \hspace*{10mm}\texttt{Hist pT("top transverse momentum", 100, 0., 200.);}\\ \hspace*{10mm}\texttt{Hist eta("top pseudorapidity", 100, -5., 5.);}\\ where the last three arguments are the number of bins, the lower edge and the upper edge of the histogram, respectively. Now we want to fill the histograms in each event, so before the end of the \textbf{event loop} insert \\ \hspace*{10mm}\texttt{pT.fill( pythia.event[iTop].pT() );}\\ \hspace*{10mm}\texttt{eta.fill( pythia.event[iTop].eta() );}\\ Finally, to write out the histograms, after the \textbf{event loop} we need a line like \hspace*{10mm}\texttt{cout << pT << eta;} \item As a final standalone exercise, consider plotting the charged multiplicity of events. You then need to have a counter set to zero for each new event. Inside the \textbf{particle loop} this counter should be incremented whenever the particle \texttt{isCharged()} and \texttt{isFinal()}. For the histogram, note that it can be treacherous to have bin limits at integers, where roundoff errors decide whichever way they go. In this particular case only even numbers are possible, so 100 bins from $-1$ to 399 would still be acceptable. \end{Itemize} \section{Input files} With the \texttt{mymain.cc} structure developed above it is necessary to recompile the main program for each minor change, e.g. if you want to rerun with more statistics. This is not time-consuming for a simple standalone run, but may become so for more realistic applications. Therefore, parameters can be put in special input ``card'' files that are read by the main program. We will now create such a file, with the same settings used in the \texttt{mymain} example program. Open a new file, \texttt{mymain.cmnd}, and input the following \begin{verbatim} ! t tbar production at the LHC Beams:idA = 2212 ! first incoming beam is a 2212, i.e. a proton. Beams:idB = 2212 ! second beam is also a proton. Beams:eCM = 7000. ! the cm energy of collisions. Top:gg2ttbar = on ! switch on the process g g -> t tbar. Top:qqbar2ttbar = on ! switch on the process q qbar -> t tbar. \end{verbatim} The \texttt{mymain.cmnd} file can contain one command per line, of the type\\ \hspace*{10mm}\texttt{variable = value}\\ All variable names are case-insensitive (the mixing of cases has been chosen purely to improve readability) and non-alphanumeric characters (such as !, \# or \$) will be interpreted as the start of a comment. All valid variables are listed in the online manual (see Section 2, point 6, above). Cut-and-paste of variable names can be used to avoid spelling mistakes. The final step is to modify our program to use this input file. The name of this input file can be hardcoded in the main program, but for more flexibility, it can also be provided as a command-line argument. To do this, replace the \texttt{int main() \{} line by \\ \hspace*{10mm} \texttt{int main(int argc, char* argv[]) \{}\\ and replace all \texttt{pythia.readString(...)} commands with the single command\\ \hspace*{10mm}\texttt{pythia.readFile(argv[1]);} The executable \texttt{mymain.exe} is then run with a command line like\\ \hspace*{10mm}\texttt{./mymain.exe mymain.cmnd > mymain.out}\\ and should give the same output as before. In addition to all the internal \texttt{Pythia} variables there exist a few defined in the database but not actually used. These are intended to be useful in the main program, and thus begin with \texttt{Main:}. The most basic of those is \texttt{Main:numberOfEvents}, which you can use to specify how many events you want to generate. To make this have any effect, you need to read it in the main program, after the \texttt{pythia.readFile(...)} command, by a line like\\ \hspace*{10mm}\texttt{int nEvent = pythia.mode("Main:numberOfEvents");}\\ and set up the \textbf{event loop} like\\ \hspace*{10mm}\texttt{for (int iEvent = 0; iEvent < nEvent; ++iEvent) \{ } You are now free to play with further options in the input file, such as: \begin{Itemize} \item \texttt{6:m0 = 175.}\\ change the top mass, which by default is 171 GeV. \item \texttt{PartonLevel:FSR = off}\\ switch off final-state radiation. \item \texttt{PartonLevel:ISR = off}\\ switch off initial-state radiation. \item \texttt{PartonLevel:MPI = off}\\ switch off multiparton interactions. \item \texttt{Tune:pp = 3} (or other values between 1 and 7) \\ different combined tunes, in particular to radiation and multiparton interactions parameters. In part this reflects that no generator is perfect, and also not all data is perfect, so different emphasis will result in different optima. In addition, detailed tuning of \texttt{Pythia}~8 is still in its infancy. \item \texttt{Random:setSeed = on}\\ \texttt{Random:seed = 123456789}\\ all runs by default use the same random-number sequence, for reproducibility, but you can pick any number between 1 and 900,000,000 to obtain a unique sequence. \end{Itemize} For instance, check the importance of FSR, ISR and MPI on the charged multiplicity of events by switching off one component at a time. The usage of further \texttt{Main:} variables is illustrated e.g.\ in \texttt{main03.cc}, and the possibility to use command-line input files in \texttt{main16.cc} and \texttt{main42.cc}. The online manual also exists in an interactive variant, where you semi-automatically can construct a file with all the command lines you wish to have. This requires that somebody installs the \texttt{pythia81xx/phpdoc} directory in a webserver. If you lack a local installation you can use the one at\\ \hspace*{10mm}\texttt{http://home.thep.lu.se/}$\sim$% \texttt{torbjorn/php81xx/Welcome.php}\\ This is not a commercial-quality product, however, and requires some user discipline. Full instructions are provided on the ``Save Settings'' page. \section{Interface to HepMC} The standard \textsc{HepMC} event-record format will be frequently used in subsequent training sessions, with a ready-made installation. However, for the ambitious, here is described how to set up the \textsc{Pythia} interface, assuming you already know where \textsc{HepMC} is installed. Note: the interface to \textsc{HepMC} version 1 is no longer supported; you must use version 2. Preferably 2.04 or later. To begin with, you need to go back to the installation procedure of section 2 and insert/redo some steps. \begin{Enumerate} \item Move back to the main \texttt{pythia81xx} directory (\texttt{cd ..} if you are in \texttt{examples}). \item Remove the currently compiled version with\\ \hspace*{10mm}\texttt{make clean} \item Configure the program in preparation for the compilation:\\ \hspace*{10mm}\texttt{./configure --with-hepmc=path}\\ where the directory-tree \texttt{path} would depend on your local installation. \item Should \texttt{configure} not recognise the version number you can supply that with an optional argument, like\\ \hspace*{10mm}\texttt{./configure --with-hepmc=path --with-hepmcversion=2.06.07} \item Recompile the program, now including the \textsc{HepMC} interface, with \texttt{make} as before, and move back to the \texttt{examples} subdirectory. \item Do either of\\ \hspace*{10mm}\texttt{source config.csh}\\ \hspace*{10mm}\texttt{source config.sh}\\ the former when you use the csh or tcsh shells, otherwise the latter. (Use \texttt{echo \$SHELL} if uncertain.) \item You can now also use the \texttt{main41.cc} and \texttt{main42.cc} examples to produce \textsc{HepMC} event files. The latter may be most useful; it presents a slight generalisation of the command-line-driven main program you constructed in Section 5. After you have built the executable you can run it with\\ \hspace*{10mm}\texttt{./main42.exe infile hepmcfile > main42.out}\\ where \texttt{infile} is an input ``card'' file (e.g. \texttt{mymain.cmnd}) and \texttt{hepmcfile} is your chosen name for the output file with \textsc{HepMC} events. \end{Enumerate} Note that the above procedure is based on the assumption that you will be running your main programs from the \texttt{examples} subdirectory. If not you will have to create your own scripts and/or makefiles to handle the linking. If you have no experience with such tasks then it is better to use any existing instructions for your local installation. If you do have such experience then a short summary of what you need to know to get going is provided. Before you run a \textsc{Pythia} program the \texttt{PYTHIA8DATA} environment variable needs to be set to point to the \texttt{xmldoc} subdirectory where all settings and particle data are stored. If you use the csh or tcsh shells this means a line like\\ \hspace*{10mm}\texttt{setenv PYTHIA8DATA /path/pythia81xx/xmldoc}\\ or else\\ \hspace*{10mm}\texttt{export PYTHIA8DATA=/path/pythia81xx/xmldoc}\\ where the correct \texttt{path} has to be found by you. Similarly, to use \textsc{HepMC}, you also have to set or append its location to the \texttt{LD\_LIBRARY\_PATH} (the \texttt{DYLD\_LIBRARY\_PATH} on Mac OSX); the \texttt{config.csh} and \texttt{config.sh} files generated above well illustrate the code needed to achieve this. Finally, the necessary linking stage can be understood from the relevant parts of the \texttt{examples/Makefile}. \section{Further studies} If you have time left, you should take the opportunity to try a few other processes or options. Below are given some examples, but feel free to pick something else that you would be more interested in. \begin{Itemize} \item One popular misconception is that the energy and momentum of a $\B$ meson has to be smaller than that of its mother $\b$ quark, and similarly for charm. The fallacy is twofold. Firstly, if the $\b$ quark is surrounded by nearby colour-connected gluons, the $\B$ meson may also pick up some of the momentum of these gluons. Secondly, the concept of smaller momentum is not Lorentz-frame-independent: if the other end of the $\b$ colour force field is a parton with a higher momentum (such as a beam remnant) the ``drag'' of the hadronization process may imply an acceleration in the lab frame (but a deceleration in the beam rest frame).\\ To study this, simulate $\b$ production, e.g.\ the process \texttt{HardQCD:gg2bbbar}. Identify $\B / \B^*$ mesons that come directly from the hadronization, for simplicity those with status code $-83$ or $-84$. In the former case the mother $\b$ quark is in the \texttt{mother1()} position, in the latter in \texttt{mother2()} (study a few event listings to see how it works). Plot the ratio of $\B$ to $\b$ energy to see what it looks like. \item One of the characteristics of multiparton-interactions (MPI) models is that they lead to strong long-range correlations, as observed in data. That is, if many hadrons are produced in one rapidity range of an event, then most likely this is an event where many MPI's occurred (and the impact parameter between the two colliding protons was small), and then one may expect a larger activity also at other rapidities.\\ To study this, select two symmetrically located, one unit wide bins in rapidity (or pseudorapidity), with a variable central separation $\Delta y$: $\left[ \Delta y/2, \Delta y/2 + 1 \right]$ and $\left[ - \Delta y/2 - 1, - \Delta y/2 \right]$. For each event you may find $n_F$ and $n_B$, the charged multiplicity in the ``forward'' and ``backward'' rapidity bins. Suitable averages over a sample of events then gives the forward--backward correlation coefficient \[ \rho_{FB}(\Delta y) = \frac{\langle n_F \, n_B \rangle - \langle n_F \rangle \langle n_B \rangle}% {\sqrt{(\langle n_F^2 \rangle - \langle n_F \rangle^2) (\langle n_B^2 \rangle - \langle n_B \rangle^2)}} = \frac{\langle n_F \, n_B \rangle - \langle n_F \rangle^2}% {\langle n_F^2 \rangle - \langle n_F \rangle^2} ~, \] where the last equality holds for symmetric distributions such as in $\p\p$ and $\pbar\p$.\\ Compare how $\rho_{FB}(\Delta y)$ changes for increasing $\Delta y = 0, 1, 2, 3, \ldots$, with and without MPI switched on (\texttt{PartonLevel:MPI = on/off}) for minimum-bias events (\texttt{SoftQCD:minBias = on}). \item Higgs production can proceed through several different production processes. For the Standard Model Higgs some process switches are:\\ \texttt{HiggsSM:ffbar2H} for $\f \fbar \to \H^0$ ($\f$ generic fermion, here mainly $\b \bbar \to \H^0$); \\ \texttt{HiggsSM:gg2H} for $\g \g \to \H^0$; \\ \texttt{HiggsSM:ffbar2HZ} for $\f \fbar \to \H^0 \Z^0$; \\ \texttt{HiggsSM:ffbar2HW} for $\f \fbar \to \H^0 \W^{\pm}$; \\ \texttt{HiggsSM:ff2Hff(t:ZZ)} for $\f \fbar \to \H^0\f \fbar$ via $\Z^0\Z^0$ fusion; \\ \texttt{HiggsSM:ff2Hff(t:WW)} for $\f \fbar \to \H^0\f \fbar$ via $\W^+\W^-$ fusion; \\ \texttt{HiggsSM:all} for all of the above (and some more). \\ Study the $\pT$ and $\eta$ spectrum of the Higgs in these processes, and compare. \item You can also vary the Higgs mass with a \texttt{25:m0 = ...} and switch off FSR/ISR/MPI as above for top. \item $\Z^0$ production to lowest order only involves one process, accessible with \texttt{WeakSingleBoson:ffbar2gmZ = on}. The problem here is that the process is $\f \fbar \to \gamma^*/\Z^0$ with full $\gamma^*/\Z^0$ interference and so a signficiant enhancement at low masses. The combined particle is always classified with code 23, however. So generate events and study the $\gamma^*/\Z^0$ mass and $\pT$ distributions. Then restrict to a more ``$\Z^0$-like'' mass range with \texttt{PhaseSpace:mHatMin = 75.} and \texttt{PhaseSpace:mHatMax = 120.} \item Using your favourite jet cluster algorithm, study the number of jets found in association with the $\Z^0$ above. You can switch off Z0 decay with \texttt{23:mayDecay = no}. If you do not have a jet finder around, to begin with you can use the simple \texttt{SlowJet} one that comes with \textsc{Pythia}, see the ``Event Analysis'' page in the online manual, which offers a choice of the $k_{\perp}$, Cambridge/Aachen and anti-$k_{\perp}$ algorithms. Again check the importance of FSR/ISR/MPI. \end{Itemize} \appendix \section{The Event Record} The event record is set up to store every step in the evolution from an initial low-multiplicity partonic process to a final high-multiplicity hadronic state, in the order that new particles are generated. The record is a vector of particles, that expands to fit the needs of the current event (plus some additional pieces of information not discussed here). Thus \texttt{event[i]} is the \texttt{i}'th particle of the current event, and you may study its properties by using various \texttt{event[i].method()} possibilities. The \texttt{event.list()} listing provides the main properties of each particles, by column: \begin{Itemize} \item \texttt{no}, the index number of the particle (\texttt{i} above); \item \texttt{id}, the PDG particle identity code (method \texttt{id()}); \item \texttt{name}, a plaintext rendering of the particle name (method \texttt{name()}), within brackets for initial or intermediate particles and without for final-state ones; \item \texttt{status}, the reason why a new particle was added to the event record (method \texttt{status()}); \item \texttt{mothers} and \texttt{daughters}, documentation on the event history (methods \texttt{mother1()}, \texttt{mother2()}, \texttt{daughter1()} and \texttt{daughter2()}); \item \texttt{colours}, the colour flow of the process (methods \texttt{col()} and \texttt{acol()}); \item \texttt{p\_x}, \texttt{p\_y}, \texttt{p\_z} and \texttt{e}, the components of the momentum four-vector $(p_x, p_y, p_z, E)$, in units of GeV with $c = 1$ (methods \texttt{px()}, \texttt{py()}, \texttt{pz()} and \texttt{e()}); \item \texttt{m}, the mass, in units as above (method \texttt{m()}). \end{Itemize} For a complete description of these and other particle properties (such as production and decay vertices, rapidity, $p_\perp$, etc), open the program's online documentation in a browser (see Section 2, point 6, above), scroll down to the ``Study Output'' section, and follow the ``Particle Properties'' link in the left-hand-side menu. For brief summaries on the less trivial of the ones above, read on. \subsection{Identity codes} A complete specification of the PDG codes is found in the Review of Particle Physics \cite{rpp}. An online listing is available from\\ \hspace*{10mm}\texttt{http://pdg.lbl.gov/2008/mcdata/mc\_particle\_id\_contents.html} A short summary of the most common \texttt{id} codes would be\\[2mm] \begin{tabular}{|cc|cc|cc|cc|cc|cc|cc|} \hline 1 & $\d$ & 11 & $\e^-$ & 21 & $\g$ & 211 & $\pi^+$ & 111 & $\pi^0$ & 213 & $\rho^+$ & 2112 & $\n$ \\ 2 & $\u$ & 12 & $\nu_{\e}$ & 22 & $\gamma$ & 311 & $\K^0$ & 221 & $\eta$ & 313 & $\K^{*0}$ & 2212 & $\p$ \\ 3 & $\s$ & 13 & $\mu^-$ & 23 & $\Z^0$ & 321 & $\K^+$ & 331 & $\eta'$ & 323 & $\K^{*+}$ & 3122 & $\Lambda^0$ \\ 4 & $\c$ & 14 & $\nu_{\mu}$ & 24 & $\W^+$ & 411 & $\D^+$ & 130 & $\K^0_{\mrm{L}}$ & 113 & $\rho^0$ & 3112 & $\Sigma^-$ \\ 5 & $\b$ & 15 & $\tau^-$ & 25 & $\H^0$ & 421 & $\D^0$ & 310 & $\K^0_{\mrm{S}}$ & 223 & $\omega$ & 3212 & $\Sigma^0$ \\ 6 & $\t$ & 16 & $\nu_{\tau}$ & & & 431 & $\D_{\s}^+$ & & & 333 & $\phi$ & 3222 & $\Sigma^+$ \\ \hline \end{tabular}\\[2mm] Antiparticles to the above, where existing as separate entities, are given with a negative sign.\\ Note that simple meson and baryon codes are constructed from the constituent (anti)quark codes, with a final spin-state-counting digit $2 s + 1$ ($\K^0_{\mrm{L}}$ and $\K^0_{\mrm{S}}$ being exceptions), and with a set of further rules to make the codes unambiguous. \subsection{Status codes} When a new particle is added to the event record, it is assigned a positive status code that describes why it has been added, as follows:\\[2mm] \begin{tabular}{|c|l|} \hline code range & explanation \\ \hline 11 -- 19 & beam particles\\ 21 -- 29 & particles of the hardest subprocess\\ 31 -- 39 & particles of subsequent subprocesses in multiparton interactions\\ 41 -- 49 & particles produced by initial-state-showers\\ 51 -- 59 & particles produced by final-state-showers\\ 61 -- 69 & particles produced by beam-remnant treatment\\ 71 -- 79 & partons in preparation of hadronization process\\ 81 -- 89 & primary hadrons produced by hadronization process\\ 91 -- 99 & particles produced in decay process, or by Bose-Einstein effects\\ \hline \end{tabular}\\[2mm] Whenever a particle is allowed to branch or decay further its status code is negated (but it is \textit{never} removed from the event record), such that only particles in the final state remain with positive codes. The \texttt{isFinal()} method returns \texttt{true/false} for positive/negative status codes. \subsection{History information} The two mother and two daughter indices of each particle provide information on the history relationship between the different entries in the event record. The detailed rules depend on the particular physics step being described, as defined by the status code. As an example, in a $2 \to 2$ process $a b \to c d$, the locations of $a$ and $b$ would set the mothers of $c$ and $d$, with the reverse relationship for daughters. When the two mother or daughter indices are not consecutive they define a range between the first and last entry, such as a string system consisting of several partons fragment into several hadrons. There are also several special cases. One such is when ``the same'' particle appears as a second copy, e.g. because its momentum has been shifted by it taking a recoil in the dipole picture of parton showers. Then the original has both daughter indices pointing to the same particle, which in its turn has both mother pointers referring back to the original. Another special case is the description of ISR by backwards evolution, where the mother is constructed at a later stage than the daughter, and therefore appears below in the event listing. If you get confused by the different special-case storage options, the two \texttt{pythia.event.motherList(i)} and \texttt{pythia.event.daughterList(i)} methods are able to return a \texttt{vector} of all mother or daughter indices of particle \texttt{i}. \subsection{Colour flow information} The colour flow information is based on the Les Houches Accord convention \cite{leshouchesaccord}. In it, the number of colours is assumed infinite, so that each new colour line can be assigned a new separate colour. These colours are given consecutive labels: 101, 102, 103, \ldots . A gluon has both a colour and an anticolour label, an (anti)quark only (anti)colour. While colours are traced consistently through hard processes and parton showers, the subsequent beam-remnant-handling step often involves a drastic change of colour labels. Firstly, previously unrelated colours and anticolours taken from the beams may at this stage be associated with each other, and be relabelled accordingly. Secondly, it appears that the close space--time overlap of many colour fields leads to reconnections, i.e. a swapping of colour labels, that tends to reduce the total length of field lines. \begin{thebibliography}{99} \bibitem{pythiaeight} T. Sj\"ostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. {\bf 178} (2008) 852 [arXiv:0710.3820] \bibitem{pythiasix} T. Sj\"ostrand, S. Mrenna and P. Skands, JHEP {\bf 05} (2006) 026 [hep-ph/0603175] \bibitem{rpp} Particle Data Group, C. Amsler et al., Physics Letters {\bf B667} (2008) 1 \bibitem{leshouchesaccord} E. Boos et al., in the Proceedings of the Workshop on Physics at TeV Colliders, Les Houches, France, 21 May - 1 Jun 2001 [hep-ph/0109068] \end{thebibliography} \end{document} pythia8-8.1.80.orig/xmldoc/Glossary.xml0000444000175000017500000000560112217346303016145 0ustar sunsun

    Glossary

    BR
    Beam Remnants; not much used since it may be confused with Branching Ratio
    BSM
    Beyond-the-Standard-Model physics, as a generic term for anything not contained within the SM
    FSR
    Final-State Radiation, implemented in terms of timelike showers
    LHA
    Les Houches Accord for user processes, describing which process-level information should be stored to allow further showering and hadronization of "skeleton" hard processes
    LHAPDF
    Les Houches Accord Parton Distribution Functions, originally a standard format for defining PDF's and later a library with such PDF's
    LHEF
    Les Houches Event File(s), a file format for storing LHA process and event information
    ISR
    Initial-State Radiation, implemented in terms of spacelike showers
    MPI
    Multiparton Interactions, i.e. several (more or less) independent parton-parton subcollisions as part of a hadron-hadron event (previously called MI for multiple interactions)
    MSSM
    Minimal Supersymmetric extension of the Standard Model
    PDF
    Parton Distribution Function (alternatively Parton Density Function)
    PDG code
    a scheme for assigning unique integers, particle identity codes, to known and hypothetical particles; code rules and tables are published in the RPP (see below).
    pileup
    several hadron-hadron collisions in a bunch crossing; not to be confused with MPI
    RPP
    Review of Particle Physics, the biannual review by the ParticleData Group (PDG) from which many Standard-Model parameter values and much particle data has been taken (but, given the poor data on many hadron resonances, a lot of extra (guess)work is needed)
    setting
    collectively used to denote all the boolean flag, integer mode, double-precision parm and string word variables that can be set by the user to steer the behaviour of a run; normally particle data are considered separately but clearly are closely related
    SLHA
    SUSY Les Houches Accord for interchange of mass and coupling information in SUSY scenarios, via a well-defined file format
    SM
    the Standard Model of particle physics
    SUSY
    SUperSYmmetry
    units
    Normal PYTHIA input, internal operations and output is based on a set of standard units, such as:
    GeV for all energies, momenta and masses, always with c = 1;
    mm for all distances and mm/c for all times, so that again they match for c = 1;
    mb for all cross sections (but input or output via the Les Houches Accord takes into account that the unit there is pb)
    pythia8-8.1.80.orig/xmldoc/UMEPSMerging.xml0000444000175000017500000002204512217346320016544 0ustar sunsun

    Unitarised Matrix Element + Parton Shower Merging

    Pythia offers the possibility to use the unitarised matrix element + parton shower merging scheme, as presented in Lon12. Unitarised ME+PS merging (UMEPS) allows for a consistent inclusion of tree-level multi-parton matrix elements into Pythia, and prevents potential changes in the inclusive production cross section. This makes it theoretically more appealing than CKKW-L merging. As in CKKW-L, UMEPS merging requires the user to supply Les Houches Event File input.

    UMEPS is different from other tree-level merging schemes in that it contains events with negative weights. These are generated by constructing parts of no-emission probabilities by reweighted higher-multiplicity samples Lon12. The main philosophy of UMEPS is "subtract what you add", meaning that in order to ensure the stability of the inclusive cross section, one has to counter the inclusion of additional tree-level matrix elements by "subtraction terms".

    The scheme closely reflects how unitarity is achieved in a non-merged shower, and indeed explicitly enforces the cancellations that are implicitly happening in a non-merged shower. This makes very low merging scale values possible.

    The usage of UMEPS is illustrated in the sample main program main86.cc, together with the input file main86.cmnd.

    Unitarised merging is heavily indebted to CKKW-L merging, and shares many settings with CKKW-L. In particular,

             The hard process (Merging:Process)needs to be defined exactly as in CKKW-L (see Defining the hard process in the CKKW-L documentation).

             The merging scale value (Merging:TMS) has to be set.

             The maximal number of additional partons Merging:nJetMax has to be set.

    UMEPS further shares the switches listed under the sections "Matrix element merging and HepMC output for RIVET" and "Further variables" in the CKKW-L documentation with CKKW-L merging. Also, all MergingHooks routines that allow for user interference in CKKW-L merging are also usable for UMEPS -- with the exception of a user-defined merging scale. Currently, UMEPS is only implemented for a merging scale defined by the minimal Pythia evolution pT value between sets of radiator, emitted and recoiler partons. This is no fundamental limitation of the method, and will possibly be lifted in the future. Since this merging scale definition is not completely obvious, UMEPS also shares the Merging:enforceCutOnLHE switch with CKKW-L. In this way, it is possible to use LHE files that are regularised only with weak cuts as input, while the merging machinery imposes the stronger merging scale cut automatically. This means that no merging scale implementation is required from the user side, but also means that it is the user's responsibility to ensure that the cuts used for generating input LHE files are always looser than the cut given by the merging scale value Merging:TMS.


    UMEPS merging with main86.cc

    The UMEPS procedure is illustrated in the sample main program main86.cc (with the input card main86.cmnd). This program produces HepMC events Dob01, that can be histogrammed (e.g. using RIVET Buc10), or used as input for a detector simulation. If the user is not familiar with HepMC analysis tools, it is possible to instead use Pythia's histogramming routines. For this, remove the lines referring to HepMC, and histogram events as illustrated (for CKKW-L) for the histogram histPTFirstSum in main84.cc, i.e. using weight*normhepmc as weight.

    In principle, no changes to main86.cc are necessary. Instead, all settings can be transferred to main86.cc through an input file. The input LHE files are also part of the (command line) input of main86.cc. Note that the sample program assumes that LHE file names are of the form name_tree_#nAdditionalJets.lhe. If you want to e.g. use the LHE files that are shipped with the Pythia distribution, you can execute main86.exe with the command

    ./main86.exe ./main86.cmnd ./w_production ./myhepmc.hepmc

    Since main86.cc is currently the "front-end" for UMEPS merging, we will briefly discuss this sample program in the following.

    Inputs

    In its current form, main86.cc uses separate tree-level LHE files for different numbers of additional partons as input. If e.g. UMEPS merging for W-boson + up to two additional partons is to be performed, three LHE files (for W+zero, W+one, W+two partons) are required. The configurations in the input files should be regularised with inclusive (i.e. weak) cuts. The actual "merging scale cut" will be handled internally. If e.g. Merging:TMS = 15 is the desired merging scale value, it is acceptable to regularise the matrix element calculation for Higgs+jets events at the LHC with the loose cuts pTjet = 5 GeV, ΔRjetA jetB = 0.01 and QjetA jetB = 5 GeV.

    All input settings are handed to main86.cc in the form of an input file. This input file has to contain

             The number of desired events (Main:numberOfEvents)

             The hard process (Merging:Process)

             The merging scale value (Merging:TMS)

             The maximal number of additional partons (Merging:nJetMax).

    Other settings are of course allowed. However, please refrain from adding switches that are used to invoke other merging schemes (e.g. Merging:doKTMerging) into the input file, since this can cause problems.

    Program flow

    The sample program starts by estimating the cross section for samples with different jet multiplicities. For this, the switch Merging:doXSectionEstimate is invoked together with the merging scale definition of Merging:doUMEPSTree, which corresponds to the minimal Pythia evolution pT value. We will come back to the latter switch below. All showering, multiparton interactions and hadronisation is, for speed reasons, switched off when estimating the cross section, since the hard cross section estimate would not be influenced by the event evolution anyway.

    After the hard cross sections are known (including the application of the merging scale cut), the first part of the UMEPS events is generated by using the following switch. Reweight events according to the UMEPS prescription for tree-level configurations.

    The weight generated by the UMEPS procedure can be accessed by using the function double Info::mergingWeight(). When printing (or histogramming) merged events, this weight, multiplied with the estimated cross section for the current sample, should be used as event weight (or to fill histogram bins).

    After this first part is complete, the outcome is an addition of reweighted tree-level samples. To restore the inclusive cross section (i.e. that the cross section after merging corresponds to the cross section of the hard process, without any additional jets), it is necessary to subtract samples. Parton shower unitarity leads to the conclusion that "resolved" and "unresolved" corrections always cancel between states that contain an additional resolved jet, and states in which we "integrate over" the phase space of the additional jet. main86.cc makes this cancellation explicit by producing (correctly weighted) counter events by switching on Reweight events according to the UMEPS prescription of reweighted, integrated configurations. Please note that, in order for this to work smoothly, the switch Merging:doUMEPSTree has to be turned off.

    The integration is achieved internally, and the number of desired integrations (which is always one for UMEPS counter events) is set by Number of hard partons to integrate out in the UMEPS procedure.

    Again, the weight generated by the UMEPS procedure can be accessed by using the function double Info::mergingWeight(). This weight, multiplied with the cross section of the current sample, and multiplied by -1, should then be used as event weight (or to fill histogram bins).

    Before returning, main86.cc prints the merged cross section after UMEPS merging. pythia8-8.1.80.orig/xmldoc/BeamParameters.xml0000444000175000017500000002654312217346277017254 0ustar sunsun

    Beam Parameters

    The settings on this page relate to the beam identities and energies, to a beam momentum spread and to a beam interaction spot. As always, momenta and energies are to be given in units of GeV, and of space and time in mm.

    Incoming beams

    There are two ways to set the identities and energies of the two incoming beam particles. One is to use the init() method with no arguments. Then the settings variables below will be read and used. The alternative is to call init(...) with arguments that provide this information. Then you need not use the variables below (although it would still be possible). Note that, if nothing is done, you will default to LHC at 14 TeV.

    Currently the beam particles must be either a hadron pair or a lepton pair. In the former category p p and pbar p combinations dominate, but it is also possible to combine with pi^+, pi^- and pi^0. In the latter e^+ e^- and mu^+ mu^- would be the most useful combinations, but also others should work if combined with an appropriate hard process. The PDG id code for the first incoming particle. Allowed codes include
    2212 = p, -2212 = pbar,
    2112 = n, -2112 = nbar,
    211 = pi^+, -211 = pi^-, 111 = pi^0,
    990 = Pomeron (used in diffractive machinery; here mainly for debug purposes),
    11 = e^-, -11 = e^+,
    13 = mu^-, -13 = mu^+,
    and a few more leptons/neutrinos in a few combinations.
    The PDG id code for the second incoming particle. Choice of frame for the two colliding particles. For options 1 - 3 the beam identities are specified above, while they are obtained by the Les Houches information for options 4 and 5. Collision CM energy, to be set if Beams:frameType = 1. The energy of the first incoming particle, moving in the +z direction, to be set if Beams:frameType = 2. If the particle energy is smaller than its mass it is assumed to be at rest. The energy of the second incoming particle, moving in the -z direction, to be set if Beams:frameType = 2. If the particle energy is smaller than its mass it is assumed to be at rest. The p_x component of the first incoming particle, to be set if Beams:frameType = 3. The p_y component of the first incoming particle, to be set if Beams:frameType = 3. The p_z component of the first incoming particle, to be set if Beams:frameType = 3. The p_x component of the second incoming particle, to be set if Beams:frameType = 3. The p_y component of the second incoming particle, to be set if Beams:frameType = 3. The p_z component of the second incoming particle, to be set if Beams:frameType = 3. The name of a Les Houches Event File, to be set if Beams:frameType = 4. As some information in a Les Houches Event File init block is only known at the end of generation, some programs choose to output this as a separate file. If Beams:LHEFheader is given, information up till the end of the init block is read from this file, with the events themselves read as usual from the file given in Beams:LHEF. Allow to begin reading events from a new LHEF or or a new LHAup instance without a completely new initialization. Only useful when Beams:frameType = 4 or 5. Read in LHEF header blocks and store them in the Info class. See also LHAupLHEF for more information. Skip the first nSkip events of the input stream (cf. the LHAup::skipEvent(nSkip) method). Only used when Beams:frameType = 4 or 5.

    Beam momentum spread

    This framework currently is intended for a modest beam spread, such as experienced at hadron colliders. Thus it can be safely assumed that the physics does not change over the CM energy range probed, so that the parameters of the physics initialization at the nominal energy can be used as is. Currently it can not be used for the more extensive energy spread expected at linear e^+ e^- colliders. Also, any attempt to combine it with external Les Houches input of parton-level events is at own risk.

    On this page you can set the momentum spread according to a simple Gaussian distribution. If you instead want a more sophisticated parametrization, you can write and link your own BeamShape class. Allow the beam momenta to be smeared around their initialization nominal values. The width of a Gaussian distribution of the p_x spread of the first incoming particle. The width of a Gaussian distribution of the p_y spread of the first incoming particle. The width of a Gaussian distribution of the p_z spread of the first incoming particle. The triply Gaussian distribution (p_x, p_y, p_z) is restricted to a maximal total deviation from the nominal values (p_x0, p_y0, p_z0) for the first incoming particle, like (p_x - p_x0)^2/sigma_px^2 + (p_y - p_y0)^2/sigma_py^2 + (p_z - p_z0)^2/sigma_pz^2 < maxDev^2 (Note the absence of a factor 2 in the denominator, unlike the Gaussians used to pick (p_x, p_y, p_z).) The width of a Gaussian distribution of the p_x spread of the second incoming particle. The width of a Gaussian distribution of the p_y spread of the second incoming particle. The width of a Gaussian distribution of the p_z spread of the second incoming particle. The triply Gaussian distribution (p_x, p_y, p_z) is restricted to a maximal total deviation from the nominal values (p_x0, p_y0, p_z0), for the second incoming particle, like (p_x - p_x0)^2/sigma_px^2 + (p_y - p_y0)^2/sigma_py^2 + (p_z - p_z0)^2/sigma_pz^2 < maxDev^2 (Note the absence of a factor 2 in the denominator, unlike the Gaussians used to pick (p_x, p_y, p_z).)

    Beam interaction vertex

    On this page you can set the spread of the interaction vertex according to a simple Gaussian distribution. If you instead want a more sophisticated parametrization, you can write and link your own BeamShape class. Allow the interaction vertex of the two colliding beams to be smeared. If off, then the vertex is set to be the origin. The width of a Gaussian distribution of the x location of the interaction vertex. The width of a Gaussian distribution of the y location of the interaction vertex. The width of a Gaussian distribution of the z location of the interaction vertex. The triply Gaussian distribution of interaction vertex position (x, y, z) is restricted to a maximal total deviation from the origin, like x^2/sigma_x^2 + y^2/sigma_y^2 + z^2/sigma_z^2 < maxDevVertex^2 (Note the absence of a factor 2 in the denominator, unlike the Gaussians used to pick (x, y, z).) The width of a Gaussian distribution of the collision time (in units of mm/c). Note that, if the above space parametrization is viewed as the effect of two incoming beams along the +-z axis, with each beam having a Gaussian spread, then the spread of the time would also become a Gaussian with the same width as the z one (times the velocity of the beams, which we expect is close to unity). For flexibility we have not enforced any such relation, however. The collision time is restricted to be in the range |t| < sigma_t * maxDevTime.

    The distributions above are all centered at the origin. It is also possible to shift the above distributions to be centered around another nominal position. You must have Beams:allowVertexSpread = on to use this possibility. The x location of the interaction vertex is centered at this value. The y location of the interaction vertex is centered at this value. The z location of the interaction vertex is centered at this value. The time t of the interaction vertex is centered at this value. pythia8-8.1.80.orig/xmldoc/SUSYLesHouchesAccord.xml0000444000175000017500000003757212217346317020265 0ustar sunsun

    SUSY Les Houches Accord

    The PYTHIA 8 program does not contain an internal spectrum calculator (a.k.a. RGE package) to provide supersymmetric couplings, mixing angles, masses and branching ratios. Thus the SUSY Les Houches Accord (SLHA) Ska04All08 is the only way of inputting SUSY models, and SUSY processes (see the SUSYProcesses page) cannot be run unless such an input has taken place.

    The SLHA input format can also be extended for use with more general BSM models, beyond SUSY. Information specific to how to use the SLHA interface for generic BSM models is collected below, under Using SLHA for generic BSM Models, with more elaborate explanations and examples in Des11.

    Most of the SUSY implementation in PYTHIA 8 is compatible with both the SLHA1 Ska04 and SLHA2 All08 conventions (with some limitations for the NMSSM in the latter case). Internally, PYTHIA 8 uses the SLHA2 conventions and translates SLHA1 input to these when necessary. See the section on SUSY Processes and Des11 for more information. Note that PYTHIA assumes that a spectrum is either fully SHLA1 or fully SLHA2 compliant. Mixing of the two standards is discouraged, as this can lead to ambiguities and inconsistencies.

    When reading LHEF files, Pythia automatically looks for SLHA information between <slha>...</slha> tags in the header of such files. When running Pythia without LHEF input (or if reading an LHEF file that does not contain SLHA information in the header), a separate file containing SLHA information may be specified using SLHA:file (see below).

    Normally the LHEF would be in uncompressed format, and thus human-readable if opened in a text editor. A possibility to read gzipped files has been added, based on the Boost and zlib libraries, which therefore have to be linked appropriately in order for this option to work. See the README file in the main directory for details on how to do this.

    Finally, the SLHA input capability can of course also be used to input SLHA-formatted MASS and DECAY tables for other particles, such as the Higgs boson, furnishing a less sophisticated but more universal complement to the standard PYTHIA 8-specific methods for inputting such information (for the latter, see the section on Particle Data and the scheme to modify it). This may at times not be desirable, so a few options can be used to curb the right of SLHA to overwrite particle data. Conversely, it is sometimes useful to allow the user to modify eg a mass parameter relative to its value in the SLHA spectrum. This is normally not permitted (the SLHA spectrum is normally self-consistent and should not be modified), but an option for allowing it is provided.

    The reading-in of information from SLHA or LHEF files is handled by the SusyLesHouches class, while the subsequent calculation of derived quantities of direct application to SUSY processes is done in the CoupSUSY, SigmaSUSY, and SUSYResonanceWidths classes.

    Sanity Checks

    As an aid for basic validation, some checks and ranges are imposed on SLHA input during initialization, as follows:
    • Several parameters (SLHA:keepSM, minMassSM, and SLHA:allowUserOverride) provide some safety against unintentionally overwriting PYTHIA's Standard-Model information. These parameters can be altered to hand over more or less control to the SLHA interface. In particular, a lot of mass and decay-table information may be included by default in some SLHA files, without it being the explicit intention of the user to overwrite the corresponding PYTHIA information. The default values of the SLHA safety parameters have been chosen so as to eliminate at least the most obvious causes of Garbage In Garbage Out. (E.g., there is usually no reason to modify the masses of well-measured SM particles, like the W and Z bosons, nor to replace their sophisticated internal decay treatments by the simplified isotropic treatment used for SLHA DECAY tables.)
    • For SLHA SUSY spectra, the interface checks the mass-ordering of the Higgs, Neutralino, and Chargino sectors, and the unitarity/orthogonality of the mixing matrices. It also performs some additional self-consistency checks on whether the correct SLHA BLOCKs for the given SUSY model have been included, and whether all required entries have been defined.
    • If MASS or DECAY information for a particle has been changed by SLHA input, the following sanity checks will be carried out. The particle will be declared stable unless there is at least one on-shell decay channel open (regardless of the presence of any DECAY information). In particular, massless particles will always be declared stable. A lower cutoff is imposed on the Breit-Wigner shape of the particle, requiring its mass to remain above the sum of masses for the lightest decay channel. Subject to that constraint, the lower cutoff will normally be placed at 5 times the width (so that the default gives a decent sampling of the shape), but the user is allowed to use the mMin parameter to choose a larger sampling range if so desired (still subject to the on-shell constraint).
    • For each decay channel in an SLHA DECAY table, PYTHIA will checks the available phase space. If the channel is on shell (sum of daughter masses is less than mass of decaying particle), then the threshold dependence is given by SLHA:meMode. If the channel is off shell, then an meMode of 100 is always used. As a further protection against GIGO, if the channel appears to be physically impossible (defined as requiring fluctuations of more than more than 100 times the effective combined widths), it is switched of and a warning message is printed.
    • DECAY table branching fractions are always interpreted as positive. However, a negative sign for one or more channels can be given, and will then be interpreted to mean that the corresponding channel(s) should be switched off for the current run. This furnishes a simple way to switch SLHA DECAY channels on and off while preserving the sum of branching fractions equal to unity.
    Note that these sanity checks will not catch all possible cases of Garbage In Garbage Out, so human verification of the input files is always a good idea, as is taking a look at any warnings or error messages printed by the SLHA interface during initialization. It is ultimately up to the user to ensure that sensible input is being given.

    SLHA Switches and Parameters

    Controls from where SLHA information is read. Name of an SLHA (or LHEF) file containing the SUSY/BSM model definition, spectra, and (optionally) decay tables. Default void signals that no such file has been assigned. Some programs write SLHA output also for SM particles where normally one would not want to have masses and decay modes changed unwittingly. Therefore, by default, known SM particles are ignored in SLHA files. To be more specific, particle data for identity codes in the ranges 1 - 24 and 81 - 999,999 are ignored. Notably this includes Z^0, W^+- and t. The SM Higgs is modified by the SLHA input, as is other codes in the range 25 - 80 and 1,000,000 - . If you switch off this flag then also SM particles are modified by SLHA input. This parameter provides an alternative possibility to ignore SLHA input for all particles with identity codes below 1,000,000 (which mainly means SM particle, but also includes e.g. the Higgs bosons in two-Higgs-doublet scenarios) whose default masses in PYTHIA lie below some threshold value, given by this parameter. The default value of 100.0 allows SLHA input to modify the top quark, but not, e.g., the Z^0 and W^+- bosons. Flag to set whether the user is allowed to modify the parameters read from an SLHA spectrum. Is normally kept off to preserve the internal self-consistency of SLHA spectra. If this flag is switched on, the mass values read from the SLHA block MASS are allowed to be modified by the user, using PYTHIA's standard readString and related methods.

    SLHA DECAY Tables

    In addition to SUSY spectra, the SLHA also defines a set of conventions for decay tables. These are not restricted to SUSY models, but can be used for arbitrary particles, either in combination with or independently of the SUSY parts of the Accord. The settings in this section control whether and how PYTHIA will make use of such tables. See also the comments under sanity checks above. Note: the PYTHIA SLHA interface is limited to at most 1→8 decays. Switch to choose whether to read in SLHA DECAY tables or not. If this switch is set to off, PYTHIA will ignore any decay tables found in the SLHA file, and all decay widths will be calculated internally by PYTHIA. If switched on, SLHA decay tables will be read in, and will then supersede PYTHIA's internal calculations, with PYTHIA only computing the decays for particles for which no SLHA decay table is found. (To set a particle stable, you may either omit an SLHA DECAY table for it and then use PYTHIA's internal id:MayDecay switch for that particle, or you may include an SLHA DECAY table for it, with the width set explicitly to zero.) This value specifies how threshold, off-shell, and phase-space weighting effects for SLHA decay channels should be treated, using the same numbering scheme as for resonances. The default (100) is to use the branching fraction given in the SLHA DECAY tables without any modifications. The corresponding partial widths remain unchanged when the resonance fluctuates in mass. Specifically there are no threshold corrections. That is, if the resonance fluctuates down in mass, to below the nominal threshold for some decay mode, it is assumed that one of the daughters could also fluctuate down to keep the channel open. (If not, there may be problems later on.) Alternative options (with values 101+) documented under resonances allow for some flexibility to apply threshold factors expressing the closing of the on-shell phase space when the daughter masses approach or exceed the parent one. Note that modes that are extremely far off shell (defined as needing a fluctuation of more than 100 times the root-sum-square of the widths of the mother and daughter particles) will always be assigned meMode = 100 and should be switched off by hand if so desired. It is up to the user to ensure that the final behaviour is consistent with what is desired (and/or to apply suitable post facto reweightings). Plotting the generator-level resonance and decay-product mass distributions (and e.g., mass differences), effective branching fractions, etc, may be of assistance to validate the behaviour of the program.

    Internal SLHA Variables

    Controls amount of text output written by the SLHA interface, with a value of 0 corresponding to the most quiet mode. The following variables are used internally by PYTHIA as local copies of SLHA information. User changes will generally have no effect, since these variables will be reset by the SLHA reader during initialization. Corresponds to SLHA block MODSEL entry 3.

    Using SLHA for generic BSM Models

    Using the QNUMBERS extension Alw07, the SLHA can also be used to define new particles, with arbitrary quantum numbers. This already serves as a useful way to introduce new particles and can be combined with MASS and DECAY tables in the usual way, to generate isotropically distributed decays or even chains of such decays. (If you want something better than isotropic, sorry, you'll have to do some actual work ...)

    A more advanced further option is to make use of the possibility in the SLHA to include user-defined blocks with arbitrary names and contents. Obviously, standalone PYTHIA 8 does not know what to do with such information. However, it does not throw it away either, but instead stores the contents of user blocks as strings, which can be read back later, with the user having full control over the format used to read the individual entries.

    The contents of both standard and user-defined SLHA blocks can be accessed in any class inheriting from PYTHIA 8's SigmaProcess class (i.e., in particular, from any semi-internal process written by a user), through its SLHA pointer, slhaPtr, by using the following methods:
    bool slhaPtr->getEntry(string blockName, double& val);
    bool slhaPtr->getEntry(string blockName, int indx, double& val);
    bool slhaPtr->getEntry(string blockName, int indx, int jndx, double& val);
    bool slhaPtr->getEntry(string blockName, int indx, int jndx, int kndx, double& val);

    This particular example assumes that the user wants to read the entries (without index, indexed, matrix-indexed, or 3-tensor-indexed, respectively) in the user-defined block blockName, and that it should be interpreted as a double. The last argument is templated, and hence if anything other than a double is desired to be read, the user has only to give the last argument a different type. If anything went wrong (i.e., the block doesn't exist, or it doesn't have an entry with that index, or that entry can't be read as a double), the method returns false; true otherwise. This effectively allows to input completely arbitrary parameters using the SLHA machinery, with the user having full control over names and conventions. Of course, it is then the user's responsibility to ensure complete consistency between the names and conventions used in the SLHA input, and those assumed in any user-written semi-internal process code.

    Note that PYTHIA 8 always initializes at least the SLHA blocks MASS and SMINPUTS, starting from its internal SM parameters and particle data table values (updated to take into account user modifications). These blocks can therefore be accessed using the slhaPtr->getEntry() methods even in the absence of SLHA input. Note: in the SMINPUTS block, PYTHIA outputs physically correct (i.e., measured) values of GF, m_Z, and alpha_EM(m_Z). However, if one attempts to compute, e.g., the W mass, at one loop from these quantities, a value of 79 GeV results, with a corresponding value for the weak mixing angle. We advise to instead take the physically measured W mass from block MASS, and recompute the EW parameters as best suited for the application at hand.

    pythia8-8.1.80.orig/xmldoc/RHadrons.xml0000444000175000017500000001576212217346317016100 0ustar sunsun

    R-hadrons

    When a coloured SUSY particle is longer-lived than typical hadronization scales, i.e. around c*tau > 1 fm, or equivalently width Gamma < 0.2 GeV, it will have time to hadronize into a colour singlet hadronic state, a R-hadron. Currently a set of such R-hadrons have been implemented for the case of a long-lived gluino, stop or sbottom. Needless to say, the normal case would be that only one of them will be long-lived enough to form R-hadrons.

    For simplicity all gluino-mesons are assumed to have light-flavour spin 1, since those are the lightest and favoured by spin-state counting. Further, all gluino-baryons are bookkept as having light-flavour spin 3/2, and flavours are listed in descending order. This is more for convenience of notation, however, since the normal baryon octet e.g. has no uuu = "p++" state. When a diquark is extracted, a mixture of spin 0 and spin 1 is allowed. Names and codes are essentially in agreement with the PDG conventions, e.g.
    1000993 R0(~g g) (or gluinoball)
    1009213 R+(~g u dbar) (or gluino-rho+)
    1092214 R+(~g uud) (or gluino-Delta+)
    For internal bookkeeping of momenta, the code 1009002, Rtemp(~g q), is used to denote the intermediate state formed when only one of the two string pieces attached to the gluino has broken.

    For the stop- and sbottom-hadrons the spin counting is simpler, since it is entirely given by the constituent quark or diquark spin. Again names and codes follow PDG conventions, e.g.
    1000612 R+(~t dbar)
    1006211 R+(~t ud0)

    The spin and electromagnetic charge of the new particle plays only a minor role in the hadronization process, that can be neglected to first approximation. Therefore it is possible to use the same R-hadrons framework instead for other BSM scenarios with long-lived coloured particles, e.g. with massive extra-dimensions copies of gluons and quarks, or with leptoquarks. This can be regulated by the switches below. Note that the codes and names of the R-hadrons is not changed when the heavy particle involved is switched, for reasons of administrative simplicity. R-hadron mass spectra and other relevant particle data is automatically updated to reflect the change, however. Allows the gluino, stop and sbottom to hadronize if their respective widths are below the limit RHadrons:maxWidth. The maximum width of the gluino for which it is possible to form R-hadrons, provided that RHadrons:allow is on. The gluino identity code. For other scenarios than SUSY this code could be changed to represent another long-lived uncharged colour octet particle, that then would be treated in the same spirit. Could be set to 0 to forbid any gluino R-hadron formation even when the above two criteria, RHadrons:allow and RHadrons:maxWidth, are met. The lightest stop identity code. For other scenarios than SUSY this code could be changed to represent another long-lived charge 2/3 colour triplet particle, that then would be treated in the same spirit. As above it could be set to 0 to forbid any stop R-hadron formation. The lightest sbottom identity code. For other scenarios than SUSY this code could be changed to represent another long-lived charge -1/3 colour triplet particle, that then would be treated in the same spirit. As above it could be set to 0 to forbid any sbottom R-hadron formation. Allows the R-hadrons to decay or not. If the gluino/stop/sbottom is stable or too long-lived to decay inside the detector this switch has no real function, since then no decays will be performed anyway. If the sparticle is so short-lived that it decays before reaching the beam pipe then having the decay on is the logical choice. So the interesting region is when the decays happens after the R-hadron has passed through part of the detector, and changed its momentum and quite possibly its flavour content before it is to decay. Then normal decays should be switched off, and the R-hadron tracked through matter by a program like GEANT Kra04,Mac07. After that, the new R-hadron info can be overwritten into the event record and the Pythia::forceRHadronDecay() method can be called to force this modified R-hadron to decay. Use simple mass formulae to construct all available R-hadron masses based on the currently initialized gluino/squark masses and the constituent masses of the other partons in the hadron. If you switch this off, it is your responsibility to set each of the R-hadron masses on your own, and set them in an internally consistent way. If you mess up on this you may generate accordingly crazy results. Specifically, it is to be assumed that none of the R-hadrons has a mass below its constituent sparticle, i.e. that the light degrees of freedom and the additional confinement gluon field gives a net positive contribution to the R-hadron mass. The fraction of produced gluino R-hadrons that are contain a "valence" gluon, with the rest containing a meson or baryon quark flavour content. Extra mass (in GeV) added to each of the one or two extra constituent masses in an R-hadron, to calculate the mass of a R-hadron. The same offset is also used when the R-hadron momentum and mass is split between the squark or gluino and the one or two light (di)quarks, one for a squark and two for a gluino. Thus once or twice this amount represents a part of the nominal squark or gluino mass that will not decay weakly, since it is taken to correspond to the cloud of gluons that surround the squark or gluino. A colour singlet system with an invariant mass less than this amount, above the R-hadron mass with the given flavour content, is assumed to collapse to this single R-hadron, whereas a full fragmentation handling is applied above this mass. Probability that a diquark extracted from the flavour code of a gluino R-hadron should be assigned spin 1, with the rest being spin 0. Does not apply for two identical quarks, where spin 1 is only possibility. Note that gluino R-hadron codes for simplicity are assigned as if spin is 1 always, and so give no guidance. For stop and sbottom the diquark spin is preserved in the particle code, so there is no corresponding issue. pythia8-8.1.80.orig/xmldoc/CompositenessProcesses.xml0000444000175000017500000001545512217346277021106 0ustar sunsun

    Compositeness Processes

    Compositeness scenarios may give rise to sharp resonances of excited quarks and leptons. An excited copy of the first generation is implemented, consisting of spin 1/2 particles. The possibility of contact interactions between SM fermions is also implemented in the context of 2 -> 2 quark or fermion-lepton scattering.

    Related to excited fermions, the current implementation contains gauge interaction production by quark-gluon fusion or lepton-photon fusion and contact interaction production by quark-quark or quark-antiquark scattering. For both the 2 -> 1 and 2 -> 2 processes a non-trivial angular dependence is included in the decay, however, only decays into gauge bosons are supported, i.e. not decays through contact interactions. In additions to the compositeness scale and couplings listed below, you are expected to change the excited-fermion masses in accordance with what is desired. See Bau90 for conventions.

    The contact interactions are implemented according to Eic83. The processes include the SM contributions as well as interference. For this reason the processes below converge toward the SM equivalents when the contact interaction contributions are close to zero, e.g. HardQCD:qq2qq and HardQCD:qqbar2qqbarNew in the case of quark scattering.

    Excited fermions, production processes

    A few different production processes have been implemented, which normally would not overlap and therefore could be run together. Common switch for the group of implemented processes that produce an excited fermion. Scatterings d g -> d^*. Code 4001. Scatterings u g -> u^*. Code 4002. Scatterings s g -> s^*. Code 4003. Scatterings c g -> c^*. Code 4004. Scatterings b g -> b^*. Code 4005. Scatterings e gamma -> e^*. Code 4011. Scatterings mu gamma -> mu^*. Code 4013. Scatterings tau gamma -> tau^*. Code 4015. Scatterings q q(bar) -> d^* q(bar). Code 4021. Scatterings q q(bar) -> u^* q(bar). Code 4022. Scatterings q q(bar) -> s^* q(bar). Code 4023. Scatterings q q(bar) -> c^* q(bar). Code 4024. Scatterings q q(bar) -> b^* q(bar). Code 4025. Scatterings q qbar -> e^*+- e^-+. Code 4031. Scatterings q qbar -> nu_e^* nu_ebar. Code 4032. Scatterings q qbar -> mu^*+- mu^-+. Code 4033. Scatterings q qbar -> nu_mu^* nu_mubar. Code 4034. Scatterings q qbar -> tau^*+- tau^-+. Code 4035. Scatterings q qbar -> nu_tau^* nu_taubar. Code 4036.

    Excited fermions, parameters

    The basic couplings of the model are Compositeness scale Lambda in GeV. Strength f of the SU(2) coupling. Strength f' of the U(1) coupling. Strength f_c of the SU(3) coupling.

    Contact interactions, production processes

    The processes including contact interactions are Scatterings q q -> q q including contact interactions. Code 4201. Scatterings q qbar -> q' qbar' including contact interactions. Code 4202. Scatterings f fbar -> e- e+ including contact interactions. Code 4203. Scatterings f fbar -> mu- mu+ including contact interactions. Code 4204. Scatterings f fbar -> tau- tau+ including contact interactions. Code 4205.

    Contact interactions, parameters

    Number of allowed outgoing new quark flavours in the above q qbar -> q' qbar' process. Similar to HardQCD:nQuarkNew for the QCD processes. Compositeness scale Lambda in GeV. Its overall normalization is largely a matter of convention. The choice made here for the q qbar -> l- l+ processes is such that the pure contact interaction part of the left-left interactions (i.e. disregarding gamma^*, Z^0 and interference terms) has the form d(sigmaHat)/d(tHat) = pi * uHat^2 / (3 * sHat^2 * Lambda^4). The corresponding part of the q qbar -> q' qbar' cross section is a factor 3 larger from colour. Helicity parameter. Helicity parameter. Helicity parameter.
    pythia8-8.1.80.orig/xmldoc/Bibliography.xml0000444000175000017500000002717712217346277017003 0ustar sunsun

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    pythia8-8.1.80.orig/xmldoc/HadronScattering.xml0000444000175000017500000000663512217346303017611 0ustar sunsun

    Hadron Scattering

    A simple hadron scattering model. It is intended to take into account that the overlap of multiple strings at low transverse dimensions is likely to lead to some collective effects, not unlike those observed in heavy-ion collisions, even if not quite as pronounced. Specifically, it is assumed that the hadrons produced can scatter against each other on the way out, before the fragmenting system has had time to expand enough that the hadrons get free. Thereby heavier particles are shifted to higher transverse momenta, at the expense of the lighter ones. Warning: This is still at an experimental level, and should not be used unless you know what you are doing. Master flag for hadron scattering. Perform hadron scattering before or after first round of decays, involving very short-lived particles like the rho. The default is to perform scattering directly after the string fragmentation, before any decays. Allow two hadrons with same parent hadron to scatter. Allow hadrons which have already scattered to scatter again. Even if switched on, the same pair can not scatter off each other twice.

    Hadron selection

    Probability that a hadron is soft enough to scatter. (A high-pT hadron presumably being part of a jet, and thus produced away from the high-particle-density region at small transverse dimensions.) N parameter as above. k parameter as above. p parameter as above.

    Scattering probability

    Probability for a pair of hadrons to scatter. j parameter as above. rMax parameter as above. Use tiling in (eta, phi) to reduce number of pairwise tests.
    pythia8-8.1.80.orig/xmldoc/HepMCInterface.xml0000444000175000017500000001661512217346303017126 0ustar sunsun

    HepMC Interface

    An interface to the HepMC Dob01 standard event record format has been provided by M. Kirsanov. To use it, the relevant libraries need to be linked, as explained in the README and README.HepMC files. Only version 2.06 (or later) of HepMC is supported as of 1 January 2013, by agreement with the LHC experimental community.

    The (simple) procedure to translate PYTHIA 8 events into HepMC ones is illustrated in the main41.cc, main42.cc main61.cc and main62.cc main programs. At the core is a call to the

    HepMC::Pythia8ToHepMC::fill_next_event( pythia, hepmcevt, ievnum = -1) 
    
    which takes a reference of the generator object and uses it, on the one hand, to read out and convert the event record in pythia.event and, on the other hand, to extract and store parton-density (PDF), cross section and other information for the hard subprocess from pythia.info. There is also an alternative form that does not requires access to the full pythia object, but only the event record, at the expense of a reduced information storage, see below.

    While PYTHIA always stores momenta in units of GeV, with c = 1, HepMC nowadays can be built either for MeV or GeV as default, a choice that can then be overridden on an event-by-event basis, see e.g. the main41.cc code. When filling the HepMC event record, PYTHIA will convert to the unit specified for the current HepMC event record.

    Also for length units there are choices, and again the PYTHIA interface will convert to the units set for the HepMC event record. Here the mm choice of PYTHIA seems to be shared by most other programs, and is HepMC default.

    The status code is now based on the new standard introduced for HepMC 2.05, see the Event::statusHepMC(...) conversion routine for details.

    The current values from pythia.info.sigmaGen() and pythia.info.sigmaErr() are stored for each event, multiplied by 10^9 to convert from mb to pb. Note that PYTHIA improves its accuracy by Monte Carlo integration in the course of the run, so the values associated with the last generated event should be the most accurate ones. If events also come with a dimensional weight, like in some Les Houches strategies, this weight is in units of pb.

    The public methods

    Here comes a complete list of all public methods of the Pythia8ToHepMC class in the HepMC (not Pythia8!) namespace. the constructor and destructor take no arguments. convert a Pythia event to a HepMC one. Will return true if succeeded. the input Pythia generator object, from which both the event and other information can be obtained. the output GenEvt event, in its standard form. set the event number of the current event. If negative then the internal event number is used, which is incremented by one for each new event. convert a Pythia event to a HepMC one. Will return true if succeeded. the input Pythia event that is to be converted to HepMC format. the output GenEvt event, in its standard form. set the event number of the current event. If negative then the internal event number is used, which is incremented by one for each new event. pointer to the Pythia Info object, which is used to extract PFD values, and process and cross section information. Without such a pointer this information therefore cannot be stored, i.e. it is equivalent to the three set_store methods below being set false. pointer to the Pythia Settings object, which is used to decide whether hadronization is carried out, and therefore whether to warn about unhadronized partons. Without such a pointer the set_free_parton_warnings method below uniquely controls the behaviour.

    The following paired methods can be used to set and get the status of some switches that modify the behaviour of the conversion routine. The set methods have the same default input values as the internal initialization ones, so that a call without an argument (re)stores the default. print a warning line, on cerr, when inconsistent mother and daughter information is encountered. check and print a warning line when unhadronized gluons or quarks are encountered in the event record. Does not apply when Pythia hadronization is switched off. Default is to do this check. if problems (like the free partons above) are encountered then the run is interrupted by an exit(1) command. Default is not to crash. the normal gluon identity code 21 is used also when parton density information is stored, unless this optional argument is set true to have gluons represented by a 0. This choice does not affect the normal event record, where a gluon is always 21. for each event store information on the two incoming flavours, their x values and common factorization scale, and the values of the two parton distributions, xf(x,Q). for each event store information on the Pythia process code, the renormalization scale, and alpha_em and alpha_s values used for the hard process. for each event store information on the Pythia cross section and its error, in pb, and the event weight. If events also come with a dimensional weight, like in some Les Houches strategies, this weight is in units of pb. pythia8-8.1.80.orig/xmldoc/UpdateHistory.xml0000444000175000017500000035124512217615210017152 0ustar sunsun

    Update History

    These update notes describe major updates relative to the baseline PYTHIA 8.100 version. However, they are less extensive than the corresponding update notes for PYTHIA 6. On the other hand, whereas the PYTHIA 6 manual is a static document, the PYTHIA 8 html/php pages are kept up to date for each subversion.

    Important note:version 8.160 does introduce some elements of backwards incompatibility. Specifically, "multiple interactions", abbreviated MI, has been renamed "multiparton interactions", MPI. This affects many parts of the code and documentation. Also some features are deprecated, although remaining until the end of the 8.1xx version series.

    Main news by version

    • 8.105: 24 February 2008
      • New option to initialize with arbitrary beam directions
        pythia.init( idA, idB, pxA, pyA, pzA, pxB, pyB, pzB)
      • Added capability to set beam energy spread and beam vertex.
        Warning: as a consequence, the old Beams group of settings has been moved to BeamRemnants, and Beams is now instead used for machine beam parameters. Therefore also some Main settings of this character have been regrouped, as follows:
        8.100 setting has been moved to
        Main:idA Beams:idA
        Main:idB Beams:idB
        Main:inCMframe (Beams:frameType)
        Main:eCM Beams:eCM
        Main:eA Beams:eA
        Main:eB Beams:eB
        Main:LHEF Beams:LHEF
      • The forceHadronLevel() method introduced for standalone hadronization.
      • main15.cc illustrated how either full hadronization or only decays of some particles can be looped over for the rest of the event retained.
      • The LHAevnt and LHAinit classes have been joined into a new LHAup one, with new options that allow the writing of a Les Houches Event File.
      • The SusyLesHouches class updated to handle SLHA version 2.
      • Updated HepMC conversion routine.
      • The static ErrorMsg class has been removed and its functionality moved into the non-static Info class, in the renamed Info file.
      • Further reduction of the use of static, with related code changes. This should allow to have several almost independent Pythia instances. Some static classes still remain, however, notably for random number generation and particle properties.
      • Limited capability to use two different Pythia instances for signal + pileup event generation, see main19.cc for an example.
      • In the Event class the = and =+ methods have been overloaded to allow the copying or appending of event records. Illustrated in main19.cc.
      • The html and php page formatting improved with cascading style sheets.
      • Several minor improvements and new options, including updated configure scripts.
    • 8.108: 1 May 2008
      • Correction in the event record, so that the beam particles in line 1 and 2 do not have any mother according to the motherList method. Previously the "system" entry in line 0 was counted as their mother, which gave rise to an unexpected extra vertex in the conversion to the HepMC format.
      • Support for HepMC version 1 is removed, to simplify the code and reflect the evolution of the field.
      • Status codes are stored in HepMC only as 1 for existing and 2 for decayed or fragmented particles (whereas previously the original PYTHIA codes were used for the latter).
      • Parton densities are stored in HepMC as xf(x,Q^2) rather than the f(x,Q^2) used in (some) previous versions.
      • The SusyLesHouches class has been updated so that reading is fully compatible with the SLHA2 standard.
      • Improved handling of the Higgs width, relevant for massive and thereby broad resonance shapes.
      • The matrix elements for neutralino pair production have now been completed and checked.
      • Ensure that alpha_strong does not blow up, by introducing a minimal scale somewhat above Lambda_3 (roughly where alpha_strong = 10).
      • New methods isValence1() and isValence2() in the Info class.
      • Protection against division by zero in calculation of decay vertex (for zero-mass gluons with zero lifetime, where there should be no displacement).
      • A new compilation option -Wshadow is introduced and code is rewritten at all places where this option gave warnings.
      • Minor library correction to allow compilation with gcc 4.3.0.
    • 8.114: 22 October 2008
      • New rescattering description operational (but still experimental) for the case that FSR is not interleaved, but saved until after MPI, ISR and beam remnants have been handled. This involves much new code in several classes.
      • A new class PartonSystems is introduced to keep track of which partons in the event record belong to which subcollision system, plus some further information on each subsystem. It takes over functionality previously found as part of the Event class, but leaves room for future growth.
      • Add optional model, wherein an increased pT0 turnoff scale for MPI and ISR is used for above-average active events, i.e. events that already have several MPI's or ISR emissions.
      • Freeze GRV 94L distribution at small Q^2 to avoid blowup.
      • The pythia.readFile(...) method can now alternatively take an istream as argument instead of a filename.
      • Minor bug correction in PartonLevel.cc; the bug could (rarely) give a segmentation fault.
    • 8.120: 10 March 2009
      • New rescattering description further developed, but not yet recommended for normal usage.
      • Include new processes for Large Extra Dimensions and Unparticles, contributed by Stefan Ask. New test program main28.cc illustrates.
      • Include further SUSY processes: neutralino-chargino and chargino-chargino pairs. The processes should be valid also in the case of non-minimal flavour violation and/or CP violation. Expanded machinery to keep track of SUSY parameters.
      • Include backwards evolution of incoming photon as part of the SpaceShower initial-state radiation description. This allows you to simulate hard collisions where one of the incoming partons is a photon. New test program main43.cc illustrates.
      • Allow separate mass and transverse momentum cuts when two hard subprocesses are generated in the same event.
      • The default value for the border between short- and long-lived particles has been changed from 1 mm to 10 mm, to better conform with LHC standards, see here. The default is still to let all unstable particles decay.
      • New ISR matrix-element correction to f -> f gamma in single W production.
      • New method Event::statusHepMC returns the status code according to the HepMC conventions agreed in February 2009. The interface to HepMC now writes out status according to this convention.
      • Add capability to link to FastJet, with expanded configure script and Makefile, and with main61.cc as new example.
      • Update of Makefile.msc, with added support for latest Visual C++ Express edition and use of regexp to check nmake version.
      • Update of LHAFortran.h and Pythia6Interface.h, to make the interface to Fortran routines work also under Windows. (Thanks to Anton Karneyeu.)
      • Updated and expanded worksheet.
      • The manual pages in the xmldoc directory, and thereby also those of the htmldoc and phpdoc directories, have been significantly updated and expanded. In particular, in many places the class of each method is explicitly shown, as well as the type of the return value and of the arguments. This upgrade is not yet completed, but already covers the more relevant sections.
      • The unary minus operator in the Vec4() returns a reference to a four-vector with all components negated, but leaves the original four-vector unchanged. Previously the four-vector itself was flipped.
      • The pPlus() and pMinus() methods of a four-vector and an event-record particle are renamed pPos() and pNeg(), respectively.
      • Include a further loop in ProcessLevel, so that a new process is generated in case of failures of a less severe nature.
      • Introduce warning message for unexpected meMode in ResonanceWidths.
      • Les Houches event reading framework has been rearranged for more flexibility. Some bugs corrected. Specifically, when scale is not set (scale = -1. in the Les Houches standard), PYTHIA did not attempt to set this scale itself, which typically lead to there not being any ISR or FSR. Now the rules for normal 1-, 2- and 3-body final states are applied, with a trivial extension of the 3-body rules for higher multiplicities.
      • Correct bug in the handling of parton densities, whereby it was not possible to switch to a new set, once a first initialization had been done.
      • Correct bugs when several Pythia::init initialization calls are made in the same run, specifically in the case that pointers to external processes have been handed in.
      • Changes in main03.cmnd and main04.cmnd so that some nonstandard options are commented out rather than active. Related comments inserted also in some other .cmnd files, but there without any change in program execution.
      • A few further minor bug fixes.
      • Update year to 2009.
    • 8.125: 16 June 2009
      • Hadronization and timelike-shower parameter default values updated according to a tune to LEP1 data by Hendrik Hoeth, using the Rivet + Professor framework.
      • Many further SUSY production processes. SLHA readin expanded to cover also masses and decay modes. Example main22.cc updated, while main33.cc now superfluous and removed.
      • Also further processes for extra dimensions.
      • Stefan Ask joins as coauthor.
      • The TimeShower::shower(...) method has gained a new argument, that forces the shower evolution to stop after a given number of branchings. A new method TimeShower::pTLastInShower() permits the last evolution pT to be read out. These extensions can be useful for matching studies.
      • New optional argument isInterleaved added to TimeShower::branch(...). Is false by default, but true when called from the parton level for interleaved evolution of several parton systems, optionally also with ISR and MPI.
      • New methods UserHooks::canSetResonanceScale() and UserHooks:scaleResonance(...) allows an optional user choice of the maximum shower scale in resonance decays.
      • A new method SpaceShower::doRestart() has been added, to help distinguish cases when a SpaceShower::branch(...) failure forces a complete restart of the evolution from ones where only the intended current branching has been vetoed.
      • When multiparton interactions are initialized, it is now possible to reduce both pT0 and pTmin if necessary to find a valid solution where sigma_jet > sigma_nondiffractive. Previously only the former would be reduced, which could lead to infinite loops if too large a pTmin was used. Thanks to Sami Kama for pointing out the problem.
      • The rescattering machinery is now essentially completed, and can be used also by others than the authors. For now, however, it can only be recommended for dedicated studies, not e.g. for generic tunes.
      • Timelike and spacelike showers, and beam remnant handling, are modified to handle rescattering partons. Specifically, a new machinery is introduced to trace the recoils from the combination of rescattering with showers and primordial kT. Can assign space- or timelike virtualities to intermediate particles to have energy and momentum conserved locally. This affects the PartonLevel, MultipartonInteractions, TimeShower, SpaceShower and BeamRemnants classes. Further details to appear in the upcoming article on rescattering. (Another change is a reversal to pre-8.114 order for non-interleaved FSR, wherein also FSR is treated before beam remnants are attached.)
      • Four new status codes introduced, as part of the rescattering description:
        45 : incoming rescattered parton, with changed kinematics owing to ISR in the mother system (cf. status 34);
        46 : incoming copy of recoiler when this is a rescattered parton (cf. status 42);
        54 : copy of a recoiler, when in the initial state of a different system from the radiator;
        55 : copy of a recoiler, when in the final state of a different system from the radiator.
      • New method Info::tooLowPTmin() can tell whether the pTmin scales for showers or multiparton interactions are too low.
      • Pion beams allowed, both pi^+, pi^- and pi^0. New machinery for the latter, where the valence flavour content is chosen to be either d dbar or u ubar for each new event. One internal pion PDF implemented, with others from LHAPDF.
      • Treatment of Pomeron-proton collisions begun.
      • Phase-space handling of hard processes and multiparton interactions slightly expanded to better allow for harder PDF's than proton ones, e.g. for Pomerons.
      • The program documentation has been expanded with an alphabetical index of all methods that are described on the webpages, see the Program Methods page. Also other sections of the documentation have been updated and expanded, including the worksheet.
      • Several list methods have been made const. For the listing of events two new methods have been added, Event::list() and Event::list(bool showScaleAndVertex, bool showMothersAndDaughters = false), that correspond to special cases of the general method.
      • A new method Pythia::LHAeventSkip(int nSkip) permits a skip-ahead of the reading of external Les Houches Events, without the necessity to generate the intervening nSkip events in full. Makes use of the new LHAup::skipEvent(int nSkip) method to perform the operations. Mainly intended for debug purposes.
      • The ClusterJet jet finder now saves the last five clustering scales. Also a minor bug fix. Thanks to Nils Lavesson for this contribution.
      • The Particle::m2() method now returns a negative number when the stored mass m is negative, as used to indicate spacelike virtualities. Also the Particle::eCalc(), Particle::mT() and Particle::mT2() methods have been modified.
      • The << method to print our a four-vector has been expanded with a fifth number, the invariant length, with a minus sign for spacelike vectors, and provided within brackets to allow a simple visual distinction.
      • New methods Rndm::dumpState(string fileName) and Rndm::readState(string fileName) allows to write or read the state of the random number generator to or from a binary file.
      • New method double GammaReal(double x) returns the value of the Gamma function for arbitrary real argument. Some cross sections for extra-dimensional processes rewritten to make use of it.
      • New example program main29.cc shows how to set up a fictitious process of a heavy system decaying to two particles or partons, with decays traced to stable particles, as relevant for astroparticle applications.
      • Main programs that illustrate the HepMC interface have been updated to use version 2.04, including units and excluding deprecated output formats.
      • The main32.cc example extended also to handle Les Houches Event Files.
      • The Makefile has been modified so that "make clean" only removes the current compilation and library files, while "make distclean" gives a more extensive reset and cleanup. Thanks to Nils Lavesson for this contribution. Some other minor Makefile corrections.
      • Several main programs that use the Main:timesToShow mode have been corrected so as not to crash if this is set to zero. Also some other cosmetics changes in main programs that do not affect the running.
      • Bug correction, in that previously a veto with user hooks was not propagated from parton showers inside resonance decays.
      • Minor bug fix in TimeShower for kinematics with unequal beam-particle masses.
      • Bug fix so that PartonLevel:MPI = off also works for minimum-bias events.
      • Minor bug fix in the impact-parameter selection of multiparton interactions. Thanks to Sami Kama for pointing it out.
      • String fragmentation for junction topology protected against numerical instability in boost.
      • Bug correction in the handling of particle decays to partons, where the scale of the partons was set before the partons had been added to some arrays, leading to indexation out of bounds. Thanks to Vladislav Burylov for discovering this bug.
      • Bug correction in the handling of particles with inhibited decay, where the decay vertex would be too far displaced, which could lead to infinite loop. Thanks to Sami Kama for debugging this.
      • Check to avoid infinite loop in matrix-element handling of two-body decays.
      • Bug correction to avoid infinite loops in Dalitz decay treatment. Some changes in the decay handling logic to allow a new try when the decay of a particle fails.
      • Minor correction, so the pointer to the Info class is set also for user-written classes derived from LHAup.
      • Correction for typo in the matrix element of the Sigma3ff2HchgchgfftWW class, for doubly charged Higgs production. Thanks to Merlin Kole for spotting it.
      • Updated colour bookkeeping in junction-antijunction annihilation avoids later problems in Pythia::check().
      • Minor updates of the Makefile.msc file to work with Visual Studio 2008. Thanks to David Bailey for these modifications.
      • Ensure that nInit in the BeamParticle class is set also for unresolved lepton beams.
      • The VetoEvolution class, derived from UserHooks, is obsolete and has been removed.
    • 8.130: 15 September 2009
      • New machinery that allows multiparton interactions inside diffractive systems. Also new optional Pomeron flux factors and Pomeron PDFs. New page on diffraction added, where further details are collected. Still not tuned, so to be used with caution.
      • Make Peter Skands' "Tune 1" parameters for ISR and MPI default. The older simpler tune is still available as an option, see Tune:pp.
      • New possible choices for a second hard process: charmonium, bottomonium, top pair and single top.
      • New code for pair production of generic colour-triplet scalar, fermion or vector. Largely written by Johan Bijnens, partly recycling existing code.
      • Add user hooks possibility to veto event after a given number of multiparton interactions.
      • Add instructions how PYTHIA 8 can be used from inside ROOT. Thanks to Andreas Morsch for providing the text and Rene Brun for a simple example.
      • The main21.cc example extended with an option for a single-particle gun.
      • Improvements and bug fixes in rescattering framework.
      • New method Hist::table(string fileName) provides a more direct way to print a two-column table of histogram contents into a file than the current Hist::table(ostream& os = cout).
      • Modify reading of external files so that a line only consisting of control characters counts as empty, the same way as a line only consisting of blanks already did. This includes carriage return, tabs and a few more, the ones represented by \n \t \v \b \r \f \a. Applies to Les Houches Event files, settings files and particle data files.
      • Fix it so that the read-in of a Les Houches Event File for the hardest process can be combined with the facility to select a specified second hard process.
      • New empty base class method LHAup::fileFound() allows the derived class LHAupLHEF to signal more clearly that a failed initialization is caused by a failure to open the desired file.
      • Check that a pointer to an LHAup object has been set in Pythia::LHAeventList() and Pythia::LHAeventSkip(...) calls.
      • Updated configure and Makefile, e.g. to build shared libraries on Mac OS X.
      • The options with a direct link to hard-process generation in PYTHIA 6 has been removed. It is hardly ever used but complicates the build structure. (Owing to its usefulness for some debug work, it was reinstated in a limited form in version 8.135. Thus main51.cc now contains the complete interface, previously in separate files, and commented-out lines in examples/Makefile suggest how PYTHIA 6 could be linked.)
      • New argument to Info::errorMsg(...) allows to show all error messages of a specific kind rather than only the first one, e.g. for initialization.
      • Correction in decay table of righthanded Majorana neutrinos. Thanks to Arnaud Ferrari and Vladimir Savinov.
      • Correction in expressions in the manual for H^+- couplings to an h^0, H^0 or A^0 and a W^+-. Thanks to Rikard Enberg.
      • Fix for accessing uninitialized memory, caused by accessing the daughters of the incoming beams before these daughters actually existed. Thanks to David Bailey and Sami Kama.
      • Uninitialized photon PDF inside the proton could give crazy results for processes with incoming photons. Thanks to Adam Davison.
      • Bug fix such that finite lifetimes can be set also for particles produced in the hard process. To exemplify, the bug affected tau leptons produced in Z^0 and W^+- decays. Thanks to Troels Petersen.
      • Bug fix in TimeShower, that beamOffset could remain uninitialized. Thanks to Sami Kama.
      • Minor correction to resonance decays: fail if the allowed mass range of a Breit-Wigner resonance is a small fraction of the total area under the resonance curve.
      • Correction when all three valence quarks were kicked out from a proton and could give false messages that beam momentum had been used up.
      • Clarify status codes needed for hadron-level standalone runs in order to avoid error messages, and modify the main21.cc example accordingly.
      • Minor corrections in the processes for extra dimensions.
      • Some other minor additions to existing facilities and minor bug fixes.
    • 8.135: 10 January 2010
      • All usage of static member methods inside Pythia8 has now been eliminated. This simplifies for you to have several simultaneous Pythia instances that are run with different conditions. The three main classes affected by this are the Settings and ParticleData databases and the Rndm random-number generator. You can no longer address the methods of these classes directly, but have to address them via the settings, particleData and rndm instances in the respective Pythia object. Also some other smaller pieces of code are affected, e.g. Standard Model and SUSY couplings (the latter in new files). Note 1: The documentation has been updated accordingly on these webpages, but the "A Brief Introduction to PYTHIA 8.1" still refers to the old behaviour of version 8.100. Note 2: the interface to the external LHAPDF library remains static, since LHAPDF is written in Fortran and thus by definition static. Note 3: if you want to have momentum smearing in CellJet you now need to send in a pointer to a random-number generator.
      • Ten new proton PDF sets are made available internally: MRST LO* (2007), MRST LO** (2008), MSTW 2008 LO (central member), MSTW 2008 NLO (central member), CTEQ6L, CTEQ6L1, CTEQ6.6 (NLO, central member), CT09MC1, CT09MC2, and CT09MCS, see PDF Selection. The Pomeron PDF data files have been renamed for consistency. Thanks to Tomas Kasemets for help with this Kas10.
      • New parameters TimeShower:pTmaxFudgeMPI and SpaceShower:pTmaxFudgeMPI introduced, to give the same functionality for multiparton interactions that TimeShower:pTmaxFudge and SpaceShower:pTmaxFudge do for the hardest.
      • A few extensions of the UserHooks framework. New methods UserHooks:canVetoISREmission() and UserHooks::doVetoISREmission(...) allows the latest initial-state emission to be studied before being finalized, with the possibility to veto it. Similarly Userhooks:canVetoFSREmission() and UserHooks::doVetoFSREmission(...) can be used to veto the latest final-state emission.
      • A number of loop counters have been introduced in the Info class, that offers some further information on the progress of the event generation, for use e.g. in conjunction with the UserHooks facility.
      • The Pythia::initTunes(...) method is made public, so that it can be called before the normal call from Pythia::init(...). That way it is possible to start out from a given tune and change a few of the parameters.
      • Bug corrected in LHAFortran.h for hard-process input from Fortran commonblock. This did not work properly when the input was used in combination with a second hard process generated internally. Thanks to Mikhail Kirsanov and Roberto Chierici.
      • Insertion of missing initialization of isInit in the Settings and ParticleData constructors, and nInit for BeamParticle. Thanks to Leif Lönnblad.
      • Updated Makefile.msc for Windows users.
      • Fix of some non-optimal use of booleans, that give warnings on a Windows compiler. Thanks to Anton Karneyeu.
      • New options for the SUSY Les Houches Accord such that, by default, particle and decay data are not overwritten for known Standard Model particles (including Z^0, W^+- and t, but excluding the Higgs).
      • Bug fix in SusyLesHouches, where the reading of SLHA information embedded in an LHEF would not stop at the end of the header section.
      • Bug correction for undefined secondary widths where decay products together are heavier than the mother. Also unit default secondary width values in the DecayChannel constructor.
      • Documentation updated, including change of current year to 2010.
    • 8.140: 16 July 2010
      • Four new draft tunes available.
      • Introduction of a new scenario for production of Hidden-Valley particles, and interleaved showering in the QCD and HV sectors, see the new Hidden Valleys description. A longer physics writeup is available Car10.
      • Implementation of 2 -> 3 phase space selection intended for QCD processes with massless partons. A new set of matching phase space cut parameters. The ten different QCD 2 -> 3 processes have been implemented making use of this new possibility, so far without a complete handling of possible colour flows, however.
      • New processes have been added for contact interactions in q q -> q q and q qbar -> q qbar scattering.
      • A process has been added for TeV^-1 Sized Extra Dimensions, which involves the electroweak KK gauge bosons, i.e. gamma_{KK}/Z_{KK}, in one TeV^-1 sized extra dimension; see main30.cc for an example. This scenario is described in Bel10. Thanks to Noam Hod and coworkers for contributing this code.
      • In the Randall-Sundrum extra-dimensional scenario a new option has been added where SM fields can exist in the bulk rather than only on a brane. (Still under development.) Furthermore production of a Kaluza-Klein gluon state has been added, and the main28.cc test program extended.
      • The scenario for monojets in Large Extra Dimensions has been expanded with an alternative for scalar graviton exchange instead of tensor one.
      • New parameters for maximum scale of timelike showers, TimeShower:pTmaxMatch, and the dampening of hard radiation, TimeShower:pTdampMatch and TimeShower:pTdampFudge, by analogy with corresponding ones for spacelike showers. Also new method TimeShower:limitPTmax(...) to implement alternative procedures. For dipoles stretched to the beam the new switch TimeShower:dampenBeamRecoil allows to dampen radiation close to the beam direction, with a changed default behaviour.
      • Azimuthal anisotropies from coherence arguments have been introduced for the spacelike parton showers, see SpaceShower:phiIntAsym and SpaceShower:strengthIntAsym. Also azimuthal anisotropies from gluon polarization have been introduced for the spacelike parton showers, see SpaceShower:phiPolAsym, and updated for timelike parton showers, see TimeShower:phiPolAsym.
      • Improvements for the matching to POWHEG LHEF-style input illustrated by the new main71.cc example. See also Cor10.
      • A set of new processes gamma gamma -> f fbar, with f quarks or leptons. Code for equivalent photon flux around an unresolved proton, with more to come. Thanks to Oystein Alvestad.
      • A new option has been included to dampen the growth of the diffractive cross sections, see Total Cross Sections.
      • A new method virtual int SigmaProcess::idSChannel() has been introduced. If overloaded to return a nonzero value then a 2 -> n process will appear listed as a 2 -> 1 -> n one. That is, an intermediate resonance with the requested identity will be inserted in the event record, even without appearing in the calculation of the matrix element proper. Thanks to Noam Hod for idea and code.
      • A new method SigmaProcess::convertM2() has been introduced to optionally allow the SigmaProcess::sigmaHat() to return the squared matrix element rather than d(sigmaHat)/d(tHat) for 2 -> 2 processes. Furthermore kinematics is stored in the new mME and pME vectors for alternative cross section encodings.
      • Different encoding of the f fbar -> Z W cross section, contributed by Merlin Kole, based on the cross section of Brown, Sahdev and Mikaelian. Gives a distinctly different cross section than the previous based on EHLQ (including their bug fix). In particular the problem with negative cross sections is now fixed.
      • Minor updates: pass xmlPath to new MSTW and CTEQ PDFs; reset beams earlier to give cleaner documentation.
      • The H1 Fit B LO parametrization to the Pomeron PDF has been included, and made new default for Pomerons. Thanks to Paul Newman for providing the data files.
      • Three changes, in principle unrelated, but with the common objective to make the generation of a given event depend only on the values determined during the initialization stage and on the state of the random-number generator when the event is begun. The new default should ensure a reproducible stop-and-restart behaviour, convenient for debug purposes. Thanks to Michael Schmelling for stressing the desire for such a behaviour.
        (i) Introduction of a new option PhaseSpace:increaseMaximum that allows to switch between two strategies for handling the (hopefully rare) cases when the assumed maximum of the cross section function is exceeded during the event generation, with a changed default behaviour. In the old default the maximum could be increased if it was exceeded during the run, thereby introducing a memory of the previously generated events.
        (ii) Updated handling of random numbers with Gaussian distributions. The gauss() method now only generates one value at a time. Instead the new gauss2() method returns a pair of Gauss numbers, with related time savings. In the old approach one Gaussian number could be buffered, which introduced a memory.
        (iii) Minor bug fix in MiniStringFragmentation, where the popcorn baryon state was not reset for each new system, again giving a (flawed) memory.
      • New directory rootexample with a simple code example how to use ROOT for histogramming in PYTHIA runs. See ROOT Usage for details. Thanks to Rene Brun.
      • In the HepMCinterface the checks for unhadronized quarks and gluons are not performed if hadronization has been switched off.
      • The UserHooks::initPtr(...) has been expanded so that pointers to more classes (beam particles, random number, couplings, etc.) are sent in, thereby increasing the scope of possible user-written code. Also, the UserHooks::doVetoProcessLevel(Event& process) now allows the process event record to be modified, even if it is not recommended. The new Info::pTnow() method returns the current pT scale of the combined MPI, ISR and FSR evolution, which can be useful for some user hooks decisions.
      • Histograms of the Hist class can now be booked with up to 1000 bins, instead of the previous maximum 100. All bins can be written to file, but the line-printer style printing will join nearby bins so at most 100 are printed, as before.
      • Updated configure and Makefile to allow 64-bit compilation and more options. Thanks to Mikhail Kirsanov, Rene Brun and Fons Rademakers.
      • Bug fix in ProcessLevel for colour flow checks of junctions. Enables the decay of a neutralino to three quarks, e.g. Thanks to Nils-Erik Bomark.
      • Bug fixes in TimeShower, where recoil partners in resonance decays of coloured particles, and recoil partners in QED dipoles when beams are not allowed to take a recoil, might not be correctly identified.
      • Bug fix in SpaceShower: when used with a fixed alpha_strong, the threshold enhancement factor of g -> Q Qbar became undefined. Thanks to Stefan Prestel.
      • Bug fix in initialization of resonance widths, where the minWidth parameter could be used uninitialized, occasionally resulting in strange initialization problems when kinematics needs to force at least one resonance to be off-shell.
      • Minor updates of main06.cc, main10.cc and main23.cc.
      • Bug fix in mother pointer of multiparton interactions in diffractive systems.
    • 8.142: 15 August 2010
      • The strategy for setting up tune values has been changed. Previously the Tune:ee and Tune:pp settings were only interpreted during the Pythia::init(...) stage. Now they are interpreted as soon as they are read. Specifically this means that it is possible to override any of the tune parameters by putting new commands below Tune:ee and Tune:pp in the Pythia::readFile(...) configuration file or in the list of Pythia::readString(...) commands.
        As a consequence of this change, the public Pythia::initTunes(...) method has been replaced by two private Settings::initTuneEE(...) and Settings::initTunePP(...) methods.
        If Tune:ee or Tune:pp are nonvanishing by default, then the corresponding tune variables are set also from the Pythia constructor, before any user changes are possible. Currently this is not relevant.
      • Bug fix in the setup of the Tune:pp = 5 and = 6 options, which meant that diffractive cross sections were not reduced as advertised.
      • The default value of MultipartonInteractions:pT0Ref has been slightly reduced so as to give a somewhat improved default description. It is not intended as a replacement for the specific tunes, however.
      • Some comparisons between tunes and data, obtained with the Rivet package, have been posted on http://home.thep.lu.se/~richard/pythia81/. Further improvements can be expected from future Professor-based tunes. The current set of 2C, 2M, 3C and 3M "draft tunes" have deliberately been chosen different also to explore a range of possibilities. One not visible in the plots is the fraction of single and double diffractive events in the inelastic cross section. This is 32% in 2C and 2M, while it was reduced to 21% in 3C and 3M, and a recent ATLAS study (ATLAS-CONF-2010-048) would suggest 28+-4%.
      • Minor changes in TimeShower and SpaceShower, as protection if the c or b masses are set small.
      • Bug fix in SpaceShower, for case when phi angle selection is biased to take into account interference effects.
      • The SigmaProcess::convertM2() method now has been implemented also for 2 -> 1 processes, so that it is possible to provide the squared matrix element instead of sigmaHat for semi-internal processes. A fixed-width Breit-Wigner is also inserted, since the matrix element is supposed not to include it.
      • New method SigmaProcess::setupForME() does an extended conversion from the internal kinematics to an almost equivalent one, better adapted to the mass conventions of matrix-element calculation programs, such as massive incoming b quarks. New flags allow to determine whether the c, b, mu and tau should be considered massless or not in the calculations.
      • Two new friend methods table of the Hist class allow to print a table with three columns, the first for the (common!) x values and the other two for the respective histogram values. A new method takeSqrt for the square root of histogram bin contents.
    • 8.145: 10 November 2010
      • Couplings is defined in StandardModel.h as a derived class of coupSM and has only one extra flag: isSUSY to check presence of extra couplings.Changed all pointers CoupSM* to Couplings* and removed explicit references to CoupSUSY*. The coupSUSY object is only initialised if SUSY couplings are present. The new pointer couplingsPtr points either to only SM couplings or SM+SUSY couplings based on SLHA data.
      • New files SusyResonanceWidths.h/cc contains the SusyResonanceWidths class, which inherits from ResonanceWidths but typecasts the couplingsPtr to (CoupSUSY*) coupSUSYPtr. This is the base class for all SUSY resonances. It contains the ResonanceSquark class for all squark decays. A new flag SLHA:useDecayTable to check if internal widths should be overwritten by those read in via SLHA.
      • Added new functionality to SusyLesHouches for read-in of generic user blocks in the SLHA format, along with methods to extract parameters from them with typecasting controlled by the user. Intended for use with user-written semi-internal processes.
      • Added Sigma1qq2antisquark cross section.
      • Some new flags and modes in the SUSY and SLHA series offer further functionality.
      • Several further changes as a consequence of the upgrade of the SUSY machinery.
      • Bug/typo fixes in rotation matrices for SUSY couplings and for the processes qqbar2squarkantisquark, qq2squarksquark and more.
      • Improved handling of colour junctions. Added new example program main72.cc, to illustrate read-in of color junction structures via LHEF (main72.lhe). The example used is SUSY with RPV.
      • New Tune 4C introduced as Tune:pp = 5. The more crude (non-)tunes 3C and 3M are removed.
      • New methods Settings::getFlagMap(...), Settings::getModeMap(...), Settings::getParmMap(...) and Settings::getWordMap(...) allows to return a map of all settings of the respective type that contain a specific string in its name.
      • Improved description of excited g^*/KK-gluon^* production in the Sigma1qqbar2KKgluonStar and ResonanceKKgluon classes.
      • Possibility added to let Hidden-Valley gamma_v have a nonzero mass and decay by mixing with the ordinary photon. Still experimental.
      • Minor bug fix in handling of three-body phase space.
      • Minor correction in Sigma2ffbar2TEVffbar class.
      • Bug fix for decays of W' to a pair of heavy fermions when gV != gA. Thanks to M. Chizhov, see arXiv:0705.3944.
      • Restore the older EHLQ-based encoding of the f fbar -> Z W cross section, which was changed in version 8.140, since comparisons with Madgraph gives much better agreement with it than with the expression of Brown, Sahdev and Mikaelian.
      • The HepMCInterface now also stores colour flow information for coloured particles.
      • Pointer to Couplings made available for particle decays.
      • Minor update in main61.cc for more elegant usage of FastJet, as suggested by Gregory Soyez.
    • 8.150: 20 April 2011
      • Tune 4C is made default. It is based on first comparisons with LHC data Cor10a, and has also been checked independently Buc11 to give reasonable agreement with many distributions.
      • The description of tau lepton decays has been significantly enhanced, to include helicity information related to the production process and hadronic currents fitted to data. A complete writeup is in preparation, while a summary can be found in Ilt12. A new flag is introduced to revert to the old behaviour, for cross-checks, see Particle Decays. The new tau decay machinery is on by default.
      • A new option MultipartonInteractions:bProfile = 4 has been introduced for the impact-parameter profile of protons in the Multiparton Interactions framework, wherein low-x partons are spread over a larger area than high-x ones, see Cor11. A new method Info::eMPI(i) gives back the enhancement factor related to the i'th interaction. The impact-parameter profile can now be selected separately for diffraction, but without a bProfile = 4 option.
      • The possibility of "hadronization" in the Hidden Valley sector has been added as a new option HiddenValley:fragment = on. This is based on a copy of the standard string fragmentation framework, but with the option of a completely separate "flavour" sector, and separately tunable longitudinal fragmentation functions and transverse momenta. For now only a simple flavour scenario is provided, where flavour-diagonal mesons can decay back into the normal visible sector while off-diagonal ones remain hidden. A writeup of the model is in preparation Car11. Also some further Hidden Valley options have been added.
      • Included possibility in TimeShower for QCD dipoles to have an adjustable normalization factor, via the new bool isFlexible and double flexFactor properties of class TimeDipoleEnd. This flexibility is used to treat radiation off colour topologies with epsilon tensors, in particular colour junctions which have all their partons in the final state. (An example is the BNV-SUSY decay ~chi0→uds.) For such topologies, the new treatment in PYTHIA 8 is that a half-strength dipole is spanned between all combinations of final-state quarks. For junctions with an incoming (anti)colour line (such as in the BNV-SUSY decay ~t*→cb), a full-strength dipole is instead spanned between the two daughters, with no radiation from the decaying object (in its CM). As will be described in a forthcoming paper with N. Desai, this should give the closest possible correspondence to the radiation patterns exhibited by higher-order matrix elements for this type of process.
      • Corrected harmless bugs in ProcessLevel::findJunctions which caused junctions of types 3 and 4 (i.e., junctions with 1 incoming color tag) to sometimes be incorrectly classified as types 1 and 2 (with all color tags outgoing), respectively. Since the parity (even/odd) of the junction kind was still correct, however, this did not cause any problems at the hadronization stage.
      • The junction-finder in ProcessLevel::findJunctions has been made more stable, and the following ordering of the color tags returned by Event::endColJunction(iJun, iLeg) is now enforced: for junction kinds 3 and 4 (one tag incoming), iLeg = 0 will return the incoming tag, while for kinds 5 and 6 (two tags incoming), iLeg = 0 and iLeg = 1 will return the incoming tags. Apart from this ordering, the color tags are ordered in ascending color tag number.
      • Declarations of friend functions moved to sit outside the class it befriends. Thanks to Axel Naumann for pointing out the incorrect previous construction.
      • The rootexample subdirectory becomes rootexamples as the old example is split into two, with improved documentation to clarify usage. Thanks to Axel Naumann and Bernhard Meirose for the new code.
      • In the Les Houches Event File machinery, input type has been changed from ifstream to istream for more flexibility.
      • R-hadron handling is largely implemented, see the R-hadrons page, although some aspects still need polishing. A new class RHadrons takes care of the hadronization and decay. Particle data have been added for R-hadrons containing a gluino, stop or sbottom, but could alternatively be used for other long-lived coloured particles. Thanks to Bernhard Meirose for support.
      • Calculations of SUSY decay widths included by N. Desai, contained in the new source files SusyResonanceWidth.cc and .h. Validation and addition of more modes is still in progress, so this implementation should be considered preliminary for now. For a list of available modes, see the SUSY Processes page.
      • A first implementation of the SLHA-based QNUMBERS interface for defining new exotic particles has been included. See Alw07 and the SUSY Les Houches Accord page.
      • Read-in of LHEF events containing Baryon Number Violating vertices has been included, using colour junctions, see the Event Record page. The advanced shower model taking into account the full colour structure of such events, developed by N. Desai and described above, is turned on by default in such events. Several test cases were used to validate this implementation, but it is possible that problems could still exist for some cases. Feedback is welcome. Thanks to the MadGraph authors for providing several test cases.
      • Some first steps taken to allow events containing colour sextets, e.g., from semi-internal processes or LHEF interfaces, and/or from SLHA DECAY tables. New colType codes 3 and -3 are introduced to describe sextets and antisextets, respectively. The state of the current implementation is that hard processes containing such states can be read in and decays generated (via DECAY tables). Parton showers can be added, but the sextets themselves do not, as yet, shower, and any undecayed sextets remaining at the hadronization stage would lead to unpredictable problems if hadronization is switched on. Thanks to J. Alwall for help with testing this implementation.
      • The functionality of the SLHA SUSY/BSM interface (see the SUSY Les Houches page) has been extended so that copies of all BLOCKs are now stored internally as strings, regardless of whether they correspond to "official" SLHA blocks or not. Their contents can subsequently be queried by a set of new templated member functions of the class SusyLesHouches. Available query functions so far include
        template <class T> bool getEntry(string, T&);,
        template <class T> bool getEntry(string, int, T&);,
        template <class T> bool getEntry(string, int, int, T&); , and
        template <class T> bool getEntry(string, int, int, int, T&);,
        where the type of the argument used in the call determines how to read the block entries. Thus, if an LHEF, SLHA, or other card file is read in by PYTHIA, the contents of any BLOCK in that file can subsequently be queried run-time using these functions. This is used, e.g., in the new interface between MADGRAPH 5 and PYTHIA 8. Thanks to the MADGRAPH team, and to J. Alwall in particular, for help and debug on this new implementation.
    • 8.153: 10 August 2011
      • The setup of tunes has been modified, see the Tunes page for details. Specifically the Tune:ee and Tune:pp modes have acquired a new option -1 for a forced restore to the default values of all settings used in the respective kind of tunes.
      • The code for handling multiparton interactions in the scenario with an x-dependent width of the Gaussian matter profile Cor11, has been improved and updated. Tune 4Cx, which is based on this option, has been added as a further tune option.
      • A possibility to bias the phase-space selection has been added, whereby some phase space regions can be oversampled, which is compensated by assigning a weight to each event. A new set of methods have been added to the UserHooks class to allow users to program how to bias the selection.
      • New options added so that matrix-element corrections can be switched off after the first branching in ISR or FSR.
      • Some new Info methods have been added to store information on latest ISR branching. The SpaceShower class has also been corrected so that the latest z = 1/2 when not defined by history. This avoids undefined values for azimuthal asymmetries. Thanks to Stefan Prestel for finding and sorting out this problem.
      • The Pythia::forceHadronLevel() method now takes an argument that optionally means that existing junction information is not overwritten. Thanks to Leif Lönnblad for pointing out the usefulness of this.
      • For particle decays to a varying number of hadrons the multiplicity increase with mass has been somewhat reduced, and especially for meMode = 23 a separate even slower increase has been introduced.
      • New possibility to force the tau polarization.
      • Bug fix for the special case in which events containing SUSY particles are generated without proper initialization of SUSY decays. This can happen, e.g., if events containing SUSY particles are read in via external LHEF files, if those files do not contain readable SLHA spectra in their headers. In this case, a failed attempt to generate sparticle decays with ill-defined couplings previously led to crashes. The program now reverts to the old behaviour, based on static decay tables, in such cases, with the default being to decay all sparticles to gravitino + particle. An error message stating that the full SUSY treatment has been switched off and why is also issued. Thanks to N. Desai for this fix.
      • The R-hadron machinery has been completed.
      • Minor change in timelike showers: gluons which fall below the pTmin cutoff by the correction for mass effects are now eliminated, while previously they were kept. This reduces the number of gluons somewhat, but has no significant effects on the hadronic final state. (Prompted by R-hadron studies, where big mass effects else give bothersome low-energy gluons.)
      • Corrected typos in two of the Upsilon wave function matrix elements, Bottomonium:OUpsilon3P08 and Bottomonium:Ochib03P01. Thanks to Beate Heinemann for pointing it out.
      • Implemented f* decay angle in f f -> f f* processes, and fixed some bugs for the same process. Thanks to Piyali Banerjee for tests.
      • Introduce possibility to separate production channels for TeV-sized extra dimensions, and a small code correction. Thanks to Noam Hod for code contribution.
      • Bug fix for neutrino beams: since neutrinos are always lefthanded there should be a factor 2 in the cross section, relative to charged leptons, from the non-need to average over incoming spin states. This is now fixed by introducing a new PDF class NeutrinoPoint for (unresolved) neutrinos, with normalization 2 rather than 1 for charged leptons. Thanks to Ryosuke Sato.
      • Bug fix for some (rarely used) particle settings, which could not be changed by users because they were read too early. Thanks to Andrew Altheimer and Gustaaf Brooijmans.
      • Bug fix in handling of tau decays, where setting of decay vertices could write outside memory. Thanks to Steven Schramm.
      • Minor expansion of the BeamParticle constructor.
      • Minor bug fix in CTEQ 6L for uninitialized variables.
      • Minor bug fix in fragmentation flavour combination to hadron.
      • Some updates of the documentation, including new pages on MadGraph 5 as a generator for semi-internal processes (thanks to Johan Alwall) and on RIVET interfacing.
      • Minor improvements of ROOT- and HepMC-related code and documentation.
      • Some cleanup of code.
    • 8.157: 10 November 2011
        Stefan Prestel joins as new member of the PYTHIA author team. He is mainly working on matching/merging issues, and has contributed the CKKW-L machinery mentioned below.
      • Merging capabilities according to the CKKW-L scheme Lon11 have been added, see the new Matrix Element Merging page. It involves new classes to reconstruct and select how a matrix-element-generated partonic configuration could have been obtained by the PYTHIA evolution, and to perform trial showers (using a new copy of the normal parton-level machinery) that introduce the appropriate Sudakov suppression factors. New examples to illustrate various common tasks are found in main81.cc, main82.cc, main83.cc and main84.cc.
      • The main71.cc program is now generalised for reading in arbitrary POWHEG LHE files, to implement a smooth matching between NLO matrix elements and the PYTHIA parton showers. Cuts are made on both ISR and FSR emissions, while previously only ISR was covered. The key assumptions are the pT definitions used for ISR and FSR, but several further options are available, as documented in the main71.cmnd file. Work is still ongoing to pick the best default options.
      • Several expansions of the UserHooks class. For both doVetoFSREmission and doVetoISREmission a new argument iSys labels the system within which the radiation occurs. For doVetoFSREmission a further argument inResonance distinguishes FSR in resonance decays from that in the hard process itself. New methods canVetoMPIEmission and doVetoMPIEmission have been added to veto multiparton interactions in the same way as FSR and ISR. In biasSelectionBy at times incorrect values for inEvent has been corrected. Also some systematization of the use of const.
      • A new model for hadron scattering is introduced, still at an early stage and therefore more intended for internal development than for the normal user. The basic idea is that a high-energy pp collision involves the fragmentation of multiparton strings that overlap in space (and time). Also the produced hadrons therefore initially overlap, and there is a strong likelihood that hadrons can scatter against each other until the system has expanded sufficiently. This can e.g. increase the transverse momentum of heavier hadrons at the expense of lighter ones.
      • A new jet finder SlowJet offers simple access to the inclusive kT, anti-kT, and Cambridge/Aachen algorithms in a cylindrical coordinate frame. The jet reconstruction is then based on sequential recombination with progressive removal, using the E recombination scheme. The minimalistic SlowJet code is much slower than FastJet Cac06, and contains less options, but reconstructs the same jets if run under identical conditions. For details see the Event Analysis page.
      • Starting in gcc 4.6, it is possible to switch off specific warnings around specific blocks of code. Although version 4.6 is some way off from being commonly found, this option has now been introduced to switch off -Wshadow warnings in HepMCInterface.cc. For other compilers, or earlier versions of gcc, the old behaviour is retained.
      • Support for reading in gzipped LHEFs has been added in the LesHouches and SusyLesHouches classes. This also affects configure and Makefiles. Unless explicitly enabled, it should not affect anything. If enabled, it relies on the Boost and zlib libraries to function, so paths to these must be set appropriately, see the README file for details. The Boost header files can give very many shadow warnings, so -Wshadow is disabled if gzip support is enabled, as described above.
      • Introduce use of the HEPMC_HAS_UNITS environment variable in the HepMCInterface.cc and main32.cc codes to automatically check whether GeV and mm can be set as relevant units. If yes, then it is set in main32.cc. If no, a conversion from GeV to MeV is done explicitly in HepMCInterface.cc. Note that, for early HepMC versions, this means a change of behaviour. Thanks to Andy Buckley.
      • A new method Info::lhaStrategy() returns the Les Houches event weighting strategy where relevant, and 0 where not. For the strategies +-4 the event weight and sum, Info::weight() and Info::weightSum(), is now in units of pb at output, as it should be at input. (While internally mb is used.)
      • New flag Check:abortIfVeto allows the user to resume control over execution in case of a veto in the event generation process.
      • New method Event::at(i) returns reference to i'th particle in the event record.
      • Introduce the Fermi constant as one of the Standard Model parameters.
      • Included automatic pre-initialization of SLHA blocks MASS and SMINPUTS using PYTHIA's SM parameters and particle data table values.
      • SUSY: added sleptons (and sneutrinos) as resonances. Corrected 2-body decay widths of gluinos, squarks and gauginos. Added sleptonic decay modes to gaugino decays. Implemented 2-body decays of sleptons (and sneutrinos) into sleptons/leptons/gauginos. Corrected slepton couplings (they now look exactly like squark couplings, using a 6x6 slepton mixing matrix).
      • New parameter Diffraction:probMaxPert introduce to give more flexibility in transition from a nonperturbative to a perturbative description of a diffractive system.
      • Bug corrected in SigmaEW.cc, for the process WeakSingleBoson:ffbar2ffbar(s:gm). Previously, all outgoing quark flavours in this process were erroneously assigned ID code 5 (b quarks). This has now been corrected so the proper ratios are obtained, with u : c : d : s : b = 4 : 4 : 1 : 1 : 1, according to the squared quark charges.
      • Changes in FragmentationSystems and StringFragmentation to reject systems with three or more interconnected junctions. This may happen in baryon-number-violating scenarios in pp collisions, if both of the beam baryon junctions are resolved and get connected via an antijunction created by a hard-process BNV vertex. In principle, this could be addressed by an extension of the existing junction fragmentation framework. However, since it happens rarely, for the time being an error message is printed and the fragmentation restarted.
      • Change in Event::copy to safeguard against attempting to copy out-of-range entries. An attempt to copy a non-existing entry will now return -1.
      • Bug fix in the machinery for the user to force the setting of tau polarization.
      • Bug fix in the initial search for a maximum of the process cross section (only affecting rare cases).
      • Corrected angular decay distributions for two compositeness processes, Sigma2qq2qStarq and Sigma2qqbar2lStarlbar.
      • Extra check in HiddenValleyFragmentation to make sure that pointers which have not been assigned with new are not deleted.
      • Some further minor changes.
    • 8.160: 23 January 2012
      • The older term "multiple interactions" has been replaced by the new standard "multiparton interactions" one, and correspondingly the abbreviation MI by MPI. This affects everything: settings, class and method names, documentation, etc. It therefore becomes necessary to rewrite user code. However, so as to keep the immediate effort at a reasonable level, the old settings names are kept as aliases. Thus PartonLevel:MI and PartonLevel:MPI are equivalent, and similarly MultipleInteractions:pT0Ref and MultipartonInteractions:pT0Ref. Should you be using methods such as double Info::pTMI(int i) you need to edit the code, however. All the example/main* files have been updated accordingly.
      • A new option Beams:frameType = 5 has been added for the case where an external generator should provide LHA process information. The new Pythia::setLHAupPtr(...) method should then be used to link in this generator. The new switch Beams:newLHEFsameInit can be used to tell that a new LHEF should be used, but without the need for a new initialization. With these two changes, all the different ways of initializing can be covered by the Pythia::init() call with no arguments. The various init(...)options with arguments are deprecated and will be removed for PYTHIA 8.2.
      • The Pythia::stat() method, with no arguments, replaces Pythia::statistics(...), although the latter remains as a deprecated alternative.
      • New settings Init:..., Next:..., and Stat:... can be used to steer some details of the operation of the Pythia::init(), Pythia::next() and Pythia::stat(), respectively. In particular it affects the amount of printout at the various stages of operation. See here for further details. This change involves several code changes, but in documentation rather than physics. Most of the Main:... settings are deprecated as a consequence.
      • The sample main programs in the examples subdirectory have been updated. This includes a change to the new favoured methods and settings outlined above, plus some update of the physics contents. Some of the examples have been combined, some others have been added (e.g. for R-hadrons), and as a consequence some renumbering has been made. See the modified list of sample main programs for the new status. In particular note that (the new) main61.cc allows streamlined input and output in HepMC, like main42.cc (previously main32.cc), but additionally links to LHAPDF.
      • The examples/configure script has new optional argument --with-pythia8. It can be used to set the new PYTHIA8LOCATION environment variable, which then is used in examples/Makefile to give the path to the PYTHIA library. Thereby it becomes possible to relocate (parts of) the examples directory and still obtain the correct path. Thanks to Mikhail Kirsanov.
      • Polarization information has been included as a new Particle property, that can be set by void pol(double polIn) and obtained by double pol(). Default value is 9., in agreement with the Les Houches standard. Event listings have been expanded to optionally display this information. Currently polarization is not used internally.
      • The matrix element merging machinery has been modified as follows.
        - Improved handling of the hard process, so that MadGraph5-produced LHE files do not produce problems (sometimes, the choices of MG4 on what to put into a LHEF have changed in MG5).
        - Improved handling of colour for easier handling of states with many quarks (the code has been tested for states with up to 5 q qbar pairs and some gluons).
        - Improved checking which clusterings are allowed. Now, clusterings should immediately be rejected if they lead to unphysical states, without the need to explicitly construct these states. This was needed to get t tbar production, VBF and some simple SUSY processes running with reasonable generality.
        - Improved handling of incomplete histories. Now there is an additional switch allowing code to try to swap some colours when fewer clusterings than requested have been found.
      • Updates in the handling of graviton resonances in scenarios with extra dimensions.
        - Now all G decays have correct angular distribution, which was not the case before for W/Z decays.
        - Added the possibility for G to only couple to longitudinal W/Z bosons, which affects both the width and angular distributions.
        - Added decays to Higgs pairs, G -> hh.
      • Bug fix in the findJunctions() function in ProcessLevel.cc. Changes introduced in version 8.145 (to allow for junctions in baryon-number-violating processes) did not correctly handle the remapping of color tags that can be applied when adding beam remnants to events with multiparton interactions. A simpler and more stable algorithm is now applied for the simplest cases, with the more complex one only invoked for cases such as BNV, which are normally considered before remnants are added, hence avoiding this particular problem. Also some other changes in the handling of junction, including a safeguard to reject systems with three or more interconnected junctions.
      • Bug fix and updates to the SLHA interface. Possibility of infinite loop during ProcessLevel::initSLHA corrected. Modifications to SusyLesHouches to allow interpretation of SLHA1 spectra with R-parity violation. Rather than reject spectra that do not conform fully to the SLHA2 standard for RPV, the interface will now first look for SLHA1 mixing matrices and attempt to translate those into SLHA2 ones if possible. In this case, warnings that the expected SLHA2 blocks were not found will be printed. It is up to the user to check that the derived SLHA2 information is correct. Corresponding additions to SusyCouplings.cc to extract mixing-matrix information from the relevant SLHA2 RPV blocks when RPV is switched on.
      • Updated SLHA example main24.cmnd to use new example spectrum, cmssm.spc, corresponding to CMSSM point 10.1.1, obtained with SOFTSUSY 3.3.0. Thanks to B. Allanach for providing the new spectrum file.
      • A new include/FastJet3.h header file simplifies interfacing of FastJet to Pythia. For details see documentation in the file itself. Thanks to Gavin Salam for this contribution.
      • The handling of diffraction has been made more flexible. Specifically the "total" Pomeron-proton cross section can now be made to depend on the mass of the diffractive system. This does not affect the diffractive cross section in pp collisions, which is set separately, but is used in the MPI machinery to affect the average number of interactions per Pomeron-proton collision. Furthermore, the allowed range for some parameters has been expanded. Thanks to Robert Ciesielski.
      • New method Pythia::forceTimeShower(...) can be used to generate a single final-state cascade from a set of partons, without any knowledge of prior history. This is mainly intended for toy studies. The meaning of the ProcessLevel:all switch has been modified so that this parton-level function is available, but not any others at this level.
      • ATLAS tune A2 now included. Thanks to Deepak Kar for providing it.
      • Change in the handling of recoils of timelike showers in resonance decays, in cases of coloured resonances such as t -> b W. In the first step the W always acts as recoiler to the b, but in subsequent step previously the W remained as recoiler to one dipole, while now all QCD-radiating partons recoil against another coloured parton. The old behaviour could give a (small) unphysical spike of radiation collinear with the colourless recoiler in the subsequent emissions (while the pattern of the first was and remains correct). The old behaviour can be recovered for checks, see TimeShower:recoilToColoured. Thanks to Yevgeny Kats for pointing out this issue (previously noted for Pythia 6 by several persons).
      • Bug fixes for rootexamples/Makefile and restoration of some deleted information in rootexamples/README. Thanks to Axel Naumann and Bernhard Meirose.
      • Bug fix, so that displaced vertices are possible in resonance decay chains. Thanks to Daniel Blackburn and Andy Buckley for pointing this out.
      • Bug fix for Info counter 2.
      • Bug fix so that sextet quarks now are read in correctly from Les Houches Event files; previously the (anti)colours were set to 0.
      • Year updated to 2012 in copyright statements etc.
      • Reformatting to reduce the number of code lines with more than 79 characters.
      • Pythia::initSLHA() moved from public to private.
      • Remove warning message when tau polarization is set by hand.
      • Several minor changes to reduce the number of warnings issued by the clang compiler. The origin of some warnings remains unclear so those remain to track down (could also be compiler bugs; note that we discuss warnings, not errors). Thanks to Randy MacLeod for bringing this up.
      • The worksheet has been updated to be in step with Pythia 8.160.
      • Several other minor corrections in the code and documentation.
    • 8.162: 12 March 2012
      • A new option allows for several partons to share the recoil in final-state radiation, seeTimelike Showers. It is mainly intended to be used in the context of matching to matrix elements, and so only to be used in the first few branchings.
      • Several new processes for LED dijet production, see Extra Dimensions.
      • Small update of the Sigma2ffbar2LEDllbar and Sigma2ffbar2LEDgammagamma LED processes.
      • New Sigma2QCffbar2llbar contact interaction process.
      • Inclusion of a new method in the matrix-element merging framework to influence the construction of histories, e.g. to already in the construction of histories disallow paths that fail the 2 -> 2 cuts.
      • Further minor updates of the matrix-element merging code, mainly for improved clarity.
      • Minor bug fix in the handling of beam and event information fed in from an LHAup instance.
      • Minor bug fix for potential crashes from uninitialized variables for the merging machinery when merging is not used.
      • Updated History class for matrix element merging, also avoiding some compiler warnings.
      • Bug fixes in the handling of correlated mass choices in resonance decays, such as H -> Z^*0 Z^*0.
      • Bug fix when the process-level execution is switched off, where Info::isResolved() could be called before its value was initialized. Thanks to Christian Pulvermacher for finding this.
      • Corrected matrix-element expression for mass selection in A^0 -> Z^*0 Z^*0 and A^0 -> W^*+ W^*-.
      • SM Higgs mass updated to 125 GeV and default width and branching ratios modified accordingly. Minor technical improvements of width calculation.
      • The usage of nested classes has been removed from SusyLesHouches, since it could give compilation errors on some platforms. The new class names begin with LH and all classes have been put inside the Pythia8 namespace.
      • Minor Makefile updates. Thanks to Mikhail Kirsanov.
      • Minor changes to avoid some clang compiler warnings on the Mac OS X platform.
    • 8.163: 27 March 2012
      • New methods in the Info class, id1pdf(), id2pdf(), x1pdf() and x2pdf(), to denote the partons for which parton distribution values have been defined. Previously this was assumed to agree with the incoming partons to the hard process, the same methods without the pdf qualifier. However, now the POWHEG approach offers a counterexample. Also the reading and handling of Les Houches (and other) events, and the interface to HepMC, has been modified accordingly.
      • The decay of Higgs and top resonances read in from Les Houches Event files is now performed with angular correlations as for internal processes. LHE files should normally contain all process-specific resonance decay chains and, if not, decays are made isotropic. The H -> WW/ZZ -> f fbar f' fbar' and t -> b W -> b f fbar correlations are process-independent, however, and thus can be handled internally. If part of the decay chain has already been set, e.g. H -> WW/Z> or t -> b W, then the subsequent decays are still isotropic.
      • Updated instructions how to link to HepMC, in README.HepMC.
      • Bug fix in the turn-on of resolved diffraction for low CM energies. Thanks to Erwin Visser.
      • Bug fix in the handling of string junctions at very high energies, caused by numerical errors. Thanks to Erwin Visser.
      • Some other small changes, mainly aesthetics.
    • 8.165: 8 May 2012
      • The MBR (Minimum Bias Rockefeller) model for single, double and central diffraction Cie12 is included as new option Diffraction:PomFlux = 5. It is specifically intended for p p and pbar p interactions, and is currently the only option that also supports central diffraction. Thus the basic machinery for Central Diffraction (a.k.a. Double Pomeron Exchange) has now been implemented. See examples/main04.cc for an example. Thanks to Robert Ciesielski for contributing the new code.
      • For a tau lepton in an external process, by default the SPINUP number in the Les Houches Accord now is interpreted as giving the tau helicity, and is used for its decay.
      • A tau coming from a W now defaults to being purely lefthanded when neither of the existing matrix elements apply.
      • Decay mode t -> H+ b included as an option.
      • Four ATLAS tunes have been implemented as options for Tune:pp: A2-minbias-mstw2008lo, AU2-cteq6l1, AU2-mstw2008lo, and AU2-ct10. The new flag Tune:preferLHAPDF can be used to switch between the LHAPDF and the internal implementation of a PDF set, in cases where both are available.
      • Reorder libraries in examples/Makefile, specifically move LIBGZIP so that it is properly linked when used. Thanks to Erik Schnetter.
      • Minor modification so that LHAPDF can be used for PDFs in the hard process, with one of the built-in PDFs for the rest, even if LHAPDF is compiled so as to handle only one concurrent PDF set.
      • Bug fix, that ParticleDecays:mixB = off did not switch off B0 - B0bar and Bs0 - Bs0bar mixing. Thanks to James Catmore.
      • Bug fix for the handling of gluon polarization of initial-state radiation, where an anisotropic azimuthal distribution was inadvertently generated in some 2 -> 1 processes. The update also includes always setting the second daughter zero for the two partons coming in to a hard 2 -> 1 process. Thanks to Antonio Policicchio.
      • Bug fix, that the setting of the number of user hooks MPI steps did not use UserHooks::canVetoMPIStep() properly.
      • Some other small changes, mainly documentation and aesthetics.
    • 8.170: 21 September 2012
      • Streamline default behaviour and options for choice of GeV or MeV for output to the HepMC event format, see HepMC Interface. Also set the mass of HepMC particles explicitly, rather than having it calculated implicitly. Thanks to James Monk and Andy Buckley.
      • The tau decay machinery has been further augmented with matrix elements and form factors for a variety of decay modes, such that all modes with a branching ratio above 0.1% are fully modeled. Several new classes and methods have been added to this end, Also, a tau pair coming from a Z^0 decay is now handled by assuming the Z^0 to be unpolarized when neither of the existing matrix elements apply. Taus coming from B baryons are handed as for B mesons.
      • Flavour violating decays have been added to the squark, gluino, neutralino and chargino decay tables.
      • Extend the UserHooks::subEvent(...) method so that it also works passably at the process level. Also new option for UserHooks::omitResonanceDecays(...).
      • New methods UserHooks::canVetoPartonLevelEarly() and UserHooks::doVetoPartonLevelEarly( const Event&) are intended to be used the same way as the existing ones without Early in their names, but allow veto right after the ISR + FSR + MPI evolution, before beam remnants are added and resonance decays are considered.
      • Central diffraction now available for all PomFlux options, not only the MBR model. This has been constructed by analogy with the respective assumptions made for single diffraction, but includes some arbitrariness. Therefore the cross section is left easily rescaleable and, for backwards compatibility with tunes that does not contain it, easily possible to switch off, see the relevant section.
      • Reading of ALPGEN parameter and event files has been added, see ALPGEN and MLM Merging.
      • MLM matching has been added, as a first step for ALPGEN events, see ALPGEN and MLM Merging.
      • The CKKW-L merging machinery has been upgraded in a number of respects.
        - More thorough treatment of pp>bb~e+e-veve~ with additional b-jets.
        - Corrected hard mu_r and mu_f choices for dijet and prompt photon.
        - More ways to define a hard process, e.g. with the LEPTONS and NEUTRINO tags. The merging will understand LHE files for mixed processes (e.g. W+ and W- production together).
        - More merging scale definitions.
        - More freedom to generate all possible histories.
        - Internal check (and cut) on Les Houches events in Pythia::mergeProcess if merging scale value of the events is below the value given to Pythia by setting Merging::TMS.
      • It now works to have R-parity violating decays of R-hadrons, i.e. baryon number violation in a vertex displaced from the primary one.
      • The documentation of diffractive processes by the Info methods has been expanded and corrected. This also include the list() method.
      • Particle masses and widths have been updated to agree with the 2012 RPP values Ber12. Thanks to Piotr Zyla for data file and James Catmore for program to update the PYTHIA tables from this input.
      • New methods jetAssignment and removeJet added to the SlowJet class.
      • Introduce angular correlation in decay chain H -> gamma Z0 -> gamma f fbar. Thanks to Tim Barklow and Michael Peskin.
      • Introduce simple way to bias the selection of 2 -> 2 processes towards larger pT values, with a compensatingly decreasing event weight, see Phase Space Cuts. Only offers a subset of the possibilities allowed by UserHooks, but simpler to use. The main08.cc program has been expanded to illustrate this possibility, and also expanded to include low-pT subsamples.
      • The two remaining non-NLO tunes from ATL12 are now included.
      • The Info methods nTried, nSelected, nAccepted, sigmaGen and SigmaErr now takes the code of an individual process as an optional argument.
      • It is now possible to generate resonance decays, followed by showers and hadronization, without having them associated with any specific process. This is part of an expanded Hadron-Level Standalone machinery, as before triggered by ProcessLevel = off, but additionally requiring Standalone:allowResDec = on. Input can either be directly into the event event record or via a (simplified) Les Houches Event File.
      • New configure script options --installdir, --prefix and --datadir can be used to set the location(s) to which the library, header and data directories will be copied by a make install subsequent to the make. Thanks to Mikhail Kirsanov.
      • Fix charge in antiparticle name when particle read in from SLHA file. Thanks to Johan Alwall.
      • Pointers now only compared with == and != (not e.g. > 0), to avoid warnings in gcc 4.7.
      • New check that version number of the code matches that of the XML files. If not, no events can be generated. Thanks to James Monk for suggestion.
      • New check that mother and daughter indices have been set to give a consistent event history. Can be switched on/off with the new Check:history flag.
      • A new method LHAup::newEventFile has been added to switch to reading in events from another LHE file without having to reinitialize the whole class. Lower-level routines like openFile and closeFile have been added to handle correct order of operations also when an intermediate gzip decompression step is involved.
      • LHAup::eventLHEF() can now be called with an optional argument false, to make event files somewhat smaller by reducing the amount of blanks.
      • A new mode Beams:nSkipLHEFatInit introduced to skip ahead the first few events in a Les Houches Event File (cf. the LHAup::skipEvent(nSkip) method).
      • Introduce a new pair of user hooks that can be used to reject the sequence of hard-process resonance decays, without rejecting the production of the primary resonances.
      • The possibility of separate multiplicative prefactors to the renormalization and factorization default pT^2 scale has been introduced for both timelike and spacelike showers.
      • Bug fixes in history information for R-hadron production, which also fixes HepMC conversion in this case.
      • Bug corrected in SigmaSusy.cc, for chargino+neutralino production. Indexing error for incoming quark states in the process Sigma2qqbar2charchi0, resulted in incorrect CKM factors.
      • Corrected a bug in SusyLesHouches.cc, for NMSSM spectra. The unitarity check on the neutralino mixing matrix was faulty, leading to erroneous messages about unitarity violations and SUSY being switched off.
      • Bug fixes in the handling of resolved and unresolved diffractive events. Thanks to Robert Ciesielski for debug.
      • Do not set up FSR dipoles for 2 -> 1 processes.
      • Check that some channel open for resonance decays. Also further check whether resonance decay treatment should be invoked.
      • Bug fix in reading of particle names from SLHA input.
      • Change mass, width and decay mode(s) of D*_s(10431). Thanks to Michal Petran.
      • Bug fix in leptoquark production (lepton sign in q g -> LQ l).
      • New argument added to SpaceShower::reassignBeamPtrs for diffractive event processing, as already available for TimeShower.
      • Do not write warnings in SpaceShower for weights above unity if the evolution scale is below 1 GeV^2.
      • Add default values for member variables in some constructors, and some related changes for AlphaStrong code.
      • Warn if negative-energy parton in hadronization.
      • The MPI pT values assumed in the beam remnant setting of primordial kT and colour reconnection probability were incorrect for diffractive events.
      • The arrays with MPI information were not reset when parton or hadron level fails and a new try is made. Only affected few events.
      • MPI statistics can not yet be accumulated for diffractive events, and therefore the relevant routine is no longer called.
      • Bug fix in the double parton scattering suppression from energy-momentum conservation.
      • Outgoing proton masses were not set in the event record for elastic scattering (but kinematics handling was correct).
      • Bug fixes in the identification and documentation of junctions, previously leading to some unnecessarily rejected events. Also other improvements leading to fewer errors.
      • Slightly increased values for FragmentationSystems:mJoin and StringFragmentation::FACSTOPMASS to reduce failure rate, without noticeably affecting event properties.
      • The Les Houches cross section error is now taken into account in the final Pythia error for strategies +-3. New methods LHAup::xSecSum() and LHAup::xErrSum() provide the necessary information.
      • When a tau pair comes from a massless photon, in dipole shower evolution, for the decay description the mother photon is reassigned to have the sum of the tau momenta.
      • Minor change in initialization sequence for user hooks, to allow for more flexibility.
      • Do not print warnings when multiparton interaction weights are only slightly above unity.
      • Do not write warnings for three known particles that are so close to threshold that widths are switched off to avoid trouble.
      • Some minor typographical changes.
    • 8.175: 18 February 2013
      • Richard Corke and Stefan Ask leave as active authors, and have new e-mail addresses.
      • Jesper Roy Christiansen and Philip Ilten join as new authors.
      • A severe bug found and corrected in the handling of junction fragmentation. For some string topologies it could lead to parts of partonic systems mainly aligned along the beam axis to obtain an effective tilt, thereby giving rise to a pair of opposing jets that should not be there. The bug was an unfortunate side consequence of the improvement of junction handling introduced in version 8.170, and do not affect versions prior to that. To the largest extent possible, it is recommended to avoid this version. Potential errors are likely to be most relevant for processes at low pT, whereas processes that already have a large scale proportionately are less affected. Sincere apologies, and thanks to Hannes Jung for discovering it.
      • The initialization is aborted when the user tries to change the value of a non-existing variable in the Settings or ParticleData databases, and it becomes impossible to generate events. This may be rather brutal, as opposed to the former policy of ignoring such commands (except for a warning), but avoids that the user wastes time on a run that is likely not to give the wanted results. Thanks to Gavin Salam for stressing this point.
      • Major updates of the merging code. CKKW-L code is made more flexible, and now includes additional options to facilitate merging of additional jets in MSSM processes. Unitarised ME+PS merging (UMEPS) is introduced as a new merging scheme for tree-level input. An example main program for UMEPS is added. UMEPS is documented in the new section UMEPS Merging. NLO merging methods are now functional. Two NLO merging schemes are implemented: NL3 and unitarised NLO+PS merging (UNLOPS), both of which are illustrated with example main programs. NLO merging is documented in NLO Merging.
      • The machinery for the MLM-style matching of jets has been expanded to cover input either from ALPGEN, as before, or from Madgraph (or other LHEF input), and expanded to cover either a matching algorithm based on the one in ALPGEN or the one in Madgraph. See Jet Matching for details.
      • Neutrons and antineutrons are now allowed as incoming beam particles. The neutron PDF is derived from the chosen proton PDF by simple isospin conjugation, and total/elastic/diffractive cross sections are assumed the same as for protons.
      • Update in Pythia.cc, to allow user to override SLHA mass values by hand, controlled by the new flag SLHA:allowUserOverride. This was motivated by people wanting to be able to read in a base SLHA spectrum and then quickly scan over particular mass values manually. Corresponding documentation update in SUSYLesHouchesAccord.xml.
      • Updates to the ResonanceWidths and SUSYResonanceWidths classes, to merge common initialization steps into the base class. Corresponding documentation update in SemiInternalResonances.xml. Also some cosmetic changes in SUSYResonanceWidths to improve conformity with CODINGSTYLE rules.
      • The SlowJet jet finder is updated with an option for an alternative R separation based on cosh(Delta y)-cos(Delta phi).
      • Statistics information on the separate subprocesses among the Les Houches external input is improved.
      • The sophisticated tau decay machinery has been expanded so that it can also handle production of taus in hypothetical lepton-number-violating processes, such as H0 -> tau+ mu-.
      • Branching ratios for most light hadrons, and the tau lepton, have been updated to agree with the 2012 Review of Particle Physics Ber12, by Anil Pratap Singh.
      • Photon radiation can now be included in leptonic two-body decays of hadrons by setting the new switch ParticleDecays:allowPhotonRadiation = on. The lower shower cutoff TimeShower:pTminChgL has been reduced so as to let the simulated photon spectrum extend to lower energies.
      • A new switch MultipartonInteractions:bSelScale has been introduced, to determine the relevant mass or pT scale of an event for the selection of impact parameter in the MPI framework. In spite of a changed default behaviour (the old being option 3), practical consequences are small for most processes.
      • The new UserHooks::retryPartonLevel() method can be overloaded, so that the same hard process is reused for a new try on the parton level, rather than being rejected completely. Thanks to Christian Bauer for suggestion.
      • A new method Event::undoDecay(int i) can be used to remove the daughters of a particle, and further descendents. Does not work for removing the daughters of a parton.
      • The interface to HepMC has been updated. In particular the support for old version has been removed, thereby allowing significant simplifications. The list of methods to set and get the behaviour of the conversion routine has also been updated. The set_event_scale method now stores the renormalization scale (rather than the pT stored previously). The examples main41, main42, main61, main62 and main84 have been updated accordingly.
      • Four new methods to interrogate the default values of the four different kinds of settings.
      • The Vec4 class has been expanded with methods to return true rapidity or pseudorapidity, and the R distance in (y, phi) or (eta, phi) cylindrical coordinates. Thanks to Andy Buckley.
      • The copy and = constructors of the Pythia class are made private so that compilers will block use of them. Thanks to Andy Buckley.
      • New option of the Pythia constructor, to omit the banner printout where necessary. Also new master switch Print:quiet to switch off most runtime program messages. Thanks to Andy Buckley.
      • Updates in the machinery that restores all affected values to their defaults before setting a new tune.
      • A new Vect class has been introduced for the Settings database. It can be used to store a vector of double-precision real values.
      • Three new groupings of existing QCD processes: SoftQCD:inelastic, HardQCD:hardccbar and HardQCD:hardbbbar.
      • New possibility to set the a and b parameters of the Lund fragmentation function separately for heavy flavour. Especially the b is expected to be universal, but Aurelien Martens and Eli Ben-Haim have found improved fits by relaxing this condition, so we formalize this possibility without recommeding it.
      • Method Pythia::getPDFPtr is made public so it can be used also outside the Pythia class to access PDF sets. Internally the PDF bookkeeping is modified to allow for the simultaneous handling of several PDF sets. Thanks to Mathias Ritzmann for providing code changes.
      • It is now possible to read the separate scale values of all outgoing particles, if this info is stored as a single line in an LHEF, begun by a single hashtag character. This is currently nonstandard and may evolve.
      • Some improvements to the install targets code in the Makefile and error detection in examples/configure. Thanks to Mikhail Kirsanov.
      • The CC and FC global environment variables can be set to specify the C++ and Fortran 77/90 compilers, otherwise set in configure and examples/configure. Thanks to Mikhail Kirsanov.
      • Check of shell choice in configure removed. Thanks to Andy Buckley.
      • Minor modifications in the Makefile and text for Root examples, relevant if shared libraries are used.
      • Previously the whole std namespace has been made available in PythiaStdlib.h. Now this behaviour has been replaced by the already-existing alternative, where only a part of std is made available, and only inside the Pythia8 namespace. Thus user code does not become reliant on the choices in PYTHIA. Some related smaller code rearrangements. Thanks to Andy Buckley.
      • When the "second hard" machinery is used to set two hard processes, the old behaviour for the SpaceShower:pTmaxMatch = 0 and TimeShower:pTmaxMatch = 0 options was to use the combined final state of the two processes to decide what pT_max scale to use. This could have unexpected consequences. Now each process is analyzed separately, and therefore has a separate scale. Also for MultipartonInteractions:pTmaxMatch = 0 the two interactions now are analyzed separately. It is then enough that one of them should limit pT_max of subsequent MPI's for such a restriction to be imposed. Thanks to Monika Jindal for discovering this bug.
      • The TimeShower:pTdampMatch option had no effect if switched on, since some code was missing. The manual description of it and the more relevant SpaceShower:pTdampMatch has been updated.
      • One minor bug fix and some corrections to make the code compile on Windows/VisualC++-2010. A simple error function parametrization has been added to PhaseSpace.h and SigmaTotal.h, to be uncommented in case erf(x) is not available by default. Thanks to Guy Barrand for providing the information.
      • Break a closed dependency loop between ParticleData.h and ResonanceWidths.h. Thanks to Andreas Schaelicke and Andy Buckley.
      • In the examples/mainXX.cc programs, class instances that have been created with a new are explicitly deleted at the end of the run. Useful if trying to track memory leaks.
      • Bug fix for R-parity violating decays of R-hadrons, to treat the special case of sequential resonance decays after the RPV one. Thanks to Mariangela Lisanti for pointing out this bug.
      • Changed the maximum allowed value for Tune:pp. Thanks to Yevgeny Kats.
      • Bug fix in the z-value weight for QED ISR emissions.
      • Some destructors moved for improved consistency.
      • Constants DEBUG renamed DBSUSY in the SusyCouplings and SusyResonanceWidths classes to avoid confusion. Thanks to Guy Barrand.
      • Many typos corrected and some other minor improvements of the online documentation.
      • The year has been updated to 2013 in files.
    • 8.176: 18 April 2013
      • Introduce weak shower, whereby W^+- and Z^0 gauge bosons can be produced interleaved with ordinary QCD and QED emissions. Currently only available for final-state radiation, and off by default, see Timelike Showers. A new status code 56 denotes W^+- and Z^0 gauge bosons produced by the FSR parton showers.
      • The gauge bosons produced by showers decay at the end of the parton-level step. New identity codes 93 for a Zcopy and 94 for a Wcopy can be used to set the decay modes of shower-produced gauge bosons separately from hard-process ones, but do not appear in event listings.
      • The Particle class has been updated with a pointer to the mother Event class, replacing the previous pointer to the ParticleData class. Thereby several old methods in the Event class can obtain new equivalents for the Particle one. That is, a call event.method(i) instead can be written event[i].method(). The duplicated methods are statusHepMC, iTopCopy, iBotCopy, iTopCopyId, iBotCopyId, motherList, daughterList, sisterList, isAncestor and undoDecay. Omitted is sisterListTopBot, while sisterList obtains an optional argument. A new method index is introduced. The now redundant Event class methods will be removed in PYTHIA version 8.2. Thanks to Andy Buckley for suggestion.
      • The initialization of SUSY couplings and particle data has been moved from the Pythia and ProcessLevel classes to a new dedicated SLHAinterface class.
      • Some SUSY 3-body decays have been implemented with Matrix Element weighting.
      • New method Info::scalup() returns the Les Houches SCALUP variable. This method is now used instead of QFac() in main31.cc, to set maximal scale for shower radiation in case that the event contains no POWHEG emission, and thereby sidesteps a potential bug when PDF information is provided in the Les Houches Event File. Also some default values have been changed in main31.cmnd. Thanks to James Monk.
      • New parameter LesHouches:mRecalculate can be used to prompt the recalculation of a particle mass from its four-momentum. This may be required for Les Houches input events where the nominal mass of the particle species is stored in the mass slot, rather than the actual mass of the current particle, as foreseen.
      • Extra checks that tracing of junctions in particular and partonic colour singlets in general are only performed when the event record contains coloured unhadronized partons. Thanks to James Catmore.
      • Minor correction related to GZIP support. Thanks to James Monk.
      • Recalculate the phase space of diffractive processes for each event when variable beam energies are allowed. Thanks to Oldrich Kepka for finding the bug.
      • Fix a bug whereby a gluon in diffractive systems would obtain a light-quark mass.
      • The Pythia::check() method can also check that each particle obeys E^2 - p^2 = m^2 (within numerical precision). Speed up the checks on mother-daughter history by streamlining the handling of simple cases.
    • 8.180: 22 September 2013
      • Nishita Desai joins as new author.
      • All the header files include/*.h have been moved to include/Pythia8/*.h to better comply with conventions in other libraries (* = generic name). Thus also all code lines #include "*.h" that refer to PYTHIA files have been changed to #include "Pythia8/*.h". Thanks to Andy Buckley for suggestion.
      • The class that converts PYTHIA events to the HepMC format is renamed from I_Pythia8 to Pythia8ToHepMC, the files where the class resides from HepMCInterface.h/.cc to Pythia8ToHepMC.h/.cc, and the subdirectory of the .cc file from hepmcinterface to pythia8tohepmc. This clarifies the role of the class and avoids potential future name clashes with other interfaces. Makefiles and example main runs have been modified accordingly. Thanks to Andy Buckley.
      • The configure/Makefile step has been extended such that a bin/pythia8-config script is constructed, to simplify subsequent linking of PYTHIA 8 and other libraries to your main program. See the README file for further instructions, the new "Compling programs against PYTHIA 8" section. Thanks to Andy Buckley for code and text.
      • The "minbias" event class has been renamed into the (inelastic) "nondiffractive" one, since the "minbias" denomination should be reserved for an experimental procedure. Needless to say, also the separation into diffraction or not could be made by experimental procedures, but here it is more generally accepted that there is an underlying theoretical description that takes precedence in cases of conflict. Thus the SoftQCD:minBias flag has been remaned SoftQCD:nonDiffractive, and the Info::isMinBias() method has been renamed Info::isNonDiffractive(). The old names have been retained as alternatives for now. Thanks to Andy Buckley.
      • Four PDF sets have been added from the NNPDF2.3 QCD+QED family: the central sets for LO with alpha_s(M_Z) = 0.130, LO with alpha_s(M_Z) = 0.119, NLO with alpha_s(M_Z) = 0.119, and NNLO with alpha_s(M_Z) = 0.119. Thanks to Juan Rojo and Stefano Carrazza for providing the code.
      • The fjcore version 3.0.5 code from FastJet has been included with the PYTHIA distribution. SlowJet now by default becomes a front end to fjcore, but the old behaviour is retained as an option. The new approach is faster, but the older one still offers a few extra possibilities. Note that the new useFJcore argument to the SlowJet constructor has been included as a new last-but-one argument, since the last one is likely to be used much more infrequently and logically depends on the value set for useFJcore. Thanks to Matteo Cacciari, Gavin Salam and Gregory Soyez for making the fjcore code freely distributable.
      • New method constituents(i) in FastJet returns a vector with the indices of the particles belonging to the i'th jet.
      • The global recoil option for final-state showers has been extended with a few more options to improve possibility for matching to output from other programs, such as aMC@NLO.
      • Further extensions of the weak-showering machinery, but still experimental. Now also includes W/Z emission in the initial state.
      • Introduce new qqbar option for SigmaProcess::inFlux() and update documentation.
      • Improve the description of meMode for resonances and illustrate how to force specific Higgs branching ratios in main16.cmnd.
      • Added two previously missing SUSY processes for associated production of a gluino with a neutralino or chargino: SUSY:qqbar2chi0gluino and SUSY:qqbar2chi+-gluino, using the cross section expressions in Fuk11. Validated against PYTHIA 6 and XSUSY.
      • Added direct slepton production from q qbar annihilation, SUSY:qqbar2sleptonantislepton. Validated against PYTHIA 6.
      • Corrected some slepton and squark EW couplings in SusyCouplings.
      • Generalized the cross section formulae for SUSY:qg2squarkgluino to the case of non-minimal flavor violation, using the expressions in Fuk11. Validated against PYTHIA 6 and XSUSY. The new implementation is compatible with both SLHA2 and SLHA1, whereas the older was only compatible with SLHA1.
      • Generalized the cross section formulae for SUSY:qqbar2gluinogluino to the case of non-minimal flavour violation, using the expressions in Fuk11. (Also corrected a factor 2 in that paper on the color factor for st and su interference terms.) The new implementation is compatible with both SLHA2 and SLHA1, whereas the older was only compatible with SLHA1.
      • Changed the default meMode for SLHA DECAY modes to 100, to allow off-shell decays. Enabled the user to choose a different meMode if desired, via a new mode, SLHA:meMode. If values different from 100 are selected (e.g., 103), modes that are extremely far off shell (defined as needing a fluctuation of more than 100 times the root-sum-square of the widths of the mother and daughter particles) will still default back to 100, though the user may of course still switch them off if so desired. Added documentation about this in SusyLesHouchesAccord.xml. Deleted the parameter SLHA:minDecayDeltaM, which would prevent the possibility of off-shell decays unless set to a large negative value.
      • Added calculation of decay lengths to SLHA DECAY modes.
      • Updated documentation of SUSY processes and SLHA-related parameters. Additional reference to the new cross sections included in the bibliography.
      • Allow six-flavour running of alpha_s above the top threshold, and implement option with CMW rescaling of the Lambda values, for use in coherent showers.
      • The merging code has been updated, with corrected handling of massive partons. This amends problems in tt̄, and makes clusterings of massive emissions W, Z, ~g possible. The bookkeeping for the hard process has been upgraded to accommodate more general BSM processes. The treatment of incomplete histories has been upgraded, so that histories which allow for at least one clustering will be used in the unitarisation. Also, states that do not allow for any clustering will not be subject to the (internal, optional) cut on the input events any longer, to guarantee full phase space coverage. This is important for processes for which a non-negligible fraction of states lead to incomplete histories, e.g. tt̄W production. Further, functionality for reclustering FSR off SUSY particles has been added. A new setting allows more easily to switch between 4-flavour and 5-flavour merging schemes.
      • The main85.cc - main88.cc have obtained support for zipped LHE input files, and have nicer printing of the inclusive cross section at the end.
      • Introduced new mode LesHouches:setLifetime so that the lifetime information in Les Houches input can be replaced by the standard PYTHIA selection procedure. By default this is applied to tau leptons, since some matrix-element generators do not set this lifetime. Thanks to James Monk and Thorsten Kuhl.
      • A new examples/main46.cc illustrates how to write a ProMC file with PYTHIA events. Thanks to Sergei Chekanov.
      • The Vect class has been renamed PVec and a new MVec class has been introduced along the same lines, see the Settings database. They can be used to store a vector of double-precision real or integer values, respectively, i.e. of parms or modes, hence the names. Thanks to Abram Krislock.
      • Two new vectors of integers SUSY:idVecA and SUSY:idVecB have been introduced to allow a more flexible selection of final states in SUSY processes, see the SUSY process selection page. The selection machinery has been expanded to cope. Thanks to Abram Krislock.
      • New switch PartonLevel:earlyResDec to give first simple option where resonances are allowed ro decay before colour reconnection and beam remnants are added.
      • Renamed the mass(...) methods to mSel(...) in the Particle, ParticleData and ParticleDataEntry classes, to avoid users mistaking Particle::mass() for Particle::m().
      • Fixed a missing (unused) argument in some derived classes when the mRecalculate parameter was introduced in Les Houches code in version 8.176.
      • Removed several unused class variables from header files, based on new compiler information.
      • Fixed a bug in Sigma2ffbar2HposHneg, where int(...) was used instead of abs.(...). Thanks to Vittorio Zecca.
      • Fixed missing re-initialization of Breit-Wigner mass generation parameters for externally set new resonance widths. Thanks to Vittorio Zecca.
      • Fixed several places where division by zero or adressing of arrays out-of-bounds could occur. While some were trivial, others revealed underlying errors, notably in the handling of some SUSY processes and resonances. New checks against unphysical SLHA input have been implemented. Also some bug fixes in the new weak-shower ISR component, the sphericity analysis, the event undo-decay option, and more. Thanks to Vittorio Zecca.
      • Bug fix in the tau decay description for decay chains like H0 -> A0 A0 -> 4 tau, caused by an erroneous assignment of the number of spin states. Thanks to Brock Tweedie.
      • Add setting of some TimeShower variables that might remain uninitialized. Thanks to Christian Pulvermacher.
      • Extra check in TimeShower for incoming massive particles, where a recalculation of kinematics to an equivalent massless case could give a slightly negative effective dipole mass (with endpoint masses subtracted). Thanks to Paolo Torrielli.
      • Updated manual on how to implement new showers, mainly detailing new optional method arguments. Thanks to Mathias Ritzmann.
      • Corrected bug in SigmaSUSY which caused flavour violating slepton production (for R-parity conserving cases too).
      • Corrected bug in SusyCouplings where tan(beta) was not read from LHA file for RPV spectrum.
      • Modified the contact interaction term normalization of the f fbar -> l lbar process to agree with the one used in PYTHIA 6. Documentation of the ContactInteractions:Lambda updated to reflect this. Thanks to Daniel Hayden.
      • Introduced copy constroctor for the Event class.
      • Reset the Higgs mass range when its mass is changed in examples/main14.cc.
      • Remove obsolete examples/main91.cc and associated Makefile code.
      • Catch cases where junction topologies are sent to the ministring machinery, which is not set up to handle it, and therefore could give segmentation faults. Very rare.
    pythia8-8.1.80.orig/xmldoc/mstw2008nlo.00.dat0000444000175000017500000120437112217346305016555 0ustar sunsun # Mon Nov 10 16:35:59 2008 # MSTW 2008 NLO PDF grid for central fit. # distance(t),tolerance(T) = 0. 0. # mCharm = 1.40 # mBottom = 4.75 # alphaS(1GeV) = 0.49128 # alphaS(MZ) = 0.12018 # alphaSorder,alphaSnfmax = 1, 5 # nExtraFlavours = 0 xg xd xu xs xc xb xdv xuv xsv -1.0407E+01 1.3098E+00 1.3144E+00 4.6749E-01 0.0000E+00 0.0000E+00 7.5402E-06 4.6422E-03 -7.3203E-04 -1.0583E+01 1.2372E+00 1.2419E+00 4.0558E-01 0.0000E+00 0.0000E+00 1.5377E-05 4.7693E-03 -7.4388E-04 -1.0365E+01 1.2000E+00 1.2048E+00 3.7621E-01 0.0000E+00 0.0000E+00 2.1813E-05 4.8647E-03 -7.5265E-04 -9.3612E+00 1.1792E+00 1.1842E+00 3.6560E-01 0.0000E+00 0.0000E+00 3.1249E-05 4.9930E-03 -7.6430E-04 -9.3612E+00 1.1792E+00 1.1842E+00 3.6560E-01 2.8558E-08 0.0000E+00 3.1249E-05 4.9930E-03 -7.6430E-04 -7.7197E+00 1.1931E+00 1.1982E+00 3.8757E-01 2.3542E-02 0.0000E+00 3.9946E-05 5.0995E-03 -7.7380E-04 -5.3103E+00 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5.4482E-08 1.4648E-08 1.6780E-05 2.8223E-17 2.9651E-06 1.1288E-07 1.4395E-05 1.0057E-07 9.9162E-08 6.6394E-08 1.2308E-08 1.4295E-05 2.3450E-17 2.9651E-06 1.2118E-07 1.2427E-05 1.1070E-07 1.0922E-07 7.7549E-08 1.0471E-08 1.2316E-05 1.9744E-17 2.9651E-06 1.3040E-07 1.0851E-05 1.2138E-07 1.1985E-07 8.9335E-08 9.0167E-09 1.0729E-05 1.6841E-17 2.9679E-06 1.4412E-07 9.4968E-06 1.3634E-07 1.3480E-07 1.0551E-07 7.7775E-09 9.3604E-06 1.4393E-17 2.9676E-06 1.6028E-07 8.3535E-06 1.5354E-07 1.5200E-07 1.2397E-07 6.7393E-09 8.2000E-06 1.2360E-17 2.9676E-06 1.7711E-07 7.4171E-06 1.7121E-07 1.6970E-07 1.4289E-07 5.8954E-09 7.2458E-06 1.0723E-17 2.9676E-06 1.9363E-07 6.6405E-06 1.8843E-07 1.8695E-07 1.6129E-07 5.2004E-09 6.4521E-06 9.3860E-18 2.9676E-06 2.1565E-07 5.9616E-06 2.1106E-07 2.0961E-07 1.8511E-07 4.5925E-09 5.7506E-06 8.2264E-18 2.9676E-06 2.8758E-07 5.4218E-06 2.8351E-07 2.8211E-07 2.5873E-07 4.0669E-09 5.1382E-06 7.2320E-18 2.9676E-06 3.6867E-07 4.9849E-06 3.6504E-07 3.6368E-07 3.4136E-07 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1.8876E-06 2.3099E-18 2.8946E-06 8.2620E-07 2.5709E-06 8.2493E-07 8.2403E-07 8.1033E-07 1.2728E-09 1.7460E-06 2.1144E-18 2.8946E-06 8.4714E-07 2.4658E-06 8.4597E-07 8.4510E-07 8.3196E-07 1.1743E-09 1.6198E-06 1.9420E-18 2.8946E-06 8.6549E-07 2.3737E-06 8.6440E-07 8.6357E-07 8.5094E-07 1.0886E-09 1.5093E-06 1.7927E-18 2.8946E-06 8.8289E-07 2.2864E-06 8.8188E-07 8.8108E-07 8.6896E-07 1.0077E-09 1.4045E-06 1.6523E-18 3.3700E-05 1.1682E-08 5.7401E-05 2.2764E-16 0.0000E+00 0.0000E+00 1.1682E-08 5.7401E-05 1.0164E-18 1.8489E-05 5.8535E-09 4.3340E-05 -2.7700E-09 0.0000E+00 0.0000E+00 8.6235E-09 4.3343E-05 7.4539E-19 1.1832E-05 4.1901E-09 3.5199E-05 -2.6997E-09 0.0000E+00 0.0000E+00 6.8897E-09 3.5202E-05 5.8953E-19 6.5298E-06 4.7220E-09 2.6688E-05 -3.9068E-10 0.0000E+00 0.0000E+00 5.1127E-09 2.6688E-05 4.3368E-19 6.5298E-06 4.7220E-09 2.6688E-05 -3.9067E-10 -9.6563E-16 0.0000E+00 5.1127E-09 2.6688E-05 4.3368E-19 4.0635E-06 7.1412E-09 2.1359E-05 3.1180E-09 1.9752E-10 0.0000E+00 4.0232E-09 2.1356E-05 3.3712E-19 2.7224E-06 1.0634E-08 1.7326E-05 7.4213E-09 1.8421E-09 0.0000E+00 3.2125E-09 1.7319E-05 2.6936E-19 2.2849E-06 1.3741E-08 1.4522E-05 1.1084E-08 3.6842E-09 0.0000E+00 2.6573E-09 1.4511E-05 2.2192E-19 2.2080E-06 1.4117E-08 1.2296E-05 1.1894E-08 3.1582E-09 0.0000E+00 2.2230E-09 1.2285E-05 1.8381E-19 2.1622E-06 1.9392E-08 1.0345E-05 1.7546E-08 7.7925E-09 0.0000E+00 1.8462E-09 1.0328E-05 1.5416E-19 2.1602E-06 2.7590E-08 8.9283E-06 2.6015E-08 1.5668E-08 0.0000E+00 1.5750E-09 8.9023E-06 1.2960E-19 2.1602E-06 3.7524E-08 7.7695E-06 3.6169E-08 2.5475E-08 0.0000E+00 1.3551E-09 7.7333E-06 1.1011E-19 2.1602E-06 4.6204E-08 6.9707E-06 4.4999E-08 3.4159E-08 0.0000E+00 1.2046E-09 6.9257E-06 9.7832E-20 2.1602E-06 1.2393E-07 4.9912E-06 1.2311E-07 1.1240E-07 0.0000E+00 8.2706E-10 4.8680E-06 6.6069E-20 2.1602E-06 1.2393E-07 4.9912E-06 1.2311E-07 1.1240E-07 1.5684E-14 8.2706E-10 4.8680E-06 6.6069E-20 2.1602E-06 1.7287E-07 4.7014E-06 1.7211E-07 1.6152E-07 4.7038E-08 7.6593E-10 4.5293E-06 6.0986E-20 2.1602E-06 2.9270E-07 3.9598E-06 2.9209E-07 2.8197E-07 1.5763E-07 6.1186E-10 3.6677E-06 4.8281E-20 2.1602E-06 3.9223E-07 3.3482E-06 3.9174E-07 3.8224E-07 2.5569E-07 4.8653E-10 2.9564E-06 3.8116E-20 2.1602E-06 4.6488E-07 2.9038E-06 4.6448E-07 4.5562E-07 3.3156E-07 3.9666E-10 2.4393E-06 3.0917E-20 2.1602E-06 5.2602E-07 2.5407E-06 5.2570E-07 5.1750E-07 3.9871E-07 3.2387E-10 2.0150E-06 2.4987E-20 2.1602E-06 5.7251E-07 2.2953E-06 5.7223E-07 5.6459E-07 4.5147E-07 2.7434E-10 1.7230E-06 2.1176E-20 2.1602E-06 6.2138E-07 2.0506E-06 6.2115E-07 6.1417E-07 5.0884E-07 2.2509E-10 1.4294E-06 1.7364E-20 2.1602E-06 6.5724E-07 1.8711E-06 6.5705E-07 6.5063E-07 5.5256E-07 1.8936E-10 1.2141E-06 1.4400E-20 2.1602E-06 6.8507E-07 1.7318E-06 6.8491E-07 6.7899E-07 5.8766E-07 1.6190E-10 1.0469E-06 1.2282E-20 2.1602E-06 7.1455E-07 1.5843E-06 7.1442E-07 7.0908E-07 6.2614E-07 1.3312E-10 8.6991E-07 1.0164E-20 2.1602E-06 7.3745E-07 1.4697E-06 7.3734E-07 7.3252E-07 6.5715E-07 1.1100E-10 7.3239E-07 8.2586E-21 2.1602E-06 7.5541E-07 1.3799E-06 7.5532E-07 7.5095E-07 6.8228E-07 9.3822E-11 6.2455E-07 6.9880E-21 2.1602E-06 7.7057E-07 1.3040E-06 7.7049E-07 7.6653E-07 7.0416E-07 7.9461E-11 5.3353E-07 5.9292E-21 2.1602E-06 7.8316E-07 1.2410E-06 7.8309E-07 7.7950E-07 7.2286E-07 6.7646E-11 4.5796E-07 4.8704E-21 2.1602E-06 7.9329E-07 1.1903E-06 7.9324E-07 7.8997E-07 7.3835E-07 5.8212E-11 3.9709E-07 4.2352E-21 2.1602E-06 8.0158E-07 1.1489E-06 8.0153E-07 7.9854E-07 7.5131E-07 5.0563E-11 3.4736E-07 3.5999E-21 2.1602E-06 8.0876E-07 1.1129E-06 8.0872E-07 8.0599E-07 7.6284E-07 4.3980E-11 3.0422E-07 3.1764E-21 2.1602E-06 8.1492E-07 1.0821E-06 8.1488E-07 8.1239E-07 7.7295E-07 3.8373E-11 2.6722E-07 2.7529E-21 2.1602E-06 8.2005E-07 1.0564E-06 8.2002E-07 8.1773E-07 7.8155E-07 3.3737E-11 2.3642E-07 2.5411E-21 2.1602E-06 8.2433E-07 1.0350E-06 8.2430E-07 8.2219E-07 7.8887E-07 2.9899E-11 2.1074E-07 2.1176E-21 2.1602E-06 8.2815E-07 1.0159E-06 8.2812E-07 8.2618E-07 7.9553E-07 2.6492E-11 1.8781E-07 1.9058E-21 2.1602E-06 8.3149E-07 9.9922E-07 8.3146E-07 8.2968E-07 8.0146E-07 2.3531E-11 1.6776E-07 1.6941E-21 2.1602E-06 8.3432E-07 9.8504E-07 8.3430E-07 8.3265E-07 8.0658E-07 2.1034E-11 1.5075E-07 1.4823E-21 2.1602E-06 8.3673E-07 9.7299E-07 8.3671E-07 8.3518E-07 8.1100E-07 1.8922E-11 1.3628E-07 1.4823E-21 2.1602E-06 8.3789E-07 9.6098E-07 8.3787E-07 8.3645E-07 8.1406E-07 1.7010E-11 1.2311E-07 1.2705E-21 2.1602E-06 8.3994E-07 9.5129E-07 8.3993E-07 8.3861E-07 8.1786E-07 1.5313E-11 1.1136E-07 1.0588E-21 2.1602E-06 8.4163E-07 9.4288E-07 8.4162E-07 8.4039E-07 8.2110E-07 1.3861E-11 1.0126E-07 1.0588E-21 2.1602E-06 8.4308E-07 9.3561E-07 8.4307E-07 8.4192E-07 8.2393E-07 1.2613E-11 9.2541E-08 8.4703E-22 2.1602E-06 8.4443E-07 9.2888E-07 8.4442E-07 8.4335E-07 8.2659E-07 1.1463E-11 8.4466E-08 8.4703E-22 2.1602E-06 8.4563E-07 9.2285E-07 8.4562E-07 8.4462E-07 8.2900E-07 1.0438E-11 7.7233E-08 8.4703E-22 2.1602E-06 8.4669E-07 9.1754E-07 8.4668E-07 8.4575E-07 8.3115E-07 9.5383E-12 7.0859E-08 6.3527E-22 2.1602E-06 8.4761E-07 9.1294E-07 8.4760E-07 8.4673E-07 8.3303E-07 8.7630E-12 6.5341E-08 6.3527E-22 2.1602E-06 8.4848E-07 9.0863E-07 8.4847E-07 8.4765E-07 8.3482E-07 8.0376E-12 6.0160E-08 6.3527E-22 pythia8-8.1.80.orig/xmldoc/RandomNumberSeed.xml0000444000175000017500000000231012217346317017533 0ustar sunsun

    Random-Number Seed

    The seed of the random number generator can be set as follows: Indicates whether a user-set seed should be used every time the Pythia::init routine is called. If off, the random number generator is initialized with its default seed at the beginning of the run, and never again. If on, each new Pythia::init call (should several be made in the same run) results in the random number being re-initialized, thereby possibly starting over with the same sequence, if you do not watch out. The seed to be used, if setSeed is on.
    A negative value gives the default seed,
    a value 0 gives a random seed based on the time, and
    a value between 1 and 900,000,000 a unique different random number sequence.

    For more on random numbers see here. This includes methods to save and restore the state of the generator, and some preprogrammed methods to generate non-uniform random numbers. pythia8-8.1.80.orig/xmldoc/ROOTusage.xml0000444000175000017500000002244512217346317016164 0ustar sunsun

    ROOT usage

    Many PYTHIA users wish to use ROOT to produce histograms, or even to run PYTHIA as a plugin to ROOT. This is possible. It is not a task supported by the PYTHIA team, however. All issues involving ROOT usage should be directed to the ROOT team, or to the local support team of your collaboration. Below some helpful hints have been collected. The text is based on contributions by Rene Brun, Andreas Morsch and Axel Naumann. Another example may be found in the VINCIA add-on program for parton showers, but this should also work for a PYTHIA standalone run.

    Note that in all that follows, a Linux-type system with a Bash shell and GNU Make is assumed. In particular, for Mac OS X, the LD_LIBRARY_PATH should be replaced with DYLD_LIBRARY_PATH and the extension for shared libraries .so should be replaced with .dylib.


    Standalone usage

    One can perform the generation and analysis of events in a completely standalone fashion, and only use ROOT to process the completed events. Some example programs are provided in the rootexamples directory, with details provided below and in the README file. The examples assume that you have already compiled the PYTHIA library, ROOT is installed, and that all paths have been setup correctly (e.g. PATH and LD_LIBRARY_PATH). If these paths are not already set, ROOT typically comes with a shell script to set these paths, which can be run with
        source /path_to_ROOT_installation/bin/thisroot.sh
    

    Histogramming with ROOT

    An example of histogramming with ROOT is provided in rootexamples/hist.cc. It may be compiled and run with the following commands
        make hist
        ./hist.exe
    
    After PYTHIA has run, a ROOT histogram of the charged multiplicity in the events will be shown. This is now stored in the hist.root file.

    Storing PYTHIA events in ROOT trees

    Instead of only generating histograms, it is possible to store entire PYTHIA events in ROOT trees. The tree example in the rootexamples subdirectory provides an example of this and is comprised of the following files
    • tree.cc is the main example program showing how PYTHIA events can be stored in ROOT trees.
    • pythiaLinkdef.h is used by Makefile to generate the dictionary for all PYTHIA classes involved in the IO, as needed for the example.
    • pythiaROOT.h is a small include declaring the Pythia8 namespace as default.

    The example may be compiled and run with
        make tree
        ./tree.exe
    
    After the example has run, the pytree.root file will now be present containing the PYTHIA events. Note that files can become quite large when many events are generated.


    PYTHIA as a plugin to ROOT

    In more ROOT-centric applications, PYTHIA can be run as a ROOT plug-in. This requires a version of ROOT that has been installed from source. The reason is that the interfaces depend on PYTHIA header files that are not distributed with ROOT. Installing ROOT is not more difficult than the PYTHIA installation, and some guidelines are provided below.

    Installation

    To be run as a plugin, PYTHIA must be compiled as a shared library. This is achieved by running the PYTHIA configure script with the --enable-shared option before make is run.

    Define an environment variable for the path to your PYTHIA installation directory
        export PYTHIA8=path_to_PYTHIA8_installation
    
    Before compiling ROOT, configure ROOT by running the configure command including the following options
        --enable-pythia8
        --with-pythia8-incdir=$PYTHIA8/include
        --with-pythia8-libdir=$PYTHIA8/lib
    
    In case ROOT has already been compiled before, it will only recompile the PYTHIA module and build the library libEGPythia8.

    Interfaces

    When running PYTHIA as a plugin, the exact interface structure becomes very relevant. ROOT provides two simple interfaces (wrappers) for PYTHIA 8. The code for these interfaces are located in
        path_to_ROOT_source/montecarlo/pythia8
    

    The two interfaces are
    • TPythia8 is an implementation of the TGenerator interface for PYTHIA 8.
      It allows you to use PYTHIA within a ROOT macro or as a plug-in for a general-purpose particle generator based on this interface. The main methods of the interface are
      • GenerateEvent() which triggers the generation of the next event, and
      • ImportParticles(TClonesArray* particles) which copies the native PYTHIA stack into a TClonesArray of TParticles.
      In addition, some methods that are directly related to corresponding PYTHIA methods are implemented
      • ReadString(const char* string) -> readString(...)
      • ReadConfigFile(const char* string) -> readFile(...)
      • Initialize(int idAin, int idBin, double ecms) -> init(...)
      • EventListing() -> event.list()
      • PrintStatistic() -> statistics()
      These methods provide already the basic PYTHIA functionality interactively from the ROOT command line. However, this does not mean that the usage of PYTHIA from within ROOT is restricted to these methods. In compiled code, one can always obtain a pointer to the Pythia instance e.g.
          TPythia8        *tp = new TPythia8();
          Pythia8::Pythia *p  = tp->Pythia8();
      giving access to the full PYTHIA functionality. To access this functionality in the CINT interpreter see the "Advanced usage" section below.
    • TPythia8Decayer is an implementation of the TVirtualMCDecayer interface.
      It allows you to use PYTHIA as a plug-in decayer for simulation frameworks based on the Virtual Monte Carlo (VMC) interface classes. The main methods of the interface are
      • TPythia8Decayer::Init() for initialisation,
      • TPythia8Decayer::Decay(Int_t pdg, TLorentzVector* p) to decay a particle with PDG code pdg and 4-momentum p, and
      • ImportParticles(TClonesArray* particles) to retrieve the decay products as TParticles in the TClonesArray particles.

    An example

    A basic example for generating minimum-bias events with PYTHIA 8 inside a ROOT macro, and filling some histograms with the kinematics of the final-state particles is provided in either of the locations below
        /path_to_ROOT_source/tutorials/pythia/pythia8.C
        /path_to_ROOT_installation/share/doc/root/tutorials/pythia/pythia8.C
    

    Note that before executing this script
    • the environment variables PYTHIA8 and PYTHIA8DATA must be setup correctly e.g.
          export PYTHIA8=/path_to_PYTHIA_installation
          export PYTHIA8DATA=$PYTHIA8/xmldoc
        
    • your LD_LIBRARY_PATH must contain the location of the PYTHIA 8 shared library, e.g.
          export LD_LIBRARY_PATH=$LD_LIBRARY_PATH:path_to_PYTHIA8_installation/lib
        
    The script can then be run with ROOT
        root pythia8.C
    
    After execution, ROOT will display some histograms from the event generation.

    Advanced usage

    To access the full PYTHIA functionality from the CINT interpreter, a ROOT dictionary must be created. An example of creating this dictionary is contained in the rootexamples directory. The pythiaDict.so library may be created by running
        make dict
    
    This may then be loaded in ROOT giving full access to the full PYTHIA 8 functionality, e.g. in an interactive session
        gSystem->Load("path_to_PYTHIA8_installation/rootexamples/pythiaDict");
        Pythia8::Pythia *p = new Pythia8::Pythia();
        p->readString("SoftQCD:nonDiffractive = on");
    
    pythia8-8.1.80.orig/xmldoc/HiddenValleyProcesses.xml0000444000175000017500000005276612217346303020617 0ustar sunsun

    Hidden Valley Processes

    This Hidden Valley (HV) scenario has been developed specifically to allow the study of visible consequences of radiation in a hidden sector, by recoil effect. A key aspect is therefore that the normal timelike showering machinery has been expanded with a third kind of radiation, in addition to the QCD and QED ones. These three kinds of radiation are fully interleaved, i.e. evolution occurs in a common pT-ordered sequence. The scenario is described in Car10. Furthermore hadronization in the hidden sector has been implemented. Three main scenarios for production into and decay out of the hidden sector can be compared, in each case either for an Abelian or a non-Abelian gauge group in the HV. For further details see Car11.

    Particle content and properties

    For simplicity we assume that the HV contains an unbroken SU(N) gauge symmetry. This is used in the calculation of production cross sections. These could be rescaled by hand for other gauge groups. is U(1) for Ngauge = 1, is SU(N) if Ngauge > 1. Note that pair production cross sections contains a factor of Ngauge for new particles in the fundamental representation of this group.

    A minimal HV particle content has been introduced. Firstly, there is a set of 12 particles that mirrors the Standard Model flavour structure, and is charged under both the SM and the HV symmetry groups. Each new particle couples flavour-diagonally to a corresponding SM state, and has the same SM charge and colour, but in addition is in the fundamental representation of the HV colour, as follows:
    Dv, identity 4900001, partner to the normal d quark;
    Uv, identity 4900002, partner to the normal u quark;
    Sv, identity 4900003, partner to the normal s quark;
    Cv, identity 4900004, partner to the normal c quark;
    Bv, identity 4900005, partner to the normal b quark;
    Tv, identity 4900006, partner to the normal t quark;
    Ev, identity 4900011, partner to the normal e lepton;
    nuEv, identity 4900012, partner to the normal nue neutrino;
    MUv, identity 4900013, partner to the normal mu lepton;
    nuMUv, identity 4900014, partner to the normal numu neutrino;
    TAUv, identity 4900015, partner to the normal tau lepton;
    nuTAUv, identity 4900016, partner to the normal nutau neutrino.
    Collectively we will refer to these states as Fv; note, however, that they need not be fermions themselves.

    In addition the model contains the HV gauge particle, either a HV-gluon or a HV-photon, but not both; see Ngauge above:
    gv, identity 4900021, is the massless gauge boson of the HV SU(N) group;
    gammav, identity 4900022, is the massless gauge boson of the HV U(1) group.

    Finally, for the basic HV scenario, there is a new massive particle with only HV charge sitting in the fundamental representation of the HV gauge group:
    qv, identity 4900101.

    The typical scenario would be for pair production of one of the states presented first above, e.g. g g -> Dv Dvbar. Such a Dv can radiate gluons and photons like an SM quark, but in addition HV-gluons or HV-photons in a similar fashion. Eventually the Dv will decay like Dv -> d + qv. The strength of this decay is not set as such, but is implicit in your choice of width for the Dv state. Thereafter the d and qv can radiate further within their respective sectors. The qv, gv or gammav are invisible, so their fate need not be considered further.

    While not part of the standard scenario, as an alternative there is also a kind of Z' resonance:
    Zv, identity 4900023, a boson that can couple both to pairs of Standard Model fermions and to qv qvbar pairs. Mass, total width and branching ratios can be set as convenient.
    This opens up for alternative processes l^+l^-, q qbar -> Zv -> qv qvbar.

    The possibility of a leakage back from the hidden sector will be considered in the Hadronization section below. For the U(1) case the gammav acquires a mass and can decay back to a Standard-Model fermion pair, while the qv remains invisible. The SU(N) alternative remains unbroken, so confinement holds and the gv is massless. A string like qv - gv - ... - gv - qvbar can break by the production of new qv - qvbar pairs, which will produce qv-qvbar mesons. It would be possible to build a rather sophisticated hidden sector by trivial extensions of the HV flavour content. For now, however, the qv can be duplicated in up to eight copies with the same properties except for the flavour charge. These are assigned codes 4900101 - 4900108. This gives a total of 64 possible lowest-lying mesons. We also include a duplication of that, into two multiplets, corresponding to the pseudoscalar and vector mesons of QCD. For now, again, these are assumed to have the same mass and other properties. Only the flavour-diagonal ones can decay back into the Standard-Model sector, however, while the rest remains in the hidden sector. It is therefore only necessary to distinguish a few states:
    pivDiag, identity 4900111, a flavour-diagonal HV-meson with spin 0 that can decay back into the Standard-Model sector;
    rhovDiag, identity 4900113, a flavour-diagonal HV-meson with spin 1 that can decay back into the Standard-Model sector;
    pivUp, identity 4900211, an off-diagonal HV-meson with spin 0 that is stable and invisible, with an antiparticle pivDn with identity -4900211; the particle is the one where the code of the flavour is larger than that of the antiflavour;
    rhovUp, identity 4900213, an off-diagonal HV-meson with spin 1 that is stable and invisible, with an antiparticle rhovDn with identity -4900213; again the particle is the one where the code of the flavour is larger than that of the antiflavour;
    ggv, identity 4900991, is only rarely used, to handle cases where it is kinematically impossible to produce an HV-meson on shell, and it therefore is assumed to de-excite by the emission of invisible gv-gv v-glueball bound states.

    Only the spin of the HV-gluon or HV-photon is determined unambiguously to be unity, for the others you can make your choice. The spin of the HV partners of the SM fermions, e.g. Dv, Uv, Ev and nuEv. The spin of qv when the Fv (the HV partners of the SM fermions) have spin 1/2. (While, if they have spin 0 or 1, the qv spin is fixed at 1/2.) If the Fv have spin 1 then their production cross section depends on the presence of anomalous magnetic dipole moment, i.e. of a kappa different from unity. For other spins this parameter is not used. allow kinematic mixing or not. strength of kinetic mixing.

    You should set the Fv and qv masses appropriately, with the latter smaller than the former two to allow decays. When U(1) hadronization is switched on, you need to set the gammav mass and decay modes. For SU(N) hadronization the HV-meson masses should be set to match the qv ones. The simplest is to assume that m_qv defines a constituent mass, so that m_HVmeson = 2 m_qv. The hvMesonDiag decay modes also need to be set.

    Production processes

    Common switch for the group of all hard Hidden Valley processes, as listed separately in the following. Pair production g g -> Dv Dvbar. Code 4901. Pair production g g -> Uv Uvbar. Code 4902. Pair production g g -> Sv Svbar. Code 4903. Pair production g g -> Cv Cvbar. Code 4904. Pair production g g -> Bv Bvbar. Code 4905. Pair production g g -> Tv Tvbar. Code 4906. Pair production q qbar -> Dv Dvbar via intermediate gluon. Code 4911. Pair production q qbar -> Uv Uvbar via intermediate gluon. Code 4912. Pair production q qbar -> Sv Svbar via intermediate gluon. Code 4913. Pair production q qbar -> Cv Cvbar via intermediate gluon. Code 4914. Pair production q qbar -> Bv Bvbar via intermediate gluon. Code 4915. Pair production q qbar -> Tv Tvbar via intermediate gluon. Code 4916. Pair production f fbar -> Dv Dvbar via intermediate gamma*/Z^*. Code 4921. Pair production f fbar -> Uv Uvbar via intermediate gamma*/Z^*. Code 4922. Pair production f fbar -> Sv Svbar via intermediate gamma*/Z^*. Code 4923. Pair production f fbar -> Cv Cvbar via intermediate gamma*/Z^*. Code 4924. Pair production f fbar -> Bv Bvbar via intermediate gamma*/Z^*. Code 4925. Pair production f fbar -> Tv Tvbar via intermediate gamma*/Z^*. Code 4926. Pair production f fbar -> Ev Evbar via intermediate gamma*/Z^*. Code 4931. Pair production f fbar -> nuEv nuEvbar via intermediate gamma*/Z^*. Code 4932. Pair production f fbar -> MUv MUvbar via intermediate gamma*/Z^*. Code 4933. Pair production f fbar -> nuMUv nuMUvbar via intermediate gamma*/Z^*. Code 4934. Pair production f fbar -> TAUv TAUvbar via intermediate gamma*/Z^*. Code 4935. Pair production f fbar -> nuTAUv nuTAUvbar via intermediate gamma*/Z^*. Code 4936. Production f fbar -> Zv where Zv is a generic resonance that couples both SM fermion pairs and a qv qvbar pair. Not part of the framework of the above processes, but as an alternative. Code 4941.

    Timelike showers

    One key point of this HV scenario is that radiation off the HV-charged particles is allowed. This is done by the standard final-state showering machinery. (HV particles are not produced in initial-state radiation.) All the (anti)particles Fv and qv have one (negative) unit of HV charge. That is, radiation closely mimics the one in QCD. Both QCD, QED and HV radiation are interleaved in one common sequence of decreasing emission pT scales. Each radiation kind defines a set of dipoles, usually spanned between a radiating parton and its recoil partner, such that the invariant mass of the pair is not changed when a radiation occurs. This need not follow from trivial colour assignments, but is often obvious. For instance, in a decay Qv -> q + qv the QCD dipole is between the q and the hole after Qv, but qv becomes the recoiler should a radiation occur, while the role of q and qv is reversed for HV radiation.

    This also includes matrix-element corrections for a number of decay processes, with colour, spin and mass effects included Nor01. They were calculated within the context of the particle content of the MSSM, however, which does not include spin 1 particles with unit colour charge. In such cases spin 0 is assumed instead. By experience, the main effects come from mass and colour flow anyway, so this is not a bad approximation. (Furthermore the MSSM formulae allow for gamma_5 factors from wave functions or vertices; these are even less important.)

    An emitted gv can branch in its turn, gv -> gv + gv. This radiation may affect momenta in the visible sector by recoil effect, but this is a minor effect relative to the primary emission of the gv. switch on final-state shower of gv or gammav in a HV production process. fixed alpha scale of gv/gammav emission; corresponds to alpha_strong of QCD or alpha_em of QED. For shower branchings such as Dv -> Dv + gv the coupling is multiplied by C_F = (N^2 - 1) / (2 * N) for an SU(N) group and for gv -> gv + gv by N. lowest allowed pT of emission. Chosen with same default as in normal QCD showers.

    Hadronization

    By default the HV particles with no Standard Model couplings are not visible. Their presence can only be deduced by the observation of missing (transverse) momentum in the event as a whole. In the current implementation it is possible to simulate two different scenarios where activity can leak back from the hidden sector.

    The first possibility is relevant for the U(1) scenario. The U(1) group may be broken, so that the gammav acquires a mass. Furthermore, the gammav may have a small mixing angle with the normal photon, or with some Z' state or other mediator, and may thus decay back into Standard Model particles. The qv still escapes undetected; recall that there is no confinement in the U(1) option.

    In order to enable this machinery two commands are necessary, 4900022:m0 = ... to set the gammav mass to the desired value, and 4900022:onMode = on to enable gammav decays. The default gammav decay table contains all Standard Model fermion-antifermion pairs, except top, with branching ratios in proportion to their coupling to the photon, whenever the production channel is allowed by kinematics. This table could easily be tailored to more specific models and needs. For instance, for a mass below 1 - 2 GeV, it would make sense to construct a table of exclusive hadronic decay channels rather than go the way via a hadronizing quark pair.

    The gammav are expected to decay so rapidly that no secondary vertex will be detectable. However, it is possible to set 4900022:tau0 to a finite lifetime (in mm) that will be used to create separated secondary vertices.

    The second, more interesting, possibility is relevant for the SU(N) scenarios. Here the gauge group remains unbroken, i.e. gv is massless, and the partons are confined. Like in QCD, the HV-partons can therefore be arranged in one single HV-colour-ordered chain, with a qv in one end, a qvbar in the other, and a varying number of gv in between. Each event will only contain (at most) one such string, (i) since perturbative branchings gv -> qv qvbar have been neglected, as is a reasonable approximation for QCD, and (ii) since HV-colours are assigned in the N_C -> infinity limit, just like in the handling of string fragmentation in QCD. The HV-string can then fragment by the nonperturbative creation of qv qvbar pairs, leading to the formation of HV-mesons along the string, each with its qv from one vertex and its qvbar from the neighbouring one.

    Since, so far, we have only assumed there to be one qv species, all produced qv qvbar HV-mesons are of the same flavour-diagonal species. Such an HV-meson can decay back to the normal sector, typically by whatever mediator particle allowed production in the first place. In this framework the full energy put into the HV sector will leak back to the normal one. To allow more flexibility, an ad hoc possibility of n_Flav different qv species is introduced. For now they are all assumed to have the same mass and other properties, but distinguished by some flavour-like property. Only the flavour-diagonal ones can decay, meaning that only a fraction (approximately) 1/n_Flav of the HV-energy leaks back, while the rest remains in the hidden sector.

    This scenario contains more parameters than the first one, for the U(1) group. They can be subdivided into two sets. One is related to particle properties, both for qv and for the two different kinds of HV-mesons, here labeled 4900111 and 4900113 for the diagonal ones, and +-4900211 and +-4900213 for the off-diagonal ones. It makes sense to set the HV-meson masses to be twice the qv one, as in a simple constituent mass context. Furthermore the hvMesonDiag decay modes need to be set up. Like with the gammav in the U(1) option, the default decay table is based on the branching ratios of an off-shell photon.

    The second set are fragmentation parameters that extend or replace the ones used in normal string fragmentation. Some of them are not encoded in the same way as normally, however, but rather scale as the qv mass is changed, so as to keep a sensible default behaviour. This does not mean that deviations from this set should not be explored, or that other scaling rules could be preferred within alternative scenarios. These parameters are as follows. switch on string fragmentation of the HV partonic system. Only relevant for SU(N) scenarios. number of different flavours assumed to exist in the hadronization description, leading to approximately 1/n_Flav of the produced HV-mesons being flavour-diagonal and capable to decay back to Standard Model particles. fraction of HV-mesons that are assigned spin 1 (vector), with the remainder spin 0 (pseudoscalar). Assuming the qv have spin 1/2 and the mass splitting is small, spin counting predicts that 3/4 of the mesons should have spin 1. The a parameter of the Lund symmetric fragmentation function. See the normal fragmentation function description for the shape of this function. The b parameter of the Lund symmetric fragmentation function, multiplied by the square of the qv mass. This scaling ensures that the fragmentation function keeps the same shape when the qv mass is changed (neglecting transverse momenta). r_qv, i.e. the Bowler correction factor to the Lund symmetric fragmentation function, which could be made weaker or stronger than its natural value. the width sigma of transverse momenta in the HV fragmentation process, normalized to the qv mass. This ensures that sigma scales proportionately to m_qv. See the normal fragmentation pT description for conventions for factors of 2. pythia8-8.1.80.orig/xmldoc/cteq6l1.tbl0000444000175000017500000065531212217346302015613 0ustar sunsun Parton Distribution Table : cteq6l1 Ordr, Nfl, lambda Qmass 1, 2, 3, 4, 5, 6 1. 5. 0.1652 0.000 0.000 0.200 1.300 4.500 180.000 NX, NT, NfMx 95 19 5 QINI, QMAX, (QV(I), I =0, NT) 1.30000E+00 1.00000E+04 1.30000E+00 1.53865E+00 1.84636E+00 2.24885E+00 2.78358E+00 3.50602E+00 4.50000E+00 6.20054E+00 8.81356E+00 1.29625E+01 1.97913E+01 3.14839E+01 5.23915E+01 9.15982E+01 1.69063E+02 3.31152E+02 6.92354E+02 1.55489E+03 3.77707E+03 1.00000E+04 XMIN, (XV(I), I =0, NX) 1.00000E-06 0.00000E+00 1.00000E-06 1.28121E-06 1.64152E-06 2.10317E-06 2.69463E-06 3.45242E-06 4.42329E-06 5.66715E-06 7.26076E-06 9.30241E-06 1.19180E-05 1.52689E-05 1.95617E-05 2.50609E-05 3.21053E-05 4.11287E-05 5.26863E-05 6.74889E-05 8.64459E-05 1.10720E-04 1.41800E-04 1.81585E-04 2.32503E-04 2.97652E-04 3.80981E-04 4.87518E-04 6.26039E-04 8.00452E-04 1.02297E-03 1.30657E-03 1.66759E-03 2.12729E-03 2.71054E-03 3.44865E-03 4.37927E-03 5.54908E-03 7.01192E-03 8.83064E-03 1.10763E-02 1.38266E-02 1.71641E-02 2.11717E-02 2.59364E-02 3.15062E-02 3.79623E-02 4.53425E-02 5.36750E-02 6.29705E-02 7.32221E-02 8.44039E-02 9.64793E-02 1.09332E-01 1.23067E-01 1.37507E-01 1.52639E-01 1.68416E-01 1.84794E-01 2.01731E-01 2.19016E-01 2.36948E-01 2.55242E-01 2.73927E-01 2.92954E-01 3.12340E-01 3.32036E-01 3.52019E-01 3.72282E-01 3.92772E-01 4.13533E-01 4.34326E-01 4.55495E-01 4.76836E-01 4.98342E-01 5.20006E-01 5.41818E-01 5.63773E-01 5.85861E-01 6.08077E-01 6.30459E-01 6.52800E-01 6.75387E-01 6.98063E-01 7.20830E-01 7.43683E-01 7.66623E-01 7.89636E-01 8.12791E-01 8.35940E-01 8.59175E-01 8.82485E-01 9.05866E-01 9.29311E-01 9.52817E-01 9.76387E-01 1.00000E+00 Parton Distribution Table: 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 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4.88083E+04 3.36615E+04 2.31910E+04 1.59615E+04 1.09739E+04 7.54238E+03 5.15078E+03 3.53769E+03 2.42969E+03 1.66923E+03 1.14769E+03 7.89689E+02 5.44533E+02 3.76625E+02 2.61605E+02 1.82653E+02 1.28385E+02 9.09820E+01 6.51030E+01 4.71067E+01 3.45095E+01 2.56216E+01 1.92803E+01 1.47243E+01 1.13933E+01 8.92762E+00 7.07576E+00 5.66466E+00 4.57443E+00 3.72147E+00 3.04579E+00 2.50777E+00 2.07005E+00 1.71457E+00 1.42288E+00 1.18213E+00 9.82502E-01 8.15993E-01 6.78183E-01 5.61591E-01 4.64282E-01 3.82688E-01 3.14364E-01 2.57083E-01 2.09212E-01 1.69323E-01 1.36168E-01 1.08800E-01 8.61847E-02 6.78328E-02 5.27793E-02 4.06450E-02 3.09429E-02 2.32583E-02 1.72355E-02 1.25719E-02 9.00948E-03 6.33280E-03 4.34700E-03 2.91771E-03 1.89821E-03 1.19511E-03 7.24322E-04 4.19853E-04 2.30804E-04 1.19230E-04 5.69190E-05 2.47869E-05 9.58467E-06 3.18707E-06 8.74235E-07 1.86959E-07 2.92339E-08 2.65384E-09 0.00000E+00 pythia8-8.1.80.orig/xmldoc/Histograms.xml0000444000175000017500000002715312217346303016470 0ustar sunsun

    Histograms

    The Hist class gives a simple implementation of one-dimensional histograms, useful for quick-and-dirty testing, without the need to link to more sophisticated packages. For this reason it is used in many of the sample main programs found in the examples subdirectory.

    Basic principles

    We here provide a simple overview of what is involved. As a first step you need to declare a histogram, with name, title, number of bins and x range (from, to).
       Hist ZpT( "Z0 pT spectrum", 100, 0., 100.);
    
    Alternatively you can first declare it and later define it:
       Hist ZpT;
       ZpT.book( "Z0 pT spectrum", 100, 0., 100.);
    
    Once declared, its contents can be added by repeated calls to fill,
       ZpT.fill( 22.7, 1.); 
    
    where the first argument is the x value and the second the weight. Since the weight defaults to 1 the last argument could have been omitted in this case.

    A set of overloaded operators have been defined, so that histograms can be added, subtracted, divided or multiplied by each other. Then the contents are modified accordingly bin by bin. Thus the relative deviation between two histograms data and theory can be found as

      diff = (data - theory) / (data + theory);
    
    assuming that diff, data and theory have been booked with the same number of bins and x range. That responsibility rests on the user; some checks are made for compatibility, but not enough to catch all possible mistakes.

    Also overloaded operations with double real numbers are available. Again these four operations are defined bin by bin, i.e. the corresponding amount is added to, subtracted from, multiplied by or divided by each bin. The double number can come before or after the histograms, with obvious results. Thus the inverse of a histogram result is given by 1. / result. The two kind of operations can be combined, e.g.

      allpT = ZpT + 2. * WpT
    
    Finally, also the +=, -+, *=, /= are overloaded, with the right-hand side being either a histogram or a real number.

    Output format

    A histogram can be printed by making use of the overloaded << operator, e.g.:

       cout << ZpT;
    
    The printout format is inspired by the old HBOOK one. To understand how to read this format, consider the simplified example
                                        
            3.50*10^ 2  9                     
            3.00*10^ 2  X   7               
            2.50*10^ 2  X  1X               
            2.00*10^ 2  X6 XX                
            1.50*10^ 2  XX5XX                 
            1.00*10^ 2  XXXXX                
            0.50*10^ 2  XXXXX        
    
              Contents 
                *10^ 2  31122
                *10^ 1  47208
                *10^ 0  79373
    
              Low edge  -- 
                *10^ 1  10001 
                *10^ 0  05050
    
    The key feature is that the Contents and Low edge have to be read vertically. For instance, the first bin has the contents 3 * 10^2 + 4 * 10^1 + 7 * 10^0 = 347. Correspondingly, the other bins have contents 179, 123, 207 and 283. The first bin stretches from -(1 * 10^1 + 0 * 10^0) = -10 to the beginning of the second bin, at -(0 * 10^1 + 5 * 10^0) = -5.

    The visual representation above the contents give a simple impression of the shape. An X means that the contents are filled up to this level, a digit in the topmost row the fraction to which the last level is filled. So the 9 of the first column indicates this bin is filled 9/10 of the way from 3.00*10^2 = 300 to 3.50*10^2 = 350, i.e. somewhere close to 345, or more precisely in the range 342.5 to 347.5.

    The printout also provides some other information, such as the number of entries, i.e. how many times the histogram has been filled, the total weight inside the histogram, the total weight in underflow and overflow, and the mean value and root-mean-square width (disregarding underflow and overflow). The mean and width assumes that all the contents is in the middle of the respective bin. This is especially relevant when you plot a integer quantity, such as a multiplicity. Then it makes sense to book with limits that are half-integers, e.g.

       Hist multMPI( "number of multiparton interactions", 20, -0.5, 19.5);
    
    so that the bins are centered at 0, 1, 2, ..., respectively. This also avoids ambiguities which bin gets to be filled if entries are exactly at the border between two bins. Also note that the fill( xValue) method automatically performs a cast to double precision where necessary, i.e. xValue can be an integer.

    The methods

    We here collect a more complete and formal overview of the methods. declare a histogram, but does not define it. declare and define a histogram, where is a string with the title of the histogram at output, is the number of bin the x range will be subdivided into, limited to be at most 1000, is the lower edge of the histogram, is the upper edge of the histogram. creates an identical copy of the histogram in the argument, including bin contents. creates an identical copy of the histogram in the argument, including bin contents, except that a new title is provided as first argument. copies all properties of the histogram in the argument, except that the original histogram title is retained. define a histogram that previously was only declared; see above for the meaning of the arguments. change the title of a histogram, but keep other properties unchanged. reset bin contents, but keep other histogram properties unchanged. fill the histogram, where is the x position where the filling should occur, and is the amount of weight to be added at this x value. appends a simple histogram printout (see above for format) to the ostream, while leaving the histogram object itself unchanged. At most 100 columns are allowed to be displayed. If the number of bins is larger than 100 then the contents of adjacent bins are added to give the value in each column. (Two by two up to 200 bins, three by three up to 300, and so on, with the very last column possibly summing fewer rows than the others.) print a two-column table, where the first column gives the center of each bin and the second one the corresponding bin contents. The desired output stream or file name can be provided as argument. The former is more flexible (e.g., it allows easy append to an existing file), whereas the latter is simpler for the case that each histogram should be a file of its own. The table may be useful for plotting e.g. with Gnuplot. print a three-column table, where the first column gives the center of each bin and the second and third ones the corresponding bin contents of the two histograms. Only works if the two histograms have the same x axis (within a tiny tolerance), else nothing will be done. return the value in bin iBin, ranging from 1 through numberOfBins, with 0 for underflow and numberOfBins + 1 for overflow. return the number of entries, i.e. the number of time that fill(...) has been called. checks that the number of bins and upper and lower limits are the same as in the histogram in the argument. by default take 10-logarithm of current contents bin by bin. With optional argument false instead take e-logarithm of contents bin by bin. If to be used, then right before the histogram is output. take square root of current contents bin by bin, with negative contents set to zero. adds or subtracts the current histogram by the contents of the histogram in the argument if sameSize(...) is true, else does nothing. multiplies or divides the current histogram by the contents of the histogram in the argument if sameSize(...) is true, else does nothing. adds or subtracts each bin content by the common offset f. multiplies or divides each bin content by the common factor f. add a constant to a histogram or two histograms to each other, bin by bin. subtract a histogram from a constant, a constant from a histogram, or two histograms from each other, bin by bin. multiply a constant by a histogram or two histograms by each other, bin by bin. divide a constant by a histogram, a histogram by a constant, or two histograms by each other, bin by bin.
    pythia8-8.1.80.orig/xmldoc/pythia8100.tex0000444000175000017500000022726312217346316016167 0ustar sunsun%% Computer Physics Communications class file, slightly modified %% for reduced inter-paragraph and inter-section spacing. \documentclass{elsartmod} % Include graphics package. \usepackage{axodraw} % Standardised indentation. \newcommand{\cindent}{\hspace*{10mm}~} %Vertical positioning of page %\setlength{\topmargin}{20mm} \begin{document} \begin{frontmatter} \begin{flushright} arXiv:0710.3820\\ CERN-LCGAPP-2007-04\\ LU TP 07-28\\ FERMILAB-PUB-07-512-CD-T\\ October 2007\\ \end{flushright} \title{A Brief Introduction to PYTHIA 8.1} \author[a,b]{Torbj\"orn Sj\"ostrand\thanksref{author}}, \author[c]{Stephen Mrenna}, \author[a,c]{Peter Skands} \thanks[author]{Corresponding author, e-mail: torbjorn@thep.lu.se} \address[a]{CERN/PH, CH--1211 Geneva 23, Switzerland} \address[b]{Department of Theoretical Physics, Lund University,\\ S\"olvegatan 14A, SE-223 62 Lund, Sweden} \address[c]{Fermi National Accelerator Laboratory, Batavia, IL 60510, USA} \begin{abstract} The \textsc{Pythia} program is a standard tool for the generation of high-energy collisions, comprising a coherent set of physics models for the evolution from a few-body hard process to a complex multihadronic final state. It contains a library of hard processes and models for initial- and final-state parton showers, multiple parton-parton interactions, beam remnants, string fragmentation and particle decays. It also has a set of utilities and interfaces to external programs. While previous versions were written in Fortran, \textsc{Pythia}~8 represents a complete rewrite in C++. The current release is the first main one after this transition, and does not yet in every respect replace the old code. It does contain some new physics aspects, on the other hand, that should make it an attractive option especially for LHC physics studies. \begin{flushleft} %Insert your suggested PACS number here PACS: 13.66.-a, 13.85.-t, 12.38.-t, 12.15.-y, 12.60.-i \end{flushleft} \begin{keyword} event generators, multiparticle production, parton showers, multiple interactions, hadronisation \end{keyword} \end{abstract} \dedicated{\rule{0mm}{8mm}Dedicated to the memory of\\[3mm] \textbf{\textit{\Large Hans-Uno Bengtsson}}\\[1mm] 1953 -- 2007\\ The father of PYTHIA} \end{frontmatter} \clearpage % Computer program descriptions should contain the following % PROGRAM SUMMARY. {\bf NEW VERSION PROGRAM SUMMARY} %Delete as appropriate. \begin{small} \noindent {\em Manuscript Title:A Brief Introduction to \textsc{Pythia} 8.1} \\ {\em Authors:Torbj\"orn Sj\"ostrand, Stephen Mrenna, Peter Skands} \\ {\em Program Title: \textsc{Pythia} 8.1} \\ {\em Journal Reference:} \\ %Leave blank, supplied by Elsevier. {\em Catalogue identifier:} \\ %Leave blank, supplied by Elsevier. {\em Licensing provisions: GPL version 2} \\ %enter "none" if CPC non-profit use license is sufficient. {\em Programming language: C++} \\ {\em Computer: commodity PCs} \\ %Computer(s) for which program has been designed. {\em Operating systems: Linux; should also work on other systems} \\ %Operating system(s) for which program has been designed. {\em RAM: 8} megabytes \\ %RAM in bytes required to execute program with typical data. %{\em Number of processors used:} \\ % %If more than one processor. %{\em Supplementary material:} \\ % % Fill in if necessary, otherwise leave out. {\em Keywords: event generators, multiparticle production, parton showers, multiple interactions, hadronisation} \\ % Please give some freely chosen keywords that we can use in a % cumulative keyword index. {\em PACS: 13.66.-a, 13.85.-t, 12.38.-t, 12.15.-y, 12.60.-i} \\ % see http://www.aip.org/pacs/pacs.html {\em Classification: 11.2 Phase Space and Event Simulation} \\ %Classify using CPC Program Library Subject Index, see ( % http://cpc.cs.qub.ac.uk/subjectIndex/SUBJECT_index.html) %e.g. 4.4 Feynman diagrams, 5 Computer Algebra. %{\em External routines/libraries: none} \\ % % Fill in if necessary, otherwise leave out. %{\em Subprograms used:} \\ % %Fill in if necessary, otherwise leave out. {\em Catalogue identifier of previous version: ADNN\_v1\_0} \\ %Only required for a New Version summary, otherwise leave out. {\em Journal reference of previous version: T. Sj\"ostrand, P. Ed\'en, C. Friberg, L. L\"onnblad, G. Miu, S. Mrenna and E. Norrbin, Computer Physics Commun. {\bf 135} (2001) 238} \\ %Only required for a New Version summary, otherwise leave out. {\em Does the new version supersede the previous version?: yes, partly} \\ %Only required for a New Version summary, otherwise leave out. \\ {\em Nature of problem: high-energy collisions between elementary particles normally give rise to complex final states, with large multiplicities of hadrons, leptons, photons and neutrinos. The relation between these final states and the underlying physics description is not a simple one, for two main reasons. Firstly, we do not even in principle have a complete understanding of the physics. Secondly, any analytical approach is made intractable by the large multiplicities. }\\ %Describe the nature of the problem here. \\ {\em Solution method: complete events are generated by Monte Carlo methods. The complexity is mastered by a subdivision of the full problem into a set of simpler separate tasks. All main aspects of the events are simulated, such as hard-process selection, initial- and final-state radiation, beam remnants, fragmentation, decays, and so on. Therefore events should be directly comparable with experimentally observable ones. The programs can be used to extract physics from comparisons with existing data, or to study physics at future experiments.}\\ %Describe the method solution here. \\ {\em Reasons for the new version: improved and expanded physics models, transition from Fortran to C++}\\ %Only required for a New Version summary, otherwise leave out. \\ {\em Summary of revisions: new user interface, transverse-momentum-ordered showers, interleaving with multiple interactions, and much more}\\ %Only required for a New Version summary, otherwise leave out. \\ {\em Restrictions: depends on the problem studied}\\ %Describe any restrictions on the complexity of the problem here. \\ {\em Unusual features: none}\\ %Describe any unusual features of the program/problem here. \\ %{\em Additional comments:}\\ %Provide any additional comments here. % \\ {\em Running time: 10--1000 events per second, depending on process studied}\\ %Give an indication of the typical running time here. % \\ %{\em References:} %\begin{refnummer} %\item Reference 1 % This is the reference list of the Program Summary %\item Reference 2 % Type references in text as [1], [2], etc. %\item Reference 3 % This list is different from the bibliography, which % % you can use in the Long Write-Up. %\end{refnummer} \end{small} \clearpage % In program descriptions the main text of the paper is listed under % the heading LONG WRITE-UP. \hspace{1pc} {\bf LONG WRITE-UP} \section{Introduction} The development of \textsc{Jetset} \cite{jetset}, containing several of the components that later were merged with \textsc{Pythia} \cite{pythiaearly}, was begun in 1978. Thus the current \textsc{Pythia}~6 generator \cite{pythiasixone, pythiasixfour} is the product of almost thirty years of development, and some of the code has not been touched in a very long time. New options have been added, but old ones seldom removed. The basic structure has been expanded in different directions, well beyond what it was once intended for, making it rather cumbersome by now. {}From the onset, all code has been written in Fortran~77. For the LHC era, the experimental community has made the decision to move heavy computing completely to C++. Fortran support may be poor to non-existing, and young experimenters will not be conversant in Fortran any longer. Therefore it is logical also to migrate \textsc{Pythia} to C++, and in the process clean up and modernise various aspects. A first attempt in this direction was the \textsc{Pythia}~7 project \cite{pythiaseven}. However, priority came to be given to the development of a generic administrative structure, renamed \textsc{ThePEG} \cite{thepeg} and adopted by the \textsc{Herwig++} \cite{herwigpp} group, while the physics parts of \textsc{Pythia}~7 remained underdeveloped. \textsc{Pythia}~8 is a clean new start, to provide a successor to \textsc{Pythia}~6. It is a completely standalone generator, thus not relying on \textsc{ThePEG} or any other external library. Some optional hooks for links to other programs are provided, however. The version presented here is the first operational one in the \textsc{Pythia}~8 series. As such it is not yet tested and tuned enough to have reached the same level of maturity as \textsc{Pythia}~6, so we expect the two to coexist for a while. It is only by an increasing use of the new version that it will mature, however, so we encourage a critical try-out, and look forward to feedback. The intention is to release a version in time for comparisons with first LHC data. Thus some areas, like $\gamma\mathrm{p}$ and $\gamma\gamma$ physics, are not yet addressed. Further, some intended processes remain to be implemented. Actually, with the rise of automatic matrix-element code generation and phase-space sampling, input of process-level events via the Les Houches Accord (LHA) \cite{lha} and with Les Houches Event Files (LHEF) \cite{lhef} reduces the need to have an extensive process library inside \textsc{Pythia} itself. Thus emphasis is more on providing a good description of subsequent steps of the story, involving elements such as initial- and final-state parton showers, multiple parton--parton interactions, string fragmentation, and decays. The current article provides an introduction to \textsc{Pythia}~8. The programming aspects are covered in more detail in a set of interlinked HTML (or alternatively PHP) pages that comes in the same package as the program files, see below. Much of the physics aspects are unchanged relative to the \textsc{Pythia}~6.4 manual \cite{pythiasixfour}, and so we refer to it and to other physics articles for that. Instead what we here give is an overview for potential users who already have some experience with event generators and want to understand how to get going with \textsc{Pythia}~8. Section \ref{sec:physics} contains an ultra-brief summary of the physics of \textsc{Pythia}~8, with particular emphasis on aspects that are different relative to \textsc{Pythia}~6. The program structure (including flow, files, documentation, and a few important warnings) is described in section \ref{sec:structure}; summaries of the main user methods, including the event record and particle classes, in section \ref{sec:main}. Section \ref{sec:databases} is concerned with the databases of flags, modes, parameters, processes, and particle data which exist in \textsc{Pythia}~8. Those who wish to link to external programs, e.g.\ to gain access to external parton distributions, standard input/output formats, and much more, will find the relevant information in section \ref{sec:external}. A brief how-to on getting going is then included in section \ref{sec:how-to}. Section \ref{sec:outlook} rounds off with an outlook. \section{Physics Summary \label{sec:physics}} This article is not intended to provide a complete description of the physics content. For this we primarily refer to the \textsc{Pythia}~6 manual \cite{pythiasixfour} and associated literature. We would like to draw attention to some key points of difference, however. Further details are available on the HTML/PHP pages in the program distribution. Some new physics aspects will eventually be covered in separate articles. The physics components are controlled by many parameters. These have been assigned sensible default values, based on previous experience with \textsc{Pythia}~6 and some first studies with the new code. We look forward to more extensive tunes by the experimental community, however. \subsection{Hard processes} Currently the program only works with $\mathrm{p}\mathrm{p}$, $\overline{\mathrm{p}}\mathrm{p}$, $\mathrm{e}^+\mathrm{e}^-$ and $\mu^+\mu^-$ incoming beams. In particular, there is no provision for $\mathrm{e}\mathrm{p}$ collisions or for incoming photon beams, neither on their own nor as flux around an electron. The list of processes currently implemented is summarised further down; it corresponds to most of the ones in \textsc{Pythia}~6, with the exception of the Supersymmetry and Technicolor sectors, which are yet to come. The cross-section expressions should be identical, but default scale choices have been changed, so that cross sections may be somewhat different for that reason. The default parton distribution remains CTEQ 5L, but ones found in the \textsc{LhaPdf} library \cite{lhapdf} can easily be linked. It is now possible to use separate PDF sets for the hard interaction, on one hand, and for the subsequent showers and multiple interactions, on the other. \subsection{Parton showers} The initial- and final-state algorithms are based on the new $p_{\perp}$-ordered evolution introduced in \textsc{Pythia}~6.3 \cite{ptshowers}, while the older mass-ordered ones have not been implemented. It is now additionally possible to have a branching of a photon to a fermion pair as part of the final-state evolution. Already in \textsc{Pythia}~6.3 the initial-state evolution and the multiple interactions were interleaved into one common decreasing $p_{\perp}$ sequence. Now also the final-state evolution is interleaved with the other two. In this context, some of that final-state radiation gets to be associated with dipoles stretched between a final-state parton and the ``hole'' left by an initial-state one, which therefore now can take a recoil. The initial-state-radiation algorithm remains unchanged in this respect, with recoils always taken by the hard scattering subsystem as a whole. \subsection{Multiple interactions and beam remnants} The multiple-interactions machinery as such contains the full functionality introduced in \textsc{Pythia}~6.3 \cite{newremnants}. Rescaled parton densities are defined after the first interaction, that take into account the nature of the previous partons extracted. Currently there is only one scenario for colour-reconnection in the final state, in which there is a certain probability for the partons of two subscatterings to have their colours interarranged in a way that reduces the total string length. (This is intermediate in character between the original strategy \cite{zijl} and the more recent ones \cite{wicke}.) The description of beam remnants is based on the new framework. In addition to the standard QCD $2 \to 2$ processes, the possibility of multiple interactions producing prompt photons, charmonia and bottomonia, low-mass Drell-Yan pairs, and $t$-channel $\gamma^*/\mathrm{Z}^0/\mathrm{W}^{\pm}$ exchange is now also included. For dedicated studies of two low-rate processes in coincidence, two hard interactions can now be set in the same event. There are no Sudakov factors included for these two interactions, similarly to normal events with one hard interaction. \subsection{Hadronisation} Hadronisation is based solely on the Lund string fragmentation framework \cite{lundreview}; older alternative descriptions have been left out. Particle data have been updated in agreement with the 2006 PDG tables \cite{pdg}. This also includes a changed content of the scalar meson multiplet. Some updated charm and bottom decay tables have been obtained from the DELPHI and LHCb collaborations. The BE$_{32}$ model for Bose--Einstein effects \cite{boseeinstein} has been implemented, but is not on by default. \subsection{Other program components} Standardised procedures have been introduced to link the program to various external programs for specific tasks, see section \ref{sec:external}. Finally, some of the old jet finders and other analysis routines are made available. Also included is a utility to generate, display and save simple one-dimensional histograms. \section{Program Structure \label{sec:structure}} \subsection{Program flow} The physics topics that have to come together in a complete event generator can crudely be subdivided into three stages: \begin{enumerate} \item The generation of a ``process'' that decides the nature of the event. Often it would be a ``hard process'', such as $\mathrm{g} \mathrm{g} \to \mathrm{h}^0 \to \mathrm{Z}^0 \mathrm{Z}^0 \to \mu^+ \mu^- \mathrm{q} \overline{\mathrm{q}}$, that is calculated in perturbation theory, but a priori we impose no requirement that a hard scale must be involved. Only a very small set of partons/particles is defined at this level, so only the main aspects of the event structure are covered. \item The generation of all subsequent activity on the partonic level, involving initial- and final-state radiation, multiple parton--parton interactions and the structure of beam remnants. Much of the phenomena are under an (approximate) perturbative control, but nonperturbative physics aspects are also important. At the end of this step, a realistic partonic structure has been obtained, e.g. with broadened jets and an underlying-event activity. \item The hadronisation of this parton configuration, by string fragmentation, followed by the decays of unstable particles. This part is almost completely nonperturbative, and so requires extensive modelling and tuning or, especially for decays, parametrisations of existing data. It is only at the end of this step that realistic events are available, as they could be observed by a detector. \end{enumerate} This division of tasks is not watertight --- parton distributions span and connect the two first steps, to give one example --- but it still helps to focus the discussion. \begin{figure}[t] \begin{picture}(430,370)(-215,10) \GBox(-215,350)(215,380){0.9} \Text(0,365)[]{The User ($\approx$ Main Program)} \GBox(-215,300)(215,330){0.9} \Text(0,315)[]{\texttt{Pythia}} \GBox(-215,250)(-170,280){0.9} \Text(-192.5,265)[]{\texttt{Info}} \GBox(-130,250)(-20,280){0.9} \Text(-75,265)[]{\texttt{Event~~process}} \GBox(20,250)(215,280){0.9} \Text(105,265)[]{\texttt{Event~~event}} \GBox(-215,110)(-85,230){0.9}\Line(-215,200)(-85,200) \Text(-150,215)[]{\texttt{ProcessLevel}} \Text(-150,185)[]{\texttt{ProcessContainer}} \Text(-150,165)[]{\texttt{PhaseSpace}} \Text(-150,145)[]{\texttt{LHAinit, LHAevnt}} \Text(-150,125)[]{\texttt{ResonanceDecays}} \GBox(-65,110)(65,230){0.9}\Line(-65,200)(65,200) \Text(0,215)[]{\texttt{PartonLevel}} \Text(0,185)[]{\texttt{TimeShower}} \Text(0,165)[]{\texttt{SpaceShower}} \Text(0,145)[]{\texttt{MultipleInteractions}} \Text(0,125)[]{\texttt{BeamRemnants}} \GBox(85,110)(215,230){0.9}\Line(85,200)(215,200) \Text(150,215)[]{\texttt{HadronLevel}} \Text(150,185)[]{\texttt{StringFragmentation}} \Text(150,165)[]{\texttt{MiniStringFrag\ldots}} \Text(150,145)[]{\texttt{ParticleDecays}} \Text(150,125)[]{\texttt{BoseEinstein}} \GBox(-130,60)(-20,90){0.9} \Text(-75,75)[]{\texttt{BeamParticle}} \GBox(20,60)(200,90){0.9} \Text(110,75)[]{\texttt{SigmaProcess, SigmaTotal}} \GBox(-215,10)(215,40){0.9} \Text(0,25)[]{\texttt{Vec4, Rndm, Hist, Settings, % ParticleDataTable, ResonanceWidths, \ldots}} \SetWidth{2} \LongArrow(0,350)(0,332) \LongArrow(-150,300)(-150,232) \LongArrow(0,300)(0,232) \Line(150,300)(150,280) \DashLine(150,280)(150,250){4} \LongArrow(150,250)(150,232) \SetWidth{1} \LongArrow(-192.5,230)(-192.5,248) \Line(-192.5,280)(-192.5,300) \DashLine(-192.5,300)(-192.5,330){4} \LongArrow(-192.5,330)(-192.5,348) \LongArrow(-107.5,230)(-107.5,248) \LongArrow(-42.5,250)(-42.5,232) \Line(-42.5,280)(-42.5,300) \DashLine(-42.5,300)(-42.5,330){4} \LongArrow(-42.5,330)(-42.5,348) \LongArrow(42.5,230)(42.5,248) \LongArrow(107.5,250)(107.5,232) \LongArrow(182.5,230)(182.5,248) \Line(182.5,280)(182.5,300) \DashLine(182.5,300)(182.5,330){4} \LongArrow(182.5,330)(182.5,348) \LongArrow(-107.5,100)(-107.5,108) \LongArrow(-107.5,100)(-107.5,92) \LongArrow(-42.5,100)(-42.5,108) \LongArrow(-42.5,100)(-42.5,92) \LongArrow(42.5,100)(42.5,108) \LongArrow(42.5,100)(42.5,92) \LongArrow(-160,50)(-160,108) \Line(-160,50)(0,50) \LongArrow(0,50)(19,59) \end{picture} \caption{The relationship between the main classes in \textsc{Pythia}~8. The thick arrows show the flow of commands to carry out different physics tasks, whereas the thinner show the flow of information between the tasks. The bottom box contains common utilities that may be used anywhere. Obviously the picture is strongly simplified. \label{fig:generatorstructure}} \hrulefill \end{figure} The structure of the \textsc{Pythia}~8 generator, as illustrated in Fig.~\ref{fig:generatorstructure}, is based on this subdivision. The main class for all user interaction is called \texttt{Pythia}. It calls on the three classes \texttt{ProcessLevel}, \texttt{PartonLevel} and \texttt{HadronLevel}, corresponding to points 1, 2 and 3 above. Each of these, in their turn, call on further classes that perform the separate kinds of physics tasks. Information is flowing between the different program elements in various ways, the most important being the event record, represented by the \texttt{Event} class. Actually, there are two objects of this class, one called \texttt{process}, that only covers the few partons of the ``hard'' process of point 1 above (i.e., containing information corresponding to what might be termed the ``matrix element'' level), and another called \texttt{event}, that covers the full story from the incoming beams to the final hadrons. A small \texttt{Info} class keeps track of useful one-of-a-kind information, such as kinematical variables of the hard process. There are also two incoming \texttt{BeamParticle}s, that keep track of the partonic content left in the beams after a number of interactions and initial-state radiations, and rescales parton distributions accordingly. The process library, as well as parametrisations of total, elastic and diffractive cross sections, are used both by the hard-process selection machinery and the multiple-interactions one. The \texttt{Settings} database keeps track of all integer, double, boolean and string variables that can be changed by the user to steer the performance of \textsc{Pythia}, except that \texttt{ParticleDataTable} is its own separate database. Finally, a number of utilities can be used just about anywhere, for Lorentz four-vectors, random numbers, jet finding and simple histograms, and for a number of other ``minor'' tasks. Orthogonally to the subdivision above, there is another, more technical classification, whereby the user interaction with the generator occurs in three phases: \begin{itemize} \item Initialisation, where the tasks to be performed are specified. \item Generation of individual events (the ``event loop''). \item Finishing, where final statistics is made available. \end{itemize} Again the subdivision (and orthogonality) is not strict, with many utilities and tasks stretching across the borders, and with no finishing step required for many aspects. Nevertheless, as a rule, these three phases are represented by different methods inside the class of a specific physics task. \subsection{Program files and documentation} The code is subdivided into a set of files, mainly by physics task. Each file typically contains one main class, but often with a few related helper classes that are not used elsewhere in the program. Normally the files come in pairs. \begin{enumerate} \item A header file, \texttt{.h} in the \texttt{include} subdirectory, where the public interface of the class is declared, and inline methods are defined. \item A source code file, \texttt{.cc} in the \texttt{src} subdirectory, where the lengthier methods are implemented. \end{enumerate} During compilation, related dependency files, \texttt{.d}, and compiled code, \texttt{.o} are created in the \texttt{tmp} subdirectory. In part the \texttt{.xml} documentation files in the \texttt{xmldoc} subdirectory have matching names, but the match is broken by the desire to group topics more by user interaction than internal operation. These files contain information on all settings and particle data, but not in a convenient-to-read format. Instead they are translated into a corresponding set of \texttt{.html} files in the \texttt{htmldoc} subdirectory and a set of \texttt{.php} files in \texttt{phpdoc}. The former set can easily be read if you open the \texttt{htmldoc/Welcome.html} file in your favourite web browser, but offers no interactivity. The latter set must be installed under a webserver (like a homepage) to function properly, and then provides a simple Graphical User Interface if you open the \texttt{phpdoc/Welcome.php} file in a web browser. For output to the \textsc{HepMC} event record format \cite{hepmc}, an interface is provided in the \texttt{hepmcinterface} subdirectory. There are also interfaces to allow parton distribution functions to be used from the \textsc{LhaPdf} library \cite{lhapdf} and hard processes from external programs. The installation procedure is described in a \texttt{README} file; it involves running a \texttt{configure} script, whereafter an ordinary \texttt{Makefile} is used. The former should be invoked with command-line arguments (or be edited) to provide the path to the \textsc{HepMC} library if this is going to be used. Compiled libraries are put in the \texttt{lib} subdirectory. Default is to build archive libraries, but optionally also shared-object ones can be built. The standard setup is intended for Linux systems, but a simplified alternative is provided for Windows users. Finally, some examples of main programs, along with input files, or ``cards'', for them, are found in the \texttt{examples} subdirectory. This directory contains its own \texttt{configure} script and \texttt{Makefile} which will allow you to build executables, see the \texttt{examples/README} file. As above, command-line arguments or brute-force editing allows you to set the \textsc{LhaPdf} and \textsc{Pythia}~6.4 paths, if so required. The executables are placed in the \texttt{bin} directory, but with links from \texttt{examples}. \subsection{Important warnings} Playing with the files in the \texttt{examples} subdirectory is encouraged, to familiarise oneself with the program. Modifying the \texttt{configure} files may be required during installation. For the rest, files should not be modified, at least not without careful consideration of consequences. In particular, the \texttt{.xml} files are set read-only, and should not be tampered with. Interspersed in them, there are lines beginning with \texttt{} containing a list of all the mothers, daughters or sisters of a particle. This list may be empty or arbitrarily large, and is given in ascending order. One data member in an Event object is used to keep track of the largest \texttt{col()} or \texttt{acol()} tag set so far, so that new ones do not clash. The event record also contains two further sets of vectors. These are intended for the expert user only, so only a few words on each. The first is a vector of junctions, i.e.\ vertices where three string pieces meet. This list is often empty or else contains only a very few per event. The second is a storage area for parton indices, classified by subsystem. Such information is needed to interleave multiple interactions, initial-state showers, final-state showers and beam remnants. It can also be used in the hadronisation. \subsection{Other event information} A set of one-of-a-kind pieces of event information is stored in the \texttt{info} object (an instance of the class \texttt{Info}) in the \texttt{Pythia} class. This is mainly intended for processes generated internally, but some of the information is also available for external processes. You can use \texttt{pythia.info.method()} to extract e.g.\ the following information: \begin{itemize} \item \texttt{list()} : list some information on the current event. \item \texttt{eCM(), s()} : the cm energy and its square. \item \texttt{name(), code()} : the name and code of the subprocess. \item \texttt{id1(), id2()} : the identities of the two partons coming in to the hard subprocess. \item \texttt{x1(), x2()} : $x$ fractions of the two partons coming in to the hard subprocess. \item \texttt{pdf1(), pdf2(), QFac(), Q2Fac()} : parton densities $x \, f_i(x,Q^2 )$ evaluated for the two incoming partons, and the associated factorisation scale $Q$ and its square. \item \texttt{mHat(), sHat(), tHat(), uHat()} : the invariant mass of the hard subprocess and the Mandelstam variables for $2 \to 2$ processes. \item \texttt{pTHat(), thetaHat()} : transverse momentum and polar scattering angle of the hard subprocess for $2 \to 2$ processes. \item \texttt{alphaS(), alphaEM(), QRen(), Q2Ren()} : $\alpha_{\mathrm{s}}$ and $\alpha_{\mathrm{em}}$ values for the hard process, and the associated renormalisation scale $Q$ and its square. \item \texttt{nTried(), nAccepted(), sigmaGen(), sigmaErr()} : the number of trial and accepted events, and the resulting estimated cross section and estimated statistical error, in units of mb, summed over the included processes. \end{itemize} In other classes there are also methods that can be called to do a sphericity or thrust analysis or search for jets with a clustering or simple cone jet finder. These take the event record as input. \section{Databases \label{sec:databases}} Inevitably one wants to be able to modify the default behaviour of a generator. Currently there are two \textsc{Pythia}~8 databases with modifiable values. One deals with general settings, the other specifically with particle data. The key method to set a new value is\\ \cindent \texttt{pythia.readString(string);}\\ The typical form of a string is\\ \cindent \texttt{"variable = value"}\\ where the equal sign is optional and the variable begins with a letter for settings and a digit for particle data. A string not beginning with either is considered as a comment and ignored. Therefore inserting an initial !, \#, \$, \%, or another such character, is a good way to comment out a command. For non-commented strings, the match of the name to the database is case-insensitive. Strings that do begin with a letter or digit and still are not recognised cause a warning to be issued, unless a second argument \texttt{false} is used in the call. Any further text after the value is ignored, so the rest of the string can be used for any comments. For variables with an allowed range, values below the minimum or above the maximum are set at the respective border. For \texttt{bool} values, the following notation may be used interchangeably: \texttt{true} = \texttt{on} = \texttt{yes} = \texttt{ok} = 1. Everything else gives \texttt{false} (including but not limited to \texttt{false}, \texttt{off}, \texttt{no} and \texttt{0}). The \texttt{readString(...)} method is convenient for changing one or two settings, but becomes cumbersome for more extensive modifications. In addition, a recompilation and relinking of the main program is necessary for any change of values. Alternatively, the changes can therefore be collected in a file, for historical reasons often called a ``card file'', where each line is a character string defined in the same manner as above (without quotation marks). The whole file can then be read and processed with a command\\ \cindent \texttt{pythia.readFile(fileName);}\\ As above, comments can be freely interspersed. \subsection{Settings} We distinguish four kinds of user-modifiable variables, by the way they have to be stored: \begin{enumerate} \item A \texttt{Flag} is an on/off switch, and is stored as a \texttt{bool}. \item A \texttt{Mode} corresponds to an enumeration of separate options, and is stored as an \texttt{int}. \item A \texttt{Parm} --- short for parameter --- takes a continuum of values, and is stored as a \texttt{double}. \item A \texttt{Word} is a text string (with no embedded blanks) and is stored as as a \texttt{string}. \end{enumerate} Collectively the four above kinds of variables are called settings. Not surprisingly, the class that stores them is called \texttt{Settings}. Each variable stored in \texttt{Settings} is associated with a few pieces of information. These are: \begin{itemize} \item The variable name, of the form \texttt{class:name} (or \texttt{file:name}, or \texttt{task:name}, usually these agree), e.g. \texttt{TimeShower:pTmin}. \item The default value, set in the original declaration, and intended to represent a reasonable choice. This value is not user modifiable. \item The current value. During construction of the \texttt{Settings} object, this value is set equal to the default value. It can subsequently be modified, e.g.\ by the \texttt{pythia.readString()} or \texttt{pythia.readFile()} methods discussed above. During the \texttt{pythia.init()} initialisation this value will be stored as a local copy in the class(es) where it is used, and thereby also control the subsequent generation. \item An allowed range of values, represented by meaningful minimum and maximum values. This has no sense for a flag or a word, is usually rather well-defined for a mode, but less so for a parameter. Either of the minimum and maximum may be left free, giving an open-ended range. Often the allowed range exaggerates the uncertainty in our current knowledge, so as not to restrict too much what the user can do. All the same, this information should not be modified by the user. \end{itemize} Technically, the \texttt{Settings} class is implemented with the help of four separate maps, one for each kind of variable, with the name used as key. The default values are taken from the \texttt{.xml} files in the \texttt{xmldoc} subdirectory. The \texttt{Settings} class is purely static, i.e.\ exists only as one global copy, that you can interact with directly by \texttt{Settings::command(argument)}. However, a \texttt{settings} object is a public member of the \texttt{Pythia} class, so an alternative notation would be \texttt{pythia.settings.command(argument)}. As already mentioned, for input the \texttt{pythia.readString(...)} method is to be preferred, since it also can handle particle data. A typical example would be\\ \cindent\texttt{pythia.readString("TimeShower:pTmin = 1.0");} You may obtain a listing of all variables in the database by calling\\ \cindent \texttt{pythia.settings.listAll();}\\ The listing is strictly alphabetical, which at least means that names in the same area are kept together, but otherwise may not be so well-structured: important and unimportant ones will appear mixed. A useful alternative is\\ \cindent \texttt{pythia.settings.listChanged();}\\ which will only print out a list of those variables that differ from their defaults. \subsection{Processes} All internal processes available in \textsc{Pythia}~8 can be switched on and off via the ordinary settings machinery just discussed, using flags of the generic type \texttt{ProcessGroup:ProcessName}. A complete list of processes currently implemented is given in Table~\ref{processes}. By default all processes are off. A whole group can be turned on by a \texttt{ProcessGroup:all = on} command, then overriding the individual flags. \begin{table} \caption{Currently implemented processes, complete with respect to groups, but with some individual processes missing for lack of space (represented by ``...''). In the names, a ``2'' separates initial and final state, an ``(s:X)'', ``(t:X)'' or ``(l:X)'' occasionally appends info on an $s$- or $t$-channel- or loop-exchanged particle $X$. \protect\label{processes}} \vspace{2mm} \texttt{ \begin{tabular}{|l|l|@{\protect\rule[-1mm]{0mm}{6mm}}} \hline ProcessGroup & ProcessName\\ \hline SoftQCD & minBias,elastic, singleDiffractive,\\ & doubleDiffractive\\ \hline HardQCD & gg2gg, gg2qqbar, qg2qg, qq2qq, qqbar2gg,\\ & qqbar2qqbarNew, gg2ccbar, qqbar2ccbar,\\ & gg2bbbar, qqbar2bbbar\\ \hline PromptPhoton & qg2qgamma, qqbar2ggamma, gg2ggamma,\\ & ffbar2gammagamma, gg2gammagamma\\ \hline WeakBosonExchange & ff2ff(t:gmZ), ff2ff(t:W)\\ \hline WeakSingleBoson & ffbar2gmZ, ffbar2W, ffbar2ffbar(s:gm)\\ \hline WeakDoubleBoson & ffbar2gmZgmZ, ffbar2ZW, ffbar2WW\\ \hline WeakBosonAndParton & qqbar2gmZg, qg2gmZq, ffbar2gmZgm, fgm2gmZf\\ & qqbar2Wg, qg2Wq, ffbar2Wgm, fgm2Wf\\ \hline Charmonium & gg2QQbar[3S1(1)]g, qg2QQbar[3PJ(8)]q, \ldots\\ \hline Bottomonium & gg2QQbar[3S1(1)]g, gg2QQbar[3P2(1)]g, \ldots\\ \hline Top & gg2ttbar, qqbar2ttbar, qq2tq(t:W), \\ & ffbar2ttbar(s:gmZ), ffbar2tqbar(s:W) \\ \hline \multicolumn{2}{|l|@{\protect\rule[-1mm]{0mm}{6mm}}}% {FourthBottom, FourthTop, FourthPair \textrm{(fourth generation)}} \\ \hline HiggsSM & ffbar2H, gg2H, ffbar2HZ, ff2Hff(t:WW), \ldots\\ \hline HiggsBSM & \textrm{h, H and A as above, charged Higgs, pairs}\\ \hline SUSY & qqbar2chi0chi0 \textrm{(not yet completed)}\\ \hline NewGaugeBoson & ffbar2gmZZprime, ffbar2Wprime, ffbar2R0\\ \hline LeftRightSymmmetry & ffbar2ZR, ffbar2WR, ffbar2HLHL, \ldots\\ \hline LeptoQuark & ql2LQ, qg2LQl, gg2LQLQbar, qqbar2LQLQbar\\ \hline ExcitedFermion & dg2dStar, qq2uStarq, qqbar2muStarmu, \ldots\\ \hline ExtraDimensionsG* & gg2G*, qqbar2G*, \ldots\\ \hline \end{tabular} } \end{table} Note that processes in the \texttt{SoftQCD} group are of a kind that cannot be input via the LHA, while essentially all other kinds could. Each process is assigned an integer code. This code is not used in the internal administration of events; it is only intended to allow a simpler user separation of different processes. Also the process name is available, as a string. For many processes it makes sense to apply phase space cuts. The ones currently available (in the \texttt{Settings} database) in particular include \begin{itemize} \item \texttt{PhaseSpace:mHatMin, PhaseSpace:mHatMax} : the range of invariant masses of the scattering process. \item \texttt{PhaseSpace:pTHatMin, PhaseSpace:pTHatMax} : the range of transverse momenta in the rest frame of the process for $2 \to 2$ and $2 \to 3$ processes (for each of the products). \end{itemize} In addition, for any resonance with a Breit-Wigner mass distribution, the allowed mass range of that particle species is taken into account, both for $2 \to 1$, $2 \to 2$ and $2 \to 3$ processes, thereby providing a further cut possibility. Note that the \texttt{SoftQCD} processes do not use any cuts but generate their respective cross sections in full. \subsection{Particle data} The following particle properties are stored in the \texttt{ParticleDataTable} class for a given PDG particle identity code \texttt{id}, here presented by the method used to access this property: \begin{itemize} \item \texttt{name(id)} : particle and antiparticle names are stored separately, the sign of \texttt{id} determines which of the two is returned, with ``void'' used to indicate the absence of an antiparticle. \item \texttt{hasAnti(id)} : \texttt{bool} whether a distinct antiparticle exists or not. \item \texttt{spinType(id)} : $2 s + 1$ for particles with defined spin, else 0. \item \texttt{chargeType(id)} : three times the charge (to make it an integer); can also be read as a \texttt{double charge(id) = chargeType(id)/3}. \item \texttt{colType(id)} : the colour type, with 0 uncoloured, 1 triplet, $-1$ antitriplet and 2 octet. \item \texttt{m0(id)} : the nominal mass $m_0$ (in GeV). \item \texttt{mWidth(id)} : the width $\Gamma$ of the Breit-Wigner mass distribution (in GeV). \item \texttt{mMin(id), mMax(id)} : the allowed mass range generated by the Breit-Wigner, $m_{\mathrm{min}} < m < m_{\mathrm{max}}$ (in GeV). \item \texttt{tau0(id)} : the nominal proper lifetime $\tau_0$ (in mm/$c$). \item \texttt{constituentMass(id)} : the constituent mass for a quark, hardcoded as $m_{\mathrm{u}} = m_{\mathrm{d}} = 0.325$, $m_{\mathrm{s}} = 0.50$, $m_{\mathrm{c}} = 1.60$ and $m_{\mathrm{b}} = 5.0$ GeV, for a diquark the sum of quark constituent masses, and for everything else the same as the ordinary mass. \item \texttt{mRun(id, massScale)} : the running mass for quarks, else the same as the nominal mass. \item \texttt{mayDecay(id)} : a flag telling whether a particle species may decay or not, offering the main user switch (whether a given particle of this kind then actually will decay also depends on other flags in the \texttt{ParticleDecays} class). \end{itemize} Similar methods can also be used to set most of these properties. Each particle kind in the \texttt{ParticleDataTable} also has a a vector of \texttt{DecayChannel}s associated with it. The following properties are stored for each decay channel: \begin{itemize} \item \texttt{onMode()} : whether a channel is on (1) or off (0), or on only for particles (2) or antiparticles (3). \item \texttt{bRatio()} : the branching ratio. \item \texttt{meMode()} : the mode of processing this channel, possibly with matrix-element information; 0 gives isotropic phase space. \item \texttt{multiplicity()} : the number of decay products in a channel, at most 8. \item \texttt{product(i)} : a list of the decay products, 8 products $0 \leq $\texttt{i}$ < 8$, with trailing unused ones set to 0. \end{itemize} The original particle data and decay table is read in from the \texttt{ParticleData.xml} file. The \texttt{ParticleDataTable} class is purely static, i.e. exists as one global copy, that you can interact directly with by \texttt{ParticleDataTable::command(argument)}. However, a \texttt{particleData} object of the \texttt{ParticleDataTable} class is a public member of the \texttt{Pythia} class, which offers an alternatively notation. As already mentioned, for input the \texttt{pythia.readString(string)} method is to be preferred, since it also can handle settings. It is only the form of the \texttt{string} that needs to be specified slightly differently than for settings, as\\ \cindent \texttt{id:property = value}.\\ The \texttt{id} part is the standard PDG particle code, i.e.\ a number, and \texttt{property} is one of the ones already described above, with a few minor differences: \texttt{name}, \texttt{antiName}, \texttt{spinType}, \texttt{chargeType}, \texttt{colType}, \texttt{m0}, \texttt{mWidth}, \texttt{mMin}, \texttt{mMax}, \texttt{tau0}, \texttt{mayDecay}, \texttt{isResonance}, \texttt{isVisible}, \texttt{doExternalDecay}, and \texttt{doForceWidth}. As before, several commands can be stored as separate lines in a file, say\\ \cindent \texttt{111:name = piZero ! normal notation pi0}\\ \cindent \texttt{3122:mayDecay = false ! Lambda0 stable}\\ \cindent \texttt{431:tau0 = 0.15 ! D\_s proper lifetime}\\ and then be read with \texttt{pythia.readFile(fileName)}. For major changes of the properties of a particle, the above one-at-a-time changes can become rather cumbersome. Therefore a few extended input formats are available, where a whole set of properties can be given after the equal sign, separated by blanks and/or by commas. One line like\\ \cindent \texttt{id:all = name antiName spinType chargeType % colType m0 mWidth mMin mMax tau0}\\ replaces all the current information on the particle itself, but keeps its decay channels, if any, while using \texttt{new} instead of \texttt{all} also removes any previous decay channels. (The flags \texttt{mayDecay}, \texttt{isResonance}, \texttt{isVisible}, \texttt{doExternalDecay}, and \texttt{doForceWidth} are in either case reset to their defaults and would have to be changed separately.) In order to change the decay data, the decay channel number needs to be given right after the particle number, i.e. the command form becomes\\ \cindent \texttt{id:channel:property = value}.\\ Recognised properties are \texttt{onMode}, \texttt{bRatio}, \texttt{meMode} and \texttt{products}, where the latter expects a list of all the decay products, separated by blanks, up until the end of the line, or until a non-number is encountered. The property \texttt{all} will replace all the information on the channel, i.e.\\ \cindent \texttt{id:channel:all = onMode bRatio meMode products }\\ To add a new channel at the end, use\\ \cindent \texttt{id:addChannel = onMode bRatio meMode products } \\ To remove all existing channels and force decays into one new channel, use\\ \cindent \texttt{id:oneChannel = onMode bRatio meMode products } \\ A first \texttt{oneChannel} command could be followed by several subsequent \texttt{addChannel} ones, to build up a completely new decay table for an existing particle.\\ It is currently not possible to remove a channel selectively, but setting its branching ratio vanishing is as effective. Often one may want to allow only a specific subset of decay channels for a particle. This can be achieved e.g.\ by a repeated use of \texttt{id:channel:onMode} commands, but there also is a set of commands that initiates a loop over all decay channels and allows a matching to be carried out. The \texttt{id:onMode} command can switch \texttt{on} or \texttt{off} all channels. The \texttt{id:onIfAny} and \texttt{id:offIfAny} will switch on/off all channels that contain any of the enumerated particles. For instance\\ \cindent \texttt{23:onMode = off}\\ \cindent \texttt{23:onIfAny = 1 2 3 4 5}\\ first switches off all $\mathrm{Z}^0$ decay modes and then switches back on any that contains one of the five lighter quarks. Other methods are \texttt{id:onIfAll} and \texttt{id:offIfAll}, and \texttt{id:onIfMatch} and \texttt{id:offIfMatch}, where all the enumerated products must be present for a decay channel to be switched on/off. The difference is that the former two allow further non-matched particles in a decay channel while the latter two do not. There are also further methods to switch on channels selectively either for the particle or for the antiparticle. When a particle is to be decayed, the branching ratios of the allowed channels are always rescaled to unit sum. There are also methods for by-hand rescaling of branching ratios. You may obtain a listing of all the particle data by calling\\ \cindent \texttt{pythia.particleData.listAll()}.\\ The listing is by increasing \texttt{id} number. To list only those particles that have been changed, instead use\\ \cindent \texttt{pythia.particleData.listChanged()}.\\ To list only one specific particle \texttt{id}, use \texttt{list(id)}. It is also possible to \texttt{list} a \texttt{vector} of \texttt{id}'s. \section{Links to external programs \label{sec:external}} While \textsc{Pythia}~8 itself is self-contained and can be run without reference to any external library, often one does want to make use of other programs that are specialised on some aspect of the generation process. The HTML/PHP documentation accompanying the code contains full information on how the different links should be set up. Here the purpose is mainly to point out the possibilities that exist. \subsection{The Les Houches interface} The Les Houches Accord for user processes (LHA) \cite{lha} is the standard way to input parton-level information from a matrix-elements-based generator into \textsc{Pythia}. The conventions for which information should be stored has been defined in a Fortran context, as two commonblocks. Here a C++ equivalent is defined, as two separate classes. The \texttt{LHAinit} and \texttt{LHAevnt} classes are base classes, containing reading and printout methods, plus a pure virtual method \texttt{set()} each. Derived classes have to provide these two virtual methods to do the actual work. Currently the only examples are for reading information at runtime from the respective Fortran commonblock or for reading it from a Les Houches Event File (LHEF) \cite{lhef}. The \texttt{LHAinit} class stores information equivalent to the \texttt{/HEPRUP/} commonblock, as required to initialise the event-generation chain. The \texttt{LHAevnt} class stores information equivalent to the \texttt{/HEPEUP/} commonblock, as required to hand in the next parton-level configuration for complete event generation. The \texttt{LHAinitFortran} and \texttt{LHAevntFortran} are two derived classes, containing \texttt{set()} members that read the respective LHA Fortran commonblock for initialisation and event information. This can be used for a runtime link to a Fortran library. As an example, an interface is provided to the \textsc{Pythia}~6.4 process library. The \texttt{LHAinitLHEF} and \texttt{LHAevntLHEF} are two other derived classes, that can read a file with initialisation and event information, assuming that the file has been written in the LHEF format. You do not need to declare these classes yourself, since a shortcut is provided by the \texttt{pythia.init(fileName)} command. If you create \texttt{LHAinit} and \texttt{LHAevnt} objects yourself, pointers to those should be handed in with the \texttt{init(...)} call, then of the form \texttt{pythia.init(LHAinit*, LHAevnt*)}. \subsection{Semi-internal processes and resonances} When you implement new processes via the Les Houches Accord you do all flavour, colour and phase-space selection externally, before your process-level events are input for further processing by \textsc{Pythia}. However, it is also possible to implement a new process in exactly the same way as the internal \textsc{Pythia} ones, thus making use of the internal phase-space selection machinery to sample an externally provided cross-section expression. The matrix-element information has to be put in a new class that derives from one of the existing classes, \texttt{Sigma1Process} for $2 \to 1$ processes, \texttt{Sigma2Process} for $2 \to 2$ ones, and \texttt{Sigma3Process} for $2 \to 3$ ones, which in their turn derive from the \texttt{SigmaProcess} base class. Note that \texttt{Pythia} is rather good at handling the phase space of $2 \to 1$ and $2 \to 2$ processes, is more primitive for $2 \to 3$ ones and does not at all address higher multiplicities. This limits the set of processes that you can implement in this framework. The produced particles may be resonances, however, so it is possible to end up with bigger "final" multiplicities through sequential decays, and to include further matrix-element weighting in those decays. In your new class you have to implement a number of methods. Chief among them is one to return the matrix-element weight for an already specified kinematics configuration and another one to set up the final-state flavours and colour flow of the process. Further methods exist, some of more informative character, such as providing the name of the process. Should you actually go ahead, it is strongly recommended to shop around for a similar process that has already been implemented, and to use that existing code as a template. Once a class has been written, a pointer of type \texttt{SigmaProcess*} to a \texttt{new} instance of your class needs to be created in the main program, and handed in with the \texttt{pythia.setSigmaPtr(...)} method. {}From there on the process will be handled on equal footing with internally implemented processes. If your new process introduces a new particle you have to add it and its decay channels to the particle database, as already explained. This only allows for a fixed width and fixed branching ratios, however, with only some minor generalisations. To obtain a dynamical calculation, where the width and the branching ratios can vary as a function of the currently chosen mass, you must also create a new class for it that derives from the \texttt{ResonanceWidths} class. In it you have to implement a method that returns the partial width for each of the possible decay channels. The structure is simpler than for the \texttt{SigmaProcess} case, but again it may be convenient to use a similar existing resonance as a template. You then hand in a pointer to an instance of this new class with the \texttt{pythia.setResonancePtr(...)} method. \subsection{Parton distribution functions} The \texttt{PDF} class is the base class for all parton distribution function parametrisations, from which specific \texttt{PDF} classes are derived. Currently the selection of sets that comes with the program is very limited; for protons only CTEQ 5L (default) and GRV 94L are available. However, a built-in interface to the \textsc{LhaPdf} library \cite{lhapdf} allows a much broader selection, if only \textsc{LhaPdf} is linked together with \textsc{Pythia}. Should this not be enough, it is possible to write your own class derived from the \texttt{PDF} base class, wherein you implement the \texttt{xfUpdate(...)} member to do the actual updating of PDFs. Once you have created two distinct \texttt{PDF} objects, \texttt{pdfA} and \texttt{pdfB}, you should supply pointers to these as arguments in a \texttt{pythia.setPDFPtr(pdfA*, pdfB*)} call. A word of warning: to switch to a new PDF set implies that a complete retuning of the generator may be required, since the underlying-event activity from multiple interactions and parton showers is changed. There is an option that allows a replacement of the PDF for the hard process only, so that this is not required. Inconsistent but convenient. \subsection{External decay packages} While \texttt{Pythia} is set up to handle any particle decays, decay products are often (but not always) distributed isotropically in phase space, i.e.\ polarisation effects and nontrivial matrix elements usually are neglected in \textsc{Pythia}. Especially for the $\tau$ lepton and for some $\mathrm{B}$ mesons it is therefore common practice to rely on dedicated decay packages \cite{tauola, evtgen}. To this end, \texttt{DecayHandler} is a base class for the external handling of decays. The user-written derived class is called if a pointer to it has been given with the \texttt{pythia.setDecayPtr(DecayHandler*, vector)} method. The second argument to this method should contain the \texttt{id} codes of all the particles that should be decayed by the external program. It is up to the author of the derived class to send different of these particles on to separate packages, if so desired. The \texttt{decay(...)} method in the user-written \texttt{DecayHandler} class should do the decay, or return \texttt{false} if it fails. In the latter case \texttt{Pythia} will try to do the decay itself. Thus one may implement some decay channels externally and leave the rest for \texttt{Pythia}, assuming the \texttt{Pythia} decay tables are adjusted accordingly. \subsection{User hooks} Sometimes it may be convenient to step in during the generation process: to modify the built-in cross sections, to veto undesirable events or simply to collect statistics at various stages of the evolution. There is a base class \texttt{UserHooks} that gives you this access at a few selected places. This class in itself does nothing; the idea is that you should write your own derived class for your task. A few very simple derived classes come with the program, mainly as illustration. There are four distinct sets of routines. Ordered by increasing complexity, rather than by their appearance in the event-generation sequence, they are: \begin{itemize} \item Ones that gives you access to the event record in between the process-level and parton-level steps, or in between the parton-level and hadron-level ones. You can study the event record and decide whether to veto this event. \item Ones that allow you to set a scale at which the combined multiple-interactions, initial-state and final-state parton-shower downwards evolution in $p_{\perp}$ is temporarily interrupted, so the event can be studied and either vetoed or allowed to continue the evolution. \item Similar ones that instead gives you access after the first few parton-shower branchings of the hardest subprocess. \item Ones that gives you access to the properties of the trial hard process, so that you can modify the internal \textsc{Pythia} cross section by your own correction factors. \end{itemize} \subsection{Random-number generators} \texttt{RndmEngine} is a base class for the external handling of random-number generation. The user-written derived class is called if a pointer to it has been handed in with the \texttt{pythia.setRndmEnginePtr(RndmEngine*)} method. Since the default Marsaglia-Zaman algorithm is quite good, there is absolutely no physics reason to replace it, but this may still be required for consistency with other program elements in big experimental frameworks. \subsection{The \textsc{HepMC} event format} The \textsc{HepMC} event format \cite{hepmc} is a standard format for the storage of events in several major experiments. The translation from the \textsc{Pythia}~8 \texttt{Event} format should be done after \texttt{pythia.next()} has generated an event. Therefore there is no need for a tight linkage, but only to call the\\ \texttt{HepMC::I\_Pythia8::fill\_next\_event( pythia.event, hepmcevt )}\\ conversion routine from the main program written by the user. Version 1 of \textsc{HepMC} makes use of the \textsc{CLHep} library \cite{clhep} for four-vectors, while version 2 is standalone; this requires some adjustments in the interface code based on which version is used. \subsection{SUSY parameter input} \textsc{Pythia}~8 does not contain a machinery for calculating masses and couplings of supersymmetric particles from some small set of input parameters. Instead the SUSY Les Houches Accord (SLHA) \cite{slha} is used to provide this information, as calculated by some external program. You need to supply the name of the file where the SLHA information is stored, in an appropriate setting, and then the rest is taken care of automatically. (Or at least will be, once SUSY processes are implemented.) \subsection{Parton showers} It is possible to replace the existing timelike and/or spacelike showers in the program by your own. This is truly for experts, since it requires a rather strict adherence to a wide set of rules. These are described in detail in the HTML/PHP documentation accompanying the code. The \textsc{Vincia} program \cite{vincia} offers a first example of a plug-in of an external (timelike) shower. \section{Getting Going \label{sec:how-to}} After you download the \texttt{pythia8100.tgz} (or later) package from the \textsc{Pythia} webpage,\\ \cindent \texttt{http://www.thep.lu.se/}$\sim$% \texttt{torbjorn/Pythia.html}\\ you can unpack it with \texttt{tar xvfz pythia8100.tgz}, into a new subdirectory \texttt{pythia8100}. The rest of the installation procedure is described in the \texttt{README} file in that directory. It is assumed you are on a Linux system; so far there is hardly any multiplatform support. After this, the main program is up to the user to write. A worksheet (found on the webpage) takes you through as step-by-step procedure, and sample main programs are provided in the \texttt{examples} subdirectory. These programs are included to serve as inspiration when starting to write your own program, by illustrating the principles involved. The information available if you open \texttt{htmldoc/Welcome.html} in your web browser will help you explore the program possibilities further. If you install the \texttt{phpdoc} subdirectory under a web server you will also get extra help to build a file of commands to the \texttt{Settings} and \texttt{ParticleDataTable} machineries, to steer the execution of your main program. Such "cards files" are separate from the main programs proper, so that minor changes can be made without any recompilation. It is then convenient to collect in the same place some run parameters, such as the number of events to generate, that could be used inside the main program. Therefore some such have been predefined, e.g.\ \texttt{Main:numberOfEvents}. Whether they actually are used is up to the author of a main program to decide. \section{Outlook \label{sec:outlook}} As already explained in the introduction, \textsc{Pythia}~8.1 is not yet a complete replacement of \textsc{Pythia}~6.4, but it is getting there, and already contains some new features not found elsewhere. In many cases the quality of the physics should be comparable between the two versions, but obviously the objective is that soon \textsc{Pythia}~8 should offer the overall better alternative. This will occur by further improvements of the existing framework and by the gradual addition of new features. \ack The support and kind hospitality of the SFT group at CERN is gratefully acknowledged by TS. Mikhail Kirsanov has developed the configure files, the makefiles and the interface to \textsc{HepMC}, and made several valuable suggestions. Ben Lloyd has written the PHP webpage framework. Bertrand Bellenot has provided a simple makefile for Win32/NMAKE. Marc Montull has helped write the extended Higgs sector. SM and PS are supported by Fermi Research Alliance, LLC, under Contract No.~DE-AC02-07CH11359 with the United States Department of Energy. This work was supported in part by the European Union Marie Curie Research Training Network MCnet under contract MRTN-CT-2006-035606. \begin{thebibliography}{99} \bibitem{jetset} T. Sj\"ostrand, Computer Physics Commun. {\bf 27} (1982) 243, {\bf 28} (1983) 229, {\bf 39} (1986) 347;\\ T. Sj\"ostrand and M. Bengtsson, Computer Physics Commun. {\bf 43} (1987) 367 \bibitem{pythiaearly} H.-U. Bengtsson, Computer Physics Commun. {\bf 31} (1984) 323;\\ H.-U. Bengtsson and G. Ingelman, Computer Physics Commun. {\bf 34} (1985) 251;\\ H.-U. Bengtsson and T. Sj\"ostrand, Computer Physics Commun. {\bf 46} (1987) 43;\\ T. Sj\"ostrand, Computer Physics Commun. {\bf 82} (1994) 74 \bibitem{pythiasixone} T. Sj\"ostrand, P. Ed\'en, C. Friberg, L. L\"onnblad, G. Miu, S. Mrenna and E. Norrbin, Computer Physics Commun. {\bf 135} (2001) 238 \bibitem{pythiasixfour} T. Sj\"ostrand, S. Mrenna and P. Skands, JHEP {\bf 05} (2006) 026 [hep-ph/0603175] \bibitem{pythiaseven} L. L\"onnblad, Computer Physics Commun. {\bf 118} (1999) 213;\\ M. Bertini, L. L\"onnblad and T. Sj\"ostrand, Computer Physics Commun. {\bf 134} (2001) 365 \bibitem{thepeg} see webpage \texttt{http://www.thep.lu.se/ThePEG/} \bibitem{herwigpp} S. Gieseke, A. Ribon, M.H. Seymour, P. Stephens and B.R. Webber, JHEP {\bf 02} (2004) 005;\\ see webpage \texttt{http://hepforge.cedar.ac.uk/herwig/} \bibitem{lha} E. Boos et al., in the Proceedings of the Workshop on Physics at TeV Colliders,\\ Les Houches, France, 21 May - 1 Jun 2001 [hep-ph/0109068] \bibitem{lhef} J. Alwall et al., Computer Physics Comm. {\bf 176} (2007) 300 \bibitem{lhapdf} M.R. Whalley, D. Bourilkov and R.C. Group, in `HERA and the LHC',\\ eds. A. De Roeck and H. Jung, CERN-2005-014, p. 575 [hep-ph/0508110] \bibitem{ptshowers} T. Sj\"ostrand and P. Skands, Eur. Phys. J {\bf C39} (2005) 129 \bibitem{newremnants} T. Sj\"ostrand and P. Skands, JHEP {\bf 03} (2004) 053 \bibitem{zijl} T. Sj\"ostrand and M. van Zijl, Phys. Rev. {\bf D36} (1987) 2019 \bibitem{wicke} P. Skands and D. Wicke, Eur. Phys. J. {\bf C52} (2007) 133 \bibitem{lundreview} B. Andersson, G. Gustafson, G. Ingelman and T. Sj\"ostrand, Phys. Rep. {\bf 97} (1983) 31 \bibitem{pdg} Particle Data Group, W.-M. Yao et al., J. Phys. {\bf G33} (2006) 1 \bibitem{boseeinstein} L. L\"onnblad and T. Sj\"ostrand, Eur. Phys. J. {\bf C2} (1998) 165 \bibitem{hepmc} M. Dobbs and J.B. Hansen, Computer Physics Comm. {\bf 134} (2001) 41 \bibitem{slha} P. Skands et al., JHEP {\bf 07} (2004) 036 \bibitem{tauola} S. Jadach, Z. W\c{a}s, R. Decker and J.H. K\"uhn, Computer Physics Commun. {\bf 76} (1993) 361 \bibitem{evtgen} D.J. Lange, Nucl. Instrum. Meth. {\bf A462} (2001) 152 \bibitem{clhep} see webpage \texttt{http://proj-clhep.web.cern.ch/proj-clhep/} \bibitem{vincia} W.T. Giele, D.A. Kosower and P.Z. Skands, arXiv:0707.3652 \end{thebibliography} \end{document} pythia8-8.1.80.orig/xmldoc/ResonanceDecays.xml0000444000175000017500000004330512217346317017420 0ustar sunsun

    Resonance Decays

    The ResonanceDecays class performs the sequential decays of all resonances formed in the hard process. Note the important distinction between "resonances" and other "particles" made in PYTHIA.
    • The list of resonances contains gamma^*/Z^0, W^+-, top, the Higgs, and essentially all new particles of Beyond-the-Standard-Model physics: further Higgs bosons, sfermions, gauginos, techniparticles, and so on. The partial widths to different decay channels are perturbatively calculable, given the parameters of the respective model, and branching ratios may be allowed to vary across a (reasonably broad) resonance peak. Usually resonances are short-lived, and therefore it makes sense to consider their decays immediately after the primary hard process has been set up. Furthermore, in several cases the decay angular distributions are encoded as part of the specific process, e.g. the W decays differently in f fbar -> W^+-, f fbar -> W^+ W^- and h^0 -> W^+ W^- . All of these particles are (in PYTHIA) only produced as part of the hard process itself, i.e. they are not produced in showers or hadronization processes. Therefore the restriction to specific decay channels can be consistently taken into account as a corresponding reduction in the cross section of a process. Finally, note that all of these resonances have an on-shell mass above 20 GeV, with the exception of some hypothetical weakly interacting and stable particles such as the gravitino.
    • The other particles include normal hadrons and the Standard-Model leptons, including the tau^+-. These can be produced in the normal hadronization and decay description, which involve unknown nonperturbative parameters and multistep chains that cannot be predicted beforehand: a hard process like g g -> g g can develop a shower with a g -> b bbar branching, where the b hadronizes to a B^0bar that oscillates to a B^0 that decays to a tau^+. Therefore any change of branching ratios - most of which are determined from data rather than from first principles anyway - will not be taken into account in the cross section of a process. Exceptions exist, but most particles in this class are made to decay isotropically. Finally, note that all of these particles have a mass below 20 GeV.
    There is one ambiguous case in this classification, namely the photon. The gamma^*/Z^0 combination contains a low-mass peak when produced in a hard process. On the other hand, photons can participate in shower evolution, and therefore a photon originally assumed massless can be assigned an arbitrarily high mass when it is allowed to branch into a fermion pair. In some cases this could lead to double-counting, e.g. between processes such as f fbar -> (gamma^*/Z^0) (gamma^*/Z^0), f fbar -> (gamma^*/Z^0) gamma and f fbar -> gamma gamma. Here it make sense to limit the lower mass allowed for the gamma^*/Z^0 combination, in 23:mMin, to be the same as the upper limit allowed for an off-shell photon in the shower evolution, in TimeShower:mMaxGamma. By default this matching is done at 10 GeV.

    In spite of the above-mentioned differences, the resonances and the other particles are all stored in one common particle data table, so as to offer a uniform interface to setting and getting properties such as name, mass, charge and decay modes, also for the particle properties in the event record. Some methods are specific to resonances, however, in particular for the calculation of partial widths and thereby of branching ratio. For resonances these can be calculated dynamically, set up at initialization for the nominal mass and then updated to the current mass when these are picked according to a Breit-Wigner resonance shape.

    Resonance Decays and Cross Sections

    As already hinted above, you have the possibility to set the allowed decay channels of resonances, see Particle Data Scheme description. For instance, if you study the process q qbar -> H^0 Z^0 you could specify that the Z^0 should decay only to lepton pairs, the H^0 only to W^+ W^-, the W^+ only to a muon and a neutrino, while the W^- can decay to anything. Unfortunately there are limits to the flexibility: you cannot set a resonance to have different properties in different places of a process, e.g. if instead H^0 -> Z^0 Z^0 in the above process then the three Z^0's would all obey the same rules.

    The restrictions on the allowed final states of a process is directly reflected in the cross section of it. That is, if some final states are excluded then the cross section is reduced accordingly. Such restrictions are built up recursively in cases of sequential decay chains. The restrictions are also reflected in the compositions of those events that actually do get to be generated. For instance, the relative rates of H^0 -> W^+ W^- and H^0 -> Z^0 Z^0 are shifted when the allowed sets of W^+- and Z^0 decay channels are changed.

    We remind that only those particles that Pythia treat as resonances enjoy this property, and only those that are considered as part of the hard process and its associated resonance decays.

    There is one key restriction on resonances: Minimal allowed width of a resonance, in GeV. If the width falls below this number the resonance is considered stable and will not be allowed to decay. This is mainly intended as a technical parameter, to avoid disasters in cases where no open decay channels exists at all. It could be used for real-life decisions as well, however, but then typically would have to be much bigger than the default value. Special caution would be needed if coloured resonance particles were made stable, since the program would not necessarily know how to hadronize them, and therefore fail at that stage.

    In spite of this technical parameter choice, it is possible to set a lifetime for a resonance, and thereby to obtain displaced vertices. If a resonance is allowed to decay it will do so, irrespective of the location of the decay vertex. This is unlike normal particle decays, where it is possible to define some region around the primary vertex within which all decays should happen, with particles leaving that region considered stable. The logic is that resonances as a rule are too short-lived for secondary vertices, so if you pick a scenario with a long-lived but unstable resonance it is because you want to study secondary vertices. How to interface those decays to a detector simulation program then is another story, to be solved separately. Do note that a special treatment is needed for coloured long-lived resonances, that form R-hadrons, and where charge and flavour may change between the production and decay vertices.

    Special properties and methods for resonances

    The method ParticleData::isResonance(id) allows you to query whether a given particle species is considered a resonance or not. You can also change the default value of this flag in the normal way, e.g. pythia.readString("id:isResonance = true").

    An option with a forced width can be set with the id:doForceWidth flag as above, and queried with ParticleData::doForceWidth(id). It is by default off, and should normally so remain. If switched on then the width stored in id:mWidth is strictly used to describe the Breit-Wigner of the resonance. This is unlike the normal behaviour of standard resonances such as the Z^0, W^+-, t or h^0, which have explicit decay-widths formulae encoded, in classes derived from the ResonanceWidths base class. These formulae are used, e.g., to derive all the Higgs partial widths as a function of the Higgs mass you choose, and at initialization overwrites the existing total width value. The reason for forcing the width to another value specified by you would normally more have to do with experimental issues than with physics ones, e.g. how sensitive your detector would be to changes in the Higgs width by a factor of two. A warning is that such a rescaling could modify the cross section of a process correspondingly for some processes, while leaving it (essentially) unchanged for others (as would seem most logical), depending on how these were encoded. A further warning is that, if you use this facility for Z^0 or Z'^0 with gamma^*/Z^0 or gamma^*/Z^0/Z'^0 interference on, then also the handling of this interference is questionable. So, if you need to use the width-rescaling option, be extremely cautious.

    If a resonance does not have a class of its own, with hardcoded equations for all relevant partial widths, then a simpler object will be created at initialization. This object will take the total width and branching ratios as is (with the optional variations explained in the next section), and thus the rescaling approach brings no further freedom.

    Mainly for internal usage, the ParticleData contain some special methods that are only meaningful for resonances:

    • resInit(...) to initialize a resonance, possibly including a recalculation of the nominal width to match the nominal mass;
    • resWidth(...) to calculate the partial and total widths at the currently selected mass;
    • resWidthOpen(...) to calculate the partial and total widths of those channels left open by user switches, at the currently selected mass;
    • resWidthStore(...) to calculate the partial and total widths of those channels left open by user switches, at the currently selected mass, and store those as input for a subsequent selection of decay channel;
    • resOpenFrac(...) to return the fraction of the total width that is open by the decay channel selection made by users (based on the choice of onMode for the various decay channels, recursively calculated for sequential decays);
    • resWidthRescaleFactor(...) returns the factor by which the internally calculated PYTHIA width has to be rescaled to give the user-enforced width;
    • resWidthChan(...) to return the width for one particular channel (currently only used for Higgs decays, to obtain instate coupling from outstate width).
    These methods actually provide an interface to the classes derived from the ResonanceWidths base class, to describe various resonances.

    Modes for Matrix Element Processing

    The meMode() value for a decay mode is used to specify nonisotropic decays or the conversion of a parton list into a set of hadrons in some channels of normal particles. For resonances it can also take a third function, namely to describe how the branching ratios and widths of a resonance should be rescaled as a function of the current mass of the decaying resonance. The rules are especially useful when new channels are added to an existing particle, or a completely new resonance added.
    • 0 : channels for which hardcoded partial-width expressions are expected to exist in the derived class of the respective resonance. Should no such code exist then the partial width defaults to zero.
    • 1 - 99 : same as 0, but normally not used for resonances.
    • 100 : calculate the partial width of the channel from its stored branching ratio times the stored total width. This value remains unchanged when the resonance fluctuates in mass. Specifically there are no threshold corrections. That is, if the resonance fluctuates down in mass, to below the nominal threshold, it is assumed that one of the daughters could also fluctuate down to keep the channel open. (If not, there may be problems later on.)
    • 101 : calculate the partial width of the channel from its stored branching ratio times the stored total width. Multiply by a step threshold, i.e. the channel is switched off when the sum of the daughter on-shell masses is above the current mother mass.
    • 102 : calculate the partial width of the channel from its stored branching ratio times the stored total width. Multiply by a smooth threshold factor beta = sqrt( (1 - m_1^2/m_2 - m_2^2/m^2)^2 - 4 m_1^2 m_2^2/m^4) for two-body decays and sqrt(1 - Sum_i m_i / m) for multibody ones. The former correctly encodes the size of the phase space but misses out on any nontrivial matrix-element behaviour, while the latter obviously is a very crude simplification of the correct phase-space expression. Specifically, it is thereby assumed that the stored branching ratio and total width did not take into account such a factor.
    • 103 : use the same kind of behaviour and threshold factor as for 102 above, but assume that such a threshold factor has been used when the default branching ratio and total width were calculated, so that one should additionally divide by the on-shell threshold factor. Specifically, this will give back the stored branching ratios for on-shell mass, unlike the 102 option. To avoid division by zero, or in general unreasonably big rescaling factors, a lower limit minThreshold (see below) on the value of the on-shell threshold factor is imposed. (In cases where a big rescaling is intentional, code 102 would be more appropriate.)
    Used uniquely for meMode = 103 to set the minimal value assumed for the threshold factor, sqrt( (1 - m_1^2/m_2 - m_2^2/m^2)^2 - 4 m_1^2 m_2^2/m^4) for two-body decays and sqrt(1 - Sum_i m_i / m) for multibody ones. Thus the inverse of this number sets an upper limit for how much the partial width of a channel can increase from the on-shell value to the value for asymptotically large resonance masses. Is mainly intended as a safety measure, to avoid unintentionally large rescalings.

    All of these meMode's may coexist for the same resonance. This would be the case e.g. if you want to add a few new channels to an already existing resonance, where the old partial widths come hardcoded while the new ones are read in from an external file. The typical example would be an MSSM Higgs sector, where partial widths to SM particles are already encoded, meMode = 0, while decay rates to sparticles are read in from some external calculation and maybe would be best approximated by using meMode = 103. Indeed the default particle table in PYTHIA uses 103 for all channels that are expected to be provided by external input.

    Some further clarification may be useful. At initialization the existing total width and on-shell branching ratios will be updated. For channels with meMode < 100 the originally stored branching ratios are irrelevant, since the existing code will anyway be used to calculate the partial widths from scratch. For channels with meMode = 100 or bigger, instead the stored branching ratio is used together with the originally stored total width to define the correct on-shell partial width. The sum of partial widths then gives the new total width, and from there new branching ratios are defined.

    In these operations the original sum of branching ratios need not be normalized to unity. For instance, you may at input have a stored total width of 1 GeV and a sum of branching ratios of 2. After initialization the width will then have been changed to 2 GeV and the sum of branching ratios rescaled to unity. This might happen e.g. if you add a few channels to an existing resonance, without changing the branching ratios of the existing channels or the total width of the resonance.

    In order to simulate the Breit-Wigner shape correctly, it is important that all channels that contribute to the total width are included in the above operations. This must be kept separate from the issue of which channels you want to have switched on for a particular study, to be considered next.

    In the event-generation process, when an off-shell resonance mass has been selected, the width and branching ratios are re-evaluated for this new mass. At this stage also the effects of restrictions on allowed decay modes are taken into account, as set by the onMode switch for each separate decay channel. Thus a channel may be on or off, with different choices of open channels between the particle and its antiparticle. In addition, even when a channel is on, the decay may be into another resonance with its selection of allowed channels. It is these kinds of restrictions that lead to the Gamma_out possibly being smaller than Gamma_tot. As a reminder, the Breit-Wigner for decays behaves like Gamma_out / ((s - m^2)^2 + s * Gamma_tot^2), where the width in the numerator is only to those channels being studied, but the one in the denominator to all channels of the particle. These ever-changing numbers are not directly visible to the user, but are only stored in a work area. pythia8-8.1.80.orig/xmldoc/ProgramFiles.xml0000444000175000017500000003231612217346316016743 0ustar sunsun

    Program Files

    The code is subdivided into a set of files, mainly by physics task. Each file typically contains one main class, but often with a few related helper classes that are not used elsewhere in the program. Normally the files come in pairs.
    • A header file, .h in the include subdirectory, where the public interface of the class is declared, and inline methods are defined.
    • A source code file, .cc in the src subdirectory, where most of the methods are implemented.
    During compilation, related dependency files, .d, and compiled code, .o are created in the tmp subdirectory.

    In part the .xml documentation files in the xmldoc subdirectory have matching names, but the match is broken by the desire to group topics more by user interaction than internal operation. On these pages the function of the different code files is summarized. Currently, each .xml file is also translated into an .html one in the htmldoc subdirectory, to allow easy viewing of the contents in a web browser, and an .php one in phpdoc, for more sophisticated interactivity if that subdirectory is installed on a web server.

    Here is the current list of files, ordered alphabetically, with a brief description of contents. contains routines to analyze events. Currently it can do sphericity, thrust, Lund/Jade/Durham jet clustering, cone-jet finding, and the kT, anti-kT and Cambridge/Aachen algorithms for hadron colliders. contains some basic facilities of general use: a random number generator Rndm, a four-vector class Vec4, and a histogram class Hist. contains information on all partons extracted from one of the two beams. Defines modified parton distributions accordingly during the showering and multiparton interactions processing, thereby extending on the one-particle-inclusive distributions defined by the previous class. Finds the internal structure for a beam remnant. adds primordial kT to the set of hard subsystems, and combines these subsystems with the two beam remnants to provide the overall energy-momentum picture. Also ties together all the colour lines into consistent singlets. generates momentum spread of beams, and spread of collision vertex position. provides a simple method to impose Bose-Einstein correlations on pairs of identical mesons. contains the event record, which basically is a vector of particles. This file also contains the Particle class, used by Event. Pythia uses two Event objects, one for the process-level record (process) and one for the complete event (event). contains the classes for describing the fragmentation steps in flavour and in longitudinal and transverse momentum. defines some containers of parton systems, for use in the fragmentation routines. turns the parton-level event above into a set of outgoing particles, by applying string fragmentation (with special treatment for low-mass systems) and secondary decays, and optionally Bose-Einstein corrections. basic classes for the handling of helicities in tau lepton decays. helicity-dependent decay matrix elements for the tau lepton. hadronization in models with a hidden sector that contains an unbroken SU(N), which gives confinement. The model and code is largely derived from the normal fragmentation classes. methods to reconstruct the imagined shower history of a matrix-element-generated multiparton configuration, as part of the CKKW-L matrix element merging. is a simple container that gives access to some information on the nature of the current process, such as Mandelstam variables. Also contains a small database for errors and warnings encountered during program execution. gives the possibility to feed in parton configurations for the subsequent event generation. One base class is defined, with containers for initialization and event information, that can be read from Pythia. Derived classes allow for a few different cases. is a header file only, for a class derived from the above LesHouches one, to be used for runtime interfacing to Fortran programs, such as PYTHIA 6. is a header file only, with interfaces to the key LHAPDF routines, as needed for a runtime interface. There is a file lhapdfdummy/LHAPDFdummy.cc with matching dummy implementations, however. This file is used to build a separate liblhapdfdummy library, to be linked when the LHAPDF library is not used, so as to avoid problems with undefined references. intercede in the normal shower evolution to construct the relevant Sudakov form factor suppressions as part of the CKKW-L matrix element merging. performs string fragmentation in cases where the colour singlet subsystem mass is so small that one or at most two primary hadrons should be produced from it. performs multiparton interactions. contains a database of all necessary particle data (masses, names, ..) and decay channels. performs the decays of all normal unstable hadrons and leptons, i.e. in mass up to and including b bbar systems. It is not intended for decays of electroweak resonances, like Z^0. contains parton distribution functions for the proton and electron. Currently very simple, with only two p parametrizations and one e ditto available, but it is possible to link in external sets. turns the (hard) process above into a complete set of partons, by adding initial- and final-state radiation, multiparton interactions, and beam remnants. keeps track of which partons belong to which partonic subsystem, i.e. one of the multiparton (semi)hard interactions with associated showers. selects a point in phase space for the hard-process generation, optimized separately for each process to give improved Monte Carlo efficiency. packages the information on a given subprocess, combining the phase-space selection and cross-section evaluation machineries with some statistics information. Also sets up the list of processes to be studied in a run. handles the generation of the (hard) process that sets the character of the event. This involves either using internally implemented processes or linking to Les Houches information. The latter can be by runtime interfaces or by reading in a file. This step also includes resonance decays. is the main class, that administrates the whole event generation process by making use of all the others classes. Objects of most other classes reside (directly or indirectly) inside Pythia, so only a Pythia object needs to be explicitly instantiated and addressed by the user. contains an interface to convert the PYTHIA 8 event record into the HepMC format. The Pythia8ToHepMC.cc file is located in the subdirectory pythia8tohepmc and is used to build a separate libpythia8tohepmc library. is only a .h file, containing a typedef for double precision complex numbers. contains most of the Stdlib headers used in PYTHIA 8, with using directives. It defines M_PI if this is not already done. Also a few simple inline methods: pow2(x), pow3(x), pow4(x), pow5(x) and pow6(x) for small integer powers, and sqrtpos(x) where a max(0., x) ensures that one does not take the square root of a negative number. Also non-inlined GammaReal(x) for the Gamma function value of a real argument. decays resonances as part of the hard-process stage, in many cases (but not all) including angular correlations between the decay products. encodes some properties of resonances, in particular the dynamic calculation of widths. handles the production and decay of hadrons formed by long-lived gluinos, stops or sbottoms. contains a database of all flags, modes, parameters and words that determine the performance of the generator. Initial values are obtained from the contents of the .xml files, but these values can then be changed by the user. contains the cross sections and matrix elements for production of some particles in compositeness scenarios, specifically excited fermions. contains the cross sections and matrix elements for electroweak processes involving photons, Z^0's and W^+-'s. contains the cross sections and matrix elements for processes in scenarios involving extra dimensions. contains the cross sections and matrix elements for some generic processes, to be used as building blocks for a few BSM scenarios. contains the cross sections and matrix elements for Higgs production. contains the cross sections and matrix elements for particle production in left-right-symmetry scenarios, specifically righthanded Z and W bosons and doubly-charged Higgs bosons. contains the cross sections and matrix elements for leptoquark production. contains the cross sections and matrix elements for a Z'^0, a W^+- and a horizontal gauge boson R^0. contains the cross sections and matrix elements for charmonium and bottomonium production. contains the base class and derived classes for the evaluation of different matrix elements. Also keeps track of allowed incoming parton configurations and their cross sections, including parton densities. In order to keep this file from becoming too big, actual cross sections are found in several separate files of derived classes: SigmaQCD, SigmaEW, SigmaOnia, SigmaHiggs, SigmaSUSY, SigmaNewGaugeBosons, SigmaLeftRightSym, SigmaLeptoquark, SigmaCompositeness, SigmaExtraDim and SigmaGeneric. contains the cross sections and matrix elements for soft and hard QCD processes. contains the cross sections and matrix elements for Supersymmetric processes. contains parametrizations of total, elastic and diffractive hadronic cross sections. performs spacelike initial-state transverse-momentum-ordered shower evolution. contains the running alpha_strong, with Lambda matching at flavour thresholds, the running alpha_em, CKM mixing matrices, and a few other parameters such as sin^2(theta_W). performs string fragmentation of a given set of partons. stores the various couplings used for SUSY cross sections and decays, as calculated from input e.g. based on the SUSY Les Houches Accord. contains information on SUSY parameters and particle data as specified by the SUSY Les Houches Accord. the main routines for handling tau lepton decays with helicity information. performs timelike final-state transverse-momentum-ordered shower evolution. Provides a way for a user to study the event at a few intermediate stages of evolution, to reject the event as a whole or to modify its cross-section weight. pythia8-8.1.80.orig/xmldoc/MainProgramSettings.xml0000444000175000017500000002766512217346304020316 0ustar sunsun

    Main-Program and Related Settings

    Introduction

    The main program is up to the user to write. However, sample main programs are provided. In one such class of programs, key settings of the run are read in from a "cards file". For experimental collaborations this is actually the most common way to run a program like PYTHIA. The commands in such a file may be of two types
    (a) instructions directly to Pythia, like which processes to generate, and
    (b) instructions to the main program for what it should do, like how many events to generate, and how many events should be listed.
    In principle these two kinds could be kept completely separate. However, to make life simpler, a number of useful main-program settings are defined on this page, so that they are recognized by the Settings machinery. They can thus be put among the other cards without distinction. It is up to you to decide which ones, if any, you actually want to use when you write your main program.

    To further reduce the necessary amount of main-program code, some of the tasks that you can steer from your main program can also be done internally. This in particular relates to some information printing. To give an example, the Main:numberToList mode can be used by you in your main program to decide to list a few of the generated events, whereas Next:numberListEvent is used internally in a pythia.next() call to do such a listing automatically. Ultimately, in both cases, a pythia.event.list() call is the one that generates the listing, explicitly in the main program in the former case, implicitly called from pythia.next() in the latter.

    The settings names on this page thus fall into four main groups

    • Init:... denote actions that automatically may be taken during the pythia.init() call.
    • Next:... denote actions that automatically may be taken during the pythia.next() call.
    • Stat:... denote actions that automatically may be taken during the pythia.stat() call.
    • Main:... denote actions that you yourself have the freedom to make use of in your main program.
    The use of several of the Main:... options is deprecated in favour of the other possibilities.

    The Main:... options works like this. Once you have used the pythia.readFile(fileName) method to read in the cards file, where the values have been set, you can interrogate the Settings database to make the values available in your main program. A slight complication is that you need to use a different Settings method for each of the four possible return types that you want to extract. To save some typing the same method names are found directly in the Pythia class, and just send on to the Settings ones to do the job, e.g.

      bool   showCS = pythia.flag("Main:showChangedSettings");
      int    nEvent = pythia.mode("Main:numberOfEvents");
      double spare1 = pythia.parm("Main:spareParm1");
      string file   = pythia.word("Main:allSettingsFile"); 
    

    Main-program settings

    The settings in this section must be under the control of the user, i.e. there are no internal equivalents. The number of events to be generated. Allow this many times that pythia.next() returns false, i.e. that an event is flawed, before aborting the run.

    Initialization settings

    Print a list of all processes that will be simulated, with their estimated cross section maxima, as used for the subsequent Monte Carlo selection. Also print corresponding Les Houches initialization data, where relevant. Print initialization information for the multiparton interactions machinery. Print a list of the changed flag/mode/parameter/word settings. Print a list of all flag/mode/parameter/word settings. Warning: this will be a long list. Print a list of particle and decay data for those particles that were changed (one way or another). In the previous listing also include the resonances that are initialized at the beginning of a run and thus get new particle data, even if these may well agree with the default ones. Warning: this will be a rather long list. Print a list of all particle and decay data. Warning: this will be a long list. Print particle and decay data for the particle with this particular identity code. Default means that no particle is printed. Deprecated. Print a list of the changed flag/mode/parameter/word settings. Deprecated. Print a list of all flag/mode/parameter/word settings. Warning: this will be a long list. Deprecated. Print a list of particle and decay data for those particles that were changed (one way or another). Deprecated. In the previous listing also include the resonances that are initialized at the beginning of a run and thus get new particle data, even if these may well agree with the default ones. Warning: this will be a rather long list. Deprecated. Print a list of all particle and decay data. Warning: this will be a long list. Deprecated. Print particle and decay data for the particle with this particular identity code. Default means that no particle is printed. Write a file with the changed flag/mode/parameter/word settings, in a format appropriate to be read in at the beginning of a new run, using the pythia.readFile(fileName) method. The name of the file to which the changed flag/mode/parameter/word settings are written if Main:writeChangedSettings is on. Write a file with all flag/mode/parameter/word settings, in a format appropriate to be read in at the beginning of a new run, using the pythia.readFile(fileName) method. The name of the file to which a flag/mode/parameter/word settings are written if Main:writeAllSettings is on.

    Event-generation settings

    Print a line telling how many events have been generated so far, once every numberCount events. If set zero then no lines are ever printed. The number of events to list the Les Houches input information for, where relevant. The number of events to list the Info information for, where relevant. The number of events to list the process record for, where relevant. The number of events to list the event record for, where relevant. In addition to the normal information in the listing of the process and event records, a second line per particle provides information on the production scale, particle polarization and production vertex. In addition to the normal information in the listing of the process and event records, further lines list all the mothers and daughters of each particle. Deprecated. The number of events to list. Deprecated. Print the number of events generated so far, this many times, i.e. once every numberOfEvents/numberToShow events.

    Statistics

    Print the available statistics on number of generated events and cross sections, where relevant. Print the available statistics on number and types of multiparton interactions, where relevant. Print the available statistics on number and types of aborts, errors and warnings. Reset the statistics of the above three kinds. The default is that all stored statistics information is unaffected by the pythia.stat() call. Counters are automatically reset in each new pythia.init() call, however, so the only time the reset option makes a difference is if stat() is called several times in a (sub)run. Print all available statistics or only the minimal set at the end of the run.

    Subruns

    You can use subruns to carry out several tasks in the same run. In that case you will need repeated instances of the first setting below in your command file, and could additionally use the second and third as well. The number of the current subrun, a non-negative integer, put as first line in a section of lines to be read for this particular subrun. If you read several Les Houches Event Files that you want to see considered as one single combined event sample you can set this flag on after the first subrun to skip (most of) the (re-)initialization step. The number of subruns you intend to use in your current run. Unlike the two settings above, Pythia itself will not interpret this number, but you could e.g. have a loop in your main program to loop over subruns from 0 through numberOfSubruns - 1.

    Spares

    For currently unforeseen purposes, a few dummy settings are made available here. The user can set the desired value in a "cards file" and then use that value in the main program as desired.
    pythia8-8.1.80.orig/xmldoc/FourthGenerationProcesses.xml0000444000175000017500000001410712217346302021514 0ustar sunsun

    Fourth-Generation Processes

    A fourth generation can be accommodated within the Standard Model, without the introduction of any new concepts. Many experimental constraints exist, but it has not been fully excluded. Therefore we offer a simple implementation, along the lines of the top. It could also be useful as a template for studies of other new particles with similar characteristics.

    The fourth generation are given names as in the third, but with a prime, i.e. b' with PDG code 7, t' with code 8, tau' with code 17, and nu'_tau with code 18. Most important for you is to assign a mass hierarchy, to decide which fermions can decay into which. The current implementation assumes that mass splittings are big enough that fourth-generation fermions can decay to third-generation ones by the emission of an on-shell W. To this end, the standard three-generation CKM mixing matrix has been extended to include a fourth generation, see below. Since no mixing has been implemented in the neutrino sector it would be assumed that the lighter of tau' and nu'_tau is stable. No decay modes have been implemented that go beyond the Standard Model, so modifications would be needed if e.g. also SUSY is included in the game.

    Production processes

    1) b' processes

    Different ways to produce b' quarks, singly or in pairs. For a b' t' pair see section 3 below. Common switch for the group of b' production. Also includes the process f fbar' -> t' b'bar in section 3 below. Scatterings g g -> b' b'bar. Code 801. Scatterings q qbar -> b' b'bar by gluon exchange. Code 802. Scatterings q q' -> b' q'' by t-channel exchange of a W^+- boson. Code 803. Scatterings f fbar -> b' b'bar by s-channel exchange of a gamma^*/Z^0 boson. Code 804. Scatterings f fbar' -> b' qbar'' by s-channel exchange of a W^+- boson. Here q'' is either u or c. Code 805. Scatterings f fbar' -> b' tbar by s-channel exchange of a W^+- boson. Code 806.

    2) t' processes

    Different ways to produce t' quarks, singly or in pairs. For a b' t' pair see section 3 below. Common switch for the group of t' production. Also includes the process f fbar' -> t' b'bar in section 3 below. Scatterings g g -> t' t'bar. Code 821. Scatterings q qbar -> t' t'bar by gluon exchange. Code 822. Scatterings q q' -> t' q'' by t-channel exchange of a W^+- boson. Code 823. Scatterings f fbar -> t' t'bar by s-channel exchange of a gamma^*/Z^0 boson. Code 824. Scatterings f fbar' -> t' qbar'' by s-channel exchange of a W^+- boson. Code 825.

    3) Pair-processes with different flavours

    Different ways to produce two different fourth-generation fermions. Scatterings f fbar' -> t' b'bar by s-channel exchange of a W^+- boson. Code 841. Scatterings f fbar' -> tau' nu'_taubar by s-channel exchange of a W^+- boson. Code 842.

    Missing in this list is scatterings q q' -> t' b' by t-channel exchange of a W^+- boson, since currently the matrix element for such processes have not been implemented for two massive particles in the final state. Since this process would involve two CKM-suppressed vertices it ought to be small.

    Parameters

    The Cabibbo-Kobayashi-Maskawa matrix is extended by seven further values. So as not to mess up the Standard Model, the normal 3 * 3 matrix is kept unitary, and so the new off-diagonal elements lead to a slight breaking of this. For exploratory studies this should be good enough; more detailed 4 * 4 tunes to data would only make sense the day there are evidence for the existence of a fourth generation. The V_ub' matrix element in the 4 * 4 CKM matrix. The V_cb' matrix element in the 4 * 4 CKM matrix. The V_tb' matrix element in the 4 * 4 CKM matrix. The V_t'd matrix element in the 4 * 4 CKM matrix. The V_t's matrix element in the 4 * 4 CKM matrix. The V_t'b matrix element in the 4 * 4 CKM matrix. The V_t'b' matrix element in the 4 * 4 CKM matrix.
    pythia8-8.1.80.orig/xmldoc/ProcessSelection.xml0000444000175000017500000001270712217346316017637 0ustar sunsun

    Process Selection

    There is no way PYTHIA could contain all processes of interest, neither in terms of potential physics topics nor in terms of high-multiplicity final states. What exists is a reasonably complete setup of all 2 -> 1 and 2 -> 2 processes within the Standard Model, plus some examples of processes beyond that, again for low multiplicities. Combined with the PYTHIA parton showers, this should be enough to get a flying start in the study of many physics scenarios. Other processes could be fed in via the Les Houches Accord or be implemented as a Semi-Internal Process. In the latter case the existing processes would act as obvious templates.

    By default all processes are switched off. You should switch on those you want to simulate. This may be done at two (occasionally three) levels, either for each individual process or for a group of processes. That is, a process is going to be generated either if its own flag or its group flag is on. There is no built-in construction to switch on a group and then switch off a few of its members.

    Each process is assigned an integer code. This code is not used in the internal administration of events (so having the same code for two completely different processes would not be a problem), but only intended to allow a simpler user separation of different processes. Also the process name is available, as a string.

    To ease navigation, the list of processes has been split into several separate pages, by main topic. The classification is hopefully intuitive, but by no means unambiguous. For instance, essentially all processes involve QCD, so the "QCD processes" are the ones that only involve QCD. (And also that is not completely true, once one includes all that may happen in multiparton interactions.) On these separate pages also appear the settings that are completely local to that particular process class, but not the ones that have a broader usage.

    QCD Processes

    QCD processes fall in two main categories: soft and hard. The soft ones contain elastic, diffractive and "minimum-bias" events, together covering the total cross section. Hard processes are the normal 2 -> 2 ones, including charm and bottom production.
    Reserved code range: 101 - 199.

    Electroweak Processes

    Prompt-photon, gamma^*/Z^0 and W^+- production, plus a few processes with t-channel boson exchange.
    Reserved code range: 201 - 299.

    Onia Processes

    Colour singlet and octet production of charmonium and bottomonium.
    Reserved code range: 401 - 499 for charmonium and 501 - 599 for bottomonium.

    Top Processes

    Top production, singly or doubly.
    Reserved code range: 601 - 699.

    Fourth-Generation Processes

    Production of hypothetical fourth-generation fermions.
    Reserved code range: 801 - 899.

    Higgs Processes

    Higgs production, within or beyond the Standard Model. See section on Left-Right-Symmetry processes for doubly charged Higgs bosons.
    Reserved code range: 901 - 999 for a Standard Model Higgs and 1001 - 1199 for MSSM Higgs bosons.

    SUSY Processes

    Production of supersymmetric particles, currently barely begun.
    Reserved code range: 1001 - 2999. (Whereof 1001 - 1199 for Higgs bosons; see above.)

    New-Gauge-Boson Processes

    Production of new gauge bosons such as Z' and W'.
    Reserved code range: 3001 - 3099.

    Left-Right-Symmetry Processes

    Production of righthanded Z_R and W_R bosons and of doubly charged Higgs bosons.
    Reserved code range: 3101 - 3199.

    Leptoquark Processes

    Production of a simple scalar leptoquark state.
    Reserved code range: 3201 - 3299.

    Compositeness Processes

    Production of excited fermion states and contact-interaction modification to interactions between fermions (excluding technicolor; see below).
    Reserved code range: 4001 - 4099.

    Technicolor Processes

    Production of technicolor particles and modifications of QCD processes by technicolor interactions. Does not exist yet.
    Reserved code range: 4101 - 4199.

    Hidden Valley Processes

    A scenario for the pair production of new particles with couplings under a new gauge group, with invisible gauge bosons. Radiation of these gauge bosons is included in the standard final-state parton shower.
    Reserved code range: 4901 - 4999.

    Extra-Dimensional Processes

    A vast area, here represented by the production of a Randall-Sundrum excited graviton state and a Kaluza-Klein gluon, a Kaluza-Klein tower of gamma/Z^0 excitations in one TeV^- sized extra dimension, several Large Extra Dimension processes, and a few related Unparticle processes.
    Reserved code range: 5001 - 5099.
    pythia8-8.1.80.orig/xmldoc/StandardModelParameters.xml0000444000175000017500000003205712217346317021121 0ustar sunsun

    Standard-Model Parameters

    The strong coupling

    The AlphaStrong class is used to provide a first- or second-order running alpha_strong (or, trivially, a zeroth-order fixed one). Formulae are the standard ones found in Yao06. The second-order expression used, eq. (9.5), may be somewhat different in other approaches (with differences formally of higher order), so do not necessarily expect perfect agreement, especially not at small Q^2 scales. The starting alpha_strong value is defined at the M_Z mass scale. The Lambda values are matched at the c, b and t flavour thresholds, such that alpha_strong is continuous. For second-order matching an approximate iterative method is used.

    For backwards compatibility, the following global switch determines whether 5- or 6-flavour running will be used above the t threshold:

    Since we allow alpha_strong to vary separately for hard processes, timelike showers, spacelike showers and multiparton interactions, all other relevant values are set in each of these classes. The default behaviour is everywhere first-order running.

    The alpha_strong calculation is initialized by init( value, order, nfmax), where value is the alpha_strong value at M_Z, order is the order of the running, 0, 1 or 2, and nfmax is the highest number of flavours to include in the running. Thereafter the value can be calculated by alphaS(scale2), where scale2 is the Q^2 scale in GeV^2.

    For applications inside shower programs, a second-order alpha_s value can be obtained as the product of the two functions alphaS1Ord(scale2) and alphaS2OrdCorr(scale2), where the first gives a simple first-order running (but with the second-order Lambda) and the second the correction factor, below unity, for the second-order terms. This allows a compact handling of evolution equations.

    Resummation arguments Cat91 show that a set of universal QCD corrections can be absorbed in coherent parton showers by applying the so-called CMW rescaling of the MSbar value of Lambda_QCD. This can be accomplished via a fourth (optional) boolean argument to init( value, order, nfmax, useCMW), with default value useCMW = false. When set to true, the translation amounts to an N_F-dependent rescaling of Lambda_QCD, relative to its MSbar value, by a factor 1.661 for NF=3, 1.618 for NF=4, 1.569 for NF=5, and 1.513 for NF=6. When using this option, be aware that the original CMW arguments were derived using two-loop running and that the CMW rescaling may need be taken into account in the context of matrix-element matching. Note also that this option has only been made available for timelike and spacelike showers, not for hard processes.

    The electromagnetic coupling

    The AlphaEM class is used to generate a running alpha_em. The input StandardModel:alphaEMmZ value at the M_Z mass is matched to a low-energy behaviour with running starting at the electron mass threshold. The matching is done by fitting an effective running coefficient in the region between the light-quark threshold and the charm/tau threshold. This procedure is approximate, but good enough for our purposes.

    Since we allow alpha_em to vary separately for hard processes, timelike showers, spacelike showers and multiparton interactions, the choice between using a fixed or a running alpha_em can be made in each of these classes. The default behaviour is everywhere first-order running. The actual values assumed at zero momentum transfer and at M_Z are only set here, however. The alpha_em value at vanishing momentum transfer (and also below m_e). The alpha_em value at the M_Z mass scale. Default is taken from Yao06.

    The alpha_em calculation is initialized by init(order), where order is the order of the running, 0 or 1, with -1 a special option to use the fix value provided at M_Z. Thereafter the value can be calculated by alphaEM(scale2), where scale2 is the Q^2 scale in GeV^2.

    The electroweak couplings

    There are two degrees of freedom that can be set, related to the electroweak mixing angle: The sine-squared of the weak mixing angle, as used in all Z^0 and W^+- masses and couplings, except for the vector couplings of fermions to the Z^0, see below. Default is the MSbar value from Yao06. The sine-squared of the weak mixing angle, as used to derive the vector couplings of fermions to the Z^0, in the relation v_f = a_f - 4 e_f sin^2(theta_W)bar. Default is the effective-angle value from Yao06.

    The Fermi constant is not much used in the currently coded matrix elements, since it is redundant, but it is available: The Fermi coupling constant, in units of GeV^-2.

    The quark weak-mixing matrix

    The absolute values of the Cabibbo-Kobayashi-Maskawa matrix elements are set by the following nine real values taken from Yao06 - currently the CP-violating phase is not taken into account in this parametrization. It is up to the user to pick a consistent unitary set of new values whenever changes are made. The V_ud CKM matrix element. The V_us CKM matrix element. The V_ub CKM matrix element. The V_cd CKM matrix element. The V_cs CKM matrix element. The V_cb CKM matrix element. The V_td CKM matrix element. The V_ts CKM matrix element. The V_tb CKM matrix element.

    The CoupSM class

    The Pythia class contains a public instance coupSM of the CoupSM class. This class contains one instance each of the AlphaStrong and AlphaEM classes, and additionally stores the weak couplings and the quark mixing matrix mentioned above. This class is used especially in the calculation of cross sections and resonance widths, but could also be used elsewhere. Specifically, as already mentioned, there are separate AlphaStrong and AlphaEM instances for timelike and spacelike showers and for multiparton interactions, while weak couplings and the quark mixing matrix are only stored here. With the exception of the first two methods below, which are for internal use, the subsequent ones could also be used externally. the constructor does nothing. Internal. this is where the AlphaStrong and AlphaEM instances are initialized, and weak couplings and the quark mixing matrix are read in and set. This is based on the values stored on this page and among the Couplings and Scales. Internal. the alpha_strong value at the quadratic scale scale2. a first-order overestimate of the full second-order alpha_strong value at the quadratic scale scale2. a multiplicative correction factor, below unity, that brings the first-order overestimate above into agreement with the full second-order alpha_strong value at the quadratic scale scale2. the three-, four-, and five-flavour Lambda scale. the alpha_em value at the quadratic scale scale2. the sine-squared and cosine-squared of the weak mixing angle, as used in the gauge-boson sector. the sine-squared of the weak mixing angle, as used to derive the vector couplings of fermions to the Z^0. the Fermi constant of weak decays, in GeV^-2. the electrical charge of a fermion, by the absolute sign of the PDF code, i.e. idAbs must be in the range between 1 and 18. the vector and axial charges of a fermion, by the absolute sign of the PDF code (a_f = +-1, v_f = a_f - 4. * sin2thetaWbar * e_f). the weak isospin, left- and righthanded charges of a fermion, by the absolute sign of the PDF code (t^3_f = a_f/2, l_f = (v_f + a_f)/2, r_f = (v_f - a_f)/2; you may find other conventions in the literature that differ by a factor of 2). common quadratic combinations of the above couplings: e_f^2, v_f^2, a_f^2, e_f * v_f, v_f^2 + a_f^2. the CKM mixing element,or the square of it, for up-type generation index genU (1 = u, 2 = c, 3 = t, 4 = t') and down-type generation index genD (1 = d, 2 = s, 3 = b, 4 = b'). the CKM mixing element,or the square of it, for flavours id1 and id2, both in the range from -18 to +18. The sign is here not checked (so it can be used both for u + dbar -> W+ and u -> d + W+, say), but impossible flavour combinations evaluate to zero. The neutrino sector is numbered by flavor eigenstates, so there is no mixing in the lepton-neutrino system. the sum of squared CKM mixing element that a given flavour can couple to, excluding the top quark and fourth generation. Is close to unity for the first two generations. Returns unity for the lepton-neutrino sector. picks a random CKM partner quark or lepton (with the same sign as id) according to the respective squared elements, again excluding the top quark and fourth generation from the list of possibilities. Unambiguous choice for the lepton-neutrino sector.
    pythia8-8.1.80.orig/xmldoc/ProgramFlow.xml0000444000175000017500000013634412217346316016616 0ustar sunsun

    Program Flow

    Recall that, to first order, the event generation process can be subdivided into three stages:
    1. Initializaion.
    2. The event loop.
    3. Finishing.
    This is reflected in how the top-level Pythia class should be used in the user-supplied main program, further outlined in the following. Since the nature of the run is defined at the initialization stage, this is where most of the PYTHIA user code has to be written. So as not to confuse the reader unduly, the description of initialization options has been subdivided into what would normally be used and what is intended for more special applications.

    At the bottom of this webpage is a complete survey of all public Pythia methods and data members, in a more formal style than the task-oriented descriptions found in the preceding sections. This offers complementary information.

    Initialization - normal usage

    1. Already at the top of the main program file, you need to include the proper header file
          #include "Pythia8/Pythia.h"
      
      To simplify typing, it also makes sense to declare
          using namespace Pythia8; 
      
    2. The first step is to create a generator object, e.g. with
           Pythia pythia;
      
      It is this object that we will use from now on. Normally a run will only contain one Pythia object. (But you can use several Pythia objects, which then will be independent of each other.)
      By default all output from Pythia will be on the cout stream, but the list methods below do allow output to alternative streams or files.
    3. You next want to set up the character of the run. The pages under the "Setup Run Tasks" heading in the index describe all the options available (with some very few exceptions, found on the other pages). The default values and your modifications are stored in two databases, one for generic settings and one for particle data. Both of these are initialized with their default values by the Pythia constructor. The default values can then be changed, primarily by one of the two ways below, or by a combination of them.

      a) You can use the

          pythia.readString(string);
      
      method repeatedly to do a change of a property at a time. The information in the string is case-insensitive, but upper- and lowercase can be combined for clarity. The rules are that
      (i) if the first nonblank character of the string is a letter it is assumed to contain a setting, and is sent on to pythia.settings.readString(string);
      (ii) if instead the string begins with a digit it is assumed to contain particle data updates, and so sent on to pythia.particleData.readString(string);
      (iii) if none of the above, the string is assumed to be a comment, i.e. nothing will be done.
      In the former two cases, a warning is issued whenever a string cannot be recognized (maybe because of a spelling mistake).
      Some examples would be
          pythia.readString("TimeShower:pTmin = 1.0");
          pythia.readString("111:mayDecay = false");
      
      The readString(string) method is intended primarily for a few changes. It can also be useful if you want to construct a parser for input files that contain commands both to PYTHIA and to other libraries.

      b) You can read in a file containing a list of those variables you want to see changed, with a

          pythia.readFile(fileName);
      
      Each line in this file with be processes by the readString(string) method introduced above. You can thus freely mix comment lines and lines handed on to Settings or to ParticleData.
      This approach is better suited for more extensive changes than a direct usage of readString(string), and can also avoid having to recompile and relink your main program between runs.
      It is also possible to read input from an istream, by default cin, rather than from a file. This may be convenient if information is generated on-the-fly, within the same run.

      Changes are made sequentially in the order the commands are encountered during execution, meaning that if a parameter is changed several times it is the last one that counts. The two special Tune:ee and Tune:pp modes are expanded to change several settings in one go, but these obey the same ordering rules.

    4. Next comes the initialization stage, where all remaining details of the generation are to be specified. There is one standard method to use for this

      pythia.init();
      with no arguments will read all relevant information from the Settings and ParticleData databases. Specifically the setup of incoming beams and energies is governed by the the beam parameters from the Beams group of variables. If you don't change any of those you will default to proton-proton collisions at 14 TeV, i.e. the nominal LHC values.

      A few alternative forms are available, where the arguments of the init(...) call can be used to set the beam parameters. These alternatives are now deprecated, and will be removed for PYTHIA 8.2.

      a) pythia.init( idA, idB, eCM);
      lets you specify the identities and the CM energy of the two incoming beam particles, with A (B) assumed moving in the +z (-z) direction.

      b) pythia.init( idA, idB, eA, eB);
      is similar, but the two beam energies can be different, so the collisions do not occur in the CM frame. If one of the beam energies is below the particle mass you obtain a fixed-target topology.

      c) pythia.init( idA, idB, pxA, pyA, pzA, pxB, pyB, pzB);
      is similar, but here you provide the three-momenta (p_x, p_y, p_z) of the two incoming particles, to allow for arbitrary beam directions.

      d) pythia.init(fileName);
      assumes a file in the Les Houches Event File format is provided.

      e) pythia.init( LHAup*);
      assumes Les Houches Accord initialization and event information is available in an LHAup class object, and that a pointer to this object is handed in.

    5. If you want to have a list of the generator and particle data used, either only what has been changed or everything, you can use
          pythia.settings.listChanged();
          pythia.settings.listAll();
          pythia.particleData.listChanged(); 
          pythia.particleData.listAll(); 
      

    The event loop

    1. Inside the event generation loop you generate the next event using the next() method,
          pythia.next();
      
      This method takes no arguments; everything has already been specified. It does return a bool value, however, false when the generation failed. This can be a "programmed death" when the supply of input parton-level configurations on file is exhausted. It can alternatively signal a failure of Pythia to generate an event, or unphysical features in the event record at the end of the generation step. It makes sense to allow a few false values before a run is aborted, so long as the related faulty events are skipped.
    2. The generated event is now stored in the event object, of type Event, which is a public member of pythia. You therefore have access to all the tools described on the pages under the "Study Output" header in the index. For instance, an event can be listed with pythia.event.list(), the identity of the i'th particle is given by pythia.event[i].id(), and so on.
      The hard process - roughly the information normally stored in the Les Houches Accord event record - is available as a second object, process, also of type Event.
      A third useful public object is info, which offers a set of one-of-a kind pieces of information about the most recent event.

    Finishing

    1. At the end of the generation process, you can call
          pythia.stat(); 
      
      to get some run statistics, on cross sections and the number of errors and warnings encountered. The alternative pythia.statistics(...); is equivalent but deprecated.

    Advanced usage, mainly for initialization

    A) Necessary data are automatically loaded when you use the default PYTHIA installation directory structure and run the main programs in the examples subdirectory. However, in the general case, you must provide the path of the xmldoc directory, where default settings and particle data are found. This can be done in two ways.
    1. You can set the environment variable PYTHIA8DATA to contain the location of the xmldoc directory. In the csh and tcsh shells this could e.g. be
           setenv PYTHIA8DATA /home/myname/pythia81xx/xmldoc
      
      while in other shells it could be
           export PYTHIA8DATA=/home/myname/pythia81xx/xmldoc
      
      where xx is the subversion number.
      Recall that environment variables set locally are only defined in the current instance of the shell. The above lines should go into your .cshrc and .bashrc files, respectively, if you want a more permanent assignment.
    2. You can provide the path as argument to the Pythia constructor, e.g.
           Pythia pythia("/home/myname/pythia81xx/xmldoc");
      
    where again xx is the subversion number.
    When PYTHIA8DATA is set it takes precedence, else the path in the constructor is used, else one defaults to the ../xmldoc directory.

    B) You can override the default behaviour of PYTHIA not only by the settings and particle data, but also by replacing some of the PYTHIA standard routines by ones of your own. Of course, this is only possible if your routines fit into the general PYTHIA framework. Therefore they must be coded according to the the rules relevant in each case, as a derived class of a PYTHIA base class, and a pointer to such an object must be handed in by one of the methods below. These calls must be made before the pythia.init(...) call.

    1. If you are not satisfied with the list of parton density functions that are implemented internally or available via the LHAPDF interface (see the PDF Selection page), you can supply your own by a call to the setPDFPtr(...) method
            pythia.setPDFptr( pdfAPtr, pdfBPtr); 
      
      where pdfAPtr and pdfBPtr are pointers to two Pythia PDF objects. Note that pdfAPtr and pdfBPtr cannot point to the same object; even if the PDF set is the same, two copies are needed to keep track of two separate sets of x and density values.
      If you further wish to use separate PDF's for the hard process of an event than the ones being used for everything else, the extended form
            pythia.setPDFptr( pdfAPtr, pdfBPtr, pdfHardAPtr, pdfHardBPtr); 
      
      allows you to specify those separately, and then the first two sets would only be used for the showers and for multiparton interactions.
    2. If you want to link to an external generator that feeds in events in the LHA format, you can call the setLHAupPtr(...) method
            pythia.setLHAupPtr( lhaUpPtr);
      
      where the lhaUpPtr derives from the LHAup base class.
    3. If you want to perform some particle decays with an external generator, you can call the setDecayPtr(...) method
            pythia.setDecayPtr( decayHandlePtr, particles);
      
      where the decayHandlePtr derives from the DecayHandler base class and particles is a vector of particle codes to be handled.
    4. If you want to use an external random number generator, you can call the setRndmEnginePtr(...) method
            pythia.setRndmEnginePtr( rndmEnginePtr); 
      
      where rndmEnginePtr derives from the RndmEngine base class. The Pythia default random number generator is perfectly good, so this is only intended for consistency in bigger frameworks.
    5. If you want to interrupt the evolution at various stages, to interrogate the event and possibly veto it, or you want to reweight the cross section, you can use
            pythia.setUserHooksPtr( userHooksPtr); 
      
      where userHooksPtr derives from the UserHooks base class.
    6. If you want to use your own merging scale definition for matrix element + parton shower merging, you can call
            pythia.setMergingHooksPtr( mergingHooksPtr); 
      
      where mergingHooksPtr derives from the MergingHooks base class.
    7. If you want to use your own parametrization of beam momentum spread and interaction vertex, rather than the provided simple Gaussian parametrization (off by default), you can call
            pythia.setBeamShapePtr( beamShapePtr); 
      
      where beamShapePtr derives from the BeamShape base class.
    8. If you want to implement a cross section of your own, but still make use of the built-in phase space selection machinery, you can use
            pythia.setSigmaPtr( sigmaPtr);
      
      where sigmaPtr of type SigmaProcess* is an instance of a class derived from one of the Sigma1Process, Sigma2Process and Sigma3Process base classes in their turn derived from SigmaProcess. This call can be used repeatedly to hand in several different processes.
    9. If your cross section contains the production of a new resonance with known analytical expression for all the relevant partial widths, you can make this resonance available to the program with
            pythia.setResonancePtr( resonancePtr);
      
      where resonancePtr of type ResonanceWidths* is an instance of a class derived from the ResonanceWidths base class. In addition you need to add the particle to the normal particle and decay database. This procedure can be used repeatedly to hand in several different resonances.
    10. If you are a real expert and want to replace the PYTHIA initial- and final-state showers, you can use
            pythia.setShowerPtr( timesDecPtr, timesPtr, spacePtr);
      
      where timesDecPtr and timesPtr derive from the TimeShower base class, and spacePtr from SpaceShower.

    C) Some comments on collecting several tasks in the same run.

    1. PYTHIA has not been written for threadsafe execution on multicore processors. If you want to use all cores, the most efficient way presumably is to start correspondingly many jobs, with different random number seeds, and add the statistics at the end. However, note that several instances can be set up in the same main program, since instances are completely independent of each other, so each instance could be run inside a separate thread.
    2. In some cases it is convenient to use more than one Pythia object. The key example would be the simultaneous generation of signal and pileup events, see main19.cc. The two objects are then set up and initialized separately, and generate events completely independently of each other. It is only afterwards that the event records are combined into one single super-event per beam crossing.
    3. When time is not an issue, it may be that you want to perform several separate subruns sequentially inside a run, e.g. to combine results for several kinematical regions or to compare results for some different tunes of the underlying event. One way to go is to create (and destroy) one pythia object for each subrun, in which case they are completely separate. You can also use the same pythia object, only doing a new init(...) call for each subrun. In that case, the settings and particle databases remain as they were in the previous subrun, only affected by the specific changes you introduced in the meantime. You can put those changes in the main program, with pythia.readString(string), using your own logic to decide which ones to execute in which subrun. A corresponding possibility exists with pythia.readFile(fileName, subrun) (or an istream instead of a fileName), which as second argument can take a non-negative subrun number. Then only those sections of the file before any Main:subrun = ... line or with matching subrun number will be read. That is, the file could have a structure like
          ( lines always read, i.e. "default values" always (re)set )
          Main:subrun = 1
          ( lines only read with readFile(fileName, 1) )
          Main:subrun = 2
          ( lines only read with readFile(fileName, 2) )
      
      Both of these possibilities are illustrated in main08.cc.
    4. When working with Les Houches Event Files, it may well be that your intended input event sample is spread over several files, that you all want to turn into complete events in one and the same run. There is no problem with looping over several subruns, where each new subrun is initialized with a new file, with name set in Beams:LHEF. However, in that case you will do a complete re-initialization each time around. If you want to avoid this, note that the flag Beams:newLHEFsameInit = true can be set for the second and subsequent subruns. Then the new file will be simulated with the same initialization data as already set in a previous pythia.init() call. The burden rests on you to ensure that this is indeed correct, e.g. that the two event samples have not been generated for different beam energies. Also note that cross sections for processes will be based on the information in the first-read file, when the full initialization is performed.

    The Pythia Class

    Here follows the complete survey of all public Pythia methods and data members.

    Constructor and destructor

    creates an instance of the Pythia event generators, and sets initial default values, notably for all settings and particle data. You may use several Pythia instances in the same run; only when you want to access external static libraries could this cause problems. (This includes in particular Fortran libraries such as LHAPDF.) allows you to choose from which directory the default settings and particle data values are read in. If the PYTHIA8DATA environment variable has been set it takes precedence. Else this optional argument allows you to choose another directory location than the default one. Note that it is only the directory location you can change, its contents must be the ones of the xmldoc directory in the standard distribution. can be set false to stop the program from printing a banner. The banner contains useful information, so this option is only intended for runs with multiple Pythia instances, where output needs to be restricted. the destructor deletes the objects created by the constructor.

    Set up run

    reads in a single string, that is interpreted as an instruction to modify the value of a setting or particle data, as already described above. the string to be interpreted as an instruction. write a warning message or not whenever the instruction does not make sense, e.g. if the variable does not exist in the databases. Note: the method returns false if it fails to make sense out of the string. reads in a whole file, where each line is interpreted as an instruction to modify the value of a setting or particle data, cf. the above readString method. All four forms of the readFile command share code for actually reading a file. the file from which instructions are read. an istream from which instructions are read. write a warning message or not whenever the instruction does not make sense, e.g. if the variable does not exist in the databases. In the command forms where warn is omitted it is true. allows you have several optional sets of commands within the same file. Only those sections of the file before any Main:subrun = ... line or following such a line with matching subrun number will be read. The subrun number should not be negative; negative codes like SUBRUNDEFAULT corresponds to no specific subrun. Note: the method returns false if it fails to make sense out of any one line. offers the possibility to link in external PDF sets for usage inside the program. The rules for constructing your own class from the PDF base class are described here. pointers to two PDF-derived objects, one for each of the incoming beams. The two objects have to be instantiated by you in your program. Even if the two beam particles are the same (protons, say) two separate instances are required, since current information is cached in the objects. If both arguments are zero then any previous linkage to external PDF's is disconnected, see further Note 2 below. pointers to two further PDF-derived objects, one for each of the incoming beams. Normally only the first two arguments above would be used, and then the same PDF sets would be invoked everywhere. If you provide these two further pointers then two different sets of PDF's are used. This second set is then exclusively for the generation of the hard process from the process matrix elements library. The first set above is for everything else, notably parton showers and multiparton interactions. Note 1: The method returns false if the input is obviously incorrect, e.g. if two (nonzero) pointers agree. Note 2: If you want to combine several subruns you can call setPDFPtr with new arguments before each Pythia::init(...) call. To revert from external PDF's to the normal internal PDF selection you must call setPDFPtr(0, 0) before Pythia::init(...). offers linkage to an external generator that feeds in events in the LHA format, see Les Houches Accord, assuming that Beams:frameType = 5 has been set. pointer to a LHAup-derived object. Note: The method currently always returns true. offers the possibility to link to an external program that can do some of the particle decays, instead of using the internal decay machinery. With particles we here mean the normal hadrons and leptons, not top quarks, electroweak bosons or new particles in BSM scenarios. The rules for constructing your own class from the DecayHandler base class are described here. Note that you can only provide one external object, but this object in its turn could very well hand on different particles to separate decay libraries. pointer to a DecayHandler-derived object. This object must be instantiated by you in your program. vector with the PDG identity codes of the particles that should be handled by the external decay package. You should only give the particle (positive) codes; the respective antiparticle is always included as well. Note: The method currently always returns true. offers the possibility to link to an external random number generator. The rules for constructing your own class from the RndmEngine base class are described here. pointer to a RndmEngine-derived object. This object must be instantiated by you in your program. Note: The method returns true if the pointer is different from 0. offers the possibility to interact with the generation process at a few different specified points, e.g. to reject undesirable events at an early stage to save computer time. The rules for constructing your own class from the UserHooks base class are described here. You can only hand in one such pointer, but this may be to a class that implements several of the different allowed possibilities. pointer to a userHooks-derived object. This object must be instantiated by you in your program. Note: The method currently always returns true. offers the possibility to provide your own shape of the momentum and space-time spread of the incoming beams. The rules for constructing your own class from the BeamShape base class are described here. pointer to a BeamShape-derived object. This object must be instantiated by you in your program. Note: The method currently always returns true. offers the possibility to link your own implementation of a process and its cross section, to make it a part of the normal process generation machinery, without having to recompile the Pythia library itself. The rules for constructing your own class from the SigmaProcess base class are described here. You may call this routine repeatedly, to add as many new processes as you wish. pointer to a SigmaProcess-derived object. This object must be instantiated by you in your program. Note: The method currently always returns true. offers the possibility to link your own implementation of the calculation of partial resonance widths, to make it a part of the normal process generation machinery, without having to recompile the Pythia library itself. This allows the decay of new resonances to be handled internally, when combined with new particle data. Note that the decay of normal hadrons cannot be modeled here; this is for New Physics resonances. The rules for constructing your own class from the ResonanceWidths base class are described here. You may call this routine repeatedly, to add as many new resonances as you wish. pointer to a ResonanceWidths-derived object. This object must be instantiated by you in your program. Note: The method currently always returns true. offers the possibility to link your own parton shower routines as replacements for the default ones. This is much more complicated since the showers are so central and are so interlinked with other parts of the program. Therefore it is also possible to do the replacement in stages, from the more independent to the more intertwined. The rules for constructing your own classes from the TimeShower and SpaceShowerbase classes are described here. These objects must be instantiated by you in your program. pointer to a TimeShower-derived object for doing timelike shower evolution in resonance decays, e.g. of a Z^0. This is decoupled from beam remnants and parton distributions, and is therefore the simplest kind of shower to write. If you provide a value 0 then the internal shower routine will be used. pointer to a TimeShower-derived object for doing all other timelike shower evolution, which is normally interleaved with multiparton interactions and spacelike showers, introducing both further physics and further technical issues. If you retain the default value 0 then the internal shower routine will be used. You are allowed to use the same pointer as above for the timesDecPtr if the same shower can fulfill both tasks. pointer to a SpaceShower-derived object for doing all spacelike shower evolution, which is normally interleaved with multiparton interactions and timelike showers. If you retain the default value 0 then the internal shower routine will be used. Note: The method currently always returns true.

    Initialize

    At the initialization stage all the information provided above is processed, and the stage is set up for the subsequent generation of events. Currently several alternative forms of the init method are available for this stage, but only the first one is recommended. initialize for collisions, in any of the five separate possibilities below. In this option the beams are not specified by input arguments, but instead by the settings in the Beam Parameters section. This allows the beams to be specified in the same file as other run instructions. The default settings give pp collisions at 14 TeV. Note: The method returns false if the initialization fails. It is then not possible to generate any events. initialize for collisions in the center-of-mass frame, with the beams moving in the +-z directions. particle identity code for the two incoming beams. the CM energy of the collisions. Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events. initialize for collisions with back-to-back beams, moving in the +-z directions, but with different energies. particle identity code for the two incoming beams. the energies of the two beams. If an energy is set to be below the mass of the respective beam particle that particle is taken to be at rest. This offers a simple possibility to simulate fixed-target collisions. Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events. initialize for collisions with arbitrary beam directions. particle identity code for the two incoming beams. the three-momentum vector (p_x, p_y, p_z) of the first incoming beam. the three-momentum vector (p_x, p_y, p_z) of the second incoming beam. Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events. initialize for hard-process collisions fed in from an external file with events, written according to the Les Houches Event File standard. the file name (including path, where required) where the events are stored, including relevant information on beam identities and energies. By default this method does a complete reinitialization of the generation process. If you set this argument to true then no reinitialization will occur, only the pointer to the event file is updated. This may come in handy if the full event sample is split across several files generated under the same conditions (except random numbers, of course). You then do the first initialization with the default, and all subsequent ones with true. Note that things may go wrong if the files are not created under the same conditions. Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events. initialize for hard-process collisions fed in from an external source of events, consistent with the Les Houches Accord standard. The rules for constructing your own class from the LHAup base class are described here. This class is also required to provide the beam parameters. pointer to a LHAup-derived object. This object must be instantiated by you in your program. Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

    Generate events

    The next() method is the main one to generate events. In this section we also put a few other specialized methods that may be useful in some circumstances. generate the next event. No input parameters are required; all instructions have already been set up in the initialization stage. Note: The method returns false if the event generation fails. The event record is then not consistent and should not be studied. When reading in hard collisions from a Les Houches Event File the problem may be that the end of the file has been reached. This can be checked with the Info::atEndOfFile() method. perform a final-state shower evolution on partons in the event event record. This could be used for externally provided simple events, or even parts of events, for which a complete generation is not foreseen. Since the mother source of the parton system is not known, one cannot expect as good accuracy as in a normal generation. When two different timelike shower instances are set up, it is the one used for showering in resonance decays that is used here. The forceTimeShower method can be used in conjunction with the forceHadronLevel one below. Further comments are found here. the first and last entry of the event record to be affected by the call. the maximum pT scale of emissions. Additionally, as always, the scale variable of each parton sets the maximum pT scale of branchings of this parton. Recall that this scale defaults to 0 if not set, so that no radiation can occur. when positive, it sets the maximum number of branchings that are allowed to occur in the shower, i.e. the shower may stop evolving before reaching the lower cutoff. The argument has no effect when zero or negative, i.e. then the shower will continue to the lower cutoff. Note: The method returns the number of branchings that has been generated. hadronize the existing event record, i.e. perform string fragmentation and particle decays. There are two main applications. Firstly, you can use the same parton-level content as a basis for repeated hadronization attempts, in schemes intended to save computer time. Secondly, you may have an external program that can simulate the full partonic level of the event - hard process, parton showers, multiparton interactions, beam remnants, colour flow, and so on - but not hadronization. Further details are found here. normally this routine will search through the event record and try to figure out if any colour junctions are present. If so, the colour topology of such junctions must be sorted out. In tricky cases this might fail, and then hadronization will not work. A user who is aware of this and knows the intended colour flow can set up the junction information (if any) in the event record, and then call forceHadronLevel(false) so as not to have this information overwritten. (If the event record contains no unhadronized partons then no junction search will be performed in any case.) Note: The method returns false if the hadronization fails. The event record is then not consistent and should not be studied. perform decays of all particles in the event record that have not been decayed but should have been done so. This can be used e.g. for repeated decay attempts, in schemes intended to save computer time. Further details are found here. Note: The method returns false if the decays fail. The event record is then not consistent and should not be studied. perform decays of R-hadrons that were previously considered stable. This could be if an R-hadron is sufficiently long-lived that it may interact in the detector between production and decay, so that its four-momentum is changed. Further details are found here. Note: The method returns false if the decays fail. The event record is then not consistent and should not be studied. list the Les Houches Accord information on the current event, see LHAup::listEvent(...). (Other listings are available via the class members below, so this listing is a special case that would not fit elsewhere.) output stream where the listing occurs. skip ahead a number of events in the Les Houches generation sequence, without doing anything further with them, see LHAup::skipEvent(nSkip). Mainly intended for debug purposes, e.g. when an event at a known location in a Les Houches Event File is causing problems. number of events to skip. Note: The method returns false if the operation fails, specifically if the end of a LHEF has been reached, cf. next() above.

    Finalize

    There is no required finalization step; you can stop generating events when and how you want. It is still recommended that you make it a routine to call the following method at the end. A second method provides a deprecated alternative. list statistics on the event generation, specifically total and partial cross sections and the number of different errors. For more details see here and for available options here. list statistics on the event generation, specifically total and partial cross sections and the number of different errors. For more details see here. if true also statistics on multiparton interactions is shown, by default not. if true then all counters, e.g on events generated and errors experienced, are reset to zero whenever the routine is called. The default instead is that all stored statistics information is unaffected by the call. Counters are automatically reset in each new Pythia::init(...) call, however, so the only time the reset option makes a difference is if statistics(...) is called several times in a (sub)run. Note: Deprecated.

    Interrogate settings

    Normally settings are used in the setup and initialization stages to determine the character of a run, e.g. read from a file with the above-described Pythia::readFile(...) method. There is no strict need for a user to interact with the Settings database in any other way. However, as an option, some settings variables have been left free for the user to set in such a file, and then use in the main program to directly affect the performance of that program, see here. A typical example would be the number of events to generate. For such applications the following shortcuts to some Settings methods may be convenient. read in a boolean variable from the Settings database. the name of the variable to be read. read in an integer variable from the Settings database. the name of the variable to be read. read in a double-precision variable from the Settings database. the name of the variable to be read. read in a string variable from the Settings database. the name of the variable to be read.

    Get a PDF set

    Pythia contains an number of parton density sets internally, plus an interface to LHAPDF. With the method below, this machinery is also made available for external usage. get a pointer to a PDF object. Which PDF is returned depends on the PDF Selection settings. the identity code of the incoming particle. should normally be 1, but 2 can be used for protons to let the PDF selection be determined by the special settings for hard processes (PDF:useHard etc.).

    Data members

    The Pythia class contains a few public data members, several of which play a central role. We list them here, with links to the places where they are further described. the hard-process event record, see here for further details. the complete event record, see here for further details. further information on the event-generation process, see here for further details. the settings database, see here for further details. the particle properties and decay tables database, see here for further details. the random number generator, see here and here for further details. Standard Model couplings and mixing matrices, see here for further details. parameters and particle data in the context of supersymmetric models, see here for further details. a grouping of the partons in the event record by subsystem, see here for further details.
    pythia8-8.1.80.orig/xmldoc/CouplingsAndScales.xml0000444000175000017500000003020512217346277020073 0ustar sunsun

    Couplings and Scales

    Here is collected some possibilities to modify the scale choices of couplings and parton densities for all internally implemented hard processes. This is based on them all being derived from the SigmaProcess base class. The matrix-element coding is also used by the multiparton-interactions machinery, but there with a separate choice of alpha_strong(M_Z^2) value and running, and separate PDF scale choices. Also, in 2 -> 2 and 2 -> 3 processes where resonances are produced, their couplings and thereby their Breit-Wigner shapes are always evaluated with the resonance mass as scale, irrespective of the choices below.

    Couplings and K factor

    The size of QCD cross sections is mainly determined by The alpha_strong value at scale M_Z^2.

    The actual value is then regulated by the running to the Q^2 renormalization scale, at which alpha_strong is evaluated Order at which alpha_strong runs,

    QED interactions are regulated by the alpha_electromagnetic value at the Q^2 renormalization scale of an interaction. The running of alpha_em used in hard processes.

    In addition there is the possibility of a global rescaling of cross sections (which could not easily be accommodated by a changed alpha_strong, since alpha_strong runs) Multiply almost all cross sections by this common fix factor. Excluded are only unresolved processes, where cross sections are better set directly, and multiparton interactions, which have a separate K factor of their own. This degree of freedom is primarily intended for hadron colliders, and should not normally be used for e^+e^- annihilation processes.

    Renormalization scales

    The Q^2 renormalization scale can be chosen among a few different alternatives, separately for 2 -> 1, 2 -> 2 and two different kinds of 2 -> 3 processes. In addition a common multiplicative factor may be imposed. The Q^2 renormalization scale for 2 -> 1 processes. The same options also apply for those 2 -> 2 and 2 -> 3 processes that have been specially marked as proceeding only through an s-channel resonance, by the isSChannel() virtual method of SigmaProcess. The Q^2 renormalization scale for 2 -> 2 processes. The Q^2 renormalization scale for "normal" 2 -> 3 processes, i.e excepting the vector-boson-fusion processes below. Here it is assumed that particle masses in the final state either match or are heavier than that of any t-channel propagator particle. (Currently only g g / q qbar -> H^0 Q Qbar processes are implemented, where the "match" criterion holds.) The Q^2 renormalization scale for 2 -> 3 vector-boson-fusion processes, i.e. f_1 f_2 -> H^0 f_3 f_4 with Z^0 or W^+- t-channel propagators. Here the transverse masses of the outgoing fermions do not reflect the virtualities of the exchanged bosons. A better estimate is obtained by replacing the final-state fermion masses by the vector-boson ones in the definition of transverse masses. We denote these combinations mT_Vi^2 = m_V^2 + pT_i^2. The Q^2 renormalization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes is multiplied by this factor relative to the scale described above (except for the options with a fix scale). Should be use sparingly for 2 -> 1 processes. A fix Q^2 value used as renormalization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes in some of the options above.

    Factorization scales

    Corresponding options exist for the Q^2 factorization scale used as argument in PDF's. Again there is a choice of form for 2 -> 1, 2 -> 2 and 2 -> 3 processes separately. For simplicity we have let the numbering of options agree, for each event class separately, between normalization and factorization scales, and the description has therefore been slightly shortened. The default values are not necessarily the same, however. The Q^2 factorization scale for 2 -> 1 processes. The same options also apply for those 2 -> 2 and 2 -> 3 processes that have been specially marked as proceeding only through an s-channel resonance. The Q^2 factorization scale for 2 -> 2 processes. The Q^2 factorization scale for "normal" 2 -> 3 processes, i.e excepting the vector-boson-fusion processes below. The Q^2 factorization scale for 2 -> 3 vector-boson-fusion processes, i.e. f_1 f_2 -> H^0 f_3 f_4 with Z^0 or W^+- t-channel propagators. Here we again introduce the combinations mT_Vi^2 = m_V^2 + pT_i^2 as replacements for the normal squared transverse masses of the two outgoing quarks. The Q^2 factorization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes is multiplied by this factor relative to the scale described above (except for the options with a fix scale). Should be use sparingly for 2 -> 1 processes. A fix Q^2 value used as factorization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes in some of the options above.
    pythia8-8.1.80.orig/xmldoc/ProgramMethods.xml0000444000175000017500000000106112217346316017275 0ustar sunsun

    Program Methods

    This is an alphabetical index of all methods that are documented elsewhere on these pages, beginning with the few methods that do not belong to a class. Many of them are only intended for experts, while undocumented ones are only for code authors.

    The index is constructed dynamically from the methods described on the other webpages, as part of the conversion from xml to html and php. Therefore this xml page is only a dummy one. pythia8-8.1.80.orig/xmldoc/SaveSettings.xml0000444000175000017500000001223512217346317016767 0ustar sunsun

    Save Settings

    The information on this webpage is only valid if you access the PHP dynamic webpages via a web browser, and does not apply to the static HTML equivalents. With PHP, all of the settings in the PYTHIA program are represented by radio buttons or fill-in boxes, that makes it easy for you to construct a file with your desired changes. This file can then be read into PYTHIA by your main program to steer the whole run.

    Basic instructions

    The functionality of the PHP option is described in the following.

    • To begin with, you must specify a (temporary) file name in the box above. If the filename already exists on the server, you will be requested to pick a new name.
    • Once you have Submitted your filename, you can browse through the pages and make your selections. The values currently selected when you load the page are the default values.
    • When you have finished making your changes to a particular page, you must click on Save Settings at the bottom of the page. This will write the changes to your temporary file. If you make a mistake, just repeat the procedure for that category again.

    • When you have finished all the changes you need, return to this page and click Finish File.
    • You will then get up a link, that you are asked to right-click with your mouse (or equivalent).
    • In the menu that appears, pick the option Save Link As (or equivalent).
    • You will now get up a file browser, for you to pick and Save the location and file name (the latter by default the same as the temporary file name).
    • At any time, if you click the RESET button, your temporary file will be erased and you can start anew.
    • Before you use a file, be sure to check it visually to confirm that you saved what you intended to. Minor corrections are easily made in a text editor.

    Supplementary notes

    The documentation files exist in three versions.

    1. As a set of .xml files, in the xmldoc/ subdirectory. These are the master copies that no user ever should touch, but that are used to generate the variants below.
    2. As a set of .html files, in the htmldoc/ subdirectory. You can open your own locally installed copy of the Welcome.html file in your web browser and thereafter navigate among all the pages. You can learn which parameters are free to be changed, but not change anything, except by brute-force cut-and-paste to a file of your own.
    3. As a set of .php files, in the phpdoc/ subdirectory. For these files to provide the functionality described above they have to accessed via a webserver. The one where you have your homepage should work fine. Alternatively you can use pages already available on another server.

    A few further comments about the operation of the PHP option:

    • To set up the PHP files on your webserver, you have to install the whole phpdoc/ subdirectory there. In addition to the .php code this includes a few more files, plus a subdirectory named files where the temporary files are stored. This subdirectory must have public write access to work (chmod a+w files if not).
    • The "temporary" files stored in files actually remain unless the RESET button is used. The good news is that this makes it possible to recover a file that otherwise might be lost. The bad news is that the files directory may need to be cleaned up from time to time. (But typically the files are pretty small, so this should not be a major problem.)
    • When you click the Save Settings button on the bottom of a page all changed settings are written on the temporary file in the format
      name-of-flag/mode/parameter/word = value
      
      with one variable per line. Thereafter all the settings on the page are restored to their default values.
    • You can return to a page to do some further changes and save those. If you change the same parameter twice, it is the last value that counts. (Both values are stored in the file, with the more recent lower down, and then PYTHIA does the changes sequentially.) However remember that unchanged values are not stored, so if you want to restore some default value it may be simpler to edit the file afterwards.
    • The changeable flags/modes/parameters/words are mainly in the "Setup Run Tasks" section of the index, but a few (less frequently used ones) can also be found lower down, in the "Study Output" and "Link to Other Programs" pages.

    • It is not (yet) possible to modify particle data within the PHP-based setup approach. This is a more difficult task, since e.g. the modifications one may want to do in a decay table can be quite interrelated. pythia8-8.1.80.orig/xmldoc/BeamRemnants.xml0000444000175000017500000003525312217346277016736 0ustar sunsun

      Beam Remnants

      Introduction

      The BeamParticle class contains information on all partons extracted from a beam (so far). As each consecutive multiparton interaction defines its respective incoming parton to the hard scattering a new slot is added to the list. This information is modified when the backwards evolution of the spacelike shower defines a new initiator parton. It is used, both for the multiparton interactions and the spacelike showers, to define rescaled parton densities based on the x and flavours already extracted, and to distinguish between valence, sea and companion quarks. Once the perturbative evolution is finished, further beam remnants are added to obtain a consistent set of flavours. The current physics framework is further described in Sjo04.

      The introduction of rescattering in the multiparton interactions framework further complicates the processing of events. Specifically, when combined with showers, the momentum of an individual parton is no longer uniquely associated with one single subcollision. Nevertheless the parton is classified with one system, owing to the technical and administrative complications of more complete classifications. Therefore the addition of primordial kT to the subsystem initiator partons does not automatically guarantee overall pT conservation. Various tricks are used to minimize the mismatch, with a brute force shift of all parton pT's as a final step.

      Much of the above information is stored in a vector of ResolvedParton objects, which each contains flavour and momentum information, as well as valence/companion information and more. The BeamParticle method list() shows the contents of this vector, mainly for debug purposes.

      The BeamRemnants class takes over for the final step of adding primordial kT to the initiators and remnants, assigning the relative longitudinal momentum sharing among the remnants, and constructing the overall kinematics and colour flow. This step couples the two sides of an event, and could therefore not be covered in the BeamParticle class, which only considers one beam at a time.

      The methods of these classes are not intended for general use, and so are not described here.

      In addition to the parameters described on this page, note that the choice of parton densities is made in the Pythia class. Then pointers to the pdf's are handed on to BeamParticle at initialization, for all subsequent usage.

      Primordial kT

      The primordial kT of initiators of hard-scattering subsystems are selected according to Gaussian distributions in p_x and p_y separately. The widths of these distributions are chosen to be dependent on the hard scale of the central process and on the mass of the whole subsystem defined by the two initiators: sigma = (sigma_soft * Q_half + sigma_hard * Q) / (Q_half + Q) * m / (m_half + m) Here Q is the hard-process renormalization scale for the hardest process and the pT scale for subsequent multiparton interactions, m the mass of the system, and sigma_soft, sigma_hard, Q_half and m_half parameters defined below. Furthermore each separately defined beam remnant has a distribution of width sigma_remn, independently of kinematical variables. Allow or not selection of primordial kT according to the parameter values below. The width sigma_soft in the above equation, assigned as a primordial kT to initiators in the soft-interaction limit. The width sigma_hard in the above equation, assigned as a primordial kT to initiators in the hard-interaction limit. The scale Q_half in the equation above, defining the half-way point between hard and soft interactions. The scale m_half in the equation above, defining the half-way point between low-mass and high-mass subsystems. (Kinematics construction can easily fail if a system is assigned a primordial kT value higher than its mass, so the mass-dampening is intended to reduce some troubles later on.) The width sigma_remn, assigned as a primordial kT to beam-remnant partons.

      A net kT imbalance is obtained from the vector sum of the primordial kT values of all initiators and all beam remnants. This quantity is compensated by a shift shared equally between all partons, except that the dampening factor m / (m_half + m) is again used to suppress the role of small-mass systems.

      Note that the current sigma definition implies that <pT^2> = <p_x^2>+ <p_y^2> = 2 sigma^2. It thus cannot be compared directly with the sigma of nonperturbative hadronization, where each quark-antiquark breakup corresponds to <pT^2> = sigma^2 and only for hadrons it holds that <pT^2> = 2 sigma^2. The comparison is further complicated by the reduction of primordial kT values by the overall compensation mechanism. Is only relevant when rescattering is switched on in the multiparton interactions scenario. For a normal interaction the rapidity and mass of a system is preserved when primordial kT is introduced, by appropriate modification of the incoming parton momenta. Kinematics construction is more complicated for a rescattering, and two options are offered. Differences between these can be used to explore systematic uncertainties in the rescattering framework.
      The default behaviour is to keep the incoming rescattered parton as is, but to modify the unrescattered incoming parton so as to preserve the invariant mass of the system. Thereby the rapidity of the rescattering is modified.
      The alternative is to retain the rapidity (and mass) of the rescattered system when primordial kT is introduced. This is made at the expense of a modified longitudinal momentum of the incoming rescattered parton, so that it does not agree with the momentum it ought to have had by the kinematics of the previous interaction.
      For a double rescattering, when both incoming partons have already scattered, there is no obvious way to retain the invariant mass of the system in the first approach, so the second is always used.

      Colour flow

      The colour flows in the separate subprocesses defined in the multiparton-interactions scenario are tied together via the assignment of colour flow in the beam remnant. This is not an unambiguous procedure, but currently no parameters are directly associated with it. However, a simple "minimal" procedure of colour flow only via the beam remnants does not result in a scenario in agreement with data, notably not a sufficiently steep rise of <pT>(n_ch). The true origin of this behaviour and the correct mechanism to reproduce it remains one of the big unsolved issues at the borderline between perturbative and nonperturbative QCD. As a simple attempt, an additional step is introduced, wherein the gluons of a lower-pT system are merged with the ones in a higher-pT one. Allow or not a system to be merged with another one. A system with a hard scale pT can be merged with one of a harder scale with a probability that is pT0_Rec^2 / (pT0_Rec^2 + pT^2), where pT0_Rec is reconnectRange times pT0, the latter being the same energy-dependent dampening parameter as used for multiparton interactions. Thus it is easy to merge a low-pT system with any other, but difficult to merge two high-pT ones with each other.

      The procedure is used iteratively. Thus first the reconnection probability P = pT0_Rec^2 / (pT0_Rec^2 + pT^2) of the lowest-pT system is found, and gives the probability for merger with the second-lowest one. If not merged, it is tested with the third-lowest one, and so on. For the m'th higher system the reconnection probability thus becomes (1 - P)^(m-1) P. That is, there is no explicit dependence on the higher pT scale, but implicitly there is via the survival probability of not already having been merged with a lower-pT system. Also note that the total reconnection probability for the lowest-pT system in an event with n systems becomes 1 - (1 - P)^(n-1). Once the fate of the lowest-pT system has been decided, the second-lowest is considered with respect to the ones above it, then the third-lowest, and so on.

      Once it has been decided which systems should be joined, the actual merging is carried out in the opposite direction. That is, first the hardest system is studied, and all colour dipoles in it are found (including to the beam remnants, as defined by the holes of the incoming partons). Next each softer system to be merged is studied in turn. Its gluons are, in decreasing pT order, inserted on the colour dipole i,j that gives the smallest (p_g p_i)(p_g p_j)/(p_i p_j), i.e. minimizes the "disturbance" on the existing dipole, in terms of pT^2 or Lambda measure (string length). The insertion of the gluon means that the old dipole is replaced by two new ones. Also the (rather few) quark-antiquark pairs that can be traced back to a gluon splitting are treated in close analogy with the gluon case. Quark lines that attach directly to the beam remnants cannot be merged but are left behind.

      The joining procedure can be viewed as a more sophisticated variant of the one introduced already in Sjo87. Clearly it is ad hoc. It hopefully captures some elements of truth. The lower pT scale a system has the larger its spatial extent and therefore the larger its overlap with other systems. It could be argued that one should classify individual initial-state partons by pT rather than the system as a whole. However, for final-state radiation, a soft gluon radiated off a hard parton is actually produced at late times and therefore probably less likely to reconnect. In the balance, a classification by system pT scale appears sensible as a first try.

      Note that the reconnection is carried out before resonance decays are considered. Colour inside a resonance therefore is not reconnected. This is a deliberate choice, but certainly open to discussion and extensions at a later stage, as is the rest of this procedure.

      Further variables

      The maximum valence quark kind allowed in acceptable incoming beams, for which multiparton interactions are simulated. Default is that hadrons may contain u, d and s quarks, but not c and b ones, since sensible kinematics has not really been worked out for the latter. When a sea quark has been found, a companion antisea quark ought to be nearby in x. The shape of this distribution can be derived from the gluon mother distribution convoluted with the g -> q qbar splitting kernel. In practice, simple solutions are only feasible if the gluon shape is assumed to be of the form g(x) ~ (1 - x)^p / x, where p is an integer power, the parameter above. Allowed values correspond to the cases programmed.
      Since the whole framework is approximate anyway, this should be good enough. Note that companions typically are found at small Q^2, if at all, so the form is supposed to represent g(x) at small Q^2 scales, close to the lower cutoff for multiparton interactions.

      When assigning relative momentum fractions to beam-remnant partons, valence quarks are chosen according to a distribution like (1 - x)^power / sqrt(x). This power is given below for quarks in mesons, and separately for u and d quarks in the proton, based on the approximate shape of low-Q^2 parton densities. The power for other baryons is derived from the proton ones, by an appropriate mixing. The x of a diquark is chosen as the sum of its two constituent x values, and can thus be above unity. (A common rescaling of all remnant partons and particles will fix that.) An additional enhancement of the diquark momentum is obtained by its x value being rescaled by the valenceDiqEnhance factor. The abovementioned power for valence quarks in mesons. The abovementioned power for valence u quarks in protons. The abovementioned power for valence d quarks in protons. Enhancement factor for valence diquarks in baryons, relative to the simple sum of the two constituent quarks. The off option is intended for debug purposes only, as follows. When more than one valence quark is kicked out of a baryon beam, as part of the multiparton interactions scenario, the subsequent hadronization is described in terms of a junction string topology. This description involves a number of technical complications that may make the program more unstable. As an alternative, by switching this option off, junction configurations are rejected (which gives an error message that the remnant flavour setup failed), and the multiparton interactions and showers are redone until a junction-free topology is found. pythia8-8.1.80.orig/xmldoc/TopProcesses.xml0000444000175000017500000000273312217346320016775 0ustar sunsun

      Top Processes

      Different ways to produce top quarks, singly or in pairs. Common switch for the group of top production. Scatterings g g -> t tbar. Code 601. Scatterings q qbar -> t tbar by gluon exchange. Code 602. Scatterings q q' -> t q'' by t-channel exchange of a W^+- boson. Code 603. Scatterings f fbar -> t tbar by s-channel exchange of a gamma^*/Z^0 boson. Code 604. Scatterings f fbar' -> t q'' by s-channel exchange of a W^+- boson. Code 605. Scatterings gamma gamma -> t tbar. Code 606.

      By default top always decays to a W and a down-type quark. It is possible to switch on the t -> H+ b decay mode. Note that its partial width is calculated using the tan(beta) value stored in HiggsHchg:tanBeta, so that it can be used without having to read in a SUSY parameter file. For the H+ to decay also Higgs:useBSM = on is necessary. pythia8-8.1.80.orig/xmldoc/ct09mcs.pds0000444000175000017500000173566712217346301015637 0ustar sunsunPDF Table for Fit #: cp6ls14 Ordr, Nfl, lambda Qmass 1, 2, 3, 4, 5, 6 2. 5. 0.2268 0.001 0.001 0.200 1.400 4.750 172.000 IPD0, IHDN, IKNL, NfMx, Nfval, KF, Nelmt 1 1 1 5 2 12 57300 NX, NT, JT, NG, NTL(NG+1) 190 24 1 3 24 (NTL(I), NTN(I), TLN(I), DTN(I), I =1, NG) 0 1 5.57275E-01 4.15705E-02 1 6 5.98845E-01 8.55946E-02 7 17 1.11241E+00 8.54274E-02 QINI, QMAX, (QV(I), TV(I), I =0, NT) 1.30000E+00 1.00000E+05 1.30000E+00 5.57275E-01 1.40000E+00 5.98845E-01 1.64727E+00 6.84440E-01 1.96658E+00 7.70034E-01 2.38526E+00 8.55629E-01 2.94342E+00 9.41223E-01 3.70108E+00 1.02682E+00 4.75000E+00 1.11241E+00 6.23021E+00 1.19784E+00 8.37178E+00 1.28327E+00 1.15499E+01 1.36869E+00 1.63983E+01 1.45412E+00 2.40214E+01 1.53955E+00 3.64069E+01 1.62498E+00 5.72629E+01 1.71040E+00 9.37788E+01 1.79583E+00 1.60488E+02 1.88126E+00 2.88130E+02 1.96669E+00 5.45004E+02 2.05211E+00 1.09118E+03 2.13754E+00 2.32426E+03 2.22297E+00 5.29613E+03 2.30840E+00 1.29876E+04 2.39382E+00 3.45020E+04 2.47925E+00 1.00000E+05 2.56468E+00 XMIN, XCR, (XV(I), I =1, NX) 1.00000E-08 1.50000E+00 1.00000E-08 1.17803E-08 1.38778E-08 1.63489E-08 1.92599E-08 2.26892E-08 2.67291E-08 3.14884E-08 3.70950E-08 4.36999E-08 5.14807E-08 6.06469E-08 7.14452E-08 8.41659E-08 9.91515E-08 1.16805E-07 1.37602E-07 1.62101E-07 1.90962E-07 2.24961E-07 2.65013E-07 3.12195E-07 3.67777E-07 4.33253E-07 5.10385E-07 6.01248E-07 7.08284E-07 8.34965E-07 9.83595E-07 1.15868E-06 1.36492E-06 1.60787E-06 1.89406E-06 2.23117E-06 2.62841E-06 3.09641E-06 3.64773E-06 4.29722E-06 5.06234E-06 5.96367E-06 7.02548E-06 8.27631E-06 9.74982E-06 1.14856E-05 1.35304E-05 1.59392E-05 1.87766E-05 2.21191E-05 2.60564E-05 3.06942E-05 3.61571E-05 4.25918E-05 5.01709E-05 5.90977E-05 6.96115E-05 8.19937E-05 9.65758E-05 1.13747E-04 1.33967E-04 1.57774E-04 1.85802E-04 2.18795E-04 2.57627E-04 3.03325E-04 3.57094E-04 4.20343E-04 4.94725E-04 5.82239E-04 6.85007E-04 8.05733E-04 9.47515E-04 1.11390E-03 1.30904E-03 1.53770E-03 1.80543E-03 2.11857E-03 2.48437E-03 2.91111E-03 3.40814E-03 3.98598E-03 4.65639E-03 5.43234E-03 6.32831E-03 7.35986E-03 8.54125E-03 9.89379E-03 1.14309E-02 1.31758E-02 1.51436E-02 1.73523E-02 1.98189E-02 2.25606E-02 2.55851E-02 2.89092E-02 3.25397E-02 3.64826E-02 4.07414E-02 4.53168E-02 5.02071E-02 5.54085E-02 6.09151E-02 6.67197E-02 7.28133E-02 7.91861E-02 8.58274E-02 9.27257E-02 9.98695E-02 1.07243E-01 1.14848E-01 1.22661E-01 1.30677E-01 1.38873E-01 1.47265E-01 1.55821E-01 1.64539E-01 1.73408E-01 1.82435E-01 1.91589E-01 2.00875E-01 2.10284E-01 2.19811E-01 2.29449E-01 2.39192E-01 2.49036E-01 2.58974E-01 2.69003E-01 2.79118E-01 2.89315E-01 2.99590E-01 3.09940E-01 3.20361E-01 3.30848E-01 3.41402E-01 3.52019E-01 3.62695E-01 3.73426E-01 3.84208E-01 3.95063E-01 4.05950E-01 4.16887E-01 4.27870E-01 4.38898E-01 4.49969E-01 4.61082E-01 4.72234E-01 4.83424E-01 4.94651E-01 5.05914E-01 5.17211E-01 5.28541E-01 5.39903E-01 5.51296E-01 5.62718E-01 5.74170E-01 5.85653E-01 5.97163E-01 6.08683E-01 6.20243E-01 6.31826E-01 6.43433E-01 6.55063E-01 6.66715E-01 6.78389E-01 6.90084E-01 7.01799E-01 7.13535E-01 7.25289E-01 7.37063E-01 7.48855E-01 7.60668E-01 7.72487E-01 7.84333E-01 7.96195E-01 8.08073E-01 8.19966E-01 8.31874E-01 8.43797E-01 8.55734E-01 8.67686E-01 8.79651E-01 8.91628E-01 9.03624E-01 9.15628E-01 9.27645E-01 9.39675E-01 9.51717E-01 9.63770E-01 9.75836E-01 9.87912E-01 1.00000E+00 Parton Distribution Table: 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 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0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 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0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00 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2.25964E+06 1.77865E+06 1.39939E+06 1.10048E+06 8.65002E+05 6.79586E+05 5.33656E+05 4.18857E+05 3.28591E+05 2.57651E+05 2.01927E+05 1.58176E+05 1.23844E+05 9.69160E+04 7.58067E+04 5.92671E+04 4.63148E+04 3.61769E+04 2.82461E+04 2.20450E+04 1.71988E+04 1.34135E+04 1.04581E+04 8.15206E+03 6.35229E+03 4.95039E+03 3.85783E+03 3.00652E+03 2.34355E+03 1.82742E+03 1.42567E+03 1.11302E+03 8.69705E+02 6.80353E+02 5.32967E+02 4.18213E+02 3.28823E+02 2.59145E+02 2.04787E+02 1.62328E+02 1.29113E+02 1.03135E+02 8.27080E+01 6.66647E+01 5.39901E+01 4.39679E+01 3.60130E+01 2.96749E+01 2.46001E+01 2.05267E+01 1.72341E+01 1.45608E+01 1.23782E+01 1.05858E+01 9.10488E+00 7.87370E+00 6.84359E+00 5.97614E+00 5.24102E+00 4.61413E+00 4.07632E+00 3.61229E+00 3.20977E+00 2.85883E+00 2.55168E+00 2.28122E+00 2.04262E+00 1.83122E+00 1.64366E+00 1.47629E+00 1.32699E+00 1.19340E+00 1.07370E+00 9.66086E-01 8.69467E-01 7.82476E-01 7.04094E-01 6.33406E-01 5.69611E-01 5.12005E-01 4.59964E-01 4.12937E-01 3.70431E-01 3.32012E-01 2.97288E-01 2.65909E-01 2.37562E-01 2.11962E-01 1.88862E-01 1.68019E-01 1.49232E-01 1.32312E-01 1.17088E-01 1.03414E-01 9.11149E-02 8.01079E-02 7.02538E-02 6.14467E-02 5.35899E-02 4.65952E-02 4.03818E-02 3.48761E-02 3.00105E-02 2.57232E-02 2.19574E-02 1.86612E-02 1.57864E-02 1.32892E-02 1.11291E-02 9.26899E-03 7.67507E-03 6.31602E-03 5.16323E-03 4.19284E-03 3.37874E-03 2.70129E-03 2.14152E-03 1.68248E-03 1.30911E-03 1.00806E-03 7.67603E-04 5.77498E-04 4.28844E-04 3.13986E-04 2.26388E-04 1.60532E-04 1.11751E-04 7.62807E-05 5.09215E-05 3.31824E-05 2.10558E-05 1.29758E-05 7.74407E-06 4.46336E-06 2.47836E-06 1.32405E-06 6.81186E-07 3.39204E-07 1.65005E-07 7.94485E-08 3.80693E-08 1.78443E-08 7.75077E-09 2.80816E-09 7.08814E-10 8.73364E-11 0.00000E+00 pythia8-8.1.80.orig/xmldoc/ErrorChecks.xml0000444000175000017500000001001012217346302016541 0ustar sunsun

      Error Checks

      There is a few settings related to error checking during program execution. Many other checks are performed as well, but do not have any specific setting related to themselves. There are a few ways in which an event can be vetoed, the most common being a User Hooks test. Normally this will simply mean that the next parton-level configuration is selected inside the Pythia::next() routine, without any need for a user intervention. With this option switched on, however, Pythia::next() will return false. It is then up to the user to decide what to do next. Check the particle data tables for potential problems during initialization. This includes inconsistent use of charge in particle names, inconsistent setup of mass, mass range, width and lifetime, sum of branching ratios not unity (allowed but discouraged) or charge not conserved in a decay channel. Warnings should be viewed as reasons to check further, but need not indicate a true problem, and also not all problems may be caught. The pythia.particleData.checkTable(level) method, used for these checks, may also be called directly. The level of verbosity and checks of particle data, if switched on. When an event has been successfully generated, check that the final event record in event does not contain any unphysical particles, or nonconserved charge or energy-momentum. If this check fails, then pythia.next() obtains the value false, i.e. the event is counted as aborted. When Check:event = on and the event is checked as above, further checks are made that all mother and daughter pointers are consistently set. Specifically that all daughters in the daughterlist (or motherList) have the particle in their respective motherList (or daughterlist). This operation takes a bit more time than the other error tests (of the order of 10% of what it takes to generate the event in the first place), and so could be switched off to save time. The number of erroneous events, in the above check, for which event listing and other detailed information will be printed. After that, only the normal error messages will be issued. Error counters are always updated, and accumulated numbers can be shown with pythia.statistics() at the end of the run. Maximum allowed summed deviation of E, p_x, p_y and p_z between the incoming beams and the final state, as a fraction of the initial energy, above which the event is counted as aborted. (Unfortunately roundoff errors do not scale linearly with the energy, and also have a very long tail. So while most events at lower energies may be correct to better than 1e-10, at LHC it does not have to signal any fundamental bug if also the default tolerance above is violated occasionally.) A check on the same summed deviation as above, but counted as a warning rather than an error, and not leading to the event being classified as aborted.
      pythia8-8.1.80.orig/xmldoc/Fragmentation.xml0000444000175000017500000003436412217346303017150 0ustar sunsun

      Fragmentation

      Fragmentation in PYTHIA is based on the Lund string model And83, Sjo84. Several different aspects are involved in the physics description, which here therefore is split accordingly. This also, at least partly, reflect the set of classes involved in the fragmentation machinery.

      The variables collected here have a very wide span of usefulness. Some would be central in any hadronization tuning exercise, others should not be touched except by experts.

      The fragmentation flavour-choice machinery is also used in a few other places of the program, notably particle decays, and is thus described on the separate Flavour Selection page.

      Fragmentation functions

      The StringZ class handles the choice of longitudinal lightcone fraction z according to one of two possible shape sets.

      The Lund symmetric fragmentation function And83 is the only alternative for light quarks. It is of the form f(z) = (1/z) * (1-z)^a * exp(-b m_T^2 / z) with the two main free parameters a and b to be tuned to data. They are stored in The a parameter of the Lund symmetric fragmentation function. The b parameter of the Lund symmetric fragmentation function.

      In principle, each flavour can have a different a. Then, for going from an old flavour i to a new j one the shape is f(z) = (1/z) * z^{a_i} * ((1-z)/z)^{a_j} * exp(-b * m_T^2 / z) This is only implemented for diquarks relative to normal quarks: allows a larger a for diquarks, with total a = aLund + aExtraDiquark.

      Finally, the Bowler modification Bow81 introduces an extra factor 1/z^{r_Q * b * m_Q^2} for heavy quarks. To keep some flexibility, a multiplicative factor r_Q is introduced, which ought to be unity (provided that quark masses were uniquely defined) but can be set in r_c, i.e. the above parameter for c quarks. r_b, i.e. the above parameter for b quarks. r_h, i.e. the above parameter for heavier hypothetical quarks, or in general any new coloured particle long-lived enough to hadronize.

      Within the string framework, the b parameter is universal, i.e. common for all flavours. Nevertheless, for fits to experimental data, better agreement can be obtained if both a_Q and b_Q can be set freely in a general expression f(z) = 1/z^{1 + r_Q * b_Q * m_Q^2} * (1-z)^a_Q * exp(-b_Q m_T^2 / z) The below switches and values can be used to achieve this. They should be used with caution and constitute clear deviations from the Lund philosophy. use the above nonstandard Lund ansatz for c quarks. use the above nonstandard Lund ansatz for b quarks. use the above nonstandard Lund ansatz for hypothetical heavier quarks. The a parameter in the nonstandard Lund ansatz for c quarks. The a parameter in the nonstandard Lund ansatz for b quarks. The a parameter in the nonstandard Lund ansatz for hypothetical heavier quarks. The b parameter in the nonstandard Lund ansatz for c quarks. The b parameter in the nonstandard Lund ansatz for b quarks. The b parameter in the nonstandard Lund ansatz for hypothetical heavier quarks.

      As another nonstandard alternative, it is possible to switch over to the Peterson/SLAC formula Pet83 f(z) = 1 / ( z * (1 - 1/z - epsilon/(1-z))^2 ) for charm, bottom and heavier (defined as above) by the three flags use Peterson for c quarks. use Peterson for b quarks. use Peterson for hypothetical heavier quarks.

      When switched on, the corresponding epsilon values are chosen to be epsilon_c, i.e. the above parameter for c quarks. epsilon_b, i.e. the above parameter for b quarks. epsilon_h, i.e. the above parameter for hypothetical heavier quarks, normalized to the case where m_h = m_b. The actually used parameter is then epsilon = epsilon_h * (m_b^2 / m_h^2). This allows a sensible scaling to a particle with an unknown higher mass without the need for a user intervention.

      Fragmentation pT

      The StringPT class handles the choice of fragmentation pT. At each string breaking the quark and antiquark of the pair are supposed to receive opposite and compensating pT kicks according to a Gaussian distribution in p_x and p_y separately. Call sigma_q the width of the p_x and p_y distributions separately, i.e. d(Prob) = exp( -(p_x^2 + p_y^2) / 2 sigma_q^2). Then the total squared width is <pT^2> = <p_x^2> + <p_y^2> = 2 sigma_q^2 = sigma^2. It is this latter number that is stored in the width sigma in the fragmentation process.

      Since a normal hadron receives pT contributions for two string breakings, it has a <p_x^2>_had = <p_y^2>_had = sigma^2, and thus <pT^2>_had = 2 sigma^2.

      Some studies on isolated particles at LEP has indicated the need for a slightly enhanced rate in the high-pT tail of the above distribution. This would have to be reviewed in the context of a complete retune of parton showers and hadronization, but for the moment we stay with the current recipe, to boost the above pT by a factor enhancedWidth for a small fraction enhancedFraction of the breakups, where enhancedFraction,the fraction of string breaks with enhanced width. enhancedWidth,the enhancement of the width in this fraction.

      Jet joining procedure

      String fragmentation is carried out iteratively from both string ends inwards, which means that the two chains of hadrons have to be joined up somewhere in the middle of the event. This joining is described by parameters that in principle follows from the standard fragmentation parameters, but in a way too complicated to parametrize. The dependence is rather mild, however, so for a sensible range of variation the parameters in this section should not be touched. Is used to define a W_min = m_q1 + m_q2 + stopMass, where m_q1 and m_q2 are the masses of the two current endpoint quarks or diquarks. Add to W_min an amount stopNewFlav * m_q_last, where q_last is the last q qbar pair produced between the final two hadrons. The W_min above is then smeared uniformly in the range W_min_smeared = W_min * [ 1 - stopSmear, 1 + stopSmear ].

      This W_min_smeared is then compared with the current remaining W_transverse to determine if there is energy left for further particle production. If not, i.e. if W_transverse < W_min_smeared, the final two particles are produced from what is currently left, if possible. (If not, the fragmentation process is started over.)

      Simplifying systems

      There are a few situations when it is meaningful to simplify the original task, one way or another. Decides whether a partonic system should be considered as a normal string or a ministring, the latter only producing one or two primary hadrons. The system mass should be above mStringMin plus the sum of quark/diquark constituent masses for a normal string description, else the ministring scenario is used. When two colour-connected partons are very nearby, with at least one being a gluon, they can be joined into one, to avoid technical problems of very small string regions. The requirement for joining is that the invariant mass of the pair is below mJoin, where a gluon only counts with half its momentum, i.e. with its contribution to the string region under consideration. (Note that, for technical reasons, the 0.2 GeV lower limit is de facto hardcoded.) When the invariant mass of two of the quarks in a three-quark junction string system becomes too small, the system is simplified to a quark-diquark simple string. The requirement for this simplification is that the diquark mass, minus the two quark masses, falls below mJoinJunction. Gluons on the string between the junction and the respective quark, if any, are counted as part of the quark four-momentum. Those on the two combined legs are clustered with the diquark when it is formed.

      Ministrings

      The MiniStringFragmentation machinery is only used when a string system has so small invariant mass that normal string fragmentation is difficult/impossible. Instead one or two particles are produced, in the former case shuffling energy-momentum relative to another colour singlet system in the event, while preserving the invariant mass of that system. With one exception parameters are the same as defined for normal string fragmentation, to the extent that they are at all applicable in this case. A discussion of the relevant physics is found in Nor00. The current implementation does not completely abide to the scheme presented there, however, but has in part been simplified. (In part for greater clarity, in part since the class is not quite finished yet.) Whenever the machinery is called, first this many attempts are made to pick two hadrons that the system fragments to. If the hadrons are too massive the attempt will fail, but a new subsequent try could involve other flavour and hadrons and thus still succeed. After nTry attempts, instead an attempt is made to produce a single hadron from the system. Should also this fail, some further attempts at obtaining two hadrons will be made before eventually giving up.

      Junction treatment

      A junction topology corresponds to an Y arrangement of strings i.e. where three string pieces have to be joined up in a junction. Such topologies can arise if several valence quarks are kicked out from a proton beam, or in baryon-number-violating SUSY decays. Special attention is necessary to handle the region just around the junction, where the baryon number topologically is located. The junction fragmentation scheme is described in Sjo03. The parameters in this section should not be touched except by experts. Used to find the effective rest frame of the junction, which is complicated when the three string legs may contain additional gluons between the junction and the endpoint. To this end, a pull is defined as a weighed sum of the momenta on each leg, where the weight is exp(- eSum / eNormJunction), with eSum the summed energy of all partons closer to the junction than the currently considered one (in the junction rest frame). Should in principle be (close to) sqrt((1 + a) / b), with a and b the parameters of the Lund symmetric fragmentation function. Retry (up to 10 times) when the first two considered strings in to a junction both have a remaining energy (in the junction rest frame) above this number. Retry (up to 10 times) when the first two considered strings in to a junction has a highest remaining energy (in the junction rest frame) above a random energy evenly distributed between eBothLeftJunction and eBothLeftJunction + eMaxLeftJunction (drawn anew for each test). Retry (up to 10 times) when the invariant mass-squared of the final leg and the leftover momentum of the first two treated legs falls below eMinLeftJunction times the energy of the final leg (in the junction rest frame).
      pythia8-8.1.80.orig/xmldoc/SUSYProcesses.xml0000444000175000017500000003572012217346317017046 0ustar sunsun

      SUSY

      Here is collected processes involving supersymmetric particle production, with the exception of the (extended) Higgs sector. Since the number of separate but closely related processes is so big, there will not be switches for each separate process but only for a reasonable set of subgroups. However, the general switches SUSY:idA and SUSY:idB,valternatively vectors SUSY:idVecA and SUSY:idVecB, may be used in conjunction with any of these groups to provide some additional flexibility to concentrate on processes involving only specific (s)particle final states, see below.

      Most of the SUSY implementation in PYTHIA 8 has been written by N. Desai and is documented in Des11. Please give due credit to external contributions to PYTHIA 8, such as this one, by including the original work in your list of references when using this implementation. The cross section formulae are mostly taken from Boz07 and Fuk11.

      Since the implementation of SUSY processes was only recently completed Des11, case-by-case validations against other codes are still recommended. A set of default validations have already been carried out by the authors, comparing to the PYTHIA 6 SUSY implementation and to the XSUSY code, using an sps1a spectrum. Explicit validations of the non-trivial SLHA2-specific extensions have generally not been carried out yet, with the exception of the R-parity violating single-sparticle production cross sections. Please report the results of any user validations you may carry out to the authors.

      Important Note on SLHA: In order to simulate SUSY processes it is required to read in the couplings and masses relevant for the scenario to be studied. This is done with the help of the SUSY Les Houches Accord (SLHA), including the SLHA2 extensions and generalizations. (Internally, the SLHA2 conventions are used. SLHA1 spectra are automatically translated into SLHA2 notation during initialization.) The reading of a relevant SLHA file must be set up, as described on the SLHA page. Attempting to generate SUSY processes without a properly initialized SLHA spectrum is strongly discouraged and may lead to unexpected results. Always check for warnings and errors reported by the SLHA reader during the initialization stage.

      SUSY Processes

      Note 1: Decays of SUSY particles are described separately below. Note 2: One special possibility is that the gluino or some squark(s) are sufficiently long-lived to hadronize. See the R-hadrons page for further details. Note 3: lepton- and photon-initial states are not yet available. Only quark/gluon-initiated 2 -> 2 and 2 -> 1 (RPV) processes have been implemented. Note 4: cross sections will be correctly folded with open branching fractions of cascade decays, but at present any difference between particle and antiparticle decay tables is not taken into account. This possibility will be included in a future update. Common switch for production of supersymmetric particles, i.e. particles with R-parity -1. Option to limit the sum over possible outgoing states in SUSY 2 -> 2 processes to ones including a specific particle identity code. The default corresponds to summing over all possible indices. A non-zero value of SUSY:idA selects only processes that contain the state corresponding to that particular particle identity code in the fundamental 2 -> 2 scattering process (summed over particle/antiparticle). It is the user's responsibility to ensure that (a subset of) the processes to be simulated actually include this particle at the 2 -> 2 level; thus, asking for the lightest neutralino (code 1000021) to be present in a squark-squark production process will give no match. As for SUSY:idA, but requires an additional particle with PDG code SUSY:idB to be present in the 2 -> 2 process. Thus, using SUSY:idA and SUSY:idB a specific subprocess can be selected. Again only the absolute sign is used, i.e. the summation over particle and antiparticle is retained. Also the order of SUSY:idA and SUSY:idB is irrelevant; since both possible orderings are checked for a match with the two outgoing particles. (Although not recommended, should SUSY:idA be zero and SUSY:idB nonzero a match is searched for just like in the normal case with SUSY:idA nonzero and SUSY:idB zero.) As for SUSY:idA, but as a vector of PDG codes. (Character-string input of such vectors should be as a comma-separated list, without any blanks.) Thus, it selects only processes that have a final-state particle corresponding to one of the identity codes in this vector. Note that, to activate this, SUSY:idA must be equal to zero; if not then the match to SUSY:idA takes precedence. As for SUSY:idB, but as a vector of PDG codes. (Character-string input of such vectors should be as a comma-separated list, without any blanks.) As above, to activate this, SUSY:idB must be equal to zero; if not then the match to SUSY:idB takes precedence. For the matching, either of SUSY:idA and SUSY:idVecA may be combined with either of SUSY:idB and SUSY:idVecB. As above one of the two outgoing SUSY particles must match one of the particles in SUSY:id(Vec)A and the other one of the particles in SUSY:id(Vec)B when both are nonzero. The value of sin2(thetaW) should be taken from

      Gluino Pair Production

      Pair production of gluinos by gluon-gluon initial states. Pair production of gluinos by quark-antiquark annihilation and t-channel squark exchange. The cross section expression follows Fuk11 and include the possibility of non-minimal flavour violation through misalignment of quarks with squarks. Only the MFV case has been explicitly validated.

      Associated Squark-Gluino Production

      Associated production of a squark with a gluino. The cross section expression follows Fuk11 and include the possibility of non-minimal flavour violation through misalignment of quarks with squarks. Only the MFV case has been explicitly validated.

      Squark Pair Production

      Pair production of a scalar quark together with a scalar antiquark by gluon annihilation via s-channel gluon exchange, t- and u-channel squark exchange, and the direct 4-point coupling. The cross section expression follows Boz07. Only the MFV case has been explicitly validated. Pair production of a scalar quark together with a scalar antiquark by quark-antiquark annihilation. For same-isospin ~q~q* production (i.e., ~u~u*, ~u~c*, ...), the s-channel gluon, photon, and Z and t-channel gluino contributions have so far been implemented (i.e., the t-channel neutralino contributions are neglected). For opposite-isospin ~q~q* production (~u~d*, ~u~s*, ...), the s-channel W and t-channel gluino contributions have been implemented (i.e., the t-channel neutralino contributions are neglected). The cross section expressions follow Boz07. Only the MFV case has been explicitly validated. (Note to PYTHIA 6 users: in older PYTHIA 6 versions, a bug caused the ~t1~t2* cross to be overcounted by a factor of 2. Starting from version 6.4.24, that generator now agrees with the implementation here.) When switched on this flag switches off all but the s-channel gluon contribution in the calculation of same-isospin squark-antisquark production cross sections. Intended for reference only. For the most accurate physics simulation, leave this flag in the off position. Pair production of scalar quarks (squark-squark and its charge conjugate process; for squark-antisquark production see above) by t- and u-channel gluino, neutralino, and chargino exchange. The cross section expressions follow Boz07. Only the MFV case has been explicitly validated. (Note to PYTHIA 6 users: PYTHIA 6 only included the gluino exchange contribution, which typically dominates due to the size of the strong coupling; for counterchecks, the flag SUSY:qq2squarksquark:onlyQCD below can be switched on to eliminate the chargino and neutralino contributions.) When switched on this flag causes the t- or u-channel neutralino and chargino contributions to be ignored in the calculation of squark pair production cross sections. Intended for reference only. For the most accurate physics simulation, leave this flag in the off position.

      Neutralino and Chargino Pair Production

      Pair production of neutralinos by quark-antiquark annihilation. With four neutralino species this gives ten separate processes, codes 1201 - 1210. The cross section expressions follow Boz07. Only the MFV case has been explicitly validated. Associated chargino-neutralino production by quark-antiquark annihilation. With four neutralino species, two chargino ones, and maintaining charge conjugate processes separate, this gives 16 separate processes, codes 1221 - 1236. The cross section expressions follow Boz07. Only the MFV case has been explicitly validated. Pair production of charginos by quark-antiquark annihilation. With two chargino species and maintaining mutually charge conjugate processes separate, this gives four separate processes, codes 1241 - 1244. The cross section expressions follow Boz07. Only the MFV case has been explicitly validated.

      Associated Neutralino/Chargino + Squark/Gluino Production

      Pair production of neutralinos from quark-gluon initial states. The cross section expressions follow Boz07. Only the MFV case has been explicitly validated. Associated chargino-squark production from quark-gluon initial states. annihilation. The cross section expressions follow Boz07. Only the MFV case has been explicitly validated. Associated neutralino-gluino production by quark-antiquark annihilation. The cross section expressions follow Fuk11. Only the MFV case has been explicitly validated. Associated chargino-gluino production by quark-antiquark annihilation. The cross section expressions follow Fuk11. Only the MFV case has been explicitly validated. (Note to PYTHIA 6 users: small differences between this implementation and PYTHIA 6 arise due to slightly different treatments of the weak mixing angle, which is fixed in PYTHIA 6, while it is computed from the SLHA input in PYTHIA 8; see SUSY:sin2thetaWMode above.)

      Slepton Production

      Pair production of slepton-antislepton via s-channel W, Z and gamma exchange. Includes both charged sleptons and sneutrinos but right handed sneutrinos currently not supported.

      R-parity violating squark production

      Resonant squark production via R-parity violating UDD couplings. The couplings must be input using the SLHA2 structure.

      Decays of SUSY Particles

      Based on the parameters read in from the SLHA, PYTHIA 8 will normally compute the decay modes of SUSY particles automatically, using the SusyResonanceDecays class(es). Essentially all tree-level 2-body decays in the MSSM have been implemented this way, excepting so far only those involving Higgs bosons (either in the in- or out-state) or gravitinos. Available channels so far include:
      • ~q → q + ~chi
      • ~q → ~q + W/Z
      • ~q → q + q (RPV UDD)
      • ~q → l + q (RPV LQD)
      • ~g → ~q + q
      • ~chi → ~chi + Z/W
      • ~chi → ~q + q
      • ~chi → ~l/~nu + l/nu
      • ~chi0 → q + q + q (RPV UDD)
      • ~l/~nu → l/nu + ~chi
      • ~l/~nu → ~l/~nu + W/Z
      All channels are still undergoing validation, so this implementation should be considered preliminary. Still missing but to be included in a forthcoming update are: 3-body decays of charginos (via RPV), and 2-body decays of squarks and gauginos with Higgs as one of the decay products. Some 3-body decays have been implemented with Matrix Element weighting. In particular, those for a neutralino to a lighter neutralino and a fermion pair can be enabled. When "on", the spin-averaged, squared matrix element is used to sample the phase space for resonance decay. Currently, only possible for a heavy neutralino decay to a light neutralino and a fermion-antifermion pair.
      pythia8-8.1.80.orig/xmldoc/ExtraDimensionalProcesses.xml0000444000175000017500000005223412217346302021502 0ustar sunsun

      Extra-Dimensional Processes

      Scenarios with extra dimensions (ED) allow a multitude of processes. Currently three different categories of processes are implemented. The first involves the production of excited Kaluza Klein states within so-called Randall-Sundrum (RS) scenarios, the second is related to resonance production in TeV-1 sized extra dimensions and the third relates to phenomena from large extra dimensions (LED). Due to the close relation between the LED model and a so-called unparticle model, similar unparticle processes are also kept in this section.

      Randall-Sundrum Resonances, production processes

      The graviton (G*) and gluon (KKgluon*) resonance states are assigned PDG code 5100039 and 5100021 respectively. The G* processes are described in Bij01 and the KKgluon* process in Ask11. Decays into fermion and boson pairs are handled with the correct angular distributions, while subsequent decays are handled isotropically.

      There are two lowest-order processes that together normally should be sufficient for a simulation of G^* production. Common switch for the group of lowest-order G^* production processes, i.e. the two ones below. Scatterings g g -> G^*. Code 5001. Scatterings f fbar -> G^*. Code 5002.

      In addition there are three first-order processes included. These are of less interest, but can be used for dedicated studies of the high-pT tail of G^* production. As usual, it would be double counting to include the lowest-order and first-order processes simultaneously. Therefore the latter ones are not included with the ExtraDimensionsG*:all = on option. In this set of processes all decay angles are assumed isotropic. Scatterings g g -> G^* g. Code 5003. Scatterings q g -> G^* q. Code 5004. Scatterings q qbar -> G^* g. Code 5005.

      There is also one process for the production of a gluon resonance. Scatterings q qbar -> g^*/KKgluon^*. Code 5006.

      Randall-Sundrum Resonances, parameters

      In the above scenario the main free parameters are the masses, which are set as usual. In addition there are the following coupling parameters. The coupling kappaMG follows the conventions in Bij01, where as the flavour dependent couplings follow the conventions used in Dav01. Parameter to choose between the two scenarios: off, SM on the TeV brane (common kappaMG coupling); on, SM in the ED bulk (flavour dependent couplings). This parameter is only relevant for the lowest-order graviton (G*) processes, where as the first-order processes corresponds to the off scenario. Parameter to specify Z/W coupling scenario: off, usual Z/W boson couplings; on, coupling only to longitudinal Z/W bosons. In both cases the GZZ and GWW values are used and this parameter is only relevant when SMinBulk = on. The formulas for longitudinal bosons should be appropriate up to O(m_V/E_V) corrections. dimensionless coupling, which enters quadratically in all partial widths of the G^*. Is kappa m_G* = sqrt(2) x_1 k / Mbar_Pl, where x_1 = 3.83 is the first zero of the J_1 Bessel function and Mbar_Pl is the modified Planck mass. Coupling between graviton and leptons. Coupling between graviton and light quarks. Coupling between graviton and bottom quark. Coupling between graviton and top quark. Coupling between graviton and gluon. Coupling between graviton and gamma. Coupling between graviton and Z boson. Coupling between graviton and W boson. Coupling between graviton and Higgs bosons. Coupling between KK-gluon and a right-handed light quark. Coupling between KK-gluon and a left-handed light quark. Coupling between KK-gluon and a right-handed bottom quark. Coupling between KK-gluon and a left-handed bottom quark. Coupling between KK-gluon and a right-handed top quark. Coupling between KK-gluon and a left-handed top quark. Choice of full g^*/KK-gluon^* structure or not in relevant processes.

      TeV^-1 Sized Extra Dimension, production processes

      This section contains a processes involving the production of electroweak KK gauge bosons, i.e. gamma_{KK}/Z_{KK}, in one TeV^-1 sized extra dimension. The process is described in Bel10 and allows for individual final states to be specified. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> d dbar , Code 5061. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> u ubar , Code 5062. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> s sbar , Code 5063. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> c cbar , Code 5064. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> b bbar , Code 5065. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> t tbar , Code 5066. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> e+ e- , Code 5071. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> nue nuebar , Code 5072. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> mu+ mu- , Code 5073. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> numu numubar , Code 5074. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> tau+ tau- , Code 5075. Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> nutau nutaubar , Code 5076.

      TeV^-1 Sized Extra Dimension, parameters

      Irrespective of the parameter options used, the particle produced, gamma_{KK}/Z_{KK}, will always be assigned code 5000023. Choice of full gamma_{KK}/Z_{KK} structure or not in relevant processes. The number of included KK excitations. The KK mass m^*, given by the inverse of the single extra dimension radius.

      Large Extra Dimensions, production processes

      The LED graviton, where the KK-modes normally are summed and do not give rise to phenomena individually, is assigned PDG code 5000039. The graviton emission and virtual graviton exchange processes use the same implementation as the corresponding unparticle processes, which are all described in Ask10. It is also possible to generate monojet events from scalar graviton emission as described in Azu05, by turning on the option GravScalar.

      Note: As discussed in Ask09, for the graviton or unparticle emission processes the underlying Breit-Wigner mass distribution should be matched to the graviton mass spectrum in order to achieve an optimal MC efficiency.

      The following lowest order graviton emission processes are available. Common switch for the group of lowest-order G jet emission processes, i.e. the three ones below. Scatterings g g -> G g. Code 5021. Scatterings q g -> G q. Code 5022. Scatterings q qbar -> G g. Code 5023. Scatterings f fbar -> G Z. Code 5024. Scatterings f fbar -> G gamma. This process corresponds to the photon limit of the G Z process, as described in Ask09. Code 5025.

      The following LED processes with virtual graviton exchange are available. Scatterings f fbar -> (LED G*) -> gamma gamma. If the graviton contribution is zero, the results corresponds to the SM contribution, i.e. equivalent to PromptPhoton:ffbar2gammagamma. Code 5026. Scatterings g g -> (LED G*) -> gamma gamma. Code 5027. Scatterings f fbar -> (LED G*) -> l l , where l is a charged lepton. If the graviton contribution is zero, the results corresponds to the SM contribution, i.e. similar to WeakSingleBoson:ffbar2gmZ. Does not include t-channel amplitude relevant for e^+e^- to e^+e^- and no K-factor is used. Code 5028. Scatterings g g -> (LED G*) -> l l. Code 5029.

      Dijet production including graviton exchange is also available, using the same effective theory approach as the LED G exchange processes above or including more detailed amplitudes in accordance with Fra11. In case of the latter, the value of LambdaT is used as the value of the cut-off scale Lambda. For this reason the dijet processes only relates to the LED model and no unparticle versions are available. The processes are grouped together like their HardQCD equivalents and should therefore converge to the same results in the limit of an insignificant graviton contribution.

      Warning: These LED dijets processes are still being validated. Common switch for the group of lowest-order jet jet production processes with graviton exchange, i.e. the six ones below. Scatterings g g -> (LED G*) -> g g. Code 5030. Scatterings g g -> (LED G*) -> q qbar. Number of outgoing flavours specified by nQuarkNew parameter below. Code 5031. Scatterings q g -> (LED G*) -> q g and qbar g -> (LED G*) -> qbar g. Code 5032. Scatterings q q(bar)' -> (LED G*) -> q q(bar)'. Including q and qbar of same or different flavours, but the outgoing flavours equals the incoming ones. Code 5033. Scatterings q qbar -> (LED G*) -> g g. Code 5034. Scatterings q qbar -> (LED G*) -> q' qbar'. Number of outgoing flavours specified by nQuarkNew parameter below. Code 5035.

      Large Extra Dimensions, parameters

      Allow the monojet processes to produce scalar graviton emission instead of the default tensor one. The scalar option is according to the processes described in Azu05 and includes two coupling constants below. Number of extra dimensions. Fundamental scale of gravity in D = 4 + n dimensions. Ultraviolet cutoff parameter for the virtual graviton exchange processes. Allows to change sign of the interference terms in the graviton exchange processes, common in connection to using the Hewett convention Hew99. Options for when the hard scale of the process (e.g. sHat) approaches or exceed the scale of validity of the low energy effective theory (e.g. M_D). Note: Option 1 only concerns the graviton emission processes and the form factor is currently not available for the scalar graviton processes. Form factor parameter. Coupling related to scalar graviton emission. Coupling related to scalar graviton emission. Number of allowed outgoing new quark flavours in the above q qbar -> (LED G*) -> q' qbar' and g g -> (LED G*) -> q' qbar' processes. Similar to HardQCD:nQuarkNew for the QCD processes. Options to specify S function for LED dijet amplitudes.

      Unparticles, production processes

      As mentioned above, the similar unparticle and graviton processes share the same implementations. The unparticle processes, however, only use the dedicated unparticle parameters below. The unparticle is also assigned the PDG code 5000039 and is therefore called Graviton in the event record. The graviton and unparticle emission as well as virtual graviton and unparticle exchange processes are described in Ask10.

      Note: As discussed in Ask09, for the graviton or unparticle emission processes the underlying Breit-Wigner mass distribution should be matched to the graviton mass spectrum in order to achieve an optimal MC efficiency.

      The following unparticle emission processes are available. Common switch for the group of lowest-order U jet emission processes, i.e. the three ones below. Scatterings g g -> U g. Code 5045. Scatterings q g -> U q. Code 5046. Scatterings q qbar -> U g. Code 5047. Scatterings f fbar -> U Z. Code 5041. Scatterings f fbar -> U gamma. This process corresponds to the photon limit of the U Z process, as described in Ask09. Code 5042.

      The following processes with virtual unparticle exchange are available. Scatterings f fbar -> (U*) -> gamma gamma. If the unparticle contribution is zero in the spin-2 case, the results corresponds to the SM contribution, i.e. equivalent to PromptPhoton:ffbar2gammagamma. Code 5043. Scatterings g g -> (U*) -> gamma gamma. Code 5044. Scatterings f fbar -> (U*) -> l lbar , where l is a charged lepton. If the unparticle contribution is zero, the results corresponds to the SM contribution, i.e. similar to WeakSingleBoson:ffbar2gmZ. Does not include t-channel amplitude relevant for e^+e^- to e^+e^- and no K-factor is used. Code 5048. Scatterings g g -> (U*) -> l lbar. Code 5049.

      Unparticles, parameters

      Unparticle spin. Scale dimension parameter. Unparticle renormalization scale. Unparticle coupling to the SM fields. Ratio, lambda'/lambda, between the two possible coupling constants of the spin-2 ME. Warning: A ratio value different from one give rise to an IR divergence which makes the event generation very slow, so this values is fixed to ratio = 1 for the moment. Options for when the hard scale of the process (e.g. sHat) approaches or exceed the scale of validity of the low energy effective theory (Lambda_U). This mode only concerns the unparticle emission processes. Chiral unparticle couplings, gXX = gLL = gRR. Only relevant for lepton production from spin-1 unparticle exchange. Chiral unparticle couplings, gXY = gLR = gRL. Only relevant for lepton production from spin-1 unparticle exchange.
      pythia8-8.1.80.orig/xmldoc/ImplementNewShowers.xml0000444000175000017500000006423112217346303020325 0ustar sunsun

      Implement New Showers

      In case you want to replace the PYTHIA initial- and final-state showers by your own, it is possible but not trivial. The point is that multiparton interactions (MPI), initial-state radiation (ISR) and final-state radiation (FSR) in general appear in one single interleaved sequence of decreasing pT values. Therefore shower replacements would have to be able to play the game by such rules, as we will outline further below. Of course, this still leaves the field open exactly how to define what to mean by pT, how to handle recoil effects, how the colour flow is affected, and so on, so there is certainly room for alternative showers. A first example of a shower implemented within the PYTHIA context is VINCIA, which however so far only handles FSR.

      For the moment we assume you want to keep the MPI part of the story unchanged, and make use of the existing beam-remnants (BR) machinery. If you want to replace both MPI, ISR, FSR and BR then you had better replace the whole PartonLevel module of the code. If, in addition, you want to produce your own hard processes, then you only need the hadron-level standalone part of the machinery.

      In order to write replacement codes for ISR and/or FSR it is useful to be aware of which information has to be shared between the different components, and which input/output structure is required of the relevant methods. For details, nothing beats studying the existing code. However, here we provide an overview, that should serve as a useful introduction.

      It should be noted that we here primarily address the problem in its full generality, with interleaved MPI, ISR and FSR. There exists an option TimeShower:interleave = off where only MPI and ISR would be interleaved and FSR be considered after these two, but still before BR. Most of the aspects described here would apply also for that case. By contrast, resonance decays are only considered after all the four above components, and timelike showers in those decays would never be interleaved with anything else, so are much simpler to administrate.

      Therefore the pythia.setShowerPtr( timesDecPtr, timesPtr, spacePtr) method allows two separate pointers to be set to instances of derived TimeShower classes. The first is only required to handle decays, say of Z^0 or Upsilon, with no dependence on beam remnants or ISR. The second, as well as spacePtr, has to handle the interleaved evolution of MPI, ISR and FSR. Therefore you are free to implement only the first, and let the PYTHIA default showers take care of the latter two. But, if you wanted to, you could also set timesDecPtr = 0 and only provide a timesPtr, or only a spacePtr. If your timelike shower does both cases, the first two pointers can agree. The only tiny point to take into account then is that init( beamAPtr, beamBPtr) is called twice, a first time to timesDecPtr with beam pointers 0, and a second time to timesPtr with nonvanishing beam pointers.

      The event record and associated information

      Obviously the main place for sharing information is the event record, specifically the Event event member of Pythia, passed around as a reference. It is assumed you already studied how it works, so here we only draw attention to a few aspects of special relevance.

      One basic principle is that existing partons should not be overwritten. Instead new partons should be created, even when a parton only receives a slightly shifted momentum and for the rest stays the same. Such "carbon copies" by final-state branchings should be denoted by both daughter indices of the original parton pointing to the copy, and both mother indices of the copy to the original. If the copy instead is intended to represent an earlier step, e.g. in ISR backwards evolution, the role of mothers and daughters is interchanged. The event.copy( iCopy, newStatus) routine can take care of this tedious task; the sign of newStatus tells the program which case to assume.

      To make the event record legible it is essential that the status codes are selected appropriately to represent the reason why each new parton is added to the record. Also remember to change the status of a parton to be negative whenever an existing parton is replaced by a set of new daughter partons.

      Another important parton property is scale(), which does not appear in the normal event listing, but only if you use the extended Event:listScaleAndVertex = on option. This property is supposed to represent the production scale (in GeV) of a parton. In the current FSR and ISR algorithms it is used to restrict from above the allowed pT values for branchings of this particular parton. Beam remnants and other partons that should not radiate are assigned scale 0.

      Auxiliary to the event record proper is the PartonSystems class, that keep track of which partons belong together in the same scattering subsystem. This information must be kept up-to-date during the shower evolution.

      For initial-state showers it is also necessary to keep track of the partonic content extracted from the beams. This information is stored in the BeamParticle class.

      The TimeShower interface

      If you want to replace the TimeShower class this would involve replacing the virtual methods among the following ones. The constructor does not need to do anything. The destructor does not need to do anything. This method only imports pointers to standard facilities, and is not virtual. You have to store your local copy of the pointers to these objects, since they have to be used during the generation, as explained above. The pointers could be zero; e.g. a local copy of TimeShower is created to handle showers in decays such as Upsilon -> q qbar from inside the ParticleDecays class. This is also the place to do initialization of whatever parameters you plan to use, e.g. by reading in them from a user-accessible database like the Settings one. The question is whether the FSR should be allowed to occur at larger scales than the hard process it surrounds. This is process-dependent, as illustrated below for the the analogous SpaeShower::limitPTmax(...) method, although the two kinds of radiation need not have to be modeled identically. The TimeShower:pTmaxMatch switch allows you to force the behaviour among three options, but you may replace by your own logic.
      The internal PYTHIA implementation also allows intermediate options, where emissions can go up to the kinematical limit but be dampened above the factorization or renormalization scale. Therefore the (square of the) latter two are provided as optional input parameters.
      Relative to the default pT_max evolution scale of the process, it may still be convenient to vary the matching slightly for the hardest interaction in an event, to probe the sensitivity to such details. The base-class implementation returns the value of the TimeShower:pTmaxFudge parameter. This is an all-in-one call for shower evolution, and as such cannot be used for the normal interleaved evolution, where only the routines below are used. It also cannot be used in resonance decays that form part of the hard process, since there the user hooks insert a potential veto step. Currently this routine is therefore only used in the hadron-level decays, e.g. Upsilon -> g g g.
      iBeg and iEnd is the position of the first and last parton of a separate system, typically produced by a resonance decay. Such a system only evolves in isolation, and in particular does not relate to the beams.
      The pTmax value sets the maximum scale for evolution, but normally you would restrict that further for each individual parton based on its respective scale value.
      The nBranchMax value, if positive, gives the maximum number of allowed branchings in the call, as useful for matching studies.
      The routine is expected to return the number of FSR branchings that were generated, but only for non-critical statistics purposes.
      Since the real action typically is delegated to the routines below, it may well be that the existing code need not be replaced.
      This is a further simplified version of the shower method above. Currently it only handles the emission of photons in the decay of a hadron into a pair of leptons, either a charged lepton-antilepton or a lepton-neutrino pair. It is properly matched to the matrix element in the decay via a virtual photon or W^+-, respectively. It is called as part of such decays if ParticleDecays:allowPhotonRadiation = on, which is not the default value. Can be used to return the pT evolution scale of the last branching in the cascade generated with the above shower(...) method. Is to be set in the internal pTLastInShower variable, and should be 0 if there were no branchings. Can be useful for matching studies. This method resets some counters and extracts the locations of outgoing partons, in preparation of using the optional global recoil scheme. Unlike prepare(...) below it is only called once during the parton-level evolution, since it only relates to the hardest interaction. Is probably of no use to most people. This method is called immediately after a new interaction (or the products of a resonance decay) has been added, and should then be used to prepare the subsystem of partons for subsequent evolution. In the current code this involves identifying all colour and charge dipole ends: the position of radiating and recoiling partons, maximum pT scales, possible higher-order matrix elements matchings to apply, and so on.
      The iSys parameter specifies which parton system is to be prepared. It is used to extract the set of partons to be treated, with rules as described in the above section on subsystems. Specifically, the first two partons represent the incoming state, or are 0 for resonance decays unrelated to the beams, while the rest are not required to be in any particular order.
      The limitPTmaxIn switch conveys the choice made on maximum scale for the dipole-ends evolution associated with the hard interaction of the event (while scales for subsequent MPIs by default are set to respect pT ordering). If true then this scale is set by the user choice options, see the TimeShower::limitPTmax method above, while if false emissions are allowed to go up to the kinematical limit. For the two-hard-interactions scenario, the two class variables dopTlimit1 and dopTlimit2 instead convey the choice made.
      The pTfirstTrialIn parameter is tentatively used in the new weak-shower part of the code. It is related to the option to shift the weak-shower evolution scale up by (some factor times) the gauge boson mass, without this backfiring on the QCD/QED evolution. Still under evolution, and normally not used.
      This method is called immediately after rescattering in the description of multiparton interactions. Thus the information on one or several systems is out-of-date, while that of the others is unchanged. We do not provide the details here, since we presume few implementors of new showers will want to touch the technicalities involved in obtaining a description of rescattering. This method is called immediately after a spacelike branching in the iSys'th subsystem. Thus the information for that system is out-of-date, while that of the others is unchanged. If you want, you are free to throw away all information for the affected subsystem and call prepare( iSys, event) to create new one. Alternatively you may choose only to update the information that has changed. This is the main driver routine for the downwards evolution. A new pT is to be selected based on the current information set up by the routines above, and along with that a branching parton or dipole. The pTbegAll scale is the maximum scale allowed, from which the downwards evolution should be begun (usually respecting the maximum scale of each individual parton). If no emission is found above pTendAll (and above the respective shower cutoff scales) then 0. should be returned and no emissions will be allowed. Both scales can vary from one event to the next: if a scale has already been selected for MPI or ISR it makes no sense to look for a scale smaller than that from FSR, since it would not be able to compete, so pTendAll is set correspondingly. As it happens, FSR is tried before ISR and MPI in the interleaved evolution, but this is an implementation detail that could well change.
      Typically the implementation of this routine would be to set up a loop over all possible radiating objects (dipoles, dipole ends, ...), for each pick its possible branching scale and then pick the one with largest scale as possible winner. At this stage no branching should actually be carried out, since MPI, ISR and FSR still have to be compared to assign the winner.
      The isFirstTrialIn is true only for the very first emission, and can then optionally be used to switch the weak-shower evolution scale up by (some factor times) the gauge boson mass.
      This method will be called once FSR has won the competition with MPI and ISR to do the next branching. The candidate branching found in the previous step should here be carried out in full. The pre-branching partons should get a negative status code and new replacement ones added to the end of the event record. Also the subsystem information should be updated, and possibly also the beams.
      Should some problem be encountered in this procedure, e.g. if some not-previously-considered kinematics requirement fails, it is allowed to return false to indicate that no branching could be carried out.
      Normally the optional isInterleaved argument would not be of interest. It can be used to separate resonance decays, false, from the interleaved evolution together with MPI and ISR, true. More precisely, it separates calls to the timesDecPtr and the timesPtr instances.
      This method is only called if rescattering is switched on in the description of multiparton interactions. It then propagates a recoil from a timelike branching to internal lines that connect systems. As for rescatterUpdate above, this is not likely to be of interest to most implementors of new showers. This method is not virtual. If a branching is constructed by the previous routine this tiny method should be able to return the number of the selected subsystem iSysSel where it occurred, so that the spacelike shower can be told which system to update, if necessary. Therefore iSysSel must be set in branch (or already in pTnext). This method is not at all required. In the current implementation it outputs a list of all the dipole ends, with information on the respective dipole. The routine is not called anywhere in the public code, but has been inserted at various places during the development/debug phase.

      The SpaceShower interface

      If you want to replace the SpaceShower class this would involve replacing the virtual methods in the following. You will find that much of the story reminds of TimeShower above, and actually some cut-and-paste of text is involved. In some respects the description is simpler, since there are no special cases for resonance decays and non-interleaved evolution. Thus there is no correspondence to the TimeShower::shower(...) routine. The constructor does not need to do anything. Also the destructor does not need to do anything. This method only imports pointers to standard facilities, and is not virtual. You have to store your local copy of the pointers to these objects, since they have to be used during the generation, as explained above. This is also the place to do initialization of whatever parameters you plan to use, e.g. by reading in them from a user-accessible database like the Settings one. The question is whether the ISR should be allowed to occur at larger scales than the hard process it surrounds. This is process-dependent. For instance, if the hard process is Z^0 production we know that ISR should be allowed to go right up to the kinematical limit. If it is a 2 -> 2 QCD process the ISR should not exceed the scale of the hard process, since if so one would double-count. The SpaceShower:pTmaxMatch switch allows you to force the behaviour, or else to program your own logic. The current default implementation limits pT whenever the final state contains a quark (except top), gluon or photon, since then the danger of double-counting is there. You may replace by your own logic, or leave as is.
      The internal PYTHIA implementation also allows intermediate options, where emissions can go up to the kinematical limit but be dampened above the factorization or renormalization scale. Therefore the (square of the) latter two are provided as optional input parameters.
      When the above method limits pT_max to the scale of the process, it may still be convenient to vary the matching slightly for the hardest interaction in an event, to probe the sensitivity to such details. The base-class implementation returns the value of the SpaceShower:pTmaxFudge parameter. This method is called immediately after a new interaction has been added, and should then be used to prepare the subsystem of partons for subsequent evolution. In the current code this involves identifying the colour and charge dipole ends: the position of radiating and recoiling partons, maximum pT scales, and possible higher-order matrix elements matchings to apply. Depending on what you have in mind you may choose to store slightly different quantities. You have to use the subsystem information described above to find the positions of the two incoming partons (and the outgoing ones) of the system, and from there the scales at which they were produced.
      The limitPTmax input agrees with the output of the previous method for the hardest process, and is always true for subsequent MPI, since there an unlimited pT for sure would lead to double-counting.
      The pTfirstTrialIn parameter is tentatively used in the new weak-shower part of the code. It is related to the option to shift the weak-shower evolution scale up by (some factor times) the gauge boson mass, without this backfiring on the QCD/QED evolution. Still under evolution, and normally not used.
      This method is called immediately after a timelike branching in the iSys'th subsystem. Thus the information for that system may be out-of-date, and to be updated. For the standard PYTHIA showers this routine does not need to do anything, but that may be different in another implementation. This is the main driver routine for the downwards evolution. A new pT is to be selected based on the current information set up by the routines above, and along with that a branching parton or dipole. The pTbegAll scale is the maximum scale allowed, from which the downwards evolution should be begun (usually respecting the maximum scale of each individual parton). If no emission is found above pTendAll (and above the respective shower cutoff scales) then 0. should be returned and no emissions will be allowed. Both scales can vary from one event to the next: if a scale has already been selected for MPI or ISR it makes no sense to look for a scale smaller than that from FSR, since it would not be able to compete, so pTendAll is set correspondingly. As it happens, FSR is tried before ISR and MPI in the interleaved evolution, but this is an implementation detail that could well change.
      Typically the implementation of this routine would be to set up a loop over all possible radiating objects (dipoles, dipole ends, ...), for each pick its possible branching scale and then pick the one with largest scale as possible winner. At this stage no branching should actually be carried out, since MPI, ISR and FSR still have to be compared to assign the winner.
      The input nRadIn provides the total number of ISR and FSR emissions already generated in the event, and so allows a special treatment for the very first emission, if desired.
      The isFirstTrialIn is true only for the very first emission, and can then optionally be used to switch the weak-shower evolution scale up by (some factor times) the gauge boson mass.
      This method will be called once ISR has won the competition with MPI and FSR to do the next branching. The candidate branching found in the previous step should here be carried out in full. The pre-branching partons should get a negative status code and new replacement ones added to the end of the event record. Also the subsystem information should be updated, and possibly also the beams.
      Should some problem be encountered in this procedure, e.g. if some not-previously-considered kinematics requirement fails, it is allowed to return false to indicate that no branching could be carried out. Also a complete restart of the parton-level description may be necessary, see doRestart() below.
      This method is not virtual. If a branching is constructed by the previous routine this tiny method should be able to return the number of the selected subsystem iSysSel where it occurred, so that the spacelike shower can be told which system to update, if necessary. Therefore iSysSel must be set in branch (or already in pTnext). This method is not virtual. If branch(...) above fails to construct a branching, and the conditions are such that the whole parton-level description should be restarted, then it should return true, else not. Currently only the rescattering description can give this kind of failures, and so the internal rescatterFail boolean must be set true when this should happen, and else false. This method is not at all required. In the current implementation it outputs a list of all the dipole ends, with information on the respective dipole. The routine is not called anywhere in the public code, but has been inserted at various places during the development/debug phase.
      pythia8-8.1.80.orig/xmldoc/lejon2.eps0000444000175000017500000203431212217346304015526 0ustar sunsun%!PS-Adobe-3.0 EPSF-3.0 %%Creator: Adobe Illustrator(R) 8.0 %%AI8_CreatorVersion: 8 %%For: (Marit M\237nter Hedlund) (ID, design och kommunikation ab) %%Title: (logo LUND UNIVERSITY V 4-f\212rg) %%CreationDate: (5/25/99) (2:16 PM) %%BoundingBox: -268 -43 201 263 %%HiResBoundingBox: -267.75 -42.75 200.25 262.25 %%DocumentProcessColors: Cyan Magenta Yellow Black %%DocumentSuppliedResources: procset Adobe_level2_AI5 1.2 0 %%+ procset Adobe_ColorImage_AI6 1.3 0 %%+ procset Adobe_Illustrator_AI5 1.3 0 %%+ procset Adobe_cshow 2.0 8 %%+ procset Adobe_shading_AI8 1.0 0 %AI5_FileFormat 4.0 %AI3_ColorUsage: Color %AI3_IncludePlacedImages %AI7_ImageSettings: 1 %%CMYKCustomColor: 1 0.5 0 0 (Bl\214) %%+ 0.5 0.4 0.3 0 (Bl\214gr\214) %%+ 0.5 0.85 1 0 (Brun) %%+ 0.75 0.05 1 0 (Gr\212sgr\232n) %%+ 0.05 0.2 0.95 0 (Guld) %%+ 1 0 0.55 0 (Havsbl\214) %%+ 0.8 0.05 0 0 (Himmelsbl\214) %%+ 1 0.9 0.1 0 (M\232rkbl\214) %%+ 0 0.45 1 0 (Orange) %%+ 1 0.72 0 0.18 (PANTONE 280 CV) %%+ 0.15 1 1 0 (R\232d) %%+ 1 0.55 1 0 (Skogsgr\232n) %%+ 0.45 0.9 0 0 (Violett) %%CMYKProcessColor: 1 1 1 1 ([Passm\212rke]) %%AI6_ColorSeparationSet: 1 1 (AI6 Default Color Separation Set) %%+ Options: 1 16 0 1 0 1 1 1 0 1 1 1 1 18 0 0 0 0 0 0 0 0 -1 -1 %%+ PPD: 1 21 0 0 60 45 2 2 1 0 0 1 0 0 0 0 0 0 0 0 0 0 () %AI3_TemplateBox: -17.75 92.25 -17.75 92.25 %AI3_TileBox: -598.75 -322.75 569.25 494.25 %AI3_DocumentPreview: Macintosh_ColorPic %AI5_ArtSize: 1190.5511 841.8898 %AI5_RulerUnits: 1 %AI5_ArtFlags: 0 0 0 1 0 0 1 0 0 %AI5_TargetResolution: 800 %AI5_NumLayers: 3 %AI8_OpenToView: -554.75 485.25 1 1146 827 18 1 1 3 40 0 0 %AI5_OpenViewLayers: 777 %%PageOrigin:-598.75 -322.75 %%AI3_PaperRect:-14 832 1189 -18 %%AI3_Margin:14 -15 -21 18 %AI7_GridSettings: 72 8 72 8 1 0 0.8 0.8 0.8 0.9 0.9 0.9 %%EndComments %%BeginProlog %%BeginResource: procset Adobe_level2_AI5 1.2 0 %%Title: (Adobe Illustrator (R) Version 5.0 Level 2 Emulation) %%Version: 1.2 0 %%CreationDate: (04/10/93) () %%Copyright: ((C) 1987-1996 Adobe Systems Incorporated All Rights Reserved) userdict /Adobe_level2_AI5 26 dict dup begin put /packedarray where not { userdict begin /packedarray { array astore readonly } bind def /setpacking /pop load def /currentpacking false def end 0 } if pop userdict /defaultpacking currentpacking put true setpacking /initialize { Adobe_level2_AI5 begin } bind def /terminate { currentdict Adobe_level2_AI5 eq { end } if } bind def mark /setcustomcolor where not { /findcmykcustomcolor { (AI8_CMYK_CustomColor) 6 packedarray } bind def /findrgbcustomcolor { (AI8_RGB_CustomColor) 5 packedarray } bind def /setcustomcolor { exch aload pop dup (AI8_CMYK_CustomColor) eq { pop pop 4 { 4 index mul 4 1 roll } repeat 5 -1 roll pop setcmykcolor } { dup (AI8_RGB_CustomColor) eq { pop pop 3 { 1 exch sub 3 index mul 1 exch sub 3 1 roll } repeat 4 -1 roll pop setrgbcolor } { pop 4 { 4 index mul 4 1 roll } repeat 5 -1 roll pop setcmykcolor } ifelse } ifelse } def } if /setAIseparationgray { false setoverprint 0 setgray /setseparationgray where{ pop setseparationgray }{ /setcolorspace where{ pop [/Separation (All) /DeviceCMYK {dup dup dup}] setcolorspace 1 exch sub setcolor }{ setgray }ifelse }ifelse } def /gt38? mark {version cvr cvx exec} stopped {cleartomark true} {38 gt exch pop} ifelse def userdict /deviceDPI 72 0 matrix defaultmatrix dtransform dup mul exch dup mul add sqrt put userdict /level2? systemdict /languagelevel known dup { pop systemdict /languagelevel get 2 ge } if put /level2ScreenFreq { begin 60 HalftoneType 1 eq { pop Frequency } if HalftoneType 2 eq { pop GrayFrequency } if HalftoneType 5 eq { pop Default level2ScreenFreq } if end } bind def userdict /currentScreenFreq level2? {currenthalftone level2ScreenFreq} {currentscreen pop pop} ifelse put level2? not { /setcmykcolor where not { /setcmykcolor { exch .11 mul add exch .59 mul add exch .3 mul add 1 exch sub setgray } def } if /currentcmykcolor where not { /currentcmykcolor { 0 0 0 1 currentgray sub } def } if /setoverprint where not { /setoverprint /pop load def } if /selectfont where not { /selectfont { exch findfont exch dup type /arraytype eq { makefont } { scalefont } ifelse setfont } bind def } if /cshow where not { /cshow { [ 0 0 5 -1 roll aload pop ] cvx bind forall } bind def } if } if cleartomark /anyColor? { add add add 0 ne } bind def /testColor { gsave setcmykcolor currentcmykcolor grestore } bind def /testCMYKColorThrough { testColor anyColor? } bind def userdict /composite? 1 0 0 0 testCMYKColorThrough 0 1 0 0 testCMYKColorThrough 0 0 1 0 testCMYKColorThrough 0 0 0 1 testCMYKColorThrough and and and put composite? not { userdict begin gsave /cyan? 1 0 0 0 testCMYKColorThrough def /magenta? 0 1 0 0 testCMYKColorThrough def /yellow? 0 0 1 0 testCMYKColorThrough def /black? 0 0 0 1 testCMYKColorThrough def grestore /isCMYKSep? cyan? magenta? yellow? black? or or or def /customColor? isCMYKSep? not def end } if end defaultpacking setpacking %%EndResource %%BeginProcSet: Adobe_ColorImage_AI6 1.3 0 userdict /Adobe_ColorImage_AI6 known not { userdict /Adobe_ColorImage_AI6 53 dict put } if userdict /Adobe_ColorImage_AI6 get begin /initialize { Adobe_ColorImage_AI6 begin Adobe_ColorImage_AI6 { dup type /arraytype eq { dup xcheck { bind } if } if pop pop } forall } def /terminate { end } def currentdict /Adobe_ColorImage_AI6_Vars known not { /Adobe_ColorImage_AI6_Vars 41 dict def } if Adobe_ColorImage_AI6_Vars begin /plateindex -1 def /_newproc null def /_proc1 null def /_proc2 null def /sourcearray 4 array def /_ptispace null def /_ptiname null def /_pti0 0 def /_pti1 0 def /_ptiproc null def /_ptiscale 0 def /_pticomps 0 def /_ptibuf 0 string def /_gtigray 0 def /_cticmyk null def /_rtirgb null def /XIEnable true def /XIType 0 def /XIEncoding 0 def /XICompression 0 def /XIChannelCount 0 def /XIBitsPerPixel 0 def /XIImageHeight 0 def /XIImageWidth 0 def /XIImageMatrix null def /XIRowBytes 0 def /XIFile null def /XIBuffer1 null def /XIBuffer2 null def /XIBuffer3 null def /XIDataProc null def /XIColorSpace /DeviceGray def /XIColorValues 0 def /XIPlateList false def end /ci6colorimage /colorimage where {/colorimage get}{null} ifelse def /ci6image systemdict /image get def /ci6curtransfer systemdict /currenttransfer get def /ci6curoverprint /currentoverprint where {/currentoverprint get}{{_of}} ifelse def /ci6foureq { 4 index ne { pop pop pop false }{ 4 index ne { pop pop false }{ 4 index ne { pop false }{ 4 index eq } ifelse } ifelse } ifelse } def /ci6testplate { Adobe_ColorImage_AI6_Vars begin /plateindex -1 def /setcmykcolor where { pop gsave 1 0 0 0 setcmykcolor systemdict /currentgray get exec 1 exch sub 0 1 0 0 setcmykcolor systemdict /currentgray get exec 1 exch sub 0 0 1 0 setcmykcolor systemdict /currentgray get exec 1 exch sub 0 0 0 1 setcmykcolor systemdict /currentgray get exec 1 exch sub grestore 1 0 0 0 ci6foureq { /plateindex 0 def }{ 0 1 0 0 ci6foureq { /plateindex 1 def }{ 0 0 1 0 ci6foureq { /plateindex 2 def }{ 0 0 0 1 ci6foureq { /plateindex 3 def }{ 0 0 0 0 ci6foureq { /plateindex 5 def } if } ifelse } ifelse } ifelse } ifelse pop pop pop pop } if plateindex end } def /ci6concatprocs { /packedarray where { pop dup type /packedarraytype eq 2 index type /packedarraytype eq or }{ false } ifelse { /_proc2 exch cvlit def /_proc1 exch cvlit def _proc1 aload pop _proc2 aload pop _proc1 length _proc2 length add packedarray cvx }{ /_proc2 exch cvlit def /_proc1 exch cvlit def /_newproc _proc1 length _proc2 length add array def _newproc 0 _proc1 putinterval _newproc _proc1 length _proc2 putinterval _newproc cvx } ifelse } def /ci6istint { type /arraytype eq } def /ci6isspot { dup type /arraytype eq { dup length 1 sub get /Separation eq }{ pop false } ifelse } def /ci6spotname { dup ci6isspot {dup length 2 sub get}{pop ()} ifelse } def /ci6altspace { aload pop pop pop ci6colormake } def /ci6numcomps { dup /DeviceGray eq { pop 1 }{ dup /DeviceRGB eq { pop 3 }{ /DeviceCMYK eq { 4 }{ 1 } ifelse } ifelse } ifelse } def /ci6marksplate { dup /DeviceGray eq { pop plateindex 3 eq }{ dup /DeviceRGB eq { pop plateindex 5 ne }{ dup /DeviceCMYK eq { pop plateindex 5 ne }{ dup ci6isspot { /findcmykcustomcolor where { pop dup length 2 sub get 0.1 0.1 0.1 0.1 5 -1 roll findcmykcustomcolor 1 setcustomcolor systemdict /currentgray get exec 1 ne }{ pop plateindex 5 ne } ifelse }{ pop plateindex 5 ne } ifelse } ifelse } ifelse } ifelse } def /ci6colormake { dup ci6numcomps exch 1 index 2 add 1 roll dup 1 eq {pop}{array astore} ifelse exch } def /ci6colorexpand { dup ci6spotname exch dup ci6istint { ci6altspace exch 4 1 roll }{ 1 3 1 roll } ifelse } def /ci6colortint { dup /DeviceGray eq { 3 1 roll 1 exch sub mul 1 exch sub exch }{ dup /DeviceRGB eq { 3 1 roll {1 exch sub 1 index mul 1 exch sub exch} forall pop 3 array astore exch }{ dup /DeviceCMYK eq { 3 1 roll {1 index mul exch} forall pop 4 array astore exch }{ 3 1 roll mul exch } ifelse } ifelse } ifelse } def /ci6colortocmyk { dup /DeviceGray eq { pop 1 exch sub 0 0 0 4 -1 roll 4 array astore }{ dup /DeviceRGB eq { pop aload pop _rgbtocmyk 4 array astore }{ dup /DeviceCMYK eq { pop }{ ci6altspace ci6colortint ci6colortocmyk } ifelse } ifelse } ifelse } def /ci6makeimagedict { 7 dict begin /ImageType 1 def /Decode exch def /DataSource exch def /ImageMatrix exch def /BitsPerComponent exch def /Height exch def /Width exch def currentdict end } def /ci6stringinvert { 0 1 2 index length 1 sub { dup 2 index exch get 255 exch sub 2 index 3 1 roll put } for } def /ci6stringknockout { 0 1 2 index length 1 sub { 255 2 index 3 1 roll put } for } def /ci6stringapply { 0 1 4 index length 1 sub { dup 4 index exch get 3 index 3 1 roll 3 index exec } for pop exch pop } def /ci6walkrgbstring { 0 3 index dup length 1 sub 0 3 3 -1 roll { 3 getinterval {} forall 5 index exec 3 index } for 5 {pop} repeat } def /ci6walkcmykstring { 0 3 index dup length 1 sub 0 4 3 -1 roll { 4 getinterval {} forall 6 index exec 3 index } for 5 { pop } repeat } def /ci6putrgbtograystr { .11 mul exch .59 mul add exch .3 mul add cvi 3 copy put pop 1 add } def /ci6putcmyktograystr { exch .11 mul add exch .59 mul add exch .3 mul add dup 255 gt { pop 255 } if 255 exch sub cvi 3 copy put pop 1 add } def /ci6rgbtograyproc { Adobe_ColorImage_AI6_Vars begin sourcearray 0 get exec XIBuffer3 dup 3 1 roll /ci6putrgbtograystr load exch ci6walkrgbstring end } def /ci6cmyktograyproc { Adobe_ColorImage_AI6_Vars begin sourcearray 0 get exec XIBuffer3 dup 3 1 roll /ci6putcmyktograystr load exch ci6walkcmykstring end } def /ci6separatecmykproc { Adobe_ColorImage_AI6_Vars begin sourcearray 0 get exec XIBuffer3 0 2 index plateindex 4 2 index length 1 sub { get 255 exch sub 3 copy put pop 1 add 2 index } for pop pop exch pop end } def /ci6compositeimage { dup 1 eq { pop pop image }{ /ci6colorimage load null ne { ci6colorimage }{ 3 1 roll pop sourcearray 0 3 -1 roll put 3 eq {/ci6rgbtograyproc}{/ci6cmyktograyproc} ifelse load image } ifelse } ifelse } def /ci6knockoutimage { gsave 0 ci6curtransfer exec 1 ci6curtransfer exec eq { 0 ci6curtransfer exec 0.5 lt }{ 0 ci6curtransfer exec 1 ci6curtransfer exec gt } ifelse {{pop 0}}{{pop 1}} ifelse systemdict /settransfer get exec ci6compositeimage grestore } def /ci6drawimage { ci6testplate -1 eq { pop ci6compositeimage }{ dup type /arraytype eq { dup length plateindex gt {plateindex get}{pop false} ifelse }{ { true }{ dup 1 eq {plateindex 3 eq}{plateindex 3 le} ifelse } ifelse } ifelse { dup 1 eq { pop pop ci6image }{ dup 3 eq { ci6compositeimage }{ pop pop sourcearray 0 3 -1 roll put /ci6separatecmykproc load ci6image } ifelse } ifelse }{ ci6curoverprint { 7 {pop} repeat }{ ci6knockoutimage } ifelse } ifelse } ifelse } def /ci6proctintimage { /_ptispace exch store /_ptiname exch store /_pti1 exch store /_pti0 exch store /_ptiproc exch store /_pticomps _ptispace ci6numcomps store /_ptiscale _pti1 _pti0 sub store level2? { _ptiname length 0 gt version cvr 2012 ge and { [/Separation _ptiname _ptispace {_ptiproc}] setcolorspace [_pti0 _pti1] ci6makeimagedict ci6image }{ [/Indexed _ptispace 255 {255 div _ptiscale mul _pti0 add _ptiproc}] setcolorspace [0 255] ci6makeimagedict ci6image } ifelse }{ _pticomps 1 eq { { dup { 255 div _ptiscale mul _pti0 add _ptiproc 255 mul cvi put } ci6stringapply } ci6concatprocs ci6image }{ { dup length _pticomps mul dup _ptibuf length ne {/_ptibuf exch string store}{pop} ifelse _ptibuf { exch _pticomps mul exch 255 div _ptiscale mul _pti0 add _ptiproc _pticomps 2 add -2 roll _pticomps 1 sub -1 0 { 1 index add 2 index exch 5 -1 roll 255 mul cvi put } for pop pop } ci6stringapply } ci6concatprocs false _pticomps /ci6colorimage load null eq {7 {pop} repeat}{ci6colorimage} ifelse } ifelse } ifelse } def /ci6graytintimage { /_gtigray 5 -1 roll store {1 _gtigray sub mul 1 exch sub} 4 1 roll /DeviceGray ci6proctintimage } def /ci6cmyktintimage { /_cticmyk 5 -1 roll store {_cticmyk {1 index mul exch} forall pop} 4 1 roll /DeviceCMYK ci6proctintimage } def /ci6rgbtintimage { /_rtirgb 5 -1 roll store {_rtirgb {1 exch sub 1 index mul 1 exch sub exch} forall pop} 4 1 roll /DeviceRGB ci6proctintimage } def /ci6tintimage { ci6testplate -1 eq { ci6colorexpand 3 -1 roll 5 -1 roll {0}{0 exch} ifelse 4 2 roll dup /DeviceGray eq { pop ci6graytintimage }{ dup /DeviceRGB eq { pop ci6rgbtintimage }{ pop ci6cmyktintimage } ifelse } ifelse }{ dup ci6marksplate { plateindex 5 lt { ci6colortocmyk plateindex get dup 0 eq ci6curoverprint and { 7 {pop} repeat }{ 1 exch sub exch {1 0}{0 1} ifelse () ci6graytintimage } ifelse }{ pop exch {0}{0 exch} ifelse 0 3 1 roll () ci6graytintimage } ifelse }{ ci6curoverprint { 8 {pop} repeat }{ pop pop pop {pop 1} 0 1 () /DeviceGray ci6proctintimage } ifelse } ifelse } ifelse } def /XINullImage { } def /XIImageMask { XIImageWidth XIImageHeight false [XIImageWidth 0 0 XIImageHeight neg 0 0] /XIDataProc load imagemask } def /XIImageTint { XIImageWidth XIImageHeight XIBitsPerPixel [XIImageWidth 0 0 XIImageHeight neg 0 0] /XIDataProc load XIType 3 eq XIColorValues XIColorSpace ci6tintimage } def /XIImage { XIImageWidth XIImageHeight XIBitsPerPixel [XIImageWidth 0 0 XIImageHeight neg 0 0] /XIDataProc load false XIChannelCount XIPlateList ci6drawimage } def /XG { pop pop } def /XF { 13 {pop} repeat } def /Xh { Adobe_ColorImage_AI6_Vars begin gsave /XIType exch def /XIImageHeight exch def /XIImageWidth exch def /XIImageMatrix exch def 0 0 moveto XIImageMatrix concat XIImageWidth XIImageHeight scale /_lp /null ddef _fc /_lp /imagemask ddef end } def /XH { Adobe_ColorImage_AI6_Vars begin grestore end } def /XIEnable { Adobe_ColorImage_AI6_Vars /XIEnable 3 -1 roll put } def /XC { Adobe_ColorImage_AI6_Vars begin ci6colormake /XIColorSpace exch def /XIColorValues exch def end } def /XIPlates { Adobe_ColorImage_AI6_Vars begin /XIPlateList exch def end } def /XI { Adobe_ColorImage_AI6_Vars begin gsave /XIType exch def cvi dup 256 idiv /XICompression exch store 256 mod /XIEncoding exch store pop pop /XIChannelCount exch def /XIBitsPerPixel exch def /XIImageHeight exch def /XIImageWidth exch def pop pop pop pop /XIImageMatrix exch def XIBitsPerPixel 1 eq { XIImageWidth 8 div ceiling cvi }{ XIImageWidth XIChannelCount mul } ifelse /XIRowBytes exch def XIEnable { /XIBuffer3 XIImageWidth string def XICompression 0 eq { /XIBuffer1 XIRowBytes string def XIEncoding 0 eq { {currentfile XIBuffer1 readhexstring pop} }{ {currentfile XIBuffer1 readstring pop} } ifelse }{ /XIBuffer1 256 string def /XIBuffer2 XIRowBytes string def {currentfile XIBuffer1 readline pop (%) anchorsearch {pop} if} /ASCII85Decode filter /DCTDecode filter /XIFile exch def {XIFile XIBuffer2 readstring pop} } ifelse /XIDataProc exch def XIType 1 ne { 0 setgray } if XIType 1 eq { XIImageMask }{ XIType 2 eq XIType 3 eq or { XIImageTint }{ XIImage } ifelse } ifelse }{ XINullImage } ifelse /XIPlateList false def grestore end } def end %%EndProcSet %%BeginResource: procset Adobe_Illustrator_AI5 1.3 0 %%Title: (Adobe Illustrator (R) Version 8.0 Full Prolog) %%Version: 1.3 0 %%CreationDate: (3/7/1994) () %%Copyright: ((C) 1987-1998 Adobe Systems Incorporated All Rights Reserved) currentpacking true setpacking userdict /Adobe_Illustrator_AI5_vars 112 dict dup begin put /_?cmyk false def /_eo false def /_lp /none def /_pf { } def /_ps { } def /_psf { } def /_pss { } def /_pjsf { } def /_pjss { } def /_pola 0 def /_doClip 0 def /cf currentflat def /_lineorientation 0 def /_charorientation 0 def /_yokoorientation 0 def /_tm matrix def /_renderStart [ /e0 /r0 /a0 /o0 /e1 /r1 /a1 /i0 ] def /_renderEnd [ null null null null /i1 /i1 /i1 /i1 ] def /_render -1 def /_shift [0 0] def /_ax 0 def /_ay 0 def /_cx 0 def /_cy 0 def /_leading [ 0 0 ] def /_ctm matrix def /_mtx matrix def /_sp 16#020 def /_hyphen (-) def /_fontSize 0 def /_fontAscent 0 def /_fontDescent 0 def /_fontHeight 0 def /_fontRotateAdjust 0 def /Ss 256 string def Ss 0 (fonts/) putinterval /_cnt 0 def /_scale [1 1] def /_nativeEncoding 0 def /_useNativeEncoding 0 def /_tempEncode 0 def /_pntr 0 def /_tDict 2 dict def /_hfname 100 string def /_hffound false def /Tx { } def /Tj { } def /CRender { } def /_AI3_savepage { } def /_gf null def /_cf 4 array def /_rgbf 3 array def /_if null def /_of false def /_fc { } def /_gs null def /_cs 4 array def /_rgbs 3 array def /_is null def /_os false def /_sc { } def /_pd 1 dict def /_ed 15 dict def /_pm matrix def /_fm null def /_fd null def /_fdd null def /_sm null def /_sd null def /_sdd null def /_i null def /_lobyte 0 def /_hibyte 0 def /_cproc null def /_cscript 0 def /_hvax 0 def /_hvay 0 def /_hvwb 0 def /_hvcx 0 def /_hvcy 0 def /_bitfont null def /_bitlobyte 0 def /_bithibyte 0 def /_bitkey null def /_bitdata null def /_bitindex 0 def /discardSave null def /buffer 256 string def /beginString null def /endString null def /endStringLength null def /layerCnt 1 def /layerCount 1 def /perCent (%) 0 get def /perCentSeen? false def /newBuff null def /newBuffButFirst null def /newBuffLast null def /clipForward? false def end userdict /Adobe_Illustrator_AI5 known not { userdict /Adobe_Illustrator_AI5 100 dict put } if userdict /Adobe_Illustrator_AI5 get begin /initialize { Adobe_Illustrator_AI5 dup begin Adobe_Illustrator_AI5_vars begin /_aicmykps where {pop /_?cmyk _aicmykps def}if discardDict { bind pop pop } forall dup /nc get begin { dup xcheck 1 index type /operatortype ne and { bind } if pop pop } forall end newpath } def /terminate { end end } def /_ null def /ddef { Adobe_Illustrator_AI5_vars 3 1 roll put } def /xput { dup load dup length exch maxlength eq { dup dup load dup length 2 mul dict copy def } if load begin def end } def /npop { { pop } repeat } def /hswj { dup stringwidth 3 2 roll { _hvwb eq { exch _hvcx add exch _hvcy add } if exch _hvax add exch _hvay add } cforall } def /vswj { 0 0 3 -1 roll { dup 255 le _charorientation 1 eq and { dup cstring stringwidth 5 2 roll _hvwb eq { exch _hvcy sub exch _hvcx sub } if exch _hvay sub exch _hvax sub 4 -1 roll sub exch 3 -1 roll sub exch } { _hvwb eq { exch _hvcy sub exch _hvcx sub } if exch _hvay sub exch _hvax sub _fontHeight sub } ifelse } cforall } def /swj { 6 1 roll /_hvay exch ddef /_hvax exch ddef /_hvwb exch ddef /_hvcy exch ddef /_hvcx exch ddef _lineorientation 0 eq { hswj } { vswj } ifelse } def /sw { 0 0 0 6 3 roll swj } def /vjss { 4 1 roll { dup cstring dup length 1 eq _charorientation 1 eq and { -90 rotate currentpoint _fontRotateAdjust add moveto gsave false charpath currentpoint 5 index setmatrix stroke grestore _fontRotateAdjust sub moveto _sp eq { 5 index 5 index rmoveto } if 2 copy rmoveto 90 rotate } { currentpoint _fontHeight sub 5 index sub 3 index _sp eq { 9 index sub } if currentpoint exch 4 index stringwidth pop 2 div sub exch _fontAscent sub moveto gsave 2 index false charpath 6 index setmatrix stroke grestore moveto pop pop } ifelse } cforall 6 npop } def /hjss { 4 1 roll { dup cstring gsave false charpath currentpoint 5 index setmatrix stroke grestore moveto _sp eq { 5 index 5 index rmoveto } if 2 copy rmoveto } cforall 6 npop } def /jss { _lineorientation 0 eq { hjss } { vjss } ifelse } def /ss { 0 0 0 7 3 roll jss } def /vjsp { 4 1 roll { dup cstring dup length 1 eq _charorientation 1 eq and { -90 rotate currentpoint _fontRotateAdjust add moveto false charpath currentpoint _fontRotateAdjust sub moveto _sp eq { 5 index 5 index rmoveto } if 2 copy rmoveto 90 rotate } { currentpoint _fontHeight sub 5 index sub 3 index _sp eq { 9 index sub } if currentpoint exch 4 index stringwidth pop 2 div sub exch _fontAscent sub moveto 2 index false charpath moveto pop pop } ifelse } cforall 6 npop } def /hjsp { 4 1 roll { dup cstring false charpath _sp eq { 5 index 5 index rmoveto } if 2 copy rmoveto } cforall 6 npop } def /jsp { matrix currentmatrix _lineorientation 0 eq {hjsp} {vjsp} ifelse } def /sp { matrix currentmatrix 0 0 0 7 3 roll _lineorientation 0 eq {hjsp} {vjsp} ifelse } def /pl { transform 0.25 sub round 0.25 add exch 0.25 sub round 0.25 add exch itransform } def /setstrokeadjust where { pop true setstrokeadjust /c { curveto } def /C /c load def /v { currentpoint 6 2 roll curveto } def /V /v load def /y { 2 copy curveto } def /Y /y load def /l { lineto } def /L /l load def /m { moveto } def } { /c { pl curveto } def /C /c load def /v { currentpoint 6 2 roll pl curveto } def /V /v load def /y { pl 2 copy curveto } def /Y /y load def /l { pl lineto } def /L /l load def /m { pl moveto } def } ifelse /d { setdash } def /cf { } def /i { dup 0 eq { pop cf } if setflat } def /j { setlinejoin } def /J { setlinecap } def /M { setmiterlimit } def /w { setlinewidth } def /XR { 0 ne /_eo exch ddef } def /H { } def /h { closepath } def /N { _pola 0 eq { _doClip 1 eq { _eo {eoclip} {clip} ifelse /_doClip 0 ddef } if newpath } { /CRender { N } ddef } ifelse } def /n { N } def /F { _pola 0 eq { _doClip 1 eq { gsave _pf grestore _eo {eoclip} {clip} ifelse newpath /_lp /none ddef _fc /_doClip 0 ddef } { _pf } ifelse } { /CRender { F } ddef } ifelse } def /f { closepath F } def /S { _pola 0 eq { _doClip 1 eq { gsave _ps grestore _eo {eoclip} {clip} ifelse newpath /_lp /none ddef _sc /_doClip 0 ddef } { _ps } ifelse } { /CRender { S } ddef } ifelse } def /s { closepath S } def /B { _pola 0 eq { _doClip 1 eq gsave F grestore { gsave S grestore _eo {eoclip} {clip} ifelse newpath /_lp /none ddef _sc /_doClip 0 ddef } { S } ifelse } { /CRender { B } ddef } ifelse } def /b { closepath B } def /W { /_doClip 1 ddef } def /* { count 0 ne { dup type /stringtype eq { pop } if } if newpath } def /u { } def /U { } def /q { _pola 0 eq { gsave } if } def /Q { _pola 0 eq { grestore } if } def /*u { _pola 1 add /_pola exch ddef } def /*U { _pola 1 sub /_pola exch ddef _pola 0 eq { CRender } if } def /D { pop } def /*w { } def /*W { } def /` { /_i save ddef clipForward? { nulldevice } if 6 1 roll 4 npop concat pop userdict begin /showpage { } def 0 setgray 0 setlinecap 1 setlinewidth 0 setlinejoin 10 setmiterlimit [] 0 setdash /setstrokeadjust where {pop false setstrokeadjust} if newpath 0 setgray false setoverprint } def /~ { end _i restore } def /_rgbtocmyk { 3 { 1 exch sub 3 1 roll } repeat 3 copy 1 4 1 roll 3 { 3 index 2 copy gt { exch } if pop 4 1 roll } repeat pop pop pop 4 1 roll 3 { 3 index sub 3 1 roll } repeat 4 -1 roll } def /setrgbfill { _rgbf astore pop /_fc { _lp /fill ne { _of setoverprint _rgbf aload pop setrgbcolor /_lp /fill ddef } if } ddef /_pf { _fc _eo {eofill} {fill} ifelse } ddef /_psf { _fc hvashow } ddef /_pjsf { _fc hvawidthshow } ddef /_lp /none ddef } def /setrgbstroke { _rgbs astore pop /_sc { _lp /stroke ne { _os setoverprint _rgbs aload pop setrgbcolor /_lp /stroke ddef } if } ddef /_ps { _sc stroke } ddef /_pss { _sc ss } ddef /_pjss { _sc jss } ddef /_lp /none ddef } def /O { 0 ne /_of exch ddef /_lp /none ddef } def /R { 0 ne /_os exch ddef /_lp /none ddef } def /g { /_gf exch ddef /_fc { _lp /fill ne { _of setoverprint _gf setgray /_lp /fill ddef } if } ddef /_pf { _fc _eo {eofill} {fill} ifelse } ddef /_psf { _fc hvashow } ddef /_pjsf { _fc hvawidthshow } ddef /_lp /none ddef } def /G { /_gs exch ddef /_sc { _lp /stroke ne { _os setoverprint _gs setgray /_lp /stroke ddef } if } ddef /_ps { _sc stroke } ddef /_pss { _sc ss } ddef /_pjss { _sc jss } ddef /_lp /none ddef } def /k { _cf astore pop /_fc { _lp /fill ne { _of setoverprint _cf aload pop setcmykcolor /_lp /fill ddef } if } ddef /_pf { _fc _eo {eofill} {fill} ifelse } ddef /_psf { _fc hvashow } ddef /_pjsf { _fc hvawidthshow } ddef /_lp /none ddef } def /K { _cs astore pop /_sc { _lp /stroke ne { _os setoverprint _cs aload pop setcmykcolor /_lp /stroke ddef } if } ddef /_ps { _sc stroke } ddef /_pss { _sc ss } ddef /_pjss { _sc jss } ddef /_lp /none ddef } def /Xa { _?cmyk { 3 npop k }{ setrgbfill 4 npop } ifelse } def /XA { _?cmyk { 3 npop K }{ setrgbstroke 4 npop } ifelse } def /Xs { /_gf exch ddef 5 npop /_fc { _lp /fill ne { _of setoverprint _gf setAIseparationgray /_lp /fill ddef } if } ddef /_pf { _fc _eo {eofill} {fill} ifelse } ddef /_psf { _fc hvashow } ddef /_pjsf { _fc hvawidthshow } ddef /_lp /none ddef } def /XS { /_gs exch ddef 5 npop /_sc { _lp /stroke ne { _os setoverprint _gs setAIseparationgray /_lp /stroke ddef } if } ddef /_ps { _sc stroke } ddef /_pss { _sc ss } ddef /_pjss { _sc jss } ddef /_lp /none ddef } def /Xx { exch /_gf exch ddef 0 eq { findcmykcustomcolor }{ _?cmyk {true}{/findrgbcustomcolor where{pop false}{true}ifelse}ifelse { 4 1 roll 3 npop findcmykcustomcolor }{ 8 -4 roll 4 npop findrgbcustomcolor } ifelse } ifelse /_if exch ddef /_fc { _lp /fill ne { _of setoverprint _if _gf 1 exch sub setcustomcolor /_lp /fill ddef } if } ddef /_pf { _fc _eo {eofill} {fill} ifelse } ddef /_psf { _fc hvashow } ddef /_pjsf { _fc hvawidthshow } ddef /_lp /none ddef } def /XX { exch /_gs exch ddef 0 eq { findcmykcustomcolor }{ _?cmyk {true}{/findrgbcustomcolor where{pop false}{true}ifelse}ifelse { 4 1 roll 3 npop findcmykcustomcolor }{ 8 -4 roll 4 npop findrgbcustomcolor } ifelse } ifelse /_is exch ddef /_sc { _lp /stroke ne { _os setoverprint _is _gs 1 exch sub setcustomcolor /_lp /stroke ddef } if } ddef /_ps { _sc stroke } ddef /_pss { _sc ss } ddef /_pjss { _sc jss } ddef /_lp /none ddef } def /x { /_gf exch ddef findcmykcustomcolor /_if exch ddef /_fc { _lp /fill ne { _of setoverprint _if _gf 1 exch sub setcustomcolor /_lp /fill ddef } if } ddef /_pf { _fc _eo {eofill} {fill} ifelse } ddef /_psf { _fc hvashow } ddef /_pjsf { _fc hvawidthshow } ddef /_lp /none ddef } def /X { /_gs exch ddef findcmykcustomcolor /_is exch ddef /_sc { _lp /stroke ne { _os setoverprint _is _gs 1 exch sub setcustomcolor /_lp /stroke ddef } if } ddef /_ps { _sc stroke } ddef /_pss { _sc ss } ddef /_pjss { _sc jss } ddef /_lp /none ddef } def /XK { 3 -1 roll pop 0 eq { 1 exch sub 3 {dup 3 1 roll mul 5 1 roll} repeat mul 4 1 roll K } { 1 exch sub 4 1 roll 3 {1 exch sub 3 index mul 1 exch sub 3 1 roll} repeat 4 -1 roll pop XA } ifelse } def /Xk { 3 -1 roll pop 0 eq { 1 exch sub 3 {dup 3 1 roll mul 5 1 roll} repeat mul 4 1 roll k } { 1 exch sub 4 1 roll 3 {1 exch sub 3 index mul 1 exch sub 3 1 roll} repeat 4 -1 roll pop Xa } ifelse } def /A { pop } def /annotatepage { userdict /annotatepage 2 copy known {get exec} {pop pop} ifelse } def /XT { pop pop } def /Xt { pop } def /discard { save /discardSave exch store discardDict begin /endString exch store gt38? { 2 add } if load stopped pop end discardSave restore } bind def userdict /discardDict 7 dict dup begin put /pre38Initialize { /endStringLength endString length store /newBuff buffer 0 endStringLength getinterval store /newBuffButFirst newBuff 1 endStringLength 1 sub getinterval store /newBuffLast newBuff endStringLength 1 sub 1 getinterval store } def /shiftBuffer { newBuff 0 newBuffButFirst putinterval newBuffLast 0 currentfile read not { stop } if put } def 0 { pre38Initialize mark currentfile newBuff readstring exch pop { { newBuff endString eq { cleartomark stop } if shiftBuffer } loop } { stop } ifelse } def 1 { pre38Initialize /beginString exch store mark currentfile newBuff readstring exch pop { { newBuff beginString eq { /layerCount dup load 1 add store } { newBuff endString eq { /layerCount dup load 1 sub store layerCount 0 eq { cleartomark stop } if } if } ifelse shiftBuffer } loop } if } def 2 { mark { currentfile buffer {readline} stopped { % assume error was due to overfilling the buffer }{ not { stop } if endString eq { cleartomark stop } if }ifelse } loop } def 3 { /beginString exch store /layerCnt 1 store mark { currentfile buffer {readline} stopped { % assume error was due to overfilling the buffer }{ not { stop } if dup beginString eq { pop /layerCnt dup load 1 add store } { endString eq { layerCnt 1 eq { cleartomark stop } { /layerCnt dup load 1 sub store } ifelse } if } ifelse }ifelse } loop } def end userdict /clipRenderOff 15 dict dup begin put { /n /N /s /S /f /F /b /B } { { _doClip 1 eq { /_doClip 0 ddef _eo {eoclip} {clip} ifelse } if newpath } def } forall /Tr /pop load def /Bb {} def /BB /pop load def /Bg {12 npop} def /Bm {6 npop} def /Bc /Bm load def /Bh {4 npop} def end /Lb { 6 npop 7 2 roll 5 npop 0 eq { 0 eq { (%AI5_BeginLayer) 1 (%AI5_EndLayer--) discard } { /clipForward? true def /Tx /pop load def /Tj /pop load def currentdict end clipRenderOff begin begin } ifelse } { 0 eq { save /discardSave exch store } if } ifelse } bind def /LB { discardSave dup null ne { restore } { pop clipForward? { currentdict end end begin /clipForward? false ddef } if } ifelse } bind def /Pb { pop pop 0 (%AI5_EndPalette) discard } bind def /Np { 0 (%AI5_End_NonPrinting--) discard } bind def /Ln /pop load def /Ap /pop load def /Ar { 72 exch div 0 dtransform dup mul exch dup mul add sqrt dup 1 lt { pop 1 } if setflat } def /Mb { q } def /Md { } def /MB { Q } def /nc 4 dict def nc begin /setgray { pop } bind def /setcmykcolor { 4 npop } bind def /setrgbcolor { 3 npop } bind def /setcustomcolor { 2 npop } bind def currentdict readonly pop end /XP { 4 npop } bind def /XD { pop } bind def end setpacking %%EndResource %%BeginResource: procset Adobe_cshow 2.0 8 %%Title: (Writing System Operators) %%Version: 2.0 8 %%CreationDate: (1/23/89) () %%Copyright: ((C) 1992-1996 Adobe Systems Incorporated All Rights Reserved) currentpacking true setpacking userdict /Adobe_cshow 14 dict dup begin put /initialize { Adobe_cshow begin Adobe_cshow { dup xcheck { bind } if pop pop } forall end Adobe_cshow begin } def /terminate { currentdict Adobe_cshow eq { end } if } def /cforall { /_lobyte 0 ddef /_hibyte 0 ddef /_cproc exch ddef /_cscript currentfont /FontScript known { currentfont /FontScript get } { -1 } ifelse ddef { /_lobyte exch ddef _hibyte 0 eq _cscript 1 eq _lobyte 129 ge _lobyte 159 le and _lobyte 224 ge _lobyte 252 le and or and _cscript 2 eq _lobyte 161 ge _lobyte 254 le and and _cscript 3 eq _lobyte 161 ge _lobyte 254 le and and _cscript 25 eq _lobyte 161 ge _lobyte 254 le and and _cscript -1 eq or or or or and { /_hibyte _lobyte ddef } { _hibyte 256 mul _lobyte add _cproc /_hibyte 0 ddef } ifelse } forall } def /cstring { dup 256 lt { (s) dup 0 4 3 roll put } { dup 256 idiv exch 256 mod (hl) dup dup 0 6 5 roll put 1 4 3 roll put } ifelse } def /clength { 0 exch { 256 lt { 1 } { 2 } ifelse add } cforall } def /hawidthshow { { dup cstring show _hvax _hvay rmoveto _hvwb eq { _hvcx _hvcy rmoveto } if } cforall } def /vawidthshow { { dup 255 le _charorientation 1 eq and { -90 rotate 0 _fontRotateAdjust rmoveto cstring _hvcx _hvcy _hvwb _hvax _hvay 6 -1 roll awidthshow 0 _fontRotateAdjust neg rmoveto 90 rotate } { currentpoint _fontHeight sub exch _hvay sub exch _hvax sub 2 index _hvwb eq { exch _hvcy sub exch _hvcx sub } if 3 2 roll cstring dup stringwidth pop 2 div neg _fontAscent neg rmoveto show moveto } ifelse } cforall } def /hvawidthshow { 6 1 roll /_hvay exch ddef /_hvax exch ddef /_hvwb exch ddef /_hvcy exch ddef /_hvcx exch ddef _lineorientation 0 eq { hawidthshow } { vawidthshow } ifelse } def /hvwidthshow { 0 0 3 -1 roll hvawidthshow } def /hvashow { 0 0 0 6 -3 roll hvawidthshow } def /hvshow { 0 0 0 0 0 6 -1 roll hvawidthshow } def currentdict readonly pop end setpacking %%EndResource %%BeginResource: procset Adobe_shading_AI8 1.0 0 %%Title: (Adobe Illustrator 8 Shading Procset) %%Version: 1.0 0 %%CreationDate: (12/17/97) () %%Copyright: ((C) 1987-1997 Adobe Systems Incorporated All Rights Reserved) userdict /defaultpacking currentpacking put true setpacking userdict /Adobe_shading_AI8 10 dict dup begin put /initialize { Adobe_shading_AI8 begin Adobe_shading_AI8 bdprocs Mesh /initialize get exec } def /terminate { currentdict Adobe_shading_AI8 eq { end } if } def /bdprocs { { dup xcheck 1 index type /arraytype eq and { bind } if pop pop } forall } def /X! {pop} def /X# {pop pop} def /Mesh 40 dict def Mesh begin /initialize { Mesh bdprocs Mesh begin /emulate? /AI8MeshEmulation where { pop AI8MeshEmulation }{ systemdict /shfill known not } ifelse def end } def /bd { shadingdict begin } def /paint { emulate? { end }{ /_lp /none ddef _fc /_lp /none ddef /AIColorSpace AIColorSpace tocolorspace store /ColorSpace AIColorSpace topsspace store version_ge_3010.106 not systemdict /setsmoothness known and { 0.0001 setsmoothness } if composite? { /DataSource getdatasrc def Matrix concat currentdict end shfill }{ AIColorSpace makesmarks AIPlateList markingplate and not isoverprint and { end }{ /ColorSpace /DeviceGray store /Decode [0 1 0 1 0 1] store /DataSource getplatesrc def Matrix concat currentdict end shfill } ifelse } ifelse } ifelse } def /shadingdict 12 dict def shadingdict begin /ShadingType 6 def /BitsPerCoordinate 16 def /BitsPerComponent 8 def /BitsPerFlag 8 def end /datafile null def /databuf 256 string def /dataptr 0 def /srcspace null def /srcchannels 0 def /dstchannels 0 def /dstplate 0 def /srctodstcolor null def /getplatesrc { /srcspace AIColorSpace store /srcchannels AIColorSpace getnchannels store /dstchannels 1 store /dstplate getplateindex store /srctodstcolor srcspace makesmarks { dstplate 4 eq { {1 exch sub} }{ {srcspace tocmyk 3 dstplate sub index 1 exch sub 5 1 roll 4 {pop} repeat} } ifelse }{ {srcchannels {pop} repeat 1} } ifelse store /datafile getdatasrc store /rdpatch168 load DataLength () /SubFileDecode filter } def /getdatasrc { /rdcmntline load /ASCII85Decode filter } def /rdpatch168 { /dataptr 0 store 49 rdcount 4 { dup {pop srcchannels getint8} if dup {pop srctodstcolor dstchannels putint8 true} if } repeat {databuf 0 dataptr getinterval}{()} ifelse } def /rdpatch3216 { /dataptr 0 store 97 rdcount 4 { dup {pop srcchannels getint16} if dup {pop srctodstcolor dstchannels putint16 true} if } repeat {databuf 0 dataptr getinterval}{()} ifelse } def /rdcount { dup 0 gt { datafile databuf dataptr 4 -1 roll getinterval readstring exch length dataptr add /dataptr exch store }{ true } ifelse } def /getint8 { mark true 3 -1 roll { dup {pop datafile read} if dup {pop 255 div true} if } repeat { counttomark 1 add -1 roll pop true }{ cleartomark false } ifelse } def /putint8 { dup dataptr add /dataptr exch store dataptr exch { 1 sub exch 255 mul cvi databuf 2 index 3 -1 roll put } repeat pop } def /getint16 { mark true 3 -1 roll { dup {pop datafile read} if dup {pop 256 mul datafile read} if dup {pop add 65535 div true} if } repeat { counttomark 1 add -1 roll pop true }{ cleartomark false } ifelse } def /putint16 { dup 2 mul dataptr add /dataptr exch store dataptr exch { 2 sub exch 65535 mul cvi dup 256 idiv databuf 3 index 3 -1 roll put 256 mod databuf 2 index 1 add 3 -1 roll put } repeat pop } def /srcbuf 256 string def /rdcmntline { currentfile srcbuf readline pop (%) anchorsearch {pop} if } def /getplateindex { 0 [cyan? magenta? yellow? black? customColor?] {{exit} if 1 add} forall } def /aicsarray 4 array def /aicsaltvals 4 array def /aicsaltcolr aicsaltvals def /tocolorspace { dup type /arraytype eq { mark exch aload pop aicsarray 0 3 -1 roll put aicsarray 1 3 -1 roll put dup aicsarray 2 3 -1 roll put gettintxform aicsarray 3 3 -1 roll put counttomark aicsaltvals 0 3 -1 roll getinterval /aicsaltcolr exch store aicsaltcolr astore pop pop aicsarray } if } def /subtintxform {aicsaltcolr {1 index mul exch} forall pop} def /addtintxform {aicsaltcolr {1 sub 1 index mul 1 add exch} forall pop} def /gettintxform { /DeviceRGB eq {/addtintxform}{/subtintxform} ifelse load } def /getnchannels { dup type /arraytype eq {0 get} if colorspacedict exch get begin Channels end } def /makesmarks { composite? { pop true }{ dup dup type /arraytype eq {0 get} if colorspacedict exch get begin MarksPlate end } ifelse } def /markingplate { composite? { pop true }{ dup type /arraytype eq { dup length getplateindex gt {getplateindex get}{pop false} ifelse } if } ifelse } def /tocmyk { dup dup type /arraytype eq {0 get} if colorspacedict exch get begin ToCMYK end } def /topsspace { dup dup type /arraytype eq {0 get} if colorspacedict exch get begin ToPSSpace end } def /colorspacedict 5 dict dup begin /DeviceGray 4 dict dup begin /Channels 1 def /MarksPlate {pop black?} def /ToCMYK {pop 1 exch sub 0 0 0 4 -1 roll} def /ToPSSpace {} def end def /DeviceRGB 4 dict dup begin /Channels 3 def /MarksPlate {pop isCMYKSep?} def /ToCMYK {pop _rgbtocmyk} def /ToPSSpace {} def end def /DeviceCMYK 4 dict dup begin /Channels 4 def /MarksPlate {pop isCMYKSep?} def /ToCMYK {pop} def /ToPSSpace {} def end def /Separation 4 dict dup begin /Channels 1 def /MarksPlate { /findcmykcustomcolor where { pop dup 1 exch ToCMYK 5 -1 roll 1 get findcmykcustomcolor 1 setcustomcolor systemdict /currentgray get exec 1 ne }{ pop false } ifelse } def /ToCMYK { dup 2 get mark exch 4 2 roll 3 get exec counttomark -1 roll tocmyk 5 -1 roll pop } def /ToPSSpace {} def end def /Process 4 dict dup begin /Channels 1 def /MarksPlate { isCMYKSep? { 1 exch ToCMYK 4 array astore getplateindex get 0 ne }{ pop false } ifelse } def /ToCMYK { dup 2 get mark exch 4 2 roll 3 get exec counttomark -1 roll tocmyk 5 -1 roll pop } def /ToPSSpace { 4 array copy dup 0 /Separation put } def end def end def /isoverprint { /currentoverprint where {pop currentoverprint}{_of} ifelse } def /version_ge_3010.106 { version {cvr} stopped { pop false }{ 3010.106 ge } ifelse } def end end defaultpacking setpacking %%EndResource %%EndProlog %%BeginSetup userdict /_useSmoothShade false put userdict /_aicmykps true put userdict /_forceToCMYK true put Adobe_level2_AI5 /initialize get exec Adobe_cshow /initialize get exec Adobe_ColorImage_AI6 /initialize get exec Adobe_shading_AI8 /initialize get exec Adobe_Illustrator_AI5 /initialize get exec %AI5_Begin_NonPrinting Np %AI3_BeginPattern: (DblLinje1.2.inre) (DblLinje1.2.inre) 1 1 39.2705 39.2706 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2702 22.175 m 39.2702 13.6108 L 26.66 13.6108 L 26.66 1.0003 L 18.0958 1.0003 L 18.0948 22.175 L 18.0958 22.175 L 18.0958 22.1752 L 39.2702 22.175 L f 39.2708 24.6929 m 15.5779 24.6929 L 15.5779 1.0003 L 14.9037 1.0003 L 14.9032 25.3675 L 39.2708 25.3675 L 39.2708 24.6929 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.inre\012 1) (DblLinje1.2.inre\012 1) 1 1 39.2705 39.2706 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2702 22.175 m 39.2702 13.6108 L 26.66 13.6108 L 26.66 1.0003 L 18.0958 1.0003 L 18.0948 22.175 L 18.0958 22.175 L 18.0958 22.1752 L 39.2702 22.175 L f 39.2708 24.6929 m 15.5779 24.6929 L 15.5779 1.0003 L 14.9037 1.0003 L 14.9032 25.3675 L 39.2708 25.3675 L 39.2708 24.6929 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.inre\012 2) (DblLinje1.2.inre\012 2) 1 1 39.2705 39.2706 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2702 22.175 m 39.2702 13.6108 L 26.66 13.6108 L 26.66 1.0003 L 18.0958 1.0003 L 18.0948 22.175 L 18.0958 22.175 L 18.0958 22.1752 L 39.2702 22.175 L f 39.2708 24.6929 m 15.5779 24.6929 L 15.5779 1.0003 L 14.9037 1.0003 L 14.9032 25.3675 L 39.2708 25.3675 L 39.2708 24.6929 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.inre\012 3) (DblLinje1.2.inre\012 3) 1 1 39.2705 39.2706 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2702 22.175 m 39.2702 13.6108 L 26.66 13.6108 L 26.66 1.0003 L 18.0958 1.0003 L 18.0948 22.175 L 18.0958 22.175 L 18.0958 22.1752 L 39.2702 22.175 L f 39.2708 24.6929 m 15.5779 24.6929 L 15.5779 1.0003 L 14.9037 1.0003 L 14.9032 25.3675 L 39.2708 25.3675 L 39.2708 24.6929 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.inre\012 4) (DblLinje1.2.inre\012 4) 1 1 39.2705 39.2706 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2702 22.175 m 39.2702 13.6108 L 26.66 13.6108 L 26.66 1.0003 L 18.0958 1.0003 L 18.0948 22.175 L 18.0958 22.175 L 18.0958 22.1752 L 39.2702 22.175 L f 39.2708 24.6929 m 15.5779 24.6929 L 15.5779 1.0003 L 14.9037 1.0003 L 14.9032 25.3675 L 39.2708 25.3675 L 39.2708 24.6929 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.sida) (DblLinje1.2.sida) 1 1 39.2706 39.2706 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2704 18.0958 m 39.2704 26.6598 L 1.0001 26.6598 L 1.0001 18.0958 L 39.2704 18.0958 L f 39.2704 14.9037 m 39.2704 15.5776 L 1.0001 15.5776 L 1.0001 14.9037 L 39.2704 14.9037 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.sida\012 1) (DblLinje1.2.sida\012 1) 1 1 39.2706 39.2706 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2704 18.0958 m 39.2704 26.6598 L 1.0001 26.6598 L 1.0001 18.0958 L 39.2704 18.0958 L f 39.2704 14.9037 m 39.2704 15.5776 L 1.0001 15.5776 L 1.0001 14.9037 L 39.2704 14.9037 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.sida\012 2) (DblLinje1.2.sida\012 2) 1 1 39.2706 39.2706 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2704 18.0958 m 39.2704 26.6598 L 1.0001 26.6598 L 1.0001 18.0958 L 39.2704 18.0958 L f 39.2704 14.9037 m 39.2704 15.5776 L 1.0001 15.5776 L 1.0001 14.9037 L 39.2704 14.9037 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.sida\012 3) (DblLinje1.2.sida\012 3) 1 1 39.2706 39.2706 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2704 18.0958 m 39.2704 26.6598 L 1.0001 26.6598 L 1.0001 18.0958 L 39.2704 18.0958 L f 39.2704 14.9037 m 39.2704 15.5776 L 1.0001 15.5776 L 1.0001 14.9037 L 39.2704 14.9037 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.sida\012 4) (DblLinje1.2.sida\012 4) 1 1 39.2706 39.2706 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2704 18.0958 m 39.2704 26.6598 L 1.0001 26.6598 L 1.0001 18.0958 L 39.2704 18.0958 L f 39.2704 14.9037 m 39.2704 15.5776 L 1.0001 15.5776 L 1.0001 14.9037 L 39.2704 14.9037 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.yttre) (DblLinje1.2.yttre) 1 1.0003 39.2706 39.271 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2708 26.6602 m 13.6111 26.6602 L 13.6111 1.0005 L 22.1751 1 L 22.1751 18.096 L 39.2708 18.096 L 39.2708 26.6602 L f 39.2708 15.578 m 24.6928 15.578 L 24.6928 1 L 25.367 1 L 25.367 14.9038 L 39.2708 14.9038 L 39.2708 15.578 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.yttre\012 1) (DblLinje1.2.yttre\012 1) 1 1.0003 39.2706 39.271 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2708 26.6602 m 13.6111 26.6602 L 13.6111 1.0005 L 22.1751 1 L 22.1751 18.096 L 39.2708 18.096 L 39.2708 26.6602 L f 39.2708 15.578 m 24.6928 15.578 L 24.6928 1 L 25.367 1 L 25.367 14.9038 L 39.2708 14.9038 L 39.2708 15.578 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.yttre\012 2) (DblLinje1.2.yttre\012 2) 1 1.0003 39.2706 39.271 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2708 26.6602 m 13.6111 26.6602 L 13.6111 1.0005 L 22.1751 1 L 22.1751 18.096 L 39.2708 18.096 L 39.2708 26.6602 L f 39.2708 15.578 m 24.6928 15.578 L 24.6928 1 L 25.367 1 L 25.367 14.9038 L 39.2708 14.9038 L 39.2708 15.578 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.yttre\012 3) (DblLinje1.2.yttre\012 3) 1 1.0003 39.2706 39.271 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2708 26.6602 m 13.6111 26.6602 L 13.6111 1.0005 L 22.1751 1 L 22.1751 18.096 L 39.2708 18.096 L 39.2708 26.6602 L f 39.2708 15.578 m 24.6928 15.578 L 24.6928 1 L 25.367 1 L 25.367 14.9038 L 39.2708 14.9038 L 39.2708 15.578 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (DblLinje1.2.yttre\012 4) (DblLinje1.2.yttre\012 4) 1 1.0003 39.2706 39.271 [ %AI3_Tile (0 O 0 R 1 0.14 0.09 0 k 1 0.14 0.09 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 39.2708 26.6602 m 13.6111 26.6602 L 13.6111 1.0005 L 22.1751 1 L 22.1751 18.096 L 39.2708 18.096 L 39.2708 26.6602 L f 39.2708 15.578 m 24.6928 15.578 L 24.6928 1 L 25.367 1 L 25.367 14.9038 L 39.2708 14.9038 L 39.2708 15.578 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter) (Diamanter) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 1) (Diamanter\012 1) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 2) (Diamanter\012 2) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 3) (Diamanter\012 3) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 4) (Diamanter\012 4) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 5) (Diamanter\012 5) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 6) (Diamanter\012 6) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 7) (Diamanter\012 7) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 8) (Diamanter\012 8) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 9) (Diamanter\012 9) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 10) (Diamanter\012 10) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Diamanter\012 11) (Diamanter\012 11) 1 1 37.1865 41.9411 [ %AI3_Tile (0 O 0 R 0.2 0 1 0 k 0.2 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.0002 1.0004 m 1.0002 41.9411 L 37.1865 41.9411 L 37.1865 1.0004 L 1.0002 1.0004 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.0936 41.9408 m 19.0929 41.9408 L 19.0933 41.9402 L 19.0936 41.9408 L f 7.0311 41.9408 m 7.0304 41.9408 L 7.0308 41.9402 L 7.0311 41.9408 L f 31.1556 41.9408 m 31.1548 41.9408 L 31.1552 41.9402 L 31.1556 41.9408 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.75 0.9 0 0 k 0.75 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.1865 1 m 37.1865 11.2349 L 31.1552 1 L 37.1865 1 L f 19.0933 1 m 31.1552 1 L 25.124 11.2349 L 19.0933 1 L f 7.0308 1 m 19.0933 1 L 13.062 11.2349 L 7.0308 1 L f 1 1 m 7.0308 1 L 1 11.2349 L 1 1 L f 37.1859 11.2349 m 37.1865 11.236 L 37.1865 31.7059 L 31.1552 21.4704 L 37.1859 11.2349 L f 19.0933 21.4704 m 25.124 11.2349 L 31.1552 21.4704 L 25.124 31.7059 L 19.0933 21.4704 L f 7.0308 21.4704 m 13.062 11.2349 L 19.0933 21.4704 L 13.062 31.7059 L 7.0308 21.4704 L f 1 31.7059 m 1 11.2349 L 7.0308 21.4704 L 1 31.7059 L f 37.1859 31.7059 m 37.1865 31.707 L 37.1865 41.9408 L 31.1556 41.9408 L 31.1552 41.9402 L 37.1859 31.7059 L f 25.124 31.7059 m 31.1552 41.9402 L 31.1548 41.9408 L 19.0936 41.9408 L 19.0933 41.9402 L 25.124 31.7059 L f 13.062 31.7059 m 19.0933 41.9402 L 19.0929 41.9408 L 7.0311 41.9408 L 7.0308 41.9402 L 13.062 31.7059 L f 7.0304 41.9408 m 1 41.9408 L 1 31.7059 L 7.0308 41.9402 L 7.0304 41.9408 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Fallande l\232v) (Fallande l\232v) 1 1 52.733 89.816 [ %AI3_Tile (0 O 0 R 0.05 0.2 1 0 k 0.05 0.2 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 52.733 89.816 m 52.733 1 L 1 1 L 1 89.816 L 52.733 89.816 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.83 0 1 0 k 0.83 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 25.317 2.083 m 25.994 2.283 26.284 2.435 V 24.815 5.147 29.266 9.428 30.186 10.168 C 30.787 9.943 30.907 7.41 30.23 6.073 C 31.073 6.196 33.262 4.818 34.02 3.529 C 34.085 4.217 35.655 7.158 36.481 7.535 C 35.561 7.933 34.896 9.406 34.134 10.854 C 35.156 11.021 36.555 10.1 38.026 9.195 C 38.541 9.996 39.915 10.968 41.174 11.484 C 40.086 12.171 39.591 12.912 39.094 14.372 C 38.052 13.806 35.865 13.657 35.336 13.944 C 35.85 15.057 38.096 15.6 38.827 15.547 C 38.573 16.409 38.425 18.562 38.598 21.155 C 36.939 19.839 35.393 18.522 33.734 18.58 C 34.003 17.158 33.367 15.353 32.99 14.86 C 32.417 15.604 32.006 16.431 32.361 18.408 C 30.908 18.893 29.671 19.439 28.297 20.697 C 28.297 18.866 27.725 17.664 26.857 16.388 C 28.117 15.9 29.389 14.697 29.385 13.658 C 28.537 13.81 26.845 14.554 26.352 15.547 C 25.634 14.8 23.95 13.491 22.346 13.487 C 23.534 12.632 24.454 11.598 24.549 9.686 C 25.802 10.657 28.255 11.272 29.635 10.674 C 24.794 6.438 25.262 3.405 25.317 2.083 C f 12.412 33.743 m 11.887 33.272 11.691 33.01 V 14.182 31.192 11.928 25.366 11.415 24.303 C 10.776 24.247 9.369 26.988 9.405 28.486 C 8.273 27.73 6.608 27.851 5.006 28.137 C 5.578 27.049 5.177 25.104 4.376 24.303 C 5.378 24.339 6.729 23.624 8.038 22.643 C 7.203 21.823 5.376 21.984 3.46 22.643 C 3.46 21.27 2.638 19.533 1.801 18.351 C 3.117 18.408 4.262 17.722 5.12 16.691 C 5.785 18.26 7.819 19.373 8.725 19.324 C 8.742 17.959 7.169 15.869 6.147 15.47 C 6.747 14.801 7.766 13.27 8.725 10.854 C 9.524 12.78 10.694 14.022 11.927 14.955 C 10.785 16.517 10.959 17.388 11.358 18.866 C 12.101 18.325 13.132 17.893 13.303 15.89 C 15.02 16.176 16.156 16.104 17.653 15.203 C 17.198 16.865 17.195 18.466 17.515 20.166 C 15.665 20.026 14.105 20.239 13.075 21.728 C 13.905 21.955 16.165 22.014 17.039 21.082 C 17.366 22.064 18.261 23.47 19.707 24.164 C 18.267 24.424 17.282 25.523 16.373 27.209 C 15.66 25.793 13.433 24.128 11.93 24.073 C 13.933 28.137 13.933 31.055 12.412 33.743 C f 31.125 30.5 m 31.445 31.128 31.648 31.385 V 34.045 29.444 38.851 32.752 39.746 33.521 C 39.636 34.153 37.511 35.29 35.794 34.26 C 36.234 35.549 35.332 37.51 34.134 38.552 C 35.873 38.451 38.019 39.813 38.541 40.555 C 38.763 39.577 39.946 38.307 41.231 37.293 C 41.582 38.266 40.887 40.384 39.971 41.986 C 41.206 42.487 42.318 43.417 42.776 44.676 C 43.233 43.359 44.236 42.685 45.58 41.929 C 44.421 40.502 43.64 38.328 43.92 37.465 C 45.243 37.8 46.814 40.518 46.937 41.607 C 47.812 40.841 49.366 40.154 51.947 39.848 C 50.246 38.77 49.884 36.778 49.3 35.347 C 48.152 35.794 45.983 35.853 45.008 35.29 C 45.721 34.711 47.061 34.16 49.071 34.146 C 49.071 32.601 49.534 31.469 50.788 30.254 C 49.065 30.267 46.965 29.781 45.469 29.389 C 45.221 30.718 44.378 32.314 43.233 32.715 C 43.227 31.854 43.493 29.605 44.378 28.938 C 43.513 28.37 42.26 26.993 41.803 25.276 C 41.181 26.601 40.32 27.906 38.457 28.35 C 39.642 29.403 40.477 31.42 40.143 32.887 C 35.091 28.905 32.414 30.203 31.125 30.5 C f 25.317 46.491 m 25.994 46.691 26.284 46.843 V 24.815 49.556 29.266 53.837 30.186 54.576 C 30.787 54.351 30.907 51.818 30.23 50.482 C 31.073 50.605 33.262 49.227 34.02 47.938 C 34.085 48.625 35.655 51.566 36.481 51.944 C 35.561 52.341 34.896 53.814 34.134 55.263 C 35.156 55.43 36.555 54.508 38.026 53.603 C 38.541 54.404 39.915 55.377 41.174 55.892 C 40.086 56.579 39.591 57.321 39.094 58.78 C 38.052 58.215 35.865 58.065 35.336 58.353 C 35.85 59.465 38.096 60.008 38.827 59.955 C 38.573 60.817 38.425 62.97 38.598 65.563 C 36.939 64.247 35.393 62.931 33.734 62.988 C 34.003 61.567 33.367 59.761 32.99 59.268 C 32.417 60.012 32.006 60.839 32.361 62.817 C 30.908 63.302 29.671 63.847 28.297 65.106 C 28.297 63.274 27.725 62.073 26.857 60.796 C 28.117 60.308 29.389 59.106 29.385 58.067 C 28.537 58.219 26.845 58.963 26.352 59.955 C 25.634 59.209 23.95 57.899 22.346 57.895 C 23.534 57.041 24.454 56.006 24.549 54.094 C 25.802 55.065 28.255 55.68 29.635 55.083 C 24.794 50.846 25.262 47.814 25.317 46.491 C f 12.412 78.151 m 11.887 77.68 11.691 77.418 V 14.182 75.601 11.928 69.774 11.415 68.711 C 10.776 68.655 9.369 71.396 9.405 72.894 C 8.273 72.138 6.608 72.259 5.006 72.545 C 5.578 71.458 5.177 69.512 4.376 68.711 C 5.378 68.747 6.729 68.032 8.038 67.052 C 7.203 66.231 5.376 66.393 3.46 67.052 C 3.46 65.678 2.638 63.941 1.801 62.759 C 3.117 62.817 4.262 62.13 5.12 61.1 C 5.785 62.669 7.819 63.781 8.725 63.732 C 8.742 62.367 7.169 60.277 6.147 59.878 C 6.747 59.209 7.766 57.678 8.725 55.263 C 9.524 57.189 10.694 58.431 11.927 59.364 C 10.785 60.925 10.959 61.796 11.358 63.274 C 12.101 62.734 13.132 62.301 13.303 60.298 C 15.02 60.584 16.156 60.512 17.653 59.612 C 17.198 61.273 17.195 62.874 17.515 64.574 C 15.665 64.434 14.105 64.648 13.075 66.136 C 13.905 66.363 16.165 66.422 17.039 65.49 C 17.366 66.472 18.261 67.878 19.707 68.572 C 18.267 68.832 17.282 69.931 16.373 71.617 C 15.66 70.202 13.433 68.536 11.93 68.482 C 13.933 72.545 13.933 75.464 12.412 78.151 C f 31.125 74.908 m 31.445 75.537 31.648 75.794 V 34.045 73.853 38.851 77.161 39.746 77.929 C 39.636 78.562 37.511 79.698 35.794 78.668 C 36.234 79.957 35.332 81.918 34.134 82.96 C 35.873 82.86 38.019 84.221 38.541 84.963 C 38.763 83.986 39.946 82.716 41.231 81.701 C 41.582 82.675 40.887 84.792 39.971 86.394 C 41.206 86.895 42.318 87.825 42.776 89.084 C 43.233 87.768 44.236 87.093 45.58 86.337 C 44.421 84.91 43.64 82.736 43.92 81.873 C 45.243 82.208 46.814 84.926 46.937 86.016 C 47.812 85.249 49.366 84.563 51.947 84.257 C 50.246 83.179 49.884 81.187 49.3 79.756 C 48.152 80.203 45.983 80.262 45.008 79.698 C 45.721 79.119 47.061 78.569 49.071 78.554 C 49.071 77.009 49.534 75.877 50.788 74.663 C 49.065 74.675 46.965 74.189 45.469 73.798 C 45.221 75.126 44.378 76.723 43.233 77.123 C 43.227 76.262 43.493 74.013 44.378 73.347 C 43.513 72.779 42.26 71.401 41.803 69.684 C 41.181 71.009 40.32 72.314 38.457 72.759 C 39.642 73.812 40.477 75.829 40.143 77.295 C 35.091 73.313 32.414 74.611 31.125 74.908 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Fallande l\232v\012 1) (Fallande l\232v\012 1) 1 1 52.733 89.816 [ %AI3_Tile (0 O 0 R 0.05 0.2 1 0 k 0.05 0.2 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 52.733 89.816 m 52.733 1 L 1 1 L 1 89.816 L 52.733 89.816 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.83 0 1 0 k 0.83 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 25.317 2.083 m 25.994 2.283 26.284 2.435 V 24.815 5.147 29.266 9.428 30.186 10.168 C 30.787 9.943 30.907 7.41 30.23 6.073 C 31.073 6.196 33.262 4.818 34.02 3.529 C 34.085 4.217 35.655 7.158 36.481 7.535 C 35.561 7.933 34.896 9.406 34.134 10.854 C 35.156 11.021 36.555 10.1 38.026 9.195 C 38.541 9.996 39.915 10.968 41.174 11.484 C 40.086 12.171 39.591 12.912 39.094 14.372 C 38.052 13.806 35.865 13.657 35.336 13.944 C 35.85 15.057 38.096 15.6 38.827 15.547 C 38.573 16.409 38.425 18.562 38.598 21.155 C 36.939 19.839 35.393 18.522 33.734 18.58 C 34.003 17.158 33.367 15.353 32.99 14.86 C 32.417 15.604 32.006 16.431 32.361 18.408 C 30.908 18.893 29.671 19.439 28.297 20.697 C 28.297 18.866 27.725 17.664 26.857 16.388 C 28.117 15.9 29.389 14.697 29.385 13.658 C 28.537 13.81 26.845 14.554 26.352 15.547 C 25.634 14.8 23.95 13.491 22.346 13.487 C 23.534 12.632 24.454 11.598 24.549 9.686 C 25.802 10.657 28.255 11.272 29.635 10.674 C 24.794 6.438 25.262 3.405 25.317 2.083 C f 12.412 33.743 m 11.887 33.272 11.691 33.01 V 14.182 31.192 11.928 25.366 11.415 24.303 C 10.776 24.247 9.369 26.988 9.405 28.486 C 8.273 27.73 6.608 27.851 5.006 28.137 C 5.578 27.049 5.177 25.104 4.376 24.303 C 5.378 24.339 6.729 23.624 8.038 22.643 C 7.203 21.823 5.376 21.984 3.46 22.643 C 3.46 21.27 2.638 19.533 1.801 18.351 C 3.117 18.408 4.262 17.722 5.12 16.691 C 5.785 18.26 7.819 19.373 8.725 19.324 C 8.742 17.959 7.169 15.869 6.147 15.47 C 6.747 14.801 7.766 13.27 8.725 10.854 C 9.524 12.78 10.694 14.022 11.927 14.955 C 10.785 16.517 10.959 17.388 11.358 18.866 C 12.101 18.325 13.132 17.893 13.303 15.89 C 15.02 16.176 16.156 16.104 17.653 15.203 C 17.198 16.865 17.195 18.466 17.515 20.166 C 15.665 20.026 14.105 20.239 13.075 21.728 C 13.905 21.955 16.165 22.014 17.039 21.082 C 17.366 22.064 18.261 23.47 19.707 24.164 C 18.267 24.424 17.282 25.523 16.373 27.209 C 15.66 25.793 13.433 24.128 11.93 24.073 C 13.933 28.137 13.933 31.055 12.412 33.743 C f 31.125 30.5 m 31.445 31.128 31.648 31.385 V 34.045 29.444 38.851 32.752 39.746 33.521 C 39.636 34.153 37.511 35.29 35.794 34.26 C 36.234 35.549 35.332 37.51 34.134 38.552 C 35.873 38.451 38.019 39.813 38.541 40.555 C 38.763 39.577 39.946 38.307 41.231 37.293 C 41.582 38.266 40.887 40.384 39.971 41.986 C 41.206 42.487 42.318 43.417 42.776 44.676 C 43.233 43.359 44.236 42.685 45.58 41.929 C 44.421 40.502 43.64 38.328 43.92 37.465 C 45.243 37.8 46.814 40.518 46.937 41.607 C 47.812 40.841 49.366 40.154 51.947 39.848 C 50.246 38.77 49.884 36.778 49.3 35.347 C 48.152 35.794 45.983 35.853 45.008 35.29 C 45.721 34.711 47.061 34.16 49.071 34.146 C 49.071 32.601 49.534 31.469 50.788 30.254 C 49.065 30.267 46.965 29.781 45.469 29.389 C 45.221 30.718 44.378 32.314 43.233 32.715 C 43.227 31.854 43.493 29.605 44.378 28.938 C 43.513 28.37 42.26 26.993 41.803 25.276 C 41.181 26.601 40.32 27.906 38.457 28.35 C 39.642 29.403 40.477 31.42 40.143 32.887 C 35.091 28.905 32.414 30.203 31.125 30.5 C f 25.317 46.491 m 25.994 46.691 26.284 46.843 V 24.815 49.556 29.266 53.837 30.186 54.576 C 30.787 54.351 30.907 51.818 30.23 50.482 C 31.073 50.605 33.262 49.227 34.02 47.938 C 34.085 48.625 35.655 51.566 36.481 51.944 C 35.561 52.341 34.896 53.814 34.134 55.263 C 35.156 55.43 36.555 54.508 38.026 53.603 C 38.541 54.404 39.915 55.377 41.174 55.892 C 40.086 56.579 39.591 57.321 39.094 58.78 C 38.052 58.215 35.865 58.065 35.336 58.353 C 35.85 59.465 38.096 60.008 38.827 59.955 C 38.573 60.817 38.425 62.97 38.598 65.563 C 36.939 64.247 35.393 62.931 33.734 62.988 C 34.003 61.567 33.367 59.761 32.99 59.268 C 32.417 60.012 32.006 60.839 32.361 62.817 C 30.908 63.302 29.671 63.847 28.297 65.106 C 28.297 63.274 27.725 62.073 26.857 60.796 C 28.117 60.308 29.389 59.106 29.385 58.067 C 28.537 58.219 26.845 58.963 26.352 59.955 C 25.634 59.209 23.95 57.899 22.346 57.895 C 23.534 57.041 24.454 56.006 24.549 54.094 C 25.802 55.065 28.255 55.68 29.635 55.083 C 24.794 50.846 25.262 47.814 25.317 46.491 C f 12.412 78.151 m 11.887 77.68 11.691 77.418 V 14.182 75.601 11.928 69.774 11.415 68.711 C 10.776 68.655 9.369 71.396 9.405 72.894 C 8.273 72.138 6.608 72.259 5.006 72.545 C 5.578 71.458 5.177 69.512 4.376 68.711 C 5.378 68.747 6.729 68.032 8.038 67.052 C 7.203 66.231 5.376 66.393 3.46 67.052 C 3.46 65.678 2.638 63.941 1.801 62.759 C 3.117 62.817 4.262 62.13 5.12 61.1 C 5.785 62.669 7.819 63.781 8.725 63.732 C 8.742 62.367 7.169 60.277 6.147 59.878 C 6.747 59.209 7.766 57.678 8.725 55.263 C 9.524 57.189 10.694 58.431 11.927 59.364 C 10.785 60.925 10.959 61.796 11.358 63.274 C 12.101 62.734 13.132 62.301 13.303 60.298 C 15.02 60.584 16.156 60.512 17.653 59.612 C 17.198 61.273 17.195 62.874 17.515 64.574 C 15.665 64.434 14.105 64.648 13.075 66.136 C 13.905 66.363 16.165 66.422 17.039 65.49 C 17.366 66.472 18.261 67.878 19.707 68.572 C 18.267 68.832 17.282 69.931 16.373 71.617 C 15.66 70.202 13.433 68.536 11.93 68.482 C 13.933 72.545 13.933 75.464 12.412 78.151 C f 31.125 74.908 m 31.445 75.537 31.648 75.794 V 34.045 73.853 38.851 77.161 39.746 77.929 C 39.636 78.562 37.511 79.698 35.794 78.668 C 36.234 79.957 35.332 81.918 34.134 82.96 C 35.873 82.86 38.019 84.221 38.541 84.963 C 38.763 83.986 39.946 82.716 41.231 81.701 C 41.582 82.675 40.887 84.792 39.971 86.394 C 41.206 86.895 42.318 87.825 42.776 89.084 C 43.233 87.768 44.236 87.093 45.58 86.337 C 44.421 84.91 43.64 82.736 43.92 81.873 C 45.243 82.208 46.814 84.926 46.937 86.016 C 47.812 85.249 49.366 84.563 51.947 84.257 C 50.246 83.179 49.884 81.187 49.3 79.756 C 48.152 80.203 45.983 80.262 45.008 79.698 C 45.721 79.119 47.061 78.569 49.071 78.554 C 49.071 77.009 49.534 75.877 50.788 74.663 C 49.065 74.675 46.965 74.189 45.469 73.798 C 45.221 75.126 44.378 76.723 43.233 77.123 C 43.227 76.262 43.493 74.013 44.378 73.347 C 43.513 72.779 42.26 71.401 41.803 69.684 C 41.181 71.009 40.32 72.314 38.457 72.759 C 39.642 73.812 40.477 75.829 40.143 77.295 C 35.091 73.313 32.414 74.611 31.125 74.908 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Fallande l\232v\012 2) (Fallande l\232v\012 2) 1 1 52.733 89.816 [ %AI3_Tile (0 O 0 R 0.05 0.2 1 0 k 0.05 0.2 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 52.733 89.816 m 52.733 1 L 1 1 L 1 89.816 L 52.733 89.816 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.83 0 1 0 k 0.83 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 25.317 2.083 m 25.994 2.283 26.284 2.435 V 24.815 5.147 29.266 9.428 30.186 10.168 C 30.787 9.943 30.907 7.41 30.23 6.073 C 31.073 6.196 33.262 4.818 34.02 3.529 C 34.085 4.217 35.655 7.158 36.481 7.535 C 35.561 7.933 34.896 9.406 34.134 10.854 C 35.156 11.021 36.555 10.1 38.026 9.195 C 38.541 9.996 39.915 10.968 41.174 11.484 C 40.086 12.171 39.591 12.912 39.094 14.372 C 38.052 13.806 35.865 13.657 35.336 13.944 C 35.85 15.057 38.096 15.6 38.827 15.547 C 38.573 16.409 38.425 18.562 38.598 21.155 C 36.939 19.839 35.393 18.522 33.734 18.58 C 34.003 17.158 33.367 15.353 32.99 14.86 C 32.417 15.604 32.006 16.431 32.361 18.408 C 30.908 18.893 29.671 19.439 28.297 20.697 C 28.297 18.866 27.725 17.664 26.857 16.388 C 28.117 15.9 29.389 14.697 29.385 13.658 C 28.537 13.81 26.845 14.554 26.352 15.547 C 25.634 14.8 23.95 13.491 22.346 13.487 C 23.534 12.632 24.454 11.598 24.549 9.686 C 25.802 10.657 28.255 11.272 29.635 10.674 C 24.794 6.438 25.262 3.405 25.317 2.083 C f 12.412 33.743 m 11.887 33.272 11.691 33.01 V 14.182 31.192 11.928 25.366 11.415 24.303 C 10.776 24.247 9.369 26.988 9.405 28.486 C 8.273 27.73 6.608 27.851 5.006 28.137 C 5.578 27.049 5.177 25.104 4.376 24.303 C 5.378 24.339 6.729 23.624 8.038 22.643 C 7.203 21.823 5.376 21.984 3.46 22.643 C 3.46 21.27 2.638 19.533 1.801 18.351 C 3.117 18.408 4.262 17.722 5.12 16.691 C 5.785 18.26 7.819 19.373 8.725 19.324 C 8.742 17.959 7.169 15.869 6.147 15.47 C 6.747 14.801 7.766 13.27 8.725 10.854 C 9.524 12.78 10.694 14.022 11.927 14.955 C 10.785 16.517 10.959 17.388 11.358 18.866 C 12.101 18.325 13.132 17.893 13.303 15.89 C 15.02 16.176 16.156 16.104 17.653 15.203 C 17.198 16.865 17.195 18.466 17.515 20.166 C 15.665 20.026 14.105 20.239 13.075 21.728 C 13.905 21.955 16.165 22.014 17.039 21.082 C 17.366 22.064 18.261 23.47 19.707 24.164 C 18.267 24.424 17.282 25.523 16.373 27.209 C 15.66 25.793 13.433 24.128 11.93 24.073 C 13.933 28.137 13.933 31.055 12.412 33.743 C f 31.125 30.5 m 31.445 31.128 31.648 31.385 V 34.045 29.444 38.851 32.752 39.746 33.521 C 39.636 34.153 37.511 35.29 35.794 34.26 C 36.234 35.549 35.332 37.51 34.134 38.552 C 35.873 38.451 38.019 39.813 38.541 40.555 C 38.763 39.577 39.946 38.307 41.231 37.293 C 41.582 38.266 40.887 40.384 39.971 41.986 C 41.206 42.487 42.318 43.417 42.776 44.676 C 43.233 43.359 44.236 42.685 45.58 41.929 C 44.421 40.502 43.64 38.328 43.92 37.465 C 45.243 37.8 46.814 40.518 46.937 41.607 C 47.812 40.841 49.366 40.154 51.947 39.848 C 50.246 38.77 49.884 36.778 49.3 35.347 C 48.152 35.794 45.983 35.853 45.008 35.29 C 45.721 34.711 47.061 34.16 49.071 34.146 C 49.071 32.601 49.534 31.469 50.788 30.254 C 49.065 30.267 46.965 29.781 45.469 29.389 C 45.221 30.718 44.378 32.314 43.233 32.715 C 43.227 31.854 43.493 29.605 44.378 28.938 C 43.513 28.37 42.26 26.993 41.803 25.276 C 41.181 26.601 40.32 27.906 38.457 28.35 C 39.642 29.403 40.477 31.42 40.143 32.887 C 35.091 28.905 32.414 30.203 31.125 30.5 C f 25.317 46.491 m 25.994 46.691 26.284 46.843 V 24.815 49.556 29.266 53.837 30.186 54.576 C 30.787 54.351 30.907 51.818 30.23 50.482 C 31.073 50.605 33.262 49.227 34.02 47.938 C 34.085 48.625 35.655 51.566 36.481 51.944 C 35.561 52.341 34.896 53.814 34.134 55.263 C 35.156 55.43 36.555 54.508 38.026 53.603 C 38.541 54.404 39.915 55.377 41.174 55.892 C 40.086 56.579 39.591 57.321 39.094 58.78 C 38.052 58.215 35.865 58.065 35.336 58.353 C 35.85 59.465 38.096 60.008 38.827 59.955 C 38.573 60.817 38.425 62.97 38.598 65.563 C 36.939 64.247 35.393 62.931 33.734 62.988 C 34.003 61.567 33.367 59.761 32.99 59.268 C 32.417 60.012 32.006 60.839 32.361 62.817 C 30.908 63.302 29.671 63.847 28.297 65.106 C 28.297 63.274 27.725 62.073 26.857 60.796 C 28.117 60.308 29.389 59.106 29.385 58.067 C 28.537 58.219 26.845 58.963 26.352 59.955 C 25.634 59.209 23.95 57.899 22.346 57.895 C 23.534 57.041 24.454 56.006 24.549 54.094 C 25.802 55.065 28.255 55.68 29.635 55.083 C 24.794 50.846 25.262 47.814 25.317 46.491 C f 12.412 78.151 m 11.887 77.68 11.691 77.418 V 14.182 75.601 11.928 69.774 11.415 68.711 C 10.776 68.655 9.369 71.396 9.405 72.894 C 8.273 72.138 6.608 72.259 5.006 72.545 C 5.578 71.458 5.177 69.512 4.376 68.711 C 5.378 68.747 6.729 68.032 8.038 67.052 C 7.203 66.231 5.376 66.393 3.46 67.052 C 3.46 65.678 2.638 63.941 1.801 62.759 C 3.117 62.817 4.262 62.13 5.12 61.1 C 5.785 62.669 7.819 63.781 8.725 63.732 C 8.742 62.367 7.169 60.277 6.147 59.878 C 6.747 59.209 7.766 57.678 8.725 55.263 C 9.524 57.189 10.694 58.431 11.927 59.364 C 10.785 60.925 10.959 61.796 11.358 63.274 C 12.101 62.734 13.132 62.301 13.303 60.298 C 15.02 60.584 16.156 60.512 17.653 59.612 C 17.198 61.273 17.195 62.874 17.515 64.574 C 15.665 64.434 14.105 64.648 13.075 66.136 C 13.905 66.363 16.165 66.422 17.039 65.49 C 17.366 66.472 18.261 67.878 19.707 68.572 C 18.267 68.832 17.282 69.931 16.373 71.617 C 15.66 70.202 13.433 68.536 11.93 68.482 C 13.933 72.545 13.933 75.464 12.412 78.151 C f 31.125 74.908 m 31.445 75.537 31.648 75.794 V 34.045 73.853 38.851 77.161 39.746 77.929 C 39.636 78.562 37.511 79.698 35.794 78.668 C 36.234 79.957 35.332 81.918 34.134 82.96 C 35.873 82.86 38.019 84.221 38.541 84.963 C 38.763 83.986 39.946 82.716 41.231 81.701 C 41.582 82.675 40.887 84.792 39.971 86.394 C 41.206 86.895 42.318 87.825 42.776 89.084 C 43.233 87.768 44.236 87.093 45.58 86.337 C 44.421 84.91 43.64 82.736 43.92 81.873 C 45.243 82.208 46.814 84.926 46.937 86.016 C 47.812 85.249 49.366 84.563 51.947 84.257 C 50.246 83.179 49.884 81.187 49.3 79.756 C 48.152 80.203 45.983 80.262 45.008 79.698 C 45.721 79.119 47.061 78.569 49.071 78.554 C 49.071 77.009 49.534 75.877 50.788 74.663 C 49.065 74.675 46.965 74.189 45.469 73.798 C 45.221 75.126 44.378 76.723 43.233 77.123 C 43.227 76.262 43.493 74.013 44.378 73.347 C 43.513 72.779 42.26 71.401 41.803 69.684 C 41.181 71.009 40.32 72.314 38.457 72.759 C 39.642 73.812 40.477 75.829 40.143 77.295 C 35.091 73.313 32.414 74.611 31.125 74.908 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Fallande l\232v\012 3) (Fallande l\232v\012 3) 1 1 52.733 89.816 [ %AI3_Tile (0 O 0 R 0.05 0.2 1 0 k 0.05 0.2 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 52.733 89.816 m 52.733 1 L 1 1 L 1 89.816 L 52.733 89.816 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.83 0 1 0 k 0.83 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 25.317 2.083 m 25.994 2.283 26.284 2.435 V 24.815 5.147 29.266 9.428 30.186 10.168 C 30.787 9.943 30.907 7.41 30.23 6.073 C 31.073 6.196 33.262 4.818 34.02 3.529 C 34.085 4.217 35.655 7.158 36.481 7.535 C 35.561 7.933 34.896 9.406 34.134 10.854 C 35.156 11.021 36.555 10.1 38.026 9.195 C 38.541 9.996 39.915 10.968 41.174 11.484 C 40.086 12.171 39.591 12.912 39.094 14.372 C 38.052 13.806 35.865 13.657 35.336 13.944 C 35.85 15.057 38.096 15.6 38.827 15.547 C 38.573 16.409 38.425 18.562 38.598 21.155 C 36.939 19.839 35.393 18.522 33.734 18.58 C 34.003 17.158 33.367 15.353 32.99 14.86 C 32.417 15.604 32.006 16.431 32.361 18.408 C 30.908 18.893 29.671 19.439 28.297 20.697 C 28.297 18.866 27.725 17.664 26.857 16.388 C 28.117 15.9 29.389 14.697 29.385 13.658 C 28.537 13.81 26.845 14.554 26.352 15.547 C 25.634 14.8 23.95 13.491 22.346 13.487 C 23.534 12.632 24.454 11.598 24.549 9.686 C 25.802 10.657 28.255 11.272 29.635 10.674 C 24.794 6.438 25.262 3.405 25.317 2.083 C f 12.412 33.743 m 11.887 33.272 11.691 33.01 V 14.182 31.192 11.928 25.366 11.415 24.303 C 10.776 24.247 9.369 26.988 9.405 28.486 C 8.273 27.73 6.608 27.851 5.006 28.137 C 5.578 27.049 5.177 25.104 4.376 24.303 C 5.378 24.339 6.729 23.624 8.038 22.643 C 7.203 21.823 5.376 21.984 3.46 22.643 C 3.46 21.27 2.638 19.533 1.801 18.351 C 3.117 18.408 4.262 17.722 5.12 16.691 C 5.785 18.26 7.819 19.373 8.725 19.324 C 8.742 17.959 7.169 15.869 6.147 15.47 C 6.747 14.801 7.766 13.27 8.725 10.854 C 9.524 12.78 10.694 14.022 11.927 14.955 C 10.785 16.517 10.959 17.388 11.358 18.866 C 12.101 18.325 13.132 17.893 13.303 15.89 C 15.02 16.176 16.156 16.104 17.653 15.203 C 17.198 16.865 17.195 18.466 17.515 20.166 C 15.665 20.026 14.105 20.239 13.075 21.728 C 13.905 21.955 16.165 22.014 17.039 21.082 C 17.366 22.064 18.261 23.47 19.707 24.164 C 18.267 24.424 17.282 25.523 16.373 27.209 C 15.66 25.793 13.433 24.128 11.93 24.073 C 13.933 28.137 13.933 31.055 12.412 33.743 C f 31.125 30.5 m 31.445 31.128 31.648 31.385 V 34.045 29.444 38.851 32.752 39.746 33.521 C 39.636 34.153 37.511 35.29 35.794 34.26 C 36.234 35.549 35.332 37.51 34.134 38.552 C 35.873 38.451 38.019 39.813 38.541 40.555 C 38.763 39.577 39.946 38.307 41.231 37.293 C 41.582 38.266 40.887 40.384 39.971 41.986 C 41.206 42.487 42.318 43.417 42.776 44.676 C 43.233 43.359 44.236 42.685 45.58 41.929 C 44.421 40.502 43.64 38.328 43.92 37.465 C 45.243 37.8 46.814 40.518 46.937 41.607 C 47.812 40.841 49.366 40.154 51.947 39.848 C 50.246 38.77 49.884 36.778 49.3 35.347 C 48.152 35.794 45.983 35.853 45.008 35.29 C 45.721 34.711 47.061 34.16 49.071 34.146 C 49.071 32.601 49.534 31.469 50.788 30.254 C 49.065 30.267 46.965 29.781 45.469 29.389 C 45.221 30.718 44.378 32.314 43.233 32.715 C 43.227 31.854 43.493 29.605 44.378 28.938 C 43.513 28.37 42.26 26.993 41.803 25.276 C 41.181 26.601 40.32 27.906 38.457 28.35 C 39.642 29.403 40.477 31.42 40.143 32.887 C 35.091 28.905 32.414 30.203 31.125 30.5 C f 25.317 46.491 m 25.994 46.691 26.284 46.843 V 24.815 49.556 29.266 53.837 30.186 54.576 C 30.787 54.351 30.907 51.818 30.23 50.482 C 31.073 50.605 33.262 49.227 34.02 47.938 C 34.085 48.625 35.655 51.566 36.481 51.944 C 35.561 52.341 34.896 53.814 34.134 55.263 C 35.156 55.43 36.555 54.508 38.026 53.603 C 38.541 54.404 39.915 55.377 41.174 55.892 C 40.086 56.579 39.591 57.321 39.094 58.78 C 38.052 58.215 35.865 58.065 35.336 58.353 C 35.85 59.465 38.096 60.008 38.827 59.955 C 38.573 60.817 38.425 62.97 38.598 65.563 C 36.939 64.247 35.393 62.931 33.734 62.988 C 34.003 61.567 33.367 59.761 32.99 59.268 C 32.417 60.012 32.006 60.839 32.361 62.817 C 30.908 63.302 29.671 63.847 28.297 65.106 C 28.297 63.274 27.725 62.073 26.857 60.796 C 28.117 60.308 29.389 59.106 29.385 58.067 C 28.537 58.219 26.845 58.963 26.352 59.955 C 25.634 59.209 23.95 57.899 22.346 57.895 C 23.534 57.041 24.454 56.006 24.549 54.094 C 25.802 55.065 28.255 55.68 29.635 55.083 C 24.794 50.846 25.262 47.814 25.317 46.491 C f 12.412 78.151 m 11.887 77.68 11.691 77.418 V 14.182 75.601 11.928 69.774 11.415 68.711 C 10.776 68.655 9.369 71.396 9.405 72.894 C 8.273 72.138 6.608 72.259 5.006 72.545 C 5.578 71.458 5.177 69.512 4.376 68.711 C 5.378 68.747 6.729 68.032 8.038 67.052 C 7.203 66.231 5.376 66.393 3.46 67.052 C 3.46 65.678 2.638 63.941 1.801 62.759 C 3.117 62.817 4.262 62.13 5.12 61.1 C 5.785 62.669 7.819 63.781 8.725 63.732 C 8.742 62.367 7.169 60.277 6.147 59.878 C 6.747 59.209 7.766 57.678 8.725 55.263 C 9.524 57.189 10.694 58.431 11.927 59.364 C 10.785 60.925 10.959 61.796 11.358 63.274 C 12.101 62.734 13.132 62.301 13.303 60.298 C 15.02 60.584 16.156 60.512 17.653 59.612 C 17.198 61.273 17.195 62.874 17.515 64.574 C 15.665 64.434 14.105 64.648 13.075 66.136 C 13.905 66.363 16.165 66.422 17.039 65.49 C 17.366 66.472 18.261 67.878 19.707 68.572 C 18.267 68.832 17.282 69.931 16.373 71.617 C 15.66 70.202 13.433 68.536 11.93 68.482 C 13.933 72.545 13.933 75.464 12.412 78.151 C f 31.125 74.908 m 31.445 75.537 31.648 75.794 V 34.045 73.853 38.851 77.161 39.746 77.929 C 39.636 78.562 37.511 79.698 35.794 78.668 C 36.234 79.957 35.332 81.918 34.134 82.96 C 35.873 82.86 38.019 84.221 38.541 84.963 C 38.763 83.986 39.946 82.716 41.231 81.701 C 41.582 82.675 40.887 84.792 39.971 86.394 C 41.206 86.895 42.318 87.825 42.776 89.084 C 43.233 87.768 44.236 87.093 45.58 86.337 C 44.421 84.91 43.64 82.736 43.92 81.873 C 45.243 82.208 46.814 84.926 46.937 86.016 C 47.812 85.249 49.366 84.563 51.947 84.257 C 50.246 83.179 49.884 81.187 49.3 79.756 C 48.152 80.203 45.983 80.262 45.008 79.698 C 45.721 79.119 47.061 78.569 49.071 78.554 C 49.071 77.009 49.534 75.877 50.788 74.663 C 49.065 74.675 46.965 74.189 45.469 73.798 C 45.221 75.126 44.378 76.723 43.233 77.123 C 43.227 76.262 43.493 74.013 44.378 73.347 C 43.513 72.779 42.26 71.401 41.803 69.684 C 41.181 71.009 40.32 72.314 38.457 72.759 C 39.642 73.812 40.477 75.829 40.143 77.295 C 35.091 73.313 32.414 74.611 31.125 74.908 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Fallande l\232v\012 4) (Fallande l\232v\012 4) 1 1 52.733 89.816 [ %AI3_Tile (0 O 0 R 0.05 0.2 1 0 k 0.05 0.2 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 52.733 89.816 m 52.733 1 L 1 1 L 1 89.816 L 52.733 89.816 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.83 0 1 0 k 0.83 0 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 25.317 2.083 m 25.994 2.283 26.284 2.435 V 24.815 5.147 29.266 9.428 30.186 10.168 C 30.787 9.943 30.907 7.41 30.23 6.073 C 31.073 6.196 33.262 4.818 34.02 3.529 C 34.085 4.217 35.655 7.158 36.481 7.535 C 35.561 7.933 34.896 9.406 34.134 10.854 C 35.156 11.021 36.555 10.1 38.026 9.195 C 38.541 9.996 39.915 10.968 41.174 11.484 C 40.086 12.171 39.591 12.912 39.094 14.372 C 38.052 13.806 35.865 13.657 35.336 13.944 C 35.85 15.057 38.096 15.6 38.827 15.547 C 38.573 16.409 38.425 18.562 38.598 21.155 C 36.939 19.839 35.393 18.522 33.734 18.58 C 34.003 17.158 33.367 15.353 32.99 14.86 C 32.417 15.604 32.006 16.431 32.361 18.408 C 30.908 18.893 29.671 19.439 28.297 20.697 C 28.297 18.866 27.725 17.664 26.857 16.388 C 28.117 15.9 29.389 14.697 29.385 13.658 C 28.537 13.81 26.845 14.554 26.352 15.547 C 25.634 14.8 23.95 13.491 22.346 13.487 C 23.534 12.632 24.454 11.598 24.549 9.686 C 25.802 10.657 28.255 11.272 29.635 10.674 C 24.794 6.438 25.262 3.405 25.317 2.083 C f 12.412 33.743 m 11.887 33.272 11.691 33.01 V 14.182 31.192 11.928 25.366 11.415 24.303 C 10.776 24.247 9.369 26.988 9.405 28.486 C 8.273 27.73 6.608 27.851 5.006 28.137 C 5.578 27.049 5.177 25.104 4.376 24.303 C 5.378 24.339 6.729 23.624 8.038 22.643 C 7.203 21.823 5.376 21.984 3.46 22.643 C 3.46 21.27 2.638 19.533 1.801 18.351 C 3.117 18.408 4.262 17.722 5.12 16.691 C 5.785 18.26 7.819 19.373 8.725 19.324 C 8.742 17.959 7.169 15.869 6.147 15.47 C 6.747 14.801 7.766 13.27 8.725 10.854 C 9.524 12.78 10.694 14.022 11.927 14.955 C 10.785 16.517 10.959 17.388 11.358 18.866 C 12.101 18.325 13.132 17.893 13.303 15.89 C 15.02 16.176 16.156 16.104 17.653 15.203 C 17.198 16.865 17.195 18.466 17.515 20.166 C 15.665 20.026 14.105 20.239 13.075 21.728 C 13.905 21.955 16.165 22.014 17.039 21.082 C 17.366 22.064 18.261 23.47 19.707 24.164 C 18.267 24.424 17.282 25.523 16.373 27.209 C 15.66 25.793 13.433 24.128 11.93 24.073 C 13.933 28.137 13.933 31.055 12.412 33.743 C f 31.125 30.5 m 31.445 31.128 31.648 31.385 V 34.045 29.444 38.851 32.752 39.746 33.521 C 39.636 34.153 37.511 35.29 35.794 34.26 C 36.234 35.549 35.332 37.51 34.134 38.552 C 35.873 38.451 38.019 39.813 38.541 40.555 C 38.763 39.577 39.946 38.307 41.231 37.293 C 41.582 38.266 40.887 40.384 39.971 41.986 C 41.206 42.487 42.318 43.417 42.776 44.676 C 43.233 43.359 44.236 42.685 45.58 41.929 C 44.421 40.502 43.64 38.328 43.92 37.465 C 45.243 37.8 46.814 40.518 46.937 41.607 C 47.812 40.841 49.366 40.154 51.947 39.848 C 50.246 38.77 49.884 36.778 49.3 35.347 C 48.152 35.794 45.983 35.853 45.008 35.29 C 45.721 34.711 47.061 34.16 49.071 34.146 C 49.071 32.601 49.534 31.469 50.788 30.254 C 49.065 30.267 46.965 29.781 45.469 29.389 C 45.221 30.718 44.378 32.314 43.233 32.715 C 43.227 31.854 43.493 29.605 44.378 28.938 C 43.513 28.37 42.26 26.993 41.803 25.276 C 41.181 26.601 40.32 27.906 38.457 28.35 C 39.642 29.403 40.477 31.42 40.143 32.887 C 35.091 28.905 32.414 30.203 31.125 30.5 C f 25.317 46.491 m 25.994 46.691 26.284 46.843 V 24.815 49.556 29.266 53.837 30.186 54.576 C 30.787 54.351 30.907 51.818 30.23 50.482 C 31.073 50.605 33.262 49.227 34.02 47.938 C 34.085 48.625 35.655 51.566 36.481 51.944 C 35.561 52.341 34.896 53.814 34.134 55.263 C 35.156 55.43 36.555 54.508 38.026 53.603 C 38.541 54.404 39.915 55.377 41.174 55.892 C 40.086 56.579 39.591 57.321 39.094 58.78 C 38.052 58.215 35.865 58.065 35.336 58.353 C 35.85 59.465 38.096 60.008 38.827 59.955 C 38.573 60.817 38.425 62.97 38.598 65.563 C 36.939 64.247 35.393 62.931 33.734 62.988 C 34.003 61.567 33.367 59.761 32.99 59.268 C 32.417 60.012 32.006 60.839 32.361 62.817 C 30.908 63.302 29.671 63.847 28.297 65.106 C 28.297 63.274 27.725 62.073 26.857 60.796 C 28.117 60.308 29.389 59.106 29.385 58.067 C 28.537 58.219 26.845 58.963 26.352 59.955 C 25.634 59.209 23.95 57.899 22.346 57.895 C 23.534 57.041 24.454 56.006 24.549 54.094 C 25.802 55.065 28.255 55.68 29.635 55.083 C 24.794 50.846 25.262 47.814 25.317 46.491 C f 12.412 78.151 m 11.887 77.68 11.691 77.418 V 14.182 75.601 11.928 69.774 11.415 68.711 C 10.776 68.655 9.369 71.396 9.405 72.894 C 8.273 72.138 6.608 72.259 5.006 72.545 C 5.578 71.458 5.177 69.512 4.376 68.711 C 5.378 68.747 6.729 68.032 8.038 67.052 C 7.203 66.231 5.376 66.393 3.46 67.052 C 3.46 65.678 2.638 63.941 1.801 62.759 C 3.117 62.817 4.262 62.13 5.12 61.1 C 5.785 62.669 7.819 63.781 8.725 63.732 C 8.742 62.367 7.169 60.277 6.147 59.878 C 6.747 59.209 7.766 57.678 8.725 55.263 C 9.524 57.189 10.694 58.431 11.927 59.364 C 10.785 60.925 10.959 61.796 11.358 63.274 C 12.101 62.734 13.132 62.301 13.303 60.298 C 15.02 60.584 16.156 60.512 17.653 59.612 C 17.198 61.273 17.195 62.874 17.515 64.574 C 15.665 64.434 14.105 64.648 13.075 66.136 C 13.905 66.363 16.165 66.422 17.039 65.49 C 17.366 66.472 18.261 67.878 19.707 68.572 C 18.267 68.832 17.282 69.931 16.373 71.617 C 15.66 70.202 13.433 68.536 11.93 68.482 C 13.933 72.545 13.933 75.464 12.412 78.151 C f 31.125 74.908 m 31.445 75.537 31.648 75.794 V 34.045 73.853 38.851 77.161 39.746 77.929 C 39.636 78.562 37.511 79.698 35.794 78.668 C 36.234 79.957 35.332 81.918 34.134 82.96 C 35.873 82.86 38.019 84.221 38.541 84.963 C 38.763 83.986 39.946 82.716 41.231 81.701 C 41.582 82.675 40.887 84.792 39.971 86.394 C 41.206 86.895 42.318 87.825 42.776 89.084 C 43.233 87.768 44.236 87.093 45.58 86.337 C 44.421 84.91 43.64 82.736 43.92 81.873 C 45.243 82.208 46.814 84.926 46.937 86.016 C 47.812 85.249 49.366 84.563 51.947 84.257 C 50.246 83.179 49.884 81.187 49.3 79.756 C 48.152 80.203 45.983 80.262 45.008 79.698 C 45.721 79.119 47.061 78.569 49.071 78.554 C 49.071 77.009 49.534 75.877 50.788 74.663 C 49.065 74.675 46.965 74.189 45.469 73.798 C 45.221 75.126 44.378 76.723 43.233 77.123 C 43.227 76.262 43.493 74.013 44.378 73.347 C 43.513 72.779 42.26 71.401 41.803 69.684 C 41.181 71.009 40.32 72.314 38.457 72.759 C 39.642 73.812 40.477 75.829 40.143 77.295 C 35.091 73.313 32.414 74.611 31.125 74.908 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Fj\212ll) (Fj\212ll) 1.6 9.3475 48.088 55.8355 [ %AI3_Tile (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 9.3475 m 1.6 55.8355 L 48.088 55.8355 L 48.088 9.3475 L 1.6 9.3475 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 17.0956 9.3475 m 12.8162 9.3475 9.3475 5.8787 9.3475 1.6 C 9.3475 5.8787 5.8787 9.3475 1.6 9.3475 C 1.6 13.6262 5.0687 17.095 9.3475 17.095 c 13.6268 17.095 17.0956 13.6262 17.0956 9.3475 C s 32.5918 9.3475 m 28.3125 9.3475 24.8437 5.8787 24.8437 1.6 C 24.8437 5.8787 21.3743 9.3475 17.0956 9.3475 C 17.0956 13.6262 20.5644 17.095 24.8437 17.095 c 29.1224 17.095 32.5918 13.6262 32.5918 9.3475 C s 48.088 9.3475 m 43.8087 9.3475 40.3399 5.8787 40.3399 1.6 C 40.3399 5.8787 36.8705 9.3475 32.5918 9.3475 C 32.5918 13.6262 36.0606 17.095 40.3399 17.095 c 44.6186 17.095 48.088 13.6262 48.088 9.3475 C s 17.0956 40.3393 m 12.8162 40.3393 9.3475 36.8699 9.3475 32.5912 C 9.3475 36.8699 5.8787 40.3393 1.6 40.3393 C 1.6 44.6181 5.0687 48.0874 9.3475 48.0874 c 13.6268 48.0874 17.0956 44.6181 17.0956 40.3393 C s 17.0956 24.8431 m 12.8162 24.8431 9.3475 21.3743 9.3475 17.095 C 9.3475 21.3743 5.8787 24.8431 1.6 24.8431 C 1.6 29.1218 5.0687 32.5912 9.3475 32.5912 c 13.6268 32.5912 17.0956 29.1218 17.0956 24.8431 C s 32.5918 24.8431 m 28.3125 24.8431 24.8437 21.3743 24.8437 17.095 C 24.8437 21.3743 21.3743 24.8431 17.0956 24.8431 C 17.0956 29.1218 20.5644 32.5912 24.8437 32.5912 c 29.1224 32.5912 32.5918 29.1218 32.5918 24.8431 C s 48.088 24.8431 m 43.8087 24.8431 40.3399 21.3743 40.3399 17.095 C 40.3399 21.3743 36.8705 24.8431 32.5918 24.8431 C 32.5918 29.1218 36.0606 32.5912 40.3399 32.5912 c 44.6186 32.5912 48.088 29.1218 48.088 24.8431 C s 32.5918 40.3393 m 28.3125 40.3393 24.8437 36.8699 24.8437 32.5912 C 24.8437 36.8699 21.3743 40.3393 17.0956 40.3393 C 17.0956 44.6181 20.5644 48.0874 24.8437 48.0874 c 29.1224 48.0874 32.5918 44.6181 32.5918 40.3393 C s 48.088 40.3393 m 43.8087 40.3393 40.3399 36.8699 40.3399 32.5912 C 40.3399 36.8699 36.8705 40.3393 32.5918 40.3393 C 32.5918 44.6181 36.0606 48.0874 40.3399 48.0874 c 44.6186 48.0874 48.088 44.6181 48.088 40.3393 C s 17.0956 55.8355 m 12.8162 55.8355 9.3475 52.3662 9.3475 48.0874 C 9.3475 52.3662 5.8787 55.8355 1.6 55.8355 C 1.6 60.1143 5.0687 63.5836 9.3475 63.5836 c 13.6268 63.5836 17.0956 60.1143 17.0956 55.8355 C s 32.5918 55.8355 m 28.3125 55.8355 24.8437 52.3662 24.8437 48.0874 C 24.8437 52.3662 21.3743 55.8355 17.0956 55.8355 C 17.0956 60.1143 20.5644 63.5836 24.8437 63.5836 c 29.1224 63.5836 32.5918 60.1143 32.5918 55.8355 C s 48.088 55.8355 m 43.8087 55.8355 40.3399 52.3662 40.3399 48.0874 C 40.3399 52.3662 36.8705 55.8355 32.5918 55.8355 C 32.5918 60.1143 36.0606 63.5836 40.3399 63.5836 c 44.6186 63.5836 48.088 60.1143 48.088 55.8355 C s %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Fj\212ll\012 1) (Fj\212ll\012 1) 1.6 9.3475 48.088 55.8355 [ %AI3_Tile (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 9.3475 m 1.6 55.8355 L 48.088 55.8355 L 48.088 9.3475 L 1.6 9.3475 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 17.0956 9.3475 m 12.8162 9.3475 9.3475 5.8787 9.3475 1.6 C 9.3475 5.8787 5.8787 9.3475 1.6 9.3475 C 1.6 13.6262 5.0687 17.095 9.3475 17.095 c 13.6268 17.095 17.0956 13.6262 17.0956 9.3475 C s 32.5918 9.3475 m 28.3125 9.3475 24.8437 5.8787 24.8437 1.6 C 24.8437 5.8787 21.3743 9.3475 17.0956 9.3475 C 17.0956 13.6262 20.5644 17.095 24.8437 17.095 c 29.1224 17.095 32.5918 13.6262 32.5918 9.3475 C s 48.088 9.3475 m 43.8087 9.3475 40.3399 5.8787 40.3399 1.6 C 40.3399 5.8787 36.8705 9.3475 32.5918 9.3475 C 32.5918 13.6262 36.0606 17.095 40.3399 17.095 c 44.6186 17.095 48.088 13.6262 48.088 9.3475 C s 17.0956 40.3393 m 12.8162 40.3393 9.3475 36.8699 9.3475 32.5912 C 9.3475 36.8699 5.8787 40.3393 1.6 40.3393 C 1.6 44.6181 5.0687 48.0874 9.3475 48.0874 c 13.6268 48.0874 17.0956 44.6181 17.0956 40.3393 C s 17.0956 24.8431 m 12.8162 24.8431 9.3475 21.3743 9.3475 17.095 C 9.3475 21.3743 5.8787 24.8431 1.6 24.8431 C 1.6 29.1218 5.0687 32.5912 9.3475 32.5912 c 13.6268 32.5912 17.0956 29.1218 17.0956 24.8431 C s 32.5918 24.8431 m 28.3125 24.8431 24.8437 21.3743 24.8437 17.095 C 24.8437 21.3743 21.3743 24.8431 17.0956 24.8431 C 17.0956 29.1218 20.5644 32.5912 24.8437 32.5912 c 29.1224 32.5912 32.5918 29.1218 32.5918 24.8431 C s 48.088 24.8431 m 43.8087 24.8431 40.3399 21.3743 40.3399 17.095 C 40.3399 21.3743 36.8705 24.8431 32.5918 24.8431 C 32.5918 29.1218 36.0606 32.5912 40.3399 32.5912 c 44.6186 32.5912 48.088 29.1218 48.088 24.8431 C s 32.5918 40.3393 m 28.3125 40.3393 24.8437 36.8699 24.8437 32.5912 C 24.8437 36.8699 21.3743 40.3393 17.0956 40.3393 C 17.0956 44.6181 20.5644 48.0874 24.8437 48.0874 c 29.1224 48.0874 32.5918 44.6181 32.5918 40.3393 C s 48.088 40.3393 m 43.8087 40.3393 40.3399 36.8699 40.3399 32.5912 C 40.3399 36.8699 36.8705 40.3393 32.5918 40.3393 C 32.5918 44.6181 36.0606 48.0874 40.3399 48.0874 c 44.6186 48.0874 48.088 44.6181 48.088 40.3393 C s 17.0956 55.8355 m 12.8162 55.8355 9.3475 52.3662 9.3475 48.0874 C 9.3475 52.3662 5.8787 55.8355 1.6 55.8355 C 1.6 60.1143 5.0687 63.5836 9.3475 63.5836 c 13.6268 63.5836 17.0956 60.1143 17.0956 55.8355 C s 32.5918 55.8355 m 28.3125 55.8355 24.8437 52.3662 24.8437 48.0874 C 24.8437 52.3662 21.3743 55.8355 17.0956 55.8355 C 17.0956 60.1143 20.5644 63.5836 24.8437 63.5836 c 29.1224 63.5836 32.5918 60.1143 32.5918 55.8355 C s 48.088 55.8355 m 43.8087 55.8355 40.3399 52.3662 40.3399 48.0874 C 40.3399 52.3662 36.8705 55.8355 32.5918 55.8355 C 32.5918 60.1143 36.0606 63.5836 40.3399 63.5836 c 44.6186 63.5836 48.088 60.1143 48.088 55.8355 C s %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Fj\212ll\012 2) (Fj\212ll\012 2) 1.6 9.3475 48.088 55.8355 [ %AI3_Tile (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 9.3475 m 1.6 55.8355 L 48.088 55.8355 L 48.088 9.3475 L 1.6 9.3475 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 17.0956 9.3475 m 12.8162 9.3475 9.3475 5.8787 9.3475 1.6 C 9.3475 5.8787 5.8787 9.3475 1.6 9.3475 C 1.6 13.6262 5.0687 17.095 9.3475 17.095 c 13.6268 17.095 17.0956 13.6262 17.0956 9.3475 C s 32.5918 9.3475 m 28.3125 9.3475 24.8437 5.8787 24.8437 1.6 C 24.8437 5.8787 21.3743 9.3475 17.0956 9.3475 C 17.0956 13.6262 20.5644 17.095 24.8437 17.095 c 29.1224 17.095 32.5918 13.6262 32.5918 9.3475 C s 48.088 9.3475 m 43.8087 9.3475 40.3399 5.8787 40.3399 1.6 C 40.3399 5.8787 36.8705 9.3475 32.5918 9.3475 C 32.5918 13.6262 36.0606 17.095 40.3399 17.095 c 44.6186 17.095 48.088 13.6262 48.088 9.3475 C s 17.0956 40.3393 m 12.8162 40.3393 9.3475 36.8699 9.3475 32.5912 C 9.3475 36.8699 5.8787 40.3393 1.6 40.3393 C 1.6 44.6181 5.0687 48.0874 9.3475 48.0874 c 13.6268 48.0874 17.0956 44.6181 17.0956 40.3393 C s 17.0956 24.8431 m 12.8162 24.8431 9.3475 21.3743 9.3475 17.095 C 9.3475 21.3743 5.8787 24.8431 1.6 24.8431 C 1.6 29.1218 5.0687 32.5912 9.3475 32.5912 c 13.6268 32.5912 17.0956 29.1218 17.0956 24.8431 C s 32.5918 24.8431 m 28.3125 24.8431 24.8437 21.3743 24.8437 17.095 C 24.8437 21.3743 21.3743 24.8431 17.0956 24.8431 C 17.0956 29.1218 20.5644 32.5912 24.8437 32.5912 c 29.1224 32.5912 32.5918 29.1218 32.5918 24.8431 C s 48.088 24.8431 m 43.8087 24.8431 40.3399 21.3743 40.3399 17.095 C 40.3399 21.3743 36.8705 24.8431 32.5918 24.8431 C 32.5918 29.1218 36.0606 32.5912 40.3399 32.5912 c 44.6186 32.5912 48.088 29.1218 48.088 24.8431 C s 32.5918 40.3393 m 28.3125 40.3393 24.8437 36.8699 24.8437 32.5912 C 24.8437 36.8699 21.3743 40.3393 17.0956 40.3393 C 17.0956 44.6181 20.5644 48.0874 24.8437 48.0874 c 29.1224 48.0874 32.5918 44.6181 32.5918 40.3393 C s 48.088 40.3393 m 43.8087 40.3393 40.3399 36.8699 40.3399 32.5912 C 40.3399 36.8699 36.8705 40.3393 32.5918 40.3393 C 32.5918 44.6181 36.0606 48.0874 40.3399 48.0874 c 44.6186 48.0874 48.088 44.6181 48.088 40.3393 C s 17.0956 55.8355 m 12.8162 55.8355 9.3475 52.3662 9.3475 48.0874 C 9.3475 52.3662 5.8787 55.8355 1.6 55.8355 C 1.6 60.1143 5.0687 63.5836 9.3475 63.5836 c 13.6268 63.5836 17.0956 60.1143 17.0956 55.8355 C s 32.5918 55.8355 m 28.3125 55.8355 24.8437 52.3662 24.8437 48.0874 C 24.8437 52.3662 21.3743 55.8355 17.0956 55.8355 C 17.0956 60.1143 20.5644 63.5836 24.8437 63.5836 c 29.1224 63.5836 32.5918 60.1143 32.5918 55.8355 C s 48.088 55.8355 m 43.8087 55.8355 40.3399 52.3662 40.3399 48.0874 C 40.3399 52.3662 36.8705 55.8355 32.5918 55.8355 C 32.5918 60.1143 36.0606 63.5836 40.3399 63.5836 c 44.6186 63.5836 48.088 60.1143 48.088 55.8355 C s %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Fj\212ll\012 3) (Fj\212ll\012 3) 1.6 9.3475 48.088 55.8355 [ %AI3_Tile (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 9.3475 m 1.6 55.8355 L 48.088 55.8355 L 48.088 9.3475 L 1.6 9.3475 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 17.0956 9.3475 m 12.8162 9.3475 9.3475 5.8787 9.3475 1.6 C 9.3475 5.8787 5.8787 9.3475 1.6 9.3475 C 1.6 13.6262 5.0687 17.095 9.3475 17.095 c 13.6268 17.095 17.0956 13.6262 17.0956 9.3475 C s 32.5918 9.3475 m 28.3125 9.3475 24.8437 5.8787 24.8437 1.6 C 24.8437 5.8787 21.3743 9.3475 17.0956 9.3475 C 17.0956 13.6262 20.5644 17.095 24.8437 17.095 c 29.1224 17.095 32.5918 13.6262 32.5918 9.3475 C s 48.088 9.3475 m 43.8087 9.3475 40.3399 5.8787 40.3399 1.6 C 40.3399 5.8787 36.8705 9.3475 32.5918 9.3475 C 32.5918 13.6262 36.0606 17.095 40.3399 17.095 c 44.6186 17.095 48.088 13.6262 48.088 9.3475 C s 17.0956 40.3393 m 12.8162 40.3393 9.3475 36.8699 9.3475 32.5912 C 9.3475 36.8699 5.8787 40.3393 1.6 40.3393 C 1.6 44.6181 5.0687 48.0874 9.3475 48.0874 c 13.6268 48.0874 17.0956 44.6181 17.0956 40.3393 C s 17.0956 24.8431 m 12.8162 24.8431 9.3475 21.3743 9.3475 17.095 C 9.3475 21.3743 5.8787 24.8431 1.6 24.8431 C 1.6 29.1218 5.0687 32.5912 9.3475 32.5912 c 13.6268 32.5912 17.0956 29.1218 17.0956 24.8431 C s 32.5918 24.8431 m 28.3125 24.8431 24.8437 21.3743 24.8437 17.095 C 24.8437 21.3743 21.3743 24.8431 17.0956 24.8431 C 17.0956 29.1218 20.5644 32.5912 24.8437 32.5912 c 29.1224 32.5912 32.5918 29.1218 32.5918 24.8431 C s 48.088 24.8431 m 43.8087 24.8431 40.3399 21.3743 40.3399 17.095 C 40.3399 21.3743 36.8705 24.8431 32.5918 24.8431 C 32.5918 29.1218 36.0606 32.5912 40.3399 32.5912 c 44.6186 32.5912 48.088 29.1218 48.088 24.8431 C s 32.5918 40.3393 m 28.3125 40.3393 24.8437 36.8699 24.8437 32.5912 C 24.8437 36.8699 21.3743 40.3393 17.0956 40.3393 C 17.0956 44.6181 20.5644 48.0874 24.8437 48.0874 c 29.1224 48.0874 32.5918 44.6181 32.5918 40.3393 C s 48.088 40.3393 m 43.8087 40.3393 40.3399 36.8699 40.3399 32.5912 C 40.3399 36.8699 36.8705 40.3393 32.5918 40.3393 C 32.5918 44.6181 36.0606 48.0874 40.3399 48.0874 c 44.6186 48.0874 48.088 44.6181 48.088 40.3393 C s 17.0956 55.8355 m 12.8162 55.8355 9.3475 52.3662 9.3475 48.0874 C 9.3475 52.3662 5.8787 55.8355 1.6 55.8355 C 1.6 60.1143 5.0687 63.5836 9.3475 63.5836 c 13.6268 63.5836 17.0956 60.1143 17.0956 55.8355 C s 32.5918 55.8355 m 28.3125 55.8355 24.8437 52.3662 24.8437 48.0874 C 24.8437 52.3662 21.3743 55.8355 17.0956 55.8355 C 17.0956 60.1143 20.5644 63.5836 24.8437 63.5836 c 29.1224 63.5836 32.5918 60.1143 32.5918 55.8355 C s 48.088 55.8355 m 43.8087 55.8355 40.3399 52.3662 40.3399 48.0874 C 40.3399 52.3662 36.8705 55.8355 32.5918 55.8355 C 32.5918 60.1143 36.0606 63.5836 40.3399 63.5836 c 44.6186 63.5836 48.088 60.1143 48.088 55.8355 C s %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Fj\212ll\012 4) (Fj\212ll\012 4) 1.6 9.3475 48.088 55.8355 [ %AI3_Tile (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 9.3475 m 1.6 55.8355 L 48.088 55.8355 L 48.088 9.3475 L 1.6 9.3475 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 17.0956 9.3475 m 12.8162 9.3475 9.3475 5.8787 9.3475 1.6 C 9.3475 5.8787 5.8787 9.3475 1.6 9.3475 C 1.6 13.6262 5.0687 17.095 9.3475 17.095 c 13.6268 17.095 17.0956 13.6262 17.0956 9.3475 C s 32.5918 9.3475 m 28.3125 9.3475 24.8437 5.8787 24.8437 1.6 C 24.8437 5.8787 21.3743 9.3475 17.0956 9.3475 C 17.0956 13.6262 20.5644 17.095 24.8437 17.095 c 29.1224 17.095 32.5918 13.6262 32.5918 9.3475 C s 48.088 9.3475 m 43.8087 9.3475 40.3399 5.8787 40.3399 1.6 C 40.3399 5.8787 36.8705 9.3475 32.5918 9.3475 C 32.5918 13.6262 36.0606 17.095 40.3399 17.095 c 44.6186 17.095 48.088 13.6262 48.088 9.3475 C s 17.0956 40.3393 m 12.8162 40.3393 9.3475 36.8699 9.3475 32.5912 C 9.3475 36.8699 5.8787 40.3393 1.6 40.3393 C 1.6 44.6181 5.0687 48.0874 9.3475 48.0874 c 13.6268 48.0874 17.0956 44.6181 17.0956 40.3393 C s 17.0956 24.8431 m 12.8162 24.8431 9.3475 21.3743 9.3475 17.095 C 9.3475 21.3743 5.8787 24.8431 1.6 24.8431 C 1.6 29.1218 5.0687 32.5912 9.3475 32.5912 c 13.6268 32.5912 17.0956 29.1218 17.0956 24.8431 C s 32.5918 24.8431 m 28.3125 24.8431 24.8437 21.3743 24.8437 17.095 C 24.8437 21.3743 21.3743 24.8431 17.0956 24.8431 C 17.0956 29.1218 20.5644 32.5912 24.8437 32.5912 c 29.1224 32.5912 32.5918 29.1218 32.5918 24.8431 C s 48.088 24.8431 m 43.8087 24.8431 40.3399 21.3743 40.3399 17.095 C 40.3399 21.3743 36.8705 24.8431 32.5918 24.8431 C 32.5918 29.1218 36.0606 32.5912 40.3399 32.5912 c 44.6186 32.5912 48.088 29.1218 48.088 24.8431 C s 32.5918 40.3393 m 28.3125 40.3393 24.8437 36.8699 24.8437 32.5912 C 24.8437 36.8699 21.3743 40.3393 17.0956 40.3393 C 17.0956 44.6181 20.5644 48.0874 24.8437 48.0874 c 29.1224 48.0874 32.5918 44.6181 32.5918 40.3393 C s 48.088 40.3393 m 43.8087 40.3393 40.3399 36.8699 40.3399 32.5912 C 40.3399 36.8699 36.8705 40.3393 32.5918 40.3393 C 32.5918 44.6181 36.0606 48.0874 40.3399 48.0874 c 44.6186 48.0874 48.088 44.6181 48.088 40.3393 C s 17.0956 55.8355 m 12.8162 55.8355 9.3475 52.3662 9.3475 48.0874 C 9.3475 52.3662 5.8787 55.8355 1.6 55.8355 C 1.6 60.1143 5.0687 63.5836 9.3475 63.5836 c 13.6268 63.5836 17.0956 60.1143 17.0956 55.8355 C s 32.5918 55.8355 m 28.3125 55.8355 24.8437 52.3662 24.8437 48.0874 C 24.8437 52.3662 21.3743 55.8355 17.0956 55.8355 C 17.0956 60.1143 20.5644 63.5836 24.8437 63.5836 c 29.1224 63.5836 32.5918 60.1143 32.5918 55.8355 C s 48.088 55.8355 m 43.8087 55.8355 40.3399 52.3662 40.3399 48.0874 C 40.3399 52.3662 36.8705 55.8355 32.5918 55.8355 C 32.5918 60.1143 36.0606 63.5836 40.3399 63.5836 c 44.6186 63.5836 48.088 60.1143 48.088 55.8355 C s %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Helstj\212rna.sida) (Helstj\212rna.sida) 1 1 33.0117 33.0117 [ %AI3_Tile (0 O 0 R 0.05 0.2 0.95 0 k 0.05 0.2 0.95 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 7.9689 26.0458 m 14.5331 22.9874 l 17.0095 29.7904 L 19.4859 22.9874 l 26.0473 26.0458 l 22.9889 19.4815 l 29.792 17.0052 l 22.9889 14.5288 l 26.0473 7.9674 l 19.4859 11.0257 l 17.0095 4.2226 l 14.5305 11.0257 l 7.9689 7.9674 l 11.0273 14.5288 l 4.2242 17.0052 l 11.0273 19.4843 L 7.9689 26.0458 l f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Helstj\212rna.sida\012 1) (Helstj\212rna.sida\012 1) 1 1 33.0117 33.0117 [ %AI3_Tile (0 O 0 R 0.05 0.2 0.95 0 k 0.05 0.2 0.95 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 7.9689 26.0458 m 14.5331 22.9874 l 17.0095 29.7904 L 19.4859 22.9874 l 26.0473 26.0458 l 22.9889 19.4815 l 29.792 17.0052 l 22.9889 14.5288 l 26.0473 7.9674 l 19.4859 11.0257 l 17.0095 4.2226 l 14.5305 11.0257 l 7.9689 7.9674 l 11.0273 14.5288 l 4.2242 17.0052 l 11.0273 19.4843 L 7.9689 26.0458 l f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Helstj\212rna.sida\012 2) (Helstj\212rna.sida\012 2) 1 1 33.0117 33.0117 [ %AI3_Tile (0 O 0 R 0.05 0.2 0.95 0 k 0.05 0.2 0.95 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 7.9689 26.0458 m 14.5331 22.9874 l 17.0095 29.7904 L 19.4859 22.9874 l 26.0473 26.0458 l 22.9889 19.4815 l 29.792 17.0052 l 22.9889 14.5288 l 26.0473 7.9674 l 19.4859 11.0257 l 17.0095 4.2226 l 14.5305 11.0257 l 7.9689 7.9674 l 11.0273 14.5288 l 4.2242 17.0052 l 11.0273 19.4843 L 7.9689 26.0458 l f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Helstj\212rna.sida\012 3) (Helstj\212rna.sida\012 3) 1 1 33.0117 33.0117 [ %AI3_Tile (0 O 0 R 0.05 0.2 0.95 0 k 0.05 0.2 0.95 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 7.9689 26.0458 m 14.5331 22.9874 l 17.0095 29.7904 L 19.4859 22.9874 l 26.0473 26.0458 l 22.9889 19.4815 l 29.792 17.0052 l 22.9889 14.5288 l 26.0473 7.9674 l 19.4859 11.0257 l 17.0095 4.2226 l 14.5305 11.0257 l 7.9689 7.9674 l 11.0273 14.5288 l 4.2242 17.0052 l 11.0273 19.4843 L 7.9689 26.0458 l f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Helstj\212rna.sida\012 4) (Helstj\212rna.sida\012 4) 1 1 33.0117 33.0117 [ %AI3_Tile (0 O 0 R 0.05 0.2 0.95 0 k 0.05 0.2 0.95 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 7.9689 26.0458 m 14.5331 22.9874 l 17.0095 29.7904 L 19.4859 22.9874 l 26.0473 26.0458 l 22.9889 19.4815 l 29.792 17.0052 l 22.9889 14.5288 l 26.0473 7.9674 l 19.4859 11.0257 l 17.0095 4.2226 l 14.5305 11.0257 l 7.9689 7.9674 l 11.0273 14.5288 l 4.2242 17.0052 l 11.0273 19.4843 L 7.9689 26.0458 l f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Konfetti) (Konfetti) 4.85 3.617 76.85 75.617 [ %AI3_Tile (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.85 3.617 m 4.85 75.617 L 76.85 75.617 L 76.85 3.617 L 4.85 3.617 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 10.6 64.867 m 7.85 62.867 l S 9.1 8.617 m 6.85 6.867 l S 78.1 68.617 m 74.85 67.867 l S 76.85 56.867 m 74.35 55.117 l S 79.6 51.617 m 76.6 51.617 l S 76.35 44.117 m 73.6 45.867 l S 78.6 35.867 m 76.6 34.367 l S 76.1 23.867 m 73.35 26.117 l S 78.1 12.867 m 73.85 13.617 l S 68.35 14.617 m 66.1 12.867 l S 76.6 30.617 m 73.6 30.617 l S 62.85 58.117 m 60.956 60.941 l S 32.85 59.617 m 31.196 62.181 l S 47.891 64.061 m 49.744 66.742 l S 72.814 2.769 m 73.928 5.729 l S 67.976 2.633 m 67.35 5.909 l S 61.85 27.617 m 59.956 30.441 l S 53.504 56.053 m 51.85 58.617 l S 52.762 1.779 m 52.876 4.776 l S 45.391 5.311 m 47.244 7.992 l S 37.062 3.375 m 35.639 5.43 l S 55.165 34.828 m 57.518 37.491 l S 20.795 3.242 m 22.12 5.193 l S 14.097 4.747 m 15.008 8.965 l S 9.736 1.91 m 8.073 4.225 l S 31.891 5.573 m 32.005 8.571 l S 12.1 70.367 m 15.6 68.867 l S 9.35 54.867 m 9.6 58.117 l S 12.85 31.867 m 14.35 28.117 l S 10.1 37.367 m 12.35 41.117 l S 34.1 71.117 m 31.85 68.617 l S 38.35 71.117 m 41.6 68.367 l S 55.1 71.117 m 58.35 69.117 l S 57.35 65.117 m 55.35 61.867 l S 64.35 66.367 m 69.35 68.617 l S 71.85 62.867 m 69.35 61.117 l S 23.6 70.867 m 23.6 67.867 l S 20.6 65.867 m 17.35 65.367 l S 24.85 61.367 m 25.35 58.117 l S 25.85 65.867 m 29.35 66.617 l S 14.1 54.117 m 16.85 56.117 l S 12.35 11.617 m 12.6 15.617 l S 12.1 19.867 m 14.35 22.367 l S 26.1 9.867 m 23.6 13.367 l S 34.6 47.117 m 32.1 45.367 l S 62.6 41.867 m 59.85 43.367 l S 31.6 35.617 m 27.85 36.367 l S 36.35 26.117 m 34.35 24.617 l S 33.85 14.117 m 31.1 16.367 l S 37.1 9.867 m 35.1 11.117 l S 34.35 20.867 m 31.35 20.867 l S 44.6 56.617 m 42.1 54.867 l S 47.35 51.367 m 44.35 51.367 l S 44.1 43.867 m 41.35 45.617 l S 43.35 33.117 m 42.6 30.617 l S 43.85 23.617 m 41.1 25.867 l S 44.35 15.617 m 42.35 16.867 l S 67.823 31.1 m 64.823 31.1 l S 27.1 32.617 m 29.6 30.867 l S 31.85 55.117 m 34.85 55.117 l S 19.6 40.867 m 22.1 39.117 l S 16.85 35.617 m 19.85 35.617 l S 20.1 28.117 m 22.85 29.867 l S 52.1 42.617 m 54.484 44.178 l S 52.437 50.146 m 54.821 48.325 l S 59.572 54.133 m 59.35 51.117 l S 50.185 10.055 m 53.234 9.928 l S 51.187 15.896 m 53.571 14.075 l S 58.322 19.883 m 59.445 16.823 l S 53.1 32.117 m 50.6 30.367 l S 52.85 24.617 m 49.6 25.617 l S 61.85 9.117 m 59.1 10.867 l S 69.35 34.617 m 66.6 36.367 l S 67.1 23.617 m 65.1 22.117 l S 24.435 46.055 m 27.484 45.928 l S 25.437 51.896 m 27.821 50.075 l S 62.6 47.117 m 65.321 46.575 l S 19.85 19.867 m 20.35 16.617 l S 21.85 21.867 m 25.35 22.617 l S 37.6 62.867 m 41.6 62.117 l S 38.323 42.1 m 38.823 38.6 l S 69.35 52.617 m 66.85 53.867 l S 14.85 62.117 m 18.1 59.367 l S 9.6 46.117 m 7.1 44.367 l S 20.6 51.617 m 18.6 50.117 l S 46.141 70.811 m 47.994 73.492 l S 69.391 40.561 m 71.244 43.242 l S 38.641 49.311 m 39.35 52.117 l S 25.141 16.811 m 25.85 19.617 l S 36.6 32.867 m 34.6 31.367 l S 6.1 68.617 m 2.85 67.867 l S 4.85 56.867 m 2.35 55.117 l S 7.6 51.617 m 4.6 51.617 l S 6.6 35.867 m 4.6 34.367 l S 6.1 12.867 m 1.85 13.617 l S 4.6 30.617 m 1.6 30.617 l S 72.814 74.769 m 73.928 77.729 l S 67.976 74.633 m 67.35 77.909 l S 52.762 73.779 m 52.876 76.776 l S 37.062 75.375 m 35.639 77.43 l S 20.795 75.242 m 22.12 77.193 l S 9.736 73.91 m 8.073 76.225 l S 10.1 23.617 m 6.35 24.367 l S 73.217 18.276 m 71.323 21.1 l S 28.823 39.6 m 29.505 42.389 l S 49.6 38.617 m 47.6 37.117 l S 60.323 73.6 m 62.323 76.6 l S 60.323 1.6 m 62.323 4.6 l S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Konfetti\012 1) (Konfetti\012 1) 4.85 3.617 76.85 75.617 [ %AI3_Tile (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.85 3.617 m 4.85 75.617 L 76.85 75.617 L 76.85 3.617 L 4.85 3.617 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 10.6 64.867 m 7.85 62.867 l S 9.1 8.617 m 6.85 6.867 l S 78.1 68.617 m 74.85 67.867 l S 76.85 56.867 m 74.35 55.117 l S 79.6 51.617 m 76.6 51.617 l S 76.35 44.117 m 73.6 45.867 l S 78.6 35.867 m 76.6 34.367 l S 76.1 23.867 m 73.35 26.117 l S 78.1 12.867 m 73.85 13.617 l S 68.35 14.617 m 66.1 12.867 l S 76.6 30.617 m 73.6 30.617 l S 62.85 58.117 m 60.956 60.941 l S 32.85 59.617 m 31.196 62.181 l S 47.891 64.061 m 49.744 66.742 l S 72.814 2.769 m 73.928 5.729 l S 67.976 2.633 m 67.35 5.909 l S 61.85 27.617 m 59.956 30.441 l S 53.504 56.053 m 51.85 58.617 l S 52.762 1.779 m 52.876 4.776 l S 45.391 5.311 m 47.244 7.992 l S 37.062 3.375 m 35.639 5.43 l S 55.165 34.828 m 57.518 37.491 l S 20.795 3.242 m 22.12 5.193 l S 14.097 4.747 m 15.008 8.965 l S 9.736 1.91 m 8.073 4.225 l S 31.891 5.573 m 32.005 8.571 l S 12.1 70.367 m 15.6 68.867 l S 9.35 54.867 m 9.6 58.117 l S 12.85 31.867 m 14.35 28.117 l S 10.1 37.367 m 12.35 41.117 l S 34.1 71.117 m 31.85 68.617 l S 38.35 71.117 m 41.6 68.367 l S 55.1 71.117 m 58.35 69.117 l S 57.35 65.117 m 55.35 61.867 l S 64.35 66.367 m 69.35 68.617 l S 71.85 62.867 m 69.35 61.117 l S 23.6 70.867 m 23.6 67.867 l S 20.6 65.867 m 17.35 65.367 l S 24.85 61.367 m 25.35 58.117 l S 25.85 65.867 m 29.35 66.617 l S 14.1 54.117 m 16.85 56.117 l S 12.35 11.617 m 12.6 15.617 l S 12.1 19.867 m 14.35 22.367 l S 26.1 9.867 m 23.6 13.367 l S 34.6 47.117 m 32.1 45.367 l S 62.6 41.867 m 59.85 43.367 l S 31.6 35.617 m 27.85 36.367 l S 36.35 26.117 m 34.35 24.617 l S 33.85 14.117 m 31.1 16.367 l S 37.1 9.867 m 35.1 11.117 l S 34.35 20.867 m 31.35 20.867 l S 44.6 56.617 m 42.1 54.867 l S 47.35 51.367 m 44.35 51.367 l S 44.1 43.867 m 41.35 45.617 l S 43.35 33.117 m 42.6 30.617 l S 43.85 23.617 m 41.1 25.867 l S 44.35 15.617 m 42.35 16.867 l S 67.823 31.1 m 64.823 31.1 l S 27.1 32.617 m 29.6 30.867 l S 31.85 55.117 m 34.85 55.117 l S 19.6 40.867 m 22.1 39.117 l S 16.85 35.617 m 19.85 35.617 l S 20.1 28.117 m 22.85 29.867 l S 52.1 42.617 m 54.484 44.178 l S 52.437 50.146 m 54.821 48.325 l S 59.572 54.133 m 59.35 51.117 l S 50.185 10.055 m 53.234 9.928 l S 51.187 15.896 m 53.571 14.075 l S 58.322 19.883 m 59.445 16.823 l S 53.1 32.117 m 50.6 30.367 l S 52.85 24.617 m 49.6 25.617 l S 61.85 9.117 m 59.1 10.867 l S 69.35 34.617 m 66.6 36.367 l S 67.1 23.617 m 65.1 22.117 l S 24.435 46.055 m 27.484 45.928 l S 25.437 51.896 m 27.821 50.075 l S 62.6 47.117 m 65.321 46.575 l S 19.85 19.867 m 20.35 16.617 l S 21.85 21.867 m 25.35 22.617 l S 37.6 62.867 m 41.6 62.117 l S 38.323 42.1 m 38.823 38.6 l S 69.35 52.617 m 66.85 53.867 l S 14.85 62.117 m 18.1 59.367 l S 9.6 46.117 m 7.1 44.367 l S 20.6 51.617 m 18.6 50.117 l S 46.141 70.811 m 47.994 73.492 l S 69.391 40.561 m 71.244 43.242 l S 38.641 49.311 m 39.35 52.117 l S 25.141 16.811 m 25.85 19.617 l S 36.6 32.867 m 34.6 31.367 l S 6.1 68.617 m 2.85 67.867 l S 4.85 56.867 m 2.35 55.117 l S 7.6 51.617 m 4.6 51.617 l S 6.6 35.867 m 4.6 34.367 l S 6.1 12.867 m 1.85 13.617 l S 4.6 30.617 m 1.6 30.617 l S 72.814 74.769 m 73.928 77.729 l S 67.976 74.633 m 67.35 77.909 l S 52.762 73.779 m 52.876 76.776 l S 37.062 75.375 m 35.639 77.43 l S 20.795 75.242 m 22.12 77.193 l S 9.736 73.91 m 8.073 76.225 l S 10.1 23.617 m 6.35 24.367 l S 73.217 18.276 m 71.323 21.1 l S 28.823 39.6 m 29.505 42.389 l S 49.6 38.617 m 47.6 37.117 l S 60.323 73.6 m 62.323 76.6 l S 60.323 1.6 m 62.323 4.6 l S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Konfetti\012 2) (Konfetti\012 2) 4.85 3.617 76.85 75.617 [ %AI3_Tile (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.85 3.617 m 4.85 75.617 L 76.85 75.617 L 76.85 3.617 L 4.85 3.617 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 10.6 64.867 m 7.85 62.867 l S 9.1 8.617 m 6.85 6.867 l S 78.1 68.617 m 74.85 67.867 l S 76.85 56.867 m 74.35 55.117 l S 79.6 51.617 m 76.6 51.617 l S 76.35 44.117 m 73.6 45.867 l S 78.6 35.867 m 76.6 34.367 l S 76.1 23.867 m 73.35 26.117 l S 78.1 12.867 m 73.85 13.617 l S 68.35 14.617 m 66.1 12.867 l S 76.6 30.617 m 73.6 30.617 l S 62.85 58.117 m 60.956 60.941 l S 32.85 59.617 m 31.196 62.181 l S 47.891 64.061 m 49.744 66.742 l S 72.814 2.769 m 73.928 5.729 l S 67.976 2.633 m 67.35 5.909 l S 61.85 27.617 m 59.956 30.441 l S 53.504 56.053 m 51.85 58.617 l S 52.762 1.779 m 52.876 4.776 l S 45.391 5.311 m 47.244 7.992 l S 37.062 3.375 m 35.639 5.43 l S 55.165 34.828 m 57.518 37.491 l S 20.795 3.242 m 22.12 5.193 l S 14.097 4.747 m 15.008 8.965 l S 9.736 1.91 m 8.073 4.225 l S 31.891 5.573 m 32.005 8.571 l S 12.1 70.367 m 15.6 68.867 l S 9.35 54.867 m 9.6 58.117 l S 12.85 31.867 m 14.35 28.117 l S 10.1 37.367 m 12.35 41.117 l S 34.1 71.117 m 31.85 68.617 l S 38.35 71.117 m 41.6 68.367 l S 55.1 71.117 m 58.35 69.117 l S 57.35 65.117 m 55.35 61.867 l S 64.35 66.367 m 69.35 68.617 l S 71.85 62.867 m 69.35 61.117 l S 23.6 70.867 m 23.6 67.867 l S 20.6 65.867 m 17.35 65.367 l S 24.85 61.367 m 25.35 58.117 l S 25.85 65.867 m 29.35 66.617 l S 14.1 54.117 m 16.85 56.117 l S 12.35 11.617 m 12.6 15.617 l S 12.1 19.867 m 14.35 22.367 l S 26.1 9.867 m 23.6 13.367 l S 34.6 47.117 m 32.1 45.367 l S 62.6 41.867 m 59.85 43.367 l S 31.6 35.617 m 27.85 36.367 l S 36.35 26.117 m 34.35 24.617 l S 33.85 14.117 m 31.1 16.367 l S 37.1 9.867 m 35.1 11.117 l S 34.35 20.867 m 31.35 20.867 l S 44.6 56.617 m 42.1 54.867 l S 47.35 51.367 m 44.35 51.367 l S 44.1 43.867 m 41.35 45.617 l S 43.35 33.117 m 42.6 30.617 l S 43.85 23.617 m 41.1 25.867 l S 44.35 15.617 m 42.35 16.867 l S 67.823 31.1 m 64.823 31.1 l S 27.1 32.617 m 29.6 30.867 l S 31.85 55.117 m 34.85 55.117 l S 19.6 40.867 m 22.1 39.117 l S 16.85 35.617 m 19.85 35.617 l S 20.1 28.117 m 22.85 29.867 l S 52.1 42.617 m 54.484 44.178 l S 52.437 50.146 m 54.821 48.325 l S 59.572 54.133 m 59.35 51.117 l S 50.185 10.055 m 53.234 9.928 l S 51.187 15.896 m 53.571 14.075 l S 58.322 19.883 m 59.445 16.823 l S 53.1 32.117 m 50.6 30.367 l S 52.85 24.617 m 49.6 25.617 l S 61.85 9.117 m 59.1 10.867 l S 69.35 34.617 m 66.6 36.367 l S 67.1 23.617 m 65.1 22.117 l S 24.435 46.055 m 27.484 45.928 l S 25.437 51.896 m 27.821 50.075 l S 62.6 47.117 m 65.321 46.575 l S 19.85 19.867 m 20.35 16.617 l S 21.85 21.867 m 25.35 22.617 l S 37.6 62.867 m 41.6 62.117 l S 38.323 42.1 m 38.823 38.6 l S 69.35 52.617 m 66.85 53.867 l S 14.85 62.117 m 18.1 59.367 l S 9.6 46.117 m 7.1 44.367 l S 20.6 51.617 m 18.6 50.117 l S 46.141 70.811 m 47.994 73.492 l S 69.391 40.561 m 71.244 43.242 l S 38.641 49.311 m 39.35 52.117 l S 25.141 16.811 m 25.85 19.617 l S 36.6 32.867 m 34.6 31.367 l S 6.1 68.617 m 2.85 67.867 l S 4.85 56.867 m 2.35 55.117 l S 7.6 51.617 m 4.6 51.617 l S 6.6 35.867 m 4.6 34.367 l S 6.1 12.867 m 1.85 13.617 l S 4.6 30.617 m 1.6 30.617 l S 72.814 74.769 m 73.928 77.729 l S 67.976 74.633 m 67.35 77.909 l S 52.762 73.779 m 52.876 76.776 l S 37.062 75.375 m 35.639 77.43 l S 20.795 75.242 m 22.12 77.193 l S 9.736 73.91 m 8.073 76.225 l S 10.1 23.617 m 6.35 24.367 l S 73.217 18.276 m 71.323 21.1 l S 28.823 39.6 m 29.505 42.389 l S 49.6 38.617 m 47.6 37.117 l S 60.323 73.6 m 62.323 76.6 l S 60.323 1.6 m 62.323 4.6 l S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Konfetti\012 3) (Konfetti\012 3) 4.85 3.617 76.85 75.617 [ %AI3_Tile (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.85 3.617 m 4.85 75.617 L 76.85 75.617 L 76.85 3.617 L 4.85 3.617 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 10.6 64.867 m 7.85 62.867 l S 9.1 8.617 m 6.85 6.867 l S 78.1 68.617 m 74.85 67.867 l S 76.85 56.867 m 74.35 55.117 l S 79.6 51.617 m 76.6 51.617 l S 76.35 44.117 m 73.6 45.867 l S 78.6 35.867 m 76.6 34.367 l S 76.1 23.867 m 73.35 26.117 l S 78.1 12.867 m 73.85 13.617 l S 68.35 14.617 m 66.1 12.867 l S 76.6 30.617 m 73.6 30.617 l S 62.85 58.117 m 60.956 60.941 l S 32.85 59.617 m 31.196 62.181 l S 47.891 64.061 m 49.744 66.742 l S 72.814 2.769 m 73.928 5.729 l S 67.976 2.633 m 67.35 5.909 l S 61.85 27.617 m 59.956 30.441 l S 53.504 56.053 m 51.85 58.617 l S 52.762 1.779 m 52.876 4.776 l S 45.391 5.311 m 47.244 7.992 l S 37.062 3.375 m 35.639 5.43 l S 55.165 34.828 m 57.518 37.491 l S 20.795 3.242 m 22.12 5.193 l S 14.097 4.747 m 15.008 8.965 l S 9.736 1.91 m 8.073 4.225 l S 31.891 5.573 m 32.005 8.571 l S 12.1 70.367 m 15.6 68.867 l S 9.35 54.867 m 9.6 58.117 l S 12.85 31.867 m 14.35 28.117 l S 10.1 37.367 m 12.35 41.117 l S 34.1 71.117 m 31.85 68.617 l S 38.35 71.117 m 41.6 68.367 l S 55.1 71.117 m 58.35 69.117 l S 57.35 65.117 m 55.35 61.867 l S 64.35 66.367 m 69.35 68.617 l S 71.85 62.867 m 69.35 61.117 l S 23.6 70.867 m 23.6 67.867 l S 20.6 65.867 m 17.35 65.367 l S 24.85 61.367 m 25.35 58.117 l S 25.85 65.867 m 29.35 66.617 l S 14.1 54.117 m 16.85 56.117 l S 12.35 11.617 m 12.6 15.617 l S 12.1 19.867 m 14.35 22.367 l S 26.1 9.867 m 23.6 13.367 l S 34.6 47.117 m 32.1 45.367 l S 62.6 41.867 m 59.85 43.367 l S 31.6 35.617 m 27.85 36.367 l S 36.35 26.117 m 34.35 24.617 l S 33.85 14.117 m 31.1 16.367 l S 37.1 9.867 m 35.1 11.117 l S 34.35 20.867 m 31.35 20.867 l S 44.6 56.617 m 42.1 54.867 l S 47.35 51.367 m 44.35 51.367 l S 44.1 43.867 m 41.35 45.617 l S 43.35 33.117 m 42.6 30.617 l S 43.85 23.617 m 41.1 25.867 l S 44.35 15.617 m 42.35 16.867 l S 67.823 31.1 m 64.823 31.1 l S 27.1 32.617 m 29.6 30.867 l S 31.85 55.117 m 34.85 55.117 l S 19.6 40.867 m 22.1 39.117 l S 16.85 35.617 m 19.85 35.617 l S 20.1 28.117 m 22.85 29.867 l S 52.1 42.617 m 54.484 44.178 l S 52.437 50.146 m 54.821 48.325 l S 59.572 54.133 m 59.35 51.117 l S 50.185 10.055 m 53.234 9.928 l S 51.187 15.896 m 53.571 14.075 l S 58.322 19.883 m 59.445 16.823 l S 53.1 32.117 m 50.6 30.367 l S 52.85 24.617 m 49.6 25.617 l S 61.85 9.117 m 59.1 10.867 l S 69.35 34.617 m 66.6 36.367 l S 67.1 23.617 m 65.1 22.117 l S 24.435 46.055 m 27.484 45.928 l S 25.437 51.896 m 27.821 50.075 l S 62.6 47.117 m 65.321 46.575 l S 19.85 19.867 m 20.35 16.617 l S 21.85 21.867 m 25.35 22.617 l S 37.6 62.867 m 41.6 62.117 l S 38.323 42.1 m 38.823 38.6 l S 69.35 52.617 m 66.85 53.867 l S 14.85 62.117 m 18.1 59.367 l S 9.6 46.117 m 7.1 44.367 l S 20.6 51.617 m 18.6 50.117 l S 46.141 70.811 m 47.994 73.492 l S 69.391 40.561 m 71.244 43.242 l S 38.641 49.311 m 39.35 52.117 l S 25.141 16.811 m 25.85 19.617 l S 36.6 32.867 m 34.6 31.367 l S 6.1 68.617 m 2.85 67.867 l S 4.85 56.867 m 2.35 55.117 l S 7.6 51.617 m 4.6 51.617 l S 6.6 35.867 m 4.6 34.367 l S 6.1 12.867 m 1.85 13.617 l S 4.6 30.617 m 1.6 30.617 l S 72.814 74.769 m 73.928 77.729 l S 67.976 74.633 m 67.35 77.909 l S 52.762 73.779 m 52.876 76.776 l S 37.062 75.375 m 35.639 77.43 l S 20.795 75.242 m 22.12 77.193 l S 9.736 73.91 m 8.073 76.225 l S 10.1 23.617 m 6.35 24.367 l S 73.217 18.276 m 71.323 21.1 l S 28.823 39.6 m 29.505 42.389 l S 49.6 38.617 m 47.6 37.117 l S 60.323 73.6 m 62.323 76.6 l S 60.323 1.6 m 62.323 4.6 l S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Konfetti\012 4) (Konfetti\012 4) 4.85 3.617 76.85 75.617 [ %AI3_Tile (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.85 3.617 m 4.85 75.617 L 76.85 75.617 L 76.85 3.617 L 4.85 3.617 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 g 0 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 10.6 64.867 m 7.85 62.867 l S 9.1 8.617 m 6.85 6.867 l S 78.1 68.617 m 74.85 67.867 l S 76.85 56.867 m 74.35 55.117 l S 79.6 51.617 m 76.6 51.617 l S 76.35 44.117 m 73.6 45.867 l S 78.6 35.867 m 76.6 34.367 l S 76.1 23.867 m 73.35 26.117 l S 78.1 12.867 m 73.85 13.617 l S 68.35 14.617 m 66.1 12.867 l S 76.6 30.617 m 73.6 30.617 l S 62.85 58.117 m 60.956 60.941 l S 32.85 59.617 m 31.196 62.181 l S 47.891 64.061 m 49.744 66.742 l S 72.814 2.769 m 73.928 5.729 l S 67.976 2.633 m 67.35 5.909 l S 61.85 27.617 m 59.956 30.441 l S 53.504 56.053 m 51.85 58.617 l S 52.762 1.779 m 52.876 4.776 l S 45.391 5.311 m 47.244 7.992 l S 37.062 3.375 m 35.639 5.43 l S 55.165 34.828 m 57.518 37.491 l S 20.795 3.242 m 22.12 5.193 l S 14.097 4.747 m 15.008 8.965 l S 9.736 1.91 m 8.073 4.225 l S 31.891 5.573 m 32.005 8.571 l S 12.1 70.367 m 15.6 68.867 l S 9.35 54.867 m 9.6 58.117 l S 12.85 31.867 m 14.35 28.117 l S 10.1 37.367 m 12.35 41.117 l S 34.1 71.117 m 31.85 68.617 l S 38.35 71.117 m 41.6 68.367 l S 55.1 71.117 m 58.35 69.117 l S 57.35 65.117 m 55.35 61.867 l S 64.35 66.367 m 69.35 68.617 l S 71.85 62.867 m 69.35 61.117 l S 23.6 70.867 m 23.6 67.867 l S 20.6 65.867 m 17.35 65.367 l S 24.85 61.367 m 25.35 58.117 l S 25.85 65.867 m 29.35 66.617 l S 14.1 54.117 m 16.85 56.117 l S 12.35 11.617 m 12.6 15.617 l S 12.1 19.867 m 14.35 22.367 l S 26.1 9.867 m 23.6 13.367 l S 34.6 47.117 m 32.1 45.367 l S 62.6 41.867 m 59.85 43.367 l S 31.6 35.617 m 27.85 36.367 l S 36.35 26.117 m 34.35 24.617 l S 33.85 14.117 m 31.1 16.367 l S 37.1 9.867 m 35.1 11.117 l S 34.35 20.867 m 31.35 20.867 l S 44.6 56.617 m 42.1 54.867 l S 47.35 51.367 m 44.35 51.367 l S 44.1 43.867 m 41.35 45.617 l S 43.35 33.117 m 42.6 30.617 l S 43.85 23.617 m 41.1 25.867 l S 44.35 15.617 m 42.35 16.867 l S 67.823 31.1 m 64.823 31.1 l S 27.1 32.617 m 29.6 30.867 l S 31.85 55.117 m 34.85 55.117 l S 19.6 40.867 m 22.1 39.117 l S 16.85 35.617 m 19.85 35.617 l S 20.1 28.117 m 22.85 29.867 l S 52.1 42.617 m 54.484 44.178 l S 52.437 50.146 m 54.821 48.325 l S 59.572 54.133 m 59.35 51.117 l S 50.185 10.055 m 53.234 9.928 l S 51.187 15.896 m 53.571 14.075 l S 58.322 19.883 m 59.445 16.823 l S 53.1 32.117 m 50.6 30.367 l S 52.85 24.617 m 49.6 25.617 l S 61.85 9.117 m 59.1 10.867 l S 69.35 34.617 m 66.6 36.367 l S 67.1 23.617 m 65.1 22.117 l S 24.435 46.055 m 27.484 45.928 l S 25.437 51.896 m 27.821 50.075 l S 62.6 47.117 m 65.321 46.575 l S 19.85 19.867 m 20.35 16.617 l S 21.85 21.867 m 25.35 22.617 l S 37.6 62.867 m 41.6 62.117 l S 38.323 42.1 m 38.823 38.6 l S 69.35 52.617 m 66.85 53.867 l S 14.85 62.117 m 18.1 59.367 l S 9.6 46.117 m 7.1 44.367 l S 20.6 51.617 m 18.6 50.117 l S 46.141 70.811 m 47.994 73.492 l S 69.391 40.561 m 71.244 43.242 l S 38.641 49.311 m 39.35 52.117 l S 25.141 16.811 m 25.85 19.617 l S 36.6 32.867 m 34.6 31.367 l S 6.1 68.617 m 2.85 67.867 l S 4.85 56.867 m 2.35 55.117 l S 7.6 51.617 m 4.6 51.617 l S 6.6 35.867 m 4.6 34.367 l S 6.1 12.867 m 1.85 13.617 l S 4.6 30.617 m 1.6 30.617 l S 72.814 74.769 m 73.928 77.729 l S 67.976 74.633 m 67.35 77.909 l S 52.762 73.779 m 52.876 76.776 l S 37.062 75.375 m 35.639 77.43 l S 20.795 75.242 m 22.12 77.193 l S 9.736 73.91 m 8.073 76.225 l S 10.1 23.617 m 6.35 24.367 l S 73.217 18.276 m 71.323 21.1 l S 28.823 39.6 m 29.505 42.389 l S 49.6 38.617 m 47.6 37.117 l S 60.323 73.6 m 62.323 76.6 l S 60.323 1.6 m 62.323 4.6 l S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.inre) (Lagerbl.inre) 1 1 28.5392 28.5392 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.2768 15.3585 m 28.9144 15.3585 L 28.9144 14.2335 L 19.2768 14.2335 L 19.2768 15.3585 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 14.7461 18.9624 m 13.0264 17.8486 11.3273 14.4193 11.3273 10.0362 c 11.3273 5.6547 12.9768 2.1518 14.744 1.1112 C 14.7443 1.1112 L 16.4707 2.1518 18.1679 5.6547 18.1679 10.0362 c 18.1679 14.4143 16.432 17.8633 14.7461 18.9624 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.inre\012 1) (Lagerbl.inre\012 1) 1 1 28.5392 28.5392 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.2768 15.3585 m 28.9144 15.3585 L 28.9144 14.2335 L 19.2768 14.2335 L 19.2768 15.3585 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 14.7461 18.9624 m 13.0264 17.8486 11.3273 14.4193 11.3273 10.0362 c 11.3273 5.6547 12.9768 2.1518 14.744 1.1112 C 14.7443 1.1112 L 16.4707 2.1518 18.1679 5.6547 18.1679 10.0362 c 18.1679 14.4143 16.432 17.8633 14.7461 18.9624 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.inre\012 2) (Lagerbl.inre\012 2) 1 1 28.5392 28.5392 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.2768 15.3585 m 28.9144 15.3585 L 28.9144 14.2335 L 19.2768 14.2335 L 19.2768 15.3585 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 14.7461 18.9624 m 13.0264 17.8486 11.3273 14.4193 11.3273 10.0362 c 11.3273 5.6547 12.9768 2.1518 14.744 1.1112 C 14.7443 1.1112 L 16.4707 2.1518 18.1679 5.6547 18.1679 10.0362 c 18.1679 14.4143 16.432 17.8633 14.7461 18.9624 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.inre\012 3) (Lagerbl.inre\012 3) 1 1 28.5392 28.5392 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.2768 15.3585 m 28.9144 15.3585 L 28.9144 14.2335 L 19.2768 14.2335 L 19.2768 15.3585 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 14.7461 18.9624 m 13.0264 17.8486 11.3273 14.4193 11.3273 10.0362 c 11.3273 5.6547 12.9768 2.1518 14.744 1.1112 C 14.7443 1.1112 L 16.4707 2.1518 18.1679 5.6547 18.1679 10.0362 c 18.1679 14.4143 16.432 17.8633 14.7461 18.9624 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.inre\012 4) (Lagerbl.inre\012 4) 1 1 28.5392 28.5392 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.2768 15.3585 m 28.9144 15.3585 L 28.9144 14.2335 L 19.2768 14.2335 L 19.2768 15.3585 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 14.7461 18.9624 m 13.0264 17.8486 11.3273 14.4193 11.3273 10.0362 c 11.3273 5.6547 12.9768 2.1518 14.744 1.1112 C 14.7443 1.1112 L 16.4707 2.1518 18.1679 5.6547 18.1679 10.0362 c 18.1679 14.4143 16.432 17.8633 14.7461 18.9624 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.sida) (Lagerbl.sida) 1.3972 1 28.9364 28.5392 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.1571 15.2998 m 1 15.2998 L 1 14.1748 L 29.1571 14.1748 L 29.1571 15.2998 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 2.0183 27.4787 m 1.5899 25.4751 2.8132 21.8488 5.9125 18.7494 c 9.0107 15.6513 12.654 14.3407 14.6395 14.8545 C 14.6398 14.8547 L 15.1246 16.8113 13.8478 20.4883 10.7496 23.5865 c 7.6538 26.6824 3.9876 27.8936 2.0183 27.4787 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.39 0.7 0.12 k 0 0.39 0.7 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 2.0183 2.0091 m 1.5899 4.0126 2.8132 7.6389 5.9125 10.7382 c 9.0107 13.8365 12.654 15.147 14.6395 14.6332 C 14.6398 14.633 L 15.1246 12.6765 13.8478 8.9993 10.7496 5.9011 c 7.6538 2.8054 3.9876 1.5941 2.0183 2.0091 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.821 2.0091 m 15.3925 4.0126 16.6159 7.6389 19.7152 10.7382 c 22.8134 13.8365 26.4567 15.147 28.4422 14.6332 C 28.4424 14.633 L 28.9273 12.6765 27.6505 8.9993 24.5523 5.9011 c 21.4565 2.8054 17.7903 1.5941 15.821 2.0091 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.39 0.7 0.12 k 0 0.39 0.7 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.821 27.4787 m 15.3925 25.4751 16.6159 21.8488 19.7152 18.7494 c 22.8134 15.6513 26.4567 14.3407 28.4422 14.8545 C 28.4424 14.8547 L 28.9273 16.8113 27.6505 20.4883 24.5523 23.5865 c 21.4565 26.6824 17.7903 27.8936 15.821 27.4787 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.sida\012 1) (Lagerbl.sida\012 1) 1.3972 1 28.9364 28.5392 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.1571 15.2998 m 1 15.2998 L 1 14.1748 L 29.1571 14.1748 L 29.1571 15.2998 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 2.0183 27.4787 m 1.5899 25.4751 2.8132 21.8488 5.9125 18.7494 c 9.0107 15.6513 12.654 14.3407 14.6395 14.8545 C 14.6398 14.8547 L 15.1246 16.8113 13.8478 20.4883 10.7496 23.5865 c 7.6538 26.6824 3.9876 27.8936 2.0183 27.4787 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.39 0.7 0.12 k 0 0.39 0.7 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 2.0183 2.0091 m 1.5899 4.0126 2.8132 7.6389 5.9125 10.7382 c 9.0107 13.8365 12.654 15.147 14.6395 14.6332 C 14.6398 14.633 L 15.1246 12.6765 13.8478 8.9993 10.7496 5.9011 c 7.6538 2.8054 3.9876 1.5941 2.0183 2.0091 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.821 2.0091 m 15.3925 4.0126 16.6159 7.6389 19.7152 10.7382 c 22.8134 13.8365 26.4567 15.147 28.4422 14.6332 C 28.4424 14.633 L 28.9273 12.6765 27.6505 8.9993 24.5523 5.9011 c 21.4565 2.8054 17.7903 1.5941 15.821 2.0091 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.39 0.7 0.12 k 0 0.39 0.7 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.821 27.4787 m 15.3925 25.4751 16.6159 21.8488 19.7152 18.7494 c 22.8134 15.6513 26.4567 14.3407 28.4422 14.8545 C 28.4424 14.8547 L 28.9273 16.8113 27.6505 20.4883 24.5523 23.5865 c 21.4565 26.6824 17.7903 27.8936 15.821 27.4787 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.sida\012 2) (Lagerbl.sida\012 2) 1.3972 1 28.9364 28.5392 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.1571 15.2998 m 1 15.2998 L 1 14.1748 L 29.1571 14.1748 L 29.1571 15.2998 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 2.0183 27.4787 m 1.5899 25.4751 2.8132 21.8488 5.9125 18.7494 c 9.0107 15.6513 12.654 14.3407 14.6395 14.8545 C 14.6398 14.8547 L 15.1246 16.8113 13.8478 20.4883 10.7496 23.5865 c 7.6538 26.6824 3.9876 27.8936 2.0183 27.4787 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.39 0.7 0.12 k 0 0.39 0.7 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 2.0183 2.0091 m 1.5899 4.0126 2.8132 7.6389 5.9125 10.7382 c 9.0107 13.8365 12.654 15.147 14.6395 14.6332 C 14.6398 14.633 L 15.1246 12.6765 13.8478 8.9993 10.7496 5.9011 c 7.6538 2.8054 3.9876 1.5941 2.0183 2.0091 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.821 2.0091 m 15.3925 4.0126 16.6159 7.6389 19.7152 10.7382 c 22.8134 13.8365 26.4567 15.147 28.4422 14.6332 C 28.4424 14.633 L 28.9273 12.6765 27.6505 8.9993 24.5523 5.9011 c 21.4565 2.8054 17.7903 1.5941 15.821 2.0091 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.39 0.7 0.12 k 0 0.39 0.7 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.821 27.4787 m 15.3925 25.4751 16.6159 21.8488 19.7152 18.7494 c 22.8134 15.6513 26.4567 14.3407 28.4422 14.8545 C 28.4424 14.8547 L 28.9273 16.8113 27.6505 20.4883 24.5523 23.5865 c 21.4565 26.6824 17.7903 27.8936 15.821 27.4787 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.sida\012 3) (Lagerbl.sida\012 3) 1.3972 1 28.9364 28.5392 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.1571 15.2998 m 1 15.2998 L 1 14.1748 L 29.1571 14.1748 L 29.1571 15.2998 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 2.0183 27.4787 m 1.5899 25.4751 2.8132 21.8488 5.9125 18.7494 c 9.0107 15.6513 12.654 14.3407 14.6395 14.8545 C 14.6398 14.8547 L 15.1246 16.8113 13.8478 20.4883 10.7496 23.5865 c 7.6538 26.6824 3.9876 27.8936 2.0183 27.4787 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.39 0.7 0.12 k 0 0.39 0.7 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 2.0183 2.0091 m 1.5899 4.0126 2.8132 7.6389 5.9125 10.7382 c 9.0107 13.8365 12.654 15.147 14.6395 14.6332 C 14.6398 14.633 L 15.1246 12.6765 13.8478 8.9993 10.7496 5.9011 c 7.6538 2.8054 3.9876 1.5941 2.0183 2.0091 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.821 2.0091 m 15.3925 4.0126 16.6159 7.6389 19.7152 10.7382 c 22.8134 13.8365 26.4567 15.147 28.4422 14.6332 C 28.4424 14.633 L 28.9273 12.6765 27.6505 8.9993 24.5523 5.9011 c 21.4565 2.8054 17.7903 1.5941 15.821 2.0091 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.39 0.7 0.12 k 0 0.39 0.7 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.821 27.4787 m 15.3925 25.4751 16.6159 21.8488 19.7152 18.7494 c 22.8134 15.6513 26.4567 14.3407 28.4422 14.8545 C 28.4424 14.8547 L 28.9273 16.8113 27.6505 20.4883 24.5523 23.5865 c 21.4565 26.6824 17.7903 27.8936 15.821 27.4787 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.sida\012 4) (Lagerbl.sida\012 4) 1.3972 1 28.9364 28.5392 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.1571 15.2998 m 1 15.2998 L 1 14.1748 L 29.1571 14.1748 L 29.1571 15.2998 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 2.0183 27.4787 m 1.5899 25.4751 2.8132 21.8488 5.9125 18.7494 c 9.0107 15.6513 12.654 14.3407 14.6395 14.8545 C 14.6398 14.8547 L 15.1246 16.8113 13.8478 20.4883 10.7496 23.5865 c 7.6538 26.6824 3.9876 27.8936 2.0183 27.4787 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.39 0.7 0.12 k 0 0.39 0.7 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 2.0183 2.0091 m 1.5899 4.0126 2.8132 7.6389 5.9125 10.7382 c 9.0107 13.8365 12.654 15.147 14.6395 14.6332 C 14.6398 14.633 L 15.1246 12.6765 13.8478 8.9993 10.7496 5.9011 c 7.6538 2.8054 3.9876 1.5941 2.0183 2.0091 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.821 2.0091 m 15.3925 4.0126 16.6159 7.6389 19.7152 10.7382 c 22.8134 13.8365 26.4567 15.147 28.4422 14.6332 C 28.4424 14.633 L 28.9273 12.6765 27.6505 8.9993 24.5523 5.9011 c 21.4565 2.8054 17.7903 1.5941 15.821 2.0091 C f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.39 0.7 0.12 k 0 0.39 0.7 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.821 27.4787 m 15.3925 25.4751 16.6159 21.8488 19.7152 18.7494 c 22.8134 15.6513 26.4567 14.3407 28.4422 14.8545 C 28.4424 14.8547 L 28.9273 16.8113 27.6505 20.4883 24.5523 23.5865 c 21.4565 26.6824 17.7903 27.8936 15.821 27.4787 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.yttre) (Lagerbl.yttre) 1 1.3751 28.5393 28.9143 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 14.2395 10.6375 m 14.2395 1 L 15.3645 1 L 15.3645 10.6375 L 14.2395 10.6375 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 10.5769 15.124 m 11.6906 16.8438 15.1198 18.5429 19.503 18.5429 c 23.8844 18.5429 27.3874 16.8935 28.428 15.1262 C 28.428 15.1259 L 27.3874 13.3995 23.8844 11.7023 19.503 11.7023 c 15.1249 11.7023 11.676 13.4382 10.5769 15.124 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.yttre\012 1) (Lagerbl.yttre\012 1) 1 1.3751 28.5393 28.9143 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 14.2395 10.6375 m 14.2395 1 L 15.3645 1 L 15.3645 10.6375 L 14.2395 10.6375 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 10.5769 15.124 m 11.6906 16.8438 15.1198 18.5429 19.503 18.5429 c 23.8844 18.5429 27.3874 16.8935 28.428 15.1262 C 28.428 15.1259 L 27.3874 13.3995 23.8844 11.7023 19.503 11.7023 c 15.1249 11.7023 11.676 13.4382 10.5769 15.124 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.yttre\012 2) (Lagerbl.yttre\012 2) 1 1.3751 28.5393 28.9143 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 14.2395 10.6375 m 14.2395 1 L 15.3645 1 L 15.3645 10.6375 L 14.2395 10.6375 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 10.5769 15.124 m 11.6906 16.8438 15.1198 18.5429 19.503 18.5429 c 23.8844 18.5429 27.3874 16.8935 28.428 15.1262 C 28.428 15.1259 L 27.3874 13.3995 23.8844 11.7023 19.503 11.7023 c 15.1249 11.7023 11.676 13.4382 10.5769 15.124 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.yttre\012 3) (Lagerbl.yttre\012 3) 1 1.3751 28.5393 28.9143 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 14.2395 10.6375 m 14.2395 1 L 15.3645 1 L 15.3645 10.6375 L 14.2395 10.6375 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 10.5769 15.124 m 11.6906 16.8438 15.1198 18.5429 19.503 18.5429 c 23.8844 18.5429 27.3874 16.8935 28.428 15.1262 C 28.428 15.1259 L 27.3874 13.3995 23.8844 11.7023 19.503 11.7023 c 15.1249 11.7023 11.676 13.4382 10.5769 15.124 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Lagerbl.yttre\012 4) (Lagerbl.yttre\012 4) 1 1.3751 28.5393 28.9143 [ %AI3_Tile (0 O 0 R 0 0.55 1 0.12 k 0 0.55 1 0.12 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 14.2395 10.6375 m 14.2395 1 L 15.3645 1 L 15.3645 10.6375 L 14.2395 10.6375 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.55 1 0.3 k 0 0.55 1 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 10.5769 15.124 m 11.6906 16.8438 15.1198 18.5429 19.503 18.5429 c 23.8844 18.5429 27.3874 16.8935 28.428 15.1262 C 28.428 15.1259 L 27.3874 13.3995 23.8844 11.7023 19.503 11.7023 c 15.1249 11.7023 11.676 13.4382 10.5769 15.124 C f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Listprofil.sida) (Listprofil.sida) 1.0006 1 29.0006 31.6124 [ %AI3_Tile (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29 4.8087 m 29 4.8087 L 29.0026 5.4927 L 1.0026 5.4927 L 1 4.8087 L 1 4.8087 L 29 4.8087 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.2 k 0 0 0 0.2 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0026 5.4927 m 29.0005 9.5045 L 1.0005 9.5045 L 1.0026 5.4927 L 29.0026 5.4927 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0005 9.5045 m 29.0011 10.4865 L 1.0011 10.4865 L 1.0005 9.5045 L 29.0005 9.5045 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0011 10.4865 m 29.003 17.209 L 1.003 17.209 L 1.0011 10.4865 L 29.0011 10.4865 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.003 17.209 m 29.0031 18.3656 L 1.0031 18.3656 L 1.003 17.209 L 29.003 17.209 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0031 18.3656 m 29.0006 30.4752 L 1.0006 30.4752 L 1.0031 18.3656 L 29.0031 18.3656 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Listprofil.sida\012 1) (Listprofil.sida\012 1) 1.0006 1 29.0006 31.6124 [ %AI3_Tile (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29 4.8087 m 29 4.8087 L 29.0026 5.4927 L 1.0026 5.4927 L 1 4.8087 L 1 4.8087 L 29 4.8087 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.2 k 0 0 0 0.2 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0026 5.4927 m 29.0005 9.5045 L 1.0005 9.5045 L 1.0026 5.4927 L 29.0026 5.4927 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0005 9.5045 m 29.0011 10.4865 L 1.0011 10.4865 L 1.0005 9.5045 L 29.0005 9.5045 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0011 10.4865 m 29.003 17.209 L 1.003 17.209 L 1.0011 10.4865 L 29.0011 10.4865 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.003 17.209 m 29.0031 18.3656 L 1.0031 18.3656 L 1.003 17.209 L 29.003 17.209 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0031 18.3656 m 29.0006 30.4752 L 1.0006 30.4752 L 1.0031 18.3656 L 29.0031 18.3656 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Listprofil.sida\012 2) (Listprofil.sida\012 2) 1.0006 1 29.0006 31.6124 [ %AI3_Tile (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29 4.8087 m 29 4.8087 L 29.0026 5.4927 L 1.0026 5.4927 L 1 4.8087 L 1 4.8087 L 29 4.8087 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.2 k 0 0 0 0.2 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0026 5.4927 m 29.0005 9.5045 L 1.0005 9.5045 L 1.0026 5.4927 L 29.0026 5.4927 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0005 9.5045 m 29.0011 10.4865 L 1.0011 10.4865 L 1.0005 9.5045 L 29.0005 9.5045 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0011 10.4865 m 29.003 17.209 L 1.003 17.209 L 1.0011 10.4865 L 29.0011 10.4865 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.003 17.209 m 29.0031 18.3656 L 1.0031 18.3656 L 1.003 17.209 L 29.003 17.209 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0031 18.3656 m 29.0006 30.4752 L 1.0006 30.4752 L 1.0031 18.3656 L 29.0031 18.3656 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Listprofil.sida\012 3) (Listprofil.sida\012 3) 1.0006 1 29.0006 31.6124 [ %AI3_Tile (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29 4.8087 m 29 4.8087 L 29.0026 5.4927 L 1.0026 5.4927 L 1 4.8087 L 1 4.8087 L 29 4.8087 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.2 k 0 0 0 0.2 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0026 5.4927 m 29.0005 9.5045 L 1.0005 9.5045 L 1.0026 5.4927 L 29.0026 5.4927 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0005 9.5045 m 29.0011 10.4865 L 1.0011 10.4865 L 1.0005 9.5045 L 29.0005 9.5045 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0011 10.4865 m 29.003 17.209 L 1.003 17.209 L 1.0011 10.4865 L 29.0011 10.4865 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.003 17.209 m 29.0031 18.3656 L 1.0031 18.3656 L 1.003 17.209 L 29.003 17.209 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0031 18.3656 m 29.0006 30.4752 L 1.0006 30.4752 L 1.0031 18.3656 L 29.0031 18.3656 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Listprofil.sida\012 4) (Listprofil.sida\012 4) 1.0006 1 29.0006 31.6124 [ %AI3_Tile (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29 4.8087 m 29 4.8087 L 29.0026 5.4927 L 1.0026 5.4927 L 1 4.8087 L 1 4.8087 L 29 4.8087 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.2 k 0 0 0 0.2 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0026 5.4927 m 29.0005 9.5045 L 1.0005 9.5045 L 1.0026 5.4927 L 29.0026 5.4927 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0005 9.5045 m 29.0011 10.4865 L 1.0011 10.4865 L 1.0005 9.5045 L 29.0005 9.5045 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0011 10.4865 m 29.003 17.209 L 1.003 17.209 L 1.0011 10.4865 L 29.0011 10.4865 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.003 17.209 m 29.0031 18.3656 L 1.0031 18.3656 L 1.003 17.209 L 29.003 17.209 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 29.0031 18.3656 m 29.0006 30.4752 L 1.0006 30.4752 L 1.0031 18.3656 L 29.0031 18.3656 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Listprofil.yttre) (Listprofil.yttre) 1 1.0004 31.6124 31.6127 [ %AI3_Tile (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6118 5.4917 m 27.1221 5.4917 L 27.1205 1.0011 L 27.8031 1.0011 L 27.8031 4.8091 L 31.6118 4.8091 L 31.6118 5.4917 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.2 k 0 0 0 0.2 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6149 9.5062 m 23.1111 9.5062 L 23.1111 1.0015 L 27.1205 1.0015 L 27.1205 5.493 L 31.6144 5.493 L 31.6149 9.5062 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6124 10.485 m 22.1297 10.485 L 22.1292 1.0015 L 23.1084 1.0015 L 23.1084 9.5049 L 31.6124 9.5049 L 31.6124 10.485 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6129 17.2066 m 15.4064 17.2085 L 15.4064 1 L 22.1301 1 L 22.1301 10.4868 L 31.6129 10.4868 L 31.6129 17.2066 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6149 18.3658 m 14.2517 18.3658 L 14.2515 1.0009 L 15.4043 1.0009 L 15.4043 17.2093 L 31.6149 17.2093 L 31.6149 18.3658 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6124 30.4755 m 2.1395 30.4755 L 2.1395 1.0015 L 14.249 1 L 14.249 18.366 L 31.6149 18.366 L 31.6124 30.4755 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.6 k 0 0 0 0.6 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.4066 16.847 m 14.2778 18.3257 l 15.4066 17.2057 l 15.4066 16.847 l f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 23.1095 9.1906 m 22.1759 10.4392 l 23.1082 9.505 l 23.1095 9.1906 l f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 27.8039 4.6026 m 27.1619 5.4533 l 27.8029 4.8093 l 27.8039 4.6026 l f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Listprofil.yttre\012 1) (Listprofil.yttre\012 1) 1 1.0004 31.6124 31.6127 [ %AI3_Tile (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6118 5.4917 m 27.1221 5.4917 L 27.1205 1.0011 L 27.8031 1.0011 L 27.8031 4.8091 L 31.6118 4.8091 L 31.6118 5.4917 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.2 k 0 0 0 0.2 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6149 9.5062 m 23.1111 9.5062 L 23.1111 1.0015 L 27.1205 1.0015 L 27.1205 5.493 L 31.6144 5.493 L 31.6149 9.5062 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6124 10.485 m 22.1297 10.485 L 22.1292 1.0015 L 23.1084 1.0015 L 23.1084 9.5049 L 31.6124 9.5049 L 31.6124 10.485 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6129 17.2066 m 15.4064 17.2085 L 15.4064 1 L 22.1301 1 L 22.1301 10.4868 L 31.6129 10.4868 L 31.6129 17.2066 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6149 18.3658 m 14.2517 18.3658 L 14.2515 1.0009 L 15.4043 1.0009 L 15.4043 17.2093 L 31.6149 17.2093 L 31.6149 18.3658 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6124 30.4755 m 2.1395 30.4755 L 2.1395 1.0015 L 14.249 1 L 14.249 18.366 L 31.6149 18.366 L 31.6124 30.4755 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.6 k 0 0 0 0.6 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.4066 16.847 m 14.2778 18.3257 l 15.4066 17.2057 l 15.4066 16.847 l f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 23.1095 9.1906 m 22.1759 10.4392 l 23.1082 9.505 l 23.1095 9.1906 l f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 27.8039 4.6026 m 27.1619 5.4533 l 27.8029 4.8093 l 27.8039 4.6026 l f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Listprofil.yttre\012 2) (Listprofil.yttre\012 2) 1 1.0004 31.6124 31.6127 [ %AI3_Tile (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6118 5.4917 m 27.1221 5.4917 L 27.1205 1.0011 L 27.8031 1.0011 L 27.8031 4.8091 L 31.6118 4.8091 L 31.6118 5.4917 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.2 k 0 0 0 0.2 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6149 9.5062 m 23.1111 9.5062 L 23.1111 1.0015 L 27.1205 1.0015 L 27.1205 5.493 L 31.6144 5.493 L 31.6149 9.5062 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6124 10.485 m 22.1297 10.485 L 22.1292 1.0015 L 23.1084 1.0015 L 23.1084 9.5049 L 31.6124 9.5049 L 31.6124 10.485 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6129 17.2066 m 15.4064 17.2085 L 15.4064 1 L 22.1301 1 L 22.1301 10.4868 L 31.6129 10.4868 L 31.6129 17.2066 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6149 18.3658 m 14.2517 18.3658 L 14.2515 1.0009 L 15.4043 1.0009 L 15.4043 17.2093 L 31.6149 17.2093 L 31.6149 18.3658 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6124 30.4755 m 2.1395 30.4755 L 2.1395 1.0015 L 14.249 1 L 14.249 18.366 L 31.6149 18.366 L 31.6124 30.4755 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.6 k 0 0 0 0.6 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.4066 16.847 m 14.2778 18.3257 l 15.4066 17.2057 l 15.4066 16.847 l f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 23.1095 9.1906 m 22.1759 10.4392 l 23.1082 9.505 l 23.1095 9.1906 l f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 27.8039 4.6026 m 27.1619 5.4533 l 27.8029 4.8093 l 27.8039 4.6026 l f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Listprofil.yttre\012 3) (Listprofil.yttre\012 3) 1 1.0004 31.6124 31.6127 [ %AI3_Tile (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6118 5.4917 m 27.1221 5.4917 L 27.1205 1.0011 L 27.8031 1.0011 L 27.8031 4.8091 L 31.6118 4.8091 L 31.6118 5.4917 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.2 k 0 0 0 0.2 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6149 9.5062 m 23.1111 9.5062 L 23.1111 1.0015 L 27.1205 1.0015 L 27.1205 5.493 L 31.6144 5.493 L 31.6149 9.5062 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6124 10.485 m 22.1297 10.485 L 22.1292 1.0015 L 23.1084 1.0015 L 23.1084 9.5049 L 31.6124 9.5049 L 31.6124 10.485 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6129 17.2066 m 15.4064 17.2085 L 15.4064 1 L 22.1301 1 L 22.1301 10.4868 L 31.6129 10.4868 L 31.6129 17.2066 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6149 18.3658 m 14.2517 18.3658 L 14.2515 1.0009 L 15.4043 1.0009 L 15.4043 17.2093 L 31.6149 17.2093 L 31.6149 18.3658 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6124 30.4755 m 2.1395 30.4755 L 2.1395 1.0015 L 14.249 1 L 14.249 18.366 L 31.6149 18.366 L 31.6124 30.4755 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.6 k 0 0 0 0.6 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.4066 16.847 m 14.2778 18.3257 l 15.4066 17.2057 l 15.4066 16.847 l f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 23.1095 9.1906 m 22.1759 10.4392 l 23.1082 9.505 l 23.1095 9.1906 l f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 27.8039 4.6026 m 27.1619 5.4533 l 27.8029 4.8093 l 27.8039 4.6026 l f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Listprofil.yttre\012 4) (Listprofil.yttre\012 4) 1 1.0004 31.6124 31.6127 [ %AI3_Tile (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6118 5.4917 m 27.1221 5.4917 L 27.1205 1.0011 L 27.8031 1.0011 L 27.8031 4.8091 L 31.6118 4.8091 L 31.6118 5.4917 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.2 k 0 0 0 0.2 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6149 9.5062 m 23.1111 9.5062 L 23.1111 1.0015 L 27.1205 1.0015 L 27.1205 5.493 L 31.6144 5.493 L 31.6149 9.5062 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6124 10.485 m 22.1297 10.485 L 22.1292 1.0015 L 23.1084 1.0015 L 23.1084 9.5049 L 31.6124 9.5049 L 31.6124 10.485 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.3 k 0 0 0 0.3 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6129 17.2066 m 15.4064 17.2085 L 15.4064 1 L 22.1301 1 L 22.1301 10.4868 L 31.6129 10.4868 L 31.6129 17.2066 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6149 18.3658 m 14.2517 18.3658 L 14.2515 1.0009 L 15.4043 1.0009 L 15.4043 17.2093 L 31.6149 17.2093 L 31.6149 18.3658 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 31.6124 30.4755 m 2.1395 30.4755 L 2.1395 1.0015 L 14.249 1 L 14.249 18.366 L 31.6149 18.366 L 31.6124 30.4755 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.6 k 0 0 0 0.6 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 15.4066 16.847 m 14.2778 18.3257 l 15.4066 17.2057 l 15.4066 16.847 l f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.5 k 0 0 0 0.5 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 23.1095 9.1906 m 22.1759 10.4392 l 23.1082 9.505 l 23.1095 9.1906 l f %AI6_EndPatternLayer ) & (0 O 0 R 0 0 0 0.4 k 0 0 0 0.4 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 27.8039 4.6026 m 27.1619 5.4533 l 27.8029 4.8093 l 27.8039 4.6026 l f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Pil1.2.sida) (Pil1.2.sida) 1 1 39.404 39.4039 [ %AI3_Tile (0 O 0 R 0.75 0.75 0.375 0 k 0.75 0.75 0.375 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 20.202 20.202 m 39.404 20.202 l S 33.904 15.6187 m 39.4248 20.202 L 39.4248 20.202 L 33.887 24.6252 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Pil1.2.sida\012 1) (Pil1.2.sida\012 1) 1 1 39.404 39.4039 [ %AI3_Tile (0 O 0 R 0.75 0.75 0.375 0 k 0.75 0.75 0.375 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 20.202 20.202 m 39.404 20.202 l S 33.904 15.6187 m 39.4248 20.202 L 39.4248 20.202 L 33.887 24.6252 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Pil1.2.sida\012 2) (Pil1.2.sida\012 2) 1 1 39.404 39.4039 [ %AI3_Tile (0 O 0 R 0.75 0.75 0.375 0 k 0.75 0.75 0.375 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 20.202 20.202 m 39.404 20.202 l S 33.904 15.6187 m 39.4248 20.202 L 39.4248 20.202 L 33.887 24.6252 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Pil1.2.sida\012 3) (Pil1.2.sida\012 3) 1 1 39.404 39.4039 [ %AI3_Tile (0 O 0 R 0.75 0.75 0.375 0 k 0.75 0.75 0.375 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 20.202 20.202 m 39.404 20.202 l S 33.904 15.6187 m 39.4248 20.202 L 39.4248 20.202 L 33.887 24.6252 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Pil1.2.sida\012 4) (Pil1.2.sida\012 4) 1 1 39.404 39.4039 [ %AI3_Tile (0 O 0 R 0.75 0.75 0.375 0 k 0.75 0.75 0.375 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 20.202 20.202 m 39.404 20.202 l S 33.904 15.6187 m 39.4248 20.202 L 39.4248 20.202 L 33.887 24.6252 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Pil1.2.ut/in) (Pil1.2.ut/in) 1 1 39.4039 39.4039 [ %AI3_Tile (0 O 0 R 0.75 0.75 0.375 0 k 0.75 0.75 0.375 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 33.9039 15.6187 m 39.4247 20.202 L 39.4247 20.202 L 33.8869 24.6252 L S 39.2997 20.202 m 24.5706 20.202 l 20.4039 20.4792 20.4039 16.8125 v 20.4039 13.1458 20.4039 12.5625 y S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Pil1.2.ut/in\012 1) (Pil1.2.ut/in\012 1) 1 1 39.4039 39.4039 [ %AI3_Tile (0 O 0 R 0.75 0.75 0.375 0 k 0.75 0.75 0.375 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 33.9039 15.6187 m 39.4247 20.202 L 39.4247 20.202 L 33.8869 24.6252 L S 39.2997 20.202 m 24.5706 20.202 l 20.4039 20.4792 20.4039 16.8125 v 20.4039 13.1458 20.4039 12.5625 y S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Pil1.2.ut/in\012 2) (Pil1.2.ut/in\012 2) 1 1 39.4039 39.4039 [ %AI3_Tile (0 O 0 R 0.75 0.75 0.375 0 k 0.75 0.75 0.375 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 33.9039 15.6187 m 39.4247 20.202 L 39.4247 20.202 L 33.8869 24.6252 L S 39.2997 20.202 m 24.5706 20.202 l 20.4039 20.4792 20.4039 16.8125 v 20.4039 13.1458 20.4039 12.5625 y S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Pil1.2.ut/in\012 3) (Pil1.2.ut/in\012 3) 1 1 39.4039 39.4039 [ %AI3_Tile (0 O 0 R 0.75 0.75 0.375 0 k 0.75 0.75 0.375 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 33.9039 15.6187 m 39.4247 20.202 L 39.4247 20.202 L 33.8869 24.6252 L S 39.2997 20.202 m 24.5706 20.202 l 20.4039 20.4792 20.4039 16.8125 v 20.4039 13.1458 20.4039 12.5625 y S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Pil1.2.ut/in\012 4) (Pil1.2.ut/in\012 4) 1 1 39.4039 39.4039 [ %AI3_Tile (0 O 0 R 0.75 0.75 0.375 0 k 0.75 0.75 0.375 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 33.9039 15.6187 m 39.4247 20.202 L 39.4247 20.202 L 33.8869 24.6252 L S 39.2997 20.202 m 24.5706 20.202 l 20.4039 20.4792 20.4039 16.8125 v 20.4039 13.1458 20.4039 12.5625 y S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster) (Prickm\232nster) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 1) (Prickm\232nster\012 1) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 2) (Prickm\232nster\012 2) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 3) (Prickm\232nster\012 3) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 4) (Prickm\232nster\012 4) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 5) (Prickm\232nster\012 5) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 6) (Prickm\232nster\012 6) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 7) (Prickm\232nster\012 7) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 8) (Prickm\232nster\012 8) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 9) (Prickm\232nster\012 9) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 10) (Prickm\232nster\012 10) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Prickm\232nster\012 11) (Prickm\232nster\012 11) 1 1 29.8 29.8 [ %AI3_Tile (0 O 0 R 0.45 0.9 0 0 k 0.45 0.9 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 29.8 L 29.8 29.8 L 29.8 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.09 0.18 0 0 k 0.09 0.18 0 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 11.08 8.2 m 11.08 9.791 9.79 11.08 8.2 11.08 c 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c f 11.08 22.6 m 11.08 24.191 9.79 25.48 8.2 25.48 c 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c f 18.28 15.4 m 18.28 16.991 16.99 18.28 15.4 18.28 c 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c f 25.48 8.2 m 25.48 9.791 24.19 11.08 22.6 11.08 c 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c f 25.48 22.6 m 25.48 24.191 24.19 25.48 22.6 25.48 c 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c f *U 26.92 1 m 29.8 1 L 29.8 3.88 L 28.209 3.88 26.92 2.591 26.92 1 C f 15.4 3.88 m 13.809 3.88 12.52 2.591 12.52 1 C 18.28 1 L 18.28 2.591 16.99 3.88 15.4 3.88 c f 1 3.88 m 1 1 L 3.88 1 L 3.88 2.591 2.59 3.88 1 3.88 C f 26.92 15.4 m 26.92 13.81 28.209 12.52 29.8 12.52 C 29.8 18.28 L 28.209 18.28 26.92 16.991 26.92 15.4 c f 15.4 18.28 m 13.809 18.28 12.52 16.991 12.52 15.4 c 12.52 13.81 13.809 12.52 15.4 12.52 c 16.99 12.52 18.28 13.81 18.28 15.4 c 18.28 16.991 16.99 18.28 15.4 18.28 c f 3.88 15.4 m 3.88 16.991 2.59 18.28 1 18.28 C 1 12.52 L 2.59 12.52 3.88 13.81 3.88 15.4 c f 29.8 26.92 m 29.8 29.8 L 26.92 29.8 L 26.92 28.21 28.209 26.92 29.8 26.92 C f 15.4 26.92 m 16.99 26.92 18.28 28.21 18.28 29.8 C 12.52 29.8 L 12.52 28.21 13.809 26.92 15.4 26.92 c f 3.88 29.8 m 1 29.8 L 1 26.92 L 2.59 26.92 3.88 28.21 3.88 29.8 C f 8.2 11.08 m 6.609 11.08 5.32 9.791 5.32 8.2 c 5.32 6.61 6.609 5.32 8.2 5.32 c 9.79 5.32 11.08 6.61 11.08 8.2 c 11.08 9.791 9.79 11.08 8.2 11.08 c f 22.6 11.08 m 21.009 11.08 19.72 9.791 19.72 8.2 c 19.72 6.61 21.009 5.32 22.6 5.32 c 24.19 5.32 25.48 6.61 25.48 8.2 c 25.48 9.791 24.19 11.08 22.6 11.08 c f 8.2 25.48 m 6.609 25.48 5.32 24.191 5.32 22.6 c 5.32 21.01 6.609 19.72 8.2 19.72 c 9.79 19.72 11.08 21.01 11.08 22.6 c 11.08 24.191 9.79 25.48 8.2 25.48 c f 22.6 25.48 m 21.009 25.48 19.72 24.191 19.72 22.6 c 19.72 21.01 21.009 19.72 22.6 19.72 c 24.19 19.72 25.48 21.01 25.48 22.6 c 25.48 24.191 24.19 25.48 22.6 25.48 c f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Rep.sida) (Rep.sida) 1 4.6 60.9998 33.3999 [ %AI3_Tile (0 O 0 R 0 0 0 1 k 0 0 0 1 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 1 j 0.6 w 4 M []0 d %AI3_Note: 0 D 0 XR 24.9999 7 m 15.6521 4.663 8.125 8.6981 1 14.1407 C S 36.9999 7 m 22.3477 3.337 12.168 15.3276 1 23.859 C S 48.9999 7 m 29.3464 2.0866 17.7386 25.3332 1 30.6213 C S 1 30.9999 m 24.9999 36.9999 36.9999 1 60.9998 7 C S 13 30.9999 m 32.6534 35.9133 44.2611 12.6667 60.9998 7.3786 C S 24.9999 30.9999 m 39.652 34.6629 49.8317 22.6722 60.9998 14.1407 C S 36.9999 30.9999 m 46.3476 33.3369 53.8749 29.3018 60.9998 23.859 C S 48.9999 30.9999 m 53.3464 32.0865 57.2978 31.7908 60.9998 30.6213 C S 13 7 m 8.6535 5.9134 4.7019 6.2091 1 7.3786 C S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Rep.sida\012 1) (Rep.sida\012 1) 1 4.6 60.9998 33.3999 [ %AI3_Tile (0 O 0 R 0 0 0 1 k 0 0 0 1 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 1 j 0.6 w 4 M []0 d %AI3_Note: 0 D 0 XR 24.9999 7 m 15.6521 4.663 8.125 8.6981 1 14.1407 C S 36.9999 7 m 22.3477 3.337 12.168 15.3276 1 23.859 C S 48.9999 7 m 29.3464 2.0866 17.7386 25.3332 1 30.6213 C S 1 30.9999 m 24.9999 36.9999 36.9999 1 60.9998 7 C S 13 30.9999 m 32.6534 35.9133 44.2611 12.6667 60.9998 7.3786 C S 24.9999 30.9999 m 39.652 34.6629 49.8317 22.6722 60.9998 14.1407 C S 36.9999 30.9999 m 46.3476 33.3369 53.8749 29.3018 60.9998 23.859 C S 48.9999 30.9999 m 53.3464 32.0865 57.2978 31.7908 60.9998 30.6213 C S 13 7 m 8.6535 5.9134 4.7019 6.2091 1 7.3786 C S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Rep.sida\012 2) (Rep.sida\012 2) 1 4.6 60.9998 33.3999 [ %AI3_Tile (0 O 0 R 0 0 0 1 k 0 0 0 1 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 1 j 0.6 w 4 M []0 d %AI3_Note: 0 D 0 XR 24.9999 7 m 15.6521 4.663 8.125 8.6981 1 14.1407 C S 36.9999 7 m 22.3477 3.337 12.168 15.3276 1 23.859 C S 48.9999 7 m 29.3464 2.0866 17.7386 25.3332 1 30.6213 C S 1 30.9999 m 24.9999 36.9999 36.9999 1 60.9998 7 C S 13 30.9999 m 32.6534 35.9133 44.2611 12.6667 60.9998 7.3786 C S 24.9999 30.9999 m 39.652 34.6629 49.8317 22.6722 60.9998 14.1407 C S 36.9999 30.9999 m 46.3476 33.3369 53.8749 29.3018 60.9998 23.859 C S 48.9999 30.9999 m 53.3464 32.0865 57.2978 31.7908 60.9998 30.6213 C S 13 7 m 8.6535 5.9134 4.7019 6.2091 1 7.3786 C S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Rep.sida\012 3) (Rep.sida\012 3) 1 4.6 60.9998 33.3999 [ %AI3_Tile (0 O 0 R 0 0 0 1 k 0 0 0 1 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 1 j 0.6 w 4 M []0 d %AI3_Note: 0 D 0 XR 24.9999 7 m 15.6521 4.663 8.125 8.6981 1 14.1407 C S 36.9999 7 m 22.3477 3.337 12.168 15.3276 1 23.859 C S 48.9999 7 m 29.3464 2.0866 17.7386 25.3332 1 30.6213 C S 1 30.9999 m 24.9999 36.9999 36.9999 1 60.9998 7 C S 13 30.9999 m 32.6534 35.9133 44.2611 12.6667 60.9998 7.3786 C S 24.9999 30.9999 m 39.652 34.6629 49.8317 22.6722 60.9998 14.1407 C S 36.9999 30.9999 m 46.3476 33.3369 53.8749 29.3018 60.9998 23.859 C S 48.9999 30.9999 m 53.3464 32.0865 57.2978 31.7908 60.9998 30.6213 C S 13 7 m 8.6535 5.9134 4.7019 6.2091 1 7.3786 C S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Rep.sida\012 4) (Rep.sida\012 4) 1 4.6 60.9998 33.3999 [ %AI3_Tile (0 O 0 R 0 0 0 1 k 0 0 0 1 K ) @ ( %AI6_BeginPatternLayer 800 Ar 1 J 1 j 0.6 w 4 M []0 d %AI3_Note: 0 D 0 XR 24.9999 7 m 15.6521 4.663 8.125 8.6981 1 14.1407 C S 36.9999 7 m 22.3477 3.337 12.168 15.3276 1 23.859 C S 48.9999 7 m 29.3464 2.0866 17.7386 25.3332 1 30.6213 C S 1 30.9999 m 24.9999 36.9999 36.9999 1 60.9998 7 C S 13 30.9999 m 32.6534 35.9133 44.2611 12.6667 60.9998 7.3786 C S 24.9999 30.9999 m 39.652 34.6629 49.8317 22.6722 60.9998 14.1407 C S 36.9999 30.9999 m 46.3476 33.3369 53.8749 29.3018 60.9998 23.859 C S 48.9999 30.9999 m 53.3464 32.0865 57.2978 31.7908 60.9998 30.6213 C S 13 7 m 8.6535 5.9134 4.7019 6.2091 1 7.3786 C S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (R\212nder) (R\212nder) 8.45 4.6001 80.45 76.6001 [ %AI3_Tile (0 O 0 R 1 0.07 1 0 k 1 0.07 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 3.6 w 4 M []0 d %AI3_Note: 0 D 0 XR 8.2 8.2 m 80.7 8.2 L S 8.2 22.6001 m 80.7 22.6001 L S 8.2 37.0002 m 80.7 37.0002 L S 8.2 51.4 m 80.7 51.4 L S 8.2 65.8001 m 80.7 65.8001 L S 8.2 15.4 m 80.7 15.4 L S 8.2 29.8001 m 80.7 29.8001 L S 8.2 44.2 m 80.7 44.2 L S 8.2 58.6001 m 80.7 58.6001 L S 8.2 73.0002 m 80.7 73.0002 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (R\212nder\012 1) (R\212nder\012 1) 8.45 4.6001 80.45 76.6001 [ %AI3_Tile (0 O 0 R 1 0.07 1 0 k 1 0.07 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 3.6 w 4 M []0 d %AI3_Note: 0 D 0 XR 8.2 8.2 m 80.7 8.2 L S 8.2 22.6001 m 80.7 22.6001 L S 8.2 37.0002 m 80.7 37.0002 L S 8.2 51.4 m 80.7 51.4 L S 8.2 65.8001 m 80.7 65.8001 L S 8.2 15.4 m 80.7 15.4 L S 8.2 29.8001 m 80.7 29.8001 L S 8.2 44.2 m 80.7 44.2 L S 8.2 58.6001 m 80.7 58.6001 L S 8.2 73.0002 m 80.7 73.0002 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (R\212nder\012 2) (R\212nder\012 2) 8.45 4.6001 80.45 76.6001 [ %AI3_Tile (0 O 0 R 1 0.07 1 0 k 1 0.07 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 3.6 w 4 M []0 d %AI3_Note: 0 D 0 XR 8.2 8.2 m 80.7 8.2 L S 8.2 22.6001 m 80.7 22.6001 L S 8.2 37.0002 m 80.7 37.0002 L S 8.2 51.4 m 80.7 51.4 L S 8.2 65.8001 m 80.7 65.8001 L S 8.2 15.4 m 80.7 15.4 L S 8.2 29.8001 m 80.7 29.8001 L S 8.2 44.2 m 80.7 44.2 L S 8.2 58.6001 m 80.7 58.6001 L S 8.2 73.0002 m 80.7 73.0002 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (R\212nder\012 3) (R\212nder\012 3) 8.45 4.6001 80.45 76.6001 [ %AI3_Tile (0 O 0 R 1 0.07 1 0 k 1 0.07 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 3.6 w 4 M []0 d %AI3_Note: 0 D 0 XR 8.2 8.2 m 80.7 8.2 L S 8.2 22.6001 m 80.7 22.6001 L S 8.2 37.0002 m 80.7 37.0002 L S 8.2 51.4 m 80.7 51.4 L S 8.2 65.8001 m 80.7 65.8001 L S 8.2 15.4 m 80.7 15.4 L S 8.2 29.8001 m 80.7 29.8001 L S 8.2 44.2 m 80.7 44.2 L S 8.2 58.6001 m 80.7 58.6001 L S 8.2 73.0002 m 80.7 73.0002 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (R\212nder\012 4) (R\212nder\012 4) 8.45 4.6001 80.45 76.6001 [ %AI3_Tile (0 O 0 R 1 0.07 1 0 k 1 0.07 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 3.6 w 4 M []0 d %AI3_Note: 0 D 0 XR 8.2 8.2 m 80.7 8.2 L S 8.2 22.6001 m 80.7 22.6001 L S 8.2 37.0002 m 80.7 37.0002 L S 8.2 51.4 m 80.7 51.4 L S 8.2 65.8001 m 80.7 65.8001 L S 8.2 15.4 m 80.7 15.4 L S 8.2 29.8001 m 80.7 29.8001 L S 8.2 44.2 m 80.7 44.2 L S 8.2 58.6001 m 80.7 58.6001 L S 8.2 73.0002 m 80.7 73.0002 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor) (Schackrutor) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 1) (Schackrutor\012 1) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 2) (Schackrutor\012 2) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 3) (Schackrutor\012 3) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 4) (Schackrutor\012 4) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 5) (Schackrutor\012 5) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 6) (Schackrutor\012 6) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 7) (Schackrutor\012 7) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 8) (Schackrutor\012 8) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 9) (Schackrutor\012 9) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 10) (Schackrutor\012 10) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Schackrutor\012 11) (Schackrutor\012 11) 1 1 31.3995 31.3995 [ %AI3_Tile (0 O 0 R 0 0.9 1 0 k 0 0.9 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 19.9995 4.8 m 27.5995 4.8 L 27.5995 12.3995 L 19.9995 12.3995 L 19.9995 4.8 L f 31.3995 27.5995 m 31.3995 31.3995 L 27.5995 31.3995 L 27.5995 27.5995 L 31.3995 27.5995 L f 19.9995 27.5995 m 19.9995 19.9995 L 27.5995 19.9995 L 27.5995 27.5995 L 19.9995 27.5995 L f 12.3995 12.3995 m 19.9995 12.3995 L 19.9995 19.9995 L 12.3995 19.9995 L 12.3995 12.3995 L f 12.3995 27.5995 m 4.8 27.5995 L 4.8 19.9995 L 12.3995 19.9995 L 12.3995 27.5995 L f 4.8 12.3995 m 4.8 4.8 L 12.3995 4.8 L 12.3995 12.3995 L 4.8 12.3995 L f 19.9995 27.5995 m 19.9995 31.3995 L 12.3995 31.3995 L 12.3995 27.5995 L 19.9995 27.5995 L f 12.3995 4.8 m 12.3995 1 L 19.9995 1 L 19.9995 4.8 L 12.3995 4.8 L f 4.8 19.9995 m 1 19.9995 L 1 12.3995 L 4.8 12.3995 L 4.8 19.9995 L f 27.5995 19.9995 m 27.5995 12.3995 L 31.3995 12.3995 L 31.3995 19.9995 L 27.5995 19.9995 L f 4.8 31.3995 m 1 31.3995 L 1 27.5995 L 4.8 27.5995 L 4.8 31.3995 L f 27.5995 1 m 31.3995 1 L 31.3995 4.8 L 27.5995 4.8 L 27.5995 1 L f 1 4.8 m 1 1 L 4.8 1 L 4.8 4.8 L 1 4.8 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.05 0.2 0 k 0 0.05 0.2 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.8 4.8 m 4.8 1 L 12.3995 1 L 12.3995 4.8 L 4.8 4.8 L f 4.8 12.3995 m 1 12.3995 L 1 4.8 L 4.8 4.8 L 4.8 12.3995 L f 19.9995 4.8 m 19.9995 1 L 27.5995 1 L 27.5995 4.8 L 19.9995 4.8 L f 12.3995 12.3995 m 12.3995 4.8 L 19.9995 4.8 L 19.9995 12.3995 L 12.3995 12.3995 L f 27.5995 4.8 m 31.3995 4.8 L 31.3995 12.3995 L 27.5995 12.3995 L 27.5995 4.8 L f 12.3995 19.9995 m 4.8 19.9995 L 4.8 12.3995 L 12.3995 12.3995 L 12.3995 19.9995 L f 4.8 27.5995 m 1 27.5995 L 1 19.9995 L 4.8 19.9995 L 4.8 27.5995 L f 19.9995 12.3995 m 27.5995 12.3995 L 27.5995 19.9995 L 19.9995 19.9995 L 19.9995 12.3995 L f 19.9995 19.9995 m 19.9995 27.5995 L 12.3995 27.5995 L 12.3995 19.9995 L 19.9995 19.9995 L f 27.5995 19.9995 m 31.3995 19.9995 L 31.3995 27.5995 L 27.5995 27.5995 L 27.5995 19.9995 L f 12.3995 27.5995 m 12.3995 31.3995 L 4.8 31.3995 L 4.8 27.5995 L 12.3995 27.5995 L f 27.5995 27.5995 m 27.5995 31.3995 L 19.9995 31.3995 L 19.9995 27.5995 L 27.5995 27.5995 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Sexh\232rning) (Sexh\232rning) 4 1.6 70.151 77.983 [ %AI3_Tile (0 O 0 R 0 1 0.35 0 k 0 1 0.35 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 70.151 77.983 m 70.151 1.6 L 4 1.6 L 4 77.983 L 70.151 77.983 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.9921 1 0 0 k 0.9921 1 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 20.538 30.244 m S 26.05 20.696 m 15.025 20.696 L 9.513 30.244 L 15.025 39.792 L 26.05 39.792 L 31.564 30.244 L 26.05 20.696 L s 20.537 11.148 m S 26.05 1.6 m 15.024 1.6 L 9.512 11.148 L 15.024 20.696 L 26.05 20.696 L 31.563 11.148 L 26.05 1.6 L s 53.614 30.244 m S 59.126 20.696 m 48.101 20.696 L 42.589 30.244 L 48.101 39.792 L 59.126 39.792 L 64.639 30.244 L 59.126 20.696 L s 53.614 11.148 m S 59.126 1.6 m 48.101 1.6 L 42.588 11.148 L 48.101 20.696 L 59.126 20.696 L 64.638 11.148 L 59.126 1.6 L s 20.538 68.436 m S 26.051 58.888 m 15.025 58.888 L 9.513 68.436 L 15.025 77.984 L 26.051 77.984 L 31.564 68.436 L 26.051 58.888 L s 20.538 49.34 m S 26.051 39.792 m 15.025 39.792 L 9.513 49.34 L 15.025 58.888 L 26.05 58.888 L 31.564 49.34 L 26.051 39.792 L s 53.614 68.436 m S 59.127 58.888 m 48.102 58.888 L 42.589 68.436 L 48.101 77.985 L 59.127 77.985 L 64.639 68.436 L 59.127 58.888 L s 53.614 49.34 m S 59.127 39.792 m 48.101 39.792 L 42.589 49.34 L 48.101 58.888 L 59.127 58.888 L 64.639 49.341 L 59.127 39.792 L s 4 20.696 m S 3.876 30.244 m 9.512 30.244 L 15.024 20.696 L 9.512 11.147 L 3.876 11.147 L S 37.075 20.696 m S 42.588 11.148 m 31.563 11.148 L 26.05 20.696 L 31.563 30.244 L 42.589 30.244 L 48.101 20.696 L 42.588 11.148 L s 37.076 58.888 m S 42.589 49.34 m 31.564 49.34 L 26.05 58.888 L 31.564 68.436 L 42.589 68.436 L 48.101 58.888 L 42.589 49.34 L s 70.151 20.696 m S 70.2094 11.147 m 64.639 11.147 L 59.127 20.696 L 64.639 30.244 L 70.2094 30.244 L S 70.152 58.888 m S 70.0427 49.34 m 64.639 49.34 L 59.127 58.888 L 64.639 68.436 L 70.0427 68.436 L S 4 58.888 m S 3.876 68.436 m 9.513 68.436 L 15.025 58.888 L 9.513 49.34 L 3.876 49.34 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Sexh\232rning\012 1) (Sexh\232rning\012 1) 4 1.6 70.151 77.983 [ %AI3_Tile (0 O 0 R 0 1 0.35 0 k 0 1 0.35 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 70.151 77.983 m 70.151 1.6 L 4 1.6 L 4 77.983 L 70.151 77.983 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.9921 1 0 0 k 0.9921 1 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 20.538 30.244 m S 26.05 20.696 m 15.025 20.696 L 9.513 30.244 L 15.025 39.792 L 26.05 39.792 L 31.564 30.244 L 26.05 20.696 L s 20.537 11.148 m S 26.05 1.6 m 15.024 1.6 L 9.512 11.148 L 15.024 20.696 L 26.05 20.696 L 31.563 11.148 L 26.05 1.6 L s 53.614 30.244 m S 59.126 20.696 m 48.101 20.696 L 42.589 30.244 L 48.101 39.792 L 59.126 39.792 L 64.639 30.244 L 59.126 20.696 L s 53.614 11.148 m S 59.126 1.6 m 48.101 1.6 L 42.588 11.148 L 48.101 20.696 L 59.126 20.696 L 64.638 11.148 L 59.126 1.6 L s 20.538 68.436 m S 26.051 58.888 m 15.025 58.888 L 9.513 68.436 L 15.025 77.984 L 26.051 77.984 L 31.564 68.436 L 26.051 58.888 L s 20.538 49.34 m S 26.051 39.792 m 15.025 39.792 L 9.513 49.34 L 15.025 58.888 L 26.05 58.888 L 31.564 49.34 L 26.051 39.792 L s 53.614 68.436 m S 59.127 58.888 m 48.102 58.888 L 42.589 68.436 L 48.101 77.985 L 59.127 77.985 L 64.639 68.436 L 59.127 58.888 L s 53.614 49.34 m S 59.127 39.792 m 48.101 39.792 L 42.589 49.34 L 48.101 58.888 L 59.127 58.888 L 64.639 49.341 L 59.127 39.792 L s 4 20.696 m S 3.876 30.244 m 9.512 30.244 L 15.024 20.696 L 9.512 11.147 L 3.876 11.147 L S 37.075 20.696 m S 42.588 11.148 m 31.563 11.148 L 26.05 20.696 L 31.563 30.244 L 42.589 30.244 L 48.101 20.696 L 42.588 11.148 L s 37.076 58.888 m S 42.589 49.34 m 31.564 49.34 L 26.05 58.888 L 31.564 68.436 L 42.589 68.436 L 48.101 58.888 L 42.589 49.34 L s 70.151 20.696 m S 70.2094 11.147 m 64.639 11.147 L 59.127 20.696 L 64.639 30.244 L 70.2094 30.244 L S 70.152 58.888 m S 70.0427 49.34 m 64.639 49.34 L 59.127 58.888 L 64.639 68.436 L 70.0427 68.436 L S 4 58.888 m S 3.876 68.436 m 9.513 68.436 L 15.025 58.888 L 9.513 49.34 L 3.876 49.34 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Sexh\232rning\012 2) (Sexh\232rning\012 2) 4 1.6 70.151 77.983 [ %AI3_Tile (0 O 0 R 0 1 0.35 0 k 0 1 0.35 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 70.151 77.983 m 70.151 1.6 L 4 1.6 L 4 77.983 L 70.151 77.983 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.9921 1 0 0 k 0.9921 1 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 20.538 30.244 m S 26.05 20.696 m 15.025 20.696 L 9.513 30.244 L 15.025 39.792 L 26.05 39.792 L 31.564 30.244 L 26.05 20.696 L s 20.537 11.148 m S 26.05 1.6 m 15.024 1.6 L 9.512 11.148 L 15.024 20.696 L 26.05 20.696 L 31.563 11.148 L 26.05 1.6 L s 53.614 30.244 m S 59.126 20.696 m 48.101 20.696 L 42.589 30.244 L 48.101 39.792 L 59.126 39.792 L 64.639 30.244 L 59.126 20.696 L s 53.614 11.148 m S 59.126 1.6 m 48.101 1.6 L 42.588 11.148 L 48.101 20.696 L 59.126 20.696 L 64.638 11.148 L 59.126 1.6 L s 20.538 68.436 m S 26.051 58.888 m 15.025 58.888 L 9.513 68.436 L 15.025 77.984 L 26.051 77.984 L 31.564 68.436 L 26.051 58.888 L s 20.538 49.34 m S 26.051 39.792 m 15.025 39.792 L 9.513 49.34 L 15.025 58.888 L 26.05 58.888 L 31.564 49.34 L 26.051 39.792 L s 53.614 68.436 m S 59.127 58.888 m 48.102 58.888 L 42.589 68.436 L 48.101 77.985 L 59.127 77.985 L 64.639 68.436 L 59.127 58.888 L s 53.614 49.34 m S 59.127 39.792 m 48.101 39.792 L 42.589 49.34 L 48.101 58.888 L 59.127 58.888 L 64.639 49.341 L 59.127 39.792 L s 4 20.696 m S 3.876 30.244 m 9.512 30.244 L 15.024 20.696 L 9.512 11.147 L 3.876 11.147 L S 37.075 20.696 m S 42.588 11.148 m 31.563 11.148 L 26.05 20.696 L 31.563 30.244 L 42.589 30.244 L 48.101 20.696 L 42.588 11.148 L s 37.076 58.888 m S 42.589 49.34 m 31.564 49.34 L 26.05 58.888 L 31.564 68.436 L 42.589 68.436 L 48.101 58.888 L 42.589 49.34 L s 70.151 20.696 m S 70.2094 11.147 m 64.639 11.147 L 59.127 20.696 L 64.639 30.244 L 70.2094 30.244 L S 70.152 58.888 m S 70.0427 49.34 m 64.639 49.34 L 59.127 58.888 L 64.639 68.436 L 70.0427 68.436 L S 4 58.888 m S 3.876 68.436 m 9.513 68.436 L 15.025 58.888 L 9.513 49.34 L 3.876 49.34 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Sexh\232rning\012 3) (Sexh\232rning\012 3) 4 1.6 70.151 77.983 [ %AI3_Tile (0 O 0 R 0 1 0.35 0 k 0 1 0.35 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 70.151 77.983 m 70.151 1.6 L 4 1.6 L 4 77.983 L 70.151 77.983 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.9921 1 0 0 k 0.9921 1 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 20.538 30.244 m S 26.05 20.696 m 15.025 20.696 L 9.513 30.244 L 15.025 39.792 L 26.05 39.792 L 31.564 30.244 L 26.05 20.696 L s 20.537 11.148 m S 26.05 1.6 m 15.024 1.6 L 9.512 11.148 L 15.024 20.696 L 26.05 20.696 L 31.563 11.148 L 26.05 1.6 L s 53.614 30.244 m S 59.126 20.696 m 48.101 20.696 L 42.589 30.244 L 48.101 39.792 L 59.126 39.792 L 64.639 30.244 L 59.126 20.696 L s 53.614 11.148 m S 59.126 1.6 m 48.101 1.6 L 42.588 11.148 L 48.101 20.696 L 59.126 20.696 L 64.638 11.148 L 59.126 1.6 L s 20.538 68.436 m S 26.051 58.888 m 15.025 58.888 L 9.513 68.436 L 15.025 77.984 L 26.051 77.984 L 31.564 68.436 L 26.051 58.888 L s 20.538 49.34 m S 26.051 39.792 m 15.025 39.792 L 9.513 49.34 L 15.025 58.888 L 26.05 58.888 L 31.564 49.34 L 26.051 39.792 L s 53.614 68.436 m S 59.127 58.888 m 48.102 58.888 L 42.589 68.436 L 48.101 77.985 L 59.127 77.985 L 64.639 68.436 L 59.127 58.888 L s 53.614 49.34 m S 59.127 39.792 m 48.101 39.792 L 42.589 49.34 L 48.101 58.888 L 59.127 58.888 L 64.639 49.341 L 59.127 39.792 L s 4 20.696 m S 3.876 30.244 m 9.512 30.244 L 15.024 20.696 L 9.512 11.147 L 3.876 11.147 L S 37.075 20.696 m S 42.588 11.148 m 31.563 11.148 L 26.05 20.696 L 31.563 30.244 L 42.589 30.244 L 48.101 20.696 L 42.588 11.148 L s 37.076 58.888 m S 42.589 49.34 m 31.564 49.34 L 26.05 58.888 L 31.564 68.436 L 42.589 68.436 L 48.101 58.888 L 42.589 49.34 L s 70.151 20.696 m S 70.2094 11.147 m 64.639 11.147 L 59.127 20.696 L 64.639 30.244 L 70.2094 30.244 L S 70.152 58.888 m S 70.0427 49.34 m 64.639 49.34 L 59.127 58.888 L 64.639 68.436 L 70.0427 68.436 L S 4 58.888 m S 3.876 68.436 m 9.513 68.436 L 15.025 58.888 L 9.513 49.34 L 3.876 49.34 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Sexh\232rning\012 4) (Sexh\232rning\012 4) 4 1.6 70.151 77.983 [ %AI3_Tile (0 O 0 R 0 1 0.35 0 k 0 1 0.35 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 70.151 77.983 m 70.151 1.6 L 4 1.6 L 4 77.983 L 70.151 77.983 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.9921 1 0 0 k 0.9921 1 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 20.538 30.244 m S 26.05 20.696 m 15.025 20.696 L 9.513 30.244 L 15.025 39.792 L 26.05 39.792 L 31.564 30.244 L 26.05 20.696 L s 20.537 11.148 m S 26.05 1.6 m 15.024 1.6 L 9.512 11.148 L 15.024 20.696 L 26.05 20.696 L 31.563 11.148 L 26.05 1.6 L s 53.614 30.244 m S 59.126 20.696 m 48.101 20.696 L 42.589 30.244 L 48.101 39.792 L 59.126 39.792 L 64.639 30.244 L 59.126 20.696 L s 53.614 11.148 m S 59.126 1.6 m 48.101 1.6 L 42.588 11.148 L 48.101 20.696 L 59.126 20.696 L 64.638 11.148 L 59.126 1.6 L s 20.538 68.436 m S 26.051 58.888 m 15.025 58.888 L 9.513 68.436 L 15.025 77.984 L 26.051 77.984 L 31.564 68.436 L 26.051 58.888 L s 20.538 49.34 m S 26.051 39.792 m 15.025 39.792 L 9.513 49.34 L 15.025 58.888 L 26.05 58.888 L 31.564 49.34 L 26.051 39.792 L s 53.614 68.436 m S 59.127 58.888 m 48.102 58.888 L 42.589 68.436 L 48.101 77.985 L 59.127 77.985 L 64.639 68.436 L 59.127 58.888 L s 53.614 49.34 m S 59.127 39.792 m 48.101 39.792 L 42.589 49.34 L 48.101 58.888 L 59.127 58.888 L 64.639 49.341 L 59.127 39.792 L s 4 20.696 m S 3.876 30.244 m 9.512 30.244 L 15.024 20.696 L 9.512 11.147 L 3.876 11.147 L S 37.075 20.696 m S 42.588 11.148 m 31.563 11.148 L 26.05 20.696 L 31.563 30.244 L 42.589 30.244 L 48.101 20.696 L 42.588 11.148 L s 37.076 58.888 m S 42.589 49.34 m 31.564 49.34 L 26.05 58.888 L 31.564 68.436 L 42.589 68.436 L 48.101 58.888 L 42.589 49.34 L s 70.151 20.696 m S 70.2094 11.147 m 64.639 11.147 L 59.127 20.696 L 64.639 30.244 L 70.2094 30.244 L S 70.152 58.888 m S 70.0427 49.34 m 64.639 49.34 L 59.127 58.888 L 64.639 68.436 L 70.0427 68.436 L S 4 58.888 m S 3.876 68.436 m 9.513 68.436 L 15.025 58.888 L 9.513 49.34 L 3.876 49.34 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Slumpm\212ssiga cirklar) (Slumpm\212ssiga cirklar) 4.365 3.849 51.13 57.85 [ %AI3_Tile (0 O 0 R 0 0.1125 0.45 0 k 0 0.1125 0.45 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.365 3.849 m 4.365 57.85 L 51.13 57.85 L 51.13 3.849 L 4.365 3.849 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.4 0.7 1 0 k 0.4 0.7 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 45.429 36.274 m 45.843 36.991 45.598 37.908 44.88 38.323 c 44.163 38.737 43.245 38.491 42.831 37.774 c 42.417 37.056 42.663 36.139 43.38 35.725 c 44.098 35.31 45.015 35.556 45.429 36.274 c s 44.179 27.926 m 43.765 28.643 42.848 28.889 42.13 28.475 c 41.413 28.06 41.167 27.143 41.581 26.425 c 41.995 25.708 42.913 25.462 43.63 25.876 c 44.348 26.291 44.593 27.208 44.179 27.926 c s 35.929 41.024 m 35.515 41.741 34.598 41.987 33.88 41.573 c 33.163 41.158 32.917 40.241 33.331 39.524 c 33.745 38.806 34.663 38.56 35.38 38.975 c 36.098 39.389 36.343 40.306 35.929 41.024 c s 28.38 34.225 m 28.794 34.942 28.549 35.859 27.831 36.274 c 27.114 36.688 26.196 36.442 25.782 35.725 c 25.368 35.007 25.614 34.09 26.331 33.675 c 27.049 33.261 27.966 33.507 28.38 34.225 c s 31.179 28.024 m 30.765 28.741 29.848 28.987 29.13 28.573 c 28.413 28.158 28.167 27.241 28.581 26.524 c 28.995 25.806 29.913 25.56 30.63 25.975 c 31.348 26.389 31.593 27.306 31.179 28.024 c s 36.792 23.349 m 35.963 23.349 35.292 22.678 35.292 21.849 c 35.292 21.021 35.963 20.349 36.792 20.349 c 37.62 20.349 38.292 21.021 38.292 21.849 c 38.292 22.678 37.62 23.349 36.792 23.349 c s 10.888 34.175 m 10.474 34.893 10.72 35.81 11.437 36.225 c 12.155 36.639 13.072 36.393 13.486 35.675 c 13.901 34.958 13.655 34.041 12.937 33.626 c 12.22 33.212 11.303 33.458 10.888 34.175 c s 11.517 26.601 m 11.931 27.318 12.848 27.564 13.566 27.15 c 14.283 26.735 14.529 25.818 14.115 25.1 c 13.701 24.383 12.783 24.137 12.066 24.551 c 11.348 24.966 11.103 25.883 11.517 26.601 c s 16.782 41.426 m 17.196 42.143 18.114 42.389 18.831 41.975 c 19.549 41.56 19.794 40.643 19.38 39.926 c 18.966 39.208 18.049 38.962 17.331 39.377 c 16.614 39.791 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3.849 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.4 0.7 1 0 k 0.4 0.7 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 45.429 36.274 m 45.843 36.991 45.598 37.908 44.88 38.323 c 44.163 38.737 43.245 38.491 42.831 37.774 c 42.417 37.056 42.663 36.139 43.38 35.725 c 44.098 35.31 45.015 35.556 45.429 36.274 c s 44.179 27.926 m 43.765 28.643 42.848 28.889 42.13 28.475 c 41.413 28.06 41.167 27.143 41.581 26.425 c 41.995 25.708 42.913 25.462 43.63 25.876 c 44.348 26.291 44.593 27.208 44.179 27.926 c s 35.929 41.024 m 35.515 41.741 34.598 41.987 33.88 41.573 c 33.163 41.158 32.917 40.241 33.331 39.524 c 33.745 38.806 34.663 38.56 35.38 38.975 c 36.098 39.389 36.343 40.306 35.929 41.024 c s 28.38 34.225 m 28.794 34.942 28.549 35.859 27.831 36.274 c 27.114 36.688 26.196 36.442 25.782 35.725 c 25.368 35.007 25.614 34.09 26.331 33.675 c 27.049 33.261 27.966 33.507 28.38 34.225 c s 31.179 28.024 m 30.765 28.741 29.848 28.987 29.13 28.573 c 28.413 28.158 28.167 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44.694 18.1 45.365 17.429 45.365 16.6 c 45.365 15.772 44.694 15.1 43.865 15.1 c 43.037 15.1 42.365 15.772 42.365 16.6 c 42.365 17.429 43.037 18.1 43.865 18.1 c s 51.13 4.6 m 50.302 4.6 49.63 3.928 49.63 3.1 c 49.63 2.272 50.302 1.6 51.13 1.6 c 51.959 1.6 52.63 2.272 52.63 3.1 c 52.63 3.928 51.959 4.6 51.13 4.6 c s 52.163 31.649 m 51.748 32.366 50.831 32.612 50.114 32.198 c 49.396 31.783 49.15 30.866 49.565 30.149 c 49.979 29.431 50.896 29.185 51.614 29.6 c 52.331 30.014 52.577 30.931 52.163 31.649 c s 51.85 51.35 m 51.021 51.35 50.35 50.678 50.35 49.85 c 50.35 49.021 51.021 48.35 51.85 48.35 c 52.678 48.35 53.35 49.021 53.35 49.85 c 53.35 50.678 52.678 51.35 51.85 51.35 c s 49.85 23.1 m 50.679 23.1 51.35 22.428 51.35 21.6 c 51.35 20.771 50.679 20.1 49.85 20.1 c 49.022 20.1 48.35 20.771 48.35 21.6 c 48.35 22.428 49.022 23.1 49.85 23.1 c s 5.13 38.85 m 4.302 38.85 3.63 39.521 3.63 40.35 c 3.63 41.178 4.302 41.85 5.13 41.85 c 5.959 41.85 6.63 41.178 6.63 40.35 c 6.63 39.521 5.959 38.85 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c s 38.944 59.275 m 38.53 59.992 37.613 60.238 36.895 59.824 c 36.178 59.409 35.932 58.492 36.346 57.775 c 36.76 57.058 37.678 56.812 38.395 57.226 c 39.113 57.64 39.358 58.557 38.944 59.275 c s 51.145 58.601 m 50.317 58.601 49.645 57.929 49.645 57.101 c 49.645 56.273 50.317 55.601 51.145 55.601 c 51.974 55.601 52.645 56.273 52.645 57.101 c 52.645 57.929 51.974 58.601 51.145 58.601 c s 4.395 58.601 m 3.567 58.601 2.895 57.929 2.895 57.101 c 2.895 56.273 3.567 55.601 4.395 55.601 c 5.224 55.601 5.895 56.273 5.895 57.101 c 5.895 57.929 5.224 58.601 4.395 58.601 c s %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Slumpm\212ssiga cirklar\012 3) (Slumpm\212ssiga cirklar\012 3) 4.365 3.849 51.13 57.85 [ %AI3_Tile (0 O 0 R 0 0.1125 0.45 0 k 0 0.1125 0.45 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.365 3.849 m 4.365 57.85 L 51.13 57.85 L 51.13 3.849 L 4.365 3.849 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.4 0.7 1 0 k 0.4 0.7 1 0 K ) @ ( 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12.015 46.241 11.098 46.487 10.38 46.073 c 9.663 45.658 9.417 44.741 9.831 44.024 c 10.245 43.306 11.163 43.06 11.88 43.475 c 12.598 43.889 12.843 44.806 12.429 45.524 c s 44.49 45.6 m 44.075 46.317 43.158 46.563 42.441 46.149 c 41.723 45.734 41.477 44.817 41.891 44.1 c 42.306 43.382 43.223 43.136 43.941 43.55 c 44.658 43.965 44.904 44.882 44.49 45.6 c s 12.679 18.524 m 12.265 19.241 11.348 19.487 10.63 19.073 c 9.913 18.658 9.667 17.741 10.081 17.024 c 10.495 16.306 11.413 16.06 12.13 16.475 c 12.848 16.889 13.093 17.806 12.679 18.524 c s 21.179 5.774 m 20.765 6.491 19.848 6.737 19.13 6.323 c 18.413 5.908 18.167 4.991 18.581 4.274 c 18.995 3.557 19.913 3.311 20.63 3.725 c 21.348 4.139 21.593 5.056 21.179 5.774 c s 38.929 5.274 m 38.515 5.991 37.598 6.237 36.88 5.823 c 36.163 5.408 35.917 4.491 36.331 3.774 c 36.745 3.057 37.663 2.811 38.38 3.225 c 39.098 3.639 39.343 4.556 38.929 5.274 c s 43.865 18.1 m 44.694 18.1 45.365 17.429 45.365 16.6 c 45.365 15.772 44.694 15.1 43.865 15.1 c 43.037 15.1 42.365 15.772 42.365 16.6 c 42.365 17.429 43.037 18.1 43.865 18.1 c s 51.13 4.6 m 50.302 4.6 49.63 3.928 49.63 3.1 c 49.63 2.272 50.302 1.6 51.13 1.6 c 51.959 1.6 52.63 2.272 52.63 3.1 c 52.63 3.928 51.959 4.6 51.13 4.6 c s 52.163 31.649 m 51.748 32.366 50.831 32.612 50.114 32.198 c 49.396 31.783 49.15 30.866 49.565 30.149 c 49.979 29.431 50.896 29.185 51.614 29.6 c 52.331 30.014 52.577 30.931 52.163 31.649 c s 51.85 51.35 m 51.021 51.35 50.35 50.678 50.35 49.85 c 50.35 49.021 51.021 48.35 51.85 48.35 c 52.678 48.35 53.35 49.021 53.35 49.85 c 53.35 50.678 52.678 51.35 51.85 51.35 c s 49.85 23.1 m 50.679 23.1 51.35 22.428 51.35 21.6 c 51.35 20.771 50.679 20.1 49.85 20.1 c 49.022 20.1 48.35 20.771 48.35 21.6 c 48.35 22.428 49.022 23.1 49.85 23.1 c s 5.13 38.85 m 4.302 38.85 3.63 39.521 3.63 40.35 c 3.63 41.178 4.302 41.85 5.13 41.85 c 5.959 41.85 6.63 41.178 6.63 40.35 c 6.63 39.521 5.959 38.85 5.13 38.85 c s 5.115 11.349 m 5.943 11.349 6.615 12.021 6.615 12.849 c 6.615 13.678 5.943 14.349 5.115 14.349 c 4.286 14.349 3.615 13.678 3.615 12.849 c 3.615 12.021 4.286 11.349 5.115 11.349 c s 4.38 4.6 m 3.552 4.6 2.88 3.928 2.88 3.1 c 2.88 2.272 3.552 1.6 4.38 1.6 c 5.209 1.6 5.88 2.272 5.88 3.1 c 5.88 3.928 5.209 4.6 4.38 4.6 c s 5.413 31.649 m 4.998 32.366 4.081 32.612 3.364 32.198 c 2.646 31.783 2.4 30.866 2.815 30.149 c 3.229 29.431 4.146 29.185 4.864 29.6 c 5.581 30.014 5.827 30.931 5.413 31.649 c s 5.1 51.35 m 4.271 51.35 3.6 50.678 3.6 49.85 c 3.6 49.021 4.271 48.35 5.1 48.35 c 5.928 48.35 6.6 49.021 6.6 49.85 c 6.6 50.678 5.928 51.35 5.1 51.35 c s 3.1 23.1 m 3.929 23.1 4.6 22.428 4.6 21.6 c 4.6 20.771 3.929 20.1 3.1 20.1 c 2.272 20.1 1.6 20.771 1.6 21.6 c 1.6 22.428 2.272 23.1 3.1 23.1 c s 21.194 59.775 m 20.78 60.492 19.863 60.738 19.145 60.324 c 18.428 59.909 18.182 58.992 18.596 58.275 c 19.01 57.558 19.928 57.312 20.645 57.726 c 21.363 58.14 21.608 59.057 21.194 59.775 c s 38.944 59.275 m 38.53 59.992 37.613 60.238 36.895 59.824 c 36.178 59.409 35.932 58.492 36.346 57.775 c 36.76 57.058 37.678 56.812 38.395 57.226 c 39.113 57.64 39.358 58.557 38.944 59.275 c s 51.145 58.601 m 50.317 58.601 49.645 57.929 49.645 57.101 c 49.645 56.273 50.317 55.601 51.145 55.601 c 51.974 55.601 52.645 56.273 52.645 57.101 c 52.645 57.929 51.974 58.601 51.145 58.601 c s 4.395 58.601 m 3.567 58.601 2.895 57.929 2.895 57.101 c 2.895 56.273 3.567 55.601 4.395 55.601 c 5.224 55.601 5.895 56.273 5.895 57.101 c 5.895 57.929 5.224 58.601 4.395 58.601 c s %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Slumpm\212ssiga cirklar\012 4) (Slumpm\212ssiga cirklar\012 4) 4.365 3.849 51.13 57.85 [ %AI3_Tile (0 O 0 R 0 0.1125 0.45 0 k 0 0.1125 0.45 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 4.365 3.849 m 4.365 57.85 L 51.13 57.85 L 51.13 3.849 L 4.365 3.849 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.4 0.7 1 0 k 0.4 0.7 1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 45.429 36.274 m 45.843 36.991 45.598 37.908 44.88 38.323 c 44.163 38.737 43.245 38.491 42.831 37.774 c 42.417 37.056 42.663 36.139 43.38 35.725 c 44.098 35.31 45.015 35.556 45.429 36.274 c s 44.179 27.926 m 43.765 28.643 42.848 28.889 42.13 28.475 c 41.413 28.06 41.167 27.143 41.581 26.425 c 41.995 25.708 42.913 25.462 43.63 25.876 c 44.348 26.291 44.593 27.208 44.179 27.926 c s 35.929 41.024 m 35.515 41.741 34.598 41.987 33.88 41.573 c 33.163 41.158 32.917 40.241 33.331 39.524 c 33.745 38.806 34.663 38.56 35.38 38.975 c 36.098 39.389 36.343 40.306 35.929 41.024 c s 28.38 34.225 m 28.794 34.942 28.549 35.859 27.831 36.274 c 27.114 36.688 26.196 36.442 25.782 35.725 c 25.368 35.007 25.614 34.09 26.331 33.675 c 27.049 33.261 27.966 33.507 28.38 34.225 c s 31.179 28.024 m 30.765 28.741 29.848 28.987 29.13 28.573 c 28.413 28.158 28.167 27.241 28.581 26.524 c 28.995 25.806 29.913 25.56 30.63 25.975 c 31.348 26.389 31.593 27.306 31.179 28.024 c s 36.792 23.349 m 35.963 23.349 35.292 22.678 35.292 21.849 c 35.292 21.021 35.963 20.349 36.792 20.349 c 37.62 20.349 38.292 21.021 38.292 21.849 c 38.292 22.678 37.62 23.349 36.792 23.349 c s 10.888 34.175 m 10.474 34.893 10.72 35.81 11.437 36.225 c 12.155 36.639 13.072 36.393 13.486 35.675 c 13.901 34.958 13.655 34.041 12.937 33.626 c 12.22 33.212 11.303 33.458 10.888 34.175 c s 11.517 26.601 m 11.931 27.318 12.848 27.564 13.566 27.15 c 14.283 26.735 14.529 25.818 14.115 25.1 c 13.701 24.383 12.783 24.137 12.066 24.551 c 11.348 24.966 11.103 25.883 11.517 26.601 c s 16.782 41.426 m 17.196 42.143 18.114 42.389 18.831 41.975 c 19.549 41.56 19.794 40.643 19.38 39.926 c 18.966 39.208 18.049 38.962 17.331 39.377 c 16.614 39.791 16.368 40.708 16.782 41.426 c s 22.365 24.35 m 23.194 24.35 23.865 23.678 23.865 22.85 c 23.865 22.021 23.194 21.35 22.365 21.35 c 21.537 21.35 20.865 22.021 20.865 22.85 c 20.865 23.678 21.537 24.35 22.365 24.35 c s 45.385 7.849 m 44.971 7.132 44.053 6.886 43.336 7.3 c 42.619 7.714 42.373 8.632 42.787 9.349 c 43.201 10.067 44.119 10.312 44.836 9.898 c 45.553 9.484 45.799 8.567 45.385 7.849 c s 29.679 7.774 m 29.265 7.056 28.348 6.81 27.63 7.225 c 26.913 7.639 26.667 8.556 27.081 9.274 c 27.495 9.991 28.413 10.237 29.13 9.823 c 29.848 9.408 30.093 8.491 29.679 7.774 c s 35.542 11.349 m 34.713 11.349 34.042 12.021 34.042 12.849 c 34.042 13.678 34.713 14.349 35.542 14.349 c 36.37 14.349 37.042 13.678 37.042 12.849 c 37.042 12.021 36.37 11.349 35.542 11.349 c s 10.13 7.475 m 10.544 6.757 11.462 6.511 12.179 6.926 c 12.897 7.34 13.142 8.257 12.728 8.975 c 12.314 9.692 11.397 9.938 10.679 9.524 c 9.962 9.109 9.716 8.192 10.13 7.475 c s 20.203 13.349 m 21.031 13.349 21.703 14.021 21.703 14.849 c 21.703 15.678 21.031 16.349 20.203 16.349 c 19.375 16.349 18.703 15.678 18.703 14.849 c 18.703 14.021 19.375 13.349 20.203 13.349 c s 44.635 54.1 m 45.049 53.382 44.803 52.465 44.086 52.051 c 43.369 51.636 42.451 51.882 42.037 52.6 c 41.623 53.317 41.869 54.234 42.586 54.649 c 43.303 55.063 44.221 54.817 44.635 54.1 c s 36.841 48.1 m 36.427 47.382 35.509 47.136 34.792 47.551 c 34.074 47.965 33.828 48.882 34.243 49.6 c 34.657 50.317 35.574 50.563 36.292 50.149 c 37.009 49.734 37.255 48.817 36.841 48.1 c s 29.728 54.725 m 30.143 54.007 29.897 53.09 29.179 52.675 c 28.462 52.261 27.544 52.507 27.13 53.225 c 26.716 53.942 26.962 54.859 27.679 55.274 c 28.397 55.688 29.314 55.442 29.728 54.725 c s 10.86 54.1 m 10.446 53.382 10.691 52.465 11.409 52.051 c 12.126 51.636 13.044 51.882 13.458 52.6 c 13.872 53.317 13.626 54.234 12.909 54.649 c 12.191 55.063 11.274 54.817 10.86 54.1 c s 19.154 49.1 m 19.568 48.382 20.486 48.136 21.203 48.551 c 21.92 48.965 22.166 49.882 21.752 50.6 c 21.338 51.317 20.42 51.563 19.703 51.149 c 18.986 50.734 18.74 49.817 19.154 49.1 c s 51.88 38.85 m 51.052 38.85 50.38 39.521 50.38 40.35 c 50.38 41.178 51.052 41.85 51.88 41.85 c 52.709 41.85 53.38 41.178 53.38 40.35 c 53.38 39.521 52.709 38.85 51.88 38.85 c s 51.865 11.349 m 52.693 11.349 53.365 12.021 53.365 12.849 c 53.365 13.678 52.693 14.349 51.865 14.349 c 51.036 14.349 50.365 13.678 50.365 12.849 c 50.365 12.021 51.036 11.349 51.865 11.349 c s 30.179 18.524 m 29.765 19.241 28.848 19.487 28.13 19.073 c 27.413 18.658 27.167 17.741 27.581 17.024 c 27.995 16.306 28.913 16.06 29.63 16.475 c 30.348 16.889 30.593 17.806 30.179 18.524 c s 21.679 31.524 m 21.265 32.241 20.348 32.487 19.63 32.073 c 18.913 31.658 18.667 30.741 19.081 30.024 c 19.495 29.306 20.413 29.06 21.13 29.475 c 21.848 29.889 22.093 30.806 21.679 31.524 c s 37.914 33.399 m 37.5 34.116 36.583 34.362 35.865 33.948 c 35.148 33.533 34.902 32.616 35.316 31.899 c 35.73 31.181 36.648 30.935 37.365 31.35 c 38.083 31.764 38.328 32.681 37.914 33.399 c s 28.929 45.024 m 28.515 45.741 27.598 45.987 26.88 45.573 c 26.163 45.158 25.917 44.241 26.331 43.524 c 26.745 42.806 27.663 42.56 28.38 42.975 c 29.098 43.389 29.343 44.306 28.929 45.024 c s 12.429 45.524 m 12.015 46.241 11.098 46.487 10.38 46.073 c 9.663 45.658 9.417 44.741 9.831 44.024 c 10.245 43.306 11.163 43.06 11.88 43.475 c 12.598 43.889 12.843 44.806 12.429 45.524 c s 44.49 45.6 m 44.075 46.317 43.158 46.563 42.441 46.149 c 41.723 45.734 41.477 44.817 41.891 44.1 c 42.306 43.382 43.223 43.136 43.941 43.55 c 44.658 43.965 44.904 44.882 44.49 45.6 c s 12.679 18.524 m 12.265 19.241 11.348 19.487 10.63 19.073 c 9.913 18.658 9.667 17.741 10.081 17.024 c 10.495 16.306 11.413 16.06 12.13 16.475 c 12.848 16.889 13.093 17.806 12.679 18.524 c s 21.179 5.774 m 20.765 6.491 19.848 6.737 19.13 6.323 c 18.413 5.908 18.167 4.991 18.581 4.274 c 18.995 3.557 19.913 3.311 20.63 3.725 c 21.348 4.139 21.593 5.056 21.179 5.774 c s 38.929 5.274 m 38.515 5.991 37.598 6.237 36.88 5.823 c 36.163 5.408 35.917 4.491 36.331 3.774 c 36.745 3.057 37.663 2.811 38.38 3.225 c 39.098 3.639 39.343 4.556 38.929 5.274 c s 43.865 18.1 m 44.694 18.1 45.365 17.429 45.365 16.6 c 45.365 15.772 44.694 15.1 43.865 15.1 c 43.037 15.1 42.365 15.772 42.365 16.6 c 42.365 17.429 43.037 18.1 43.865 18.1 c s 51.13 4.6 m 50.302 4.6 49.63 3.928 49.63 3.1 c 49.63 2.272 50.302 1.6 51.13 1.6 c 51.959 1.6 52.63 2.272 52.63 3.1 c 52.63 3.928 51.959 4.6 51.13 4.6 c s 52.163 31.649 m 51.748 32.366 50.831 32.612 50.114 32.198 c 49.396 31.783 49.15 30.866 49.565 30.149 c 49.979 29.431 50.896 29.185 51.614 29.6 c 52.331 30.014 52.577 30.931 52.163 31.649 c s 51.85 51.35 m 51.021 51.35 50.35 50.678 50.35 49.85 c 50.35 49.021 51.021 48.35 51.85 48.35 c 52.678 48.35 53.35 49.021 53.35 49.85 c 53.35 50.678 52.678 51.35 51.85 51.35 c s 49.85 23.1 m 50.679 23.1 51.35 22.428 51.35 21.6 c 51.35 20.771 50.679 20.1 49.85 20.1 c 49.022 20.1 48.35 20.771 48.35 21.6 c 48.35 22.428 49.022 23.1 49.85 23.1 c s 5.13 38.85 m 4.302 38.85 3.63 39.521 3.63 40.35 c 3.63 41.178 4.302 41.85 5.13 41.85 c 5.959 41.85 6.63 41.178 6.63 40.35 c 6.63 39.521 5.959 38.85 5.13 38.85 c s 5.115 11.349 m 5.943 11.349 6.615 12.021 6.615 12.849 c 6.615 13.678 5.943 14.349 5.115 14.349 c 4.286 14.349 3.615 13.678 3.615 12.849 c 3.615 12.021 4.286 11.349 5.115 11.349 c s 4.38 4.6 m 3.552 4.6 2.88 3.928 2.88 3.1 c 2.88 2.272 3.552 1.6 4.38 1.6 c 5.209 1.6 5.88 2.272 5.88 3.1 c 5.88 3.928 5.209 4.6 4.38 4.6 c s 5.413 31.649 m 4.998 32.366 4.081 32.612 3.364 32.198 c 2.646 31.783 2.4 30.866 2.815 30.149 c 3.229 29.431 4.146 29.185 4.864 29.6 c 5.581 30.014 5.827 30.931 5.413 31.649 c s 5.1 51.35 m 4.271 51.35 3.6 50.678 3.6 49.85 c 3.6 49.021 4.271 48.35 5.1 48.35 c 5.928 48.35 6.6 49.021 6.6 49.85 c 6.6 50.678 5.928 51.35 5.1 51.35 c s 3.1 23.1 m 3.929 23.1 4.6 22.428 4.6 21.6 c 4.6 20.771 3.929 20.1 3.1 20.1 c 2.272 20.1 1.6 20.771 1.6 21.6 c 1.6 22.428 2.272 23.1 3.1 23.1 c s 21.194 59.775 m 20.78 60.492 19.863 60.738 19.145 60.324 c 18.428 59.909 18.182 58.992 18.596 58.275 c 19.01 57.558 19.928 57.312 20.645 57.726 c 21.363 58.14 21.608 59.057 21.194 59.775 c s 38.944 59.275 m 38.53 59.992 37.613 60.238 36.895 59.824 c 36.178 59.409 35.932 58.492 36.346 57.775 c 36.76 57.058 37.678 56.812 38.395 57.226 c 39.113 57.64 39.358 58.557 38.944 59.275 c s 51.145 58.601 m 50.317 58.601 49.645 57.929 49.645 57.101 c 49.645 56.273 50.317 55.601 51.145 55.601 c 51.974 55.601 52.645 56.273 52.645 57.101 c 52.645 57.929 51.974 58.601 51.145 58.601 c s 4.395 58.601 m 3.567 58.601 2.895 57.929 2.895 57.101 c 2.895 56.273 3.567 55.601 4.395 55.601 c 5.224 55.601 5.895 56.273 5.895 57.101 c 5.895 57.929 5.224 58.601 4.395 58.601 c s %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor) (Stj\212rnor) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 1) (Stj\212rnor\012 1) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 2) (Stj\212rnor\012 2) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 3) (Stj\212rnor\012 3) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 4) (Stj\212rnor\012 4) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 5) (Stj\212rnor\012 5) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 6) (Stj\212rnor\012 6) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 7) (Stj\212rnor\012 7) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 8) (Stj\212rnor\012 8) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 9) (Stj\212rnor\012 9) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 10) (Stj\212rnor\012 10) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Stj\212rnor\012 11) (Stj\212rnor\012 11) 1 1 63.384 84.766 [ %AI3_Tile (0 O 0 R 1 0.9 0.1 0 k 1 0.9 0.1 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1 1 m 1 84.766 L 63.384 84.766 L 63.384 1 L 1 1 L f %AI6_EndPatternLayer ) & (0 O 0 R 0 0.25 1 0 k 0 0.25 1 0 K ) @ ( %AI6_BeginPatternLayer *u 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 37.668 67.113 m 43.924 62.567 L 41.535 55.213 L 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L f 16.596 59.757 m 22.851 55.212 L 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L f 20.462 20.683 m 26.719 25.229 L 18.985 25.229 L 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L f 38.447 34.271 m 36.058 41.625 L 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L f 51.657 20.683 m 57.914 25.229 L 50.18 25.229 L 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L f *U 34.581 4.288 m 32.192 11.643 L 29.803 4.289 L 22.069 4.289 L 26.5962 1 L 37.7885 1 L 42.315 4.288 L 34.581 4.288 L f 53.261 4.289 m 57.7882 1 L 63.384 1 L 63.384 11.643 L 60.995 4.289 L 53.261 4.289 L f 4.866 41.625 m 11.123 46.171 L 3.389 46.171 L 1 53.526 L 1 38.816 L 7.255 34.271 L 4.866 41.625 L f 36.058 41.625 m 42.315 46.171 L 34.581 46.171 L 32.192 53.526 L 29.803 46.172 L 22.069 46.172 L 28.325 41.626 L 25.936 34.272 L 32.192 38.816 L 38.447 34.271 L 36.058 41.625 L f 53.261 46.172 m 59.517 41.626 L 57.128 34.272 L 63.384 38.816 L 63.384 53.526 L 60.995 46.172 L 53.261 46.172 L f 4.866 83.508 m 6.5974 84.766 L 1 84.766 L 1 80.699 L 7.255 76.154 L 4.866 83.508 L f 25.936 76.155 m 32.192 80.699 L 38.447 76.154 L 36.058 83.508 L 37.7895 84.766 L 26.5951 84.766 L 28.325 83.509 L 25.936 76.155 L f 22.851 55.212 m 20.462 62.566 L 26.719 67.112 L 18.985 67.112 L 16.596 74.467 L 14.207 67.113 L 6.473 67.113 L 12.729 62.567 L 10.34 55.213 L 16.596 59.757 L 22.851 55.212 L f 41.535 55.213 m 47.791 59.757 L 54.046 55.212 L 51.657 62.566 L 57.914 67.112 L 50.18 67.112 L 47.791 74.467 L 45.402 67.113 L 37.668 67.113 L 43.924 62.567 L 41.535 55.213 L f 50.18 25.229 m 47.791 32.584 L 45.402 25.23 L 37.668 25.23 L 43.924 20.684 L 41.535 13.33 L 47.791 17.874 L 54.046 13.329 L 51.657 20.683 L 57.914 25.229 L 50.18 25.229 L f 18.985 25.229 m 16.596 32.584 L 14.207 25.23 L 6.473 25.23 L 12.729 20.684 L 10.34 13.33 L 16.596 17.874 L 22.851 13.329 L 20.462 20.683 L 26.719 25.229 L 18.985 25.229 L f 3.388 4.289 m 1 11.643 L 1 1 L 6.5948 1 L 11.122 4.289 L 3.388 4.289 L f 57.128 76.154 m 63.384 80.699 L 63.384 84.766 L 57.7855 84.766 L 59.517 83.508 L 57.128 76.154 L f %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Tegelv\212gg\012 1) (Tegelv\212gg\012 1) 1.6 1.6 73.6 73.6 [ %AI3_Tile (0 O 0 R 0.3 0.85 0.85 0 k 0.3 0.85 0.85 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 1.6 m 1.6 73.6 L 73.6 73.6 L 73.6 1.6 L 1.6 1.6 L f %AI6_EndPatternLayer ) & (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 70.01 m 73.6 70.01 l S 1.6 62.809 m 73.6 62.809 L S 1.6 55.609 m 73.6 55.609 L S 1.6 48.408 m 73.6 48.408 L S 1.6 41.208 m 73.6 41.208 L S 1.6 34.007 m 73.6 34.007 L S 1.6 26.807 m 73.6 26.807 L S 1.6 19.606 m 73.6 19.606 L S 1.6 12.406 m 73.6 12.406 L S 1.6 5.206 m 73.6 5.206 L S 70.01 70.01 m 70.01 62.822 l S 55.61 70.01 m 55.61 62.822 L S 41.21 70.01 m 41.21 62.822 L S 26.81 70.01 m 26.81 62.822 L S 12.41 70.01 m 12.41 62.822 L S 70.01 55.572 m 70.01 48.385 l S 55.61 55.572 m 55.61 48.385 L S 41.21 55.572 m 41.21 48.385 L S 26.81 55.572 m 26.81 48.385 L S 12.41 55.572 m 12.41 48.385 L S 70.01 41.197 m 70.01 34.01 l S 55.61 41.197 m 55.61 34.01 L S 41.21 41.197 m 41.21 34.01 L S 26.81 41.197 m 26.81 34.01 L S 12.41 41.197 m 12.41 34.01 L S 70.01 26.822 m 70.01 19.635 l S 55.61 26.822 m 55.61 19.635 L S 41.21 26.822 m 41.21 19.635 L S 26.81 26.822 m 26.81 19.635 L S 12.41 26.822 m 12.41 19.635 L S 70.01 12.385 m 70.01 5.197 l S 55.61 12.385 m 55.61 5.197 L S 41.21 12.385 m 41.21 5.197 L S 26.81 12.385 m 26.81 5.197 L S 12.41 12.385 m 12.41 5.197 L S 62.797 5.197 m 62.797 1.6 L S 48.397 5.197 m 48.397 1.6 L S 33.997 5.197 m 33.997 1.6 L S 19.597 5.197 m 19.597 1.6 L S 5.197 5.197 m 5.197 1.6 l S 62.797 19.635 m 62.797 12.447 L S 48.397 19.635 m 48.397 12.447 L S 33.997 19.635 m 33.997 12.447 L S 19.597 19.635 m 19.597 12.447 L S 5.197 19.635 m 5.197 12.447 l S 62.797 34.01 m 62.797 26.822 L S 48.397 34.01 m 48.397 26.822 L S 19.597 34.01 m 19.597 26.822 L S 5.197 34.01 m 5.197 26.822 l S 62.797 48.385 m 62.797 41.197 L S 48.397 48.385 m 48.397 41.197 L S 33.997 48.385 m 33.997 41.197 L S 19.597 48.385 m 19.597 41.197 L S 5.197 48.385 m 5.197 41.197 l S 62.797 62.822 m 62.797 55.635 L S 48.397 62.822 m 48.397 55.635 L S 33.997 62.822 m 33.997 55.635 L S 19.597 62.822 m 19.597 55.635 L S 5.197 62.822 m 5.197 55.635 l S 62.797 73.5589 m 62.797 70.072 L S 48.397 73.5589 m 48.397 70.072 L S 33.997 73.5589 m 33.997 70.072 L S 19.597 73.5589 m 19.597 70.072 L S 5.197 73.5589 m 5.197 70.072 l S 33.997 34.01 m 33.997 26.822 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Tegelv\212gg\012 2) (Tegelv\212gg\012 2) 1.6 1.6 73.6 73.6 [ %AI3_Tile (0 O 0 R 0.3 0.85 0.85 0 k 0.3 0.85 0.85 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 1.6 m 1.6 73.6 L 73.6 73.6 L 73.6 1.6 L 1.6 1.6 L f %AI6_EndPatternLayer ) & (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 70.01 m 73.6 70.01 l S 1.6 62.809 m 73.6 62.809 L S 1.6 55.609 m 73.6 55.609 L S 1.6 48.408 m 73.6 48.408 L S 1.6 41.208 m 73.6 41.208 L S 1.6 34.007 m 73.6 34.007 L S 1.6 26.807 m 73.6 26.807 L S 1.6 19.606 m 73.6 19.606 L S 1.6 12.406 m 73.6 12.406 L S 1.6 5.206 m 73.6 5.206 L S 70.01 70.01 m 70.01 62.822 l S 55.61 70.01 m 55.61 62.822 L S 41.21 70.01 m 41.21 62.822 L S 26.81 70.01 m 26.81 62.822 L S 12.41 70.01 m 12.41 62.822 L S 70.01 55.572 m 70.01 48.385 l S 55.61 55.572 m 55.61 48.385 L S 41.21 55.572 m 41.21 48.385 L S 26.81 55.572 m 26.81 48.385 L S 12.41 55.572 m 12.41 48.385 L S 70.01 41.197 m 70.01 34.01 l S 55.61 41.197 m 55.61 34.01 L S 41.21 41.197 m 41.21 34.01 L S 26.81 41.197 m 26.81 34.01 L S 12.41 41.197 m 12.41 34.01 L S 70.01 26.822 m 70.01 19.635 l S 55.61 26.822 m 55.61 19.635 L S 41.21 26.822 m 41.21 19.635 L S 26.81 26.822 m 26.81 19.635 L S 12.41 26.822 m 12.41 19.635 L S 70.01 12.385 m 70.01 5.197 l S 55.61 12.385 m 55.61 5.197 L S 41.21 12.385 m 41.21 5.197 L S 26.81 12.385 m 26.81 5.197 L S 12.41 12.385 m 12.41 5.197 L S 62.797 5.197 m 62.797 1.6 L S 48.397 5.197 m 48.397 1.6 L S 33.997 5.197 m 33.997 1.6 L S 19.597 5.197 m 19.597 1.6 L S 5.197 5.197 m 5.197 1.6 l S 62.797 19.635 m 62.797 12.447 L S 48.397 19.635 m 48.397 12.447 L S 33.997 19.635 m 33.997 12.447 L S 19.597 19.635 m 19.597 12.447 L S 5.197 19.635 m 5.197 12.447 l S 62.797 34.01 m 62.797 26.822 L S 48.397 34.01 m 48.397 26.822 L S 19.597 34.01 m 19.597 26.822 L S 5.197 34.01 m 5.197 26.822 l S 62.797 48.385 m 62.797 41.197 L S 48.397 48.385 m 48.397 41.197 L S 33.997 48.385 m 33.997 41.197 L S 19.597 48.385 m 19.597 41.197 L S 5.197 48.385 m 5.197 41.197 l S 62.797 62.822 m 62.797 55.635 L S 48.397 62.822 m 48.397 55.635 L S 33.997 62.822 m 33.997 55.635 L S 19.597 62.822 m 19.597 55.635 L S 5.197 62.822 m 5.197 55.635 l S 62.797 73.5589 m 62.797 70.072 L S 48.397 73.5589 m 48.397 70.072 L S 33.997 73.5589 m 33.997 70.072 L S 19.597 73.5589 m 19.597 70.072 L S 5.197 73.5589 m 5.197 70.072 l S 33.997 34.01 m 33.997 26.822 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Tegelv\212gg\012 3) (Tegelv\212gg\012 3) 1.6 1.6 73.6 73.6 [ %AI3_Tile (0 O 0 R 0.3 0.85 0.85 0 k 0.3 0.85 0.85 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 1.6 m 1.6 73.6 L 73.6 73.6 L 73.6 1.6 L 1.6 1.6 L f %AI6_EndPatternLayer ) & (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 70.01 m 73.6 70.01 l S 1.6 62.809 m 73.6 62.809 L S 1.6 55.609 m 73.6 55.609 L S 1.6 48.408 m 73.6 48.408 L S 1.6 41.208 m 73.6 41.208 L S 1.6 34.007 m 73.6 34.007 L S 1.6 26.807 m 73.6 26.807 L S 1.6 19.606 m 73.6 19.606 L S 1.6 12.406 m 73.6 12.406 L S 1.6 5.206 m 73.6 5.206 L S 70.01 70.01 m 70.01 62.822 l S 55.61 70.01 m 55.61 62.822 L S 41.21 70.01 m 41.21 62.822 L S 26.81 70.01 m 26.81 62.822 L S 12.41 70.01 m 12.41 62.822 L S 70.01 55.572 m 70.01 48.385 l S 55.61 55.572 m 55.61 48.385 L S 41.21 55.572 m 41.21 48.385 L S 26.81 55.572 m 26.81 48.385 L S 12.41 55.572 m 12.41 48.385 L S 70.01 41.197 m 70.01 34.01 l S 55.61 41.197 m 55.61 34.01 L S 41.21 41.197 m 41.21 34.01 L S 26.81 41.197 m 26.81 34.01 L S 12.41 41.197 m 12.41 34.01 L S 70.01 26.822 m 70.01 19.635 l S 55.61 26.822 m 55.61 19.635 L S 41.21 26.822 m 41.21 19.635 L S 26.81 26.822 m 26.81 19.635 L S 12.41 26.822 m 12.41 19.635 L S 70.01 12.385 m 70.01 5.197 l S 55.61 12.385 m 55.61 5.197 L S 41.21 12.385 m 41.21 5.197 L S 26.81 12.385 m 26.81 5.197 L S 12.41 12.385 m 12.41 5.197 L S 62.797 5.197 m 62.797 1.6 L S 48.397 5.197 m 48.397 1.6 L S 33.997 5.197 m 33.997 1.6 L S 19.597 5.197 m 19.597 1.6 L S 5.197 5.197 m 5.197 1.6 l S 62.797 19.635 m 62.797 12.447 L S 48.397 19.635 m 48.397 12.447 L S 33.997 19.635 m 33.997 12.447 L S 19.597 19.635 m 19.597 12.447 L S 5.197 19.635 m 5.197 12.447 l S 62.797 34.01 m 62.797 26.822 L S 48.397 34.01 m 48.397 26.822 L S 19.597 34.01 m 19.597 26.822 L S 5.197 34.01 m 5.197 26.822 l S 62.797 48.385 m 62.797 41.197 L S 48.397 48.385 m 48.397 41.197 L S 33.997 48.385 m 33.997 41.197 L S 19.597 48.385 m 19.597 41.197 L S 5.197 48.385 m 5.197 41.197 l S 62.797 62.822 m 62.797 55.635 L S 48.397 62.822 m 48.397 55.635 L S 33.997 62.822 m 33.997 55.635 L S 19.597 62.822 m 19.597 55.635 L S 5.197 62.822 m 5.197 55.635 l S 62.797 73.5589 m 62.797 70.072 L S 48.397 73.5589 m 48.397 70.072 L S 33.997 73.5589 m 33.997 70.072 L S 19.597 73.5589 m 19.597 70.072 L S 5.197 73.5589 m 5.197 70.072 l S 33.997 34.01 m 33.997 26.822 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Tegelv\212gg\012 4) (Tegelv\212gg\012 4) 1.6 1.6 73.6 73.6 [ %AI3_Tile (0 O 0 R 0.3 0.85 0.85 0 k 0.3 0.85 0.85 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 1.6 m 1.6 73.6 L 73.6 73.6 L 73.6 1.6 L 1.6 1.6 L f %AI6_EndPatternLayer ) & (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 70.01 m 73.6 70.01 l S 1.6 62.809 m 73.6 62.809 L S 1.6 55.609 m 73.6 55.609 L S 1.6 48.408 m 73.6 48.408 L S 1.6 41.208 m 73.6 41.208 L S 1.6 34.007 m 73.6 34.007 L S 1.6 26.807 m 73.6 26.807 L S 1.6 19.606 m 73.6 19.606 L S 1.6 12.406 m 73.6 12.406 L S 1.6 5.206 m 73.6 5.206 L S 70.01 70.01 m 70.01 62.822 l S 55.61 70.01 m 55.61 62.822 L S 41.21 70.01 m 41.21 62.822 L S 26.81 70.01 m 26.81 62.822 L S 12.41 70.01 m 12.41 62.822 L S 70.01 55.572 m 70.01 48.385 l S 55.61 55.572 m 55.61 48.385 L S 41.21 55.572 m 41.21 48.385 L S 26.81 55.572 m 26.81 48.385 L S 12.41 55.572 m 12.41 48.385 L S 70.01 41.197 m 70.01 34.01 l S 55.61 41.197 m 55.61 34.01 L S 41.21 41.197 m 41.21 34.01 L S 26.81 41.197 m 26.81 34.01 L S 12.41 41.197 m 12.41 34.01 L S 70.01 26.822 m 70.01 19.635 l S 55.61 26.822 m 55.61 19.635 L S 41.21 26.822 m 41.21 19.635 L S 26.81 26.822 m 26.81 19.635 L S 12.41 26.822 m 12.41 19.635 L S 70.01 12.385 m 70.01 5.197 l S 55.61 12.385 m 55.61 5.197 L S 41.21 12.385 m 41.21 5.197 L S 26.81 12.385 m 26.81 5.197 L S 12.41 12.385 m 12.41 5.197 L S 62.797 5.197 m 62.797 1.6 L S 48.397 5.197 m 48.397 1.6 L S 33.997 5.197 m 33.997 1.6 L S 19.597 5.197 m 19.597 1.6 L S 5.197 5.197 m 5.197 1.6 l S 62.797 19.635 m 62.797 12.447 L S 48.397 19.635 m 48.397 12.447 L S 33.997 19.635 m 33.997 12.447 L S 19.597 19.635 m 19.597 12.447 L S 5.197 19.635 m 5.197 12.447 l S 62.797 34.01 m 62.797 26.822 L S 48.397 34.01 m 48.397 26.822 L S 19.597 34.01 m 19.597 26.822 L S 5.197 34.01 m 5.197 26.822 l S 62.797 48.385 m 62.797 41.197 L S 48.397 48.385 m 48.397 41.197 L S 33.997 48.385 m 33.997 41.197 L S 19.597 48.385 m 19.597 41.197 L S 5.197 48.385 m 5.197 41.197 l S 62.797 62.822 m 62.797 55.635 L S 48.397 62.822 m 48.397 55.635 L S 33.997 62.822 m 33.997 55.635 L S 19.597 62.822 m 19.597 55.635 L S 5.197 62.822 m 5.197 55.635 l S 62.797 73.5589 m 62.797 70.072 L S 48.397 73.5589 m 48.397 70.072 L S 33.997 73.5589 m 33.997 70.072 L S 19.597 73.5589 m 19.597 70.072 L S 5.197 73.5589 m 5.197 70.072 l S 33.997 34.01 m 33.997 26.822 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (Tegelv\212gg\012 5) (Tegelv\212gg\012 5) 1.6 1.6 73.6 73.6 [ %AI3_Tile (0 O 0 R 0.3 0.85 0.85 0 k 0.3 0.85 0.85 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 1.6 m 1.6 73.6 L 73.6 73.6 L 73.6 1.6 L 1.6 1.6 L f %AI6_EndPatternLayer ) & (0 O 0 R 1 g 1 G ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.3 w 4 M []0 d %AI3_Note: 0 D 0 XR 1.6 70.01 m 73.6 70.01 l S 1.6 62.809 m 73.6 62.809 L S 1.6 55.609 m 73.6 55.609 L S 1.6 48.408 m 73.6 48.408 L S 1.6 41.208 m 73.6 41.208 L S 1.6 34.007 m 73.6 34.007 L S 1.6 26.807 m 73.6 26.807 L S 1.6 19.606 m 73.6 19.606 L S 1.6 12.406 m 73.6 12.406 L S 1.6 5.206 m 73.6 5.206 L S 70.01 70.01 m 70.01 62.822 l S 55.61 70.01 m 55.61 62.822 L S 41.21 70.01 m 41.21 62.822 L S 26.81 70.01 m 26.81 62.822 L S 12.41 70.01 m 12.41 62.822 L S 70.01 55.572 m 70.01 48.385 l S 55.61 55.572 m 55.61 48.385 L S 41.21 55.572 m 41.21 48.385 L S 26.81 55.572 m 26.81 48.385 L S 12.41 55.572 m 12.41 48.385 L S 70.01 41.197 m 70.01 34.01 l S 55.61 41.197 m 55.61 34.01 L S 41.21 41.197 m 41.21 34.01 L S 26.81 41.197 m 26.81 34.01 L S 12.41 41.197 m 12.41 34.01 L S 70.01 26.822 m 70.01 19.635 l S 55.61 26.822 m 55.61 19.635 L S 41.21 26.822 m 41.21 19.635 L S 26.81 26.822 m 26.81 19.635 L S 12.41 26.822 m 12.41 19.635 L S 70.01 12.385 m 70.01 5.197 l S 55.61 12.385 m 55.61 5.197 L S 41.21 12.385 m 41.21 5.197 L S 26.81 12.385 m 26.81 5.197 L S 12.41 12.385 m 12.41 5.197 L S 62.797 5.197 m 62.797 1.6 L S 48.397 5.197 m 48.397 1.6 L S 33.997 5.197 m 33.997 1.6 L S 19.597 5.197 m 19.597 1.6 L S 5.197 5.197 m 5.197 1.6 l S 62.797 19.635 m 62.797 12.447 L S 48.397 19.635 m 48.397 12.447 L S 33.997 19.635 m 33.997 12.447 L S 19.597 19.635 m 19.597 12.447 L S 5.197 19.635 m 5.197 12.447 l S 62.797 34.01 m 62.797 26.822 L S 48.397 34.01 m 48.397 26.822 L S 19.597 34.01 m 19.597 26.822 L S 5.197 34.01 m 5.197 26.822 l S 62.797 48.385 m 62.797 41.197 L S 48.397 48.385 m 48.397 41.197 L S 33.997 48.385 m 33.997 41.197 L S 19.597 48.385 m 19.597 41.197 L S 5.197 48.385 m 5.197 41.197 l S 62.797 62.822 m 62.797 55.635 L S 48.397 62.822 m 48.397 55.635 L S 33.997 62.822 m 33.997 55.635 L S 19.597 62.822 m 19.597 55.635 L S 5.197 62.822 m 5.197 55.635 l S 62.797 73.5589 m 62.797 70.072 L S 48.397 73.5589 m 48.397 70.072 L S 33.997 73.5589 m 33.997 70.072 L S 19.597 73.5589 m 19.597 70.072 L S 5.197 73.5589 m 5.197 70.072 l S 33.997 34.01 m 33.997 26.822 L S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (V\214gor-genomskinliga) (V\214gor-genomskinliga) 17.926 10.516 68.663 69.012 [ %AI3_Tile (0 O 0 R 1 0 0.3 0 k 1 0 0.3 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 17.926 69.012 m 17.926 10.516 L 68.663 10.516 L 68.663 69.012 L 17.926 69.012 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.55 0 0 0 k 0.55 0 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.75 w 4 M []0 d %AI3_Note: 0 D 0 XR 65.335 70.465 m 65.881 68.746 67.444 68.168 68.663 69.012 C 67.538 69.668 68.011 71.255 69.686 70.933 c 72.124 70.464 71.894 67.213 70.53 65.589 c 68.561 63.245 64.565 60.995 53.241 71.117 C S 39.964 70.465 m 40.511 68.746 42.074 68.168 43.293 69.012 C 42.168 69.668 42.64 71.255 44.316 70.933 c 46.753 70.464 46.524 67.213 45.16 65.589 c 43.191 63.245 39.195 60.995 27.87 71.117 c S 14.594 70.465 m 15.141 68.746 16.704 68.168 17.923 69.012 C 16.798 69.668 17.27 71.255 18.945 70.933 c 21.382 70.464 21.153 67.213 19.789 65.589 c 17.821 63.245 13.825 60.995 2.5 71.117 c S 10.959 51.619 m 22.282 41.497 26.278 43.747 28.247 46.09 c 29.611 47.715 29.841 50.965 27.403 51.434 c 25.728 51.757 25.255 50.169 26.38 49.513 C 25.161 48.669 23.599 49.248 23.052 50.966 c 22.723 51.997 23.38 53.966 24.872 54.903 c 27.267 56.406 31.371 56.05 36.328 51.619 c 47.653 41.497 51.649 43.746 53.618 46.09 c 54.982 47.715 55.212 50.965 52.774 51.434 c 51.099 51.757 50.626 50.169 51.751 49.513 C 50.532 48.669 48.97 49.248 48.423 50.966 c 48.094 51.997 48.751 53.966 50.243 54.903 c 52.638 56.406 56.742 56.05 61.699 51.619 C 73.024 41.497 77.02 43.747 78.988 46.09 c S 70.156 32.12 m 65.199 36.551 61.095 36.907 58.7 35.404 c 57.208 34.468 56.552 32.499 56.88 31.468 c 57.427 29.749 58.99 29.171 60.208 30.015 C 59.083 30.671 59.556 32.258 61.231 31.936 c 63.669 31.467 63.439 28.216 62.075 26.592 c 60.106 24.248 56.11 21.998 44.786 32.12 C 39.829 36.551 35.725 36.907 33.33 35.404 c 31.838 34.468 31.182 32.499 31.51 31.468 c 32.056 29.749 33.619 29.171 34.838 30.015 C 33.713 30.671 34.186 32.258 35.861 31.936 c 38.299 31.467 38.069 28.216 36.705 26.592 c 34.737 24.248 30.74 21.998 19.415 32.12 c 14.458 36.551 10.354 36.907 7.96 35.404 c S 19.792 7.094 m 21.157 8.719 21.386 11.968 18.949 12.437 c 17.274 12.76 16.801 11.172 17.926 10.516 C 16.708 9.673 15.145 10.252 14.598 11.969 c 14.27 13 14.926 14.969 16.418 15.906 c 18.812 17.409 22.916 17.053 27.874 12.622 c 39.199 2.5 43.195 4.75 45.163 7.094 c 46.528 8.719 46.757 11.968 44.32 12.437 c 42.644 12.76 42.172 11.172 43.297 10.516 C 42.078 9.673 40.515 10.252 39.968 11.969 c 39.64 13 40.297 14.969 41.788 15.906 c 44.183 17.409 48.287 17.053 53.245 12.622 C 64.569 2.5 68.565 4.75 70.534 7.094 c 71.898 8.719 72.127 11.968 69.69 12.437 c 68.014 12.76 67.542 11.172 68.667 10.516 C 67.448 9.673 65.885 10.252 65.338 11.969 c 65.011 13 65.667 14.969 67.159 15.906 c 69.553 17.409 73.657 17.053 78.615 12.622 c S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (V\214gor-genomskinliga\012 1) (V\214gor-genomskinliga\012 1) 17.926 10.516 68.663 69.012 [ %AI3_Tile (0 O 0 R 1 0 0.3 0 k 1 0 0.3 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 17.926 69.012 m 17.926 10.516 L 68.663 10.516 L 68.663 69.012 L 17.926 69.012 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.55 0 0 0 k 0.55 0 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.75 w 4 M []0 d %AI3_Note: 0 D 0 XR 65.335 70.465 m 65.881 68.746 67.444 68.168 68.663 69.012 C 67.538 69.668 68.011 71.255 69.686 70.933 c 72.124 70.464 71.894 67.213 70.53 65.589 c 68.561 63.245 64.565 60.995 53.241 71.117 C S 39.964 70.465 m 40.511 68.746 42.074 68.168 43.293 69.012 C 42.168 69.668 42.64 71.255 44.316 70.933 c 46.753 70.464 46.524 67.213 45.16 65.589 c 43.191 63.245 39.195 60.995 27.87 71.117 c S 14.594 70.465 m 15.141 68.746 16.704 68.168 17.923 69.012 C 16.798 69.668 17.27 71.255 18.945 70.933 c 21.382 70.464 21.153 67.213 19.789 65.589 c 17.821 63.245 13.825 60.995 2.5 71.117 c S 10.959 51.619 m 22.282 41.497 26.278 43.747 28.247 46.09 c 29.611 47.715 29.841 50.965 27.403 51.434 c 25.728 51.757 25.255 50.169 26.38 49.513 C 25.161 48.669 23.599 49.248 23.052 50.966 c 22.723 51.997 23.38 53.966 24.872 54.903 c 27.267 56.406 31.371 56.05 36.328 51.619 c 47.653 41.497 51.649 43.746 53.618 46.09 c 54.982 47.715 55.212 50.965 52.774 51.434 c 51.099 51.757 50.626 50.169 51.751 49.513 C 50.532 48.669 48.97 49.248 48.423 50.966 c 48.094 51.997 48.751 53.966 50.243 54.903 c 52.638 56.406 56.742 56.05 61.699 51.619 C 73.024 41.497 77.02 43.747 78.988 46.09 c S 70.156 32.12 m 65.199 36.551 61.095 36.907 58.7 35.404 c 57.208 34.468 56.552 32.499 56.88 31.468 c 57.427 29.749 58.99 29.171 60.208 30.015 C 59.083 30.671 59.556 32.258 61.231 31.936 c 63.669 31.467 63.439 28.216 62.075 26.592 c 60.106 24.248 56.11 21.998 44.786 32.12 C 39.829 36.551 35.725 36.907 33.33 35.404 c 31.838 34.468 31.182 32.499 31.51 31.468 c 32.056 29.749 33.619 29.171 34.838 30.015 C 33.713 30.671 34.186 32.258 35.861 31.936 c 38.299 31.467 38.069 28.216 36.705 26.592 c 34.737 24.248 30.74 21.998 19.415 32.12 c 14.458 36.551 10.354 36.907 7.96 35.404 c S 19.792 7.094 m 21.157 8.719 21.386 11.968 18.949 12.437 c 17.274 12.76 16.801 11.172 17.926 10.516 C 16.708 9.673 15.145 10.252 14.598 11.969 c 14.27 13 14.926 14.969 16.418 15.906 c 18.812 17.409 22.916 17.053 27.874 12.622 c 39.199 2.5 43.195 4.75 45.163 7.094 c 46.528 8.719 46.757 11.968 44.32 12.437 c 42.644 12.76 42.172 11.172 43.297 10.516 C 42.078 9.673 40.515 10.252 39.968 11.969 c 39.64 13 40.297 14.969 41.788 15.906 c 44.183 17.409 48.287 17.053 53.245 12.622 C 64.569 2.5 68.565 4.75 70.534 7.094 c 71.898 8.719 72.127 11.968 69.69 12.437 c 68.014 12.76 67.542 11.172 68.667 10.516 C 67.448 9.673 65.885 10.252 65.338 11.969 c 65.011 13 65.667 14.969 67.159 15.906 c 69.553 17.409 73.657 17.053 78.615 12.622 c S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (V\214gor-genomskinliga\012 2) (V\214gor-genomskinliga\012 2) 17.926 10.516 68.663 69.012 [ %AI3_Tile (0 O 0 R 1 0 0.3 0 k 1 0 0.3 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 17.926 69.012 m 17.926 10.516 L 68.663 10.516 L 68.663 69.012 L 17.926 69.012 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.55 0 0 0 k 0.55 0 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.75 w 4 M []0 d %AI3_Note: 0 D 0 XR 65.335 70.465 m 65.881 68.746 67.444 68.168 68.663 69.012 C 67.538 69.668 68.011 71.255 69.686 70.933 c 72.124 70.464 71.894 67.213 70.53 65.589 c 68.561 63.245 64.565 60.995 53.241 71.117 C S 39.964 70.465 m 40.511 68.746 42.074 68.168 43.293 69.012 C 42.168 69.668 42.64 71.255 44.316 70.933 c 46.753 70.464 46.524 67.213 45.16 65.589 c 43.191 63.245 39.195 60.995 27.87 71.117 c S 14.594 70.465 m 15.141 68.746 16.704 68.168 17.923 69.012 C 16.798 69.668 17.27 71.255 18.945 70.933 c 21.382 70.464 21.153 67.213 19.789 65.589 c 17.821 63.245 13.825 60.995 2.5 71.117 c S 10.959 51.619 m 22.282 41.497 26.278 43.747 28.247 46.09 c 29.611 47.715 29.841 50.965 27.403 51.434 c 25.728 51.757 25.255 50.169 26.38 49.513 C 25.161 48.669 23.599 49.248 23.052 50.966 c 22.723 51.997 23.38 53.966 24.872 54.903 c 27.267 56.406 31.371 56.05 36.328 51.619 c 47.653 41.497 51.649 43.746 53.618 46.09 c 54.982 47.715 55.212 50.965 52.774 51.434 c 51.099 51.757 50.626 50.169 51.751 49.513 C 50.532 48.669 48.97 49.248 48.423 50.966 c 48.094 51.997 48.751 53.966 50.243 54.903 c 52.638 56.406 56.742 56.05 61.699 51.619 C 73.024 41.497 77.02 43.747 78.988 46.09 c S 70.156 32.12 m 65.199 36.551 61.095 36.907 58.7 35.404 c 57.208 34.468 56.552 32.499 56.88 31.468 c 57.427 29.749 58.99 29.171 60.208 30.015 C 59.083 30.671 59.556 32.258 61.231 31.936 c 63.669 31.467 63.439 28.216 62.075 26.592 c 60.106 24.248 56.11 21.998 44.786 32.12 C 39.829 36.551 35.725 36.907 33.33 35.404 c 31.838 34.468 31.182 32.499 31.51 31.468 c 32.056 29.749 33.619 29.171 34.838 30.015 C 33.713 30.671 34.186 32.258 35.861 31.936 c 38.299 31.467 38.069 28.216 36.705 26.592 c 34.737 24.248 30.74 21.998 19.415 32.12 c 14.458 36.551 10.354 36.907 7.96 35.404 c S 19.792 7.094 m 21.157 8.719 21.386 11.968 18.949 12.437 c 17.274 12.76 16.801 11.172 17.926 10.516 C 16.708 9.673 15.145 10.252 14.598 11.969 c 14.27 13 14.926 14.969 16.418 15.906 c 18.812 17.409 22.916 17.053 27.874 12.622 c 39.199 2.5 43.195 4.75 45.163 7.094 c 46.528 8.719 46.757 11.968 44.32 12.437 c 42.644 12.76 42.172 11.172 43.297 10.516 C 42.078 9.673 40.515 10.252 39.968 11.969 c 39.64 13 40.297 14.969 41.788 15.906 c 44.183 17.409 48.287 17.053 53.245 12.622 C 64.569 2.5 68.565 4.75 70.534 7.094 c 71.898 8.719 72.127 11.968 69.69 12.437 c 68.014 12.76 67.542 11.172 68.667 10.516 C 67.448 9.673 65.885 10.252 65.338 11.969 c 65.011 13 65.667 14.969 67.159 15.906 c 69.553 17.409 73.657 17.053 78.615 12.622 c S %AI6_EndPatternLayer ) & ] E %AI3_EndPattern %AI3_BeginPattern: (V\214gor-genomskinliga\012 3) (V\214gor-genomskinliga\012 3) 17.926 10.516 68.663 69.012 [ %AI3_Tile (0 O 0 R 1 0 0.3 0 k 1 0 0.3 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 1 w 4 M []0 d %AI3_Note: 1 D 0 XR 17.926 69.012 m 17.926 10.516 L 68.663 10.516 L 68.663 69.012 L 17.926 69.012 L f %AI6_EndPatternLayer ) & (0 O 0 R 0.55 0 0 0 k 0.55 0 0 0 K ) @ ( %AI6_BeginPatternLayer 800 Ar 0 J 0 j 0.75 w 4 M []0 d %AI3_Note: 0 D 0 XR 65.335 70.465 m 65.881 68.746 67.444 68.168 68.663 69.012 C 67.538 69.668 68.011 71.255 69.686 70.933 c 72.124 70.464 71.894 67.213 70.53 65.589 c 68.561 63.245 64.565 60.995 53.241 71.117 C S 39.964 70.465 m 40.511 68.746 42.074 68.168 43.293 69.012 C 42.168 69.668 42.64 71.255 44.316 70.933 c 46.753 70.464 46.524 67.213 45.16 65.589 c 43.191 63.245 39.195 60.995 27.87 71.117 c S 14.594 70.465 m 15.141 68.746 16.704 68.168 17.923 69.012 C 16.798 69.668 17.27 71.255 18.945 70.933 c 21.382 70.464 21.153 67.213 19.789 65.589 c 17.821 63.245 13.825 60.995 2.5 71.117 c S 10.959 51.619 m 22.282 41.497 26.278 43.747 28.247 46.09 c 29.611 47.715 29.841 50.965 27.403 51.434 c 25.728 51.757 25.255 50.169 26.38 49.513 C 25.161 48.669 23.599 49.248 23.052 50.966 c 22.723 51.997 23.38 53.966 24.872 54.903 c 27.267 56.406 31.371 56.05 36.328 51.619 c 47.653 41.497 51.649 43.746 53.618 46.09 c 54.982 47.715 55.212 50.965 52.774 51.434 c 51.099 51.757 50.626 50.169 51.751 49.513 C 50.532 48.669 48.97 49.248 48.423 50.966 c 48.094 51.997 48.751 53.966 50.243 54.903 c 52.638 56.406 56.742 56.05 61.699 51.619 C 73.024 41.497 77.02 43.747 78.988 46.09 c S 70.156 32.12 m 65.199 36.551 61.095 36.907 58.7 35.404 c 57.208 34.468 56.552 32.499 56.88 31.468 c 57.427 29.749 58.99 29.171 60.208 30.015 C 59.083 30.671 59.556 32.258 61.231 31.936 c 63.669 31.467 63.439 28.216 62.075 26.592 c 60.106 24.248 56.11 21.998 44.786 32.12 C 39.829 36.551 35.725 36.907 33.33 35.404 c 31.838 34.468 31.182 32.499 31.51 31.468 c 32.056 29.749 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r 0 1 1 0 1 %_Br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r 1 0 %_Br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r 0 1 1 0 1 %_Br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r 1 0 %_Br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r 0 1 1 0 1 %_Br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r 1 0 %_Br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r [ 0 1 1 0 1 50 0 %_BS %_0 1 1 0 1 50 0 Bs 0 1 1 0 1 50 0.005 %_BS %_0 1 1 0 1 50 0 Bs 0 1 1 0 1 50 12.4975 %_BS %_0 1 1 0 1 50 12.5 Bs 0 0 0 0 1 50 12.5025 %_BS %_0 0 0 0 1 50 12.5 Bs 0 0 0 0 1 50 24.9975 %_BS %_0 0 0 0 1 50 25 Bs 0 1 1 0 1 50 25.0025 %_BS %_0 1 1 0 1 50 25 Bs 0 1 1 0 1 50 37.4975 %_BS %_0 1 1 0 1 50 37.5 Bs 0 0 0 0 1 50 37.5025 %_BS %_0 0 0 0 1 50 37.5 Bs 0 0 0 0 1 50 49.9975 %_BS %_0 0 0 0 1 50 50 Bs 0 1 1 0 1 50 50.0025 %_BS %_0 1 1 0 1 50 50 Bs 0 1 1 0 1 50 62.4975 %_BS %_0 1 1 0 1 50 62.5 Bs 0 0 0 0 1 50 62.5025 %_BS %_0 0 0 0 1 50 62.5 Bs 0 0 0 0 1 50 74.9975 %_BS %_0 0 0 0 1 50 75 Bs 0 1 1 0 1 50 75.0025 %_BS %_0 1 1 0 1 50 75 Bs 0 1 1 0 1 50 87.4975 %_BS %_0 1 1 0 1 50 87.5 Bs 0 0 0 0 1 50 87.5025 %_BS %_0 0 0 0 1 50 87.5 Bs 0 0 0 0 1 50 99.995 %_BS %_0 0 0 0 1 50 100 Bs 0 1 1 0 1 50 100 %_BS %_0 1 1 0 1 50 100 Bs BD %AI5_EndGradient %AI5_End_NonPrinting-- %AI5_BeginPalette 0 0 Pb 1 1 1 1 ([Passm\212rke]) 0 Xs ([Passm\212rke]) Pc 0 0 0 0 k (C=0 M=0 Y=0 K=0) Pc 0 0 0 1 k (C=0 M=0 Y=0 K=100) Pc 0 0.45 0.6 0 k (C=0 M=45 Y=60 K=0) Pc 0 0.5 0.05 0 k (C=0 M=50 Y=5 K=0) Pc 0 0.9 1 0 k (C=0 M=90 Y=100 K=0) Pc 1 0.2 1 0 k (C=100 M=20 Y=100 K=0) Pc 1 0.4 0.15 0 k (C=100 M=40 Y=15 K=0) Pc 0.2 0 1 0 k (C=20 M=0 Y=100 K=0) Pc 0.25 1 0.25 0 k (C=25 M=100 Y=25 K=0) Pc 0.4 0.4 0.4 0 k (C=40 M=40 Y=40 K=0) Pc 0.4 0.7 1 0 k (C=40 M=70 Y=100 K=0) Pc 0.75 0.9 0 0 k (C=75 M=90 Y=0 K=0) Pc 1 0 0.55 0 (Havsbl\214) 0 x (Havsbl\214) Pc 1 0.5 0 0 (Bl\214) 0 x (Bl\214) Pc 0.5 0.4 0.3 0 (Bl\214gr\214) 0 x (Bl\214gr\214) Pc 0.8 0.05 0 0 (Himmelsbl\214) 0 x (Himmelsbl\214) Pc 0.5 0.85 1 0 (Brun) 0 x (Brun) Pc 1 0.9 0.1 0 (M\232rkbl\214) 0 x (M\232rkbl\214) Pc 1 0.55 1 0 (Skogsgr\232n) 0 x (Skogsgr\232n) Pc 0.05 0.2 0.95 0 (Guld) 0 x (Guld) Pc 0.75 0.05 1 0 (Gr\212sgr\232n) 0 x (Gr\212sgr\232n) Pc 0 0.45 1 0 (Orange) 0 x (Orange) Pc 0.15 1 1 0 (R\232d) 0 x (R\232d) Pc 0.45 0.9 0 0 (Violett) 0 x (Violett) Pc Bb 2 (Svart, vit) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Svart, vit) Pc Bb 2 (Krom) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Krom) Pc Bb 2 (Gr\232nbl\214) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Gr\232nbl\214) Pc Bb 2 (Orange, gr\232n, violett) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Orange, gr\232n, violett) Pc Bb 2 (Rosa, gul, gr\232n) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Rosa, gul, gr\232n) Pc Bb 2 (Lila, r\232d, gul) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Lila, r\232d, gul) Pc Bb 2 (Regnb\214ge) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Regnb\214ge) Pc Bb 2 (St\214lr\232r) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (St\214lr\232r) Pc Bb 0 0 0 0 Bh 2 (Vit & r\232d radiell) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Vit & r\232d radiell) Pc Bb 0 0 0 0 Bh 2 (Gul & orange radiell) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Gul & orange radiell) Pc Bb 0 0 0 0 Bh 2 (Gul & lila radiell) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Gul & lila radiell) Pc Bb 2 (Gul, violett, orange, bl\214) -4337.75 4412.25 0 0 1 0 0 1 0 0 Bg 0 BB (Gul, violett, orange, bl\214) Pc (Pil1.2.ut/in) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Pil1.2.ut/in) Pc (Pil1.2.sida) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Pil1.2.sida) Pc (Tegelv\212gg\012 5) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Tegelv\212gg\012 5) Pc (Schackrutor) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor) Pc (Konfetti) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Konfetti) Pc (DblLinje1.2.inre) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.inre) Pc (DblLinje1.2.yttre) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.yttre) Pc (DblLinje1.2.sida) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.sida) Pc (Diamanter) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter) Pc (Sexh\232rning) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Sexh\232rning) Pc (Lagerbl.inre) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.inre) Pc (Lagerbl.yttre) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.yttre) Pc (Lagerbl.sida) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.sida) Pc (Fallande l\232v) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Fallande l\232v) Pc (Prickm\232nster) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster) Pc (Slumpm\212ssiga cirklar) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Slumpm\212ssiga cirklar) Pc (Rep.sida) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Rep.sida) Pc (Fj\212ll) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Fj\212ll) Pc (Helstj\212rna.sida) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Helstj\212rna.sida) Pc (Stj\212rnor) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor) Pc (R\212nder) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (R\212nder) Pc (Listprofil.yttre) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Listprofil.yttre) Pc (Listprofil.sida) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Listprofil.sida) Pc (V\214gor-genomskinliga) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (V\214gor-genomskinliga) Pc (Schackrutor\012 11) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 11) Pc (Diamanter\012 11) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 11) Pc (Prickm\232nster\012 11) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 11) Pc (Stj\212rnor\012 11) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 11) Pc (Schackrutor\012 10) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 10) Pc (Diamanter\012 10) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 10) Pc (Prickm\232nster\012 10) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 10) Pc (Stj\212rnor\012 10) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 10) Pc (Pil1.2.ut/in\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Pil1.2.ut/in\012 4) Pc (Pil1.2.sida\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Pil1.2.sida\012 4) Pc (Tegelv\212gg\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Tegelv\212gg\012 4) Pc (Schackrutor\012 9) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 9) Pc (Konfetti\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Konfetti\012 4) Pc (DblLinje1.2.inre\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.inre\012 4) Pc (DblLinje1.2.yttre\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.yttre\012 4) Pc (DblLinje1.2.sida\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.sida\012 4) Pc (Diamanter\012 9) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 9) Pc (Sexh\232rning\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Sexh\232rning\012 4) Pc (Lagerbl.inre\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.inre\012 4) Pc (Lagerbl.yttre\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.yttre\012 4) Pc (Lagerbl.sida\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.sida\012 4) Pc (Fallande l\232v\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Fallande l\232v\012 4) Pc (Prickm\232nster\012 9) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 9) Pc (Slumpm\212ssiga cirklar\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Slumpm\212ssiga cirklar\012 4) Pc (Rep.sida\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Rep.sida\012 4) Pc (Fj\212ll\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Fj\212ll\012 4) Pc (Helstj\212rna.sida\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Helstj\212rna.sida\012 4) Pc (Stj\212rnor\012 9) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 9) Pc (R\212nder\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (R\212nder\012 4) Pc (Listprofil.yttre\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Listprofil.yttre\012 4) Pc (Listprofil.sida\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Listprofil.sida\012 4) Pc (V\214gor-genomskinliga\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (V\214gor-genomskinliga\012 4) Pc (Schackrutor\012 8) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 8) Pc (Diamanter\012 8) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 8) Pc (Prickm\232nster\012 8) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 8) Pc (Stj\212rnor\012 8) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 8) Pc (Schackrutor\012 7) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 7) Pc (Diamanter\012 7) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 7) Pc (Prickm\232nster\012 7) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 7) Pc (Stj\212rnor\012 7) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 7) Pc (Pil1.2.ut/in\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Pil1.2.ut/in\012 3) Pc (Pil1.2.sida\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Pil1.2.sida\012 3) Pc (Tegelv\212gg\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Tegelv\212gg\012 3) Pc (Schackrutor\012 6) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 6) Pc (Konfetti\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Konfetti\012 3) Pc (DblLinje1.2.inre\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.inre\012 3) Pc (DblLinje1.2.yttre\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.yttre\012 3) Pc (DblLinje1.2.sida\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.sida\012 3) Pc (Diamanter\012 6) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 6) Pc (Sexh\232rning\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Sexh\232rning\012 3) Pc (Lagerbl.inre\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.inre\012 3) Pc (Lagerbl.yttre\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.yttre\012 3) Pc (Lagerbl.sida\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.sida\012 3) Pc (Fallande l\232v\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Fallande l\232v\012 3) Pc (Prickm\232nster\012 6) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 6) Pc (Slumpm\212ssiga cirklar\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Slumpm\212ssiga cirklar\012 3) Pc (Rep.sida\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Rep.sida\012 3) Pc (Fj\212ll\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Fj\212ll\012 3) Pc (Helstj\212rna.sida\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Helstj\212rna.sida\012 3) Pc (Stj\212rnor\012 6) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 6) Pc (R\212nder\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (R\212nder\012 3) Pc (Listprofil.yttre\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Listprofil.yttre\012 3) Pc (Listprofil.sida\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Listprofil.sida\012 3) Pc (V\214gor-genomskinliga\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (V\214gor-genomskinliga\012 3) Pc (Schackrutor\012 5) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 5) Pc (Diamanter\012 5) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 5) Pc (Prickm\232nster\012 5) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 5) Pc (Stj\212rnor\012 5) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 5) Pc (Schackrutor\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 4) Pc (Diamanter\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 4) Pc (Prickm\232nster\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 4) Pc (Stj\212rnor\012 4) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 4) Pc (Pil1.2.ut/in\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Pil1.2.ut/in\012 2) Pc (Pil1.2.sida\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Pil1.2.sida\012 2) Pc (Tegelv\212gg\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Tegelv\212gg\012 2) Pc (Schackrutor\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 3) Pc (Konfetti\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Konfetti\012 2) Pc (DblLinje1.2.inre\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.inre\012 2) Pc (DblLinje1.2.yttre\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.yttre\012 2) Pc (DblLinje1.2.sida\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.sida\012 2) Pc (Diamanter\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 3) Pc (Sexh\232rning\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Sexh\232rning\012 2) Pc (Lagerbl.inre\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.inre\012 2) Pc (Lagerbl.yttre\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.yttre\012 2) Pc (Lagerbl.sida\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.sida\012 2) Pc (Fallande l\232v\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Fallande l\232v\012 2) Pc (Prickm\232nster\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 3) Pc (Slumpm\212ssiga cirklar\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Slumpm\212ssiga cirklar\012 2) Pc (Rep.sida\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Rep.sida\012 2) Pc (Fj\212ll\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Fj\212ll\012 2) Pc (Helstj\212rna.sida\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Helstj\212rna.sida\012 2) Pc (Stj\212rnor\012 3) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 3) Pc (R\212nder\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (R\212nder\012 2) Pc (Listprofil.yttre\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Listprofil.yttre\012 2) Pc (Listprofil.sida\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Listprofil.sida\012 2) Pc (V\214gor-genomskinliga\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (V\214gor-genomskinliga\012 2) Pc (Schackrutor\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 2) Pc (Diamanter\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 2) Pc (Prickm\232nster\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 2) Pc (Stj\212rnor\012 2) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 2) Pc (Pil1.2.ut/in\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Pil1.2.ut/in\012 1) Pc (Pil1.2.sida\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Pil1.2.sida\012 1) Pc (Tegelv\212gg\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Tegelv\212gg\012 1) Pc (Schackrutor\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Schackrutor\012 1) Pc (Konfetti\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Konfetti\012 1) Pc (DblLinje1.2.inre\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.inre\012 1) Pc (DblLinje1.2.yttre\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.yttre\012 1) Pc (DblLinje1.2.sida\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (DblLinje1.2.sida\012 1) Pc (Diamanter\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Diamanter\012 1) Pc (Sexh\232rning\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Sexh\232rning\012 1) Pc (Lagerbl.inre\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.inre\012 1) Pc (Lagerbl.yttre\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.yttre\012 1) Pc (Lagerbl.sida\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Lagerbl.sida\012 1) Pc (Fallande l\232v\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Fallande l\232v\012 1) Pc (Prickm\232nster\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Prickm\232nster\012 1) Pc (Slumpm\212ssiga cirklar\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Slumpm\212ssiga cirklar\012 1) Pc (Rep.sida\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Rep.sida\012 1) Pc (Fj\212ll\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Fj\212ll\012 1) Pc (Helstj\212rna.sida\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Helstj\212rna.sida\012 1) Pc (Stj\212rnor\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Stj\212rnor\012 1) Pc (R\212nder\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (R\212nder\012 1) Pc (Listprofil.yttre\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Listprofil.yttre\012 1) Pc (Listprofil.sida\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (Listprofil.sida\012 1) Pc (V\214gor-genomskinliga\012 1) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p (V\214gor-genomskinliga\012 1) Pc 0 0 0 0 k (C=0 M=0 Y=0 K=0) Pc (C=0 M=0 Y=0 K=0) Pc (C=0 M=0 Y=0 K=0) Pc (C=0 M=0 Y=0 K=0) Pc (C=0 M=0 Y=0 K=0) Pc 0 0.38 1 0.26 k (C=0 M=38 Y=100 K=26) Pc 1 0.72 0 0.18 (PANTONE 280 CV) 0 x (PANTONE 280 CV) Pc PB %AI5_EndPalette %AI5_Begin_NonPrinting Np %AI5_End_NonPrinting-- %AI5_Begin_NonPrinting Np %AI8_PluginGroupInfo (Adobe Path Blends) (Adobe \205verg\214ngar) (\205verg\214ngar) %AI8_PluginGroupInfo (Adobe Calligraphic Brush Tool) (\201ngra Ny kalligrafisk pensel) (Kalligrafisk pensel) %AI8_PluginGroupInfo (Adobe PatternOnPath Brush Tool) (Adobe M\232nsterpenslar) (Konstn\212rlig pensel) %AI8_PluginGroupInfo (Adobe ArtOnPath Brush Tool) (Adobe Konstn\212rliga penslar) (Konstn\212rlig pensel) %AI8_PluginGroupInfo (Adobe Scatter Brush Tool) 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      Onia Processes

      Production of J/psi or Upsilon, directly and via chi states and the colour-octet mechanism. In each process the square-bracketed expression specifies the state in spectroscopic notation, (2S+1) L J, followed by (1) for colour-singlet states and (8) for colour-octet ditto.

      The original Fortran code for these processes has been contributed by Stefan Wolf [unpublished]. For the C++ version only the unpolarized expressions are retained, since the theoretical predictions of the colour-octet model anyway do not agree with the experimental observations. Furthermore, the polarization effects are modest, so isotropic decay is not a bad starting point. Such an event sample can afterwards be reweighted at will by the user, to test various assumptions.

      The description of final-state radiation is in this case based on some further model assumptions.

      Most of the processes below are divergent in the limit pT -> 0, and therefore a pTmin scale should be set. Comparisons with data indicate that this divergence can be tamed the same way as for the normal QCD 2 -> 2 cross sections Bar06,Kra08, which makes sense, since they are all dominated by the same kind of t-channel gluon exchange. It is therefore possible to use the SuppressSmallPT user hook to impose a reweighting that cancels the low-pT divergence.

      An eikonalized description of these processes is included in the multiparton-interactions framework. Here the low-pT dampening is automatic, and additionally the framework is more consistent (e.g. with respect to energy-momentum constraints and the impact-parameter description) for events where the onium production is not the hardest subprocess, as would often be the case in the low-pT limit.

      Charmonium

      Common switch for the group of charmonium production. g g -> ccbar[3S1(1)] g. Code 401. g g -> ccbar[3P0(1)] g. Code 402. g g -> ccbar[3P1(1)] g. Code 403. g g -> ccbar[3P2(1)] g. Code 404. q g -> ccbar[3P0(1)] q. Code 405. q g -> ccbar[3P1(1)] q. Code 406. q g -> ccbar[3P2(1)] q. Code 407. q qbar -> ccbar[3P0(1)] g. Code 408. q qbar -> ccbar[3P1(1)] g. Code 409. q qbar -> ccbar[3P2(1)] g. Code 410. g g -> ccbar[3S1(8)] g. Code 411. g g -> ccbar[3S1(8)] g. Code 412. g g -> ccbar[3S1(8)] g. Code 413. q g -> ccbar[3S1(8)] q. Code 414. q g -> ccbar[3S1(8)] q. Code 415. q g -> ccbar[3S1(8)] q. Code 416. q qbar -> ccbar[3S1(8)] g. Code 417. q qbar -> ccbar[3S1(8)] g. Code 418. q qbar -> ccbar[3S1(8)] g. Code 419.

      Bottomonium

      Common switch for the group of charmonium production. g g -> bbbar[3S1(1)] g. Code 501. g g -> bbbar[3P0(1)] g. Code 502. g g -> bbbar[3P1(1)] g. Code 503. g g -> bbbar[3P2(1)] g. Code 504. q g -> bbbar[3P0(1)] q. Code 505. q g -> bbbar[3P1(1)] q. Code 506. q g -> bbbar[3P2(1)] q. Code 507. q qbar -> bbbar[3P0(1)] g. Code 508. q qbar -> bbbar[3P1(1)] g. Code 509. q qbar -> bbbar[3P2(1)] g. Code 510. g g -> bbbar[3S1(8)] g. Code 511. g g -> bbbar[3S1(8)] g. Code 512. g g -> bbbar[3S1(8)] g. Code 513. q g -> bbbar[3S1(8)] q. Code 514. q g -> bbbar[3S1(8)] q. Code 515. q g -> bbbar[3S1(8)] q. Code 516. q qbar -> bbbar[3S1(8)] g. Code 517. q qbar -> bbbar[3S1(8)] g. Code 518. q qbar -> bbbar[3S1(8)] g. Code 519.

      Onium matrix elements

      The implementation of charmonium and bottomonium production, including the colour-octet production mechanism, requires information on NRQCD matrix elements for the various wavefunctions involved. Default values for these are encoded in the following ten variables. They are taken from Nas00; see also Bar06. <O(J/psi)[3S1(1)]>. <O(J/psi)[3S1(8)]>. <O(J/psi)[1S0(8)]>. <O(J/psi)[3P0(8)]>/m_c^2. <O(chi_c0)[3P0(8)]>/m_c^2. <O(Upsilon)[3S1(1)]>. <O(Upsilon)[3S1(8)]>. <O(Upsilon)[1S0(8)]>. <O(Upsilon)[3P0(8)]>/m_b^2. <O(chi_b0)[3P0(8)]>/m_b^2.
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      Semi-Internal Processes

      Normally users are expected to implement new processes via the Les Houches Accord. Then you do all flavour, colour and phase-space selection externally, before your process-level events are input for further processing by PYTHIA. However, it is also possible to implement a new process in exactly the same way as the internal PYTHIA ones, thus making use of the internal phase space selection machinery to sample an externally provided cross-section expression. The MadGraph 5 program Alw11 allows you to do exactly that, i.e. it can be used to generate C++ code that can be linked into the existing PYTHIA framework, see here.

      Should you decide to go ahead on your own, this page gives a brief summary how to do that. If you additionally want to introduce a new resonance species, with its own internal width calculations, you will find further instructions here. It is strongly recommended to shop around for a similar process that has already been implemented, and to use that existing code as a template. Look for processes with the same combinations of incoming flavours and colour flows, rather than the shape of the cross section itself. With a reasonable such match the task should be of medium difficulty, without it more demanding.

      PYTHIA is rather good at handling the phase space of 2 -> 1 and 2 -> 2 processes, is more primitive for 2 -> 3 ones and does not at all address higher multiplicities. This limits the set of processes that you can implement in this framework. The produced particles may be resonances, however, so it is possible to end up with bigger "final" multiplicities through sequential decays, and to include further matrix-element weighting in those decays.

      There are three steps involved in implementing a process:

      1. making use of the PYTHIA-provided kinematics information to calculate the relevant cross section,
      2. writing a new class, where the matrix elements are implemented, including information on incoming and outgoing flavours and colours, and
      3. making the process available.
      We consider these aspects in turn. An example where it all comes together is found in main22.cc.

      The Cross Section Calculation

      The key method for the cross section calculation is SigmaProcess::sigmaHat(), described below. At the point when it is called, the kinematics has already been set up, and from these phase space variables the differential cross section is to be calculated.

      For a 2 -> 1 process, the returned value should be sigmaHat(sHat), where mH (= mHat), sH (= sHat) and sH2 (= sHat^2) are available to be used. Incoming partons are massless. Overload the convertM2() method below if you instead plan to return |M|^2.

      For a 2 -> 2 process, instead d(sigmaHat)/d(tHat) should be returned, based on provided mH, sH, sH2, tH, tH2, uH, uH2, m3, s3, m4, s4 and pT2 values (s3 = m3*m3 etc.). Incoming partons are massless. Overload the convertM2() method below if you instead plan to return |M|^2.

      For a 2 -> 3 process, instead |M|^2 should be returned, with normalization such that |M|^2 / (2 sHat) integrated over the three-body phase space gives the cross section. Here no standard set of Mandelstam-style variables exists. Instead the obvious ones, mH, sH, m3, s3, m4, s4, m5, s5, are complemented by the four-vectors p3cm, p4cm, p5cm, from which further invariants may be calculated. The four-vectors are defined in the CM frame of the subcollision, with massless incoming partons along the +-z axis.

      In either case, alpha_s and alpha_em have already been calculated, and are stored in alpS and alpEM. Also other standard variables may be used, like CoupEW::sin2thetaW(), and related flavour-dependent vector and axial couplings in CoupEW and CKM combinations in VCKM.

      In case some of the final-state particles are resonances, their squared masses have already been selected according to a Breit-Wigner with a linearly running width Gamma(m) = Gamma(m_0) * m / m_0. More precisely, the mass spectrum is weighted according to w_BW(m^2) d(m^2), where w_BW(m^2) = (1/pi) * (m * Gamma(m)) / ( (m^2 - m_0^2)^2 + (m * Gamma(m))^2 ) . If you would like to have another expression, the above weights are stored in runBW3, runBW4 and runBW5, respectively. If you divide out one of these factors, you just remain with a phase space selection d(m^2) for this particle, and can multiply on your desired shape factor instead. Unfortunately, the Monte Carlo efficiency will drop if your new mass distribution differs dramatically from the input one. Therefore it does make sense to adjust the database value of the width to be slightly (but not too much) broader than the distribution you have in mind. Also note that, already by default, the wings of the Breit-Wigner are oversampled (with a compensating lower internal weight) by partly sampling like (a + b/m^2 + c/m^4) d(m^2), where the last term is only used for gamma^*/Z^0.

      As alternative to the kinematics variables defined above, also the two arrays mME[5] and pME[5], for masses and four-momenta, respectively, can be used for cross-section calculations. Here indices 0 and 1 are the two incoming beams, and 2 and onwards the outgoing particles. Note that this differs by one step from the normal internal labeling, where slot 0 is left empty. The four-momenta are defined in the rest frame of the subcollision, with the incoming partons along the +-z direction. The kinematics need not agree with the "correct" one stored in the event record, for three reasons.
      1) Gauge invariance forces matrix-element calculations to use the same masses for incoming as outgoing legs of a particle species, say b quarks. Therefore the kinematics of the two incoming partons is recalculated, relative to the normal event record, to put the partons on the mass shell. (Note that initial masses is a technical issue, not the correct physics picture: the incoming partons are likely to be spacelike virtual rather than on the mass shell.)
      2) In principle each fermion flavour has to be treated separately, owing to a different mass. However, in many cases fermions can be assumed massless, which speeds up the calculations, and further gains occur if then different flavours can use the same cross-section expression. In MadGraph the default is that fermions up to and including the c quark and the mu lepton are considered massless, while the b quark and the tau lepton are considered massive. This can be modified however, and below we provide four flags that can be used to consider the "borderline" fermions either as massless or as massive when matrix elements are evaluated, to match the assumptions made for the matrix elements themselves.
      3) For 2 -> 2 and 2 -> 3 processes of massive identical particles (or antiparticles) in the final state, such as t tbar or W^+ W^-, the kinematics is here adjusted so that the two or three particles have the same mass, formed as a suitable average of the actual Breit-Wigner-distributed masses. This allows the evaluation of matrix-element expressions that only have meaning if the two/three have the same mass.
      Thus the mass array mME[5] and the four-momentum array pME[5] present values both for initial- and final-state particles based on these mass principles suited for matrix-element input. Note that these variables therefore differ from the kinematics stored in the event record proper, where incoming fermions are always massless and outgoing resonances have independent Breit-Wigner mass distributions.
      The conversion from the normal to the special kinematics is done by calling the setupForME() method. This you have to do yourself in the SigmaHat() member of your derived class. Alternatively it could be done in SigmaKin(), i.e. before the loop over incoming flavours, but then these would be considered massless. The identity of final-state particles is obtained from the id3Mass(), id4Mass() and id5Mass() methods. Should the conversion to mME[5] and pME[5] not work, setupForME() will return false, and then the cross section should be put zero. Let the c quark be massive or not in the kinematics set up for external matrix-element evaluation. Let the b quark be massive or not in the kinematics set up for external matrix-element evaluation. Let the mu lepton be massive or not in the kinematics set up for external matrix-element evaluation. Let the tau lepton be massive or not in the kinematics set up for external matrix-element evaluation.

      The Cross Section Class

      The matrix-element information has to be encoded in a new class. The relevant code could either be put before the main program in the same file, or be stored separately, e.g. in a matched pair of .h and .cc files. The latter may be more convenient, in particular if the cross sections are lengthy, or if you intend to build up your own little process library, but of course requires that these additional files are correctly compiled and linked.

      The class has to be derived either from Sigma1Process, for 2 -> 1 processes, from Sigma2Process, for 2 -> 2 ones, or from Sigma3Process, for 2 -> 3 ones. (The Sigma0Process class is used for elastic, diffractive and minimum-bias events, and is not recommended for use beyond that.) These are in their turn derived from the SigmaProcess base class.

      The class can implement a number of methods. Some of these are compulsory, others strongly recommended, and the rest are to be used only when the need arises to override the default behaviour. The methods are:

      A constructor for the derived class obviously must be available. Here you are quite free to allow a list of arguments, to set the parameters of your model, or even to create a set of closely related but distinct processes. For instance, g g -> Q Qbar, Q = c or b, is only coded once, and then the constructor takes the quark code (4 or 5) as argument, to allow the proper amount of differentiation.

      A destructor is only needed if you plan to delete the process before the natural end of the run, and require some special behaviour at that point. If you call such a destructor you will leave a pointer dangling inside the Pythia object you gave it in to, if that still exists. is called once during initialization, and can then be used to set up parameters, such as masses and couplings, and perform calculations that need not be repeated for each new event, thereby saving time. This method needs not be implemented, since in principle all calculations can be done in sigmaHat below. is called once a kinematical configuration has been determined, but before the two incoming flavours are known. This routine can therefore be used to perform calculations that otherwise might have to be repeated over and over again in sigmaHat below. For instance a flavour-independent cross section calculation for a q g initial state would be repeated 20 times in sigmaHat, five times for the five quark flavours allowed in the incoming beams, times twice to include antiquarks, times twice since the (anti)quark could be in either of the two beams. You could therefore calculate the result once only and store it as a private data member of the class. It is optional whether you want to use this method, however, or put everything in sigmaHat. is the key method for cross section calculations and returns a cross section value, as described in the previous section. It is called when also a preliminary set of incoming flavours has been picked, in addition to the kinematical ones already available for sigmaKin. Typically sigmaHat is called inside a loop over all allowed incoming flavour combinations, stored in id1 and id2, with fixed kinematics, as already illustrated above. The sum over the different flavour combinations provides the total cross section, while their relative size is used to make a selection of a specific incoming state. to be called by the user from inside sigmaHat() (or possibly sigmaKin()) to setup alternative kinematics in the mME[5] and pME[5] arrays, better suited for matrix-element calculations. See the end of the previous section for a more detailed description. Should the method return false then the conversion did not work, and sigmaHat() (or sigmaKin()) should be set to vanish. is called only once an initial state and a kinematical configuration has been picked. This routine must set the complete flavour information and the colour flow of the process. This may involve further random choices, between different possible final-state flavours or between possible competing colour flows. Private data members of the class may be used to retain some information from the previous steps above.
      When this routine is called the two incoming flavours have already been selected and are available in id1 and id2, whereas the one, two or three outgoing ones either are fixed for a given process or can be determined from the instate (e.g. whether a W^+ or W^- was produced). There is also a standard method in VCKM to pick a final flavour from an initial one with CKM mixing. Once you have figured out the value of id3 and, the case being, id4 and id5, you store these values permanently by a call setId( id1, id2, id3, id4, id5), where the last two may be omitted if irrelevant.
      Correspondingly, the colours are stored with setColAcol( col1, acol1, col2, acol2, col3, acol3, col4, acol4, col5, acol5), where the final ones may be omitted if irrelevant. Les Houches style colour tags are used, but starting with number 1 (and later shifted by the currently requested offset). The input is grouped particle by particle, with the colour index before the anticolour one. You may need to select colour flow dynamically, depending on the kinematics, when several distinct possibilities exist. Trivial operations, like swapping colours and anticolours, can be done with existing methods.
      When the id3Mass() and id4Mass() methods have been used, the order of the outgoing particles may be inconsistent with the way the tHat and uHat variables have been defined. A typical example would be a process like q g -> q' W with tHat defined between incoming and outgoing quark, but where id3Mass() = 24 and so the process is to be stored as q g -> W q'. One should then put the variable swapTU = true in setIdColAcol() for each event where the tHat and uHat variables should be swapped before the event kinematics is reconstructed. This variable is automatically restored to false for each new event.
      is called to allow a reweighting of the simultaneous flavour choices of resonance decay products. Is currently only used for the q qbar -> gamma*/Z^0 gamma*/Z^0 process, and will likely not be of interest for you. is called when the basic process has one or several resonances, after each set of related resonances in process[i], iResBeg <= i <= iResEnd, has been allowed to decay. The calculated weight, to be normalized to the range between 0 and 1, is used to decide whether to accept the decay(s) or try for a new decay configuration. The base-class version of this method returns unity, i.e. gives isotropic decays by default. This method may be called repeatedly for a single event. For instance, in q qbar -> H^0 Z^0 with H^0 -> W^+ W^-, a first call would be made after the H^0 and Z^0 decays, and then depend only on the Z^0 decay angles since the H^0 decays isotropically. The second call would be after the W^+ W^- decays and then involve correlations between the four daughter fermions. returns the name of the process, as you want it to be shown in listings. returns an integer identifier of the process. This has no internal function, but is only intended as a service for the user to rapidly (and hopefully uniquely) identify which process occurred in a given event. Numbers below 10000 are reserved for internal PYTHIA use. this string specifies the combinations of incoming partons that are allowed for the process under consideration, and thereby which incoming flavours id1 and id2 the sigmaHat() calls will be looped over. It is always possible to pick a wider flavour selection than strictly required and then put to zero cross sections in the superfluous channels, but of course this may cost some extra execution time. Currently allowed options are:
      * gg: two gluons.
      * qg: one (anti)quark and one gluon.
      * qq: any combination of two quarks, two antiquarks or a quark and an antiquark.
      * qqbar: any combination of a quark and an antiquark; a subset of the qq option.
      * qqbarSame: a quark and its antiquark; a subset of the qqbar option.
      * ff: any combination of two fermions, two antifermions or a fermion and an antifermion; is the same as qq for hadron beams but also allows processes to work with lepton beams.
      * ffbar: any combination of a fermion and an antifermion; is the same as qqbar for hadron beams but also allows processes to work with lepton beams.
      * ffbarSame: a fermion and its antifermion; is the same as qqbarSame for hadron beams but also allows processes to work with lepton beams.
      * ffbarChg: a fermion and an antifermion that combine to give charge +-1.
      * fgm: a fermion and a photon (gamma).
      * ggm: a gluon and a photon.
      * gmgm: two photons.
      it is assumed that cross sections normally come in dimensions such that they, when integrated over the relevant phase space, obtain the dimension GeV^-2, and therefore need to be converted to mb. If the cross section is already encoded as mb then convert2mb() should be overloaded to instead return false. it is assumed that 2 -> 1 cross sections are encoded as sigmaHat(sHat), and 2 -> 2 ones as d(sigmaHat)/d(tHat) in the SigmaProcess::sigmaHat() methods. If convertM2() is overloaded to instead return true then the return value is instead assumed to be the squared matrix element |M|^2, and SigmaProcess::sigmaHatWrap(...) converts to sigmaHat(sHat) or d(sigmaHat)/d(tHat), respectively. This switch has no effect on 2 -> 3 processes, where |M|^2 is the only allowed input anyway. are the one, two or three final-state flavours, where masses are to be selected before the matrix elements are evaluated. Only the absolute value should be given. For massless particles, like gluons and photons, one need not give anything, i.e. one defaults to 0. The same goes for normal light quarks, where masses presumably are not implemented in the matrix elements. Later on, these quarks can still (automatically) obtain constituent masses, once a u, d or s flavour has been selected. are the codes of up to two s-channel resonances contributing to the matrix elements. These are used by the program to improve the phase-space selection efficiency, by partly sampling according to the relevant Breit-Wigner distributions. Massless resonances (the gluon and photon) need not be specified. normally the choice of renormalization and factorization scales in 2 -> 2 and 2 -> 3 processes is based on the assumption that t- and u-channel exchanges dominates the cross section. In cases such as f fbar -> gamma* -> f' fbar' a 2 -> 2 process actually ought to be given scales as a 2 -> 1 one, in the sense that it proceeds entirely through an s-channel resonance. This can be achieved if you override the default false to return true. See further the page on couplings and scales. normally no intermediate state is shown in the event record for 2 -> 2 and 2 -> 3 processes. However, in case that idSChannel is overloaded to return a nonzero value, an intermediate particle with that identity code is inserted into the event record, to make it a 2 -> 1 -> 2 or 2 -> 1 -> 3 process. Thus if both isSChannel and idSChannel are overloaded, a process will behave and look like it proceeded through a resonance. The one difference is that the implementation of the matrix element is not based on the division into a production and a decay of an intermediate resonance, but is directly describing the transition from the initial to the final state. there are two different 3-body phase-space selection machineries, of which the non-QCD one is default. If you overload this method instead the QCD-inspired machinery will be used. The differences between these two is related to which phase space cuts can be set, and also that the QCD machinery assumes (almost) massless outgoing partons. the non-QCD 2 -> 3 phase space selection machinery is rather primitive, as already mentioned. The efficiency can be improved in processes that proceed though t-channel exchanges, such as q qbar' -> H^0 q qbar' via Z^0 Z^0 fusion, if the identity of the t-channel-exchanged particles on the two side of the event are provided. Only the absolute value is of interest. in the above kind of 2 -> 3 phase-space selection, the sampling of pT^2 is done with one part flat, one part weighted like 1 / (pT^2 + m_R^2) and one part like 1 / (pT^2 + m_R^2)^2. The above values provide the relative amount put in the latter two channels, respectively, with the first obtaining the rest. Thus the sum of tChanFracPow1() and tChanFracPow2() must be below unity. The final results should be independent of these numbers, but the Monte Carlo efficiency may be quite low for a bad choice. Here m_R is the mass of the exchanged resonance specified by idTchan1() or idTchan2(). Note that the order of the final-state listing is important in the above q qbar' -> H^0 q qbar' example, i.e. the H^0 must be returned by id3Mass(), since it is actually the pT^2 of the latter two that are selected independently, with the first pT then fixed by transverse-momentum conservation. in 2 -> 3 processes the phase space selection used here involves a twofold ambiguity basically corresponding to a flipping of the positions of last two outgoing particles. These are assumed equally likely by default, false, but for processes proceeding entirely through t-channel exchange the Monte Carlo efficiency can be improved by making a preselection based on the relative propagator weights, true. allows a possibility to override the global mode WeakZ0:gmZmode for a specific process. The global mode normally is used to switch off parts of the gamma^*/Z^0 propagator for test purposes. The above local mode is useful for processes where a Z^0 really is that and nothing more, such as q qbar -> H^0 Z^0. The default value -1 returned by gmZmode() ensures that the global mode is used, while 0 gives full gamma^*/Z^0 interference, 1 gamma^* only and 2 Z^0 only.

      Access to a process

      Once you have implemented a class, it is straightforward to make use of it in a run. Assume you have written a new class MySigma, which inherits from Sigma1Process, Sigma2Process or Sigma3Process, which in their turn inherit from SigmaProcess. You then create an instance of this class and hand it in to a pythia object with
            SigmaProcess* mySigma = new MySigma();
            pythia.setSigmaPtr( mySigma); 
      
      If you have several processes you can repeat the procedure any number of times. When pythia.init(...) is called these processes are initialized along with any internal processes you may have switched on, and treated in exactly the same manner. The pythia.next() will therefore generate a mix of the different kinds of processes without distinction. See also the Program Flow description.

      If the code should be of good quality and general usefulness, it would be simple to include it as a permanently available process in the standard program distribution. The final step of that integration ought to be left for the PYTHIA authors, but here is a description of what is required.

      A flag has to be defined, that allows the process to be switched on; by default it should always be off. The name of the flag should be chosen of the type model:process. Here the model would be related to the general scenario considered, e.g. Compositeness, while process would specify instate and outstate, separated by a 2 (= to), e.g. ug2u*g. When several processes are implemented and "belong together" it is also useful to define a model:all switch that affects all the separate processes.

      The flags should normally be stored in the ProcessSelection.xml file or one of its daughters for a specific kind of processes. This is to make them easily found by users. You could create and use your own .xml file, so long as you then add that name to the list of files in the Index.xml file. (If not, the flags would never be created and the program would not work.)

      In the ProcessContainer.c file, the SetupContainers::init() method needs to be expanded to create instances of the processes switched on. This code is fairly repetitive, and should be easy to copy and modify from the code already there. The basic structure is
      (i) check whether a process is requested by the user and, if so,
      (ii) create an instance of the matrix-element class,
      (iii)create a container for the matrix element and its associated phase-space handling, and
      (iv) add the container to the existing process list.

      Two minor variations are possible. One is that a set of related processes are lumped inside the the same initial check, i.e. are switched on all together. The second is that the matrix-element constructor may take arguments, as specified by you (see above). If so, the same basic matrix element may be recycled for a set of related processes, e.g. one for a composite u and one for a composite d. Obviously these variations may be combined. pythia8-8.1.80.orig/xmldoc/LeftRightSymmetryProcesses.xml0000444000175000017500000001412012217346303021667 0ustar sunsun

      Left-Right-Symmetry Processes

      At current energies, the world is left-handed, i.e. the Standard Model contains an SU(2)_L group. Left-right symmetry at some larger scale implies the need for an SU(2)_R group. Thus the particle content is expanded by right-handed Z_R^0 and W_R^+- and right-handed neutrinos. The Higgs fields have to be in a triplet representation, leading to doubly-charged Higgs particles, one set for each of the two SU(2) groups. Also the number of neutral and singly-charged Higgs states is increased relative to the Standard Model, but a search for the lowest-lying states of this kind is no different from e.g. the freedom already accorded by the MSSM Higgs scenarios.

      PYTHIA implements the scenario of Hui97.

      The W_R^+- has been implemented as a simple copy of the ordinary W^+-, with the exception that it couples to right-handed neutrinos instead of the ordinary left-handed ones. Thus the standard CKM matrix is used in the quark sector, and the same vector and axial coupling strengths, leaving only the mass as free parameter. The Z_R^0 implementation (without interference with the photon or the ordinary Z^0) allows decays both to left- and right-handed neutrinos, as well as other fermions, according to one specific model ansatz. Obviously both the W_R^+- and the Z_R^0 descriptions are likely to be simplifications, but provide a starting point.

      For the doubly-charged Higgs bosons, the main decay modes implemented are H_L^++ -> W_L^+ W_L^+, l_i^+ l_j^+ (i, j generation indices) and H_R^++ -> W_R^+ W_R^+, l_i^+ l_j^+.

      The right-handed neutrinos can be allowed to decay further. Assuming them to have a mass below that of W_R^+-, they decay to three-body states via a virtual W_R^+-, nu_Rl -> l+- f fbar', where both lepton charges are allowed owing to the Majorana character of the neutrinos. If there is a significant mass splitting, also sequential decays nu_Rl -> l+- l'-+ nu'_Rl are allowed. Currently the decays are isotropic in phase space. If the neutrino masses are close to or above the W_R^ ones, this description has to be substituted by a sequential decay via a real W_R^ (not implemented, but actually simpler to do than the one here).

      Production processes

      A few different production processes have been implemented, which normally would not overlap and therefore could be run together. Common switch for the group of implemented processes within a left-right-symmetric scenario. Scatterings f fbar -> Z_R^0. Code 3101. Scatterings W_R^+. Code 3102. Scatterings l_i l_j -> H_L^--. Code 3121. Scatterings l_i gamma -> H_L^-- e^+. Code 3122. Scatterings l_i gamma -> H_L^-- mu^+. Code 3123. Scatterings l_i gamma -> H_L^-- tau^+. Code 3124. Scatterings f_1 f_2 -> H_L^-- f_3 f_4 via WW fusion. Code 3125. Scatterings f fbar -> H_L^++ H_L^--. Code 3126. Scatterings l_i l_j -> H_R^--. Code 3141. Scatterings l_i gamma -> H_R^-- e^+. Code 3142. Scatterings l_i gamma -> H_R^-- mu^+. Code 3143. Scatterings l_i gamma -> H_R^-- tau^+. Code 3144. Scatterings f_1 f_2 -> H_R^-- f_3 f_4 via WW fusion. Code 3145. Scatterings f fbar -> H_R^++ H_L^--. Code 3146.

      Parameters

      The basic couplings of the model are lefthanded coupling g_L = e / sin(theta). righthanded coupling g_R, assumed the same as g_L. vacuum expectation value v_L (in GeV) for the left-triplet.

      The corresponding vacuum expectation value v_R is assumed given by v_R = sqrt(2) M_WR / g_R and is not stored explicitly.

      The Yukawa couplings of a lepton pair to a H^--, assumed the same for H_L^-- and H_R^--, is described by a symmetric 3-by-3 matrix. The default matrix is dominated by the diagonal elements and especially by the tau tau one. Yukawa coupling for H^-- -> e- e-. Yukawa coupling for H^-- -> mu- e-. Yukawa coupling for H^-- -> mu- mu-. Yukawa coupling for H^-- -> tau- e-. Yukawa coupling for H^-- -> tau- mu-. 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      User Hooks

      Sometimes it may be convenient to step in during the generation process: to modify the built-in cross sections, to veto undesirable events or simply to collect statistics at various stages of the evolution. There is a base class UserHooks that gives you this access at a few selected places. This class in itself does nothing; the idea is that you should write your own derived class for your task. One simple derived class (SuppressSmallPT) comes with the program, mainly as illustration, and the main10.cc program provides a complete (toy) example how a derived class could be set up and used.

      There are six sets of routines, that give you different kinds of freedom. They are, in no particular order:
      (i) Ones that give you access to the event record in between the process-level and parton-level steps, or in between the parton-level and hadron-level ones. You can study the event record and decide whether to veto this event.
      (ii) Ones that allow you to set a scale at which the combined parton-level MPI+ISR+FSR downwards evolution in pT is temporarily interrupted, so the event can be studied and either vetoed or allowed to continue the evolution.
      (iii) Ones that allow you to to study the event after the first few ISR/FSR emissions, or first few MPI, so the event can be vetoed or allowed to continue the evolution.
      (iv) Ones that allow you to study the latest initial- or final-state emission and veto that emission, without vetoing the event as a whole.
      (v) Ones that give you access to the properties of the trial hard process, so that you can modify the internal Pythia cross section, alternatively the phase space sampling, by your own correction factors.
      (vi) Ones that allow you to reject the decay sequence of resonances at the process level.
      (vii) Ones that let you set the scale of shower evolution, specifically for matching in resonance decays.
      They are described further in the following numbered subsections.

      All the possibilities above can be combined freely and also be combined with the standard flags. An event would then survive only if it survived each of the possible veto methods. There are no hidden interdependencies in this game, but of course some combinations may not be particularly meaningful. For instance, if you set PartonLevel:all = off then the doVetoPT(...) and doVetoPartonLevel(...) locations in the code are not even reached, so they would never be called.

      The effect of the vetoes of types (i), (ii) and (iii) can be studied in the output of the Pythia::statistics() method. The "Selected" column represents the number of events that were found acceptable by the internal Pythia machinery, whereas the "Accepted" one are the events that also survived the user cuts. The cross section is based on the latter number, and so is reduced by the amount associated by the vetoed events. Also type (v) modifies the cross section, while types (iv), (vi) and (vii) do not.

      A warning. When you program your own derived class, do remember that you must exactly match the arguments of the base-class methods you overload. If not, your methods will be considered as completely new ones, and compile without any warnings, but not be used inside Pythia. So, at the debug stage, do insert some suitable print statements to check that the new methods are called (and do what they should).

      The basic components

      For a derived UserHooks class to be called during the execution, a pointer to an object of this class should be handed in with the
      Pythia::setUserHooksPtr( UserHooks*)
      method. The first step therefore is to construct your own derived class, of course. This must contain a constructor and a destructor. The initPtr method comes "for free", and is set up without any intervention from you. The constructor and destructor do not need to do anything. this (non-virtual) method is automatically called during the initialization stage to set several useful pointers, and to set up the workEvent below. The corresponding objects can later be used to extract some useful information.
      Info: general event and run information, including some loop counters.
      Settings: the settings used to determine the character of the run.
      ParticleData: the particle data used in the event record (including workEvent below).
      Rndm: the random number generator, that you could also use in your code.
      BeamParticle: the beamAPtr and beamBPtr beam particles contain info on partons extracted from the two incoming beams, on the PDFs used, and more. In cases when diffraction is simulated, also special Pomeron beams beamPomAPtr and beamPomBPtr are introduced, for the Pomerons residing inside the respective proton.
      CoupSM: Standard Model couplings.
      PartonSystems: the list of partons that belong to each individual subcollision system.
      SigmaTotal: total/elastic/diffractive cross section parametrizations.

      Next you overload the desired methods listed in the sections below. These often come in pairs or triplets, where the first must return true for the last method to be called. This latter method typically hands you a reference to the event record, which you then can use to decide whether or not to veto. Often the event record can be quite lengthy and difficult to overview. The following methods and data member can then come in handy. is a protected method that you can make use of in your own methods to extract a simplified list of the hard process, where all resonance decay chains are omitted. Intended for the can/doVetoProcessLevel routines. Note that the normal process-level generation does include resonance decays. That is, if a top quark is produced in the hard process, then also decays such as t -> b W+, W+ -> u dbar will be generated and stored in process. The omitResonanceDecays routine will take the input process and copy it to workEvent (see below), minus the resonance decay chains. All particles produced in the hard process, such as the top, will be considered final-state ones, with positive status and no daughters, just as it is before resonances are allowed to decay.
      (In the PartonLevel routines, these decay chains will initially not be copied from process to event. Instead the combined MPI, ISR and FSR evolution is done with the top above as final particle. Only afterwards will the resonance decay chains be copied over, with kinematics changes reflecting those of the top, and showers in the decays carried out.)
      For the default finalOnly = false the beam particles and incoming partons are retained, so the event looks like a normal event record up to the point of resonance decays, with a normal history setup.
      With finalOnly = true only the final-state partons are retained in the list. It therefore becomes similar in functionality to the subEvent method below, with the difference that subEvent counts the decay products of the resonances as the final state, whereas here the resonances themselves are the final state. Since the history has been removed in this option, mother1() and mother2() return 0, while daughter1() and daughter2() both return the index of the same parton in the original event record.
      is a protected method that you can make use of in your own methods to extract a brief list of the current partons of interest, with all irrelevant ones omitted. It is primarily intended to track the evolution at the parton level, notably the shower evolution of the hardest (i.e. first) interaction.
      For the default isHardest = true only the outgoing partons from the hardest interaction (including the partons added to it by ISR and FSR) are extracted, as relevant e.g. for doVetoPT( iPos, event) with iPos = 0 - 4. With isHardest = false instead the outgoing partons of the latest "subprocess" are extracted, as relevant when iPos = 5, where it corresponds to the outgoing partons in the currently considered decay.
      The method also works at the process level, but there simply extracts all final-state partons in the event, and thus offers no extra functionality.
      The result is stored in workEvent below. Since the history has been removed, mother1() and mother2() return 0, while daughter1() and daughter2() both return the index of the same parton in the original event record (event; possibly process), so that you can trace the full history, if of interest.
      This protected class member contains the outcome of the above omitResonanceDecays(...) and subEvent(...) methods. Alternatively you can use it for whatever temporary purposes you wish. You are free to use standard operations, e.g. to boost the event to its rest frame before analysis, or remove particles that should not be analyzed. The workEvent can also be sent on to a jet clustering algorithm.

      (i) Interrupt between the main generation levels

      This routine is called by Pythia::init(), after the beams have been set up, but before any other initialisation. Therefore, at this stage, it is still possible to modify settings (apart from Beams:*) and particle data. This is mainly intended to be used in conjunction with Les Houches Event files, where headers are read in during beam initialisation, see the header functions in the Info class. In the base class this method returns true. By returning false, PYTHIA initialisation will be aborted. In the base class this method returns false. If you redefine it to return true then the method doVetoProcessLevel(...) will be called immediately after a hard process (and associated resonance decays) has been selected and stored in the process event record.
      At this stage, the process record typically contains the two beams in slots 1 and 2, the two incoming partons to the hard process in slots 3 and 4, the N (usually 1, 2 or 3) primary produced particles in slots 5 through 4 + N, and thereafter recursively the resonance decay chains, if any. Use the method omitResonanceDecays(...) if you want to skip these decay chains. There are exceptions to this structure, for soft QCD processes (where the partonic process may not yet have been selected at this stage), and when a second hard process has been requested (where two hard processes are bookkept). In general it is useful to begin the development work by listing a few process records, to clarify what the structure is for the cases of interest.
      can optionally be called, as described above. You can study the process event record of the hard process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next(). Warning: Normally you should not modify the process event record. However, for some matrix-element-matching procedures it may become unavoidable. If so, be very careful, since there are many pitfalls. Only to give one example: if you modify the incoming partons then also the information stored in the beam particles may need to be modified. Note: the above veto is different from setting the flag PartonLevel:all = off. Also in the latter case the event generation will stop after the process level, but an event generated up to this point is considered perfectly acceptable. It can be studied and it contributes to the cross section. That is, PartonLevel:all = off is intended for simple studies of hard processes, where one can save a lot of time by not generating the rest of the story. By contrast, the doVetoProcessLevel() method allows you to throw away uninteresting events at an early stage to save time, but those events that do survive the veto are allowed to develop into complete final states (unless flags have been set otherwise). In the base class this method returns false. If you redefine it to return true then the method doVetoPartonLevel(...) will be called immediately after the parton level has been generated and stored in the event event record. Thus showers, multiparton interactions and beam remnants have been set up, but hadronization and decays have not yet been performed. This is already a fairly complete event, possibly with quite a complex parton-level history. Therefore it is usually only meaningful to study the hardest interaction, e.g. using subEvent(...) introduced above, or fairly generic properties, such as the parton-level jet structure. can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next(). Note: the above veto is different from setting the flag HadronLevel:all = off. Also in the latter case the event generation will stop after the parton level, but an event generated up to this point is considered perfectly acceptable. It can be studied and it contributes to the cross section. That is, HadronLevel:all = off is intended for simple studies of complete partonic states, where one can save time by not generating the complete hadronic final state. By contrast, the doVetoPartonLevel() method allows you to throw away uninteresting events to save time that way, but those events that do survive the veto are allowed to develop into complete final states (unless flags have been set otherwise). is very similar to canVetoPartonLevel() above, except that the chance to veto appears somewhat earlier in the generation chain, after showers and multiparton interactions, but before the beam remnants and resonance decays have been added. It is therefore somewhat more convenient for many matrix element strategies, where the primordial kT added along with the beam remnants should not be included. is very similar to doVetoPartonLevel(...) above, but the veto can be done earlier, as described for canVetoPartonLevelEarly().

      (ii) Interrupt during the parton-level evolution, at a pT scale

      During the parton-level evolution, multiparton interactions (MPI), initial-state radiation (ISR) and final-state radiation (FSR) are normally evolved downwards in one interleaved evolution sequence of decreasing pT values. For some applications, e.g matrix-element-matching approaches, it may be convenient to stop the evolution temporarily when the "hard" emissions have been considered, but before continuing with the more time-consuming soft activity. Based on these hard partons one can make a decision whether the event at all falls in the intended event class, e.g. has the "right" number of parton-level jets. If yes then, as for the methods above, the evolution will continue all the way up to a complete event. Also as above, if no, then the event will not be considered in the final cross section.

      Recall that the new or modified partons resulting from a MPI, ISR or FSR step are always appended to the end of the then-current event record. Previously existing partons are not touched, except for the status, mother and daughter values, which are updated to reflect the modified history. It is therefore straightforward to find the partons associated with the most recent occurrence.
      An MPI results in four new partons being appended, two incoming and two outgoing ones.
      An ISR results in the whole affected system being copied down, with one of the two incoming partons being replaced by a new one, and one more outgoing parton.
      An FSR results in three new partons, two that come from the branching and one that takes the recoil.
      The story becomes more messy when rescattering is allowed as part of the MPI machinery. Then there will not only be a new system, as outlined above, but additionally some existing systems will undergo cascade effects, and be copied down with changed kinematics.

      In this subsection we outline the possibility to interrupt at a given pT scale, in the next to interrupt after a given number of emissions. In the base class this method returns false. If you redefine it to return true then the method doVetoPT(...) will interrupt the downward evolution at scaleVetoPT(). In the base class this method returns 0. You should redefine it to return the pT scale at which you want to study the event. can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next(). is the position/status when the routine is called, information that can help you decide your course of action: when no MPI, ISR or FSR occurred above the veto scale; when inside the interleaved MPI + ISR + FSR evolution, after an MPI process; when inside the interleaved MPI + ISR + FSR evolution, after an ISR emission; when inside the interleaved MPI + ISR + FSR evolution, after an FSR emission; for the optional case where FSR is deferred from the interleaved evolution and only considered separately afterward (then alternative 3 would never occur); is for subsequent resonance decays, and is called once for each decaying resonance in a chain such as t -> b W, W -> u dbar. the event record contains a list of all partons generated so far, also including intermediate ones not part of the "current final state", and also those from further multiparton interactions. This may not be desirable for comparisons with matrix-element calculations. You may want to make use of the subEvent(...) method below to obtain a simplified event record workEvent.

      (iii) Interrupt during the parton-level evolution, after a step

      These options are closely related to the ones above in section (ii), so we do not repeat the introduction, nor the possibilities to study the event record, also by using subEvent(...) and workEvent. What is different is that the methods in this section give access to the event as it looks like after each of the first few steps in the downwards evolution, irrespective of the pT scales of these branchings. Furthermore, it is here assumed that the focus normally is on the hardest subprocess, so that ISR/FSR emissions associated with additional MPI's are not considered. For MPI studies, however, a separate simpler alternative is offered to consider the event after a given number of interactions. In the base class this method returns false. If you redefine it to return true then the method doVetoStep(...) will interrupt the downward ISR and FSR evolution the first numberVetoStep() times. Returns the number of steps n each of ISR and FSR, for the hardest interaction, that you want to be able to study. That is, the method will be called after the first n ISR emissions, irrespective of the number of FSR ones at the time, and after the first n FSR emissions, irrespective of the number of ISR ones. The number of steps defaults to the first one only, but you are free to pick another value. Note that double diffraction is handled as two separate Pomeron-proton collisions, and thus has two sequences of emissions. can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next(). is the position/status when the routine is called, information that can help you decide your course of action. Agrees with options 2 - 5 of the doVetoPT(...) routine above, while options 0 and 1 are not relevant here. is the number of ISR emissions in the hardest process so far. For resonance decays, iPos = 5, it is 0. is the number of FSR emissions in the hardest process so far. For resonance decays, iPos = 5, it is the number of emissions in the currently studied system. the event record contains a list of all partons generated so far, also including intermediate ones not part of the "current final state", and also those from further multiparton interactions. This may not be desirable for comparisons with matrix-element calculations. You may want to make use of the subEvent(...) method above to obtain a simplified event record. In the base class this method returns false. If you redefine it to return true then the method doVetoMPIStep(...) will interrupt the downward MPI evolution the first numberVetoMPIStep() times. Returns the number of steps in the MPI evolution that you want to be able to study, right after each new step has been taken and the subcollision has been added to the event record. The number of steps defaults to the first one only, but you are free to pick another value. Note that the hardest interaction of an events counts as the first multiparton interaction. For most hard processes it thus at the first step offers nothing not available with the VetoProcessLevel functionality above. For the minimum-bias and diffractive systems the hardest interaction is not selected at the process level, however, so there a check after the first multiparton interaction offers new functionality. Note that double diffraction is handled as two separate Pomeron-proton collisions, and thus has two sequences of interactions. Also, if you have set up a second hard process then a check is made after these first two, and the first interaction coming from the MPI machinery would have sequence number 3. can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next(). is the number of MPI subprocesses has occurred so far. the event record contains a list of all partons generated so far, also including intermediate ones not part of the "current final state", e.g. leftovers from the ISR and FSR evolution of previously generated systems. The most recently added one has not had time to radiate, of course.

      (iv) Veto emissions

      The methods in this group are intended to allow the veto of an emission in ISR, FSR or MPI, without affecting the evolution in any other way. If an emission is vetoed, the event record is "rolled back" to the way it was before the emission occurred, and the evolution in pT is continued downwards from the rejected value. The decision can be based on full knowledge of the kinematics of the shower branching or MPI.

      To identify where shower emissions originated, the ISR/FSR veto routines are passed the system from which the radiation occurred, according to the Parton Systems class (see Advanced Usage). Note, however, that inside the veto routines only the event record has been updated; all other information, including the Parton Systems, reflects the event before the shower branching or MPI has taken place. In the base class this method returns false. If you redefine it to return true then the method doVetoISREmission(...) will interrupt the initial-state shower immediately after each emission and allow that emission to be vetoed. can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the emission, true, or not, false. If you veto, then the latest emission is removed from the event record. In either case the evolution of the shower will continue from the point where it was left off. is the size of the event record before the latest emission was added to it. It will also become the new size if the emission is vetoed. the event record contains a list of all partons generated so far. Of special interest are the ones associated with the most recent emission, which are stored in entries from sizeOld through event.size() - 1 inclusive. If you veto the emission these entries will be removed, and the history info in the remaining partons will be restored to a state as if the emission had never occurred. the system where the radiation occurs, according to Parton Systems. In the base class this method returns false. If you redefine it to return true then the method doVetoFSREmission(...) will interrupt the final-state shower immediately after each emission and allow that emission to be vetoed. can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the emission, true, or not, false. If you veto, then the latest emission is removed from the event record. In either case the evolution of the shower will continue from the point where it was left off. is the size of the event record before the latest emission was added to it. It will also become the new size if the emission is vetoed. the event record contains a list of all partons generated so far. Of special interest are the ones associated with the most recent emission, which are stored in entries from sizeOld through event.size() - 1 inclusive. If you veto the emission these entries will be removed, and the history info in the remaining partons will be restored to a state as if the emission had never occurred. the system where the radiation occurs, according to Parton Systems. true if the emission takes place in a resonance decay, subsequent to the hard process. In the base class this method returns false. If you redefine it to return true then the method doVetoMPIEmission(...) will interrupt the MPI machinery immediately after each multiparton interaction and allow it to be vetoed. can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the MPI, true, or not, false. If you veto, then the latest MPI is removed from the event record. In either case the interleaved evolution will continue from the point where it was left off. is the size of the event record before the latest MPI was added to it. It will also become the new size if the MPI is vetoed. the event record contains a list of all partons generated so far. Of special interest are the ones associated with the most recent MPI, which are stored in entries from sizeOld through event.size() - 1 inclusive. If you veto the MPI these entries will be removed.

      (v) Modify cross-sections or phase space sampling

      This section addresses two related but different topics. In both cases the sampling of events in phase space is modified, so that some regions are more populated while others are depleted. In the first case, this is assumed to be because the physical cross section should be modified relative to the built-in Pythia form. Therefore not only the relative population of phase space is changed, but also the integrated cross section of the process. In the second case the repopulation is only to be viewed as a technical trick to sample some phase-space regions better, so as to reduce the statistical error. There each event instead obtains a compensating weight, the inverse of the differential cross section reweighting factor, in such a way that the integrated cross section is unchanged. Below these two cases are considered separately, but note that they share many points. In the base class this method returns false. If you redefine it to return true then the method multiplySigmaBy(...) will allow you to modify the cross section weight assigned to the current event. when called this method should provide the factor by which you want to see the cross section weight of the current event modified. If you return unity then the normal cross section is obtained. Note that, unlike the methods above, these modifications do not lead to a difference between the number of "selected" events and the number of "accepted" ones, since the modifications occur already before the "selected" level. The integrated cross section of a process is modified, of course. Note that the cross section is only modifiable for normal hard processes. It does not affect the cross section in further multiparton interactions, nor in elastic/diffractive/minimum-bias events. : what makes this routine somewhat tricky to write is that the hard-process event has not yet been constructed, so one is restricted to use the information available in the phase-space and cross-section objects currently being accessed. Which of their methods are applicable depends on the process, in particular the number of final-state particles. The multiplySigmaBy code in UserHooks.cc contains explicit instructions about which methods provide meaningful information, and so offers a convenient starting point. : this flag is true when the method is called from within the event-generation machinery and false when it is called at the initialization stage of the run, when the cross section is explored to find a maximum for later Monte Carlo usage. Cross-section modifications should be independent of this flag, for consistency, but if multiplySigmaBy(...) is used to collect statistics on the original kinematics distributions before cuts, then it is important to be able to exclude the initialization stage from comparisons.

      One derived class is supplied as an example how this facility can be used to reweight cross sections in the same spirit as is done with QCD cross sections for the minimum-bias/underlying-event description: suppress small-pT production for 2 -> 2 processes only, while leaving other processes unaffected. The basic suppression factor is pT^4 / ((k*pT0)^2 + pT^2)^2, where pT refers to the current hard subprocess and pT0 is the same energy-dependent dampening scale as used for multiparton interactions. This class contains canModifySigma() and multiplySigmaBy() methods that overload the base class ones. The optional arguments of the constructor provides further variability. corresponds to the additional factor k in the above formula. It is by default equal to 1 but can be used to explore deviations from the expected value. if this number n is bigger than the default 0, the corresponding number of alpha_strong factors is also reweighted from the normal renormalization scale to a modified one, i.e. a further suppression factor ( alpha_s((k*pT0)^2 + Q^2_ren) / alpha_s(Q^2_ren) )^n is introduced. regulates which kind of new alpha_strong value is evaluated for the numerator in the above expression. It is by default the same as set for multiparton interactions (i.e. same starting value at M_Z and same order of running), but if false instead the one for hard subprocesses. The denominator alpha_s(Q^2_ren) is always the value used for the "original", unweighted cross section.

      The second main case of the current section involves three methods, as follows. In the base class this method returns false. If you redefine it to return true then the method biasSelectionBy(...) will allow you to modify the phase space sampling, with a compensating event weight, such that the cross section is unchanged. You cannot combine this kind of reweighting with the selection of a second hard process. when called this method should provide the factor by which you want to see the phase space sampling of the current event modified. Events are assigned a weight being the inverse of this, such that the integrated cross section of a process is unchanged. Note that the selection is only modifiable for normal hard processes. It does not affect the selection in further multiparton interactions, nor in elastic/diffractive/minimum-bias events. : what makes this routine somewhat tricky to write is that the hard-process event has not yet been constructed, so one is restricted to use the information available in the phase-space and cross-section objects currently being accessed. Which of their methods are applicable depends on the process, in particular the number of final-state particles. The biasSelectionBy code in UserHooks.cc contains explicit instructions about which methods provide meaningful information, and so offers a convenient starting point. : this flag is true when the method is called from within the event-generation machinery and false when it is called at the initialization stage of the run, when the cross section is explored to find a maximum for later Monte Carlo usage. Cross-section modifications should be independent of this flag, for consistency, but if biasSelectionBy(...) is used to collect statistics on the original kinematics distributions before cuts, then it is important to be able to exclude the initialization stage from comparisons. Returns the weight you should assign to the event, to use e.g. when you histogram results. It is the exact inverse of the weight you used to modify the phase-space sampling, a weight that must be stored in the selBias member variable, such that this routine can return 1/selBias. The weight is also returned by the Info::weight() method, which may be more convenient to use.

      (vi) Reject the decay sequence of resonances

      Resonance decays are performed already at the process level, as an integrated second step of the hard process itself. One reason is that the matrix element of many processes encode nontrivial decay angular distributions. Another is to have equivalence with Les Houches input, where resonance decays typically are provided from the onset. The methods in this section allow you to veto that decay sequence and try a new one. Unlike the veto of the whole process-level step, in point (i), the first step of the hard process is retained, i.e. where the resonances are produced. For this reason the cross section is not affected here but, depending on context, you may want to introduce your own counters to check how often a new set of decay modes and kinematics is selected, and correct accordingly.

      The main method below is applied after all decays. For the production of a t tbar pair this typically means after four decays, namely those of the t, the tbar, the W+ and the W-. If Les Houches events are processed, the rollback is to the level of the originally read events. For top, that might mean either to the tops, or to the W bosons, or no rollback at all, depending on how the process generation was set up. In the base class this method returns false. If you redefine it to return true then the method doVetoResonanceDecays(...) will be called immediately after the resonance decays have been selected and stored in the process event record, as described above for canVetoProcessLevel(). can optionally be called, as described above. You can study the process event record of the hard process. Based on that you can decide whether to reject the sequence of resonance decays that was not already fixed by the production step of the hard process (which can vary depending on how a process has been set up, see above). If you veto, then a new resonance decay sequence is selected, but the production step remains unchanged. The cross section remains unaffected by this veto, for better or worse. Warning: Normally you should not modify the process event record. However, as an extreme measure, parts or the complete decay chain could be overwritten. If so, be very careful.

      (vii) Modify scale in shower evolution

      The choice of maximum shower scale in resonance decays is normally not a big issue, since the shower here is expected to cover the full phase space. In some special cases a matching scheme is intended, where hard radiation is covered by matrix elements, and only softer by showers. The below two methods support such an approach. Note that the two methods are not used in the TimeShower class itself, but when showers are called from the PartonLevel generation. Thus user calls directly to TimeShower are not affected. In the base class this method returns false. If you redefine it to return true then the method scaleResonance(...) will set the initial scale of downwards shower evolution. can optionally be called, as described above. You should return the maximum scale, in GeV, from which the shower evolution will begin. The base class method returns 0, i.e. gives no shower evolution at all. You can study, but not modify, the event event record of the partonic process to check which resonance is decaying, and into what. is the location in the event record of the resonance that decayed to the particles that now will shower. the event record contains a list of all partons generated so far, specifically the decaying resonance and its immediate decay products.
      pythia8-8.1.80.orig/xmldoc/pomH1JetsGluon.data0000444000175000017500000034714412217346316017311 0ustar sunsun-6.907755E+00-6.837980E+00-6.768205E+00-6.698429E+00-6.628654E+00-6.558879E+00 -6.489103E+00-6.419328E+00-6.349553E+00-6.279778E+00-6.210002E+00-6.140227E+00 -6.070452E+00-6.000676E+00-5.930901E+00-5.861126E+00-5.791350E+00-5.721575E+00 -5.651800E+00-5.582024E+00-5.512249E+00-5.442474E+00-5.372699E+00-5.302923E+00 -5.233148E+00-5.163373E+00-5.093597E+00-5.023822E+00-4.954047E+00-4.884271E+00 -4.814496E+00-4.744721E+00-4.674945E+00-4.605170E+00-4.535395E+00-4.465620E+00 -4.395844E+00-4.326069E+00-4.256294E+00-4.186518E+00-4.116743E+00-4.046968E+00 -3.977192E+00-3.907417E+00-3.837642E+00-3.767867E+00-3.698091E+00-3.628316E+00 -3.558541E+00-3.488765E+00-3.418990E+00-3.349215E+00-3.279439E+00-3.209664E+00 -3.139889E+00-3.070113E+00-3.000338E+00-2.930563E+00-2.860788E+00-2.791012E+00 -2.721237E+00-2.651462E+00-2.581686E+00-2.511911E+00-2.442136E+00-2.372360E+00 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      Event Analysis

      Introduction

      The routines in this section are intended to be used to analyze event properties. As such they are not part of the main event generation chain, but can be used in comparisons between Monte Carlo events and real data. They are rather free-standing, but assume that input is provided in the PYTHIA 8 Event format, and use a few basic facilities such as four-vectors. Their ordering is mainly by history; for current LHC applications the final one, SlowJet, is of special interest.

      In addition to the methods presented here, there is also the possibility to make use of external jet finders .

      Sphericity

      The standard sphericity tensor is S^{ab} = (sum_i p_i^a p_i^b) / (sum_i p_i^2) where the sum i runs over the particles in the event, a, b = x, y, z, and p without such an index is the absolute size of the three-momentum . This tensor can be diagonalized to find eigenvalues and eigenvectors.

      The above tensor can be generalized by introducing a power r, such that S^{ab} = (sum_i p_i^a p_i^b p_i^{r-2}) / (sum_i p_i^r) In particular, r = 1 gives a linear dependence on momenta and thus a collinear safe definition, unlike sphericity.

      To do sphericity analyses you have to set up a Sphericity instance, and then feed in events to it, one at a time. The results for the latest event are available as output from a few methods. create a sphericity analysis object, where is the power r defined above, i.e. gives Sphericity, and gives the linear form. tells which particles are analyzed, all final-state particles, all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and only charged final-state particles. perform a sphericity analysis, where is an object of the Event class, most likely the pythia.event one. is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
      If the routine returns false the analysis failed, e.g. if too few particles are present to analyze.

      After the analysis has been performed, a few methods are available to return the result of the analysis of the latest event: gives the sphericity (or equivalent if r is not 2), gives the aplanarity (with the same comment), gives one of the three eigenvalues for i = 1, 2 or 3, in descending order, gives the matching normalized eigenvector, as a Vec4 with vanishing time/energy component. provides a listing of the above information.

      There is also one method that returns information accumulated for all the events analyzed so far. tells the number of times analyze(...) failed to analyze events, i.e. returned false.

      Thrust

      Thrust is obtained by varying the thrust axis so that the longitudinal momentum component projected onto it is maximized, and thrust itself is then defined as the sum of absolute longitudinal momenta divided by the sum of absolute momenta. The major axis is found correspondingly in the plane transverse to thrust, and the minor one is then defined to be transverse to both. Oblateness is the difference between the major and the minor values.

      The calculation of thrust is more computer-time-intensive than e.g. linear sphericity, introduced above, and has no specific advantages except historical precedent. In the PYTHIA 6 implementation the search was sped up at the price of then not being guaranteed to hit the absolute maximum. The current implementation studies all possibilities, but at the price of being slower, with time consumption for an event with n particles growing like n^3.

      To do thrust analyses you have to set up a Thrust instance, and then feed in events to it, one at a time. The results for the latest event are available as output from a few methods. create a thrust analysis object, where tells which particles are analyzed, all final-state particles, all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and only charged final-state particles. perform a thrust analysis, where is an object of the Event class, most likely the pythia.event one. is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
      If the routine returns false the analysis failed, e.g. if too few particles are present to analyze.

      After the analysis has been performed, a few methods are available to return the result of the analysis of the latest event: gives the thrust, major, minor and oblateness values, respectively, gives the matching normalized event-axis vectors, for i = 1, 2 or 3 corresponding to thrust, major or minor, as a Vec4 with vanishing time/energy component. provides a listing of the above information.

      There is also one method that returns information accumulated for all the events analyzed so far. tells the number of times analyze(...) failed to analyze events, i.e. returned false.

      ClusterJet

      ClusterJet (a.k.a. LUCLUS and PYCLUS) is a clustering algorithm of the type used for analyses of e^+e^- events, see the PYTHIA 6 manual. All visible particles in the events are clustered into jets. A few options are available for some well-known distance measures. Cutoff distances can either be given in terms of a scaled quadratic quantity like y = pT^2/E^2 or an unscaled linear one like pT.

      Note that we have deliberately chosen not to include the e^+e^- equivalents of the Cambridge/Aachen and anti-kRT algorithms. These tend to be good at clustering the densely populated (in angle) cores of jets, but less successful for the sparsely populated transverse regions, where many jets may come to consist of a single low-momentum particle. In hadron collisions such jets could easily be disregarded, while in e^+e^- annihilation all particles derive back from the hard process.

      To do jet finding analyses you have to set up a ClusterJet instance, and then feed in events to it, one at a time. The results for the latest event are available as output from a few methods. create a ClusterJet instance, where distance measure, to be provided as a character string (actually, only the first character is necessary) the Lund pT distance, the JADE mass distance, and the Durham kT measure. tells which particles are analyzed, all final-state particles, all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and only charged final-state particles. masses assumed for the particles used in the analysis all massless, photons are massless while all others are assigned the pi+- mass, and all given their correct masses. perform or not a early preclustering step, where nearby particles are lumped together so as to speed up the subsequent normal clustering. reassign all particles to the nearest jet each time after two jets have been joined. performs a jet finding analysis, where is an object of the Event class, most likely the pythia.event one. is the cutoff joining scale, below which jets are joined. Is given in quadratic dimensionless quantities. Either yScale or pTscale must be set nonvanishing, and the larger of the two dictates the actual value. is the cutoff joining scale, below which jets are joined. Is given in linear quantities, such as pT or m depending on the measure used, but always in units of GeV. Either yScale or pTscale must be set nonvanishing, and the larger of the two dictates the actual value. the minimum number of jets to be reconstructed. If used, it can override the yScale and pTscale values. the maximum number of jets to be reconstructed. Is not used if below nJetMin. If used, it can override the yScale and pTscale values. Thus e.g. nJetMin = nJetMax = 3 can be used to reconstruct exactly 3 jets. is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
      If the routine returns false the analysis failed, e.g. because the number of particles was smaller than the minimum number of jets requested.

      After the analysis has been performed, a few ClusterJet class methods are available to return the result of the analysis: gives the number of jets found, with jets numbered 0 through size() - 1. gives a Vec4 corresponding to the four-momentum defined by the sum of all the contributing particles to the i'th jet. the number of particles that have been clustered into the i'th jet. gives the index of the jet that the particle i of the event record belongs to, provides a listing of the reconstructed jets. the number of most recent clustering scales that have been stored for readout with the next method. Normally this would be five, but less if fewer clustering steps occurred. clustering scales, with distance(0) being the most recent one, i.e. normally the highest, up to distance(4) being the fifth most recent. That is, with n being the final number of jets, ClusterJet::size(), the scales at which n+1 jets become n, n+2 become n+1, and so on till n+5 become n+4. Nonexisting clustering scales are returned as zero. The physical interpretation of a scale is as provided by the respective distance measure (Lund, JADE, Durham).

      There is also one method that returns information accumulated for all the events analyzed so far. tells the number of times analyze(...) failed to analyze events, i.e. returned false.

      CellJet

      CellJet (a.k.a. PYCELL) is a simple cone jet finder in the UA1 spirit, see the PYTHIA 6 manual. It works in an (eta, phi, eT) space, where eta is pseudorapidity, phi azimuthal angle and eT transverse energy. It will draw cones in R = sqrt(Delta-eta^2 + Delta-phi^2) around seed cells. If the total eT inside the cone exceeds the threshold, a jet is formed, and the cells are removed from further analysis. There are no split or merge procedures, so later-found jets may be missing some of the edge regions already used up by previous ones. Not all particles in the event are assigned to jets; leftovers may be viewed as belonging to beam remnants or the underlying event. It is not used by any experimental collaboration, but is closely related to the more recent and better theoretically motivated anti-kT algorithm Cac08.

      To do jet finding analyses you have to set up a CellJet instance, and then feed in events to it, one at a time. Especially note that, if you want to use the options where energies are smeared in order so emulate detector imperfections, you must hand in an external random number generator, preferably the one residing in the Pythia class. The results for the latest event are available as output from a few methods. create a CellJet instance, where the maximum +-pseudorapidity that the detector is assumed to cover. the number of equal-sized bins that the +-etaMax range is assumed to be divided into. the number of equal-sized bins that the phi range +-pi is assumed to be divided into. tells which particles are analyzed, all final-state particles, all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and only charged final-state particles. strategy to smear the actual eT bin by bin, no smearing, smear the eT according to a Gaussian with width resolution * sqrt(eT), with the Gaussian truncated at 0 and upperCut * eT, smear the e = eT * cosh(eta) according to a Gaussian with width resolution * sqrt(e), with the Gaussian truncated at 0 and upperCut * e. see above. see above. completely neglect all bins with an eT < threshold. the random-number generator used to select the smearing described above. Must be handed in for smearing to be possible. If your Pythia class instance is named pythia, then &pythia.rndm would be the logical choice. performs a jet finding analysis, where is an object of the Event class, most likely the pythia.event one. is the minimum transverse energy inside a cone for this to be accepted as a jet. is the size of the cone in (eta, phi) space drawn around the geometric center of the jet. the minimum eT in a cell for this to be acceptable as the trial center of a jet. is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
      If the routine returns false the analysis failed, but currently this is not foreseen ever to happen.

      After the analysis has been performed, a few CellJet class methods are available to return the result of the analysis: gives the number of jets found, with jets numbered 0 through size() - 1, gives the eT of the i'th jet, where jets have been ordered with decreasing eT values, gives the eta and phi coordinates of the geometrical center of the i'th jet, gives the eta and phi coordinates of the eT-weighted center of the i'th jet, gives the number of particles clustered into the i'th jet, gives a Vec4 corresponding to the four-momentum defined by the eT and the weighted center of the i'th jet, gives a Vec4 corresponding to the four-momentum defined by the sum of all the contributing cells to the i'th jet, where each cell contributes a four-momentum as if all the eT is deposited in the center of the cell, gives the invariant mass of the i'th jet, defined by the pMassive above, provides a listing of the above information (except pMassless, for reasons of space).

      There is also one method that returns information accumulated for all the events analyzed so far. tells the number of times analyze(...) failed to analyze events, i.e. returned false.

      SlowJet

      SlowJet is a simple program for doing jet finding according to either of the kT, anti-kT, and Cambridge/Aachen algorithms, in a cylindrical coordinate frame. The name is obviously an homage to the FastJet program Cac06, Cac12. That package contains many more algorithms, with many more options, and, above all, is much faster. Therefore SlowJet is not so much intended for massive processing of data or Monte Carlo files as for simple first tests. Nevertheless, within the advertised capabilities of SlowJet, it has been checked to find identically the same jets as FastJet. The time consumption typically is around or below that to generate an LHC pp event in the first place, so is not prohibitive. But the time rises rapidly for large multiplicities, so obviously SlowJet can not be used for tricks like distributing a dense grid of pseudoparticles to be able to define jet areas, like FastJet can, and also not for events with much pileup or other noise.

      The recent introduction of fjcore, containing the core functionality of FastJet in a very much smaller package, has changed the conditions. It now is possible (even encouraged by the authors) to distribute the two fjcore files as part of the PYTHIA package. Therefore the SlowJet class doubles as a convenient front end to fjcore, managing the conversion back and forth between PYTHIA and FastJet variables. Some applications may still benefit from using the native codes, but the default now is to let SlowJet call on fjcore for the jet finding.

      The first step is to decide which particles should be included in the analysis, and with what four-momenta. The SlowJet constructor allows to pick a maximum pseudorapidity defined by the extent of the assumed detector, to pick among some standard options of which particles to analyze, and to allow for some standard mass assumptions, like that all charged particles have the pion mass. Obviously this is only a restricted set of possibilities.

      Full flexibility can be obtained by deriving from the base class SlowJetHook to write your own include method. This will be presented with one final-state particle at a time, and should return true for those particles that should be analyzed. It is also possible to return modified four-momenta and masses, to take into account detector smearing effects or particle identity misassignments, but you must respect E^2 - p^2 = m^2.

      Alternatively you can modify the event record itself, or a copy of it (if you want to keep the original intact). For instance, only final particles are considered in the analysis, i.e. particles with positive status code, so negative status code should then be assigned to those particles that you do not want to see analyzed. Again four-momenta and masses can be modified, subject to E^2 - p^2 = m^2.

      The jet reconstructions is then based on sequential recombination with progressive removal, using the E recombination scheme. To be more specific, the algorithm works as follows.

      1. Each particle to be analyzed defines an original cluster. It has a well-defined four-momentum and mass at input. From this information the triplet (pT, y, phi) is calculated, i.e. the transverse momentum, rapidity and azimuthal angle of the cluster.
      2. Define distance measures of all clusters i to the beam d_iB = pT_i^2p and of all pairs (i,j) relative to each other d_ij = min( pT_i^2p, pT_j^2p) DeltaR_ij^2 / R^2 where DeltaR_ij^2 = (y_i - y_j)^2 + (phi_i - phi_j)^2. The jet algorithm is determined by the user-selected p value, where p = -1 corresponds to the anti-kT one, p = 0 to the Cambridge/Aachen one and p = 1 to the kT one. Also R is chosen by the user, to give an approximate measure of the size of jets. However, note that jets need not have a circular shape in (y, phi) space, so R can not straight off be interpreted as a jet radius.
      3. Find the smallest of all d_iB and d_ij.
      4. If this is a d_iB then cluster i is removed from the clusters list and instead added to the jets list. Optionally, a pTjetMin requirement is imposed, where only clusters with pT > pTjetMin are added to the jets list. If so, some of the analyzed particles will not be part of any final jet.
      5. If instead the smallest measure is a d_ij then the four-momenta of the i and j clusters are added to define a single new cluster. Convert this four-momentum to a new (pT, y, phi) triplet and update the list of d_iB and d_ij.
      6. Return to step 3 until no clusters remain.

      To do jet finding analyses you first have to set up a SlowJet instance, where the arguments of the constructor specifies the details of the subsequent analyses. Thereafter you can feed in events to it, one at a time, and have them analyzed by the analyze method. Information on the resulting jets can be extracted by a few different methods. The minimal procedure only requires one call per event to do the analysis. We will begin by presenting it, and only afterwards some extensions. create a SlowJet instance, where tells (half) the power of the transverse-momentum dependence of the distance measure, the anti-kT algorithm, the Cambridge/Aachen algorithm, and the kT algorithm. the R size parameter, which is crudely related to the radius of the jet cone in (y, phi) space around the center of the jet. the minimum transverse momentum required for a cluster to become a jet. By default all clusters become jets, and therefore all analyzed particles are assigned to a jet. For comparisons with perturbative QCD, however, it is only meaningful to consider jets with a significant pT. the maximum +-pseudorapidity that the detector is assumed to cover. If you pick a value above 20 there is assumed to be full coverage (obviously only meaningful for theoretical studies). tells which particles are analyzed, all final-state particles, all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and only charged final-state particles. masses assumed for the particles used in the analysis all massless, photons are massless while all others are assigned the pi+- mass, and all given their correct masses. gives the possibility to send in your own selection routine for which particles should be part of the analysis; see further below on the SlowJetHook class. If this pointer is sent in nonzero, etaMax and massSet are disregarded, and select only gives the basic selection, to which the user can add further requirements. choice of code used for finding the jets. Does not affect the outcome of the analysis, but only the speed, and some more specialized options. use the fjcore package of FastJet 3.0.5. use the native SlowJet implementation, which gives a slower jet finding, but allows some extra options of step-by-step jet joining. definition of R distance between two jets. This switch is only meaningful for useFJcore = false; within the fjcore package the standard option below is always used. standard, as described above, DeltaR_ij^2 = (y_i - y_j)^2 + (phi_i - phi_j)^2. alternative, DeltaR_ij^2 = 2 (cosh(y_i - y_j) - cos(phi_i - phi_j)), which corresponds to the rim of the "deformed cone" giving a constant invariant mass between the two partons considered (for fixed masses and transverse momenta). performs a jet finding analysis, where is an object of the Event class, most likely the pythia.event one.
      If the routine returns false the analysis failed, but currently this is not foreseen ever to happen.

      After the analysis has been performed, a few SlowJet class methods are available to return the result of the analysis: gives the original number of particles (and thus clusters) that the analysis starts with. gives the number of jets found, with jets numbered 0 through sizeJet() - 1, and ordered in terms of decreasing transverse momentum values w.r.t. the beam axis, gives the transverse momentum pT of the i'th jet, gives the rapidity y and azimuthal angle phi of the center of the i'th jet (defined by the vector sum of constituent four-momenta), gives a Vec4 corresponding to the four-momentum sum of the particles assigned to the i'th jet, and the invariant mass of this four-vector, gives the number of particles clustered into the i'th jet, gives a list of the indices of the particles that have been clustered into the i'th jet, gives the index of the jet that the particle i of the event record belongs to, or -1 if there is no jet containing particle i, removes the i'th jet, provides a listing of the basic jet information from above.

      These are the basic methods. For more sophisticated usage it is possible to trace the clustering, one step at a time. It requires the native jet finding code, useFJcore = false in the constructor. If so, the setup method should be used to read in the event and find the initial smallest distance. Each subsequent doStep will then do one cluster joining and find the new smallest distance. You can therefore interrogate which clusters will be joined next before the joining actually is performed. Alternatively you can take several steps in one go, or take steps down to a predetermined number of jets plus remaining clusters. selects the particles to be analyzed, calculates initial distances, and finds the initial smallest distance. is an object of the Event class, most likely the pythia.event one.
      If the routine returns false the setup failed, but currently this is not foreseen ever to happen.
      do the next step of the clustering. This can either be that two clusters are joined to one, or that a cluster is promoted to a jet (which is discarded if its pT value is below pTjetMin).
      The routine will only return false if there are no clusters left, or if useFJcore = true.
      calls the doStep() method nStep times, if possible. Will return false if the list of clusters is emptied before then. The stored jet information is still perfectly fine; it is only the number of steps that is wrong. Will also return false if useFJcore = true. calls the doStep() method until a total of nStop jet and cluster objects remain. Will return false if this is not possible, specifically if the number of objects already is smaller than nStop when the method is called. The stored jet and cluster information is still perfectly fine; it only does not have the expected multiplicity. Will also return false if useFJcore = true. gives the total current number of jets and clusters. The jets are numbered 0 through sizeJet() - 1, while the clusters are numbered sizeJet() through sizeAll() - 1. (Internally jets and clusters are represented by two separate arrays, but are here presented in one flat range.) Note that the jets are ordered in decreasing pT, while the clusters are not ordered. When useFJcore = true there are no intermediate steps, and thus the number of clusters is zero (after jet finding).

      With this extension, the methods double pT(int i), double y(int i), double phi(int i), Vec4 p(int i), double m(int i) and int multiplicity(int i) can be used as before. Furthermore, list() generalizes provides a listing of the above information. lists both jets and clusters if true, else only jets.

      Three further methods can be used to check what will happen next. if the next step is to join two clusters, then the methods give the (i,j, d_ij) values, if instead to promote a cluster to a jet then (i, -1, d_iB). If no clusters remain then (-1, -1, 0.). Note that the cluster numbers are offset as described above, i.e. they begin at sizeJet(), which of course easily could be subtracted off. Also note that the jet and cluster lists are (moderately) reshuffled in each new step. When useFJcore = true there are no intermediate steps, and thus these methods do not return meaningul information.

      Finally, and separately, the SlowJetHook class can be used for a more smart selection of which particles to include in the analysis. For instance, isolated and/or high-pT muons, electrons and photons should presumably be identified separately at an early stage, and then not clustered to jets.

      Technically, it works like with User Hooks. That is, PYTHIA contains the base class. You write a derived class. In the main program you create an instance of this class, and hand it in to SlowJet; in this case already as part of the constructor.

      The following methods should be defined in your derived class. the constructor and destructor need not do anything, and if so you need not write your own destructor. is the main method that you will need to write. It will be called once for each final-state particle in an event, subject to the value of the select switch in the SlowJet constructor. The value select = 2 may be convenient since then you do not need to remove e.g. neutrinos yourself, but use select = 1 for full control. The method should then return true if you want to see particle included in the jet clustering, and false if not. is the index in the event record of the currently studied particle. is an object of the Event class, most likely the pythia.event one, where the currently studied particle is found. is at input the four-momentum of the currently studied particle. You can change the values, e.g. to take into account energy smearing in the detector, to define the initial cluster value, without corrupting the event record itself. is at input the mass of the currently studied particle. You can change the value, e.g. to take into account particle misidentification, to define the initial cluster value, without corrupting the event record itself. Note that the changes of pSel and mSel must be coordinated such that E^2 - p^2 = m^2 holds.

      It is also possible to define further methods of your own. One such could e.g. be called directly in the main program before the analyze method is called, to identify and bookkeep some event properties you may not want to reanalyze for each individual particle. pythia8-8.1.80.orig/xmldoc/EventStatistics.xml0000444000175000017500000001366612217346302017507 0ustar sunsun

      Event Statistics

      At the end of the run you will want to write out the final statistics on number of events generated, the corresponding cross sections and the number of errors encountered. This is done either with the pythia.stat() method or the pythia.statistics() one, assuming pythia is an instance of the Pythia class.The former method is steered entirely by settings values, see here. The latter, deprecated one instead takes two arguments: write out statistics on cross sections and errors. This is based on calls to the methods below, for the two kinds of information. if true it allows a more extensive listing than the default one, see multiparton-interactions statistics below. if true it implies that all counters, e.g on events generated and errors experienced, are reset to zero whenever the routine is called. The default instead is that all stored statistics information is unaffected by the call. Counters are automatically reset in each new Pythia::init() call, however, so the only time the reset option makes a difference is if statistics(...) is called several times in a (sub)run.

      Cross-section statistics

      The ProcessLevel::statistics() method cannot be accessed directly, but only via the Pythia::stat() and Pythia::statistics(...) calls above. When called it will loop over the list of existing processes, and for each write out name, code, the number of tried, selected and accepted events, the cross section and the estimated error on the latter. The three different event numbers are related to the Monte Carlo method used, whereby an initial upper estimate of the cross section is used to select a large number of trial phase-space points, whereof then not all survive. Rejections are normally done by the internal machinery, but can also be obtained by user hooks. Therefore:
      • tried events reflect the original number of phase-space points probed, as part of the upper estimate;
      • selected events correspond to those that survive the internal Monte-Carlo selection procedure;
      • accepted events are those that also survive the additional user cuts.
      In most runs there would be no user hooks implemented, and then the numbers of selected and of accepted events will agree. Aborted events (see below) usually appear in the selected statistics but not in the accepted one.

      For Les Houches events the total cross section will be correctly displayed; however the (optional) error value will not be used, so that the reported error will be smaller than the correct statistical ones, and often vanish completely. Furthermore, while the number of events is shown for each user process, the cross section is only for the sum of them.

      Error messages

      When Pythia is run, errors may occur, and give rise to warning messages. These may be of varying severity, as follows:
      • Abort means things went seriously wrong, and the initialization or event generation failed. In the former case it is not possible to generate events at all, in the latter the current event is flawed and should be skipped. In either case the respective method, Pythia::init() or Pythia::next(), then also returns the value false. There are occasions where an abort may be deliberate, such as when a file of Les Houches Events is read and the end of the file is reached.
      • Error normally is less severe. Typically the program will back up one step and try again. There are cases where this is not possible, in particular during the initialization and the generation of a hard process, and then the error may be followed by an abort as a direct consequence (with two separate messages).
      • Warning is even less severe. In some cases the program will try again, with good chances of success, in others no measure at all need to be taken.

      The error messages is handled by a small part of the Info class. It is handed any abort, error or warning messages during the event generation phase, and will store each distinct message, with a counter for how many times it is issued. Thus it is possible to limit the number of identical messages issued, currently hardcoded so that each kind of error message is only printed once (static const int TIMESTOPRINT = 1). This can be overridden by the calling routine, so that all messages of this kind are shown, which is particularly relevant for the initialization stage. The summary table printed by Pythia::statistics() provides a table with all the different messages issued, in alphabetical order, with the total number of times each was generated.

      Multiparton-interactions statistics

      If you call Pythia::statistics(true), i.e. with the first optional argument true, also statistics on multiparton interactions is printed, comprising a list of all allowed subprocesses with how many times each of them has been generated. For the nondiffractive process this also includes the hardest interaction, while else the hardest process is excluded from the statistics. (This is because the hardest process is of the same character and generated by the same machinery in the former case but not in the latter. Also, for the former case only, the standard statistics listing only lists nondiffractive as one single process, i.e. does not further specify the character of the hardest subprocess, so there is not any overlap between the two.)
      pythia8-8.1.80.orig/xmldoc/BoseEinsteinEffects.xml0000444000175000017500000001242712217346277020247 0ustar sunsun

      Bose-Einstein Effects

      The BoseEinstein class performs shifts of momenta of identical particles to provide a crude estimate of Bose-Einstein effects. The algorithm is the BE_32 one described in Lon95, with a Gaussian parametrization of the enhancement. We emphasize that this approach is not based on any first-principles quantum mechanical description of interference phenomena; such approaches anyway have many problems to contend with. Instead a cruder but more robust approach is adopted, wherein BE effects are introduced after the event has already been generated, with the exception of the decays of long-lived particles. The trick is that momenta of identical particles are shifted relative to each other so as to provide an enhancement of pairs closely separated, which is compensated by a depletion of pairs in an intermediate region of separation.

      More precisely, the intended target form of the BE correlations in BE_32 is f_2(Q) = (1 + lambda * exp(-Q^2 R^2)) * (1 + alpha * lambda * exp(-Q^2 R^2/9) * (1 - exp(-Q^2 R^2/4))) where Q^2 = (p_1 + p_2)^2 - (m_1 + m_2)^2. Here the strength lambda and effective radius R are the two main parameters. The first factor of the equation is implemented by pulling pairs of identical hadrons closer to each other. This is done in such a way that three-momentum is conserved, but at the price of a small but non-negligible negative shift in the energy of the event. The second factor compensates this by pushing particles apart. The negative alpha parameter is determined iteratively, separately for each event, so as to restore energy conservation. The effective radius parameter is here R/3, i.e. effects extend further out in Q. Without the dampening (1 - exp(-Q^2 R^2/4)) in the second factor the value at the origin would become f_2(0) = (1 + lambda) * (1 + alpha * lambda), with it the desired value f_2(0) = (1 + lambda) is restored. The end result can be viewed as a poor man's rendering of a rapidly dampened oscillatory behaviour in Q.

      Further details can be found in Lon95. For instance, the target is implemented under the assumption that the initial distribution in Q can be well approximated by pure phase space at small values, and implicitly generates higher-order effects by the way the algorithm is implemented. The algorithm is applied after the decay of short-lived resonances such as the rho, but before the decay of longer-lived particles.

      This algorithm is known to do a reasonable job of describing BE phenomena at LEP. It has not been tested against data for hadron colliders, to the best of our knowledge, so one should exercise some judgment before using it. Therefore by default the master switch HadronLevel:BoseEinstein is off. Furthermore, the implementation found here is not (yet) as sophisticated as the one used at LEP2, in that no provision is made for particles from separate colour singlet systems, such as W's and Z's, interfering only at a reduced rate.

      Warning: The algorithm will create a new copy of each particle with shifted momentum by BE effects, with status code 99, while the original particle with the original momentum at the same time will be marked as decayed. This means that if you e.g. search for all pi+- in an event you will often obtain the same particle twice. One way to protect yourself from unwanted doublecounting is to use only particles with a positive status code, i.e. ones for which event[i].isFinal() is true.

      Main parameters

      Include effects or not for identical pi^+, pi^- and pi^0. Include effects or not for identical K^+, K^-, K_S^0 and K_L^0. Include effects or not for identical eta and eta'. The strength parameter for Bose-Einstein effects. On physical grounds it should not be above unity, but imperfections in the formalism used may require that nevertheless. The size parameter of the region in Q space over which Bose-Einstein effects are significant. Can be thought of as the inverse of an effective distance in normal space, R = hbar / QRef, with R as used in the above equation. That is, f_2(Q) = (1 + lambda * exp(-(Q/QRef)^2)) * (...). Particle species with a width above this value (in GeV) are assumed to be so short-lived that they decay before Bose-Einstein effects are considered, while otherwise they do not. In the former case the decay products thus can obtain shifted momenta, in the latter not. The default has been picked such that both rho and K^* decay products would be modified.
      pythia8-8.1.80.orig/xmldoc/SettingsScheme.xml0000444000175000017500000004724712217346317017310 0ustar sunsun

      The Settings Scheme

      The Settings class keeps track of all the flags, modes, parameters and words used during the event generation. As such, it serves all the Pythia program elements from one central repository. Accessing it allows the user to modify the generator behaviour.

      Each Pythia object has a public member settings of the Settings class. Therefore you access the settings methods as pythia.settings.command(argument), assuming that pythia is an instance of the Pythia class. Further, for the most frequent user tasks, Pythia methods have been defined, so that pythia.command(argument) would work, see further below.

      The central section on this page is the Operation one. The preceding concepts section is there mainly to introduce the basic structure and the set of properties that can be accessed. The subsequent sections provide a complete listing of the existing public methods, which most users probably will have little interaction with.

      Concepts

      We distinguish six kinds of user-modifiable variables, by the way they have to be stored:
      1. Flags are on/off switches, and are stored as bool.
      2. Modes corresponds to a finite enumeration of separate options, and are stored as int.
      3. Parameters take a continuum of values, and are stored as double. The shorthand notation parm is used in the C++ code and XML tags.
      4. Words are simple character strings and are stored as string. No blanks or double quotation marks (") may appear inside a word, the former to simplify parsing of an input file and the latter not to cause conflicts with XML attribute delimiters. Currently the main application is to store file names.
      5. Vectors of modes take a variable length, and are stored as vector<int>. The shorthand notation mvec is used in the C++ code and XML tags. When the vector is input as a string, all the values have to be given as a comma-separated list with no blanks, to simplify parsing.
      6. Vectors of parameters take a variable length and for each element a continuum of values, and are stored as vector<double>. The shorthand notation pvec is used in the C++ code and XML tag. When the vector is input as a string, all the values have to be given as a comma-separated list with no blanks, to simplify parsing.
      Note that all shorthands have been chosen four letters long.

      In general, each variable stored in Settings is associated with four kinds of information:

      • The variable name, of the form class:name (or file:name, usually these agree), e.g. TimeShower:pTmin. The class/file part usually identifies the .xml file where the variable is defined, and the part of the program where it is used, but such a connection cannot be strictly upheld, since e.g. the same variable may be used in a few different cases (even if most of them are not).
      • The default value, set in the original declaration, and intended to represent a reasonable choice.
      • The current value, which differs from the default when the user so requests.
      • An allowed range of values, represented by meaningful minimum and maximum values. This has no sense for a flag or a word (and is not used there), is usually rather well-defined for a mode or mvec, but less so for a parm or pvec. Often the allowed range exaggerates the degree of our current knowledge, so as not to restrict too much what the user can do. One may choose not to set the lower or upper limit, in which case the range is open-ended.

      Technically, the Settings class is implemented with the help of six separate maps, one for each kind of variable, with the variable name used as key.

      Operation

      The normal flow of setting values is:

      1. When a Pythia object pythia is created, the member pythia.settings is asked to scan the files listed in the Index.xml file in the xmldoc subdirectory.

        In all of the files scanned, lines beginning with <flag, <mode, <parm, <word, <mvec or <pvec are identified, and the information on such a line is used to define a new flag, mode, parameter, word, or vector of modes or parameters. To exemplify, consider a line

        <parm name="TimeShower:pTmin" default="0.5" min="0.1" max="2.0">
        
        which appears in the TimeShower.xml file, and there defines a parameter TimeShower:pTmin with default value 0.5 GeV and allowed variation in the range 0.1 - 2.0 GeV. The min and max values are optional. Important: the values in the .xml files should not be changed, except by the PYTHIA authors. Any changes should be done with the help of the methods described below.
      2. Between the creation of the Pythia object and the init call for it, you may use several alternative methods to modify some of the default values. The same variable can be changed several times. If so, it is the last read value that counts. The two special Tune:ee and Tune:pp modes and the Print:quiet flag are expanded to change several settings in one go, but these obey the same ordering rules.

        a) Inside your main program you can directly set values with

            pythia.readString(string) 
        
        where both the variable name and the value are contained inside the character string, separated by blanks and/or a =, e.g.
            pythia.readString("TimeShower:pTmin = 1.0"); 
        
        The match of the name to the database is case-insensitive. Names that do not match an existing variable are ignored. A warning is printed, however. Strings beginning with a non-alphanumeric character, like # or !, are assumed to be comments and are not processed at all. Values below the minimum or above the maximum are set at the respective border. For bool values, the following notation may be used interchangeably: true = on = yes = ok = 1, while everything else gives false (including but not limited to false, off, no and 0).

        b) The Pythia readString(string) method actually does not do changes itself, but sends on the string either to the Settings class or to ParticleData. The former holds if the string begins with a letter, the latter if it begins with a digit. If desired, it is possible to communicate directly with the corresponding Settings method:

            pythia.settings.readString("TimeShower:pTmin = 1.0"); 
        
        In this case, changes intended for ParticleData would not be understood.

        c) Underlying the settings.readString(string) method are the settings-type-sensitive commands in the Settings, that are split by names containing flag, mode, parm or word. Thus, the example now reads

            pythia.settings.parm("TimeShower:pTmin", 1.0); 
        
        Such a form could be convenient e.g. if a parameter is calculated at the beginning of the main program, and thus is available as a variable rather than as a character string. Note that Boolean values must here be given as true or false i.e. there is less flexibility than with the previous methods.

        At the same level, there are several different methods available. These are included in the full description below, but normally the user should have no need for them.

        d) A simpler and more useful way is to collect all your changes in a separate file, with one line per change, e.g.

            TimeShower:pTmin = 1.0
        
        Each line is read in as a string and processed with the methods already introduced. The file can be read by the
            pythia.readFile(fileName); 
        
        method (or an istream instead of a fileName). The file can freely mix commands to the Settings and ParticleData classes, and so is preferable. Lines with settings are handled by calls to the pythia.settings.readString(string) method.
      3. In the pythia.init(...) call, many of the various other program elements are initialized, making use of the current values in the database. Once initialized, the common Settings database is likely not consulted again by these routines. It is therefore not productive to do further changes in mid-run: at best nothing changes, at worst you may set up inconsistencies.

        A routine reInit(fileName) is provided, and can be used to zero all the maps and reinitialize them from scratch. Such a call might be useful if several subruns are to be made with widely different parameter sets - normally the maps are only built from scratch once, namely when the Pythia() object is created. A more economical alternative is offered by resetAll(), however, which sets all variables back to their default values.

      4. You may at any time obtain a listing of all variables in the database by calling
            pythia.settings.listAll();
        
        The listing is strictly alphabetical, which at least means that names from the same file are kept together, but otherwise may not be so well-structured: important and unimportant ones will appear mixed. A more relevant alternative is
            pythia.settings.listChanged();
        
        where you will only get those variables that differ from their defaults. Or you can use
            pythia.settings.list("string");
        
        where only those variables with names that contain the string (case-insensitive match) are listed. Thus, with a string shower, the shower-related variables would be shown.
      5. The above listings are in a tabular form that cannot be read back in. Assuming you want to save all changed settings (maybe because you read in changes from several files), you can do that by calling
            pythia.settings.writeFile(fileName);
        
        This file could then directly be read in by readFile(fileName) in a subsequent (identical) run. Some variants of this command are listed below.

      Methods

      The complete list of methods and arguments is as follows. Most of the ones of interest to the user have already been mentioned above. Others can be used, but the same functionality is better achieved by higher-level routines. Some are part of the internal machinery, and should not be touched by user.

      Note that there is no Settings::readFile(...) method. The intention is that you should use Pythia::readFile(...). It parses and decides which individual lines should be sent on to Settings::readString(...). the constructor, which takes no arguments. Internal. initialize pointer to error-message database. Internal. read in the settings database. read in the settings from all the files listed in this file, and assumed to be located in the same subdirectory. By default nothing is done if the method has already been called once. If true the further settings read in are added to the current database. stream for error printout. Note: The method returns false if it fails. overwrite the existing database. read in the settings from all the files listed in this file, and assumed to be located in the same subdirectory. stream for error printout. Note: The method returns false if it fails. read in a string, and change the relevant quantity in the database. It is normally used indirectly, via Pythia::readString(...) and Pythia::readFile(...). the string to be interpreted as an instruction. write a warning message or not whenever the instruction does not make sense, e.g. if the variable does not exist in the databases. stream for error printout. Note: the method returns false if it fails to make sense out of the input string. write current settings to a file or to an ostream. file or stream on which settings are written. normally only settings that have been changed are written, but if true then all settings are output. Note: the method returns false if it fails. list all or changed settings, or a group of them. list all those settings where the name contains the match (sub)string (case-insensitive). output stream for the listing. reset all current values to their defaults. return true if an entry of the given name and kind exists, else false. add an entry of the respective kind to the database. The name and default value(s) always has to be supplied, for Mode, Parm, MVec and PVec additionally if lower and/or upper limits are to be imposed and, if so, what those limit are. return the current value(s) of the respective setting. If the name does not exist in the database, a value false, 0, 0., " ", or a vector of length 1 and value 0 or 0., respectively, is returned. return the default value(s) of the respective setting. If the name does not exist in the database, a value false, 0, 0., " ", or a vector of length 1 and value 0 or 0., respectively, is returned. return a map of all settings of the respective type that contain the string "match" in its name. change the current value(s) of the respective setting to the provided new value(s). If lower or upper limits have been set, input values outside the allowed range are reinterpreted as being a the nearest limit. as above, but do not check lower and upper limits, so that the current value(s) can be put outside the intended borders. reset the current value to the default one. pythia8-8.1.80.orig/xmldoc/CKKWLMerging.xml0000444000175000017500000015332012217346277016542 0ustar sunsun

      CKKW-L Merging

      CKKW-L merging Lon01 allows for a consistent merging of parton showers with matrix elements to include multiple well-separated partons. The algorithm implemented in PYTHIA is described in Lon11. To perform matrix element merging, the user has to supply LHE files Alw07 for the hard process and the corresponding process with up to N additional jets.

      The usage of the merging procedure is illustrated in a few example main programs (main81.cc, main82.cc, main83.cc, main84.cc and main85.cc, together with the input files main81.cmnd, main82.cmnd, main84.cmnd and main85.cmnd). These examples should of course only serve as an illustration, and as such will not make use of the merging in all possible ways. For full generality, the example programs link to LHAPDF, FastJet and HepMC. Of course the user is welcome to remove these dependencies. To remove the FastJet dependence, the functions calculating example observables have to be deleted. Removing the LHAPDF dependence requires changing the cmnd input files to choose an inbuilt PDF, as outlined in the PDF documentation. The HepMC dependence can be removed by erasing the code allowing for HepMC output.

      Please note that a detailed tutorial on merging in Pythia is available from http://home.thep.lu.se/~torbjorn/pythia8/mergingworksheet8160.pdf.

      Three very short LHE files (w+_production_lhc_0.lhe, w+_production_lhc_1.lhe, w+_production_lhc_2.lhe) are included in the distribution. These files are not intended for physics studies, but only serve as input for the example main programs. For realistic studies, the user has to supply LHE files.

      In the generation of LHE files, the value of the factorisation scale used in the PDFs is not important, since the cross section will be multiplied by ratios of PDFs to adjust to the PYTHIA starting scales. The same is true for the renormalisation scale (and starting value αs(MZ)) used to evaluate αs. Coupling and scale choices by the user will be transferred to the merging routines.

      Multi-jet events can suffer from infrared divergences in the calculation. Sensible matrix element generator (MEG) outputs should not contain phase space points in which the calculation is ill-defined, meaning infrared regions need to be removed by cuts. This is most conveniently done by disallowing the MEG to produce partons below a minimal parton-parton separation in a certain jet algorithm. Using dedicated cuts to regularise MEG output is of course possible as well. Any regularisation criterion defines the matrix element region: The parts of phase space in which the fixed order calculation is considered valid and preferable to the parton shower. Matrix element merging is combining MEG events in the matrix element region with parton shower events in regions outside the regularisation cut (often called parton shower region). Because the regularisation cut defines a boundary between the matrix element and parton shower regions, i.e. the regions to be merged into one inclusive sample, it is usually called merging scale . Since many different cut choices may regularise the MEG calculation, many different merging scale definitions are possible. A few standard choices are listed below, as well as documentation on how to use a user-defined cut criterion. In combining matrix element and parton shower regions, the CKKW-L prescription tries to minimise the dependence on the merging scale. This can only be achieved if the combination of MEG events and parton shower populates the whole phase space. Additional cuts on the partons in the LHEF generation should hence be avoided as much as possible, meaning that the merging scale cut should always pose a more stringent cut than all other cuts on the partons. Of course, if the hard process itself is divergent, cuts need to be made. However, this should be chosen in such a way as to not exclude regions that will be available to the matrix elements with additional jets. An example is QCD di-jet production with additional jets: Say the 2 -> 2 process is regularised with a pTmin cut of pTminCut = 100 GeV, and the 2 - >3 sample is regularised with a kTmin-cut of kTminCut = 50 GeV. This would mean that when reclustering the emission in the 2 -> 3 sample, we could end up with a pT value pTminNow of the 2 -> 2 configuration with pTminCut > pTminNow, which is excluded in the 2 -> 2 sample. Thus, the 2 -> 3 sample will include a Sudakov factor not included in the 2 -> 2 sample, resulting in merging scale dependencies. Such dependencies can be avoided if the additional cuts on the hard process are minimal.

      Of course, additional cuts on electroweak particles are allowed. These should be the same for all samples with 0 <= n <= N additional partons.

      If it is not possible to generate LHE files with minimal cuts, the user can choose to use the MergingHooks structures in order to decide how much influence to attribute to parton shower histories in which the reclustered lowest multiplicity process does not pass the matrix element cuts. This is described below.

      When generating LHE files, we advise against putting unstable particles (e.g. massive gauge bosons) in the final state. Rather, specify a resonance by its decay products, e.g. if Les Houches events for the pp → Z + jets → e+e- + jets process are desired, generate the matrix element events with the Z decay included. From a physical point of view, on-shell final massive gauge bosons should not be considered part of a hard process, since only the boson decay products will be detectable. Furthermore, non-narrow-width approximation contributions are not present if the ME generator only produces on-shell bosons. Interference effects between different production channels for the decay products would also be neglected. These points seem an unnecessary restriction on the accuracy of the ME calculation. In addition, there is a technical reason for this strategy. Since some matrix element generators choose to put additional information on intermediate bosons into Les Houches events, depending on if they pass a certain criterion (e.g. being close to the mass shell), without exact knowledge of this criterion, the only feasible way of bookkeeping the hard process is by identifying outgoing decay products.

      Despite these considerations, (massive) gauge bosons in the final state are allowed in the hard process definition. This is useful particularly for Higgs physics, when different decays of the Higgs boson need to be simulated after the LHEF generation.

      For all merging purposes, processes with different charge of outgoing leptons are considered different processes. That means e.g. that e+νe+ jets and e-ν̄e + jets are considered independent processes. If the user wishes to generate distributions including effects of more than one process, merged samples for all independent processes should be generated separately and added afterwards. Alternatively, to combine simple processes, combined LHE files can be used in conjunction with flexible containers (see below).

      When the matrix element merging is used to produce HepMC Dob01 files to be analysed with RIVET Buc10, special care needs to taken in how the cross section is read by RIVET (see below).

      To specify the merging conditions, additionally information on the merging scale value and the functional definition of the merging scale is needed. A few standard definitions of merging scales are available. We hope this makes the user interface less cumbersome.

      Different choices intrinsic to the CKKW-L merging procedure might be relevant for the user as well. The base class MergingHooks gives the user the opportunity to define the functional form of the merging scale. In the following, the usage of the merging machinery to consistently include LHE files with additional jets into PYTHIA will be discussed.


      Merging scale definitions

      The quickest way to include processes with additional jets is to produce LHE files with one of the standard ways to define the merging scale. Three standard ways to define a merging scale (minimal kT, minimal evolution pT and by three cuts) are implemented. All of these prescriptions are equivalent - different definitions have only been introduced for the convenience of users, who might be limited by which cuts can be used in the generation of LHE files. Below, we describe how to switch on and use these different merging scale definitions.

      Merging with merging scale defined in kT:

      If the additional jets in the LHE files have been regulated by a kT cut, the user can supply the merging scale definition by setting this flag to on. kT here and below means cutting on Durham kT for e+e- collisions, and cutting on longitudinally invariant kT for hadronic collisions. Please note that this particular merging scale definition will check kT between all pairs of u,d,c,s,b,g partons.

      Currently, the name longitudinally invariant kT is used for a few jet recombination algorithms with slightly different jet measures. A specific form can be chosen by setting the switch Precise functional definition of longitudinally invariant kT. For e+e- collisions, Durham kT is always defined by the square root of min{ 2*min[ Ei2, Ej2] * [ 1 - cosθij] }, so that this switch will have no effect. Maximal number of additional jets in the matrix element The value of the merging scale. The name is inspired by the scale in evolution equations, which is often called 't', and the suffix 'MS' stands for merging scale. In the particular case of kT-merging, this would be the value of the kT-cut in GeV. For any merging scale definition, this input is considered the actual value of the merging scale. The string specifying the hard core process, in MG4/ME notation.

      If e.g. W + jets merging should be performed, set this to pp>e+ve (without white spaces or quotation marks). This string may contain resonances in the MG/ME notation, e.g. for merging pp→Z W+→q q̄ e+νe + jets, the string pp>(z>jj)(w+>e+ve) would be applicable.

      A lot more flexible hard process definitions are possible. To not dwell too much on these details here, we will come back to the process string at the end of this section. Even easier, but highly non-general, is to perform the merging with MadGraph/MadEvent-produced LHE files, with a merging scale defined by a kT cut. For this, set this switch to on. The merging scale value will be read from the +1 jet LHE file by searching for the string ktdurham, and extracting the value from value = ktdurham. Also, the hard process will be read from the +0 jet LHE file, from the line containing the string @1 (the tag specifying the first process in the MadGraph process card). For this to work, PYTHIA should be initialised on LHE files called NameOfYourLesHouchesFile_0.lhe (+0 jet sample) and NameOfYourLesHouchesFile_1.lhe (+1 jet sample) and the same naming convention for LHE files with two or more additional jets. Since for this option, the merging scale value is read from the LHEF, no merging scale value needs to be supplied by setting Merging:TMS . Also, the hard process is read from LHEF, the input Merging::Process does not have to be defined. However, the maximal number of merged jets still has to be supplied by setting Merging:nJetMax.

      Merging with merging scale defined in Pythia evolution pT:

      If the LHE file has been regularised by cutting on the minimal Pythia evolution pT in the state, this can also be used as a merging scale right away. For this, change the switch The merging scale is then defined by finding the minimal Pythia evolution pT between sets of radiator, emitted and recoiler partons. For this particular merging scale definition, u,d,c,s,b,g are considered partons. The Pythia evolution pT of a single three-parton set is defined by

      pTevol = zijk(1-zijk) Qij2 for FSR, where i is the radiating parton, j is the emitted parton and k is the recoiler, and Qij2 = (pi + pj)2 , and zijk = xi,jk / (xi,jk + xj,ik) with xi,jk = 2 pi (pi + pj + pk) / (pi + pj + pk)2

      pTevol = (1-zijk) Qij2 for ISR, where i is the radiating parton, j is the emitted parton and k is the second initial state parton, and Qij2 = -(pi - pj)2 , and zijk = (pi - pj + pk)2 / (pi + pk)2 .

      When using this option, the merging scale is defined by the minimum pTevol for all combinations of three partons in the event, irrespective of flavour or colour-connections. The merging scale value will be read from the Merging:TMS parameter, so that this needs to be set just as in the case of the kT-merging prescription. Of course you will also need to set Merging:Process and the maximal number of additional matrix element jets Merging:nJetMax.

      Merging with merging scale defined by a combination of cuts:

      It is possible to regularise QCD divergences in a LHE file by applying cuts to the kinematical pT of jets (pTi), combined with a cut on ΔRij between jets and a cut on invariant mass Qij of jet pairs. The combination of these standard cuts can also serve as a merging scale. For this, use this setting This switch will use cuts on (pTi), ΔRij and Qij to define when parton shower emissions are allowed. Please note for this particular merging scale definition, only light jets (u,d,c,s,g) are checked.

      The values of the cuts will then be read from The value of the invariant mass cut Qij of pairs of final state partons used in the matrix element generation. The value of the minimal transverse momentum cut pTi on final state partons, as used in the matrix element generation. The value of the minimal ΔRij separation between pairs of final state partons used in the matrix element generation, where ΔRij2 = (Δyij)2 + (Δφij)2.

      With knowledge of these values, and Merging:doCutBasedMerging, Pythia will use these cuts as a separation between matrix element phase space and parton shower region. If e.g. the Les Houches Events have been generated with the cuts ΔRij = 0.1 , pTi= 20 GeV and Qij = 40 GeV, set Merging:QijMS=40., Merging:pTjMS=20., Merging:dRijMS=0.1 to perform a cut-based merging. Of course you will also need to set Merging:Process and the maximal number of additional matrix element jets Merging:nJetMax.

      Les Houches events outside the matrix element region

      Before continuing, we would like to point out that in general, the user should make sure that the events in the Les Houches file are actually calculated using the regularisation cut definition and value(s) supplied to Pythia as merging scale definition and value(s). However, if LH files with a large number of events and loose merging scale cuts are available, it might be useful to choose a higher merging scale value, e.g. for merging scale variations as part of uncertainty assessments. If CKKW-L merging is enabled, Pythia will by default check if events read from Les Houches file are in the matrix element region as defined by the merging scale definition and merging scale value. Events outside the matrix element region will be discarded. This will lead to warnings of the form "Les Houches Event fails merging scale cut. Cut by rejecting event". These warnings should, in this case, rather be regarded as information. To change the default behaviour, use the flag This will check if the events read from LHE file are in the matrix element region as defined by the merging scale definition and value(s). If on, LHE input outside the matrix element region will be rejected. If off, every event is assumed to pass the merging scale cut.

      Defining the hard process

      To perform CKKW-L matrix element merging, the user has to decide on a hard process, and communicate this choice to Pythia. This is done by setting the input Merging:Process

      For single processes in the Standard Model or the MSSM, MG4/ME notation is applicable. However, for some purposes, using a single simple process string is not satisfactory. Mixed W+ and W- events in a single LHE file is a common example. For this case, it would of course be perfectly allowed to perform twice, once for W+ production and once for W- production, and then add the results. Nevertheless, it seems reasonable to alleviate difficulties by allowing for less restrictive hard process definitions. Two generalisations of the process tag are available: Containers and user-defined particle tags. The syntax of these settings is described below.

      In case you want multiple processes in a LHE file to be treated on equal footing (e.g. W+ + jets and W- + jets), you should use flexible containers do specify the hard process. So far, we allow the use of the containers LEPTONS, NEUTRINOS, BQUARKS. If you use these containers, the hard process definition is relatively flexible, meaning that Pythia will attempt a merging of QCD jets for each event in the LHE file, and assume that all particles matching one of the containers are products of the hard process. This is best explained by examples. If you want to have both pp → e+ νe + jets and pp → e- ν̄e + jets events in a single file, you can set Merging:Process=pp>LEPTONS,NEUTRINOS as hard process (note that for readability, you are allowed to use commata to separate container names). Combining e.g. the processes pp → e+ νe and pp → μ+ νμ is possible with the hard process definition pp>LEPTONS,NEUTRINOS.

      For maximal flexibility, the definition of the hard process by these containers does not mean that each Les Houches event needs to contain particles to match each container. It is enough if one container is matched. This means that with the string pp>LEPTONS,NEUTRINOS, you can immediately process pp → e+ e- events mixed with pp → e+ νe events, since particles matching at least one container can be found in both cases. Another example for the usage of containers is mixing pp → e+ νe and pp → tt̄ → e+ νe e- ν̄e bb̄. This can be accommodated by the hard process string Merging:Process=pp>LEPTONS,NEUTRINOS,BQUARKS.

      There is however a conceptual limitation to containers: The hard process definition is necessary to ensure that when constructing lower multiplicity states (that will be used to calculate the correct merging weight), the structure of the hard process will be preserved. If e.g. we want the hard process to be pp → Z → bb̄ , we should ensure that the lowest multiplicity state contains a colour-singlet bb̄-pair. When reconstructing intermediate lower multiplicity states from multi-jet matrix elements, we should thus always be able to find at least one bb̄-pair. By mixing different processes in a LHE file, this requirement might already be violated at the level of Les Houches events. Flexible containers cannot give strong conditions which flavours should be preserved in the construction of the hard process. In order to avoid non-sensible results, it is hence assumed that all particles matching any of the containers will be part of the lowest multiplicity process. This implies that if you decide to use the BQUARKS container, all b-quarks in the LHE file will be interpreted as hard process particles, and never as additional radiation.

      Another way to specify the hard process particles is to explicitly define the particle names and identifiers. This is necessary if the matrix element merging in Pythia does not contain the particles of interest. To make sure that the hard process is still treated correctly, it is possible to define particles in the process string. If you e.g. want the hard process to contain a particle "zeta~" with PDG identifier "12345", produced in proton collisions, you have to include a user-defined particle tag by setting the process string to pp>{zeta~,12345}. The user-defined particle is enclosed in curly brackets, with syntax {particle_name,particle_identifier}, where "particle_name" and "particle_identifier" are the particle name and particle identifier used for this particle in the input LHE file. User-defined particles are only allowed in the final state. You are free to fix user-defined particles with more common ones, as long as user-defined particles are put before more common particles in the process string. This means that if you e.g. wanted the hard process to contain a graviton in association with a positron and an electron-neutrino, you have to define the hard process as pp>{G,39}e+ve.

      Below you can find a list of particles predefined in the merging. If you wish to include a hard process with different final state particles, you may use the "curly bracket notation" outlined above.

      The set of incoming particles us limited to: e- (electron), e+ (positron), mu- (muon), mu+ (antimuon), p (proton, container to hold all initial state coloured particles), p~ (identical to p container).

      The following intermediate particles are allowed: a (photon), z (Z boson), w- (W- boson), w+ (W+ boson), h (scalar Higgs boson), W (container to hold both W- and W+ boson), t (top quark), t~ (anti-top), dl, dl~, ul, ul~, sl, sl~, cl, cl~, b1, b1~, t1, t1~, dr, dr~, ur, ur~, sr, sr~, cr, cr~, b2, b2~, t2, t2~ (all MSSM squarks).

      We have pre-defined the outgoing particles: e+, e-, ve~, ve, mu+, mu-, vm~, vm, ta+, ta-, vt~, vt (all SM leptons and neutrinos), j~ (container to hold all final state coloured particles), j (container to hold all final state coloured particles), NEUTRINOS (container to hold all final state neutrinos and anti-neutrinos), LEPTONS (container to hold all final state leptons and anti-leptons), BQUARKS (container to hold final state b-quarks), d~, d, u~, u, s~, s, c~, c, b~, b, t~, t (all SM quarks), a, z, w-, w+ (all SM electro-weak bosons), h (scalar Higgs boson), W (container to hold both W- and W+ boson), n1 (MSSM neutralino), dl~, dl, ul~, ul, sl~, sl, cl~, cl, b1~, b1, t1~, t1, dr~, dr, ur~, ur, sr~, sr, cr~, cr, b2~, b2, t2~, t2 (all MSSM squarks). Other outgoing particles are possible if you use the "curly bracket notation" described earlier.


      Histogramming the events

      After the event has been processed, histograms for observables of interest need to be filled. In order to achieve good statistical accuracy for all jet multiplicities and all subprocesses contributing to one jet multiplicity, generally a fixed number of unit-weighted events is read from each Les Houches Event file. To then arrive at the correct prediction, for each of these events, histogram bins should be filled with the corresponding cross section, or weighted with unit weight and normalised at the end to the generated cross section for each jet multiplicity separately.

      Still another, even more important, event weight that has to applied on an event-by-event basis is the CKKW-L-weight. This corrective weight is the main outcome of the merging procedure and includes the correct no-emission probabilities, PDF weights and αs factors. This means that the merging implementation will generate weighted events. The CKKW-L-weight can be accessed by the following function:

      double Info::mergingWeight()  
      Returns the CKKW-L weight for the current event.

      Note that to avoid confusion, this function does not include the the weight of a phase space point (given by Info::weight()). This weight will differ from unity when reading in weighted Les Houches events. In this case, the full weight with which to fill histogram bins is Info::mergingWeight() * Info::weight().

      Finally, to arrive at a correct relative normalisation of the contributions from different number of additional jets in the matrix element, each histogram should be rescaled with the accepted cross section given by Info::sigmaGen(). The accepted cross section includes the effect of vetoes generating Sudakov form factors for the matrix elements, and is in general only known after the run.

      This final step can of course be skipped if the accepted cross section had been estimated before the histogramming run, and histogram bins had instead been filled with the weight Info::mergingWeight() * σest(number of additional jets in current ME sample). This is the way HepMC events should be weighted to produce correct relative weights of events (see below, and particularly examine the example programs main84.cc and main85.cc).

      Examples how to use these options are given in main81.cc (kT merging), main84.cc (automatic MG/ME merging for RIVET usage), and main85.cc (HepMC output for RIVET usage).


      Merging with user-defined merging scale function

      For all other merging scale definitions, the procedure is slightly more complicated, since the user has to write a small piece of code defining the merging scale. To allow for a user defined procedure, set the input General user defined merging on/off.

      Then, set the Merging:nJetMax, Merging:TMS and Merging:Process input as before.

      Since during execution, PYTHIA needs to evaluate the merging scale with the definition of the user, the user interface is designed in a way similar to the UserHooks strategy. The class controlling the merging scale definition is called MergingHooks.

      Initialisation

      To initialise the merging with user-defined merging scale, we should construct a class derived from MergingHooks, with a constructor and destructor

      The constructor and destructor do not need to do anything.

      For the class to be called during execution, a pointer to an object of the class should be handed in with the
      Pythia::setMergingHooksPtr( MergingHooks*) method. An examples of this procedure are given in main82.cc.

      Defining a merging scale

      Then, in the spirit of the UserHooks class, the user needs to supply the process to be merged by defining a methods to evaluate the merging scale variable. This method will have to calculate the value of the merging scale defined in some variable from the input event record. An example of such a function is given in main82.cc.

      The base class MergingHooks contains many functions giving information on the hard process, to make the definition of the merging scale as easy as possible: Return the maximum number of additional jets to be merged. Returns the number of outgoing partons in the hard core process. Returns the number of outgoing leptons in the hard core process. Returns the number of incoming partons in the hard core process. Returns the number of incoming leptons in the hard core process. The number of resonances in the hard process reconstructed from the current event. If e.g. the ME configuration was pp -> (w+->e+ve)(z -> mu+mu-)jj, and the ME generator put both intermediate bosons into the LHE file, this will return 2. Returns the value used as the merging scale.

      Filling output histograms for the event then proceeds along the lines described above in "Histogramming the events".

      The full procedure is outlined in main82.cc. Special care needs to be taken when the output is stored in the form of HepMC files for RIVET usage.

      Defining a cut on lowest jet multiplicity events

      It can sometimes happen that when generating LHE files, a fairly restrictive cut has been used when generating the lowest multiplicity matrix element configurations. Then, it can happen that states that are (in the generation of a parton shower history) constructed by reclustering from higher multiplicity configurations, do not pass this matrix element cut.

      Consider as an example pure QCD dijet merging, when up to one additional jet should be merged. Three-jet matrix element configurations for which the reclustered two-jet state does not pass the cuts applied to the two-jet matrix element would never have been produced by showering the two-jet matrix element. This means that the three-jet matrix element includes regions of phase space that would never have been populated by the parton shower. Thus, since the matrix element phase space is larger than the shower phase space, merging scale dependencies are expected. A priori, this is not troublesome, since the aim of matrix element merging is to include regions of phase space outside the range of the parton shower approximation into the shower. An example is the inclusion of configurations with only unordered histories.

      Clearly, if the parton shower phase space is very constrained by applying stringent cuts to the two-jet matrix element, merging scale dependencies can become sizable, as was e.g. seen in Lon11 when forcing shower emissions to be ordered both in the evolution variable and in rapidity. To influence the effect of large phase space differences for shower emissions and matrix element configurations due to LHEF generation cuts, the user has to write a small piece of code overwriting method This routine will be supplied internally with the lowest multiplicity reclustered state as an input Event. From this input event, the user can then check if matrix element cuts are fulfilled. The return value will be internally multiplied to the CKKW-L weight of the current event. Thus, if the user wishes to suppress contributions not passing particular cuts, a number smaller than unity can be returned.

      Note that this method gives the user access to the lowest multiplicity state, which ( e.g. in the case of incomplete histories) does not have to be a 2 → 2 configuration. Also, changing the weight of the current event by hand is of course a major intervention in the algorithm, and should be considered very carefully. Generally, if this facility would have to be used extensively, it is certainly preferable to be less restrictive when applying additional, non-merging-scale-related cuts to the matrix element.

      An example how to force a cut on lowest multiplicity reclustered states for pure QCD matrix element configurations is given by main83.cc (to be used with e.g. main82.cmnd).

      Influencing the construction of all possible histories

      Even more powerful - and dangerous - is influencing the construction of histories directly. This should only be attempted by expert users. If you believe manipulations completely unavoidable, we advise you to take great care when redefining the following functions. In the base class this method returns false. If you redefine it to return true then the method doCutOnRecState(...) will be called for each reclustered state encountered in the generation of all possible histories of the matrix element state. This routine will be supplied internally with every possible reclustered event that can be reached by reclustering any number of partons in the matrix element input state. The new, reclustered, states can then be analysed. If the method returns false, the history to which the state belongs will be treated as if it were unordered, i.e. this path will only be chosen if no other histories are available. In this way, the number of histories not fulfilling the user criterion will be minimised.

      Clearly, these methods are highly intrusive. It could e.g. happen that no history is allowed, which would make merging impossible. One example where this method could be useful is if cuts on the core 2 -> 2 processes have to be checked, and the method MergingHooks::dampenIfFailCuts(const Event& event) is not sufficiently effective.

      Defining the hard process matrix element

      The MergingHooks class also allows the expert user to define the matrix element of the hard process, by defining the method This routine will be supplied internally with the reconstructed lowest-multiplicity event. From this, it is possible to calculate the squared matrix element of the hard process, by using the information stored in the event record. The function should return a double value that corresponds to the matrix element at the phase space point given by the input event record. This number will then be multiplied to the product of splitting functions that define the probability of the current path of the parton shower history. In this way, the hard process configuration can be taken into account when choosing the parton shower history, which is, internally, used to generate the "merging weight".

      The inclusion of the hard process matrix element into the choice of histories becomes relevant when the hard process matrix element has very strong phase space dependencies. QCD dijet cross sections for example strongly depend on the transverse momentum of the jets. So far, the authors have not encountered any changes upon inclusion of the full hard process matrix element, even for the QCD dijet case.


      Matrix element merging and HepMC output for RIVET

      Examples how to produce matrix element merged events to be analysed with RIVET are given by main84.cc and main85.cc.

      The main issue is that the output of separate RIVET runs can not in general be combined. To perform a matrix element merging, we however need to runs over different LHE files. The solution to this problem (so far) is to only perform one RIVET run for all matrix elements, i.e. print the events for all ME parton multiplicities, with the correct weights, to a single HepMC file. Since the correct weight includes the cross section of the different samples after Sudakov vetoes --- which is not a priori known --- the cross sections have to be estimated in a test run, before the actual production run is performed. Finally, the cross section of the last event in the HepMC file has to be taken as the full merged cross section sigma_merge = Sum_{i=0}^N Sum_{j=0}*^{nEvents} sigma_est(i)*wckkwl(j).

      This procedure is outlined in main84.cc. Input LHE files with only very inclusive cuts pose further difficulties. For such files (which were already addressed under the heading Les Houches events outside the matrix element region), the cross section after the merging scale cut is not known before the cut is performed. Using Pythia's UserHooks facilities, it is possible to produce a valid estimate of the cross section after cuts. This however entails a careful cut definition by the user, which might become cumbersome for some in-built merging scale definitions. A reasonable alternative is using the switch If on, estimate cross section after merging scale cut. This switch has to be used in conjunction with a merging scale definition (e.g. Merging:doPTLundMerging = on). Then, this merging scale definition will be used as a cut on the input events. After the requested number of Monte Carlo events, the cross section after the cut can be extracted by inferring the Info::sigmaGen() method, and the number of accepted events by using Info::nAccepted()

      This switch also relies on knowledge on how many partons a LHE file should contain. This is important for real-emission kinematics in the case of NLO merging. The number of (additional) partons in a LHE file can be set with Exact number of additional jets requested for a particular LHE file. If a file should for example only contain W+ g g events, this switch should be set to "2" for this LHE file. For NLO merging schemes (see NLO Merging), this number has to be set.

      The usage of these switches to obtain the necessary cross section estimate is illustrated in main85.cc. The example main85.cc program is intended as a "front-end" for CKKW-L merging in Pythia8, so we will discuss the program briefly. main85.cc should be used together with an input file (like main85.cmnd). The executable should be invoked with three arguments: the input file, the "name" of the input LHE files, and the name of the output HepMC event file. To use the LHE files that are shipped with the Pythia distribution, a valid usage would be

      ./main85.exe ./main85.cmnd ./w_production ./myhepmc.hepmc

      If you want to use other input LHE files, note that main85.cc assumes the naming convention name_tree_#nAdditionalJets.lhe. All settings can be included though the input file, so that main85.cc does not have to be changed explicitly. main85.cc first switches off showers, multiparton interactions and hadronisation, and estimates the cross sections (after enforcing the merging scale cut) of samples for different numbers of additional jets. Then, showers, MPI and hadronisation are switched on again, and the CKKW-L merging procedure is performed. Events will be read in a decreasing sequence of jet multiplicities, which also means that e.g. events with two additional partons in the LHE file will be printed to the HepMC file before events with one additional parton.


      Further variables

      For more advanced manipulations of the merging machinery, all parameter changes that were investigated in Lon11 are supplied. Please check Lon11 for a detailed discussion of the switches.

      These switches allow enthusiastic users to perform a systematic assessment of the merging prescription. Apart from this, we advise the non-expert user to keep the default values. This switch controls which quarks flavours (labelled by PDG id's) are considered additional partons. If e.g. set to 4, then u-, d-, c- and s-quarks will be merged, while b-quarks will not be considered in the merging (corresponding to a 4-flavour merging scheme). We advise caution when changing this number. In particular, please ensure that the allowed flavour for additional partons in the input LHE file does not exceed this value, since unnecessary double-counting might occur otherwise. If on, use the correct massive evolution variable and massive splitting kernels in the reconstruction and picking of parton shower histories of the matrix element. If off, reconstruct evolution scales, kinematics and splitting kernels as if all partons were massless. If on, preferably pick parton shower histories of the matrix element which have strongly ordered consecutive splittings, i.e. paths in which consecutive reclustered evolution scales are separated by a user-defined factor. The factor by which scales should differ to be classified as strongly ordered. If on, preferably pick parton shower histories of the matrix element with consecutive splittings ordered in rapidity and pT. If on, pick parton shower histories of the matrix element by the full shower splitting kernels, including potential ME corrections and Jacobians from joined evolution measures. If on, pick parton shower histories of the matrix element by the shower splitting kernels divided by the evolution pT. If on, exclusively pick parton shower histories of the matrix element for which have the smallest sum of scalar evolution pT for consecutive splittings has been calculated. If on, then also include PDF ratios and αs factors in the splitting probabilities used for picking a parton shower history of the matrix element, when picking histories by the full shower splitting probability. As argued in Lon11, this should not be done since a reweighting with PDF ratios and αs factors will be performed. However, it can give useful insight in how sensitive the results are to the prescription on how to choose PS histories. Normalisation factor with which to multiply splitting probability for splittings without joined evolution equation. Normalisation factor with which to multiply splitting probability for final state splittings with an initial state recoiler. Factor with which to multiply the scalar pT of a final state splitting, when choosing the history by the smallest sum of scalar pT. Default value taken from Herwig++ Tul09. Factor with which to multiply the scalar pT of an initial state splitting, when choosing the history by the smallest sum of scalar pT. Default value taken from Herwig++ Tul09. When the parton shower history of the matrix element contains a sequence of splittings which are not ordered in evolution pT (called an unordered history), this sequence is interpreted as a combined emission. Then, a decision on which starting scale for trial emissions off reconstructed states in this sequence of unordered splittings has to be made. Two options are available: Prescription which scale to use to evaluate αs weight for splittings in a sequence of splittings which are not ordered in evolution pT. Prescription which scale to use to evaluate ratios of parton distributions for splittings in a sequence of splittings which are not ordered in evolution pT. When no complete parton shower history (i.e. starting from a 2 → 2 process) for a matrix element with additional jets can be found, such a configuration is said to have an incomplete history. Since in incomplete histories, not all shower starting scales are determined by clusterings, a prescription for setting the starting scale of trial showers in incomplete histories is needed. Three options are provided. If on, this will allow the algorithm to swap one colour index in the state, when trying to find all possible clusterings, if no clustering has been found, but more clusterings had been requested. In this way, some incomplete histories can be avoided. Generally, we advise the non-expert user to not touch this switch, because a slight change in the colour structure can change the radiation pattern. To however study the sensitivity of the predictions on these effects, allowing for colour reshuffling can be useful. If on, this will allow the algorithm to use a dynamical renormalisation scale to evaluate the strong couplings of the core hard process in dijet and prompt photon events. This means that the value of αs used as coupling of the hard process in the matrix element generation will be replaced with a running coupling evaluated at the geometric mean of the squared transverse masses of the two outgoing particles, as is the default prescription in Pythia. If on, this will allow the algorithm to use a dynamical factorisation scale to evaluate parton distributions associated with the hadronic cross section of the core hard process in dijet and prompt photon events. In the calculation of PDF ratios as part of the CKKW-L weight of an event, parton distributions that should be evaluated at the scale of the core 2 - >2 process will be evaluated using the dynamical factorisation scale Pythia would attribute to this process. This means that the hard process factorisation scale is set to the smaller of the squared transverse masses of the two outgoing particles. Remove products of resonances in the hard process, in case Pythia generates decay products before merging. This makes merging possible even for an indeterminate final state, if Pythia itself has produced the decay products. The merging methods will instead be invoked on the "non-decayed" event, thus removing the limitation to only one decay channel when performing the merging. This switch is necessary e.g. for slepton pair production in association with additional QCD jets, if the input LHE file contains the resonant sleptons, and Pythia decides on a decay according to the branching fractions read from SLHA input. Allow clustering of gluon emission off squarks. Allow clustering of W boson, if interpreted as a final state emission. This switch should not be used until electro-weak showers become available. pythia8-8.1.80.orig/xmldoc/mstw2008lo.00.dat0000444000175000017500000120437012217346305016376 0ustar sunsun # Thu Nov 6 19:08:12 2008 # MSTW 2008 LO PDF grid for central fit. # distance(t),tolerance(T) = 0. 0. # mCharm = 1.40 # mBottom = 4.75 # alphaS(1GeV) = 0.68183 # alphaS(MZ) = 0.13939 # alphaSorder,alphaSnfmax = 0, 5 # nExtraFlavours = 0 xg xd xu xs xc xb xdv xuv xsv 1.3241E+02 1.1742E+00 1.1767E+00 4.8673E-01 0.0000E+00 0.0000E+00 1.9861E-04 2.6691E-03 -7.2535E-04 1.3796E+02 1.7390E+00 1.7415E+00 1.0578E+00 0.0000E+00 0.0000E+00 2.1538E-04 2.7734E-03 -7.3571E-04 1.4346E+02 2.1713E+00 2.1739E+00 1.4948E+00 0.0000E+00 0.0000E+00 2.2894E-04 2.8541E-03 -7.4354E-04 1.5307E+02 2.7759E+00 2.7786E+00 2.1057E+00 0.0000E+00 0.0000E+00 2.4858E-04 2.9662E-03 -7.5416E-04 1.5307E+02 2.7759E+00 2.7786E+00 2.1057E+00 1.4899E-06 0.0000E+00 2.4858E-04 2.9662E-03 -7.5416E-04 1.6275E+02 3.3097E+00 3.3125E+00 2.6446E+00 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2.3867E-07 1.1588E-05 1.8218E-07 1.7709E-07 1.6644E-07 5.6485E-08 1.1406E-05 1.6996E-15 1.3315E-03 4.0797E-06 1.1201E-03 1.3571E-14 0.0000E+00 0.0000E+00 4.0797E-06 1.1201E-03 2.7131E-14 7.8048E-04 3.2560E-06 8.7438E-04 1.5075E-07 0.0000E+00 0.0000E+00 3.1053E-06 8.7423E-04 2.0106E-14 5.2147E-04 2.7267E-06 7.2616E-04 1.9528E-07 0.0000E+00 0.0000E+00 2.5315E-06 7.2597E-04 1.6071E-14 3.0130E-04 2.1306E-06 5.6533E-04 2.0759E-07 0.0000E+00 0.0000E+00 1.9230E-06 5.6512E-04 1.1892E-14 3.0130E-04 2.1306E-06 5.6533E-04 2.0759E-07 9.3404E-14 0.0000E+00 1.9230E-06 5.6512E-04 1.1892E-14 1.8971E-04 1.7274E-06 4.5915E-04 1.9640E-07 2.9019E-08 0.0000E+00 1.5310E-06 4.5896E-04 9.2689E-15 1.2241E-04 1.4139E-06 3.7738E-04 1.7851E-07 4.0503E-08 0.0000E+00 1.2354E-06 3.7720E-04 7.3325E-15 8.4367E-05 1.1920E-06 3.1965E-04 1.6158E-07 4.4261E-08 0.0000E+00 1.0305E-06 3.1949E-04 6.0158E-15 5.9339E-05 1.0146E-06 2.7332E-04 1.4597E-07 4.5228E-08 0.0000E+00 8.6861E-07 2.7317E-04 4.9934E-15 4.1083E-05 8.5785E-07 2.3212E-04 1.3094E-07 4.4933E-08 0.0000E+00 7.2691E-07 2.3199E-04 4.1130E-15 2.9956E-05 7.4350E-07 2.0179E-04 1.1938E-07 4.4223E-08 0.0000E+00 6.2412E-07 2.0167E-04 3.4841E-15 2.2231E-05 6.4979E-07 1.7669E-04 1.0963E-07 4.3454E-08 0.0000E+00 5.4016E-07 1.7658E-04 2.9777E-15 1.7598E-05 5.8518E-07 1.5922E-04 1.0282E-07 4.2903E-08 0.0000E+00 4.8236E-07 1.5912E-04 2.6331E-15 8.3833E-06 4.2210E-07 1.1409E-04 8.6171E-08 4.2466E-08 0.0000E+00 3.3593E-07 1.1401E-04 1.7778E-15 8.3833E-06 4.2210E-07 1.1409E-04 8.6171E-08 4.2467E-08 1.9783E-16 3.3593E-07 1.1401E-04 1.7778E-15 7.1988E-06 3.9539E-07 1.0645E-04 8.3781E-08 4.2834E-08 6.1246E-10 3.1161E-07 1.0637E-04 1.6388E-15 4.6586E-06 3.2887E-07 8.6957E-05 7.8575E-08 4.4687E-08 3.2726E-09 2.5029E-07 8.6878E-05 1.2924E-15 3.1047E-06 2.7582E-07 7.0754E-05 7.5592E-08 4.7610E-08 7.4611E-09 2.0023E-07 7.0679E-05 1.0151E-15 2.5013E-06 2.3869E-07 5.8892E-05 7.4494E-08 5.0869E-08 1.2138E-08 1.6420E-07 5.8818E-05 8.1904E-16 2.4614E-06 2.0996E-07 4.9095E-05 7.5064E-08 5.5069E-08 1.7958E-08 1.3489E-07 4.9020E-05 6.6229E-16 2.4509E-06 1.9171E-07 4.2311E-05 7.6834E-08 5.9375E-08 2.3710E-08 1.1488E-07 4.2234E-05 5.5684E-16 2.4513E-06 1.7501E-07 3.5443E-05 8.0121E-08 6.5253E-08 3.1420E-08 9.4887E-08 3.5363E-05 4.5308E-16 2.4513E-06 1.6406E-07 3.0372E-05 8.3736E-08 7.0803E-08 3.8629E-08 8.0321E-08 3.0289E-05 3.7858E-16 2.4513E-06 1.5652E-07 2.6411E-05 8.7444E-08 7.6038E-08 4.5392E-08 6.9075E-08 2.6324E-05 3.2179E-16 2.4513E-06 1.5006E-07 2.2187E-05 9.2826E-08 8.3068E-08 5.4350E-08 5.7229E-08 2.2094E-05 2.6280E-16 2.4513E-06 1.4699E-07 1.8880E-05 9.8911E-08 9.0461E-08 6.3521E-08 4.8074E-08 1.8781E-05 2.1787E-16 2.4513E-06 1.4634E-07 1.6269E-05 1.0542E-07 9.8015E-08 7.2695E-08 4.0927E-08 1.6163E-05 1.8326E-16 2.4513E-06 1.4743E-07 1.4049E-05 1.1252E-07 1.0602E-07 8.2266E-08 3.4917E-08 1.3936E-05 1.5452E-16 2.4513E-06 1.4979E-07 1.2193E-05 1.1984E-07 1.1411E-07 9.1836E-08 2.9944E-08 1.2073E-05 1.3102E-16 2.4513E-06 1.5288E-07 1.0688E-05 1.2693E-07 1.2183E-07 1.0090E-07 2.5950E-08 1.0561E-05 1.1237E-16 2.4513E-06 1.5737E-07 9.4513E-06 1.3468E-07 1.3010E-07 1.1038E-07 2.2694E-08 9.3167E-06 9.7316E-17 2.4513E-06 1.6571E-07 8.3751E-06 1.4584E-07 1.4173E-07 1.2316E-07 1.9876E-08 8.2292E-06 8.4425E-17 2.4513E-06 1.7621E-07 7.4484E-06 1.5875E-07 1.5505E-07 1.3758E-07 1.7462E-08 7.2896E-06 7.3492E-17 2.4513E-06 1.8765E-07 6.6742E-06 1.7219E-07 1.6884E-07 1.5235E-07 1.5456E-08 6.5020E-06 6.4487E-17 2.4513E-06 1.9929E-07 6.0263E-06 1.8550E-07 1.8245E-07 1.6685E-07 1.3785E-08 5.8408E-06 5.7055E-17 2.4513E-06 2.2480E-07 5.4589E-06 2.1251E-07 2.0972E-07 1.9499E-07 1.2294E-08 5.2464E-06 5.0479E-17 2.4513E-06 2.6882E-07 4.9808E-06 2.5783E-07 2.5528E-07 2.4135E-07 1.0992E-08 4.7230E-06 4.4782E-17 2.4513E-06 3.3861E-07 4.6047E-06 3.2872E-07 3.2638E-07 3.1319E-07 9.8872E-09 4.2759E-06 3.9989E-17 2.4513E-06 3.9771E-07 4.2821E-06 3.8876E-07 3.8660E-07 3.7408E-07 8.9481E-09 3.8933E-06 3.5944E-17 2.4513E-06 4.5192E-07 3.9866E-06 4.4383E-07 4.4183E-07 4.2995E-07 8.0931E-09 3.5428E-06 3.2288E-17 2.4513E-06 5.0062E-07 3.7215E-06 4.9329E-07 4.9144E-07 4.8017E-07 7.3308E-09 3.2282E-06 2.9051E-17 2.4513E-06 5.4283E-07 3.4920E-06 5.3616E-07 5.3445E-07 5.2373E-07 6.6749E-09 2.9559E-06 2.6285E-17 2.4513E-06 5.7952E-07 3.2928E-06 5.7342E-07 5.7182E-07 5.6161E-07 6.1086E-09 2.7193E-06 2.3913E-17 2.4513E-06 6.1372E-07 3.1072E-06 6.0814E-07 6.0665E-07 5.9693E-07 5.5841E-09 2.4991E-06 2.1729E-17 2.4513E-06 6.4546E-07 2.9408E-06 6.4034E-07 6.3896E-07 6.2970E-07 5.1140E-09 2.3005E-06 1.9784E-17 2.4513E-06 6.7434E-07 2.7942E-06 6.6964E-07 6.6835E-07 6.5952E-07 4.6995E-09 2.1245E-06 1.8078E-17 2.4513E-06 6.9957E-07 2.6665E-06 6.9523E-07 6.9402E-07 6.8558E-07 4.3405E-09 1.9712E-06 1.6611E-17 2.4513E-06 7.2341E-07 2.5460E-06 7.1941E-07 7.1827E-07 7.1021E-07 4.0031E-09 1.8266E-06 1.5238E-17 2.5564E-04 1.2672E-07 1.4179E-04 1.5154E-17 0.0000E+00 0.0000E+00 1.2672E-07 1.4179E-04 3.0303E-17 1.3610E-04 1.0654E-07 1.0605E-04 1.3798E-08 0.0000E+00 0.0000E+00 9.2742E-08 1.0603E-04 2.1833E-17 8.4637E-05 9.1347E-08 8.5304E-05 1.7922E-08 0.0000E+00 0.0000E+00 7.3426E-08 8.5286E-05 1.7090E-17 4.4395E-05 7.3971E-08 6.3625E-05 2.0340E-08 0.0000E+00 0.0000E+00 5.3631E-08 6.3605E-05 1.2285E-17 4.4395E-05 7.3971E-08 6.3625E-05 2.0340E-08 7.6780E-15 0.0000E+00 5.3631E-08 6.3605E-05 1.2285E-17 2.5844E-05 6.2677E-08 4.9887E-05 2.1331E-08 2.8414E-09 0.0000E+00 4.1346E-08 4.9866E-05 9.3546E-18 1.5508E-05 5.4516E-08 3.9671E-05 2.2147E-08 5.2401E-09 0.0000E+00 3.2368E-08 3.9649E-05 7.2404E-18 1.0072E-05 4.9343E-08 3.2681E-05 2.3022E-08 7.3851E-09 0.0000E+00 2.6321E-08 3.2658E-05 5.8276E-18 6.7205E-06 4.6046E-08 2.7226E-05 2.4383E-08 9.8758E-09 0.0000E+00 2.1663E-08 2.7202E-05 4.7535E-18 4.4280E-06 4.4269E-08 2.2507E-05 2.6584E-08 1.3188E-08 0.0000E+00 1.7685E-08 2.2480E-05 3.8455E-18 3.1251E-06 4.3956E-08 1.9121E-05 2.9090E-08 1.6592E-08 0.0000E+00 1.4866E-08 1.9092E-05 3.2103E-18 2.3595E-06 4.4575E-08 1.6386E-05 3.1963E-08 2.0276E-08 0.0000E+00 1.2612E-08 1.6354E-05 2.7020E-18 2.0403E-06 4.5564E-08 1.4520E-05 3.4476E-08 2.3398E-08 0.0000E+00 1.1088E-08 1.4486E-05 2.3624E-18 1.9008E-06 4.7362E-08 9.8657E-06 4.0014E-08 3.0735E-08 0.0000E+00 7.3475E-09 9.8257E-06 1.5399E-18 1.9008E-06 4.7362E-08 9.8657E-06 4.0014E-08 3.0735E-08 -8.9609E-16 7.3475E-09 9.8257E-06 1.5399E-18 1.9018E-06 4.9978E-08 9.1078E-06 4.3231E-08 3.4301E-08 -2.5267E-09 6.7465E-09 9.0646E-06 1.4095E-18 1.9017E-06 6.1816E-08 7.2206E-06 5.6557E-08 4.8590E-08 -3.9159E-10 5.2596E-09 7.1640E-06 1.0876E-18 1.9017E-06 7.7893E-08 5.7105E-06 7.3811E-08 6.6750E-08 1.1005E-08 4.0823E-09 5.6367E-06 8.3560E-19 1.9017E-06 1.0330E-07 4.6541E-06 1.0004E-07 9.3725E-08 3.5434E-08 3.2592E-09 4.5541E-06 6.6111E-19 1.9017E-06 2.0933E-07 3.8928E-06 2.0672E-07 2.0109E-07 1.4263E-07 2.6077E-09 3.6861E-06 5.2431E-19 1.9017E-06 2.9060E-07 3.3895E-06 2.8843E-07 2.8331E-07 2.2598E-07 2.1735E-09 3.1011E-06 4.3410E-19 1.9017E-06 3.7098E-07 2.8936E-06 3.6923E-07 3.6468E-07 3.0978E-07 1.7501E-09 2.5243E-06 3.4665E-19 1.9017E-06 4.2900E-07 2.5372E-06 4.2755E-07 4.2345E-07 3.7131E-07 1.4490E-09 2.1097E-06 2.8503E-19 1.9017E-06 4.7359E-07 2.2656E-06 4.7237E-07 4.6865E-07 4.1933E-07 1.2214E-09 1.7933E-06 2.3876E-19 1.9017E-06 5.2618E-07 1.9894E-06 5.2520E-07 5.2191E-07 4.7640E-07 9.8718E-10 1.4642E-06 1.9164E-19 1.9017E-06 5.6783E-07 1.7804E-06 5.6702E-07 5.6410E-07 5.2222E-07 8.1046E-10 1.2134E-06 1.5628E-19 1.9017E-06 5.9994E-07 1.6193E-06 5.9927E-07 5.9665E-07 5.5811E-07 6.7556E-10 1.0201E-06 1.2938E-19 1.9017E-06 6.2661E-07 1.4855E-06 6.2605E-07 6.2371E-07 5.8840E-07 5.6451E-10 8.5948E-07 1.0736E-19 1.9017E-06 6.4843E-07 1.3761E-06 6.4795E-07 6.4585E-07 6.1355E-07 4.7450E-10 7.2817E-07 8.9574E-20 1.9017E-06 6.6574E-07 1.2893E-06 6.6533E-07 6.6344E-07 6.3383E-07 4.0365E-10 6.2395E-07 7.5809E-20 1.9017E-06 6.7970E-07 1.2192E-06 6.7936E-07 6.7764E-07 6.5042E-07 3.4690E-10 5.3986E-07 6.4798E-20 1.9017E-06 6.9166E-07 1.1592E-06 6.9136E-07 6.8981E-07 6.6482E-07 2.9868E-10 4.6787E-07 5.5481E-20 1.9017E-06 7.0180E-07 1.1084E-06 7.0155E-07 7.0014E-07 6.7721E-07 2.5807E-10 4.0682E-07 4.7646E-20 1.9017E-06 7.1015E-07 1.0665E-06 7.0993E-07 7.0864E-07 6.8754E-07 2.2485E-10 3.5657E-07 4.1505E-20 1.9017E-06 7.1704E-07 1.0320E-06 7.1684E-07 7.1566E-07 6.9617E-07 1.9762E-10 3.1511E-07 3.6211E-20 1.9017E-06 7.2313E-07 1.0014E-06 7.2295E-07 7.2188E-07 7.0389E-07 1.7369E-10 2.7846E-07 3.1764E-20 1.9017E-06 7.2840E-07 9.7496E-07 7.2825E-07 7.2726E-07 7.1067E-07 1.5308E-10 2.4671E-07 2.7952E-20 1.9017E-06 7.3283E-07 9.5273E-07 7.3270E-07 7.3179E-07 7.1643E-07 1.3585E-10 2.2003E-07 2.4564E-20 1.9017E-06 7.3657E-07 9.3398E-07 7.3645E-07 7.3561E-07 7.2134E-07 1.2140E-10 1.9753E-07 2.2023E-20 1.9017E-06 7.3995E-07 9.1704E-07 7.3984E-07 7.3906E-07 7.2583E-07 1.0841E-10 1.7720E-07 1.9482E-20 1.9017E-06 7.4294E-07 9.0206E-07 7.4284E-07 7.4212E-07 7.2984E-07 9.6970E-11 1.5922E-07 1.7364E-20 1.9017E-06 7.4548E-07 8.8927E-07 7.4540E-07 7.4473E-07 7.3330E-07 8.7254E-11 1.4388E-07 1.5670E-20 1.9017E-06 7.4767E-07 8.7831E-07 7.4759E-07 7.4697E-07 7.3629E-07 7.8964E-11 1.3072E-07 1.4188E-20 1.9017E-06 7.4968E-07 8.6823E-07 7.4961E-07 7.4904E-07 7.3907E-07 7.1368E-11 1.1862E-07 1.2705E-20 1.9017E-06 7.5147E-07 8.5926E-07 7.5140E-07 7.5087E-07 7.4157E-07 6.4643E-11 1.0786E-07 1.1435E-20 1.9017E-06 7.5304E-07 8.5141E-07 7.5298E-07 7.5248E-07 7.4378E-07 5.8773E-11 9.8429E-08 1.0376E-20 1.9017E-06 7.5438E-07 8.4465E-07 7.5433E-07 7.5386E-07 7.4570E-07 5.3747E-11 9.0321E-08 9.5291E-21 1.9017E-06 7.5564E-07 8.3834E-07 7.5559E-07 7.5516E-07 7.4750E-07 4.9067E-11 8.2746E-08 8.6821E-21 pythia8-8.1.80.orig/xmldoc/EventInformation.xml0000444000175000017500000006724412217346302017643 0ustar sunsun

      Event Information

      The Info class collects various one-of-a-kind information, some relevant for all events and others for the current event. An object info is a public member of the Pythia class, so if you e.g. have declared Pythia pythia, the Info methods can be accessed by pythia.info.method(). Most of this is information that could also be obtained e.g. from the event record, but is here more directly available. It is primarily intended for processes generated internally in PYTHIA, but many of the methods would work also for events fed in via the Les Houches Accord.

      List information

      a listing of most of the information set for the current event.

      The beams

      the identities of the two beam particles. the longitudinal momenta of the two beam particles. the energies of the two beam particles. the masses of the two beam particles. the CM energy and its square for the two beams.

      Initialization

      normally false, but true if the proposed pTmin scale was too low in timelike or spacelike showers, or in multiparton interactions. In the former case the pTmin is raised to some minimal value, in the latter the initialization fails (it is impossible to obtain a minijet cross section bigger than the nondiffractive one by reducing pTmin).

      The event type

      the name and code of the process that occurred. the number of final-state partons in the hard process. are beam particles resolved, i.e. were PDF's used for the process? is either beam diffractively excited? is there central diffraction (a.k.a. double Pomeron exchange)? is the process the SoftQCD:nonDiffractive one, i.e. corresponding to the full inelastic nondiffractive part of the total cross section. (Note that a hard process, say Z^0 production, normally is nondiffractive, but this is not what we aim at here, and so the method would return false, unless the Z^0 had been generated as part of the MPI machinery for the SoftQCD:nonDiffractive component.) the same as above, retained for backwards compatibility, but to be removed in PYTHIA 8.2. has the process been generated from external Les Houches Accord information? true if a linked Les Houches class refuses to return any further events, presumably because it has reached the end of the file from which events have been read in. does the process have a subprocess classification? Currently only true for nondiffractive and Les Houches events, where it allows the hardest collision to be identified. the name, code and number of final-state partons in the subprocess that occurred when hasSub() is true. For a minimum-bias event the code would always be 101, while codeSub() would vary depending on the actual hardest interaction, e.g. 111 for g g -> g g. For a Les Houches event the code would always be 9999, while codeSub() would be the external user-defined classification code. The methods below would also provide information for such particular subcollisions.

      Hard process initiators

      The methods in this sections refer to the two initial partons of the hard 2 -> n process (diffraction excluded; see below). the identities of the two partons coming in to the hard process. x fractions of the two partons coming in to the hard process. rapidity and scaled mass-squared of the hard-process subsystem, as defined by the above x values. true if the two hard incoming partons have been picked to belong to the valence piece of the parton-density distribution, else false. Should be interpreted with caution. Information is not set if you switch off parton-level processing.

      Hard process parton densities and scales

      The methods in this section refer to the partons for which parton densities have been defined, in order to calculate the cross section of the hard process (diffraction excluded; see below).

      These partons would normally agree with the ones above, the initiators of the 2 -> n process, but it does not have to be so. Currently the one counterexample is POWHEG events Ali10. Here the original hard process could be 2 -> (n-1). The NLO machinery at times would add an initial-state branching to give a 2 -> n process with a changed initial state. In that case the values in this section refer to the original 2 -> (n-1) state and the initiator ones above to the complete2 -> n process. The Info::list() printout will contain a warning in such cases.

      For external events in the Les Houches format, the pdf information is obtained from the optional #pdf line. When this information is absent, the parton identities and x values agree with the initiator ones above, while the pdf values are unknown and therefore set to vanish. The alpha_s and alpha_em values are part of the compulsory information. The factorization and renormalization scales are both equated with the one compulsory scale value in the Les Houches standard, except when a #pdf line provides the factorization scale separately. If alpha_s, alpha_em or the compulsory scale value are negative at input then new values are defined as for internal processes. the identities of the two partons for which parton density values are defined. x fractions of the two partons for which parton density values are defined. parton densities x*f(x,Q^2) evaluated for the two incoming partons; could be used e.g. for reweighting purposes in conjunction with the idpdf, xpdf and QFac methods. Events obtained from external programs or files may not contain this information and, if so, 0 is returned. the Q or Q^2 factorization scale at which the densities were evaluated. the alpha_strong and alpha_electromagnetic values used for the hard process. the Q or Q^2 renormalization scale at which alpha_strong and alpha_electromagnetic were evaluated. returns the stored SCALUP value for Les Houches events, and else zero. It may agree with both the QFac() and QRen() values, as explained above. However, to repeat, should the input SCALUP scale be negative, separate positive factorization and renormalization scales are calculated and set as for internally generated events. Furthermore, when PDF info is supplied for the Les Houches event, the factorization scale is set by this PDF info (scalePDF), which can disagree with SCALUP.

      Hard process kinematics

      The methods in this section provide info on the kinematics of the hard processes, with special emphasis on 2 -> 2 (diffraction excluded; see below). the invariant mass and its square for the hard process. the remaining two Mandelstam variables; only defined for 2 -> 2 processes. transverse momentum and its square in the rest frame of a 2 -> 2 processes. the masses of the two outgoing particles in a 2 -> 2 processes. the polar and azimuthal scattering angles in the rest frame of a 2 -> 2 process.

      Diffraction

      Information on the primary elastic or diffractive process (A B -> A B, X1 B, A X2, X1 X2, A X B) can be obtained with the methods in the "Hard process kinematics" section above. The variables here obviously are s, t, u, ... rather than sHat, tHat, uHat, ..., but the method names remain to avoid unnecessary duplication. Most other methods are irrelevant for a primary elastic/diffractive process.

      Central diffraction A B -> A X B is a 2 -> 3 process, and therefore most of the 2 -> 2 variables are no longer relevant. The tHat() and uHat() methods instead return the two t values at the A -> A and B -> B vertices, and pTHat() the average transverse momentum of the three outgoing "particles", while thetaHat() and phiHat() are undefined.

      While the primary interaction does not contain a hard process, the diffractive subsystems can contain them, but need not. Specifically, double diffraction can contain two separate hard subprocesses, which breaks the methods above. Most of them have been expanded with an optional argument to address properties of diffractive subsystems. This argument can take four values:

      • 0 : default argument, used for normal nondiffractive events or the primary elastic/diffractive process (see above);
      • 1 : the X1 system in single diffraction A B -> X1 B or double diffraction A B -> X1 X2;
      • 2 : the X2 system in single diffraction A B -> A X2 or double diffraction A B -> X1 X2;
      • 3 : the X system in central diffraction A B -> A X B.
      The argument is defined for all of the methods in the three sections above, "Hard process initiators", "Hard process parton densities and scales" and "Hard process kinematics", with the exception of the isValence methods. Also the four final methods of "The event type" section, the ...Sub() methods, take this argument. But recall that they will only provide meaningful answers, firstly if there is a system of the requested type, and secondly if there is a hard subprocess in this system. A simple check for this is that id1() has to be nonvanishing. The methods below this section do not currently provide information specific to diffractive subsystems, e.g. the MPI information is not bookkept in such cases.

      Event weight and activity

      weight assigned to the current event. Is normally 1 and thus uninteresting. However, there are several cases where one may have nontrivial event weights. These weights must the be used e.g. when filling histograms.
      (i) In the PhaseSpace:increaseMaximum = off default strategy, an event with a differential cross-section above the assumed one (in a given phase-space point) is assigned a weight correspondingly above unity. This should happen only very rarely, if at all, and so could normally be disregarded.
      (ii) The User Hooks class offers the possibility to bias the selection of phase space points, which means that events come with a compensating weight, stored here.
      (iii) For Les Houches events some strategies allow negative weights, which then after unweighting lead to events with weight -1. There are also Les Houches strategies where no unweighting is done, so events come with a weight. Specifically, for strategies +4 and -4, the event weight is in units of pb. (Internally in mb, but converted at output.)
      Sum of weights accumulated during the run. For unweighted events this agrees with the number of generated events. In order to obtain histograms normalized "per event", at the end of a run, histogram contents should be divided by this weight. (And additionally divided by the bin width.) Normalization to cross section also required multiplication by sigmaGen() below. normally 0, but if Les Houches events are input then it gives the event weighting strategy, see Les Houches Accord. the number of emissions in the initial-state showering, in the final-state showering excluding resonance decays, and in the final-state showering inside resonance decays, respectively. Maximum pT scales set for MPI, ISR and FSR, given the process type and scale choice for the hard interactions. The actual evolution will run down from these scales. The current pT scale in the combined MPI, ISR and FSR evolution. Useful for classification in user hooks, but not once the event has been evolved. combined leading-order merging weight assigned to the current event, if tree-level multi-jet merging (i.e. CKKW-L or UMEPS merging) is attempted. If tree-level multi-jet merging is performed, all histograms should be filled with this weight, as discussed in CKKW-L Merging and UMEPS Merging. combined NLO merging weight assigned to the current event, if NLO multi-jet merging (i.e. NL3 or UNLOPS merging) is attempted. If NLO multi-jet merging is performed, all histograms should be filled with this weight, as discussed in NLO Merging .

      Multiparton interactions

      As already noted, these methods do not make sense for diffractive topologies, and should not be used there. Partly this is physics, but mainly it is for technical reasons, e.g. that double diffraction involves two separate systems that would have to be bookkept as such. The value of a0 when an x-dependent matter profile is used, MultipartonInteractions:bProfile = 4. The impact parameter b assumed for the current collision when multiparton interactions are simulated. Is not expressed in any physical size (like fm), but only rescaled so that the average should be unity for minimum-bias events (meaning less than that for events with hard processes). The choice of impact parameter implies an enhancement or depletion of the rate of subsequent interactions, as given by this number. Again the average is normalized be unity for minimum-bias events (meaning more than that for events with hard processes). The number of hard interactions in the current event. Is 0 for elastic and diffractive events, and else at least 1, with more possible from multiparton interactions. the process code and transverse momentum of the i'th subprocess, with i in the range from 0 to nMPI() - 1. The values for subprocess 0 is redundant with information already provided above. are normally zero. However, if the i'th subprocess is a rescattering, i.e. either or both incoming partons come from the outgoing state of previous scatterings, they give the position in the event record of the outgoing-state parton that rescatters. iAMPI and iBMPI then denote partons coming from the first or second beam, respectively. The enhancement or depletion of the rate of the i'th subprocess. Is primarily of interest for the MultipartonInteractions:bProfile = 4 option, where the size of the proton depends on the x values of the colliding partons. Note that eMPI(0) = enhanceMPI().

      Cross sections

      Here are the currently available methods related to the event sample as a whole, for the default value i = 0, and otherwise for the specific process code provided as argument. This is the number obtained with Info::code(), while the further subdivision given by Info::codeSub() is not bookkept. While continuously updated during the run, it is recommended only to study these properties at the end of the event generation, when the full statistics is available. The individual process results are not available if a second hard process has been chosen, but can be gleaned from the pythia.stat() output. the total number of tried phase-space points, selected hard processes and finally accepted events, summed over all allowed processes (i = 0) or for the given process. The first number is only intended for a study of the phase-space selection efficiency. The last two numbers usually only disagree if the user introduces some veto during the event-generation process; then the former is the number of acceptable events found by PYTHIA and the latter the number that also were approved by the user. If you set a second hard process there may also be a mismatch. the estimated cross section and its estimated error, summed over all allowed processes (i = 0) or for the given process, in units of mb. The numbers refer to the accepted event sample above, i.e. after any user veto.

      Loop counters

      Mainly for internal/debug purposes, a number of loop counters from various parts of the program are stored in the Info class, so that one can keep track of how the event generation is progressing. This may be especially useful in the context of the User Hooks facility. the method that gives you access to the value of the various loop counters. the counter number you want to access: counters that refer to the run as a whole, i.e. are set 0 at the beginning of the run and then only can increase. the number of successful constructor calls for the Pythia class (can only be 0 or 1). the number of times a Pythia::init(...) call has been begun. the number of times a Pythia::init(...) call has been completed successfully. the number of times a Pythia::next() call has been begun. the number of times a Pythia::next() call has been completed successfully. counters that refer to each individual event, and are reset and updated in the top-level Pythia::next() method. the number of times the selection of a new hard process has been begun. Normally this should only happen once, unless a user veto is set to abort the current process and try a new one. the number of times the selection of a new hard process has been completed successfully. as 11, but additionally the process should survive any user veto and go on to the parton- and hadron-level stages. as 11, but additionally the process should survive the parton- and hadron-level stage and any user cuts. the number of times the loop over parton- and hadron-level processing has begun for a hard process. Is reset each time counter 12 above is reached. the number of times the above loop has successfully completed the parton-level step. the number of times the above loop has successfully completed the checks and user vetoes after the parton-level step. the number of times the above loop has successfully completed the hadron-level step. the number of times the above loop has successfully completed the checks and user vetoes after the hadron-level step. counters that refer to a local part of the individual event, and are reset at the beginning of this part. the current system being processed in PartonLevel::next(). Is almost always 1, but for double diffraction the two diffractive systems are 1 and 2, respectively. the number of times the processing of the current system (see above) has begun. the number of times a step has begun in the combined MPI/ISR/FSR evolution downwards in pT for the current system. the number of times MPI has been selected for the downwards step above. the number of times ISR has been selected for the downwards step above. the number of times FSR has been selected for the downwards step above. the number of times MPI has been accepted as the downwards step above, after the vetoes. the number of times ISR has been accepted as the downwards step above, after the vetoes. the number of times FSR has been accepted as the downwards step above, after the vetoes. the number of times a step has begun in the separate (optional) FSR evolution downwards in pT for the current system. the number of times FSR has been selected for the downwards step above. the number of times FSR has been accepted as the downwards step above, after the vetoes. counters that are unused (currently), and that therefore are free to use, with the help of the two methods below. set the above counters to a given value. Only to be used by you for the unassigned counters 40 - 49. the counter number, see above. set the counter to this number; normally the default value is what you want. increase the above counters by a given amount. Only to be used by you for the unassigned counters 40 - 49. the counter number, see above. increase the counter by this amount; normally the default value is what you want.

      Parton shower history

      The following methods are mainly intended for internal use, e.g. for matrix-element matching. set/get knowledge whether the likely shower history of an event has been traced. set/get value of z in latest ISR branching. set/get value of pT^2 in latest ISR branching.

      Header information

      A simple string key/value store, mainly intended for accessing information that is stored in the header block of Les Houches Event (LHE) files. In principle, any LHAup derived class can set this header information, which can then be read out later. Although the naming convention is arbitrary, in practice, it is dictated by the XML-like format of LHE files, see Les Houches Accord for more details. return the header named key return a vector of all header key names set the header named key with the contents of val
      pythia8-8.1.80.orig/xmldoc/SemiInternalResonances.xml0000444000175000017500000002640612217346317020770 0ustar sunsun

      Semi-Internal Resonances

      The introduction of a new semi-internal process may also involve a new particle, not currently implemented in PYTHIA. Often it is then enough to use the standard machinery to introduce a new particle (id:all = ...) and new decay channels (id:addChannel = ...). By default this only allows you to define a fixed total width and fixed branching ratios. Using meMode values 100 or bigger provides the possibility of a very simple threshold behaviour.

      If you want to have complete freedom, however, there are two ways to go. One is that you make the resonance decay part of the hard process itself, either using the Les Houches interface or a semi-internal process. The other is for you to create a new ResonanceWidths object, where you write the code needed for a calculation of the partial width of a particular channel.

      Here we will explain what is involved in setting up a resonance. Should you actually go ahead with this, it is strongly recommended to use an existing resonance as a template, to get the correct structure. There also exists a sample main program, main22.cc, that illustrates how you could combine a new process and a new resonance.

      There are three steps involved in implementing a new resonance:
      1) providing the standard particle information, as already outlined above (id:all = ..., id:addChannel = ...), except that now branching ratios need not be specified, since they anyway will be overwritten by the dynamically calculated values.
      2) writing the class that calculates the partial widths.
      3) handing in a pointer to an instance of this class to PYTHIA.
      We consider the latter two aspects in turn.

      The ResonanceWidths Class

      The resonance-width calculation has to be encoded in a new class. The relevant code could either be put before the main program in the same file, or be stored separately, e.g. in a matched pair of .h and .cc files. The latter may be more convenient, in particular if the calculations are lengthy, or likely to be used in many different runs, but of course requires that these additional files are correctly compiled and linked.

      The class has to be derived from the ResonanceWidths base class. It can implement a number of methods. The constructor and the calcWidth ones are always needed, while others are for convenience. Much of the administrative machinery is handled by methods in the base class.

      Thus, in particular, you must implement expressions for all possible final states, whether switched on in the current run or not, since all contribute to the total width needed in the denominator of the Breit-Wigner expression. Then the methods in the base class take care of selecting only allowed channels where that is required, and also of including effects of closed channels in secondary decays. These methods can be accessed indirectly via the res... methods of the normal particle database.

      A constructor for the derived class obviously must be available. Here you are quite free to allow a list of arguments, to set the parameters of your model. The constructor must call the base-class initBasic(idResIn) method, where the argument idResIn is the PDG-style identity code you have chosen for the new resonance. When you create several related resonances as instances of the same class you would naturally make idResIn an argument of the constructor; for the PYTHIA classes this convention is used also in cases when it is not needed.
      The initBasic(...) method will hook up the ResonanceWidths object with the corresponding entry in the generic particle database, i.e. with the normal particle information you set up in point 1) above. It will store, in base-class member variables, a number of quantities that you later may find useful:
      idRes : the identity code you provide;
      hasAntiRes : whether there is an antiparticle;
      mRes : resonance mass;
      GammaRes resonance width;
      m2Res : the squared mass;
      GamMRat : the ratio of width to mass.

      A destructor is only needed if you plan to delete the resonance before the natural end of the run, and require some special behaviour at that point. If you call such a destructor you will leave a pointer dangling inside the Pythia object you gave it in to, if that still exists. is called once during initialization, and can then be used to set up further parameters specific to this particle species, such as couplings, and perform calculations that need not be repeated for each new event, thereby saving time. This method needs not be implemented. is called once a mass has been chosen for the resonance, but before a specific final state is considered. This routine can therefore be used to perform calculations that otherwise might have to be repeated over and over again in calcWidth below. It is optional whether you want to use this method, however, or put everything in calcWidth().
      The optional argument will have the value true when the resonance is initialized, and then be false throughout the event generation, should you wish to make a distinction. In PYTHIA such a distinction is made for gamma^*/Z^0 and gamma^*/Z^0/Z'^0, owing to the necessity of a special description of interference effects, but not for other resonances.
      In addition to the base-class member variables already described above, mHat contains the current mass of the resonance. At initialization this agrees with the nominal mass mRes, but during the run it will not (in general).
      is the key method for width calculations and returns a partial width value, as further described below. It is called for a specific final state, typically in a loop over all allowed final states, subsequent to the calcPreFac(...) call above. Information on the final state is stored in a number of base-class variables, for you to use in your calculations:
      iChannel : the channel number in the list of possible decay channels;
      mult : the number of decay products;
      id1, id2, id3 : the identity code of up to the first three decay products, arranged in descending order of the absolute value of the identity code;
      id1Abs, id2Abs, id3Abs : the absolute value of the above three identity codes;
      mHat : the current resonance mass, which is the same as in the latest calcPreFac(...) call;
      mf1, mf2, mf3 : masses of the above decay products;
      mr1, mr2, mr3 : squared ratio of the product masses to the resonance mass;
      ps : is only meaningful for two-body decays, where it gives the phase-space factor ps = sqrt( (1. - mr1 - mr2)^2 - 4. * mr1 * mr2 );
      In two-body decays the third slot is zero for the above properties. Should there be more than three particles in the decay, you would have to take care of the subsequent products yourself, e.g. using
      particlePtr->decay[iChannel].product(j);
      to extract the j'th decay products (with j = 0 for the first, etc.). Currently we are not aware of any such examples.
      The base class also contains methods for alpha_em and alpha_strong evaluation, and can access many standard-model couplings; see the existing code for examples.
      The result of your calculation should be stored in
      widNow : the partial width of the current channel, expressed in GeV.
      is not normally used. In PYTHIA the only exception is Higgs decays, where it is used to define the width (except for colour factors) associated with a specific incoming/outgoing state. It allows the results of some loop expressions to be pretabulated. can normally be left dummy (and then always returns true) but can optionally be used to determine whether to force dynamical width calculation to be switched off (return false). An example is provided by the SUSYResonanceWidths class, in which the implementation of this method checks for the existence of SLHA decay tables for the particular resonance in question, and checks if those tables should be given precedence over the internal width calculation. can normally be left dummy, but for advanced implementations it provides a possibility to initialize data members of the derived class at a very early stage during initialization, before any of the other members are called. An example is provided by the SUSYResonanceWidths class, in which an internal pointer to a derived Couplings class must be (re)set before any of the other methods are used. A return value of false can be used to signal that this initialization step failed.

      Access to resonance widths

      Once you have implemented a class, it is straightforward to make use of it in a run. Assume you have written a new class MyResonance, which inherits from ResonanceWidths. You then create an instance of this class and hand it in to a pythia object with
            ResonanceWidths* myResonance = new MyResonance();
            pythia.setResonancePtr( myResonance); 
      
      If you have several resonances you can repeat the procedure any number of times. When pythia.init(...) is called these resonances are initialized along with all the internal resonances, and treated in exactly the same manner. See also the Program Flow description.

      If the code should be of good quality and general usefulness, it would be simple to include it as a permanently available process in the standard program distribution. The final step of that integration ought to be left for the PYTHIA authors, but basically all that is needed is to add one line in ParticleData::initResonances, where one creates an instance of the resonance in the same way as for the resonances already there. In addition, the particle data and decay table for the new resonance has to be added to the permanent particle database, and the code itself to include/ResonanceWidths.h and src/ResonanceWidths.cc. pythia8-8.1.80.orig/include/0000755000175000017500000000000012217346224013757 5ustar sunsunpythia8-8.1.80.orig/include/.DS_Store0000644000175000017500000001400412217346224015441 0ustar sunsunBud1ia8lg1ScoPythia8lg1Scomp RPythia8moDDdutcPythia8modDdutcPythia8ph1Scomp p  @ @ @ @ EDSDB ` @ @ @pythia8-8.1.80.orig/include/Pythia8/0000755000175000017500000000000012217346232015304 5ustar sunsunpythia8-8.1.80.orig/include/Pythia8/MultipartonInteractions.h0000644000175000017500000002677212217346230022372 0ustar sunsun// MultipartonInteractions.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the main classes for multiparton interactions physics. // SigmaMultiparton stores allowed processes by in-flavour combination. // MultipartonInteractions: generates multiparton parton-parton interactions. #ifndef Pythia8_MultipartonInteractions_H #define Pythia8_MultipartonInteractions_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/PartonSystems.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" #include "Pythia8/SigmaTotal.h" #include "Pythia8/SigmaProcess.h" #include "Pythia8/StandardModel.h" #include "Pythia8/UserHooks.h" namespace Pythia8 { //========================================================================== // SigmaMultiparton is a helper class to MultipartonInteractions. // It packs pointers to the allowed processes for different // flavour combinations and levels of ambition. class SigmaMultiparton { public: // Constructor. SigmaMultiparton() {} // Destructor. ~SigmaMultiparton() { for (int i = 0; i < int(sigmaT.size()); ++i) delete sigmaT[i]; for (int i = 0; i < int(sigmaU.size()); ++i) delete sigmaU[i];} // Initialize list of processes. bool init(int inState, int processLevel, Info* infoPtr, Settings* settingsPtr, ParticleData* particleDataPtr, Rndm* rndmPtrIn, BeamParticle* beamAPtr, BeamParticle* beamBPtr, Couplings* couplingsPtr); // Calculate cross section summed over possibilities. double sigma( int id1, int id2, double x1, double x2, double sHat, double tHat, double uHat, double alpS, double alpEM, bool restore = false, bool pickOtherIn = false); // Return whether the other, rare processes were selected. bool pickedOther() {return pickOther;} // Return one subprocess, picked according to relative cross sections. SigmaProcess* sigmaSel(); bool swapTU() {return pickedU;} // Return code or name of a specified process, for statistics table. int nProc() const {return nChan;} int codeProc(int iProc) const {return sigmaT[iProc]->code();} string nameProc(int iProc) const {return sigmaT[iProc]->name();} private: // Constants: could only be changed in the code itself. static const double MASSMARGIN, OTHERFRAC; // Number of processes. Some use massive matrix elements. int nChan; vector needMasses; vector m3Fix, m4Fix, sHatMin; // Vector of process list, one for t-channel and one for u-channel. vector sigmaT, sigmaU; // Values of cross sections in process list above. vector sigmaTval, sigmaUval; double sigmaTsum, sigmaUsum; bool pickOther, pickedU; // Pointer to the random number generator. Rndm* rndmPtr; }; //========================================================================== // The MultipartonInteractions class contains the main methods for the // generation of multiparton parton-parton interactions in hadronic collisions. class MultipartonInteractions { public: // Constructor. MultipartonInteractions() : bIsSet(false) {} // Initialize the generation process for given beams. bool init( bool doMPIinit, int iDiffSysIn, Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtr, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, Couplings* couplingsPtrIn, PartonSystems* partonSystemsPtrIn, SigmaTotal* sigmaTotPtrIn, UserHooks* userHooksPtrIn, ostream& os = cout); // Reset impact parameter choice and update the CM energy. void reset(); // Select first = hardest pT in nondiffractive process. void pTfirst(); // Set up kinematics for first = hardest pT in nondiffractive process. void setupFirstSys( Event& process); // Find whether to limit maximum scale of emissions. bool limitPTmax( Event& event); // Prepare system for evolution. void prepare(Event& event, double pTscale = 1000.) { if (!bSetInFirst) overlapNext(event, pTscale); } // Select next pT in downwards evolution. double pTnext( double pTbegAll, double pTendAll, Event& event); // Set up kinematics of acceptable interaction. bool scatter( Event& event); // Set "empty" values to avoid query of undefined quantities. void setEmpty() {pT2Ren = alpS = alpEM = x1 = x2 = pT2Fac = xPDF1now = xPDF2now = 0.; bIsSet = false;} // Get some information on current interaction. double Q2Ren() const {return pT2Ren;} double alphaSH() const {return alpS;} double alphaEMH() const {return alpEM;} double x1H() const {return x1;} double x2H() const {return x2;} double Q2Fac() const {return pT2Fac;} double pdf1() const {return xPDF1now;} double pdf2() const {return xPDF2now;} double bMPI() const {return (bIsSet) ? bNow / bAvg : 0.;} double enhanceMPI() const {return (bIsSet) ? enhanceB / zeroIntCorr : 1.;} // For x-dependent matter profile, return incoming valence/sea // decision from trial interactions. int getVSC1() const {return vsc1;} int getVSC2() const {return vsc2;} // Update and print statistics on number of processes. // Note: currently only valid for nondiffractive systems, not diffraction?? void accumulate() { int iBeg = (infoPtr->isNonDiffractive()) ? 0 : 1; for (int i = iBeg; i < infoPtr->nMPI(); ++i) ++nGen[ infoPtr->codeMPI(i) ];} void statistics(bool resetStat = false, ostream& os = cout); void resetStatistics() { for ( map::iterator iter = nGen.begin(); iter != nGen.end(); ++iter) iter->second = 0; } private: // Constants: could only be changed in the code itself. static const bool SHIFTFACSCALE, PREPICKRESCATTER; static const double SIGMAFUDGE, RPT20, PT0STEP, SIGMASTEP, PT0MIN, EXPPOWMIN, PROBATLOWB, BSTEP, BMAX, EXPMAX, KCONVERGE, CONVERT2MB, ROOTMIN, ECMDEV, WTACCWARN; // Initialization data, read from Settings. bool allowRescatter, allowDoubleRes, canVetoMPI; int pTmaxMatch, alphaSorder, alphaEMorder, alphaSnfmax, bProfile, processLevel, bSelScale, rescatterMode, nQuarkIn, nSample, enhanceScreening; double alphaSvalue, Kfactor, pT0Ref, ecmRef, ecmPow, pTmin, coreRadius, coreFraction, expPow, ySepResc, deltaYResc, sigmaPomP, mPomP, pPomP, mMaxPertDiff, mMinPertDiff; // x-dependent matter profile: // Constants. static const int XDEP_BBIN; static const double XDEP_A0, XDEP_A1, XDEP_BSTEP, XDEP_BSTEPINC, XDEP_CUTOFF, XDEP_WARN, XDEP_SMB2FM; // Table of Int( dSigma/dX * O(b, X), dX ) in bins of b for fast // integration. Only needed during initialisation. vector sigmaIntWgt, sigmaSumWgt; // a1: value of a1 constant, taken from settings database. // a0now (a02now): tuned value of a0 (squared value). // bstepNow: current size of bins in b. // a2max: given an xMin, a maximal (squared) value of the // width, to be used in overestimate Omax(b). // enhanceBmax, retain enhanceB as enhancement factor for the hardest // enhanceBnow: interaction. Use enhanceBmax as overestimate for fastPT2, // and enhanceBnow to store the value for the current // interaction. double a1, a0now, a02now, bstepNow, a2max, b2now, enhanceBmax, enhanceBnow; // Storage for trial interactions. int id1Save, id2Save; double pT2Save, x1Save, x2Save, sHatSave, tHatSave, uHatSave, alpSsave, alpEMsave, pT2FacSave, pT2RenSave, xPDF1nowSave, xPDF2nowSave; SigmaProcess *dSigmaDtSelSave; // vsc1, vsc2: for minimum-bias events with trial interaction, store // decision on whether hard interaction was valence or sea. int vsc1, vsc2; // Other initialization data. bool hasBaryonBeams, hasLowPow, globalRecoilFSR; int iDiffSys, nMaxGlobalRecoilFSR; double eCM, sCM, pT0, pT20, pT2min, pTmax, pT2max, pT20R, pT20minR, pT20maxR, pT20min0maxR, pT2maxmin, sigmaND, pT4dSigmaMax, pT4dProbMax, dSigmaApprox, sigmaInt, sudExpPT[101], zeroIntCorr, normOverlap, nAvg, kNow, normPi, bAvg, bDiv, probLowB, radius2B, radius2C, fracA, fracB, fracC, fracAhigh, fracBhigh, fracChigh, fracABChigh, expRev, cDiv, cMax; // Properties specific to current system. bool bIsSet, bSetInFirst, isAtLowB, pickOtherSel; int id1, id2, i1Sel, i2Sel, id1Sel, id2Sel; double bNow, enhanceB, pT2, pT2shift, pT2Ren, pT2Fac, x1, x2, xT, xT2, tau, y, sHat, tHat, uHat, alpS, alpEM, xPDF1now, xPDF2now, dSigmaSum, x1Sel, x2Sel, sHatSel, tHatSel, uHatSel; // Stored values for mass interpolation for diffractive systems. int nStep, iStepFrom, iStepTo; double eCMsave, eStepSize, eStepSave, eStepFrom, eStepTo, pT0Save[5], pT4dSigmaMaxSave[5], pT4dProbMaxSave[5], sigmaIntSave[5], sudExpPTSave[5][101], zeroIntCorrSave[5], normOverlapSave[5], kNowSave[5], bAvgSave[5], bDivSave[5], probLowBSave[5], fracAhighSave[5], fracBhighSave[5], fracChighSave[5], fracABChighSave[5], cDivSave[5], cMaxSave[5]; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to the two incoming beams. BeamParticle* beamAPtr; BeamParticle* beamBPtr; // Pointers to Standard Model couplings. Couplings* couplingsPtr; // Pointer to information on subcollision parton locations. PartonSystems* partonSystemsPtr; // Pointer to total cross section parametrization. SigmaTotal* sigmaTotPtr; // Pointer to user hooks. UserHooks* userHooksPtr; // Collections of parton-level 2 -> 2 cross sections. Selected one. SigmaMultiparton sigma2gg, sigma2qg, sigma2qqbarSame, sigma2qq; SigmaMultiparton* sigma2Sel; SigmaProcess* dSigmaDtSel; // Statistics on generated 2 -> 2 processes. map nGen; // alphaStrong and alphaEM calculations. AlphaStrong alphaS; AlphaEM alphaEM; // Scattered partons. vector scatteredA, scatteredB; // Determine constant in d(Prob)/d(pT2) < const / (pT2 + r * pT20)^2. void upperEnvelope(); // Integrate the parton-parton interaction cross section. void jetCrossSection(); // Evaluate "Sudakov form factor" for not having a harder interaction. double sudakov(double pT2sud, double enhance = 1.); // Do a quick evolution towards the next smaller pT. double fastPT2( double pT2beg); // Calculate the actual cross section, either for the first interaction // (including at initialization) or for any subsequent in the sequence. double sigmaPT2scatter(bool isFirst = false); // Find the partons that may rescatter. void findScatteredPartons( Event& event); // Calculate the actual cross section for a rescattering. double sigmaPT2rescatter( Event& event); // Calculate factor relating matter overlap and interaction rate. void overlapInit(); // Pick impact parameter and interaction rate enhancement, // either before the first interaction (for nondiffractive) or after it. void overlapFirst(); void overlapNext(Event& event, double pTscale); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_MultipartonInteractions_H pythia8-8.1.80.orig/include/Pythia8/Merging.h0000644000175000017500000000651212217346227017055 0ustar sunsun// Merging.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file is written by Stefan Prestel. // Merging: Wpapper class to interface matrix element merging schemes with // Pythia #ifndef Pythia8_Merging_H #define Pythia8_Merging_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" #include "Pythia8/PartonLevel.h" #include "Pythia8/MergingHooks.h" #include "Pythia8/History.h" namespace Pythia8 { //========================================================================== // Merging is a wrapper class for the interface of matrix element merging and // Pythia8. class Merging { public: // Constructor. Merging() { settingsPtr = 0; infoPtr = 0; particleDataPtr = 0; rndmPtr = 0; beamAPtr = 0; beamBPtr = 0; trialPartonLevelPtr = 0; mergingHooksPtr = 0; } // Make Pythia class friend friend class Pythia; // Destructor. ~Merging(){} protected: //----------------------------------------------------------------------// // The members //----------------------------------------------------------------------// // Settings: databases of flags/modes/parms/words to control run. Settings* settingsPtr; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to random number generator. Rndm* rndmPtr; // Pointer to trial PartonLevel object PartonLevel* trialPartonLevelPtr; // Pointer to trial MergingHooks object MergingHooks* mergingHooksPtr; // Pointers to beam particles. BeamParticle* beamAPtr; BeamParticle* beamBPtr; // Minimal value found for the merging scale in events. double tmsNowMin; static const double TMSMISMATCH; // Initialisation function for internal use inside Pythia source code void init( Settings* settingsPtrIn, Info* infoPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, MergingHooks* mergingHooksPtrIn, PartonLevel* trialPartonLevelPtrIn ); // Function to print statistics. void statistics(ostream& os = cout); //----------------------------------------------------------------------// // Functions that implement matrix element merging. //----------------------------------------------------------------------// // Function to steer different merging prescriptions. int mergeProcess( Event& process); // Function to perform CKKW-L merging on the event. int mergeProcessCKKWL( Event& process); // Function to perform UMEPS merging on the event. int mergeProcessUMEPS( Event& process); // Function to perform NL3 NLO merging on the event. int mergeProcessNL3( Event& process); // Function to perform UNLOPS merging on the event. int mergeProcessUNLOPS( Event& process); // Function to apply the merging scale cut on an input event. bool cutOnProcess( Event& process); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_Merging_H pythia8-8.1.80.orig/include/Pythia8/ResonanceDecays.h0000644000175000017500000000442612217346230020527 0ustar sunsun// ResonanceDecays.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the main class for performing resonance decays. // ResonanceDecays: handles the sequential decay of resonances in process. #ifndef Pythia8_ResonanceDecays_H #define Pythia8_ResonanceDecays_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/ResonanceWidths.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // The ResonanceDecays class handles the sequential decay of resonances // that are part of the hard process (t, W, Z, H, SUSY,...). class ResonanceDecays { public: // Constructor. ResonanceDecays() {} // Store pointers to Info and Rndm for error messages and random numbers. void init(Info* infoPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn) {infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn;} // Generate the next decay sequence. bool next( Event& process, int iDecNow = 0); private: // Constants: could only be changed in the code itself. static const int NTRYCHANNEL, NTRYMASSES; static const double MSAFETY, WIDTHCUT, TINY, TINYBWRANGE, WTCORRECTION[11]; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Select masses of decay products. bool pickMasses(); // Select colours of decay products. bool pickColours(int iDec, Event& process); // Select kinematics isotropic in phase space. bool pickKinematics(); // Flavour, colour and momentum information. int id0, mult; double m0; vector idProd, cols, acols; vector mProd; vector pProd; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_ResonanceDecays_H pythia8-8.1.80.orig/include/Pythia8/Event.h0000644000175000017500000006340412217346226016550 0ustar sunsun// Event.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for the Particle and Event classes. // Particle: information on an instance of a particle. // Junction: information on a junction between three colours. // Event: list of particles in the current event. #ifndef Pythia8_Event_H #define Pythia8_Event_H #include "Pythia8/Basics.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" namespace Pythia8 { //========================================================================== // Forward references to ParticleDataEntry and ResonanceWidths classes. class ParticleDataEntry; class ResonanceWidths; class Event; //========================================================================== // Particle class. // This class holds info on a particle in general. class Particle { public: // Constructors. Particle() : idSave(0), statusSave(0), mother1Save(0), mother2Save(0), daughter1Save(0), daughter2Save(0), colSave(0), acolSave(0), pSave(Vec4(0.,0.,0.,0.)), mSave(0.), scaleSave(0.), polSave(9.), hasVertexSave(false), vProdSave(Vec4(0.,0.,0.,0.)), tauSave(0.), pdePtr(0), evtPtr(0) { } Particle(int idIn, int statusIn = 0, int mother1In = 0, int mother2In = 0, int daughter1In = 0, int daughter2In = 0, int colIn = 0, int acolIn = 0, double pxIn = 0., double pyIn = 0., double pzIn = 0., double eIn = 0., double mIn = 0., double scaleIn = 0., double polIn = 9.) : idSave(idIn), statusSave(statusIn), mother1Save(mother1In), mother2Save(mother2In), daughter1Save(daughter1In), daughter2Save(daughter2In), colSave(colIn), acolSave(acolIn), pSave(Vec4(pxIn, pyIn, pzIn, eIn)), mSave(mIn), scaleSave(scaleIn), polSave(polIn), hasVertexSave(false), vProdSave(Vec4(0.,0.,0.,0.)), tauSave(0.), pdePtr(0), evtPtr(0) { } Particle(int idIn, int statusIn, int mother1In, int mother2In, int daughter1In, int daughter2In, int colIn, int acolIn, Vec4 pIn, double mIn = 0., double scaleIn = 0., double polIn = 9.) : idSave(idIn), statusSave(statusIn), mother1Save(mother1In), mother2Save(mother2In), daughter1Save(daughter1In), daughter2Save(daughter2In), colSave(colIn), acolSave(acolIn), pSave(pIn), mSave(mIn), scaleSave(scaleIn), polSave(polIn), hasVertexSave(false), vProdSave(Vec4(0.,0.,0.,0.)), tauSave(0.), pdePtr(0), evtPtr(0) { } Particle(const Particle& pt) : idSave(pt.idSave), statusSave(pt.statusSave), mother1Save(pt.mother1Save), mother2Save(pt.mother2Save), daughter1Save(pt.daughter1Save), daughter2Save(pt.daughter2Save), colSave(pt.colSave), acolSave(pt.acolSave), pSave(pt.pSave), mSave(pt.mSave), scaleSave(pt.scaleSave), polSave(pt.polSave), hasVertexSave(pt.hasVertexSave), vProdSave(pt.vProdSave), tauSave(pt.tauSave), pdePtr(pt.pdePtr), evtPtr(pt.evtPtr) { } Particle& operator=(const Particle& pt) {if (this != &pt) { idSave = pt.idSave; statusSave = pt.statusSave; mother1Save = pt.mother1Save; mother2Save = pt.mother2Save; daughter1Save = pt.daughter1Save; daughter2Save = pt.daughter2Save; colSave = pt.colSave; acolSave = pt.acolSave; pSave = pt.pSave; mSave = pt.mSave; scaleSave = pt.scaleSave; polSave = pt.polSave; hasVertexSave = pt.hasVertexSave; vProdSave = pt.vProdSave; tauSave = pt.tauSave; pdePtr = pt.pdePtr; evtPtr = pt.evtPtr; } return *this; } // Member functions to set the Event and ParticleDataEntry pointers. void setEvtPtr(Event* evtPtrIn) { evtPtr = evtPtrIn; setPDEPtr();} void setPDEPtr(ParticleDataEntry* pdePtrIn = 0); // Member functions for input. void id(int idIn) {idSave = idIn; setPDEPtr();} void status(int statusIn) {statusSave = statusIn;} void statusPos() {statusSave = abs(statusSave);} void statusNeg() {statusSave = -abs(statusSave);} void statusCode(int statusIn) {statusSave = (statusSave > 0) ? abs(statusIn) : -abs(statusIn);} void mother1(int mother1In) {mother1Save = mother1In;} void mother2(int mother2In) {mother2Save = mother2In;} void mothers(int mother1In = 0, int mother2In = 0) {mother1Save = mother1In; mother2Save = mother2In;} void daughter1(int daughter1In) {daughter1Save = daughter1In;} void daughter2(int daughter2In) {daughter2Save = daughter2In;} void daughters(int daughter1In = 0, int daughter2In = 0) {daughter1Save = daughter1In; daughter2Save = daughter2In;} void col(int colIn) {colSave = colIn;} void acol(int acolIn) {acolSave = acolIn;} void cols(int colIn = 0,int acolIn = 0) {colSave = colIn; acolSave = acolIn;} void p(Vec4 pIn) {pSave = pIn;} void p(double pxIn, double pyIn, double pzIn, double eIn) {pSave.p(pxIn, pyIn, pzIn, eIn);} void px(double pxIn) {pSave.px(pxIn);} void py(double pyIn) {pSave.py(pyIn);} void pz(double pzIn) {pSave.pz(pzIn);} void e(double eIn) {pSave.e(eIn);} void m(double mIn) {mSave = mIn;} void scale(double scaleIn) {scaleSave = scaleIn;} void pol(double polIn) {polSave = polIn;} void vProd(Vec4 vProdIn) {vProdSave = vProdIn; hasVertexSave = true;} void vProd(double xProdIn, double yProdIn, double zProdIn, double tProdIn) {vProdSave.p(xProdIn, yProdIn, zProdIn, tProdIn); hasVertexSave = true;} void xProd(double xProdIn) {vProdSave.px(xProdIn); hasVertexSave = true;} void yProd(double yProdIn) {vProdSave.py(yProdIn); hasVertexSave = true;} void zProd(double zProdIn) {vProdSave.pz(zProdIn); hasVertexSave = true;} void tProd(double tProdIn) {vProdSave.e(tProdIn); hasVertexSave = true;} void tau(double tauIn) {tauSave = tauIn;} // Member functions for output. int id() const {return idSave;} int status() const {return statusSave;} int mother1() const {return mother1Save;} int mother2() const {return mother2Save;} int daughter1() const {return daughter1Save;} int daughter2() const {return daughter2Save;} int col() const {return colSave;} int acol() const {return acolSave;} Vec4 p() const {return pSave;} double px() const {return pSave.px();} double py() const {return pSave.py();} double pz() const {return pSave.pz();} double e() const {return pSave.e();} double m() const {return mSave;} double scale() const {return scaleSave;} double pol() const {return polSave;} bool hasVertex() const {return hasVertexSave;} Vec4 vProd() const {return vProdSave;} double xProd() const {return vProdSave.px();} double yProd() const {return vProdSave.py();} double zProd() const {return vProdSave.pz();} double tProd() const {return vProdSave.e();} double tau() const {return tauSave;} // Member functions for output; derived int and bool quantities. int idAbs() const {return abs(idSave);} int statusAbs() const {return abs(statusSave);} bool isFinal() const {return (statusSave > 0);} bool isRescatteredIncoming() const {return (statusSave == -34 || statusSave == -45 || statusSave == -46 || statusSave == -54);} // Member functions for output; derived double quantities. double m2() const {return (mSave >= 0.) ? mSave*mSave : -mSave*mSave;} double mCalc() const {return pSave.mCalc();} double m2Calc() const {return pSave.m2Calc();} double eCalc() const {return sqrt(abs(m2() + pSave.pAbs2()));} double pT() const {return pSave.pT();} double pT2() const {return pSave.pT2();} double mT() const {double temp = m2() + pSave.pT2(); return (temp >= 0.) ? sqrt(temp) : -sqrt(-temp);} double mT2() const {return m2() + pSave.pT2();} double pAbs() const {return pSave.pAbs();} double pAbs2() const {return pSave.pAbs2();} double eT() const {return pSave.eT();} double eT2() const {return pSave.eT2();} double theta() const {return pSave.theta();} double phi() const {return pSave.phi();} double thetaXZ() const {return pSave.thetaXZ();} double pPos() const {return pSave.pPos();} double pNeg() const {return pSave.pNeg();} double y() const; double eta() const; Vec4 vDec() const {return (tauSave > 0. && mSave > 0.) ? vProdSave + tauSave * pSave / mSave : vProdSave;} double xDec() const {return (tauSave > 0. && mSave > 0.) ? vProdSave.px() + tauSave * pSave.px() / mSave : vProdSave.px();} double yDec() const {return (tauSave > 0. && mSave > 0.) ? vProdSave.py() + tauSave * pSave.py() / mSave : vProdSave.py();} double zDec() const {return (tauSave > 0. && mSave > 0.) ? vProdSave.pz() + tauSave * pSave.pz() / mSave : vProdSave.pz();} double tDec() const {return (tauSave > 0. && mSave > 0.) ? vProdSave.e() + tauSave * pSave.e() / mSave : vProdSave.e();} // Methods that can refer back to the event the particle belongs to. int index() const; int statusHepMC() const; int iTopCopy() const; int iBotCopy() const; int iTopCopyId() const; int iBotCopyId() const; vector motherList() const; vector daughterList() const; vector sisterList(bool traceTopBot = false) const; bool isAncestor(int iAncestor) const; bool undoDecay(); // Further output, based on a pointer to a ParticleDataEntry object. string name() const { return (pdePtr != 0) ? pdePtr->name(idSave) : " ";} string nameWithStatus(int maxLen = 20) const; int spinType() const { return (pdePtr != 0) ? pdePtr->spinType() : 0;} int chargeType() const { return (pdePtr != 0) ? pdePtr->chargeType(idSave) : 0;} double charge() const { return (pdePtr != 0) ? pdePtr->charge(idSave) : 0;} bool isCharged() const { return (pdePtr != 0) ? (pdePtr->chargeType(idSave) != 0) : false;} bool isNeutral() const { return (pdePtr != 0) ? (pdePtr->chargeType(idSave) == 0) : false;} int colType() const { return (pdePtr != 0) ? pdePtr->colType(idSave) : 0;} double m0() const { return (pdePtr != 0) ? pdePtr->m0() : 0.;} double mWidth() const { return (pdePtr != 0) ? pdePtr->mWidth() : 0.;} double mMin() const { return (pdePtr != 0) ? pdePtr->mMin() : 0.;} double mMax() const { return (pdePtr != 0) ? pdePtr->mMax() : 0.;} double mSel() const { return (pdePtr != 0) ? pdePtr->mSel() : 0.;} double constituentMass() const { return (pdePtr != 0) ? pdePtr->constituentMass() : 0.;} double tau0() const { return (pdePtr != 0) ? pdePtr->tau0() : 0.;} bool mayDecay() const { return (pdePtr != 0) ? pdePtr->mayDecay() : false;} bool canDecay() const { return (pdePtr != 0) ? pdePtr->canDecay() : false;} bool doExternalDecay() const { return (pdePtr != 0) ? pdePtr->doExternalDecay() : false;} bool isResonance() const { return (pdePtr != 0) ? pdePtr->isResonance() : false;} bool isVisible() const { return (pdePtr != 0) ? pdePtr->isVisible() : false;} bool isLepton() const { return (pdePtr != 0) ? pdePtr->isLepton() : false;} bool isQuark() const { return (pdePtr != 0) ? pdePtr->isQuark() : false;} bool isGluon() const { return (pdePtr != 0) ? pdePtr->isGluon() : false;} bool isDiquark() const { return (pdePtr != 0) ? pdePtr->isDiquark() : false;} bool isParton() const { return (pdePtr != 0) ? pdePtr->isParton() : false;} bool isHadron() const { return (pdePtr != 0) ? pdePtr->isHadron() : false;} ParticleDataEntry& particleDataEntry() const {return *pdePtr;} // Member functions that perform operations. void rescale3(double fac) {pSave.rescale3(fac);} void rescale4(double fac) {pSave.rescale4(fac);} void rescale5(double fac) {pSave.rescale4(fac); mSave *= fac;} void rot(double thetaIn, double phiIn) {pSave.rot(thetaIn, phiIn); if (hasVertexSave) vProdSave.rot(thetaIn, phiIn);} void bst(double betaX, double betaY, double betaZ) { pSave.bst(betaX, betaY, betaZ); if (hasVertexSave) vProdSave.bst(betaX, betaY, betaZ);} void bst(double betaX, double betaY, double betaZ, double gamma) { pSave.bst(betaX, betaY, betaZ, gamma); if (hasVertexSave) vProdSave.bst(betaX, betaY, betaZ, gamma);} void bst(const Vec4& pBst) {pSave.bst(pBst); if (hasVertexSave) vProdSave.bst(pBst);} void bst(const Vec4& pBst, double mBst) {pSave.bst(pBst, mBst); if (hasVertexSave) vProdSave.bst(pBst, mBst);} void bstback(const Vec4& pBst) {pSave.bstback(pBst); if (hasVertexSave) vProdSave.bstback(pBst);} void bstback(const Vec4& pBst, double mBst) {pSave.bstback(pBst, mBst); if (hasVertexSave) vProdSave.bstback(pBst, mBst);} void rotbst(const RotBstMatrix& M) {pSave.rotbst(M); if (hasVertexSave) vProdSave.rotbst(M);} void offsetHistory( int minMother, int addMother, int minDaughter, int addDaughter); void offsetCol( int addCol); private: // Constants: could only be changed in the code itself. static const double TINY; // Properties of the current particle. int idSave, statusSave, mother1Save, mother2Save, daughter1Save, daughter2Save, colSave, acolSave; Vec4 pSave; double mSave, scaleSave, polSave; bool hasVertexSave; Vec4 vProdSave; double tauSave; // Pointer to properties of the particle species. // Should no be saved in a persistent copy of the event record. // The //! below is ROOT notation that this member should not be saved. // Event::restorePtrs() can be called to restore the missing information. ParticleDataEntry* pdePtr; //! // Pointer to the whole event record to which the particle belongs (if any). // As above it should not be saved. Event* evtPtr; //! }; // Invariant mass of a pair and its square. // (Not part of class proper, but tightly linked.) double m(const Particle&, const Particle&); double m2(const Particle&, const Particle&); //========================================================================== // The junction class stores what kind of junction it is, the colour indices // of the legs at the junction and as far out as legs have been traced, // and the status codes assigned for fragmentation of each leg. class Junction { public: // Constructors. Junction() : remainsSave(true), kindSave(0) { for (int j = 0; j < 3; ++j) { colSave[j] = 0; endColSave[j] = 0; statusSave[j] = 0; } } Junction( int kindIn, int col0In, int col1In, int col2In) : remainsSave(true), kindSave(kindIn) {colSave[0] = col0In; colSave[1] = col1In; colSave[2] = col2In; for (int j = 0; j < 3; ++j) { endColSave[j] = colSave[j]; statusSave[j] = 0; } } Junction(const Junction& ju) : remainsSave(ju.remainsSave), kindSave(ju.kindSave) { for (int j = 0; j < 3; ++j) { colSave[j] = ju.colSave[j]; endColSave[j] = ju.endColSave[j]; statusSave[j] = ju.statusSave[j]; } } Junction& operator=(const Junction& ju) {if (this != &ju) { remainsSave = ju.remainsSave; kindSave = ju.kindSave; for (int j = 0; j < 3; ++j) { colSave[j] = ju.colSave[j]; endColSave[j] = ju.endColSave[j]; statusSave[j] = ju.statusSave[j]; } } return *this; } // Set values. void remains(bool remainsIn) {remainsSave = remainsIn;} void col(int j, int colIn) {colSave[j] = colIn; endColSave[j] = colIn;} void cols(int j, int colIn, int endColIn) {colSave[j] = colIn; endColSave[j] = endColIn;} void endCol(int j, int endColIn) {endColSave[j] = endColIn;} void status(int j, int statusIn) {statusSave[j] = statusIn;} // Read out value. bool remains() const {return remainsSave;} int kind() const {return kindSave;} int col(int j) const {return colSave[j];} int endCol(int j) const {return endColSave[j];} int status(int j) const {return statusSave[j];} private: // Kind, positions of the three ends and their status codes. bool remainsSave; int kindSave, colSave[3], endColSave[3], statusSave[3]; }; //========================================================================== // The Event class holds all info on the generated event. class Event { public: // Constructors. Event(int capacity = 100) : startColTag(100), maxColTag(100), savedSize(0), savedJunctionSize(0), scaleSave(0.), scaleSecondSave(0.), headerList("----------------------------------------"), particleDataPtr(0) { entry.reserve(capacity); } Event& operator=(const Event& oldEvent); Event(const Event& oldEvent) {*this = oldEvent;} // Initialize header for event listing, particle data table, and colour. void init( string headerIn = "", ParticleData* particleDataPtrIn = 0, int startColTagIn = 100) { headerList.replace(0, headerIn.length() + 2, headerIn + " "); particleDataPtr = particleDataPtrIn; startColTag = startColTagIn;} // Clear event record. void clear() {entry.resize(0); maxColTag = startColTag; scaleSave = 0.; scaleSecondSave = 0.; clearJunctions();} // Clear event record, and set first particle empty. void reset() {clear(); append(90, -11, 0, 0, 0., 0., 0., 0., 0.);} // Overload index operator to access element of event record. Particle& operator[](int i) {return entry[i];} const Particle& operator[](int i) const {return entry[i];} // Implement standard references to elements in the particle array. Particle& front() {return entry.front();} Particle& at(int i) {return entry.at(i);} Particle& back() {return entry.back();} // Event record size. int size() const {return entry.size();} // Put a new particle at the end of the event record; return index. int append(Particle entryIn) { entry.push_back(entryIn); setEvtPtr(); if (entryIn.col() > maxColTag) maxColTag = entryIn.col(); if (entryIn.acol() > maxColTag) maxColTag = entryIn.acol(); return entry.size() - 1; } int append(int id, int status, int mother1, int mother2, int daughter1, int daughter2, int col, int acol, double px, double py, double pz, double e, double m = 0., double scaleIn = 0., double polIn = 9.) { entry.push_back( Particle(id, status, mother1, mother2, daughter1, daughter2, col, acol, px, py, pz, e, m, scaleIn, polIn) ); setEvtPtr(); if (col > maxColTag) maxColTag = col; if (acol > maxColTag) maxColTag = acol; return entry.size() - 1; } int append(int id, int status, int mother1, int mother2, int daughter1, int daughter2, int col, int acol, Vec4 p, double m = 0., double scaleIn = 0., double polIn = 9.) { entry.push_back( Particle(id, status, mother1, mother2, daughter1, daughter2, col, acol, p, m, scaleIn, polIn) ); setEvtPtr(); if (col > maxColTag) maxColTag = col; if (acol > maxColTag) maxColTag = acol; return entry.size() - 1; } // Brief versions of append: no mothers and no daughters. int append(int id, int status, int col, int acol, double px, double py, double pz, double e, double m = 0., double scaleIn = 0., double polIn = 9.) { entry.push_back( Particle(id, status, 0, 0, 0, 0, col, acol, px, py, pz, e, m, scaleIn, polIn) ); setEvtPtr(); if (col > maxColTag) maxColTag = col; if (acol > maxColTag) maxColTag = acol; return entry.size() - 1; } int append(int id, int status, int col, int acol, Vec4 p, double m = 0., double scaleIn = 0., double polIn = 9.) {entry.push_back( Particle(id, status, 0, 0, 0, 0, col, acol, p, m, scaleIn, polIn) ); setEvtPtr(); if (col > maxColTag) maxColTag = col; if (acol > maxColTag) maxColTag = acol; return entry.size() - 1; } // Set pointer to the event for a particle, by default latest one. void setEvtPtr(int iSet = -1) {if (iSet < 0) iSet = entry.size() - 1; entry[iSet].setEvtPtr( this);} // Add a copy of an existing particle at the end of the event record. int copy(int iCopy, int newStatus = 0); // List the particles in an event. void list() const; void list(ostream& os) const; void list(bool showScaleAndVertex, bool showMothersAndDaughters = false) const; void list(bool showScaleAndVertex, bool showMothersAndDaughters, ostream& os) const; // Remove last n entries. void popBack(int nRemove = 1) { if (nRemove ==1) entry.pop_back(); else {int newSize = max( 0, size() - nRemove); entry.resize(newSize);} } // Remove entries from iFirst to iLast, including endpoints. void remove(int iFirst, int iLast) { if (iFirst < 0 || iLast >= int(entry.size()) || iLast < iFirst) return; entry.erase( entry.begin() + iFirst, entry.begin() + iLast + 1); } // Undo the decay of a single particle (where daughters well-defined). bool undoDecay(int i); // Restore all ParticleDataEntry* pointers in the Particle vector. // Useful when a persistent copy of the event record is read back in. void restorePtrs() { for (int i = 0; i < size(); ++i) setEvtPtr(i); } // Save or restore the size of the event record (throwing at the end). void saveSize() {savedSize = entry.size();} void restoreSize() {entry.resize(savedSize);} int savedSizeValue() {return savedSize;} // Initialize and access colour tag information. void initColTag(int colTag = 0) {maxColTag = max( colTag,startColTag);} int lastColTag() const {return maxColTag;} int nextColTag() {return ++maxColTag;} // Access scale for which event as a whole is defined. void scale( double scaleIn) {scaleSave = scaleIn;} double scale() const {return scaleSave;} // Need a second scale if two hard interactions in event. void scaleSecond( double scaleSecondIn) {scaleSecondSave = scaleSecondIn;} double scaleSecond() const {return scaleSecondSave;} // Find complete list of daughters and mothers. vector motherList(int i) const; vector daughterList(int i) const; // Convert to HepMC status code conventions. int statusHepMC(int i) const; // Trace the first and last copy of one and the same particle. int iTopCopy(int i) const; int iBotCopy(int i) const; // Trace the first and last copy of a particle, using flavour match. int iTopCopyId(int i) const; int iBotCopyId(int i) const; // Find list of sisters, also tracking up and down identical copies. vector sisterList(int i) const; vector sisterListTopBot(int i, bool widenSearch = true) const; // Check whether two particles have a direct mother-daughter relation. bool isAncestor(int i, int iAncestor) const; // Member functions for rotations and boosts of an event. void rot(double theta, double phi) {for (int i = 0; i < size(); ++i) entry[i].rot(theta, phi);} void bst(double betaX, double betaY, double betaZ) {for (int i = 0; i < size(); ++i) entry[i].bst(betaX, betaY, betaZ);} void bst(double betaX, double betaY, double betaZ, double gamma) {for (int i = 0; i < size(); ++i) entry[i].bst(betaX, betaY, betaZ, gamma);} void bst(const Vec4& vec) {for (int i = 0; i < size(); ++i) entry[i].bst(vec);} void rotbst(const RotBstMatrix& M) {for (int i = 0; i < size(); ++i) entry[i].rotbst(M);} // Clear the list of junctions. void clearJunctions() {junction.resize(0);} // Add a junction to the list, study it or extra input. void appendJunction( int kind, int col0, int col1, int col2) { junction.push_back( Junction( kind, col0, col1, col2) );} void appendJunction(Junction junctionIn) {junction.push_back(junctionIn);} int sizeJunction() const {return junction.size();} bool remainsJunction(int i) const {return junction[i].remains();} void remainsJunction(int i, bool remainsIn) {junction[i].remains(remainsIn);} int kindJunction(int i) const {return junction[i].kind();} int colJunction( int i, int j) const {return junction[i].col(j);} void colJunction( int i, int j, int colIn) {junction[i].col(j, colIn);} int endColJunction( int i, int j) const {return junction[i].endCol(j);} void endColJunction( int i, int j, int endColIn) {junction[i].endCol(j, endColIn);} int statusJunction( int i, int j) const {return junction[i].status(j);} void statusJunction( int i, int j, int statusIn) {junction[i].status(j, statusIn);} Junction& getJunction(int i) {return junction[i];} const Junction& getJunction(int i) const {return junction[i];} void eraseJunction(int i); // Save or restore the size of the junction list (throwing at the end). void saveJunctionSize() {savedJunctionSize = junction.size();} void restoreJunctionSize() {junction.resize(savedJunctionSize);} // List any junctions in the event; for debug mainly. void listJunctions(ostream& os = cout) const; // Operator overloading allows to append one event to an existing one. // Warning: particles should be OK, but some other information unreliable. Event& operator+=(const Event& addEvent); private: // The Particle class needs to access particle data. friend class Particle; // Constants: could only be changed in the code itself. static const int IPERLINE; // Initialization data, normally only set once. int startColTag; // The event: a vector containing all particles (entries). // The explicit use of Pythia8:: qualifier patches a limitation in ROOT. vector entry; // The list of junctions. // The explicit use of Pythia8:: qualifier patches a limitation in ROOT. vector junction; // The maximum colour tag of the event so far. int maxColTag; // Saved entry and junction list sizes, for simple restoration. int savedSize, savedJunctionSize; // The scale of the event; linear quantity in GeV. double scaleSave, scaleSecondSave; // Header specification in event listing (at most 40 characters wide). string headerList; // Pointer to the particle data table. // The //! below is ROOT notation that this member should not be saved. ParticleData* particleDataPtr; //! }; //========================================================================== } // end namespace Pythia8 #endif // end Pythia8_Event_H pythia8-8.1.80.orig/include/Pythia8/SigmaSUSY.h0000644000175000017500000005240212217346232017244 0ustar sunsun// SigmaSUSY.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // Main authors of this file: N. Desai, P. Skands // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for Supersymmetric process differential cross sections. // Contains classes derived from SigmaProcess via Sigma2Process. #ifndef Pythia8_SigmaSUSY_H #define Pythia8_SigmaSUSY_H #include "Pythia8/PhaseSpace.h" #include "Pythia8/PythiaComplex.h" #include "Pythia8/SigmaProcess.h" #include "Pythia8/SusyCouplings.h" namespace Pythia8 { //========================================================================== // An intermediate class for SUSY 2 -> 2 processes with nontrivial decay angles. class Sigma2SUSY : public Sigma2Process { public: // Constructor. Sigma2SUSY() { }; // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); }; //========================================================================== // A derived class for q qbar -> neutralino_i neutralino_j. class Sigma2qqbar2chi0chi0 : public Sigma2SUSY { public: // Constructor. Sigma2qqbar2chi0chi0() {}; // Constructor. Sigma2qqbar2chi0chi0(int id3chiIn, int id4chiIn, int codeIn) { // Save ordering indices and process code id3chi = id3chiIn; id4chi = id4chiIn; codeSave = codeIn; // Construct id codes from ordering indices. id3 = 1000022; if (id3chi == 2) id3 = 1000023; if (id3chi == 3) id3 = 1000025; if (id3chi == 4) id3 = 1000035; if (id3chi == 5) id3 = 1000045; id4 = 1000022; if (id4chi == 2) id4 = 1000023; if (id4chi == 3) id4 = 1000025; if (id4chi == 4) id4 = 1000035; if (id4chi == 5) id4 = 1000045; } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. // virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ff";} virtual int id3Mass() const {return abs(id3);} virtual int id4Mass() const {return abs(id4);} virtual int resonanceA() const {return 23;} virtual bool isSUSY() const {return true;} virtual double getSigma0() const {return sigma0;} protected: // Basic process information int id3chi, id4chi, codeSave; string nameSave; // Values stored for later use double sigma0, ui, uj, ti, tj, openFracPair; complex propZ; CoupSUSY* coupSUSYPtr; }; //========================================================================== // A derived class for q qbar -> neutralino_i chargino_j. class Sigma2qqbar2charchi0 : public Sigma2qqbar2chi0chi0 { public: // Constructor. Sigma2qqbar2charchi0(int id3chiIn, int id4chiIn, int codeIn) { // Save ordering indices and process code id3chi = id3chiIn; id4chi = id4chiIn; codeSave = codeIn; // Construct id codes from ordering indices. id3 = (abs(id3chi) == 2) ? 1000037 : 1000024; if (id3chi < 0) id3 = -id3; id4 = 1000022; if (id4chi == 2) id4 = 1000023; if (id4chi == 3) id4 = 1000025; if (id4chi == 4) id4 = 1000035; if (id4chi == 5) id4 = 1000045; } // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); virtual int resonanceA() const {return 24;} protected : complex propW; }; //========================================================================== // A derived class for q qbar -> chargino+_i chargino-_j. class Sigma2qqbar2charchar : public Sigma2qqbar2chi0chi0 { public: // Constructor. Sigma2qqbar2charchar(int id3chiIn, int id4chiIn, int codeIn) { // Save ordering indices and process code id3chi = id3chiIn; id4chi = id4chiIn; codeSave = codeIn; // Construct id codes from ordering indices. id3 = (abs(id3chi) == 2) ? 1000037 : 1000024; id4 = (abs(id4chi) == 2) ? -1000037 : -1000024; } // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); }; //========================================================================== // A derived class for q g -> neutralino_i squark_j (and cc) class Sigma2qg2chi0squark : public Sigma2Process { public: // Constructor. Sigma2qg2chi0squark() { }; // Constructor. Sigma2qg2chi0squark(int id3chiIn, int id4sqIn, bool isUp, int codeIn) { // Save ordering indices and process code id3chi = id3chiIn; id4sq = id4sqIn; codeSave = codeIn; // Construct id codes from ordering indices. id3 = 1000022; if (id3chi == 2) id3 = 1000023; if (id3chi == 3) id3 = 1000025; if (id3chi == 4) id3 = 1000035; if (id3chi == 5) id3 = 1000045; id4 = 1000001 + (isUp ? 1 : 0); if (id4sq == 2) id4 = 1000003 + (isUp ? 1 : 0); if (id4sq == 3) id4 = 1000005 + (isUp ? 1 : 0); if (id4sq == 4) id4 = 2000001 + (isUp ? 1 : 0); if (id4sq == 5) id4 = 2000003 + (isUp ? 1 : 0); if (id4sq == 6) id4 = 2000005 + (isUp ? 1 : 0); } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return abs(id3);} virtual int id4Mass() const {return abs(id4);} virtual bool isSUSY() const {return true;} protected: // Basic process information int id3chi, id4sq, codeSave; string nameSave; // Values stored for later use double sigma0, ui, uj, ti, tj, openFracPair; //SUSY couplings CoupSUSY* coupSUSYPtr; }; //========================================================================== // A derived class for q g -> chargino_i squark_j (incl cc) class Sigma2qg2charsquark : public Sigma2qg2chi0squark { public: // Constructor. Sigma2qg2charsquark(int id3chiIn, int id4sqIn, bool isUp, int codeIn) { // Save ordering indices and process code id3chi = id3chiIn; id4sq = id4sqIn; codeSave = codeIn; // Construct id codes from ordering indices. id3Sav = 1000024; if (abs(id3chi) == 2) id3Sav = 1000037; if (isUp) id3Sav = -id3Sav; id4Sav = 1000001 + (isUp ? 1 : 0); if (id4sq == 2) id4Sav = 1000003 + (isUp ? 1 : 0); if (id4sq == 3) id4Sav = 1000005 + (isUp ? 1 : 0); if (id4sq == 4) id4Sav = 2000001 + (isUp ? 1 : 0); if (id4sq == 5) id4Sav = 2000003 + (isUp ? 1 : 0); if (id4sq == 6) id4Sav = 2000005 + (isUp ? 1 : 0); // Initial values, can be swapped to charge conjugates event by event. id3 = id3Sav; id4 = id4Sav; } // Initialize process. virtual void initProc(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); private: // Basic process information int id3Sav, id4Sav; }; //========================================================================== // A derived class for q q' -> ~q_i ~q_j class Sigma2qq2squarksquark : public Sigma2Process { public: // Constructor. Sigma2qq2squarksquark() {} // Constructor. Sigma2qq2squarksquark(int id3In, int id4In, int codeIn) { // Save ordering indices and process code id3Sav = id3In; id4Sav = id4In; codeSave = codeIn; // Initial values (flipped for c.c.) id3 = id3Sav; id4 = id4Sav; } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qq";} virtual int id3Mass() const {return abs(id3Sav);} virtual int id4Mass() const {return abs(id4Sav);} virtual bool isSUSY() const {return true;} private: // Basic process information int id3Sav, id4Sav, codeSave, iGen3, iGen4, nNeut; string nameSave; bool isUD; // Storage of mass squares double m2Glu; vector m2Neut, m2Char; // Flavor-independent prefactors. double sigmaChar, sigmaNeut, sigmaGlu; double sigmaCharNeut, sigmaCharGlu, sigmaNeutGlu; double openFracPair; // Point-by-point info double tGlu, uGlu; vector tNeut, uNeut, tChar, uChar; double sumCt, sumCu, sumNt, sumNu, sumGt, sumGu, sumInterference; //SUSY couplings CoupSUSY* coupSUSYPtr; }; //========================================================================== // A derived class for q qbar' -> ~q_i ~q*_j class Sigma2qqbar2squarkantisquark : public Sigma2Process { public: // Constructor. Sigma2qqbar2squarkantisquark() {} // Constructor. Sigma2qqbar2squarkantisquark(int id3In, int id4In, int codeIn) { // Save ordering indices and process code // (always store squark first, antisquark second) id3Sav = abs(id3In); id4Sav = -abs(id4In); codeSave = codeIn; // Initial values id3 = id3Sav; id4 = id4Sav; } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qq";} virtual int id3Mass() const {return abs(id3Sav);} virtual int id4Mass() const {return abs(id4Sav);} virtual bool isSUSY() const {return true;} private: // Basic process information int id3Sav, id4Sav, codeSave, iGen3, iGen4, nNeut; string nameSave; bool isUD, isCC; // Storage of mass squares double m2Glu; vector m2Neut; // Flavor-independent prefactors: EW, strong, and interference double xW; double openFracPair; double sigmaEW, sigmaGlu, sigmaEWG; // Point-by-point info double tGlu, uGlu; vector tNeut, uNeut; complex propZW; double sumColS, sumColT, sumInterference; //SUSY couplings CoupSUSY* coupSUSYPtr; }; //========================================================================== // A derived class for g g -> ~q ~q* class Sigma2gg2squarkantisquark : public Sigma2Process { public: // Constructor. Sigma2gg2squarkantisquark() { } // Constructor. Sigma2gg2squarkantisquark(int id34In, int codeIn) { // Save ordering indices and process code // (always store squark first, antisquark second) id3Sav = abs(id34In); id4Sav = -abs(id34In); codeSave = codeIn; // Initial values id3 = id3Sav; id4 = id4Sav; } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return abs(id3Sav);} virtual int id4Mass() const {return abs(id4Sav);} virtual bool isSUSY() const {return true;} private: // Basic process information int id3Sav, id4Sav, codeSave; string nameSave; double sigma, m2Sq, openFracPair; //SUSY couplings CoupSUSY* coupSUSYPtr; }; //========================================================================== // A derived class for q g -> ~q ~g class Sigma2qg2squarkgluino : public Sigma2Process { public: // Constructor. Sigma2qg2squarkgluino() {} // Constructor. Sigma2qg2squarkgluino(int id3In, int codeIn) { // Save ordering indices and process code id3Sav = abs(id3In); codeSave = codeIn; // Initial values id3 = id3Sav; id4 = 1000021; } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return abs(id3Sav);} virtual int id4Mass() const {return 1000021;} virtual bool isSUSY() const {return true;} private: // Basic process information int id3Sav, codeSave; string nameSave; double sigmaA, sigmaB, comFacHat, m2Glu, m2Sq, openFracPair; //SUSY couplings CoupSUSY* coupSUSYPtr; }; //========================================================================== // A derived class for g g -> gluino gluino. class Sigma2gg2gluinogluino : public Sigma2Process { public: // Constructor. Sigma2gg2gluinogluino() { } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "g g -> gluino gluino";} virtual int code() const {return 1201;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return 1000021;} virtual int id4Mass() const {return 1000021;} virtual bool isSUSY() const {return true;} private: // Values stored for process type and colour flow selection. double sigTS, sigUS, sigTU, sigSum, sigma, openFracPair; //SUSY couplings CoupSUSY* coupSUSYPtr; }; //========================================================================== // A derived class for q qbar -> gluino gluino. class Sigma2qqbar2gluinogluino : public Sigma2Process { public: // Constructor. Sigma2qqbar2gluinogluino() { } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> gluino gluino";} virtual int code() const {return 1202;} virtual string inFlux() const {return "qq";} virtual int id3Mass() const {return 1000021;} virtual int id4Mass() const {return 1000021;} virtual bool isSUSY() const {return true;} private: // Values stored for process type and colour flow selection. double openFracPair, s34Avg, sigS, tHG, uHG, tHG2, uHG2; //SUSY couplings CoupSUSY* coupSUSYPtr; }; //========================================================================== class Sigma1qq2antisquark : public Sigma1Process { public: // Constructor. Sigma1qq2antisquark() {} Sigma1qq2antisquark(int id3In) { idRes = id3In; } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qq";} virtual bool isSUSY() const {return true;} virtual bool isRPV() const {return true;} virtual int resonanceA() const {return idRes;} private: // Values stored for process type and colour flow selection. double mRes, GammaRes, m2Res, sigBW, widthOut; int codeSave, idRes; string nameSave; //SUSY couplings CoupSUSY* coupSUSYPtr; }; //========================================================================== // A derived class for q qbar -> neutralino_i gluino. class Sigma2qqbar2chi0gluino : public Sigma2SUSY { public: // Constructor. Sigma2qqbar2chi0gluino() {}; // Constructor. Sigma2qqbar2chi0gluino(int id4chiIn, int codeIn) { // Save ordering indices and process code id3 = 1000021; id4chi = id4chiIn; codeSave = codeIn; // Construct id codes from ordering indices. id4 = 1000022; if (id4chi == 2) id4 = 1000023; if (id4chi == 3) id4 = 1000025; if (id4chi == 4) id4 = 1000035; if (id4chi == 5) id4 = 1000045; } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. // virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ff";} virtual int id3Mass() const {return abs(id3);} virtual int id4Mass() const {return abs(id4);} virtual int resonanceA() const {return 23;} virtual bool isSUSY() const {return true;} virtual double getSigma0() const {return sigma0;} protected: // Basic process information int id3chi, id4chi, codeSave; string nameSave; // Values stored for later use double sigma0, ui, uj, ti, tj, openFracPair; CoupSUSY* coupSUSYPtr; }; //========================================================================== // A derived class for q qbar -> neutralino_i chargino_j. class Sigma2qqbar2chargluino : public Sigma2qqbar2chi0gluino { public: // Constructor. Sigma2qqbar2chargluino(int id4chiIn, int codeIn) { // Save ordering indices and process code id3 = 1000021; id4chi = id4chiIn; codeSave = codeIn; // Construct id codes from ordering indices. id4 = (abs(id4chi) == 2) ? 1000037 : 1000024; if (id4chi < 0) id4 = -id4; } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); virtual int resonanceA() const {return 24;} protected : complex propW; }; //========================================================================== // A derived class for q qbar' -> ~q_i ~q*_j class Sigma2qqbar2sleptonantislepton : public Sigma2qqbar2squarkantisquark { public: // Constructor. Sigma2qqbar2sleptonantislepton() {} // Constructor. Sigma2qqbar2sleptonantislepton(int id3In, int id4In, int codeIn) { // Save ordering indices and process code // (always store squark first, antisquark second) id3Sav = abs(id3In); id4Sav = -abs(id4In); codeSave = codeIn; // Initial values id3 = id3Sav; id4 = id4Sav; } // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qq";} virtual int id3Mass() const {return abs(id3Sav);} virtual int id4Mass() const {return abs(id4Sav);} virtual bool isSUSY() const {return true;} private: // Basic process information int id3Sav, id4Sav, codeSave, iGen3, iGen4, nNeut; string nameSave; bool isUD; // Storage of mass squares vector m2Neut; // Flavor-independent prefactors: EW, strong, and interference double xW; double openFracPair; double sigmaEW; // Point-by-point info vector tNeut, uNeut; complex propZW; double sumColS, sumColT, sumInterference; //SUSY couplings CoupSUSY* coupSUSYPtr; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaSUSY_H pythia8-8.1.80.orig/include/Pythia8/BoseEinstein.h0000644000175000017500000000524712217346226020057 0ustar sunsun// Bose-Einstein.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the classes to handle Bose-Einstein effects. // BoseEinsteinHadron: simple working container for particle momenta. // BoseEinstein: main class to perform the task. #ifndef Pythia8_BoseEinstein_H #define Pythia8_BoseEinstein_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // The BoseEinsteinHadron class is a simple container for studied hadrons. class BoseEinsteinHadron { public: // Constructors. BoseEinsteinHadron() : id(0), iPos(0), p(0.), pShift(0.), pComp(0.), m2(0.) {} BoseEinsteinHadron(int idIn, int iPosIn, Vec4 pIn, double mIn) : id(idIn), iPos(iPosIn), p(pIn), pShift(0.), pComp(0.) {m2 = mIn*mIn;} // Information on hadron - all public. int id, iPos; Vec4 p, pShift, pComp; double m2; }; //========================================================================== // The BoseEinstein class shifts the momenta of identical particles relative // to each other, to simulate Bose-Einstein effects to some approximation. class BoseEinstein { public: // Constructor. BoseEinstein() {} // Find settings. Precalculate table used to find momentum shifts. bool init(Info* infoPtrIn, Settings& settings, ParticleData& particleData); // Perform Bose-Einstein corrections on an event. bool shiftEvent( Event& event); private: // Constants: could only be changed in the code itself. static const int IDHADRON[9], ITABLE[9], NCOMPSTEP; static const double STEPSIZE, Q2MIN, COMPRELERR, COMPFACMAX; // Initialization data, read from Settings. bool doPion, doKaon, doEta; double lambda, QRef; // Pointer to various information on the generation. Info* infoPtr; // Table of momentum shifts for different hadron species. int nStep[4], nStep3[4], nStored[10]; double QRef2, QRef3, R2Ref, R2Ref2, R2Ref3, mHadron[9], mPair[4], m2Pair[4], deltaQ[4], deltaQ3[4], maxQ[4], maxQ3[4]; double shift[4][200], shift3[4][200]; // Vector of hadrons to study. vector hadronBE; // Calculate shift and (unnormalized) compensation for pair. void shiftPair(int i1, int i2, int iHad); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_BoseEinstein_H pythia8-8.1.80.orig/include/Pythia8/SusyResonanceWidths.h0000644000175000017500000001501112217346232021437 0ustar sunsun// SusyResonanceWidths.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand // Main author of this file: N. Desai // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for resonance properties: dynamical widths etc. // SusyResonanceWidths: base class for all SUSY resonances. #ifndef Pythia8_SusyResonanceWidths_H #define Pythia8_SusyResonanceWidths_H #include "Pythia8/ResonanceWidths.h" #include "Pythia8/SusyCouplings.h" namespace Pythia8 { class ParticleData; //========================================================================== class WidthFunction { public: // Constructor and destructor. WidthFunction() { }; virtual ~WidthFunction() { }; void init( ParticleData* particleDataPtrIn, CoupSUSY* coupSUSYPtrIn); virtual void setInternal(int idResIn, int id1In, int id2In, int id3In, int idIntIn, int) {setInternal2(idResIn, id1In, id2In, id3In, idIntIn);} virtual double function(double m12); virtual double function(double m12, double m23); protected: void setInternal2(int idResIn, int id1In, int id2In, int id3In, int idIntIn); ParticleData* particleDataPtr; CoupSUSY* coupSUSYPtr; int id1,id2,id3; // Variables for 3-body decays double mRes, mInt, gammaInt, m1,m2,m3; int idRes, idInt,iSq,iQ,iX; bool isSqDown; }; //========================================================================== class Psi: public WidthFunction { public: // Destructor. virtual ~Psi() { }; virtual void setInternal(int idResIn, int id1In, int id2In, int id3In, int idIntIn, int); virtual double function(double m12); }; //========================================================================== class Upsilon: public WidthFunction { public: // Destructor. virtual ~Upsilon() { }; virtual void setInternal(int idResIn, int id1In, int id2In, int id3In, int idIntIn, int idInt2); virtual double function(double m12); protected: int iSq2, idInt2; double mInt2, gammaInt2; }; //========================================================================== class Phi: public WidthFunction { public: // Destructor. virtual ~Phi() { }; virtual void setInternal(int idResIn, int id1In, int id2In, int id3In, int idIntIn, int idInt2); virtual double function(double m12sqIn); protected: int iSq2, idInt2; double mInt2, gammaInt2, m12sq; private: double function2(double m23sq); double integrateGauss(double m23min, double m23max, double tol); }; //========================================================================== class SUSYResonanceWidths : public ResonanceWidths{ public: SUSYResonanceWidths() {} // Return particle type int typeNeut(int idPDG); int typeChar(int idPDG); protected: // Virtual methods to handle model-specific (non-SM) part of initialization virtual bool initBSM(); virtual bool allowCalc(); // Gaussian integrator double integrateGauss( WidthFunction* widthFn, double, double, double); // SUSY couplings CoupSUSY* coupSUSYPtr; static const bool DBSUSY; }; //========================================================================== // The ResonanceSquark class handles the Squark resonances. class ResonanceSquark : public SUSYResonanceWidths { public: // Constructor. ResonanceSquark(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool calledFromInit = false); double s2W; }; //========================================================================== // The ResonanceGluino class handles the Gluino resonances. class ResonanceGluino : public SUSYResonanceWidths { public: // Constructor. ResonanceGluino(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool calledFromInit = false); }; //========================================================================== // The ResonanceNeut class handles the Neutralino resonances. class ResonanceNeut : public SUSYResonanceWidths { public: // Constructor. ResonanceNeut(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double kinFac2; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool calledFromInit = false); double s2W; // Functions for 3-body decays Psi psi; Phi phi; Upsilon upsil; }; //========================================================================== // The ResonanceChar class handles the Chargino resonances. class ResonanceChar : public SUSYResonanceWidths { public: // Constructor. ResonanceChar(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double kinFac2; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool calledFromInit = false); double s2W; //Functions for 3-body decays Psi psi; Phi phi; Upsilon upsil; }; //========================================================================== // The ResonanceSlepton class handles the Slepton/Sneutrino resonances. class ResonanceSlepton : public SUSYResonanceWidths { public: // Constructor. ResonanceSlepton(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Calculate width for currently considered channel. virtual void calcWidth(bool calledFromInit = false); double s2W; }; //========================================================================== } // end namespace Pythia8 #endif // end Pythia8_SusyResonanceWidths_H pythia8-8.1.80.orig/include/Pythia8/LHAFortran.h0000644000175000017500000000733612217346227017432 0ustar sunsun// LHAFortran.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for Fortran Les Houches Accord user process information. // LHAupFortran: derived class with the HEPRUP and HEPEUP Fortran info. // You are expected to supply the fillHepRup and fillHepEup methods. #ifndef Pythia8_LHAFortran_H #define Pythia8_LHAFortran_H #include "Pythia8/PythiaStdlib.h" namespace Pythia8 { //========================================================================== // Give access to the HEPRUP and HEPEUP Fortran commonblocks. #ifdef _WIN32 #define heprup_ HEPRUP #define hepeup_ HEPEUP #endif extern "C" { extern struct { int idbmup[2]; double ebmup[2]; int pdfgup[2], pdfsup[2], idwtup, nprup; double xsecup[100], xerrup[100], xmaxup[100]; int lprup[100]; } heprup_; extern struct { int nup, idprup; double xwgtup, scalup, aqedup, aqcdup; int idup[500], istup[500], mothup[500][2], icolup[500][2]; double pup[500][5], vtimup[500],spinup[500]; } hepeup_; } //========================================================================== // A derived class with initialization information from the HEPRUP // Fortran commonblock and event information from the HEPEUP one. class LHAupFortran : public LHAup { public: // Constructor. LHAupFortran() {} // Routine for doing the job of setting initialization info. bool setInit() { // Call the routine that does the job. if (!fillHepRup()) return false; // Store beam and strategy info. setBeamA(heprup_.idbmup[0], heprup_.ebmup[0], heprup_.pdfgup[0], heprup_.pdfsup[0]); setBeamB(heprup_.idbmup[1], heprup_.ebmup[1], heprup_.pdfgup[1], heprup_.pdfsup[1]); setStrategy(heprup_.idwtup); // Store process info. Protect against vanishing cross section. for (int ip = 0; ip < heprup_.nprup; ++ip) { double xsec = max( 1e-10, heprup_.xsecup[ip]); addProcess( heprup_.lprup[ip], xsec, heprup_.xerrup[ip], heprup_.xmaxup[ip] ); } // Store the beam energies to calculate x values later. eBeamA = heprup_.ebmup[0]; eBeamB = heprup_.ebmup[1]; // Done. return true; } // Routine for doing the job of setting info on next event. bool setEvent(int idProcIn = 0, double = -1.) { // In some strategies the type of the next event has been set. hepeup_.idprup = idProcIn; // Call the routine that does the job. if (!fillHepEup()) return false; // Store process info. setProcess(hepeup_.idprup, hepeup_.xwgtup, hepeup_.scalup, hepeup_.aqedup, hepeup_.aqcdup); // Store particle info. for (int ip = 0; ip < hepeup_.nup; ++ip) addParticle(hepeup_.idup[ip], hepeup_.istup[ip], hepeup_.mothup[ip][0], hepeup_.mothup[ip][1], hepeup_.icolup[ip][0], hepeup_.icolup[ip][1], hepeup_.pup[ip][0], hepeup_.pup[ip][1], hepeup_.pup[ip][2], hepeup_.pup[ip][3], hepeup_.pup[ip][4], hepeup_.vtimup[ip], hepeup_.spinup[ip]) ; // Store x values (here E = pup[ip][3]), but note incomplete info. setPdf( hepeup_.idup[0], hepeup_.idup[1], hepeup_.pup[0][3]/eBeamA, hepeup_.pup[1][3]/eBeamB, 0., 0., 0., false); // Done. return true; } private: // Save beam energies to calculate x values. double eBeamA, eBeamB; // User-written routine that does the intialization and fills heprup. bool fillHepRup(); // User-written routine that does the event generation and fills hepeup. bool fillHepEup(); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_LHAFortran_H pythia8-8.1.80.orig/include/Pythia8/SpaceShower.h0000644000175000017500000002141512217346232017703 0ustar sunsun// SpaceShower.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for the spacelike initial-state showers. // SpaceDipoleEnd: radiating dipole end in ISR. // SpaceShower: handles the showering description. #ifndef Pythia8_SpaceShower_H #define Pythia8_SpaceShower_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonSystems.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" #include "Pythia8/StandardModel.h" #include "Pythia8/UserHooks.h" #include "Pythia8/MergingHooks.h" namespace Pythia8 { //========================================================================== // Data on radiating dipole ends, only used inside SpaceShower. class SpaceDipoleEnd { public: // Constructor. SpaceDipoleEnd( int systemIn = 0, int sideIn = 0, int iRadiatorIn = 0, int iRecoilerIn = 0, double pTmaxIn = 0., int colTypeIn = 0, int chgTypeIn = 0, int weakTypeIn = 0, int MEtypeIn = 0, bool normalRecoilIn = true, int weakPolIn = 0) : system(systemIn), side(sideIn), iRadiator(iRadiatorIn), iRecoiler(iRecoilerIn), pTmax(pTmaxIn), colType(colTypeIn), chgType(chgTypeIn), weakType(weakTypeIn), MEtype(MEtypeIn), normalRecoil(normalRecoilIn), weakPol(weakPolIn), nBranch(0), pT2Old(0.), zOld(0.5) { } // Store values for trial emission. void store( int idDaughterIn, int idMotherIn, int idSisterIn, double x1In, double x2In, double m2DipIn, double pT2In, double zIn, double xMoIn, double Q2In, double mSisterIn, double m2SisterIn, double pT2corrIn) {idDaughter = idDaughterIn; idMother = idMotherIn; idSister = idSisterIn; x1 = x1In; x2 = x2In; m2Dip = m2DipIn; pT2 = pT2In; z = zIn; xMo = xMoIn; Q2 = Q2In; mSister = mSisterIn; m2Sister = m2SisterIn; pT2corr = pT2corrIn;} // Basic properties related to evolution and matrix element corrections. int system, side, iRadiator, iRecoiler; double pTmax; int colType, chgType, weakType, MEtype; bool normalRecoil; int weakPol; // Properties specific to current trial emission. int nBranch, idDaughter, idMother, idSister, iFinPol; double x1, x2, m2Dip, pT2, z, xMo, Q2, mSister, m2Sister, pT2corr, pT2Old, zOld, asymPol; } ; //========================================================================== // The SpaceShower class does spacelike showers. class SpaceShower { public: // Constructor. SpaceShower() {beamOffset = 0;} // Destructor. virtual ~SpaceShower() {} // Initialize various pointers. // (Separated from rest of init since not virtual.) void initPtr(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, CoupSM* coupSMPtrIn, PartonSystems* partonSystemsPtrIn, UserHooks* userHooksPtrIn, MergingHooks* mergingHooksPtrIn = 0) { infoPtr = infoPtrIn; settingsPtr = settingsPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; coupSMPtr = coupSMPtrIn; partonSystemsPtr = partonSystemsPtrIn; userHooksPtr = userHooksPtrIn; mergingHooksPtr = mergingHooksPtrIn;} // Initialize generation. Possibility to force re-initialization by hand. virtual void init(BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn); // New beams possible for handling of hard diffraction. (Not virtual.) void reassignBeamPtrs( BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, int beamOffsetIn = 0) {beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; beamOffset = beamOffsetIn;} // Find whether to limit maximum scale of emissions, and whether to dampen. virtual bool limitPTmax( Event& event, double Q2Fac = 0., double Q2Ren = 0.); // Potential enhancement factor of pTmax scale for hardest emission. virtual double enhancePTmax() const {return pTmaxFudge;} // Prepare system for evolution; identify ME. virtual void prepare( int iSys, Event& event, bool limitPTmaxIn = true, double pTfirstTrialIn = 1e9); // Update dipole list after each FSR emission. Currently superfluous. // Usage: update( iSys, event). virtual void update( int , Event& ) {} // Select next pT in downwards evolution. virtual double pTnext( Event& event, double pTbegAll, double pTendAll, int nRadIn = -1, bool isFirstTrial = false); // ME corrections and kinematics that may give failure. virtual bool branch( Event& event); // Tell which system was the last processed one. int system() const {return iSysSel;} // Flag for failure in branch(...) that will force a retry of parton level. bool doRestart() const {return rescatterFail;} // Print dipole list; for debug mainly. virtual void list(ostream& os = cout) const; protected: // Pointer to various information on the generation. Info* infoPtr; // Pointer to the settings database. Settings* settingsPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointer to Standard Model couplings. CoupSM* coupSMPtr; // Pointers to the two incoming beams. Offset their location in event. BeamParticle* beamAPtr; BeamParticle* beamBPtr; int beamOffset; // Pointer to information on subcollision parton locations. PartonSystems* partonSystemsPtr; // Pointer to userHooks object for user interaction with program. UserHooks* userHooksPtr; // Store properties to be returned by methods. bool rescatterFail; int iSysSel; double pTmaxFudge; private: // Constants: could only be changed in the code itself. static const int MAXLOOPTINYPDF; static const double CTHRESHOLD, BTHRESHOLD, EVALPDFSTEP, TINYPDF, TINYKERNELPDF, TINYPT2, HEAVYPT2EVOL, HEAVYXEVOL, EXTRASPACEQ, LAMBDA3MARGIN, PT2MINWARN, LEPTONXMIN, LEPTONXMAX, LEPTONPT2MIN, LEPTONFUDGE; // Initialization data, normally only set once. bool doQCDshower, doQEDshowerByQ, doQEDshowerByL, useSamePTasMPI, doWeakShower, doMEcorrections, doMEafterFirst, doPhiPolAsym, doPhiIntAsym, doRapidityOrder, doSecondHard, canVetoEmission, alphaSuseCMW, singleWeakEmission, dopTdampMass, vetoWeakJets; int pTmaxMatch, pTdampMatch, alphaSorder, alphaSnfmax, alphaEMorder, nQuarkIn, enhanceScreening, weakMode; double pTdampFudge, mc, mb, m2c, m2b, renormMultFac, factorMultFac, alphaSvalue, alphaS2pi, Lambda3flav, Lambda4flav, Lambda5flav, Lambda3flav2, Lambda4flav2, Lambda5flav2, pT0Ref, ecmRef, ecmPow, pTmin, sCM, eCM, pT0, pTminChgQ, pTminChgL, pT20, pT2min, pT2minChgQ, pT2minChgL, pTweakCut, pT2weakCut, pTmaxFudgeMPI, strengthIntAsym, weakEnhancement, pTfirstTrial, extraScaleTerm, mZ, gammaZ, thetaWRat, mW, gammaW, vetoWeakJetspTcut; // alphaStrong and alphaEM calculations. AlphaStrong alphaS; AlphaEM alphaEM; // Some current values. bool sideA, dopTlimit1, dopTlimit2, dopTdamp, hasWeaklyRadiated; int iNow, iRec, idDaughter, nRad, idResFirst, idResSecond; double xDaughter, x1Now, x2Now, m2Dip, m2Rec, pT2damp, pTbegRef; // List of emissions in different sides in different systems. vector nRadA,nRadB; // All dipole ends vector dipEnd; // Pointers to the current and hardest (so far) dipole ends. int iDipNow, iSysNow; SpaceDipoleEnd* dipEndNow; int iDipSel; SpaceDipoleEnd* dipEndSel; // Evolve a QCD dipole end. void pT2nextQCD( double pT2begDip, double pT2endDip); // Evolve a QCD dipole end near heavy quark threshold region. void pT2nearQCDthreshold( BeamParticle& beam, double m2Massive, double m2Threshold, double xMaxAbs, double zMinAbs, double zMaxMassive); // Evolve a QED dipole end. void pT2nextQED( double pT2begDip, double pT2endDip); // Evolve a Weak dipole end. void pT2nextWeak( double pT2begDip, double pT2endDip); // Find class of ME correction. int findMEtype( int iSys, Event& event); // Provide maximum of expected ME weight; for preweighting of evolution. double calcMEmax( int MEtype, int idMother, int idDaughterIn); // Provide actual ME weight for current branching. double calcMEcorr(int MEtype, int idMother, int idDaughterIn, double M2, double z, double Q2, double m2Sister); // Find coefficient of azimuthal asymmetry from gluon polarization. void findAsymPol( Event& event, SpaceDipoleEnd* dip); // Pointer to MergingHooks object for NLO merging. MergingHooks* mergingHooksPtr; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SpaceShower_H pythia8-8.1.80.orig/include/Pythia8/SigmaHiggs.h0000644000175000017500000005554412217346231017513 0ustar sunsun// SigmaHiggs.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // Part of code written by Marc Montull, CERN summer student 2007. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for Higgs process differential cross sections. // Contains classes derived from SigmaProcess via Sigma2Process. #ifndef Pythia8_SigmaHiggs_H #define Pythia8_SigmaHiggs_H #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // A derived class for f fbar -> H0 (SM), H1, H2 or A3 (BSM). class Sigma1ffbar2H : public Sigma1Process { public: // Constructor. Sigma1ffbar2H(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ffbarSame";} virtual int resonanceA() const {return idRes;} private: // An H0, H1, H2 or A3 resonance object provides coupling // and propagator expressions. ParticleDataEntry* HResPtr; double mRes, GammaRes, m2Res, GamMRat, sigBW, widthOut; int higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for g g -> H0 (SM), H1, H2 or A3 (BSM). class Sigma1gg2H : public Sigma1Process { public: // Constructor. Sigma1gg2H(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave ;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gg";} virtual int resonanceA() const {return idRes;} private: // A H0, H1, H2 or A3 resonance object provides coupling // and propagator expressions. ParticleDataEntry* HResPtr; double mRes, GammaRes, m2Res, GamMRat, sigma; int higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for gamma gamma -> H0 (SM Higgs), H1, H2 or A3 (BSM Higgs). class Sigma1gmgm2H : public Sigma1Process { public: // Constructor. Sigma1gmgm2H(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gmgm";} virtual int resonanceA() const {return idRes;} private: // A H0, H1, H2 or A3 resonance object provides coupling // and propagator expressions. ParticleDataEntry* HResPtr; double mRes, GammaRes, m2Res, GamMRat, sigma; int higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for f fbar -> H Z0. // (H can be H0 SM or H1, H2, A3 from BSM). class Sigma2ffbar2HZ : public Sigma2Process { public: // Constructor. Sigma2ffbar2HZ(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ffbarSame";} virtual bool isSChannel() const {return true;} virtual int id3Mass() const {return idRes;} virtual int id4Mass() const {return 23;} virtual int resonanceA() const {return 23;} virtual int gmZmode() const {return 2;} private: // Store Z0 mass and width. double mZ, widZ, mZS, mwZS, thetaWRat, sigma0, openFracPair, coup2Z; int higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for f fbar -> H W+- (Standard Model Higgs). // (H can be H0 SM or H1, H2, A3 from BSM). class Sigma2ffbar2HW : public Sigma2Process { public: // Constructor. Sigma2ffbar2HW(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ffbarChg";} virtual bool isSChannel() const {return true;} virtual int id3Mass() const {return idRes;} virtual int id4Mass() const {return 24;} virtual int resonanceA() const {return 24;} private: // Store W+- mass and width, and couplings. double mW, widW, mWS, mwWS, thetaWRat, sigma0, openFracPairPos, openFracPairNeg, coup2W; int higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for f f' -> H f f' (Z0 Z0 fusion of SM or BSM Higgs). // (H can be H0 SM or H1, H2, A3 from BSM). class Sigma3ff2HfftZZ : public Sigma3Process { public: // Constructor. Sigma3ff2HfftZZ(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ff";} virtual int id3Mass() const {return idRes;} // Instructions for 3-body phase space with t-channel propagators. virtual int idTchan1() const {return 23;} virtual int idTchan2() const {return 23;} virtual double tChanFracPow1() const {return 0.05;} virtual double tChanFracPow2() const {return 0.9;} virtual bool useMirrorWeight() const {return true;} private: // Store standard factors. double mZS, prefac, sigma1, sigma2, openFrac, coup2Z; int higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for f_1 f_2 -> H f_3 f_4 (W+ W- fusion of SM or BSM Higgs). // (H can be H0 SM or H1, H2, A3 from BSM). class Sigma3ff2HfftWW : public Sigma3Process { public: // Constructor. Sigma3ff2HfftWW(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ff";} virtual int id3Mass() const {return idRes;} // Instructions for 3-body phase space with t-channel propagators. virtual int idTchan1() const {return 24;} virtual int idTchan2() const {return 24;} virtual double tChanFracPow1() const {return 0.05;} virtual double tChanFracPow2() const {return 0.9;} virtual bool useMirrorWeight() const {return true;} private: // Store standard prefactor. double mWS, prefac, sigma0, openFrac, coup2W; int higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for g g -> H Q Qbar (Q Qbar fusion of SM or BSM Higgs). // (H can be H0 SM or H1, H2, A3 from BSM). class Sigma3gg2HQQbar : public Sigma3Process { public: // Constructor. Sigma3gg2HQQbar(int idIn, int higgsTypeIn) : idNew(idIn), higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return idRes;} virtual int id4Mass() const {return idNew;} virtual int id5Mass() const {return idNew;} // Instructions for 3-body phase space with t-channel propagators. virtual int idTchan1() const {return idNew;} virtual int idTchan2() const {return idNew;} virtual double tChanFracPow1() const {return 0.4;} virtual double tChanFracPow2() const {return 0.2;} virtual bool useMirrorWeight() const {return false;} private: // Store flavour-specific process information and standard prefactor. double prefac, sigma, openFracTriplet, coup2Q; int idNew, higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for q qbar -> H Q Qbar (Q Qbar fusion of SM or BSM Higgs). // (H can be H0 SM or H1, H2, A3 from BSM). class Sigma3qqbar2HQQbar : public Sigma3Process { public: // Constructor. Sigma3qqbar2HQQbar(int idIn, int higgsTypeIn) : idNew(idIn), higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return idRes;} virtual int id4Mass() const {return idNew;} virtual int id5Mass() const {return idNew;} // Instructions for 3-body phase space with t-channel propagators. virtual int idTchan1() const {return idNew;} virtual int idTchan2() const {return idNew;} virtual double tChanFracPow1() const {return 0.4;} virtual double tChanFracPow2() const {return 0.2;} virtual bool useMirrorWeight() const {return false;} private: // Store flavour-specific process information and standard prefactor. double prefac, sigma, openFracTriplet, coup2Q; int idNew, higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for q g -> H q (SM or BSM Higgs). // (H can be H0 SM or H1, H2, A3 from BSM). class Sigma2qg2Hq : public Sigma2Process { public: // Constructor. Sigma2qg2Hq(int idIn, int higgsTypeIn) : idNew(idIn), higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return idRes;} virtual int id4Mass() const {return idNew;} private: // Store flavour-specific process information and standard prefactor. double m2W, thetaWRat, sigma, openFrac; int idNew, higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for g g -> H0 g (SM or BSM Higgs via heavy top loop). // (H can be H0 SM or H1, H2, A3 from BSM). class Sigma2gg2Hglt : public Sigma2Process { public: // Constructor. Sigma2gg2Hglt(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return idRes;} private: // Store standard prefactor. double widHgg, sigma, openFrac; int higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for q g -> H q (SM or BSM Higgs via heavy top loop). // (H can be H0 SM or H1, H2, A3 from BSM). class Sigma2qg2Hqlt : public Sigma2Process { public: // Constructor. Sigma2qg2Hqlt(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return idRes;} private: // Store standard prefactor. double widHgg, sigma, openFrac; int higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for q qbar -> H g (SM or BSM Higgs via heavy top loop). // (H can be H0 SM or H1, H2, A3 from BSM). class Sigma2qqbar2Hglt : public Sigma2Process { public: // Constructor. Sigma2qqbar2Hglt(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return idRes;} private: // Store standard prefactor. double widHgg, sigma, openFrac; int higgsType, codeSave, idRes; string nameSave; }; //========================================================================== // A derived class for f fbar' -> H+-. class Sigma1ffbar2Hchg : public Sigma1Process { public: // Constructor. Sigma1ffbar2Hchg() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar' -> H+-";} virtual int code() const {return 961;} virtual string inFlux() const {return "ffbarChg";} virtual int resonanceA() const {return 37;} private: // A H0 resonance object provides coupling and propagator expressions. ParticleDataEntry* HResPtr; double mRes, GammaRes, m2Res, GamMRat, m2W, thetaWRat, tan2Beta, sigBW, widthOutPos, widthOutNeg; }; //========================================================================== // A derived class for q g -> H+- q'. class Sigma2qg2Hchgq : public Sigma2Process { public: // Constructor. Sigma2qg2Hchgq(int idIn, int codeIn, string nameIn) : idNew(idIn), codeSave(codeIn), nameSave(nameIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return 37;} virtual int id4Mass() const {return idNew;} private: // Store flavour-specific process information and standard prefactor. int idNew, codeSave, idOld, idUp, idDn; string nameSave; double m2W, thetaWRat, tan2Beta, sigma, openFracPos, openFracNeg; }; //========================================================================== // A derived class for f fbar -> A0(H_3) h0(H_1) or A0(H_3) H0(H_2). class Sigma2ffbar2A3H12 : public Sigma2Process { public: // Constructor. Sigma2ffbar2A3H12(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ffbarSame";} virtual int id3Mass() const {return 36;} virtual int id4Mass() const {return higgs12;} private: // Store flavour-specific process information and standard prefactor. int higgsType, higgs12, codeSave; string nameSave; double coupZA3H12, m2Z, mGammaZ, thetaWRat, openFrac, sigma0; }; //========================================================================== // A derived class for f fbar -> H+- h0(H_1) or H+- H0(H_2). class Sigma2ffbar2HchgH12 : public Sigma2Process { public: // Constructor. Sigma2ffbar2HchgH12(int higgsTypeIn) : higgsType(higgsTypeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ffbarChg";} virtual int id3Mass() const {return 37;} virtual int id4Mass() const {return higgs12;} private: // Store flavour-specific process information and standard prefactor. int higgsType, higgs12, codeSave; string nameSave; double coupWHchgH12, m2W, mGammaW, thetaWRat, openFracPos, openFracNeg, sigma0; }; //========================================================================== // A derived class for f fbar -> H+ H-. class Sigma2ffbar2HposHneg : public Sigma2Process { public: // Constructor. Sigma2ffbar2HposHneg() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar -> H+ H-";} virtual int code() const {return 1085;} virtual string inFlux() const {return "ffbarSame";} virtual int id3Mass() const {return 37;} virtual int id4Mass() const {return 37;} private: // Store flavour-specific process information and standard prefactor. double m2Z, mGammaZ, thetaWRat, eH, lH, openFrac, gamSig, intSig, resSig; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaHiggs_H pythia8-8.1.80.orig/include/Pythia8/HadronLevel.h0000644000175000017500000001061512217346227017667 0ustar sunsun// HadronLevel.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the main class for hadron-level generation. // HadronLevel: handles administration of fragmentation and decay. #ifndef Pythia8_HadronLevel_H #define Pythia8_HadronLevel_H #include "Pythia8/Basics.h" #include "Pythia8/BoseEinstein.h" #include "Pythia8/Event.h" #include "Pythia8/FragmentationFlavZpT.h" #include "Pythia8/FragmentationSystems.h" #include "Pythia8/HadronScatter.h" #include "Pythia8/HiddenValleyFragmentation.h" #include "Pythia8/Info.h" #include "Pythia8/MiniStringFragmentation.h" #include "Pythia8/ParticleData.h" #include "Pythia8/ParticleDecays.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/RHadrons.h" #include "Pythia8/Settings.h" #include "Pythia8/StringFragmentation.h" #include "Pythia8/TimeShower.h" namespace Pythia8 { //========================================================================== // The HadronLevel class contains the top-level routines to generate // the transition from the partonic to the hadronic stage of an event. class HadronLevel { public: // Constructor. HadronLevel() {} // Initialize HadronLevel classes as required. bool init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, Couplings* couplingsPtrIn, TimeShower* timesDecPtr, RHadrons* rHadronsPtrIn, DecayHandler* decayHandlePtr, vector handledParticles); // Get pointer to StringFlav instance (needed by BeamParticle). StringFlav* getStringFlavPtr() {return &flavSel;} // Generate the next event. bool next(Event& event); // Special routine to allow more decays if on/off switches changed. bool moreDecays(Event& event); private: // Constants: could only be changed in the code itself. static const int NTRYJNREST; static const double JJSTRINGM2MAX, JJSTRINGM2FRAC, CONVJNREST, MTHAD; // Initialization data, read from Settings. bool doHadronize, doDecay, doBoseEinstein, allowRH; double mStringMin, eNormJunction, widthSepBE; // Settings for hadron scattering --rjc bool doHadronScatter, hsAfterDecay; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to Standard Model couplings. Couplings* couplingsPtr; // Configuration of colour-singlet systems. ColConfig colConfig; // Colour information. vector iColEnd, iAcolEnd, iColAndAcol, iParton, iPartonJun, iPartonAntiJun, iJunLegA, iJunLegB, iJunLegC, iAntiLegA, iAntiLegB, iAntiLegC, iGluLeg; vector m2Pair; // The generator class for normal string fragmentation. StringFragmentation stringFrag; // The generator class for special low-mass string fragmentation. MiniStringFragmentation ministringFrag; // The generator class for normal decays. ParticleDecays decays; // The generator class for hadron scattering --rjc HadronScatter hadronScatter; // The generator class for Bose-Einstein effects. BoseEinstein boseEinstein; // Classes for flavour, pT and z generation. StringFlav flavSel; StringPT pTSel; StringZ zSel; // The RHadrons class is used to fragment off and decay R-hadrons. RHadrons* rHadronsPtr; // Special class for Hidden-Valley hadronization. Not always used. HiddenValleyFragmentation hiddenvalleyFrag; bool useHiddenValley; // Special case: colour-octet onium decays, to be done initially. bool decayOctetOnia(Event& event); // Trace colour flow in the event to form colour singlet subsystems. bool findSinglets(Event& event); // Trace a colour line, from a colour, from an anticolour, or in loop. bool traceFromCol(int indxCol, Event& event, int iJun = -1, int iCol = -1); bool traceFromAcol(int indxCol, Event& event, int iJun = -1, int iCol = -1); bool traceInLoop(int indxCol, int indxAcol, Event& event); // Split junction-antijunction system into two, or simplify other way. bool splitJunctionPair(Event& event); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_HadronLevel_H pythia8-8.1.80.orig/include/Pythia8/LHAPDFInterface.h0000644000175000017500000000462412217346227020246 0ustar sunsun// LHAPDFInterface.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for the LHAPDF f77 external linkage to C++. // All required code is contained here, i.e. there is no matching .cc file. #ifndef Pythia8_LHAPDFInterface_H #define Pythia8_LHAPDFInterface_H namespace Pythia8 { //========================================================================== // Declare the LHAPDF f77 subroutines that are needed. extern "C" { extern void initpdfsetm_(int&, const char*, int); extern void initpdfsetbynamem_(int&, const char*, int); extern void initpdfm_(int&, int&); extern void evolvepdfm_(int&, double&, double&, double*); extern void evolvepdfphotonm_(int&, double&, double&, double*, double&); extern void setlhaparm_(const char*, int); } //========================================================================== // Interfaces to the above routines, to make the C++ calls similar to f77. class LHAPDFInterface { public: // Initialize set with full pathname, allowing multiple sets. static void initPDFsetM( int& nSet, string name) { const char* cName = name.c_str(); int lenName = name.length(); initpdfsetm_( nSet, cName, lenName); } // Initialize set with simple name, allowing multiple sets. static void initPDFsetByNameM( int& nSet, string name) { const char* cName = name.c_str(); int lenName = name.length(); initpdfsetbynamem_( nSet, cName, lenName); } // Initialize member of set. static void initPDFM(int& nSet, int member) { initpdfm_(nSet, member); } // Evaluate x f_i(x, Q). static void evolvePDFM( int& nSet, double x, double Q, double* xfArray) { evolvepdfm_( nSet, x, Q, xfArray); } // Evaluate x f_i(x, Q) including photon static void evolvePDFPHOTONM( int& nSet, double x, double Q, double* xfArray, double& xPhoton) { evolvepdfphotonm_( nSet, x, Q, xfArray, xPhoton); } // Extrapolate PDF set beyond boundaries, or freeze them there. static void setPDFparm(string name) { const char* cName = name.c_str(); int lenName = name.length(); setlhaparm_( cName, lenName); } }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_LHAPDFInterface_H pythia8-8.1.80.orig/include/Pythia8/HelicityMatrixElements.h0000644000175000017500000004051512217346227022122 0ustar sunsun// HelicityMatrixElements.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Philip Ilten, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for a number of physics classes used in tau decays. #ifndef Pythia8_HelicityMatrixElements_H #define Pythia8_HelicityMatrixElements_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/HelicityBasics.h" #include "Pythia8/PythiaComplex.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/StandardModel.h" namespace Pythia8 { //========================================================================== // The helicity matrix element class. class HelicityMatrixElement { public: // Constructor and destructor. HelicityMatrixElement() {}; virtual ~HelicityMatrixElement() {}; // Initialize the physics matrices and pointers. virtual void initPointers(ParticleData*, Couplings*); // Initialize the channel. virtual HelicityMatrixElement* initChannel(vector&); // Calculate the matrix element weight for a decay. virtual double decayWeight(vector&); // Calculate the maximum matrix element decay weight. virtual double decayWeightMax(vector&) {return DECAYWEIGHTMAX;} // Calculate the helicity matrix element. virtual complex calculateME(vector){return complex(0,0);} // Calculate the decay matrix for a particle. virtual void calculateD(vector&); // Calculate the density matrix for a particle. virtual void calculateRho(unsigned int, vector&); // Set a fermion line. void setFermionLine(int, HelicityParticle&, HelicityParticle&); // Calculate Breit-Wigner's with running widths and fixed. virtual complex breitWigner(double s, double M, double G); virtual complex sBreitWigner(double m0, double m1, double s, double M, double G); virtual complex pBreitWigner(double m0, double m1, double s, double M, double G); virtual complex dBreitWigner(double m0, double m1, double s, double M, double G); protected: // Maximum decay weight. WARNING: hardcoded constant. double DECAYWEIGHTMAX; // Physics matrices. vector< GammaMatrix > gamma; // Particle map vector. vector< int > pMap; // Particle ID vector. vector< int > pID; // Particle mass vector. vector< double > pM; // Wave functions. vector< vector< Wave4 > > u; // Initialize the constants for the matrix element (called by initChannel). virtual void initConstants() {}; // Initialize the wave functions (called by decayWeight and calculateRho/D). virtual void initWaves(vector&) {}; // Pointer to particle data. ParticleData* particleDataPtr; // Pointer to Standard Model constants. Couplings* couplingsPtr; private: // Recursive sub-method to calculate the density matrix for a particle. void calculateRho(unsigned int, vector&, vector&, vector&, unsigned int); // Recursive sub-method to calculate the decay matrix for a particle. void calculateD(vector&, vector&, vector&, unsigned int); // Recursive sub-method to calculate the matrix element weight for a decay. void decayWeight(vector&, vector&, vector&, complex&, unsigned int); // Calculate the product of the decay matrices for a hard process. complex calculateProductD(unsigned int, unsigned int, vector&, vector&, vector&); // Calculate the product of the decay matrices for a decay process. complex calculateProductD(vector&, vector&, vector&); }; //========================================================================== // Helicity matrix element for the hard process of two fermions -> W -> // two fermions. class HMETwoFermions2W2TwoFermions : public HelicityMatrixElement { public: void initWaves(vector&); complex calculateME(vector); }; //========================================================================== // Helicity matrix element for the hard process of two fermions -> // photon -> two fermions. class HMETwoFermions2Gamma2TwoFermions : public HelicityMatrixElement { public: void initWaves(vector&); complex calculateME(vector); private: // Fermion line charge and interaction energy. double p0Q, p2Q, s; }; //========================================================================== // Helicity matrix element for the hard process of two fermions -> // Z -> two fermions. class HMETwoFermions2Z2TwoFermions : public HelicityMatrixElement { public: void initConstants(); void initWaves(vector&); complex calculateME(vector); private: // Vector and axial couplings. double p0CA, p2CA, p0CV, p2CV; // Weinberg angle, Z width (on-shell), Z mass (on-shell), and s. double cos2W, sin2W, zG, zM, s; // Bool whether the incoming fermions are oriented with the z-axis. bool zaxis; }; //========================================================================== // Helicity matrix element for the hard process of two fermions -> // photon/Z -> two fermions with full interference. // In general the initPointers and initChannel methods should not need to be // redeclared, but in this case each matrix element needs to be initialized. class HMETwoFermions2GammaZ2TwoFermions : public HelicityMatrixElement { public: HelicityMatrixElement* initChannel(vector&); void initPointers(ParticleData*, Couplings*); void initWaves(vector&); complex calculateME(vector); private: HMETwoFermions2Z2TwoFermions zHME; HMETwoFermions2Gamma2TwoFermions gHME; }; //========================================================================== // Helicity matrix element for the hard process of Z -> two fermions. class HMEZ2TwoFermions : public HelicityMatrixElement { public: void initConstants(); void initWaves(vector&); complex calculateME(vector); private: // Vector and axial couplings. double p2CA, p2CV; }; //========================================================================== // Helicity matrix element for the decay of a CP even Higgs -> two fermions. // Because the Higgs is spin zero the Higgs production mechanism is not // needed for calculating helicity density matrices. class HMEHiggsEven2TwoFermions : public HelicityMatrixElement { public: void initWaves(vector&); complex calculateME(vector); private: // Coupling constants of the fermions with the Higgs. double p2CA, p2CV; }; //========================================================================== // Helicity matrix element for the decay of a CP odd Higgs -> two fermions. class HMEHiggsOdd2TwoFermions : public HelicityMatrixElement { public: void initWaves(vector&); complex calculateME(vector); private: // Coupling constants of the fermions with the Higgs. double p2CA, p2CV; }; //========================================================================== // Helicity matrix element for the decay of a charged Higgs -> two fermions. class HMEHiggsCharged2TwoFermions : public HelicityMatrixElement { public: void initWaves(vector&); complex calculateME(vector); private: // Coupling constants of the fermions with the Higgs. double p2CA, p2CV; }; //========================================================================== // Helicity matrix element which provides an unpolarized on-diagonal helicity // density matrix. Used for unknown hard processes. class HMEUnpolarized : public HelicityMatrixElement { public: void calculateRho(unsigned int, vector&); }; //========================================================================== // Base class for all tau decay helicity matrix elements. class HMETauDecay : public HelicityMatrixElement { public: virtual void initWaves(vector&); virtual complex calculateME(vector); virtual double decayWeightMax(vector&); protected: virtual void initHadronicCurrent(vector&) {}; virtual void calculateResonanceWeights(vector&, vector&, vector&); }; //========================================================================== // Helicity matrix element for a tau decaying into a single scalar meson. class HMETau2Meson : public HMETauDecay { public: void initConstants(); void initHadronicCurrent(vector&); }; //========================================================================== // Helicity matrix element for a tau decaying into two leptons. class HMETau2TwoLeptons : public HMETauDecay { public: void initConstants(); void initWaves(vector&); complex calculateME(vector); }; //========================================================================== // Helicity matrix element for a tau decaying into two mesons through a // vector meson resonance. class HMETau2TwoMesonsViaVector : public HMETauDecay { public: void initConstants(); void initHadronicCurrent(vector&); private: // Resonance masses, widths, and weights. vector vecM, vecG, vecP, vecA; vector vecW; }; //========================================================================== // Helicity matrix element for a tau decay into two mesons through a vector // or scalar meson resonance. class HMETau2TwoMesonsViaVectorScalar : public HMETauDecay { public: void initConstants(); void initHadronicCurrent(vector&); private: // Coupling to vector and scalar resonances. double scaC, vecC; // Resonance masses, widths, and weights. vector scaM, scaG, scaP, scaA, vecM, vecG, vecP, vecA; vector scaW, vecW; }; //========================================================================== // Helicity matrix element for a tau decay into three mesons (base class). class HMETau2ThreeMesons : public HMETauDecay { public: void initConstants(); void initHadronicCurrent(vector&); protected: // Decay mode of the tau. enum Mode{Pi0Pi0Pim, PimPimPip, Pi0PimK0b, PimPipKm, Pi0PimEta, PimKmKp, Pi0K0Km, KlPimKs, Pi0Pi0Km, KlKlPim, PimKsKs, PimK0bK0, Uknown}; Mode mode; // Initialize decay mode and resonance constants (called by initConstants). virtual void initMode(); virtual void initResonances() {;} // Initialize the momenta. virtual void initMomenta(vector&); // Center of mass energies and momenta. double s1, s2, s3, s4; Wave4 q, q2, q3, q4; // Stored a1 Breit-Wigner (for speed). complex a1BW; // Form factors. virtual complex F1() {return complex(0, 0);} virtual complex F2() {return complex(0, 0);} virtual complex F3() {return complex(0, 0);} virtual complex F4() {return complex(0, 0);} // Phase space and Breit-Wigner for the a1. virtual double a1PhaseSpace(double); virtual complex a1BreitWigner(double); // Sum running p and fixed width Breit-Wigner resonances. complex T(double m0, double m1, double s, vector& M, vector& G, vector& W); complex T(double s, vector& M, vector& G, vector& W); }; //========================================================================== // Helicity matrix element for a tau decay into three pions. class HMETau2ThreePions : public HMETau2ThreeMesons { private: void initResonances(); // Resonance masses, widths, and weights. vector rhoM, rhoG, rhoPp, rhoAp, rhoPd, rhoAd; double f0M, f0G, f0P, f0A, f2M, f2G, f2P, f2A; double sigM, sigG, sigP, sigA; vector rhoWp, rhoWd; complex f0W, f2W, sigW; // Form factors. complex F1(); complex F2(); complex F3(); // Running width and Breit-Wigner for the a1. double a1PhaseSpace(double); complex a1BreitWigner(double); }; //========================================================================== // Helicity matrix element for a tau decay into three mesons with kaons. class HMETau2ThreeMesonsWithKaons : public HMETau2ThreeMesons { private: void initResonances(); // Resonance masses, widths, and weights. vector rhoMa, rhoGa, rhoWa, rhoMv, rhoGv, rhoWv; vector kstarMa, kstarGa, kstarWa, kstarMv, kstarGv, kstarWv; vector k1Ma, k1Ga, k1Wa, k1Mb, k1Gb, k1Wb; vector omegaM, omegaG, omegaW; double kM, piM, piW; // Form factors. complex F1(); complex F2(); complex F4(); }; //========================================================================== // Helicity matrix element for a tau decay into generic three mesons. class HMETau2ThreeMesonsGeneric : public HMETau2ThreeMesons { private: void initResonances(); // Resonance masses, widths, and weights. vector rhoMa, rhoGa, rhoWa, rhoMv, rhoGv, rhoWv; vector kstarM, kstarG, kstarW, k1M, k1G, k1W; double kM, piM, piW; // Form factors. complex F1(); complex F2(); complex F4(); }; //========================================================================== // Helicity matrix element for a tau decay into two pions and a photon. class HMETau2TwoPionsGamma : public HMETauDecay { public: void initConstants(); void initWaves(vector&); complex calculateME(vector); protected: // Resonance masses, widths, and weights. vector rhoM, rhoG, rhoW, omegaM, omegaG, omegaW; double piM; // Form factor. complex F(double s, vector M, vector G, vector W); }; //========================================================================== // Helicity matrix element for a tau decay into four pions. class HMETau2FourPions : public HMETauDecay { public: void initConstants(); void initHadronicCurrent(vector& p); private: // G-function form factors (fits). double G(int i, double s); // T-vector functions. Wave4 t1(Wave4&, Wave4&, Wave4&, Wave4&, Wave4&); Wave4 t2(Wave4&, Wave4&, Wave4&, Wave4&, Wave4&); Wave4 t3(Wave4&, Wave4&, Wave4&, Wave4&, Wave4&); // Breit-Wigner denominators for the intermediate mesons. complex a1D(double s); complex rhoD(double s); complex sigD(double s); complex omeD(double s); // Form factors needed for the a1, rho, and omega. double a1FormFactor(double s); double rhoFormFactor1(double s); double rhoFormFactor2(double s); double omeFormFactor(double s); // Masses and widths of the intermediate mesons. double a1M, a1G, rhoM, rhoG, sigM, sigG, omeM, omeG; // Masses for the pions (charged and neutral). double picM, pinM; // Amplitude, phases, and weights for mixing. double sigA, sigP, omeA, omeP; complex sigW, omeW; // Cut-off for a1 form factor. double lambda2; }; //========================================================================== // Helicity matrix element for a tau decaying into five pions. class HMETau2FivePions : public HMETauDecay { public: void initConstants(); void initHadronicCurrent(vector&); private: // Hadronic currents. Wave4 Ja(Wave4 &q, Wave4 &q1, Wave4 &q2, Wave4 &q3, Wave4 &q4, Wave4 &q5); Wave4 Jb(Wave4 &q, Wave4 &q1, Wave4 &q2, Wave4 &q3, Wave4 &q4, Wave4 &q5); // Simplified s-wave Breit-Wigner assuming massless products. complex breitWigner(double s, double M, double G); // Masses and widths of intermediates. double a1M, a1G, rhoM, rhoG, omegaM, omegaG, omegaW, sigmaM, sigmaG, sigmaW; }; //========================================================================== // Helicity matrix element for a tau decay into flat phase space. class HMETau2PhaseSpace : public HMETauDecay { public: void initWaves(vector&) {}; complex calculateME(vector) {return 1;} void calculateD(vector&) {}; void calculateRho(unsigned int, vector&) {}; double decayWeight(vector&) {return 1.0;} double decayWeightMax(vector&) {return 1.0;} }; //========================================================================== } // end namespace Pythia8 #endif // end Pythia8_HelicityMatrixElements_H pythia8-8.1.80.orig/include/Pythia8/BeamRemnants.h0000644000175000017500000000562612217346226020045 0ustar sunsun// BeamRemnants.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for beam-remnants handling. // BeamRemnants: matches the remnants between the two beams. #ifndef Pythia8_BeamRemnants_H #define Pythia8_BeamRemnants_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Event.h" #include "Pythia8/FragmentationFlavZpT.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonDistributions.h" #include "Pythia8/PartonSystems.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // This class matches the kinematics of the hard-scattering subsystems // (with primordial kT added) to that of the two beam remnants. class BeamRemnants { public: // Constructor. BeamRemnants() : iDS(0) { } // Initialization. bool init( Info* infoPtrIn, Settings& settings, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, PartonSystems* partonSystemsPtrIn); // New beams possible for handling of hard diffraction. void reassignBeamPtrs( BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, int iDSin) {beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; iDS = iDSin;} // Select the flavours/kinematics/colours of the two beam remnants. bool add( Event& event); private: // Constants: could only be changed in the code itself. static const bool ALLOWCOLOURTWICE, CORRECTMISMATCH; static const int NTRYCOLMATCH, NTRYKINMATCH; // Initialization data, read from Settings. bool doPrimordialKT, allowRescatter, doRescatterRestoreY, doReconnect; double primordialKTsoft, primordialKThard, primordialKTremnant, halfScaleForKT, halfMassForKT, reconnectRange, pT0Ref, ecmRef, ecmPow; // Information set for events. int nSys, oldSize, iDS; double eCM, sCM, pT0, pT20Rec; // Colour collapses (when one colour is mapped onto another). vector colFrom, colTo; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to the two incoming beams. BeamParticle* beamAPtr; BeamParticle* beamBPtr; // Pointer to information on subcollision parton locations. PartonSystems* partonSystemsPtr; // Do the kinematics of the collision subsystems and two beam remnants. bool setKinematics( Event& event); // Allow colour reconnections. bool reconnectColours( Event& event); // Check that colours are consistent. bool checkColours( Event& event); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_BeamRemnants_H pythia8-8.1.80.orig/include/Pythia8/StringFragmentation.h0000644000175000017500000001314412217346232021445 0ustar sunsun// StringFragmentation.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the classes for string fragmentation. // StringEnd: keeps track of the fragmentation step. // StringFragmentation: is the top-level class. #ifndef Pythia8_StringFragmentation_H #define Pythia8_StringFragmentation_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/FragmentationFlavZpT.h" #include "Pythia8/FragmentationSystems.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // The StringEnd class contains the information related to // one of the current endpoints of the string system. // Only to be used inside StringFragmentation, so no private members. class StringEnd { public: // Constructor. StringEnd() {} // Save pointers. void init( ParticleData* particleDataPtrIn, StringFlav* flavSelPtrIn, StringPT* pTSelPtrIn, StringZ* zSelPtrIn) { particleDataPtr = particleDataPtrIn; flavSelPtr = flavSelPtrIn; pTSelPtr = pTSelPtrIn; zSelPtr = zSelPtrIn;} // Set up initial endpoint values from input. void setUp(bool fromPosIn, int iEndIn, int idOldIn, int iMaxIn, double pxIn, double pyIn, double GammaIn, double xPosIn, double xNegIn); // Fragment off one hadron from the string system, in flavour and pT. void newHadron(); // Fragment off one hadron from the string system, in momentum space, // by taking steps either from positive or from negative end. Vec4 kinematicsHadron(StringSystem& system); // Update string end information after a hadron has been removed. void update(); // Constants: could only be changed in the code itself. static const double TINY, PT2SAME; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointers to classes for flavour, pT and z generation. StringFlav* flavSelPtr; StringPT* pTSelPtr; StringZ* zSelPtr; // Data members. bool fromPos; int iEnd, iMax, idHad, iPosOld, iNegOld, iPosNew, iNegNew; double pxOld, pyOld, pxNew, pyNew, pxHad, pyHad, mHad, mT2Had, zHad, GammaOld, GammaNew, xPosOld, xPosNew, xPosHad, xNegOld, xNegNew, xNegHad; FlavContainer flavOld, flavNew; Vec4 pHad, pSoFar; }; //========================================================================== // The StringFragmentation class contains the top-level routines // to fragment a colour singlet partonic system. class StringFragmentation { public: // Constructor. StringFragmentation() {} // Initialize and save pointers. void init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, StringFlav* flavSelPtrIn, StringPT* pTSelPtrIn, StringZ* zSelPtrIn); // Do the fragmentation: driver routine. bool fragment( int iSub, ColConfig& colConfig, Event& event); // Find the boost matrix to the rest frame of a junction. RotBstMatrix junctionRestFrame(Vec4& p0, Vec4& p1, Vec4& p2); private: // Constants: could only be changed in the code itself. static const int NTRYFLAV, NTRYJOIN, NSTOPMASS, NTRYJNREST, NTRYJNMATCH, NTRYJRFEQ; static const double FACSTOPMASS, CLOSEDM2MAX, CLOSEDM2FRAC, EXPMAX, MATCHPOSNEG, EJNWEIGHTMAX, CONVJNREST, M2MAXJRF, EEXTRAJNMATCH, MDIQUARKMIN, CONVJRFEQ; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to classes for flavour, pT and z generation. StringFlav* flavSelPtr; StringPT* pTSelPtr; StringZ* zSelPtr; // Initialization data, read from Settings. double stopMass, stopNewFlav, stopSmear, eNormJunction, eBothLeftJunction, eMaxLeftJunction, eMinLeftJunction, mJoin, bLund; // Data members. bool hasJunction, isClosed; int iPos, iNeg; double w2Rem, stopMassNow; Vec4 pSum, pRem, pJunctionHadrons; // List of partons in string system. vector iParton; // Temporary event record for the produced particles. Event hadrons; // Information on the system of string regions. StringSystem system, systemMin, systemMid; // Information on the two current endpoints of the fragmenting system. StringEnd posEnd, negEnd; // Find region where to put first string break for closed gluon loop. vector findFirstRegion(vector& iPartonIn, Event& event); // Set flavours and momentum position for initial string endpoints. void setStartEnds(int idPos, int idNeg, StringSystem systemNow); // Check remaining energy-momentum whether it is OK to continue. bool energyUsedUp(bool fromPos); // Produce the final two partons to complete the system. bool finalTwo(bool fromPos); // Construct a special joining region for the final two hadrons. StringRegion finalRegion(); // Store the hadrons in the normal event record, ordered from one end. void store(Event& event); // Fragment off two of the string legs in to a junction. bool fragmentToJunction(Event& event); // Join extra nearby partons when stuck. int extraJoin(double facExtra, Event& event); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_StringFragmentation_H pythia8-8.1.80.orig/include/Pythia8/SigmaTotal.h0000644000175000017500000001130212217346232017516 0ustar sunsun// SigmaTotal.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the class for cross section parametrizations. // SigmaTotal: total and partial cross section in hadron-hadron collisions. #ifndef Pythia8_SigmaTotal_H #define Pythia8_SigmaTotal_H #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // The SigmaTotal class contains parametrizations of total, elastic and // diffractive cross sections, and of the respective slope parameter. class SigmaTotal { public: // Constructor. SigmaTotal() : isCalc(false) {}; // Store pointers and initialize data members. void init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn ); // Calculate, or recalculate for new beams or new energy. bool calc(int idA, int idB, double eCM); // Confirm that initialization worked. bool hasSigmaTot() const {return isCalc;} // Read out total and partial cross sections. double sigmaTot() const {return sigTot;} double sigmaEl() const {return sigEl;} double sigmaXB() const {return sigXB;} double sigmaAX() const {return sigAX;} double sigmaXX() const {return sigXX;} double sigmaAXB() const {return sigAXB;} double sigmaND() const {return sigND;} // Calculate cross sections in MBR model. bool calcMBRxsecs(int idA, int idB, double eCM); // Get maximum of xi,dy distribution in MBR model (for event generation). double ddpMax() const {return ddpmax;} double sdpMax() const {return sdpmax;} double dpepMax() const {return dpepmax;} // Read out slope b in exp(b*t) dependence. double bSlopeEl() const {return bEl;} double bSlopeXB(double sX) const { return 2.*bB + alP2 * log(s/sX) ;} double bSlopeAX(double sX) const { return 2.*bA + alP2 * log(s/sX) ;} double bSlopeXX(double sX1, double sX2) const { return alP2 * log( exp(4.) + s * s0 / (sX1 * sX2) ) ;} // Read out parameters of diffractive mass spectra. double mMinXB() const {return mMinXBsave;} double mMinAX() const {return mMinAXsave;} double mMinAXB() const {return mMinAXBsave;} double cRes() const {return CRES;} double mResXB() const {return mResXBsave;} double mResAX() const {return mResAXsave;} double sProton() const {return SPROTON;} // Read out parameters of trial t spectra. double bMinSlopeXB() const { return max(2., 2. * bB);} double bMinSlopeAX() const { return max(2., 2. * bA);} double bMinSlopeXX() const { return alP2 * 4.;} private: // Decide whether default or MBR diffractive cross sections. int PomFlux; // Constants: could only be changed in the code itself. static const int IHADATABLE[], IHADBTABLE[], ISDTABLE[], IDDTABLE[]; static const double MMIN, EPSILON, ETA, X[], Y[], BETA0[], BHAD[], ALPHAPRIME, CONVERTEL, CONVERTSD, CONVERTDD, MMIN0, CRES, MRES0, CSD[10][8], CDD[10][9], SPROTON; // Integration of MBR cross sections and form factor approximation. static const int NINTEG, NINTEG2; static const double HBARC2, FFA1, FFA2,FFB1, FFB2; // Initialization data, normally only set once. bool isCalc, setTotal, zeroAXB, doDampen, setElastic; double sigAXB2TeV, sigTotOwn, sigElOwn, sigXBOwn, sigAXOwn, sigXXOwn, sigAXBOwn, maxXBOwn, maxAXOwn, maxXXOwn, maxAXBOwn, bSlope, rho, lambda, tAbsMin, alphaEM0, sigmaPomP, mPomP, pPomP; // Parameters of MBR model. double MBReps, MBRalpha, MBRbeta0, MBRsigma0, m2min, dyminSDflux, dyminDDflux, dyminCDflux, dyminSD, dyminDD, dyminCD, dyminSigSD, dyminSigDD, dyminSigCD, sdpmax, ddpmax, dpepmax; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Store values found by calc. double sigTot, sigEl, sigXB, sigAX, sigXX, sigAXB, sigND, bEl, s, bA, bB, alP2, s0, mMinXBsave, mMinAXsave, mMinAXBsave, mResXBsave, mResAXsave; // The error function erf(x) should normally be in your math library, // but if not uncomment this simple parametrization by Sergei Winitzki. //double erf(double x) { double x2 = x * x; double kx2 = 0.147 * x2; // double tmp = sqrt(1. - exp(-x2 * (4./M_PI + kx2) / (1. + kx2))); // return ((x >= 0.) ? tmp : -tmp); } }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaTotal_H pythia8-8.1.80.orig/include/Pythia8/SigmaCompositeness.h0000644000175000017500000002130612217346231021272 0ustar sunsun// SigmaCompositeness.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for compositiness-process differential cross sections. // Contains classes derived from SigmaProcess via Sigma(1/2)Process. #ifndef Pythia8_SigmaCompositeness_H #define Pythia8_SigmaCompositeness_H #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // A derived class for q g -> q^* (excited quark state). class Sigma1qg2qStar : public Sigma1Process { public: // Constructor. Sigma1qg2qStar(int idqIn) : idq(idqIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for q* decay angles (else inactive). virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qg";} virtual int resonanceA() const {return idRes;} private: // Parameters set at initialization or for current kinematics. int idq, idRes, codeSave; string nameSave; double mRes, GammaRes, m2Res, GamMRat, Lambda, coupFcol, widthIn, sigBW; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* qStarPtr; }; //========================================================================== // A derived class for l gamma -> l^* (excited lepton state). class Sigma1lgm2lStar : public Sigma1Process { public: // Constructor. Sigma1lgm2lStar(int idlIn) : idl(idlIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for l* decay angles (else inactive). virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "fgm";} virtual int resonanceA() const {return idRes;} private: // Parameters set at initialization or for current kinematics. int idl, idRes, codeSave; string nameSave; double mRes, GammaRes, m2Res, GamMRat, Lambda, coupChg, widthIn, sigBW; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* qStarPtr; }; //========================================================================== // A derived class for q q' -> q^* q' (excited quark state). class Sigma2qq2qStarq : public Sigma2Process { public: // Constructor. Sigma2qq2qStarq(int idqIn) : idq(idqIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for q* decay angles (else inactive). virtual double weightDecay(Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qq";} virtual int id3Mass() const {return idRes;} private: // Parameters set at initialization or for current kinematics. int idq, idRes, codeSave; string nameSave; double Lambda, preFac, openFracPos, openFracNeg, sigmaA, sigmaB; }; //========================================================================== // A derived class for q qbar -> l^* lbar (excited lepton state). class Sigma2qqbar2lStarlbar : public Sigma2Process { public: // Constructor. Sigma2qqbar2lStarlbar(int idlIn) : idl(idlIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for l* decay angles (else inactive). virtual double weightDecay(Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return idRes;} private: // Parameters set at initialization or for current kinematics. int idl, idRes, codeSave; string nameSave; double Lambda, preFac, openFracPos, openFracNeg, sigma; }; //========================================================================== // A derived class for q q -> q q (quark contact interactions). // Based on, Sigma2qq2qq (QCD). class Sigma2QCqq2qq : public Sigma2Process { public: // Constructor. Sigma2QCqq2qq(){} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q q(bar)' -> (QC) -> q q(bar)'";} virtual int code() const {return 4201;} virtual string inFlux() const {return "qq";} private: // Values stored for colour flow selection. double sigT, sigU, sigTU, sigST, sigSum, sigQCSTU, sigQCUTS; // Compositeness parameters. double qCLambda2; int qCetaLL, qCetaRR, qCetaLR; }; //========================================================================== // A derived class for q qbar -> q' qbar' (quark contact interactions). // Based on, Sigma2qqbar2qqbarNew(QCD). // Note: This process give the same contributions for q == q' and q != q'. class Sigma2QCqqbar2qqbar : public Sigma2Process { public: // Constructor. Sigma2QCqqbar2qqbar(){} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> (QC) -> q' qbar' (uds)";} virtual int code() const {return 4202;} virtual string inFlux() const {return "qqbarSame";} private: // Number of outgoing quark flavours to be considered, given that // matrix elements are calculated in the massless approximation. int qCnQuarkNew; // Values stored for colour flow selection. int idNew; double mNew, m2New, sigS, sigma; // Compositeness parameters. double qCLambda2; int qCetaLL, qCetaRR, qCetaLR; }; //========================================================================== // A derived class for f fbar -> l lbar // (contact interactions). // Does not include t-channel contributions relevant for e^+e^- to e^+e^- class Sigma2QCffbar2llbar : public Sigma2Process { public: // Constructor: bool Graviton = true, to use LED graviton settings. Sigma2QCffbar2llbar (int idIn, int codeIn) : idNew(idIn), codeNew(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section; // first step when inflavours unknown. virtual void sigmaKin(); // Evaluate sigmaHat(sHat); second step for given inflavours. virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameNew;} virtual int code() const {return codeNew;} virtual string inFlux() const {return "ffbarSame";} virtual bool isSChannel() const {return true;} private: // Process values. string nameNew; int idNew, codeNew; double qCmNew, qCmNew2, qCmZ, qCmZ2, qCGZ, qCGZ2, sigma0; // Compositeness parameters. double qCLambda2; int qCetaLL, qCetaRR, qCetaLR; double qCPropGm, qCrePropZ, qCimPropZ; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaCompositeness_H pythia8-8.1.80.orig/include/Pythia8/HelicityBasics.h0000644000175000017500000002012512217346227020360 0ustar sunsun// HelicityBasics.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Philip Ilten, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for a number of helper classes used in tau decays. #ifndef Pythia8_HelicityBasics_H #define Pythia8_HelicityBasics_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/PythiaComplex.h" #include "Pythia8/PythiaStdlib.h" namespace Pythia8 { //========================================================================== // The Wave4 class provides a class for complex four-vector wave functions. // The Wave4 class can be multiplied with the GammaMatrix class to allow // for the writing of helicity matrix elements. class Wave4 { public: // Constructors and destructor. Wave4() {}; Wave4(complex v0, complex v1, complex v2, complex v3) {val[0] = v0; val[1] = v1; val[2] = v2; val[3] = v3;} Wave4(Vec4 v) {val[0] = v.e(); val[1] = v.px(); val[2] = v.py(); val[3] = v.pz();} ~Wave4() {}; // Access an element of the wave vector. complex& operator() (int i) {return val[i];} // Wave4 + Wave4. Wave4 operator+(Wave4 w) {return Wave4( val[0] + w.val[0], val[1] + w.val[1], val[2] + w.val[2], val[3] + w.val[3]);} // Wave4 - Wave4. Wave4 operator-(Wave4 w) {return Wave4( val[0] - w.val[0], val[1] - w.val[1], val[2] - w.val[2], val[3] - w.val[3]);} // - Wave4. Wave4 operator-() {return Wave4(-val[0], -val[1], -val[2], -val[3]);} // Wave4 * Wave4. complex operator*(Wave4 w) {return val[0] * w.val[0] + val[1] * w.val[1] + val[2] * w.val[2] + val[3] * w.val[3];} // Wave4 * complex. Wave4 operator*(complex s) {return Wave4(val[0] * s, val[1] * s, val[2] * s, val[3] * s);} // complex * Wave4. friend Wave4 operator*(complex s, const Wave4& w); // Wave4 * double. Wave4 operator*(double s) {return Wave4(val[0] * s, val[1] * s, val[2] * s, val[3] * s);} // double * Wave4. friend Wave4 operator*(double s, const Wave4& w); // Wave4 / complex. Wave4 operator/(complex s) {return Wave4(val[0] / s, val[1] / s, val[2] / s, val[3] / s);} // Wave4 / double. Wave4 operator/(double s) {return Wave4(val[0] / s, val[1] / s, val[2]/s, val[3]/s);} // Complex conjugate. friend Wave4 conj(Wave4 w); // Permutation operator. friend Wave4 epsilon(Wave4 w1, Wave4 w2, Wave4 w3); // Invariant squared mass for REAL Wave4 (to save time). friend double m2(Wave4 w); friend double m2(Wave4 w1, Wave4 w2); // Wave4 * GammaMatrix multiplication is defined in the GammaMatrix class. // Print a Wave4 vector. friend ostream& operator<<(ostream& output, Wave4 w); protected: complex val[4]; }; //-------------------------------------------------------------------------- // Namespace function declarations; friends of Wave4 class. Wave4 operator*(complex s, const Wave4& w); Wave4 conj(Wave4 w); Wave4 epsilon(Wave4 w1, Wave4 w2, Wave4 w3); double m2(Wave4 w); double m2(Wave4 w1, Wave4 w2); ostream& operator<< (ostream& os, Wave4 w); //========================================================================== // The GammaMatrix class is a special sparse matrix class used to write // helicity matrix elements in conjuction with the Wave4 class. Note that // only left to right multplication of Wave4 vectors with the GammaMatrix // class is allowed. Additionally, subtracting a scalar from a GammaMatrix // (or subtracting a GammaMatrix from a scalar) subtracts the scalar from //each non-zero element of the GammaMatrix. This is designed specifically // with the (1 - gamma^5) structure of matrix elements in mind. class GammaMatrix { public: // Constructors and destructor. GammaMatrix() {}; GammaMatrix(int mu); ~GammaMatrix() {}; // Access an element of the matrix. complex& operator() (int I, int J) {if (index[J] == I) return val[J]; else return COMPLEXZERO; } // Wave4 * GammaMatrix. friend Wave4 operator*(Wave4 w, GammaMatrix g); // GammaMatrix * Scalar. GammaMatrix operator*(complex s) {val[0] = s*val[0]; val[1] = s*val[1]; val[2] = s*val[2]; val[3] = s*val[3]; return *this;} // Scalar * GammaMatrix. friend GammaMatrix operator*(complex s, GammaMatrix g); // Gamma5 - I * Scalar. GammaMatrix operator-(complex s) {val[0] = val[0] - s; val[1] = val[1] - s; val[2] = val[2] - s; val[3] = val[3] - s; return *this;} // I * Scalar - Gamma5. friend GammaMatrix operator-(complex s, GammaMatrix g); // Gamma5 + I * Scalar GammaMatrix operator+(complex s) {val[0] = val[0] + s; val[1] = val[1] + s; val[2] = val[2] + s; val[3] = val[3] + s; return *this;} // I * Scalar + Gamma5 friend GammaMatrix operator+(complex s, GammaMatrix g); // << GammaMatrix. friend ostream& operator<< (ostream& os, GammaMatrix g); protected: complex val[4]; int index[4]; // Need to define complex 0 as a variable for operator() to work. complex COMPLEXZERO; }; //-------------------------------------------------------------------------- // Namespace function declarations; friends of GammaMatrix class. Wave4 operator*(Wave4 w, GammaMatrix g); GammaMatrix operator*(complex s, GammaMatrix g); GammaMatrix operator-(complex s, GammaMatrix g); GammaMatrix operator+(complex s, GammaMatrix g); ostream& operator<< (ostream& os, GammaMatrix g); //========================================================================== // Helicity particle class containing helicity information, derived from // particle base class. class HelicityParticle : public Particle { public: // Constructors. HelicityParticle() : Particle() { direction = 1;} HelicityParticle(int idIn, int statusIn = 0, int mother1In = 0, int mother2In = 0, int daughter1In = 0, int daughter2In = 0, int colIn = 0, int acolIn = 0, double pxIn = 0., double pyIn = 0., double pzIn = 0., double eIn = 0., double mIn = 0., double scaleIn = 0., ParticleData* ptr = 0) : Particle(idIn, statusIn, mother1In, mother2In, daughter1In, daughter2In, colIn, acolIn, pxIn, pyIn, pzIn, eIn, mIn, scaleIn) { if (ptr) setPDEPtr( ptr->particleDataEntryPtr( idIn) ); rho = vector< vector >(spinStates(), vector(spinStates(), 0)); D = vector< vector >(spinStates(), vector(spinStates(), 0)); for (int i = 0; i < spinStates(); i++) { rho[i][i] = 0.5; D[i][i] = 1.;} direction = 1; } HelicityParticle(int idIn, int statusIn, int mother1In, int mother2In, int daughter1In, int daughter2In, int colIn, int acolIn, Vec4 pIn, double mIn = 0., double scaleIn = 0., ParticleData* ptr = 0) : Particle(idIn, statusIn, mother1In, mother2In, daughter1In, daughter2In, colIn, acolIn, pIn, mIn, scaleIn) { if (ptr) setPDEPtr( ptr->particleDataEntryPtr( idIn) ); rho = vector< vector >(spinStates(), vector(spinStates(), 0)); D = vector< vector >(spinStates(), vector(spinStates(), 0)); for (int i = 0; i < spinStates(); i++) { rho[i][i] = 0.5; D[i][i] = 1;} direction = 1; } HelicityParticle(const Particle& ptIn, ParticleData* ptr = 0) : Particle(ptIn) { if (ptr) setPDEPtr( ptr->particleDataEntryPtr( id()) ); rho = vector< vector >(spinStates(), vector(spinStates(), 0)); D = vector< vector >(spinStates(), vector(spinStates(), 0)); for (int i = 0; i < spinStates(); i++) { rho[i][i] = 0.5; D[i][i] = 1;} direction = 1; } // Methods. Wave4 wave(int h); Wave4 waveBar(int h); void normalize(vector< vector >& m); int spinStates(); // Event record position. int idx; // Flag for whether particle is incoming (-1) or outgoing (1). int direction; // Helicity density matrix. vector< vector > rho; // Decay matrix. vector< vector > D; private: // Constants: could only be changed in the code itself. static const double TOLERANCE; }; //========================================================================== } // end namespace Pythia8 #endif // end Pythia8_HelicityBasics_H pythia8-8.1.80.orig/include/Pythia8/MergingHooks.h0000644000175000017500000007111012217346227020055 0ustar sunsun// MergingHooks.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file is written by Stefan Prestel. // Header file to allow user access to program at different stages. // HardProcess: Container class for the hard process to be merged. Holds the // bookkeeping of particles not be be reclustered // MergingHooks: Steering class for matrix element merging. Some functions can // be redefined in a derived class to have access to the merging #ifndef Pythia8_MergingHooks_H #define Pythia8_MergingHooks_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonSystems.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // Declaration of hard process class // This class holds information on the desired hard 2->2 process // for the merging. // This class is a container class for History class use. class HardProcess { public: // Flavour of the first incoming particle int hardIncoming1; // Flavour of the second incoming particle int hardIncoming2; // Flavours of the outgoing particles vector hardOutgoing1; vector hardOutgoing2; // Flavour of intermediate bosons in the hard 2->2 vector hardIntermediate; // Current reference event Event state; // Potential positions of outgoing particles in reference event vector PosOutgoing1; vector PosOutgoing2; // Potential positions of intermediate bosons in reference event vector PosIntermediate; // Information on merging scale read from LHE file double tms; // Default constructor HardProcess(){} // Default destructor ~HardProcess(){} // Copy constructor HardProcess( const HardProcess& hardProcessIn ) : state(hardProcessIn.state), tms(hardProcessIn.tms) { hardIncoming1 = hardProcessIn.hardIncoming1; hardIncoming2 = hardProcessIn.hardIncoming2; for(int i =0; i < int(hardProcessIn.hardOutgoing1.size());++i) hardOutgoing1.push_back( hardProcessIn.hardOutgoing1[i]); for(int i =0; i < int(hardProcessIn.hardOutgoing2.size());++i) hardOutgoing2.push_back( hardProcessIn.hardOutgoing2[i]); for(int i =0; i < int(hardProcessIn.hardIntermediate.size());++i) hardIntermediate.push_back( hardProcessIn.hardIntermediate[i]); for(int i =0; i < int(hardProcessIn.PosOutgoing1.size());++i) PosOutgoing1.push_back( hardProcessIn.PosOutgoing1[i]); for(int i =0; i < int(hardProcessIn.PosOutgoing2.size());++i) PosOutgoing2.push_back( hardProcessIn.PosOutgoing2[i]); for(int i =0; i < int(hardProcessIn.PosIntermediate.size());++i) PosIntermediate.push_back( hardProcessIn.PosIntermediate[i]); } // Constructor with path to LHE file HardProcess( string LHEfile, ParticleData* particleData) { state = Event(); state.init("(hard process)", particleData); translateLHEFString(LHEfile); } // Constructor with core process input void initOnProcess( string process, ParticleData* particleData); // Constructor with path to LHE file input void initOnLHEF( string LHEfile, ParticleData* particleData); // Function to access the LHE file and read relevant information void translateLHEFString( string LHEpath); // Function to translate the process string (in MG/ME notation) void translateProcessString( string process); // Function to clear hard process information void clear(); // Function to check whether the sets of candidates Pos1, Pos2, together // with the proposed candidate iPos give an allowed hard process state bool allowCandidates(int iPos, vector Pos1, vector Pos2, const Event& event); // Function to identify the hard subprocess in the current event void storeCandidates( const Event& event, string process); // Function to check if the particle event[iPos] matches any of // the stored outgoing particles of the hard subprocess bool matchesAnyOutgoing(int iPos, const Event& event); // Function to check if instead of the particle event[iCandidate], another // particle could serve as part of the hard process. Assumes that iCandidate // is already stored as part of the hard process. bool findOtherCandidates(int iPos, const Event& event, bool doReplace); // Function to exchange a stored hard process candidate with another choice. bool exchangeCandidates( vector candidates1, vector candidates2, map further1, map further2); // Function to get the number of coloured final state partons in the // hard process int nQuarksOut(); // Function to get the number of uncoloured final state particles in the // hard process int nLeptonOut(); // Function to get the number of electroweak final state bosons in the // hard process int nBosonsOut(); // Function to get the number of coloured initial state partons in the // hard process int nQuarksIn(); // Function to get the number of uncoloured initial state particles in the // hard process int nLeptonIn(); // Function to report if a resonace decay was found in the 2->2 sub-process // of the current state int hasResInCurrent(); // Function to report the number of resonace decays in the 2->2 sub-process // of the current state int nResInCurrent(); // Function to report if a resonace decay was found in the 2->2 hard process bool hasResInProc(); // Function to print the hard process (for debug) void list() const; // Function to print the hard process candidates in the // Matrix element state (for debug) void listCandidates() const; }; //========================================================================== // MergingHooks is base class for user input to the merging procedure. class MergingHooks { public: // Constructor. MergingHooks() : doUserMergingSave(false), doMGMergingSave(false), doKTMergingSave(false), doPTLundMergingSave(false), doCutBasedMergingSave(false), doNL3TreeSave(false), doNL3LoopSave(false), doNL3SubtSave(false), doUNLOPSTreeSave(false), doUNLOPSLoopSave(false), doUNLOPSSubtSave(false), doUNLOPSSubtNLOSave(false), doUMEPSTreeSave(false), doUMEPSSubtSave(false), doEstimateXSection(false), doRemoveDecayProducts(false), doOrderHistoriesSave(true), doCutOnRecStateSave(false), doWClusteringSave(false), doSQCDClusteringSave(false), doIgnoreEmissionsSave(true), doIgnoreStepSave(true) { inputEvent = Event(); resonances.resize(0); infoPtr = 0; particleDataPtr = 0; partonSystemsPtr = 0;} // Make History class friend to allow access to advanced switches friend class History; // Make Pythia class friend friend class Pythia; // Make PartonLevel class friend friend class PartonLevel; // Make SpaceShower class friend friend class SpaceShower; // Make TimeShower class friend friend class TimeShower; // Make Merging class friend friend class Merging; //----------------------------------------------------------------------// // Functions that allow user interference //----------------------------------------------------------------------// // Destructor. virtual ~MergingHooks(){} // Function encoding the functional definition of the merging scale virtual double tmsDefinition( const Event& event){ return event[0].e();} // Function to dampen weights calculated from histories with lowest // multiplicity reclustered events that do not pass the ME cuts virtual double dampenIfFailCuts( const Event& inEvent ) { // Dummy statement to avoid compiler warnings if(false) cout << inEvent[0].e(); return 1.; } // Hooks to disallow states in the construction of all histories, e.g. // because jets are below the merging scale or fail the matrix element cuts // Function to allow interference in the construction of histories virtual bool canCutOnRecState() { return doCutOnRecStateSave; } // Function to check reclustered state while generating all possible // histories // Function implementing check of reclustered events while constructing // all possible histories virtual bool doCutOnRecState( const Event& event ) { // Dummy statement to avoid compiler warnings. if(false) cout << event[0].e(); // Count number of final state partons. int nPartons = 0; for( int i=0; i < int(event.size()); ++i) if( event[i].isFinal() && (event[i].isGluon() || event[i].isQuark()) ) nPartons++; // For gg -> h, allow only histories with gluons in initial state if( hasEffectiveG2EW() && nPartons < 2){ if(event[3].id() != 21 && event[4].id() != 21) return true; } return false; } // Function to allow not counting a trial emission. virtual bool canVetoTrialEmission() { return false;} // Function to check if trial emission should be rejected. virtual bool doVetoTrialEmission( const Event&, const Event& ) { return false; } // Function to calculate the hard process matrix element. virtual double hardProcessME( const Event& inEvent ) { // Dummy statement to avoid compiler warnings. if ( false ) cout << inEvent[0].e(); return 1.; } //----------------------------------------------------------------------// // Simple output functions //----------------------------------------------------------------------// // Function returning the value of the merging scale. double tms() { if(doCutBasedMergingSave) return 0.; else return tmsValueSave; } // Function returning the value of the Delta R_{ij} cut for // cut based merging scale definition. double dRijMS() { return ((tmsListSave.size() == 3) ? tmsListSave[0] : 0.); } // Function returning the value of the pT_{i} cut for // cut based merging scale definition. double pTiMS() { return ((tmsListSave.size() == 3) ? tmsListSave[1] : 0.); } // Function returning the value of the pT_{i} cut for // cut based merging scale definition. double QijMS() { return ((tmsListSave.size() == 3) ? tmsListSave[2] : 0.); } // Function returning the value of the maximal number of merged jets. int nMaxJets() { return nJetMaxSave;} // Function returning the value of the maximal number of merged jets, // for which NLO corrections are available. int nMaxJetsNLO() { return nJetMaxNLOSave;} // Function to return hard process string. string getProcessString() { return processSave;} // Function to return the number of outgoing partons in the core process int nHardOutPartons(){ return hardProcess.nQuarksOut();} // Function to return the number of outgoing leptons in the core process int nHardOutLeptons(){ return hardProcess.nLeptonOut();} // Function to return the number of outgoing electroweak bosons in the core // process. int nHardOutBosons(){ return hardProcess.nBosonsOut();} // Function to return the number of incoming partons (hadrons) in the core // process. int nHardInPartons(){ return hardProcess.nQuarksIn();} // Function to return the number of incoming leptons in the core process. int nHardInLeptons(){ return hardProcess.nLeptonIn();} // Function to report the number of resonace decays in the 2->2 sub-process // of the current state. int nResInCurrent(){ return hardProcess.nResInCurrent();} // Function to determine if user defined merging should be applied. bool doUserMerging(){ return doUserMergingSave;} // Function to determine if automated MG/ME merging should be applied. bool doMGMerging() { return doMGMergingSave;} // Function to determine if KT merging should be applied. bool doKTMerging() { return doKTMergingSave;} // Function to determine if PTLund merging should be applied. bool doPTLundMerging() { return doPTLundMergingSave;} // Function to determine if cut based merging should be applied. bool doCutBasedMerging() { return doCutBasedMergingSave;} bool doCKKWLMerging() { return (doUserMergingSave || doMGMergingSave || doKTMergingSave || doPTLundMergingSave || doCutBasedMergingSave); } // Functions to determine if and which part of UMEPS merging // should be applied bool doUMEPSTree() { return doUMEPSTreeSave;} bool doUMEPSSubt() { return doUMEPSSubtSave;} bool doUMEPSMerging() { return (doUMEPSTreeSave || doUMEPSSubtSave);} // Functions to determine if and which part of NL3 merging // should be applied bool doNL3Tree() { return doNL3TreeSave;} bool doNL3Loop() { return doNL3LoopSave;} bool doNL3Subt() { return doNL3SubtSave;} bool doNL3Merging() { return (doNL3TreeSave || doNL3LoopSave || doNL3SubtSave); } // Functions to determine if and which part of UNLOPS merging // should be applied bool doUNLOPSTree() { return doUNLOPSTreeSave;} bool doUNLOPSLoop() { return doUNLOPSLoopSave;} bool doUNLOPSSubt() { return doUNLOPSSubtSave;} bool doUNLOPSSubtNLO() { return doUNLOPSSubtNLOSave;} bool doUNLOPSMerging() { return (doUNLOPSTreeSave || doUNLOPSLoopSave || doUNLOPSSubtSave || doUNLOPSSubtNLOSave); } // Return the number clustering steps that have actually been done. int nRecluster() { return nReclusterSave;} //----------------------------------------------------------------------// // Output functions to analyse/prepare event for merging //----------------------------------------------------------------------// // Function to check if event contains an emission not present in the hard // process. bool isFirstEmission(const Event& event); // Function to allow effective gg -> EW boson couplings. bool hasEffectiveG2EW() { if ( getProcessString().compare("pp>h") == 0 ) return true; return false; } // Return event stripped from decay products. Event bareEvent( const Event& inputEventIn, bool storeInputEvent ); // Write event with decay products attached to argument. bool reattachResonanceDecays( Event& process ); // Check if particle at position iPos is part of the hard sub-system bool isInHard( int iPos, const Event& event); // Function to return the number of clustering steps for the current event int getNumberOfClusteringSteps(const Event& event); //----------------------------------------------------------------------// // Functions to steer contruction of histories //----------------------------------------------------------------------// // Function to force preferred picking of ordered histories. By default, // unordered histories will only be considered if no ordered histories // were found. void orderHistories( bool doOrderHistoriesIn) { doOrderHistoriesSave = doOrderHistoriesIn; } // Function to force cut on reconstructed states internally, as needed // for gg -> Higgs to ensure that e.g. uu~ -> Higgs is not constructed. void allowCutOnRecState( bool doCutOnRecStateIn) { doCutOnRecStateSave = doCutOnRecStateIn; } // Function to allow final state clusterings of W-bosons void doWClustering( bool doWClusteringIn ) { doWClusteringSave = doWClusteringIn; } //----------------------------------------------------------------------// // Functions used as default merging scales //----------------------------------------------------------------------// // Function to check if the input particle is a light jet, i.e. should be // checked against the merging scale defintion. bool checkAgainstCut( const Particle& particle); // Function to return the value of the merging scale function in the // current event. double tmsNow( const Event& event ); // Find the minimal Lund pT between coloured partons in the event double rhoms( const Event& event, bool withColour); // Function to calculate the minimal kT in the event double kTms(const Event & event); // Find the if the event passes the Delta R_{ij}, pT_{i} and Q_{ij} cuts on // the matrix element, as needed for cut-based merging scale definition double cutbasedms( const Event& event ); protected: //----------------------------------------------------------------------// // The members, switches etc. //----------------------------------------------------------------------// // Helper class doing all the core process book-keeping HardProcess hardProcess; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the particle systems. PartonSystems* partonSystemsPtr; // AlphaS objects for alphaS reweighting use AlphaStrong AlphaS_FSRSave; AlphaStrong AlphaS_ISRSave; AlphaEM AlphaEM_FSRSave; // Saved path to LHE file for more automated merging string lheInputFile; // Flags for merging procedure definition. bool doUserMergingSave, doMGMergingSave, doKTMergingSave, doPTLundMergingSave, doCutBasedMergingSave, includeMassiveSave, enforceStrongOrderingSave, orderInRapiditySave, pickByFullPSave, pickByPoPT2Save, includeRedundantSave, pickBySumPTSave, allowColourShufflingSave, resetHardQRenSave, resetHardQFacSave; int unorderedScalePrescipSave, unorderedASscalePrescipSave, unorderedPDFscalePrescipSave, incompleteScalePrescipSave, ktTypeSave, nReclusterSave, nQuarksMergeSave; double scaleSeparationFactorSave, nonJoinedNormSave, fsrInRecNormSave, herwigAcollFSRSave, herwigAcollISRSave, pT0ISRSave, pTcutSave; bool doNL3TreeSave, doNL3LoopSave, doNL3SubtSave; bool doUNLOPSTreeSave, doUNLOPSLoopSave, doUNLOPSSubtSave, doUNLOPSSubtNLOSave; bool doUMEPSTreeSave, doUMEPSSubtSave; // Flag to only do phase space cut, rejecting events below the tms cut. bool doEstimateXSection; // Save input event in case decay products need to be detached. Event inputEvent; vector< pair > resonances; bool doRemoveDecayProducts; // Starting scale for attaching MPI. double muMISave; // Precalculated K-factors. double kFactor0jSave; double kFactor1jSave; double kFactor2jSave; // Saved members. double tmsValueSave; int nJetMaxSave; int nJetMaxNLOSave; string processSave; // List of cut values to used to define a merging scale. Ordering: // 0: DeltaR_{jet_i,jet_j,min} // 1: p_{T,jet_i,min} // 2: Q_{jet_i,jet_j,min} vector tmsListSave; // INTERNAL Hooks to allow construction of all histories, // including un-ordered ones bool doOrderHistoriesSave; // INTERNAL Hooks to disallow states in the construction of all histories, // e.g. because jets are below the merging scale, of to avoid the // construction of uu~ -> Higgs histories. bool doCutOnRecStateSave; // INTERNAL Hooks to allow clustering W bosons. bool doWClusteringSave, doSQCDClusteringSave; // Store / get first scale in PDF's that Pythia should have used double muFSave; double muRSave; // Store / get factorisation scale used in matrix element calculation. double muFinMESave; double muRinMESave; // Flag to indicate trial shower usage. bool doIgnoreEmissionsSave; // Flag to indicate if events should be vetoed. bool doIgnoreStepSave; // Stored weights in case veot needs to be revoked double pTsave; double weightCKKWL1Save, weightCKKWL2Save; int nMinMPISave; // Save CKKW-L weight / O(\alpha_s) weight. double weightCKKWLSave, weightFIRSTSave; //----------------------------------------------------------------------// // Generic setup functions //----------------------------------------------------------------------// // Functions for internal use inside Pythia source code // Initialize. void init( Settings settings, Info* infoPtrIn, ParticleData* particleDataPtrIn, PartonSystems* partonSystemsPtrIn, ostream& os = cout); // Function storing candidates for the hard process in the current event // Needed in order not to cluster members of the core process void storeHardProcessCandidates(const Event& event){ hardProcess.storeCandidates(event,getProcessString()); } // Function to set the path to the LHE file, so that more automated merging // can be used. // Remove "_1.lhe" suffix from LHE file name. // This is done so that the HarsProcess class can access both the +0 and +1 // LHE files to find both the merging scale and the core process string // Store. void setLHEInputFile( string lheFile) { lheInputFile = lheFile.substr(0,lheFile.size()-6); } //----------------------------------------------------------------------// // Functions for output of class members. //----------------------------------------------------------------------// // Return AlphaStrong objects AlphaStrong* AlphaS_FSR() { return &AlphaS_FSRSave;} AlphaStrong* AlphaS_ISR() { return &AlphaS_ISRSave;} AlphaEM* AlphaEM_FSR() { return &AlphaEM_FSRSave;} // Functions to return advanced merging switches // Include masses in definition of evolution pT and splitting kernels bool includeMassive() { return includeMassiveSave;} // Prefer strongly ordered histories bool enforceStrongOrdering() { return enforceStrongOrderingSave;} // Prefer histories ordered in rapidity and evolution pT bool orderInRapidity() { return orderInRapiditySave;} // Pick history probabilistically by full (correct) splitting probabilities bool pickByFull() { return pickByFullPSave;} // Pick history probabilistically, with easier form of probabilities bool pickByPoPT2() { return pickByPoPT2Save;} // Include redundant terms (e.g. PDF ratios) in the splitting probabilities bool includeRedundant(){ return includeRedundantSave;} // Pick by winner-takes-it-all, with minimum sum of scalar evolution pT bool pickBySumPT(){ return pickBySumPTSave;} // Prescription for combined scale of unordered emissions // 0 : use larger scale // 1 : use smaller scale int unorderedScalePrescip() { return unorderedScalePrescipSave;} // Prescription for combined scale used in alpha_s for unordered emissions // 0 : use combined emission scale in alpha_s weight for both (!) splittings // 1 : use original reclustered scales of each emission in alpha_s weight int unorderedASscalePrescip() { return unorderedASscalePrescipSave;} // Prescription for combined scale used in PDF ratios for unordered // emissions // 0 : use combined emission scale in PDFs for both (!) splittings // 1 : use original reclustered scales of each emission in PDF ratiost int unorderedPDFscalePrescip() { return unorderedPDFscalePrescipSave;} // Prescription for starting scale of incomplete histories // 0: use factorization scale // 1: use sHat // 2: use s int incompleteScalePrescip() { return incompleteScalePrescipSave;} // Allow swapping one colour index while reclustering bool allowColourShuffling() { return allowColourShufflingSave;} // Allow use of dynamical renormalisation scale of the core 2-> 2 process. bool resetHardQRen() { return resetHardQRenSave; } // Allow use of dynamical factorisation scale of the core 2-> 2 process. bool resetHardQFac() { return resetHardQFacSave; } // Factor by which two scales should differ to be classified strongly // ordered. double scaleSeparationFactor() { return scaleSeparationFactorSave;} // Absolute normalization of splitting probability for non-joined // evolution. double nonJoinedNorm() { return nonJoinedNormSave;} // Absolute normalization of splitting probability for final state // splittings with initial state recoiler double fsrInRecNorm() { return fsrInRecNormSave;} // Factor multiplying scalar evolution pT for FSR splitting, when picking // history by minimum scalar pT (see Jonathan Tully's thesis) double herwigAcollFSR() { return herwigAcollFSRSave;} // Factor multiplying scalar evolution pT for ISR splitting, when picking // history by minimum scalar pT (see Jonathan Tully's thesis) double herwigAcollISR() { return herwigAcollISRSave;} // ISR regularisation scale double pT0ISR() { return pT0ISRSave;} // Shower cut-off scale double pTcut() { return pTcutSave;} // MI starting scale. void muMI( double mu) { muMISave = mu; } double muMI() { return muMISave;} // Full k-Factor for current event double kFactor(int njet = 0) { return (njet == 0) ? kFactor0jSave :(njet == 1) ? kFactor1jSave : kFactor2jSave; } // O(\alhpa_s)-term of the k-Factor for current event double k1Factor( int njet = 0) { return (kFactor(njet) - 1)/infoPtr->alphaS(); } // Function to return if construction of histories is biased towards ordered // histories. bool orderHistories() { return doOrderHistoriesSave;} // INTERNAL Hooks to disallow states in the construction of all histories, // e.g. because jets are below the merging scale, of to avoid the // construction of uu~ -> Higgs histories. bool allowCutOnRecState() { return doCutOnRecStateSave;} // INTERNAL Hooks to allow clustering W bosons. bool doWClustering() { return doWClusteringSave;} // INTERNAL Hooks to allow clustering clustering of gluons to squarks. bool doSQCDClustering() { return doSQCDClusteringSave;} // Store / get first scale in PDF's that Pythia should have used double muF() { return (muFSave > 0.) ? muFSave : infoPtr->QFac();} double muR() { return (muRSave > 0.) ? muRSave : infoPtr->QRen();} // Store / get factorisation scale used in matrix element calculation. double muFinME() { return (muFinMESave > 0.) ? muFinMESave : infoPtr->QFac();} double muRinME() { return (muRinMESave > 0.) ? muRinMESave : infoPtr->QRen();} //----------------------------------------------------------------------// // Functions to steer shower evolution //----------------------------------------------------------------------// // Flag to indicate trial shower usage. void doIgnoreEmissions( bool doIgnoreIn ) { doIgnoreEmissionsSave = doIgnoreIn; } // Function to allow not counting a trial emission. bool canVetoEmission() { return !doIgnoreEmissionsSave; } // Function to check if emission should be rejected. bool doVetoEmission( const Event& ); // Flag to indicate if events should be vetoed. void doIgnoreStep( bool doIgnoreIn ) { doIgnoreStepSave = doIgnoreIn; } // Function to allow event veto. bool canVetoStep() { return !doIgnoreStepSave; } // Function to check event veto. bool doVetoStep( const Event& process, const Event& event, bool doResonance = false ); // Stored weights in case veot needs to be revoked void storeWeights( double weight ){ weightCKKWL1Save = weightCKKWL2Save = weight; } // Set starting scales bool setShowerStartingScales( bool isTrial, bool doMergeFirstEmm, double& pTscaleIn, const Event& event, double& pTmaxFSRIn, bool& limitPTmaxFSRin, double& pTmaxISRIn, bool& limitPTmaxISRin, double& pTmaxMPIIn, bool& limitPTmaxMPIin ); void nMinMPI( int nMinMPIIn ) { nMinMPISave = nMinMPIIn; } int nMinMPI() { return nMinMPISave;} //----------------------------------------------------------------------// // Functions for internal merging scale definions //----------------------------------------------------------------------// // Function to calculate the kT separation between two particles double kTdurham(const Particle& RadAfterBranch, const Particle& EmtAfterBranch, int Type, double D ); // Function to compute "pythia pT separation" from Particle input double rhoPythia(const Particle& RadAfterBranch, const Particle& EmtAfterBranch, const Particle& RecAfterBranch, int ShowerType); // Function to find a colour (anticolour) index in the input event, // used to find colour-connected recoilers int findColour(int col, int iExclude1, int iExclude2, const Event& event, int type, bool isHardIn); // Function to compute Delta R separation from 4-vector input double deltaRij(Vec4 jet1, Vec4 jet2); //----------------------------------------------------------------------// // Functions for weight management //----------------------------------------------------------------------// // Function to get the CKKW-L weight for the current event double getWeightNLO() { return (weightCKKWLSave - weightFIRSTSave);} // Return CKKW-L weight. double getWeightCKKWL() { return weightCKKWLSave; } // Return O(\alpha_s) weight. double getWeightFIRST() { return weightFIRSTSave; } // Set CKKW-L weight. void setWeightCKKWL( double weightIn){ weightCKKWLSave = weightIn; infoPtr->setWeightCKKWL(weightIn); } // Set O(\alpha_s) weight. void setWeightFIRST( double weightIn){ weightFIRSTSave = weightIn; infoPtr->setWeightFIRST(weightIn); } }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_MergingHooks_H pythia8-8.1.80.orig/include/Pythia8/UserHooks.h0000644000175000017500000002426612217346232017411 0ustar sunsun// UserHooks.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file to allow user access to program at different stages. // UserHooks: almost empty base class, with user to write the rela code. // MyUserHooks: derived class, only intended as an example. #ifndef Pythia8_UserHooks_H #define Pythia8_UserHooks_H #include "Pythia8/Event.h" #include "Pythia8/PartonSystems.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // Forward reference to the PhaseSpace class. class PhaseSpace; //========================================================================== // UserHooks is base class for user access to program execution. class UserHooks { public: // Destructor. virtual ~UserHooks() {} // Initialize pointers and workEvent. Note: not virtual. void initPtr( Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, BeamParticle* beamPomAPtrIn, BeamParticle* beamPomBPtrIn, CoupSM* coupSMPtrIn, PartonSystems* partonSystemsPtrIn, SigmaTotal* sigmaTotPtrIn) { infoPtr = infoPtrIn; settingsPtr = settingsPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; beamPomAPtr = beamPomAPtrIn; beamPomBPtr = beamPomBPtrIn; coupSMPtr = coupSMPtrIn; partonSystemsPtr = partonSystemsPtrIn; sigmaTotPtr = sigmaTotPtrIn; workEvent.init("(work event)", particleDataPtr);} // Initialisation after beams have been set by Pythia::init() virtual bool initAfterBeams() { return true; } // Possibility to modify cross section of process. virtual bool canModifySigma() {return false;} // Multiplicative factor modifying the cross section of a hard process. virtual double multiplySigmaBy(const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool inEvent); // Possibility to bias selection of events, compensated by a weight. virtual bool canBiasSelection() {return false;} // Multiplicative factor in the phase space selection of a hard process. virtual double biasSelectionBy(const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool inEvent); // Event weight to compensate for selection weight above. virtual double biasedSelectionWeight() {return 1./selBias;} // Possibility to veto event after process-level selection. virtual bool canVetoProcessLevel() {return false;} // Decide whether to veto current process or not, based on process record. // Usage: doVetoProcessLevel( process). virtual bool doVetoProcessLevel(Event& ) {return false;} // Possibility to veto resonance decay chain. virtual bool canVetoResonanceDecays() {return false;} // Decide whether to veto current resonance decay chain or not, based on // process record. Usage: doVetoProcessLevel( process). virtual bool doVetoResonanceDecays(Event& ) {return false;} // Possibility to veto MPI + ISR + FSR evolution and kill event, // making decision at a fixed pT scale. Useful for MLM-style matching. virtual bool canVetoPT() {return false;} // Transverse-momentum scale for veto test. virtual double scaleVetoPT() {return 0.;} // Decide whether to veto current event or not, based on event record. // Usage: doVetoPT( iPos, event), where iPos = 0: no emissions so far; // iPos = 1/2/3 joint evolution, latest step was MPI/ISR/FSR; // iPos = 4: FSR only afterwards; iPos = 5: FSR in resonance decay. virtual bool doVetoPT( int , const Event& ) {return false;} // Possibility to veto MPI + ISR + FSR evolution and kill event, // making decision after fixed number of ISR or FSR steps. virtual bool canVetoStep() {return false;} // Up to how many ISR + FSR steps of hardest interaction should be checked. virtual int numberVetoStep() {return 1;} // Decide whether to veto current event or not, based on event record. // Usage: doVetoStep( iPos, nISR, nFSR, event), where iPos as above, // nISR and nFSR number of emissions so far for hard interaction only. virtual bool doVetoStep( int , int , int , const Event& ) {return false;} // Possibility to veto MPI + ISR + FSR evolution and kill event, // making decision after fixed number of MPI steps. virtual bool canVetoMPIStep() {return false;} // Up to how many MPI steps should be checked. virtual int numberVetoMPIStep() {return 1;} // Decide whether to veto current event or not, based on event record. // Usage: doVetoMPIStep( nMPI, event), where nMPI is number of MPI's so far. virtual bool doVetoMPIStep( int , const Event& ) {return false;} // Possibility to veto event after ISR + FSR + MPI in parton level, // but before beam remnants and resonance decays. virtual bool canVetoPartonLevelEarly() {return false;} // Decide whether to veto current partons or not, based on event record. // Usage: doVetoPartonLevelEarly( event). virtual bool doVetoPartonLevelEarly( const Event& ) {return false;} // Retry same ProcessLevel with a new PartonLevel after a veto in // doVetoPT, doVetoStep, doVetoMPIStep or doVetoPartonLevelEarly // if you overload this method to return true. virtual bool retryPartonLevel() {return false;} // Possibility to veto event after parton-level selection. virtual bool canVetoPartonLevel() {return false;} // Decide whether to veto current partons or not, based on event record. // Usage: doVetoPartonLevel( event). virtual bool doVetoPartonLevel( const Event& ) {return false;} // Possibility to set initial scale in TimeShower for resonance decay. virtual bool canSetResonanceScale() {return false;} // Initial scale for TimeShower evolution. // Usage: scaleResonance( iRes, event), where iRes is location // of decaying resonance in the event record. virtual double scaleResonance( int, const Event& ) {return 0.;} // Possibility to veto an emission in the ISR machinery. virtual bool canVetoISREmission() {return false;} // Decide whether to veto current emission or not, based on event record. // Usage: doVetoISREmission( sizeOld, event, iSys) where sizeOld is size // of event record before current emission-to-be-scrutinized was added, // and iSys is the system of the radiation (according to PartonSystems). virtual bool doVetoISREmission( int, const Event&, int ) {return false;} // Possibility to veto an emission in the FSR machinery. virtual bool canVetoFSREmission() {return false;} // Decide whether to veto current emission or not, based on event record. // Usage: doVetoFSREmission( sizeOld, event, iSys, inResonance) where // sizeOld is size of event record before current emission-to-be-scrutinized // was added, iSys is the system of the radiation (according to // PartonSystems), and inResonance is true if the emission takes place in a // resonance decay. virtual bool doVetoFSREmission( int, const Event&, int, bool = false ) {return false;} // Possibility to veto an MPI. virtual bool canVetoMPIEmission() { return false; } // Decide whether to veto an MPI based on event record. // Usage: doVetoMPIEmission( sizeOld, event) where sizeOld // is size of event record before the current MPI. virtual bool doVetoMPIEmission(int, const Event &) { return false; } protected: // Constructor. UserHooks() : infoPtr(0), settingsPtr(0), particleDataPtr(0), rndmPtr(0), beamAPtr(0), beamBPtr(0), beamPomAPtr(0), beamPomBPtr(0), coupSMPtr(0), partonSystemsPtr(0), sigmaTotPtr(0), selBias(1.) {} // Pointer to various information on the generation. Info* infoPtr; // Pointer to the settings database. Settings* settingsPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to the two incoming beams and to Pomeron beam-inside-beam. BeamParticle* beamAPtr; BeamParticle* beamBPtr; BeamParticle* beamPomAPtr; BeamParticle* beamPomBPtr; // Pointers to Standard Model couplings. CoupSM* coupSMPtr; // Pointer to information on subcollision parton locations. PartonSystems* partonSystemsPtr; // Pointer to the total/elastic/diffractive cross sections. SigmaTotal* sigmaTotPtr; // omitResonanceDecays omits resonance decay chains from process record. void omitResonanceDecays(const Event& process, bool finalOnly = false); // subEvent extracts currently resolved partons in the hard process. void subEvent(const Event& event, bool isHardest = true); // Have one event object around as work area. Event workEvent; // User-imposed selection bias. double selBias; }; //========================================================================== // SuppressSmallPT is a derived class for user access to program execution. // It is a simple example, illustrating how to suppress the cross section // of 2 -> 2 processes by a factor pT^4 / (pT0^2 + pT^2)^2, with pT0 input, // and also modify alpha_strong scale similarly. class SuppressSmallPT : public UserHooks { public: // Constructor. SuppressSmallPT( double pT0timesMPIIn = 1., int numberAlphaSIn = 0, bool useSameAlphaSasMPIIn = true) : pT20(0.) {isInit = false; pT0timesMPI = pT0timesMPIIn; numberAlphaS = numberAlphaSIn; useSameAlphaSasMPI = useSameAlphaSasMPIIn;} // Possibility to modify cross section of process. virtual bool canModifySigma() {return true;} // Multiplicative factor modifying the cross section of a hard process. // Usage: inEvent is true for event generation, false for initialization. virtual double multiplySigmaBy(const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool ); private: // Save input properties and the squared pT0 scale. bool isInit, useSameAlphaSasMPI; int numberAlphaS; double pT0timesMPI, pT20; // Alpha_strong calculation. AlphaStrong alphaS; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_UserHooks_H pythia8-8.1.80.orig/include/Pythia8/ProcessLevel.h0000644000175000017500000001212312217346230020060 0ustar sunsun// ProcessLevel.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the main class for process-level event generation. // ProcessLevel: administrates the selection of "hard" process. #ifndef Pythia8_ProcessLevel_H #define Pythia8_ProcessLevel_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonDistributions.h" #include "Pythia8/ProcessContainer.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/ResonanceDecays.h" #include "Pythia8/Settings.h" #include "Pythia8/SigmaTotal.h" #include "Pythia8/SusyCouplings.h" #include "Pythia8/SLHAinterface.h" #include "Pythia8/StandardModel.h" #include "Pythia8/UserHooks.h" namespace Pythia8 { //========================================================================== // The ProcessLevel class contains the top-level routines to generate // the characteristic "hard" process of an event. class ProcessLevel { public: // Constructor. ProcessLevel() : iLHACont(-1) {} // Destructor to delete processes in containers. ~ProcessLevel(); // Initialization. bool init( Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, Couplings* couplingsPtrIn, SigmaTotal* sigmaTotPtrIn, bool doLHAin, SLHAinterface* slhaInterfacePtrIn, UserHooks* userHooksPtrIn, vector& sigmaPtrs, ostream& os = cout); // Store or replace Les Houches pointer. void setLHAPtr( LHAup* lhaUpPtrIn) {lhaUpPtr = lhaUpPtrIn; if (iLHACont >= 0) containerPtrs[iLHACont]->setLHAPtr(lhaUpPtr);} // Generate the next "hard" process. bool next( Event& process); // Special case: LHA input of resonance decay only. bool nextLHAdec( Event& process); // Accumulate and update statistics (after possible user veto). void accumulate(); // Print statistics on cross sections and number of events. void statistics(bool reset = false, ostream& os = cout); // Reset statistics. void resetStatistics(); // Add any junctions to the process event record list. void findJunctions( Event& junEvent); // Initialize and call resonance decays separately. void initDecays( Info* infoPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, LHAup* lhaUpPtrIn) { infoPtr = infoPtrIn; resonanceDecays.init( infoPtrIn, particleDataPtrIn, rndmPtrIn); containerLHAdec.setLHAPtr(lhaUpPtrIn, particleDataPtrIn); } bool nextDecays( Event& process) { return resonanceDecays.next( process);} private: // Constants: could only be changed in the code itself. static const int MAXLOOP; // Generic info for process generation. bool doSecondHard, doSameCuts, allHardSame, noneHardSame, someHardSame, cutsAgree, cutsOverlap, doResDecays; int nImpact, startColTag; double mHatMin1, mHatMax1, pTHatMin1, pTHatMax1, mHatMin2, mHatMax2, pTHatMin2, pTHatMax2, sigmaND, sumImpactFac, sum2ImpactFac; // Vector of containers of internally-generated processes. vector containerPtrs; int iContainer, iLHACont; double sigmaMaxSum; // Ditto for optional choice of a second hard process. vector container2Ptrs; int i2Container; double sigma2MaxSum; // Single half-dummy container for LHA input of resonance decay only. ProcessContainer containerLHAdec; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to the two incoming beams. BeamParticle* beamAPtr; BeamParticle* beamBPtr; // Pointer to Standard Model couplings, including alphaS and alphaEM. Couplings* couplingsPtr; // Pointer to SigmaTotal object needed to handle soft QCD processes. SigmaTotal* sigmaTotPtr; // Pointer to SusyLesHouches object for interface to SUSY spectra. SLHAinterface* slhaInterfacePtr; // Pointer to userHooks object for user interaction with program. UserHooks* userHooksPtr; // Pointer to LHAup for generating external events. LHAup* lhaUpPtr; // ResonanceDecay object does sequential resonance decays. ResonanceDecays resonanceDecays; // Generate the next event with one interaction. bool nextOne( Event& process); // Generate the next event with two hard interactions. bool nextTwo( Event& process); // Append the second to the first process list. void combineProcessRecords( Event& process, Event& process2); // Check that colours match up. bool checkColours( Event& process); // Print statistics when two hard processes allowed. void statistics2(bool reset, ostream& os = cout); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_ProcessLevel_H pythia8-8.1.80.orig/include/Pythia8/HadronScatter.h0000644000175000017500000001266012217346227020227 0ustar sunsun// HadronScatter.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. #ifndef Pythia8_HadronScatter_H #define Pythia8_HadronScatter_H #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/PythiaComplex.h" namespace Pythia8 { class SigmaPartialWave { public: // Initialisation bool init(int, string, string, Info *, ParticleData *, Rndm *); // Read data file bool readFile(string, string); // Set the subprocess/incoming particles bool setSubprocess(int); bool setSubprocess(int, int); // Return sigma total/elastic, dSigma/dCos(theta) double sigmaEl(double Wcm) { return sigma(0, Wcm); } double sigmaTot(double Wcm) { return sigma(1, Wcm); } double dSigma(double Wcm, double cTheta) { return sigma(2, Wcm, cTheta); } // Return a cos(theta) value double pickCosTheta(double); // Return maximum sigma elastic double getSigmaElMax() { return sigElMax; } private: // Pointers Info *infoPtr; ParticleData *particleDataPtr; Rndm *rndmPtr; // Constants static const int LSHIFT, ISHIFT, SUBBIN, ITER; static const double CONVERT2MB, WCMBIN, CTBIN, MASSSAFETY, GRIDSAFETY; static const complex BINEND; // Settings int process, subprocess, subprocessMax, norm; // Current incoming and maximum L/I values int idA, idB, Lmax, Imax; // Masses of incoming, last bin, maximum sigma elastic double mA, mB, binMax, sigElMax; // Map subprocess to incoming and vice versa: // sp2in[subprocess] = idA, idB // in2sp[idA, idB] = subprocess map < int, pair < int, int > > sp2in; map < pair < int, int >, int > in2sp; // Isospin coefficients isoCoeff[subprocess][2I] map < int, map < int, double > > isoCoeff; // Storage for partial wave data: // pwData[L * LSHIFT + 2I * ISHIFT + 2J][eNow] = T map < int, map < double, complex > > pwData; // Values of Pl and Pl' as computed by legendreP vector < double > PlVec, PlpVec; // Integration grid [subprocess][WcmBin][cosThetaBin] vector < vector < vector < double > > > gridMax; vector < vector < double > > gridNorm; // Setup subprocesses (including isospin coefficients) void setupSubprocesses(); // Setup grids for integration void setupGrid(); // Routine for calculating sigma total/elastic and dSigma/dCos(theta) double sigma(int, double, double = 0.); // Generate Legendre polynomials (and optionally derivatives) void legendreP(double, bool = false); }; //========================================================================== // HadronScatterPair class // Simple class to hold details of a pair of hadrons which will scatter. // Stores indices in event record and the measure used for ordering // Store a pair of indices typedef pair < int, int > HSIndex; class HadronScatterPair { public: // Constructor HadronScatterPair(const HSIndex &i1in, int yt1in, int pt1in, const HSIndex &i2in, int yt2in, int pt2in, double measureIn) : i1(i1in), yt1(yt1in), pt1(pt1in), i2(i2in), yt2(yt2in), pt2(pt2in), measure(measureIn) {} // Operator for sorting according to ordering measure bool operator<(const HadronScatterPair& in) const { return this->measure < in.measure; } // Indices into event record of hadrons to scatter HSIndex i1; int yt1, pt1; HSIndex i2; int yt2, pt2; // Ordering measure double measure; }; //========================================================================== // HadronScatter class class HadronScatter { public: // Constructor. HadronScatter() {} // Initialisation bool init(Info* infoPtrIn, Settings& settings, Rndm* rndmPtrIn, ParticleData *particleDataPtr); // Perform all hadron scatterings void scatter(Event&); private: // Pointer to various information on the generation. Info* infoPtr; Rndm* rndmPtr; // Settings bool doHadronScatter, afterDecay, allowDecayProd, scatterRepeat, doTile; int hadronSelect, scatterProb; double Npar, kPar, pPar, jPar, rMax, rMax2; double pTsigma, pTsigma2, pT0MPI; // Tiling int ytMax, ptMax; double yMin, yMax, ytSize, ptSize; vector < vector < set < HSIndex > > > tile; // Keep track of scattered pairs set < HSIndex > scattered; // Partial wave amplitudes SigmaPartialWave sigmaPW[3]; // Maximum sigma elastic double sigElMax; // Decide if a hadron can scatter bool canScatter(Event &, int); // Probability for a pair of hadrons to scatter bool doesScatter(Event &, const HSIndex &, const HSIndex &); // Calculate measure for ordering of scatterings double measure(Event &, int, int); // Perform a single hadron scattering bool hadronScatter(Event &, HadronScatterPair &); // Tiling functions bool tileIntProb(vector < HadronScatterPair > &, Event &, const HSIndex &, int, int, bool); int yTile(Event& event, int idx) { return (doTile) ? int((event[idx].y() - yMin) / ytSize) : 0; } int pTile(Event& event, int idx) { return (doTile) ? int((event[idx].phi() + M_PI) / ptSize) : 0; } // Debug void debugOutput(); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_HadronScatter_H pythia8-8.1.80.orig/include/Pythia8/BeamShape.h0000644000175000017500000000354212217346226017311 0ustar sunsun// BeamShape.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header for classes to set beam momentum and interaction vertex spread. #ifndef Pythia8_BeamShape_H #define Pythia8_BeamShape_H #include "Pythia8/Basics.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // Base class to set beam momentum and interaction spot spread. class BeamShape { public: // Constructor. BeamShape() {} // Destructor. virtual ~BeamShape() {} // Initialize beam parameters. virtual void init( Settings& settings, Rndm* rndmPtrIn); // Set the two beam momentum deviations and the beam vertex. virtual void pick(); // Methods to read out the choice made with the above method. Vec4 deltaPA() const {return Vec4( deltaPxA, deltaPyA, deltaPzA, 0);} Vec4 deltaPB() const {return Vec4( deltaPxB, deltaPyB, deltaPzB, 0);} Vec4 vertex() const {return Vec4( vertexX, vertexY, vertexZ, vertexT);} protected: // Values to be set. double deltaPxA, deltaPyA, deltaPzA, deltaPxB, deltaPyB, deltaPzB, vertexX, vertexY, vertexZ, vertexT; // Parameters of Gaussian parametrizations. bool allowMomentumSpread, allowVertexSpread; double sigmaPxA, sigmaPyA, sigmaPzA, maxDevA, sigmaPxB, sigmaPyB, sigmaPzB, maxDevB, sigmaVertexX, sigmaVertexY, sigmaVertexZ, maxDevVertex, sigmaTime, maxDevTime, offsetX, offsetY, offsetZ, offsetT; // Pointer to the random number generator. Rndm* rndmPtr; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_BeamShape_H pythia8-8.1.80.orig/include/Pythia8/Info.h0000644000175000017500000004315212217346227016361 0ustar sunsun// Info.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains a class that keep track of generic event info. // Info: contains information on the generation process and errors. #ifndef Pythia8_Info_H #define Pythia8_Info_H #include "Pythia8/PythiaStdlib.h" namespace Pythia8 { //========================================================================== // The Info class contains a mixed bag of information on the event // generation activity, especially on the current subprocess properties, // and on the number of errors encountered. This is used by the // generation machinery, but can also be read by the user. // Note: some methods that maybe should not be accessible to the user // are still public, to work also for user-written FSR/ISR classes. class Info { public: // Constructor. Info() : eCMSave(0.), lowPTmin(false), a0MPISave(0.), weightCKKWLSave(1.), weightFIRSTSave(0.) { for (int i = 0; i < 40; ++i) counters[i] = 0;} // Listing of most available information on current event. void list(ostream& os = cout) const; // Beam particles (in rest frame). CM energy of event. int idA() const {return idASave;} int idB() const {return idBSave;} double pzA() const {return pzASave;} double pzB() const {return pzBSave;} double eA() const {return eASave;} double eB() const {return eBSave;} double mA() const {return mASave;} double mB() const {return mBSave;} double eCM() const {return eCMSave;} double s() const {return sSave;} // Warnings from initialization. bool tooLowPTmin() const {return lowPTmin;} // Process name and code, and the number of final-state particles. string name() const {return nameSave;} int code() const {return codeSave;} int nFinal() const {return nFinalSave;} // Are beam particles resolved, with pdf's? Are they diffractive? bool isResolved() const {return isRes;} bool isDiffractiveA() const {return isDiffA;} bool isDiffractiveB() const {return isDiffB;} bool isDiffractiveC() const {return isDiffC;} bool isNonDiffractive() const {return isND;} // Retained for backwards compatibility. bool isMinBias() const {return isND;} // Information for Les Houches Accord and reading files. bool isLHA() const {return isLH;} bool atEndOfFile() const {return atEOF;} // For nondiffractive and Les Houches Accord identify hardest subprocess. bool hasSub(int i = 0) const {return hasSubSave[i];} string nameSub(int i = 0) const {return nameSubSave[i];} int codeSub(int i = 0) const {return codeSubSave[i];} int nFinalSub(int i = 0) const {return nFinalSubSave[i];} // Incoming parton flavours and x values. int id1(int i = 0) const {return id1Save[i];} int id2(int i = 0) const {return id2Save[i];} double x1(int i = 0) const {return x1Save[i];} double x2(int i = 0) const {return x2Save[i];} double y(int i = 0) const {return 0.5 * log( x1Save[i] / x2Save[i]);} double tau(int i = 0) const {return x1Save[i] * x2Save[i];} // Hard process flavours, x values, parton densities, couplings, Q2 scales. int id1pdf(int i = 0) const {return id1pdfSave[i];} int id2pdf(int i = 0) const {return id2pdfSave[i];} double x1pdf(int i = 0) const {return x1pdfSave[i];} double x2pdf(int i = 0) const {return x2pdfSave[i];} double pdf1(int i = 0) const {return pdf1Save[i];} double pdf2(int i = 0) const {return pdf2Save[i];} double QFac(int i = 0) const {return sqrtpos(Q2FacSave[i]);} double Q2Fac(int i = 0) const {return Q2FacSave[i];} bool isValence1() const {return isVal1;} bool isValence2() const {return isVal2;} double alphaS(int i = 0) const {return alphaSSave[i];} double alphaEM(int i = 0) const {return alphaEMSave[i];} double QRen(int i = 0) const {return sqrtpos(Q2RenSave[i]);} double Q2Ren(int i = 0) const {return Q2RenSave[i];} double scalup(int i = 0) const {return scalupSave[i];} // Mandelstam variables (notation as if subcollision). double mHat(int i = 0) const {return sqrt(sH[i]);} double sHat(int i = 0) const {return sH[i];} double tHat(int i = 0) const {return tH[i];} double uHat(int i = 0) const {return uH[i];} double pTHat(int i = 0) const {return pTH[i];} double pT2Hat(int i = 0) const {return pTH[i] * pTH[i];} double m3Hat(int i = 0) const {return m3H[i];} double m4Hat(int i = 0) const {return m4H[i];} double thetaHat(int i = 0) const {return thetaH[i];} double phiHat(int i = 0) const {return phiH[i];} // Weight of current event; normally 1, but used for Les Houches events // or when reweighting phase space selection. Conversion from mb to pb // for LHA strategy +-4. Also cumulative sum. double weight() const; double weightSum() const; double lhaStrategy() const {return lhaStrategySave;} // Number of times other steps have been carried out. int nISR() const {return nISRSave;} int nFSRinProc() const {return nFSRinProcSave;} int nFSRinRes() const {return nFSRinResSave;} // Maximum pT scales for MPI, ISR and FSR (in hard process). double pTmaxMPI() const {return pTmaxMPISave;} double pTmaxISR() const {return pTmaxISRSave;} double pTmaxFSR() const {return pTmaxFSRSave;} // Current evolution scale (for UserHooks). double pTnow() const {return pTnowSave;} // Impact parameter picture, global information double a0MPI() const {return a0MPISave;} // Impact parameter picture, as set by hardest interaction. double bMPI() const {return (bIsSet) ? bMPISave : 1.;} double enhanceMPI() const {return (bIsSet) ? enhanceMPISave : 1.;} double eMPI(int i) const {return (bIsSet) ? eMPISave[i] : 1.;} // Number of multiparton interactions, with code and pT for them. int nMPI() const {return nMPISave;} int codeMPI(int i) const {return codeMPISave[i];} double pTMPI(int i) const {return pTMPISave[i];} int iAMPI(int i) const {return iAMPISave[i];} int iBMPI(int i) const {return iBMPISave[i];} // Cross section estimate. long nTried(int i = 0) {return (i == 0) ? nTry : nTryM[i];} long nSelected(int i = 0) {return (i == 0) ? nSel : nSelM[i];} long nAccepted(int i = 0) {return (i == 0) ? nAcc : nAccM[i];} double sigmaGen(int i = 0) {return (i == 0) ? sigGen : sigGenM[i];} double sigmaErr(int i = 0) {return (i == 0) ? sigErr : sigErrM[i];} // Counters for number of loops in various places. int getCounter( int i) const {return counters[i];} // Set or increase the value stored in a counter. void setCounter( int i, int value = 0) {counters[i] = value;} void addCounter( int i, int value = 1) {counters[i] += value;} // Reset to empty map of error messages. void errorReset() {messages.clear();} // Print a message the first few times. Insert in database. void errorMsg(string messageIn, string extraIn = " ", bool showAlways = false, ostream& os = cout); // Provide total number of errors/aborts/warnings experienced to date. int errorTotalNumber(); // Print statistics on errors/aborts/warnings. void errorStatistics(ostream& os = cout); // Set initialization warning flag when too low pTmin in ISR/FSR/MPI. void setTooLowPTmin(bool lowPTminIn) {lowPTmin = lowPTminIn;} // Set info on valence character of hard collision partons. void setValence( bool isVal1In, bool isVal2In) {isVal1 = isVal1In; isVal2 = isVal2In;} // Set and get some MPI/ISR/FSR properties needed for matching, // i.e. mainly of internal relevance. void hasHistory( bool hasHistoryIn) {hasHistorySave = hasHistoryIn;} bool hasHistory() {return hasHistorySave;} void zNowISR( double zNowIn) {zNowISRSave = zNowIn;} double zNowISR() {return zNowISRSave;} void pT2NowISR( double pT2NowIn) {pT2NowISRSave = pT2NowIn;} double pT2NowISR() {return pT2NowISRSave;} // Return CKKW-L weight. double getWeightCKKWL() const { return weightCKKWLSave;} // Set CKKW-L weight. void setWeightCKKWL( double weightIn) { weightCKKWLSave = weightIn;} // Return merging weight. double mergingWeight() const { return weightCKKWLSave;} // Return the complete NLO weight. double mergingWeightNLO() const { return (weightCKKWLSave - weightFIRSTSave); } // Return the O(\alpha_s)-term of the CKKW-L weight. double getWeightFIRST() const { return weightFIRSTSave;} // Set the O(\alpha_s)-term of the CKKW-L weight. void setWeightFIRST( double weightIn) { weightFIRSTSave = weightIn;} // Return an LHEF header string header(const string &key) { if (headers.find(key) == headers.end()) return ""; else return headers[key]; } // Return a list of all header key names vector < string > headerKeys() { vector < string > keys; for (map < string, string >::iterator it = headers.begin(); it != headers.end(); it++) keys.push_back(it->first); return keys; } private: // Number of times the same error message is repeated, unless overridden. static const int TIMESTOPRINT; // Allow conversion from mb to pb. static const double CONVERTMB2PB; // Store common beam quantities. int idASave, idBSave; double pzASave, eASave,mASave, pzBSave, eBSave, mBSave, eCMSave, sSave; // Store initialization information. bool lowPTmin; // Store common integrated cross section quantities. long nTry, nSel, nAcc; double sigGen, sigErr, wtAccSum; map nTryM, nSelM, nAccM; map sigGenM, sigErrM; int lhaStrategySave; // Store common MPI information. double a0MPISave; // Store current-event quantities. bool isRes, isDiffA, isDiffB, isDiffC, isND, isLH, hasSubSave[4], bIsSet, evolIsSet, atEOF, isVal1, isVal2, hasHistorySave; int codeSave, codeSubSave[4], nFinalSave, nFinalSubSave[4], nTotal, id1Save[4], id2Save[4], id1pdfSave[4], id2pdfSave[4], nMPISave, nISRSave, nFSRinProcSave, nFSRinResSave; double x1Save[4], x2Save[4], x1pdfSave[4], x2pdfSave[4], pdf1Save[4], pdf2Save[4], Q2FacSave[4], alphaEMSave[4], alphaSSave[4], Q2RenSave[4], scalupSave[4], sH[4], tH[4], uH[4], pTH[4], m3H[4], m4H[4], thetaH[4], phiH[4], weightSave, bMPISave, enhanceMPISave, pTmaxMPISave, pTmaxISRSave, pTmaxFSRSave, pTnowSave, zNowISRSave, pT2NowISRSave; string nameSave, nameSubSave[4]; vector codeMPISave, iAMPISave, iBMPISave; vector pTMPISave, eMPISave; // Vector of various loop counters. int counters[50]; // Map for all error messages. map messages; // Map for LHEF headers map headers; // Friend classes allowed to set info. friend class Pythia; friend class ProcessLevel; friend class ProcessContainer; friend class PartonLevel; friend class MultipartonInteractions; friend class LHAup; // Set info on the two incoming beams: only from Pythia class. void setBeamA( int idAin, double pzAin, double eAin, double mAin) { idASave = idAin; pzASave = pzAin; eASave = eAin; mASave = mAin;} void setBeamB( int idBin, double pzBin, double eBin, double mBin) { idBSave = idBin; pzBSave = pzBin; eBSave = eBin; mBSave = mBin;} void setECM( double eCMin) {eCMSave = eCMin; sSave = eCMSave * eCMSave;} // Reset info for current event: only from Pythia class. void clear() { isRes = isDiffA = isDiffB = isDiffC = isND = isLH = bIsSet = evolIsSet = atEOF = isVal1 = isVal2 = hasHistorySave = false; codeSave = nFinalSave = nTotal = nMPISave = nISRSave = nFSRinProcSave = nFSRinResSave = 0; weightSave = bMPISave = enhanceMPISave = weightCKKWLSave = 1.; pTmaxMPISave = pTmaxISRSave = pTmaxFSRSave = pTnowSave = zNowISRSave = pT2NowISRSave = weightFIRSTSave = 0.; nameSave = " "; for (int i = 0; i < 4; ++i) { hasSubSave[i] = false; codeSubSave[i] = nFinalSubSave[i] = id1pdfSave[i] = id2pdfSave[i] = id1Save[i] = id2Save[i] = 0; x1pdfSave[i] = x2pdfSave[i] = pdf1Save[i] = pdf2Save[i] = Q2FacSave[i] = alphaEMSave[i] = alphaSSave[i] = Q2RenSave[i] = scalupSave[i] = x1Save[i] = x2Save[i] = sH[i] = tH[i] = uH[i] = pTH[i] = m3H[i] = m4H[i] = thetaH[i] = phiH[i] = 0.; nameSubSave[i] = " "; } codeMPISave.resize(0); iAMPISave.resize(0); iBMPISave.resize(0); pTMPISave.resize(0); eMPISave.resize(0); } // Reset info arrays only for parton and hadron level. int sizeMPIarrays() const { return codeMPISave.size(); } void resizeMPIarrays(int newSize) { codeMPISave.resize(newSize); iAMPISave.resize(newSize); iBMPISave.resize(newSize); pTMPISave.resize(newSize); eMPISave.resize(newSize); } // Set info on the (sub)process: from ProcessLevel, ProcessContainer or // MultipartonInteractions classes. void setType( string nameIn, int codeIn, int nFinalIn, bool isNonDiffIn = false, bool isResolvedIn = true, bool isDiffractiveAin = false, bool isDiffractiveBin = false, bool isDiffractiveCin = false, bool isLHAin = false) { nameSave = nameIn; codeSave = codeIn; nFinalSave = nFinalIn; isND = isNonDiffIn; isRes = isResolvedIn; isDiffA = isDiffractiveAin; isDiffB = isDiffractiveBin; isDiffC = isDiffractiveCin; isLH = isLHAin; nTotal = 2 + nFinalSave; bIsSet = false; hasSubSave[0] = false; nameSubSave[0] = " "; codeSubSave[0] = 0; nFinalSubSave[0] = 0; evolIsSet = false;} void setSubType( int iDS, string nameSubIn, int codeSubIn, int nFinalSubIn) { hasSubSave[iDS] = true; nameSubSave[iDS] = nameSubIn; codeSubSave[iDS] = codeSubIn; nFinalSubSave[iDS] = nFinalSubIn;} void setPDFalpha( int iDS, int id1pdfIn, int id2pdfIn, double x1pdfIn, double x2pdfIn, double pdf1In, double pdf2In, double Q2FacIn, double alphaEMIn, double alphaSIn, double Q2RenIn, double scalupIn) { id1pdfSave[iDS] = id1pdfIn; id2pdfSave[iDS] = id2pdfIn; x1pdfSave[iDS] = x1pdfIn; x2pdfSave[iDS] = x2pdfIn; pdf1Save[iDS] = pdf1In; pdf2Save[iDS] = pdf2In; Q2FacSave[iDS] = Q2FacIn; alphaEMSave[iDS] = alphaEMIn; alphaSSave[iDS] = alphaSIn; Q2RenSave[iDS] = Q2RenIn; scalupSave[iDS] = scalupIn;} void setKin( int iDS, int id1In, int id2In, double x1In, double x2In, double sHatIn, double tHatIn, double uHatIn, double pTHatIn, double m3HatIn, double m4HatIn, double thetaHatIn, double phiHatIn) { id1Save[iDS] = id1In; id2Save[iDS] = id2In; x1Save[iDS] = x1In; x2Save[iDS] = x2In; sH[iDS] = sHatIn; tH[iDS] = tHatIn; uH[iDS] = uHatIn; pTH[iDS] = pTHatIn; m3H[iDS] = m3HatIn; m4H[iDS] = m4HatIn; thetaH[iDS] = thetaHatIn; phiH[iDS] = phiHatIn;} void setTypeMPI( int codeMPIIn, double pTMPIIn, int iAMPIIn = 0, int iBMPIIn = 0, double eMPIIn = 1.) {codeMPISave.push_back(codeMPIIn); pTMPISave.push_back(pTMPIIn); iAMPISave.push_back(iAMPIIn); iBMPISave.push_back(iBMPIIn); eMPISave.push_back(eMPIIn); } // Set info on cross section: from ProcessLevel (reset in Pythia). void sigmaReset() { nTry = nSel = nAcc = 0; sigGen = sigErr = wtAccSum = 0.; nTryM.clear(); nSelM.clear(); nAccM.clear(); sigGenM.clear(); sigErrM.clear();} void setSigma( int i, long nTryIn, long nSelIn, long nAccIn, double sigGenIn, double sigErrIn, double wtAccSumIn) { if (i == 0) {nTry = nTryIn; nSel = nSelIn; nAcc = nAccIn; sigGen = sigGenIn; sigErr = sigErrIn; wtAccSum = wtAccSumIn;} else { nTryM[i] = nTryIn; nSelM[i] = nSelIn; nAccM[i] = nAccIn; sigGenM[i] = sigGenIn; sigErrM[i] = sigErrIn;} } // Set info on impact parameter: from PartonLevel. void setImpact( double bMPIIn, double enhanceMPIIn, bool bIsSetIn = true) { bMPISave = bMPIIn; enhanceMPISave = eMPISave[0] = enhanceMPIIn, bIsSet = bIsSetIn;} // Set info on pTmax scales and number of evolution steps: from PartonLevel. void setPartEvolved( int nMPIIn, int nISRIn) { nMPISave = nMPIIn; nISRSave = nISRIn;} void setEvolution( double pTmaxMPIIn, double pTmaxISRIn, double pTmaxFSRIn, int nMPIIn, int nISRIn, int nFSRinProcIn, int nFSRinResIn) { pTmaxMPISave = pTmaxMPIIn; pTmaxISRSave = pTmaxISRIn; pTmaxFSRSave = pTmaxFSRIn; nMPISave = nMPIIn; nISRSave = nISRIn; nFSRinProcSave = nFSRinProcIn; nFSRinResSave = nFSRinResIn; evolIsSet = true;} // Set current pT evolution scale for MPI/ISR/FSR; from PartonLevel. void setPTnow( double pTnowIn) {pTnowSave = pTnowIn;} // Set a0 from MultipartonInteractions. void seta0MPI(double a0MPIin) {a0MPISave = a0MPIin;} // Set info whether reading of Les Houches Accord file at end. void setEndOfFile( bool atEOFin) {atEOF = atEOFin;} // Set event weight; currently only for Les Houches description. void setWeight( double weightIn, int lhaStrategyIn) { weightSave = weightIn; lhaStrategySave = lhaStrategyIn; } // Save merging weight (i.e. CKKW-L-type weight, summed O(\alpha_s) weight) double weightCKKWLSave, weightFIRSTSave; // Set LHEF headers void setHeader(const string &key, const string &val) { headers[key] = val; } }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_Info_H pythia8-8.1.80.orig/include/Pythia8/SigmaLeptoquark.h0000644000175000017500000001123512217346231020566 0ustar sunsun// SigmaLeptoquark.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for leptoquark-process differential cross sections. // Contains classes derived from SigmaProcess via Sigma(1/2)Process. // Note: since leptoquark assumed scalar no need for decay-angles routines. #ifndef Pythia8_SigmaLeptoquark_H #define Pythia8_SigmaLeptoquark_H #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // A derived class for q l -> LQ (leptoquark). class Sigma1ql2LeptoQuark : public Sigma1Process { public: // Constructor. Sigma1ql2LeptoQuark() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q l -> LQ (leptoquark)";} virtual int code() const {return 3201;} virtual string inFlux() const {return "ff";} virtual int resonanceA() const {return 42;} private: // Parameters set at initialization or for current kinematics. int idQuark, idLepton; double mRes, GammaRes, m2Res, GamMRat, kCoup, widthIn, sigBW; // Pointer to properties of the particle species, to access decay channel. ParticleDataEntry* LQPtr; }; //========================================================================== // A derived class for q g -> LQ l (leptoquark). class Sigma2qg2LeptoQuarkl : public Sigma2Process { public: // Constructor. Sigma2qg2LeptoQuarkl() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q g -> LQ l (leptoquark)";} virtual int code() const {return 3202;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return 42;} private: // Parameters set at initialization or for current kinematics. int idQuark, idLepton; double mRes, GammaRes, m2Res, GamMRat, kCoup, openFracPos, openFracNeg, sigma0; }; //========================================================================== // A derived class for g g -> LQ LQbar (leptoquark). class Sigma2gg2LQLQbar : public Sigma2Process { public: // Constructor. Sigma2gg2LQLQbar() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "g g -> LQ LQbar (leptoquark)";} virtual int code() const {return 3203;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return 42;} virtual int id4Mass() const {return 42;} private: // Parameters set at initialization or for current kinematics. double mRes, GammaRes, m2Res, GamMRat, openFrac, sigma; }; //========================================================================== // A derived class for q qbar -> LQ LQbar (leptoquark). class Sigma2qqbar2LQLQbar : public Sigma2Process { public: // Constructor. Sigma2qqbar2LQLQbar() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() { return (abs(id1) == idQuark) ? sigmaSame : sigmaDiff;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> LQ LQbar (leptoquark)";} virtual int code() const {return 3204;} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return 42;} virtual int id4Mass() const {return 42;} private: // Parameters set at initialization or for current kinematics. int idQuark; double mRes, GammaRes, m2Res, GamMRat, kCoup, openFrac, sigmaDiff, sigmaSame; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaLeptoquark_H pythia8-8.1.80.orig/include/Pythia8/SigmaProcess.h0000644000175000017500000005475312217346231020071 0ustar sunsun// SigmaProcess.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for hard-process differential cross sections. // SigmaProcess: base class for cross sections. // Sigma0Process: base class for unresolved processes, derived from above. // Sigma1Process: base class for 2 -> 1 processes, derived from above. // Sigma2Process: base class for 2 -> 2 processes, derived from above. // Sigma3Process: base class for 2 -> 3 processes, derived from above. // SigmaLHAProcess: wrapper class for Les Houches Accord external input. // Actual physics processes are found in separate files: // SigmaQCD for QCD processes; // SigmaEW for electroweak processes (including photon production); // SigmaOnia for charmonium and bottomonium processes; // SigmaHiggs for Higgs processes; // SigmaSUSY for supersymmetric production; // SigmaLeftRightSym for processes in left-right-symmetric scenarios; // SigmaLeptoquark for leptoquark production. // SigmaExtraDim for processes in scenarios for extra dimensions; // SigmaGeneric for generic scalar/fermion/vector pair production. #ifndef Pythia8_SigmaProcess_H #define Pythia8_SigmaProcess_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/LesHouches.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonDistributions.h" #include "Pythia8/PythiaComplex.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/ResonanceWidths.h" #include "Pythia8/Settings.h" #include "Pythia8/SigmaTotal.h" #include "Pythia8/StandardModel.h" #include "Pythia8/SLHAinterface.h" #include "Pythia8/SusyLesHouches.h" namespace Pythia8 { //========================================================================== // InBeam is a simple helper class for partons and their flux in a beam. class InBeam { public: // Constructor. InBeam( int idIn = 0) : id(idIn), pdf(0.) {} // Values. int id; double pdf; }; //========================================================================== // InPair is a simple helper class for colliding parton pairs and their flux. class InPair { public: // Constructor. InPair( int idAIn = 0, int idBIn = 0) : idA(idAIn), idB(idBIn), pdfA(0.), pdfB(0.), pdfSigma(0.) {} // Values. int idA, idB; double pdfA, pdfB, pdfSigma; }; //========================================================================== // SigmaProcess is the base class for cross section calculations. class SigmaProcess { public: // Destructor. virtual ~SigmaProcess() {} // Perform simple initialization and store pointers. void init(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, Couplings* couplings, SigmaTotal* sigmaTotPtrIn = 0, SLHAinterface* slhaInterfacePtrIn = 0); // Store or replace Les Houches pointer. void setLHAPtr( LHAup* lhaUpPtrIn) {lhaUpPtr = lhaUpPtrIn;} // Initialize process. Only used for some processes. virtual void initProc() {} // Set up allowed flux of incoming partons. Default is no flux. virtual bool initFlux(); // Input and complement kinematics for resolved 2 -> 1 process. // Usage: set1Kin( x1in, x2in, sHin). virtual void set1Kin( double , double , double ) {} // Input and complement kinematics for resolved 2 -> 2 process. // Usage: set2Kin( x1in, x2in, sHin, tHin, m3in, m4in, runBW3in, runBW4in). virtual void set2Kin( double , double , double , double , double , double, double, double ) {} // Ditto, but for Multiparton Interactions applications, so different input. // Usage: set2KinMPI( x1in, x2in, sHin, tHin, uHin, // alpSin, alpEMin, needMasses, m3in, m4in) virtual void set2KinMPI( double , double , double , double , double , double , double , bool , double , double ) {} // Input and complement kinematics for resolved 2 -> 3 process. // Usage: set3Kin( x1in, x2in, sHin, p3prel, p4prel, p5prel, // m3in, m4in, m5in, runBW3in, runBW4in, runBW5in); virtual void set3Kin( double , double , double , Vec4 , Vec4 , Vec4 , double , double , double , double , double , double ) {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin() {} // Evaluate sigma for unresolved, sigmaHat(sHat) for 2 -> 1 processes, // d(sigmaHat)/d(tHat) for (resolved) 2 -> 2 processes, and |M|^2 for // 2 -> 3 processes. Answer in "native" units, either mb or GeV^-2. virtual double sigmaHat() {return 0.;} // Wrapper to sigmaHat, to (a) store current incoming flavours and // (b) convert from GeV^-2 to mb where required. // For 2 -> 1/2 also (c) convert from from |M|^2 to d(sigmaHat)/d(tHat). virtual double sigmaHatWrap(int id1in = 0, int id2in = 0) { id1 = id1in; id2 = id2in; return ( convert2mb() ? CONVERT2MB * sigmaHat() : sigmaHat() ); } // Convolute above with parton flux and K factor. Sum over open channels. virtual double sigmaPDF(); // Select incoming parton channel and extract parton densities (resolved). void pickInState(int id1in = 0, int id2in = 0); // Select flavour, colour and anticolour. virtual void setIdColAcol() {} // Perform kinematics for a Multiparton Interaction, in its rest frame. virtual bool final2KinMPI( int = 0, int = 0, Vec4 = 0., Vec4 = 0., double = 0., double = 0.) {return true;} // Evaluate weight for simultaneous flavours (only gamma*/Z0 gamma*/Z0). // Usage: weightDecayFlav( process). virtual double weightDecayFlav( Event&) {return 1.;} // Evaluate weight for decay angular configuration. // Usage: weightDecay( process, iResBeg, iResEnd), where // iResBeg <= i < iResEnd is range of sister partons to test decays of. virtual double weightDecay( Event&, int, int) {return 1.;} // Set scale, when that is missing for an external LHA process. virtual void setScale() {} // Process name and code, and the number of final-state particles. virtual string name() const {return "unnamed process";} virtual int code() const {return 0;} virtual int nFinal() const {return 2;} // Need to know which incoming partons to set up interaction for. virtual string inFlux() const {return "unknown";} // Need to know whether to convert cross section answer from GeV^-2 to mb. virtual bool convert2mb() const {return true;} // For 2 -> 2 process optional conversion from |M|^2 to d(sigmaHat)/d(tHat). virtual bool convertM2() const {return false;} // Special treatment needed for Les Houches processes. virtual bool isLHA() const {return false;} // Special treatment needed for elastic and diffractive processes. virtual bool isNonDiff() const {return false;} virtual bool isResolved() const {return true;} virtual bool isDiffA() const {return false;} virtual bool isDiffB() const {return false;} virtual bool isDiffC() const {return false;} // Special treatment needed for SUSY processes. virtual bool isSUSY() const {return false;} // Special treatment needed if negative cross sections allowed. virtual bool allowNegativeSigma() const {return false;} // Flavours in 2 -> 2/3 processes where masses needed from beginning. // (For a light quark masses will be used in the final kinematics, // but not at the matrix-element level. For a gluon no masses at all.) virtual int id3Mass() const {return 0;} virtual int id4Mass() const {return 0;} virtual int id5Mass() const {return 0;} // Special treatment needed if process contains an s-channel resonance. virtual int resonanceA() const {return 0;} virtual int resonanceB() const {return 0;} // 2 -> 2 and 2 -> 3 processes only through s-channel exchange. virtual bool isSChannel() const {return false;} // NOAM: Insert an intermediate resonance in 2 -> 1 -> 2 (or 3) listings. virtual int idSChannel() const {return 0;} // QCD 2 -> 3 processes need special phase space selection machinery. virtual bool isQCD3body() const {return false;} // Special treatment in 2 -> 3 with two massive propagators. virtual int idTchan1() const {return 0;} virtual int idTchan2() const {return 0;} virtual double tChanFracPow1() const {return 0.3;} virtual double tChanFracPow2() const {return 0.3;} virtual bool useMirrorWeight() const {return false;} // Special process-specific gamma*/Z0 choice if >=0 (e.g. f fbar -> H0 Z0). virtual int gmZmode() const {return -1;} // Tell whether tHat and uHat are swapped (= same as swap 3 and 4). bool swappedTU() const {return swapTU;} // Give back particle properties: flavours, colours, masses, or all. int id(int i) const {return idSave[i];} int col(int i) const {return colSave[i];} int acol(int i) const {return acolSave[i];} double m(int i) const {return mSave[i];} Particle getParton(int i) const {return parton[i];} // Give back couplings and parton densities. Not all known for nondiffractive. double Q2Ren() const {return Q2RenSave;} double alphaEMRen() const {return alpEM;} double alphaSRen() const {return alpS;} double Q2Fac() const {return Q2FacSave;} double pdf1() const {return pdf1Save;} double pdf2() const {return pdf2Save;} // Give back angles; relevant only for multipe-interactions processes. double thetaMPI() const {return atan2( sinTheta, cosTheta);} double phiMPI() const {return phi;} double sHBetaMPI() const {return sHBeta;} double pT2MPI() const {return pT2Mass;} double pTMPIFin() const {return pTFin;} // Save and load kinematics for trial interactions void saveKin() { for (int i = 0; i < 6; i++) { partonT[i] = parton[i]; mSaveT[i] = mSave[i]; } pTFinT = pTFin; phiT = phi; cosThetaT = cosTheta; sinThetaT = sinTheta; } void loadKin() { for (int i = 0; i < 6; i++) { parton[i] = partonT[i]; mSave[i] = mSaveT[i]; } pTFin = pTFinT; cosTheta = cosThetaT; sinTheta = sinThetaT; phi = phiT; } void swapKin() { for (int i = 0; i < 6; i++) { swap(parton[i], partonT[i]); swap(mSave[i], mSaveT[i]); } swap(pTFin, pTFinT); swap(cosTheta, cosThetaT); swap(sinTheta, sinThetaT); swap(phi, phiT); } protected: // Constructor. SigmaProcess() : infoPtr(0), settingsPtr(0), particleDataPtr(0), rndmPtr(0), beamAPtr(0), beamBPtr(0), couplingsPtr(0), sigmaTotPtr(0), slhaPtr(0), lhaUpPtr(0) {for (int i = 0; i < 6; ++i) mSave[i] = 0.;} // Constants: could only be changed in the code itself. static const double CONVERT2MB, MASSMARGIN, COMPRELERR; static const int NCOMPSTEP; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the settings database. Settings* settingsPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to incoming beams. BeamParticle* beamAPtr; BeamParticle* beamBPtr; // Pointer to Standard Model couplings, including alphaS and alphaEM. Couplings* couplingsPtr; // Pointer to the total/elastic/diffractive cross section object. SigmaTotal* sigmaTotPtr; // Pointer to an SLHA object. SusyLesHouches* slhaPtr; // Pointer to LHAup for generating external events. LHAup* lhaUpPtr; // Initialization data, normally only set once. int nQuarkIn, renormScale1, renormScale2, renormScale3, renormScale3VV, factorScale1, factorScale2, factorScale3, factorScale3VV; double Kfactor, mcME, mbME, mmuME, mtauME, renormMultFac, renormFixScale, factorMultFac, factorFixScale; // CP violation parameters for Higgs sector, normally only set once. int higgsH1parity, higgsH2parity, higgsA3parity; double higgsH1eta, higgsH2eta, higgsA3eta; // Information on incoming beams. int idA, idB; double mA, mB; bool isLeptonA, isLeptonB, hasLeptonBeams; // Partons in beams, with PDF's. vector inBeamA; vector inBeamB; void addBeamA(int idIn) {inBeamA.push_back(InBeam(idIn));} void addBeamB(int idIn) {inBeamB.push_back(InBeam(idIn));} int sizeBeamA() const {return inBeamA.size();} int sizeBeamB() const {return inBeamB.size();} // Allowed colliding parton pairs, with pdf's. vector inPair; void addPair(int idAIn, int idBIn) { inPair.push_back(InPair(idAIn, idBIn));} int sizePair() const {return inPair.size();} // Store common subprocess kinematics quantities. double mH, sH, sH2; // Store Q2 renormalization and factorization scales, and related values. double Q2RenSave, alpEM, alpS, Q2FacSave, x1Save, x2Save, pdf1Save, pdf2Save, sigmaSumSave; // Store flavour, colour, anticolour, mass, angles and the whole particle. int id1, id2, id3, id4, id5; int idSave[6], colSave[6], acolSave[6]; double mSave[6], cosTheta, sinTheta, phi, sHMass, sHBeta, pT2Mass, pTFin; Particle parton[6]; // Minimal set of saved kinematics for trial interactions when // using the x-dependent matter profile of multiparton interactions. Particle partonT[6]; double mSaveT[6], pTFinT, cosThetaT, sinThetaT, phiT; // Calculate and store all modified masses and four-vectors // intended for matrix elements. Return false if failed. virtual bool setupForME() {return true;} bool setupForMEin(); double mME[5]; Vec4 pME[5]; // Store whether tHat and uHat are swapped (= same as swap 3 and 4). bool swapTU; // Set flavour, colour and anticolour. void setId( int id1in = 0, int id2in = 0, int id3in = 0, int id4in = 0, int id5in = 0) {idSave[1] = id1in; idSave[2] = id2in; idSave[3] = id3in; idSave[4] = id4in; idSave[5] = id5in;} void setColAcol( int col1 = 0, int acol1 = 0, int col2 = 0, int acol2 = 0, int col3 = 0, int acol3 = 0, int col4 = 0, int acol4 = 0, int col5 = 0, int acol5 = 0) { colSave[1] = col1; acolSave[1] = acol1; colSave[2] = col2; acolSave[2] = acol2; colSave[3] = col3; acolSave[3] = acol3; colSave[4] = col4; acolSave[4] = acol4; colSave[5] = col5; acolSave[5] = acol5; } void swapColAcol() { swap(colSave[1], acolSave[1]); swap(colSave[2], acolSave[2]); swap(colSave[3], acolSave[3]); swap(colSave[4], acolSave[4]); swap(colSave[5], acolSave[5]);} void swapCol1234() { swap(colSave[1], colSave[2]); swap(colSave[3], colSave[4]); swap(acolSave[1], acolSave[2]); swap(acolSave[3], acolSave[4]);} void swapCol12() { swap(colSave[1], colSave[2]); swap(acolSave[1], acolSave[2]);} void swapCol34() { swap(colSave[3], colSave[4]); swap(acolSave[3], acolSave[4]);} // Common code for top and Higgs secondary decay angular weights. double weightTopDecay( Event& process, int iResBeg, int iResEnd); double weightHiggsDecay( Event& process, int iResBeg, int iResEnd); }; //========================================================================== // Sigma0Process is the base class for unresolved and minimum-bias processes. // It is derived from SigmaProcess. class Sigma0Process : public SigmaProcess { public: // Destructor. virtual ~Sigma0Process() {} // Number of final-state particles. virtual int nFinal() const {return 2;}; // No partonic flux to be set up. virtual bool initFlux() {return true;} // Evaluate sigma for unresolved processes. virtual double sigmaHat() {return 0.;} // Since no PDF's there is no difference from above. virtual double sigmaPDF() {return sigmaHat();} // Answer for these processes already in mb, so do not convert. virtual bool convert2mb() const {return false;} protected: // Constructor. Sigma0Process() {} }; //========================================================================== // Sigma1Process is the base class for 2 -> 1 processes. // It is derived from SigmaProcess. class Sigma1Process : public SigmaProcess { public: // Destructor. virtual ~Sigma1Process() {} // Number of final-state particles. virtual int nFinal() const {return 1;}; // Input and complement kinematics for resolved 2 -> 1 process. virtual void set1Kin( double x1in, double x2in, double sHin) { store1Kin( x1in, x2in, sHin); sigmaKin();} // Evaluate sigmaHat(sHat) for resolved 2 -> 1 processes. virtual double sigmaHat() {return 0.;} // Wrapper to sigmaHat, to (a) store current incoming flavours, // (b) convert from GeV^-2 to mb where required, and // (c) convert from |M|^2 to d(sigmaHat)/d(tHat) where required. virtual double sigmaHatWrap(int id1in = 0, int id2in = 0); protected: // Constructor. Sigma1Process() {} // Store kinematics and set scales for resolved 2 -> 1 process. virtual void store1Kin( double x1in, double x2in, double sHin); // Calculate modified masses and four-vectors for matrix elements. virtual bool setupForME(); }; //========================================================================== // Sigma2Process is the base class for 2 -> 2 processes. // It is derived from SigmaProcess. class Sigma2Process : public SigmaProcess { public: // Destructor. virtual ~Sigma2Process() {} // Number of final-state particles. virtual int nFinal() const {return 2;}; // Input and complement kinematics for resolved 2 -> 2 process. virtual void set2Kin( double x1in, double x2in, double sHin, double tHin, double m3in, double m4in, double runBW3in, double runBW4in) { store2Kin( x1in, x2in, sHin, tHin, m3in, m4in, runBW3in, runBW4in); sigmaKin();} // Ditto, but for Multiparton Interactions applications, so different input. virtual void set2KinMPI( double x1in, double x2in, double sHin, double tHin, double uHin, double alpSin, double alpEMin, bool needMasses, double m3in, double m4in) { store2KinMPI( x1in, x2in, sHin, tHin, uHin, alpSin, alpEMin, needMasses, m3in, m4in); sigmaKin();} // Evaluate d(sigmaHat)/d(tHat) for resolved 2 -> 2 processes. virtual double sigmaHat() {return 0.;} // Wrapper to sigmaHat, to (a) store current incoming flavours, // (b) convert from GeV^-2 to mb where required, and // (c) convert from |M|^2 to d(sigmaHat)/d(tHat) where required. virtual double sigmaHatWrap(int id1in = 0, int id2in = 0) { id1 = id1in; id2 = id2in; double sigmaTmp = sigmaHat(); if (convertM2()) sigmaTmp /= 16. * M_PI * sH2; if (convert2mb()) sigmaTmp *= CONVERT2MB; return sigmaTmp;} // Perform kinematics for a Multiparton Interaction, in its rest frame. virtual bool final2KinMPI( int i1Res = 0, int i2Res = 0, Vec4 p1Res = 0., Vec4 p2Res = 0., double m1Res = 0., double m2Res = 0.); protected: // Constructor. Sigma2Process() : tH(0.), uH(0.), tH2(0.), uH2(0.), m3(0.), s3(0.), m4(0.), s4(0.), pT2(0.), runBW3(0.), runBW4(0.) {} // Store kinematics and set scales for resolved 2 -> 2 process. virtual void store2Kin( double x1in, double x2in, double sHin, double tHin, double m3in, double m4in, double runBW3in, double runBW4in); virtual void store2KinMPI( double x1in, double x2in, double sHin, double tHin, double uHin, double alpSin, double alpEMin, bool needMasses, double m3in, double m4in); // Calculate modified masses and four-vectors for matrix elements. virtual bool setupForME(); // Store subprocess kinematics quantities. double tH, uH, tH2, uH2, m3, s3, m4, s4, pT2, runBW3, runBW4; }; //========================================================================== // Sigma3Process is the base class for 2 -> 3 processes. // It is derived from SigmaProcess. class Sigma3Process : public SigmaProcess { public: // Destructor. virtual ~Sigma3Process() {} // Number of final-state particles. virtual int nFinal() const {return 3;}; // Input and complement kinematics for resolved 2 -> 3 process. virtual void set3Kin( double x1in, double x2in, double sHin, Vec4 p3cmIn, Vec4 p4cmIn, Vec4 p5cmIn, double m3in, double m4in, double m5in, double runBW3in, double runBW4in, double runBW5in) { store3Kin( x1in, x2in, sHin, p3cmIn, p4cmIn, p5cmIn, m3in, m4in, m5in, runBW3in, runBW4in, runBW5in); sigmaKin();} // Evaluate d(sigmaHat)/d(tHat) for resolved 2 -> 3 processes. virtual double sigmaHat() {return 0.;} protected: // Constructor. Sigma3Process() {} // Store kinematics and set scales for resolved 2 -> 3 process. virtual void store3Kin( double x1in, double x2in, double sHin, Vec4 p3cmIn, Vec4 p4cmIn, Vec4 p5cmIn, double m3in, double m4in, double m5in, double runBW3in, double runBW4in, double runBW5in); // Calculate modified masses and four-vectors for matrix elements. virtual bool setupForME(); // Store subprocess kinematics quantities. double m3, s3, m4, s4, m5, s5, runBW3, runBW4, runBW5; Vec4 p3cm, p4cm, p5cm; }; //========================================================================== // SigmaLHAProcess is a wrapper class for Les Houches Accord external input. // It is derived from SigmaProcess. class SigmaLHAProcess : public SigmaProcess { public: // Constructor. SigmaLHAProcess() {} // Destructor. virtual ~SigmaLHAProcess() {} // No partonic flux to be set up. virtual bool initFlux() {return true;} // Dummy function: action is put in PhaseSpaceLHA. virtual double sigmaPDF() {return 1.;} // Evaluate weight for decay angular configuration, where relevant. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Set scale, when that is missing for an external LHA process. virtual void setScale(); // Info on the subprocess. virtual string name() const {return "Les Houches User Process(es)";} virtual int code() const {return 9999;} // Number of final-state particles depends on current process choice. virtual int nFinal() const; // Answer for these processes not in GeV^-2, so do not do this conversion. virtual bool convert2mb() const {return false;} // Ensure special treatment of Les Houches processes. virtual bool isLHA() const {return true;} // Special treatment needed if negative cross sections allowed. virtual bool allowNegativeSigma() const { return (lhaUpPtr->strategy() < 0);} private: }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaProcess_H pythia8-8.1.80.orig/include/Pythia8/SigmaEW.h0000644000175000017500000006452312217346231016762 0ustar sunsun// SigmaEW.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for electroweak process differential cross sections. // Contains classes derived from SigmaProcess via Sigma(1/2)Process. #ifndef Pythia8_SigmaEW_H #define Pythia8_SigmaEW_H #include "Pythia8/PythiaComplex.h" #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // A derived class for q g -> q gamma (q = u, d, s, c, b). // Use massless approximation also for Q since no alternative. class Sigma2qg2qgamma : public Sigma2Process { public: // Constructor. Sigma2qg2qgamma() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q g -> q gamma (udscb)";} virtual int code() const {return 201;} virtual string inFlux() const {return "qg";} private: // Values stored for later use. double sigUS, sigma0; }; //========================================================================== // A derived class for q qbar -> g gamma. class Sigma2qqbar2ggamma : public Sigma2Process { public: // Constructor. Sigma2qqbar2ggamma() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> g gamma";} virtual int code() const {return 202;} virtual string inFlux() const {return "qqbarSame";} private: // Values stored for later use. double sigma0; }; //========================================================================== // A derived class for g g -> g gamma. class Sigma2gg2ggamma : public Sigma2Process { public: // Constructor. Sigma2gg2ggamma() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "g g -> g gamma";} virtual int code() const {return 203;} virtual string inFlux() const {return "gg";} private: // Values stored for later use. double chargeSum, sigma; }; //========================================================================== // A derived class for f fbar -> gamma gamma. class Sigma2ffbar2gammagamma : public Sigma2Process { public: // Constructor. Sigma2ffbar2gammagamma() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "f fbar -> gamma gamma";} virtual int code() const {return 204;} virtual string inFlux() const {return "ffbarSame";} private: // Values stored for later use. double sigTU, sigma0; }; //========================================================================== // A derived class for g g -> gamma gamma. class Sigma2gg2gammagamma : public Sigma2Process { public: // Constructor. Sigma2gg2gammagamma() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "g g -> gamma gamma";} virtual int code() const {return 205;} virtual string inFlux() const {return "gg";} private: double charge2Sum, sigma; }; //========================================================================== // A derived class for f f' -> f f' via t-channel gamma*/Z0 exchange. class Sigma2ff2fftgmZ : public Sigma2Process { public: // Constructor. Sigma2ff2fftgmZ() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "f f' -> f f' (t-channel gamma*/Z0)";} virtual int code() const {return 211;} virtual string inFlux() const {return "ff";} private: // Z parameters for propagator. int gmZmode; double mZ, mZS, thetaWRat, sigmagmgm, sigmagmZ, sigmaZZ; }; //========================================================================== // A derived class for f_1 f_2 -> f_3 f_4 via t-channel W+- exchange. class Sigma2ff2fftW : public Sigma2Process { public: // Constructor. Sigma2ff2fftW() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "f_1 f_2 -> f_3 f_4 (t-channel W+-)";} virtual int code() const {return 212;} virtual string inFlux() const {return "ff";} private: // W parameters for propagator. double mW, mWS, thetaWRat, sigma0; }; //========================================================================== // A derived class for q q' -> Q q" via t-channel W+- exchange. // Related to Sigma2ff2fftW class, but with massive matrix elements. class Sigma2qq2QqtW : public Sigma2Process { public: // Constructor. Sigma2qq2QqtW(int idIn, int codeIn) : idNew(idIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angles in top decay (else inactive). virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ff";} virtual int id3Mass() const {return idNew;} private: // Values stored for process type. W parameters for propagator. int idNew, codeSave; string nameSave; double mW, mWS, thetaWRat, sigma0, openFracPos, openFracNeg; }; //========================================================================== // A derived class for f fbar -> gamma*/Z0. class Sigma1ffbar2gmZ : public Sigma1Process { public: // Constructor. Sigma1ffbar2gmZ() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for Z decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar -> gamma*/Z0";} virtual int code() const {return 221;} virtual string inFlux() const {return "ffbarSame";} virtual int resonanceA() const {return 23;} private: // Parameters set at initialization or for each new event. int gmZmode; double mRes, GammaRes, m2Res, GamMRat, thetaWRat, gamSum, intSum, resSum, gamProp, intProp, resProp; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* particlePtr; }; //========================================================================== // A derived class for f fbar' -> W+-. class Sigma1ffbar2W : public Sigma1Process { public: // Constructor. Sigma1ffbar2W() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar' -> W+-";} virtual int code() const {return 222;} virtual string inFlux() const {return "ffbarChg";} virtual int resonanceA() const {return 24;} private: // Parameters set at initialization. double mRes, GammaRes, m2Res, GamMRat, thetaWRat, sigma0Pos, sigma0Neg; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* particlePtr; }; //========================================================================== // A derived class for f fbar -> gamma* -> f' fbar', summed over light f'. // Allows pT-ordered evolution for multiparton interactions. class Sigma2ffbar2ffbarsgm : public Sigma2Process { public: // Constructor. Sigma2ffbar2ffbarsgm() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const { return "f fbar -> f' fbar' (s-channel gamma*)";} virtual int code() const {return 223;} virtual string inFlux() const {return "ffbarSame";} virtual bool isSChannel() const {return true;} private: // Values stored for later use. int idNew; double sigma0; }; //========================================================================== // A derived class for f fbar -> gamma*/Z0 -> F Fbar, for one heavy F. // Allows pT cuts as for other 2 -> 2 processes. class Sigma2ffbar2FFbarsgmZ : public Sigma2Process { public: // Constructor. Sigma2ffbar2FFbarsgmZ(int idIn, int codeIn) : idNew(idIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angles in top decay (else inactive). virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ffbarSame";} virtual bool isSChannel() const {return true;} virtual int id3Mass() const {return idNew;} virtual int id4Mass() const {return idNew;} virtual int resonanceA() const {return 23;} private: // Values stored for process type. Z parameters for propagator. int idNew, codeSave, gmZmode; string nameSave; bool isPhysical; double ef, vf, af, mRes, GammaRes, m2Res, GamMRat, thetaWRat, mr, betaf, cosThe, gamProp, intProp, resProp, openFracPair; }; //========================================================================== // A derived class for f fbar' -> W+- -> F fbar", for one or two heavy F. // Allows pT cuts as for other 2 -> 2 processes. class Sigma2ffbar2FfbarsW : public Sigma2Process { public: // Constructor. Sigma2ffbar2FfbarsW(int idIn, int idIn2, int codeIn) : idNew(idIn), idNew2(idIn2), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angles in top decay (else inactive). virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ffbarChg";} virtual bool isSChannel() const {return true;} virtual int id3Mass() const {return idNew;} virtual int id4Mass() const {return idPartner;} virtual int resonanceA() const {return 24;} private: // Values stored for process type. W parameters for propagator. int idNew, idNew2, codeSave, idPartner; string nameSave; bool isPhysical; double V2New, mRes, GammaRes, m2Res, GamMRat, thetaWRat, sigma0, openFracPos, openFracNeg; }; //========================================================================== // An intermediate class for f fbar -> gamma*/Z0/W+- gamma*/Z0/W-+. class Sigma2ffbargmZWgmZW : public Sigma2Process { public: // Constructor. Sigma2ffbargmZWgmZW() {} protected: // Internal products. Vec4 pRot[7]; complex hA[7][7]; complex hC[7][7]; // Calculate and store internal products. void setupProd( Event& process, int i1, int i2, int i3, int i4, int i5, int i6); // Evaluate the F function of Gunion and Kunszt. complex fGK(int i1, int i2, int i3, int i4, int i5, int i6); // Evaluate the Xi function of Gunion and Kunszt. double xiGK( double tHnow, double uHnow); // Evaluate the Xj function of Gunion and Kunszt. double xjGK( double tHnow, double uHnow); private: }; //========================================================================== // A derived class for f fbar -> gamma*/Z0 gamma*/Z0. class Sigma2ffbar2gmZgmZ : public Sigma2ffbargmZWgmZW { public: // Constructor. Sigma2ffbar2gmZgmZ() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for simultaneous flavour choices. virtual double weightDecayFlav( Event& process); // Evaluate weight for decay angles of the two gamma*/Z0. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar -> gamma*/Z0 gamma*/Z0";} virtual int code() const {return 231;} virtual string inFlux() const {return "ffbarSame";} virtual int id3Mass() const {return 23;} virtual int id4Mass() const {return 23;} private: // Parameters set at initialization or for each new event. int gmZmode, i1, i2, i3, i4, i5, i6; double mRes, GammaRes, m2Res, GamMRat, thetaWRat, sigma0, gamSum3, intSum3, resSum3, gamProp3, intProp3, resProp3, gamSum4, intSum4, resSum4, gamProp4, intProp4, resProp4, c3LL, c3LR, c3RL, c3RR, c4LL, c4LR, c4RL, c4RR, flavWt; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* particlePtr; }; //========================================================================== // A derived class for f fbar' -> Z0 W+-. (Here pure Z0, unfortunately.) class Sigma2ffbar2ZW : public Sigma2ffbargmZWgmZW { public: // Constructor. Sigma2ffbar2ZW() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for Z0 and W+- decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar' -> Z0 W+- (no gamma*!)";} virtual int code() const {return 232;} virtual string inFlux() const {return "ffbarChg";} virtual int id3Mass() const {return 23;} virtual int id4Mass() const {return 24;} virtual int resonanceA() const {return 24;} private: // Store W+- mass and width, and couplings. double mW, widW, mWS, mwWS, sin2thetaW, cos2thetaW, thetaWRat, cotT, thetaWpt, thetaWmm, lun, lde, sigma0, openFracPos, openFracNeg; }; //========================================================================== // A derived class for f fbar -> W+ W-. class Sigma2ffbar2WW : public Sigma2ffbargmZWgmZW { public: // Constructor. Sigma2ffbar2WW() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W+ and W- decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar -> W+ W-";} virtual int code() const {return 233;} virtual string inFlux() const {return "ffbarSame";} virtual int id3Mass() const {return 24;} virtual int id4Mass() const {return -24;} virtual int resonanceA() const {return 23;} private: // Store Z0 mass and width. double mZ, widZ, mZS, mwZS, thetaWRat, sigma0, cgg, cgZ, cZZ, cfg, cfZ, cff, gSS, gTT, gST, gUU, gSU, openFracPair; }; //========================================================================== // An intermediate class for f fbar -> gamma*/Z0 g/gamma and permutations. class Sigma2ffbargmZggm : public Sigma2Process { public: // Constructor. Sigma2ffbargmZggm() {} // Initialize process. virtual void initProc(); // Evaluate weight for gamma&/Z0 decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); protected: // Parameters set at initialization or for each new event. int gmZmode; double mRes, GammaRes, m2Res, GamMRat, thetaWRat, gamSum, intSum, resSum, gamProp, intProp, resProp; // Evaluate current sum of flavour couplings times phase space. void flavSum(); // Evaluate current propagator terms of cross section. void propTerm(); private: // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* particlePtr; }; //========================================================================== // A derived class for q qbar -> gamma*/Z0 g. class Sigma2qqbar2gmZg : public Sigma2ffbargmZggm { public: // Constructor. Sigma2qqbar2gmZg() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> gamma*/Z0 g";} virtual int code() const {return 241;} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return 23;} private: // Values stored for later use. double sigma0; }; //========================================================================== // A derived class for q g -> gamma*/Z0 q. class Sigma2qg2gmZq : public Sigma2ffbargmZggm { public: // Constructor. Sigma2qg2gmZq() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q g-> gamma*/Z0 q";} virtual int code() const {return 242;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return 23;} private: // Values stored for later use. double sigma0; }; //========================================================================== // A derived class for f fbar' -> gamma*/Z0 gamma. class Sigma2ffbar2gmZgm : public Sigma2ffbargmZggm { public: // Constructor. Sigma2ffbar2gmZgm() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "f fbar -> gamma*/Z0 gamma";} virtual int code() const {return 243;} virtual string inFlux() const {return "ffbarSame";} virtual int id3Mass() const {return 23;} private: // Values stored for later use. double sigma0; }; //========================================================================== // A derived class for f gamma -> gamma*/Z0 f. class Sigma2fgm2gmZf : public Sigma2ffbargmZggm { public: // Constructor. Sigma2fgm2gmZf() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "f gamma -> gamma*/Z0 f";} virtual int code() const {return 244;} virtual string inFlux() const {return "fgm";} virtual int id3Mass() const {return 23;} private: // Values stored for later use. double sigma0; }; //========================================================================== // An intermediate class for f fbar -> W+- g/gamma and permutations. class Sigma2ffbarWggm : public Sigma2Process { public: // Constructor. Sigma2ffbarWggm() {} // Evaluate weight for gamma&/Z0 decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); private: }; //========================================================================== // A derived class for q qbar' -> W+- g. class Sigma2qqbar2Wg : public Sigma2ffbarWggm { public: // Constructor. Sigma2qqbar2Wg() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar' -> W+- g";} virtual int code() const {return 251;} virtual string inFlux() const {return "ffbarChg";} virtual int id3Mass() const {return 24;} private: // Values stored for later use. double sigma0, openFracPos, openFracNeg; }; //========================================================================== // A derived class for q g -> W+- q'. class Sigma2qg2Wq : public Sigma2ffbarWggm { public: // Constructor. Sigma2qg2Wq() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q g-> W+- q'";} virtual int code() const {return 252;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return 24;} private: // Values stored for later use. double sigma0, openFracPos, openFracNeg; }; //========================================================================== // A derived class for f fbar' -> W+- gamma. class Sigma2ffbar2Wgm : public Sigma2ffbarWggm { public: // Constructor. Sigma2ffbar2Wgm() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "f fbar' -> W+- gamma";} virtual int code() const {return 253;} virtual string inFlux() const {return "ffbarChg";} virtual int id3Mass() const {return 24;} private: // Values stored for later use. double sigma0, openFracPos, openFracNeg; }; //========================================================================== // A derived class for f gamma -> W+- f'. class Sigma2fgm2Wf : public Sigma2ffbarWggm { public: // Constructor. Sigma2fgm2Wf() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "f gamma -> W+- f'";} virtual int code() const {return 254;} virtual string inFlux() const {return "fgm";} virtual int id3Mass() const {return 24;} private: // Values stored for later use. double sigma0, openFracPos, openFracNeg; }; //========================================================================== // A derived class for gamma gamma -> f fbar. class Sigma2gmgm2ffbar : public Sigma2Process { public: // Constructor. Sigma2gmgm2ffbar(int idIn, int codeIn) : idNew(idIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gmgm";} virtual int id3Mass() const {return idMass;} virtual int id4Mass() const {return idMass;} private: // Member variables. int idNew, codeSave, idMass, idNow; string nameSave; double ef4, s34Avg, sigTU, sigma, openFracPair; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaEW_H pythia8-8.1.80.orig/include/Pythia8/SigmaExtraDim.h0000644000175000017500000006675312217346231020173 0ustar sunsun// SigmaExtraDim.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Author: Stefan Ask for the *LED* routines. // Header file for extra-dimensional-process differential cross sections. // Contains classes derived from SigmaProcess via Sigma(1/2)Process. #ifndef Pythia8_SigmaExtraDim_H #define Pythia8_SigmaExtraDim_H #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // A derived class for g g -> G^* (excited graviton state). class Sigma1gg2GravitonStar : public Sigma1Process { public: // Constructor. Sigma1gg2GravitonStar() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for G* decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "g g -> G*";} virtual int code() const {return 5001;} virtual string inFlux() const {return "gg";} virtual int resonanceA() const {return idGstar;} private: // Parameters set at initialization or for current kinematics. bool eDsmbulk, eDvlvl; int idGstar; double mRes, GammaRes, m2Res, GamMRat, kappaMG, sigma; // Couplings between graviton and SM (indexed by particle id). double eDcoupling[27]; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* gStarPtr; }; //========================================================================== // A derived class for f fbar -> G^* (excited graviton state). class Sigma1ffbar2GravitonStar : public Sigma1Process { public: // Constructor. Sigma1ffbar2GravitonStar() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for G* decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar -> G*";} virtual int code() const {return 5002;} virtual string inFlux() const {return "ffbarSame";} virtual int resonanceA() const {return idGstar;} private: // Parameters set at initialization or for current kinematics. bool eDsmbulk, eDvlvl; int idGstar; double mRes, GammaRes, m2Res, GamMRat, kappaMG, sigma0; // Couplings between graviton and SM (indexed by particle id). double eDcoupling[27]; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* gStarPtr; }; //========================================================================== // A derived class for q qbar -> g^*/KK-gluon^* (excited kk-gluon state). class Sigma1qqbar2KKgluonStar : public Sigma1Process { public: // Constructor. Sigma1qqbar2KKgluonStar() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for g* decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "q qbar -> g*/KK-gluon*";} virtual int code() const {return 5006;} virtual string inFlux() const {return "qqbarSame";} virtual int resonanceA() const {return idKKgluon;} private: // Parameters set at initialization or for current kinematics. int idKKgluon; double mRes, GammaRes, m2Res, GamMRat; double sumSM, sumInt, sumKK, sigSM, sigInt, sigKK; // Couplings between kk gluon and SM (indexed by particle id). // Helicity dependent couplings. Use vector/axial-vector // couplings internally, gv/ga = 0.5 * (gL +/- gR). double eDgv[10], eDga[10]; // Interference parameter. int interfMode; // Pointer to properties of the particle species, to access decay // channels. ParticleDataEntry* gStarPtr; }; //========================================================================== // A derived class for g g -> G^* g (excited graviton state). class Sigma2gg2GravitonStarg : public Sigma2Process { public: // Constructor. Sigma2gg2GravitonStarg() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight: currently isotropic (except secondary top decay).. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "g g -> G* g";} virtual int code() const {return 5003;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return idGstar;} private: // Parameters set at initialization or for current kinematics. int idGstar; double mRes, GammaRes, m2Res, GamMRat, kappaMG, openFrac, sigma; }; //========================================================================== // A derived class for q g -> G^* q (excited graviton state). class Sigma2qg2GravitonStarq : public Sigma2Process { public: // Constructor. Sigma2qg2GravitonStarq() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight: currently isotropic (except secondary top decay). virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "q g -> G* q";} virtual int code() const {return 5004;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return idGstar;} private: // Parameters set at initialization or for current kinematics. int idGstar; double mRes, GammaRes, m2Res, GamMRat, kappaMG, openFrac, sigma; }; //========================================================================== // A derived class for q qbar -> G^* g (excited graviton state). class Sigma2qqbar2GravitonStarg : public Sigma2Process { public: // Constructor. Sigma2qqbar2GravitonStarg() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight: currently isotropic (except secondary top decay). virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "q qbar -> G* g";} virtual int code() const {return 5005;} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return idGstar;} private: // Parameters set at initialization or for current kinematics. int idGstar; double mRes, GammaRes, m2Res, GamMRat, kappaMG, openFrac, sigma; }; //========================================================================== // NOAM: A derived class for, f fbar -> (gamma/Z)_KKTower -> F Fbar, // for one heavy F. // Process provided by N. Hod et al. and is described in arXiv:XXXX.YYYY class Sigma2ffbar2TEVffbar : public Sigma2Process { public: // Constructor. Sigma2ffbar2TEVffbar(int idIn, int codeIn) : idNew(idIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angles in top decay (else inactive). virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ffbarSame";} virtual bool isSChannel() const {return true;} virtual int idSChannel() const {return 5000023;} virtual int resonanceA() const {return 23;} virtual int resonanceB() const {return 5000023;} virtual int id3Mass() const {return idNew;} virtual int id4Mass() const {return idNew;} // Add phase-space sampling also around the Z_KK resonance. virtual int resonanceA(); virtual int resonanceB(); private: // Values stored for process type. string nameSave; int idNew, gmZmode, codeSave, nexcitationmax; bool isPhysical; double gPlusf, gMinusf, gPlusF, gMinusF, gPlusTop, gMinusTop, gf, gF; double mRes, m2Res, mStar, mTop, m2Top, mZKKn, m2ZKKn, m2gmKKn, mgmKKn, alphaemfixed; double helicityME2, coefTot, coefAngular; double mr, betaf, cosThe, openFracPair; double wgmKKFactor, wgmKKn, wZKKn, wZ0, ttbarwZKKn, ttbarwgmKKn, ttbarwFactorA, ttbarwFactorB; double phaseSpacemHatMin, phaseSpacemHatMax; complex gammaProp, resProp, gmPropKK, ZPropKK, totalProp; complex mI; }; //========================================================================== // A derived class for g g -> U/G g (real graviton emission in // large extra dimensions or unparticle emission). class Sigma2gg2LEDUnparticleg : public Sigma2Process { public: // Constructor: bool Graviton = true, to use LED graviton settings. Sigma2gg2LEDUnparticleg( bool Graviton ) : eDgraviton(Graviton) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section; // first step when inflavours unknown. virtual void sigmaKin(); // Evaluate sigmaHat(sHat); second step for given inflavours. virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return (eDgraviton ? "g g -> G g" : "g g -> U g") ;} virtual int code() const {return (eDgraviton ? 5021 : 5045);} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return 5000039;} virtual int id4Mass() const {return 21;} private: bool eDgraviton; int eDspin, eDnGrav, eDidG, eDcutoff; double mG, mGS, eDsigma0, eDdU, eDLambdaU, eDlambda, eDconstantTerm, eDtff, eDcf; }; //========================================================================== // A derived class for q g -> U/G q (real graviton emission in // large extra dimensions or unparticle emission). class Sigma2qg2LEDUnparticleq : public Sigma2Process { public: // Constructor: bool Graviton = true, to use LED graviton settings. Sigma2qg2LEDUnparticleq( bool Graviton) : eDgraviton(Graviton) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section; // first step when inflavours unknown. virtual void sigmaKin(); // Evaluate sigmaHat(sHat); second step for given inflavours. virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return (eDgraviton ? "q g -> G q" : "q g -> U q") ;} virtual int code() const {return (eDgraviton ? 5022 : 5046);} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return 5000039;} private: bool eDgraviton; int eDspin, eDnGrav, eDidG, eDcutoff; double mG, mGS, eDsigma0, eDdU, eDLambdaU, eDlambda, eDconstantTerm, eDtff, eDgf, eDcf; }; //========================================================================== // A derived class for q qbar -> U/G g (real graviton emission in // large extra dimensions or unparticle emission). class Sigma2qqbar2LEDUnparticleg : public Sigma2Process { public: // Constructor: bool Graviton = true, to use LED graviton settings. Sigma2qqbar2LEDUnparticleg( bool Graviton) : eDgraviton(Graviton) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section; // first step when inflavours unknown. virtual void sigmaKin(); // Evaluate sigmaHat(sHat); second step for given inflavours. virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return (eDgraviton ? "q qbar -> G g" : "q qbar -> U g") ;} virtual int code() const {return (eDgraviton ? 5023 : 5047);} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return 5000039;} virtual int id4Mass() const {return 21;} private: bool eDgraviton; int eDspin, eDnGrav, eDidG, eDcutoff; double mG, mGS, eDsigma0, eDdU, eDLambdaU, eDlambda, eDconstantTerm, eDtff, eDgf, eDcf; }; //========================================================================== // A derived class for f fbar -> U/G Z (real graviton emission in // large extra dimensions or unparticle emission). class Sigma2ffbar2LEDUnparticleZ : public Sigma2Process { public: // Constructor: bool Graviton = true, to use LED graviton settings. Sigma2ffbar2LEDUnparticleZ( bool Graviton) : eDgraviton(Graviton) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section; // first step when inflavours unknown. virtual void sigmaKin(); // Evaluate sigmaHat(sHat); second step for given inflavours. virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return (eDgraviton ? "f fbar -> G Z" : "f fbar -> U Z") ;} virtual int code() const {return (eDgraviton ? 5024 : 5041);} virtual string inFlux() const {return "ffbarSame";} virtual int id3Mass() const {return 5000039;} virtual int id4Mass() const {return 23;} virtual int resonanceA() const {return 23;} virtual int gmZmode() const {return 2;} private: // Constants: could only be changed in the code itself. static const double FIXRATIO; int eDspin, eDnGrav, eDcutoff, eDidG; bool eDgraviton; double eDdU, eDLambdaU, eDlambda, eDratio, eDlambdaPrime, eDtff, eDconstantTerm; double sHS, tHS, uHS, tHC, uHC, tHQ, uHQ, tHuH, mU, mUS, mZ, widZ, mZS, mwZS, eDsigma0; }; //========================================================================== // A derived class for f fbar -> U/G gamma (real graviton emission in // large extra dimensions or unparticle emission). class Sigma2ffbar2LEDUnparticlegamma : public Sigma2Process { public: // Constructor: bool Graviton = true, to use LED graviton settings. Sigma2ffbar2LEDUnparticlegamma( bool Graviton) : eDgraviton(Graviton) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section; // first step when inflavours unknown. virtual void sigmaKin(); // Evaluate sigmaHat(sHat); second step for given inflavours. virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return (eDgraviton ? "f fbar -> G gamma" : "f fbar -> U gamma") ;} virtual int code() const {return (eDgraviton ? 5025 : 5042);} virtual string inFlux() const {return "ffbarSame";} virtual int id3Mass() const {return 5000039;} virtual int id4Mass() const {return 22;} private: // Constants: could only be changed in the code itself. static const double FIXRATIO; int eDspin, eDnGrav, eDcutoff, eDidG; bool eDgraviton; double eDdU, eDLambdaU, eDlambda, eDratio, eDlambdaPrime, eDtff, eDconstantTerm; double sHS, tHS, uHS, tHC, uHC, tHQ, uHQ, tHuH, mU, mUS, mZ, mZS, eDsigma0; }; //========================================================================== // A derived class for f fbar -> (LED G*/U*) -> gamma gamma // (virtual graviton/unparticle exchange). class Sigma2ffbar2LEDgammagamma : public Sigma2Process { public: // Constructor: bool Graviton = true, to use LED graviton settings. Sigma2ffbar2LEDgammagamma( bool Graviton) : eDgraviton(Graviton) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section; // first step when inflavours unknown. virtual void sigmaKin(); // Evaluate sigmaHat(sHat); second step for given inflavours. virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return (eDgraviton ? "f fbar -> (LED G*) -> gamma gamma" : "f fbar -> (U*) -> gamma gamma") ;} virtual int code() const {return (eDgraviton ? 5026 : 5043);} virtual string inFlux() const {return "ffbarSame";} private: int eDspin, eDcutoff, eDnGrav, eDnegInt; bool eDgraviton; double eDdU, eDLambdaU, eDlambda, eDlambda2chi, eDterm1, eDterm2, eDterm3, eDtff; }; //========================================================================== // A derived class for g g -> (LED G*/U*) -> gamma gamma // (virtual graviton/unparticle exchange). class Sigma2gg2LEDgammagamma : public Sigma2Process { public: // Constructor: bool Graviton = true, to use LED graviton settings. Sigma2gg2LEDgammagamma( bool Graviton) : eDgraviton(Graviton) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section; // first step when inflavours unknown. virtual void sigmaKin(); // Evaluate sigmaHat(sHat); second step for given inflavours. virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return (eDgraviton ? "g g -> (LED G*) -> gamma gamma" : "g g -> (U*) -> gamma gamma") ;} virtual int code() const {return (eDgraviton ? 5027 : 5044);} virtual string inFlux() const {return "gg";} private: int eDspin, eDcutoff, eDnGrav; bool eDgraviton; double eDdU, eDLambdaU, eDlambda, eDlambda2chi, eDsigma0, eDtff; }; //========================================================================== // A derived class for f fbar -> (LED G*/U*) -> l lbar // (virtual graviton/unparticle exchange). // Does not include t-channel contributions relevant for e^+e^- to e^+e^- class Sigma2ffbar2LEDllbar : public Sigma2Process { public: // Constructor: bool Graviton = true, to use LED graviton settings. Sigma2ffbar2LEDllbar( bool Graviton) : eDgraviton(Graviton) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section; // first step when inflavours unknown. virtual void sigmaKin(); // Evaluate sigmaHat(sHat); second step for given inflavours. virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return (eDgraviton ? "f fbar -> (LED G*) -> l l" : "f fbar -> (U*) -> l l") ;} virtual int code() const {return (eDgraviton ? 5028 : 5048);} virtual string inFlux() const {return "ffbarSame";} virtual bool isSChannel() const {return true;} private: int eDspin, eDcutoff, eDnGrav,eDnxx, eDnxy, eDnegInt; bool eDgraviton; double eDdU, eDLambdaU, eDlambda, eDlambda2chi, eDtff, eDmZ, eDmZS, eDGZ, eDGZS, eDabsMeU, eDdenomPropZ, eDrePropGamma, eDrePropZ, eDimPropZ, eDabsAS, eDreA, eDreABW, eDpoly1, eDpoly2, eDpoly3; }; //========================================================================== // A derived class for g g -> (LED G*/U*) -> l lbar // (virtual graviton/unparticle exchange). class Sigma2gg2LEDllbar : public Sigma2Process { public: // Constructor: bool Graviton = true, to use LED graviton settings. Sigma2gg2LEDllbar( bool Graviton) : eDgraviton(Graviton) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section; // first step when inflavours unknown. virtual void sigmaKin(); // Evaluate sigmaHat(sHat); second step for given inflavours. virtual double sigmaHat() {return eDsigma0;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return (eDgraviton ? "g g -> (LED G*) -> l l" : "g g -> (U*) -> l l") ;} virtual int code() const {return (eDgraviton ? 5029 : 5049);} virtual string inFlux() const {return "gg";} private: int eDspin, eDcutoff, eDnGrav; bool eDgraviton; double eDdU, eDLambdaU, eDlambda, eDlambda2chi, eDsigma0, eDtff; }; //========================================================================== // A derived class for g g -> (LED G*) -> g g. class Sigma2gg2LEDgg : public Sigma2Process { public: // Constructor. Sigma2gg2LEDgg() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "g g -> (LED G*) -> g g";} virtual int code() const {return 5030;} virtual string inFlux() const {return "gg";} private: // Values stored for colour flow selection. double sigTS, sigUS, sigTU, sigSum, sigma; // Model parameters. int eDopMode, eDnGrav, eDcutoff, eDnegInt; double eDMD, eDLambdaT, eDtff; }; //========================================================================== // A derived class for g g -> (LED G*) -> q qbar. class Sigma2gg2LEDqqbar : public Sigma2Process { public: // Constructor. Sigma2gg2LEDqqbar() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "g g -> (LED G*) -> q qbar (uds)";} virtual int code() const {return 5031;} virtual string inFlux() const {return "gg";} private: // Number of quarks to be considered in massless approximation. int nQuarkNew; // Values stored for colour flow selection. int idNew; double mNew, m2New, sigTS, sigUS, sigSum, sigma; // Model parameters. int eDopMode, eDnGrav, eDcutoff, eDnegInt; double eDMD, eDLambdaT, eDtff; }; //========================================================================== // A derived class for q g -> (LED G*) -> q g. // Use massless approximation also for Q since no alternative. class Sigma2qg2LEDqg : public Sigma2Process { public: // Constructor. Sigma2qg2LEDqg() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q g -> (LED G*) -> q g";} virtual int code() const {return 5032;} virtual string inFlux() const {return "qg";} private: // Values stored for colour flow selection. double sigTS, sigTU, sigSum, sigma; // Model parameters. int eDopMode, eDnGrav, eDcutoff, eDnegInt; double eDMD, eDLambdaT, eDtff; }; //========================================================================== // A derived class for q q(bar)' -> (LED G*) -> q q(bar)'. class Sigma2qq2LEDqq : public Sigma2Process { public: // Constructor. Sigma2qq2LEDqq() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q q(bar)' -> (LED G*) -> q q(bar)'";} virtual int code() const {return 5033;} virtual string inFlux() const {return "qq";} private: // Values stored for colour flow selection. double sigT, sigU, sigTU, sigST, sigSum; double sigGrT1, sigGrT2, sigGrU, sigGrTU, sigGrST; // Model parameters. int eDopMode, eDnGrav, eDcutoff, eDnegInt; double eDMD, eDLambdaT, eDtff; }; //========================================================================== // A derived class for q qbar -> (LED G*) -> g g. class Sigma2qqbar2LEDgg : public Sigma2Process { public: // Constructor. Sigma2qqbar2LEDgg() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> (LED G*) -> g g";} virtual int code() const {return 5034;} virtual string inFlux() const {return "qqbarSame";} private: // Values stored for colour flow selection. double sigTS, sigUS, sigSum, sigma; // Model parameters. int eDopMode, eDnGrav, eDcutoff, eDnegInt; double eDMD, eDLambdaT, eDtff; }; //========================================================================== // A derived class for q qbar -> (LED G*) -> q' qbar'. class Sigma2qqbar2LEDqqbarNew : public Sigma2Process { public: // Constructor. Sigma2qqbar2LEDqqbarNew() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> (LED G*) -> q' qbar' (uds)";} virtual int code() const {return 5035;} virtual string inFlux() const {return "qqbarSame";} private: // Number of quarks to be considered in massless approximation. int nQuarkNew; // Values stored for colour flow selection. int idNew; double mNew, m2New, sigS, sigma; // Model parameters. int eDopMode, eDnGrav, eDcutoff; double eDMD, eDLambdaT, eDtff; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaExtraDim_H pythia8-8.1.80.orig/include/Pythia8/MiniStringFragmentation.h0000644000175000017500000000503312217346227022264 0ustar sunsun// MiniStringFragmentation.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the class for "cluster" fragmentation. // MiniStringFragmentation: handle the fragmentation of low-mass systems. #ifndef Pythia8_MiniStringFragmentation_H #define Pythia8_MiniStringFragmentation_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/FragmentationFlavZpT.h" #include "Pythia8/FragmentationSystems.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // The MiniStringFragmentation class contains the routines to fragment // occasional low-mass colour singlet partonic systems, where the string // approach is not directly applicable (for technical reasons). class MiniStringFragmentation { public: // Constructor. MiniStringFragmentation() {} // Initialize and save pointers. void init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, StringFlav* flavSelPtrIn, StringPT* pTSelPtrIn, StringZ* zSelPtrIn); // Do the fragmentation: driver routine. bool fragment( int iSub, ColConfig& colConfig, Event& event, bool isDiff = false); private: // Constants: could only be changed in the code itself. static const int NTRYDIFFRACTIVE, NTRYLASTRESORT, NTRYFLAV; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to classes for flavour, pT and z generation. StringFlav* flavSelPtr; StringPT* pTSelPtr; StringZ* zSelPtr; // Initialization data, read from Settings. int nTryMass; double bLund; // Data members. bool isClosed; double mSum, m2Sum; Vec4 pSum; vector iParton; FlavContainer flav1, flav2; // Attempt to produce two particles from a cluster. bool ministring2two( int nTry, Event& event); // Attempt to produce one particle from a cluster. bool ministring2one( int iSub, ColConfig& colConfig, Event& event); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_MiniStringFragmentation_H pythia8-8.1.80.orig/include/Pythia8/FragmentationSystems.h0000644000175000017500000001420512217346227021651 0ustar sunsun// FragmentationSystems.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains auxiliary classes in the fragmentation process. // ColSinglet contains info on an individual singlet. // ColConfig describes the colour configuration of the whole event. // StringRegion keeps track on string momenta and directions. // StringSystem contains all the StringRegions of the colour singlet. #ifndef Pythia8_FragmentationSystems_H #define Pythia8_FragmentationSystems_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/FragmentationFlavZpT.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // The ColSinglet class contains info on an individual singlet. // Only to be used inside ColConfig, so no private members. class ColSinglet { public: // Constructors. ColSinglet() : pSum(0., 0., 0., 0.), mass(0.), massExcess(0.), hasJunction(false), isClosed(false), isCollected(false) {} ColSinglet(vector& iPartonIn, Vec4 pSumIn, double massIn, double massExcessIn, bool hasJunctionIn = false, bool isClosedIn = false, bool isCollectedIn = false) : iParton(iPartonIn), pSum(pSumIn), mass(massIn), massExcess(massExcessIn), hasJunction(hasJunctionIn), isClosed(isClosedIn), isCollected(isCollectedIn) {} // Size of iParton array. int size() const { return iParton.size();} // Stored quantities. vector iParton; Vec4 pSum; double mass, massExcess; bool hasJunction, isClosed, isCollected; }; //========================================================================== // The ColConfig class describes the colour configuration of the whole event. class ColConfig { public: // Constructor. ColConfig() {singlets.resize(0);} // Initialize and save pointers. void init(Info* infoPtrIn, Settings& settings, StringFlav* flavSelPtrIn); // Number of colour singlets. int size() const {return singlets.size();} // Overload index operator to access separate colour singlets. ColSinglet& operator[](int iSub) {return singlets[iSub];} // Clear contents. void clear() {singlets.resize(0);} // Insert a new colour singlet system in ascending mass order. // Calculate its properties. Join nearby partons. bool insert( vector& iPartonIn, Event& event); // Erase a colour singlet system. (Rare operation.) void erase(int iSub) {singlets.erase(singlets.begin() + iSub);} // Collect all partons of singlet to be consecutively ordered. void collect(int iSub, Event& event, bool skipTrivial = true); // Find to which singlet system a particle belongs. int findSinglet(int i); // List all currently identified singlets. void list(ostream& os = cout) const; private: // Constants: could only be changed in the code itself. static const double CONSTITUENTMASS; // Pointer to various information on the generation. Info* infoPtr; // Pointer to class for flavour generation. StringFlav* flavSelPtr; // Initialization data, to be read from Settings. double mJoin, mJoinJunction, mStringMin; // List of all separate colour singlets. vector singlets; // Join two legs of junction to a diquark for small invariant masses. bool joinJunction( vector& iPartonIn, Event& event, double massExcessIn); }; //========================================================================== // The StringRegion class contains the information related to // one string section in the evolution of a multiparton system. // Only to be used inside StringFragmentation and MiniStringFragmentation, // so no private members. class StringRegion { public: // Constructor. StringRegion() : isSetUp(false), isEmpty(true) {} // Constants: could only be changed in the code itself. static const double MJOIN, TINY; // Data members. bool isSetUp, isEmpty; Vec4 pPos, pNeg, eX, eY; double w2, xPosProj, xNegProj, pxProj, pyProj; // Set up four-vectors for longitudinal and transverse directions. void setUp(Vec4 p1, Vec4 p2, bool isMassless = false); // Construct a four-momentum from (x+, x-, px, py). Vec4 pHad( double xPosIn, double xNegIn, double pxIn, double pyIn) { return xPosIn * pPos + xNegIn * pNeg + pxIn * eX + pyIn * eY; } // Project a four-momentum onto (x+, x-, px, py). Read out projection. void project(Vec4 pIn); void project( double pxIn, double pyIn, double pzIn, double eIn) { project( Vec4( pxIn, pyIn, pzIn, eIn) ); } double xPos() const {return xPosProj;} double xNeg() const {return xNegProj;} double px() const {return pxProj;} double py() const {return pyProj;} }; //========================================================================== // The StringSystem class contains the complete set of all string regions. // Only to be used inside StringFragmentation, so no private members. class StringSystem { public: // Constructor. StringSystem() {} // Set up system from parton list. void setUp(vector& iSys, Event& event); // Calculate string region from (iPos, iNeg) pair. int iReg( int iPos, int iNeg) const {return (iPos * (indxReg - iPos)) / 2 + iNeg;} // Reference to string region specified by (iPos, iNeg) pair. StringRegion& region(int iPos, int iNeg) {return system[iReg(iPos, iNeg)];} // Reference to low string region specified either by iPos or iNeg. StringRegion& regionLowPos(int iPos) { return system[iReg(iPos, iMax - iPos)]; } StringRegion& regionLowNeg(int iNeg) { return system[iReg(iMax - iNeg, iNeg)]; } // Main content: a vector with all the string regions of the system. vector system; // Other data members. int sizePartons, sizeStrings, sizeRegions, indxReg, iMax; double mJoin, m2Join; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_FragmentationSystems_H pythia8-8.1.80.orig/include/Pythia8/PythiaComplex.h0000644000175000017500000000115112217346230020237 0ustar sunsun// PythiaComplex.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for typedef'd double precision complex numbers. #ifndef Pythia8_PythiaComplex_H #define Pythia8_PythiaComplex_H // Stdlib header for complex numbers. # include namespace Pythia8 { // Convenient typedef for double precision complex numbers. typedef std::complex complex; } // end namespace Pythia8 #endif // Pythia8_PythiaComplex_H pythia8-8.1.80.orig/include/Pythia8/PartonLevel.h0000644000175000017500000001552412217346230017715 0ustar sunsun// PartonLevel.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the main class for parton-level event generation // PartonLevel: administrates showers, multiparton interactions and remnants. #ifndef Pythia8_PartonLevel_H #define Pythia8_PartonLevel_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/BeamRemnants.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/MultipartonInteractions.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonSystems.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/ResonanceDecays.h" #include "Pythia8/RHadrons.h" #include "Pythia8/Settings.h" #include "Pythia8/SigmaTotal.h" #include "Pythia8/SpaceShower.h" #include "Pythia8/StandardModel.h" #include "Pythia8/TimeShower.h" #include "Pythia8/UserHooks.h" #include "Pythia8/MergingHooks.h" namespace Pythia8 { //========================================================================== // The PartonLevel class contains the top-level routines to generate // the partonic activity of an event. class PartonLevel { public: // Constructor. PartonLevel() : userHooksPtr(0) {} // Initialization of all classes at the parton level. bool init( Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, BeamParticle* beamPomAPtrIn, BeamParticle* beamPomBPtrIn, Couplings* couplingsPtrIn, PartonSystems* partonSystemsPtrIn, SigmaTotal* sigmaTotPtr, TimeShower* timesDecPtrIn, TimeShower* timesPtrIn, SpaceShower* spacePtrIn, RHadrons* rHadronsPtrIn, UserHooks* userHooksPtrIn, MergingHooks* mergingHooksPtr, bool useAsTrial); // Generate the next parton-level process. bool next( Event& process, Event& event); // Perform showers in resonance decay chains. (For special cases.) void setupShowerSys( Event& process, Event& event); bool resonanceShowers( Event& process, Event& event, bool skipForR); // Perform decays and showers of W and Z emitted in shower. bool wzDecayShowers( Event& event); // Tell whether failure was due to vetoing. bool hasVetoed() const {return doVeto;} // Accumulate, print and reset statistics. void accumulate() {if (isResolved && !isDiff) multiPtr->accumulate();} void statistics(bool reset = false) { if (doMPI) multiMB.statistics(reset);} // For now no separate statistics for diffraction?? //if (doMPISDA && doDiffraction) multiSDA.statistics(reset); //if (doMPISDB && doDiffraction) multiSDB.statistics(reset);} void resetStatistics() { if (doMPI) multiMB.resetStatistics(); } // Reset PartonLevel object for trial shower usage. void resetTrial(); // Provide the pT scale of the last branching in the shower. double pTLastInShower(){ return pTLastBranch; } // Provide the type of the last branching in the shower. int typeLastInShower(){ return typeLastBranch; } private: // Constants: could only be changed in the code itself. static const int NTRY; // Initialization data, mainly read from Settings. bool doNonDiff, doDiffraction, doMPI, doMPIMB, doMPISDA, doMPISDB, doMPICD, doMPIinit, doISR, doFSRduringProcess, doFSRafterProcess, doFSRinResonances, doRemnants, doSecondHard, hasLeptonBeams, hasPointLeptons, canVetoPT, canVetoStep, canVetoMPIStep, canVetoEarly, canSetScale, allowRH, earlyResDec; double mMinDiff, mWidthDiff, pMaxDiff; // Event generation strategy. Number of steps. Maximum pT scales. bool doVeto; int nMPI, nISR, nFSRinProc, nFSRinRes, nISRhard, nFSRhard, typeLatest, nVetoStep, typeVetoStep, nVetoMPIStep, iSysNow; double pTsaveMPI, pTsaveISR, pTsaveFSR, pTvetoPT; // Current event properties. bool isNonDiff, isDiffA, isDiffB, isDiffC, isDiff, isSingleDiff, isDoubleDiff, isCentralDiff, isResolved, isResolvedA, isResolvedB, isResolvedC; int sizeProcess, sizeEvent, nHardDone, nHardDoneRHad, iDS; double eCMsave; vector inRHadDecay; vector iPosBefShow; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to the two incoming beams. BeamParticle* beamAPtr; BeamParticle* beamBPtr; // Spare copies of normal pointers. Pointers to Pomeron beam-inside-beam. BeamParticle* beamHadAPtr; BeamParticle* beamHadBPtr; BeamParticle* beamPomAPtr; BeamParticle* beamPomBPtr; // Pointers to Standard Model couplings. Couplings* couplingsPtr; // Pointer to information on subcollision parton locations. PartonSystems* partonSystemsPtr; // Pointer to userHooks object for user interaction with program. UserHooks* userHooksPtr; // Pointers to timelike showers for resonance decays and the rest. TimeShower* timesDecPtr; TimeShower* timesPtr; // Pointer to spacelike showers. SpaceShower* spacePtr; // The generator classes for multiparton interactions. MultipartonInteractions multiMB; MultipartonInteractions multiSDA; MultipartonInteractions multiSDB; MultipartonInteractions multiCD; MultipartonInteractions* multiPtr; // The generator class to construct beam-remnant kinematics. BeamRemnants remnants; // Separate instance for central diffraction. BeamRemnants remnantsCD; // The RHadrons class is used to fragment off and decay R-hadrons. RHadrons* rHadronsPtr; // ResonanceDecay object does sequential resonance decays. ResonanceDecays resonanceDecays; // Resolved diffraction: find how many systems should have it. int decideResolvedDiff( Event& process); // Set up an unresolved process, i.e. elastic or diffractive. bool setupUnresolvedSys( Event& process, Event& event); // Set up the hard process, excluding subsequent resonance decays. void setupHardSys( Event& process, Event& event); // Resolved diffraction: pick whether to have it and set up for it. void setupResolvedDiff( Event& process); // Resolved diffraction: restore normal behaviour. void leaveResolvedDiff( int iHardLoop, Event& process, Event& event); // Pointer to MergingHooks object for user interaction with the merging. MergingHooks* mergingHooksPtr; // Parameters to specify trial shower usage bool doTrial; int nTrialEmissions; // Parameters to store to veto trial showers double pTLastBranch; int typeLastBranch; // Parameters to specify merging usage bool canRemoveEvent, canRemoveEmission; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_PartonLevel_H pythia8-8.1.80.orig/include/Pythia8/PartonSystems.h0000644000175000017500000000651112217346230020311 0ustar sunsun// PartonSystems.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains auxiliary classes for the parton-level processes. // PartonSystem contains info on a single partonic subcollision. // PartonSystems describes the set of subcollisions in the whole event. #ifndef Pythia8_PartonSystems_H #define Pythia8_PartonSystems_H #include "Pythia8/PythiaStdlib.h" namespace Pythia8 { //========================================================================== // The PartonSystem class contains info on an individual singlet. // Only to be used inside PartonSystems, so no private members. class PartonSystem { public: // Constructors. PartonSystem() : iInA(0), iInB(0), sHat(0.) {iOut.reserve(10);} // Stored quantities. int iInA, iInB; vector iOut; double sHat, pTHat; }; //========================================================================== // The PartonSystems class describes the whole set of subcollisions. class PartonSystems { public: // Constructor. PartonSystems() {systems.resize(0);} // Reset system list to empty. void clear() {systems.resize(0);} // Add new subsystem to list; return its index. Number of subsystems. int addSys() {systems.push_back(PartonSystem()); return systems.size() - 1;} int sizeSys() const {return systems.size();} // Set, add or replace info to one system. void setInA(int iSys, int iPos) {systems[iSys].iInA = iPos;} void setInB(int iSys, int iPos) {systems[iSys].iInB = iPos;} void addOut(int iSys, int iPos) {systems[iSys].iOut.push_back(iPos);} void setOut(int iSys, int iMem, int iPos) {systems[iSys].iOut[iMem] = iPos;} void replace(int iSys, int iPosOld, int iPosNew); void setSHat(int iSys, double sHatIn) {systems[iSys].sHat = sHatIn;} void setPTHat(int iSys, double pTHatIn) {systems[iSys].pTHat = pTHatIn;} void setSizeSys(int iSize) {systems.resize(iSize);} // Get info on one system. bool hasInAB(int iSys) const {return ( (systems[iSys].iInA > 0) || (systems[iSys].iInB > 0) ) ;} int getInA(int iSys) const {return systems[iSys].iInA;} int getInB(int iSys) const {return systems[iSys].iInB;} int sizeOut(int iSys) const {return systems[iSys].iOut.size();} int getOut(int iSys, int iMem) const {return systems[iSys].iOut[iMem];} int sizeAll(int iSys) const {return (hasInAB(iSys)) ? systems[iSys].iOut.size() + 2 : systems[iSys].iOut.size();} int getAll(int iSys, int iMem) const; double getSHat(int iSys) const {return systems[iSys].sHat;} double getPTHat(int iSys) const {return systems[iSys].pTHat;} // Find system of given outgoing parton, optionally also incoming one. int getSystemOf(int iPos, bool alsoIn = false) const; // Find iOut index of given system and event record index int getIndexOfOut(int iSys, int iPos) const; // List all current systems. void list(ostream& os = cout) const; private: // List of all separate partonic subsystems. vector systems; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_PartonSystems_H pythia8-8.1.80.orig/include/Pythia8/StandardModel.h0000644000175000017500000001535612217346232020210 0ustar sunsun// StandardModel.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file gives access to some Standard Model parameters. // AlphaStrong: fix or first- or second-order running alpha_strong. #ifndef Pythia8_StandardModel_H #define Pythia8_StandardModel_H #include "Pythia8/Basics.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // The AlphaStrong class calculates the alpha_strong value at an arbitrary // scale, given the value at m_Z, to zeroth, first or second order. class AlphaStrong { public: // Constructors. AlphaStrong() : isInit(false), order(0), Lambda3Save(0.), Lambda4Save(0.), Lambda5Save(0.), Lambda6Save(0.), Lambda3Save2(0.), Lambda4Save2(0.), Lambda5Save2(0.), Lambda6Save2(0.), scale2Min(0.), mc2(0.), mb2(0.), mt2(0.), lastCallToFull(false), valueRef(0.), valueNow(0.), scale2Now(0.) {} AlphaStrong(double valueIn, int orderIn = 1) { init( valueIn, orderIn) ;} // Initialization for given value at M_Z and given order. virtual void init(double valueIn = 0.12, int orderIn = 1, int nfmaxIn = 6, bool useCMWIn = false); // alpha_S value and Lambda values. double alphaS(double scale2); double alphaS1Ord(double scale2); double alphaS2OrdCorr(double scale2); double Lambda3() const { return Lambda3Save; } double Lambda4() const { return Lambda4Save; } double Lambda5() const { return Lambda5Save; } double Lambda6() const { return (nfmax >= 6) ? Lambda6Save : Lambda5Save; } // Info: tell which scales we use for flavour thresholds. double muThres(int idQ); double muThres2(int idQ); // Return the CMW factor (for nF between 3 and 6). double facCMW( int nFin); // Protected data members: accessible to derived classes. protected: // Initialization data member. bool isInit; // Running order and max number of flavours to use in running. int order, nfmax; // Lambda values. double Lambda3Save, Lambda4Save, Lambda5Save, Lambda6Save; double Lambda3Save2, Lambda4Save2, Lambda5Save2, Lambda6Save2; // Smallest allowed renormalization scale. double scale2Min; // Flavour thresholds. static const double MC, MB, MZ, MT; double mc2, mb2, mt2; // CMW rescaling factors. bool useCMW; static const double FACCMW3, FACCMW4, FACCMW5, FACCMW6; // Safety margins to avoid getting too close to LambdaQCD. static const double SAFETYMARGIN1, SAFETYMARGIN2; // Private data members: not accessible to derived classes. private: // Private constants: could only be changed in the code itself. static const int NITER; // Private data members. bool lastCallToFull; double valueRef, valueNow, scale2Now; }; //========================================================================== // The AlphaEM class calculates the alpha_electromagnetic value at an // arbitrary scale, given the value at 0 and m_Z, to zeroth or first order. class AlphaEM { public: // Constructors. AlphaEM() {} // Initialization for a given order. void init(int orderIn, Settings* settingsPtr); // alpha_EM value. double alphaEM(double scale2); private: // Constants: could only be changed in the code itself. static const double MZ, Q2STEP[5], BRUNDEF[5]; // Data members. int order; double alpEM0, alpEMmZ, mZ2, bRun[5], alpEMstep[5]; }; //========================================================================== // The CoupSM class stores and returns electroweak couplings, // including Cabibbo-Kobayashi-Maskawa mass mixing matrix elements. class CoupSM { public: // Constructor. CoupSM() {} // Initialize, normally from Pythia::init(). void init(Settings& settings, Rndm* rndmPtrIn); // alpha_S value and Lambda values. double alphaS(double scale2) {return alphaSlocal.alphaS(scale2);} double alphaS1Ord(double scale2) {return alphaSlocal.alphaS1Ord(scale2);} double alphaS2OrdCorr(double scale2) { return alphaSlocal.alphaS2OrdCorr(scale2);} double Lambda3() const {return alphaSlocal.Lambda3();} double Lambda4() const {return alphaSlocal.Lambda4();} double Lambda5() const {return alphaSlocal.Lambda5();} // Return alpha_EM value. double alphaEM(double scale2) {return alphaEMlocal.alphaEM(scale2);} // Return electroweak mixing angle and Fermi constant. double sin2thetaW() {return s2tW;} double cos2thetaW() {return c2tW;} double sin2thetaWbar() {return s2tWbar;} double GF() {return GFermi;} // Return electroweak couplings of quarks and leptons. double ef(int idAbs) {return efSave[idAbs];} double vf(int idAbs) {return vfSave[idAbs];} double af(int idAbs) {return afSave[idAbs];} double t3f(int idAbs) {return 0.5*afSave[idAbs];} double lf(int idAbs) {return lfSave[idAbs];} double rf(int idAbs) {return rfSave[idAbs];} // Return some squared couplings and other combinations. double ef2(int idAbs) {return ef2Save[idAbs];} double vf2(int idAbs) {return vf2Save[idAbs];} double af2(int idAbs) {return af2Save[idAbs];} double efvf(int idAbs) {return efvfSave[idAbs];} double vf2af2(int idAbs) {return vf2af2Save[idAbs];} // Return CKM value or square: // first index 1/2/3/4 = u/c/t/t', second 1/2/3/4 = d/s/b/b'. double VCKMgen(int genU, int genD) {return VCKMsave[genU][genD];} double V2CKMgen(int genU, int genD) {return V2CKMsave[genU][genD];} // Return CKM value or square for incoming flavours (sign irrelevant). double VCKMid(int id1, int id2); double V2CKMid(int id1, int id2); // Return CKM sum of squares for given inflavour, or random outflavour. double V2CKMsum(int id) {return V2CKMout[abs(id)];} int V2CKMpick(int id); protected: // Constants: could only be changed in the code itself. static const double efSave[20], afSave[20]; // Couplings and VCKM matrix (index 0 not used). double s2tW, c2tW, s2tWbar, GFermi, vfSave[20], lfSave[20], rfSave[20], ef2Save[20], vf2Save[20], af2Save[20], efvfSave[20], vf2af2Save[20], VCKMsave[5][5], V2CKMsave[5][5], V2CKMout[20]; // Pointer to the random number generator. Rndm* rndmPtr; // An AlphaStrong instance for general use (but not MPI, ISR, FSR). AlphaStrong alphaSlocal; // An AlphaEM instance for general use (but not MPI, ISR, FSR). AlphaEM alphaEMlocal; }; //========================================================================== // Generic couplings class class Couplings : public CoupSM { public: Couplings() : isSUSY(false) {} bool isSUSY; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_StandardModel_H pythia8-8.1.80.orig/include/Pythia8/SigmaNewGaugeBosons.h0000644000175000017500000001222612217346231021326 0ustar sunsun// SigmaNewGaugeBosons.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for new-gauge-boson-process differential cross sections. // Contains classes derived from SigmaProcess via Sigma1Process. #ifndef Pythia8_SigmaNewGaugeBosons_H #define Pythia8_SigmaNewGaugeBosons_H #include "Pythia8/PythiaComplex.h" #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // An intermediate class for f fbar -> Z'/W' -> WW/WZ -> 4 fermions. // Copied from SigmaEW for gauge-boson-pair production. class Sigma1ffbarZprimeWprime: public Sigma1Process { public: // Constructor. Sigma1ffbarZprimeWprime() {} protected: // Internal products. Vec4 pRot[7]; complex hA[7][7]; complex hC[7][7]; // Calculate and store internal products. void setupProd( Event& process, int i1, int i2, int i3, int i4, int i5, int i6); // Evaluate the F function of Gunion and Kunszt. complex fGK(int i1, int i2, int i3, int i4, int i5, int i6); // Evaluate the Xi function of Gunion and Kunszt. double xiGK( double tHnow, double uHnow, double s3now, double s4now); // Evaluate the Xj function of Gunion and Kunszt. double xjGK( double tHnow, double uHnow, double s3now, double s4now); private: }; //========================================================================== // A derived class for f fbar -> gamma*/Z0/Z'0. class Sigma1ffbar2gmZZprime : public Sigma1ffbarZprimeWprime { public: // Constructor. Sigma1ffbar2gmZZprime() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for Z' decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar -> gamma*/Z0/Zprime0";} virtual int code() const {return 3001;} virtual string inFlux() const {return "ffbarSame";} virtual int resonanceA() const {return 23;} virtual int resonanceB() const {return 32;} private: // Parameters set at initialization or for each new event. int gmZmode; double mRes, GammaRes, m2Res, GamMRat, sin2tW, cos2tW, thetaWRat, mZ, GammaZ, m2Z, GamMRatZ, afZp[20], vfZp[20], coupZpWW, anglesZpWW, gamSum, gamZSum, ZSum, gamZpSum, ZZpSum, ZpSum, gamNorm, gamZNorm, ZNorm, gamZpNorm, ZZpNorm, ZpNorm; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* particlePtr; }; //========================================================================== // A derived class for f fbar' -> W'+-. class Sigma1ffbar2Wprime : public Sigma1ffbarZprimeWprime { public: // Constructor. Sigma1ffbar2Wprime() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar' -> W'+-";} virtual int code() const {return 3021;} virtual string inFlux() const {return "ffbarChg";} virtual int resonanceA() const {return 34;} private: // Parameters set at initialization. double mRes, GammaRes, m2Res, GamMRat, thetaWRat, sigma0Pos, sigma0Neg, aqWp, vqWp, alWp, vlWp, coupWpWZ, anglesWpWZ; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* particlePtr; }; //========================================================================== // A derived class for f fbar' -> R^0 (horizontal gauge boson). class Sigma1ffbar2Rhorizontal : public Sigma1Process { public: // Constructor. Sigma1ffbar2Rhorizontal() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "f fbar' -> R^0";} virtual int code() const {return 3041;} virtual string inFlux() const {return "ffbar";} virtual int resonanceA() const {return 41;} private: // Parameters set at initialization. double mRes, GammaRes, m2Res, GamMRat, thetaWRat, sigma0Pos, sigma0Neg; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* particlePtr; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia_SigmaNewGaugeBosons_H pythia8-8.1.80.orig/include/Pythia8/ParticleDecays.h0000644000175000017500000001100612217346230020345 0ustar sunsun// ParticleDecays.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the classes to perform a particle decay. // DecayHandler: base class for external handling of decays. // ParticleDecays: decay a particle. #ifndef Pythia8_ParticleDecays_H #define Pythia8_ParticleDecays_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/FragmentationFlavZpT.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" #include "Pythia8/TimeShower.h" #include "Pythia8/TauDecays.h" namespace Pythia8 { //========================================================================== // DecayHandler is base class for the external handling of decays. // There is only one pure virtual method, that should do the decay. class DecayHandler { public: // Destructor. virtual ~DecayHandler() {} // A pure virtual method, wherein the derived class method does a decay. virtual bool decay(vector& idProd, vector& mProd, vector& pProd, int iDec, const Event& event) = 0; }; //========================================================================== // The ParticleDecays class contains the routines to decay a particle. class ParticleDecays { public: // Constructor. ParticleDecays() {} // Initialize: store pointers and find settings void init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, Couplings* couplingsPtrIn, TimeShower* timesDecPtrIn, StringFlav* flavSelPtrIn, DecayHandler* decayHandlePtrIn, vector handledParticles); // Perform a decay of a single particle. bool decay(int iDec, Event& event); // Did decay result in new partons to hadronize? bool moreToDo() const {return hasPartons && keepPartons;} private: // Constants: could only be changed in the code itself. static const int NTRYDECAY, NTRYPICK, NTRYMEWT, NTRYDALITZ; static const double MSAFEDALITZ, WTCORRECTION[11]; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to Standard Model couplings. Couplings* couplingsPtr; // Pointers to timelike showers, for decays to partons (e.g. Upsilon). TimeShower* timesDecPtr; // Pointer to class for flavour generation; needed when to pick hadrons. StringFlav* flavSelPtr; // Pointer to a handler of external decays. DecayHandler* decayHandlePtr; // Initialization data, read from Settings. bool limitTau0, limitTau, limitRadius, limitCylinder, limitDecay, mixB, doFSRinDecays, doGammaRad; int sophisticatedTau; double mSafety, tau0Max, tauMax, rMax, xyMax, zMax, xBdMix, xBsMix, sigmaSoft, multIncrease, multIncreaseWeak, multRefMass, multGoffset, colRearrange, stopMass, sRhoDal, wRhoDal; // Multiplicity. Decay products positions and masses. bool hasPartons, keepPartons; int idDec, meMode, mult; double scale; vector iProd, idProd, cols, acols, idPartons; vector mProd, mInv, rndmOrd; vector pInv, pProd; vector flavEnds; // Pointer to particle data for currently decaying particle ParticleDataEntry* decDataPtr; // Tau particle decayer. TauDecays tauDecayer; // Check whether a decay is allowed, given the upcoming decay vertex. bool checkVertex(Particle& decayer); // Check for oscillations B0 <-> B0bar or B_s0 <-> B_s0bar. bool oscillateB(Particle& decayer); // Do a one-body decay. bool oneBody(Event& event); // Do a two-body decay; bool twoBody(Event& event); // Do a three-body decay; bool threeBody(Event& event); // Do a multibody decay using the M-generator algorithm. bool mGenerator(Event& event); // Select mass of lepton pair in a Dalitz decay. bool dalitzMass(); // Do kinematics of gamma* -> l- l+ in Dalitz decay. bool dalitzKinematics(Event& event); // Translate a partonic content into a set of actual hadrons. bool pickHadrons(); // Set colour flow and scale in a decay explicitly to partons. bool setColours(Event& event); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_ParticleDecays_H pythia8-8.1.80.orig/include/Pythia8/ProcessContainer.h0000644000175000017500000001705412217346230020743 0ustar sunsun// ProcessContainer.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the collected machinery of a process. // ProcessContainer: contains information on a particular process. // SetupContainers: administrates the selection/creation of processes. #ifndef Pythia8_ProcessContainer_H #define Pythia8_ProcessContainer_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonDistributions.h" #include "Pythia8/PhaseSpace.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/ResonanceDecays.h" #include "Pythia8/Settings.h" #include "Pythia8/SigmaProcess.h" #include "Pythia8/SigmaTotal.h" #include "Pythia8/StandardModel.h" #include "Pythia8/SusyCouplings.h" #include "Pythia8/SLHAinterface.h" #include "Pythia8/UserHooks.h" namespace Pythia8 { //========================================================================== // The ProcessContainer class combines pointers to matrix element and // phase space generator with general generation info. class ProcessContainer { public: // Constructor. ProcessContainer(SigmaProcess* sigmaProcessPtrIn = 0, bool externalPtrIn = false) : sigmaProcessPtr(sigmaProcessPtrIn), externalPtr(externalPtrIn), phaseSpacePtr(0) {} // Destructor. Do not destroy external sigmaProcessPtr. ~ProcessContainer() {delete phaseSpacePtr; if (!externalPtr) delete sigmaProcessPtr;} // Initialize phase space and counters. bool init(bool isFirst, Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtr, BeamParticle* beamBPtr, Couplings* couplings, SigmaTotal* sigmaTotPtr, ResonanceDecays* resDecaysPtrIn, SLHAinterface* slhaInterfacePtr, UserHooks* userHooksPtr); // Store or replace Les Houches pointer. void setLHAPtr( LHAup* lhaUpPtrIn, ParticleData* particleDataPtrIn = 0) {lhaUpPtr = lhaUpPtrIn; if (particleDataPtrIn != 0) particleDataPtr = particleDataPtrIn; if (sigmaProcessPtr != 0) sigmaProcessPtr->setLHAPtr(lhaUpPtr); if (phaseSpacePtr != 0) phaseSpacePtr->setLHAPtr(lhaUpPtr);} // Update the CM energy of the event. void newECM(double eCM) {phaseSpacePtr->newECM(eCM);} // Generate a trial event; accepted or not. bool trialProcess(); // Pick flavours and colour flow of process. bool constructState(); // Give the hard subprocess (with option for a second hard subprocess). bool constructProcess( Event& process, bool isHardest = true); // Give the Les Houches decay chain for external resonance. bool constructDecays( Event& process); // Do resonance decays. bool decayResonances( Event& process); // Accumulate statistics after user veto. void accumulate(); // Reset statistics on events generated so far. void reset(); // Process name and code, and the number of final-state particles. string name() const {return sigmaProcessPtr->name();} int code() const {return sigmaProcessPtr->code();} int nFinal() const {return sigmaProcessPtr->nFinal();} bool isSUSY() const {return sigmaProcessPtr->isSUSY();} // Member functions for info on generation process. bool newSigmaMax() const {return newSigmaMx;} double sigmaMax() const {return sigmaMx;} long nTried() const {return nTry;} long nSelected() const {return nSel;} long nAccepted() const {return nAcc;} double weightSum() const {return wtAccSum;} double sigmaSelMC() {if (nTry > nTryStat) sigmaDelta(); return sigmaAvg;} double sigmaMC() {if (nTry > nTryStat) sigmaDelta(); return sigmaFin;} double deltaMC() {if (nTry > nTryStat) sigmaDelta(); return deltaFin;} // Some kinematics quantities. int id1() const {return sigmaProcessPtr->id(1);} int id2() const {return sigmaProcessPtr->id(2);} double x1() const {return phaseSpacePtr->x1();} double x2() const {return phaseSpacePtr->x2();} double Q2Fac() const {return sigmaProcessPtr->Q2Fac();} double mHat() const {return sqrtpos(phaseSpacePtr->sHat());} double pTHat() const {return phaseSpacePtr->pTHat();} // Tell whether container is for Les Houches events. bool isLHAContainer() const {return isLHA;} int lhaStrategy() const {return lhaStrat;} // Info on Les Houches events. int codeLHASize() const {return codeLHA.size();} int subCodeLHA(int i) const {return codeLHA[i];} long nTriedLHA(int i) const {return nTryLHA[i];} long nSelectedLHA(int i) const {return nSelLHA[i];} long nAcceptedLHA(int i) const {return nAccLHA[i];} // When two hard processes set or get info whether process is matched. void isSame( bool isSameIn) { isSameSave = isSameIn;} bool isSame() const {return isSameSave;} private: // Constants: could only be changed in the code itself. static const int N12SAMPLE, N3SAMPLE; // Pointer to the subprocess matrix element. Mark if external. SigmaProcess* sigmaProcessPtr; bool externalPtr; // Pointer to the phase space generator. PhaseSpace* phaseSpacePtr; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointer to ResonanceDecays object for sequential resonance decays. ResonanceDecays* resDecaysPtr; // Pointer to userHooks object for user interaction with program. UserHooks* userHooksPtr; // Pointer to LHAup for generating external events. LHAup* lhaUpPtr; // Possibility to modify Les Houches input. int setLifetime; // Info on process. bool isLHA, isNonDiff, isResolved, isDiffA, isDiffB, isDiffC, isQCD3body, allowNegSig, isSameSave, increaseMaximum, canVetoResDecay; int lhaStrat, lhaStratAbs; // Statistics on generation process. (Long integers just in case.) bool newSigmaMx; long nTry, nSel, nAcc, nTryStat; double sigmaMx, sigmaSgn, sigmaSum, sigma2Sum, sigmaNeg, sigmaAvg, sigmaFin, deltaFin, weightNow, wtAccSum; // Statistics for Les Houches event classification. vector codeLHA; vector nTryLHA, nSelLHA, nAccLHA; // Estimate integrated cross section and its uncertainty. void sigmaDelta(); }; //========================================================================== // The SetupContainers class turns the list of user-requested processes // into a vector of ProcessContainer objects, each with a process. class SetupContainers { public: // Constructor. SetupContainers() {} // Initialization assuming all necessary data already read. bool init(vector& containerPtrs, Settings& settings, ParticleData* particleDataPtr, Couplings* couplings); // Initialization of a second hard process. bool init2(vector& container2Ptrs, Settings& settings); private: // Methods to check that outgoing SUSY particles are allowed ones. void setupIdVecs( Settings& settings); bool allowIdVals( int idCheck1, int idCheck2); // Arrays of allowed outgoing SUSY particles and their lengths. vector idVecA, idVecB; int nVecA, nVecB; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_ProcessContainer_H pythia8-8.1.80.orig/include/Pythia8/TauDecays.h0000644000175000017500000000766412217346232017354 0ustar sunsun// TauDecays.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Philip Ilten, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for the TauDecays class. #ifndef Pythia8_TauDecays_H #define Pythia8_TauDecays_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/HelicityBasics.h" #include "Pythia8/HelicityMatrixElements.h" #include "Pythia8/PythiaComplex.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // TauDecays class. // This class decays tau leptons, with helicity information. class TauDecays { public: // Constructor and destructor. TauDecays() {}; ~TauDecays() {} // Initializer. void init(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, Couplings* couplingsPtrIn); // Decay a tau or correlated tau pair. bool decay(int iDec, Event& event); // Choose a decay channel for a particle. vector createChildren(HelicityParticle parent); // Perform an N-body isotropic decay. void isotropicDecay(vector& p); // Write the decay to event record. void writeDecay(Event& event, vector& p); private: // Constants: could only be changed in the code itself. static const int NTRYCHANNEL, NTRYDECAY; static const double WTCORRECTION[11]; // Flag whether a correlated tau decay should be performed. bool correlated; // User selected mode and mother for tau decays. int tauMode, tauMother, tauModeSave, tauMotherSave; // User selected polarization for tau decays. double polarization, polSave; // Helicity matrix element pointers. HelicityMatrixElement* hardME; HelicityMatrixElement* decayME; // Hard process helicity matrix elements. HMETwoFermions2W2TwoFermions hmeTwoFermions2W2TwoFermions; HMETwoFermions2Z2TwoFermions hmeTwoFermions2Z2TwoFermions; HMETwoFermions2Gamma2TwoFermions hmeTwoFermions2Gamma2TwoFermions; HMETwoFermions2GammaZ2TwoFermions hmeTwoFermions2GammaZ2TwoFermions; HMEZ2TwoFermions hmeZ2TwoFermions; HMEHiggsEven2TwoFermions hmeHiggsEven2TwoFermions; HMEHiggsOdd2TwoFermions hmeHiggsOdd2TwoFermions; HMEHiggsCharged2TwoFermions hmeHiggsCharged2TwoFermions; HMEUnpolarized hmeUnpolarized; // Tau decay helicity matrix elements. HMETau2Meson hmeTau2Meson; HMETau2TwoLeptons hmeTau2TwoLeptons; HMETau2TwoMesonsViaVector hmeTau2TwoMesonsViaVector; HMETau2TwoMesonsViaVectorScalar hmeTau2TwoMesonsViaVectorScalar; HMETau2ThreePions hmeTau2ThreePions; HMETau2ThreeMesonsWithKaons hmeTau2ThreeMesonsWithKaons; HMETau2ThreeMesonsGeneric hmeTau2ThreeMesonsGeneric; HMETau2TwoPionsGamma hmeTau2TwoPionsGamma; HMETau2FourPions hmeTau2FourPions; HMETau2FivePions hmeTau2FivePions; HMETau2PhaseSpace hmeTau2PhaseSpace; // Particles of the hard process. HelicityParticle in1, in2, mediator, out1, out2; vector particles; // The info pointer for the Pythia class. Info* infoPtr; // Pointer to settings database. Settings* settingsPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointer to SM coupling data. Couplings* couplingsPtr; // Parameters to determine if correlated partner should decay. double tau0Max, tauMax, rMax, xyMax, zMax; bool limitTau0, limitTau, limitRadius, limitCylinder, limitDecay; }; //========================================================================== } // end namespace Pythia8 #endif // end Pythia8_TauDecays_H pythia8-8.1.80.orig/include/Pythia8/Basics.h0000644000175000017500000004033012217346226016664 0ustar sunsun// Basics.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for basic, often-used helper classes. // RndmEngine: base class for external random number generators. // Rndm: random number generator. // Vec4: simple four-vectors. // RotBstMatrix: matrices encoding rotations and boosts of Vec4 objects. // Hist: simple one-dimensional histograms. #ifndef Pythia8_Basics_H #define Pythia8_Basics_H #include "Pythia8/PythiaStdlib.h" namespace Pythia8 { //========================================================================== // RndmEngine is the base class for external random number generators. // There is only one pure virtual method, that should do the generation. class RndmEngine { public: // Destructor. virtual ~RndmEngine() {} // A pure virtual method, wherein the derived class method // generates a random number uniformly distributed between 1 and 1. virtual double flat() = 0; }; //========================================================================== // Rndm class. // This class handles random number generation according to the // Marsaglia-Zaman-Tsang algorithm. class Rndm { public: // Constructors. Rndm() : initRndm(false), seedSave(0), sequence(0), useExternalRndm(false), rndmEngPtr(0) { } Rndm(int seedIn) : initRndm(false), seedSave(0), sequence(0), useExternalRndm(false), rndmEngPtr(0) { init(seedIn);} // Possibility to pass in pointer for external random number generation. bool rndmEnginePtr( RndmEngine* rndmEngPtrIn); // Initialize, normally at construction or in first call. void init(int seedIn = 0) ; // Generate next random number uniformly between 0 and 1. double flat() ; // Generate random numbers according to exp(-x). double exp() { return -log(flat()) ;} // Generate random numbers according to x * exp(-x). double xexp() { return -log(flat() * flat()) ;} // Generate random numbers according to exp(-x^2/2). double gauss() {return sqrt(-2. * log(flat())) * cos(M_PI * flat());} // Generate two random numbers according to exp(-x^2/2-y^2/2). pair gauss2() {double r = sqrt(-2. * log(flat())); double phi = 2. * M_PI * flat(); return pair(r * sin(phi), r * cos(phi));} // Pick one option among vector of (positive) probabilities. int pick(const vector& prob) ; // Save or read current state to or from a binary file. bool dumpState(string fileName); bool readState(string fileName); private: // Default random number sequence. static const int DEFAULTSEED; // State of the random number generator. bool initRndm; int i97, j97, seedSave; long sequence; double u[97], c, cd, cm; // Pointer for external random number generation. bool useExternalRndm; RndmEngine* rndmEngPtr; }; //========================================================================== // Forward reference to RotBstMatrix class; needed in Vec4 class. class RotBstMatrix; //-------------------------------------------------------------------------- // Vec4 class. // This class implements four-vectors, in energy-momentum space. // (But can equally well be used to hold space-time four-vectors.) class Vec4 { public: // Constructors. Vec4(double xIn = 0., double yIn = 0., double zIn = 0., double tIn = 0.) : xx(xIn), yy(yIn), zz(zIn), tt(tIn) { } Vec4(const Vec4& v) : xx(v.xx), yy(v.yy), zz(v.zz), tt(v.tt) { } Vec4& operator=(const Vec4& v) { if (this != &v) { xx = v.xx; yy = v.yy; zz = v.zz; tt = v.tt; } return *this; } Vec4& operator=(double value) { xx = value; yy = value; zz = value; tt = value; return *this; } // Member functions for input. void reset() {xx = 0.; yy = 0.; zz = 0.; tt = 0.;} void p(double xIn, double yIn, double zIn, double tIn) {xx = xIn; yy = yIn; zz = zIn; tt = tIn;} void p(Vec4 pIn) {xx = pIn.xx; yy = pIn.yy; zz = pIn.zz; tt = pIn.tt;} void px(double xIn) {xx = xIn;} void py(double yIn) {yy = yIn;} void pz(double zIn) {zz = zIn;} void e(double tIn) {tt = tIn;} // Member functions for output. double px() const {return xx;} double py() const {return yy;} double pz() const {return zz;} double e() const {return tt;} double mCalc() const {double temp = tt*tt - xx*xx - yy*yy - zz*zz; return (temp >= 0.) ? sqrt(temp) : -sqrt(-temp);} double m2Calc() const {return tt*tt - xx*xx - yy*yy - zz*zz;} double pT() const {return sqrt(xx*xx + yy*yy);} double pT2() const {return xx*xx + yy*yy;} double pAbs() const {return sqrt(xx*xx + yy*yy + zz*zz);} double pAbs2() const {return xx*xx + yy*yy + zz*zz;} double eT() const {double temp = xx*xx + yy*yy; return tt * sqrt( temp / (temp + zz*zz) );} double eT2() const {double temp = xx*xx + yy*yy; return tt*tt * temp / (temp + zz*zz);} double theta() const {return atan2(sqrt(xx*xx + yy*yy), zz);} double phi() const {return atan2(yy,xx);} double thetaXZ() const {return atan2(xx,zz);} double pPos() const {return tt + zz;} double pNeg() const {return tt - zz;} double rap() const {return 0.5 * log( (tt + zz) / (tt - zz) );} double eta() const {double xyz = sqrt(xx*xx + yy*yy + zz*zz); return 0.5 * log( (xyz + zz) / (xyz - zz) );} // Member functions that perform operations. void rescale3(double fac) {xx *= fac; yy *= fac; zz *= fac;} void rescale4(double fac) {xx *= fac; yy *= fac; zz *= fac; tt *= fac;} void flip3() {xx = -xx; yy = -yy; zz = -zz;} void flip4() {xx = -xx; yy = -yy; zz = -zz; tt = -tt;} void rot(double thetaIn, double phiIn); void rotaxis(double phiIn, double nx, double ny, double nz); void rotaxis(double phiIn, const Vec4& n); void bst(double betaX, double betaY, double betaZ); void bst(double betaX, double betaY, double betaZ, double gamma); void bst(const Vec4& pIn); void bst(const Vec4& pIn, double mIn); void bstback(const Vec4& pIn); void bstback(const Vec4& pIn, double mIn); void rotbst(const RotBstMatrix& M); // Operator overloading with member functions Vec4 operator-() {Vec4 tmp; tmp.xx = -xx; tmp.yy = -yy; tmp.zz = -zz; tmp.tt = -tt; return tmp;} Vec4& operator+=(const Vec4& v) {xx += v.xx; yy += v.yy; zz += v.zz; tt += v.tt; return *this;} Vec4& operator-=(const Vec4& v) {xx -= v.xx; yy -= v.yy; zz -= v.zz; tt -= v.tt; return *this;} Vec4& operator*=(double f) {xx *= f; yy *= f; zz *= f; tt *= f; return *this;} Vec4& operator/=(double f) {xx /= f; yy /= f; zz /= f; tt /= f; return *this;} // Operator overloading with friends friend Vec4 operator+(const Vec4& v1, const Vec4& v2); friend Vec4 operator-(const Vec4& v1, const Vec4& v2); friend Vec4 operator*(double f, const Vec4& v1); friend Vec4 operator*(const Vec4& v1, double f); friend Vec4 operator/(const Vec4& v1, double f); friend double operator*(const Vec4& v1, const Vec4& v2); // Invariant mass of a pair and its square. friend double m(const Vec4& v1, const Vec4& v2); friend double m2(const Vec4& v1, const Vec4& v2); // Scalar and cross product of 3-vector parts. friend double dot3(const Vec4& v1, const Vec4& v2); friend Vec4 cross3(const Vec4& v1, const Vec4& v2); // theta is polar angle between v1 and v2. friend double theta(const Vec4& v1, const Vec4& v2); friend double costheta(const Vec4& v1, const Vec4& v2); // phi is azimuthal angle between v1 and v2 around z axis. friend double phi(const Vec4& v1, const Vec4& v2); friend double cosphi(const Vec4& v1, const Vec4& v2); // phi is azimuthal angle between v1 and v2 around n axis. friend double phi(const Vec4& v1, const Vec4& v2, const Vec4& n); friend double cosphi(const Vec4& v1, const Vec4& v2, const Vec4& n); // R is distance in cylindrical (y/eta, phi) coordinates. friend double RRapPhi(const Vec4& v1, const Vec4& v2); friend double REtaPhi(const Vec4& v1, const Vec4& v2); // Print a four-vector. friend ostream& operator<<(ostream&, const Vec4& v) ; private: // Constants: could only be changed in the code itself. static const double TINY; // The four-vector data members. double xx, yy, zz, tt; }; //-------------------------------------------------------------------------- // Namespace function declarations; friends of Vec4 class. // Implementation of operator overloading with friends. inline Vec4 operator+(const Vec4& v1, const Vec4& v2) {Vec4 v = v1 ; return v += v2;} inline Vec4 operator-(const Vec4& v1, const Vec4& v2) {Vec4 v = v1 ; return v -= v2;} inline Vec4 operator*(double f, const Vec4& v1) {Vec4 v = v1; return v *= f;} inline Vec4 operator*(const Vec4& v1, double f) {Vec4 v = v1; return v *= f;} inline Vec4 operator/(const Vec4& v1, double f) {Vec4 v = v1; return v /= f;} inline double operator*(const Vec4& v1, const Vec4& v2) {return v1.tt*v2.tt - v1.xx*v2.xx - v1.yy*v2.yy - v1.zz*v2.zz;} // Invariant mass of a pair and its square. double m(const Vec4& v1, const Vec4& v2); double m2(const Vec4& v1, const Vec4& v2); // Scalar and cross product of 3-vector parts. double dot3(const Vec4& v1, const Vec4& v2); Vec4 cross3(const Vec4& v1, const Vec4& v2); // theta is polar angle between v1 and v2. double theta(const Vec4& v1, const Vec4& v2); double costheta(const Vec4& v1, const Vec4& v2); // phi is azimuthal angle between v1 and v2 around z axis. double phi(const Vec4& v1, const Vec4& v2); double cosphi(const Vec4& v1, const Vec4& v2); // phi is azimuthal angle between v1 and v2 around n axis. double phi(const Vec4& v1, const Vec4& v2, const Vec4& n); double cosphi(const Vec4& v1, const Vec4& v2, const Vec4& n); // R is distance in cylindrical (y/eta, phi) coordinates. double RRapPhi(const Vec4& v1, const Vec4& v2); double REtaPhi(const Vec4& v1, const Vec4& v2); // Print a four-vector. ostream& operator<<(ostream&, const Vec4& v) ; //========================================================================== // RotBstMatrix class. // This class implements 4 * 4 matrices that encode an arbitrary combination // of rotations and boosts, that can be applied to Vec4 four-vectors. class RotBstMatrix { public: // Constructors. RotBstMatrix() {for (int i = 0; i < 4; ++i) { for (int j = 0; j < 4; ++j) { M[i][j] = (i==j) ? 1. : 0.; } } } RotBstMatrix(const RotBstMatrix& Min) { for (int i = 0; i < 4; ++i) { for (int j = 0; j < 4; ++j) { M[i][j] = Min.M[i][j]; } } } RotBstMatrix& operator=(const RotBstMatrix& Min) {if (this != &Min) { for (int i = 0; i < 4; ++i) { for (int j = 0; j < 4; ++j) { M[i][j] = Min.M[i][j]; } } } return *this; } // Member functions. void rot(double = 0., double = 0.); void rot(const Vec4& p); void bst(double = 0., double = 0., double = 0.); void bst(const Vec4&); void bstback(const Vec4&); void bst(const Vec4&, const Vec4&); void toCMframe(const Vec4&, const Vec4&); void fromCMframe(const Vec4&, const Vec4&); void rotbst(const RotBstMatrix&); void invert(); void reset(); // Crude estimate deviation from unit matrix. double deviation() const; // Print a transformation matrix. friend ostream& operator<<(ostream&, const RotBstMatrix&) ; // Private members to be accessible from Vec4. friend class Vec4; private: // Constants: could only be changed in the code itself. static const double TINY; // The rotation-and-boost matrix data members. double M[4][4]; }; //-------------------------------------------------------------------------- // Namespace function declaration; friend of RotBstMatrix class. // Print a transformation matrix. ostream& operator<<(ostream&, const RotBstMatrix&) ; //========================================================================== // Hist class. // This class handles a single histogram at a time. class Hist{ public: // Constructors, including copy constructors. Hist() {;} Hist(string titleIn, int nBinIn = 100, double xMinIn = 0., double xMaxIn = 1.) { book(titleIn, nBinIn, xMinIn, xMaxIn);} Hist(const Hist& h) : title(h.title), nBin(h.nBin), nFill(h.nFill), xMin(h.xMin), xMax(h.xMax), dx(h.dx), under(h.under), inside(h.inside), over(h.over), res(h.res) { } Hist(string titleIn, const Hist& h) : title(titleIn), nBin(h.nBin), nFill(h.nFill), xMin(h.xMin), xMax(h.xMax), dx(h.dx), under(h.under), inside(h.inside), over(h.over), res(h.res) { } Hist& operator=(const Hist& h) { if(this != &h) { nBin = h.nBin; nFill = h.nFill; xMin = h.xMin; xMax = h.xMax; dx = h.dx; under = h.under; inside = h.inside; over = h.over; res = h.res; } return *this; } // Book a histogram. void book(string titleIn = " ", int nBinIn = 100, double xMinIn = 0., double xMaxIn = 1.) ; // Set title of a histogram. void name(string titleIn = " ") {title = titleIn; } // Reset bin contents. void null() ; // Fill bin with weight. void fill(double x, double w = 1.) ; // Print a histogram with overloaded << operator. friend ostream& operator<<(ostream& os, const Hist& h) ; // Print histogram contents as a table (e.g. for Gnuplot). void table(ostream& os = cout) const ; void table(string fileName) const { ofstream streamName(fileName.c_str()); table(streamName); } // Print a table out of two histograms with same x axis. friend void table(const Hist& h1, const Hist& h2, ostream& os) ; friend void table(const Hist& h1, const Hist& h2, string fileName) ; // Return content of specific bin: 0 gives underflow and nBin+1 overflow. double getBinContent(int iBin) ; // Return number of entries int getEntries() {return nFill; } // Check whether another histogram has same size and limits. bool sameSize(const Hist& h) const ; // Take logarithm (base 10 or e) of bin contents. void takeLog(bool tenLog = true) ; // Take square root of bin contents. void takeSqrt() ; // Operator overloading with member functions Hist& operator+=(const Hist& h) ; Hist& operator-=(const Hist& h) ; Hist& operator*=(const Hist& h) ; Hist& operator/=(const Hist& h) ; Hist& operator+=(double f) ; Hist& operator-=(double f) ; Hist& operator*=(double f) ; Hist& operator/=(double f) ; // Operator overloading with friends friend Hist operator+(double f, const Hist& h1); friend Hist operator+(const Hist& h1, double f); friend Hist operator+(const Hist& h1, const Hist& h2); friend Hist operator-(double f, const Hist& h1); friend Hist operator-(const Hist& h1, double f); friend Hist operator-(const Hist& h1, const Hist& h2); friend Hist operator*(double f, const Hist& h1); friend Hist operator*(const Hist& h1, double f); friend Hist operator*(const Hist& h1, const Hist& h2); friend Hist operator/(double f, const Hist& h1); friend Hist operator/(const Hist& h1, double f); friend Hist operator/(const Hist& h1, const Hist& h2); private: // Constants: could only be changed in the code itself. static const int NBINMAX, NCOLMAX, NLINES; static const double TOLERANCE, TINY, LARGE, SMALLFRAC, DYAC[]; static const char NUMBER[]; // Properties and contents of a histogram. string title; int nBin, nFill; double xMin, xMax, dx, under, inside, over; vector res; }; //-------------------------------------------------------------------------- // Namespace function declarations; friends of Hist class. // Print a histogram with overloaded << operator. ostream& operator<<(ostream& os, const Hist& h) ; // Print a table out of two histograms with same x axis. void table(const Hist& h1, const Hist& h2, ostream& os = cout) ; void table(const Hist& h1, const Hist& h2, string fileName) ; // Operator overloading with friends Hist operator+(double f, const Hist& h1); Hist operator+(const Hist& h1, double f); Hist operator+(const Hist& h1, const Hist& h2); Hist operator-(double f, const Hist& h1); Hist operator-(const Hist& h1, double f); Hist operator-(const Hist& h1, const Hist& h2); Hist operator*(double f, const Hist& h1); Hist operator*(const Hist& h1, double f); Hist operator*(const Hist& h1, const Hist& h2); Hist operator/(double f, const Hist& h1); Hist operator/(const Hist& h1, double f); Hist operator/(const Hist& h1, const Hist& h2); //========================================================================== } // end namespace Pythia8 #endif // end Pythia8_Basics_H pythia8-8.1.80.orig/include/Pythia8/RHadrons.h0000644000175000017500000001003512217346231017173 0ustar sunsun// RHadrons.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains a class for the production and decay // of long-lived heavy coloured particles, for now the gluino. #ifndef Pythia8_RHadrons_H #define Pythia8_RHadrons_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/FragmentationFlavZpT.h" #include "Pythia8/FragmentationSystems.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // The RHadrons class contains the routines for the production and decay // of long-lived heavy coloured particles. class RHadrons { public: // Constructor. RHadrons() : nRHad(0) {} // Initialization of R-hadron handling. bool init( Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn); // Pointers to flavours and z sent from HadronLevel. void fragPtrs( StringFlav* flavSelPtrIn, StringZ* zSelPtrIn) { flavSelPtr = flavSelPtrIn; zSelPtr = zSelPtrIn;} // Produce R-hadrons. bool produce( ColConfig& colConfig, Event& event); // Decay R-hadrons. bool decay( Event& event); // Tell whether a given particle is supposed to form R-hadrons. bool givesRHadron(int id); // Tell whether any R-hadrons have been formed. bool exist() {return (nRHad > 0);} // Tell whether a R-hadron production+decay happened, and trace down. int trace(int i) { for (int iR = 0; iR < nRHad; ++iR) if (iBefRHad[iR] == i || iCreRHad[iR] == i) return iAftRHad[iR]; return 0;} private: // Constants: could only be changed in the code itself. static const int IDRHADSB[14], IDRHADST[14], IDRHADGO[38], NTRYMAX; static const double MSAFETY, EGBORROWMAX; // Initialization data, mainly read from Settings. bool allowRH, allowRSb, allowRSt, allowRGo, allowSomeR, setMassesRH; int idRSb, idRSt, idRGo; double maxWidthRH, probGluinoballRH, mOffsetCloudRH, mCollapseRH, diquarkSpin1RH, m0Sb, m0St, m0Go; // Current event properties. vector iBefRHad, iCreRHad, iRHadron, iAftRHad; vector isTriplet; int nRHad, iRHad, iBef, iSys; ColSinglet* systemPtr; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to classes for flavour and z generation. StringFlav* flavSelPtr; StringZ* zSelPtr; // Split a system that contains both a sparticle and a junction. bool splitOffJunction( ColConfig& colConfig, Event& event); // Open up a closed gluon/gluino loop. bool openClosedLoop( ColConfig& colConfig, Event& event); // Split a single colour singlet that contains two sparticles. bool splitSystem( ColConfig& colConfig, Event& event); // Produce a R-hadron from a squark. bool produceSquark( ColConfig& colConfig, Event& event); // Produce a R-hadron from a gluino. bool produceGluino( ColConfig& colConfig, Event& event); // Construct R-hadron code from squark and (di)quark codes. int toIdWithSquark( int id1, int id2); // Construct squark and (di)quark codes from R-hadron code. pair fromIdWithSquark( int idRHad); // Construct R-hadron code from endpoints and a gluino. int toIdWithGluino( int id1, int id2); // Construct endpoint codes from R-hadron code with a gluino. pair fromIdWithGluino( int idRHad); // Construct modified four-vectors to match modified masses. bool newKin( Vec4 pOld1, Vec4 pOld2, double mNew1, double mNew2, Vec4& pNew1, Vec4& pNew2, bool checkMargin = true); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_RHadrons_H pythia8-8.1.80.orig/include/Pythia8/FastJet3.h0000644000175000017500000002005312217346226017103 0ustar sunsun// FastJet3.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This header file written by Gavin Salam. #ifndef Pythia8_FastJet3_H #define Pythia8_FastJet3_H //---------------------------------------------------------------------- /// \file FastJet3Pythia8.hh /// /// Code providing an interface for FastJet 3 to make use of Pythia8 /// particles and momenta. Given a /// /// \code /// Pythia8::Particle py8_particle; /// \endcode /// /// you may write /// /// \code /// fastjet::PseudoJet fj_particle = py8_particle; /// \endcode /// /// A copy of the Pythia8::Particle can then be accessed as /// /// \code /// fj_particle.user_info() /// \endcode /// /// so that one can obtain information about the particle such as /// /// \code /// fj_particle.user_info().status(); /// fj_particle.user_info().charge(); /// \endcode /// /// etc. Note that because the construction of a PseudoJet from the /// Pythia8 particle involves taking a copy of the whole particle /// (which has a number of member variables), there will be a small /// time penalty at that point. /// /// This file also defines a number of selectors that act on such /// PseudoJets, such as /// /// \code /// SelectorIsCharged(); /// SelectorId(int id); /// \endcode /// /// so that one can for example write /// /// \code /// vector charged_constituents /// = SelectorIsCharged()(jet.constituents()); /// \endcode /// /// The full list of Pythia8-specific selectors is to be found at the /// end of this file. They can be combined with each other and with /// FastJet selectors using standard boolean operators. They are all /// in the fastjet namespace. /// /// If you do not need the above facilities, then you may instead /// construct the PseudoJet from the pythia8 particle's 4-vector /// /// \code /// PseudoJet fj_particle = py8_particle.p(); /// \endcode /// /// NB: this code is entirely given as an include file. If compilation /// time is critical for your application, you may wish to split it /// into separate .cc and .hh files. /// // ---------------------------------------------------------------------- // Copyright 2011 by Matteo Cacciari, Gavin Salam and Gregory // Soyez. Permission is granted to redistribute this file and modify // it, as long as this notice is retained and any changes are clearly // marked. No warranties are provided! // ---------------------------------------------------------------------- #include "fastjet/config.h" // will allow a test for FJ3 #include "fastjet/ClusterSequence.hh" // also gives PseudoJet & JetDefinition #include "fastjet/Selector.hh" #include "Event.h" // this is what we need from Pythia8 // FASTJET_VERSION is only defined from version 3 onwards so we can // use it to test that we have a sufficiently recent version #ifndef FASTJET_VERSION #error "FastJet 3 is required in order to obtain the features of this interface" #endif FASTJET_BEGIN_NAMESPACE // place the code here inside the FJ namespace /// \class Py8Particle /// /// A class derived from a pythia 8 particle and that also derives /// from PseudoJet::UserInfoBase, so that it can be used as UserInfo /// inside PseudoJets, but also be cast back to the Pythia8 particle class Py8Particle: public Pythia8::Particle, public PseudoJet::UserInfoBase { public: Py8Particle(const Pythia8::Particle & particle) : Particle(particle) {} }; /// specialization of the PseudoJet constructor so that it can take a /// pythia8 particle (and makes a copy of it as user info); template<> inline PseudoJet::PseudoJet(const Pythia8::Particle & particle) { reset(particle.px(),particle.py(),particle.pz(), particle.e()); set_user_info(new Py8Particle(particle)); } /// specialization of the PseudoJet constructor so that it can take a /// pythia8 Vec4. There is then no particular user info available. template<> inline PseudoJet::PseudoJet(const Pythia8::Vec4 & particle) { reset(particle.px(),particle.py(),particle.pz(), particle.e()); } /// \class SelectorWorkerPy8 /// /// A template class to help with the creation of Selectors for Pythia /// particle properties. It's not necessary to understand how this /// works in order to use the selectors. See below for the actual list /// of selectors. /// /// (But if you're curious, essentially it stores a pointer to a /// member function of Pythia8::Particle, and when called to select /// particles, executes it and checks the return value is equal to /// that requested in the constructor). template class SelectorWorkerPy8 : public SelectorWorker { public: /// the typedef helps with the notation for member function pointers typedef T (Pythia8::Particle::*Py8ParticleFnPtr)() const; /// c'tor, which takes the member fn pointer and the return value /// that it should be equal to SelectorWorkerPy8(Py8ParticleFnPtr member_fn_ptr, T value) : _member_fn_ptr(member_fn_ptr), _value(value) {}; /// the one function from SelectorWorker that must be overloaded to /// get functioning selection. It makes sure that the PseudoJet /// actually has Pythia8::Particle user info before checking /// its value. bool pass(const PseudoJet & p) const { const Pythia8::Particle * py8_particle = dynamic_cast(p.user_info_ptr()); if (py8_particle == 0) { return false; // no info, so false } else { return (py8_particle->*_member_fn_ptr)() == _value; } } private: Py8ParticleFnPtr _member_fn_ptr; T _value; }; /// @name Boolean FJ3/PY8 Selectors /// /// A series of selectors for boolean properties of PseudoJets with /// Pythia8::Particle information; PseudoJets without /// Pythia8::Particle structure never pass these selectors. /// ///\{ inline Selector SelectorIsFinal () {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isFinal , true));} inline Selector SelectorIsCharged () {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isCharged , true));} inline Selector SelectorIsNeutral () {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isNeutral , true));} inline Selector SelectorIsResonance() {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isResonance, true));} inline Selector SelectorIsVisible () {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isVisible , true));} inline Selector SelectorIsLepton () {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isLepton , true));} inline Selector SelectorIsQuark () {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isQuark , true));} inline Selector SelectorIsGluon () {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isGluon , true));} inline Selector SelectorIsDiquark () {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isDiquark , true));} inline Selector SelectorIsParton () {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isParton , true));} inline Selector SelectorIsHadron () {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::isHadron , true));} ///\} /// @name Integer FJ3/PY8 Selectors /// /// A series of selectors for integer properties of PseudoJets with /// Pythia8::Particle information; PseudoJets without /// Pythia8::Particle structure never pass these selectors. /// ///\{ inline Selector SelectorId (int i) {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::id , i));} inline Selector SelectorIdAbs (int i) {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::idAbs , i));} inline Selector SelectorStatus (int i) {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::status , i));} inline Selector SelectorStatusAbs(int i) {return Selector(new SelectorWorkerPy8(&Pythia8::Particle::statusAbs, i));} ///\} FASTJET_END_NAMESPACE #endif // Pythia8_FastJet3_H pythia8-8.1.80.orig/include/Pythia8/PartonDistributions.h0000644000175000017500000003750112217346230021507 0ustar sunsun// PartonDistributions.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for parton densities. // PDF: base class. // LHAPDF: derived class for interface to the LHAPDF library. // GRV94L: derived class for the GRV 94L parton densities. // CTEQ5L: derived class for the CTEQ 5L parton densities. // MSTWpdf: derived class for MRST LO*, LO**, MSTW 2008 LO, NLO. // CTEQ6pdf: derived class for CTEQ 6L, 6L1, 66, CT09 MC1, MC2, (MCS?). // ProtonPoint: unresolved proton with equivalent photon spectrum. // GRVpiL: derived class for the GRV LO pion parton densities. // PomFix: derived class for Q2-independent Pomeron parton densities. // PomH1FitAB: derived class for the H1 2006 Fit A and Fit B Pomeron PDFs. // PomH1Jets: derived class for the H1 2007 Jets Pomeron PDFs. // Lepton: derived class for parton densities inside a lepton. // LeptonPoint: derived class for unresolved lepton (mainly dummy). // NNPDF: derived class for the NNPDF2.3 QCD+QED PDF sets. #ifndef Pythia8_PartonDistributions_H #define Pythia8_PartonDistributions_H #include "Pythia8/Basics.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" namespace Pythia8 { //========================================================================== // Base class for parton distribution functions. class PDF { public: // Constructor. PDF(int idBeamIn = 2212) {idBeam = idBeamIn; idBeamAbs = abs(idBeam); setValenceContent(); idSav = 9; xSav = -1.; Q2Sav = -1.; xu = 0.; xd = 0.; xs = 0.; xubar = 0.; xdbar = 0.; xsbar = 0.; xc = 0.; xb = 0.; xg = 0.; xlepton = 0.; xgamma = 0.; xuVal = 0.; xuSea = 0.; xdVal = 0.; xdSea = 0.; isSet = true; isInit = false;} // Destructor. virtual ~PDF() {} // Confirm that PDF has been set up (important for LHAPDF and H1 Pomeron). bool isSetup() {return isSet;} // Dynamic choice of meson valence flavours for pi0, K0S, K0L, Pomeron. void newValenceContent(int idVal1In, int idVal2In) { idVal1 = idVal1In; idVal2 = idVal2In;} // Allow extrapolation beyond boundaries. This is optional. virtual void setExtrapolate(bool) {} // Read out parton density double xf(int id, double x, double Q2); // Read out valence and sea part of parton densities. double xfVal(int id, double x, double Q2); double xfSea(int id, double x, double Q2); protected: // Store relevant quantities. int idBeam, idBeamAbs, idSav, idVal1, idVal2; double xSav, Q2Sav; double xu, xd, xs, xubar, xdbar, xsbar, xc, xb, xg, xlepton, xgamma, xuVal, xuSea, xdVal, xdSea; bool isSet, isInit; // Resolve valence content for assumed meson. Possibly modified later. void setValenceContent(); // Update parton densities. virtual void xfUpdate(int id, double x, double Q2) = 0; }; //========================================================================== // Provide interface to the LHAPDF library of parton densities. class LHAPDF : public PDF { public: // Constructor. LHAPDF(int idBeamIn, string setName, int member, int nSetIn = 1, Info* infoPtr = 0) : PDF(idBeamIn), nSet(nSetIn) {init( setName, member, infoPtr);} // Allow extrapolation beyond boundaries. This is optional. void setExtrapolate(bool extrapol); // Find out the nSet number corresponding to a name and member. // Returns -1 if no such LHAPDF set has been initialized. static int findNSet(string setName, int member); // Return the lowest non-occupied nSet number. static int freeNSet(); private: // Initialization of PDF set. void init(string setName, int member, Info* infoPtr); // Update all PDF values. void xfUpdate(int , double x, double Q2); // Current set and pdf values. int nSet; double xfArray[13]; bool hasPhoton; double xPhoton; // Keep track of what sets have been initialized in LHAPDFInterface. // The key is the nSet index, the value is a pair (name, member number). static map< int, pair > initializedSets; }; //========================================================================== // Gives the GRV 94L (leading order) parton distribution function set // in parametrized form. Authors: M. Glueck, E. Reya and A. Vogt. class GRV94L : public PDF { public: // Constructor. GRV94L(int idBeamIn = 2212) : PDF(idBeamIn) {} private: // Update PDF values. void xfUpdate(int , double x, double Q2); // Auxiliary routines used during the updating. double grvv (double x, double n, double ak, double bk, double a, double b, double c, double d); double grvw (double x, double s, double al, double be, double ak, double bk, double a, double b, double c, double d, double e, double es); double grvs (double x, double s, double sth, double al, double be, double ak, double ag, double b, double d, double e, double es); }; //========================================================================== // Gives the CTEQ 5L (leading order) parton distribution function set // in parametrized form. Parametrization by J. Pumplin. Authors: CTEQ. class CTEQ5L : public PDF { public: // Constructor. CTEQ5L(int idBeamIn = 2212) : PDF(idBeamIn) {} private: // Update PDF values. void xfUpdate(int , double x, double Q2); }; //========================================================================== // The MSTWpdf class. // MRST LO*(*) and MSTW 2008 PDF's, specifically the LO one. // Original C++ version by Jeppe Andersen. // Modified by Graeme Watt . // Sets available: // iFit = 1 : MRST LO* (2007). // iFit = 2 : MRST LO** (2008). // iFit = 3 : MSTW 2008 LO, central member. // iFit = 4 : MSTW 2008 NLO, central member. (Warning!) class MSTWpdf : public PDF { public: // Constructor. MSTWpdf(int idBeamIn = 2212, int iFitIn = 1, string xmlPath = "../xmldoc/", Info* infoPtr = 0) : PDF(idBeamIn) {init( iFitIn, xmlPath, infoPtr);} private: // Constants: could only be changed in the code itself. static const int np, nx, nq, nqc0, nqb0; static const double xmin, xmax, qsqmin, qsqmax, xxInit[65], qqInit[49]; // Data read in from grid file or set at initialization. int iFit, alphaSorder, alphaSnfmax; double mCharm, mBottom, alphaSQ0, alphaSMZ, distance, tolerance, xx[65], qq[49], c[13][64][48][5][5]; // Initialization of data array. void init( int iFitIn, string xmlPath, Info* infoPtr); // Update PDF values. void xfUpdate(int , double x, double Q2); // Evaluate PDF of one flavour species. double parton(int flavour,double x,double q); double parton_interpolate(int flavour,double xxx,double qqq); double parton_extrapolate(int flavour,double xxx,double qqq); // Auxiliary routines for evaluation. int locate(double xx[],int n,double x); double polderivative1(double x1, double x2, double x3, double y1, double y2, double y3); double polderivative2(double x1, double x2, double x3, double y1, double y2, double y3); double polderivative3(double x1, double x2, double x3, double y1, double y2, double y3); }; //========================================================================== // The CTEQ6pdf class. // Sets available: // iFit = 1 : CTEQ6L // iFit = 2 : CTEQ6L1 // iFit = 3 : CTEQ66.00 (NLO, central member) // iFit = 4 : CT09MC1 // iFit = 5 : CT09MC2 // iFit = 6 : CT09MCS (not yet implemented) class CTEQ6pdf : public PDF { public: // Constructor. CTEQ6pdf(int idBeamIn = 2212, int iFitIn = 1, string xmlPath = "../xmldoc/", Info* infoPtr = 0) : PDF(idBeamIn) {init( iFitIn, xmlPath, infoPtr);} private: // Constants: could only be changed in the code itself. static const double EPSILON, XPOWER; // Data read in from grid file or set at initialization. int iFit, order, nQuark, nfMx, mxVal, nX, nT, nG, iGridX, iGridQ, iGridLX, iGridLQ; double lambda, mQ[7], qIni, qMax, tv[26], xMin, xv[202], upd[57773], xvpow[202], xMinEps, xMaxEps, qMinEps, qMaxEps, fVec[5], tConst[9], xConst[9], xLast, qLast; // Initialization of data array. void init( int iFitIn, string xmlPath, Info* infoPtr); // Update PDF values. void xfUpdate(int id, double x, double Q2); // Evaluate PDF of one flavour species. double parton6(int iParton, double x, double q); // Interpolation in grid. double polint4F(double xgrid[], double fgrid[], double xin); }; //========================================================================== // SA Unresolved proton: equivalent photon spectrum from // V.M. Budnev, I.F. Ginzburg, G.V. Meledin and V.G. Serbo, // Phys. Rept. 15 (1974/1975) 181. class ProtonPoint : public PDF { public: // Constructor. ProtonPoint(int idBeamIn = 2212, Info* infoPtrIn = 0) : PDF(idBeamIn), m_infoPtr(infoPtrIn) {} private: // Stored value for PDF choice. static const double ALPHAEM, Q2MAX, Q20, A, B, C; // Update PDF values. void xfUpdate(int , double x, double Q2); // phi function from Q2 integration. double phiFunc(double x, double Q); // Info and errors Info* m_infoPtr; }; //========================================================================== // Gives the GRV 1992 pi+ (leading order) parton distribution function set // in parametrized form. Authors: Glueck, Reya and Vogt. class GRVpiL : public PDF { public: // Constructor. GRVpiL(int idBeamIn = 221) : PDF(idBeamIn) {} private: // Update PDF values. void xfUpdate(int , double x, double Q2); }; //========================================================================== // Gives generic Q2-independent Pomeron PDF. class PomFix : public PDF { public: // Constructor. PomFix(int idBeamIn = 990, double PomGluonAIn = 0., double PomGluonBIn = 0., double PomQuarkAIn = 0., double PomQuarkBIn = 0., double PomQuarkFracIn = 0., double PomStrangeSuppIn = 0.) : PDF(idBeamIn), PomGluonA(PomGluonAIn), PomGluonB(PomGluonBIn), PomQuarkA(PomQuarkAIn), PomQuarkB(PomQuarkBIn), PomQuarkFrac(PomQuarkFracIn), PomStrangeSupp(PomStrangeSuppIn) {init();} private: // Stored value for PDF choice. double PomGluonA, PomGluonB, PomQuarkA, PomQuarkB, PomQuarkFrac, PomStrangeSupp, normGluon, normQuark; // Initialization of some constants. void init(); // Update PDF values. void xfUpdate(int , double x, double); }; //========================================================================== // The H1 2006 Fit A and Fit B Pomeron parametrization. // H1 Collaboration, A. Aktas et al., "Measurement and QCD Analysis of // the Diffractive Deep-Inelastic Scattering Cross Section at HERA", // DESY-06-049, Eur. Phys. J. C48 (2006) 715. e-Print: hep-ex/0606004. class PomH1FitAB : public PDF { public: // Constructor. PomH1FitAB(int idBeamIn = 990, int iFit = 1, double rescaleIn = 1., string xmlPath = "../xmldoc/", Info* infoPtr = 0) : PDF(idBeamIn) {rescale = rescaleIn; init( iFit, xmlPath, infoPtr);} private: // Limits for grid in x, in Q2, and data in (x, Q2). int nx, nQ2; double rescale, xlow, xupp, dx, Q2low, Q2upp, dQ2; double gluonGrid[100][30]; double quarkGrid[100][30]; // Initialization of data array. void init( int iFit, string xmlPath, Info* infoPtr); // Update PDF values. void xfUpdate(int , double x, double ); }; //========================================================================== // The H1 2007 Jets Pomeron parametrization.. // H1 Collaboration, A. Aktas et al., "Dijet Cross Sections and Parton // Densities in Diffractive DIS at HERA", DESY-07-115, Aug 2007. 33pp. // Published in JHEP 0710:042,2007. e-Print: arXiv:0708.3217 [hep-ex] class PomH1Jets : public PDF { public: // Constructor. PomH1Jets(int idBeamIn = 990, double rescaleIn = 1., string xmlPath = "../xmldoc/", Info* infoPtr = 0) : PDF(idBeamIn) {rescale = rescaleIn; init( xmlPath, infoPtr);} private: // Arrays for grid in x, in Q2, and data in (x, Q2). double rescale; double xGrid[100]; double Q2Grid[88]; double gluonGrid[100][88]; double singletGrid[100][88]; double charmGrid[100][88]; // Initialization of data array. void init( string xmlPath, Info* infoPtr); // Update PDF values. void xfUpdate(int id, double x, double ); }; //========================================================================== // Gives electron (or muon, or tau) parton distribution. class Lepton : public PDF { public: // Constructor. Lepton(int idBeamIn = 11) : PDF(idBeamIn) {} private: // Constants: could only be changed in the code itself. static const double ALPHAEM, ME, MMU, MTAU; // Update PDF values. void xfUpdate(int id, double x, double Q2); // The squared lepton mass, set at initialization. double m2Lep; }; //========================================================================== // Gives electron (or other lepton) parton distribution when unresolved. class LeptonPoint : public PDF { public: // Constructor. LeptonPoint(int idBeamIn = 11) : PDF(idBeamIn) {} private: // Update PDF values in trivial way. void xfUpdate(int , double , double ) {xlepton = 1; xgamma = 0.;} }; //========================================================================== // Gives neutrino parton distribution when unresolved (only choice for now). // Note factor of 2 since only lefthanded implies no spin averaging. class NeutrinoPoint : public PDF { public: // Constructor. NeutrinoPoint(int idBeamIn = 12) : PDF(idBeamIn) {} private: // Update PDF values, with spin factor of 2. void xfUpdate(int , double , double ) {xlepton = 2; xgamma = 0.;} }; //========================================================================== // The NNPDF class. // Sets available: // Leading order QCD+QED Proton PDF sets // iFit = 1 : NNPDF2.3 QCD+QED LO, alphas(MZ) = 0.130 // iFit = 2 : NNPDF2.3 QCD+QED LO, alphas(MZ) = 0.119 // (Next-to-)Next-to-Leading order QCD+QED Proton PDF sets // iFit = 3 : NNPDF2.3 QCD+QED NLO, alphas(MZ) = 0.119 // iFit = 4 : NNPDF2.3 QCD+QED NNLO, alphas(MZ) = 0.119 // Code provided by Juan Rojo and Stefano Carrazza. class NNPDF : public PDF { public: // Constructor. NNPDF(int idBeamIn = 2212, int iFitIn = 1, string xmlPath = "../xmldoc/", Info* infoPtr = 0) : PDF(idBeamIn), fPDFGrid(NULL), fXGrid(NULL), fLogXGrid(NULL), fQ2Grid(NULL), fLogQ2Grid(NULL), fRes(NULL) { init( iFitIn, xmlPath, infoPtr); }; // Destructor. ~NNPDF() { if (fPDFGrid) { for (int i = 0; i < fNFL; i++) { for (int j = 0; j < fNX; j++) if (fPDFGrid[i][j]) delete[] fPDFGrid[i][j]; if (fPDFGrid[i]) delete[] fPDFGrid[i]; } delete[] fPDFGrid; } if (fXGrid) delete[] fXGrid; if (fLogXGrid) delete[] fLogXGrid; if (fQ2Grid) delete[] fQ2Grid; if (fLogQ2Grid) delete[] fLogQ2Grid; if (fRes) delete[] fRes; }; private: // Constants: could only be changed in the code itself. static const double fXMINGRID; // Number of flavors (including photon) and interpolation parameters. static const int fNFL = 14; static const int fM = 4; static const int fN = 2; // Variables to be set during code initialization. int iFit, fNX, fNQ2; double ***fPDFGrid; double *fXGrid; double *fLogXGrid; double *fQ2Grid; double *fLogQ2Grid; double *fRes; // Initialization of data array. void init( int iFitIn, string xmlPath, Info* infoPtr); // Update PDF values. void xfUpdate(int id, double x, double Q2); // Interpolation in the grid for a given PDF flavour. void xfxevolve(double x, double Q2); // 1D and 2D polynomial interpolation. void polint(double xa[], double ya[], int n, double x, double& y, double& dy); void polin2(double x1a[], double x2a[], double ya[][fN], double x1, double x2, double& y, double& dy); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_PartonDistributions_H pythia8-8.1.80.orig/include/Pythia8/Pythia8ToHepMC.h0000644000175000017500000000631412217346230020165 0ustar sunsun// Pythia8ToHepMC.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Author: Mikhail Kirsanov, Mikhail.Kirsanov@cern.ch // Header file for the Pythia8ToHepMC class, // which converts a PYTHIA event record to the standard HepMC format. #ifndef Pythia8_Pythia8ToHepMC_H #define Pythia8_Pythia8ToHepMC_H #include #include "HepMC/IO_BaseClass.h" #include "Pythia8/Pythia.h" namespace HepMC { // Forward references to some classes. class GenEvent; class GenVertex; class GenParticle; //========================================================================== // The Pythia8ToHepMC class. class Pythia8ToHepMC : public IO_BaseClass { public: // Constructor and destructor. Pythia8ToHepMC() : m_internal_event_number(0), m_print_inconsistency(true), m_free_parton_warnings(true), m_crash_on_problem(false), m_convert_gluon_to_0(false), m_store_pdf(true), m_store_proc(true), m_store_xsec(true) {;} virtual ~Pythia8ToHepMC() {;} // The recommended method to convert Pythia events into HepMC ones. bool fill_next_event( Pythia8::Pythia& pythia, GenEvent* evt, int ievnum = -1 ) {return fill_next_event( pythia.event, evt, ievnum, &pythia.info, &pythia.settings);} // Alternative method to convert Pythia events into HepMC ones. bool fill_next_event( Pythia8::Event& pyev, GenEvent* evt, int ievnum = -1, Pythia8::Info* pyinfo = 0, Pythia8::Settings* pyset = 0); // Read out values for some switches. bool print_inconsistency() const {return m_print_inconsistency;} bool free_parton_warnings() const {return m_free_parton_warnings;} bool crash_on_problem() const {return m_crash_on_problem;} bool convert_gluon_to_0() const {return m_convert_gluon_to_0;} bool store_pdf() const {return m_store_pdf;} bool store_proc() const {return m_store_proc;} bool store_xsec() const {return m_store_xsec;} // Set values for some switches. void set_print_inconsistency(bool b = true) {m_print_inconsistency = b;} void set_free_parton_warnings(bool b = true) {m_free_parton_warnings = b;} void set_crash_on_problem(bool b = false) {m_crash_on_problem = b;} void set_convert_gluon_to_0(bool b = false) {m_convert_gluon_to_0 = b;} void set_store_pdf(bool b = true) {m_store_pdf = b;} void set_store_proc(bool b = true) {m_store_proc = b;} void set_store_xsec(bool b = true) {m_store_xsec = b;} private: // Following methods are not implemented for this class. virtual bool fill_next_event( GenEvent* ) { return 0; } virtual void write_event( const GenEvent* ) {;} // Use of copy constructor is not allowed. Pythia8ToHepMC( const Pythia8ToHepMC& ) : IO_BaseClass() {;} // Data members. int m_internal_event_number; bool m_print_inconsistency, m_free_parton_warnings, m_crash_on_problem, m_convert_gluon_to_0, m_store_pdf, m_store_proc, m_store_xsec; }; //========================================================================== } // end namespace HepMC #endif // end Pythia8_Pythia8ToHepMC_H pythia8-8.1.80.orig/include/Pythia8/SigmaLeftRightSym.h0000644000175000017500000001716312217346231021026 0ustar sunsun// SigmaLeftRightSym.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for left-rights-symmetry differential cross sections. // Contains classes derived from SigmaProcess via Sigma(1/2/3)Process. #ifndef Pythia8_SigmaLeftRightSym_H #define Pythia8_SigmaLeftRightSym_H #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // A derived class for f fbar -> Z_R^0 (righthanded gauge boson). class Sigma1ffbar2ZRight : public Sigma1Process { public: // Constructor. Sigma1ffbar2ZRight() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for G* decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar -> Z_R^0";} virtual int code() const {return 3101;} virtual string inFlux() const {return "ffbarSame";} virtual int resonanceA() const {return idZR;} private: // Parameters set at initialization or for current kinematics. int idZR; double mRes, GammaRes, m2Res, GamMRat, sin2tW, sigma0; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* ZRPtr; }; //========================================================================== // A derived class for f fbar' -> W_R^+- (righthanded gauge boson). class Sigma1ffbar2WRight : public Sigma1Process { public: // Constructor. Sigma1ffbar2WRight() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar' -> W_R^+-";} virtual int code() const {return 3102;} virtual string inFlux() const {return "ffbarChg";} virtual int resonanceA() const {return idWR;} private: // Parameters set at initialization. int idWR; double mRes, GammaRes, m2Res, GamMRat, thetaWRat, sigma0Pos, sigma0Neg; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* particlePtr; }; //========================================================================== // A derived class for l l -> H_L^++-- or H_R^++-- (doubly charged Higgs). class Sigma1ll2Hchgchg : public Sigma1Process { public: // Constructor. Sigma1ll2Hchgchg(int leftRightIn ) : leftRight(leftRightIn) {} // Initialize process. virtual void initProc(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ff";} virtual int resonanceA() const {return idHLR;} private: // Parameters set at initialization. int leftRight, idHLR, codeSave; string nameSave; double mRes, GammaRes, m2Res, GamMRat, yukawa[4][4]; // Pointer to properties of the particle species, to access decay channels. ParticleDataEntry* particlePtr; }; //========================================================================== // A derived class for l- gamma -> H_(L/R)^-- l+ (doubly charged Higgs). class Sigma2lgm2Hchgchgl : public Sigma2Process { public: // Constructor. Sigma2lgm2Hchgchgl(int leftRightIn, int idLepIn ) : leftRight(leftRightIn), idLep(idLepIn) {} // Initialize process. virtual void initProc(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "fgm";} virtual int resonanceA() const {return idHLR;} private: // Parameters set at initialization. int leftRight, idHLR, idLep, codeSave; string nameSave; double yukawa[4], openFracPos, openFracNeg; }; //========================================================================== // A derived class for f_1 f_2 -> H_(L/R)^++-- f_3 f_4 (W+- W+- fusion). class Sigma3ff2HchgchgfftWW : public Sigma3Process { public: // Constructor. Sigma3ff2HchgchgfftWW(int leftRightIn) : leftRight(leftRightIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ff";} virtual int id3Mass() const {return idHLR;} // Instructions for 3-body phase space with t-channel propagators. virtual int idTchan1() const {return 9900024;} virtual int idTchan2() const {return 9900024;} virtual double tChanFracPow1() const {return 0.05;} virtual double tChanFracPow2() const {return 0.9;} virtual bool useMirrorWeight() const {return true;} private: // Store standard prefactor. int leftRight, idHLR, codeSave; string nameSave; double mWS, prefac, sigma0TU, sigma0T, openFracPos, openFracNeg; }; //========================================================================== // A derived class for f fbar -> H_(L/R)^++ H_(L/R)^-- (doubly charged Higgs). class Sigma2ffbar2HchgchgHchgchg : public Sigma2Process { public: // Constructor. Sigma2ffbar2HchgchgHchgchg(int leftRightIn) : leftRight(leftRightIn) {} // Initialize process. virtual void initProc(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angle. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ffbarSame";} virtual int id3Mass() const {return idHLR;} virtual int id4Mass() const {return idHLR;} virtual int resonanceA() const {return 23;} private: // Parameters set at initialization. int leftRight, idHLR, codeSave; string nameSave; double mRes, GammaRes, m2Res, GamMRat, sin2tW, preFac, yukawa[4][4], openFrac; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaLeftRightSym_H pythia8-8.1.80.orig/include/Pythia8/SLHAinterface.h0000644000175000017500000000407012217346232020066 0ustar sunsun// SLHAinterface.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // Main authors of this file: N. Desai, P. Skands // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for SUSY Les Houches Accord Interface. // Handles the communication between PYTHIA and the SusyLesHouches classes. #ifndef Pythia8_SLHAinterface_H #define Pythia8_SLHAinterface_H #include "Pythia8/Basics.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" #include "Pythia8/StandardModel.h" #include "Pythia8/SusyCouplings.h" #include "Pythia8/SusyLesHouches.h" namespace Pythia8 { //========================================================================== // The SLHAinterface class handles communication between Pythia and // SusyLesHouches. class SLHAinterface { public: // Constructor. SLHAinterface() {} ; // Set pointers void setPtr( Info* infoPtrIn ) {infoPtr = infoPtrIn;} // Initialize and switch to SUSY couplings if reading SLHA spectrum void init( Settings& settings, Rndm* rndmPtr, Couplings* couplingsPtrIn, ParticleData* particleDataPtr, bool& useSHLAcouplings ); // Initialize SUSY Les Houches Accord data. bool initSLHA(Settings& settings, ParticleData* particleDataPtr); // Initialize SLHA blocks SMINPUTS and MASS from PYTHIA SM parameter values. // E.g., to make sure that there are no important unfilled entries void pythia2slha(ParticleData* particleDataPtr); // SusyLesHouches - SLHA object for interface to SUSY spectra. SusyLesHouches slha; // SLHA derived couplings class and pointer to Couplings object CoupSUSY coupSUSY; Couplings* couplingsPtr; // Pointers to PYTHIA objects Info* infoPtr; Settings* settingsPtr; // Internal data members int meMode; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SLHAinterface_H pythia8-8.1.80.orig/include/Pythia8/Settings.h0000644000175000017500000002361212217346231017260 0ustar sunsun// Settings.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for the settings database. // Flag: helper class with bool flags. // Mode: helper class with int modes. // Parm: (short for parameter) helper class with double parameters. // Word: helper class with string words. // MVec: vector of Modes (integers). // PVec: vector of Parms (doubles). // Settings: maps of flags, modes, parms and words with input/output. #ifndef Pythia8_Settings_H #define Pythia8_Settings_H #include "Pythia8/Info.h" #include "Pythia8/PythiaStdlib.h" namespace Pythia8 { //========================================================================== // Class for bool flags. class Flag { public: // Constructor Flag(string nameIn = " ", bool defaultIn = false) : name(nameIn), valNow(defaultIn) , valDefault(defaultIn) { } // Data members. string name; bool valNow, valDefault; }; //========================================================================== // Class for integer modes. class Mode { public: // Constructor Mode(string nameIn = " ", int defaultIn = 0, bool hasMinIn = false, bool hasMaxIn = false, int minIn = 0, int maxIn = 0) : name(nameIn), valNow(defaultIn), valDefault(defaultIn), hasMin(hasMinIn), hasMax(hasMaxIn), valMin(minIn), valMax(maxIn) { } // Data members. string name; int valNow, valDefault; bool hasMin, hasMax; int valMin, valMax; }; //========================================================================== // Class for double parms (where parm is shorthand for parameter). class Parm { public: // Constructor Parm(string nameIn = " ", double defaultIn = 0., bool hasMinIn = false, bool hasMaxIn = false, double minIn = 0., double maxIn = 0.) : name(nameIn), valNow(defaultIn), valDefault(defaultIn), hasMin(hasMinIn), hasMax(hasMaxIn), valMin(minIn), valMax(maxIn) { } // Data members. string name; double valNow, valDefault; bool hasMin, hasMax; double valMin, valMax; }; //========================================================================== // Class for string words. class Word { public: // Constructor Word(string nameIn = " ", string defaultIn = " ") : name(nameIn), valNow(defaultIn) , valDefault(defaultIn) { } // Data members. string name, valNow, valDefault; }; //========================================================================== // Class for vector of integers. class MVec { public: // Constructor MVec(string nameIn = " ", vector defaultIn = vector(1, 0), bool hasMinIn = false, bool hasMaxIn = false, int minIn = 0, int maxIn = 0) : name(nameIn), valNow(defaultIn), valDefault(defaultIn), hasMin(hasMinIn), hasMax(hasMaxIn), valMin(minIn), valMax(maxIn) { } // Data members. string name; vector valNow, valDefault; bool hasMin, hasMax; int valMin, valMax; }; //========================================================================== // Class for vector of doubles. class PVec { public: // Constructor PVec(string nameIn = " ", vector defaultIn = vector(1, 0.), bool hasMinIn = false, bool hasMaxIn = false, double minIn = 0., double maxIn = 0.) : name(nameIn), valNow(defaultIn), valDefault(defaultIn), hasMin(hasMinIn), hasMax(hasMaxIn), valMin(minIn), valMax(maxIn) { } // Data members. string name; vector valNow, valDefault; bool hasMin, hasMax; double valMin, valMax; }; //========================================================================== // This class holds info on flags (bool), modes (int), parms (double), // words (string), mvecs (vector of int) and pvecs (vector of double). class Settings { public: // Constructor. Settings() : isInit(false), readingFailedSave(false) {} // Initialize Info pointer. void initPtr(Info* infoPtrIn) {infoPtr = infoPtrIn;} // Read in database from specific file. bool init(string startFile = "../xmldoc/Index.xml", bool append = false, ostream& os = cout) ; // Overwrite existing database by reading from specific file. bool reInit(string startFile = "../xmldoc/Index.xml", ostream& os = cout) ; // Read in one update from a single line. bool readString(string line, bool warn = true, ostream& os = cout) ; // Keep track whether any readings have failed, invalidating run setup. bool readingFailed() {return readingFailedSave;} // Write updates or everything to user-defined file. bool writeFile(string toFile, bool writeAll = false) ; bool writeFile(ostream& os = cout, bool writeAll = false) ; // Print out table of database, either all or only changed ones, // or ones containing a given string. void listAll(ostream& os = cout) { list( true, false, " ", os); } void listChanged(ostream& os = cout) { list (false, false, " ", os); } void list(string match, ostream& os = cout) { list (false, true, match, os); } // Reset all values to their defaults. void resetAll() ; // Query existence of an entry. bool isFlag(string keyIn) { return (flags.find(toLower(keyIn)) != flags.end()); } bool isMode(string keyIn) { return (modes.find(toLower(keyIn)) != modes.end()); } bool isParm(string keyIn) { return (parms.find(toLower(keyIn)) != parms.end()); } bool isWord(string keyIn) { return (words.find(toLower(keyIn)) != words.end()); } bool isMVec(string keyIn) { return (mvecs.find(toLower(keyIn)) != mvecs.end()); } bool isPVec(string keyIn) { return (pvecs.find(toLower(keyIn)) != pvecs.end()); } // Add new entry. void addFlag(string keyIn, bool defaultIn) { flags[toLower(keyIn)] = Flag(keyIn, defaultIn); } void addMode(string keyIn, int defaultIn, bool hasMinIn, bool hasMaxIn, int minIn, int maxIn) { modes[toLower(keyIn)] = Mode(keyIn, defaultIn, hasMinIn, hasMaxIn, minIn, maxIn); } void addParm(string keyIn, double defaultIn, bool hasMinIn, bool hasMaxIn, double minIn, double maxIn) { parms[toLower(keyIn)] = Parm(keyIn, defaultIn, hasMinIn, hasMaxIn, minIn, maxIn); } void addWord(string keyIn, string defaultIn) { words[toLower(keyIn)] = Word(keyIn, defaultIn); } void addMVec(string keyIn, vector defaultIn, bool hasMinIn, bool hasMaxIn, int minIn, int maxIn) { mvecs[toLower(keyIn)] = MVec(keyIn, defaultIn, hasMinIn, hasMaxIn, minIn, maxIn); } void addPVec(string keyIn, vector defaultIn, bool hasMinIn, bool hasMaxIn, double minIn, double maxIn) { pvecs[toLower(keyIn)] = PVec(keyIn, defaultIn, hasMinIn, hasMaxIn, minIn, maxIn); } // Give back current value, with check that key exists. bool flag(string keyIn); int mode(string keyIn); double parm(string keyIn); string word(string keyIn); vector mvec(string keyIn); vector pvec(string keyIn); // Give back default value, with check that key exists. bool flagDefault(string keyIn); int modeDefault(string keyIn); double parmDefault(string keyIn); string wordDefault(string keyIn); vector mvecDefault(string keyIn); vector pvecDefault(string keyIn); // Give back a map of all entries whose names match the string "match". map getFlagMap(string match); map getModeMap(string match); map getParmMap(string match); map getWordMap(string match); map getMVecMap(string match); map getPVecMap(string match); // Change current value, respecting limits. void flag(string keyIn, bool nowIn); void mode(string keyIn, int nowIn); void parm(string keyIn, double nowIn); void word(string keyIn, string nowIn); void mvec(string keyIn, vector nowIn); void pvec(string keyIn, vector nowIn); // Change current value, disregarding limits. void forceMode(string keyIn, int nowIn); void forceParm(string keyIn, double nowIn); void forceMVec(string keyIn, vector nowIn); void forcePVec(string keyIn, vector nowIn); // Restore current value to default. void resetFlag(string keyIn); void resetMode(string keyIn); void resetParm(string keyIn); void resetWord(string keyIn); void resetMVec(string keyIn); void resetPVec(string keyIn); private: // Pointer to various information on the generation. Info* infoPtr; // Map for bool flags. map flags; // Map for integer modes. map modes; // Map for double parms. map parms; // Map for string words. map words; // Map for vectors of int. map mvecs; // Map for vectors of double. map pvecs; // Flags that initialization has been performed; whether any failures. bool isInit, readingFailedSave; // Print out table of database, called from listAll and listChanged. void list(bool doListAll, bool doListString, string match, ostream& os = cout); // Master switch for program printout. void printQuiet(bool quiet); // Restore settings used in tunes to e+e- and pp/ppbar data. void resetTuneEE(); void resetTunePP(); // Initialize tunes to e+e- and pp/ppbar data. void initTuneEE(int eeTune); void initTunePP(int ppTune); // Useful functions for string handling. string toLower(const string& name); bool boolString(string tag); string attributeValue(string line, string attribute); bool boolAttributeValue(string line, string attribute); int intAttributeValue(string line, string attribute); double doubleAttributeValue(string line, string attribute); vector intVectorAttributeValue(string line, string attribute); vector doubleVectorAttributeValue(string line, string attribute); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_Settings_H pythia8-8.1.80.orig/include/Pythia8/SigmaQCD.h0000644000175000017500000005252712217346231017057 0ustar sunsun// SigmaQCD.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for QCD process differential cross sections. // Contains classes derived from SigmaProcess via Sigma(0/2)Process. #ifndef Pythia8_SigmaQCD_H #define Pythia8_SigmaQCD_H #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // A derived class for minimum-bias (inelastic, nondiffractive) events. class Sigma0nonDiffractive : public Sigma0Process { public: // Constructor. Sigma0nonDiffractive() {} // Evaluate sigma. virtual double sigmaHat() {return sigmaTotPtr->sigmaND();} // Select flavour, colour and anticolour. virtual void setIdColAcol() {} // Info on the subprocess. virtual string name() const {return "non-diffractive";} virtual int code() const {return 101;} virtual bool isNonDiff() const {return true;} private: }; //========================================================================== // A derived class for elastic scattering A B -> A B. class Sigma0AB2AB : public Sigma0Process { public: // Constructor. Sigma0AB2AB() {} // Evaluate sigma. virtual double sigmaHat() {return sigmaTotPtr->sigmaEl();} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "A B -> A B elastic";} virtual int code() const {return 102;} virtual bool isResolved() const {return false;} private: }; //========================================================================== // A derived class for single diffractive scattering A B -> X B. class Sigma0AB2XB : public Sigma0Process { public: // Constructor. Sigma0AB2XB() {} // Evaluate sigma. virtual double sigmaHat() {return sigmaTotPtr->sigmaXB();} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "A B -> X B single diffractive";} virtual int code() const {return 103;} virtual bool isResolved() const {return false;} virtual bool isDiffA() const {return true;}; private: }; //========================================================================== // A derived class for single diffractive scattering A B -> A X. class Sigma0AB2AX : public Sigma0Process { public: // Constructor. Sigma0AB2AX() {} // Evaluate sigma. virtual double sigmaHat() {return sigmaTotPtr->sigmaAX();} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "A B -> A X single diffractive";} virtual int code() const {return 104;} virtual bool isResolved() const {return false;} virtual bool isDiffB() const {return true;}; private: }; //========================================================================== // A derived class for double diffractive scattering A B -> X X. class Sigma0AB2XX : public Sigma0Process { public: // Constructor. Sigma0AB2XX() {} // Evaluate sigma. virtual double sigmaHat() {return sigmaTotPtr->sigmaXX();} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "A B -> X X double diffractive";} virtual int code() const {return 105;} virtual bool isResolved() const {return false;} virtual bool isDiffA() const {return true;}; virtual bool isDiffB() const {return true;}; private: }; //========================================================================== // A derived class for central diffractive scattering A B -> A X B. class Sigma0AB2AXB : public Sigma0Process { public: // Constructor. Sigma0AB2AXB() {} // Evaluate sigma. virtual double sigmaHat() {return sigmaTotPtr->sigmaAXB();} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "A B -> A X B central diffractive";} virtual int code() const {return 106;} virtual int nFinal() const {return 3;} virtual bool isResolved() const {return false;} virtual bool isDiffC() const {return true;}; private: }; //========================================================================== // A derived class for g g -> g g. class Sigma2gg2gg : public Sigma2Process { public: // Constructor. Sigma2gg2gg() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "g g -> g g";} virtual int code() const {return 111;} virtual string inFlux() const {return "gg";} private: // Values stored for colour flow selection. double sigTS, sigUS, sigTU, sigSum, sigma; }; //========================================================================== // A derived class for g g -> q qbar (q = u, d, s, i.e. almost massless). class Sigma2gg2qqbar : public Sigma2Process { public: // Constructor. Sigma2gg2qqbar() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "g g -> q qbar (uds)";} virtual int code() const {return 112;} virtual string inFlux() const {return "gg";} private: // Number of quarks to be considered in massless approximation. int nQuarkNew; // Values stored for colour flow selection. int idNew; double mNew, m2New, sigTS, sigUS, sigSum, sigma; }; //========================================================================== // A derived class for q g -> q g (q = u, d, s, c, b). // Use massless approximation also for Q since no alternative. class Sigma2qg2qg : public Sigma2Process { public: // Constructor. Sigma2qg2qg() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q g -> q g";} virtual int code() const {return 113;} virtual string inFlux() const {return "qg";} private: // Values stored for colour flow selection. double sigTS, sigTU, sigSum, sigma; }; //========================================================================== // A derived class for q qbar' -> q qbar' or q q' -> q q' // (qbar qbar' -> qbar qbar'), q' may be same as q. class Sigma2qq2qq : public Sigma2Process { public: // Constructor. Sigma2qq2qq() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q q(bar)' -> q q(bar)'";} virtual int code() const {return 114;} virtual string inFlux() const {return "qq";} private: // Values stored for colour flow selection. double sigT, sigU, sigTU, sigST, sigSum; }; //========================================================================== // A derived class for q qbar -> g g. class Sigma2qqbar2gg : public Sigma2Process { public: // Constructor. Sigma2qqbar2gg() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> g g";} virtual int code() const {return 115;} virtual string inFlux() const {return "qqbarSame";} private: // Values stored for colour flow selection. double sigTS, sigUS, sigSum, sigma; }; //========================================================================== // A derived class for q qbar -> q' qbar'. class Sigma2qqbar2qqbarNew : public Sigma2Process { public: // Constructor. Sigma2qqbar2qqbarNew() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> q' qbar' (uds)";} virtual int code() const {return 116;} virtual string inFlux() const {return "qqbarSame";} private: // Number of quarks to be considered in massless approximation. int nQuarkNew; // Values stored for colour flow selection. int idNew; double mNew, m2New, sigS, sigma; }; //========================================================================== // A derived class for g g -> Q Qbar (Q = c, b or t). class Sigma2gg2QQbar : public Sigma2Process { public: // Constructor. Sigma2gg2QQbar(int idIn, int codeIn) : idNew(idIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angles in top decay (else inactive). virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return idNew;} virtual int id4Mass() const {return idNew;} private: // Values stored for process type and colour flow selection. int idNew, codeSave; string nameSave; double sigTS, sigUS, sigSum, sigma, openFracPair; }; //========================================================================== // A derived class for q qbar -> Q Qbar (Q = c, b or t). class Sigma2qqbar2QQbar : public Sigma2Process { public: // Constructor. Sigma2qqbar2QQbar(int idIn, int codeIn) : idNew(idIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for W decay angles in top decay (else inactive). virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return idNew;} virtual int id4Mass() const {return idNew;} private: // Values stored for process type. int idNew, codeSave; string nameSave; double sigma, openFracPair; }; //========================================================================== // A derived class for g g -> g g g. class Sigma3gg2ggg : public Sigma3Process { public: // Constructor. Sigma3gg2ggg() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "g g -> g g g";} virtual int code() const {return 131;} virtual int nFinal() const {return 3;} virtual string inFlux() const {return "gg";} virtual bool isQCD3body() const {return true;} private: // Values stored for colour flow selection. double sigma; // Intermediate storage and calculation of four-products. double pp[6][6]; double cycle(int i1, int i2, int i3, int i4, int i5) {return pp[i1][i2] * pp[i2][i3] * pp[i3][i4] * pp[i4][i5] * pp[i5][i1];} }; //========================================================================== // A derived class for q qbar -> g g g. class Sigma3qqbar2ggg : public Sigma3Process { public: // Constructor. Sigma3qqbar2ggg() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> g g g";} virtual int code() const {return 132;} virtual int nFinal() const {return 3;} virtual string inFlux() const {return "qqbarSame";} virtual bool isQCD3body() const {return true;} protected: // Pick/map a random final state configuration int config; inline void pickFinal() { config = int( 6 * rndmPtr->flat() ); } inline void mapFinal(); // |M|^2 calculation inline double m2Calc(); // Four-vectors for |M|^2 calculation Vec4 pCM[5]; // Intermediate storage and calculation of four-products double a[3], b[3], pp[3][3], ab[3][3]; // Values stored for colour flow selection. double sigma; }; //========================================================================== // A derived class for q g -> q g g // Derived from Sigma3qqbar2ggg class Sigma3qg2qgg : public Sigma3qqbar2ggg { public: // Constructor. Sigma3qg2qgg() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q g -> q g g";} virtual int code() const {return 133;} virtual int nFinal() const {return 3;} virtual string inFlux() const {return "qg";} virtual bool isQCD3body() const {return true;} private: // Sigma for (qg) and (gq) incoming double sigma[2]; }; //========================================================================== // A derived class for g g -> q qbar g // Derived from Sigma3qqbar2ggg class Sigma3gg2qqbarg : public Sigma3qqbar2ggg { public: // Constructor. Sigma3gg2qqbarg() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "g g -> q qbar g";} virtual int code() const {return 138;} virtual int nFinal() const {return 3;} virtual string inFlux() const {return "gg";} virtual bool isQCD3body() const {return true;} private: // Number of quarks to be considered in massless approximation. int nQuarkNew; }; //========================================================================== // A derived class for q q' -> q q' g class Sigma3qq2qqgDiff : public Sigma3Process { public: // Constructor. Sigma3qq2qqgDiff() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q(bar) q(bar)' -> q(bar) q(bar)' g";} virtual int code() const {return 134;} virtual int nFinal() const {return 3;} virtual string inFlux() const {return "qq";} virtual bool isQCD3body() const {return true;} protected: // Pick/map a random final state configuration int config; inline void pickFinal() { config = int( 6 * rndmPtr->flat() ); } inline void mapFinal(); // |M|^2 calculation inline double m2Calc(); // Kinematic configuration Vec4 pCM[5]; // Four-products double s, t, u, sp, tp, up; // Cross section double sigma; }; //========================================================================== // A derived class for q qbar -> q' qbar' g // Derived from Sigma3qq2qqgDiff class Sigma3qqbar2qqbargDiff : public Sigma3qq2qqgDiff { public: // Constructor. Sigma3qqbar2qqbargDiff() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> q' qbar' g";} virtual int code() const {return 136;} virtual int nFinal() const {return 3;} virtual string inFlux() const {return "qqbarSame";} virtual bool isQCD3body() const {return true;} private: // Number of quarks to be considered in massless approximation. int nQuarkNew; }; //========================================================================== // A derived class for q g -> q q' qbar' // Derived from Sigma3qq2qqgDiff class Sigma3qg2qqqbarDiff : public Sigma3qq2qqgDiff { public: // Constructor. Sigma3qg2qqqbarDiff() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q g -> q q' qbar'";} virtual int code() const {return 139;} virtual int nFinal() const {return 3;} virtual string inFlux() const {return "qg";} virtual bool isQCD3body() const {return true;} private: // Number of quarks to be considered in massless approximation. int nQuarkNew; // gq and qg incoming double sigma[2]; }; //========================================================================== // A derived class for q q -> q q g class Sigma3qq2qqgSame : public Sigma3Process { public: // Constructor. Sigma3qq2qqgSame() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q(bar) q(bar) -> q(bar) q(bar) g";} virtual int code() const {return 135;} virtual int nFinal() const {return 3;} virtual string inFlux() const {return "qq";} virtual bool isQCD3body() const {return true;} protected: // Pick/map a random final state configuration int config; inline void pickFinal() { config = int( 6 * rndmPtr->flat() ); } inline void mapFinal(); // |M|^2 calculation inline double m2Calc(); // Kinematic configuration Vec4 pCM[5]; // Four-products double s, t, u, sp, tp, up; double ssp, ttp, uup, s_sp, t_tp, u_up; // Cross section double sigma; }; //========================================================================== // A derived class for q q -> q q g // Derived from Sigma3qq2qqgSame class Sigma3qqbar2qqbargSame : public Sigma3qq2qqgSame { public: // Constructor. Sigma3qqbar2qqbargSame() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q qbar -> q qbar g";} virtual int code() const {return 137;} virtual int nFinal() const {return 3;} virtual string inFlux() const {return "qqbarSame";} virtual bool isQCD3body() const {return true;} private: }; //========================================================================== // A derived class for q g -> q qbar q; same flavour. // Derived from Sigma3qq2qqgSame class Sigma3qg2qqqbarSame : public Sigma3qq2qqgSame { public: // Constructor. Sigma3qg2qqqbarSame() {} // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return "q g -> q q qbar";} virtual int code() const {return 140;} virtual int nFinal() const {return 3;} virtual string inFlux() const {return "qg";} virtual bool isQCD3body() const {return true;} private: // gq and qg incoming double sigma[2]; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaQCD_H pythia8-8.1.80.orig/include/Pythia8/FJcore.h0000644000175000017500000020676712217346226016652 0ustar sunsun// fjcore -- extracted from FastJet v3.0.5 (http://fastjet.fr) // // fjcore constitutes a digest of the main FastJet functionality. // The files fjcore.hh and fjcore.cc are meant to provide easy access to these // core functions, in the form of single files and without the need of a full // FastJet installation: // // g++ main.cc fjcore.cc // // with main.cc including fjcore.hh. // // The results are expected to be identical to those obtained by linking to // the full FastJet distribution. // // NOTE THAT, IN ORDER TO MAKE IT POSSIBLE FOR FJCORE AND THE FULL FASTJET // TO COEXIST, THE FORMER USES THE "fjcore" NAMESPACE INSTEAD OF "fastjet". // // In particular, fjcore provides: // // - access to all native pp and ee algorithms, kt, anti-kt, C/A. // For C/A, the NlnN method is available, while anti-kt and kt // are limited to the N^2 one (still the fastest for N < 20k particles) // - access to selectors, for implementing cuts and selections // - access to all functionalities related to pseudojets (e.g. a jet's // structure or user-defined information) // // Instead, it does NOT provide: // // - jet areas functionality // - background estimation // - access to other algorithms via plugins // - interface to CGAL // - fastjet tools, e.g. filters, taggers // // If these functionalities are needed, the full FastJet installation must be // used. The code will be fully compatible, with the sole replacement of the // header files and of the fjcore namespace with the fastjet one. // // fjcore.hh and fjcore.cc are not meant to be human-readable. // For documentation, see the full FastJet manual and doxygen at http://fastjet.fr // // Like FastJet, fjcore is released under the terms of the GNU General Public // License version 2 (GPLv2). If you use this code as part of work towards a // scientific publication, whether directly or contained within another program // (e.g. Delphes, SpartyJet, Rivet, LHC collaboration software frameworks, // etc.), you should include a citation to // // EPJC72(2012)1896 [arXiv:1111.6097] (FastJet User Manual) // and, optionally, Phys.Lett.B641 (2006) 57 [arXiv:hep-ph/0512210] // // Copyright (c) 2005-2013, Matteo Cacciari, Gavin P. Salam and Gregory Soyez // //---------------------------------------------------------------------- // This file is part of FastJet. // // FastJet is free software; you can redistribute it and/or modify // it under the terms of the GNU General Public License as published by // the Free Software Foundation; either version 2 of the License, or // (at your option) any later version. // // The algorithms that underlie FastJet have required considerable // development and are described in hep-ph/0512210. If you use // FastJet as part of work towards a scientific publication, please // include a citation to the FastJet paper. // // FastJet is distributed in the hope that it will be useful, // but WITHOUT ANY WARRANTY; without even the implied warranty of // MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the // GNU General Public License for more details. // // You should have received a copy of the GNU General Public License // along with FastJet. If not, see . //---------------------------------------------------------------------- // #ifndef __FJCORE_HH__ #define __FJCORE_HH__ #define __FJCORE__ // remove all the non-core code (a safekeeper) #define __FJCORE_DROP_CGAL // disable CGAL support #ifndef __FJCORE_FASTJET_BASE_HH__ #define __FJCORE_FASTJET_BASE_HH__ #define FJCORE_BEGIN_NAMESPACE namespace fjcore { #define FJCORE_END_NAMESPACE } #endif // __FJCORE_FASTJET_BASE_HH__ #ifndef __FJCORE_NUMCONSTS__ #define __FJCORE_NUMCONSTS__ FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh const double pi = 3.141592653589793238462643383279502884197; const double twopi = 6.283185307179586476925286766559005768394; const double pisq = 9.869604401089358618834490999876151135314; const double zeta2 = 1.644934066848226436472415166646025189219; const double zeta3 = 1.202056903159594285399738161511449990765; const double eulergamma = 0.577215664901532860606512090082402431042; const double ln2 = 0.693147180559945309417232121458176568076; FJCORE_END_NAMESPACE #endif // __FJCORE_NUMCONSTS__ #ifndef __FJCORE_INTERNAL_IS_BASE_HH__ #define __FJCORE_INTERNAL_IS_BASE_HH__ FJCORE_BEGIN_NAMESPACE template struct integral_type{ static const T value = _t; ///< the value (only member carrying info) typedef T value_type; ///< a typedef for the type T typedef integral_type type; ///< a typedef for the whole structure }; template const T integral_type::value; typedef integral_type true_type; ///< the bool 'true' value promoted to a type typedef integral_type false_type; ///< the bool 'false' value promoted to a type typedef char (&__yes_type)[1]; //< the yes type typedef char (&__no_type) [2]; //< the no type template struct __inheritance_helper{ #if !((_MSC_VER !=0 ) && (_MSC_VER == 1310)) // MSVC 7.1 template static __yes_type check_sig(D const volatile *, T); #else static __yes_type check_sig(D const volatile *, long); #endif static __no_type check_sig(B const volatile *, int); }; template struct IsBaseAndDerived{ #if ((_MSC_FULL_VER != 0) && (_MSC_FULL_VER >= 140050000)) #pragma warning(push) #pragma warning(disable:6334) #endif struct Host{ #if !((_MSC_VER !=0 ) && (_MSC_VER == 1310)) operator B const volatile *() const; #else operator B const volatile * const&() const; #endif operator D const volatile *(); }; static const bool value = ((sizeof(B)!=0) && (sizeof(D)!=0) && (sizeof(__inheritance_helper::check_sig(Host(), 0)) == sizeof(__yes_type))); #if ((_MSC_FULL_VER != 0) && (_MSC_FULL_VER >= 140050000)) #pragma warning(pop) #endif }; template B* cast_if_derived(D* d){ return IsBaseAndDerived::value ? (B*)(d) : 0; } FJCORE_END_NAMESPACE #endif // __IS_BASE_OF_HH__ #ifndef _INCLUDE_FJCORE_CONFIG_AUTO_H #define _INCLUDE_FJCORE_CONFIG_AUTO_H 1 #ifndef FJCORE_HAVE_DLFCN_H #define FJCORE_HAVE_DLFCN_H 1 #endif #ifndef FJCORE_HAVE_EXECINFO_H #define FJCORE_HAVE_EXECINFO_H 1 #endif #ifndef FJCORE_HAVE_INTTYPES_H #define FJCORE_HAVE_INTTYPES_H 1 #endif #ifndef FJCORE_HAVE_LIBM #define FJCORE_HAVE_LIBM 1 #endif #ifndef FJCORE_HAVE_MEMORY_H #define FJCORE_HAVE_MEMORY_H 1 #endif #ifndef FJCORE_HAVE_STDINT_H #define FJCORE_HAVE_STDINT_H 1 #endif #ifndef FJCORE_HAVE_STDLIB_H #define FJCORE_HAVE_STDLIB_H 1 #endif #ifndef FJCORE_HAVE_STRINGS_H #define FJCORE_HAVE_STRINGS_H 1 #endif #ifndef FJCORE_HAVE_STRING_H #define FJCORE_HAVE_STRING_H 1 #endif #ifndef FJCORE_HAVE_SYS_STAT_H #define FJCORE_HAVE_SYS_STAT_H 1 #endif #ifndef FJCORE_HAVE_SYS_TYPES_H #define FJCORE_HAVE_SYS_TYPES_H 1 #endif #ifndef FJCORE_HAVE_UNISTD_H #define FJCORE_HAVE_UNISTD_H 1 #endif #ifndef FJCORE_LT_OBJDIR #define FJCORE_LT_OBJDIR ".libs/" #endif #ifndef FJCORE_PACKAGE #define FJCORE_PACKAGE "fastjet" #endif #ifndef FJCORE_PACKAGE_BUGREPORT #define FJCORE_PACKAGE_BUGREPORT "" #endif #ifndef FJCORE_PACKAGE_NAME #define FJCORE_PACKAGE_NAME "FastJet" #endif #ifndef FJCORE_PACKAGE_STRING #define FJCORE_PACKAGE_STRING "FastJet 3.0.5" #endif #ifndef FJCORE_PACKAGE_TARNAME #define FJCORE_PACKAGE_TARNAME "fastjet" #endif #ifndef FJCORE_PACKAGE_VERSION #define FJCORE_PACKAGE_VERSION "3.0.5" #endif #ifndef FJCORE_STDC_HEADERS #define FJCORE_STDC_HEADERS 1 #endif #ifndef FJCORE_VERSION #define FJCORE_VERSION "3.0.5" #endif #endif #ifndef __FJCORE_CONFIG_H__ #define __FJCORE_CONFIG_H__ #endif // __FJCORE_CONFIG_H__ #ifndef __FJCORE_SHARED_PTR_HH__ #define __FJCORE_SHARED_PTR_HH__ #include // for NULL!!! #ifdef __FJCORE_USETR1SHAREDPTR #include #endif // __FJCORE_USETR1SHAREDPTR FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh #ifdef __FJCORE_USETR1SHAREDPTR template class SharedPtr : public std::tr1::shared_ptr { public: SharedPtr() : std::tr1::shared_ptr() {} SharedPtr(T * t) : std::tr1::shared_ptr(t) {} SharedPtr(const SharedPtr & t) : std::tr1::shared_ptr(t) {} inline operator bool() const {return (this->get()!=NULL);} T* operator ()() const{ return this->get(); // automatically returns NULL when out-of-scope } }; #else // __FJCORE_USETR1SHAREDPTR template class SharedPtr{ public: class __SharedCountingPtr; SharedPtr() : _ptr(NULL){} template explicit SharedPtr(Y* ptr){ _ptr = new __SharedCountingPtr(ptr); } SharedPtr(SharedPtr const & share) : _ptr(share._get_container()){ if (_ptr!=NULL) ++(*_ptr); } ~SharedPtr(){ if (_ptr==NULL) return; _decrease_count(); } void reset(){ SharedPtr().swap(*this); } template void reset(Y * ptr){ SharedPtr(ptr).swap(*this); } template void reset(SharedPtr const & share){ if (_ptr!=NULL){ if (_ptr == share._get_container()) return; _decrease_count(); } _ptr = share._get_container(); // Note: automatically set it to NULL if share is empty if (_ptr!=NULL) ++(*_ptr); } SharedPtr& operator=(SharedPtr const & share){ reset(share); return *this; } template SharedPtr& operator=(SharedPtr const & share){ reset(share); return *this; } T* operator ()() const{ if (_ptr==NULL) return NULL; return _ptr->get(); // automatically returns NULL when out-of-scope } inline T& operator*() const{ return *(_ptr->get()); } inline T* operator->() const{ if (_ptr==NULL) return NULL; return _ptr->get(); } inline T* get() const{ if (_ptr==NULL) return NULL; return _ptr->get(); } inline bool unique() const{ return (use_count()==1); } inline long use_count() const{ if (_ptr==NULL) return 0; return _ptr->use_count(); // automatically returns NULL when out-of-scope } inline operator bool() const{ return (get()!=NULL); } inline void swap(SharedPtr & share){ __SharedCountingPtr* share_container = share._ptr; share._ptr = _ptr; _ptr = share_container; } void set_count(const long & count){ if (_ptr==NULL) return; _ptr->set_count(count); } class __SharedCountingPtr{ public: __SharedCountingPtr() : _ptr(NULL), _count(0){} template explicit __SharedCountingPtr(Y* ptr) : _ptr(ptr), _count(1){} ~__SharedCountingPtr(){ if (_ptr!=NULL){ delete _ptr;} } inline T* get() const {return _ptr;} inline long use_count() const {return _count;} inline long operator++(){return ++_count;} inline long operator--(){return --_count;} inline long operator++(int){return _count++;} inline long operator--(int){return _count--;} void set_count(const long & count){ _count = count; } private: T *_ptr; ///< the pointer we're counting the references to long _count; ///< the number of references }; private: inline __SharedCountingPtr* _get_container() const{ return _ptr; } void _decrease_count(){ (*_ptr)--; if (_ptr->use_count()==0) delete _ptr; // that automatically deletes the object itself } __SharedCountingPtr *_ptr; }; template inline bool operator==(SharedPtr const & t, SharedPtr const & u){ return t.get() == u.get(); } template inline bool operator!=(SharedPtr const & t, SharedPtr const & u){ return t.get() != u.get(); } template inline bool operator<(SharedPtr const & t, SharedPtr const & u){ return t.get() < u.get(); } template inline void swap(SharedPtr & a, SharedPtr & b){ return a.swap(b); } template inline T* get_pointer(SharedPtr const & t){ return t.get(); } #endif // __FJCORE_USETR1SHAREDPTR FJCORE_END_NAMESPACE // defined in fastjet/internal/base.hh #endif // __FJCORE_SHARED_PTR_HH__ #ifndef __FJCORE_ERROR_HH__ #define __FJCORE_ERROR_HH__ #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class Error { public: Error() {} Error(const std::string & message); virtual ~Error() {} std::string message() const {return _message;} static void set_print_errors(bool print_errors) {_print_errors = print_errors;} static void set_print_backtrace(bool enabled) {_print_backtrace = enabled;} static void set_default_stream(std::ostream * ostr) { _default_ostr = ostr; } private: std::string _message; ///< error message static bool _print_errors; ///< do we print anything? static bool _print_backtrace; ///< do we print the backtrace? static std::ostream * _default_ostr; ///< the output stream (cerr if not set) }; FJCORE_END_NAMESPACE #endif // __FJCORE_ERROR_HH__ #ifndef __FJCORE_LIMITEDWARNING_HH__ #define __FJCORE_LIMITEDWARNING_HH__ #include #include #include FJCORE_BEGIN_NAMESPACE class LimitedWarning { public: LimitedWarning() : _max_warn(_max_warn_default), _n_warn_so_far(0), _this_warning_summary(0) {} LimitedWarning(int max_warn) : _max_warn(max_warn), _n_warn_so_far(0), _this_warning_summary(0) {} void warn(const std::string & warning); void warn(const std::string & warning, std::ostream * ostr); static void set_default_stream(std::ostream * ostr) { _default_ostr = ostr; } static void set_default_max_warn(int max_warn) { _max_warn_default = max_warn; } static std::string summary(); private: int _max_warn, _n_warn_so_far; static int _max_warn_default; static std::ostream * _default_ostr; typedef std::pair Summary; static std::list< Summary > _global_warnings_summary; Summary * _this_warning_summary; }; FJCORE_END_NAMESPACE #endif // __FJCORE_LIMITEDWARNING_HH__ #ifndef __FJCORE_PSEUDOJET_STRUCTURE_BASE_HH__ #define __FJCORE_PSEUDOJET_STRUCTURE_BASE_HH__ #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class PseudoJet; class ClusterSequence; class PseudoJetStructureBase{ public: PseudoJetStructureBase(){}; virtual ~PseudoJetStructureBase(){}; virtual std::string description() const{ return "PseudoJet with an unknown structure"; } virtual bool has_associated_cluster_sequence() const { return false;} virtual const ClusterSequence* associated_cluster_sequence() const; virtual bool has_valid_cluster_sequence() const {return false;} virtual const ClusterSequence * validated_cs() const; virtual bool has_partner(const PseudoJet &reference, PseudoJet &partner) const; virtual bool has_child(const PseudoJet &reference, PseudoJet &child) const; virtual bool has_parents(const PseudoJet &reference, PseudoJet &parent1, PseudoJet &parent2) const; virtual bool object_in_jet(const PseudoJet &reference, const PseudoJet &jet) const; virtual bool has_constituents() const {return false;} virtual std::vector constituents(const PseudoJet &reference) const; virtual bool has_exclusive_subjets() const {return false;} virtual std::vector exclusive_subjets(const PseudoJet &reference, const double & dcut) const; virtual int n_exclusive_subjets(const PseudoJet &reference, const double & dcut) const; virtual std::vector exclusive_subjets_up_to (const PseudoJet &reference, int nsub) const; virtual double exclusive_subdmerge(const PseudoJet &reference, int nsub) const; virtual double exclusive_subdmerge_max(const PseudoJet &reference, int nsub) const; virtual bool has_pieces(const PseudoJet & /* reference */) const { return false;} virtual std::vector pieces(const PseudoJet & /* reference */ ) const; }; FJCORE_END_NAMESPACE #endif // __FJCORE_PSEUDOJET_STRUCTURE_BASE_HH__ #ifndef __FJCORE_PSEUDOJET_HH__ #define __FJCORE_PSEUDOJET_HH__ #include #include #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh const double MaxRap = 1e5; const double pseudojet_invalid_phi = -100.0; const double pseudojet_invalid_rap = -1e200; class PseudoJet { public: PseudoJet() : _px(0), _py(0), _pz(0), _E(0) {_finish_init(); _reset_indices();} PseudoJet(const double px, const double py, const double pz, const double E); template PseudoJet(const L & some_four_vector); PseudoJet(bool /* dummy */) {} virtual ~PseudoJet(){}; inline double E() const {return _E;} inline double e() const {return _E;} // like CLHEP inline double px() const {return _px;} inline double py() const {return _py;} inline double pz() const {return _pz;} inline double phi() const {return phi_02pi();} inline double phi_std() const { _ensure_valid_rap_phi(); return _phi > pi ? _phi-twopi : _phi;} inline double phi_02pi() const { _ensure_valid_rap_phi(); return _phi; } inline double rap() const { _ensure_valid_rap_phi(); return _rap; } inline double rapidity() const {return rap();} // like CLHEP double pseudorapidity() const; double eta() const {return pseudorapidity();} inline double pt2() const {return _kt2;} inline double pt() const {return sqrt(_kt2);} inline double perp2() const {return _kt2;} // like CLHEP inline double perp() const {return sqrt(_kt2);} // like CLHEP inline double kt2() const {return _kt2;} // for bkwds compatibility inline double m2() const {return (_E+_pz)*(_E-_pz)-_kt2;} inline double m() const; inline double mperp2() const {return (_E+_pz)*(_E-_pz);} inline double mperp() const {return sqrt(std::abs(mperp2()));} inline double mt2() const {return (_E+_pz)*(_E-_pz);} inline double mt() const {return sqrt(std::abs(mperp2()));} inline double modp2() const {return _kt2+_pz*_pz;} inline double modp() const {return sqrt(_kt2+_pz*_pz);} inline double Et() const {return (_kt2==0) ? 0.0 : _E/sqrt(1.0+_pz*_pz/_kt2);} inline double Et2() const {return (_kt2==0) ? 0.0 : _E*_E/(1.0+_pz*_pz/_kt2);} double operator () (int i) const ; inline double operator [] (int i) const { return (*this)(i); }; // this too double kt_distance(const PseudoJet & other) const; double plain_distance(const PseudoJet & other) const; inline double squared_distance(const PseudoJet & other) const { return plain_distance(other);} inline double delta_R(const PseudoJet & other) const { return sqrt(squared_distance(other)); } double delta_phi_to(const PseudoJet & other) const; inline double beam_distance() const {return _kt2;} std::valarray four_mom() const; enum { X=0, Y=1, Z=2, T=3, NUM_COORDINATES=4, SIZE=NUM_COORDINATES }; PseudoJet & boost(const PseudoJet & prest); PseudoJet & unboost(const PseudoJet & prest); void operator*=(double); void operator/=(double); void operator+=(const PseudoJet &); void operator-=(const PseudoJet &); inline void reset(double px, double py, double pz, double E); inline void reset(const PseudoJet & psjet) { (*this) = psjet; } template inline void reset(const L & some_four_vector) { const PseudoJet * pj = fjcore::cast_if_derived(&some_four_vector); if (pj){ (*this) = *pj; } else { reset(some_four_vector[0], some_four_vector[1], some_four_vector[2], some_four_vector[3]); } } inline void reset_PtYPhiM(double pt_in, double y_in, double phi_in, double m_in=0.0) { reset_momentum_PtYPhiM(pt_in, y_in, phi_in, m_in); _reset_indices(); } inline void reset_momentum(double px, double py, double pz, double E); inline void reset_momentum(const PseudoJet & pj); void reset_momentum_PtYPhiM(double pt, double y, double phi, double m=0.0); template inline void reset_momentum(const L & some_four_vector) { reset_momentum(some_four_vector[0], some_four_vector[1], some_four_vector[2], some_four_vector[3]); } void set_cached_rap_phi(double rap, double phi); inline int user_index() const {return _user_index;} inline void set_user_index(const int index) {_user_index = index;} class UserInfoBase{ public: UserInfoBase(){}; virtual ~UserInfoBase(){}; }; class InexistentUserInfo : public Error { public: InexistentUserInfo(); }; void set_user_info(UserInfoBase * user_info_in) { _user_info.reset(user_info_in); } template const L & user_info() const{ if (_user_info.get() == 0) throw InexistentUserInfo(); return dynamic_cast(* _user_info.get()); } bool has_user_info() const{ return _user_info.get(); } template bool has_user_info() const{ return _user_info.get() && dynamic_cast(_user_info.get()); } const UserInfoBase * user_info_ptr() const{ if (!_user_info()) return NULL; return _user_info.get(); } const SharedPtr & user_info_shared_ptr() const{ return _user_info; } SharedPtr & user_info_shared_ptr(){ return _user_info; } std::string description() const; bool has_associated_cluster_sequence() const; bool has_associated_cs() const {return has_associated_cluster_sequence();} bool has_valid_cluster_sequence() const; bool has_valid_cs() const {return has_valid_cluster_sequence();} const ClusterSequence* associated_cluster_sequence() const; const ClusterSequence* associated_cs() const {return associated_cluster_sequence();} inline const ClusterSequence * validated_cluster_sequence() const { return validated_cs(); } const ClusterSequence * validated_cs() const; void set_structure_shared_ptr(const SharedPtr &structure); bool has_structure() const; const PseudoJetStructureBase* structure_ptr() const; PseudoJetStructureBase* structure_non_const_ptr(); const PseudoJetStructureBase* validated_structure_ptr() const; const SharedPtr & structure_shared_ptr() const; template const StructureType & structure() const; template bool has_structure_of() const; template const typename TransformerType::StructureType & structure_of() const; virtual bool has_partner(PseudoJet &partner) const; virtual bool has_child(PseudoJet &child) const; virtual bool has_parents(PseudoJet &parent1, PseudoJet &parent2) const; virtual bool contains(const PseudoJet &constituent) const; virtual bool is_inside(const PseudoJet &jet) const; virtual bool has_constituents() const; virtual std::vector constituents() const; virtual bool has_exclusive_subjets() const; std::vector exclusive_subjets (const double & dcut) const; int n_exclusive_subjets(const double & dcut) const; std::vector exclusive_subjets (int nsub) const; std::vector exclusive_subjets_up_to (int nsub) const; double exclusive_subdmerge(int nsub) const; double exclusive_subdmerge_max(int nsub) const; virtual bool has_pieces() const; virtual std::vector pieces() const; inline int cluster_hist_index() const {return _cluster_hist_index;} inline void set_cluster_hist_index(const int index) {_cluster_hist_index = index;} inline int cluster_sequence_history_index() const { return cluster_hist_index();} inline void set_cluster_sequence_history_index(const int index) { set_cluster_hist_index(index);} protected: SharedPtr _structure; SharedPtr _user_info; private: double _px,_py,_pz,_E; mutable double _phi, _rap; double _kt2; int _cluster_hist_index, _user_index; void _finish_init(); void _reset_indices(); inline void _ensure_valid_rap_phi() const { if (_phi == pseudojet_invalid_phi) _set_rap_phi(); } void _set_rap_phi() const; }; PseudoJet operator+(const PseudoJet &, const PseudoJet &); PseudoJet operator-(const PseudoJet &, const PseudoJet &); PseudoJet operator*(double, const PseudoJet &); PseudoJet operator*(const PseudoJet &, double); PseudoJet operator/(const PseudoJet &, double); bool operator==(const PseudoJet &, const PseudoJet &); inline bool operator!=(const PseudoJet & a, const PseudoJet & b) {return !(a==b);} bool operator==(const PseudoJet & jet, const double val); inline bool operator!=(const PseudoJet & a, const double & val) {return !(a==val);} inline double dot_product(const PseudoJet & a, const PseudoJet & b) { return a.E()*b.E() - a.px()*b.px() - a.py()*b.py() - a.pz()*b.pz(); } bool have_same_momentum(const PseudoJet &, const PseudoJet &); PseudoJet PtYPhiM(double pt, double y, double phi, double m = 0.0); std::vector sorted_by_pt(const std::vector & jets); std::vector sorted_by_rapidity(const std::vector & jets); std::vector sorted_by_E(const std::vector & jets); std::vector sorted_by_pz(const std::vector & jets); void sort_indices(std::vector & indices, const std::vector & values); template std::vector objects_sorted_by_values(const std::vector & objects, const std::vector & values); class IndexedSortHelper { public: inline IndexedSortHelper (const std::vector * reference_values) { _ref_values = reference_values; }; inline int operator() (const int & i1, const int & i2) const { return (*_ref_values)[i1] < (*_ref_values)[i2]; }; private: const std::vector * _ref_values; }; template inline PseudoJet::PseudoJet(const L & some_four_vector) { reset(some_four_vector); } inline void PseudoJet::_reset_indices() { set_cluster_hist_index(-1); set_user_index(-1); _structure.reset(); _user_info.reset(); } inline double PseudoJet::m() const { double mm = m2(); return mm < 0.0 ? -std::sqrt(-mm) : std::sqrt(mm); } inline void PseudoJet::reset(double px_in, double py_in, double pz_in, double E_in) { _px = px_in; _py = py_in; _pz = pz_in; _E = E_in; _finish_init(); _reset_indices(); } inline void PseudoJet::reset_momentum(double px_in, double py_in, double pz_in, double E_in) { _px = px_in; _py = py_in; _pz = pz_in; _E = E_in; _finish_init(); } inline void PseudoJet::reset_momentum(const PseudoJet & pj) { _px = pj._px ; _py = pj._py ; _pz = pj._pz ; _E = pj._E ; _phi = pj._phi; _rap = pj._rap; _kt2 = pj._kt2; } template const StructureType & PseudoJet::structure() const{ return dynamic_cast(* validated_structure_ptr()); } template bool PseudoJet::has_structure_of() const{ if (!_structure()) return false; return dynamic_cast(_structure.get()) != 0; } template const typename TransformerType::StructureType & PseudoJet::structure_of() const{ if (!_structure()) throw Error("Trying to access the structure of a PseudoJet without an associated structure"); return dynamic_cast(*_structure); } PseudoJet join(const std::vector & pieces); PseudoJet join(const PseudoJet & j1); PseudoJet join(const PseudoJet & j1, const PseudoJet & j2); PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3); PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3, const PseudoJet & j4); FJCORE_END_NAMESPACE #endif // __FJCORE_PSEUDOJET_HH__ #ifndef __FJCORE_FUNCTION_OF_PSEUDOJET_HH__ #define __FJCORE_FUNCTION_OF_PSEUDOJET_HH__ FJCORE_BEGIN_NAMESPACE template class FunctionOfPseudoJet{ public: FunctionOfPseudoJet(){} FunctionOfPseudoJet(const TOut &constant_value); virtual ~FunctionOfPseudoJet(){} virtual std::string description() const{ return "";} virtual TOut result(const PseudoJet &pj) const = 0; TOut operator()(const PseudoJet &pj) const { return result(pj);} std::vector operator()(const std::vector &pjs) const { std::vector res(pjs.size()); for (unsigned int i=0; i #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class Selector; class SelectorWorker { public: virtual ~SelectorWorker() {} virtual bool pass(const PseudoJet & jet) const = 0; virtual void terminator(std::vector & jets) const { for (unsigned i = 0; i < jets.size(); i++) { if (jets[i] && !pass(*jets[i])) jets[i] = NULL; } } virtual bool applies_jet_by_jet() const {return true;} virtual std::string description() const {return "missing description";} virtual bool takes_reference() const { return false;} virtual void set_reference(const PseudoJet & /*reference*/){ throw Error("set_reference(...) cannot be used for a selector worker that does not take a reference"); } virtual SelectorWorker* copy(){ throw Error("this SelectorWorker has nothing to copy"); } virtual void get_rapidity_extent(double & rapmin, double & rapmax) const { rapmax = std::numeric_limits::infinity(); rapmin = -rapmax; } virtual bool is_geometric() const { return false;} virtual bool has_finite_area() const; virtual bool has_known_area() const { return false;} virtual double known_area() const{ throw Error("this selector has no computable area"); } }; class Selector{ public: Selector() {} Selector(SelectorWorker * worker_in) {_worker.reset(worker_in);} virtual ~Selector(){} bool pass(const PseudoJet & jet) const { if (!validated_worker()->applies_jet_by_jet()) { throw Error("Cannot apply this selector to an individual jet"); } return _worker->pass(jet); } bool operator()(const PseudoJet & jet) const { return pass(jet); } unsigned int count(const std::vector & jets) const; void sift(const std::vector & jets, std::vector & jets_that_pass, std::vector & jets_that_fail) const; bool applies_jet_by_jet() const { return validated_worker()->applies_jet_by_jet(); } std::vector operator()(const std::vector & jets) const; virtual void nullify_non_selected(std::vector & jets) const { validated_worker()->terminator(jets); } void get_rapidity_extent(double &rapmin, double &rapmax) const { return validated_worker()->get_rapidity_extent(rapmin, rapmax); } std::string description() const { return validated_worker()->description(); } bool is_geometric() const{ return validated_worker()->is_geometric(); } bool has_finite_area() const{ return validated_worker()->has_finite_area(); } const SharedPtr & worker() const {return _worker;} const SelectorWorker* validated_worker() const { const SelectorWorker* worker_ptr = _worker.get(); if (worker_ptr == 0) throw InvalidWorker(); return worker_ptr; } bool takes_reference() const { return validated_worker()->takes_reference(); } const Selector & set_reference(const PseudoJet &reference){ if (! validated_worker()->takes_reference()){ return *this; } _copy_worker_if_needed(); _worker->set_reference(reference); return *this; } class InvalidWorker : public Error { public: InvalidWorker() : Error("Attempt to use Selector with no valid underlying worker") {} }; class InvalidArea : public Error { public: InvalidArea() : Error("Attempt to obtain area from Selector for which this is not meaningful") {} }; Selector & operator &=(const Selector & b); Selector & operator |=(const Selector & b); protected: void _copy_worker_if_needed(){ if (_worker.unique()) return; _worker.reset(_worker->copy()); } private: SharedPtr _worker; ///< the underlying worker }; Selector SelectorIdentity(); Selector operator!(const Selector & s); Selector operator ||(const Selector & s1, const Selector & s2); Selector operator&&(const Selector & s1, const Selector & s2); Selector operator*(const Selector & s1, const Selector & s2); Selector SelectorPtMin(double ptmin); ///< select objects with pt >= ptmin Selector SelectorPtMax(double ptmax); ///< select objects with pt <= ptmax Selector SelectorPtRange(double ptmin, double ptmax); ///< select objects with ptmin <= pt <= ptmax Selector SelectorEtMin(double Etmin); ///< select objects with Et >= Etmin Selector SelectorEtMax(double Etmax); ///< select objects with Et <= Etmax Selector SelectorEtRange(double Etmin, double Etmax); ///< select objects with Etmin <= Et <= Etmax Selector SelectorEMin(double Emin); ///< select objects with E >= Emin Selector SelectorEMax(double Emax); ///< select objects with E <= Emax Selector SelectorERange(double Emin, double Emax); ///< select objects with Emin <= E <= Emax Selector SelectorMassMin(double Mmin); ///< select objects with Mass >= Mmin Selector SelectorMassMax(double Mmax); ///< select objects with Mass <= Mmax Selector SelectorMassRange(double Mmin, double Mmax); ///< select objects with Mmin <= Mass <= Mmax Selector SelectorRapMin(double rapmin); ///< select objects with rap >= rapmin Selector SelectorRapMax(double rapmax); ///< select objects with rap <= rapmax Selector SelectorRapRange(double rapmin, double rapmax); ///< select objects with rapmin <= rap <= rapmax Selector SelectorAbsRapMin(double absrapmin); ///< select objects with |rap| >= absrapmin Selector SelectorAbsRapMax(double absrapmax); ///< select objects with |rap| <= absrapmax Selector SelectorAbsRapRange(double absrapmin, double absrapmax); ///< select objects with absrapmin <= |rap| <= absrapmax Selector SelectorEtaMin(double etamin); ///< select objects with eta >= etamin Selector SelectorEtaMax(double etamax); ///< select objects with eta <= etamax Selector SelectorEtaRange(double etamin, double etamax); ///< select objects with etamin <= eta <= etamax Selector SelectorAbsEtaMin(double absetamin); ///< select objects with |eta| >= absetamin Selector SelectorAbsEtaMax(double absetamax); ///< select objects with |eta| <= absetamax Selector SelectorAbsEtaRange(double absetamin, double absetamax); ///< select objects with absetamin <= |eta| <= absetamax Selector SelectorPhiRange(double phimin, double phimax); ///< select objects with phimin <= phi <= phimax Selector SelectorRapPhiRange(double rapmin, double rapmax, double phimin, double phimax); Selector SelectorNHardest(unsigned int n); Selector SelectorCircle(const double & radius); Selector SelectorDoughnut(const double & radius_in, const double & radius_out); Selector SelectorStrip(const double & half_width); Selector SelectorRectangle(const double & half_rap_width, const double & half_phi_width); Selector SelectorPtFractionMin(double fraction); Selector SelectorIsZero(); FJCORE_END_NAMESPACE // defined in fastjet/internal/base.hh #endif // __FJCORE_SELECTOR_HH__ #ifndef __FJCORE_JETDEFINITION_HH__ #define __FJCORE_JETDEFINITION_HH__ #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh std::string fastjet_version_string(); enum Strategy { N2MinHeapTiled = -4, N2Tiled = -3, N2PoorTiled = -2, N2Plain = -1, N3Dumb = 0, Best = 1, NlnN = 2, NlnN3pi = 3, NlnN4pi = 4, NlnNCam4pi = 14, NlnNCam2pi2R = 13, NlnNCam = 12, // 2piMultD plugin_strategy = 999 }; enum JetAlgorithm { kt_algorithm=0, cambridge_algorithm=1, antikt_algorithm=2, genkt_algorithm=3, cambridge_for_passive_algorithm=11, genkt_for_passive_algorithm=13, ee_kt_algorithm=50, ee_genkt_algorithm=53, plugin_algorithm = 99, undefined_jet_algorithm = 999 }; typedef JetAlgorithm JetFinder; const JetAlgorithm aachen_algorithm = cambridge_algorithm; const JetAlgorithm cambridge_aachen_algorithm = cambridge_algorithm; enum RecombinationScheme { E_scheme=0, pt_scheme=1, pt2_scheme=2, Et_scheme=3, Et2_scheme=4, BIpt_scheme=5, BIpt2_scheme=6, external_scheme = 99 }; class ClusterSequence; class JetDefinition { public: class Plugin; class Recombiner; JetDefinition(JetAlgorithm jet_algorithm_in, double R_in, RecombinationScheme recomb_scheme_in = E_scheme, Strategy strategy_in = Best) { *this = JetDefinition(jet_algorithm_in, R_in, strategy_in, recomb_scheme_in, 1); } JetDefinition(JetAlgorithm jet_algorithm_in, RecombinationScheme recomb_scheme_in = E_scheme, Strategy strategy_in = Best) { double dummyR = 0.0; *this = JetDefinition(jet_algorithm_in, dummyR, strategy_in, recomb_scheme_in, 0); } JetDefinition(JetAlgorithm jet_algorithm_in, double R_in, double xtra_param_in, RecombinationScheme recomb_scheme_in = E_scheme, Strategy strategy_in = Best) { *this = JetDefinition(jet_algorithm_in, R_in, strategy_in, recomb_scheme_in, 2); set_extra_param(xtra_param_in); } JetDefinition(JetAlgorithm jet_algorithm_in, double R_in, const Recombiner * recombiner_in, Strategy strategy_in = Best) { *this = JetDefinition(jet_algorithm_in, R_in, external_scheme, strategy_in); _recombiner = recombiner_in; } JetDefinition(JetAlgorithm jet_algorithm_in, const Recombiner * recombiner_in, Strategy strategy_in = Best) { *this = JetDefinition(jet_algorithm_in, external_scheme, strategy_in); _recombiner = recombiner_in; } JetDefinition(JetAlgorithm jet_algorithm_in, double R_in, double xtra_param_in, const Recombiner * recombiner_in, Strategy strategy_in = Best) { *this = JetDefinition(jet_algorithm_in, R_in, external_scheme, strategy_in); _recombiner = recombiner_in; set_extra_param(xtra_param_in); } JetDefinition() { *this = JetDefinition(undefined_jet_algorithm, 1.0); } JetDefinition(const Plugin * plugin_in) { _plugin = plugin_in; _strategy = plugin_strategy; _Rparam = _plugin->R(); _jet_algorithm = plugin_algorithm; set_recombination_scheme(E_scheme); } JetDefinition(JetAlgorithm jet_algorithm_in, double R_in, Strategy strategy_in, RecombinationScheme recomb_scheme_in = E_scheme, int nparameters_in = 1); static const double max_allowable_R; //= 1000.0; void set_recombination_scheme(RecombinationScheme); void set_recombiner(const Recombiner * recomb) { if (_recombiner_shared()) _recombiner_shared.reset(recomb); _recombiner = recomb; _default_recombiner = DefaultRecombiner(external_scheme); } void delete_recombiner_when_unused(); const Plugin * plugin() const {return _plugin;}; void delete_plugin_when_unused(); JetAlgorithm jet_algorithm () const {return _jet_algorithm ;} JetAlgorithm jet_finder () const {return _jet_algorithm ;} double R () const {return _Rparam ;} double extra_param () const {return _extra_param ;} Strategy strategy () const {return _strategy ;} RecombinationScheme recombination_scheme() const { return _default_recombiner.scheme();} void set_jet_algorithm(JetAlgorithm njf) {_jet_algorithm = njf;} void set_jet_finder(JetAlgorithm njf) {_jet_algorithm = njf;} void set_extra_param(double xtra_param) {_extra_param = xtra_param;} const Recombiner * recombiner() const { return _recombiner == 0 ? & _default_recombiner : _recombiner;} bool has_same_recombiner(const JetDefinition &other_jd) const; std::string description() const; public: class Recombiner { public: virtual std::string description() const = 0; virtual void recombine(const PseudoJet & pa, const PseudoJet & pb, PseudoJet & pab) const = 0; virtual void preprocess(PseudoJet & ) const {}; virtual ~Recombiner() {}; inline void plus_equal(PseudoJet & pa, const PseudoJet & pb) const { PseudoJet pres; recombine(pa,pb,pres); pa = pres; } }; class DefaultRecombiner : public Recombiner { public: DefaultRecombiner(RecombinationScheme recomb_scheme = E_scheme) : _recomb_scheme(recomb_scheme) {} virtual std::string description() const; virtual void recombine(const PseudoJet & pa, const PseudoJet & pb, PseudoJet & pab) const; virtual void preprocess(PseudoJet & p) const; RecombinationScheme scheme() const {return _recomb_scheme;} private: RecombinationScheme _recomb_scheme; }; class Plugin{ public: virtual std::string description() const = 0; virtual void run_clustering(ClusterSequence &) const = 0; virtual double R() const = 0; virtual bool supports_ghosted_passive_areas() const {return false;} virtual void set_ghost_separation_scale(double scale) const; virtual double ghost_separation_scale() const {return 0.0;} virtual bool exclusive_sequence_meaningful() const {return false;} virtual ~Plugin() {}; }; private: JetAlgorithm _jet_algorithm; double _Rparam; double _extra_param ; ///< parameter whose meaning varies according to context Strategy _strategy ; const Plugin * _plugin; SharedPtr _plugin_shared; DefaultRecombiner _default_recombiner; const Recombiner * _recombiner; SharedPtr _recombiner_shared; }; PseudoJet join(const std::vector & pieces, const JetDefinition::Recombiner & recombiner); PseudoJet join(const PseudoJet & j1, const JetDefinition::Recombiner & recombiner); PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const JetDefinition::Recombiner & recombiner); PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3, const JetDefinition::Recombiner & recombiner); PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3, const PseudoJet & j4, const JetDefinition::Recombiner & recombiner); FJCORE_END_NAMESPACE #endif // __FJCORE_JETDEFINITION_HH__ #ifndef __FJCORE_COMPOSITEJET_STRUCTURE_HH__ #define __FJCORE_COMPOSITEJET_STRUCTURE_HH__ FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class CompositeJetStructure : public PseudoJetStructureBase{ public: CompositeJetStructure() : _area_4vector_ptr(0){}; CompositeJetStructure(const std::vector & initial_pieces, const JetDefinition::Recombiner * recombiner = 0); virtual ~CompositeJetStructure(){ if (_area_4vector_ptr) delete _area_4vector_ptr; }; virtual std::string description() const; virtual bool has_constituents() const; virtual std::vector constituents(const PseudoJet &jet) const; virtual bool has_pieces(const PseudoJet & /*jet*/) const {return true;} virtual std::vector pieces(const PseudoJet &jet) const; protected: std::vector _pieces; ///< the pieces building the jet PseudoJet * _area_4vector_ptr; ///< pointer to the 4-vector jet area }; template PseudoJet join(const std::vector & pieces){ PseudoJet result(0.0,0.0,0.0,0.0); for (unsigned int i=0; i(cj_struct)); return result; } template PseudoJet join(const PseudoJet & j1){ return join(std::vector(1,j1)); } template PseudoJet join(const PseudoJet & j1, const PseudoJet & j2){ std::vector pieces; pieces.push_back(j1); pieces.push_back(j2); return join(pieces); } template PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3){ std::vector pieces; pieces.push_back(j1); pieces.push_back(j2); pieces.push_back(j3); return join(pieces); } template PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3, const PseudoJet & j4){ std::vector pieces; pieces.push_back(j1); pieces.push_back(j2); pieces.push_back(j3); pieces.push_back(j4); return join(pieces); } template PseudoJet join(const std::vector & pieces, const JetDefinition::Recombiner & recombiner){ PseudoJet result; if (pieces.size()>0){ result = pieces[0]; for (unsigned int i=1; i(cj_struct)); return result; } template PseudoJet join(const PseudoJet & j1, const JetDefinition::Recombiner & recombiner){ return join(std::vector(1,j1), recombiner); } template PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const JetDefinition::Recombiner & recombiner){ std::vector pieces; pieces.push_back(j1); pieces.push_back(j2); return join(pieces, recombiner); } template PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3, const JetDefinition::Recombiner & recombiner){ std::vector pieces; pieces.push_back(j1); pieces.push_back(j2); pieces.push_back(j3); return join(pieces, recombiner); } template PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3, const PseudoJet & j4, const JetDefinition::Recombiner & recombiner){ std::vector pieces; pieces.push_back(j1); pieces.push_back(j2); pieces.push_back(j3); pieces.push_back(j4); return join(pieces, recombiner); } FJCORE_END_NAMESPACE // defined in fastjet/internal/base.hh #endif // __FJCORE_MERGEDJET_STRUCTURE_HH__ #ifndef __FJCORE_CLUSTER_SEQUENCE_STRUCTURE_HH__ #define __FJCORE_CLUSTER_SEQUENCE_STRUCTURE_HH__ #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class ClusterSequenceStructure : public PseudoJetStructureBase{ public: ClusterSequenceStructure() : _associated_cs(NULL){} ClusterSequenceStructure(const ClusterSequence *cs){ set_associated_cs(cs); }; virtual ~ClusterSequenceStructure(); virtual std::string description() const{ return "PseudoJet with an associated ClusterSequence"; } virtual bool has_associated_cluster_sequence() const{ return true;} virtual const ClusterSequence* associated_cluster_sequence() const; virtual bool has_valid_cluster_sequence() const; virtual const ClusterSequence * validated_cs() const; virtual void set_associated_cs(const ClusterSequence * new_cs){ _associated_cs = new_cs; } virtual bool has_partner(const PseudoJet &reference, PseudoJet &partner) const; virtual bool has_child(const PseudoJet &reference, PseudoJet &child) const; virtual bool has_parents(const PseudoJet &reference, PseudoJet &parent1, PseudoJet &parent2) const; virtual bool object_in_jet(const PseudoJet &reference, const PseudoJet &jet) const; virtual bool has_constituents() const; virtual std::vector constituents(const PseudoJet &reference) const; virtual bool has_exclusive_subjets() const; virtual std::vector exclusive_subjets(const PseudoJet &reference, const double & dcut) const; virtual int n_exclusive_subjets(const PseudoJet &reference, const double & dcut) const; virtual std::vector exclusive_subjets_up_to (const PseudoJet &reference, int nsub) const; virtual double exclusive_subdmerge(const PseudoJet &reference, int nsub) const; virtual double exclusive_subdmerge_max(const PseudoJet &reference, int nsub) const; virtual bool has_pieces(const PseudoJet &reference) const; virtual std::vector pieces(const PseudoJet &reference) const; protected: const ClusterSequence *_associated_cs; }; FJCORE_END_NAMESPACE #endif // __FJCORE_CLUSTER_SEQUENCE_STRUCTURE_HH__ #ifndef __FJCORE_CLUSTERSEQUENCE_HH__ #define __FJCORE_CLUSTERSEQUENCE_HH__ #include #include #include #include #include #include #include #include // needed to get double std::abs(double) FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class ClusterSequenceStructure; class DynamicNearestNeighbours; class ClusterSequence { public: ClusterSequence () : _deletes_self_when_unused(false) {} template ClusterSequence ( const std::vector & pseudojets, const JetDefinition & jet_def, const bool & writeout_combinations = false); ClusterSequence (const ClusterSequence & cs) : _deletes_self_when_unused(false) { transfer_from_sequence(cs); } virtual ~ClusterSequence (); //{} std::vector inclusive_jets (const double & ptmin = 0.0) const; int n_exclusive_jets (const double & dcut) const; std::vector exclusive_jets (const double & dcut) const; std::vector exclusive_jets (const int & njets) const; std::vector exclusive_jets_up_to (const int & njets) const; double exclusive_dmerge (const int & njets) const; double exclusive_dmerge_max (const int & njets) const; double exclusive_ymerge (int njets) const {return exclusive_dmerge(njets) / Q2();} double exclusive_ymerge_max (int njets) const {return exclusive_dmerge_max(njets)/Q2();} int n_exclusive_jets_ycut (double ycut) const {return n_exclusive_jets(ycut*Q2());} std::vector exclusive_jets_ycut (double ycut) const { int njets = n_exclusive_jets_ycut(ycut); return exclusive_jets(njets); } std::vector exclusive_subjets (const PseudoJet & jet, const double & dcut) const; int n_exclusive_subjets(const PseudoJet & jet, const double & dcut) const; std::vector exclusive_subjets (const PseudoJet & jet, int nsub) const; std::vector exclusive_subjets_up_to (const PseudoJet & jet, int nsub) const; double exclusive_subdmerge(const PseudoJet & jet, int nsub) const; double exclusive_subdmerge_max(const PseudoJet & jet, int nsub) const; double Q() const {return _Qtot;} double Q2() const {return _Qtot*_Qtot;} bool object_in_jet(const PseudoJet & object, const PseudoJet & jet) const; bool has_parents(const PseudoJet & jet, PseudoJet & parent1, PseudoJet & parent2) const; bool has_child(const PseudoJet & jet, PseudoJet & child) const; bool has_child(const PseudoJet & jet, const PseudoJet * & childp) const; bool has_partner(const PseudoJet & jet, PseudoJet & partner) const; std::vector constituents (const PseudoJet & jet) const; void print_jets_for_root(const std::vector & jets, std::ostream & ostr = std::cout) const; void print_jets_for_root(const std::vector & jets, const std::string & filename, const std::string & comment = "") const; void add_constituents (const PseudoJet & jet, std::vector & subjet_vector) const; inline Strategy strategy_used () const {return _strategy;} std::string strategy_string () const {return strategy_string(_strategy);} std::string strategy_string (Strategy strategy_in) const; const JetDefinition & jet_def() const {return _jet_def;} void delete_self_when_unused(); bool will_delete_self_when_unused() const {return _deletes_self_when_unused;} void signal_imminent_self_deletion() const; double jet_scale_for_algorithm(const PseudoJet & jet) const; void plugin_record_ij_recombination(int jet_i, int jet_j, double dij, int & newjet_k) { assert(plugin_activated()); _do_ij_recombination_step(jet_i, jet_j, dij, newjet_k); } void plugin_record_ij_recombination(int jet_i, int jet_j, double dij, const PseudoJet & newjet, int & newjet_k); void plugin_record_iB_recombination(int jet_i, double diB) { assert(plugin_activated()); _do_iB_recombination_step(jet_i, diB); } class Extras { public: virtual ~Extras() {} virtual std::string description() const {return "This is a dummy extras class that contains no extra information! Derive from it if you want to use it to provide extra information from a plugin jet finder";} }; inline void plugin_associate_extras(std::auto_ptr extras_in) { _extras.reset(extras_in.release()); } inline bool plugin_activated() const {return _plugin_activated;} const Extras * extras() const {return _extras.get();} template void plugin_simple_N2_cluster () { assert(plugin_activated()); _simple_N2_cluster(); } public: struct history_element{ int parent1; /// index in _history where first parent of this jet int parent2; /// index in _history where second parent of this jet int child; /// index in _history where the current jet is /// recombined with another jet to form its child. It /// is Invalid if this jet does not further /// recombine. int jetp_index; /// index in the _jets vector where we will find the double dij; /// the distance corresponding to the recombination /// at this stage of the clustering. double max_dij_so_far; /// the largest recombination distance seen /// so far in the clustering history. }; enum JetType {Invalid=-3, InexistentParent = -2, BeamJet = -1}; const std::vector & jets() const; const std::vector & history() const; unsigned int n_particles() const; std::vector particle_jet_indices(const std::vector &) const; std::vector unique_history_order() const; std::vector unclustered_particles() const; std::vector childless_pseudojets() const; bool contains(const PseudoJet & object) const; void transfer_from_sequence(const ClusterSequence & from_seq, const FunctionOfPseudoJet * action_on_jets = 0); const SharedPtr & structure_shared_ptr() const{ return _structure_shared_ptr; } typedef ClusterSequenceStructure StructureType; static void print_banner(); static void set_fastjet_banner_stream(std::ostream * ostr) {_fastjet_banner_ostr = ostr;} static std::ostream * fastjet_banner_stream() {return _fastjet_banner_ostr;} private: static std::ostream * _fastjet_banner_ostr; protected: JetDefinition _jet_def; template void _transfer_input_jets( const std::vector & pseudojets); void _initialise_and_run (const JetDefinition & jet_def, const bool & writeout_combinations); void _initialise_and_run_no_decant(); void _decant_options(const JetDefinition & jet_def, const bool & writeout_combinations); void _decant_options_partial(); void _fill_initial_history(); void _do_ij_recombination_step(const int & jet_i, const int & jet_j, const double & dij, int & newjet_k); void _do_iB_recombination_step(const int & jet_i, const double & diB); void _set_structure_shared_ptr(PseudoJet & j); void _update_structure_use_count(); std::vector _jets; std::vector _history; void get_subhist_set(std::set & subhist, const PseudoJet & jet, double dcut, int maxjet) const; bool _writeout_combinations; int _initial_n; double _Rparam, _R2, _invR2; double _Qtot; Strategy _strategy; JetAlgorithm _jet_algorithm; SharedPtr _structure_shared_ptr; //< will actually be of type ClusterSequenceStructure int _structure_use_count_after_construction; //< info of use when CS handles its own memory mutable bool _deletes_self_when_unused; private: bool _plugin_activated; SharedPtr _extras; // things the plugin might want to add void _really_dumb_cluster (); void _delaunay_cluster (); template void _simple_N2_cluster (); void _tiled_N2_cluster (); void _faster_tiled_N2_cluster (); void _minheap_faster_tiled_N2_cluster(); void _CP2DChan_cluster(); void _CP2DChan_cluster_2pi2R (); void _CP2DChan_cluster_2piMultD (); void _CP2DChan_limited_cluster(double D); void _do_Cambridge_inclusive_jets(); void _fast_NsqrtN_cluster(); void _add_step_to_history(const int & step_number, const int & parent1, const int & parent2, const int & jetp_index, const double & dij); void _extract_tree_children(int pos, std::valarray &, const std::valarray &, std::vector &) const; void _extract_tree_parents (int pos, std::valarray &, const std::valarray &, std::vector &) const; typedef std::pair TwoVertices; typedef std::pair DijEntry; typedef std::multimap DistMap; void _add_ktdistance_to_map(const int & ii, DistMap & DijMap, const DynamicNearestNeighbours * DNN); static bool _first_time; static int _n_exclusive_warnings; static LimitedWarning _changed_strategy_warning; struct BriefJet { double eta, phi, kt2, NN_dist; BriefJet * NN; int _jets_index; }; class TiledJet { public: double eta, phi, kt2, NN_dist; TiledJet * NN, *previous, * next; int _jets_index, tile_index, diJ_posn; inline void label_minheap_update_needed() {diJ_posn = 1;} inline void label_minheap_update_done() {diJ_posn = 0;} inline bool minheap_update_needed() const {return diJ_posn==1;} }; template void _bj_set_jetinfo( J * const jet, const int _jets_index) const; void _bj_remove_from_tiles( TiledJet * const jet) const; template double _bj_dist(const J * const jeta, const J * const jetb) const; template double _bj_diJ(const J * const jeta) const; template inline J * _bj_of_hindex( const int hist_index, J * const head, J * const tail) const { J * res; for(res = head; res_jets_index].cluster_hist_index() == hist_index) {break;} } return res; } template void _bj_set_NN_nocross(J * const jeta, J * const head, const J * const tail) const; template void _bj_set_NN_crosscheck(J * const jeta, J * const head, const J * const tail) const; static const int n_tile_neighbours = 9; struct Tile { Tile * begin_tiles[n_tile_neighbours]; Tile ** surrounding_tiles; Tile ** RH_tiles; Tile ** end_tiles; TiledJet * head; bool tagged; }; std::vector _tiles; double _tiles_eta_min, _tiles_eta_max; double _tile_size_eta, _tile_size_phi; int _n_tiles_phi,_tiles_ieta_min,_tiles_ieta_max; inline int _tile_index (int ieta, int iphi) const { return (ieta-_tiles_ieta_min)*_n_tiles_phi + (iphi+_n_tiles_phi) % _n_tiles_phi; } int _tile_index(const double & eta, const double & phi) const; void _tj_set_jetinfo ( TiledJet * const jet, const int _jets_index); void _bj_remove_from_tiles(TiledJet * const jet); void _initialise_tiles(); void _print_tiles(TiledJet * briefjets ) const; void _add_neighbours_to_tile_union(const int tile_index, std::vector & tile_union, int & n_near_tiles) const; void _add_untagged_neighbours_to_tile_union(const int tile_index, std::vector & tile_union, int & n_near_tiles); struct EEBriefJet { double NN_dist; // obligatorily present double kt2; // obligatorily present == E^2 in general EEBriefJet * NN; // must be present too int _jets_index; // must also be present! double nx, ny, nz; // our internal storage for fast distance calcs }; void _simple_N2_cluster_BriefJet(); void _simple_N2_cluster_EEBriefJet(); }; template void ClusterSequence::_transfer_input_jets( const std::vector & pseudojets) { _jets.reserve(pseudojets.size()*2); for (unsigned int i = 0; i < pseudojets.size(); i++) { _jets.push_back(pseudojets[i]);} } template ClusterSequence::ClusterSequence ( const std::vector & pseudojets, const JetDefinition & jet_def_in, const bool & writeout_combinations) : _jet_def(jet_def_in), _writeout_combinations(writeout_combinations), _structure_shared_ptr(new ClusterSequenceStructure(this)) { _transfer_input_jets(pseudojets); _decant_options_partial(); _initialise_and_run_no_decant(); } inline const std::vector & ClusterSequence::jets () const { return _jets; } inline const std::vector & ClusterSequence::history () const { return _history; } inline unsigned int ClusterSequence::n_particles() const {return _initial_n;} template inline void ClusterSequence::_bj_set_jetinfo( J * const jetA, const int _jets_index) const { jetA->eta = _jets[_jets_index].rap(); jetA->phi = _jets[_jets_index].phi_02pi(); jetA->kt2 = jet_scale_for_algorithm(_jets[_jets_index]); jetA->_jets_index = _jets_index; jetA->NN_dist = _R2; jetA->NN = NULL; } template inline double ClusterSequence::_bj_dist( const J * const jetA, const J * const jetB) const { double dphi = std::abs(jetA->phi - jetB->phi); double deta = (jetA->eta - jetB->eta); if (dphi > pi) {dphi = twopi - dphi;} return dphi*dphi + deta*deta; } template inline double ClusterSequence::_bj_diJ(const J * const jet) const { double kt2 = jet->kt2; if (jet->NN != NULL) {if (jet->NN->kt2 < kt2) {kt2 = jet->NN->kt2;}} return jet->NN_dist * kt2; } template inline void ClusterSequence::_bj_set_NN_nocross( J * const jet, J * const head, const J * const tail) const { double NN_dist = _R2; J * NN = NULL; if (head < jet) { for (J * jetB = head; jetB != jet; jetB++) { double dist = _bj_dist(jet,jetB); if (dist < NN_dist) { NN_dist = dist; NN = jetB; } } } if (tail > jet) { for (J * jetB = jet+1; jetB != tail; jetB++) { double dist = _bj_dist(jet,jetB); if (dist < NN_dist) { NN_dist = dist; NN = jetB; } } } jet->NN = NN; jet->NN_dist = NN_dist; } template inline void ClusterSequence::_bj_set_NN_crosscheck(J * const jet, J * const head, const J * const tail) const { double NN_dist = _R2; J * NN = NULL; for (J * jetB = head; jetB != tail; jetB++) { double dist = _bj_dist(jet,jetB); if (dist < NN_dist) { NN_dist = dist; NN = jetB; } if (dist < jetB->NN_dist) { jetB->NN_dist = dist; jetB->NN = jet; } } jet->NN = NN; jet->NN_dist = NN_dist; } FJCORE_END_NAMESPACE #endif // __FJCORE_CLUSTERSEQUENCE_HH__ #ifndef __FJCORE_NNH_HH__ #define __FJCORE_NNH_HH__ FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class _NoInfo {}; template class NNHInfo { public: NNHInfo() : _info(NULL) {} NNHInfo(I * info) : _info(info) {} template void init_jet(NNBJ * briefjet, const fjcore::PseudoJet & jet, int index) { briefjet->init(jet, index, _info);} private: I * _info; }; template<> class NNHInfo<_NoInfo> { public: NNHInfo() {} NNHInfo(_NoInfo * ) {} template void init_jet(NNBJ * briefjet, const fjcore::PseudoJet & jet, int index) { briefjet->init(jet, index);} }; template class NNH : public NNHInfo { public: NNH(const std::vector & jets) {start(jets);} NNH(const std::vector & jets, I * info) : NNHInfo(info) {start(jets);} void start(const std::vector & jets); double dij_min(int & iA, int & iB); void remove_jet(int iA); void merge_jets(int iA, int iB, const PseudoJet & jet, int jet_index); ~NNH() { delete[] briefjets; } private: class NNBJ; // forward declaration void set_NN_crosscheck(NNBJ * jet, NNBJ * begin, NNBJ * end); void set_NN_nocross (NNBJ * jet, NNBJ * begin, NNBJ * end); NNBJ * briefjets; NNBJ * head, * tail; int n; std::vector where_is; class NNBJ : public BJ { public: void init(const PseudoJet & jet, int index_in) { BJ::init(jet); other_init(index_in); } void init(const PseudoJet & jet, int index_in, I * info) { BJ::init(jet, info); other_init(index_in); } void other_init(int index_in) { _index = index_in; NN_dist = BJ::beam_distance(); NN = NULL; } int index() const {return _index;} double NN_dist; NNBJ * NN; private: int _index; }; }; template void NNH::start(const std::vector & jets) { n = jets.size(); briefjets = new NNBJ[n]; where_is.resize(2*n); NNBJ * jetA = briefjets; for (int i = 0; i< n; i++) { this->init_jet(jetA, jets[i], i); where_is[i] = jetA; jetA++; // move on to next entry of briefjets } tail = jetA; // a semaphore for the end of briefjets head = briefjets; // a nicer way of naming start for (jetA = head + 1; jetA != tail; jetA++) { set_NN_crosscheck(jetA, head, jetA); } } template double NNH::dij_min(int & iA, int & iB) { double diJ_min = briefjets[0].NN_dist; int diJ_min_jet = 0; for (int i = 1; i < n; i++) { if (briefjets[i].NN_dist < diJ_min) { diJ_min_jet = i; diJ_min = briefjets[i].NN_dist; } } NNBJ * jetA = & briefjets[diJ_min_jet]; iA = jetA->index(); iB = jetA->NN ? jetA->NN->index() : -1; return diJ_min; } template void NNH::remove_jet(int iA) { NNBJ * jetA = where_is[iA]; tail--; n--; *jetA = *tail; where_is[jetA->index()] = jetA; for (NNBJ * jetI = head; jetI != tail; jetI++) { if (jetI->NN == jetA) set_NN_nocross(jetI, head, tail); if (jetI->NN == tail) {jetI->NN = jetA;} } } template void NNH::merge_jets(int iA, int iB, const PseudoJet & jet, int index) { NNBJ * jetA = where_is[iA]; NNBJ * jetB = where_is[iB]; if (jetA < jetB) std::swap(jetA,jetB); this->init_jet(jetB, jet, index); if (index >= int(where_is.size())) where_is.resize(2*index); where_is[jetB->index()] = jetB; tail--; n--; *jetA = *tail; where_is[jetA->index()] = jetA; for (NNBJ * jetI = head; jetI != tail; jetI++) { if (jetI->NN == jetA || jetI->NN == jetB) { set_NN_nocross(jetI, head, tail); } double dist = jetI->distance(jetB); if (dist < jetI->NN_dist) { if (jetI != jetB) { jetI->NN_dist = dist; jetI->NN = jetB; } } if (dist < jetB->NN_dist) { if (jetI != jetB) { jetB->NN_dist = dist; jetB->NN = jetI; } } if (jetI->NN == tail) {jetI->NN = jetA;} } } template void NNH::set_NN_crosscheck(NNBJ * jet, NNBJ * begin, NNBJ * end) { double NN_dist = jet->beam_distance(); NNBJ * NN = NULL; for (NNBJ * jetB = begin; jetB != end; jetB++) { double dist = jet->distance(jetB); if (dist < NN_dist) { NN_dist = dist; NN = jetB; } if (dist < jetB->NN_dist) { jetB->NN_dist = dist; jetB->NN = jet; } } jet->NN = NN; jet->NN_dist = NN_dist; } template void NNH::set_NN_nocross( NNBJ * jet, NNBJ * begin, NNBJ * end) { double NN_dist = jet->beam_distance(); NNBJ * NN = NULL; if (begin < jet) { for (NNBJ * jetB = begin; jetB != jet; jetB++) { double dist = jet->distance(jetB); if (dist < NN_dist) { NN_dist = dist; NN = jetB; } } } if (end > jet) { for (NNBJ * jetB = jet+1; jetB != end; jetB++) { double dist = jet->distance (jetB); if (dist < NN_dist) { NN_dist = dist; NN = jetB; } } } jet->NN = NN; jet->NN_dist = NN_dist; } FJCORE_END_NAMESPACE // defined in fastjet/internal/base.hh #endif // __FJCORE_NNH_HH__ #endif pythia8-8.1.80.orig/include/Pythia8/Analysis.h0000644000175000017500000004125312217346224017246 0ustar sunsun// Analysis.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for the Sphericity, Thrust, ClusterJet and CellJet classes. // Sphericity: sphericity analysis of the event. // Thrust: thrust analysis of the event. // ClusterJet: clustering jet finder. // CellJet: calorimetric cone jet finder. // SlowJet: recombination algorithm; lightweight version of FastJet. #ifndef Pythia8_Analysis_H #define Pythia8_Analysis_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/PythiaStdlib.h" namespace Pythia8 { //========================================================================== // Sphericity class. // This class performs (optionally modified) sphericity analysis on an event. class Sphericity { public: // Constructor. Sphericity(double powerIn = 2., int selectIn = 2) : power(powerIn), select(selectIn), nFew(0) {powerInt = 0; if (abs(power - 1.) < 0.01) powerInt = 1; if (abs(power - 2.) < 0.01) powerInt = 2; powerMod = 0.5 * power - 1.;} // Analyze event. bool analyze(const Event& event, ostream& os = cout); // Return info on results of analysis. double sphericity() const {return 1.5 * (eVal2 + eVal3);} double aplanarity() const {return 1.5 * eVal3;} double eigenValue(int i) const {return (i < 2) ? eVal1 : ( (i < 3) ? eVal2 : eVal3 ) ;} Vec4 eventAxis(int i) const {return (i < 2) ? eVec1 : ( (i < 3) ? eVec2 : eVec3 ) ;} // Provide a listing of the info. void list(ostream& os = cout) const; // Tell how many events could not be analyzed. int nError() const {return nFew;} private: // Constants: could only be changed in the code itself. static const int NSTUDYMIN, TIMESTOPRINT; static const double P2MIN, EIGENVALUEMIN; // Properties of analysis. double power; int select, powerInt; double powerMod; // Outcome of analysis. double eVal1, eVal2, eVal3; Vec4 eVec1, eVec2, eVec3; // Error statistics; int nFew; }; //========================================================================== // Thrust class. // This class performs thrust analysis on an event. class Thrust { public: // Constructor. Thrust(int selectIn = 2) : select(selectIn), nFew(0) {} // Analyze event. bool analyze(const Event& event, ostream& os = cout); // Return info on results of analysis. double thrust() const {return eVal1;} double tMajor() const {return eVal2;} double tMinor() const {return eVal3;} double oblateness() const {return eVal2 - eVal3;} Vec4 eventAxis(int i) const {return (i < 2) ? eVec1 : ( (i < 3) ? eVec2 : eVec3 ) ;} // Provide a listing of the info. void list(ostream& os = cout) const; // Tell how many events could not be analyzed. int nError() const {return nFew;} private: // Constants: could only be changed in the code itself. static const int NSTUDYMIN, TIMESTOPRINT; static const double MAJORMIN; // Properties of analysis. int select; // Outcome of analysis. double eVal1, eVal2, eVal3; Vec4 eVec1, eVec2, eVec3; // Error statistics; int nFew; }; //========================================================================== // SingleClusterJet class. // Simple helper class to ClusterJet for a jet and its contents. class SingleClusterJet { public: // Constructors. SingleClusterJet(Vec4 pJetIn = 0., int motherIn = 0) : pJet(pJetIn), mother(motherIn), daughter(0), multiplicity(1), isAssigned(false) {pAbs = max( PABSMIN, pJet.pAbs());} SingleClusterJet& operator=(const SingleClusterJet& j) { if (this != &j) { pJet = j.pJet; mother = j.mother; daughter = j.daughter; multiplicity = j.multiplicity; pAbs = j.pAbs; isAssigned = j.isAssigned;} return *this; } // Properties of jet. // Note: mother, daughter and isAssigned only used for original // particles, multiplicity and pTemp only for reconstructed jets. Vec4 pJet; int mother, daughter, multiplicity; bool isAssigned; double pAbs; Vec4 pTemp; // Distance measures (Lund, JADE, Durham) with friend. friend double dist2Fun(int measure, const SingleClusterJet& j1, const SingleClusterJet& j2); private: // Constants: could only be changed in the code itself. static const double PABSMIN; } ; //-------------------------------------------------------------------------- // Namespace function declarations; friend of SingleClusterJet. // Distance measures (Lund, JADE, Durham) with friend. double dist2Fun(int measure, const SingleClusterJet& j1, const SingleClusterJet& j2); //========================================================================== // ClusterJet class. // This class performs a jet clustering according to different // distance measures: Lund, JADE or Durham. class ClusterJet { public: // Constructor. ClusterJet(string measureIn = "Lund", int selectIn = 2, int massSetIn = 2, bool preclusterIn = false, bool reassignIn = false) : measure(1), select(selectIn), massSet(massSetIn), doPrecluster(preclusterIn), doReassign(reassignIn), nFew(0) { char firstChar = toupper(measureIn[0]); if (firstChar == 'J') measure = 2; if (firstChar == 'D') measure = 3; } // Analyze event. bool analyze(const Event& event, double yScaleIn, double pTscaleIn, int nJetMinIn = 1, int nJetMaxIn = 0, ostream& os = cout); // Return info on jets produced. int size() const {return jets.size();} Vec4 p(int i) const {return jets[i].pJet;} int mult(int i) const {return jets[i].multiplicity;} // Return belonging of particle to one of the jets (-1 if none). int jetAssignment(int i) const { for (int iP = 0; iP < int(particles.size()); ++iP) if (particles[iP].mother == i) return particles[iP].daughter; return -1;} // Provide a listing of the info. void list(ostream& os = cout) const; // Return info on clustering values. int distanceSize() const {return distances.size();} double distance(int i) const { return (i < distanceSize()) ? distances[i] : 0.; } // Tell how many events could not be analyzed. int nError() const {return nFew;} private: // Constants: could only be changed in the code itself. static const int TIMESTOPRINT; static const double PIMASS, PABSMIN, PRECLUSTERFRAC, PRECLUSTERSTEP; // Properties of analysis. int measure, select, massSet; bool doPrecluster, doReassign; double yScale, pTscale; int nJetMin, nJetMax; // Temporary results. double dist2Join, dist2BigMin, distPre, dist2Pre; vector particles; int nParticles; // Error statistics; int nFew; // Member functions for some operations (for clarity). void precluster(); void reassign(); // Outcome of analysis: ET-ordered list of jets. vector jets; // Outcome of analysis: the distance values where the jets were merged. deque distances; }; //========================================================================== // SingleCell class. // Simple helper class to CellJet for a cell and its contents. class SingleCell { public: // Constructor. SingleCell(int iCellIn = 0, double etaCellIn = 0., double phiCellIn = 0., double eTcellIn = 0., int multiplicityIn = 0) : iCell(iCellIn), etaCell(etaCellIn), phiCell(phiCellIn), eTcell(eTcellIn), multiplicity(multiplicityIn), canBeSeed(true), isUsed(false), isAssigned(false) {} // Properties of cell. int iCell; double etaCell, phiCell, eTcell; int multiplicity; bool canBeSeed, isUsed, isAssigned; } ; //========================================================================== // SingleCellJet class. // Simple helper class to CellJet for a jet and its contents. class SingleCellJet { public: // Constructor. SingleCellJet(double eTjetIn = 0., double etaCenterIn = 0., double phiCenterIn = 0., double etaWeightedIn = 0., double phiWeightedIn = 0., int multiplicityIn = 0, Vec4 pMassiveIn = 0.) : eTjet(eTjetIn), etaCenter(etaCenterIn), phiCenter(phiCenterIn), etaWeighted(etaWeightedIn), phiWeighted(phiWeightedIn), multiplicity(multiplicityIn), pMassive(pMassiveIn) {} // Properties of jet. double eTjet, etaCenter, phiCenter, etaWeighted, phiWeighted; int multiplicity; Vec4 pMassive; } ; //========================================================================== // CellJet class. // This class performs a cone jet search in (eta, phi, E_T) space. class CellJet { public: // Constructor. CellJet(double etaMaxIn = 5., int nEtaIn = 50, int nPhiIn = 32, int selectIn = 2, int smearIn = 0, double resolutionIn = 0.5, double upperCutIn = 2., double thresholdIn = 0., Rndm* rndmPtrIn = 0) : etaMax(etaMaxIn), nEta(nEtaIn), nPhi(nPhiIn), select(selectIn), smear(smearIn), resolution(resolutionIn), upperCut(upperCutIn), threshold(thresholdIn), nFew(0), rndmPtr(rndmPtrIn) { } // Analyze event. bool analyze(const Event& event, double eTjetMinIn = 20., double coneRadiusIn = 0.7, double eTseedIn = 1.5, ostream& os = cout); // Return info on results of analysis. int size() const {return jets.size();} double eT(int i) const {return jets[i].eTjet;} double etaCenter(int i) const {return jets[i].etaCenter;} double phiCenter(int i) const {return jets[i].phiCenter;} double etaWeighted(int i) const {return jets[i].etaWeighted;} double phiWeighted(int i) const {return jets[i].phiWeighted;} int multiplicity(int i) const {return jets[i].multiplicity;} Vec4 pMassless(int i) const {return jets[i].eTjet * Vec4( cos(jets[i].phiWeighted), sin(jets[i].phiWeighted), sinh(jets[i].etaWeighted), cosh(jets[i].etaWeighted) );} Vec4 pMassive(int i) const {return jets[i].pMassive;} double m(int i) const {return jets[i].pMassive.mCalc();} // Provide a listing of the info. void list(ostream& os = cout) const; // Tell how many events could not be analyzed: so far never. int nError() const {return nFew;} private: // Constants: could only be changed in the code itself. static const int TIMESTOPRINT; // Properties of analysis. double etaMax; int nEta, nPhi, select, smear; double resolution, upperCut, threshold; double eTjetMin, coneRadius, eTseed; // Error statistics; int nFew; // Outcome of analysis: ET-ordered list of jets. vector jets; // Pointer to the random number generator (needed for energy smearing). Rndm* rndmPtr; }; //========================================================================== // SlowJetHook class. // Base class, used to derive your own class with your selection criteria. class SlowJetHook { public: // Destructor. virtual ~SlowJetHook() { } // Method to be overloaded. // It will be called for all final-state particles, one at a time, and // should return true if the particle should be analyzed, false if not. // The particle is in location iSel of the event record. // If you wish you can also modify the four-momentum and mass that will // be used in the analysis, without affecting the event record itself, // by changing pSel and mSel. Remember to respect E^2 - p^2 = m^2. virtual bool include(int iSel, const Event& event, Vec4& pSel, double& mSel) = 0; }; //========================================================================== // SingleSlowJet class. // Simple helper class to SlowJet for a jet and its contents. class SingleSlowJet { public: // Constructors. SingleSlowJet( Vec4 pIn = 0., double pT2In = 0., double yIn = 0., double phiIn = 0., int idxIn = 0) : p(pIn), pT2(pT2In), y(yIn), phi(phiIn), mult(1) { idx.insert(idxIn); } SingleSlowJet(const SingleSlowJet& ssj) : p(ssj.p), pT2(ssj.pT2), y(ssj.y), phi(ssj.phi), mult(ssj.mult), idx(ssj.idx) { } SingleSlowJet& operator=(const SingleSlowJet& ssj) { if (this != &ssj) { p = ssj.p; pT2 = ssj.pT2; y = ssj.y; phi = ssj.phi; mult = ssj.mult; idx = ssj.idx; } return *this; } // Properties of jet. Vec4 p; double pT2, y, phi; int mult; set idx; }; //========================================================================== // SlowJet class. // This class performs a recombination jet search in (y, phi, pT) space. class SlowJet { public: // Constructor. SlowJet(int powerIn, double Rin, double pTjetMinIn = 0., double etaMaxIn = 25., int selectIn = 2, int massSetIn = 2, SlowJetHook* sjHookPtrIn = 0, bool useFJcoreIn = true, bool useStandardRin = true) : power(powerIn), R(Rin), pTjetMin(pTjetMinIn), etaMax(etaMaxIn), select(selectIn), massSet(massSetIn), sjHookPtr(sjHookPtrIn), useFJcore(useFJcoreIn), useStandardR(useStandardRin) { isAnti = (power < 0); isKT = (power > 0); R2 = R*R; pT2jetMin = pTjetMin*pTjetMin; cutInEta = (etaMax <= 20.); chargedOnly = (select > 2); visibleOnly = (select == 2); modifyMass = (massSet < 2); noHook = (sjHookPtr == 0);} // Analyze event, all in one go. bool analyze(const Event& event) { if ( !setup(event) ) return false; if (useFJcore) return clusterFJ(); while (clSize > 0) doStep(); return true; } // Set up list of particles to analyze, and initial distances. bool setup(const Event& event); // Do one recombination step, possibly giving a jet. bool doStep(); // Do several recombinations steps, if possible. bool doNSteps(int nStep) { if (useFJcore) return false; while(nStep > 0 && clSize > 0) { doStep(); --nStep;} return (nStep == 0); } // Do recombinations until fixed numbers of clusters and jets remain. bool stopAtN(int nStop) { if (useFJcore) return false; while (clSize + jtSize > nStop && clSize > 0) doStep(); return (clSize + jtSize == nStop); } // Return info on jet (+cluster) results of analysis. int sizeOrig() const {return origSize;} int sizeJet() const {return jtSize;} int sizeAll() const {return jtSize + clSize;} double pT(int i) const {return (i < jtSize) ? sqrt(jets[i].pT2) : sqrt(clusters[i - jtSize].pT2);} double y(int i) const {return (i < jtSize) ? jets[i].y : clusters[i - jtSize].y;} double phi(int i) const {return (i < jtSize) ? jets[i].phi : clusters[i - jtSize].phi;} Vec4 p(int i) const {return (i < jtSize) ? jets[i].p : clusters[i - jtSize].p;} double m(int i) const {return (i < jtSize) ? jets[i].p.mCalc() : clusters[i - jtSize].p.mCalc();} int multiplicity(int i) const {return (i < jtSize) ? jets[i].mult : clusters[i - jtSize].mult;} // Return info on next step to be taken. int iNext() const {return (iMin == -1) ? -1 : iMin + jtSize;} int jNext() const {return (jMin == -1) ? -1 : jMin + jtSize;} double dNext() const {return dMin;} // Provide a listing of the info. void list(bool listAll = false, ostream& os = cout) const; // Give a list of all particles in the jet. vector constituents(int j) { vector cTemp; for (set::iterator idxTmp = jets[j].idx.begin(); idxTmp != jets[j].idx.end(); ++idxTmp) cTemp.push_back( *idxTmp); return cTemp; } // Give the index of the jet that the particle i of the event record // belongs to. Returns -1 if particle i is not found in a jet. int jetAssignment(int i) { for (int j = 0; j < sizeJet(); ++j) if (jets[j].idx.find(i) != jets[j].idx.end()) return j; return -1; } // Remove a jet. void removeJet(int i) { if (i < 0 || i >= jtSize) return; jets.erase(jets.begin() + i); jtSize--; } private: // Constants: could only be changed in the code itself. static const int TIMESTOPRINT; static const double PIMASS, TINY; // Properties of analysis as such. int power; double R, pTjetMin, etaMax, R2, pT2jetMin; int select, massSet; // SlowJetHook can be used to tailor particle selection step. SlowJetHook* sjHookPtr; bool useFJcore, useStandardR, isAnti, isKT, cutInEta, chargedOnly, visibleOnly, modifyMass, noHook; // Intermediate clustering objects and final jet objects. vector clusters; vector jets; // Intermediate clustering distances. vector diB; vector dij; // Other intermediate variables. int origSize, clSize, clLast, jtSize, iMin, jMin; double dPhi, dijTemp, dMin; // Find next cluster pair to join. void findNext(); // Use FJcore interface to perform clustering. bool clusterFJ(); }; //========================================================================== } // end namespace Pythia8 #endif // end Pythia8_Analysis_H pythia8-8.1.80.orig/include/Pythia8/SigmaOnia.h0000644000175000017500000001734512217346231017335 0ustar sunsun// SigmaOnia.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for charmonia/bottomonia process differential cross sections. // Contains classes derived from SigmaProcess via Sigma2Process. #ifndef Pythia8_SigmaOnia_H #define Pythia8_SigmaOnia_H #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // A derived class for g g -> QQbar[3S1(1)] g (Q = c or b). class Sigma2gg2QQbar3S11g : public Sigma2Process { public: // Constructor. Sigma2gg2QQbar3S11g(int idIn, int codeIn) : idNew(idIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return idHad;} private: // Values stored for process type and colour flow selection. int idNew, idHad, codeSave; string nameSave; double oniumME, sigma; }; //========================================================================== // A derived class for g g -> QQbar[3PJ(1)] g (Q = c or b, J = 0, 1 or 2). class Sigma2gg2QQbar3PJ1g : public Sigma2Process { public: // Constructor. Sigma2gg2QQbar3PJ1g(int idIn, int jIn, int codeIn) : idNew(idIn), jSave(jIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return idHad;} private: // Values stored for process type and colour flow selection. int idNew, idHad, jSave, codeSave; string nameSave; double oniumME, sigma; }; //========================================================================== // A derived class for q g -> QQbar[3PJ(1)] q (Q = c or b, J = 0, 1 or 2). class Sigma2qg2QQbar3PJ1q : public Sigma2Process { public: // Constructor. Sigma2qg2QQbar3PJ1q(int idIn, int jIn, int codeIn) : idNew(idIn), jSave(jIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return idHad;} private: // Values stored for process type and colour flow selection. int idNew, idHad, jSave, codeSave; string nameSave; double oniumME, sigma; }; //========================================================================== // A derived class for q qbar -> QQbar[3PJ(1)] g (Q = c or b, J = 0, 1 or 2). class Sigma2qqbar2QQbar3PJ1g : public Sigma2Process { public: // Constructor. Sigma2qqbar2QQbar3PJ1g(int idIn, int jIn, int codeIn) : idNew(idIn), jSave(jIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return idHad;} private: // Values stored for process type and colour flow selection. int idNew, idHad, jSave, codeSave; string nameSave; double oniumME, sigma; }; //========================================================================== // A derived class for g g -> QQbar[X(8)] g (Q = c or b, X = 3S1, 1S0 or 3PJ). class Sigma2gg2QQbarX8g : public Sigma2Process { public: // Constructor. Sigma2gg2QQbarX8g(int idIn, int stateIn, int codeIn) : idNew(idIn), stateSave(stateIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return idHad;} private: // Values stored for process type and colour flow selection. int idNew, idHad, stateSave, codeSave; string nameSave; double oniumME, sigma; }; //========================================================================== // A derived class for q g -> QQbar[X(8)] q (Q = c or b, X = 3S1, 1S0 or 3PJ). class Sigma2qg2QQbarX8q : public Sigma2Process { public: // Constructor. Sigma2qg2QQbarX8q(int idIn, int stateIn, int codeIn) : idNew(idIn), stateSave(stateIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qg";} virtual int id3Mass() const {return idHad;} private: // Values stored for process type and colour flow selection. int idNew, idHad, stateSave, codeSave; string nameSave; double oniumME, sigma; }; //========================================================================== // A derived class for q qbar -> QQbar[X(8)] g (Q = c or b, // X = 3S1, 1S0 or 3PJ). class Sigma2qqbar2QQbarX8g : public Sigma2Process { public: // Constructor. Sigma2qqbar2QQbarX8g(int idIn, int stateIn, int codeIn) : idNew(idIn), stateSave(stateIn), codeSave(codeIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate d(sigmaHat)/d(tHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return idHad;} private: // Values stored for process type and colour flow selection. int idNew, idHad, stateSave, codeSave; string nameSave; double oniumME, sigma; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaOnia_H pythia8-8.1.80.orig/include/Pythia8/PhaseSpace.h0000644000175000017500000004311512217346230017473 0ustar sunsun// PhaseSpace.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for phase space generators in kinematics selection. // PhaseSpace: base class for phase space generators. // Base class for derived classes> 2 ->1 , 2 -> 2, 2 -> 2 elastic/diffractive, // 2 -> 2 nondiffractive, 2 -> 3, Les Houches. #ifndef Pythia8_PhaseSpace_H #define Pythia8_PhaseSpace_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Info.h" #include "Pythia8/LesHouches.h" #include "Pythia8/MultipartonInteractions.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonDistributions.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/SigmaProcess.h" #include "Pythia8/SigmaTotal.h" #include "Pythia8/Settings.h" #include "Pythia8/StandardModel.h" #include "Pythia8/UserHooks.h" namespace Pythia8 { //========================================================================== // Forward reference to the UserHooks class. class UserHooks; //========================================================================== // PhaseSpace is a base class for phase space generators // used in the selection of hard-process kinematics. class PhaseSpace { public: // Destructor. virtual ~PhaseSpace() {} // Perform simple initialization and store pointers. void init(bool isFirst, SigmaProcess* sigmaProcessPtrIn, Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, Couplings* couplingsPtrIn, SigmaTotal* sigmaTotPtrIn, UserHooks* userHooksPtrIn); // Update the CM energy of the event. void newECM(double eCMin) {eCM = eCMin; s = eCM * eCM;} // Store or replace Les Houches pointer. void setLHAPtr(LHAup* lhaUpPtrIn) {lhaUpPtr = lhaUpPtrIn;} // A pure virtual method, wherein an optimization procedure // is used to determine how phase space should be sampled. virtual bool setupSampling() = 0; // A pure virtual method, wherein a trial event kinematics // is to be selected in the derived class. virtual bool trialKin(bool inEvent = true, bool repeatSame = false) = 0; // A pure virtual method, wherein the accepted event kinematics // is to be constructed in the derived class. virtual bool finalKin() = 0; // Allow for nonisotropic decays when ME's available. void decayKinematics( Event& process); // Give back current or maximum cross section, or set latter. double sigmaNow() const {return sigmaNw;} double sigmaMax() const {return sigmaMx;} double biasSelectionWeight() const {return biasWt;} bool newSigmaMax() const {return newSigmaMx;} void setSigmaMax(double sigmaMaxIn) {sigmaMx = sigmaMaxIn;} // For Les Houches with negative event weight needs virtual double sigmaSumSigned() const {return sigmaMx;} // Give back constructed four-vectors and known masses. Vec4 p(int i) const {return pH[i];} double m(int i) const {return mH[i];} // Give back other event properties. double ecm() const {return eCM;} double x1() const {return x1H;} double x2() const {return x2H;} double sHat() const {return sH;} double tHat() const {return tH;} double uHat() const {return uH;} double pTHat() const {return pTH;} double thetaHat() const {return theta;} double phiHat() const {return phi;} double runBW3() const {return runBW3H;} double runBW4() const {return runBW4H;} double runBW5() const {return runBW5H;} // Inform whether beam particles are resolved in partons or scatter directly. virtual bool isResolved() const {return true;} protected: // Constructor. PhaseSpace() {} // Constants: could only be changed in the code itself. static const int NMAXTRY, NTRY3BODY; static const double SAFETYMARGIN, TINY, EVENFRAC, SAMESIGMA, WIDTHMARGIN, SAMEMASS, MASSMARGIN, EXTRABWWTMAX, THRESHOLDSIZE, THRESHOLDSTEP, YRANGEMARGIN, LEPTONXMIN, LEPTONXMAX, LEPTONXLOGMIN, LEPTONXLOGMAX, LEPTONTAUMIN, SHATMINZ, PT2RATMINZ, WTCORRECTION[11]; // MBR constants: form factor appoximation with two exponents. static const double FFA1, FFA2,FFB1, FFB2; // Pointer to cross section. SigmaProcess* sigmaProcessPtr; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the settings database. Settings* settingsPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to incoming beams. BeamParticle* beamAPtr; BeamParticle* beamBPtr; // Pointer to Standard Model couplings. Couplings* couplingsPtr; // Pointer to the total/elastic/diffractive cross section object. SigmaTotal* sigmaTotPtr; // Pointer to userHooks object for user interaction with program. UserHooks* userHooksPtr; // Pointer to LHAup for generating external events. LHAup* lhaUpPtr; // Initialization data, normally only set once. bool useBreitWigners, doEnergySpread, showSearch, showViolation, increaseMaximum; int gmZmodeGlobal; double mHatGlobalMin, mHatGlobalMax, pTHatGlobalMin, pTHatGlobalMax, pTHatMinDiverge, minWidthBreitWigners, mRecalculate; // Information on incoming beams. int idA, idB; double mA, mB, eCM, s; bool hasLeptonBeams, hasPointLeptons; // Cross section information. bool newSigmaMx, canModifySigma, canBiasSelection, canBias2Sel; int gmZmode; double bias2SelPow, bias2SelRef, wtBW, sigmaNw, sigmaMx, sigmaPos, sigmaNeg, biasWt; // Process-specific kinematics properties, almost always available. double mHatMin, mHatMax, sHatMin, sHatMax, pTHatMin, pTHatMax, pT2HatMin, pT2HatMax; // Event-specific kinematics properties, almost always available. double x1H, x2H, m3, m4, m5, s3, s4, s5, mHat, sH, tH, uH, pAbs, p2Abs, pTH, theta, phi, betaZ; Vec4 pH[6]; double mH[6]; // Reselect decay products momenta isotropically in phase space. void decayKinematicsStep( Event& process, int iRes); // Much common code for normal 2 -> 1, 2 -> 2 and 2 -> 3 cases: // Determine how phase space should be sampled. void setup3Body(); bool setupSampling123(bool is2, bool is3, ostream& os = cout); // Select a trial kinematics phase space point. bool trialKin123(bool is2, bool is3, bool inEvent = true, ostream& os = cout); // Presence and properties of any s-channel resonances. int idResA, idResB; double mResA, mResB, GammaResA, GammaResB, tauResA, tauResB, widResA, widResB; bool sameResMass; // Kinematics properties specific to 2 -> 1/2/3. bool useMirrorWeight; double tau, y, z, tauMin, tauMax, yMax, zMin, zMax, ratio34, unity34, zNeg, zPos, wtTau, wtY, wtZ, wt3Body, runBW3H, runBW4H, runBW5H, intTau0, intTau1, intTau2, intTau3, intTau4, intTau5, intTau6, intY0, intY12, intY34, intY56, mTchan1, sTchan1, mTchan2, sTchan2, frac3Flat, frac3Pow1, frac3Pow2; Vec4 p3cm, p4cm, p5cm; // Coefficients for optimized selection in 2 -> 1/2/3. int nTau, nY, nZ; double tauCoef[8], yCoef[8], zCoef[8], tauCoefSum[8], yCoefSum[8], zCoefSum[8]; // Calculate kinematical limits for 2 -> 1/2/3. bool limitTau(bool is2, bool is3); bool limitY(); bool limitZ(); // Select kinematical variable between defined limits for 2 -> 1/2/3. void selectTau(int iTau, double tauVal, bool is2); void selectY(int iY, double yVal); void selectZ(int iZ, double zVal); bool select3Body(); // Solve equation system for better phase space coefficients in 2 -> 1/2/3. void solveSys( int n, int bin[8], double vec[8], double mat[8][8], double coef[8], ostream& os = cout); // Properties specific to resonance mass selection in 2 -> 2 and 2 -> 3. bool useBW[6]; int idMass[6]; double mPeak[6], sPeak[6], mWidth[6], mMin[6], mMax[6], mw[6], wmRat[6], mLower[6], mUpper[6], sLower[6], sUpper[6], fracFlat[6], fracInv[6], fracInv2[6], atanLower[6], atanUpper[6], intBW[6], intFlat[6], intInv[6], intInv2[6]; // Setup mass selection for one resonance at a time. Split in two parts. void setupMass1(int iM); void setupMass2(int iM, double distToThresh); // Do mass selection and find the associated weight. void trialMass(int iM); double weightMass(int iM); // The error function erf(x) should normally be in your math library, // but if not uncomment this simple parametrization by Sergei Winitzki. //double erf(double x) { double x2 = x * x; double kx2 = 0.147 * x2; // double tmp = sqrt(1. - exp(-x2 * (4./M_PI + kx2) / (1. + kx2))); // return ((x >= 0.) ? tmp : -tmp); } }; //========================================================================== // A derived class with 2 -> 1 kinematics set up in tau, y. class PhaseSpace2to1tauy : public PhaseSpace { public: // Constructor. PhaseSpace2to1tauy() {} // Optimize subsequent kinematics selection. virtual bool setupSampling() {if (!setupMass()) return false; return setupSampling123(false, false);} // Construct the trial kinematics. virtual bool trialKin(bool inEvent = true, bool = false) {wtBW = 1.; return trialKin123(false, false, inEvent);} // Construct the final event kinematics. virtual bool finalKin(); private: // Set up allowed mass range. bool setupMass(); }; //========================================================================== // A derived class with 2 -> 2 kinematics set up in tau, y, z = cos(theta). class PhaseSpace2to2tauyz : public PhaseSpace { public: // Constructor. PhaseSpace2to2tauyz() {} // Optimize subsequent kinematics selection. virtual bool setupSampling() {if (!setupMasses()) return false; return setupSampling123(true, false);} // Construct the trial kinematics. virtual bool trialKin(bool inEvent = true, bool = false) { if (!trialMasses()) return false; return trialKin123(true, false, inEvent);} // Construct the final event kinematics. virtual bool finalKin(); private: // Set up for fixed or Breit-Wigner mass selection. bool setupMasses(); // Select fixed or Breit-Wigner-distributed masses. bool trialMasses(); // Pick off-shell initialization masses when on-shell not allowed. bool constrainedM3M4(); bool constrainedM3(); bool constrainedM4(); }; //========================================================================== // A derived class with 2 -> 2 kinematics set up for elastic scattering. class PhaseSpace2to2elastic : public PhaseSpace { public: // Constructor. PhaseSpace2to2elastic() {} // Construct the trial or final event kinematics. virtual bool setupSampling(); virtual bool trialKin(bool inEvent = true, bool = false); virtual bool finalKin(); // Are beam particles resolved in partons or scatter directly? virtual bool isResolved() const {return false;} private: // Constants: could only be changed in the code itself. static const double EXPMAX, CONVERTEL; // Kinematics properties specific to 2 -> 2 elastic. bool useCoulomb; double s1, s2, bSlope, lambda12S, tLow, tUpp, tAux, sigmaTot, rho, lambda, tAbsMin, phaseCst, alphaEM0, sigmaNuc, sigmaCou, signCou; // Calculation of alphaElectromagnetic. AlphaEM alphaEM; }; //========================================================================== // A derived class with 2 -> 2 kinematics set up for diffractive scattering. class PhaseSpace2to2diffractive : public PhaseSpace { public: // Constructor. PhaseSpace2to2diffractive(bool isDiffAin = false, bool isDiffBin = false) : isDiffA(isDiffAin), isDiffB(isDiffBin) {} // Construct the trial or final event kinematics. virtual bool setupSampling(); virtual bool trialKin(bool inEvent = true, bool = false); virtual bool finalKin(); // Are beam particles resolved in partons or scatter directly? virtual bool isResolved() const {return false;} private: // Constants: could only be changed in the code itself. static const int NTRY; static const double EXPMAX, DIFFMASSMARGIN; // Initialization data, in constructor or read from Settings. bool isDiffA, isDiffB; int PomFlux; double epsilonPF, alphaPrimePF; // Initialization: kinematics properties specific to 2 -> 2 diffractive. double m3ElDiff, m4ElDiff, s1, s2, lambda12, lambda34, tLow, tUpp, cRes, sResXB, sResAX, sProton, bMin, bSlope, bSlope1, bSlope2, probSlope1, xIntPF, xtCorPF, mp24DL, coefDL, tAux, tAux1, tAux2; // Parameters for MBR model. double sdpmax, ddpmax, dymin0, dymax, amx, am1, am2, t; double eps, alph, alph2, m2min, dyminSD, dyminDD, dyminSigSD, dyminSigDD; }; //========================================================================== // A derived class with 2 -> 3 kinematics set up for central diffractive // scattering. class PhaseSpace2to3diffractive : public PhaseSpace { public: // Constructor. PhaseSpace2to3diffractive() {} // Construct the trial or final event kinematics. virtual bool setupSampling(); virtual bool trialKin(bool inEvent = true, bool = false); virtual bool finalKin(); // Are beam particles resolved in partons or scatter directly? virtual bool isResolved() const {return false;} private: // Constants: could only be changed in the code itself. static const int NTRY, NINTEG2; static const double EXPMAX, DIFFMASSMIN, DIFFMASSMARGIN; // Local variables to calculate DPE kinematics. int PomFlux; double epsilonPF, alphaPrimePF, s1, s2, m5min, s5min, tLow[2], tUpp[2], bMin[2], tAux[2], bSlope1, bSlope2, probSlope1[2], tAux1[2], tAux2[2], bSlope, xIntPF, xIntInvPF, xtCorPF, mp24DL, coefDL, epsMBR, alphMBR, m2minMBR, dyminMBR, dyminSigMBR, dyminInvMBR, dpepmax, t1, t2; Vec4 p1, p2, p3, p4, p5; }; //========================================================================== // A derived class for nondiffractive events. Hardly does anything, since // the real action is taken care of by the MultipartonInteractions class. class PhaseSpace2to2nondiffractive : public PhaseSpace { public: // Constructor. PhaseSpace2to2nondiffractive() {} // Construct the trial or final event kinematics. virtual bool setupSampling() {sigmaNw = sigmaProcessPtr->sigmaHat(); sigmaMx = sigmaNw; return true;} virtual bool trialKin( bool , bool = false) {return true;} virtual bool finalKin() {return true;} private: }; //========================================================================== // A derived class with 2 -> 3 kinematics 1 + 2 -> 3 + 4 + 5 set up in // tau, y, pT2_4, pT2_5, phi_4, phi_5 and y_3 (partial cylindrical symmetry). class PhaseSpace2to3tauycyl : public PhaseSpace { public: // Constructor. PhaseSpace2to3tauycyl() {} // Optimize subsequent kinematics selection. virtual bool setupSampling() {if (!setupMasses()) return false; setup3Body(); return setupSampling123(false, true);} // Construct the trial kinematics. virtual bool trialKin(bool inEvent = true, bool = false) { if (!trialMasses()) return false; return trialKin123(false, true, inEvent);} // Construct the final event kinematics. virtual bool finalKin(); private: // Constants: could only be changed in the code itself. static const int NITERNR; // Set up for fixed or Breit-Wigner mass selection. bool setupMasses(); // Select fixed or Breit-Wigner-distributed masses. bool trialMasses(); }; //========================================================================== // A derived class with 2 -> 3 kinematics 1 + 2 -> 3 + 4 + 5 set up in // y3, y4, y5, pT2_3, pT2_5, phi_3 and phi_5, and with R separation cut. // Intended specifically for (essentially massless) 2 -> 3 QCD processes. class PhaseSpace2to3yyycyl : public PhaseSpace { public: // Constructor. PhaseSpace2to3yyycyl() {} // Optimize subsequent kinematics selection. virtual bool setupSampling(); // Construct the trial kinematics. virtual bool trialKin(bool inEvent = true, bool = false); // Construct the final event kinematics. virtual bool finalKin(); private: // Phase space cuts specifically for 2 -> 3 QCD processes. double pTHat3Min, pTHat3Max, pTHat5Min, pTHat5Max, RsepMin, R2sepMin; bool hasBaryonBeams; // Event kinematics choices. double pT3Min, pT3Max, pT5Min, pT5Max, y3Max, y4Max, y5Max, pT3, pT4, pT5, phi3, phi4, phi5, y3, y4, y5, dphi; Vec4 pInSum; }; //========================================================================== // A derived class for Les Houches events. class PhaseSpaceLHA : public PhaseSpace { public: // Constructor. PhaseSpaceLHA() {idProcSave = 0;} // Find maximal cross section for comparison with internal processes. virtual bool setupSampling(); // Construct the next process, by interface to Les Houches class. virtual bool trialKin( bool , bool repeatSame = false); // Set scale, alpha_s and alpha_em if not done. virtual bool finalKin() {sigmaProcessPtr->setScale(); return true;} // For Les Houches with negative event weight needs virtual double sigmaSumSigned() const {return sigmaSgn;} private: // Constants. static const double CONVERTPB2MB; // Local properties. int strategy, stratAbs, nProc, idProcSave; double xMaxAbsSum, xSecSgnSum, sigmaSgn; vector idProc; vector xMaxAbsProc; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_PhaseSpace_H pythia8-8.1.80.orig/include/Pythia8/TimeShower.h0000644000175000017500000002605312217346232017551 0ustar sunsun// TimeShower.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for the timelike final-state showers. // TimeDipoleEnd: data on a radiating dipole end. // TimeShower: handles the showering description. #ifndef Pythia8_TimeShower_H #define Pythia8_TimeShower_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonSystems.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" #include "Pythia8/StandardModel.h" #include "Pythia8/UserHooks.h" #include "Pythia8/MergingHooks.h" namespace Pythia8 { //========================================================================== // Data on radiating dipole ends; only used inside TimeShower class. class TimeDipoleEnd { public: // Constructors. TimeDipoleEnd() : iRadiator(-1), iRecoiler(-1), pTmax(0.), colType(0), chgType(0), gamType(0), weakType(0), isrType(0), system(0), systemRec(0), MEtype(0), iMEpartner(-1), weakPol(0), isOctetOnium(false), isHiddenValley(false), colvType(0), MEmix(0.), MEorder(true), MEsplit(true), MEgluinoRec(false), isFlexible(false) { } TimeDipoleEnd(int iRadiatorIn, int iRecoilerIn, double pTmaxIn = 0., int colIn = 0, int chgIn = 0, int gamIn = 0, int weakTypeIn = 0, int isrIn = 0, int systemIn = 0, int MEtypeIn = 0, int iMEpartnerIn = -1, int weakPolIn = 0, bool isOctetOniumIn = false, bool isHiddenValleyIn = false, int colvTypeIn = 0, double MEmixIn = 0., bool MEorderIn = true, bool MEsplitIn = true, bool MEgluinoRecIn = false, bool isFlexibleIn = false) : iRadiator(iRadiatorIn), iRecoiler(iRecoilerIn), pTmax(pTmaxIn), colType(colIn), chgType(chgIn), gamType(gamIn), weakType(weakTypeIn), isrType(isrIn), system(systemIn), systemRec(systemIn), MEtype(MEtypeIn), iMEpartner(iMEpartnerIn), weakPol(weakPolIn), isOctetOnium(isOctetOniumIn), isHiddenValley(isHiddenValleyIn), colvType(colvTypeIn), MEmix(MEmixIn), MEorder (MEorderIn), MEsplit(MEsplitIn), MEgluinoRec(MEgluinoRecIn), isFlexible(isFlexibleIn) { } // Basic properties related to dipole and matrix element corrections. int iRadiator, iRecoiler; double pTmax; int colType, chgType, gamType, weakType, isrType, system, systemRec, MEtype, iMEpartner, weakPol; bool isOctetOnium, isHiddenValley; int colvType; double MEmix; bool MEorder, MEsplit, MEgluinoRec, isFlexible; // Properties specific to current trial emission. int flavour, iAunt; double mRad, m2Rad, mRec, m2Rec, mDip, m2Dip, m2DipCorr, pT2, m2, z, mFlavour, asymPol, flexFactor; } ; //========================================================================== // The TimeShower class does timelike showers. class TimeShower { public: // Constructor. TimeShower() {beamOffset = 0;} // Destructor. virtual ~TimeShower() {} // Initialize various pointers. // (Separated from rest of init since not virtual.) void initPtr(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, CoupSM* coupSMPtrIn, PartonSystems* partonSystemsPtrIn, UserHooks* userHooksPtrIn, MergingHooks* mergingHooksPtrIn = 0) { infoPtr = infoPtrIn; settingsPtr = settingsPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; coupSMPtr = coupSMPtrIn; partonSystemsPtr = partonSystemsPtrIn; userHooksPtr = userHooksPtrIn; mergingHooksPtr = mergingHooksPtrIn;} // Initialize alphaStrong and related pTmin parameters. virtual void init( BeamParticle* beamAPtrIn = 0, BeamParticle* beamBPtrIn = 0); // New beams possible for handling of hard diffraction. (Not virtual.) void reassignBeamPtrs( BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, int beamOffsetIn = 0) {beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; beamOffset = beamOffsetIn;} // Find whether to limit maximum scale of emissions, and whether to dampen. virtual bool limitPTmax( Event& event, double Q2Fac = 0., double Q2Ren = 0.); // Potential enhancement factor of pTmax scale for hardest emission. double enhancePTmax() {return pTmaxFudge;} // Top-level routine to do a full time-like shower in resonance decay. virtual int shower( int iBeg, int iEnd, Event& event, double pTmax, int nBranchMax = 0); // Top-level routine for QED radiation in hadronic decay to two leptons. virtual int showerQED( int i1, int i2, Event& event, double pTmax); // Provide the pT scale of the last branching in the above shower. double pTLastInShower() {return pTLastBranch;} // Global recoil: reset counters and store locations of outgoing partons. virtual void prepareGlobal( Event& event); // Prepare system for evolution after each new interaction; identify ME. virtual void prepare( int iSys, Event& event, bool limitPTmaxIn = true, double pTfirstTrialIn = 1e9); // Update dipole list after a multiparton interactions rescattering. virtual void rescatterUpdate( int iSys, Event& event); // Update dipole list after each ISR emission. virtual void update( int iSys, Event& event); // Select next pT in downwards evolution. virtual double pTnext( Event& event, double pTbegAll, double pTendAll, bool isFirstTrial = false); // ME corrections and kinematics that may give failure. virtual bool branch( Event& event, bool isInterleaved = false); // Tell which system was the last processed one. int system() const {return iSysSel;}; // Print dipole list; for debug mainly. virtual void list( ostream& os = cout) const; protected: // Pointer to various information on the generation. Info* infoPtr; // Pointer to the settings database. Settings* settingsPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointer to Standard Model couplings. CoupSM* coupSMPtr; // Pointers to the two incoming beams. Offset their location in event. BeamParticle* beamAPtr; BeamParticle* beamBPtr; int beamOffset; // Pointer to information on subcollision parton locations. PartonSystems* partonSystemsPtr; // Pointer to userHooks object for user interaction with program. UserHooks* userHooksPtr; // Store properties to be returned by methods. int iSysSel; double pTmaxFudge, pTLastBranch; private: // Constants: could only be changed in the code itself. static const double SIMPLIFYROOT, XMARGIN, XMARGINCOMB, TINYPDF, LARGEM2, THRESHM2, LAMBDA3MARGIN; // Rescatter: try to fix up recoil between systems static const bool FIXRESCATTER, VETONEGENERGY; static const double MAXVIRTUALITYFRACTION, MAXNEGENERGYFRACTION; // Initialization data, normally only set once. bool doQCDshower, doQEDshowerByQ, doQEDshowerByL, doQEDshowerByGamma, doWeakShower, doMEcorrections, doMEafterFirst, doPhiPolAsym, doInterleave, allowBeamRecoil, dampenBeamRecoil, recoilToColoured, allowRescatter, canVetoEmission, doHVshower, brokenHVsym, globalRecoil, useLocalRecoilNow, doSecondHard, singleWeakEmission, dopTdampMass, alphaSuseCMW; int pTmaxMatch, pTdampMatch, alphaSorder, alphaSnfmax, nGluonToQuark, alphaEMorder, nGammaToQuark, nGammaToLepton, nCHV, idHV, nMaxGlobalRecoil, weakMode; double pTdampFudge, mc, mb, m2c, m2b, renormMultFac, factorMultFac, alphaSvalue, alphaS2pi, Lambda3flav, Lambda4flav, Lambda5flav, Lambda3flav2, Lambda4flav2, Lambda5flav2, pTcolCutMin, pTcolCut, pT2colCut, pTchgQCut, pT2chgQCut, pTchgLCut, pT2chgLCut, pTweakCut, pT2weakCut, mMaxGamma, m2MaxGamma, octetOniumFraction, octetOniumColFac, mZ, gammaZ, thetaWRat, mW, gammaW, CFHV, alphaHVfix, pThvCut, pT2hvCut, mHV, pTmaxFudgeMPI, weakEnhancement, pTfirstTrial, extraScaleTerm; // alphaStrong and alphaEM calculations. AlphaStrong alphaS; AlphaEM alphaEM; // Some current values. bool dopTlimit1, dopTlimit2, dopTdamp, hasWeaklyRadiated; double pT2damp, kRad, kEmt; // All dipole ends and a pointer to the selected hardest dipole end. vector dipEnd; TimeDipoleEnd* dipSel; int iDipSel; // Setup a dipole end, either QCD, QED/photon, weak or Hidden Valley one. void setupQCDdip( int iSys, int i, int colTag, int colSign, Event& event, bool isOctetOnium = false, bool limitPTmaxIn = true); void setupQEDdip( int iSys, int i, int chgType, int gamType, Event& event, bool limitPTmaxIn = true); void setupWeakdip( int iSys, int i,int weakType, Event& event, bool limitPTmaxIn = true); void setupHVdip( int iSys, int i, Event& event, bool limitPTmaxIn = true); // Evolve a QCD dipole end. void pT2nextQCD( double pT2begDip, double pT2sel, TimeDipoleEnd& dip, Event& event); // Evolve a QED dipole end, either charged or photon. void pT2nextQED( double pT2begDip, double pT2sel, TimeDipoleEnd& dip, Event& event); // Evolve a weak dipole end. void pT2nextWeak( double pT2begDip, double pT2sel, TimeDipoleEnd& dip, Event& event); // Evolve a Hidden Valley dipole end. void pT2nextHV( double pT2begDip, double pT2sel, TimeDipoleEnd& dip, Event& ); // Find kind of QCD ME correction. void findMEtype( Event& event, TimeDipoleEnd& dip); // Find type of particle; used by findMEtype. int findMEparticle( int id, bool isHiddenColour = false); // Find mixture of V and A in gamma/Z: energy- and flavour-dependent. double gammaZmix( Event& event, int iRes, int iDau1, int iDau2); // Set up to calculate QCD ME correction with calcMEcorr. double findMEcorr(TimeDipoleEnd* dip, Particle& rad, Particle& partner, Particle& emt, bool cutEdge = true); // Calculate value of QCD ME correction. double calcMEcorr( int kind, int combiIn, double mixIn, double x1, double x2, double r1, double r2, double r3 = 0., bool cutEdge = true); // Find coefficient of azimuthal asymmetry from gluon polarization. void findAsymPol( Event& event, TimeDipoleEnd* dip); // Rescatter: propagate dipole recoil to internal lines connecting systems. bool rescatterPropagateRecoil( Event& event, Vec4& pNew); // Properties stored for (some) global recoil schemes. // Vectors of event indices defining the hard process. vector hardPartons; // Number of proposed splittings, number of partons in current hard event, // number of partons in Born-type hard event (distinguish between S and H). int nProposed, nHard, nFinalBorn, nMaxGlobalBranch; // Number of splittings with global recoil (currently only 1). int nGlobal, globalRecoilMode; // Switch to constrain recoiling system. bool limitMUQ; // Pointer to MergingHooks object for NLO merging. MergingHooks* mergingHooksPtr; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_TimeShower_H pythia8-8.1.80.orig/include/Pythia8/HiddenValleyFragmentation.h0000644000175000017500000001137612217346227022560 0ustar sunsun// HiddenValleyFragmentation.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the classes for Hidden-Valley fragmentation. #ifndef Pythia8_HiddenValleyFragmentation_H #define Pythia8_HiddenValleyFragmentation_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/FragmentationFlavZpT.h" #include "Pythia8/FragmentationSystems.h" #include "Pythia8/Info.h" #include "Pythia8/MiniStringFragmentation.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" #include "Pythia8/StringFragmentation.h" namespace Pythia8 { //========================================================================== // The HVStringFlav class is used to select HV-quark and HV-hadron flavours. class HVStringFlav : public StringFlav { public: // Constructor. HVStringFlav() {} // Destructor. ~HVStringFlav() {} // Initialize data members. void init(Settings& settings, Rndm* rndmPtrIn); // Pick a new flavour (including diquarks) given an incoming one. FlavContainer pick(FlavContainer& flavOld); // Combine two flavours (including diquarks) to produce a hadron. int combine(FlavContainer& flav1, FlavContainer& flav2); private: // Initialization data, to be read from Settings. int nFlav; double probVector; }; //========================================================================== // The HVStringPT class is used to select select HV transverse momenta. class HVStringPT : public StringPT { public: // Constructor. HVStringPT() {} // Destructor. ~HVStringPT() {} // Initialize data members. void init(Settings& settings, ParticleData& particleData, Rndm* rndmPtrIn); }; //========================================================================== // The HVStringZ class is used to sample the HV fragmentation function f(z). class HVStringZ : public StringZ { public: // Constructor. HVStringZ() {} // Destructor. ~HVStringZ() {} // Initialize data members. void init(Settings& settings, ParticleData& particleData, Rndm* rndmPtrIn); // Fragmentation function: top-level to determine parameters. double zFrag( int idOld, int idNew = 0, double mT2 = 1.); // Parameters for stopping in the middle; for now hardcoded. virtual double stopMass() {return 1.5 * mhvMeson;} virtual double stopNewFlav() {return 2.0;} virtual double stopSmear() {return 0.2;} private: // Initialization data, to be read from Settings and ParticleData. double mqv2, bmqv2, rFactqv, mhvMeson; }; //========================================================================== // The HiddenValleyFragmentation class contains the routines // to fragment a Hidden Valley partonic system. class HiddenValleyFragmentation { public: // Constructor. HiddenValleyFragmentation() : doHVfrag(false), hvFlavSelPtr(NULL), hvPTSelPtr(NULL), hvZSelPtr(NULL) {} // Destructor. ~HiddenValleyFragmentation() { if (doHVfrag) { if (hvZSelPtr) delete hvZSelPtr; if (hvPTSelPtr) delete hvPTSelPtr; if (hvFlavSelPtr) delete hvFlavSelPtr;} } // Initialize and save pointers. bool init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn); // Do the fragmentation: driver routine. bool fragment(Event& event); private: // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Data mambers. bool doHVfrag; int nFlav, hvOldSize, hvNewSize; double mhvMeson, mSys; vector ihvParton; // Configuration of colour-singlet systems. ColConfig hvColConfig; // Temporary event record for the Hidden Valley system. Event hvEvent; // The generator class for Hidden Valley string fragmentation. StringFragmentation hvStringFrag; // The generator class for special low-mass HV string fragmentation. MiniStringFragmentation hvMinistringFrag; // Pointers to classes for flavour, pT and z generation in HV sector. StringFlav* hvFlavSelPtr; StringPT* hvPTSelPtr; StringZ* hvZSelPtr; // Extract HV-particles from event to hvEvent. Assign HV-colours. bool extractHVevent(Event& event); // Collapse of low-mass system to one HV-meson. bool collapseToMeson(); // Insert HV particles from hvEvent to event. bool insertHVevent(Event& event); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_HiddenValleyFragmentation_H pythia8-8.1.80.orig/include/Pythia8/FragmentationFlavZpT.h0000644000175000017500000001517112217346227021533 0ustar sunsun// FragmentationFlavZpT.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains helper classes for fragmentation. // StringFlav is used to select quark and hadron flavours. // StringPT is used to select transverse momenta. // StringZ is used to sample the fragmentation function f(z). #ifndef Pythia8_FragmentationFlavZpT_H #define Pythia8_FragmentationFlavZpT_H #include "Pythia8/Basics.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // The FlavContainer class is a simple container for flavour, // including the extra properties needed for popcorn baryon handling. // id = current flavour. // rank = current rank; 0 for endpoint flavour and then increase by 1. // nPop = number of popcorn mesons yet to be produced (1 or 0). // idPop = (absolute sign of) popcorn quark, shared between B and Bbar. // idVtx = (absolute sign of) vertex (= non-shared) quark in diquark. class FlavContainer { public: // Constructor. FlavContainer(int idIn = 0, int rankIn = 0, int nPopIn = 0, int idPopIn = 0, int idVtxIn = 0) : id(idIn), rank(rankIn), nPop(nPopIn), idPop(idPopIn), idVtx(idVtxIn) {} // Overloaded equal operator. FlavContainer& operator=(const FlavContainer& flav) { if (this != &flav) { id = flav.id; rank = flav.rank; nPop = flav.nPop; idPop = flav.idPop; idVtx = flav.idVtx; } return *this; } // Invert flavour. FlavContainer& anti() {id = -id; return *this;} // Read in a container into another, without/with id sign flip. FlavContainer& copy(const FlavContainer& flav) { if (this != &flav) { id = flav.id; rank = flav.rank; nPop = flav.nPop; idPop = flav.idPop; idVtx = flav.idVtx; } return *this; } FlavContainer& anti(const FlavContainer& flav) { if (this != &flav) { id = -flav.id; rank = flav.rank; nPop = flav.nPop; idPop = flav.idPop; idVtx = flav.idVtx; } return *this; } // Check whether is diquark. bool isDiquark() {int idAbs = abs(id); return (idAbs > 1000 && idAbs < 10000 && (idAbs/10)%10 == 0);} // Stored properties. int id, rank, nPop, idPop, idVtx; }; //========================================================================== // The StringFlav class is used to select quark and hadron flavours. class StringFlav { public: // Constructor. StringFlav() {} // Destructor. virtual ~StringFlav() {} // Initialize data members. virtual void init(Settings& settings, Rndm* rndmPtrIn); // Pick a light d, u or s quark according to fixed ratios. int pickLightQ() { double rndmFlav = probQandS * rndmPtr->flat(); if (rndmFlav < 1.) return 1; if (rndmFlav < 2.) return 2; return 3; } // Pick a new flavour (including diquarks) given an incoming one. virtual FlavContainer pick(FlavContainer& flavOld); // Combine two flavours (including diquarks) to produce a hadron. virtual int combine(FlavContainer& flav1, FlavContainer& flav2); // Assign popcorn quark inside an original (= rank 0) diquark. void assignPopQ(FlavContainer& flav); // Combine two quarks to produce a diquark. int makeDiquark(int id1, int id2, int idHad = 0); protected: // Pointer to the random number generator. Rndm* rndmPtr; private: // Constants: could only be changed in the code itself. static const int mesonMultipletCode[6]; static const double baryonCGOct[6], baryonCGDec[6]; // Initialization data, to be read from Settings. bool suppressLeadingB; double probQQtoQ, probStoUD, probSQtoQQ, probQQ1toQQ0, probQandQQ, probQandS, probQandSinQQ, probQQ1corr, probQQ1corrInv, probQQ1norm, mesonRate[4][6], mesonRateSum[4], mesonMix1[2][6], mesonMix2[2][6], etaSup, etaPrimeSup, decupletSup, baryonCGSum[6], baryonCGMax[6], popcornRate, popcornSpair, popcornSmeson, scbBM[3], popFrac, popS[3], dWT[3][7], lightLeadingBSup, heavyLeadingBSup; }; //========================================================================== // The StringZ class is used to sample the fragmentation function f(z). class StringZ { public: // Constructor. StringZ() {} // Destructor. virtual ~StringZ() {} // Initialize data members. virtual void init(Settings& settings, ParticleData& particleData, Rndm* rndmPtrIn); // Fragmentation function: top-level to determine parameters. virtual double zFrag( int idOld, int idNew = 0, double mT2 = 1.); // Parameters for stopping in the middle; overloaded for Hidden Valley. virtual double stopMass() {return stopM;} virtual double stopNewFlav() {return stopNF;} virtual double stopSmear() {return stopS;} // b fragmentation parameter needed to weight final two solutions. virtual double bAreaLund() {return bLund;} protected: // Constants: could only be changed in the code itself. static const double CFROMUNITY, AFROMZERO, AFROMC, EXPMAX; // Initialization data, to be read from Settings. bool useNonStandC, useNonStandB, useNonStandH, usePetersonC, usePetersonB, usePetersonH; double mc2, mb2, aLund, bLund, aExtraDiquark, rFactC, rFactB, rFactH, aNonC, aNonB, aNonH, bNonC, bNonB, bNonH, epsilonC, epsilonB, epsilonH, stopM, stopNF, stopS; // Fragmentation function: select z according to provided parameters. double zLund( double a, double b, double c = 1.); double zPeterson( double epsilon); // Pointer to the random number generator. Rndm* rndmPtr; }; //========================================================================== // The StringPT class is used to select select transverse momenta. class StringPT { public: // Constructor. StringPT() {} // Destructor. virtual ~StringPT() {} // Initialize data members. virtual void init(Settings& settings, ParticleData& particleData, Rndm* rndmPtrIn); // Return px and py as a pair in the same call. pair pxy(); // Gaussian suppression of given pT2; used in MiniStringFragmentation. double suppressPT2(double pT2) { return exp( -pT2 / sigma2Had); } protected: // Constants: could only be changed in the code itself. static const double SIGMAMIN; // Initialization data, to be read from Settings. double sigmaQ, enhancedFraction, enhancedWidth, sigma2Had; // Pointer to the random number generator. Rndm* rndmPtr; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_FragmentationFlavZpT_H pythia8-8.1.80.orig/include/Pythia8/Pythia.h0000644000175000017500000002737712217346230016731 0ustar sunsun// Pythia.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file contains the main class for event generation. // Pythia: provide the main user interface to everything else. #ifndef Pythia8_Pythia_H #define Pythia8_Pythia_H #include "Pythia8/Analysis.h" #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/BeamShape.h" #include "Pythia8/Event.h" #include "Pythia8/FragmentationFlavZpT.h" #include "Pythia8/HadronLevel.h" #include "Pythia8/History.h" #include "Pythia8/Info.h" #include "Pythia8/LesHouches.h" #include "Pythia8/PartonLevel.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonDistributions.h" #include "Pythia8/PartonSystems.h" #include "Pythia8/ProcessLevel.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/ResonanceWidths.h" #include "Pythia8/RHadrons.h" #include "Pythia8/Settings.h" #include "Pythia8/SigmaTotal.h" #include "Pythia8/SpaceShower.h" #include "Pythia8/StandardModel.h" #include "Pythia8/SLHAinterface.h" #include "Pythia8/TimeShower.h" #include "Pythia8/UserHooks.h" #include "Pythia8/MergingHooks.h" #include "Pythia8/Merging.h" namespace Pythia8 { //========================================================================== // The Pythia class contains the top-level routines to generate an event. class Pythia { public: // Constructor. (See Pythia.cc file.) Pythia(string xmlDir = "../xmldoc", bool printBanner = true); // Destructor. (See Pythia.cc file.) ~Pythia(); // Read in one update for a setting or particle data from a single line. bool readString(string, bool warn = true); // Read in updates for settings or particle data from user-defined file. bool readFile(string fileName, bool warn = true, int subrun = SUBRUNDEFAULT); bool readFile(string fileName, int subrun) { return readFile(fileName, true, subrun);} bool readFile(istream& is = cin, bool warn = true, int subrun = SUBRUNDEFAULT); bool readFile(istream& is, int subrun) { return readFile(is, true, subrun);} // Possibility to pass in pointers to PDF's. bool setPDFPtr( PDF* pdfAPtrIn, PDF* pdfBPtrIn, PDF* pdfHardAPtrIn = 0, PDF* pdfHardBPtrIn = 0, PDF* pdfPomAPtrIn = 0, PDF* pdfPomBPtrIn = 0); // Possibility to pass in pointer to external LHA-interfaced generator. bool setLHAupPtr( LHAup* lhaUpPtrIn) {lhaUpPtr = lhaUpPtrIn; return true;} // Possibility to pass in pointer for external handling of some decays. bool setDecayPtr( DecayHandler* decayHandlePtrIn, vector handledParticlesIn) {decayHandlePtr = decayHandlePtrIn; handledParticles.resize(0); for(int i = 0; i < int(handledParticlesIn.size()); ++i) handledParticles.push_back( handledParticlesIn[i] ); return true;} // Possibility to pass in pointer for external random number generation. bool setRndmEnginePtr( RndmEngine* rndmEnginePtrIn) { return rndm.rndmEnginePtr( rndmEnginePtrIn);} // Possibility to pass in pointer for user hooks. bool setUserHooksPtr( UserHooks* userHooksPtrIn) { userHooksPtr = userHooksPtrIn; return true;} // Possibility to pass in pointer for merging hooks. bool setMergingHooksPtr( MergingHooks* mergingHooksPtrIn) { mergingHooksPtr = mergingHooksPtrIn; return true;} // Possibility to pass in pointer for beam shape. bool setBeamShapePtr( BeamShape* beamShapePtrIn) { beamShapePtr = beamShapePtrIn; return true;} // Possibility to pass in pointer(s) for external cross section. bool setSigmaPtr( SigmaProcess* sigmaPtrIn) { sigmaPtrs.push_back( sigmaPtrIn); return true;} // Possibility to pass in pointer(s) for external resonance. bool setResonancePtr( ResonanceWidths* resonancePtrIn) { resonancePtrs.push_back( resonancePtrIn); return true;} // Possibility to pass in pointer for external showers. bool setShowerPtr( TimeShower* timesDecPtrIn, TimeShower* timesPtrIn = 0, SpaceShower* spacePtrIn = 0) { timesDecPtr = timesDecPtrIn; timesPtr = timesPtrIn; spacePtr = spacePtrIn; return true;} // Initialization using the Beams variables. bool init(); // Deprecated: initialization in the CM frame. bool init( int idAin, int idBin, double eCMin); // Deprecated: initialization with two collinear beams, e.g. fixed target. bool init( int idAin, int idBin, double eAin, double eBin); // Deprecated: initialization with two acollinear beams. bool init( int idAin, int idBin, double pxAin, double pyAin, double pzAin, double pxBin, double pyBin, double pzBin); // Deprecated: initialization by a Les Houches Event File. bool init( string LesHouchesEventFile, bool skipInit = false); // Deprecated: initialization according to the Les Houches Accord. bool init( LHAup* lhaUpPtrIn); // Generate the next event. bool next(); // Generate only a single timelike shower as in a decay. int forceTimeShower( int iBeg, int iEnd, double pTmax, int nBranchMax = 0) { return timesDecPtr->shower( iBeg, iEnd, event, pTmax, nBranchMax); } // Generate only the hadronization/decay stage. bool forceHadronLevel( bool findJunctions = true); // Special routine to allow more decays if on/off switches changed. bool moreDecays() {return hadronLevel.moreDecays(event);} // Special routine to force R-hadron decay when not done before. bool forceRHadronDecays() {return doRHadronDecays();} // List the current Les Houches event. void LHAeventList(ostream& os = cout) { if (lhaUpPtr != 0) lhaUpPtr->listEvent(os);} // Skip a number of Les Houches events at input. bool LHAeventSkip(int nSkip) { if (lhaUpPtr != 0) return lhaUpPtr->skipEvent(nSkip); return false;} // Main routine to provide final statistics on generation. void stat(); // Deprecated: alternative to provide final statistics on generation. void statistics(bool all = false, bool reset = false); // Read in settings values: shorthand, not new functionality. bool flag(string key) {return settings.flag(key);} int mode(string key) {return settings.mode(key);} double parm(string key) {return settings.parm(key);} string word(string key) {return settings.word(key);} // Auxiliary to set parton densities among list of possibilities. PDF* getPDFPtr(int idIn, int sequence = 1); // The event record for the parton-level central process. Event process; // The event record for the complete event history. Event event; // Information on the generation: current subprocess and error statistics. Info info; // Settings: databases of flags/modes/parms/words to control run. Settings settings; // ParticleData: the particle data table/database. ParticleData particleData; // Random number generator. Rndm rndm; // Standard Model couplings, including alphaS and alphaEM. Couplings couplings; Couplings* couplingsPtr; // SLHA Interface SLHAinterface slhaInterface; // The partonic content of each subcollision system (auxiliary to event). PartonSystems partonSystems; // Merging object as wrapper for matrix element merging routines. Merging merging; // Pointer to MergingHooks object for user interaction with the merging. // MergingHooks also more generally steers the matrix element merging. MergingHooks* mergingHooksPtr; private: // Copy and = constructors are made private so they cannot be used. Pythia(const Pythia&); Pythia& operator=(const Pythia&); // Constants: could only be changed in the code itself. static const double VERSIONNUMBERCODE; static const int NTRY, SUBRUNDEFAULT; // Initialization data, extracted from database. string xmlPath; bool doProcessLevel, doPartonLevel, doHadronLevel, doDiffraction, doResDec, doFSRinRes, decayRHadrons, abortIfVeto, checkEvent, checkHistory; int nErrList; double epTolErr, epTolWarn; // Initialization data, extracted from init(...) call. bool isConstructed, isInit, isUnresolvedA, isUnresolvedB, showSaV, showMaD; int idA, idB, frameType, boostType, nCount, nShowLHA, nShowInfo, nShowProc, nShowEvt; double mA, mB, pxA, pxB, pyA, pyB, pzA, pzB, eA, eB, pzAcm, pzBcm, eCM, betaZ, gammaZ; Vec4 pAinit, pBinit, pAnow, pBnow; RotBstMatrix MfromCM, MtoCM; // information for error checkout. int nErrEvent; vector iErrId, iErrCol, iErrEpm, iErrNan, iErrNanVtx; // Pointers to the parton distributions of the two incoming beams. PDF* pdfAPtr; PDF* pdfBPtr; // Extra PDF pointers to be used in hard processes only. PDF* pdfHardAPtr; PDF* pdfHardBPtr; // Extra Pomeron PDF pointers to be used in diffractive processes only. PDF* pdfPomAPtr; PDF* pdfPomBPtr; // Keep track when "new" has been used and needs a "delete" for PDF's. bool useNewPdfA, useNewPdfB, useNewPdfHard, useNewPdfPomA, useNewPdfPomB; // The two incoming beams. BeamParticle beamA; BeamParticle beamB; // Alternative Pomeron beam-inside-beam. BeamParticle beamPomA; BeamParticle beamPomB; // LHAup object for generating external events. bool doLHA, useNewLHA; LHAup* lhaUpPtr; // Pointer to external decay handler and list of particles it handles. DecayHandler* decayHandlePtr; vector handledParticles; // Pointer to UserHooks object for user interaction with program. UserHooks* userHooksPtr; bool hasUserHooks, doVetoProcess, doVetoPartons, retryPartonLevel; // Pointer to BeamShape object for beam momentum and interaction vertex. BeamShape* beamShapePtr; bool useNewBeamShape, doMomentumSpread, doVertexSpread; // Pointers to external processes derived from the Pythia base classes. vector sigmaPtrs; // Pointers to external calculation of resonance widths. vector resonancePtrs; // Pointers to timelike and spacelike showers. TimeShower* timesDecPtr; TimeShower* timesPtr; SpaceShower* spacePtr; bool useNewTimes, useNewSpace; // The main generator class to define the core process of the event. ProcessLevel processLevel; // The main generator class to produce the parton level of the event. PartonLevel partonLevel; // The main generator class to perform trial showers of the event. PartonLevel trialPartonLevel; // Flags for defining the merging scheme. bool hasMergingHooks, hasOwnMergingHooks, doMerging; // The main generator class to produce the hadron level of the event. HadronLevel hadronLevel; // The total cross section class is used both on process and parton level. SigmaTotal sigmaTot; // The RHadrons class is used both at PartonLevel and HadronLevel. RHadrons rHadrons; // Write the Pythia banner, with symbol and version information. void banner(ostream& os = cout); // Check for lines in file that mark the beginning of new subrun. int readSubrun(string line, bool warn = true, ostream& os = cout); // Check that combinations of settings are allowed; change if not. void checkSettings(); // Check that beams and beam combination can be handled. bool checkBeams(); // Calculate kinematics at initialization. bool initKinematics(); // Set up pointers to PDFs. bool initPDFs(); // Recalculate kinematics for each event when beam momentum has a spread. void nextKinematics(); // Boost from CM frame to lab frame, or inverse. Set production vertex. void boostAndVertex(bool toLab, bool setVertex); // Perform R-hadron decays. bool doRHadronDecays(); // Check that the final event makes sense. bool check(ostream& os = cout); // Initialization of SLHA data. bool initSLHA (); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_Pythia_H pythia8-8.1.80.orig/include/Pythia8/ParticleData.h0000644000175000017500000006512612217346230020022 0ustar sunsun// ParticleData.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for the classes containing particle data. // DecayChannel contains info on a single decay channel. // ParticleDataEntry contains info on a single particle species. // ParticleData collects info on all particles as a map. #ifndef Pythia8_ParticleData_H #define Pythia8_ParticleData_H #include "Pythia8/Basics.h" #include "Pythia8/Info.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" #include "Pythia8/StandardModel.h" namespace Pythia8 { //========================================================================== // Forward reference to some classes. class ParticleData; class ResonanceWidths; class Couplings; class CoupSUSY; class SUSYResonanceWidths; //========================================================================== // This class holds info on a single decay channel. class DecayChannel { public: // Constructor. DecayChannel(int onModeIn = 0, double bRatioIn = 0., int meModeIn = 0, int prod0 = 0, int prod1 = 0, int prod2 = 0, int prod3 = 0, int prod4 = 0, int prod5 = 0, int prod6 = 0, int prod7 = 0) : onModeSave(onModeIn), bRatioSave(bRatioIn), currentBRSave(0.), onShellWidthSave(0.), openSecPos(1.), openSecNeg(1.), meModeSave(meModeIn), nProd(0), hasChangedSave(true) { prod[0] = prod0; prod[1] = prod1; prod[2] = prod2; prod[3] = prod3; prod[4] = prod4; prod[5] = prod5; prod[6] = prod6; prod[7] = prod7; for (int j = 0; j < 8; ++j) if (prod[j] != 0 && j == nProd) ++nProd; } // Member functions for input. void onMode(int onModeIn) {onModeSave = onModeIn; hasChangedSave = true;} void bRatio(double bRatioIn, bool countAsChanged = true) { bRatioSave = bRatioIn; if (countAsChanged) hasChangedSave = true;} void rescaleBR(double fac) {bRatioSave *= fac; hasChangedSave = true;} void meMode(int meModeIn) {meModeSave = meModeIn; hasChangedSave = true;} void multiplicity(int multIn) {nProd = multIn; hasChangedSave = true;} void product(int i, int prodIn) {prod[i] = prodIn; nProd = 0; for (int j = 0; j < 8; ++j) if (prod[j] != 0 && j == nProd) ++nProd; hasChangedSave = true;} void setHasChanged(bool hasChangedIn) {hasChangedSave = hasChangedIn;} // Member functions for output. int onMode() const {return onModeSave;} double bRatio() const {return bRatioSave;} int meMode() const {return meModeSave;} int multiplicity() const {return nProd;} int product(int i) const {return (i >= 0 && i < nProd) ? prod[i] : 0;} bool hasChanged() const { return hasChangedSave;} // Check for presence of particles anywhere in decay list. bool contains(int id1) const; bool contains(int id1, int id2) const; bool contains(int id1, int id2, int id3) const; // Input/output for current selection of decay modes. // Takes into account on/off switches and dynamic width for resonances. void currentBR(double currentBRIn) {currentBRSave = currentBRIn;} double currentBR() const {return currentBRSave;} // Input/output for nominal partial width; used by resonances. void onShellWidth(double onShellWidthIn) { onShellWidthSave = onShellWidthIn;} double onShellWidth() const {return onShellWidthSave;} void onShellWidthFactor(double factor) {onShellWidthSave *= factor;} // Input/output for fraction of secondary open widths; used by resonances. void openSec(int idSgn, double openSecIn) { if (idSgn > 0) openSecPos = openSecIn; else openSecNeg = openSecIn;} double openSec(int idSgn) const { return (idSgn > 0) ? openSecPos : openSecNeg;} private: // Decay channel info. int onModeSave; double bRatioSave, currentBRSave, onShellWidthSave, openSecPos, openSecNeg; int meModeSave, nProd, prod[8]; bool hasChangedSave; }; //========================================================================== // This class holds info on a single particle species. class ParticleDataEntry { public: // Constructors: for antiparticle exists or not. ParticleDataEntry(int idIn = 0, string nameIn = " ", int spinTypeIn = 0, int chargeTypeIn = 0, int colTypeIn = 0, double m0In = 0., double mWidthIn = 0., double mMinIn = 0., double mMaxIn = 0., double tau0In = 0.) : idSave(abs(idIn)), nameSave(nameIn), antiNameSave("void"), spinTypeSave(spinTypeIn), chargeTypeSave(chargeTypeIn), colTypeSave(colTypeIn), m0Save(m0In), mWidthSave (mWidthIn), mMinSave(mMinIn), mMaxSave(mMaxIn), tau0Save(tau0In), hasAntiSave(false), hasChangedSave(true), resonancePtr(0) {setDefaults();} ParticleDataEntry(int idIn, string nameIn, string antiNameIn, int spinTypeIn = 0, int chargeTypeIn = 0, int colTypeIn = 0, double m0In = 0., double mWidthIn = 0., double mMinIn = 0., double mMaxIn = 0., double tau0In = 0.) : idSave(abs(idIn)), nameSave(nameIn), antiNameSave(antiNameIn), spinTypeSave(spinTypeIn), chargeTypeSave(chargeTypeIn), colTypeSave(colTypeIn), m0Save(m0In), mWidthSave (mWidthIn), mMinSave(mMinIn), mMaxSave(mMaxIn), tau0Save(tau0In), hasAntiSave(true), hasChangedSave(true), resonancePtr(0) {setDefaults(); if (toLower(antiNameIn) == "void") hasAntiSave = false;} // Destructor: delete any ResonanceWidths object. ~ParticleDataEntry(); // Initialization of some particle flags. void setDefaults(); // Store pointer to whole particle data table/database. void initPtr( ParticleData* particleDataPtrIn) { particleDataPtr = particleDataPtrIn;} // Reset all the properties of an existing particle. void setAll(string nameIn, string antiNameIn, int spinTypeIn = 0, int chargeTypeIn = 0, int colTypeIn = 0, double m0In = 0., double mWidthIn = 0., double mMinIn = 0., double mMaxIn = 0., double tau0In = 0.) {nameSave = nameIn; antiNameSave = antiNameIn; hasAntiSave = true; if (toLower(antiNameIn) == "void") hasAntiSave = false; spinTypeSave = spinTypeIn; chargeTypeSave = chargeTypeIn; colTypeSave = colTypeIn; m0Save = m0In; mWidthSave = mWidthIn; mMinSave = mMinIn; mMaxSave = mMaxIn; tau0Save = tau0In; setDefaults(); hasChangedSave = true;} // Change current values one at a time (or set if not set before). // (Must use set here since else name+signature clash with get methods.) void setName(string nameIn) {nameSave = nameIn; hasChangedSave = true;} void setAntiName(string antiNameIn) {antiNameSave = antiNameIn; hasChangedSave = true;} void setNames(string nameIn, string antiNameIn) {nameSave = nameIn; antiNameSave = antiNameIn; hasAntiSave = true; if (toLower(antiNameIn) == "void") hasAntiSave = false; hasChangedSave = true;} void setSpinType(int spinTypeIn) {spinTypeSave = spinTypeIn; hasChangedSave = true;} void setChargeType(int chargeTypeIn) {chargeTypeSave = chargeTypeIn; hasChangedSave = true;} void setColType(int colTypeIn) {colTypeSave = colTypeIn; hasChangedSave = true;} void setM0(double m0In) {m0Save = m0In; setConstituentMass(); hasChangedSave = true;} void setMWidth(double mWidthIn, bool countAsChanged = true) { mWidthSave = mWidthIn; if (countAsChanged) hasChangedSave = true;} void setMMin(double mMinIn) {mMinSave = mMinIn; hasChangedSave = true;} void setMMax(double mMaxIn) {mMaxSave = mMaxIn; hasChangedSave = true;} // Special options specifically when cutting wings of Breit-Wigners. void setMMinNoChange(double mMinIn) {mMinSave = mMinIn;} void setMMaxNoChange(double mMaxIn) {mMaxSave = mMaxIn;} void setTau0(double tau0In) {tau0Save = tau0In; hasChangedSave = true;} void setIsResonance(bool isResonanceIn) {isResonanceSave = isResonanceIn; hasChangedSave = true;} void setMayDecay(bool mayDecayIn, bool countAsChanged = true) { mayDecaySave = mayDecayIn; if (countAsChanged) hasChangedSave = true;} void setDoExternalDecay(bool doExternalDecayIn) {doExternalDecaySave = doExternalDecayIn; hasChangedSave = true;} void setIsVisible(bool isVisibleIn) {isVisibleSave = isVisibleIn; hasChangedSave = true;} void setDoForceWidth(bool doForceWidthIn) {doForceWidthSave = doForceWidthIn; hasChangedSave = true;} void setHasChanged(bool hasChangedIn) {hasChangedSave = hasChangedIn; for (int i = 0; i < int(channels.size()); ++i) channels[i].setHasChanged(hasChangedIn);} // Give back current values. int id() const { return idSave; } bool hasAnti() const { return hasAntiSave; } string name(int idIn = 1) const { return (idIn > 0) ? nameSave : antiNameSave; } int spinType() const {return spinTypeSave; } int chargeType(int idIn = 1) const { return (idIn > 0) ? chargeTypeSave : -chargeTypeSave; } double charge(int idIn = 1) const { return (idIn > 0) ? chargeTypeSave / 3. : -chargeTypeSave / 3.; } int colType(int idIn = 1) const { if (colTypeSave == 2) return colTypeSave; return (idIn > 0) ? colTypeSave : -colTypeSave; } double m0() const { return m0Save; } double mWidth() const { return mWidthSave; } double mMin() const { return mMinSave; } double mMax() const { return mMaxSave; } double m0Min() const { return (modeBWnow == 0) ? m0Save : mMinSave; } double m0Max() const { return (modeBWnow == 0) ? m0Save : mMaxSave; } double tau0() const { return tau0Save; } bool isResonance() const { return isResonanceSave; } bool mayDecay() const { return mayDecaySave; } bool doExternalDecay() const { return doExternalDecaySave; } bool isVisible() const { return isVisibleSave; } bool doForceWidth() const { return doForceWidthSave; } bool hasChanged() const { if (hasChangedSave) return true; for (int i = 0; i < int(channels.size()); ++i) if (channels[i].hasChanged()) return true; return false;} // Set and give back several mass-related quantities. void initBWmass(); double constituentMass() const { return constituentMassSave; } double mSel(); double mRun(double mH); // Give back other quantities. bool useBreitWigner() const { return (modeBWnow > 0); } bool canDecay() const { return (channels.size() > 0);} bool isLepton() const { return (idSave > 10 && idSave < 19);} bool isQuark() const { return (idSave != 0 && idSave < 9);} bool isGluon() const { return (idSave == 21);} bool isDiquark() const { return (idSave > 1000 && idSave < 10000 && (idSave/10)%10 == 0);} bool isParton() const { return ( idSave == 21 || (idSave != 0 && idSave < 6) || (idSave > 1000 && idSave < 5510 && (idSave/10)%10 == 0) );} bool isHadron() const; bool isMeson() const; bool isBaryon() const; // Intermediate octet ccbar or bbar states in colour-octet model. bool isOctetHadron() const {return (idSave == 9900441 || idSave == 9900443 || idSave == 9900551 || idSave == 9900553 || idSave == 9910441 || idSave == 9910551); } int heaviestQuark(int idIn = 1) const; int baryonNumberType(int idIn = 1) const; // Reset to empty decay table. void clearChannels() {channels.resize(0);} // Add a decay channel to the decay table. void addChannel(int onMode = 0, double bRatio = 0., int meMode = 0, int prod0 = 0, int prod1 = 0, int prod2 = 0, int prod3 = 0, int prod4 = 0, int prod5 = 0, int prod6 = 0, int prod7 = 0) { channels.push_back( DecayChannel( onMode, bRatio, meMode, prod0, prod1, prod2, prod3, prod4, prod5, prod6, prod7) ); } // Decay table size. int sizeChannels() const {return channels.size();} // Gain access to a channel in the decay table. DecayChannel& channel(int i){return channels[i];} const DecayChannel& channel(int i) const {return channels[i];} // Rescale sum of branching ratios to unity. void rescaleBR(double newSumBR = 1.); // Random choice of decay channel according to branching ratios. bool preparePick(int idSgn, double mHat = 0., int idInFlav = 0); DecayChannel& pickChannel(); // Access methods stored in ResonanceWidths. void setResonancePtr(ResonanceWidths* resonancePtrIn); ResonanceWidths* getResonancePtr() {return resonancePtr;} void resInit(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Couplings* couplingsPtrIn); double resWidth(int idSgn, double mHat, int idIn = 0, bool openOnly = false, bool setBR = false); double resWidthOpen(int idSgn, double mHat, int idIn = 0); double resWidthStore(int idSgn, double mHat, int idIn = 0); double resOpenFrac(int idSgn); double resWidthRescaleFactor(); double resWidthChan(double mHat, int idAbs1 = 0, int idAbs2 = 0); private: // Constants: could only be changed in the code itself. static const int INVISIBLENUMBER, INVISIBLETABLE[50], KNOWNNOWIDTH[3]; static const double MAXTAU0FORDECAY,MINMASSRESONANCE, NARROWMASS, CONSTITUENTMASSTABLE[10]; // Particle data. int idSave; string nameSave, antiNameSave; int spinTypeSave, chargeTypeSave, colTypeSave; double m0Save, mWidthSave, mMinSave, mMaxSave, tau0Save, constituentMassSave; bool hasAntiSave, isResonanceSave, mayDecaySave, doExternalDecaySave, isVisibleSave, doForceWidthSave, hasChangedSave; // Extra data for mass selection according to a Breit-Wigner. int modeBWnow; double atanLow, atanDif, mThr; // A vector containing all the decay channels of the particle. vector channels; // Summed branching ratio of currently open channels. double currentBRSum; // Pointer to ResonanceWidths object; only used for some particles. ResonanceWidths* resonancePtr; // Pointer to the full particle data table. ParticleData* particleDataPtr; // Set constituent mass. void setConstituentMass(); // Useful functions for string handling. string toLower(const string& nameConv) { string temp(nameConv); for (int i = 0; i < int(temp.length()); ++i) temp[i] = tolower(temp[i]); return temp; } }; //========================================================================== // This class holds a map of all ParticleDataEntries. class ParticleData { public: // Constructor. ParticleData() : infoPtr(0), settingsPtr(0), rndmPtr(0), couplingsPtr(0), particlePtr(0), isInit(false), readingFailedSave(false) {} // Initialize pointers. void initPtr(Info* infoPtrIn, Settings* settingsPtrIn, Rndm* rndmPtrIn, Couplings* couplingsPtrIn) {infoPtr = infoPtrIn; settingsPtr = settingsPtrIn; rndmPtr = rndmPtrIn; couplingsPtr = couplingsPtrIn;} // Read in database from specific file. bool init(string startFile = "../xmldoc/ParticleData.xml") { initCommon(); return readXML(startFile);} // Overwrite existing database by reading from specific file. bool reInit(string startFile, bool xmlFormat = true) { initCommon(); return (xmlFormat) ? readXML(startFile) : readFF(startFile);} // Initialize pointers, normal Breit-Wigners and special resonances. void initWidths(vector resonancePtrs); // Read or list whole (or part of) database from/to an XML file. bool readXML(string inFile, bool reset = true) ; void listXML(string outFile); // Read or list whole (or part of) database from/to a free format file. bool readFF(string inFile, bool reset = true) ; void listFF(string outFile); // Read in one update from a single line. bool readString(string lineIn, bool warn = true, ostream& os = cout) ; // Keep track whether any readings have failed, invalidating run setup. bool readingFailed() {return readingFailedSave;} // Print out table of whole database, or of only part of it. void listAll(ostream& os = cout) {list(false, true, os);} void listChanged(ostream& os = cout) {list(true, false, os);} void listChanged(bool changedRes, ostream& os = cout) { list(true, changedRes, os);} void list(bool changedOnly = false, bool changedRes = true, ostream& os = cout); // Print out specified particles. void list(int idList, ostream& os = cout) {vector idListTemp; idListTemp.push_back(idList); list( idListTemp, os);} void list(vector idList, ostream& os = cout); // Check that table makes sense, especially for decays. void checkTable(ostream& os = cout) {checkTable(1, os);}; void checkTable(int verbosity, ostream& os = cout) ; // Add new entry. void addParticle(int idIn, string nameIn = " ", int spinTypeIn = 0, int chargeTypeIn = 0, int colTypeIn = 0, double m0In = 0., double mWidthIn = 0., double mMinIn = 0., double mMaxIn = 0., double tau0In = 0.) { pdt[abs(idIn)] = ParticleDataEntry(idIn, nameIn, spinTypeIn, chargeTypeIn, colTypeIn, m0In, mWidthIn, mMinIn, mMaxIn, tau0In); } void addParticle(int idIn, string nameIn, string antiNameIn, int spinTypeIn = 0, int chargeTypeIn = 0, int colTypeIn = 0, double m0In = 0., double mWidthIn = 0., double mMinIn = 0., double mMaxIn = 0., double tau0In = 0.) { pdt[abs(idIn)] = ParticleDataEntry(idIn, nameIn, antiNameIn, spinTypeIn, chargeTypeIn, colTypeIn, m0In, mWidthIn, mMinIn, mMaxIn, tau0In); } // Reset all the properties of an entry in one go. void setAll(int idIn, string nameIn, string antiNameIn, int spinTypeIn = 0, int chargeTypeIn = 0, int colTypeIn = 0, double m0In = 0., double mWidthIn = 0., double mMinIn = 0., double mMaxIn = 0.,double tau0In = 0.) { if (isParticle(idIn)) pdt[abs(idIn)].setAll( nameIn, antiNameIn, spinTypeIn, chargeTypeIn, colTypeIn, m0In, mWidthIn, mMinIn, mMaxIn, tau0In); } // Query existence of an entry. bool isParticle(int idIn) { if (pdt.find(abs(idIn)) == pdt.end()) return false; if (idIn > 0 || pdt[abs(idIn)].hasAnti()) return true; return false; } // Return the id of the sequentially next particle stored in table. int nextId(int idIn) ; // Change current values one at a time (or set if not set before). void name(int idIn, string nameIn) { if (isParticle(idIn)) pdt[abs(idIn)].setName(nameIn); } void antiName(int idIn, string antiNameIn) { if (isParticle(idIn)) pdt[abs(idIn)].setAntiName(antiNameIn); } void names(int idIn, string nameIn, string antiNameIn) { if (isParticle(idIn)) pdt[abs(idIn)].setNames(nameIn, antiNameIn); } void spinType(int idIn, int spinTypeIn) { if (isParticle(idIn)) pdt[abs(idIn)].setSpinType(spinTypeIn); } void chargeType(int idIn, int chargeTypeIn) { if (isParticle(idIn)) pdt[abs(idIn)].setChargeType(chargeTypeIn); } void colType(int idIn, int colTypeIn) { if (isParticle(idIn)) pdt[abs(idIn)].setColType(colTypeIn); } void m0(int idIn, double m0In) { if (isParticle(idIn)) pdt[abs(idIn)].setM0(m0In); } void mWidth(int idIn, double mWidthIn) { if (isParticle(idIn)) pdt[abs(idIn)].setMWidth(mWidthIn); } void mMin(int idIn, double mMinIn) { if (isParticle(idIn)) pdt[abs(idIn)].setMMin(mMinIn); } void mMax(int idIn, double mMaxIn) { if (isParticle(idIn)) pdt[abs(idIn)].setMMax(mMaxIn); } void tau0(int idIn, double tau0In) { if (isParticle(idIn)) pdt[abs(idIn)].setTau0(tau0In); } void isResonance(int idIn, bool isResonanceIn) { if (isParticle(idIn)) pdt[abs(idIn)].setIsResonance(isResonanceIn); } void mayDecay(int idIn, bool mayDecayIn) { if (isParticle(idIn)) pdt[abs(idIn)].setMayDecay(mayDecayIn); } void doExternalDecay(int idIn, bool doExternalDecayIn) { if (isParticle(idIn)) pdt[abs(idIn)].setDoExternalDecay(doExternalDecayIn); } void isVisible(int idIn, bool isVisibleIn) { if (isParticle(idIn)) pdt[abs(idIn)].setIsVisible(isVisibleIn); } void doForceWidth(int idIn, bool doForceWidthIn) { if (isParticle(idIn)) pdt[abs(idIn)].setDoForceWidth(doForceWidthIn); } void hasChanged(int idIn, bool hasChangedIn) { if (isParticle(idIn)) pdt[abs(idIn)].setHasChanged(hasChangedIn); } // Give back current values. bool hasAnti(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].hasAnti() : false ; } string name(int idIn) { return (isParticle(abs(idIn))) ? pdt[abs(idIn)].name(idIn) : " "; } int spinType(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].spinType() : 0 ; } int chargeType(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].chargeType(idIn) : 0 ; } double charge(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].charge(idIn) : 0 ; } int colType(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].colType(idIn) : 0 ; } double m0(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].m0() : 0. ; } double mWidth(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].mWidth() : 0. ; } double mMin(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].mMin() : 0. ; } double m0Min(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].m0Min() : 0. ; } double mMax(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].mMax() : 0. ; } double m0Max(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].m0Max() : 0. ; } double tau0(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].tau0() : 0. ; } bool isResonance(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isResonance() : false ; } bool mayDecay(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].mayDecay() : false ; } bool doExternalDecay(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].doExternalDecay() : false ; } bool isVisible(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isVisible() : false ; } bool doForceWidth(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].doForceWidth() : false ; } bool hasChanged(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].hasChanged() : false ; } // Give back special mass-related quantities. bool useBreitWigner(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].useBreitWigner() : false ; } double constituentMass(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].constituentMass() : 0. ; } double mSel(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].mSel() : 0. ; } double mRun(int idIn, double mH) { return isParticle(idIn) ? pdt[abs(idIn)].mRun(mH) : 0. ; } // Give back other quantities. bool canDecay(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].canDecay() : false ; } bool isLepton(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isLepton() : false ; } bool isQuark(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isQuark() : false ; } bool isGluon(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isGluon() : false ; } bool isDiquark(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isDiquark() : false ; } bool isParton(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isParton() : false ; } bool isHadron(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isHadron() : false ; } bool isMeson(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isMeson() : false ; } bool isBaryon(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isBaryon() : false ; } bool isOctetHadron(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].isOctetHadron() : false ; } int heaviestQuark(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].heaviestQuark(idIn) : 0 ; } int baryonNumberType(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].baryonNumberType(idIn) : 0 ; } // Change branching ratios. void rescaleBR(int idIn, double newSumBR = 1.) { if (isParticle(idIn)) pdt[abs(idIn)].rescaleBR(newSumBR); } // Access methods stored in ResonanceWidths. void setResonancePtr(int idIn, ResonanceWidths* resonancePtrIn) { if (isParticle(idIn)) pdt[abs(idIn)].setResonancePtr( resonancePtrIn);} void resInit(int idIn) { if (isParticle(idIn)) pdt[abs(idIn)].resInit(infoPtr, settingsPtr, this, couplingsPtr);} double resWidth(int idIn, double mHat, int idInFlav = 0, bool openOnly = false, bool setBR = false) { return isParticle(idIn) ? pdt[abs(idIn)].resWidth(idIn, mHat, idInFlav, openOnly, setBR) : 0.;} double resWidthOpen(int idIn, double mHat, int idInFlav = 0) { return isParticle(idIn) ? pdt[abs(idIn)].resWidthOpen(idIn, mHat, idInFlav) : 0.;} double resWidthStore(int idIn, double mHat, int idInFlav = 0) { return isParticle(idIn) ? pdt[abs(idIn)].resWidthStore(idIn, mHat, idInFlav) : 0.;} double resOpenFrac(int id1In, int id2In = 0, int id3In = 0); double resWidthRescaleFactor(int idIn) { return isParticle(idIn) ? pdt[abs(idIn)].resWidthRescaleFactor() : 0.;} double resWidthChan(int idIn, double mHat, int idAbs1 = 0, int idAbs2 = 0) { return isParticle(idIn) ? pdt[abs(idIn)].resWidthChan( mHat, idAbs1, idAbs2) : 0.;} // Return pointer to entry. ParticleDataEntry* particleDataEntryPtr(int idIn) { return (isParticle(idIn)) ? &pdt[abs(idIn)] : &pdt[0]; } private: // Common data, accessible for the individual particles. int modeBreitWigner; double maxEnhanceBW, mQRun[7], Lambda5Run; // The individual particle need access to the full database. friend class ParticleDataEntry; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the settings database. Settings* settingsPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointer to Standard Model couplings. Couplings* couplingsPtr; // All particle data stored in a map. map pdt; // Pointer to current particle (e.g. when reading decay channels). ParticleDataEntry* particlePtr; // Flag that initialization has been performed; whether any failures. bool isInit, readingFailedSave; // Method for common setting of particle-specific info. void initCommon(); // Useful functions for string handling. string toLower(const string& nameConv) { string temp(nameConv); for (int i = 0; i < int(temp.length()); ++i) temp[i] = tolower(temp[i]); return temp; } bool boolString(string tag) { string tagLow = toLower(tag); return ( tagLow == "true" || tagLow == "1" || tagLow == "on" || tagLow == "yes" || tagLow == "ok" ); } // Extract XML value following XML attribute. string attributeValue(string line, string attribute); bool boolAttributeValue(string line, string attribute); int intAttributeValue(string line, string attribute); double doubleAttributeValue(string line, string attribute); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_ParticleData_H pythia8-8.1.80.orig/include/Pythia8/PythiaStdlib.h0000644000175000017500000000502612217346230020056 0ustar sunsun// PythiaStdlib.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for functionality pulled in from Stdlib, // plus a few useful utilities (small powers; positive square root, // Gamma function). #ifndef Pythia8_PythiaStdlib_H #define Pythia8_PythiaStdlib_H // Stdlib header files for mathematics. #include #include #include // Stdlib header files for strings and containers. #include #include #include #include #include // Stdlib header file for input and output. #include #include #include #include // Define pi if not yet done. #ifndef M_PI #define M_PI 3.1415926535897932385 #endif // By this declaration you do not need to use std:: qualifier everywhere. //using namespace std; // Alternatively you can specify exactly which std:: methods will be used. // Now made default so std does not spill outside namespace Pythia8. namespace Pythia8 { // Generic utilities and mathematical functions. using std::swap; using std::max; using std::min; using std::abs; using std::sort; // Strings and containers. using std::pair; using std::make_pair; using std::string; using std::vector; using std::map; using std::multimap; using std::deque; using std::set; // Input/output streams. using std::cin; using std::cout; using std::cerr; using std::istream; using std::ostream; using std::fstream; using std::ifstream; using std::ofstream; using std::stringstream; using std::istringstream; using std::ostringstream; using std::ios; // Input/output formatting. using std::endl; using std::fixed; using std::scientific; using std::left; using std::right; using std::setw; using std::setprecision; } // end namespace Pythia8 namespace Pythia8 { // Powers of small integers - for balance speed/code clarity. inline double pow2(const double& x) {return x*x;} inline double pow3(const double& x) {return x*x*x;} inline double pow4(const double& x) {return x*x*x*x;} inline double pow5(const double& x) {return x*x*x*x*x;} inline double pow6(const double& x) {return x*x*x*x*x*x;} // Avoid problem with negative square root argument (from roundoff). inline double sqrtpos(const double& x) {return sqrt( max( 0., x));} // The Gamma function for real argument. double GammaReal(double x); } // end namespace Pythia8 #endif // Pythia8_PythiaStdlib_H pythia8-8.1.80.orig/include/Pythia8/LesHouches.h0000644000175000017500000003615012217346227017530 0ustar sunsun// LesHouches.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for Les Houches Accord user process information. // LHAProcess: stores a single process; used by the other classes. // LHAParticle: stores a single particle; used by the other classes. // LHAup: base class for initialization and event information. // LHAupLHEF: derived class for reading from an Les Houches Event File. // Code for interfacing with Fortran commonblocks is found in LHAFortran.h. #ifndef Pythia8_LesHouches_H #define Pythia8_LesHouches_H #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // A class for the processes stored in LHAup. class LHAProcess { public: // Constructors. LHAProcess() : idProc(0), xSecProc(0.), xErrProc(0.), xMaxProc(0.) { } LHAProcess(int idProcIn, double xSecIn, double xErrIn, double xMaxIn) : idProc(idProcIn), xSecProc(xSecIn), xErrProc(xErrIn), xMaxProc(xMaxIn) { } // Process properties. int idProc; double xSecProc, xErrProc, xMaxProc; } ; //========================================================================== // A class for the particles stored in LHAup. class LHAParticle { public: // Constructors. LHAParticle() : idPart(0), statusPart(0), mother1Part(0), mother2Part(0), col1Part(0), col2Part(0), pxPart(0.), pyPart(0.), pzPart(0.), ePart(0.), mPart(0.), tauPart(0.), spinPart(9.), scalePart(-1.) { } LHAParticle(int idIn, int statusIn, int mother1In, int mother2In, int col1In, int col2In, double pxIn, double pyIn, double pzIn, double eIn, double mIn, double tauIn, double spinIn, double scaleIn) : idPart(idIn), statusPart(statusIn), mother1Part(mother1In), mother2Part(mother2In), col1Part(col1In), col2Part(col2In), pxPart(pxIn), pyPart(pyIn), pzPart(pzIn), ePart(eIn), mPart(mIn), tauPart(tauIn), spinPart(spinIn), scalePart(scaleIn) { } // Particle properties. int idPart, statusPart, mother1Part, mother2Part, col1Part, col2Part; double pxPart, pyPart, pzPart, ePart, mPart, tauPart, spinPart, scalePart; } ; //========================================================================== // LHAup is base class for initialization and event information // from an external parton-level generator. class LHAup { public: // Destructor. virtual ~LHAup() {} // Set info pointer. void setPtr(Info* infoPtrIn) {infoPtr = infoPtrIn;} // Method to be used for LHAupLHEF derived class. virtual void newEventFile(const char*) {} virtual bool fileFound() {return true;} // A pure virtual method setInit, wherein all initialization information // is supposed to be set in the derived class. Can do this by reading a // file or some other way, as desired. Returns false if it did not work. virtual bool setInit() = 0; // Give back info on beams. int idBeamA() const {return idBeamASave;} int idBeamB() const {return idBeamBSave;} double eBeamA() const {return eBeamASave;} double eBeamB() const {return eBeamBSave;} int pdfGroupBeamA() const {return pdfGroupBeamASave;} int pdfGroupBeamB() const {return pdfGroupBeamBSave;} int pdfSetBeamA() const {return pdfSetBeamASave;} int pdfSetBeamB() const {return pdfSetBeamBSave;} // Give back weight strategy. int strategy() const {return strategySave;} // Give back info on processes. int sizeProc() const {return processes.size();} int idProcess(int proc) const {return processes[proc].idProc;} double xSec(int proc) const {return processes[proc].xSecProc;} double xErr(int proc) const {return processes[proc].xErrProc;} double xMax(int proc) const {return processes[proc].xMaxProc;} double xSecSum() const {return xSecSumSave;} double xErrSum() const {return xErrSumSave;} // Print the initialization info; useful to check that setting it worked. void listInit(ostream& os = cout); // A pure virtual method setEvent, wherein information on the next event // is supposed to be set in the derived class. // Strategies +-1 and +-2: idProcIn is the process type, selected by PYTHIA. // Strategies +-3 and +-4: idProcIn is dummy; process choice is made locally. // The method can find the next event by a runtime interface to another // program, or by reading a file, as desired. // The method should return false if it did not work. virtual bool setEvent(int idProcIn = 0, double mRecalculate = -1.) = 0; // Give back process number, weight, scale, alpha_em, alpha_s. int idProcess() const {return idProc;} double weight() const {return weightProc;} double scale() const {return scaleProc;} double alphaQED() const {return alphaQEDProc;} double alphaQCD() const {return alphaQCDProc;} // Give back info on separate particle. int sizePart() const {return particles.size();} int id(int part) const {return particles[part].idPart;} int status(int part) const {return particles[part].statusPart;} int mother1(int part) const {return particles[part].mother1Part;} int mother2(int part) const {return particles[part].mother2Part;} int col1(int part) const {return particles[part].col1Part;} int col2(int part) const {return particles[part].col2Part;} double px(int part) const {return particles[part].pxPart;} double py(int part) const {return particles[part].pyPart;} double pz(int part) const {return particles[part].pzPart;} double e(int part) const {return particles[part].ePart;} double m(int part) const {return particles[part].mPart;} double tau(int part) const {return particles[part].tauPart;} double spin(int part) const {return particles[part].spinPart;} double scale(int part) const {return particles[part].scalePart;} // Give back info on flavour and x values of hard-process initiators. int id1() const {return id1Save;} int id2() const {return id2Save;} double x1() const {return x1Save;} double x2() const {return x2Save;} // Optional: give back info on parton density values of event. bool pdfIsSet() const {return pdfIsSetSave;} int id1pdf() const {return id1pdfSave;} int id2pdf() const {return id2pdfSave;} double x1pdf() const {return x1pdfSave;} double x2pdf() const {return x2pdfSave;} double scalePDF() const {return scalePDFSave;} double pdf1() const {return pdf1Save;} double pdf2() const {return pdf2Save;} // Print the info; useful to check that reading an event worked. void listEvent(ostream& os = cout); // Skip ahead a number of events, which are not considered further. // Mainly intended for debug when using the LHAupLHEF class. virtual bool skipEvent(int nSkip) { for (int iSkip = 0; iSkip < nSkip; ++iSkip) if (!setEvent()) return false; return true;} // Four routines to write a Les Houches Event file in steps. bool openLHEF(string fileNameIn); bool initLHEF(); bool eventLHEF(bool verbose = true); bool closeLHEF(bool updateInit = false); protected: // Constructor. Sets default to be that events come with unit weight. LHAup(int strategyIn = 3) : strategySave(strategyIn) { processes.reserve(10); particles.reserve(20); } // Allow conversion from mb to pb. static const double CONVERTMB2PB; // Pointer to various information on the generation. Info* infoPtr; // Input beam info. void setBeamA(int idIn, double eIn, int pdfGroupIn = 0, int pdfSetIn = 0) { idBeamASave = idIn; eBeamASave = eIn; pdfGroupBeamASave = pdfGroupIn; pdfSetBeamASave = pdfSetIn;} void setBeamB(int idIn, double eIn, int pdfGroupIn = 0, int pdfSetIn = 0) { idBeamBSave = idIn; eBeamBSave = eIn; pdfGroupBeamBSave = pdfGroupIn; pdfSetBeamBSave = pdfSetIn;} // Input process weight strategy. void setStrategy(int strategyIn) {strategySave = strategyIn;} // Input process info. void addProcess(int idProcIn, double xSecIn = 1., double xErrIn = 0., double xMaxIn = 1.) { processes.push_back( LHAProcess( idProcIn, xSecIn, xErrIn, xMaxIn)); } // Possibility to update some cross section info at end of run. void setXSec(int iP, double xSecIn) {processes[iP].xSecProc = xSecIn;} void setXErr(int iP, double xErrIn) {processes[iP].xErrProc = xErrIn;} void setXMax(int iP, double xMaxIn) {processes[iP].xMaxProc = xMaxIn;} // Input info on the selected process. void setProcess(int idProcIn = 0, double weightIn = 1., double scaleIn = 0., double alphaQEDIn = 0.0073, double alphaQCDIn = 0.12) { idProc = idProcIn; weightProc = weightIn; scaleProc = scaleIn; alphaQEDProc = alphaQEDIn; alphaQCDProc = alphaQCDIn; // Clear particle list. Add empty zeroth particle for correct indices. particles.clear(); addParticle(0); pdfIsSetSave = false;} // Input particle info, one particle at the time. void addParticle(LHAParticle particleIn) { particles.push_back(particleIn);} void addParticle(int idIn, int statusIn = 0, int mother1In = 0, int mother2In = 0, int col1In = 0, int col2In = 0, double pxIn = 0., double pyIn = 0., double pzIn = 0., double eIn = 0., double mIn = 0., double tauIn = 0., double spinIn = 9., double scaleIn = -1.) { particles.push_back( LHAParticle( idIn, statusIn, mother1In, mother2In, col1In, col2In, pxIn, pyIn, pzIn, eIn, mIn, tauIn, spinIn, scaleIn) ); } // Input info on flavour and x values of hard-process initiators. void setIdX(int id1In, int id2In, double x1In, double x2In) { id1Save = id1In; id2Save = id2In; x1Save = x1In; x2Save = x2In;} // Optionally input info on parton density values of event. void setPdf(int id1pdfIn, int id2pdfIn, double x1pdfIn, double x2pdfIn, double scalePDFIn, double pdf1In, double pdf2In, bool pdfIsSetIn) { id1pdfSave = id1pdfIn; id2pdfSave = id2pdfIn; x1pdfSave = x1pdfIn; x2pdfSave = x2pdfIn; scalePDFSave = scalePDFIn; pdf1Save = pdf1In; pdf2Save = pdf2In; pdfIsSetSave = pdfIsSetIn;} // Three routines for LHEF files, but put here for flexibility. bool setInitLHEF(istream& is, bool readHeaders = false); bool setNewEventLHEF(istream& is, double mRecalculate = -1.); bool setOldEventLHEF(); // Helper routines to open and close a file handling GZIPSUPPORT: // ifstream ifs; // istream *is = openFile("myFile.txt", ifs); // -- Process file using is -- // closeFile(is, ifs); istream* openFile(const char *fn, ifstream &ifs); void closeFile(istream *&is, ifstream &ifs); // LHAup is a friend class to infoPtr, but derived classes // are not. This wrapper function can be used by derived classes // to set headers in the Info class. void setInfoHeader(const string &key, const string &val) { infoPtr->setHeader(key, val); } // Event properties from LHEF files, for repeated use. int nupSave, idprupSave; double xwgtupSave, scalupSave, aqedupSave, aqcdupSave, xSecSumSave, xErrSumSave; vector particlesSave; bool getPDFSave, getScale; int id1InSave, id2InSave, id1pdfInSave, id2pdfInSave; double x1InSave, x2InSave, x1pdfInSave, x2pdfInSave, scalePDFInSave, pdf1InSave, pdf2InSave; private: // Event weighting and mixing strategy. int strategySave; // Beam particle properties. int idBeamASave, idBeamBSave; double eBeamASave, eBeamBSave; int pdfGroupBeamASave, pdfGroupBeamBSave, pdfSetBeamASave, pdfSetBeamBSave; // The process list, stored as a vector of processes. vector processes; // Store info on the selected process. int idProc; double weightProc, scaleProc, alphaQEDProc, alphaQCDProc; // The particle list, stored as a vector of particles. vector particles; // Info on initiators and optionally on parton density values of event. bool pdfIsSetSave; int id1Save, id2Save, id1pdfSave, id2pdfSave; double x1Save, x2Save, x1pdfSave, x2pdfSave, scalePDFSave, pdf1Save, pdf2Save; // File to which to write Les Houches Event File information. string fileName; fstream osLHEF; char dateNow[12]; char timeNow[9]; }; //========================================================================== // A derived class with information read from a Les Houches Event File. class LHAupLHEF : public LHAup { public: // Constructor. LHAupLHEF(const char* fileIn, const char* headerIn = NULL, bool readHeaders = false); // Destructor. ~LHAupLHEF(); // Helper routine to correctly close files void closeAllFiles() { // Close header file if separate, and close main file if (isHead != is) closeFile(isHead, ifsHead); closeFile(is, ifs); } // Want to use new file with events, but without reinitialization. void newEventFile(const char* fileIn) { // Close files and then open new file closeAllFiles(); is = openFile(fileIn, ifs); // Set isHead to is to keep expected behaviour in // fileFound() and closeAllFiles() isHead = is; } // Confirm that file was found and opened as expected. bool fileFound() { return (isHead->good() && is->good()); } // Routine for doing the job of reading and setting initialization info. bool setInit() {return setInitLHEF(*isHead, readHeaders);} // Routine for doing the job of reading and setting info on next event. bool setEvent(int = 0, double mRecalculate = -1.) { if (!setNewEventLHEF(*is, mRecalculate)) return false; return setOldEventLHEF(); } // Skip ahead a number of events, which are not considered further. bool skipEvent(int nSkip) {for (int iSkip = 0; iSkip < nSkip; ++iSkip) if (!setNewEventLHEF(*is)) return false; return true;} private: // File from which to read (or a stringstream). // Optionally also a file from which to read the LHEF header. ifstream ifs, ifsHead; istream *is, *isHead; // Flag to read headers or not bool readHeaders; }; //========================================================================== // A derived class with information read from PYTHIA 8 itself, for output. class LHAupFromPYTHIA8 : public LHAup { public: // Constructor. LHAupFromPYTHIA8(Event* processPtrIn, Info* infoPtrIn) { processPtr = processPtrIn; infoPtr = infoPtrIn;} // Destructor. ~LHAupFromPYTHIA8() {} // Routine for doing the job of reading and setting initialization info. bool setInit(); // Routine for doing the job of reading and setting info on next event. bool setEvent(int = 0, double = -1.); // Update cross-section information at the end of the run. bool updateSigma(); private: // Pointers to process event record and further information. Event* processPtr; Info* infoPtr; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_LesHouches_H pythia8-8.1.80.orig/include/Pythia8/SusyLesHouches.h0000644000175000017500000007124212217346232020411 0ustar sunsun// SusyLesHouches.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // Main authors of this file: N. Desai, P. Skands // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for SUSY Les Houches Accord Interface // Is independent of the rest of the PYTHIA implementation and thus could // be re-used stand-alone or merged into other applications, subject to // the MCnet Guidelines mentioned above. #ifndef SLHA_H #define SLHA_H // Stdlib header files for string and character manipulation. #include #include // Stdlib header files for containers. #include #include // Stdlib header files for input/output. #include #include #include #include // Stdlib header files for mathematics. #include #include // Stdlib namespace using namespace std; //************************* SLHA AUX CLASSES *****************************// namespace Pythia8 { //class LHblock: the generic SLHA block (see below for matrices) //Explicit typing required, e.g. block minpar; template class LHblock { public: //Constructor. LHblock() : idnow(0) {} ; //Does block exist? bool exists() { return int(entry.size()) == 0 ? false : true ; }; //Clear block void clear() { entry.clear(); }; //set: set block entry values. //Possible return values from set: // 0: normal return. Entry did not previously exist and has been created. // 1: normal return. Entry did previously exist and has been overwritten. //-1: failure. int set(int iIn,T valIn) { int alreadyexisting=exists(iIn)?1:0; entry[iIn]=valIn; return alreadyexisting; }; // Read index and value from SLHA data line int set(istringstream& linestream, bool indexed=true) { i = 0; if (indexed) linestream >> i >> val; else linestream >> val; return linestream ? set(i,val) : -1; }; // With i already given, read value from remaining SLHA data line int set(int iIn,istringstream& linestream) { linestream >> val; return linestream ? set(iIn,val) : -1; }; // Shorthand for entry[0]. Used e.g. for block ALPHA. void set(T valIn) { entry[0]=valIn; }; // Does entry i already exist in this block? bool exists(int iIn) {return entry.find(iIn) != entry.end() ? true : false;}; // Indexing with (). Output only. T operator()() { if (exists(0)) {return entry[0];} else {T dummy(0); return dummy;}; }; T operator()(int iIn) { if (exists(iIn)) {return entry[iIn];} else {T dummy(0); return dummy;}; }; // Size of map int size() {return int(entry.size());}; // First and next key code int first() { idnow = entry.begin()->first; return idnow; }; int next() { typename map::iterator itnow; itnow = ++entry.find(idnow); if ( itnow == entry.end() ) itnow=entry.begin(); return idnow = itnow->first; }; // Simple print utility void print() { bool finished=false; int ibegin=first(); i=ibegin; while (!finished) { cout << " "<< i << " " << entry[i] < entry; private: int idnow; double qDRbar; //Auxiliary vars int i; T val; }; // Derived class for generic blocks containing vectors of strings. class LHgenericBlock : public LHblock { public: //Constructor. LHgenericBlock() { } ; // Read index and value from SLHA data line int set(string lineIn) { entry[entry.size()] = lineIn; return 0; }; }; // class LHmatrixBlock: the generic SLHA matrix // Explicit sizing required, e.g.LHmatrixBlock<4> nmix; template class LHmatrixBlock { public: //Constructor. Set uninitialized and explicitly zero. LHmatrixBlock() { initialized=false; for (i=1;i<=size;i++) { for (j=1;j<=size;j++) { entry[i][j]=0.0; }; }; }; // Assignment LHmatrixBlock& operator=(const LHmatrixBlock& m) { if (this != &m) { for (i=0;i0 && jIn>0 && iIn<=size && jIn<=size) { entry[iIn][jIn]=valIn; initialized=true; return 0; } else { return -1; }; }; // Set entry from linestream (used during file read) int set(istringstream& linestream) { linestream >> i >> j >> val; return linestream ? set(i,j,val) : -1; }; // () Overloading: Get entry double operator()(int iIn, int jIn) const { return (iIn <= size && jIn <= size && iIn > 0 && jIn > 0) ? entry[iIn][jIn] : 0.0; }; // Set and get scale for DRbar running LHblocks. void setq(double qIn) { qDRbar=qIn; } double q() { return qDRbar; } // Simple print utility, to be elaborated on. void print() { for (i=1;i<=size;i++) { cout << " "< rvlam; template class LHtensor3Block { public: //Constructor. Set uninitialized and explicitly zero. LHtensor3Block() { initialized=false; for (i=1;i<=size;i++) { for (j=1;j<=size;j++) { for (k=1;k<=size;k++) { entry[i][j][k]=0.0; }; }; }; }; // Assignment LHtensor3Block& operator=(const LHtensor3Block& m) { if (this != &m) { for (i=0;i0 && jIn>0 && kIn>0 && iIn<=size && jIn<=size && kIn<=size) { entry[iIn][jIn][kIn]=valIn; initialized=true; return 0; } else { return -1; }; }; // Set entry from linestream (used during file read) int set(istringstream& linestream) { linestream >> i >> j >> k >> val; return linestream ? set(i,j,k,val) : -1; }; // () Overloading: Get entry double operator()(int iIn, int jIn, int kIn) const { return (iIn <= size && jIn <= size && kIn <= size && iIn > 0 && jIn > 0 && kIn > 0) ? entry[iIn][jIn][kIn] : 0.0; }; // Set and get scale for DRbar running LHblocks. void setq(double qIn) { qDRbar=qIn; } double q() { return qDRbar; } // Simple print utility, to be elaborated on. void print() { for (i=1;i<=size;i++) { for (j=1;j<=size;j++) { cout << " "< idDaIn, string cIn="") { setChannel(bratIn,nDaIn,idDaIn,cIn); } // Functions to set decay channel information void setChannel(double bratIn, int nDaIn, vector idDaIn, string cIn="") { brat = bratIn; for (int i=0; i<=nDaIn; i++) { if (i < int(idDaIn.size())) idDa.push_back(idDaIn[i]); comment = cIn; } } void setBrat(double bratIn) {brat=bratIn;} void setIdDa(vector idDaIn) {idDa = idDaIn;} // Functions to get decay channel information double getBrat() {return brat;} int getNDa() {return int(idDa.size());} vector getIdDa() {return idDa;} string getComment() {return comment;} private: double brat; vector idDa; string comment; }; class LHdecayTable { public: LHdecayTable() : id(0), width(0.0) {}; LHdecayTable(int idIn) : id(idIn), width(0.0) {}; LHdecayTable(int idIn, double widthIn) : id(idIn), width(widthIn) {}; // Functions to get PDG code (id) and width int getId() {return id;} double getWidth() {return width;} // Functions to set PDG code (id) and width void setId(int idIn) {id = idIn;} void setWidth(double widthIn) {width=widthIn;} // Function to reset size and width (width -> 0 by default) void reset(double widthIn=0.0) {table.resize(0); width=widthIn;} // Function to add another decay channel void addChannel(LHdecayChannel channelIn) {table.push_back(channelIn);} void addChannel(double bratIn, int nDaIn, vector idDaIn, string cIn="") { LHdecayChannel newChannel(bratIn, nDaIn, idDaIn, cIn); table.push_back(newChannel); } // Function to return number of decay channels int size() {return int(table.size());} // Function to return a branching ratio double getBrat(int iChannel) { if (iChannel >= 0 && iChannel < int(table.size())) { return table[iChannel].getBrat(); } else { return 0.0; } } // Function to return daughter PDG codes vector getIdDa(int iChannel) { if (iChannel >= 0 && iChannel < int(table.size())) { return table[iChannel].getIdDa(); } else { vector dum; return dum; } } // Function to return a decay channel LHdecayChannel getChannel(int iChannel) { if (iChannel >= 0 && iChannel < int(table.size())) { return table[iChannel]; } else { LHdecayChannel dum; return dum; } } private: int id; double width; vector table; }; //========================================================================== class SusyLesHouches { public: //Constructor, with and without filename. SusyLesHouches(int verboseIn=1) : verbose(verboseIn), headerPrinted(false), footerPrinted(false), filePrinted(false), slhaRead(false), lhefRead(false), lhefSlha(false), useDecay(true) {}; SusyLesHouches(string filename, int verboseIn=1) : verbose(verboseIn), headerPrinted(false), footerPrinted(false), filePrinted(false), slhaRead(true), lhefRead(false), lhefSlha(false), useDecay(true) {readFile(filename);}; //***************************** SLHA FILE I/O *****************************// // Read and write SLHA files int readFile(string slhaFileIn="slha.spc",int verboseIn=1, bool useDecayIn=true); //int writeFile(string filename): write SLHA file on filename //Output utilities void printHeader(); // print Header void printFooter(); // print Footer void printSpectrum(int ifail=0); // print Spectrum // Check spectrum and decays int checkSpectrum(); int checkDecays(); // File Name (can be either SLHA or LHEF) string slhaFile; // Class for SLHA data entry class Entry { public: //Constructor. Entry() : isIntP(false), isDoubleP(false), isStringP(false), n(0), d(0.0), s(""), commentP("") {} // Generic functions to inquire whether an int, double, or string bool isInt(){return isIntP;} bool isDouble(){return isDoubleP;} bool isString(){return isStringP;} // = Overloading: Set entry to int, double, or string Entry& operator=(double& val) { d=val;isIntP=false;isDoubleP=true;isStringP=false; return *this; }; Entry& operator=(int& val) { n=val;isIntP=true;isDoubleP=false;isStringP=false; return *this; }; Entry& operator=(string& val) { s=val;isIntP=false;isDoubleP=false;isStringP=true; return *this; }; // Set and Get comment void setComment(string comment) {commentP=comment;} void getComment(string comment) {comment=commentP;} // Generic functions to get value bool get(int& val) {val=n; return isIntP;} bool get(double& val) {val=d; return isDoubleP;} bool get(string& val) {val=s; return isStringP;} private: bool isIntP, isDoubleP, isStringP; int n; double d; string s; string commentP; }; //*************************** THE SLHA1 BLOCKS ***************************// //Blocks for model definition: LHblock modsel; LHblock modsel21; LHblock modsel12; LHblock minpar; LHblock extpar; LHblock sminputs; //Blocks for RGE program specific output LHblock spinfo; LHblock spinfo3; LHblock spinfo4; //Blocks for DCY program specific output LHblock dcinfo; LHblock dcinfo3; LHblock dcinfo4; //Blocks for mass and coupling spectrum LHblock mass; LHmatrixBlock<4> nmix; LHmatrixBlock<2> umix; LHmatrixBlock<2> vmix; LHmatrixBlock<2> stopmix; LHmatrixBlock<2> sbotmix; LHmatrixBlock<2> staumix; LHblock alpha; LHblock hmix; LHblock gauge; LHblock msoft; LHmatrixBlock<3> au; LHmatrixBlock<3> ad; LHmatrixBlock<3> ae; LHmatrixBlock<3> yu; LHmatrixBlock<3> yd; LHmatrixBlock<3> ye; //************************ THE SLHA1 DECAY TABLES ************************// vector decays; map decayIndices; //********************* THE BSM-SLHA QNUMBERS BLOCKS *********************// vector< LHblock > qnumbers; // Zero'th entry is PDG code vector< string > qnumbersName; vector< string > qnumbersAntiName; //*************************** THE SLHA2 BLOCKS ***************************// //Additions to SLHA1 LHblock qextpar; //FLV Input LHblock vckmin; // The input CKM Wolfenstein parms. LHblock upmnsin; // The input PMNS PDG parms. LHmatrixBlock<3> msq2in; // The input upper off-diagonal msq2 LHmatrixBlock<3> msu2in; // The input upper off-diagonal msu2 LHmatrixBlock<3> msd2in; // The input upper off-diagonal msd2 LHmatrixBlock<3> msl2in; // The input upper off-diagonal msl2 LHmatrixBlock<3> mse2in; // The input upper off-diagonal mse2 LHmatrixBlock<3> tuin; // The input upper off-diagonal TU LHmatrixBlock<3> tdin; // The input upper off-diagonal TD LHmatrixBlock<3> tein; // The input upper off-diagonal TE //FLV Output LHmatrixBlock<3> vckm; // The output DRbar running Re{VCKM} at Q LHmatrixBlock<3> upmns; // The output DRbar running Re{UPMNS} at Q LHmatrixBlock<3> msq2; // The output DRbar running msq2 at Q LHmatrixBlock<3> msu2; // The output DRbar running msu2 at Q LHmatrixBlock<3> msd2; // The output DRbar running msd2 at Q LHmatrixBlock<3> msl2; // The output DRbar running msl2 at Q LHmatrixBlock<3> mse2; // The output DRbar running mse2 at Q LHmatrixBlock<3> tu; // The output DRbar running TU at Q LHmatrixBlock<3> td; // The output DRbar running TD at Q LHmatrixBlock<3> te; // The output DRbar running TE at Q LHmatrixBlock<6> usqmix; // The Re{} up squark mixing matrix LHmatrixBlock<6> dsqmix; // The Re{} down squark mixing matrix LHmatrixBlock<6> selmix; // The Re{} selectron mixing matrix LHmatrixBlock<3> snumix; // The Re{} sneutrino mixing matrix LHmatrixBlock<3> snsmix; // The scalar sneutrino mixing matrix LHmatrixBlock<3> snamix; // The pseudoscalar neutrino mixing matrix //RPV Input LHtensor3Block<3> rvlamllein; // The input LNV lambda couplings LHtensor3Block<3> rvlamlqdin; // The input LNV lambda' couplings LHtensor3Block<3> rvlamuddin; // The input BNV lambda'' couplings LHtensor3Block<3> rvtllein; // The input LNV T couplings LHtensor3Block<3> rvtlqdin; // The input LNV T' couplings LHtensor3Block<3> rvtuddin; // The input BNV T'' couplings LHblock rvkappain; // The input LNV kappa couplings LHblock rvdin; // The input LNV D terms LHblock rvm2lh1in; // The input LNV m2LH1 couplings LHblock rvsnvevin; // The input LNV sneutrino vevs //RPV Output LHtensor3Block<3> rvlamlle; // The output LNV lambda couplings LHtensor3Block<3> rvlamlqd; // The output LNV lambda' couplings LHtensor3Block<3> rvlamudd; // The output BNV lambda'' couplings LHtensor3Block<3> rvtlle; // The output LNV T couplings LHtensor3Block<3> rvtlqd; // The output LNV T' couplings LHtensor3Block<3> rvtudd; // The output BNV T'' couplings LHblock rvkappa; // The output LNV kappa couplings LHblock rvd; // The output LNV D terms LHblock rvm2lh1; // The output LNV m2LH1 couplings LHblock rvsnvev; // The output LNV sneutrino vevs LHmatrixBlock<7> rvnmix; // The RPV neutralino mixing matrix LHmatrixBlock<5> rvumix; // The RPV chargino L mixing matrix LHmatrixBlock<5> rvvmix; // The RPV chargino R mixing matrix LHmatrixBlock<5> rvhmix; // The RPV neutral scalar mixing matrix LHmatrixBlock<5> rvamix; // The RPV neutral pseudoscalar mixing matrix LHmatrixBlock<8> rvlmix; // The RPV charged fermion mixing matrix //CPV Input LHblock imminpar; LHblock imextpar; //CPV Output LHmatrixBlock<4> cvhmix; // The CPV Higgs mixing matrix LHmatrixBlock<4> imcvhmix; // Optional: imaginary components LHmatrixBlock<3> imau,imad,imae; // Im{} of AU, AD, AE LHblock imhmix; LHblock immsoft; //CPV + FLV Input LHmatrixBlock<3> immsq2in; // The Im{} input upper off-diagonal msq2 LHmatrixBlock<3> immsu2in; // The Im{} input upper off-diagonal msu2 LHmatrixBlock<3> immsd2in; // The Im{} input upper off-diagonal msd2 LHmatrixBlock<3> immsl2in; // The Im{} input upper off-diagonal msl2 LHmatrixBlock<3> immse2in; // The Im{} input upper off-diagonal mse2 LHmatrixBlock<3> imtuin,imtdin,imtein; // The Im{} input upper off-diagonal T //CPV + FLV Output LHmatrixBlock<3> imvckm; // The output DRbar running Im{VCKM} at Q LHmatrixBlock<3> imupmns; // The output DRbar running Im{UPMNS} at Q LHmatrixBlock<3> immsq2; // The output DRbar running msq2 at Q LHmatrixBlock<3> immsu2; // The output DRbar running msu2 at Q LHmatrixBlock<3> immsd2; // The output DRbar running msd2 at Q LHmatrixBlock<3> immsl2; // The output DRbar running msl2 at Q LHmatrixBlock<3> immse2; // The output DRbar running mse2 at Q LHmatrixBlock<3> imtu,imtd,imte; // Im{} of TU, TD, TE LHmatrixBlock<6> imusqmix;// The Im{} up squark mixing matrix LHmatrixBlock<6> imdsqmix; // The Im{} down squark mixing matrix LHmatrixBlock<6> imselmix; // The Im{} selectron mixing matrix LHmatrixBlock<3> imsnumix; // The Im{} sneutrino mixing matrix LHmatrixBlock<4> imnmix; // The Im{} neutralino mixing matrix LHmatrixBlock<4> imumix; // The Im{} chargino L mixing matrix LHmatrixBlock<4> imvmix; // The Im{} chargino R mixing matrix //NMSSM Input // All input is in EXTPAR //NMSSM Output LHblock nmssmrun; // The LHblock of NMSSM running parameters LHmatrixBlock<3> nmhmix; // The NMSSM scalar Higgs mixing LHmatrixBlock<3> nmamix; // The NMSSM pseudoscalar Higgs mixing LHmatrixBlock<5> nmnmix; // The NMSSM neutralino mixing LHmatrixBlock<5> imnmnmix; // Im{} (for future use) //*************************** SET BLOCK VALUE ****************************// template int set(string,T); template int set(string,int,T); template int set(string,int,int,T); template int set(string,int,int,int,T); //********************* GENERIC/USER-DEFINED BLOCKS **********************// // bool getEntry(name, indices, value) // = true if LHblock and entry exists (value returned in value, // typecast by user in call) // = false otherwise map genericBlocks; template bool getEntry(string, T&); template bool getEntry(string, int, T&); template bool getEntry(string, int, int, T&); template bool getEntry(string, int, int, int, T&); template bool getEntry(string, vector, T&); // Output of messages from SLHA interface void message(int, string,string ,int line=0); //***************************** SLHA PRIVATE *****************************// private: //SLHA I/O int verbose; bool headerPrinted, footerPrinted, filePrinted; bool slhaRead, lhefRead, lhefSlha, useDecay; }; //-------------------------------------------------------------------------- // utilities to set generic blocks template int SusyLesHouches::set(string blockName, T val) { // Make sure everything is interpreted as lower case (for safety) for (int iC=0; iC int SusyLesHouches::set(string blockName, int indx, T val) { // Make sure everything is interpreted as lower case (for safety) for (int iC=0; iC int SusyLesHouches::set(string blockName, int indx, int jndx, T val) { // Make sure everything is interpreted as lower case (for safety) for (int iC=0; iC int SusyLesHouches::set(string blockName, int indx, int jndx, int kndx, T val) { // Make sure everything is interpreted as lower case (for safety) for (int iC=0; iC bool SusyLesHouches::getEntry(string blockName, T& val) { // Make sure everything is interpret as lower case (for safety) for (int iC=0; iC= 2) { message(1,"getEntry","attempting to extract un-indexed entry " "from multi-entry block "+blockName); return false; } // Attempt to extract value as class T LHgenericBlock block = genericBlocks[blockName]; istringstream linestream(block(0)); linestream >> val; if ( !linestream ) { message(1,"getEntry","problem extracting un-indexed entry " "from block "+blockName); return false; } // If made it all the way here, value was successfully extracted. // Return true. return true; } template bool SusyLesHouches::getEntry(string blockName, int indx, T& val) { // Make sure everything is interpret as lower case (for safety) for (int iC=0; iC> indxNow >> valNow; // If index found and value was readable, return true if (linestream && indxNow == indx) { val = valNow; return true; } } // If index not found or unreadable, return false message(1,"getEntry","problem extracting indexed entry from block " +blockName); return false; } template bool SusyLesHouches::getEntry(string blockName, int indx, int jndx, T& val) { // Make sure everything is interpret as lower case (for safety) for (int iC=0; iC> indxNow >> jndxNow >> valNow; // If index found and value was readable, return true if (linestream && indxNow == indx && jndxNow == jndx) { val = valNow; return true; } } // If index not found or unreadable, return false message(1,"getEntry","problem extracting matrix-indexed entry from block " +blockName); return false; } template bool SusyLesHouches::getEntry(string blockName, int indx, int jndx, int kndx, T& val) { // Make sure everything is interpret as lower case (for safety) for (int iC=0; iC> indxNow >> jndxNow >> kndxNow >> valNow; // If index found and value was readable, return true if (linestream && indxNow == indx && jndxNow == jndx && kndxNow == kndx) { val = valNow; return true; } } // If index not found or unreadable, return false message(1,"getEntry","problem extracting tensor-indexed entry from block " +blockName); return false; } } #endif pythia8-8.1.80.orig/include/Pythia8/SusyCouplings.h0000644000175000017500000001211312217346232020302 0ustar sunsun// SusyCouplings.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // Main authors of this file: N. Desai, P. Skands // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for setup of common SUSY couplings. #ifndef Pythia8_SusyCouplings_H #define Pythia8_SusyCouplings_H #include "Pythia8/PythiaComplex.h" #include "Pythia8/Settings.h" #include "Pythia8/StandardModel.h" #include "Pythia8/SusyLesHouches.h" namespace Pythia8 { class ParticleData; //========================================================================== // CoupSUSY // Auxiliary class to compute and store various SM and SUSY couplings. class CoupSUSY : public Couplings{ public: // Constructor CoupSUSY() {isInit=false; isNMSSM = false; isSUSY=true;} // Initialize void initSUSY(SusyLesHouches* slhaPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn); // Status flag. Flag for NMSSM. bool isInit, isNMSSM; // Z and W pole masses and widths double mWpole, wWpole, mZpole, wZpole; // Running masses and weak mixing angle // (default to pole values if no running available) double mW, mZ, sin2W, sinW, cosW; // Tanbeta double tanb, cosb, sinb; //Higgs-sector parameters double muHiggs, alphaHiggs, mAHiggs; // ~qq~g couplings complex LsddG[7][4], RsddG[7][4]; complex LsuuG[7][4], RsuuG[7][4]; // Assume generation index for Squark. Translate if PDG code instead. complex getLsqqG(int iGenSq, int idQ) {if (abs(iGenSq) > 1000000) iGenSq = 3*(abs(iGenSq)/2000000) + (abs(iGenSq)%10+1)/2; return (abs(idQ)%2 == 0) ? LsuuG[iGenSq][abs(idQ)/2] : LsddG[iGenSq][(abs(idQ)+1)/2] ;} complex getRsqqG(int iGenSq, int idQ) {if (abs(iGenSq) > 1000000) iGenSq = 3*(abs(iGenSq)/2000000) + (abs(iGenSq)%10+1)/2; return (abs(idQ)%2 == 0) ? RsuuG[iGenSq][abs(idQ)/2] : RsddG[iGenSq][(abs(idQ)+1)/2] ;} // ~chi0~chi0Z couplings complex OLpp[6][6], ORpp[6][6]; // ~chi+~chi-Z couplings complex OLp[3][3], ORp[3][3]; // ~chi0~chi+W couplings complex OL[6][3], OR[6][3]; // qqZ couplings double LqqZ[7], RqqZ[7]; // ~q~qZ couplings complex LsdsdZ[7][7], RsdsdZ[7][7]; complex LsusuZ[7][7], RsusuZ[7][7]; complex getLsqsqZ(int idSq1, int idSq2) { if (abs(idSq1)%2 != abs(idSq2)%2) return complex(0.0,0.0); int iGen1 = 3*(abs(idSq1)/2000000) + (abs(idSq1)%10+1)/2; int iGen2 = 3*(abs(idSq2)/2000000) + (abs(idSq2)%10+1)/2; return (abs(idSq1)%2 == 0) ? LsusuZ[iGen1][iGen2] : LsdsdZ[iGen1][iGen2];} complex getRsqsqZ(int idSq1, int idSq2) { if (abs(idSq1)%2 != abs(idSq2)%2) return complex(0.0,0.0); int iGen1 = 3*(abs(idSq1)/2000000) + (abs(idSq1)%10+1)/2; int iGen2 = 3*(abs(idSq2)/2000000) + (abs(idSq2)%10+1)/2; return (abs(idSq1)%2 == 0) ? RsusuZ[iGen1][iGen2] : RsdsdZ[iGen1][iGen2];} // udW couplings complex LudW[4][4], RudW[4][4]; // ~u~dW couplings complex LsusdW[7][7], RsusdW[7][7]; // ~qq~chi0 couplings complex LsddX[7][4][6], RsddX[7][4][6]; complex LsuuX[7][4][6], RsuuX[7][4][6]; complex getLsqqX(int iSq, int idQ, int iNeut) {return (abs(idQ)%2 == 0) ? LsuuX[iSq][abs(idQ)/2][iNeut] : LsddX[iSq][(abs(idQ)+1)/2][iNeut] ;} complex getRsqqX(int iSq, int idQ, int iNeut) {return (abs(idQ)%2 == 0) ? RsuuX[iSq][abs(idQ)/2][iNeut] : RsddX[iSq][(abs(idQ)+1)/2][iNeut] ;} // ~du~chi+ couplings complex LsduX[7][4][3], RsduX[7][4][3]; // ~ud~chi+ couplings complex LsudX[7][4][3], RsudX[7][4][3]; //llZ couplings double LllZ[7], RllZ[7]; //lvW couplings complex LlvW[4][4], RlvW[4][4]; // ~l~lZ couplings complex LslslZ[7][7],RslslZ[7][7]; complex LsvsvZ[7][7],RsvsvZ[7][7]; // ~l~vW couplings complex LslsvW[7][7], RslsvW[7][7]; // ~ll~chi0 couplings complex LsvvX[7][4][6], RsvvX[7][4][6]; complex LsllX[7][4][6], RsllX[7][4][6]; // ~vl~chi+ couplings complex LsvlX[7][4][3], RsvlX[7][4][3]; // ~lv~chi+ couplings complex LslvX[7][4][3], RslvX[7][4][3]; // RPV couplings double rvLLE[4][4][4], rvLQD[4][4][4], rvUDD[4][4][4]; // Flags for RPV couplings bool isLLE, isLQD, isUDD; //Squark mixing matrix: needed for RPV complex Rusq[7][7], Rdsq[7][7]; // Return neutralino, chargino, sup, sdown and slepton flavour codes. int idNeut(int idChi); int idChar(int idChi); int idSup(int iSup); int idSdown(int iSdown); int idSlep(int iSlep); //Reverse lookup for neutralinos and charginos int typeNeut(int idPDG); int typeChar(int idPDG); // Return a particle name, given the PDG code. string getName(int pdgCode); // Pointer to SLHA instance // Used in SusyResonanceWidths for checking if decay table exists SusyLesHouches* slhaPtr; private: // Debug flag static const bool DBSUSY; // Pointer to the settings database. Settings* settingsPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SusyCouplings_H pythia8-8.1.80.orig/include/Pythia8/SigmaGeneric.h0000644000175000017500000001273612217346231020022 0ustar sunsun// SigmaGeneric.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Johan Bijnens,Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for various generic production processes, to be used as // building blocks for some BSM processes. // Currently represented by QCD pair production of colour triplet objects, // with spin either 0, 1/2 or 1. #ifndef Pythia8_SigmaGeneric_H #define Pythia8_SigmaGeneric_H #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // A derived class for g g -> qG qGbar (generic quark of spin 0, 1/2 or 1). class Sigma2gg2qGqGbar : public Sigma2Process { public: // Constructor. Sigma2gg2qGqGbar(int idIn, int codeIn, int spinIn, string nameIn = "g g -> qG qGbar") : idNew(idIn), codeSave(codeIn), spinSave(spinIn), nameSave(nameIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "gg";} virtual int id3Mass() const {return idNew;} virtual int id4Mass() const {return idNew;} private: // Values stored for process type and colour flow selection. int idNew, codeSave, spinSave, nCHV; string nameSave; bool hasKappa; double openFracPair, sigma, sigTS, sigUS, sigSum, kappam1; }; //========================================================================== // A derived class for q qbar -> qG qGbar (generic quark of spin 0, 1/2 or 1). class Sigma2qqbar2qGqGbar : public Sigma2Process { public: // Constructor. Sigma2qqbar2qGqGbar(int idIn, int codeIn, int spinIn, string nameIn = "q qbar -> qG qGbar") : idNew(idIn), codeSave(codeIn), spinSave(spinIn), nameSave(nameIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "qqbarSame";} virtual int id3Mass() const {return idNew;} virtual int id4Mass() const {return idNew;} private: // Values stored for process type and colour flow selection. int idNew, codeSave, spinSave, nCHV; string nameSave; double openFracPair, sigma, sigSum, kappa; }; //========================================================================== // A derived class for f fbar -> fG fGbar (generic spin 0, 1/2 or 1 particle) // via gamma^*/Z^* s-channel exchange. Still under development!! ?? class Sigma2ffbar2fGfGbar : public Sigma2Process { public: // Constructor. Sigma2ffbar2fGfGbar(int idIn, int codeIn, int spinIn, string nameIn = "q qbar -> qG qGbar") : idNew(idIn), codeSave(codeIn), spinSave(spinIn), nameSave(nameIn) {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Info on the subprocess. virtual string name() const {return nameSave;} virtual int code() const {return codeSave;} virtual string inFlux() const {return "ffbarSame";} virtual int id3Mass() const {return idNew;} virtual int id4Mass() const {return idNew;} private: // Values stored for process type and colour flow selection. int idNew, codeSave, spinSave, nCHV; string nameSave; bool hasColour; double eQHV2, openFracPair, sigma0, sigSum, kappa, colFac; }; //========================================================================== // A derived class for f fbar -> Zv, where Zv couples both to the SM and // to a hidden sector. Primitive coupling structure. class Sigma1ffbar2Zv : public Sigma1Process { public: // Constructor. Sigma1ffbar2Zv() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat) for given inflavours. virtual double sigmaHat(); // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "f fbar -> Zv";} virtual int code() const {return 4941;} virtual string inFlux() const {return "ffbarSame";} virtual int resonanceA() const {return 4900023;} private: // Store flavour-specific process information and standard prefactor. int idZv; double mRes, GammaRes, m2Res, GamMRat, sigOut; // Pointer to properties of Zv, to access decay width. ParticleDataEntry* particlePtr; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_SigmaGeneric_H pythia8-8.1.80.orig/include/Pythia8/BeamParticle.h0000644000175000017500000002615012217346226020014 0ustar sunsun// BeamParticle.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for information on incoming beams. // ResolvedParton: an initiator or remnant in beam. // BeamParticle: contains partons, parton densities, etc. #ifndef Pythia8_BeamParticle_H #define Pythia8_BeamParticle_H #include "Pythia8/Basics.h" #include "Pythia8/Event.h" #include "Pythia8/FragmentationFlavZpT.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PartonDistributions.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" namespace Pythia8 { //========================================================================== // This class holds info on a parton resolved inside the incoming beam, // i.e. either an initiator (part of a hard or a multiparton interaction) // or a remnant (part of the beam remnant treatment). // The companion code is -1 from onset and for g, is -2 for an unmatched // sea quark, is >= 0 for a matched sea quark, with the number giving the // companion position, and is -3 for a valence quark. // Rescattering partons properly do not belong here, but bookkeeping is // simpler with them, so they are stored with companion code -10. class ResolvedParton { public: // Constructor. ResolvedParton( int iPosIn = 0, int idIn = 0, double xIn = 0., int companionIn = -1) : iPosRes(iPosIn), idRes(idIn), xRes(xIn), companionRes(companionIn), xqCompRes(0.), mRes(0.), factorRes(1.), colRes(0), acolRes(0) { } // Set info on initiator or remnant parton. void iPos( int iPosIn) {iPosRes = iPosIn;} void id( int idIn) {idRes = idIn;} void x( double xIn) {xRes = xIn;} void update( int iPosIn, int idIn, double xIn) {iPosRes = iPosIn; idRes = idIn; xRes = xIn;} void companion( int companionIn) {companionRes = companionIn;} void xqCompanion( double xqCompIn) {xqCompRes = xqCompIn;} void p(Vec4 pIn) {pRes = pIn;} void px(double pxIn) {pRes.px(pxIn);} void py(double pyIn) {pRes.py(pyIn);} void pz(double pzIn) {pRes.pz(pzIn);} void e(double eIn) {pRes.e(eIn);} void m(double mIn) {mRes = mIn;} void col(int colIn) {colRes = colIn;} void acol(int acolIn) {acolRes = acolIn;} void cols(int colIn = 0,int acolIn = 0) {colRes = colIn; acolRes = acolIn;} void scalePT( double factorIn) {pRes.px(factorIn * pRes.px()); pRes.py(factorIn * pRes.py()); factorRes *= factorIn;} void scaleX( double factorIn) {xRes *= factorIn;} // Get info on initiator or remnant parton. int iPos() const {return iPosRes;} int id() const {return idRes;} double x() const {return xRes;} int companion() const {return companionRes;} bool isValence() const {return (companionRes == -3);} bool isUnmatched() const {return (companionRes == -2);} bool isCompanion() const {return (companionRes >= 0);} bool isFromBeam() const {return (companionRes > -10);} double xqCompanion() const {return xqCompRes;} Vec4 p() const {return pRes;} double px() const {return pRes.px();} double py() const {return pRes.py();} double pz() const {return pRes.pz();} double e() const {return pRes.e();} double m() const {return mRes;} double pT() const {return pRes.pT();} double mT2() const {return (mRes >= 0.) ? mRes*mRes + pRes.pT2() : - mRes*mRes + pRes.pT2();} double pPos() const {return pRes.e() + pRes.pz();} double pNeg() const {return pRes.e() - pRes.pz();} int col() const {return colRes;} int acol() const {return acolRes;} double pTfactor() const {return factorRes;} private: // Properties of a resolved parton. int iPosRes, idRes; double xRes; // Companion code and distribution value, if any. int companionRes; double xqCompRes; // Four-momentum and mass; for remnant kinematics construction. Vec4 pRes; double mRes, factorRes; // Colour codes. int colRes, acolRes; }; //========================================================================== // This class holds info on a beam particle in the evolution of // initial-state radiation and multiparton interactions. class BeamParticle { public: // Constructor. BeamParticle() : nInit(0) {resolved.resize(0); Q2ValFracSav = -1.;} // Initialize data on a beam particle and save pointers. void init( int idIn, double pzIn, double eIn, double mIn, Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, PDF* pdfInPtr, PDF* pdfHardInPtr, bool isUnresolvedIn, StringFlav* flavSelPtrIn); // Initialize only the two pdf pointers. void initPDFPtr(PDF* pdfInPtr, PDF* pdfHardInPtr) { pdfBeamPtr = pdfInPtr; pdfHardBeamPtr = pdfHardInPtr; } // For mesons like pi0 valence content varies from event to event. void newValenceContent(); // Set new pZ and E, but keep the rest the same. void newPzE( double pzIn, double eIn) {pBeam = Vec4( 0., 0., pzIn, eIn);} // Member functions for output. int id() const {return idBeam;} Vec4 p() const {return pBeam;} double px() const {return pBeam.px();} double py() const {return pBeam.py();} double pz() const {return pBeam.pz();} double e() const {return pBeam.e();} double m() const {return mBeam;} bool isLepton() const {return isLeptonBeam;} bool isUnresolved() const {return isUnresolvedBeam;} // As hadrons here we only count those we know how to handle remnants for. bool isHadron() const {return isHadronBeam;} bool isMeson() const {return isMesonBeam;} bool isBaryon() const {return isBaryonBeam;} // Maximum x remaining after previous MPI and ISR, plus safety margin. double xMax(int iSkip = -1); // Special hard-process parton distributions (can agree with standard ones). double xfHard(int idIn, double x, double Q2) {return pdfHardBeamPtr->xf(idIn, x, Q2);} // Standard parton distributions. double xf(int idIn, double x, double Q2) {return pdfBeamPtr->xf(idIn, x, Q2);} // Ditto, split into valence and sea parts (where gluon counts as sea). double xfVal(int idIn, double x, double Q2) {return pdfBeamPtr->xfVal(idIn, x, Q2);} double xfSea(int idIn, double x, double Q2) {return pdfBeamPtr->xfSea(idIn, x, Q2);} // Rescaled parton distributions, as needed for MPI and ISR. // For ISR also allow split valence/sea, and only return relevant part. double xfMPI(int idIn, double x, double Q2) {return xfModified(-1, idIn, x, Q2);} double xfISR(int indexMPI, int idIn, double x, double Q2) {return xfModified( indexMPI, idIn, x, Q2);} // Decide whether chosen quark is valence, sea or companion. int pickValSeaComp(); // Initialize kind of incoming beam particle. void initBeamKind(); // Overload index operator to access a resolved parton from the list. ResolvedParton& operator[](int i) {return resolved[i];} const ResolvedParton& operator[](int i) const {return resolved[i];} // Total number of partons extracted from beam, and initiators only. int size() const {return resolved.size();} int sizeInit() const {return nInit;} // Clear list of resolved partons. void clear() {resolved.resize(0); nInit = 0;} // Add a resolved parton to list. int append( int iPos, int idIn, double x, int companion = -1) {resolved.push_back( ResolvedParton( iPos, idIn, x, companion) ); return resolved.size() - 1;} // Print extracted parton list; for debug mainly. void list(ostream& os = cout) const; // How many different flavours, and how many quarks of given flavour. int nValenceKinds() const {return nValKinds;} int nValence(int idIn) const {for (int i = 0; i < nValKinds; ++i) if (idIn == idVal[i]) return nVal[i]; return 0;} // Test whether a lepton is to be considered as unresolved. bool isUnresolvedLepton(); // Add extra remnant flavours to make valence and sea come out right. bool remnantFlavours(Event& event); // Correlate all initiators and remnants to make a colour singlet. bool remnantColours(Event& event, vector& colFrom, vector& colTo); // Pick unrescaled x of remnant parton (valence or sea). double xRemnant(int i); // Tell whether a junction has been resolved, and its junction colours. bool hasJunction() const {return hasJunctionBeam;} int junctionCol(int i) const {return junCol[i];} void junctionCol(int i, int col) {junCol[i] = col;} // For a diffractive system, decide whether to kick out gluon or quark. bool pickGluon(double mDiff); // Pick a valence quark at random, and provide the remaining flavour. int pickValence(); int pickRemnant() const {return idVal2;} // Share lightcone momentum between two remnants in a diffractive system. // At the same time generate a relative pT for the two. double zShare( double mDiff, double m1, double m2); double pxShare() const {return pxRel;} double pyShare() const {return pyRel;} private: // Constants: could only be changed in the code itself. static const double XMINUNRESOLVED; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointer to the random number generator. Rndm* rndmPtr; // Pointers to PDF sets. PDF* pdfBeamPtr; PDF* pdfHardBeamPtr; // Pointer to class for flavour generation. StringFlav* flavSelPtr; // Initialization data, normally only set once. bool allowJunction; int maxValQuark, companionPower; double valencePowerMeson, valencePowerUinP, valencePowerDinP, valenceDiqEnhance, pickQuarkNorm, pickQuarkPower, diffPrimKTwidth, diffLargeMassSuppress; // Basic properties of a beam particle. int idBeam, idBeamAbs; Vec4 pBeam; double mBeam; // Beam kind. Valence flavour content for hadrons. bool isUnresolvedBeam, isLeptonBeam, isHadronBeam, isMesonBeam, isBaryonBeam; int nValKinds, idVal[3], nVal[3]; // Current parton density, by valence, sea and companion. int idSave, iSkipSave, nValLeft[3]; double xqgTot, xqVal, xqgSea, xqCompSum; // The list of resolved partons. vector resolved; // Status after all initiators have been accounted for. Junction content. int nInit; bool hasJunctionBeam; int junCol[3]; // Routine to calculate pdf's given previous interactions. double xfModified( int iSkip, int idIn, double x, double Q2); // Fraction of hadron momentum sitting in a valence quark distribution. double xValFrac(int j, double Q2); double Q2ValFracSav, uValInt, dValInt; // Fraction of hadron momentum sitting in a companion quark distribution. double xCompFrac(double xs); // Value of companion quark PDF, also given the sea quark x. double xCompDist(double xc, double xs); // Valence quark subdivision for diffractive systems. int idVal1, idVal2, idVal3; double zRel, pxRel, pyRel; }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_BeamParticle_H pythia8-8.1.80.orig/include/Pythia8/History.h0000644000175000017500000010074712217346227017133 0ustar sunsun// History.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file is written by Stefan Prestel. // It contains the main class for matrix element merging. // Header file for the Clustering and History classes. #ifndef Pythia8_History_H #define Pythia8_History_H #include "Pythia8/Basics.h" #include "Pythia8/BeamParticle.h" #include "Pythia8/Event.h" #include "Pythia8/Info.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" #include "Pythia8/PartonLevel.h" namespace Pythia8 { //========================================================================== // Declaration of Clustering class. // This class holds information about one radiator, recoiler, emitted system. // This class is a container class for History class use. class Clustering { public: // The emitted parton location. int emitted; // The emittor parton int emittor; // The recoiler parton. int recoiler; // The colour connected recoiler (Can be different for ISR) int partner; // The scale associated with this clustering. double pTscale; // Default constructor Clustering(){ emitted = 0; emittor = 0; recoiler = 0; partner = 0; pTscale = 0.0; } // Default destructor ~Clustering(){} // Copy constructor Clustering( const Clustering& inSystem ){ emitted = inSystem.emitted; emittor = inSystem.emittor; recoiler = inSystem.recoiler; partner = inSystem.partner; pTscale = inSystem.pTscale; } // Constructor with input Clustering( int emtIn, int radIn, int recIn, int partnerIn, double pTscaleIn ){ emitted = emtIn; emittor = radIn; recoiler = recIn; partner = partnerIn; pTscale = pTscaleIn; } // Function to return pythia pT scale of clustering double pT() const { return pTscale; } // print for debug void list() const; }; //========================================================================== // Declaration of History class // // A History object represents an event in a given step in the CKKW-L // clustering procedure. It defines a tree-like recursive structure, // where the root node represents the state with n jets as given by // the matrix element generator, and is characterized by the member // variable mother being null. The leaves on the tree corresponds to a // fully clustered paths where the original n-jets has been clustered // down to the Born-level state. Also states which cannot be clustered // down to the Born-level are possible - these will be called // incomplete. The leaves are characterized by the vector of children // being empty. class History { public: // The only constructor. Default arguments are used when creating // the initial history node. The \a depth is the maximum number of // clusterings requested. \a scalein is the scale at which the \a // statein was clustered (should be set to the merging scale for the // initial history node. \a beamAIn and beamBIn are needed to // calcutate PDF ratios, \a particleDataIn to have access to the // correct masses of particles. If \a isOrdered is true, the previous // clusterings has been ordered. \a is the PDF ratio for this // clustering (=1 for FSR clusterings). \a probin is the accumulated // probabilities for the previous clusterings, and \ mothin is the // previous history node (null for the initial node). History( int depth, double scalein, Event statein, Clustering c, MergingHooks* mergingHooksPtrIn, BeamParticle beamAIn, BeamParticle beamBIn, ParticleData* particleDataPtrIn, Info* infoPtrIn, bool isOrdered, bool isStronglyOrdered, bool isAllowed, bool isNextInInput, double probin, History * mothin); // The destructor deletes each child. ~History() { for ( int i = 0, N = children.size(); i < N; ++i ) delete children[i]; } // Function to project paths onto desired paths. bool projectOntoDesiredHistories(); // For CKKW-L, NL3 and UMEPS: // In the initial history node, select one of the paths according to // the probabilities. This function should be called for the initial // history node. // IN trialShower* : Previously initialised trialShower object, // to perform trial showering and as // repository of pointers to initialise alphaS // PartonSystems* : PartonSystems object needed to initialise // shower objects // OUT double : (Sukadov) , (alpha_S ratios) , (PDF ratios) double weightTREE(PartonLevel* trial, AlphaStrong * asFSR, AlphaStrong * asISR, double RN); // For default NL3: // Return weight of virtual correction and subtractive for NL3 merging double weightLOOP(PartonLevel* trial, double RN); // Return O(\alpha_s)-term of CKKWL-weight for NL3 merging double weightFIRST(PartonLevel* trial, AlphaStrong* asFSR, AlphaStrong* asISR, double RN, Rndm* rndmPtr ); // For UMEPS: double weight_UMEPS_TREE(PartonLevel* trial, AlphaStrong * asFSR, AlphaStrong * asISR, double RN); double weight_UMEPS_SUBT(PartonLevel* trial, AlphaStrong * asFSR, AlphaStrong * asISR, double RN); // For unitary NL3: double weight_UNLOPS_TREE(PartonLevel* trial, AlphaStrong * asFSR, AlphaStrong * asISR, double RN); double weight_UNLOPS_SUBT(PartonLevel* trial, AlphaStrong * asFSR, AlphaStrong * asISR, double RN); double weight_UNLOPS_LOOP(PartonLevel* trial, double RN); double weight_UNLOPS_SUBTNLO(PartonLevel* trial, double RN); double weight_UNLOPS_CORRECTION( int order, PartonLevel* trial, AlphaStrong* asFSR, AlphaStrong* asISR, double RN, Rndm* rndmPtr ); // Function to check if any allowed histories were found bool foundAllowedHistories() { return (children.size() > 0 && foundAllowedPath); } // Function to check if any ordered histories were found bool foundOrderedHistories() { return (children.size() > 0 && foundOrderedPath); } // Function to check if any ordered histories were found bool foundCompleteHistories() { return (children.size() > 0 && foundCompletePath); } // Function to set the state with complete scales for evolution void getStartingConditions( const double RN, Event& outState ); // Function to get the state with complete scales for evolution bool getClusteredEvent( const double RN, int nSteps, Event& outState); // Function to get the first reclustered state above the merging scale. bool getFirstClusteredEventAboveTMS( const double RN, int nDesired, Event& process, int & nPerformed, bool updateProcess = true ); // Function to return the depth of the history (i.e. the number of // reclustered splittings) int nClusterings(); // Function to get the lowest multiplicity reclustered event Event lowestMultProc( const double RN) { // Return lowest multiplicity state return (select(RN)->state); } // Calculate and return pdf ratio double getPDFratio( int side, bool forSudakov, bool useHardPDF, int flavNum, double xNum, double muNum, int flavDen, double xDen, double muDen); // Function to print the history that would be chosen from the random number // RN. Mainly for debugging. void printHistory( const double RN ); // Function to print the states in a history, starting from the hard process. // Mainly for debugging. void printStates(); // Make Pythia class friend friend class Pythia; // Make Merging class friend friend class Merging; private: // Number of trial emission to use for calculating the average number of // emissions static const int NTRIAL; // Function to set all scales in the sequence of states. This is a // wrapper routine for setScales and setEventScales methods void setScalesInHistory(); // Function to find the index (in the mother histories) of the // child history, thus providing a way access the path from both // initial history (mother == 0) and final history (all children == 0) // IN vector : The index of each child in the children vector // of the current history node will be saved in // this vector // NO OUTPUT void findPath(vector& out); // Functions to set the parton production scales and enforce // ordering on the scales of the respective clusterings stored in // the History node: // Method will start from lowest multiplicity state and move to // higher states, setting the production scales the shower would // have used. // When arriving at the highest multiplicity, the method will switch // and go back in direction of lower states to check and enforce // ordering for unordered histories. // IN vector : Vector of positions of the chosen child // in the mother history to allow to move // in direction initial->final along path // bool : True: Move in direction low->high // multiplicity and set production scales // False: Move in direction high->low // multiplicity and check and enforce // ordering // NO OUTPUT void setScales( vector index, bool forward); // Function to find a particle in all higher multiplicity events // along the history path and set its production scale to the input // scale // IN int iPart : Parton in refEvent to be checked / rescaled // Event& refEvent : Reference event for iPart // double scale : Scale to be set as production scale for // unchanged copies of iPart in subsequent steps void scaleCopies(int iPart, const Event& refEvent, double rho); // Function to set the OVERALL EVENT SCALES [=state.scale()] to // the scale of the last clustering // NO INPUT // NO OUTPUT void setEventScales(); // Function to print information on the reconstructed scales in one path. // For debug only. void printScales() { if ( mother ) mother->printScales(); cout << " size " << state.size() << " scale " << scale << " clusterIn " << clusterIn.pT() << " state.scale() " << state.scale() << endl; } // Function to project paths onto desired paths. bool trimHistories(); // Function to tag history for removal. void remove(){ doInclude = false; } // Function to return flag of allowed histories to choose from. bool keep(){ return doInclude; } // Function implementing checks on a paths, for deciding if the path should // be considered valid or not. bool keepHistory(); // Function to check if a path is ordered in evolution pT. bool isOrderedPath( double maxscale ); bool followsInputPath(); // Function to check if all reconstucted states in a path pass the merging // scale cut. bool allIntermediateAboveRhoMS( double rhoms, bool good = true ); // Function to check if any ordered paths were found (and kept). bool foundAnyOrderedPaths(); // Functions to return the z value of the last ISR splitting // NO INPUT // OUTPUT double : z value of last ISR splitting in history double zISR(); // Functions to return the z value of the last FSR splitting // NO INPUT // OUTPUT double : z value of last FSR splitting in history double zFSR(); // Functions to return the pT scale of the last ISR splitting // NO INPUT // OUTPUT double : pT scale of last ISR splitting in history double pTISR(); // Functions to return the pT scale of the last FSR splitting // NO INPUT // OUTPUT double : pT scale of last FSR splitting in history double pTFSR(); // Functions to return the event with nSteps additional partons // INPUT int : Number of splittings in the event, // as counted from core 2->2 process // OUTPUT Event : event with nSteps additional partons Event clusteredState( int nSteps); // Function to choose a path from all paths in the tree // according to their splitting probabilities // IN double : Random number // OUT History* : Leaf of history path chosen History * select(double rnd); // For a full path, find the weight calculated from the ratio of // couplings, the no-emission probabilities, and possible PDF // ratios. This function should only be called for the last history // node of a full path. // IN TimeShower : Already initialised shower object to be used as // trial shower // double : alpha_s value used in ME calculation // double : Maximal mass scale of the problem (e.g. E_CM) // AlphaStrong: Initialised shower alpha_s object for FSR alpha_s // ratio calculation // AlphaStrong: Initialised shower alpha_s object for ISR alpha_s // ratio calculation (can be different from previous) double weightTree(PartonLevel* trial, double as0, double maxscale, double pdfScale, AlphaStrong * asFSR, AlphaStrong * asISR, double& asWeight, double& pdfWeight); // Function to return the \alpha_s-ratio part of the CKKWL weight. double weightTreeALPHAS( double as0, AlphaStrong * asFSR, AlphaStrong * asISR ); // Function to return the PDF-ratio part of the CKKWL weight. double weightTreePDFs( double maxscale, double pdfScale ); // Function to return the no-emission probability part of the CKKWL weight. double weightTreeEmissions( PartonLevel* trial, int type, int njetMax, double maxscale ); // Function to generate the O(\alpha_s)-term of the CKKWL-weight double weightFirst(PartonLevel* trial, double as0, double muR, double maxscale, AlphaStrong * asFSR, AlphaStrong * asISR, Rndm* rndmPtr ); // Function to generate the O(\alpha_s)-term of the \alpha_s-ratios // appearing in the CKKWL-weight. double weightFirstALPHAS( double as0, double muR, AlphaStrong * asFSR, AlphaStrong * asISR); // Function to generate the O(\alpha_s)-term of the PDF-ratios // appearing in the CKKWL-weight. double weightFirstPDFs( double as0, double maxscale, double pdfScale, Rndm* rndmPtr ); // Function to generate the O(\alpha_s)-term of the no-emission // probabilities appearing in the CKKWL-weight. double weightFirstEmissions(PartonLevel* trial, double as0, double maxscale, AlphaStrong * asFSR, AlphaStrong * asISR, bool fixpdf, bool fixas ); // Function to return the default factorisation scale of the hard process. double hardFacScale(const Event& event); // Function to return the default renormalisation scale of the hard process. double hardRenScale(const Event& event); // Perform a trial shower using the \a pythia object between // maxscale down to this scale and return the corresponding Sudakov // form factor. // IN trialShower : Shower object used as trial shower // double : Maximum scale for trial shower branching // OUT 0.0 : trial shower emission outside allowed pT range // 1.0 : trial shower successful (any emission was below // the minimal scale ) double doTrialShower(PartonLevel* trial, int type, double maxscale, double minscale = 0.); // Function to bookkeep the indices of weights generated in countEmissions bool updateind(vector & ind, int i, int N); // Function to count number of emissions between two scales for NLO merging vector countEmissions(PartonLevel* trial, double maxscale, double minscale, int showerType, double as0, AlphaStrong * asFSR, AlphaStrong * asISR, int N, bool fixpdf, bool fixas); // Function to integrate PDF ratios between two scales over x and t, // where the PDFs are always evaluated at the lower t-integration limit double monteCarloPDFratios(int flav, double x, double maxScale, double minScale, double pdfScale, double asME, Rndm* rndmPtr); // Default: Check if a ordered (and complete) path has been found in // the initial node, in which case we will no longer be interested in // any unordered paths. bool onlyOrderedPaths(); // Check if a strongly ordered (and complete) path has been found in the // initial node, in which case we will no longer be interested in // any unordered paths. bool onlyStronglyOrderedPaths(); // Check if an allowed (according to user-criterion) path has been found in // the initial node, in which case we will no longer be interested in // any forbidden paths. bool onlyAllowedPaths(); // When a full path has been found, register it with the initial // history node. // IN History : History to be registered as path // bool : Specifying if clusterings so far were ordered // bool : Specifying if path is complete down to 2->2 process // OUT true if History object forms a plausible path (eg prob>0 ...) bool registerPath(History & l, bool isOrdered, bool isStronglyOrdered, bool isAllowed, bool isComplete); // For the history-defining state (and if necessary interfering // states), find all possible clusterings. // NO INPUT // OUT vector of all (rad,rec,emt) systems vector getAllQCDClusterings(); // For one given state, find all possible clusterings. // IN Event : state to be investigated // OUT vector of all (rad,rec,emt) systems in the state vector getQCDClusterings( const Event& event); // Function to construct (rad,rec,emt) triples from the event // IN int : Position of Emitted in event record for which // dipoles should be constructed // int : Colour topogy to be tested // 1= g -> qqbar, causing 2 -> 2 dipole splitting // 2= q(bar) -> q(bar) g && g -> gg, // causing a 2 -> 3 dipole splitting // Event : event record to be checked for ptential partners // OUT vector of all allowed radiator+recoiler+emitted triples vector findQCDTriple (int EmtTagIn, int colTopIn, const Event& event, vector PosFinalPartn, vector PosInitPartn ); vector getAllEWClusterings(); vector getEWClusterings( const Event& event); vector findEWTriple( int EmtTagIn, const Event& event, vector PosFinalPartn ); vector getAllSQCDClusterings(); vector getSQCDClusterings( const Event& event); vector findSQCDTriple (int EmtTagIn, int colTopIn, const Event& event, vector PosFinalPartn, vector PosInitPartn ); // Calculate and return the probability of a clustering. // IN Clustering : rad,rec,emt - System for which the splitting // probability should be calcuated // OUT splitting probability double getProb(const Clustering & SystemIn); // Set up the beams (fill the beam particles with the correct // current incoming particles) to allow calculation of splitting // probability. // For interleaved evolution, set assignments dividing PDFs into // sea and valence content. This assignment is, until a history path // is chosen and a first trial shower performed, not fully correct // (since content is chosen form too high x and too low scale). The // assignment used for reweighting will be corrected after trial // showering void setupBeams(); // Calculate the PDF ratio used in the argument of the no-emission // probability. double pdfForSudakov(); // Calculate the hard process matrix element to include in the selection // probability. double hardProcessME( const Event& event); // Perform the clustering of the current state and return the // clustered state. // IN Clustering : rad,rec,emt triple to be clustered to two partons // OUT clustered state Event cluster(const Clustering & inSystem); // Function to get the flavour of the radiator before the splitting // for clustering // IN int : Position of the radiator after the splitting, in the event // int : Position of the emitted after the splitting, in the event // Event : Reference event // OUT int : Flavour of the radiator before the splitting int getRadBeforeFlav(const int RadAfter, const int EmtAfter, const Event& event); // Function to get the colour of the radiator before the splitting // for clustering // IN int : Position of the radiator after the splitting, in the event // int : Position of the emitted after the splitting, in the event // Event : Reference event // OUT int : Colour of the radiator before the splitting int getRadBeforeCol(const int RadAfter, const int EmtAfter, const Event& event); // Function to get the anticolour of the radiator before the splitting // for clustering // IN int : Position of the radiator after the splitting, in the event // int : Position of the emitted after the splitting, in the event // Event : Reference event // OUT int : Anticolour of the radiator before the splitting int getRadBeforeAcol(const int RadAfter, const int EmtAfter, const Event& event); // Function to get the parton connected to in by a colour line // IN int : Position of parton for which partner should be found // Event : Reference event // OUT int : If a colour line connects the "in" parton with another // parton, return the Position of the partner, else return 0 int getColPartner(const int in, const Event& event); // Function to get the parton connected to in by an anticolour line // IN int : Position of parton for which partner should be found // Event : Reference event // OUT int : If an anticolour line connects the "in" parton with another // parton, return the Position of the partner, else return 0 int getAcolPartner(const int in, const Event& event); // Function to get the list of partons connected to the particle // formed by reclusterinf emt and rad by colour and anticolour lines // IN int : Position of radiator in the clustering // IN int : Position of emitted in the clustering // Event : Reference event // OUT vector : List of positions of all partons that are connected // to the parton that will be formed // by clustering emt and rad. vector getReclusteredPartners(const int rad, const int emt, const Event& event); // Function to extract a chain of colour-connected partons in // the event // IN int : Type of parton from which to start extracting a // parton chain. If the starting point is a quark // i.e. flavType = 1, a chain of partons that are // consecutively connected by colour-lines will be // extracted. If the starting point is an antiquark // i.e. flavType =-1, a chain of partons that are // consecutively connected by anticolour-lines // will be extracted. // IN int : Position of the parton from which a // colour-connected chain should be derived // IN Event : Refernence event // IN/OUT vector : Partons that should be excluded from the search. // OUT vector : Positions of partons along the chain // OUT bool : Found singlet / did not find singlet bool getColSinglet(const int flavType, const int iParton, const Event& event, vector& exclude, vector& colSinglet); // Function to check that a set of partons forms a colour singlet // IN Event : Reference event // IN vector : Positions of the partons in the set // OUT bool : Is a colour singlet / is not bool isColSinglet( const Event& event, vector system); // Function to check that a set of partons forms a flavour singlet // IN Event : Reference event // IN vector : Positions of the partons in the set // IN int : Flavour of all the quarks in the set, if // all quarks in a set should have a fixed flavour // OUT bool : Is a flavour singlet / is not bool isFlavSinglet( const Event& event, vector system, int flav=0); // Function to properly colour-connect the radiator to the rest of // the event, as needed during clustering // IN Particle& : Particle to be connected // Particle : Recoiler forming a dipole with Radiator // Event : event to which Radiator shall be appended // OUT true : Radiator could be connected to the event // false : Radiator could not be connected to the // event or the resulting event was // non-valid bool connectRadiator( Particle& Radiator, const int RadType, const Particle& Recoiler, const int RecType, const Event& event ); // Function to find a colour (anticolour) index in the input event // IN int col : Colour tag to be investigated // int iExclude1 : Identifier of first particle to be excluded // from search // int iExclude2 : Identifier of second particle to be excluded // from search // Event event : event to be searched for colour tag // int type : Tag to define if col should be counted as // colour (type = 1) [->find anti-colour index // contracted with col] // anticolour (type = 2) [->find colour index // contracted with col] // OUT int : Position of particle in event record // contraced with col [0 if col is free tag] int FindCol(int col, int iExclude1, int iExclude2, const Event& event, int type, bool isHardIn); // Function to in the input event find a particle with quantum // numbers matching those of the input particle // IN Particle : Particle to be searched for // Event : Event to be searched in // OUT int : > 0 : Position of matching particle in event // < 0 : No match in event int FindParticle( const Particle& particle, const Event& event, bool checkStatus = true ); // Function to check if rad,emt,rec triple is allowed for clustering // IN int rad,emt,rec,partner : Positions (in event record) of the three // particles considered for clustering, and the // correct colour-connected recoiler (=partner) // Event event : Reference event bool allowedClustering( int rad, int emt, int rec, int partner, const Event& event ); // Function to check if rad,emt,rec triple is results in // colour singlet radBefore+recBefore // IN int rad,emt,rec : Positions (in event record) of the three // particles considered for clustering // Event event : Reference event bool isSinglett( int rad, int emt, int rec, const Event& event ); // Function to check if event is sensibly constructed: Meaning // that all colour indices are contracted and that the charge in // initial and final states matches // IN event : event to be checked // OUT TRUE : event is properly construced // FALSE : event not valid bool validEvent( const Event& event ); // Function to check whether two clusterings are identical, used // for finding the history path in the mother -> children direction bool equalClustering( Clustering clus1 , Clustering clus2 ); // Chose dummy scale for event construction. By default, choose // sHat for 2->Boson(->2)+ n partons processes and // M_Boson for 2->Boson(->) processes double choseHardScale( const Event& event ) const; // If the state has an incoming hadron return the flavour of the // parton entering the hard interaction. Otherwise return 0 int getCurrentFlav(const int) const; // If the state has an incoming hadron return the x-value for the // parton entering the hard interaction. Otherwise return 0. double getCurrentX(const int) const; double getCurrentZ(const int rad, const int rec, const int emt) const; // Function to compute "pythia pT separation" from Particle input double pTLund(const Particle& RadAfterBranch,const Particle& EmtAfterBranch, const Particle& RecAfterBranch, int ShowerType); // Function to return the position of the initial line before (or after) // a single (!) splitting. int posChangedIncoming(const Event& event, bool before); // Function to give back the ratio of PDFs and PDF * splitting kernels // needed to convert a splitting at scale pdfScale, chosen with running // PDFs, to a splitting chosen with PDFs at a fixed scale mu. As needed to // properly count emissions. double pdfFactor( const Event& event, const int type, double pdfScale, double mu ); // Function giving the product of splitting kernels and PDFs so that the // resulting flavour is given by flav. This is used as a helper routine // to dgauss double integrand(int flav, double x, double scaleInt, double z); //----------------------------------------------------------------------// // Class members. //----------------------------------------------------------------------// // The state of the event correponding to this step in the // reconstruction. Event state; // The previous step from which this step has been clustered. If // null, this is the initial step with the n-jet state generated by // the matrix element. History * mother; // The different steps corresponding to possible clusterings of this // state. vector children; // The different paths which have been reconstructed indexed with // the (incremental) corresponding probability. This map is empty // unless this is the initial step (mother == 0). map paths; // The sum of the probabilities of the full paths. This is zero // unless this is the initial step (mother == 0). double sumpath; // The different allowed paths after projection, indexed with // the (incremental) corresponding probability. This map is empty // unless this is the initial step (mother == 0). map goodBranches, badBranches; // The sum of the probabilities of allowed paths after projection. This is // zero unless this is the initial step (mother == 0). double sumGoodBranches, sumBadBranches; // This is set true if an ordered (and complete) path has been found // and inserted in paths. bool foundOrderedPath; // This is set true if a strongly ordered (and complete) path has been found // and inserted in paths. bool foundStronglyOrderedPath; // This is set true if an allowed (according to a user criterion) path has // been found and inserted in paths. bool foundAllowedPath; // This is set true if a complete (with the required number of // clusterings) path has been found and inserted in paths. bool foundCompletePath; // The scale of this step, corresponding to clustering which // constructed the corresponding state (or the merging scale in case // mother == 0). double scale; // Flag indicating if a clustering in the construction of all histories is // the next clustering demanded by inout clusterings in LesHouches 2.0 // accord. bool nextInInput; // The probability associated with this step and the previous steps. double prob; // The partons and scale of the last clustering. Clustering clusterIn; int iReclusteredOld, iReclusteredNew; // Flag to include the path amongst allowed paths. bool doInclude; // Pointer to MergingHooks object to get all the settings. MergingHooks* mergingHooksPtr; // The default constructor is private. History() {} // The copy-constructor is private. History(const History &) {} // The assignment operator is private. History & operator=(const History &) { return *this; } // BeamParticle to get access to PDFs BeamParticle beamA; BeamParticle beamB; // ParticleData needed to initialise the shower AND to get the // correct masses of partons needed in calculation of probability ParticleData* particleDataPtr; // Info object to have access to all information read from LHE file Info* infoPtr; // Minimal scalar sum of pT used in Herwig to choose history double sumScalarPT; }; //========================================================================== } // end namespace Pythia8 #endif // end Pythia8_History_H pythia8-8.1.80.orig/include/Pythia8/ResonanceWidths.h0000644000175000017500000004341112217346231020557 0ustar sunsun// ResonanceWidths.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Header file for resonance properties: dynamical widths etc. // ResonanceWidths: base class for all resonances. // ResonanceGmZ, ...: derived classes for individual resonances. #ifndef Pythia8_ResonanceWidths_H #define Pythia8_ResonanceWidths_H #include "Pythia8/Basics.h" #include "Pythia8/Info.h" #include "Pythia8/PythiaStdlib.h" #include "Pythia8/Settings.h" #include "Pythia8/StandardModel.h" namespace Pythia8 { //========================================================================== // Forward references to ParticleData and StandardModel classes. class DecayChannel; class ParticleData; class ParticleDataEntry; class Couplings; //========================================================================== // The ResonanceWidths is the base class. Also used for generic resonaces. class ResonanceWidths { public: // Destructor. virtual ~ResonanceWidths() {} // Set up standard properties. void initBasic(int idResIn, bool isGenericIn = false) { idRes = idResIn; isGeneric = isGenericIn;} // Calculate and store partial and total widths at the nominal mass. virtual bool init(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Couplings* couplingsPtrIn); // Return identity of particle species. int id() const {return idRes;} // Calculate the total/open width for given mass, charge and instate. double width(int idSgn, double mHatIn, int idInFlavIn = 0, bool openOnly = false, bool setBR = false, int idOutFlav1 = 0, int idOutFlav2 = 0); // Special case to calculate open final-state width. double widthOpen(int idSgn, double mHatIn, int idIn = 0) { return width( idSgn, mHatIn, idIn, true, false);} // Special case to store open final-state widths for channel selection. double widthStore(int idSgn, double mHatIn, int idIn = 0) { return width( idSgn, mHatIn, idIn, true, true);} // Return fraction of width open for particle and antiparticle. double openFrac(int idSgn) {return (idSgn > 0) ? openPos : openNeg;} // Return forced rescaling factor of resonance width. double widthRescaleFactor() {return forceFactor;} // Special case to calculate one final-state width. // Currently only used for Higgs -> qqbar, g g or gamma gamma. double widthChan(double mHatIn, int idOutFlav1, int idOutFlav2) { return width( 1, mHatIn, 0, false, false, idOutFlav1, idOutFlav2);} protected: // Constructor. ResonanceWidths() {} // Constants: could only be changed in the code itself. static const int NPOINT; static const double MASSMARGIN; // Particle properties always present. int idRes, hasAntiRes; bool doForceWidth, isGeneric, allowCalcWidth; double minWidth, minThreshold, mRes, GammaRes, m2Res, GamMRat, openPos, openNeg, forceFactor; // Properties for currently studied decay channel(s). int iChannel, onMode, meMode, mult, id1, id2, id3, id1Abs, id2Abs, id3Abs, idInFlav; double widNow, mHat, mf1, mf2, mf3, mr1, mr2, mr3, ps, kinFac, alpEM, alpS, colQ, preFac; // Pointer to properties of the particle species. ParticleDataEntry* particlePtr; // Pointer to various information on the generation. Info* infoPtr; // Pointer to the settings database. Settings* settingsPtr; // Pointer to the particle data table. ParticleData* particleDataPtr; // Pointers to Standard Model and SUSY couplings. Couplings* couplingsPtr; // Initialize constants. virtual void initConstants() {} // Virtual methods to handle model-specific (non-SM) part of initialization // for use by derived classes that implement additional models (eg SUSY). virtual bool initBSM() {return true;} virtual bool allowCalc() {return true;} // Calculate various common prefactors for the current mass. // Optional argument calledFromInit only used for Z0. virtual void calcPreFac(bool = false) {} // Calculate width for currently considered channel. // Optional argument calledFromInit only used for Z0. virtual void calcWidth(bool = false) {} // Simple routines for matrix-element integration over Breit-Wigners. double numInt1BW(double mHatIn, double m1, double Gamma1, double mMin1, double m2, int psMode = 1); double numInt2BW(double mHatIn, double m1, double Gamma1, double mMin1, double m2, double Gamma2, double mMin2, int psMode = 1); }; //========================================================================== // The ResonanceGeneric class handles a generic resonance. // Only needs a constructor; for the rest uses defaults in base class. class ResonanceGeneric : public ResonanceWidths { public: // Constructor. ResonanceGeneric(int idResIn) {initBasic(idResIn, true);} }; //========================================================================== // The ResonanceGmZ class handles the gamma*/Z0 resonance. class ResonanceGmZ : public ResonanceWidths { public: // Constructor. ResonanceGmZ(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. int gmZmode; double thetaWRat, ei2, eivi, vi2ai2, gamNorm, intNorm, resNorm; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool calledFromInit = false); }; //========================================================================== // The ResonanceW class handles the W+- resonance. class ResonanceW : public ResonanceWidths { public: // Constructor. ResonanceW(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double thetaWRat, alpEM; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceTop class handles the top/antitop resonance. class ResonanceTop : public ResonanceWidths { public: // Constructor. ResonanceTop(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double thetaWRat, m2W, tanBeta, tan2Beta, mbRun; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceFour class handles fourth-generation resonances. class ResonanceFour : public ResonanceWidths { public: // Constructor. ResonanceFour(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double thetaWRat, m2W; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceH class handles the SM and BSM Higgs resonance. // higgsType = 0 : SM H; = 1: h^0/H_1; = 2 : H^0/H_2; = 3 : A^0/A_3. class ResonanceH : public ResonanceWidths { public: // Constructor. ResonanceH(int higgsTypeIn, int idResIn) : higgsType(higgsTypeIn) {initBasic(idResIn);} private: // Constants: could only be changed in the code itself. static const double MASSMINWZ, MASSMINT, GAMMAMARGIN; // Higgs type in current instance. int higgsType; // Locally stored properties and couplings. bool useCubicWidth, useRunLoopMass; double sin2tW, cos2tW, mT, mZ, mW, mHchg, GammaT, GammaZ, GammaW, coup2d, coup2u, coup2l, coup2Z, coup2W, coup2Hchg, coup2H1H1, coup2A3A3, coup2H1Z, coup2A3Z, coup2A3H1, coup2HchgW, mLowT, mStepT, mLowZ, mStepZ, mLowW, mStepW, kinFacT[101], kinFacZ[101], kinFacW[101]; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); // Sum up loop contributions in Higgs -> g + g. double eta2gg(); // Sum up loop contributions in Higgs -> gamma + gamma. double eta2gaga(); // Sum up loop contributions in Higgs -> gamma + Z0. double eta2gaZ(); }; //========================================================================== // The ResonanceHchg class handles the H+- resonance. class ResonanceHchg : public ResonanceWidths { public: // Constructor. ResonanceHchg(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. bool useCubicWidth; double thetaWRat, mW, tanBeta, tan2Beta, coup2H1W; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceZprime class handles the gamma*/Z0 /Z'^0 resonance. class ResonanceZprime : public ResonanceWidths { public: // Constructor. ResonanceZprime(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. int gmZmode; double sin2tW, cos2tW, thetaWRat, mZ, GammaZ, m2Z, GamMRatZ, afZp[20], vfZp[20], coupZpWW, ei2, eivi, vai2, eivpi, vaivapi, vapi2, gamNorm, gamZNorm, ZNorm, gamZpNorm, ZZpNorm, ZpNorm; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool calledFromInit = false); }; //========================================================================== // The ResonanceWprime class handles the W'+- resonance. class ResonanceWprime : public ResonanceWidths { public: // Constructor. ResonanceWprime(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double thetaWRat, cos2tW, alpEM, aqWp, vqWp, alWp, vlWp, coupWpWZ; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceRhorizontal class handles the R^0 resonance. class ResonanceRhorizontal : public ResonanceWidths { public: // Constructor. ResonanceRhorizontal(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double thetaWRat; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceExcited class handles excited-fermion resonances. class ResonanceExcited : public ResonanceWidths { public: // Constructor. ResonanceExcited(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double Lambda, coupF, coupFprime, coupFcol, sin2tW, cos2tW; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceGraviton class handles the excited Graviton resonance. class ResonanceGraviton : public ResonanceWidths { public: // Constructor. ResonanceGraviton(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. bool eDsmbulk, eDvlvl; double kappaMG; // Couplings between graviton and SM (map from particle id to coupling). double eDcoupling[27]; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceKKgluon class handles the g^*/KK-gluon^* resonance. class ResonanceKKgluon : public ResonanceWidths { public: // Constructor. ResonanceKKgluon(int idResIn) {initBasic(idResIn);} private: // Locally stored properties. double normSM, normInt, normKK; // Couplings between kk gluon and SM (indexed by particle id). // Helicity dependent couplings. Use vector/axial-vector // couplings internally, gv/ga = 0.5 * (gL +/- gR). double eDgv[10], eDga[10]; // Interference parameter. int interfMode; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool calledFromInit = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool calledFromInit = false); }; //========================================================================== // The ResonanceLeptoquark class handles the LQ/LQbar resonance. class ResonanceLeptoquark : public ResonanceWidths { public: // Constructor. ResonanceLeptoquark(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double kCoup; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceNuRight class handles righthanded Majorana neutrinos. class ResonanceNuRight : public ResonanceWidths { public: // Constructor. ResonanceNuRight(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double thetaWRat, mWR; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceZRight class handles the Z_R^0 resonance. class ResonanceZRight : public ResonanceWidths { public: // Constructor. ResonanceZRight(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double sin2tW, thetaWRat; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceWRight class handles the W_R+- resonance. class ResonanceWRight : public ResonanceWidths { public: // Constructor. ResonanceWRight(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double thetaWRat; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceHchgchgLeft class handles the H++/H-- (left) resonance. class ResonanceHchgchgLeft : public ResonanceWidths { public: // Constructor. ResonanceHchgchgLeft(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double yukawa[4][4], gL, vL, mW; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== // The ResonanceHchgchgRight class handles the H++/H-- (right) resonance. class ResonanceHchgchgRight : public ResonanceWidths { public: // Constructor. ResonanceHchgchgRight(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. int idWR; double yukawa[4][4], gR; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. virtual void calcPreFac(bool = false); // Caclulate width for currently considered channel. virtual void calcWidth(bool = false); }; //========================================================================== } // end namespace Pythia8 #endif // Pythia8_ResonanceWidths_H pythia8-8.1.80.orig/examples/0000755000175000017500000000000012217357205014153 5ustar sunsunpythia8-8.1.80.orig/examples/main46.cc0000644000175000017500000001564012217346166015572 0ustar sunsun// main46.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // // Author: S.Chekanov (ANL). // An example of how to write ProMC files. // // The ProMC library is described at http://atlaswww.hep.anl.gov/asc/promc/ // A makefile can be found in the ProMC package, in examples/pythia. #include #include "Pythia.h" // ProMC file #include "ProMCHeader.pb.h" #include "ProMC.pb.h" #include "ProMCBook.h" using namespace Pythia8; //-------------------------------------------------------------------------- string getEnvVar( std::string const & key ) { char * val = getenv( key.c_str() ); return (val == NULL) ? std::string("") : std::string(val); } //-------------------------------------------------------------------------- void readPDG( ProMCHeader * header ) { string temp_string; istringstream curstring; string PdgTableFilename = getEnvVar("PROMC") + "/data/particle.tbl"; if (PdgTableFilename.size() < 2) { cout << "** ERROR: PROMC variable not set. Did you run source.sh" << " **" << endl; exit(1); } ifstream file_to_read(PdgTableFilename.c_str()); if (!file_to_read.good()) { cout << "** ERROR: PDG Table (" << PdgTableFilename << ") not found! exit. **" << endl; exit(1); return; } // First three lines of the file are useless. getline(file_to_read,temp_string); getline(file_to_read,temp_string); getline(file_to_read,temp_string); while (getline(file_to_read,temp_string)) { // Needed when using several times istringstream::str(string). curstring.clear(); curstring.str(temp_string); long int ID; std::string name; int charge; float mass; float width; float lifetime; // ID name chg mass total width lifetime // 1 d -1 0.33000 0.00000 0.00000E+00 // in the table, the charge is in units of e+/3 // the total width is in GeV // the lifetime is ctau in mm curstring >> ID >> name >> charge >> mass >> width >> lifetime; ProMCHeader_ParticleData* pp= header->add_particledata(); pp->set_id(ID); pp->set_mass(mass); pp->set_name(name); pp->set_width(width); pp->set_lifetime(lifetime); cout << ID << " " << name << " " << mass << endl; } } //-------------------------------------------------------------------------- int main() { int Ntot = 1000; // Total number of events. // Generator. Process selection. LHC initialization. Pythia pythia; pythia.readString("WeakSingleBoson:ffbar2gmZ = on"); pythia.readString("PhaseSpace:mHatMin = 80."); pythia.readString("PhaseSpace:mHatMax = 120."); pythia.readString("Random:setSeed = on"); pythia.readString("Random:seed = 0"); pythia.init( 2212, 2212, 14000.); // **************** book ProMC file ********************** ProMCBook* epbook = new ProMCBook("Pythia8.promc","w"); epbook->setDescription(Ntot,"PYTHIA8"); // Info on incoming beams and CM energy. ProMCHeader header; header.set_id1( pythia.info.idA() ); header.set_id2( pythia.info.idB() ); header.set_ecm( pythia.info.eCM() ); header.set_s( pythia.info.s() ); // Use the range 0.01 MeV to 20 TeV using varints (integers). // With particle in GeV, we multiply it by kEV, to get 0.01 MeV = 1 unit. const double kEV = 1000*100; // With particle in mm, we multiply it by kL to get 0.01 mm = 1 unit. const double kL = 100; // Set units. header.set_momentumunit( (int)kEV ); header.set_lengthunit( (int)kL ); // Store a map with PDG information (stored in the header). readPDG( &header ); epbook->setHeader(header); // write header // Begin event loop. Generate event. Skip if error. for (int n = 0; n < Ntot; n++) { if (!pythia.next()) { // If failure because reached end of file then exit event loop. if (pythia.info.atEndOfFile()) { cout << " Aborted since reached end of Les Houches Event File\n"; break; } continue; } //************ ProMC file ***************// ProMCEvent promc; // Fill event information. ProMCEvent_Event *eve = promc.mutable_event(); eve->set_number(n); eve->set_process_id( pythia.info.code() ); // process ID eve->set_scale( pythia.info.pTHat( )); // relevant for 2 -> 2 only eve->set_alpha_qed( pythia.info.alphaEM() ); eve->set_alpha_qcd( pythia.info.alphaS() ); eve->set_scale_pdf( pythia.info.QFac() ); eve->set_x1( pythia.info.x1pdf() ); eve->set_x2( pythia.info.x2pdf() ); eve->set_id1( pythia.info.id1pdf() ); eve->set_id2( pythia.info.id2pdf() ); eve->set_pdf1( pythia.info.pdf1() ); eve->set_pdf2( pythia.info.pdf2() ); eve->set_weight( pythia.info.weight() ); // Fill truth particle information, looping over all particles in event. ProMCEvent_Particles *pa= promc.mutable_particles(); for (int i = 0; i < pythia.event.size(); i++) { // Fill information particle by particle. pa->add_id( i ); pa->add_pdg_id( pythia.event[i].id() ); // Particle status in HEPMC style. pa->add_status( pythia.event.statusHepMC(i) ); pa->add_mother1( pythia.event[i].mother1() ); pa->add_mother2( pythia.event[i].mother2() ); pa->add_daughter1( pythia.event[i].daughter1() ); pa->add_daughter2( pythia.event[i].daughter2() ); // Only store three-momentum and mass, so need to calculate energy. pa->add_px( (int)(pythia.event[i].px()*kEV) ); pa->add_py( (int)(pythia.event[i].py()*kEV) ); pa->add_pz( (int)(pythia.event[i].pz()*kEV) ); pa->add_mass( (int)(pythia.event[i].m()*kEV) ); // Store production vertex; will often be the origin. pa->add_x( int(pythia.event[i].xProd()*kL) ); pa->add_y( int(pythia.event[i].yProd()*kL) ); pa->add_z( int(pythia.event[i].zProd()*kL) ); pa->add_t( int(pythia.event[i].tProd()*kL) ); } // end loop over particles in the event epbook->write(promc); // write event } // end loop over events // Print statistics. pythia.stat(); double sigmapb = pythia.info.sigmaGen() * 1.0E9; cout << "== Cross section for this run = " << sigmapb << " pb" << endl; cout << "== Events for this run = " << Ntot << endl; double lumi = (Ntot/sigmapb)/1000; cout << "== Luminosity for this run = " << lumi << " fb-1" << endl; cout << "\n\n"; // Save post-generation statistics for ProMC. ProMCStat stat; stat.set_cross_section_accumulated( sigmapb ); // in pb stat.set_cross_section_error_accumulated( pythia.info.sigmaErr() * 1e9 ); stat.set_luminosity_accumulated( Ntot/sigmapb ); stat.set_ntried( pythia.info.nTried() ); stat.set_nselected( pythia.info.nSelected() ); stat.set_naccepted( pythia.info.nAccepted() ); epbook->setStatistics( stat ); // Close the ProMC file. epbook->close(); // close return 0; } pythia8-8.1.80.orig/examples/main53.cmnd0000644000175000017500000000301612217346166016116 0ustar sunsun! main53.cmnd ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! 1) Settings used in the main program. Main:numberOfEvents = 1000 ! number of events to generate ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showChangedParticleData = off ! list changed particle data Next:numberCount = 100 ! print message every n events Next:numberShowInfo = 2 ! print event information n times Next:numberShowProcess = 2 ! print process record n times Next:numberShowEvent = 1 ! print event record n times ! 3) Include photon-in-proton: use MRST2004qed set PDF:useLHAPDF = on PDF:LHAPDFset = MRST2004qed.LHgrid ! 4 Two options to select hard process to generate. ! A) Read in external event with incoming photon in the ME, ! from pre-generated .lhe file (thanks to SANC and R. Sadykov). #Beams:frameType = 4 ! read in LHE file #Beams:LHEF = photoninproton.lhe ! name of LHE file ! B) Select internal Pythia processes. ! Use that default is 14 TeV pp,so don't set beams. WeakBosonAndParton:fgm2Wf = on ! fermion gamma -> W+- fermion' ! 5) Test flags to simplify generation PartonLevel:MPI = off ! no multiparton interactions #PartonLevel:ISR = off ! initial-state radiation #PartonLevel:FSR = off ! no final-state radiation HadronLevel:Hadronize = off ! no hadronization pythia8-8.1.80.orig/examples/powheg-hvq.lhe0000644000175000017500000024675612217346206016755 0ustar sunsun 2212 2212 7.00000E+03 7.00000E+03 -1 -1 -1 -1 3 1 8.00334E+02 0.00000E+00 0.00000E+00 1006 5 1006 1.00000E+00 1.90417E+01 0.00000E+00 0.00000E+00 21 -1 0 0 134 135 0.000000000E+00 0.000000000E+00 2.693639711E+02 2.693639711E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 132 133 0.000000000E+00 0.000000000E+00 -5.818116662E+02 5.818116662E+02 0.000000000E+00 0.00000E+00 9.000E+00 6 1 1 2 132 0 5.649633545E+01 -1.409096557E+02 -3.628291203E+02 4.288745010E+02 1.710000000E+02 0.00000E+00 9.000E+00 -6 1 1 2 0 135 -4.477951077E+01 1.559196728E+02 1.766816856E+02 2.945735341E+02 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2.977159935E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 132 133 0.000000000E+00 0.000000000E+00 -2.715145965E+02 2.715145965E+02 0.000000000E+00 0.00000E+00 9.000E+00 6 1 1 2 132 0 8.111268631E+01 -9.658722517E+01 -7.114617623E+01 2.240784201E+02 1.710000000E+02 0.00000E+00 9.000E+00 -6 1 1 2 0 135 -1.298412468E+02 1.325033574E+02 1.214290855E+02 2.800034141E+02 1.710000000E+02 0.00000E+00 9.000E+00 21 1 1 2 134 133 4.872856046E+01 -3.591613220E+01 -2.408151225E+01 6.514875585E+01 0.000000000E+00 0.00000E+00 9.000E+00 5 1006 1.00000E+00 1.82989E+00 0.00000E+00 0.00000E+00 2 -1 0 0 133 0 0.000000000E+00 0.000000000E+00 1.258544828E+03 1.258544828E+03 0.000000000E+00 0.00000E+00 9.000E+00 -2 -1 0 0 0 142 0.000000000E+00 0.000000000E+00 -3.260468596E+01 3.260468596E+01 0.000000000E+00 0.00000E+00 9.000E+00 6 1 1 2 132 0 9.259376250E+01 2.321880847E+01 4.617504519E+02 5.015647493E+02 1.710000000E+02 0.00000E+00 9.000E+00 -6 1 1 2 0 142 -9.404940295E+01 -2.210993165E+01 7.505312565E+02 7.758042963E+02 1.710000000E+02 0.00000E+00 9.000E+00 21 1 1 2 133 132 1.455640454E+00 -1.108876822E+00 1.365843395E+01 1.378046861E+01 0.000000000E+00 0.00000E+00 9.000E+00 5 1006 1.00000E+00 3.01969E+01 0.00000E+00 0.00000E+00 21 -1 0 0 134 135 0.000000000E+00 0.000000000E+00 2.809997865E+02 2.809997865E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 132 133 0.000000000E+00 0.000000000E+00 -3.286596627E+02 3.286596627E+02 0.000000000E+00 0.00000E+00 9.000E+00 6 1 1 2 132 0 1.212346839E+02 5.299358720E+01 -1.840791451E+02 2.839582725E+02 1.710000000E+02 0.00000E+00 9.000E+00 -6 1 1 2 0 135 -1.443546756E+02 -3.356891035E+01 1.681313186E+02 2.819118380E+02 1.710000000E+02 0.00000E+00 9.000E+00 21 1 1 2 134 133 2.311999174E+01 -1.942467684E+01 -3.171204968E+01 4.378933869E+01 0.000000000E+00 0.00000E+00 9.000E+00 pythia8-8.1.80.orig/examples/main07.cc0000644000175000017500000000676412217346163015573 0ustar sunsun// main07.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Illustration how to generate various two-body channels from // astroparticle processes, e.g. neutralino annihilation or decay. // To this end a "blob" of energy is created with unit cross section, // from the fictitious collision of two non-radiating incoming e+e-. // In the accompanying main29.cmnd file the decay channels of this // blob can be set up. Furthermore, only gamma, e+-, p/pbar and // neutrinos are stable, everything else is set to decay. // (The "single-particle gun" of main21.cc offers another possible // approach to the same problem.) #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // A derived class for (e+ e- ->) GenericResonance -> various final states. class Sigma1GenRes : public Sigma1Process { public: // Constructor. Sigma1GenRes() {} // Evaluate sigmaHat(sHat): dummy unit cross section. virtual double sigmaHat() {return 1.;} // Select flavour. No colour or anticolour. virtual void setIdColAcol() {setId( -11, 11, 999999); setColAcol( 0, 0, 0, 0, 0, 0);} // Info on the subprocess. virtual string name() const {return "GenericResonance";} virtual int code() const {return 9001;} virtual string inFlux() const {return "ffbarSame";} }; //========================================================================== int main() { // Pythia generator. Pythia pythia; // A class to generate the fictitious resonance initial state. SigmaProcess* sigma1GenRes = new Sigma1GenRes(); // Hand pointer to Pythia. pythia.setSigmaPtr( sigma1GenRes); // Read in the rest of the settings and data from a separate file. pythia.readFile("main07.cmnd"); // Initialization. pythia.init(); // Extract settings to be used in the main program. int nEvent = pythia.mode("Main:numberOfEvents"); int nAbort = pythia.mode("Main:timesAllowErrors"); // Histogram particle spectra. Hist eGamma("energy spectrum of photons", 100, 0., 250.); Hist eE( "energy spectrum of e+ and e-", 100, 0., 250.); Hist eP( "energy spectrum of p and pbar", 100, 0., 250.); Hist eNu( "energy spectrum of neutrinos", 100, 0., 250.); Hist eRest( "energy spectrum of rest particles", 100, 0., 250.); // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if many failures. if (!pythia.next()) { if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Loop over all particles and analyze the final-state ones. for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].isFinal()) { int idAbs = pythia.event[i].idAbs(); double eI = pythia.event[i].e(); if (idAbs == 22) eGamma.fill(eI); else if (idAbs == 11) eE.fill(eI); else if (idAbs == 2212) eP.fill(eI); else if (idAbs == 12 || idAbs == 14 || idAbs == 16) eNu.fill(eI); else { eRest.fill(eI); cout << " Error: stable id = " << pythia.event[i].id() << endl; } } // End of event loop. } // Final statistics and histograms. pythia.stat(); cout << eGamma << eE << eP << eNu << eRest; // Done. delete sigma1GenRes; return 0; } pythia8-8.1.80.orig/examples/main14.cc0000644000175000017500000001673712217346164015573 0ustar sunsun// main14.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Comparison with some PYTHIA 6.413 cross sections process by process. // Several processes have been left out to keep reasonable execution time. // Some processes are not handled absolutely identically, so minor // systematic differences may occur in addition to the statistical ones. // (For some MSSM Higgs processes 6.413 has been modified to use // running quark masses in loops, like 8.1, to allow proper comparison.) // Subruns 0 - 5 : QCD jets // 6 - 10 : prompt photons. // 11 - 12 : t-channel gamma/Z/W exchange. // 13 - 23 : gamma*/Z^0/W^+-, singly, in pairs or with parton // 24 - 25 : onia. // 26 - 30 : top. // 31 - 40 : Standard Model Higgs. // 41 - 45 : MSSM Higgses (trivial couplings). // 46 - 47 : Z' and W' // 48 - 51 : Left-right-symmetric scenario. // 52 - 52 : Leptoquark. // 53 - 55 : Excited fermions (compositeness). // 56 - 56 : excited Graviton (RS extra dimensions). #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // First and last process to test: can run from 0 through 40. int iFirst = 0; int iLast = 56; // Statistics. Pythia6 run was with 10000, so no point to use more. int nEvent = 10000; // Normally one subprocess word per subrun, but exceptions exist. int nSub[100]; for (int i = 0; i < 100; ++i) nSub[i] = 1; nSub[1] = 3; nSub[5] = 3; // Starting positions in subprocess words list, recursively defined. int iBeg[101] = { 0 }; for (int i = 0; i < 100; ++i) iBeg[i + 1] = iBeg[i] + nSub[i]; // List of subprocess words. string processes[61] = { "HardQCD:gg2gg", "HardQCD:gg2qqbar", "HardQCD:gg2ccbar", "HardQCD:gg2bbbar","HardQCD:qg2qg" , "HardQCD:qq2qq", "HardQCD:qqbar2gg", "HardQCD:qqbar2qqbarNew", "HardQCD:qqbar2ccbar", "HardQCD:qqbar2bbbar", "PromptPhoton:qg2qgamma", "PromptPhoton:qqbar2ggamma", "PromptPhoton:gg2ggamma", "PromptPhoton:ffbar2gammagamma", "PromptPhoton:gg2gammagamma", "WeakBosonExchange:ff2ff(t:gmZ)", "WeakBosonExchange:ff2ff(t:W)", "WeakSingleBoson:ffbar2gmZ", "WeakSingleBoson:ffbar2W", "WeakDoubleBoson:ffbar2gmZgmZ", "WeakDoubleBoson:ffbar2ZW", "WeakDoubleBoson:ffbar2WW", "WeakBosonAndParton:qqbar2gmZg", "WeakBosonAndParton:qg2gmZq", "WeakBosonAndParton:ffbar2gmZgm", "WeakBosonAndParton:qqbar2Wg", "WeakBosonAndParton:qg2Wq", "WeakBosonAndParton:ffbar2Wgm", "Charmonium:all", "Bottomonium:all", "Top:gg2ttbar", "Top:qqbar2ttbar", "Top:qq2tq(t:W)", "Top:ffbar2ttbar(s:gmZ)", "Top:ffbar2tqbar(s:W)", "HiggsSM:ffbar2H", "HiggsSM:gg2H", "HiggsSM:ffbar2HZ", "HiggsSM:ffbar2HW", "HiggsSM:ff2Hff(t:ZZ)", "HiggsSM:ff2Hff(t:WW)", "HiggsSM:qg2Hq", "HiggsSM:gg2Hg(l:t)", "HiggsSM:qg2Hq(l:t)", "HiggsSM:qqbar2Hg(l:t)", "HiggsBSM:allH1", "HiggsBSM:allH2", "HiggsBSM:allA3", "HiggsBSM:allH+-", "HiggsBSM:allHpair", "NewGaugeBoson:ffbar2gmZZprime", "NewGaugeBoson:ffbar2Wprime", "LeftRightSymmmetry:ffbar2ZR", "LeftRightSymmmetry:ffbar2WR", "LeftRightSymmmetry:ffbar2HLHL", "LeftRightSymmmetry:ffbar2HRHR", "LeptoQuark:all", "ExcitedFermion:dg2dStar", "ExcitedFermion:qq2dStarq", "ExcitedFermion:qqbar2eStare", "ExtraDimensionsG*:all" }; // List of cross sections from Pythia6. double sigma6[57] = { 4.960e-01, 1.627e-02, 2.790e-01, 2.800e-02, 3.310e-04, 3.653e-04, 1.697e-04, 1.163e-05, 1.065e-07, 8.259e-08, 8.237e-08, 2.544e-05, 5.321e-06, 5.571e-05, 1.621e-04, 9.039e-09, 2.247e-08, 5.893e-08, 3.781e-06, 1.078e-05, 4.551e-08, 1.025e-05, 3.208e-05, 5.435e-08, 1.038e-04, 3.929e-05, 4.155e-07, 6.685e-08, 1.898e-07, 4.240e-10, 7.142e-09, 1.547e-10, 7.064e-09, 1.316e-10, 2.332e-10, 5.105e-10, 1.316e-09, 4.462e-11, 5.557e-09, 1.966e-09, 8.725e-12, 2.450e-08, 5.839e-09, 1.687e-08, 8.950e-11, 4.188e-11, 1.980e-07, 4.551e-07, 6.005e-09, 1.102e-07, 7.784e-11, 3.488e-11, 6.006e-08, 3.235e-06, 1.689e-05, 5.986e-07, 3.241e-10 }; // Generator. Pythia pythia; // Standard set of masses for comparison with Fortran code. pythia.readString("5:m0 = 4.2"); pythia.readString("6:m0 = 175."); pythia.readString("23:m0 = 91.2"); pythia.readString("24:m0 = 80."); // Same kinematics cuts as Fortran code. pythia.readString("PhaseSpace:pTHatMin = 20."); pythia.readString("6:mMin = 20."); pythia.readString("23:mMin = 20."); pythia.readString("24:mMin = 20."); pythia.readString("25:mMin = 20."); pythia.readString("32:mMin = 400."); pythia.readString("34:mMin = 400."); pythia.readString("42:mMin = 50."); pythia.readString("5000039:mMin = 50."); // Also same renormalization and factorization scale. pythia.readString("SigmaProcess:renormScale2 = 3"); pythia.readString("SigmaProcess:factorScale2 = 3"); // Switch off unnecessary parts. pythia.readString("PartonLevel:all = off"); pythia.readString("ProcessLevel:resonanceDecays = off"); // No printing of settings, particle data or events. pythia.readString("Init:showProcesses = off"); pythia.readString("Init:showChangedSettings = off"); pythia.readString("Init:showChangedParticleData = off"); pythia.readString("Next:numberCount = 0"); pythia.readString("Next:numberShowInfo = 0"); pythia.readString("Next:numberShowProcess = 0"); pythia.readString("Next:numberShowEvent = 0"); // Debug: show information on cross section maximum and violation. //pythia.readString("PhaseSpace:showSearch = on"); //pythia.readString("PhaseSpace:showViolation = on"); // Loop over processes. for (int iProc = iFirst; iProc <= iLast; ++iProc) { cout << "\n Begin subrun number " << iProc << " : "; // Switch off previous process(es) and switch on new one(s). if (iProc > iFirst) for (int i = iBeg[iProc - 1]; i < iBeg[iProc]; ++i) pythia.readString( processes[i] + " = off" ); for (int i = iBeg[iProc]; i < iBeg[iProc + 1]; ++i) { pythia.readString( processes[i] + " = on" ); if (i > iBeg[iProc]) cout << " + "; cout << processes[i]; } cout << endl; // Switch between SM and MSSM Higgs scenario. if (iProc <= 40) { pythia.readString("Higgs:useBSM = off"); pythia.readString("25:m0 = 200."); } else { pythia.readString("Higgs:useBSM = on"); pythia.readString("25:m0 = 115."); pythia.readString("35:m0 = 300."); pythia.readString("36:m0 = 300."); pythia.readString("37:m0 = 320."); // With default option Higgs:clipWings = on need to reset mass range. pythia.readString("25:mMin = 50."); pythia.readString("25:mMax = 0."); } // Initialize for LHC. pythia.readString("Beams:eCM = 14000."); pythia.init(); // Debug: show initialized resonance data first time around. //if (iProc == iFirst) pythia.particleData.listChanged(true); // Generate events to get cross section statistics. for (int iEvent = 0; iEvent < nEvent; ++iEvent) pythia.next(); // Show statistics. //pythia.stat(); double sigma = pythia.info.sigmaGen(); cout << " Cross section is " << scientific << setprecision(3) << sigma << " and in Pythia6 was " << sigma6[iProc] << ",\n i.e. now is factor >>> " << fixed << sigma / sigma6[iProc] << " <<< different" <flag("JetMatching:setMad",false); if (!AlpgenHooks::initAfterBeams()) return false; if (!JetMatchingMadgraph::initAfterBeams()) return false; return true; } // Process level vetos. virtual bool canVetoProcessLevel() { return JetMatchingMadgraph::canVetoProcessLevel(); } virtual bool doVetoProcessLevel(Event& proc) { return JetMatchingMadgraph::doVetoProcessLevel(proc); } // Parton level vetos (before beam remnants and resonance decays). virtual bool canVetoPartonLevelEarly() { return JetMatchingMadgraph::canVetoPartonLevelEarly(); } virtual bool doVetoPartonLevelEarly(const Event& proc) { return JetMatchingMadgraph::doVetoPartonLevelEarly(proc); } }; //========================================================================== class CombineMatchingInput { public: // Constructor and destructor. CombineMatchingInput() {} ~CombineMatchingInput() {} // Return a hook relevant for combination of input and matching. UserHooks* getHook(Pythia& pythia) { // Find input source and matching scheme. bool isAlpgenFile = ( pythia.word("Alpgen:file") != "void" ); int scheme = pythia.mode("JetMatching:scheme"); // Return relevant UserHooks. if (isAlpgenFile) { if (scheme == 2) return new JetMatchingAlpgenInputAlpgen(pythia); if (scheme == 1) return new JetMatchingMadgraphInputAlpgen(pythia); } else { if (scheme == 2) return new JetMatchingAlpgen(); if (scheme == 1) return new JetMatchingMadgraph(); } // If fail then abort message and return VOID. pythia.info.errorMsg("Abort from CombinedInputMatching::getHook: " "settings unavailable"); return NULL; } }; //========================================================================== #endif // Pythia8_CombineMatchingInput_H pythia8-8.1.80.orig/examples/main82.cc0000644000175000017500000002533612217346167015576 0ustar sunsun// main82.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This program is written by Stefan Prestel. // It illustrates how to do CKKW-L merging, // see the Matrix Element Merging page in the online manual. #include "Pythia8/Pythia.h" using namespace Pythia8; // Functions for histogramming #include "fastjet/PseudoJet.hh" #include "fastjet/ClusterSequence.hh" #include "fastjet/CDFMidPointPlugin.hh" #include "fastjet/CDFJetCluPlugin.hh" #include "fastjet/D0RunIIConePlugin.hh" //========================================================================== // Find the Durham kT separation of the clustering from // nJetMin --> nJetMin-1 jets in te input event double pTfirstJet( const Event& event, int nJetMin, double Rparam) { double yPartonMax = 4.; // Fastjet analysis - select algorithm and parameters fastjet::Strategy strategy = fastjet::Best; fastjet::RecombinationScheme recombScheme = fastjet::E_scheme; fastjet::JetDefinition *jetDef = NULL; // For hadronic collision, use hadronic Durham kT measure if(event[3].colType() != 0 || event[4].colType() != 0) jetDef = new fastjet::JetDefinition(fastjet::kt_algorithm, Rparam, recombScheme, strategy); // For e+e- collision, use e+e- Durham kT measure else jetDef = new fastjet::JetDefinition(fastjet::ee_kt_algorithm, recombScheme, strategy); // Fastjet input std::vector fjInputs; // Reset Fastjet input fjInputs.resize(0); // Loop over event record to decide what to pass to FastJet for (int i = 0; i < event.size(); ++i) { // (Final state && coloured+photons) only! if ( !event[i].isFinal() || event[i].isLepton() || event[i].id() == 23 || abs(event[i].id()) == 24 || abs(event[i].y()) > yPartonMax) continue; // Store as input to Fastjet fjInputs.push_back( fastjet::PseudoJet (event[i].px(), event[i].py(), event[i].pz(),event[i].e() ) ); } // Do nothing for empty input if (int(fjInputs.size()) == 0) { delete jetDef; return 0.0; } // Run Fastjet algorithm fastjet::ClusterSequence clustSeq(fjInputs, *jetDef); // Extract kT of first clustering double pTFirst = sqrt(clustSeq.exclusive_dmerge_max(nJetMin-1)); delete jetDef; // Return kT return pTFirst; } //========================================================================== // Class for user interaction with the merging class MyMergingHooks : public MergingHooks { private: public: // Default constructor MyMergingHooks(); // Destructor ~MyMergingHooks(); // Functional definition of the merging scale virtual double tmsDefinition( const Event& event); // Helper function for tms definition double myKTdurham(const Particle& RadAfterBranch, const Particle& EmtAfterBranch, int Type, double D ); }; //-------------------------------------------------------------------------- // Constructor MyMergingHooks::MyMergingHooks() {} // Destructor MyMergingHooks::~MyMergingHooks() {} //-------------------------------------------------------------------------- // Definition of the merging scale double MyMergingHooks::tmsDefinition( const Event& event){ // Cut only on QCD partons! // Count particle types int nFinalColoured = 0; int nFinalNow =0; for( int i=0; i < event.size(); ++i) { if(event[i].isFinal()){ if(event[i].id() != 23 && abs(event[i].id()) != 24) nFinalNow++; if( event[i].colType() != 0) nFinalColoured++; } } // Use MergingHooks in-built functions to get information on the hard process int nLeptons = nHardOutLeptons(); int nQuarks = nHardOutPartons(); int nResNow = nResInCurrent(); // Check if photons, electrons etc. have been produced. If so, do not veto if(nFinalNow - ( (nLeptons+nQuarks)/2 - nResNow)*2 != nFinalColoured){ // Sometimes, Pythia detaches the decay products even though no // resonance was put into the LHE file, to catch this, add another // if statement if(nFinalNow != nFinalColoured) return 0.; } // Check that one parton has been produced. If not (e.g. in MPI), do not veto int nMPI = infoPtr->nMPI(); if(nMPI > 1) return 0.; // Declare kT algorithm parameters double Dparam = 0.4; int kTtype = -1; // Declare final parton vector vector FinalPartPos; FinalPartPos.clear(); // Search event record for final state partons for (int i=0; i < event.size(); ++i) if(event[i].isFinal() && event[i].colType() != 0) FinalPartPos.push_back(i); // Find minimal Durham kT in event, using own function: Check // definition of separation int type = (event[3].colType() == 0 && event[4].colType() == 0) ? 1 : kTtype; // Find minimal kT double ktmin = event[0].e(); for(int i=0; i < int(FinalPartPos.size()); ++i){ double kt12 = ktmin; // Compute separation to the beam axis for hadronic collisions if(type == -1 || type == -2) { double temp = event[FinalPartPos[i]].pT(); kt12 = min(kt12, temp); } // Compute separation to other final state jets for(int j=i+1; j < int(FinalPartPos.size()); ++j) { double temp = kTdurham( event[FinalPartPos[i]], event[FinalPartPos[j]], type, Dparam); kt12 = min(kt12, temp); } // Keep the minimal Durham separation ktmin = min(ktmin,kt12); } // Return minimal Durham kT return ktmin; } //-------------------------------------------------------------------------- // Function to compute durham y separation from Particle input double MyMergingHooks::myKTdurham(const Particle& RadAfterBranch, const Particle& EmtAfterBranch, int Type, double D ){ // Declare return variable double ktdur; // Save 4-momenta of final state particles Vec4 jet1 = RadAfterBranch.p(); Vec4 jet2 = EmtAfterBranch.p(); if( Type == 1) { // Get angle between jets for e+e- collisions, make sure that // -1 <= cos(theta) <= 1 double costh; if (jet1.pAbs()*jet2.pAbs() <=0.) costh = 1.; else { costh = costheta(jet1,jet2); } // Calculate kt durham separation between jets for e+e- collisions ktdur = 2.0*min( pow(jet1.e(),2) , (pow(jet2.e(),2)) )*(1.0 - costh); } else if( Type == -1 ){ // Get delta_eta and cosh(Delta_eta) for hadronic collisions double eta1 = 0.5*log( (jet1.e() + jet1.pz()) / (jet1.e() - jet1.pz()) ); double eta2 = 0.5*log( (jet2.e() + jet2.pz()) / (jet2.e() - jet2.pz()) ); // Get delta_phi and cos(Delta_phi) for hadronic collisions double pt1 = sqrt( pow(jet1.px(),2) + pow(jet1.py(),2) ); double pt2 = sqrt( pow(jet2.px(),2) + pow(jet2.py(),2) ); double cosdPhi = ( jet1.px()*jet2.px() + jet1.py()*jet2.py() ) / (pt1*pt2); double dPhi = acos( cosdPhi ); // Calculate kT durham like fastjet ktdur = min( pow(pt1,2),pow(pt2,2) ) * ( pow(eta1-eta2,2) + pow(dPhi,2) ) / pow(D,2); } else if( Type == -2 ){ // Get delta_eta and cosh(Delta_eta) for hadronic collisions double eta1 = 0.5*log( (jet1.e() + jet1.pz()) / (jet1.e() - jet1.pz()) ); double eta2 = 0.5*log( (jet2.e() + jet2.pz()) / (jet2.e() - jet2.pz()) ); double coshdEta = cosh( eta1 - eta2 ); // Get delta_phi and cos(Delta_phi) for hadronic collisions double pt1 = sqrt( pow(jet1.px(),2) + pow(jet1.py(),2) ); double pt2 = sqrt( pow(jet2.px(),2) + pow(jet2.py(),2) ); double cosdPhi = ( jet1.px()*jet2.px() + jet1.py()*jet2.py() ) / (pt1*pt2); // Calculate kT durham separation "SHERPA-like" ktdur = 2.0*min( pow(pt1,2),pow(pt2,2) ) * ( coshdEta - cosdPhi ) / pow(D,2); } else { ktdur = 0.0; } // Return kT return sqrt(ktdur); } //========================================================================== // Example main programm to illustrate merging int main( int argc, char* argv[] ){ // Check that correct number of command-line arguments if (argc != 4) { cerr << " Unexpected number of command-line arguments. \n You are" << " expected to provide the arguments \n" << " 1. Input file for settings \n" << " 2. Full name of the input LHE file (with path) \n" << " 3. Path for output histogram files \n" << " Program stopped. " << endl; return 1; } Pythia pythia; // Input parameters: // 1. Input file for settings // 2. Path to input LHE file // 3. OUtput histogram path pythia.readFile(argv[1]); string iPath = string(argv[2]); string oPath = string(argv[3]); // Number of events int nEvent = pythia.mode("Main:numberOfEvents"); // Construct user inut for merging MergingHooks* myMergingHooks = new MyMergingHooks(); pythia.setMergingHooksPtr( myMergingHooks ); // For ISR regularisation off pythia.settings.forceParm("SpaceShower:pT0Ref",0.); // Declare histograms Hist histPTFirst("pT of first jet",100,0.,100.); Hist histPTSecond("pT of second jet",100,0.,100.); // Read in ME configurations pythia.init(iPath,false); if(pythia.flag("Main:showChangedSettings")) { pythia.settings.listChanged(); } // Start generation loop for( int iEvent=0; iEvent typeIdx[3]; set typeSet[3]; // Momenta output of jet algorithm (to provide same output regardless of // the selected jet algorithm) vector jetMomenta; // CellJet specific int nEta, nPhi; double eTseed, eTthreshold; // Merging procedure parameters int jetAllow, jetMatch, exclusiveMode; double coneMatchLight, coneRadiusHeavy, coneMatchHeavy; bool exclusive; // Store the minimum eT/pT of matched light jets double eTpTlightMin; }; //========================================================================== // Declaration of main UserHooks class to perform Alpgen matching. class JetMatchingAlpgen : virtual public JetMatching { public: // Constructor and destructor JetMatchingAlpgen() { } ~JetMatchingAlpgen() { } // Initialisation bool initAfterBeams(); private: // Different steps of the matching algorithm. void sortIncomingProcess(const Event &); void jetAlgorithmInput(const Event &, int); void runJetAlgorithm(); bool matchPartonsToJets(int); int matchPartonsToJetsLight(); int matchPartonsToJetsHeavy(); // Sorting utility void sortTypeIdx(vector < int > &vecIn); // Constants static const double GHOSTENERGY, ZEROTHRESHOLD; }; //========================================================================== // Declaration of main UserHooks class to perform Madgraph matching. class JetMatchingMadgraph : virtual public JetMatching { public: // Constructor and destructor JetMatchingMadgraph() { } ~JetMatchingMadgraph() { } // Initialisation bool initAfterBeams(); protected: // Different steps of the matching algorithm. void sortIncomingProcess(const Event &); void jetAlgorithmInput(const Event &, int); void runJetAlgorithm(); bool matchPartonsToJets(int); int matchPartonsToJetsLight(); int matchPartonsToJetsHeavy(); // Variables. int nQmatch; double qCut, qCutSq, clFact; }; //========================================================================== // Main implementation of JetMatching class. // This may be split out to a separate C++ file if desired, // but currently included here for ease of use. //-------------------------------------------------------------------------- // Constants to be changed for debug printout or extra checks. const bool JetMatching::MATCHINGDEBUG = false; const bool JetMatching::MATCHINGCHECK = false; //-------------------------------------------------------------------------- // Early parton level veto (before beam remnants and resonance showers) bool JetMatching::doVetoPartonLevelEarly(const Event& event) { // 1) Sort the original incoming process. After this step is performed, // the following assignments have been made: // eventProcessOrig - the original incoming process // eventProcess - the final-state of the incoming process with // resonance decays removed (and resonances // themselves now with positive status code) // typeIdx[0/1/2] - Indices into 'eventProcess' of // light jets/heavy jets/other // typeSet[0/1/2] - Indices into 'event' of light jets/heavy jets/other // workEvent - partons from the hardest subsystem + ISR + FSR only sortIncomingProcess(event); // Debug printout. if (MATCHINGDEBUG) { // Begin cout << endl << "-------- Begin Madgraph Debug --------" << endl; // Original incoming process cout << endl << "Original incoming process:"; eventProcessOrig.list(); // Final-state of original incoming process cout << endl << "Final-state incoming process:"; eventProcess.list(); // List categories of sorted particles for (size_t i = 0; i < typeIdx[0].size(); i++) cout << ((i == 0) ? "Light jets: " : ", ") << setw(3) << typeIdx[0][i]; if( typeIdx[0].size()== 0 ) cout << "Light jets: None"; for (size_t i = 0; i < typeIdx[1].size(); i++) cout << ((i == 0) ? "\nHeavy jets: " : ", ") << setw(3) << typeIdx[1][i]; for (size_t i = 0; i < typeIdx[2].size(); i++) cout << ((i == 0) ? "\nOther: " : ", ") << setw(3) << typeIdx[2][i]; // Full event at this stage cout << endl << endl << "Event:"; event.list(); // Work event (partons from hardest subsystem + ISR + FSR) cout << endl << "Work event:"; workEvent.list(); } // 2) Light/heavy jets: iType = 0 (light jets), 1 (heavy jets) int iTypeEnd = (typeIdx[1].empty()) ? 1 : 2; for (int iType = 0; iType < iTypeEnd; iType++) { // 2a) Find particles which will be passed from the jet algorithm. // Input from 'workEvent' and output in 'workEventJet'. jetAlgorithmInput(event, iType); // Debug printout. if (MATCHINGDEBUG) { // Jet algorithm event cout << endl << "Jet algorithm event (iType = " << iType << "):"; workEventJet.list(); } // 2b) Run jet algorithm on 'workEventJet'. // Output is stored in jetMomenta. runJetAlgorithm(); // 2c) Match partons to jets and decide if veto is necessary if (matchPartonsToJets(iType) == true) { // Debug printout. if (MATCHINGDEBUG) { cout << endl << "Event vetoed" << endl << "---------- End MLM Debug ----------" << endl; } return true; } } // Debug printout. if (MATCHINGDEBUG) { cout << endl << "Event accepted" << endl << "---------- End MLM Debug ----------" << endl; } // If we reached here, then no veto return false; } //========================================================================== // Main implementation of Alpgen UserHooks class. // This may be split out to a separate C++ file if desired, // but currently included here for ease of use. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // The energy of ghost particles. For technical reasons, this cannot be // set arbitrarily low, see 'Particle::TINY' in 'Event.cc' for details. const double JetMatchingAlpgen::GHOSTENERGY = 1e-15; // A zero threshold value for double comparisons. const double JetMatchingAlpgen::ZEROTHRESHOLD = 1e-10; //-------------------------------------------------------------------------- // Function to sort typeIdx vectors into descending eT/pT order. // Uses a selection sort, as number of partons generally small // and so efficiency not a worry. void JetMatchingAlpgen::sortTypeIdx(vector < int > &vecIn) { for (size_t i = 0; i < vecIn.size(); i++) { size_t jMax = i; double vMax = (jetAlgorithm == 1) ? eventProcess[vecIn[i]].eT() : eventProcess[vecIn[i]].pT(); for (size_t j = i + 1; j < vecIn.size(); j++) { double vNow = (jetAlgorithm == 1) ? eventProcess[vecIn[j]].eT() : eventProcess[vecIn[j]].pT(); if (vNow > vMax) { vMax = vNow; jMax = j; } } if (jMax != i) swap(vecIn[i], vecIn[jMax]); } } //-------------------------------------------------------------------------- // Initialisation routine automatically called from Pythia::init(). // Setup all parts needed for the merging. bool JetMatchingAlpgen::initAfterBeams() { // Read in parameters doMerge = settingsPtr->flag("JetMatching:merge"); jetAlgorithm = settingsPtr->mode("JetMatching:jetAlgorithm"); nJet = settingsPtr->mode("JetMatching:nJet"); nJetMax = settingsPtr->mode("JetMatching:nJetMax"); eTjetMin = settingsPtr->parm("JetMatching:eTjetMin"); coneRadius = settingsPtr->parm("JetMatching:coneRadius"); etaJetMax = settingsPtr->parm("JetMatching:etaJetMax"); // Use etaJetMax + coneRadius in input to jet algorithms etaJetMaxAlgo = etaJetMax + coneRadius; // CellJet specific nEta = settingsPtr->mode("JetMatching:nEta"); nPhi = settingsPtr->mode("JetMatching:nPhi"); eTseed = settingsPtr->parm("JetMatching:eTseed"); eTthreshold = settingsPtr->parm("JetMatching:eTthreshold"); // SlowJet specific slowJetPower = settingsPtr->mode("JetMatching:slowJetPower"); coneMatchLight = settingsPtr->parm("JetMatching:coneMatchLight"); coneRadiusHeavy = settingsPtr->parm("JetMatching:coneRadiusHeavy"); if (coneRadiusHeavy < 0.) coneRadiusHeavy = coneRadius; coneMatchHeavy = settingsPtr->parm("JetMatching:coneMatchHeavy"); // Matching procedure jetAllow = settingsPtr->mode("JetMatching:jetAllow"); jetMatch = settingsPtr->mode("JetMatching:jetMatch"); exclusiveMode = settingsPtr->mode("JetMatching:exclusive"); // If not merging, then done if (!doMerge) return true; // Exclusive mode; if set to 2, then set based on nJet/nJetMax if (exclusiveMode == 2) { // No nJet or nJetMax, so default to exclusive mode if (nJet < 0 || nJetMax < 0) { infoPtr->errorMsg("Warning in JetMatchingAlpgen:init: " "missing jet multiplicity information; running in exclusive mode"); exclusive = true; // Inclusive if nJet == nJetMax, exclusive otherwise } else { exclusive = (nJet == nJetMax) ? false : true; } // Otherwise, just set as given } else { exclusive = (exclusiveMode == 0) ? false : true; } // Initialise chosen jet algorithm. CellJet. if (jetAlgorithm == 1) { // Extra options for CellJet. nSel = 1 means that all final-state // particles are taken and we retain control of what to select. // smear/resolution/upperCut are not used and are set to default values. int nSel = 2, smear = 0; double resolution = 0.5, upperCut = 2.; cellJet = new CellJet(etaJetMaxAlgo, nEta, nPhi, nSel, smear, resolution, upperCut, eTthreshold); // SlowJet } else if (jetAlgorithm == 2) { slowJet = new SlowJet(slowJetPower, coneRadius, eTjetMin, etaJetMaxAlgo); } // Check the jetMatch parameter; option 2 only works with SlowJet if (jetAlgorithm == 1 && jetMatch == 2) { infoPtr->errorMsg("Warning in JetMatchingAlpgen:init: " "jetMatch = 2 only valid with SlowJet algorithm. " "Reverting to jetMatch = 1"); jetMatch = 1; } // Setup local event records eventProcessOrig.init("(eventProcessOrig)", particleDataPtr); eventProcess.init("(eventProcess)", particleDataPtr); workEventJet.init("(workEventJet)", particleDataPtr); // Print information string jetStr = (jetAlgorithm == 1) ? "CellJet" : (slowJetPower == -1) ? "anti-kT" : (slowJetPower == 0) ? "C/A" : (slowJetPower == 1) ? "kT" : "unknown"; string modeStr = (exclusive) ? "exclusive" : "inclusive"; stringstream nJetStr, nJetMaxStr; if (nJet >= 0) nJetStr << nJet; else nJetStr << "unknown"; if (nJetMax >= 0) nJetMaxStr << nJetMax; else nJetMaxStr << "unknown"; cout << endl << " *------- MLM matching parameters -------*" << endl << " | nJet | " << setw(14) << nJetStr.str() << " |" << endl << " | nJetMax | " << setw(14) << nJetMaxStr.str() << " |" << endl << " | Jet algorithm | " << setw(14) << jetStr << " |" << endl << " | eTjetMin | " << setw(14) << eTjetMin << " |" << endl << " | coneRadius | " << setw(14) << coneRadius << " |" << endl << " | etaJetMax | " << setw(14) << etaJetMax << " |" << endl << " | jetAllow | " << setw(14) << jetAllow << " |" << endl << " | jetMatch | " << setw(14) << jetMatch << " |" << endl << " | coneMatchLight | " << setw(14) << coneMatchLight << " |" << endl << " | coneRadiusHeavy | " << setw(14) << coneRadiusHeavy << " |" << endl << " | coneMatchHeavy | " << setw(14) << coneMatchHeavy << " |" << endl << " | Mode | " << setw(14) << modeStr << " |" << endl << " *-----------------------------------------*" << endl; return true; } //-------------------------------------------------------------------------- // Step (1): sort the incoming particles void JetMatchingAlpgen::sortIncomingProcess(const Event &event) { // Remove resonance decays from original process and keep only final // state. Resonances will have positive status code after this step. omitResonanceDecays(eventProcessOrig, true); eventProcess = workEvent; // Sort original process final state into light/heavy jets and 'other'. // Criteria: // 1 <= ID <= 5 and massless, or ID == 21 --> light jet (typeIdx[0]) // 4 <= ID <= 6 and massive --> heavy jet (typeIdx[1]) // All else --> other (typeIdx[2]) // Note that 'typeIdx' stores indices into 'eventProcess' (after resonance // decays are omitted), while 'typeSet' stores indices into the original // process record, 'eventProcessOrig', but these indices are also valid // in 'event'. for (int i = 0; i < 3; i++) { typeIdx[i].clear(); typeSet[i].clear(); } for (int i = 0; i < eventProcess.size(); i++) { // Ignore nonfinal and default to 'other' if (!eventProcess[i].isFinal()) continue; int idx = 2; // Light jets if (eventProcess[i].id() == ID_GLUON || (eventProcess[i].idAbs() <= ID_BOT && abs(eventProcess[i].m()) < ZEROTHRESHOLD)) idx = 0; // Heavy jets else if (eventProcess[i].idAbs() >= ID_CHARM && eventProcess[i].idAbs() <= ID_TOP) idx = 1; // Store typeIdx[idx].push_back(i); typeSet[idx].insert(eventProcess[i].daughter1()); } // Extract partons from hardest subsystem + ISR + FSR only into // workEvent. Note no resonance showers or MPIs. subEvent(event); } //-------------------------------------------------------------------------- // Step (2a): pick which particles to pass to the jet algorithm void JetMatchingAlpgen::jetAlgorithmInput(const Event &event, int iType) { // Take input from 'workEvent' and put output in 'workEventJet' workEventJet = workEvent; // Loop over particles and decide what to pass to the jet algorithm for (int i = 0; i < workEventJet.size(); ++i) { if (!workEventJet[i].isFinal()) continue; // jetAllow option to disallow certain particle types if (jetAllow == 1) { // Original AG+Py6 algorithm explicitly excludes tops, // leptons and photons. int id = workEventJet[i].idAbs(); if ( (id >= ID_LEPMIN && id <= ID_LEPMAX) || id == ID_TOP || id == ID_PHOTON) { workEventJet[i].statusNeg(); continue; } } // Get the index of this particle in original event int idx = workEventJet[i].daughter1(); // Start with particle idx, and afterwards track mothers while (true) { // Light jets if (iType == 0) { // Do not include if originates from heavy jet or 'other' if (typeSet[1].find(idx) != typeSet[1].end() || typeSet[2].find(idx) != typeSet[2].end()) { workEventJet[i].statusNeg(); break; } // Made it to start of event record so done if (idx == 0) break; // Otherwise next mother and continue idx = event[idx].mother1(); // Heavy jets } else if (iType == 1) { // Only include if originates from heavy jet if (typeSet[1].find(idx) != typeSet[1].end()) break; // Made it to start of event record with no heavy jet mother, // so DO NOT include particle if (idx == 0) { workEventJet[i].statusNeg(); break; } // Otherwise next mother and continue idx = event[idx].mother1(); } // if (iType) } // while (true) } // for (i) // For jetMatch = 2, insert ghost particles corresponding to // each hard parton in the original process if (jetMatch == 2) { for (int i = 0; i < int(typeIdx[iType].size()); i++) { // Get y/phi of the parton Vec4 pIn = eventProcess[typeIdx[iType][i]].p(); double y = pIn.rap(); double phi = pIn.phi(); // Create a ghost particle and add to the workEventJet double e = GHOSTENERGY; double e2y = exp(2. * y); double pz = e * (e2y - 1.) / (e2y + 1.); double pt = sqrt(e*e - pz*pz); double px = pt * cos(phi); double py = pt * sin(phi); workEventJet.append( ID_GLUON, 99, 0, 0, 0, 0, 0, 0, px, py, pz, e); // Extra check on reconstructed y/phi values. If many warnings // of this type, GHOSTENERGY may be set too low. if (MATCHINGCHECK) { int lastIdx = workEventJet.size() - 1; if (abs(y - workEventJet[lastIdx].y()) > ZEROTHRESHOLD || abs(phi - workEventJet[lastIdx].phi()) > ZEROTHRESHOLD) infoPtr->errorMsg("Warning in JetMatchingAlpgen:jetAlgorithmInput: " "ghost particle y/phi mismatch"); } } // for (i) } // if (jetMatch == 2) } //-------------------------------------------------------------------------- // Step (2b): run jet algorithm and provide common output void JetMatchingAlpgen::runJetAlgorithm() { // Run the jet clustering algorithm if (jetAlgorithm == 1) cellJet->analyze(workEventJet, eTjetMin, coneRadius, eTseed); else slowJet->analyze(workEventJet); // Extract four-momenta of jets with |eta| < etaJetMax and // put into jetMomenta. Note that this is done backwards as // jets are removed with SlowJet. jetMomenta.clear(); int iJet = (jetAlgorithm == 1) ? cellJet->size() - 1: slowJet->sizeJet() - 1; for (int i = iJet; i > -1; i--) { Vec4 jetMom = (jetAlgorithm == 1) ? cellJet->pMassive(i) : slowJet->p(i); double eta = jetMom.eta(); if (abs(eta) > etaJetMax) { if (jetAlgorithm == 2) slowJet->removeJet(i); continue; } jetMomenta.push_back(jetMom); } // Reverse jetMomenta to restore eT/pT ordering reverse(jetMomenta.begin(), jetMomenta.end()); } //-------------------------------------------------------------------------- // Step (2c): veto decision (returning true vetoes the event) bool JetMatchingAlpgen::matchPartonsToJets(int iType) { // Use two different routines for light/heavy jets as // different veto conditions and for clarity if (iType == 0) return (matchPartonsToJetsLight() > 0); else return (matchPartonsToJetsHeavy() > 0); } //-------------------------------------------------------------------------- // Step(2c): light jets // Return codes are given indicating the reason for a veto. // Although not currently used, they are a useful debugging tool: // 0 = no veto // 1 = veto as number of jets less than number of partons // 2 = veto as exclusive mode and number of jets greater than // number of partons // 3 = veto as inclusive mode and there would be an extra jet // that is harder than any matched soft jet // 4 = veto as there is a parton which does not match a jet int JetMatchingAlpgen::matchPartonsToJetsLight() { // Always veto if number of jets is less than original number of jets if (jetMomenta.size() < typeIdx[0].size()) return LESS_JETS; // Veto if in exclusive mode and number of jets bigger than original if (exclusive && jetMomenta.size() > typeIdx[0].size()) return MORE_JETS; // Sort partons by eT/pT sortTypeIdx(typeIdx[0]); // Number of hard partons int nParton = typeIdx[0].size(); // Keep track of which jets have been assigned a hard parton vector < bool > jetAssigned; jetAssigned.assign(jetMomenta.size(), false); // Jet matching procedure: (1) deltaR between partons and jets if (jetMatch == 1) { // Loop over light hard partons and get 4-momentum for (int i = 0; i < nParton; i++) { Vec4 p1 = eventProcess[typeIdx[0][i]].p(); // Track which jet has the minimal dR measure with this parton int jMin = -1; double dRmin = 0.; // Loop over all jets (skipping those already assigned). for (int j = 0; j < int(jetMomenta.size()); j++) { if (jetAssigned[j]) continue; // DeltaR between parton/jet and store if minimum double dR = (jetAlgorithm == 1) ? REtaPhi(p1, jetMomenta[j]) : RRapPhi(p1, jetMomenta[j]); if (jMin < 0 || dR < dRmin) { dRmin = dR; jMin = j; } } // for (j) // Check for jet-parton match if (jMin >= 0 && dRmin < coneRadius * coneMatchLight) { // If the matched jet is not one of the nParton hardest jets, // the extra left over jet would be harder than some of the // matched jets. This is disallowed, so veto. if (jMin >= nParton) return HARD_JET; // Mark jet as assigned. jetAssigned[jMin] = true; // If no match, then event will be vetoed in all cases } else return UNMATCHED_PARTON; } // for (i) // Jet matching procedure: (2) ghost particles in SlowJet } else { // Loop over added 'ghost' particles and find if assigned to a jet for (int i = workEventJet.size() - nParton; i < workEventJet.size(); i++) { int jMin = slowJet->jetAssignment(i); // Veto if: // 1) not one of nParton hardest jets // 2) not assigned to a jet // 3) jet has already been assigned if (jMin >= nParton) return HARD_JET; if (jMin < 0 || jetAssigned[jMin]) return UNMATCHED_PARTON; // Mark jet as assigned jetAssigned[jMin] = true; } // for (i) } // if (jetMatch) // Minimal eT/pT (CellJet/SlowJet) of matched light jets. Needed // later for heavy jet vetos in inclusive mode. if (nParton > 0) eTpTlightMin = (jetAlgorithm == 1) ? jetMomenta[nParton - 1].eT() : jetMomenta[nParton - 1].pT(); else eTpTlightMin = -1.; // No veto return NONE; } //-------------------------------------------------------------------------- // Step(2c): heavy jets // Return codes are given indicating the reason for a veto. // Although not currently used, they are a useful debugging tool: // 0 = no veto as there are no extra jets present // 1 = veto as in exclusive mode and extra jets present // 2 = veto as in inclusive mode and extra jets were harder // than any matched light jet int JetMatchingAlpgen::matchPartonsToJetsHeavy() { // If there are no extra jets, then accept if (jetMomenta.empty()) return NONE; // Number of hard partons int nParton = typeIdx[1].size(); // Remove jets that are close to heavy quarks set < int > removeJets; // Jet matching procedure: (1) deltaR between partons and jets if (jetMatch == 1) { // Loop over heavy hard partons and get 4-momentum for (int i = 0; i < nParton; i++) { Vec4 p1 = eventProcess[typeIdx[1][i]].p(); // Loop over all jets, find dR and mark for removal if match for (int j = 0; j < int(jetMomenta.size()); j++) { double dR = (jetAlgorithm == 1) ? REtaPhi(p1, jetMomenta[j]) : RRapPhi(p1, jetMomenta[j]); if (dR < coneRadiusHeavy * coneMatchHeavy) removeJets.insert(j); } // for (j) } // for (i) // Jet matching procedure: (2) ghost particles in SlowJet } else { // Loop over added 'ghost' particles and if assigned to a jet // then mark this jet for removal for (int i = workEventJet.size() - nParton; i < workEventJet.size(); i++) { int jMin = slowJet->jetAssignment(i); if (jMin >= 0) removeJets.insert(jMin); } } // Remove jets (backwards order to not disturb indices) for (set < int >::reverse_iterator it = removeJets.rbegin(); it != removeJets.rend(); it++) jetMomenta.erase(jetMomenta.begin() + *it); // Handle case if there are still extra jets if (!jetMomenta.empty()) { // Exclusive mode, so immediate veto if (exclusive) return MORE_JETS; // Inclusive mode; extra jets must be softer than any matched light jet else if (eTpTlightMin >= 0.) for (size_t j = 0; j < jetMomenta.size(); j++) { // CellJet uses eT, SlowJet uses pT if ( (jetAlgorithm == 1 && jetMomenta[j].eT() > eTpTlightMin) || (jetAlgorithm == 2 && jetMomenta[j].pT() > eTpTlightMin) ) return HARD_JET; } } // if (!jetMomenta.empty()) // No extra jets were present so no veto return NONE; } //========================================================================== // Main implementation of Madgraph UserHooks class. // This may be split out to a separate C++ file if desired, // but currently included here for ease of use. //-------------------------------------------------------------------------- // Initialisation routine automatically called from Pythia::init(). // Setup all parts needed for the merging. bool JetMatchingMadgraph::initAfterBeams() { // Read in Madgraph specific configuration variables bool setMad = settingsPtr->flag("JetMatching:setMad"); // If Madgraph parameters are present, then parse in MadgraphPar object MadgraphPar par(infoPtr); string parStr = infoPtr->header("MGRunCard"); if (!parStr.empty()) { par.parse(parStr); par.printParams(); } // Set Madgraph merging parameters from the file if requested if (setMad) { if ( par.haveParam("xqcut") && par.haveParam("maxjetflavor") && par.haveParam("alpsfact") && par.haveParam("ickkw") ) { settingsPtr->flag("JetMatching:merge", par.getParam("ickkw")); settingsPtr->parm("JetMatching:qCut", par.getParam("xqcut")); settingsPtr->mode("JetMatching:nQmatch", par.getParamAsInt("maxjetflavor")); settingsPtr->parm("JetMatching:clFact", clFact = par.getParam("alpsfact")); if (par.getParamAsInt("ickkw") == 0) infoPtr->errorMsg("Error in JetMatchingMadgraph:init: " "Madgraph file parameters are not set for merging"); // Warn if setMad requested, but one or more parameters not present } else { infoPtr->errorMsg("Warning in JetMatchingMadgraph:init: " "Madgraph merging parameters not found"); if (!par.haveParam("xqcut")) infoPtr->errorMsg("Warning in " "JetMatchingMadgraph:init: No xqcut"); if (!par.haveParam("ickkw")) infoPtr->errorMsg("Warning in " "JetMatchingMadgraph:init: No ickkw"); if (!par.haveParam("maxjetflavor")) infoPtr->errorMsg("Warning in " "JetMatchingMadgraph:init: No maxjetflavor"); if (!par.haveParam("alpsfact")) infoPtr->errorMsg("Warning in " "JetMatchingMadgraph:init: No alpsfact"); } } // Read in Madgraph merging parameters doMerge = settingsPtr->flag("JetMatching:merge"); qCut = settingsPtr->parm("JetMatching:qCut"); nQmatch = settingsPtr->mode("JetMatching:nQmatch"); clFact = settingsPtr->parm("JetMatching:clFact"); // Read in jet algorithm parameters jetAlgorithm = settingsPtr->mode("JetMatching:jetAlgorithm"); nJetMax = settingsPtr->mode("JetMatching:nJetMax"); eTjetMin = settingsPtr->parm("JetMatching:eTjetMin"); coneRadius = settingsPtr->parm("JetMatching:coneRadius"); etaJetMax = settingsPtr->parm("JetMatching:etaJetMax"); slowJetPower = settingsPtr->mode("JetMatching:slowJetPower"); // Matching procedure jetAllow = settingsPtr->mode("JetMatching:jetAllow"); exclusiveMode = settingsPtr->mode("JetMatching:exclusive"); qCutSq = pow(qCut,2); etaJetMaxAlgo = etaJetMax; // If not merging, then done if (!doMerge) return true; // Exclusive mode; if set to 2, then set based on nJet/nJetMax if (exclusiveMode == 2) { // No nJet or nJetMax, so default to exclusive mode if (nJetMax < 0) { infoPtr->errorMsg("Warning in JetMatchingMadgraph:init: " "missing jet multiplicity information; running in exclusive mode"); exclusiveMode = 1; } } // Initialise chosen jet algorithm. // Currently, this only supports the kT-algorithm in SlowJet. // Use the QCD distance measure by default. jetAlgorithm = 2; slowJetPower = 1; slowJet = new SlowJet(slowJetPower, coneRadius, eTjetMin, etaJetMaxAlgo, 2, 2, NULL, false); // Setup local event records eventProcessOrig.init("(eventProcessOrig)", particleDataPtr); eventProcess.init("(eventProcess)", particleDataPtr); workEventJet.init("(workEventJet)", particleDataPtr); // Print information string jetStr = (jetAlgorithm == 1) ? "CellJet" : (slowJetPower == -1) ? "anti-kT" : (slowJetPower == 0) ? "C/A" : (slowJetPower == 1) ? "kT" : "unknown"; string modeStr = (exclusiveMode) ? "exclusive" : "inclusive"; cout << endl << " *----- Madgraph matching parameters -----*" << endl << " | qCut | " << setw(14) << qCut << " |" << endl << " | nQmatch | " << setw(14) << nQmatch << " |" << endl << " | clFact | " << setw(14) << clFact << " |" << endl << " | Jet algorithm | " << setw(14) << jetStr << " |" << endl << " | eTjetMin | " << setw(14) << eTjetMin << " |" << endl << " | etaJetMax | " << setw(14) << etaJetMax << " |" << endl << " | jetAllow | " << setw(14) << jetAllow << " |" << endl << " | Mode | " << setw(14) << modeStr << " |" << endl << " *-----------------------------------------*" << endl; return true; } //-------------------------------------------------------------------------- // Step (1): sort the incoming particles void JetMatchingMadgraph::sortIncomingProcess(const Event &event) { // Remove resonance decays from original process and keep only final // state. Resonances will have positive status code after this step. omitResonanceDecays(eventProcessOrig, true); eventProcess = workEvent; // Sort original process final state into light/heavy jets and 'other'. // Criteria: // 1 <= ID <= nQmatch, or ID == 21 --> light jet (typeIdx[0]) // nQMatch < ID --> heavy jet (typeIdx[1]) // All else --> other (typeIdx[2]) // Note that 'typeIdx' stores indices into 'eventProcess' (after resonance // decays are omitted), while 'typeSet' stores indices into the original // process record, 'eventProcessOrig', but these indices are also valid // in 'event'. for (int i = 0; i < 3; i++) { typeIdx[i].clear(); typeSet[i].clear(); } for (int i = 0; i < eventProcess.size(); i++) { // Ignore non-final state and default to 'other' if (!eventProcess[i].isFinal()) continue; int idx = 2; // Light jets: all gluons and quarks with id less than or equal to nQmatch if (eventProcess[i].id() == ID_GLUON || (eventProcess[i].idAbs() <= nQmatch) ) idx = 0; // Heavy jets: all quarks with id greater than nQmatch else if (eventProcess[i].idAbs() > nQmatch && eventProcess[i].idAbs() <= ID_TOP) idx = 1; // Store typeIdx[idx].push_back(i); typeSet[idx].insert(eventProcess[i].daughter1()); } // Exclusive mode; if set to 2, then set based on nJet/nJetMax if (exclusiveMode == 2) { // Inclusive if nJet == nJetMax, exclusive otherwise int nParton = typeIdx[0].size(); exclusive = (nParton == nJetMax) ? false : true; // Otherwise, just set as given } else { exclusive = (exclusiveMode == 0) ? false : true; } // Extract partons from hardest subsystem + ISR + FSR only into // workEvent. Note no resonance showers or MPIs. subEvent(event); } //-------------------------------------------------------------------------- // Step (2a): pick which particles to pass to the jet algorithm void JetMatchingMadgraph::jetAlgorithmInput(const Event &event, int iType) { // Take input from 'workEvent' and put output in 'workEventJet' workEventJet = workEvent; // Loop over particles and decide what to pass to the jet algorithm for (int i = 0; i < workEventJet.size(); ++i) { if (!workEventJet[i].isFinal()) continue; // jetAllow option to disallow certain particle types if (jetAllow == 1) { // Original AG+Py6 algorithm explicitly excludes tops, // leptons and photons. int id = workEventJet[i].idAbs(); if ((id >= ID_LEPMIN && id <= ID_LEPMAX) || id == ID_TOP || id == ID_PHOTON) { workEventJet[i].statusNeg(); continue; } } // Get the index of this particle in original event int idx = workEventJet[i].daughter1(); // Start with particle idx, and afterwards track mothers while (true) { // Light jets if (iType == 0) { // Do not include if originates from heavy jet or 'other' if (typeSet[1].find(idx) != typeSet[1].end() || typeSet[2].find(idx) != typeSet[2].end()) { workEventJet[i].statusNeg(); break; } // Made it to start of event record so done if (idx == 0) break; // Otherwise next mother and continue idx = event[idx].mother1(); // Heavy jets } else if (iType == 1) { // Only include if originates from heavy jet if (typeSet[1].find(idx) != typeSet[1].end()) break; // Made it to start of event record with no heavy jet mother, // so DO NOT include particle if (idx == 0) { workEventJet[i].statusNeg(); break; } // Otherwise next mother and continue idx = event[idx].mother1(); } // if (iType) } // while (true) } // for (i) } //-------------------------------------------------------------------------- // Step (2b): run jet algorithm and provide common output // This does nothing, because the jet algorithm is run several times // in the matching algorithm. void JetMatchingMadgraph::runJetAlgorithm() {; } //-------------------------------------------------------------------------- // Step (2c): veto decision (returning true vetoes the event) bool JetMatchingMadgraph::matchPartonsToJets(int iType) { // Use two different routines for light/heavy jets as // different veto conditions and for clarity if (iType == 0) return (matchPartonsToJetsLight() > 0); else return (matchPartonsToJetsHeavy() > 0); } //-------------------------------------------------------------------------- // Step(2c): light jets // Return codes are given indicating the reason for a veto. // Although not currently used, they are a useful debugging tool: // 0 = no veto // 1 = veto as number of jets less than number of partons // 2 = veto as exclusive mode and number of jets greater than // number of partons // 3 = veto as inclusive mode and there would be an extra jet // that is harder than any matched soft jet // 4 = veto as there is a parton which does not match a jet int JetMatchingMadgraph::matchPartonsToJetsLight() { // Count the number of hard partons int nParton = typeIdx[0].size(); // Initialize SlowJet with current working event if (!slowJet->setup(workEventJet) ) { infoPtr->errorMsg("Warning in JetMatchingMadgraph:matchPartonsToJets" "Light: the SlowJet algorithm failed on setup"); return NONE; } double localQcutSq = qCutSq; double dOld = 0.0; // Cluster in steps to find all hadronic jets at the scale qCut while ( slowJet->sizeAll() - slowJet->sizeJet() > 0 ) { if( slowJet->dNext() > localQcutSq ) break; dOld = slowJet->dNext(); slowJet->doStep(); } int nJets = slowJet->sizeJet(); int nClus = slowJet->sizeAll(); // Debug printout. if (MATCHINGDEBUG) slowJet->list(true); // Count of the number of hadronic jets in SlowJet accounting int nCLjets = nClus - nJets; // Compare number of hadronic jets to number of partons // Veto event if too few hadronic jets if ( nCLjets < nParton ) return LESS_JETS; // In exclusive mode, do not allow more hadronic jets than partons if ( exclusive ) { if ( nCLjets > nParton ) return MORE_JETS; // In inclusive mode, there can be more hadronic jets than partons, // provided that all partons have a matching hadronic jet } else { if (!slowJet->setup(workEventJet) ) { infoPtr->errorMsg("Warning in JetMatchingMadgraph:matchPartonsToJets" "Light: the SlowJet algorithm failed on setup"); return NONE; } // Cluster into hadronic jets until there are the same number as partons while ( slowJet->sizeAll() - slowJet->sizeJet() > nParton ) slowJet->doStep(); // Sort partons in pT. Update local qCut value. // Hadronic jets are already sorted in pT. localQcutSq = dOld; if ( clFact >= 0. && nParton > 0 ) { vector partonPt; for (int i = 0; i < nParton; ++i) partonPt.push_back( eventProcess[typeIdx[0][i]].pT2() ); sort( partonPt.begin(), partonPt.end()); localQcutSq = max( qCutSq, partonPt[0]); } nJets = slowJet->sizeJet(); nClus = slowJet->sizeAll(); } // Update scale if clustering factor is non-zero if ( clFact != 0. ) localQcutSq *= pow2(clFact); Event tempEvent; tempEvent.init( "(tempEvent)", particleDataPtr); int nPass = 0; double pTminEstimate = -1.; // Construct a master copy of the event containing only the // hardest nParton hadronic clusters. While constructing the event, // the parton type (ID_GLUON) and status (98,99) are arbitrary. for (int i = nJets; i < nClus; ++i) { tempEvent.append( ID_GLUON, 98, 0, 0, 0, 0, 0, 0, slowJet->p(i).px(), slowJet->p(i).py(), slowJet->p(i).pz(), slowJet->p(i).e() ); ++nPass; pTminEstimate = max( pTminEstimate, slowJet->pT(i)); if(nPass == nParton) break; } size_t tempSize = tempEvent.size(); // This keeps track of which hadronic jets are matched to parton vector jetAssigned; jetAssigned.assign( tempSize, false); // Take the list of unmatched hadronic jets and append a parton, one at // a time. The parton will be clustered with the "closest" hadronic jet // or the beam if the distance measure is below the cut. When a hadronic // jet is matched to a parton, it is removed from the list of unmatched // hadronic jets. This process continues until all hadronic jets are // matched to partons or it is not possible to make a match. int iNow = 0; while ( iNow < nParton ) { Event tempEventJet; tempEventJet.init("(tempEventJet)", particleDataPtr); for (size_t i = 0; i < tempSize; ++i) { if (jetAssigned[i]) continue; Vec4 pIn = tempEvent[i].p(); // Append unmatched hadronic jets tempEventJet.append( ID_GLUON, 98, 0, 0, 0, 0, 0, 0, pIn.px(), pIn.py(), pIn.pz(), pIn.e() ); } Vec4 pIn = eventProcess[typeIdx[0][iNow]].p(); // Append the current parton tempEventJet.append( ID_GLUON, 99, 0, 0, 0, 0, 0, 0, pIn.px(), pIn.py(), pIn.pz(), pIn.e() ); if ( !slowJet->setup(tempEventJet) ) { infoPtr->errorMsg("Warning in JetMatchingMadgraph:matchPartonsToJets" "Light: the SlowJet algorithm failed on setup"); } return NONE; // These are the conditions for the hadronic jet to match the parton // at the local qCut scale if ( slowJet->iNext() == tempEventJet.size() - 1 && slowJet->jNext() > -1 && slowJet->dNext() < localQcutSq ) { int iKnt = -1; for (size_t i = 0; i != tempSize; ++i) { if (jetAssigned[i]) continue; ++iKnt; // Identify the hadronic jet that matches the parton if (iKnt == slowJet->jNext() ) jetAssigned[i] = true; } } else { return UNMATCHED_PARTON; } ++iNow; } // Minimal eT/pT (CellJet/SlowJet) of matched light jets. // Needed later for heavy jet vetos in inclusive mode. // This information is not used currently. if (nParton > 0 && pTminEstimate > 0) eTpTlightMin = pTminEstimate; else eTpTlightMin = -1.; // No veto return NONE; } //-------------------------------------------------------------------------- // Step(2c): heavy jets // Return codes are given indicating the reason for a veto. // Although not currently used, they are a useful debugging tool: // 0 = no veto as there are no extra jets present // 1 = veto as in exclusive mode and extra jets present // 2 = veto as in inclusive mode and extra jets were harder // than any matched light jet int JetMatchingMadgraph::matchPartonsToJetsHeavy() { // Currently, heavy jets are unmatched // If there are no extra jets, then accept if (jetMomenta.empty()) return NONE; // No extra jets were present so no veto return NONE; } //========================================================================== #endif // end Pythia8_JetMatching_H pythia8-8.1.80.orig/examples/main87.cmnd0000644000175000017500000000276612217346167016141 0ustar sunsun! main87.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. // Number of events generated Main:numberOfEvents = 1000 // Shower options HadronLevel:all = on PartonLevel:MPI = on // Core process for merging Merging:Process = pp>LEPTONS,NEUTRINOS // Maximal number of additional LO jets. Merging:nJetMax = 2 // Maximal number of additional NLO jets. Merging:nJetMaxNLO = 1 // Merging scale value. Merging:TMS = 15 // Values of (fixed) scales in the matrix element calculation. Merging:muFacInME = 80.4 Merging:muRenInME = 91.188 // Values of (fixed) scales for the PS lowest multiplicity process. Merging:muFac = 80.4 Merging:muRen = 91.188 // Include PDFs into the choice of histories. Merging:includeRedundant = on // Switch off enforced rapidity ordering SpaceShower:rapidityOrder = off // Since NL3 is a next-to-leading order merging method, next-to-leading // order PDFs are necessary. However, the parton shower and multiparton // interactions favour leading-order PDFs, since multiparton interactions // probe the incoming hadron at small momentum scales. Until a NLO-merged // tune becomes available, NLO PDFs should be used throughout. // Example PDF files generated with CTEQ6M PDFs. PDF:useLHAPDF = on PDF:LHAPDFset = cteq6m.LHpdf SpaceShower:alphaSvalue = 0.118 TimeShower:alphaSvalue = 0.118 pythia8-8.1.80.orig/examples/main52.cc0000644000175000017500000002047612217346166015572 0ustar sunsun// main52.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Studies of hadron-level and parton-level minimum-bias quantities, // comparing internal default PDF with one from LHAPDF. // Major differences indicate need for major retuning, e.g. pT0Ref. // Access time information. #include #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Machine: 1 = Tevatron, 2 = LHC. Statistics. int machine = 1; int nEvent = 10000; // Select new PDF set; LHAPDF file name conventions. //string pdfSet = "cteq5l.LHgrid"; //string pdfSet = "cteq61.LHpdf"; //string pdfSet = "cteq61.LHgrid"; //string pdfSet = "MRST2004nlo.LHgrid"; string pdfSet = "MRST2001lo.LHgrid"; // Histograms for hadron-level quantities. double nMax = (machine == 1) ? 199.5 : 399.5; Hist nChargedOld("n_charged old PDF", 100, -0.5, nMax); Hist nChargedNew("n_charged new PDF", 100, -0.5, nMax); Hist nChargedRat("n_charged new/old PDF", 100, -0.5, nMax); Hist ySpecOld("y charged distribution old PDF", 100, -10., 10.); Hist ySpecNew("y charged distribution new PDF", 100, -10., 10.); Hist ySpecRat("y charged distribution new/old PDF", 100, -10., 10.); Hist pTSpecOld("pT charged distribution old PDF", 100, 0., 20.); Hist pTSpecNew("pT charged distribution new PDF", 100, 0., 20.); Hist pTSpecRat("pT charged distribution new/old PDF", 100, 0., 20.); Hist avgPTnChOld("(n_charged) old PDF", 100, -0.5, nMax); Hist avgPTnChNew("(n_charged) new PDF", 100, -0.5, nMax); Hist avgPTnChRat("(n_charged) new/old PDF", 100, -0.5, nMax); // Histograms for parton-level quantities. Hist xDistOld("MPI log(x) distribution old PDF", 80, -8., 0.); Hist xDistNew("MPI log(x) distribution new PDF", 80, -8., 0.); Hist xDistRat("MPI log(x) distribution new/old PDF", 80, -8., 0.); Hist pTDistOld("MPI pT (=Q) distribution old PDF", 100, 0., 20.); Hist pTDistNew("MPI pT (=Q) distribution new PDF", 100, 0., 20.); Hist pTDistRat("MPI pT (=Q) distribution new/old PDF", 100, 0., 20.); // Loop over one default run and one with new PDF. for (int iRun = 0; iRun < 2; ++iRun) { // Get starting time in seconds. time_t tBegin = time(0); // Generator. Pythia pythia; Event& event = pythia.event; // Generate minimum-bias events, with or without double diffraction. pythia.readString("SoftQCD:nonDiffractive = on"); //pythia.readString("SoftQCD:doubleDiffractive = on"); // Generate QCD jet events, above some threshold. //pythia.readString("HardQCD:all = on"); //pythia.readString("PhaseSpace:pTHatMin = 50."); // In second run pick new PDF set. if (iRun == 1) { pythia.readString("PDF:useLHAPDF = on"); pythia.readString("PDF:LHAPDFset = " + pdfSet); // Allow extrapolation of PDF's beyond x and Q2 boundaries, at own risk. // Default behaviour is to freeze PDF's at boundaries. pythia.readString("PDF:extrapolateLHAPDF = on"); // Need to change pT0Ref depending on choice of PDF. // One possibility: retune to same . //pythia.readString("MultipartonInteractions:pT0Ref = 2.17"); } // Tevatron/LHC initialization. double eCM = (machine == 1) ? 1960. : 7000.; pythia.settings.parm("Beams:eCM", eCM); if (machine == 1) pythia.readString("Beams:idB = -2212"); pythia.init(); // Begin event loop. for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Skip if error. if (!pythia.next()) continue; // Statistics on multiplicity and pT. int nCh = 0; double pTsum = 0.; for (int i = 0; i < event.size(); ++i) if (event[i].isFinal() && event[i].isCharged()) { ++nCh; pTsum += event[i].pT(); // Fill histograms for charged y and pT spectra. if (iRun == 0) { ySpecOld.fill( event[i].y() ); pTSpecOld.fill( event[i].pT() ); } else { ySpecNew.fill( event[i].y() ); pTSpecNew.fill( event[i].pT() ); } } // Fill histograms for summed quantities. if (iRun == 0) { nChargedOld.fill( nCh ); avgPTnChOld.fill( nCh, pTsum / max(1, nCh) ); } else { nChargedNew.fill( nCh ); avgPTnChNew.fill( nCh, pTsum / max(1, nCh) ); } // Loop through event record and fill x of all incoming partons. for (int i = 1; i < event.size(); ++i) if (event[i].status() == -21 || event[i].status() == -31) { double x = 2. * event[i].e() / eCM; if (iRun == 0) xDistOld.fill( log10(x) ); else xDistNew.fill( log10(x) ); } // Loop through multiparton interactions list and fill pT of all MPI's. for (int i = 0; i < pythia.info.nMPI(); ++i) { double pT = pythia.info.pTMPI(i); if (iRun == 0) pTDistOld.fill( pT ); else pTDistNew.fill( pT ); } // End of event loop. } // Statistics. pythia.readString("Stat:showPartonLevel = on"); pythia.stat(); // Get finishing time in seconds. Print used time. time_t tEnd = time(0); cout << "\n This subrun took " << tEnd - tBegin << " seconds \n" << endl; // End of loop over two runs. } // Form (n_charged) ratios. avgPTnChOld /= nChargedOld; avgPTnChNew /= nChargedNew; // Take ratios of new to old distributions. nChargedRat = nChargedNew / nChargedOld; ySpecRat = ySpecNew / ySpecOld; pTSpecRat = pTSpecNew / pTSpecOld; avgPTnChRat = avgPTnChNew / avgPTnChOld; xDistRat = xDistNew / xDistOld; pTDistRat = pTDistNew / pTDistOld; // Print histograms. cout << nChargedOld << nChargedNew << nChargedRat << ySpecOld << ySpecNew << ySpecRat << pTSpecOld << pTSpecNew << pTSpecRat << avgPTnChOld << avgPTnChNew << avgPTnChRat << xDistOld << xDistNew << xDistRat << pTDistOld << pTDistNew << pTDistRat; // Second part of study, as simple extra check: // Begin fill shape of effective PDF at typical MPI Q2 = 10 scale: // F_effective(x) = (9/4) x*g(x) + Sum_i (x*q_i(x) + x*qbar_i(x)). double Q2 = 10.; PDF* oldPDF = new CTEQ5L(2212); PDF* newPDF = new LHAPDF(2212, pdfSet, 0); // Histograms. Hist effFlinOld("F_effective( x, Q2 = 10) old", 100 , 0., 1.); Hist effFlinNew("F_effective( x, Q2 = 10) new", 100 , 0., 1.); Hist effFlinRat("F_effective( x, Q2 = 10) new/old", 100 , 0., 1.); Hist effFlogOld("F_effective( x, Q2 = 10) old", 80 , -8., 0.); Hist effFlogNew("F_effective( x, Q2 = 10) new", 80 , -8., 0.); Hist effFlogRat("F_effective( x, Q2 = 10) new/old", 80 , -8., 0.); // Loop over x values, in a linear scale. for (int iX = 0; iX < 99; ++iX) { double x = 0.005 + 0.01 * iX; // Evaluate old summed PDF. double oldSum = 2.25 * oldPDF->xf( 21, x, Q2); for (int i = 1; i < 6; ++i) oldSum += oldPDF->xf( i, x, Q2) + oldPDF->xf( -i, x, Q2); effFlinOld.fill ( x, oldSum ); // Evaluate new summed PDF. double newSum = 2.25 * newPDF->xf( 21, x, Q2); for (int i = 1; i < 6; ++i) newSum += newPDF->xf( i, x, Q2) + newPDF->xf( -i, x, Q2); effFlinNew.fill ( x, newSum ); //End loop over x values, in a linear scale. } // Loop over x values, in a logarithmic scale for (int iX = 0; iX < 80; ++iX) { double xLog = -(0.1 * iX + 0.05); double x = pow( 10., xLog); // Evaluate old summed PDF. double oldSum = 2.25 * oldPDF->xf( 21, x, Q2); for (int i = 1; i < 6; ++i) oldSum += oldPDF->xf( i, x, Q2) + oldPDF->xf( -i, x, Q2); effFlogOld.fill ( xLog, oldSum ); // Evaluate new summed PDF. double newSum = 2.25 * newPDF->xf( 21, x, Q2); for (int i = 1; i < 6; ++i) newSum += newPDF->xf( i, x, Q2) + newPDF->xf( -i, x, Q2); effFlogNew.fill ( xLog, newSum ); //End loop over x values, in a logarithmic scale. } // Take ratios of new to old distributions. effFlinRat = effFlinNew / effFlinOld; effFlogRat = effFlogNew / effFlogOld; // Print histograms. cout << effFlinOld << effFlinNew << effFlinRat << effFlogOld << effFlogNew << effFlogRat; // Done. delete oldPDF; delete newPDF; return 0; } pythia8-8.1.80.orig/examples/main32.cc0000644000175000017500000000400212217346165015552 0ustar sunsun// main32.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a sample program showing Alpgen- or Madgraph-style MLM matching // for Madgraph LHEF or native Alpgen format event files. // // Please see the 'Jet Matching Style' manual page for a description of the // parameters and user options. // Includes and namespace #include "Pythia8/Pythia.h" #include "CombineMatchingInput.h" using namespace Pythia8; //========================================================================== int main() { // Generator and read in commands. Pythia pythia; pythia.readFile("main32.cmnd"); // Extract settings to be used in the main program. int nEvent = pythia.mode("Main:numberOfEvents"); int nAbort = pythia.mode("Main:timesAllowErrors"); int nSkip = pythia.mode("Main:spareMode1"); // Create UserHooks pointer. Stop if it failed. Pass pointer to Pythia. CombineMatchingInput combined; UserHooks* matching = combined.getHook(pythia); if (!matching) return 1; pythia.setUserHooksPtr(matching); // Initialise Pythia. if (!pythia.init()) { cout << "Error: could not initialise Pythia" << endl; return 1; }; // Optionally skip ahead in LHEF. pythia.LHAeventSkip( nSkip ); // Begin event loop. Optionally quit it before end of file. int iAbort = 0; for (int iEvent = 0; ; ++iEvent) { if (nEvent > 0 && iEvent >= nEvent) break; // Generate events. Quit if at end of file or many failures. if (!pythia.next()) { if (pythia.info.atEndOfFile()) { cout << "Info: end of input file reached" << endl; break; } if (++iAbort < nAbort) continue; cout << "Abort: too many errors in generation" << endl; break; } // Event analysis goes here. // End of event loop. } // Final statistics and done. pythia.stat(); delete matching; return 0; } pythia8-8.1.80.orig/examples/main31.cc0000644000175000017500000005070612217346165015565 0ustar sunsun// main31.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Richard Corke, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // Use userhooks to veto PYTHIA emissions above the POWHEG scale. class PowhegHooks : public UserHooks { public: // Constructor and destructor. PowhegHooks(int nFinalIn, int vetoModeIn, int vetoCountIn, int pThardModeIn, int pTemtModeIn, int emittedModeIn, int pTdefModeIn, int MPIvetoModeIn) : nFinal(nFinalIn), vetoMode(vetoModeIn), vetoCount(vetoCountIn), pThardMode(pThardModeIn), pTemtMode(pTemtModeIn), emittedMode(emittedModeIn), pTdefMode(pTdefModeIn), MPIvetoMode(MPIvetoModeIn) {}; ~PowhegHooks() {} //-------------------------------------------------------------------------- // Routines to calculate the pT (according to pTdefMode) in a splitting: // ISR: i (radiator after) -> j (emitted after) k (radiator before) // FSR: i (radiator before) -> j (emitted after) k (radiator after) // For the Pythia pT definition, a recoiler (after) must be specified. // Compute the Pythia pT separation. Based on pTLund function in History.cc double pTpythia(const Event &e, int RadAfterBranch, int EmtAfterBranch, int RecAfterBranch, bool FSR) { // Convenient shorthands for later Vec4 radVec = e[RadAfterBranch].p(); Vec4 emtVec = e[EmtAfterBranch].p(); Vec4 recVec = e[RecAfterBranch].p(); int radID = e[RadAfterBranch].id(); // Calculate virtuality of splitting double sign = (FSR) ? 1. : -1.; Vec4 Q(radVec + sign * emtVec); double Qsq = sign * Q.m2Calc(); // Mass term of radiator double m2Rad = (abs(radID) >= 4 && abs(radID) < 7) ? pow2(particleDataPtr->m0(radID)) : 0.; // z values for FSR and ISR double z, pTnow; if (FSR) { // Construct 2 -> 3 variables Vec4 sum = radVec + recVec + emtVec; double m2Dip = sum.m2Calc(); double x1 = 2. * (sum * radVec) / m2Dip; double x3 = 2. * (sum * emtVec) / m2Dip; z = x1 / (x1 + x3); pTnow = z * (1. - z); } else { // Construct dipoles before/after splitting Vec4 qBR(radVec - emtVec + recVec); Vec4 qAR(radVec + recVec); z = qBR.m2Calc() / qAR.m2Calc(); pTnow = (1. - z); } // Virtuality with correct sign pTnow *= (Qsq - sign * m2Rad); // Can get negative pT for massive splittings if (pTnow < 0.) { cout << "Warning: pTpythia was negative" << endl; return -1.; } #ifdef DBGOUTPUT cout << "pTpythia: rad = " << RadAfterBranch << ", emt = " << EmtAfterBranch << ", rec = " << RecAfterBranch << ", pTnow = " << sqrt(pTnow) << endl; #endif // Return pT return sqrt(pTnow); } // Compute the POWHEG pT separation between i and j double pTpowheg(const Event &e, int i, int j, bool FSR) { // pT value for FSR and ISR double pTnow = 0.; if (FSR) { // POWHEG d_ij (in CM frame). Note that the incoming beams have not // been updated in the parton systems pointer yet (i.e. prior to any // potential recoil). int iInA = partonSystemsPtr->getInA(0); int iInB = partonSystemsPtr->getInB(0); double betaZ = - ( e[iInA].pz() + e[iInB].pz() ) / ( e[iInA].e() + e[iInB].e() ); Vec4 iVecBst(e[i].p()), jVecBst(e[j].p()); iVecBst.bst(0., 0., betaZ); jVecBst.bst(0., 0., betaZ); pTnow = sqrt( (iVecBst + jVecBst).m2Calc() * iVecBst.e() * jVecBst.e() / pow2(iVecBst.e() + jVecBst.e()) ); } else { // POWHEG pT_ISR is just kinematic pT pTnow = e[j].pT(); } // Check result if (pTnow < 0.) { cout << "Warning: pTpowheg was negative" << endl; return -1.; } #ifdef DBGOUTPUT cout << "pTpowheg: i = " << i << ", j = " << j << ", pTnow = " << pTnow << endl; #endif return pTnow; } // Calculate pT for a splitting based on pTdefMode. // If j is -1, all final-state partons are tried. // If i, k, r and xSR are -1, then all incoming and outgoing // partons are tried. // xSR set to 0 means ISR, while xSR set to 1 means FSR double pTcalc(const Event &e, int i, int j, int k, int r, int xSRin) { // Loop over ISR and FSR if necessary double pTemt = -1., pTnow; int xSR1 = (xSRin == -1) ? 0 : xSRin; int xSR2 = (xSRin == -1) ? 2 : xSRin + 1; for (int xSR = xSR1; xSR < xSR2; xSR++) { // FSR flag bool FSR = (xSR == 0) ? false : true; // If all necessary arguments have been given, then directly calculate. // POWHEG ISR and FSR, need i and j. if ((pTdefMode == 0 || pTdefMode == 1) && i > 0 && j > 0) { pTemt = pTpowheg(e, i, j, (pTdefMode == 0) ? false : FSR); // Pythia ISR, need i, j and r. } else if (!FSR && pTdefMode == 2 && i > 0 && j > 0 && r > 0) { pTemt = pTpythia(e, i, j, r, FSR); // Pythia FSR, need k, j and r. } else if (FSR && pTdefMode == 2 && j > 0 && k > 0 && r > 0) { pTemt = pTpythia(e, k, j, r, FSR); // Otherwise need to try all possible combintations. } else { // Start by finding incoming legs to the hard system after // branching (radiator after branching, i for ISR). // Use partonSystemsPtr to find incoming just prior to the // branching and track mothers. int iInA = partonSystemsPtr->getInA(0); int iInB = partonSystemsPtr->getInB(0); while (e[iInA].mother1() != 1) { iInA = e[iInA].mother1(); } while (e[iInB].mother1() != 2) { iInB = e[iInB].mother1(); } // If we do not have j, then try all final-state partons int jNow = (j > 0) ? j : 0; int jMax = (j > 0) ? j + 1 : e.size(); for (; jNow < jMax; jNow++) { // Final-state and coloured jNow only if (!e[jNow].isFinal() || e[jNow].colType() == 0) continue; // POWHEG if (pTdefMode == 0 || pTdefMode == 1) { // ISR - only done once as just kinematical pT if (!FSR) { pTnow = pTpowheg(e, iInA, jNow, (pTdefMode == 0) ? false : FSR); if (pTnow > 0.) pTemt = (pTemt < 0) ? pTnow : min(pTemt, pTnow); // FSR - try all outgoing partons from system before branching // as i. Note that for the hard system, there is no // "before branching" information. } else { int outSize = partonSystemsPtr->sizeOut(0); for (int iMem = 0; iMem < outSize; iMem++) { int iNow = partonSystemsPtr->getOut(0, iMem); // Coloured only, i != jNow and no carbon copies if (iNow == jNow || e[iNow].colType() == 0) continue; if (jNow == e[iNow].daughter1() && jNow == e[iNow].daughter2()) continue; pTnow = pTpowheg(e, iNow, jNow, (pTdefMode == 0) ? false : FSR); if (pTnow > 0.) pTemt = (pTemt < 0) ? pTnow : min(pTemt, pTnow); } // for (iMem) } // if (!FSR) // Pythia } else if (pTdefMode == 2) { // ISR - other incoming as recoiler if (!FSR) { pTnow = pTpythia(e, iInA, jNow, iInB, FSR); if (pTnow > 0.) pTemt = (pTemt < 0) ? pTnow : min(pTemt, pTnow); pTnow = pTpythia(e, iInB, jNow, iInA, FSR); if (pTnow > 0.) pTemt = (pTemt < 0) ? pTnow : min(pTemt, pTnow); // FSR - try all final-state coloured partons as radiator // after emission (k). } else { for (int kNow = 0; kNow < e.size(); kNow++) { if (kNow == jNow || !e[kNow].isFinal() || e[kNow].colType() == 0) continue; // For this kNow, need to have a recoiler. // Try two incoming. pTnow = pTpythia(e, kNow, jNow, iInA, FSR); if (pTnow > 0.) pTemt = (pTemt < 0) ? pTnow : min(pTemt, pTnow); pTnow = pTpythia(e, kNow, jNow, iInB, FSR); if (pTnow > 0.) pTemt = (pTemt < 0) ? pTnow : min(pTemt, pTnow); // Try all other outgoing. for (int rNow = 0; rNow < e.size(); rNow++) { if (rNow == kNow || rNow == jNow || !e[rNow].isFinal() || e[rNow].colType() == 0) continue; pTnow = pTpythia(e, kNow, jNow, rNow, FSR); if (pTnow > 0.) pTemt = (pTemt < 0) ? pTnow : min(pTemt, pTnow); } // for (rNow) } // for (kNow) } // if (!FSR) } // if (pTdefMode) } // for (j) } } // for (xSR) #ifdef DBGOUTPUT cout << "pTcalc: i = " << i << ", j = " << j << ", k = " << k << ", r = " << r << ", xSR = " << xSRin << ", pTemt = " << pTemt << endl; #endif return pTemt; } //-------------------------------------------------------------------------- // Extraction of pThard based on the incoming event. // Assume that all the final-state particles are in a continuous block // at the end of the event and the final entry is the POWHEG emission. // If there is no POWHEG emission, then pThard is set to SCALUP. bool canVetoMPIStep() { return true; } int numberVetoMPIStep() { return 1; } bool doVetoMPIStep(int nMPI, const Event &e) { // Extra check on nMPI if (nMPI > 1) return false; // Find if there is a POWHEG emission. Go backwards through the // event record until there is a non-final particle. Also sum pT and // find pT_1 for possible MPI vetoing int count = 0; double pT1 = 0., pTsum = 0.; for (int i = e.size() - 1; i > 0; i--) { if (e[i].isFinal()) { count++; pT1 = e[i].pT(); pTsum += e[i].pT(); } else break; } // Extra check that we have the correct final state if (count != nFinal && count != nFinal + 1) { cout << "Error: wrong number of final state particles in event" << endl; exit(1); } // Flag if POWHEG radiation present and index bool isEmt = (count == nFinal) ? false : true; int iEmt = (isEmt) ? e.size() - 1 : -1; // If there is no radiation or if pThardMode is 0 then set pThard to SCALUP. if (!isEmt || pThardMode == 0) { pThard = infoPtr->scalup(); // If pThardMode is 1 then the pT of the POWHEG emission is checked against // all other incoming and outgoing partons, with the minimal value taken } else if (pThardMode == 1) { pThard = pTcalc(e, -1, iEmt, -1, -1, -1); // If pThardMode is 2, then the pT of all final-state partons is checked // against all other incoming and outgoing partons, with the minimal value // taken } else if (pThardMode == 2) { pThard = pTcalc(e, -1, -1, -1, -1, -1); } // Find MPI veto pT if necessary if (MPIvetoMode == 1) { pTMPI = (isEmt) ? pTsum / 2. : pT1; } #ifdef DBGOUTPUT cout << "doVetoMPIStep: Qfac = " << infoPtr->scalup() << ", pThard = " << pThard << endl << endl; #endif // Initialise other variables accepted = false; nAcceptSeq = nISRveto = nFSRveto = 0; // Do not veto the event return false; } //-------------------------------------------------------------------------- // ISR veto bool canVetoISREmission() { return (vetoMode == 0) ? false : true; } bool doVetoISREmission(int, const Event &e, int iSys) { // Must be radiation from the hard system if (iSys != 0) return false; // If we already have accepted 'vetoCount' emissions in a row, do nothing if (vetoMode == 1 && nAcceptSeq >= vetoCount) return false; // Pythia radiator after, emitted and recoiler after. int iRadAft = -1, iEmt = -1, iRecAft = -1; for (int i = e.size() - 1; i > 0; i--) { if (iRadAft == -1 && e[i].status() == -41) iRadAft = i; else if (iEmt == -1 && e[i].status() == 43) iEmt = i; else if (iRecAft == -1 && e[i].status() == -42) iRecAft = i; if (iRadAft != -1 && iEmt != -1 && iRecAft != -1) break; } if (iRadAft == -1 || iEmt == -1 || iRecAft == -1) { e.list(); cout << "Error: couldn't find Pythia ISR emission" << endl; exit(1); } // pTemtMode == 0: pT of emitted w.r.t. radiator // pTemtMode == 1: min(pT of emitted w.r.t. all incoming/outgoing) // pTemtMode == 2: min(pT of all outgoing w.r.t. all incoming/outgoing) int xSR = (pTemtMode == 0) ? 0 : -1; int i = (pTemtMode == 0) ? iRadAft : -1; int j = (pTemtMode != 2) ? iEmt : -1; int k = -1; int r = (pTemtMode == 0) ? iRecAft : -1; double pTemt = pTcalc(e, i, j, k, r, xSR); #ifdef DBGOUTPUT cout << "doVetoISREmission: pTemt = " << pTemt << endl << endl; #endif // Veto if pTemt > pThard if (pTemt > pThard) { nAcceptSeq = 0; nISRveto++; return true; } // Else mark that an emission has been accepted and continue nAcceptSeq++; accepted = true; return false; } //-------------------------------------------------------------------------- // FSR veto bool canVetoFSREmission() { return (vetoMode == 0) ? false : true; } bool doVetoFSREmission(int, const Event &e, int iSys, bool) { // Must be radiation from the hard system if (iSys != 0) return false; // If we already have accepted 'vetoCount' emissions in a row, do nothing if (vetoMode == 1 && nAcceptSeq >= vetoCount) return false; // Pythia radiator (before and after), emitted and recoiler (after) int iRecAft = e.size() - 1; int iEmt = e.size() - 2; int iRadAft = e.size() - 3; int iRadBef = e[iEmt].mother1(); if ( (e[iRecAft].status() != 52 && e[iRecAft].status() != -53) || e[iEmt].status() != 51 || e[iRadAft].status() != 51) { e.list(); cout << "Error: couldn't find Pythia FSR emission" << endl; exit(1); } // Behaviour based on pTemtMode: // 0 - pT of emitted w.r.t. radiator before // 1 - min(pT of emitted w.r.t. all incoming/outgoing) // 2 - min(pT of all outgoing w.r.t. all incoming/outgoing) int xSR = (pTemtMode == 0) ? 1 : -1; int i = (pTemtMode == 0) ? iRadBef : -1; int k = (pTemtMode == 0) ? iRadAft : -1; int r = (pTemtMode == 0) ? iRecAft : -1; // When pTemtMode is 0 or 1, iEmt has been selected double pTemt = 0.; if (pTemtMode == 0 || pTemtMode == 1) { // Which parton is emitted, based on emittedMode: // 0 - Pythia definition of emitted // 1 - Pythia definition of radiated after emission // 2 - Random selection of emitted or radiated after emission // 3 - Try both emitted and radiated after emission int j = iRadAft; if (emittedMode == 0 || (emittedMode == 2 && rndmPtr->flat() < 0.5)) j++; for (int jLoop = 0; jLoop < 2; jLoop++) { if (jLoop == 0) pTemt = pTcalc(e, i, j, k, r, xSR); else if (jLoop == 1) pTemt = min(pTemt, pTcalc(e, i, j, k, r, xSR)); // For emittedMode == 3, have tried iRadAft, now try iEmt if (emittedMode != 3) break; if (k != -1) swap(j, k); else j = iEmt; } // If pTemtMode is 2, then try all final-state partons as emitted } else if (pTemtMode == 2) { pTemt = pTcalc(e, i, -1, k, r, xSR); } #ifdef DBGOUTPUT cout << "doVetoFSREmission: pTemt = " << pTemt << endl << endl; #endif // Veto if pTemt > pThard if (pTemt > pThard) { nAcceptSeq = 0; nFSRveto++; return true; } // Else mark that an emission has been accepted and continue nAcceptSeq++; accepted = true; return false; } //-------------------------------------------------------------------------- // MPI veto bool canVetoMPIEmission() { return (MPIvetoMode == 0) ? false : true; } bool doVetoMPIEmission(int, const Event &e) { if (MPIvetoMode == 1) { if (e[e.size() - 1].pT() > pTMPI) { #ifdef DBGOUTPUT cout << "doVetoMPIEmission: pTnow = " << e[e.size() - 1].pT() << ", pTMPI = " << pTMPI << endl << endl; #endif return true; } } return false; } //-------------------------------------------------------------------------- // Functions to return information int getNISRveto() { return nISRveto; } int getNFSRveto() { return nFSRveto; } private: int nFinal, vetoMode, vetoCount, pThardMode, pTemtMode, emittedMode, pTdefMode, MPIvetoMode; double pThard, pTMPI; bool accepted; // The number of accepted emissions (in a row) int nAcceptSeq; // Statistics on vetos unsigned long int nISRveto, nFSRveto; }; //========================================================================== int main(int, char **) { // Generator Pythia pythia; // Add further settings that can be set in the configuration file pythia.settings.addMode("POWHEG:nFinal", 2, true, false, 1, 0); pythia.settings.addMode("POWHEG:veto", 0, true, true, 0, 2); pythia.settings.addMode("POWHEG:vetoCount", 3, true, false, 0, 0); pythia.settings.addMode("POWHEG:pThard", 0, true, true, 0, 2); pythia.settings.addMode("POWHEG:pTemt", 0, true, true, 0, 2); pythia.settings.addMode("POWHEG:emitted", 0, true, true, 0, 3); pythia.settings.addMode("POWHEG:pTdef", 0, true, true, 0, 2); pythia.settings.addMode("POWHEG:MPIveto", 0, true, true, 0, 1); // Load configuration file pythia.readFile("main31.cmnd"); // Read in main settings int nEvent = pythia.settings.mode("Main:numberOfEvents"); int nError = pythia.settings.mode("Main:timesAllowErrors"); // Read in POWHEG settings int nFinal = pythia.settings.mode("POWHEG:nFinal"); int vetoMode = pythia.settings.mode("POWHEG:veto"); int vetoCount = pythia.settings.mode("POWHEG:vetoCount"); int pThardMode = pythia.settings.mode("POWHEG:pThard"); int pTemtMode = pythia.settings.mode("POWHEG:pTemt"); int emittedMode = pythia.settings.mode("POWHEG:emitted"); int pTdefMode = pythia.settings.mode("POWHEG:pTdef"); int MPIvetoMode = pythia.settings.mode("POWHEG:MPIveto"); bool loadHooks = (vetoMode > 0 || MPIvetoMode > 0); // Add in user hooks for shower vetoing PowhegHooks *powhegHooks = NULL; if (loadHooks) { // Set ISR and FSR to start at the kinematical limit if (vetoMode > 0) { pythia.readString("SpaceShower:pTmaxMatch = 2"); pythia.readString("TimeShower:pTmaxMatch = 2"); } // Set MPI to start at the kinematical limit if (MPIvetoMode > 0) { pythia.readString("MultipartonInteractions:pTmaxMatch = 2"); } powhegHooks = new PowhegHooks(nFinal, vetoMode, vetoCount, pThardMode, pTemtMode, emittedMode, pTdefMode, MPIvetoMode); pythia.setUserHooksPtr((UserHooks *) powhegHooks); } // Initialise and list settings pythia.init(); // Counters for number of ISR/FSR emissions vetoed unsigned long int nISRveto = 0, nFSRveto = 0; // Begin event loop; generate until nEvent events are processed // or end of LHEF file int iEvent = 0, iError = 0; while (true) { // Generate the next event if (!pythia.next()) { // If failure because reached end of file then exit event loop if (pythia.info.atEndOfFile()) break; // Otherwise count event failure and continue/exit as necessary cout << "Warning: event " << iEvent << " failed" << endl; if (++iError == nError) { cout << "Error: too many event failures.. exiting" << endl; break; } continue; } /* * Process dependent checks and analysis may be inserted here */ // Update ISR/FSR veto counters if (loadHooks) { nISRveto += powhegHooks->getNISRveto(); nFSRveto += powhegHooks->getNFSRveto(); } // If nEvent is set, check and exit loop if necessary ++iEvent; if (nEvent != 0 && iEvent == nEvent) break; } // End of event loop. // Statistics, histograms and veto information pythia.stat(); cout << "Number of ISR emissions vetoed: " << nISRveto << endl; cout << "Number of FSR emissions vetoed: " << nFSRveto << endl; cout << endl; // Done. if (powhegHooks) delete powhegHooks; return 0; } pythia8-8.1.80.orig/examples/w+_production_lhc_1.lhe0000644000175000017500000033321012217346207020504 0ustar sunsun

      # MG/ME version : 4.4.48 # madgraph version : 4.4.5 # template version : 2.4.25 # helas version : 3.8 # model version : sm_1.2.1 #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # proc_card.dat * # * # This file is used to generate the code for a specific process. * # Some notation/conventions: * # * # 0. Do not modify the TAGS and their order. * # 1. hash/pound is a comment. * # 2. The number after the @ is used as an identifier for the class * # of processes. It can be any positive integer. * # 3. The number of lines for the max couplings depends on how many * # different classes of couplings are present in the model * # In the SM these are just two: QED (which include EW) and QCD * # 4. Write "end_coup" after the couplings list, * # to tell MG that the couplings input is over. * # 5. Write "done" after the proc list to * # to tell MG that the proc input is over. * # 6. Some model names available at present are: * # sm = Standard Model * # smckm = Standard Model with Cabibbo matrix * # mssm = Minimal Supersymmetric Standard Model * # 2hdm = Generic Two Higgs Doublet model * # heft = Higgs EFT (+Standard Model) * # usrmod = User Model * # 7. Don't leave spaces between the particles name in the * # definition of the multiparticles. * #********************************************************************* #********************************************************************* # Process(es) requested : mg2 input * #********************************************************************* # Begin PROCESS # This is TAG. Do not modify this line pp>e+vej @1 # First Process QCD=99 # Max QCD couplings QED=2 # Max QED couplings end_coup # End the couplings input done # this tells MG there are no more procs # End PROCESS # This is TAG. Do not modify this line #********************************************************************* # Model information * #********************************************************************* # Begin MODEL # This is TAG. Do not modify this line sm # End MODEL # This is TAG. Do not modify this line #********************************************************************* # Start multiparticle definitions * #********************************************************************* # Begin MULTIPARTICLES # This is TAG. Do not modify this line P uu~dd~cc~ss~g J uu~dd~cc~ss~g L+ e+mu+ L- e-mu- vl vevm vl~ ve~vm~ # End MULTIPARTICLES # This is TAG. Do not modify this line #****************************************************************** # MadGraph/MadEvent * #****************************************************************** # Les Houches friendly file for the SM parameters of MadGraph * # Spectrum and decay widths produced by SMCalc * #****************************************************************** #*Please note the following IMPORTANT issues: * # * #0. REFRAIN from editing this file by hand! Some of the parame- * # ters are not independent * # (such as G_Fermi, alpha_em, sin(theta_W),MZ,MW) and serious * # problems might be encountered (such as violation of unitarity * # or gauge invariance). Always use a calculator. * # * #1. alpha_S(MZ) has been used in the calculation of the parameters* # but, for consistency, it will be reset by madgraph to the * # value expected IF the pdfs for collisions with hadrons are * # used. This value is KEPT by madgraph when no pdf are used * # lpp(i)=0 . * # * #2. Values of the charm and bottom kinematic (pole) masses are * # those used in the matrix elements and phase space UNLESS they * # are set to ZERO from the start in the model (particles.dat) * # This happens, for example, when using 5-flavor QCD where * # charm and bottom are treated as partons in the initial state * # and a zero mass might be hardwired in the model definition. * # * #****************************************************************** Block SMINPUTS # Standard Model inputs 1 1.32506980E+02 # alpha_em(MZ)(-1) SM MSbar 2 1.16639000E-05 # G_Fermi 3 1.18000000E-01 # alpha_s(MZ) SM MSbar 4 9.11880000E+01 # Z mass (as input parameter) Block MGYUKAWA # Yukawa masses m/v=y/sqrt(2) # PDG YMASS 5 4.20000000E+00 # mbottom for the Yukawa y_b 4 1.42000000E+00 # mcharm for the Yukawa y_c 6 1.64500000E+02 # mtop for the Yukawa y_t 15 1.77700000E+00 # mtau for the Yukawa y_ta Block MGCKM # CKM elements for MadGraph 1 1 9.75000000E-01 # Vud for Cabibbo matrix Block MASS # Mass spectrum (kinematic masses) # PDG Mass 5 4.70000000E+00 # bottom pole mass 6 1.74300000E+02 # top pole mass 15 1.77700000E+00 # tau mass 23 9.11880000E+01 # Z mass 24 8.04190000E+01 # W mass 25 1.20000000E+02 # H mass # PDG Width DECAY 6 1.50833649E+00 # top width DECAY 23 2.44140351E+00 # Z width DECAY 24 2.04759951E+00 # W width DECAY 25 5.75308848E-03 # H width # BR NDA ID1 ID2 8.27451012E-02 2 4 -4 # BR( H -> c cbar ) 7.17809696E-01 2 5 -5 # BR( H -> b bbar ) 0.00000000E+00 2 6 -6 # BR( H -> t tbar ) 4.31720144E-02 2 15 -15 # BR( H -> tau- tau+) 6.90597075E-03 2 23 23 # BR( H -> Z Z^(*)) 7.45906395E-02 2 24 -24 # BR( H -> W W^(*)) 3.01765558E-02 2 21 21 # BR( H -> g g ) 1.42800773E-03 2 22 22 # BR( H -> A A ) #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # run_card.dat * # * # This file is used to set the parameters of the run. * # * # Some notation/conventions: * # * # Lines starting with a '# ' are info or comments * # * # mind the format: value = variable ! comment * #********************************************************************* # #******************* # Running parameters #******************* # #********************************************************************* # Tag name for the run (one word) * #********************************************************************* 'fermi' = run_tag ! name of the run #********************************************************************* # Run to generate the grid pack * #********************************************************************* .false. = gridpack !True = setting up the grid pack #********************************************************************* # Number of events and rnd seed * #********************************************************************* 100 = nevents ! Number of unweighted events requested 25490 = iseed ! rnd seed (0=assigned automatically=default)) #********************************************************************* # Collider type and energy * #********************************************************************* 1 = lpp1 ! beam 1 type (0=NO PDF) 1 = lpp2 ! beam 2 type (0=NO PDF) 3500.0 = ebeam1 ! beam 1 energy in GeV 3500.0 = ebeam2 ! beam 2 energy in GeV #********************************************************************* # Beam polarization from -100 (left-handed) to 100 (right-handed) * #********************************************************************* 0 = polbeam1 ! beam polarization for beam 1 0 = polbeam2 ! beam polarization for beam 2 #********************************************************************* # PDF CHOICE: this automatically fixes also alpha_s and its evol. * #********************************************************************* # 'cteq6_l' = pdlabel ! PDF set 'lhapdf' = pdlabel ! PDF label 10042 = lhaid ! PDF set #********************************************************************* # Renormalization and factorization scales * #********************************************************************* T = fixed_ren_scale ! if .true. use fixed ren scale T = fixed_fac_scale ! if .true. use fixed fac scale 91.188 = scale ! fixed ren scale 80.4 = dsqrt_q2fact1 ! fixed fact scale for pdf1 80.4 = dsqrt_q2fact2 ! fixed fact scale for pdf2 1 = scalefact ! scale factor for event-by-event scales #********************************************************************* # Matching - Warning! ickkw > 0 is still beta #********************************************************************* 0 = ickkw ! 0 no matching, 1 MLM, 2 CKKW matching 1 = highestmult ! for ickkw=2, highest mult group 1 = ktscheme ! for ickkw=1, 1 Durham kT, 2 Pythia pTE 1 = alpsfact ! scale factor for QCD emission vx F = chcluster ! cluster only according to channel diag F = pdfwgt ! for ickkw=1, perform pdf reweighting #********************************************************************* # #********************************** # BW cutoff (M+/-bwcutoff*Gamma) #********************************** 15d0 = bwcutoff #******************* # Standard Cuts #******************* # #********************************************************************* # Minimum and maximum pt's * #********************************************************************* 0d0 = ptj ! minimum pt for the jets 0d0 = ptb ! minimum pt for the b 0d0 = pta ! minimum pt for the photons 0d0 = ptl ! minimum pt for the charged leptons 0d0 = misset ! minimum missing Et (sum of neutrino's momenta) 0d0 = ptheavy ! minimum pt for one heavy final state 0d0 = ptonium ! minimum pt for the quarkonium states 1d9 = ptjmax ! maximum pt for the jets 1d9 = ptbmax ! maximum pt for the b 1d9 = ptamax ! maximum pt for the photons 1d9 = ptlmax ! maximum pt for the charged leptons 1d9 = missetmax ! maximum missing Et (sum of neutrino's momenta) #********************************************************************* # Minimum and maximum E's (in the lab frame) * #********************************************************************* 0d0 = ej ! minimum E for the jets 0d0 = eb ! minimum E for the b 0d0 = ea ! minimum E for the photons 0d0 = el ! minimum E for the charged leptons 1d9 = ejmax ! maximum E for the jets 1d9 = ebmax ! maximum E for the b 1d9 = eamax ! maximum E for the photons 1d9 = elmax ! maximum E for the charged leptons #********************************************************************* # Maximum and minimum rapidity * #********************************************************************* 1d9 = etaj ! max rap for the jets 1d9 = etab ! max rap for the b 1d9 = etaa ! max rap for the photons 1d9 = etal ! max rap for the charged leptons 1d9 = etaonium ! max rap for the quarkonium states 0d0 = etajmin ! min rap for the jets 0d0 = etabmin ! min rap for the b 0d0 = etaamin ! min rap for the photons 0d0 = etalmin ! main rap for the charged leptons #********************************************************************* # Minimum and maximum DeltaR distance * #********************************************************************* 0d0 = drjj ! min distance between jets 0d0 = drbb ! min distance between b's 0d0 = drll ! min distance between leptons 0d0 = draa ! min distance between gammas 0d0 = drbj ! min distance between b and jet 0d0 = draj ! min distance between gamma and jet 0d0 = drjl ! min distance between jet and lepton 0d0 = drab ! min distance between gamma and b 0d0 = drbl ! min distance between b and lepton 0d0 = dral ! min distance between gamma and lepton 1d9 = drjjmax ! max distance between jets 1d9 = drbbmax ! max distance between b's 1d9 = drllmax ! max distance between leptons 1d9 = draamax ! max distance between gammas 1d9 = drbjmax ! max distance between b and jet 1d9 = drajmax ! max distance between gamma and jet 1d9 = drjlmax ! max distance between jet and lepton 1d9 = drabmax ! max distance between gamma and b 1d9 = drblmax ! max distance between b and lepton 1d9 = dralmax ! maxdistance between gamma and lepton #********************************************************************* # Minimum and maximum invariant mass for pairs * #********************************************************************* 0d0 = mmjj ! min invariant mass of a jet pair 0d0 = mmbb ! min invariant mass of a b pair 0d0 = mmaa ! min invariant mass of gamma gamma pair 0d0 = mmll ! min invariant mass of l+l- (same flavour) lepton pair 1d9 = mmjjmax ! max invariant mass of a jet pair 1d9 = mmbbmax ! max invariant mass of a b pair 1d9 = mmaamax ! max invariant mass of gamma gamma pair 1d9 = mmllmax ! max invariant mass of l+l- (same flavour) lepton pair #********************************************************************* # Minimum and maximum invariant mass for all letpons * #********************************************************************* 0d0 = mmnl ! min invariant mass for all letpons (l+- and vl) 1d9 = mmnlmax ! max invariant mass for all letpons (l+- and vl) #********************************************************************* # Inclusive cuts * #********************************************************************* 0d0 = xptj ! minimum pt for at least one jet 0d0 = xptb ! minimum pt for at least one b 0d0 = xpta ! minimum pt for at least one photon 0d0 = xptl ! minimum pt for at least one charged lepton #********************************************************************* # Control the pt's of the jets sorted by pt * #********************************************************************* 0d0 = ptj1min ! minimum pt for the leading jet in pt 0d0 = ptj2min ! minimum pt for the second jet in pt 0d0 = ptj3min ! minimum pt for the third jet in pt 0d0 = ptj4min ! minimum pt for the fourth jet in pt 1d9 = ptj1max ! maximum pt for the leading jet in pt 1d9 = ptj2max ! maximum pt for the second jet in pt 1d9 = ptj3max ! maximum pt for the third jet in pt 1d9 = ptj4max ! maximum pt for the fourth jet in pt 0 = cutuse ! reject event if fails any (0) / all (1) jet pt cuts #********************************************************************* # Control the Ht(k)=Sum of k leading jets * #********************************************************************* 0d0 = htjmin ! minimum jet HT=Sum(jet pt) 1d9 = htjmax ! maximum jet HT=Sum(jet pt) 0d0 = ht2min ! minimum Ht for the two leading jets 0d0 = ht3min ! minimum Ht for the three leading jets 0d0 = ht4min ! minimum Ht for the four leading jets 1d9 = ht2max ! maximum Ht for the two leading jets 1d9 = ht3max ! maximum Ht for the three leading jets 1d9 = ht4max ! maximum Ht for the four leading jets #********************************************************************* # WBF cuts * #********************************************************************* 0 = xetamin ! minimum rapidity for two jets in the WBF case 0 = deltaeta ! minimum rapidity for two jets in the WBF case #********************************************************************* # maximal pdg code for quark to be considered as a jet * # otherwise b cuts are applied * #********************************************************************* 4 = maxjetflavor #********************************************************************* # Jet measure cuts * #********************************************************************* 0 = xqcut ! minimum kt jet measure between partons #********************************************************************* 30d0 = ktdurham ! minimum durham kt jet measure between partons 0.4 = dparameter ! D parameter for hadronic kT T = dokt ! T: enable durham kt cut #********************************************************************* # Number of Events : 100 # Integrated weight (pb) : .45148E+03 # Truncated wgt (pb) : .00000E+00 # Unit wgt : .45148E+01
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0.44763582618E+02 0.00000000000E+00 0. -1. 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 -0.19560307388E+03 0.19560307388E+03 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.58900031250E+02 0.12421205031E+02 -0.14938693493E+03 0.18015361857E+03 0.80717841533E+02 0. 0. -11 1 3 3 0 0 0.21420131338E+02 -0.33185482604E+02 -0.42299855262E+02 0.57873794047E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.37479899911E+02 0.45606687635E+02 -0.10708707967E+03 0.12227982453E+03 0.00000000000E+00 0. -1. 3 1 1 2 501 0 -0.58900031250E+02 -0.12421205031E+02 -0.14525563263E+01 0.60213037920E+02 0.00000000000E+00 0. -1. 6 1 0.4514800E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 502 0 0.00000000000E+00 0.00000000000E+00 0.51955446632E+03 0.51955446632E+03 0.00000000000E+00 0. -1. 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 -0.12780905702E+02 0.12780905702E+02 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.59196724780E+02 -0.46636073649E+01 0.24055841591E+03 0.25957814530E+03 0.77372221069E+02 0. 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0.00000000000E+00 0. -1. 6 1 0.4514800E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 502 0 0.00000000000E+00 0.00000000000E+00 0.21929483601E+03 0.21929483601E+03 0.00000000000E+00 0. -1. 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 -0.18169599239E+02 0.18169599239E+02 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.34628427257E+02 -0.12547840950E+02 0.15881961196E+03 0.18137217039E+03 0.79470867373E+02 0. 0. -11 1 3 3 0 0 -0.15991554477E+01 -0.24801592254E+02 0.85039590287E+01 0.26267729168E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.36227582705E+02 0.12253751304E+02 0.15031565293E+03 0.15510444122E+03 0.00000000000E+00 0. -1. 1 1 1 2 501 0 -0.34628427257E+02 0.12547840950E+02 0.42305624814E+02 0.56092264866E+02 0.00000000000E+00 0. -1. pythia8-8.1.80.orig/examples/main09.cc0000644000175000017500000000522012217346164015560 0ustar sunsun// main09.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Generate a predetermined second hard interaction. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator. Pythia pythia; Event& event = pythia.event; // Select first hard process (just a small sample of possibilities). //pythia.readString("HardQCD:all = on"); pythia.readString("Top:all = on"); //pythia.readString("WeakSingleBoson:ffbar2gmZ = on"); //pythia.readString("WeakSingleBoson:ffbar2W = on"); // Select second hard process (complete list of options). pythia.readString("SecondHard:generate = on"); //pythia.readString("SecondHard:TwoJets = on"); pythia.readString("SecondHard:PhotonAndJet = on"); //pythia.readString("SecondHard:TwoPhotons = on"); //pythia.readString("SecondHard:SingleGmZ = on"); //pythia.readString("SecondHard:SingleW = on"); //pythia.readString("SecondHard:TwoBJets = on"); // Kinematics cuts, common for the two. pythia.readString("PhaseSpace:mHatMin = 40."); pythia.readString("PhaseSpace:pTHatMin = 20."); // Initialize for LHC at 8 TeV. pythia.readString("Beams:eCM = 8000."); pythia.init(); // Histogram. Hist pTfirst("pT first collision", 100, 0., 400.); Hist pTsecond("pT second collision", 100, 0., 200.); Hist pTdiff("pT first-second collision", 100, -100., 300.); Hist nMult("number of multiparton interactions", 100, -0.5, 99.5); Hist bMore("b enhancement factor", 100, 0., 10.); Hist nChg("charged multiplicity", 100, -0.5, 999.5); // Generate events. for (int iev = 0; iev < 1000; ++iev) { pythia.next(); // Histogram pT. double pT1 = pythia.info.pTMPI(0); double pT2 = pythia.info.pTMPI(1); pTfirst.fill( pT1 ); pTsecond.fill( pT2 ); pTdiff.fill( pT1 - pT2 ); // Histogram multiparton interactions double nMPI = pythia.info.nMPI(); nMult.fill( nMPI ); bMore.fill( pythia.info.enhanceMPI() ); // Histogram charged multiplicity. int nCharged = 0; for (int i = 0; i < event.size(); ++i) if (event[i].isFinal() && event[i].isCharged()) ++nCharged; nChg.fill( nCharged ); } // Compare full statistics listing with what is set in info. pythia.stat(); cout << scientific << setprecision(3) << "\n From pythia.info: sigma = " << pythia.info.sigmaGen() << " +- " << pythia.info.sigmaErr() << endl; // Print histograms. cout << pTfirst << pTsecond << pTdiff << nMult << bMore << nChg; // Done. return 0; } pythia8-8.1.80.orig/examples/main86.cc0000644000175000017500000003005212217346167015571 0ustar sunsun// main86.cc is a part of the PYTHIA event generator. // Copyright (C) 2011 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This program is written by Stefan Prestel. // It illustrates how to do UMEPS merging, // see the Matrix Element Merging page in the online manual. #include "Pythia8/Pythia.h" #include "Pythia8/Pythia8ToHepMC.h" #include "HepMC/GenEvent.h" #include "HepMC/IO_GenEvent.h" // Following line to be used with HepMC 2.04 onwards. #include "HepMC/Units.h" using namespace Pythia8; //========================================================================== // Example main programm to illustrate merging int main( int argc, char* argv[] ){ // Check that correct number of command-line arguments if (argc != 4) { cerr << " Unexpected number of command-line arguments ("< xsecLO; vector nAcceptLO; cout << endl << endl << endl; cout << "Start estimating umeps tree level cross section" << endl; while(njetcounterLO >= 0) { // From njet, choose LHE file stringstream in; in << "_" << njetcounterLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathTree+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathTree + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); pythia.settings.mode("Merging:nRequested", njetcounterLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Start generation loop for( int iEvent=0; iEvent 0 ) njetcounterLO--; else break; } // end loop over different jet multiplicities // Switch off cross section estimation. pythia.settings.flag("Merging:doXSectionEstimate", false); // Switch showering and multiple interaction back on. pythia.settings.flag("PartonLevel:FSR",fsr); pythia.settings.flag("PartonLevel:ISR",isr); pythia.settings.flag("HadronLevel:all",had); pythia.settings.flag("PartonLevel:MPI",mpi); // Declare sample cross section for output. double sigmaTemp = 0.; vector sampleXStree; vector sampleXSsubtTree; // Cross section an error. double sigmaTotal = 0.; double errorTotal = 0.; int sizeLO = int(xsecLO.size()); njetcounterLO = nMaxLO; iPathTree = iPath + "_tree"; while(njetcounterLO >= 0){ // From njet, choose LHE file stringstream in; in << "_" << njetcounterLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathTree+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathTree + in.str(); pythia.settings.flag("Merging:doUMEPSTree",true); pythia.settings.flag("Merging:doUMEPSSubt",false); pythia.settings.mode("Merging:nRecluster",0); LHAupLHEF lhareader((char*)(LHEfile).c_str()); cout << endl << endl << endl << "Start tree level treatment for " << njetcounterLO << " jets" << endl; pythia.settings.mode("Merging:nRequested", njetcounterLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Remember position in vector of cross section estimates. int iNow = sizeLO-1-njetcounterLO; // Start generation loop for( int iEvent=0; iEventweights().push_back(weight*normhepmc); // Fill HepMC event. ToHepMC.fill_next_event( pythia, hepmcevt ); // Add the weight of the current event to the cross section. sigmaTotal += weight*normhepmc; sigmaTemp += weight*normhepmc; errorTotal += pow2(weight*normhepmc); // Report cross section to hepmc HepMC::GenCrossSection xsec; xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } // end loop over events to generate // print cross section, errors pythia.stat(); // Save sample cross section for output. sampleXStree.push_back(sigmaTemp); sigmaTemp = 0.; // Restart with ME of a reduced the number of jets if( njetcounterLO > 0 ) njetcounterLO--; else break; } cout << endl << endl << endl; cout << "Do UMEPS subtraction" << endl; int njetcounterLS = nMaxLO; string iPathSubt = iPath + "_tree"; while(njetcounterLS >= 1){ // From njet, choose LHE file stringstream in; in << "_" << njetcounterLS << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathSubt+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathSubt + in.str(); pythia.settings.flag("Merging:doUMEPSTree",false); pythia.settings.flag("Merging:doUMEPSSubt",true); pythia.settings.mode("Merging:nRecluster",1); LHAupLHEF lhareader((char*)(LHEfile).c_str()); cout << endl << endl << endl << "Start subtractive treatment for " << njetcounterLS << " jets" << endl; pythia.settings.mode("Merging:nRequested", njetcounterLS); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Remember position in vector of cross section estimates. int iNow = sizeLO-1-njetcounterLS; // Start generation loop for( int iEvent=0; iEventweights().push_back(weight*normhepmc); // Fill HepMC event. ToHepMC.fill_next_event( pythia, hepmcevt ); // Add the weight of the current event to the cross section. sigmaTotal += weight*normhepmc; sigmaTemp += weight*normhepmc; errorTotal += pow2(weight*normhepmc); // Report cross section to hepmc. HepMC::GenCrossSection xsec; xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } // end loop over events to generate // print cross section, errors pythia.stat(); // Save sample cross section for output. sampleXSsubtTree.push_back(sigmaTemp); sigmaTemp = 0.; // Restart with ME of a reduced the number of jets if( njetcounterLS > 1 ) njetcounterLS--; else break; } // Print cross section information. cout << endl << endl; cout << " *---------------------------------------------------*" << endl; cout << " | |" << endl; cout << " | Sample cross sections after UMEPS merging |" << endl; cout << " | |" << endl; cout << " | Leading order cross sections (mb): |" << endl; for (int i = 0; i < int(sampleXStree.size()); ++i) cout << " | " << sampleXStree.size()-1-i << "-jet: " << setw(17) << scientific << setprecision(6) << sampleXStree[i] << " |" << endl; cout << " | |" << endl; cout << " | Leading-order subtractive cross sections (mb): |" << endl; for (int i = 0; i < int(sampleXSsubtTree.size()); ++i) cout << " | " << sampleXSsubtTree.size()-1-i+1 << "-jet: " << setw(17) << scientific << setprecision(6) << sampleXSsubtTree[i] << " |" << endl; cout << " | |" << endl; cout << " |---------------------------------------------------|" << endl; cout << " |---------------------------------------------------|" << endl; cout << " | Inclusive cross sections: |" << endl; cout << " | |" << endl; cout << " | UMEPS merged inclusive cross section: |" << endl; cout << " | " << setw(17) << scientific << setprecision(6) << sigmaTotal << " +- " << setw(17) << sqrt(errorTotal) << " mb " << " |" << endl; cout << " | |" << endl; cout << " | LO inclusive cross section: |" << endl; cout << " | " << setw(17) << scientific << setprecision(6) << xsecLO.back() << " mb |" << endl; cout << " | |" << endl; cout << " *---------------------------------------------------*" << endl; cout << endl << endl; // Done return 0; } pythia8-8.1.80.orig/examples/main86.cmnd0000644000175000017500000000204112217346167016122 0ustar sunsun! main86.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. // Number of events generated Main:numberOfEvents = 1000 // Specify shower options HadronLevel:all = on PartonLevel:MPI = on // Core process for merging Merging:Process = pp>LEPTONS,NEUTRINOS // Maximal number of additional LO jets. Merging:nJetMax = 2 // Merging scale value. Merging:TMS = 15 // Switch off enforced rapidity ordering SpaceShower:rapidityOrder = off // Since UMEPS is a tree-level merging method, both leading-order and // next-to-neading order PDFs are allowed. However, from parton shower // considerations, leading-order PDFs are preferred, since multiparton // interactions probe the incoming hadron at small momentum scales. // Example PDF files generated with CTEQ6M PDFs. PDF:useLHAPDF = on PDF:LHAPDFset = cteq6m.LHpdf SpaceShower:alphaSvalue = 0.118 TimeShower:alphaSvalue = 0.118 pythia8-8.1.80.orig/examples/cmssm.spc0000644000175000017500000001423612217346162016012 0ustar sunsun# SOFTSUSY3.3.0 SLHA compliant output # B.C. Allanach, Comput. Phys. Commun. 143 (2002) 305-331, hep-ph/0104145 # CMSSM 10.1.1 input - see arXiv:1109.3859 Block SPINFO # Program information 1 SOFTSUSY # spectrum calculator 2 3.3.0 # version number Block MODSEL # Select model 1 1 # sugra Block SMINPUTS # Standard Model inputs 1 1.27934000e+02 # alpha_em^(-1)(MZ) SM MSbar 2 1.16637000e-05 # G_Fermi 3 1.17200000e-01 # alpha_s(MZ)MSbar 4 9.11876000e+01 # MZ(pole) 5 4.25000000e+00 # mb(mb) 6 1.74300000e+02 # Mtop(pole) 7 1.77700000e+00 # Mtau(pole) Block MINPAR # SUSY breaking input parameters 1 1.25000000e+02 # m0 2 5.00000000e+02 # m12 3 1.00000000e+01 # tanb 4 1.00000000e+00 # sign(mu) 5 0.00000000e+00 # A0 # Low energy data in SOFTSUSY: MIXING=0 TOLERANCE=1.00000000e-03 # mgut=1.87825797e+16 GeV Block MASS # Mass spectrum # PDG code mass particle 24 8.04613815e+01 # MW 25 1.15412339e+02 # h0 35 7.21892898e+02 # H0 36 7.21606682e+02 # A0 37 7.26310615e+02 # H+ 1000021 1.14687814e+03 # ~g 1000022 2.04168238e+02 # ~neutralino(1) 1000023 3.86197315e+02 # ~neutralino(2) 1000024 3.86332261e+02 # ~chargino(1) 1000025 -6.39638883e+02 # ~neutralino(3) 1000035 6.53032956e+02 # ~neutralino(4) 1000037 6.52679913e+02 # ~chargino(2) 1000001 1.05561088e+03 # ~d_L 1000002 1.05278695e+03 # ~u_L 1000003 1.05560831e+03 # ~s_L 1000004 1.05278437e+03 # ~c_L 1000005 9.65462335e+02 # ~b_1 1000006 8.03540912e+02 # ~t_1 1000011 3.61778036e+02 # ~e_L 1000012 3.52902884e+02 # ~nue_L 1000013 3.61861990e+02 # ~mu_L 1000014 3.52899536e+02 # ~numu_L 1000015 2.22692429e+02 # ~stau_1 1000016 3.51730554e+02 # ~nu_tau_L 2000001 1.01102319e+03 # ~d_R 2000002 1.01434248e+03 # ~u_R 2000003 1.01102050e+03 # ~s_R 2000004 1.01433974e+03 # ~c_R 2000005 1.00775879e+03 # ~b_2 2000006 1.01102814e+03 # ~t_2 2000011 2.29874717e+02 # ~e_R 2000013 2.29864278e+02 # ~mu_R 2000015 3.62940076e+02 # ~stau_2 Block alpha # Effective Higgs mixing parameter -1.06797662e-01 # alpha Block nmix # neutralino mixing matrix 1 1 9.95886986e-01 # N_{1,1} 1 2 -1.72694202e-02 # N_{1,2} 1 3 8.22024839e-02 # N_{1,3} 1 4 -3.39651202e-02 # N_{1,4} 2 1 3.74375188e-02 # N_{2,1} 2 2 9.71264892e-01 # N_{2,2} 2 3 -1.95766260e-01 # N_{2,3} 2 4 1.30071184e-01 # N_{2,4} 3 1 -3.30727556e-02 # N_{3,1} 3 2 4.82085025e-02 # N_{3,2} 3 3 7.03472841e-01 # N_{3,3} 3 4 7.08313557e-01 # N_{3,4} 4 1 -7.55892561e-02 # N_{4,1} 4 2 2.32426798e-01 # N_{4,2} 4 3 6.78265645e-01 # N_{4,3} 4 4 -6.92978905e-01 # N_{4,4} Block Umix # chargino U mixing matrix 1 1 9.60950435e-01 # U_{1,1} 1 2 -2.76720547e-01 # U_{1,2} 2 1 2.76720547e-01 # U_{2,1} 2 2 9.60950435e-01 # U_{2,2} Block Vmix # chargino V mixing matrix 1 1 9.82582136e-01 # V_{1,1} 1 2 -1.85828808e-01 # V_{1,2} 2 1 1.85828808e-01 # V_{2,1} 2 2 9.82582136e-01 # V_{2,2} Block stopmix # stop mixing matrix 1 1 4.24985787e-01 # F_{11} 1 2 9.05200023e-01 # F_{12} 2 1 9.05200023e-01 # F_{21} 2 2 -4.24985787e-01 # F_{22} Block sbotmix # sbottom mixing matrix 1 1 9.75941340e-01 # F_{11} 1 2 2.18033254e-01 # F_{12} 2 1 -2.18033254e-01 # F_{21} 2 2 9.75941340e-01 # F_{22} Block staumix # stau mixing matrix 1 1 1.42739201e-01 # F_{11} 1 2 9.89760335e-01 # F_{12} 2 1 9.89760335e-01 # F_{21} 2 2 -1.42739201e-01 # F_{22} Block gauge Q= 8.73811408e+02 # SM gauge couplings 1 3.62408332e-01 # g'(Q)MSSM DRbar 2 6.43000889e-01 # g(Q)MSSM DRbar 3 1.06090510e+00 # g3(Q)MSSM DRbar Block yu Q= 8.73811408e+02 3 3 8.67028746e-01 # Yt(Q)MSSM DRbar Block yd Q= 8.73811408e+02 3 3 1.35275115e-01 # Yb(Q)MSSM DRbar Block ye Q= 8.73811408e+02 3 3 1.00502013e-01 # Ytau(Q)MSSM DRbar Block hmix Q= 8.73811408e+02 # Higgs mixing parameters 1 6.34225757e+02 # mu(Q)MSSM DRbar 2 9.66949856e+00 # tan beta(Q)MSSM DRbar 3 2.44043659e+02 # higgs vev(Q)MSSM DRbar 4 5.40020729e+05 # mA^2(Q)MSSM DRbar Block msoft Q= 8.73811408e+02 # MSSM DRbar SUSY breaking parameters 1 2.09217931e+02 # M_1(Q) 2 3.88513213e+02 # M_2(Q) 3 1.11375823e+03 # M_3(Q) 21 1.09175993e+05 # mH1^2(Q) 22 -3.89577899e+05 # mH2^2(Q) 31 3.54297503e+02 # meL(Q) 32 3.54294169e+02 # mmuL(Q) 33 3.53288859e+02 # mtauL(Q) 34 2.22024882e+02 # meR(Q) 35 2.22014061e+02 # mmuR(Q) 36 2.18730815e+02 # mtauR(Q) 41 1.01868349e+03 # mqL1(Q) 42 1.01868086e+03 # mqL2(Q) 43 9.38174894e+02 # mqL3(Q) 44 9.80660335e+02 # muR(Q) 45 9.80657548e+02 # mcR(Q) 46 8.05547302e+02 # mtR(Q) 47 9.76062679e+02 # mdR(Q) 48 9.76059936e+02 # msR(Q) 49 9.71058708e+02 # mbR(Q) Block au Q= 8.73811408e+02 1 1 -1.13744947e+03 # Au(Q)MSSM DRbar 2 2 -1.13744435e+03 # Ac(Q)MSSM DRbar 3 3 -8.73322525e+02 # At(Q)MSSM DRbar Block ad Q= 8.73811408e+02 1 1 -1.39629474e+03 # Ad(Q)MSSM DRbar 2 2 -1.39628999e+03 # As(Q)MSSM DRbar 3 3 -1.30365153e+03 # Ab(Q)MSSM DRbar Block ae Q= 8.73811408e+02 1 1 -2.99482647e+02 # Ae(Q)MSSM DRbar 2 2 -2.99477266e+02 # Amu(Q)MSSM DRbar 3 3 -2.97855048e+02 # Atau(Q)MSSM DRbar pythia8-8.1.80.orig/examples/main13.cc0000644000175000017500000000417412217346164015562 0ustar sunsun// main13.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how two Les Houches Event Files can be combined in PYTHIA, // just like in main12.cc, but here with the difference that information is // stored in main13.cmnd and read out using the subruns possibility. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Book histogram. Hist nCharged("charged particle multiplicity",100,-0.5,399.5); // Generator. Pythia pythia; // Read in subrun-independent data from main13.cmnd. pythia.readFile( "main13.cmnd", 0); // Extract data to be used in main program. Set counters. int nSubrun = pythia.mode("Main:numberOfSubruns"); int nAbort = pythia.mode("Main:timesAllowErrors"); int iAbort = 0; // Begin loop over subruns. for (int iSubrun = 1; iSubrun <= nSubrun; ++iSubrun) { // Read in subrun-specific data from main13.cmnd. pythia.readFile( "main13.cmnd", iSubrun); // Initialize generator. pythia.init(); // Begin infinite event loop - to be exited at end of file. for (int iEvent = 0; ; ++iEvent) { // Generate next event. if (!pythia.next()) { // Leave event loop if at end of file. if (pythia.info.atEndOfFile()) break; // First few failures write off as "acceptable" errors, then quit. if (++iAbort < nAbort) continue; break; } // Sum up final charged multiplicity and fill in histogram. int nChg = 0; for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].isFinal() && pythia.event[i].isCharged()) ++nChg; nCharged.fill(nChg); // End of event loop. } // End of subrun loop. } // Give statistics. Print histogram. pythia.stat(); cout << nCharged; // Done. return 0; } pythia8-8.1.80.orig/examples/main15.cc0000644000175000017500000001645512217346164015571 0ustar sunsun// main15.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how either // (a) B decays (sections marked "Repeated decays:), or // (b) all hadronization (sections marked "Repeated hadronization:") // could be repeated a number of times for each event, // to improve statistics when this could be a problem. // Option (a) is faster than (b), but less generic. // Note 1: the compartmentalization of hadronization in forceHadronLevel // from the rest of the event processing somewhat limits the ways the // program can retry in case of problems, and so an occasional abort // may occur more easily than normally. // Note 2: for simple cases, where it is only one particle that is to be // decayed repeatedly, the event[i].undoDecay() method is handy. // When used for several particles, remember that the position of // some particles may be moved by the undoDecay step. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Main switches: redo B decays only or redo all hadronization, but not both. bool redoBDecays = false; bool redoHadrons = true; if (redoHadrons) redoBDecays = false; // Number of events. Number to list redone events. int nEvent = 100; int nListRedo = 1; // Number of times decays/hadronization should be redone for each event. int nRepeat = 10; if (!redoBDecays && !redoHadrons) nRepeat = 1; // Generator. Shorthand for event. Pythia pythia; Event& event = pythia.event; // Simulate b production above given pTmin scale. // Warning: these processes do not catch all possible production modes. // You would need to use HardQCD:all or even SoftQCD:nonDiffractive for that. pythia.readString("HardQCD:gg2bbbar = on"); pythia.readString("HardQCD:qqbar2bbbar = on"); pythia.readString("PhaseSpace:pTHatMin = 50."); // Repeated decays: list of weakly decaying B hadrons. // Note: this list is overkill; some will never be produced. int bCodes[28] = {511, 521, 531, 541, 5122, 5132, 5142, 5232, 5242, 5332, 5342, 5412, 5414, 5422, 5424, 5432, 5434, 5442, 5444, 5512, 5514, 5522, 5524, 5532, 5534, 5542, 5544, 5544 }; int nCodes = 28; // Repeated decays: location of B handrons. vector iBHad; int nBHad = 0; // Repeated hadronization: spare copy of event. Event savedEvent; // Repeated hadronization: switch off normal HadronLevel call. if (redoHadrons) pythia.readString("HadronLevel:all = off"); // Initialize for LHC energies; default 14 TeV pythia.init(); // Histogram invariant mass of muon pairs. Hist nBperEvent("number of b quarks in an event", 10, -0.5, 9.5); Hist nSameEvent("number of times same event is used", 10, -0.5, 9.5); Hist oppSignMass("mass of opposite-sign muon pair", 100, 0.0, 100.0); Hist sameSignMass("mass of same-sign muon pair", 100, 0.0, 100.0); // Begin event loop. for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Repeated decays: switch off decays of weakly decaying B hadrons. // (More compact solution than repeated readString(..).) if (redoBDecays) for (int iC = 0; iC < nCodes; ++iC) pythia.particleData.mayDecay( bCodes[iC], false); // Generate event. Skip it if error. if (!pythia.next()) continue; // Find and histogram number of b quarks. int nBquark = 0; int stat; for (int i = 0; i < event.size(); ++i) { stat = event[i].statusAbs(); if (event[i].idAbs() == 5 && (stat == 62 || stat == 63)) ++nBquark; } nBperEvent.fill( nBquark ); // Repeated decays: find all locations where B hadrons are stored. if (redoBDecays) { iBHad.resize(0); for (int i = 0; i < event.size(); ++i) { int idAbs = event[i].idAbs(); for (int iC = 0; iC < 28; ++iC) if (idAbs == bCodes[iC]) { iBHad.push_back(i); break; } } // Repeated decays: check that #b = #B. nBHad = iBHad.size(); if (nBquark != nBHad) cout << " Warning: " << nBquark << " b quarks but " << nBHad << " B hadrons" << endl; // Repeated decays: store size of current event. event.saveSize(); // Repeated decays: switch back on weakly decaying B hadrons. for (int iC = 0; iC < nCodes; ++iC) pythia.particleData.mayDecay( bCodes[iC], true); // Repeated hadronization: copy event into spare position. } else if (redoHadrons) { savedEvent = event; } // Begin loop over rounds of decays / hadronization for same event. int nWithPair = 0; for (int iRepeat = 0; iRepeat < nRepeat; ++iRepeat) { // Repeated decays: remove B decay products from previous round. if (redoBDecays) { if (iRepeat > 0) { event.restoreSize(); // Repeated decays: mark decayed B hadrons as undecayed. for (int iB = 0; iB < nBHad; ++iB) event[ iBHad[iB] ].statusPos(); } // Repeated decays: do decays of B hadrons, sequentially for products. // Note: modeDecays does not work for bottomonium (or heavier) states, // since there decays like Upsilon -> g g g also need hadronization. // Also, there is no provision for Bose-Einstein effects. if (!pythia.moreDecays()) continue; // Repeated hadronization: restore saved event record. } else if (redoHadrons) { if (iRepeat > 0) event = savedEvent; // Repeated hadronization: do HadronLevel (repeatedly). // Note: argument false needed owing to bug in junction search?? if (!pythia.forceHadronLevel(false)) continue; } // List last repetition of first few events. if ( (redoBDecays || redoHadrons) && iEvent < nListRedo && iRepeat == nRepeat - 1) event.list(); // Look for muons among decay products (also from charm/tau/...). vector iMuNeg, iMuPos; for (int i = 0; i < event.size(); ++i) { int id = event[i].id(); if (id == 13) iMuNeg.push_back(i); if (id == -13) iMuPos.push_back(i); } // Check whether pair(s) present. int nMuNeg = iMuNeg.size(); int nMuPos = iMuPos.size(); if (nMuNeg + nMuPos > 1) { ++nWithPair; // Fill masses of opposite-sign pairs. for (int iN = 0; iN < nMuNeg; ++iN) for (int iP = 0; iP < nMuPos; ++iP) oppSignMass.fill( (event[iMuNeg[iN]].p() + event[iMuPos[iP]].p()).mCalc() ); // Fill masses of same-sign pairs. for (int i1 = 0; i1 < nMuNeg - 1; ++i1) for (int i2 = i1 + 1; i2 < nMuNeg; ++i2) sameSignMass.fill( (event[iMuNeg[i1]].p() + event[iMuNeg[i2]].p()).mCalc() ); for (int i1 = 0; i1 < nMuPos - 1; ++i1) for (int i2 = i1 + 1; i2 < nMuPos; ++i2) sameSignMass.fill( (event[iMuPos[i1]].p() + event[iMuPos[i2]].p()).mCalc() ); // Finished analysis of current round. } // End of loop over many rounds. fill number of rounds with pairs. } nSameEvent.fill( nWithPair ); // End of event loop. } // Statistics. Histograms. pythia.stat(); cout << nBperEvent << nSameEvent << oppSignMass << sameSignMass << endl; // Done. return 0; } pythia8-8.1.80.orig/examples/w_production_tree_2.lhe0000644000175000017500000070574312217346211020634 0ustar sunsun
      # MG version : 5.1.5.5 #************************************************************ #* MadGraph 5 * #* * #* * * * #* * * * * * #* * * * * 5 * * * * * #* * * * * * #* * * * #* * #* * #* VERSION 1.5.5 2012-11-18 * #* * #* The MadGraph Development Team - Please visit us at * #* https://server06.fynu.ucl.ac.be/projects/madgraph * #* * #************************************************************ #* * #* Command File for MadGraph 5 * #* * #* run as ./bin/mg5 filename * #* * #************************************************************ set group_subprocesses Auto set ignore_six_quark_processes False set gauge unitary set complex_mass_scheme False import model sm define p = g u c d s u~ c~ d~ s~ define j = g u c d s u~ c~ d~ s~ define l+ = e+ mu+ define l- = e- mu- define vl = ve vm vt define vl~ = ve~ vm~ vt~ # Specify process(es) to run generate p p > w+ j j , w+ > e+ ve QED=2 @1 add process p p > w- j j , w- > e- ve~ QED=2 @2 # Output processes to MadEvent directory output -f #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # proc_card.dat * #********************************************************************* # * # This Files is generated by MADGRAPH 5 * # * # WARNING: This Files is generated for MADEVENT (compatibility issue)* # This files is NOT a valid MG4 proc_card.dat * # Running this in MG4 will NEVER reproduce the result of MG5* # * #********************************************************************* #********************************************************************* # Process(es) requested : mg2 input * #********************************************************************* # Begin PROCESS # This is TAG. Do not modify this line p p > w+ j j , w+ > e+ ve @1 #Process # Be carefull the coupling are here in MG5 convention QED=2 end_coup # End the couplings input done # this tells MG there are no more procs # End PROCESS # This is TAG. Do not modify this line #********************************************************************* # Model information * #********************************************************************* # Begin MODEL # This is TAG. Do not modify this line sm # End MODEL # This is TAG. Do not modify this line #********************************************************************* # Start multiparticle definitions * #********************************************************************* # Begin MULTIPARTICLES # This is TAG. Do not modify this line # End MULTIPARTICLES # This is TAG. Do not modify this line ###################################################################### ## PARAM_CARD AUTOMATICALY GENERATED BY MG5 FOLLOWING UFO MODEL #### ###################################################################### ## ## ## Width set on Auto will be computed following the information ## ## present in the decay.py files of the model. By default, ## ## this is only 1->2 decay modes. ## ## ## ###################################################################### ################################### ## INFORMATION FOR MASS ################################### Block mass 5 4.700000e+00 # MB 6 1.730000e+02 # MT 15 1.777000e+00 # MTA 23 9.118800e+01 # MZ 25 1.200000e+02 # MH ## Not dependent paramater. ## Those values should be edited following the ## analytical expression. MG5 ignore those values ## but they are important for interfacing the output of MG5 ## to external program such as Pythia. 1 0.000000 # d : 0.0 2 0.000000 # u : 0.0 3 0.000000 # s : 0.0 4 0.000000 # c : 0.0 11 0.000000 # e- : 0.0 12 0.000000 # ve : 0.0 13 0.000000 # mu- : 0.0 14 0.000000 # vm : 0.0 16 0.000000 # vt : 0.0 21 0.000000 # g : 0.0 22 0.000000 # a : 0.0 24 80.419002 # w+ : cmath.sqrt(MZ__exp__2/2. + cmath.sqrt(MZ__exp__4/4. - (aEW*cmath.pi*MZ__exp__2)/(Gf*sqrt__2))) ################################### ## INFORMATION FOR SMINPUTS ################################### Block sminputs 1 1.325070e+02 # aEWM1 2 1.166390e-05 # Gf 3 1.180000e-01 # aS ################################### ## INFORMATION FOR YUKAWA ################################### Block yukawa 5 4.200000e+00 # ymb 6 1.645000e+02 # ymt 15 1.777000e+00 # ymtau ################################### ## INFORMATION FOR DECAY ################################### DECAY 6 1.491500e+00 # WT DECAY 23 2.441404e+00 # WZ DECAY 24 2.047600e+00 # WW DECAY 25 5.753088e-03 # WH ## Not dependent paramater. ## Those values should be edited following the ## analytical expression. MG5 ignore those values ## but they are important for interfacing the output of MG5 ## to external program such as Pythia. DECAY 1 0.000000 # d : 0.0 DECAY 2 0.000000 # u : 0.0 DECAY 3 0.000000 # s : 0.0 DECAY 4 0.000000 # c : 0.0 DECAY 5 0.000000 # b : 0.0 DECAY 11 0.000000 # e- : 0.0 DECAY 12 0.000000 # ve : 0.0 DECAY 13 0.000000 # mu- : 0.0 DECAY 14 0.000000 # vm : 0.0 DECAY 15 0.000000 # ta- : 0.0 DECAY 16 0.000000 # vt : 0.0 DECAY 21 0.000000 # g : 0.0 DECAY 22 0.000000 # a : 0.0 #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # run_card.dat * # * # This file is used to set the parameters of the run. * # * # Some notation/conventions: * # * # Lines starting with a '# ' are info or comments * # * # mind the format: value = variable ! comment * #********************************************************************* # #******************* # Running parameters #******************* # #********************************************************************* # Tag name for the run (one word) * #********************************************************************* tag_1 = run_tag ! name of the run #********************************************************************* # Run to generate the grid pack * #********************************************************************* .false. = gridpack !True = setting up the grid pack #********************************************************************* # Number of events and rnd seed * # Warning: Do not generate more than 1M events in a single run * # If you want to run Pythia, avoid more than 50k events in a run. * #********************************************************************* 1000 = nevents ! Number of unweighted events requested 387 = iseed ! rnd seed (0=assigned automatically=default)) #********************************************************************* # Collider type and energy * # lpp: 0=No PDF, 1=proton, -1=antiproton, 2=photon from proton, * # 3=photon from electron * #********************************************************************* 1 = lpp1 ! beam 1 type 1 = lpp2 ! beam 2 type 3500 = ebeam1 ! beam 1 total energy in GeV 3500 = ebeam2 ! beam 2 total energy in GeV #********************************************************************* # Beam polarization from -100 (left-handed) to 100 (right-handed) * #********************************************************************* 0 = polbeam1 ! beam polarization for beam 1 0 = polbeam2 ! beam polarization for beam 2 #********************************************************************* # PDF CHOICE: this automatically fixes also alpha_s and its evol. * #********************************************************************* 'lhapdf' = pdlabel ! PDF set 10042 = lhaid ! PDF set cteq6m #********************************************************************* # Renormalization and factorization scales * #********************************************************************* T = fixed_ren_scale ! if .true. use fixed ren scale T = fixed_fac_scale ! if .true. use fixed fac scale 91.1880 = scale ! fixed ren scale 80.4 = dsqrt_q2fact1 ! fixed fact scale for pdf1 80.4 = dsqrt_q2fact2 ! fixed fact scale for pdf2 1 = scalefact ! scale factor for event-by-event scales #********************************************************************* # Matching - Warning! ickkw > 1 is still beta #********************************************************************* 0 = ickkw ! 0 no matching, 1 MLM, 2 CKKW matching 1 = highestmult ! for ickkw=2, highest mult group 1 = ktscheme ! for ickkw=1, 1 Durham kT, 2 Pythia pTE 1 = alpsfact ! scale factor for QCD emission vx F = chcluster ! cluster only according to channel diag F = pdfwgt ! for ickkw=1, perform pdf reweighting #********************************************************************* # Automatic ptj and mjj cuts if xqcut > 0 # (turn off for VBF and single top processes) #********************************************************** F = auto_ptj_mjj ! Automatic setting of ptj and mjj #********************************************************** # #********************************** # BW cutoff (M+/-bwcutoff*Gamma) #********************************** 5 = bwcutoff ! (M+/-bwcutoff*Gamma) #********************************************************** # Apply pt/E/eta/dr/mij cuts on decay products or not # (note that etmiss/ptll/ptheavy/ht/sorted cuts always apply) #********************************************************** F = cut_decays ! Cut decay products #************************************************************* # Number of helicities to sum per event (0 = all helicities) # 0 gives more stable result, but longer run time (needed for # long decay chains e.g.). # Use >=2 if most helicities contribute, e.g. pure QCD. #************************************************************* 0 = nhel ! Number of helicities used per event #******************* # Standard Cuts #******************* # #********************************************************************* # Minimum and maximum pt's (for max, -1 means no cut) * #********************************************************************* 5 = ptj ! minimum pt for the jets 0 = ptb ! minimum pt for the b 0 = pta ! minimum pt for the photons 0 = ptl ! minimum pt for the charged leptons 0 = misset ! minimum missing Et (sum of neutrino's momenta) 0 = ptheavy ! minimum pt for one heavy final state 0 = ptonium ! minimum pt for the quarkonium states -1 = ptjmax ! maximum pt for the jets -1 = ptbmax ! maximum pt for the b -1 = ptamax ! maximum pt for the photons -1 = ptlmax ! maximum pt for the charged leptons -1 = missetmax ! maximum missing Et (sum of neutrino's momenta) #********************************************************************* # Minimum and maximum E's (in the lab frame) * #********************************************************************* 0 = ej ! minimum E for the jets 0 = eb ! minimum E for the b 0 = ea ! minimum E for the photons 0 = el ! minimum E for the charged leptons -1 = ejmax ! maximum E for the jets -1 = ebmax ! maximum E for the b -1 = eamax ! maximum E for the photons -1 = elmax ! maximum E for the charged leptons #********************************************************************* # Maximum and minimum absolute rapidity (for max, -1 means no cut) * #********************************************************************* -1 = etaj ! max rap for the jets -1 = etab ! max rap for the b -1 = etaa ! max rap for the photons -1 = etal ! max rap for the charged leptons -1 = etaonium ! max rap for the quarkonium states 0 = etajmin ! min rap for the jets 0 = etabmin ! min rap for the b 0 = etaamin ! min rap for the photons 0 = etalmin ! main rap for the charged leptons #********************************************************************* # Minimum and maximum DeltaR distance * #********************************************************************* 1d-2 = drjj ! min distance between jets 0 = drbb ! min distance between b's 0 = drll ! min distance between leptons 0 = draa ! min distance between gammas 0 = drbj ! min distance between b and jet 0 = draj ! min distance between gamma and jet 0 = drjl ! min distance between jet and lepton 0 = drab ! min distance between gamma and b 0 = drbl ! min distance between b and lepton 0 = dral ! min distance between gamma and lepton -1 = drjjmax ! max distance between jets -1 = drbbmax ! max distance between b's -1 = drllmax ! max distance between leptons -1 = draamax ! max distance between gammas -1 = drbjmax ! max distance between b and jet -1 = drajmax ! max distance between gamma and jet -1 = drjlmax ! max distance between jet and lepton -1 = drabmax ! max distance between gamma and b -1 = drblmax ! max distance between b and lepton -1 = dralmax ! maxdistance between gamma and lepton #********************************************************************* # Minimum and maximum invariant mass for pairs * #********************************************************************* 5.0 = mmjj ! min invariant mass of a jet pair 0 = mmbb ! min invariant mass of a b pair 0 = mmaa ! min invariant mass of gamma gamma pair 0 = mmll ! min invariant mass of l+l- (same flavour) lepton pair -1 = mmjjmax ! max invariant mass of a jet pair -1 = mmbbmax ! max invariant mass of a b pair -1 = mmaamax ! max invariant mass of gamma gamma pair -1 = mmllmax ! max invariant mass of l+l- (same flavour) lepton pair #********************************************************************* # Minimum and maximum invariant mass for all letpons * #********************************************************************* 0 = mmnl ! min invariant mass for all letpons (l+- and vl) -1 = mmnlmax ! max invariant mass for all letpons (l+- and vl) #********************************************************************* # Minimum and maximum pt for 4-momenta sum of leptons * #********************************************************************* 0 = ptllmin ! Minimum pt for 4-momenta sum of leptons(l and vl) -1 = ptllmax ! Maximum pt for 4-momenta sum of leptons(l and vl) #********************************************************************* # Inclusive cuts * #********************************************************************* 0 = xptj ! minimum pt for at least one jet 0 = xptb ! minimum pt for at least one b 0 = xpta ! minimum pt for at least one photon 0 = xptl ! minimum pt for at least one charged lepton #********************************************************************* # Control the pt's of the jets sorted by pt * #********************************************************************* 0 = ptj1min ! minimum pt for the leading jet in pt 0 = ptj2min ! minimum pt for the second jet in pt 0 = ptj3min ! minimum pt for the third jet in pt 0 = ptj4min ! minimum pt for the fourth jet in pt -1 = ptj1max ! maximum pt for the leading jet in pt -1 = ptj2max ! maximum pt for the second jet in pt -1 = ptj3max ! maximum pt for the third jet in pt -1 = ptj4max ! maximum pt for the fourth jet in pt 0 = cutuse ! reject event if fails any (0) / all (1) jet pt cuts #********************************************************************* # Control the pt's of leptons sorted by pt * #********************************************************************* 0 = ptl1min ! minimum pt for the leading lepton in pt 0 = ptl2min ! minimum pt for the second lepton in pt 0 = ptl3min ! minimum pt for the third lepton in pt 0 = ptl4min ! minimum pt for the fourth lepton in pt -1 = ptl1max ! maximum pt for the leading lepton in pt -1 = ptl2max ! maximum pt for the second lepton in pt -1 = ptl3max ! maximum pt for the third lepton in pt -1 = ptl4max ! maximum pt for the fourth lepton in pt #********************************************************************* # Control the Ht(k)=Sum of k leading jets * #********************************************************************* 0 = htjmin ! minimum jet HT=Sum(jet pt) -1 = htjmax ! maximum jet HT=Sum(jet pt) 0 = ihtmin !inclusive Ht for all partons (including b) -1 = ihtmax !inclusive Ht for all partons (including b) 0 = ht2min ! minimum Ht for the two leading jets 0 = ht3min ! minimum Ht for the three leading jets 0 = ht4min ! minimum Ht for the four leading jets -1 = ht2max ! maximum Ht for the two leading jets -1 = ht3max ! maximum Ht for the three leading jets -1 = ht4max ! maximum Ht for the four leading jets #********************************************************************* # WBF cuts * #********************************************************************* 0 = xetamin ! minimum rapidity for two jets in the WBF case 0 = deltaeta ! minimum rapidity for two jets in the WBF case #********************************************************************* # maximal pdg code for quark to be considered as a light jet * # (otherwise b cuts are applied) * #********************************************************************* 4 = maxjetflavor ! Maximum jet pdg code #********************************************************************* # Jet measure cuts * #********************************************************************* 2.0 = xqcut ! minimum kt jet measure between partons #********************************************************************* 0d0 = kt_durham ! minimum durham kt jet measure between partons 0.4 = d_parameter ! D parameter for hadronic kT F = do_kt_durham ! T: enable durham kt cut 15 = pt_pythia ! minimum pythia pt jet measure between partons 2 = njets_requested ! number of jets above the pythia pt cut T = do_pt_pythia ! T: enable pythia pt cut #********************************************************************* # Number of Events : 1000 # Integrated weight (pb) : .91728E+03 # Truncated wgt (pb) : .00000E+00 # Unit wgt : .91728E+00
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      pythia8-8.1.80.orig/examples/main12.cc0000644000175000017500000000751112217346164015557 0ustar sunsun// main12.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how Les Houches Event File input can be used in PYTHIA. // It uses two LHE files, ttbar.lhe and ttbar2.lhe, which are combined // using Beams:newLHEFsameInit = on to skip new initialization second time. // Then the second file is viewed as a simple continuation of the first, // just split for practical reasons, rather than as a separate new run // with a new set of processes. // In the first file top decays have been performed, in the second not, // and are instead handled by the internal PYTHIA resonance-decay machinery. // Furthermore the internal top production processes are switched on and // mixed in, giving an unrealistic "double up" total top cross section. // Much of this of course is not intended to be realistic, // but rather illustrates several tricks that can be useful. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Number of listed events. Allow for possibility of a few faulty events. int nPrintLHA = 1; int nPrintRest = 0; int nAbort = 10; // Generator Pythia pythia; // Switch on internal ttbar production. pythia.readString("Top:gg2ttbar = on"); pythia.readString("Top:qqbar2ttbar = on"); // Use same top mass as in Pythia 6.4 to simplify comparison. pythia.readString("6:m0 = 175."); // No automatic event listings - do it manually below. pythia.readString("Next:numberShowLHA = 0"); pythia.readString("Next:numberShowInfo = 0"); pythia.readString("Next:numberShowProcess = 0"); pythia.readString("Next:numberShowEvent = 0"); // Initialize Les Houches Event File run. pythia.readString("Beams:frameType = 4"); pythia.readString("Beams:LHEF = ttbar.lhe"); pythia.init(); // Book histogram. Hist nCharged("charged particle multiplicity",100,-0.5,399.5); // Set counters. int iPrintLHA = 0; int iPrintRest = 0; int iAbort = 0; int iFile = 1; // Begin event loop for (int iEvent = 0; ; ++iEvent) { // Generate until none left in input file. if (!pythia.next()) { if (pythia.info.atEndOfFile()) { // First time open next file, second time stop event loop. if (iFile == 1) { pythia.readString("Beams:newLHEFsameInit = on"); pythia.readString("Beams:LHEF = ttbar2.lhe"); pythia.init(); ++iFile; continue; } else break; } // First few failures write off as "acceptable" errors, then quit. if (++iAbort < nAbort) continue; break; } // List first few Les Houches and other events. if (pythia.info.isLHA() && iPrintLHA < nPrintLHA) { pythia.LHAeventList(); pythia.info.list(); pythia.process.list(); pythia.event.list(); ++iPrintLHA; } else if (!pythia.info.isLHA() && iPrintRest < nPrintRest) { pythia.info.list(); pythia.process.list(); pythia.event.list(); ++iPrintRest; } // Sum up final charged multiplicity and fill in histogram. int nChg = 0; for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].isFinal() && pythia.event[i].isCharged()) ++nChg; nCharged.fill(nChg); // End of event loop. } // Give statistics. Print histogram. pythia.stat(); cout << nCharged; // Done. return 0; } pythia8-8.1.80.orig/examples/main06.cc0000644000175000017500000001147212217346163015562 0ustar sunsun// main06.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It studies event properties of LEP1 events. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator. Pythia pythia; // Allow no substructure in e+- beams: normal for corrected LEP data. pythia.readString("PDF:lepton = off"); // Process selection. pythia.readString("WeakSingleBoson:ffbar2gmZ = on"); // Switch off all Z0 decays and then switch back on those to quarks. pythia.readString("23:onMode = off"); pythia.readString("23:onIfAny = 1 2 3 4 5"); // LEP1 initialization at Z0 mass. pythia.readString("Beams:idA = 11"); pythia.readString("Beams:idB = -11"); double mZ = pythia.particleData.m0(23); pythia.settings.parm("Beams:eCM", mZ); pythia.init(); // Histograms. Hist nCharge("charged multiplicity", 100, -0.5, 99.5); Hist spheri("Sphericity", 100, 0., 1.); Hist linea("Linearity", 100, 0., 1.); Hist thrust("thrust", 100, 0.5, 1.); Hist oblateness("oblateness", 100, 0., 1.); Hist sAxis("cos(theta_Sphericity)", 100, -1., 1.); Hist lAxis("cos(theta_Linearity)", 100, -1., 1.); Hist tAxis("cos(theta_Thrust)", 100, -1., 1.); Hist nLund("Lund jet multiplicity", 40, -0.5, 39.5); Hist nJade("Jade jet multiplicity", 40, -0.5, 39.5); Hist nDurham("Durham jet multiplicity", 40, -0.5, 39.5); Hist eDifLund("Lund e_i - e_{i+1}", 100, -5.,45.); Hist eDifJade("Jade e_i - e_{i+1}", 100, -5.,45.); Hist eDifDurham("Durham e_i - e_{i+1}", 100, -5.,45.); // Set up Sphericity, "Linearity", Thrust and cluster jet analyses. Sphericity sph; Sphericity lin(1.); Thrust thr; ClusterJet lund("Lund"); ClusterJet jade("Jade"); ClusterJet durham("Durham"); // Begin event loop. Generate event. Skip if error. List first few. for (int iEvent = 0; iEvent < 10000; ++iEvent) { if (!pythia.next()) continue; // Find and histogram charged multiplicity. int nCh = 0; for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].isFinal() && pythia.event[i].isCharged()) ++nCh; nCharge.fill( nCh ); // Find and histogram sphericity. if (sph.analyze( pythia.event )) { if (iEvent < 3) sph.list(); spheri.fill( sph.sphericity() ); sAxis.fill( sph.eventAxis(1).pz() ); double e1 = sph.eigenValue(1); double e2 = sph.eigenValue(2); double e3 = sph.eigenValue(3); if (e2 > e1 || e3 > e2) cout << "eigenvalues out of order: " << e1 << " " << e2 << " " << e3 << endl; } // Find and histogram linearized sphericity. if (lin.analyze( pythia.event )) { if (iEvent < 3) lin.list(); linea.fill( lin.sphericity() ); lAxis.fill( lin.eventAxis(1).pz() ); double e1 = lin.eigenValue(1); double e2 = lin.eigenValue(2); double e3 = lin.eigenValue(3); if (e2 > e1 || e3 > e2) cout << "eigenvalues out of order: " << e1 << " " << e2 << " " << e3 << endl; } // Find and histogram thrust. if (thr.analyze( pythia.event )) { if (iEvent < 3) thr.list(); thrust.fill( thr.thrust() ); oblateness.fill( thr.oblateness() ); tAxis.fill( thr.eventAxis(1).pz() ); if ( abs(thr.eventAxis(1).pAbs() - 1.) > 1e-8 || abs(thr.eventAxis(2).pAbs() - 1.) > 1e-8 || abs(thr.eventAxis(3).pAbs() - 1.) > 1e-8 || abs(thr.eventAxis(1) * thr.eventAxis(2)) > 1e-8 || abs(thr.eventAxis(1) * thr.eventAxis(3)) > 1e-8 || abs(thr.eventAxis(2) * thr.eventAxis(3)) > 1e-8 ) { cout << " suspicious Thrust eigenvectors " << endl; thr.list(); } } // Find and histogram cluster jets: Lund, Jade and Durham distance. if (lund.analyze( pythia.event, 0.01, 0.)) { if (iEvent < 3) lund.list(); nLund.fill( lund.size() ); for (int j = 0; j < lund.size() - 1; ++j) eDifLund.fill( lund.p(j).e() - lund.p(j+1).e() ); } if (jade.analyze( pythia.event, 0.01, 0.)) { if (iEvent < 3) jade.list(); nJade.fill( jade.size() ); for (int j = 0; j < jade.size() - 1; ++j) eDifJade.fill( jade.p(j).e() - jade.p(j+1).e() ); } if (durham.analyze( pythia.event, 0.01, 0.)) { if (iEvent < 3) durham.list(); nDurham.fill( durham.size() ); for (int j = 0; j < durham.size() - 1; ++j) eDifDurham.fill( durham.p(j).e() - durham.p(j+1).e() ); } // End of event loop. Statistics. Output histograms. } pythia.stat(); cout << nCharge << spheri << linea << thrust << oblateness << sAxis << lAxis << tAxis << nLund << nJade << nDurham << eDifLund << eDifJade << eDifDurham; // Done. return 0; } pythia8-8.1.80.orig/examples/photoninproton.lhe0000644000175000017500000000237612217346205017753 0ustar sunsun 2212 2212 7.000000E+03 7.000000E+03 0 0 20400 20400 -3 1 5.441 0.213 1.000000E+00 10001 6 10001 1 91.1876 0.0072973525679 0.1176 3 -1 0 0 501 0 0 0 13.9260428506 13.9268506661 0.15 0. 9. 22 -1 0 0 0 0 0 0 -143.300093156 143.300093156 0 0. 9. 3 1 1 2 501 0 0.123089545501 0.57536030523 3.57351962704 3.62473903086 0.15 0. 9. 23 2 1 2 0 0 -0.123097411612 -0.575397073974 -132.949026139 153.60346533 76.9300641834 0. 9. -13 1 4 4 0 0 17.868156742 17.3756611276 -8.11961843096 26.2130500349 0.105658368999 0. 9. 13 1 4 4 0 0 -17.9912541536 -17.9510582016 -124.829407708 127.390415295 0.105658369006 0. 9. pythia8-8.1.80.orig/examples/main51.cc0000644000175000017500000001120012217346166015552 0ustar sunsun// main51.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Test of LHAPDF interface and whether PDF's behave sensibly. #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // Integration to check momentum sum rule. double integrate(PDF* nowPDF, double Q2) { // Number of points, x ranges and initial values. int nLin = 980; int nLog = 1000; double xLin = 0.02; double xLog = 1e-8; double dxLin = (1. - xLin) / nLin; double dxLog = log(xLin / xLog) / nLog; double sum = 0.; double x, sumNow; // Integration at large x in linear steps. for (int iLin = 0; iLin < nLin; ++iLin) { x = xLin + (iLin + 0.5) * dxLin; sumNow = nowPDF->xf( 21, x, Q2); for (int i = 1; i < 6; ++i) sumNow += nowPDF->xf( i, x, Q2) + nowPDF->xf( -i, x, Q2); sum += dxLin * sumNow; } // Integration at small x in logarithmic steps. for (int iLog = 0; iLog < nLog; ++iLog) { x = xLog * pow( xLin / xLog, (iLog + 0.5) / nLog ); sumNow = nowPDF->xf( 21, x, Q2); for (int i = 1; i < 6; ++i) sumNow += nowPDF->xf( i, x, Q2) + nowPDF->xf( -i, x, Q2); sum += dxLog * x * sumNow; } // Done. return sum; } //========================================================================== int main() { // The Pythia class itself is not used, but some facilities that come along. //Pythia pythia; // Chosen new PDF set; LHAPDF file name conventions. //string pdfSet = "cteq5l.LHgrid"; //string pdfSet = "cteq61.LHpdf"; //string pdfSet = "cteq61.LHgrid"; //string pdfSet = "MRST2004nlo.LHgrid"; //string pdfSet = "MRST2001lo.LHgrid"; string pdfSet = "MRST2007lomod.LHgrid"; // Pointers to old default and new tryout PDF sets. PDF* oldPDF = new CTEQ5L(2212); PDF* newPDF = new LHAPDF(2212, pdfSet, 0); // Alternative: compare two Pomeron PDF's. Boost second by factor 2. //PDF* oldPDF = new PomFix( 990, -0.2, 2.5, 0., 3., 0.4, 0.5); //PDF* newPDF = new PomH1Jets( 990, 2.); //PDF* oldPDF = new PomH1FitAB( 990, 2); //PDF* newPDF = new PomH1FitAB( 990, 3); // Allow extrapolation of PDF's beyond x and Q2 boundaries, at own risk. // Default behaviour is to freeze PDF's at boundaries. newPDF->setExtrapolate(true); // Histogram F(x, Q2) = (9/4) x*g(x, Q2) + sum_{i = q, qbar} x*f_i(x, Q2) // for range 10^{-8} < x < 1 logarithmic in x and for Q2 = 4 and 100. Hist oldF4("F( x, Q2 = 4) old", 80 , -8., 0.); Hist newF4("F( x, Q2 = 4) new", 80 , -8., 0.); Hist ratF4("F( x, Q2 = 4) new/old", 80 , -8., 0.); Hist oldF100("F( x, Q2 = 100) old", 80 , -8., 0.); Hist newF100("F( x, Q2 = 100) new", 80 , -8., 0.); Hist ratF100("F( x, Q2 = 100) new/old", 80 , -8., 0.); // Loop over the two Q2 values. for (int iQ = 0; iQ < 2; ++iQ) { double Q2 = (iQ == 0) ? 4. : 100; // Loop over x values, in a logarithmic scale for (int iX = 0; iX < 80; ++iX) { double xLog = -(0.1 * iX + 0.05); double x = pow( 10., xLog); // Evaluate old summed PDF. double oldSum = 2.25 * oldPDF->xf( 21, x, Q2); for (int i = 1; i < 6; ++i) oldSum += oldPDF->xf( i, x, Q2) + oldPDF->xf( -i, x, Q2); if (iQ == 0) oldF4.fill ( xLog, oldSum ); else oldF100.fill ( xLog, oldSum ); // Evaluate new summed PDF. double newSum = 2.25 * newPDF->xf( 21, x, Q2); for (int i = 1; i < 6; ++i) newSum += newPDF->xf( i, x, Q2) + newPDF->xf( -i, x, Q2); if (iQ == 0) newF4.fill ( xLog, newSum ); else newF100.fill ( xLog, newSum ); //End loops over x and Q2 values. } } // Show F(x, Q2) and their ratio new/old. ratF4 = newF4 / oldF4; ratF100 = newF100 / oldF100; cout << oldF4 << newF4 << ratF4 << oldF100 << newF100 << ratF100; // Histogram momentum sum as a function of Q2 (or rather log10(Q2)). Hist oldXSum("momentum sum(log10(Q2)) old", 100, -2., 8.); Hist newXSum("momentum sum(log10(Q2)) new", 100, -2., 8.); // Loop over Q2 values. for (int iQ = 0; iQ < 100; ++iQ) { double log10Q2 = -2.0 + 0.1 * iQ + 0.05; double Q2 = pow( 10., log10Q2); // Evaluate old and new momentum sums. double oldSum = integrate( oldPDF, Q2); oldXSum.fill( log10Q2, oldSum); double newSum = integrate( newPDF, Q2); newXSum.fill( log10Q2, newSum); } // Show momentum sum as a function of Q2. cout << oldXSum << newXSum; // Done. delete oldPDF; delete newPDF; return 0; } pythia8-8.1.80.orig/examples/main13.cmnd0000644000175000017500000000277212217346164016120 0ustar sunsun! main13.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! Names are case-insensitive - but spellings-sensitive! ! The settings here are illustrative, not always physics-motivated. ! 1) Settings used in the main program. Main:timesAllowErrors = 3 ! how many aborts before run stops ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showChangedParticleData = off ! list changed particle data Next:numberCount = 0 ! print message every n events, 0 = off Next:numberShowLHA = 1 ! print LHA information n times Next:numberShowInfo = 1 ! print event information n times Next:numberShowProcess = 1 ! print process record n times Next:numberShowEvent = 0 ! print event record n times ! 3) Other common settings. 6:m0 = 175. ! same m_t as Pythia 6.4 to compare ! 4) The number of subruns to execute. Main:numberOfSubruns = 2 ! 5) Information specific to the first subrun Main:subrun = 1 ! matches readFile( ..., 1) Beams:frameType = 4 ! use LHEF input Beams:LHEF = ttbar.lhe ! first LHEF event file ! 6) Information specific to the second subrun Main:subrun = 2 ! matches readFile( ..., 2) Beams:newLHEFsameInit = on ! no reinitialization needed/wanted Beams:LHEF = ttbar2.lhe ! second LHEF event file pythia8-8.1.80.orig/examples/main88.cc0000644000175000017500000005556412217346170015604 0ustar sunsun// main88.cc is a part of the PYTHIA event generator. // Copyright (C) 2011 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This program is written by Stefan Prestel. // It illustrates how to do UNLOPS merging, // see the NLO Merging page in the online manual. #include "Pythia8/Pythia.h" #include "Pythia8/Pythia8ToHepMC.h" #include "HepMC/GenEvent.h" #include "HepMC/IO_GenEvent.h" // Following line to be used with HepMC 2.04 onwards. #include "HepMC/Units.h" using namespace Pythia8; //========================================================================== // Example main programm to illustrate UNLOPS merging int main( int argc, char* argv[] ){ // Check that correct number of command-line arguments if (argc != 4) { cerr << " Unexpected number of command-line arguments ("< xsecLO; vector nSelectedLO; vector nAcceptLO; vector strategyLO; cout << endl << endl << endl; cout << "Start estimating unlops tree level cross section" << endl; while(njetcounterLO >= 0){ // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathTree+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathTree + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); pythia.settings.mode("Merging:nRequested", njetcounterLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Start generation loop for( int iEvent=0; iEvent 0 ) njetcounterLO--; else break; } //----------------------------------------------------------------------------- //----------------------------------------------------------------------------- cout << endl << endl << endl; cout << "Start estimating unlops virtual corrections cross section" << endl; pythia.settings.flag("Merging:doUNLOPSTree",false); pythia.settings.flag("Merging:doUNLOPSLoop", true); int njetcounterNLO = nMaxNLO; string iPathLoop = iPath + "_powheg"; // Save estimates in vectors. vector xsecNLO; vector nSelectedNLO; vector nAcceptNLO; vector strategyNLO; while(njetcounterNLO >= 0){ // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterNLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathLoop+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathLoop + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); pythia.settings.mode("Merging:nRequested", njetcounterNLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Start generation loop for( int iEvent=0; iEvent 0 ) njetcounterNLO--; else break; } // Set k-factors int sizeLO = int(xsecLO.size()); int sizeNLO = int(xsecNLO.size()); double k0 = 1.; double k1 = 1.; double k2 = 1.; // Lowest order k-factor only if ( false ) k1 = k2 = k0 = xsecNLO.back() / xsecLO.back(); // No k-factors if ( true ) k0 = k1 = k2 = 1.; cout << " K-Factors :" << endl; cout << "k0 = " << k0 << endl; cout << "k1 = " << k1 << endl; cout << "k2 = " << k2 << endl; // Switch off cross section estimation. pythia.settings.flag("Merging:doXSectionEstimate", false); // Switch showering and multiple interaction back on. pythia.settings.flag("PartonLevel:FSR",fsr); pythia.settings.flag("PartonLevel:ISR",isr); pythia.settings.flag("HadronLevel:all",had); pythia.settings.flag("PartonLevel:MPI",mpi); //----------------------------------------------------------------------------- //----------------------------------------------------------------------------- // Declare sample cross section for output. double sigmaTemp = 0.; vector sampleXStree; vector sampleXSvirt; vector sampleXSsubtTree; vector sampleXSsubtVirt; // Cross section an error. double sigmaTotal = 0.; double errorTotal = 0.; // Switch on tree-level processing. pythia.settings.flag("Merging:doUNLOPSTree",true); pythia.settings.flag("Merging:doUNLOPSLoop",false); pythia.settings.flag("Merging:doUNLOPSSubt",false); pythia.settings.flag("Merging:doUNLOPSSubtNLO",false); pythia.settings.mode("Merging:nRecluster",0); // Start looping through input event files. njetcounterLO = nMaxLO; iPathTree = iPath + "_tree"; while(njetcounterLO >= 0){ // Set k factors pythia.settings.parm("Merging:kFactor0j", k0); pythia.settings.parm("Merging:kFactor1j", k1); pythia.settings.parm("Merging:kFactor2j", k2); // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathTree+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathTree + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); cout << endl << endl << endl << "Start tree level treatment for " << njetcounterLO << " jets" << endl; // UNLOPS does not contain a zero-jet tree-level sample. if ( njetcounterLO == 0 ) break; pythia.settings.mode("Merging:nRequested", njetcounterLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Remember position in vector of cross section estimates. int iNow = sizeLO-1-njetcounterLO; // Start generation loop for( int iEvent=0; iEventweights().push_back(weightNLO*normhepmc); // Fill HepMC event. ToHepMC.fill_next_event( pythia, hepmcevt ); // Add the weight of the current event to the cross section. sigmaTotal += weightNLO*normhepmc; sigmaTemp += weightNLO*normhepmc; errorTotal += pow2(weightNLO*normhepmc); // Report cross section to hepmc. HepMC::GenCrossSection xsec; xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } // end loop over events to generate // print cross section, errors pythia.stat(); // Save sample cross section for output. sampleXStree.push_back(sigmaTemp); sigmaTemp = 0.; // Restart with ME of a reduced the number of jets if( njetcounterLO > 0 ) njetcounterLO--; else break; } //----------------------------------------------------------------------------- //----------------------------------------------------------------------------- cout << endl << endl << endl; cout << "Start unlops virtual corrections part" << endl; // Switch on loop-level processing. pythia.settings.flag("Merging:doUNLOPSTree",false); pythia.settings.flag("Merging:doUNLOPSLoop",true); pythia.settings.flag("Merging:doUNLOPSSubt",false); pythia.settings.flag("Merging:doUNLOPSSubtNLO",false); pythia.settings.mode("Merging:nRecluster",0); njetcounterNLO = nMaxNLO; iPathLoop= iPath + "_powheg"; while(njetcounterNLO >= 0){ // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterNLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathLoop+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathLoop + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); cout << endl << endl << endl << "Start loop level treatment for " << njetcounterNLO << " jets" << endl; pythia.settings.mode("Merging:nRequested", njetcounterNLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Remember position in vector of cross section estimates. int iNow = sizeNLO-1-njetcounterNLO; // Start generation loop for( int iEvent=0; iEventweights().push_back(weightNLO*normhepmc); // Fill HepMC event. ToHepMC.fill_next_event( pythia, hepmcevt ); // Add the weight of the current event to the cross section. sigmaTotal += weightNLO*normhepmc; sigmaTemp += weightNLO*normhepmc; errorTotal += pow2(weightNLO*normhepmc); // Report cross section to hepmc HepMC::GenCrossSection xsec; xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } // end loop over events to generate // print cross section, errors pythia.stat(); // Save sample cross section for output. sampleXSvirt.push_back(sigmaTemp); sigmaTemp = 0.; // Restart with ME of a reduced the number of jets if( njetcounterNLO > 0) njetcounterNLO--; else break; } //----------------------------------------------------------------------------- //----------------------------------------------------------------------------- cout << endl << endl << endl; cout << "Shower subtractive events" << endl; // Switch on processing of counter-events. pythia.settings.flag("Merging:doUNLOPSTree",false); pythia.settings.flag("Merging:doUNLOPSLoop",false); pythia.settings.flag("Merging:doUNLOPSSubt",true); pythia.settings.flag("Merging:doUNLOPSSubtNLO",false); pythia.settings.mode("Merging:nRecluster",1); int nMaxCT = nMaxLO; int njetcounterCT = nMaxCT; string iPathSubt= iPath + "_tree"; while(njetcounterCT >= 1){ // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterCT << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathSubt+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathSubt + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); cout << endl << endl << endl << "Start subtractive treatment for " << njetcounterCT << " jets" << endl; pythia.settings.mode("Merging:nRequested", njetcounterCT); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Remember position in vector of cross section estimates. int iNow = sizeLO-1-njetcounterCT; // Start generation loop for( int iEvent=0; iEventweights().push_back(weightNLO*normhepmc); // Fill HepMC event. ToHepMC.fill_next_event( pythia, hepmcevt ); // Add the weight of the current event to the cross section. sigmaTotal += weightNLO*normhepmc; sigmaTemp += weightNLO*normhepmc; errorTotal += pow2(weightNLO*normhepmc); // Report cross section to hepmc. HepMC::GenCrossSection xsec; xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } // end loop over events to generate // print cross section, errors pythia.stat(); // Save sample cross section for output. sampleXSsubtTree.push_back(sigmaTemp); sigmaTemp = 0.; // Restart with ME of a reduced the number of jets if( njetcounterCT > 1 ) njetcounterCT--; else break; } //----------------------------------------------------------------------------- //----------------------------------------------------------------------------- cout << endl << endl << endl; cout << "Shower subtractive events" << endl; pythia.settings.flag("Merging:doUNLOPSTree",false); pythia.settings.flag("Merging:doUNLOPSLoop",false); pythia.settings.flag("Merging:doUNLOPSSubt",false); pythia.settings.flag("Merging:doUNLOPSSubtNLO",true); pythia.settings.mode("Merging:nRecluster",1); nMaxCT = nMaxNLO; njetcounterCT = nMaxCT; iPathSubt= iPath + "_powheg"; while(njetcounterCT >= 1){ // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterCT << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathSubt+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathSubt + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); cout << endl << endl << endl << "Start subtractive treatment for " << njetcounterCT << " nlo jets" << endl; pythia.settings.mode("Merging:nRequested", njetcounterCT); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Remember position in vector of cross section estimates. int iNow = sizeNLO-1-njetcounterCT; // Start generation loop for( int iEvent=0; iEventweights().push_back(weightNLO*normhepmc); // Fill HepMC event. ToHepMC.fill_next_event( pythia, hepmcevt ); // Add the weight of the current event to the cross section. sigmaTotal += weightNLO*normhepmc; sigmaTemp += weightNLO*normhepmc; errorTotal += pow2(weightNLO*normhepmc); // Report cross section to hepmc. HepMC::GenCrossSection xsec; xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } // end loop over events to generate // print cross section, errors pythia.stat(); // Save sample cross section for output. sampleXSsubtVirt.push_back(sigmaTemp); sigmaTemp = 0.; // Restart with ME of a reduced the number of jets if( njetcounterCT > 1 ) njetcounterCT--; else break; } // Print cross section information. cout << endl << endl; cout << " *---------------------------------------------------*" << endl; cout << " | |" << endl; cout << " | Sample cross sections after UNLOPS merging |" << endl; cout << " | |" << endl; cout << " | Leading order cross sections (mb): |" << endl; for (int i = 0; i < int(sampleXStree.size()); ++i) cout << " | " << sampleXStree.size()-1-i+1 << "-jet: " << setw(17) << scientific << setprecision(6) << sampleXStree[i] << " |" << endl; cout << " | (No 0-jet tree-level sample in UNLOPS) |" << endl; cout << " | |" << endl; cout << " | NLO order cross sections (mb): |" << endl; for (int i = 0; i < int(sampleXSvirt.size()); ++i) cout << " | " << sampleXSvirt.size()-1-i << "-jet: " << setw(17) << scientific << setprecision(6) << sampleXSvirt[i] << " |" << endl; cout << " | |" << endl; cout << " | Leading-order subtractive cross sections (mb): |" << endl; for (int i = 0; i < int(sampleXSsubtTree.size()); ++i) cout << " | " << sampleXSsubtTree.size()-1-i+1 << "-jet: " << setw(17) << scientific << setprecision(6) << sampleXSsubtTree[i] << " |" << endl; cout << " | |" << endl; if ( sampleXSsubtVirt.size() > 0) { cout << " | NLO subtractive cross sections (mb): |" << endl; for (int i = 0; i < int(sampleXSsubtVirt.size()); ++i) cout << " | " << sampleXSsubtVirt.size()-1-i+1 << "-jet: " << setw(17) << scientific << setprecision(6) << sampleXSsubtVirt[i] << " |" << endl; cout << " | |" << endl; } cout << " |---------------------------------------------------|" << endl; cout << " |---------------------------------------------------|" << endl; cout << " | Inclusive cross sections: |" << endl; cout << " | |" << endl; cout << " | UNLOPS merged inclusive cross section: |" << endl; cout << " | " << setw(17) << scientific << setprecision(6) << sigmaTotal << " +- " << setw(17) << sqrt(errorTotal) << " mb " << " |" << endl; cout << " | |" << endl; cout << " | NLO inclusive cross section: |" << endl; cout << " | " << setw(17) << scientific << setprecision(6) << xsecNLO.back() << " mb |" << endl; cout << " | |" << endl; cout << " | LO inclusive cross section: |" << endl; cout << " | " << setw(17) << scientific << setprecision(6) << xsecLO.back() << " mb |" << endl; cout << " | |" << endl; cout << " *---------------------------------------------------*" << endl; cout << endl << endl; // Done return 0; } pythia8-8.1.80.orig/examples/Makefile0000644000175000017500000001164612217346170015622 0ustar sunsun# # Examples Makefile. # # M. Kirsanov 07.04.2006 # Modified 18.11.2006 # 26.03.2008 CLHEP dependency removed SHELL = /bin/sh -include config.mk ifeq (x$(PYTHIA8LOCATION),x) PYTHIA8LOCATION=.. endif -include $(PYTHIA8LOCATION)/config.mk # Location of directories. TOPDIR=$(shell \pwd) INCDIR=include SRCDIR=src LIBDIR=lib LIBDIRARCH=lib/archive BINDIR=bin # Libraries to include if GZIP support is enabled ifeq (x$(ENABLEGZIP),xyes) LIBGZIP=-L$(BOOSTLIBLOCATION) -lboost_iostreams -L$(ZLIBLOCATION) -lz endif # There is no default behaviour, so remind user. all: @echo "Usage: for NN = example number: make mainNN" # Create an executable for one of the normal test programs main00 main01 main02 main03 main04 main05 main06 main07 main08 main09 main10 \ main11 main12 main13 main14 main15 main16 main17 main18 main19 main20 \ main21 main22 main23 main24 main25 main26 main27 main28 main29 main30 \ main31 main32 main33 main34 main35 main36 main37 main38 main39 main40: \ $(PYTHIA8LOCATION)/$(LIBDIRARCH)/libpythia8.a @mkdir -p $(BINDIR) $(CXX) $(CXXFLAGS) -I$(PYTHIA8LOCATION)/$(INCDIR) $@.cc -o $(BINDIR)/$@.exe \ -L$(PYTHIA8LOCATION)/$(LIBDIRARCH) -lpythia8 -llhapdfdummy $(LIBGZIP) @ln -fs $(BINDIR)/$@.exe $@.exe # Create an executable linked to HepMC (if all goes well). # Owing to excessive warning output -Wshadow is not used for HepMC. ifneq (x$(HEPMCLOCATION),x) main41 main42: \ $(PYTHIA8LOCATION)/$(LIBDIRARCH)/libpythia8.a $(PYTHIA8LOCATION)/$(LIBDIRARCH)/libpythia8tohepmc.a @mkdir -p $(BINDIR) $(CXX) $(CXXFLAGS) -Wno-shadow -I$(PYTHIA8LOCATION)/$(INCDIR) -I$(HEPMCLOCATION)/include \ $@.cc -o $(BINDIR)/$@.exe \ -L$(PYTHIA8LOCATION)/$(LIBDIRARCH) -lpythia8 -llhapdfdummy $(LIBGZIP) \ -lpythia8tohepmc \ -L$(HEPMCLOCATION)/lib -lHepMC @ln -fs $(BINDIR)/$@.exe $@.exe else main41 main42: @echo ERROR, this target needs HepMC, variable HEPMCLOCATION endif # Create an executable that links to LHAPDF main51 main52 main53: $(PYTHIA8LOCATION)/$(LIBDIRARCH)/libpythia8.a @mkdir -p $(BINDIR) $(CXX) $(CXXFLAGS) -I$(PYTHIA8LOCATION)/$(INCDIR) $@.cc -o $(BINDIR)/$@.exe \ -L$(PYTHIA8LOCATION)/$(LIBDIRARCH) -lpythia8 $(LIBGZIP) \ -L$(LHAPDFLOCATION) $(LHAPDFLIBNAME) \ $(FLIBS) @ln -fs $(BINDIR)/$@.exe $@.exe # Create an executable that links to LHAPDF and HepMC main61 main62 main85 main86 main87 main88: \ $(PYTHIA8LOCATION)/$(LIBDIRARCH)/libpythia8.a $(PYTHIA8LOCATION)/$(LIBDIRARCH)/libpythia8tohepmc.a @mkdir -p $(BINDIR) $(CXX) $(CXXFLAGS) -Wno-shadow -I$(PYTHIA8LOCATION)/$(INCDIR) -I$(HEPMCLOCATION)/include \ $@.cc -o $(BINDIR)/$@.exe \ -L$(PYTHIA8LOCATION)/$(LIBDIRARCH) -lpythia8 -lpythia8tohepmc $(LIBGZIP) \ -L$(LHAPDFLOCATION) $(LHAPDFLIBNAME) \ -L$(HEPMCLOCATION)/lib -lHepMC \ $(FLIBS) @ln -fs $(BINDIR)/$@.exe $@.exe # Create an executable that links to Fastjet # Owing to excessive warning output -Wshadow is not used for Fastjet. # (Fixed as of Fastjet 3.0.1, so will be modified eventually.) ifneq (x$(FASTJETLOCATION),x) main71 main72: $(PYTHIA8LOCATION)/$(LIBDIRARCH)/libpythia8.a @mkdir -p $(BINDIR) # Note: $(CXXFLAGS) is after Fastjet flags as Fastjet includes # optimisation/debug flags which may be unwanted (e.g. -g -O2) $(CXX) -I$(PYTHIA8LOCATION)/$(INCDIR) $@.cc \ `$(FASTJETLOCATION)/bin/fastjet-config --cxxflags --plugins` \ $(CXXFLAGS) -Wno-shadow \ -o $(BINDIR)/$@.exe \ -L$(PYTHIA8LOCATION)/$(LIBDIRARCH) -lpythia8 -llhapdfdummy $(LIBGZIP) \ -L$(FASTJETLOCATION)/lib \ `$(FASTJETLOCATION)/bin/fastjet-config --libs --plugins` @ln -fs $(BINDIR)/$@.exe $@.exe @rm -f $@.o else main71 main72: @echo ERROR, this target needs Fastjet, variable FASTJETLOCATION endif # Create an executable that links to Fastjet, HepMC and LHApdf # Owing to excessive warning output -Wshadow is not used for Fastjet. # (Fixed as of Fastjet 3.0.1, so will be modified eventually.) ifneq (x$(FASTJETLOCATION),x) main81 main82 main83 main84: \ $(PYTHIA8LOCATION)/$(LIBDIRARCH)/libpythia8.a $(PYTHIA8LOCATION)/$(LIBDIRARCH)/libpythia8tohepmc.a @mkdir -p $(BINDIR) # Note: $(CXXFLAGS) is after Fastjet flags as Fastjet includes # optimisation/debug flags which may be unwanted (e.g. -g -O2) $(CXX) -I$(PYTHIA8LOCATION)/$(INCDIR) $@.cc \ `$(FASTJETLOCATION)/bin/fastjet-config --cxxflags --plugins` \ $(CXXFLAGS) -Wno-shadow \ -I$(PYTHIA8LOCATION)/$(INCDIR) -I$(HEPMCLOCATION)/include \ -o $(BINDIR)/$@.exe \ -L$(PYTHIA8LOCATION)/$(LIBDIRARCH) -lpythia8 \ -L$(LHAPDFLOCATION) $(LHAPDFLIBNAME) \ -lpythia8tohepmc \ -L$(HEPMCLOCATION)/lib -lHepMC \ -L$(FASTJETLOCATION)/lib \ -L$(LHAPDFLOCATION)/lib \ `$(FASTJETLOCATION)/bin/fastjet-config --libs --plugins` @ln -fs $(BINDIR)/$@.exe $@.exe @rm -f $@.o else main81 main82 main83 main84: @echo ERROR, this target needs Fastjet, variable FASTJETLOCATION endif # Clean up: remove executables and outdated files. .PHONY: clean clean: rm -rf $(BINDIR) rm -rf *.exe rm -f *~; rm -f \#*; rm -f core* pythia8-8.1.80.orig/examples/main05.cc0000644000175000017500000001200712217346163015554 0ustar sunsun// main05.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It studies jet production at the LHC, using SlowJet and CellJet. // Note: the two finders are intended to construct approximately the same // jet properties, but provides output in slightly different format, // and have here not been optimized to show maximum possible agreement. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Number of events, generated and listed ones. int nEvent = 500; int nListJets = 5; // Generator. LHC process and output selection. Initialization. Pythia pythia; pythia.readString("Beams:eCM = 14000."); pythia.readString("HardQCD:all = on"); pythia.readString("PhaseSpace:pTHatMin = 200."); pythia.readString("Next:numberShowInfo = 0"); pythia.readString("Next:numberShowProcess = 0"); pythia.readString("Next:numberShowEvent = 0"); pythia.init(); // Common parameters for the two jet finders. double etaMax = 4.; double radius = 0.7; double pTjetMin = 10.; // Exclude neutrinos (and other invisible) from study. int nSel = 2; // Range and granularity of CellJet jet finder. int nEta = 80; int nPhi = 64; // Set up SlowJet jet finder, with anti-kT clustering // and pion mass assumed for non-photons.. SlowJet slowJet( -1, radius, pTjetMin, etaMax, nSel, 1); // Set up CellJet jet finder. CellJet cellJet( etaMax, nEta, nPhi, nSel); // Histograms. Note similarity in names, even when the two jet finders // do not calculate identically the same property (pT vs. ET, y vs. eta). Hist nJetsS("number of jets, SlowJet", 50, -0.5, 49.5); Hist nJetsC("number of jets, CellJet", 50, -0.5, 49.5); Hist nJetsD("number of jets, CellJet - SlowJet", 45, -22.5, 22.5); Hist eTjetsS("pT for jets, SlowJet", 100, 0., 500.); Hist eTjetsC("eT for jets, CellJet", 100, 0., 500.); Hist etaJetsS("y for jets, SlowJet", 100, -5., 5.); Hist etaJetsC("eta for jets, CellJet", 100, -5., 5.); Hist phiJetsS("phi for jets, SlowJwt", 100, -M_PI, M_PI); Hist phiJetsC("phi for jets, CellJet", 100, -M_PI, M_PI); Hist distJetsS("R distance between jets, SlowJet", 100, 0., 10.); Hist distJetsC("R distance between jets, CellJet", 100, 0., 10.); Hist eTdiffS("pT difference, SlowJet", 100, -100., 400.); Hist eTdiffC("eT difference, CellJet", 100, -100., 400.); // Begin event loop. Generate event. Skip if error. for (int iEvent = 0; iEvent < nEvent; ++iEvent) { if (!pythia.next()) continue; // Analyze Slowet jet properties. List first few. slowJet. analyze( pythia.event ); if (iEvent < nListJets) slowJet.list(); // Fill SlowJet inclusive jet distributions. nJetsS.fill( slowJet.sizeJet() ); for (int i = 0; i < slowJet.sizeJet(); ++i) { eTjetsS.fill( slowJet.pT(i) ); etaJetsS.fill( slowJet.y(i) ); phiJetsS.fill( slowJet.phi(i) ); } // Fill SlowJet distance between jets. for (int i = 0; i < slowJet.sizeJet() - 1; ++i) for (int j = i +1; j < slowJet.sizeJet(); ++j) { double dEta = slowJet.y(i) - slowJet.y(j); double dPhi = abs( slowJet.phi(i) - slowJet.phi(j) ); if (dPhi > M_PI) dPhi = 2. * M_PI - dPhi; double dR = sqrt( pow2(dEta) + pow2(dPhi) ); distJetsS.fill( dR ); } // Fill SlowJet pT-difference between jets (to check ordering of list). for (int i = 1; i < slowJet.sizeJet(); ++i) eTdiffS.fill( slowJet.pT(i-1) - slowJet.pT(i) ); // Analyze CellJet jet properties. List first few. cellJet. analyze( pythia.event, pTjetMin, radius ); if (iEvent < nListJets) cellJet.list(); // Fill CellJet inclusive jet distributions. nJetsC.fill( cellJet.size() ); for (int i = 0; i < cellJet.size(); ++i) { eTjetsC.fill( cellJet.eT(i) ); etaJetsC.fill( cellJet.etaWeighted(i) ); phiJetsC.fill( cellJet.phiWeighted(i) ); } // Fill CellJet distance between jets. for (int i = 0; i < cellJet.size() - 1; ++i) for (int j = i +1; j < cellJet.size(); ++j) { double dEta = cellJet.etaWeighted(i) - cellJet.etaWeighted(j); double dPhi = abs( cellJet.phiWeighted(i) - cellJet.phiWeighted(j) ); if (dPhi > M_PI) dPhi = 2. * M_PI - dPhi; double dR = sqrt( pow2(dEta) + pow2(dPhi) ); distJetsC.fill( dR ); } // Fill CellJet ET-difference between jets (to check ordering of list). for (int i = 1; i < cellJet.size(); ++i) eTdiffC.fill( cellJet.eT(i-1) - cellJet.eT(i) ); // Compare number of jets for the two finders. nJetsD.fill( cellJet.size() - slowJet.sizeJet() ); // End of event loop. Statistics. Histograms. } pythia.stat(); cout << nJetsS << nJetsC << nJetsD << eTjetsS << eTjetsC << etaJetsS << etaJetsC << phiJetsS << phiJetsC << distJetsS << distJetsC << eTdiffS << eTdiffC; // Done. return 0; } pythia8-8.1.80.orig/examples/main16.cmnd0000644000175000017500000000672312217346164016123 0ustar sunsun! File: main16.cmnd ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! Names are case-insensitive - but spellings-sensitive! ! The changes here are illustrative, not always physics-motivated. ! 1) Settings that are used in the main program. Main:numberOfEvents = 1000 ! number of events to generate Main:timesAllowErrors = 10 ! abort run after this many flawed events ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showChangedParticleData = on ! list changed particle data #Init:showChangedResonanceData = on ! also print changed resonance data #Init:showOneParticleData = 25 ! print data for this particular particle Next:numberCount = 100 ! print message every n events Next:numberShowInfo = 1 ! print event information n times Next:numberShowProcess = 1 ! print process record n times Next:numberShowEvent = 0 ! print event record n times Stat:showPartonLevel = on ! more statistics on MPI ! 3) Beam settings. Beams:idA = 2212 ! first beam, p = 2212, pbar = -2212 Beams:idB = 2212 ! second beam, p = 2212, pbar = -2212 Beams:eCM = 14000. ! CM energy of collision, LHC ! 4) Settings for hard-process generation internal to Pythia8. HiggsSM:gg2H = on ! Higgs production by gluon-gluon fusion ! 5) Set Higgs mass, width and branching ratios by hand. ! Values for 125 GeV SM Higgs taken from ! Handbook of LHC Higgs Cross Sections: 1. Inclusive Observables, ! S. Dittmaier et al., CERN-2011-002 [arXiv:1101.0593]. ! Note: sum is not quite unity, and so BR's are rescaled accordingly. 25:m0 = 125.0 ! Higgs mass 25:mWidth = 0.00403 ! Higgs width 25:0:bRatio = 0.0 ! H -> d dbar 25:1:bRatio = 0.0 ! H -> u ubar 25:2:bRatio = 0.00044 ! H -> s sbar 25:3:bRatio = 0.0268 ! H -> c cbar 25:4:bRatio = 0.578 ! H -> b bbar 25:5:bRatio = 0.0 ! H -> t tbar 25:6:bRatio = 0.0 ! H -> e+ e- 25:7:bRatio = 0.000221 ! H -> mu+ mu- 25:8:bRatio = 0.0637 ! H -> tau+ tau- 25:9:bRatio = 0.0856 ! H -> g g 25:10:bRatio = 0.00230 ! H -> gamma gamma 25:11:bRatio = 0.00155 ! H -> gamma Z 25:12:bRatio = 0.0267 ! H -> Z0 Z0 25:13:bRatio = 0.216 ! H -> W+ W- 25:0:meMode = 100 ! set meMode = 100 so that 25:1:meMode = 100 ! branching ratios are not 25:2:meMode = 100 ! overwritten at initialization 25:3:meMode = 100 25:4:meMode = 100 25:5:meMode = 100 25:6:meMode = 100 25:7:meMode = 100 25:8:meMode = 100 25:9:meMode = 100 25:10:meMode = 100 25:11:meMode = 100 25:12:meMode = 100 25:13:meMode = 100 ! 6) Switch off some key components of the simulation, for comparisons. #PartonLevel:all = off ! stop after hard process #PartonLevel:MPI = off ! no multiparton interactions #PartonLevel:ISR = off ! no initial-state radiation #PartonLevel:FSR = off ! no final-state radiation #HadronLevel:all = off ! stop after parton level #HadronLevel:Hadronize = off ! no hadronization #HadronLevel:Decay = off ! no decays ! 7) Any other changes you desire. pythia8-8.1.80.orig/examples/main19.cc0000644000175000017500000001534612217346164015573 0ustar sunsun// main19.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This program runs four instances of Pythia simultaneously, // one for signal events, one for pileup background ones, and two // For beam-gas background ones. Note that Pythia does not do nuclear // effects, so beam-gas is represented by "fixed-target" pp collisions. // The = and += overloaded operators are used to join several // event records into one, but should be used with caution. // Note that each instance of Pythia is independent of any other, // but with two important points to remember. // 1) By default all generate the same random number sequence, // which has to be corrected if they are to generate the same // physics, like the two beam-gas ones below. // 2) Interfaces to external Fortran programs are "by definition" static. // Thus it is not a good idea to use LHAPDF to set different PDF's // in different instances. #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // Method to pick a number according to a Poissonian distribution. int poisson(double nAvg, Rndm& rndm) { // Set maximum to avoid overflow. const int NMAX = 100; // Random number. double rPoisson = rndm.flat() * exp(nAvg); // Initialize. double rSum = 0.; double rTerm = 1.; // Add to sum and check whether done. for (int i = 0; i < NMAX; ) { rSum += rTerm; if (rSum > rPoisson) return i; // Evaluate next term. ++i; rTerm *= nAvg / i; } // Emergency return. return NMAX; } //========================================================================== int main() { // Number of signal events to generate. int nEvent = 100; // Beam Energy. double eBeam = 7000.; // Average number of pileup events per signal event. double nPileupAvg = 2.5; // Average number of beam-gas events per signal ones, on two sides. double nBeamAGasAvg = 0.5; double nBeamBGasAvg = 0.5; // Four generator instances. Pythia pythiaSignal; Pythia pythiaPileup; Pythia pythiaBeamAGas; Pythia pythiaBeamBGas; // One object where all individual events are to be collected. Event sumEvent; // Switch off automatic event listing. pythiaSignal.readString("Next:numberShowInfo = 0"); pythiaSignal.readString("Next:numberShowProcess = 0"); pythiaSignal.readString("Next:numberShowEvent = 0"); pythiaPileup.readString("Next:numberShowInfo = 0"); pythiaPileup.readString("Next:numberShowProcess = 0"); pythiaPileup.readString("Next:numberShowEvent = 0"); pythiaBeamAGas.readString("Next:numberShowInfo = 0"); pythiaBeamAGas.readString("Next:numberShowProcess = 0"); pythiaBeamAGas.readString("Next:numberShowEvent = 0"); pythiaBeamBGas.readString("Next:numberShowInfo = 0"); pythiaBeamBGas.readString("Next:numberShowProcess = 0"); pythiaBeamBGas.readString("Next:numberShowEvent = 0"); // Initialize generator for signal processes. pythiaSignal.readString("HardQCD:all = on"); pythiaSignal.readString("PhaseSpace:pTHatMin = 50."); pythiaSignal.settings.parm("Beams:eCM", 2. * eBeam); pythiaSignal.init(); // Initialize generator for pileup (background) processes. pythiaPileup.readString("Random:setSeed = on"); pythiaPileup.readString("Random:seed = 10000002"); pythiaPileup.readString("SoftQCD:all = on"); pythiaPileup.settings.parm("Beams:eCM", 2. * eBeam); pythiaPileup.init(); // Initialize generators for beam A - gas (background) processes. pythiaBeamAGas.readString("Random:setSeed = on"); pythiaBeamAGas.readString("Random:seed = 10000003"); pythiaBeamAGas.readString("SoftQCD:all = on"); pythiaBeamAGas.readString("Beams:frameType = 2"); pythiaBeamAGas.settings.parm("Beams:eA", eBeam); pythiaBeamAGas.settings.parm("Beams:eB", 0.); pythiaBeamAGas.init(); // Initialize generators for beam B - gas (background) processes. pythiaBeamBGas.readString("Random:setSeed = on"); pythiaBeamBGas.readString("Random:seed = 10000004"); pythiaBeamBGas.readString("SoftQCD:all = on"); pythiaBeamBGas.readString("Beams:frameType = 2"); pythiaBeamBGas.settings.parm("Beams:eA", 0.); pythiaBeamBGas.settings.parm("Beams:eB", eBeam); pythiaBeamBGas.init(); // Histograms: number of pileups, total charged multiplicity. Hist nPileH("number of pileup events per signal event", 100, -0.5, 99.5); Hist nAGH("number of beam A + gas events per signal event", 100, -0.5, 99.5); Hist nBGH("number of beam B + gas events per signal event", 100, -0.5, 99.5); Hist nChgH("number of charged multiplicity",100, -0.5, 1999.5); Hist sumPZH("total pZ of system",100, -100000., 100000.); // Loop over events. for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate a signal event. Copy this event into sumEvent. if (!pythiaSignal.next()) continue; sumEvent = pythiaSignal.event; // Select the number of pileup events to generate. int nPileup = poisson(nPileupAvg, pythiaPileup.rndm); nPileH.fill( nPileup ); // Generate a number of pileup events. Add them to sumEvent. for (int iPileup = 0; iPileup < nPileup; ++iPileup) { pythiaPileup.next(); sumEvent += pythiaPileup.event; } // Select the number of beam A + gas events to generate. int nBeamAGas = poisson(nBeamAGasAvg, pythiaBeamAGas.rndm); nAGH.fill( nBeamAGas ); // Generate a number of beam A + gas events. Add them to sumEvent. for (int iAG = 0; iAG < nBeamAGas; ++iAG) { pythiaBeamAGas.next(); sumEvent += pythiaBeamAGas.event; } // Select the number of beam B + gas events to generate. int nBeamBGas = poisson(nBeamBGasAvg, pythiaBeamBGas.rndm); nBGH.fill( nBeamBGas ); // Generate a number of beam B + gas events. Add them to sumEvent. for (int iBG = 0; iBG < nBeamBGas; ++iBG) { pythiaBeamBGas.next(); sumEvent += pythiaBeamBGas.event; } // List first few events. if (iEvent < 1) { pythiaSignal.info.list(); pythiaSignal.process.list(); sumEvent.list(); } // Find charged multiplicity. int nChg = 0; for (int i = 0; i < sumEvent.size(); ++i) if (sumEvent[i].isFinal() && sumEvent[i].isCharged()) ++nChg; nChgH.fill( nChg ); // Fill net pZ - nonvanishing owing to beam + gas. sumPZH.fill( sumEvent[0].pz() ); // End of event loop } // Statistics. Histograms. pythiaSignal.stat(); pythiaPileup.stat(); pythiaBeamAGas.stat(); pythiaBeamBGas.stat(); cout << nPileH << nAGH << nBGH << nChgH << sumPZH; return 0; } pythia8-8.1.80.orig/examples/main28.cc0000644000175000017500000001720512217346165015570 0ustar sunsun// main28.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Peter Skands, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Example of of R-hadron production. // Several of the possibilities shown here, like displaced vertices, // are extras that need not be used for the basic setup. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Key settings to be used in the main program. // nGluino = 0, 1, 2 give stop pair, single gluino or gluino pair. int nGluino = 2; int nEvent = 200; int nAbort = 3; int nList = 0; double eCM = 7000.; // Generator. Shorthand for the event. Pythia pythia; Event& event = pythia.event; // Set up beams: p p is default so only need set energy. pythia.settings.parm("Beams:eCM", eCM); // Squark pair: use stop-antistop as example. if (nGluino == 0) { pythia.readString("SUSY:gg2squarkantisquark = on"); pythia.readString("SUSY:idA = 1000006"); pythia.readString("SUSY:idB = 1000006"); // Squark-gluino pair: also supersymmetric u has been made long-lived. // Stop does not work since then one would need inoming top PDF. // Nevertheless R-hadrons are numbered/named as if containing a stop. } else if (nGluino == 1) { pythia.readString("SUSY:qg2squarkgluino = on"); pythia.readString("SUSY:idA = 1000002"); pythia.readString("RHadrons:idStop = 1000002"); pythia.readString("SUSY:idB = 1000021"); // Gluino pair. } else { pythia.readString("SUSY:gg2gluinogluino = on"); } // Use hacked sps1a file, with stop (+su) and gluino made long-lived. // This is based on the width being less than 0.2 GeV by default. pythia.readString("SLHA:file = sps1aNarrowStopGluino.spc"); // Further hacked file, to test R-parity violating gluino decay. //pythia.readString("SLHA:file = sps1aNarrowStopGluinoRPV.spc"); // Allow R-hadron formation. pythia.readString("Rhadrons:allow = on"); // If you want to do the decay separately later, // you need to switch off automatic decays. pythia.readString("RHadrons:allowDecay = off"); // Fraction of gluinoballs. pythia.readString("RHadrons:probGluinoball = 0.1"); // Switch off key components. //pythia.readString("PartonLevel:MPI = off"); //pythia.readString("PartonLevel:ISR = off"); //pythia.readString("PartonLevel:FSR = off"); //pythia.readString("HadronLevel:Hadronize = off"); // Allow the R-hadrons to have secondary vertices: set c*tau in mm. // Note that width and lifetime can be set independently. // (Nonzero small widths are needed e.g. to select branching ratios.) pythia.readString("1000002:tau0 = 200."); pythia.readString("1000006:tau0 = 250."); pythia.readString("1000021:tau0 = 300."); // Checks. Optionally relax E-p-conservation. pythia.readString("Check:nErrList = 2"); //pythia.readString("Check:epTolErr = 2e-3"); // Possibility to switch off particle data and event listings. // Also to shop location of displaced vertices. pythia.readString("Init:showChangedSettings = on"); pythia.readString("Init:showChangedParticleData = off"); pythia.readString("Next:numberShowInfo = 1"); pythia.readString("Next:numberShowProcess = 1"); pythia.readString("Next:numberShowEvent = 0"); pythia.readString("Next:showScaleAndVertex = on"); // Initialize. pythia.init(); // Histograms. Hist nChargedH("charged multiplicity", 100, -0.5, 799.5); Hist dndyChargedH("dn/dy charged", 100, -10., 10.); Hist dndyRH("dn/dy R-hadrons", 100, -5., 5.); Hist pTRH("pT R-hadrons", 100, 0., 1000.); Hist xRH("p_RHadron / p_sparticle", 100, 0.9, 1.1); Hist mDiff("m(Rhadron) - m(sparticle)", 100, 0., 5.); Hist decVtx("R-hadron decay vertex (mm from origin)", 100, 0., 1000.); // R-hadron flavour composition. map flavours; // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if failure. if (!pythia.next()) { if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Loop over final charged particles in the event. // The R-hadrons may not yet have decayed here. int nCharged = 0; Vec4 pSum; for (int i = 0; i < event.size(); ++i) { if (event[i].isFinal()) { pSum += event[i].p(); if (event[i].isCharged()) { ++nCharged; dndyChargedH.fill( event[i].y() ); } } } nChargedH.fill( nCharged ); // Loop over final R-hadrons in the event: kinematic distribution for (int i = 0; i < event.size(); ++i) { int idAbs = event[i].idAbs(); if (idAbs > 1000100 && idAbs < 2000000 && idAbs != 1009002) { ++flavours[ event[i].id() ]; dndyRH.fill( event[i].y() ); pTRH.fill( event[i].pT() ); // Trace back to mother; compare momenta and masses. int iMother = i; while( event[iMother].statusAbs() > 100) iMother = event[iMother].mother1(); double xFrac = event[i].pAbs() / event[iMother].pAbs(); xRH.fill( xFrac); double mShift = event[i].m() - event[iMother].m(); mDiff.fill( mShift ); // Separation of R-hadron decay vertex from origin. // Don't be fooled by pAbs(); it gives the three-vector length // of any Vec4, also one representing spatial coordinates. double dist = event[i].vDec().pAbs(); decVtx.fill( dist); // This is a place where you could allow a R-hadron shift of // identity, momentum and decay vertex to allow for detector effects. // Identity not illustrated here; requires a change of mass as well. // Toy model: assume an exponential energy loss, < > = 1 GeV, // but at most half of kinetic energy. Unchanged direction. // Note that event will no longer conserve energy and momentum. double eLossAvg = 1.; double eLoss = 0.; do { eLoss = eLossAvg * pythia.rndm.exp(); } while (eLoss > 0.5 * (event[i].e() - event[i].m())); double eNew = event[i].e() - eLoss; Vec4 pNew = event[i].p() * sqrt( pow2(eNew) - pow2(event[i].m()) ) / event[i].pAbs(); pNew.e( eNew); event[i].p( pNew); // The decay vertex will be calculated based on the production vertex, // the proper lifetime tau and the NEW four-momentum, rather than // e.g. some average momentum, if you do not set it by hand. // This commented-out piece illustrates brute-force setting, // but you should provide real numbers from some tracking program. // With tau = 0 the decay is right at the chosen point. //event[i].tau( 0.); //event[i].vProd( 132., 155., 233., 177.); // End of loop over final R-hadrons. } } // If you have set R-hadrons stable above, // you can still force them to decay at this stage. pythia.forceRHadronDecays(); if (iEvent < nList) pythia.event.list(true); // End of event loop. } // Final statistics, flavour composition and histogram output. pythia.stat(); cout << "\n Composition of produced R-hadrons \n code " << "name times " << endl; for (map::iterator flavNow = flavours.begin(); flavNow != flavours.end(); ++flavNow) cout << setw(8) << flavNow->first << setw(16) << pythia.particleData.name(flavNow->first) << setw(8) << flavNow->second << endl; cout << nChargedH << dndyChargedH << dndyRH << pTRH << xRH << mDiff << decVtx; // Done. return 0; } pythia8-8.1.80.orig/examples/main72.cc0000644000175000017500000002470612217346167015575 0ustar sunsun// main72.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It compares SlowJet, FJcore and FastJet, showing that they find the same jets. #include "Pythia8/Pythia.h" // The FastJet3.h header enables automatic initialisation of // fastjet::PseudoJet objects from Pythia8 Particle and Vec4 objects, // as well as advanced features such as access to (a copy of) // the original Pythia 8 Particle directly from the PseudoJet, // and fastjet selectors that make use of the Particle properties. // See the extensive comments in the header file for further details // and examples. #include "Pythia8/FastJet3.h" using namespace Pythia8; int main() { // Number of events, generated and listed ones (for jets). int nEvent = 1000; int nListJets = 3; // Select common parameters for SlowJet and FastJet analyses. int power = -1; // -1 = anti-kT; 0 = C/A; 1 = kT. double R = 0.7; // Jet size. double pTMin = 5.0; // Min jet pT. double etaMax = 5.0; // Pseudorapidity range of detector. int select = 2; // Which particles are included? int massSet = 2; // Which mass are they assumed to have? // Generator. Shorthand for event. Pythia pythia; Event& event = pythia.event; // Process selection. pythia.readString("HardQCD:all = on"); pythia.readString("PhaseSpace:pTHatMin = 200."); // No event record printout. pythia.readString("Next:numberShowInfo = 0"); pythia.readString("Next:numberShowProcess = 0"); pythia.readString("Next:numberShowEvent = 0"); // LHC initialization. pythia.readString("Beams:eCM = 14000."); pythia.init(); // Set up SlowJet jet finder in native mode. SlowJet slowJet( power, R, pTMin, etaMax, select, massSet, 0, false); // Set up SlowJet jet finder as a wrapper to the fjcore package. // Note that this is now the default SlowJet constructor choice. SlowJet fjCore( power, R, pTMin, etaMax, select, massSet, 0, true); // Set up FastJet jet finder. // one can use either explicitly use antikt, cambridge, etc., or // just use genkt_algorithm with specification of power //fastjet::JetAlgorithm algorithm; //if (power == -1) algorithm = fastjet::antikt_algorithm; //if (power == 0) algorithm = fastjet::cambridge_algorithm; //if (power == 1) algorithm = fastjet::kt_algorithm; //fastjet::JetDefinition jetDef(algorithm, R); // there's no need for a pointer to the jetDef (it's a fairly small object) fastjet::JetDefinition jetDef(fastjet::genkt_algorithm, R, power); std::vector fjInputs; // Histograms. Hist nJetsS("number of jets (SlowJet)", 100, -0.5, 99.5); Hist nJetsC("number of jets, FJcore - SlowJet ", 99, -49.5, 49.5); Hist nJetsF("number of jets, FastJet - SlowJet", 99, -49.5, 49.5); Hist pTjetsS("pT for jets (SlowJet)", 100, 0., 500.); Hist pTjetsC("pT for jets, FJcore - SlowJet ", 100, -10., 10.); Hist pTjetsF("pT for jets, FastJet - SlowJet", 100, -10., 10.); Hist etaJetsS("eta for jets (SlowJet)", 100, -5., 5.); Hist phiJetsS("phi for jets (SlowJet)", 100, -M_PI, M_PI); Hist RdistC("R distance FJcore to SlowJet ", 100, 0., 1.); Hist RdistF("R distance FastJet to SlowJet", 100, 0., 1.); Hist distJets("R distance between jets", 100, 0., 10.); Hist pTdiff("pT difference between consecutive jets", 100, -100., 400.); Hist nAna("multiplicity of analyzed event", 100, -0.5, 999.5); Hist tGen("generation time as fn of multiplicity", 100, -0.5, 999.5); Hist tSlow("SlowJet time as fn of multiplicity", 100, -0.5, 999.5); Hist tCore("FJcore time as fn of multiplicity ", 100, -0.5, 999.5); Hist tFast("FastJet time as fn of multiplicity", 100, -0.5, 999.5); Hist tSlowGen("SlowJet/generation time as fn of multiplicity", 100, -0.5, 999.5); Hist tCoreGen("FJcore/generation time as fn of multiplicity", 100, -0.5, 999.5); Hist tFastGen("FastJet/generation time as fn of multiplicity", 100, -0.5, 999.5); Hist tFastCore("FastJet/FJcore time as fn of multiplicity", 100, -0.5, 999.5); // Begin event loop. Generate event. Skip if error. for (int iEvent = 0; iEvent < nEvent; ++iEvent) { clock_t befGen = clock(); if (!pythia.next()) continue; clock_t aftGen = clock(); // Begin SlowJet analysis of jet properties. List first few. clock_t befSlow = clock(); slowJet.analyze( pythia.event ); clock_t aftSlow = clock(); if (iEvent < nListJets) slowJet.list(); // Fill inclusive SlowJet jet distributions. int nSlow = slowJet.sizeJet(); nJetsS.fill( nSlow ); for (int i = 0; i < nSlow; ++i) { pTjetsS.fill( slowJet.pT(i) ); etaJetsS.fill( slowJet.y(i) ); phiJetsS.fill( slowJet.phi(i) ); } // Fill distance between SlowJet jets. for (int i = 0; i < nSlow - 1; ++i) for (int j = i + 1; j < nSlow; ++j) { double dY = slowJet.y(i) - slowJet.y(j); double dPhi = abs( slowJet.phi(i) - slowJet.phi(j) ); if (dPhi > M_PI) dPhi = 2. * M_PI - dPhi; double dR = sqrt( pow2(dY) + pow2(dPhi) ); distJets.fill( dR ); } // Fill pT-difference between SlowJet jets (to check ordering of list). for (int i = 1; i < nSlow; ++i) pTdiff.fill( slowJet.pT(i-1)- slowJet.pT(i) ); // Begin FJcore analysis of jet properties. List first few. clock_t befCore = clock(); fjCore.analyze( pythia.event ); clock_t aftCore = clock(); if (iEvent < nListJets) fjCore.list(); // Fill distribution of fjCore jets relative to SlowJet ones. int nCore = fjCore.sizeJet(); nJetsC.fill( nCore - nSlow); if (nCore == nSlow) { for (int i = 0; i < nCore; ++i) { pTjetsC.fill( fjCore.pT(i) - slowJet.pT(i) ); double dist2 = pow2( fjCore.y(i) - slowJet.y(i)) + pow2( fjCore.phi(i) - slowJet.phi(i) ); RdistC.fill( sqrt(dist2) ); } } // Begin FastJet analysis: extract particles from event record. clock_t befFast = clock(); fjInputs.resize(0); Vec4 pTemp; double mTemp; int nAnalyze = 0; for (int i = 0; i < event.size(); ++i) if (event[i].isFinal()) { // Require visible/charged particles inside detector. if (select > 2 && event[i].isNeutral() ) continue; else if (select == 2 && !event[i].isVisible() ) continue; if (etaMax < 20. && abs(event[i].eta()) > etaMax) continue; // Create a PseudoJet from the complete Pythia particle. fastjet::PseudoJet particleTemp = event[i]; // Optionally modify mass and energy. pTemp = event[i].p(); mTemp = event[i].m(); if (massSet < 2) { mTemp = (massSet == 0 || event[i].id() == 22) ? 0. : 0.13957; pTemp.e( sqrt(pTemp.pAbs2() + mTemp*mTemp) ); particleTemp.reset_momentum( pTemp.px(), pTemp.py(), pTemp.pz(), pTemp.e() ); } // Store acceptable particles as input to Fastjet. // Conversion to PseudoJet is performed automatically // with the help of the code in FastJet3.h. fjInputs.push_back( particleTemp); ++nAnalyze; } // Run Fastjet algorithm and sort jets in pT order. vector inclusiveJets, sortedJets; fastjet::ClusterSequence clustSeq(fjInputs, jetDef); inclusiveJets = clustSeq.inclusive_jets(pTMin); sortedJets = sorted_by_pt(inclusiveJets); clock_t aftFast = clock(); // List first few FastJet jets and some info about them. // Note: the final few columns are illustrative of what information // can be extracted, but does not exhaust the possibilities. if (iEvent < nListJets) { cout << "\n -------- FastJet jets, p = " << setw(2) << power << " --------------------------------------------------\n\n " << " i pT y phi mult chgmult photons" << " hardest pT in neutral " << endl << " " << " constituent hadrons " << endl; for (int i = 0; i < int(sortedJets.size()); ++i) { vector constituents = sortedJets[i].constituents(); fastjet::PseudoJet hardest = fastjet::SelectorNHardest(1)(constituents)[0]; vector neutral_hadrons = ( fastjet::SelectorIsHadron() && fastjet::SelectorIsNeutral())(constituents); double neutral_hadrons_pt = join(neutral_hadrons).perp(); cout << setw(4) << i << fixed << setprecision(3) << setw(11) << sortedJets[i].perp() << setw(9) << sortedJets[i].rap() << setw(9) << sortedJets[i].phi_std() << setw(6) << constituents.size() << setw(8) << fastjet::SelectorIsCharged().count(constituents) << setw(8) << fastjet::SelectorId(22).count(constituents) << setw(13) << hardest.user_info().name() << " " << setw(10) << neutral_hadrons_pt << endl; } cout << "\n -------- End FastJet Listing ------------------" << "---------------------------------" << endl; } // Fill distribution of FastJet jets relative to SlowJet ones. int nFast = sortedJets.size(); nJetsF.fill( nFast - nSlow); if (nFast == nSlow) { for (int i = 0; i < nFast; ++i) { pTjetsF.fill( sortedJets[i].perp() - slowJet.pT(i) ); double dist2 = pow2( sortedJets[i].rap() - slowJet.y(i)) + pow2( sortedJets[i].phi_std() - slowJet.phi(i)); RdistF.fill( sqrt(dist2) ); } } // Comparison of time consumption by analyzed multiplicity. nAna.fill( nAnalyze); tGen.fill( nAnalyze, aftGen - befGen); tSlow.fill( nAnalyze, aftSlow - befSlow); tCore.fill( nAnalyze, aftCore - befCore); tFast.fill( nAnalyze, aftFast - befFast); // End of event loop. } // Statistics. Histograms. pythia.stat(); tSlowGen = tSlow / tGen; tCoreGen = tCore / tGen; tFastGen = tFast / tGen; tFastCore = tFast / tCore; tGen /= nAna; tSlow /= nAna; tCore /= nAna; tFast /= nAna; cout << nJetsS << nJetsC << nJetsF << pTjetsS << pTjetsC << pTjetsF << etaJetsS << phiJetsS << RdistC << RdistF << distJets << pTdiff << nAna << tGen << tSlow << tCore << tFast << tSlowGen << tCoreGen << tFastGen << tFastCore; // Done. return 0; } pythia8-8.1.80.orig/examples/sps1aWithDecays.spc0000644000175000017500000013613312217346207017705 0ustar sunsun##****************************************************************** ## MadGraph/MadEvent * ##****************************************************************** ## * ## param_card corresponding the SPS point 1a (by SoftSusy 2.0.5) * ## * ##****************************************************************** ## Les Houches friendly file for the (MS)SM parameters of MadGraph * ## SM parameter set and decay widths produced by MSSMCalc * ##****************************************************************** ##*Please note the following IMPORTANT issues: * ## * ##0. REFRAIN from editing this file by hand! Some of the parame- * ## ters are not independent. Always use a calculator. * ## * ##1. alpha_S(MZ) has been used in the calculation of the parameters* ## This value is KEPT by madgraph when no pdf are used lpp(i)=0, * ## but, for consistency, it will be reset by madgraph to the * ## value expected IF the pdfs for collisions with hadrons are * ## used. * ## * ##2. Values of the charm and bottom kinematic (pole) masses are * ## those used in the matrix elements and phase space UNLESS they * ## are set to ZERO from the start in the model (particles.dat) * ## This happens, for example, when using 5-flavor QCD where * ## charm and bottom are treated as partons in the initial state * ## and a zero mass might be hardwired in the model definition. * ## * ## The SUSY decays have calculated using SDECAY 1.1a * ## * ##****************************************************************** # BLOCK DCINFO # Decay Program information 1 SDECAY # decay calculator 2 1.1a # version number # BLOCK SPINFO # Spectrum calculator information 1 SOFTSUSY # spectrum calculator 2 2.0.5 # version number # BLOCK MODSEL # Model selection 1 1 sugra # BLOCK SMINPUTS # Standard Model inputs 1 1.27934000E+02 # alpha_em^-1(M_Z)^MSbar 2 1.16637000E-05 # G_F [GeV^-2] 3 1.18000000E-01 # alpha_S(M_Z)^MSbar 4 9.11876000E+01 # M_Z pole mass 5 4.25000000E+00 # mb(mb)^MSbar 6 1.75000000E+02 # mt pole mass 7 1.77700000E+00 # mtau pole mass # BLOCK MINPAR # Input parameters - minimal models 1 1.00000000E+02 # m0 2 2.50000000E+02 # m12 3 1.00000000E+01 # tanb 4 1.00000000E+00 # sign(mu) 5 -1.00000000E+02 # A0 # BLOCK MASS # Mass Spectrum # PDG code mass particle 5 4.88991651E+00 # b-quark pole mass calculated from mb(mb)_Msbar 6 1.75000000E+02 # mt pole mass (not read by ME) 24 7.98290131E+01 # W+ 25 1.10899057E+02 # h 35 3.99960116E+02 # H 36 3.99583917E+02 # A 37 4.07879012E+02 # H+ 1000001 5.68441109E+02 # ~d_L 2000001 5.45228462E+02 # ~d_R 1000002 5.61119014E+02 # ~u_L 2000002 5.49259265E+02 # ~u_R 1000003 5.68441109E+02 # ~s_L 2000003 5.45228462E+02 # ~s_R 1000004 5.61119014E+02 # ~c_L 2000004 5.49259265E+02 # ~c_R 1000005 5.13065179E+02 # ~b_1 2000005 5.43726676E+02 # ~b_2 1000006 3.99668493E+02 # ~t_1 2000006 5.85785818E+02 # ~t_2 1000011 2.02915690E+02 # ~e_L 2000011 1.44102799E+02 # ~e_R 1000012 1.85258326E+02 # ~nu_eL 1000013 2.02915690E+02 # ~mu_L 2000013 1.44102799E+02 # ~mu_R 1000014 1.85258326E+02 # ~nu_muL 1000015 1.34490864E+02 # ~tau_1 2000015 2.06867805E+02 # ~tau_2 1000016 1.84708464E+02 # ~nu_tauL 1000021 6.07713704E+02 # ~g 1000022 9.66880686E+01 # ~chi_10 1000023 1.81088157E+02 # ~chi_20 1000025 -3.63756027E+02 # ~chi_30 1000035 3.81729382E+02 # ~chi_40 1000024 1.81696474E+02 # ~chi_1+ 1000037 3.79939320E+02 # ~chi_2+ # BLOCK NMIX # Neutralino Mixing Matrix 1 1 9.86364430E-01 # N_11 1 2 -5.31103553E-02 # N_12 1 3 1.46433995E-01 # N_13 1 4 -5.31186117E-02 # N_14 2 1 9.93505358E-02 # N_21 2 2 9.44949299E-01 # N_22 2 3 -2.69846720E-01 # N_23 2 4 1.56150698E-01 # N_24 3 1 -6.03388002E-02 # N_31 3 2 8.77004854E-02 # N_32 3 3 6.95877493E-01 # N_33 3 4 7.10226984E-01 # N_34 4 1 -1.16507132E-01 # N_41 4 2 3.10739017E-01 # N_42 4 3 6.49225960E-01 # N_43 4 4 -6.84377823E-01 # N_44 # BLOCK UMIX # Chargino Mixing Matrix U 1 1 9.16834859E-01 # U_11 1 2 -3.99266629E-01 # U_12 2 1 3.99266629E-01 # U_21 2 2 9.16834859E-01 # U_22 # BLOCK VMIX # Chargino Mixing Matrix V 1 1 9.72557835E-01 # V_11 1 2 -2.32661249E-01 # V_12 2 1 2.32661249E-01 # V_21 2 2 9.72557835E-01 # V_22 # BLOCK STOPMIX # Stop Mixing Matrix 1 1 5.53644960E-01 # O_{11} 1 2 8.32752820E-01 # O_{12} 2 1 8.32752820E-01 # O_{21} 2 2 -5.53644960E-01 # O_{22} # BLOCK SBOTMIX # Sbottom Mixing Matrix 1 1 9.38737896E-01 # O_{11} 1 2 3.44631925E-01 # O_{12} 2 1 -3.44631925E-01 # O_{21} 2 2 9.38737896E-01 # O_{22} # BLOCK STAUMIX # Stau Mixing Matrix 1 1 2.82487190E-01 # O_{11} 1 2 9.59271071E-01 # O_{12} 2 1 9.59271071E-01 # O_{21} 2 2 -2.82487190E-01 # O_{22} # BLOCK ALPHA # Higgs mixing -1.13825210E-01 # Mixing angle in the neutral Higgs boson sector # BLOCK HMIX Q= 4.67034192E+02 # DRbar Higgs Parameters 1 3.57680977E+02 # mu(Q)MSSM DRbar 2 9.74862403E+00 # tan beta(Q)MSSM DRba 3 2.44894549E+02 # higgs vev(Q)MSSM DRb 4 1.66439065E+05 # mA^2(Q)MSSM DRbar # BLOCK GAUGE Q= 4.67034192E+02 # The gauge couplings 3 1.10178679E+00 # g3(Q) MSbar # BLOCK AU Q= 4.67034192E+02 # The trilinear couplings 1 1 0.00000000E+00 # A_u(Q) DRbar 2 2 0.00000000E+00 # A_c(Q) DRbar 3 3 -4.98129778E+02 # A_t(Q) DRbar # BLOCK AD Q= 4.67034192E+02 # The trilinear couplings 1 1 0.00000000E+00 # A_d(Q) DRbar 2 2 0.00000000E+00 # A_s(Q) DRbar 3 3 -7.97274397E+02 # A_b(Q) DRbar # BLOCK AE Q= 4.67034192E+02 # The trilinear couplings 1 1 0.00000000E+00 # A_e(Q) DRbar 2 2 0.00000000E+00 # A_mu(Q) DRbar 3 3 -2.51776873E+02 # A_tau(Q) DRbar # BLOCK YU Q= 4.67034192E+02 # The Yukawa couplings 3 3 8.92844550E-01 # y_t(Q) DRbar # BLOCK YD Q= 4.67034192E+02 # The Yukawa couplings 3 3 1.38840206E-01 # y_b(Q) DRbar # BLOCK YE Q= 4.67034192E+02 # The Yukawa couplings 3 3 1.00890810E-01 # y_tau(Q) DRbar # BLOCK MSOFT Q= 4.67034192E+02 # The soft SUSY breaking masses at the scale Q 1 1.01396534E+02 # M_1(Q) 2 1.91504241E+02 # M_2(Q) 3 5.88263031E+02 # M_3(Q) 21 3.23374943E+04 # mH1^2(Q) 22 -1.28800134E+05 # mH2^2(Q) 31 1.95334764E+02 # meL(Q) 32 1.95334764E+02 # mmuL(Q) 33 1.94495956E+02 # mtauL(Q) 34 1.36494061E+02 # meR(Q) 35 1.36494061E+02 # mmuR(Q) 36 1.34043428E+02 # mtauR(Q) 41 5.47573466E+02 # mqL1(Q) 42 5.47573466E+02 # mqL2(Q) 43 4.98763839E+02 # mqL3(Q) 44 5.29511195E+02 # muR(Q) 45 5.29511195E+02 # mcR(Q) 46 4.23245877E+02 # mtR(Q) 47 5.23148807E+02 # mdR(Q) 48 5.23148807E+02 # msR(Q) 49 5.19867261E+02 # mbR(Q) # # # # ================= # |The decay table| # ================= # # - The multi-body decays for the inos, stops and sbottoms are included. # # PDG Width DECAY 25 1.98610799E-03 # h decays # BR NDA ID1 ID2 1.45642955E-01 2 15 -15 # BR(H1 -> tau- tau+) 8.19070713E-01 2 5 -5 # BR(H1 -> b bb) 3.36338173E-02 2 24 -24 # BR(H1 -> W+ W-) 1.65251528E-03 2 23 23 # BR(H1 -> Z Z) # # PDG Width DECAY 35 5.74801389E-01 # H decays # BR NDA ID1 ID2 1.39072676E-01 2 15 -15 # BR(H -> tau- tau+) 4.84110879E-02 2 6 -6 # BR(H -> t tb) 7.89500067E-01 2 5 -5 # BR(H -> b bb) 3.87681171E-03 2 24 -24 # BR(H -> W+ W-) 1.80454752E-03 2 23 23 # BR(H -> Z Z) 0.00000000E+00 2 24 -37 # BR(H -> W+ H-) 0.00000000E+00 2 -24 37 # BR(H -> W- H+) 0.00000000E+00 2 37 -37 # BR(H -> H+ H-) 1.73348101E-02 2 25 25 # BR(H -> h h) 0.00000000E+00 2 36 36 # BR(H -> A A) # # PDG Width DECAY 36 6.32178488E-01 # A decays # BR NDA ID1 ID2 1.26659725E-01 2 15 -15 # BR(A -> tau- tau+) 1.51081526E-01 2 6 -6 # BR(A -> t tb) 7.19406137E-01 2 5 -5 # BR(A -> b bb) 2.85261228E-03 2 23 25 # BR(A -> Z h) 0.00000000E+00 2 23 35 # BR(A -> Z H) 0.00000000E+00 2 24 -37 # BR(A -> W+ H-) 0.00000000E+00 2 -24 37 # BR(A -> W- H+) # # PDG Width DECAY 37 5.46962813E-01 # H+ decays # BR NDA ID1 ID2 1.49435135E-01 2 -15 16 # BR(H+ -> tau+ nu_tau) 8.46811711E-01 2 6 -5 # BR(H+ -> t bb) 3.75315387E-03 2 24 25 # BR(H+ -> W+ h) 0.00000000E+00 2 24 35 # BR(H+ -> W+ H) 0.00000000E+00 2 24 36 # BR(H+ -> W+ A) # # PDG Width DECAY 1000021 5.50675438E+00 # gluino decays # BR NDA ID1 ID2 2.08454202E-02 2 1000001 -1 # BR(~g -> ~d_L db) 2.08454202E-02 2 -1000001 1 # BR(~g -> ~d_L* d ) 5.07075274E-02 2 2000001 -1 # BR(~g -> ~d_R db) 5.07075274E-02 2 -2000001 1 # BR(~g -> ~d_R* d ) 2.89787767E-02 2 1000002 -2 # BR(~g -> ~u_L ub) 2.89787767E-02 2 -1000002 2 # BR(~g -> ~u_L* u ) 4.46872773E-02 2 2000002 -2 # BR(~g -> ~u_R ub) 4.46872773E-02 2 -2000002 2 # BR(~g -> ~u_R* u ) 2.08454202E-02 2 1000003 -3 # BR(~g -> ~s_L sb) 2.08454202E-02 2 -1000003 3 # BR(~g -> ~s_L* s ) 5.07075274E-02 2 2000003 -3 # BR(~g -> ~s_R sb) 5.07075274E-02 2 -2000003 3 # BR(~g -> ~s_R* s ) 2.89787767E-02 2 1000004 -4 # BR(~g -> ~c_L cb) 2.89787767E-02 2 -1000004 4 # BR(~g -> ~c_L* c ) 4.46872773E-02 2 2000004 -4 # BR(~g -> ~c_R cb) 4.46872773E-02 2 -2000004 4 # BR(~g -> ~c_R* c ) 1.05840237E-01 2 1000005 -5 # BR(~g -> ~b_1 bb) 1.05840237E-01 2 -1000005 5 # BR(~g -> ~b_1* b ) 5.56574805E-02 2 2000005 -5 # BR(~g -> ~b_2 bb) 5.56574805E-02 2 -2000005 5 # BR(~g -> ~b_2* b ) 4.80642793E-02 2 1000006 -6 # BR(~g -> ~t_1 tb) 4.80642793E-02 2 -1000006 6 # BR(~g -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~g -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~g -> ~t_2* t ) # # PDG Width DECAY 1000006 2.02159578E+00 # stop1 decays # BR NDA ID1 ID2 1.92947616E-01 2 1000022 6 # BR(~t_1 -> ~chi_10 t ) 1.17469211E-01 2 1000023 6 # BR(~t_1 -> ~chi_20 t ) 0.00000000E+00 2 1000025 6 # BR(~t_1 -> ~chi_30 t ) 0.00000000E+00 2 1000035 6 # BR(~t_1 -> ~chi_40 t ) 6.75747693E-01 2 1000024 5 # BR(~t_1 -> ~chi_1+ b ) 1.38354802E-02 2 1000037 5 # BR(~t_1 -> ~chi_2+ b ) 0.00000000E+00 2 1000021 6 # BR(~t_1 -> ~g t ) 0.00000000E+00 2 1000005 37 # BR(~t_1 -> ~b_1 H+) 0.00000000E+00 2 2000005 37 # BR(~t_1 -> ~b_2 H+) 0.00000000E+00 2 1000005 24 # BR(~t_1 -> ~b_1 W+) 0.00000000E+00 2 2000005 24 # BR(~t_1 -> ~b_2 W+) # # PDG Width DECAY 2000006 7.37313275E+00 # stop2 decays # BR NDA ID1 ID2 2.96825635E-02 2 1000022 6 # BR(~t_2 -> ~chi_10 t ) 8.68035358E-02 2 1000023 6 # BR(~t_2 -> ~chi_20 t ) 4.18408351E-02 2 1000025 6 # BR(~t_2 -> ~chi_30 t ) 1.93281647E-01 2 1000035 6 # BR(~t_2 -> ~chi_40 t ) 2.19632356E-01 2 1000024 5 # BR(~t_2 -> ~chi_1+ b ) 2.02206148E-01 2 1000037 5 # BR(~t_2 -> ~chi_2+ b ) 0.00000000E+00 2 1000021 6 # BR(~t_2 -> ~g t ) 3.66397706E-02 2 1000006 25 # BR(~t_2 -> ~t_1 h ) 0.00000000E+00 2 1000006 35 # BR(~t_2 -> ~t_1 H ) 0.00000000E+00 2 1000006 36 # BR(~t_2 -> ~t_1 A ) 0.00000000E+00 2 1000005 37 # BR(~t_2 -> ~b_1 H+) 0.00000000E+00 2 2000005 37 # BR(~t_2 -> ~b_2 H+) 1.89913144E-01 2 1000006 23 # BR(~t_2 -> ~t_1 Z ) 0.00000000E+00 2 1000005 24 # BR(~t_2 -> ~b_1 W+) 0.00000000E+00 2 2000005 24 # BR(~t_2 -> ~b_2 W+) # # PDG Width DECAY 1000005 3.73627601E+00 # sbottom1 decays # BR NDA ID1 ID2 4.43307074E-02 2 1000022 5 # BR(~b_1 -> ~chi_10 b ) 3.56319904E-01 2 1000023 5 # BR(~b_1 -> ~chi_20 b ) 5.16083795E-03 2 1000025 5 # BR(~b_1 -> ~chi_30 b ) 1.04105080E-02 2 1000035 5 # BR(~b_1 -> ~chi_40 b ) 4.45830064E-01 2 -1000024 6 # BR(~b_1 -> ~chi_1- t ) 0.00000000E+00 2 -1000037 6 # BR(~b_1 -> ~chi_2- t ) 0.00000000E+00 2 1000021 5 # BR(~b_1 -> ~g b ) 0.00000000E+00 2 1000006 -37 # BR(~b_1 -> ~t_1 H-) 0.00000000E+00 2 2000006 -37 # BR(~b_1 -> ~t_2 H-) 1.37947979E-01 2 1000006 -24 # BR(~b_1 -> ~t_1 W-) 0.00000000E+00 2 2000006 -24 # BR(~b_1 -> ~t_2 W-) # # PDG Width DECAY 2000005 8.01566294E-01 # sbottom2 decays # BR NDA ID1 ID2 2.86200590E-01 2 1000022 5 # BR(~b_2 -> ~chi_10 b ) 1.40315912E-01 2 1000023 5 # BR(~b_2 -> ~chi_20 b ) 5.32635592E-02 2 1000025 5 # BR(~b_2 -> ~chi_30 b ) 7.48748121E-02 2 1000035 5 # BR(~b_2 -> ~chi_40 b ) 1.79734294E-01 2 -1000024 6 # BR(~b_2 -> ~chi_1- t ) 0.00000000E+00 2 -1000037 6 # BR(~b_2 -> ~chi_2- t ) 0.00000000E+00 2 1000021 5 # BR(~b_2 -> ~g b ) 0.00000000E+00 2 1000005 25 # BR(~b_2 -> ~b_1 h ) 0.00000000E+00 2 1000005 35 # BR(~b_2 -> ~b_1 H ) 0.00000000E+00 2 1000005 36 # BR(~b_2 -> ~b_1 A ) 0.00000000E+00 2 1000006 -37 # BR(~b_2 -> ~t_1 H-) 0.00000000E+00 2 2000006 -37 # BR(~b_2 -> ~t_2 H-) 0.00000000E+00 2 1000005 23 # BR(~b_2 -> ~b_1 Z ) 2.65610832E-01 2 1000006 -24 # BR(~b_2 -> ~t_1 W-) 0.00000000E+00 2 2000006 -24 # BR(~b_2 -> ~t_2 W-) # # PDG Width DECAY 1000002 5.47719539E+00 # sup_L decays # BR NDA ID1 ID2 6.65240987E-03 2 1000022 2 # BR(~u_L -> ~chi_10 u) 3.19051458E-01 2 1000023 2 # BR(~u_L -> ~chi_20 u) 8.44929059E-04 2 1000025 2 # BR(~u_L -> ~chi_30 u) 1.03485173E-02 2 1000035 2 # BR(~u_L -> ~chi_40 u) 6.49499518E-01 2 1000024 1 # BR(~u_L -> ~chi_1+ d) 1.36031676E-02 2 1000037 1 # BR(~u_L -> ~chi_2+ d) 0.00000000E+00 2 1000021 2 # BR(~u_L -> ~g u) # # PDG Width DECAY 2000002 1.15297292E+00 # sup_R decays # BR NDA ID1 ID2 9.86377420E-01 2 1000022 2 # BR(~u_R -> ~chi_10 u) 8.46640647E-03 2 1000023 2 # BR(~u_R -> ~chi_20 u) 1.23894695E-03 2 1000025 2 # BR(~u_R -> ~chi_30 u) 3.91722611E-03 2 1000035 2 # BR(~u_R -> ~chi_40 u) 0.00000000E+00 2 1000024 1 # BR(~u_R -> ~chi_1+ d) 0.00000000E+00 2 1000037 1 # BR(~u_R -> ~chi_2+ d) 0.00000000E+00 2 1000021 2 # BR(~u_R -> ~g u) # # PDG Width DECAY 1000001 5.31278772E+00 # sdown_L decays # BR NDA ID1 ID2 2.32317969E-02 2 1000022 1 # BR(~d_L -> ~chi_10 d) 3.10235077E-01 2 1000023 1 # BR(~d_L -> ~chi_20 d) 1.52334771E-03 2 1000025 1 # BR(~d_L -> ~chi_30 d) 1.48849798E-02 2 1000035 1 # BR(~d_L -> ~chi_40 d) 6.06452481E-01 2 -1000024 2 # BR(~d_L -> ~chi_1- u) 4.36723179E-02 2 -1000037 2 # BR(~d_L -> ~chi_2- u) 0.00000000E+00 2 1000021 1 # BR(~d_L -> ~g d) # # PDG Width DECAY 2000001 2.85812308E-01 # sdown_R decays # BR NDA ID1 ID2 9.86529614E-01 2 1000022 1 # BR(~d_R -> ~chi_10 d) 8.44510350E-03 2 1000023 1 # BR(~d_R -> ~chi_20 d) 1.21172119E-03 2 1000025 1 # BR(~d_R -> ~chi_30 d) 3.81356102E-03 2 1000035 1 # BR(~d_R -> ~chi_40 d) 0.00000000E+00 2 -1000024 2 # BR(~d_R -> ~chi_1- u) 0.00000000E+00 2 -1000037 2 # BR(~d_R -> ~chi_2- u) 0.00000000E+00 2 1000021 1 # BR(~d_R -> ~g d) # # PDG Width DECAY 1000004 5.47719539E+00 # scharm_L decays # BR NDA ID1 ID2 6.65240987E-03 2 1000022 4 # BR(~c_L -> ~chi_10 c) 3.19051458E-01 2 1000023 4 # BR(~c_L -> ~chi_20 c) 8.44929059E-04 2 1000025 4 # BR(~c_L -> ~chi_30 c) 1.03485173E-02 2 1000035 4 # BR(~c_L -> ~chi_40 c) 6.49499518E-01 2 1000024 3 # BR(~c_L -> ~chi_1+ s) 1.36031676E-02 2 1000037 3 # BR(~c_L -> ~chi_2+ s) 0.00000000E+00 2 1000021 4 # BR(~c_L -> ~g c) # # PDG Width DECAY 2000004 1.15297292E+00 # scharm_R decays # BR NDA ID1 ID2 9.86377420E-01 2 1000022 4 # BR(~c_R -> ~chi_10 c) 8.46640647E-03 2 1000023 4 # BR(~c_R -> ~chi_20 c) 1.23894695E-03 2 1000025 4 # BR(~c_R -> ~chi_30 c) 3.91722611E-03 2 1000035 4 # BR(~c_R -> ~chi_40 c) 0.00000000E+00 2 1000024 3 # BR(~c_R -> ~chi_1+ s) 0.00000000E+00 2 1000037 3 # BR(~c_R -> ~chi_2+ s) 0.00000000E+00 2 1000021 4 # BR(~c_R -> ~g c) # # PDG Width DECAY 1000003 5.31278772E+00 # sstrange_L decays # BR NDA ID1 ID2 2.32317969E-02 2 1000022 3 # BR(~s_L -> ~chi_10 s) 3.10235077E-01 2 1000023 3 # BR(~s_L -> ~chi_20 s) 1.52334771E-03 2 1000025 3 # BR(~s_L -> ~chi_30 s) 1.48849798E-02 2 1000035 3 # BR(~s_L -> ~chi_40 s) 6.06452481E-01 2 -1000024 4 # BR(~s_L -> ~chi_1- c) 4.36723179E-02 2 -1000037 4 # BR(~s_L -> ~chi_2- c) 0.00000000E+00 2 1000021 3 # BR(~s_L -> ~g s) # # PDG Width DECAY 2000003 2.85812308E-01 # sstrange_R decays # BR NDA ID1 ID2 9.86529614E-01 2 1000022 3 # BR(~s_R -> ~chi_10 s) 8.44510350E-03 2 1000023 3 # BR(~s_R -> ~chi_20 s) 1.21172119E-03 2 1000025 3 # BR(~s_R -> ~chi_30 s) 3.81356102E-03 2 1000035 3 # BR(~s_R -> ~chi_40 s) 0.00000000E+00 2 -1000024 4 # BR(~s_R -> ~chi_1- c) 0.00000000E+00 2 -1000037 4 # BR(~s_R -> ~chi_2- c) 0.00000000E+00 2 1000021 3 # BR(~s_R -> ~g s) # # PDG Width DECAY 1000011 2.13682161E-01 # selectron_L decays # BR NDA ID1 ID2 5.73155386E-01 2 1000022 11 # BR(~e_L -> ~chi_10 e-) 1.64522579E-01 2 1000023 11 # BR(~e_L -> ~chi_20 e-) 0.00000000E+00 2 1000025 11 # BR(~e_L -> ~chi_30 e-) 0.00000000E+00 2 1000035 11 # BR(~e_L -> ~chi_40 e-) 2.62322035E-01 2 -1000024 12 # BR(~e_L -> ~chi_1- nu_e) 0.00000000E+00 2 -1000037 12 # BR(~e_L -> ~chi_2- nu_e) # # PDG Width DECAY 2000011 2.16121626E-01 # selectron_R decays # BR NDA ID1 ID2 1.00000000E+00 2 1000022 11 # BR(~e_R -> ~chi_10 e-) 0.00000000E+00 2 1000023 11 # BR(~e_R -> ~chi_20 e-) 0.00000000E+00 2 1000025 11 # BR(~e_R -> ~chi_30 e-) 0.00000000E+00 2 1000035 11 # BR(~e_R -> ~chi_40 e-) 0.00000000E+00 2 -1000024 12 # BR(~e_R -> ~chi_1- nu_e) 0.00000000E+00 2 -1000037 12 # BR(~e_R -> ~chi_2- nu_e) # # PDG Width DECAY 1000013 2.13682161E-01 # smuon_L decays # BR NDA ID1 ID2 5.73155386E-01 2 1000022 13 # BR(~mu_L -> ~chi_10 mu-) 1.64522579E-01 2 1000023 13 # BR(~mu_L -> ~chi_20 mu-) 0.00000000E+00 2 1000025 13 # BR(~mu_L -> ~chi_30 mu-) 0.00000000E+00 2 1000035 13 # BR(~mu_L -> ~chi_40 mu-) 2.62322035E-01 2 -1000024 14 # BR(~mu_L -> ~chi_1- nu_mu) 0.00000000E+00 2 -1000037 14 # BR(~mu_L -> ~chi_2- nu_mu) # # PDG Width DECAY 2000013 2.16121626E-01 # smuon_R decays # BR NDA ID1 ID2 1.00000000E+00 2 1000022 13 # BR(~mu_R -> ~chi_10 mu-) 0.00000000E+00 2 1000023 13 # BR(~mu_R -> ~chi_20 mu-) 0.00000000E+00 2 1000025 13 # BR(~mu_R -> ~chi_30 mu-) 0.00000000E+00 2 1000035 13 # BR(~mu_R -> ~chi_40 mu-) 0.00000000E+00 2 -1000024 14 # BR(~mu_R -> ~chi_1- nu_mu) 0.00000000E+00 2 -1000037 14 # BR(~mu_R -> ~chi_2- nu_mu) # # PDG Width DECAY 1000015 1.48327268E-01 # stau_1 decays # BR NDA ID1 ID2 1.00000000E+00 2 1000022 15 # BR(~tau_1 -> ~chi_10 tau-) 0.00000000E+00 2 1000023 15 # BR(~tau_1 -> ~chi_20 tau-) 0.00000000E+00 2 1000025 15 # BR(~tau_1 -> ~chi_30 tau-) 0.00000000E+00 2 1000035 15 # BR(~tau_1 -> ~chi_40 tau-) 0.00000000E+00 2 -1000024 16 # BR(~tau_1 -> ~chi_1- nu_tau) 0.00000000E+00 2 -1000037 16 # BR(~tau_1 -> ~chi_2- nu_tau) 0.00000000E+00 2 1000016 -37 # BR(~tau_1 -> ~nu_tauL H-) 0.00000000E+00 2 1000016 -24 # BR(~tau_1 -> ~nu_tauL W-) # # PDG Width DECAY 2000015 2.69906096E-01 # stau_2 decays # BR NDA ID1 ID2 5.96653046E-01 2 1000022 15 # BR(~tau_2 -> ~chi_10 tau-) 1.54536760E-01 2 1000023 15 # BR(~tau_2 -> ~chi_20 tau-) 0.00000000E+00 2 1000025 15 # BR(~tau_2 -> ~chi_30 tau-) 0.00000000E+00 2 1000035 15 # BR(~tau_2 -> ~chi_40 tau-) 2.48810195E-01 2 -1000024 16 # BR(~tau_2 -> ~chi_1- nu_tau) 0.00000000E+00 2 -1000037 16 # BR(~tau_2 -> ~chi_2- nu_tau) 0.00000000E+00 2 1000016 -37 # BR(~tau_2 -> ~nu_tauL H-) 0.00000000E+00 2 1000016 -24 # BR(~tau_2 -> ~nu_tauL W-) 0.00000000E+00 2 1000015 25 # BR(~tau_2 -> ~tau_1 h) 0.00000000E+00 2 1000015 35 # BR(~tau_2 -> ~tau_1 H) 0.00000000E+00 2 1000015 36 # BR(~tau_2 -> ~tau_1 A) 0.00000000E+00 2 1000015 23 # BR(~tau_2 -> ~tau_1 Z) # # PDG Width DECAY 1000012 1.49881634E-01 # snu_eL decays # BR NDA ID1 ID2 9.77700764E-01 2 1000022 12 # BR(~nu_eL -> ~chi_10 nu_e) 8.11554922E-03 2 1000023 12 # BR(~nu_eL -> ~chi_20 nu_e) 0.00000000E+00 2 1000025 12 # BR(~nu_eL -> ~chi_30 nu_e) 0.00000000E+00 2 1000035 12 # BR(~nu_eL -> ~chi_40 nu_e) 1.41836867E-02 2 1000024 11 # BR(~nu_eL -> ~chi_1+ e-) 0.00000000E+00 2 1000037 11 # BR(~nu_eL -> ~chi_2+ e-) # # PDG Width DECAY 1000014 1.49881634E-01 # snu_muL decays # BR NDA ID1 ID2 9.77700764E-01 2 1000022 14 # BR(~nu_muL -> ~chi_10 nu_mu) 8.11554922E-03 2 1000023 14 # BR(~nu_muL -> ~chi_20 nu_mu) 0.00000000E+00 2 1000025 14 # BR(~nu_muL -> ~chi_30 nu_mu) 0.00000000E+00 2 1000035 14 # BR(~nu_muL -> ~chi_40 nu_mu) 1.41836867E-02 2 1000024 13 # BR(~nu_muL -> ~chi_1+ mu-) 0.00000000E+00 2 1000037 13 # BR(~nu_muL -> ~chi_2+ mu-) # # PDG Width DECAY 1000016 1.47518977E-01 # snu_tauL decays # BR NDA ID1 ID2 9.85994529E-01 2 1000022 16 # BR(~nu_tauL -> ~chi_10 nu_tau) 6.25129612E-03 2 1000023 16 # BR(~nu_tauL -> ~chi_20 nu_tau) 0.00000000E+00 2 1000025 16 # BR(~nu_tauL -> ~chi_30 nu_tau) 0.00000000E+00 2 1000035 16 # BR(~nu_tauL -> ~chi_40 nu_tau) 7.75417479E-03 2 1000024 15 # BR(~nu_tauL -> ~chi_1+ tau-) 0.00000000E+00 2 1000037 15 # BR(~nu_tauL -> ~chi_2+ tau-) 0.00000000E+00 2 -1000015 -37 # BR(~nu_tauL -> ~tau_1+ H-) 0.00000000E+00 2 -2000015 -37 # BR(~nu_tauL -> ~tau_2+ H-) 0.00000000E+00 2 -1000015 -24 # BR(~nu_tauL -> ~tau_1+ W-) 0.00000000E+00 2 -2000015 -24 # BR(~nu_tauL -> ~tau_2+ W-) # # PDG Width DECAY 1000024 1.70414503E-02 # chargino1+ decays # BR NDA ID1 ID2 0.00000000E+00 2 1000002 -1 # BR(~chi_1+ -> ~u_L db) 0.00000000E+00 2 2000002 -1 # BR(~chi_1+ -> ~u_R db) 0.00000000E+00 2 -1000001 2 # BR(~chi_1+ -> ~d_L* u ) 0.00000000E+00 2 -2000001 2 # BR(~chi_1+ -> ~d_R* u ) 0.00000000E+00 2 1000004 -3 # BR(~chi_1+ -> ~c_L sb) 0.00000000E+00 2 2000004 -3 # BR(~chi_1+ -> ~c_R sb) 0.00000000E+00 2 -1000003 4 # BR(~chi_1+ -> ~s_L* c ) 0.00000000E+00 2 -2000003 4 # BR(~chi_1+ -> ~s_R* c ) 0.00000000E+00 2 1000006 -5 # BR(~chi_1+ -> ~t_1 bb) 0.00000000E+00 2 2000006 -5 # BR(~chi_1+ -> ~t_2 bb) 0.00000000E+00 2 -1000005 6 # BR(~chi_1+ -> ~b_1* t ) 0.00000000E+00 2 -2000005 6 # BR(~chi_1+ -> ~b_2* t ) 0.00000000E+00 2 1000012 -11 # BR(~chi_1+ -> ~nu_eL e+ ) 0.00000000E+00 2 1000014 -13 # BR(~chi_1+ -> ~nu_muL mu+ ) 0.00000000E+00 2 1000016 -15 # BR(~chi_1+ -> ~nu_tau1 tau+) 0.00000000E+00 2 -1000011 12 # BR(~chi_1+ -> ~e_L+ nu_e) 0.00000000E+00 2 -2000011 12 # BR(~chi_1+ -> ~e_R+ nu_e) 0.00000000E+00 2 -1000013 14 # BR(~chi_1+ -> ~mu_L+ nu_mu) 0.00000000E+00 2 -2000013 14 # BR(~chi_1+ -> ~mu_R+ nu_mu) 9.25161117E-01 2 -1000015 16 # BR(~chi_1+ -> ~tau_1+ nu_tau) 0.00000000E+00 2 -2000015 16 # BR(~chi_1+ -> ~tau_2+ nu_tau) 7.48388828E-02 2 1000022 24 # BR(~chi_1+ -> ~chi_10 W+) 0.00000000E+00 2 1000023 24 # BR(~chi_1+ -> ~chi_20 W+) 0.00000000E+00 2 1000025 24 # BR(~chi_1+ -> ~chi_30 W+) 0.00000000E+00 2 1000035 24 # BR(~chi_1+ -> ~chi_40 W+) 0.00000000E+00 2 1000022 37 # BR(~chi_1+ -> ~chi_10 H+) 0.00000000E+00 2 1000023 37 # BR(~chi_1+ -> ~chi_20 H+) 0.00000000E+00 2 1000025 37 # BR(~chi_1+ -> ~chi_30 H+) 0.00000000E+00 2 1000035 37 # BR(~chi_1+ -> ~chi_40 H+) # # PDG Width DECAY 1000037 2.48689510E+00 # chargino2+ decays # BR NDA ID1 ID2 0.00000000E+00 2 1000002 -1 # BR(~chi_2+ -> ~u_L db) 0.00000000E+00 2 2000002 -1 # BR(~chi_2+ -> ~u_R db) 0.00000000E+00 2 -1000001 2 # BR(~chi_2+ -> ~d_L* u ) 0.00000000E+00 2 -2000001 2 # BR(~chi_2+ -> ~d_R* u ) 0.00000000E+00 2 1000004 -3 # BR(~chi_2+ -> ~c_L sb) 0.00000000E+00 2 2000004 -3 # BR(~chi_2+ -> ~c_R sb) 0.00000000E+00 2 -1000003 4 # BR(~chi_2+ -> ~s_L* c ) 0.00000000E+00 2 -2000003 4 # BR(~chi_2+ -> ~s_R* c ) 0.00000000E+00 2 1000006 -5 # BR(~chi_2+ -> ~t_1 bb) 0.00000000E+00 2 2000006 -5 # BR(~chi_2+ -> ~t_2 bb) 0.00000000E+00 2 -1000005 6 # BR(~chi_2+ -> ~b_1* t ) 0.00000000E+00 2 -2000005 6 # BR(~chi_2+ -> ~b_2* t ) 2.00968837E-02 2 1000012 -11 # BR(~chi_2+ -> ~nu_eL e+ ) 2.00968837E-02 2 1000014 -13 # BR(~chi_2+ -> ~nu_muL mu+ ) 2.74507395E-02 2 1000016 -15 # BR(~chi_2+ -> ~nu_tau1 tau+) 5.20406111E-02 2 -1000011 12 # BR(~chi_2+ -> ~e_L+ nu_e) 0.00000000E+00 2 -2000011 12 # BR(~chi_2+ -> ~e_R+ nu_e) 5.20406111E-02 2 -1000013 14 # BR(~chi_2+ -> ~mu_L+ nu_mu) 0.00000000E+00 2 -2000013 14 # BR(~chi_2+ -> ~mu_R+ nu_mu) 2.82859898E-04 2 -1000015 16 # BR(~chi_2+ -> ~tau_1+ nu_tau) 5.66729336E-02 2 -2000015 16 # BR(~chi_2+ -> ~tau_2+ nu_tau) 2.31513269E-01 2 1000024 23 # BR(~chi_2+ -> ~chi_1+ Z ) 6.76715120E-02 2 1000022 24 # BR(~chi_2+ -> ~chi_10 W+) 2.93654849E-01 2 1000023 24 # BR(~chi_2+ -> ~chi_20 W+) 0.00000000E+00 2 1000025 24 # BR(~chi_2+ -> ~chi_30 W+) 0.00000000E+00 2 1000035 24 # BR(~chi_2+ -> ~chi_40 W+) 1.78478848E-01 2 1000024 25 # BR(~chi_2+ -> ~chi_1+ h ) 0.00000000E+00 2 1000024 35 # BR(~chi_2+ -> ~chi_1+ H ) 0.00000000E+00 2 1000024 36 # BR(~chi_2+ -> ~chi_1+ A ) 0.00000000E+00 2 1000022 37 # BR(~chi_2+ -> ~chi_10 H+) 0.00000000E+00 2 1000023 37 # BR(~chi_2+ -> ~chi_20 H+) 0.00000000E+00 2 1000025 37 # BR(~chi_2+ -> ~chi_30 H+) 0.00000000E+00 2 1000035 37 # BR(~chi_2+ -> ~chi_40 H+) # # PDG Width DECAY 1000022 0.00000000E+00 # neutralino1 decays # # PDG Width DECAY 1000023 2.07770048E-02 # neutralino2 decays # BR NDA ID1 ID2 0.00000000E+00 2 1000022 23 # BR(~chi_20 -> ~chi_10 Z ) 0.00000000E+00 2 1000024 -24 # BR(~chi_20 -> ~chi_1+ W-) 0.00000000E+00 2 -1000024 24 # BR(~chi_20 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_20 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_20 -> ~chi_2- W+) 0.00000000E+00 2 1000022 25 # BR(~chi_20 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_20 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_20 -> ~chi_10 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_20 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_20 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_20 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_20 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_20 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_20 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_20 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_20 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_20 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_20 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_20 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_20 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_20 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_20 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_20 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_20 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_20 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_20 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_20 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_20 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_20 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_20 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_20 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_20 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_20 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_20 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_20 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_20 -> ~b_2* b ) 0.00000000E+00 2 1000011 -11 # BR(~chi_20 -> ~e_L- e+) 0.00000000E+00 2 -1000011 11 # BR(~chi_20 -> ~e_L+ e-) 2.95071995E-02 2 2000011 -11 # BR(~chi_20 -> ~e_R- e+) 2.95071995E-02 2 -2000011 11 # BR(~chi_20 -> ~e_R+ e-) 0.00000000E+00 2 1000013 -13 # BR(~chi_20 -> ~mu_L- mu+) 0.00000000E+00 2 -1000013 13 # BR(~chi_20 -> ~mu_L+ mu-) 2.95071995E-02 2 2000013 -13 # BR(~chi_20 -> ~mu_R- mu+) 2.95071995E-02 2 -2000013 13 # BR(~chi_20 -> ~mu_R+ mu-) 4.40985601E-01 2 1000015 -15 # BR(~chi_20 -> ~tau_1- tau+) 4.40985601E-01 2 -1000015 15 # BR(~chi_20 -> ~tau_1+ tau-) 0.00000000E+00 2 2000015 -15 # BR(~chi_20 -> ~tau_2- tau+) 0.00000000E+00 2 -2000015 15 # BR(~chi_20 -> ~tau_2+ tau-) 0.00000000E+00 2 1000012 -12 # BR(~chi_20 -> ~nu_eL nu_eb) 0.00000000E+00 2 -1000012 12 # BR(~chi_20 -> ~nu_eL* nu_e ) 0.00000000E+00 2 1000014 -14 # BR(~chi_20 -> ~nu_muL nu_mub) 0.00000000E+00 2 -1000014 14 # BR(~chi_20 -> ~nu_muL* nu_mu ) 0.00000000E+00 2 1000016 -16 # BR(~chi_20 -> ~nu_tau1 nu_taub) 0.00000000E+00 2 -1000016 16 # BR(~chi_20 -> ~nu_tau1* nu_tau ) # # PDG Width DECAY 1000025 1.91598495E+00 # neutralino3 decays # BR NDA ID1 ID2 1.13226601E-01 2 1000022 23 # BR(~chi_30 -> ~chi_10 Z ) 2.11969194E-01 2 1000023 23 # BR(~chi_30 -> ~chi_20 Z ) 2.95329778E-01 2 1000024 -24 # BR(~chi_30 -> ~chi_1+ W-) 2.95329778E-01 2 -1000024 24 # BR(~chi_30 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_30 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_30 -> ~chi_2- W+) 2.13076490E-02 2 1000022 25 # BR(~chi_30 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_30 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_30 -> ~chi_10 A ) 1.24538329E-02 2 1000023 25 # BR(~chi_30 -> ~chi_20 h ) 0.00000000E+00 2 1000023 35 # BR(~chi_30 -> ~chi_20 H ) 0.00000000E+00 2 1000023 36 # BR(~chi_30 -> ~chi_20 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_30 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_30 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_30 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_30 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_30 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_30 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_30 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_30 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_30 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_30 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_30 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_30 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_30 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_30 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_30 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_30 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_30 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_30 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_30 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_30 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_30 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_30 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_30 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_30 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_30 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_30 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_30 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_30 -> ~b_2* b ) 5.57220455E-04 2 1000011 -11 # BR(~chi_30 -> ~e_L- e+) 5.57220455E-04 2 -1000011 11 # BR(~chi_30 -> ~e_L+ e-) 1.25266782E-03 2 2000011 -11 # BR(~chi_30 -> ~e_R- e+) 1.25266782E-03 2 -2000011 11 # BR(~chi_30 -> ~e_R+ e-) 5.57220455E-04 2 1000013 -13 # BR(~chi_30 -> ~mu_L- mu+) 5.57220455E-04 2 -1000013 13 # BR(~chi_30 -> ~mu_L+ mu-) 1.25266782E-03 2 2000013 -13 # BR(~chi_30 -> ~mu_R- mu+) 1.25266782E-03 2 -2000013 13 # BR(~chi_30 -> ~mu_R+ mu-) 5.26279239E-03 2 1000015 -15 # BR(~chi_30 -> ~tau_1- tau+) 5.26279239E-03 2 -1000015 15 # BR(~chi_30 -> ~tau_1+ tau-) 6.72814564E-03 2 2000015 -15 # BR(~chi_30 -> ~tau_2- tau+) 6.72814564E-03 2 -2000015 15 # BR(~chi_30 -> ~tau_2+ tau-) 3.18920485E-03 2 1000012 -12 # BR(~chi_30 -> ~nu_eL nu_eb) 3.18920485E-03 2 -1000012 12 # BR(~chi_30 -> ~nu_eL* nu_e ) 3.18920485E-03 2 1000014 -14 # BR(~chi_30 -> ~nu_muL nu_mub) 3.18920485E-03 2 -1000014 14 # BR(~chi_30 -> ~nu_muL* nu_mu ) 3.20245934E-03 2 1000016 -16 # BR(~chi_30 -> ~nu_tau1 nu_taub) 3.20245934E-03 2 -1000016 16 # BR(~chi_30 -> ~nu_tau1* nu_tau ) # # PDG Width DECAY 1000035 2.58585079E+00 # neutralino4 decays # BR NDA ID1 ID2 2.15369294E-02 2 1000022 23 # BR(~chi_40 -> ~chi_10 Z ) 1.85499971E-02 2 1000023 23 # BR(~chi_40 -> ~chi_20 Z ) 0.00000000E+00 2 1000025 23 # BR(~chi_40 -> ~chi_30 Z ) 2.49541430E-01 2 1000024 -24 # BR(~chi_40 -> ~chi_1+ W-) 2.49541430E-01 2 -1000024 24 # BR(~chi_40 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_40 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_40 -> ~chi_2- W+) 6.93213268E-02 2 1000022 25 # BR(~chi_40 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_40 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_40 -> ~chi_10 A ) 1.47602336E-01 2 1000023 25 # BR(~chi_40 -> ~chi_20 h ) 0.00000000E+00 2 1000023 35 # BR(~chi_40 -> ~chi_20 H ) 0.00000000E+00 2 1000023 36 # BR(~chi_40 -> ~chi_20 A ) 0.00000000E+00 2 1000025 25 # BR(~chi_40 -> ~chi_30 h ) 0.00000000E+00 2 1000025 35 # BR(~chi_40 -> ~chi_30 H ) 0.00000000E+00 2 1000025 36 # BR(~chi_40 -> ~chi_30 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_40 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_40 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_40 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_40 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_40 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_40 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_40 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_40 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_40 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_40 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_40 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_40 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_40 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_40 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_40 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_40 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_40 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_40 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_40 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_40 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_40 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_40 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_40 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_40 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_40 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_40 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_40 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_40 -> ~b_2* b ) 9.64835418E-03 2 1000011 -11 # BR(~chi_40 -> ~e_L- e+) 9.64835418E-03 2 -1000011 11 # BR(~chi_40 -> ~e_L+ e-) 3.75684470E-03 2 2000011 -11 # BR(~chi_40 -> ~e_R- e+) 3.75684470E-03 2 -2000011 11 # BR(~chi_40 -> ~e_R+ e-) 9.64835418E-03 2 1000013 -13 # BR(~chi_40 -> ~mu_L- mu+) 9.64835418E-03 2 -1000013 13 # BR(~chi_40 -> ~mu_L+ mu-) 3.75684470E-03 2 2000013 -13 # BR(~chi_40 -> ~mu_R- mu+) 3.75684470E-03 2 -2000013 13 # BR(~chi_40 -> ~mu_R+ mu-) 2.68215241E-03 2 1000015 -15 # BR(~chi_40 -> ~tau_1- tau+) 2.68215241E-03 2 -1000015 15 # BR(~chi_40 -> ~tau_1+ tau-) 1.62289809E-02 2 2000015 -15 # BR(~chi_40 -> ~tau_2- tau+) 1.62289809E-02 2 -2000015 15 # BR(~chi_40 -> ~tau_2+ tau-) 2.53796547E-02 2 1000012 -12 # BR(~chi_40 -> ~nu_eL nu_eb) 2.53796547E-02 2 -1000012 12 # BR(~chi_40 -> ~nu_eL* nu_e ) 2.53796547E-02 2 1000014 -14 # BR(~chi_40 -> ~nu_muL nu_mub) 2.53796547E-02 2 -1000014 14 # BR(~chi_40 -> ~nu_muL* nu_mu ) 2.54724352E-02 2 1000016 -16 # BR(~chi_40 -> ~nu_tau1 nu_taub) 2.54724352E-02 2 -1000016 16 # BR(~chi_40 -> ~nu_tau1* nu_tau ) pythia8-8.1.80.orig/examples/w+_production_lhc_2.lhe0000644000175000017500000036601512217346207020516 0ustar sunsun
      # MG/ME version : 4.4.48 # madgraph version : 4.4.5 # template version : 2.4.25 # helas version : 3.8 # model version : sm_1.2.1 #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # proc_card.dat * # * # This file is used to generate the code for a specific process. * # Some notation/conventions: * # * # 0. Do not modify the TAGS and their order. * # 1. hash/pound is a comment. * # 2. The number after the @ is used as an identifier for the class * # of processes. It can be any positive integer. * # 3. The number of lines for the max couplings depends on how many * # different classes of couplings are present in the model * # In the SM these are just two: QED (which include EW) and QCD * # 4. Write "end_coup" after the couplings list, * # to tell MG that the couplings input is over. * # 5. Write "done" after the proc list to * # to tell MG that the proc input is over. * # 6. Some model names available at present are: * # sm = Standard Model * # smckm = Standard Model with Cabibbo matrix * # mssm = Minimal Supersymmetric Standard Model * # 2hdm = Generic Two Higgs Doublet model * # heft = Higgs EFT (+Standard Model) * # usrmod = User Model * # 7. Don't leave spaces between the particles name in the * # definition of the multiparticles. * #********************************************************************* #********************************************************************* # Process(es) requested : mg2 input * #********************************************************************* # Begin PROCESS # This is TAG. Do not modify this line pp>e+vejj @1 # First Process QCD=99 # Max QCD couplings QED=2 # Max QED couplings end_coup # End the couplings input done # this tells MG there are no more procs # End PROCESS # This is TAG. Do not modify this line #********************************************************************* # Model information * #********************************************************************* # Begin MODEL # This is TAG. Do not modify this line sm # End MODEL # This is TAG. Do not modify this line #********************************************************************* # Start multiparticle definitions * #********************************************************************* # Begin MULTIPARTICLES # This is TAG. Do not modify this line P uu~dd~cc~ss~g J uu~dd~cc~ss~g L+ e+mu+ L- e-mu- vl vevm vl~ ve~vm~ # End MULTIPARTICLES # This is TAG. Do not modify this line #****************************************************************** # MadGraph/MadEvent * #****************************************************************** # Les Houches friendly file for the SM parameters of MadGraph * # Spectrum and decay widths produced by SMCalc * #****************************************************************** #*Please note the following IMPORTANT issues: * # * #0. REFRAIN from editing this file by hand! Some of the parame- * # ters are not independent * # (such as G_Fermi, alpha_em, sin(theta_W),MZ,MW) and serious * # problems might be encountered (such as violation of unitarity * # or gauge invariance). Always use a calculator. * # * #1. alpha_S(MZ) has been used in the calculation of the parameters* # but, for consistency, it will be reset by madgraph to the * # value expected IF the pdfs for collisions with hadrons are * # used. This value is KEPT by madgraph when no pdf are used * # lpp(i)=0 . * # * #2. Values of the charm and bottom kinematic (pole) masses are * # those used in the matrix elements and phase space UNLESS they * # are set to ZERO from the start in the model (particles.dat) * # This happens, for example, when using 5-flavor QCD where * # charm and bottom are treated as partons in the initial state * # and a zero mass might be hardwired in the model definition. * # * #****************************************************************** Block SMINPUTS # Standard Model inputs 1 1.32506980E+02 # alpha_em(MZ)(-1) SM MSbar 2 1.16639000E-05 # G_Fermi 3 1.18000000E-01 # alpha_s(MZ) SM MSbar 4 9.11880000E+01 # Z mass (as input parameter) Block MGYUKAWA # Yukawa masses m/v=y/sqrt(2) # PDG YMASS 5 4.20000000E+00 # mbottom for the Yukawa y_b 4 1.42000000E+00 # mcharm for the Yukawa y_c 6 1.64500000E+02 # mtop for the Yukawa y_t 15 1.77700000E+00 # mtau for the Yukawa y_ta Block MGCKM # CKM elements for MadGraph 1 1 9.75000000E-01 # Vud for Cabibbo matrix Block MASS # Mass spectrum (kinematic masses) # PDG Mass 5 4.70000000E+00 # bottom pole mass 6 1.74300000E+02 # top pole mass 15 1.77700000E+00 # tau mass 23 9.11880000E+01 # Z mass 24 8.04190000E+01 # W mass 25 1.20000000E+02 # H mass # PDG Width DECAY 6 1.50833649E+00 # top width DECAY 23 2.44140351E+00 # Z width DECAY 24 2.04759951E+00 # W width DECAY 25 5.75308848E-03 # H width # BR NDA ID1 ID2 8.27451012E-02 2 4 -4 # BR( H -> c cbar ) 7.17809696E-01 2 5 -5 # BR( H -> b bbar ) 0.00000000E+00 2 6 -6 # BR( H -> t tbar ) 4.31720144E-02 2 15 -15 # BR( H -> tau- tau+) 6.90597075E-03 2 23 23 # BR( H -> Z Z^(*)) 7.45906395E-02 2 24 -24 # BR( H -> W W^(*)) 3.01765558E-02 2 21 21 # BR( H -> g g ) 1.42800773E-03 2 22 22 # BR( H -> A A ) #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # run_card.dat * # * # This file is used to set the parameters of the run. * # * # Some notation/conventions: * # * # Lines starting with a '# ' are info or comments * # * # mind the format: value = variable ! comment * #********************************************************************* # #******************* # Running parameters #******************* # #********************************************************************* # Tag name for the run (one word) * #********************************************************************* 'fermi' = run_tag ! name of the run #********************************************************************* # Run to generate the grid pack * #********************************************************************* .false. = gridpack !True = setting up the grid pack #********************************************************************* # Number of events and rnd seed * #********************************************************************* 100 = nevents ! Number of unweighted events requested 25531 = iseed ! rnd seed (0=assigned automatically=default)) #********************************************************************* # Collider type and energy * #********************************************************************* 1 = lpp1 ! beam 1 type (0=NO PDF) 1 = lpp2 ! beam 2 type (0=NO PDF) 3500.0 = ebeam1 ! beam 1 energy in GeV 3500.0 = ebeam2 ! beam 2 energy in GeV #********************************************************************* # Beam polarization from -100 (left-handed) to 100 (right-handed) * #********************************************************************* 0 = polbeam1 ! beam polarization for beam 1 0 = polbeam2 ! beam polarization for beam 2 #********************************************************************* # PDF CHOICE: this automatically fixes also alpha_s and its evol. * #********************************************************************* # 'cteq6_l' = pdlabel ! PDF set 'lhapdf' = pdlabel ! PDF label 10042 = lhaid ! PDF set #********************************************************************* # Renormalization and factorization scales * #********************************************************************* T = fixed_ren_scale ! if .true. use fixed ren scale T = fixed_fac_scale ! if .true. use fixed fac scale 91.188 = scale ! fixed ren scale 80.4 = dsqrt_q2fact1 ! fixed fact scale for pdf1 80.4 = dsqrt_q2fact2 ! fixed fact scale for pdf2 1 = scalefact ! scale factor for event-by-event scales #********************************************************************* # Matching - Warning! ickkw > 0 is still beta #********************************************************************* 0 = ickkw ! 0 no matching, 1 MLM, 2 CKKW matching 1 = highestmult ! for ickkw=2, highest mult group 1 = ktscheme ! for ickkw=1, 1 Durham kT, 2 Pythia pTE 1 = alpsfact ! scale factor for QCD emission vx F = chcluster ! cluster only according to channel diag F = pdfwgt ! for ickkw=1, perform pdf reweighting #********************************************************************* # #********************************** # BW cutoff (M+/-bwcutoff*Gamma) #********************************** 15d0 = bwcutoff #******************* # Standard Cuts #******************* # #********************************************************************* # Minimum and maximum pt's * #********************************************************************* 0d0 = ptj ! minimum pt for the jets 0d0 = ptb ! minimum pt for the b 0d0 = pta ! minimum pt for the photons 0d0 = ptl ! minimum pt for the charged leptons 0d0 = misset ! minimum missing Et (sum of neutrino's momenta) 0d0 = ptheavy ! minimum pt for one heavy final state 0d0 = ptonium ! minimum pt for the quarkonium states 1d9 = ptjmax ! maximum pt for the jets 1d9 = ptbmax ! maximum pt for the b 1d9 = ptamax ! maximum pt for the photons 1d9 = ptlmax ! maximum pt for the charged leptons 1d9 = missetmax ! maximum missing Et (sum of neutrino's momenta) #********************************************************************* # Minimum and maximum E's (in the lab frame) * #********************************************************************* 0d0 = ej ! minimum E for the jets 0d0 = eb ! minimum E for the b 0d0 = ea ! minimum E for the photons 0d0 = el ! minimum E for the charged leptons 1d9 = ejmax ! maximum E for the jets 1d9 = ebmax ! maximum E for the b 1d9 = eamax ! maximum E for the photons 1d9 = elmax ! maximum E for the charged leptons #********************************************************************* # Maximum and minimum rapidity * #********************************************************************* 1d9 = etaj ! max rap for the jets 1d9 = etab ! max rap for the b 1d9 = etaa ! max rap for the photons 1d9 = etal ! max rap for the charged leptons 1d9 = etaonium ! max rap for the quarkonium states 0d0 = etajmin ! min rap for the jets 0d0 = etabmin ! min rap for the b 0d0 = etaamin ! min rap for the photons 0d0 = etalmin ! main rap for the charged leptons #********************************************************************* # Minimum and maximum DeltaR distance * #********************************************************************* 0d0 = drjj ! min distance between jets 0d0 = drbb ! min distance between b's 0d0 = drll ! min distance between leptons 0d0 = draa ! min distance between gammas 0d0 = drbj ! min distance between b and jet 0d0 = draj ! min distance between gamma and jet 0d0 = drjl ! min distance between jet and lepton 0d0 = drab ! min distance between gamma and b 0d0 = drbl ! min distance between b and lepton 0d0 = dral ! min distance between gamma and lepton 1d9 = drjjmax ! max distance between jets 1d9 = drbbmax ! max distance between b's 1d9 = drllmax ! max distance between leptons 1d9 = draamax ! max distance between gammas 1d9 = drbjmax ! max distance between b and jet 1d9 = drajmax ! max distance between gamma and jet 1d9 = drjlmax ! max distance between jet and lepton 1d9 = drabmax ! max distance between gamma and b 1d9 = drblmax ! max distance between b and lepton 1d9 = dralmax ! maxdistance between gamma and lepton #********************************************************************* # Minimum and maximum invariant mass for pairs * #********************************************************************* 0d0 = mmjj ! min invariant mass of a jet pair 0d0 = mmbb ! min invariant mass of a b pair 0d0 = mmaa ! min invariant mass of gamma gamma pair 0d0 = mmll ! min invariant mass of l+l- (same flavour) lepton pair 1d9 = mmjjmax ! max invariant mass of a jet pair 1d9 = mmbbmax ! max invariant mass of a b pair 1d9 = mmaamax ! max invariant mass of gamma gamma pair 1d9 = mmllmax ! max invariant mass of l+l- (same flavour) lepton pair #********************************************************************* # Minimum and maximum invariant mass for all letpons * #********************************************************************* 0d0 = mmnl ! min invariant mass for all letpons (l+- and vl) 1d9 = mmnlmax ! max invariant mass for all letpons (l+- and vl) #********************************************************************* # Inclusive cuts * #********************************************************************* 0d0 = xptj ! minimum pt for at least one jet 0d0 = xptb ! minimum pt for at least one b 0d0 = xpta ! minimum pt for at least one photon 0d0 = xptl ! minimum pt for at least one charged lepton #********************************************************************* # Control the pt's of the jets sorted by pt * #********************************************************************* 0d0 = ptj1min ! minimum pt for the leading jet in pt 0d0 = ptj2min ! minimum pt for the second jet in pt 0d0 = ptj3min ! minimum pt for the third jet in pt 0d0 = ptj4min ! minimum pt for the fourth jet in pt 1d9 = ptj1max ! maximum pt for the leading jet in pt 1d9 = ptj2max ! maximum pt for the second jet in pt 1d9 = ptj3max ! maximum pt for the third jet in pt 1d9 = ptj4max ! maximum pt for the fourth jet in pt 0 = cutuse ! reject event if fails any (0) / all (1) jet pt cuts #********************************************************************* # Control the Ht(k)=Sum of k leading jets * #********************************************************************* 0d0 = htjmin ! minimum jet HT=Sum(jet pt) 1d9 = htjmax ! maximum jet HT=Sum(jet pt) 0d0 = ht2min ! minimum Ht for the two leading jets 0d0 = ht3min ! minimum Ht for the three leading jets 0d0 = ht4min ! minimum Ht for the four leading jets 1d9 = ht2max ! maximum Ht for the two leading jets 1d9 = ht3max ! maximum Ht for the three leading jets 1d9 = ht4max ! maximum Ht for the four leading jets #********************************************************************* # WBF cuts * #********************************************************************* 0 = xetamin ! minimum rapidity for two jets in the WBF case 0 = deltaeta ! minimum rapidity for two jets in the WBF case #********************************************************************* # maximal pdg code for quark to be considered as a jet * # otherwise b cuts are applied * #********************************************************************* 4 = maxjetflavor #********************************************************************* # Jet measure cuts * #********************************************************************* 0 = xqcut ! minimum kt jet measure between partons #********************************************************************* 30d0 = ktdurham ! minimum durham kt jet measure between partons 0.4 = dparameter ! D parameter for hadronic kT T = dokt ! T: enable durham kt cut #********************************************************************* # Number of Events : 100 # Integrated weight (pb) : .14364E+03 # Truncated wgt (pb) : .33911E+00 # Unit wgt : .14364E+01
      2212 2212 0.35000000000E+04 0.35000000000E+04 0 0 10042 10042 3 1 0.14364000000E+03 0.22892000000E+02 0.14364000000E+01 1 7 1 0.1436400E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.12445661806E+03 0.12445661806E+03 0.00000000000E+00 0. 1. 2 -1 0 0 502 0 0.00000000000E+00 0.00000000000E+00 -0.83658800179E+03 0.83658800179E+03 0.00000000000E+00 0. -1. 24 2 1 2 0 0 -0.36481067053E+02 -0.11381786397E+03 -0.40635105062E+03 0.43130873836E+03 0.81367542855E+02 0. 0. -11 1 3 3 0 0 -0.19230533854E+02 -0.76117812777E+02 -0.13001840708E+03 0.15188324804E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.17250533200E+02 -0.37700051198E+02 -0.27633264354E+03 0.27942549032E+03 0.00000000000E+00 0. -1. 2 1 1 2 502 0 0.11241185340E+03 0.81335386120E+02 0.62594572251E+02 0.15221678716E+03 0.00000000000E+00 0. 1. 1 1 1 2 501 0 -0.75930786342E+02 0.32482477855E+02 -0.36837490536E+03 0.37751909433E+03 0.00000000000E+00 0. -1. 7 1 0.1436400E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 0.10196056713E+03 0.10196056713E+03 0.00000000000E+00 0. -1. 2 -1 0 0 503 0 0.00000000000E+00 0.00000000000E+00 -0.12817175353E+03 0.12817175353E+03 0.00000000000E+00 0. -1. 24 2 1 2 0 0 -0.25089597872E+02 0.15355294877E+02 -0.52367837400E+02 0.10131029773E+03 0.81585004939E+02 0. 0. -11 1 3 3 0 0 -0.29973574745E+02 -0.51425790837E+01 -0.68384868912E+02 0.74842177940E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.48839768734E+01 0.20497873961E+02 0.16017031512E+02 0.26468119795E+02 0.00000000000E+00 0. -1. 1 1 1 2 501 0 -0.42724633456E+02 -0.56638472062E+00 -0.18208506603E+02 0.46446364856E+02 0.00000000000E+00 0. -1. 21 1 1 2 503 502 0.67814231328E+02 -0.14788910157E+02 0.44365157605E+02 0.82375658077E+02 0.00000000000E+00 0. -1. 7 1 0.1436400E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 0.17024516624E+02 0.17024516624E+02 0.00000000000E+00 0. 1. 2 -1 0 0 503 0 0.00000000000E+00 0.00000000000E+00 -0.14009935504E+04 0.14009935504E+04 0.00000000000E+00 0. -1. 24 2 1 2 0 0 -0.68155630538E+02 0.28426620245E+02 -0.35406731981E+03 0.37042551135E+03 0.79988310344E+02 0. 0. -11 1 3 3 0 0 -0.46747594686E+02 -0.18573217095E+02 -0.11002912538E+03 0.12098227322E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.21408035852E+02 0.46999837339E+02 -0.24403819443E+03 0.24944323813E+03 0.00000000000E+00 0. -1. 1 1 1 2 501 0 0.42597355292E+02 0.59996774161E+02 -0.73467085209E+03 0.73834640143E+03 0.00000000000E+00 0. -1. 21 1 1 2 503 502 0.25558275246E+02 -0.88423394406E+02 -0.29523086189E+03 0.30924615425E+03 0.00000000000E+00 0. 1. 7 1 0.1436400E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 0.45803314715E+02 0.45803314715E+02 0.00000000000E+00 0. 1. 2 -1 0 0 503 0 0.00000000000E+00 0.00000000000E+00 -0.16319962968E+04 0.16319962968E+04 0.00000000000E+00 0. -1. 24 2 1 2 0 0 -0.14143440409E+01 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0.22079975265E+02 -0.92283839044E+02 0.10823297105E+03 0.00000000000E+00 0. -1. 7 1 0.1436400E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 0.67387042861E+02 0.67387042861E+02 0.00000000000E+00 0. -1. 2 -1 0 0 503 0 0.00000000000E+00 0.00000000000E+00 -0.35440220412E+03 0.35440220412E+03 0.00000000000E+00 0. -1. 24 2 1 2 0 0 -0.36782924884E+02 -0.11464048763E+02 -0.29760992957E+03 0.30826236448E+03 0.70495440977E+02 0. 0. -11 1 3 3 0 0 0.44579698945E+00 -0.26117424682E+02 -0.41430612245E+02 0.48977691227E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.37228721873E+02 0.14653375919E+02 -0.25617931732E+03 0.25928467325E+03 0.00000000000E+00 0. -1. 1 1 1 2 501 0 0.66508912789E+02 0.51654213217E+01 -0.20759392617E+02 0.69864650859E+02 0.00000000000E+00 0. -1. 21 1 1 2 503 502 -0.29725987905E+02 0.62986274413E+01 0.31354160928E+02 0.43662231644E+02 0.00000000000E+00 0. -1. 7 1 0.1436400E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 0.10208101305E+03 0.10208101305E+03 0.00000000000E+00 0. 1. 2 -1 0 0 503 0 0.00000000000E+00 0.00000000000E+00 -0.28228504581E+03 0.28228504581E+03 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.33280732607E+02 0.32594632505E+02 -0.22924640512E+03 0.25051495981E+03 0.89631543551E+02 0. 0. -11 1 3 3 0 0 0.33983033792E+02 -0.13535267990E+02 -0.34166683611E+02 0.50054094081E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.70230118499E+00 0.46129900495E+02 -0.19507972151E+03 0.20046086573E+03 0.00000000000E+00 0. -1. 1 1 1 2 501 0 -0.41500655851E+02 0.24752848180E+02 -0.11900571735E+02 0.49765766715E+02 0.00000000000E+00 0. -1. 21 1 1 2 503 502 0.82199232434E+01 -0.57347480685E+02 0.60942944090E+02 0.84085332332E+02 0.00000000000E+00 0. 1. 7 1 0.1436400E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 0.21166038492E+03 0.21166038492E+03 0.00000000000E+00 0. 1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.73570815511E+02 0.73570815511E+02 0.00000000000E+00 0. 1. 24 2 1 2 0 0 -0.92623972060E+02 0.22390589193E+02 0.36639116236E+02 0.12916856852E+03 0.79129991603E+02 0. 0. -11 1 3 3 0 0 -0.97284396395E+02 -0.17456543466E+00 0.41253043184E+02 0.10566975834E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.46604243343E+01 0.22565154627E+02 -0.46139269471E+01 0.23498810187E+02 0.00000000000E+00 0. -1. -2 1 1 2 0 503 0.53677941683E+02 -0.80241789584E+01 0.93964061820E+01 0.55081769401E+02 0.00000000000E+00 0. 1. 21 1 1 2 503 502 0.38946030378E+02 -0.14366410234E+02 0.92054046986E+02 0.10098086250E+03 0.00000000000E+00 0. 1. 7 1 0.1436400E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 -1 -1 0 0 0 502 0.00000000000E+00 0.00000000000E+00 0.55192142218E+03 0.55192142218E+03 0.00000000000E+00 0. 1. 2 -1 0 0 502 0 0.00000000000E+00 0.00000000000E+00 -0.16599278963E+03 0.16599278963E+03 0.00000000000E+00 0. -1. 24 2 1 2 0 0 -0.52300364109E+02 0.14809676510E+02 0.60226005692E+02 0.11428705245E+03 0.80496608575E+02 0. 0. -11 1 3 3 0 0 -0.38523770664E+02 -0.18707753761E+02 -0.13408631297E+01 0.42846923704E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.13776593446E+02 0.33517430271E+02 0.61566868822E+02 0.71440128748E+02 0.00000000000E+00 0. -1. 2 1 1 2 501 0 0.12079590779E+03 -0.32514585252E+02 -0.10734497036E+03 0.16483868555E+03 0.00000000000E+00 0. -1. -2 1 1 2 0 501 -0.68495543681E+02 0.17704908743E+02 0.43304759721E+03 0.43878847381E+03 0.00000000000E+00 0. 1. 7 1 0.1436400E+01 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 503 0 0.00000000000E+00 0.00000000000E+00 0.33261236559E+03 0.33261236559E+03 0.00000000000E+00 0. -1. 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 -0.86835017945E+02 0.86835017945E+02 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.85800718565E+02 -0.13641941028E+01 0.30202213667E+02 0.12155983330E+03 0.80628748162E+02 0. 0. -11 1 3 3 0 0 0.38778309605E+02 0.24755408391E+02 -0.17932244817E+02 0.49377656330E+02 0.00000000000E+00 0. 1. 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      pythia8-8.1.80.orig/examples/sps1aNarrowStopGluinoRPV.spc0000644000175000017500000013345612217346206021531 0ustar sunsun## Important note! ## This file has been modified by hand to give the gluino, the stop_1 ## and the su_L very narrow widths, such that it can be used to try out ## the R-hadron machinery. It is not a realistic SUSY scenario. ## ##****************************************************************** ## MadGraph/MadEvent * ##****************************************************************** ## * ## param_card corresponding the SPS point 1a (by SoftSusy 2.0.5) * ## * ##****************************************************************** ## Les Houches friendly file for the (MS)SM parameters of MadGraph * ## SM parameter set and decay widths produced by MSSMCalc * ##****************************************************************** ##*Please note the following IMPORTANT issues: * ## * ##0. REFRAIN from editing this file by hand! Some of the parame- * ## ters are not independent. Always use a calculator. * ## * ##1. alpha_S(MZ) has been used in the calculation of the parameters* ## This value is KEPT by madgraph when no pdf are used lpp(i)=0, * ## but, for consistency, it will be reset by madgraph to the * ## value expected IF the pdfs for collisions with hadrons are * ## used. * ## * ##2. Values of the charm and bottom kinematic (pole) masses are * ## those used in the matrix elements and phase space UNLESS they * ## are set to ZERO from the start in the model (particles.dat) * ## This happens, for example, when using 5-flavor QCD where * ## charm and bottom are treated as partons in the initial state * ## and a zero mass might be hardwired in the model definition. * ## * ## The SUSY decays have calculated using SDECAY 1.1a * ## * ##****************************************************************** # BLOCK DCINFO # Decay Program information 1 SDECAY # decay calculator 2 1.1a # version number # BLOCK SPINFO # Spectrum calculator information 1 SOFTSUSY # spectrum calculator 2 2.0.5 # version number # BLOCK MODSEL # Model selection 1 1 sugra # BLOCK SMINPUTS # Standard Model inputs 1 1.27934000E+02 # alpha_em^-1(M_Z)^MSbar 2 1.16637000E-05 # G_F [GeV^-2] 3 1.18000000E-01 # alpha_S(M_Z)^MSbar 4 9.11876000E+01 # M_Z pole mass 5 4.25000000E+00 # mb(mb)^MSbar 6 1.75000000E+02 # mt pole mass 7 1.77700000E+00 # mtau pole mass # BLOCK MINPAR # Input parameters - minimal models 1 1.00000000E+02 # m0 2 2.50000000E+02 # m12 3 1.00000000E+01 # tanb 4 1.00000000E+00 # sign(mu) 5 -1.00000000E+02 # A0 # BLOCK MASS # Mass Spectrum # PDG code mass particle 5 4.88991651E+00 # b-quark pole mass calculated from mb(mb)_Msbar 6 1.75000000E+02 # mt pole mass (not read by ME) 24 7.98290131E+01 # W+ 25 1.10899057E+02 # h 35 3.99960116E+02 # H 36 3.99583917E+02 # A 37 4.07879012E+02 # H+ 1000001 5.68441109E+02 # ~d_L 2000001 5.45228462E+02 # ~d_R 1000002 5.61119014E+02 # ~u_L 2000002 5.49259265E+02 # ~u_R 1000003 5.68441109E+02 # ~s_L 2000003 5.45228462E+02 # ~s_R 1000004 5.61119014E+02 # ~c_L 2000004 5.49259265E+02 # ~c_R 1000005 5.13065179E+02 # ~b_1 2000005 5.43726676E+02 # ~b_2 1000006 3.99668493E+02 # ~t_1 2000006 5.85785818E+02 # ~t_2 1000011 2.02915690E+02 # ~e_L 2000011 1.44102799E+02 # ~e_R 1000012 1.85258326E+02 # ~nu_eL 1000013 2.02915690E+02 # ~mu_L 2000013 1.44102799E+02 # ~mu_R 1000014 1.85258326E+02 # ~nu_muL 1000015 1.34490864E+02 # ~tau_1 2000015 2.06867805E+02 # ~tau_2 1000016 1.84708464E+02 # ~nu_tauL 1000021 6.07713704E+02 # ~g 1000022 9.66880686E+01 # ~chi_10 1000023 1.81088157E+02 # ~chi_20 1000025 -3.63756027E+02 # ~chi_30 1000035 3.81729382E+02 # ~chi_40 1000024 1.81696474E+02 # ~chi_1+ 1000037 3.79939320E+02 # ~chi_2+ # BLOCK NMIX # Neutralino Mixing Matrix 1 1 9.86364430E-01 # N_11 1 2 -5.31103553E-02 # N_12 1 3 1.46433995E-01 # N_13 1 4 -5.31186117E-02 # N_14 2 1 9.93505358E-02 # N_21 2 2 9.44949299E-01 # N_22 2 3 -2.69846720E-01 # N_23 2 4 1.56150698E-01 # N_24 3 1 -6.03388002E-02 # N_31 3 2 8.77004854E-02 # N_32 3 3 6.95877493E-01 # N_33 3 4 7.10226984E-01 # N_34 4 1 -1.16507132E-01 # N_41 4 2 3.10739017E-01 # N_42 4 3 6.49225960E-01 # N_43 4 4 -6.84377823E-01 # N_44 # BLOCK UMIX # Chargino Mixing Matrix U 1 1 9.16834859E-01 # U_11 1 2 -3.99266629E-01 # U_12 2 1 3.99266629E-01 # U_21 2 2 9.16834859E-01 # U_22 # BLOCK VMIX # Chargino Mixing Matrix V 1 1 9.72557835E-01 # V_11 1 2 -2.32661249E-01 # V_12 2 1 2.32661249E-01 # V_21 2 2 9.72557835E-01 # V_22 # BLOCK STOPMIX # Stop Mixing Matrix 1 1 5.53644960E-01 # O_{11} 1 2 8.32752820E-01 # O_{12} 2 1 8.32752820E-01 # O_{21} 2 2 -5.53644960E-01 # O_{22} # BLOCK SBOTMIX # Sbottom Mixing Matrix 1 1 9.38737896E-01 # O_{11} 1 2 3.44631925E-01 # O_{12} 2 1 -3.44631925E-01 # O_{21} 2 2 9.38737896E-01 # O_{22} # BLOCK STAUMIX # Stau Mixing Matrix 1 1 2.82487190E-01 # O_{11} 1 2 9.59271071E-01 # O_{12} 2 1 9.59271071E-01 # O_{21} 2 2 -2.82487190E-01 # O_{22} # BLOCK ALPHA # Higgs mixing -1.13825210E-01 # Mixing angle in the neutral Higgs boson sector # BLOCK HMIX Q= 4.67034192E+02 # DRbar Higgs Parameters 1 3.57680977E+02 # mu(Q)MSSM DRbar 2 9.74862403E+00 # tan beta(Q)MSSM DRba 3 2.44894549E+02 # higgs vev(Q)MSSM DRb 4 1.66439065E+05 # mA^2(Q)MSSM DRbar # BLOCK GAUGE Q= 4.67034192E+02 # The gauge couplings 3 1.10178679E+00 # g3(Q) MSbar # BLOCK AU Q= 4.67034192E+02 # The trilinear couplings 1 1 0.00000000E+00 # A_u(Q) DRbar 2 2 0.00000000E+00 # A_c(Q) DRbar 3 3 -4.98129778E+02 # A_t(Q) DRbar # BLOCK AD Q= 4.67034192E+02 # The trilinear couplings 1 1 0.00000000E+00 # A_d(Q) DRbar 2 2 0.00000000E+00 # A_s(Q) DRbar 3 3 -7.97274397E+02 # A_b(Q) DRbar # BLOCK AE Q= 4.67034192E+02 # The trilinear couplings 1 1 0.00000000E+00 # A_e(Q) DRbar 2 2 0.00000000E+00 # A_mu(Q) DRbar 3 3 -2.51776873E+02 # A_tau(Q) DRbar # BLOCK YU Q= 4.67034192E+02 # The Yukawa couplings 3 3 8.92844550E-01 # y_t(Q) DRbar # BLOCK YD Q= 4.67034192E+02 # The Yukawa couplings 3 3 1.38840206E-01 # y_b(Q) DRbar # BLOCK YE Q= 4.67034192E+02 # The Yukawa couplings 3 3 1.00890810E-01 # y_tau(Q) DRbar # BLOCK MSOFT Q= 4.67034192E+02 # The soft SUSY breaking masses at the scale Q 1 1.01396534E+02 # M_1(Q) 2 1.91504241E+02 # M_2(Q) 3 5.88263031E+02 # M_3(Q) 21 3.23374943E+04 # mH1^2(Q) 22 -1.28800134E+05 # mH2^2(Q) 31 1.95334764E+02 # meL(Q) 32 1.95334764E+02 # mmuL(Q) 33 1.94495956E+02 # mtauL(Q) 34 1.36494061E+02 # meR(Q) 35 1.36494061E+02 # mmuR(Q) 36 1.34043428E+02 # mtauR(Q) 41 5.47573466E+02 # mqL1(Q) 42 5.47573466E+02 # mqL2(Q) 43 4.98763839E+02 # mqL3(Q) 44 5.29511195E+02 # muR(Q) 45 5.29511195E+02 # mcR(Q) 46 4.23245877E+02 # mtR(Q) 47 5.23148807E+02 # mdR(Q) 48 5.23148807E+02 # msR(Q) 49 5.19867261E+02 # mbR(Q) # # # # ================= # |The decay table| # ================= # # - The multi-body decays for the inos, stops and sbottoms are included. # # PDG Width DECAY 25 1.98610799E-03 # h decays # BR NDA ID1 ID2 1.45642955E-01 2 15 -15 # BR(H1 -> tau- tau+) 8.19070713E-01 2 5 -5 # BR(H1 -> b bb) 3.36338173E-02 2 24 -24 # BR(H1 -> W+ W-) 1.65251528E-03 2 23 23 # BR(H1 -> Z Z) # # PDG Width DECAY 35 5.74801389E-01 # H decays # BR NDA ID1 ID2 1.39072676E-01 2 15 -15 # BR(H -> tau- tau+) 4.84110879E-02 2 6 -6 # BR(H -> t tb) 7.89500067E-01 2 5 -5 # BR(H -> b bb) 3.87681171E-03 2 24 -24 # BR(H -> W+ W-) 1.80454752E-03 2 23 23 # BR(H -> Z Z) 0.00000000E+00 2 24 -37 # BR(H -> W+ H-) 0.00000000E+00 2 -24 37 # BR(H -> W- H+) 0.00000000E+00 2 37 -37 # BR(H -> H+ H-) 1.73348101E-02 2 25 25 # BR(H -> h h) 0.00000000E+00 2 36 36 # BR(H -> A A) # # PDG Width DECAY 36 6.32178488E-01 # A decays # BR NDA ID1 ID2 1.26659725E-01 2 15 -15 # BR(A -> tau- tau+) 1.51081526E-01 2 6 -6 # BR(A -> t tb) 7.19406137E-01 2 5 -5 # BR(A -> b bb) 2.85261228E-03 2 23 25 # BR(A -> Z h) 0.00000000E+00 2 23 35 # BR(A -> Z H) 0.00000000E+00 2 24 -37 # BR(A -> W+ H-) 0.00000000E+00 2 -24 37 # BR(A -> W- H+) # # PDG Width DECAY 37 5.46962813E-01 # H+ decays # BR NDA ID1 ID2 1.49435135E-01 2 -15 16 # BR(H+ -> tau+ nu_tau) 8.46811711E-01 2 6 -5 # BR(H+ -> t bb) 3.75315387E-03 2 24 25 # BR(H+ -> W+ h) 0.00000000E+00 2 24 35 # BR(H+ -> W+ H) 0.00000000E+00 2 24 36 # BR(H+ -> W+ A) # # PDG Width DECAY 1000021 0.01E+00 # gluino decays # BR NDA ID1 ID2 ID3 0.50000000E+00 3 2 3 5 # BR(~g -> u s b) 0.50000000E+00 3 -2 -3 -5 # BR(~g -> ubar sbar bbar) # # PDG Width DECAY 1000006 0.01E+00 # stop1 decays # BR NDA ID1 ID2 1.92947616E-01 2 1000022 6 # BR(~t_1 -> ~chi_10 t ) 1.17469211E-01 2 1000023 6 # BR(~t_1 -> ~chi_20 t ) 0.00000000E+00 2 1000025 6 # BR(~t_1 -> ~chi_30 t ) 0.00000000E+00 2 1000035 6 # BR(~t_1 -> ~chi_40 t ) 6.75747693E-01 2 1000024 5 # BR(~t_1 -> ~chi_1+ b ) 1.38354802E-02 2 1000037 5 # BR(~t_1 -> ~chi_2+ b ) 0.00000000E+00 2 1000021 6 # BR(~t_1 -> ~g t ) 0.00000000E+00 2 1000005 37 # BR(~t_1 -> ~b_1 H+) 0.00000000E+00 2 2000005 37 # BR(~t_1 -> ~b_2 H+) 0.00000000E+00 2 1000005 24 # BR(~t_1 -> ~b_1 W+) 0.00000000E+00 2 2000005 24 # BR(~t_1 -> ~b_2 W+) # # PDG Width DECAY 2000006 7.37313275E+00 # stop2 decays # BR NDA ID1 ID2 2.96825635E-02 2 1000022 6 # BR(~t_2 -> ~chi_10 t ) 8.68035358E-02 2 1000023 6 # BR(~t_2 -> ~chi_20 t ) 4.18408351E-02 2 1000025 6 # BR(~t_2 -> ~chi_30 t ) 1.93281647E-01 2 1000035 6 # BR(~t_2 -> ~chi_40 t ) 2.19632356E-01 2 1000024 5 # BR(~t_2 -> ~chi_1+ b ) 2.02206148E-01 2 1000037 5 # BR(~t_2 -> ~chi_2+ b ) 0.00000000E+00 2 1000021 6 # BR(~t_2 -> ~g t ) 3.66397706E-02 2 1000006 25 # BR(~t_2 -> ~t_1 h ) 0.00000000E+00 2 1000006 35 # BR(~t_2 -> ~t_1 H ) 0.00000000E+00 2 1000006 36 # BR(~t_2 -> ~t_1 A ) 0.00000000E+00 2 1000005 37 # BR(~t_2 -> ~b_1 H+) 0.00000000E+00 2 2000005 37 # BR(~t_2 -> ~b_2 H+) 1.89913144E-01 2 1000006 23 # BR(~t_2 -> ~t_1 Z ) 0.00000000E+00 2 1000005 24 # BR(~t_2 -> ~b_1 W+) 0.00000000E+00 2 2000005 24 # BR(~t_2 -> ~b_2 W+) # # PDG Width DECAY 1000005 3.73627601E+00 # sbottom1 decays # BR NDA ID1 ID2 4.43307074E-02 2 1000022 5 # BR(~b_1 -> ~chi_10 b ) 3.56319904E-01 2 1000023 5 # BR(~b_1 -> ~chi_20 b ) 5.16083795E-03 2 1000025 5 # BR(~b_1 -> ~chi_30 b ) 1.04105080E-02 2 1000035 5 # BR(~b_1 -> ~chi_40 b ) 4.45830064E-01 2 -1000024 6 # BR(~b_1 -> ~chi_1- t ) 0.00000000E+00 2 -1000037 6 # BR(~b_1 -> ~chi_2- t ) 0.00000000E+00 2 1000021 5 # BR(~b_1 -> ~g b ) 0.00000000E+00 2 1000006 -37 # BR(~b_1 -> ~t_1 H-) 0.00000000E+00 2 2000006 -37 # BR(~b_1 -> ~t_2 H-) 1.37947979E-01 2 1000006 -24 # BR(~b_1 -> ~t_1 W-) 0.00000000E+00 2 2000006 -24 # BR(~b_1 -> ~t_2 W-) # # PDG Width DECAY 2000005 8.01566294E-01 # sbottom2 decays # BR NDA ID1 ID2 2.86200590E-01 2 1000022 5 # BR(~b_2 -> ~chi_10 b ) 1.40315912E-01 2 1000023 5 # BR(~b_2 -> ~chi_20 b ) 5.32635592E-02 2 1000025 5 # BR(~b_2 -> ~chi_30 b ) 7.48748121E-02 2 1000035 5 # BR(~b_2 -> ~chi_40 b ) 1.79734294E-01 2 -1000024 6 # BR(~b_2 -> ~chi_1- t ) 0.00000000E+00 2 -1000037 6 # BR(~b_2 -> ~chi_2- t ) 0.00000000E+00 2 1000021 5 # BR(~b_2 -> ~g b ) 0.00000000E+00 2 1000005 25 # BR(~b_2 -> ~b_1 h ) 0.00000000E+00 2 1000005 35 # BR(~b_2 -> ~b_1 H ) 0.00000000E+00 2 1000005 36 # BR(~b_2 -> ~b_1 A ) 0.00000000E+00 2 1000006 -37 # BR(~b_2 -> ~t_1 H-) 0.00000000E+00 2 2000006 -37 # BR(~b_2 -> ~t_2 H-) 0.00000000E+00 2 1000005 23 # BR(~b_2 -> ~b_1 Z ) 2.65610832E-01 2 1000006 -24 # BR(~b_2 -> ~t_1 W-) 0.00000000E+00 2 2000006 -24 # BR(~b_2 -> ~t_2 W-) # # PDG Width DECAY 1000002 0.01E+00 # sup_L decays # BR NDA ID1 ID2 6.65240987E-03 2 1000022 2 # BR(~u_L -> ~chi_10 u) 3.19051458E-01 2 1000023 2 # BR(~u_L -> ~chi_20 u) 8.44929059E-04 2 1000025 2 # BR(~u_L -> ~chi_30 u) 1.03485173E-02 2 1000035 2 # BR(~u_L -> ~chi_40 u) 6.49499518E-01 2 1000024 1 # BR(~u_L -> ~chi_1+ d) 1.36031676E-02 2 1000037 1 # BR(~u_L -> ~chi_2+ d) 0.00000000E+00 2 1000021 2 # BR(~u_L -> ~g u) # # PDG Width DECAY 2000002 1.15297292E+00 # sup_R decays # BR NDA ID1 ID2 9.86377420E-01 2 1000022 2 # BR(~u_R -> ~chi_10 u) 8.46640647E-03 2 1000023 2 # BR(~u_R -> ~chi_20 u) 1.23894695E-03 2 1000025 2 # BR(~u_R -> ~chi_30 u) 3.91722611E-03 2 1000035 2 # BR(~u_R -> ~chi_40 u) 0.00000000E+00 2 1000024 1 # BR(~u_R -> ~chi_1+ d) 0.00000000E+00 2 1000037 1 # BR(~u_R -> ~chi_2+ d) 0.00000000E+00 2 1000021 2 # BR(~u_R -> ~g u) # # PDG Width DECAY 1000001 5.31278772E+00 # sdown_L decays # BR NDA ID1 ID2 2.32317969E-02 2 1000022 1 # BR(~d_L -> ~chi_10 d) 3.10235077E-01 2 1000023 1 # BR(~d_L -> ~chi_20 d) 1.52334771E-03 2 1000025 1 # BR(~d_L -> ~chi_30 d) 1.48849798E-02 2 1000035 1 # BR(~d_L -> ~chi_40 d) 6.06452481E-01 2 -1000024 2 # BR(~d_L -> ~chi_1- u) 4.36723179E-02 2 -1000037 2 # BR(~d_L -> ~chi_2- u) 0.00000000E+00 2 1000021 1 # BR(~d_L -> ~g d) # # PDG Width DECAY 2000001 2.85812308E-01 # sdown_R decays # BR NDA ID1 ID2 9.86529614E-01 2 1000022 1 # BR(~d_R -> ~chi_10 d) 8.44510350E-03 2 1000023 1 # BR(~d_R -> ~chi_20 d) 1.21172119E-03 2 1000025 1 # BR(~d_R -> ~chi_30 d) 3.81356102E-03 2 1000035 1 # BR(~d_R -> ~chi_40 d) 0.00000000E+00 2 -1000024 2 # BR(~d_R -> ~chi_1- u) 0.00000000E+00 2 -1000037 2 # BR(~d_R -> ~chi_2- u) 0.00000000E+00 2 1000021 1 # BR(~d_R -> ~g d) # # PDG Width DECAY 1000004 5.47719539E+00 # scharm_L decays # BR NDA ID1 ID2 6.65240987E-03 2 1000022 4 # BR(~c_L -> ~chi_10 c) 3.19051458E-01 2 1000023 4 # BR(~c_L -> ~chi_20 c) 8.44929059E-04 2 1000025 4 # BR(~c_L -> ~chi_30 c) 1.03485173E-02 2 1000035 4 # BR(~c_L -> ~chi_40 c) 6.49499518E-01 2 1000024 3 # BR(~c_L -> ~chi_1+ s) 1.36031676E-02 2 1000037 3 # BR(~c_L -> ~chi_2+ s) 0.00000000E+00 2 1000021 4 # BR(~c_L -> ~g c) # # PDG Width DECAY 2000004 1.15297292E+00 # scharm_R decays # BR NDA ID1 ID2 9.86377420E-01 2 1000022 4 # BR(~c_R -> ~chi_10 c) 8.46640647E-03 2 1000023 4 # BR(~c_R -> ~chi_20 c) 1.23894695E-03 2 1000025 4 # BR(~c_R -> ~chi_30 c) 3.91722611E-03 2 1000035 4 # BR(~c_R -> ~chi_40 c) 0.00000000E+00 2 1000024 3 # BR(~c_R -> ~chi_1+ s) 0.00000000E+00 2 1000037 3 # BR(~c_R -> ~chi_2+ s) 0.00000000E+00 2 1000021 4 # BR(~c_R -> ~g c) # # PDG Width DECAY 1000003 5.31278772E+00 # sstrange_L decays # BR NDA ID1 ID2 2.32317969E-02 2 1000022 3 # BR(~s_L -> ~chi_10 s) 3.10235077E-01 2 1000023 3 # BR(~s_L -> ~chi_20 s) 1.52334771E-03 2 1000025 3 # BR(~s_L -> ~chi_30 s) 1.48849798E-02 2 1000035 3 # BR(~s_L -> ~chi_40 s) 6.06452481E-01 2 -1000024 4 # BR(~s_L -> ~chi_1- c) 4.36723179E-02 2 -1000037 4 # BR(~s_L -> ~chi_2- c) 0.00000000E+00 2 1000021 3 # BR(~s_L -> ~g s) # # PDG Width DECAY 2000003 2.85812308E-01 # sstrange_R decays # BR NDA ID1 ID2 9.86529614E-01 2 1000022 3 # BR(~s_R -> ~chi_10 s) 8.44510350E-03 2 1000023 3 # BR(~s_R -> ~chi_20 s) 1.21172119E-03 2 1000025 3 # BR(~s_R -> ~chi_30 s) 3.81356102E-03 2 1000035 3 # BR(~s_R -> ~chi_40 s) 0.00000000E+00 2 -1000024 4 # BR(~s_R -> ~chi_1- c) 0.00000000E+00 2 -1000037 4 # BR(~s_R -> ~chi_2- c) 0.00000000E+00 2 1000021 3 # BR(~s_R -> ~g s) # # PDG Width DECAY 1000011 2.13682161E-01 # selectron_L decays # BR NDA ID1 ID2 5.73155386E-01 2 1000022 11 # BR(~e_L -> ~chi_10 e-) 1.64522579E-01 2 1000023 11 # BR(~e_L -> ~chi_20 e-) 0.00000000E+00 2 1000025 11 # BR(~e_L -> ~chi_30 e-) 0.00000000E+00 2 1000035 11 # BR(~e_L -> ~chi_40 e-) 2.62322035E-01 2 -1000024 12 # BR(~e_L -> ~chi_1- nu_e) 0.00000000E+00 2 -1000037 12 # BR(~e_L -> ~chi_2- nu_e) # # PDG Width DECAY 2000011 2.16121626E-01 # selectron_R decays # BR NDA ID1 ID2 1.00000000E+00 2 1000022 11 # BR(~e_R -> ~chi_10 e-) 0.00000000E+00 2 1000023 11 # BR(~e_R -> ~chi_20 e-) 0.00000000E+00 2 1000025 11 # BR(~e_R -> ~chi_30 e-) 0.00000000E+00 2 1000035 11 # BR(~e_R -> ~chi_40 e-) 0.00000000E+00 2 -1000024 12 # BR(~e_R -> ~chi_1- nu_e) 0.00000000E+00 2 -1000037 12 # BR(~e_R -> ~chi_2- nu_e) # # PDG Width DECAY 1000013 2.13682161E-01 # smuon_L decays # BR NDA ID1 ID2 5.73155386E-01 2 1000022 13 # BR(~mu_L -> ~chi_10 mu-) 1.64522579E-01 2 1000023 13 # BR(~mu_L -> ~chi_20 mu-) 0.00000000E+00 2 1000025 13 # BR(~mu_L -> ~chi_30 mu-) 0.00000000E+00 2 1000035 13 # BR(~mu_L -> ~chi_40 mu-) 2.62322035E-01 2 -1000024 14 # BR(~mu_L -> ~chi_1- nu_mu) 0.00000000E+00 2 -1000037 14 # BR(~mu_L -> ~chi_2- nu_mu) # # PDG Width DECAY 2000013 2.16121626E-01 # smuon_R decays # BR NDA ID1 ID2 1.00000000E+00 2 1000022 13 # BR(~mu_R -> ~chi_10 mu-) 0.00000000E+00 2 1000023 13 # BR(~mu_R -> ~chi_20 mu-) 0.00000000E+00 2 1000025 13 # BR(~mu_R -> ~chi_30 mu-) 0.00000000E+00 2 1000035 13 # BR(~mu_R -> ~chi_40 mu-) 0.00000000E+00 2 -1000024 14 # BR(~mu_R -> ~chi_1- nu_mu) 0.00000000E+00 2 -1000037 14 # BR(~mu_R -> ~chi_2- nu_mu) # # PDG Width DECAY 1000015 1.48327268E-01 # stau_1 decays # BR NDA ID1 ID2 1.00000000E+00 2 1000022 15 # BR(~tau_1 -> ~chi_10 tau-) 0.00000000E+00 2 1000023 15 # BR(~tau_1 -> ~chi_20 tau-) 0.00000000E+00 2 1000025 15 # BR(~tau_1 -> ~chi_30 tau-) 0.00000000E+00 2 1000035 15 # BR(~tau_1 -> ~chi_40 tau-) 0.00000000E+00 2 -1000024 16 # BR(~tau_1 -> ~chi_1- nu_tau) 0.00000000E+00 2 -1000037 16 # BR(~tau_1 -> ~chi_2- nu_tau) 0.00000000E+00 2 1000016 -37 # BR(~tau_1 -> ~nu_tauL H-) 0.00000000E+00 2 1000016 -24 # BR(~tau_1 -> ~nu_tauL W-) # # PDG Width DECAY 2000015 2.69906096E-01 # stau_2 decays # BR NDA ID1 ID2 5.96653046E-01 2 1000022 15 # BR(~tau_2 -> ~chi_10 tau-) 1.54536760E-01 2 1000023 15 # BR(~tau_2 -> ~chi_20 tau-) 0.00000000E+00 2 1000025 15 # BR(~tau_2 -> ~chi_30 tau-) 0.00000000E+00 2 1000035 15 # BR(~tau_2 -> ~chi_40 tau-) 2.48810195E-01 2 -1000024 16 # BR(~tau_2 -> ~chi_1- nu_tau) 0.00000000E+00 2 -1000037 16 # BR(~tau_2 -> ~chi_2- nu_tau) 0.00000000E+00 2 1000016 -37 # BR(~tau_2 -> ~nu_tauL H-) 0.00000000E+00 2 1000016 -24 # BR(~tau_2 -> ~nu_tauL W-) 0.00000000E+00 2 1000015 25 # BR(~tau_2 -> ~tau_1 h) 0.00000000E+00 2 1000015 35 # BR(~tau_2 -> ~tau_1 H) 0.00000000E+00 2 1000015 36 # BR(~tau_2 -> ~tau_1 A) 0.00000000E+00 2 1000015 23 # BR(~tau_2 -> ~tau_1 Z) # # PDG Width DECAY 1000012 1.49881634E-01 # snu_eL decays # BR NDA ID1 ID2 9.77700764E-01 2 1000022 12 # BR(~nu_eL -> ~chi_10 nu_e) 8.11554922E-03 2 1000023 12 # BR(~nu_eL -> ~chi_20 nu_e) 0.00000000E+00 2 1000025 12 # BR(~nu_eL -> ~chi_30 nu_e) 0.00000000E+00 2 1000035 12 # BR(~nu_eL -> ~chi_40 nu_e) 1.41836867E-02 2 1000024 11 # BR(~nu_eL -> ~chi_1+ e-) 0.00000000E+00 2 1000037 11 # BR(~nu_eL -> ~chi_2+ e-) # # PDG Width DECAY 1000014 1.49881634E-01 # snu_muL decays # BR NDA ID1 ID2 9.77700764E-01 2 1000022 14 # BR(~nu_muL -> ~chi_10 nu_mu) 8.11554922E-03 2 1000023 14 # BR(~nu_muL -> ~chi_20 nu_mu) 0.00000000E+00 2 1000025 14 # BR(~nu_muL -> ~chi_30 nu_mu) 0.00000000E+00 2 1000035 14 # BR(~nu_muL -> ~chi_40 nu_mu) 1.41836867E-02 2 1000024 13 # BR(~nu_muL -> ~chi_1+ mu-) 0.00000000E+00 2 1000037 13 # BR(~nu_muL -> ~chi_2+ mu-) # # PDG Width DECAY 1000016 1.47518977E-01 # snu_tauL decays # BR NDA ID1 ID2 9.85994529E-01 2 1000022 16 # BR(~nu_tauL -> ~chi_10 nu_tau) 6.25129612E-03 2 1000023 16 # BR(~nu_tauL -> ~chi_20 nu_tau) 0.00000000E+00 2 1000025 16 # BR(~nu_tauL -> ~chi_30 nu_tau) 0.00000000E+00 2 1000035 16 # BR(~nu_tauL -> ~chi_40 nu_tau) 7.75417479E-03 2 1000024 15 # BR(~nu_tauL -> ~chi_1+ tau-) 0.00000000E+00 2 1000037 15 # BR(~nu_tauL -> ~chi_2+ tau-) 0.00000000E+00 2 -1000015 -37 # BR(~nu_tauL -> ~tau_1+ H-) 0.00000000E+00 2 -2000015 -37 # BR(~nu_tauL -> ~tau_2+ H-) 0.00000000E+00 2 -1000015 -24 # BR(~nu_tauL -> ~tau_1+ W-) 0.00000000E+00 2 -2000015 -24 # BR(~nu_tauL -> ~tau_2+ W-) # # PDG Width DECAY 1000024 1.70414503E-02 # chargino1+ decays # BR NDA ID1 ID2 0.00000000E+00 2 1000002 -1 # BR(~chi_1+ -> ~u_L db) 0.00000000E+00 2 2000002 -1 # BR(~chi_1+ -> ~u_R db) 0.00000000E+00 2 -1000001 2 # BR(~chi_1+ -> ~d_L* u ) 0.00000000E+00 2 -2000001 2 # BR(~chi_1+ -> ~d_R* u ) 0.00000000E+00 2 1000004 -3 # BR(~chi_1+ -> ~c_L sb) 0.00000000E+00 2 2000004 -3 # BR(~chi_1+ -> ~c_R sb) 0.00000000E+00 2 -1000003 4 # BR(~chi_1+ -> ~s_L* c ) 0.00000000E+00 2 -2000003 4 # BR(~chi_1+ -> ~s_R* c ) 0.00000000E+00 2 1000006 -5 # BR(~chi_1+ -> ~t_1 bb) 0.00000000E+00 2 2000006 -5 # BR(~chi_1+ -> ~t_2 bb) 0.00000000E+00 2 -1000005 6 # BR(~chi_1+ -> ~b_1* t ) 0.00000000E+00 2 -2000005 6 # BR(~chi_1+ -> ~b_2* t ) 0.00000000E+00 2 1000012 -11 # BR(~chi_1+ -> ~nu_eL e+ ) 0.00000000E+00 2 1000014 -13 # BR(~chi_1+ -> ~nu_muL mu+ ) 0.00000000E+00 2 1000016 -15 # BR(~chi_1+ -> ~nu_tau1 tau+) 0.00000000E+00 2 -1000011 12 # BR(~chi_1+ -> ~e_L+ nu_e) 0.00000000E+00 2 -2000011 12 # BR(~chi_1+ -> ~e_R+ nu_e) 0.00000000E+00 2 -1000013 14 # BR(~chi_1+ -> ~mu_L+ nu_mu) 0.00000000E+00 2 -2000013 14 # BR(~chi_1+ -> ~mu_R+ nu_mu) 9.25161117E-01 2 -1000015 16 # BR(~chi_1+ -> ~tau_1+ nu_tau) 0.00000000E+00 2 -2000015 16 # BR(~chi_1+ -> ~tau_2+ nu_tau) 7.48388828E-02 2 1000022 24 # BR(~chi_1+ -> ~chi_10 W+) 0.00000000E+00 2 1000023 24 # BR(~chi_1+ -> ~chi_20 W+) 0.00000000E+00 2 1000025 24 # BR(~chi_1+ -> ~chi_30 W+) 0.00000000E+00 2 1000035 24 # BR(~chi_1+ -> ~chi_40 W+) 0.00000000E+00 2 1000022 37 # BR(~chi_1+ -> ~chi_10 H+) 0.00000000E+00 2 1000023 37 # BR(~chi_1+ -> ~chi_20 H+) 0.00000000E+00 2 1000025 37 # BR(~chi_1+ -> ~chi_30 H+) 0.00000000E+00 2 1000035 37 # BR(~chi_1+ -> ~chi_40 H+) # # PDG Width DECAY 1000037 2.48689510E+00 # chargino2+ decays # BR NDA ID1 ID2 0.00000000E+00 2 1000002 -1 # BR(~chi_2+ -> ~u_L db) 0.00000000E+00 2 2000002 -1 # BR(~chi_2+ -> ~u_R db) 0.00000000E+00 2 -1000001 2 # BR(~chi_2+ -> ~d_L* u ) 0.00000000E+00 2 -2000001 2 # BR(~chi_2+ -> ~d_R* u ) 0.00000000E+00 2 1000004 -3 # BR(~chi_2+ -> ~c_L sb) 0.00000000E+00 2 2000004 -3 # BR(~chi_2+ -> ~c_R sb) 0.00000000E+00 2 -1000003 4 # BR(~chi_2+ -> ~s_L* c ) 0.00000000E+00 2 -2000003 4 # BR(~chi_2+ -> ~s_R* c ) 0.00000000E+00 2 1000006 -5 # BR(~chi_2+ -> ~t_1 bb) 0.00000000E+00 2 2000006 -5 # BR(~chi_2+ -> ~t_2 bb) 0.00000000E+00 2 -1000005 6 # BR(~chi_2+ -> ~b_1* t ) 0.00000000E+00 2 -2000005 6 # BR(~chi_2+ -> ~b_2* t ) 2.00968837E-02 2 1000012 -11 # BR(~chi_2+ -> ~nu_eL e+ ) 2.00968837E-02 2 1000014 -13 # BR(~chi_2+ -> ~nu_muL mu+ ) 2.74507395E-02 2 1000016 -15 # BR(~chi_2+ -> ~nu_tau1 tau+) 5.20406111E-02 2 -1000011 12 # BR(~chi_2+ -> ~e_L+ nu_e) 0.00000000E+00 2 -2000011 12 # BR(~chi_2+ -> ~e_R+ nu_e) 5.20406111E-02 2 -1000013 14 # BR(~chi_2+ -> ~mu_L+ nu_mu) 0.00000000E+00 2 -2000013 14 # BR(~chi_2+ -> ~mu_R+ nu_mu) 2.82859898E-04 2 -1000015 16 # BR(~chi_2+ -> ~tau_1+ nu_tau) 5.66729336E-02 2 -2000015 16 # BR(~chi_2+ -> ~tau_2+ nu_tau) 2.31513269E-01 2 1000024 23 # BR(~chi_2+ -> ~chi_1+ Z ) 6.76715120E-02 2 1000022 24 # BR(~chi_2+ -> ~chi_10 W+) 2.93654849E-01 2 1000023 24 # BR(~chi_2+ -> ~chi_20 W+) 0.00000000E+00 2 1000025 24 # BR(~chi_2+ -> ~chi_30 W+) 0.00000000E+00 2 1000035 24 # BR(~chi_2+ -> ~chi_40 W+) 1.78478848E-01 2 1000024 25 # BR(~chi_2+ -> ~chi_1+ h ) 0.00000000E+00 2 1000024 35 # BR(~chi_2+ -> ~chi_1+ H ) 0.00000000E+00 2 1000024 36 # BR(~chi_2+ -> ~chi_1+ A ) 0.00000000E+00 2 1000022 37 # BR(~chi_2+ -> ~chi_10 H+) 0.00000000E+00 2 1000023 37 # BR(~chi_2+ -> ~chi_20 H+) 0.00000000E+00 2 1000025 37 # BR(~chi_2+ -> ~chi_30 H+) 0.00000000E+00 2 1000035 37 # BR(~chi_2+ -> ~chi_40 H+) # # PDG Width DECAY 1000022 0.00000000E+00 # neutralino1 decays # # PDG Width DECAY 1000023 2.07770048E-02 # neutralino2 decays # BR NDA ID1 ID2 0.00000000E+00 2 1000022 23 # BR(~chi_20 -> ~chi_10 Z ) 0.00000000E+00 2 1000024 -24 # BR(~chi_20 -> ~chi_1+ W-) 0.00000000E+00 2 -1000024 24 # BR(~chi_20 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_20 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_20 -> ~chi_2- W+) 0.00000000E+00 2 1000022 25 # BR(~chi_20 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_20 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_20 -> ~chi_10 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_20 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_20 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_20 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_20 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_20 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_20 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_20 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_20 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_20 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_20 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_20 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_20 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_20 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_20 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_20 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_20 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_20 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_20 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_20 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_20 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_20 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_20 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_20 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_20 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_20 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_20 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_20 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_20 -> ~b_2* b ) 0.00000000E+00 2 1000011 -11 # BR(~chi_20 -> ~e_L- e+) 0.00000000E+00 2 -1000011 11 # BR(~chi_20 -> ~e_L+ e-) 2.95071995E-02 2 2000011 -11 # BR(~chi_20 -> ~e_R- e+) 2.95071995E-02 2 -2000011 11 # BR(~chi_20 -> ~e_R+ e-) 0.00000000E+00 2 1000013 -13 # BR(~chi_20 -> ~mu_L- mu+) 0.00000000E+00 2 -1000013 13 # BR(~chi_20 -> ~mu_L+ mu-) 2.95071995E-02 2 2000013 -13 # BR(~chi_20 -> ~mu_R- mu+) 2.95071995E-02 2 -2000013 13 # BR(~chi_20 -> ~mu_R+ mu-) 4.40985601E-01 2 1000015 -15 # BR(~chi_20 -> ~tau_1- tau+) 4.40985601E-01 2 -1000015 15 # BR(~chi_20 -> ~tau_1+ tau-) 0.00000000E+00 2 2000015 -15 # BR(~chi_20 -> ~tau_2- tau+) 0.00000000E+00 2 -2000015 15 # BR(~chi_20 -> ~tau_2+ tau-) 0.00000000E+00 2 1000012 -12 # BR(~chi_20 -> ~nu_eL nu_eb) 0.00000000E+00 2 -1000012 12 # BR(~chi_20 -> ~nu_eL* nu_e ) 0.00000000E+00 2 1000014 -14 # BR(~chi_20 -> ~nu_muL nu_mub) 0.00000000E+00 2 -1000014 14 # BR(~chi_20 -> ~nu_muL* nu_mu ) 0.00000000E+00 2 1000016 -16 # BR(~chi_20 -> ~nu_tau1 nu_taub) 0.00000000E+00 2 -1000016 16 # BR(~chi_20 -> ~nu_tau1* nu_tau ) # # PDG Width DECAY 1000025 1.91598495E+00 # neutralino3 decays # BR NDA ID1 ID2 1.13226601E-01 2 1000022 23 # BR(~chi_30 -> ~chi_10 Z ) 2.11969194E-01 2 1000023 23 # BR(~chi_30 -> ~chi_20 Z ) 2.95329778E-01 2 1000024 -24 # BR(~chi_30 -> ~chi_1+ W-) 2.95329778E-01 2 -1000024 24 # BR(~chi_30 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_30 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_30 -> ~chi_2- W+) 2.13076490E-02 2 1000022 25 # BR(~chi_30 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_30 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_30 -> ~chi_10 A ) 1.24538329E-02 2 1000023 25 # BR(~chi_30 -> ~chi_20 h ) 0.00000000E+00 2 1000023 35 # BR(~chi_30 -> ~chi_20 H ) 0.00000000E+00 2 1000023 36 # BR(~chi_30 -> ~chi_20 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_30 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_30 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_30 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_30 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_30 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_30 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_30 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_30 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_30 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_30 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_30 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_30 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_30 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_30 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_30 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_30 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_30 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_30 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_30 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_30 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_30 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_30 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_30 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_30 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_30 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_30 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_30 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_30 -> ~b_2* b ) 5.57220455E-04 2 1000011 -11 # BR(~chi_30 -> ~e_L- e+) 5.57220455E-04 2 -1000011 11 # BR(~chi_30 -> ~e_L+ e-) 1.25266782E-03 2 2000011 -11 # BR(~chi_30 -> ~e_R- e+) 1.25266782E-03 2 -2000011 11 # BR(~chi_30 -> ~e_R+ e-) 5.57220455E-04 2 1000013 -13 # BR(~chi_30 -> ~mu_L- mu+) 5.57220455E-04 2 -1000013 13 # BR(~chi_30 -> ~mu_L+ mu-) 1.25266782E-03 2 2000013 -13 # BR(~chi_30 -> ~mu_R- mu+) 1.25266782E-03 2 -2000013 13 # BR(~chi_30 -> ~mu_R+ mu-) 5.26279239E-03 2 1000015 -15 # BR(~chi_30 -> ~tau_1- tau+) 5.26279239E-03 2 -1000015 15 # BR(~chi_30 -> ~tau_1+ tau-) 6.72814564E-03 2 2000015 -15 # BR(~chi_30 -> ~tau_2- tau+) 6.72814564E-03 2 -2000015 15 # BR(~chi_30 -> ~tau_2+ tau-) 3.18920485E-03 2 1000012 -12 # BR(~chi_30 -> ~nu_eL nu_eb) 3.18920485E-03 2 -1000012 12 # BR(~chi_30 -> ~nu_eL* nu_e ) 3.18920485E-03 2 1000014 -14 # BR(~chi_30 -> ~nu_muL nu_mub) 3.18920485E-03 2 -1000014 14 # BR(~chi_30 -> ~nu_muL* nu_mu ) 3.20245934E-03 2 1000016 -16 # BR(~chi_30 -> ~nu_tau1 nu_taub) 3.20245934E-03 2 -1000016 16 # BR(~chi_30 -> ~nu_tau1* nu_tau ) # # PDG Width DECAY 1000035 2.58585079E+00 # neutralino4 decays # BR NDA ID1 ID2 2.15369294E-02 2 1000022 23 # BR(~chi_40 -> ~chi_10 Z ) 1.85499971E-02 2 1000023 23 # BR(~chi_40 -> ~chi_20 Z ) 0.00000000E+00 2 1000025 23 # BR(~chi_40 -> ~chi_30 Z ) 2.49541430E-01 2 1000024 -24 # BR(~chi_40 -> ~chi_1+ W-) 2.49541430E-01 2 -1000024 24 # BR(~chi_40 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_40 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_40 -> ~chi_2- W+) 6.93213268E-02 2 1000022 25 # BR(~chi_40 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_40 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_40 -> ~chi_10 A ) 1.47602336E-01 2 1000023 25 # BR(~chi_40 -> ~chi_20 h ) 0.00000000E+00 2 1000023 35 # BR(~chi_40 -> ~chi_20 H ) 0.00000000E+00 2 1000023 36 # BR(~chi_40 -> ~chi_20 A ) 0.00000000E+00 2 1000025 25 # BR(~chi_40 -> ~chi_30 h ) 0.00000000E+00 2 1000025 35 # BR(~chi_40 -> ~chi_30 H ) 0.00000000E+00 2 1000025 36 # BR(~chi_40 -> ~chi_30 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_40 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_40 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_40 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_40 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_40 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_40 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_40 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_40 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_40 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_40 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_40 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_40 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_40 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_40 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_40 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_40 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_40 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_40 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_40 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_40 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_40 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_40 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_40 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_40 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_40 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_40 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_40 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_40 -> ~b_2* b ) 9.64835418E-03 2 1000011 -11 # BR(~chi_40 -> ~e_L- e+) 9.64835418E-03 2 -1000011 11 # BR(~chi_40 -> ~e_L+ e-) 3.75684470E-03 2 2000011 -11 # BR(~chi_40 -> ~e_R- e+) 3.75684470E-03 2 -2000011 11 # BR(~chi_40 -> ~e_R+ e-) 9.64835418E-03 2 1000013 -13 # BR(~chi_40 -> ~mu_L- mu+) 9.64835418E-03 2 -1000013 13 # BR(~chi_40 -> ~mu_L+ mu-) 3.75684470E-03 2 2000013 -13 # BR(~chi_40 -> ~mu_R- mu+) 3.75684470E-03 2 -2000013 13 # BR(~chi_40 -> ~mu_R+ mu-) 2.68215241E-03 2 1000015 -15 # BR(~chi_40 -> ~tau_1- tau+) 2.68215241E-03 2 -1000015 15 # BR(~chi_40 -> ~tau_1+ tau-) 1.62289809E-02 2 2000015 -15 # BR(~chi_40 -> ~tau_2- tau+) 1.62289809E-02 2 -2000015 15 # BR(~chi_40 -> ~tau_2+ tau-) 2.53796547E-02 2 1000012 -12 # BR(~chi_40 -> ~nu_eL nu_eb) 2.53796547E-02 2 -1000012 12 # BR(~chi_40 -> ~nu_eL* nu_e ) 2.53796547E-02 2 1000014 -14 # BR(~chi_40 -> ~nu_muL nu_mub) 2.53796547E-02 2 -1000014 14 # BR(~chi_40 -> ~nu_muL* nu_mu ) 2.54724352E-02 2 1000016 -16 # BR(~chi_40 -> ~nu_tau1 nu_taub) 2.54724352E-02 2 -1000016 16 # BR(~chi_40 -> ~nu_tau1* nu_tau ) pythia8-8.1.80.orig/examples/main84.cmnd0000644000175000017500000000107212217346167016123 0ustar sunsun! main84.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. // specify statistics parameters Main:numberOfEvents = 100 // number of events generated // specify shower options SpaceShower:MEafterFirst = off TimeShower:MEafterFirst = off // specify merging options Merging:doMGMerging = on Merging:Process = pp>e+ve Merging:TMS = 30. Merging:nJetMax = 2 // specify PDF set PDF:useLHAPDF = on PDF:LHAPDFset = cteq6ll.LHpdf pythia8-8.1.80.orig/examples/main71.cc0000644000175000017500000002017312217346167015566 0ustar sunsun// main71.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Richard Corke. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. /* * Simple example of fastjet analysis. Roughly follows analysis of: * T. Aaltonen et al. [CDF Collaboration], * Measurement of the cross section for W-boson production in association * with jets in ppbar collisions at sqrt(s)=1.96$ TeV * Phys. Rev. D 77 (2008) 011108 * arXiv:0711.4044 [hep-ex] * * Cuts: * ET(elec) > 20GeV * |eta(elec)| < 1.1 * ET(missing) > 30GeV * ET(jet) > 20GeV * |eta(jet)| < 2.0 * deltaR(elec, jet) > 0.52 * Not used: * mT(W) > 20GeV */ #include "Pythia8/Pythia.h" // This is the minimal interface needed to access FastJet. // A more sophisticated interface is demonstrated in main72.cc. #include "fastjet/PseudoJet.hh" #include "fastjet/ClusterSequence.hh" using namespace Pythia8; // Experimental cross section // sigma(W -> ev + >= n-jet; ET(n'th-jet) > 25GeV), n = 0, 1, 2, 3, 4 const double expCrossSec[] = { 798.0, 53.5, 6.8, 0.84, 0.074 }; int main() { // Settings int nEvent = 10000; bool doMPI = true; // Generator Pythia pythia; // Single W production pythia.readString("WeakSingleBoson:ffbar2W = on"); // Force decay W->ev pythia.readString("24:onMode = off"); pythia.readString("24:onIfAny = 11 12"); // Multiparton Interactions if (doMPI == false) pythia.readString("PartonLevel:MPI = off"); // Initialisation, p pbar @ 1.96 TeV pythia.readString("Beams:idB = -2212"); pythia.readString("Beams:eCM = 1960."); pythia.init(); // Histograms Hist dSigma1("1-jet cross-section (E_jet1 > 20 GeV)", 70, 0.0, 350.0); Hist dSigma2("2-jet cross-section (E_jet2 > 20 GeV)", 38, 0.0, 190.0); Hist dSigma3("3-jet cross-section (E_jet3 > 20 GeV)", 16, 0.0, 80.0); Hist dSigma4("4-jet cross-section (E_jet4 > 20 GeV)", 7, 0.0, 35.0); Hist *dSigmaHist[5] = { NULL, &dSigma1, &dSigma2, &dSigma3, &dSigma4 }; double dSigmaBin[5] = { 0.0, 350.0 / 70.0, 190.0 / 38.0, 80.0 / 16.0, 35.0 / 7.0 }; // Fastjet analysis - select algorithm and parameters double Rparam = 0.4; fastjet::Strategy strategy = fastjet::Best; fastjet::RecombinationScheme recombScheme = fastjet::E_scheme; fastjet::JetDefinition *jetDef = NULL; jetDef = new fastjet::JetDefinition(fastjet::kt_algorithm, Rparam, recombScheme, strategy); // Fastjet input std::vector fjInputs; // Statistics for later int nEventAccept25[5] = { 0, 0, 0, 0, 0 }; int vetoCount[4] = { 0, 0, 0, 0 }; const char *vetoStr[] = { "ET(elec)", "|eta(elec)|", "ET(missing)", "deltaR(elec, jet)" }; bool firstEvent = true; // Begin event loop. Generate event. Skip if error. for (int iEvent = 0; iEvent < nEvent; ++iEvent) { if (!pythia.next()) continue; // Need to find the electron from the W decay - cheat a bit here // and find it from the W in the event record int idxW = -1; for (int i = pythia.event.size() - 1; i > 0; i--) { if (pythia.event[i].idAbs() == 24) { idxW = i; break; } } if (idxW == -1) { cout << "Error: Could not find W" << endl; continue; } // Find the electron from the W decay int idxElec = idxW; while(true) { int daughter = pythia.event[idxElec].daughter1(); if (daughter == 0) break; else idxElec = daughter; } if (pythia.event[idxElec].idAbs() != 11 || !pythia.event[idxElec].isFinal()) { cout << "Error: Found incorrect decay product of the W" << endl; continue; } // Electron cuts if (pythia.event[idxElec].pT() < 20.0) { vetoCount[0]++; continue; } if (abs(pythia.event[idxElec].eta()) > 1.1) { vetoCount[1]++; continue; } // Reset Fastjet input fjInputs.resize(0); // Keep track of missing ET Vec4 missingETvec; // Loop over event record to decide what to pass to FastJet for (int i = 0; i < pythia.event.size(); ++i) { // Final state only if (!pythia.event[i].isFinal()) continue; // No neutrinos if (pythia.event[i].idAbs() == 12 || pythia.event[i].idAbs() == 14 || pythia.event[i].idAbs() == 16) continue; // Only |eta| < 3.6 if (fabs(pythia.event[i].eta()) > 3.6) continue; // Missing ET missingETvec += pythia.event[i].p(); // Do not include the electron from the W decay if (i == idxElec) continue; // Store as input to Fastjet fjInputs.push_back( fastjet::PseudoJet( pythia.event[i].px(), pythia.event[i].py(), pythia.event[i].pz(), pythia.event[i].e() ) ); } if (fjInputs.size() == 0) { cout << "Error: event with no final state particles" << endl; continue; } // Run Fastjet algorithm vector inclusiveJets, sortedJets; fastjet::ClusterSequence clustSeq(fjInputs, *jetDef); // For the first event, print the FastJet details if (firstEvent) { cout << "Ran " << jetDef->description() << endl; cout << "Strategy adopted by FastJet was " << clustSeq.strategy_string() << endl << endl; firstEvent = false; } // Extract inclusive jets sorted by pT (note minimum pT of 20.0 GeV) inclusiveJets = clustSeq.inclusive_jets(20.0); sortedJets = sorted_by_pt(inclusiveJets); // Missing ET cut double missingET = missingETvec.pT(); if (missingET < 30.0) { vetoCount[2]++; continue; } // Keep track of jets with pT > 20/25 GeV int jetCount20 = 0, jetCount25 = 0; // For the deltaR calculation below bool vetoEvent = false; fastjet::PseudoJet fjElec(pythia.event[idxElec].px(), pythia.event[idxElec].py(), pythia.event[idxElec].pz(), pythia.event[idxElec].e()); for (unsigned int i = 0; i < sortedJets.size(); i++) { // Only count jets that have |eta| < 2.0 if (fabs(sortedJets[i].rap()) > 2.0) continue; // Check distance between W decay electron and jets if (fjElec.squared_distance(sortedJets[i]) < 0.52 * 0.52) { vetoEvent = true; break; } // Fill dSigma histograms and count jets with ET > 25.0 if (sortedJets[i].perp() > 25.0) jetCount25++; if (jetCount20 <= 3) dSigmaHist[++jetCount20]->fill(sortedJets[i].perp()); } if (vetoEvent) { vetoCount[3]++; continue; } if (jetCount25 > 4) jetCount25 = 4; for (int i = jetCount25; i >= 0; i--) nEventAccept25[i]++; // End of event loop. } // Statistics pythia.stat(); // Output histograms double sigmapb = pythia.info.sigmaGen() * 1.0E9; for (int i = 1; i <= 4; i++) (*dSigmaHist[i]) = ((*dSigmaHist[i]) * sigmapb) / nEvent / dSigmaBin[i]; cout << dSigma1 << dSigma2 << dSigma3 << dSigma4 << endl; // Output cross-sections cout << "Jet algorithm is kT" << endl; cout << "Multiparton interactions are switched " << ( (doMPI) ? "on" : "off" ) << endl; cout << endl << nEvent << " events generated. " << nEventAccept25[0] << " events passed cuts." << endl; cout << "Vetos:" << endl; for (int i = 0; i < 4; i++) cout << " " << vetoStr[i] << " = " << vetoCount[i] << endl; cout << endl << "Inclusive cross-sections (pb):" << endl; for (int i = 0; i < 5; i++) { cout << scientific << setprecision(3) << " " << i << "-jet - Pythia = " << ((double) nEventAccept25[i] / (double) nEvent) * sigmapb; cout << ", Experimental = " << expCrossSec[i]; if (i != 0) { cout << scientific << setprecision(3) << ", Pythia ratio to " << i - 1 << "-jet = " << ((double) nEventAccept25[i] / (double) nEventAccept25[i - 1]); cout << scientific << setprecision(3) << ", Experimental ratio to " << i - 1 << "-jet = " << expCrossSec[i] / expCrossSec[i - 1]; } cout << endl; } // Done. delete jetDef; return 0; } pythia8-8.1.80.orig/examples/main04.cmnd0000644000175000017500000000555612217346163016122 0ustar sunsun! File: main04.cmnd ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! Names are case-insensitive - but spellings-sensitive! ! The changes here are illustrative, not always physics-motivated. ! 1) Settings used in the main program. Main:numberOfEvents = 1000 ! number of events to generate Main:timesAllowErrors = 10 ! how many aborts before run stops ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showChangedParticleData = off ! list changed particle data Next:numberCount = 500 ! print message every n events Next:numberShowInfo = 3 ! print event information n times Next:numberShowProcess = 0 ! print process record n times Next:numberShowEvent = 0 ! print event record n times ! 3) Beam parameter settings. Values below agree with default ones. Beams:idA = 2212 ! first beam, p = 2212, pbar = -2212 Beams:idB = 2212 ! second beam, p = 2212, pbar = -2212 Beams:eCM = 14000. ! CM energy of collision ! 4) Settings for the hard-process generation. SoftQCD:all = on ! Allow total sigma = elastic/SD/DD/ND ! Optionally only study one or a few processes at a time. #SoftQCD:elastic = on ! Elastic #SoftQCD:singleDiffractive = on ! Single diffractive #SoftQCD:doubleDiffractive = on ! Double diffractive #SoftQCD:centralDiffractive = on ! Central diffractive #SoftQCD:nonDiffractive = on ! Nondiffractive (inelastic) #SoftQCD:inelastic = on ! All inelastic ! 5) Optionally switch on hand-set cross section and Coulomb term. ! Note: these values are illustrative only, not to be taken seriously. #SigmaTotal:setOwn = on ! set your own total/elastic/diffr. sigma #SigmaTotal:sigmaTot = 106. ! total cross section (excluding Coulomb) #SigmaTotal:sigmaXX = 5. ! reduce double diffractive cross section #SigmaElastic:setOwn = on ! suboption for Coulomb term in elastic #SigmaElastic:tAbsMin = 4e-5 ! divergence requires lower cutoff ! 6) Optionally select diffractive model. Diffraction:PomFlux = 5 ! the MBR model for diffraction ! 7) Multiparton interactions and impact parameter picture. ! Note: these values are illustrative only, not to be taken seriously. MultipartonInteractions:pT0Ref = 2. MultipartonInteractions:ecmRef = 1960. MultipartonInteractions:ecmPow = 0.16 MultipartonInteractions:pTmin = 0.2 MultipartonInteractions:bProfile = 2 #MultipartonInteractions:coreRadius = 0.4 #MultipartonInteractions:coreFraction = 0.5 MultipartonInteractions:expPow = 1. ! 8) Other settings. Can be expanded as desired. ! Note: may overwrite some of the values above, so watch out. #Tune:pp = 6 ! use Tune 4Cx pythia8-8.1.80.orig/examples/main32_unw.par0000644000175000017500000000333012217346166016644 0ustar sunsun W + 3 jets W-> ell nu ======================================= Generation cuts for the partonic event sample: Light jets: ptmin= 15.0000000000000 |etamax|= 6.00000000000000 dR(j-j)> 0.700000000000000 Leptons: ptmin(lep)= 0.00000000000000 |etamax|= 10.0000000000000 Et(miss)> 0.00000000000000 dR(l-j)> 0.00000000000000 ************** run parameters 3 ! hard process code 0.000 4.700 174.300 80.419 91.188 120.000 ! mc,mb,mt,mw,mz,mh 2 1.00000000000000 ! ih2 3 4000.00000000000 ! ebeam 4 9.00000000000000 ! ndns 5 1.00000000000000 ! iqopt 6 1.00000000000000 ! qfac 7 1.00000000000000 ! ickkw 8 1.00000000000000 ! ktfac 10 3.00000000000000 ! njets 30 15.0000000000000 ! ptjmin 33 0.00000000000000 ! ptlmin 34 0.00000000000000 ! metmin 40 6.00000000000000 ! etajmax 43 10.0000000000000 ! etalmax 50 0.700000000000000 ! drjmin 55 0.00000000000000 ! drlmin 90 28639.0000000000 ! iseed1 91 4774.00000000000 ! iseed2 110 0.260000000000000 ! xlclu 111 1.00000000000000 ! lpclu 151 1.00000000000000 ! iwdecmod 160 1.00000000000000 ! cluopt 190 29570.0000000000 ! iseed3 191 60156.0000000000 ! iseed4 ************** end parameters 912.905 0.0914176 ! Crosssection +- error (pb) 100 29787.4 ! unwtd events, lum (pb-1) Njob= 2 pythia8-8.1.80.orig/examples/main53.cc0000644000175000017500000000433212217346166015564 0ustar sunsun// main53.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Peter Skands, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how to interface an external process with an incoming photon // in a hadron beam, using the MRST2004QED PDF set. // All input apart from the name of the external LHEF file is specified in the // main53.cmnd file. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator. Shorthand for the event. Pythia pythia; Event& event = pythia.event; // Read in commands from external file. pythia.readFile("main53.cmnd"); // Extract settings to be used in the main program. int nEvent = pythia.mode("Main:numberOfEvents"); // Initialize. Either of two opions, to be picked in main53.cmnd. // 1) Read in external event with incoming photon in the ME, // from pre-generated .lhe file (thanks to SANC and R. Sadykov). // 2) Use internal fermion gamma -> W+- fermion' process. pythia.init(); // Histograms for pT distribution in gluon production vertex. Hist pTprim( "pT of photon production, no ISR", 100, 0., 100.); Hist pTwith( "pT of photon production, with ISR", 100, 0., 100.); // Begin event loop. for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if failure. if (!pythia.next()) { break; } // Analyze event to find branching where photon is produced. int iGam = (event[3].id() == 22) ? 3 : 4; int iGamMother = iGam; for ( ; ; ) { iGamMother = event[iGam].mother1(); if (iGamMother < iGam || event[iGamMother].id() != 22) break; iGam = iGamMother; } // Find and histogram pT in this branching. if (iGamMother < iGam) pTprim.fill( event[iGam].pT() ); else { int iQ = iGamMother; int size = event.size(); do ++iQ; while (event[iQ].status() != -43 && iQ < size - 1); if (event[iQ].status() == -43) pTwith.fill( event[iQ].pT() ); } // End of event loop. } // Final statistics and histogram output. pythia.stat(); cout << pTprim << pTwith; return 0; } pythia8-8.1.80.orig/examples/.DS_Store0000644000175000017500000001400412217346162015635 0ustar sunsunBud1eflg1Scompoutreflg1ScompB>outrefmoDDdutcoutrefmodDdutcoutrefph1ScompB  @ @ @ @ EDSDB ` @ @ @pythia8-8.1.80.orig/examples/powheg-dijets.lhe0000644000175000017500000025117712217346206017432 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9.000E+00 21 1 1 2 516 513 -3.859801335E+00 3.411371117E+00 -3.247021116E+01 3.287628525E+01 4.768371582E-07 0.00000E+00 9.000E+00 5 10001 1.00000E+00 2.93654E+00 -1.00000E+00 2.99572E-01 21 -1 0 0 514 512 0.000000000E+00 0.000000000E+00 1.627825865E+02 1.627825865E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 515 513 0.000000000E+00 0.000000000E+00 -6.331390121E+01 6.331390121E+01 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 514 513 -1.093822726E+01 3.897253757E-01 -6.257447494E+01 6.352449618E+01 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 511 512 7.813518560E+00 1.604576127E+00 1.393464170E+02 1.395745309E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 515 511 3.124708704E+00 -1.994301502E+00 2.269674322E+01 2.299746064E+01 3.371747881E-07 0.00000E+00 9.000E+00 5 10001 1.00000E+00 5.94913E+00 -1.00000E+00 2.25969E-01 21 -1 0 0 512 511 0.000000000E+00 0.000000000E+00 2.510866350E+02 2.510866350E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 515 516 0.000000000E+00 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516 5.058900302E+00 7.453961411E+00 1.203515478E+02 1.206882309E+02 0.000000000E+00 0.00000E+00 9.000E+00 5 10001 1.00000E+00 2.74497E+01 -1.00000E+00 1.55733E-01 21 -1 0 0 511 512 0.000000000E+00 0.000000000E+00 1.369601849E+01 1.369601849E+01 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 512 513 0.000000000E+00 0.000000000E+00 -3.913226884E+01 3.913226884E+01 0.000000000E+00 0.00000E+00 9.000E+00 -2 1 1 2 0 514 1.554245643E+00 1.458487529E-01 -8.174441764E-01 1.792781740E+00 3.300000131E-01 0.00000E+00 9.000E+00 2 1 1 2 511 0 -4.989424514E+00 -2.106353058E+01 -5.148217274E+00 2.225263397E+01 3.300000131E-01 0.00000E+00 9.000E+00 21 1 1 2 514 513 3.435178871E+00 2.091768182E+01 -1.947058891E+01 2.878287163E+01 3.371747881E-07 0.00000E+00 9.000E+00 5 10001 1.00000E+00 5.90578E+00 -1.00000E+00 2.26465E-01 21 -1 0 0 515 511 0.000000000E+00 0.000000000E+00 8.767705897E+00 8.767705897E+00 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 512 516 0.000000000E+00 0.000000000E+00 -2.439037700E+02 2.439037700E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 515 516 5.527622097E+00 1.182081557E+01 -2.133602170E+02 2.137589027E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 512 513 3.780135220E-01 -1.186271853E+01 -2.795186414E+01 3.036731292E+01 7.539457465E-07 0.00000E+00 9.000E+00 21 1 1 2 513 511 -5.905635619E+00 4.190295858E-02 6.176016996E+00 8.545260315E+00 3.153981341E-07 0.00000E+00 9.000E+00 5 10001 1.00000E+00 6.57277E+01 -1.00000E+00 1.32595E-01 21 -1 0 0 513 511 0.000000000E+00 0.000000000E+00 1.744926529E+01 1.744926529E+01 0.000000000E+00 0.00000E+00 9.000E+00 2 -1 0 0 512 0 0.000000000E+00 0.000000000E+00 -1.632366789E+02 1.632366789E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 512 514 -3.008360477E-01 2.451892898E+01 -8.198490931E+00 2.585505046E+01 3.153981341E-07 0.00000E+00 9.000E+00 2 1 1 2 513 0 -7.594576664E+00 1.071410329E+01 -1.061353970E+02 1.069453178E+02 3.300000131E-01 0.00000E+00 9.000E+00 21 1 1 2 514 511 7.895412711E+00 -3.523303227E+01 -3.145352572E+01 4.788557596E+01 4.768371582E-07 0.00000E+00 9.000E+00 5 10001 1.00000E+00 1.06178E+01 -1.00000E+00 1.92738E-01 21 -1 0 0 513 514 0.000000000E+00 0.000000000E+00 1.919386585E+02 1.919386585E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 512 511 0.000000000E+00 0.000000000E+00 -2.043998595E+01 2.043998595E+01 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 515 511 -2.269433070E+01 2.799925520E+01 2.838975543E+01 4.587994280E+01 8.259061849E-07 0.00000E+00 9.000E+00 21 1 1 2 512 514 1.650603059E+01 -1.937125251E+01 2.592327208E+00 2.558152907E+01 6.982907363E-07 0.00000E+00 9.000E+00 21 1 1 2 513 515 6.188300111E+00 -8.628002693E+00 1.405165900E+02 1.409171726E+02 1.907348633E-06 0.00000E+00 9.000E+00 5 10001 1.00000E+00 1.62405E+01 -1.00000E+00 1.74147E-01 -1 -1 0 0 0 515 0.000000000E+00 0.000000000E+00 2.087709428E+01 2.087709428E+01 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 513 514 0.000000000E+00 0.000000000E+00 -8.968351325E+01 8.968351325E+01 0.000000000E+00 0.00000E+00 9.000E+00 -1 1 1 2 0 514 1.653377672E+01 -9.906316233E+00 1.486984070E+01 2.434588130E+01 3.300000131E-01 0.00000E+00 9.000E+00 21 1 1 2 511 515 -5.293438346E+00 2.845894775E+00 -1.326157869E+01 1.455984464E+01 2.920019320E-07 0.00000E+00 9.000E+00 21 1 1 2 513 511 -1.124033837E+01 7.060421458E+00 -7.041468097E+01 7.165488158E+01 1.907348633E-06 0.00000E+00 9.000E+00 5 10001 1.00000E+00 5.70835E+00 -1.00000E+00 2.28805E-01 21 -1 0 0 512 511 0.000000000E+00 0.000000000E+00 3.559724264E-01 3.559724264E-01 0.000000000E+00 0.00000E+00 9.000E+00 2 -1 0 0 513 0 0.000000000E+00 0.000000000E+00 -1.288230549E+03 1.288230549E+03 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 513 511 -8.034579759E+00 -1.932888378E+01 -6.211716878E+02 6.215242763E+02 7.629394531E-06 0.00000E+00 9.000E+00 2 1 1 2 514 0 1.745519615E+00 1.203314229E+01 -3.405643128E+02 3.407814599E+02 3.300000131E-01 0.00000E+00 9.000E+00 21 1 1 2 512 514 6.289060144E+00 7.295741490E+00 -3.261385761E+02 3.262807854E+02 5.394796609E-06 0.00000E+00 9.000E+00 5 10001 1.00000E+00 1.22761E+01 -1.00000E+00 1.85943E-01 21 -1 0 0 513 514 0.000000000E+00 0.000000000E+00 2.178628795E+01 2.178628795E+01 0.000000000E+00 0.00000E+00 9.000E+00 -2 -1 0 0 0 515 0.000000000E+00 0.000000000E+00 -2.269207226E+01 2.269207226E+01 0.000000000E+00 0.00000E+00 9.000E+00 -2 1 1 2 0 511 -6.830666042E+00 2.759337951E+00 -7.101712596E+00 1.023792783E+01 3.300000131E-01 0.00000E+00 9.000E+00 21 1 1 2 513 515 5.568058776E+00 -1.300742883E+01 1.503681926E+01 2.064709221E+01 3.769728732E-07 0.00000E+00 9.000E+00 21 1 1 2 511 514 1.262607267E+00 1.024809088E+01 -8.840890978E+00 1.359334017E+01 2.064765462E-07 0.00000E+00 9.000E+00 5 10001 1.00000E+00 7.18535E+00 -1.00000E+00 2.13892E-01 21 -1 0 0 512 513 0.000000000E+00 0.000000000E+00 1.838150044E+01 1.838150044E+01 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 511 514 0.000000000E+00 0.000000000E+00 -1.764127484E+01 1.764127484E+01 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 512 514 1.062526379E+00 -1.322844083E+01 -7.887989197E+00 1.543829597E+01 3.371747881E-07 0.00000E+00 9.000E+00 21 1 1 2 511 516 5.419529341E+00 1.012808017E+01 5.728519644E+00 1.283609144E+01 3.475518164E-07 0.00000E+00 9.000E+00 21 1 1 2 516 513 -6.482055720E+00 3.100360661E+00 2.899695146E+00 7.748387866E+00 7.300048300E-08 0.00000E+00 9.000E+00 5 10001 1.00000E+00 9.25839E+00 -1.00000E+00 1.99646E-01 21 -1 0 0 515 513 0.000000000E+00 0.000000000E+00 2.244293193E+02 2.244293193E+02 0.000000000E+00 0.00000E+00 9.000E+00 -3 -1 0 0 0 515 0.000000000E+00 0.000000000E+00 -6.469621264E+00 6.469621264E+00 0.000000000E+00 0.00000E+00 9.000E+00 -3 1 1 2 0 511 4.797243839E+00 1.345526354E+01 6.047719900E+00 1.552039243E+01 5.000000000E-01 0.00000E+00 9.000E+00 21 1 1 2 512 513 -1.511447225E+00 -1.015207652E+01 2.101451502E+02 2.103956589E+02 3.814697266E-06 0.00000E+00 9.000E+00 21 1 1 2 511 512 -3.285796613E+00 -3.303187015E+00 1.766827886E+00 4.982889184E+00 2.493441184E-07 0.00000E+00 9.000E+00 #Random number generator exit values: 7421 819682768 67 pythia8-8.1.80.orig/examples/main87.cc0000644000175000017500000004615512217346167015605 0ustar sunsun// main87.cc is a part of the PYTHIA event generator. // Copyright (C) 2011 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This program is written by Stefan Prestel. // It illustrates how to do NL3 merging, // see the Matrix Element Merging page in the online manual. #include "Pythia8/Pythia.h" #include "Pythia8/Pythia8ToHepMC.h" #include "HepMC/GenEvent.h" #include "HepMC/IO_GenEvent.h" // Following line to be used with HepMC 2.04 onwards. #include "HepMC/Units.h" using namespace Pythia8; //========================================================================== // Example main programm to illustrate merging int main( int argc, char* argv[] ){ // Check that correct number of command-line arguments if (argc != 4) { cerr << " Unexpected number of command-line arguments ("< xsecLO; vector nSelectedLO; vector nAcceptLO; cout << endl << endl << endl; cout << "Start estimating nl3 tree level cross section" << endl; while(njetcounterLO >= 0){ // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathTree+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathTree + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); pythia.settings.mode("Merging:nRequested", njetcounterLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Start generation loop for( int iEvent=0; iEvent 0 ) njetcounterLO--; else break; } //----------------------------------------------------------------------------- //----------------------------------------------------------------------------- cout << endl << endl << endl; cout << "Start estimating nl3 virtual corrections cross section" << endl; pythia.settings.flag("Merging:doNL3Tree",false); pythia.settings.flag("Merging:doNL3Loop",true); int njetcounterNLO = nMaxNLO; string iPathLoop= iPath + "_powheg"; vector xsecNLO; vector nSelectedNLO; vector nAcceptNLO; vector strategyNLO; while(njetcounterNLO >= 0){ // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterNLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathLoop+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathLoop + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); pythia.settings.mode("Merging:nRequested", njetcounterNLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Start generation loop for( int iEvent=0; iEvent 0 ) njetcounterNLO--; else break; } // Set k-factors int sizeLO = int(xsecLO.size()); int sizeNLO = int(xsecNLO.size()); double k0 = 1.; double k1 = 1.; double k2 = 1.; // Lowest order k-factor only if ( false ) k1 = k2 = k0 = xsecNLO.back() / xsecLO.back(); // No k-factors if ( true ) k0 = k1 = k2 = 1.; cout << " K-Factors :" << endl; cout << "k0 = " << k0 << endl; cout << "k1 = " << k1 << endl; cout << "k2 = " << k2 << endl; // Switch off cross section estimation. pythia.settings.flag("Merging:doXSectionEstimate", false); // Switch showering and multiple interaction back on. pythia.settings.flag("PartonLevel:FSR",fsr); pythia.settings.flag("PartonLevel:ISR",isr); pythia.settings.flag("HadronLevel:all",had); pythia.settings.flag("PartonLevel:MPI",mpi); //----------------------------------------------------------------------------- //----------------------------------------------------------------------------- // Declare sample cross section for output. double sigmaTemp = 0.; vector sampleXStree; vector sampleXSvirt; vector sampleXSsubtTree; // Cross section an error. double sigmaTotal = 0.; double errorTotal = 0.; // Switch on tree-level processing. pythia.settings.flag("Merging:doNL3Tree",true); pythia.settings.flag("Merging:doNL3Loop",false); pythia.settings.flag("Merging:doNL3Subt",false); pythia.settings.mode("Merging:nRecluster",0); pythia.settings.mode("Merging:nRequested", -1); njetcounterLO = nMaxLO; iPathTree = iPath + "_tree"; while(njetcounterLO >= 0){ // Set k factors pythia.settings.parm("Merging:kFactor0j", k0); pythia.settings.parm("Merging:kFactor1j", k1); pythia.settings.parm("Merging:kFactor2j", k2); // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathTree+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathTree + in.str(); cout << endl << endl << endl << "Start tree level treatment for " << njetcounterLO << " jets" << endl; LHAupLHEF lhareader((char*)(LHEfile).c_str()); pythia.settings.mode("Merging:nRequested", njetcounterLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Remember position in vector of cross section estimates. int iNow = sizeLO-1-njetcounterLO; // Start generation loop for( int iEvent=0; iEventweights().push_back(weightNLO*normhepmc); // Fill HepMC event. ToHepMC.fill_next_event( pythia, hepmcevt ); // Add the weight of the current event to the cross section. sigmaTotal += weightNLO*normhepmc; sigmaTemp += weightNLO*normhepmc; errorTotal += pow2(weightNLO*normhepmc); // Report cross section to hepmc HepMC::GenCrossSection xsec; xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } // end loop over events to generate // print cross section, errors pythia.stat(); // Save sample cross section for output. sampleXStree.push_back(sigmaTemp); sigmaTemp = 0.; // Restart with ME of a reduced the number of jets if( njetcounterLO > 0 ) njetcounterLO--; else break; } //----------------------------------------------------------------------------- //----------------------------------------------------------------------------- cout << endl << endl << endl; cout << "Start nl3 virtual corrections part" << endl; // Switch on loop-level processing. pythia.settings.flag("Merging:doNL3Tree",false); pythia.settings.flag("Merging:doNL3Loop",true); pythia.settings.flag("Merging:doNL3Subt",false); pythia.settings.mode("Merging:nRecluster",0); njetcounterNLO = nMaxNLO; iPathLoop = iPath + "_powheg"; while(njetcounterNLO >= 0){ // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterNLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathLoop+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathLoop + in.str(); cout << endl << endl << endl << "Start loop level treatment for " << njetcounterNLO << " jets" << endl; LHAupLHEF lhareader((char*)(LHEfile).c_str()); pythia.settings.mode("Merging:nRequested", njetcounterNLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Remember position in vector of cross section estimates. int iNow = sizeNLO-1-njetcounterNLO; // Start generation loop for( int iEvent=0; iEventweights().push_back(weightNLO*normhepmc); // Fill HepMC event. ToHepMC.fill_next_event( pythia, hepmcevt ); // Add the weight of the current event to the cross section. sigmaTotal += weightNLO*normhepmc; sigmaTemp += weightNLO*normhepmc; errorTotal += pow2(weightNLO*normhepmc); // Report cross section to hepmc HepMC::GenCrossSection xsec; xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } // end loop over events to generate // print cross section, errors pythia.stat(); // Save sample cross section for output. sampleXSvirt.push_back(sigmaTemp); sigmaTemp = 0.; // Restart with ME of a reduced the number of jets if( njetcounterNLO > 0) njetcounterNLO--; else break; } //----------------------------------------------------------------------------- //----------------------------------------------------------------------------- cout << endl << endl << endl; cout << "Shower subtractive events" << endl; // Switch on processing of counter-events. pythia.settings.flag("Merging:doNL3Tree",false); pythia.settings.flag("Merging:doNL3Loop",false); pythia.settings.flag("Merging:doNL3Subt",true); pythia.settings.mode("Merging:nRecluster",1); pythia.settings.mode("Merging:nRequested", -1); int nMaxCT = nMaxNLO + 1; int njetcounterCT = nMaxCT; string iPathSubt = iPath + "_tree"; while(njetcounterCT >= 1){ // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterCT << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathSubt+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathSubt + in.str(); cout << endl << endl << endl << "Start subtractive treatment for " << njetcounterCT << " jets" << endl; LHAupLHEF lhareader((char*)(LHEfile).c_str()); pythia.settings.mode("Merging:nRequested", njetcounterCT); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Remember position in vector of cross section estimates. int iNow = sizeLO-1-njetcounterCT; // Start generation loop for( int iEvent=0; iEventweights().push_back( weightNLO*normhepmc); // Fill HepMC event. ToHepMC.fill_next_event( pythia, hepmcevt ); // Add the weight of the current event to the cross section. sigmaTotal += weightNLO*normhepmc; sigmaTemp += weightNLO*normhepmc; errorTotal += pow2(weightNLO*normhepmc); // Report cross section to hepmc HepMC::GenCrossSection xsec; xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } // end loop over events to generate // print cross section, errors pythia.stat(); // Save sample cross section for output. sampleXSsubtTree.push_back(sigmaTemp); sigmaTemp = 0.; // Restart with ME of a reduced the number of jets if( njetcounterCT > 1 ) njetcounterCT--; else break; } // Print cross section information. cout << endl << endl; cout << " *---------------------------------------------------*" << endl; cout << " | |" << endl; cout << " | Sample cross sections after NL3 merging |" << endl; cout << " | |" << endl; cout << " | Leading order cross sections (mb): |" << endl; for (int i = 0; i < int(sampleXStree.size()); ++i) cout << " | " << sampleXStree.size()-1-i << "-jet: " << setw(17) << scientific << setprecision(6) << sampleXStree[i] << " |" << endl; cout << " | |" << endl; cout << " | NLO order cross sections (mb): |" << endl; for (int i = 0; i < int(sampleXSvirt.size()); ++i) cout << " | " << sampleXSvirt.size()-1-i << "-jet: " << setw(17) << scientific << setprecision(6) << sampleXSvirt[i] << " |" << endl; cout << " | |" << endl; cout << " | Leading-order subtractive cross sections (mb): |" << endl; for (int i = 0; i < int(sampleXSsubtTree.size()); ++i) cout << " | " << sampleXSsubtTree.size()-1-i+1 << "-jet: " << setw(17) << scientific << setprecision(6) << sampleXSsubtTree[i] << " |" << endl; cout << " | |" << endl; cout << " |---------------------------------------------------|" << endl; cout << " |---------------------------------------------------|" << endl; cout << " | Inclusive cross sections: |" << endl; cout << " | |" << endl; cout << " | NL3 merged inclusive cross section: |" << endl; cout << " | " << setw(17) << scientific << setprecision(6) << sigmaTotal << " +- " << setw(17) << sqrt(errorTotal) << " mb " << " |" << endl; cout << " | |" << endl; cout << " | NLO inclusive cross section: |" << endl; cout << " | " << setw(17) << scientific << setprecision(6) << xsecNLO.back() << " mb |" << endl; cout << " | |" << endl; cout << " | LO inclusive cross section: |" << endl; cout << " | " << setw(17) << scientific << setprecision(6) << xsecLO.back() << " mb |" << endl; cout << " | |" << endl; cout << " *---------------------------------------------------*" << endl; cout << endl << endl; // Done return 0; } pythia8-8.1.80.orig/examples/main20.cc0000644000175000017500000000361612217346164015560 0ustar sunsun// main20.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. It shows how PYTHIA 8 can write // a Les Houches Event File based on its process-level events. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator. Pythia pythia; // Process selection. Minimal masses for gamma*/Z and W+-. pythia.readString("WeakDoubleBoson:all = on"); pythia.readString("23:mMin = 50."); pythia.readString("24:mMin = 50."); // Switch off generation of steps subsequent to the process level one. // (These will not be stored anyway, so only steal time.) pythia.readString("PartonLevel:all = off"); // Create an LHAup object that can access relevant information in pythia. LHAupFromPYTHIA8 myLHA(&pythia.process, &pythia.info); // Open a file on which LHEF events should be stored, and write header. myLHA.openLHEF("weakbosons.lhe"); // LHC 8 TeV initialization. pythia.readString("Beams:eCM = 8000."); pythia.init(); // Store initialization info in the LHAup object. myLHA.setInit(); // Write out this initialization info on the file. myLHA.initLHEF(); // Loop over events. for (int i = 0; i < 100; ++i) { // Generate an event. pythia.next(); // Store event info in the LHAup object. myLHA.setEvent(); // Write out this event info on the file. // With optional argument (verbose =) false the file is smaller. myLHA.eventLHEF(); } // Statistics: full printout. pythia.stat(); // Update the cross section info based on Monte Carlo integration during run. myLHA.updateSigma(); // Write endtag. Overwrite initialization info with new cross sections. myLHA.closeLHEF(true); // Done. return 0; } pythia8-8.1.80.orig/examples/main83.cc0000644000175000017500000002662612217346167015602 0ustar sunsun// main83.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This program is written by Stefan Prestel. // It illustrates how to do CKKW-L merging, // see the Matrix Element Merging page in the online manual. #include "Pythia8/Pythia.h" using namespace Pythia8; // Functions for histogramming #include "fastjet/PseudoJet.hh" #include "fastjet/ClusterSequence.hh" #include "fastjet/CDFMidPointPlugin.hh" #include "fastjet/CDFJetCluPlugin.hh" #include "fastjet/D0RunIIConePlugin.hh" //========================================================================== // Find the Durham kT separation of the clustering from // nJetMin --> nJetMin-1 jets in te input event double pTfirstJet( const Event& event, int nJetMin, double Rparam) { double yPartonMax = 4.; // Fastjet analysis - select algorithm and parameters fastjet::Strategy strategy = fastjet::Best; fastjet::RecombinationScheme recombScheme = fastjet::E_scheme; fastjet::JetDefinition *jetDef = NULL; // For hadronic collision, use hadronic Durham kT measure if(event[3].colType() != 0 || event[4].colType() != 0) jetDef = new fastjet::JetDefinition(fastjet::kt_algorithm, Rparam, recombScheme, strategy); // For e+e- collision, use e+e- Durham kT measure else jetDef = new fastjet::JetDefinition(fastjet::ee_kt_algorithm, recombScheme, strategy); // Fastjet input std::vector fjInputs; // Reset Fastjet input fjInputs.resize(0); // Loop over event record to decide what to pass to FastJet for (int i = 0; i < event.size(); ++i) { // (Final state && coloured+photons) only! if ( !event[i].isFinal() || event[i].isLepton() || event[i].id() == 23 || abs(event[i].id()) == 24 || abs(event[i].y()) > yPartonMax) continue; // Store as input to Fastjet fjInputs.push_back( fastjet::PseudoJet (event[i].px(), event[i].py(), event[i].pz(),event[i].e() ) ); } // Do nothing for empty input if (int(fjInputs.size()) == 0) { delete jetDef; return 0.0; } // Run Fastjet algorithm fastjet::ClusterSequence clustSeq(fjInputs, *jetDef); // Extract kT of first clustering double pTFirst = sqrt(clustSeq.exclusive_dmerge_max(nJetMin-1)); delete jetDef; // Return kT return pTFirst; } //========================================================================== // Class for user interaction with the merging class MyMergingHooks : public MergingHooks { private: public: // Default constructor MyMergingHooks(); // Destructor ~MyMergingHooks(); // Functional definition of the merging scale virtual double tmsDefinition( const Event& event); // Function to dampen weights calculated from histories with lowest // multiplicity reclustered events that do not pass the ME cuts virtual double dampenIfFailCuts( const Event& inEvent ); // Helper function for tms definition double myKTdurham(const Particle& RadAfterBranch, const Particle& EmtAfterBranch, int Type, double D ); }; //-------------------------------------------------------------------------- // Constructor MyMergingHooks::MyMergingHooks() {} // Desctructor MyMergingHooks::~MyMergingHooks() {} //-------------------------------------------------------------------------- double MyMergingHooks::dampenIfFailCuts( const Event& inEvent ){ // Get pT for pure QCD 2->2 state double pT = 0.; for( int i=0; i < inEvent.size(); ++i) if(inEvent[i].isFinal() && inEvent[i].colType() != 0) { pT = sqrt(pow(inEvent[i].px(),2) + pow(inEvent[i].py(),2)); break; } // Veto history if lowest multiplicity event does not pass ME cuts if(pT < 10.) return 0.; return 1.; } //-------------------------------------------------------------------------- // Definition of the merging scale double MyMergingHooks::tmsDefinition( const Event& event){ // Cut only on QCD partons! // Count particle types int nFinalColoured = 0; int nFinalNow =0; for( int i=0; i < event.size(); ++i) { if(event[i].isFinal()){ if(event[i].id() != 23 && abs(event[i].id()) != 24) nFinalNow++; if( event[i].colType() != 0) nFinalColoured++; } } // Use MergingHooks in-built functions to get information on the hard process int nLeptons = nHardOutLeptons(); int nQuarks = nHardOutPartons(); int nResNow = nResInCurrent(); // Check if photons, electrons etc. have been produced. If so, do not veto if(nFinalNow - ( (nLeptons+nQuarks)/2 - nResNow)*2 != nFinalColoured){ // Sometimes, Pythia detaches the decay products even though no // resonance was put into the LHE file, to catch this, add another // if statement if(nFinalNow != nFinalColoured) return 0.; } // Check that one parton has been produced. If not (e.g. in MPI), do not veto int nMPI = infoPtr->nMPI(); if(nMPI > 1) return 0.; // Declare kT algorithm parameters double Dparam = 0.4; int kTtype = -1; // Declare final parton vector vector FinalPartPos; FinalPartPos.clear(); // Search event record for final state partons for (int i=0; i < event.size(); ++i) if(event[i].isFinal() && event[i].colType() != 0) FinalPartPos.push_back(i); // Find minimal Durham kT in event, using own function: Check // definition of separation int type = (event[3].colType() == 0 && event[4].colType() == 0) ? 1 : kTtype; // Find minimal kT double ktmin = event[0].e(); for(int i=0; i < int(FinalPartPos.size()); ++i){ double kt12 = ktmin; // Compute separation to the beam axis for hadronic collisions if(type == -1 || type == -2) { double temp = event[FinalPartPos[i]].pT(); kt12 = min(kt12, temp); } // Compute separation to other final state jets for(int j=i+1; j < int(FinalPartPos.size()); ++j) { double temp = kTdurham( event[FinalPartPos[i]], event[FinalPartPos[j]], type, Dparam); kt12 = min(kt12, temp); } // Keep the minimal Durham separation ktmin = min(ktmin,kt12); } // Return minimal Durham kT return ktmin; } //-------------------------------------------------------------------------- // Function to compute durham y separation from Particle input double MyMergingHooks::myKTdurham(const Particle& RadAfterBranch, const Particle& EmtAfterBranch, int Type, double D ){ // Declare return variable double ktdur; // Save 4-momenta of final state particles Vec4 jet1 = RadAfterBranch.p(); Vec4 jet2 = EmtAfterBranch.p(); if( Type == 1) { // Get angle between jets for e+e- collisions, make sure that // -1 <= cos(theta) <= 1 double costh; if (jet1.pAbs()*jet2.pAbs() <=0.) costh = 1.; else { costh = costheta(jet1,jet2); } // Calculate kt durham separation between jets for e+e- collisions ktdur = 2.0*min( pow(jet1.e(),2) , (pow(jet2.e(),2)) )*(1.0 - costh); } else if( Type == -1 ){ // Get delta_eta and cosh(Delta_eta) for hadronic collisions double eta1 = 0.5*log( (jet1.e() + jet1.pz()) / (jet1.e() - jet1.pz()) ); double eta2 = 0.5*log( (jet2.e() + jet2.pz()) / (jet2.e() - jet2.pz()) ); // Get delta_phi and cos(Delta_phi) for hadronic collisions double pt1 = sqrt( pow(jet1.px(),2) + pow(jet1.py(),2) ); double pt2 = sqrt( pow(jet2.px(),2) + pow(jet2.py(),2) ); double cosdPhi = ( jet1.px()*jet2.px() + jet1.py()*jet2.py() ) / (pt1*pt2); double dPhi = acos( cosdPhi ); // Calculate kT durham like fastjet ktdur = min( pow(pt1,2),pow(pt2,2) ) * ( pow(eta1-eta2,2) + pow(dPhi,2) ) / pow(D,2); } else if( Type == -2 ){ // Get delta_eta and cosh(Delta_eta) for hadronic collisions double eta1 = 0.5*log( (jet1.e() + jet1.pz()) / (jet1.e() - jet1.pz()) ); double eta2 = 0.5*log( (jet2.e() + jet2.pz()) / (jet2.e() - jet2.pz()) ); double coshdEta = cosh( eta1 - eta2 ); // Get delta_phi and cos(Delta_phi) for hadronic collisions double pt1 = sqrt( pow(jet1.px(),2) + pow(jet1.py(),2) ); double pt2 = sqrt( pow(jet2.px(),2) + pow(jet2.py(),2) ); double cosdPhi = ( jet1.px()*jet2.px() + jet1.py()*jet2.py() ) / (pt1*pt2); // Calculate kT durham separation "SHERPA-like" ktdur = 2.0*min( pow(pt1,2),pow(pt2,2) ) * ( coshdEta - cosdPhi ) / pow(D,2); } else { ktdur = 0.0; } // Return kT return sqrt(ktdur); } //========================================================================== // Example main programm to illustrate merging int main( int argc, char* argv[] ){ // Check that correct number of command-line arguments if (argc != 4) { cerr << " Unexpected number of command-line arguments. \n You are" << " expected to provide the arguments \n" << " 1. Input file for settings \n" << " 2. Full name of the input LHE file (with path) \n" << " 3. Path for output histogram files \n" << " Program stopped. " << endl; return 1; } Pythia pythia; // Input parameters: // 1. Input file for settings // 2. Path to input LHE file // 3. OUtput histogram path pythia.readFile(argv[1]); string iPath = string(argv[2]); string oPath = string(argv[3]); // Number of events int nEvent = pythia.mode("Main:numberOfEvents"); // Construct user inut for merging MergingHooks* myMergingHooks = new MyMergingHooks(); pythia.setMergingHooksPtr( myMergingHooks ); // For ISR regularisation off pythia.settings.forceParm("SpaceShower:pT0Ref",0.); // Declare histograms Hist histPTFirst("pT of first jet",100,0.,100.); Hist histPTSecond("pT of second jet",100,0.,100.); // Read in ME configurations pythia.init(iPath,false); if(pythia.flag("Main:showChangedSettings")) { pythia.settings.listChanged(); } // Start generation loop for( int iEvent=0; iEvent out // The main program contains no analysis; this is intended to happen later. // It therefore "never" has to be recompiled to handle different tasks. // WARNING: typically one needs 25 MB/100 events at the LHC. // Therefore large event samples may be impractical. #include "Pythia8/Pythia.h" #include "Pythia8/Pythia8ToHepMC.h" #include "HepMC/GenEvent.h" #include "HepMC/IO_GenEvent.h" using namespace Pythia8; int main(int argc, char* argv[]) { // Check that correct number of command-line arguments if (argc != 3) { cerr << " Unexpected number of command-line arguments. \n You are" << " expected to provide one input and one output file name. \n" << " Program stopped! " << endl; return 1; } // Check that the provided input name corresponds to an existing file. ifstream is(argv[1]); if (!is) { cerr << " Command-line file " << argv[1] << " was not found. \n" << " Program stopped! " << endl; return 1; } // Confirm that external files will be used for input and output. cout << "\n >>> PYTHIA settings will be read from file " << argv[1] << " <<< \n >>> HepMC events will be written to file " << argv[2] << " <<< \n" << endl; // Interface for conversion from Pythia8::Event to HepMC event. HepMC::Pythia8ToHepMC ToHepMC; // Specify file where HepMC events will be stored. HepMC::IO_GenEvent ascii_io(argv[2], std::ios::out); // Generator. Pythia pythia; // Read in commands from external file. pythia.readFile(argv[1]); // Extract settings to be used in the main program. int nEvent = pythia.mode("Main:numberOfEvents"); int nAbort = pythia.mode("Main:timesAllowErrors"); // Initialization. pythia.init(); // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate event. if (!pythia.next()) { // If failure because reached end of file then exit event loop. if (pythia.info.atEndOfFile()) { cout << " Aborted since reached end of Les Houches Event File\n"; break; } // First few failures write off as "acceptable" errors, then quit. if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Construct new empty HepMC event and fill it. // Units will be as chosen for HepMC build, but can be changed // by arguments, e.g. GenEvt( HepMC::Units::GEV, HepMC::Units::MM) HepMC::GenEvent* hepmcevt = new HepMC::GenEvent(); ToHepMC.fill_next_event( pythia, hepmcevt ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; // End of event loop. Statistics. } pythia.stat(); // Done. return 0; } pythia8-8.1.80.orig/examples/main16.cc0000644000175000017500000001112312217346164015555 0ustar sunsun// main16.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates (a) how to collect the analysis code in a separate class // and (b) how to provide the .cmnd filename on the command line // Once you have linked the main program you can run it with a command line // ./main16.exe main16.cmnd > out16 #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // Put all your own analysis code in the myAnalysis class. class MyAnalysis { public: // Constructor can be empty. MyAnalysis() {} // Initialization actions. void init(); // Analysis of each new event. void analyze(Event& event); // Show final results. void finish(); private: // Declare variables and objects that span init - analyze - finish. int nEvt; Hist brH, yH, etaChg, mult; }; //-------------------------------------------------------------------------- // The initialization code. void MyAnalysis::init() { // Initialize counter for number of events. nEvt = 0; // Book histograms. brH.book("Higgs branching ratios by flavour", 30, -0.5, 29.5); yH.book("Higgs rapidity", 100, -10., 10.); etaChg.book("charged pseudorapidity", 100, -10., 10.); mult.book( "charged multiplicity", 100, -0.5, 799.5); } //-------------------------------------------------------------------------- // The event analysis code. void MyAnalysis::analyze(Event& event) { // Increase counter. ++nEvt; // Find latest copy of Higgs and plot its rapidity. int iH = 0; for (int i = 0; i < event.size(); ++i) if (event[i].id() == 25) iH = i; yH.fill( event[iH].y() ); // Plot flavour of decay channel. int idDau1 = event[ event[iH].daughter1() ].idAbs(); int idDau2 = event[ event[iH].daughter2() ].idAbs(); int iChan = 29; if (idDau2 == idDau1 && idDau1 < 25) iChan = idDau1; if (min( idDau1, idDau2) == 22 && max( idDau1, idDau2) == 23) iChan = 26; brH.fill( iChan); // Plot pseudorapidity distribution. Sum up charged multiplicity. int nChg = 0; for (int i = 0; i < event.size(); ++i) if (event[i].isFinal() && event[i].isCharged()) { etaChg.fill( event[i].eta() ); ++nChg; } mult.fill( nChg ); } //-------------------------------------------------------------------------- // The finishing code. void MyAnalysis::finish() { // Normalize histograms. double binFactor = 5. / nEvt; yH *= binFactor; etaChg *= binFactor; // Print histograms. cout << brH << yH << etaChg << mult; } //========================================================================== // You should not need to touch the main program: its actions are // determined by the .cmnd file and the rest belongs in MyAnalysis. int main(int argc, char* argv[]) { // Check that correct number of command-line arguments if (argc != 2) { cerr << " Unexpected number of command-line arguments. \n" << " You are expected to provide a file name and nothing else. \n" << " Program stopped! " << endl; return 1; } // Check that the provided file name corresponds to an existing file. ifstream is(argv[1]); if (!is) { cerr << " Command-line file " << argv[1] << " was not found. \n" << " Program stopped! " << endl; return 1; } // Confirm that external file will be used for settings.. cout << " PYTHIA settings will be read from file " << argv[1] << endl; // Declare generator. Read in commands from external file. Pythia pythia; pythia.readFile(argv[1]); // Initialization. pythia.init(); // Declare user analysis class. Do initialization part of it. MyAnalysis myAnalysis; myAnalysis.init(); // Read in number of event and maximal number of aborts. int nEvent = pythia.mode("Main:numberOfEvents"); int nAbort = pythia.mode("Main:timesAllowErrors"); bool hasPL = pythia.flag("PartonLevel:all"); // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if too many failures. if (!pythia.next()) { if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // User Analysis of current event. myAnalysis.analyze( (hasPL ? pythia.event : pythia.process) ); // End of event loop. } // Final statistics. pythia.stat(); // User finishing. myAnalysis.finish(); // Done. return 0; } pythia8-8.1.80.orig/examples/main25.cc0000644000175000017500000000431612217346165015564 0ustar sunsun// main25.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how Les Houches Event File input can be used in Pythia8. // Here the very few events are generated with MadGraph, and illustrate // more complicated colour topologies. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator Pythia pythia; // Stick with default values, so do not bother with a separate file // for changes. However, do one change, to show readString in action. pythia.readString("PartonLevel:ISR = off"); pythia.readString("PartonLevel:FSR = off"); pythia.readString("PartonLevel:MPI = off"); pythia.readString("HadronLevel:Hadronize = on"); // Initialize Les Houches Event File run. pythia.readString("Beams:frameType = 4"); pythia.readString("Beams:LHEF = main25.lhe"); pythia.init(); // Book histogram. Hist nCharged("charged particle multiplicity",100,-0.5,399.5); // Allow for possibility of a few faulty events. int nAbort = 10; int iAbort = 0; // Begin event loop; generate until none left in input file. for (int iEvent = 0; ; ++iEvent) { cout << endl << "Begin event # " << iEvent << endl; // Generate events, and check whether generation failed. if (!pythia.next()) { // If failure because reached end of file then exit event loop. if (pythia.info.atEndOfFile()) break; // First few failures write off as "acceptable" errors, then quit. if (++iAbort < nAbort) continue; break; } // Sum up final charged multiplicity and fill in histogram. int nChg = 0; for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].isFinal() && pythia.event[i].isCharged()) ++nChg; nCharged.fill(nChg); // End of event loop. } // Give statistics. Print histogram. pythia.stat(); cout << nCharged; // Done. return 0; } pythia8-8.1.80.orig/examples/w_production_tree_0.lhe0000644000175000017500000053270712217346210020627 0ustar sunsun
      # MG version : 5.1.5.5 #************************************************************ #* MadGraph 5 * #* * #* * * * #* * * * * * #* * * * * 5 * * * * * #* * * * * * #* * * * #* * #* * #* VERSION 1.5.5 2012-11-18 * #* * #* The MadGraph Development Team - Please visit us at * #* https://server06.fynu.ucl.ac.be/projects/madgraph * #* * #************************************************************ #* * #* Command File for MadGraph 5 * #* * #* run as ./bin/mg5 filename * #* * #************************************************************ set group_subprocesses Auto set ignore_six_quark_processes False set gauge unitary set complex_mass_scheme False import model sm define p = g u c d s u~ c~ d~ s~ define j = g u c d s u~ c~ d~ s~ define l+ = e+ mu+ define l- = e- mu- define vl = ve vm vt define vl~ = ve~ vm~ vt~ # Specify process(es) to run generate p p > w+ , w+ > e+ ve QED=2 @1 add process p p > w- , w- > e- ve~ QED=2 @2 # Output processes to MadEvent directory output -f #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # proc_card.dat * #********************************************************************* # * # This Files is generated by MADGRAPH 5 * # * # WARNING: This Files is generated for MADEVENT (compatibility issue)* # This files is NOT a valid MG4 proc_card.dat * # Running this in MG4 will NEVER reproduce the result of MG5* # * #********************************************************************* #********************************************************************* # Process(es) requested : mg2 input * #********************************************************************* # Begin PROCESS # This is TAG. Do not modify this line p p > w+ , w+ > e+ ve @1 #Process # Be carefull the coupling are here in MG5 convention QED=2 end_coup # End the couplings input done # this tells MG there are no more procs # End PROCESS # This is TAG. Do not modify this line #********************************************************************* # Model information * #********************************************************************* # Begin MODEL # This is TAG. Do not modify this line sm # End MODEL # This is TAG. Do not modify this line #********************************************************************* # Start multiparticle definitions * #********************************************************************* # Begin MULTIPARTICLES # This is TAG. Do not modify this line # End MULTIPARTICLES # This is TAG. Do not modify this line ###################################################################### ## PARAM_CARD AUTOMATICALY GENERATED BY MG5 FOLLOWING UFO MODEL #### ###################################################################### ## ## ## Width set on Auto will be computed following the information ## ## present in the decay.py files of the model. By default, ## ## this is only 1->2 decay modes. ## ## ## ###################################################################### ################################### ## INFORMATION FOR MASS ################################### Block mass 5 4.700000e+00 # MB 6 1.730000e+02 # MT 15 1.777000e+00 # MTA 23 9.118800e+01 # MZ 25 1.200000e+02 # MH ## Not dependent paramater. ## Those values should be edited following the ## analytical expression. MG5 ignore those values ## but they are important for interfacing the output of MG5 ## to external program such as Pythia. 1 0.000000 # d : 0.0 2 0.000000 # u : 0.0 3 0.000000 # s : 0.0 4 0.000000 # c : 0.0 11 0.000000 # e- : 0.0 12 0.000000 # ve : 0.0 13 0.000000 # mu- : 0.0 14 0.000000 # vm : 0.0 16 0.000000 # vt : 0.0 21 0.000000 # g : 0.0 22 0.000000 # a : 0.0 24 80.419002 # w+ : cmath.sqrt(MZ__exp__2/2. + cmath.sqrt(MZ__exp__4/4. - (aEW*cmath.pi*MZ__exp__2)/(Gf*sqrt__2))) ################################### ## INFORMATION FOR SMINPUTS ################################### Block sminputs 1 1.325070e+02 # aEWM1 2 1.166390e-05 # Gf 3 1.180000e-01 # aS ################################### ## INFORMATION FOR YUKAWA ################################### Block yukawa 5 4.200000e+00 # ymb 6 1.645000e+02 # ymt 15 1.777000e+00 # ymtau ################################### ## INFORMATION FOR DECAY ################################### DECAY 6 1.491500e+00 # WT DECAY 23 2.441404e+00 # WZ DECAY 24 2.047600e+00 # WW DECAY 25 5.753088e-03 # WH ## Not dependent paramater. ## Those values should be edited following the ## analytical expression. MG5 ignore those values ## but they are important for interfacing the output of MG5 ## to external program such as Pythia. DECAY 1 0.000000 # d : 0.0 DECAY 2 0.000000 # u : 0.0 DECAY 3 0.000000 # s : 0.0 DECAY 4 0.000000 # c : 0.0 DECAY 5 0.000000 # b : 0.0 DECAY 11 0.000000 # e- : 0.0 DECAY 12 0.000000 # ve : 0.0 DECAY 13 0.000000 # mu- : 0.0 DECAY 14 0.000000 # vm : 0.0 DECAY 15 0.000000 # ta- : 0.0 DECAY 16 0.000000 # vt : 0.0 DECAY 21 0.000000 # g : 0.0 DECAY 22 0.000000 # a : 0.0 #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # run_card.dat * # * # This file is used to set the parameters of the run. * # * # Some notation/conventions: * # * # Lines starting with a '# ' are info or comments * # * # mind the format: value = variable ! comment * #********************************************************************* # #******************* # Running parameters #******************* # #********************************************************************* # Tag name for the run (one word) * #********************************************************************* tag_1 = run_tag ! name of the run #********************************************************************* # Run to generate the grid pack * #********************************************************************* .false. = gridpack !True = setting up the grid pack #********************************************************************* # Number of events and rnd seed * # Warning: Do not generate more than 1M events in a single run * # If you want to run Pythia, avoid more than 50k events in a run. * #********************************************************************* 1000 = nevents ! Number of unweighted events requested 405 = iseed ! rnd seed (0=assigned automatically=default)) #********************************************************************* # Collider type and energy * # lpp: 0=No PDF, 1=proton, -1=antiproton, 2=photon from proton, * # 3=photon from electron * #********************************************************************* 1 = lpp1 ! beam 1 type 1 = lpp2 ! beam 2 type 3500 = ebeam1 ! beam 1 total energy in GeV 3500 = ebeam2 ! beam 2 total energy in GeV #********************************************************************* # Beam polarization from -100 (left-handed) to 100 (right-handed) * #********************************************************************* 0 = polbeam1 ! beam polarization for beam 1 0 = polbeam2 ! beam polarization for beam 2 #********************************************************************* # PDF CHOICE: this automatically fixes also alpha_s and its evol. * #********************************************************************* 'lhapdf' = pdlabel ! PDF set 10042 = lhaid ! PDF set cteq6m #********************************************************************* # Renormalization and factorization scales * #********************************************************************* T = fixed_ren_scale ! if .true. use fixed ren scale T = fixed_fac_scale ! if .true. use fixed fac scale 91.1880 = scale ! fixed ren scale 80.4 = dsqrt_q2fact1 ! fixed fact scale for pdf1 80.4 = dsqrt_q2fact2 ! fixed fact scale for pdf2 1 = scalefact ! scale factor for event-by-event scales #********************************************************************* # Matching - Warning! ickkw > 1 is still beta #********************************************************************* 0 = ickkw ! 0 no matching, 1 MLM, 2 CKKW matching 1 = highestmult ! for ickkw=2, highest mult group 1 = ktscheme ! for ickkw=1, 1 Durham kT, 2 Pythia pTE 1 = alpsfact ! scale factor for QCD emission vx F = chcluster ! cluster only according to channel diag F = pdfwgt ! for ickkw=1, perform pdf reweighting #********************************************************************* # Automatic ptj and mjj cuts if xqcut > 0 # (turn off for VBF and single top processes) #********************************************************** F = auto_ptj_mjj ! Automatic setting of ptj and mjj #********************************************************** # #********************************** # BW cutoff (M+/-bwcutoff*Gamma) #********************************** 5 = bwcutoff ! (M+/-bwcutoff*Gamma) #********************************************************** # Apply pt/E/eta/dr/mij cuts on decay products or not # (note that etmiss/ptll/ptheavy/ht/sorted cuts always apply) #********************************************************** F = cut_decays ! Cut decay products #************************************************************* # Number of helicities to sum per event (0 = all helicities) # 0 gives more stable result, but longer run time (needed for # long decay chains e.g.). # Use >=2 if most helicities contribute, e.g. pure QCD. #************************************************************* 0 = nhel ! Number of helicities used per event #******************* # Standard Cuts #******************* # #********************************************************************* # Minimum and maximum pt's (for max, -1 means no cut) * #********************************************************************* 5 = ptj ! minimum pt for the jets 0 = ptb ! minimum pt for the b 0 = pta ! minimum pt for the photons 0 = ptl ! minimum pt for the charged leptons 0 = misset ! minimum missing Et (sum of neutrino's momenta) 0 = ptheavy ! minimum pt for one heavy final state 0 = ptonium ! minimum pt for the quarkonium states -1 = ptjmax ! maximum pt for the jets -1 = ptbmax ! maximum pt for the b -1 = ptamax ! maximum pt for the photons -1 = ptlmax ! maximum pt for the charged leptons -1 = missetmax ! maximum missing Et (sum of neutrino's momenta) #********************************************************************* # Minimum and maximum E's (in the lab frame) * #********************************************************************* 0 = ej ! minimum E for the jets 0 = eb ! minimum E for the b 0 = ea ! minimum E for the photons 0 = el ! minimum E for the charged leptons -1 = ejmax ! maximum E for the jets -1 = ebmax ! maximum E for the b -1 = eamax ! maximum E for the photons -1 = elmax ! maximum E for the charged leptons #********************************************************************* # Maximum and minimum absolute rapidity (for max, -1 means no cut) * #********************************************************************* -1 = etaj ! max rap for the jets -1 = etab ! max rap for the b -1 = etaa ! max rap for the photons -1 = etal ! max rap for the charged leptons -1 = etaonium ! max rap for the quarkonium states 0 = etajmin ! min rap for the jets 0 = etabmin ! min rap for the b 0 = etaamin ! min rap for the photons 0 = etalmin ! main rap for the charged leptons #********************************************************************* # Minimum and maximum DeltaR distance * #********************************************************************* 1d-2 = drjj ! min distance between jets 0 = drbb ! min distance between b's 0 = drll ! min distance between leptons 0 = draa ! min distance between gammas 0 = drbj ! min distance between b and jet 0 = draj ! min distance between gamma and jet 0 = drjl ! min distance between jet and lepton 0 = drab ! min distance between gamma and b 0 = drbl ! min distance between b and lepton 0 = dral ! min distance between gamma and lepton -1 = drjjmax ! max distance between jets -1 = drbbmax ! max distance between b's -1 = drllmax ! max distance between leptons -1 = draamax ! max distance between gammas -1 = drbjmax ! max distance between b and jet -1 = drajmax ! max distance between gamma and jet -1 = drjlmax ! max distance between jet and lepton -1 = drabmax ! max distance between gamma and b -1 = drblmax ! max distance between b and lepton -1 = dralmax ! maxdistance between gamma and lepton #********************************************************************* # Minimum and maximum invariant mass for pairs * #********************************************************************* 5.0 = mmjj ! min invariant mass of a jet pair 0 = mmbb ! min invariant mass of a b pair 0 = mmaa ! min invariant mass of gamma gamma pair 0 = mmll ! min invariant mass of l+l- (same flavour) lepton pair -1 = mmjjmax ! max invariant mass of a jet pair -1 = mmbbmax ! max invariant mass of a b pair -1 = mmaamax ! max invariant mass of gamma gamma pair -1 = mmllmax ! max invariant mass of l+l- (same flavour) lepton pair #********************************************************************* # Minimum and maximum invariant mass for all letpons * #********************************************************************* 0 = mmnl ! min invariant mass for all letpons (l+- and vl) -1 = mmnlmax ! max invariant mass for all letpons (l+- and vl) #********************************************************************* # Minimum and maximum pt for 4-momenta sum of leptons * #********************************************************************* 0 = ptllmin ! Minimum pt for 4-momenta sum of leptons(l and vl) -1 = ptllmax ! Maximum pt for 4-momenta sum of leptons(l and vl) #********************************************************************* # Inclusive cuts * #********************************************************************* 0 = xptj ! minimum pt for at least one jet 0 = xptb ! minimum pt for at least one b 0 = xpta ! minimum pt for at least one photon 0 = xptl ! minimum pt for at least one charged lepton #********************************************************************* # Control the pt's of the jets sorted by pt * #********************************************************************* 0 = ptj1min ! minimum pt for the leading jet in pt 0 = ptj2min ! minimum pt for the second jet in pt 0 = ptj3min ! minimum pt for the third jet in pt 0 = ptj4min ! minimum pt for the fourth jet in pt -1 = ptj1max ! maximum pt for the leading jet in pt -1 = ptj2max ! maximum pt for the second jet in pt -1 = ptj3max ! maximum pt for the third jet in pt -1 = ptj4max ! maximum pt for the fourth jet in pt 0 = cutuse ! reject event if fails any (0) / all (1) jet pt cuts #********************************************************************* # Control the pt's of leptons sorted by pt * #********************************************************************* 0 = ptl1min ! minimum pt for the leading lepton in pt 0 = ptl2min ! minimum pt for the second lepton in pt 0 = ptl3min ! minimum pt for the third lepton in pt 0 = ptl4min ! minimum pt for the fourth lepton in pt -1 = ptl1max ! maximum pt for the leading lepton in pt -1 = ptl2max ! maximum pt for the second lepton in pt -1 = ptl3max ! maximum pt for the third lepton in pt -1 = ptl4max ! maximum pt for the fourth lepton in pt #********************************************************************* # Control the Ht(k)=Sum of k leading jets * #********************************************************************* 0 = htjmin ! minimum jet HT=Sum(jet pt) -1 = htjmax ! maximum jet HT=Sum(jet pt) 0 = ihtmin !inclusive Ht for all partons (including b) -1 = ihtmax !inclusive Ht for all partons (including b) 0 = ht2min ! minimum Ht for the two leading jets 0 = ht3min ! minimum Ht for the three leading jets 0 = ht4min ! minimum Ht for the four leading jets -1 = ht2max ! maximum Ht for the two leading jets -1 = ht3max ! maximum Ht for the three leading jets -1 = ht4max ! maximum Ht for the four leading jets #********************************************************************* # WBF cuts * #********************************************************************* 0 = xetamin ! minimum rapidity for two jets in the WBF case 0 = deltaeta ! minimum rapidity for two jets in the WBF case #********************************************************************* # maximal pdg code for quark to be considered as a light jet * # (otherwise b cuts are applied) * #********************************************************************* 4 = maxjetflavor ! Maximum jet pdg code #********************************************************************* # Jet measure cuts * #********************************************************************* 2.0 = xqcut ! minimum kt jet measure between partons #********************************************************************* 0d0 = kt_durham ! minimum durham kt jet measure between partons 0.4 = d_parameter ! D parameter for hadronic kT F = do_kt_durham ! T: enable durham kt cut 15 = pt_pythia ! minimum pythia pt jet measure between partons 0 = njets_requested ! number of jets above the pythia pt cut F = do_pt_pythia ! T: enable pythia pt cut #********************************************************************* # Number of Events : 1000 # Integrated weight (pb) : .77489E+04 # Truncated wgt (pb) : .00000E+00 # Unit wgt : .77489E+01
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0.17374029245E+03 0.78126888996E+02 0. 0. 11 1 3 3 0 0 -0.33426492472E+02 -0.20134043763E+02 0.73587212912E+02 0.83293385220E+02 0.00000000000E+00 0. -1. -12 1 3 3 0 0 0.33426492472E+02 0.20134043763E+02 0.81596157451E+02 0.90446907233E+02 0.00000000000E+00 0. 1. 5 2 0.7748900E+01 0.8040000E+02 0.7957747E-01 0.1297830E+00 -2 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.82796144466E+02 0.82796144466E+02 0.00000000000E+00 0. 1. 1 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.20991858480E+02 0.20991858480E+02 0.00000000000E+00 0. -1. -24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.61804285986E+02 0.10378800295E+03 0.83379732485E+02 0. 0. 11 1 3 3 0 0 -0.18671527633E+02 -0.28465863399E+02 0.94719642999E+00 0.34056254995E+02 0.00000000000E+00 0. -1. -12 1 3 3 0 0 0.18671527633E+02 0.28465863399E+02 0.60857089556E+02 0.69731747952E+02 0.00000000000E+00 0. 1. 5 1 0.7748900E+01 0.8040000E+02 0.7957747E-01 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.14507825950E+02 0.14507825950E+02 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.10989263741E+03 0.10989263741E+03 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.95384811464E+02 0.12440046336E+03 0.79857454423E+02 0. 0. -11 1 3 3 0 0 -0.15279227815E+02 -0.32815073425E+02 -0.21439308541E+02 0.42070509828E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.15279227815E+02 0.32815073425E+02 -0.73945502923E+02 0.82329953535E+02 0.00000000000E+00 0. -1. 5 2 0.7748900E+01 0.8040000E+02 0.7957747E-01 0.1297830E+00 -2 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.23815101595E+02 0.23815101595E+02 0.00000000000E+00 0. 1. 1 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.72225949519E+02 0.72225949519E+02 0.00000000000E+00 0. -1. -24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.48410847924E+02 0.96041051115E+02 0.82947412874E+02 0. 0. 11 1 3 3 0 0 -0.94552434349E+01 -0.29618084122E+02 0.75762803513E+01 0.32000508737E+02 0.00000000000E+00 0. -1. -12 1 3 3 0 0 0.94552434349E+01 0.29618084122E+02 -0.55987128276E+02 0.64040542378E+02 0.00000000000E+00 0. 1. 5 1 0.7748900E+01 0.8040000E+02 0.7957747E-01 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.34774279113E+03 0.34774279113E+03 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.47085848384E+01 0.47085848384E+01 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.34303420629E+03 0.35245137597E+03 0.80929016650E+02 0. 0. -11 1 3 3 0 0 -0.36423706288E+02 -0.10600316872E+01 0.94891863416E+02 0.10164780268E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.36423706288E+02 0.10600316872E+01 0.24814234287E+03 0.25080357329E+03 0.00000000000E+00 0. -1. 5 1 0.7748900E+01 0.8040000E+02 0.7957747E-01 0.1297830E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.28655595845E+02 0.28655595845E+02 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.57801864173E+02 0.57801864173E+02 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.29146268328E+02 0.86457460018E+02 0.81396482942E+02 0. 0. -11 1 3 3 0 0 -0.32487478391E+02 -0.30488386207E+00 0.11462500849E+02 0.34451678219E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.32487478391E+02 0.30488386207E+00 -0.40608769178E+02 0.52005781799E+02 0.00000000000E+00 0. -1. 5 1 0.7748900E+01 0.8040000E+02 0.7957747E-01 0.1297830E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.18652832683E+02 0.18652832683E+02 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.83004085098E+02 0.83004085098E+02 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.64351252415E+02 0.10165691778E+03 0.78695903613E+02 0. 0. -11 1 3 3 0 0 -0.19513332204E+02 -0.27059375156E+02 -0.52249377865E+01 0.33768030627E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.19513332204E+02 0.27059375156E+02 -0.59126314629E+02 0.67888887155E+02 0.00000000000E+00 0. -1. 5 2 0.7748900E+01 0.8040000E+02 0.7957747E-01 0.1297830E+00 1 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.23805522586E+01 0.23805522586E+01 0.00000000000E+00 0. -1. -2 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.68585056640E+03 0.68585056640E+03 0.00000000000E+00 0. 1. -24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.68347001414E+03 0.68823111866E+03 0.80813442320E+02 0. 0. 11 1 3 3 0 0 -0.24946384749E+02 0.76684487255E+01 -0.79027540856E+02 0.83225473455E+02 0.00000000000E+00 0. -1. -12 1 3 3 0 0 0.24946384749E+02 -0.76684487255E+01 -0.60444247329E+03 0.60500564521E+03 0.00000000000E+00 0. 1.
      pythia8-8.1.80.orig/examples/main85.cmnd0000644000175000017500000000254012217346167016125 0ustar sunsun! main85.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. // Number of events generated Main:numberOfEvents = 1000 // Shower options HadronLevel:all = on PartonLevel:MPI = on // Core process for merging Merging:Process = pp>LEPTONS,NEUTRINOS // Maximal number of additional jets. Merging:nJetMax = 2 // Jet-separation merging Merging:doKTMerging = off Merging:doMGMerging = off Merging:doUserMerging = off Merging:doPTLundMerging = on // Merging scale value. Merging:TMS = 15 // Cut-based merging Merging:doCutBasedMerging = off // Merging scale values. Merging:QijMS = 0 Merging:pTiMS = 0 Merging:dRijMS = 0 // Switch off enforced rapidity ordering SpaceShower:rapidityOrder = off // Since CKKW-L is a tree-level merging method, both leading-order and // next-to-neading order PDFs are allowed. However, from parton shower // considerations, leading-order PDFs are preferred, since multiparton // interactions probe the incoming hadron at small momentum scales. // Example PDF files generated with CTEQ6M PDFs. PDF:useLHAPDF = on PDF:LHAPDFset = cteq6m.LHpdf SpaceShower:alphaSvalue = 0.118 TimeShower:alphaSvalue = 0.118 pythia8-8.1.80.orig/examples/main02.cc0000644000175000017500000000243112217346163015551 0ustar sunsun// main02.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. It fits on one slide in a talk. // It studies the pT_Z spectrum at the Tevatron. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator. Process selection. Tevatron initialization. Histogram. Pythia pythia; pythia.readString("Beams:idB = -2212"); pythia.readString("Beams:eCM = 1960."); pythia.readString("WeakSingleBoson:ffbar2gmZ = on"); pythia.readString("PhaseSpace:mHatMin = 80."); pythia.readString("PhaseSpace:mHatMax = 120."); pythia.init(); Hist pTZ("dN/dpTZ", 100, 0., 100.); // Begin event loop. Generate event. Skip if error. List first one. for (int iEvent = 0; iEvent < 1000; ++iEvent) { if (!pythia.next()) continue; // Loop over particles in event. Find last Z0 copy. Fill its pT. int iZ = 0; for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].id() == 23) iZ = i; pTZ.fill( pythia.event[iZ].pT() ); // End of event loop. Statistics. Histogram. Done. } pythia.stat(); cout << pTZ; return 0; } pythia8-8.1.80.orig/examples/main42.cc0000644000175000017500000000634612217346166015571 0ustar sunsun// main42.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Author: Mikhail Kirsanov, Mikhail.Kirsanov@cern.ch. // This program illustrates how a file with HepMC events // can be generated by Pythia8. // Input and output files are specified on the command line, e.g. like // ./main42.exe main42.cmnd hepmcout42.dat > out // The main program contains no analysis; this is intended to happen later. // It therefore "never" has to be recompiled to handle different tasks. // WARNING: typically one needs 25 MB/100 events at the LHC. // Therefore large event samples may be impractical. #include "Pythia8/Pythia.h" #include "Pythia8/Pythia8ToHepMC.h" #include "HepMC/GenEvent.h" #include "HepMC/IO_GenEvent.h" using namespace Pythia8; int main(int argc, char* argv[]) { // Check that correct number of command-line arguments if (argc != 3) { cerr << " Unexpected number of command-line arguments. \n You are" << " expected to provide one input and one output file name. \n" << " Program stopped! " << endl; return 1; } // Check that the provided input name corresponds to an existing file. ifstream is(argv[1]); if (!is) { cerr << " Command-line file " << argv[1] << " was not found. \n" << " Program stopped! " << endl; return 1; } // Confirm that external files will be used for input and output. cout << "\n >>> PYTHIA settings will be read from file " << argv[1] << " <<< \n >>> HepMC events will be written to file " << argv[2] << " <<< \n" << endl; // Interface for conversion from Pythia8::Event to HepMC event. HepMC::Pythia8ToHepMC ToHepMC; // Specify file where HepMC events will be stored. HepMC::IO_GenEvent ascii_io(argv[2], std::ios::out); // Generator. Pythia pythia; // Read in commands from external file. pythia.readFile(argv[1]); // Extract settings to be used in the main program. int nEvent = pythia.mode("Main:numberOfEvents"); int nAbort = pythia.mode("Main:timesAllowErrors"); // Initialization. pythia.init(); // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate event. if (!pythia.next()) { // If failure because reached end of file then exit event loop. if (pythia.info.atEndOfFile()) { cout << " Aborted since reached end of Les Houches Event File\n"; break; } // First few failures write off as "acceptable" errors, then quit. if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Construct new empty HepMC event and fill it. // Units will be as chosen for HepMC build, but can be changed // by arguments, e.g. GenEvt( HepMC::Units::GEV, HepMC::Units::MM) HepMC::GenEvent* hepmcevt = new HepMC::GenEvent(); ToHepMC.fill_next_event( pythia, hepmcevt ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; // End of event loop. Statistics. } pythia.stat(); // Done. return 0; } pythia8-8.1.80.orig/examples/main24.cmnd0000644000175000017500000000410012217346165016106 0ustar sunsun! main24.cmnd ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! 1) Settings used in the main program. Main:numberOfEvents = 10000 ! number of events to generate Main:timesAllowErrors = 3 ! how many aborts before run stops ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showChangedParticleData = off ! list changed particle data Next:numberCount = 500 ! print message every n events Next:numberShowInfo = 2 ! print event information n times Next:numberShowProcess = 2 ! print process record n times Next:numberShowEvent = 2 ! print event record n times ! 3) Beam parameter settings. Values below agree with default ones. Beams:idA = 2212 ! first beam, p = 2212, pbar = -2212 Beams:idB = 2212 ! second beam, p = 2212, pbar = -2212 Beams:eCM = 10000. ! CM energy of collision ! 4) Read SLHA spectrum SLHA:file = cmssm.spc ! Sample SLHA1 spectrum for CMSSM-10.1.1 #SLHA:file = sps1aWithDecays.spc ! Older example including DECAY tables ! 5) Process selection SUSY:all = on ! Switches on ALL (~400) SUSY processes #SUSY:gg2gluinogluino = on #SUSY:qqbar2gluinogluino = on #SUSY:qg2squarkgluino = on #SUSY:gg2squarkantisquark = on #SUSY:qqbar2squarkantisquark = on #SUSY:qq2squarksquark = on #SUSY:qqbar2chi0chi0 = on #SUSY:qqbar2chi+-chi0 = on #SUSY:qqbar2chi+chi- = on #SUSY:qg2chi0squark = on #SUSY:qg2chi+-squark = on ! Optionally select only specific sparticle codes in the final state #SUSY:idA = 2000001 ! 0: all #SUSY:idB = 2000001 ! 0: all ! 6) Settings for the event generation process in the Pythia8 library. PartonLevel:MPI = off ! no multiparton interactions PartonLevel:ISR = off ! no initial-state radiation PartonLevel:FSR = off ! no final-state radiation HadronLevel:Hadronize = off ! no hadronization pythia8-8.1.80.orig/examples/configure0000755000175000017500000004072412217346163016072 0ustar sunsun#!/bin/sh # # Configuration script, to be run before making examples # # Author: M. Kirsanov # # User-changeable part ------------------------------- # #LCG platform. Can be needed if external libraries are specified if [ x$MYLCGPLATFORM = x ]; then export MYLCGPLATFORM=x86_64-slc5-gcc43-opt fi # Defaults export COMPMODE=OPT export PYTHIA8LOCATION=.. # check arguments for arg in $* ; do if [ "x$arg" = "x--enable-debug" ] ; then COMPMODE=DBG elif [ "x$arg" = "x--enable-shared" ] ; then SHAREDLIBS=yes elif [ "x$arg" = "x--help" ] ; then echo "Usage: ./configure [options] , where options are:" echo "--help : prints this help" echo "--enable-debug : turns on debugging flags and turns off optimization" echo "--enable-shared : use shared library (not yet implemented) (default no)" echo "--lcgplatform=name : LCG platform name, default is slc4_ia32_gcc34" echo "--with-pythia8=p8path : path to pythia8 installation dir to find libs, includes and pars (default is ..)" echo "--with-lhapdf=lhapdfpath : path to LHAPDF libraries dir (LHAPDF must be version 5.3 or higher)" echo "--with-lhapdfversion=v : LHAPDF version (simplified alternative when using CERN AFS MCGenerators, e.g. =5.5.1.a)" echo "--with-lhapdflibname=n : lhapdf library name line (default is -lLHAPDF)" echo "--with-lhapdfsets=path : path to LHAPDF data (default is lhapdfpath/../PDFsets, CERN AFS default is lhapdfpath/../../../share/PDFsets)" echo "--with-fastjet=path : path to fastjet (default = /usr/local)" echo "--with-fastjetversion=v : fastjet version (simplified alternative when using CERN AFS external, e.g. =2.3.3)" exit elif [ x`echo x${arg} | grep "="` != x ] ; then option=`echo ${arg} | awk -F = '{print $1}'` value=`echo ${arg} | awk -F = '{print $2}'` if [ "x${option}" = "x--lcgplatform" ] ; then MYLCGPLATFORM=${value} elif [ "x${option}" = "x--with-pythia8" ] ; then PYTHIA8LOCATION=${value} elif [ "x${option}" = "x--with-lhapdfversion" ] ; then LHAPDFVERSION=${value} elif [ "x${option}" = "x--with-lhapdf" ] ; then LHAPDFLOCATION=${value} elif [ "x${option}" = "x--with-lhapdflibname" ] ; then LHAPDFLIBNAME=${value} elif [ "x${option}" = "x--with-lhapdfsets" ] ; then LHAPDFSETSLOCATION=${value} elif [ "x${option}" = "x--with-fastjetversion" ] ; then FASTJETVERSION=${value} elif [ "x${option}" = "x--with-fastjet" ] ; then FASTJETLOCATION=${value} else echo "${arg}: wrong option. Ignored." >&2 fi else echo "${arg}: wrong option. Ignored." >&2 fi done echo compilation mode is $COMPMODE # LHAPDF location # The default values here correspond to CERN AFS (but you may want to change # the version and/or platform). if [ x${LHAPDFLOCATION} != x ]; then if [ x${LHAPDFSETSLOCATION} = x ]; then export LHAPDFSETSLOCATION=${LHAPDFLOCATION}/../PDFsets if [ ! -d ${LHAPDFSETSLOCATION} ]; then export LHAPDFSETSLOCATION=${LHAPDFLOCATION}/../../share/lhapdf/PDFsets fi if [ ! -d ${LHAPDFSETSLOCATION} ]; then export LHAPDFSETSLOCATION=${LHAPDFLOCATION}/../share/lhapdf/PDFsets fi if [ ! -d ${LHAPDFSETSLOCATION} ]; then export LHAPDFSETSLOCATION=${LHAPDFLOCATION}/../../../share/lhapdf/PDFsets fi fi fi if [ x${LHAPDFVERSION} = x ]; then export LHAPDFVERSION=5.7.0 else if [ x${LHAPDFLOCATION} = x ]; then export LHAPDFLOCATION=/afs/cern.ch/sw/lcg/external/MCGenerators/lhapdf/${LHAPDFVERSION}/${MYLCGPLATFORM}/lib/archive if [ x${LHAPDFSETSLOCATION} = x ]; then export LHAPDFSETSLOCATION=/afs/cern.ch/sw/lcg/external/MCGenerators/lhapdf/${LHAPDFVERSION}/share/PDFsets fi fi fi if [ x${LHAPDFLOCATION} = x ]; then export LHAPDFLOCATION=/afs/cern.ch/sw/lcg/external/MCGenerators/lhapdf/${LHAPDFVERSION}/${MYLCGPLATFORM}/lib/archive fi if [ x${LHAPDFLIBNAME} = x ]; then export LHAPDFLIBNAME="-lLHAPDF" fi if [ x${LHAPDFSETSLOCATION} = x ]; then export LHAPDFSETSLOCATION=/afs/cern.ch/sw/lcg/external/MCGenerators/lhapdf/${LHAPDFVERSION}/share/PDFsets fi # Fastjet location if [ x${FASTJETVERSION} != x ]; then export FASTJETLOCATION=/afs/cern.ch/sw/lcg/external/fastjet/${FASTJETVERSION}/${MYLCGPLATFORM} fi if [ x${FASTJETLOCATION} = x ]; then export FASTJETLOCATION=/usr/local fi # # User-changeable part, experts ----------------------------- # # export FFLAGS_OPT="-O2 -Wuninitialized" # -Wuninitialized outputs many irrelevant warnings and therefore obscurs export FFLAGS_OPT="-O2" export FFLAGS_DBG=-g export CFLAGS_OPT=-O2 export CFLAGS_DBG=-g export CXXFLAGS_OPT="-O2 -ansi -pedantic -W -Wall" export CXXFLAGS_DBG="-g -ansi -pedantic -W -Wall" # # Find platform. # export ARCH0="`uname`" export ARCH=${ARCH0} export theGcc=`g++ --version | head -n 1 | awk '{print$3}' | awk -F . '{print $1}'` if [ ${theGcc} = 4 ]; then export ARCH=${ARCH}-gcc4 fi echo Platform is $ARCH #default platform settings: if [ x$FC = x ]; then export FC=g77 fi if [ x$CC = x ]; then export CC=gcc fi export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" export FLIBS="-lfrtbegin -lg2c" if [ ${COMPMODE} = OPT ]; then export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" fi if [ ${COMPMODE} = DBG ]; then export FFLAGS="${FFLAGS_DBG}" export CFLAGS="${CFLAGS_DBG}" export CXXFLAGS="${CXXFLAGS_DBG}" fi if [ $ARCH = Linux ]; then if [ x$FC = x ]; then export FC=g77 fi export FFLAGS="${FFLAGS_OPT} -Wno-globals" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" export FLIBS="-lfrtbegin -lg2c" if [ ${COMPMODE} = OPT ]; then export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" fi if [ ${COMPMODE} = DBG ]; then export FFLAGS="${FFLAGS_DBG} -Wno-globals" export CFLAGS="${CFLAGS_DBG}" export CXXFLAGS="${CXXFLAGS_DBG}" fi fi # Linux platform with gcc4: new Fortran90 compiler. if [ $ARCH = Linux-gcc4 ]; then if [ x$FC = x ]; then export FC=gfortran fi export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" export FLIBS="-lgfortran -lgfortranbegin" if [ ${COMPMODE} = OPT ]; then export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" fi if [ ${COMPMODE} = DBG ]; then export FFLAGS="${FFLAGS_DBG}" export CFLAGS="${CFLAGS_DBG}" export CXXFLAGS="${CXXFLAGS_DBG}" fi fi # Mac-OSX with gcc4 if [ $ARCH = Darwin-gcc4 ]; then if [ x$FC = x ]; then export FC=gfortran fi export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" export FLIBS="-lgfortran" if [ ${COMPMODE} = OPT ]; then export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" fi if [ ${COMPMODE} = DBG ]; then export FFLAGS="${FFLAGS_DBG}" export CFLAGS="${CFLAGS_DBG}" export CXXFLAGS="${CXXFLAGS_DBG}" fi fi # Mac-OSX with gcc3; is not tested if [ $ARCH = Darwin ]; then if [ x$FC = x ]; then export FC=g77 fi export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" export FLIBS="-lfrtbegin -lg2c" if [ ${COMPMODE} = OPT ]; then export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" fi if [ ${COMPMODE} = DBG ]; then export FFLAGS="${FFLAGS_DBG}" export CFLAGS="${CFLAGS_DBG}" export CXXFLAGS="${CXXFLAGS_DBG}" fi fi #Platform & opt/dbg - independent flags and variables: # # End of the user-changeable part --------------------------- # # Checks # if [ ! -d ${PYTHIA8LOCATION}/lib ]; then echo ERROR: pythia8 libraries not found at ${PYTHIA8LOCATION}/lib exit fi if [ $?LHAPDFLOCATION ]; then if [ x${LHAPDFLOCATION} != x ]; then if [ ! -d ${LHAPDFLOCATION} ]; then echo WARNING in LHAPDFLOCATION: directory ${LHAPDFLOCATION} does not exist echo ...so you cannot run main programs that use LHAPDF fi if [ ! -e ${LHAPDFLOCATION}/libLHAPDF.so ] && \ [ ! -e ${LHAPDFLOCATION}/libLHAPDF.dylib ] && \ [ ! -e ${LHAPDFLOCATION}/libLHAPDF.a ]; then echo WARNING in LHAPDFLOCATION: LHAPDF libraries are not found in ${LHAPDFLOCATION} echo "please specify path to the LHAPDF libraries directory (add /lib to the path?)" echo ...otherwise you cannot run main programs that use LHAPDF fi if [ ! -d ${LHAPDFSETSLOCATION} ]; then echo WARNING in LHAPDFSETSLOCATION: directory ${LHAPDFSETSLOCATION} does not exist echo ...so you cannot run main programs that use LHAPDF fi fi fi # Fastjet if [ -x ${FASTJETLOCATION}/bin/fastjet-config ]; then FASTJETVERSION1=`${FASTJETLOCATION}/bin/fastjet-config --version` echo Found fastjet version ${FASTJETVERSION1} at ${FASTJETLOCATION} else echo WARNING: FastJet not found, the corresponding examples will not work echo ...so you cannot run main programs that use FastJet export FASTJETLOCATION= fi rm -f config.mk echo SHELL = /bin/sh > config.mk #echo ARCH = ${ARCH} >> config.mk #echo MYLCGPLATFORM = ${MYLCGPLATFORM} >> config.mk #echo FC = ${FC} >> config.mk #echo CC = ${CC} >> config.mk #echo FFLAGS = ${FFLAGS} >> config.mk #echo CFLAGS = ${CFLAGS} >> config.mk #echo CXXFLAGS = ${CXXFLAGS} >> config.mk #echo FLIBS = ${FLIBS} >> config.mk # echo PYTHIA8LOCATION = ${PYTHIA8LOCATION} >> config.mk if [ x${LHAPDFVERSION} != x ]; then echo LHAPDFVERSION = ${LHAPDFVERSION} >> config.mk fi if [ x${LHAPDFLOCATION} != x ]; then echo LHAPDFLOCATION = ${LHAPDFLOCATION} >> config.mk fi if [ "x${LHAPDFLIBNAME}" != "x" ]; then echo "LHAPDFLIBNAME = ${LHAPDFLIBNAME}" >> config.mk fi # Fastjet if [ "x${FASTJETLOCATION}" != "x" ]; then echo "FASTJETLOCATION = ${FASTJETLOCATION}" >> config.mk fi # if [ ${PYTHIA8LOCATION} != .. ]; then if [ ! -e config.csh ]; then echo "#!/bin/csh" > config.csh echo "setenv PYTHIA8DATA ${PYTHIA8LOCATION}/xmldoc" >> config.csh echo "#!/bin/sh" > config.sh echo "export PYTHIA8DATA=${PYTHIA8LOCATION}/xmldoc" >> config.sh else echo "setenv PYTHIA8DATA ${PYTHIA8LOCATION}/xmldoc" >> config.csh echo "export PYTHIA8DATA=${PYTHIA8LOCATION}/xmldoc" >> config.sh fi fi # # For the moment we take archive libraries of lhapdf, so actions with # LD_LIBRARY_PATH are not needed, this is for the future. # Setting LHAPATH is always needed # Linux platforms: if [ $ARCH0 != Darwin ]; then if [ x${LHAPDFLOCATION} != x ]; then if [ ! -e config.csh ]; then echo "#!/bin/csh" > config.csh echo 'if( ! $?LD_LIBRARY_PATH ) then' >> config.csh echo " setenv LD_LIBRARY_PATH ${LHAPDFLOCATION}" >> config.csh echo "else" >> config.csh echo " setenv LD_LIBRARY_PATH" '${LD_LIBRARY_PATH}'":${LHAPDFLOCATION}" >> config.csh echo "endif" >> config.csh echo "setenv LHAPATH ${LHAPDFSETSLOCATION}" >> config.csh echo "#!/bin/sh" > config.sh echo 'if [ ! $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH=${LHAPDFLOCATION}" >> config.sh echo fi >> config.sh echo 'if [ $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH="'${LD_LIBRARY_PATH}'":${LHAPDFLOCATION}" >> config.sh echo fi >> config.sh echo "export LHAPATH=${LHAPDFSETSLOCATION}" >> config.sh else echo 'if( ! $?LD_LIBRARY_PATH ) then' >> config.csh echo " setenv LD_LIBRARY_PATH ${LHAPDFLOCATION}" >> config.csh echo "else" >> config.csh echo " setenv LD_LIBRARY_PATH" '${LD_LIBRARY_PATH}'":${LHAPDFLOCATION}" >> config.csh echo "endif" >> config.csh echo "setenv LHAPATH ${LHAPDFSETSLOCATION}" >> config.csh echo 'if [ ! $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH=${LHAPDFLOCATION}" >> config.sh echo fi >> config.sh echo 'if [ $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH="'${LD_LIBRARY_PATH}'":${LHAPDFLOCATION}" >> config.sh echo fi >> config.sh echo "export LHAPATH=${LHAPDFSETSLOCATION}" >> config.sh fi fi if [ x${FASTJETLOCATION} != x ]; then if [ ! -e config.csh ]; then echo "#!/bin/csh" > config.csh echo 'if( ! $?LD_LIBRARY_PATH ) then' >> config.csh echo " setenv LD_LIBRARY_PATH ${FASTJETLOCATION}/lib" >> config.csh echo "else" >> config.csh echo " setenv LD_LIBRARY_PATH" '${LD_LIBRARY_PATH}'":${FASTJETLOCATION}/lib" >> config.csh echo "endif" >> config.csh echo "#!/bin/sh" > config.sh echo 'if [ ! $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH=${FASTJETLOCATION}/lib" >> config.sh echo fi >> config.sh echo 'if [ $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH="'${LD_LIBRARY_PATH}'":${FASTJETLOCATION}/lib" >> config.sh echo fi >> config.sh else echo 'if( ! $?LD_LIBRARY_PATH ) then' >> config.csh echo " setenv LD_LIBRARY_PATH ${FASTJETLOCATION}/lib" >> config.csh echo "else" >> config.csh echo " setenv LD_LIBRARY_PATH" '${LD_LIBRARY_PATH}'":${FASTJETLOCATION}/lib" >> config.csh echo "endif" >> config.csh echo 'if [ ! $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH=${FASTJETLOCATION}/lib" >> config.sh echo fi >> config.sh echo 'if [ $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH="'${LD_LIBRARY_PATH}'":${FASTJETLOCATION}/lib" >> config.sh echo fi >> config.sh fi fi # Mac-OSX platforms: else if [ x${LHAPDFLOCATION} != x ]; then if [ ! -e config.csh ]; then echo "#!/bin/csh" > config.csh echo 'if( ! $?LD_LIBRARY_PATH ) then' >> config.csh echo " setenv LD_LIBRARY_PATH ${LHAPDFLOCATION}" >> config.csh echo "else" >> config.csh echo " setenv LD_LIBRARY_PATH" '${LD_LIBRARY_PATH}'":${LHAPDFLOCATION}" >> config.csh echo "endif" >> config.csh echo "setenv LHAPATH ${LHAPDFSETSLOCATION}" >> config.csh echo "#!/bin/sh" > config.sh echo 'if [ ! $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH=${LHAPDFLOCATION}" >> config.sh echo fi >> config.sh echo 'if [ $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH="'${LD_LIBRARY_PATH}'":${LHAPDFLOCATION}" >> config.sh echo fi >> config.sh echo "export LHAPATH=${LHAPDFSETSLOCATION}" >> config.sh else echo 'if( ! $?LD_LIBRARY_PATH ) then' >> config.csh echo " setenv LD_LIBRARY_PATH ${LHAPDFLOCATION}" >> config.csh echo "else" >> config.csh echo " setenv LD_LIBRARY_PATH" '${LD_LIBRARY_PATH}'":${LHAPDFLOCATION}" >> config.csh echo "endif" >> config.csh echo "setenv LHAPATH ${LHAPDFSETSLOCATION}" >> config.csh echo 'if [ ! $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH=${LHAPDFLOCATION}" >> config.sh echo fi >> config.sh echo 'if [ $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH="'${LD_LIBRARY_PATH}'":${LHAPDFLOCATION}" >> config.sh echo fi >> config.sh echo "export LHAPATH=${LHAPDFSETSLOCATION}" >> config.sh fi fi if [ x${FASTJETLOCATION} != x ]; then if [ ! -e config.csh ]; then echo "#!/bin/csh" > config.csh echo 'if( ! $?LD_LIBRARY_PATH ) then' >> config.csh echo " setenv LD_LIBRARY_PATH ${FASTJETLOCATION}/lib" >> config.csh echo "else" >> config.csh echo " setenv LD_LIBRARY_PATH" '${LD_LIBRARY_PATH}'":${FASTJETLOCATION}/lib" >> config.csh echo "endif" >> config.csh echo "#!/bin/sh" > config.sh echo 'if [ ! $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH=${FASTJETLOCATION}/lib" >> config.sh echo fi >> config.sh echo 'if [ $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH="'${LD_LIBRARY_PATH}'":${FASTJETLOCATION}/lib" >> config.sh echo fi >> config.sh else echo 'if( ! $?LD_LIBRARY_PATH ) then' >> config.csh echo " setenv LD_LIBRARY_PATH ${FASTJETLOCATION}/lib" >> config.csh echo "else" >> config.csh echo " setenv LD_LIBRARY_PATH" '${LD_LIBRARY_PATH}'":${FASTJETLOCATION}/lib" >> config.csh echo "endif" >> config.csh echo 'if [ ! $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH=${FASTJETLOCATION}/lib" >> config.sh echo fi >> config.sh echo 'if [ $?LD_LIBRARY_PATH ]; then' >> config.sh echo " export LD_LIBRARY_PATH="'${LD_LIBRARY_PATH}'":${FASTJETLOCATION}/lib" >> config.sh echo fi >> config.sh fi fi fi pythia8-8.1.80.orig/examples/w+_production_lhc_0.lhe0000644000175000017500000030017212217346207020504 0ustar sunsun
      # MG/ME version : 4.4.48 # madgraph version : 4.4.5 # template version : 2.4.25 # helas version : 3.8 # model version : sm_1.2.1 #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # proc_card.dat * # * # This file is used to generate the code for a specific process. * # Some notation/conventions: * # * # 0. Do not modify the TAGS and their order. * # 1. hash/pound is a comment. * # 2. The number after the @ is used as an identifier for the class * # of processes. It can be any positive integer. * # 3. The number of lines for the max couplings depends on how many * # different classes of couplings are present in the model * # In the SM these are just two: QED (which include EW) and QCD * # 4. Write "end_coup" after the couplings list, * # to tell MG that the couplings input is over. * # 5. Write "done" after the proc list to * # to tell MG that the proc input is over. * # 6. Some model names available at present are: * # sm = Standard Model * # smckm = Standard Model with Cabibbo matrix * # mssm = Minimal Supersymmetric Standard Model * # 2hdm = Generic Two Higgs Doublet model * # heft = Higgs EFT (+Standard Model) * # usrmod = User Model * # 7. Don't leave spaces between the particles name in the * # definition of the multiparticles. * #********************************************************************* #********************************************************************* # Process(es) requested : mg2 input * #********************************************************************* # Begin PROCESS # This is TAG. Do not modify this line pp>e+ve @1 # First Process QCD=99 # Max QCD couplings QED=2 # Max QED couplings end_coup # End the couplings input done # this tells MG there are no more procs # End PROCESS # This is TAG. Do not modify this line #********************************************************************* # Model information * #********************************************************************* # Begin MODEL # This is TAG. Do not modify this line sm # End MODEL # This is TAG. Do not modify this line #********************************************************************* # Start multiparticle definitions * #********************************************************************* # Begin MULTIPARTICLES # This is TAG. Do not modify this line P uu~dd~cc~ss~g J uu~dd~cc~ss~g L+ e+mu+ L- e-mu- vl vevm vl~ ve~vm~ # End MULTIPARTICLES # This is TAG. Do not modify this line #****************************************************************** # MadGraph/MadEvent * #****************************************************************** # Les Houches friendly file for the SM parameters of MadGraph * # Spectrum and decay widths produced by SMCalc * #****************************************************************** #*Please note the following IMPORTANT issues: * # * #0. REFRAIN from editing this file by hand! Some of the parame- * # ters are not independent * # (such as G_Fermi, alpha_em, sin(theta_W),MZ,MW) and serious * # problems might be encountered (such as violation of unitarity * # or gauge invariance). Always use a calculator. * # * #1. alpha_S(MZ) has been used in the calculation of the parameters* # but, for consistency, it will be reset by madgraph to the * # value expected IF the pdfs for collisions with hadrons are * # used. This value is KEPT by madgraph when no pdf are used * # lpp(i)=0 . * # * #2. Values of the charm and bottom kinematic (pole) masses are * # those used in the matrix elements and phase space UNLESS they * # are set to ZERO from the start in the model (particles.dat) * # This happens, for example, when using 5-flavor QCD where * # charm and bottom are treated as partons in the initial state * # and a zero mass might be hardwired in the model definition. * # * #****************************************************************** Block SMINPUTS # Standard Model inputs 1 1.32506980E+02 # alpha_em(MZ)(-1) SM MSbar 2 1.16639000E-05 # G_Fermi 3 1.18000000E-01 # alpha_s(MZ) SM MSbar 4 9.11880000E+01 # Z mass (as input parameter) Block MGYUKAWA # Yukawa masses m/v=y/sqrt(2) # PDG YMASS 5 4.20000000E+00 # mbottom for the Yukawa y_b 4 1.42000000E+00 # mcharm for the Yukawa y_c 6 1.64500000E+02 # mtop for the Yukawa y_t 15 1.77700000E+00 # mtau for the Yukawa y_ta Block MGCKM # CKM elements for MadGraph 1 1 9.75000000E-01 # Vud for Cabibbo matrix Block MASS # Mass spectrum (kinematic masses) # PDG Mass 5 4.70000000E+00 # bottom pole mass 6 1.74300000E+02 # top pole mass 15 1.77700000E+00 # tau mass 23 9.11880000E+01 # Z mass 24 8.04190000E+01 # W mass 25 1.20000000E+02 # H mass # PDG Width DECAY 6 1.50833649E+00 # top width DECAY 23 2.44140351E+00 # Z width DECAY 24 2.04759951E+00 # W width DECAY 25 5.75308848E-03 # H width # BR NDA ID1 ID2 8.27451012E-02 2 4 -4 # BR( H -> c cbar ) 7.17809696E-01 2 5 -5 # BR( H -> b bbar ) 0.00000000E+00 2 6 -6 # BR( H -> t tbar ) 4.31720144E-02 2 15 -15 # BR( H -> tau- tau+) 6.90597075E-03 2 23 23 # BR( H -> Z Z^(*)) 7.45906395E-02 2 24 -24 # BR( H -> W W^(*)) 3.01765558E-02 2 21 21 # BR( H -> g g ) 1.42800773E-03 2 22 22 # BR( H -> A A ) #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # run_card.dat * # * # This file is used to set the parameters of the run. * # * # Some notation/conventions: * # * # Lines starting with a '# ' are info or comments * # * # mind the format: value = variable ! comment * #********************************************************************* # #******************* # Running parameters #******************* # #********************************************************************* # Tag name for the run (one word) * #********************************************************************* 'fermi' = run_tag ! name of the run #********************************************************************* # Run to generate the grid pack * #********************************************************************* .false. = gridpack !True = setting up the grid pack #********************************************************************* # Number of events and rnd seed * #********************************************************************* 100 = nevents ! Number of unweighted events requested 25484 = iseed ! rnd seed (0=assigned automatically=default)) #********************************************************************* # Collider type and energy * #********************************************************************* 1 = lpp1 ! beam 1 type (0=NO PDF) 1 = lpp2 ! beam 2 type (0=NO PDF) 3500.0 = ebeam1 ! beam 1 energy in GeV 3500.0 = ebeam2 ! beam 2 energy in GeV #********************************************************************* # Beam polarization from -100 (left-handed) to 100 (right-handed) * #********************************************************************* 0 = polbeam1 ! beam polarization for beam 1 0 = polbeam2 ! beam polarization for beam 2 #********************************************************************* # PDF CHOICE: this automatically fixes also alpha_s and its evol. * #********************************************************************* # 'cteq6_l' = pdlabel ! PDF set 'lhapdf' = pdlabel ! PDF label 10042 = lhaid ! PDF set #********************************************************************* # Renormalization and factorization scales * #********************************************************************* T = fixed_ren_scale ! if .true. use fixed ren scale T = fixed_fac_scale ! if .true. use fixed fac scale 91.188 = scale ! fixed ren scale 80.4 = dsqrt_q2fact1 ! fixed fact scale for pdf1 80.4 = dsqrt_q2fact2 ! fixed fact scale for pdf2 1 = scalefact ! scale factor for event-by-event scales #********************************************************************* # Matching - Warning! ickkw > 0 is still beta #********************************************************************* 0 = ickkw ! 0 no matching, 1 MLM, 2 CKKW matching 1 = highestmult ! for ickkw=2, highest mult group 1 = ktscheme ! for ickkw=1, 1 Durham kT, 2 Pythia pTE 1 = alpsfact ! scale factor for QCD emission vx F = chcluster ! cluster only according to channel diag F = pdfwgt ! for ickkw=1, perform pdf reweighting #********************************************************************* # #********************************** # BW cutoff (M+/-bwcutoff*Gamma) #********************************** 15d0 = bwcutoff #******************* # Standard Cuts #******************* # #********************************************************************* # Minimum and maximum pt's * #********************************************************************* 0d0 = ptj ! minimum pt for the jets 0d0 = ptb ! minimum pt for the b 0d0 = pta ! minimum pt for the photons 0d0 = ptl ! minimum pt for the charged leptons 0d0 = misset ! minimum missing Et (sum of neutrino's momenta) 0d0 = ptheavy ! minimum pt for one heavy final state 0d0 = ptonium ! minimum pt for the quarkonium states 1d9 = ptjmax ! maximum pt for the jets 1d9 = ptbmax ! maximum pt for the b 1d9 = ptamax ! maximum pt for the photons 1d9 = ptlmax ! maximum pt for the charged leptons 1d9 = missetmax ! maximum missing Et (sum of neutrino's momenta) #********************************************************************* # Minimum and maximum E's (in the lab frame) * #********************************************************************* 0d0 = ej ! minimum E for the jets 0d0 = eb ! minimum E for the b 0d0 = ea ! minimum E for the photons 0d0 = el ! minimum E for the charged leptons 1d9 = ejmax ! maximum E for the jets 1d9 = ebmax ! maximum E for the b 1d9 = eamax ! maximum E for the photons 1d9 = elmax ! maximum E for the charged leptons #********************************************************************* # Maximum and minimum rapidity * #********************************************************************* 1d9 = etaj ! max rap for the jets 1d9 = etab ! max rap for the b 1d9 = etaa ! max rap for the photons 1d9 = etal ! max rap for the charged leptons 1d9 = etaonium ! max rap for the quarkonium states 0d0 = etajmin ! min rap for the jets 0d0 = etabmin ! min rap for the b 0d0 = etaamin ! min rap for the photons 0d0 = etalmin ! main rap for the charged leptons #********************************************************************* # Minimum and maximum DeltaR distance * #********************************************************************* 0d0 = drjj ! min distance between jets 0d0 = drbb ! min distance between b's 0d0 = drll ! min distance between leptons 0d0 = draa ! min distance between gammas 0d0 = drbj ! min distance between b and jet 0d0 = draj ! min distance between gamma and jet 0d0 = drjl ! min distance between jet and lepton 0d0 = drab ! min distance between gamma and b 0d0 = drbl ! min distance between b and lepton 0d0 = dral ! min distance between gamma and lepton 1d9 = drjjmax ! max distance between jets 1d9 = drbbmax ! max distance between b's 1d9 = drllmax ! max distance between leptons 1d9 = draamax ! max distance between gammas 1d9 = drbjmax ! max distance between b and jet 1d9 = drajmax ! max distance between gamma and jet 1d9 = drjlmax ! max distance between jet and lepton 1d9 = drabmax ! max distance between gamma and b 1d9 = drblmax ! max distance between b and lepton 1d9 = dralmax ! maxdistance between gamma and lepton #********************************************************************* # Minimum and maximum invariant mass for pairs * #********************************************************************* 0d0 = mmjj ! min invariant mass of a jet pair 0d0 = mmbb ! min invariant mass of a b pair 0d0 = mmaa ! min invariant mass of gamma gamma pair 0d0 = mmll ! min invariant mass of l+l- (same flavour) lepton pair 1d9 = mmjjmax ! max invariant mass of a jet pair 1d9 = mmbbmax ! max invariant mass of a b pair 1d9 = mmaamax ! max invariant mass of gamma gamma pair 1d9 = mmllmax ! max invariant mass of l+l- (same flavour) lepton pair #********************************************************************* # Minimum and maximum invariant mass for all letpons * #********************************************************************* 0d0 = mmnl ! min invariant mass for all letpons (l+- and vl) 1d9 = mmnlmax ! max invariant mass for all letpons (l+- and vl) #********************************************************************* # Inclusive cuts * #********************************************************************* 0d0 = xptj ! minimum pt for at least one jet 0d0 = xptb ! minimum pt for at least one b 0d0 = xpta ! minimum pt for at least one photon 0d0 = xptl ! minimum pt for at least one charged lepton #********************************************************************* # Control the pt's of the jets sorted by pt * #********************************************************************* 0d0 = ptj1min ! minimum pt for the leading jet in pt 0d0 = ptj2min ! minimum pt for the second jet in pt 0d0 = ptj3min ! minimum pt for the third jet in pt 0d0 = ptj4min ! minimum pt for the fourth jet in pt 1d9 = ptj1max ! maximum pt for the leading jet in pt 1d9 = ptj2max ! maximum pt for the second jet in pt 1d9 = ptj3max ! maximum pt for the third jet in pt 1d9 = ptj4max ! maximum pt for the fourth jet in pt 0 = cutuse ! reject event if fails any (0) / all (1) jet pt cuts #********************************************************************* # Control the Ht(k)=Sum of k leading jets * #********************************************************************* 0d0 = htjmin ! minimum jet HT=Sum(jet pt) 1d9 = htjmax ! maximum jet HT=Sum(jet pt) 0d0 = ht2min ! minimum Ht for the two leading jets 0d0 = ht3min ! minimum Ht for the three leading jets 0d0 = ht4min ! minimum Ht for the four leading jets 1d9 = ht2max ! maximum Ht for the two leading jets 1d9 = ht3max ! maximum Ht for the three leading jets 1d9 = ht4max ! maximum Ht for the four leading jets #********************************************************************* # WBF cuts * #********************************************************************* 0 = xetamin ! minimum rapidity for two jets in the WBF case 0 = deltaeta ! minimum rapidity for two jets in the WBF case #********************************************************************* # maximal pdg code for quark to be considered as a jet * # otherwise b cuts are applied * #********************************************************************* 4 = maxjetflavor #********************************************************************* # Jet measure cuts * #********************************************************************* 0 = xqcut ! minimum kt jet measure between partons #********************************************************************* 30d0 = ktdurham ! minimum durham kt jet measure between partons 0.4 = dparameter ! D parameter for hadronic kT T = dokt ! T: enable durham kt cut #********************************************************************* # Number of Events : 100 # Integrated weight (pb) : .49226E+04 # Truncated wgt (pb) : .00000E+00 # Unit wgt : .49226E+02
      2212 2212 0.35000000000E+04 0.35000000000E+04 0 0 10042 10042 3 1 0.49226000000E+04 0.00000000000E+00 0.49226000000E+02 1 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.39919743011E+03 0.39919743011E+03 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.39435316792E+01 0.39435316792E+01 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.39525389843E+03 0.40314096179E+03 0.79353581190E+02 0. 0. -11 1 3 3 0 0 -0.30323238127E+02 0.99501563813E+01 0.31739128930E+03 0.31899174739E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.30323238127E+02 -0.99501563813E+01 0.77862609129E+02 0.84149214393E+02 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.95197490922E+00 0.95197490922E+00 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.16818866900E+04 0.16818866900E+04 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.16809347151E+04 0.16828386649E+04 0.80027843381E+02 0. 0. -11 1 3 3 0 0 0.15828281049E+02 0.19870783518E+02 -0.19038362578E+03 0.19207110007E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.15828281049E+02 -0.19870783518E+02 -0.14905510894E+04 0.14907675649E+04 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.77615790458E+01 0.77615790458E+01 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.19850039189E+03 0.19850039189E+03 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.19073881285E+03 0.20626197094E+03 0.78502903954E+02 0. 0. -11 1 3 3 0 0 -0.15174502607E+01 -0.38183717099E+02 -0.71813441871E+02 0.81347829351E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.15174502607E+01 0.38183717099E+02 -0.11892537098E+03 0.12491414159E+03 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 4 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.42072561924E+02 0.42072561924E+02 0.00000000000E+00 0. -1. -3 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.38977124225E+02 0.38977124225E+02 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.30954376995E+01 0.81049686149E+02 0.80990554328E+02 0. 0. -11 1 3 3 0 0 -0.28819538317E+02 -0.19571059338E+02 -0.19113791286E+02 0.39735741717E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.28819538317E+02 0.19571059338E+02 0.22209228986E+02 0.41313944432E+02 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.29212167130E+03 0.29212167130E+03 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.55038951545E+01 0.55038951545E+01 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.28661777615E+03 0.29762556646E+03 0.80194938774E+02 0. 0. -11 1 3 3 0 0 0.37828819818E+02 0.10343604175E+02 0.11230311451E+03 0.11895376953E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.37828819818E+02 -0.10343604175E+02 0.17431466164E+03 0.17867179693E+03 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.35659668297E+02 0.35659668297E+02 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.47413529497E+02 0.47413529497E+02 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.11753861200E+02 0.83073197794E+02 0.82237478917E+02 0. 0. -11 1 3 3 0 0 0.17908814678E+02 0.31450351122E+02 -0.25591936663E+02 0.44326035815E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.17908814678E+02 -0.31450351122E+02 0.13838075463E+02 0.38747161979E+02 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.78286723267E+02 0.78286723267E+02 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.20682610751E+02 0.20682610751E+02 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.57604112516E+02 0.98969334018E+02 0.80477918072E+02 0. 0. -11 1 3 3 0 0 0.45563844284E+01 0.64666299972E+01 0.77321057628E+02 0.77724667226E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.45563844284E+01 -0.64666299972E+01 -0.19716945112E+02 0.21244666792E+02 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.25858372726E+03 0.25858372726E+03 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.60682033233E+01 0.60682033233E+01 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.25251552394E+03 0.26465193059E+03 0.79224709104E+02 0. 0. -11 1 3 3 0 0 -0.75337744095E+01 0.37543559491E+02 0.92377876673E+02 0.99999743573E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.75337744095E+01 -0.37543559491E+02 0.16013764727E+03 0.16465218702E+03 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.99793468094E+01 0.99793468094E+01 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.15366187616E+03 0.15366187616E+03 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.14368252936E+03 0.16364122297E+03 0.78318456411E+02 0. 0. -11 1 3 3 0 0 0.28595787235E+01 -0.38771325641E+02 -0.62029316186E+02 0.73205388797E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.28595787235E+01 0.38771325641E+02 -0.81653213170E+02 0.90435834177E+02 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.13366889958E+02 0.13366889958E+02 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.13169266044E+03 0.13169266044E+03 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.11832577049E+03 0.14505955040E+03 0.83912366202E+02 0. 0. -11 1 3 3 0 0 0.20800831356E+01 -0.16415437871E+02 0.74881500340E+01 0.18162206288E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.20800831356E+01 0.16415437871E+02 -0.12581392052E+03 0.12689734411E+03 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 -3 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.23508893876E+02 0.23508893876E+02 0.00000000000E+00 0. 1. 4 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.62402811503E+02 0.62402811503E+02 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.38893917627E+02 0.85911705379E+02 0.76603422200E+02 0. 0. -11 1 3 3 0 0 -0.29265800776E+02 0.24238545228E+02 -0.14065228425E+02 0.40519437564E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.29265800776E+02 -0.24238545228E+02 -0.24828689202E+02 0.45392267815E+02 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.27282780432E+03 0.27282780432E+03 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.64177401499E+01 0.64177401499E+01 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.26641006417E+03 0.27924554447E+03 0.83688421034E+02 0. 0. -11 1 3 3 0 0 0.19130104104E+02 -0.92728176467E+01 0.12944227845E+02 0.24889738139E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.19130104104E+02 0.92728176467E+01 0.25346583633E+03 0.25435580633E+03 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.39513784705E+03 0.39513784705E+03 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.40736220105E+01 0.40736220105E+01 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.39106422504E+03 0.39921146906E+03 0.80240693688E+02 0. 0. -11 1 3 3 0 0 0.33663610850E+02 -0.15942952840E+02 0.26969823342E+03 0.27225824790E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.33663610850E+02 0.15942952840E+02 0.12136599162E+03 0.12695322115E+03 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.17519046473E+03 0.17519046473E+03 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.10852647909E+02 0.10852647909E+02 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.16433781682E+03 0.18604311263E+03 0.87207349016E+02 0. 0. -11 1 3 3 0 0 -0.22790142761E+02 0.37167122110E+02 0.83669631687E+02 0.94347193067E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.22790142761E+02 -0.37167122110E+02 0.80668185129E+02 0.91695919566E+02 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.23019714065E+02 0.23019714065E+02 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.11793932553E+03 0.11793932553E+03 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.94919611467E+02 0.14095903960E+03 0.10420997171E+03 0. 0. -11 1 3 3 0 0 -0.47607202185E+02 -0.43901888807E+01 -0.75483063192E+02 0.89349942849E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.47607202185E+02 0.43901888807E+01 -0.19436548274E+02 0.51609096748E+02 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.75272410826E+03 0.75272410826E+03 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.20883876140E+01 0.20883876140E+01 0.00000000000E+00 0. 1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.75063572065E+03 0.75481249587E+03 0.79296398518E+02 0. 0. -11 1 3 3 0 0 0.41790278289E+00 0.33861691010E+02 0.17903714993E+03 0.18221166213E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.41790278289E+00 -0.33861691010E+02 0.57159857072E+03 0.57260083375E+03 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.84408307748E+01 0.84408307748E+01 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.19802713894E+03 0.19802713894E+03 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.18958630817E+03 0.20646796972E+03 0.81768296268E+02 0. 0. -11 1 3 3 0 0 0.38292425724E+02 0.13677083195E+02 -0.84038424370E+02 0.93358605619E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.38292425724E+02 -0.13677083195E+02 -0.10554788380E+03 0.11310936410E+03 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.45702754300E+02 0.45702754300E+02 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.36413234308E+02 0.36413234308E+02 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 0.92895199919E+01 0.82115988609E+02 0.81588849750E+02 0. 0. -11 1 3 3 0 0 0.27791331129E+02 0.82413736022E+01 0.33533989076E+02 0.44326140686E+02 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.27791331129E+02 -0.82413736022E+01 -0.24244469084E+02 0.37789847922E+02 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 -3 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.36981841238E+01 0.36981841238E+01 0.00000000000E+00 0. 1. 4 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.47472474352E+03 0.47472474352E+03 0.00000000000E+00 0. -1. 24 2 1 2 0 0 0.00000000000E+00 0.00000000000E+00 -0.47102655940E+03 0.47842292765E+03 0.83800226961E+02 0. 0. -11 1 3 3 0 0 -0.62653031138E+01 0.17182953310E+02 -0.45073241493E+03 0.45110333381E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 0.62653031138E+01 -0.17182953310E+02 -0.20294144468E+02 0.27319593834E+02 0.00000000000E+00 0. -1. 5 1 0.4922600E+02 0.8040000E+02 0.7546772E-02 0.1297830E+00 2 -1 0 0 501 0 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      pythia8-8.1.80.orig/examples/main62.cmnd0000644000175000017500000000416712217346166016126 0ustar sunsun! main62.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! Names are case-insensitive - but spellings-sensitive! ! The settings here are illustrative, not always physics-motivated. ! 1) Settings used in the main program. Main:timesAllowErrors = 3 ! how many aborts before run stops ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showAllSettings = off ! list all settings Init:showChangedParticleData = on ! list changed particle data Init:showAllParticleData = off ! list all particle data Next:numberCount = 1000 ! print message every n events Next:numberShowLHA = 1 ! print LHA information n times Next:numberShowInfo = 1 ! print event information n times Next:numberShowProcess = 1 ! print process record n times Next:numberShowEvent = 1 ! print event record n times Stat:showPartonLevel = off ! additional statistics on MPI ! 3) PDF settings. Default is to use internal PDFs PDF:useLHAPDF = on ! some pdf sets examples: cteq61.LHpdf cteq61.LHgrid MRST2004nlo.LHgrid PDF:LHAPDFset = MRST2001lo.LHgrid ! Allow extrapolation of PDF's beyond x and Q2 boundaries, at own risk. ! Default behaviour is to freeze PDF's at boundaries. PDF:extrapolateLHAPDF = on ! 4) Other common settings. 6:m0 = 175. ! same m_t as Pythia 6.4 to compare #ParticleDecays:limitTau0 = on ! set long-lived particle stable ... #ParticleDecays:tau0Max = 10 ! ... if c*tau0 > 10 mm ! 5) The number of subruns to execute. Main:numberOfSubruns = 2 ! 6) Information specific to the first subrun Main:subrun = 1 ! matches readFile( ..., 1) Beams:frameType = 4 ! use LHEF input Beams:LHEF = ttbar.lhe ! first LHEF event file ! 7) Information specific to the second subrun Main:subrun = 2 ! matches readFile( ..., 2) Beams:newLHEFsameInit = on ! no reinitialization needed/wanted Beams:LHEF = ttbar2.lhe ! second LHEF event file pythia8-8.1.80.orig/examples/main01.cc0000644000175000017500000000235012217346163015550 0ustar sunsun// main01.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. It fits on one slide in a talk. // It studies the charged multiplicity distribution at the LHC. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator. Process selection. LHC initialization. Histogram. Pythia pythia; pythia.readString("Beams:eCM = 8000."); pythia.readString("HardQCD:all = on"); pythia.readString("PhaseSpace:pTHatMin = 20."); pythia.init(); Hist mult("charged multiplicity", 100, -0.5, 799.5); // Begin event loop. Generate event. Skip if error. List first one. for (int iEvent = 0; iEvent < 100; ++iEvent) { if (!pythia.next()) continue; // Find number of all final charged particles and fill histogram. int nCharged = 0; for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].isFinal() && pythia.event[i].isCharged()) ++nCharged; mult.fill( nCharged ); // End of event loop. Statistics. Histogram. Done. } pythia.stat(); cout << mult; return 0; } pythia8-8.1.80.orig/examples/ttbar2.lhe0000644000175000017500000021350112217346207016045 0ustar sunsun 2212 -2212 9.800000E+02 9.800000E+02 0 0 7 7 3 2 5.534984E+00 5.591178E-01 1.000000E+00 81 1.886281E-01 1.333802E-01 1.000000E+00 82 4 81 1.000000E+00 2.779475E+02 7.861651E-03 1.084400E-01 2 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 3.0163058970E+02 3.0163058970E+02 0.0000000000E+00 0. 9. -2 -1 0 0 0 102 0.0000000000E+00 0.0000000000E+00 -2.9643457592E+02 2.9643457592E+02 0.0000000000E+00 0. 9. 6 1 1 2 101 0 -1.3588865269E+02 -1.6715922432E+02 1.1286978960E+02 3.0000050129E+02 1.7564959199E+02 0. 9. -6 1 1 2 0 102 1.3588865269E+02 1.6715922432E+02 -1.0767377581E+02 2.9806466432E+02 1.7561597284E+02 0. 9. #pdf 2 -2 3.0778631602E-01 3.0248426114E-01 2.7794748919E+02 3.1211535198E-01 3.1936736456E-01 4 81 1.000000E+00 2.065406E+02 7.835319E-03 1.128749E-01 2 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 2.8246988013E+02 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1.4784168136E-01 1.9142921403E+02 3.6751303814E-01 5.2407902205E-01 4 81 1.000000E+00 2.006447E+02 7.832761E-03 1.133269E-01 2 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 9.0642848113E+01 9.0642848113E+01 0.0000000000E+00 0. 9. -2 -1 0 0 0 102 0.0000000000E+00 0.0000000000E+00 -4.5134335725E+02 4.5134335725E+02 0.0000000000E+00 0. 9. 6 1 1 2 101 0 5.3033149673E+01 -7.9472874554E+01 -1.4477241363E+02 2.4623371072E+02 1.7476709014E+02 0. 9. -6 1 1 2 0 102 -5.3033149673E+01 7.9472874554E+01 -2.1592809551E+02 2.9575249464E+02 1.7809026616E+02 0. 9. #pdf 2 -2 9.2492702157E-02 4.6055444618E-01 2.0064469119E+02 5.6041197383E-01 1.4239601412E-01 pythia8-8.1.80.orig/examples/main42.cmnd0000644000175000017500000000450612217346166016121 0ustar sunsun! File: main42.cmnd ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! Names are case-insensitive - but spellings-sensitive! ! The changes here are illustrative, not always physics-motivated. ! 1) Settings that will be used in a main program. Main:numberOfEvents = 200 ! number of events to generate Main:timesAllowErrors = 3 ! abort run after this many flawed events ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showAllSettings = off ! list all settings Init:showChangedParticleData = on ! list changed particle data Init:showAllParticleData = off ! list all particle data Next:numberCount = 1000 ! print message every n events Next:numberShowLHA = 1 ! print LHA information n times Next:numberShowInfo = 1 ! print event information n times Next:numberShowProcess = 1 ! print process record n times Next:numberShowEvent = 1 ! print event record n times Stat:showPartonLevel = on ! additional statistics on MPI ! 3) Beam parameter settings. Values below agree with default ones. Beams:idA = 2212 ! first beam, p = 2212, pbar = -2212 Beams:idB = 2212 ! second beam, p = 2212, pbar = -2212 Beams:eCM = 14000. ! CM energy of collision ! 4a) Pick processes and kinematics cuts. Charmonium:gg2QQbar[3S1(1)]g = on ! colour singlet charmonium production Charmonium:gg2QQbar[3P0(1)]g = on ! " Charmonium:gg2QQbar[3P1(1)]g = on ! " Charmonium:gg2QQbar[3P2(1)]g = on ! " PhaseSpace:pTHatMin = 20. ! minimum pT of hard process ! 4b) Alternative beam and process selection from a Les Houches Event File. ! NOTE: to use this option, comment out the lines in section 4a above ! and uncomment the ones below. Section 3 is ignored for frameType = 4. #Beams:frameType = 4 ! read info from a LHEF #Beams:LHEF = ttbar.lhe ! the LHEF to read from ! 5) Other settings. Can be expanded as desired. ! Note: may overwrite some of the values above, so watch out. #Tune:pp = 6 ! use Tune 4Cx #ParticleDecays:limitTau0 = on ! set long-lived particle stable ... #ParticleDecays:tau0Max = 10 ! ... if c*tau0 > 10 mm pythia8-8.1.80.orig/examples/main62.cc0000644000175000017500000000746412217346166015575 0ustar sunsun// main62.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Author: Mikhail Kirsanov, Mikhail.Kirsanov@cern.ch. // This program illustrates how a file with HepMC events // can be generated by Pythia8. // It is similar to main42 and main61, except that it is compiled with LHAPDF // and allows for several subruns, e.g. from related LHEF. // Input and output files are specified on the command line, e.g. like // ./main62.exe main62.cmnd hepmcout62.dat > out // The main program contains no analysis; this is intended to happen later. // It therefore "never" has to be recompiled to handle different tasks. // WARNING: typically one needs 25 MB/100 events at the LHC. // Therefore large event samples may be impractical. #include "Pythia8/Pythia.h" #include "Pythia8/Pythia8ToHepMC.h" #include "HepMC/GenEvent.h" #include "HepMC/IO_GenEvent.h" using namespace Pythia8; int main(int argc, char* argv[]) { // Check that correct number of command-line arguments if (argc != 3) { cerr << " Unexpected number of command-line arguments. \n You are" << " expected to provide one input and one output file name. \n" << " Program stopped! " << endl; return 1; } // Check that the provided input name corresponds to an existing file. ifstream is(argv[1]); if (!is) { cerr << " Command-line file " << argv[1] << " was not found. \n" << " Program stopped! " << endl; return 1; } // Confirm that external files will be used for input and output. cout << "\n >>> PYTHIA settings will be read from file " << argv[1] << " <<< \n >>> HepMC events will be written to file " << argv[2] << " <<< \n" << endl; // Interface for conversion from Pythia8::Event to HepMC event. HepMC::Pythia8ToHepMC ToHepMC; // Specify file where HepMC events will be stored. HepMC::IO_GenEvent ascii_io(argv[2], std::ios::out); // Generator. Pythia pythia; // Read in subrun-independent commands from external file. pythia.readFile( argv[1]); // Extract data to be used in main program. Set counters. int nSubrun = pythia.mode("Main:numberOfSubruns"); int nAbort = pythia.mode("Main:timesAllowErrors"); int iAbort = 0; // Begin loop over subruns. for (int iSubrun = 1; iSubrun <= nSubrun; ++iSubrun) { // Read in subrun-specific data from external file. pythia.readFile( argv[1], iSubrun); // Initialization. pythia.init(); // Print name of Les Houches Event File. string lheFile = pythia.settings.word("Beams:LHEF"); cout << "\n >>> Now begin subrun " << iSubrun << " with events from file " << lheFile << " <<< \n" << endl; // Begin infinite event loop - to be exited at end of file. for (int iEvent = 0; ; ++iEvent) { // Generate event. if (!pythia.next()) { // Leave event loop if at end of file. if (pythia.info.atEndOfFile()) break; // First few failures write off as "acceptable" errors, then quit. if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Construct new empty HepMC event and fill it. // Units will be as chosen for HepMC build, but can be changed // by arguments, e.g. GenEvt( HepMC::Units::GEV, HepMC::Units::MM) HepMC::GenEvent* hepmcevt = new HepMC::GenEvent(); ToHepMC.fill_next_event( pythia, hepmcevt ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; // End of event loop. } // End of subrun loop. } // Statistics. pythia.stat(); // Done. return 0; } pythia8-8.1.80.orig/examples/main11.cc0000644000175000017500000000365012217346164015556 0ustar sunsun// main11.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how Les Houches Event File input can be used in Pythia8. // It uses the ttsample.lhe input file, the latter only with 100 events. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator. We here stick with default values, but changes // could be inserted with readString or readFile. Pythia pythia; // Initialize Les Houches Event File run. List initialization information. pythia.readString("Beams:frameType = 4"); pythia.readString("Beams:LHEF = ttbar.lhe"); pythia.init(); // Book histogram. Hist nCharged("charged particle multiplicity",100,-0.5,399.5); // Allow for possibility of a few faulty events. int nAbort = 10; int iAbort = 0; // Begin event loop; generate until none left in input file. for (int iEvent = 0; ; ++iEvent) { // Generate events, and check whether generation failed. if (!pythia.next()) { // If failure because reached end of file then exit event loop. if (pythia.info.atEndOfFile()) break; // First few failures write off as "acceptable" errors, then quit. if (++iAbort < nAbort) continue; break; } // Sum up final charged multiplicity and fill in histogram. int nChg = 0; for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].isFinal() && pythia.event[i].isCharged()) ++nChg; nCharged.fill(nChg); // End of event loop. } // Give statistics. Print histogram. pythia.stat(); cout << nCharged; // Done. return 0; } pythia8-8.1.80.orig/examples/main88.cmnd0000644000175000017500000000277112217346170016130 0ustar sunsun! main88.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. // Number of events generated Main:numberOfEvents = 1000 // Shower options HadronLevel:all = on PartonLevel:MPI = on // Core process for merging Merging:Process = pp>LEPTONS,NEUTRINOS // Maximal number of additional LO jets. Merging:nJetMax = 2 // Maximal number of additional NLO jets. Merging:nJetMaxNLO = 1 // Merging scale value. Merging:TMS = 15 // Values of (fixed) scales in the matrix element calculation. Merging:muFacInME = 80.4 Merging:muRenInME = 91.188 // Values of (fixed) scales for the PS lowest multiplicity process. Merging:muFac = 80.4 Merging:muRen = 91.188 // Include PDFs into the choice of histories. Merging:includeRedundant = on // Switch off enforced rapidity ordering SpaceShower:rapidityOrder = off // Since UNLOPS is a next-to-leading order merging method, next-to-leading // order PDFs are necessary. However, the parton shower and multiparton // interactions favour leading-order PDFs, since multiparton interactions // probe the incoming hadron at small momentum scales. Until a NLO-merged // tune becomes available, NLO PDFs should be used throughout. // Example PDF files generated with CTEQ6M PDFs PDF:useLHAPDF = on PDF:LHAPDFset = cteq6m.LHpdf SpaceShower:alphaSvalue = 0.118 TimeShower:alphaSvalue = 0.118 pythia8-8.1.80.orig/examples/sps1aNarrowStopGluino.spc0000644000175000017500000013645512217346206021143 0ustar sunsun## Important note! ## This file has been modified by hand to give the gluino, the stop_1 ## and the su_L very narrow widths, such that it can be used to try out ## the R-hadron machinery. It is not a realistic SUSY scenario. ## ##****************************************************************** ## MadGraph/MadEvent * ##****************************************************************** ## * ## param_card corresponding the SPS point 1a (by SoftSusy 2.0.5) * ## * ##****************************************************************** ## Les Houches friendly file for the (MS)SM parameters of MadGraph * ## SM parameter set and decay widths produced by MSSMCalc * ##****************************************************************** ##*Please note the following IMPORTANT issues: * ## * ##0. REFRAIN from editing this file by hand! Some of the parame- * ## ters are not independent. Always use a calculator. * ## * ##1. alpha_S(MZ) has been used in the calculation of the parameters* ## This value is KEPT by madgraph when no pdf are used lpp(i)=0, * ## but, for consistency, it will be reset by madgraph to the * ## value expected IF the pdfs for collisions with hadrons are * ## used. * ## * ##2. Values of the charm and bottom kinematic (pole) masses are * ## those used in the matrix elements and phase space UNLESS they * ## are set to ZERO from the start in the model (particles.dat) * ## This happens, for example, when using 5-flavor QCD where * ## charm and bottom are treated as partons in the initial state * ## and a zero mass might be hardwired in the model definition. * ## * ## The SUSY decays have calculated using SDECAY 1.1a * ## * ##****************************************************************** # BLOCK DCINFO # Decay Program information 1 SDECAY # decay calculator 2 1.1a # version number # BLOCK SPINFO # Spectrum calculator information 1 SOFTSUSY # spectrum calculator 2 2.0.5 # version number # BLOCK MODSEL # Model selection 1 1 sugra # BLOCK SMINPUTS # Standard Model inputs 1 1.27934000E+02 # alpha_em^-1(M_Z)^MSbar 2 1.16637000E-05 # G_F [GeV^-2] 3 1.18000000E-01 # alpha_S(M_Z)^MSbar 4 9.11876000E+01 # M_Z pole mass 5 4.25000000E+00 # mb(mb)^MSbar 6 1.75000000E+02 # mt pole mass 7 1.77700000E+00 # mtau pole mass # BLOCK MINPAR # Input parameters - minimal models 1 1.00000000E+02 # m0 2 2.50000000E+02 # m12 3 1.00000000E+01 # tanb 4 1.00000000E+00 # sign(mu) 5 -1.00000000E+02 # A0 # BLOCK MASS # Mass Spectrum # PDG code mass particle 5 4.88991651E+00 # b-quark pole mass calculated from mb(mb)_Msbar 6 1.75000000E+02 # mt pole mass (not read by ME) 24 7.98290131E+01 # W+ 25 1.10899057E+02 # h 35 3.99960116E+02 # H 36 3.99583917E+02 # A 37 4.07879012E+02 # H+ 1000001 5.68441109E+02 # ~d_L 2000001 5.45228462E+02 # ~d_R 1000002 5.61119014E+02 # ~u_L 2000002 5.49259265E+02 # ~u_R 1000003 5.68441109E+02 # ~s_L 2000003 5.45228462E+02 # ~s_R 1000004 5.61119014E+02 # ~c_L 2000004 5.49259265E+02 # ~c_R 1000005 5.13065179E+02 # ~b_1 2000005 5.43726676E+02 # ~b_2 1000006 3.99668493E+02 # ~t_1 2000006 5.85785818E+02 # ~t_2 1000011 2.02915690E+02 # ~e_L 2000011 1.44102799E+02 # ~e_R 1000012 1.85258326E+02 # ~nu_eL 1000013 2.02915690E+02 # ~mu_L 2000013 1.44102799E+02 # ~mu_R 1000014 1.85258326E+02 # ~nu_muL 1000015 1.34490864E+02 # ~tau_1 2000015 2.06867805E+02 # ~tau_2 1000016 1.84708464E+02 # ~nu_tauL 1000021 6.07713704E+02 # ~g 1000022 9.66880686E+01 # ~chi_10 1000023 1.81088157E+02 # ~chi_20 1000025 -3.63756027E+02 # ~chi_30 1000035 3.81729382E+02 # ~chi_40 1000024 1.81696474E+02 # ~chi_1+ 1000037 3.79939320E+02 # ~chi_2+ # BLOCK NMIX # Neutralino Mixing Matrix 1 1 9.86364430E-01 # N_11 1 2 -5.31103553E-02 # N_12 1 3 1.46433995E-01 # N_13 1 4 -5.31186117E-02 # N_14 2 1 9.93505358E-02 # N_21 2 2 9.44949299E-01 # N_22 2 3 -2.69846720E-01 # N_23 2 4 1.56150698E-01 # N_24 3 1 -6.03388002E-02 # N_31 3 2 8.77004854E-02 # N_32 3 3 6.95877493E-01 # N_33 3 4 7.10226984E-01 # N_34 4 1 -1.16507132E-01 # N_41 4 2 3.10739017E-01 # N_42 4 3 6.49225960E-01 # N_43 4 4 -6.84377823E-01 # N_44 # BLOCK UMIX # Chargino Mixing Matrix U 1 1 9.16834859E-01 # U_11 1 2 -3.99266629E-01 # U_12 2 1 3.99266629E-01 # U_21 2 2 9.16834859E-01 # U_22 # BLOCK VMIX # Chargino Mixing Matrix V 1 1 9.72557835E-01 # V_11 1 2 -2.32661249E-01 # V_12 2 1 2.32661249E-01 # V_21 2 2 9.72557835E-01 # V_22 # BLOCK STOPMIX # Stop Mixing Matrix 1 1 5.53644960E-01 # O_{11} 1 2 8.32752820E-01 # O_{12} 2 1 8.32752820E-01 # O_{21} 2 2 -5.53644960E-01 # O_{22} # BLOCK SBOTMIX # Sbottom Mixing Matrix 1 1 9.38737896E-01 # O_{11} 1 2 3.44631925E-01 # O_{12} 2 1 -3.44631925E-01 # O_{21} 2 2 9.38737896E-01 # O_{22} # BLOCK STAUMIX # Stau Mixing Matrix 1 1 2.82487190E-01 # O_{11} 1 2 9.59271071E-01 # O_{12} 2 1 9.59271071E-01 # O_{21} 2 2 -2.82487190E-01 # O_{22} # BLOCK ALPHA # Higgs mixing -1.13825210E-01 # Mixing angle in the neutral Higgs boson sector # BLOCK HMIX Q= 4.67034192E+02 # DRbar Higgs Parameters 1 3.57680977E+02 # mu(Q)MSSM DRbar 2 9.74862403E+00 # tan beta(Q)MSSM DRba 3 2.44894549E+02 # higgs vev(Q)MSSM DRb 4 1.66439065E+05 # mA^2(Q)MSSM DRbar # BLOCK GAUGE Q= 4.67034192E+02 # The gauge couplings 3 1.10178679E+00 # g3(Q) MSbar # BLOCK AU Q= 4.67034192E+02 # The trilinear couplings 1 1 0.00000000E+00 # A_u(Q) DRbar 2 2 0.00000000E+00 # A_c(Q) DRbar 3 3 -4.98129778E+02 # A_t(Q) DRbar # BLOCK AD Q= 4.67034192E+02 # The trilinear couplings 1 1 0.00000000E+00 # A_d(Q) DRbar 2 2 0.00000000E+00 # A_s(Q) DRbar 3 3 -7.97274397E+02 # A_b(Q) DRbar # BLOCK AE Q= 4.67034192E+02 # The trilinear couplings 1 1 0.00000000E+00 # A_e(Q) DRbar 2 2 0.00000000E+00 # A_mu(Q) DRbar 3 3 -2.51776873E+02 # A_tau(Q) DRbar # BLOCK YU Q= 4.67034192E+02 # The Yukawa couplings 3 3 8.92844550E-01 # y_t(Q) DRbar # BLOCK YD Q= 4.67034192E+02 # The Yukawa couplings 3 3 1.38840206E-01 # y_b(Q) DRbar # BLOCK YE Q= 4.67034192E+02 # The Yukawa couplings 3 3 1.00890810E-01 # y_tau(Q) DRbar # BLOCK MSOFT Q= 4.67034192E+02 # The soft SUSY breaking masses at the scale Q 1 1.01396534E+02 # M_1(Q) 2 1.91504241E+02 # M_2(Q) 3 5.88263031E+02 # M_3(Q) 21 3.23374943E+04 # mH1^2(Q) 22 -1.28800134E+05 # mH2^2(Q) 31 1.95334764E+02 # meL(Q) 32 1.95334764E+02 # mmuL(Q) 33 1.94495956E+02 # mtauL(Q) 34 1.36494061E+02 # meR(Q) 35 1.36494061E+02 # mmuR(Q) 36 1.34043428E+02 # mtauR(Q) 41 5.47573466E+02 # mqL1(Q) 42 5.47573466E+02 # mqL2(Q) 43 4.98763839E+02 # mqL3(Q) 44 5.29511195E+02 # muR(Q) 45 5.29511195E+02 # mcR(Q) 46 4.23245877E+02 # mtR(Q) 47 5.23148807E+02 # mdR(Q) 48 5.23148807E+02 # msR(Q) 49 5.19867261E+02 # mbR(Q) # # # # ================= # |The decay table| # ================= # # - The multi-body decays for the inos, stops and sbottoms are included. # # PDG Width DECAY 25 1.98610799E-03 # h decays # BR NDA ID1 ID2 1.45642955E-01 2 15 -15 # BR(H1 -> tau- tau+) 8.19070713E-01 2 5 -5 # BR(H1 -> b bb) 3.36338173E-02 2 24 -24 # BR(H1 -> W+ W-) 1.65251528E-03 2 23 23 # BR(H1 -> Z Z) # # PDG Width DECAY 35 5.74801389E-01 # H decays # BR NDA ID1 ID2 1.39072676E-01 2 15 -15 # BR(H -> tau- tau+) 4.84110879E-02 2 6 -6 # BR(H -> t tb) 7.89500067E-01 2 5 -5 # BR(H -> b bb) 3.87681171E-03 2 24 -24 # BR(H -> W+ W-) 1.80454752E-03 2 23 23 # BR(H -> Z Z) 0.00000000E+00 2 24 -37 # BR(H -> W+ H-) 0.00000000E+00 2 -24 37 # BR(H -> W- H+) 0.00000000E+00 2 37 -37 # BR(H -> H+ H-) 1.73348101E-02 2 25 25 # BR(H -> h h) 0.00000000E+00 2 36 36 # BR(H -> A A) # # PDG Width DECAY 36 6.32178488E-01 # A decays # BR NDA ID1 ID2 1.26659725E-01 2 15 -15 # BR(A -> tau- tau+) 1.51081526E-01 2 6 -6 # BR(A -> t tb) 7.19406137E-01 2 5 -5 # BR(A -> b bb) 2.85261228E-03 2 23 25 # BR(A -> Z h) 0.00000000E+00 2 23 35 # BR(A -> Z H) 0.00000000E+00 2 24 -37 # BR(A -> W+ H-) 0.00000000E+00 2 -24 37 # BR(A -> W- H+) # # PDG Width DECAY 37 5.46962813E-01 # H+ decays # BR NDA ID1 ID2 1.49435135E-01 2 -15 16 # BR(H+ -> tau+ nu_tau) 8.46811711E-01 2 6 -5 # BR(H+ -> t bb) 3.75315387E-03 2 24 25 # BR(H+ -> W+ h) 0.00000000E+00 2 24 35 # BR(H+ -> W+ H) 0.00000000E+00 2 24 36 # BR(H+ -> W+ A) # # PDG Width DECAY 1000021 0.01E+00 # gluino decays # BR NDA ID1 ID2 2.08454202E-02 2 1000001 -1 # BR(~g -> ~d_L db) 2.08454202E-02 2 -1000001 1 # BR(~g -> ~d_L* d ) 5.07075274E-02 2 2000001 -1 # BR(~g -> ~d_R db) 5.07075274E-02 2 -2000001 1 # BR(~g -> ~d_R* d ) 2.89787767E-02 2 1000002 -2 # BR(~g -> ~u_L ub) 2.89787767E-02 2 -1000002 2 # BR(~g -> ~u_L* u ) 4.46872773E-02 2 2000002 -2 # BR(~g -> ~u_R ub) 4.46872773E-02 2 -2000002 2 # BR(~g -> ~u_R* u ) 2.08454202E-02 2 1000003 -3 # BR(~g -> ~s_L sb) 2.08454202E-02 2 -1000003 3 # BR(~g -> ~s_L* s ) 5.07075274E-02 2 2000003 -3 # BR(~g -> ~s_R sb) 5.07075274E-02 2 -2000003 3 # BR(~g -> ~s_R* s ) 2.89787767E-02 2 1000004 -4 # BR(~g -> ~c_L cb) 2.89787767E-02 2 -1000004 4 # BR(~g -> ~c_L* c ) 4.46872773E-02 2 2000004 -4 # BR(~g -> ~c_R cb) 4.46872773E-02 2 -2000004 4 # BR(~g -> ~c_R* c ) 1.05840237E-01 2 1000005 -5 # BR(~g -> ~b_1 bb) 1.05840237E-01 2 -1000005 5 # BR(~g -> ~b_1* b ) 5.56574805E-02 2 2000005 -5 # BR(~g -> ~b_2 bb) 5.56574805E-02 2 -2000005 5 # BR(~g -> ~b_2* b ) 4.80642793E-02 2 1000006 -6 # BR(~g -> ~t_1 tb) 4.80642793E-02 2 -1000006 6 # BR(~g -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~g -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~g -> ~t_2* t ) # # PDG Width DECAY 1000006 0.01E+00 # stop1 decays # BR NDA ID1 ID2 1.92947616E-01 2 1000022 6 # BR(~t_1 -> ~chi_10 t ) 1.17469211E-01 2 1000023 6 # BR(~t_1 -> ~chi_20 t ) 0.00000000E+00 2 1000025 6 # BR(~t_1 -> ~chi_30 t ) 0.00000000E+00 2 1000035 6 # BR(~t_1 -> ~chi_40 t ) 6.75747693E-01 2 1000024 5 # BR(~t_1 -> ~chi_1+ b ) 1.38354802E-02 2 1000037 5 # BR(~t_1 -> ~chi_2+ b ) 0.00000000E+00 2 1000021 6 # BR(~t_1 -> ~g t ) 0.00000000E+00 2 1000005 37 # BR(~t_1 -> ~b_1 H+) 0.00000000E+00 2 2000005 37 # BR(~t_1 -> ~b_2 H+) 0.00000000E+00 2 1000005 24 # BR(~t_1 -> ~b_1 W+) 0.00000000E+00 2 2000005 24 # BR(~t_1 -> ~b_2 W+) # # PDG Width DECAY 2000006 7.37313275E+00 # stop2 decays # BR NDA ID1 ID2 2.96825635E-02 2 1000022 6 # BR(~t_2 -> ~chi_10 t ) 8.68035358E-02 2 1000023 6 # BR(~t_2 -> ~chi_20 t ) 4.18408351E-02 2 1000025 6 # BR(~t_2 -> ~chi_30 t ) 1.93281647E-01 2 1000035 6 # BR(~t_2 -> ~chi_40 t ) 2.19632356E-01 2 1000024 5 # BR(~t_2 -> ~chi_1+ b ) 2.02206148E-01 2 1000037 5 # BR(~t_2 -> ~chi_2+ b ) 0.00000000E+00 2 1000021 6 # BR(~t_2 -> ~g t ) 3.66397706E-02 2 1000006 25 # BR(~t_2 -> ~t_1 h ) 0.00000000E+00 2 1000006 35 # BR(~t_2 -> ~t_1 H ) 0.00000000E+00 2 1000006 36 # BR(~t_2 -> ~t_1 A ) 0.00000000E+00 2 1000005 37 # BR(~t_2 -> ~b_1 H+) 0.00000000E+00 2 2000005 37 # BR(~t_2 -> ~b_2 H+) 1.89913144E-01 2 1000006 23 # BR(~t_2 -> ~t_1 Z ) 0.00000000E+00 2 1000005 24 # BR(~t_2 -> ~b_1 W+) 0.00000000E+00 2 2000005 24 # BR(~t_2 -> ~b_2 W+) # # PDG Width DECAY 1000005 3.73627601E+00 # sbottom1 decays # BR NDA ID1 ID2 4.43307074E-02 2 1000022 5 # BR(~b_1 -> ~chi_10 b ) 3.56319904E-01 2 1000023 5 # BR(~b_1 -> ~chi_20 b ) 5.16083795E-03 2 1000025 5 # BR(~b_1 -> ~chi_30 b ) 1.04105080E-02 2 1000035 5 # BR(~b_1 -> ~chi_40 b ) 4.45830064E-01 2 -1000024 6 # BR(~b_1 -> ~chi_1- t ) 0.00000000E+00 2 -1000037 6 # BR(~b_1 -> ~chi_2- t ) 0.00000000E+00 2 1000021 5 # BR(~b_1 -> ~g b ) 0.00000000E+00 2 1000006 -37 # BR(~b_1 -> ~t_1 H-) 0.00000000E+00 2 2000006 -37 # BR(~b_1 -> ~t_2 H-) 1.37947979E-01 2 1000006 -24 # BR(~b_1 -> ~t_1 W-) 0.00000000E+00 2 2000006 -24 # BR(~b_1 -> ~t_2 W-) # # PDG Width DECAY 2000005 8.01566294E-01 # sbottom2 decays # BR NDA ID1 ID2 2.86200590E-01 2 1000022 5 # BR(~b_2 -> ~chi_10 b ) 1.40315912E-01 2 1000023 5 # BR(~b_2 -> ~chi_20 b ) 5.32635592E-02 2 1000025 5 # BR(~b_2 -> ~chi_30 b ) 7.48748121E-02 2 1000035 5 # BR(~b_2 -> ~chi_40 b ) 1.79734294E-01 2 -1000024 6 # BR(~b_2 -> ~chi_1- t ) 0.00000000E+00 2 -1000037 6 # BR(~b_2 -> ~chi_2- t ) 0.00000000E+00 2 1000021 5 # BR(~b_2 -> ~g b ) 0.00000000E+00 2 1000005 25 # BR(~b_2 -> ~b_1 h ) 0.00000000E+00 2 1000005 35 # BR(~b_2 -> ~b_1 H ) 0.00000000E+00 2 1000005 36 # BR(~b_2 -> ~b_1 A ) 0.00000000E+00 2 1000006 -37 # BR(~b_2 -> ~t_1 H-) 0.00000000E+00 2 2000006 -37 # BR(~b_2 -> ~t_2 H-) 0.00000000E+00 2 1000005 23 # BR(~b_2 -> ~b_1 Z ) 2.65610832E-01 2 1000006 -24 # BR(~b_2 -> ~t_1 W-) 0.00000000E+00 2 2000006 -24 # BR(~b_2 -> ~t_2 W-) # # PDG Width DECAY 1000002 0.01E+00 # sup_L decays # BR NDA ID1 ID2 6.65240987E-03 2 1000022 2 # BR(~u_L -> ~chi_10 u) 3.19051458E-01 2 1000023 2 # BR(~u_L -> ~chi_20 u) 8.44929059E-04 2 1000025 2 # BR(~u_L -> ~chi_30 u) 1.03485173E-02 2 1000035 2 # BR(~u_L -> ~chi_40 u) 6.49499518E-01 2 1000024 1 # BR(~u_L -> ~chi_1+ d) 1.36031676E-02 2 1000037 1 # BR(~u_L -> ~chi_2+ d) 0.00000000E+00 2 1000021 2 # BR(~u_L -> ~g u) # # PDG Width DECAY 2000002 1.15297292E+00 # sup_R decays # BR NDA ID1 ID2 9.86377420E-01 2 1000022 2 # BR(~u_R -> ~chi_10 u) 8.46640647E-03 2 1000023 2 # BR(~u_R -> ~chi_20 u) 1.23894695E-03 2 1000025 2 # BR(~u_R -> ~chi_30 u) 3.91722611E-03 2 1000035 2 # BR(~u_R -> ~chi_40 u) 0.00000000E+00 2 1000024 1 # BR(~u_R -> ~chi_1+ d) 0.00000000E+00 2 1000037 1 # BR(~u_R -> ~chi_2+ d) 0.00000000E+00 2 1000021 2 # BR(~u_R -> ~g u) # # PDG Width DECAY 1000001 5.31278772E+00 # sdown_L decays # BR NDA ID1 ID2 2.32317969E-02 2 1000022 1 # BR(~d_L -> ~chi_10 d) 3.10235077E-01 2 1000023 1 # BR(~d_L -> ~chi_20 d) 1.52334771E-03 2 1000025 1 # BR(~d_L -> ~chi_30 d) 1.48849798E-02 2 1000035 1 # BR(~d_L -> ~chi_40 d) 6.06452481E-01 2 -1000024 2 # BR(~d_L -> ~chi_1- u) 4.36723179E-02 2 -1000037 2 # BR(~d_L -> ~chi_2- u) 0.00000000E+00 2 1000021 1 # BR(~d_L -> ~g d) # # PDG Width DECAY 2000001 2.85812308E-01 # sdown_R decays # BR NDA ID1 ID2 9.86529614E-01 2 1000022 1 # BR(~d_R -> ~chi_10 d) 8.44510350E-03 2 1000023 1 # BR(~d_R -> ~chi_20 d) 1.21172119E-03 2 1000025 1 # BR(~d_R -> ~chi_30 d) 3.81356102E-03 2 1000035 1 # BR(~d_R -> ~chi_40 d) 0.00000000E+00 2 -1000024 2 # BR(~d_R -> ~chi_1- u) 0.00000000E+00 2 -1000037 2 # BR(~d_R -> ~chi_2- u) 0.00000000E+00 2 1000021 1 # BR(~d_R -> ~g d) # # PDG Width DECAY 1000004 5.47719539E+00 # scharm_L decays # BR NDA ID1 ID2 6.65240987E-03 2 1000022 4 # BR(~c_L -> ~chi_10 c) 3.19051458E-01 2 1000023 4 # BR(~c_L -> ~chi_20 c) 8.44929059E-04 2 1000025 4 # BR(~c_L -> ~chi_30 c) 1.03485173E-02 2 1000035 4 # BR(~c_L -> ~chi_40 c) 6.49499518E-01 2 1000024 3 # BR(~c_L -> ~chi_1+ s) 1.36031676E-02 2 1000037 3 # BR(~c_L -> ~chi_2+ s) 0.00000000E+00 2 1000021 4 # BR(~c_L -> ~g c) # # PDG Width DECAY 2000004 1.15297292E+00 # scharm_R decays # BR NDA ID1 ID2 9.86377420E-01 2 1000022 4 # BR(~c_R -> ~chi_10 c) 8.46640647E-03 2 1000023 4 # BR(~c_R -> ~chi_20 c) 1.23894695E-03 2 1000025 4 # BR(~c_R -> ~chi_30 c) 3.91722611E-03 2 1000035 4 # BR(~c_R -> ~chi_40 c) 0.00000000E+00 2 1000024 3 # BR(~c_R -> ~chi_1+ s) 0.00000000E+00 2 1000037 3 # BR(~c_R -> ~chi_2+ s) 0.00000000E+00 2 1000021 4 # BR(~c_R -> ~g c) # # PDG Width DECAY 1000003 5.31278772E+00 # sstrange_L decays # BR NDA ID1 ID2 2.32317969E-02 2 1000022 3 # BR(~s_L -> ~chi_10 s) 3.10235077E-01 2 1000023 3 # BR(~s_L -> ~chi_20 s) 1.52334771E-03 2 1000025 3 # BR(~s_L -> ~chi_30 s) 1.48849798E-02 2 1000035 3 # BR(~s_L -> ~chi_40 s) 6.06452481E-01 2 -1000024 4 # BR(~s_L -> ~chi_1- c) 4.36723179E-02 2 -1000037 4 # BR(~s_L -> ~chi_2- c) 0.00000000E+00 2 1000021 3 # BR(~s_L -> ~g s) # # PDG Width DECAY 2000003 2.85812308E-01 # sstrange_R decays # BR NDA ID1 ID2 9.86529614E-01 2 1000022 3 # BR(~s_R -> ~chi_10 s) 8.44510350E-03 2 1000023 3 # BR(~s_R -> ~chi_20 s) 1.21172119E-03 2 1000025 3 # BR(~s_R -> ~chi_30 s) 3.81356102E-03 2 1000035 3 # BR(~s_R -> ~chi_40 s) 0.00000000E+00 2 -1000024 4 # BR(~s_R -> ~chi_1- c) 0.00000000E+00 2 -1000037 4 # BR(~s_R -> ~chi_2- c) 0.00000000E+00 2 1000021 3 # BR(~s_R -> ~g s) # # PDG Width DECAY 1000011 2.13682161E-01 # selectron_L decays # BR NDA ID1 ID2 5.73155386E-01 2 1000022 11 # BR(~e_L -> ~chi_10 e-) 1.64522579E-01 2 1000023 11 # BR(~e_L -> ~chi_20 e-) 0.00000000E+00 2 1000025 11 # BR(~e_L -> ~chi_30 e-) 0.00000000E+00 2 1000035 11 # BR(~e_L -> ~chi_40 e-) 2.62322035E-01 2 -1000024 12 # BR(~e_L -> ~chi_1- nu_e) 0.00000000E+00 2 -1000037 12 # BR(~e_L -> ~chi_2- nu_e) # # PDG Width DECAY 2000011 2.16121626E-01 # selectron_R decays # BR NDA ID1 ID2 1.00000000E+00 2 1000022 11 # BR(~e_R -> ~chi_10 e-) 0.00000000E+00 2 1000023 11 # BR(~e_R -> ~chi_20 e-) 0.00000000E+00 2 1000025 11 # BR(~e_R -> ~chi_30 e-) 0.00000000E+00 2 1000035 11 # BR(~e_R -> ~chi_40 e-) 0.00000000E+00 2 -1000024 12 # BR(~e_R -> ~chi_1- nu_e) 0.00000000E+00 2 -1000037 12 # BR(~e_R -> ~chi_2- nu_e) # # PDG Width DECAY 1000013 2.13682161E-01 # smuon_L decays # BR NDA ID1 ID2 5.73155386E-01 2 1000022 13 # BR(~mu_L -> ~chi_10 mu-) 1.64522579E-01 2 1000023 13 # BR(~mu_L -> ~chi_20 mu-) 0.00000000E+00 2 1000025 13 # BR(~mu_L -> ~chi_30 mu-) 0.00000000E+00 2 1000035 13 # BR(~mu_L -> ~chi_40 mu-) 2.62322035E-01 2 -1000024 14 # BR(~mu_L -> ~chi_1- nu_mu) 0.00000000E+00 2 -1000037 14 # BR(~mu_L -> ~chi_2- nu_mu) # # PDG Width DECAY 2000013 2.16121626E-01 # smuon_R decays # BR NDA ID1 ID2 1.00000000E+00 2 1000022 13 # BR(~mu_R -> ~chi_10 mu-) 0.00000000E+00 2 1000023 13 # BR(~mu_R -> ~chi_20 mu-) 0.00000000E+00 2 1000025 13 # BR(~mu_R -> ~chi_30 mu-) 0.00000000E+00 2 1000035 13 # BR(~mu_R -> ~chi_40 mu-) 0.00000000E+00 2 -1000024 14 # BR(~mu_R -> ~chi_1- nu_mu) 0.00000000E+00 2 -1000037 14 # BR(~mu_R -> ~chi_2- nu_mu) # # PDG Width DECAY 1000015 1.48327268E-01 # stau_1 decays # BR NDA ID1 ID2 1.00000000E+00 2 1000022 15 # BR(~tau_1 -> ~chi_10 tau-) 0.00000000E+00 2 1000023 15 # BR(~tau_1 -> ~chi_20 tau-) 0.00000000E+00 2 1000025 15 # BR(~tau_1 -> ~chi_30 tau-) 0.00000000E+00 2 1000035 15 # BR(~tau_1 -> ~chi_40 tau-) 0.00000000E+00 2 -1000024 16 # BR(~tau_1 -> ~chi_1- nu_tau) 0.00000000E+00 2 -1000037 16 # BR(~tau_1 -> ~chi_2- nu_tau) 0.00000000E+00 2 1000016 -37 # BR(~tau_1 -> ~nu_tauL H-) 0.00000000E+00 2 1000016 -24 # BR(~tau_1 -> ~nu_tauL W-) # # PDG Width DECAY 2000015 2.69906096E-01 # stau_2 decays # BR NDA ID1 ID2 5.96653046E-01 2 1000022 15 # BR(~tau_2 -> ~chi_10 tau-) 1.54536760E-01 2 1000023 15 # BR(~tau_2 -> ~chi_20 tau-) 0.00000000E+00 2 1000025 15 # BR(~tau_2 -> ~chi_30 tau-) 0.00000000E+00 2 1000035 15 # BR(~tau_2 -> ~chi_40 tau-) 2.48810195E-01 2 -1000024 16 # BR(~tau_2 -> ~chi_1- nu_tau) 0.00000000E+00 2 -1000037 16 # BR(~tau_2 -> ~chi_2- nu_tau) 0.00000000E+00 2 1000016 -37 # BR(~tau_2 -> ~nu_tauL H-) 0.00000000E+00 2 1000016 -24 # BR(~tau_2 -> ~nu_tauL W-) 0.00000000E+00 2 1000015 25 # BR(~tau_2 -> ~tau_1 h) 0.00000000E+00 2 1000015 35 # BR(~tau_2 -> ~tau_1 H) 0.00000000E+00 2 1000015 36 # BR(~tau_2 -> ~tau_1 A) 0.00000000E+00 2 1000015 23 # BR(~tau_2 -> ~tau_1 Z) # # PDG Width DECAY 1000012 1.49881634E-01 # snu_eL decays # BR NDA ID1 ID2 9.77700764E-01 2 1000022 12 # BR(~nu_eL -> ~chi_10 nu_e) 8.11554922E-03 2 1000023 12 # BR(~nu_eL -> ~chi_20 nu_e) 0.00000000E+00 2 1000025 12 # BR(~nu_eL -> ~chi_30 nu_e) 0.00000000E+00 2 1000035 12 # BR(~nu_eL -> ~chi_40 nu_e) 1.41836867E-02 2 1000024 11 # BR(~nu_eL -> ~chi_1+ e-) 0.00000000E+00 2 1000037 11 # BR(~nu_eL -> ~chi_2+ e-) # # PDG Width DECAY 1000014 1.49881634E-01 # snu_muL decays # BR NDA ID1 ID2 9.77700764E-01 2 1000022 14 # BR(~nu_muL -> ~chi_10 nu_mu) 8.11554922E-03 2 1000023 14 # BR(~nu_muL -> ~chi_20 nu_mu) 0.00000000E+00 2 1000025 14 # BR(~nu_muL -> ~chi_30 nu_mu) 0.00000000E+00 2 1000035 14 # BR(~nu_muL -> ~chi_40 nu_mu) 1.41836867E-02 2 1000024 13 # BR(~nu_muL -> ~chi_1+ mu-) 0.00000000E+00 2 1000037 13 # BR(~nu_muL -> ~chi_2+ mu-) # # PDG Width DECAY 1000016 1.47518977E-01 # snu_tauL decays # BR NDA ID1 ID2 9.85994529E-01 2 1000022 16 # BR(~nu_tauL -> ~chi_10 nu_tau) 6.25129612E-03 2 1000023 16 # BR(~nu_tauL -> ~chi_20 nu_tau) 0.00000000E+00 2 1000025 16 # BR(~nu_tauL -> ~chi_30 nu_tau) 0.00000000E+00 2 1000035 16 # BR(~nu_tauL -> ~chi_40 nu_tau) 7.75417479E-03 2 1000024 15 # BR(~nu_tauL -> ~chi_1+ tau-) 0.00000000E+00 2 1000037 15 # BR(~nu_tauL -> ~chi_2+ tau-) 0.00000000E+00 2 -1000015 -37 # BR(~nu_tauL -> ~tau_1+ H-) 0.00000000E+00 2 -2000015 -37 # BR(~nu_tauL -> ~tau_2+ H-) 0.00000000E+00 2 -1000015 -24 # BR(~nu_tauL -> ~tau_1+ W-) 0.00000000E+00 2 -2000015 -24 # BR(~nu_tauL -> ~tau_2+ W-) # # PDG Width DECAY 1000024 1.70414503E-02 # chargino1+ decays # BR NDA ID1 ID2 0.00000000E+00 2 1000002 -1 # BR(~chi_1+ -> ~u_L db) 0.00000000E+00 2 2000002 -1 # BR(~chi_1+ -> ~u_R db) 0.00000000E+00 2 -1000001 2 # BR(~chi_1+ -> ~d_L* u ) 0.00000000E+00 2 -2000001 2 # BR(~chi_1+ -> ~d_R* u ) 0.00000000E+00 2 1000004 -3 # BR(~chi_1+ -> ~c_L sb) 0.00000000E+00 2 2000004 -3 # BR(~chi_1+ -> ~c_R sb) 0.00000000E+00 2 -1000003 4 # BR(~chi_1+ -> ~s_L* c ) 0.00000000E+00 2 -2000003 4 # BR(~chi_1+ -> ~s_R* c ) 0.00000000E+00 2 1000006 -5 # BR(~chi_1+ -> ~t_1 bb) 0.00000000E+00 2 2000006 -5 # BR(~chi_1+ -> ~t_2 bb) 0.00000000E+00 2 -1000005 6 # BR(~chi_1+ -> ~b_1* t ) 0.00000000E+00 2 -2000005 6 # BR(~chi_1+ -> ~b_2* t ) 0.00000000E+00 2 1000012 -11 # BR(~chi_1+ -> ~nu_eL e+ ) 0.00000000E+00 2 1000014 -13 # BR(~chi_1+ -> ~nu_muL mu+ ) 0.00000000E+00 2 1000016 -15 # BR(~chi_1+ -> ~nu_tau1 tau+) 0.00000000E+00 2 -1000011 12 # BR(~chi_1+ -> ~e_L+ nu_e) 0.00000000E+00 2 -2000011 12 # BR(~chi_1+ -> ~e_R+ nu_e) 0.00000000E+00 2 -1000013 14 # BR(~chi_1+ -> ~mu_L+ nu_mu) 0.00000000E+00 2 -2000013 14 # BR(~chi_1+ -> ~mu_R+ nu_mu) 9.25161117E-01 2 -1000015 16 # BR(~chi_1+ -> ~tau_1+ nu_tau) 0.00000000E+00 2 -2000015 16 # BR(~chi_1+ -> ~tau_2+ nu_tau) 7.48388828E-02 2 1000022 24 # BR(~chi_1+ -> ~chi_10 W+) 0.00000000E+00 2 1000023 24 # BR(~chi_1+ -> ~chi_20 W+) 0.00000000E+00 2 1000025 24 # BR(~chi_1+ -> ~chi_30 W+) 0.00000000E+00 2 1000035 24 # BR(~chi_1+ -> ~chi_40 W+) 0.00000000E+00 2 1000022 37 # BR(~chi_1+ -> ~chi_10 H+) 0.00000000E+00 2 1000023 37 # BR(~chi_1+ -> ~chi_20 H+) 0.00000000E+00 2 1000025 37 # BR(~chi_1+ -> ~chi_30 H+) 0.00000000E+00 2 1000035 37 # BR(~chi_1+ -> ~chi_40 H+) # # PDG Width DECAY 1000037 2.48689510E+00 # chargino2+ decays # BR NDA ID1 ID2 0.00000000E+00 2 1000002 -1 # BR(~chi_2+ -> ~u_L db) 0.00000000E+00 2 2000002 -1 # BR(~chi_2+ -> ~u_R db) 0.00000000E+00 2 -1000001 2 # BR(~chi_2+ -> ~d_L* u ) 0.00000000E+00 2 -2000001 2 # BR(~chi_2+ -> ~d_R* u ) 0.00000000E+00 2 1000004 -3 # BR(~chi_2+ -> ~c_L sb) 0.00000000E+00 2 2000004 -3 # BR(~chi_2+ -> ~c_R sb) 0.00000000E+00 2 -1000003 4 # BR(~chi_2+ -> ~s_L* c ) 0.00000000E+00 2 -2000003 4 # BR(~chi_2+ -> ~s_R* c ) 0.00000000E+00 2 1000006 -5 # BR(~chi_2+ -> ~t_1 bb) 0.00000000E+00 2 2000006 -5 # BR(~chi_2+ -> ~t_2 bb) 0.00000000E+00 2 -1000005 6 # BR(~chi_2+ -> ~b_1* t ) 0.00000000E+00 2 -2000005 6 # BR(~chi_2+ -> ~b_2* t ) 2.00968837E-02 2 1000012 -11 # BR(~chi_2+ -> ~nu_eL e+ ) 2.00968837E-02 2 1000014 -13 # BR(~chi_2+ -> ~nu_muL mu+ ) 2.74507395E-02 2 1000016 -15 # BR(~chi_2+ -> ~nu_tau1 tau+) 5.20406111E-02 2 -1000011 12 # BR(~chi_2+ -> ~e_L+ nu_e) 0.00000000E+00 2 -2000011 12 # BR(~chi_2+ -> ~e_R+ nu_e) 5.20406111E-02 2 -1000013 14 # BR(~chi_2+ -> ~mu_L+ nu_mu) 0.00000000E+00 2 -2000013 14 # BR(~chi_2+ -> ~mu_R+ nu_mu) 2.82859898E-04 2 -1000015 16 # BR(~chi_2+ -> ~tau_1+ nu_tau) 5.66729336E-02 2 -2000015 16 # BR(~chi_2+ -> ~tau_2+ nu_tau) 2.31513269E-01 2 1000024 23 # BR(~chi_2+ -> ~chi_1+ Z ) 6.76715120E-02 2 1000022 24 # BR(~chi_2+ -> ~chi_10 W+) 2.93654849E-01 2 1000023 24 # BR(~chi_2+ -> ~chi_20 W+) 0.00000000E+00 2 1000025 24 # BR(~chi_2+ -> ~chi_30 W+) 0.00000000E+00 2 1000035 24 # BR(~chi_2+ -> ~chi_40 W+) 1.78478848E-01 2 1000024 25 # BR(~chi_2+ -> ~chi_1+ h ) 0.00000000E+00 2 1000024 35 # BR(~chi_2+ -> ~chi_1+ H ) 0.00000000E+00 2 1000024 36 # BR(~chi_2+ -> ~chi_1+ A ) 0.00000000E+00 2 1000022 37 # BR(~chi_2+ -> ~chi_10 H+) 0.00000000E+00 2 1000023 37 # BR(~chi_2+ -> ~chi_20 H+) 0.00000000E+00 2 1000025 37 # BR(~chi_2+ -> ~chi_30 H+) 0.00000000E+00 2 1000035 37 # BR(~chi_2+ -> ~chi_40 H+) # # PDG Width DECAY 1000022 0.00000000E+00 # neutralino1 decays # # PDG Width DECAY 1000023 2.07770048E-02 # neutralino2 decays # BR NDA ID1 ID2 0.00000000E+00 2 1000022 23 # BR(~chi_20 -> ~chi_10 Z ) 0.00000000E+00 2 1000024 -24 # BR(~chi_20 -> ~chi_1+ W-) 0.00000000E+00 2 -1000024 24 # BR(~chi_20 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_20 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_20 -> ~chi_2- W+) 0.00000000E+00 2 1000022 25 # BR(~chi_20 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_20 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_20 -> ~chi_10 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_20 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_20 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_20 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_20 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_20 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_20 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_20 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_20 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_20 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_20 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_20 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_20 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_20 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_20 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_20 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_20 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_20 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_20 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_20 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_20 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_20 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_20 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_20 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_20 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_20 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_20 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_20 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_20 -> ~b_2* b ) 0.00000000E+00 2 1000011 -11 # BR(~chi_20 -> ~e_L- e+) 0.00000000E+00 2 -1000011 11 # BR(~chi_20 -> ~e_L+ e-) 2.95071995E-02 2 2000011 -11 # BR(~chi_20 -> ~e_R- e+) 2.95071995E-02 2 -2000011 11 # BR(~chi_20 -> ~e_R+ e-) 0.00000000E+00 2 1000013 -13 # BR(~chi_20 -> ~mu_L- mu+) 0.00000000E+00 2 -1000013 13 # BR(~chi_20 -> ~mu_L+ mu-) 2.95071995E-02 2 2000013 -13 # BR(~chi_20 -> ~mu_R- mu+) 2.95071995E-02 2 -2000013 13 # BR(~chi_20 -> ~mu_R+ mu-) 4.40985601E-01 2 1000015 -15 # BR(~chi_20 -> ~tau_1- tau+) 4.40985601E-01 2 -1000015 15 # BR(~chi_20 -> ~tau_1+ tau-) 0.00000000E+00 2 2000015 -15 # BR(~chi_20 -> ~tau_2- tau+) 0.00000000E+00 2 -2000015 15 # BR(~chi_20 -> ~tau_2+ tau-) 0.00000000E+00 2 1000012 -12 # BR(~chi_20 -> ~nu_eL nu_eb) 0.00000000E+00 2 -1000012 12 # BR(~chi_20 -> ~nu_eL* nu_e ) 0.00000000E+00 2 1000014 -14 # BR(~chi_20 -> ~nu_muL nu_mub) 0.00000000E+00 2 -1000014 14 # BR(~chi_20 -> ~nu_muL* nu_mu ) 0.00000000E+00 2 1000016 -16 # BR(~chi_20 -> ~nu_tau1 nu_taub) 0.00000000E+00 2 -1000016 16 # BR(~chi_20 -> ~nu_tau1* nu_tau ) # # PDG Width DECAY 1000025 1.91598495E+00 # neutralino3 decays # BR NDA ID1 ID2 1.13226601E-01 2 1000022 23 # BR(~chi_30 -> ~chi_10 Z ) 2.11969194E-01 2 1000023 23 # BR(~chi_30 -> ~chi_20 Z ) 2.95329778E-01 2 1000024 -24 # BR(~chi_30 -> ~chi_1+ W-) 2.95329778E-01 2 -1000024 24 # BR(~chi_30 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_30 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_30 -> ~chi_2- W+) 2.13076490E-02 2 1000022 25 # BR(~chi_30 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_30 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_30 -> ~chi_10 A ) 1.24538329E-02 2 1000023 25 # BR(~chi_30 -> ~chi_20 h ) 0.00000000E+00 2 1000023 35 # BR(~chi_30 -> ~chi_20 H ) 0.00000000E+00 2 1000023 36 # BR(~chi_30 -> ~chi_20 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_30 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_30 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_30 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_30 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_30 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_30 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_30 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_30 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_30 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_30 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_30 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_30 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_30 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_30 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_30 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_30 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_30 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_30 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_30 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_30 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_30 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_30 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_30 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_30 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_30 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_30 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_30 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_30 -> ~b_2* b ) 5.57220455E-04 2 1000011 -11 # BR(~chi_30 -> ~e_L- e+) 5.57220455E-04 2 -1000011 11 # BR(~chi_30 -> ~e_L+ e-) 1.25266782E-03 2 2000011 -11 # BR(~chi_30 -> ~e_R- e+) 1.25266782E-03 2 -2000011 11 # BR(~chi_30 -> ~e_R+ e-) 5.57220455E-04 2 1000013 -13 # BR(~chi_30 -> ~mu_L- mu+) 5.57220455E-04 2 -1000013 13 # BR(~chi_30 -> ~mu_L+ mu-) 1.25266782E-03 2 2000013 -13 # BR(~chi_30 -> ~mu_R- mu+) 1.25266782E-03 2 -2000013 13 # BR(~chi_30 -> ~mu_R+ mu-) 5.26279239E-03 2 1000015 -15 # BR(~chi_30 -> ~tau_1- tau+) 5.26279239E-03 2 -1000015 15 # BR(~chi_30 -> ~tau_1+ tau-) 6.72814564E-03 2 2000015 -15 # BR(~chi_30 -> ~tau_2- tau+) 6.72814564E-03 2 -2000015 15 # BR(~chi_30 -> ~tau_2+ tau-) 3.18920485E-03 2 1000012 -12 # BR(~chi_30 -> ~nu_eL nu_eb) 3.18920485E-03 2 -1000012 12 # BR(~chi_30 -> ~nu_eL* nu_e ) 3.18920485E-03 2 1000014 -14 # BR(~chi_30 -> ~nu_muL nu_mub) 3.18920485E-03 2 -1000014 14 # BR(~chi_30 -> ~nu_muL* nu_mu ) 3.20245934E-03 2 1000016 -16 # BR(~chi_30 -> ~nu_tau1 nu_taub) 3.20245934E-03 2 -1000016 16 # BR(~chi_30 -> ~nu_tau1* nu_tau ) # # PDG Width DECAY 1000035 2.58585079E+00 # neutralino4 decays # BR NDA ID1 ID2 2.15369294E-02 2 1000022 23 # BR(~chi_40 -> ~chi_10 Z ) 1.85499971E-02 2 1000023 23 # BR(~chi_40 -> ~chi_20 Z ) 0.00000000E+00 2 1000025 23 # BR(~chi_40 -> ~chi_30 Z ) 2.49541430E-01 2 1000024 -24 # BR(~chi_40 -> ~chi_1+ W-) 2.49541430E-01 2 -1000024 24 # BR(~chi_40 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_40 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_40 -> ~chi_2- W+) 6.93213268E-02 2 1000022 25 # BR(~chi_40 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_40 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_40 -> ~chi_10 A ) 1.47602336E-01 2 1000023 25 # BR(~chi_40 -> ~chi_20 h ) 0.00000000E+00 2 1000023 35 # BR(~chi_40 -> ~chi_20 H ) 0.00000000E+00 2 1000023 36 # BR(~chi_40 -> ~chi_20 A ) 0.00000000E+00 2 1000025 25 # BR(~chi_40 -> ~chi_30 h ) 0.00000000E+00 2 1000025 35 # BR(~chi_40 -> ~chi_30 H ) 0.00000000E+00 2 1000025 36 # BR(~chi_40 -> ~chi_30 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_40 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_40 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_40 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_40 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_40 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_40 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_40 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_40 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_40 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_40 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_40 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_40 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_40 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_40 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_40 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_40 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_40 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_40 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_40 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_40 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_40 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_40 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_40 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_40 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_40 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_40 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_40 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_40 -> ~b_2* b ) 9.64835418E-03 2 1000011 -11 # BR(~chi_40 -> ~e_L- e+) 9.64835418E-03 2 -1000011 11 # BR(~chi_40 -> ~e_L+ e-) 3.75684470E-03 2 2000011 -11 # BR(~chi_40 -> ~e_R- e+) 3.75684470E-03 2 -2000011 11 # BR(~chi_40 -> ~e_R+ e-) 9.64835418E-03 2 1000013 -13 # BR(~chi_40 -> ~mu_L- mu+) 9.64835418E-03 2 -1000013 13 # BR(~chi_40 -> ~mu_L+ mu-) 3.75684470E-03 2 2000013 -13 # BR(~chi_40 -> ~mu_R- mu+) 3.75684470E-03 2 -2000013 13 # BR(~chi_40 -> ~mu_R+ mu-) 2.68215241E-03 2 1000015 -15 # BR(~chi_40 -> ~tau_1- tau+) 2.68215241E-03 2 -1000015 15 # BR(~chi_40 -> ~tau_1+ tau-) 1.62289809E-02 2 2000015 -15 # BR(~chi_40 -> ~tau_2- tau+) 1.62289809E-02 2 -2000015 15 # BR(~chi_40 -> ~tau_2+ tau-) 2.53796547E-02 2 1000012 -12 # BR(~chi_40 -> ~nu_eL nu_eb) 2.53796547E-02 2 -1000012 12 # BR(~chi_40 -> ~nu_eL* nu_e ) 2.53796547E-02 2 1000014 -14 # BR(~chi_40 -> ~nu_muL nu_mub) 2.53796547E-02 2 -1000014 14 # BR(~chi_40 -> ~nu_muL* nu_mu ) 2.54724352E-02 2 1000016 -16 # BR(~chi_40 -> ~nu_tau1 nu_taub) 2.54724352E-02 2 -1000016 16 # BR(~chi_40 -> ~nu_tau1* nu_tau ) pythia8-8.1.80.orig/examples/main03.cc0000644000175000017500000000524712217346163015562 0ustar sunsun// main03.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how different processes can be selected and studied. // All input is specified in the main03.cmnd file. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator. Pythia pythia; // Shorthand for the event record in pythia. Event& event = pythia.event; // Read in commands from external file. pythia.readFile("main03.cmnd"); // Extract settings to be used in the main program. int nEvent = pythia.mode("Main:numberOfEvents"); int nAbort = pythia.mode("Main:timesAllowErrors"); // Initialize. pythia.init(); // Book histograms. Hist pThard("process pT scale", 100, 0., 500.); Hist nFinal("final particle multiplicity", 100, -0.5, 1599.5); Hist nCharged("charged particle multiplicity", 100, -0.5, 799.5); Hist dndy("dn/dy for charged particles", 100, -10., 10.); Hist dndeta("dn/d(eta) for charged particles", 100, -10., 10.); Hist dndpT("dn/dpT for charged particles", 100, 0., 10.); Hist epCons("deviation from energy-momentum conservation", 100, 0., 1e-6); // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if many failures. if (!pythia.next()) { if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Fill hard scale of event. pThard.fill( pythia.info.pTHat() ); // Loop over final particles in the event. int nFin = 0; int nChg = 0; Vec4 pSum; for (int i = 0; i < event.size(); ++i) if (event[i].isFinal()) { // Analyze all particles. nFin++; pSum += event[i].p(); // Analyze charged particles and fill histograms. if (event[i].isCharged()) { ++nChg; dndy.fill( event[i].y() ); dndeta.fill( event[i].eta() ); dndpT.fill( event[i].pT() ); } // End of particle loop. Fill global properties. } nFinal.fill( nFin ); nCharged.fill( nChg ); pSum /= event[0].e(); double epDev = abs(pSum.e() - 1.) + abs(pSum.px()) + abs(pSum.py()) + abs(pSum.pz()); epCons.fill(epDev); // End of event loop. } // Final statistics. Normalize and output histograms. pythia.stat(); dndy *= 5. / nEvent; dndeta *= 5. / nEvent; dndpT *= 10. / nEvent; cout << pThard << nFinal << nCharged << dndy << dndeta << dndpT << epCons; // Done. return 0; } pythia8-8.1.80.orig/examples/main81.cc0000644000175000017500000001323612217346167015571 0ustar sunsun// main81.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This program is written by Stefan Prestel. // It illustrates how to do CKKW-L merging, // see the Matrix Element Merging page in the online manual. #include "Pythia8/Pythia.h" using namespace Pythia8; // Functions for histogramming #include "fastjet/PseudoJet.hh" #include "fastjet/ClusterSequence.hh" #include "fastjet/CDFMidPointPlugin.hh" #include "fastjet/CDFJetCluPlugin.hh" #include "fastjet/D0RunIIConePlugin.hh" //========================================================================== // Find the Durham kT separation of the clustering from // nJetMin --> nJetMin-1 jets in the input event double pTfirstJet( const Event& event, int nJetMin, double Rparam) { double yPartonMax = 4.; // Fastjet analysis - select algorithm and parameters fastjet::Strategy strategy = fastjet::Best; fastjet::RecombinationScheme recombScheme = fastjet::E_scheme; fastjet::JetDefinition *jetDef = NULL; // For hadronic collision, use hadronic Durham kT measure if(event[3].colType() != 0 || event[4].colType() != 0) jetDef = new fastjet::JetDefinition(fastjet::kt_algorithm, Rparam, recombScheme, strategy); // For e+e- collision, use e+e- Durham kT measure else jetDef = new fastjet::JetDefinition(fastjet::ee_kt_algorithm, recombScheme, strategy); // Fastjet input std::vector fjInputs; // Reset Fastjet input fjInputs.resize(0); // Loop over event record to decide what to pass to FastJet for (int i = 0; i < event.size(); ++i) { // (Final state && coloured+photons) only! if ( !event[i].isFinal() || event[i].isLepton() || event[i].id() == 23 || abs(event[i].id()) == 24 || abs(event[i].y()) > yPartonMax) continue; // Store as input to Fastjet fjInputs.push_back( fastjet::PseudoJet (event[i].px(), event[i].py(), event[i].pz(),event[i].e() ) ); } // Do nothing for empty input if (int(fjInputs.size()) == 0) { delete jetDef; return 0.0; } // Run Fastjet algorithm fastjet::ClusterSequence clustSeq(fjInputs, *jetDef); // Extract kT of first clustering double pTFirst = sqrt(clustSeq.exclusive_dmerge_max(nJetMin-1)); delete jetDef; // Return kT return pTFirst; } //========================================================================== // Example main programm to illustrate merging int main( int argc, char* argv[] ){ // Check that correct number of command-line arguments if (argc != 4) { cerr << " Unexpected number of command-line arguments ("< 2212 2212 3.50000E+03 3.50000E+03 -1 -1 -1 -1 3 1 9.62391E+03 1.19770E+01 1.00000E+00 666 6 666 1.00000E+00 1.08102E+01 -1.00000E+00 1.91870E-01 2 -1 0 0 501 0 0.000000000E+00 0.000000000E+00 1.223562932E+03 1.223562932E+03 0.000000000E+00 0.00000E+00 9.000E+00 -1 -1 0 0 0 511 0.000000000E+00 0.000000000E+00 -1.736171058E+00 1.736171058E+00 0.000000000E+00 0.00000E+00 9.000E+00 24 2 1 2 0 0 3.932753134E+00 -1.006945456E+01 1.145984662E+03 1.148690458E+03 7.805167033E+01 0.00000E+00 9.000E+00 -11 1 3 3 0 0 1.535353801E+01 -4.194455050E+01 6.041563996E+02 6.058052754E+02 5.108846754E-04 0.00000E+00 9.000E+00 12 1 3 3 0 0 -1.142078487E+01 3.187509593E+01 5.418282621E+02 5.428851828E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 501 511 -3.932753134E+00 1.006945456E+01 7.584209883E+01 7.660864454E+01 1.907348633E-06 0.00000E+00 9.000E+00 6 666 1.00000E+00 9.68455E+00 -1.00000E+00 1.97321E-01 2 -1 0 0 501 0 0.000000000E+00 0.000000000E+00 4.093279891E+01 4.093279891E+01 0.000000000E+00 0.00000E+00 9.000E+00 -1 -1 0 0 0 511 0.000000000E+00 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1.179968763E+02 8.104092112E+01 0.00000E+00 9.000E+00 11 1 3 3 0 0 -3.959997318E+01 -2.184036454E+00 2.492761123E+01 4.684350214E+01 5.110003775E-04 0.00000E+00 9.000E+00 -12 1 3 3 0 0 3.707919903E+01 -2.175515014E+00 6.068939598E+01 7.115337414E+01 1.507891493E-06 0.00000E+00 9.000E+00 21 1 1 2 511 501 2.520774147E+00 4.359551468E+00 -3.593765406E+00 6.186690642E+00 9.424321831E-08 0.00000E+00 9.000E+00 6 666 1.00000E+00 1.74748E+00 -1.00000E+00 3.92585E-01 1 -1 0 0 501 0 0.000000000E+00 0.000000000E+00 1.693607755E+02 1.693607755E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 511 501 0.000000000E+00 0.000000000E+00 -2.581118363E+01 2.581118363E+01 0.000000000E+00 0.00000E+00 9.000E+00 -24 2 1 2 0 0 6.303165629E-01 -1.629838542E+00 1.605810456E+02 1.780510920E+02 7.689515903E+01 0.00000E+00 9.000E+00 11 1 3 3 0 0 2.585048594E+01 1.469515965E+01 1.360608012E+02 1.392721687E+02 5.109950380E-04 0.00000E+00 9.000E+00 -12 1 3 3 0 0 -2.522016937E+01 -1.632499820E+01 2.452024441E+01 3.877892334E+01 8.920806376E-07 0.00000E+00 9.000E+00 2 1 1 2 511 0 -6.303165629E-01 1.629838542E+00 -1.703145377E+01 1.712086710E+01 6.743495762E-07 0.00000E+00 9.000E+00 6 666 1.00000E+00 7.28934E+00 -1.00000E+00 2.13028E-01 1 -1 0 0 501 0 0.000000000E+00 0.000000000E+00 2.118283831E+02 2.118283831E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 511 501 0.000000000E+00 0.000000000E+00 -2.334646142E+01 2.334646142E+01 0.000000000E+00 0.00000E+00 9.000E+00 -24 2 1 2 0 0 -3.665688238E+00 6.300573186E+00 2.026738963E+02 2.192203268E+02 8.323285980E+01 0.00000E+00 9.000E+00 11 1 3 3 0 0 -7.572470176E+00 3.595366166E+00 2.101742438E+02 2.103413458E+02 5.109914783E-04 0.00000E+00 9.000E+00 -12 1 3 3 0 0 3.906781938E+00 2.705207020E+00 -7.500347573E+00 8.878981014E+00 6.690604782E-07 0.00000E+00 9.000E+00 4 1 1 2 511 0 3.665688238E+00 -6.300573186E+00 -1.419197460E+01 1.595451773E+01 2.920019320E-07 0.00000E+00 9.000E+00 pythia8-8.1.80.orig/examples/main25.lhe0000644000175000017500000007442312217346165015755 0ustar sunsun # Warning: this file has been mercilessly hacked in order to test # read-in of exotic LHEF color structures and does not in any way # yield physical cross sections or process combinations. # Event 0: single-stop production (through RPV), without stop decay # Event 1: single-antistop production (through RPV), without stop decay # Event 2: single-stop production (through RPV), including RPV stop decay # Event 3: single-antistop production (through RPV), including RPV stop decay # Event 4: color-sextet example # Event 5-9: copies of 1-5, to test whether any failures are repeated or not # Event 10-15: examples with ME-generated BNV tbar->qq' decays and c.c. # Event 16-19: same as 10-15, but without intermediate tops in event record
      Block QNUMBERS 9000006 # sextet 1 4 # 3 times electric charge 2 1 # number of spin states (2S+1) 3 6 # colour rep (1: singlet, 3: triplet, 8: octet) 4 1 # Particle/Antiparticle distinction (0=own anti) DECAY 9000006 1.0 1.0 2 2 2 # BLOCK MODSEL # Model selection 1 1 # # BLOCK SMINPUTS # Standard Model inputs 1 1.27908957E+02 # alpha_em^-1(M_Z)^MSbar 2 1.16637000E-05 # G_F [GeV^-2] 3 1.17200000E-01 # alpha_S(M_Z)^MSbar 4 9.11876000E+01 # M_Z pole mass 5 4.21400000E+00 # mb(mb)^MSbar 6 1.75000000E+02 # mt pole mass 7 1.77700000E+00 # mtau pole mass # BLOCK MINPAR # Input parameters - minimal models 1 1.00000000E+02 # m0 2 2.50000000E+02 # m12 3 1.00000000E+01 # tanb 4 1.00000000E+00 # sign(mu) 5 -1.00000000E+02 # A0 # BLOCK MASS # Mass Spectrum # PDG code mass particle 5 4.83960131E+00 # b-quark pole mass calculated from mb(mb)_Msbar 6 1.75000000E+02 # t-quark 24 7.98255860E+01 # W+ 25 1.10864387E+02 # h 35 3.98301591E+02 # H 36 3.97919472E+02 # A 37 4.06256283E+02 # H+ 1000001 1.00000000E+04 # ~d_L 2000001 1.00000000E+04 # ~d_R 1000002 1.00000000E+03 # ~u_L 2000002 1.00000000E+03 # ~u_R 1000003 1.00000000E+04 # ~s_L 2000003 1.00000000E+04 # ~s_R 1000004 1.00000000E+03 # ~c_L 2000004 1.00000000E+03 # ~c_R 1000005 1.00000000E+04 # ~b_1 2000005 1.00000000E+04 # ~b_2 1000006 1.00000000E+04 # ~t_1 2000006 1.00000000E+04 # ~t_2 1000011 2.02759518E+04 # ~e_L 2000011 2.44071249E+04 # ~e_R 1000012 1.85089670E+04 # ~nu_eL 1000013 2.02759518E+04 # ~mu_L 2000013 2.44071249E+04 # ~mu_R 1000014 1.85089670E+04 # ~nu_muL 1000015 2.34518561E+04 # ~tau_1 2000015 2.06687916E+04 # ~tau_2 1000016 2.84540383E+04 # ~nu_tauL 1000021 7.00000000E+01 # ~g 1000022 4.00000000E+01 # ~chi_10 1000023 6.00000000E+01 # ~chi_20 1000025 7.00000000E+01 # ~chi_30 1000035 8.00000000E+01 # ~chi_40 1000024 1.81692495E+04 # ~chi_1+ 1000037 2.78328056E+04 # ~chi_2+ 9000006 5.000000e+02 # MSIX # BLOCK NMIX # Neutralino Mixing Matrix 1 1 1.00000000E+00 # N_11 1 2 0.00000000E+00 # N_12 1 3 0.00000000E+00 # N_13 1 4 0.00000000E+00 # N_14 2 1 0.00000000E+00 # N_21 2 2 1.00000000E+00 # N_22 2 3 0.00000000E+00 # N_23 2 4 0.00000000E+00 # N_24 3 1 0.00000000E+00 # N_31 3 2 0.00000000E+00 # N_32 3 3 1.00000000E+00 # N_33 3 4 0.00000000E+00 # N_34 4 1 0.00000000E+00 # N_41 4 2 0.00000000E+00 # N_42 4 3 0.00000000E+00 # N_43 4 4 1.00000000E+00 # N_44 # BLOCK UMIX # Chargino Mixing Matrix U 1 1 9.15420024E-01 # U_11 1 2 -4.02499912E-01 # U_12 2 1 4.02499912E-01 # U_21 2 2 9.15420024E-01 # U_22 # BLOCK VMIX # Chargino Mixing Matrix V 1 1 9.71869719E-01 # V_11 1 2 -2.35519104E-01 # V_12 2 1 2.35519104E-01 # V_21 2 2 9.71869719E-01 # V_22 # BLOCK STOPMIX # Stop Mixing Matrix 1 1 5.53439333E-01 # O_{11} 1 2 8.32889491E-01 # O_{12} 2 1 8.32889491E-01 # O_{21} 2 2 -5.53439333E-01 # O_{22} # BLOCK SBOTMIX # Sbottom Mixing Matrix 1 1 9.38417028E-01 # O_{11} 1 2 3.45504676E-01 # O_{12} 2 1 -3.45504676E-01 # O_{21} 2 2 9.38417028E-01 # O_{22} # BLOCK STAUMIX # Stau Mixing Matrix 1 1 2.82029170E-01 # O_{11} 1 2 9.59405830E-01 # O_{12} 2 1 9.59405830E-01 # O_{21} 2 2 -2.82029170E-01 # O_{22} # BLOCK ALPHA # Higgs mixing -1.13921380E-01 # Mixing angle in the neutral Higgs boson sector # BLOCK HMIX Q= 4.64669301E+02 # DRbar Higgs Parameters 1 3.55825714E+02 # mu(Q)MSSM DRbar 2 9.74915511E+00 # tan beta(Q)MSSM DRb 3 2.45016153E+02 # higgs vev(Q)MSSM DR 4 1.65064712E+05 # mA^2(Q)MSSM DRbar # BLOCK GAUGE Q= 4.64669301E+02 # The gauge couplings 3 1.09904885E+00 # g3(Q) MSbar # BLOCK AU Q= 4.64669301E+02 # The trilinear couplings 3 3 -4.93817451E+02 # A_t(Q) DRbar # BLOCK AD Q= 4.64669301E+02 # The trilinear couplings 3 3 -7.92162211E+02 # A_b(Q) DRbar # BLOCK AE Q= 4.64669301E+02 # The trilinear couplings 3 3 -2.51387472E+02 # A_tau(Q) DRbar # BLOCK YU Q= 4.64669301E+02 # The Yukawa couplings 3 3 8.93473447E-01 # y_t(Q) DRbar # BLOCK YD Q= 4.64669301E+02 # The Yukawa couplings 3 3 1.38175832E-01 # y_b(Q) DRbar # BLOCK YE Q= 4.64669301E+02 # The Yukawa couplings 3 3 1.00857841E-01 # y_tau(Q) DRbar # BLOCK MSOFT Q= 4.64669301E+02 # The soft SUSY breaking masses at the scale Q 1 1.01827998E+02 # M_1(Q) 2 1.91741376E+02 # M_2(Q) 3 5.85672962E+02 # M_3(Q) 21 3.23731728E+04 # mH1^2(Q) 22 -1.27530881E+05 # mH2^2(Q) 31 1.95176637E+02 # meL(Q) 32 1.95173849E+02 # mmuL(Q) 33 1.94341202E+02 # mtauL(Q) 34 1.36451646E+02 # meR(Q) 35 1.36443562E+02 # mmuR(Q) 36 1.34012141E+02 # mtauR(Q) 41 5.44872770E+02 # mqL1(Q) 42 5.44870961E+02 # mqL2(Q) 43 4.96219687E+02 # mqL3(Q) 44 5.26745075E+02 # muR(Q) 45 5.26743591E+02 # mcR(Q) 46 4.20715350E+02 # mtR(Q) 47 5.20424597E+02 # mdR(Q) 48 5.20422269E+02 # msR(Q) 49 5.17185468E+02 # mbR(Q) # #
      2212 2212 4.000000000E+03 4.000000000E+03 0 0 10042 10042 3 1 0.38860417163E+04 0.40300000000E+01 0.38944147080E-01 661 5 1 0.3170300E+01 0.3481367E+03 0.7816531E-02 0.1072161E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.47745618421E+03 0.47745618421E+03 0.00000000000E+00 0. 1. -3 -1 0 0 0 502 0.00000000000E+00 0.00000000000E+00 -0.63460896214E+02 0.63460896214E+02 0.00000000000E+00 0. 1. 1000006 2 1 2 503 0 0.00000000000E+00 0.00000000000E+00 0.41399528800E+03 0.54091708043E+03 0.34813673953E+03 0. 0. 6 1 3 3 503 0 0.55019726270E+02 0.55098735010E+02 0.35262804618E+03 0.40046621559E+03 0.17310000000E+03 0. -1. 1000022 1 3 3 0 0 -0.55019726270E+02 -0.55098735010E+02 0.61367241818E+02 0.14045086483E+03 0.99486010000E+02 0. -1. 5 1 0.3170300E+01 0.3481367E+03 0.7816531E-02 0.1072161E+00 1 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.47745618421E+03 0.47745618421E+03 0.00000000000E+00 0. 1. 3 -1 0 0 502 0 0.00000000000E+00 0.00000000000E+00 -0.63460896214E+02 0.63460896214E+02 0.00000000000E+00 0. 1. -1000006 2 1 2 0 503 0.00000000000E+00 0.00000000000E+00 0.41399528800E+03 0.54091708043E+03 0.34813673953E+03 0. 0. -6 1 3 3 0 503 0.55019726270E+02 0.55098735010E+02 0.35262804618E+03 0.40046621559E+03 0.17310000000E+03 0. -1. 1000022 1 3 3 0 0 -0.55019726270E+02 -0.55098735010E+02 0.61367241818E+02 0.14045086483E+03 0.99486010000E+02 0. -1. 5 2 0.3170300E+01 0.3481367E+03 0.7816531E-02 0.1072161E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.47745618421E+03 0.47745618421E+03 0.00000000000E+00 0. 1. -3 -1 0 0 0 502 0.00000000000E+00 0.00000000000E+00 -0.63460896214E+02 0.63460896214E+02 0.00000000000E+00 0. 1. 1000006 2 1 2 503 0 0.00000000000E+00 0.00000000000E+00 0.41399528800E+03 0.54091708043E+03 0.34813673953E+03 0. 0. -5 1 3 3 0 504 0.55019726270E+02 0.55098735010E+02 0.35262804618E+03 0.40046621559E+03 0.17310000000E+03 0. -1. -3 1 3 3 0 505 -0.55019726270E+02 -0.55098735010E+02 0.61367241818E+02 0.14045086483E+03 0.99486010000E+02 0. -1. 5 3 0.3170300E+01 0.3481367E+03 0.7816531E-02 0.1072161E+00 1 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.47745618421E+03 0.47745618421E+03 0.00000000000E+00 0. 1. 3 -1 0 0 502 0 0.00000000000E+00 0.00000000000E+00 -0.63460896214E+02 0.63460896214E+02 0.00000000000E+00 0. 1. -1000006 2 1 2 0 503 0.00000000000E+00 0.00000000000E+00 0.41399528800E+03 0.54091708043E+03 0.34813673953E+03 0. 0. 5 1 3 3 504 0 0.55019726270E+02 0.55098735010E+02 0.35262804618E+03 0.40046621559E+03 0.17310000000E+03 0. -1. 3 1 3 3 505 0 -0.55019726270E+02 -0.55098735010E+02 0.61367241818E+02 0.14045086483E+03 0.99486010000E+02 0. -1. 6 6 0.8174600E-05 0.2051526E+03 0.7957747E-01 0.1151852E+00 21 -1 0 0 502 503 0.00000000000E+00 0.00000000000E+00 0.10846490736E+03 0.10846490736E+03 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.22846826344E+04 0.22846826344E+04 0.00000000000E+00 0. 1. 9000006 2 1 2 501 -502 0.12250970092E+03 -0.18220128689E+03 -0.64334482025E+03 0.84463041750E+03 0.50130035774E+03 0. 0. 2 1 3 3 502 0 0.26809456118E+03 -0.24324065396E+03 -0.55810782099E+03 0.66522556274E+03 0.00000000000E+00 0. -1. 2 1 3 3 501 0 -0.14558486026E+03 0.61039367074E+02 -0.85236999257E+02 0.17940485476E+03 0.00000000000E+00 0. -1. -2 1 1 2 0 503 -0.12250970092E+03 0.18220128689E+03 -0.15328729068E+04 0.15485171242E+04 0.00000000000E+00 0. -1. 5 1 0.3170300E+01 0.3481367E+03 0.7816531E-02 0.1072161E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.47745618421E+03 0.47745618421E+03 0.00000000000E+00 0. 1. -3 -1 0 0 0 502 0.00000000000E+00 0.00000000000E+00 -0.63460896214E+02 0.63460896214E+02 0.00000000000E+00 0. 1. 1000006 2 1 2 503 0 0.00000000000E+00 0.00000000000E+00 0.41399528800E+03 0.54091708043E+03 0.34813673953E+03 0. 0. 6 1 3 3 503 0 0.55019726270E+02 0.55098735010E+02 0.35262804618E+03 0.40046621559E+03 0.17310000000E+03 0. -1. 1000022 1 3 3 0 0 -0.55019726270E+02 -0.55098735010E+02 0.61367241818E+02 0.14045086483E+03 0.99486010000E+02 0. -1. 5 1 0.3170300E+01 0.3481367E+03 0.7816531E-02 0.1072161E+00 1 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.47745618421E+03 0.47745618421E+03 0.00000000000E+00 0. 1. 3 -1 0 0 502 0 0.00000000000E+00 0.00000000000E+00 -0.63460896214E+02 0.63460896214E+02 0.00000000000E+00 0. 1. -1000006 2 1 2 0 503 0.00000000000E+00 0.00000000000E+00 0.41399528800E+03 0.54091708043E+03 0.34813673953E+03 0. 0. -6 1 3 3 0 503 0.55019726270E+02 0.55098735010E+02 0.35262804618E+03 0.40046621559E+03 0.17310000000E+03 0. -1. 1000022 1 3 3 0 0 -0.55019726270E+02 -0.55098735010E+02 0.61367241818E+02 0.14045086483E+03 0.99486010000E+02 0. -1. 5 2 0.3170300E+01 0.3481367E+03 0.7816531E-02 0.1072161E+00 -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.47745618421E+03 0.47745618421E+03 0.00000000000E+00 0. 1. -3 -1 0 0 0 502 0.00000000000E+00 0.00000000000E+00 -0.63460896214E+02 0.63460896214E+02 0.00000000000E+00 0. 1. 1000006 2 1 2 503 0 0.00000000000E+00 0.00000000000E+00 0.41399528800E+03 0.54091708043E+03 0.34813673953E+03 0. 0. -5 1 3 3 0 504 0.55019726270E+02 0.55098735010E+02 0.35262804618E+03 0.40046621559E+03 0.17310000000E+03 0. -1. -3 1 3 3 0 505 -0.55019726270E+02 -0.55098735010E+02 0.61367241818E+02 0.14045086483E+03 0.99486010000E+02 0. -1. 5 3 0.3170300E+01 0.3481367E+03 0.7816531E-02 0.1072161E+00 1 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 0.47745618421E+03 0.47745618421E+03 0.00000000000E+00 0. 1. 3 -1 0 0 502 0 0.00000000000E+00 0.00000000000E+00 -0.63460896214E+02 0.63460896214E+02 0.00000000000E+00 0. 1. -1000006 2 1 2 0 503 0.00000000000E+00 0.00000000000E+00 0.41399528800E+03 0.54091708043E+03 0.34813673953E+03 0. 0. 5 1 3 3 504 0 0.55019726270E+02 0.55098735010E+02 0.35262804618E+03 0.40046621559E+03 0.17310000000E+03 0. -1. 3 1 3 3 505 0 -0.55019726270E+02 -0.55098735010E+02 0.61367241818E+02 0.14045086483E+03 0.99486010000E+02 0. -1. 6 6 0.8174600E-05 0.2051526E+03 0.7957747E-01 0.1151852E+00 21 -1 0 0 502 503 0.00000000000E+00 0.00000000000E+00 0.10846490736E+03 0.10846490736E+03 0.00000000000E+00 0. 1. 2 -1 0 0 501 0 0.00000000000E+00 0.00000000000E+00 -0.22846826344E+04 0.22846826344E+04 0.00000000000E+00 0. 1. 9000006 2 1 2 501 -502 0.12250970092E+03 -0.18220128689E+03 -0.64334482025E+03 0.84463041750E+03 0.50130035774E+03 0. 0. 2 1 3 3 502 0 0.26809456118E+03 -0.24324065396E+03 -0.55810782099E+03 0.66522556274E+03 0.00000000000E+00 0. -1. 2 1 3 3 501 0 -0.14558486026E+03 0.61039367074E+02 -0.85236999257E+02 0.17940485476E+03 0.00000000000E+00 0. -1. -2 1 1 2 0 503 -0.12250970092E+03 0.18220128689E+03 -0.15328729068E+04 0.15485171242E+04 0.00000000000E+00 0. -1. 10 4 0.4424100E-06 0.2568823E+03 0.7957747E-01 0.1116564E+00 21 -1 0 0 506 502 0.00000000000E+00 0.00000000000E+00 0.21186259724E+03 0.21186259724E+03 0.00000000000E+00 0. -1. 21 -1 0 0 501 505 0.00000000000E+00 0.00000000000E+00 -0.16618043635E+04 0.16618043635E+04 0.00000000000E+00 0. 1. 6 2 1 2 501 0 0.21050055906E+01 -0.12646481280E+03 -0.46769970456E+03 0.51517427668E+03 0.17511065581E+03 0. 0. -6 2 1 2 0 502 0.44468730011E+02 0.23281490019E+03 -0.11321259313E+04 0.11689019978E+04 0.16864907487E+03 0. 0. 5 1 3 3 501 0 0.35441129604E+02 -0.11182665728E+03 -0.18441642927E+03 0.21861560861E+03 0.47000000000E+01 0. -1. 24 1 3 3 0 0 -0.33336124013E+02 -0.14638155518E+02 -0.28328327530E+03 0.29655866806E+03 0.79825163827E+02 0. 0. 5 1 4 4 503 0 0.73122549278E+02 0.88974785110E+02 -0.50093469550E+03 0.51402439510E+03 0.47000000000E+01 0. 1. 4 1 4 4 504 0 0.23108286112E+02 0.16188486457E+01 -0.80342656533E+02 0.83615524975E+02 0.00000000000E+00 0. -1. 13 1 4 4 0 0 -0.51762105379E+02 0.14222126643E+03 -0.55084857930E+03 0.57126207777E+03 0.00000000000E+00 0. -1. 21 1 1 2 506 505 -0.46573735602E+02 -0.10635008739E+03 0.14988386962E+03 0.18959068624E+03 0.00000000000E+00 0. -1. 10 4 0.4424100E-06 0.1846345E+03 0.7957747E-01 0.1285453E+00 2 -1 0 0 505 0 0.00000000000E+00 0.00000000000E+00 0.53829730604E+03 0.53829730604E+03 0.00000000000E+00 0. 1. 21 -1 0 0 501 505 0.00000000000E+00 0.00000000000E+00 -0.12887145459E+03 0.12887145459E+03 0.00000000000E+00 0. -1. 6 2 1 2 501 0 -0.29184274828E+02 -0.41594869008E+02 0.34999722596E+00 0.18188079259E+03 0.17463861312E+03 0. 0. -6 2 1 2 0 504 0.18203269668E+02 0.92364043781E+02 0.25662136433E+03 0.32422753507E+03 0.17437458030E+03 0. 0. 5 1 3 3 501 0 -0.16021667828E+02 -0.87211017623E+02 0.45227058793E+01 0.88910068627E+02 0.47000000000E+01 0. -1. 24 1 3 3 0 0 -0.13162607000E+02 0.45616148615E+02 -0.41727086534E+01 0.92970723968E+02 0.79825163827E+02 0. 0. 5 1 4 4 503 0 0.26369419717E+02 0.80308803866E+02 0.12716614143E+03 0.15276834686E+03 0.47000000000E+01 0. 1. 4 1 4 4 502 0 -0.59188545736E+02 -0.21060851541E+01 0.74023432789E+02 0.94800781341E+02 0.00000000000E+00 0. -1. 13 1 4 4 0 0 0.51022395687E+02 0.14161325069E+02 0.55431790113E+02 0.76658406874E+02 0.00000000000E+00 0. -1. 2 1 1 2 504 0 0.10981005160E+02 -0.50769174774E+02 0.15245448988E+03 0.16106043297E+03 0.00000000000E+00 0. 1. 10 4 0.4424100E-06 0.1833245E+03 0.7957747E-01 0.1291926E+00 -4 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 0.19595686468E+04 0.19595686468E+04 0.00000000000E+00 0. -1. 21 -1 0 0 501 505 0.00000000000E+00 0.00000000000E+00 -0.34817667906E+02 0.34817667906E+02 0.00000000000E+00 0. -1. 6 2 1 2 502 0 -0.61259507050E+02 -0.41786766991E+02 0.49355918747E+03 0.52906197135E+03 0.17551933481E+03 0. 0. -6 2 1 2 0 505 0.40208347004E+02 -0.24505892948E+01 0.47311584845E+03 0.50599665819E+03 0.17484649120E+03 0. 0. 5 1 3 3 502 0 -0.62830116761E+02 0.19282692430E+02 0.33431638324E+03 0.34074767776E+03 0.47000000000E+01 0. -1. 24 1 3 3 0 0 0.15706097109E+01 -0.61069459420E+02 0.15924280424E+03 0.18831429359E+03 0.79825163827E+02 0. 0. 5 1 4 4 504 0 -0.17488523649E+01 -0.48849580901E+02 0.97631774158E+02 0.10928583332E+03 0.47000000000E+01 0. 1. 4 1 4 4 503 0 0.86512049635E+01 0.78879187898E+02 0.20005161664E+03 0.21521482048E+03 0.00000000000E+00 0. -1. 13 1 4 4 0 0 0.33305994406E+02 -0.32480196292E+02 0.17543245765E+03 0.18149600440E+03 0.00000000000E+00 0. -1. -4 1 1 2 0 502 0.21051160046E+02 0.44237356286E+02 0.95807594295E+03 0.95932768515E+03 0.00000000000E+00 0. -1. 10 4 0.4424100E-06 0.2615950E+03 0.7957747E-01 0.1113805E+00 21 -1 0 0 501 505 0.00000000000E+00 0.00000000000E+00 0.21305752611E+04 0.21305752611E+04 0.00000000000E+00 0. 1. 21 -1 0 0 505 506 0.00000000000E+00 0.00000000000E+00 -0.62792335854E+02 0.62792335854E+02 0.00000000000E+00 0. -1. 6 2 1 2 501 0 0.10282766577E+03 0.82376162276E+02 0.92460870052E+03 0.95007295907E+03 0.17429290724E+03 0. 0. -6 2 1 2 0 504 0.12585274818E+03 -0.74074721592E+02 0.79616848462E+03 0.82763055559E+03 0.17251696161E+03 0. 0. 5 1 3 3 501 0 0.82350354911E+02 0.10068431408E+03 0.64486048176E+03 0.65786476041E+03 0.47000000000E+01 0. -1. 24 1 3 3 0 0 0.20477310855E+02 -0.18308151801E+02 0.27974821876E+03 0.29220819865E+03 0.79825163827E+02 0. -1. 5 1 4 4 503 0 -0.52882542877E+01 0.42371188374E+02 0.20886491026E+03 0.21323677914E+03 0.47000000000E+01 0. 1. 4 1 4 4 502 0 0.47097981041E+02 -0.30312803662E+02 0.25197849456E+03 0.25812835490E+03 0.00000000000E+00 0. 1. 13 1 4 4 0 0 0.84043021428E+02 -0.86133106304E+02 0.33532507980E+03 0.35626542156E+03 0.00000000000E+00 0. -1. 21 1 1 2 504 506 -0.22868041395E+03 -0.83014406843E+01 0.34700574008E+03 0.41566408227E+03 0.00000000000E+00 0. -1. 10 4 0.4424100E-06 0.1881356E+03 0.7957747E-01 0.1166043E+00 21 -1 0 0 501 505 0.00000000000E+00 0.00000000000E+00 0.10093773553E+03 0.10093773553E+03 0.00000000000E+00 0. -1. 21 -1 0 0 505 506 0.00000000000E+00 0.00000000000E+00 -0.43620324447E+03 0.43620324447E+03 0.00000000000E+00 0. -1. 6 2 1 2 501 0 -0.13170184984E+02 0.74177342582E+02 -0.81031403980E+02 0.20591574103E+03 0.17366482674E+03 0. 0. -6 2 1 2 0 504 -0.85985973022E+01 -0.64416371097E+02 -0.20710425430E+03 0.27840119833E+03 0.17433201180E+03 0. 0. 5 1 3 3 501 0 0.81755880555E+01 -0.22233870180E+02 0.29111730430E+02 0.37825494998E+02 0.47000000000E+01 0. -1. 24 1 3 3 0 0 -0.21345773040E+02 0.96411212762E+02 -0.11014313441E+03 0.16809024603E+03 0.79825163827E+02 0. -1. 5 1 4 4 503 0 -0.20409420345E+02 0.22876851571E+02 0.55767425928E+01 0.31513248556E+02 0.47000000000E+01 0. 1. 4 1 4 4 502 0 0.22560813830E+02 -0.81527820613E+02 -0.21780631025E+03 0.23365650995E+03 0.00000000000E+00 0. -1. 13 1 4 4 0 0 -0.10749990787E+02 -0.57654020542E+01 0.51253133574E+01 0.13231439823E+02 0.00000000000E+00 0. -1. 21 1 1 2 504 506 0.21768782286E+02 -0.97609714857E+01 -0.47129850661E+02 0.52824040643E+02 0.00000000000E+00 0. 1. 10 4 0.4424100E-06 0.1864067E+03 0.7957747E-01 0.1167576E+00 21 -1 0 0 503 504 0.00000000000E+00 0.00000000000E+00 0.14984513090E+03 0.14984513090E+03 0.00000000000E+00 0. 1. 21 -1 0 0 506 505 0.00000000000E+00 0.00000000000E+00 -0.10249066020E+04 0.10249066020E+04 0.00000000000E+00 0. -1. 6 2 1 2 503 0 -0.16509325939E+03 -0.88762921909E+02 -0.19566835178E+03 0.32232437068E+03 0.17456304145E+03 0. 0. -6 2 1 2 0 505 0.13103545612E+02 0.46991711201E+02 -0.67049684814E+03 0.69455130076E+03 0.17451522053E+03 0. 0. -5 1 3 3 0 502 -0.86500026434E+02 -0.95458583889E+02 -0.13362133160E+03 0.18566460640E+03 0.47000000000E+01 0. -1. -4 1 3 3 0 501 -0.41727434534E+02 -0.34800616684E+02 -0.60238943028E+02 0.81123313367E+02 0.00000000000E+00 0. 1. -13 1 3 3 0 0 -0.36865798426E+02 0.41496278664E+02 -0.18080771498E+01 0.55536450909E+02 0.00000000000E+00 0. 1. -5 1 4 4 0 505 0.56709234087E+02 0.44332967666E+02 -0.45419550304E+03 0.45988802358E+03 0.47000000000E+01 0. 1. -24 1 4 4 0 0 -0.43605688475E+02 0.26587435347E+01 -0.21630134510E+03 0.23466327718E+03 0.79825163827E+02 0. -1. 21 1 1 2 506 504 0.15198971378E+03 0.41771210708E+02 -0.88962711757E+01 0.15787606145E+03 0.00000000000E+00 0. 1. 10 4 0.4424100E-06 0.2259499E+03 0.7957747E-01 0.1136429E+00 21 -1 0 0 503 504 0.00000000000E+00 0.00000000000E+00 0.33775267147E+03 0.33775267147E+03 0.00000000000E+00 0. 1. 21 -1 0 0 504 505 0.00000000000E+00 0.00000000000E+00 -0.25756936200E+03 0.25756936200E+03 0.00000000000E+00 0. 1. 6 2 1 2 503 0 -0.65592825348E+02 0.12828116235E+03 0.20579661139E+03 0.30719636238E+03 0.17680182253E+03 0. 0. -6 2 1 2 0 506 0.27026512974E+02 -0.12960085316E+03 -0.11319636195E+03 0.24758825095E+03 0.17595372149E+03 0. 0. -5 1 3 3 0 502 -0.54166499632E+02 -0.89574428511E+01 0.72867804204E+02 0.91356731303E+02 0.47000000000E+01 0. -1. -4 1 3 3 0 501 -0.28264383917E+02 0.12978775938E+03 0.14273394296E+03 0.19497875873E+03 0.00000000000E+00 0. 1. -13 1 3 3 0 0 0.16838058202E+02 0.74508458201E+01 -0.98051357762E+01 0.20860872346E+02 0.00000000000E+00 0. 1. -5 1 4 4 0 506 -0.43891501090E+02 -0.49854929182E+01 -0.60843502736E+02 0.75334858020E+02 0.47000000000E+01 0. 1. -24 1 4 4 0 0 0.70918014064E+02 -0.12461536024E+03 -0.52352859212E+02 0.17225339293E+03 0.79825163827E+02 0. 0. 21 1 1 2 506 505 0.38566312374E+02 0.13196908068E+01 -0.12416939962E+02 0.40537420144E+02 0.00000000000E+00 0. -1. 10 4 0.4424100E-06 0.2180063E+03 0.7957747E-01 0.1142097E+00 21 -1 0 0 501 505 0.00000000000E+00 0.00000000000E+00 0.69867021183E+03 0.69867021183E+03 0.00000000000E+00 0. 1. 21 -1 0 0 505 506 0.00000000000E+00 0.00000000000E+00 -0.40018043993E+03 0.40018043993E+03 0.00000000000E+00 0. 1. 6 2 1 2 501 0 0.73833194922E+02 -0.55665332998E+02 0.34347952129E+03 0.39527886248E+03 0.17238685450E+03 0. 0. -6 2 1 2 0 504 -0.15618008153E+03 0.84244097789E+02 0.27372308068E+03 0.37315444171E+03 0.18119223657E+03 0. 0. 5 1 3 3 501 0 -0.41970554796E+02 -0.15122504862E+02 0.49045269333E+02 0.66466127216E+02 0.47000000000E+01 0. -1. 24 1 3 3 0 0 0.11580374972E+03 -0.40542828136E+02 0.29443425196E+03 0.32881273526E+03 0.79825163827E+02 0. 0. 5 1 4 4 503 0 -0.16548216023E+03 0.49780000384E+02 0.14668057822E+03 0.22671496603E+03 0.47000000000E+01 0. 1. 4 1 4 4 502 0 0.29819793781E+02 -0.31475104447E+01 0.53068865626E+02 0.60954338828E+02 0.00000000000E+00 0. -1. 13 1 4 4 0 0 -0.20517715077E+02 0.37611607850E+02 0.73973636827E+02 0.85485136851E+02 0.00000000000E+00 0. -1. 21 1 1 2 504 506 0.82346886607E+02 -0.28578764791E+02 -0.31871283006E+03 0.33041734757E+03 0.00000000000E+00 0. 1. 7 0 0.1670621E-05 0.2083507E+03 0.7957747E-01 0.1149353E+00 21 -1 0 0 503 504 0.00000000000E+00 0.00000000000E+00 0.17415333744E+03 0.17415333744E+03 0.00000000000E+00 0. -1. 21 -1 0 0 504 505 0.00000000000E+00 0.00000000000E+00 -0.42651677420E+03 0.42651677420E+03 0.00000000000E+00 0. -1. -5 1 1 2 0 505 -0.12321332363E+02 0.20380105994E+02 -0.18383192781E+03 0.18542769921E+03 0.47000000000E+01 0. 1. -4 1 1 2 0 501 -0.95177811857E+02 -0.24755314057E+02 0.96510409946E+01 0.98827123991E+02 0.14200000000E+01 0. -1. -13 1 1 2 0 0 0.29205706274E+02 -0.55806117872E+02 0.20669105497E+02 0.66291169525E+02 0.10566000000E+00 0. 1. -5 1 1 2 0 502 -0.31766731223E+02 0.20590446512E+02 0.37535630411E+02 0.53517335981E+02 0.47000000000E+01 0. -1. -24 1 1 2 0 0 0.11006016917E+03 0.39590879424E+02 -0.13638728585E+03 0.19660678293E+03 0.79825163827E+02 0. 0. 7 0 0.1482316E-05 0.1992671E+03 0.7957747E-01 0.1156583E+00 21 -1 0 0 505 502 0.00000000000E+00 0.00000000000E+00 0.27227457777E+03 0.27227457777E+03 0.00000000000E+00 0. 1. 21 -1 0 0 501 505 0.00000000000E+00 0.00000000000E+00 -0.15795229186E+03 0.15795229186E+03 0.00000000000E+00 0. 1. 5 1 1 2 503 0 -0.56847234724E+02 -0.15035316131E+02 0.17052270511E+02 0.61404712820E+02 0.47000000000E+01 0. 1. 24 1 1 2 0 0 0.22591738017E+02 0.21332907202E+02 0.63846317992E+02 0.10683580232E+03 0.79825163827E+02 0. 0. 5 1 1 2 501 0 0.40735390586E+02 0.39271897315E+02 -0.73215747780E+02 0.92651441909E+02 0.47000000000E+01 0. -1. 4 1 1 2 504 0 0.93891362881E+01 -0.38400352485E+02 0.13243242799E+03 0.13821399109E+03 0.14200000000E+01 0. -1. 13 1 1 2 0 0 -0.15869030167E+02 -0.71691359006E+01 -0.25792982802E+02 0.31120921481E+02 0.10566000000E+00 0. -1. 9 0 0.9369500E-06 0.1863158E+03 0.7957747E-01 0.1167657E+00 21 -1 0 0 502 501 0.00000000000E+00 0.00000000000E+00 0.12342052313E+03 0.12342052313E+03 0.00000000000E+00 0. -1. 21 -1 0 0 503 502 0.00000000000E+00 0.00000000000E+00 -0.33180194320E+03 0.33180194320E+03 0.00000000000E+00 0. -1. -5 1 1 2 0 504 0.38318612105E+02 -0.56752065691E+02 -0.60710649153E+02 0.91635069239E+02 0.47000000000E+01 0. -1. -4 1 1 2 0 505 -0.68115828337E+02 0.24751715411E+02 -0.62693257320E+02 0.95837750387E+02 0.14200000000E+01 0. 1. -13 1 1 2 0 0 0.23716050790E+02 -0.32892734355E+02 -0.71226400994E+02 0.81960932163E+02 0.10566000000E+00 0. 1. -5 1 1 2 0 501 -0.27845898475E+02 0.90528149499E+02 -0.64430536491E+01 0.95049160195E+02 0.47000000000E+01 0. 1. -24 1 1 2 0 0 0.33927063917E+02 -0.25635064864E+02 -0.73080589579E+01 0.90739554343E+02 0.79825163827E+02 0. 1. 9 0 0.1482316E-05 0.1962662E+03 0.7957747E-01 0.1159065E+00 21 -1 0 0 505 502 0.00000000000E+00 0.00000000000E+00 0.11931216444E+03 0.11931216444E+03 0.00000000000E+00 0. 1. 21 -1 0 0 501 505 0.00000000000E+00 0.00000000000E+00 -0.31973272796E+03 0.31973272796E+03 0.00000000000E+00 0. 1. 5 1 1 2 501 0 0.24542568681E+02 -0.36208849786E+02 -0.47487783694E+02 0.64734828960E+02 0.47000000000E+01 0. -1. 24 1 1 2 0 0 -0.11246782816E+03 0.52175348208E+02 -0.61553734788E+02 0.15978797945E+03 0.79825163827E+02 0. -1. 5 1 1 2 503 0 0.12311735588E+02 0.76079021489E+01 0.25250884129E+01 0.15424820251E+02 0.47000000000E+01 0. 1. 4 1 1 2 504 0 0.35080206863E+02 0.65281062252E+02 -0.20447072707E+02 0.76891723772E+02 0.14200000000E+01 0. -1. 13 1 1 2 0 0 0.40533317023E+02 -0.88855462822E+02 -0.73457060739E+02 0.12220553997E+03 0.10566000000E+00 0. -1.
      pythia8-8.1.80.orig/examples/snowmass2.spc0000644000175000017500000014342512217346206016626 0ustar sunsun##****************************************************************** ## MadGraph/MadEvent * ##****************************************************************** ## * ## param_card corresponding the SPS point 2 (by SoftSusy 2.0.5) * ## * ##****************************************************************** ## Les Houches friendly file for the (MS)SM parameters of MadGraph * ## SM parameter set and decay widths produced by MSSMCalc * ##****************************************************************** ##*Please note the following IMPORTANT issues: * ## * ##0. REFRAIN from editing this file by hand! Some of the parame- * ## ters are not independent. Always use a calculator. * ## * ##1. alpha_S(MZ) has been used in the calculation of the parameters* ## This value is KEPT by madgraph when no pdf are used lpp(i)=0, * ## but, for consistency, it will be reset by madgraph to the * ## value expected IF the pdfs for collisions with hadrons are * ## used. * ## * ##2. Values of the charm and bottom kinematic (pole) masses are * ## those used in the matrix elements and phase space UNLESS they * ## are set to ZERO from the start in the model (particles.dat) * ## This happens, for example, when using 5-flavor QCD where * ## charm and bottom are treated as partons in the initial state * ## and a zero mass might be hardwired in the model definition. * ## * ## The SUSY decays have calculated using SDECAY 1.1a * ## * ##****************************************************************** # BLOCK DCINFO # Decay Program information 1 SDECAY # decay calculator 2 1.1a # version number # BLOCK SPINFO # Spectrum calculator information 1 SOFTSUSY # spectrum calculator 2 2.0.5 # version number # BLOCK MODSEL # Model selection 1 1 sugra # BLOCK SMINPUTS # Standard Model inputs 1 1.27934000E+02 # alpha_em^-1(M_Z)^MSbar 2 1.16637000E-05 # G_F [GeV^-2] 3 1.18000000E-01 # alpha_S(M_Z)^MSbar 4 9.11876000E+01 # M_Z pole mass 5 4.25000000E+00 # mb(mb)^MSbar 6 1.75000000E+02 # mt pole mass 7 1.77700000E+00 # mtau pole mass # BLOCK MINPAR # Input parameters - minimal models 1 1.45000000E+03 # m0 2 3.00000000E+02 # m12 3 1.00000000E+01 # tanb 4 1.00000000E+00 # sign(mu) # BLOCK MASS # Mass Spectrum # PDG code mass particle 5 4.88991651E+00 # b-quark pole mass calculated from mb(mb)_Msbar 6 1.75000000E+02 # mt pole mass (not read by ME) 24 7.98290131E+01 # W+ 25 1.15172279E+02 # h 35 1.51114877E+03 # H 36 1.51103826E+03 # A 37 1.51343530E+03 # H+ 1000001 1.55931152E+03 # ~d_L 2000001 1.55240630E+03 # ~d_R 1000002 1.55431328E+03 # ~u_L 2000002 1.55382420E+03 # ~u_R 1000003 1.55931152E+03 # ~s_L 2000003 1.55240630E+03 # ~s_R 1000004 1.55431328E+03 # ~c_L 2000004 1.55382420E+03 # ~c_R 1000005 1.28421793E+03 # ~b_1 2000005 1.53908204E+03 # ~b_2 1000006 9.50096226E+02 # ~t_1 2000006 1.29611751E+03 # ~t_2 1000011 1.45911583E+03 # ~e_L 2000011 1.45303116E+03 # ~e_R 1000012 1.45599000E+03 # ~nu_eL 1000013 1.45911583E+03 # ~mu_L 2000013 1.45303116E+03 # ~mu_R 1000014 1.45599000E+03 # ~nu_muL 1000015 1.44007642E+03 # ~tau_1 2000015 1.45350507E+03 # ~tau_2 1000016 1.45001839E+03 # ~nu_tauL 1000021 7.81898886E+02 # ~g 1000022 1.22849441E+02 # ~chi_10 1000023 2.35046162E+02 # ~chi_20 1000025 -4.69015751E+02 # ~chi_30 1000035 4.83058535E+02 # ~chi_40 1000024 2.37406034E+02 # ~chi_1+ 1000037 4.84104812E+02 # ~chi_2+ # BLOCK NMIX # Neutralino Mixing Matrix 1 1 9.92797628E-01 # N_11 1 2 -3.04145381E-02 # N_12 1 3 1.09080644E-01 # N_13 1 4 -3.91054708E-02 # N_14 2 1 5.84996523E-02 # N_21 2 2 9.66019640E-01 # N_22 2 3 -2.17829192E-01 # N_23 2 4 1.26231093E-01 # N_24 3 1 -4.69368399E-02 # N_31 3 2 6.81242959E-02 # N_32 3 3 7.00360055E-01 # N_33 3 4 7.08979412E-01 # N_34 4 1 -9.34215858E-02 # N_41 4 2 2.47467354E-01 # N_42 4 3 6.70930436E-01 # N_43 4 4 -6.92737083E-01 # N_44 # BLOCK UMIX # Chargino Mixing Matrix U 1 1 9.48909352E-01 # U_11 1 2 -3.15548795E-01 # U_12 2 1 3.15548795E-01 # U_21 2 2 9.48909352E-01 # U_22 # BLOCK VMIX # Chargino Mixing Matrix V 1 1 9.83010683E-01 # V_11 1 2 -1.83548349E-01 # V_12 2 1 1.83548349E-01 # V_21 2 2 9.83010683E-01 # V_22 # BLOCK STOPMIX # Stop Mixing Matrix 1 1 1.25445912E-01 # O_{11} 1 2 9.92100460E-01 # O_{12} 2 1 9.92100460E-01 # O_{21} 2 2 -1.25445912E-01 # O_{22} # BLOCK SBOTMIX # Sbottom Mixing Matrix 1 1 9.99839511E-01 # O_{11} 1 2 1.79151679E-02 # O_{12} 2 1 -1.79151679E-02 # O_{21} 2 2 9.99839511E-01 # O_{22} # BLOCK STAUMIX # Stau Mixing Matrix 1 1 2.14038360E-01 # O_{11} 1 2 9.76825256E-01 # O_{12} 2 1 9.76825256E-01 # O_{21} 2 2 -2.14038360E-01 # O_{22} # BLOCK ALPHA # Higgs mixing -1.04393740E-01 # Mixing angle in the neutral Higgs boson sector # BLOCK HMIX Q= 1.09862507E+03 # DRbar Higgs Parameters 1 4.64310302E+02 # mu(Q)MSSM DRbar 2 9.63167226E+00 # tan beta(Q)MSSM DRba 3 2.43241679E+02 # higgs vev(Q)MSSM DRb 4 2.30234275E+06 # mA^2(Q)MSSM DRbar # BLOCK GAUGE Q= 1.09862507E+03 # The gauge couplings 3 1.05313071E+00 # g3(Q) MSbar # BLOCK AU Q= 1.09862507E+03 # The trilinear couplings 1 1 0.00000000E+00 # A_u(Q) DRbar 2 2 0.00000000E+00 # A_c(Q) DRbar 3 3 -5.20713786E+02 # A_t(Q) DRbar # BLOCK AD Q= 1.09862507E+03 # The trilinear couplings 1 1 0.00000000E+00 # A_d(Q) DRbar 2 2 0.00000000E+00 # A_s(Q) DRbar 3 3 -7.83275622E+02 # A_b(Q) DRbar # BLOCK AE Q= 1.09862507E+03 # The trilinear couplings 1 1 0.00000000E+00 # A_e(Q) DRbar 2 2 0.00000000E+00 # A_mu(Q) DRbar 3 3 -1.78852193E+02 # A_tau(Q) DRbar # BLOCK YU Q= 1.09862507E+03 # The Yukawa couplings 3 3 8.73306713E-01 # y_t(Q) DRbar # BLOCK YD Q= 1.09862507E+03 # The Yukawa couplings 3 3 1.36198959E-01 # y_b(Q) DRbar # BLOCK YE Q= 1.09862507E+03 # The Yukawa couplings 3 3 9.90900945E-02 # y_tau(Q) DRbar # BLOCK MSOFT Q= 1.09862507E+03 # The soft SUSY breaking masses at the scale Q 1 1.25459404E+02 # M_1(Q) 2 2.33056280E+02 # M_2(Q) 3 6.69284431E+02 # M_3(Q) 21 2.04348830E+06 # mH1^2(Q) 22 -1.69489026E+05 # mH2^2(Q) 31 1.45570737E+03 # meL(Q) 32 1.45570737E+03 # mmuL(Q) 33 1.44967248E+03 # mtauL(Q) 34 1.45113170E+03 # meR(Q) 35 1.45113170E+03 # mmuR(Q) 36 1.43894634E+03 # mtauR(Q) 41 1.53851945E+03 # mqL1(Q) 42 1.53851945E+03 # mqL2(Q) 43 1.27150657E+03 # mqL3(Q) 44 1.53533107E+03 # muR(Q) 45 1.53533107E+03 # mcR(Q) 46 9.34674342E+02 # mtR(Q) 47 1.53339994E+03 # mdR(Q) 48 1.53339994E+03 # msR(Q) 49 1.52101430E+03 # mbR(Q) # # # # ================= # |The decay table| # ================= # # - The multi-body decays for the inos, stops and sbottoms are included. # # - The SUSY decays of the top quark are included. # # # PDG Width DECAY 23 2.41143316E+00 # Z width (SM calculation) DECAY 24 2.00282196E+00 # W width (SM calculation) # # PDG Width DECAY 6 1.56194983E+00 # top decays # BR NDA ID1 ID2 1.00000000E+00 2 5 24 # BR(t -> b W+) 0.00000000E+00 2 5 37 # BR(t -> b H+) 0.00000000E+00 2 1000006 1000022 # BR(t -> ~t_1 ~chi_10) 0.00000000E+00 2 1000006 1000023 # BR(t -> ~t_1 ~chi_20) 0.00000000E+00 2 1000006 1000025 # BR(t -> ~t_1 ~chi_30) 0.00000000E+00 2 1000006 1000035 # BR(t -> ~t_1 ~chi_40) 0.00000000E+00 2 2000006 1000022 # BR(t -> ~t_2 ~chi_10) 0.00000000E+00 2 2000006 1000023 # BR(t -> ~t_2 ~chi_20) 0.00000000E+00 2 2000006 1000025 # BR(t -> ~t_2 ~chi_30) 0.00000000E+00 2 2000006 1000035 # BR(t -> ~t_2 ~chi_40) # # PDG Width DECAY 25 1.74556397E-03 # h decays # BR NDA ID1 ID2 1.39750346E-01 2 15 -15 # BR(H1 -> tau- tau+) 7.84634857E-01 2 5 -5 # BR(H1 -> b bb) 7.08726118E-02 2 24 -24 # BR(H1 -> W+ W-) 4.74218479E-03 2 23 23 # BR(H1 -> Z Z) # # PDG Width DECAY 35 2.63857501E+00 # H decays # BR NDA ID1 ID2 1.10658102E-01 2 15 -15 # BR(H -> tau- tau+) 2.60600489E-01 2 6 -6 # BR(H -> t tb) 6.27144880E-01 2 5 -5 # BR(H -> b bb) 3.73136377E-04 2 24 -24 # BR(H -> W+ W-) 1.85618475E-04 2 23 23 # BR(H -> Z Z) 0.00000000E+00 2 24 -37 # BR(H -> W+ H-) 0.00000000E+00 2 -24 37 # BR(H -> W- H+) 0.00000000E+00 2 37 -37 # BR(H -> H+ H-) 1.03777426E-03 2 25 25 # BR(H -> h h) 0.00000000E+00 2 36 36 # BR(H -> A A) # # PDG Width DECAY 36 2.66158444E+00 # A decays # BR NDA ID1 ID2 1.09715563E-01 2 15 -15 # BR(A -> tau- tau+) 2.68093243E-01 2 6 -6 # BR(A -> t tb) 6.21825730E-01 2 5 -5 # BR(A -> b bb) 3.65463754E-04 2 23 25 # BR(A -> Z h) 0.00000000E+00 2 23 35 # BR(A -> Z H) 0.00000000E+00 2 24 -37 # BR(A -> W+ H-) 0.00000000E+00 2 -24 37 # BR(A -> W- H+) # # PDG Width DECAY 37 2.62953484E+00 # H+ decays # BR NDA ID1 ID2 1.11229134E-01 2 -15 16 # BR(H+ -> tau+ nu_tau) 8.88398184E-01 2 6 -5 # BR(H+ -> t bb) 3.72682177E-04 2 24 25 # BR(H+ -> W+ h) 0.00000000E+00 2 24 35 # BR(H+ -> W+ H) 0.00000000E+00 2 24 36 # BR(H+ -> W+ A) # # PDG Width DECAY 1000021 2.61914150E-03 # gluino decays # BR NDA ID1 ID2 ID3 1.08568721E-02 3 1000022 1 -1 # BR(~g -> ~chi_10 d db) 3.85532351E-02 3 1000023 1 -1 # BR(~g -> ~chi_20 d db) 1.44423781E-05 3 1000025 1 -1 # BR(~g -> ~chi_30 d db) 3.78641719E-04 3 1000035 1 -1 # BR(~g -> ~chi_40 d db) 3.38409830E-02 3 1000022 2 -2 # BR(~g -> ~chi_10 u ub) 4.09634282E-02 3 1000023 2 -2 # BR(~g -> ~chi_20 u ub) 1.12060501E-05 3 1000025 2 -2 # BR(~g -> ~chi_30 u ub) 3.11741607E-04 3 1000035 2 -2 # BR(~g -> ~chi_40 u ub) 1.08568721E-02 3 1000022 3 -3 # BR(~g -> ~chi_10 s sb) 3.85532351E-02 3 1000023 3 -3 # BR(~g -> ~chi_20 s sb) 1.44423781E-05 3 1000025 3 -3 # BR(~g -> ~chi_30 s sb) 3.78641719E-04 3 1000035 3 -3 # BR(~g -> ~chi_40 s sb) 3.38409830E-02 3 1000022 4 -4 # BR(~g -> ~chi_10 c cb) 4.09634282E-02 3 1000023 4 -4 # BR(~g -> ~chi_20 c cb) 1.12060501E-05 3 1000025 4 -4 # BR(~g -> ~chi_30 c cb) 3.11741607E-04 3 1000035 4 -4 # BR(~g -> ~chi_40 c cb) 1.53100058E-02 3 1000022 5 -5 # BR(~g -> ~chi_10 b bb) 9.65125323E-02 3 1000023 5 -5 # BR(~g -> ~chi_20 b bb) 1.06208080E-03 3 1000025 5 -5 # BR(~g -> ~chi_30 b bb) 1.83692827E-03 3 1000035 5 -5 # BR(~g -> ~chi_40 b bb) 9.92065188E-02 3 1000022 6 -6 # BR(~g -> ~chi_10 t tb) 1.17953941E-02 3 1000023 6 -6 # BR(~g -> ~chi_20 t tb) 0.00000000E+00 3 1000025 6 -6 # BR(~g -> ~chi_30 t tb) 0.00000000E+00 3 1000035 6 -6 # BR(~g -> ~chi_40 t tb) 7.85597617E-02 3 1000024 1 -2 # BR(~g -> ~chi_1+ d ub) 7.85597617E-02 3 -1000024 2 -1 # BR(~g -> ~chi_1- u db) 6.72469173E-04 3 1000037 1 -2 # BR(~g -> ~chi_2+ d ub) 6.72469173E-04 3 -1000037 2 -1 # BR(~g -> ~chi_2- u db) 7.85597617E-02 3 1000024 3 -4 # BR(~g -> ~chi_1+ s cb) 7.85597617E-02 3 -1000024 4 -3 # BR(~g -> ~chi_1- c sb) 6.72469173E-04 3 1000037 3 -4 # BR(~g -> ~chi_2+ s cb) 6.72469173E-04 3 -1000037 4 -3 # BR(~g -> ~chi_2- c sb) 7.99935892E-02 3 1000024 5 -6 # BR(~g -> ~chi_1+ b tb) 7.99935892E-02 3 -1000024 6 -5 # BR(~g -> ~chi_1- t bb) 2.37496688E-02 3 1000037 5 -6 # BR(~g -> ~chi_2+ b tb) 2.37496688E-02 3 -1000037 6 -5 # BR(~g -> ~chi_2- t bb) 0.00000000E+00 3 1000006 -5 -24 # BR(~g -> ~t_1 bb W-) 0.00000000E+00 3 -1000006 5 24 # BR(~g -> ~t_1* b W+) 0.00000000E+00 3 1000006 -5 -37 # BR(~g -> ~t_1 bb H-) 0.00000000E+00 3 -1000006 5 37 # BR(~g -> ~t_1* b H+) # # PDG Width DECAY 1000006 1.75928469E+01 # stop1 decays # BR NDA ID1 ID2 1.09448984E-01 2 1000022 6 # BR(~t_1 -> ~chi_10 t ) 2.41846014E-02 2 1000023 6 # BR(~t_1 -> ~chi_20 t ) 2.27512666E-01 2 1000025 6 # BR(~t_1 -> ~chi_30 t ) 1.72542842E-01 2 1000035 6 # BR(~t_1 -> ~chi_40 t ) 5.39584750E-02 2 1000024 5 # BR(~t_1 -> ~chi_1+ b ) 4.12352432E-01 2 1000037 5 # BR(~t_1 -> ~chi_2+ b ) 0.00000000E+00 2 1000021 6 # BR(~t_1 -> ~g t ) 0.00000000E+00 2 1000005 37 # BR(~t_1 -> ~b_1 H+) 0.00000000E+00 2 2000005 37 # BR(~t_1 -> ~b_2 H+) 0.00000000E+00 2 1000005 24 # BR(~t_1 -> ~b_1 W+) 0.00000000E+00 2 2000005 24 # BR(~t_1 -> ~b_2 W+) # # PDG Width DECAY 2000006 5.75326698E+01 # stop2 decays # BR NDA ID1 ID2 2.30908763E-03 2 1000022 6 # BR(~t_2 -> ~chi_10 t ) 7.77273606E-02 2 1000023 6 # BR(~t_2 -> ~chi_20 t ) 1.19356099E-01 2 1000025 6 # BR(~t_2 -> ~chi_30 t ) 1.33939015E-01 2 1000035 6 # BR(~t_2 -> ~chi_40 t ) 1.57657021E-01 2 1000024 5 # BR(~t_2 -> ~chi_1+ b ) 2.24336879E-02 2 1000037 5 # BR(~t_2 -> ~chi_2+ b ) 4.56063239E-01 2 1000021 6 # BR(~t_2 -> ~g t ) 1.34554106E-02 2 1000006 25 # BR(~t_2 -> ~t_1 h ) 0.00000000E+00 2 1000006 35 # BR(~t_2 -> ~t_1 H ) 0.00000000E+00 2 1000006 36 # BR(~t_2 -> ~t_1 A ) 0.00000000E+00 2 1000005 37 # BR(~t_2 -> ~b_1 H+) 0.00000000E+00 2 2000005 37 # BR(~t_2 -> ~b_2 H+) 1.70590802E-02 2 1000006 23 # BR(~t_2 -> ~t_1 Z ) 0.00000000E+00 2 1000005 24 # BR(~t_2 -> ~b_1 W+) 0.00000000E+00 2 2000005 24 # BR(~t_2 -> ~b_2 W+) # # PDG Width DECAY 1000005 6.09457233E+01 # sbottom1 decays # BR NDA ID1 ID2 4.08034135E-03 2 1000022 5 # BR(~b_1 -> ~chi_10 b ) 7.56044373E-02 2 1000023 5 # BR(~b_1 -> ~chi_20 b ) 3.20158717E-03 2 1000025 5 # BR(~b_1 -> ~chi_30 b ) 7.01193659E-03 2 1000035 5 # BR(~b_1 -> ~chi_40 b ) 1.48222955E-01 2 -1000024 6 # BR(~b_1 -> ~chi_1- t ) 2.40382303E-01 2 -1000037 6 # BR(~b_1 -> ~chi_2- t ) 4.91084085E-01 2 1000021 5 # BR(~b_1 -> ~g b ) 0.00000000E+00 2 1000006 -37 # BR(~b_1 -> ~t_1 H-) 0.00000000E+00 2 2000006 -37 # BR(~b_1 -> ~t_2 H-) 3.04123541E-02 2 1000006 -24 # BR(~b_1 -> ~t_1 W-) 0.00000000E+00 2 2000006 -24 # BR(~b_1 -> ~t_2 W-) # # PDG Width DECAY 2000005 5.16683385E+01 # sbottom2 decays # BR NDA ID1 ID2 1.64661552E-02 2 1000022 5 # BR(~b_2 -> ~chi_10 b ) 3.30476030E-04 2 1000023 5 # BR(~b_2 -> ~chi_20 b ) 4.53772512E-03 2 1000025 5 # BR(~b_2 -> ~chi_30 b ) 4.36303330E-03 2 1000035 5 # BR(~b_2 -> ~chi_40 b ) 5.69055898E-04 2 -1000024 6 # BR(~b_2 -> ~chi_1- t ) 8.49106743E-03 2 -1000037 6 # BR(~b_2 -> ~chi_2- t ) 9.64528400E-01 2 1000021 5 # BR(~b_2 -> ~g b ) 1.88178360E-04 2 1000005 25 # BR(~b_2 -> ~b_1 h ) 0.00000000E+00 2 1000005 35 # BR(~b_2 -> ~b_1 H ) 0.00000000E+00 2 1000005 36 # BR(~b_2 -> ~b_1 A ) 0.00000000E+00 2 1000006 -37 # BR(~b_2 -> ~t_1 H-) 0.00000000E+00 2 2000006 -37 # BR(~b_2 -> ~t_2 H-) 1.69299183E-04 2 1000005 23 # BR(~b_2 -> ~b_1 Z ) 5.38503978E-05 2 1000006 -24 # BR(~b_2 -> ~t_1 W-) 3.02759424E-04 2 2000006 -24 # BR(~b_2 -> ~t_2 W-) # # PDG Width DECAY 1000002 6.97366941E+01 # sup_L decays # BR NDA ID1 ID2 2.13518517E-03 2 1000022 2 # BR(~u_L -> ~chi_10 u) 8.49210037E-02 2 1000023 2 # BR(~u_L -> ~chi_20 u) 2.72533879E-04 2 1000025 2 # BR(~u_L -> ~chi_30 u) 4.03435386E-03 2 1000035 2 # BR(~u_L -> ~chi_40 u) 1.71851278E-01 2 1000024 1 # BR(~u_L -> ~chi_1+ d) 5.12165391E-03 2 1000037 1 # BR(~u_L -> ~chi_2+ d) 7.31663991E-01 2 1000021 2 # BR(~u_L -> ~g u) # # PDG Width DECAY 2000002 5.44569139E+01 # sup_R decays # BR NDA ID1 ID2 6.29470484E-02 2 1000022 2 # BR(~u_R -> ~chi_10 u) 2.11300540E-04 2 1000023 2 # BR(~u_R -> ~chi_20 u) 1.17692759E-04 2 1000025 2 # BR(~u_R -> ~chi_30 u) 4.60583405E-04 2 1000035 2 # BR(~u_R -> ~chi_40 u) 0.00000000E+00 2 1000024 1 # BR(~u_R -> ~chi_1+ d) 0.00000000E+00 2 1000037 1 # BR(~u_R -> ~chi_2+ d) 9.36263375E-01 2 1000021 2 # BR(~u_R -> ~g u) # # PDG Width DECAY 1000001 7.00587302E+01 # sdown_L decays # BR NDA ID1 ID2 4.17598062E-03 2 1000022 1 # BR(~d_L -> ~chi_10 d) 8.11292744E-02 2 1000023 1 # BR(~d_L -> ~chi_20 d) 4.53766766E-04 2 1000025 1 # BR(~d_L -> ~chi_30 d) 5.32901315E-03 2 1000035 1 # BR(~d_L -> ~chi_40 d) 1.59960207E-01 2 -1000024 2 # BR(~d_L -> ~chi_1- u) 1.51367547E-02 2 -1000037 2 # BR(~d_L -> ~chi_2- u) 7.33815004E-01 2 1000021 1 # BR(~d_L -> ~g d) # # PDG Width DECAY 2000001 5.17432847E+01 # sdown_R decays # BR NDA ID1 ID2 1.65465685E-02 2 1000022 1 # BR(~d_R -> ~chi_10 d) 5.55400145E-05 2 1000023 1 # BR(~d_R -> ~chi_20 d) 3.09266699E-05 2 1000025 1 # BR(~d_R -> ~chi_30 d) 1.21026644E-04 2 1000035 1 # BR(~d_R -> ~chi_40 d) 0.00000000E+00 2 -1000024 2 # BR(~d_R -> ~chi_1- u) 0.00000000E+00 2 -1000037 2 # BR(~d_R -> ~chi_2- u) 9.83245938E-01 2 1000021 1 # BR(~d_R -> ~g d) # # PDG Width DECAY 1000004 6.97366941E+01 # scharm_L decays # BR NDA ID1 ID2 2.13518517E-03 2 1000022 4 # BR(~c_L -> ~chi_10 c) 8.49210037E-02 2 1000023 4 # BR(~c_L -> ~chi_20 c) 2.72533879E-04 2 1000025 4 # BR(~c_L -> ~chi_30 c) 4.03435386E-03 2 1000035 4 # BR(~c_L -> ~chi_40 c) 1.71851278E-01 2 1000024 3 # BR(~c_L -> ~chi_1+ s) 5.12165391E-03 2 1000037 3 # BR(~c_L -> ~chi_2+ s) 7.31663991E-01 2 1000021 4 # BR(~c_L -> ~g c) # # PDG Width DECAY 2000004 5.44569139E+01 # scharm_R decays # BR NDA ID1 ID2 6.29470484E-02 2 1000022 4 # BR(~c_R -> ~chi_10 c) 2.11300540E-04 2 1000023 4 # BR(~c_R -> ~chi_20 c) 1.17692759E-04 2 1000025 4 # BR(~c_R -> ~chi_30 c) 4.60583405E-04 2 1000035 4 # BR(~c_R -> ~chi_40 c) 0.00000000E+00 2 1000024 3 # BR(~c_R -> ~chi_1+ s) 0.00000000E+00 2 1000037 3 # BR(~c_R -> ~chi_2+ s) 9.36263375E-01 2 1000021 4 # BR(~c_R -> ~g c) # # PDG Width DECAY 1000003 7.00587302E+01 # sstrange_L decays # BR NDA ID1 ID2 4.17598062E-03 2 1000022 3 # BR(~s_L -> ~chi_10 s) 8.11292744E-02 2 1000023 3 # BR(~s_L -> ~chi_20 s) 4.53766766E-04 2 1000025 3 # BR(~s_L -> ~chi_30 s) 5.32901315E-03 2 1000035 3 # BR(~s_L -> ~chi_40 s) 1.59960207E-01 2 -1000024 4 # BR(~s_L -> ~chi_1- c) 1.51367547E-02 2 -1000037 4 # BR(~s_L -> ~chi_2- c) 7.33815004E-01 2 1000021 3 # BR(~s_L -> ~g s) # # PDG Width DECAY 2000003 5.17432847E+01 # sstrange_R decays # BR NDA ID1 ID2 1.65465685E-02 2 1000022 3 # BR(~s_R -> ~chi_10 s) 5.55400145E-05 2 1000023 3 # BR(~s_R -> ~chi_20 s) 3.09266699E-05 2 1000025 3 # BR(~s_R -> ~chi_30 s) 1.21026644E-04 2 1000035 3 # BR(~s_R -> ~chi_40 s) 0.00000000E+00 2 -1000024 4 # BR(~s_R -> ~chi_1- c) 0.00000000E+00 2 -1000037 4 # BR(~s_R -> ~chi_2- c) 9.83245938E-01 2 1000021 3 # BR(~s_R -> ~g s) # # PDG Width DECAY 1000011 1.89560173E+01 # selectron_L decays # BR NDA ID1 ID2 8.50695192E-02 2 1000022 11 # BR(~e_L -> ~chi_10 e-) 3.04422052E-01 2 1000023 11 # BR(~e_L -> ~chi_20 e-) 4.61195429E-04 2 1000025 11 # BR(~e_L -> ~chi_30 e-) 9.79407881E-03 2 1000035 11 # BR(~e_L -> ~chi_40 e-) 5.49478974E-01 2 -1000024 12 # BR(~e_L -> ~chi_1- nu_e) 5.07741802E-02 2 -1000037 12 # BR(~e_L -> ~chi_2- nu_e) # # PDG Width DECAY 2000011 7.28776336E+00 # selectron_R decays # BR NDA ID1 ID2 9.87881974E-01 2 1000022 11 # BR(~e_R -> ~chi_10 e-) 3.29981923E-03 2 1000023 11 # BR(~e_R -> ~chi_20 e-) 1.79752313E-03 2 1000025 11 # BR(~e_R -> ~chi_30 e-) 7.02068362E-03 2 1000035 11 # BR(~e_R -> ~chi_40 e-) 0.00000000E+00 2 -1000024 12 # BR(~e_R -> ~chi_1- nu_e) 0.00000000E+00 2 -1000037 12 # BR(~e_R -> ~chi_2- nu_e) # # PDG Width DECAY 1000013 1.89560173E+01 # smuon_L decays # BR NDA ID1 ID2 8.50695192E-02 2 1000022 13 # BR(~mu_L -> ~chi_10 mu-) 3.04422052E-01 2 1000023 13 # BR(~mu_L -> ~chi_20 mu-) 4.61195429E-04 2 1000025 13 # BR(~mu_L -> ~chi_30 mu-) 9.79407881E-03 2 1000035 13 # BR(~mu_L -> ~chi_40 mu-) 5.49478974E-01 2 -1000024 14 # BR(~mu_L -> ~chi_1- nu_mu) 5.07741802E-02 2 -1000037 14 # BR(~mu_L -> ~chi_2- nu_mu) # # PDG Width DECAY 2000013 7.28776336E+00 # smuon_R decays # BR NDA ID1 ID2 9.87881974E-01 2 1000022 13 # BR(~mu_R -> ~chi_10 mu-) 3.29981923E-03 2 1000023 13 # BR(~mu_R -> ~chi_20 mu-) 1.79752313E-03 2 1000025 13 # BR(~mu_R -> ~chi_30 mu-) 7.02068362E-03 2 1000035 13 # BR(~mu_R -> ~chi_40 mu-) 0.00000000E+00 2 -1000024 14 # BR(~mu_R -> ~chi_1- nu_mu) 0.00000000E+00 2 -1000037 14 # BR(~mu_R -> ~chi_2- nu_mu) # # PDG Width DECAY 1000015 8.24807251E+00 # stau_1 decays # BR NDA ID1 ID2 8.38602901E-01 2 1000022 15 # BR(~tau_1 -> ~chi_10 tau-) 4.86007412E-02 2 1000023 15 # BR(~tau_1 -> ~chi_20 tau-) 1.14356540E-02 2 1000025 15 # BR(~tau_1 -> ~chi_30 tau-) 8.52209631E-03 2 1000035 15 # BR(~tau_1 -> ~chi_40 tau-) 8.65282764E-02 2 -1000024 16 # BR(~tau_1 -> ~chi_1- nu_tau) 6.31033104E-03 2 -1000037 16 # BR(~tau_1 -> ~chi_2- nu_tau) 0.00000000E+00 2 1000016 -37 # BR(~tau_1 -> ~nu_tauL H-) 0.00000000E+00 2 1000016 -24 # BR(~tau_1 -> ~nu_tauL W-) # # PDG Width DECAY 2000015 1.85221018E+01 # stau_2 decays # BR NDA ID1 ID2 9.88781367E-02 2 1000022 15 # BR(~tau_2 -> ~chi_10 tau-) 2.91028031E-01 2 1000023 15 # BR(~tau_2 -> ~chi_20 tau-) 8.07736393E-03 2 1000025 15 # BR(~tau_2 -> ~chi_30 tau-) 1.98225111E-02 2 1000035 15 # BR(~tau_2 -> ~chi_40 tau-) 5.22468322E-01 2 -1000024 16 # BR(~tau_2 -> ~chi_1- nu_tau) 5.97256353E-02 2 -1000037 16 # BR(~tau_2 -> ~chi_2- nu_tau) 0.00000000E+00 2 1000016 -37 # BR(~tau_2 -> ~nu_tauL H-) 0.00000000E+00 2 1000016 -24 # BR(~tau_2 -> ~nu_tauL W-) 0.00000000E+00 2 1000015 25 # BR(~tau_2 -> ~tau_1 h) 0.00000000E+00 2 1000015 35 # BR(~tau_2 -> ~tau_1 H) 0.00000000E+00 2 1000015 36 # BR(~tau_2 -> ~tau_1 A) 0.00000000E+00 2 1000015 23 # BR(~tau_2 -> ~tau_1 Z) # # PDG Width DECAY 1000012 1.89960334E+01 # snu_eL decays # BR NDA ID1 ID2 1.05777173E-01 2 1000022 12 # BR(~nu_eL -> ~chi_10 nu_e) 2.65110565E-01 2 1000023 12 # BR(~nu_eL -> ~chi_20 nu_e) 2.27708934E-03 2 1000025 12 # BR(~nu_eL -> ~chi_30 nu_e) 2.27045033E-02 2 1000035 12 # BR(~nu_eL -> ~chi_40 nu_e) 5.87042258E-01 2 1000024 11 # BR(~nu_eL -> ~chi_1+ e-) 1.70884115E-02 2 1000037 11 # BR(~nu_eL -> ~chi_2+ e-) # # PDG Width DECAY 1000014 1.89960334E+01 # snu_muL decays # BR NDA ID1 ID2 1.05777173E-01 2 1000022 14 # BR(~nu_muL -> ~chi_10 nu_mu) 2.65110565E-01 2 1000023 14 # BR(~nu_muL -> ~chi_20 nu_mu) 2.27708934E-03 2 1000025 14 # BR(~nu_muL -> ~chi_30 nu_mu) 2.27045033E-02 2 1000035 14 # BR(~nu_muL -> ~chi_40 nu_mu) 5.87042258E-01 2 1000024 13 # BR(~nu_muL -> ~chi_1+ mu-) 1.70884115E-02 2 1000037 13 # BR(~nu_muL -> ~chi_2+ mu-) # # PDG Width DECAY 1000016 1.91370930E+01 # snu_tauL decays # BR NDA ID1 ID2 1.04554475E-01 2 1000022 16 # BR(~nu_tauL -> ~chi_10 nu_tau) 2.61961375E-01 2 1000023 16 # BR(~nu_tauL -> ~chi_20 nu_tau) 2.24673432E-03 2 1000025 16 # BR(~nu_tauL -> ~chi_30 nu_tau) 2.23989114E-02 2 1000035 16 # BR(~nu_tauL -> ~chi_40 nu_tau) 5.81434076E-01 2 1000024 15 # BR(~nu_tauL -> ~chi_1+ tau-) 2.74044284E-02 2 1000037 15 # BR(~nu_tauL -> ~chi_2+ tau-) 0.00000000E+00 2 -1000015 -37 # BR(~nu_tauL -> ~tau_1+ H-) 0.00000000E+00 2 -2000015 -37 # BR(~nu_tauL -> ~tau_2+ H-) 0.00000000E+00 2 -1000015 -24 # BR(~nu_tauL -> ~tau_1+ W-) 0.00000000E+00 2 -2000015 -24 # BR(~nu_tauL -> ~tau_2+ W-) # # PDG Width DECAY 1000024 6.04568843E-03 # chargino1+ decays # BR NDA ID1 ID2 0.00000000E+00 2 1000002 -1 # BR(~chi_1+ -> ~u_L db) 0.00000000E+00 2 2000002 -1 # BR(~chi_1+ -> ~u_R db) 0.00000000E+00 2 -1000001 2 # BR(~chi_1+ -> ~d_L* u ) 0.00000000E+00 2 -2000001 2 # BR(~chi_1+ -> ~d_R* u ) 0.00000000E+00 2 1000004 -3 # BR(~chi_1+ -> ~c_L sb) 0.00000000E+00 2 2000004 -3 # BR(~chi_1+ -> ~c_R sb) 0.00000000E+00 2 -1000003 4 # BR(~chi_1+ -> ~s_L* c ) 0.00000000E+00 2 -2000003 4 # BR(~chi_1+ -> ~s_R* c ) 0.00000000E+00 2 1000006 -5 # BR(~chi_1+ -> ~t_1 bb) 0.00000000E+00 2 2000006 -5 # BR(~chi_1+ -> ~t_2 bb) 0.00000000E+00 2 -1000005 6 # BR(~chi_1+ -> ~b_1* t ) 0.00000000E+00 2 -2000005 6 # BR(~chi_1+ -> ~b_2* t ) 0.00000000E+00 2 1000012 -11 # BR(~chi_1+ -> ~nu_eL e+ ) 0.00000000E+00 2 1000014 -13 # BR(~chi_1+ -> ~nu_muL mu+ ) 0.00000000E+00 2 1000016 -15 # BR(~chi_1+ -> ~nu_tau1 tau+) 0.00000000E+00 2 -1000011 12 # BR(~chi_1+ -> ~e_L+ nu_e) 0.00000000E+00 2 -2000011 12 # BR(~chi_1+ -> ~e_R+ nu_e) 0.00000000E+00 2 -1000013 14 # BR(~chi_1+ -> ~mu_L+ nu_mu) 0.00000000E+00 2 -2000013 14 # BR(~chi_1+ -> ~mu_R+ nu_mu) 0.00000000E+00 2 -1000015 16 # BR(~chi_1+ -> ~tau_1+ nu_tau) 0.00000000E+00 2 -2000015 16 # BR(~chi_1+ -> ~tau_2+ nu_tau) 1.00000000E+00 2 1000022 24 # BR(~chi_1+ -> ~chi_10 W+) 0.00000000E+00 2 1000023 24 # BR(~chi_1+ -> ~chi_20 W+) 0.00000000E+00 2 1000025 24 # BR(~chi_1+ -> ~chi_30 W+) 0.00000000E+00 2 1000035 24 # BR(~chi_1+ -> ~chi_40 W+) 0.00000000E+00 2 1000022 37 # BR(~chi_1+ -> ~chi_10 H+) 0.00000000E+00 2 1000023 37 # BR(~chi_1+ -> ~chi_20 H+) 0.00000000E+00 2 1000025 37 # BR(~chi_1+ -> ~chi_30 H+) 0.00000000E+00 2 1000035 37 # BR(~chi_1+ -> ~chi_40 H+) # # PDG Width DECAY 1000037 2.80411818E+00 # chargino2+ decays # BR NDA ID1 ID2 0.00000000E+00 2 1000002 -1 # BR(~chi_2+ -> ~u_L db) 0.00000000E+00 2 2000002 -1 # BR(~chi_2+ -> ~u_R db) 0.00000000E+00 2 -1000001 2 # BR(~chi_2+ -> ~d_L* u ) 0.00000000E+00 2 -2000001 2 # BR(~chi_2+ -> ~d_R* u ) 0.00000000E+00 2 1000004 -3 # BR(~chi_2+ -> ~c_L sb) 0.00000000E+00 2 2000004 -3 # BR(~chi_2+ -> ~c_R sb) 0.00000000E+00 2 -1000003 4 # BR(~chi_2+ -> ~s_L* c ) 0.00000000E+00 2 -2000003 4 # BR(~chi_2+ -> ~s_R* c ) 0.00000000E+00 2 1000006 -5 # BR(~chi_2+ -> ~t_1 bb) 0.00000000E+00 2 2000006 -5 # BR(~chi_2+ -> ~t_2 bb) 0.00000000E+00 2 -1000005 6 # BR(~chi_2+ -> ~b_1* t ) 0.00000000E+00 2 -2000005 6 # BR(~chi_2+ -> ~b_2* t ) 0.00000000E+00 2 1000012 -11 # BR(~chi_2+ -> ~nu_eL e+ ) 0.00000000E+00 2 1000014 -13 # BR(~chi_2+ -> ~nu_muL mu+ ) 0.00000000E+00 2 1000016 -15 # BR(~chi_2+ -> ~nu_tau1 tau+) 0.00000000E+00 2 -1000011 12 # BR(~chi_2+ -> ~e_L+ nu_e) 0.00000000E+00 2 -2000011 12 # BR(~chi_2+ -> ~e_R+ nu_e) 0.00000000E+00 2 -1000013 14 # BR(~chi_2+ -> ~mu_L+ nu_mu) 0.00000000E+00 2 -2000013 14 # BR(~chi_2+ -> ~mu_R+ nu_mu) 0.00000000E+00 2 -1000015 16 # BR(~chi_2+ -> ~tau_1+ nu_tau) 0.00000000E+00 2 -2000015 16 # BR(~chi_2+ -> ~tau_2+ nu_tau) 2.98772282E-01 2 1000024 23 # BR(~chi_2+ -> ~chi_1+ Z ) 9.50834392E-02 2 1000022 24 # BR(~chi_2+ -> ~chi_10 W+) 3.47817700E-01 2 1000023 24 # BR(~chi_2+ -> ~chi_20 W+) 0.00000000E+00 2 1000025 24 # BR(~chi_2+ -> ~chi_30 W+) 0.00000000E+00 2 1000035 24 # BR(~chi_2+ -> ~chi_40 W+) 2.58326579E-01 2 1000024 25 # BR(~chi_2+ -> ~chi_1+ h ) 0.00000000E+00 2 1000024 35 # BR(~chi_2+ -> ~chi_1+ H ) 0.00000000E+00 2 1000024 36 # BR(~chi_2+ -> ~chi_1+ A ) 0.00000000E+00 2 1000022 37 # BR(~chi_2+ -> ~chi_10 H+) 0.00000000E+00 2 1000023 37 # BR(~chi_2+ -> ~chi_20 H+) 0.00000000E+00 2 1000025 37 # BR(~chi_2+ -> ~chi_30 H+) 0.00000000E+00 2 1000035 37 # BR(~chi_2+ -> ~chi_40 H+) # # PDG Width DECAY 1000022 0.00000000E+00 # neutralino1 decays # # PDG Width DECAY 1000023 1.00000000E-03 # neutralino2 decays # BR NDA ID1 ID2 1.00000000E+00 2 1000022 23 # BR(~chi_20 -> ~chi_10 Z ) 0.00000000E+00 2 1000024 -24 # BR(~chi_20 -> ~chi_1+ W-) 0.00000000E+00 2 -1000024 24 # BR(~chi_20 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_20 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_20 -> ~chi_2- W+) 0.00000000E+00 2 1000022 25 # BR(~chi_20 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_20 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_20 -> ~chi_10 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_20 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_20 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_20 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_20 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_20 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_20 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_20 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_20 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_20 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_20 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_20 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_20 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_20 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_20 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_20 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_20 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_20 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_20 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_20 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_20 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_20 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_20 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_20 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_20 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_20 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_20 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_20 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_20 -> ~b_2* b ) 0.00000000E+00 2 1000011 -11 # BR(~chi_20 -> ~e_L- e+) 0.00000000E+00 2 -1000011 11 # BR(~chi_20 -> ~e_L+ e-) 0.00000000E+00 2 2000011 -11 # BR(~chi_20 -> ~e_R- e+) 0.00000000E+00 2 -2000011 11 # BR(~chi_20 -> ~e_R+ e-) 0.00000000E+00 2 1000013 -13 # BR(~chi_20 -> ~mu_L- mu+) 0.00000000E+00 2 -1000013 13 # BR(~chi_20 -> ~mu_L+ mu-) 0.00000000E+00 2 2000013 -13 # BR(~chi_20 -> ~mu_R- mu+) 0.00000000E+00 2 -2000013 13 # BR(~chi_20 -> ~mu_R+ mu-) 0.00000000E+00 2 1000015 -15 # BR(~chi_20 -> ~tau_1- tau+) 0.00000000E+00 2 -1000015 15 # BR(~chi_20 -> ~tau_1+ tau-) 0.00000000E+00 2 2000015 -15 # BR(~chi_20 -> ~tau_2- tau+) 0.00000000E+00 2 -2000015 15 # BR(~chi_20 -> ~tau_2+ tau-) 0.00000000E+00 2 1000012 -12 # BR(~chi_20 -> ~nu_eL nu_eb) 0.00000000E+00 2 -1000012 12 # BR(~chi_20 -> ~nu_eL* nu_e ) 0.00000000E+00 2 1000014 -14 # BR(~chi_20 -> ~nu_muL nu_mub) 0.00000000E+00 2 -1000014 14 # BR(~chi_20 -> ~nu_muL* nu_mu ) 0.00000000E+00 2 1000016 -16 # BR(~chi_20 -> ~nu_tau1 nu_taub) 0.00000000E+00 2 -1000016 16 # BR(~chi_20 -> ~nu_tau1* nu_tau ) # # PDG Width DECAY 1000025 2.66094361E+00 # neutralino3 decays # BR NDA ID1 ID2 1.03551919E-01 2 1000022 23 # BR(~chi_30 -> ~chi_10 Z ) 2.50581402E-01 2 1000023 23 # BR(~chi_30 -> ~chi_20 Z ) 3.04220186E-01 2 1000024 -24 # BR(~chi_30 -> ~chi_1+ W-) 3.04220186E-01 2 -1000024 24 # BR(~chi_30 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_30 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_30 -> ~chi_2- W+) 2.11117491E-02 2 1000022 25 # BR(~chi_30 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_30 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_30 -> ~chi_10 A ) 1.63145570E-02 2 1000023 25 # BR(~chi_30 -> ~chi_20 h ) 0.00000000E+00 2 1000023 35 # BR(~chi_30 -> ~chi_20 H ) 0.00000000E+00 2 1000023 36 # BR(~chi_30 -> ~chi_20 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_30 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_30 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_30 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_30 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_30 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_30 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_30 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_30 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_30 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_30 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_30 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_30 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_30 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_30 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_30 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_30 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_30 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_30 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_30 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_30 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_30 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_30 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_30 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_30 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_30 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_30 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_30 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_30 -> ~b_2* b ) 0.00000000E+00 2 1000011 -11 # BR(~chi_30 -> ~e_L- e+) 0.00000000E+00 2 -1000011 11 # BR(~chi_30 -> ~e_L+ e-) 0.00000000E+00 2 2000011 -11 # BR(~chi_30 -> ~e_R- e+) 0.00000000E+00 2 -2000011 11 # BR(~chi_30 -> ~e_R+ e-) 0.00000000E+00 2 1000013 -13 # BR(~chi_30 -> ~mu_L- mu+) 0.00000000E+00 2 -1000013 13 # BR(~chi_30 -> ~mu_L+ mu-) 0.00000000E+00 2 2000013 -13 # BR(~chi_30 -> ~mu_R- mu+) 0.00000000E+00 2 -2000013 13 # BR(~chi_30 -> ~mu_R+ mu-) 0.00000000E+00 2 1000015 -15 # BR(~chi_30 -> ~tau_1- tau+) 0.00000000E+00 2 -1000015 15 # BR(~chi_30 -> ~tau_1+ tau-) 0.00000000E+00 2 2000015 -15 # BR(~chi_30 -> ~tau_2- tau+) 0.00000000E+00 2 -2000015 15 # BR(~chi_30 -> ~tau_2+ tau-) 0.00000000E+00 2 1000012 -12 # BR(~chi_30 -> ~nu_eL nu_eb) 0.00000000E+00 2 -1000012 12 # BR(~chi_30 -> ~nu_eL* nu_e ) 0.00000000E+00 2 1000014 -14 # BR(~chi_30 -> ~nu_muL nu_mub) 0.00000000E+00 2 -1000014 14 # BR(~chi_30 -> ~nu_muL* nu_mu ) 0.00000000E+00 2 1000016 -16 # BR(~chi_30 -> ~nu_tau1 nu_taub) 0.00000000E+00 2 -1000016 16 # BR(~chi_30 -> ~nu_tau1* nu_tau ) # # PDG Width DECAY 1000035 2.76313390E+00 # neutralino4 decays # BR NDA ID1 ID2 2.45444969E-02 2 1000022 23 # BR(~chi_40 -> ~chi_10 Z ) 2.36477385E-02 2 1000023 23 # BR(~chi_40 -> ~chi_20 Z ) 0.00000000E+00 2 1000025 23 # BR(~chi_40 -> ~chi_30 Z ) 3.16676477E-01 2 1000024 -24 # BR(~chi_40 -> ~chi_1+ W-) 3.16676477E-01 2 -1000024 24 # BR(~chi_40 -> ~chi_1- W+) 0.00000000E+00 2 1000037 -24 # BR(~chi_40 -> ~chi_2+ W-) 0.00000000E+00 2 -1000037 24 # BR(~chi_40 -> ~chi_2- W+) 8.67251407E-02 2 1000022 25 # BR(~chi_40 -> ~chi_10 h ) 0.00000000E+00 2 1000022 35 # BR(~chi_40 -> ~chi_10 H ) 0.00000000E+00 2 1000022 36 # BR(~chi_40 -> ~chi_10 A ) 2.31729670E-01 2 1000023 25 # BR(~chi_40 -> ~chi_20 h ) 0.00000000E+00 2 1000023 35 # BR(~chi_40 -> ~chi_20 H ) 0.00000000E+00 2 1000023 36 # BR(~chi_40 -> ~chi_20 A ) 0.00000000E+00 2 1000025 25 # BR(~chi_40 -> ~chi_30 h ) 0.00000000E+00 2 1000025 35 # BR(~chi_40 -> ~chi_30 H ) 0.00000000E+00 2 1000025 36 # BR(~chi_40 -> ~chi_30 A ) 0.00000000E+00 2 1000024 -37 # BR(~chi_40 -> ~chi_1+ H-) 0.00000000E+00 2 -1000024 37 # BR(~chi_40 -> ~chi_1- H+) 0.00000000E+00 2 1000037 -37 # BR(~chi_40 -> ~chi_2+ H-) 0.00000000E+00 2 -1000037 37 # BR(~chi_40 -> ~chi_2- H+) 0.00000000E+00 2 1000002 -2 # BR(~chi_40 -> ~u_L ub) 0.00000000E+00 2 -1000002 2 # BR(~chi_40 -> ~u_L* u ) 0.00000000E+00 2 2000002 -2 # BR(~chi_40 -> ~u_R ub) 0.00000000E+00 2 -2000002 2 # BR(~chi_40 -> ~u_R* u ) 0.00000000E+00 2 1000001 -1 # BR(~chi_40 -> ~d_L db) 0.00000000E+00 2 -1000001 1 # BR(~chi_40 -> ~d_L* d ) 0.00000000E+00 2 2000001 -1 # BR(~chi_40 -> ~d_R db) 0.00000000E+00 2 -2000001 1 # BR(~chi_40 -> ~d_R* d ) 0.00000000E+00 2 1000004 -4 # BR(~chi_40 -> ~c_L cb) 0.00000000E+00 2 -1000004 4 # BR(~chi_40 -> ~c_L* c ) 0.00000000E+00 2 2000004 -4 # BR(~chi_40 -> ~c_R cb) 0.00000000E+00 2 -2000004 4 # BR(~chi_40 -> ~c_R* c ) 0.00000000E+00 2 1000003 -3 # BR(~chi_40 -> ~s_L sb) 0.00000000E+00 2 -1000003 3 # BR(~chi_40 -> ~s_L* s ) 0.00000000E+00 2 2000003 -3 # BR(~chi_40 -> ~s_R sb) 0.00000000E+00 2 -2000003 3 # BR(~chi_40 -> ~s_R* s ) 0.00000000E+00 2 1000006 -6 # BR(~chi_40 -> ~t_1 tb) 0.00000000E+00 2 -1000006 6 # BR(~chi_40 -> ~t_1* t ) 0.00000000E+00 2 2000006 -6 # BR(~chi_40 -> ~t_2 tb) 0.00000000E+00 2 -2000006 6 # BR(~chi_40 -> ~t_2* t ) 0.00000000E+00 2 1000005 -5 # BR(~chi_40 -> ~b_1 bb) 0.00000000E+00 2 -1000005 5 # BR(~chi_40 -> ~b_1* b ) 0.00000000E+00 2 2000005 -5 # BR(~chi_40 -> ~b_2 bb) 0.00000000E+00 2 -2000005 5 # BR(~chi_40 -> ~b_2* b ) 0.00000000E+00 2 1000011 -11 # BR(~chi_40 -> ~e_L- e+) 0.00000000E+00 2 -1000011 11 # BR(~chi_40 -> ~e_L+ e-) 0.00000000E+00 2 2000011 -11 # BR(~chi_40 -> ~e_R- e+) 0.00000000E+00 2 -2000011 11 # BR(~chi_40 -> ~e_R+ e-) 0.00000000E+00 2 1000013 -13 # BR(~chi_40 -> ~mu_L- mu+) 0.00000000E+00 2 -1000013 13 # BR(~chi_40 -> ~mu_L+ mu-) 0.00000000E+00 2 2000013 -13 # BR(~chi_40 -> ~mu_R- mu+) 0.00000000E+00 2 -2000013 13 # BR(~chi_40 -> ~mu_R+ mu-) 0.00000000E+00 2 1000015 -15 # BR(~chi_40 -> ~tau_1- tau+) 0.00000000E+00 2 -1000015 15 # BR(~chi_40 -> ~tau_1+ tau-) 0.00000000E+00 2 2000015 -15 # BR(~chi_40 -> ~tau_2- tau+) 0.00000000E+00 2 -2000015 15 # BR(~chi_40 -> ~tau_2+ tau-) 0.00000000E+00 2 1000012 -12 # BR(~chi_40 -> ~nu_eL nu_eb) 0.00000000E+00 2 -1000012 12 # BR(~chi_40 -> ~nu_eL* nu_e ) 0.00000000E+00 2 1000014 -14 # BR(~chi_40 -> ~nu_muL nu_mub) 0.00000000E+00 2 -1000014 14 # BR(~chi_40 -> ~nu_muL* nu_mu ) 0.00000000E+00 2 1000016 -16 # BR(~chi_40 -> ~nu_tau1 nu_taub) 0.00000000E+00 2 -1000016 16 # BR(~chi_40 -> ~nu_tau1* nu_tau ) pythia8-8.1.80.orig/examples/main24.cc0000644000175000017500000000421512217346165015561 0ustar sunsun// main24.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Peter Skands, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how to run SUSY processes in Pythia8. // All input is specified in the main22.cmnd file. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator. Shorthand for the event. Pythia pythia; Event& event = pythia.event; // Read in commands from external file. pythia.readFile("main24.cmnd"); // Extract settings to be used in the main program. int nEvent = pythia.mode("Main:numberOfEvents"); int nAbort = pythia.mode("Main:timesAllowErrors"); double eCM = pythia.parm("Beams:eCM"); // Initialize. pythia.init(); // Histograms. double epTol = 1e-6 * eCM; Hist epCons("deviation from energy-momentum conservation",100,0.,epTol); Hist nFinal("final particle multiplicity",100,-0.5,799.5); Hist dnparticledy("dn/dy for particles",100,-10.,10.); // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if failure. if (!pythia.next()) { if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Loop over final particles in the event. int nFin = 0; Vec4 pSum; for (int i = 0; i < event.size(); ++i) if (event[i].isFinal()) { nFin++; pSum += event[i].p(); dnparticledy.fill(event[i].y()); } // Check and print event with too big energy-momentum deviation. nFinal.fill(nFin); double epDev = abs(pSum.e() - eCM) + abs(pSum.px()) + abs(pSum.py()) + abs(pSum.pz()); epCons.fill(epDev); if (epDev > epTol) { cout << " Warning! Event with epDev = " << scientific << setprecision(4) << epDev << " now listed:"; event.list(); } // End of event loop. } // Final statistics and histogram output. pythia.stat(); cout << epCons << nFinal << dnparticledy; return 0; } pythia8-8.1.80.orig/examples/ttbar.lhe0000644000175000017500000052660112217346207015773 0ustar sunsun 2212 -2212 9.800000E+02 9.800000E+02 0 0 7 7 3 2 5.220106E+00 5.384128E-01 1.000000E+00 81 2.602564E-01 1.062492E-01 1.000000E+00 82 12 81 1.000000E+00 1.733125E+02 7.819848E-03 1.156692E-01 2 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 1.0838163607E+02 1.0838163607E+02 0.0000000000E+00 0. 9. -2 -1 0 0 0 102 0.0000000000E+00 0.0000000000E+00 -2.7976111253E+02 2.7976111253E+02 0.0000000000E+00 0. 9. 6 2 1 2 101 0 3.3629095553E+01 8.9115695965E+00 -1.1059648961E+02 2.1241781824E+02 1.7798711709E+02 0. 9. -6 2 1 2 0 102 -3.3629095553E+01 -8.9115695965E+00 -6.0782986840E+01 1.7572493036E+02 1.6116559038E+02 0. 9. 24 2 3 0 0 0 -3.0884654830E+01 -1.2140252163E+01 -4.7852784957E+00 8.6623320800E+01 7.9871479200E+01 0. 9. 5 1 3 0 101 0 6.4513750383E+01 2.1051821759E+01 -1.0581121112E+02 1.2579449744E+02 4.8000000000E+00 0. 9. -24 2 4 0 0 0 -5.0940382043E+01 3.4880802250E+01 -7.5291578188E+01 1.2621743906E+02 8.0314552164E+01 0. 9. -5 1 4 0 0 102 1.7311286490E+01 -4.3792371846E+01 1.4508591348E+01 4.9507491299E+01 4.8000000000E+00 0. 9. -1 1 5 0 0 103 1.8584463332E+01 9.1657242037E+00 1.8652036768E+01 2.7881896512E+01 3.3000000000E-01 0. 9. 2 1 5 0 103 0 -4.9469118162E+01 -2.1305976366E+01 -2.3437315264E+01 5.8741424288E+01 3.3000000000E-01 0. 9. 13 1 7 0 0 0 9.6912588119E+00 3.9074488577E+01 -2.5560060185E+01 4.7687147069E+01 1.0566000000E-01 0. 9. -14 1 7 0 0 0 -6.0631640855E+01 -4.1936863270E+00 -4.9731518002E+01 7.8530291993E+01 0.0000000000E+00 0. 9. #pdf 2 -2 1.1059350620E-01 2.8547052299E-01 1.7331247164E+02 5.5300424188E-01 3.5718362666E-01 12 81 1.000000E+00 2.453729E+02 7.850576E-03 1.102586E-01 2 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 1.4168500180E+02 1.4168500180E+02 0.0000000000E+00 0. 9. -2 -1 0 0 0 102 0.0000000000E+00 0.0000000000E+00 -5.1193431229E+02 5.1193431229E+02 0.0000000000E+00 0. 9. 6 2 1 2 101 0 1.4483021237E+02 -9.1836222700E+01 -3.2020944169E+02 4.0376632938E+02 1.7630507646E+02 0. 9. -6 2 1 2 0 102 -1.4483021237E+02 9.1836222700E+01 -5.0039868808E+01 2.4985298471E+02 1.7467925831E+02 0. 9. 24 2 3 0 0 0 6.6573250937E+01 -1.0557760324E+02 -2.7628620725E+02 3.1285280962E+02 7.7228130408E+01 0. 9. 5 1 3 0 101 0 7.8256961429E+01 1.3741380542E+01 -4.3923234434E+01 9.0913519757E+01 4.8000000000E+00 0. 9. -24 2 4 0 0 0 -5.2331928485E+01 1.3655957736E+01 3.5832022017E+01 1.0130969814E+02 7.7811343743E+01 0. 9. -5 1 4 0 0 102 -9.2498283882E+01 7.8180264964E+01 -8.5871890826E+01 1.4854328657E+02 4.8000000000E+00 0. 9. -3 1 5 0 0 103 1.3698476364E+01 -8.8968981168E+01 -1.5010039084E+02 1.7502429887E+02 5.0000000000E-01 0. 9. 4 1 5 0 103 0 5.2874774574E+01 -1.6608622073E+01 -1.2618581641E+02 1.3782851075E+02 1.5000000000E+00 0. 9. 15 1 7 0 0 0 -5.3810426731E+01 -1.6793177176E+00 -8.3584775043E+00 5.4510586203E+01 1.7770000000E+00 0. 9. -16 1 7 0 0 0 1.4784982465E+00 1.5335275454E+01 4.4190499522E+01 4.6799111939E+01 0.0000000000E+00 0. 9. #pdf 2 -2 1.4457653245E-01 5.2238195132E-01 2.4537286698E+02 5.2138927060E-01 8.9715910577E-02 12 81 1.000000E+00 1.776410E+02 7.822020E-03 1.152678E-01 2 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 2.1971684569E+02 2.1971684569E+02 0.0000000000E+00 0. 9. -2 -1 0 0 0 102 0.0000000000E+00 0.0000000000E+00 -1.4407440590E+02 1.4407440590E+02 0.0000000000E+00 0. 9. 6 2 1 2 101 0 -2.8007358027E+01 -1.4336341199E+01 4.8014156840E+01 1.8405373765E+02 1.7487274317E+02 0. 9. -6 2 1 2 0 102 2.8007358027E+01 1.4336341199E+01 2.7628282952E+01 1.7973751394E+02 1.7479218837E+02 0. 9. 24 2 3 0 0 0 -1.9076498236E+01 -7.5377093349E+01 1.2033037033E+01 1.1247570567E+02 8.0376435601E+01 0. 9. 5 1 3 0 101 0 -8.9308597910E+00 6.1040752150E+01 3.5981119807E+01 7.1578031980E+01 4.8000000000E+00 0. 9. -24 2 4 0 0 0 -1.6204445062E+01 4.9039786977E+01 -3.0703182195E+01 9.8591888630E+01 7.8167706633E+01 0. 9. -5 1 4 0 0 102 4.4211803088E+01 -3.4703445778E+01 5.8331465148E+01 8.1145625313E+01 4.8000000000E+00 0. 9. -1 1 5 0 0 103 1.8159044482E+01 -6.8058553500E+00 2.6779046411E+01 3.3065038791E+01 3.3000000000E-01 0. 9. 2 1 5 0 103 0 -3.7235542717E+01 -6.8571237999E+01 -1.4746009379E+01 7.9410666883E+01 3.3000000000E-01 0. 9. 1 1 7 0 104 0 1.6465237456E+01 5.7169697352E+01 -2.4579279760E+01 6.4371796878E+01 3.3000000000E-01 0. 9. -2 1 7 0 0 104 -3.2669682518E+01 -8.1299103748E+00 -6.1239024357E+00 3.4220091752E+01 3.3000000000E-01 0. 9. #pdf 2 -2 2.2420086295E-01 1.4701469990E-01 1.7764102987E+02 4.4040101215E-01 5.2651382636E-01 12 81 1.000000E+00 2.161450E+02 7.839339E-03 1.121726E-01 2 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 2.0905097329E+02 2.0905097329E+02 0.0000000000E+00 0. 9. -2 -1 0 0 0 102 0.0000000000E+00 0.0000000000E+00 -2.2387000524E+02 2.2387000524E+02 0.0000000000E+00 0. 9. 6 2 1 2 101 0 -2.8666225329E+01 1.2254465689E+02 -1.6459167668E+01 2.1588531728E+02 1.7463281654E+02 0. 9. -6 2 1 2 0 102 2.8666225329E+01 -1.2254465689E+02 1.6401357138E+00 2.1703566125E+02 1.7681301650E+02 0. 9. 24 2 3 0 0 0 4.3122883270E+01 9.3368100532E+01 1.9268215950E+01 1.3041933870E+02 7.7850847804E+01 0. 9. 5 1 3 0 101 0 -7.1789108599E+01 2.9176556359E+01 -3.5727383618E+01 8.5465978580E+01 4.8000000000E+00 0. 9. -24 2 4 0 0 0 8.0222330450E+01 -8.3419791329E+01 3.4131504051E+01 1.4445800562E+02 7.9427148575E+01 0. 9. -5 1 4 0 0 102 -5.1556105120E+01 -3.9124865562E+01 -3.2491368337E+01 7.2577655631E+01 4.8000000000E+00 0. 9. -1 1 5 0 0 103 -2.0727740885E+01 8.6000619505E+00 7.4013836638E+00 2.3632386420E+01 3.3000000000E-01 0. 9. 2 1 5 0 103 0 6.3850624155E+01 8.4768038581E+01 1.1866832286E+01 1.0678695229E+02 3.3000000000E-01 0. 9. 15 1 7 0 0 0 2.3287382355E+01 -7.9738850156E+01 2.4246092562E+01 8.6554128351E+01 1.7770000000E+00 0. 9. -16 1 7 0 0 0 5.6934948095E+01 -3.6809411735E+00 9.8854114887E+00 5.7903877269E+01 0.0000000000E+00 0. 9. #pdf 2 -2 2.1331731968E-01 2.2843878086E-01 2.1614503722E+02 4.4865471863E-01 4.2889225859E-01 12 81 1.000000E+00 2.722156E+02 7.859798E-03 1.087399E-01 1 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 3.0998147853E+02 3.0998147853E+02 0.0000000000E+00 0. 9. -1 -1 0 0 0 102 0.0000000000E+00 0.0000000000E+00 -4.2658276564E+02 4.2658276564E+02 0.0000000000E+00 0. 9. 6 2 1 2 101 0 1.5202805136E+02 -1.3564883740E+02 -3.0207433868E+02 4.0425677542E+02 1.7510425150E+02 0. 9. -6 2 1 2 0 102 -1.5202805136E+02 1.3564883740E+02 1.8547305157E+02 3.3230746875E+02 1.8578176832E+02 0. 9. 24 2 3 0 0 0 7.0178719712E+01 -1.1462538992E+02 -2.7233123119E+02 3.1454060698E+02 8.1899091839E+01 0. 9. 5 1 3 0 101 0 8.1849331652E+01 -2.1023447476E+01 -2.9743107493E+01 8.9716168437E+01 4.8000000000E+00 0. 9. -24 2 4 0 0 0 -1.2759536169E+02 1.6377098894E+02 1.1113217675E+02 2.4901630836E+02 8.0976836044E+01 0. 9. -5 1 4 0 0 102 -2.4432689677E+01 -2.8122151538E+01 7.4340874815E+01 8.3291160397E+01 4.8000000000E+00 0. 9. -11 1 5 0 0 0 6.6986380224E+01 -9.2588244672E+01 -1.4177276647E+02 1.8209688493E+02 5.1000000000E-04 0. 9. 12 1 5 0 0 0 3.1923394877E+00 -2.2037145252E+01 -1.3055846472E+02 1.3244372206E+02 0.0000000000E+00 0. 9. 3 1 7 0 103 0 -4.5335729587E+01 4.3867031558E+01 7.7191694899E+01 9.9691788008E+01 5.0000000000E-01 0. 9. -4 1 7 0 0 103 -8.2259632100E+01 1.1990395738E+02 3.3940481854E+01 1.4932452035E+02 1.5000000000E+00 0. 9. #pdf 1 -1 3.1630763115E-01 4.3528853637E-01 2.7221557203E+02 1.1050631792E-01 4.7561700247E-02 12 81 1.000000E+00 1.977178E+02 7.831463E-03 1.135577E-01 2 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 1.1823767072E+02 1.1823767072E+02 0.0000000000E+00 0. 9. -2 -1 0 0 0 102 0.0000000000E+00 0.0000000000E+00 -4.8148219772E+02 4.8148219772E+02 0.0000000000E+00 0. 9. 6 2 1 2 101 0 -8.4928893369E+01 2.4123465107E+01 -1.4991519216E+01 2.0021660930E+02 1.7907285247E+02 0. 9. -6 2 1 2 0 102 8.4928893369E+01 -2.4123465107E+01 -3.4825300778E+02 3.9950325915E+02 1.7472217416E+02 0. 9. 24 2 3 0 0 0 -1.1650448565E+02 -1.5078974208E-01 2.4126028322E+01 1.4418554647E+02 8.1449914996E+01 0. 9. 5 1 3 0 101 0 3.1575592283E+01 2.4274254849E+01 -3.9117547538E+01 5.6031062830E+01 4.8000000000E+00 0. 9. -24 2 4 0 0 0 5.7935094570E+01 4.8480092038E+01 -2.5062691315E+02 2.7478823986E+02 8.3593855407E+01 0. 9. -5 1 4 0 0 102 2.6993798799E+01 -7.2603557145E+01 -9.7626094629E+01 1.2471501929E+02 4.8000000000E+00 0. 9. -11 1 5 0 0 0 -8.2872280006E+01 -7.5913977740E+00 -2.2508140913E+01 8.6209399262E+01 5.1000000000E-04 0. 9. 12 1 5 0 0 0 -3.3632205646E+01 7.4406080319E+00 4.6634169235E+01 5.7976147205E+01 0.0000000000E+00 0. 9. 3 1 7 0 103 0 7.8662492185E+01 4.4746476970E+01 -1.8697297810E+02 2.0772380561E+02 5.0000000000E-01 0. 9. -4 1 7 0 0 103 -2.0727397615E+01 3.7336150680E+00 -6.3653935055E+01 6.7064434250E+01 1.5000000000E+00 0. 9. #pdf 2 -2 1.2065068441E-01 4.9130836502E-01 1.9771778073E+02 5.4447327184E-01 1.1619205578E-01 12 81 1.000000E+00 1.778823E+02 7.822140E-03 1.152458E-01 2 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 2.6099463532E+02 2.6099463532E+02 0.0000000000E+00 0. 9. -2 -1 0 0 0 102 0.0000000000E+00 0.0000000000E+00 -1.2339705519E+02 1.2339705519E+02 0.0000000000E+00 0. 9. 6 2 1 2 101 0 1.1263886129E+01 -3.0918480940E+01 9.3920878645E+01 2.0039694932E+02 1.7393958220E+02 0. 9. -6 2 1 2 0 102 -1.1263886129E+01 3.0918480940E+01 4.3676701490E+01 1.8399474119E+02 1.7568034306E+02 0. 9. 24 2 3 0 0 0 2.3686034966E+01 -3.1285621318E+01 -1.8359766575E+01 8.7328705038E+01 7.5824820087E+01 0. 9. 5 1 3 0 101 0 -1.2422148837E+01 3.6714037733E-01 1.1228064522E+02 1.1306824428E+02 4.8000000000E+00 0. 9. -24 2 4 0 0 0 -9.7678187022E+00 -2.6477734534E+00 9.3092581616E+01 1.2404558890E+02 8.1355137433E+01 0. 9. -5 1 4 0 0 102 -1.4960674270E+00 3.3566254394E+01 -4.9415880126E+01 5.9949152291E+01 4.8000000000E+00 0. 9. -1 1 5 0 0 103 3.7923403358E+01 -4.2796342204E+01 5.2809339439E+00 5.7425678852E+01 3.3000000000E-01 0. 9. 2 1 5 0 103 0 -1.4237368392E+01 1.1510720887E+01 -2.3640700519E+01 2.9903026186E+01 3.3000000000E-01 0. 9. 13 1 7 0 0 0 -1.8752289513E+01 2.6628018535E+01 7.8954453617E+00 3.3511922573E+01 1.0566000000E-01 0. 9. -14 1 7 0 0 0 8.9844708106E+00 -2.9275791988E+01 8.5197136254E+01 9.0533666325E+01 0.0000000000E+00 0. 9. #pdf 2 -2 2.6632105645E-01 1.2591536243E-01 1.7788228746E+02 3.8308755338E-01 5.4288594974E-01 12 81 1.000000E+00 1.900883E+02 7.827990E-03 1.141802E-01 2 -1 0 0 101 0 0.0000000000E+00 0.0000000000E+00 2.5577458420E+02 2.5577458420E+02 0.0000000000E+00 0. 9. -2 -1 0 0 0 102 0.0000000000E+00 0.0000000000E+00 -3.7117852951E+02 3.7117852951E+02 0.0000000000E+00 0. 9. 6 2 1 2 101 0 -2.9845004492E+00 -6.9372751383E+01 -3.0431396972E+02 3.5834295286E+02 1.7601475455E+02 0. 9. -6 2 1 2 0 102 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pythia8-8.1.80.orig/examples/main07.cmnd0000644000175000017500000000371512217346163016120 0ustar sunsun! main07.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! 1) Settings used in the main program. Main:numberOfEvents = 1000 ! number of events to generate Main:timesAllowErrors = 5 ! allow a few failures before quitting ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showChangedParticleData = on ! list changed particle data Next:numberCount = 100 ! print message every n events Next:numberShowInfo = 1 ! print event information n times Next:numberShowProcess = 1 ! print process record n times Next:numberShowEvent = 1 ! print event record n times ! 3) Beam parameter settings. Incoming beams do not radiate. Beams:idA = -11 ! ficititious incoming e+ Beams:idB = 11 ! ficititious incoming e- PDF:lepton = off ! no radiation off ficititious e+e- Beams:eCM = 500. ! CM energy of collision ! 4) Set up properties of the GeneralResonance and its decay channels. ! id:all = name antiName spinType chargeType colType m0 mWidth mMin mMax tau0 999999:all = GeneralResonance void 1 0 0 500. 1. 0. 0. 0. ! id:addChannel = onMode bRatio meMode product1 product2 ... ! Note: sum of branching ratios automatically rescaled to 1. ! Current channels illustrative only; insert your own decay list. 999999:addChannel = 1 0.2 101 1 -1 ! -> d dbar 999999:addChannel = 1 0.2 101 6 -6 ! -> t tbar 999999:addChannel = 1 0.2 101 15 -15 ! -> tau- tau+ 999999:addChannel = 1 0.2 101 24 -24 ! -> W+ W- 999999:addChannel = 1 0.2 101 25 25 ! -> h0 h0 ! 5) Tell that also long-lived should decay. 13:mayDecay = true ! mu+- 211:mayDecay = true ! pi+- 321:mayDecay = true ! K+- 130:mayDecay = true ! K0_L 2112:mayDecay = true ! n pythia8-8.1.80.orig/examples/main81.cmnd0000644000175000017500000000130312217346167016115 0ustar sunsun! main81.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. // specify statistics parameters Main:numberOfEvents = 100 // number of events generated // specify shower options HadronLevel:all = off PartonLevel:MPI = off SpaceShower:MEafterFirst = off TimeShower:MEafterFirst = off Merging:doKTMerging = on Merging:ktType = 2 Merging:Process = pp>e+ve Merging:TMS = 30. Merging:nJetMax = 2 Tune:pp = 5 SpaceShower:rapidityOrder = off // specify PDF set PDF:useLHAPDF = on PDF:LHAPDFset = cteq6ll.LHpdf pythia8-8.1.80.orig/examples/main31.cmnd0000644000175000017500000000613512217346165016116 0ustar sunsun! main31.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! Names are case-insensitive - but spellings-sensitive! ! The settings here are illustrative, not always physics-motivated. ! You should carefully consider what changes need be done for the ! process you study currently, and consider some of the options ! as reasonable measures of uncertainties in the matching process. ! Number of events - use 0 for all LHEF events in the input file. Main:numberOfEvents = 0 ! Number of events to list and number of errors to allow. Next:numberShowLHA = 1 Next:numberShowInfo = 1 Next:numberShowProcess = 1 Next:numberShowEvent = 1 Main:timesAllowErrors = 10 ! List changed settings or particle data. Init:showChangedSettings = on Init:showChangedParticleData = off ! Input file. Beams:frameType = 4 ! t tbar pair production. #Beams:LHEF = powheg-hvq.lhe ! QCD 2- and 3-jet events. Beams:LHEF = powheg-dijets.lhe ! Number of outgoing particles of POWHEG Born level process ! (i.e. not counting additional POWHEG radiation) POWHEG:nFinal = 2 ! How vetoing is performed: ! 0 - No vetoing is performed (userhooks are not loaded) ! 1 - Showers are started at the kinematical limit. ! Emissions are vetoed if pTemt > pThard. ! See also POWHEG:vetoCount below POWHEG:veto = 1 ! After 'vetoCount' accepted emissions in a row, no more emissions ! are checked. 'vetoCount = 0' means all emissions are checked. POWHEG:vetoCount = 3 ! Selection of pThard (note, for events where there is no ! radiation, pThard is always set to be SCALUP): ! 0 - pThard = SCALUP (of the LHA/LHEF standard) ! 1 - the pT of the POWHEG emission is tested against all other ! incoming and outgoing partons, with the minimal value chosen ! 2 - the pT of all final-state partons is tested against all other ! incoming and outgoing partons, with the minimal value chosen POWHEG:pThard = 2 ! Selection of pTemt: ! 0 - pTemt is pT of the emitted parton w.r.t. radiating parton ! 1 - pT of the emission is checked against all incoming and outgoing ! partons. pTemt is set to the minimum of these values ! 2 - the pT of all final-state partons is tested against all other ! incoming and outgoing partons, with the minimal value chosen ! WARNING: the choice here can give significant variations in the final ! distributions, notably in the tail to large pT values. POWHEG:pTemt = 0 ! Selection of emitted parton for FSR ! 0 - Pythia definition of emitted ! 1 - Pythia definition of radiator ! 2 - Random selection of emitted or radiator ! 3 - Both are emitted and radiator are tried POWHEG:emitted = 0 ! pT definitions ! 0 - POWHEG ISR pT definition is used for both ISR and FSR ! 1 - POWHEG ISR pT and FSR d_ij definitions ! 2 - Pythia definitions POWHEG:pTdef = 1 ! MPI vetoing ! 0 - No MPI vetoing is done ! 1 - When there is no radiation, MPIs with a scale above pT_1 are vetoed, ! else MPIs with a scale above (pT_1 + pT_2 + pT_3) / 2 are vetoed POWHEG:MPIveto = 0 ! Further options (optional, for tryout) !PartonLevel:MPI = off !HadronLevel:All = off pythia8-8.1.80.orig/examples/w_production_powheg_1.lhe0000644000175000017500000067534412217346210021167 0ustar sunsun 2212 2212 3.50000E+03 3.50000E+03 -1 -1 -1 -1 3 1 7.01866E+03 2.61866E+01 1.00000E+00 666 7 666 1.00000E+00 2.44640E+00 -1.00000E+00 3.26456E-01 -1 -1 0 0 0 502 0.000000000E+00 0.000000000E+00 6.223165355E+01 6.223165355E+01 0.000000000E+00 0.00000E+00 9.000E+00 2 -1 0 0 501 0 0.000000000E+00 0.000000000E+00 -3.250432853E+01 3.250432853E+01 0.000000000E+00 0.00000E+00 9.000E+00 24 2 1 2 0 0 3.470977685E+00 -6.183760623E+00 3.129024099E+01 8.696813904E+01 8.083372715E+01 0.00000E+00 9.000E+00 -11 1 3 3 0 0 2.749826076E+01 2.502736253E+01 8.566554374E-01 3.719216421E+01 5.109989100E-04 0.00000E+00 9.000E+00 12 1 3 3 0 0 -2.402728307E+01 -3.121112315E+01 3.043358556E+01 4.977597483E+01 1.066240300E-06 0.00000E+00 9.000E+00 21 1 1 2 512 502 -1.277084208E+00 3.126176245E+00 -2.084678738E+00 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2.027906047E+02 7.742150037E+01 0.00000E+00 9.000E+00 11 1 3 3 0 0 -2.257961136E+01 -1.359749499E+01 -1.610562000E+02 1.631987447E+02 5.109989100E-04 0.00000E+00 9.000E+00 -12 1 3 3 0 0 2.876245439E+01 7.439599766E+00 -2.617038315E+01 3.959186005E+01 4.768371582E-07 0.00000E+00 9.000E+00 21 1 1 2 501 502 -8.206300890E+00 3.159219300E+00 -3.324853699E+01 3.439170326E+01 4.768371582E-07 0.00000E+00 9.000E+00 2 1 1 2 512 0 2.023457858E+00 2.998675926E+00 1.773058443E+01 1.809585763E+01 0.000000000E+00 0.00000E+00 9.000E+00 7 666 1.00000E+00 6.31139E+00 -1.00000E+00 2.22036E-01 -2 -1 0 0 0 502 0.000000000E+00 0.000000000E+00 1.590847496E+02 1.590847496E+02 0.000000000E+00 0.00000E+00 9.000E+00 21 -1 0 0 512 501 0.000000000E+00 0.000000000E+00 -4.182234709E+01 4.182234709E+01 0.000000000E+00 0.00000E+00 9.000E+00 -24 2 1 2 0 0 -4.305028124E+00 -2.962282634E+00 1.463171238E+02 1.666830296E+02 7.966946264E+01 0.00000E+00 9.000E+00 11 1 3 3 0 0 3.142870612E+01 9.553005008E+00 3.046568375E+01 4.480157764E+01 5.109989100E-04 0.00000E+00 9.000E+00 -12 1 3 3 0 0 -3.573373424E+01 -1.251528764E+01 1.158514400E+02 1.218814520E+02 1.348699152E-06 0.00000E+00 9.000E+00 -1 1 1 2 0 501 8.411417496E+00 -1.830551116E+00 -6.455107274E+00 1.075970593E+01 0.000000000E+00 0.00000E+00 9.000E+00 21 1 1 2 512 502 -4.106389372E+00 4.792833749E+00 -2.259961401E+01 2.346436111E+01 5.331201500E-07 0.00000E+00 9.000E+00 pythia8-8.1.80.orig/examples/main41.cc0000644000175000017500000000424412217346166015563 0ustar sunsun// main41.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Author: Mikhail Kirsanov, Mikhail.Kirsanov@cern.ch, based on main01.cc. // This program illustrates how HepMC can be interfaced to Pythia8. // It studies the charged multiplicity distribution at the LHC. // HepMC events are output to the hepmcout41.dat file. // WARNING: typically one needs 25 MB/100 events at the LHC. // Therefore large event samples may be impractical. #include "Pythia8/Pythia.h" #include "Pythia8/Pythia8ToHepMC.h" #include "HepMC/GenEvent.h" #include "HepMC/IO_GenEvent.h" using namespace Pythia8; int main() { // Interface for conversion from Pythia8::Event to HepMC event. HepMC::Pythia8ToHepMC ToHepMC; // Specify file where HepMC events will be stored. HepMC::IO_GenEvent ascii_io("hepmcout41.dat", std::ios::out); // Generator. Process selection. LHC initialization. Histogram. Pythia pythia; pythia.readString("Beams:eCM = 8000."); pythia.readString("HardQCD:all = on"); pythia.readString("PhaseSpace:pTHatMin = 20."); pythia.init(); Hist mult("charged multiplicity", 100, -0.5, 799.5); // Begin event loop. Generate event. Skip if error. for (int iEvent = 0; iEvent < 100; ++iEvent) { if (!pythia.next()) continue; // Find number of all final charged particles and fill histogram. int nCharged = 0; for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].isFinal() && pythia.event[i].isCharged()) ++nCharged; mult.fill( nCharged ); // Construct new empty HepMC event and fill it. // Units will be as chosen for HepMC build; but can be changed // by arguments, e.g. GenEvt( HepMC::Units::GEV, HepMC::Units::MM) HepMC::GenEvent* hepmcevt = new HepMC::GenEvent(); ToHepMC.fill_next_event( pythia, hepmcevt ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; // End of event loop. Statistics. Histogram. } pythia.stat(); cout << mult; // Done. return 0; } pythia8-8.1.80.orig/examples/outref/0000755000175000017500000000000012217360175015457 5ustar sunsunpythia8-8.1.80.orig/examples/outref/out220000644000175000017500000104171212217346174016366 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:06:41 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | q qbar -> Theta 621 | 3.798e-07 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 57.54 mb | | | | pT0 = 3.08 gives sigmaInteraction = 270.41 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Check:nErrList | 2 | 0 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products 663 Theta 3 0 0 342.00000 3.35160 300.00000 400.00000 0.00000e+00 1 1 0 1 0 0 1 0.0306122 0 1 -1 1 1 0.0306122 0 2 -2 2 1 0.0306122 0 3 -3 3 1 0.0306122 0 4 -4 4 1 0.0306122 0 5 -5 5 1 0.0102041 0 11 -11 6 1 0.0102041 0 13 -13 7 1 0.0102041 0 15 -15 8 1 0.8163265 0 21 21 21 -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. In 1: id = 1, x = 2.179e-02, pdf = 5.162e-01 at Q2 = 1.178e+05. In 2: id = -1, x = 2.757e-02, pdf = 3.031e-01 at same Q2. Subprocess q qbar -> Theta with code 621 is 2 -> 1. It has sHat = 1.178e+05. alphaEM = 7.937e-03, alphaS = 1.117e-01 at Q2 = 1.178e+05. Impact parameter b = 4.179e-01 gives enhancement factor = 2.668e+00. Max pT scale for MPI = 1.400e+04, ISR = 1.400e+04, FSR = 1.400e+04. Number of MPI = 8, ISR = 18, FSRproc = 121, FSRreson = 47. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 1 (d) -21 1 0 5 0 101 0 0.000 0.000 152.515 152.515 0.000 4 -1 (dbar) -21 2 0 5 0 0 101 0.000 0.000 -193.021 193.021 0.000 5 663 (Theta) -22 3 4 6 8 0 0 0.000 0.000 -40.506 345.536 343.154 6 21 g 23 5 0 0 0 102 104 57.112 26.044 -101.513 119.352 0.000 7 21 g 23 5 0 0 0 103 102 14.750 -2.106 -71.781 73.311 0.000 8 21 g 23 5 0 0 0 104 103 -71.862 -23.938 132.789 152.872 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 -40.506 345.536 343.154 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 526 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 527 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 1 (d) -21 6 0 5 0 101 0 0.000 0.000 152.515 152.515 0.000 4 -1 (dbar) -21 7 7 5 0 0 101 0.000 0.000 -193.021 193.021 0.000 5 663 (Theta) -22 3 4 8 8 0 0 0.000 0.000 -40.506 345.536 343.154 6 1 (d) -41 19 0 9 3 105 0 -0.000 0.000 164.209 164.209 0.000 7 -1 (dbar) -42 20 20 4 4 0 101 0.000 -0.000 -193.021 193.021 0.000 8 663 (Theta) -44 5 5 21 21 0 0 6.836 -9.129 -33.342 344.958 343.154 9 21 (g) -43 6 0 22 22 105 101 -6.836 9.129 4.529 12.271 0.000 10 4 (c) -31 14 14 12 13 106 0 0.000 0.000 17.276 17.276 0.000 11 21 (g) -31 15 0 12 13 107 106 0.000 0.000 -16.534 16.534 0.000 12 4 (c) -33 10 11 16 16 108 0 2.832 -9.721 13.865 17.234 1.500 13 21 (g) -33 10 11 17 17 107 108 -2.832 9.721 -13.123 16.575 0.000 14 4 (c) -42 24 24 10 10 106 0 0.000 -0.000 17.276 17.276 0.000 15 21 (g) -41 25 0 18 11 109 106 -0.000 0.000 -1605.149 1605.149 0.000 16 4 (c) -44 12 12 26 26 108 0 3.013 -10.600 15.378 18.978 1.500 17 21 (g) -44 13 13 27 27 107 108 -1.234 1.975 -15.783 15.954 0.000 18 21 (g) -43 15 0 28 28 109 107 -1.778 8.625 -1587.468 1587.493 0.000 19 21 (g) -41 66 66 23 6 105 110 0.000 0.000 189.412 189.412 0.000 20 -1 (dbar) -42 65 65 7 7 0 101 -0.000 -0.000 -193.021 193.021 0.000 21 663 (Theta) -44 8 8 68 68 0 0 -0.672 -10.140 -31.962 344.789 343.154 22 21 (g) -44 9 9 63 64 105 101 -7.240 9.075 4.437 12.428 0.000 23 -1 (dbar) -43 19 0 70 70 0 110 7.912 1.065 23.916 25.216 0.330 24 4 (c) -42 102 0 14 14 106 0 0.000 -0.000 17.276 17.276 0.000 25 21 (g) -41 103 103 29 15 109 111 -0.000 0.000 -3189.214 3189.214 0.000 26 4 (c) -44 16 16 104 104 108 0 3.006 -10.599 15.356 18.959 1.500 27 21 (g) -44 17 17 62 62 107 108 -1.297 1.981 -15.792 15.968 0.000 28 21 (g) -44 18 18 60 61 109 107 -8.026 9.208 -1588.618 1588.665 0.000 29 21 (g) -43 25 0 107 107 106 111 6.317 -0.590 -1582.885 1582.898 0.000 30 21 (g) -31 34 0 32 33 113 114 0.000 0.000 0.474 0.474 0.000 31 2 (u) -31 35 35 32 33 112 0 0.000 0.000 -153.690 153.690 0.000 32 21 (g) -33 30 31 36 36 112 114 -2.131 4.642 -14.871 15.724 0.000 33 2 (u) -33 30 31 37 37 113 0 2.131 -4.642 -138.345 138.440 0.330 34 21 (g) -41 39 0 38 30 113 115 -0.000 -0.000 1.535 1.535 0.000 35 2 (u) -42 40 40 31 31 112 0 -0.000 -0.000 -153.690 153.690 0.000 36 21 (g) -44 32 32 41 41 112 114 1.817 6.494 -23.254 24.212 0.000 37 2 (u) -44 33 33 42 42 113 0 2.569 -4.437 -124.051 124.157 0.330 38 21 (g) -43 34 0 43 43 114 115 -4.386 -2.057 -4.851 6.856 0.000 39 21 (g) -41 45 0 44 34 116 115 0.000 0.000 2.880 2.880 0.000 40 2 (u) -42 46 46 35 35 112 0 0.000 0.000 -153.690 153.690 0.000 41 21 (g) -44 36 36 47 47 112 114 0.353 6.240 -18.821 19.831 0.000 42 2 (u) -44 37 37 48 48 113 0 2.407 -4.465 -115.108 115.220 0.330 43 21 (g) -44 38 38 49 49 114 115 -7.451 -2.589 -13.651 15.766 0.000 44 21 (g) -43 39 0 50 50 116 113 4.691 0.814 -3.230 5.753 0.000 45 21 (g) -41 89 89 51 39 117 115 -0.000 -0.000 1088.890 1088.890 0.000 46 2 (u) -42 584 584 40 40 112 0 0.000 0.000 -153.690 153.690 0.000 47 21 (g) -44 41 41 128 129 112 114 -0.498 6.133 -17.971 18.995 0.000 48 2 (u) -44 42 42 176 176 113 0 2.312 -4.477 -112.076 112.190 0.330 49 21 (g) -44 43 43 87 88 114 115 -9.231 -2.812 -20.650 22.794 0.000 50 21 (g) -44 44 44 80 80 116 113 2.567 0.547 -0.068 2.625 0.000 51 21 (g) -43 45 0 78 79 117 116 4.850 0.609 1085.965 1085.976 0.000 52 21 (g) -31 73 0 54 55 118 119 0.000 0.000 7.521 7.521 0.000 53 21 (g) -31 74 74 54 55 120 121 0.000 0.000 -152.496 152.496 0.000 54 21 (g) -33 52 53 75 75 118 121 3.986 1.359 6.900 8.084 0.000 55 21 (g) -33 52 53 76 76 120 119 -3.986 -1.359 -151.875 151.933 0.000 56 21 (g) -31 110 0 58 59 123 124 0.000 0.000 1.420 1.420 0.000 57 1 (d) -31 111 111 58 59 122 0 0.000 0.000 -1187.938 1187.938 0.000 58 21 (g) -33 56 57 112 112 122 124 3.365 -0.764 -0.682 3.517 0.000 59 1 (d) -33 56 57 113 113 123 0 -3.365 0.764 -1185.836 1185.841 0.330 60 21 (g) -51 28 0 106 106 109 125 -5.619 5.626 -591.217 591.271 0.000 61 21 (g) -51 28 0 108 108 125 107 -2.531 3.771 -998.906 998.916 0.000 62 21 (g) -52 27 27 105 105 107 108 -1.173 1.792 -14.286 14.446 0.000 63 21 (g) -51 22 0 69 69 105 126 -5.955 4.474 5.097 9.025 0.000 64 21 (g) -51 22 0 71 71 126 101 -1.286 4.601 -2.788 5.531 0.000 65 -1 (dbar) -53 67 0 20 20 0 101 0.000 -0.000 -195.149 195.149 0.000 66 21 (g) -42 94 0 19 19 105 110 -0.000 0.000 189.412 189.412 0.000 67 -1 (dbar) -41 95 95 72 65 0 127 0.000 -0.000 -201.927 201.927 0.000 68 663 (Theta) -44 21 21 96 96 0 0 -0.678 -7.268 -32.678 344.783 343.154 69 21 (g) -44 63 63 97 97 105 126 -5.955 4.504 5.114 9.050 0.000 70 -1 (dbar) -44 23 23 98 98 0 110 7.912 1.075 23.877 25.179 0.330 71 21 (g) -44 64 64 99 99 126 101 -1.286 4.664 -2.763 5.572 0.000 72 21 (g) -43 67 0 100 100 101 127 0.006 -2.975 -6.065 6.756 0.000 73 21 (g) -41 81 81 77 52 128 119 -0.000 -0.000 13.560 13.560 0.000 74 21 (g) -42 82 0 53 53 120 121 0.000 0.000 -152.496 152.496 0.000 75 21 (g) -44 54 54 83 83 118 121 1.579 -0.493 7.436 7.617 0.000 76 21 (g) -44 55 55 84 84 120 119 -3.996 -1.366 -151.988 152.047 0.000 77 21 (g) -43 73 0 85 85 128 118 2.417 1.859 5.617 6.391 0.000 78 21 (g) -51 51 0 179 179 117 129 3.957 2.447 1059.150 1059.160 0.000 79 21 (g) -51 51 0 131 132 129 116 0.967 -1.822 26.813 26.893 0.000 80 21 (g) -52 50 50 133 133 116 113 2.492 0.531 -0.066 2.549 0.000 81 21 (g) -42 121 0 73 73 128 119 -0.000 -0.000 13.560 13.560 0.000 82 -2 (ubar) -41 122 122 86 74 0 121 0.000 0.000 -426.914 426.914 0.000 83 21 (g) -44 75 75 123 123 118 121 1.581 -0.493 7.438 7.620 0.000 84 21 (g) -44 76 76 124 124 120 119 -1.355 -0.845 -152.223 152.231 0.000 85 21 (g) -44 77 77 125 125 128 118 2.423 1.861 5.633 6.408 0.000 86 -2 (ubar) -43 82 0 126 126 0 120 -2.649 -0.522 -274.201 274.215 0.330 87 21 (g) -51 49 0 130 130 114 130 -9.159 -4.958 -18.595 21.313 0.000 88 21 (g) -51 49 0 118 119 130 115 -0.073 2.145 -1.116 2.420 0.000 89 21 (g) -53 120 120 45 45 117 115 -0.000 -0.000 1089.829 1089.829 0.000 90 21 (g) -31 193 193 92 93 131 132 0.000 0.000 9.911 9.911 0.000 91 21 (g) -31 186 186 92 93 133 134 0.000 0.000 -258.665 258.665 0.000 92 21 (g) -33 90 91 195 195 131 134 0.919 2.253 -258.510 258.521 0.000 93 21 (g) -33 90 91 184 185 133 132 -0.919 -2.253 9.756 10.055 0.000 94 21 (g) -41 211 0 101 66 105 135 0.000 -0.000 255.156 255.156 0.000 95 -1 (dbar) -42 212 212 67 67 0 127 0.000 0.000 -201.927 201.927 0.000 96 663 (Theta) -44 68 68 213 213 0 0 -0.997 -9.230 -32.680 344.831 343.154 97 21 (g) -44 69 69 214 214 105 126 -5.969 4.415 5.138 9.029 0.000 98 -1 (dbar) -44 70 70 161 162 0 110 7.862 0.767 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-73 631 668 941 941 241 115 -0.379 -0.005 18.563 18.568 0.189 894 21 (g) -73 536 549 896 0 151 221 0.591 0.273 5.781 5.817 0.035 895 -1 (dbar) -73 530 535 1230 1230 0 209 3.983 -0.351 9.503 10.317 0.374 896 21 (g) -73 555 894 1227 1227 151 246 2.110 0.664 15.372 15.535 0.421 897 21 (g) -73 545 551 1228 1228 234 151 -0.019 0.082 1.340 1.444 0.530 898 21 (g) -73 808 809 957 957 303 308 4.168 0.666 -2.141 4.735 0.165 899 21 (g) -73 829 830 954 954 314 276 2.941 -0.375 -3.222 4.402 0.458 900 -1 (dbar) -73 793 794 958 958 0 303 -0.519 -0.681 -4.233 4.396 0.822 901 -2 (ubar) -73 805 825 911 911 0 277 1.508 0.563 -13.382 13.489 0.542 902 21 (g) -73 844 845 1030 1030 319 281 -14.587 -3.081 22.489 26.982 0.140 903 21 (g) -73 790 791 1029 1029 281 302 -5.313 -1.296 7.771 9.507 0.299 904 21 (g) -73 820 821 1024 1024 293 312 0.631 -3.614 4.758 6.017 0.314 905 21 (g) -73 841 842 1015 1015 318 287 1.507 -0.895 -1.095 2.098 0.366 906 21 (g) -73 799 800 1033 1033 305 284 -6.508 -0.422 6.459 9.187 0.386 907 21 (g) -73 817 818 1026 1026 274 311 -0.013 0.203 0.634 0.785 0.415 908 21 (g) -73 835 836 1012 1012 316 292 1.334 -0.508 -1.952 2.459 0.446 909 21 (g) -73 823 824 1018 1018 313 310 -5.333 1.143 9.944 11.352 0.494 910 1 (d) -71 806 806 912 913 277 0 4.485 0.152 -29.120 29.465 0.330 911 -2 (ubar) -71 901 901 912 913 0 277 1.508 0.563 -13.382 13.489 0.542 912 111 (pi0) -82 910 911 1541 1542 0 0 5.805 0.768 -38.220 38.666 0.135 913 -211 pi- 82 910 911 0 0 0 0 0.188 -0.053 -4.282 4.289 0.140 914 2 (u) -71 698 698 916 918 136 0 0.052 -0.106 13.161 13.166 0.330 915 -4 (cbar) -71 565 565 916 918 0 136 -1.754 0.281 4.056 4.675 1.500 916 321 K+ 83 914 915 0 0 0 0 -0.049 -0.122 9.675 9.689 0.494 917 -321 K- 84 914 915 0 0 0 0 -0.408 0.317 1.400 1.572 0.494 918 -423 (D*bar0) -84 914 915 1543 1544 0 0 -1.244 -0.019 6.142 6.580 2.007 919 1 (d) -71 889 889 925 930 190 0 1.422 1.837 4.497 5.083 0.462 920 21 (g) -71 891 891 925 930 264 190 -0.691 0.992 2.631 2.946 0.543 921 21 (g) -71 887 887 925 930 188 264 -1.026 0.890 0.859 1.610 0.099 922 21 (g) -71 615 615 925 930 216 188 0.143 0.124 -0.166 0.252 0.000 923 21 (g) -71 890 890 925 930 139 216 0.188 1.507 1.661 2.261 0.218 924 -3 (sbar) -71 595 595 925 930 0 139 -1.106 1.912 1.080 2.509 0.500 925 -211 pi- 83 919 924 0 0 0 0 0.204 0.044 0.389 0.463 0.140 926 323 (K*+) -83 919 924 1347 1348 0 0 0.615 2.594 5.914 6.543 0.856 927 -311 (Kbar0) -83 919 924 1349 1349 0 0 -0.419 0.380 -0.042 0.755 0.498 928 2112 n0 83 919 924 0 0 0 0 0.027 0.646 1.524 1.903 0.940 929 -2212 pbar- 84 919 924 0 0 0 0 -0.950 2.203 1.751 3.115 0.938 930 321 K+ 84 919 924 0 0 0 0 -0.547 1.395 1.026 1.881 0.494 931 2 (u) -71 853 853 933 939 109 0 -4.070 3.421 -472.237 472.268 0.794 932 2203 (uu_1) -71 700 700 933 939 0 109 0.511 -0.728 -1130.819 1130.820 0.771 933 111 (pi0) -83 931 932 1545 1546 0 0 -1.186 1.118 -134.394 134.404 0.135 934 2212 p+ 83 931 932 0 0 0 0 -0.602 0.638 -210.988 210.992 0.938 935 111 (pi0) -83 931 932 1547 1548 0 0 -1.108 0.488 -146.907 146.912 0.135 936 -2212 pbar- 83 931 932 0 0 0 0 -0.750 0.361 -88.626 88.635 0.938 937 113 (rho0) -84 931 932 1350 1351 0 0 0.046 0.133 -134.182 134.184 0.700 938 2212 p+ 84 931 932 0 0 0 0 -0.162 0.470 -632.198 632.199 0.938 939 211 pi+ 84 931 932 0 0 0 0 0.203 -0.515 -255.762 255.763 0.140 940 2 (u) -71 699 699 944 951 115 0 -0.261 0.767 393.834 393.835 0.330 941 21 (g) -71 893 893 944 951 241 115 -0.379 -0.005 18.563 18.568 0.189 942 21 (g) -71 638 638 944 951 225 241 -0.020 0.657 4.719 4.764 0.000 943 -1 (dbar) -71 892 892 944 951 0 225 1.614 1.597 7.980 8.304 0.354 944 111 (pi0) -83 940 943 1549 1550 0 0 -0.026 0.241 80.449 80.450 0.135 945 211 pi+ 83 940 943 0 0 0 0 0.136 0.251 194.944 194.945 0.140 946 313 (K*0) -83 940 943 1352 1353 0 0 -0.325 0.375 111.831 111.836 0.949 947 -311 (Kbar0) -84 940 943 1354 1354 0 0 -0.355 0.349 19.287 19.300 0.498 948 313 (K*0) -84 940 943 1355 1356 0 0 0.193 0.172 5.266 5.344 0.874 949 -321 K- 84 940 943 0 0 0 0 0.295 0.232 4.686 4.727 0.494 950 111 (pi0) -84 940 943 1551 1552 0 0 -0.007 0.079 1.208 1.218 0.135 951 213 (rho+) -84 940 943 1357 1358 0 0 1.042 1.318 7.423 7.651 0.781 952 3 (s) -71 780 780 959 970 299 0 46.222 -13.751 -45.413 66.243 0.500 953 21 (g) -71 788 788 959 970 276 299 10.322 -2.601 -9.620 14.348 0.000 954 21 (g) -71 899 899 959 970 314 276 2.941 -0.375 -3.222 4.402 0.458 955 21 (g) -71 828 828 959 970 295 314 2.245 0.325 -1.759 2.871 0.000 956 21 (g) -71 807 807 959 970 308 295 4.113 -0.456 -2.570 4.871 0.000 957 21 (g) -71 898 898 959 970 303 308 4.168 0.666 -2.141 4.735 0.165 958 -1 (dbar) -71 900 900 959 970 0 303 -0.519 -0.681 -4.233 4.396 0.822 959 -313 (K*bar0) -83 952 958 1359 1360 0 0 12.348 -2.842 -11.931 17.424 0.855 960 -213 (rho-) -83 952 958 1361 1362 0 0 20.603 -6.627 -20.368 29.727 0.678 961 2212 p+ 83 952 958 0 0 0 0 14.704 -3.735 -14.489 21.000 0.938 962 -2212 pbar- 83 952 958 0 0 0 0 8.524 -2.223 -7.629 11.691 0.938 963 211 pi+ 83 952 958 0 0 0 0 1.163 -0.396 -1.596 2.019 0.140 964 -213 (rho-) -83 952 958 1363 1364 0 0 5.822 -0.683 -4.631 7.517 0.842 965 211 pi+ 83 952 958 0 0 0 0 0.756 -0.052 -0.169 0.789 0.140 966 -211 pi- 83 952 958 0 0 0 0 5.151 -0.094 -4.147 6.615 0.140 967 111 (pi0) -84 952 958 1553 1554 0 0 0.041 0.277 -0.211 0.376 0.135 968 2212 p+ 84 952 958 0 0 0 0 0.230 -0.042 -1.202 1.543 0.938 969 -2112 nbar0 84 952 958 0 0 0 0 0.058 -0.274 -1.840 2.085 0.940 970 223 (omega) -84 952 958 1555 1557 0 0 0.094 -0.179 -0.744 1.081 0.758 971 3 (s) -71 878 878 989 1009 122 0 1.906 -1.022 -0.185 2.338 0.869 972 21 (g) -71 871 871 989 1009 197 122 1.723 -3.524 -1.039 4.061 0.162 973 21 (g) -71 877 877 989 1009 208 197 0.027 -0.811 0.649 1.112 0.397 974 21 (g) -71 695 695 989 1009 160 208 0.751 -0.925 1.237 1.718 0.000 975 21 (g) -71 614 614 989 1009 257 160 -1.867 -0.203 -4.002 4.421 0.000 976 21 (g) -71 881 881 989 1009 152 257 -1.183 -0.675 -2.572 2.958 0.530 977 21 (g) -71 872 872 989 1009 201 152 -1.922 -0.484 -5.279 5.644 0.235 978 21 (g) -71 605 605 989 1009 237 201 -2.601 -1.807 -3.632 4.818 0.000 979 21 (g) -71 879 879 989 1009 256 237 -1.332 -0.543 -2.586 2.996 0.466 980 21 (g) -71 618 618 989 1009 114 256 -0.149 -0.338 -1.505 1.549 0.000 981 21 (g) -71 876 876 989 1009 228 114 -1.301 0.561 -3.750 4.022 0.334 982 21 (g) -71 620 620 989 1009 255 228 0.074 1.022 -4.901 5.006 0.000 983 21 (g) -71 880 880 989 1009 112 255 0.480 3.879 -8.767 9.613 0.525 984 21 (g) -71 873 873 989 1009 123 112 0.705 1.590 -3.991 4.360 0.243 985 21 (g) -71 874 874 989 1009 220 123 0.668 1.301 -24.304 24.349 0.261 986 21 (g) -71 875 875 989 1009 265 220 1.229 0.167 -50.068 50.084 0.289 987 21 (g) -71 658 658 989 1009 171 265 -0.602 -0.722 -98.156 98.160 0.000 988 -2 (ubar) -71 643 643 989 1009 0 171 -0.821 -1.403 -94.623 94.638 0.330 989 -313 (K*bar0) -83 971 988 1365 1366 0 0 1.357 -1.122 -0.293 2.014 0.931 990 -213 (rho-) -83 971 988 1367 1368 0 0 1.379 -2.268 0.264 2.850 1.003 991 213 (rho+) -83 971 988 1369 1370 0 0 0.445 -0.856 -0.263 1.252 0.754 992 223 (omega) -83 971 988 1558 1560 0 0 0.578 -0.814 0.329 1.303 0.770 993 111 (pi0) -83 971 988 1561 1562 0 0 0.301 -0.428 -0.443 0.699 0.135 994 111 (pi0) -83 971 988 1563 1564 0 0 0.096 -0.709 0.118 0.738 0.135 995 111 (pi0) -83 971 988 1565 1566 0 0 0.045 0.249 0.235 0.371 0.135 996 313 (K*0) -83 971 988 1371 1372 0 0 -0.553 -0.530 -0.605 1.321 0.890 997 -321 K- 83 971 988 0 0 0 0 0.001 -0.051 -1.165 1.266 0.494 998 213 (rho+) -83 971 988 1373 1374 0 0 -2.112 -0.455 -3.636 4.291 0.722 999 1114 (Delta-) -83 971 988 1375 1376 0 0 -5.760 -2.418 -10.976 12.679 1.128 1000 -2114 (Deltabar0) -84 971 988 1377 1378 0 0 -0.860 -0.537 -2.959 3.388 1.303 1001 2114 (Delta0) -84 971 988 1379 1380 0 0 0.059 0.462 -3.244 3.483 1.181 1002 223 (omega) -84 971 988 1567 1569 0 0 -0.394 1.729 -5.872 6.183 0.780 1003 -1114 (Deltabar+) -84 971 988 1381 1382 0 0 0.112 2.321 -6.547 7.042 1.150 1004 -213 (rho-) -84 971 988 1383 1384 0 0 0.005 1.020 -4.702 4.872 0.770 1005 213 (rho+) -84 971 988 1385 1386 0 0 0.401 1.306 -4.692 4.947 0.768 1006 -211 pi- 84 971 988 0 0 0 0 0.626 0.420 -13.239 13.261 0.140 1007 2224 (Delta++) -84 971 988 1387 1388 0 0 0.035 0.298 -18.987 19.042 1.415 1008 223 (omega) -84 971 988 1570 1571 0 0 1.361 0.561 -50.498 50.526 0.782 1009 -2224 (Deltabar--) -84 971 988 1389 1390 0 0 -1.338 -2.117 -180.300 180.322 1.341 1010 2 (u) -71 826 826 1039 1081 300 0 1.268 0.300 -5.556 5.717 0.330 1011 21 (g) -71 827 827 1039 1081 292 300 -0.020 0.247 -4.089 4.096 0.000 1012 21 (g) -71 908 908 1039 1081 316 292 1.334 -0.508 -1.952 2.459 0.446 1013 21 (g) -71 834 834 1039 1081 306 316 2.720 -1.237 -1.400 3.299 0.000 1014 21 (g) -71 801 801 1039 1081 287 306 0.260 -0.297 0.050 0.399 0.000 1015 21 (g) -71 905 905 1039 1081 318 287 1.507 -0.895 -1.095 2.098 0.366 1016 21 (g) -71 840 840 1039 1081 103 318 0.031 -0.634 -0.843 1.056 0.000 1017 21 (g) -71 814 814 1039 1081 310 103 0.019 0.187 0.226 0.294 0.000 1018 21 (g) -71 909 909 1039 1081 313 310 -5.333 1.143 9.944 11.352 0.494 1019 21 (g) -71 839 839 1039 1081 275 313 -2.659 0.400 6.266 6.818 0.000 1020 21 (g) -71 838 838 1039 1081 317 275 -0.336 -0.126 1.242 1.292 0.000 1021 21 (g) -71 837 837 1039 1081 286 317 -2.369 -3.467 5.612 7.009 0.000 1022 21 (g) -71 779 779 1039 1081 280 286 -0.311 -1.447 3.449 3.753 0.000 1023 21 (g) -71 819 819 1039 1081 312 280 -0.225 -2.884 2.786 4.017 0.000 1024 21 (g) -71 904 904 1039 1081 293 312 0.631 -3.614 4.758 6.017 0.314 1025 21 (g) -71 816 816 1039 1081 311 293 -0.131 -1.120 1.088 1.567 0.000 1026 21 (g) -71 907 907 1039 1081 274 311 -0.013 0.203 0.634 0.785 0.415 1027 21 (g) -71 797 797 1039 1081 288 274 -6.731 -2.317 10.189 12.429 0.000 1028 21 (g) -71 789 789 1039 1081 302 288 -8.390 -3.486 14.455 17.074 0.000 1029 21 (g) -71 903 903 1039 1081 281 302 -5.313 -1.296 7.771 9.507 0.299 1030 21 (g) -71 902 902 1039 1081 319 281 -14.587 -3.081 22.489 26.982 0.140 1031 21 (g) -71 843 843 1039 1081 296 319 -7.686 -1.247 12.620 14.829 0.000 1032 21 (g) -71 771 771 1039 1081 284 296 -0.040 -0.209 0.623 0.658 0.000 1033 21 (g) -71 906 906 1039 1081 305 284 -6.508 -0.422 6.459 9.187 0.386 1034 21 (g) -71 831 831 1039 1081 315 305 -1.024 -0.335 1.067 1.516 0.000 1035 21 (g) -71 832 832 1039 1081 104 315 0.107 0.176 -0.186 0.277 0.000 1036 21 (g) -71 833 833 1039 1081 283 104 -5.220 7.319 -2.932 9.456 0.000 1037 21 (g) -71 766 766 1039 1081 294 283 -0.187 0.388 -0.365 0.564 0.000 1038 -3 (sbar) -71 765 765 1039 1081 0 294 -17.845 26.959 -14.568 35.465 0.500 1039 113 (rho0) -83 1010 1038 1391 1392 0 0 0.470 0.222 -3.085 3.215 0.742 1040 211 pi+ 83 1010 1038 0 0 0 0 0.172 -0.079 -1.316 1.337 0.140 1041 -213 (rho-) -83 1010 1038 1393 1394 0 0 1.879 0.083 -4.395 4.840 0.762 1042 321 K+ 83 1010 1038 0 0 0 0 0.016 -0.735 -1.306 1.578 0.494 1043 333 (phi) -83 1010 1038 1572 1573 0 0 0.688 -0.155 -1.335 1.820 1.017 1044 -311 (Kbar0) -83 1010 1038 1395 1395 0 0 1.075 0.081 -0.735 1.397 0.498 1045 -213 (rho-) -83 1010 1038 1396 1397 0 0 1.800 -1.642 -1.873 3.146 0.671 1046 111 (pi0) -83 1010 1038 1574 1575 0 0 1.203 -0.294 -0.043 1.246 0.135 1047 213 (rho+) -83 1010 1038 1398 1399 0 0 -0.940 0.113 0.239 1.266 0.806 1048 223 (omega) -83 1010 1038 1576 1578 0 0 0.080 -0.443 1.902 2.103 0.776 1049 111 (pi0) -83 1010 1038 1579 1580 0 0 -2.410 0.360 2.978 3.850 0.135 1050 -213 (rho-) -83 1010 1038 1400 1401 0 0 -2.299 0.728 6.135 6.649 0.867 1051 221 (eta) -83 1010 1038 1581 1583 0 0 -1.618 -0.081 2.073 2.687 0.548 1052 113 (rho0) -83 1010 1038 1402 1403 0 0 -0.480 -0.248 1.636 1.934 0.878 1053 113 (rho0) -83 1010 1038 1404 1405 0 0 -1.330 -0.753 3.021 3.469 0.757 1054 111 (pi0) -83 1010 1038 1584 1585 0 0 -0.043 -0.019 0.969 0.979 0.135 1055 211 pi+ 83 1010 1038 0 0 0 0 -0.918 -1.997 3.534 4.164 0.140 1056 111 (pi0) -83 1010 1038 1586 1587 0 0 -0.717 -0.446 0.696 1.103 0.135 1057 111 (pi0) -83 1010 1038 1588 1589 0 0 -0.456 -2.566 4.237 4.976 0.135 1058 311 (K0) -83 1010 1038 1406 1406 0 0 0.049 -1.777 2.242 2.904 0.498 1059 3214 (Sigma*0) -83 1010 1038 1407 1408 0 0 0.281 -3.867 5.126 6.570 1.365 1060 -2114 (Deltabar0) -83 1010 1038 1409 1410 0 0 -3.790 -1.083 5.565 6.930 1.233 1061 223 (omega) -84 1010 1038 1590 1592 0 0 -1.289 -0.841 2.787 3.278 0.782 1062 2112 n0 84 1010 1038 0 0 0 0 -4.859 -1.619 7.203 8.889 0.940 1063 -2212 pbar- 84 1010 1038 0 0 0 0 -4.625 -1.070 7.481 8.909 0.938 1064 323 (K*+) -84 1010 1038 1411 1412 0 0 -11.041 -3.602 18.563 21.915 0.882 1065 -311 (Kbar0) -84 1010 1038 1413 1413 0 0 -4.892 -0.956 6.863 8.497 0.498 1066 -211 pi- 84 1010 1038 0 0 0 0 -1.003 -0.143 1.901 2.158 0.140 1067 213 (rho+) -84 1010 1038 1414 1415 0 0 -5.560 -1.499 8.393 10.203 0.710 1068 -213 (rho-) -84 1010 1038 1416 1417 0 0 -5.194 -0.751 7.461 9.154 0.771 1069 111 (pi0) -84 1010 1038 1593 1594 0 0 -2.195 -0.081 3.187 3.873 0.135 1070 111 (pi0) -84 1010 1038 1595 1596 0 0 -0.457 -0.139 0.816 0.955 0.135 1071 213 (rho+) -84 1010 1038 1418 1419 0 0 -3.347 -0.747 3.401 4.892 0.779 1072 -211 pi- 84 1010 1038 0 0 0 0 -0.020 -0.118 0.366 0.409 0.140 1073 211 pi+ 84 1010 1038 0 0 0 0 -0.203 0.490 0.300 0.625 0.140 1074 -213 (rho-) -84 1010 1038 1420 1421 0 0 -1.258 0.037 0.683 1.634 0.786 1075 113 (rho0) -84 1010 1038 1422 1423 0 0 -1.145 0.860 -0.204 1.714 0.920 1076 211 pi+ 84 1010 1038 0 0 0 0 -0.288 0.997 0.294 1.087 0.140 1077 -213 (rho-) -84 1010 1038 1424 1425 0 0 -1.884 1.445 -0.738 2.757 1.192 1078 223 (omega) -84 1010 1038 1597 1599 0 0 -1.424 3.043 -1.441 3.738 0.780 1079 211 pi+ 84 1010 1038 0 0 0 0 -0.361 0.694 -0.146 0.808 0.140 1080 313 (K*0) -84 1010 1038 1426 1427 0 0 -3.115 4.007 -2.092 5.561 0.890 1081 333 (phi) -84 1010 1038 1600 1601 0 0 -15.602 23.292 -12.597 30.751 1.021 1082 2 (u) -71 697 697 1084 1095 154 0 -0.680 0.447 1214.323 1214.324 0.330 1083 -2 (ubar) -71 690 690 1084 1095 0 154 0.317 1.929 -6.362 6.664 0.330 1084 323 (K*+) -83 1082 1083 1428 1429 0 0 -0.614 0.215 843.026 843.027 0.932 1085 -321 K- 83 1082 1083 0 0 0 0 -0.147 0.392 168.658 168.659 0.494 1086 211 pi+ 83 1082 1083 0 0 0 0 0.038 0.049 142.633 142.633 0.140 1087 -211 pi- 83 1082 1083 0 0 0 0 0.020 -0.058 4.402 4.404 0.140 1088 211 pi+ 83 1082 1083 0 0 0 0 -0.321 -0.376 38.182 38.186 0.140 1089 -211 pi- 84 1082 1083 0 0 0 0 0.472 0.452 4.091 4.145 0.140 1090 111 (pi0) -84 1082 1083 1602 1603 0 0 0.182 -0.267 1.337 1.382 0.135 1091 223 (omega) -84 1082 1083 1604 1606 0 0 -0.458 0.070 10.913 10.951 0.789 1092 211 pi+ 84 1082 1083 0 0 0 0 0.368 -0.071 0.421 0.580 0.140 1093 2212 p+ 84 1082 1083 0 0 0 0 -0.327 0.493 -0.480 1.209 0.938 1094 223 (omega) -84 1082 1083 1607 1609 0 0 0.267 0.167 -1.308 1.508 0.681 1095 -2224 (Deltabar--) -84 1082 1083 1430 1431 0 0 0.157 1.309 -3.911 4.305 1.223 1096 1 (d) -71 538 538 1110 1146 124 0 -1.240 -1.054 252.439 252.444 0.330 1097 21 (g) -71 557 557 1110 1146 266 124 0.030 -0.015 -0.000 0.034 0.000 1098 21 (g) -71 532 532 1110 1146 196 266 0.369 -0.542 -10.266 10.287 0.000 1099 21 (g) -71 847 847 1110 1146 214 196 -0.513 -1.006 -0.521 1.285 0.324 1100 21 (g) -71 554 554 1110 1146 242 214 0.266 -0.280 -0.595 0.710 0.000 1101 21 (g) -71 547 547 1110 1146 101 242 -0.522 0.035 -0.365 0.638 0.000 1102 21 (g) -71 542 542 1110 1146 192 101 -1.157 2.022 -1.192 2.617 0.000 1103 21 (g) -71 531 531 1110 1146 126 192 0.280 1.215 -0.860 1.514 0.000 1104 21 (g) -71 540 540 1110 1146 177 126 -0.752 0.916 0.011 1.185 0.000 1105 21 (g) -71 846 846 1110 1146 218 177 -4.066 3.639 4.199 6.891 0.284 1106 21 (g) -71 556 556 1110 1146 262 218 -0.399 0.749 1.338 1.585 0.000 1107 21 (g) -71 548 548 1110 1146 238 262 0.064 -0.066 -0.062 0.111 0.000 1108 21 (g) -71 848 848 1110 1146 105 238 -0.920 -0.420 2.017 2.294 0.416 1109 -1 (dbar) -71 539 539 1110 1146 0 105 -0.462 -0.040 336.984 336.985 0.330 1110 -211 pi- 83 1096 1109 0 0 0 0 -0.824 0.353 62.393 62.400 0.140 1111 211 pi+ 83 1096 1109 0 0 0 0 -0.296 -1.449 144.431 144.439 0.140 1112 221 (eta) -83 1096 1109 1610 1611 0 0 -0.261 -0.015 34.107 34.113 0.548 1113 -211 pi- 83 1096 1109 0 0 0 0 0.350 -0.057 1.033 1.101 0.140 1114 223 (omega) -83 1096 1109 1612 1614 0 0 0.445 0.299 5.868 5.944 0.784 1115 3122 (Lambda0) -83 1096 1109 1615 1616 0 0 -0.714 -0.344 2.865 3.175 1.116 1116 313 (K*0) -83 1096 1109 1432 1433 0 0 0.134 -0.021 0.195 0.840 0.805 1117 -3112 (Sigmabar+) -83 1096 1109 1617 1618 0 0 -0.351 -0.015 -0.578 1.375 1.197 1118 -321 K- 83 1096 1109 0 0 0 0 0.388 -0.038 0.074 0.633 0.494 1119 223 (omega) -83 1096 1109 1619 1621 0 0 0.227 0.084 -0.786 1.129 0.773 1120 211 pi+ 83 1096 1109 0 0 0 0 -0.045 -0.139 -1.856 1.867 0.140 1121 -211 pi- 83 1096 1109 0 0 0 0 -0.303 -0.109 -0.211 0.410 0.140 1122 223 (omega) -83 1096 1109 1622 1623 0 0 0.326 -0.641 -5.094 5.203 0.781 1123 211 pi+ 83 1096 1109 0 0 0 0 -0.091 0.056 0.023 0.178 0.140 1124 -211 pi- 83 1096 1109 0 0 0 0 -0.158 -0.544 -0.554 0.804 0.140 1125 211 pi+ 83 1096 1109 0 0 0 0 -0.229 0.629 -0.685 0.968 0.140 1126 113 (rho0) -83 1096 1109 1434 1435 0 0 -0.465 -0.477 -1.043 1.460 0.776 1127 -211 pi- 84 1096 1109 0 0 0 0 -0.377 1.016 -0.753 1.327 0.140 1128 211 pi+ 84 1096 1109 0 0 0 0 -1.030 2.213 -0.000 2.445 0.140 1129 111 (pi0) -84 1096 1109 1624 1625 0 0 -0.211 -0.316 0.096 0.414 0.135 1130 -213 (rho-) -84 1096 1109 1436 1437 0 0 -0.980 1.418 0.767 1.998 0.657 1131 111 (pi0) -84 1096 1109 1626 1627 0 0 -0.084 0.068 0.193 0.259 0.135 1132 211 pi+ 84 1096 1109 0 0 0 0 -0.306 0.421 0.146 0.558 0.140 1133 -211 pi- 84 1096 1109 0 0 0 0 -0.297 0.487 1.036 1.191 0.140 1134 113 (rho0) -84 1096 1109 1438 1439 0 0 -1.250 1.189 0.692 2.310 1.372 1135 211 pi+ 84 1096 1109 0 0 0 0 -0.146 0.451 1.001 1.116 0.140 1136 111 (pi0) -84 1096 1109 1628 1629 0 0 -0.982 0.371 0.889 1.382 0.135 1137 111 (pi0) -84 1096 1109 1630 1631 0 0 0.001 -0.060 0.084 0.170 0.135 1138 -213 (rho-) -84 1096 1109 1440 1441 0 0 -0.590 0.388 1.909 2.184 0.790 1139 111 (pi0) -84 1096 1109 1632 1633 0 0 0.122 0.174 0.267 0.367 0.135 1140 2212 p+ 84 1096 1109 0 0 0 0 -0.069 0.098 3.855 3.969 0.938 1141 -2112 nbar0 84 1096 1109 0 0 0 0 0.353 -0.333 10.765 10.817 0.940 1142 -211 pi- 84 1096 1109 0 0 0 0 -0.837 -0.022 47.970 47.977 0.140 1143 221 (eta) -84 1096 1109 1634 1635 0 0 0.177 0.488 26.207 26.218 0.548 1144 323 (K*+) -84 1096 1109 1442 1443 0 0 -0.002 -0.312 30.308 30.322 0.867 1145 -313 (K*bar0) -84 1096 1109 1444 1445 0 0 -0.310 -0.132 123.425 123.429 0.892 1146 111 (pi0) -84 1096 1109 1636 1637 0 0 -0.334 -0.030 94.087 94.087 0.135 1147 2 (u) -71 884 884 1152 1167 144 0 -1.260 -0.101 -73.514 73.528 0.659 1148 21 (g) -71 665 665 1152 1167 231 144 -1.577 1.066 -295.089 295.095 0.000 1149 21 (g) -71 883 883 1152 1167 155 231 -0.672 -0.111 -377.705 377.706 0.373 1150 21 (g) -71 885 885 1152 1167 159 155 0.334 1.163 -259.062 259.065 0.586 1151 -2 (ubar) -71 694 694 1152 1167 0 159 -0.526 0.982 12.303 12.358 0.330 1152 211 pi+ 83 1147 1151 0 0 0 0 -0.002 0.529 -59.495 59.498 0.140 1153 111 (pi0) -83 1147 1151 1638 1639 0 0 -1.479 0.465 -178.845 178.852 0.135 1154 223 (omega) -83 1147 1151 1640 1642 0 0 -0.155 -0.856 -129.754 129.759 0.781 1155 311 (K0) -83 1147 1151 1446 1446 0 0 -1.215 1.017 -297.394 297.399 0.498 1156 -323 (K*-) -83 1147 1151 1447 1448 0 0 0.074 0.398 -51.818 51.826 0.810 1157 221 (eta) -83 1147 1151 1643 1645 0 0 -0.467 0.526 -180.303 180.305 0.548 1158 111 (pi0) -83 1147 1151 1646 1647 0 0 -0.381 -0.438 -58.059 58.062 0.135 1159 213 (rho+) -83 1147 1151 1449 1450 0 0 0.402 0.284 -17.239 17.271 0.927 1160 2112 n0 83 1147 1151 0 0 0 0 0.077 0.030 -18.758 18.782 0.940 1161 -2112 nbar0 84 1147 1151 0 0 0 0 -0.040 0.493 -9.598 9.656 0.940 1162 113 (rho0) -84 1147 1151 1451 1452 0 0 0.026 -0.154 -2.061 2.223 0.817 1163 223 (omega) -84 1147 1151 1648 1649 0 0 0.148 0.009 -1.204 1.445 0.785 1164 111 (pi0) -84 1147 1151 1650 1651 0 0 -0.245 -0.595 0.581 0.877 0.135 1165 -211 pi- 84 1147 1151 0 0 0 0 -0.014 0.794 -0.070 0.810 0.140 1166 211 pi+ 84 1147 1151 0 0 0 0 -0.377 0.378 10.198 10.213 0.140 1167 -211 pi- 84 1147 1151 0 0 0 0 -0.054 0.118 0.752 0.775 0.140 1168 1 (d) -71 650 650 1170 1183 138 0 -2.752 1.732 -566.583 566.593 0.330 1169 -2 (ubar) -71 655 655 1170 1183 0 138 2.171 -1.766 28.273 28.413 0.330 1170 -211 pi- 83 1168 1169 0 0 0 0 -0.065 -0.007 -4.589 4.591 0.140 1171 223 (omega) -83 1168 1169 1652 1654 0 0 -2.349 1.881 -497.011 497.020 0.776 1172 211 pi+ 83 1168 1169 0 0 0 0 -0.392 -0.333 -19.273 19.280 0.140 1173 -211 pi- 83 1168 1169 0 0 0 0 0.320 0.089 -7.395 7.404 0.140 1174 211 pi+ 83 1168 1169 0 0 0 0 -0.231 -0.210 -15.562 15.565 0.140 1175 -211 pi- 83 1168 1169 0 0 0 0 0.160 0.475 -7.473 7.492 0.140 1176 213 (rho+) -83 1168 1169 1453 1454 0 0 -0.217 -0.090 -3.790 3.862 0.703 1177 -213 (rho-) -83 1168 1169 1455 1456 0 0 0.277 -0.349 -5.953 6.027 0.833 1178 213 (rho+) -84 1168 1169 1457 1458 0 0 -0.371 -0.024 -2.242 2.396 0.758 1179 313 (K*0) -84 1168 1169 1459 1460 0 0 -0.139 0.364 -2.036 2.300 0.998 1180 -311 (Kbar0) -84 1168 1169 1461 1461 0 0 0.145 -0.594 0.143 0.802 0.498 1181 311 (K0) -84 1168 1169 1462 1462 0 0 -0.198 0.823 -0.157 0.994 0.498 1182 -311 (Kbar0) -84 1168 1169 1463 1463 0 0 1.129 -0.820 7.582 7.725 0.498 1183 -213 (rho-) -84 1168 1169 1464 1465 0 0 1.351 -1.239 19.445 19.546 0.754 1184 4 (c) -71 560 560 1196 1217 108 0 4.883 -13.455 13.960 20.050 1.500 1185 21 (g) -71 580 580 1196 1217 258 108 -0.103 0.361 -1.118 1.180 0.000 1186 21 (g) -71 852 852 1196 1217 195 258 0.925 0.460 -2.691 2.936 0.560 1187 21 (g) -71 849 849 1196 1217 233 195 -0.216 0.369 -5.181 5.202 0.179 1188 21 (g) -71 561 561 1196 1217 148 233 -0.144 0.141 -0.213 0.293 0.000 1189 21 (g) -71 581 581 1196 1217 261 148 0.629 0.162 -4.877 4.920 0.000 1190 21 (g) -71 566 566 1196 1217 182 261 -0.235 -0.039 -3.449 3.457 0.000 1191 21 (g) -71 851 851 1196 1217 263 182 -0.692 0.667 -86.923 86.929 0.448 1192 21 (g) -71 582 582 1196 1217 107 263 -1.776 0.118 -141.570 141.581 0.000 1193 21 (g) -71 850 850 1196 1217 252 107 -0.691 0.814 -329.253 329.255 0.320 1194 21 (g) -71 579 579 1196 1217 125 252 -0.684 1.910 -376.536 376.542 0.000 1195 -2 (ubar) -71 570 570 1196 1217 0 125 -1.257 2.117 -178.548 178.565 0.330 1196 423 (D*0) -83 1184 1195 1655 1656 0 0 3.719 -10.218 10.819 15.470 2.007 1197 111 (pi0) -83 1184 1195 1657 1658 0 0 0.336 -0.540 0.222 0.687 0.135 1198 323 (K*+) -83 1184 1195 1466 1467 0 0 0.609 -1.672 1.853 2.733 0.931 1199 -311 (Kbar0) -83 1184 1195 1468 1468 0 0 0.019 -0.518 0.132 0.730 0.498 1200 -213 (rho-) -83 1184 1195 1469 1470 0 0 0.411 0.646 -1.221 1.558 0.591 1201 213 (rho+) -83 1184 1195 1471 1472 0 0 -0.109 -0.592 -1.751 2.293 1.354 1202 223 (omega) -83 1184 1195 1659 1661 0 0 -0.039 -0.137 -0.358 0.870 0.780 1203 -211 pi- 83 1184 1195 0 0 0 0 0.200 0.334 -0.212 0.465 0.140 1204 211 pi+ 83 1184 1195 0 0 0 0 0.025 0.385 -2.347 2.382 0.140 1205 111 (pi0) -83 1184 1195 1662 1663 0 0 0.629 -0.023 -3.955 4.007 0.135 1206 221 (eta) -83 1184 1195 1664 1666 0 0 -0.174 0.228 -4.653 4.694 0.548 1207 113 (rho0) -83 1184 1195 1473 1474 0 0 0.191 -0.300 -10.631 10.659 0.687 1208 -213 (rho-) -83 1184 1195 1475 1476 0 0 -0.667 0.843 -89.808 89.817 0.608 1209 221 (eta) -83 1184 1195 1667 1669 0 0 -0.235 0.007 -12.827 12.841 0.548 1210 111 (pi0) -84 1184 1195 1670 1671 0 0 -0.686 0.478 -95.675 95.678 0.135 1211 213 (rho+) -84 1184 1195 1477 1478 0 0 -0.373 0.099 -47.899 47.907 0.789 1212 -211 pi- 84 1184 1195 0 0 0 0 -0.259 0.254 -172.250 172.250 0.140 1213 223 (omega) -84 1184 1195 1672 1673 0 0 -0.489 0.818 -117.754 117.760 0.786 1214 111 (pi0) -84 1184 1195 1674 1675 0 0 -0.650 0.507 -90.435 90.439 0.135 1215 211 pi+ 84 1184 1195 0 0 0 0 -0.406 0.490 -217.484 217.485 0.140 1216 113 (rho0) -84 1184 1195 1479 1480 0 0 -0.849 1.606 -164.681 164.692 0.696 1217 -211 pi- 84 1184 1195 0 0 0 0 -0.563 0.931 -95.487 95.494 0.140 1218 1 (d) -71 701 701 1231 1258 111 0 -0.489 -0.643 -81.625 81.629 0.330 1219 21 (g) -71 573 573 1231 1258 198 111 2.878 -0.665 -723.877 723.883 0.000 1220 21 (g) -71 563 563 1231 1258 162 198 4.091 -1.037 -711.629 711.641 0.000 1221 21 (g) -71 577 577 1231 1258 247 162 0.219 -0.271 -34.119 34.121 0.000 1222 21 (g) -71 568 568 1231 1258 106 247 0.107 0.822 -178.213 178.215 0.000 1223 21 (g) -71 533 533 1231 1258 205 106 0.267 1.704 25.987 26.045 0.000 1224 21 (g) -71 544 544 1231 1258 165 205 0.875 0.473 18.543 18.570 0.000 1225 21 (g) -71 537 537 1231 1258 110 165 -0.141 0.032 10.452 10.453 0.000 1226 21 (g) -71 541 541 1231 1258 246 110 0.326 0.551 2.582 2.660 0.000 1227 21 (g) -71 896 896 1231 1258 151 246 2.110 0.664 15.372 15.535 0.421 1228 21 (g) -71 897 897 1231 1258 234 151 -0.019 0.082 1.340 1.444 0.530 1229 21 (g) -71 552 552 1231 1258 209 234 1.026 -0.020 5.796 5.886 0.000 1230 -1 (dbar) -71 895 895 1231 1258 0 209 3.983 -0.351 9.503 10.317 0.374 1231 111 (pi0) -83 1218 1230 1676 1677 0 0 0.497 0.133 -79.472 79.473 0.135 1232 -213 (rho-) -83 1218 1230 1481 1482 0 0 0.142 -0.928 -272.395 272.398 0.779 1233 223 (omega) -83 1218 1230 1678 1680 0 0 1.561 -0.473 -318.786 318.791 0.770 1234 211 pi+ 83 1218 1230 0 0 0 0 -0.034 -0.106 -22.295 22.296 0.140 1235 111 (pi0) -83 1218 1230 1681 1682 0 0 0.746 -0.243 -105.023 105.026 0.135 1236 111 (pi0) -83 1218 1230 1683 1684 0 0 0.464 -0.326 -72.981 72.984 0.135 1237 -211 pi- 83 1218 1230 0 0 0 0 1.280 0.245 -308.034 308.037 0.140 1238 211 pi+ 83 1218 1230 0 0 0 0 0.293 -0.070 -37.191 37.192 0.140 1239 311 (K0) -83 1218 1230 1483 1483 0 0 0.974 0.041 -313.043 313.045 0.498 1240 -321 K- 83 1218 1230 0 0 0 0 0.046 0.100 -19.956 19.962 0.494 1241 211 pi+ 83 1218 1230 0 0 0 0 0.917 -0.324 -80.150 80.156 0.140 1242 311 (K0) -83 1218 1230 1484 1484 0 0 0.067 -0.578 -26.464 26.475 0.498 1243 -311 (Kbar0) -83 1218 1230 1485 1485 0 0 -0.443 0.873 -17.933 17.967 0.498 1244 -211 pi- 83 1218 1230 0 0 0 0 -0.004 -0.186 -20.245 20.246 0.140 1245 213 (rho+) -83 1218 1230 1486 1487 0 0 0.672 -0.038 -20.626 20.667 1.108 1246 -213 (rho-) -83 1218 1230 1488 1489 0 0 -0.197 0.078 -13.236 13.267 0.887 1247 113 (rho0) -83 1218 1230 1490 1491 0 0 -0.441 -0.068 -0.845 1.165 0.666 1248 211 pi+ 84 1218 1230 0 0 0 0 0.065 -0.246 0.708 0.765 0.140 1249 111 (pi0) -84 1218 1230 1685 1686 0 0 0.704 0.470 -0.139 0.868 0.135 1250 111 (pi0) -84 1218 1230 1687 1688 0 0 -0.701 0.403 7.965 8.007 0.135 1251 311 (K0) -84 1218 1230 1492 1492 0 0 0.625 0.524 18.856 18.881 0.498 1252 -311 (Kbar0) -84 1218 1230 1493 1493 0 0 0.710 0.265 5.430 5.505 0.498 1253 -211 pi- 84 1218 1230 0 0 0 0 -0.086 1.033 10.776 10.826 0.140 1254 223 (omega) -84 1218 1230 1689 1691 0 0 0.766 0.320 17.145 17.183 0.782 1255 213 (rho+) -84 1218 1230 1494 1495 0 0 0.648 0.553 5.623 5.749 0.845 1256 221 (eta) -84 1218 1230 1692 1693 0 0 1.303 0.082 9.256 9.364 0.548 1257 113 (rho0) -84 1218 1230 1496 1497 0 0 1.077 0.387 3.779 4.023 0.769 1258 221 (eta) -84 1218 1230 1694 1696 0 0 3.580 -0.579 9.390 10.081 0.548 1259 2 (u) -71 862 862 1284 1326 119 0 -1.622 -0.826 -52.894 52.933 0.898 1260 21 (g) -71 600 600 1284 1326 113 119 2.335 -3.393 -94.787 94.877 0.000 1261 21 (g) -71 856 856 1284 1326 223 113 0.526 -0.205 -3.284 3.335 0.133 1262 21 (g) -71 601 601 1284 1326 180 223 0.104 0.339 -0.033 0.356 0.000 1263 21 (g) -71 863 863 1284 1326 249 180 0.265 -1.893 -1.831 2.670 0.355 1264 21 (g) -71 619 619 1284 1326 156 249 0.263 0.143 -0.662 0.726 0.000 1265 21 (g) -71 588 588 1284 1326 116 156 1.215 0.975 -0.816 1.759 0.000 1266 21 (g) -71 599 599 1284 1326 163 116 -0.100 0.104 -0.172 0.224 0.000 1267 21 (g) -71 858 858 1284 1326 243 163 0.824 0.451 0.842 1.283 0.236 1268 21 (g) -71 859 859 1284 1326 253 243 1.565 -0.412 3.396 3.770 0.252 1269 21 (g) -71 857 857 1284 1326 199 253 1.954 0.322 6.325 6.630 0.190 1270 21 (g) -71 865 865 1284 1326 141 199 2.359 -0.309 15.309 15.497 0.398 1271 21 (g) -71 864 864 1284 1326 213 141 0.054 -1.124 5.883 6.002 0.393 1272 21 (g) -71 674 674 1284 1326 161 213 -1.683 -1.382 5.138 5.580 0.000 1273 21 (g) -71 680 680 1284 1326 248 161 -0.630 -0.164 0.720 0.970 0.000 1274 21 (g) -71 860 860 1284 1326 167 248 -1.387 0.439 12.421 12.509 0.279 1275 21 (g) -71 632 632 1284 1326 145 167 -0.652 -0.194 2.943 3.021 0.000 1276 21 (g) -71 866 866 1284 1326 227 145 0.265 -1.682 66.321 66.345 0.493 1277 21 (g) -71 661 661 1284 1326 240 227 0.638 0.020 16.143 16.156 0.000 1278 21 (g) -71 611 611 1284 1326 219 240 0.945 -0.022 63.359 63.366 0.000 1279 21 (g) -71 608 608 1284 1326 215 219 0.764 0.608 79.085 79.091 0.000 1280 21 (g) -71 603 603 1284 1326 191 215 0.096 0.377 68.214 68.215 0.000 1281 21 (g) -71 589 589 1284 1326 117 191 4.205 3.359 796.399 796.417 0.000 1282 21 (g) -71 634 634 1284 1326 142 117 0.948 0.196 143.297 143.301 0.000 1283 2101 (ud_0) -71 696 696 1284 1326 0 142 0.096 0.454 1440.814 1440.814 0.579 1284 321 K+ 83 1259 1283 0 0 0 0 -0.200 -0.390 -9.978 9.999 0.494 1285 -311 (Kbar0) -83 1259 1283 1498 1498 0 0 -1.153 -0.499 -37.093 37.117 0.498 1286 221 (eta) -83 1259 1283 1697 1698 0 0 1.139 -1.832 -54.574 54.619 0.548 1287 -211 pi- 83 1259 1283 0 0 0 0 0.098 0.154 -4.040 4.046 0.140 1288 213 (rho+) -83 1259 1283 1499 1500 0 0 1.061 -0.781 -29.397 29.446 1.061 1289 311 (K0) -83 1259 1283 1501 1501 0 0 -0.145 -0.521 -14.381 14.400 0.498 1290 -313 (K*bar0) -83 1259 1283 1502 1503 0 0 0.377 -1.153 -2.412 2.890 1.030 1291 -211 pi- 83 1259 1283 0 0 0 0 -0.100 0.154 0.029 0.232 0.140 1292 321 K+ 83 1259 1283 0 0 0 0 0.638 -0.291 -0.691 1.101 0.494 1293 -311 (Kbar0) -83 1259 1283 1504 1504 0 0 0.324 -0.151 -0.385 0.724 0.498 1294 113 (rho0) -83 1259 1283 1505 1506 0 0 0.615 0.055 -0.638 1.162 0.749 1295 -213 (rho-) -83 1259 1283 1507 1508 0 0 0.145 0.131 0.014 0.776 0.751 1296 211 pi+ 83 1259 1283 0 0 0 0 0.202 0.327 -0.244 0.476 0.140 1297 223 (omega) -83 1259 1283 1699 1701 0 0 1.218 0.076 1.561 2.131 0.785 1298 221 (eta) -83 1259 1283 1702 1703 0 0 0.512 0.159 0.481 0.905 0.548 1299 -211 pi- 83 1259 1283 0 0 0 0 -0.132 0.093 1.440 1.456 0.140 1300 211 pi+ 83 1259 1283 0 0 0 0 1.210 -0.361 2.507 2.811 0.140 1301 -213 (rho-) -83 1259 1283 1509 1510 0 0 0.667 0.567 6.037 6.136 0.665 1302 211 pi+ 83 1259 1283 0 0 0 0 0.734 -0.356 2.379 2.519 0.140 1303 313 (K*0) -83 1259 1283 1511 1512 0 0 0.504 -0.946 4.564 4.777 0.920 1304 -313 (K*bar0) -83 1259 1283 1513 1514 0 0 1.740 0.022 10.517 10.723 1.168 1305 111 (pi0) -83 1259 1283 1704 1705 0 0 -0.191 -0.779 1.343 1.570 0.135 1306 3112 (Sigma-) -83 1259 1283 1706 1707 0 0 -1.179 -0.095 6.623 6.834 1.197 1307 113 (rho0) -83 1259 1283 1515 1516 0 0 -1.537 -0.741 8.195 8.438 1.065 1308 -3114 (Sigma*bar+) -83 1259 1283 1517 1518 0 0 -0.002 -0.810 13.929 14.022 1.400 1309 -213 (rho-) -83 1259 1283 1519 1520 0 0 -0.589 0.759 11.514 11.608 1.112 1310 223 (omega) -84 1259 1283 1708 1710 0 0 -0.325 -0.754 16.514 16.553 0.788 1311 211 pi+ 84 1259 1283 0 0 0 0 -0.032 -0.156 2.719 2.727 0.140 1312 -211 pi- 84 1259 1283 0 0 0 0 0.382 -0.352 24.395 24.400 0.140 1313 211 pi+ 84 1259 1283 0 0 0 0 0.631 0.258 38.498 38.504 0.140 1314 -211 pi- 84 1259 1283 0 0 0 0 0.114 -0.187 19.875 19.877 0.140 1315 221 (eta) -84 1259 1283 1711 1713 0 0 0.123 0.139 68.767 68.769 0.548 1316 111 (pi0) -84 1259 1283 1714 1715 0 0 0.170 0.454 42.867 42.870 0.135 1317 2212 p+ 84 1259 1283 0 0 0 0 0.946 0.371 151.125 151.132 0.938 1318 111 (pi0) -84 1259 1283 1716 1717 0 0 0.546 -0.031 51.944 51.947 0.135 1319 -2212 pbar- 84 1259 1283 0 0 0 0 1.640 1.239 267.848 267.857 0.938 1320 213 (rho+) -84 1259 1283 1521 1522 0 0 1.532 0.738 258.903 258.910 0.709 1321 111 (pi0) -84 1259 1283 1718 1719 0 0 0.181 -0.075 38.679 38.679 0.135 1322 221 (eta) -84 1259 1283 1720 1722 0 0 0.114 0.658 173.469 173.471 0.548 1323 -213 (rho-) -84 1259 1283 1523 1524 0 0 0.573 0.343 185.822 185.825 0.768 1324 211 pi+ 84 1259 1283 0 0 0 0 0.242 0.213 59.965 59.966 0.140 1325 -211 pi- 84 1259 1283 0 0 0 0 0.575 0.142 423.985 423.985 0.140 1326 2212 p+ 84 1259 1283 0 0 0 0 -0.023 0.389 829.454 829.455 0.938 1327 2 (u) -71 630 630 1329 1346 147 0 -1.548 -1.476 1688.804 1688.806 0.330 1328 -2 (ubar) -71 629 629 1329 1346 0 147 -2.851 -1.912 -273.985 274.006 0.330 1329 211 pi+ 83 1327 1328 0 0 0 0 -0.284 -0.378 634.169 634.169 0.140 1330 1114 (Delta-) -83 1327 1328 1525 1526 0 0 -0.587 -1.029 562.070 562.073 1.310 1331 -1114 (Deltabar+) -83 1327 1328 1527 1528 0 0 -0.499 0.270 329.329 329.333 1.429 1332 -211 pi- 83 1327 1328 0 0 0 0 -0.234 -0.059 58.739 58.740 0.140 1333 2212 p+ 83 1327 1328 0 0 0 0 0.067 -0.888 67.194 67.207 0.938 1334 -211 pi- 83 1327 1328 0 0 0 0 -0.140 0.535 16.297 16.307 0.140 1335 -2114 (Deltabar0) -83 1327 1328 1529 1530 0 0 -0.031 -0.150 10.555 10.637 1.312 1336 111 (pi0) -83 1327 1328 1723 1724 0 0 0.170 -0.008 0.906 0.931 0.135 1337 223 (omega) -83 1327 1328 1725 1727 0 0 -0.010 0.305 5.064 5.126 0.731 1338 113 (rho0) -83 1327 1328 1531 1532 0 0 0.034 -0.233 2.896 3.012 0.792 1339 221 (eta) -83 1327 1328 1728 1729 0 0 0.115 0.152 0.500 0.766 0.548 1340 211 pi+ 84 1327 1328 0 0 0 0 0.029 0.267 -0.639 0.707 0.140 1341 111 (pi0) -84 1327 1328 1730 1731 0 0 -0.172 -0.254 0.204 0.393 0.135 1342 -211 pi- 84 1327 1328 0 0 0 0 -0.179 -0.344 0.276 0.496 0.140 1343 221 (eta) -84 1327 1328 1732 1733 0 0 0.475 0.803 -5.427 5.534 0.548 1344 211 pi+ 84 1327 1328 0 0 0 0 -0.517 -0.549 -6.505 6.550 0.140 1345 113 (rho0) -84 1327 1328 1533 1534 0 0 -2.173 -1.919 -228.415 228.435 0.891 1346 -211 pi- 84 1327 1328 0 0 0 0 -0.461 0.088 -32.394 32.398 0.140 1347 311 (K0) -91 926 0 1535 1535 0 0 0.579 2.247 4.592 5.169 0.498 1348 211 pi+ 91 926 0 0 0 0 0 0.036 0.347 1.322 1.374 0.140 1349 130 K_L0 91 927 927 0 0 0 0 -0.419 0.380 -0.042 0.755 0.498 1350 211 pi+ 91 937 0 0 0 0 0 0.241 0.052 -113.349 113.350 0.140 1351 -211 pi- 91 937 0 0 0 0 0 -0.196 0.081 -20.833 20.834 0.140 1352 321 K+ 91 946 0 0 0 0 0 -0.436 0.273 53.267 53.272 0.494 1353 -211 pi- 91 946 0 0 0 0 0 0.111 0.102 58.564 58.564 0.140 1354 130 K_L0 91 947 947 0 0 0 0 -0.355 0.349 19.287 19.300 0.498 1355 311 (K0) -91 948 0 1536 1536 0 0 0.036 -0.149 3.391 3.431 0.498 1356 111 (pi0) -91 948 0 1734 1735 0 0 0.157 0.321 1.875 1.913 0.135 1357 211 pi+ 91 951 0 0 0 0 0 0.221 0.012 0.606 0.660 0.140 1358 111 (pi0) -91 951 0 1736 1737 0 0 0.821 1.306 6.816 6.990 0.135 1359 -321 K- 91 959 0 0 0 0 0 6.557 -1.683 -6.613 9.476 0.494 1360 211 pi+ 91 959 0 0 0 0 0 5.791 -1.159 -5.317 7.948 0.140 1361 -211 pi- 91 960 0 0 0 0 0 3.597 -1.363 -3.753 5.376 0.140 1362 111 (pi0) -91 960 0 1738 1739 0 0 17.006 -5.264 -16.614 24.351 0.135 1363 -211 pi- 91 964 0 0 0 0 0 3.425 -0.058 -2.930 4.510 0.140 1364 111 (pi0) -91 964 0 1740 1741 0 0 2.396 -0.625 -1.700 3.007 0.135 1365 -311 (Kbar0) -91 989 0 1537 1537 0 0 0.331 -0.293 -0.113 0.675 0.498 1366 111 (pi0) -91 989 0 1742 1743 0 0 1.026 -0.829 -0.180 1.338 0.135 1367 -211 pi- 91 990 0 0 0 0 0 1.159 -2.271 0.352 2.577 0.140 1368 111 (pi0) -91 990 0 1744 1745 0 0 0.220 0.003 -0.088 0.272 0.135 1369 211 pi+ 91 991 0 0 0 0 0 0.256 0.044 -0.071 0.303 0.140 1370 111 (pi0) -91 991 0 1746 1747 0 0 0.189 -0.900 -0.192 0.949 0.135 1371 321 K+ 91 996 0 0 0 0 0 -0.163 -0.099 -0.100 0.538 0.494 1372 -211 pi- 91 996 0 0 0 0 0 -0.390 -0.431 -0.505 0.783 0.140 1373 211 pi+ 91 998 0 0 0 0 0 -0.347 -0.170 -0.319 0.520 0.140 1374 111 (pi0) -91 998 0 1748 1749 0 0 -1.765 -0.285 -3.317 3.771 0.135 1375 2112 n0 91 999 0 0 0 0 0 -4.893 -2.123 -9.555 10.983 0.940 1376 -211 pi- 91 999 0 0 0 0 0 -0.867 -0.294 -1.421 1.696 0.140 1377 -2112 nbar0 91 1000 0 0 0 0 0 -0.971 -0.405 -2.349 2.740 0.940 1378 111 (pi0) -91 1000 0 1750 1751 0 0 0.111 -0.132 -0.609 0.648 0.135 1379 2112 n0 91 1001 0 0 0 0 0 0.042 0.432 -3.150 3.315 0.940 1380 111 (pi0) -91 1001 0 1752 1753 0 0 0.016 0.029 -0.094 0.168 0.135 1381 -2112 nbar0 91 1003 0 0 0 0 0 0.063 1.841 -5.602 5.971 0.940 1382 211 pi+ 91 1003 0 0 0 0 0 0.049 0.480 -0.945 1.070 0.140 1383 -211 pi- 91 1004 0 0 0 0 0 -0.155 1.016 -3.425 3.579 0.140 1384 111 (pi0) -91 1004 0 1754 1755 0 0 0.159 0.004 -1.277 1.294 0.135 1385 211 pi+ 91 1005 0 0 0 0 0 0.459 1.128 -3.027 3.266 0.140 1386 111 (pi0) -91 1005 0 1756 1757 0 0 -0.058 0.178 -1.665 1.681 0.135 1387 2212 p+ 91 1007 0 0 0 0 0 0.005 0.315 -9.054 9.108 0.938 1388 211 pi+ 91 1007 0 0 0 0 0 0.030 -0.017 -9.933 9.934 0.140 1389 -2212 pbar- 91 1009 0 0 0 0 0 -0.563 -1.178 -95.794 95.808 0.938 1390 -211 pi- 91 1009 0 0 0 0 0 -0.775 -0.938 -84.506 84.514 0.140 1391 211 pi+ 91 1039 0 0 0 0 0 -0.103 0.212 -1.489 1.514 0.140 1392 -211 pi- 91 1039 0 0 0 0 0 0.572 0.011 -1.596 1.701 0.140 1393 -211 pi- 91 1041 0 0 0 0 0 0.999 -0.006 -1.476 1.788 0.140 1394 111 (pi0) -91 1041 0 1758 1759 0 0 0.879 0.089 -2.918 3.052 0.135 1395 130 K_L0 91 1044 1044 0 0 0 0 1.075 0.081 -0.735 1.397 0.498 1396 -211 pi- 91 1045 0 0 0 0 0 0.441 -0.412 -0.176 0.644 0.140 1397 111 (pi0) -91 1045 0 1760 1761 0 0 1.359 -1.231 -1.697 2.502 0.135 1398 211 pi+ 91 1047 0 0 0 0 0 -0.629 0.420 0.249 0.808 0.140 1399 111 (pi0) -91 1047 0 1762 1763 0 0 -0.311 -0.307 -0.010 0.458 0.135 1400 -211 pi- 91 1050 0 0 0 0 0 -1.148 0.582 4.134 4.332 0.140 1401 111 (pi0) -91 1050 0 1764 1765 0 0 -1.150 0.146 2.002 2.317 0.135 1402 211 pi+ 91 1052 0 0 0 0 0 -0.024 -0.404 0.348 0.552 0.140 1403 -211 pi- 91 1052 0 0 0 0 0 -0.456 0.156 1.287 1.382 0.140 1404 211 pi+ 91 1053 0 0 0 0 0 -0.964 -0.198 1.452 1.760 0.140 1405 -211 pi- 91 1053 0 0 0 0 0 -0.366 -0.554 1.568 1.709 0.140 1406 130 K_L0 91 1058 1058 0 0 0 0 0.049 -1.777 2.242 2.904 0.498 1407 3122 (Lambda0) -91 1059 0 1766 1767 0 0 0.202 -2.635 3.582 4.589 1.116 1408 111 (pi0) -91 1059 0 1768 1769 0 0 0.078 -1.232 1.544 1.981 0.135 1409 -2112 nbar0 91 1060 0 0 0 0 0 -3.105 -0.651 4.482 5.570 0.940 1410 111 (pi0) -91 1060 0 1770 1771 0 0 -0.685 -0.432 1.084 1.360 0.135 1411 321 K+ 91 1064 0 0 0 0 0 -8.933 -2.807 14.530 17.292 0.494 1412 111 (pi0) -91 1064 0 1772 1773 0 0 -2.108 -0.795 4.034 4.622 0.135 1413 130 K_L0 91 1065 1065 0 0 0 0 -4.892 -0.956 6.863 8.497 0.498 1414 211 pi+ 91 1067 0 0 0 0 0 -2.730 -0.400 4.055 4.907 0.140 1415 111 (pi0) -91 1067 0 1774 1775 0 0 -2.830 -1.100 4.337 5.296 0.135 1416 -211 pi- 91 1068 0 0 0 0 0 -4.048 -0.372 5.374 6.740 0.140 1417 111 (pi0) -91 1068 0 1776 1777 0 0 -1.146 -0.379 2.087 2.414 0.135 1418 211 pi+ 91 1071 0 0 0 0 0 -3.194 -0.783 3.066 4.498 0.140 1419 111 (pi0) -91 1071 0 1778 1779 0 0 -0.153 0.036 0.335 0.394 0.135 1420 -211 pi- 91 1074 0 0 0 0 0 -1.243 0.136 0.737 1.458 0.140 1421 111 (pi0) -91 1074 0 1780 1781 0 0 -0.015 -0.099 -0.053 0.176 0.135 1422 211 pi+ 91 1075 0 0 0 0 0 -0.701 0.938 0.046 1.180 0.140 1423 -211 pi- 91 1075 0 0 0 0 0 -0.444 -0.078 -0.251 0.534 0.140 1424 -211 pi- 91 1077 0 0 0 0 0 -0.743 1.289 -0.351 1.535 0.140 1425 111 (pi0) -91 1077 0 1782 1783 0 0 -1.141 0.156 -0.387 1.222 0.135 1426 321 K+ 91 1080 0 0 0 0 0 -1.449 1.627 -1.083 2.483 0.494 1427 -211 pi- 91 1080 0 0 0 0 0 -1.665 2.380 -1.009 3.078 0.140 1428 311 (K0) -91 1084 0 1538 1538 0 0 -0.549 0.318 449.764 449.765 0.498 1429 211 pi+ 91 1084 0 0 0 0 0 -0.066 -0.103 393.262 393.262 0.140 1430 -2212 pbar- 91 1095 0 0 0 0 0 0.342 1.018 -3.127 3.437 0.938 1431 -211 pi- 91 1095 0 0 0 0 0 -0.185 0.292 -0.784 0.868 0.140 1432 321 K+ 91 1116 0 0 0 0 0 0.299 0.068 0.162 0.603 0.494 1433 -211 pi- 91 1116 0 0 0 0 0 -0.165 -0.089 0.033 0.236 0.140 1434 211 pi+ 91 1126 0 0 0 0 0 -0.104 -0.321 -0.032 0.367 0.140 1435 -211 pi- 91 1126 0 0 0 0 0 -0.361 -0.155 -1.011 1.093 0.140 1436 -211 pi- 91 1130 0 0 0 0 0 -0.955 1.078 0.456 1.517 0.140 1437 111 (pi0) -91 1130 0 1784 1785 0 0 -0.025 0.341 0.311 0.481 0.135 1438 211 pi+ 91 1134 0 0 0 0 0 -0.738 0.893 1.080 1.590 0.140 1439 -211 pi- 91 1134 0 0 0 0 0 -0.512 0.296 -0.388 0.721 0.140 1440 -211 pi- 91 1138 0 0 0 0 0 -0.394 0.280 1.847 1.915 0.140 1441 111 (pi0) -91 1138 0 1786 1787 0 0 -0.196 0.108 0.062 0.269 0.135 1442 311 (K0) -91 1144 0 1539 1539 0 0 0.000 -0.472 19.868 19.879 0.498 1443 211 pi+ 91 1144 0 0 0 0 0 -0.002 0.160 10.440 10.442 0.140 1444 -321 K- 91 1145 0 0 0 0 0 -0.304 0.183 75.075 75.078 0.494 1445 211 pi+ 91 1145 0 0 0 0 0 -0.006 -0.314 48.350 48.351 0.140 1446 130 K_L0 91 1155 1155 0 0 0 0 -1.215 1.017 -297.394 297.399 0.498 1447 -321 K- 91 1156 0 0 0 0 0 -0.161 0.158 -32.066 32.070 0.494 1448 111 (pi0) -91 1156 0 1788 1789 0 0 0.234 0.241 -19.752 19.755 0.135 1449 211 pi+ 91 1159 0 0 0 0 0 -0.090 -0.027 -11.433 11.434 0.140 1450 111 (pi0) -91 1159 0 1790 1791 0 0 0.493 0.310 -5.806 5.837 0.135 1451 211 pi+ 91 1162 0 0 0 0 0 -0.088 -0.426 -1.557 1.622 0.140 1452 -211 pi- 91 1162 0 0 0 0 0 0.114 0.271 -0.504 0.600 0.140 1453 211 pi+ 91 1176 0 0 0 0 0 -0.178 -0.367 -2.256 2.297 0.140 1454 111 (pi0) -91 1176 0 1792 1793 0 0 -0.039 0.277 -1.533 1.564 0.135 1455 -211 pi- 91 1177 0 0 0 0 0 0.214 -0.559 -5.092 5.129 0.140 1456 111 (pi0) -91 1177 0 1794 1795 0 0 0.062 0.210 -0.861 0.899 0.135 1457 211 pi+ 91 1178 0 0 0 0 0 -0.477 -0.205 -1.069 1.196 0.140 1458 111 (pi0) -91 1178 0 1796 1797 0 0 0.105 0.181 -1.173 1.199 0.135 1459 321 K+ 91 1179 0 0 0 0 0 0.084 0.165 -1.847 1.921 0.494 1460 -211 pi- 91 1179 0 0 0 0 0 -0.222 0.199 -0.189 0.380 0.140 1461 130 K_L0 91 1180 1180 0 0 0 0 0.145 -0.594 0.143 0.802 0.498 1462 130 K_L0 91 1181 1181 0 0 0 0 -0.198 0.823 -0.157 0.994 0.498 1463 310 (K_S0) -91 1182 1182 1798 1799 0 0 1.129 -0.820 7.582 7.725 0.498 1464 -211 pi- 91 1183 0 0 0 0 0 1.265 -1.292 17.905 17.997 0.140 1465 111 (pi0) -91 1183 0 1800 1801 0 0 0.085 0.053 1.540 1.549 0.135 1466 311 (K0) -91 1198 0 1540 1540 0 0 0.245 -0.452 0.810 1.081 0.498 1467 211 pi+ 91 1198 0 0 0 0 0 0.364 -1.220 1.043 1.652 0.140 1468 310 (K_S0) -91 1199 1199 1802 1803 0 0 0.019 -0.518 0.132 0.730 0.498 1469 -211 pi- 91 1200 0 0 0 0 0 0.068 0.421 -0.943 1.045 0.140 1470 111 (pi0) -91 1200 0 1804 1805 0 0 0.343 0.225 -0.278 0.513 0.135 1471 211 pi+ 91 1201 0 0 0 0 0 -0.231 -0.351 -1.904 1.955 0.140 1472 111 (pi0) -91 1201 0 1806 1807 0 0 0.122 -0.242 0.153 0.339 0.135 1473 211 pi+ 91 1207 0 0 0 0 0 -0.190 -0.169 -2.477 2.494 0.140 1474 -211 pi- 91 1207 0 0 0 0 0 0.381 -0.131 -8.154 8.165 0.140 1475 -211 pi- 91 1208 0 0 0 0 0 -0.006 0.031 -19.960 19.961 0.140 1476 111 (pi0) -91 1208 0 1808 1809 0 0 -0.661 0.812 -69.848 69.856 0.135 1477 211 pi+ 91 1211 0 0 0 0 0 -0.584 -0.001 -36.108 36.113 0.140 1478 111 (pi0) -91 1211 0 1810 1811 0 0 0.210 0.100 -11.790 11.793 0.135 1479 211 pi+ 91 1216 0 0 0 0 0 -0.763 0.797 -101.661 101.667 0.140 1480 -211 pi- 91 1216 0 0 0 0 0 -0.086 0.809 -63.020 63.026 0.140 1481 -211 pi- 91 1232 0 0 0 0 0 -0.268 -0.170 -72.765 72.766 0.140 1482 111 (pi0) -91 1232 0 1812 1813 0 0 0.410 -0.758 -199.630 199.632 0.135 1483 130 K_L0 91 1239 1239 0 0 0 0 0.974 0.041 -313.043 313.045 0.498 1484 310 (K_S0) -91 1242 1242 1814 1815 0 0 0.067 -0.578 -26.464 26.475 0.498 1485 130 K_L0 91 1243 1243 0 0 0 0 -0.443 0.873 -17.933 17.967 0.498 1486 211 pi+ 91 1245 0 0 0 0 0 0.426 -0.336 -18.024 18.032 0.140 1487 111 (pi0) -91 1245 0 1816 1817 0 0 0.246 0.298 -2.602 2.634 0.135 1488 -211 pi- 91 1246 0 0 0 0 0 -0.355 -0.120 -2.896 2.924 0.140 1489 111 (pi0) -91 1246 0 1818 1819 0 0 0.157 0.197 -10.339 10.343 0.135 1490 211 pi+ 91 1247 0 0 0 0 0 -0.503 0.142 -0.587 0.798 0.140 1491 -211 pi- 91 1247 0 0 0 0 0 0.062 -0.211 -0.258 0.366 0.140 1492 130 K_L0 91 1251 1251 0 0 0 0 0.625 0.524 18.856 18.881 0.498 1493 130 K_L0 91 1252 1252 0 0 0 0 0.710 0.265 5.430 5.505 0.498 1494 211 pi+ 91 1255 0 0 0 0 0 0.632 0.188 4.695 4.743 0.140 1495 111 (pi0) -91 1255 0 1820 1821 0 0 0.016 0.365 0.928 1.007 0.135 1496 211 pi+ 91 1257 0 0 0 0 0 0.647 0.552 1.961 2.142 0.140 1497 -211 pi- 91 1257 0 0 0 0 0 0.430 -0.165 1.818 1.881 0.140 1498 310 (K_S0) -91 1285 1285 1822 1823 0 0 -1.153 -0.499 -37.093 37.117 0.498 1499 211 pi+ 91 1288 0 0 0 0 0 0.021 -0.561 -13.598 13.611 0.140 1500 111 (pi0) -91 1288 0 1824 1825 0 0 1.040 -0.219 -15.799 15.835 0.135 1501 130 K_L0 91 1289 1289 0 0 0 0 -0.145 -0.521 -14.381 14.400 0.498 1502 -321 K- 91 1290 0 0 0 0 0 0.025 -0.163 -0.955 1.088 0.494 1503 211 pi+ 91 1290 0 0 0 0 0 0.352 -0.991 -1.457 1.802 0.140 1504 310 (K_S0) -91 1293 1293 1826 1827 0 0 0.324 -0.151 -0.385 0.724 0.498 1505 211 pi+ 91 1294 0 0 0 0 0 0.341 0.376 -0.335 0.624 0.140 1506 -211 pi- 91 1294 0 0 0 0 0 0.274 -0.321 -0.303 0.538 0.140 1507 -211 pi- 91 1295 0 0 0 0 0 0.222 0.044 -0.309 0.407 0.140 1508 111 (pi0) -91 1295 0 1828 1829 0 0 -0.077 0.087 0.323 0.369 0.135 1509 -211 pi- 91 1301 0 0 0 0 0 -0.006 0.340 2.408 2.436 0.140 1510 111 (pi0) -91 1301 0 1830 1831 0 0 0.674 0.227 3.630 3.701 0.135 1511 321 K+ 91 1303 0 0 0 0 0 0.114 -0.354 2.871 2.936 0.494 1512 -211 pi- 91 1303 0 0 0 0 0 0.390 -0.592 1.693 1.841 0.140 1513 -321 K- 91 1304 0 0 0 0 0 0.639 -0.346 5.678 5.745 0.494 1514 211 pi+ 91 1304 0 0 0 0 0 1.101 0.369 4.839 4.978 0.140 1515 211 pi+ 91 1307 0 0 0 0 0 -1.198 -0.280 6.970 7.079 0.140 1516 -211 pi- 91 1307 0 0 0 0 0 -0.339 -0.460 1.225 1.359 0.140 1517 -3122 (Lambdabar0) -91 1308 0 1832 1833 0 0 -0.189 -0.761 11.070 11.154 1.116 1518 211 pi+ 91 1308 0 0 0 0 0 0.187 -0.049 2.858 2.868 0.140 1519 -211 pi- 91 1309 0 0 0 0 0 -0.793 0.562 10.503 10.549 0.140 1520 111 (pi0) -91 1309 0 1834 1835 0 0 0.204 0.196 1.011 1.059 0.135 1521 211 pi+ 91 1320 0 0 0 0 0 0.647 0.547 90.661 90.665 0.140 1522 111 (pi0) -91 1320 0 1836 1837 0 0 0.885 0.191 168.242 168.245 0.135 1523 -211 pi- 91 1323 0 0 0 0 0 0.699 0.249 114.655 114.657 0.140 1524 111 (pi0) -91 1323 0 1838 1839 0 0 -0.126 0.093 71.167 71.167 0.135 1525 2112 n0 91 1330 0 0 0 0 0 -0.441 -0.412 349.228 349.230 0.940 1526 -211 pi- 91 1330 0 0 0 0 0 -0.146 -0.616 212.843 212.844 0.140 1527 -2112 nbar0 91 1331 0 0 0 0 0 -0.424 -0.180 203.979 203.981 0.940 1528 211 pi+ 91 1331 0 0 0 0 0 -0.075 0.450 125.350 125.351 0.140 1529 -2112 nbar0 91 1335 0 0 0 0 0 -0.274 -0.204 9.129 9.183 0.940 1530 111 (pi0) -91 1335 0 1840 1841 0 0 0.243 0.054 1.426 1.454 0.135 1531 211 pi+ 91 1338 0 0 0 0 0 0.276 -0.164 0.578 0.676 0.140 1532 -211 pi- 91 1338 0 0 0 0 0 -0.242 -0.069 2.318 2.336 0.140 1533 211 pi+ 91 1345 0 0 0 0 0 -0.794 -0.262 -78.411 78.415 0.140 1534 -211 pi- 91 1345 0 0 0 0 0 -1.379 -1.657 -150.004 150.020 0.140 1535 310 (K_S0) -91 1347 1347 1842 1843 0 0 0.579 2.247 4.592 5.169 0.498 1536 130 K_L0 91 1355 1355 0 0 0 0 0.036 -0.149 3.391 3.431 0.498 1537 310 (K_S0) -91 1365 1365 1844 1845 0 0 0.331 -0.293 -0.113 0.675 0.498 1538 310 (K_S0) -91 1428 1428 1846 1847 0 0 -0.549 0.318 449.764 449.765 0.498 1539 310 (K_S0) -91 1442 1442 1848 1849 0 0 0.000 -0.472 19.868 19.879 0.498 1540 130 K_L0 91 1466 1466 0 0 0 0 0.245 -0.452 0.810 1.081 0.498 1541 22 gamma 91 912 0 0 0 0 0 2.154 0.346 -14.403 14.568 0.000 1542 22 gamma 91 912 0 0 0 0 0 3.651 0.422 -23.816 24.098 0.000 1543 -421 (Dbar0) -91 918 0 1850 1852 0 0 -1.068 0.062 5.820 6.205 1.865 1544 22 gamma 91 918 0 0 0 0 0 -0.176 -0.081 0.322 0.376 0.000 1545 22 gamma 91 933 0 0 0 0 0 -1.038 1.018 -117.053 117.062 0.000 1546 22 gamma 91 933 0 0 0 0 0 -0.148 0.099 -17.341 17.342 0.000 1547 22 gamma 91 935 0 0 0 0 0 -0.329 0.178 -52.119 52.120 0.000 1548 22 gamma 91 935 0 0 0 0 0 -0.779 0.310 -94.788 94.792 0.000 1549 22 gamma 91 944 0 0 0 0 0 -0.076 0.194 60.666 60.666 0.000 1550 22 gamma 91 944 0 0 0 0 0 0.050 0.046 19.784 19.784 0.000 1551 22 gamma 91 950 0 0 0 0 0 -0.020 0.049 1.155 1.156 0.000 1552 22 gamma 91 950 0 0 0 0 0 0.013 0.029 0.054 0.063 0.000 1553 22 gamma 91 967 0 0 0 0 0 0.082 0.202 -0.113 0.245 0.000 1554 22 gamma 91 967 0 0 0 0 0 -0.041 0.075 -0.098 0.130 0.000 1555 211 pi+ 91 970 0 0 0 0 0 0.036 -0.279 -0.375 0.490 0.140 1556 -211 pi- 91 970 0 0 0 0 0 0.038 -0.009 0.037 0.150 0.140 1557 111 (pi0) -91 970 0 1853 1854 0 0 0.019 0.109 -0.406 0.442 0.135 1558 211 pi+ 91 992 0 0 0 0 0 0.082 -0.459 0.007 0.487 0.140 1559 -211 pi- 91 992 0 0 0 0 0 0.278 -0.379 0.182 0.524 0.140 1560 111 (pi0) -91 992 0 1855 1856 0 0 0.218 0.025 0.139 0.293 0.135 1561 22 gamma 91 993 0 0 0 0 0 0.217 -0.351 -0.276 0.496 0.000 1562 22 gamma 91 993 0 0 0 0 0 0.084 -0.077 -0.168 0.203 0.000 1563 22 gamma 91 994 0 0 0 0 0 0.089 -0.549 0.035 0.557 0.000 1564 22 gamma 91 994 0 0 0 0 0 0.007 -0.160 0.083 0.181 0.000 1565 22 gamma 91 995 0 0 0 0 0 0.047 0.240 0.154 0.289 0.000 1566 22 gamma 91 995 0 0 0 0 0 -0.002 0.009 0.081 0.082 0.000 1567 211 pi+ 91 1002 0 0 0 0 0 0.028 0.132 -1.034 1.052 0.140 1568 -211 pi- 91 1002 0 0 0 0 0 0.014 0.254 -0.755 0.809 0.140 1569 111 (pi0) -91 1002 0 1857 1858 0 0 -0.436 1.343 -4.083 4.322 0.135 1570 111 (pi0) -91 1008 0 1859 1860 0 0 0.519 0.014 -27.951 27.956 0.135 1571 22 gamma 91 1008 0 0 0 0 0 0.842 0.547 -22.547 22.569 0.000 1572 321 K+ 91 1043 0 0 0 0 0 0.298 0.040 -0.596 0.830 0.494 1573 -321 K- 91 1043 0 0 0 0 0 0.390 -0.195 -0.739 0.990 0.494 1574 22 gamma 91 1046 0 0 0 0 0 0.542 -0.073 0.014 0.547 0.000 1575 22 gamma 91 1046 0 0 0 0 0 0.661 -0.221 -0.058 0.699 0.000 1576 211 pi+ 91 1048 0 0 0 0 0 0.182 0.006 0.704 0.740 0.140 1577 -211 pi- 91 1048 0 0 0 0 0 -0.079 -0.455 0.732 0.877 0.140 1578 111 (pi0) -91 1048 0 1861 1862 0 0 -0.023 0.006 0.466 0.486 0.135 1579 22 gamma 91 1049 0 0 0 0 0 -1.509 0.235 1.967 2.490 0.000 1580 22 gamma 91 1049 0 0 0 0 0 -0.901 0.126 1.011 1.360 0.000 1581 111 (pi0) -91 1051 0 1863 1864 0 0 -0.510 0.145 0.676 0.870 0.135 1582 111 (pi0) -91 1051 0 1865 1866 0 0 -0.601 -0.123 0.741 0.971 0.135 1583 111 (pi0) -91 1051 0 1867 1868 0 0 -0.507 -0.103 0.655 0.846 0.135 1584 22 gamma 91 1054 0 0 0 0 0 0.014 0.045 0.187 0.193 0.000 1585 22 gamma 91 1054 0 0 0 0 0 -0.057 -0.064 0.782 0.787 0.000 1586 22 gamma 91 1056 0 0 0 0 0 -0.494 -0.373 0.476 0.781 0.000 1587 22 gamma 91 1056 0 0 0 0 0 -0.223 -0.073 0.220 0.322 0.000 1588 22 gamma 91 1057 0 0 0 0 0 -0.270 -1.165 1.896 2.241 0.000 1589 22 gamma 91 1057 0 0 0 0 0 -0.185 -1.401 2.341 2.734 0.000 1590 211 pi+ 91 1061 0 0 0 0 0 -0.593 -0.294 1.572 1.711 0.140 1591 -211 pi- 91 1061 0 0 0 0 0 -0.604 -0.411 0.752 1.058 0.140 1592 111 (pi0) -91 1061 0 1869 1870 0 0 -0.092 -0.137 0.462 0.509 0.135 1593 22 gamma 91 1069 0 0 0 0 0 -1.573 -0.114 2.327 2.811 0.000 1594 22 gamma 91 1069 0 0 0 0 0 -0.622 0.033 0.860 1.062 0.000 1595 22 gamma 91 1070 0 0 0 0 0 -0.385 -0.098 0.564 0.690 0.000 1596 22 gamma 91 1070 0 0 0 0 0 -0.072 -0.041 0.252 0.265 0.000 1597 211 pi+ 91 1078 0 0 0 0 0 -0.221 0.551 -0.053 0.612 0.140 1598 -211 pi- 91 1078 0 0 0 0 0 -0.682 1.317 -0.563 1.592 0.140 1599 111 (pi0) -91 1078 0 1871 1872 0 0 -0.521 1.175 -0.825 1.534 0.135 1600 321 K+ 91 1081 0 0 0 0 0 -6.230 9.369 -4.976 12.313 0.494 1601 -321 K- 91 1081 0 0 0 0 0 -9.372 13.923 -7.620 18.439 0.494 1602 22 gamma 91 1090 0 0 0 0 0 0.133 -0.158 0.581 0.616 0.000 1603 22 gamma 91 1090 0 0 0 0 0 0.049 -0.109 0.756 0.765 0.000 1604 211 pi+ 91 1091 0 0 0 0 0 -0.126 0.167 4.514 4.521 0.140 1605 -211 pi- 91 1091 0 0 0 0 0 0.074 -0.050 0.962 0.976 0.140 1606 111 (pi0) -91 1091 0 1873 1874 0 0 -0.407 -0.047 5.437 5.454 0.135 1607 211 pi+ 91 1094 0 0 0 0 0 0.320 0.093 -0.774 0.854 0.140 1608 -211 pi- 91 1094 0 0 0 0 0 -0.118 0.009 -0.409 0.448 0.140 1609 111 (pi0) -91 1094 0 1875 1876 0 0 0.065 0.066 -0.126 0.206 0.135 1610 22 gamma 91 1112 0 0 0 0 0 -0.400 -0.122 20.427 20.431 0.000 1611 22 gamma 91 1112 0 0 0 0 0 0.139 0.108 13.681 13.682 0.000 1612 211 pi+ 91 1114 0 0 0 0 0 0.072 -0.124 1.570 1.583 0.140 1613 -211 pi- 91 1114 0 0 0 0 0 0.047 0.014 1.789 1.795 0.140 1614 111 (pi0) -91 1114 0 1877 1878 0 0 0.326 0.409 2.509 2.566 0.135 1615 2212 p+ 91 1115 0 0 0 0 0 -0.649 -0.393 2.526 2.800 0.938 1616 -211 pi- 91 1115 0 0 0 0 0 -0.065 0.049 0.339 0.376 0.140 1617 -2112 nbar0 91 1117 0 0 0 0 0 -0.113 -0.096 -0.372 1.021 0.940 1618 211 pi+ 91 1117 0 0 0 0 0 -0.238 0.081 -0.206 0.354 0.140 1619 211 pi+ 91 1119 0 0 0 0 0 0.233 0.050 -0.525 0.593 0.140 1620 -211 pi- 91 1119 0 0 0 0 0 0.015 0.200 -0.088 0.260 0.140 1621 111 (pi0) -91 1119 0 1879 1880 0 0 -0.021 -0.166 -0.173 0.276 0.135 1622 111 (pi0) -91 1122 0 1881 1882 0 0 -0.163 0.048 -1.064 1.085 0.135 1623 22 gamma 91 1122 0 0 0 0 0 0.489 -0.688 -4.030 4.118 0.000 1624 22 gamma 91 1129 0 0 0 0 0 0.013 -0.055 -0.004 0.056 0.000 1625 22 gamma 91 1129 0 0 0 0 0 -0.224 -0.261 0.100 0.358 0.000 1626 22 gamma 91 1131 0 0 0 0 0 -0.014 0.022 0.170 0.172 0.000 1627 22 gamma 91 1131 0 0 0 0 0 -0.070 0.046 0.022 0.087 0.000 1628 22 gamma 91 1136 0 0 0 0 0 -0.287 0.081 0.326 0.442 0.000 1629 22 gamma 91 1136 0 0 0 0 0 -0.696 0.290 0.563 0.941 0.000 1630 22 gamma 91 1137 0 0 0 0 0 0.046 -0.045 0.101 0.120 0.000 1631 22 gamma 91 1137 0 0 0 0 0 -0.044 -0.015 -0.017 0.050 0.000 1632 22 gamma 91 1139 0 0 0 0 0 0.082 0.081 0.233 0.260 0.000 1633 22 gamma 91 1139 0 0 0 0 0 0.040 0.093 0.034 0.107 0.000 1634 22 gamma 91 1143 0 0 0 0 0 0.068 0.368 6.880 6.891 0.000 1635 22 gamma 91 1143 0 0 0 0 0 0.109 0.119 19.327 19.328 0.000 1636 22 gamma 91 1146 0 0 0 0 0 -0.122 0.041 45.087 45.087 0.000 1637 22 gamma 91 1146 0 0 0 0 0 -0.212 -0.071 48.999 49.000 0.000 1638 22 gamma 91 1153 0 0 0 0 0 -0.833 0.263 -108.355 108.359 0.000 1639 22 gamma 91 1153 0 0 0 0 0 -0.646 0.202 -70.489 70.493 0.000 1640 211 pi+ 91 1154 0 0 0 0 0 0.025 0.060 -11.422 11.423 0.140 1641 -211 pi- 91 1154 0 0 0 0 0 0.013 -0.322 -34.475 34.477 0.140 1642 111 (pi0) -91 1154 0 1883 1884 0 0 -0.193 -0.594 -83.857 83.859 0.135 1643 211 pi+ 91 1157 0 0 0 0 0 -0.096 0.225 -53.734 53.735 0.140 1644 -211 pi- 91 1157 0 0 0 0 0 -0.205 0.050 -73.863 73.864 0.140 1645 111 (pi0) -91 1157 0 1885 1886 0 0 -0.166 0.251 -52.705 52.706 0.135 1646 22 gamma 91 1158 0 0 0 0 0 -0.112 -0.063 -16.422 16.422 0.000 1647 22 gamma 91 1158 0 0 0 0 0 -0.268 -0.374 -41.637 41.640 0.000 1648 211 pi+ 91 1163 0 0 0 0 0 -0.240 0.035 -0.161 0.323 0.140 1649 -211 pi- 91 1163 0 0 0 0 0 0.389 -0.027 -1.042 1.121 0.140 1650 22 gamma 91 1164 0 0 0 0 0 -0.248 -0.550 0.571 0.831 0.000 1651 22 gamma 91 1164 0 0 0 0 0 0.004 -0.046 0.010 0.047 0.000 1652 211 pi+ 91 1171 0 0 0 0 0 -0.718 0.585 -195.959 195.962 0.140 1653 -211 pi- 91 1171 0 0 0 0 0 -0.228 0.252 -49.800 49.802 0.140 1654 111 (pi0) -91 1171 0 1887 1888 0 0 -1.403 1.044 -251.251 251.257 0.135 1655 421 (D0) -91 1196 0 1889 1891 0 0 3.547 -9.697 10.264 14.678 1.865 1656 111 (pi0) -91 1196 0 1892 1893 0 0 0.172 -0.521 0.554 0.792 0.135 1657 22 gamma 91 1197 0 0 0 0 0 0.124 -0.317 0.145 0.370 0.000 1658 22 gamma 91 1197 0 0 0 0 0 0.212 -0.223 0.077 0.317 0.000 1659 211 pi+ 91 1202 0 0 0 0 0 0.135 -0.138 -0.333 0.410 0.140 1660 -211 pi- 91 1202 0 0 0 0 0 -0.192 -0.094 -0.105 0.276 0.140 1661 111 (pi0) -91 1202 0 1894 1895 0 0 0.018 0.094 0.080 0.184 0.135 1662 22 gamma 91 1205 0 0 0 0 0 0.013 0.021 -0.115 0.118 0.000 1663 22 gamma 91 1205 0 0 0 0 0 0.617 -0.044 -3.839 3.889 0.000 1664 111 (pi0) -91 1206 0 1896 1897 0 0 -0.107 -0.024 -2.079 2.086 0.135 1665 111 (pi0) -91 1206 0 1898 1899 0 0 -0.117 0.085 -1.203 1.219 0.135 1666 111 (pi0) -91 1206 0 1900 1901 0 0 0.049 0.167 -1.371 1.389 0.135 1667 211 pi+ 91 1209 0 0 0 0 0 -0.046 -0.042 -3.724 3.727 0.140 1668 -211 pi- 91 1209 0 0 0 0 0 0.016 -0.039 -6.348 6.350 0.140 1669 22 gamma 91 1209 0 0 0 0 0 -0.205 0.088 -2.755 2.764 0.000 1670 22 gamma 91 1210 0 0 0 0 0 -0.608 0.469 -86.171 86.175 0.000 1671 22 gamma 91 1210 0 0 0 0 0 -0.078 0.008 -9.503 9.504 0.000 1672 111 (pi0) -91 1213 0 1902 1903 0 0 -0.039 0.360 -80.690 80.691 0.135 1673 22 gamma 91 1213 0 0 0 0 0 -0.450 0.457 -37.064 37.069 0.000 1674 22 gamma 91 1214 0 0 0 0 0 -0.632 0.502 -89.605 89.609 0.000 1675 22 gamma 91 1214 0 0 0 0 0 -0.019 0.005 -0.830 0.830 0.000 1676 22 gamma 91 1231 0 0 0 0 0 0.359 0.110 -65.561 65.562 0.000 1677 22 gamma 91 1231 0 0 0 0 0 0.138 0.024 -13.910 13.911 0.000 1678 211 pi+ 91 1233 0 0 0 0 0 0.289 -0.245 -56.813 56.814 0.140 1679 -211 pi- 91 1233 0 0 0 0 0 0.251 0.092 -68.519 68.520 0.140 1680 111 (pi0) -91 1233 0 1904 1905 0 0 1.021 -0.320 -193.454 193.457 0.135 1681 22 gamma 91 1235 0 0 0 0 0 0.168 -0.008 -26.855 26.855 0.000 1682 22 gamma 91 1235 0 0 0 0 0 0.579 -0.235 -78.169 78.171 0.000 1683 22 gamma 91 1236 0 0 0 0 0 0.460 -0.337 -70.656 70.659 0.000 1684 22 gamma 91 1236 0 0 0 0 0 0.004 0.011 -2.325 2.325 0.000 1685 22 gamma 91 1249 0 0 0 0 0 0.065 0.036 -0.053 0.091 0.000 1686 22 gamma 91 1249 0 0 0 0 0 0.639 0.434 -0.087 0.777 0.000 1687 22 gamma 91 1250 0 0 0 0 0 -0.562 0.358 6.906 6.938 0.000 1688 22 gamma 91 1250 0 0 0 0 0 -0.138 0.045 1.059 1.069 0.000 1689 211 pi+ 91 1254 0 0 0 0 0 0.280 0.110 3.982 3.995 0.140 1690 -211 pi- 91 1254 0 0 0 0 0 0.510 0.230 12.254 12.268 0.140 1691 111 (pi0) -91 1254 0 1906 1907 0 0 -0.025 -0.020 0.909 0.920 0.135 1692 22 gamma 91 1256 0 0 0 0 0 0.046 -0.019 0.046 0.068 0.000 1693 22 gamma 91 1256 0 0 0 0 0 1.256 0.101 9.210 9.296 0.000 1694 111 (pi0) -91 1258 0 1908 1909 0 0 0.512 -0.050 1.391 1.489 0.135 1695 111 (pi0) -91 1258 0 1910 1911 0 0 1.508 -0.377 3.818 4.125 0.135 1696 111 (pi0) -91 1258 0 1912 1913 0 0 1.559 -0.153 4.180 4.467 0.135 1697 22 gamma 91 1286 0 0 0 0 0 0.495 -0.850 -18.367 18.393 0.000 1698 22 gamma 91 1286 0 0 0 0 0 0.644 -0.982 -36.207 36.226 0.000 1699 211 pi+ 91 1297 0 0 0 0 0 0.181 0.195 0.236 0.382 0.140 1700 -211 pi- 91 1297 0 0 0 0 0 0.617 0.049 0.539 0.833 0.140 1701 111 (pi0) -91 1297 0 1914 1915 0 0 0.420 -0.168 0.786 0.917 0.135 1702 22 gamma 91 1298 0 0 0 0 0 -0.044 0.104 -0.059 0.128 0.000 1703 22 gamma 91 1298 0 0 0 0 0 0.556 0.055 0.540 0.777 0.000 1704 22 gamma 91 1305 0 0 0 0 0 -0.112 -0.202 0.391 0.454 0.000 1705 22 gamma 91 1305 0 0 0 0 0 -0.079 -0.576 0.952 1.116 0.000 1706 2112 n0 91 1306 0 0 0 0 0 -1.062 0.023 6.175 6.336 0.940 1707 -211 pi- 91 1306 0 0 0 0 0 -0.117 -0.118 0.448 0.498 0.140 1708 211 pi+ 91 1310 0 0 0 0 0 -0.075 -0.256 1.972 1.995 0.140 1709 -211 pi- 91 1310 0 0 0 0 0 -0.030 -0.143 7.476 7.479 0.140 1710 111 (pi0) -91 1310 0 1916 1917 0 0 -0.220 -0.355 7.066 7.080 0.135 1711 211 pi+ 91 1315 0 0 0 0 0 0.160 0.086 45.304 45.305 0.140 1712 -211 pi- 91 1315 0 0 0 0 0 -0.057 0.008 11.356 11.357 0.140 1713 111 (pi0) -91 1315 0 1918 1919 0 0 0.019 0.044 12.107 12.108 0.135 1714 22 gamma 91 1316 0 0 0 0 0 0.128 0.155 17.342 17.343 0.000 1715 22 gamma 91 1316 0 0 0 0 0 0.042 0.299 25.525 25.527 0.000 1716 22 gamma 91 1318 0 0 0 0 0 0.252 0.011 18.168 18.170 0.000 1717 22 gamma 91 1318 0 0 0 0 0 0.295 -0.042 33.776 33.777 0.000 1718 22 gamma 91 1321 0 0 0 0 0 0.195 -0.079 30.975 30.976 0.000 1719 22 gamma 91 1321 0 0 0 0 0 -0.015 0.004 7.704 7.704 0.000 1720 111 (pi0) -91 1322 0 1920 1921 0 0 0.048 0.178 75.140 75.140 0.135 1721 111 (pi0) -91 1322 0 1922 1923 0 0 -0.004 0.152 21.835 21.836 0.135 1722 111 (pi0) -91 1322 0 1924 1925 0 0 0.071 0.328 76.494 76.495 0.135 1723 22 gamma 91 1336 0 0 0 0 0 0.109 0.043 0.720 0.730 0.000 1724 22 gamma 91 1336 0 0 0 0 0 0.060 -0.051 0.186 0.202 0.000 1725 211 pi+ 91 1337 0 0 0 0 0 -0.105 0.088 0.489 0.526 0.140 1726 -211 pi- 91 1337 0 0 0 0 0 0.183 0.070 1.982 1.996 0.140 1727 111 (pi0) -91 1337 0 1926 1927 0 0 -0.088 0.147 2.594 2.603 0.135 1728 22 gamma 91 1339 0 0 0 0 0 -0.210 0.137 0.172 0.304 0.000 1729 22 gamma 91 1339 0 0 0 0 0 0.325 0.015 0.328 0.461 0.000 1730 22 gamma 91 1341 0 0 0 0 0 -0.047 -0.184 0.098 0.214 0.000 1731 22 gamma 91 1341 0 0 0 0 0 -0.126 -0.069 0.106 0.178 0.000 1732 22 gamma 91 1343 0 0 0 0 0 0.058 0.393 -3.431 3.454 0.000 1733 22 gamma 91 1343 0 0 0 0 0 0.417 0.411 -1.996 2.080 0.000 1734 22 gamma 91 1356 0 0 0 0 0 0.144 0.318 1.864 1.897 0.000 1735 22 gamma 91 1356 0 0 0 0 0 0.013 0.002 0.011 0.017 0.000 1736 22 gamma 91 1358 0 0 0 0 0 0.488 0.885 4.574 4.685 0.000 1737 22 gamma 91 1358 0 0 0 0 0 0.333 0.421 2.242 2.305 0.000 1738 22 gamma 91 1362 0 0 0 0 0 16.154 -5.018 -15.819 23.160 0.000 1739 22 gamma 91 1362 0 0 0 0 0 0.852 -0.246 -0.796 1.191 0.000 1740 22 gamma 91 1364 0 0 0 0 0 1.441 -0.409 -0.958 1.778 0.000 1741 22 gamma 91 1364 0 0 0 0 0 0.955 -0.216 -0.742 1.229 0.000 1742 22 gamma 91 1366 0 0 0 0 0 0.014 -0.004 0.011 0.019 0.000 1743 22 gamma 91 1366 0 0 0 0 0 1.012 -0.825 -0.191 1.320 0.000 1744 22 gamma 91 1368 0 0 0 0 0 0.116 -0.015 0.023 0.120 0.000 1745 22 gamma 91 1368 0 0 0 0 0 0.103 0.018 -0.111 0.152 0.000 1746 22 gamma 91 1370 0 0 0 0 0 0.079 -0.469 -0.033 0.477 0.000 1747 22 gamma 91 1370 0 0 0 0 0 0.110 -0.430 -0.159 0.472 0.000 1748 22 gamma 91 1374 0 0 0 0 0 -0.104 0.012 -0.167 0.198 0.000 1749 22 gamma 91 1374 0 0 0 0 0 -1.661 -0.297 -3.150 3.573 0.000 1750 22 gamma 91 1378 0 0 0 0 0 0.091 -0.087 -0.571 0.585 0.000 1751 22 gamma 91 1378 0 0 0 0 0 0.020 -0.045 -0.038 0.063 0.000 1752 22 gamma 91 1380 0 0 0 0 0 -0.023 0.041 0.017 0.050 0.000 1753 22 gamma 91 1380 0 0 0 0 0 0.039 -0.011 -0.111 0.118 0.000 1754 22 gamma 91 1384 0 0 0 0 0 0.016 -0.035 -0.091 0.099 0.000 1755 22 gamma 91 1384 0 0 0 0 0 0.143 0.039 -1.185 1.194 0.000 1756 22 gamma 91 1386 0 0 0 0 0 0.039 0.026 -0.483 0.485 0.000 1757 22 gamma 91 1386 0 0 0 0 0 -0.097 0.152 -1.182 1.196 0.000 1758 22 gamma 91 1394 0 0 0 0 0 0.883 0.088 -2.915 3.047 0.000 1759 22 gamma 91 1394 0 0 0 0 0 -0.004 0.001 -0.003 0.005 0.000 1760 22 gamma 91 1397 0 0 0 0 0 0.875 -0.868 -1.179 1.706 0.000 1761 22 gamma 91 1397 0 0 0 0 0 0.484 -0.362 -0.518 0.796 0.000 1762 22 gamma 91 1399 0 0 0 0 0 -0.287 -0.213 -0.030 0.358 0.000 1763 22 gamma 91 1399 0 0 0 0 0 -0.025 -0.094 0.020 0.100 0.000 1764 22 gamma 91 1401 0 0 0 0 0 -0.502 0.115 0.799 0.950 0.000 1765 22 gamma 91 1401 0 0 0 0 0 -0.649 0.031 1.203 1.367 0.000 1766 2112 n0 91 1407 0 0 0 0 0 0.248 -2.083 2.864 3.672 0.940 1767 111 (pi0) -91 1407 0 1928 1929 0 0 -0.045 -0.552 0.718 0.917 0.135 1768 22 gamma 91 1408 0 0 0 0 0 0.089 -0.465 0.635 0.793 0.000 1769 22 gamma 91 1408 0 0 0 0 0 -0.011 -0.766 0.909 1.189 0.000 1770 22 gamma 91 1410 0 0 0 0 0 -0.174 -0.089 0.176 0.263 0.000 1771 22 gamma 91 1410 0 0 0 0 0 -0.512 -0.343 0.908 1.097 0.000 1772 22 gamma 91 1412 0 0 0 0 0 -1.417 -0.471 2.716 3.099 0.000 1773 22 gamma 91 1412 0 0 0 0 0 -0.692 -0.324 1.318 1.523 0.000 1774 22 gamma 91 1415 0 0 0 0 0 -2.502 -0.988 3.909 4.746 0.000 1775 22 gamma 91 1415 0 0 0 0 0 -0.328 -0.112 0.428 0.551 0.000 1776 22 gamma 91 1417 0 0 0 0 0 -0.490 -0.187 1.031 1.157 0.000 1777 22 gamma 91 1417 0 0 0 0 0 -0.656 -0.191 1.056 1.258 0.000 1778 22 gamma 91 1419 0 0 0 0 0 -0.066 -0.032 0.050 0.089 0.000 1779 22 gamma 91 1419 0 0 0 0 0 -0.088 0.068 0.285 0.305 0.000 1780 22 gamma 91 1421 0 0 0 0 0 0.042 -0.048 0.023 0.068 0.000 1781 22 gamma 91 1421 0 0 0 0 0 -0.057 -0.050 -0.076 0.108 0.000 1782 22 gamma 91 1425 0 0 0 0 0 -0.293 0.017 -0.042 0.297 0.000 1783 22 gamma 91 1425 0 0 0 0 0 -0.848 0.139 -0.345 0.926 0.000 1784 22 gamma 91 1437 0 0 0 0 0 0.026 0.247 0.158 0.294 0.000 1785 22 gamma 91 1437 0 0 0 0 0 -0.052 0.094 0.153 0.187 0.000 1786 22 gamma 91 1441 0 0 0 0 0 -0.074 -0.018 -0.014 0.078 0.000 1787 22 gamma 91 1441 0 0 0 0 0 -0.122 0.126 0.076 0.191 0.000 1788 22 gamma 91 1448 0 0 0 0 0 0.094 0.169 -8.390 8.392 0.000 1789 22 gamma 91 1448 0 0 0 0 0 0.140 0.072 -11.362 11.364 0.000 1790 22 gamma 91 1450 0 0 0 0 0 0.334 0.238 -3.459 3.484 0.000 1791 22 gamma 91 1450 0 0 0 0 0 0.159 0.072 -2.346 2.353 0.000 1792 22 gamma 91 1454 0 0 0 0 0 0.041 0.182 -0.912 0.931 0.000 1793 22 gamma 91 1454 0 0 0 0 0 -0.080 0.095 -0.621 0.633 0.000 1794 22 gamma 91 1456 0 0 0 0 0 0.002 0.152 -0.711 0.727 0.000 1795 22 gamma 91 1456 0 0 0 0 0 0.060 0.057 -0.150 0.172 0.000 1796 22 gamma 91 1458 0 0 0 0 0 0.117 0.134 -0.651 0.675 0.000 1797 22 gamma 91 1458 0 0 0 0 0 -0.012 0.047 -0.522 0.524 0.000 1798 211 pi+ 91 1463 0 0 0 0 0 0.877 -0.413 5.277 5.367 0.140 1799 -211 pi- 91 1463 0 0 0 0 0 0.253 -0.407 2.305 2.359 0.140 1800 22 gamma 91 1465 0 0 0 0 0 -0.007 0.040 1.027 1.027 0.000 1801 22 gamma 91 1465 0 0 0 0 0 0.092 0.013 0.513 0.521 0.000 1802 211 pi+ 91 1468 0 0 0 0 0 0.012 -0.424 -0.086 0.455 0.140 1803 -211 pi- 91 1468 0 0 0 0 0 0.007 -0.093 0.218 0.275 0.140 1804 22 gamma 91 1470 0 0 0 0 0 0.114 0.148 -0.091 0.208 0.000 1805 22 gamma 91 1470 0 0 0 0 0 0.229 0.076 -0.187 0.305 0.000 1806 22 gamma 91 1472 0 0 0 0 0 0.005 0.004 -0.017 0.018 0.000 1807 22 gamma 91 1472 0 0 0 0 0 0.117 -0.246 0.170 0.321 0.000 1808 22 gamma 91 1476 0 0 0 0 0 -0.449 0.634 -49.587 49.593 0.000 1809 22 gamma 91 1476 0 0 0 0 0 -0.212 0.178 -20.261 20.263 0.000 1810 22 gamma 91 1478 0 0 0 0 0 0.117 0.086 -4.258 4.261 0.000 1811 22 gamma 91 1478 0 0 0 0 0 0.093 0.013 -7.532 7.532 0.000 1812 22 gamma 91 1482 0 0 0 0 0 0.252 -0.590 -147.798 147.799 0.000 1813 22 gamma 91 1482 0 0 0 0 0 0.158 -0.168 -51.832 51.833 0.000 1814 211 pi+ 91 1484 0 0 0 0 0 0.054 -0.022 -2.763 2.767 0.140 1815 -211 pi- 91 1484 0 0 0 0 0 0.013 -0.555 -23.702 23.709 0.140 1816 22 gamma 91 1487 0 0 0 0 0 0.121 0.214 -1.914 1.930 0.000 1817 22 gamma 91 1487 0 0 0 0 0 0.125 0.084 -0.688 0.704 0.000 1818 22 gamma 91 1489 0 0 0 0 0 0.035 0.140 -4.216 4.218 0.000 1819 22 gamma 91 1489 0 0 0 0 0 0.122 0.057 -6.124 6.125 0.000 1820 22 gamma 91 1495 0 0 0 0 0 0.005 0.313 0.628 0.702 0.000 1821 22 gamma 91 1495 0 0 0 0 0 0.012 0.052 0.300 0.305 0.000 1822 111 (pi0) -91 1498 0 1930 1931 0 0 -0.223 -0.048 -4.383 4.391 0.135 1823 111 (pi0) -91 1498 0 1932 1933 0 0 -0.930 -0.451 -32.710 32.726 0.135 1824 22 gamma 91 1500 0 0 0 0 0 0.508 -0.155 -7.152 7.172 0.000 1825 22 gamma 91 1500 0 0 0 0 0 0.532 -0.064 -8.647 8.664 0.000 1826 211 pi+ 91 1504 0 0 0 0 0 0.353 -0.144 -0.412 0.578 0.140 1827 -211 pi- 91 1504 0 0 0 0 0 -0.029 -0.007 0.027 0.145 0.140 1828 22 gamma 91 1508 0 0 0 0 0 -0.053 0.036 0.030 0.071 0.000 1829 22 gamma 91 1508 0 0 0 0 0 -0.024 0.051 0.293 0.298 0.000 1830 22 gamma 91 1510 0 0 0 0 0 0.234 0.119 1.071 1.103 0.000 1831 22 gamma 91 1510 0 0 0 0 0 0.440 0.108 2.559 2.598 0.000 1832 -2212 pbar- 91 1517 0 0 0 0 0 -0.085 -0.556 9.023 9.089 0.938 1833 211 pi+ 91 1517 0 0 0 0 0 -0.104 -0.205 2.048 2.065 0.140 1834 22 gamma 91 1520 0 0 0 0 0 0.005 0.063 0.346 0.352 0.000 1835 22 gamma 91 1520 0 0 0 0 0 0.199 0.134 0.665 0.707 0.000 1836 22 gamma 91 1522 0 0 0 0 0 0.708 0.104 126.542 126.544 0.000 1837 22 gamma 91 1522 0 0 0 0 0 0.177 0.087 41.700 41.700 0.000 1838 22 gamma 91 1524 0 0 0 0 0 -0.006 0.016 0.895 0.895 0.000 1839 22 gamma 91 1524 0 0 0 0 0 -0.120 0.078 70.272 70.272 0.000 1840 22 gamma 91 1530 0 0 0 0 0 0.181 -0.024 0.960 0.977 0.000 1841 22 gamma 91 1530 0 0 0 0 0 0.062 0.079 0.466 0.477 0.000 1842 211 pi+ 91 1535 0 0 0 0 0 0.257 1.408 2.432 2.826 0.140 1843 -211 pi- 91 1535 0 0 0 0 0 0.322 0.839 2.160 2.344 0.140 1844 211 pi+ 91 1537 0 0 0 0 0 0.047 -0.125 0.138 0.238 0.140 1845 -211 pi- 91 1537 0 0 0 0 0 0.284 -0.168 -0.251 0.438 0.140 1846 111 (pi0) -91 1538 0 1934 1935 0 0 -0.367 0.056 325.610 325.610 0.135 1847 111 (pi0) -91 1538 0 1936 1937 0 0 -0.181 0.262 124.154 124.155 0.135 1848 111 (pi0) -91 1539 0 1938 1939 0 0 -0.182 -0.378 12.524 12.531 0.135 1849 111 (pi0) -91 1539 0 1940 1941 0 0 0.182 -0.095 7.344 7.348 0.135 1850 321 K+ 91 1543 0 0 0 0 0 0.158 0.549 2.013 2.150 0.494 1851 -211 pi- 91 1543 0 0 0 0 0 -0.539 -0.200 1.175 1.316 0.140 1852 111 (pi0) -91 1543 0 1942 1943 0 0 -0.687 -0.287 2.632 2.738 0.135 1853 22 gamma 91 1557 0 0 0 0 0 0.028 -0.021 -0.038 0.052 0.000 1854 22 gamma 91 1557 0 0 0 0 0 -0.009 0.130 -0.368 0.390 0.000 1855 22 gamma 91 1560 0 0 0 0 0 0.195 0.053 0.068 0.213 0.000 1856 22 gamma 91 1560 0 0 0 0 0 0.024 -0.028 0.071 0.080 0.000 1857 22 gamma 91 1569 0 0 0 0 0 -0.370 1.249 -3.709 3.931 0.000 1858 22 gamma 91 1569 0 0 0 0 0 -0.066 0.094 -0.374 0.391 0.000 1859 22 gamma 91 1570 0 0 0 0 0 0.295 0.064 -13.951 13.954 0.000 1860 22 gamma 91 1570 0 0 0 0 0 0.224 -0.050 -14.000 14.002 0.000 1861 22 gamma 91 1578 0 0 0 0 0 -0.020 -0.015 0.007 0.026 0.000 1862 22 gamma 91 1578 0 0 0 0 0 -0.003 0.020 0.460 0.460 0.000 1863 22 gamma 91 1581 0 0 0 0 0 -0.305 0.153 0.444 0.560 0.000 1864 22 gamma 91 1581 0 0 0 0 0 -0.206 -0.008 0.232 0.310 0.000 1865 22 gamma 91 1582 0 0 0 0 0 -0.563 -0.081 0.698 0.900 0.000 1866 22 gamma 91 1582 0 0 0 0 0 -0.038 -0.042 0.044 0.071 0.000 1867 22 gamma 91 1583 0 0 0 0 0 0.000 -0.021 0.025 0.033 0.000 1868 22 gamma 91 1583 0 0 0 0 0 -0.507 -0.083 0.630 0.813 0.000 1869 22 gamma 91 1592 0 0 0 0 0 -0.030 0.024 0.063 0.074 0.000 1870 22 gamma 91 1592 0 0 0 0 0 -0.062 -0.161 0.399 0.435 0.000 1871 22 gamma 91 1599 0 0 0 0 0 -0.401 0.913 -0.704 1.221 0.000 1872 22 gamma 91 1599 0 0 0 0 0 -0.120 0.262 -0.121 0.313 0.000 1873 22 gamma 91 1606 0 0 0 0 0 -0.208 -0.092 2.929 2.938 0.000 1874 22 gamma 91 1606 0 0 0 0 0 -0.198 0.045 2.508 2.517 0.000 1875 22 gamma 91 1609 0 0 0 0 0 0.003 0.083 -0.113 0.141 0.000 1876 22 gamma 91 1609 0 0 0 0 0 0.062 -0.017 -0.012 0.066 0.000 1877 22 gamma 91 1614 0 0 0 0 0 -0.010 0.019 0.179 0.180 0.000 1878 22 gamma 91 1614 0 0 0 0 0 0.336 0.391 2.330 2.386 0.000 1879 22 gamma 91 1621 0 0 0 0 0 -0.070 -0.068 -0.119 0.153 0.000 1880 22 gamma 91 1621 0 0 0 0 0 0.049 -0.099 -0.054 0.123 0.000 1881 22 gamma 91 1622 0 0 0 0 0 -0.026 -0.030 -0.461 0.463 0.000 1882 22 gamma 91 1622 0 0 0 0 0 -0.137 0.078 -0.602 0.623 0.000 1883 22 gamma 91 1642 0 0 0 0 0 -0.029 -0.157 -29.468 29.469 0.000 1884 22 gamma 91 1642 0 0 0 0 0 -0.164 -0.437 -54.388 54.390 0.000 1885 22 gamma 91 1645 0 0 0 0 0 -0.021 -0.016 -4.163 4.163 0.000 1886 22 gamma 91 1645 0 0 0 0 0 -0.145 0.267 -48.542 48.543 0.000 1887 22 gamma 91 1654 0 0 0 0 0 -0.175 0.136 -25.935 25.936 0.000 1888 22 gamma 91 1654 0 0 0 0 0 -1.229 0.908 -225.316 225.321 0.000 1889 -321 K- 91 1655 0 0 0 0 0 0.128 -1.041 1.065 1.574 0.494 1890 211 pi+ 91 1655 0 0 0 0 0 2.953 -7.017 7.293 10.544 0.140 1891 111 (pi0) -91 1655 0 1944 1945 0 0 0.465 -1.639 1.906 2.560 0.135 1892 22 gamma 91 1656 0 0 0 0 0 0.105 -0.380 0.310 0.501 0.000 1893 22 gamma 91 1656 0 0 0 0 0 0.067 -0.141 0.245 0.290 0.000 1894 22 gamma 91 1661 0 0 0 0 0 -0.046 0.062 0.081 0.112 0.000 1895 22 gamma 91 1661 0 0 0 0 0 0.065 0.032 -0.001 0.072 0.000 1896 22 gamma 91 1664 0 0 0 0 0 -0.052 -0.030 -0.279 0.285 0.000 1897 22 gamma 91 1664 0 0 0 0 0 -0.055 0.006 -1.800 1.801 0.000 1898 22 gamma 91 1665 0 0 0 0 0 0.026 0.036 -0.195 0.200 0.000 1899 22 gamma 91 1665 0 0 0 0 0 -0.143 0.049 -1.008 1.019 0.000 1900 22 gamma 91 1666 0 0 0 0 0 0.054 0.004 -0.250 0.256 0.000 1901 22 gamma 91 1666 0 0 0 0 0 -0.005 0.163 -1.121 1.133 0.000 1902 22 gamma 91 1672 0 0 0 0 0 0.050 0.117 -25.138 25.139 0.000 1903 22 gamma 91 1672 0 0 0 0 0 -0.089 0.243 -55.552 55.552 0.000 1904 22 gamma 91 1680 0 0 0 0 0 0.501 -0.195 -107.325 107.326 0.000 1905 22 gamma 91 1680 0 0 0 0 0 0.519 -0.125 -86.129 86.130 0.000 1906 22 gamma 91 1691 0 0 0 0 0 0.016 -0.064 0.664 0.667 0.000 1907 22 gamma 91 1691 0 0 0 0 0 -0.041 0.044 0.245 0.253 0.000 1908 22 gamma 91 1694 0 0 0 0 0 0.350 0.030 0.921 0.986 0.000 1909 22 gamma 91 1694 0 0 0 0 0 0.163 -0.080 0.470 0.503 0.000 1910 22 gamma 91 1695 0 0 0 0 0 0.012 -0.017 0.063 0.067 0.000 1911 22 gamma 91 1695 0 0 0 0 0 1.497 -0.360 3.755 4.058 0.000 1912 22 gamma 91 1696 0 0 0 0 0 1.447 -0.170 3.932 4.194 0.000 1913 22 gamma 91 1696 0 0 0 0 0 0.112 0.017 0.248 0.273 0.000 1914 22 gamma 91 1701 0 0 0 0 0 0.010 -0.038 0.095 0.103 0.000 1915 22 gamma 91 1701 0 0 0 0 0 0.410 -0.129 0.691 0.814 0.000 1916 22 gamma 91 1710 0 0 0 0 0 -0.033 -0.180 3.017 3.023 0.000 1917 22 gamma 91 1710 0 0 0 0 0 -0.187 -0.176 4.049 4.057 0.000 1918 22 gamma 91 1713 0 0 0 0 0 0.044 0.082 9.476 9.477 0.000 1919 22 gamma 91 1713 0 0 0 0 0 -0.025 -0.038 2.631 2.631 0.000 1920 22 gamma 91 1720 0 0 0 0 0 0.044 0.051 10.311 10.311 0.000 1921 22 gamma 91 1720 0 0 0 0 0 0.004 0.126 64.828 64.829 0.000 1922 22 gamma 91 1721 0 0 0 0 0 0.014 0.071 17.463 17.463 0.000 1923 22 gamma 91 1721 0 0 0 0 0 -0.018 0.082 4.372 4.373 0.000 1924 22 gamma 91 1722 0 0 0 0 0 -0.037 0.096 18.032 18.032 0.000 1925 22 gamma 91 1722 0 0 0 0 0 0.108 0.232 58.463 58.463 0.000 1926 22 gamma 91 1727 0 0 0 0 0 -0.102 0.128 2.523 2.528 0.000 1927 22 gamma 91 1727 0 0 0 0 0 0.014 0.019 0.071 0.075 0.000 1928 22 gamma 91 1767 0 0 0 0 0 0.009 -0.020 0.000 0.022 0.000 1929 22 gamma 91 1767 0 0 0 0 0 -0.054 -0.532 0.717 0.895 0.000 1930 22 gamma 91 1822 0 0 0 0 0 -0.226 -0.035 -4.339 4.345 0.000 1931 22 gamma 91 1822 0 0 0 0 0 0.003 -0.013 -0.045 0.046 0.000 1932 22 gamma 91 1823 0 0 0 0 0 -0.264 -0.193 -10.942 10.946 0.000 1933 22 gamma 91 1823 0 0 0 0 0 -0.666 -0.257 -21.768 21.780 0.000 1934 22 gamma 91 1846 0 0 0 0 0 -0.280 0.082 207.821 207.821 0.000 1935 22 gamma 91 1846 0 0 0 0 0 -0.087 -0.026 117.789 117.789 0.000 1936 22 gamma 91 1847 0 0 0 0 0 -0.027 0.032 5.517 5.517 0.000 1937 22 gamma 91 1847 0 0 0 0 0 -0.154 0.230 118.637 118.638 0.000 1938 22 gamma 91 1848 0 0 0 0 0 -0.009 -0.167 4.424 4.427 0.000 1939 22 gamma 91 1848 0 0 0 0 0 -0.173 -0.211 8.100 8.104 0.000 1940 22 gamma 91 1849 0 0 0 0 0 -0.006 0.023 0.533 0.533 0.000 1941 22 gamma 91 1849 0 0 0 0 0 0.188 -0.117 6.811 6.815 0.000 1942 22 gamma 91 1852 0 0 0 0 0 -0.273 -0.051 1.076 1.111 0.000 1943 22 gamma 91 1852 0 0 0 0 0 -0.414 -0.236 1.556 1.627 0.000 1944 22 gamma 91 1891 0 0 0 0 0 0.309 -1.162 1.255 1.738 0.000 1945 22 gamma 91 1891 0 0 0 0 0 0.156 -0.477 0.651 0.822 0.000 Charge sum: 2.000 Momentum sum: 0.000 0.000 -0.000 14000.000 14000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Warning in SpaceShower::pT2nextQCD: weight above unity PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again PYTHIA Warning in Pythia::check: energy-momentum not quite conserved *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | q qbar -> Theta 621 | 5737 1000 1000 | 6.503e-08 1.378e-09 | | | | | | sum | 5737 1000 1000 | 6.503e-08 1.378e-09 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 3 Error in Pythia::next: hadronLevel failed; try again | | 3 Error in StringFragmentation::fragment: stuck in joining | | 1 Warning in Pythia::check: energy-momentum not quite conserved | | 8 Warning in SpaceShower::pT2nextQCD: weight above unity | | 2 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:07 Theta mass 2.08*10^ 2 1 2.00*10^ 2 X 1.92*10^ 2 X 1.84*10^ 2 X 1.76*10^ 2 8X 1.68*10^ 2 XX 1.60*10^ 2 XX 1.52*10^ 2 XX 1.44*10^ 2 XX 1.36*10^ 2 XX 1.28*10^ 2 XX 1.20*10^ 2 XX 1.12*10^ 2 6XX 1.04*10^ 2 XXX 0.96*10^ 2 XXX4 0.88*10^ 2 XXXX 0.80*10^ 2 XXXX 0.72*10^ 2 XXXX 0.64*10^ 2 9XXXX4 0.56*10^ 2 XXXXXX 0.48*10^ 2 XXXXXX5 0.40*10^ 2 1XXXXXXX 0.32*10^ 2 XXXXXXXX1 0.24*10^ 2 214XXXXXXXXX4 0.16*10^ 2 12XXXXXXXXXXXXX24 0.08*10^ 2 11 13 1 3 14 313 1 43635XXXXXXXXXXXXXXXXX88656313 44 13 3 41 11 3 11 3 Contents *10^ 2 0000000000000000000000000000000000000000112000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000000000000000000000000000111136070954211100000000000000000000000000000000000000000000000000 *10^ 0 1100000120102000013002120010325249087933941194590166545212033012020000031000001100000020110000020000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 3333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333 *10^ 1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 0 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 Entries = 1000 Mean = 3.4231e+02 Underflow = 0.0000e+00 Low edge = 3.0000e+02 All chan = 1.0000e+03 Rms = 7.2008e+00 Overflow = 0.0000e+00 High edge = 4.0000e+02 pythia8-8.1.80.orig/examples/outref/out190000644000175000017500000075734312217346174016411 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:05:55 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:05:55 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:05:55 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:05:56 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> g g 111 | 1.252e-01 | | g g -> q qbar (uds) 112 | 1.483e-03 | | q g -> q g 113 | 1.005e-01 | | q q(bar)' -> q q(bar)' 114 | 1.148e-02 | | q qbar -> g g 115 | 8.118e-05 | | q qbar -> q' qbar' (uds) 116 | 3.858e-05 | | g g -> c cbar 121 | 4.935e-04 | | q qbar -> c cbar 122 | 1.285e-05 | | g g -> b bbar 123 | 4.851e-04 | | q qbar -> b bbar 124 | 1.273e-05 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 57.54 mb | | | | pT0 = 3.08 gives sigmaInteraction = 271.14 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | HardQCD:all | on | off | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberShowEvent | 0 | 1 0 | | Next:numberShowInfo | 0 | 1 0 | | Next:numberShowProcess | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:pTHatMin | 50.00000 | 0.0 0.0 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | non-diffractive 101 | 5.754e+01 | | A B -> A B elastic 102 | 2.221e+01 | | A B -> X B single diffractive 103 | 6.442e+00 | | A B -> A X single diffractive 104 | 6.442e+00 | | A B -> X X double diffractive 105 | 8.881e+00 | | A B -> A X B central diffractive 106 | 0.000e+00 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 57.54 mb | | | | pT0 = 3.08 gives sigmaInteraction = 267.82 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* PYTHIA Warning in MultipartonInteractions::init: maximum increased by factor 1.095 *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction XB | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.78 gives sigmaInteraction = 11.43 mb: accepted | | diffractive mass = 6.117e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.10 gives sigmaInteraction = 13.47 mb: accepted | | diffractive mass = 3.742e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.55 gives sigmaInteraction = 15.31 mb: accepted | | diffractive mass = 2.289e+03 GeV and sigmaNorm = 10.000 mb | | pT0 = 2.18 gives sigmaInteraction = 25.39 mb: accepted | | diffractive mass = 1.400e+04 GeV and sigmaNorm = 10.000 mb | | pT0 = 3.08 gives sigmaInteraction = 47.27 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction AX | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.78 gives sigmaInteraction = 11.56 mb: accepted | | diffractive mass = 6.117e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.10 gives sigmaInteraction = 13.53 mb: accepted | | diffractive mass = 3.742e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.55 gives sigmaInteraction = 15.41 mb: accepted | | diffractive mass = 2.289e+03 GeV and sigmaNorm = 10.000 mb | | pT0 = 2.18 gives sigmaInteraction = 25.33 mb: accepted | | diffractive mass = 1.400e+04 GeV and sigmaNorm = 10.000 mb | | pT0 = 3.08 gives sigmaInteraction = 48.07 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction AXB | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.78 gives sigmaInteraction = 2.37 mb: rejected | | pT0 = 0.70 gives sigmaInteraction = 3.60 mb: rejected | | pT0 = 0.63 gives sigmaInteraction = 5.51 mb: rejected | | pT0 = 0.57 gives sigmaInteraction = 8.50 mb: rejected | | pT0 = 0.51 gives sigmaInteraction = 13.21 mb: accepted | | diffractive mass = 6.117e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.10 gives sigmaInteraction = 1.61 mb: rejected | | pT0 = 0.99 gives sigmaInteraction = 2.18 mb: rejected | | pT0 = 0.89 gives sigmaInteraction = 2.94 mb: rejected | | pT0 = 0.80 gives sigmaInteraction = 4.00 mb: rejected | | pT0 = 0.72 gives sigmaInteraction = 5.58 mb: rejected | | pT0 = 0.65 gives sigmaInteraction = 7.89 mb: rejected | | pT0 = 0.58 gives sigmaInteraction = 11.34 mb: accepted | | diffractive mass = 3.742e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.55 gives sigmaInteraction = 2.29 mb: rejected | | pT0 = 1.39 gives sigmaInteraction = 2.78 mb: rejected | | pT0 = 1.25 gives sigmaInteraction = 3.36 mb: rejected | | pT0 = 1.13 gives sigmaInteraction = 4.02 mb: rejected | | pT0 = 1.01 gives sigmaInteraction = 4.86 mb: rejected | | pT0 = 0.91 gives sigmaInteraction = 5.89 mb: rejected | | pT0 = 0.82 gives sigmaInteraction = 7.20 mb: rejected | | pT0 = 0.74 gives sigmaInteraction = 8.90 mb: rejected | | pT0 = 0.67 gives sigmaInteraction = 11.27 mb: accepted | | diffractive mass = 2.289e+03 GeV and sigmaNorm = 10.000 mb | | pT0 = 2.18 gives sigmaInteraction = 4.17 mb: rejected | | pT0 = 1.96 gives sigmaInteraction = 5.00 mb: rejected | | pT0 = 1.77 gives sigmaInteraction = 5.87 mb: rejected | | pT0 = 1.59 gives sigmaInteraction = 6.85 mb: rejected | | pT0 = 1.43 gives sigmaInteraction = 8.06 mb: rejected | | pT0 = 1.29 gives sigmaInteraction = 9.21 mb: rejected | | pT0 = 1.16 gives sigmaInteraction = 10.52 mb: rejected | | pT0 = 1.04 gives sigmaInteraction = 12.04 mb: accepted | | diffractive mass = 1.400e+04 GeV and sigmaNorm = 10.000 mb | | pT0 = 3.08 gives sigmaInteraction = 6.61 mb: rejected | | pT0 = 2.77 gives sigmaInteraction = 7.85 mb: rejected | | pT0 = 2.49 gives sigmaInteraction = 9.42 mb: rejected | | pT0 = 2.24 gives sigmaInteraction = 10.92 mb: rejected | | pT0 = 2.02 gives sigmaInteraction = 12.76 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberShowEvent | 0 | 1 0 | | Next:numberShowInfo | 0 | 1 0 | | Next:numberShowProcess | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | Random:seed | 10000002 | -1 900000000 | | Random:setSeed | on | off | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SoftQCD:all | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.146e+02 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | non-diffractive 101 | 2.668e+01 | | A B -> A B elastic 102 | 8.457e+00 | | A B -> X B single diffractive 103 | 4.352e+00 | | A B -> A X single diffractive 104 | 4.352e+00 | | A B -> X X double diffractive 105 | 3.613e+00 | | A B -> A X B central diffractive 106 | 0.000e+00 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 26.68 mb | | | | pT0 = 1.24 gives sigmaInteraction = 79.09 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction XB | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.78 gives sigmaInteraction = 11.56 mb: accepted | | diffractive mass = 1.840e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.87 gives sigmaInteraction = 13.04 mb: accepted | | diffractive mass = 3.386e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.98 gives sigmaInteraction = 13.53 mb: accepted | | diffractive mass = 6.229e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.10 gives sigmaInteraction = 13.54 mb: accepted | | diffractive mass = 1.146e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.24 gives sigmaInteraction = 13.62 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* PYTHIA Warning in MultipartonInteractions::init: maximum increased by factor 5.066 *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction AX | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.78 gives sigmaInteraction = 11.52 mb: accepted | | diffractive mass = 1.840e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.87 gives sigmaInteraction = 12.93 mb: accepted | | diffractive mass = 3.386e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.98 gives sigmaInteraction = 13.56 mb: accepted | | diffractive mass = 6.229e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.10 gives sigmaInteraction = 13.46 mb: accepted | | diffractive mass = 1.146e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.24 gives sigmaInteraction = 13.54 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction AXB | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.78 gives sigmaInteraction = 2.36 mb: rejected | | pT0 = 0.70 gives sigmaInteraction = 3.59 mb: rejected | | pT0 = 0.63 gives sigmaInteraction = 5.46 mb: rejected | | pT0 = 0.57 gives sigmaInteraction = 8.44 mb: rejected | | pT0 = 0.51 gives sigmaInteraction = 13.34 mb: accepted | | diffractive mass = 1.840e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.87 gives sigmaInteraction = 2.01 mb: rejected | | pT0 = 0.79 gives sigmaInteraction = 2.95 mb: rejected | | pT0 = 0.71 gives sigmaInteraction = 4.36 mb: rejected | | pT0 = 0.64 gives sigmaInteraction = 6.55 mb: rejected | | pT0 = 0.57 gives sigmaInteraction = 9.84 mb: rejected | | pT0 = 0.52 gives sigmaInteraction = 15.08 mb: accepted | | diffractive mass = 3.386e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.98 gives sigmaInteraction = 1.73 mb: rejected | | pT0 = 0.88 gives sigmaInteraction = 2.45 mb: rejected | | pT0 = 0.79 gives sigmaInteraction = 3.49 mb: rejected | | pT0 = 0.71 gives sigmaInteraction = 4.93 mb: rejected | | pT0 = 0.64 gives sigmaInteraction = 7.26 mb: rejected | | pT0 = 0.58 gives sigmaInteraction = 10.62 mb: rejected | | pT0 = 0.52 gives sigmaInteraction = 16.02 mb: accepted | | diffractive mass = 6.229e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.10 gives sigmaInteraction = 1.61 mb: rejected | | pT0 = 0.99 gives sigmaInteraction = 2.16 mb: rejected | | pT0 = 0.89 gives sigmaInteraction = 2.91 mb: rejected | | pT0 = 0.80 gives sigmaInteraction = 3.97 mb: rejected | | pT0 = 0.72 gives sigmaInteraction = 5.54 mb: rejected | | pT0 = 0.65 gives sigmaInteraction = 7.89 mb: rejected | | pT0 = 0.58 gives sigmaInteraction = 11.16 mb: accepted | | diffractive mass = 1.146e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.24 gives sigmaInteraction = 1.67 mb: rejected | | pT0 = 1.11 gives sigmaInteraction = 2.14 mb: rejected | | pT0 = 1.00 gives sigmaInteraction = 2.76 mb: rejected | | pT0 = 0.90 gives sigmaInteraction = 3.59 mb: rejected | | pT0 = 0.81 gives sigmaInteraction = 4.71 mb: rejected | | pT0 = 0.73 gives sigmaInteraction = 6.23 mb: rejected | | pT0 = 0.66 gives sigmaInteraction = 8.57 mb: rejected | | pT0 = 0.59 gives sigmaInteraction = 11.90 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eB | 0.0 | 7000.000 0.0 | | Beams:frameType | 2 | 1 1 5 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberShowEvent | 0 | 1 0 | | Next:numberShowInfo | 0 | 1 0 | | Next:numberShowProcess | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | Random:seed | 10000003 | -1 900000000 | | Random:setSeed | on | off | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SoftQCD:all | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.146e+02 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | non-diffractive 101 | 2.668e+01 | | A B -> A B elastic 102 | 8.457e+00 | | A B -> X B single diffractive 103 | 4.352e+00 | | A B -> A X single diffractive 104 | 4.352e+00 | | A B -> X X double diffractive 105 | 3.613e+00 | | A B -> A X B central diffractive 106 | 0.000e+00 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 26.68 mb | | | | pT0 = 1.24 gives sigmaInteraction = 79.01 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction XB | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.78 gives sigmaInteraction = 11.52 mb: accepted | | diffractive mass = 1.840e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.87 gives sigmaInteraction = 12.97 mb: accepted | | diffractive mass = 3.386e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.98 gives sigmaInteraction = 13.56 mb: accepted | | diffractive mass = 6.229e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.10 gives sigmaInteraction = 13.52 mb: accepted | | diffractive mass = 1.146e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.24 gives sigmaInteraction = 13.56 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* PYTHIA Warning in MultipartonInteractions::init: maximum increased by factor 4.950 *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction AX | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.78 gives sigmaInteraction = 11.58 mb: accepted | | diffractive mass = 1.840e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.87 gives sigmaInteraction = 12.93 mb: accepted | | diffractive mass = 3.386e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.98 gives sigmaInteraction = 13.53 mb: accepted | | diffractive mass = 6.229e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.10 gives sigmaInteraction = 13.52 mb: accepted | | diffractive mass = 1.146e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.24 gives sigmaInteraction = 13.54 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction AXB | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.78 gives sigmaInteraction = 2.36 mb: rejected | | pT0 = 0.70 gives sigmaInteraction = 3.58 mb: rejected | | pT0 = 0.63 gives sigmaInteraction = 5.49 mb: rejected | | pT0 = 0.57 gives sigmaInteraction = 8.48 mb: rejected | | pT0 = 0.51 gives sigmaInteraction = 13.29 mb: accepted | | diffractive mass = 1.840e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.87 gives sigmaInteraction = 2.01 mb: rejected | | pT0 = 0.79 gives sigmaInteraction = 2.96 mb: rejected | | pT0 = 0.71 gives sigmaInteraction = 4.37 mb: rejected | | pT0 = 0.64 gives sigmaInteraction = 6.51 mb: rejected | | pT0 = 0.57 gives sigmaInteraction = 9.77 mb: rejected | | pT0 = 0.52 gives sigmaInteraction = 15.23 mb: accepted | | diffractive mass = 3.386e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.98 gives sigmaInteraction = 1.74 mb: rejected | | pT0 = 0.88 gives sigmaInteraction = 2.44 mb: rejected | | pT0 = 0.79 gives sigmaInteraction = 3.46 mb: rejected | | pT0 = 0.71 gives sigmaInteraction = 4.97 mb: rejected | | pT0 = 0.64 gives sigmaInteraction = 7.28 mb: rejected | | pT0 = 0.58 gives sigmaInteraction = 10.72 mb: rejected | | pT0 = 0.52 gives sigmaInteraction = 16.10 mb: accepted | | diffractive mass = 6.229e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.10 gives sigmaInteraction = 1.61 mb: rejected | | pT0 = 0.99 gives sigmaInteraction = 2.16 mb: rejected | | pT0 = 0.89 gives sigmaInteraction = 2.95 mb: rejected | | pT0 = 0.80 gives sigmaInteraction = 4.01 mb: rejected | | pT0 = 0.72 gives sigmaInteraction = 5.51 mb: rejected | | pT0 = 0.65 gives sigmaInteraction = 7.85 mb: rejected | | pT0 = 0.58 gives sigmaInteraction = 11.23 mb: accepted | | diffractive mass = 1.146e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.24 gives sigmaInteraction = 1.67 mb: rejected | | pT0 = 1.11 gives sigmaInteraction = 2.14 mb: rejected | | pT0 = 1.00 gives sigmaInteraction = 2.78 mb: rejected | | pT0 = 0.90 gives sigmaInteraction = 3.61 mb: rejected | | pT0 = 0.81 gives sigmaInteraction = 4.68 mb: rejected | | pT0 = 0.73 gives sigmaInteraction = 6.29 mb: rejected | | pT0 = 0.66 gives sigmaInteraction = 8.62 mb: rejected | | pT0 = 0.59 gives sigmaInteraction = 11.97 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eA | 0.0 | 7000.000 0.0 | | Beams:frameType | 2 | 1 1 5 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberShowEvent | 0 | 1 0 | | Next:numberShowInfo | 0 | 1 0 | | Next:numberShowProcess | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | Random:seed | 10000004 | -1 900000000 | | Random:setSeed | on | off | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SoftQCD:all | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. In 1: id = 21, x = 6.463e-02, pdf = 1.528e+00 at Q2 = 2.733e+03. In 2: id = 21, x = 9.072e-04, pdf = 3.619e+01 at same Q2. Subprocess g g -> g g with code 111 is 2 -> 2. It has sHat = 1.149e+04, tHat = -7.014e+03, uHat = -4.478e+03, pTHat = 5.228e+01, m3Hat = 0.000e+00, m4Hat = 0.000e+00, thetaHat = 1.793e+00, phiHat = 2.945e+00. alphaEM = 7.769e-03, alphaS = 1.486e-01 at Q2 = 2.733e+03. Impact parameter b = 8.013e-01 gives enhancement factor = 1.239e+00. Max pT scale for MPI = 5.228e+01, ISR = 5.228e+01, FSR = 5.228e+01. Number of MPI = 4, ISR = 12, FSRproc = 75, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 21 (g) -21 1 0 5 6 101 102 0.000 0.000 452.424 452.424 0.000 4 21 (g) -21 2 0 5 6 103 104 0.000 0.000 -6.351 6.351 0.000 5 21 g 23 3 4 0 0 101 104 -51.277 10.190 172.418 180.170 0.000 6 21 g 23 3 4 0 0 103 102 51.277 -10.190 273.656 278.605 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 446.074 458.775 107.203 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (combination of several events) ------------------------------------------------------------------ no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 -7000.000 21000.938 19799.985 1 2212 (p+) -12 0 0 412 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 413 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 21 (g) -21 7 0 5 6 101 102 0.000 0.000 452.424 452.424 0.000 4 21 (g) -21 8 8 5 6 103 104 0.000 0.000 -6.351 6.351 0.000 5 21 (g) -23 3 4 9 9 101 104 -51.277 10.190 172.418 180.170 0.000 6 21 (g) -23 3 4 10 10 103 102 51.277 -10.190 273.656 278.605 0.000 7 21 (g) -41 12 0 11 3 105 102 0.000 0.000 608.185 608.185 0.000 8 21 (g) -42 13 13 4 4 103 104 0.000 0.000 -6.351 6.351 0.000 9 21 (g) -44 5 5 14 14 101 104 -45.413 11.498 211.603 216.727 0.000 10 21 (g) -44 6 6 15 15 103 102 60.463 -8.141 332.674 338.222 0.000 11 21 (g) -43 7 0 16 16 105 101 -15.050 -3.357 57.558 59.587 0.000 12 21 (g) -41 18 18 17 7 105 106 -0.000 0.000 1201.550 1201.550 0.000 13 21 (g) -42 19 0 8 8 103 104 0.000 -0.000 -6.351 6.351 0.000 14 21 (g) -44 9 9 20 20 101 104 -45.845 4.952 222.042 226.779 0.000 15 21 (g) -44 10 10 21 21 103 102 59.787 -18.394 348.712 354.278 0.000 16 21 (g) -44 11 11 22 22 105 101 -15.168 -5.148 60.329 62.419 0.000 17 21 (g) -43 12 0 23 23 102 106 1.225 18.590 564.117 564.424 0.000 18 21 (g) -42 28 28 12 12 105 106 -0.000 0.000 1201.550 1201.550 0.000 19 21 (g) -41 27 27 24 13 103 107 0.000 -0.000 -6.953 6.953 0.000 20 21 (g) -44 14 14 30 30 101 104 -44.144 2.549 193.779 198.760 0.000 21 21 (g) -44 15 15 25 26 103 102 61.785 -21.218 361.693 367.545 0.000 22 21 (g) -44 16 16 32 32 105 101 -14.417 -6.208 54.964 57.162 0.000 23 21 (g) -44 17 17 33 33 102 106 1.335 18.434 528.031 528.354 0.000 24 21 (g) -43 19 0 34 34 104 107 -4.559 6.442 56.131 56.683 0.000 25 21 (g) -51 21 0 31 31 108 102 29.572 -17.531 156.904 160.626 0.000 26 21 (g) -51 21 0 35 35 103 108 32.213 -3.686 204.577 207.131 0.000 27 21 (g) -53 29 0 19 19 103 107 0.000 -0.000 -7.165 7.165 0.000 28 21 (g) -42 37 0 18 18 105 106 -0.000 -0.000 1201.550 1201.550 0.000 29 21 (g) -41 38 38 36 27 109 107 0.000 0.000 -13.219 13.219 0.000 30 21 (g) -44 20 20 39 39 101 104 -44.154 1.093 193.115 198.101 0.000 31 21 (g) -44 25 25 40 40 108 102 29.565 -18.620 161.945 165.671 0.000 32 21 (g) -44 22 22 41 41 105 101 -14.422 -6.850 56.837 59.037 0.000 33 21 (g) -44 23 23 42 42 102 106 1.335 18.339 522.070 522.393 0.000 34 21 (g) -44 24 24 43 43 104 107 -4.560 6.281 54.219 54.771 0.000 35 21 (g) -44 26 26 44 44 103 108 32.208 -4.433 205.467 208.023 0.000 36 21 (g) -43 29 0 45 45 109 103 0.029 4.190 -5.321 6.773 0.000 37 1 (d) -41 127 127 46 28 105 0 0.000 0.000 1435.822 1435.822 0.000 38 21 (g) -42 60 60 29 29 109 107 -0.000 -0.000 -13.219 13.219 0.000 39 21 (g) -44 30 30 51 52 101 104 -44.305 0.512 193.362 198.374 0.000 40 21 (g) -44 31 31 69 69 108 102 29.438 -19.106 162.149 165.903 0.000 41 21 (g) -44 32 32 89 90 105 101 -14.467 -7.022 56.899 59.128 0.000 42 21 (g) -44 33 33 67 68 102 106 0.932 16.788 522.790 523.061 0.000 43 21 (g) -44 34 34 53 53 104 107 -4.602 6.119 54.299 54.836 0.000 44 21 (g) -44 35 35 82 82 103 108 32.048 -5.047 205.749 208.291 0.000 45 21 (g) -44 36 36 61 62 109 103 0.028 4.188 -5.306 6.759 0.000 46 1 (d) -43 37 0 137 137 106 0 0.928 3.568 232.659 232.689 0.330 47 21 (g) -31 75 75 49 50 110 111 0.000 0.000 0.066 0.066 0.000 48 21 (g) -31 76 0 49 50 112 113 0.000 0.000 -146.727 146.727 0.000 49 21 (g) -33 47 48 77 77 110 113 -2.539 1.052 -39.094 39.190 0.000 50 21 (g) -33 47 48 78 78 112 111 2.539 -1.052 -107.567 107.602 0.000 51 21 (g) -51 39 0 66 66 101 114 -39.112 0.509 163.363 167.980 0.000 52 21 (g) -51 39 0 64 65 114 104 -5.723 0.706 36.242 36.698 0.000 53 21 (g) -52 43 43 58 59 104 107 -4.073 5.415 48.056 48.532 0.000 54 2 (u) -31 70 70 56 57 115 0 0.000 0.000 1628.366 1628.366 0.000 55 21 (g) -31 71 0 56 57 116 115 0.000 0.000 -0.015 0.015 0.000 56 2 (u) -33 54 55 72 72 117 0 0.590 2.182 1535.817 1535.818 0.330 57 21 (g) -33 54 55 73 73 116 117 -0.590 -2.182 92.534 92.562 0.000 58 21 (g) -51 53 0 134 134 104 118 -1.115 3.721 37.304 37.505 0.000 59 21 (g) -51 53 0 122 123 118 107 -2.958 1.695 10.623 11.156 0.000 60 21 (g) -53 63 63 38 38 109 107 -0.000 0.000 -13.349 13.349 0.000 61 21 (g) -51 45 0 80 81 119 103 0.766 3.275 -3.433 4.806 0.000 62 21 (g) -51 45 0 140 140 109 119 -0.738 0.913 -8.477 8.558 0.000 63 21 (g) -53 124 124 60 60 109 107 -0.000 0.000 -19.954 19.954 0.000 64 21 (g) -51 52 0 138 138 120 104 -14.317 2.264 72.890 74.317 0.000 65 21 (g) -51 52 0 141 141 114 120 -9.301 -1.325 38.098 39.239 0.000 66 21 (g) -52 51 51 91 91 101 114 -21.216 0.276 88.617 91.122 0.000 67 21 (g) -51 42 0 119 120 121 106 1.831 17.563 511.142 511.447 0.000 68 21 (g) -51 42 0 121 121 102 121 -0.244 -1.200 15.262 15.311 0.000 69 21 (g) -52 40 40 106 106 108 102 28.782 -18.681 158.536 162.206 0.000 70 2 (u) -42 95 95 54 54 115 0 0.000 -0.000 1628.366 1628.366 0.000 71 21 (g) -41 96 0 74 55 116 122 -0.000 0.000 -0.261 0.261 0.000 72 2 (u) -44 56 56 97 97 117 0 0.510 2.269 1552.923 1552.925 0.330 73 21 (g) -44 57 57 98 98 116 117 -1.879 -0.762 71.204 71.233 0.000 74 21 (g) -43 71 0 99 99 115 122 1.369 -1.507 3.978 4.469 0.000 75 21 (g) -42 83 0 47 47 110 111 0.000 -0.000 0.066 0.066 0.000 76 -2 (ubar) -41 84 84 79 48 0 113 -0.000 0.000 -643.345 643.345 0.000 77 21 (g) -44 49 49 85 85 110 113 -2.873 1.407 -43.671 43.788 0.000 78 21 (g) -44 50 50 86 86 112 111 1.620 -0.075 -120.189 120.200 0.000 79 -2 (ubar) -43 76 0 87 87 0 112 1.253 -1.332 -479.419 479.423 0.330 80 21 (g) -51 61 0 136 136 119 123 -1.139 2.039 -2.673 3.550 0.000 81 21 (g) -51 61 0 94 94 123 103 2.088 1.207 0.417 2.448 0.000 82 21 (g) -52 44 44 92 93 103 108 31.865 -5.018 204.572 207.100 0.000 83 21 (g) -41 214 214 88 75 110 124 0.000 0.000 0.082 0.082 0.000 84 -2 (ubar) -42 238 238 76 76 0 113 0.000 -0.000 -643.345 643.345 0.000 85 21 (g) -44 77 77 236 237 110 113 -4.055 1.795 -77.277 77.405 0.000 86 21 (g) -44 78 78 166 166 112 111 1.509 -0.039 -95.870 95.882 0.000 87 -2 (ubar) -44 79 79 164 165 0 112 1.216 -1.320 -425.631 425.635 0.330 88 21 (g) -43 83 0 212 213 111 124 1.329 -0.436 -44.484 44.506 0.000 89 21 (g) -51 41 0 103 103 105 125 -13.084 -6.446 49.613 51.713 0.000 90 21 (g) -51 41 0 101 102 125 101 -5.689 -0.520 25.271 25.909 0.000 91 21 (g) -52 66 66 113 114 101 114 -16.910 0.220 70.632 72.629 0.000 92 21 (g) -51 82 0 104 105 126 108 30.540 -4.010 199.056 201.425 0.000 93 21 (g) -51 82 0 107 108 103 126 1.428 -0.948 5.537 5.796 0.000 94 21 (g) -52 81 81 109 109 123 103 1.985 1.147 0.396 2.326 0.000 95 2 (u) -42 248 248 70 70 115 0 -0.000 0.000 1628.366 1628.366 0.000 96 21 (g) -41 249 0 100 71 116 127 0.000 -0.000 -3.686 3.686 0.000 97 2 (u) -44 72 72 172 172 117 0 0.507 2.271 1552.967 1552.969 0.330 98 21 (g) -44 73 73 170 171 116 117 -1.942 -0.726 74.342 74.371 0.000 99 21 (g) -44 74 74 116 117 115 122 0.305 -0.899 0.672 1.163 0.000 100 21 (g) -43 96 0 118 118 122 127 1.130 -0.646 -3.301 3.549 0.000 101 21 (g) -51 90 0 115 115 128 101 -11.030 -3.085 43.953 45.420 0.000 102 21 (g) -51 90 0 146 146 125 128 0.124 -0.006 1.102 1.109 0.000 103 21 (g) -52 89 89 125 126 105 125 -7.866 -3.875 29.829 31.092 0.000 104 21 (g) -51 92 0 110 111 126 129 29.138 -3.401 189.592 191.848 0.000 105 21 (g) -51 92 0 147 147 129 108 3.420 -1.918 20.577 20.947 0.000 106 21 (g) -52 69 69 131 131 108 102 26.765 -17.371 147.423 150.837 0.000 107 21 (g) -51 93 0 112 112 130 126 2.025 -0.260 5.916 6.259 0.000 108 21 (g) -51 93 0 148 148 103 130 0.123 -0.272 -0.236 0.381 0.000 109 21 (g) -52 94 94 143 143 123 103 1.266 0.731 0.253 1.484 0.000 110 21 (g) -51 104 0 135 135 131 129 20.694 -1.855 139.750 141.286 0.000 111 21 (g) -51 104 0 149 149 126 131 8.789 -1.591 50.851 51.629 0.000 112 21 (g) -52 107 107 145 145 130 126 1.679 -0.216 4.907 5.191 0.000 113 21 (g) -51 91 0 130 130 132 114 -2.930 0.496 14.728 15.025 0.000 114 21 (g) -51 91 0 150 150 101 132 -17.405 -1.233 69.549 71.705 0.000 115 21 (g) -52 101 101 144 144 128 101 -7.606 -2.127 30.307 31.319 0.000 116 21 (g) -51 99 0 221 222 115 133 0.321 -0.666 0.742 1.047 0.000 117 21 (g) -51 99 0 223 223 133 122 0.561 -0.563 -1.755 1.926 0.000 118 21 (g) -52 100 100 253 253 122 127 0.553 -0.316 -1.617 1.738 0.000 119 21 (g) -51 67 0 133 133 134 106 2.026 12.594 345.618 345.853 0.000 120 21 (g) -51 67 0 151 151 121 134 -0.208 4.902 166.373 166.445 0.000 121 21 (g) -52 68 68 142 142 102 121 -0.230 -1.133 14.412 14.459 0.000 122 21 (g) -51 59 0 139 139 118 135 -2.522 0.293 8.576 8.944 0.000 123 21 (g) -51 59 0 152 152 135 107 -0.436 1.402 1.876 2.383 0.000 124 21 (g) -53 129 129 63 63 109 107 -0.000 0.000 -20.124 20.124 0.000 125 21 (g) -51 103 0 132 132 136 125 -6.681 -2.271 26.192 27.126 0.000 126 21 (g) -51 103 0 153 153 105 136 -1.185 -1.604 5.895 6.223 0.000 127 1 (d) -53 128 0 37 37 105 0 -0.000 -0.000 1438.079 1438.079 0.000 128 1 (d) -41 342 342 154 127 137 0 -0.000 0.000 1985.787 1985.787 0.000 129 21 (g) -42 343 0 124 124 109 107 0.000 -0.000 -20.124 20.124 0.000 130 21 (g) -44 113 113 315 316 132 114 -2.920 0.492 14.730 15.025 0.000 131 21 (g) -44 106 106 157 157 108 102 26.867 -17.408 147.417 150.853 0.000 132 21 (g) -44 125 125 208 208 136 125 -6.663 -2.278 26.195 27.125 0.000 133 21 (g) -44 119 119 158 159 134 106 2.263 12.509 345.630 345.864 0.000 134 21 (g) -44 58 58 169 169 104 118 -1.089 3.711 37.306 37.506 0.000 135 21 (g) -44 110 110 179 180 131 129 20.790 -1.889 139.748 141.298 0.000 136 21 (g) -44 80 80 188 189 119 123 -1.138 2.039 -2.673 3.549 0.000 137 1 (d) -44 46 46 160 160 106 0 1.087 3.511 232.667 232.697 0.330 138 21 (g) -44 64 64 167 168 120 104 -14.266 2.246 72.897 74.314 0.000 139 21 (g) -44 122 122 191 192 118 135 -2.516 0.291 8.577 8.943 0.000 140 21 (g) -44 62 62 190 190 109 119 -0.738 0.913 -8.476 8.557 0.000 141 21 (g) -44 65 65 306 307 114 120 -9.275 -1.334 38.102 39.237 0.000 142 21 (g) -44 121 121 155 156 102 121 -0.220 -1.137 14.413 14.459 0.000 143 21 (g) -44 109 109 357 357 123 103 1.266 0.731 0.252 1.484 0.000 144 21 (g) -44 115 115 323 323 128 101 -7.585 -2.135 30.311 31.318 0.000 145 21 (g) -44 112 112 288 289 130 126 1.683 -0.217 4.906 5.191 0.000 146 21 (g) -44 102 102 206 207 125 128 0.125 -0.006 1.102 1.109 0.000 147 21 (g) -44 105 105 215 216 129 108 3.434 -1.923 20.576 20.949 0.000 148 21 (g) -44 108 108 362 362 103 130 0.123 -0.272 -0.236 0.381 0.000 149 21 (g) -44 111 111 181 181 126 131 8.824 -1.603 50.849 51.634 0.000 150 21 (g) -44 114 114 321 322 101 132 -17.356 -1.251 69.558 71.701 0.000 151 21 (g) -44 120 120 220 220 121 134 -0.094 4.861 166.379 166.450 0.000 152 21 (g) -44 123 123 193 193 135 107 -0.435 1.402 1.877 2.382 0.000 153 21 (g) -44 126 126 163 163 105 136 -1.181 -1.606 5.896 6.223 0.000 154 21 (g) -43 128 0 161 162 137 105 -0.985 0.352 547.658 547.659 0.000 155 21 (g) -51 142 0 218 219 138 121 -0.084 -1.646 8.725 8.879 0.000 156 21 (g) -51 142 0 196 196 102 138 1.131 -0.312 12.643 12.698 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-84 613 627 809 810 0 0 -0.969 1.133 4.387 4.692 0.738 653 211 pi+ 84 613 627 0 0 0 0 -0.152 0.098 0.567 0.611 0.140 654 113 (rho0) -84 613 627 811 812 0 0 -0.547 0.065 3.846 3.959 0.763 655 313 (K*0) -84 613 627 813 814 0 0 -0.667 0.609 13.404 13.464 0.892 656 -323 (K*-) -84 613 627 815 816 0 0 -0.469 -0.389 28.310 28.332 0.943 657 223 (omega) -84 613 627 909 911 0 0 -0.407 0.188 18.849 18.871 0.783 658 211 pi+ 84 613 627 0 0 0 0 -0.448 -0.076 6.004 6.023 0.140 659 223 (omega) -84 613 627 912 914 0 0 -0.431 0.248 37.651 37.662 0.783 660 -211 pi- 84 613 627 0 0 0 0 -0.268 0.564 4.273 4.321 0.140 661 111 (pi0) -84 613 627 915 916 0 0 0.243 -0.018 1.363 1.391 0.135 662 321 K+ 84 613 627 0 0 0 0 -0.988 1.928 14.309 14.480 0.494 663 -323 (K*-) -84 613 627 817 818 0 0 -3.303 0.623 21.386 21.671 0.983 664 213 (rho+) -84 613 627 819 820 0 0 -5.002 0.949 25.595 26.107 0.753 665 2 (u) -71 446 446 670 687 147 0 0.414 0.083 60.125 60.127 0.330 666 21 (g) -71 538 538 670 687 161 147 -0.477 1.325 246.350 246.354 0.288 667 21 (g) -71 463 463 670 687 140 161 -0.906 0.384 242.358 242.360 0.000 668 21 (g) -71 438 438 670 687 137 140 -0.669 -0.191 90.311 90.313 0.000 669 -1 (dbar) -71 514 514 670 687 0 137 -0.114 0.329 -406.104 406.104 0.330 670 211 pi+ 83 665 669 0 0 0 0 0.126 0.148 52.883 52.884 0.140 671 113 (rho0) -83 665 669 821 822 0 0 -0.031 0.329 113.349 113.351 0.711 672 111 (pi0) -83 665 669 917 918 0 0 0.059 0.266 68.032 68.033 0.135 673 113 (rho0) -83 665 669 823 824 0 0 -1.537 0.719 228.580 228.587 0.665 674 111 (pi0) -83 665 669 919 920 0 0 0.195 -0.099 139.679 139.679 0.135 675 113 (rho0) -83 665 669 825 826 0 0 -0.221 0.403 19.653 19.700 1.276 676 223 (omega) -83 665 669 921 923 0 0 -0.379 -0.444 13.596 13.650 1.071 677 2112 n0 83 665 669 0 0 0 0 0.534 0.396 0.550 1.276 0.940 678 -2212 pbar- 83 665 669 0 0 0 0 -0.148 -0.072 1.550 1.819 0.938 679 323 (K*+) -83 665 669 827 828 0 0 -0.203 -0.101 0.086 0.887 0.853 680 -311 (Kbar0) -84 665 669 829 829 0 0 -0.095 0.319 -0.943 1.117 0.498 681 113 (rho0) -84 665 669 830 831 0 0 0.359 -0.160 -1.929 2.122 0.792 682 -211 pi- 84 665 669 0 0 0 0 -0.132 -0.332 -1.439 1.489 0.140 683 213 (rho+) -84 665 669 832 833 0 0 -0.422 0.262 -24.865 24.881 0.765 684 -211 pi- 84 665 669 0 0 0 0 0.548 -0.514 -20.455 20.469 0.140 685 113 (rho0) -84 665 669 834 835 0 0 -0.146 0.414 -17.973 17.996 0.798 686 213 (rho+) -84 665 669 836 837 0 0 0.205 0.276 -217.420 217.422 0.826 687 111 (pi0) -84 665 669 924 925 0 0 -0.462 0.122 -119.895 119.896 0.135 688 2 (u) -71 515 515 715 769 199 0 0.839 0.451 3368.847 3368.847 0.330 689 21 (g) -71 481 481 715 769 113 141 2.610 -3.104 -208.639 208.678 0.000 690 21 (g) -71 524 524 715 769 141 144 0.892 -0.112 -61.896 61.903 0.193 691 21 (g) -71 489 489 715 769 144 181 1.176 -0.028 -408.203 408.204 0.000 692 21 (g) -71 526 526 715 769 181 162 -0.302 -0.369 -12.051 12.063 0.248 693 21 (g) -71 529 529 715 769 162 163 -2.377 -0.389 -47.270 47.333 0.450 694 21 (g) -71 525 525 715 769 163 109 -2.178 0.899 -36.398 36.475 0.200 695 21 (g) -71 424 424 715 769 109 119 -0.392 0.488 -4.747 4.788 0.000 696 21 (g) -71 458 458 715 769 119 133 -1.552 1.501 -5.604 6.006 0.000 697 21 (g) -71 522 522 715 769 133 160 0.113 0.794 -2.910 3.024 0.176 698 21 (g) -71 531 531 715 769 160 123 0.292 1.421 -1.359 2.075 0.596 699 21 (g) -71 427 427 715 769 123 103 1.269 0.730 0.253 1.485 0.000 700 21 (g) -71 432 432 715 769 103 157 0.124 -0.274 -0.235 0.381 0.000 701 21 (g) -71 502 502 715 769 157 130 0.507 -0.338 0.532 0.808 0.000 702 21 (g) -71 429 429 715 769 130 190 2.620 -0.044 10.047 10.383 0.000 703 21 (g) -71 527 527 715 769 190 126 0.539 -0.420 3.386 3.465 0.273 704 21 (g) -71 433 433 715 769 126 131 4.168 -0.719 24.052 24.421 0.000 705 21 (g) -71 444 444 715 769 131 185 14.445 -1.396 93.990 95.104 0.000 706 21 (g) -71 528 528 715 769 185 179 3.730 -0.061 25.157 25.435 0.336 707 21 (g) -71 419 419 715 769 179 129 4.259 -0.686 29.754 30.065 0.000 708 21 (g) -71 455 455 715 769 129 155 4.653 -1.487 26.621 27.065 0.000 709 21 (g) -71 431 431 715 769 155 197 3.087 -1.758 19.883 20.198 0.000 710 21 (g) -71 530 530 715 769 197 150 3.869 -2.679 22.604 23.095 0.557 711 21 (g) -71 521 521 715 769 150 173 14.834 -9.631 80.364 82.288 0.125 712 21 (g) -71 457 457 715 769 173 151 2.074 -1.656 14.075 14.323 0.000 713 1 (d) -71 451 451 715 769 151 0 0.687 -0.126 5.240 5.297 0.330 714 2 (u) -71 518 518 715 769 127 0 -0.410 0.385 -743.417 743.417 0.330 715 213 (rho+) -85 688 714 838 839 0 0 -0.397 0.374 -527.767 527.768 0.699 716 311 (K0) -85 688 714 840 840 0 0 -0.391 0.218 -68.134 68.137 0.498 717 221 (eta) -86 688 714 926 927 0 0 2.595 -1.722 17.641 17.922 0.548 718 223 (omega) -86 688 714 928 930 0 0 6.208 -3.744 31.492 32.325 0.807 719 313 (K*0) -86 688 714 841 842 0 0 5.830 -3.674 37.212 37.856 0.939 720 -311 (Kbar0) -86 688 714 843 843 0 0 2.474 -1.663 13.570 13.902 0.498 721 -211 pi- 86 688 714 0 0 0 0 6.285 -3.709 35.700 36.438 0.140 722 321 K+ 86 688 714 0 0 0 0 3.294 -0.922 16.750 17.103 0.494 723 -321 K- 86 688 714 0 0 0 0 1.453 0.008 12.751 12.843 0.494 724 213 (rho+) -86 688 714 844 845 0 0 2.848 -1.252 16.845 17.143 0.659 725 3122 (Lambda0) -86 688 714 931 932 0 0 9.790 -1.596 62.710 63.499 1.116 726 -3322 (Xibar0) -86 688 714 933 934 0 0 10.425 -1.811 67.281 68.120 1.315 727 -323 (K*-) -86 688 714 846 847 0 0 2.790 0.099 17.603 17.845 0.896 728 321 K+ 86 688 714 0 0 0 0 3.398 -0.060 17.674 18.005 0.494 729 221 (eta) -86 688 714 935 937 0 0 0.455 -0.910 3.863 4.032 0.548 730 -323 (K*-) -86 688 714 848 849 0 0 1.152 0.029 3.424 3.717 0.876 731 213 (rho+) -86 688 714 850 851 0 0 0.581 0.352 0.749 1.244 0.724 732 -211 pi- 86 688 714 0 0 0 0 0.301 -0.129 0.215 0.416 0.140 733 221 (eta) -86 688 714 938 940 0 0 0.289 0.052 0.229 0.662 0.548 734 211 pi+ 86 688 714 0 0 0 0 0.318 0.659 -0.597 0.955 0.140 735 2214 (Delta+) -86 688 714 852 853 0 0 0.202 0.541 -1.590 2.086 1.221 736 111 (pi0) -86 688 714 941 942 0 0 0.388 0.469 -0.480 0.787 0.135 737 -2224 (Deltabar--) -86 688 714 854 855 0 0 -0.624 0.725 -2.890 3.284 1.232 738 213 (rho+) -86 688 714 856 857 0 0 0.028 0.598 -3.728 3.944 1.138 739 311 (K0) -86 688 714 858 858 0 0 -0.612 0.550 -4.955 5.047 0.498 740 -311 (Kbar0) -86 688 714 859 859 0 0 -0.038 0.088 -1.764 1.835 0.498 741 113 (rho0) -86 688 714 860 861 0 0 -1.099 0.930 -14.318 14.417 0.876 742 311 (K0) -86 688 714 862 862 0 0 -2.047 -0.351 -31.589 31.661 0.498 743 -321 K- 86 688 714 0 0 0 0 -0.190 0.395 -12.856 12.873 0.494 744 221 (eta) -86 688 714 943 944 0 0 -1.543 0.412 -40.425 40.460 0.548 745 211 pi+ 86 688 714 0 0 0 0 0.037 -0.241 -14.613 14.615 0.140 746 313 (K*0) -86 688 714 863 864 0 0 0.304 -0.292 -47.505 47.516 0.907 747 -323 (K*-) -86 688 714 865 866 0 0 -0.182 0.127 -80.917 80.923 0.902 748 223 (omega) -86 688 714 945 947 0 0 0.617 -0.131 -82.526 82.532 0.784 749 2212 p+ 86 688 714 0 0 0 0 0.550 -0.622 -133.184 133.189 0.938 750 -2212 pbar- 86 688 714 0 0 0 0 0.463 -0.683 -80.421 80.430 0.938 751 211 pi+ 86 688 714 0 0 0 0 0.481 -0.082 -22.623 22.629 0.140 752 -211 pi- 86 688 714 0 0 0 0 -0.002 -0.052 -20.681 20.681 0.140 753 113 (rho0) -86 688 714 867 868 0 0 1.285 -1.144 -165.506 165.521 1.380 754 211 pi+ 86 688 714 0 0 0 0 0.047 0.020 -4.664 4.666 0.140 755 211 pi+ 83 688 714 0 0 0 0 0.267 -0.065 938.781 938.781 0.140 756 -211 pi- 83 688 714 0 0 0 0 0.510 0.504 1378.255 1378.255 0.140 757 111 (pi0) -83 688 714 948 949 0 0 0.338 -0.108 211.072 211.072 0.135 758 223 (omega) -83 688 714 950 952 0 0 -0.065 -0.077 507.242 507.243 0.781 759 2224 (Delta++) -83 688 714 869 870 0 0 -0.309 0.630 229.764 229.768 1.214 760 -211 pi- 83 688 714 0 0 0 0 0.122 -0.105 93.456 93.456 0.140 761 -2212 pbar- 83 688 714 0 0 0 0 0.161 -0.185 5.635 5.717 0.938 762 113 (rho0) -83 688 714 871 872 0 0 -0.030 -0.274 2.100 2.224 0.679 763 211 pi+ 83 688 714 0 0 0 0 -0.280 0.274 1.276 1.342 0.140 764 111 (pi0) -84 688 714 953 954 0 0 0.148 0.060 -0.552 0.590 0.135 765 -213 (rho-) -84 688 714 873 874 0 0 0.450 0.066 -0.044 0.945 0.827 766 213 (rho+) -84 688 714 875 876 0 0 -0.312 -0.394 -0.015 1.166 1.052 767 223 (omega) -84 688 714 955 956 0 0 0.063 0.189 -1.990 2.143 0.768 768 -211 pi- 84 688 714 0 0 0 0 -0.132 0.064 -34.049 34.050 0.140 769 3212 (Sigma0) -84 688 714 957 958 0 0 0.881 -1.044 -130.831 130.843 1.193 770 321 K+ 91 547 0 0 0 0 0 0.132 -0.567 -347.994 347.995 0.494 771 -211 pi- 91 547 0 0 0 0 0 0.193 -0.028 -49.871 49.871 0.140 772 -211 pi- 91 565 0 0 0 0 0 -2.611 0.329 17.109 17.311 0.140 773 111 (pi0) -91 565 0 959 960 0 0 -0.245 -0.029 0.905 0.948 0.135 774 211 pi+ 91 566 0 0 0 0 0 -1.695 -0.316 9.234 9.395 0.140 775 111 (pi0) -91 566 0 961 962 0 0 -0.606 0.314 3.150 3.226 0.135 776 -211 pi- 91 571 0 0 0 0 0 -3.312 -0.097 14.215 14.596 0.140 777 111 (pi0) -91 571 0 963 964 0 0 -0.596 -0.298 1.776 1.902 0.135 778 211 pi+ 91 573 0 0 0 0 0 -1.651 -0.908 7.307 7.547 0.140 779 -211 pi- 91 573 0 0 0 0 0 -1.706 -1.273 5.799 6.178 0.140 780 -321 K- 91 590 0 0 0 0 0 -0.057 2.485 67.006 67.054 0.494 781 211 pi+ 91 590 0 0 0 0 0 0.165 0.959 35.331 35.345 0.140 782 -3122 (Lambdabar0) -91 599 0 965 966 0 0 0.773 -0.112 19.164 19.212 1.116 783 -211 pi- 91 599 0 0 0 0 0 0.101 0.236 5.278 5.286 0.140 784 310 (K_S0) -91 600 600 967 968 0 0 -0.083 -0.656 10.281 10.314 0.498 785 211 pi+ 91 601 0 0 0 0 0 1.347 -1.035 7.851 8.034 0.140 786 -211 pi- 91 601 0 0 0 0 0 0.195 0.321 0.915 0.999 0.140 787 130 K_L0 91 605 605 0 0 0 0 -0.375 -0.859 12.793 12.837 0.498 788 -211 pi- 91 610 0 0 0 0 0 0.535 -0.258 -2.422 2.498 0.140 789 111 (pi0) -91 610 0 969 970 0 0 0.090 0.130 -4.672 4.677 0.135 790 211 pi+ 91 611 0 0 0 0 0 0.392 -0.384 -7.646 7.667 0.140 791 -211 pi- 91 611 0 0 0 0 0 -0.193 0.091 -2.267 2.282 0.140 792 211 pi+ 91 612 0 0 0 0 0 0.061 0.251 -22.317 22.319 0.140 793 -211 pi- 91 612 0 0 0 0 0 -0.052 -0.264 -11.900 11.904 0.140 794 211 pi+ 91 633 0 0 0 0 0 -0.151 0.339 14.217 14.222 0.140 795 111 (pi0) -91 633 0 971 972 0 0 0.316 0.119 55.303 55.304 0.135 796 321 K+ 91 635 0 0 0 0 0 0.417 -0.086 1.427 1.569 0.494 797 -211 pi- 91 635 0 0 0 0 0 -0.105 0.068 1.143 1.158 0.140 798 310 (K_S0) -91 636 636 973 974 0 0 -0.055 -0.368 1.004 1.180 0.498 799 -211 pi- 91 637 0 0 0 0 0 0.423 -0.235 0.537 0.736 0.140 800 111 (pi0) -91 637 0 975 976 0 0 -0.200 0.151 0.033 0.286 0.135 801 -211 pi- 91 645 0 0 0 0 0 0.209 -0.339 -0.997 1.083 0.140 802 111 (pi0) -91 645 0 977 978 0 0 0.145 0.278 -3.100 3.119 0.135 803 211 pi+ 91 646 0 0 0 0 0 -0.055 0.331 -4.602 4.616 0.140 804 111 (pi0) -91 646 0 979 980 0 0 0.163 -0.102 -0.574 0.620 0.135 805 211 pi+ 91 648 0 0 0 0 0 0.008 0.148 0.017 0.204 0.140 806 111 (pi0) -91 648 0 981 982 0 0 -0.498 -0.013 -1.398 1.490 0.135 807 -211 pi- 91 651 0 0 0 0 0 -0.838 -0.033 2.892 3.014 0.140 808 111 (pi0) -91 651 0 983 984 0 0 0.073 -0.013 0.128 0.200 0.135 809 211 pi+ 91 652 0 0 0 0 0 -0.224 0.640 1.272 1.448 0.140 810 -211 pi- 91 652 0 0 0 0 0 -0.745 0.493 3.115 3.244 0.140 811 211 pi+ 91 654 0 0 0 0 0 -0.637 -0.150 2.798 2.877 0.140 812 -211 pi- 91 654 0 0 0 0 0 0.090 0.214 1.048 1.082 0.140 813 321 K+ 91 655 0 0 0 0 0 -0.353 0.323 4.868 4.916 0.494 814 -211 pi- 91 655 0 0 0 0 0 -0.314 0.287 8.536 8.548 0.140 815 -311 (Kbar0) -91 656 0 877 877 0 0 -0.505 -0.489 26.435 26.449 0.498 816 -211 pi- 91 656 0 0 0 0 0 0.037 0.100 1.875 1.883 0.140 817 -311 (Kbar0) -91 663 0 878 878 0 0 -1.387 0.068 7.772 7.911 0.498 818 -211 pi- 91 663 0 0 0 0 0 -1.915 0.555 13.614 13.760 0.140 819 211 pi+ 91 664 0 0 0 0 0 -2.120 0.470 12.677 12.863 0.140 820 111 (pi0) -91 664 0 985 986 0 0 -2.882 0.479 12.918 13.245 0.135 821 211 pi+ 91 671 0 0 0 0 0 -0.236 0.247 29.674 29.677 0.140 822 -211 pi- 91 671 0 0 0 0 0 0.205 0.081 83.674 83.675 0.140 823 211 pi+ 91 673 0 0 0 0 0 -0.216 -0.042 20.929 20.931 0.140 824 -211 pi- 91 673 0 0 0 0 0 -1.321 0.761 207.650 207.656 0.140 825 211 pi+ 91 675 0 0 0 0 0 -0.725 0.367 11.028 11.059 0.140 826 -211 pi- 91 675 0 0 0 0 0 0.504 0.036 8.625 8.641 0.140 827 311 (K0) -91 679 0 879 879 0 0 -0.374 -0.088 -0.045 0.630 0.498 828 211 pi+ 91 679 0 0 0 0 0 0.171 -0.014 0.130 0.257 0.140 829 310 (K_S0) -91 680 680 987 988 0 0 -0.095 0.319 -0.943 1.117 0.498 830 211 pi+ 91 681 0 0 0 0 0 0.270 -0.426 -0.846 0.994 0.140 831 -211 pi- 91 681 0 0 0 0 0 0.088 0.266 -1.083 1.128 0.140 832 211 pi+ 91 683 0 0 0 0 0 -0.560 0.016 -13.387 13.400 0.140 833 111 (pi0) -91 683 0 989 990 0 0 0.139 0.246 -11.477 11.481 0.135 834 211 pi+ 91 685 0 0 0 0 0 0.192 0.205 -2.847 2.864 0.140 835 -211 pi- 91 685 0 0 0 0 0 -0.338 0.210 -15.125 15.131 0.140 836 211 pi+ 91 686 0 0 0 0 0 0.298 0.207 -43.092 43.094 0.140 837 111 (pi0) -91 686 0 991 992 0 0 -0.093 0.069 -174.328 174.328 0.135 838 211 pi+ 91 715 0 0 0 0 0 -0.218 0.494 -246.664 246.665 0.140 839 111 (pi0) -91 715 0 993 994 0 0 -0.179 -0.119 -281.103 281.103 0.135 840 310 (K_S0) -91 716 716 995 996 0 0 -0.391 0.218 -68.134 68.137 0.498 841 311 (K0) -91 719 0 880 880 0 0 3.975 -2.673 24.286 24.759 0.498 842 111 (pi0) -91 719 0 997 998 0 0 1.855 -1.001 12.926 13.097 0.135 843 310 (K_S0) -91 720 720 999 1000 0 0 2.474 -1.663 13.570 13.902 0.498 844 211 pi+ 91 724 0 0 0 0 0 1.309 -0.897 8.143 8.297 0.140 845 111 (pi0) -91 724 0 1001 1002 0 0 1.539 -0.355 8.702 8.845 0.135 846 -321 K- 91 727 0 0 0 0 0 2.282 -0.036 12.729 12.942 0.494 847 111 (pi0) -91 727 0 1003 1004 0 0 0.508 0.135 4.873 4.903 0.135 848 -321 K- 91 730 0 0 0 0 0 0.647 -0.228 2.319 2.468 0.494 849 111 (pi0) -91 730 0 1005 1006 0 0 0.505 0.257 1.105 1.249 0.135 850 211 pi+ 91 731 0 0 0 0 0 0.342 -0.167 0.290 0.498 0.140 851 111 (pi0) -91 731 0 1007 1008 0 0 0.238 0.519 0.459 0.745 0.135 852 2212 p+ 91 735 0 0 0 0 0 0.016 0.493 -1.026 1.475 0.938 853 111 (pi0) -91 735 0 1009 1010 0 0 0.186 0.048 -0.564 0.611 0.135 854 -2212 pbar- 91 737 0 0 0 0 0 -0.620 0.567 -1.955 2.326 0.938 855 -211 pi- 91 737 0 0 0 0 0 -0.004 0.158 -0.935 0.958 0.140 856 211 pi+ 91 738 0 0 0 0 0 0.460 0.246 -2.813 2.864 0.140 857 111 (pi0) -91 738 0 1011 1012 0 0 -0.431 0.351 -0.915 1.079 0.135 858 310 (K_S0) -91 739 739 1013 1014 0 0 -0.612 0.550 -4.955 5.047 0.498 859 310 (K_S0) -91 740 740 1015 1016 0 0 -0.038 0.088 -1.764 1.835 0.498 860 211 pi+ 91 741 0 0 0 0 0 -0.027 0.470 -3.286 3.322 0.140 861 -211 pi- 91 741 0 0 0 0 0 -1.072 0.460 -11.033 11.095 0.140 862 130 K_L0 91 742 742 0 0 0 0 -2.047 -0.351 -31.589 31.661 0.498 863 321 K+ 91 746 0 0 0 0 0 0.325 -0.244 -45.669 45.673 0.494 864 -211 pi- 91 746 0 0 0 0 0 -0.021 -0.049 -1.836 1.842 0.140 865 -321 K- 91 747 0 0 0 0 0 -0.273 0.125 -76.750 76.752 0.494 866 111 (pi0) -91 747 0 1017 1018 0 0 0.090 0.002 -4.167 4.171 0.135 867 211 pi+ 91 753 0 0 0 0 0 0.958 -1.028 -157.146 157.153 0.140 868 -211 pi- 91 753 0 0 0 0 0 0.326 -0.117 -8.360 8.368 0.140 869 2212 p+ 91 759 0 0 0 0 0 -0.191 0.568 153.639 153.643 0.938 870 211 pi+ 91 759 0 0 0 0 0 -0.118 0.062 76.125 76.125 0.140 871 211 pi+ 91 762 0 0 0 0 0 0.167 -0.274 0.524 0.630 0.140 872 -211 pi- 91 762 0 0 0 0 0 -0.196 -0.000 1.576 1.594 0.140 873 -211 pi- 91 765 0 0 0 0 0 -0.208 0.010 -0.097 0.269 0.140 874 111 (pi0) -91 765 0 1019 1020 0 0 0.658 0.056 0.053 0.676 0.135 875 211 pi+ 91 766 0 0 0 0 0 -0.197 0.153 -0.387 0.481 0.140 876 111 (pi0) -91 766 0 1021 1023 0 0 -0.115 -0.547 0.372 0.685 0.135 877 310 (K_S0) -91 815 815 1024 1025 0 0 -0.505 -0.489 26.435 26.449 0.498 878 130 K_L0 91 817 817 0 0 0 0 -1.387 0.068 7.772 7.911 0.498 879 310 (K_S0) -91 827 827 1026 1027 0 0 -0.374 -0.088 -0.045 0.630 0.498 880 310 (K_S0) -91 841 841 1028 1029 0 0 3.975 -2.673 24.286 24.759 0.498 881 2212 p+ 91 568 0 0 0 0 0 -10.141 -0.632 40.143 41.420 0.938 882 111 (pi0) -91 568 0 1030 1031 0 0 -5.423 -0.311 21.688 22.358 0.135 883 -2212 pbar- 91 569 0 0 0 0 0 -5.902 -0.870 23.015 23.794 0.938 884 111 (pi0) -91 569 0 1032 1033 0 0 -1.399 -0.292 6.396 6.555 0.135 885 211 pi+ 91 572 0 0 0 0 0 -4.064 -0.989 16.146 16.679 0.140 886 -211 pi- 91 572 0 0 0 0 0 -0.485 -0.106 1.687 1.764 0.140 887 111 (pi0) -91 572 0 1034 1035 0 0 -1.748 -0.184 6.032 6.285 0.135 888 111 (pi0) -91 574 0 1036 1037 0 0 -0.142 0.177 0.723 0.770 0.135 889 22 gamma 91 574 0 0 0 0 0 -0.728 -0.276 6.757 6.802 0.000 890 22 gamma 91 575 0 0 0 0 0 -0.068 0.001 0.045 0.082 0.000 891 22 gamma 91 575 0 0 0 0 0 -1.153 -1.045 5.738 5.945 0.000 892 22 gamma 91 591 0 0 0 0 0 0.191 0.719 18.926 18.940 0.000 893 22 gamma 91 591 0 0 0 0 0 0.190 1.368 37.165 37.191 0.000 894 211 pi+ 91 594 0 0 0 0 0 0.173 0.768 19.765 19.781 0.140 895 -211 pi- 91 594 0 0 0 0 0 0.097 0.508 16.168 16.176 0.140 896 111 (pi0) -91 594 0 1038 1039 0 0 -0.047 0.360 13.536 13.542 0.135 897 22 gamma 91 602 0 0 0 0 0 0.738 -0.675 6.411 6.488 0.000 898 22 gamma 91 602 0 0 0 0 0 0.091 -0.072 1.098 1.104 0.000 899 22 gamma 91 606 0 0 0 0 0 -0.004 -0.012 0.034 0.037 0.000 900 22 gamma 91 606 0 0 0 0 0 0.492 -0.039 0.708 0.863 0.000 901 22 gamma 91 608 0 0 0 0 0 -0.064 -0.057 0.226 0.242 0.000 902 22 gamma 91 608 0 0 0 0 0 0.017 -0.157 0.187 0.245 0.000 903 22 gamma 91 630 0 0 0 0 0 -0.069 0.094 29.523 29.523 0.000 904 22 gamma 91 630 0 0 0 0 0 0.369 -0.490 100.792 100.794 0.000 905 22 gamma 91 634 0 0 0 0 0 -0.039 -0.005 0.122 0.128 0.000 906 22 gamma 91 634 0 0 0 0 0 -0.300 -0.121 26.477 26.479 0.000 907 22 gamma 91 638 0 0 0 0 0 -0.226 0.391 0.194 0.492 0.000 908 22 gamma 91 638 0 0 0 0 0 -0.025 0.070 0.101 0.125 0.000 909 211 pi+ 91 657 0 0 0 0 0 -0.335 -0.002 6.024 6.035 0.140 910 -211 pi- 91 657 0 0 0 0 0 -0.029 0.289 10.079 10.084 0.140 911 111 (pi0) -91 657 0 1040 1041 0 0 -0.043 -0.100 2.747 2.752 0.135 912 211 pi+ 91 659 0 0 0 0 0 -0.315 0.090 21.546 21.549 0.140 913 -211 pi- 91 659 0 0 0 0 0 -0.023 -0.063 11.004 11.005 0.140 914 111 (pi0) -91 659 0 1042 1043 0 0 -0.093 0.221 5.101 5.109 0.135 915 22 gamma 91 661 0 0 0 0 0 0.125 -0.039 1.011 1.020 0.000 916 22 gamma 91 661 0 0 0 0 0 0.117 0.021 0.352 0.371 0.000 917 22 gamma 91 672 0 0 0 0 0 0.013 -0.008 1.178 1.178 0.000 918 22 gamma 91 672 0 0 0 0 0 0.046 0.274 66.854 66.855 0.000 919 22 gamma 91 674 0 0 0 0 0 0.174 -0.093 83.573 83.573 0.000 920 22 gamma 91 674 0 0 0 0 0 0.021 -0.007 56.105 56.105 0.000 921 211 pi+ 91 676 0 0 0 0 0 -0.309 -0.547 6.864 6.894 0.140 922 -211 pi- 91 676 0 0 0 0 0 0.206 0.094 3.293 3.304 0.140 923 111 (pi0) -91 676 0 1044 1045 0 0 -0.277 0.008 3.438 3.452 0.135 924 22 gamma 91 687 0 0 0 0 0 -0.275 0.135 -67.887 67.887 0.000 925 22 gamma 91 687 0 0 0 0 0 -0.187 -0.013 -52.008 52.009 0.000 926 22 gamma 91 717 0 0 0 0 0 1.170 -0.569 8.528 8.627 0.000 927 22 gamma 91 717 0 0 0 0 0 1.424 -1.153 9.113 9.295 0.000 928 211 pi+ 91 718 0 0 0 0 0 2.461 -1.456 13.424 13.726 0.140 929 -211 pi- 91 718 0 0 0 0 0 2.767 -1.495 12.932 13.310 0.140 930 111 (pi0) -91 718 0 1046 1047 0 0 0.979 -0.793 5.136 5.290 0.135 931 2212 p+ 91 725 0 0 0 0 0 7.741 -1.183 49.480 50.104 0.938 932 -211 pi- 91 725 0 0 0 0 0 2.049 -0.413 13.230 13.395 0.140 933 -3122 (Lambdabar0) -91 726 0 1048 1049 0 0 9.465 -1.540 61.277 62.033 1.116 934 111 (pi0) -91 726 0 1050 1051 0 0 0.960 -0.271 6.003 6.087 0.135 935 111 (pi0) -91 729 0 1052 1053 0 0 0.189 -0.417 1.437 1.514 0.135 936 111 (pi0) -91 729 0 1054 1055 0 0 0.138 -0.289 0.856 0.924 0.135 937 111 (pi0) -91 729 0 1056 1057 0 0 0.128 -0.204 1.571 1.595 0.135 938 211 pi+ 91 733 0 0 0 0 0 0.024 -0.091 0.078 0.185 0.140 939 -211 pi- 91 733 0 0 0 0 0 0.160 -0.050 0.137 0.257 0.140 940 22 gamma 91 733 0 0 0 0 0 0.104 0.193 0.014 0.219 0.000 941 22 gamma 91 736 0 0 0 0 0 0.003 0.017 -0.053 0.056 0.000 942 22 gamma 91 736 0 0 0 0 0 0.384 0.452 -0.427 0.731 0.000 943 22 gamma 91 744 0 0 0 0 0 -0.901 0.103 -28.132 28.146 0.000 944 22 gamma 91 744 0 0 0 0 0 -0.641 0.310 -12.293 12.313 0.000 945 211 pi+ 91 748 0 0 0 0 0 0.064 0.087 -27.806 27.806 0.140 946 -211 pi- 91 748 0 0 0 0 0 0.066 -0.109 -6.346 6.349 0.140 947 111 (pi0) -91 748 0 1058 1059 0 0 0.487 -0.108 -48.374 48.377 0.135 948 22 gamma 91 757 0 0 0 0 0 0.058 -0.046 76.422 76.422 0.000 949 22 gamma 91 757 0 0 0 0 0 0.280 -0.062 134.650 134.650 0.000 950 211 pi+ 91 758 0 0 0 0 0 -0.013 -0.074 44.517 44.518 0.140 951 -211 pi- 91 758 0 0 0 0 0 -0.169 -0.186 286.066 286.066 0.140 952 111 (pi0) -91 758 0 1060 1061 0 0 0.118 0.183 176.659 176.659 0.135 953 22 gamma 91 764 0 0 0 0 0 0.103 0.102 -0.420 0.444 0.000 954 22 gamma 91 764 0 0 0 0 0 0.045 -0.043 -0.132 0.146 0.000 955 111 (pi0) -91 767 0 1062 1063 0 0 0.108 0.474 -1.282 1.378 0.135 956 22 gamma 91 767 0 0 0 0 0 -0.045 -0.285 -0.708 0.764 0.000 957 3122 (Lambda0) -91 769 0 1064 1065 0 0 0.799 -1.009 -118.491 118.503 1.116 958 22 gamma 91 769 0 0 0 0 0 0.081 -0.034 -12.339 12.340 0.000 959 22 gamma 91 773 0 0 0 0 0 -0.080 -0.075 0.385 0.400 0.000 960 22 gamma 91 773 0 0 0 0 0 -0.165 0.046 0.520 0.548 0.000 961 22 gamma 91 775 0 0 0 0 0 -0.608 0.319 3.078 3.154 0.000 962 22 gamma 91 775 0 0 0 0 0 0.003 -0.005 0.071 0.072 0.000 963 22 gamma 91 777 0 0 0 0 0 -0.396 -0.125 1.098 1.174 0.000 964 22 gamma 91 777 0 0 0 0 0 -0.200 -0.173 0.678 0.728 0.000 965 -2112 nbar0 91 782 0 0 0 0 0 0.650 -0.160 17.409 17.447 0.940 966 111 (pi0) -91 782 0 1066 1067 0 0 0.123 0.049 1.755 1.765 0.135 967 211 pi+ 91 784 0 0 0 0 0 -0.141 -0.147 1.824 1.841 0.140 968 -211 pi- 91 784 0 0 0 0 0 0.057 -0.509 8.457 8.473 0.140 969 22 gamma 91 789 0 0 0 0 0 -0.011 -0.006 -0.051 0.053 0.000 970 22 gamma 91 789 0 0 0 0 0 0.101 0.137 -4.621 4.624 0.000 971 22 gamma 91 795 0 0 0 0 0 0.269 0.127 39.467 39.468 0.000 972 22 gamma 91 795 0 0 0 0 0 0.047 -0.008 15.836 15.836 0.000 973 111 (pi0) -91 798 0 1068 1069 0 0 -0.140 -0.216 0.882 0.929 0.135 974 111 (pi0) -91 798 0 1070 1071 0 0 0.085 -0.151 0.121 0.251 0.135 975 22 gamma 91 800 0 0 0 0 0 -0.191 0.073 0.038 0.208 0.000 976 22 gamma 91 800 0 0 0 0 0 -0.009 0.078 -0.005 0.079 0.000 977 22 gamma 91 802 0 0 0 0 0 0.027 0.012 -0.775 0.776 0.000 978 22 gamma 91 802 0 0 0 0 0 0.117 0.266 -2.325 2.343 0.000 979 22 gamma 91 804 0 0 0 0 0 0.158 -0.058 -0.536 0.562 0.000 980 22 gamma 91 804 0 0 0 0 0 0.005 -0.044 -0.038 0.058 0.000 981 22 gamma 91 806 0 0 0 0 0 -0.317 0.012 -1.052 1.099 0.000 982 22 gamma 91 806 0 0 0 0 0 -0.181 -0.026 -0.345 0.391 0.000 983 22 gamma 91 808 0 0 0 0 0 0.070 -0.068 0.091 0.134 0.000 984 22 gamma 91 808 0 0 0 0 0 0.003 0.055 0.037 0.066 0.000 985 22 gamma 91 820 0 0 0 0 0 -1.558 0.319 6.882 7.064 0.000 986 22 gamma 91 820 0 0 0 0 0 -1.324 0.160 6.035 6.181 0.000 987 211 pi+ 91 829 0 0 0 0 0 -0.203 0.051 -0.257 0.360 0.140 988 -211 pi- 91 829 0 0 0 0 0 0.108 0.268 -0.686 0.757 0.140 989 22 gamma 91 833 0 0 0 0 0 0.037 0.197 -7.232 7.235 0.000 990 22 gamma 91 833 0 0 0 0 0 0.101 0.049 -4.245 4.247 0.000 991 22 gamma 91 837 0 0 0 0 0 -0.096 0.059 -173.200 173.200 0.000 992 22 gamma 91 837 0 0 0 0 0 0.003 0.011 -1.127 1.127 0.000 993 22 gamma 91 839 0 0 0 0 0 -0.011 0.003 -1.676 1.676 0.000 994 22 gamma 91 839 0 0 0 0 0 -0.168 -0.123 -279.427 279.427 0.000 995 211 pi+ 91 840 0 0 0 0 0 -0.173 0.098 -11.497 11.500 0.140 996 -211 pi- 91 840 0 0 0 0 0 -0.217 0.120 -56.637 56.637 0.140 997 22 gamma 91 842 0 0 0 0 0 0.613 -0.320 3.862 3.923 0.000 998 22 gamma 91 842 0 0 0 0 0 1.242 -0.681 9.064 9.174 0.000 999 211 pi+ 91 843 0 0 0 0 0 0.917 -0.404 4.240 4.359 0.140 1000 -211 pi- 91 843 0 0 0 0 0 1.557 -1.258 9.330 9.544 0.140 1001 22 gamma 91 845 0 0 0 0 0 1.063 -0.289 5.799 5.903 0.000 1002 22 gamma 91 845 0 0 0 0 0 0.476 -0.066 2.903 2.943 0.000 1003 22 gamma 91 847 0 0 0 0 0 0.318 0.021 2.651 2.670 0.000 1004 22 gamma 91 847 0 0 0 0 0 0.190 0.114 2.222 2.233 0.000 1005 22 gamma 91 849 0 0 0 0 0 0.157 0.151 0.446 0.497 0.000 1006 22 gamma 91 849 0 0 0 0 0 0.348 0.106 0.659 0.753 0.000 1007 22 gamma 91 851 0 0 0 0 0 0.240 0.430 0.423 0.649 0.000 1008 22 gamma 91 851 0 0 0 0 0 -0.002 0.089 0.037 0.096 0.000 1009 22 gamma 91 853 0 0 0 0 0 0.014 -0.038 -0.131 0.137 0.000 1010 22 gamma 91 853 0 0 0 0 0 0.172 0.086 -0.433 0.474 0.000 1011 22 gamma 91 857 0 0 0 0 0 -0.024 0.058 -0.054 0.083 0.000 1012 22 gamma 91 857 0 0 0 0 0 -0.407 0.293 -0.861 0.996 0.000 1013 211 pi+ 91 858 0 0 0 0 0 -0.063 0.051 -1.626 1.634 0.140 1014 -211 pi- 91 858 0 0 0 0 0 -0.548 0.499 -3.329 3.413 0.140 1015 111 (pi0) -91 859 0 1072 1073 0 0 0.109 -0.123 -0.865 0.891 0.135 1016 111 (pi0) -91 859 0 1074 1075 0 0 -0.146 0.211 -0.899 0.944 0.135 1017 22 gamma 91 866 0 0 0 0 0 -0.021 -0.038 -1.159 1.160 0.000 1018 22 gamma 91 866 0 0 0 0 0 0.112 0.041 -3.008 3.010 0.000 1019 22 gamma 91 874 0 0 0 0 0 0.295 0.062 -0.032 0.303 0.000 1020 22 gamma 91 874 0 0 0 0 0 0.363 -0.006 0.086 0.373 0.000 1021 22 gamma 91 876 0 0 0 0 0 -0.037 -0.262 0.251 0.365 0.000 1022 11 e- 91 876 0 0 0 0 0 -0.074 -0.280 0.116 0.312 0.001 1023 -11 e+ 91 876 0 0 0 0 0 -0.004 -0.006 0.005 0.009 0.001 1024 211 pi+ 91 877 0 0 0 0 0 -0.276 -0.505 18.216 18.226 0.140 1025 -211 pi- 91 877 0 0 0 0 0 -0.230 0.016 8.219 8.223 0.140 1026 211 pi+ 91 879 0 0 0 0 0 -0.421 -0.142 -0.073 0.471 0.140 1027 -211 pi- 91 879 0 0 0 0 0 0.047 0.054 0.028 0.159 0.140 1028 211 pi+ 91 880 0 0 0 0 0 0.988 -0.820 5.967 6.105 0.140 1029 -211 pi- 91 880 0 0 0 0 0 2.987 -1.853 18.319 18.654 0.140 1030 22 gamma 91 882 0 0 0 0 0 -3.316 -0.130 13.358 13.764 0.000 1031 22 gamma 91 882 0 0 0 0 0 -2.107 -0.181 8.330 8.594 0.000 1032 22 gamma 91 884 0 0 0 0 0 -0.353 -0.080 1.367 1.415 0.000 1033 22 gamma 91 884 0 0 0 0 0 -1.046 -0.212 5.029 5.141 0.000 1034 22 gamma 91 887 0 0 0 0 0 -1.714 -0.165 5.934 6.179 0.000 1035 22 gamma 91 887 0 0 0 0 0 -0.034 -0.019 0.098 0.106 0.000 1036 22 gamma 91 888 0 0 0 0 0 -0.118 0.170 0.714 0.744 0.000 1037 22 gamma 91 888 0 0 0 0 0 -0.024 0.007 0.009 0.026 0.000 1038 22 gamma 91 896 0 0 0 0 0 0.010 0.302 9.851 9.856 0.000 1039 22 gamma 91 896 0 0 0 0 0 -0.057 0.058 3.685 3.686 0.000 1040 22 gamma 91 911 0 0 0 0 0 -0.088 -0.041 1.315 1.318 0.000 1041 22 gamma 91 911 0 0 0 0 0 0.045 -0.059 1.432 1.434 0.000 1042 22 gamma 91 914 0 0 0 0 0 0.016 0.128 2.818 2.821 0.000 1043 22 gamma 91 914 0 0 0 0 0 -0.108 0.093 2.283 2.288 0.000 1044 22 gamma 91 923 0 0 0 0 0 0.013 -0.012 0.263 0.264 0.000 1045 22 gamma 91 923 0 0 0 0 0 -0.289 0.020 3.175 3.188 0.000 1046 22 gamma 91 930 0 0 0 0 0 0.674 -0.599 3.846 3.951 0.000 1047 22 gamma 91 930 0 0 0 0 0 0.305 -0.194 1.289 1.339 0.000 1048 -2212 pbar- 91 933 0 0 0 0 0 8.231 -1.275 53.677 54.327 0.938 1049 211 pi+ 91 933 0 0 0 0 0 1.234 -0.265 7.601 7.706 0.140 1050 22 gamma 91 934 0 0 0 0 0 0.357 -0.098 2.638 2.664 0.000 1051 22 gamma 91 934 0 0 0 0 0 0.602 -0.174 3.365 3.423 0.000 1052 22 gamma 91 935 0 0 0 0 0 0.111 -0.172 0.454 0.498 0.000 1053 22 gamma 91 935 0 0 0 0 0 0.078 -0.244 0.983 1.016 0.000 1054 22 gamma 91 936 0 0 0 0 0 0.020 -0.046 0.039 0.063 0.000 1055 22 gamma 91 936 0 0 0 0 0 0.118 -0.244 0.817 0.861 0.000 1056 22 gamma 91 937 0 0 0 0 0 0.109 -0.057 0.866 0.874 0.000 1057 22 gamma 91 937 0 0 0 0 0 0.019 -0.147 0.705 0.720 0.000 1058 22 gamma 91 947 0 0 0 0 0 0.060 -0.018 -2.927 2.928 0.000 1059 22 gamma 91 947 0 0 0 0 0 0.427 -0.091 -45.447 45.449 0.000 1060 22 gamma 91 952 0 0 0 0 0 0.050 0.178 140.345 140.346 0.000 1061 22 gamma 91 952 0 0 0 0 0 0.068 0.005 36.313 36.314 0.000 1062 22 gamma 91 955 0 0 0 0 0 0.098 0.255 -0.859 0.901 0.000 1063 22 gamma 91 955 0 0 0 0 0 0.010 0.219 -0.424 0.477 0.000 1064 2112 n0 91 957 0 0 0 0 0 0.794 -0.895 -108.706 108.717 0.940 1065 111 (pi0) -91 957 0 1076 1077 0 0 0.005 -0.115 -9.785 9.787 0.135 1066 22 gamma 91 966 0 0 0 0 0 0.071 0.017 0.294 0.303 0.000 1067 22 gamma 91 966 0 0 0 0 0 0.052 0.032 1.461 1.462 0.000 1068 22 gamma 91 973 0 0 0 0 0 -0.062 -0.001 0.200 0.209 0.000 1069 22 gamma 91 973 0 0 0 0 0 -0.078 -0.215 0.682 0.720 0.000 1070 22 gamma 91 974 0 0 0 0 0 0.001 -0.009 0.081 0.081 0.000 1071 22 gamma 91 974 0 0 0 0 0 0.084 -0.142 0.041 0.170 0.000 1072 22 gamma 91 1015 0 0 0 0 0 0.114 -0.144 -0.677 0.701 0.000 1073 22 gamma 91 1015 0 0 0 0 0 -0.006 0.021 -0.188 0.190 0.000 1074 22 gamma 91 1016 0 0 0 0 0 -0.029 0.119 -0.576 0.589 0.000 1075 22 gamma 91 1016 0 0 0 0 0 -0.117 0.093 -0.323 0.355 0.000 1076 22 gamma 91 1065 0 0 0 0 0 -0.006 0.025 -0.634 0.635 0.000 1077 22 gamma 91 1065 0 0 0 0 0 0.011 -0.140 -9.151 9.152 0.000 1078 2212 (p+) -12 0 0 1087 0 0 0 0.000 0.000 0.000 0.938 0.938 1079 2212 (p+) -12 0 0 1088 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 1080 21 (g) -31 1086 1086 1082 1083 306 307 0.000 0.000 0.001 0.001 0.000 1081 2 (u) -31 1088 1088 1082 1083 305 0 0.000 0.000 -3508.781 3508.781 0.000 1082 21 (g) -33 1080 1081 1089 1089 305 307 0.738 -1.660 -1577.793 1577.794 0.000 1083 2 (u) -33 1080 1081 1084 1085 306 0 -0.738 1.660 -1930.987 1930.988 0.330 1084 2 (u) -51 1083 0 1090 1090 308 0 -0.880 1.420 -1392.353 1392.354 0.330 1085 21 (g) -51 1083 0 1091 1091 306 308 0.142 0.241 -538.634 538.634 0.000 1086 21 (g) -53 1087 1087 1080 1080 306 307 -0.000 0.000 0.001 0.001 0.000 1087 21 (g) -61 1078 0 1086 1086 306 307 -0.187 0.449 -54.989 54.991 0.000 1088 2 (u) -61 1079 0 1081 1081 305 0 0.022 -0.319 -3458.865 3458.865 0.000 1089 21 (g) -62 1082 1082 1096 1096 305 307 0.654 -1.549 -1175.017 1175.018 0.000 1090 2 (u) -62 1084 1084 1107 1120 308 0 -0.958 1.476 -1768.274 1768.275 0.330 1091 21 (g) -62 1085 1085 1107 1120 306 308 0.139 0.203 -570.563 570.563 0.000 1092 2101 (ud_0) -63 1078 0 1107 1120 0 306 0.091 -0.360 0.134 0.701 0.579 1093 2 (u) -63 1078 0 1095 1095 307 0 0.095 -0.088 -0.573 0.674 0.330 1094 2103 (ud_1) -63 1079 0 1097 1097 0 305 -0.022 0.319 -3485.707 3485.707 0.771 1095 2 (u) -71 1093 1093 1098 1106 307 0 0.095 -0.088 -0.573 0.674 0.330 1096 21 (g) -71 1089 1089 1098 1106 305 307 0.654 -1.549 -1175.017 1175.018 0.000 1097 2103 (ud_1) -71 1094 1094 1098 1106 0 305 -0.022 0.319 -3485.707 3485.707 0.771 1098 213 (rho+) -83 1095 1097 1121 1122 0 0 0.036 -0.165 -4.594 4.662 0.774 1099 -211 pi- 83 1095 1097 0 0 0 0 0.087 0.071 -1.915 1.924 0.140 1100 221 (eta) -83 1095 1097 1137 1139 0 0 -0.344 0.089 -11.653 11.671 0.548 1101 213 (rho+) -83 1095 1097 1123 1124 0 0 0.499 -0.215 -118.333 118.336 0.742 1102 -211 pi- 83 1095 1097 0 0 0 0 0.057 -0.032 -31.882 31.882 0.140 1103 223 (omega) -83 1095 1097 1140 1142 0 0 -0.140 -0.534 -226.149 226.151 0.784 1104 223 (omega) -83 1095 1097 1143 1145 0 0 0.433 -0.270 -412.383 412.384 0.785 1105 113 (rho0) -84 1095 1097 1125 1126 0 0 0.105 -0.006 -2084.013 2084.013 0.630 1106 2214 (Delta+) -84 1095 1097 1127 1128 0 0 -0.006 -0.257 -1770.375 1770.375 1.235 1107 213 (rho+) -83 1090 1092 1129 1130 0 0 -0.286 0.985 -1321.583 1321.584 1.488 1108 223 (omega) -83 1090 1092 1146 1148 0 0 -0.571 0.804 -845.323 845.324 0.781 1109 -211 pi- 83 1090 1092 0 0 0 0 0.150 -0.633 -17.661 17.674 0.140 1110 111 (pi0) -83 1090 1092 1149 1150 0 0 -0.033 0.623 -27.708 27.715 0.135 1111 213 (rho+) -83 1090 1092 1131 1132 0 0 -0.221 -0.254 -53.143 53.149 0.749 1112 -211 pi- 83 1090 1092 0 0 0 0 0.446 -0.204 -16.026 16.034 0.140 1113 213 (rho+) -83 1090 1092 1133 1134 0 0 -0.079 0.467 -15.344 15.382 0.976 1114 -213 (rho-) -83 1090 1092 1135 1136 0 0 -0.211 -0.601 -31.702 31.718 0.801 1115 111 (pi0) -84 1090 1092 1151 1152 0 0 -0.243 0.575 -4.043 4.093 0.135 1116 223 (omega) -84 1090 1092 1153 1155 0 0 0.310 -0.526 -2.711 2.889 0.790 1117 211 pi+ 84 1090 1092 0 0 0 0 -0.121 0.049 -0.375 0.421 0.140 1118 -211 pi- 84 1090 1092 0 0 0 0 0.467 0.188 -0.640 0.826 0.140 1119 111 (pi0) -84 1090 1092 1156 1157 0 0 -0.197 -0.083 -0.668 0.714 0.135 1120 2212 p+ 84 1090 1092 0 0 0 0 -0.139 -0.070 -1.776 2.015 0.938 1121 211 pi+ 91 1098 0 0 0 0 0 0.195 -0.013 -0.451 0.511 0.140 1122 111 (pi0) -91 1098 0 1158 1159 0 0 -0.159 -0.152 -4.142 4.150 0.135 1123 211 pi+ 91 1101 0 0 0 0 0 0.053 0.202 -19.821 19.822 0.140 1124 111 (pi0) -91 1101 0 1160 1161 0 0 0.446 -0.417 -98.512 98.514 0.135 1125 211 pi+ 91 1105 0 0 0 0 0 0.319 -0.094 -1361.716 1361.717 0.140 1126 -211 pi- 91 1105 0 0 0 0 0 -0.213 0.088 -722.297 722.297 0.140 1127 2112 n0 91 1106 0 0 0 0 0 0.003 -0.428 -1375.904 1375.904 0.940 1128 211 pi+ 91 1106 0 0 0 0 0 -0.009 0.171 -394.471 394.472 0.140 1129 211 pi+ 91 1107 0 0 0 0 0 -0.872 0.764 -843.072 843.073 0.140 1130 111 (pi0) -91 1107 0 1162 1163 0 0 0.585 0.222 -478.511 478.511 0.135 1131 211 pi+ 91 1111 0 0 0 0 0 0.201 0.090 -17.710 17.712 0.140 1132 111 (pi0) -91 1111 0 1164 1165 0 0 -0.421 -0.344 -35.433 35.437 0.135 1133 211 pi+ 91 1113 0 0 0 0 0 0.049 0.642 -6.227 6.262 0.140 1134 111 (pi0) -91 1113 0 1166 1167 0 0 -0.128 -0.175 -9.116 9.120 0.135 1135 -211 pi- 91 1114 0 0 0 0 0 -0.407 -0.366 -11.625 11.639 0.140 1136 111 (pi0) -91 1114 0 1168 1169 0 0 0.196 -0.235 -20.076 20.079 0.135 1137 211 pi+ 91 1100 0 0 0 0 0 -0.078 -0.130 -3.542 3.548 0.140 1138 -211 pi- 91 1100 0 0 0 0 0 -0.113 0.139 -4.105 4.111 0.140 1139 111 (pi0) -91 1100 0 1170 1171 0 0 -0.154 0.080 -4.006 4.012 0.135 1140 111 (pi0) -91 1103 0 1172 1173 0 0 -0.093 -0.396 -161.935 161.936 0.135 1141 11 e- 91 1103 0 0 0 0 0 0.072 0.083 -6.657 6.658 0.001 1142 -11 e+ 91 1103 0 0 0 0 0 -0.120 -0.221 -57.556 57.557 0.001 1143 211 pi+ 91 1104 0 0 0 0 0 -0.052 -0.267 -170.577 170.577 0.140 1144 -211 pi- 91 1104 0 0 0 0 0 0.129 0.093 -109.659 109.659 0.140 1145 111 (pi0) -91 1104 0 1174 1175 0 0 0.357 -0.097 -132.148 132.148 0.135 1146 211 pi+ 91 1108 0 0 0 0 0 -0.134 0.110 -68.161 68.162 0.140 1147 -211 pi- 91 1108 0 0 0 0 0 -0.336 0.315 -294.315 294.316 0.140 1148 111 (pi0) -91 1108 0 1176 1177 0 0 -0.101 0.378 -482.847 482.847 0.135 1149 22 gamma 91 1110 0 0 0 0 0 0.034 0.118 -4.022 4.023 0.000 1150 22 gamma 91 1110 0 0 0 0 0 -0.066 0.504 -23.686 23.691 0.000 1151 22 gamma 91 1115 0 0 0 0 0 -0.081 0.237 -1.227 1.252 0.000 1152 22 gamma 91 1115 0 0 0 0 0 -0.162 0.338 -2.816 2.841 0.000 1153 211 pi+ 91 1116 0 0 0 0 0 -0.083 -0.025 -0.333 0.371 0.140 1154 -211 pi- 91 1116 0 0 0 0 0 0.035 -0.241 -0.417 0.502 0.140 1155 111 (pi0) -91 1116 0 1178 1179 0 0 0.359 -0.260 -1.961 2.015 0.135 1156 22 gamma 91 1119 0 0 0 0 0 -0.123 -0.106 -0.547 0.571 0.000 1157 22 gamma 91 1119 0 0 0 0 0 -0.074 0.023 -0.121 0.143 0.000 1158 22 gamma 91 1122 0 0 0 0 0 -0.088 -0.009 -2.082 2.084 0.000 1159 22 gamma 91 1122 0 0 0 0 0 -0.071 -0.143 -2.060 2.066 0.000 1160 22 gamma 91 1124 0 0 0 0 0 0.375 -0.301 -69.359 69.360 0.000 1161 22 gamma 91 1124 0 0 0 0 0 0.071 -0.116 -29.153 29.153 0.000 1162 22 gamma 91 1130 0 0 0 0 0 0.151 0.016 -85.555 85.555 0.000 1163 22 gamma 91 1130 0 0 0 0 0 0.435 0.206 -392.956 392.956 0.000 1164 22 gamma 91 1132 0 0 0 0 0 -0.350 -0.323 -27.930 27.934 0.000 1165 22 gamma 91 1132 0 0 0 0 0 -0.072 -0.020 -7.503 7.503 0.000 1166 22 gamma 91 1134 0 0 0 0 0 -0.126 -0.105 -7.809 7.811 0.000 1167 22 gamma 91 1134 0 0 0 0 0 -0.002 -0.069 -1.308 1.309 0.000 1168 22 gamma 91 1136 0 0 0 0 0 0.195 -0.147 -15.809 15.811 0.000 1169 22 gamma 91 1136 0 0 0 0 0 0.001 -0.088 -4.267 4.268 0.000 1170 22 gamma 91 1139 0 0 0 0 0 -0.138 0.003 -2.215 2.219 0.000 1171 22 gamma 91 1139 0 0 0 0 0 -0.016 0.077 -1.791 1.793 0.000 1172 22 gamma 91 1140 0 0 0 0 0 0.033 -0.054 -28.403 28.403 0.000 1173 22 gamma 91 1140 0 0 0 0 0 -0.126 -0.342 -133.532 133.533 0.000 1174 22 gamma 91 1145 0 0 0 0 0 0.361 -0.074 -126.697 126.698 0.000 1175 22 gamma 91 1145 0 0 0 0 0 -0.004 -0.023 -5.450 5.450 0.000 1176 22 gamma 91 1148 0 0 0 0 0 -0.099 0.361 -399.501 399.501 0.000 1177 22 gamma 91 1148 0 0 0 0 0 -0.002 0.016 -83.346 83.346 0.000 1178 22 gamma 91 1155 0 0 0 0 0 0.113 -0.132 -0.544 0.571 0.000 1179 22 gamma 91 1155 0 0 0 0 0 0.245 -0.128 -1.417 1.444 0.000 Charge sum: 4.000 Momentum sum: -0.000 0.000 -7000.000 21000.938 19799.985 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Error in BeamRemnants::setKinematics: kinematics construction failed PYTHIA Warning in MultipartonInteractions::pTnext: weight above unity PYTHIA Warning in SpaceShower::pT2nextQCD: weight above unity PYTHIA Warning in MultipartonInteractions::pTnext: weight above unity PYTHIA Error in BeamRemnants::setKinematics: kinematics construction failed PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> g g 111 | 438 60 60 | 1.552e-02 1.115e-03 | | g g -> q qbar (uds) 112 | 5 0 0 | 0.000e+00 0.000e+00 | | q g -> q g 113 | 394 38 38 | 1.041e-02 9.303e-04 | | q q(bar)' -> q q(bar)' 114 | 42 2 2 | 9.190e-04 1.942e-04 | | q qbar -> g g 115 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar -> q' qbar' (uds) 116 | 0 0 0 | 0.000e+00 0.000e+00 | | g g -> c cbar 121 | 3 0 0 | 0.000e+00 0.000e+00 | | q qbar -> c cbar 122 | 0 0 0 | 0.000e+00 0.000e+00 | | g g -> b bbar 123 | 3 0 0 | 0.000e+00 0.000e+00 | | q qbar -> b bbar 124 | 0 0 0 | 0.000e+00 0.000e+00 | | | | | | sum | 885 100 100 | 2.685e-02 1.465e-03 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Error in Pythia::next: hadronLevel failed; try again | | 1 Error in StringFragmentation::fragment: stuck in joining | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | non-diffractive 101 | 123 123 123 | 5.754e+01 0.000e+00 | | A B -> A B elastic 102 | 55 55 55 | 2.221e+01 1.017e-07 | | A B -> X B single diffractive 103 | 20 20 20 | 6.442e+00 0.000e+00 | | A B -> A X single diffractive 104 | 13 13 13 | 6.442e+00 0.000e+00 | | A B -> X X double diffractive 105 | 18 18 18 | 8.881e+00 0.000e+00 | | | | | | sum | 229 229 229 | 1.015e+02 1.017e-07 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Error in BeamRemnants::setKinematics: kinematics construction failed | | 4 Warning in MultipartonInteractions::init: maximum increased | | 3 Warning in SpaceShower::pT2nextQCD: weight above unity | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | non-diffractive 101 | 25 25 25 | 2.668e+01 1.168e-07 | | A B -> A B elastic 102 | 4 4 4 | 8.457e+00 0.000e+00 | | A B -> X B single diffractive 103 | 3 3 3 | 4.352e+00 0.000e+00 | | A B -> A X single diffractive 104 | 6 6 6 | 4.352e+00 3.441e-08 | | A B -> X X double diffractive 105 | 4 4 4 | 3.613e+00 0.000e+00 | | | | | | sum | 42 42 42 | 4.746e+01 1.218e-07 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 3 Warning in MultipartonInteractions::init: maximum increased | | 3 Warning in MultipartonInteractions::pTnext: weight above unity | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | non-diffractive 101 | 34 34 34 | 2.668e+01 0.000e+00 | | A B -> A B elastic 102 | 11 11 11 | 8.457e+00 0.000e+00 | | A B -> X B single diffractive 103 | 4 4 4 | 4.352e+00 0.000e+00 | | A B -> A X single diffractive 104 | 4 4 4 | 4.352e+00 0.000e+00 | | A B -> X X double diffractive 105 | 7 7 7 | 3.613e+00 2.253e-08 | | | | | | sum | 60 60 60 | 4.746e+01 2.253e-08 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 3 Error in BeamRemnants::setKinematics: kinematics construction failed | | 3 Warning in MultipartonInteractions::init: maximum increased | | 1 Warning in MultipartonInteractions::pTnext: weight above unity | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:06 number of pileup events per signal event 2.70*10^ 1 X 2.60*10^ 1 X 2.50*10^ 1 X 2.40*10^ 1 X 2.30*10^ 1 X 2.20*10^ 1 XX 2.10*10^ 1 XX 2.00*10^ 1 XX 1.90*10^ 1 XXX 1.80*10^ 1 XXX 1.70*10^ 1 XXX 1.60*10^ 1 XXX 1.50*10^ 1 XXX 1.40*10^ 1 XXX 1.30*10^ 1 XXX 1.20*10^ 1 XXX 1.10*10^ 1 XXXXX 1.00*10^ 1 XXXXX 0.90*10^ 1 XXXXX 0.80*10^ 1 XXXXXX 0.70*10^ 1 XXXXXX 0.60*10^ 1 XXXXXX 0.50*10^ 1 XXXXXX 0.40*10^ 1 XXXXXX 0.30*10^ 1 XXXXXX 0.20*10^ 1 XXXXXXX 0.10*10^ 1 XXXXXXX Contents *10^ 1 1221100000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 1279182000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 1 0000000000011111111112222222222333333333344444444445555555555666666666677777777778888888888999999999 *10^ 0 0012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789012345678 *10^-1 5555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555 Entries = 100 Mean = 2.2900e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+02 Rms = 1.4986e+00 Overflow = 0.0000e+00 High edge = 9.9500e+01 2013-09-20 16:06 number of beam A + gas events per signal event 6.25*10^ 1 8 6.00*10^ 1 X 5.75*10^ 1 X 5.50*10^ 1 X 5.25*10^ 1 X 5.00*10^ 1 X 4.75*10^ 1 X 4.50*10^ 1 X 4.25*10^ 1 X 4.00*10^ 1 X 3.75*10^ 1 X 3.50*10^ 1 X6 3.25*10^ 1 XX 3.00*10^ 1 XX 2.75*10^ 1 XX 2.50*10^ 1 XX 2.25*10^ 1 XX 2.00*10^ 1 XX 1.75*10^ 1 XX 1.50*10^ 1 XX 1.25*10^ 1 XX 1.00*10^ 1 XX 0.75*10^ 1 XX 0.50*10^ 1 XX6 0.25*10^ 1 XXX Contents *10^ 1 6300000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 2440000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 1 0000000000011111111112222222222333333333344444444445555555555666666666677777777778888888888999999999 *10^ 0 0012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789012345678 *10^-1 5555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555 Entries = 100 Mean = 4.2000e-01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+02 Rms = 5.6886e-01 Overflow = 0.0000e+00 High edge = 9.9500e+01 2013-09-20 16:06 number of beam B + gas events per signal event 5.40*10^ 1 5 5.20*10^ 1 X 5.00*10^ 1 X 4.80*10^ 1 X 4.60*10^ 1 X 4.40*10^ 1 X 4.20*10^ 1 X 4.00*10^ 1 X 3.80*10^ 1 X5 3.60*10^ 1 XX 3.40*10^ 1 XX 3.20*10^ 1 XX 3.00*10^ 1 XX 2.80*10^ 1 XX 2.60*10^ 1 XX 2.40*10^ 1 XX 2.20*10^ 1 XX 2.00*10^ 1 XX 1.80*10^ 1 XX 1.60*10^ 1 XX 1.40*10^ 1 XX 1.20*10^ 1 XX 1.00*10^ 1 XX 0.80*10^ 1 XXX 0.60*10^ 1 XXX 0.40*10^ 1 XXX 0.20*10^ 1 XXX55 Contents *10^ 1 5300000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 3781100000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 1 0000000000011111111112222222222333333333344444444445555555555666666666677777777778888888888999999999 *10^ 0 0012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789012345678 *10^-1 5555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555 Entries = 100 Mean = 6.0000e-01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+02 Rms = 7.6158e-01 Overflow = 0.0000e+00 High edge = 9.9500e+01 2013-09-20 16:06 number of charged multiplicity 8.10*10^ 0 7 7.80*10^ 0 X 7.50*10^ 0 X 7.20*10^ 0 X 6.90*10^ 0 X 6.60*10^ 0 X 6.30*10^ 0 X 6.00*10^ 0 X X X X 5.70*10^ 0 X X X X 5.40*10^ 0 X X X X 5.10*10^ 0 X7 X777X X 4.80*10^ 0 XX XXXXX X 4.50*10^ 0 XX XXXXX X 4.20*10^ 0 33XX XXXXX X 3 3 3.90*10^ 0 XXXX XXXXX X X X 3.60*10^ 0 XXXX XXXXX X X X 3.30*10^ 0 XXXX XXXXX X X X 3.00*10^ 0 XXXXX XXXXXXX X X X X 2.70*10^ 0 XXXXX XXXXXXX X X X X 2.40*10^ 0 XXXXX XXXXXXX X X X X 2.10*10^ 0 7 XXXXX7XXXXXXX X77X7X7X77 7 7 1.80*10^ 0 X XXXXXXXXXXXXX XXXXXXXXXX X X 1.50*10^ 0 X XXXXXXXXXXXXX XXXXXXXXXX X X 1.20*10^ 0 X 3XXXXXXXXXXXXX3XXXXXXXXXX 3 X3 X3 3 0.90*10^ 0 X XXXXXXXXXXXXXXXXXXXXXXXXX X XX XX X 0.60*10^ 0 X XXXXXXXXXXXXXXXXXXXXXXXXX X XX XX X 0.30*10^ 0 X XXXXXXXXXXXXXXXXXXXXXXXXX X XX XX X Contents *10^ 0 0000020134485236555631322624242201021002100000100000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 3 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^ 2 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^ 1 0246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 100 Mean = 3.9750e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+02 Rms = 1.7230e+02 Overflow = 0.0000e+00 High edge = 1.9995e+03 2013-09-20 16:06 total pZ of system 4.60*10^ 1 5 4.40*10^ 1 X 4.20*10^ 1 X 4.00*10^ 1 X 3.80*10^ 1 X 3.60*10^ 1 X 3.40*10^ 1 X 3.20*10^ 1 X 3.00*10^ 1 X 2.80*10^ 1 X 2.60*10^ 1 X 2.40*10^ 1 5 X X 2.20*10^ 1 X X X 2.00*10^ 1 X X X 1.80*10^ 1 X X X 1.60*10^ 1 X X X 1.40*10^ 1 X X X 1.20*10^ 1 X X X 1.00*10^ 1 X X X 0.80*10^ 1 X X X 0.60*10^ 1 X X X X 0.40*10^ 1 X X X X 0.20*10^ 1 5 5 X X X X Contents *10^ 1 0000000000000000000000000000000000000000000000200040020000000000000000000000000000000000000000000000 *10^ 0 0000000000000000000000000000000000001001000600300050040000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 5 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 4 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^ 3 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 100 Mean = -7.4000e+02 Underflow = 0.0000e+00 Low edge = -1.0000e+05 All chan = 1.0000e+02 Rms = 6.6912e+03 Overflow = 0.0000e+00 High edge = 1.0000e+05 pythia8-8.1.80.orig/examples/outref/out260000644000175000017500000116440712217346175016402 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:07:55 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* PYTHIA Warning in PhaseSpace2to2tauyz::trialKin: maximum for cross section violated *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> G g 5021 | 1.796e-10 | | q g -> G q 5022 | 5.141e-10 | | q qbar -> G g 5023 | 2.501e-10 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 57.54 mb | | | | pT0 = 3.08 gives sigmaInteraction = 270.80 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | ExtraDimensionsLED:CutOffMode | 3 | 0 0 3 | | ExtraDimensionsLED:MD | 4000.000 | 2000.000 100.00000 | | ExtraDimensionsLED:monojet | on | off | | ExtraDimensionsLED:n | 4 | 2 1 | | ExtraDimensionsLED:t | 2.00000 | 1.00000 0.0010000 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | ParticleDecays:sophisticatedTau | 0 | 1 0 3 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:pTHatMin | 700.00000 | 0.0 0.0 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products 5000039 Graviton 5 0 0 2.500e+03 1.500e+03 1.000e+00 1.399e+04 0.00000e+00 0 0 0 0 0 -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. In 1: id = 1, x = 3.686e-01, pdf = 6.707e-02 at Q2 = 7.158e+05. In 2: id = -1, x = 1.685e-01, pdf = 4.734e-02 at same Q2. Subprocess q qbar -> G g with code 5023 is 2 -> 2. It has sHat = 1.217e+07, tHat = -8.411e+06, uHat = -1.036e+06, pTHat = 8.460e+02, m3Hat = 1.651e+03, m4Hat = 0.000e+00, thetaHat = 2.467e+00, phiHat = 2.377e+00. alphaEM = 8.057e-03, alphaS = 9.622e-02 at Q2 = 1.569e+06. Impact parameter b = 4.834e-01 gives enhancement factor = 2.422e+00. Max pT scale for MPI = 1.400e+04, ISR = 8.460e+02, FSR = 8.460e+02. Number of MPI = 9, ISR = 22, FSRproc = 200, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 1 (d) -21 1 0 5 6 101 0 0.000 0.000 2580.068 2580.068 0.000 4 -1 (dbar) -21 2 0 5 6 0 102 0.000 0.000 -1179.348 1179.348 0.000 5 5000039 Graviton 23 3 4 0 0 0 0 -610.695 585.530 -281.876 1876.088 1650.593 6 21 g 23 3 4 0 0 101 102 610.695 -585.530 1682.596 1883.328 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 1400.720 3759.416 3488.724 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 860 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 861 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 1 (d) -21 7 0 5 6 101 0 0.000 0.000 2580.068 2580.068 0.000 4 -1 (dbar) -21 8 8 5 6 0 102 0.000 0.000 -1179.348 1179.348 0.000 5 5000039 (Graviton) -23 3 4 9 9 0 0 -610.695 585.530 -281.876 1876.088 1650.593 6 21 (g) -23 3 4 10 10 101 102 610.695 -585.530 1682.596 1883.328 0.000 7 1 (d) -41 12 12 11 3 103 0 -0.000 -0.000 2981.578 2981.578 0.000 8 -1 (dbar) -42 13 0 4 4 0 102 0.000 0.000 -1179.348 1179.348 0.000 9 5000039 (Graviton) -44 5 5 14 14 0 0 -607.453 618.803 -279.100 1885.277 1650.593 10 21 (g) -44 6 6 15 15 101 102 617.948 -511.105 1706.846 1885.845 0.000 11 21 (g) -43 7 0 16 16 103 101 -10.496 -107.698 374.484 389.804 0.000 12 1 (d) -42 26 26 7 7 103 0 0.000 0.000 2981.578 2981.578 0.000 13 -1 (dbar) -41 43 43 17 8 0 104 -0.000 -0.000 -1339.277 1339.277 0.000 14 5000039 (Graviton) -44 9 9 44 44 0 0 -626.138 604.368 -278.600 1886.633 1650.593 15 21 (g) -44 10 10 18 19 101 102 616.403 -512.299 1704.186 1883.256 0.000 16 21 (g) -44 11 11 24 25 103 101 -10.628 -107.800 375.139 390.466 0.000 17 21 (g) -43 13 0 20 20 102 104 20.363 15.732 -158.425 160.501 0.000 18 21 (g) -51 15 0 29 29 101 105 463.317 -369.882 1309.856 1437.775 0.000 19 21 (g) -51 15 0 23 23 105 102 153.144 -142.372 393.877 445.940 0.000 20 21 (g) -52 17 17 21 22 102 104 20.305 15.687 -157.972 160.042 0.000 21 21 (g) -51 20 0 47 47 106 104 -12.853 -12.784 -18.153 25.655 0.000 22 21 (g) -51 20 0 32 32 102 106 35.441 26.348 -133.945 141.037 0.000 23 21 (g) -52 19 19 30 31 105 102 150.860 -140.249 388.003 439.289 0.000 24 21 (g) -51 16 0 27 28 107 101 10.372 -81.759 267.502 279.910 0.000 25 21 (g) -51 16 0 36 37 103 107 -21.000 -26.041 190.276 193.194 0.000 26 1 (d) -53 38 38 12 12 103 0 0.000 0.000 3064.216 3064.216 0.000 27 21 (g) -51 24 0 41 41 107 108 28.405 -49.427 106.406 120.715 0.000 28 21 (g) -51 24 0 51 51 108 101 14.104 -57.988 251.951 258.922 0.000 29 21 (g) -52 18 18 45 45 101 105 431.181 -344.226 1219.001 1338.048 0.000 30 21 (g) -51 23 0 35 35 105 109 151.562 -129.253 382.776 431.503 0.000 31 21 (g) -51 23 0 33 34 109 102 0.037 -10.447 2.435 10.727 0.000 32 21 (g) -52 22 22 49 49 102 106 34.703 25.799 -131.152 138.097 0.000 33 -4 (cbar) -51 31 0 52 52 0 102 20.253 -26.121 28.015 43.355 1.500 34 4 (c) -51 31 0 53 53 109 0 3.052 -4.169 33.185 33.619 1.500 35 21 (g) -52 30 30 48 48 105 109 128.294 -109.410 324.010 365.256 0.000 36 21 (g) -51 25 0 39 40 110 107 5.786 -7.910 74.474 75.116 0.000 37 21 (g) -51 25 0 54 54 103 110 -26.787 -18.131 228.664 230.940 0.000 38 1 (d) -53 42 0 26 26 103 0 0.000 0.000 3177.078 3177.078 0.000 39 21 (g) -51 36 0 50 50 110 111 12.895 -3.410 56.861 58.405 0.000 40 21 (g) -51 36 0 55 55 111 107 4.662 -24.982 61.706 66.735 0.000 41 21 (g) -52 27 27 46 46 107 108 16.634 -28.945 62.312 70.691 0.000 42 1 (d) -41 146 146 56 38 112 0 -0.000 -0.000 3371.702 3371.702 0.000 43 -1 (dbar) -42 147 0 13 13 0 104 -0.000 -0.000 -1339.277 1339.277 0.000 44 5000039 (Graviton) -44 14 14 148 148 0 0 -626.607 602.157 -277.799 1885.963 1650.593 45 21 (g) -44 29 29 92 92 101 105 430.436 -347.741 1218.760 1338.497 0.000 46 21 (g) -44 41 41 59 59 107 108 16.595 -29.128 62.282 70.731 0.000 47 21 (g) -44 21 21 93 94 106 104 -12.855 -12.794 -18.173 25.675 0.000 48 21 (g) -44 35 35 90 91 105 109 128.093 -110.357 323.926 365.396 0.000 49 21 (g) -44 32 32 82 83 102 106 34.700 25.789 -131.095 138.041 0.000 50 21 (g) -44 39 39 111 111 110 111 12.862 -3.569 56.865 58.411 0.000 51 21 (g) -44 28 28 57 58 108 101 13.955 -58.690 251.896 259.019 0.000 52 -4 (cbar) -44 33 33 84 84 0 102 20.232 -26.219 27.989 43.387 1.500 53 4 (c) -44 34 34 157 157 109 0 3.033 -4.261 33.183 33.626 1.500 54 21 (g) -44 37 37 64 65 103 110 -26.920 -18.763 228.649 230.992 0.000 55 21 (g) -44 40 40 109 110 111 107 4.625 -25.158 61.679 66.773 0.000 56 21 (g) -43 42 0 66 66 112 103 1.851 8.736 194.263 194.468 0.000 57 21 (g) -51 51 0 112 113 113 101 1.364 -7.211 56.913 57.384 0.000 58 21 (g) -51 51 0 114 114 108 113 16.044 -57.540 207.942 216.352 0.000 59 21 (g) -52 46 46 150 150 107 108 13.142 -23.067 49.323 56.014 0.000 60 21 (g) -31 71 0 62 63 115 114 0.000 0.000 6.942 6.942 0.000 61 21 (g) -31 72 72 62 63 117 116 0.000 0.000 -14.371 14.371 0.000 62 21 (g) -33 60 61 73 73 117 114 3.780 5.992 3.797 8.038 0.000 63 21 (g) -33 60 61 74 74 115 116 -3.780 -5.992 -11.226 13.274 0.000 64 21 (g) -51 54 0 158 158 118 110 -25.099 -20.273 238.505 240.677 0.000 65 21 (g) -51 54 0 162 162 103 118 -1.433 3.341 30.870 31.083 0.000 66 21 (g) -52 56 56 160 160 112 103 1.463 6.905 153.538 153.700 0.000 67 21 (g) -31 85 85 69 70 120 119 0.000 0.000 1.583 1.583 0.000 68 21 (g) -31 86 0 69 70 122 121 0.000 0.000 -32.892 32.892 0.000 69 21 (g) -33 67 68 87 87 122 119 -6.269 -1.586 -23.302 24.183 0.000 70 21 (g) -33 67 68 88 88 120 121 6.269 1.586 -8.007 10.292 0.000 71 21 (g) -41 76 76 75 60 123 114 -0.000 0.000 13.650 13.650 0.000 72 21 (g) -42 77 0 61 61 117 116 0.000 0.000 -14.371 14.371 0.000 73 21 (g) -44 62 62 78 78 117 114 5.317 10.324 2.183 11.816 0.000 74 21 (g) -44 63 63 79 79 115 116 -3.514 -5.242 -7.006 9.430 0.000 75 21 (g) -43 71 0 80 80 123 115 -1.803 -5.081 4.103 6.775 0.000 76 21 (g) -42 120 0 71 71 123 114 0.000 -0.000 13.650 13.650 0.000 77 21 (g) -41 121 121 81 72 124 116 -0.000 0.000 -19.189 19.189 0.000 78 21 (g) -44 73 73 122 122 117 114 6.663 10.299 1.333 12.338 0.000 79 21 (g) -44 74 74 123 123 115 116 -1.217 -5.285 -8.606 10.173 0.000 80 21 (g) -44 75 75 124 124 123 115 -1.429 -5.088 3.048 6.101 0.000 81 21 (g) -43 77 0 125 125 124 117 -4.017 0.075 -1.314 4.227 0.000 82 21 (g) -51 49 0 95 95 125 106 19.010 20.152 -84.444 88.873 0.000 83 21 (g) -51 49 0 143 144 102 125 15.804 5.489 -46.493 49.412 0.000 84 -4 (cbar) -52 52 52 145 145 0 102 20.119 -26.072 27.831 43.143 1.500 85 21 (g) -42 129 129 67 67 120 119 -0.000 0.000 1.583 1.583 0.000 86 21 (g) -41 216 0 89 68 122 126 0.000 -0.000 -43.571 43.571 0.000 87 21 (g) -44 69 69 127 128 122 119 -7.083 -0.887 -29.807 30.650 0.000 88 21 (g) -44 70 70 218 218 120 121 5.955 1.856 -10.815 12.485 0.000 89 21 (g) -43 86 0 219 219 121 126 1.128 -0.969 -1.366 2.019 0.000 90 21 (g) -51 48 0 152 152 127 109 87.525 -78.698 223.108 252.252 0.000 91 21 (g) -51 48 0 164 164 105 127 63.820 -50.444 166.656 185.450 0.000 92 21 (g) -52 45 45 149 149 101 105 407.183 -328.956 1152.922 1266.191 0.000 93 -2 (ubar) -51 47 0 151 151 0 104 -13.174 -8.863 -16.827 23.138 0.330 94 2 (u) -51 47 0 132 132 106 0 0.886 -3.330 -3.866 5.190 0.330 95 21 (g) -52 82 82 130 131 125 106 18.442 19.551 -81.924 86.220 0.000 96 21 (g) -31 104 0 98 99 129 128 0.000 0.000 299.966 299.966 0.000 97 21 (g) -31 105 105 98 99 130 129 0.000 0.000 -0.608 0.608 0.000 98 21 (g) -33 96 97 106 106 131 128 2.245 1.936 296.299 296.314 0.000 99 21 (g) -33 96 97 107 107 130 131 -2.245 -1.936 3.058 4.259 0.000 100 21 (g) -31 115 115 102 103 132 133 0.000 0.000 20.193 20.193 0.000 101 21 (g) -31 116 0 102 103 133 134 0.000 0.000 -0.438 0.438 0.000 102 21 (g) -33 100 101 117 117 132 135 2.020 2.040 12.582 12.905 0.000 103 21 (g) -33 100 101 118 118 135 134 -2.020 -2.040 7.173 7.726 0.000 104 21 (g) -41 245 245 108 96 136 128 -0.000 0.000 345.858 345.858 0.000 105 21 (g) -42 246 0 97 97 130 129 0.000 -0.000 -0.608 0.608 0.000 106 21 (g) -44 98 98 142 142 131 128 3.792 0.835 319.986 320.010 0.000 107 21 (g) -44 99 99 140 141 130 131 -2.226 -1.950 3.397 4.505 0.000 108 21 (g) -43 104 0 249 249 136 129 -1.566 1.115 21.866 21.950 0.000 109 21 (g) -51 55 0 159 159 137 107 3.627 -7.493 27.941 29.154 0.000 110 21 (g) -51 55 0 166 166 111 137 2.145 -17.984 38.809 42.827 0.000 111 21 (g) -52 50 50 154 154 110 111 11.715 -3.251 51.795 53.202 0.000 112 21 (g) -51 57 0 155 155 138 101 -0.445 0.247 5.705 5.728 0.000 113 21 (g) -51 57 0 167 167 113 138 3.279 -12.729 70.259 71.478 0.000 114 21 (g) -52 58 58 161 161 108 113 14.574 -52.268 188.891 196.531 0.000 115 21 (g) -42 209 209 100 100 132 133 -0.000 -0.000 20.193 20.193 0.000 116 21 (g) -41 210 0 119 101 133 139 0.000 0.000 -1.044 1.044 0.000 117 21 (g) -44 102 102 211 211 132 135 2.765 2.385 15.507 15.931 0.000 118 21 (g) -44 103 103 212 212 135 134 -0.745 -1.451 1.470 2.195 0.000 119 21 (g) -43 116 0 213 213 134 139 -2.020 -0.934 2.172 3.110 0.000 120 -1 (dbar) -41 364 364 126 76 0 114 -0.000 -0.000 174.635 174.635 0.000 121 21 (g) -42 699 699 77 77 124 116 -0.000 -0.000 -19.189 19.189 0.000 122 21 (g) -44 78 78 171 172 117 114 7.780 10.806 0.434 13.322 0.000 123 21 (g) -44 79 79 202 202 115 116 -1.089 -5.227 -8.256 9.832 0.000 124 21 (g) -44 80 80 133 134 123 115 -0.681 -4.749 3.353 5.853 0.000 125 21 (g) -44 81 81 173 173 124 117 -3.779 0.183 -0.976 3.908 0.000 126 -1 (dbar) -43 120 0 135 135 0 123 -2.231 -1.012 160.890 160.909 0.330 127 4 (c) -51 87 0 217 217 122 0 -3.733 -0.147 -22.922 23.273 1.500 128 -4 (cbar) -51 87 0 220 220 0 119 -3.350 -0.740 -6.640 7.623 1.500 129 21 (g) -53 215 215 85 85 120 119 -0.000 0.000 1.828 1.828 0.000 130 21 (g) -51 95 0 153 153 125 140 18.500 16.980 -74.150 78.287 0.000 131 21 (g) -51 95 0 168 168 140 106 0.034 2.223 -8.171 8.468 0.000 132 2 (u) -52 94 94 165 165 106 0 0.795 -2.982 -3.469 4.655 0.330 133 21 (g) -51 124 0 200 201 141 115 -0.675 -2.569 11.687 11.985 0.000 134 21 (g) -51 124 0 188 189 123 141 -0.123 -2.232 0.033 2.236 0.000 135 -1 (dbar) -52 126 126 190 190 0 123 -2.115 -0.960 152.523 152.541 0.330 136 21 (g) -31 180 180 138 139 142 143 0.000 0.000 0.201 0.201 0.000 137 21 (g) -31 181 0 138 139 143 144 0.000 0.000 -63.186 63.186 0.000 138 21 (g) -33 136 137 182 182 142 145 2.001 0.973 -6.725 7.084 0.000 139 21 (g) -33 136 137 183 183 145 144 -2.001 -0.973 -56.260 56.304 0.000 140 21 (g) -51 107 0 176 176 130 146 -3.403 -0.416 6.445 7.300 0.000 141 21 (g) -51 107 0 174 175 146 131 1.305 -1.506 7.698 7.952 0.000 142 21 (g) -52 106 106 177 178 131 128 3.664 0.807 309.241 309.264 0.000 143 21 (g) -51 83 0 163 163 147 125 16.693 5.177 -46.449 49.628 0.000 144 21 (g) -51 83 0 169 169 102 147 -0.416 -0.302 0.612 0.799 0.000 145 -4 (cbar) -52 84 84 156 156 0 102 19.645 -25.458 27.175 42.128 1.500 146 1 (d) -42 382 0 42 42 112 0 -0.000 0.000 3371.702 3371.702 0.000 147 -1 (dbar) -41 383 383 170 43 0 148 0.000 -0.000 -1404.407 1404.407 0.000 148 5000039 (Graviton) -44 44 44 384 384 0 0 -627.613 603.420 -277.165 1886.608 1650.593 149 21 (g) -44 92 92 194 195 101 105 407.131 -328.890 1152.534 1265.804 0.000 150 21 (g) -44 59 59 222 223 107 108 13.139 -23.063 49.303 55.994 0.000 151 -2 (ubar) -44 93 93 205 205 0 104 -13.193 -8.840 -16.826 23.139 0.330 152 21 (g) -44 90 90 260 261 127 109 87.511 -78.681 223.020 252.165 0.000 153 21 (g) -44 130 130 359 360 125 140 18.429 17.069 -74.149 78.289 0.000 154 21 (g) -44 111 111 292 293 110 111 11.714 -3.250 51.787 53.195 0.000 155 21 (g) -44 112 112 197 198 138 101 -0.445 0.247 5.705 5.728 0.000 156 -4 (cbar) -44 145 145 324 325 0 102 19.638 -25.449 27.151 42.104 1.500 157 4 (c) -44 53 53 262 262 109 0 3.033 -4.261 33.179 33.622 1.500 158 21 (g) -44 64 64 185 186 118 110 -25.100 -20.271 238.504 240.676 0.000 159 21 (g) -44 109 109 395 395 137 107 3.626 -7.492 27.934 29.148 0.000 160 21 (g) -44 66 66 208 208 112 103 1.463 6.905 153.540 153.703 0.000 161 21 (g) -44 114 114 224 224 108 113 14.571 -52.264 188.853 196.492 0.000 162 21 (g) -44 65 65 187 187 103 118 -1.433 3.341 30.872 31.085 0.000 163 21 (g) -44 143 143 191 192 147 125 16.649 5.233 -46.454 49.624 0.000 164 21 (g) -44 91 91 196 196 105 127 63.812 -50.433 166.595 185.390 0.000 165 2 (u) -44 132 132 268 268 106 0 0.792 -2.977 -3.471 4.653 0.330 166 21 (g) -44 110 110 294 294 111 137 2.143 -17.982 38.797 42.815 0.000 167 21 (g) -44 113 113 403 403 113 138 3.279 -12.728 70.250 71.469 0.000 168 21 (g) -44 131 131 266 267 140 106 0.026 2.233 -8.169 8.469 0.000 169 21 (g) -44 144 144 193 193 102 147 -0.416 -0.302 0.612 0.799 0.000 170 21 (g) -43 147 0 203 204 104 148 1.246 -1.564 -65.108 65.139 0.000 171 21 (g) -51 122 0 310 311 149 114 5.046 10.056 -0.448 11.260 0.000 172 21 (g) -51 122 0 312 312 117 149 2.283 0.771 0.765 2.529 0.000 173 21 (g) -52 125 125 428 429 124 117 -3.328 0.161 -0.859 3.441 0.000 174 21 (g) -51 141 0 179 179 150 131 -0.388 -1.135 11.788 11.849 0.000 175 21 (g) -51 141 0 251 251 146 150 -0.506 -0.640 0.074 0.819 0.000 176 21 (g) -52 140 140 248 248 130 146 -1.204 -0.147 2.280 2.583 0.000 177 21 (g) -51 142 0 247 247 151 128 -0.766 0.577 82.628 82.634 0.000 178 21 (g) -51 142 0 252 252 131 151 4.286 -0.193 230.998 231.038 0.000 179 21 (g) -52 174 174 250 250 150 131 -0.244 -0.713 7.403 7.441 0.000 180 21 (g) -42 275 0 136 136 142 143 -0.000 0.000 0.201 0.201 0.000 181 1 (d) -41 276 276 184 137 143 0 0.000 -0.000 -107.570 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(ubar) -73 868 897 1425 1425 0 238 6.548 -1.817 26.713 27.566 0.353 1124 21 (g) -73 909 932 1413 1413 318 270 10.563 -36.287 131.841 137.151 0.218 1125 21 (g) -73 921 954 1406 1406 338 154 0.693 -0.535 2.022 2.238 0.393 1126 21 (g) -73 864 945 1419 1419 107 310 1.453 -2.074 4.698 5.353 0.422 1127 21 (g) -73 917 950 1424 1424 238 324 0.131 -3.714 7.349 8.248 0.457 1128 21 (g) -73 907 920 1420 1420 243 107 1.230 -1.581 7.933 8.198 0.506 1129 21 (g) -73 866 955 1378 1378 348 176 21.899 -19.381 56.031 63.203 0.189 1130 21 (g) -73 878 928 1381 1381 268 127 35.925 -27.864 92.881 103.412 0.490 1131 21 (g) -73 896 901 1380 1380 127 353 5.933 -4.795 15.119 16.943 0.533 1132 21 (g) -73 1017 1018 1471 1471 174 284 2.608 -0.752 -3.548 4.468 0.087 1133 21 (g) -73 939 1014 1139 0 288 125 1.584 0.727 -4.552 4.876 0.154 1134 2 (u) -73 879 1021 1461 1461 298 0 1.143 -1.978 -3.093 3.877 0.500 1135 21 (g) -73 882 910 1464 1464 140 220 0.941 1.243 -2.771 3.186 0.202 1136 21 (g) -73 877 940 1469 1469 291 350 0.466 0.520 -1.168 1.391 0.290 1137 21 (g) -73 914 1020 1462 1462 120 298 -0.764 -0.550 -1.557 1.881 0.477 1138 21 (g) -73 883 1022 1476 1476 277 147 0.557 -0.013 0.053 0.757 0.510 1139 21 (g) -73 957 1133 1468 1468 350 125 10.164 4.101 -30.420 32.338 0.528 1140 21 (g) -73 867 937 1465 1465 283 140 13.393 12.142 -51.399 54.488 0.539 1141 21 (g) -73 923 946 1214 1214 312 249 -0.758 -1.112 10.261 10.354 0.334 1142 -4 (cbar) -73 943 1015 1599 1599 0 203 -4.315 -1.477 -9.372 10.576 1.796 1143 21 (g) -73 874 908 1144 0 211 213 0.349 2.214 48.739 48.791 0.333 1144 2 (u) -73 931 1143 1202 1202 211 0 1.008 6.061 121.540 121.698 0.816 1145 21 (g) -73 925 942 1311 1311 110 299 -1.607 -1.484 19.048 19.176 0.294 1146 2 (u) -73 936 949 1308 1308 282 0 4.408 -1.506 19.015 19.592 0.755 1147 21 (g) -73 1028 1062 1152 0 132 196 0.268 -0.758 5.336 5.396 0.004 1148 3 (s) -73 975 1115 1152 0 196 0 1.147 -1.554 15.611 15.740 0.559 1149 21 (g) -73 1036 1039 1324 1324 294 246 1.308 -0.538 68.783 68.798 0.133 1150 21 (g) -73 1006 1040 1331 1331 263 337 -0.703 -0.180 4.860 4.917 0.179 1151 21 (g) -73 1000 1033 1328 1328 308 151 -1.331 0.696 94.694 94.706 0.186 1152 3 (s) -73 1147 1148 1321 1321 132 0 1.415 -2.312 20.947 21.136 0.784 1153 21 (g) -73 1025 1093 1327 1327 151 304 -0.732 0.818 121.887 121.893 0.282 1154 21 (g) -73 1034 1114 1325 1325 293 294 0.943 0.530 83.366 83.374 0.386 1155 21 (g) -73 992 1068 1332 1332 217 263 -0.616 0.253 21.872 21.886 0.446 1156 21 (g) -73 996 1073 1164 0 273 289 0.004 0.638 -0.029 0.640 0.034 1157 21 (g) -73 1056 1067 1167 0 269 322 -0.686 0.263 0.155 0.752 0.038 1158 21 (g) -73 1080 1117 1523 1523 333 145 0.017 0.612 -10.238 10.256 0.063 1159 21 (g) -73 1074 1078 1521 1521 359 351 -0.831 0.082 -7.638 7.684 0.080 1160 21 (g) -73 1046 1096 1511 1511 259 233 0.760 0.224 -0.572 0.982 0.100 1161 21 (g) -73 984 1090 1515 1515 117 230 -0.312 0.612 -0.095 0.702 0.111 1162 21 (g) -73 1077 1091 1165 0 351 287 -0.447 -0.541 -5.510 5.555 0.115 1163 21 (g) -73 1001 1088 1513 1513 149 311 1.374 2.126 0.521 2.589 0.156 1164 21 (g) -73 993 1156 1509 1509 250 289 0.036 0.780 0.061 0.811 0.210 1165 21 (g) -73 1102 1162 1520 1520 351 124 -0.652 -0.739 -6.915 6.989 0.250 1166 21 (g) -73 986 1103 1512 1512 311 259 0.434 0.878 -2.211 2.434 0.275 1167 21 (g) -73 966 1157 1518 1518 303 322 -1.815 0.646 -0.013 1.956 0.338 1168 21 (g) -73 1049 1065 1528 1528 335 309 -2.568 0.554 -900.241 900.245 0.385 1169 21 (g) -73 963 976 1510 1510 233 250 2.350 2.631 -1.287 3.775 0.389 1170 21 (g) -73 1064 1113 1526 1526 343 229 -1.608 1.509 -169.732 169.747 0.469 1171 21 (g) -73 1008 1060 1179 0 261 221 0.724 0.276 2.082 2.222 0.050 1172 21 (g) -73 974 1026 1288 1288 130 152 -2.232 0.203 3.520 4.173 0.079 1173 21 (g) -73 1043 1110 1180 0 166 172 -0.506 0.673 2.544 2.681 0.082 1174 21 (g) -73 998 1029 1177 0 292 301 -1.482 -1.254 1.104 2.239 0.158 1175 -3 (sbar) -73 970 1055 1290 1290 0 166 0.059 0.566 2.011 2.189 0.652 1176 21 (g) -73 990 1045 1282 1282 345 155 -0.575 -0.593 2.699 2.829 0.191 1177 21 (g) -73 968 1174 1287 1287 152 301 -1.479 -1.292 1.142 2.293 0.309 1178 21 (g) -73 987 997 1286 1286 301 141 -0.017 -0.273 -0.319 0.575 0.394 1179 21 (g) -73 1053 1171 1284 1284 261 135 3.155 0.521 9.429 9.964 0.405 1180 21 (g) -73 1107 1173 1289 1289 166 130 -1.773 2.247 6.814 7.405 0.458 1181 21 (g) -73 1072 1089 1283 1283 135 345 0.254 -1.040 6.115 6.237 0.598 1182 21 (g) -73 953 1019 1250 1250 126 122 -0.097 0.094 -2.467 2.483 0.255 1183 21 (g) -73 980 1058 1230 1230 134 321 0.715 0.106 0.906 1.161 0.063 1184 2 (u) -73 1027 1116 1227 1227 290 0 -2.064 0.394 20.992 21.100 0.396 1185 21 (g) -73 985 1035 1186 0 150 297 -0.563 -0.399 0.881 1.124 0.104 1186 21 (g) -73 1037 1185 1228 1228 150 290 -1.063 -0.980 2.376 2.804 0.356 1187 21 (g) -73 1092 1095 1189 0 342 114 -0.376 -0.583 139.677 139.679 0.148 1188 21 (g) -73 1051 1082 1190 0 251 236 0.407 0.615 6.015 6.063 0.177 1189 21 (g) -73 1083 1187 1356 1356 236 114 -0.327 -0.725 159.015 159.017 0.355 1190 21 (g) -73 1054 1188 1357 1357 320 236 1.069 0.953 12.228 12.320 0.454 1191 21 (g) -73 1071 1087 1263 1263 169 192 0.351 -0.427 -43.062 43.066 0.185 1192 21 (g) -73 1106 1109 1264 1264 244 169 -0.706 -0.962 -56.853 56.867 0.367 1193 2 (u) -73 1061 1070 1262 1262 192 0 -0.221 -0.123 -247.626 247.627 0.685 1194 21 (g) -73 972 1052 1200 0 328 275 -0.789 -0.186 -0.958 1.255 0.050 1195 21 (g) -73 1004 1050 1567 1567 201 326 0.361 0.426 0.565 0.798 0.071 1196 21 (g) -73 995 1057 1563 1563 275 346 0.443 -0.626 -1.433 1.628 0.101 1197 21 (g) -73 1044 1094 1201 0 231 279 0.823 -0.531 0.083 1.011 0.234 1198 21 (g) -73 1059 1069 1560 1560 302 255 -0.194 -0.929 -3.411 3.549 0.248 1199 21 (g) -73 978 1009 1562 1562 346 202 0.161 -2.327 -1.198 2.639 0.295 1200 21 (g) -73 988 1194 1564 1564 245 275 -0.977 -0.414 -1.327 1.729 0.320 1201 21 (g) -73 994 1197 1565 1565 231 245 0.975 -0.684 0.291 1.310 0.462 1202 2 (u) -71 1144 1144 1204 1206 211 0 1.008 6.061 121.540 121.698 0.816 1203 -2 (ubar) -71 906 906 1204 1206 0 211 -0.488 1.556 68.754 68.774 0.330 1204 213 (rho+) -83 1202 1203 1619 1620 0 0 0.679 2.657 56.054 56.126 0.697 1205 -211 pi- 83 1202 1203 0 0 0 0 0.167 3.393 65.735 65.823 0.140 1206 111 (pi0) -84 1202 1203 1790 1791 0 0 -0.327 1.567 68.505 68.524 0.135 1207 2 (u) -71 1122 1122 1210 1212 209 0 -0.766 0.091 137.626 137.630 0.594 1208 2 (u) -71 1120 1120 1210 1212 364 0 0.110 -1.076 220.503 220.505 0.330 1209 2 (u) -71 1118 1118 1210 1212 362 0 -0.092 -0.361 745.505 745.505 0.330 1210 323 (K*+) -86 1207 1209 1621 1622 0 0 -0.294 -0.170 206.209 206.212 0.934 1211 213 (rho+) -83 1207 1209 1623 1624 0 0 -0.478 -0.436 603.730 603.731 0.710 1212 3212 (Sigma0) -84 1207 1209 1792 1793 0 0 0.024 -0.740 293.694 293.698 1.193 1213 3 (s) -71 885 885 1219 1226 249 0 -5.992 -2.376 50.628 51.039 0.500 1214 21 (g) -71 1141 1141 1219 1226 312 249 -0.758 -1.112 10.261 10.354 0.334 1215 21 (g) -71 876 876 1219 1226 223 312 -0.663 0.152 3.430 3.497 0.000 1216 21 (g) -71 935 935 1219 1226 278 223 0.161 0.274 8.269 8.275 0.000 1217 21 (g) -71 913 913 1219 1226 157 278 -0.486 1.455 12.760 12.851 0.000 1218 -2 (ubar) -71 890 890 1219 1226 0 157 0.107 0.698 10.657 10.685 0.330 1219 -313 (K*bar0) -83 1213 1218 1625 1626 0 0 -1.818 -1.178 16.455 16.619 0.860 1220 313 (K*0) -83 1213 1218 1627 1628 0 0 -2.941 -0.860 24.195 24.405 0.891 1221 -321 K- 83 1213 1218 0 0 0 0 -0.780 -0.648 11.150 11.207 0.494 1222 213 (rho+) -83 1213 1218 1629 1630 0 0 -1.514 -0.226 10.959 11.097 0.837 1223 311 (K0) -84 1213 1218 1631 1631 0 0 -0.262 0.239 15.254 15.266 0.498 1224 -311 (Kbar0) -84 1213 1218 1632 1632 0 0 -0.364 0.891 10.469 10.525 0.498 1225 111 (pi0) -84 1213 1218 1794 1795 0 0 -0.038 0.709 5.406 5.454 0.135 1226 -211 pi- 84 1213 1218 0 0 0 0 0.086 0.164 2.116 2.129 0.140 1227 2 (u) -71 1184 1184 1232 1240 290 0 -2.064 0.394 20.992 21.100 0.396 1228 21 (g) -71 1186 1186 1232 1240 150 290 -1.063 -0.980 2.376 2.804 0.356 1229 21 (g) -71 1002 1002 1232 1240 321 150 0.176 0.419 -0.080 0.461 0.000 1230 21 (g) -71 1183 1183 1232 1240 134 321 0.715 0.106 0.906 1.161 0.063 1231 -2 (ubar) -71 979 979 1232 1240 0 134 1.488 2.816 1.260 3.441 0.330 1232 223 (omega) -83 1227 1231 1796 1798 0 0 -1.102 -0.458 9.444 9.551 0.784 1233 2214 (Delta+) -83 1227 1231 1633 1634 0 0 -0.843 0.553 8.407 8.554 1.211 1234 223 (omega) -83 1227 1231 1799 1801 0 0 -0.362 -0.093 1.036 1.353 0.786 1235 -2212 pbar- 83 1227 1231 0 0 0 0 0.071 0.077 1.268 1.581 0.938 1236 223 (omega) -84 1227 1231 1802 1804 0 0 -0.279 0.349 2.760 2.904 0.784 1237 321 K+ 84 1227 1231 0 0 0 0 0.022 -0.136 0.760 0.916 0.494 1238 -323 (K*-) -84 1227 1231 1635 1636 0 0 0.621 0.383 0.575 1.296 0.903 1239 211 pi+ 84 1227 1231 0 0 0 0 0.426 0.140 0.304 0.559 0.140 1240 -211 pi- 84 1227 1231 0 0 0 0 0.697 1.939 0.899 2.253 0.140 1241 1 (d) -71 1079 1079 1243 1248 128 0 -0.571 0.822 -46.316 46.328 0.330 1242 -2 (ubar) -71 1100 1100 1243 1248 0 128 0.087 -0.295 0.986 1.084 0.330 1243 113 (rho0) -83 1241 1242 1637 1638 0 0 -0.276 0.423 -24.791 24.812 0.895 1244 -211 pi- 83 1241 1242 0 0 0 0 0.002 -0.007 -7.322 7.323 0.140 1245 321 K+ 83 1241 1242 0 0 0 0 -0.143 0.154 -7.159 7.179 0.494 1246 -323 (K*-) -84 1241 1242 1639 1640 0 0 -0.378 -0.085 -5.834 5.936 1.024 1247 2212 p+ 84 1241 1242 0 0 0 0 0.235 -0.041 -0.607 1.143 0.938 1248 -2212 pbar- 84 1241 1242 0 0 0 0 0.076 0.083 0.382 1.019 0.938 1249 4 (c) -71 1012 1012 1255 1261 122 0 -4.156 -0.236 -24.010 24.414 1.500 1250 21 (g) -71 1182 1182 1255 1261 126 122 -0.097 0.094 -2.467 2.483 0.255 1251 21 (g) -71 902 902 1255 1261 222 126 -0.534 -0.582 -2.402 2.529 0.000 1252 21 (g) -71 912 912 1255 1261 254 222 -0.185 -1.267 -1.200 1.755 0.000 1253 21 (g) -71 924 924 1255 1261 104 254 -1.069 -0.260 -1.362 1.750 0.000 1254 -2 (ubar) -71 865 865 1255 1261 0 104 -10.208 -6.866 -13.019 17.915 0.330 1255 411 (D+) -83 1249 1254 1805 1807 0 0 -2.865 -0.367 -18.563 18.879 1.870 1256 2112 n0 83 1249 1254 0 0 0 0 -1.240 -0.445 -6.389 6.590 0.940 1257 223 (omega) -83 1249 1254 1808 1810 0 0 -0.547 -0.023 -2.246 2.440 0.778 1258 -2112 nbar0 83 1249 1254 0 0 0 0 -1.081 -1.304 -3.169 3.715 0.940 1259 -213 (rho-) -83 1249 1254 1641 1642 0 0 -0.785 -0.832 -1.799 2.306 0.880 1260 211 pi+ 83 1249 1254 0 0 0 0 -1.118 -0.240 -1.320 1.752 0.140 1261 -213 (rho-) -84 1249 1254 1643 1644 0 0 -8.612 -5.904 -10.974 15.165 0.728 1262 2 (u) -71 1193 1193 1267 1279 192 0 -0.221 -0.123 -247.626 247.627 0.685 1263 21 (g) -71 1191 1191 1267 1279 169 192 0.351 -0.427 -43.062 43.066 0.185 1264 21 (g) -71 1192 1192 1267 1279 244 169 -0.706 -0.962 -56.853 56.867 0.367 1265 21 (g) -71 1063 1063 1267 1279 305 244 -0.367 -0.871 -16.236 16.264 0.000 1266 2203 (uu_1) -71 1121 1121 1267 1279 0 305 -0.153 -0.369 -3404.870 3404.871 0.771 1267 211 pi+ 83 1262 1266 0 0 0 0 -0.090 -0.593 -229.156 229.157 0.140 1268 -211 pi- 83 1262 1266 0 0 0 0 0.119 0.251 -24.923 24.925 0.140 1269 211 pi+ 83 1262 1266 0 0 0 0 -0.031 -0.529 -17.635 17.644 0.140 1270 111 (pi0) -83 1262 1266 1811 1812 0 0 -0.468 -0.328 -30.298 30.303 0.135 1271 2114 (Delta0) -83 1262 1266 1645 1646 0 0 -0.230 -0.423 -119.112 119.120 1.297 1272 -2114 (Deltabar0) -83 1262 1266 1647 1648 0 0 0.008 -0.701 -66.152 66.167 1.237 1273 -213 (rho-) -83 1262 1266 1649 1650 0 0 -0.299 -0.096 -378.338 378.339 0.806 1274 211 pi+ 83 1262 1266 0 0 0 0 -0.278 0.120 -51.163 51.164 0.140 1275 2112 n0 83 1262 1266 0 0 0 0 0.025 -0.219 -840.549 840.549 0.940 1276 -2212 pbar- 84 1262 1266 0 0 0 0 -0.055 -0.286 -221.395 221.397 0.938 1277 211 pi+ 84 1262 1266 0 0 0 0 0.582 0.115 -649.657 649.657 0.140 1278 -211 pi- 84 1262 1266 0 0 0 0 -0.242 0.203 -237.482 237.483 0.140 1279 2224 (Delta++) -84 1262 1266 1651 1652 0 0 -0.138 -0.266 -902.789 902.789 1.095 1280 1 (d) -71 1005 1005 1291 1307 115 0 -0.103 0.004 0.146 0.375 0.330 1281 21 (g) -71 971 971 1291 1307 155 115 -0.472 -2.181 5.342 5.790 0.000 1282 21 (g) -71 1176 1176 1291 1307 345 155 -0.575 -0.593 2.699 2.829 0.191 1283 21 (g) -71 1181 1181 1291 1307 135 345 0.254 -1.040 6.115 6.237 0.598 1284 21 (g) -71 1179 1179 1291 1307 261 135 3.155 0.521 9.429 9.964 0.405 1285 21 (g) -71 965 965 1291 1307 141 261 -0.018 0.401 0.557 0.687 0.000 1286 21 (g) -71 1178 1178 1291 1307 301 141 -0.017 -0.273 -0.319 0.575 0.394 1287 21 (g) -71 1177 1177 1291 1307 152 301 -1.479 -1.292 1.142 2.293 0.309 1288 21 (g) -71 1172 1172 1291 1307 130 152 -2.232 0.203 3.520 4.173 0.079 1289 21 (g) -71 1180 1180 1291 1307 166 130 -1.773 2.247 6.814 7.405 0.458 1290 -3 (sbar) -71 1175 1175 1291 1307 0 166 0.059 0.566 2.011 2.189 0.652 1291 -213 (rho-) -83 1280 1290 1653 1654 0 0 -0.611 -1.367 3.416 3.818 0.813 1292 221 (eta) -83 1280 1290 1813 1814 0 0 -0.090 -0.100 1.594 1.691 0.548 1293 211 pi+ 83 1280 1290 0 0 0 0 0.494 -0.593 2.931 3.034 0.140 1294 3212 (Sigma0) -83 1280 1290 1815 1816 0 0 0.020 -0.984 3.820 4.121 1.193 1295 -3212 (Sigmabar0) -84 1280 1290 1817 1818 0 0 1.123 0.242 4.031 4.358 1.193 1296 -211 pi- 84 1280 1290 0 0 0 0 -0.257 -0.028 0.320 0.435 0.140 1297 111 (pi0) -84 1280 1290 1819 1820 0 0 -0.399 -0.139 0.964 1.061 0.135 1298 111 (pi0) -84 1280 1290 1821 1822 0 0 0.486 -0.439 1.936 2.048 0.135 1299 323 (K*+) -84 1280 1290 1655 1656 0 0 0.823 0.430 3.146 3.397 0.884 1300 3122 (Lambda0) -84 1280 1290 1823 1824 0 0 -0.333 -0.462 1.327 1.825 1.116 1301 -2112 nbar0 84 1280 1290 0 0 0 0 0.039 -0.507 1.688 1.998 0.940 1302 -211 pi- 84 1280 1290 0 0 0 0 0.053 0.323 0.189 0.403 0.140 1303 213 (rho+) -84 1280 1290 1657 1658 0 0 -1.547 0.427 2.064 2.733 0.796 1304 -213 (rho-) -84 1280 1290 1659 1660 0 0 -0.267 -0.328 0.773 1.134 0.714 1305 2224 (Delta++) -84 1280 1290 1661 1662 0 0 -1.415 0.280 2.484 3.178 1.360 1306 -211 pi- 84 1280 1290 0 0 0 0 0.026 -0.016 0.539 0.557 0.140 1307 -3122 (Lambdabar0) -84 1280 1290 1825 1826 0 0 -1.347 1.825 6.234 6.727 1.116 1308 2 (u) -71 1146 1146 1313 1320 282 0 4.408 -1.506 19.015 19.592 0.755 1309 21 (g) -71 903 903 1313 1320 307 282 0.753 -0.775 8.581 8.649 0.000 1310 21 (g) -71 944 944 1313 1320 299 307 0.033 -0.723 2.698 2.794 0.000 1311 21 (g) -71 1145 1145 1313 1320 110 299 -1.607 -1.484 19.048 19.176 0.294 1312 -3 (sbar) -71 872 872 1313 1320 0 110 -15.779 -14.475 155.867 157.332 0.500 1313 213 (rho+) -83 1308 1312 1663 1664 0 0 2.194 -0.716 11.470 11.731 0.865 1314 223 (omega) -83 1308 1312 1827 1829 0 0 1.496 -0.489 8.471 8.651 0.778 1315 -213 (rho-) -83 1308 1312 1665 1666 0 0 0.994 -1.535 7.377 7.635 0.728 1316 221 (eta) -83 1308 1312 1830 1831 0 0 -0.195 -0.002 4.546 4.583 0.548 1317 111 (pi0) -83 1308 1312 1832 1833 0 0 -0.642 -1.542 11.847 11.965 0.135 1318 113 (rho0) -84 1308 1312 1667 1668 0 0 -7.952 -6.626 77.117 77.813 0.806 1319 111 (pi0) -84 1308 1312 1834 1835 0 0 -1.326 -2.102 18.890 19.053 0.135 1320 321 K+ 84 1308 1312 0 0 0 0 -6.760 -5.951 65.493 66.111 0.494 1321 3 (s) -71 1152 1152 1334 1354 132 0 1.415 -2.312 20.947 21.136 0.784 1322 21 (g) -71 1038 1038 1334 1354 313 132 0.079 -0.243 10.810 10.813 0.000 1323 21 (g) -71 1030 1030 1334 1354 246 313 2.813 -0.337 123.340 123.372 0.000 1324 21 (g) -71 1149 1149 1334 1354 294 246 1.308 -0.538 68.783 68.798 0.133 1325 21 (g) -71 1154 1154 1334 1354 293 294 0.943 0.530 83.366 83.374 0.386 1326 21 (g) -71 1086 1086 1334 1354 304 293 0.654 2.462 655.391 655.396 0.000 1327 21 (g) -71 1153 1153 1334 1354 151 304 -0.732 0.818 121.887 121.893 0.282 1328 21 (g) -71 1151 1151 1334 1354 308 151 -1.331 0.696 94.694 94.706 0.186 1329 21 (g) -71 991 991 1334 1354 266 308 -0.848 -0.875 33.056 33.078 0.000 1330 21 (g) -71 983 983 1334 1354 337 266 -0.695 -0.114 34.001 34.008 0.000 1331 21 (g) -71 1150 1150 1334 1354 263 337 -0.703 -0.180 4.860 4.917 0.179 1332 21 (g) -71 1155 1155 1334 1354 217 263 -0.616 0.253 21.872 21.886 0.446 1333 -1 (dbar) -71 967 967 1334 1354 0 217 -0.680 -0.642 26.457 26.476 0.330 1334 -321 K- 83 1321 1333 0 0 0 0 0.361 -0.218 15.659 15.672 0.494 1335 213 (rho+) -83 1321 1333 1669 1670 0 0 0.666 -0.482 22.793 22.822 0.789 1336 111 (pi0) -83 1321 1333 1836 1837 0 0 0.427 -1.582 11.948 12.061 0.135 1337 -211 pi- 83 1321 1333 0 0 0 0 1.356 -0.335 24.297 24.338 0.140 1338 211 pi+ 83 1321 1333 0 0 0 0 0.214 0.279 31.139 31.141 0.140 1339 -213 (rho-) -83 1321 1333 1671 1672 0 0 0.822 -0.200 26.877 26.898 0.629 1340 221 (eta) -83 1321 1333 1838 1840 0 0 0.400 -0.354 107.789 107.792 0.548 1341 223 (omega) -83 1321 1333 1841 1843 0 0 1.386 -0.006 80.453 80.469 0.785 1342 113 (rho0) -83 1321 1333 1673 1674 0 0 0.853 0.370 93.185 93.193 0.889 1343 321 K+ 83 1321 1333 0 0 0 0 0.333 0.088 143.471 143.473 0.494 1344 3122 (Lambda0) -84 1321 1333 1844 1845 0 0 -0.826 1.534 335.349 335.355 1.116 1345 211 pi+ 84 1321 1333 0 0 0 0 0.281 0.631 60.136 60.140 0.140 1346 -2224 (Deltabar--) -84 1321 1333 1675 1676 0 0 -0.064 0.186 110.721 110.729 1.335 1347 211 pi+ 84 1321 1333 0 0 0 0 -0.280 0.116 6.903 6.911 0.140 1348 -211 pi- 84 1321 1333 0 0 0 0 -0.906 0.236 99.987 99.992 0.140 1349 223 (omega) -84 1321 1333 1846 1848 0 0 -0.376 0.223 26.594 26.609 0.767 1350 211 pi+ 84 1321 1333 0 0 0 0 -0.529 0.044 17.619 17.628 0.140 1351 -211 pi- 84 1321 1333 0 0 0 0 -0.274 -0.261 5.295 5.310 0.140 1352 321 K+ 84 1321 1333 0 0 0 0 -0.298 -0.149 16.254 16.265 0.494 1353 -323 (K*-) -84 1321 1333 1677 1678 0 0 -1.607 -0.194 35.906 35.952 0.863 1354 213 (rho+) -84 1321 1333 1679 1680 0 0 -0.332 -0.406 27.088 27.103 0.760 1355 1 (d) -71 1031 1031 1360 1370 114 0 1.836 0.563 -1.201 2.289 0.330 1356 21 (g) -71 1189 1189 1360 1370 236 114 -0.327 -0.725 159.015 159.017 0.355 1357 21 (g) -71 1190 1190 1360 1370 320 236 1.069 0.953 12.228 12.320 0.454 1358 21 (g) -71 1047 1047 1360 1370 300 320 1.964 0.901 12.382 12.569 0.000 1359 -2 (ubar) -71 1032 1032 1360 1370 0 300 0.554 0.673 2.145 2.339 0.330 1360 111 (pi0) -83 1355 1359 1849 1850 0 0 1.008 0.054 -0.499 1.134 0.135 1361 311 (K0) -83 1355 1359 1681 1681 0 0 0.585 0.033 0.116 0.777 0.498 1362 -323 (K*-) -83 1355 1359 1682 1683 0 0 0.326 0.579 0.028 1.169 0.961 1363 223 (omega) -83 1355 1359 1851 1853 0 0 -0.032 -0.069 8.413 8.449 0.780 1364 2214 (Delta+) -83 1355 1359 1684 1685 0 0 -0.475 -0.406 24.976 25.019 1.329 1365 -211 pi- 84 1355 1359 0 0 0 0 0.319 0.281 79.213 79.214 0.140 1366 -3112 (Sigmabar+) -84 1355 1359 1854 1855 0 0 0.387 0.014 39.905 39.925 1.197 1367 -311 (Kbar0) -84 1355 1359 1686 1686 0 0 0.286 0.210 3.084 3.144 0.498 1368 -211 pi- 84 1355 1359 0 0 0 0 0.271 0.076 7.167 7.174 0.140 1369 2224 (Delta++) -84 1355 1359 1687 1688 0 0 0.316 0.300 6.692 6.812 1.196 1370 -2224 (Deltabar--) -84 1355 1359 1689 1690 0 0 2.105 1.294 15.473 15.717 1.223 1371 4 (c) -71 871 871 1385 1402 109 0 2.928 -4.089 31.794 32.224 1.500 1372 21 (g) -71 898 898 1385 1402 188 109 0.540 -0.467 2.149 2.264 0.000 1373 21 (g) -71 951 951 1385 1402 327 188 1.017 -1.068 2.135 2.595 0.000 1374 21 (g) -71 916 916 1385 1402 235 327 7.069 -6.617 18.265 20.673 0.000 1375 21 (g) -71 899 899 1385 1402 257 235 1.604 -1.126 3.430 3.951 0.000 1376 21 (g) -71 926 926 1385 1402 187 257 21.205 -18.850 55.845 62.639 0.000 1377 21 (g) -71 893 893 1385 1402 176 187 33.158 -30.266 86.601 97.545 0.000 1378 21 (g) -71 1129 1129 1385 1402 348 176 21.899 -19.381 56.031 63.203 0.189 1379 21 (g) -71 958 958 1385 1402 353 348 6.474 -5.122 14.156 16.387 0.000 1380 21 (g) -71 1131 1131 1385 1402 127 353 5.933 -4.795 15.119 16.943 0.533 1381 21 (g) -71 1130 1130 1385 1402 268 127 35.925 -27.864 92.881 103.412 0.490 1382 21 (g) -71 959 959 1385 1402 354 268 8.490 -6.892 24.573 26.896 0.000 1383 21 (g) -71 930 930 1385 1402 105 354 31.983 -26.167 89.059 98.179 0.000 1384 -4 (cbar) -71 887 887 1385 1402 0 105 292.983 -236.995 831.012 912.463 1.500 1385 411 (D+) -83 1371 1384 1856 1857 0 0 2.458 -3.465 22.906 23.371 1.870 1386 313 (K*0) -83 1371 1384 1691 1692 0 0 1.031 -1.105 8.248 8.434 0.900 1387 -321 K- 83 1371 1384 0 0 0 0 0.547 -0.384 2.746 2.869 0.494 1388 111 (pi0) -83 1371 1384 1858 1859 0 0 0.204 -0.842 1.417 1.667 0.135 1389 223 (omega) -83 1371 1384 1860 1862 0 0 5.744 -4.496 14.673 16.405 0.779 1390 211 pi+ 83 1371 1384 0 0 0 0 6.811 -6.850 19.670 21.914 0.140 1391 -213 (rho-) -83 1371 1384 1693 1694 0 0 22.883 -19.993 57.658 65.180 0.755 1392 331 (eta') -83 1371 1384 1863 1865 0 0 35.384 -31.560 91.462 103.025 0.958 1393 213 (rho+) -83 1371 1384 1695 1696 0 0 13.430 -11.979 34.021 38.502 1.066 1394 -213 (rho-) -83 1371 1384 1697 1698 0 0 7.571 -5.796 18.866 21.153 0.798 1395 213 (rho+) -84 1371 1384 1699 1700 0 0 24.297 -19.954 62.261 69.753 0.754 1396 111 (pi0) -84 1371 1384 1866 1867 0 0 7.729 -5.456 21.490 23.481 0.135 1397 -211 pi- 84 1371 1384 0 0 0 0 16.518 -13.978 45.182 50.097 0.140 1398 211 pi+ 84 1371 1384 0 0 0 0 3.709 -2.820 9.506 10.588 0.140 1399 -211 pi- 84 1371 1384 0 0 0 0 12.437 -9.906 33.823 37.374 0.140 1400 211 pi+ 84 1371 1384 0 0 0 0 15.705 -12.495 45.151 49.411 0.140 1401 -211 pi- 84 1371 1384 0 0 0 0 3.057 -2.417 7.898 8.809 0.140 1402 -423 (D*bar0) -84 1371 1384 1868 1869 0 0 291.694 -236.203 826.070 907.344 2.007 1403 4 (c) -71 863 863 1426 1460 101 0 78.618 -62.775 218.954 240.966 1.500 1404 21 (g) -71 938 938 1426 1460 285 101 6.661 -4.857 17.165 19.042 0.000 1405 21 (g) -71 888 888 1426 1460 154 285 5.159 -3.324 15.191 16.384 0.000 1406 21 (g) -71 1125 1125 1426 1460 338 154 0.693 -0.535 2.022 2.238 0.393 1407 21 (g) -71 869 869 1426 1460 138 338 -0.739 -0.604 4.284 4.389 0.000 1408 21 (g) -71 960 960 1426 1460 358 138 0.625 -4.305 21.345 21.784 0.000 1409 21 (g) -71 918 918 1426 1460 240 358 1.205 -5.554 32.428 32.923 0.000 1410 21 (g) -71 881 881 1426 1460 113 240 1.335 -2.969 17.194 17.499 0.000 1411 21 (g) -71 875 875 1426 1460 349 113 1.463 -4.118 12.895 13.616 0.000 1412 21 (g) -71 956 956 1426 1460 270 349 0.606 -2.821 10.476 10.867 0.000 1413 21 (g) -71 1124 1124 1426 1460 318 270 10.563 -36.287 131.841 137.151 0.218 1414 21 (g) -71 948 948 1426 1460 108 318 1.705 -7.619 27.917 28.988 0.000 1415 21 (g) -71 922 922 1426 1460 248 108 0.035 0.060 0.081 0.107 0.000 1416 21 (g) -71 891 891 1426 1460 182 248 4.163 -9.534 23.221 25.445 0.000 1417 21 (g) -71 947 947 1426 1460 314 182 2.911 -4.762 9.202 10.763 0.000 1418 21 (g) -71 895 895 1426 1460 310 314 4.541 -7.525 16.785 18.947 0.000 1419 21 (g) -71 1126 1126 1426 1460 107 310 1.453 -2.074 4.698 5.353 0.422 1420 21 (g) -71 1128 1128 1426 1460 243 107 1.230 -1.581 7.933 8.198 0.506 1421 21 (g) -71 873 873 1426 1460 137 243 2.735 -6.531 21.107 22.263 0.000 1422 21 (g) -71 880 880 1426 1460 111 137 1.568 -13.090 28.258 31.182 0.000 1423 21 (g) -71 933 933 1426 1460 324 111 -0.091 -0.073 0.042 0.124 0.000 1424 21 (g) -71 1127 1127 1426 1460 238 324 0.131 -3.714 7.349 8.248 0.457 1425 -2 (ubar) -71 1123 1123 1426 1460 0 238 6.548 -1.817 26.713 27.566 0.353 1426 413 (D*+) -83 1403 1425 1870 1871 0 0 67.475 -53.672 187.616 206.489 2.010 1427 -211 pi- 83 1403 1425 0 0 0 0 2.294 -1.571 5.728 6.368 0.140 1428 213 (rho+) -83 1403 1425 1701 1702 0 0 12.460 -9.968 35.245 38.695 0.703 1429 111 (pi0) -83 1403 1425 1872 1873 0 0 4.189 -3.035 11.410 12.529 0.135 1430 -211 pi- 83 1403 1425 0 0 0 0 2.113 -2.181 7.449 8.046 0.140 1431 211 pi+ 83 1403 1425 0 0 0 0 0.206 0.528 1.712 1.809 0.140 1432 113 (rho0) -83 1403 1425 1703 1704 0 0 1.958 -2.181 7.445 8.042 0.814 1433 -213 (rho-) -83 1403 1425 1705 1706 0 0 0.166 -1.517 9.504 9.663 0.851 1434 113 (rho0) -83 1403 1425 1707 1708 0 0 1.394 -5.428 28.424 28.994 1.150 1435 211 pi+ 83 1403 1425 0 0 0 0 -0.242 -0.497 1.698 1.792 0.140 1436 111 (pi0) -83 1403 1425 1874 1875 0 0 0.936 -3.291 16.308 16.663 0.135 1437 -213 (rho-) -83 1403 1425 1709 1710 0 0 0.562 -2.593 14.313 14.580 0.833 1438 211 pi+ 83 1403 1425 0 0 0 0 0.909 -2.645 11.747 12.077 0.140 1439 -213 (rho-) -83 1403 1425 1711 1712 0 0 5.817 -19.656 71.582 74.464 0.846 1440 211 pi+ 83 1403 1425 0 0 0 0 0.219 -2.550 9.795 10.125 0.140 1441 221 (eta) -83 1403 1425 1876 1877 0 0 1.532 -5.065 16.261 17.110 0.548 1442 111 (pi0) -83 1403 1425 1878 1879 0 0 3.137 -9.416 35.283 36.653 0.135 1443 221 (eta) -83 1403 1425 1880 1881 0 0 3.509 -11.459 41.714 43.405 0.548 1444 -211 pi- 83 1403 1425 0 0 0 0 -0.027 -0.380 0.689 0.799 0.140 1445 211 pi+ 83 1403 1425 0 0 0 0 0.347 -1.932 4.825 5.211 0.140 1446 111 (pi0) -83 1403 1425 1882 1883 0 0 3.181 -7.174 16.808 18.551 0.135 1447 223 (omega) -84 1403 1425 1884 1886 0 0 3.944 -5.341 13.071 14.682 0.781 1448 111 (pi0) -84 1403 1425 1887 1888 0 0 1.421 -2.965 5.245 6.192 0.135 1449 -213 (rho-) -84 1403 1425 1713 1714 0 0 2.354 -3.870 8.153 9.348 0.634 1450 213 (rho+) -84 1403 1425 1715 1716 0 0 1.630 -2.381 8.698 9.204 0.852 1451 3112 (Sigma-) -84 1403 1425 1889 1890 0 0 1.740 -5.866 15.988 17.160 1.197 1452 -3112 (Sigmabar+) -84 1403 1425 1891 1892 0 0 2.253 -4.912 14.297 15.331 1.197 1453 -211 pi- 84 1403 1425 0 0 0 0 -0.060 -3.903 8.153 9.041 0.140 1454 213 (rho+) -84 1403 1425 1717 1718 0 0 0.276 -1.290 4.352 4.612 0.767 1455 221 (eta) -84 1403 1425 1893 1894 0 0 1.140 -6.383 14.247 15.662 0.548 1456 -213 (rho-) -84 1403 1425 1719 1720 0 0 0.314 -0.933 2.545 2.844 0.799 1457 323 (K*+) -84 1403 1425 1721 1722 0 0 0.238 -0.846 3.402 3.627 0.901 1458 -311 (Kbar0) -84 1403 1425 1723 1723 0 0 3.367 -0.652 11.642 12.147 0.498 1459 223 (omega) -84 1403 1425 1895 1897 0 0 1.691 -1.344 8.729 9.028 0.793 1460 -211 pi- 84 1403 1425 0 0 0 0 0.677 -0.037 3.021 3.099 0.140 1461 2 (u) -71 1134 1134 1480 1505 298 0 1.143 -1.978 -3.093 3.877 0.500 1462 21 (g) -71 1137 1137 1480 1505 120 298 -0.764 -0.550 -1.557 1.881 0.477 1463 21 (g) -71 894 894 1480 1505 220 120 -0.662 0.416 -5.008 5.068 0.000 1464 21 (g) -71 1135 1135 1480 1505 140 220 0.941 1.243 -2.771 3.186 0.202 1465 21 (g) -71 1140 1140 1480 1505 283 140 13.393 12.142 -51.399 54.488 0.539 1466 21 (g) -71 915 915 1480 1505 205 283 2.956 3.073 -13.944 14.581 0.000 1467 21 (g) -71 904 904 1480 1505 125 205 2.079 1.362 -7.739 8.129 0.000 1468 21 (g) -71 1139 1139 1480 1505 350 125 10.164 4.101 -30.420 32.338 0.528 1469 21 (g) -71 1136 1136 1480 1505 291 350 0.466 0.520 -1.168 1.391 0.290 1470 21 (g) -71 1013 1013 1480 1505 284 291 2.571 0.533 -3.924 4.721 0.000 1471 21 (g) -71 1132 1132 1480 1505 174 284 2.608 -0.752 -3.548 4.468 0.087 1472 21 (g) -71 892 892 1480 1505 175 174 2.191 -0.381 -3.995 4.572 0.000 1473 21 (g) -71 886 886 1480 1505 267 175 4.231 1.056 -12.320 13.069 0.000 1474 21 (g) -71 929 929 1480 1505 295 267 0.510 0.904 -1.682 1.976 0.000 1475 21 (g) -71 941 941 1480 1505 147 295 -0.077 -0.225 -0.388 0.456 0.000 1476 21 (g) -71 1138 1138 1480 1505 277 147 0.557 -0.013 0.053 0.757 0.510 1477 21 (g) -71 934 934 1480 1505 102 277 0.462 -1.751 1.542 2.379 0.000 1478 21 (g) -71 900 900 1480 1505 193 102 4.212 -6.510 6.706 10.252 0.000 1479 -4 (cbar) -71 870 870 1480 1505 0 193 14.485 -17.579 19.090 29.757 1.500 1480 211 pi+ 83 1461 1479 0 0 0 0 0.539 -1.972 -3.766 4.288 0.140 1481 -211 pi- 83 1461 1479 0 0 0 0 -0.219 0.374 -0.114 0.470 0.140 1482 213 (rho+) -83 1461 1479 1724 1725 0 0 -0.078 -0.592 -4.320 4.434 0.802 1483 223 (omega) -83 1461 1479 1898 1900 0 0 0.816 0.930 -1.834 2.347 0.783 1484 311 (K0) -83 1461 1479 1726 1726 0 0 0.105 0.463 -4.607 4.658 0.498 1485 -313 (K*bar0) -83 1461 1479 1727 1728 0 0 3.280 3.156 -12.365 13.206 0.896 1486 -211 pi- 83 1461 1479 0 0 0 0 0.499 0.453 -1.801 1.928 0.140 1487 113 (rho0) -83 1461 1479 1729 1730 0 0 6.803 6.496 -27.552 29.124 0.787 1488 211 pi+ 83 1461 1479 0 0 0 0 2.609 2.754 -11.608 12.213 0.140 1489 223 (omega) -83 1461 1479 1901 1903 0 0 3.435 2.294 -11.563 12.304 0.778 1490 -211 pi- 83 1461 1479 0 0 0 0 4.098 1.907 -12.212 13.022 0.140 1491 223 (omega) -83 1461 1479 1904 1905 0 0 1.570 1.249 -5.635 6.034 0.792 1492 211 pi+ 83 1461 1479 0 0 0 0 4.772 1.243 -13.487 14.361 0.140 1493 -211 pi- 84 1461 1479 0 0 0 0 0.314 0.765 -2.142 2.300 0.140 1494 211 pi+ 84 1461 1479 0 0 0 0 3.785 -0.017 -5.989 7.086 0.140 1495 311 (K0) -84 1461 1479 1731 1731 0 0 1.832 1.619 -6.173 6.658 0.498 1496 -323 (K*-) -84 1461 1479 1732 1733 0 0 3.798 -0.332 -7.249 8.238 0.883 1497 323 (K*+) -84 1461 1479 1734 1735 0 0 1.189 -0.289 -3.153 3.494 0.875 1498 -323 (K*-) -84 1461 1479 1736 1737 0 0 3.106 0.893 -6.739 7.523 0.860 1499 211 pi+ 84 1461 1479 0 0 0 0 -0.395 -0.086 -0.333 0.542 0.140 1500 221 (eta) -84 1461 1479 1906 1907 0 0 -0.204 -0.384 0.391 0.802 0.548 1501 -211 pi- 84 1461 1479 0 0 0 0 0.709 -0.388 -0.084 0.825 0.140 1502 321 K+ 84 1461 1479 0 0 0 0 3.585 -4.819 5.319 8.038 0.494 1503 -311 (Kbar0) -84 1461 1479 1738 1738 0 0 1.689 -2.138 2.392 3.659 0.498 1504 -211 pi- 84 1461 1479 0 0 0 0 1.999 -1.642 1.574 3.032 0.140 1505 -423 (D*bar0) -84 1461 1479 1908 1909 0 0 11.827 -16.324 17.487 26.761 2.007 1506 2 (u) -71 981 981 1530 1556 206 0 0.075 0.272 0.610 0.749 0.330 1507 21 (g) -71 989 989 1530 1556 339 206 0.415 0.827 -0.184 0.943 0.000 1508 21 (g) -71 1007 1007 1530 1556 289 339 -0.002 0.425 0.489 0.648 0.000 1509 21 (g) -71 1164 1164 1530 1556 250 289 0.036 0.780 0.061 0.811 0.210 1510 21 (g) -71 1169 1169 1530 1556 233 250 2.350 2.631 -1.287 3.775 0.389 1511 21 (g) -71 1160 1160 1530 1556 259 233 0.760 0.224 -0.572 0.982 0.100 1512 21 (g) -71 1166 1166 1530 1556 311 259 0.434 0.878 -2.211 2.434 0.275 1513 21 (g) -71 1163 1163 1530 1556 149 311 1.374 2.126 0.521 2.589 0.156 1514 21 (g) -71 969 969 1530 1556 230 149 1.030 -0.058 0.489 1.142 0.000 1515 21 (g) -71 1161 1161 1530 1556 117 230 -0.312 0.612 -0.095 0.702 0.111 1516 21 (g) -71 982 982 1530 1556 210 117 -0.094 -0.148 0.089 0.197 0.000 1517 21 (g) -71 1003 1003 1530 1556 322 210 -0.373 0.253 -0.714 0.844 0.000 1518 21 (g) -71 1167 1167 1530 1556 303 322 -1.815 0.646 -0.013 1.956 0.338 1519 21 (g) -71 999 999 1530 1556 124 303 -1.258 -0.142 -0.410 1.331 0.000 1520 21 (g) -71 1165 1165 1530 1556 351 124 -0.652 -0.739 -6.915 6.989 0.250 1521 21 (g) -71 1159 1159 1530 1556 359 351 -0.831 0.082 -7.638 7.684 0.080 1522 21 (g) -71 1081 1081 1530 1556 145 359 -0.170 0.600 -3.617 3.670 0.000 1523 21 (g) -71 1158 1158 1530 1556 333 145 0.017 0.612 -10.238 10.256 0.063 1524 21 (g) -71 1097 1097 1530 1556 357 333 -0.642 0.167 -12.639 12.656 0.000 1525 21 (g) -71 1085 1085 1530 1556 229 357 0.210 0.253 -12.783 12.787 0.000 1526 21 (g) -71 1170 1170 1530 1556 343 229 -1.608 1.509 -169.732 169.747 0.469 1527 21 (g) -71 1048 1048 1530 1556 309 343 -0.298 0.398 -281.050 281.050 0.000 1528 21 (g) -71 1168 1168 1530 1556 335 309 -2.568 0.554 -900.241 900.245 0.385 1529 -2 (ubar) -71 1066 1066 1530 1556 0 335 0.131 -0.187 -257.584 257.584 0.330 1530 211 pi+ 83 1506 1529 0 0 0 0 0.543 0.477 0.020 0.736 0.140 1531 111 (pi0) -83 1506 1529 1910 1911 0 0 -0.275 0.932 -0.070 0.984 0.135 1532 -211 pi- 83 1506 1529 0 0 0 0 0.164 0.099 0.464 0.521 0.140 1533 211 pi+ 83 1506 1529 0 0 0 0 0.283 0.566 0.109 0.657 0.140 1534 223 (omega) -83 1506 1529 1912 1914 0 0 1.126 1.170 -0.339 1.835 0.784 1535 -211 pi- 83 1506 1529 0 0 0 0 0.185 0.102 -0.292 0.386 0.140 1536 213 (rho+) -83 1506 1529 1739 1740 0 0 0.411 1.085 -1.012 1.918 1.143 1537 221 (eta) -83 1506 1529 1915 1916 0 0 1.437 1.747 -0.263 2.342 0.548 1538 223 (omega) -83 1506 1529 1917 1919 0 0 0.508 0.553 -0.298 1.125 0.782 1539 -211 pi- 83 1506 1529 0 0 0 0 0.127 -0.169 -0.339 0.423 0.140 1540 223 (omega) -83 1506 1529 1920 1922 0 0 0.802 1.190 -0.443 1.689 0.772 1541 3212 (Sigma0) -84 1506 1529 1923 1924 0 0 0.122 0.238 -0.184 1.236 1.193 1542 331 (eta') -84 1506 1529 1925 1927 0 0 -0.053 0.394 -0.036 1.037 0.958 1543 -3122 (Lambdabar0) -84 1506 1529 1928 1929 0 0 -0.577 0.634 0.416 1.467 1.116 1544 3222 (Sigma+) -84 1506 1529 1930 1931 0 0 -1.393 -0.088 -1.400 2.307 1.189 1545 -3212 (Sigmabar0) -84 1506 1529 1932 1933 0 0 -0.263 0.255 -1.588 2.019 1.193 1546 2112 n0 84 1506 1529 0 0 0 0 -0.729 0.031 -2.042 2.363 0.940 1547 113 (rho0) -84 1506 1529 1741 1742 0 0 -0.394 -0.067 -4.911 4.996 0.828 1548 -2212 pbar- 84 1506 1529 0 0 0 0 -0.242 0.422 -3.156 3.328 0.938 1549 223 (omega) -84 1506 1529 1934 1935 0 0 -1.102 0.035 -32.169 32.197 0.783 1550 113 (rho0) -84 1506 1529 1743 1744 0 0 0.141 0.178 -8.436 8.474 0.764 1551 211 pi+ 84 1506 1529 0 0 0 0 -0.738 0.801 -57.675 57.686 0.140 1552 2114 (Delta0) -84 1506 1529 1745 1746 0 0 0.116 0.183 -79.645 79.655 1.211 1553 -2214 (Deltabar-) -84 1506 1529 1747 1748 0 0 -0.816 0.770 -119.650 119.662 1.263 1554 223 (omega) -84 1506 1529 1936 1938 0 0 -1.441 0.931 -377.007 377.012 0.785 1555 2212 p+ 84 1506 1529 0 0 0 0 -0.474 -0.077 -364.456 364.457 0.938 1556 -2212 pbar- 84 1506 1529 0 0 0 0 -1.259 0.180 -611.258 611.260 0.938 1557 2 (u) -71 1084 1084 1569 1591 116 0 0.175 -0.423 377.518 377.519 0.330 1558 21 (g) -71 1108 1108 1569 1591 170 116 0.245 -0.422 -7.187 7.203 0.000 1559 21 (g) -71 1101 1101 1569 1591 255 170 1.983 -0.548 -16.677 16.804 0.000 1560 21 (g) -71 1198 1198 1569 1591 302 255 -0.194 -0.929 -3.411 3.549 0.248 1561 21 (g) -71 964 964 1569 1591 202 302 -1.026 -2.790 -3.550 4.631 0.000 1562 21 (g) -71 1199 1199 1569 1591 346 202 0.161 -2.327 -1.198 2.639 0.295 1563 21 (g) -71 1196 1196 1569 1591 275 346 0.443 -0.626 -1.433 1.628 0.101 1564 21 (g) -71 1200 1200 1569 1591 245 275 -0.977 -0.414 -1.327 1.729 0.320 1565 21 (g) -71 1201 1201 1569 1591 231 245 0.975 -0.684 0.291 1.310 0.462 1566 21 (g) -71 977 977 1569 1591 326 231 -0.286 -0.893 -1.068 1.422 0.000 1567 21 (g) -71 1195 1195 1569 1591 201 326 0.361 0.426 0.565 0.798 0.071 1568 -1 (dbar) -71 973 973 1569 1591 0 201 -0.041 -0.017 1.217 1.262 0.330 1569 223 (omega) -83 1557 1568 1939 1941 0 0 -0.125 -0.083 137.135 137.137 0.784 1570 221 (eta) -83 1557 1568 1942 1944 0 0 0.034 0.137 208.758 208.759 0.548 1571 213 (rho+) -83 1557 1568 1749 1750 0 0 0.207 -0.930 22.283 22.329 1.087 1572 -211 pi- 83 1557 1568 0 0 0 0 0.104 0.117 0.835 0.861 0.140 1573 213 (rho+) -83 1557 1568 1751 1752 0 0 0.183 0.169 5.439 5.494 0.732 1574 2112 n0 83 1557 1568 0 0 0 0 -0.476 -0.051 2.508 2.720 0.940 1575 -2112 nbar0 83 1557 1568 0 0 0 0 0.483 0.206 -1.184 1.600 0.940 1576 111 (pi0) -83 1557 1568 1945 1946 0 0 -0.170 -0.004 -0.021 0.218 0.135 1577 -211 pi- 83 1557 1568 0 0 0 0 0.195 -0.064 -0.256 0.357 0.140 1578 211 pi+ 83 1557 1568 0 0 0 0 0.022 0.139 -1.250 1.266 0.140 1579 -213 (rho-) -83 1557 1568 1753 1754 0 0 0.726 -0.484 -8.662 8.728 0.625 1580 323 (K*+) -83 1557 1568 1755 1756 0 0 0.031 -0.977 -6.512 6.643 0.871 1581 -323 (K*-) -83 1557 1568 1757 1758 0 0 0.735 -0.097 -5.753 5.857 0.815 1582 111 (pi0) -83 1557 1568 1947 1948 0 0 -0.159 -1.092 -1.493 1.862 0.135 1583 111 (pi0) -83 1557 1568 1949 1950 0 0 -0.300 -0.552 -0.318 0.717 0.135 1584 211 pi+ 83 1557 1568 0 0 0 0 0.233 -0.567 -3.708 3.761 0.140 1585 223 (omega) -84 1557 1568 1951 1953 0 0 -0.140 -1.357 -1.268 2.024 0.794 1586 113 (rho0) -84 1557 1568 1759 1760 0 0 -0.160 -2.459 -1.929 3.214 0.732 1587 313 (K*0) -84 1557 1568 1761 1762 0 0 0.055 0.044 -0.268 0.946 0.905 1588 -311 (Kbar0) -84 1557 1568 1763 1763 0 0 -0.246 -1.561 -2.010 2.605 0.498 1589 223 (omega) -84 1557 1568 1954 1956 0 0 0.556 -0.139 1.614 1.889 0.795 1590 -213 (rho-) -84 1557 1568 1764 1765 0 0 0.055 -0.276 -0.085 1.209 1.172 1591 211 pi+ 84 1557 1568 0 0 0 0 -0.023 0.235 -0.114 0.297 0.140 1592 1 (d) -71 1119 1119 1600 1618 148 0 -0.048 0.212 537.730 537.730 0.330 1593 21 (g) -71 884 884 1600 1618 264 148 -0.197 -1.179 -20.281 20.316 0.000 1594 21 (g) -71 927 927 1600 1618 331 264 -0.427 -0.576 -19.637 19.650 0.000 1595 21 (g) -71 952 952 1600 1618 156 331 0.293 0.041 -11.793 11.797 0.000 1596 21 (g) -71 919 919 1600 1618 241 156 0.305 -0.287 -2.534 2.569 0.000 1597 21 (g) -71 1016 1016 1600 1618 260 241 2.193 -0.156 -16.443 16.589 0.000 1598 21 (g) -71 889 889 1600 1618 203 260 0.805 0.814 -6.372 6.474 0.000 1599 -4 (cbar) -71 1142 1142 1600 1618 0 203 -4.315 -1.477 -9.372 10.576 1.796 1600 -213 (rho-) -83 1592 1599 1766 1767 0 0 -0.163 0.434 481.231 481.232 0.685 1601 213 (rho+) -83 1592 1599 1768 1769 0 0 -0.021 -0.275 47.402 47.414 1.036 1602 -211 pi- 83 1592 1599 0 0 0 0 0.247 0.078 3.187 3.200 0.140 1603 223 (omega) -83 1592 1599 1957 1959 0 0 -0.274 0.474 3.889 4.005 0.785 1604 213 (rho+) -83 1592 1599 1770 1771 0 0 -0.164 -0.470 0.659 1.559 1.321 1605 -211 pi- 83 1592 1599 0 0 0 0 0.278 0.146 0.468 0.580 0.140 1606 211 pi+ 83 1592 1599 0 0 0 0 0.289 -0.003 -0.148 0.354 0.140 1607 -211 pi- 83 1592 1599 0 0 0 0 -0.351 -0.299 -0.154 0.506 0.140 1608 113 (rho0) -83 1592 1599 1772 1773 0 0 0.163 -0.236 -7.983 8.042 0.926 1609 111 (pi0) -83 1592 1599 1960 1961 0 0 0.016 -0.544 -6.353 6.378 0.135 1610 111 (pi0) -83 1592 1599 1962 1963 0 0 -0.199 -0.239 -6.551 6.560 0.135 1611 113 (rho0) -83 1592 1599 1774 1775 0 0 0.242 -0.260 -17.978 18.001 0.830 1612 211 pi+ 83 1592 1599 0 0 0 0 0.909 -0.107 -3.065 3.202 0.140 1613 223 (omega) -84 1592 1599 1964 1966 0 0 0.109 0.311 -12.957 12.985 0.782 1614 -211 pi- 84 1592 1599 0 0 0 0 0.175 -0.359 -4.766 4.785 0.140 1615 213 (rho+) -84 1592 1599 1776 1777 0 0 0.690 -0.565 -12.877 12.944 0.969 1616 221 (eta) -84 1592 1599 1967 1969 0 0 0.522 0.333 -2.249 2.396 0.548 1617 113 (rho0) -84 1592 1599 1778 1779 0 0 -0.812 -0.673 -3.122 3.359 0.652 1618 -413 (D*-) -84 1592 1599 1970 1971 0 0 -3.045 -0.355 -7.334 8.199 2.010 1619 211 pi+ 91 1204 0 0 0 0 0 -0.104 0.568 11.392 11.408 0.140 1620 111 (pi0) -91 1204 0 1972 1973 0 0 0.784 2.089 44.662 44.718 0.135 1621 321 K+ 91 1210 0 0 0 0 0 -0.280 0.096 175.587 175.588 0.494 1622 111 (pi0) -91 1210 0 1974 1975 0 0 -0.015 -0.266 30.623 30.624 0.135 1623 211 pi+ 91 1211 0 0 0 0 0 0.049 -0.369 202.681 202.682 0.140 1624 111 (pi0) -91 1211 0 1976 1977 0 0 -0.527 -0.067 401.049 401.049 0.135 1625 -321 K- 91 1219 0 0 0 0 0 -1.653 -0.837 12.981 13.122 0.494 1626 211 pi+ 91 1219 0 0 0 0 0 -0.165 -0.342 3.474 3.497 0.140 1627 311 (K0) -91 1220 0 1780 1780 0 0 -1.259 -0.491 9.538 9.646 0.498 1628 111 (pi0) -91 1220 0 1978 1979 0 0 -1.682 -0.369 14.657 14.758 0.135 1629 211 pi+ 91 1222 0 0 0 0 0 -1.462 -0.371 8.916 9.044 0.140 1630 111 (pi0) -91 1222 0 1980 1981 0 0 -0.052 0.146 2.043 2.053 0.135 1631 130 K_L0 91 1223 1223 0 0 0 0 -0.262 0.239 15.254 15.266 0.498 1632 310 (K_S0) -91 1224 1224 1982 1983 0 0 -0.364 0.891 10.469 10.525 0.498 1633 2112 n0 91 1233 0 0 0 0 0 -0.483 0.445 6.869 6.964 0.940 1634 211 pi+ 91 1233 0 0 0 0 0 -0.360 0.108 1.539 1.590 0.140 1635 -311 (Kbar0) -91 1238 0 1781 1781 0 0 0.693 0.476 0.509 1.102 0.498 1636 -211 pi- 91 1238 0 0 0 0 0 -0.072 -0.093 0.067 0.194 0.140 1637 211 pi+ 91 1243 0 0 0 0 0 0.218 -0.092 -4.589 4.597 0.140 1638 -211 pi- 91 1243 0 0 0 0 0 -0.494 0.516 -20.202 20.215 0.140 1639 -321 K- 91 1246 0 0 0 0 0 -0.372 0.273 -2.938 3.014 0.494 1640 111 (pi0) -91 1246 0 1984 1985 0 0 -0.006 -0.359 -2.896 2.921 0.135 1641 -211 pi- 91 1259 0 0 0 0 0 -0.889 -0.463 -1.464 1.780 0.140 1642 111 (pi0) -91 1259 0 1986 1987 0 0 0.104 -0.369 -0.335 0.527 0.135 1643 -211 pi- 91 1261 0 0 0 0 0 -8.012 -5.539 -10.384 14.238 0.140 1644 111 (pi0) -91 1261 0 1988 1989 0 0 -0.600 -0.366 -0.589 0.927 0.135 1645 2112 n0 91 1271 0 0 0 0 0 -0.368 -0.222 -74.525 74.532 0.940 1646 111 (pi0) -91 1271 0 1990 1991 0 0 0.138 -0.201 -44.587 44.588 0.135 1647 -2212 pbar- 91 1272 0 0 0 0 0 -0.030 -0.810 -58.529 58.542 0.938 1648 211 pi+ 91 1272 0 0 0 0 0 0.038 0.109 -7.623 7.625 0.140 1649 -211 pi- 91 1273 0 0 0 0 0 0.228 -0.102 -84.250 84.250 0.140 1650 111 (pi0) -91 1273 0 1992 1993 0 0 -0.527 0.006 -294.089 294.089 0.135 1651 2212 p+ 91 1279 0 0 0 0 0 -0.143 -0.175 -742.590 742.591 0.938 1652 211 pi+ 91 1279 0 0 0 0 0 0.005 -0.091 -160.199 160.199 0.140 1653 -211 pi- 91 1291 0 0 0 0 0 -0.740 -1.262 2.753 3.121 0.140 1654 111 (pi0) -91 1291 0 1994 1995 0 0 0.128 -0.104 0.663 0.697 0.135 1655 311 (K0) -91 1299 0 1782 1782 0 0 0.631 0.015 1.956 2.115 0.498 1656 211 pi+ 91 1299 0 0 0 0 0 0.192 0.416 1.189 1.282 0.140 1657 211 pi+ 91 1303 0 0 0 0 0 -0.522 0.228 0.254 0.639 0.140 1658 111 (pi0) -91 1303 0 1996 1997 0 0 -1.025 0.199 1.810 2.094 0.135 1659 -211 pi- 91 1304 0 0 0 0 0 0.057 0.076 -0.028 0.171 0.140 1660 111 (pi0) -91 1304 0 1998 1999 0 0 -0.324 -0.403 0.801 0.963 0.135 1661 2212 p+ 91 1305 0 0 0 0 0 -1.303 0.515 2.090 2.686 0.938 1662 211 pi+ 91 1305 0 0 0 0 0 -0.111 -0.235 0.394 0.492 0.140 1663 211 pi+ 91 1313 0 0 0 0 0 0.617 -0.598 3.647 3.750 0.140 1664 111 (pi0) -91 1313 0 2000 2001 0 0 1.576 -0.118 7.822 7.982 0.135 1665 -211 pi- 91 1315 0 0 0 0 0 0.384 -0.256 1.143 1.240 0.140 1666 111 (pi0) -91 1315 0 2002 2003 0 0 0.609 -1.279 6.234 6.394 0.135 1667 211 pi+ 91 1318 0 0 0 0 0 -5.489 -4.202 52.943 53.393 0.140 1668 -211 pi- 91 1318 0 0 0 0 0 -2.463 -2.424 24.174 24.420 0.140 1669 211 pi+ 91 1335 0 0 0 0 0 0.654 -0.068 16.308 16.322 0.140 1670 111 (pi0) -91 1335 0 2004 2005 0 0 0.012 -0.414 6.485 6.500 0.135 1671 -211 pi- 91 1339 0 0 0 0 0 0.691 -0.131 13.405 13.424 0.140 1672 111 (pi0) -91 1339 0 2006 2007 0 0 0.130 -0.069 13.472 13.474 0.135 1673 211 pi+ 91 1342 0 0 0 0 0 0.947 0.361 62.052 62.060 0.140 1674 -211 pi- 91 1342 0 0 0 0 0 -0.094 0.009 31.133 31.133 0.140 1675 -2212 pbar- 91 1346 0 0 0 0 0 -0.062 -0.126 93.559 93.564 0.938 1676 -211 pi- 91 1346 0 0 0 0 0 -0.002 0.313 17.162 17.166 0.140 1677 -311 (Kbar0) -91 1353 0 1783 1783 0 0 -0.777 -0.220 22.858 22.878 0.498 1678 -211 pi- 91 1353 0 0 0 0 0 -0.830 0.026 13.047 13.074 0.140 1679 211 pi+ 91 1354 0 0 0 0 0 0.206 -0.061 5.715 5.720 0.140 1680 111 (pi0) -91 1354 0 2008 2009 0 0 -0.538 -0.345 21.373 21.383 0.135 1681 310 (K_S0) -91 1361 1361 2010 2011 0 0 0.585 0.033 0.116 0.777 0.498 1682 -311 (Kbar0) -91 1362 0 1784 1784 0 0 -0.073 0.148 -0.139 0.542 0.498 1683 -211 pi- 91 1362 0 0 0 0 0 0.400 0.430 0.167 0.626 0.140 1684 2212 p+ 91 1364 0 0 0 0 0 -0.643 -0.191 20.902 20.934 0.938 1685 111 (pi0) -91 1364 0 2012 2013 0 0 0.168 -0.215 4.074 4.085 0.135 1686 310 (K_S0) -91 1367 1367 2014 2015 0 0 0.286 0.210 3.084 3.144 0.498 1687 2212 p+ 91 1369 0 0 0 0 0 0.403 0.360 6.070 6.166 0.938 1688 211 pi+ 91 1369 0 0 0 0 0 -0.087 -0.060 0.622 0.646 0.140 1689 -2212 pbar- 91 1370 0 0 0 0 0 1.702 1.053 13.709 13.886 0.938 1690 -211 pi- 91 1370 0 0 0 0 0 0.402 0.240 1.764 1.831 0.140 1691 311 (K0) -91 1386 0 1785 1785 0 0 0.659 -0.704 3.865 4.015 0.498 1692 111 (pi0) -91 1386 0 2016 2017 0 0 0.372 -0.401 4.383 4.419 0.135 1693 -211 pi- 91 1391 0 0 0 0 0 4.010 -3.844 10.565 11.937 0.140 1694 111 (pi0) -91 1391 0 2018 2019 0 0 18.874 -16.149 47.093 53.243 0.135 1695 211 pi+ 91 1393 0 0 0 0 0 4.033 -2.995 9.298 10.569 0.140 1696 111 (pi0) -91 1393 0 2020 2021 0 0 9.397 -8.984 24.722 27.932 0.135 1697 -211 pi- 91 1394 0 0 0 0 0 0.445 -0.400 1.522 1.641 0.140 1698 111 (pi0) -91 1394 0 2022 2023 0 0 7.126 -5.396 17.344 19.512 0.135 1699 211 pi+ 91 1395 0 0 0 0 0 9.172 -7.252 22.582 25.430 0.140 1700 111 (pi0) -91 1395 0 2024 2025 0 0 15.125 -12.702 39.679 44.323 0.135 1701 211 pi+ 91 1428 0 0 0 0 0 1.544 -1.485 4.707 5.174 0.140 1702 111 (pi0) -91 1428 0 2026 2027 0 0 10.916 -8.483 30.537 33.521 0.135 1703 211 pi+ 91 1432 0 0 0 0 0 0.801 -0.399 1.981 2.178 0.140 1704 -211 pi- 91 1432 0 0 0 0 0 1.157 -1.783 5.464 5.865 0.140 1705 -211 pi- 91 1433 0 0 0 0 0 -0.178 -0.054 1.037 1.063 0.140 1706 111 (pi0) -91 1433 0 2028 2029 0 0 0.345 -1.463 8.466 8.600 0.135 1707 211 pi+ 91 1434 0 0 0 0 0 0.704 -2.658 11.134 11.470 0.140 1708 -211 pi- 91 1434 0 0 0 0 0 0.690 -2.770 17.290 17.524 0.140 1709 -211 pi- 91 1437 0 0 0 0 0 -0.037 -1.564 8.784 8.923 0.140 1710 111 (pi0) -91 1437 0 2030 2031 0 0 0.599 -1.029 5.529 5.658 0.135 1711 -211 pi- 91 1439 0 0 0 0 0 3.409 -12.820 45.944 47.821 0.140 1712 111 (pi0) -91 1439 0 2032 2033 0 0 2.408 -6.836 25.639 26.644 0.135 1713 -211 pi- 91 1449 0 0 0 0 0 0.327 -0.353 1.117 1.224 0.140 1714 111 (pi0) -91 1449 0 2034 2035 0 0 2.027 -3.517 7.036 8.124 0.135 1715 211 pi+ 91 1450 0 0 0 0 0 0.433 -0.289 2.377 2.437 0.140 1716 111 (pi0) -91 1450 0 2036 2037 0 0 1.197 -2.092 6.321 6.766 0.135 1717 211 pi+ 91 1454 0 0 0 0 0 -0.062 -0.011 0.199 0.251 0.140 1718 111 (pi0) -91 1454 0 2038 2039 0 0 0.338 -1.279 4.153 4.361 0.135 1719 -211 pi- 91 1456 0 0 0 0 0 -0.040 -0.191 0.099 0.259 0.140 1720 111 (pi0) -91 1456 0 2040 2041 0 0 0.354 -0.743 2.446 2.584 0.135 1721 311 (K0) -91 1457 0 1786 1786 0 0 0.361 -0.751 3.168 3.314 0.498 1722 211 pi+ 91 1457 0 0 0 0 0 -0.123 -0.095 0.234 0.314 0.140 1723 310 (K_S0) -91 1458 1458 2042 2043 0 0 3.367 -0.652 11.642 12.147 0.498 1724 211 pi+ 91 1482 0 0 0 0 0 0.094 0.150 -0.960 0.986 0.140 1725 111 (pi0) -91 1482 0 2044 2045 0 0 -0.172 -0.742 -3.361 3.449 0.135 1726 130 K_L0 91 1484 1484 0 0 0 0 0.105 0.463 -4.607 4.658 0.498 1727 -321 K- 91 1485 0 0 0 0 0 3.127 3.020 -11.411 12.221 0.494 1728 211 pi+ 91 1485 0 0 0 0 0 0.153 0.136 -0.954 0.986 0.140 1729 211 pi+ 91 1487 0 0 0 0 0 1.280 1.035 -5.569 5.809 0.140 1730 -211 pi- 91 1487 0 0 0 0 0 5.524 5.461 -21.983 23.315 0.140 1731 310 (K_S0) -91 1495 1495 2046 2047 0 0 1.832 1.619 -6.173 6.658 0.498 1732 -311 (Kbar0) -91 1496 0 1787 1787 0 0 1.779 0.068 -3.297 3.780 0.498 1733 -211 pi- 91 1496 0 0 0 0 0 2.019 -0.400 -3.952 4.459 0.140 1734 321 K+ 91 1497 0 0 0 0 0 1.127 -0.415 -2.573 2.882 0.494 1735 111 (pi0) -91 1497 0 2048 2049 0 0 0.063 0.125 -0.580 0.612 0.135 1736 -321 K- 91 1498 0 0 0 0 0 2.962 0.924 -6.258 7.002 0.494 1737 111 (pi0) -91 1498 0 2050 2051 0 0 0.144 -0.031 -0.481 0.521 0.135 1738 130 K_L0 91 1503 1503 0 0 0 0 1.689 -2.138 2.392 3.659 0.498 1739 211 pi+ 91 1536 0 0 0 0 0 0.120 1.178 -0.471 1.282 0.140 1740 111 (pi0) -91 1536 0 2052 2054 0 0 0.291 -0.093 -0.541 0.636 0.135 1741 211 pi+ 91 1547 0 0 0 0 0 -0.480 0.205 -3.871 3.909 0.140 1742 -211 pi- 91 1547 0 0 0 0 0 0.087 -0.273 -1.040 1.087 0.140 1743 211 pi+ 91 1550 0 0 0 0 0 -0.028 0.022 -0.297 0.330 0.140 1744 -211 pi- 91 1550 0 0 0 0 0 0.169 0.156 -8.139 8.144 0.140 1745 2112 n0 91 1552 0 0 0 0 0 0.057 0.005 -71.608 71.614 0.940 1746 111 (pi0) -91 1552 0 2055 2056 0 0 0.059 0.178 -8.038 8.041 0.135 1747 -2112 nbar0 91 1553 0 0 0 0 0 -0.327 0.502 -78.273 78.281 0.940 1748 -211 pi- 91 1553 0 0 0 0 0 -0.489 0.268 -41.377 41.381 0.140 1749 211 pi+ 91 1571 0 0 0 0 0 0.300 0.141 6.001 6.012 0.140 1750 111 (pi0) -91 1571 0 2057 2058 0 0 -0.094 -1.072 16.282 16.318 0.135 1751 211 pi+ 91 1573 0 0 0 0 0 0.021 0.381 4.176 4.196 0.140 1752 111 (pi0) -91 1573 0 2059 2060 0 0 0.161 -0.212 1.263 1.298 0.135 1753 -211 pi- 91 1579 0 0 0 0 0 0.690 -0.572 -7.197 7.254 0.140 1754 111 (pi0) -91 1579 0 2061 2062 0 0 0.036 0.088 -1.465 1.474 0.135 1755 311 (K0) -91 1580 0 1788 1788 0 0 -0.200 -0.531 -3.091 3.182 0.498 1756 211 pi+ 91 1580 0 0 0 0 0 0.231 -0.446 -3.421 3.461 0.140 1757 -311 (Kbar0) -91 1581 0 1789 1789 0 0 0.469 0.161 -3.487 3.557 0.498 1758 -211 pi- 91 1581 0 0 0 0 0 0.265 -0.259 -2.266 2.300 0.140 1759 211 pi+ 91 1586 0 0 0 0 0 -0.033 -0.625 -0.892 1.099 0.140 1760 -211 pi- 91 1586 0 0 0 0 0 -0.127 -1.834 -1.037 2.115 0.140 1761 321 K+ 91 1587 0 0 0 0 0 0.262 0.062 0.023 0.563 0.494 1762 -211 pi- 91 1587 0 0 0 0 0 -0.206 -0.018 -0.291 0.383 0.140 1763 130 K_L0 91 1588 1588 0 0 0 0 -0.246 -1.561 -2.010 2.605 0.498 1764 -211 pi- 91 1590 0 0 0 0 0 -0.233 -0.257 0.451 0.586 0.140 1765 111 (pi0) -91 1590 0 2063 2064 0 0 0.288 -0.019 -0.535 0.623 0.135 1766 -211 pi- 91 1600 0 0 0 0 0 -0.217 0.536 428.078 428.078 0.140 1767 111 (pi0) -91 1600 0 2065 2066 0 0 0.054 -0.102 53.153 53.154 0.135 1768 211 pi+ 91 1601 0 0 0 0 0 -0.359 -0.384 38.706 38.710 0.140 1769 111 (pi0) -91 1601 0 2067 2068 0 0 0.338 0.110 8.696 8.704 0.135 1770 211 pi+ 91 1604 0 0 0 0 0 -0.616 -0.337 -0.025 0.717 0.140 1771 111 (pi0) -91 1604 0 2069 2070 0 0 0.452 -0.134 0.684 0.842 0.135 1772 211 pi+ 91 1608 0 0 0 0 0 0.222 -0.151 -7.725 7.731 0.140 1773 -211 pi- 91 1608 0 0 0 0 0 -0.059 -0.084 -0.258 0.311 0.140 1774 211 pi+ 91 1611 0 0 0 0 0 0.276 -0.387 -16.788 16.795 0.140 1775 -211 pi- 91 1611 0 0 0 0 0 -0.034 0.127 -1.190 1.205 0.140 1776 211 pi+ 91 1615 0 0 0 0 0 0.392 -0.589 -11.705 11.727 0.140 1777 111 (pi0) -91 1615 0 2071 2072 0 0 0.298 0.024 -1.172 1.217 0.135 1778 211 pi+ 91 1617 0 0 0 0 0 -0.424 -0.162 -2.032 2.087 0.140 1779 -211 pi- 91 1617 0 0 0 0 0 -0.388 -0.511 -1.090 1.272 0.140 1780 130 K_L0 91 1627 1627 0 0 0 0 -1.259 -0.491 9.538 9.646 0.498 1781 310 (K_S0) -91 1635 1635 2073 2074 0 0 0.693 0.476 0.509 1.102 0.498 1782 130 K_L0 91 1655 1655 0 0 0 0 0.631 0.015 1.956 2.115 0.498 1783 310 (K_S0) -91 1677 1677 2075 2076 0 0 -0.777 -0.220 22.858 22.878 0.498 1784 310 (K_S0) -91 1682 1682 2077 2078 0 0 -0.073 0.148 -0.139 0.542 0.498 1785 310 (K_S0) -91 1691 1691 2079 2080 0 0 0.659 -0.704 3.865 4.015 0.498 1786 310 (K_S0) -91 1721 1721 2081 2082 0 0 0.361 -0.751 3.168 3.314 0.498 1787 130 K_L0 91 1732 1732 0 0 0 0 1.779 0.068 -3.297 3.780 0.498 1788 310 (K_S0) -91 1755 1755 2083 2084 0 0 -0.200 -0.531 -3.091 3.182 0.498 1789 130 K_L0 91 1757 1757 0 0 0 0 0.469 0.161 -3.487 3.557 0.498 1790 22 gamma 91 1206 0 0 0 0 0 0.004 0.184 8.253 8.255 0.000 1791 22 gamma 91 1206 0 0 0 0 0 -0.331 1.383 60.251 60.268 0.000 1792 3122 (Lambda0) -91 1212 0 2085 2086 0 0 0.082 -0.662 264.530 264.533 1.116 1793 22 gamma 91 1212 0 0 0 0 0 -0.058 -0.078 29.165 29.165 0.000 1794 22 gamma 91 1225 0 0 0 0 0 0.048 0.168 1.264 1.276 0.000 1795 22 gamma 91 1225 0 0 0 0 0 -0.087 0.541 4.142 4.178 0.000 1796 211 pi+ 91 1232 0 0 0 0 0 -0.907 -0.180 5.602 5.680 0.140 1797 -211 pi- 91 1232 0 0 0 0 0 -0.072 -0.042 1.906 1.913 0.140 1798 111 (pi0) -91 1232 0 2087 2088 0 0 -0.123 -0.236 1.936 1.959 0.135 1799 211 pi+ 91 1234 0 0 0 0 0 0.046 0.097 0.135 0.222 0.140 1800 -211 pi- 91 1234 0 0 0 0 0 -0.343 -0.013 0.794 0.876 0.140 1801 111 (pi0) -91 1234 0 2089 2090 0 0 -0.065 -0.176 0.107 0.255 0.135 1802 211 pi+ 91 1236 0 0 0 0 0 -0.130 -0.084 0.326 0.387 0.140 1803 -211 pi- 91 1236 0 0 0 0 0 0.031 0.175 0.451 0.504 0.140 1804 111 (pi0) -91 1236 0 2091 2092 0 0 -0.181 0.258 1.983 2.012 0.135 1805 -11 e+ 91 1255 0 0 0 0 0 -1.008 -0.273 -3.656 3.802 0.001 1806 12 nu_e 91 1255 0 0 0 0 0 -0.856 -0.032 -4.360 4.444 0.000 1807 -313 (K*bar0) -91 1255 0 2093 2094 0 0 -1.001 -0.062 -10.547 10.633 0.909 1808 211 pi+ 91 1257 0 0 0 0 0 -0.276 -0.290 -1.006 1.091 0.140 1809 -211 pi- 91 1257 0 0 0 0 0 -0.198 0.113 -0.940 0.978 0.140 1810 111 (pi0) -91 1257 0 2095 2096 0 0 -0.073 0.154 -0.300 0.371 0.135 1811 22 gamma 91 1270 0 0 0 0 0 -0.422 -0.248 -26.788 26.792 0.000 1812 22 gamma 91 1270 0 0 0 0 0 -0.046 -0.080 -3.510 3.511 0.000 1813 22 gamma 91 1292 0 0 0 0 0 0.160 0.126 0.384 0.434 0.000 1814 22 gamma 91 1292 0 0 0 0 0 -0.251 -0.226 1.210 1.256 0.000 1815 3122 (Lambda0) -91 1294 0 2097 2098 0 0 -0.052 -0.892 3.529 3.807 1.116 1816 22 gamma 91 1294 0 0 0 0 0 0.072 -0.092 0.291 0.314 0.000 1817 -3122 (Lambdabar0) -91 1295 0 2099 2100 0 0 1.013 0.270 3.864 4.156 1.116 1818 22 gamma 91 1295 0 0 0 0 0 0.110 -0.027 0.167 0.202 0.000 1819 22 gamma 91 1297 0 0 0 0 0 -0.287 -0.054 0.752 0.807 0.000 1820 22 gamma 91 1297 0 0 0 0 0 -0.112 -0.085 0.212 0.255 0.000 1821 22 gamma 91 1298 0 0 0 0 0 0.147 -0.199 0.858 0.893 0.000 1822 22 gamma 91 1298 0 0 0 0 0 0.339 -0.240 1.077 1.155 0.000 1823 2112 n0 91 1300 0 0 0 0 0 -0.340 -0.437 1.275 1.678 0.940 1824 111 (pi0) -91 1300 0 2101 2102 0 0 0.007 -0.025 0.052 0.147 0.135 1825 -2212 pbar- 91 1307 0 0 0 0 0 -0.985 1.414 4.789 5.175 0.938 1826 211 pi+ 91 1307 0 0 0 0 0 -0.363 0.411 1.445 1.552 0.140 1827 211 pi+ 91 1314 0 0 0 0 0 0.905 -0.238 5.557 5.637 0.140 1828 -211 pi- 91 1314 0 0 0 0 0 0.410 -0.315 1.996 2.067 0.140 1829 111 (pi0) -91 1314 0 2103 2104 0 0 0.181 0.064 0.917 0.947 0.135 1830 22 gamma 91 1316 0 0 0 0 0 0.026 -0.249 1.882 1.898 0.000 1831 22 gamma 91 1316 0 0 0 0 0 -0.220 0.247 2.664 2.685 0.000 1832 22 gamma 91 1317 0 0 0 0 0 -0.559 -1.357 10.692 10.792 0.000 1833 22 gamma 91 1317 0 0 0 0 0 -0.083 -0.185 1.155 1.172 0.000 1834 22 gamma 91 1319 0 0 0 0 0 -0.103 -0.145 1.633 1.643 0.000 1835 22 gamma 91 1319 0 0 0 0 0 -1.224 -1.957 17.257 17.410 0.000 1836 22 gamma 91 1336 0 0 0 0 0 0.219 -0.680 4.789 4.842 0.000 1837 22 gamma 91 1336 0 0 0 0 0 0.208 -0.902 7.160 7.219 0.000 1838 111 (pi0) -91 1340 0 2105 2106 0 0 0.134 0.003 31.859 31.860 0.135 1839 111 (pi0) -91 1340 0 2107 2108 0 0 0.131 -0.128 18.836 18.837 0.135 1840 111 (pi0) -91 1340 0 2109 2110 0 0 0.136 -0.229 57.094 57.094 0.135 1841 211 pi+ 91 1341 0 0 0 0 0 0.786 -0.146 53.652 53.659 0.140 1842 -211 pi- 91 1341 0 0 0 0 0 0.501 0.071 21.933 21.939 0.140 1843 111 (pi0) -91 1341 0 2111 2112 0 0 0.098 0.068 4.868 4.871 0.135 1844 2212 p+ 91 1344 0 0 0 0 0 -0.652 1.224 257.390 257.396 0.938 1845 -211 pi- 91 1344 0 0 0 0 0 -0.174 0.310 77.958 77.959 0.140 1846 211 pi+ 91 1349 0 0 0 0 0 -0.013 0.264 17.654 17.656 0.140 1847 -211 pi- 91 1349 0 0 0 0 0 -0.224 0.003 4.610 4.618 0.140 1848 111 (pi0) -91 1349 0 2113 2114 0 0 -0.140 -0.044 4.330 4.334 0.135 1849 22 gamma 91 1360 0 0 0 0 0 0.829 0.058 -0.352 0.902 0.000 1850 22 gamma 91 1360 0 0 0 0 0 0.179 -0.004 -0.147 0.232 0.000 1851 211 pi+ 91 1363 0 0 0 0 0 -0.010 0.257 3.523 3.535 0.140 1852 -211 pi- 91 1363 0 0 0 0 0 -0.038 -0.131 3.378 3.384 0.140 1853 111 (pi0) -91 1363 0 2115 2116 0 0 0.015 -0.195 1.512 1.530 0.135 1854 -2112 nbar0 91 1366 0 0 0 0 0 0.470 0.042 37.190 37.205 0.940 1855 211 pi+ 91 1366 0 0 0 0 0 -0.083 -0.028 2.715 2.720 0.140 1856 323 (K*+) -91 1385 0 2117 2118 0 0 1.240 -1.516 10.673 10.884 0.848 1857 -313 (K*bar0) -91 1385 0 2119 2120 0 0 1.218 -1.948 12.233 12.487 1.001 1858 22 gamma 91 1388 0 0 0 0 0 0.181 -0.592 1.097 1.259 0.000 1859 22 gamma 91 1388 0 0 0 0 0 0.024 -0.251 0.321 0.408 0.000 1860 211 pi+ 91 1389 0 0 0 0 0 0.780 -0.580 1.596 1.874 0.140 1861 -211 pi- 91 1389 0 0 0 0 0 2.155 -1.685 5.337 5.999 0.140 1862 111 (pi0) -91 1389 0 2121 2122 0 0 2.810 -2.232 7.740 8.532 0.135 1863 211 pi+ 91 1392 0 0 0 0 0 1.880 -1.740 4.910 5.539 0.140 1864 -211 pi- 91 1392 0 0 0 0 0 5.733 -5.104 14.757 16.635 0.140 1865 221 (eta) -91 1392 0 2123 2124 0 0 27.771 -24.716 71.795 80.851 0.548 1866 22 gamma 91 1396 0 0 0 0 0 3.109 -2.276 8.741 9.552 0.000 1867 22 gamma 91 1396 0 0 0 0 0 4.620 -3.180 12.749 13.928 0.000 1868 -421 (Dbar0) -91 1402 0 2125 2127 0 0 272.779 -220.834 772.446 848.441 1.865 1869 111 (pi0) -91 1402 0 2128 2129 0 0 18.915 -15.369 53.624 58.903 0.135 1870 411 (D+) -91 1426 0 2130 2133 0 0 62.451 -49.651 173.687 191.144 1.870 1871 111 (pi0) -91 1426 0 2134 2135 0 0 5.024 -4.022 13.929 15.344 0.135 1872 22 gamma 91 1429 0 0 0 0 0 0.603 -0.495 1.749 1.915 0.000 1873 22 gamma 91 1429 0 0 0 0 0 3.586 -2.540 9.662 10.614 0.000 1874 22 gamma 91 1436 0 0 0 0 0 0.539 -2.129 10.470 10.698 0.000 1875 22 gamma 91 1436 0 0 0 0 0 0.398 -1.161 5.838 5.965 0.000 1876 22 gamma 91 1441 0 0 0 0 0 1.548 -4.604 14.942 15.711 0.000 1877 22 gamma 91 1441 0 0 0 0 0 -0.017 -0.462 1.320 1.398 0.000 1878 22 gamma 91 1442 0 0 0 0 0 2.764 -8.189 30.614 31.811 0.000 1879 22 gamma 91 1442 0 0 0 0 0 0.373 -1.227 4.669 4.842 0.000 1880 22 gamma 91 1443 0 0 0 0 0 2.868 -9.507 33.805 35.233 0.000 1881 22 gamma 91 1443 0 0 0 0 0 0.640 -1.952 7.909 8.172 0.000 1882 22 gamma 91 1446 0 0 0 0 0 0.224 -0.438 1.097 1.202 0.000 1883 22 gamma 91 1446 0 0 0 0 0 2.956 -6.736 15.712 17.348 0.000 1884 211 pi+ 91 1447 0 0 0 0 0 0.232 -0.468 1.154 1.275 0.140 1885 -211 pi- 91 1447 0 0 0 0 0 2.763 -3.761 8.817 9.977 0.140 1886 111 (pi0) -91 1447 0 2136 2137 0 0 0.949 -1.111 3.100 3.430 0.135 1887 22 gamma 91 1448 0 0 0 0 0 0.801 -1.591 2.732 3.262 0.000 1888 22 gamma 91 1448 0 0 0 0 0 0.620 -1.374 2.513 2.930 0.000 1889 2112 n0 91 1451 0 0 0 0 0 1.160 -4.449 11.757 12.659 0.940 1890 -211 pi- 91 1451 0 0 0 0 0 0.580 -1.417 4.230 4.501 0.140 1891 -2112 nbar0 91 1452 0 0 0 0 0 2.106 -4.406 12.488 13.441 0.940 1892 211 pi+ 91 1452 0 0 0 0 0 0.147 -0.506 1.809 1.890 0.140 1893 22 gamma 91 1455 0 0 0 0 0 0.713 -3.385 8.201 8.901 0.000 1894 22 gamma 91 1455 0 0 0 0 0 0.427 -2.997 6.046 6.762 0.000 1895 211 pi+ 91 1459 0 0 0 0 0 0.324 -0.166 1.419 1.471 0.140 1896 -211 pi- 91 1459 0 0 0 0 0 0.938 -0.919 4.207 4.409 0.140 1897 111 (pi0) -91 1459 0 2138 2139 0 0 0.429 -0.258 3.104 3.147 0.135 1898 211 pi+ 91 1483 0 0 0 0 0 0.090 0.246 -0.169 0.341 0.140 1899 -211 pi- 91 1483 0 0 0 0 0 0.607 0.629 -1.549 1.784 0.140 1900 111 (pi0) -91 1483 0 2140 2141 0 0 0.120 0.055 -0.116 0.222 0.135 1901 211 pi+ 91 1489 0 0 0 0 0 1.193 0.789 -3.409 3.700 0.140 1902 -211 pi- 91 1489 0 0 0 0 0 0.723 0.720 -3.031 3.201 0.140 1903 111 (pi0) -91 1489 0 2142 2143 0 0 1.519 0.784 -5.124 5.403 0.135 1904 111 (pi0) -91 1491 0 2144 2145 0 0 1.417 0.811 -3.745 4.087 0.135 1905 22 gamma 91 1491 0 0 0 0 0 0.154 0.438 -1.891 1.947 0.000 1906 22 gamma 91 1500 0 0 0 0 0 0.136 -0.045 0.271 0.306 0.000 1907 22 gamma 91 1500 0 0 0 0 0 -0.340 -0.339 0.121 0.495 0.000 1908 -421 (Dbar0) -91 1505 0 2146 2148 0 0 10.965 -15.164 16.182 24.809 1.865 1909 111 (pi0) -91 1505 0 2149 2150 0 0 0.862 -1.160 1.305 1.952 0.135 1910 22 gamma 91 1531 0 0 0 0 0 -0.232 0.560 -0.031 0.607 0.000 1911 22 gamma 91 1531 0 0 0 0 0 -0.043 0.373 -0.039 0.377 0.000 1912 211 pi+ 91 1534 0 0 0 0 0 0.230 0.547 -0.135 0.624 0.140 1913 -211 pi- 91 1534 0 0 0 0 0 0.607 0.354 -0.309 0.781 0.140 1914 111 (pi0) -91 1534 0 2151 2152 0 0 0.289 0.269 0.105 0.430 0.135 1915 22 gamma 91 1537 0 0 0 0 0 1.172 1.270 -0.412 1.776 0.000 1916 22 gamma 91 1537 0 0 0 0 0 0.265 0.477 0.149 0.566 0.000 1917 211 pi+ 91 1538 0 0 0 0 0 0.356 0.043 -0.264 0.467 0.140 1918 -211 pi- 91 1538 0 0 0 0 0 0.118 0.287 0.110 0.358 0.140 1919 111 (pi0) -91 1538 0 2153 2154 0 0 0.033 0.223 -0.144 0.300 0.135 1920 211 pi+ 91 1540 0 0 0 0 0 0.548 0.808 -0.252 1.018 0.140 1921 -211 pi- 91 1540 0 0 0 0 0 0.228 0.044 -0.129 0.300 0.140 1922 111 (pi0) -91 1540 0 2155 2156 0 0 0.026 0.339 -0.063 0.371 0.135 1923 3122 (Lambda0) -91 1541 0 2157 2158 0 0 0.051 0.258 -0.193 1.162 1.116 1924 22 gamma 91 1541 0 0 0 0 0 0.070 -0.020 0.010 0.074 0.000 1925 211 pi+ 91 1542 0 0 0 0 0 -0.057 0.091 0.059 0.186 0.140 1926 -211 pi- 91 1542 0 0 0 0 0 0.021 0.261 -0.035 0.299 0.140 1927 221 (eta) -91 1542 0 2159 2160 0 0 -0.017 0.041 -0.060 0.553 0.548 1928 -2212 pbar- 91 1543 0 0 0 0 0 -0.436 0.427 0.312 1.162 0.938 1929 211 pi+ 91 1543 0 0 0 0 0 -0.141 0.208 0.104 0.306 0.140 1930 2212 p+ 91 1544 0 0 0 0 0 -0.940 -0.201 -1.098 1.735 0.938 1931 111 (pi0) -91 1544 0 2161 2162 0 0 -0.453 0.113 -0.302 0.572 0.135 1932 -3122 (Lambdabar0) -91 1545 0 2163 2164 0 0 -0.293 0.229 -1.406 1.833 1.116 1933 22 gamma 91 1545 0 0 0 0 0 0.031 0.027 -0.182 0.187 0.000 1934 111 (pi0) -91 1549 0 2165 2166 0 0 -0.595 0.388 -19.413 19.426 0.135 1935 22 gamma 91 1549 0 0 0 0 0 -0.507 -0.353 -12.756 12.771 0.000 1936 211 pi+ 91 1554 0 0 0 0 0 -0.290 0.184 -60.179 60.180 0.140 1937 -211 pi- 91 1554 0 0 0 0 0 -0.844 0.726 -272.197 272.199 0.140 1938 111 (pi0) -91 1554 0 2167 2168 0 0 -0.308 0.022 -44.632 44.633 0.135 1939 211 pi+ 91 1569 0 0 0 0 0 0.059 -0.148 20.314 20.315 0.140 1940 -211 pi- 91 1569 0 0 0 0 0 0.091 -0.060 60.326 60.326 0.140 1941 111 (pi0) -91 1569 0 2169 2170 0 0 -0.274 0.125 56.495 56.496 0.135 1942 111 (pi0) -91 1570 0 2171 2172 0 0 0.133 0.007 41.814 41.815 0.135 1943 111 (pi0) -91 1570 0 2173 2174 0 0 -0.071 0.123 102.344 102.344 0.135 1944 111 (pi0) -91 1570 0 2175 2176 0 0 -0.028 0.007 64.600 64.600 0.135 1945 22 gamma 91 1576 0 0 0 0 0 -0.093 -0.066 0.009 0.114 0.000 1946 22 gamma 91 1576 0 0 0 0 0 -0.077 0.062 -0.030 0.104 0.000 1947 22 gamma 91 1582 0 0 0 0 0 -0.151 -1.093 -1.487 1.851 0.000 1948 22 gamma 91 1582 0 0 0 0 0 -0.008 0.001 -0.007 0.010 0.000 1949 22 gamma 91 1583 0 0 0 0 0 -0.303 -0.483 -0.306 0.647 0.000 1950 22 gamma 91 1583 0 0 0 0 0 0.002 -0.069 -0.012 0.070 0.000 1951 211 pi+ 91 1585 0 0 0 0 0 -0.095 -0.390 -0.570 0.711 0.140 1952 -211 pi- 91 1585 0 0 0 0 0 0.106 -0.082 -0.056 0.202 0.140 1953 111 (pi0) -91 1585 0 2177 2178 0 0 -0.151 -0.885 -0.642 1.112 0.135 1954 211 pi+ 91 1589 0 0 0 0 0 0.010 -0.100 0.201 0.265 0.140 1955 -211 pi- 91 1589 0 0 0 0 0 0.068 -0.032 0.884 0.898 0.140 1956 111 (pi0) -91 1589 0 2179 2180 0 0 0.478 -0.007 0.530 0.726 0.135 1957 211 pi+ 91 1603 0 0 0 0 0 -0.036 -0.107 0.326 0.372 0.140 1958 -211 pi- 91 1603 0 0 0 0 0 -0.197 0.246 1.787 1.820 0.140 1959 111 (pi0) -91 1603 0 2181 2182 0 0 -0.041 0.336 1.776 1.813 0.135 1960 22 gamma 91 1609 0 0 0 0 0 -0.030 -0.272 -3.800 3.810 0.000 1961 22 gamma 91 1609 0 0 0 0 0 0.045 -0.272 -2.553 2.568 0.000 1962 22 gamma 91 1610 0 0 0 0 0 -0.143 -0.154 -3.016 3.024 0.000 1963 22 gamma 91 1610 0 0 0 0 0 -0.057 -0.085 -3.535 3.536 0.000 1964 211 pi+ 91 1613 0 0 0 0 0 -0.032 -0.095 -6.227 6.229 0.140 1965 -211 pi- 91 1613 0 0 0 0 0 -0.032 0.318 -4.059 4.074 0.140 1966 111 (pi0) -91 1613 0 2183 2184 0 0 0.173 0.088 -2.671 2.682 0.135 1967 211 pi+ 91 1616 0 0 0 0 0 0.167 0.195 -0.721 0.778 0.140 1968 -211 pi- 91 1616 0 0 0 0 0 0.008 0.062 -0.463 0.488 0.140 1969 111 (pi0) -91 1616 0 2185 2186 0 0 0.346 0.076 -1.066 1.131 0.135 1970 -421 (Dbar0) -91 1618 0 2187 2189 0 0 -2.834 -0.292 -6.831 7.632 1.865 1971 -211 pi- 91 1618 0 0 0 0 0 -0.211 -0.063 -0.503 0.566 0.140 1972 22 gamma 91 1620 0 0 0 0 0 0.230 0.639 14.857 14.872 0.000 1973 22 gamma 91 1620 0 0 0 0 0 0.554 1.450 29.805 29.846 0.000 1974 22 gamma 91 1622 0 0 0 0 0 0.012 -0.143 22.801 22.801 0.000 1975 22 gamma 91 1622 0 0 0 0 0 -0.026 -0.122 7.822 7.823 0.000 1976 22 gamma 91 1624 0 0 0 0 0 -0.457 -0.071 307.257 307.258 0.000 1977 22 gamma 91 1624 0 0 0 0 0 -0.069 0.004 93.792 93.792 0.000 1978 22 gamma 91 1628 0 0 0 0 0 -1.391 -0.312 12.536 12.617 0.000 1979 22 gamma 91 1628 0 0 0 0 0 -0.291 -0.057 2.121 2.142 0.000 1980 22 gamma 91 1630 0 0 0 0 0 -0.039 -0.014 0.591 0.592 0.000 1981 22 gamma 91 1630 0 0 0 0 0 -0.013 0.160 1.452 1.461 0.000 1982 211 pi+ 91 1632 0 0 0 0 0 -0.292 0.739 6.494 6.544 0.140 1983 -211 pi- 91 1632 0 0 0 0 0 -0.072 0.152 3.976 3.982 0.140 1984 22 gamma 91 1640 0 0 0 0 0 0.035 -0.310 -2.590 2.609 0.000 1985 22 gamma 91 1640 0 0 0 0 0 -0.041 -0.048 -0.306 0.313 0.000 1986 22 gamma 91 1642 0 0 0 0 0 0.010 -0.254 -0.176 0.309 0.000 1987 22 gamma 91 1642 0 0 0 0 0 0.094 -0.115 -0.159 0.217 0.000 1988 22 gamma 91 1644 0 0 0 0 0 -0.455 -0.217 -0.459 0.682 0.000 1989 22 gamma 91 1644 0 0 0 0 0 -0.145 -0.148 -0.130 0.245 0.000 1990 22 gamma 91 1646 0 0 0 0 0 0.098 -0.213 -39.682 39.683 0.000 1991 22 gamma 91 1646 0 0 0 0 0 0.040 0.012 -4.905 4.905 0.000 1992 22 gamma 91 1650 0 0 0 0 0 -0.101 -0.027 -37.047 37.047 0.000 1993 22 gamma 91 1650 0 0 0 0 0 -0.426 0.034 -257.041 257.042 0.000 1994 22 gamma 91 1654 0 0 0 0 0 0.113 -0.116 0.657 0.677 0.000 1995 22 gamma 91 1654 0 0 0 0 0 0.015 0.012 0.007 0.020 0.000 1996 22 gamma 91 1658 0 0 0 0 0 -0.910 0.131 1.571 1.820 0.000 1997 22 gamma 91 1658 0 0 0 0 0 -0.116 0.068 0.239 0.274 0.000 1998 22 gamma 91 1660 0 0 0 0 0 -0.164 -0.303 0.548 0.648 0.000 1999 22 gamma 91 1660 0 0 0 0 0 -0.160 -0.100 0.253 0.315 0.000 2000 22 gamma 91 1664 0 0 0 0 0 1.505 -0.096 7.556 7.705 0.000 2001 22 gamma 91 1664 0 0 0 0 0 0.071 -0.022 0.267 0.277 0.000 2002 22 gamma 91 1666 0 0 0 0 0 0.037 -0.061 0.470 0.476 0.000 2003 22 gamma 91 1666 0 0 0 0 0 0.572 -1.218 5.764 5.919 0.000 2004 22 gamma 91 1670 0 0 0 0 0 0.057 -0.282 4.915 4.923 0.000 2005 22 gamma 91 1670 0 0 0 0 0 -0.046 -0.132 1.571 1.577 0.000 2006 22 gamma 91 1672 0 0 0 0 0 0.048 -0.101 7.533 7.533 0.000 2007 22 gamma 91 1672 0 0 0 0 0 0.082 0.032 5.940 5.940 0.000 2008 22 gamma 91 1680 0 0 0 0 0 -0.523 -0.301 19.152 19.161 0.000 2009 22 gamma 91 1680 0 0 0 0 0 -0.016 -0.044 2.221 2.222 0.000 2010 111 (pi0) -91 1681 0 2190 2191 0 0 0.038 -0.100 -0.042 0.177 0.135 2011 111 (pi0) -91 1681 0 2192 2193 0 0 0.547 0.133 0.158 0.600 0.135 2012 22 gamma 91 1685 0 0 0 0 0 0.058 -0.040 0.454 0.460 0.000 2013 22 gamma 91 1685 0 0 0 0 0 0.110 -0.175 3.620 3.626 0.000 2014 111 (pi0) -91 1686 0 2194 2195 0 0 0.049 0.152 2.339 2.348 0.135 2015 111 (pi0) -91 1686 0 2196 2197 0 0 0.238 0.058 0.746 0.796 0.135 2016 22 gamma 91 1692 0 0 0 0 0 0.359 -0.399 3.993 4.029 0.000 2017 22 gamma 91 1692 0 0 0 0 0 0.014 -0.002 0.390 0.390 0.000 2018 22 gamma 91 1694 0 0 0 0 0 8.884 -7.513 22.040 24.922 0.000 2019 22 gamma 91 1694 0 0 0 0 0 9.990 -8.636 25.054 28.321 0.000 2020 22 gamma 91 1696 0 0 0 0 0 6.963 -6.590 18.303 20.662 0.000 2021 22 gamma 91 1696 0 0 0 0 0 2.434 -2.394 6.419 7.270 0.000 2022 22 gamma 91 1698 0 0 0 0 0 2.726 -2.104 6.556 7.405 0.000 2023 22 gamma 91 1698 0 0 0 0 0 4.399 -3.292 10.788 12.107 0.000 2024 22 gamma 91 1700 0 0 0 0 0 6.335 -5.234 16.509 18.441 0.000 2025 22 gamma 91 1700 0 0 0 0 0 8.789 -7.468 23.170 25.882 0.000 2026 22 gamma 91 1702 0 0 0 0 0 1.367 -1.115 3.857 4.241 0.000 2027 22 gamma 91 1702 0 0 0 0 0 9.549 -7.368 26.680 29.280 0.000 2028 22 gamma 91 1706 0 0 0 0 0 0.007 -0.215 1.328 1.345 0.000 2029 22 gamma 91 1706 0 0 0 0 0 0.338 -1.248 7.138 7.255 0.000 2030 22 gamma 91 1710 0 0 0 0 0 0.586 -1.029 5.439 5.567 0.000 2031 22 gamma 91 1710 0 0 0 0 0 0.013 0.000 0.090 0.091 0.000 2032 22 gamma 91 1712 0 0 0 0 0 0.935 -2.497 9.571 9.936 0.000 2033 22 gamma 91 1712 0 0 0 0 0 1.472 -4.339 16.067 16.708 0.000 2034 22 gamma 91 1714 0 0 0 0 0 0.032 -0.098 0.179 0.206 0.000 2035 22 gamma 91 1714 0 0 0 0 0 1.995 -3.419 6.857 7.918 0.000 2036 22 gamma 91 1716 0 0 0 0 0 0.793 -1.258 3.941 4.213 0.000 2037 22 gamma 91 1716 0 0 0 0 0 0.404 -0.834 2.380 2.554 0.000 2038 22 gamma 91 1718 0 0 0 0 0 0.309 -1.007 3.407 3.566 0.000 2039 22 gamma 91 1718 0 0 0 0 0 0.029 -0.272 0.746 0.795 0.000 2040 22 gamma 91 1720 0 0 0 0 0 0.218 -0.559 1.893 1.986 0.000 2041 22 gamma 91 1720 0 0 0 0 0 0.136 -0.184 0.553 0.598 0.000 2042 211 pi+ 91 1723 0 0 0 0 0 0.416 -0.166 1.735 1.797 0.140 2043 -211 pi- 91 1723 0 0 0 0 0 2.951 -0.486 9.908 10.350 0.140 2044 22 gamma 91 1725 0 0 0 0 0 -0.075 -0.121 -0.519 0.538 0.000 2045 22 gamma 91 1725 0 0 0 0 0 -0.097 -0.622 -2.842 2.910 0.000 2046 211 pi+ 91 1731 0 0 0 0 0 0.899 0.802 -2.495 2.774 0.140 2047 -211 pi- 91 1731 0 0 0 0 0 0.932 0.817 -3.678 3.884 0.140 2048 22 gamma 91 1735 0 0 0 0 0 0.070 0.055 -0.139 0.165 0.000 2049 22 gamma 91 1735 0 0 0 0 0 -0.007 0.071 -0.442 0.447 0.000 2050 22 gamma 91 1737 0 0 0 0 0 0.065 0.053 -0.189 0.207 0.000 2051 22 gamma 91 1737 0 0 0 0 0 0.079 -0.084 -0.292 0.314 0.000 2052 22 gamma 91 1740 0 0 0 0 0 0.150 0.009 -0.184 0.238 0.000 2053 11 e- 91 1740 0 0 0 0 0 0.028 -0.030 -0.108 0.116 0.001 2054 -11 e+ 91 1740 0 0 0 0 0 0.113 -0.072 -0.249 0.282 0.001 2055 22 gamma 91 1746 0 0 0 0 0 0.067 0.196 -7.634 7.637 0.000 2056 22 gamma 91 1746 0 0 0 0 0 -0.008 -0.018 -0.404 0.404 0.000 2057 22 gamma 91 1750 0 0 0 0 0 -0.092 -1.001 14.604 14.639 0.000 2058 22 gamma 91 1750 0 0 0 0 0 -0.002 -0.070 1.678 1.679 0.000 2059 22 gamma 91 1752 0 0 0 0 0 0.122 -0.095 0.927 0.940 0.000 2060 22 gamma 91 1752 0 0 0 0 0 0.040 -0.117 0.336 0.358 0.000 2061 22 gamma 91 1754 0 0 0 0 0 0.066 -0.003 -0.465 0.470 0.000 2062 22 gamma 91 1754 0 0 0 0 0 -0.030 0.091 -1.000 1.004 0.000 2063 22 gamma 91 1765 0 0 0 0 0 0.175 0.053 -0.345 0.391 0.000 2064 22 gamma 91 1765 0 0 0 0 0 0.113 -0.071 -0.190 0.232 0.000 2065 22 gamma 91 1767 0 0 0 0 0 -0.034 -0.068 16.179 16.179 0.000 2066 22 gamma 91 1767 0 0 0 0 0 0.088 -0.035 36.975 36.975 0.000 2067 22 gamma 91 1769 0 0 0 0 0 0.164 0.019 2.662 2.667 0.000 2068 22 gamma 91 1769 0 0 0 0 0 0.174 0.091 6.034 6.038 0.000 2069 22 gamma 91 1771 0 0 0 0 0 0.120 -0.020 0.286 0.311 0.000 2070 22 gamma 91 1771 0 0 0 0 0 0.333 -0.114 0.398 0.531 0.000 2071 22 gamma 91 1777 0 0 0 0 0 0.006 0.019 -0.019 0.028 0.000 2072 22 gamma 91 1777 0 0 0 0 0 0.292 0.005 -1.153 1.189 0.000 2073 111 (pi0) -91 1781 0 2198 2199 0 0 0.496 0.283 0.534 0.793 0.135 2074 111 (pi0) -91 1781 0 2200 2201 0 0 0.197 0.193 -0.025 0.309 0.135 2075 211 pi+ 91 1783 0 0 0 0 0 -0.028 0.006 2.391 2.395 0.140 2076 -211 pi- 91 1783 0 0 0 0 0 -0.750 -0.226 20.467 20.483 0.140 2077 211 pi+ 91 1784 0 0 0 0 0 0.153 0.120 0.003 0.240 0.140 2078 -211 pi- 91 1784 0 0 0 0 0 -0.227 0.028 -0.141 0.303 0.140 2079 211 pi+ 91 1785 0 0 0 0 0 0.358 -0.109 1.603 1.652 0.140 2080 -211 pi- 91 1785 0 0 0 0 0 0.301 -0.596 2.262 2.363 0.140 2081 211 pi+ 91 1786 0 0 0 0 0 -0.056 -0.138 0.481 0.522 0.140 2082 -211 pi- 91 1786 0 0 0 0 0 0.417 -0.612 2.688 2.791 0.140 2083 111 (pi0) -91 1788 0 2202 2203 0 0 -0.177 -0.429 -1.380 1.462 0.135 2084 111 (pi0) -91 1788 0 2204 2206 0 0 -0.024 -0.101 -1.712 1.720 0.135 2085 2112 n0 91 1792 0 0 0 0 0 0.035 -0.519 238.110 238.112 0.940 2086 111 (pi0) -91 1792 0 2207 2208 0 0 0.047 -0.143 26.420 26.421 0.135 2087 22 gamma 91 1798 0 0 0 0 0 -0.041 -0.206 1.435 1.451 0.000 2088 22 gamma 91 1798 0 0 0 0 0 -0.082 -0.030 0.500 0.508 0.000 2089 22 gamma 91 1801 0 0 0 0 0 -0.017 -0.029 0.094 0.100 0.000 2090 22 gamma 91 1801 0 0 0 0 0 -0.048 -0.147 0.013 0.155 0.000 2091 22 gamma 91 1804 0 0 0 0 0 -0.033 0.003 0.457 0.458 0.000 2092 22 gamma 91 1804 0 0 0 0 0 -0.148 0.255 1.526 1.554 0.000 2093 -321 K- 91 1807 0 0 0 0 0 -0.569 -0.124 -8.580 8.614 0.494 2094 211 pi+ 91 1807 0 0 0 0 0 -0.432 0.063 -1.967 2.019 0.140 2095 22 gamma 91 1810 0 0 0 0 0 -0.016 0.159 -0.223 0.274 0.000 2096 22 gamma 91 1810 0 0 0 0 0 -0.057 -0.005 -0.078 0.097 0.000 2097 2112 n0 91 1815 0 0 0 0 0 -0.092 -0.769 2.769 3.025 0.940 2098 111 (pi0) -91 1815 0 2209 2210 0 0 0.040 -0.123 0.760 0.782 0.135 2099 -2212 pbar- 91 1817 0 0 0 0 0 0.774 0.170 2.930 3.176 0.938 2100 211 pi+ 91 1817 0 0 0 0 0 0.240 0.100 0.934 0.979 0.140 2101 22 gamma 91 1824 0 0 0 0 0 -0.014 0.015 -0.040 0.045 0.000 2102 22 gamma 91 1824 0 0 0 0 0 0.020 -0.040 0.092 0.102 0.000 2103 22 gamma 91 1829 0 0 0 0 0 0.062 0.072 0.608 0.615 0.000 2104 22 gamma 91 1829 0 0 0 0 0 0.119 -0.009 0.309 0.332 0.000 2105 22 gamma 91 1838 0 0 0 0 0 0.030 -0.008 1.227 1.227 0.000 2106 22 gamma 91 1838 0 0 0 0 0 0.104 0.010 30.633 30.633 0.000 2107 22 gamma 91 1839 0 0 0 0 0 0.147 -0.135 14.989 14.990 0.000 2108 22 gamma 91 1839 0 0 0 0 0 -0.016 0.008 3.847 3.847 0.000 2109 22 gamma 91 1840 0 0 0 0 0 -0.017 -0.091 16.905 16.906 0.000 2110 22 gamma 91 1840 0 0 0 0 0 0.153 -0.138 40.188 40.189 0.000 2111 22 gamma 91 1843 0 0 0 0 0 0.107 0.100 3.728 3.731 0.000 2112 22 gamma 91 1843 0 0 0 0 0 -0.008 -0.032 1.140 1.140 0.000 2113 22 gamma 91 1848 0 0 0 0 0 -0.007 0.036 0.467 0.468 0.000 2114 22 gamma 91 1848 0 0 0 0 0 -0.133 -0.081 3.863 3.866 0.000 2115 22 gamma 91 1853 0 0 0 0 0 -0.033 -0.006 0.411 0.412 0.000 2116 22 gamma 91 1853 0 0 0 0 0 0.049 -0.189 1.101 1.118 0.000 2117 311 (K0) -91 1856 0 2211 2211 0 0 0.729 -1.232 6.971 7.134 0.498 2118 211 pi+ 91 1856 0 0 0 0 0 0.510 -0.284 3.702 3.751 0.140 2119 -311 (Kbar0) -91 1857 0 2212 2212 0 0 1.134 -1.271 9.662 9.823 0.498 2120 111 (pi0) -91 1857 0 2213 2214 0 0 0.084 -0.678 2.571 2.663 0.135 2121 22 gamma 91 1862 0 0 0 0 0 0.720 -0.589 2.145 2.338 0.000 2122 22 gamma 91 1862 0 0 0 0 0 2.090 -1.643 5.595 6.194 0.000 2123 22 gamma 91 1865 0 0 0 0 0 3.574 -3.429 9.601 10.804 0.000 2124 22 gamma 91 1865 0 0 0 0 0 24.197 -21.287 62.194 70.047 0.000 2125 -211 pi- 91 1868 0 0 0 0 0 124.537 -100.752 354.410 388.930 0.140 2126 211 pi+ 91 1868 0 0 0 0 0 102.352 -82.701 287.661 316.330 0.140 2127 111 (pi0) -91 1868 0 2215 2216 0 0 45.890 -37.381 130.375 143.181 0.135 2128 22 gamma 91 1869 0 0 0 0 0 13.927 -11.355 39.658 43.539 0.000 2129 22 gamma 91 1869 0 0 0 0 0 4.989 -4.015 13.966 15.364 0.000 2130 -13 mu+ 91 1870 0 0 0 0 0 20.844 -16.374 57.982 63.754 0.106 2131 14 nu_mu 91 1870 0 0 0 0 0 4.824 -4.234 13.379 14.839 0.000 2132 -321 K- 91 1870 0 0 0 0 0 17.308 -13.944 48.662 53.499 0.494 2133 211 pi+ 91 1870 0 0 0 0 0 19.474 -15.099 53.665 59.052 0.140 2134 22 gamma 91 1871 0 0 0 0 0 1.508 -1.236 4.360 4.776 0.000 2135 22 gamma 91 1871 0 0 0 0 0 3.515 -2.786 9.569 10.568 0.000 2136 22 gamma 91 1886 0 0 0 0 0 0.207 -0.163 0.538 0.599 0.000 2137 22 gamma 91 1886 0 0 0 0 0 0.742 -0.948 2.562 2.830 0.000 2138 22 gamma 91 1897 0 0 0 0 0 0.413 -0.239 2.674 2.716 0.000 2139 22 gamma 91 1897 0 0 0 0 0 0.016 -0.019 0.430 0.431 0.000 2140 22 gamma 91 1900 0 0 0 0 0 0.082 0.088 -0.034 0.125 0.000 2141 22 gamma 91 1900 0 0 0 0 0 0.038 -0.034 -0.082 0.096 0.000 2142 22 gamma 91 1903 0 0 0 0 0 1.142 0.632 -4.037 4.243 0.000 2143 22 gamma 91 1903 0 0 0 0 0 0.377 0.153 -1.086 1.160 0.000 2144 22 gamma 91 1904 0 0 0 0 0 0.506 0.287 -1.177 1.313 0.000 2145 22 gamma 91 1904 0 0 0 0 0 0.911 0.524 -2.568 2.775 0.000 2146 310 (K_S0) -91 1908 0 2217 2218 0 0 9.180 -12.789 13.564 20.786 0.498 2147 -211 pi- 91 1908 0 0 0 0 0 0.135 -0.103 0.342 0.406 0.140 2148 211 pi+ 91 1908 0 0 0 0 0 1.650 -2.272 2.277 3.617 0.140 2149 22 gamma 91 1909 0 0 0 0 0 0.691 -0.928 1.114 1.606 0.000 2150 22 gamma 91 1909 0 0 0 0 0 0.171 -0.232 0.191 0.346 0.000 2151 22 gamma 91 1914 0 0 0 0 0 0.164 0.224 0.106 0.297 0.000 2152 22 gamma 91 1914 0 0 0 0 0 0.125 0.045 -0.002 0.133 0.000 2153 22 gamma 91 1919 0 0 0 0 0 0.031 0.096 0.008 0.102 0.000 2154 22 gamma 91 1919 0 0 0 0 0 0.002 0.127 -0.152 0.198 0.000 2155 22 gamma 91 1922 0 0 0 0 0 0.041 0.287 -0.003 0.290 0.000 2156 22 gamma 91 1922 0 0 0 0 0 -0.015 0.052 -0.060 0.081 0.000 2157 2212 p+ 91 1923 0 0 0 0 0 0.107 0.162 -0.218 0.983 0.938 2158 -211 pi- 91 1923 0 0 0 0 0 -0.056 0.096 0.024 0.180 0.140 2159 22 gamma 91 1927 0 0 0 0 0 -0.146 -0.211 -0.081 0.269 0.000 2160 22 gamma 91 1927 0 0 0 0 0 0.129 0.252 0.021 0.284 0.000 2161 22 gamma 91 1931 0 0 0 0 0 -0.315 0.025 -0.154 0.351 0.000 2162 22 gamma 91 1931 0 0 0 0 0 -0.138 0.088 -0.149 0.221 0.000 2163 -2112 nbar0 91 1932 0 0 0 0 0 -0.144 0.208 -1.140 1.498 0.940 2164 111 (pi0) -91 1932 0 2219 2220 0 0 -0.149 0.021 -0.266 0.334 0.135 2165 22 gamma 91 1934 0 0 0 0 0 -0.093 0.043 -4.237 4.238 0.000 2166 22 gamma 91 1934 0 0 0 0 0 -0.502 0.345 -15.176 15.188 0.000 2167 22 gamma 91 1938 0 0 0 0 0 -0.012 -0.033 -5.847 5.847 0.000 2168 22 gamma 91 1938 0 0 0 0 0 -0.296 0.055 -38.784 38.786 0.000 2169 22 gamma 91 1941 0 0 0 0 0 -0.020 -0.011 12.441 12.441 0.000 2170 22 gamma 91 1941 0 0 0 0 0 -0.254 0.136 44.054 44.055 0.000 2171 22 gamma 91 1942 0 0 0 0 0 0.050 -0.031 30.710 30.710 0.000 2172 22 gamma 91 1942 0 0 0 0 0 0.083 0.038 11.104 11.105 0.000 2173 22 gamma 91 1943 0 0 0 0 0 -0.065 0.015 18.901 18.901 0.000 2174 22 gamma 91 1943 0 0 0 0 0 -0.006 0.109 83.443 83.443 0.000 2175 22 gamma 91 1944 0 0 0 0 0 0.027 0.045 45.856 45.856 0.000 2176 22 gamma 91 1944 0 0 0 0 0 -0.055 -0.038 18.744 18.744 0.000 2177 22 gamma 91 1953 0 0 0 0 0 -0.001 -0.130 -0.044 0.138 0.000 2178 22 gamma 91 1953 0 0 0 0 0 -0.150 -0.754 -0.597 0.974 0.000 2179 22 gamma 91 1956 0 0 0 0 0 0.458 -0.020 0.532 0.702 0.000 2180 22 gamma 91 1956 0 0 0 0 0 0.020 0.013 -0.002 0.024 0.000 2181 22 gamma 91 1959 0 0 0 0 0 -0.049 0.029 0.255 0.262 0.000 2182 22 gamma 91 1959 0 0 0 0 0 0.008 0.307 1.520 1.551 0.000 2183 22 gamma 91 1966 0 0 0 0 0 0.166 0.108 -2.594 2.601 0.000 2184 22 gamma 91 1966 0 0 0 0 0 0.007 -0.020 -0.077 0.080 0.000 2185 22 gamma 91 1969 0 0 0 0 0 0.210 0.087 -0.812 0.844 0.000 2186 22 gamma 91 1969 0 0 0 0 0 0.135 -0.010 -0.253 0.288 0.000 2187 310 (K_S0) -91 1970 0 2221 2222 0 0 -0.567 -0.502 -1.246 1.541 0.498 2188 -211 pi- 91 1970 0 0 0 0 0 -1.041 0.347 -1.845 2.151 0.140 2189 211 pi+ 91 1970 0 0 0 0 0 -1.226 -0.137 -3.739 3.940 0.140 2190 22 gamma 91 2010 0 0 0 0 0 0.010 0.009 -0.061 0.062 0.000 2191 22 gamma 91 2010 0 0 0 0 0 0.028 -0.110 0.019 0.115 0.000 2192 22 gamma 91 2011 0 0 0 0 0 0.463 0.122 0.182 0.513 0.000 2193 22 gamma 91 2011 0 0 0 0 0 0.083 0.012 -0.024 0.087 0.000 2194 22 gamma 91 2014 0 0 0 0 0 0.041 -0.004 0.883 0.884 0.000 2195 22 gamma 91 2014 0 0 0 0 0 0.007 0.156 1.455 1.464 0.000 2196 22 gamma 91 2015 0 0 0 0 0 0.161 -0.016 0.335 0.372 0.000 2197 22 gamma 91 2015 0 0 0 0 0 0.077 0.074 0.411 0.424 0.000 2198 22 gamma 91 2073 0 0 0 0 0 0.314 0.125 0.374 0.504 0.000 2199 22 gamma 91 2073 0 0 0 0 0 0.181 0.158 0.160 0.289 0.000 2200 22 gamma 91 2074 0 0 0 0 0 -0.008 -0.001 0.020 0.022 0.000 2201 22 gamma 91 2074 0 0 0 0 0 0.205 0.195 -0.046 0.287 0.000 2202 22 gamma 91 2083 0 0 0 0 0 -0.016 -0.216 -0.618 0.655 0.000 2203 22 gamma 91 2083 0 0 0 0 0 -0.160 -0.213 -0.762 0.807 0.000 2204 22 gamma 91 2084 0 0 0 0 0 0.042 -0.030 -0.248 0.253 0.000 2205 11 e- 91 2084 0 0 0 0 0 -0.042 -0.049 -1.010 1.012 0.001 2206 -11 e+ 91 2084 0 0 0 0 0 -0.024 -0.022 -0.453 0.454 0.001 2207 22 gamma 91 2086 0 0 0 0 0 -0.024 -0.003 9.941 9.941 0.000 2208 22 gamma 91 2086 0 0 0 0 0 0.070 -0.140 16.479 16.480 0.000 2209 22 gamma 91 2098 0 0 0 0 0 -0.018 0.022 0.089 0.093 0.000 2210 22 gamma 91 2098 0 0 0 0 0 0.058 -0.146 0.671 0.689 0.000 2211 130 K_L0 91 2117 2117 0 0 0 0 0.729 -1.232 6.971 7.134 0.498 2212 130 K_L0 91 2119 2119 0 0 0 0 1.134 -1.271 9.662 9.823 0.498 2213 22 gamma 91 2120 0 0 0 0 0 0.042 -0.134 0.362 0.388 0.000 2214 22 gamma 91 2120 0 0 0 0 0 0.042 -0.544 2.209 2.275 0.000 2215 22 gamma 91 2127 0 0 0 0 0 36.928 -30.028 104.756 115.062 0.000 2216 22 gamma 91 2127 0 0 0 0 0 8.962 -7.352 25.619 28.119 0.000 2217 211 pi+ 91 2146 0 0 0 0 0 2.547 -3.831 4.053 6.132 0.140 2218 -211 pi- 91 2146 0 0 0 0 0 6.633 -8.958 9.511 14.653 0.140 2219 22 gamma 91 2164 0 0 0 0 0 0.002 0.033 -0.117 0.122 0.000 2220 22 gamma 91 2164 0 0 0 0 0 -0.151 -0.012 -0.149 0.213 0.000 2221 211 pi+ 91 2187 0 0 0 0 0 -0.334 -0.487 -0.670 0.904 0.140 2222 -211 pi- 91 2187 0 0 0 0 0 -0.232 -0.016 -0.576 0.637 0.140 Charge sum: 2.000 Momentum sum: -0.000 0.000 0.000 14000.000 14000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Warning in SpaceShower::pT2nextQCD: weight above unity PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> G g 5021 | 2745 185 185 | 1.210e-11 5.566e-13 | | q g -> G q 5022 | 7960 668 668 | 4.489e-11 1.012e-12 | | q qbar -> G g 5023 | 3961 147 147 | 9.339e-12 2.968e-13 | | | | | | sum | 14666 1000 1000 | 6.633e-11 1.193e-12 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Error in Pythia::next: hadronLevel failed; try again | | 1 Error in StringFragmentation::fragment: stuck in joining | | 88 Warning in PhaseSpace2to2tauyz::trialKin: maximum for cross section violated | | 2 Warning in SpaceShower::pT2nextQCD: weight above unity | | 1 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:08 dN/m: graviton mass spectrum 4.05*10^ 1 7 3.90*10^ 1 X 3.75*10^ 1 X 7 3.60*10^ 1 X X 3.45*10^ 1 X 7X 3.30*10^ 1 X XXX 3.15*10^ 1 X XXX 7 3.00*10^ 1 X X XXXX X 2.85*10^ 1 X X XXXX X 7 2.70*10^ 1 X XXX XXXX X X 2.55*10^ 1 X XXX XXXX X X 2.40*10^ 1 X XXX XXXX X 3 X 2.25*10^ 1 7 X7 XXX XXXX X7X 7X 2.10*10^ 1 XXXX33XXXXXXXXXXXXXX3XX 1.95*10^ 1 XXXXXXXXXXXXXXXXXXXXXXX7 7 1.80*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXX X X X 1.65*10^ 1 7 XXXXXXXXXXXXXXXXXXXXXXXXX 7 X X X 1.50*10^ 1 X XXXXXXXXXXXXXXXXXXXXXXXXX3X X X X 1.35*10^ 1 7 X7XXXXXXXXXXXXXXXXXXXXXXXXXXX X X777X 1.20*10^ 1 3XX3XXXXXXXXXXXXXXXXXXXXXXXXXXXXX 3XXXXXXXX3 1.05*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7XXXXXXXXXX 7 0.90*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 3 0.75*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7X X 77 0.60*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3X XX 3 3 0.45*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX7X 7 X 0.30*10^ 1 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 3X3XX3 333 3 33 3 0.15*10^ 1 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7XXXXXX 7XXX X777 7XX 7 X7 77 7 Contents *10^ 1 0000000011111112222223242233332322222211111111111111010000000000000000000000000000000000000000000000 *10^ 0 0000203912316382172000701134701123102894601282933381705837745124253201222021110122010210110100000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 3 0000000000000001111111111111122222222222222333333333333333444444444444445555555555555566666666666666 *10^ 2 0012234456778990112344566788901123345567889001223455677899012234456678990112334566788900123345567789 *10^ 1 0741852963074185296307418529630741852963074185296307418529630741852963074185296307418529630741852963 Entries = 1000 Mean = 2.2527e+03 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 9.9900e+02 Rms = 1.0675e+03 Overflow = 1.0000e+00 High edge = 7.0000e+03 2013-09-20 16:08 dN/dETjet: monojet check 5.80*10^ 1 X 5.60*10^ 1 X 5.40*10^ 1 5X 5.20*10^ 1 XX 5.00*10^ 1 XX 4.80*10^ 1 XX 4.60*10^ 1 XX 4.40*10^ 1 XX 4.20*10^ 1 XX5 4.00*10^ 1 XXX 3.80*10^ 1 XXX 3.60*10^ 1 XXXX 3.40*10^ 1 XXXX 3.20*10^ 1 XXXX 3.00*10^ 1 XXXX 2.80*10^ 1 XXXX 2.60*10^ 1 XXXX 2.40*10^ 1 XXXX 2.20*10^ 1 XXXXX 2.00*10^ 1 XXXXX 1.80*10^ 1 XXXXX 1.60*10^ 1 XXXXX5 1.40*10^ 1 XXXXXXX 5 1.20*10^ 1 XXXXXXXXXX 1.00*10^ 1 XXXXXXXXXX 5 0.80*10^ 1 XXXXXXXXXXX X 0.60*10^ 1 XXXXXXXXXXX X 5 0.40*10^ 1 XXXXXXXXXXXXX X X 0.20*10^ 1 XXXXXXXXXXXXXXX5X5 55 Contents *10^ 1 0000000000000055432111110000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000000000038162542328492415101100000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 3 0000000000000001111111111111122222222222222333333333333333444444444444445555555555555566666666666666 *10^ 2 0012234456778990112344566788901123345567889001223455677899012234456678990112334566788900123345567789 *10^ 1 0741852963074185296307418529630741852963074185296307418529630741852963074185296307418529630741852963 Entries = 312 Mean = 1.2968e+03 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 3.1200e+02 Rms = 2.9040e+02 Overflow = 0.0000e+00 High edge = 7.0000e+03 pythia8-8.1.80.orig/examples/outref/out280000644000175000017500000016746512217346176016413 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:08:39 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *----------------------- SusyLesHouches SUSY/BSM Interface ------------------------* | Last Change 01 Aug 2012 - P. Skands | Parsing: sps1aNarrowStopGluino.spc *------------------------------------------------------------------------------------* | | Spectrum Calculator was: SOFTSUSY version: 2.0.5 | Read SLHA spectrum from: sps1aNarrowStopGluino.spc | | ~g m | 1000021 607.714 | | ~d m ~dL ~sL ~bL ~dR ~sR ~bR | 1000001 568.441 1.000 0.000 0.000 0.000 0.000 0.000 | 1000003 568.441 0.000 1.000 0.000 0.000 0.000 0.000 | 1000005 513.065 0.000 0.000 0.939 0.000 0.000 0.345 | 2000001 545.228 0.000 0.000 0.000 1.000 0.000 0.000 | 2000003 545.228 0.000 0.000 0.000 0.000 1.000 0.000 | 2000005 543.727 0.000 0.000 -0.345 0.000 0.000 0.939 | | ~u m ~uL ~cL ~tL ~uR ~cR ~tR | 1000002 561.119 1.000 0.000 0.000 0.000 0.000 0.000 | 1000004 561.119 0.000 1.000 0.000 0.000 0.000 0.000 | 1000006 399.668 0.000 0.000 0.554 0.000 0.000 0.833 | 2000002 549.259 0.000 0.000 0.000 1.000 0.000 0.000 | 2000004 549.259 0.000 0.000 0.000 0.000 1.000 0.000 | 2000006 585.786 0.000 0.000 0.833 0.000 0.000 -0.554 | | ~e m ~eL ~muL ~tauL ~eR ~muR ~tauR | 1000011 202.916 1.000 0.000 0.000 0.000 0.000 0.000 | 1000013 202.916 0.000 1.000 0.000 0.000 0.000 0.000 | 1000015 134.491 0.000 0.000 0.282 0.000 0.000 0.959 | 2000011 144.103 0.000 0.000 0.000 1.000 0.000 0.000 | 2000013 144.103 0.000 0.000 0.000 0.000 1.000 0.000 | 2000015 206.868 0.000 0.000 0.959 0.000 0.000 -0.282 | | ~nu m ~nu_e ~nu_mu ~nu_tau | 1000012 185.258 1.000 0.000 0.000 | 1000014 185.258 0.000 1.000 0.000 | 1000016 184.708 0.000 0.000 1.000 | | ~chi0 m ~B ~W_3 ~H_1 ~H_2 | 1000022 96.688 0.986 -0.053 0.146 -0.053 | 1000023 181.088 0.099 0.945 -0.270 0.156 | 1000025 -363.756 -0.060 0.088 0.696 0.710 | 1000035 381.729 -0.117 0.311 0.649 -0.684 | | ~chi+ m U: ~W ~H | V: ~W ~H | 1000024 181.696 0.917 -0.399 | 0.973 -0.233 | 1000037 379.939 0.399 0.917 | 0.233 0.973 | | Higgs | alpha -0.114 | mu 357.681 (DRbar running value at Q = 467.034 GeV) | tan(beta) 9.749 (DRbar running value at Q = 467.034 GeV) | v 244.895 (DRbar running value at Q = 467.034 GeV) | mA 1.664e+05 (DRbar running value at Q = 467.034 GeV) | | Gauge | g' absent | g absent | g3 1.102 (DRbar running value at Q = 467.034 GeV) | *------------------------------------------------------------------------------------* PYTHIA Warning in SLHAinterface::initSLHA(): adding off shell DECAY mode 25 -> 24 -24 PYTHIA Warning in SLHAinterface::initSLHA(): adding off shell DECAY mode 25 -> 23 23 | (SLHA::initSUSY) Warning: Block GAUGE not found or incomplete; using sin(thetaW) at mZ *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 7.000e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> gluino gluino 1201 | 1.755e-09 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 50.91 mb | | | | pT0 = 2.70 gives sigmaInteraction = 208.15 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eCM | 7000.000 | 14000.000 10.00000 | | Check:nErrList | 2 | 0 | | HiggsA3:coup2d | 9.74862 | 1.00000 | | HiggsA3:coup2H1Z | -0.0116039 | 1.00000 | | HiggsA3:coup2H2Z | 0.99993 | 1.00000 | | HiggsA3:coup2l | 0.10258 | 1.00000 | | HiggsA3:coup2u | 0.10258 | 1.00000 | | HiggsH1:coup2d | 1.11305 | 1.00000 | | HiggsH1:coup2Hchg | 0.58109 | 0.0 | | HiggsH1:coup2l | 0.99874 | 1.00000 | | HiggsH1:coup2u | 0.99874 | 1.00000 | | HiggsH1:coup2W | 0.99993 | 1.00000 | | HiggsH1:coup2Z | 0.99993 | 1.00000 | | HiggsH2:coup2A3A3 | 0.20991 | 1.00000 | | HiggsH2:coup2d | 9.73636 | 1.00000 | | HiggsH2:coup2H1H1 | -0.64972 | 1.00000 | | HiggsH2:coup2Hchg | 0.19206 | 0.0 | | HiggsH2:coup2HchgW | 0.99993 | 0.0 | | HiggsH2:coup2l | -0.11418 | 1.00000 | | HiggsH2:coup2u | -0.11418 | 1.00000 | | HiggsH2:coup2W | -0.0116039 | 1.00000 | | HiggsH2:coup2Z | -0.0116039 | 1.00000 | | HiggsHchg:coup2H1W | -0.0116039 | 1.00000 | | HiggsHchg:coup2H2W | 0.99993 | 0.0 | | HiggsHchg:tanBeta | 9.74862 | 5.00000 | | Init:showChangedParticleData | off | on | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberShowEvent | 0 | 1 0 | | Next:showScaleAndVertex | on | off | | PDF:pSet | 8 | 2 1 16 | | RHadrons:allow | on | off | | RHadrons:allowDecay | off | on | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SLHA:file | sps1aNarrowStopGluino.spc | void | | SpaceShower:rapidityOrder | on | off | | SUSY:gg2gluinogluino | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 3.500e+03, e = 3.500e+03, m = 9.383e-01. Beam B: id = 2212, pz = -3.500e+03, e = 3.500e+03, m = 9.383e-01. In 1: id = 21, x = 1.104e-01, pdf = 5.410e-01 at Q2 = 5.021e+05. In 2: id = 21, x = 3.773e-01, pdf = 1.845e-02 at same Q2. Subprocess g g -> gluino gluino with code 1201 is 2 -> 2. It has sHat = 2.042e+06, tHat = -7.827e+05, uHat = -5.206e+05, pTHat = 3.644e+02, m3Hat = 6.077e+02, m4Hat = 6.077e+02, thetaHat = 1.817e+00, phiHat = 6.080e+00. alphaEM = 8.004e-03, alphaS = 1.025e-01 at Q2 = 5.021e+05. Impact parameter b = 5.185e-01 gives enhancement factor = 2.227e+00. Max pT scale for MPI = 7.000e+03, ISR = 7.000e+03, FSR = 7.000e+03. Number of MPI = 7, ISR = 12, FSRproc = 96, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m scale pol xProd yProd zProd tProd tau 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 7000.000 7000.000 0.000 9.000 0.000e+00 0.000e+00 0.000e+00 0.000e+00 0.000e+00 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 3500.000 3500.000 0.938 0.000 9.000 0.000e+00 0.000e+00 0.000e+00 0.000e+00 0.000e+00 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -3500.000 3500.000 0.938 0.000 9.000 0.000e+00 0.000e+00 0.000e+00 0.000e+00 0.000e+00 3 21 (g) -21 1 0 5 6 102 101 0.000 0.000 386.573 386.573 0.000 708.570 9.000 0.000e+00 0.000e+00 0.000e+00 0.000e+00 0.000e+00 4 21 (g) -21 2 0 5 6 104 103 0.000 0.000 -1320.534 1320.534 0.000 708.570 9.000 0.000e+00 0.000e+00 0.000e+00 0.000e+00 0.000e+00 5 1000021 (~g) -22 3 4 7 8 104 101 356.830 -73.671 -576.548 913.498 607.714 708.570 9.000 0.000e+00 0.000e+00 0.000e+00 0.000e+00 4.814e-13 6 1000021 (~g) -22 3 4 9 10 102 103 -356.830 73.671 -357.413 793.609 607.714 708.570 9.000 0.000e+00 0.000e+00 0.000e+00 0.000e+00 2.235e-11 7 1000006 (~t_1) -22 5 0 11 12 104 0 198.604 -14.767 -473.440 650.801 399.668 607.714 9.000 2.827e-13 -5.836e-14 -4.567e-13 7.237e-13 1.362e-11 8 -6 (tbar) -22 5 0 13 14 0 101 158.226 -58.904 -103.107 262.697 172.839 607.714 9.000 2.827e-13 -5.836e-14 -4.567e-13 7.237e-13 0.000e+00 9 1000005 (~b_1) -22 6 0 15 16 102 0 -216.618 68.267 -223.262 599.423 507.817 607.714 9.000 -1.312e-11 2.709e-12 -1.314e-11 2.918e-11 2.456e-15 10 -5 bbar 23 6 0 0 0 0 103 -140.212 5.405 -134.151 194.186 4.800 607.714 9.000 -1.312e-11 2.709e-12 -1.314e-11 2.918e-11 0.000e+00 11 1000024 (~chi_1+) -22 7 0 17 18 0 0 252.259 -93.090 -255.521 413.051 181.714 399.668 9.000 7.052e-12 -5.617e-13 -1.659e-11 2.291e-11 1.471e-11 12 5 b 23 7 0 0 0 104 0 -53.655 78.323 -217.919 237.750 4.800 399.668 9.000 7.052e-12 -5.617e-13 -1.659e-11 2.291e-11 0.000e+00 13 -24 (W-) -22 8 0 19 20 0 0 105.688 -19.214 -134.288 189.684 80.049 172.839 9.000 2.827e-13 -5.836e-14 -4.567e-13 7.237e-13 0.000e+00 14 -5 bbar 23 8 0 0 0 0 101 52.538 -39.690 31.181 73.012 4.800 172.839 9.000 2.827e-13 -5.836e-14 -4.567e-13 7.237e-13 0.000e+00 15 -1000024 (~chi_1-) -22 9 0 21 22 0 0 -195.068 203.312 -103.345 350.830 181.698 507.817 9.000 -1.312e-11 2.710e-12 -1.314e-11 2.919e-11 4.661e-12 16 6 (t) -22 9 0 23 24 102 0 -21.550 -135.045 -119.917 248.594 169.461 507.817 9.000 -1.312e-11 2.710e-12 -1.314e-11 2.919e-11 0.000e+00 17 -1000015 (~tau_1+) -22 11 0 25 26 0 0 218.535 -118.109 -220.258 358.217 134.533 181.714 9.000 2.747e-11 -8.095e-12 -3.727e-11 5.633e-11 9.246e-13 18 16 nu_tau 23 11 0 0 0 0 0 33.724 25.019 -35.264 54.834 0.000 181.714 9.000 2.747e-11 -8.095e-12 -3.727e-11 5.633e-11 0.000e+00 19 13 mu- 23 13 0 0 0 0 0 56.371 -43.493 -106.455 128.071 0.106 80.049 9.000 2.827e-13 -5.836e-14 -4.567e-13 7.237e-13 3.098e+05 20 -14 nu_mubar 23 13 0 0 0 0 0 49.316 24.279 -27.833 61.613 0.000 80.049 9.000 2.827e-13 -5.836e-14 -4.567e-13 7.237e-13 0.000e+00 21 1000015 (~tau_1-) -22 15 0 27 28 0 0 -184.688 137.664 -98.013 284.153 134.444 181.698 9.000 -1.813e-11 7.925e-12 -1.580e-11 3.819e-11 1.177e-12 22 -16 nu_taubar 23 15 0 0 0 0 0 -10.379 65.648 -5.332 66.677 0.000 181.698 9.000 -1.813e-11 7.925e-12 -1.580e-11 3.819e-11 0.000e+00 23 24 (W+) -22 16 0 29 30 0 0 24.569 -85.677 -12.293 121.432 81.550 169.461 9.000 -1.312e-11 2.710e-12 -1.314e-11 2.919e-11 0.000e+00 24 5 b 23 16 0 0 0 102 0 -46.119 -49.368 -107.624 127.162 4.800 169.461 9.000 -1.312e-11 2.710e-12 -1.314e-11 2.919e-11 0.000e+00 25 1000022 ~chi_10 23 17 0 0 0 0 0 155.665 -120.048 -179.812 283.415 96.688 134.533 9.000 2.897e-11 -8.907e-12 -3.879e-11 5.879e-11 0.000e+00 26 -15 tau+ 23 17 0 0 0 0 0 62.870 1.939 -40.446 74.802 1.777 134.533 9.000 2.897e-11 -8.907e-12 -3.879e-11 5.879e-11 2.655e-01 27 1000022 ~chi_10 23 21 0 0 0 0 0 -121.719 103.531 -37.784 190.553 96.688 134.444 9.000 -1.974e-11 9.129e-12 -1.665e-11 4.067e-11 0.000e+00 28 15 tau- 23 21 0 0 0 0 0 -62.969 34.133 -60.230 93.600 1.777 134.444 9.000 -1.974e-11 9.129e-12 -1.665e-11 4.067e-11 7.161e-02 29 -15 tau+ 23 23 0 0 0 0 0 10.022 -29.238 -44.982 54.606 1.777 81.550 9.000 -1.312e-11 2.710e-12 -1.314e-11 2.919e-11 2.541e-01 30 16 nu_tau 23 23 0 0 0 0 0 14.546 -56.439 32.690 66.825 0.000 81.550 9.000 -1.312e-11 2.710e-12 -1.314e-11 2.919e-11 0.000e+00 Charge sum: 0.000 Momentum sum: 0.000 -0.000 -933.960 1707.107 1428.961 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Warning in TauDecays::decay: unknown tau production, assuming unpolarized and uncorrelated PYTHIA Error in StringFragmentation::fragmentToJunction: caught in junction flavour loop PYTHIA Error in Pythia::next: hadronLevel failed; try again PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> gluino gluino 1201 | 2265 200 200 | 1.473e-10 5.959e-12 | | | | | | sum | 2265 200 200 | 1.473e-10 5.959e-12 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 2 Error in Pythia::next: hadronLevel failed; try again | | 2 Error in StringFragmentation::fragmentToJunction: caught in junction flavour loop | | 2 Warning in SLHAinterface::initSLHA(): adding off shell DECAY mode | | 1 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | 273 Warning in TauDecays::decay: unknown tau production, assuming unpolarized and uncorrelated | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* Composition of produced R-hadrons code name times -1093224 Rbar-(~g suu) 2 -1093214 Rbar0(~g sud) 4 -1093114 Rbar+(~g sdd) 1 -1092214 Rbar-(~g uud) 9 -1092114 Rbar0(~g udd) 8 -1009323 R-(~g s ubar) 15 -1009313 R0(~g s dbar) 14 -1009213 R-(~g d ubar) 52 1000993 R0(~g g) 41 1009113 R0(~g d dbar) 61 1009213 R+(~g u dbar) 62 1009223 R0(~g u ubar) 62 1009313 R0(~g d sbar) 12 1009323 R+(~g u sbar) 11 1009333 R0(~g s sbar) 6 1091114 R-(~g ddd) 1 1092114 R0(~g udd) 22 1092214 R+(~g uud) 7 1092224 R++(~g uuu) 2 1093114 R-(~g sdd) 1 1093214 R0(~g sud) 3 1093224 R+(~g suu) 4 2013-09-20 16:08 charged multiplicity 1.40*10^ 1 X 1.35*10^ 1 X 1.30*10^ 1 X 1.25*10^ 1 X 1.20*10^ 1 XX X 1.15*10^ 1 XX X 1.10*10^ 1 XX X X X X 1.05*10^ 1 XX X X X X 1.00*10^ 1 XX X XXXX X 0.95*10^ 1 XX X XXXX X 0.90*10^ 1 XXXX XXXXXXXXX 0.85*10^ 1 XXXX XXXXXXXXX 0.80*10^ 1 XXXX XXXXXXXXX X 0.75*10^ 1 XXXX XXXXXXXXX X 0.70*10^ 1 XXXX XXXXXXXXX X 0.65*10^ 1 XXXX XXXXXXXXX X 0.60*10^ 1 XXXXXXXXXXXXXX X X 0.55*10^ 1 XXXXXXXXXXXXXX X X 0.50*10^ 1 X XXXXXXXXXXXXXXXXX X 0.45*10^ 1 X XXXXXXXXXXXXXXXXX X 0.40*10^ 1 X XXXXXXXXXXXXXXXXXX X 0.35*10^ 1 X XXXXXXXXXXXXXXXXXX X 0.30*10^ 1 XXXXXXXXXXXXXXXXXXXXXXX XX 0.25*10^ 1 XXXXXXXXXXXXXXXXXXXXXXX XX 0.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.15*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.10*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 0.05*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX Contents *10^ 1 0000000000001100101111010000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0000003534994269192010915653822233200011000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 200 Mean = 1.5094e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 2.0000e+02 Rms = 5.5307e+01 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:08 dn/dy charged 0.96*10^ 3 6 0.92*10^ 3 966X 26 0.88*10^ 3 1XXXX8XX 0.84*10^ 3 XXXXXXXXX 0.80*10^ 3 1 XXXXXXXXX 0.76*10^ 3 8X8XXXXXXXXX6 6 0.72*10^ 3 XXXXXXXXXXXXX X 0.68*10^ 3 6XXXXXXXXXXXXX8X63 0.64*10^ 3 3XXXXXXXXXXXXXXXXXX 0.60*10^ 3 22XXXXXXXXXXXXXXXXXXX6 0.56*10^ 3 57XXXXXXXXXXXXXXXXXXXXXXX26 0.52*10^ 3 1XXXXXXXXXXXXXXXXXXXXXXXXXXX2 0.48*10^ 3 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.44*10^ 3 95XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX714 0.40*10^ 3 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.36*10^ 3 13XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 6 0.32*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9XX 0.28*10^ 3 97XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.24*10^ 3 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX65 0.20*10^ 3 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX42 0.16*10^ 3 442XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX61 0.12*10^ 3 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6 1 0.08*10^ 3 2445696XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3414 0.04*10^ 3 1 23598XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8X6432 1 Contents *10^ 2 0000000000000000000001111222233344445555667778899998897676655554444433332221111110000000000000000000 *10^ 1 0000000001233555667683328007623832683466165654410047804746586248520171415217642207855453321100000000 *10^ 0 0000104181163047026497474916641840529779043320555542726033220629663554497485634159435271847091211000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 30046 Mean = 3.1152e-03 Underflow = 0.0000e+00 Low edge = -1.0000e+01 All chan = 3.0046e+04 Rms = 2.8765e+00 Overflow = 0.0000e+00 High edge = 1.0000e+01 2013-09-20 16:08 dn/dy R-hadrons 3.00*10^ 1 X 2 2.88*10^ 1 X X 2.76*10^ 1 5X 5 X 2.64*10^ 1 XX X X 2.52*10^ 1 XX X X 2.40*10^ 1 XXXX XX 2.28*10^ 1 XXXX3 XX 2.16*10^ 1 XXXXX XX 2.04*10^ 1 XXXXX XX 1.92*10^ 1 8 XXXXX XX 1.80*10^ 1 X X XXXXX XX2 1.68*10^ 1 X X3XXXXX XXX 1.56*10^ 1 X 5XXXXXXX5XXX 5 1.44*10^ 1 X XXXXXXXXXXXX X 1.32*10^ 1 X XXXXXXXXXXXX X8 1.20*10^ 1 XXXXXXXXXXXXXXXXX2 1.08*10^ 1 3XXXXXXXXXXXXXXXXXX 0.96*10^ 1 5 XXXXXXXXXXXXXXXXXXX 0.84*10^ 1 X XXXXXXXXXXXXXXXXXXX 0.72*10^ 1 X8XXXXXXXXXXXXXXXXXXX8 0.60*10^ 1 XXXXXXXXXXXXXXXXXXXXXX X 0.48*10^ 1 XXXXXXXXXXXXXXXXXXXXXX 3X 0.36*10^ 1 5 XXXXXXXXXXXXXXXXXXXXXX5XX 0.24*10^ 1 X XXXXXXXXXXXXXXXXXXXXXXXXX 0.12*10^ 1 8 8X8XXXXXXXXXXXXXXXXXXXXXXXXX8 8 Contents *10^ 1 0000000000000000000000000000000000000000111111232221221111100000000000000000000000000000000000000000 *10^ 0 0000000000000000000000000000000001013197082596704725947253173461000100000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 5444444444433333333332222222222111111111100000000000000000001111111111222222222233333333334444444444 *10^-1 0987654321098765432109876543210987654321098765432101234567890123456789012345678901234567890123456789 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 400 Mean = -5.5250e-02 Underflow = 0.0000e+00 Low edge = -5.0000e+00 All chan = 4.0000e+02 Rms = 5.9820e-01 Overflow = 0.0000e+00 High edge = 5.0000e+00 2013-09-20 16:08 pT R-hadrons 1.50*10^ 1 X X 1.44*10^ 1 X 3 333 X 1.38*10^ 1 X X XXX X 1.32*10^ 1 X X XXX7 X 1.26*10^ 1 X X XXXX X 1.20*10^ 1 X X XXXXX X 1.14*10^ 1 X X3 XXXXX 3 X 1.08*10^ 1 X XX XXXXX X X 1.02*10^ 1 X7 XX 7 XXXXX X 7 X 0.96*10^ 1 XX XX X XXXXX X X X 0.90*10^ 1 XX XX XXXXXXX X X XX XX 0.84*10^ 1 3 3 XX 3XX XXXXXXX X X3XX XX 0.78*10^ 1 X X XX XXX XXXXXXX X XXXX XX 0.72*10^ 1 X X XX77XXX7XXXXXXX X XXXX7 7 XX7 0.66*10^ 1 X X XXXXXXXXXXXXXXX X XXXXX X XXX 0.60*10^ 1 XXX X XXXXXXXXXXXXXXX X XXXXX XX XXX X X 0.54*10^ 1 33XXX X3XXXXXXXXXXXXXXX X3XXXXX XX3XXX X3 3 3X 0.48*10^ 1 XXXXX XXXXXXXXXXXXXXXXX XXXXXXX XXXXXX XX X XX 0.42*10^ 1 XXXXX XXXXXXXXXXXXXXXXX XXXXXXX7XXXXXX 7XX X XX 0.36*10^ 1 XXXXX XXXXXXXXXXXXXXXXX XXXXXXXXXXXXXX XXX X XX 0.30*10^ 1 XXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX X XX X X 0.24*10^ 1 XXXXX3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX33XXX3X333XX 3 X3 3 3 X3 0.18*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X XX X X XX 0.12*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 7XX X77X 7XX7 7 7 7 7 7 7 77 0.06*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X XXX XXXX XXXX X X X X X X XX Contents *10^ 1 0000000000011000110101111101010010000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0005566828550778417094443231508957476599722465252225602013202112013210101001001000000100000010001100 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 1 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^ 0 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 400 Mean = 2.8427e+02 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 3.9700e+02 Rms = 1.6550e+02 Overflow = 3.0000e+00 High edge = 1.0000e+03 2013-09-20 16:08 p_RHadron / p_sparticle 0.92*10^ 2 8 0.88*10^ 2 X 0.84*10^ 2 X 0.80*10^ 2 X 0.76*10^ 2 XX 0.72*10^ 2 XX 0.68*10^ 2 XX 0.64*10^ 2 XXX 0.60*10^ 2 XXX 0.56*10^ 2 3XXX 0.52*10^ 2 XXXX 0.48*10^ 2 XXXX 0.44*10^ 2 XXXX 0.40*10^ 2 XXXX 0.36*10^ 2 XXXX 0.32*10^ 2 XXXX5 0.28*10^ 2 2XXXXX 0.24*10^ 2 XXXXXX 0.20*10^ 2 XXXXXX 0.16*10^ 2 XXXXXXX 0.12*10^ 2 5XXXXXXX 0.08*10^ 2 5XXXXXXXX7 0.04*10^ 2 5 3 3 5883XXXXXXXXXX533353 3 Contents *10^ 1 0000000000000000000000000000000000000000000000125796310000000000000000000000000000000000000000000000 *10^ 0 0000000000000000000200000001010000000000023316053614067211121000000000000000000000000000100000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000000000000000000000000000000001111111111111111111111111111111111111111111111111111 *10^-1 9999999999999999999999999999999999999999999999990000000000000000000000000000000000000000000000000011 *10^-2 0001111122222333334444455555666667777788888999990000011111222223333344444555556666677777888889999900 Entries = 400 Mean = 9.9997e-01 Underflow = 0.0000e+00 Low edge = 9.0000e-01 All chan = 4.0000e+02 Rms = 8.0573e-03 Overflow = 0.0000e+00 High edge = 1.1000e+00 2013-09-20 16:08 m(Rhadron) - m(sparticle) 1.16*10^ 2 X 1.12*10^ 2 X 1.08*10^ 2 X 1.04*10^ 2 X 1.00*10^ 2 X 0.96*10^ 2 X 0.92*10^ 2 X 0.88*10^ 2 X 0.84*10^ 2 X 0.80*10^ 2 X 0.76*10^ 2 X 0.72*10^ 2 X 0.68*10^ 2 X 0.64*10^ 2 X 0.60*10^ 2 X 0.56*10^ 2 X 0.52*10^ 2 X X 0.48*10^ 2 X X 8 0.44*10^ 2 X3X X 0.40*10^ 2 XXX X 0.36*10^ 2 XXX X 0.32*10^ 2 XXX X 0.28*10^ 2 XXX X 0.24*10^ 2 XXX 7 X 0.20*10^ 2 XXXXX X 7 0.16*10^ 2 XXXXX X X 0.12*10^ 2 XXXXX2 X 7X 2 0.08*10^ 2 2 XXXXXX5X7XX 2X 0.04*10^ 2 33 33 8X8XXXXXXXXXXX5XX335X335 35 3 3 Contents *10^ 2 0000000000000000000000000000000100000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000000000000000000000000145220040110000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000000000000000000110110353612039677192591124112001201001000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^-1 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^-2 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 400 Mean = 1.7671e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 3.9900e+02 Rms = 2.5528e-01 Overflow = 1.0000e+00 High edge = 5.0000e+00 2013-09-20 16:08 R-hadron decay vertex (mm from origin) 4.05*10^ 2 7 3.90*10^ 2 X 3.75*10^ 2 X 3.60*10^ 2 X 3.45*10^ 2 X 3.30*10^ 2 X 3.15*10^ 2 X 3.00*10^ 2 X 2.85*10^ 2 X 2.70*10^ 2 X 2.55*10^ 2 X 2.40*10^ 2 X 2.25*10^ 2 X 2.10*10^ 2 X 1.95*10^ 2 X 1.80*10^ 2 X 1.65*10^ 2 X 1.50*10^ 2 X 1.35*10^ 2 X 1.20*10^ 2 X 1.05*10^ 2 X 0.90*10^ 2 X 0.75*10^ 2 X 0.60*10^ 2 X 0.45*10^ 2 X 0.30*10^ 2 X 0.15*10^ 2 X Contents *10^ 2 4000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 1 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^ 0 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 400 Mean = 5.0000e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 4.0000e+02 Rms = 0.0000e+00 Overflow = 0.0000e+00 High edge = 1.0000e+03 pythia8-8.1.80.orig/examples/outref/out060000644000175000017500000026756612217346171016405 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:01:47 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide e- with e+ at a CM energy of 9.119e+01 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | f fbar -> gamma*/Z0 221 | 4.350e-05 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eCM | 91.18760 | 14000.000 10.00000 | | Beams:idA | 11 | 2212 | | Beams:idB | -11 | 2212 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PDF:lepton | off | on | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | WeakSingleBoson:ffbar2gmZ | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products 23 Z0 3 0 0 91.18760 2.50687 10.00000 0.00000 0.00000e+00 1 1 0 0 0 0 1 0.1541199 0 1 -1 1 1 0.1195484 0 2 -2 2 1 0.1541093 0 3 -3 3 1 0.1193873 0 4 -4 4 1 0.1523969 0 5 -5 5 0 0.0335122 0 11 -11 6 0 0.0666593 0 12 -12 7 0 0.0335119 0 13 -13 8 0 0.0666593 0 14 -14 9 0 0.0334363 0 15 -15 10 0 0.0666593 0 16 -16 -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 11, pz = 4.559e+01, e = 4.559e+01, m = 5.110e-04. Beam B: id = -11, pz = -4.559e+01, e = 4.559e+01, m = 5.110e-04. In 1: id = 11, x = 1.000e+00, pdf = 1.000e+00 at Q2 = 8.315e+03. In 2: id = -11, x = 1.000e+00, pdf = 1.000e+00 at same Q2. Subprocess f fbar -> gamma*/Z0 with code 221 is 2 -> 1. It has sHat = 8.315e+03. alphaEM = 7.818e-03, alphaS = 1.350e-01 at Q2 = 8.315e+03. Impact parameter b = 0.000e+00 gives enhancement factor = 1.000e+00. Max pT scale for MPI = 9.119e+01, ISR = 9.119e+01, FSR = 9.119e+01. Number of MPI = 1, ISR = 0, FSRproc = 0, FSRreson = 11. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 91.188 91.188 1 11 (e-) -12 0 0 3 0 0 0 0.000 0.000 45.594 45.594 0.001 2 -11 (e+) -12 0 0 4 0 0 0 0.000 0.000 -45.594 45.594 0.001 3 11 (e-) -21 1 0 5 0 0 0 0.000 0.000 45.594 45.594 0.000 4 -11 (e+) -21 2 0 5 0 0 0 0.000 0.000 -45.594 45.594 0.000 5 23 (Z0) -22 3 4 6 7 0 0 0.000 0.000 0.000 91.188 91.188 6 4 c 23 5 0 0 0 101 0 -7.270 -38.218 23.730 45.594 1.500 7 -4 cbar 23 5 0 0 0 0 101 7.270 38.218 -23.730 45.594 1.500 Charge sum: 0.000 Momentum sum: 0.000 0.000 0.000 91.188 91.188 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 91.188 91.188 1 11 (e-) -12 0 0 3 0 0 0 0.000 0.000 45.594 45.594 0.001 2 -11 (e+) -12 0 0 4 0 0 0 0.000 0.000 -45.594 45.594 0.001 3 11 (e-) -21 1 0 5 0 0 0 0.000 0.000 45.594 45.594 0.000 4 -11 (e+) -21 2 0 5 0 0 0 0.000 0.000 -45.594 45.594 0.000 5 23 (Z0) -22 3 4 6 7 0 0 0.000 0.000 0.000 91.188 91.188 6 4 (c) -23 5 0 10 10 101 0 -7.270 -38.218 23.730 45.594 1.500 7 -4 (cbar) -23 5 0 8 9 0 101 7.270 38.218 -23.730 45.594 1.500 8 -4 (cbar) -51 7 0 11 12 0 103 2.515 35.231 -23.921 42.685 1.500 9 21 (g) -51 7 0 13 13 103 101 4.451 1.390 1.183 4.810 0.000 10 4 (c) -52 6 6 14 15 101 0 -6.966 -36.622 22.739 43.692 1.500 11 -4 (cbar) -51 8 0 48 48 0 105 0.242 19.486 -12.862 23.398 1.500 12 21 (g) -51 8 0 17 18 105 103 2.375 15.777 -11.032 19.397 0.000 13 21 (g) -52 9 9 16 16 103 101 4.349 1.359 1.156 4.701 0.000 14 4 (c) -51 10 0 40 40 106 0 -4.425 -27.750 17.958 33.382 1.500 15 21 (g) -51 10 0 25 25 101 106 -2.484 -8.854 4.796 10.371 0.000 16 21 (g) -52 13 13 19 19 103 101 4.292 1.341 1.141 4.639 0.000 17 21 (g) -51 12 0 20 21 105 107 2.121 13.919 -8.485 16.438 0.000 18 21 (g) -51 12 0 22 22 107 103 0.459 1.922 -2.492 3.181 0.000 19 21 (g) -52 16 16 23 24 103 101 4.087 1.277 1.086 4.417 0.000 20 21 (g) -51 17 0 26 27 105 108 2.038 12.366 -8.566 15.180 0.000 21 21 (g) -51 17 0 28 28 108 107 0.246 2.238 -0.808 2.392 0.000 22 21 (g) -52 18 18 42 0 107 103 0.296 1.237 -1.603 2.046 0.000 23 1 (d) -51 19 0 42 0 103 0 0.079 0.152 -0.317 0.488 0.330 24 -1 (dbar) -51 19 0 31 31 0 101 3.916 0.799 1.579 4.310 0.330 25 21 (g) -52 15 15 29 30 101 106 -2.392 -8.528 4.619 9.990 0.000 26 21 (g) -51 20 0 47 47 105 109 1.812 7.502 -5.091 9.246 0.000 27 21 (g) -51 20 0 41 0 109 108 0.381 6.266 -3.981 7.433 0.000 28 21 (g) -52 21 21 41 0 108 107 0.092 0.836 -0.302 0.894 0.000 29 21 (g) -51 25 0 35 36 111 106 -1.126 -4.462 2.990 5.488 0.000 30 21 (g) -51 25 0 32 33 101 111 -1.225 -4.058 1.646 4.547 0.000 31 -1 (dbar) -52 24 24 34 34 0 101 3.875 0.791 1.563 4.265 0.330 32 21 (g) -51 30 0 37 37 112 111 -0.620 -3.733 1.285 3.996 0.000 33 21 (g) -51 30 0 58 58 101 112 -0.473 -0.298 0.414 0.696 0.000 34 -1 (dbar) -52 31 31 59 59 0 101 3.743 0.763 1.510 4.121 0.330 35 21 (g) -51 29 0 38 39 113 106 0.029 0.018 -0.005 0.034 0.000 36 21 (g) -51 29 0 56 56 111 113 -1.541 -6.804 3.794 7.941 0.000 37 21 (g) -52 32 32 57 57 112 111 -0.234 -1.409 0.485 1.508 0.000 38 21 (g) -51 35 0 44 0 113 116 -0.458 -5.058 3.082 5.941 0.000 39 21 (g) -51 35 0 43 0 116 106 -0.553 -1.396 1.100 1.861 0.000 40 4 (c) -52 14 14 43 0 106 0 -3.384 -21.278 13.772 25.614 1.500 41 21 (g) -73 27 28 46 46 109 107 0.473 7.102 -4.283 8.327 0.579 42 1 (d) -73 22 23 45 45 107 0 0.374 1.388 -1.920 2.534 0.819 43 4 (c) -73 39 40 44 0 116 0 -3.938 -22.674 14.871 27.476 2.039 44 4 (c) -73 38 43 55 55 113 0 -4.396 -27.732 17.953 33.416 2.443 45 1 (d) -71 42 42 49 54 107 0 0.374 1.388 -1.920 2.534 0.819 46 21 (g) -71 41 41 49 54 109 107 0.473 7.102 -4.283 8.327 0.579 47 21 (g) -71 26 26 49 54 105 109 1.812 7.502 -5.091 9.246 0.000 48 -4 (cbar) -71 11 11 49 54 0 105 0.242 19.486 -12.862 23.398 1.500 49 111 (pi0) -83 45 48 73 74 0 0 0.467 0.873 -0.553 1.142 0.135 50 223 (omega) -83 45 48 75 77 0 0 0.279 3.286 -2.683 4.323 0.784 51 113 (rho0) -83 45 48 67 68 0 0 0.163 1.520 -1.472 2.261 0.781 52 -211 pi- 84 45 48 0 0 0 0 0.538 5.364 -3.349 6.348 0.140 53 321 K+ 84 45 48 0 0 0 0 0.589 6.097 -4.418 7.568 0.494 54 -433 (D*_s-) -84 45 48 78 79 0 0 0.864 18.339 -11.681 21.862 2.112 55 4 (c) -71 44 44 60 66 113 0 -4.396 -27.732 17.953 33.416 2.443 56 21 (g) -71 36 36 60 66 111 113 -1.541 -6.804 3.794 7.941 0.000 57 21 (g) -71 37 37 60 66 112 111 -0.234 -1.409 0.485 1.508 0.000 58 21 (g) -71 33 33 60 66 101 112 -0.473 -0.298 0.414 0.696 0.000 59 -1 (dbar) -71 34 34 60 66 0 101 3.743 0.763 1.510 4.121 0.330 60 433 (D*_s+) -83 55 59 80 81 0 0 -4.365 -25.108 15.669 29.991 2.112 61 -321 K- 83 55 59 0 0 0 0 -0.057 -4.172 2.561 4.921 0.494 62 211 pi+ 83 55 59 0 0 0 0 -1.590 -5.755 3.637 6.993 0.140 63 113 (rho0) -84 55 59 69 70 0 0 -0.099 -0.410 0.291 0.855 0.684 64 223 (omega) -84 55 59 82 84 0 0 0.542 0.065 0.855 1.288 0.795 65 -211 pi- 84 55 59 0 0 0 0 1.390 -0.801 0.056 1.611 0.140 66 213 (rho+) -84 55 59 71 72 0 0 1.277 0.702 1.086 2.023 0.888 67 211 pi+ 91 51 0 0 0 0 0 0.078 0.040 -0.382 0.416 0.140 68 -211 pi- 91 51 0 0 0 0 0 0.085 1.480 -1.089 1.845 0.140 69 211 pi+ 91 63 0 0 0 0 0 -0.233 -0.003 -0.066 0.280 0.140 70 -211 pi- 91 63 0 0 0 0 0 0.134 -0.407 0.358 0.575 0.140 71 211 pi+ 91 66 0 0 0 0 0 1.284 0.732 1.143 1.874 0.140 72 111 (pi0) -91 66 0 85 86 0 0 -0.007 -0.030 -0.057 0.150 0.135 73 22 gamma 91 49 0 0 0 0 0 0.331 0.704 -0.476 0.911 0.000 74 22 gamma 91 49 0 0 0 0 0 0.136 0.170 -0.078 0.231 0.000 75 211 pi+ 91 50 0 0 0 0 0 -0.024 1.306 -1.039 1.675 0.140 76 -211 pi- 91 50 0 0 0 0 0 0.396 1.696 -1.354 2.210 0.140 77 111 (pi0) -91 50 0 87 88 0 0 -0.093 0.284 -0.291 0.438 0.135 78 -431 (D_s-) -91 54 0 89 90 0 0 0.759 17.340 -11.188 20.744 1.968 79 22 gamma 91 54 0 0 0 0 0 0.105 0.999 -0.493 1.119 0.000 80 431 (D_s+) -91 60 0 91 92 0 0 -4.128 -24.034 14.849 28.619 1.968 81 22 gamma 91 60 0 0 0 0 0 -0.236 -1.074 0.820 1.372 0.000 82 211 pi+ 91 64 0 0 0 0 0 0.182 -0.113 0.281 0.380 0.140 83 -211 pi- 91 64 0 0 0 0 0 -0.037 -0.103 0.058 0.187 0.140 84 111 (pi0) -91 64 0 93 94 0 0 0.397 0.281 0.516 0.722 0.135 85 22 gamma 91 72 0 0 0 0 0 0.017 -0.040 0.034 0.055 0.000 86 22 gamma 91 72 0 0 0 0 0 -0.023 0.010 -0.091 0.095 0.000 87 22 gamma 91 77 0 0 0 0 0 -0.068 0.055 -0.035 0.094 0.000 88 22 gamma 91 77 0 0 0 0 0 -0.025 0.229 -0.255 0.344 0.000 89 333 (phi) -91 78 0 95 96 0 0 0.948 13.421 -8.611 16.007 1.021 90 -213 (rho-) -91 78 0 97 98 0 0 -0.189 3.919 -2.577 4.737 0.635 91 -15 (tau+) -91 80 0 99 101 0 0 -4.032 -22.771 13.946 27.064 1.777 92 16 nu_tau 91 80 0 0 0 0 0 -0.096 -1.262 0.903 1.555 0.000 93 22 gamma 91 84 0 0 0 0 0 0.176 0.203 0.305 0.407 0.000 94 22 gamma 91 84 0 0 0 0 0 0.221 0.078 0.211 0.315 0.000 95 130 K_L0 91 89 0 0 0 0 0 0.351 6.501 -4.134 7.728 0.498 96 310 (K_S0) -91 89 0 102 103 0 0 0.598 6.920 -4.477 8.278 0.498 97 -211 pi- 91 90 0 0 0 0 0 -0.281 1.284 -1.042 1.683 0.140 98 111 (pi0) -91 90 0 104 105 0 0 0.092 2.635 -1.536 3.054 0.135 99 -16 nu_taubar 91 91 0 0 0 0 0 0.100 -0.434 0.408 0.604 0.000 100 111 (pi0) -91 91 0 106 107 0 0 -0.191 -2.298 1.427 2.715 0.135 101 211 pi+ 91 91 0 0 0 0 0 -3.941 -20.039 12.111 23.745 0.140 102 211 pi+ 91 96 0 0 0 0 0 0.003 0.728 -0.499 0.894 0.140 103 -211 pi- 91 96 0 0 0 0 0 0.594 6.191 -3.978 7.384 0.140 104 22 gamma 91 98 0 0 0 0 0 0.003 1.651 -1.002 1.931 0.000 105 22 gamma 91 98 0 0 0 0 0 0.089 0.983 -0.534 1.122 0.000 106 22 gamma 91 100 0 0 0 0 0 -0.209 -2.108 1.293 2.482 0.000 107 22 gamma 91 100 0 0 0 0 0 0.019 -0.190 0.134 0.233 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 -0.000 91.188 91.188 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Sphericity Listing -------- no lambda e_x e_y e_z 1 0.98903 0.13845 0.84116 -0.52277 2 0.00862 -0.91349 -0.09545 -0.39551 3 0.00235 0.38259 -0.53230 -0.75517 -------- End PYTHIA Sphericity Listing ---- -------- PYTHIA Sphericity Listing -------- Nonstandard momentum power = 1.000 no lambda e_x e_y e_z 1 0.93601 0.09874 0.83519 -0.54102 2 0.04749 -0.86684 -0.19482 -0.45895 3 0.01650 0.48871 -0.51429 -0.70474 -------- End PYTHIA Sphericity Listing ---- -------- PYTHIA Thrust Listing ------------ value e_x e_y e_z Thr 0.94950 0.09744 0.84420 -0.52709 Maj 0.11287 0.92660 0.11632 0.35760 Min 0.05898 0.36319 -0.52325 -0.77091 -------- End PYTHIA Thrust Listing -------- -------- PYTHIA ClusterJet Listing, Lund pT = 8.900 GeV --- no mult p_x p_y p_z e m 0 14 -2.648 -33.789 23.003 45.149 18.988 1 19 2.644 35.485 -24.314 43.880 8.250 -------- End PYTHIA ClusterJet Listing ----------------------- -------- PYTHIA ClusterJet Listing, JADE m = 8.900 GeV --- no mult p_x p_y p_z e m 0 15 2.891 35.384 -23.739 42.995 4.967 1 6 -6.071 -33.252 20.481 39.698 3.737 2 12 3.177 -0.435 1.947 6.335 5.105 -------- End PYTHIA ClusterJet Listing ----------------------- -------- PYTHIA ClusterJet Listing, Durham kT = 8.900 GeV --- no mult p_x p_y p_z e m 0 14 -2.648 -33.789 23.003 45.149 18.988 1 19 2.644 35.485 -24.314 43.880 8.250 -------- End PYTHIA ClusterJet Listing ----------------------- -------- PYTHIA Sphericity Listing -------- no lambda e_x e_y e_z 1 0.98689 0.04610 0.95166 -0.30367 2 0.00797 -0.60161 -0.21623 -0.76897 3 0.00514 0.79746 -0.21815 -0.56256 -------- End PYTHIA Sphericity Listing ---- -------- PYTHIA Sphericity Listing -------- Nonstandard momentum power = 1.000 no lambda e_x e_y e_z 1 0.93790 0.01419 0.95978 -0.28038 2 0.03743 -0.92334 -0.09503 -0.37203 3 0.02467 0.38371 -0.26417 -0.88486 -------- End PYTHIA Sphericity Listing ---- -------- PYTHIA Thrust Listing ------------ value e_x e_y e_z Thr 0.96280 0.00057 -0.96019 0.27933 Maj 0.11698 -0.99948 0.00848 0.03118 Min 0.10110 -0.03231 -0.27921 -0.95969 -------- End PYTHIA Thrust Listing -------- -------- PYTHIA ClusterJet Listing, Lund pT = 9.119 GeV --- no mult p_x p_y p_z e m 0 20 -0.096 41.836 -12.218 45.689 13.710 1 17 0.096 -41.836 12.218 45.499 13.062 -------- End PYTHIA ClusterJet Listing ----------------------- -------- PYTHIA ClusterJet Listing, JADE m = 9.119 GeV --- no mult p_x p_y p_z e m 0 17 1.052 38.268 -13.295 41.295 7.932 1 10 -2.608 -38.540 9.260 39.878 3.519 2 10 1.557 0.271 4.035 10.015 9.029 -------- End PYTHIA ClusterJet Listing ----------------------- -------- PYTHIA ClusterJet Listing, Durham kT = 9.119 GeV --- no mult p_x p_y p_z e m 0 20 -0.096 41.836 -12.218 45.689 13.710 1 17 0.096 -41.836 12.218 45.499 13.062 -------- End PYTHIA ClusterJet Listing ----------------------- -------- PYTHIA Sphericity Listing -------- no lambda e_x e_y e_z 1 0.99048 -0.13619 0.87594 -0.46279 2 0.00805 -0.17813 -0.48118 -0.85833 3 0.00146 0.97454 0.03446 -0.22157 -------- End PYTHIA Sphericity Listing ---- -------- PYTHIA Sphericity Listing -------- Nonstandard momentum power = 1.000 no lambda e_x e_y e_z 1 0.94946 -0.14752 0.87183 -0.46706 2 0.04051 -0.14698 -0.48631 -0.86134 3 0.01003 0.97808 0.05842 -0.19989 -------- End PYTHIA Sphericity Listing ---- -------- PYTHIA Thrust Listing ------------ value e_x e_y e_z Thr 0.97063 -0.15123 0.86516 -0.47815 Maj 0.11091 0.30667 0.50091 0.80935 Min 0.06005 0.93972 -0.02424 -0.34107 -------- End PYTHIA Thrust Listing -------- -------- PYTHIA ClusterJet Listing, Lund pT = 9.119 GeV --- no mult p_x p_y p_z e m 0 28 -6.653 38.061 -21.035 46.804 15.978 1 9 6.653 -38.061 21.035 44.383 5.876 -------- End PYTHIA ClusterJet Listing ----------------------- -------- PYTHIA ClusterJet Listing, JADE m = 9.119 GeV --- no mult p_x p_y p_z e m 0 8 6.563 -38.126 20.673 43.979 3.189 1 22 -5.048 35.837 -16.144 40.160 6.511 2 7 -1.515 2.289 -4.529 7.049 4.652 -------- End PYTHIA ClusterJet Listing ----------------------- -------- PYTHIA ClusterJet Listing, Durham kT = 9.119 GeV --- no mult p_x p_y p_z e m 0 28 -6.653 38.061 -21.035 46.804 15.978 1 9 6.653 -38.061 21.035 44.383 5.876 -------- End PYTHIA ClusterJet Listing ----------------------- Pythia::next(): 1000 events have been generated Pythia::next(): 2000 events have been generated PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again Pythia::next(): 3000 events have been generated Pythia::next(): 4000 events have been generated Pythia::next(): 5000 events have been generated Pythia::next(): 6000 events have been generated Pythia::next(): 7000 events have been generated Pythia::next(): 8000 events have been generated Pythia::next(): 9000 events have been generated *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | f fbar -> gamma*/Z0 221 | 10505 10000 10000 | 4.143e-05 0.000e+00 | | | | | | sum | 10505 10000 10000 | 4.143e-05 0.000e+00 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Error in Pythia::next: hadronLevel failed; try again | | 1 Error in StringFragmentation::fragment: stuck in joining | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:02 charged multiplicity 1.30*10^ 3 1 3 1.25*10^ 3 X 6 X 1.20*10^ 3 X X X 1.15*10^ 3 X X X 6 1.10*10^ 3 X X X X 1.05*10^ 3 X X X X 1.00*10^ 3 3 X X X X 0.95*10^ 3 X X X X X 6 0.90*10^ 3 X X X X X X 0.85*10^ 3 X X X X X X 0.80*10^ 3 X X X X X X 1 0.75*10^ 3 X X X X X X X 0.70*10^ 3 X X X X X X X 0.65*10^ 3 1 X X X X X X X 0.60*10^ 3 X X X X X X X X 0.55*10^ 3 X X X X X X X X 0.50*10^ 3 X X X X X X X X 7 0.45*10^ 3 X X X X X X X X X 0.40*10^ 3 X X X X X X X X X 7 0.35*10^ 3 X X X X X X X X X X 0.30*10^ 3 7 X X X X X X X X X X 0.25*10^ 3 X X X X X X X X X X X 5 0.20*10^ 3 X X X X X X X X X X X X 1 0.15*10^ 3 X X X X X X X X X X X X X 0.10*10^ 3 6 X X X X X X X X X X X X X X 0.05*10^ 3 5 X X X X X X X X X X X X X X X X 8 4 3 1 1 Contents *10^ 3 0000000000000000101010100000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0000000000206090202020109070403020101000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000002070800060503060202050808020500050301010000000000000000000000000000000000000000000000000000000 *10^ 0 0000107080603060602040909040307040300020808030403000000000000000000000000000000000000000000000000000 Low edge - *10^ 1 0000000000011111111112222222222333333333344444444445555555555666666666677777777778888888888999999999 *10^ 0 0012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789012345678 *10^-1 5555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555 Entries = 10000 Mean = 2.0496e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+04 Rms = 6.3135e+00 Overflow = 0.0000e+00 High edge = 9.9500e+01 2013-09-20 16:02 Sphericity 2.00*10^ 3 8 1.92*10^ 3 X 1.84*10^ 3 X 1.76*10^ 3 X 1.68*10^ 3 XX 1.60*10^ 3 XX 1.52*10^ 3 XX 1.44*10^ 3 XX 1.36*10^ 3 XX 1.28*10^ 3 XX8 1.20*10^ 3 XXX 1.12*10^ 3 XXX 1.04*10^ 3 XXX 0.96*10^ 3 XXX 0.88*10^ 3 XXX9 0.80*10^ 3 XXXX 0.72*10^ 3 XXXX 0.64*10^ 3 XXXX4 0.56*10^ 3 XXXXX 0.48*10^ 3 XXXXX8 0.40*10^ 3 XXXXXX6 0.32*10^ 3 XXXXXXX91 0.24*10^ 3 XXXXXXXXX71 0.16*10^ 3 XXXXXXXXXXXXX42 1 0.08*10^ 3 XXXXXXXXXXXXXXXX9XX778686655453433323231122221112 11111111111111 11 Contents *10^ 3 1110000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 6928543322111100000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 7866966151655198788556564433332322212121111111011000000001000000000000000000000000000000000000000000 *10^ 0 7059185106967053440874008986473084332812059550904299957780497785332333742010000010000000000000000000 Low edge *10^-1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-2 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 10000 Mean = 7.1445e-02 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+04 Rms = 1.0470e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:02 Linearity 7.25*10^ 2 9 7.00*10^ 2 X6 6.75*10^ 2 8XX 6.50*10^ 2 XXXX 6.25*10^ 2 XXXX 6.00*10^ 2 XXXXX 5.75*10^ 2 XXXXX 5.50*10^ 2 XXXXX 5.25*10^ 2 XXXXX 5.00*10^ 2 6XXXXX 4.75*10^ 2 XXXXXX4 4.50*10^ 2 XXXXXXX4 4.25*10^ 2 XXXXXXXX5 4.00*10^ 2 XXXXXXXXX 3.75*10^ 2 XXXXXXXXX6 3.50*10^ 2 XXXXXXXXXX5 3.25*10^ 2 XXXXXXXXXXX 3.00*10^ 2 XXXXXXXXXXX1 2.75*10^ 2 XXXXXXXXXXXX 2.50*10^ 2 XXXXXXXXXXXX771 2.25*10^ 2 XXXXXXXXXXXXXXX 2.00*10^ 2 9XXXXXXXXXXXXXXXX74 1.75*10^ 2 XXXXXXXXXXXXXXXXXXX6 1.50*10^ 2 XXXXXXXXXXXXXXXXXXXX667 1.25*10^ 2 XXXXXXXXXXXXXXXXXXXXXXX 2 1.00*10^ 2 XXXXXXXXXXXXXXXXXXXXXXX8X4442 12 0.75*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5561 3 0.50*10^ 2 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7XX53485 1 0.25*10^ 2 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7576988654665333522432221212 Contents *10^ 2 0014676664443322221111111010000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0399729405316374429986434908888778666545533343222221111212111111000100000000000000000000000000000000 *10^ 0 4481121919426772379256192544561571226237183558664578374290431642877365986552534111001000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^-1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-2 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 10000 Mean = 1.5704e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+04 Rms = 1.3255e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:02 thrust 8.40*10^ 2 15 8.10*10^ 2 XX 7.80*10^ 2 XX 7.50*10^ 2 6XX6 7.20*10^ 2 XXXX 6.90*10^ 2 XXXX 6.60*10^ 2 1XXXX 6.30*10^ 2 XXXXX 6.00*10^ 2 XXXXX 5.70*10^ 2 XXXXX 5.40*10^ 2 XXXXX 5.10*10^ 2 47XXXXX 4.80*10^ 2 XXXXXXX3 4.50*10^ 2 XXXXXXXX 4.20*10^ 2 7XXXXXXXX 3.90*10^ 2 7XXXXXXXXX 3.60*10^ 2 XXXXXXXXXX 3.30*10^ 2 XXXXXXXXXX 3.00*10^ 2 9XXXXXXXXXXX 2.70*10^ 2 6XXXXXXXXXXXX 2.40*10^ 2 17XXXXXXXXXXXXX 2.10*10^ 2 3 8XXXXXXXXXXXXXXX 1.80*10^ 2 X2XXXXXXXXXXXXXXXX 1.50*10^ 2 267XXXXXXXXXXXXXXXXXX4 1.20*10^ 2 3 8 XXXXXXXXXXXXXXXXXXXXXX 0.90*10^ 2 11 2 6664XXX7XXXXXXXXXXXXXXXXXXXXXX 0.60*10^ 2 11 43332XX6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.30*10^ 2 1 111122311241224337446554875694XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 Contents *10^ 2 0000000000000000000000000000000000000000000000000000000000000000000000000001011111222223344567887410 *10^ 1 0000000000000000000000000000000010001000101211111122112133343343664667777981823485013590819033123531 *10^ 0 0000000000000000000000102123345504461467390033744251586333018906329708993995267186541881001029468810 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^-1 5555555555555555555566666666666666666666777777777777777777778888888888888888888899999999999999999999 *10^-2 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^-3 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 10000 Mean = 9.3244e-01 Underflow = 0.0000e+00 Low edge = 5.0000e-01 All chan = 1.0000e+04 Rms = 5.9866e-02 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:02 oblateness 1.30*10^ 3 22 1.25*10^ 3 XX 1.20*10^ 3 XX 1.15*10^ 3 XX 1.10*10^ 3 XX4 1.05*10^ 3 XXX 1.00*10^ 3 XXX 0.95*10^ 3 XXX 0.90*10^ 3 XXX 0.85*10^ 3 XXXX 0.80*10^ 3 XXXX 0.75*10^ 3 XXXX 0.70*10^ 3 XXXX 0.65*10^ 3 9XXXX 0.60*10^ 3 XXXXX7 0.55*10^ 3 XXXXXX8 0.50*10^ 3 XXXXXXX5 0.45*10^ 3 XXXXXXXX 0.40*10^ 3 XXXXXXXX 0.35*10^ 3 XXXXXXXX86 0.30*10^ 3 XXXXXXXXXX1 0.25*10^ 3 XXXXXXXXXXX77 0.20*10^ 3 XXXXXXXXXXXXXXX2 0.15*10^ 3 XXXXXXXXXXXXXXXX8521 0.10*10^ 3 XXXXXXXXXXXXXXXXXXXX836414 0.05*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXX8X98636345222331111 11 Contents *10^ 3 0111000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 6220855433222121111100000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 4556584742533906320086765753544313122111110000000000000000000000000000000000000000000000000000000000 *10^ 0 4998171729575912838786997029131142613110534353144101000000000000000000000000000000000000000000000000 Low edge *10^-1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-2 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 10000 Mean = 7.8683e-02 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+04 Rms = 7.9085e-02 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:02 cos(theta_Sphericity) 1.52*10^ 2 X 1.48*10^ 2 X 5 1.44*10^ 2 2X X X 1.40*10^ 2 XX X X 1.36*10^ 2 XX 5 X 7 2 X X 1.32*10^ 2 XX5X7X X X 7X XX 1.28*10^ 2 XXXXXXXX XX XX2XXX57 1.24*10^ 2 XXXXXXXX X XX 3 58 XXXXXXXX 1.20*10^ 2 XXXXXXXX X XX X X5XX5X XXXXXXXX 1.16*10^ 2 XXXXXXXX58X8XX X X XXXXXX XXXXXXXX 1.12*10^ 2 XXXXXXXXXXXXXX5 5 3 X X XXXXXX XXXXXXXX 1.08*10^ 2 XXXXXXXXXXXXXXX5X3XX X X X3 X8 XXXXXXXXXXXXXXX 1.04*10^ 2 XXXXXXXXXXXXXXXXXXXX X X XX XX 8XXXXXXXXXXXXXXX 1.00*10^ 2 XXXXXXXXXXXXXXXXXXXX 3 X X X3 8 X X XX XX XXXXXXXXXXXXXXXX 0.96*10^ 2 XXXXXXXXXXXXXXXXXXXX8X X X 353XX X 8 XX3 X 5XX 3XX XXXXXXXXXXXXXXXX 0.92*10^ 2 XXXXXXXXXXXXXXXXXXXXXX8X X XXXXX 5X X 3 X 5X 3 3XXX X 8 XXX XXX3XXXXXXXXXXXXXXXX 0.88*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXX3X5XXXXX83 XX X X X X XX XX XXXX X X XXX5XXXXXXXXXXXXXXXXXXXX 0.84*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 5 3X X X X X XX XX8XXXX X X XXXXXXXXXXXXXXXXXXXXXXXX 0.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8XX8 X8XX X 5 X X 3X XX XXXXXXX8X3X5XXXXXXXXXXXXXXXXXXXXXXXX 0.76*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5XXXX X3 3X XXX 3XXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.72*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX8 XX XXX8 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.68*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX3XXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.64*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3XXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.60*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.56*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 2 1111111111111111111100010100001000000000000000000000000000000000000010001000011001101111111111111111 *10^ 1 4533332311213210100099908189990988799778789687767768787567797997888809970797900892080212212034223422 *10^ 0 1204168545453806058957105663430775902942919143153889681693756022893906398718485631793082380816582467 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-2 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 10000 Mean = -6.5860e-03 Underflow = 0.0000e+00 Low edge = -1.0000e+00 All chan = 1.0000e+04 Rms = 6.2599e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:02 cos(theta_Linearity) 15.00*10^ 1 3 14.70*10^ 1 X 14.40*10^ 1 7 X 3 X 14.10*10^ 1 X7 X3 X X 13.80*10^ 1 XX3 XX X 3X 3 13.50*10^ 1 XXX XX 3 X XX X 13.20*10^ 1 XXXXXX X X X XX X 12.90*10^ 1 XXXXXXXX 73 X X X XX X 12.60*10^ 1 XXXXXXXX XX X X X XXXX 12.30*10^ 1 XXXXXXXX XX X X7X XXXX 12.00*10^ 1 XXXXXXXX XX XXXXX XXXX 11.70*10^ 1 XXXXXXXXX3 XX 3 3 3 3XX XXXXX7XXXX 11.40*10^ 1 XXXXXXXXXX XX7XXX X 3XXXX XXXXXXXXXX 11.10*10^ 1 XXXXXXXXXX7XXXXXX X XXXXX XXXXXXXXXX 10.80*10^ 1 XXXXXXXXXXXXXXXXX 3 X 7 XXXXX XXXXXXXXXX 10.50*10^ 1 XXXXXXXXXXXXXXXXX77X X X 7 XXXXX XXXXXXXXXX 10.20*10^ 1 XXXXXXXXXXXXXXXXXXXX 7 X X X 3X X3X XXXXXXXXXXXXXXXX 9.90*10^ 1 XXXXXXXXXXXXXXXXXXXX X X3 X X XXX3XXX XXXXXXXXXXXXXXXX 9.60*10^ 1 XXXXXXXXXXXXXXXXXXXX X7XX 3 X X 3 XXXXXXXX XXXXXXXXXXXXXXXX 9.30*10^ 1 XXXXXXXXXXXXXXXXXXXX XXXXX X7 3 X X X 3X X XXXXXXXXXXXXXXXXXXXXXXXXX 9.00*10^ 1 XXXXXXXXXXXXXXXXXXXX XXXXX3XX7X X 7X 73X 3X 7X 7XXX X 3X XXXXXXXXXXXXXXXXXXXXXXXXX 8.70*10^ 1 XXXXXXXXXXXXXXXXXXXX XXXXXXXXXX X3 7 XX XXX XX 3XX3XXXX7X XXXXXXXXXXXXXXXXXXXXXXXXXXXX 8.40*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX37X3 XX XXX XX XXXXXXXXXX7XXXXXXXXXXXXXXXXXXXXXXXXXXXX 8.10*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX XXX XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 7.80*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 3 XXX3 X XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 7.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 377X XXXX X XX3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 7.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3XXX XXXX XXXXX X 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 6.90*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7XXXX XXXXX X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 6.60*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3XXXXX X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 6.30*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 6.00*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 2 1111111111111111111100101000000010000000000000000000000000000001000000000000011011101111111111111111 *10^ 1 4433432311122111100089091989989808888877789677776788975767897880889998988989900900091111103242213423 *10^ 0 3062899375087354544643155784291475236220290834464298368820803594591306038476902720232457722022966466 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-2 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 10000 Mean = -6.6080e-03 Underflow = 0.0000e+00 Low edge = -1.0000e+00 All chan = 1.0000e+04 Rms = 6.2579e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:02 cos(theta_Thrust) 1.56*10^ 2 7 1.52*10^ 2 7 X 1.48*10^ 2 X X 1.44*10^ 2 2 X X 1.40*10^ 2 X2 5 X XX 1.36*10^ 2 XX2 7 X X XX27 1.32*10^ 2 XXX5X X 57 5 5X XXXX 1.28*10^ 2 XXXXX2 X XX X5XXX5XXXX 1.24*10^ 2 XXXXXX X3 X 8X 3 8 XX XXXXXXXXXX 1.20*10^ 2 XXXXXX8 XX X XX X X XX XXXXXXXXXX 1.16*10^ 2 XXXXXXXXXX5X XX X3X XX XXXXXXXXXX 1.12*10^ 2 XXXXXXXXXXXX XX 3 33XXX XX XXXXXXXXXX 1.08*10^ 2 XXXXXXXXXXXX XX X X 5 3 XXXXX 5XX XXXXXXXXXX 1.04*10^ 2 XXXXXXXXXXXX XX 3 X X X 3 3 X 8 X XXXXX3XXX XXXXXXXXXX 1.00*10^ 2 XXXXXXXXXXXX XX X X 5X X X X X X 8 X 8X X XXXXXXXXXXXXXXXXXXXX 0.96*10^ 2 XXXXXXXXXXXX XXXX5X8 X8 XX X X X 5 X X X X 8XX8X5XXXXXXXXXXXXXXXXXXXX 0.92*10^ 2 XXXXXXXXXXXX3XXXXXXX XX XX8 X5 X5 X8 X 3 3 X 5X X X8 X8XXXXXXXXXXXXXXXXXXXXXXXXXX 0.88*10^ 2 XXXXXXXXXXXXXXXXXXXXXXX XXX XX3 XX XX X X XX 5X 3XX 8X XX5XXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.84*10^ 2 XXXXXXXXXXXXXXXXXXXXXXX XXX XXX XX5XX X 3 X XX 8 XX XXX XXX8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXXX3XXX XXX XXXXX X 5X X 853XX3 X X XX XXX8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.76*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXX XXX XXXXX X XX X XXXXXX X X XX8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.72*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXX XXX5XXXXX XXXX X XXXXXX X X8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.68*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXX38XXXX3X XXXXXX X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.64*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXX8XXXXXXXXXXXXXXXXX58XXXXXX8X8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 2 1111111111110110100001000100100010010000000000000000000000000001000100001000101011111111111111111111 *10^ 1 4333321122138229099980979096098709809669778686677788768687897890788089980999090900212003303235225433 *10^ 0 1730559641489346146584578813005000291572281592398789733301645501947139166159355499133160100601865035 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-2 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 10000 Mean = 1.5196e-02 Underflow = 0.0000e+00 Low edge = -1.0000e+00 All chan = 1.0000e+04 Rms = 6.2560e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:02 Lund jet multiplicity 8.10*10^ 3 4 7.80*10^ 3 X 7.50*10^ 3 X 7.20*10^ 3 X 6.90*10^ 3 X 6.60*10^ 3 X 6.30*10^ 3 X 6.00*10^ 3 X 5.70*10^ 3 X 5.40*10^ 3 X 5.10*10^ 3 X 4.80*10^ 3 X 4.50*10^ 3 X 4.20*10^ 3 X 3.90*10^ 3 X 3.60*10^ 3 X 3.30*10^ 3 X 3.00*10^ 3 X 2.70*10^ 3 X 2.40*10^ 3 X 2.10*10^ 3 X8 1.80*10^ 3 XX 1.50*10^ 3 XX 1.20*10^ 3 XX 0.90*10^ 3 XX 0.60*10^ 3 XX 0.30*10^ 3 XX2 Contents *10^ 3 0072000000000000000000000000000000000000 *10^ 2 0090000000000000000000000000000000000000 *10^ 1 0002600000000000000000000000000000000000 *10^ 0 0087500000000000000000000000000000000000 Low edge - *10^ 1 0000000000011111111112222222222333333333 *10^ 0 0012345678901234567890123456789012345678 *10^-1 5555555555555555555555555555555555555555 Entries = 10000 Mean = 2.2157e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+04 Rms = 4.2682e-01 Overflow = 0.0000e+00 High edge = 3.9500e+01 2013-09-20 16:02 Jade jet multiplicity 5.20*10^ 3 6 5.00*10^ 3 X 4.80*10^ 3 X 4.60*10^ 3 X 4.40*10^ 3 X 4.20*10^ 3 X 4.00*10^ 3 X 3.80*10^ 3 X 3.60*10^ 3 X 3.40*10^ 3 X 3.20*10^ 3 X 3.00*10^ 3 X 2.80*10^ 3 2X 2.60*10^ 3 XX 2.40*10^ 3 XX 2.20*10^ 3 XX 2.00*10^ 3 XX7 1.80*10^ 3 XXX 1.60*10^ 3 XXX 1.40*10^ 3 XXX 1.20*10^ 3 XXX 1.00*10^ 3 XXX 0.80*10^ 3 XXX 0.60*10^ 3 XXX 0.40*10^ 3 XXX4 0.20*10^ 3 XXXX1 Contents *10^ 3 0025100000000000000000000000000000000000 *10^ 2 0061920000000000000000000000000000000000 *10^ 1 0032471000000000000000000000000000000000 *10^ 0 0084674100000000000000000000000000000000 Low edge - *10^ 1 0000000000011111111112222222222333333333 *10^ 0 0012345678901234567890123456789012345678 *10^-1 5555555555555555555555555555555555555555 Entries = 10000 Mean = 2.9908e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+04 Rms = 7.6375e-01 Overflow = 0.0000e+00 High edge = 3.9500e+01 2013-09-20 16:02 Durham jet multiplicity 6.50*10^ 3 5 6.25*10^ 3 X 6.00*10^ 3 X 5.75*10^ 3 X 5.50*10^ 3 X 5.25*10^ 3 X 5.00*10^ 3 X 4.75*10^ 3 X 4.50*10^ 3 X 4.25*10^ 3 X 4.00*10^ 3 X 3.75*10^ 3 X 3.50*10^ 3 X 3.25*10^ 3 X5 3.00*10^ 3 XX 2.75*10^ 3 XX 2.50*10^ 3 XX 2.25*10^ 3 XX 2.00*10^ 3 XX 1.75*10^ 3 XX 1.50*10^ 3 XX 1.25*10^ 3 XX 1.00*10^ 3 XX 0.75*10^ 3 XX 0.50*10^ 3 XX8 0.25*10^ 3 XXX1 Contents *10^ 3 0063000000000000000000000000000000000000 *10^ 2 0031400000000000000000000000000000000000 *10^ 1 0073630000000000000000000000000000000000 *10^ 0 0033121000000000000000000000000000000000 Low edge - *10^ 1 0000000000011111111112222222222333333333 *10^ 0 0012345678901234567890123456789012345678 *10^-1 5555555555555555555555555555555555555555 Entries = 10000 Mean = 2.4155e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+04 Rms = 5.9620e-01 Overflow = 0.0000e+00 High edge = 3.9500e+01 2013-09-20 16:02 Lund e_i - e_{i+1} 1.30*10^ 3 5 1.25*10^ 3 X4 1.20*10^ 3 XX 1.15*10^ 3 XX 1.10*10^ 3 XX 1.05*10^ 3 XX3 1.00*10^ 3 XXX 0.95*10^ 3 XXX 0.90*10^ 3 XXX4 0.85*10^ 3 XXXX 0.80*10^ 3 XXXX 0.75*10^ 3 XXXX5 0.70*10^ 3 XXXXX 0.65*10^ 3 XXXXX4 0.60*10^ 3 XXXXXX1 0.55*10^ 3 XXXXXXX2 0.50*10^ 3 XXXXXXXX 0.45*10^ 3 XXXXXXXX4 0.40*10^ 3 XXXXXXXXX9 0.35*10^ 3 XXXXXXXXXX4 0.30*10^ 3 XXXXXXXXXXX54 0.25*10^ 3 XXXXXXXXXXXXXX21 0.20*10^ 3 XXXXXXXXXXXXXXXX752 0.15*10^ 3 XXXXXXXXXXXXXXXXXXXX85936113 0.10*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXX5555625 2 2 0.05*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX888787676656454353233111 Contents *10^ 3 0000000000111000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0000000000220876554332222211111111111100000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000721622511927650087553241300177778575556544333333332222112111100000000000000000000000000000 *10^ 0 0000000000325940328715818753918736044774660961900021968415107804875524476500000000000000000000000000 Low edge ---------- *10^ 1 0000000000000000000000000000001111111111111111111122222222222222222222333333333333333333334444444444 *10^ 0 5443322110001122334455667788990011223344556677889900112233445566778899001122334455667788990011223344 *10^-1 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 12157 Mean = 5.7359e+00 Underflow = 0.0000e+00 Low edge = -5.0000e+00 All chan = 1.2157e+04 Rms = 6.2913e+00 Overflow = 0.0000e+00 High edge = 4.5000e+01 2013-09-20 16:02 Jade e_i - e_{i+1} 1.50*10^ 3 1 1.45*10^ 3 X 1.40*10^ 3 X 1.35*10^ 3 X 1.30*10^ 3 X 1.25*10^ 3 X4 1.20*10^ 3 XX 1.15*10^ 3 XX 1.10*10^ 3 XX2 1.05*10^ 3 XXX 1.00*10^ 3 XXX 0.95*10^ 3 XXX 0.90*10^ 3 XXX7 0.85*10^ 3 XXXX 0.80*10^ 3 XXXX 0.75*10^ 3 XXXX8 0.70*10^ 3 XXXXX 0.65*10^ 3 XXXXX3 0.60*10^ 3 XXXXXX 0.55*10^ 3 XXXXXX81 0.50*10^ 3 XXXXXXXX3 0.45*10^ 3 XXXXXXXXXX 0.40*10^ 3 XXXXXXXXXXX865 3 0.35*10^ 3 XXXXXXXXXXXXXX76X 2 1 0.30*10^ 3 XXXXXXXXXXXXXXXXXXX8X215 0.25*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXX8X8 13 0.20*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXX7XX792X62 2 0.15*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7X753 2 1 4 2 1 2 2 1 113 0.10*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX988XX6X97X8846X7X887X7787X75X9978X8XXX767552 0.05*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX72 Contents *10^ 3 0000000000111000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0000000000420876554433333333323222222212211121111111000110000100001010001000010010000101110000000000 *10^ 1 0000000000525841406599873260190557545480189507635321989017998089782818880888808709989080018887753000 *10^ 0 0000000000409716155192056940105974122154665909039444390018933492221329974748693486550684346174584810 Low edge ---------- *10^ 1 0000000000000000000000000000001111111111111111111122222222222222222222333333333333333333334444444444 *10^ 0 5443322110001122334455667788990011223344556677889900112233445566778899001122334455667788990011223344 *10^-1 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 19908 Mean = 1.1849e+01 Underflow = 0.0000e+00 Low edge = -5.0000e+00 All chan = 1.9908e+04 Rms = 1.1773e+01 Overflow = 0.0000e+00 High edge = 4.5000e+01 2013-09-20 16:02 Durham e_i - e_{i+1} 1.56*10^ 3 5 1.50*10^ 3 X 1.44*10^ 3 X 1.38*10^ 3 X6 1.32*10^ 3 XX 1.26*10^ 3 XX 1.20*10^ 3 XX 1.14*10^ 3 XX1 1.08*10^ 3 XXX 1.02*10^ 3 XXX 0.96*10^ 3 XXX 0.90*10^ 3 XXX8 0.84*10^ 3 XXXX 0.78*10^ 3 XXXX2 0.72*10^ 3 XXXXX 0.66*10^ 3 XXXXX 0.60*10^ 3 XXXXX6 0.54*10^ 3 XXXXXX7 0.48*10^ 3 XXXXXXX 0.42*10^ 3 XXXXXXX850 0.36*10^ 3 XXXXXXXXXX 0.30*10^ 3 XXXXXXXXXX992 0.24*10^ 3 XXXXXXXXXXXXX6755224 1 0.18*10^ 3 XXXXXXXXXXXXXXXXXXXX39X4X3522 3412 0.12*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX8XXXXX9X79564 2 111 0.06*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9XXX887XX776676966653553222 Contents *10^ 3 0000000000111000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0000000000530875543322222221121111111111111111111000000000000000000000000000000000000000000000000000 *10^ 1 0000000000358827218699412019903774834331342311101898565666444554433435333212211110000000000000000000 *10^ 0 0000000000097598408362984713516282688500714093906985993645871793248061535857884401000000000000000000 Low edge ---------- *10^ 1 0000000000000000000000000000001111111111111111111122222222222222222222333333333333333333334444444444 *10^ 0 5443322110001122334455667788990011223344556677889900112233445566778899001122334455667788990011223344 *10^-1 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 14155 Mean = 7.3911e+00 Underflow = 0.0000e+00 Low edge = -5.0000e+00 All chan = 1.4155e+04 Rms = 8.0035e+00 Overflow = 0.0000e+00 High edge = 4.5000e+01 pythia8-8.1.80.orig/examples/outref/out050000644000175000017500000023231212217346170016360 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:01:28 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> g g 111 | 1.522e-04 | | g g -> q qbar (uds) 112 | 2.736e-06 | | q g -> q g 113 | 3.573e-04 | | q q(bar)' -> q q(bar)' 114 | 6.125e-05 | | q qbar -> g g 115 | 4.929e-07 | | q qbar -> q' qbar' (uds) 116 | 2.760e-07 | | g g -> c cbar 121 | 9.119e-07 | | q qbar -> c cbar 122 | 9.199e-08 | | g g -> b bbar 123 | 9.109e-07 | | q qbar -> b bbar 124 | 9.193e-08 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 57.54 mb | | | | pT0 = 3.08 gives sigmaInteraction = 271.14 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | HardQCD:all | on | off | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberShowEvent | 0 | 1 0 | | Next:numberShowInfo | 0 | 1 0 | | Next:numberShowProcess | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:pTHatMin | 200.00000 | 0.0 0.0 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- #-------------------------------------------------------------------------- # FastJet release 3.0.5 [fjcore] # M. Cacciari, G.P. Salam and G. Soyez # A software package for jet finding and analysis at colliders # http://fastjet.fr # # Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package # for scientific work and optionally PLB641(2006)57 [hep-ph/0512210]. # # FastJet is provided without warranty under the terms of the GNU GPLv2. # It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code # and 3rd party plugin jet algorithms. See COPYING file for details. #-------------------------------------------------------------------------- -- PYTHIA SlowJet(fjcore) Listing, p = -1, R = 0.700, pTjetMin = 10.000, etaMax = 4.000 -- no pTjet y phi mult p_x p_y p_z e m 0 227.513 -0.934 0.775 44 162.570 159.164 -247.397 337.716 32.932 1 223.408 0.523 -2.340 35 -155.470 -160.438 123.076 256.484 26.926 2 24.202 2.045 -2.192 38 -14.084 -19.682 100.043 103.452 10.387 3 15.149 -3.524 -1.998 20 -6.282 -13.785 -278.618 279.103 6.384 4 13.849 -2.459 1.156 24 5.576 12.677 -90.094 91.423 7.022 -------- End PYTHIA SlowJet Listing -------------------------------------------------------- -------- PYTHIA CellJet Listing, eTjetMin = 10.000, coneRadius = 0.700 ------------------------------ no eTjet etaCtr phiCtr etaWt phiWt mult p_x p_y p_z e m 0 227.680 -0.850 0.834 -0.928 0.792 44 159.251 161.309 -244.251 334.859 33.026 1 223.759 0.550 -2.307 0.543 -2.328 34 -153.272 -162.056 128.190 258.628 26.479 2 23.067 2.350 -2.405 2.254 -2.291 30 -14.754 -16.853 113.101 115.616 8.573 3 14.613 -3.650 -1.914 -3.551 -1.960 18 -5.452 -13.281 -263.138 263.574 4.838 4 11.827 -2.550 1.424 -2.556 1.255 20 3.538 10.847 -78.959 79.916 4.665 -------- End PYTHIA CellJet Listing ------------------------------------------------------------------- -- PYTHIA SlowJet(fjcore) Listing, p = -1, R = 0.700, pTjetMin = 10.000, etaMax = 4.000 -- no pTjet y phi mult p_x p_y p_z e m 0 237.720 -1.404 0.338 68 224.280 78.799 -471.539 532.122 65.527 1 215.422 -1.049 -2.725 62 -197.010 -87.141 -274.595 351.485 41.627 2 24.909 -1.847 -3.068 30 -24.841 -1.835 -81.548 85.705 8.647 3 18.165 -1.664 1.510 16 1.096 18.132 -48.839 52.471 6.163 4 15.624 2.764 1.466 17 1.627 15.539 129.560 130.594 4.976 5 11.743 0.436 -2.342 17 -8.183 -8.422 5.770 14.062 5.152 -------- End PYTHIA SlowJet Listing -------------------------------------------------------- -------- PYTHIA CellJet Listing, eTjetMin = 10.000, coneRadius = 0.700 ------------------------------ no eTjet etaCtr phiCtr etaWt phiWt mult p_x p_y p_z e m 0 240.790 -1.350 0.442 -1.407 0.345 67 221.081 79.715 -466.449 525.921 61.544 1 215.978 -1.050 -2.700 -1.035 -2.728 60 -196.412 -86.232 -268.464 345.872 39.256 2 26.107 -1.750 -2.994 -1.834 -3.031 31 -25.223 -2.766 -81.146 85.390 7.929 3 17.118 2.650 1.522 2.727 1.507 19 1.067 16.688 134.019 135.175 5.616 4 17.042 -1.650 1.620 -1.685 1.536 15 0.578 16.761 -45.299 48.523 4.612 5 11.719 -2.850 2.700 -2.744 2.760 17 -10.280 4.179 -93.127 93.901 4.643 6 10.256 0.550 -3.093 0.492 -2.939 15 -9.515 -1.956 5.351 11.771 3.946 -------- End PYTHIA CellJet Listing ------------------------------------------------------------------- -- PYTHIA SlowJet(fjcore) Listing, p = -1, R = 0.700, pTjetMin = 10.000, etaMax = 4.000 -- no pTjet y phi mult p_x p_y p_z e m 0 243.686 -0.516 2.992 59 -240.958 36.359 -133.217 280.865 41.894 1 197.697 1.118 -0.470 54 176.284 -89.488 272.443 337.663 26.595 2 99.553 -1.604 0.664 38 78.387 61.370 -243.033 263.528 21.714 3 13.074 -2.076 2.422 13 -9.834 8.615 -53.706 55.423 4.060 4 11.140 3.292 -2.024 10 -4.878 -10.015 160.984 161.430 4.411 -------- End PYTHIA SlowJet Listing -------------------------------------------------------- -------- PYTHIA CellJet Listing, eTjetMin = 10.000, coneRadius = 0.700 ------------------------------ no eTjet etaCtr phiCtr etaWt phiWt mult p_x p_y p_z e m 0 243.269 -0.450 2.994 -0.518 3.008 57 -239.611 32.256 -132.400 278.173 37.370 1 197.833 1.150 -0.442 1.131 -0.446 53 178.002 -85.005 275.891 339.998 23.907 2 100.919 -1.650 0.638 -1.606 0.678 38 77.430 62.318 -243.637 264.067 22.211 3 13.951 -2.050 2.503 -2.053 2.467 14 -10.652 8.554 -54.632 56.462 4.085 4 11.282 3.350 -2.013 3.300 -2.018 10 -4.811 -10.056 159.878 160.316 3.971 -------- End PYTHIA CellJet Listing ------------------------------------------------------------------- -- PYTHIA SlowJet(fjcore) Listing, p = -1, R = 0.700, pTjetMin = 10.000, etaMax = 4.000 -- no pTjet y phi mult p_x p_y p_z e m 0 236.430 0.441 -2.931 74 -231.207 -49.419 109.591 264.461 45.062 1 181.314 0.896 -0.263 81 175.100 -47.059 193.792 271.220 55.950 2 111.235 -1.098 1.594 39 -2.565 111.205 -150.230 187.836 18.442 3 103.965 1.777 -0.577 39 87.130 -56.720 313.892 332.387 33.828 4 48.053 -1.532 2.591 46 -40.957 25.133 -112.854 123.909 17.558 5 35.178 1.958 1.521 21 1.764 35.134 126.030 131.158 9.017 6 29.513 2.852 -0.120 14 29.302 -3.525 260.099 261.839 6.103 7 13.256 -2.164 -2.053 12 -6.146 -11.745 -59.122 60.705 3.727 8 11.585 -1.979 1.712 18 -1.632 11.470 -43.464 45.155 3.960 9 10.328 -3.389 -0.927 18 6.197 -8.262 -167.077 167.457 4.555 -------- End PYTHIA SlowJet Listing -------------------------------------------------------- -------- PYTHIA CellJet Listing, eTjetMin = 10.000, coneRadius = 0.700 ------------------------------ no eTjet etaCtr phiCtr etaWt phiWt mult p_x p_y p_z e m 0 237.919 0.450 -2.896 0.440 -2.945 71 -231.472 -46.077 108.922 263.376 42.432 1 150.041 0.750 -0.245 0.793 -0.209 52 144.669 -30.818 132.439 200.709 29.415 2 125.363 1.550 -0.638 1.574 -0.552 63 105.248 -64.797 298.967 325.774 38.360 3 111.520 -1.050 1.620 -1.081 1.603 38 -3.581 111.080 -146.715 184.878 17.402 4 48.529 -1.450 2.700 -1.532 2.593 41 -40.393 24.757 -110.272 121.091 16.082 5 37.844 2.850 -0.147 2.721 -0.212 20 36.584 -7.882 295.140 297.720 11.347 6 36.335 1.850 1.522 1.932 1.538 23 1.170 35.833 125.135 130.500 9.280 7 13.070 -2.150 -2.111 -2.156 -2.056 10 -6.044 -11.422 -56.371 57.908 2.956 8 12.505 -1.950 1.718 -1.955 1.708 20 -1.694 11.969 -44.174 45.976 4.042 9 10.723 -3.350 -0.834 -3.418 -0.917 18 6.329 -8.240 -169.745 170.109 3.988 -------- End PYTHIA CellJet Listing ------------------------------------------------------------------- -- PYTHIA SlowJet(fjcore) Listing, p = -1, R = 0.700, pTjetMin = 10.000, etaMax = 4.000 -- no pTjet y phi mult p_x p_y p_z e m 0 268.595 -1.409 0.611 63 219.973 154.127 -522.163 588.528 39.588 1 233.293 0.561 -2.528 50 -190.753 -134.309 139.311 273.770 33.418 2 15.891 -0.422 -2.646 17 -13.980 -7.555 -7.509 18.833 6.765 3 15.139 1.695 2.664 22 -13.449 6.952 44.692 47.808 7.686 4 14.469 -2.343 0.136 28 14.335 1.964 -82.689 84.227 6.885 5 13.647 -1.835 -2.349 21 -9.577 -9.722 -44.881 47.228 5.467 6 10.801 -3.690 -2.236 17 -6.665 -8.499 -230.415 230.703 3.996 -------- End PYTHIA SlowJet Listing -------------------------------------------------------- -------- PYTHIA CellJet Listing, eTjetMin = 10.000, coneRadius = 0.700 ------------------------------ no eTjet etaCtr phiCtr etaWt phiWt mult p_x p_y p_z e m 0 269.855 -1.450 0.540 -1.421 0.604 61 220.671 152.216 -528.324 593.691 38.436 1 233.792 0.550 -2.503 0.554 -2.520 50 -188.948 -135.443 136.773 271.646 32.225 2 14.709 -0.750 -2.602 -0.452 -2.678 17 -12.871 -6.428 -7.285 17.063 5.577 3 13.355 -2.050 -2.405 -1.885 -2.351 16 -9.143 -9.239 -43.692 45.753 3.920 4 12.124 -2.750 0.442 -2.538 0.295 24 11.312 3.428 -81.078 82.087 4.989 5 11.174 -3.650 -2.111 -3.705 -2.201 17 -6.312 -8.664 -229.989 230.268 3.659 6 10.831 2.250 2.111 2.214 2.179 14 -5.945 8.510 51.011 52.240 4.373 7 10.606 -0.950 -1.522 -0.940 -1.597 17 -0.241 -10.067 -11.715 15.928 3.880 -------- End PYTHIA CellJet Listing ------------------------------------------------------------------- PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> g g 111 | 992 156 156 | 2.452e-05 9.322e-07 | | g g -> q qbar (uds) 112 | 13 5 5 | 6.471e-07 2.027e-07 | | q g -> q g 113 | 2202 279 279 | 4.035e-05 1.385e-06 | | q q(bar)' -> q q(bar)' 114 | 385 56 56 | 8.929e-06 6.646e-07 | | q qbar -> g g 115 | 4 1 1 | 1.742e-07 1.742e-07 | | q qbar -> q' qbar' (uds) 116 | 0 0 0 | 0.000e+00 0.000e+00 | | g g -> c cbar 121 | 6 2 2 | 2.708e-07 9.573e-08 | | q qbar -> c cbar 122 | 0 0 0 | 0.000e+00 0.000e+00 | | g g -> b bbar 123 | 3 0 0 | 0.000e+00 0.000e+00 | | q qbar -> b bbar 124 | 2 1 1 | 4.301e-08 4.301e-08 | | | | | | sum | 3607 500 500 | 7.494e-05 1.819e-06 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 2 Error in Pythia::next: hadronLevel failed; try again | | 2 Error in StringFragmentation::fragment: stuck in joining | | 1 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:01 number of jets, SlowJet 1.04*10^ 2 5 1.00*10^ 2 X 0.96*10^ 2 X 0.92*10^ 2 X 0.88*10^ 2 X 0.84*10^ 2 X 0.80*10^ 2 X 0.76*10^ 2 X 0.72*10^ 2 X 0.68*10^ 2 X8 0.64*10^ 2 XXX5 0.60*10^ 2 XXXX 0.56*10^ 2 XXXX 0.52*10^ 2 XXXX 0.48*10^ 2 XXXX3 0.44*10^ 2 8XXXXX5 0.40*10^ 2 XXXXXXX 0.36*10^ 2 XXXXXXX 0.32*10^ 2 XXXXXXX 0.28*10^ 2 XXXXXXX 0.24*10^ 2 XXXXXXX 0.20*10^ 2 2XXXXXXX25 0.16*10^ 2 XXXXXXXXXX 0.12*10^ 2 XXXXXXXXXXX 0.08*10^ 2 XXXXXXXXXXXX 0.04*10^ 2 XXXXXXXXXXXX53 Contents *10^ 2 00000100000000000000000000000000000000000000000000 *10^ 1 00146066441110000000000000000000000000000000000000 *10^ 0 00734272527828210000000000000000000000000000000000 *10^-1 00000000000000000000000000000000000000000000000000 Low edge - *10^ 1 00000000000111111111122222222223333333333444444444 *10^ 0 00123456789012345678901234567890123456789012345678 *10^-1 55555555555555555555555555555555555555555555555555 Entries = 500 Mean = 6.3240e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 5.0000e+02 Rms = 2.5844e+00 Overflow = 0.0000e+00 High edge = 4.9500e+01 2013-09-20 16:01 number of jets, CellJet 8.40*10^ 1 X3 8.10*10^ 1 XX 7.80*10^ 1 XX 7.50*10^ 1 XX 7.20*10^ 1 XX 6.90*10^ 1 XX 6.60*10^ 1 XX 6.30*10^ 1 XX 6.00*10^ 1 XX 7 5.70*10^ 1 XX7X 5.40*10^ 1 3XXXX 5.10*10^ 1 XXXXX 4.80*10^ 1 XXXXX 4.50*10^ 1 XXXXX 4.20*10^ 1 XXXXX 3.90*10^ 1 XXXXXX 3.60*10^ 1 XXXXXX X 3.30*10^ 1 XXXXXX7X 3.00*10^ 1 XXXXXXXX 2.70*10^ 1 XXXXXXXX 2.40*10^ 1 XXXXXXXX 2.10*10^ 1 XXXXXXXX 1.80*10^ 1 XXXXXXXX 1.50*10^ 1 7XXXXXXXX 1.20*10^ 1 XXXXXXXXX7 X 0.90*10^ 1 XXXXXXXXXXXX3 0.60*10^ 1 XXXXXXXXXXXXX7 0.30*10^ 1 XXXXXXXXXXXXXX 7 Contents *10^ 1 00135885533101000000000000000000000000000000000000 *10^ 0 00492426926192750200000000000000000000000000000000 *10^-1 00000000000000000000000000000000000000000000000000 *10^-2 00000000000000000000000000000000000000000000000000 Low edge - *10^ 1 00000000000111111111122222222223333333333444444444 *10^ 0 00123456789012345678901234567890123456789012345678 *10^-1 55555555555555555555555555555555555555555555555555 Entries = 500 Mean = 6.7380e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 5.0000e+02 Rms = 2.8400e+00 Overflow = 0.0000e+00 High edge = 4.9500e+01 2013-09-20 16:01 number of jets, CellJet - SlowJet 2.70*10^ 2 2 2.60*10^ 2 X 2.50*10^ 2 X 2.40*10^ 2 X 2.30*10^ 2 X 2.20*10^ 2 X 2.10*10^ 2 X 2.00*10^ 2 X 1.90*10^ 2 X 1.80*10^ 2 X 1.70*10^ 2 X 1.60*10^ 2 X 1.50*10^ 2 X 1.40*10^ 2 X8 1.30*10^ 2 XX 1.20*10^ 2 XX 1.10*10^ 2 XX 1.00*10^ 2 XX 0.90*10^ 2 XX 0.80*10^ 2 XX 0.70*10^ 2 XX 0.60*10^ 2 XX 0.50*10^ 2 XX4 0.40*10^ 2 9XXX 0.30*10^ 2 XXXX 0.20*10^ 2 XXXX 0.10*10^ 2 16XXXX631 Contents *10^ 2 000000000000000000000021000000000000000000000 *10^ 1 000000000000000000000363400000000000000000000 *10^ 0 000000000000000000016928463100000000000000000 *10^-1 000000000000000000000000000000000000000000000 Low edge ----------------------- *10^ 1 222111111111100000000000000000000111111111122 *10^ 0 210987654321098765432100123456789012345678901 *10^-1 555555555555555555555555555555555555555555555 Entries = 500 Mean = 4.1400e-01 Underflow = 0.0000e+00 Low edge = -2.2500e+01 All chan = 5.0000e+02 Rms = 9.2445e-01 Overflow = 0.0000e+00 High edge = 2.2500e+01 2013-09-20 16:01 pT for jets, SlowJet 7.80*10^ 2 4 7.50*10^ 2 X 7.20*10^ 2 X 6.90*10^ 2 X 6.60*10^ 2 X 6.30*10^ 2 X 6.00*10^ 2 X 5.70*10^ 2 X 5.40*10^ 2 X 5.10*10^ 2 X 4.80*10^ 2 X 4.50*10^ 2 X 4.20*10^ 2 X 3.90*10^ 2 X 3.60*10^ 2 X1 3.30*10^ 2 XX 3.00*10^ 2 XX 2.70*10^ 2 XX 2.40*10^ 2 XX 2.10*10^ 2 XX8 1.80*10^ 2 XXX 1.50*10^ 2 XXX4 1.20*10^ 2 XXXX7 0.90*10^ 2 XXXXX341 0.60*10^ 2 XXXXXXXX18 1 265742133 0.30*10^ 2 XXXXXXXXXXX99X65653737646463757778X9XXXXXXXXXXXX96879666734535431132113111 1 1 11 11 1 1 Contents *10^ 2 0073211000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0063031676353223111112121111112122223223344543344221222111211101100000000000000000000000000000000000 *10^ 0 0012520933250862749600029283901612030791794027200987426797101595292297428232131121240122102010011012 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^ 1 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^ 0 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 3162 Mean = 9.8442e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 3.1490e+03 Rms = 1.0454e+02 Overflow = 1.3000e+01 High edge = 5.0000e+02 2013-09-20 16:01 eT for jets, CellJet 0.96*10^ 3 5 0.92*10^ 3 X 0.88*10^ 3 X 0.84*10^ 3 X 0.80*10^ 3 X 0.76*10^ 3 X 0.72*10^ 3 X 0.68*10^ 3 X 0.64*10^ 3 X 0.60*10^ 3 X 0.56*10^ 3 X 0.52*10^ 3 X 0.48*10^ 3 X 0.44*10^ 3 X 0.40*10^ 3 X 0.36*10^ 3 X3 0.32*10^ 3 XX 0.28*10^ 3 XX 0.24*10^ 3 XX5 0.20*10^ 3 XXX 0.16*10^ 3 XXX5 0.12*10^ 3 XXXX42 0.08*10^ 3 XXXXXX841 2122 0.04*10^ 3 XXXXXXXXXX88776454345553543354565688689XXXX898X9755657455334233311121 111 1 1 1 11 1 1 1 Contents *10^ 2 0093210000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0033249875443322212111111111111112123323344443333322221211111101110000000000000000000000000000000000 *10^ 0 0093025735210397450536999486438794920333584880439660129659942573024558315641313021340111202010020011 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^ 1 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^ 0 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 3369 Mean = 9.3154e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 3.3550e+03 Rms = 1.0305e+02 Overflow = 1.4000e+01 High edge = 5.0000e+02 2013-09-20 16:01 y for jets, SlowJet 7.25*10^ 1 4 4 7.00*10^ 1 2 2 X X 6.75*10^ 1 X 8 X 8 X X 8 6.50*10^ 1 X X 22X 6 X6 X X XX 6 6.25*10^ 1 X X XXX X XX X X XX X 6.00*10^ 1 X X XXX X XX X6X X 6XX X 5.75*10^ 1 X X 4XXX X XX XXX X XXX X 8 5.50*10^ 1 X 2XX XXXX X XX XXX X6XXX6 XX2 X 5.25*10^ 1 4 X XXX XXXX8 X XX4 XXX48XXXXXX8XXX X 4 5.00*10^ 1 X X XXX2XXXXX2XXXXX XXXXXXXXXXXXXXX6X X 4.75*10^ 1 X X XXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXX X 4.50*10^ 1 2 6 X X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 4.25*10^ 1 X X X X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4X 4 8 8 4.00*10^ 1 X X XX X6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X X 3.75*10^ 1 X X XX4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X X 3.50*10^ 1 X 2X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6X X 2X 3.25*10^ 1 X XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X XX 3.00*10^ 1 2 X XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 2 2.75*10^ 1 X 8 X XX4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X8 2.50*10^ 1 X X2XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX26X XX 2.25*10^ 1 X XXXX4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8XX 4 2.00*10^ 1 2XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 1.75*10^ 1 XXX4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 1.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 1.25*10^ 1 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8X 8 1.00*10^ 1 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2 0.75*10^ 1 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2 0.25*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 1 0000000000000112212222242342354363565456665465665475755655665565545453434334222322212110000000000000 *10^ 0 0000000000069280068073531346510689375863382840741519112049754245397114102032534028721028630000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 5444444444433333333332222222222111111111100000000000000000001111111111222222222233333333334444444444 *10^-1 0987654321098765432109876543210987654321098765432101234567890123456789012345678901234567890123456789 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 3162 Mean = -1.0247e-02 Underflow = 0.0000e+00 Low edge = -5.0000e+00 All chan = 3.1620e+03 Rms = 1.7845e+00 Overflow = 0.0000e+00 High edge = 5.0000e+00 2013-09-20 16:01 eta for jets, CellJet 7.80*10^ 1 X 7 7 X 7.50*10^ 1 X X X X 7.20*10^ 1 X X X 7 X 6.90*10^ 1 X X X X X 3 7 6.60*10^ 1 7 3 X X X X X X X X 6.30*10^ 1 X X X XX XX X XX3 33X X X 6.00*10^ 1 X7 X7 X7XX XX 3 X XXX 3XXX XXX 5.70*10^ 1 3 XX XX7 XXXX XX7X73X XXX7XXXX XXX 3 5.40*10^ 1 X XX XXX XXXX XXXXXXX3XXXXXXXXXXXX737X 5.10*10^ 1 X 7XX7XXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXX 4.80*10^ 1 X XXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 X 4.50*10^ 1 X XXXXXXX7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 3 4.20*10^ 1 X XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X 33 3.90*10^ 1 X 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7X X XX 3.60*10^ 1 X 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X3XX 3.30*10^ 1 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3XXXX 3 3.00*10^ 1 X X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7X 7 2.70*10^ 1 7 X X7X7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 2.40*10^ 1 X7X3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX3 7 2.10*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXX X 1.80*10^ 1 77 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3XXXX73X 1.50*10^ 1 XX7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 1.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.90*10^ 1 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.60*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.30*10^ 1 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 1 0000000000001111122322242333453565565547576566555575766556675666555543434344231222211210000000000000 *10^ 0 0000000000172774863027626576259059049648973163686572131681184708323568813400916794276349830000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 5444444444433333333332222222222111111111100000000000000000001111111111222222222233333333334444444444 *10^-1 0987654321098765432109876543210987654321098765432101234567890123456789012345678901234567890123456789 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 3369 Mean = -1.2185e-02 Underflow = 0.0000e+00 Low edge = -5.0000e+00 All chan = 3.3690e+03 Rms = 1.7931e+00 Overflow = 0.0000e+00 High edge = 5.0000e+00 2013-09-20 16:01 phi for jets, SlowJwt 4.60*10^ 1 X 4.50*10^ 1 X 4.40*10^ 1 X X 4.30*10^ 1 X X 4.20*10^ 1 X X X X 4.10*10^ 1 X X X X X X 4.00*10^ 1 X X X X X X X 3.90*10^ 1 X X X X X X X X X X X X 3.80*10^ 1 X X X X X X X X X X X X X 3.70*10^ 1 X X X X X X X X X X X X X X X X X 3.60*10^ 1 X X X X X X X X X X X X X X X X X X X XXXX 3.50*10^ 1 X X X X X X X X X X X X X X X X X X X X X X X XXXX 3.40*10^ 1 XX X X X XX X X XX XX X X X X X X X X X X X X X X X XXXX 3.30*10^ 1 XXXX X X X XXXX X XX XX X X X X X XX X X X X X X X X X X X XXXXX 3.20*10^ 1 XXXX X XX X XXXXX X XXX X XX X X X X XXX X XX X X X XXX X X XX XXX X XXXXX 3.10*10^ 1 XXXXXXX XXX XX XXXXX X XXX X XX X X XX XXXXXX XX XX X X X XXXXX XXXX XXX X XXXXX 3.00*10^ 1 XXXXXXXXXXX XX XXXXX X X XXX X XX X XX XX XXXXXX XX XXXX X X XXXXX XXXX XXX XXXXXXX 2.90*10^ 1 XXXXXXXXXXXX XX XXXXX XXXXXXXXX XX XXX X XXXXX XXXXXX XX XXXX X X X XXXXXX XXXX XXX XXXXXXXXX 2.80*10^ 1 XXXXXXXXXXXXX XX XXXXXXXXXXXXXXXXXXX XXX X XXXXX XXXXXX XXX XXXX XXX X XXXXXXX XXXXXXXX XXXXXXXXX 2.70*10^ 1 XXXXXXXXXXXXX XX XXXXXXXXXXXXXXXXXXXX XXX X XXXXX XXXXXX XXX XXXX XXX X XXXXXXX XXXXXXXXX XXXXXXXXX 2.60*10^ 1 XXXXXXXXXXXXX XX XXXXXXXXXXXXXXXXXXXX XXX X XXXXX XXXXXX XXX XXXX XXX X XXXXXXX XXXXXXXXX XXXXXXXXXX 2.50*10^ 1 XXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXX X XXXXX XXXXXXXXXX XXXX XXX X XXXXXXX XXXXXXXXX XXXXXXXXXX 2.40*10^ 1 XXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXX X XXXXX XXXXXXXXXXXXXXX XXXXX XXXXXXX XXXXXXXXX XXXXXXXXXX 2.30*10^ 1 XXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXX X XXXXX XXXXXXXXXXXXXXXXXXXXX XXXXXXX XXXXXXXXXXXXXXXXXXXX 2.20*10^ 1 XXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 2.10*10^ 1 XXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 2.00*10^ 1 XXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.90*10^ 1 XXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.80*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 1 2333333333332233123433323232433232222223323233233243343322332333323222322334342233342333222333333322 *10^ 0 9334914101728515884135289909642928997594626190951211222158124370537894329622108231248728736903669699 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 3332222222222222222111111111111111100000000000000000000000000000001111111111111111222222222222222233 *10^-1 1009887765543322100988776554332110098876655433211000112334556678890011233455677889001223345567788900 *10^-2 4825936048159260471582603715826937148259370481593606395184073952841739628517306285174062951840639528 Entries = 3162 Mean = 9.2598e-03 Underflow = 0.0000e+00 Low edge = -3.1416e+00 All chan = 3.1620e+03 Rms = 1.8303e+00 Overflow = 0.0000e+00 High edge = 3.1416e+00 2013-09-20 16:01 phi for jets, CellJet 5.64*10^ 1 7 5.52*10^ 1 X 5.40*10^ 1 X 5.28*10^ 1 X 5.16*10^ 1 X 5.04*10^ 1 X 4.92*10^ 1 X 4.80*10^ 1 X 4.68*10^ 1 3 X 4.56*10^ 1 5 5 X 5 X 4.44*10^ 1 7 X 7 X X X X 4.32*10^ 1 X X X X X X X 8 8 4.20*10^ 1 X X X X X X X 2 X X X X X X 4.08*10^ 1 X X X X 3 X X X X 3 X X X X X X 3.96*10^ 1 X X X 5X 5 X 5 X X X X X X X X X X 5 5 X 3.84*10^ 1 7X X X XX X X X X 7 X 7 X X X X X X X X 7X X X 3.72*10^ 1 XX X 8 X8 XX X X X X X X X X X X 8 X X8 X 8X X XX X X 3.60*10^ 1 XX2X X XX XX XX X 2X X X X X 2 X X XX X X X X X XX2X XX 2X XX X2XX 3.48*10^ 1 3XXXX X XX XX XX X XX 3X X X X X X X XX X X X X X3 3 XXXX XX XX XX XXXX 3.36*10^ 1 XXXXX X XX XX XX X XX XX X X X X 5X X XX X X X X XX X XXXX XX XX 5 XX5XXXX 3.24*10^ 1 XXXXX X XX XX XX7X 7XX XX X X X7 X7XX X XX X X X7 X XX X 7 XXXX XX7 XX X XXXXXXX 3.12*10^ 1 XXXXX X XX XX XXXX8XXX XX X X XX XXXX X XX8X X XX8X8 XX8X X XXXX XXX8XX X XXXXXXX 3.00*10^ 1 2XXXXX X XX2 XX XX XXXXXXXX XX X X X XX 2 XXXX X2XXXXXX2XXXXX2XXXXX2XX XXXX XXXXXXX X 2XXXXXXX 2.88*10^ 1 XXXXXX X3XXX XX 3XX XXXXXXXX3XX X X X XX3X XXXX3 XXXXXXXXXXXXXXXXXXXXXXX XXXX XXXXXXX X XXXXXXXX 2.76*10^ 1 5XXXXXX XXXXX XX XXX5XXXXXXXXXXX5X X X XXXX XXXXX5XXXXXXXXXXXXXXXXXXXXXXX XXXX XXXXXXX5X XXXXXXXX 5 2.64*10^ 1 XXXXXXX7XXXXX7XX XXXXXXXXXXXXXXXXX X X XXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXX7 XXXXXXXXX XXXXXXXX7X 2.52*10^ 1 XXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXX8X8X XXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXX8XXXXXXXXX8XXXXXXXXXX 2.40*10^ 1 XXXXXXXXXXXXXXXX2XXXXXXXXXXXXXXXXXXXXXXXXXX2XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXX 2.28*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3XXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 1 2233434232432233223423334333323324232324322233332242433433233343233333233243342233533342322333334322 *10^ 0 7948254678579600389476920125984672585042289352388759161006972121906414920267556507621537359893953667 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 3332222222222222222111111111111111100000000000000000000000000000001111111111111111222222222222222233 *10^-1 1009887765543322100988776554332110098876655433211000112334556678890011233455677889001223345567788900 *10^-2 4825936048159260471582603715826937148259370481593606395184073952841739628517306285174062951840639528 Entries = 3369 Mean = 1.3843e-02 Underflow = 1.0000e+01 Low edge = -3.1416e+00 All chan = 3.3430e+03 Rms = 1.8234e+00 Overflow = 1.6000e+01 High edge = 3.1416e+00 2013-09-20 16:01 R distance between jets, SlowJet 4.20*10^ 2 8 4.05*10^ 2 X 3.90*10^ 2 9X 3.75*10^ 2 XX 3.60*10^ 2 4 XX 3.45*10^ 2 XXXX 3.30*10^ 2 82XXXX9 3.15*10^ 2 39 XXXXXXX 3.00*10^ 2 XX6XXXXXXX 2.85*10^ 2 7XXXXXXXXXX 2.70*10^ 2 7XXXXXXXXXXX11 2.55*10^ 2 113XXXXXXXXXXXXXX 2.40*10^ 2 7 XXXXXXXXXXXXXXXXX 2.25*10^ 2 1X69 XXXXXXXXXXXXXXXXXX4 2.10*10^ 2 XXXX 95XXXXXXXXXXXXXXXXXXX55 1.95*10^ 2 XXXX7XXXXXXXXXXXXXXXXXXXXXXXX 1.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX1 1.65*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX29 1.50*10^ 2 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX11 1.35*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9 7 1.20*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.05*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.90*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 71 0.75*10^ 2 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9XX 9 0.60*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9X8X9 0.45*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 3 0.30*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6X84111 0.15*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX89777323111 1 Contents *10^ 2 0000000012222112222222233233333432222211111111100000000000000000000000000000000000000000000000000000 *10^ 1 0000000641312990024446801921548125510065633323087875756543232211111111000000000000000000000000000000 *10^ 0 0000000511594159351256144478159787662263466300033679370855447176723100535211000100000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-1 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 10087 Mean = 2.9016e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0087e+04 Rms = 1.2633e+00 Overflow = 0.0000e+00 High edge = 1.0000e+01 2013-09-20 16:01 R distance between jets, CellJet 4.80*10^ 2 7 4.60*10^ 2 9X 4.40*10^ 2 XX 4.20*10^ 2 8XX 4.00*10^ 2 83XXX 3.80*10^ 2 3 XXXXX 3.60*10^ 2 X9XXXXX6 3.40*10^ 2 5 XXXXXXXXX 3.20*10^ 2 X3XXXXXXXXXX 3.00*10^ 2 1 6XXXXXXXXXXXX 2.80*10^ 2 4XX9XXXXXXXXXXXXX7 2.60*10^ 2 5XXXXXXXXXXXXXXXXXX81 2.40*10^ 2 7XX 4 4XXXXXXXXXXXXXXXXXXXXX4 2.20*10^ 2 XXX9X7XXXXXXXXXXXXXXXXXXXXXXX 2.00*10^ 2 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 7 1.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4X56 1.60*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 35 1.40*10^ 2 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7XX 1.20*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 1.00*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6872 0.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8X5251 0.60*10^ 2 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX20 0.40*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX626 0.20*10^ 2 38XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9X85934212121 1 Contents *10^ 2 0000000112222222222222333333344433222211111111100000000000000000000000000000000000000000000000000000 *10^ 1 0000014393441212567879304659815751754286977345199987776764432311111110000000000000000000000000000000 *10^ 0 0000554254007737089271050685567429451897301561727346905125113199895077843414300001000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-1 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 11682 Mean = 2.8997e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.1682e+04 Rms = 1.2872e+00 Overflow = 0.0000e+00 High edge = 1.0000e+01 2013-09-20 16:01 pT difference, SlowJet 0.92*10^ 3 9 0.88*10^ 3 X 0.84*10^ 3 X 0.80*10^ 3 X 0.76*10^ 3 X 0.72*10^ 3 X 0.68*10^ 3 X 0.64*10^ 3 X 0.60*10^ 3 X 0.56*10^ 3 X 0.52*10^ 3 X 0.48*10^ 3 X 0.44*10^ 3 X 0.40*10^ 3 X 0.36*10^ 3 X 0.32*10^ 3 X 0.28*10^ 3 X9 0.24*10^ 3 XX 0.20*10^ 3 XX8 0.16*10^ 3 XXX3 0.12*10^ 3 XXXX51 0.08*10^ 3 XXXXXX7522 2 0.04*10^ 3 XXXXXXXXXXX98XX85764664353535244444533353132211113111111111 1 Contents *10^ 2 0000000000000000000092111000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000000000000017930865444334431221221111111011111111111010000001000000000000000000000000000000 *10^ 0 0000000000000000000046220568770500719925427294839977657940193528743520434223323110102111101010100101 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------- *10^ 2 1000000000000000000000000000000000000000111111111111111111112222222222222222222233333333333333333333 *10^ 1 0998877665544332211000112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^ 0 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 2662 Mean = 4.4746e+01 Underflow = 0.0000e+00 Low edge = -1.0000e+02 All chan = 2.6560e+03 Rms = 6.4630e+01 Overflow = 6.0000e+00 High edge = 4.0000e+02 2013-09-20 16:01 eT difference, CellJet 1.08*10^ 3 4 1.04*10^ 3 X 1.00*10^ 3 X 0.96*10^ 3 X 0.92*10^ 3 X 0.88*10^ 3 X 0.84*10^ 3 X 0.80*10^ 3 X 0.76*10^ 3 X 0.72*10^ 3 X 0.68*10^ 3 X 0.64*10^ 3 X 0.60*10^ 3 X 0.56*10^ 3 X 0.52*10^ 3 X 0.48*10^ 3 X 0.44*10^ 3 X 0.40*10^ 3 X 0.36*10^ 3 X1 0.32*10^ 3 XX 0.28*10^ 3 XX 0.24*10^ 3 XX 0.20*10^ 3 XX9 0.16*10^ 3 XXX 1 0.12*10^ 3 XXX9X 0.08*10^ 3 XXXXXX86213 0.04*10^ 3 XXXXXXXXXXX79XX9595555453344344534553334323221111111111111 11 1 Contents *10^ 3 0000000000000000000010000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0000000000000000000003111000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000000000000052912876445233332321221111111112111211111010000000000000000000000000000000000000 *10^ 0 0000000000000000000063543032632748840708107943552671159031351917764526652353231220101102011000110001 Low edge -------------------- *10^ 2 1000000000000000000000000000000000000000111111111111111111112222222222222222222233333333333333333333 *10^ 1 0998877665544332211000112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^ 0 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 2869 Mean = 4.2130e+01 Underflow = 0.0000e+00 Low edge = -1.0000e+02 All chan = 2.8620e+03 Rms = 6.3197e+01 Overflow = 7.0000e+00 High edge = 4.0000e+02 pythia8-8.1.80.orig/examples/outref/out140000644000175000017500000003300712217346172016362 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:03:44 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* Begin subrun number 0 : HardQCD:gg2gg Cross section is 5.874e-01 and in Pythia6 was 4.960e-01, i.e. now is factor >>> 1.184 <<< different Begin subrun number 1 : HardQCD:gg2qqbar + HardQCD:gg2ccbar + HardQCD:gg2bbbar Cross section is 1.919e-02 and in Pythia6 was 1.627e-02, i.e. now is factor >>> 1.180 <<< different Begin subrun number 2 : HardQCD:qg2qg Cross section is 3.222e-01 and in Pythia6 was 2.790e-01, i.e. now is factor >>> 1.155 <<< different Begin subrun number 3 : HardQCD:qq2qq Cross section is 3.187e-02 and in Pythia6 was 2.800e-02, i.e. now is factor >>> 1.138 <<< different Begin subrun number 4 : HardQCD:qqbar2gg Cross section is 3.835e-04 and in Pythia6 was 3.310e-04, i.e. now is factor >>> 1.159 <<< different Begin subrun number 5 : HardQCD:qqbar2qqbarNew + HardQCD:qqbar2ccbar + HardQCD:qqbar2bbbar Cross section is 4.118e-04 and in Pythia6 was 3.653e-04, i.e. now is factor >>> 1.127 <<< different Begin subrun number 6 : PromptPhoton:qg2qgamma Cross section is 1.797e-04 and in Pythia6 was 1.697e-04, i.e. now is factor >>> 1.059 <<< different Begin subrun number 7 : PromptPhoton:qqbar2ggamma Cross section is 1.261e-05 and in Pythia6 was 1.163e-05, i.e. now is factor >>> 1.085 <<< different Begin subrun number 8 : PromptPhoton:gg2ggamma Cross section is 1.346e-07 and in Pythia6 was 1.065e-07, i.e. now is factor >>> 1.263 <<< different Begin subrun number 9 : PromptPhoton:ffbar2gammagamma Cross section is 8.390e-08 and in Pythia6 was 8.259e-08, i.e. now is factor >>> 1.016 <<< different Begin subrun number 10 : PromptPhoton:gg2gammagamma Cross section is 9.827e-08 and in Pythia6 was 8.237e-08, i.e. now is factor >>> 1.193 <<< different Begin subrun number 11 : WeakBosonExchange:ff2ff(t:gmZ) Cross section is 2.551e-05 and in Pythia6 was 2.544e-05, i.e. now is factor >>> 1.003 <<< different Begin subrun number 12 : WeakBosonExchange:ff2ff(t:W) Cross section is 5.354e-06 and in Pythia6 was 5.321e-06, i.e. now is factor >>> 1.006 <<< different Begin subrun number 13 : WeakSingleBoson:ffbar2gmZ Cross section is 5.639e-05 and in Pythia6 was 5.571e-05, i.e. now is factor >>> 1.012 <<< different Begin subrun number 14 : WeakSingleBoson:ffbar2W Cross section is 1.647e-04 and in Pythia6 was 1.621e-04, i.e. now is factor >>> 1.016 <<< different Begin subrun number 15 : WeakDoubleBoson:ffbar2gmZgmZ Cross section is 9.302e-09 and in Pythia6 was 9.039e-09, i.e. now is factor >>> 1.029 <<< different Begin subrun number 16 : WeakDoubleBoson:ffbar2ZW Cross section is 2.271e-08 and in Pythia6 was 2.247e-08, i.e. now is factor >>> 1.011 <<< different Begin subrun number 17 : WeakDoubleBoson:ffbar2WW Cross section is 6.121e-08 and in Pythia6 was 5.893e-08, i.e. now is factor >>> 1.039 <<< different Begin subrun number 18 : WeakBosonAndParton:qqbar2gmZg Cross section is 4.078e-06 and in Pythia6 was 3.781e-06, i.e. now is factor >>> 1.078 <<< different Begin subrun number 19 : WeakBosonAndParton:qg2gmZq Cross section is 1.193e-05 and in Pythia6 was 1.078e-05, i.e. now is factor >>> 1.106 <<< different Begin subrun number 20 : WeakBosonAndParton:ffbar2gmZgm Cross section is 4.760e-08 and in Pythia6 was 4.551e-08, i.e. now is factor >>> 1.046 <<< different Begin subrun number 21 : WeakBosonAndParton:qqbar2Wg Cross section is 1.098e-05 and in Pythia6 was 1.025e-05, i.e. now is factor >>> 1.071 <<< different Begin subrun number 22 : WeakBosonAndParton:qg2Wq Cross section is 3.438e-05 and in Pythia6 was 3.208e-05, i.e. now is factor >>> 1.072 <<< different Begin subrun number 23 : WeakBosonAndParton:ffbar2Wgm Cross section is 5.530e-08 and in Pythia6 was 5.435e-08, i.e. now is factor >>> 1.018 <<< different Begin subrun number 24 : Charmonium:all Cross section is 1.350e-04 and in Pythia6 was 1.038e-04, i.e. now is factor >>> 1.300 <<< different Begin subrun number 25 : Bottomonium:all Cross section is 4.690e-05 and in Pythia6 was 3.929e-05, i.e. now is factor >>> 1.194 <<< different Begin subrun number 26 : Top:gg2ttbar Cross section is 4.741e-07 and in Pythia6 was 4.155e-07, i.e. now is factor >>> 1.141 <<< different Begin subrun number 27 : Top:qqbar2ttbar Cross section is 7.393e-08 and in Pythia6 was 6.685e-08, i.e. now is factor >>> 1.106 <<< different Begin subrun number 28 : Top:qq2tq(t:W) Cross section is 2.043e-07 and in Pythia6 was 1.898e-07, i.e. now is factor >>> 1.076 <<< different Begin subrun number 29 : Top:ffbar2ttbar(s:gmZ) Cross section is 4.253e-10 and in Pythia6 was 4.240e-10, i.e. now is factor >>> 1.003 <<< different Begin subrun number 30 : Top:ffbar2tqbar(s:W) PYTHIA Warning in PhaseSpace2to2tauyz::trialKin: maximum for cross section violated Cross section is 7.264e-09 and in Pythia6 was 7.142e-09, i.e. now is factor >>> 1.017 <<< different Begin subrun number 31 : HiggsSM:ffbar2H Cross section is 1.934e-10 and in Pythia6 was 1.547e-10, i.e. now is factor >>> 1.250 <<< different Begin subrun number 32 : HiggsSM:gg2H Cross section is 9.142e-09 and in Pythia6 was 7.064e-09, i.e. now is factor >>> 1.294 <<< different Begin subrun number 33 : HiggsSM:ffbar2HZ Cross section is 1.385e-10 and in Pythia6 was 1.316e-10, i.e. now is factor >>> 1.052 <<< different Begin subrun number 34 : HiggsSM:ffbar2HW Cross section is 2.479e-10 and in Pythia6 was 2.332e-10, i.e. now is factor >>> 1.063 <<< different Begin subrun number 35 : HiggsSM:ff2Hff(t:ZZ) Cross section is 5.132e-10 and in Pythia6 was 5.105e-10, i.e. now is factor >>> 1.005 <<< different Begin subrun number 36 : HiggsSM:ff2Hff(t:WW) Cross section is 1.319e-09 and in Pythia6 was 1.316e-09, i.e. now is factor >>> 1.002 <<< different Begin subrun number 37 : HiggsSM:qg2Hq Cross section is 5.799e-11 and in Pythia6 was 4.462e-11, i.e. now is factor >>> 1.300 <<< different Begin subrun number 38 : HiggsSM:gg2Hg(l:t) Cross section is 7.393e-09 and in Pythia6 was 5.557e-09, i.e. now is factor >>> 1.330 <<< different Begin subrun number 39 : HiggsSM:qg2Hq(l:t) Cross section is 2.544e-09 and in Pythia6 was 1.966e-09, i.e. now is factor >>> 1.294 <<< different Begin subrun number 40 : HiggsSM:qqbar2Hg(l:t) Cross section is 1.094e-11 and in Pythia6 was 8.725e-12, i.e. now is factor >>> 1.253 <<< different Begin subrun number 41 : HiggsBSM:allH1 PYTHIA Warning in ParticleDataEntry::initBWmass: switching off width for id = 25 Cross section is 3.230e-08 and in Pythia6 was 2.450e-08, i.e. now is factor >>> 1.318 <<< different Begin subrun number 42 : HiggsBSM:allH2 Cross section is 6.934e-09 and in Pythia6 was 5.839e-09, i.e. now is factor >>> 1.188 <<< different Begin subrun number 43 : HiggsBSM:allA3 Cross section is 2.125e-08 and in Pythia6 was 1.687e-08, i.e. now is factor >>> 1.260 <<< different Begin subrun number 44 : HiggsBSM:allH+- Cross section is 9.041e-11 and in Pythia6 was 8.950e-11, i.e. now is factor >>> 1.010 <<< different Begin subrun number 45 : HiggsBSM:allHpair Cross section is 4.254e-11 and in Pythia6 was 4.188e-11, i.e. now is factor >>> 1.016 <<< different Begin subrun number 46 : NewGaugeBoson:ffbar2gmZZprime Cross section is 2.000e-07 and in Pythia6 was 1.980e-07, i.e. now is factor >>> 1.010 <<< different Begin subrun number 47 : NewGaugeBoson:ffbar2Wprime Cross section is 4.570e-07 and in Pythia6 was 4.551e-07, i.e. now is factor >>> 1.004 <<< different Begin subrun number 48 : LeftRightSymmmetry:ffbar2ZR Cross section is 5.979e-09 and in Pythia6 was 6.005e-09, i.e. now is factor >>> 0.996 <<< different Begin subrun number 49 : LeftRightSymmmetry:ffbar2WR Cross section is 1.116e-07 and in Pythia6 was 1.102e-07, i.e. now is factor >>> 1.013 <<< different Begin subrun number 50 : LeftRightSymmmetry:ffbar2HLHL Cross section is 7.787e-11 and in Pythia6 was 7.784e-11, i.e. now is factor >>> 1.000 <<< different Begin subrun number 51 : LeftRightSymmmetry:ffbar2HRHR Cross section is 3.513e-11 and in Pythia6 was 3.488e-11, i.e. now is factor >>> 1.007 <<< different Begin subrun number 52 : LeptoQuark:all Cross section is 6.696e-08 and in Pythia6 was 6.006e-08, i.e. now is factor >>> 1.115 <<< different Begin subrun number 53 : ExcitedFermion:dg2dStar Cross section is 3.555e-06 and in Pythia6 was 3.235e-06, i.e. now is factor >>> 1.099 <<< different Begin subrun number 54 : ExcitedFermion:qq2dStarq Cross section is 1.841e-05 and in Pythia6 was 1.689e-05, i.e. now is factor >>> 1.090 <<< different Begin subrun number 55 : ExcitedFermion:qqbar2eStare Cross section is 5.791e-07 and in Pythia6 was 5.986e-07, i.e. now is factor >>> 0.967 <<< different Begin subrun number 56 : ExtraDimensionsG*:all Cross section is 3.102e-10 and in Pythia6 was 3.241e-10, i.e. now is factor >>> 0.957 <<< different pythia8-8.1.80.orig/examples/outref/out130000644000175000017500000005622612217346172016371 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:03:41 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with pbar- at a CM energy of 1.960e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | Les Houches User Process(es) 9999 | 5.480e-09 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 40.89 mb | | | | pT0 = 2.12 gives sigmaInteraction = 136.66 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:frameType | 4 | 1 1 5 | | Beams:LHEF | ttbar.lhe | void | | Init:showChangedParticleData | off | on | | Main:numberOfSubruns | 2 | 0 0 | | Main:subrun | 1 | -999 0 | | Main:timesAllowErrors | 3 | 10 0 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberCount | 0 | 1000 0 | | Next:numberShowEvent | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- LHA initialization information ------------ beam kind energy pdfgrp pdfset A 2212 980.000 0 7 B -2212 980.000 0 7 Event weighting strategy = 3 Processes, with strategy-dependent cross section info number xsec (pb) xerr (pb) xmax (pb) 81 5.2201e+00 5.3841e-01 1.0000e+00 82 2.6026e-01 1.0625e-01 1.0000e+00 -------- End LHA initialization information -------- -------- LHA event information and listing ---------------------------------------------------------------------- process = 81 weight = 1.0000e+00 scale = 1.7331e+02 (GeV) alpha_em = 7.8198e-03 alpha_strong = 1.1567e-01 Participating Particles no id stat mothers colours p_x p_y p_z e m tau spin 1 2 -1 0 0 101 0 0.000 0.000 108.382 108.382 0.000 0.000 9.000 2 -2 -1 0 0 0 102 0.000 0.000 -279.761 279.761 0.000 0.000 9.000 3 6 2 1 2 101 0 33.629 8.912 -110.596 212.418 177.987 0.000 9.000 4 -6 2 1 2 0 102 -33.629 -8.912 -60.783 175.725 161.166 0.000 9.000 5 24 2 3 0 0 0 -30.885 -12.140 -4.785 86.623 79.871 0.000 9.000 6 5 1 3 0 101 0 64.514 21.052 -105.811 125.794 4.800 0.000 9.000 7 -24 2 4 0 0 0 -50.940 34.881 -75.292 126.217 80.315 0.000 9.000 8 -5 1 4 0 0 102 17.311 -43.792 14.509 49.507 4.800 0.000 9.000 9 -1 1 5 0 0 103 18.584 9.166 18.652 27.882 0.330 0.000 9.000 10 2 1 5 0 103 0 -49.469 -21.306 -23.437 58.741 0.330 0.000 9.000 11 13 1 7 0 0 0 9.691 39.074 -25.560 47.687 0.106 0.000 9.000 12 -14 1 7 0 0 0 -60.632 -4.194 -49.732 78.530 0.000 0.000 9.000 pdf: id1 = 2 id2 = -2 x1 = 1.106e-01 x2 = 2.855e-01 scalePDF = 1.733e+02 pdf1 = 5.530e-01 pdf2 = 3.572e-01 -------- End LHA event information and listing ------------------------------------------------------------------ -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 9.800e+02, e = 9.800e+02, m = 9.383e-01. Beam B: id = -2212, pz = -9.800e+02, e = 9.800e+02, m = 9.383e-01. In 1: id = 2, x = 1.106e-01, pdf = 5.530e-01 at Q2 = 3.004e+04. In 2: id = -2, x = 2.855e-01, pdf = 3.572e-01 at same Q2. Process Les Houches User Process(es) with code 9999 is 2 -> 2. Subprocess user process 81 with code 81 is 2 -> 2. It has sHat = 1.213e+05, tHat = -3.834e+04, uHat = -2.529e+04, pTHat = 3.479e+01, m3Hat = 1.780e+02, m4Hat = 1.612e+02, thetaHat = 2.065e+00, phiHat = 2.590e-01. alphaEM = 7.820e-03, alphaS = 1.157e-01 at Q2 = 3.004e+04. Impact parameter b = 6.777e-01 gives enhancement factor = 1.623e+00. Max pT scale for MPI = 1.960e+03, ISR = 1.960e+03, FSR = 1.960e+03. Number of MPI = 6, ISR = 12, FSRproc = 46, FSRreson = 25. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 1960.000 1960.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 980.000 980.000 0.938 2 -2212 (pbar-) -12 0 0 4 0 0 0 0.000 0.000 -980.000 980.000 0.938 3 2 (u) -21 1 0 5 6 101 0 0.000 0.000 108.382 108.382 0.000 4 -2 (ubar) -21 2 0 5 6 0 102 0.000 0.000 -279.761 279.761 0.000 5 6 (t) -22 3 4 7 8 101 0 33.629 8.912 -110.596 212.418 177.987 6 -6 (tbar) -22 3 4 9 10 0 102 -33.629 -8.912 -60.783 175.725 161.166 7 24 (W+) -22 5 0 11 12 0 0 -30.885 -12.140 -4.785 86.623 79.871 8 5 b 23 5 0 0 0 101 0 64.514 21.052 -105.811 125.794 4.800 9 -24 (W-) -22 6 0 13 14 0 0 -50.940 34.881 -75.292 126.217 80.315 10 -5 bbar 23 6 0 0 0 0 102 17.311 -43.792 14.509 49.507 4.800 11 -1 dbar 23 7 0 0 0 0 103 18.584 9.166 18.652 27.882 0.330 12 2 u 23 7 0 0 0 103 0 -49.469 -21.306 -23.437 58.741 0.330 13 13 mu- 23 9 0 0 0 0 0 9.691 39.074 -25.560 47.687 0.106 14 -14 nu_mubar 23 9 0 0 0 0 0 -60.632 -4.194 -49.732 78.530 0.000 Charge sum: 0.000 Momentum sum: -0.000 0.000 -171.379 388.143 348.258 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Warning in TimeShower::findMEcorr: ME weight above PS one PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again PYTHIA Abort from Pythia::next: reached end of Les Houches Events File *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | Les Houches User Process(es) 9999 | 200 200 200 | 5.480e-09 5.488e-10 | | ... whereof user classification code 81 | 192 192 192 | | | ... whereof user classification code 82 | 8 8 8 | | | | | | | sum | 200 200 200 | 5.480e-09 5.488e-10 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 2 Abort from Pythia::next: reached end of Les Houches Events File | | 2 Error in Pythia::next: hadronLevel failed; try again | | 2 Error in StringFragmentation::fragment: stuck in joining | | 2 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | 1 Warning in TimeShower::findMEcorr: ME weight above PS one | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:03 charged particle multiplicity 1.30*10^ 1 X 1.25*10^ 1 X 1.20*10^ 1 X 1.15*10^ 1 X 1.10*10^ 1 X X X 1.05*10^ 1 X X X 1.00*10^ 1 X XXX X 0.95*10^ 1 X XXX X 0.90*10^ 1 X XXXXX X 0.85*10^ 1 X XXXXX X 0.80*10^ 1 XXXXXXX X XX 0.75*10^ 1 XXXXXXX X XX 0.70*10^ 1 X XXXXXXX XX XX 0.65*10^ 1 X XXXXXXX XX XX 0.60*10^ 1 X XXXXXXX XX XX X 0.55*10^ 1 X XXXXXXX XX XX X 0.50*10^ 1 X XXXXXXXXX XXXXX X 0.45*10^ 1 X XXXXXXXXX XXXXX X 0.40*10^ 1 X XX XX XXXXXXXXX XXXXXX XXX X X 0.35*10^ 1 X XX XX XXXXXXXXX XXXXXX XXX X X 0.30*10^ 1 XX XX XXX XXXXXXXXXXXXXXXX XXX X X X 0.25*10^ 1 XX XX XXX XXXXXXXXXXXXXXXX XXX X X X 0.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX 0.15*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX 0.10*10^ 1 X XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXX X X X 0.05*10^ 1 X XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXX X X X Contents *10^ 1 0000000000000000000000000001011101000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000010000110137244234421800193553875984246424042310010100000000000000000001000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^ 1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^ 0 1482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 200 Mean = 1.3612e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 2.0000e+02 Rms = 3.9486e+01 Overflow = 0.0000e+00 High edge = 3.9950e+02 pythia8-8.1.80.orig/examples/outref/out230000644000175000017500000024435412217346175016376 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:07:10 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> g g 111 | 2.255e-01 | | g g -> q qbar (uds) 112 | 2.395e-03 | | q g -> q g 113 | 1.265e-01 | | q q(bar)' -> q q(bar)' 114 | 1.237e-02 | | q qbar -> g g 115 | 8.594e-05 | | q qbar -> q' qbar' (uds) 116 | 2.341e-05 | | g g -> c cbar 121 | 7.920e-04 | | q qbar -> c cbar 122 | 7.761e-06 | | g g -> b bbar 123 | 7.365e-04 | | q qbar -> b bbar 124 | 7.389e-06 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:allowMomentumSpread | on | off | | Beams:allowVertexSpread | on | off | | Beams:frameType | 3 | 1 1 5 | | Beams:pxA | 1.00000 | 0.0 | | Beams:pxB | 1.00000 | 0.0 | | Beams:sigmaPxA | 0.10000 | 0.0 0.0 | | Beams:sigmaPxB | 0.10000 | 0.0 0.0 | | Beams:sigmaPyA | 0.10000 | 0.0 0.0 | | Beams:sigmaPyB | 0.10000 | 0.0 0.0 | | Beams:sigmaPzA | 5.00000 | 0.0 0.0 | | Beams:sigmaPzB | 5.00000 | 0.0 0.0 | | Beams:sigmaVertexX | 0.30000 | 0.0 0.0 | | Beams:sigmaVertexY | 0.30000 | 0.0 0.0 | | Beams:sigmaVertexZ | 50.00000 | 0.0 0.0 | | HardQCD:all | on | off | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PartonLevel:all | off | on | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:pTHatMin | 20.00000 | 0.0 0.0 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 6.997e+03, e = 6.997e+03, m = 9.383e-01. Beam B: id = 2212, pz = -6.997e+03, e = 6.997e+03, m = 9.383e-01. In 1: id = 21, x = 1.228e-02, pdf = 1.880e+00 at Q2 = 7.575e+02. In 2: id = 2, x = 9.239e-03, pdf = 1.406e-01 at same Q2. Subprocess q g -> q g with code 113 is 2 -> 2. It has sHat = 2.222e+04, tHat = -7.852e+02, uHat = -2.144e+04, pTHat = 2.752e+01, m3Hat = 0.000e+00, m4Hat = 3.300e-01, thetaHat = 3.782e-01, phiHat = 1.152e-01. alphaEM = 7.713e-03, alphaS = 1.682e-01 at Q2 = 7.575e+02. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 2.052 0.071 -3.177 13994.162 13994.162 1 2212 (p+) -12 0 0 3 0 0 0 1.033 -0.015 6995.493 6995.493 0.938 2 2212 (p+) -12 0 0 4 0 0 0 1.019 0.086 -6998.669 6998.670 0.938 3 21 (g) -21 1 0 5 6 102 101 0.013 -0.000 85.913 85.913 0.000 4 2 (u) -21 2 0 5 6 101 0 0.009 0.001 -64.662 64.662 0.000 5 21 g 23 3 4 0 0 102 103 27.353 3.162 80.592 85.166 0.000 6 2 u 23 3 4 0 0 103 0 -27.331 -3.162 -59.341 65.410 0.330 Charge sum: 0.667 Momentum sum: 0.022 0.001 21.251 150.575 149.068 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- Pythia::next(): 1000 events have been generated Pythia::next(): 2000 events have been generated Pythia::next(): 3000 events have been generated Pythia::next(): 4000 events have been generated Pythia::next(): 5000 events have been generated Pythia::next(): 6000 events have been generated Pythia::next(): 7000 events have been generated Pythia::next(): 8000 events have been generated Pythia::next(): 9000 events have been generated *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> g g 111 | 41218 6167 6167 | 3.385e-02 2.310e-04 | | g g -> q qbar (uds) 112 | 440 67 67 | 3.741e-04 2.391e-05 | | q g -> q g 113 | 23082 3359 3359 | 1.851e-02 1.696e-04 | | q q(bar)' -> q q(bar)' 114 | 2228 352 352 | 2.006e-03 5.547e-05 | | q qbar -> g g 115 | 16 1 1 | 1.414e-05 1.414e-05 | | q qbar -> q' qbar' (uds) 116 | 5 0 0 | 0.000e+00 0.000e+00 | | g g -> c cbar 121 | 145 21 21 | 1.262e-04 1.433e-05 | | q qbar -> c cbar 122 | 3 1 1 | 1.278e-06 1.278e-06 | | g g -> b bbar 123 | 133 32 32 | 1.421e-04 1.410e-05 | | q qbar -> b bbar 124 | 3 0 0 | 0.000e+00 0.000e+00 | | | | | | sum | 67273 10000 10000 | 5.503e-02 2.939e-04 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 0 no errors or warnings to report | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:07 center-of-mass energy deviation 5.60*10^ 2 5 5.40*10^ 2 6 X 1 5.20*10^ 2 X1 X5X 5.00*10^ 2 6XXXXXX 4.80*10^ 2 XXXXXXX4 4.60*10^ 2 XXXXXXXXX7 4.40*10^ 2 XXXXXXXXXX 4.20*10^ 2 XXXXXXXXXX 1 4.00*10^ 2 XXXXXXXXXX9X 3.80*10^ 2 159XXXXXXXXXXXX 3.60*10^ 2 XXXXXXXXXXXXXXX 3.40*10^ 2 XXXXXXXXXXXXXXX5 3.20*10^ 2 3XXXXXXXXXXXXXXXX 3.00*10^ 2 XXXXXXXXXXXXXXXXX 2.80*10^ 2 XXXXXXXXXXXXXXXXX55 2.60*10^ 2 XXXXXXXXXXXXXXXXXXX 2.40*10^ 2 5XXXXXXXXXXXXXXXXXXX 2.20*10^ 2 4XXXXXXXXXXXXXXXXXXXX2 2.00*10^ 2 XXXXXXXXXXXXXXXXXXXXXX 1.80*10^ 2 9XXXXXXXXXXXXXXXXXXXXXX7 1.60*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXX 1.40*10^ 2 2XXXXXXXXXXXXXXXXXXXXXXXX2 1.20*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXX2 1.00*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.80*10^ 2 9XXXXXXXXXXXXXXXXXXXXXXXXXXXX5 0.60*10^ 2 24XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX44 0.40*10^ 2 25XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 0.20*10^ 2 1336XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX85311 Contents *10^ 2 0000000000000000000000000000000000001112233334455455544343222111000000000000000000000000000000000000 *10^ 1 0000000000000000000000000000001224470270306676930941265903770720744310000000000000000000000000000000 *10^ 0 0000000000000000000000000002552395870588062980211990284810003445087669731000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 1 2111111111111111111111111100000000000000000000000000000000000000000000000001111111111111111111111111 *10^ 0 0998887766655444332221100099888776665544433222110000011222334445566677888990001122233444556667788899 *10^-1 0628406284062840628406284062840628406284062840628404826048260482604826048260482604826048260482604826 Entries = 10000 Mean = -5.8000e-03 Underflow = 0.0000e+00 Low edge = -2.0000e+01 All chan = 1.0000e+04 Rms = 2.8836e+00 Overflow = 0.0000e+00 High edge = 2.0000e+01 2013-09-20 16:07 net pX offset 6.00*10^ 2 5 5.80*10^ 2 X 5.60*10^ 2 31435X 5.40*10^ 2 XXXXXX3 5.20*10^ 2 XXXXXXX4 5.00*10^ 2 XXXXXXXX 4.80*10^ 2 XXXXXXXXX 4.60*10^ 2 15XXXXXXXXX 4.40*10^ 2 XXXXXXXXXXX9 4.20*10^ 2 XXXXXXXXXXXX 4.00*10^ 2 XXXXXXXXXXXX 3.80*10^ 2 8XXXXXXXXXXXX 3.60*10^ 2 XXXXXXXXXXXXX4 3.40*10^ 2 5XXXXXXXXXXXXXX 3.20*10^ 2 XXXXXXXXXXXXXXX 3.00*10^ 2 XXXXXXXXXXXXXXX4 2.80*10^ 2 XXXXXXXXXXXXXXXX7 2.60*10^ 2 8XXXXXXXXXXXXXXXXX 2.40*10^ 2 3XXXXXXXXXXXXXXXXXX7 2.20*10^ 2 XXXXXXXXXXXXXXXXXXXX 2.00*10^ 2 XXXXXXXXXXXXXXXXXXXX 1.80*10^ 2 32XXXXXXXXXXXXXXXXXXXXX 1.60*10^ 2 XXXXXXXXXXXXXXXXXXXXXXX 1.40*10^ 2 5XXXXXXXXXXXXXXXXXXXXXXX42 1.20*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXX 1.00*10^ 2 7XXXXXXXXXXXXXXXXXXXXXXXXXX 0.80*10^ 2 5XXXXXXXXXXXXXXXXXXXXXXXXXXX70 0.60*10^ 2 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.40*10^ 2 17XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9X6 0.20*10^ 2 111 133388XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX633111 1 Contents *10^ 2 0000000000000000000000000000000000000111223344555555554432221110000000000000000000000000000000000000 *10^ 1 0000000000000000000000000000001123579366252745444458207348738227634321000000000000000000000000000000 *10^ 0 0000000000000000000001110036665523304064569520528609579888330843180102751130020000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-2 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 10000 Mean = -2.1280e-03 Underflow = 0.0000e+00 Low edge = -1.0000e+00 All chan = 1.0000e+04 Rms = 1.3987e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:07 net pY offset 6.00*10^ 2 3 5.80*10^ 2 X 5.60*10^ 2 1 X 5.40*10^ 2 X 19X7X 5.20*10^ 2 X5XXXXX 5.00*10^ 2 XXXXXXX4 4.80*10^ 2 XXXXXXXX5 4.60*10^ 2 26XXXXXXXXX 4.40*10^ 2 XXXXXXXXXXX5 4.20*10^ 2 XXXXXXXXXXXX 4.00*10^ 2 XXXXXXXXXXXX 3.80*10^ 2 XXXXXXXXXXXX8 3.60*10^ 2 8XXXXXXXXXXXXX 3.40*10^ 2 5XXXXXXXXXXXXXX4 3.20*10^ 2 XXXXXXXXXXXXXXXX 3.00*10^ 2 XXXXXXXXXXXXXXXX 2.80*10^ 2 XXXXXXXXXXXXXXXX8 2.60*10^ 2 7XXXXXXXXXXXXXXXXX 2.40*10^ 2 1XXXXXXXXXXXXXXXXXX 2.20*10^ 2 XXXXXXXXXXXXXXXXXXX71 2.00*10^ 2 XXXXXXXXXXXXXXXXXXXXX 1.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXX 1.60*10^ 2 7XXXXXXXXXXXXXXXXXXXXXXX 1.40*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXX 1.20*10^ 2 0XXXXXXXXXXXXXXXXXXXXXXXXX7 1.00*10^ 2 8XXXXXXXXXXXXXXXXXXXXXXXXXXX 0.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXX9 0.60*10^ 2 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.40*10^ 2 152XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX262 0.20*10^ 2 111529XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6651 1 1 Contents *10^ 2 0000000000000000000000000000000000000111223344555555544433222111000000000000000000000000000000000000 *10^ 1 0000000000000000000000000000001232469058253545412383386372710521752321110000000000000000000000000000 *10^ 0 0000000000000000000000000122948105807130230643202854989058642903754131201020000001000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-2 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 10000 Mean = 2.6600e-03 Underflow = 0.0000e+00 Low edge = -1.0000e+00 All chan = 1.0000e+04 Rms = 1.4156e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:07 net pZ offset 3.00*10^ 2 2 2.90*10^ 2 7 1 6X 2.80*10^ 2 X X XX 2.70*10^ 2 1 1 X5X XX 7 2.60*10^ 2 X X XXX XX X 2.50*10^ 2 X X XXXX5XX X 2.40*10^ 2 X X6XXXXXXXX X 2.30*10^ 2 46 X4XXXXXXXXXX X32 2.20*10^ 2 9 XX XXXXXXXXXXXX XXX642 2.10*10^ 2 X XXXXXXXXXXXXXXX6XXXXXX44 2.00*10^ 2 2X XXXXXXXXXXXXXXXXXXXXXXXX 1.90*10^ 2 XX2XXXXXXXXXXXXXXXXXXXXXXXX6 1.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.70*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXX7 2 1.60*10^ 2 87XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.50*10^ 2 9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 1.40*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.30*10^ 2 8 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.20*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX87 4 1.10*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 1.00*10^ 2 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9X 0.90*10^ 2 X1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.80*10^ 2 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.70*10^ 2 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX72 0.60*10^ 2 X5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX1 0.50*10^ 2 5 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 0.40*10^ 2 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9 31 0.30*10^ 2 68XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6 0.20*10^ 2 2 1 59XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX94 8 0.10*10^ 2 11 23227X8X7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX88X45322 2 Contents *10^ 2 0000000000000000000000000000111111111212222222222222222222222221111111010000000000000000000000000000 *10^ 1 0000000000010101122344465798022244559182216263458684890622111008666411918766543333211001000000000000 *10^ 0 0011002322728175968250755631080309872924601416007515626732642446702587944772159031694888453220200000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 10000 Mean = -3.3840e-02 Underflow = 0.0000e+00 Low edge = -1.0000e+01 All chan = 1.0000e+04 Rms = 2.8985e+00 Overflow = 0.0000e+00 High edge = 1.0000e+01 2013-09-20 16:07 individual abs(pZ) offset 8.40*10^ 2 8 8.10*10^ 2 1X 7.80*10^ 2 XX 7.50*10^ 2 6XX1 7.20*10^ 2 XXXXX5 6.90*10^ 2 XXXXXX541 6.60*10^ 2 648XXXXXXXXX 6.30*10^ 2 4XXXXXXXXXXXX 6.00*10^ 2 XXXXXXXXXXXXX2 5.70*10^ 2 27XXXXXXXXXXXXXX 1 5.40*10^ 2 XXXXXXXXXXXXXXXX2X 5.10*10^ 2 XXXXXXXXXXXXXXXXXX 7 4.80*10^ 2 XXXXXXXXXXXXXXXXXXX6X3 4.50*10^ 2 9XXXXXXXXXXXXXXXXXXXXXX 4.20*10^ 2 96XXXXXXXXXXXXXXXXXXXXXXX3 3.90*10^ 2 7XXXXXXXXXXXXXXXXXXXXXXXXXX1 3.60*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXX 3.30*10^ 2 57XXXXXXXXXXXXXXXXXXXXXXXXXXXX76 3.00*10^ 2 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 2.70*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9 2.40*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 2.10*10^ 2 9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX72 1.80*10^ 2 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2 1.50*10^ 2 36XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.20*10^ 2 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.90*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 0.60*10^ 2 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.30*10^ 2 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6 Contents *10^ 2 0000000000000000000000000000111222333444455666677787766655545433332221110000000000000000000000000000 *10^ 1 0000000000000000000000000149335039128104846144513832077671460596216208517410000000000000000000000000 *10^ 0 0000000000000000000000000334079692521877152183597333442277482983277625620280000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 20000 Mean = -3.8200e-03 Underflow = 0.0000e+00 Low edge = -1.0000e+01 All chan = 2.0000e+04 Rms = 2.0437e+00 Overflow = 0.0000e+00 High edge = 1.0000e+01 2013-09-20 16:07 vertex x position 2.90*10^ 2 7 2.80*10^ 2 X5X3 3 2.70*10^ 2 6 XXXXX X 2.60*10^ 2 X XXXXX3 X3 2.50*10^ 2 X XXXXXX1XX7 2.40*10^ 2 3 X XXXXXXXXXX 2 2.30*10^ 2 8X X6XXXXXXXXXX7X962 2.20*10^ 2 XX XXXXXXXXXXXXXXXXX 4 2.10*10^ 2 XXXXXXXXXXXXXXXXXXXXX 4 X 2.00*10^ 2 XXXXXXXXXXXXXXXXXXXXX3X X 1.90*10^ 2 XXXXXXXXXXXXXXXXXXXXXXX6X 1.80*10^ 2 424XXXXXXXXXXXXXXXXXXXXXXXXX 1.70*10^ 2 22XXXXXXXXXXXXXXXXXXXXXXXXXXXX 8 1.60*10^ 2 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X3 1.50*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 1.40*10^ 2 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8XX 1 1.30*10^ 2 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9X 1.20*10^ 2 X8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.10*10^ 2 19XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2X 2 1.00*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 0.90*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9X4 0.80*10^ 2 254XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6 0.70*10^ 2 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.60*10^ 2 6 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2 3 0.50*10^ 2 XX9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7X68 0.40*10^ 2 1 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.30*10^ 2 4X94XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX57X 0.20*10^ 2 X936XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2173 0.10*10^ 2 41 443345699XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX869835362 3 Contents *10^ 2 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position 2.90*10^ 2 3 2.80*10^ 2 7X 2.70*10^ 2 XX 9 9 2.60*10^ 2 3XXXXX4 X7 2.50*10^ 2 24 4XXXXXXX XX9 2.40*10^ 2 X1XX9XXXXXXXX XXX 2.30*10^ 2 3XXXXXXXXXXXXX9XXX 6 2.20*10^ 2 XXXXXXXXXXXXXXXXXX X 2.10*10^ 2 2 5XXXXXXXXXXXXXXXXXX7X 6 2.00*10^ 2 X XXXXXXXXXXXXXXXXXXXXX9 X2 1.90*10^ 2 7 X4XXXXXXXXXXXXXXXXXXXXXX XX 5 1.80*10^ 2 X XXXXXXXXXXXXXXXXXXXXXXXXXXX X 1.70*10^ 2 8 X3XXXXXXXXXXXXXXXXXXXXXXXXXXX X 1.60*10^ 2 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXX1X 1.50*10^ 2 X2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.40*10^ 2 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9 1.30*10^ 2 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9 1.20*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX51 1.10*10^ 2 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX67 1.00*10^ 2 698XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.90*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9 3 0.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX67X 0.70*10^ 2 2695XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2 0.60*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.50*10^ 2 85XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX24 2 0.40*10^ 2 88XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3X1 0.30*10^ 2 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9 0.20*10^ 2 45749XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX856 1 0.10*10^ 2 22233345678XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4X776548121512 Contents *10^ 2 0000000000000000000000000000001111111212222222222222222222221121111111110000000000000000000000000000 *10^ 1 0000000000001111112334466669990236486080243443456786652654029809583211008778644343211101000000000000 *10^ 0 0222333456780457498888526956982238273245301249430730949979769062159951679673224321985641776548121512 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-2 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 10000 Mean = 2.7094e-03 Underflow = 3.0000e+00 Low edge = -1.0000e+00 All chan = 9.9910e+03 Rms = 2.9668e-01 Overflow = 6.0000e+00 High edge = 1.0000e+00 2013-09-20 16:07 vertex z position 4.05*10^ 2 1 5 3.90*10^ 2 X X 3.75*10^ 2 3 X X48 3.60*10^ 2 X8X7XXX 3.45*10^ 2 6 3XXXXXXX 3.30*10^ 2 X2XXXXXXXX 26 3.15*10^ 2 1XXXXXXXXXX7XX 3.00*10^ 2 XXXXXXXXXXXXXX 2.85*10^ 2 XXXXXXXXXXXXXX 1 2.70*10^ 2 13XXXXXXXXXXXXXX7X 2.55*10^ 2 9 XXXXXXXXXXXXXXXXXX3 2.40*10^ 2 4X XXXXXXXXXXXXXXXXXXX9 2.25*10^ 2 6XX7XXXXXXXXXXXXXXXXXXXX 2.10*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXX7 1.95*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXX8 1.80*10^ 2 9XXXXXXXXXXXXXXXXXXXXXXXXXX46 1.65*10^ 2 355XXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.50*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.35*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.20*10^ 2 83XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX891 1.05*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 0.90*10^ 2 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.75*10^ 2 X9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 0.60*10^ 2 53XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 0.45*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 0.30*10^ 2 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX1 0.15*10^ 2 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 Contents *10^ 2 0000000000000000000000000000000111111222222333333333333332222211111110000000000000000000000000000000 *10^ 1 0000000000000000000000000025587105557135255031365959671126743097751109754100000000000000000000000000 *10^ 0 0000000000000000000000000623034795789914169198557268620846149621407968272660000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 2 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^ 0 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 10000 Mean = -1.6920e-01 Underflow = 0.0000e+00 Low edge = -1.0000e+02 All chan = 1.0000e+04 Rms = 2.0433e+01 Overflow = 0.0000e+00 High edge = 1.0000e+02 2013-09-20 16:07 vertex time 4.05*10^ 2 X 2 3.90*10^ 2 X5X4 3.75*10^ 2 7XXXX 3.60*10^ 2 7 XXXXXX 3.45*10^ 2 X9XXXXXX 3.30*10^ 2 53XXXXXXXX 1 3.15*10^ 2 3XXXXXXXXXX5X 3.00*10^ 2 XXXXXXXXXXXXX16 2.85*10^ 2 8 XXXXXXXXXXXXXXX 2.70*10^ 2 X4XXXXXXXXXXXXXXX4 2.55*10^ 2 XXXXXXXXXXXXXXXXXX 2.40*10^ 2 4XXXXXXXXXXXXXXXXXXX2 2.25*10^ 2 33XXXXXXXXXXXXXXXXXXXXX7 2.10*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXX87 1.95*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXX51 1.80*10^ 2 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.65*10^ 2 X9XXXXXXXXXXXXXXXXXXXXXXXXXXXX7 1.50*10^ 2 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.35*10^ 2 59XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 1.20*10^ 2 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 1.05*10^ 2 X9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.90*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9 0.75*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX77 0.60*10^ 2 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.45*10^ 2 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2 0.30*10^ 2 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.15*10^ 2 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 Contents *10^ 2 0000000000000000000000000000001111111222222333333433333322222221111100000000000000000000000000000000 *10^ 1 0000000000000000000000000023561023476113486022547089860189622008863198773200000000000000000000000000 *10^ 0 0000000000000000000000000629003374233451021520630533108674180768101069013650000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 2 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^ 0 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 10000 Mean = -9.0000e-03 Underflow = 0.0000e+00 Low edge = -1.0000e+02 All chan = 1.0000e+04 Rms = 2.0365e+01 Overflow = 0.0000e+00 High edge = 1.0000e+02 2013-09-20 16:07 vertex |x| + |t| 4.20*10^ 2 1 4.05*10^ 2 X 3.90*10^ 2 8X 3.75*10^ 2 9 97XX 3.60*10^ 2 2 X9XXXX 3.45*10^ 2 63X3XXXXXX 3.30*10^ 2 1 XXXXXXXXXX 3.15*10^ 2 X XXXXXXXXXX 3.00*10^ 2 X379XXXXXXXXXX 2.85*10^ 2 76XXXXXXXXXXXXXX 2.70*10^ 2 1 8 XXXXXXXXXXXXXXXX 2.55*10^ 2 X7X XXXXXXXXXXXXXXXX 2.40*10^ 2 9XXXX8XXXXXXXXXXXXXXXX 2.25*10^ 2 6XXXXXXXXXXXXXXXXXXXXXX 2.10*10^ 2 13XXXXXXXXXXXXXXXXXXXXXXX 1.95*10^ 2 54 XXXXXXXXXXXXXXXXXXXXXXXXX 1.80*10^ 2 8 XX3XXXXXXXXXXXXXXXXXXXXXXXXX 1.65*10^ 2 1 9X7XXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.50*10^ 2 2X7 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.35*10^ 2 XXX7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.20*10^ 2 X45XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.05*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.90*10^ 2 57 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.75*10^ 2 1 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.60*10^ 2 X7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.45*10^ 2 57XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.30*10^ 2 9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.15*10^ 2 196XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 2 0000000000001111111111111112222222223222333333333400000000000000000000000000000000000000000000000000 *10^ 1 0102346568872113543676887991355643871899334375778000000000000000000000000000000000000000000000000000 *10^ 0 2499702663650128251470860799861707096959948538317700000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 0 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 10000 Mean = 3.3302e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+04 Rms = 1.1810e+01 Overflow = 0.0000e+00 High edge = 1.0000e+02 2013-09-20 16:07 standard random number distribution 10.64*10^ 2 8 10.60*10^ 2 X 10.56*10^ 2 3 X 3 3 10.52*10^ 2 X X X X 10.48*10^ 2 X XX X X 5 10.44*10^ 2 X 8 X XX X X X 10.40*10^ 2 X X X XX X X X X 10.36*10^ 2 5 5 X X X X XX X X X 3 X X 10.32*10^ 2 X X 5 X X X X X X XX X X X X X 5 X X 10.28*10^ 2 X X X X XX X X X X XX 5 X XXX X X X X X 10.24*10^ 2 X X X X XX X X X X XX X X XXX X X8 X X 5 X5 10.20*10^ 2 X 3 X 5 X X XX X 5X X X XX X X X XXX 3X XX X X X XX 10.16*10^ 2 3X X X X X X 8XX8X XX X X XX3 X X 3X XXX XX XX8 X X X5XX 10.12*10^ 2 XX X X X 3 X X XXXXX XX X X XXX X8X XX XXX8 XX XXX5 5 X X XXXX 10.08*10^ 2 XX X X X X X X XXXXX XX X X 35 XXX XXX XX 3 XXXX XX XXXX8 X X X XXXX 10.04*10^ 2 XX3 X X X X X X XXXXX XX X X XX XXX XXX XX X XXXX XX XXXXX3 X X3 X X XXXX 10.00*10^ 2 XXX X X X X X X X3 XXXXX XX X X XX XXX XXX XX X XXXX XXXXXXXXX X XX X X XXXX 9.96*10^ 2 XXX X X X X X X5XX XXXXX XX X X 5XX XXX XXX XX X XXXXXXXXXXXXXX X XX X XXXXXX 9.92*10^ 2 XXX X3X X X X X XXXX XXXXX XX X X XXX XXX XXX5 XX 8X XXXXXXXXXXXXXX X8XX X XXXXXX 9.88*10^ 2 XXX XXX X X X X XXXX XXXXX3XX X X XXX XXX XXXX XX XX XXXXXXXXXXXXXX58XXXX X3 XXXXXX 9.84*10^ 2 XXX XXX5X X X X XXXX XXXXXXXX X X XXX XXX XXXX 8XX XX 58XXXXXXXXXXXXXXXXXXXX XX XXXXXX 9.80*10^ 2 XXX XXXXX XXX X X X XXXX53XXXXXXXX X X XXXX XXX 8 XXXX XXX XX XXXXXXXXXXXXXXXXXXXXXX XX XXXXXX 9.76*10^ 2 XXX XXXXX XXX X X X XXXXXXXXXXXXXX X X XXXXXXXX5 X 5 XXXX XXX XX 8XXXXXXXXXXXXXXXXXXXXXX XXXXXXXXX 9.72*10^ 2 XXX XXXXX8XXX X X X XXXXXXXXXXXXXX X X XXXXXXXXX X XXXXXXXXXX XX XXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXX 9.68*10^ 2 XXX 5XXXXXXXXX X X X XXXXXXXXXXXXXX X X XXXXXXXXX X XXXXXXXXXX XX XXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXX 9.64*10^ 2 XXX XXXXXXXXXX XXX X XXXXXXXXXXXXXX5XX XXXXXXXXXXX X XXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXX 9.60*10^ 2 XXX XXXXXXXXXX XXX X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXX 9.56*10^ 2 XXXXXXXXXXXXXX XXX X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5XXXXXXXXX 9.52*10^ 2 XXXXXXXXXXXXXX XXX3X8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 9.48*10^ 2 XXXXXXXXXXXXXX3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 9.44*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 3 1110000101001001010001010001111101101001000110111000000111000110010000111101111111110010110100101111 *10^ 2 0009999090990990909990909990000090090990999009000999999000999009909999000090000000009909009099090000 *10^ 1 1305698081783841604853949771421381563663689007461767477212978156906788323191403211008809105387592142 *10^ 0 3416629027104058499010447875385258322406404566833409442610023330154523286167003350716741014056362462 Low edge *10^-1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-2 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 100000 Mean = 5.0146e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+05 Rms = 2.8882e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:07 standard random number correlation 2.00*10^ 3 746 1.92*10^ 3 XXXXX55 1 1.84*10^ 3 XXXXXXXX74X 1.76*10^ 3 XXXXXXXXXXX636 1.68*10^ 3 XXXXXXXXXXXXXX9X669 1.60*10^ 3 XXXXXXXXXXXXXXXXXXX47582 1.52*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXX311 2 1.44*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXX4X43121 1.36*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 1.28*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX667 1.20*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9695 1 1.12*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7X2371 1 1.04*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX1X 0.96*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX64863 4 0.88*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6X47 0.80*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX494263 0.72*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 0.64*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX939611 0.56*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX53 0 0.48*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX88X 2 0.40*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX98532 0.32*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7733 0.24*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX32 0.16*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX99833 0.08*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9552 Contents *10^ 3 1111111111111111111111111111111111111111111111111010000000000000000000000000000000000000000000000000 *10^ 2 9999988887877766666555554443433333322221111010000909999989887777776656655554443433333222211111110000 *10^ 1 7562187419420267546576836459598677484559796925694752142041355943646382176206689188543996687544007331 *10^ 0 3183818230886697279182146814835552308155130977125108365491293184657179015433548496967582136292655798 Low edge *10^-1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-2 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 100000 Mean = 3.3483e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+05 Rms = 2.3638e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:07 stupid random number distribution 10.70*10^ 2 6 10.65*10^ 2 X 10.60*10^ 2 4 X 10.55*10^ 2 X 8 2 X 10.50*10^ 2 X 6 X X X 6 X X 10.45*10^ 2 X X X X X X X X X 10.40*10^ 2 X X X 8 X X X X X X 10.35*10^ 2 X X 2 XX X4 X X X X X X X 4 X 10.30*10^ 2 X X 8 4X XX XX X X X X 4 X 6 X8 X X 2 8 6 2 X 10.25*10^ 2 X X X XX XX XX X X X 2 2X X X X XX 6X X X X X X X 10.20*10^ 2 X X X XX XX XX 8 X X X X XX X4 X X XX XX X X X4X 2XX X X 10.15*10^ 2 X X XX4XX XX XX X X2 X X X XX XX 6 X X XX XX X X XXX XXX X X 10.10*10^ 2 X X X XXXXX XX XX X XX X X X XX XX X 6X X XX XX6 X XX XXX XXX X X 10.05*10^ 2 X X 6 X XXXXXXXX XX X XX X X X XX XX X XX X 6 4 X2 8XX XXX X2 2 XX XXX XXX X 4X 10.00*10^ 2 X X X X XXXXXXXX XX X XX X X X XX XX X XX 4X X X XXX XXX XXX XX X XX XXX XXX 4 X XX 9.95*10^ 2 2 8X X X4X8 2 XXXXXXXXXXX X XX X X X 4XX XX X X XX XX X X XXX XXX XXX XX X XX XXX XXX X X2XX 9.90*10^ 2 X XX64X XXXX X XXXXXXXXXXX X XX X X X2 XXXXXX X X XX2XX X X XXX XXX XXX XX2X XXXXXX XXX X XXXX 9.85*10^ 2 X XXXXX XXXX X XXXXXXXXXXX X4XX X6X XX XXXXXX X X XXXXX X4 X XXX XXX XXX XXXX XXXXXX XXX X XXXX 9.80*10^ 2 X XXXXX XXXX8X XXXXXXXXXXX XXXX XXX XX XXXXXX8X X XXXXX XX X XXX XXX8 XXX XXXX XXXXXX XXX X6XXXX 9.75*10^ 2 X XXXXX XXXXXX8XXXXXXXXXXX XXXX XXX XX XXXXXXXX X XXXXX XX X XXX XXXX XXX XXXX XXXXXX XXX XXXXXX 9.70*10^ 2 X XXXXX XXXXXXXXXXXXXXXXXX XXXX XXX XX XXXXXXXX X XXXXX XX X4XXX XXXX XXX8XXXX XXXXXX4XXX XXXXXX 9.65*10^ 2 X XXXXX XXXXXXXXXXXXXXXXXX XXXX XXX8XX XXXXXXXX 8X XXXXX2 XXXXXXXX8XXXX XXXXXXXX XXXXXXXXXX XXXXXX 9.60*10^ 2 X4XXXXX XXXXXXXXXXXXXXXXXX XXXX2XXXXXXX XXXXXXXX XX XXXXXX XXXXXXXXXXXXX XXXXXXXX XXXXXXXXXX6XXXXXX 9.55*10^ 2 XXXXXXX6XXXXXXXXXXXXXXXXXX XXXXXXXXXXXX4XXXXXXXX6XX XXXXXX4XXXXXXXXXXXXX XXXXXXXX XXXXXXXXXXXXXXXXXX 9.50*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXX 9.45*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXX 9.40*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXX6XXXXXXXXXXXXXXXXXXXXXXXX8XXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXX 9.35*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2XXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 3 0001001010100001111111101101011001010100011011010000110010010010111011100111011010110111011100010110 *10^ 2 9990990909099990000000090090900990909099900900909999009909909909000900099000900909009000900099909009 *10^ 1 9594885509197972112303493331851565866285924921715693038906508606020603273250630805219212612259729055 *10^ 0 1745877332049149527155859289241601384162218077933459856751232527081445991308921610000679768087861205 Low edge *10^-1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-2 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 100000 Mean = 4.9964e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+05 Rms = 2.8886e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:07 stupid random number correlation 2.08*10^ 3 9 2.00*10^ 3 X8 33 1.92*10^ 3 XX9XX43 1.84*10^ 3 XXXXXXX864 4 1.76*10^ 3 XXXXXXXXXXX X3535 1 1.68*10^ 3 XXXXXXXXXXXXXXXXX5X733 1.60*10^ 3 XXXXXXXXXXXXXXXXXXXXXX8 6 1.52*10^ 3 XXXXXXXXXXXXXXXXXXXXXXX8X9 1.44*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXX7X98 1.36*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX38631 1.28*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX235 21 1.20*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6XX2 1.12*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8222 1.04*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7215 0.96*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX82 0.88*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX97 418 0.80*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8XXX9 0.72*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7968 1 0.64*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9X7722 0.56*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX652 0.48*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9614 0.40*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX44 0.32*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX97644 0.24*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8561 0.16*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX531 0.08*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX531 Contents *10^ 3 2111111111111111111111111111111111111111111111111000000000000000000000000000000000000000000000000000 *10^ 2 0999988887767777766666555544443333322222122110000999998887888767676666655554444433333222212111100000 *10^ 1 6814476208589020138522806114326042087124710305551769549758206991803341177229740395510876290661087420 *10^ 0 9441454058904537965526548372423279398921148458955979978051867024706365654833197572230539385636556226 Low edge *10^-1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-2 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 100000 Mean = 3.3274e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+05 Rms = 2.3547e-01 Overflow = 0.0000e+00 High edge = 1.0000e+00 pythia8-8.1.80.orig/examples/outref/out210000644000175000017500000037744012217346174016376 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:06:29 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberShowEvent | 0 | 1 0 | | Next:numberShowInfo | 0 | 1 0 | | Next:numberShowProcess | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | ProcessLevel:all | off | on | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | Standalone:allowResDec | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 125.000 125.000 1 25 (h0(H_1)) -22 0 0 2 3 0 0 0.000 0.000 -0.000 125.000 125.000 2 5 (b) -23 1 0 4 5 101 0 9.619 44.029 -43.036 62.500 4.800 3 -5 (bbar) -23 1 0 6 6 0 101 -9.619 -44.029 43.036 62.500 4.800 4 5 (b) -51 2 0 9 9 103 0 12.291 44.095 -33.839 57.128 4.800 5 21 (g) -51 2 0 7 8 101 103 -3.104 -2.042 -7.266 8.161 0.000 6 -5 (bbar) -52 3 3 12 12 0 101 -9.188 -42.053 41.105 59.712 4.800 7 2 (u) -51 5 0 10 11 101 0 3.549 -1.325 -0.290 3.814 0.330 8 -2 (ubar) -51 5 0 18 18 0 103 -2.868 12.640 -17.013 21.390 0.330 9 5 (b) -52 4 4 16 17 103 0 8.506 30.737 -23.802 40.084 4.800 10 2 (u) -51 7 0 15 15 106 0 2.734 0.087 -0.066 2.756 0.330 11 21 (g) -51 7 0 13 14 101 106 0.437 -3.070 1.404 3.404 0.000 12 -5 (bbar) -52 6 6 30 30 0 101 -8.809 -40.394 39.477 57.365 4.800 13 21 (g) -51 11 0 21 21 101 107 -0.246 -1.898 1.433 2.390 0.000 14 21 (g) -51 11 0 19 20 107 106 1.797 -1.115 -0.065 2.116 0.000 15 2 (u) -52 10 10 32 0 106 0 1.620 0.030 -0.029 1.653 0.330 16 5 (b) -51 9 0 33 36 108 0 8.616 30.887 -24.300 40.519 4.800 17 21 (g) -51 9 0 33 36 103 108 -0.291 0.644 -0.573 0.910 0.000 18 -2 (ubar) -52 8 8 33 36 0 103 -2.687 11.846 -15.943 20.045 0.330 19 21 (g) -51 14 0 24 24 109 106 1.856 -1.469 0.523 2.424 0.000 20 21 (g) -51 14 0 22 23 107 109 -0.120 -0.118 -0.232 0.287 0.000 21 21 (g) -52 13 13 25 26 101 107 -0.185 -1.426 1.076 1.796 0.000 22 21 (g) -51 20 0 27 27 107 110 0.792 -0.825 0.658 1.320 0.000 23 21 (g) -51 20 0 38 38 110 109 0.503 -0.413 -0.491 0.815 0.000 24 21 (g) -52 19 19 32 0 109 106 0.441 -0.349 0.124 0.576 0.000 25 21 (g) -51 21 0 28 29 101 112 -0.088 -1.207 0.446 1.289 0.000 26 21 (g) -51 21 0 31 0 112 107 0.426 -0.765 1.065 1.379 0.000 27 21 (g) -52 22 22 31 0 107 110 0.269 -0.280 0.223 0.448 0.000 28 21 (g) -51 25 0 40 40 113 112 -0.816 -2.526 2.096 3.382 0.000 29 21 (g) -51 25 0 41 41 101 113 0.219 -0.848 0.621 1.074 0.000 30 -5 (bbar) -52 12 12 42 42 0 101 -8.300 -38.227 37.206 54.199 4.800 31 21 (g) -73 26 27 39 39 112 110 0.695 -1.044 1.288 1.826 0.319 32 2 (u) -73 15 24 37 37 109 0 2.060 -0.319 0.095 2.229 0.783 33 -523 (B*-) -83 16 18 55 56 0 0 7.951 29.422 -23.162 38.649 5.325 34 223 (omega) -83 16 18 57 59 0 0 -0.436 4.586 -5.151 6.955 0.785 35 223 (omega) -83 16 18 60 62 0 0 -0.362 1.653 -2.256 2.931 0.798 36 223 (omega) -84 16 18 63 65 0 0 -1.515 7.717 -10.246 12.940 0.788 37 2 (u) -71 32 32 43 48 109 0 2.060 -0.319 0.095 2.229 0.783 38 21 (g) -71 23 23 43 48 110 109 0.503 -0.413 -0.491 0.815 0.000 39 21 (g) -71 31 31 43 48 112 110 0.695 -1.044 1.288 1.826 0.319 40 21 (g) -71 28 28 43 48 113 112 -0.816 -2.526 2.096 3.382 0.000 41 21 (g) -71 29 29 43 48 101 113 0.219 -0.848 0.621 1.074 0.000 42 -5 (bbar) -71 30 30 43 48 0 101 -8.300 -38.227 37.206 54.199 4.800 43 113 (rho0) -83 37 42 49 50 0 0 1.504 -0.208 -0.170 1.686 0.714 44 213 (rho+) -83 37 42 51 52 0 0 1.079 -0.409 0.204 1.378 0.725 45 113 (rho0) -83 37 42 53 54 0 0 -0.038 -0.410 0.299 0.845 0.675 46 111 (pi0) -83 37 42 66 67 0 0 0.522 -1.143 1.060 1.650 0.135 47 111 (pi0) -84 37 42 68 69 0 0 -0.425 -2.431 1.906 3.121 0.135 48 513 (B*0) -84 37 42 70 71 0 0 -8.281 -38.776 37.517 54.845 5.325 49 211 pi+ 91 43 0 0 0 0 0 0.058 0.052 -0.137 0.210 0.140 50 -211 pi- 91 43 0 0 0 0 0 1.446 -0.260 -0.033 1.476 0.140 51 211 pi+ 91 44 0 0 0 0 0 1.071 -0.305 0.014 1.123 0.140 52 111 (pi0) -91 44 0 72 73 0 0 0.008 -0.104 0.190 0.255 0.135 53 211 pi+ 91 45 0 0 0 0 0 -0.254 -0.097 0.315 0.439 0.140 54 -211 pi- 91 45 0 0 0 0 0 0.217 -0.313 -0.016 0.406 0.140 55 -521 (B-) -91 33 0 74 76 0 0 7.944 29.383 -23.095 38.571 5.279 56 22 gamma 91 33 0 0 0 0 0 0.008 0.040 -0.067 0.078 0.000 57 211 pi+ 91 34 0 0 0 0 0 -0.141 1.258 -1.310 1.827 0.140 58 -211 pi- 91 34 0 0 0 0 0 -0.295 3.180 -3.628 4.836 0.140 59 111 (pi0) -91 34 0 77 78 0 0 -0.001 0.147 -0.213 0.292 0.135 60 211 pi+ 91 35 0 0 0 0 0 -0.122 0.197 -0.116 0.294 0.140 61 -211 pi- 91 35 0 0 0 0 0 -0.139 0.349 -0.761 0.860 0.140 62 111 (pi0) -91 35 0 79 80 0 0 -0.101 1.106 -1.379 1.776 0.135 63 211 pi+ 91 36 0 0 0 0 0 -0.441 1.727 -2.133 2.783 0.140 64 -211 pi- 91 36 0 0 0 0 0 -1.054 5.523 -7.468 9.349 0.140 65 111 (pi0) -91 36 0 81 82 0 0 -0.020 0.467 -0.645 0.808 0.135 66 22 gamma 91 46 0 0 0 0 0 0.236 -0.534 0.580 0.823 0.000 67 22 gamma 91 46 0 0 0 0 0 0.286 -0.610 0.480 0.827 0.000 68 22 gamma 91 47 0 0 0 0 0 -0.149 -0.527 0.420 0.690 0.000 69 22 gamma 91 47 0 0 0 0 0 -0.276 -1.904 1.486 2.431 0.000 70 511 (B0) -91 48 0 83 85 0 0 -8.156 -38.170 36.901 53.973 5.280 71 22 gamma 91 48 0 0 0 0 0 -0.125 -0.605 0.615 0.872 0.000 72 22 gamma 91 52 0 0 0 0 0 0.052 -0.106 0.169 0.206 0.000 73 22 gamma 91 52 0 0 0 0 0 -0.044 0.002 0.020 0.049 0.000 74 -12 nu_ebar 91 55 0 0 0 0 0 2.890 10.038 -6.939 12.541 0.000 75 11 e- 91 55 0 0 0 0 0 1.631 3.172 -4.058 5.403 0.001 76 10423 (D_10) -91 55 0 86 87 0 0 3.423 16.172 -12.099 20.628 2.422 77 22 gamma 91 59 0 0 0 0 0 -0.067 0.080 -0.125 0.163 0.000 78 22 gamma 91 59 0 0 0 0 0 0.066 0.067 -0.088 0.129 0.000 79 22 gamma 91 62 0 0 0 0 0 0.008 0.015 -0.004 0.018 0.000 80 22 gamma 91 62 0 0 0 0 0 -0.109 1.091 -1.374 1.758 0.000 81 22 gamma 91 65 0 0 0 0 0 -0.034 0.030 -0.096 0.106 0.000 82 22 gamma 91 65 0 0 0 0 0 0.014 0.437 -0.549 0.702 0.000 83 12 nu_e 91 70 0 0 0 0 0 -0.853 -6.345 4.137 7.622 0.000 84 -11 e+ 91 70 0 0 0 0 0 -0.693 -4.047 5.464 6.835 0.001 85 -213 (rho-) -91 70 0 88 89 0 0 -6.610 -27.779 27.300 39.516 0.928 86 413 (D*+) -91 76 0 90 91 0 0 2.323 12.200 -9.251 15.616 2.010 87 -211 pi- 91 76 0 0 0 0 0 1.100 3.972 -2.848 5.012 0.140 88 -211 pi- 91 85 0 0 0 0 0 -1.406 -4.823 5.091 7.154 0.140 89 111 (pi0) -91 85 0 92 93 0 0 -5.205 -22.956 22.209 32.362 0.135 90 421 (D0) -91 86 0 94 96 0 0 2.110 11.122 -8.462 14.256 1.865 91 211 pi+ 91 86 0 0 0 0 0 0.213 1.078 -0.789 1.360 0.140 92 22 gamma 91 89 0 0 0 0 0 -0.707 -3.095 3.058 4.408 0.000 93 22 gamma 91 89 0 0 0 0 0 -4.498 -19.861 19.151 27.954 0.000 94 -321 K- 91 90 0 0 0 0 0 2.099 10.050 -7.821 12.916 0.494 95 211 pi+ 91 90 0 0 0 0 0 0.005 0.873 -0.323 0.941 0.140 96 111 (pi0) -91 90 0 97 98 0 0 0.006 0.199 -0.318 0.398 0.135 97 22 gamma 91 96 0 0 0 0 0 0.002 -0.020 -0.039 0.044 0.000 98 22 gamma 91 96 0 0 0 0 0 0.004 0.219 -0.279 0.354 0.000 Charge sum: 0.000 Momentum sum: -0.000 -0.000 0.000 125.000 125.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Junction Listing (complete event) ------------ no kind col0 col1 col2 endc0 endc1 endc2 stat0 stat1 stat2 no junctions present -------- End PYTHIA Junction Listing -------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 124.978 124.978 1 25 (h0(H_1)) -22 0 0 2 3 0 0 -0.000 -0.000 0.000 124.978 124.978 2 5 (b) -23 1 0 4 5 101 0 30.059 -53.927 -8.378 62.489 4.800 3 -5 (bbar) -23 1 0 6 6 0 101 -30.059 53.927 8.378 62.489 4.800 4 5 (b) -51 2 0 12 12 102 0 22.189 -25.598 -17.970 38.647 4.800 5 21 (g) -51 2 0 9 9 101 102 6.026 -25.022 10.106 27.650 0.000 6 -5 (bbar) -52 3 3 7 8 0 101 -28.216 50.620 7.865 58.680 4.800 7 -5 (bbar) -51 6 0 21 21 0 103 -24.347 46.335 15.459 54.788 4.800 8 21 (g) -51 6 0 16 17 103 101 -3.143 1.271 -6.377 7.222 0.000 9 21 (g) -52 5 5 10 11 101 102 5.301 -22.008 8.889 24.320 0.000 10 3 (s) -51 9 0 18 18 101 0 2.509 -9.317 -7.209 12.055 0.500 11 -3 (sbar) -51 9 0 15 15 0 102 10.772 -21.485 9.293 25.773 0.500 12 5 (b) -52 4 4 13 14 102 0 14.209 -16.804 -11.166 25.140 4.800 13 5 (b) -51 12 0 60 60 104 0 14.358 -17.796 -9.642 25.276 4.800 14 21 (g) -51 12 0 22 23 102 104 0.381 -0.067 -1.065 1.133 0.000 15 -3 (sbar) -52 11 11 24 24 0 102 10.241 -20.427 8.834 24.504 0.500 16 21 (g) -51 8 0 19 20 103 105 -0.257 0.332 -6.200 6.214 0.000 17 21 (g) -51 8 0 30 30 105 101 -2.500 -0.489 -1.277 2.849 0.000 18 3 (s) -52 10 10 54 54 101 0 2.123 -7.890 -6.110 10.214 0.500 19 21 (g) -51 16 0 27 27 106 105 1.742 0.460 -3.375 3.826 0.000 20 21 (g) -51 16 0 25 26 103 106 -2.581 0.979 -2.447 3.689 0.000 21 -5 (bbar) -52 7 7 39 39 0 103 -23.765 45.228 15.081 53.487 4.800 22 21 (g) -51 14 0 31 32 108 104 2.190 -0.717 -0.293 2.323 0.000 23 21 (g) -51 14 0 33 33 102 108 -0.254 -2.450 0.571 2.529 0.000 24 -3 (sbar) -52 15 15 34 35 0 102 8.687 -17.326 7.492 20.786 0.500 25 21 (g) -51 20 0 37 38 103 109 -1.113 -0.412 -3.297 3.504 0.000 26 21 (g) -51 20 0 49 50 109 106 -0.710 1.591 -0.618 1.849 0.000 27 21 (g) -52 19 19 28 29 106 105 0.984 0.260 -1.907 2.162 0.000 28 21 (g) -51 27 0 51 51 106 112 0.218 0.390 -2.770 2.806 0.000 29 21 (g) -51 27 0 80 80 112 105 -0.276 -0.333 0.330 0.544 0.000 30 21 (g) -52 17 17 52 53 105 101 -1.457 -0.285 -0.744 1.661 0.000 31 21 (g) -51 22 0 46 47 114 104 1.728 -0.154 0.140 1.741 0.000 32 21 (g) -51 22 0 48 48 108 114 0.356 -1.576 -0.198 1.627 0.000 33 21 (g) -52 23 23 36 36 102 108 -0.149 -1.437 0.335 1.483 0.000 34 -3 (sbar) -51 24 0 69 69 0 117 8.396 -16.297 7.175 19.693 0.500 35 21 (g) -51 24 0 62 0 117 102 0.243 -1.490 0.424 1.568 0.000 36 21 (g) -52 33 33 62 0 102 108 -0.101 -0.976 0.227 1.007 0.000 37 21 (g) -51 25 0 43 44 118 109 -1.175 -0.844 -2.069 2.524 0.000 38 21 (g) -51 25 0 40 41 103 118 -0.104 0.748 -1.120 1.351 0.000 39 -5 (bbar) -52 21 21 42 42 0 103 -23.600 44.912 14.973 53.116 4.800 40 21 (g) -51 38 0 45 45 119 118 -0.572 1.772 -1.294 2.267 0.000 41 21 (g) -51 38 0 87 87 103 119 -0.546 0.894 0.840 1.343 0.000 42 -5 (bbar) -52 39 39 88 88 0 103 -22.587 42.994 14.308 50.857 4.800 43 21 (g) -51 37 0 84 84 120 109 -1.397 0.233 -1.843 2.324 0.000 44 21 (g) -51 37 0 85 85 118 120 0.063 -0.585 -0.585 0.830 0.000 45 21 (g) -52 40 40 86 86 119 118 -0.413 1.279 -0.935 1.637 0.000 46 21 (g) -51 31 0 58 59 121 104 1.562 -1.142 0.152 1.941 0.000 47 21 (g) -51 31 0 66 66 114 121 0.313 0.338 -0.093 0.470 0.000 48 21 (g) -52 32 32 67 67 108 114 0.210 -0.926 -0.116 0.957 0.000 49 21 (g) -51 26 0 83 83 109 122 -0.953 0.873 -0.551 1.405 0.000 50 21 (g) -51 26 0 55 56 122 106 0.300 0.821 -0.796 1.182 0.000 51 21 (g) -52 28 28 57 57 106 112 0.161 0.287 -2.041 2.067 0.000 52 21 (g) -51 30 0 79 79 105 123 -0.631 0.263 -0.192 0.710 0.000 53 21 (g) -51 30 0 78 78 123 101 -0.716 -0.951 -0.864 1.471 0.000 54 3 (s) -52 18 18 77 77 101 0 2.013 -7.487 -5.798 9.694 0.500 55 21 (g) -51 50 0 82 82 122 125 0.033 1.038 -1.752 2.037 0.000 56 21 (g) -51 50 0 61 0 125 106 0.386 -0.004 -0.553 0.674 0.000 57 21 (g) -52 51 51 61 0 106 112 0.042 0.075 -0.532 0.538 0.000 58 21 (g) -51 46 0 65 65 121 126 1.861 -1.303 -0.511 2.328 0.000 59 21 (g) -51 46 0 64 64 126 104 0.225 -0.621 0.111 0.670 0.000 60 5 (b) -52 13 13 63 63 104 0 13.834 -17.014 -9.090 24.219 4.800 61 21 (g) -73 56 57 81 81 125 112 0.428 0.070 -1.085 1.213 0.326 62 21 (g) -73 35 36 68 68 117 108 0.142 -2.466 0.651 2.575 0.327 63 5 (b) -71 60 60 70 76 104 0 13.834 -17.014 -9.090 24.219 4.800 64 21 (g) -71 59 59 70 76 126 104 0.225 -0.621 0.111 0.670 0.000 65 21 (g) -71 58 58 70 76 121 126 1.861 -1.303 -0.511 2.328 0.000 66 21 (g) -71 47 47 70 76 114 121 0.313 0.338 -0.093 0.470 0.000 67 21 (g) -71 48 48 70 76 108 114 0.210 -0.926 -0.116 0.957 0.000 68 21 (g) -71 62 62 70 76 117 108 0.142 -2.466 0.651 2.575 0.327 69 -3 (sbar) -71 34 34 70 76 0 117 8.396 -16.297 7.175 19.693 0.500 70 5122 (Lambda_b0) -83 63 69 113 115 0 0 13.680 -16.819 -8.371 23.909 5.619 71 111 (pi0) -83 63 69 116 117 0 0 2.402 -1.050 -1.266 2.914 0.135 72 -2212 pbar- 84 63 69 0 0 0 0 0.856 -2.652 0.722 3.027 0.938 73 323 (K*+) -84 63 69 103 104 0 0 1.411 -3.638 1.058 4.142 0.900 74 -321 K- 84 63 69 0 0 0 0 0.346 -1.301 0.625 1.565 0.494 75 111 (pi0) -84 63 69 118 119 0 0 0.067 -0.237 -0.070 0.290 0.135 76 321 K+ 84 63 69 0 0 0 0 6.220 -12.592 5.429 15.065 0.494 77 3 (s) -71 54 54 89 102 101 0 2.013 -7.487 -5.798 9.694 0.500 78 21 (g) -71 53 53 89 102 123 101 -0.716 -0.951 -0.864 1.471 0.000 79 21 (g) -71 52 52 89 102 105 123 -0.631 0.263 -0.192 0.710 0.000 80 21 (g) -71 29 29 89 102 112 105 -0.276 -0.333 0.330 0.544 0.000 81 21 (g) -71 61 61 89 102 125 112 0.428 0.070 -1.085 1.213 0.326 82 21 (g) -71 55 55 89 102 122 125 0.033 1.038 -1.752 2.037 0.000 83 21 (g) -71 49 49 89 102 109 122 -0.953 0.873 -0.551 1.405 0.000 84 21 (g) -71 43 43 89 102 120 109 -1.397 0.233 -1.843 2.324 0.000 85 21 (g) -71 44 44 89 102 118 120 0.063 -0.585 -0.585 0.830 0.000 86 21 (g) -71 45 45 89 102 119 118 -0.413 1.279 -0.935 1.637 0.000 87 21 (g) -71 41 41 89 102 103 119 -0.546 0.894 0.840 1.343 0.000 88 -5 (bbar) -71 42 42 89 102 0 103 -22.587 42.994 14.308 50.857 4.800 89 -323 (K*-) -83 77 88 105 106 0 0 1.838 -6.705 -5.102 8.698 1.138 90 211 pi+ 83 77 88 0 0 0 0 -0.330 -0.934 -0.760 1.256 0.140 91 313 (K*0) -83 77 88 107 108 0 0 -0.425 -0.776 -0.758 1.437 0.840 92 -321 K- 83 77 88 0 0 0 0 0.024 0.194 -0.803 0.963 0.494 93 211 pi+ 83 77 88 0 0 0 0 -0.165 -0.506 0.174 0.577 0.140 94 223 (omega) -84 77 88 120 121 0 0 -0.356 0.957 -1.455 1.940 0.779 95 -211 pi- 84 77 88 0 0 0 0 -0.455 0.719 -0.307 0.915 0.140 96 211 pi+ 84 77 88 0 0 0 0 -0.295 -0.305 -0.485 0.660 0.140 97 223 (omega) -84 77 88 122 124 0 0 0.147 0.333 -1.268 1.531 0.777 98 2112 n0 84 77 88 0 0 0 0 -1.320 0.676 -1.638 2.401 0.940 99 221 (eta) -84 77 88 125 127 0 0 -0.960 0.578 -0.140 1.255 0.548 100 -2114 (Deltabar0) -84 77 88 109 110 0 0 -0.794 2.658 0.621 3.161 1.381 101 -211 pi- 84 77 88 0 0 0 0 -0.390 0.471 -0.227 0.667 0.140 102 523 (B*+) -84 77 88 128 129 0 0 -21.499 40.930 14.021 48.605 5.325 103 311 (K0) -91 73 0 111 111 0 0 0.630 -2.413 0.608 2.615 0.498 104 211 pi+ 91 73 0 0 0 0 0 0.781 -1.225 0.450 1.527 0.140 105 -311 (Kbar0) -91 89 0 112 112 0 0 0.512 -3.192 -2.670 4.222 0.498 106 -211 pi- 91 89 0 0 0 0 0 1.327 -3.513 -2.432 4.476 0.140 107 321 K+ 91 91 0 0 0 0 0 -0.463 -0.567 -0.338 0.945 0.494 108 -211 pi- 91 91 0 0 0 0 0 0.037 -0.209 -0.421 0.492 0.140 109 -2112 nbar0 91 100 0 0 0 0 0 -0.446 2.418 0.663 2.715 0.940 110 111 (pi0) -91 100 0 130 131 0 0 -0.349 0.240 -0.042 0.446 0.135 111 130 K_L0 91 103 103 0 0 0 0 0.630 -2.413 0.608 2.615 0.498 112 310 (K_S0) -91 105 105 132 133 0 0 0.512 -3.192 -2.670 4.222 0.498 113 -311 (Kbar0) -91 70 0 134 134 0 0 2.251 -2.418 -0.249 3.350 0.498 114 -413 (D*-) -91 70 0 135 136 0 0 5.989 -7.321 -4.070 10.491 2.010 115 4122 (Lambda_c+) -91 70 0 137 140 0 0 5.440 -7.080 -4.052 10.068 2.286 116 22 gamma 91 71 0 0 0 0 0 1.012 -0.506 -0.509 1.240 0.000 117 22 gamma 91 71 0 0 0 0 0 1.391 -0.544 -0.757 1.674 0.000 118 22 gamma 91 75 0 0 0 0 0 0.058 -0.251 -0.049 0.263 0.000 119 22 gamma 91 75 0 0 0 0 0 0.009 0.014 -0.021 0.027 0.000 120 111 (pi0) -91 94 0 141 142 0 0 -0.485 0.250 -0.569 0.800 0.135 121 22 gamma 91 94 0 0 0 0 0 0.129 0.706 -0.886 1.140 0.000 122 211 pi+ 91 97 0 0 0 0 0 0.237 -0.046 -0.717 0.769 0.140 123 -211 pi- 91 97 0 0 0 0 0 -0.087 0.278 -0.481 0.580 0.140 124 111 (pi0) -91 97 0 143 144 0 0 -0.003 0.100 -0.070 0.182 0.135 125 211 pi+ 91 99 0 0 0 0 0 -0.207 0.267 -0.019 0.366 0.140 126 -211 pi- 91 99 0 0 0 0 0 -0.508 0.236 -0.006 0.578 0.140 127 111 (pi0) -91 99 0 145 146 0 0 -0.245 0.075 -0.116 0.311 0.135 128 521 (B+) -91 102 0 147 149 0 0 -21.172 40.378 13.844 47.939 5.279 129 22 gamma 91 102 0 0 0 0 0 -0.327 0.553 0.177 0.666 0.000 130 22 gamma 91 110 0 0 0 0 0 -0.329 0.257 -0.047 0.420 0.000 131 22 gamma 91 110 0 0 0 0 0 -0.020 -0.017 0.005 0.026 0.000 132 211 pi+ 91 112 0 0 0 0 0 0.429 -1.479 -1.366 2.064 0.140 133 -211 pi- 91 112 0 0 0 0 0 0.082 -1.713 -1.304 2.158 0.140 134 130 K_L0 91 113 113 0 0 0 0 2.251 -2.418 -0.249 3.350 0.498 135 -421 (Dbar0) -91 114 0 150 154 0 0 5.636 -6.835 -3.806 9.821 1.865 136 -211 pi- 91 114 0 0 0 0 0 0.353 -0.487 -0.264 0.671 0.140 137 -11 e+ 91 115 0 0 0 0 0 0.743 -1.568 -0.848 1.931 0.001 138 12 nu_e 91 115 0 0 0 0 0 1.742 -1.704 -1.157 2.697 0.000 139 2112 n0 91 115 0 0 0 0 0 1.738 -2.875 -1.248 3.705 0.940 140 111 (pi0) -91 115 0 155 156 0 0 1.218 -0.933 -0.798 1.735 0.135 141 22 gamma 91 120 0 0 0 0 0 -0.110 0.102 -0.095 0.177 0.000 142 22 gamma 91 120 0 0 0 0 0 -0.375 0.148 -0.474 0.623 0.000 143 22 gamma 91 124 0 0 0 0 0 -0.059 0.059 -0.000 0.084 0.000 144 22 gamma 91 124 0 0 0 0 0 0.056 0.041 -0.070 0.099 0.000 145 22 gamma 91 127 0 0 0 0 0 -0.238 0.034 -0.072 0.251 0.000 146 22 gamma 91 127 0 0 0 0 0 -0.006 0.041 -0.044 0.060 0.000 147 -423 (D*bar0) -91 128 0 157 158 0 0 -16.530 28.646 9.678 34.519 2.007 148 221 (eta) -91 128 0 159 161 0 0 -3.628 9.184 3.008 10.338 0.548 149 213 (rho+) -91 128 0 162 163 0 0 -1.014 2.547 1.157 3.083 0.805 150 -311 (Kbar0) -91 135 0 164 164 0 0 1.219 -1.405 -0.652 2.033 0.498 151 -211 pi- 91 135 0 0 0 0 0 0.338 -0.352 -0.124 0.522 0.140 152 211 pi+ 91 135 0 0 0 0 0 1.415 -1.381 -1.071 2.253 0.140 153 111 (pi0) -91 135 0 165 166 0 0 1.036 -1.882 -0.691 2.261 0.135 154 111 (pi0) -91 135 0 167 168 0 0 1.628 -1.814 -1.268 2.751 0.135 155 22 gamma 91 140 0 0 0 0 0 0.758 -0.548 -0.554 1.087 0.000 156 22 gamma 91 140 0 0 0 0 0 0.460 -0.385 -0.244 0.648 0.000 157 -421 (Dbar0) -91 147 0 169 170 0 0 -14.299 24.869 8.413 29.953 1.865 158 22 gamma 91 147 0 0 0 0 0 -2.231 3.778 1.266 4.566 0.000 159 111 (pi0) -91 148 0 171 172 0 0 -0.680 2.011 0.583 2.206 0.135 160 111 (pi0) -91 148 0 173 174 0 0 -1.948 4.569 1.573 5.212 0.135 161 111 (pi0) -91 148 0 175 176 0 0 -1.001 2.604 0.852 2.920 0.135 162 211 pi+ 91 149 0 0 0 0 0 -0.773 1.325 0.313 1.572 0.140 163 111 (pi0) -91 149 0 177 178 0 0 -0.241 1.222 0.844 1.511 0.135 164 130 K_L0 91 150 150 0 0 0 0 1.219 -1.405 -0.652 2.033 0.498 165 22 gamma 91 153 0 0 0 0 0 0.890 -1.562 -0.622 1.902 0.000 166 22 gamma 91 153 0 0 0 0 0 0.147 -0.321 -0.069 0.359 0.000 167 22 gamma 91 154 0 0 0 0 0 0.689 -0.718 -0.453 1.094 0.000 168 22 gamma 91 154 0 0 0 0 0 0.939 -1.096 -0.815 1.657 0.000 169 323 (K*+) -91 157 0 179 180 0 0 -8.920 15.418 5.207 18.580 0.908 170 -213 (rho-) -91 157 0 181 182 0 0 -5.379 9.451 3.206 11.372 0.900 171 22 gamma 91 159 0 0 0 0 0 -0.477 1.366 0.460 1.518 0.000 172 22 gamma 91 159 0 0 0 0 0 -0.203 0.646 0.123 0.688 0.000 173 22 gamma 91 160 0 0 0 0 0 -1.078 2.419 0.893 2.795 0.000 174 22 gamma 91 160 0 0 0 0 0 -0.870 2.150 0.680 2.417 0.000 175 22 gamma 91 161 0 0 0 0 0 -0.733 1.966 0.697 2.211 0.000 176 22 gamma 91 161 0 0 0 0 0 -0.268 0.638 0.155 0.709 0.000 177 22 gamma 91 163 0 0 0 0 0 -0.235 1.188 0.788 1.445 0.000 178 22 gamma 91 163 0 0 0 0 0 -0.006 0.034 0.056 0.066 0.000 179 311 (K0) -91 169 0 183 183 0 0 -7.026 11.603 3.905 14.124 0.498 180 211 pi+ 91 169 0 0 0 0 0 -1.895 3.815 1.301 4.456 0.140 181 -211 pi- 91 170 0 0 0 0 0 -2.683 3.869 1.458 4.930 0.140 182 111 (pi0) -91 170 0 184 185 0 0 -2.696 5.582 1.748 6.442 0.135 183 310 (K_S0) -91 179 179 186 187 0 0 -7.026 11.603 3.905 14.124 0.498 184 22 gamma 91 182 0 0 0 0 0 -1.540 3.038 0.946 3.535 0.000 185 22 gamma 91 182 0 0 0 0 0 -1.156 2.544 0.802 2.907 0.000 186 211 pi+ 91 183 0 0 0 0 0 -5.488 8.757 2.961 10.751 0.140 187 -211 pi- 91 183 0 0 0 0 0 -1.538 2.847 0.944 3.373 0.140 Charge sum: 0.000 Momentum sum: 0.000 -0.000 -0.000 124.978 124.978 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Junction Listing (complete event) ------------ no kind col0 col1 col2 endc0 endc1 endc2 stat0 stat1 stat2 no junctions present -------- End PYTHIA Junction Listing -------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 124.999 124.999 1 25 (h0(H_1)) -22 0 0 2 3 0 0 0.000 -0.000 -0.000 124.999 124.999 2 21 (g) -23 1 0 6 6 101 102 48.989 21.008 32.633 62.499 0.000 3 21 (g) -23 1 0 4 5 102 101 -48.989 -21.008 -32.633 62.499 0.000 4 21 (g) -51 3 0 7 8 103 101 -33.990 -21.150 -34.446 52.813 0.000 5 21 (g) -51 3 0 9 9 102 103 -12.423 1.247 3.529 12.974 0.000 6 21 (g) -52 2 2 10 11 101 102 46.412 19.903 30.917 59.212 0.000 7 21 (g) -51 4 0 12 12 104 101 -29.874 -15.663 -32.536 46.866 0.000 8 21 (g) -51 4 0 57 57 103 104 -6.521 -5.246 -1.226 8.459 0.000 9 21 (g) -52 5 5 13 14 102 103 -10.018 1.006 2.846 10.462 0.000 10 21 (g) -51 6 0 15 15 105 102 38.644 18.437 21.422 47.876 0.000 11 21 (g) -51 6 0 21 21 101 105 7.439 1.294 9.136 11.853 0.000 12 21 (g) -52 7 7 19 20 104 101 -29.544 -15.490 -32.178 46.349 0.000 13 21 (g) -51 9 0 18 18 106 103 -9.958 3.186 2.849 10.836 0.000 14 21 (g) -51 9 0 16 17 102 106 3.552 -0.457 1.999 4.101 0.000 15 21 (g) -52 10 10 25 26 105 102 35.032 16.713 19.420 43.402 0.000 16 21 (g) -51 14 0 40 41 102 107 2.269 -0.780 4.223 4.856 0.000 17 21 (g) -51 14 0 30 30 107 106 -1.797 1.309 -1.342 2.597 0.000 18 21 (g) -52 13 13 28 29 106 103 -6.877 2.200 1.968 7.484 0.000 19 21 (g) -51 12 0 24 24 104 108 -29.727 -15.488 -29.730 44.804 0.000 20 21 (g) -51 12 0 22 23 108 101 0.527 0.058 -2.025 2.093 0.000 21 21 (g) -52 11 11 27 27 101 105 7.095 1.234 8.713 11.304 0.000 22 21 (g) -51 20 0 37 38 109 101 0.347 -0.173 -2.718 2.745 0.000 23 21 (g) -51 20 0 85 86 108 109 -6.147 -3.066 -5.635 8.885 0.000 24 21 (g) -52 19 19 63 63 104 108 -23.400 -12.191 -23.402 35.268 0.000 25 21 (g) -51 15 0 36 36 110 102 7.214 2.723 2.856 8.222 0.000 26 21 (g) -51 15 0 33 33 105 110 28.402 14.092 17.281 36.110 0.000 27 21 (g) -52 21 21 31 32 101 105 6.511 1.132 7.996 10.373 0.000 28 21 (g) -51 18 0 52 53 111 103 -2.996 2.235 1.281 3.952 0.000 29 21 (g) -51 18 0 54 54 106 111 -4.748 0.597 0.039 4.785 0.000 30 21 (g) -52 17 17 42 42 107 106 -0.930 0.678 -0.695 1.344 0.000 31 21 (g) -51 27 0 39 39 101 112 7.368 1.028 8.137 11.025 0.000 32 21 (g) -51 27 0 45 45 112 105 1.877 1.461 1.522 2.824 0.000 33 21 (g) -52 26 26 34 35 105 110 25.668 12.736 15.618 32.634 0.000 34 21 (g) -51 33 0 43 44 105 113 16.931 7.654 10.398 21.292 0.000 35 21 (g) -51 33 0 46 47 113 110 10.623 5.793 5.967 13.491 0.000 36 21 (g) -52 25 25 48 48 110 102 5.328 2.011 2.109 6.073 0.000 37 21 (g) -51 22 0 69 69 109 114 0.406 0.519 -2.341 2.431 0.000 38 21 (g) -51 22 0 49 50 114 101 0.193 -0.656 -0.099 0.691 0.000 39 21 (g) -52 31 31 51 51 101 112 7.116 0.992 7.858 10.647 0.000 40 21 (g) -51 16 0 129 129 102 115 -0.086 0.364 0.623 0.727 0.000 41 21 (g) -51 16 0 82 83 115 107 2.238 -1.060 3.512 4.298 0.000 42 21 (g) -52 30 30 84 84 107 106 -0.814 0.593 -0.608 1.176 0.000 43 -2 (ubar) -51 34 0 133 133 0 113 2.397 1.102 1.875 3.253 0.330 44 2 (u) -51 34 0 99 99 105 0 15.807 7.544 9.556 19.954 0.330 45 21 (g) -52 32 32 100 100 112 105 0.604 0.470 0.490 0.908 0.000 46 21 (g) -51 35 0 58 59 113 116 14.211 6.808 7.064 17.269 0.000 47 21 (g) -51 35 0 60 60 116 110 0.610 0.569 0.565 1.008 0.000 48 21 (g) -52 36 36 97 0 110 102 1.130 0.426 0.447 1.288 0.000 49 21 (g) -51 38 0 67 68 114 117 1.041 -0.583 1.056 1.594 0.000 50 21 (g) -51 38 0 94 0 117 101 -0.054 0.038 -0.278 0.286 0.000 51 21 (g) -52 39 39 101 101 101 112 6.321 0.882 6.981 9.459 0.000 52 21 (g) -51 28 0 55 56 118 103 -2.451 1.146 1.265 2.987 0.000 53 21 (g) -51 28 0 124 124 111 118 -1.498 1.208 0.024 1.924 0.000 54 21 (g) -52 29 29 125 125 106 111 -3.795 0.477 0.031 3.825 0.000 55 21 (g) -51 52 0 123 123 118 119 -1.942 0.712 0.285 2.088 0.000 56 21 (g) -51 52 0 81 81 119 103 -0.761 0.231 0.933 1.226 0.000 57 21 (g) -52 8 8 61 62 103 104 -6.269 -5.043 -1.179 8.132 0.000 58 21 (g) -51 46 0 132 132 113 120 5.134 2.903 2.253 6.313 0.000 59 21 (g) -51 46 0 131 131 120 116 9.500 4.300 5.201 11.653 0.000 60 21 (g) -52 47 47 97 0 116 110 0.188 0.176 0.174 0.311 0.000 61 21 (g) -51 57 0 79 80 103 121 -5.014 -3.314 -1.002 6.094 0.000 62 21 (g) -51 57 0 66 66 121 104 -1.553 -1.885 -0.475 2.489 0.000 63 21 (g) -52 24 24 64 65 104 108 -23.101 -12.036 -23.103 34.817 0.000 64 21 (g) -51 63 0 117 117 122 108 -19.381 -10.676 -19.557 29.531 0.000 65 21 (g) -51 63 0 70 71 104 122 -3.798 -1.454 -3.570 5.411 0.000 66 21 (g) -52 62 62 72 72 121 104 -1.476 -1.791 -0.451 2.364 0.000 67 21 (g) -51 49 0 76 77 123 117 0.666 0.130 -0.097 0.686 0.000 68 21 (g) -51 49 0 75 75 114 123 0.421 -0.655 0.890 1.182 0.000 69 21 (g) -52 37 37 73 74 109 114 0.360 0.460 -2.077 2.158 0.000 70 21 (g) -51 65 0 118 118 124 122 -2.801 -0.664 -2.363 3.724 0.000 71 21 (g) -51 65 0 119 119 104 124 -1.300 -1.158 -1.300 2.172 0.000 72 21 (g) -52 66 66 120 120 121 104 -1.173 -1.424 -0.359 1.879 0.000 73 1 (d) -51 69 0 87 87 109 0 0.418 0.114 -1.846 1.925 0.330 74 -1 (dbar) -51 69 0 104 104 0 114 0.008 0.243 -0.090 0.420 0.330 75 21 (g) -52 68 68 78 78 114 123 0.354 -0.551 0.749 0.995 0.000 76 21 (g) -51 67 0 93 93 126 117 0.061 -0.341 -0.138 0.372 0.000 77 21 (g) -51 67 0 91 92 123 126 0.872 0.055 0.605 1.063 0.000 78 21 (g) -52 75 75 95 0 114 123 0.087 -0.136 0.185 0.245 0.000 79 21 (g) -51 61 0 121 121 127 121 -4.861 -3.184 -1.094 5.913 0.000 80 21 (g) -51 61 0 98 0 103 127 -0.279 -0.091 0.245 0.382 0.000 81 21 (g) -52 56 56 98 0 119 103 -0.636 0.193 0.779 1.024 0.000 82 21 (g) -51 41 0 128 128 115 128 1.476 -0.842 1.668 2.382 0.000 83 21 (g) -51 41 0 127 127 128 107 0.726 -0.193 1.818 1.967 0.000 84 21 (g) -52 42 42 126 126 107 106 -0.779 0.567 -0.581 1.125 0.000 85 21 (g) -51 23 0 88 89 108 129 -5.828 -3.028 -5.804 8.765 0.000 86 21 (g) -51 23 0 90 90 129 109 -0.276 -0.025 0.015 0.277 0.000 87 1 (d) -52 73 73 113 113 109 0 0.376 0.101 -1.692 1.767 0.330 88 21 (g) -51 85 0 116 116 108 130 -2.689 -1.861 -2.763 4.281 0.000 89 21 (g) -51 85 0 115 115 130 129 -3.265 -1.179 -3.034 4.610 0.000 90 21 (g) -52 86 86 114 114 129 109 -0.150 -0.013 0.008 0.151 0.000 91 21 (g) -51 77 0 95 0 123 131 0.980 -0.361 0.537 1.174 0.000 92 21 (g) -51 77 0 96 0 131 126 -0.061 0.157 -0.037 0.172 0.000 93 21 (g) -52 76 76 94 0 126 117 0.015 -0.081 -0.033 0.089 0.000 94 21 (g) -73 50 93 96 0 126 101 -0.039 -0.043 -0.311 0.375 0.200 95 21 (g) -73 78 91 103 103 114 131 1.067 -0.497 0.722 1.420 0.329 96 21 (g) -73 92 94 102 102 131 101 -0.101 0.114 -0.348 0.547 0.393 97 21 (g) -73 48 60 130 130 116 102 1.318 0.602 0.621 1.598 0.264 98 21 (g) -73 80 81 122 122 119 127 -0.915 0.102 1.024 1.406 0.286 99 2 (u) -71 44 44 105 112 105 0 15.807 7.544 9.556 19.954 0.330 100 21 (g) -71 45 45 105 112 112 105 0.604 0.470 0.490 0.908 0.000 101 21 (g) -71 51 51 105 112 101 112 6.321 0.882 6.981 9.459 0.000 102 21 (g) -71 96 96 105 112 131 101 -0.101 0.114 -0.348 0.547 0.393 103 21 (g) -71 95 95 105 112 114 131 1.067 -0.497 0.722 1.420 0.329 104 -1 (dbar) -71 74 74 105 112 0 114 0.008 0.243 -0.090 0.420 0.330 105 3222 (Sigma+) -83 99 104 184 185 0 0 6.599 3.094 4.898 8.862 1.189 106 -213 (rho-) -83 99 104 160 161 0 0 4.136 1.386 1.924 4.830 0.773 107 -3114 (Sigma*bar+) -83 99 104 162 163 0 0 9.319 3.922 6.764 12.277 1.658 108 -211 pi- 83 99 104 0 0 0 0 2.675 0.854 3.137 4.212 0.140 109 211 pi+ 84 99 104 0 0 0 0 -0.037 -0.400 0.121 0.442 0.140 110 -211 pi- 84 99 104 0 0 0 0 0.542 0.037 0.139 0.577 0.140 111 111 (pi0) -84 99 104 186 187 0 0 0.243 -0.105 0.064 0.304 0.135 112 213 (rho+) -84 99 104 164 165 0 0 0.231 -0.034 0.263 1.204 1.151 113 1 (d) -71 87 87 134 159 109 0 0.376 0.101 -1.692 1.767 0.330 114 21 (g) -71 90 90 134 159 129 109 -0.150 -0.013 0.008 0.151 0.000 115 21 (g) -71 89 89 134 159 130 129 -3.265 -1.179 -3.034 4.610 0.000 116 21 (g) -71 88 88 134 159 108 130 -2.689 -1.861 -2.763 4.281 0.000 117 21 (g) -71 64 64 134 159 122 108 -19.381 -10.676 -19.557 29.531 0.000 118 21 (g) -71 70 70 134 159 124 122 -2.801 -0.664 -2.363 3.724 0.000 119 21 (g) -71 71 71 134 159 104 124 -1.300 -1.158 -1.300 2.172 0.000 120 21 (g) -71 72 72 134 159 121 104 -1.173 -1.424 -0.359 1.879 0.000 121 21 (g) -71 79 79 134 159 127 121 -4.861 -3.184 -1.094 5.913 0.000 122 21 (g) -71 98 98 134 159 119 127 -0.915 0.102 1.024 1.406 0.286 123 21 (g) -71 55 55 134 159 118 119 -1.942 0.712 0.285 2.088 0.000 124 21 (g) -71 53 53 134 159 111 118 -1.498 1.208 0.024 1.924 0.000 125 21 (g) -71 54 54 134 159 106 111 -3.795 0.477 0.031 3.825 0.000 126 21 (g) -71 84 84 134 159 107 106 -0.779 0.567 -0.581 1.125 0.000 127 21 (g) -71 83 83 134 159 128 107 0.726 -0.193 1.818 1.967 0.000 128 21 (g) -71 82 82 134 159 115 128 1.476 -0.842 1.668 2.382 0.000 129 21 (g) -71 40 40 134 159 102 115 -0.086 0.364 0.623 0.727 0.000 130 21 (g) -71 97 97 134 159 116 102 1.318 0.602 0.621 1.598 0.264 131 21 (g) -71 59 59 134 159 120 116 9.500 4.300 5.201 11.653 0.000 132 21 (g) -71 58 58 134 159 113 120 5.134 2.903 2.253 6.313 0.000 133 -2 (ubar) -71 43 43 134 159 0 113 2.397 1.102 1.875 3.253 0.330 134 -213 (rho-) -83 113 133 166 167 0 0 -0.182 -0.401 -0.935 1.407 0.955 135 111 (pi0) -83 113 133 188 189 0 0 -0.317 0.080 -0.874 0.943 0.135 136 211 pi+ 83 113 133 0 0 0 0 -0.985 -0.373 -1.338 1.709 0.140 137 1114 (Delta-) -83 113 133 168 169 0 0 -3.299 -1.516 -3.295 5.036 1.151 138 213 (rho+) -83 113 133 170 171 0 0 -1.924 -1.456 -2.390 3.469 0.709 139 -2212 pbar- 83 113 133 0 0 0 0 -9.256 -4.321 -8.417 13.269 0.938 140 211 pi+ 83 113 133 0 0 0 0 -1.841 -0.923 -2.072 2.924 0.140 141 111 (pi0) -83 113 133 190 191 0 0 -0.697 -0.339 -0.442 0.902 0.135 142 2112 n0 83 113 133 0 0 0 0 -6.937 -4.370 -6.973 10.804 0.940 143 -2212 pbar- 83 113 133 0 0 0 0 -1.895 -1.387 -1.692 3.043 0.938 144 221 (eta) -83 113 133 192 194 0 0 -0.824 -0.518 -0.480 1.216 0.548 145 213 (rho+) -83 113 133 172 173 0 0 -4.275 -2.442 -2.514 5.690 1.347 146 3112 (Sigma-) -83 113 133 195 196 0 0 -2.384 -1.321 -0.525 3.023 1.197 147 -3122 (Lambdabar0) -83 113 133 197 198 0 0 -1.222 0.328 0.699 1.826 1.116 148 113 (rho0) -83 113 133 174 175 0 0 -2.228 -0.293 -0.050 2.373 0.761 149 111 (pi0) -83 113 133 199 200 0 0 -2.810 1.714 0.956 3.430 0.135 150 211 pi+ 84 113 133 0 0 0 0 -2.158 0.166 -0.529 2.233 0.140 151 -213 (rho-) -84 113 133 176 177 0 0 -0.619 0.397 -0.193 1.062 0.741 152 213 (rho+) -84 113 133 178 179 0 0 0.578 -0.562 1.775 2.115 0.821 153 -211 pi- 84 113 133 0 0 0 0 0.212 0.162 -0.020 0.302 0.140 154 211 pi+ 84 113 133 0 0 0 0 0.605 0.532 0.119 0.826 0.140 155 -211 pi- 84 113 133 0 0 0 0 1.633 -0.764 2.344 2.960 0.140 156 211 pi+ 84 113 133 0 0 0 0 1.269 0.793 0.824 1.714 0.140 157 113 (rho0) -84 113 133 180 181 0 0 4.723 2.557 2.721 6.085 0.883 158 -213 (rho-) -84 113 133 182 183 0 0 5.774 3.047 3.408 7.452 1.134 159 223 (omega) -84 113 133 201 203 0 0 5.352 2.457 2.584 6.480 0.790 160 -211 pi- 91 106 0 0 0 0 0 2.568 1.128 0.968 2.970 0.140 161 111 (pi0) -91 106 0 204 205 0 0 1.568 0.258 0.956 1.860 0.135 162 -3122 (Lambdabar0) -91 107 0 206 207 0 0 9.154 3.926 6.551 11.973 1.116 163 211 pi+ 91 107 0 0 0 0 0 0.165 -0.003 0.214 0.304 0.140 164 211 pi+ 91 112 0 0 0 0 0 -0.021 0.516 0.232 0.583 0.140 165 111 (pi0) -91 112 0 208 209 0 0 0.252 -0.550 0.031 0.621 0.135 166 -211 pi- 91 134 0 0 0 0 0 -0.079 -0.653 -0.377 0.771 0.140 167 111 (pi0) -91 134 0 210 211 0 0 -0.103 0.253 -0.558 0.635 0.135 168 2112 n0 91 137 0 0 0 0 0 -2.921 -1.426 -3.055 4.559 0.940 169 -211 pi- 91 137 0 0 0 0 0 -0.378 -0.090 -0.240 0.478 0.140 170 211 pi+ 91 138 0 0 0 0 0 -1.122 -0.560 -1.538 1.989 0.140 171 111 (pi0) -91 138 0 212 213 0 0 -0.802 -0.896 -0.852 1.480 0.135 172 211 pi+ 91 145 0 0 0 0 0 -3.124 -1.311 -1.175 3.588 0.140 173 111 (pi0) -91 145 0 214 215 0 0 -1.152 -1.131 -1.339 2.102 0.135 174 211 pi+ 91 148 0 0 0 0 0 -0.909 0.152 0.196 0.952 0.140 175 -211 pi- 91 148 0 0 0 0 0 -1.319 -0.445 -0.246 1.421 0.140 176 -211 pi- 91 151 0 0 0 0 0 -0.166 -0.173 -0.160 0.321 0.140 177 111 (pi0) -91 151 0 216 217 0 0 -0.452 0.570 -0.033 0.741 0.135 178 211 pi+ 91 152 0 0 0 0 0 0.562 -0.046 1.187 1.321 0.140 179 111 (pi0) -91 152 0 218 220 0 0 0.016 -0.516 0.588 0.794 0.135 180 211 pi+ 91 157 0 0 0 0 0 0.678 0.485 0.748 1.129 0.140 181 -211 pi- 91 157 0 0 0 0 0 4.045 2.071 1.973 4.956 0.140 182 -211 pi- 91 158 0 0 0 0 0 0.344 -0.049 0.203 0.425 0.140 183 111 (pi0) -91 158 0 221 222 0 0 5.431 3.096 3.206 7.027 0.135 184 2212 p+ 91 105 0 0 0 0 0 6.297 2.883 4.697 8.420 0.938 185 111 (pi0) -91 105 0 223 224 0 0 0.302 0.211 0.201 0.441 0.135 186 22 gamma 91 111 0 0 0 0 0 0.114 0.007 -0.017 0.115 0.000 187 22 gamma 91 111 0 0 0 0 0 0.130 -0.112 0.081 0.189 0.000 188 22 gamma 91 135 0 0 0 0 0 -0.146 -0.006 -0.524 0.544 0.000 189 22 gamma 91 135 0 0 0 0 0 -0.171 0.086 -0.350 0.399 0.000 190 22 gamma 91 141 0 0 0 0 0 -0.674 -0.344 -0.447 0.879 0.000 191 22 gamma 91 141 0 0 0 0 0 -0.023 0.004 0.005 0.023 0.000 192 22 gamma 91 144 0 0 0 0 0 -0.547 -0.214 -0.008 0.587 0.000 193 11 e- 91 144 0 0 0 0 0 -0.051 -0.061 -0.060 0.100 0.001 194 -11 e+ 91 144 0 0 0 0 0 -0.227 -0.243 -0.412 0.530 0.001 195 2112 n0 91 146 0 0 0 0 0 -2.027 -1.104 -0.252 2.505 0.940 196 -211 pi- 91 146 0 0 0 0 0 -0.357 -0.217 -0.273 0.518 0.140 197 -2212 pbar- 91 147 0 0 0 0 0 -0.985 0.234 0.669 1.533 0.938 198 211 pi+ 91 147 0 0 0 0 0 -0.237 0.094 0.030 0.292 0.140 199 22 gamma 91 149 0 0 0 0 0 -1.420 0.898 0.552 1.769 0.000 200 22 gamma 91 149 0 0 0 0 0 -1.390 0.816 0.404 1.661 0.000 201 211 pi+ 91 159 0 0 0 0 0 1.984 0.747 0.676 2.229 0.140 202 -211 pi- 91 159 0 0 0 0 0 2.890 1.476 1.650 3.643 0.140 203 111 (pi0) -91 159 0 225 226 0 0 0.478 0.234 0.258 0.607 0.135 204 22 gamma 91 161 0 0 0 0 0 1.498 0.250 0.878 1.754 0.000 205 22 gamma 91 161 0 0 0 0 0 0.070 0.009 0.079 0.106 0.000 206 -2112 nbar0 91 162 0 0 0 0 0 6.978 2.954 5.013 9.134 0.940 207 111 (pi0) -91 162 0 227 228 0 0 2.176 0.972 1.537 2.839 0.135 208 22 gamma 91 165 0 0 0 0 0 0.055 -0.277 -0.000 0.282 0.000 209 22 gamma 91 165 0 0 0 0 0 0.198 -0.273 0.031 0.338 0.000 210 22 gamma 91 167 0 0 0 0 0 -0.135 0.185 -0.406 0.466 0.000 211 22 gamma 91 167 0 0 0 0 0 0.032 0.068 -0.151 0.169 0.000 212 22 gamma 91 171 0 0 0 0 0 -0.290 -0.420 -0.382 0.638 0.000 213 22 gamma 91 171 0 0 0 0 0 -0.512 -0.476 -0.470 0.842 0.000 214 22 gamma 91 173 0 0 0 0 0 -0.962 -0.948 -1.182 1.795 0.000 215 22 gamma 91 173 0 0 0 0 0 -0.190 -0.183 -0.157 0.307 0.000 216 22 gamma 91 177 0 0 0 0 0 -0.001 -0.004 0.009 0.010 0.000 217 22 gamma 91 177 0 0 0 0 0 -0.451 0.574 -0.041 0.731 0.000 218 22 gamma 91 179 0 0 0 0 0 -0.055 -0.193 0.187 0.274 0.000 219 11 e- 91 179 0 0 0 0 0 0.023 -0.106 0.128 0.168 0.001 220 -11 e+ 91 179 0 0 0 0 0 0.047 -0.217 0.273 0.351 0.001 221 22 gamma 91 183 0 0 0 0 0 4.496 2.514 2.609 5.774 0.000 222 22 gamma 91 183 0 0 0 0 0 0.935 0.582 0.597 1.253 0.000 223 22 gamma 91 185 0 0 0 0 0 0.093 0.120 0.027 0.154 0.000 224 22 gamma 91 185 0 0 0 0 0 0.209 0.091 0.174 0.287 0.000 225 22 gamma 91 203 0 0 0 0 0 0.348 0.187 0.251 0.469 0.000 226 22 gamma 91 203 0 0 0 0 0 0.130 0.047 0.007 0.138 0.000 227 22 gamma 91 207 0 0 0 0 0 0.315 0.093 0.194 0.382 0.000 228 22 gamma 91 207 0 0 0 0 0 1.861 0.879 1.343 2.457 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 0.000 124.999 124.999 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Junction Listing (complete event) ------------ no kind col0 col1 col2 endc0 endc1 endc2 stat0 stat1 stat2 no junctions present -------- End PYTHIA Junction Listing -------------------------- Pythia::next(): 1000 events have been generated PYTHIA Warning in TimeShower::findMEcorr: ME weight above PS one Pythia::next(): 2000 events have been generated Pythia::next(): 3000 events have been generated Pythia::next(): 4000 events have been generated Pythia::next(): 5000 events have been generated Pythia::next(): 6000 events have been generated Pythia::next(): 7000 events have been generated Pythia::next(): 8000 events have been generated Pythia::next(): 9000 events have been generated *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 9 Warning in TimeShower::findMEcorr: ME weight above PS one | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:06 deviation from energy-momentum conservation 1.00*10^ 4 X 0.96*10^ 4 X 0.92*10^ 4 X 0.88*10^ 4 X 0.84*10^ 4 X 0.80*10^ 4 X 0.76*10^ 4 X 0.72*10^ 4 X 0.68*10^ 4 X 0.64*10^ 4 X 0.60*10^ 4 X 0.56*10^ 4 X 0.52*10^ 4 X 0.48*10^ 4 X 0.44*10^ 4 X 0.40*10^ 4 X 0.36*10^ 4 X 0.32*10^ 4 X 0.28*10^ 4 X 0.24*10^ 4 X 0.20*10^ 4 X 0.16*10^ 4 X 0.12*10^ 4 X 0.08*10^ 4 X 0.04*10^ 4 X Contents *10^ 4 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^-5 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-6 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-7 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 10000 Mean = 5.0000e-07 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+04 Rms = 0.0000e+00 Overflow = 0.0000e+00 High edge = 1.0000e-04 2013-09-20 16:06 deviation from charge conservation 1.00*10^ 4 X 0.96*10^ 4 X 0.92*10^ 4 X 0.88*10^ 4 X 0.84*10^ 4 X 0.80*10^ 4 X 0.76*10^ 4 X 0.72*10^ 4 X 0.68*10^ 4 X 0.64*10^ 4 X 0.60*10^ 4 X 0.56*10^ 4 X 0.52*10^ 4 X 0.48*10^ 4 X 0.44*10^ 4 X 0.40*10^ 4 X 0.36*10^ 4 X 0.32*10^ 4 X 0.28*10^ 4 X 0.24*10^ 4 X 0.20*10^ 4 X 0.16*10^ 4 X 0.12*10^ 4 X 0.08*10^ 4 X 0.04*10^ 4 X Contents *10^ 4 000000000000000000000000000010000000000000000000000000000 *10^ 3 000000000000000000000000000000000000000000000000000000000 *10^ 2 000000000000000000000000000000000000000000000000000000000 *10^ 1 000000000000000000000000000000000000000000000000000000000 Low edge ----------------------------- *10^ 0 998887776665554443332221110000001112223334445556667778889 *10^-1 518518518518518518518518518511581581581581581581581581581 *10^-2 073073073073073073073073073077037037037037037037037037037 Entries = 10000 Mean = 0.0000e+00 Underflow = 0.0000e+00 Low edge = -9.5000e+00 All chan = 1.0000e+04 Rms = 0.0000e+00 Overflow = 0.0000e+00 High edge = 9.5000e+00 2013-09-20 16:06 final particle multiplicity 2.24*10^ 2 4 4 2.16*10^ 2 X X X5 8 2.08*10^ 2 X X 8XX5X X 2.00*10^ 2 X 5 X XXXXX X 8 5 1.92*10^ 2 X4 X X XXXXX XXXX5X 1 1.84*10^ 2 XX X X XXXXX6XXXXXX4 5X3 1.76*10^ 2 XX X1XXXXXXXXXXXXXXX 3XXX 1.68*10^ 2 XX 3 XXXXXXXXXXXXXXXXX XXXX 1.60*10^ 2 XX X6XXXXXXXXXXXXXXXXX8XXXX3 1.52*10^ 2 XX 16XXXXXXXXXXXXXXXXXXXXXXXXXX 6 1.44*10^ 2 9XX XXXXXXXXXXXXXXXXXXXXXXXXXXXX53X 1.36*10^ 2 XXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6X 1.28*10^ 2 XXX 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 6X 1.20*10^ 2 XXX 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 4 1.12*10^ 2 XXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9XX3X 1.04*10^ 2 XXXX1 3X 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.96*10^ 2 XXXXX XX4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1X 3 0.88*10^ 2 9XXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5XX X 0.80*10^ 2 XXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX68XX 0.72*10^ 2 XXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.64*10^ 2 XXXXXX 85XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX66 0.56*10^ 2 XXXXXX1 92XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.48*10^ 2 XXXXXXX 5 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 2 0.40*10^ 2 5XXXXXXX1 2X5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6X79 X4 0.32*10^ 2 XXXXXXXXX 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX715 0.24*10^ 2 7 XXXXXXXXX 267XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2 0.16*10^ 2 X XXXXXXXXX9 44XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX1X 0.08*10^ 2 XXXXXXXXXXXX689XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 2 0000001211000000000000000000000001011111111112122222121111111111111111111111000000000000000000000000 *10^ 1 0020384181943100011122234345566790901244565961701101809998975788754343312201889779866543433343322101 *10^ 0 0028673972793556711812944615020284103159227699666244182828698005840893615865496780011687289205058896 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 1 0000000000011111111112222222222333333333344444444445555555555666666666677777777778888888888999999999 *10^ 0 0012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789012345678 *10^-1 5555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555 Entries = 10000 Mean = 5.0917e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 9.8450e+03 Rms = 2.1681e+01 Overflow = 1.5500e+02 High edge = 9.9500e+01 2013-09-20 16:06 dn/dp for particles 7.50*10^ 4 5 7.25*10^ 4 X 7.00*10^ 4 X3 6.75*10^ 4 XX 6.50*10^ 4 XX 6.25*10^ 4 XX 6.00*10^ 4 XX 5.75*10^ 4 XX 5.50*10^ 4 XX3 5.25*10^ 4 XXX 5.00*10^ 4 XXX 4.75*10^ 4 XXX 4.50*10^ 4 XXX 4.25*10^ 4 XXX4 4.00*10^ 4 XXXX 3.75*10^ 4 XXXX 3.50*10^ 4 XXXX 3.25*10^ 4 XXXX9 3.00*10^ 4 XXXXX 2.75*10^ 4 XXXXX3 2.50*10^ 4 XXXXXX 2.25*10^ 4 XXXXXX6 2.00*10^ 4 XXXXXXX2 1.75*10^ 4 XXXXXXXX2 1.50*10^ 4 XXXXXXXXX4 1.25*10^ 4 XXXXXXXXXX71 1.00*10^ 4 XXXXXXXXXXXX73 0.75*10^ 4 XXXXXXXXXXXXXXX642 0.50*10^ 4 XXXXXXXXXXXXXXXXXXX87654321 0.25*10^ 4 XXXXXXXXXXXXXXXXXXXXXXXXXXXX9998877666555444444333333322222222222221111111111111111111111111111111 Contents *10^ 4 7654322111110000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 3 3831251853109876654443333222222111111111111110000000000000000000000000000000000000000000000000000000 *10^ 2 7120384044631245059629742975321997755433210009987777666565555444443333323222222222222111111111111111 *10^ 1 0445106785845447363127113199476246990934418326187854841602002780138776290989855532304977887455553622 Low edge *10^ 1 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^ 0 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^-1 0246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 518206 Mean = 2.0298e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 5.1176e+05 Rms = 2.8901e+00 Overflow = 6.4430e+03 High edge = 2.0000e+01 2013-09-20 16:06 particle flow in event plane 18.64*10^ 2 6 6 18.56*10^ 2 X X 18.48*10^ 2 4 X X 18.40*10^ 2 3 8 X X X 18.32*10^ 2 X X X X 4 X 8 X 18.24*10^ 2 6 X X 1 X X5X X X X 18.16*10^ 2 X X 3 X X X XXX X X X 18.08*10^ 2 3 X X X 8X X X9 1 XXX X 5 X X X 18.00*10^ 2 X X X X XX X XX X XXX X X 8 9 X X5 X 17.92*10^ 2 X 6 X 3 X X X XX X XX XX8 XXX3 5X 5 X X X X XX X 17.84*10^ 2 5X3 4X X X X X X XX X XX XXX XXXX 5 XX X X X X 5 X4XX X 17.76*10^ 2 XXX XX X X X X X XX X XX XXX XXXX X XX16 X X X 3 X X XXXX6X 17.68*10^ 2 XXX XX X X X X 5 X XX X XX XXX 1XXXX X XXXX X X X X 3 X X1 XXXXXX 17.60*10^ 2 43XXX XX9X 5 X X X X X 9XX X 54 1XX XXX XXXXX X XXXX X X X X X X6XX 3 XXXXXX 17.52*10^ 2 8XXXXX6XXXX X6 X X X X XX XXX X 9XX XXX XXX XXXXX X XXXX X9 X X X X XXXX X XXXXXX 17.44*10^ 2 XXXXXXXXXXX XX9X 4X8X X XX XXX X XXX XXX XXX XXXXX X XXXX XX X X95X X6XXXX8X 8XXXXXX 17.36*10^ 2 XXXXXXXXXXX XXXX XXXX 4 X XX5XXX X XXX4XXX XXX XXXXX X XXXX XX 6X XXXX XXXXXXXX XXXXXXX 17.28*10^ 2 XXXXXXXXXXX XXXX XXXX X X XXXXXXX X XXXXXXX XXX XXXXXXX 3X 5XXXX XX XX XXXX XXXXXXXX 5XXXXXXX 17.20*10^ 2 XXXXXXXXXXX XXXX5XXXX9X3 X XXXXXXX X XXXXXXX XXX XXXXXXX XX XXXXX XX XX6XXXX 5XXXXXXXX XXXXXXXX 17.12*10^ 2 XXXXXXXXXXX XXXXXXXXXXXX68X3 XXXXXXX X1XXXXXXX8 XXX8XXXXXXX XX XXXXX XX4XXXXXXX XXXXXXXXX XXXXXXXX 17.04*10^ 2 XXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXX XXXXXXXXXXX XX XXXXX4 XXXXXXXXXX XXXXXXXXX 5XXXXXXXX 16.96*10^ 2 XXXXXXXXXXX4XXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXX XXXXXXXXXXX1XX XXXXXX XXXXXXXXXX XXXXXXXXX XXXXXXXXX 16.88*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXX XXXXXXXXXXXXXX XXXXXX XXXXXXXXXX XXXXXXXXX XXXXXXXXX 16.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXX5XXXXXXXXXXXXXX XXXXXX XXXXXXXXXX6XXXXXXXXX XXXXXXXXX 16.72*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6XXXXXX9XXXXXXXXXXXXXXXXXXXX XXXXXXXXX 16.64*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6XXXXXXXXX Contents *10^ 3 1111111111111111111111111111111111111111111111111111111111111111111111111111111111111111111111111111 *10^ 2 7777777777867777778787777777778777886877777788767877788877767767787766777787777767777777776777878778 *10^ 1 5558974785095448132431310160021535037105553530179091642282882262866797850301944771649586456024376970 *10^ 0 0540289999216936691249149046480229622751651387062100130768092894819391817347830076219701241042091638 Low edge -------------------------------------------------- *10^ 0 3332222222222222222111111111111111100000000000000000000000000000001111111111111111222222222222222233 *10^-1 1009887765543322100988776554332110098876655433211000112334556678890011233455677889001223345567788900 *10^-2 4825936048159260471582603715826937148259370481593606395184073952841739628517306285174062951840639528 Entries = 175656 Mean = 4.9792e-04 Underflow = 0.0000e+00 Low edge = -3.1416e+00 All chan = 1.7566e+05 Rms = 1.8156e+00 Overflow = 0.0000e+00 High edge = 3.1416e+00 2013-09-20 16:06 energy flow in event plane 12.10*10^ 3 5 12.00*10^ 3 X 11.90*10^ 3 X 11.80*10^ 3 X 11.70*10^ 3 X 11.60*10^ 3 6 4 7 X 11.50*10^ 3 X X 7 X X 11.40*10^ 3 X 1 X 5 3 X X X 11.30*10^ 3 5 X 1 4 X X X X4X8 X X X 11.20*10^ 3 X X X 6 X 8 X X XX XXXX X X 8 X9 11.10*10^ 3 X X XX X X 4 X X X XX 8XXXX X XX X 2 XX 11.00*10^ 3 X8X 3 XX X X X1 X X 3 X XX XXXXX X XX X X 5 3 6 XX 10.90*10^ 3 5XXX X XX X X 1 XX X X X X XX XXXXX 3 X XX4 X XX X X X 7 XX 10.80*10^ 3 XXXX X XX X 9 X X XX 5 X X X X XX XXXXX X X XXX X XX X X X 7X XX 10.70*10^ 3 XXXX X XX X67X X X 3 3 XX XXX X X X XX2XXXXX4 X X XXX 9 X XX X X 5 X XX XX 10.60*10^ 3 XXXX X6 XX XXXX X X X X XX XXX X X X XXXXXXXXX X X XXX X X XX 7X X9X X XX 5XX6 10.50*10^ 3 XXXX XX2XX XXXXX X2 X X X XX XXX XXX X2 XXXXXXXXX X X XXX X X 3 XX XX XXX X XX XXXX 10.40*10^ 3 XXXX XXXXX XXXXX XX X X 4 X9 XX XXX XXX XX XXXXXXXXX X XX 3XXX X XXX XX XX XXX X5XX7XXXX 10.30*10^ 3 XXXX XXXXX1 XXXXX XX X X X2 XX XX XXX6XXX XX XXXXXXXXX X9XX XXXX X XXX XX 1 XX XXX XXXXXXXXX 10.20*10^ 3 XXXX XXXXXX XXXXX6XX1X X XX XX9XX XXXXXXX XX XXXXXXXXX XXXX XXXX X XXX XX X3393XX XXX XXXXXXXXX 10.10*10^ 3 XXXX XXXXXX XXXXXXXXXX X XX XXXXX XXXXXXX XX XXXXXXXXX XXXX XXXX X XXX XX XXXXXXXX XXX XXXXXXXXX 10.00*10^ 3 XXXX5XXXXXX X XXXXXXXXXX X XXXXXXXX XXXXXXX XX XXXXXXXXX XXXX XXXX X XXX XX XXXXXXXX5XXX XXXXXXXXX 9.90*10^ 3 XXXXXXXXXXX2X1XXXXXXXXXX X XXXXXXXX XXXXXXX XX XXXXXXXXX XXXX XXXX X XXX XX85XXXXXXXXXXXX XXXXXXXXX 9.80*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXX14X XXXXXXXX XXXXXXX7XX1XXXXXXXXX XXXX XXXX4X XXX5XXXXXXXXXXXXXXXX XXXXXXXXX 9.70*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXX XXXXXXXXXXX XXXXXXXXXXXXXXXXXXXX3XXXXXXXXX 9.60*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXX XXXXXXXXXXX5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 9.50*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7XXXXXXXXXXXXXXXXXXXX4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 4 1111011111101011111111110010111111110111111101101111111110111101111010111011001111111101110111111111 *10^ 3 0101900011090910000010009909000000109001010091091101111109001090110909100901990000000090009000000210 *10^ 2 8295995412280816675124187767320631094771235973475260323264824473158765144790881211115999566937835015 *10^ 1 5586536201120166790642111430420399417508610370214028543844397003074495803502850133937553953657775596 Low edge -------------------------------------------------- *10^ 0 3332222222222222222111111111111111100000000000000000000000000000001111111111111111222222222222222233 *10^-1 1009887765543322100988776554332110098876655433211000112334556678890011233455677889001223345567788900 *10^-2 4825936048159260471582603715826937148259370481593606395184073952841739628517306285174062951840639528 Entries = 175656 Mean = -1.4973e-03 Underflow = 0.0000e+00 Low edge = -3.1416e+00 All chan = 1.0563e+06 Rms = 1.8170e+00 Overflow = 0.0000e+00 High edge = 3.1416e+00 2013-09-20 16:06 parton flow in event plane 14.40*10^ 2 1 14.32*10^ 2 X 14.24*10^ 2 X 14.16*10^ 2 X 14.08*10^ 2 X 6 14.00*10^ 2 6 X X 5 3 4 13.92*10^ 2 X X 9 98 X X X X X 13.84*10^ 2 X 1 6 6 69 6 X X XX 5 X X 9 X X X X1 5 13.76*10^ 2 X X X 1X 3XX X X X XX51X X 5 X X X X 5 X X XX X 13.68*10^ 2 X6X X XX XXX X X X XXXXX X 6X X 9 X1 6 6 4 X X X X X XX X 13.60*10^ 2 XXX X 5 5XX XXX X X X 8 X XXXXX X XX X1 X 8XXX X X X X36 X 9X 8X X 4 XX X 13.52*10^ 2 XXXXX X XXX XXX1 X1 X X XX 1X XXXXX4 X 3 XX XX X XXXX X6X X XXX X XX XX X 6 X XXX X 13.44*10^ 2 XXXXX X XXX XXXX XX X X XX XX XXXXXX X X XX6XX X XXXX XXX5X XXX X XX1XX X3 X X XXX X 13.36*10^ 2 1 XXXXX 3 X5XXX XXXX6XX X X XX XX XXXXXX X X 8XXXXX8X XXXX XXXXX XXX X XXXXX XX X X8XXX3X 13.28*10^ 2 XX XXXXX 3 X XXXXX XXXXXXX8 X X6XX XX XXXXXX3X X XXXXXXXX6 XXXX1XXXXX XXX X XXXXX5XX X XXXXXXX 13.20*10^ 2 XX XXXXX X5X XXXXX XXXXXXXX X XXXX XX XXXXXXXX X XXXXXXXXX XXXXXXXXXX XXX X XXXXXXXX58X XXXXXXX 13.12*10^ 2 XX XXXXX XXX XXXXX1XXXXXXXX X 9XXXX XX XXXXXXXX X6XXXXXXXXX XXXXXXXXXX XXX X XXXXXXXXXXX6XXXXXXX 13.04*10^ 2 XX XXXXXXXXX3XXXXXXXXXXXXXX X 8XXXXX XX XXXXXXXX XXXXXXXXXXX XXXXXXXXXX XXX X XXXXXXXXXXXXXXXXXXX 12.96*10^ 2 XX XXXXXXXXXXXXXXXXXXXXXXXX X XXXXXX XX XXXXXXXX XXXXXXXXXXX XXXXXXXXXX9XXX6 X9XXXXXXXXXXXXXXXXXXX 12.88*10^ 2 XX6XXXXXXXXXXXXXXXXXXXXXXXX X XXXXXX9XX XXXXXXXX XXXXXXXXXXX1XXXXXXXXXXXXXXX6XXXXXXXXXXXXXXXXXXXXX 12.80*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXX 9X XXXXXXXXX XXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 12.72*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXX XX5XXXXXXXXX9XXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 12.64*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXX5XXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 12.56*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 12.48*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 3 1111111111111111111111111111111111111111111111111111111111111111111111111111111111111111111111111111 *10^ 2 3323333333332333333333333332223233433323323333333323333334333323333333333233322323333333333333333333 *10^ 1 2289675802139535680788436426678601325584979976842844036740536285866264646975598995735929311405359738 *10^ 0 8957572142608626915013530560491821358275111029072476945215347518310159503564735259278644868995425700 Low edge -------------------------------------------------- *10^ 0 3332222222222222222111111111111111100000000000000000000000000000001111111111111111222222222222222233 *10^-1 1009887765543322100988776554332110098876655433211000112334556678890011233455677889001223345567788900 *10^-2 4825936048159260471582603715826937148259370481593606395184073952841739628517306285174062951840639528 Entries = 134392 Mean = 4.7141e-03 Underflow = 0.0000e+00 Low edge = -3.1416e+00 All chan = 1.3439e+05 Rms = 1.8145e+00 Overflow = 0.0000e+00 High edge = 3.1416e+00 2013-09-20 16:06 dn/dy all primaries 2.00*10^ 4 33 1.92*10^ 4 XX 1.84*10^ 4 1XX4 1.76*10^ 4 XXXX 1.68*10^ 4 XXXX 1.60*10^ 4 XXXX 1.52*10^ 4 5XXXX3 1.44*10^ 4 XXXXXX 1.36*10^ 4 XXXXXX 1.28*10^ 4 XXXXXX 1.20*10^ 4 4XXXXXX5 1.12*10^ 4 XXXXXXXX 1.04*10^ 4 XXXXXXXX 0.96*10^ 4 XXXXXXXX 0.88*10^ 4 3XXXXXXXX4 0.80*10^ 4 XXXXXXXXXX 0.72*10^ 4 XXXXXXXXXX 0.64*10^ 4 2XXXXXXXXXX1 0.56*10^ 4 XXXXXXXXXXXX 0.48*10^ 4 XXXXXXXXXXXX 0.40*10^ 4 XXXXXXXXXXXXX9 0.32*10^ 4 1XXXXXXXXXXXXXX1 0.24*10^ 4 XXXXXXXXXXXXXXXX 0.16*10^ 4 2XXXXXXXXXXXXXXXXX92 0.08*10^ 4 12247XXXXXXXXXXXXXXXXXXXX74211 Contents *10^ 4 0000000000000000000000000000000000000000000000111111110000000000000000000000000000000000000000000000 *10^ 3 0000000000000000000000000000000000000000112458147997418532100000000000000000000000000000000000000000 *10^ 2 0000000000000000000000000000000000001135055072586449653794595311000000000000000000000000000000000000 *10^ 1 0000000000000000000000000000000112244837070455138553563259048360532100000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 175656 Mean = -2.0426e-03 Underflow = 0.0000e+00 Low edge = -1.0000e+01 All chan = 1.7566e+05 Rms = 7.7149e-01 Overflow = 0.0000e+00 High edge = 1.0000e+01 2013-09-20 16:06 multiplicity status code 85 1.00*10^ 4 X 0.96*10^ 4 X 0.92*10^ 4 X 0.88*10^ 4 X 0.84*10^ 4 X 0.80*10^ 4 X 0.76*10^ 4 X 0.72*10^ 4 X 0.68*10^ 4 X 0.64*10^ 4 X 0.60*10^ 4 X 0.56*10^ 4 X 0.52*10^ 4 X 0.48*10^ 4 X 0.44*10^ 4 X 0.40*10^ 4 X 0.36*10^ 4 X 0.32*10^ 4 X 0.28*10^ 4 X 0.24*10^ 4 X 0.20*10^ 4 X 0.16*10^ 4 X 0.12*10^ 4 X 0.08*10^ 4 X 0.04*10^ 4 X Contents *10^ 4 10000000000000000000000000000000000000000000000000 *10^ 3 00000000000000000000000000000000000000000000000000 *10^ 2 00000000000000000000000000000000000000000000000000 *10^ 1 00000000000000000000000000000000000000000000000000 Low edge - *10^ 1 00000000000111111111122222222223333333333444444444 *10^ 0 00123456789012345678901234567890123456789012345678 *10^-1 55555555555555555555555555555555555555555555555555 Entries = 10000 Mean = 0.0000e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+04 Rms = 0.0000e+00 Overflow = 0.0000e+00 High edge = 4.9500e+01 2013-09-20 16:06 multiplicity status code 86 1.00*10^ 4 X 0.96*10^ 4 X 0.92*10^ 4 X 0.88*10^ 4 X 0.84*10^ 4 X 0.80*10^ 4 X 0.76*10^ 4 X 0.72*10^ 4 X 0.68*10^ 4 X 0.64*10^ 4 X 0.60*10^ 4 X 0.56*10^ 4 X 0.52*10^ 4 X 0.48*10^ 4 X 0.44*10^ 4 X 0.40*10^ 4 X 0.36*10^ 4 X 0.32*10^ 4 X 0.28*10^ 4 X 0.24*10^ 4 X 0.20*10^ 4 X 0.16*10^ 4 X 0.12*10^ 4 X 0.08*10^ 4 X 0.04*10^ 4 X Contents *10^ 4 10000000000000000000000000000000000000000000000000 *10^ 3 00000000000000000000000000000000000000000000000000 *10^ 2 00000000000000000000000000000000000000000000000000 *10^ 1 00000000000000000000000000000000000000000000000000 Low edge - *10^ 1 00000000000111111111122222222223333333333444444444 *10^ 0 00123456789012345678901234567890123456789012345678 *10^-1 55555555555555555555555555555555555555555555555555 Entries = 10000 Mean = 0.0000e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+04 Rms = 0.0000e+00 Overflow = 0.0000e+00 High edge = 4.9500e+01 2013-09-20 16:06 multiplicity status code 83 1.04*10^ 3 2 1.00*10^ 3 X 0.96*10^ 3 X 0.92*10^ 3 X 6 0.88*10^ 3 X X 0.84*10^ 3 X X3 0.80*10^ 3 X XXX3 0.76*10^ 3 X 6XXXX 0.72*10^ 3 X XXXXX 0.68*10^ 3 X XXXXX5 0.64*10^ 3 X 4XXXXXX 0.60*10^ 3 X XXXXXXX 0.56*10^ 3 X XXXXXXX 0.52*10^ 3 X XXXXXXX6 0.48*10^ 3 X XXXXXXXX8 0.44*10^ 3 X XXXXXXXXX2 0.40*10^ 3 X XXXXXXXXXX 0.36*10^ 3 X 1XXXXXXXXXX6 0.32*10^ 3 X XXXXXXXXXXXX7 0.28*10^ 3 X XXXXXXXXXXXXX2 0.24*10^ 3 X XXXXXXXXXXXXXX5 0.20*10^ 3 X XXXXXXXXXXXXXXX 0.16*10^ 3 X 9XXXXXXXXXXXXXXX56 0.12*10^ 3 X XXXXXXXXXXXXXXXXXX5 0.08*10^ 3 X XXXXXXXXXXXXXXXXXXX8612 0.04*10^ 3 X4XXXXXXXXXXXXXXXXXXXXXXX83221 1 1 Contents *10^ 3 10000000000000000000000000000000000000000000000000 *10^ 2 00136798776544332211000000000000000000000000000000 *10^ 1 01521401975070404244976443100000000000000000000000 *10^ 0 85646230839439279105932571488615041100100000000000 Low edge - *10^ 1 00000000000111111111122222222223333333333444444444 *10^ 0 00123456789012345678901234567890123456789012345678 *10^-1 55555555555555555555555555555555555555555555555555 Entries = 10000 Mean = 8.6655e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+04 Rms = 5.5230e+00 Overflow = 0.0000e+00 High edge = 4.9500e+01 2013-09-20 16:06 multiplicity status code 84 1.04*10^ 3 2 1.00*10^ 3 X 0.96*10^ 3 X 0.92*10^ 3 X 0.88*10^ 3 X 86 0.84*10^ 3 X XX 0.80*10^ 3 X 6XX5 0.76*10^ 3 X XXXX4 0.72*10^ 3 X XXXXX 0.68*10^ 3 X XXXXX 0.64*10^ 3 X XXXXXX 0.60*10^ 3 X 4XXXXXX 0.56*10^ 3 X XXXXXXX5 0.52*10^ 3 X XXXXXXXX 0.48*10^ 3 X XXXXXXXX5 0.44*10^ 3 X XXXXXXXXX4 0.40*10^ 3 X XXXXXXXXXX2 0.36*10^ 3 X 3XXXXXXXXXXX 0.32*10^ 3 X XXXXXXXXXXXX3 0.28*10^ 3 X XXXXXXXXXXXXX 0.24*10^ 3 X XXXXXXXXXXXXX5 0.20*10^ 3 X XXXXXXXXXXXXXXX21 0.16*10^ 3 X 1XXXXXXXXXXXXXXXXX 0.12*10^ 3 X XXXXXXXXXXXXXXXXXX60 0.08*10^ 3 X XXXXXXXXXXXXXXXXXXXX51 0.04*10^ 3 X7XXXXXXXXXXXXXXXXXXXXXXX95322111 11 Contents *10^ 3 10000000000000000000000000000000000000000000000000 *10^ 2 00135788776544322211100000000000000000000000000000 *10^ 1 02237876834461692066085433110000000000000000000000 *10^ 0 89437326170116602174529284937752302300100000000000 Low edge - *10^ 1 00000000000111111111122222222223333333333444444444 *10^ 0 00123456789012345678901234567890123456789012345678 *10^-1 55555555555555555555555555555555555555555555555555 Entries = 10000 Mean = 8.7141e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+04 Rms = 5.5726e+00 Overflow = 0.0000e+00 High edge = 4.9500e+01 2013-09-20 16:06 dn/dy primaries junction 2.00*10^ 4 33 1.92*10^ 4 XX 1.84*10^ 4 1XX4 1.76*10^ 4 XXXX 1.68*10^ 4 XXXX 1.60*10^ 4 XXXX 1.52*10^ 4 5XXXX3 1.44*10^ 4 XXXXXX 1.36*10^ 4 XXXXXX 1.28*10^ 4 XXXXXX 1.20*10^ 4 4XXXXXX5 1.12*10^ 4 XXXXXXXX 1.04*10^ 4 XXXXXXXX 0.96*10^ 4 XXXXXXXX 0.88*10^ 4 3XXXXXXXX4 0.80*10^ 4 XXXXXXXXXX 0.72*10^ 4 XXXXXXXXXX 0.64*10^ 4 2XXXXXXXXXX1 0.56*10^ 4 XXXXXXXXXXXX 0.48*10^ 4 XXXXXXXXXXXX 0.40*10^ 4 XXXXXXXXXXXXX9 0.32*10^ 4 1XXXXXXXXXXXXXX1 0.24*10^ 4 XXXXXXXXXXXXXXXX 0.16*10^ 4 2XXXXXXXXXXXXXXXXX92 0.08*10^ 4 12247XXXXXXXXXXXXXXXXXXXX74211 Contents *10^ 4 0000000000000000000000000000000000000000000000111111110000000000000000000000000000000000000000000000 *10^ 3 0000000000000000000000000000000000000000112458147997418532100000000000000000000000000000000000000000 *10^ 2 0000000000000000000000000000000000001135055072586449653794595311000000000000000000000000000000000000 *10^ 1 0000000000000000000000000000000112244837070455138553563259048360532100000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 175656 Mean = -2.0426e-03 Underflow = 0.0000e+00 Low edge = -1.0000e+01 All chan = 1.7566e+05 Rms = 7.7149e-01 Overflow = 0.0000e+00 High edge = 1.0000e+01 pythia8-8.1.80.orig/examples/outref/out090000644000175000017500000053347112217346171016377 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:02:59 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 8.000e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> t tbar 601 | 1.510e-06 | | q qbar -> t tbar 602 | 3.802e-07 | | q q -> t q (t-channel W+-) 603 | 1.418e-06 | | f fbar -> t tbar (s-channel gamma*/Z0) 604 | 2.659e-09 | | f fbar -> t qbar (s-channel W+-) 605 | 5.498e-08 | | gamma gamma -> t tbar 606 | 0.000e+00 | | | | |------------------------------------------------------------------| | | | | q g -> q gamma (udscb) 201 | 3.652e-04 | | q qbar -> g gamma 202 | 2.368e-05 | | g g -> g gamma 203 | 1.962e-07 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 52.12 mb | | | | pT0 = 2.77 gives sigmaInteraction = 218.50 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eCM | 8000.000 | 14000.000 10.00000 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:mHatMin | 40.00000 | 4.00000 0.0 | | PhaseSpace:pTHatMin | 20.00000 | 0.0 0.0 | | SecondHard:generate | on | off | | SecondHard:PhotonAndJet | on | off | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | Top:all | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 4.000e+03, e = 4.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -4.000e+03, e = 4.000e+03, m = 9.383e-01. In 1: id = 2, x = 2.955e-02, pdf = 6.112e-01 at Q2 = 6.247e+04. In 2: id = -1, x = 3.303e-02, pdf = 2.695e-01 at same Q2. Subprocess f fbar -> t qbar (s-channel W+-) with code 605 is 2 -> 2. It has sHat = 6.247e+04, tHat = -1.348e+04, uHat = -2.095e+04, pTHat = 6.715e+01, m3Hat = 1.674e+02, m4Hat = 4.800e+00, thetaHat = 1.352e+00, phiHat = 3.539e+00. alphaEM = 7.908e-03, alphaS = 1.163e-01 at Q2 = 6.247e+04. Impact parameter b = 1.206e+00 gives enhancement factor = 3.453e-01. Max pT scale for MPI = 2.220e+01, ISR = 2.499e+02, FSR = 2.499e+02. Number of MPI = 3, ISR = 9, FSRproc = 64, FSRreson = 11. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 8000.000 8000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 4000.000 4000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -4000.000 4000.000 0.938 3 2 (u) -21 1 0 5 6 101 0 0.000 0.000 118.206 118.206 0.000 4 -1 (dbar) -21 2 0 5 6 0 101 0.000 0.000 -132.123 132.123 0.000 5 6 (t) -22 3 4 11 12 102 0 -61.925 -25.975 4.891 180.428 167.395 6 -5 bbar 23 3 4 0 0 0 102 61.925 25.975 -18.808 69.901 4.800 7 21 (g) -21 1 0 9 10 105 104 0.000 0.000 2.300 2.300 0.000 8 2 (u) -21 2 0 9 10 104 0 0.000 0.000 -221.087 221.087 0.000 9 22 gamma 23 7 8 0 0 0 0 -20.049 9.533 -128.941 130.838 0.000 10 2 u 23 7 8 0 0 105 0 20.049 -9.533 -89.846 92.548 0.330 11 24 (W+) -22 5 0 13 14 0 0 -27.766 -53.699 53.594 114.622 81.309 12 5 b 23 5 0 0 0 102 0 -34.159 27.725 -48.703 65.807 4.800 13 -1 dbar 23 11 0 0 0 0 103 -21.530 18.774 15.854 32.672 0.330 14 2 u 23 11 0 0 0 103 0 -6.236 -72.473 37.740 81.949 0.330 Charge sum: 1.667 Momentum sum: -0.000 0.000 -232.704 473.716 412.620 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 8000.000 8000.000 1 2212 (p+) -12 0 0 280 0 0 0 0.000 0.000 4000.000 4000.000 0.938 2 2212 (p+) -12 0 0 281 0 0 0 0.000 0.000 -4000.000 4000.000 0.938 3 2 (u) -21 11 0 5 6 101 0 0.000 0.000 118.206 118.206 0.000 4 -1 (dbar) -21 12 12 5 6 0 101 0.000 0.000 -132.123 132.123 0.000 5 6 (t) -22 3 4 13 13 102 0 -61.925 -25.975 4.891 180.428 167.395 6 -5 (bbar) -23 3 4 14 14 0 102 61.925 25.975 -18.808 69.901 4.800 7 21 (g) -21 16 0 9 10 105 104 0.000 0.000 2.300 2.300 0.000 8 2 (u) -21 17 17 9 10 104 0 0.000 0.000 -221.087 221.087 0.000 9 22 (gamma) -23 7 8 18 18 0 0 -20.049 9.533 -128.941 130.838 0.000 10 2 (u) -23 7 8 19 19 105 0 20.049 -9.533 -89.846 92.548 0.330 11 2 (u) -41 63 63 15 3 106 0 -0.000 0.000 157.153 157.153 0.000 12 -1 (dbar) -42 64 0 4 4 0 101 0.000 -0.000 -132.123 132.123 0.000 13 6 (t) -44 5 5 29 29 102 0 -75.276 -22.800 4.238 185.001 167.395 14 -5 (bbar) -44 6 6 27 28 0 102 58.244 26.850 -13.553 65.727 4.800 15 21 (g) -43 11 0 67 67 106 101 17.032 -4.050 34.345 38.549 0.000 16 21 (g) -41 21 21 20 7 105 107 0.000 0.000 7.038 7.038 0.000 17 2 (u) -42 22 0 8 8 104 0 0.000 -0.000 -221.087 221.087 0.000 18 22 (gamma) -44 9 9 23 23 0 0 -25.226 11.672 -176.766 178.938 0.000 19 2 (u) -44 10 10 24 24 105 0 12.673 -6.484 -31.216 34.311 0.330 20 21 (g) -43 16 0 25 25 104 107 12.553 -5.188 -6.065 14.876 0.000 21 21 (g) -42 30 0 16 16 105 107 0.000 0.000 7.038 7.038 0.000 22 2 (u) -41 31 31 26 17 108 0 -0.000 -0.000 -678.456 678.456 0.000 23 22 (gamma) -44 18 18 32 32 0 0 -22.808 18.912 -180.501 182.917 0.000 24 2 (u) -44 19 19 33 33 105 0 13.119 -5.151 -31.990 34.958 0.330 25 21 (g) -44 20 20 34 34 104 107 12.696 -4.762 -6.401 14.994 0.000 26 21 (g) -43 22 0 35 35 108 104 -3.006 -9.000 -452.525 452.625 0.000 27 -5 (bbar) -51 14 0 66 66 0 109 43.316 18.956 -5.175 47.806 4.800 28 21 (g) -51 14 0 68 68 109 102 14.299 7.648 -8.281 18.208 0.000 29 6 (t) -52 13 13 65 65 102 0 -74.647 -22.554 4.141 184.713 167.395 30 21 (g) -41 37 37 36 21 110 107 0.000 0.000 45.575 45.575 0.000 31 2 (u) -42 38 0 22 22 108 0 0.000 0.000 -678.456 678.456 0.000 32 22 (gamma) -44 23 23 39 39 0 0 -22.105 19.420 -177.707 180.126 0.000 33 2 (u) -44 24 24 40 40 105 0 13.982 -4.527 -34.857 37.830 0.330 34 21 (g) -44 25 25 41 41 104 107 15.197 -2.957 -9.620 18.227 0.000 35 21 (g) -44 26 26 42 42 108 104 -2.977 -8.979 -449.057 449.156 0.000 36 21 (g) -43 30 0 43 43 110 105 -4.097 -2.957 38.359 38.691 0.000 37 21 (g) -42 90 90 30 30 110 107 0.000 0.000 45.575 45.575 0.000 38 2 (u) -41 121 121 44 31 111 0 -0.000 -0.000 -934.218 934.218 0.000 39 22 (gamma) -44 32 32 122 122 0 0 -23.380 19.256 -177.761 180.323 0.000 40 2 (u) -44 33 33 85 86 105 0 13.724 -4.560 -34.931 37.807 0.330 41 21 (g) -44 34 34 51 51 104 107 15.097 -2.970 -9.686 18.181 0.000 42 21 (g) -44 35 35 49 50 108 104 -6.177 -9.391 -449.352 449.492 0.000 43 21 (g) -44 36 36 87 87 110 105 -4.098 -2.957 38.348 38.680 0.000 44 21 (g) -43 38 0 60 61 111 108 4.833 0.622 -255.262 255.309 0.000 45 21 (g) -31 52 0 47 48 114 113 0.000 0.000 3.596 3.596 0.000 46 -1 (dbar) -31 53 53 47 48 0 112 0.000 0.000 -5.441 5.441 0.000 47 21 (g) -33 45 46 54 54 114 112 3.894 -1.565 -2.329 4.800 0.000 48 -1 (dbar) -33 45 46 55 55 0 113 -3.894 1.565 0.484 4.238 0.330 49 21 (g) -51 42 0 62 62 108 115 -4.482 -7.339 -441.472 441.556 0.000 50 21 (g) -51 42 0 82 83 115 104 -1.161 -2.157 -8.222 8.579 0.000 51 21 (g) -52 41 41 88 89 104 107 14.564 -2.865 -9.343 17.539 0.000 52 21 (g) -41 204 204 56 45 114 116 0.000 -0.000 139.236 139.236 0.000 53 -1 (dbar) -42 353 353 46 46 0 112 0.000 0.000 -5.441 5.441 0.000 54 21 (g) -44 47 47 202 203 114 112 3.679 -2.823 -2.222 5.142 0.000 55 -1 (dbar) -44 48 48 59 59 0 113 -4.305 -0.837 1.056 4.523 0.330 56 21 (g) -43 52 0 57 58 113 116 0.626 3.660 134.961 135.012 0.000 57 -1 (dbar) -51 56 0 356 356 0 116 1.198 1.155 116.343 116.355 0.330 58 1 (d) -51 56 0 136 137 113 0 -0.748 2.470 18.660 18.840 0.330 59 -1 (dbar) -52 55 55 138 138 0 113 -4.129 -0.803 1.014 4.340 0.330 60 1 (d) -51 44 0 127 127 111 0 2.238 -1.884 -164.162 164.188 0.330 61 -1 (dbar) -51 44 0 99 99 0 108 2.140 1.760 -135.964 135.992 0.330 62 21 (g) -52 49 49 84 84 108 115 -4.026 -6.593 -396.609 396.684 0.000 63 2 (u) -42 75 75 11 11 106 0 -0.000 -0.000 157.153 157.153 0.000 64 -1 (dbar) -41 104 104 69 12 0 117 0.000 0.000 -158.192 158.192 0.000 65 6 (t) -44 29 29 72 72 102 0 -75.727 -23.058 4.613 185.226 167.395 66 -5 (bbar) -44 27 27 106 106 0 109 42.999 18.808 -5.496 47.497 4.800 67 21 (g) -44 15 15 73 74 106 101 17.007 -4.061 34.246 38.451 0.000 68 21 (g) -44 28 28 70 71 109 102 14.141 7.574 -8.391 18.104 0.000 69 21 (g) -43 64 0 78 78 101 117 1.581 0.737 -26.011 26.069 0.000 70 21 (g) -51 68 0 108 108 109 118 12.253 4.979 -5.782 14.435 0.000 71 21 (g) -51 68 0 79 80 118 102 1.552 2.452 -2.494 3.826 0.000 72 6 (t) -52 65 65 81 81 102 0 -75.392 -22.915 4.498 185.068 167.395 73 21 (g) -51 67 0 76 77 119 101 11.239 -3.585 26.758 29.243 0.000 74 21 (g) -51 67 0 94 95 106 119 5.768 -0.476 8.874 10.595 0.000 75 2 (u) -53 96 96 63 63 106 0 -0.000 0.000 158.540 158.540 0.000 76 21 (g) -51 73 0 107 107 119 120 11.530 -4.191 26.450 29.157 0.000 77 21 (g) -51 73 0 112 112 120 101 -0.250 0.625 -0.374 0.770 0.000 78 21 (g) -52 69 69 109 109 101 117 1.539 0.718 -25.328 25.385 0.000 79 21 (g) -51 71 0 102 102 118 121 2.044 1.204 -1.277 2.694 0.000 80 21 (g) -51 71 0 100 101 121 102 -1.482 0.450 -0.555 1.645 0.000 81 6 (t) -52 72 72 105 105 102 0 -74.402 -22.117 3.836 184.555 167.395 82 21 (g) -51 50 0 128 128 122 104 -2.115 -2.761 -20.194 20.491 0.000 83 21 (g) -51 50 0 130 130 115 122 0.776 0.313 -5.516 5.579 0.000 84 21 (g) -52 62 62 97 98 108 115 -3.849 -6.303 -379.122 379.193 0.000 85 2 (u) -51 40 0 123 123 123 0 5.420 -0.355 -13.337 14.405 0.330 86 21 (g) -51 40 0 93 93 105 123 8.297 -4.210 -21.537 23.460 0.000 87 21 (g) -52 43 43 91 92 110 105 -4.092 -2.952 38.291 38.622 0.000 88 21 (g) -51 51 0 124 124 104 125 15.150 -2.419 -8.751 17.662 0.000 89 21 (g) -51 51 0 132 132 125 107 -0.586 -0.446 0.344 0.813 0.000 90 21 (g) -53 120 0 37 37 110 107 0.000 -0.000 46.511 46.511 0.000 91 21 (g) -51 87 0 126 126 110 126 -2.637 -0.850 27.708 27.846 0.000 92 21 (g) -51 87 0 133 133 126 105 -1.434 -2.113 10.529 10.834 0.000 93 21 (g) -52 86 86 131 131 105 123 8.276 -4.200 -21.483 23.402 0.000 94 21 (g) -51 74 0 111 111 127 119 3.417 -1.392 4.925 6.154 0.000 95 21 (g) -51 74 0 114 114 106 127 2.351 0.916 6.227 6.718 0.000 96 2 (u) -53 103 0 75 75 106 0 -0.000 0.000 160.818 160.818 0.000 97 -3 (sbar) -51 84 0 125 125 0 115 -1.166 -4.095 -206.770 206.814 0.500 98 3 (s) -51 84 0 134 134 108 0 -2.515 -2.069 -182.850 182.880 0.500 99 -1 (dbar) -52 61 61 129 129 0 108 1.972 1.622 -125.465 125.491 0.330 100 -1 (dbar) -51 80 0 113 113 0 102 0.060 0.570 -1.639 1.767 0.330 101 1 (d) -51 80 0 115 115 121 0 -0.682 0.386 0.547 1.011 0.330 102 21 (g) -52 79 79 110 110 118 121 1.184 0.698 -0.740 1.561 0.000 103 2 (u) -41 216 216 116 96 128 0 0.000 0.000 167.364 167.364 0.000 104 -1 (dbar) -42 281 281 64 64 0 117 -0.000 0.000 -158.192 158.192 0.000 105 6 (t) -44 81 81 282 282 102 0 -75.019 -21.991 3.660 184.786 167.395 106 -5 (bbar) -44 66 66 240 240 0 109 42.861 18.836 -5.354 47.367 4.800 107 21 (g) -44 76 76 119 119 119 120 11.348 -4.153 26.499 29.124 0.000 108 21 (g) -44 70 70 156 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2.465 2.487 0.000 538 21 (g) -71 414 414 543 563 150 183 -0.881 -2.329 8.857 9.213 0.492 539 21 (g) -71 330 330 543 563 126 150 -0.616 0.128 3.650 3.704 0.000 540 21 (g) -71 315 315 543 563 182 126 -1.614 0.015 19.699 19.765 0.000 541 21 (g) -71 413 413 543 563 110 182 0.038 0.399 15.775 15.780 0.119 542 -1 (dbar) -71 356 356 543 563 0 110 2.511 0.851 116.539 116.570 0.330 543 213 (rho+) -83 529 542 669 670 0 0 4.067 -0.810 -10.518 11.331 0.752 544 113 (rho0) -83 529 542 671 672 0 0 3.259 -1.321 -7.040 7.915 0.840 545 313 (K*0) -83 529 542 673 674 0 0 1.224 0.025 -2.894 3.274 0.922 546 221 (eta) -83 529 542 766 768 0 0 1.272 0.069 -3.012 3.316 0.548 547 -311 (Kbar0) -83 529 542 675 675 0 0 2.703 -1.608 -8.333 8.920 0.498 548 223 (omega) -83 529 542 769 771 0 0 0.632 -0.001 -1.873 2.124 0.777 549 111 (pi0) -83 529 542 772 773 0 0 0.213 0.174 0.285 0.418 0.135 550 223 (omega) -83 529 542 774 776 0 0 0.116 -0.450 -0.132 0.915 0.777 551 111 (pi0) -84 529 542 777 778 0 0 0.271 -0.130 1.146 1.193 0.135 552 -213 (rho-) -84 529 542 676 677 0 0 0.070 -0.699 1.692 2.083 0.991 553 211 pi+ 84 529 542 0 0 0 0 -0.696 0.009 2.372 2.476 0.140 554 113 (rho0) -84 529 542 678 679 0 0 -0.776 -0.216 1.359 1.762 0.780 555 -211 pi- 84 529 542 0 0 0 0 0.497 -0.270 2.915 2.973 0.140 556 213 (rho+) -84 529 542 680 681 0 0 -0.959 -0.309 9.989 10.090 1.011 557 111 (pi0) -84 529 542 779 780 0 0 -0.045 -0.451 9.741 9.752 0.135 558 111 (pi0) -84 529 542 781 782 0 0 0.079 0.175 0.604 0.648 0.135 559 111 (pi0) -84 529 542 783 784 0 0 -0.816 -0.365 9.194 9.238 0.135 560 -213 (rho-) -84 529 542 682 683 0 0 -0.011 0.217 10.822 10.852 0.777 561 211 pi+ 84 529 542 0 0 0 0 0.543 0.605 23.954 23.969 0.140 562 2112 n0 84 529 542 0 0 0 0 0.359 -0.098 21.032 21.056 0.940 563 -2112 nbar0 84 529 542 0 0 0 0 1.033 0.577 71.375 71.391 0.940 564 1 (d) -71 316 316 569 585 173 0 2.223 -2.073 -192.311 192.336 0.330 565 21 (g) -71 341 341 569 585 111 173 -0.007 0.224 -16.273 16.275 0.000 566 21 (g) -71 354 354 569 585 160 111 4.075 -3.326 -1.204 5.396 0.000 567 21 (g) -71 361 361 569 585 114 160 0.593 0.176 -0.175 0.643 0.000 568 -2 (ubar) -71 367 367 569 585 0 114 0.094 -0.320 75.655 75.656 0.330 569 311 (K0) -83 564 568 684 684 0 0 1.364 -1.065 -97.032 97.048 0.498 570 -323 (K*-) -83 564 568 685 686 0 0 -0.052 -0.043 -23.821 23.836 0.825 571 211 pi+ 83 564 568 0 0 0 0 0.812 -0.621 -60.039 60.048 0.140 572 111 (pi0) -83 564 568 785 786 0 0 -0.174 -0.011 -2.577 2.586 0.135 573 221 (eta) -83 564 568 787 788 0 0 -0.030 0.090 -8.295 8.313 0.548 574 -213 (rho-) -83 564 568 687 688 0 0 0.818 -0.331 -8.042 8.204 1.358 575 223 (omega) -83 564 568 789 791 0 0 -0.369 0.204 -3.738 3.833 0.735 576 223 (omega) -83 564 568 792 794 0 0 0.470 -0.250 -3.553 3.672 0.760 577 213 (rho+) -83 564 568 689 690 0 0 0.645 -1.015 -0.320 1.470 0.782 578 -211 pi- 84 564 568 0 0 0 0 0.338 -0.272 -0.868 0.980 0.140 579 223 (omega) -84 564 568 795 797 0 0 0.350 -0.163 -0.620 1.079 0.794 580 211 pi+ 84 564 568 0 0 0 0 1.669 -0.457 -1.034 2.021 0.140 581 -213 (rho-) -84 564 568 691 692 0 0 1.048 -1.275 0.749 2.238 1.312 582 213 (rho+) -84 564 568 693 694 0 0 0.124 -0.043 13.389 13.415 0.820 583 -211 pi- 84 564 568 0 0 0 0 -0.374 0.338 8.434 8.450 0.140 584 221 (eta) -84 564 568 798 799 0 0 0.750 -0.326 50.988 50.997 0.548 585 111 (pi0) -84 564 568 800 801 0 0 -0.411 -0.078 2.069 2.115 0.135 586 2 (u) -71 366 366 602 635 129 0 -0.134 -0.682 3460.541 3460.541 0.330 587 21 (g) -71 324 324 602 635 167 129 0.819 0.194 76.219 76.224 0.000 588 21 (g) -71 339 339 602 635 107 167 0.121 0.228 1.523 1.545 0.000 589 21 (g) -71 326 326 602 635 190 107 -0.106 0.348 0.150 0.394 0.000 590 21 (g) -71 420 420 602 635 186 190 -0.277 0.045 3.689 3.722 0.410 591 21 (g) -71 348 348 602 635 125 186 -0.004 -0.720 0.694 1.000 0.000 592 21 (g) -71 349 349 602 635 188 125 0.673 -0.330 -0.154 0.765 0.000 593 21 (g) -71 332 332 602 635 145 188 8.195 -0.882 -5.472 9.893 0.000 594 21 (g) -71 419 419 602 635 134 145 3.147 -0.522 -0.191 3.222 0.410 595 21 (g) -71 327 327 602 635 137 134 2.308 -0.375 -1.509 2.783 0.000 596 21 (g) -71 328 328 602 635 104 137 0.493 -0.417 -2.470 2.553 0.000 597 21 (g) -71 350 350 602 635 189 104 -0.383 -0.648 -2.598 2.705 0.000 598 21 (g) -71 317 317 602 635 122 189 -1.452 -1.943 -16.239 16.419 0.000 599 21 (g) -71 319 319 602 635 141 122 0.783 -0.342 -5.494 5.560 0.000 600 21 (g) -71 329 329 602 635 115 141 -0.133 0.229 -21.817 21.818 0.000 601 -3 (sbar) -71 314 314 602 635 0 115 -1.062 -3.631 -184.893 184.932 0.500 602 221 (eta) -83 586 601 802 804 0 0 -0.072 -0.192 1029.273 1029.274 0.548 603 213 (rho+) -83 586 601 695 696 0 0 0.252 -0.432 826.675 826.676 0.774 604 -211 pi- 83 586 601 0 0 0 0 -0.105 0.144 1311.419 1311.419 0.140 605 321 K+ 83 586 601 0 0 0 0 -0.095 -0.114 264.782 264.782 0.494 606 -311 (Kbar0) -83 586 601 697 697 0 0 0.485 -0.184 42.142 42.148 0.498 607 -211 pi- 83 586 601 0 0 0 0 -0.222 0.379 19.087 19.092 0.140 608 211 pi+ 83 586 601 0 0 0 0 0.236 -0.112 14.652 14.655 0.140 609 223 (omega) -83 586 601 805 807 0 0 -0.046 0.259 16.065 16.087 0.800 610 111 (pi0) -83 586 601 808 809 0 0 0.242 0.329 7.411 7.423 0.135 611 -211 pi- 83 586 601 0 0 0 0 0.061 -0.493 3.185 3.227 0.140 612 331 (eta') -83 586 601 810 812 0 0 0.198 0.259 5.542 5.633 0.958 613 223 (omega) -83 586 601 813 815 0 0 -0.033 -0.097 0.847 1.162 0.788 614 2212 p+ 83 586 601 0 0 0 0 -0.189 0.047 0.519 1.090 0.938 615 -2112 nbar0 83 586 601 0 0 0 0 0.360 -0.294 0.190 1.065 0.940 616 -211 pi- 83 586 601 0 0 0 0 0.837 0.067 0.416 0.947 0.140 617 321 K+ 83 586 601 0 0 0 0 2.307 -0.543 -1.913 3.085 0.494 618 -323 (K*-) -83 586 601 698 699 0 0 1.391 -0.399 -0.287 1.774 0.986 619 211 pi+ 83 586 601 0 0 0 0 6.096 -0.964 -3.742 7.219 0.140 620 221 (eta) -84 586 601 816 818 0 0 0.784 -0.219 0.086 0.985 0.548 621 -211 pi- 84 586 601 0 0 0 0 0.705 -0.117 -0.398 0.830 0.140 622 323 (K*+) -84 586 601 700 701 0 0 0.601 -0.235 -1.089 1.555 0.903 623 -323 (K*-) -84 586 601 702 703 0 0 0.505 -0.120 -2.005 2.262 0.910 624 111 (pi0) -84 586 601 819 821 0 0 -0.222 -0.211 -0.320 0.463 0.135 625 321 K+ 84 586 601 0 0 0 0 0.255 -0.325 -2.766 2.840 0.494 626 -311 (Kbar0) -84 586 601 704 704 0 0 -0.077 -0.485 -2.166 2.277 0.498 627 -211 pi- 84 586 601 0 0 0 0 -0.098 0.112 -0.164 0.262 0.140 628 211 pi+ 84 586 601 0 0 0 0 0.037 -0.112 -3.992 3.996 0.140 629 -211 pi- 84 586 601 0 0 0 0 0.138 -0.620 -3.253 3.318 0.140 630 221 (eta) -84 586 601 822 823 0 0 0.356 -0.022 -2.181 2.277 0.548 631 213 (rho+) -84 586 601 705 706 0 0 -1.053 -1.457 -14.001 14.143 0.865 632 311 (K0) -84 586 601 707 707 0 0 0.434 -0.086 -20.569 20.580 0.498 633 -313 (K*bar0) -84 586 601 708 709 0 0 -0.411 -0.132 -22.216 22.238 0.878 634 -211 pi- 84 586 601 0 0 0 0 0.099 0.110 -1.745 1.757 0.140 635 321 K+ 84 586 601 0 0 0 0 -0.768 -3.187 -157.501 157.536 0.494 636 2112 n0 91 427 0 0 0 0 0 -0.430 1.083 -2250.372 2250.373 0.940 637 211 pi+ 91 427 0 0 0 0 0 -0.383 0.061 -454.339 454.340 0.140 638 211 pi+ 91 431 0 0 0 0 0 -0.035 0.757 -0.087 0.776 0.140 639 -211 pi- 91 431 0 0 0 0 0 0.574 0.311 0.259 0.716 0.140 640 -211 pi- 91 432 0 0 0 0 0 -0.108 0.370 -0.069 0.416 0.140 641 111 (pi0) -91 432 0 824 825 0 0 -0.031 -0.274 -0.071 0.315 0.135 642 211 pi+ 91 445 0 0 0 0 0 -1.331 -0.798 0.574 1.660 0.140 643 111 (pi0) -91 445 0 826 827 0 0 -1.700 0.172 0.307 1.741 0.135 644 -311 (Kbar0) -91 449 0 710 710 0 0 -0.702 -0.831 -68.052 68.062 0.498 645 -211 pi- 91 449 0 0 0 0 0 0.053 -0.394 -13.973 13.979 0.140 646 -211 pi- 91 460 0 0 0 0 0 1.018 0.061 -0.795 1.301 0.140 647 111 (pi0) -91 460 0 828 829 0 0 0.776 0.760 -0.447 1.182 0.135 648 211 pi+ 91 472 0 0 0 0 0 -1.595 0.572 -2.092 2.696 0.140 649 111 (pi0) -91 472 0 830 831 0 0 -2.537 2.193 -2.713 4.315 0.135 650 130 K_L0 91 475 475 0 0 0 0 -0.997 0.840 -1.315 1.917 0.498 651 -321 K- 91 476 0 0 0 0 0 -0.691 0.906 -1.382 1.858 0.494 652 211 pi+ 91 476 0 0 0 0 0 -0.473 0.141 -0.909 1.044 0.140 653 -211 pi- 91 484 0 0 0 0 0 -0.275 0.069 -5.645 5.654 0.140 654 111 (pi0) -91 484 0 832 833 0 0 0.460 -0.359 -7.341 7.365 0.135 655 310 (K_S0) -91 502 502 834 835 0 0 2.824 -1.183 3.867 4.958 0.498 656 130 K_L0 91 503 503 0 0 0 0 1.532 -0.985 4.500 4.880 0.498 657 -211 pi- 91 505 0 0 0 0 0 0.426 0.132 2.105 2.156 0.140 658 111 (pi0) -91 505 0 836 837 0 0 0.585 -0.742 3.464 3.593 0.135 659 211 pi+ 91 506 0 0 0 0 0 0.215 0.252 3.210 3.230 0.140 660 111 (pi0) -91 506 0 838 839 0 0 0.167 -0.014 0.174 0.276 0.135 661 211 pi+ 91 507 0 0 0 0 0 0.418 0.431 1.360 1.494 0.140 662 -211 pi- 91 507 0 0 0 0 0 0.443 0.135 4.690 4.715 0.140 663 -211 pi- 91 520 0 0 0 0 0 -0.295 -1.012 0.717 1.282 0.140 664 111 (pi0) -91 520 0 840 841 0 0 0.416 -0.902 0.330 1.055 0.135 665 211 pi+ 91 525 0 0 0 0 0 -4.289 3.094 3.123 6.143 0.140 666 -211 pi- 91 525 0 0 0 0 0 -0.208 0.265 0.153 0.395 0.140 667 211 pi+ 91 528 0 0 0 0 0 -10.219 6.599 5.840 13.495 0.140 668 -211 pi- 91 528 0 0 0 0 0 -5.245 3.921 3.738 7.542 0.140 669 211 pi+ 91 543 0 0 0 0 0 1.495 -0.597 -3.601 3.947 0.140 670 111 (pi0) -91 543 0 842 843 0 0 2.572 -0.213 -6.916 7.383 0.135 671 211 pi+ 91 544 0 0 0 0 0 2.878 -0.877 -5.773 6.512 0.140 672 -211 pi- 91 544 0 0 0 0 0 0.381 -0.445 -1.267 1.403 0.140 673 321 K+ 91 545 0 0 0 0 0 0.604 0.171 -1.051 1.320 0.494 674 -211 pi- 91 545 0 0 0 0 0 0.620 -0.146 -1.842 1.954 0.140 675 130 K_L0 91 547 547 0 0 0 0 2.703 -1.608 -8.333 8.920 0.498 676 -211 pi- 91 552 0 0 0 0 0 -0.263 -0.773 1.338 1.573 0.140 677 111 (pi0) -91 552 0 844 845 0 0 0.333 0.074 0.355 0.510 0.135 678 211 pi+ 91 554 0 0 0 0 0 -0.742 -0.213 0.595 0.985 0.140 679 -211 pi- 91 554 0 0 0 0 0 -0.034 -0.003 0.764 0.777 0.140 680 211 pi+ 91 556 0 0 0 0 0 -0.101 -0.146 6.018 6.022 0.140 681 111 (pi0) -91 556 0 846 847 0 0 -0.858 -0.163 3.971 4.068 0.135 682 -211 pi- 91 560 0 0 0 0 0 -0.167 0.448 6.591 6.610 0.140 683 111 (pi0) -91 560 0 848 849 0 0 0.155 -0.230 4.231 4.243 0.135 684 310 (K_S0) -91 569 569 850 851 0 0 1.364 -1.065 -97.032 97.048 0.498 685 -311 (Kbar0) -91 570 0 711 711 0 0 -0.046 -0.160 -10.478 10.491 0.498 686 -211 pi- 91 570 0 0 0 0 0 -0.007 0.117 -13.343 13.344 0.140 687 -211 pi- 91 574 0 0 0 0 0 -0.341 -0.142 -2.940 2.966 0.140 688 111 (pi0) -91 574 0 852 853 0 0 1.159 -0.190 -5.102 5.238 0.135 689 211 pi+ 91 577 0 0 0 0 0 0.363 -0.837 -0.519 1.059 0.140 690 111 (pi0) -91 577 0 854 855 0 0 0.282 -0.178 0.199 0.411 0.135 691 -211 pi- 91 581 0 0 0 0 0 1.022 -1.487 0.801 1.979 0.140 692 111 (pi0) -91 581 0 856 857 0 0 0.025 0.212 -0.052 0.258 0.135 693 211 pi+ 91 582 0 0 0 0 0 0.161 -0.043 12.992 12.994 0.140 694 111 (pi0) -91 582 0 858 859 0 0 -0.037 -0.000 0.397 0.421 0.135 695 211 pi+ 91 603 0 0 0 0 0 -0.030 0.182 185.420 185.420 0.140 696 111 (pi0) -91 603 0 860 861 0 0 0.282 -0.613 641.255 641.255 0.135 697 130 K_L0 91 606 606 0 0 0 0 0.485 -0.184 42.142 42.148 0.498 698 -321 K- 91 618 0 0 0 0 0 1.256 -0.505 -0.441 1.507 0.494 699 111 (pi0) -91 618 0 862 863 0 0 0.135 0.106 0.154 0.267 0.135 700 311 (K0) -91 622 0 712 712 0 0 0.337 -0.246 -1.075 1.255 0.498 701 211 pi+ 91 622 0 0 0 0 0 0.265 0.011 -0.014 0.300 0.140 702 -311 (Kbar0) -91 623 0 713 713 0 0 0.433 0.199 -1.400 1.560 0.498 703 -211 pi- 91 623 0 0 0 0 0 0.072 -0.319 -0.605 0.702 0.140 704 310 (K_S0) -91 626 626 864 865 0 0 -0.077 -0.485 -2.166 2.277 0.498 705 211 pi+ 91 631 0 0 0 0 0 -0.167 -0.881 -7.498 7.553 0.140 706 111 (pi0) -91 631 0 866 867 0 0 -0.886 -0.575 -6.503 6.590 0.135 707 130 K_L0 91 632 632 0 0 0 0 0.434 -0.086 -20.569 20.580 0.498 708 -321 K- 91 633 0 0 0 0 0 -0.564 -0.150 -18.438 18.454 0.494 709 211 pi+ 91 633 0 0 0 0 0 0.153 0.018 -3.779 3.784 0.140 710 310 (K_S0) -91 644 644 868 869 0 0 -0.702 -0.831 -68.052 68.062 0.498 711 310 (K_S0) -91 685 685 870 871 0 0 -0.046 -0.160 -10.478 10.491 0.498 712 130 K_L0 91 700 700 0 0 0 0 0.337 -0.246 -1.075 1.255 0.498 713 130 K_L0 91 702 702 0 0 0 0 0.433 0.199 -1.400 1.560 0.498 714 22 gamma 91 439 0 0 0 0 0 0.168 -0.201 0.719 0.765 0.000 715 22 gamma 91 439 0 0 0 0 0 0.046 -0.086 0.105 0.143 0.000 716 22 gamma 91 440 0 0 0 0 0 0.353 0.035 0.562 0.665 0.000 717 22 gamma 91 440 0 0 0 0 0 -0.031 -0.078 1.314 1.316 0.000 718 211 pi+ 91 443 0 0 0 0 0 0.182 0.020 0.262 0.349 0.140 719 -211 pi- 91 443 0 0 0 0 0 0.042 0.179 0.264 0.351 0.140 720 111 (pi0) -91 443 0 872 873 0 0 -0.338 0.214 0.297 0.516 0.135 721 22 gamma 91 444 0 0 0 0 0 0.017 -0.001 0.082 0.084 0.000 722 22 gamma 91 444 0 0 0 0 0 -0.084 -0.253 0.363 0.451 0.000 723 22 gamma 91 450 0 0 0 0 0 -0.618 -0.293 -35.227 35.233 0.000 724 22 gamma 91 450 0 0 0 0 0 -0.466 -0.236 -33.651 33.655 0.000 725 211 pi+ 91 451 0 0 0 0 0 -0.242 -0.051 -29.286 29.288 0.140 726 -211 pi- 91 451 0 0 0 0 0 -0.043 0.106 -11.422 11.423 0.140 727 111 (pi0) -91 451 0 874 875 0 0 -0.056 0.113 -20.260 20.261 0.135 728 22 gamma 91 453 0 0 0 0 0 0.360 0.612 -48.638 48.643 0.000 729 22 gamma 91 453 0 0 0 0 0 0.150 0.127 -15.325 15.326 0.000 730 211 pi+ 91 462 0 0 0 0 0 1.502 0.768 -0.274 1.715 0.140 731 -211 pi- 91 462 0 0 0 0 0 1.234 0.390 -0.314 1.339 0.140 732 111 (pi0) -91 462 0 876 877 0 0 4.751 2.304 -1.504 5.492 0.135 733 111 (pi0) -91 463 0 878 879 0 0 1.120 0.434 -0.067 1.211 0.135 734 2212 p+ 91 463 0 0 0 0 0 6.360 2.498 -0.858 6.950 0.938 735 111 (pi0) -91 463 0 880 881 0 0 1.156 0.436 -0.047 1.243 0.135 736 -3122 (Lambdabar0) -91 463 0 882 883 0 0 8.305 3.425 -0.749 9.083 1.116 737 -323 (K*-) -91 463 0 884 885 0 0 8.232 3.724 -0.987 9.133 0.896 738 -421 (Dbar0) -91 463 0 886 887 0 0 13.896 6.098 -1.998 15.420 1.865 739 -511 (Bbar0) -91 470 0 888 889 0 0 -28.334 19.827 -35.199 49.626 5.280 740 22 gamma 91 470 0 0 0 0 0 -0.347 0.197 -0.372 0.545 0.000 741 22 gamma 91 486 0 0 0 0 0 -0.010 0.090 0.060 0.109 0.000 742 22 gamma 91 486 0 0 0 0 0 -0.396 0.059 -0.889 0.975 0.000 743 22 gamma 91 488 0 0 0 0 0 0.222 1.041 -0.232 1.089 0.000 744 22 gamma 91 488 0 0 0 0 0 0.041 0.724 -0.148 0.740 0.000 745 211 pi+ 91 498 0 0 0 0 0 0.614 -0.182 1.809 1.924 0.140 746 -211 pi- 91 498 0 0 0 0 0 0.275 -0.075 0.527 0.616 0.140 747 111 (pi0) -91 498 0 890 891 0 0 0.146 -0.424 1.137 1.230 0.135 748 22 gamma 91 499 0 0 0 0 0 0.143 -0.050 0.373 0.402 0.000 749 22 gamma 91 499 0 0 0 0 0 1.927 -0.581 3.788 4.289 0.000 750 22 gamma 91 500 0 0 0 0 0 0.400 -0.166 1.026 1.114 0.000 751 22 gamma 91 500 0 0 0 0 0 2.061 -1.149 6.016 6.462 0.000 752 111 (pi0) -91 504 0 892 893 0 0 0.394 0.066 0.752 0.862 0.135 753 111 (pi0) -91 504 0 894 895 0 0 0.632 0.148 1.369 1.521 0.135 754 221 (eta) -91 504 0 896 898 0 0 0.646 0.062 2.089 2.255 0.548 755 22 gamma 91 515 0 0 0 0 0 -0.842 -4.497 2.320 5.129 0.000 756 22 gamma 91 515 0 0 0 0 0 -1.164 -5.437 2.863 6.254 0.000 757 22 gamma 91 516 0 0 0 0 0 -1.306 -6.782 3.741 7.855 0.000 758 22 gamma 91 516 0 0 0 0 0 -2.205 -11.533 6.160 13.260 0.000 759 22 gamma 91 517 0 0 0 0 0 -1.334 -7.445 3.827 8.477 0.000 760 22 gamma 91 517 0 0 0 0 0 -2.856 -15.043 7.870 17.216 0.000 761 111 (pi0) -91 519 0 899 900 0 0 -0.116 -0.587 0.284 0.676 0.135 762 111 (pi0) -91 519 0 901 902 0 0 -0.813 -4.130 2.007 4.665 0.135 763 111 (pi0) -91 519 0 903 904 0 0 -0.251 -1.202 0.607 1.376 0.135 764 22 gamma 91 521 0 0 0 0 0 -0.013 -0.236 0.070 0.246 0.000 765 22 gamma 91 521 0 0 0 0 0 -0.447 -2.980 1.307 3.285 0.000 766 111 (pi0) -91 546 0 905 906 0 0 0.312 0.022 -0.550 0.647 0.135 767 111 (pi0) -91 546 0 907 908 0 0 0.762 -0.028 -1.749 1.912 0.135 768 111 (pi0) -91 546 0 909 910 0 0 0.197 0.075 -0.714 0.757 0.135 769 211 pi+ 91 548 0 0 0 0 0 0.181 0.085 -0.131 0.277 0.140 770 -211 pi- 91 548 0 0 0 0 0 0.304 0.084 -1.136 1.187 0.140 771 111 (pi0) -91 548 0 911 912 0 0 0.146 -0.170 -0.606 0.660 0.135 772 22 gamma 91 549 0 0 0 0 0 0.075 0.088 0.035 0.120 0.000 773 22 gamma 91 549 0 0 0 0 0 0.138 0.087 0.249 0.298 0.000 774 211 pi+ 91 550 0 0 0 0 0 0.063 -0.289 -0.290 0.437 0.140 775 -211 pi- 91 550 0 0 0 0 0 -0.065 -0.184 0.174 0.296 0.140 776 111 (pi0) -91 550 0 913 914 0 0 0.117 0.023 -0.015 0.181 0.135 777 22 gamma 91 551 0 0 0 0 0 0.119 0.014 0.426 0.442 0.000 778 22 gamma 91 551 0 0 0 0 0 0.152 -0.144 0.721 0.750 0.000 779 22 gamma 91 557 0 0 0 0 0 -0.023 -0.365 8.711 8.718 0.000 780 22 gamma 91 557 0 0 0 0 0 -0.022 -0.086 1.030 1.034 0.000 781 22 gamma 91 558 0 0 0 0 0 0.053 -0.004 0.123 0.134 0.000 782 22 gamma 91 558 0 0 0 0 0 0.026 0.179 0.481 0.514 0.000 783 22 gamma 91 559 0 0 0 0 0 -0.102 -0.098 1.532 1.538 0.000 784 22 gamma 91 559 0 0 0 0 0 -0.714 -0.267 7.662 7.700 0.000 785 22 gamma 91 572 0 0 0 0 0 -0.119 0.041 -2.059 2.063 0.000 786 22 gamma 91 572 0 0 0 0 0 -0.055 -0.053 -0.517 0.523 0.000 787 22 gamma 91 573 0 0 0 0 0 0.186 -0.124 -4.872 4.878 0.000 788 22 gamma 91 573 0 0 0 0 0 -0.216 0.213 -3.422 3.436 0.000 789 211 pi+ 91 575 0 0 0 0 0 -0.164 0.182 -1.693 1.717 0.140 790 -211 pi- 91 575 0 0 0 0 0 -0.216 -0.018 -1.888 1.905 0.140 791 111 (pi0) -91 575 0 915 916 0 0 0.011 0.040 -0.157 0.211 0.135 792 211 pi+ 91 576 0 0 0 0 0 0.090 -0.140 -1.512 1.528 0.140 793 -211 pi- 91 576 0 0 0 0 0 0.355 -0.246 -1.235 1.316 0.140 794 111 (pi0) -91 576 0 917 918 0 0 0.025 0.136 -0.805 0.828 0.135 795 211 pi+ 91 579 0 0 0 0 0 0.115 -0.240 -0.371 0.478 0.140 796 -211 pi- 91 579 0 0 0 0 0 0.070 -0.044 0.088 0.185 0.140 797 111 (pi0) -91 579 0 919 920 0 0 0.164 0.121 -0.337 0.416 0.135 798 22 gamma 91 584 0 0 0 0 0 0.807 -0.342 41.225 41.234 0.000 799 22 gamma 91 584 0 0 0 0 0 -0.057 0.016 9.763 9.763 0.000 800 22 gamma 91 585 0 0 0 0 0 -0.087 -0.004 0.222 0.238 0.000 801 22 gamma 91 585 0 0 0 0 0 -0.324 -0.074 1.847 1.877 0.000 802 111 (pi0) -91 602 0 921 922 0 0 -0.080 -0.223 459.309 459.309 0.135 803 111 (pi0) -91 602 0 923 924 0 0 0.032 -0.054 291.909 291.909 0.135 804 111 (pi0) -91 602 0 925 926 0 0 -0.024 0.086 278.056 278.056 0.135 805 211 pi+ 91 609 0 0 0 0 0 -0.163 -0.030 6.862 6.866 0.140 806 -211 pi- 91 609 0 0 0 0 0 -0.131 0.018 2.733 2.739 0.140 807 111 (pi0) -91 609 0 927 928 0 0 0.248 0.272 6.470 6.482 0.135 808 22 gamma 91 610 0 0 0 0 0 0.049 0.154 3.558 3.561 0.000 809 22 gamma 91 610 0 0 0 0 0 0.193 0.175 3.853 3.862 0.000 810 211 pi+ 91 612 0 0 0 0 0 0.098 -0.036 0.801 0.820 0.140 811 -211 pi- 91 612 0 0 0 0 0 -0.037 0.144 2.047 2.057 0.140 812 221 (eta) -91 612 0 929 931 0 0 0.137 0.150 2.694 2.757 0.548 813 211 pi+ 91 613 0 0 0 0 0 0.103 0.123 0.178 0.277 0.140 814 -211 pi- 91 613 0 0 0 0 0 0.004 -0.093 0.626 0.648 0.140 815 111 (pi0) -91 613 0 932 933 0 0 -0.140 -0.127 0.043 0.236 0.135 816 211 pi+ 91 620 0 0 0 0 0 0.166 0.012 -0.096 0.237 0.140 817 -211 pi- 91 620 0 0 0 0 0 0.580 -0.126 0.185 0.637 0.140 818 22 gamma 91 620 0 0 0 0 0 0.039 -0.104 -0.004 0.111 0.000 819 22 gamma 91 624 0 0 0 0 0 -0.035 -0.120 -0.145 0.191 0.000 820 11 e- 91 624 0 0 0 0 0 -0.079 -0.039 -0.075 0.116 0.001 821 -11 e+ 91 624 0 0 0 0 0 -0.107 -0.053 -0.101 0.156 0.001 822 22 gamma 91 630 0 0 0 0 0 0.016 -0.244 -0.915 0.947 0.000 823 22 gamma 91 630 0 0 0 0 0 0.341 0.222 -1.266 1.330 0.000 824 22 gamma 91 641 0 0 0 0 0 -0.011 -0.039 0.038 0.055 0.000 825 22 gamma 91 641 0 0 0 0 0 -0.021 -0.235 -0.109 0.260 0.000 826 22 gamma 91 643 0 0 0 0 0 -1.678 0.174 0.287 1.711 0.000 827 22 gamma 91 643 0 0 0 0 0 -0.022 -0.002 0.020 0.030 0.000 828 22 gamma 91 647 0 0 0 0 0 0.002 -0.003 -0.011 0.012 0.000 829 22 gamma 91 647 0 0 0 0 0 0.774 0.762 -0.436 1.171 0.000 830 22 gamma 91 649 0 0 0 0 0 -1.254 1.114 -1.438 2.210 0.000 831 22 gamma 91 649 0 0 0 0 0 -1.283 1.079 -1.274 2.106 0.000 832 22 gamma 91 654 0 0 0 0 0 0.081 -0.010 -0.818 0.822 0.000 833 22 gamma 91 654 0 0 0 0 0 0.379 -0.350 -6.523 6.543 0.000 834 111 (pi0) -91 655 0 934 935 0 0 1.803 -0.748 2.768 3.390 0.135 835 111 (pi0) -91 655 0 936 937 0 0 1.021 -0.435 1.100 1.568 0.135 836 22 gamma 91 658 0 0 0 0 0 0.345 -0.331 1.682 1.749 0.000 837 22 gamma 91 658 0 0 0 0 0 0.240 -0.411 1.782 1.844 0.000 838 22 gamma 91 660 0 0 0 0 0 0.016 -0.050 0.016 0.055 0.000 839 22 gamma 91 660 0 0 0 0 0 0.151 0.037 0.158 0.221 0.000 840 22 gamma 91 664 0 0 0 0 0 0.230 -0.423 0.222 0.530 0.000 841 22 gamma 91 664 0 0 0 0 0 0.186 -0.479 0.108 0.525 0.000 842 22 gamma 91 670 0 0 0 0 0 1.955 -0.134 -5.392 5.738 0.000 843 22 gamma 91 670 0 0 0 0 0 0.616 -0.079 -1.524 1.646 0.000 844 22 gamma 91 677 0 0 0 0 0 0.296 0.049 0.356 0.466 0.000 845 22 gamma 91 677 0 0 0 0 0 0.037 0.025 -0.001 0.044 0.000 846 22 gamma 91 681 0 0 0 0 0 -0.119 0.019 0.451 0.466 0.000 847 22 gamma 91 681 0 0 0 0 0 -0.740 -0.182 3.520 3.602 0.000 848 22 gamma 91 683 0 0 0 0 0 0.032 -0.164 2.535 2.541 0.000 849 22 gamma 91 683 0 0 0 0 0 0.123 -0.066 1.696 1.702 0.000 850 211 pi+ 91 684 0 0 0 0 0 0.475 -0.525 -31.255 31.264 0.140 851 -211 pi- 91 684 0 0 0 0 0 0.889 -0.539 -65.776 65.785 0.140 852 22 gamma 91 688 0 0 0 0 0 0.412 -0.119 -1.682 1.736 0.000 853 22 gamma 91 688 0 0 0 0 0 0.748 -0.070 -3.421 3.502 0.000 854 22 gamma 91 690 0 0 0 0 0 0.150 -0.169 0.108 0.251 0.000 855 22 gamma 91 690 0 0 0 0 0 0.132 -0.009 0.091 0.160 0.000 856 22 gamma 91 692 0 0 0 0 0 -0.048 0.118 -0.056 0.139 0.000 857 22 gamma 91 692 0 0 0 0 0 0.073 0.095 0.004 0.119 0.000 858 22 gamma 91 694 0 0 0 0 0 0.003 -0.011 -0.008 0.014 0.000 859 22 gamma 91 694 0 0 0 0 0 -0.040 0.010 0.405 0.407 0.000 860 22 gamma 91 696 0 0 0 0 0 0.214 -0.555 531.893 531.893 0.000 861 22 gamma 91 696 0 0 0 0 0 0.068 -0.058 109.362 109.362 0.000 862 22 gamma 91 699 0 0 0 0 0 0.025 0.090 0.118 0.151 0.000 863 22 gamma 91 699 0 0 0 0 0 0.109 0.016 0.035 0.116 0.000 864 211 pi+ 91 704 0 0 0 0 0 -0.035 -0.010 -0.190 0.239 0.140 865 -211 pi- 91 704 0 0 0 0 0 -0.042 -0.475 -1.977 2.038 0.140 866 22 gamma 91 706 0 0 0 0 0 -0.818 -0.485 -5.714 5.793 0.000 867 22 gamma 91 706 0 0 0 0 0 -0.068 -0.090 -0.789 0.797 0.000 868 211 pi+ 91 710 0 0 0 0 0 -0.265 -0.379 -40.990 40.993 0.140 869 -211 pi- 91 710 0 0 0 0 0 -0.437 -0.452 -27.061 27.069 0.140 870 211 pi+ 91 711 0 0 0 0 0 -0.015 -0.002 -8.589 8.590 0.140 871 -211 pi- 91 711 0 0 0 0 0 -0.031 -0.158 -1.889 1.901 0.140 872 22 gamma 91 720 0 0 0 0 0 -0.118 0.150 0.110 0.221 0.000 873 22 gamma 91 720 0 0 0 0 0 -0.221 0.063 0.186 0.296 0.000 874 22 gamma 91 727 0 0 0 0 0 0.021 0.039 -1.825 1.826 0.000 875 22 gamma 91 727 0 0 0 0 0 -0.076 0.074 -18.435 18.436 0.000 876 22 gamma 91 732 0 0 0 0 0 3.141 1.589 -1.026 3.667 0.000 877 22 gamma 91 732 0 0 0 0 0 1.610 0.715 -0.478 1.826 0.000 878 22 gamma 91 733 0 0 0 0 0 0.812 0.356 -0.094 0.891 0.000 879 22 gamma 91 733 0 0 0 0 0 0.309 0.078 0.028 0.320 0.000 880 22 gamma 91 735 0 0 0 0 0 0.823 0.258 0.006 0.863 0.000 881 22 gamma 91 735 0 0 0 0 0 0.332 0.178 -0.052 0.381 0.000 882 -2112 nbar0 91 736 0 0 0 0 0 7.089 2.928 -0.743 7.763 0.940 883 111 (pi0) -91 736 0 938 939 0 0 1.216 0.497 -0.006 1.320 0.135 884 -321 K- 91 737 0 0 0 0 0 7.537 3.518 -0.789 8.369 0.494 885 111 (pi0) -91 737 0 940 941 0 0 0.696 0.206 -0.198 0.764 0.135 886 221 (eta) -91 738 0 942 943 0 0 6.575 2.008 -0.693 6.931 0.548 887 111 (pi0) -91 738 0 944 945 0 0 7.322 4.090 -1.305 8.488 0.135 888 -433 (D*_s-) -91 739 0 946 947 0 0 -6.653 4.520 -9.546 12.660 2.112 889 413 (D*+) -91 739 0 948 949 0 0 -21.682 15.307 -25.652 36.966 2.010 890 22 gamma 91 747 0 0 0 0 0 0.080 -0.107 0.462 0.480 0.000 891 22 gamma 91 747 0 0 0 0 0 0.066 -0.318 0.676 0.750 0.000 892 22 gamma 91 752 0 0 0 0 0 0.230 0.013 0.299 0.377 0.000 893 22 gamma 91 752 0 0 0 0 0 0.164 0.053 0.454 0.485 0.000 894 22 gamma 91 753 0 0 0 0 0 0.012 0.006 0.108 0.109 0.000 895 22 gamma 91 753 0 0 0 0 0 0.620 0.142 1.261 1.412 0.000 896 211 pi+ 91 754 0 0 0 0 0 0.095 0.006 0.647 0.668 0.140 897 -211 pi- 91 754 0 0 0 0 0 0.270 0.146 0.730 0.804 0.140 898 111 (pi0) -91 754 0 950 951 0 0 0.282 -0.089 0.712 0.783 0.135 899 22 gamma 91 761 0 0 0 0 0 -0.057 -0.499 0.199 0.540 0.000 900 22 gamma 91 761 0 0 0 0 0 -0.059 -0.088 0.085 0.136 0.000 901 22 gamma 91 762 0 0 0 0 0 -0.141 -0.820 0.342 0.899 0.000 902 22 gamma 91 762 0 0 0 0 0 -0.671 -3.310 1.665 3.765 0.000 903 22 gamma 91 763 0 0 0 0 0 -0.119 -0.587 0.221 0.638 0.000 904 22 gamma 91 763 0 0 0 0 0 -0.133 -0.615 0.386 0.738 0.000 905 22 gamma 91 766 0 0 0 0 0 0.203 0.012 -0.467 0.509 0.000 906 22 gamma 91 766 0 0 0 0 0 0.110 0.010 -0.083 0.138 0.000 907 22 gamma 91 767 0 0 0 0 0 0.410 -0.082 -0.972 1.058 0.000 908 22 gamma 91 767 0 0 0 0 0 0.352 0.053 -0.777 0.854 0.000 909 22 gamma 91 768 0 0 0 0 0 0.024 0.043 -0.337 0.340 0.000 910 22 gamma 91 768 0 0 0 0 0 0.173 0.032 -0.377 0.416 0.000 911 22 gamma 91 771 0 0 0 0 0 0.141 -0.088 -0.298 0.341 0.000 912 22 gamma 91 771 0 0 0 0 0 0.005 -0.082 -0.308 0.319 0.000 913 22 gamma 91 776 0 0 0 0 0 0.137 0.045 -0.032 0.147 0.000 914 22 gamma 91 776 0 0 0 0 0 -0.019 -0.021 0.017 0.034 0.000 915 22 gamma 91 791 0 0 0 0 0 0.013 -0.049 -0.044 0.067 0.000 916 22 gamma 91 791 0 0 0 0 0 -0.002 0.089 -0.113 0.144 0.000 917 22 gamma 91 794 0 0 0 0 0 -0.007 0.004 -0.409 0.409 0.000 918 22 gamma 91 794 0 0 0 0 0 0.033 0.132 -0.397 0.419 0.000 919 22 gamma 91 797 0 0 0 0 0 0.121 0.047 -0.098 0.163 0.000 920 22 gamma 91 797 0 0 0 0 0 0.043 0.074 -0.239 0.254 0.000 921 22 gamma 91 802 0 0 0 0 0 0.031 -0.096 204.138 204.138 0.000 922 22 gamma 91 802 0 0 0 0 0 -0.112 -0.127 255.171 255.171 0.000 923 22 gamma 91 803 0 0 0 0 0 0.064 -0.003 68.206 68.207 0.000 924 22 gamma 91 803 0 0 0 0 0 -0.032 -0.051 223.703 223.703 0.000 925 22 gamma 91 804 0 0 0 0 0 -0.033 -0.030 64.649 64.649 0.000 926 22 gamma 91 804 0 0 0 0 0 0.010 0.116 213.407 213.407 0.000 927 22 gamma 91 807 0 0 0 0 0 0.204 0.152 3.563 3.572 0.000 928 22 gamma 91 807 0 0 0 0 0 0.044 0.119 2.907 2.909 0.000 929 111 (pi0) -91 812 0 952 953 0 0 0.067 -0.007 0.384 0.413 0.135 930 111 (pi0) -91 812 0 954 955 0 0 0.070 -0.000 0.509 0.531 0.135 931 111 (pi0) -91 812 0 956 957 0 0 -0.000 0.157 1.800 1.812 0.135 932 22 gamma 91 815 0 0 0 0 0 -0.113 -0.118 0.086 0.184 0.000 933 22 gamma 91 815 0 0 0 0 0 -0.027 -0.009 -0.043 0.052 0.000 934 22 gamma 91 834 0 0 0 0 0 1.683 -0.729 2.623 3.201 0.000 935 22 gamma 91 834 0 0 0 0 0 0.120 -0.020 0.144 0.189 0.000 936 22 gamma 91 835 0 0 0 0 0 0.038 -0.038 0.086 0.102 0.000 937 22 gamma 91 835 0 0 0 0 0 0.983 -0.397 1.013 1.466 0.000 938 22 gamma 91 883 0 0 0 0 0 1.143 0.442 0.020 1.226 0.000 939 22 gamma 91 883 0 0 0 0 0 0.073 0.055 -0.026 0.094 0.000 940 22 gamma 91 885 0 0 0 0 0 0.370 0.179 -0.102 0.423 0.000 941 22 gamma 91 885 0 0 0 0 0 0.326 0.027 -0.095 0.341 0.000 942 22 gamma 91 886 0 0 0 0 0 4.239 1.559 -0.517 4.546 0.000 943 22 gamma 91 886 0 0 0 0 0 2.336 0.449 -0.175 2.385 0.000 944 22 gamma 91 887 0 0 0 0 0 6.572 3.628 -1.185 7.600 0.000 945 22 gamma 91 887 0 0 0 0 0 0.749 0.462 -0.120 0.888 0.000 946 -431 (D_s-) -91 888 0 958 960 0 0 -6.163 4.206 -8.651 11.593 1.968 947 22 gamma 91 888 0 0 0 0 0 -0.490 0.313 -0.895 1.068 0.000 948 421 (D0) -91 889 0 961 966 0 0 -19.979 14.069 -23.588 34.014 1.865 949 211 pi+ 91 889 0 0 0 0 0 -1.703 1.238 -2.064 2.951 0.140 950 22 gamma 91 898 0 0 0 0 0 0.209 -0.007 0.537 0.576 0.000 951 22 gamma 91 898 0 0 0 0 0 0.073 -0.081 0.175 0.207 0.000 952 22 gamma 91 929 0 0 0 0 0 0.065 -0.038 0.092 0.119 0.000 953 22 gamma 91 929 0 0 0 0 0 0.002 0.031 0.292 0.294 0.000 954 22 gamma 91 930 0 0 0 0 0 0.056 -0.032 0.484 0.488 0.000 955 22 gamma 91 930 0 0 0 0 0 0.014 0.032 0.025 0.043 0.000 956 22 gamma 91 931 0 0 0 0 0 -0.046 0.039 1.013 1.014 0.000 957 22 gamma 91 931 0 0 0 0 0 0.046 0.118 0.788 0.798 0.000 958 13 mu- 91 946 0 0 0 0 0 -2.436 2.161 -4.073 5.216 0.106 959 -14 nu_mubar 91 946 0 0 0 0 0 -0.241 0.341 -0.653 0.775 0.000 960 331 (eta') -91 946 0 967 968 0 0 -3.486 1.704 -3.925 5.602 0.958 961 311 (K0) -91 948 0 969 969 0 0 -3.361 2.476 -4.228 5.962 0.498 962 211 pi+ 91 948 0 0 0 0 0 -2.961 1.886 -3.586 5.021 0.140 963 -211 pi- 91 948 0 0 0 0 0 -2.777 1.923 -3.084 4.576 0.140 964 111 (pi0) -91 948 0 970 971 0 0 -6.491 4.773 -7.886 11.275 0.135 965 111 (pi0) -91 948 0 972 973 0 0 -2.371 1.746 -2.789 4.058 0.135 966 111 (pi0) -91 948 0 974 975 0 0 -2.018 1.265 -2.015 3.123 0.135 967 113 (rho0) -91 960 0 976 977 0 0 -3.006 1.322 -3.527 4.870 0.706 968 22 gamma 91 960 0 0 0 0 0 -0.480 0.382 -0.398 0.731 0.000 969 130 K_L0 91 961 961 0 0 0 0 -3.361 2.476 -4.228 5.962 0.498 970 22 gamma 91 964 0 0 0 0 0 -5.145 3.835 -6.232 8.945 0.000 971 22 gamma 91 964 0 0 0 0 0 -1.345 0.938 -1.655 2.330 0.000 972 22 gamma 91 965 0 0 0 0 0 -1.173 0.836 -1.452 2.045 0.000 973 22 gamma 91 965 0 0 0 0 0 -1.199 0.910 -1.337 2.013 0.000 974 22 gamma 91 966 0 0 0 0 0 -0.555 0.338 -0.473 0.804 0.000 975 22 gamma 91 966 0 0 0 0 0 -1.463 0.927 -1.542 2.319 0.000 976 211 pi+ 91 967 0 0 0 0 0 -1.612 0.933 -2.337 2.992 0.140 977 -211 pi- 91 967 0 0 0 0 0 -1.394 0.389 -1.190 1.879 0.140 Charge sum: 2.000 Momentum sum: 0.000 -0.000 -0.000 8000.000 8000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame PYTHIA Warning in SpaceShower::pT2nextQCD: weight above unity PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again PYTHIA Warning in TimeShower::findMEcorr: ME weight above PS one PYTHIA Error in SpaceShower::pT2nearQCDthreshold: stuck in loop *------- PYTHIA Event and Cross Section Statistics --------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |------------------------------------------------------------------------------------------------------------| | | | | | First hard process: | | | | | | | | g g -> t tbar 601 | 8010 611 555 | 3.375e-13 1.423e-14 | | q qbar -> t tbar 602 | 2055 189 150 | 8.782e-14 5.506e-15 | | q q -> t q (t-channel W+-) 603 | 7576 329 268 | 1.577e-13 8.161e-15 | | f fbar -> t tbar (s-channel gamma*/Z0) 604 | 16 2 2 | 7.600e-16 3.020e-16 | | f fbar -> t qbar (s-channel W+-) 605 | 328 28 25 | 1.111e-14 1.494e-15 | | | | | | sum | 17985 1159 1000 | 5.949e-13 2.347e-14 | | | | | |------------------------------------------------------------------------------------------------------------| | | | | | Second hard process: | | | | | | | | q g -> q gamma (udscb) 201 | 4402 1074 926 | 5.498e-13 2.198e-14 | | q qbar -> g gamma 202 | 290 84 73 | 4.366e-14 3.322e-15 | | g g -> g gamma 203 | 1 1 1 | 1.053e-15 1.054e-15 | | | | | | sum | 4693 1159 1000 | 5.945e-13 2.355e-14 | | | | | |------------------------------------------------------------------------------------------------------------| | | | Uncombined cross sections for the two event sets were 2.131e-07 and 9.731e-05 mb, respectively, combined | | using a sigma(nonDiffractive) of 5.212e+01 mb and an impact-parameter enhancement factor of 1.732e+00. | | | *------- End PYTHIA Event and Cross Section Statistics -----------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Error in Pythia::next: hadronLevel failed; try again | | 2 Error in SpaceShower::pT2nearQCDthreshold: stuck in loop | | 1 Error in StringFragmentation::fragment: stuck in joining | | 1 Warning in SpaceShower::pT2nextQCD: weight above unity | | 7 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | 1 Warning in TimeShower::findMEcorr: ME weight above PS one | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* From pythia.info: sigma = 5.947e-13 +- 2.876e-14 2013-09-20 16:03 pT first collision 4.50*10^ 1 3 4.35*10^ 1 X 4.20*10^ 1 X 4.05*10^ 1 X 3.90*10^ 1 X3 3 3.75*10^ 1 XX X 3.60*10^ 1 XX X 3.45*10^ 1 XX X 3.30*10^ 1 XX X3 XX 3 3.15*10^ 1 XX XX XX X 3.00*10^ 1 3XX X XX XX 3X3 X 2.85*10^ 1 XXX X7 XX XX XXX X 2.70*10^ 1 XXX XXXXX XX XXX X 3 X 2.55*10^ 1 XXX XXXXX XX XXX X7 X X 2.40*10^ 1 XXXXXXXXX XX XXX XX X X 2.25*10^ 1 7 XXXXXXXXX7XX7XXX XX X X 2.10*10^ 1 XXXXXXXXXXXXXXXXXX XXXX3XX3 X 1.95*10^ 1 XXXXXXXXXXXXXXXXXX7XXXXXXXX X 1.80*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX X 1.65*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX X 1.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX 3 3X 1.35*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX77 X XX 1.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX3XX X 1.05*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXX 7X 0.90*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXX 3XX 0.75*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXX7 XXX 7 7 0.60*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 XXX3X X 3 3 0.45*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXX X X7 X 7 0.30*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3X3XXXX X3 X X 0.15*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 777777 7 X X7 7 7 Contents *10^ 1 0000022243232233233223213222222211101111200001100000000000000000000000000000000000000000000000000000 *10^ 0 0000021948408782233292990516017083364214175380257337335423253430320011111100103031000000010100000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^ 1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^ 0 0482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 1000 Mean = 9.9278e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 9.9200e+02 Rms = 5.9909e+01 Overflow = 8.0000e+00 High edge = 4.0000e+02 2013-09-20 16:03 pT second collision 2.50*10^ 2 6 2.40*10^ 2 X 2.30*10^ 2 X 2.20*10^ 2 X 2.10*10^ 2 X 2.00*10^ 2 XX 1.90*10^ 2 XX 1.80*10^ 2 XX 1.70*10^ 2 XX 1.60*10^ 2 XX 1.50*10^ 2 XX 1.40*10^ 2 XX2 1.30*10^ 2 XXX 1.20*10^ 2 XXX 1.10*10^ 2 XXX 1.00*10^ 2 XXX4 0.90*10^ 2 XXXX 0.80*10^ 2 XXXX 0.70*10^ 2 XXXX8 0.60*10^ 2 XXXXX7 0.50*10^ 2 XXXXXX 0.40*10^ 2 XXXXXX9 0.30*10^ 2 XXXXXXX XX 0.20*10^ 2 XXXXXXX8XX22 0.10*10^ 2 XXXXXXXXXXXX8693423416112 332 1 1 1 1 Contents *10^ 2 0000000000221000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000403965313311000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000000602487980022869342341611200332010000001000100100000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^ 1 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^ 0 0246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 1000 Mean = 2.8232e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+03 Rms = 1.0305e+01 Overflow = 0.0000e+00 High edge = 2.0000e+02 2013-09-20 16:03 pT first-second collision 4.35*10^ 1 7 4.20*10^ 1 X 4.05*10^ 1 X 3.90*10^ 1 X 3 X 3.75*10^ 1 X X X 3.60*10^ 1 XX X 3X X 3.45*10^ 1 XX X XX X 3.30*10^ 1 XX X XX X 3.15*10^ 1 XX X XX X 7 3.00*10^ 1 XX X XX XX X 2.85*10^ 1 XX X XX 7XX X 2.70*10^ 1 XXX X XX XXX X 2.55*10^ 1 XXX7X XX XXX X 7 7 2.40*10^ 1 XXXXX XXXXXXX3X 3X X XX 2.25*10^ 1 XXXXX XXXXXXXXX7 XX X XX 2.10*10^ 1 3XXXXX XXXXXXXXXXXXX X XX 3 1.95*10^ 1 XXXXXX7XXXXXXXXXXXXX X XX X 1.80*10^ 1 3XXXXXXXXXXXXXXXXXXXXXX XXXX 3 1.65*10^ 1 XXXXXXXXXXXXXXXXXXXXXXX7XXXX X 1.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX3 X 1.35*10^ 1 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 7 1.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX X 1.05*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 7XX X 7 0.90*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 3X3 0.75*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 XXX 7 7 0.60*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 XXX3X X 3 3X 0.45*10^ 1 7 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7XXXXX X X XX 0.30*10^ 1 3XX3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX XX 3 3 33 0.15*10^ 1 7 7 7 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX7XX X7X 7 77XX 7777 Contents *10^ 1 0000000000000000000000011223323133222432222231212212110111001000010000000000000000000000000000000000 *10^ 0 0000001000001010233243937076956958448303421318564580409027993754808573733503331560212001011220111100 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge ------------------------- *10^ 2 1000000000000000000000000000000000000000000000000011111111111111111111111112222222222222222222222222 *10^ 1 0998887766655444332221100000112223344455666778889900011222334445566677888990001122233444556667788899 *10^ 0 0628406284062840628406284048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 1000 Mean = 7.0024e+01 Underflow = 0.0000e+00 Low edge = -1.0000e+02 All chan = 9.8800e+02 Rms = 5.8907e+01 Overflow = 1.2000e+01 High edge = 3.0000e+02 2013-09-20 16:03 number of multiparton interactions 1.00*10^ 2 33 0.96*10^ 2 XX 0.92*10^ 2 XX 0.88*10^ 2 8X XXX 0.84*10^ 2 XXX XXX 0.80*10^ 2 XXX XXX5 0.76*10^ 2 XXX5XXXX8 0.72*10^ 2 XXXXXXXXX3 0.68*10^ 2 XXXXXXXXXX 0.64*10^ 2 XXXXXXXXXX 0.60*10^ 2 XXXXXXXXXX 0.56*10^ 2 XXXXXXXXXX 0.52*10^ 2 XXXXXXXXXX 0.48*10^ 2 XXXXXXXXXX 0.44*10^ 2 XXXXXXXXXX3 0.40*10^ 2 XXXXXXXXXXXX 0.36*10^ 2 XXXXXXXXXXXX 0.32*10^ 2 XXXXXXXXXXXX5 0.28*10^ 2 XXXXXXXXXXXXX 0.24*10^ 2 XXXXXXXXXXXXX7 0.20*10^ 2 XXXXXXXXXXXXXX 0.16*10^ 2 XXXXXXXXXXXXXX 0.12*10^ 2 XXXXXXXXXXXXXX 7 0.08*10^ 2 XXXXXXXXXXXXXXXX 0.04*10^ 2 XXXXXXXXXXXXXXXX8X35 Contents *10^ 1 0088878997764432010000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0078448778591003813412000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 1 0000000000011111111112222222222333333333344444444445555555555666666666677777777778888888888999999999 *10^ 0 0012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789012345678 *10^-1 5555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555 Entries = 1000 Mean = 7.6220e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+03 Rms = 3.8960e+00 Overflow = 0.0000e+00 High edge = 9.9500e+01 2013-09-20 16:03 b enhancement factor 3.75*10^ 1 7 3.60*10^ 1 XX X X 3.45*10^ 1 XX 7 X X 3.30*10^ 1 X XX X3 X3 3 XX X X 3.15*10^ 1 X XX XX XX X XX7X 7X 3.00*10^ 1 X3 XX3 XX 3 XX X XX XXXX XX 2.85*10^ 1 XX 7XXX XX X XX X XX XXXX XX 2.70*10^ 1 XX XXXXXX XX X XXXX3 X XX3XXXX XX 2.55*10^ 1 XX XXXXXX XX7X XXXXX X XXXXXXX XX 2.40*10^ 1 XX XXXXXX3XXXX XXXXXX XXXXXXXXXXXX 2.25*10^ 1 XX7XXXXXXXXXXX XXXXXX7XXXXXXXXXXXX 2.10*10^ 1 XXXXXXXXXXXXXX3XXXXXXXXXXXXXXXXXXX 1.95*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.80*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.65*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.35*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.05*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.90*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.75*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.60*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.45*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.30*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.15*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 1 3222332222332222233222323323333233100000000000000000000000000000000000000000000000000000000000000000 *10^ 0 3928669773425904772762042066313413200000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-1 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 1000 Mean = 1.7332e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+03 Rms = 1.0094e+00 Overflow = 0.0000e+00 High edge = 1.0000e+01 2013-09-20 16:03 charged multiplicity 6.50*10^ 1 6 6 6.25*10^ 1 X X 6.00*10^ 1 X X 5.75*10^ 1 X 4 X 5.50*10^ 1 X 2 X6X 5.25*10^ 1 4X X 8XXX 5.00*10^ 1 2XXXX XXXX 4.75*10^ 1 4XXXXX XXXX 4.50*10^ 1 XXXXXX XXXX 2 4.25*10^ 1 8XXXXXX XXXX X 4.00*10^ 1 XXXXXXX6XXXX2X 3.75*10^ 1 XXXXXXXXXXXXXX 3.50*10^ 1 6 XXXXXXXXXXXXXX 3.25*10^ 1 X 8XXXXXXXXXXXXXX 3.00*10^ 1 XXXXXXXXXXXXXXXXX 2.75*10^ 1 XXXXXXXXXXXXXXXXX 8 2.50*10^ 1 XXXXXXXXXXXXXXXXX X 2.25*10^ 1 XXXXXXXXXXXXXXXXX8X 2.00*10^ 1 6XXXXXXXXXXXXXXXXXXX62 1.75*10^ 1 4XXXXXXXXXXXXXXXXXXXXXX 1.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXX6 1.25*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXX88 1.00*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXX6 2 0.75*10^ 1 4XXXXXXXXXXXXXXXXXXXXXXXXXXX X 0.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6X 2 0.25*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 4X 4 4 Contents *10^ 1 0000000000011333444565535556342211111000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000055669402268140392644832798422948200130101000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 1 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^ 0 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 1000 Mean = 2.3285e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+03 Rms = 6.7954e+01 Overflow = 0.0000e+00 High edge = 9.9950e+02 pythia8-8.1.80.orig/examples/outref/out100000644000175000017500000023466012217346171016365 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:03:26 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with pbar- at a CM energy of 1.960e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> g g 111 | 9.243e-04 | | g g -> q qbar (uds) 112 | 1.929e-05 | | q g -> q g 113 | 2.225e-03 | | q q(bar)' -> q q(bar)' 114 | 5.402e-04 | | q qbar -> g g 115 | 1.133e-05 | | q qbar -> q' qbar' (uds) 116 | 5.152e-06 | | g g -> c cbar 121 | 6.400e-06 | | q qbar -> c cbar 122 | 1.716e-06 | | g g -> b bbar 123 | 6.288e-06 | | q qbar -> b bbar 124 | 1.700e-06 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 40.89 mb | | | | pT0 = 2.12 gives sigmaInteraction = 136.64 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eCM | 1960.000 | 14000.000 10.00000 | | Beams:idB | -2212 | 2212 | | HadronLevel:all | off | on | | HardQCD:all | on | off | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:pTHatMin | 50.00000 | 0.0 0.0 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- #-------------------------------------------------------------------------- # FastJet release 3.0.5 [fjcore] # M. Cacciari, G.P. Salam and G. Soyez # A software package for jet finding and analysis at colliders # http://fastjet.fr # # Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package # for scientific work and optionally PLB641(2006)57 [hep-ph/0512210]. # # FastJet is provided without warranty under the terms of the GNU GPLv2. # It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code # and 3rd party plugin jet algorithms. See COPYING file for details. #-------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 9.800e+02, e = 9.800e+02, m = 9.383e-01. Beam B: id = -2212, pz = -9.800e+02, e = 9.800e+02, m = 9.383e-01. In 1: id = 21, x = 1.674e-02, pdf = 5.616e+00 at Q2 = 3.757e+03. In 2: id = -2, x = 3.431e-01, pdf = 3.057e-01 at same Q2. Subprocess q g -> q g with code 113 is 2 -> 2. It has sHat = 2.207e+04, tHat = -4.802e+03, uHat = -1.727e+04, pTHat = 6.130e+01, m3Hat = 0.000e+00, m4Hat = 3.300e-01, thetaHat = 9.706e-01, phiHat = 4.191e+00. alphaEM = 7.782e-03, alphaS = 1.445e-01 at Q2 = 3.757e+03. Impact parameter b = 1.308e+00 gives enhancement factor = 2.650e-01. Max pT scale for MPI = 6.130e+01, ISR = 6.130e+01, FSR = 6.130e+01. Number of MPI = 1, ISR = 4, FSRproc = 62, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 1960.000 1960.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 980.000 980.000 0.938 2 -2212 (pbar-) -12 0 0 4 0 0 0 0.000 0.000 -980.000 980.000 0.938 3 21 (g) -21 1 0 5 6 103 102 0.000 0.000 16.408 16.408 0.000 4 -2 (ubar) -21 2 0 5 6 0 101 0.000 0.000 -336.270 336.270 0.000 5 21 g 23 3 4 0 0 103 101 -30.528 -53.153 -60.333 86.008 0.000 6 -2 ubar 23 3 4 0 0 0 102 30.528 53.153 -259.529 266.670 0.330 Charge sum: -0.667 Momentum sum: 0.000 0.000 -319.862 352.678 148.558 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 1960.000 1960.000 1 2212 (p+) -12 0 0 241 0 0 0 0.000 0.000 980.000 980.000 0.938 2 -2212 (pbar-) -12 0 0 242 0 0 0 0.000 0.000 -980.000 980.000 0.938 3 21 (g) -21 7 0 5 6 103 102 0.000 0.000 16.408 16.408 0.000 4 -2 (ubar) -21 8 8 5 6 0 101 0.000 0.000 -336.270 336.270 0.000 5 21 (g) -23 3 4 9 9 103 101 -30.528 -53.153 -60.333 86.008 0.000 6 -2 (ubar) -23 3 4 10 10 0 102 30.528 53.153 -259.529 266.670 0.330 7 21 (g) -41 12 12 11 3 104 102 0.000 0.000 22.579 22.579 0.000 8 -2 (ubar) -42 13 0 4 4 0 101 -0.000 -0.000 -336.270 336.270 0.000 9 21 (g) -44 5 5 14 14 103 101 -29.310 -34.602 -17.943 48.768 0.000 10 -2 (ubar) -44 6 6 15 15 0 102 30.867 58.313 -249.609 258.182 0.330 11 21 (g) -43 7 0 16 16 104 103 -1.557 -23.711 -46.139 51.899 0.000 12 21 (g) -42 18 18 7 7 104 102 0.000 0.000 22.579 22.579 0.000 13 -2 (ubar) -41 19 0 17 8 0 105 -0.000 -0.000 -430.461 430.461 0.000 14 21 (g) -44 9 9 20 20 103 101 -29.954 -36.608 -22.180 52.243 0.000 15 -2 (ubar) -44 10 10 21 21 0 102 25.968 43.042 -281.014 285.475 0.330 16 21 (g) -44 11 11 22 22 104 103 -2.502 -26.659 -51.407 57.963 0.000 17 21 (g) -43 13 0 23 23 101 105 6.488 20.225 -53.282 57.359 0.000 18 21 (g) -42 27 27 12 12 104 102 0.000 0.000 22.579 22.579 0.000 19 -2 (ubar) -41 92 92 24 13 0 106 -0.000 -0.000 -480.936 480.936 0.000 20 21 (g) -44 14 14 33 33 103 101 -30.703 -36.851 -23.125 53.249 0.000 21 -2 (ubar) -44 15 15 28 29 0 102 20.266 41.189 -288.855 292.480 0.330 22 21 (g) -44 16 16 25 26 104 103 -3.603 -27.017 -52.809 59.428 0.000 23 21 (g) -44 17 17 31 32 101 105 5.375 19.863 -54.906 58.635 0.000 24 21 (g) -43 19 0 55 56 105 106 8.666 2.817 -38.664 39.723 0.000 25 21 (g) -51 22 0 40 41 107 103 -7.547 -19.526 -24.227 32.018 0.000 26 21 (g) -51 22 0 34 35 104 107 3.943 -7.492 -27.356 28.636 0.000 27 21 (g) 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102 0.458 8.225 -50.582 51.248 0.000 260 21 g 62 205 205 0 0 139 160 1.310 -0.342 -1.255 1.846 0.000 261 21 g 62 214 214 0 0 164 101 -4.637 -5.590 -2.938 7.835 0.000 262 21 g 62 225 225 0 0 146 120 -0.203 -0.177 -0.046 0.273 0.000 263 21 g 62 238 238 0 0 173 108 1.952 3.705 -32.447 32.716 0.000 264 21 g 62 124 124 0 0 130 122 0.862 -0.034 -3.056 3.176 0.000 265 21 g 62 202 202 0 0 159 135 1.494 1.758 -2.886 3.695 0.000 266 21 g 62 178 178 0 0 151 111 0.144 -0.056 -0.060 0.166 0.000 267 21 g 62 217 217 0 0 111 166 -0.007 1.187 -2.780 3.023 0.000 268 21 g 62 235 235 0 0 171 126 -0.669 -0.532 -0.871 1.220 0.000 269 21 g 62 226 226 0 0 168 127 -0.723 -0.311 -0.676 1.037 0.000 270 21 g 62 222 222 0 0 133 128 -0.168 -0.069 1.294 1.307 0.000 271 21 g 62 142 142 0 0 136 129 -0.147 0.038 -0.039 0.157 0.000 272 21 g 62 208 208 0 0 162 130 2.021 1.308 -8.549 8.882 0.000 273 21 g 62 175 175 0 0 107 150 -0.680 -2.584 -0.879 2.813 0.000 274 21 g 62 231 231 0 0 132 107 0.037 0.052 -0.015 0.065 0.000 275 21 g 62 220 220 0 0 129 167 -0.647 0.233 -0.042 0.689 0.000 276 21 g 62 137 137 0 0 134 114 0.576 4.603 -10.805 11.759 0.000 277 21 g 62 140 140 0 0 135 123 -0.395 0.485 -0.888 1.086 0.000 278 21 g 62 143 143 0 0 102 136 0.353 2.293 -11.527 11.758 0.000 279 21 g 62 146 146 0 0 127 137 -0.475 0.051 -1.615 1.685 0.000 280 21 g 62 149 149 0 0 118 139 2.544 -1.915 -3.444 4.690 0.000 281 21 g 62 229 229 0 0 158 169 0.067 -0.816 -3.555 3.648 0.000 282 21 g 62 211 211 0 0 163 106 -0.200 -0.234 -5.140 5.149 0.000 283 21 g 62 186 186 0 0 117 143 0.320 0.957 -8.401 8.461 0.000 284 21 g 62 169 169 0 0 104 147 -0.100 0.082 0.131 0.184 0.000 285 21 g 62 193 193 0 0 108 156 0.516 1.314 -5.192 5.381 0.000 286 2 u 62 223 223 0 0 101 0 -1.096 -1.346 -1.611 2.391 0.330 287 21 g 62 170 170 0 0 147 144 0.559 -1.218 -1.083 1.723 0.000 288 21 g 62 181 181 0 0 103 152 -2.768 -4.034 -2.834 5.654 0.000 289 21 g 62 176 176 0 0 150 131 0.091 -0.119 -0.314 0.348 0.000 290 21 g 62 179 179 0 0 124 151 1.247 0.351 -6.168 6.302 0.000 291 21 g 62 182 182 0 0 152 148 -3.632 -4.777 -2.307 6.429 0.000 292 21 g 62 234 234 0 0 154 117 0.374 0.346 -1.466 1.552 0.000 293 21 g 62 207 207 0 0 115 155 -0.159 -0.255 -0.187 0.354 0.000 294 -2 ubar 62 191 191 0 0 0 105 0.326 1.640 -4.303 4.628 0.330 295 21 g 62 194 194 0 0 156 145 1.825 1.799 -7.459 7.887 0.000 296 21 g 62 213 213 0 0 142 157 0.010 0.063 -0.762 0.765 0.000 297 21 g 62 200 200 0 0 140 158 0.191 -0.051 -0.413 0.458 0.000 298 21 g 62 203 203 0 0 126 159 -0.094 0.041 -0.571 0.581 0.000 299 21 g 62 206 206 0 0 160 115 -0.135 0.080 -0.127 0.202 0.000 300 21 g 62 209 209 0 0 116 162 1.914 2.336 -11.217 11.617 0.000 301 21 g 62 212 212 0 0 157 163 0.493 0.303 -12.098 12.112 0.000 302 21 g 62 215 215 0 0 119 164 -2.039 -1.996 -1.649 3.295 0.000 303 21 g 62 218 218 0 0 166 125 1.248 2.199 -6.882 7.332 0.000 304 21 g 62 221 221 0 0 167 133 0.105 0.148 0.505 0.537 0.000 305 -2 ubar 62 224 224 0 0 0 146 -1.359 -1.037 -2.008 2.657 0.330 306 21 g 62 227 227 0 0 110 168 0.231 -0.147 -0.185 0.331 0.000 307 21 g 62 230 230 0 0 169 132 -0.205 -0.203 -4.876 4.885 0.000 308 21 g 62 233 233 0 0 170 154 0.876 1.910 -8.174 8.440 0.000 309 21 g 62 236 236 0 0 109 171 0.054 0.136 0.043 0.152 0.000 310 21 g 62 239 239 0 0 121 173 -0.077 0.083 -0.682 0.692 0.000 311 2103 ud_1 63 1 0 0 0 0 104 0.621 -1.268 946.334 946.335 0.771 312 2 u 63 1 0 0 0 128 0 0.172 -1.723 5.114 5.410 0.330 313 -2103 ud_1bar 63 2 0 0 0 106 0 -0.078 -0.104 -482.679 482.680 0.771 Charge sum: 0.000 Momentum sum: 0.000 0.000 -0.000 1960.000 1960.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Warning in SpaceShower::pT2nextQCD: weight above unity PYTHIA Warning in MultipartonInteractions::pTnext: weight above unity *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> g g 111 | 5595 896 283 | 4.646e-05 2.408e-06 | | g g -> q qbar (uds) 112 | 123 33 9 | 1.116e-06 3.368e-07 | | q g -> q g 113 | 13603 1616 517 | 8.763e-05 3.365e-06 | | q q(bar)' -> q q(bar)' 114 | 3284 458 182 | 2.991e-05 1.875e-06 | | q qbar -> g g 115 | 79 16 6 | 8.121e-07 2.877e-07 | | q qbar -> q' qbar' (uds) 116 | 30 7 0 | 0.000e+00 0.000e+00 | | g g -> c cbar 121 | 36 9 0 | 0.000e+00 0.000e+00 | | q qbar -> c cbar 122 | 11 3 1 | 1.955e-07 1.955e-07 | | g g -> b bbar 123 | 33 4 2 | 6.435e-07 3.491e-07 | | q qbar -> b bbar 124 | 12 5 0 | 0.000e+00 0.000e+00 | | | | | | sum | 22806 3047 1000 | 1.668e-04 4.582e-06 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Warning in MultipartonInteractions::pTnext: weight above unity | | 5 Warning in SpaceShower::pT2nextQCD: weight above unity | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:03 trial pT spectrum 4.05*10^ 3 2 3.90*10^ 3 X 3.75*10^ 3 X 3.60*10^ 3 X 3.45*10^ 3 7X 3.30*10^ 3 XX 3.15*10^ 3 XX 3.00*10^ 3 XX 2.85*10^ 3 XX 2.70*10^ 3 XX8 2.55*10^ 3 XXX 2.40*10^ 3 XXX 2.25*10^ 3 XXX 2.10*10^ 3 XXX 1.95*10^ 3 XXX7 1.80*10^ 3 XXXX 1.65*10^ 3 XXXX 1.50*10^ 3 XXXX5 1.35*10^ 3 XXXXX 1.20*10^ 3 XXXXX2 1.05*10^ 3 XXXXXX 0.90*10^ 3 XXXXXX7 0.75*10^ 3 XXXXXXXX2 0.60*10^ 3 XXXXXXXXX5 0.45*10^ 3 XXXXXXXXXX852 0.30*10^ 3 XXXXXXXXXXXXXX622 1 0.15*10^ 3 XXXXXXXXXXXXXXXXXXXX9977666655444334333333232222322222121111122 111111111111111111111111 Contents *10^ 3 0000000000003321110000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0000000000004968408765433221111111110000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000000369286522173948845633109988766554465543442332333232232212111230121121111100111111112111 *10^ 0 0000000000003678670288351302360111145647192749701148567856469718761691771417619618059988476733350503 Low edge *10^ 2 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^ 1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^ 0 0482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 22806 Mean = 8.2664e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 2.2186e+04 Rms = 5.4652e+01 Overflow = 6.2000e+02 High edge = 4.0000e+02 2013-09-20 16:03 selected pT spectrum (before veto) 7.50*10^ 2 X 7.20*10^ 2 X 6.90*10^ 2 X 6.60*10^ 2 X 6.30*10^ 2 X 6.00*10^ 2 6X 5.70*10^ 2 XX 5.40*10^ 2 XX9 5.10*10^ 2 XXX 4.80*10^ 2 XXX 4.50*10^ 2 XXX 4.20*10^ 2 XXX 3.90*10^ 2 XXX 3.60*10^ 2 XXX 3.30*10^ 2 XXX6 3.00*10^ 2 XXXX 2.70*10^ 2 XXXX 2.40*10^ 2 XXXX6 2.10*10^ 2 XXXXX 1.80*10^ 2 XXXXX2 1.50*10^ 2 XXXXXX 1.20*10^ 2 XXXXXXX 0.90*10^ 2 XXXXXXX84 0.60*10^ 2 XXXXXXXXX52 0.30*10^ 2 XXXXXXXXXXX97732111111111 1 Contents *10^ 2 0000000000005753211000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000008531252874322200000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000000009178870525770186422332422020000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^ 1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^ 0 0482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 3047 Mean = 6.1396e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 3.0470e+03 Rms = 1.3077e+01 Overflow = 0.0000e+00 High edge = 4.0000e+02 2013-09-20 16:03 accepted pT spectrum (after veto) 2.70*10^ 2 1 2.60*10^ 2 X 2.50*10^ 2 X 2.40*10^ 2 X 2.30*10^ 2 X 2.20*10^ 2 X 2.10*10^ 2 X 2.00*10^ 2 6X 1.90*10^ 2 XX6 1.80*10^ 2 XXX 1.70*10^ 2 XXX 1.60*10^ 2 XXX 1.50*10^ 2 XXX 1.40*10^ 2 XXX 1.30*10^ 2 XXX 1.20*10^ 2 XXX 1.10*10^ 2 XXX7 1.00*10^ 2 XXXX 0.90*10^ 2 XXXX 0.80*10^ 2 XXXX4 0.70*10^ 2 XXXXX 0.60*10^ 2 XXXXX 0.50*10^ 2 XXXXX 0.40*10^ 2 XXXXXX4 0.30*10^ 2 XXXXXXX92 0.20*10^ 2 XXXXXXXXX51 0.10*10^ 2 XXXXXXXXXXX74312 1112 2 1 Contents *10^ 2 0000000000001211000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000009680743221100000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000000006167404925174312011120201000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^ 1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^ 0 0482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 1000 Mean = 6.0592e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+03 Rms = 1.2265e+01 Overflow = 0.0000e+00 High edge = 4.0000e+02 2013-09-20 16:03 number of partons before veto 6.00*10^ 2 9 5.80*10^ 2 X 5.60*10^ 2 8X 5.40*10^ 2 XX 5.20*10^ 2 XX1 5.00*10^ 2 XXX 4.80*10^ 2 XXX 4.60*10^ 2 XXX 4.40*10^ 2 XXX 4.20*10^ 2 XXX 4.00*10^ 2 XXX 3.80*10^ 2 XXX8 3.60*10^ 2 9XXXX 3.40*10^ 2 XXXXX 3.20*10^ 2 XXXXX 3.00*10^ 2 XXXXX 2.80*10^ 2 XXXXX 2.60*10^ 2 XXXXX 2.40*10^ 2 XXXXX9 2.20*10^ 2 XXXXXX 2.00*10^ 2 XXXXXX 1.80*10^ 2 XXXXXX 1.60*10^ 2 8XXXXXX 1.40*10^ 2 XXXXXXX8 1.20*10^ 2 XXXXXXXX 1.00*10^ 2 XXXXXXXX 0.80*10^ 2 XXXXXXXX5 0.60*10^ 2 XXXXXXXXX 0.40*10^ 2 XXXXXXXXX7 0.20*10^ 2 XXXXXXXXXX63111 Contents *10^ 2 00135553210000000000 *10^ 1 00555907336310000000 *10^ 0 00686735879427131000 *10^-1 00000000000000000000 Low edge - *10^ 1 00000000000111111111 *10^ 0 00123456789012345678 *10^-1 55555555555555555555 Entries = 3047 Mean = 5.4969e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 3.0470e+03 Rms = 2.1021e+00 Overflow = 0.0000e+00 High edge = 1.9500e+01 2013-09-20 16:03 number of jets before veto 1.00*10^ 3 X 0.96*10^ 3 X 0.92*10^ 3 X 0.88*10^ 3 X 0.84*10^ 3 XX 0.80*10^ 3 XX 0.76*10^ 3 XX2 0.72*10^ 3 XXX 0.68*10^ 3 XXX 0.64*10^ 3 XXX 0.60*10^ 3 XXX 0.56*10^ 3 XXX 0.52*10^ 3 XXX 0.48*10^ 3 XXX 0.44*10^ 3 XXX 0.40*10^ 3 XXX 0.36*10^ 3 XXX 0.32*10^ 3 XXX2 0.28*10^ 3 XXXX 0.24*10^ 3 XXXX 0.20*10^ 3 XXXX 0.16*10^ 3 XXXX2 0.12*10^ 3 XXXXX 0.08*10^ 3 XXXXX1 0.04*10^ 3 XXXXXX31 Contents *10^ 3 00010000000000000000 *10^ 2 00807210000000000000 *10^ 1 00402824100000000000 *10^ 0 00008995321000000000 Low edge - *10^ 1 00000000000111111111 *10^ 0 00123456789012345678 *10^-1 55555555555555555555 Entries = 3047 Mean = 3.3666e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 3.0470e+03 Rms = 1.2342e+00 Overflow = 0.0000e+00 High edge = 1.9500e+01 2013-09-20 16:03 number of partons after veto 2.60*10^ 2 55 2.50*10^ 2 XX 2.40*10^ 2 XX 2.30*10^ 2 XX 2.20*10^ 2 XX 2.10*10^ 2 XX 2.00*10^ 2 XX 1.90*10^ 2 XX6 1.80*10^ 2 XXX 1.70*10^ 2 XXX 1.60*10^ 2 XXX 1.50*10^ 2 XXX 1.40*10^ 2 XXX 1.30*10^ 2 XXX 1.20*10^ 2 9XXX7 1.10*10^ 2 XXXXX 1.00*10^ 2 XXXXX 0.90*10^ 2 XXXXX 0.80*10^ 2 XXXXX 0.70*10^ 2 XXXXX 0.60*10^ 2 XXXXX 0.50*10^ 2 XXXXX7 0.40*10^ 2 XXXXXX 0.30*10^ 2 XXXXXX 0.20*10^ 2 XXXXXX4 0.10*10^ 2 1XXXXXXX5 1 Contents *10^ 2 00012211000000000000 *10^ 1 00015581410000000000 *10^ 0 00195567745010000000 *10^-1 00000000000000000000 Low edge - *10^ 1 00000000000111111111 *10^ 0 00123456789012345678 *10^-1 55555555555555555555 Entries = 1000 Mean = 5.1530e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+03 Rms = 1.4804e+00 Overflow = 0.0000e+00 High edge = 1.9500e+01 2013-09-20 16:03 number of FSR emissions at first ISR emission 2.08*10^ 3 7 2.00*10^ 3 X 1.92*10^ 3 X 1.84*10^ 3 X 1.76*10^ 3 X 1.68*10^ 3 X 1.60*10^ 3 X 1.52*10^ 3 X 1.44*10^ 3 X 1.36*10^ 3 X 1.28*10^ 3 X 1.20*10^ 3 X 1.12*10^ 3 X 1.04*10^ 3 X 0.96*10^ 3 X 0.88*10^ 3 X 0.80*10^ 3 X 0.72*10^ 3 X 0.64*10^ 3 X 0.56*10^ 3 X 0.48*10^ 3 X5 0.40*10^ 3 XX 0.32*10^ 3 XX 0.24*10^ 3 XX 0.16*10^ 3 XX7 0.08*10^ 3 XXX83111 Contents *10^ 3 20000000000000000000 *10^ 2 04100000000000000000 *10^ 1 54362100000000000000 *10^ 0 73221274201000000000 Low edge - *10^ 1 00000000000111111111 *10^ 0 00123456789012345678 *10^-1 55555555555555555555 Entries = 2742 Mean = 4.1335e-01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 2.7410e+03 Rms = 9.3039e-01 Overflow = 1.0000e+00 High edge = 1.9500e+01 pythia8-8.1.80.orig/examples/outref/out160000644000175000017500000012065712217346173016375 0ustar sunsun PYTHIA settings will be read from file main16.cmnd *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:04:55 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> H (SM) 902 | 3.091e-07 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 57.54 mb | | | | pT0 = 3.08 gives sigmaInteraction = 270.41 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | HiggsSM:gg2H | on | off | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberCount | 100 | 1000 0 | | Next:numberShowEvent | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | Stat:showPartonLevel | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products 25 h0(H_1) 1 0 0 125.00000 0.00404 124.79824 125.20176 0.00000e+00 1 1 0 0 0 0 1 0.0000000 100 1 -1 1 1 0.0000000 100 2 -2 2 1 0.0004394 100 3 -3 3 1 0.0267649 100 4 -4 4 1 0.5772432 100 5 -5 5 1 0.0000000 100 6 -6 6 1 0.0000000 100 11 -11 7 1 0.0002207 100 13 -13 8 1 0.0636166 100 15 -15 9 1 0.0854879 100 21 21 10 1 0.0022970 100 22 22 11 1 0.0015480 100 22 23 12 1 0.0266650 100 23 23 13 1 0.2157172 100 24 -24 14 1 0.0000000 103 1000022 1000022 15 1 0.0000000 103 1000023 1000022 16 1 0.0000000 103 1000023 1000023 17 1 0.0000000 103 1000025 1000022 18 1 0.0000000 103 1000025 1000023 19 1 0.0000000 103 1000025 1000025 20 1 0.0000000 103 1000035 1000022 21 1 0.0000000 103 1000035 1000023 22 1 0.0000000 103 1000035 1000025 23 1 0.0000000 103 1000035 1000035 24 1 0.0000000 103 1000024 -1000024 25 1 0.0000000 103 1000024 -1000037 26 1 0.0000000 103 1000037 -1000024 27 1 0.0000000 103 1000037 -1000037 28 1 0.0000000 103 1000001 -1000001 29 1 0.0000000 103 2000001 -2000001 30 1 0.0000000 103 1000001 -2000001 31 1 0.0000000 103 -1000001 2000001 32 1 0.0000000 103 1000002 -1000002 33 1 0.0000000 103 2000002 -2000002 34 1 0.0000000 103 1000002 -2000002 35 1 0.0000000 103 -1000002 2000002 36 1 0.0000000 103 1000003 -1000003 37 1 0.0000000 103 2000003 -2000003 38 1 0.0000000 103 1000003 -2000003 39 1 0.0000000 103 -1000003 2000003 40 1 0.0000000 103 1000004 -1000004 41 1 0.0000000 103 2000004 -2000004 42 1 0.0000000 103 1000004 -2000004 43 1 0.0000000 103 -1000004 2000004 44 1 0.0000000 103 1000005 -1000005 45 1 0.0000000 103 2000005 -2000005 46 1 0.0000000 103 1000005 -2000005 47 1 0.0000000 103 -1000005 2000005 48 1 0.0000000 103 1000006 -1000006 49 1 0.0000000 103 2000006 -2000006 50 1 0.0000000 103 1000006 -2000006 51 1 0.0000000 103 -1000006 2000006 52 1 0.0000000 103 1000011 -1000011 53 1 0.0000000 103 2000011 -2000011 54 1 0.0000000 103 1000011 -2000011 55 1 0.0000000 103 -1000011 2000011 56 1 0.0000000 103 1000012 -1000012 57 1 0.0000000 103 2000012 -2000012 58 1 0.0000000 103 1000012 -2000012 59 1 0.0000000 103 -1000012 2000012 60 1 0.0000000 103 1000013 -1000013 61 1 0.0000000 103 2000013 -2000013 62 1 0.0000000 103 1000013 -2000013 63 1 0.0000000 103 -1000013 2000013 64 1 0.0000000 103 1000014 -1000014 65 1 0.0000000 103 2000014 -2000014 66 1 0.0000000 103 1000014 -2000014 67 1 0.0000000 103 -1000014 2000014 68 1 0.0000000 103 1000015 -1000015 69 1 0.0000000 103 2000015 -2000015 70 1 0.0000000 103 1000015 -2000015 71 1 0.0000000 103 -1000015 2000015 72 1 0.0000000 103 1000016 -1000016 73 1 0.0000000 103 2000016 -2000016 74 1 0.0000000 103 1000016 -2000016 75 1 0.0000000 103 -1000016 2000016 -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. In 1: id = 21, x = 3.775e-03, pdf = 1.694e+01 at Q2 = 1.563e+04. In 2: id = 21, x = 2.112e-02, pdf = 4.577e+00 at same Q2. Subprocess g g -> H (SM) with code 902 is 2 -> 1. It has sHat = 1.563e+04. alphaEM = 7.846e-03, alphaS = 1.283e-01 at Q2 = 1.563e+04. Impact parameter b = 8.974e-01 gives enhancement factor = 9.479e-01. Max pT scale for MPI = 1.400e+04, ISR = 1.400e+04, FSR = 1.400e+04. Number of MPI = 9, ISR = 25, FSRproc = 144, FSRreson = 13. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 21 (g) -21 1 0 5 0 101 102 0.000 0.000 26.423 26.423 0.000 4 21 (g) -21 2 0 5 0 102 101 0.000 0.000 -147.839 147.839 0.000 5 25 (h0(H_1)) -22 3 4 6 7 0 0 0.000 0.000 -121.416 174.261 125.001 6 5 b 23 5 0 0 0 103 0 -49.481 -24.369 -20.278 58.961 4.800 7 -5 bbar 23 5 0 0 0 0 103 49.481 24.369 -101.138 115.300 4.800 Charge sum: 0.000 Momentum sum: 0.000 0.000 -121.416 174.261 125.001 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- Pythia::next(): 100 events have been generated PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame Pythia::next(): 200 events have been generated Pythia::next(): 300 events have been generated PYTHIA Warning in Pythia::check: energy-momentum not quite conserved Pythia::next(): 400 events have been generated PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again Pythia::next(): 500 events have been generated PYTHIA Warning in TimeShower::findMEcorr: ME weight above PS one PYTHIA Warning in TimeShower::pTnext: negative dipole mass. Pythia::next(): 600 events have been generated Pythia::next(): 700 events have been generated Pythia::next(): 800 events have been generated Pythia::next(): 900 events have been generated *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> H (SM) 902 | 10431 1000 1000 | 3.026e-08 7.053e-10 | | | | | | sum | 10431 1000 1000 | 3.026e-08 7.053e-10 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Multiparton Interactions Statistics --------* | | | Note: excludes hardest subprocess if already listed above | | | | Subprocess Code | Times | | | | |-------------------------------------------------------------| | | | | g g -> g g 111 | 5039 | | g g -> q qbar (uds) 112 | 60 | | q g -> q g 113 | 1871 | | q q(bar)' -> q q(bar)' 114 | 126 | | q qbar -> g g 115 | 4 | | q qbar -> q' qbar' (uds) 116 | 0 | | g g -> c cbar 121 | 23 | | q qbar -> c cbar 122 | 0 | | g g -> b bbar 123 | 8 | | q qbar -> b bbar 124 | 0 | | q g -> q gamma (udscb) 201 | 0 | | q qbar -> g gamma 202 | 0 | | g g -> g gamma 203 | 0 | | f fbar -> gamma gamma 204 | 0 | | g g -> gamma gamma 205 | 0 | | f f' -> f f' (t-channel gamma*/Z0) 211 | 0 | | f_1 f_2 -> f_3 f_4 (t-channel W+-) 212 | 0 | | f fbar -> f' fbar' (s-channel gamma*) 223 | 0 | | g g -> ccbar[3S1(1)] g 401 | 0 | | g g -> ccbar[3P0(1)] g 402 | 3 | | g g -> ccbar[3P1(1)] g 403 | 1 | | g g -> ccbar[3P2(1)] g 404 | 2 | | q g -> ccbar[3P0(1)] q 405 | 0 | | q g -> ccbar[3P1(1)] q 406 | 0 | | q g -> ccbar[3P2(1)] q 407 | 0 | | q qbar -> ccbar[3P0(1)] g 408 | 0 | | q qbar -> ccbar[3P1(1)] g 409 | 0 | | q qbar -> ccbar[3P2(1)] g 410 | 0 | | g g -> ccbar[3S1(8)] g 411 | 0 | | g g -> ccbar[1S0(8)] g 412 | 0 | | g g -> ccbar[3PJ(8)] g 413 | 1 | | q g -> ccbar[3S1(8)] q 414 | 0 | | q g -> ccbar[1S0(8)] q 415 | 0 | | q g -> ccbar[3PJ(8)] q 416 | 0 | | q qbar -> ccbar[3S1(8)] g 417 | 0 | | q qbar -> ccbar[1S0(8)] g 418 | 0 | | q qbar -> ccbar[3PJ(8)] g 419 | 0 | | g g -> bbbar[3S1(1)] g 501 | 0 | | g g -> bbbar[3P0(1)] g 502 | 1 | | g g -> bbbar[3P1(1)] g 503 | 0 | | g g -> bbbar[3P2(1)] g 504 | 0 | | q g -> bbbar[3P0(1)] q 505 | 0 | | q g -> bbbar[3P1(1)] q 506 | 0 | | q g -> bbbar[3P2(1)] q 507 | 0 | | q qbar -> bbbar[3P0(1)] g 508 | 0 | | q qbar -> bbbar[3P1(1)] g 509 | 0 | | q qbar -> bbbar[3P2(1)] g 510 | 0 | | g g -> bbbar[3S1(8)] g 511 | 0 | | g g -> bbbar[1S0(8)] g 512 | 0 | | g g -> bbbar[3PJ(8)] g 513 | 0 | | q g -> bbbar[3S1(8)] q 514 | 0 | | q g -> bbbar[1S0(8)] q 515 | 0 | | q g -> bbbar[3PJ(8)] q 516 | 0 | | q qbar -> bbbar[3S1(8)] g 517 | 0 | | q qbar -> bbbar[1S0(8)] g 518 | 0 | | q qbar -> bbbar[3PJ(8)] g 519 | 0 | | | | sum | 7139 | | | | *------- End PYTHIA Multiparton Interactions Statistics -----* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Error in Pythia::next: hadronLevel failed; try again | | 1 Error in StringFragmentation::fragment: stuck in joining | | 1 Warning in Pythia::check: energy-momentum not quite conserved | | 6 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | 1 Warning in TimeShower::findMEcorr: ME weight above PS one | | 1 Warning in TimeShower::pTnext: negative dipole mass. | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:05 Higgs branching ratios by flavour 5.80*10^ 2 9 5.60*10^ 2 X 5.40*10^ 2 X 5.20*10^ 2 X 5.00*10^ 2 X 4.80*10^ 2 X 4.60*10^ 2 X 4.40*10^ 2 X 4.20*10^ 2 X 4.00*10^ 2 X 3.80*10^ 2 X 3.60*10^ 2 X 3.40*10^ 2 X 3.20*10^ 2 X 3.00*10^ 2 X 2.80*10^ 2 X 2.60*10^ 2 X 2.40*10^ 2 X 1 2.20*10^ 2 X X 2.00*10^ 2 X X 1.80*10^ 2 X X 1.60*10^ 2 X X 1.40*10^ 2 X X 1.20*10^ 2 X X 1.00*10^ 2 X 3 X 0.80*10^ 2 X 0 X X 0.60*10^ 2 X X X X 0.40*10^ 2 4X X X 1X 0.20*10^ 2 XX X X1XX 1 Contents *10^ 2 000005000000000000000000200000 *10^ 1 000027000000000600000802200000 *10^ 0 000087000000000100000711203000 *10^-1 000000000000000000000000000000 Low edge - *10^ 1 000000000001111111111222222222 *10^ 0 001234567890123456789012345678 *10^-1 555555555555555555555555555555 Entries = 1000 Mean = 1.1650e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+03 Rms = 8.5285e+00 Overflow = 0.0000e+00 High edge = 2.9500e+01 2013-09-20 16:05 Higgs rapidity 3.00*10^-1 5 2.90*10^-1 X 5 2.80*10^-1 X X 2.70*10^-1 X X5 5 2.60*10^-1 X XX X 2.50*10^-1 X XX XX 2.40*10^-1 X XX XX 2.30*10^-1 5X XXX5XX 2.20*10^-1 XX XXXXXXX 2.10*10^-1 XXX XXXXXXX5 5 2.00*10^-1 XXXXXXXXXXXX X 1.90*10^-1 XXXXXXXXXXXXX X 1.80*10^-1 XXXXXXXXXXXXX X 1.70*10^-1 XXXXXXXXXXXXX XX 1.60*10^-1 X XXXXXXXXXXXXX5XX 1.50*10^-1 X XXXXXXXXXXXXXXXX 1.40*10^-1 X 5XXXXXXXXXXXXXXXXX 1.30*10^-1 X XXXXXXXXXXXXXXXXXX 1.20*10^-1 X XXXXXXXXXXXXXXXXXX 1.10*10^-1 5 XXXXXXXXXXXXXXXXXXXXX5 1.00*10^-1 X XXXXXXXXXXXXXXXXXXXXXX 0.90*10^-1 X XXXXXXXXXXXXXXXXXXXXXX5 0.80*10^-1 X XXXXXXXXXXXXXXXXXXXXXXX 5 0.70*10^-1 X XXXXXXXXXXXXXXXXXXXXXXXXX 0.60*10^-1 X XXXXXXXXXXXXXXXXXXXXXXXXX 0.50*10^-1 5XXXXXXXXXXXXXXXXXXXXXXXXXXX X 0.40*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX5X5 0.30*10^-1 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.20*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.10*10^-1 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 Contents *10^-1 0000000000000000000000000000000000000101111122222222222212111000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000112224056134912903862562050710877353000000000000000000000000000000000 *10^-3 0000000000000000000000000000500000505500050005500555050555005505505500000000000000000000000000000000 *10^-4 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 1000 Mean = 3.1000e-02 Underflow = 0.0000e+00 Low edge = -1.0000e+01 All chan = 5.0000e+00 Rms = 1.4403e+00 Overflow = 0.0000e+00 High edge = 1.0000e+01 2013-09-20 16:05 charged pseudorapidity 2.50*10^ 1 2 72 2.40*10^ 1 197966XXXX57 6 2.30*10^ 1 2XXXXXXXXXXXX8X442 2.20*10^ 1 8XXXXXXXXXXXXXXXXXXX63 2.10*10^ 1 26XXXXXXXXXXXXXXXXXXXXXXX1 2.00*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXX4 1.90*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.80*10^ 1 X9XXXXXXXXXXXXXXXXXXXXXXXXXXXXX95 1.70*10^ 1 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 1.60*10^ 1 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.50*10^ 1 23XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX97 1.40*10^ 1 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX62 1.30*10^ 1 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2 1.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 1.10*10^ 1 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2 1.00*10^ 1 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 0.90*10^ 1 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 0.80*10^ 1 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX71 0.70*10^ 1 28XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.60*10^ 1 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 0.50*10^ 1 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6 0.40*10^ 1 69XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX86 0.30*10^ 1 37XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX62 0.20*10^ 1 14398XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX99532 0.10*10^ 1 223568XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9964422 Contents *10^ 1 0000000000000000000000001111111111111222222222222222222222222221111111111111000000000000000000000000 *10^ 0 0000000111112223345667890122344566878000123333334344332322211109877644332100987765433222111110000000 *10^-1 1234589143873696973288727007523059099269720879652961468533296213095396612791246143576951894219964321 *10^-2 6117928234760865599322334214351927036237619900292678893879055916042329254275898330993988718783333847 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 224884 Mean = -8.2795e-03 Underflow = 4.1500e-01 Low edge = -1.0000e+01 All chan = 1.1237e+03 Rms = 3.4416e+00 Overflow = 3.3000e-01 High edge = 1.0000e+01 2013-09-20 16:05 charged multiplicity 4.50*10^ 1 3 4.35*10^ 1 X 4.20*10^ 1 X 4.05*10^ 1 X 3.90*10^ 1 X 3.75*10^ 1 X 3.60*10^ 1 X X X 3.45*10^ 1 X X X 3.30*10^ 1 X X 3 XX 3XX 33 X 3 3.15*10^ 1 X X X XX XXX XX7X X 3.00*10^ 1 X X X XXXXXX3X3XXXX X 3 2.85*10^ 1 X7 7X X XXXXXXXXXXXXX X X 2.70*10^ 1 XX3XX X XXXXXXXXXXXXXX X X 2.55*10^ 1 XXXXX X XXXXXXXXXXXXXX X X 2.40*10^ 1 XXXXX X XXXXXXXXXXXXXX X X 2.25*10^ 1 XXXXX7X7XXXXXXXXXXXXXX X X 2.10*10^ 1 3 X 3XXXXXXXXXXXXXXXXXXXXXXXX X 1.95*10^ 1 X X XXXXXXXXXXXXXXXXXXXXXXXXX7X7 1.80*10^ 1 X3X3XXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.65*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 3 1.35*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 7 1.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X 1.05*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X 0.90*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 0.75*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7X 0.60*10^ 1 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X3 0.45*10^ 1 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX77XX 7 0.30*10^ 1 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 3 0.15*10^ 1 X7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 7X 7 Contents *10^ 1 0000000000212123222323233334323233332231211010100000000000000000000000000000000000000000000000000000 *10^ 0 0000002163071703868622236024390922137129995947344653334101201000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 1000 Mean = 2.2539e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+03 Rms = 8.3664e+01 Overflow = 0.0000e+00 High edge = 7.9950e+02 pythia8-8.1.80.orig/examples/outref/out170000644000175000017500000023765712217346173016407 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:05:29 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* PYTHIA Warning in PhaseSpace2to2tauyz::trialKin: maximum for cross section violated *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 7.000e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> ccbar[3S1(1)] g 401 | 8.792e-03 | | g g -> ccbar[3P0(1)] g 402 | 9.242e-01 | | g g -> ccbar[3P1(1)] g 403 | 1.136e+00 | | g g -> ccbar[3P2(1)] g 404 | 1.649e+00 | | q g -> ccbar[3P0(1)] q 405 | 5.302e-01 | | q g -> ccbar[3P1(1)] q 406 | 2.373e-01 | | q g -> ccbar[3P2(1)] q 407 | 4.568e-01 | | q qbar -> ccbar[3P0(1)] g 408 | 1.976e-06 | | q qbar -> ccbar[3P1(1)] g 409 | 6.824e-05 | | q qbar -> ccbar[3P2(1)] g 410 | 4.379e-05 | | g g -> ccbar[3S1(8)] g 411 | 1.871e-01 | | g g -> ccbar[1S0(8)] g 412 | 1.002e-01 | | g g -> ccbar[3PJ(8)] g 413 | 1.323e-01 | | q g -> ccbar[3S1(8)] q 414 | 3.935e-02 | | q g -> ccbar[1S0(8)] q 415 | 2.947e-02 | | q g -> ccbar[3PJ(8)] q 416 | 6.154e-02 | | q qbar -> ccbar[3S1(8)] g 417 | 1.198e-04 | | q qbar -> ccbar[1S0(8)] g 418 | 1.980e-06 | | q qbar -> ccbar[3PJ(8)] g 419 | 5.259e-06 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 50.91 mb | | | | pT0 = 2.70 gives sigmaInteraction = 207.48 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eCM | 7000.000 | 14000.000 10.00000 | | Charmonium:all | on | off | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberShowEvent | 0 | 1 0 | | Next:numberShowInfo | 0 | 1 0 | | Next:numberShowProcess | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:pTHatMin | 0.50000 | 0.0 0.0 | | PhaseSpace:pTHatMinDiverge | 0.50000 | 1.00000 0.50000 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products 443 J/psi 3 0 0 3.09692 0.00009 3.09602 3.09782 0.00000e+00 0 1 1 1 0 0 1 0.8023950 43 83 -83 1 1 0.0594000 0 11 -11 2 1 0.0593000 0 13 -13 3 1 0.0130000 0 441 22 4 1 0.0056000 0 113 111 5 1 0.0056500 0 213 -211 6 1 0.0056500 0 -213 211 7 1 0.0036000 0 115 113 8 1 0.0036000 0 -215 213 9 1 0.0036000 0 215 -213 10 1 0.0043000 0 225 223 11 1 0.0022000 0 313 -315 12 1 0.0022000 0 323 -325 13 1 0.0022000 0 -323 325 14 1 0.0025000 0 321 -323 15 1 0.0025000 0 -321 323 16 1 0.0021000 0 311 -313 17 1 0.0021000 0 -311 313 18 1 0.0019000 0 20323 -321 19 1 0.0019000 0 -20323 321 20 1 0.0015000 0 10213 -211 21 1 0.0015000 0 -10213 211 22 1 0.0023000 0 10113 111 23 1 0.0004800 0 10331 223 24 1 0.0007400 0 223 221 25 1 0.0003600 0 10331 333 26 1 0.0008000 0 333 335 27 1 0.0006800 0 20333 223 28 1 0.0007400 0 333 221 29 1 0.0004500 0 223 111 30 1 0.0004000 0 333 331 31 1 0.0003200 0 333 9010221 32 1 0.0002600 0 333 20223 33 1 0.0001930 0 113 221 34 1 0.0001820 0 223 331 35 1 0.0001400 0 223 9010221 36 1 0.0001050 0 113 331 37 1 0.0011000 0 2224 -2224 38 1 0.0005150 0 3112 -3112 39 1 0.0005900 0 3314 -3314 40 1 0.0003200 0 3324 -3324 41 1 0.0003200 0 3324 -3324 42 1 0.0001550 0 3114 -3114 43 1 0.0001550 0 3224 -3224 -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- J/psi decay performed, J/psi in line 125, mother id = 20443 -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 7000.000 7000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 3500.000 3500.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -3500.000 3500.000 0.938 3 21 (g) -21 1 0 5 6 102 101 0.000 0.000 1159.576 1159.576 0.000 4 21 (g) -21 2 0 5 6 103 102 0.000 0.000 -2.633 2.633 0.000 5 20443 chi_1c 23 3 4 0 0 0 0 1.842 -0.440 -1.121 4.144 3.511 6 21 g 23 3 4 0 0 103 101 -1.842 0.440 1158.064 1158.065 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 1156.943 1162.209 110.510 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 7000.000 7000.000 1 2212 (p+) -12 0 0 30 0 0 0 0.000 0.000 3500.000 3500.000 0.938 2 2212 (p+) -12 0 0 31 0 0 0 0.000 0.000 -3500.000 3500.000 0.938 3 21 (g) -21 7 0 5 6 102 101 0.000 0.000 1159.576 1159.576 0.000 4 21 (g) -21 8 8 5 6 103 102 0.000 0.000 -2.633 2.633 0.000 5 20443 (chi_1c) -23 3 4 9 9 0 0 1.842 -0.440 -1.121 4.144 3.511 6 21 (g) -23 3 4 10 10 103 101 -1.842 0.440 1158.064 1158.065 0.000 7 21 (g) -41 21 21 11 3 104 101 0.000 0.000 1184.592 1184.592 0.000 8 21 (g) -42 14 14 4 4 103 102 -0.000 0.000 -2.633 2.633 0.000 9 20443 (chi_1c) -44 5 5 23 23 0 0 1.841 -0.439 -1.090 4.135 3.511 10 21 (g) -44 6 6 12 13 103 101 -2.689 1.160 1166.418 1166.422 0.000 11 21 (g) -43 7 0 15 16 104 102 0.847 -0.722 16.631 16.668 0.000 12 21 (g) -51 10 0 18 19 105 101 -0.941 1.020 610.152 610.154 0.000 13 21 (g) -51 10 0 20 20 103 105 -1.748 0.140 556.266 556.268 0.000 14 21 (g) -53 17 17 8 8 103 102 0.000 0.000 -2.633 2.633 0.000 15 21 (g) -51 11 0 25 25 104 106 -0.023 -0.364 9.736 9.743 0.000 16 21 (g) -51 11 0 27 27 106 102 0.870 -0.358 6.878 6.942 0.000 17 21 (g) -53 22 0 14 14 103 102 -0.000 0.000 -2.650 2.650 0.000 18 21 (g) -51 12 0 24 24 107 101 -0.171 0.437 120.877 120.878 0.000 19 21 (g) -51 12 0 28 28 105 107 -1.588 0.649 749.942 749.944 0.000 20 21 (g) -52 13 13 26 26 103 105 -0.929 0.074 295.599 295.600 0.000 21 21 (g) -42 30 30 7 7 104 101 -0.000 0.000 1184.592 1184.592 0.000 22 21 (g) -41 31 31 29 17 103 108 0.000 -0.000 -54.517 54.517 0.000 23 20443 (chi_1c) -44 9 9 32 32 0 0 1.931 -0.810 -1.014 4.211 3.511 24 21 (g) -44 18 18 33 33 107 101 -0.171 0.437 120.842 120.843 0.000 25 21 (g) -44 15 15 34 34 104 106 -0.023 -0.364 9.762 9.768 0.000 26 21 (g) -44 20 20 35 35 103 105 -0.929 0.074 295.574 295.575 0.000 27 21 (g) -44 16 16 36 36 106 102 0.871 -0.363 6.919 6.983 0.000 28 21 (g) -44 19 19 37 37 105 107 -1.588 0.649 749.859 749.861 0.000 29 21 (g) -43 22 0 38 38 102 108 -0.091 0.376 -51.866 51.868 0.000 30 21 (g) -61 1 0 21 21 104 101 0.544 -2.769 1184.599 1184.602 0.000 31 21 (g) -61 2 0 22 22 103 108 0.268 0.721 -54.513 54.519 0.000 32 20443 (chi_1c) -62 23 23 125 126 0 0 1.944 -0.779 -1.016 4.212 3.511 33 21 (g) -62 24 24 66 66 107 101 -0.116 0.154 120.846 120.846 0.000 34 21 (g) -62 25 25 47 47 104 106 -0.018 -0.387 9.759 9.766 0.000 35 21 (g) -62 26 26 43 0 103 105 -0.793 -0.617 295.574 295.576 0.000 36 21 (g) -62 27 27 46 46 106 102 0.875 -0.378 6.918 6.983 0.000 37 21 (g) -62 28 28 43 0 105 107 -1.244 -1.104 749.865 749.867 0.000 38 21 (g) -62 29 29 45 45 102 108 0.164 1.062 -51.860 51.871 0.000 39 2203 (uu_1) -63 1 0 48 48 0 104 0.166 1.537 2288.275 2288.276 0.771 40 1 (d) -63 1 0 65 65 101 0 -0.711 1.232 27.098 27.137 0.330 41 2101 (ud_0) -63 2 0 68 68 0 103 -0.416 -0.337 -3424.924 3424.924 0.579 42 2 (u) -63 2 0 44 44 108 0 0.148 -0.384 -20.535 20.542 0.330 43 21 (g) -73 35 37 67 67 103 107 -2.037 -1.720 1045.439 1045.442 0.562 44 2 (u) -71 42 42 49 64 108 0 0.148 -0.384 -20.535 20.542 0.330 45 21 (g) -71 38 38 49 64 102 108 0.164 1.062 -51.860 51.871 0.000 46 21 (g) -71 36 36 49 64 106 102 0.875 -0.378 6.918 6.983 0.000 47 21 (g) -71 34 34 49 64 104 106 -0.018 -0.387 9.759 9.766 0.000 48 2203 (uu_1) -71 39 39 49 64 0 104 0.166 1.537 2288.275 2288.276 0.771 49 211 pi+ 83 44 48 0 0 0 0 0.496 0.477 -26.274 26.283 0.140 50 -213 (rho-) -83 44 48 95 96 0 0 -0.197 -0.236 -25.055 25.066 0.690 51 321 K+ 83 44 48 0 0 0 0 0.112 -0.323 -19.485 19.495 0.494 52 -321 K- 83 44 48 0 0 0 0 0.085 0.554 -0.465 0.880 0.494 53 213 (rho+) -83 44 48 97 98 0 0 -0.056 0.685 -0.435 1.125 0.778 54 2112 n0 83 44 48 0 0 0 0 -0.366 -1.017 4.781 4.991 0.940 55 111 (pi0) -83 44 48 127 128 0 0 0.631 0.220 3.943 4.002 0.135 56 -2212 pbar- 83 44 48 0 0 0 0 0.392 -0.322 15.537 15.574 0.938 57 211 pi+ 84 44 48 0 0 0 0 0.128 0.340 53.886 53.888 0.140 58 111 (pi0) -84 44 48 129 130 0 0 -0.085 -0.162 11.569 11.572 0.135 59 -211 pi- 84 44 48 0 0 0 0 0.280 -0.139 87.467 87.468 0.140 60 111 (pi0) -84 44 48 131 132 0 0 -0.258 0.202 161.901 161.902 0.135 61 211 pi+ 84 44 48 0 0 0 0 -0.334 0.392 112.295 112.296 0.140 62 113 (rho0) -84 44 48 99 100 0 0 0.378 -0.059 177.745 177.749 1.079 63 -211 pi- 84 44 48 0 0 0 0 0.282 0.028 25.624 25.626 0.140 64 2224 (Delta++) -84 44 48 101 102 0 0 -0.153 0.811 1649.522 1649.522 1.372 65 1 (d) -71 40 40 69 94 101 0 -0.711 1.232 27.098 27.137 0.330 66 21 (g) -71 33 33 69 94 107 101 -0.116 0.154 120.846 120.846 0.000 67 21 (g) -71 43 43 69 94 103 107 -2.037 -1.720 1045.439 1045.442 0.562 68 2101 (ud_0) -71 41 41 69 94 0 103 -0.416 -0.337 -3424.924 3424.924 0.579 69 -211 pi- 83 65 68 0 0 0 0 -0.154 0.175 18.020 18.022 0.140 70 2224 (Delta++) -83 65 68 103 104 0 0 -0.415 0.499 41.297 41.323 1.324 71 -213 (rho-) -83 65 68 105 106 0 0 -0.079 0.750 62.618 62.627 0.764 72 -2214 (Deltabar-) -83 65 68 107 108 0 0 -1.136 -1.025 470.881 470.885 1.200 73 331 (eta') -83 65 68 133 134 0 0 -0.210 -0.069 99.026 99.031 0.958 74 221 (eta) -83 65 68 135 136 0 0 -0.259 -0.226 183.151 183.152 0.548 75 321 K+ 83 65 68 0 0 0 0 -0.285 0.118 66.597 66.600 0.494 76 -323 (K*-) -83 65 68 109 110 0 0 -0.271 -0.456 196.872 196.875 0.894 77 323 (K*+) -83 65 68 111 112 0 0 -0.185 0.229 33.304 33.317 0.869 78 -321 K- 83 65 68 0 0 0 0 -0.158 0.112 11.983 11.995 0.494 79 321 K+ 83 65 68 0 0 0 0 0.109 -0.471 5.196 5.241 0.494 80 -323 (K*-) -84 65 68 113 114 0 0 0.208 0.181 0.855 1.267 0.893 81 213 (rho+) -84 65 68 115 116 0 0 0.074 -0.583 1.740 1.909 0.520 82 313 (K*0) -84 65 68 117 118 0 0 0.070 0.707 1.113 1.623 0.943 83 -321 K- 84 65 68 0 0 0 0 -0.218 -0.295 -1.930 2.026 0.494 84 211 pi+ 84 65 68 0 0 0 0 0.190 -0.194 -2.094 2.116 0.140 85 111 (pi0) -84 65 68 137 138 0 0 -0.205 0.306 -1.520 1.570 0.135 86 223 (omega) -84 65 68 139 141 0 0 0.112 0.379 -3.605 3.709 0.779 87 -211 pi- 84 65 68 0 0 0 0 -0.377 -0.674 -71.076 71.080 0.140 88 211 pi+ 84 65 68 0 0 0 0 0.393 -0.024 -44.260 44.262 0.140 89 221 (eta) -84 65 68 142 143 0 0 0.001 0.736 -61.861 61.868 0.548 90 311 (K0) -84 65 68 119 119 0 0 -0.370 -0.463 -101.356 101.359 0.498 91 -321 K- 84 65 68 0 0 0 0 0.078 -0.114 -487.830 487.831 0.494 92 211 pi+ 84 65 68 0 0 0 0 0.155 0.094 -156.898 156.898 0.140 93 -213 (rho-) -84 65 68 120 121 0 0 -0.082 -0.027 -1095.477 1095.477 0.759 94 2212 p+ 84 65 68 0 0 0 0 -0.267 -0.337 -1396.287 1396.287 0.938 95 -211 pi- 91 50 0 0 0 0 0 0.197 -0.199 -14.032 14.035 0.140 96 111 (pi0) -91 50 0 144 145 0 0 -0.394 -0.037 -11.023 11.031 0.135 97 211 pi+ 91 53 0 0 0 0 0 0.197 0.241 0.117 0.361 0.140 98 111 (pi0) -91 53 0 146 147 0 0 -0.254 0.443 -0.552 0.764 0.135 99 211 pi+ 91 62 0 0 0 0 0 0.069 0.386 33.213 33.216 0.140 100 -211 pi- 91 62 0 0 0 0 0 0.309 -0.445 144.532 144.533 0.140 101 2212 p+ 91 64 0 0 0 0 0 0.143 0.323 944.004 944.004 0.938 102 211 pi+ 91 64 0 0 0 0 0 -0.296 0.489 705.518 705.518 0.140 103 2212 p+ 91 70 0 0 0 0 0 -0.482 0.622 30.624 30.649 0.938 104 211 pi+ 91 70 0 0 0 0 0 0.067 -0.123 10.673 10.675 0.140 105 -211 pi- 91 71 0 0 0 0 0 -0.375 0.272 24.137 24.142 0.140 106 111 (pi0) -91 71 0 148 149 0 0 0.296 0.478 38.480 38.485 0.135 107 -2212 pbar- 91 72 0 0 0 0 0 -0.664 -0.774 317.780 317.783 0.938 108 111 (pi0) -91 72 0 150 151 0 0 -0.472 -0.252 153.101 153.102 0.135 109 -321 K- 91 76 0 0 0 0 0 0.005 -0.470 160.400 160.402 0.494 110 111 (pi0) -91 76 0 152 153 0 0 -0.276 0.014 36.472 36.473 0.135 111 311 (K0) -91 77 0 122 122 0 0 -0.304 0.172 15.965 15.976 0.498 112 211 pi+ 91 77 0 0 0 0 0 0.119 0.057 17.340 17.341 0.140 113 -311 (Kbar0) -91 80 0 123 123 0 0 0.146 0.268 0.247 0.634 0.498 114 -211 pi- 91 80 0 0 0 0 0 0.063 -0.087 0.608 0.633 0.140 115 211 pi+ 91 81 0 0 0 0 0 0.182 -0.441 1.502 1.582 0.140 116 111 (pi0) -91 81 0 154 155 0 0 -0.108 -0.142 0.238 0.326 0.135 117 311 (K0) -91 82 0 124 124 0 0 0.067 0.279 0.206 0.610 0.498 118 111 (pi0) -91 82 0 156 157 0 0 0.003 0.429 0.908 1.013 0.135 119 130 K_L0 91 90 90 0 0 0 0 -0.370 -0.463 -101.356 101.359 0.498 120 -211 pi- 91 93 0 0 0 0 0 0.084 0.007 -54.312 54.312 0.140 121 111 (pi0) -91 93 0 158 159 0 0 -0.165 -0.034 -1041.165 1041.165 0.135 122 310 (K_S0) -91 111 111 160 161 0 0 -0.304 0.172 15.965 15.976 0.498 123 130 K_L0 91 113 113 0 0 0 0 0.146 0.268 0.247 0.634 0.498 124 310 (K_S0) -91 117 117 162 163 0 0 0.067 0.279 0.206 0.610 0.498 125 443 (J/psi) -91 32 0 164 165 0 0 1.695 -0.657 -1.296 3.818 3.097 126 22 gamma 91 32 0 0 0 0 0 0.250 -0.122 0.280 0.395 0.000 127 22 gamma 91 55 0 0 0 0 0 0.290 0.040 1.508 1.536 0.000 128 22 gamma 91 55 0 0 0 0 0 0.341 0.180 2.436 2.466 0.000 129 22 gamma 91 58 0 0 0 0 0 -0.085 -0.136 5.914 5.917 0.000 130 22 gamma 91 58 0 0 0 0 0 -0.000 -0.026 5.655 5.655 0.000 131 22 gamma 91 60 0 0 0 0 0 -0.115 0.174 92.277 92.277 0.000 132 22 gamma 91 60 0 0 0 0 0 -0.143 0.028 69.624 69.625 0.000 133 113 (rho0) -91 73 0 166 167 0 0 -0.283 -0.071 94.584 94.588 0.851 134 22 gamma 91 73 0 0 0 0 0 0.073 0.002 4.442 4.443 0.000 135 22 gamma 91 74 0 0 0 0 0 -0.014 -0.349 125.627 125.628 0.000 136 22 gamma 91 74 0 0 0 0 0 -0.245 0.123 57.524 57.525 0.000 137 22 gamma 91 85 0 0 0 0 0 -0.127 0.132 -0.507 0.540 0.000 138 22 gamma 91 85 0 0 0 0 0 -0.079 0.174 -1.013 1.030 0.000 139 211 pi+ 91 86 0 0 0 0 0 0.213 0.161 -1.579 1.608 0.140 140 -211 pi- 91 86 0 0 0 0 0 -0.158 0.100 -1.762 1.778 0.140 141 111 (pi0) -91 86 0 168 169 0 0 0.057 0.118 -0.263 0.324 0.135 142 22 gamma 91 89 0 0 0 0 0 -0.027 -0.018 -19.895 19.895 0.000 143 22 gamma 91 89 0 0 0 0 0 0.028 0.754 -41.966 41.973 0.000 144 22 gamma 91 96 0 0 0 0 0 -0.083 0.006 -4.054 4.055 0.000 145 22 gamma 91 96 0 0 0 0 0 -0.311 -0.043 -6.969 6.976 0.000 146 22 gamma 91 98 0 0 0 0 0 -0.106 0.075 -0.114 0.173 0.000 147 22 gamma 91 98 0 0 0 0 0 -0.147 0.369 -0.438 0.592 0.000 148 22 gamma 91 106 0 0 0 0 0 0.298 0.486 37.659 37.663 0.000 149 22 gamma 91 106 0 0 0 0 0 -0.001 -0.008 0.821 0.821 0.000 150 22 gamma 91 108 0 0 0 0 0 -0.387 -0.141 115.893 115.894 0.000 151 22 gamma 91 108 0 0 0 0 0 -0.085 -0.111 37.207 37.208 0.000 152 22 gamma 91 110 0 0 0 0 0 -0.051 -0.008 2.435 2.436 0.000 153 22 gamma 91 110 0 0 0 0 0 -0.225 0.022 34.037 34.037 0.000 154 22 gamma 91 116 0 0 0 0 0 -0.087 -0.044 0.194 0.217 0.000 155 22 gamma 91 116 0 0 0 0 0 -0.020 -0.098 0.044 0.110 0.000 156 22 gamma 91 118 0 0 0 0 0 -0.028 0.301 0.743 0.802 0.000 157 22 gamma 91 118 0 0 0 0 0 0.031 0.128 0.164 0.210 0.000 158 22 gamma 91 121 0 0 0 0 0 -0.013 0.036 -100.001 100.001 0.000 159 22 gamma 91 121 0 0 0 0 0 -0.152 -0.070 -941.164 941.164 0.000 160 211 pi+ 91 122 0 0 0 0 0 -0.083 0.277 9.567 9.573 0.140 161 -211 pi- 91 122 0 0 0 0 0 -0.221 -0.104 6.397 6.404 0.140 162 211 pi+ 91 124 0 0 0 0 0 0.224 0.205 0.048 0.337 0.140 163 -211 pi- 91 124 0 0 0 0 0 -0.157 0.074 0.158 0.273 0.140 164 -13 mu+ 93 125 0 0 0 0 0 0.672 -1.594 -1.638 2.385 0.106 165 13 mu- 93 125 0 0 0 0 0 1.022 0.937 0.343 1.432 0.106 166 211 pi+ 91 133 0 0 0 0 0 -0.500 0.155 65.690 65.692 0.140 167 -211 pi- 91 133 0 0 0 0 0 0.217 -0.226 28.894 28.896 0.140 168 22 gamma 91 141 0 0 0 0 0 0.101 0.072 -0.184 0.222 0.000 169 22 gamma 91 141 0 0 0 0 0 -0.044 0.046 -0.079 0.102 0.000 Charge sum: 2.000 Momentum sum: 0.000 0.000 -0.000 7000.000 7000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- J/psi decay performed, J/psi in line 38, mother id = 9910441 -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 7000.000 7000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 3500.000 3500.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -3500.000 3500.000 0.938 3 21 (g) -21 1 0 5 6 101 102 0.000 0.000 5.996 5.996 0.000 4 21 (g) -21 2 0 5 6 103 104 0.000 0.000 -33.036 33.036 0.000 5 9910441 ccbar[3P0(8)] 23 3 4 0 0 101 104 -3.166 -2.365 -32.168 32.558 3.100 6 21 g 23 3 4 0 0 103 102 3.166 2.365 5.128 6.474 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 -27.040 39.032 28.148 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 7000.000 7000.000 1 2212 (p+) -12 0 0 26 0 0 0 0.000 0.000 3500.000 3500.000 0.938 2 2212 (p+) -12 0 0 27 0 0 0 0.000 0.000 -3500.000 3500.000 0.938 3 21 (g) -21 7 0 5 6 101 102 0.000 0.000 5.996 5.996 0.000 4 21 (g) -21 8 8 5 6 103 104 0.000 0.000 -33.036 33.036 0.000 5 9910441 (ccbar[3P0(8)]) -23 3 4 9 9 101 104 -3.166 -2.365 -32.168 32.558 3.100 6 21 (g) -23 3 4 10 10 103 102 3.166 2.365 5.128 6.474 0.000 7 21 (g) -41 18 18 11 3 101 105 0.000 0.000 17.043 17.043 0.000 8 21 (g) -42 14 14 4 4 103 104 0.000 -0.000 -33.036 33.036 0.000 9 9910441 (ccbar[3P0(8)]) -44 5 5 20 20 101 104 -3.149 -2.395 -32.146 32.536 3.100 10 21 (g) -44 6 6 12 13 103 102 3.659 1.480 5.143 6.484 0.000 11 21 (g) -43 7 0 17 17 102 105 -0.510 0.915 11.009 11.059 0.000 12 21 (g) -51 10 0 15 16 106 102 3.344 0.744 5.123 6.163 0.000 13 21 (g) -51 10 0 23 23 103 106 0.315 0.736 -0.769 1.110 0.000 14 21 (g) -53 19 0 8 8 103 104 0.000 -0.000 -33.826 33.826 0.000 15 21 (g) -51 12 0 21 21 106 107 1.490 -0.188 1.452 2.089 0.000 16 21 (g) -51 12 0 24 24 107 102 1.790 1.046 5.050 5.460 0.000 17 21 (g) -52 11 11 22 22 102 105 -0.446 0.800 9.630 9.674 0.000 18 21 (g) -42 26 26 7 7 101 105 -0.000 -0.000 17.043 17.043 0.000 19 21 (g) -41 27 27 25 14 103 108 0.000 0.000 -63.624 63.624 0.000 20 9910441 (ccbar[3P0(8)]) -44 9 9 28 28 101 104 -3.360 -2.787 -32.126 32.569 3.100 21 21 (g) -44 15 15 29 29 106 107 1.488 -0.192 1.448 2.085 0.000 22 21 (g) -44 17 17 30 30 102 105 -0.446 0.800 9.625 9.668 0.000 23 21 (g) -44 13 13 31 31 103 106 0.309 0.725 -0.775 1.105 0.000 24 21 (g) -44 16 16 32 32 107 102 1.789 1.044 5.037 5.446 0.000 25 21 (g) -43 19 0 33 33 104 108 0.221 0.410 -29.790 29.794 0.000 26 21 (g) -61 1 0 18 18 101 105 -1.705 1.964 16.946 17.144 0.000 27 21 (g) -61 2 0 19 19 103 108 0.534 -0.810 -63.541 63.549 0.000 28 9910441 (ccbar[3P0(8)]) -62 20 20 38 39 101 104 -3.111 -3.173 -32.089 32.543 3.100 29 21 (g) -62 21 21 63 63 106 107 1.313 0.009 1.531 2.017 0.000 30 21 (g) -62 22 22 61 61 102 105 -1.410 1.910 9.494 9.787 0.000 31 21 (g) -62 23 23 64 64 103 106 0.300 0.732 -0.804 1.128 0.000 32 21 (g) -62 24 24 62 62 107 102 1.266 1.645 5.038 5.449 0.000 33 21 (g) -62 25 25 40 0 104 108 0.471 0.031 -29.765 29.769 0.000 34 2101 (ud_0) -63 1 0 43 43 0 101 1.095 -0.265 3208.263 3208.263 0.579 35 2 (u) -63 1 0 60 60 105 0 0.609 -1.699 274.677 274.683 0.330 36 2 (u) -63 2 0 41 41 108 0 -0.279 0.715 -21.898 21.914 0.330 37 2101 (ud_0) -63 2 0 65 65 0 103 -0.256 0.095 -3414.447 3414.447 0.579 38 443 (J/psi) -91 28 0 118 119 0 0 -3.104 -3.168 -32.028 32.482 3.097 39 21 (g) -91 28 0 40 0 101 104 -0.007 -0.005 -0.060 0.061 0.000 40 21 (g) -73 33 39 42 42 101 108 0.464 0.026 -29.826 29.830 0.205 41 2 (u) -71 36 36 44 59 108 0 -0.279 0.715 -21.898 21.914 0.330 42 21 (g) -71 40 40 44 59 101 108 0.464 0.026 -29.826 29.830 0.205 43 2101 (ud_0) -71 34 34 44 59 0 101 1.095 -0.265 3208.263 3208.263 0.579 44 111 (pi0) -83 41 43 120 121 0 0 0.166 0.084 -3.415 3.423 0.135 45 211 pi+ 83 41 43 0 0 0 0 -0.232 0.064 -19.119 19.121 0.140 46 313 (K*0) -83 41 43 91 92 0 0 0.570 0.972 -28.560 28.598 0.960 47 -313 (K*bar0) -83 41 43 93 94 0 0 -0.051 -0.133 1.451 1.872 1.173 48 -213 (rho-) -83 41 43 95 96 0 0 -0.307 -0.009 2.115 2.255 0.720 49 211 pi+ 83 41 43 0 0 0 0 -0.098 -0.329 0.130 0.393 0.140 50 111 (pi0) -83 41 43 122 123 0 0 -0.006 0.212 0.095 0.269 0.135 51 -211 pi- 83 41 43 0 0 0 0 -0.378 0.263 0.835 0.964 0.140 52 211 pi+ 83 41 43 0 0 0 0 0.384 -0.509 2.513 2.596 0.140 53 221 (eta) -84 41 43 124 126 0 0 0.367 -0.155 16.306 16.320 0.548 54 -213 (rho-) -84 41 43 97 98 0 0 -0.146 0.069 87.540 87.544 0.793 55 111 (pi0) -84 41 43 127 128 0 0 0.339 -0.098 105.990 105.991 0.135 56 213 (rho+) -84 41 43 99 100 0 0 -0.546 0.442 198.655 198.658 0.850 57 111 (pi0) -84 41 43 129 130 0 0 0.713 -0.036 557.157 557.157 0.135 58 221 (eta) -84 41 43 131 132 0 0 0.138 -0.224 701.749 701.750 0.548 59 2112 n0 84 41 43 0 0 0 0 0.367 -0.137 1533.097 1533.097 0.940 60 2 (u) -71 35 35 66 90 105 0 0.609 -1.699 274.677 274.683 0.330 61 21 (g) -71 30 30 66 90 102 105 -1.410 1.910 9.494 9.787 0.000 62 21 (g) -71 32 32 66 90 107 102 1.266 1.645 5.038 5.449 0.000 63 21 (g) -71 29 29 66 90 106 107 1.313 0.009 1.531 2.017 0.000 64 21 (g) -71 31 31 66 90 103 106 0.300 0.732 -0.804 1.128 0.000 65 2101 (ud_0) -71 37 37 66 90 0 103 -0.256 0.095 -3414.447 3414.447 0.579 66 211 pi+ 83 60 65 0 0 0 0 0.326 -0.586 44.279 44.285 0.140 67 111 (pi0) -83 60 65 133 134 0 0 -0.155 0.332 13.049 13.055 0.135 68 -211 pi- 83 60 65 0 0 0 0 0.004 -1.336 145.955 145.961 0.140 69 113 (rho0) -83 60 65 101 102 0 0 0.135 -0.085 33.496 33.505 0.733 70 211 pi+ 83 60 65 0 0 0 0 -0.068 0.098 14.080 14.082 0.140 71 2112 n0 83 60 65 0 0 0 0 -0.250 0.763 11.307 11.374 0.940 72 211 pi+ 83 60 65 0 0 0 0 -0.004 -0.441 4.415 4.439 0.140 73 -2212 pbar- 83 60 65 0 0 0 0 0.205 0.371 12.014 12.058 0.938 74 -213 (rho-) -83 60 65 103 104 0 0 -0.003 1.236 4.653 4.898 0.904 75 113 (rho0) -83 60 65 105 106 0 0 -0.050 0.576 2.352 2.501 0.624 76 111 (pi0) -83 60 65 135 136 0 0 0.277 0.267 0.859 0.951 0.135 77 111 (pi0) -83 60 65 137 138 0 0 0.447 -0.276 2.034 2.105 0.135 78 221 (eta) -83 60 65 139 141 0 0 0.462 0.846 0.680 1.301 0.548 79 213 (rho+) -83 60 65 107 108 0 0 0.544 0.135 0.615 1.321 1.026 80 313 (K*0) -83 60 65 109 110 0 0 0.301 0.668 -0.151 1.227 0.972 81 -311 (Kbar0) -83 60 65 111 111 0 0 -0.129 -0.061 -0.487 0.711 0.498 82 311 (K0) -84 60 65 112 112 0 0 0.505 0.243 -12.024 12.047 0.498 83 221 (eta) -84 60 65 142 144 0 0 -0.767 -0.084 -12.255 12.292 0.548 84 -321 K- 84 60 65 0 0 0 0 0.380 0.018 -24.437 24.445 0.494 85 213 (rho+) -84 60 65 113 114 0 0 -0.106 -0.071 -57.711 57.719 0.934 86 111 (pi0) -84 60 65 145 146 0 0 0.251 0.068 -74.575 74.576 0.135 87 -211 pi- 84 60 65 0 0 0 0 -0.079 -0.184 -87.822 87.823 0.140 88 223 (omega) -84 60 65 147 149 0 0 0.083 -0.203 -623.354 623.355 0.782 89 2214 (Delta+) -84 60 65 115 116 0 0 -0.403 0.152 -900.021 900.023 1.345 90 223 (omega) -84 60 65 150 152 0 0 -0.083 0.247 -1621.460 1621.461 0.782 91 311 (K0) -91 46 0 117 117 0 0 0.376 0.917 -17.197 17.233 0.498 92 111 (pi0) -91 46 0 153 154 0 0 0.194 0.054 -11.363 11.366 0.135 93 -321 K- 91 47 0 0 0 0 0 -0.449 -0.284 1.008 1.242 0.494 94 211 pi+ 91 47 0 0 0 0 0 0.397 0.151 0.443 0.630 0.140 95 -211 pi- 91 48 0 0 0 0 0 -0.327 0.197 0.629 0.749 0.140 96 111 (pi0) -91 48 0 155 156 0 0 0.020 -0.206 1.485 1.506 0.135 97 -211 pi- 91 54 0 0 0 0 0 -0.226 0.371 57.412 57.414 0.140 98 111 (pi0) -91 54 0 157 158 0 0 0.081 -0.302 30.128 30.130 0.135 99 211 pi+ 91 56 0 0 0 0 0 -0.478 0.366 191.729 191.730 0.140 100 111 (pi0) -91 56 0 159 160 0 0 -0.068 0.076 6.926 6.929 0.135 101 211 pi+ 91 69 0 0 0 0 0 -0.196 -0.031 24.323 24.324 0.140 102 -211 pi- 91 69 0 0 0 0 0 0.331 -0.054 9.174 9.181 0.140 103 -211 pi- 91 74 0 0 0 0 0 -0.009 0.010 0.079 0.161 0.140 104 111 (pi0) -91 74 0 161 162 0 0 0.007 1.226 4.574 4.737 0.135 105 211 pi+ 91 75 0 0 0 0 0 0.091 0.179 1.668 1.686 0.140 106 -211 pi- 91 75 0 0 0 0 0 -0.141 0.397 0.683 0.815 0.140 107 211 pi+ 91 79 0 0 0 0 0 0.063 -0.389 0.095 0.429 0.140 108 111 (pi0) -91 79 0 163 164 0 0 0.481 0.525 0.519 0.891 0.135 109 321 K+ 91 80 0 0 0 0 0 0.218 0.827 -0.094 0.992 0.494 110 -211 pi- 91 80 0 0 0 0 0 0.083 -0.159 -0.058 0.234 0.140 111 310 (K_S0) -91 81 81 165 166 0 0 -0.129 -0.061 -0.487 0.711 0.498 112 310 (K_S0) -91 82 82 167 168 0 0 0.505 0.243 -12.024 12.047 0.498 113 211 pi+ 91 85 0 0 0 0 0 -0.246 -0.193 -53.721 53.722 0.140 114 111 (pi0) -91 85 0 169 170 0 0 0.140 0.123 -3.990 3.996 0.135 115 2112 n0 91 89 0 0 0 0 0 -0.189 0.414 -688.867 688.868 0.940 116 211 pi+ 91 89 0 0 0 0 0 -0.214 -0.262 -211.154 211.154 0.140 117 130 K_L0 91 91 91 0 0 0 0 0.376 0.917 -17.197 17.233 0.498 118 -13 mu+ 93 38 0 0 0 0 0 0.013 -0.590 -13.658 13.671 0.106 119 13 mu- 93 38 0 0 0 0 0 -3.118 -2.578 -18.371 18.811 0.106 120 22 gamma 91 44 0 0 0 0 0 0.018 0.049 -0.341 0.345 0.000 121 22 gamma 91 44 0 0 0 0 0 0.148 0.035 -3.075 3.078 0.000 122 22 gamma 91 50 0 0 0 0 0 0.029 0.212 0.069 0.225 0.000 123 22 gamma 91 50 0 0 0 0 0 -0.035 -0.001 0.026 0.043 0.000 124 211 pi+ 91 53 0 0 0 0 0 0.165 -0.123 5.610 5.615 0.140 125 -211 pi- 91 53 0 0 0 0 0 0.130 0.043 2.853 2.860 0.140 126 111 (pi0) -91 53 0 171 172 0 0 0.072 -0.075 7.843 7.845 0.135 127 22 gamma 91 55 0 0 0 0 0 0.050 -0.051 11.543 11.544 0.000 128 22 gamma 91 55 0 0 0 0 0 0.290 -0.047 94.447 94.447 0.000 129 22 gamma 91 57 0 0 0 0 0 0.014 -0.017 8.301 8.301 0.000 130 22 gamma 91 57 0 0 0 0 0 0.699 -0.019 548.856 548.856 0.000 131 22 gamma 91 58 0 0 0 0 0 0.115 -0.120 54.507 54.507 0.000 132 22 gamma 91 58 0 0 0 0 0 0.023 -0.104 647.243 647.243 0.000 133 22 gamma 91 67 0 0 0 0 0 -0.143 0.265 11.926 11.929 0.000 134 22 gamma 91 67 0 0 0 0 0 -0.012 0.066 1.123 1.125 0.000 135 22 gamma 91 76 0 0 0 0 0 0.187 0.219 0.740 0.794 0.000 136 22 gamma 91 76 0 0 0 0 0 0.090 0.049 0.119 0.157 0.000 137 22 gamma 91 77 0 0 0 0 0 0.401 -0.289 1.860 1.925 0.000 138 22 gamma 91 77 0 0 0 0 0 0.046 0.013 0.174 0.180 0.000 139 111 (pi0) -91 78 0 173 174 0 0 0.143 0.289 0.290 0.454 0.135 140 111 (pi0) -91 78 0 175 176 0 0 0.198 0.273 0.048 0.367 0.135 141 111 (pi0) -91 78 0 177 178 0 0 0.121 0.284 0.342 0.480 0.135 142 111 (pi0) -91 83 0 179 180 0 0 -0.190 -0.007 -5.406 5.411 0.135 143 111 (pi0) -91 83 0 181 182 0 0 -0.217 0.021 -3.067 3.078 0.135 144 111 (pi0) -91 83 0 183 184 0 0 -0.360 -0.098 -3.782 3.803 0.135 145 22 gamma 91 86 0 0 0 0 0 0.176 0.008 -33.415 33.416 0.000 146 22 gamma 91 86 0 0 0 0 0 0.075 0.060 -41.160 41.160 0.000 147 211 pi+ 91 88 0 0 0 0 0 0.124 0.135 -187.490 187.490 0.140 148 -211 pi- 91 88 0 0 0 0 0 -0.116 0.022 -112.263 112.263 0.140 149 111 (pi0) -91 88 0 185 186 0 0 0.076 -0.360 -323.602 323.602 0.135 150 211 pi+ 91 90 0 0 0 0 0 -0.122 -0.046 -776.087 776.087 0.140 151 -211 pi- 91 90 0 0 0 0 0 -0.028 0.269 -751.994 751.994 0.140 152 111 (pi0) -91 90 0 187 188 0 0 0.067 0.024 -93.380 93.380 0.135 153 22 gamma 91 92 0 0 0 0 0 -0.005 -0.005 -0.039 0.039 0.000 154 22 gamma 91 92 0 0 0 0 0 0.199 0.059 -11.324 11.326 0.000 155 22 gamma 91 96 0 0 0 0 0 0.044 -0.216 1.290 1.308 0.000 156 22 gamma 91 96 0 0 0 0 0 -0.024 0.010 0.196 0.197 0.000 157 22 gamma 91 98 0 0 0 0 0 -0.008 -0.198 20.468 20.469 0.000 158 22 gamma 91 98 0 0 0 0 0 0.089 -0.104 9.659 9.660 0.000 159 22 gamma 91 100 0 0 0 0 0 -0.022 -0.038 1.299 1.299 0.000 160 22 gamma 91 100 0 0 0 0 0 -0.046 0.114 5.628 5.629 0.000 161 22 gamma 91 104 0 0 0 0 0 0.023 0.223 1.033 1.057 0.000 162 22 gamma 91 104 0 0 0 0 0 -0.016 1.003 3.541 3.680 0.000 163 22 gamma 91 108 0 0 0 0 0 0.024 -0.000 0.001 0.024 0.000 164 22 gamma 91 108 0 0 0 0 0 0.457 0.525 0.518 0.868 0.000 165 111 (pi0) -91 111 0 189 190 0 0 0.046 0.122 -0.339 0.388 0.135 166 111 (pi0) -91 111 0 191 192 0 0 -0.175 -0.183 -0.148 0.323 0.135 167 211 pi+ 91 112 0 0 0 0 0 0.192 0.319 -6.541 6.553 0.140 168 -211 pi- 91 112 0 0 0 0 0 0.314 -0.077 -5.483 5.494 0.140 169 22 gamma 91 114 0 0 0 0 0 0.022 -0.028 -0.417 0.418 0.000 170 22 gamma 91 114 0 0 0 0 0 0.118 0.150 -3.573 3.578 0.000 171 22 gamma 91 126 0 0 0 0 0 0.031 0.039 2.297 2.297 0.000 172 22 gamma 91 126 0 0 0 0 0 0.040 -0.113 5.546 5.548 0.000 173 22 gamma 91 139 0 0 0 0 0 0.122 0.141 0.223 0.290 0.000 174 22 gamma 91 139 0 0 0 0 0 0.022 0.148 0.067 0.164 0.000 175 22 gamma 91 140 0 0 0 0 0 0.170 0.194 0.090 0.273 0.000 176 22 gamma 91 140 0 0 0 0 0 0.028 0.080 -0.041 0.094 0.000 177 22 gamma 91 141 0 0 0 0 0 -0.011 0.069 0.024 0.074 0.000 178 22 gamma 91 141 0 0 0 0 0 0.132 0.214 0.318 0.406 0.000 179 22 gamma 91 142 0 0 0 0 0 -0.003 0.039 -1.113 1.113 0.000 180 22 gamma 91 142 0 0 0 0 0 -0.188 -0.046 -4.293 4.298 0.000 181 22 gamma 91 143 0 0 0 0 0 -0.159 0.030 -1.342 1.351 0.000 182 22 gamma 91 143 0 0 0 0 0 -0.058 -0.009 -1.725 1.726 0.000 183 22 gamma 91 144 0 0 0 0 0 -0.287 -0.034 -3.160 3.173 0.000 184 22 gamma 91 144 0 0 0 0 0 -0.073 -0.064 -0.622 0.629 0.000 185 22 gamma 91 149 0 0 0 0 0 -0.023 -0.215 -183.563 183.563 0.000 186 22 gamma 91 149 0 0 0 0 0 0.099 -0.146 -140.039 140.039 0.000 187 22 gamma 91 152 0 0 0 0 0 0.076 0.011 -24.253 24.253 0.000 188 22 gamma 91 152 0 0 0 0 0 -0.010 0.014 -69.127 69.127 0.000 189 22 gamma 91 165 0 0 0 0 0 0.003 -0.012 0.007 0.014 0.000 190 22 gamma 91 165 0 0 0 0 0 0.043 0.135 -0.346 0.374 0.000 191 22 gamma 91 166 0 0 0 0 0 -0.023 -0.093 -0.007 0.096 0.000 192 22 gamma 91 166 0 0 0 0 0 -0.153 -0.089 -0.141 0.227 0.000 Charge sum: 2.000 Momentum sum: -0.000 -0.000 -0.000 7000.000 7000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- J/psi decay performed, J/psi in line 370, mother id = 20443 J/psi decay performed, J/psi in line 912, mother id = 20443 J/psi decay performed, J/psi in line 265, mother id = 9910441 J/psi decay performed, J/psi in line 971, mother id = 20443 J/psi decay performed, J/psi in line 180, mother id = 9900443 J/psi decay performed, J/psi in line 636, mother id = 445 J/psi decay performed, J/psi in line 313, mother id = 9900443 J/psi decay performed, J/psi in line 197, mother id = 445 PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame Pythia::next(): 1000 events have been generated PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> ccbar[3S1(1)] g 401 | 143 10 10 | 6.447e-04 1.167e-04 | | g g -> ccbar[3P0(1)] g 402 | 13681 433 433 | 3.173e-02 1.111e-03 | | g g -> ccbar[3P1(1)] g 403 | 16931 429 429 | 2.723e-02 8.090e-04 | | g g -> ccbar[3P2(1)] g 404 | 24450 572 572 | 3.866e-02 9.994e-04 | | q g -> ccbar[3P0(1)] q 405 | 7800 92 92 | 5.781e-03 3.065e-04 | | q g -> ccbar[3P1(1)] q 406 | 3436 78 78 | 5.093e-03 3.445e-04 | | q g -> ccbar[3P2(1)] q 407 | 6793 120 120 | 7.651e-03 3.984e-04 | | q qbar -> ccbar[3P0(1)] g 408 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar -> ccbar[3P1(1)] g 409 | 2 0 0 | 0.000e+00 0.000e+00 | | q qbar -> ccbar[3P2(1)] g 410 | 1 0 0 | 0.000e+00 0.000e+00 | | g g -> ccbar[3S1(8)] g 411 | 2835 83 83 | 6.449e-03 3.894e-04 | | g g -> ccbar[1S0(8)] g 412 | 1505 50 50 | 3.169e-03 3.011e-04 | | g g -> ccbar[3PJ(8)] g 413 | 1989 87 87 | 5.593e-03 4.753e-04 | | q g -> ccbar[3S1(8)] q 414 | 595 23 23 | 1.505e-03 1.919e-04 | | q g -> ccbar[1S0(8)] q 415 | 427 9 9 | 5.952e-04 1.108e-04 | | q g -> ccbar[3PJ(8)] q 416 | 917 14 14 | 1.088e-03 1.579e-04 | | q qbar -> ccbar[3S1(8)] g 417 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar -> ccbar[1S0(8)] g 418 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar -> ccbar[3PJ(8)] g 419 | 0 0 0 | 0.000e+00 0.000e+00 | | | | | | sum | 81505 2000 2000 | 1.352e-01 1.953e-03 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Error in Pythia::next: hadronLevel failed; try again | | 1 Error in StringFragmentation::fragment: stuck in joining | | 146 Warning in PhaseSpace2to2tauyz::trialKin: maximum for cross section violated | | 6 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:05 pTHat of hard subprocess 3.48*10^ 2 3 3.36*10^ 2 X 3.24*10^ 2 X 3.12*10^ 2 X3 3.00*10^ 2 XX 2.88*10^ 2 XX 2.76*10^ 2 XX 2.64*10^ 2 3XX 2.52*10^ 2 XXX 2.40*10^ 2 XXX83 2.28*10^ 2 XXXXX 2.16*10^ 2 XXXXX 2.04*10^ 2 XXXXX 1.92*10^ 2 XXXXX 1.80*10^ 2 XXXXX 1.68*10^ 2 XXXXX 1.56*10^ 2 XXXXX5 1.44*10^ 2 XXXXXX 1.32*10^ 2 XXXXXX 1.20*10^ 2 XXXXXX 1.08*10^ 2 3XXXXXX 0.96*10^ 2 XXXXXXX6 0.84*10^ 2 XXXXXXXX4 0.72*10^ 2 XXXXXXXXX 0.60*10^ 2 XXXXXXXXX5 0.48*10^ 2 XXXXXXXXXX 0.36*10^ 2 9XXXXXXXXXX25 0.24*10^ 2 XXXXXXXXXXXXX52 0.12*10^ 2 XXXXXXXXXXXXXXX8635111121 3 2 1 1 Contents *10^ 2 0002332210000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0395303359752311000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0595937101747085973611112103020001010000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^ 0 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^-1 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 2000 Mean = 3.3197e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 2.0000e+03 Rms = 1.7512e+00 Overflow = 0.0000e+00 High edge = 5.0000e+01 2013-09-20 16:05 pT of J/Psi 7.50*10^ 1 6 7.25*10^ 1 X4 7.00*10^ 1 XX 6.75*10^ 1 XX 6.50*10^ 1 XX6 6.25*10^ 1 XXX4 6.00*10^ 1 XXXX 5.75*10^ 1 XXXX 5.50*10^ 1 XXXX 5.25*10^ 1 XXXX 8 5.00*10^ 1 6XXXX X 4.75*10^ 1 XXXXX4X 4.50*10^ 1 XXXXXXX6 4.25*10^ 1 XXXXXXXX 4.00*10^ 1 XXXXXXXX 3.75*10^ 1 XXXXXXXX 3.50*10^ 1 XXXXXXXX 3.25*10^ 1 XXXXXXXX4 3.00*10^ 1 2XXXXXXXXX 2.75*10^ 1 XXXXXXXXXX 2.50*10^ 1 XXXXXXXXXX 2.25*10^ 1 XXXXXXXXXX 2.00*10^ 1 XXXXXXXXXXX 1.75*10^ 1 XXXXXXXXXXX 1.50*10^ 1 2XXXXXXXXXXX22 1.25*10^ 1 XXXXXXXXXXXXXX4 1.00*10^ 1 XXXXXXXXXXXXXXX 0.75*10^ 1 XXXXXXXXXXXXXXX88 0.50*10^ 1 XXXXXXXXXXXXXXXXX 2 2 0.25*10^ 1 XXXXXXXXXXXXXXXXX8X 844X44 4 4 Contents *10^ 1 1247766454321110000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 3894141624103317723021131100000010100000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^ 0 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^-1 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 620 Mean = 3.5024e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 6.2000e+02 Rms = 2.2078e+00 Overflow = 0.0000e+00 High edge = 5.0000e+01 pythia8-8.1.80.orig/examples/outref/out020000644000175000017500000037742012217346170016367 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:00:13 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with pbar- at a CM energy of 1.960e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | f fbar -> gamma*/Z0 221 | 2.186e-05 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 40.89 mb | | | | pT0 = 2.12 gives sigmaInteraction = 136.80 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eCM | 1960.000 | 14000.000 10.00000 | | Beams:idB | -2212 | 2212 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:mHatMax | 120.00000 | -1.00000 | | PhaseSpace:mHatMin | 80.00000 | 4.00000 0.0 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | WeakSingleBoson:ffbar2gmZ | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 9.800e+02, e = 9.800e+02, m = 9.383e-01. Beam B: id = -2212, pz = -9.800e+02, e = 9.800e+02, m = 9.383e-01. In 1: id = 1, x = 5.616e-03, pdf = 7.757e-01 at Q2 = 8.254e+03. In 2: id = -1, x = 3.826e-01, pdf = 8.111e-02 at same Q2. Subprocess f fbar -> gamma*/Z0 with code 221 is 2 -> 1. It has sHat = 8.254e+03. alphaEM = 7.817e-03, alphaS = 1.351e-01 at Q2 = 8.254e+03. Impact parameter b = 2.761e-01 gives enhancement factor = 2.827e+00. Max pT scale for MPI = 1.960e+03, ISR = 1.960e+03, FSR = 1.960e+03. Number of MPI = 7, ISR = 6, FSRproc = 39, FSRreson = 17. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 1960.000 1960.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 980.000 980.000 0.938 2 -2212 (pbar-) -12 0 0 4 0 0 0 0.000 0.000 -980.000 980.000 0.938 3 1 (d) -21 1 0 5 0 101 0 0.000 0.000 5.503 5.503 0.000 4 -1 (dbar) -21 2 0 5 0 0 101 0.000 0.000 -374.961 374.961 0.000 5 23 (Z0) -22 3 4 6 7 0 0 0.000 0.000 -369.458 380.465 90.854 6 4 c 23 5 0 0 0 102 0 40.598 -5.065 -267.166 270.285 1.500 7 -4 cbar 23 5 0 0 0 0 102 -40.598 5.065 -102.292 110.180 1.500 Charge sum: 0.000 Momentum sum: 0.000 0.000 -369.458 380.465 90.854 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 1960.000 1960.000 1 2212 (p+) -12 0 0 198 0 0 0 0.000 0.000 980.000 980.000 0.938 2 -2212 (pbar-) -12 0 0 199 0 0 0 0.000 0.000 -980.000 980.000 0.938 3 1 (d) -21 198 198 5 0 101 0 0.000 0.000 5.503 5.503 0.000 4 -1 (dbar) -21 199 199 5 0 0 101 0.000 0.000 -374.961 374.961 0.000 5 23 (Z0) -22 3 4 200 200 0 0 0.000 0.000 -369.458 380.465 90.854 6 21 (g) -31 10 10 8 9 104 103 0.000 0.000 2.874 2.874 0.000 7 21 (g) -31 11 0 8 9 105 104 0.000 0.000 -64.663 64.663 0.000 8 21 (g) -33 6 7 12 12 106 103 4.205 -1.656 0.964 4.621 0.000 9 21 (g) -33 6 7 13 13 105 106 -4.205 1.656 -62.753 62.916 0.000 10 21 (g) -42 33 33 6 6 104 103 0.000 -0.000 2.874 2.874 0.000 11 21 (g) -41 35 35 14 7 105 107 -0.000 0.000 -109.594 109.594 0.000 12 21 (g) -44 8 8 22 23 106 103 4.261 -1.722 0.910 4.685 0.000 13 21 (g) -44 9 9 24 24 105 106 -2.297 -0.617 -64.829 64.872 0.000 14 21 (g) -43 11 0 31 32 104 107 -1.963 2.338 -42.802 42.911 0.000 15 21 (g) -31 25 25 17 18 108 109 0.000 0.000 145.678 145.678 0.000 16 21 (g) -31 26 0 17 18 109 110 0.000 0.000 -1.138 1.138 0.000 17 21 (g) -33 15 16 19 20 108 111 -2.131 1.064 144.411 144.431 0.000 18 21 (g) -33 15 16 21 21 111 110 2.131 -1.064 0.128 2.385 0.000 19 21 (g) -51 17 0 27 27 108 112 -2.160 -1.017 120.302 120.325 0.000 20 21 (g) -51 17 0 29 29 112 111 0.114 2.039 24.114 24.201 0.000 21 21 (g) -52 18 18 28 28 111 110 2.046 -1.022 0.123 2.290 0.000 22 21 (g) -51 12 0 36 36 113 103 2.756 0.289 1.279 3.052 0.000 23 21 (g) -51 12 0 39 39 106 113 1.453 -2.025 -1.824 3.088 0.000 24 21 (g) -52 13 13 37 37 105 106 -2.246 -0.603 -63.374 63.416 0.000 25 21 (g) -42 226 226 15 15 108 109 -0.000 0.000 145.678 145.678 0.000 26 21 (g) -41 227 227 30 16 114 110 0.000 -0.000 -3.743 3.743 0.000 27 21 (g) -44 19 19 66 66 108 112 -2.151 -1.033 119.424 119.448 0.000 28 21 (g) -44 21 21 79 80 111 110 2.835 -2.465 2.145 4.326 0.000 29 21 (g) -44 20 20 64 65 112 111 0.146 1.981 22.675 22.762 0.000 30 21 (g) -43 26 0 231 231 114 109 -0.829 1.517 -2.310 2.885 0.000 31 21 (g) -51 14 0 38 38 115 107 -2.845 3.087 -37.223 37.459 0.000 32 21 (g) -51 14 0 40 40 104 115 0.881 -0.748 -5.454 5.576 0.000 33 21 (g) -53 34 0 10 10 104 103 0.000 -0.000 2.998 2.998 0.000 34 21 (g) -41 92 92 41 33 104 116 -0.000 -0.000 14.290 14.290 0.000 35 21 (g) -42 93 0 11 11 105 107 0.000 0.000 -109.594 109.594 0.000 36 21 (g) -44 22 22 70 71 113 103 3.263 1.395 0.722 3.621 0.000 37 21 (g) -44 24 24 95 95 105 106 -2.241 -0.592 -62.787 62.830 0.000 38 21 (g) -44 31 31 58 59 115 107 -2.817 3.147 -37.585 37.821 0.000 39 21 (g) -44 23 23 75 75 106 113 1.601 -1.702 -1.519 2.787 0.000 40 21 (g) -44 32 32 60 60 104 115 0.895 -0.717 -5.356 5.478 0.000 41 21 (g) -43 34 0 72 72 103 116 -0.701 -1.531 11.222 11.347 0.000 42 2 (u) -31 239 239 44 45 117 0 0.000 0.000 247.809 247.809 0.000 43 21 (g) -31 240 240 44 45 118 117 0.000 0.000 -1.093 1.093 0.000 44 2 (u) -33 42 43 46 47 119 0 1.498 -0.634 247.199 247.205 0.330 45 21 (g) -33 42 43 48 48 118 119 -1.498 0.634 -0.484 1.697 0.000 46 2 (u) -51 44 0 137 138 120 0 0.154 0.544 197.004 197.005 0.330 47 21 (g) -51 44 0 63 63 119 120 1.326 -1.170 50.190 50.221 0.000 48 21 (g) -52 45 45 61 62 118 119 -1.480 0.626 -0.478 1.676 0.000 49 21 (g) -31 53 0 51 52 121 122 0.000 0.000 38.712 38.712 0.000 50 21 (g) -31 54 54 51 52 122 123 0.000 0.000 -1.426 1.426 0.000 51 21 (g) -33 49 50 55 55 121 124 0.423 -1.394 38.322 38.350 0.000 52 21 (g) -33 49 50 56 56 124 123 -0.423 1.394 -1.037 1.788 0.000 53 21 (g) -41 249 249 57 49 125 122 -0.000 0.000 244.566 244.566 0.000 54 21 (g) -42 250 250 50 50 122 123 0.000 -0.000 -1.426 1.426 0.000 55 21 (g) -44 51 51 67 68 121 124 -0.323 -0.168 38.769 38.771 0.000 56 21 (g) -44 52 52 69 69 124 123 -0.431 1.406 -1.043 1.803 0.000 57 21 (g) -43 53 0 161 161 125 121 0.753 -1.238 205.414 205.419 0.000 58 21 (g) -51 38 0 87 87 126 107 -2.039 2.004 -15.618 15.877 0.000 59 21 (g) -51 38 0 85 86 115 126 -0.456 0.886 -23.892 23.913 0.000 60 21 (g) -52 40 40 98 98 104 115 0.574 -0.460 -3.431 3.509 0.000 61 21 (g) -51 48 0 127 127 118 127 -1.000 1.652 0.261 1.948 0.000 62 21 (g) -51 48 0 125 126 127 119 -0.429 -1.071 1.188 1.656 0.000 63 21 (g) -52 47 47 139 139 119 120 1.275 -1.125 48.263 48.293 0.000 64 21 (g) -51 29 0 81 81 128 111 0.223 1.712 46.220 46.253 0.000 65 21 (g) -51 29 0 150 151 112 128 -0.546 0.044 2.481 2.541 0.000 66 21 (g) -52 27 27 152 152 108 112 -1.683 -0.808 93.398 93.416 0.000 67 21 (g) -51 55 0 76 77 121 129 0.792 -0.629 5.223 5.320 0.000 68 21 (g) -51 55 0 78 78 129 124 -1.132 0.519 33.503 33.526 0.000 69 21 (g) -52 56 56 84 84 124 123 -0.413 1.347 -1.000 1.728 0.000 70 21 (g) -51 36 0 73 74 113 130 1.398 0.859 2.036 2.615 0.000 71 21 (g) -51 36 0 101 101 130 103 1.809 0.414 -0.426 1.904 0.000 72 21 (g) -52 41 41 99 99 103 116 -0.646 -1.410 10.334 10.449 0.000 73 21 (g) -51 70 0 94 94 131 130 2.102 0.182 1.733 2.730 0.000 74 21 (g) -51 70 0 102 102 113 131 -0.362 0.314 -0.022 0.480 0.000 75 21 (g) -52 39 39 97 97 106 113 1.259 -1.338 -1.194 2.191 0.000 76 21 (g) -51 67 0 153 154 121 132 0.406 -0.909 16.781 16.811 0.000 77 21 (g) -51 67 0 155 155 132 129 -0.056 0.482 1.503 1.579 0.000 78 21 (g) -52 68 68 82 83 129 124 -0.691 0.317 20.442 20.456 0.000 79 21 (g) -51 28 0 119 120 133 110 2.977 -1.540 1.813 3.811 0.000 80 21 (g) -51 28 0 121 121 111 133 -0.134 -0.864 1.984 2.168 0.000 81 21 (g) -52 64 64 156 157 128 111 0.215 1.651 44.569 44.600 0.000 82 21 (g) -51 78 0 144 145 129 134 -0.765 0.441 20.468 20.487 0.000 83 21 (g) -51 78 0 146 146 134 124 0.038 -0.006 -0.114 0.120 0.000 84 21 (g) -52 69 69 252 252 124 123 -0.377 1.229 -0.912 1.576 0.000 85 1 (d) -51 59 0 100 100 115 0 0.301 0.139 -7.170 7.185 0.330 86 -1 (dbar) -51 59 0 103 103 0 126 -1.533 1.509 -22.663 22.767 0.330 87 21 (g) -52 58 58 96 96 126 107 -1.264 1.241 -9.677 9.838 0.000 88 1 (d) -31 262 262 90 91 135 0 0.000 0.000 56.111 56.111 0.000 89 21 (g) -31 263 263 90 91 136 137 0.000 0.000 -5.099 5.099 0.000 90 1 (d) -33 88 89 264 264 136 0 0.691 -0.455 56.073 56.080 0.330 91 21 (g) -33 88 89 265 265 135 137 -0.691 0.455 -5.062 5.129 0.000 92 21 (g) -42 105 0 34 34 104 116 0.000 -0.000 14.290 14.290 0.000 93 21 (g) -41 106 106 104 35 105 138 -0.000 0.000 -123.927 123.927 0.000 94 21 (g) -44 73 73 107 107 131 130 2.105 0.180 1.737 2.735 0.000 95 21 (g) -44 37 37 108 108 105 106 -1.840 -0.805 -62.847 62.879 0.000 96 21 (g) -44 87 87 109 109 126 107 -1.201 1.208 -9.692 9.840 0.000 97 21 (g) -44 75 75 110 110 106 113 1.269 -1.344 -1.190 2.198 0.000 98 21 (g) -44 60 60 111 111 104 115 0.596 -0.471 -3.432 3.515 0.000 99 21 (g) -44 72 72 112 112 103 116 -0.645 -1.410 10.325 10.441 0.000 100 1 (d) -44 85 85 113 113 115 0 0.347 0.114 -7.176 7.192 0.330 101 21 (g) -44 71 71 114 114 130 103 1.817 0.410 -0.422 1.910 0.000 102 21 (g) -44 74 74 115 115 113 131 -0.361 0.313 -0.024 0.478 0.000 103 -1 (dbar) -44 86 86 116 116 0 126 -1.388 1.432 -22.690 22.780 0.330 104 21 (g) -43 93 0 117 117 107 138 -0.699 0.371 -14.226 14.248 0.000 105 21 (g) -41 201 201 118 92 104 139 0.000 0.000 63.915 63.915 0.000 106 21 (g) -42 202 202 93 93 105 138 -0.000 0.000 -123.927 123.927 0.000 107 21 (g) -44 94 94 122 123 131 130 2.039 0.081 1.771 2.702 0.000 108 21 (g) -44 95 95 130 130 105 106 -1.840 -0.805 -62.886 62.918 0.000 109 21 (g) -44 96 96 174 175 126 107 -1.203 1.205 -9.682 9.830 0.000 110 21 (g) -44 97 97 128 129 106 113 1.255 -1.366 -1.201 2.210 0.000 111 21 (g) -44 98 98 207 207 104 115 0.594 -0.473 -3.433 3.516 0.000 112 21 (g) -44 99 99 136 136 103 116 -0.951 -1.867 10.278 10.489 0.000 113 1 (d) -44 100 100 209 209 115 0 0.346 0.114 -7.167 7.184 0.330 114 21 (g) -44 101 101 180 181 130 103 1.795 0.378 -0.387 1.875 0.000 115 21 (g) -44 102 102 124 124 113 131 -0.367 0.303 -0.023 0.477 0.000 116 -1 (dbar) -44 103 103 212 212 0 126 -1.389 1.430 -22.676 22.766 0.330 117 21 (g) -44 104 104 176 176 107 138 -0.700 0.370 -14.227 14.249 0.000 118 21 (g) -43 105 0 134 135 116 139 0.421 0.630 49.621 49.626 0.000 119 21 (g) -51 79 0 229 229 140 110 1.751 -1.415 0.711 2.361 0.000 120 21 (g) -51 79 0 179 179 133 140 1.185 -0.394 1.719 2.124 0.000 121 21 (g) -52 80 80 158 158 111 133 -0.093 -0.595 1.367 1.494 0.000 122 21 (g) -51 107 0 203 203 141 130 -0.031 -0.363 0.516 0.631 0.000 123 21 (g) -51 107 0 188 188 131 141 1.872 0.608 1.243 2.328 0.000 124 21 (g) -52 115 115 186 187 113 131 -0.169 0.140 -0.010 0.220 0.000 125 21 (g) -51 62 0 244 244 142 119 0.100 -0.008 1.076 1.081 0.000 126 21 (g) -51 62 0 162 163 127 142 -0.764 -0.674 0.173 1.033 0.000 127 21 (g) -52 61 61 164 164 118 127 -0.765 1.263 0.199 1.490 0.000 128 21 (g) -51 110 0 131 132 143 113 0.493 0.317 -1.616 1.719 0.000 129 21 (g) -51 110 0 133 133 106 143 0.707 -1.706 -1.428 2.335 0.000 130 21 (g) -52 108 108 204 204 105 106 -1.786 -0.782 -61.042 61.073 0.000 131 21 (g) -51 128 0 173 173 144 113 0.259 0.457 -0.972 1.105 0.000 132 21 (g) -51 128 0 171 172 143 144 0.599 -1.022 -1.381 1.820 0.000 133 21 (g) -52 129 129 216 216 106 143 0.342 -0.825 -0.691 1.129 0.000 134 21 (g) -51 118 0 165 166 145 139 0.007 0.320 49.282 49.283 0.000 135 21 (g) -51 118 0 167 167 116 145 0.299 0.084 1.579 1.609 0.000 136 21 (g) -52 112 112 182 182 103 116 -0.836 -1.642 9.037 9.223 0.000 137 2 (u) -51 46 0 241 241 146 0 0.769 0.415 113.210 113.214 0.330 138 21 (g) -51 46 0 149 149 120 146 -0.449 -0.017 90.056 90.057 0.000 139 21 (g) -52 63 63 147 148 119 120 1.110 -0.979 42.001 42.027 0.000 140 21 (g) -31 266 266 142 143 148 149 0.000 0.000 7.354 7.354 0.000 141 1 (d) -31 267 267 142 143 147 0 0.000 0.000 -0.075 0.075 0.000 142 21 (g) -33 140 141 268 268 147 149 -0.585 0.123 5.346 5.379 0.000 143 1 (d) -33 140 141 269 269 148 0 0.585 -0.123 1.933 2.050 0.330 144 21 (g) -51 82 0 168 169 129 150 -0.655 0.873 16.528 16.564 0.000 145 21 (g) -51 82 0 170 170 150 134 -0.103 -0.433 3.919 3.945 0.000 146 21 (g) -52 83 83 256 256 134 124 0.031 -0.005 -0.093 0.099 0.000 147 3 (s) -51 139 0 243 243 119 0 0.209 -0.004 18.089 18.097 0.500 148 -3 (sbar) -51 139 0 247 247 0 120 0.773 -0.979 49.481 49.499 0.500 149 21 (g) -52 138 138 246 246 120 146 -0.322 -0.012 64.488 64.488 0.000 150 -3 (sbar) -51 65 0 232 232 0 128 -0.185 -0.217 6.832 6.856 0.500 151 3 (s) -51 65 0 197 197 112 0 -0.585 0.154 8.067 8.105 0.500 152 21 (g) -52 66 66 195 196 108 112 -1.459 -0.700 80.980 80.996 0.000 153 21 (g) -51 76 0 159 160 121 152 -0.166 -0.623 12.940 12.956 0.000 154 21 (g) -51 76 0 258 258 152 132 0.554 -0.134 4.313 4.351 0.000 155 21 (g) -52 77 77 189 190 132 129 -0.038 0.331 1.030 1.082 0.000 156 21 (g) -51 81 0 230 230 128 153 0.519 0.429 19.749 19.760 0.000 157 21 (g) -51 81 0 236 236 153 111 -0.311 1.176 24.928 24.958 0.000 158 21 (g) -52 121 121 177 178 111 133 -0.085 -0.548 1.259 1.376 0.000 159 21 (g) -51 153 0 251 251 154 152 -0.100 -0.088 0.762 0.773 0.000 160 21 (g) -51 153 0 259 259 121 154 0.111 -0.826 60.472 60.478 0.000 161 21 (g) -52 57 57 253 253 125 121 0.576 -0.947 157.120 157.124 0.000 162 21 (g) -51 126 0 245 245 155 142 -1.016 -0.152 0.482 1.134 0.000 163 21 (g) -51 126 0 248 248 127 155 0.041 -0.174 -0.254 0.310 0.000 164 21 (g) -52 127 127 242 242 118 127 -0.554 0.914 0.144 1.079 0.000 165 21 (g) -51 134 0 214 214 156 139 -0.062 -0.336 13.478 13.482 0.000 166 21 (g) -51 134 0 219 219 145 156 0.169 0.684 36.332 36.339 0.000 167 21 (g) -52 135 135 218 218 116 145 0.199 0.056 1.052 1.072 0.000 168 21 (g) -51 144 0 191 191 129 157 -0.630 0.547 18.442 18.461 0.000 169 21 (g) -51 144 0 260 260 157 150 -0.081 0.090 0.221 0.252 0.000 170 21 (g) -52 145 145 257 257 150 134 -0.047 -0.197 1.784 1.795 0.000 171 21 (g) -51 132 0 217 217 143 158 -0.009 -0.097 -1.057 1.061 0.000 172 21 (g) -51 132 0 220 220 158 144 0.733 -0.706 -0.791 1.289 0.000 173 21 (g) -52 131 131 206 206 144 113 0.135 0.238 -0.506 0.575 0.000 174 21 (g) -51 109 0 205 205 126 159 -0.217 0.308 -6.596 6.607 0.000 175 21 (g) -51 109 0 221 221 159 107 -1.301 1.064 -9.482 9.629 0.000 176 21 (g) -52 117 117 213 213 107 138 -0.385 0.204 -7.831 7.843 0.000 177 21 (g) -51 158 0 233 233 111 160 0.620 -0.935 1.748 2.076 0.000 178 21 (g) -51 158 0 237 237 160 133 -0.016 0.157 0.512 0.536 0.000 179 21 (g) -52 120 120 234 234 133 140 0.495 -0.165 0.718 0.888 0.000 180 21 (g) -51 114 0 192 193 130 161 1.900 0.138 -0.289 1.927 0.000 181 21 (g) -51 114 0 185 185 161 103 -0.150 0.152 0.386 0.441 0.000 182 21 (g) -52 136 136 183 184 103 116 -0.792 -1.554 8.554 8.730 0.000 183 21 (g) -51 182 0 208 208 162 116 0.165 -0.138 1.270 1.288 0.000 184 21 (g) -51 182 0 223 223 103 162 -1.039 -1.333 7.495 7.683 0.000 185 21 (g) -52 181 181 194 194 161 103 -0.068 0.069 0.174 0.199 0.000 186 21 (g) -51 124 0 211 211 113 163 0.484 -0.139 0.043 0.506 0.000 187 21 (g) -51 124 0 224 224 163 131 0.223 0.563 0.529 0.804 0.000 188 21 (g) -52 123 123 215 215 131 141 0.996 0.323 0.661 1.238 0.000 189 2 (u) -51 155 0 255 255 132 0 -0.307 0.423 8.283 8.306 0.330 190 -2 (ubar) -51 155 0 261 261 0 129 -0.041 0.177 1.815 1.854 0.330 191 21 (g) -52 168 168 254 254 129 157 -0.320 0.278 9.374 9.384 0.000 192 21 (g) -51 180 0 210 210 130 164 0.168 -0.010 -0.302 0.346 0.000 193 21 (g) -51 180 0 225 225 164 161 1.690 0.191 0.121 1.705 0.000 194 21 (g) -52 185 185 222 222 161 103 -0.026 0.026 0.066 0.075 0.000 195 21 (g) -51 152 0 228 228 108 165 -0.372 -0.576 33.829 33.836 0.000 196 21 (g) -51 152 0 238 238 165 112 -1.143 -0.094 47.052 47.066 0.000 197 3 (s) -52 151 151 235 235 112 0 -0.529 0.123 8.166 8.199 0.500 198 1 (d) -61 1 0 3 3 101 0 0.554 0.553 5.474 5.530 0.000 199 -1 (dbar) -61 2 0 4 4 0 101 -0.368 -1.837 -374.969 374.974 0.000 200 23 (Z0) -62 5 5 274 275 0 0 0.187 -1.284 -369.496 380.504 90.854 201 21 (g) -61 1 0 105 105 104 101 1.859 0.234 63.899 63.926 0.000 202 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133 462 462 106 143 0.339 -0.821 -0.697 1.129 0.000 217 21 (g) -62 171 171 461 461 143 158 -0.020 -0.093 -1.056 1.061 0.000 218 21 (g) -62 167 167 342 0 116 145 0.230 0.060 1.047 1.074 0.000 219 21 (g) -62 166 166 465 465 145 156 1.226 0.817 36.319 36.349 0.000 220 21 (g) -62 172 172 460 460 158 144 0.729 -0.701 -0.806 1.293 0.000 221 21 (g) -62 175 175 419 419 159 107 -1.399 1.097 -9.455 9.620 0.000 222 21 (g) -62 194 194 343 0 161 103 -0.024 0.026 0.066 0.075 0.000 223 21 (g) -62 184 184 343 0 103 162 -0.819 -1.305 7.514 7.670 0.000 224 21 (g) -62 187 187 457 457 163 131 0.241 0.566 0.524 0.808 0.000 225 21 (g) -62 193 193 468 468 164 161 1.708 0.197 0.088 1.722 0.000 226 21 (g) -61 1 0 25 25 108 109 2.322 -0.574 146.028 146.048 0.000 227 21 (g) -61 2 0 26 26 114 110 1.677 -0.099 -3.559 3.936 0.000 228 21 (g) -62 195 195 328 0 108 121 0.168 -0.709 33.837 33.845 0.000 229 21 (g) -62 119 119 436 436 140 134 2.152 -1.444 1.150 2.835 0.000 230 21 (g) -62 156 156 356 356 128 153 0.838 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-0.225 -1.254 60.433 60.447 0.000 260 21 (g) -62 169 169 331 0 157 160 -0.060 0.088 0.172 0.202 0.000 261 -2 (ubar) -62 190 190 440 440 0 111 -0.024 0.165 1.794 1.832 0.330 262 1 (d) -61 1 0 88 88 137 0 -1.914 -0.738 56.233 56.271 0.000 263 21 (g) -61 2 0 89 89 136 137 -0.334 -0.373 -5.082 5.107 0.000 264 1 (d) -62 90 90 417 417 136 0 -1.222 -1.193 56.199 56.226 0.330 265 21 (g) -62 91 91 434 434 135 110 -1.026 0.082 -5.048 5.151 0.000 266 21 (g) -61 1 0 140 140 148 108 -0.057 0.474 7.992 8.006 0.000 267 1 (d) -61 2 0 141 141 108 0 -0.044 0.695 1.279 1.457 0.000 268 21 (g) -62 142 142 340 0 147 132 -0.641 0.665 6.801 6.864 0.000 269 1 (d) -62 143 143 364 364 148 0 0.540 0.504 2.470 2.599 0.330 270 2 (u) -63 1 0 344 344 109 0 -0.023 0.273 7.782 7.794 0.330 271 -1 (dbar) -63 1 0 365 365 0 148 -0.333 0.042 197.866 197.866 0.330 272 -2203 (uu_1bar) -63 2 0 433 433 110 0 -1.104 1.173 -461.573 461.576 0.771 273 -1 (dbar) -63 2 0 377 377 0 114 -0.254 0.213 -7.995 8.009 0.330 274 4 (c) -23 200 0 276 277 102 0 40.730 -5.977 -267.193 270.350 1.500 275 -4 (cbar) -23 200 0 278 278 0 102 -40.543 4.693 -102.302 110.154 1.500 276 4 (c) -51 274 0 282 283 171 0 8.956 -10.722 -127.181 127.955 1.500 277 21 (g) -51 274 0 281 281 102 171 29.002 5.066 -146.993 149.912 0.000 278 -4 (cbar) -52 275 275 279 280 0 102 -37.771 4.373 -95.322 102.637 1.500 279 -4 (cbar) -51 278 0 294 295 0 174 -32.518 0.298 -80.951 87.252 1.500 280 21 (g) -51 278 0 291 292 174 102 -4.630 4.183 -17.531 18.609 0.000 281 21 (g) -52 277 277 284 284 102 171 28.379 4.957 -143.832 146.688 0.000 282 4 (c) -51 276 0 287 287 176 0 7.097 -10.207 -111.174 111.877 1.500 283 21 (g) -51 276 0 285 286 171 176 5.328 0.091 -33.590 34.010 0.000 284 21 (g) -52 281 281 293 293 102 171 24.909 4.351 -126.249 128.757 0.000 285 2 (u) -51 283 0 305 305 171 0 3.691 -0.931 -19.721 20.087 0.330 286 -2 (ubar) -51 283 0 288 289 0 176 2.182 0.194 -22.683 22.791 0.330 287 4 (c) -52 282 282 290 290 176 0 6.553 -9.380 -102.359 103.008 1.500 288 -2 (ubar) -51 286 0 297 298 0 177 0.459 -0.270 -17.266 17.277 0.330 289 21 (g) -51 286 0 299 299 177 176 2.731 -1.079 -21.504 21.703 0.000 290 4 (c) -52 287 287 348 348 176 0 5.545 -7.837 -86.273 86.819 1.500 291 21 (g) -51 280 0 296 296 174 178 -4.067 3.616 -12.826 13.933 0.000 292 21 (g) -51 280 0 300 301 178 102 0.019 0.669 -7.657 7.686 0.000 293 21 (g) -52 284 284 302 302 102 171 24.327 4.249 -123.298 125.746 0.000 294 -4 (cbar) -51 279 0 323 323 0 179 -30.736 -0.032 -75.677 81.695 1.500 295 21 (g) -51 279 0 315 316 179 174 -2.111 0.624 -6.316 6.688 0.000 296 21 (g) -52 291 291 317 317 174 178 -3.737 3.323 -11.785 12.802 0.000 297 -2 (ubar) -51 288 0 314 314 0 180 1.649 -1.027 -29.250 29.316 0.330 298 21 (g) -51 288 0 312 313 180 177 0.702 0.010 -2.918 3.001 0.000 299 21 (g) -52 289 289 330 0 177 176 0.838 -0.331 -6.602 6.663 0.000 300 21 (g) -51 292 0 326 326 178 181 1.652 0.356 -13.455 13.561 0.000 301 21 (g) -51 292 0 306 307 181 102 -0.071 0.585 -2.115 2.195 0.000 302 21 (g) -52 293 293 303 304 102 171 22.766 3.977 -115.384 117.676 0.000 303 21 (g) -51 302 0 308 308 102 182 18.386 2.471 -92.068 93.919 0.000 304 21 (g) -51 302 0 318 319 182 171 4.811 1.379 -25.628 26.112 0.000 305 2 (u) -52 285 285 335 0 171 0 3.260 -0.804 -17.409 17.733 0.330 306 21 (g) -51 301 0 309 310 181 183 0.935 0.959 -7.322 7.444 0.000 307 21 (g) -51 301 0 311 311 183 102 0.114 -0.224 -0.403 0.475 0.000 308 21 (g) -52 303 303 320 320 102 182 17.265 2.320 -86.458 88.195 0.000 309 21 (g) -51 306 0 336 0 181 184 1.043 0.464 -7.237 7.327 0.000 310 21 (g) -51 306 0 334 0 184 183 -0.009 0.302 -0.435 0.529 0.000 311 21 (g) -52 307 307 334 0 183 102 0.015 -0.030 -0.053 0.063 0.000 312 21 (g) -51 298 0 330 0 185 177 0.438 -0.114 -1.370 1.443 0.000 313 21 (g) -51 298 0 329 0 180 185 0.871 -0.270 -12.661 12.694 0.000 314 -2 (ubar) -52 297 297 329 0 0 180 1.042 -0.633 -18.137 18.181 0.330 315 21 (g) -51 295 0 321 322 179 186 -2.700 1.097 -8.572 9.054 0.000 316 21 (g) -51 295 0 333 0 186 174 -0.942 0.888 -2.572 2.880 0.000 317 21 (g) -52 296 296 324 325 174 178 -2.206 1.961 -6.956 7.556 0.000 318 21 (g) -51 304 0 335 0 187 171 0.511 0.005 -3.461 3.498 0.000 319 21 (g) -51 304 0 393 393 182 187 11.160 2.296 -56.522 57.659 0.000 320 21 (g) -52 308 308 394 394 102 182 10.405 1.398 -52.103 53.150 0.000 321 21 (g) -51 315 0 399 399 188 186 -2.065 0.745 -7.420 7.738 0.000 322 21 (g) -51 315 0 337 0 179 188 -3.174 0.322 -7.354 8.016 0.000 323 -4 (cbar) -52 294 294 337 0 0 179 -28.198 -0.001 -69.476 74.995 1.500 324 21 (g) -51 317 0 333 0 174 189 -1.447 1.643 -4.472 4.979 0.000 325 21 (g) -51 317 0 397 397 189 178 -0.695 0.332 -3.003 3.100 0.000 326 21 (g) -52 300 300 336 0 178 181 1.588 0.342 -12.936 13.038 0.000 327 3 (s) -73 235 254 501 501 129 0 -0.758 0.305 17.203 17.238 0.741 328 21 (g) -73 228 259 497 497 108 125 -0.057 -1.963 94.270 94.291 0.393 329 -2 (ubar) -73 313 314 350 350 0 185 1.913 -0.903 -30.798 30.875 0.506 330 21 (g) -73 299 312 349 349 185 176 1.276 -0.446 -7.972 8.106 0.574 331 21 (g) -73 237 260 438 438 157 133 -0.062 0.244 0.680 0.734 0.113 332 21 (g) -73 248 256 435 435 134 135 0.126 -0.232 -0.254 0.499 0.339 333 21 (g) -73 316 324 398 398 186 189 -2.389 2.531 -7.044 7.859 0.162 334 21 (g) -73 310 311 395 395 184 102 0.006 0.272 -0.488 0.592 0.195 335 2 (u) -73 305 318 392 392 187 0 3.772 -0.799 -20.869 21.231 0.598 336 21 (g) -73 309 326 396 396 178 184 2.632 0.806 -20.174 20.365 0.416 337 -4 (cbar) -73 322 323 400 400 0 188 -31.372 0.320 -76.829 83.011 1.936 338 21 (g) -73 251 257 372 372 154 119 -0.144 -0.302 2.438 2.464 0.122 339 21 (g) -73 244 258 357 357 152 128 0.649 -0.169 5.776 5.816 0.098 340 2 (u) -73 255 268 354 354 147 0 -0.977 1.031 14.859 14.944 0.708 341 -1 (dbar) -73 205 212 420 420 0 159 -1.911 1.837 -29.237 29.362 0.548 342 21 (g) -73 208 218 466 466 162 145 0.432 -0.073 2.314 2.364 0.200 343 21 (g) -73 222 223 467 467 161 162 -0.842 -1.279 7.580 7.745 0.430 344 2 (u) -71 270 270 346 347 109 0 -0.023 0.273 7.782 7.794 0.330 345 -3 (sbar) -71 247 247 346 347 0 109 0.565 -0.689 49.536 49.546 0.500 346 213 (rho+) -82 344 345 515 516 0 0 0.332 -0.623 42.402 42.413 0.667 347 311 (K0) -82 344 345 517 517 0 0 0.210 0.208 14.916 14.928 0.498 348 4 (c) -71 290 290 351 353 176 0 5.545 -7.837 -86.273 86.819 1.500 349 21 (g) -71 330 330 351 353 185 176 1.276 -0.446 -7.972 8.106 0.574 350 -2 (ubar) -71 329 329 351 353 0 185 1.913 -0.903 -30.798 30.875 0.506 351 433 (D*_s+) -83 348 350 620 621 0 0 5.497 -7.814 -87.432 87.978 2.112 352 -311 (Kbar0) -84 348 350 518 518 0 0 2.072 -0.963 -17.066 17.225 0.498 353 -213 (rho-) -84 348 350 519 520 0 0 1.166 -0.409 -20.545 20.596 0.760 354 2 (u) -71 340 340 359 363 147 0 -0.977 1.031 14.859 14.944 0.708 355 21 (g) -71 236 236 359 363 153 147 0.092 1.077 24.908 24.932 0.000 356 21 (g) -71 230 230 359 363 128 153 0.838 0.350 19.904 19.925 0.000 357 21 (g) -71 339 339 359 363 152 128 0.649 -0.169 5.776 5.816 0.098 358 -3 (sbar) -71 232 232 359 363 0 152 -0.071 -0.244 6.811 6.834 0.500 359 211 pi+ 83 354 358 0 0 0 0 -0.152 -0.015 1.882 1.893 0.140 360 -211 pi- 84 354 358 0 0 0 0 0.141 1.282 26.538 26.570 0.140 361 331 (eta') -84 354 358 622 624 0 0 -0.143 0.005 7.303 7.367 0.958 362 323 (K*+) -84 354 358 521 522 0 0 0.149 0.985 19.837 19.881 0.877 363 333 (phi) -84 354 358 625 626 0 0 0.535 -0.213 16.699 16.739 1.005 364 1 (d) -71 269 269 366 370 148 0 0.540 0.504 2.470 2.599 0.330 365 -1 (dbar) -71 271 271 366 370 0 148 -0.333 0.042 197.866 197.866 0.330 366 -211 pi- 83 364 365 0 0 0 0 0.023 0.248 0.794 0.844 0.140 367 213 (rho+) -84 364 365 523 524 0 0 0.171 -0.017 14.144 14.196 1.200 368 311 (K0) -84 364 365 525 525 0 0 0.367 -0.077 19.317 19.328 0.498 369 -313 (K*bar0) -84 364 365 526 527 0 0 -0.259 0.232 37.482 37.495 0.894 370 113 (rho0) -84 364 365 528 529 0 0 -0.095 0.161 128.598 128.604 1.205 371 3 (s) -71 243 243 378 391 119 0 0.132 0.102 18.085 18.092 0.500 372 21 (g) -71 338 338 378 391 154 119 -0.144 -0.302 2.438 2.464 0.122 373 21 (g) -71 245 245 378 391 155 154 -1.116 -0.209 0.657 1.312 0.000 374 21 (g) -71 242 242 378 391 118 155 -0.695 0.828 0.151 1.092 0.000 375 21 (g) -71 252 252 378 391 124 118 1.408 1.246 -0.525 1.952 0.000 376 21 (g) -71 231 231 378 391 114 124 0.335 1.447 -2.378 2.804 0.000 377 -1 (dbar) -71 273 273 378 391 0 114 -0.254 0.213 -7.995 8.009 0.330 378 -313 (K*bar0) -83 371 377 530 531 0 0 -0.175 -0.206 5.412 5.492 0.894 379 111 (pi0) -83 371 377 627 628 0 0 0.037 -0.122 0.707 0.731 0.135 380 311 (K0) -83 371 377 532 532 0 0 -0.142 -0.056 3.312 3.353 0.498 381 -311 (Kbar0) -83 371 377 533 533 0 0 0.017 0.655 7.016 7.064 0.498 382 111 (pi0) -83 371 377 629 630 0 0 0.233 -0.220 0.724 0.804 0.135 383 -211 pi- 83 371 377 0 0 0 0 -0.477 -0.630 3.469 3.561 0.140 384 211 pi+ 84 371 377 0 0 0 0 -0.489 0.738 0.156 0.910 0.140 385 223 (omega) -84 371 377 631 633 0 0 0.546 0.485 -0.019 1.072 0.785 386 313 (K*0) -84 371 377 534 535 0 0 0.054 0.540 -0.147 1.000 0.828 387 -313 (K*bar0) -84 371 377 536 537 0 0 -0.590 0.664 -1.380 1.877 0.912 388 311 (K0) -84 371 377 538 538 0 0 -0.142 -0.030 -0.437 0.678 0.498 389 -311 (Kbar0) -84 371 377 539 539 0 0 0.544 0.384 -0.385 0.916 0.498 390 -211 pi- 84 371 377 0 0 0 0 0.111 0.424 -6.007 6.025 0.140 391 213 (rho+) -84 371 377 540 541 0 0 0.139 0.699 -1.988 2.242 0.752 392 2 (u) -71 335 335 401 416 187 0 3.772 -0.799 -20.869 21.231 0.598 393 21 (g) -71 319 319 401 416 182 187 11.160 2.296 -56.522 57.659 0.000 394 21 (g) -71 320 320 401 416 102 182 10.405 1.398 -52.103 53.150 0.000 395 21 (g) -71 334 334 401 416 184 102 0.006 0.272 -0.488 0.592 0.195 396 21 (g) -71 336 336 401 416 178 184 2.632 0.806 -20.174 20.365 0.416 397 21 (g) -71 325 325 401 416 189 178 -0.695 0.332 -3.003 3.100 0.000 398 21 (g) -71 333 333 401 416 186 189 -2.389 2.531 -7.044 7.859 0.162 399 21 (g) -71 321 321 401 416 188 186 -2.065 0.745 -7.420 7.738 0.000 400 -4 (cbar) -71 337 337 401 416 0 188 -31.372 0.320 -76.829 83.011 1.936 401 211 pi+ 83 392 400 0 0 0 0 2.680 0.181 -13.568 13.832 0.140 402 -211 pi- 83 392 400 0 0 0 0 0.825 -0.293 -6.657 6.716 0.140 403 113 (rho0) -83 392 400 542 543 0 0 8.562 1.036 -40.190 41.114 0.823 404 213 (rho+) -83 392 400 544 545 0 0 2.425 0.411 -12.542 12.802 0.726 405 -211 pi- 83 392 400 0 0 0 0 0.322 -0.239 -3.088 3.117 0.140 406 213 (rho+) -83 392 400 546 547 0 0 7.785 1.983 -42.535 43.294 0.778 407 111 (pi0) -83 392 400 634 635 0 0 1.774 0.147 -7.405 7.617 0.135 408 -213 (rho-) -83 392 400 548 549 0 0 2.211 0.328 -11.242 11.500 0.935 409 111 (pi0) -84 392 400 636 637 0 0 -0.093 0.023 -3.338 3.342 0.135 410 221 (eta) -84 392 400 638 639 0 0 0.256 0.133 -2.397 2.476 0.548 411 3122 (Lambda0) -84 392 400 640 641 0 0 0.516 0.868 -8.680 8.810 1.116 412 -3312 (Xibar+) -84 392 400 642 643 0 0 -2.260 1.708 -9.277 9.789 1.322 413 -313 (K*bar0) -84 392 400 550 551 0 0 -2.267 -0.058 -5.267 5.839 1.097 414 -211 pi- 84 392 400 0 0 0 0 -2.787 1.036 -8.164 8.689 0.140 415 2212 p+ 84 392 400 0 0 0 0 -3.912 0.490 -10.279 11.049 0.938 416 -4122 (Lambda_cbar-) -84 392 400 644 649 0 0 -24.587 0.148 -59.823 64.719 2.286 417 1 (d) -71 264 264 421 432 136 0 -1.222 -1.193 56.199 56.226 0.330 418 21 (g) -71 213 213 421 432 107 136 -0.467 0.230 -7.823 7.840 0.000 419 21 (g) -71 221 221 421 432 159 107 -1.399 1.097 -9.455 9.620 0.000 420 -1 (dbar) -71 341 341 421 432 0 159 -1.911 1.837 -29.237 29.362 0.548 421 113 (rho0) -83 417 420 552 553 0 0 -0.503 -0.287 19.030 19.054 0.746 422 -211 pi- 83 417 420 0 0 0 0 -0.188 0.254 7.063 7.072 0.140 423 211 pi+ 83 417 420 0 0 0 0 0.040 -0.566 16.371 16.382 0.140 424 223 (omega) -83 417 420 650 652 0 0 -0.181 -0.360 6.781 6.838 0.783 425 -211 pi- 83 417 420 0 0 0 0 -0.413 -0.060 4.071 4.095 0.140 426 2214 (Delta+) -84 417 420 554 555 0 0 0.256 -0.069 2.033 2.403 1.255 427 -211 pi- 84 417 420 0 0 0 0 0.066 0.065 0.501 0.529 0.140 428 -2114 (Deltabar0) -84 417 420 556 557 0 0 -1.185 0.458 -6.746 6.989 1.311 429 111 (pi0) -84 417 420 653 655 0 0 -1.394 0.869 -19.805 19.873 0.135 430 113 (rho0) -84 417 420 558 559 0 0 -0.928 1.063 -13.221 13.353 1.224 431 211 pi+ 84 417 420 0 0 0 0 -0.328 0.233 -4.107 4.129 0.140 432 111 (pi0) -84 417 420 656 657 0 0 -0.240 0.371 -2.287 2.333 0.135 433 -2203 (uu_1bar) -71 272 272 441 454 110 0 -1.104 1.173 -461.573 461.576 0.771 434 21 (g) -71 265 265 441 454 135 110 -1.026 0.082 -5.048 5.151 0.000 435 21 (g) -71 332 332 441 454 134 135 0.126 -0.232 -0.254 0.499 0.339 436 21 (g) -71 229 229 441 454 140 134 2.152 -1.444 1.150 2.835 0.000 437 21 (g) -71 234 234 441 454 133 140 0.548 -0.170 0.833 1.011 0.000 438 21 (g) -71 331 331 441 454 157 133 -0.062 0.244 0.680 0.734 0.113 439 21 (g) -71 233 233 441 454 111 157 0.726 -0.947 1.905 2.248 0.000 440 -2 (ubar) -71 261 261 441 454 0 111 -0.024 0.165 1.794 1.832 0.330 441 221 (eta) -83 433 440 658 660 0 0 -0.099 0.326 -111.317 111.319 0.548 442 -2224 (Deltabar--) -83 433 440 560 561 0 0 -0.331 0.638 -194.198 194.204 1.412 443 111 (pi0) -83 433 440 661 663 0 0 -0.391 -0.079 -38.203 38.205 0.135 444 331 (eta') -83 433 440 664 666 0 0 -0.725 -0.130 -95.729 95.737 0.958 445 111 (pi0) -83 433 440 667 668 0 0 -0.232 0.765 -3.811 3.896 0.135 446 211 pi+ 83 433 440 0 0 0 0 -0.227 -0.292 -15.662 15.667 0.140 447 -211 pi- 84 433 440 0 0 0 0 0.437 0.357 -5.664 5.694 0.140 448 213 (rho+) -84 433 440 562 563 0 0 -0.507 -1.090 -1.065 1.763 0.728 449 -211 pi- 84 433 440 0 0 0 0 0.406 0.202 -0.420 0.634 0.140 450 2224 (Delta++) -84 433 440 564 565 0 0 0.709 -0.147 0.142 1.423 1.217 451 -2214 (Deltabar-) -84 433 440 566 567 0 0 0.960 -0.903 2.029 2.757 1.322 452 -211 pi- 84 433 440 0 0 0 0 0.224 -0.106 -0.276 0.396 0.140 453 213 (rho+) -84 433 440 568 569 0 0 0.804 -0.685 2.554 2.842 0.661 454 -213 (rho-) -84 433 440 570 571 0 0 0.309 0.012 1.108 1.349 0.705 455 21 (g) -71 203 203 470 493 141 130 -0.015 -0.361 0.516 0.630 0.000 456 21 (g) -71 215 215 470 493 131 141 1.020 0.328 0.641 1.249 0.000 457 21 (g) -71 224 224 470 493 163 131 0.241 0.566 0.524 0.808 0.000 458 21 (g) -71 211 211 470 493 113 163 0.490 -0.137 0.033 0.510 0.000 459 21 (g) -71 206 206 470 493 144 113 0.130 0.240 -0.509 0.577 0.000 460 21 (g) -71 220 220 470 493 158 144 0.729 -0.701 -0.806 1.293 0.000 461 21 (g) -71 217 217 470 493 143 158 -0.020 -0.093 -1.056 1.061 0.000 462 21 (g) -71 216 216 470 493 106 143 0.339 -0.821 -0.697 1.129 0.000 463 21 (g) -71 204 204 470 493 101 106 -2.424 -0.575 -60.999 61.050 0.000 464 21 (g) -71 214 214 470 493 156 101 0.330 -0.286 13.475 13.482 0.000 465 21 (g) -71 219 219 470 493 145 156 1.226 0.817 36.319 36.349 0.000 466 21 (g) -71 342 342 470 493 162 145 0.432 -0.073 2.314 2.364 0.200 467 21 (g) -71 343 343 470 493 161 162 -0.842 -1.279 7.580 7.745 0.430 468 21 (g) -71 225 225 470 493 164 161 1.708 0.197 0.088 1.722 0.000 469 21 (g) -71 210 210 470 493 130 164 0.165 -0.009 -0.305 0.347 0.000 470 223 (omega) -83 455 469 669 671 0 0 -0.077 0.251 -0.144 0.847 0.792 471 -213 (rho-) -83 455 469 572 573 0 0 -0.504 0.184 -0.043 0.908 0.731 472 113 (rho0) -83 455 469 574 575 0 0 0.175 -0.348 2.874 3.028 0.871 473 213 (rho+) -83 455 469 576 577 0 0 0.594 0.412 16.047 16.078 0.686 474 221 (eta) -83 455 469 672 674 0 0 0.787 0.020 13.914 13.947 0.548 475 313 (K*0) -83 455 469 578 579 0 0 0.048 -0.224 12.840 12.874 0.898 476 -313 (K*bar0) -83 455 469 580 581 0 0 -0.011 -0.318 2.429 2.602 0.878 477 -213 (rho-) -83 455 469 582 583 0 0 0.328 0.179 5.643 5.705 0.752 478 2212 p+ 83 455 469 0 0 0 0 -0.335 -0.619 3.833 4.008 0.938 479 211 pi+ 84 455 469 0 0 0 0 0.826 -0.303 -0.020 0.891 0.140 480 -2224 (Deltabar--) -84 455 469 584 585 0 0 -0.068 0.414 1.455 1.955 1.237 481 221 (eta) -84 455 469 675 676 0 0 2.143 -0.280 -0.279 2.247 0.548 482 213 (rho+) -84 455 469 586 587 0 0 0.066 -0.309 0.288 0.895 0.786 483 -213 (rho-) -84 455 469 588 589 0 0 -0.007 0.230 -0.520 0.952 0.764 484 111 (pi0) -84 455 469 677 678 0 0 0.981 0.192 0.263 1.042 0.135 485 113 (rho0) -84 455 469 590 591 0 0 0.315 -0.612 -2.911 3.123 0.895 486 213 (rho+) -84 455 469 592 593 0 0 -0.627 -0.082 -5.005 5.122 0.883 487 -211 pi- 84 455 469 0 0 0 0 0.408 -0.287 -3.931 3.965 0.140 488 221 (eta) -84 455 469 679 680 0 0 -0.003 -0.020 -7.279 7.299 0.548 489 211 pi+ 84 455 469 0 0 0 0 -0.741 -0.454 -7.795 7.845 0.140 490 313 (K*0) -84 455 469 594 595 0 0 -0.001 0.148 -10.423 10.462 0.901 491 3122 (Lambda0) -84 455 469 681 682 0 0 -0.786 -0.128 -12.596 12.670 1.116 492 -2112 nbar0 84 455 469 0 0 0 0 -0.338 -0.242 -9.819 9.872 0.940 493 113 (rho0) -84 455 469 596 597 0 0 0.336 0.007 -1.703 1.977 0.946 494 2 (u) -71 241 241 502 514 137 0 0.297 1.083 113.217 113.223 0.330 495 21 (g) -71 207 207 502 514 104 115 0.559 -0.461 -3.444 3.520 0.000 496 1 (d) -71 209 209 502 514 115 0 0.272 0.138 -7.173 7.187 0.330 497 21 (g) -71 328 328 502 514 108 125 -0.057 -1.963 94.270 94.291 0.393 498 21 (g) -71 253 253 502 514 125 165 -0.308 -2.059 157.238 157.252 0.000 499 21 (g) -71 238 238 502 514 165 120 -0.394 -0.279 46.919 46.922 0.000 500 21 (g) -71 246 246 502 514 120 129 -0.591 0.369 64.628 64.631 0.000 501 3 (s) -71 327 327 502 514 129 0 -0.758 0.305 17.203 17.238 0.741 502 323 (K*+) -85 494 501 598 599 0 0 0.573 0.821 93.569 93.578 0.924 503 -311 (Kbar0) -86 494 501 600 600 0 0 -0.812 0.955 27.226 27.260 0.498 504 2112 n0 86 494 501 0 0 0 0 -0.751 -1.635 145.971 145.985 0.940 505 -2112 nbar0 86 494 501 0 0 0 0 -0.325 -0.678 45.893 45.909 0.940 506 -213 (rho-) -86 494 501 601 602 0 0 0.536 -0.174 67.453 67.459 0.700 507 -213 (rho-) -83 494 501 603 604 0 0 0.637 -0.153 -6.372 6.492 1.059 508 211 pi+ 83 494 501 0 0 0 0 0.024 0.337 -1.045 1.107 0.140 509 223 (omega) -83 494 501 683 685 0 0 -0.045 -0.352 -1.698 1.904 0.785 510 -213 (rho-) -83 494 501 605 606 0 0 0.171 -0.123 -0.538 0.902 0.693 511 323 (K*+) -83 494 501 607 608 0 0 -0.077 0.132 0.081 0.900 0.884 512 331 (eta') -84 494 501 686 687 0 0 0.214 -0.090 1.480 1.778 0.959 513 -313 (K*bar0) -84 494 501 609 610 0 0 -0.007 -0.037 3.057 3.181 0.878 514 3212 (Sigma0) -84 494 501 688 689 0 0 -1.116 -1.869 107.781 107.809 1.193 515 211 pi+ 91 346 0 0 0 0 0 0.264 -0.335 36.064 36.067 0.140 516 111 (pi0) -91 346 0 690 691 0 0 0.068 -0.288 6.338 6.346 0.135 517 310 (K_S0) -91 347 347 692 693 0 0 0.210 0.208 14.916 14.928 0.498 518 310 (K_S0) -91 352 352 694 695 0 0 2.072 -0.963 -17.066 17.225 0.498 519 -211 pi- 91 353 0 0 0 0 0 0.792 -0.051 -15.915 15.936 0.140 520 111 (pi0) -91 353 0 696 697 0 0 0.374 -0.357 -4.629 4.660 0.135 521 311 (K0) -91 362 0 611 611 0 0 -0.109 0.792 16.221 16.248 0.498 522 211 pi+ 91 362 0 0 0 0 0 0.258 0.192 3.616 3.633 0.140 523 211 pi+ 91 367 0 0 0 0 0 -0.242 -0.364 10.466 10.476 0.140 524 111 (pi0) -91 367 0 698 699 0 0 0.413 0.347 3.678 3.720 0.135 525 130 K_L0 91 368 368 0 0 0 0 0.367 -0.077 19.317 19.328 0.498 526 -321 K- 91 369 0 0 0 0 0 -0.070 -0.140 20.997 21.003 0.494 527 211 pi+ 91 369 0 0 0 0 0 -0.189 0.372 16.485 16.491 0.140 528 211 pi+ 91 370 0 0 0 0 0 -0.414 -0.319 85.236 85.238 0.140 529 -211 pi- 91 370 0 0 0 0 0 0.319 0.480 43.362 43.366 0.140 530 -311 (Kbar0) -91 378 0 612 612 0 0 -0.037 0.152 3.319 3.360 0.498 531 111 (pi0) -91 378 0 700 701 0 0 -0.138 -0.358 2.093 2.132 0.135 532 130 K_L0 91 380 380 0 0 0 0 -0.142 -0.056 3.312 3.353 0.498 533 310 (K_S0) -91 381 381 702 703 0 0 0.017 0.655 7.016 7.064 0.498 534 311 (K0) -91 386 0 613 613 0 0 -0.120 0.145 -0.131 0.548 0.498 535 111 (pi0) -91 386 0 704 705 0 0 0.174 0.395 -0.015 0.452 0.135 536 -321 K- 91 387 0 0 0 0 0 -0.654 0.735 -1.142 1.586 0.494 537 211 pi+ 91 387 0 0 0 0 0 0.063 -0.071 -0.238 0.292 0.140 538 310 (K_S0) -91 388 388 706 707 0 0 -0.142 -0.030 -0.437 0.678 0.498 539 130 K_L0 91 389 389 0 0 0 0 0.544 0.384 -0.385 0.916 0.498 540 211 pi+ 91 391 0 0 0 0 0 0.315 0.655 -1.805 1.951 0.140 541 111 (pi0) -91 391 0 708 709 0 0 -0.176 0.044 -0.183 0.291 0.135 542 211 pi+ 91 403 0 0 0 0 0 4.724 0.206 -21.338 21.857 0.140 543 -211 pi- 91 403 0 0 0 0 0 3.838 0.830 -18.852 19.257 0.140 544 211 pi+ 91 404 0 0 0 0 0 2.226 0.273 -10.285 10.528 0.140 545 111 (pi0) -91 404 0 710 711 0 0 0.200 0.139 -2.257 2.274 0.135 546 211 pi+ 91 406 0 0 0 0 0 0.448 0.214 -3.196 3.238 0.140 547 111 (pi0) -91 406 0 712 713 0 0 7.337 1.769 -39.339 40.057 0.135 548 -211 pi- 91 408 0 0 0 0 0 0.936 -0.136 -3.078 3.223 0.140 549 111 (pi0) -91 408 0 714 715 0 0 1.275 0.464 -8.164 8.277 0.135 550 -321 K- 91 413 0 0 0 0 0 -0.438 0.138 -1.400 1.554 0.494 551 211 pi+ 91 413 0 0 0 0 0 -1.829 -0.197 -3.867 4.285 0.140 552 211 pi+ 91 421 0 0 0 0 0 -0.050 0.180 7.978 7.982 0.140 553 -211 pi- 91 421 0 0 0 0 0 -0.453 -0.467 11.052 11.072 0.140 554 2112 n0 91 426 0 0 0 0 0 0.071 0.105 1.790 2.026 0.940 555 211 pi+ 91 426 0 0 0 0 0 0.185 -0.174 0.242 0.378 0.140 556 -2112 nbar0 91 428 0 0 0 0 0 -1.252 0.457 -5.596 5.829 0.940 557 111 (pi0) -91 428 0 716 717 0 0 0.067 0.001 -1.150 1.160 0.135 558 211 pi+ 91 430 0 0 0 0 0 -0.454 0.742 -3.357 3.470 0.140 559 -211 pi- 91 430 0 0 0 0 0 -0.475 0.320 -9.865 9.882 0.140 560 -2212 pbar- 91 442 0 0 0 0 0 -0.163 0.576 -100.104 100.110 0.938 561 -211 pi- 91 442 0 0 0 0 0 -0.168 0.062 -94.094 94.094 0.140 562 211 pi+ 91 448 0 0 0 0 0 0.132 -0.381 -0.214 0.478 0.140 563 111 (pi0) -91 448 0 718 719 0 0 -0.640 -0.709 -0.850 1.285 0.135 564 2212 p+ 91 450 0 0 0 0 0 0.328 -0.162 0.139 1.017 0.938 565 211 pi+ 91 450 0 0 0 0 0 0.381 0.015 0.002 0.406 0.140 566 -2112 nbar0 91 451 0 0 0 0 0 1.046 -0.727 1.522 2.196 0.940 567 -211 pi- 91 451 0 0 0 0 0 -0.087 -0.176 0.507 0.561 0.140 568 211 pi+ 91 453 0 0 0 0 0 0.619 -0.195 1.037 1.231 0.140 569 111 (pi0) -91 453 0 720 721 0 0 0.185 -0.490 1.517 1.611 0.135 570 -211 pi- 91 454 0 0 0 0 0 0.406 0.111 1.062 1.150 0.140 571 111 (pi0) -91 454 0 722 723 0 0 -0.097 -0.099 0.046 0.199 0.135 572 -211 pi- 91 471 0 0 0 0 0 -0.132 0.381 -0.151 0.453 0.140 573 111 (pi0) -91 471 0 724 725 0 0 -0.372 -0.197 0.108 0.455 0.135 574 211 pi+ 91 472 0 0 0 0 0 0.303 -0.265 0.552 0.697 0.140 575 -211 pi- 91 472 0 0 0 0 0 -0.128 -0.084 2.322 2.331 0.140 576 211 pi+ 91 473 0 0 0 0 0 0.500 0.504 9.220 9.248 0.140 577 111 (pi0) -91 473 0 726 727 0 0 0.094 -0.092 6.827 6.830 0.135 578 311 (K0) -91 475 0 614 614 0 0 0.095 -0.382 6.760 6.789 0.498 579 111 (pi0) -91 475 0 728 729 0 0 -0.047 0.157 6.081 6.084 0.135 580 -311 (Kbar0) -91 476 0 615 615 0 0 0.051 -0.358 1.067 1.232 0.498 581 111 (pi0) -91 476 0 730 731 0 0 -0.061 0.040 1.362 1.370 0.135 582 -211 pi- 91 477 0 0 0 0 0 0.096 -0.256 1.531 1.562 0.140 583 111 (pi0) -91 477 0 732 733 0 0 0.232 0.435 4.111 4.143 0.135 584 -2212 pbar- 91 480 0 0 0 0 0 -0.169 0.136 0.944 1.348 0.938 585 -211 pi- 91 480 0 0 0 0 0 0.101 0.278 0.511 0.607 0.140 586 211 pi+ 91 482 0 0 0 0 0 0.063 0.069 -0.201 0.262 0.140 587 111 (pi0) -91 482 0 734 735 0 0 0.003 -0.378 0.489 0.633 0.135 588 -211 pi- 91 483 0 0 0 0 0 0.268 0.050 0.019 0.307 0.140 589 111 (pi0) -91 483 0 736 737 0 0 -0.275 0.180 -0.539 0.646 0.135 590 211 pi+ 91 485 0 0 0 0 0 0.418 0.044 -0.978 1.074 0.140 591 -211 pi- 91 485 0 0 0 0 0 -0.103 -0.656 -1.933 2.049 0.140 592 211 pi+ 91 486 0 0 0 0 0 -0.808 0.003 -3.360 3.459 0.140 593 111 (pi0) -91 486 0 738 739 0 0 0.182 -0.085 -1.645 1.663 0.135 594 311 (K0) -91 490 0 616 616 0 0 -0.095 -0.060 -9.065 9.080 0.498 595 111 (pi0) -91 490 0 740 741 0 0 0.094 0.207 -1.357 1.383 0.135 596 211 pi+ 91 493 0 0 0 0 0 0.294 -0.380 -0.512 0.716 0.140 597 -211 pi- 91 493 0 0 0 0 0 0.041 0.388 -1.191 1.261 0.140 598 311 (K0) -91 502 0 617 617 0 0 0.225 0.699 47.914 47.922 0.498 599 211 pi+ 91 502 0 0 0 0 0 0.348 0.122 45.654 45.656 0.140 600 130 K_L0 91 503 503 0 0 0 0 -0.812 0.955 27.226 27.260 0.498 601 -211 pi- 91 506 0 0 0 0 0 0.355 -0.320 58.097 58.099 0.140 602 111 (pi0) -91 506 0 742 743 0 0 0.181 0.146 9.356 9.359 0.135 603 -211 pi- 91 507 0 0 0 0 0 0.336 -0.590 -3.246 3.319 0.140 604 111 (pi0) -91 507 0 744 745 0 0 0.302 0.436 -3.126 3.173 0.135 605 -211 pi- 91 510 0 0 0 0 0 -0.093 0.022 -0.546 0.572 0.140 606 111 (pi0) -91 510 0 746 747 0 0 0.264 -0.145 0.009 0.330 0.135 607 311 (K0) -91 511 0 618 618 0 0 0.004 0.074 -0.224 0.551 0.498 608 211 pi+ 91 511 0 0 0 0 0 -0.082 0.058 0.305 0.350 0.140 609 -311 (Kbar0) -91 513 0 619 619 0 0 0.232 0.041 1.504 1.602 0.498 610 111 (pi0) -91 513 0 748 749 0 0 -0.239 -0.078 1.553 1.579 0.135 611 130 K_L0 91 521 521 0 0 0 0 -0.109 0.792 16.221 16.248 0.498 612 310 (K_S0) -91 530 530 750 751 0 0 -0.037 0.152 3.319 3.360 0.498 613 130 K_L0 91 534 534 0 0 0 0 -0.120 0.145 -0.131 0.548 0.498 614 310 (K_S0) -91 578 578 752 753 0 0 0.095 -0.382 6.760 6.789 0.498 615 310 (K_S0) -91 580 580 754 755 0 0 0.051 -0.358 1.067 1.232 0.498 616 310 (K_S0) -91 594 594 756 757 0 0 -0.095 -0.060 -9.065 9.080 0.498 617 310 (K_S0) -91 598 598 758 759 0 0 0.225 0.699 47.914 47.922 0.498 618 130 K_L0 91 607 607 0 0 0 0 0.004 0.074 -0.224 0.551 0.498 619 130 K_L0 91 609 609 0 0 0 0 0.232 0.041 1.504 1.602 0.498 620 431 (D_s+) -91 351 0 760 761 0 0 5.459 -7.768 -87.230 87.768 1.968 621 22 gamma 91 351 0 0 0 0 0 0.038 -0.046 -0.202 0.211 0.000 622 111 (pi0) -91 361 0 762 763 0 0 -0.060 0.133 1.080 1.098 0.135 623 111 (pi0) -91 361 0 764 765 0 0 -0.020 0.042 2.203 2.208 0.135 624 221 (eta) -91 361 0 766 767 0 0 -0.063 -0.170 4.021 4.062 0.548 625 321 K+ 91 363 0 0 0 0 0 0.261 -0.012 8.258 8.277 0.494 626 -321 K- 91 363 0 0 0 0 0 0.273 -0.201 8.441 8.462 0.494 627 22 gamma 91 379 0 0 0 0 0 0.031 -0.152 0.581 0.601 0.000 628 22 gamma 91 379 0 0 0 0 0 0.005 0.030 0.126 0.130 0.000 629 22 gamma 91 382 0 0 0 0 0 0.070 0.004 0.132 0.150 0.000 630 22 gamma 91 382 0 0 0 0 0 0.163 -0.225 0.592 0.654 0.000 631 211 pi+ 91 385 0 0 0 0 0 0.203 0.211 0.277 0.427 0.140 632 -211 pi- 91 385 0 0 0 0 0 0.006 0.090 -0.083 0.186 0.140 633 111 (pi0) -91 385 0 768 769 0 0 0.337 0.184 -0.214 0.460 0.135 634 22 gamma 91 407 0 0 0 0 0 1.724 0.154 -7.095 7.303 0.000 635 22 gamma 91 407 0 0 0 0 0 0.050 -0.007 -0.311 0.315 0.000 636 22 gamma 91 409 0 0 0 0 0 -0.115 0.051 -2.255 2.258 0.000 637 22 gamma 91 409 0 0 0 0 0 0.022 -0.028 -1.083 1.084 0.000 638 22 gamma 91 410 0 0 0 0 0 0.254 -0.132 -0.669 0.728 0.000 639 22 gamma 91 410 0 0 0 0 0 0.002 0.265 -1.728 1.748 0.000 640 2212 p+ 91 411 0 0 0 0 0 0.524 0.801 -8.041 8.152 0.938 641 -211 pi- 91 411 0 0 0 0 0 -0.008 0.067 -0.639 0.658 0.140 642 -3122 (Lambdabar0) -91 412 0 770 771 0 0 -1.774 1.253 -7.451 7.841 1.116 643 211 pi+ 91 412 0 0 0 0 0 -0.486 0.456 -1.826 1.948 0.140 644 111 (pi0) -91 416 0 772 773 0 0 -1.648 0.118 -4.033 4.361 0.135 645 111 (pi0) -91 416 0 774 775 0 0 -5.547 -0.243 -13.054 14.186 0.135 646 111 (pi0) -91 416 0 776 777 0 0 -0.760 0.021 -2.015 2.158 0.135 647 111 (pi0) -91 416 0 778 779 0 0 -0.899 0.042 -2.215 2.395 0.135 648 -3222 (Sigmabar-) -91 416 0 780 781 0 0 -13.964 0.223 -34.493 37.232 1.189 649 111 (pi0) -91 416 0 782 783 0 0 -1.769 -0.014 -4.013 4.387 0.135 650 211 pi+ 91 424 0 0 0 0 0 -0.158 0.143 1.924 1.941 0.140 651 -211 pi- 91 424 0 0 0 0 0 0.092 -0.320 3.272 3.292 0.140 652 111 (pi0) -91 424 0 784 785 0 0 -0.115 -0.182 1.584 1.605 0.135 653 22 gamma 91 429 0 0 0 0 0 -0.777 0.444 -10.075 10.115 0.000 654 11 e- 91 429 0 0 0 0 0 -0.192 0.133 -3.025 3.034 0.001 655 -11 e+ 91 429 0 0 0 0 0 -0.425 0.292 -6.704 6.724 0.001 656 22 gamma 91 432 0 0 0 0 0 0.014 0.011 -0.048 0.051 0.000 657 22 gamma 91 432 0 0 0 0 0 -0.254 0.360 -2.239 2.282 0.000 658 111 (pi0) -91 441 0 786 787 0 0 -0.032 0.197 -53.003 53.003 0.135 659 111 (pi0) -91 441 0 788 789 0 0 -0.151 0.031 -30.075 30.075 0.135 660 111 (pi0) -91 441 0 790 791 0 0 0.085 0.098 -28.240 28.241 0.135 661 22 gamma 91 443 0 0 0 0 0 -0.255 -0.087 -20.164 20.165 0.000 662 11 e- 91 443 0 0 0 0 0 -0.010 -0.003 -1.228 1.228 0.001 663 -11 e+ 91 443 0 0 0 0 0 -0.126 0.011 -16.811 16.812 0.001 664 211 pi+ 91 444 0 0 0 0 0 -0.120 0.017 -17.013 17.014 0.140 665 -211 pi- 91 444 0 0 0 0 0 -0.274 -0.177 -36.956 36.958 0.140 666 221 (eta) -91 444 0 792 793 0 0 -0.331 0.031 -41.760 41.765 0.548 667 22 gamma 91 445 0 0 0 0 0 -0.071 0.231 -0.874 0.907 0.000 668 22 gamma 91 445 0 0 0 0 0 -0.161 0.534 -2.937 2.989 0.000 669 211 pi+ 91 470 0 0 0 0 0 -0.138 0.213 -0.014 0.290 0.140 670 -211 pi- 91 470 0 0 0 0 0 0.160 0.212 -0.053 0.304 0.140 671 111 (pi0) -91 470 0 794 795 0 0 -0.098 -0.174 -0.076 0.252 0.135 672 111 (pi0) -91 474 0 796 797 0 0 0.263 0.141 5.665 5.674 0.135 673 111 (pi0) -91 474 0 798 799 0 0 0.277 -0.034 5.236 5.245 0.135 674 111 (pi0) -91 474 0 800 801 0 0 0.248 -0.087 3.014 3.028 0.135 675 22 gamma 91 481 0 0 0 0 0 1.997 -0.128 -0.335 2.029 0.000 676 22 gamma 91 481 0 0 0 0 0 0.146 -0.152 0.056 0.218 0.000 677 22 gamma 91 484 0 0 0 0 0 0.460 0.072 0.190 0.503 0.000 678 22 gamma 91 484 0 0 0 0 0 0.521 0.120 0.073 0.539 0.000 679 22 gamma 91 488 0 0 0 0 0 -0.126 -0.028 -0.418 0.438 0.000 680 22 gamma 91 488 0 0 0 0 0 0.123 0.008 -6.861 6.862 0.000 681 2212 p+ 91 491 0 0 0 0 0 -0.567 -0.162 -10.028 10.089 0.938 682 -211 pi- 91 491 0 0 0 0 0 -0.219 0.034 -2.567 2.581 0.140 683 211 pi+ 91 509 0 0 0 0 0 0.117 -0.092 -0.210 0.293 0.140 684 -211 pi- 91 509 0 0 0 0 0 -0.257 -0.164 -0.480 0.585 0.140 685 111 (pi0) -91 509 0 802 803 0 0 0.094 -0.097 -1.008 1.026 0.135 686 113 (rho0) -91 512 0 804 805 0 0 0.083 -0.125 1.235 1.499 0.836 687 22 gamma 91 512 0 0 0 0 0 0.130 0.035 0.245 0.279 0.000 688 3122 (Lambda0) -91 514 0 806 807 0 0 -1.030 -1.829 105.126 105.153 1.116 689 22 gamma 91 514 0 0 0 0 0 -0.086 -0.040 2.655 2.656 0.000 690 22 gamma 91 516 0 0 0 0 0 -0.024 -0.145 2.251 2.256 0.000 691 22 gamma 91 516 0 0 0 0 0 0.092 -0.143 4.086 4.090 0.000 692 211 pi+ 91 517 0 0 0 0 0 0.085 -0.019 10.572 10.574 0.140 693 -211 pi- 91 517 0 0 0 0 0 0.125 0.227 4.344 4.354 0.140 694 111 (pi0) -91 518 0 808 809 0 0 0.364 -0.056 -2.391 2.423 0.135 695 111 (pi0) -91 518 0 810 811 0 0 1.708 -0.907 -14.675 14.803 0.135 696 22 gamma 91 520 0 0 0 0 0 0.259 -0.315 -3.792 3.814 0.000 697 22 gamma 91 520 0 0 0 0 0 0.115 -0.042 -0.837 0.846 0.000 698 22 gamma 91 524 0 0 0 0 0 0.062 0.019 0.731 0.734 0.000 699 22 gamma 91 524 0 0 0 0 0 0.351 0.328 2.947 2.986 0.000 700 22 gamma 91 531 0 0 0 0 0 0.015 -0.138 0.694 0.707 0.000 701 22 gamma 91 531 0 0 0 0 0 -0.153 -0.221 1.399 1.424 0.000 702 111 (pi0) -91 533 0 812 813 0 0 -0.156 0.116 2.338 2.350 0.135 703 111 (pi0) -91 533 0 814 815 0 0 0.174 0.539 4.678 4.714 0.135 704 22 gamma 91 535 0 0 0 0 0 0.057 0.090 0.053 0.119 0.000 705 22 gamma 91 535 0 0 0 0 0 0.117 0.305 -0.068 0.333 0.000 706 211 pi+ 91 538 0 0 0 0 0 -0.024 -0.114 -0.441 0.477 0.140 707 -211 pi- 91 538 0 0 0 0 0 -0.118 0.084 0.004 0.201 0.140 708 22 gamma 91 541 0 0 0 0 0 -0.190 0.047 -0.192 0.274 0.000 709 22 gamma 91 541 0 0 0 0 0 0.014 -0.003 0.008 0.017 0.000 710 22 gamma 91 545 0 0 0 0 0 0.219 0.135 -2.050 2.066 0.000 711 22 gamma 91 545 0 0 0 0 0 -0.020 0.004 -0.207 0.208 0.000 712 22 gamma 91 547 0 0 0 0 0 2.659 0.699 -14.160 14.424 0.000 713 22 gamma 91 547 0 0 0 0 0 4.677 1.070 -25.179 25.632 0.000 714 22 gamma 91 549 0 0 0 0 0 0.530 0.123 -3.215 3.261 0.000 715 22 gamma 91 549 0 0 0 0 0 0.745 0.341 -4.949 5.016 0.000 716 22 gamma 91 557 0 0 0 0 0 0.046 -0.065 -0.681 0.686 0.000 717 22 gamma 91 557 0 0 0 0 0 0.021 0.066 -0.468 0.474 0.000 718 22 gamma 91 563 0 0 0 0 0 -0.153 -0.263 -0.266 0.404 0.000 719 22 gamma 91 563 0 0 0 0 0 -0.487 -0.446 -0.584 0.881 0.000 720 22 gamma 91 569 0 0 0 0 0 0.189 -0.481 1.385 1.478 0.000 721 22 gamma 91 569 0 0 0 0 0 -0.004 -0.010 0.133 0.133 0.000 722 22 gamma 91 571 0 0 0 0 0 -0.095 -0.023 -0.018 0.099 0.000 723 22 gamma 91 571 0 0 0 0 0 -0.002 -0.076 0.064 0.099 0.000 724 22 gamma 91 573 0 0 0 0 0 -0.143 -0.118 -0.010 0.186 0.000 725 22 gamma 91 573 0 0 0 0 0 -0.229 -0.079 0.118 0.269 0.000 726 22 gamma 91 577 0 0 0 0 0 0.080 -0.058 1.976 1.978 0.000 727 22 gamma 91 577 0 0 0 0 0 0.014 -0.034 4.851 4.852 0.000 728 22 gamma 91 579 0 0 0 0 0 -0.049 -0.005 1.237 1.238 0.000 729 22 gamma 91 579 0 0 0 0 0 0.002 0.162 4.843 4.846 0.000 730 22 gamma 91 581 0 0 0 0 0 -0.092 -0.002 0.625 0.632 0.000 731 22 gamma 91 581 0 0 0 0 0 0.031 0.042 0.737 0.739 0.000 732 22 gamma 91 583 0 0 0 0 0 0.129 0.223 1.602 1.622 0.000 733 22 gamma 91 583 0 0 0 0 0 0.103 0.212 2.509 2.520 0.000 734 22 gamma 91 587 0 0 0 0 0 -0.001 -0.086 0.035 0.093 0.000 735 22 gamma 91 587 0 0 0 0 0 0.004 -0.293 0.454 0.540 0.000 736 22 gamma 91 589 0 0 0 0 0 -0.005 -0.001 0.008 0.009 0.000 737 22 gamma 91 589 0 0 0 0 0 -0.270 0.181 -0.547 0.636 0.000 738 22 gamma 91 593 0 0 0 0 0 0.121 -0.056 -1.458 1.464 0.000 739 22 gamma 91 593 0 0 0 0 0 0.060 -0.029 -0.188 0.199 0.000 740 22 gamma 91 595 0 0 0 0 0 -0.013 0.064 -0.168 0.181 0.000 741 22 gamma 91 595 0 0 0 0 0 0.107 0.144 -1.189 1.202 0.000 742 22 gamma 91 602 0 0 0 0 0 0.129 0.142 8.574 8.576 0.000 743 22 gamma 91 602 0 0 0 0 0 0.051 0.003 0.782 0.784 0.000 744 22 gamma 91 604 0 0 0 0 0 0.033 0.077 -0.825 0.830 0.000 745 22 gamma 91 604 0 0 0 0 0 0.269 0.359 -2.300 2.344 0.000 746 22 gamma 91 606 0 0 0 0 0 0.138 -0.028 -0.048 0.149 0.000 747 22 gamma 91 606 0 0 0 0 0 0.126 -0.117 0.057 0.181 0.000 748 22 gamma 91 610 0 0 0 0 0 -0.227 -0.025 1.172 1.194 0.000 749 22 gamma 91 610 0 0 0 0 0 -0.012 -0.054 0.381 0.385 0.000 750 211 pi+ 91 612 0 0 0 0 0 0.160 -0.025 1.683 1.696 0.140 751 -211 pi- 91 612 0 0 0 0 0 -0.197 0.177 1.637 1.664 0.140 752 211 pi+ 91 614 0 0 0 0 0 0.239 -0.147 4.075 4.087 0.140 753 -211 pi- 91 614 0 0 0 0 0 -0.144 -0.235 2.684 2.702 0.140 754 211 pi+ 91 615 0 0 0 0 0 -0.134 -0.035 0.216 0.292 0.140 755 -211 pi- 91 615 0 0 0 0 0 0.185 -0.323 0.851 0.940 0.140 756 211 pi+ 91 616 0 0 0 0 0 -0.256 -0.036 -4.905 4.914 0.140 757 -211 pi- 91 616 0 0 0 0 0 0.161 -0.024 -4.160 4.166 0.140 758 211 pi+ 91 617 0 0 0 0 0 0.318 0.393 24.586 24.591 0.140 759 -211 pi- 91 617 0 0 0 0 0 -0.094 0.307 23.328 23.331 0.140 760 221 (eta) -91 620 0 816 818 0 0 4.473 -6.508 -71.653 72.089 0.548 761 213 (rho+) -91 620 0 819 820 0 0 0.986 -1.260 -15.577 15.678 0.779 762 22 gamma 91 622 0 0 0 0 0 0.016 0.105 0.790 0.797 0.000 763 22 gamma 91 622 0 0 0 0 0 -0.076 0.028 0.290 0.301 0.000 764 22 gamma 91 623 0 0 0 0 0 -0.023 0.064 0.514 0.519 0.000 765 22 gamma 91 623 0 0 0 0 0 0.002 -0.022 1.689 1.689 0.000 766 22 gamma 91 624 0 0 0 0 0 0.236 -0.130 2.208 2.224 0.000 767 22 gamma 91 624 0 0 0 0 0 -0.299 -0.040 1.813 1.838 0.000 768 22 gamma 91 633 0 0 0 0 0 0.279 0.127 -0.105 0.324 0.000 769 22 gamma 91 633 0 0 0 0 0 0.058 0.058 -0.109 0.136 0.000 770 -2212 pbar- 91 642 0 0 0 0 0 -1.432 0.999 -5.763 6.095 0.938 771 211 pi+ 91 642 0 0 0 0 0 -0.342 0.254 -1.688 1.746 0.140 772 22 gamma 91 644 0 0 0 0 0 -0.552 0.099 -1.428 1.534 0.000 773 22 gamma 91 644 0 0 0 0 0 -1.097 0.019 -2.606 2.827 0.000 774 22 gamma 91 645 0 0 0 0 0 -4.326 -0.135 -10.138 11.024 0.000 775 22 gamma 91 645 0 0 0 0 0 -1.221 -0.108 -2.916 3.163 0.000 776 22 gamma 91 646 0 0 0 0 0 -0.363 -0.028 -1.117 1.175 0.000 777 22 gamma 91 646 0 0 0 0 0 -0.397 0.049 -0.898 0.983 0.000 778 22 gamma 91 647 0 0 0 0 0 -0.476 -0.027 -1.043 1.147 0.000 779 22 gamma 91 647 0 0 0 0 0 -0.423 0.069 -1.172 1.248 0.000 780 -2212 pbar- 91 648 0 0 0 0 0 -12.710 0.343 -31.439 33.926 0.938 781 111 (pi0) -91 648 0 821 822 0 0 -1.254 -0.120 -3.054 3.306 0.135 782 22 gamma 91 649 0 0 0 0 0 -0.822 -0.051 -1.991 2.155 0.000 783 22 gamma 91 649 0 0 0 0 0 -0.946 0.037 -2.021 2.232 0.000 784 22 gamma 91 652 0 0 0 0 0 0.017 -0.088 0.673 0.679 0.000 785 22 gamma 91 652 0 0 0 0 0 -0.132 -0.094 0.911 0.925 0.000 786 22 gamma 91 658 0 0 0 0 0 0.049 0.074 -25.091 25.091 0.000 787 22 gamma 91 658 0 0 0 0 0 -0.082 0.123 -27.912 27.913 0.000 788 22 gamma 91 659 0 0 0 0 0 -0.062 0.076 -18.566 18.566 0.000 789 22 gamma 91 659 0 0 0 0 0 -0.090 -0.046 -11.509 11.509 0.000 790 22 gamma 91 660 0 0 0 0 0 -0.016 -0.017 -8.234 8.234 0.000 791 22 gamma 91 660 0 0 0 0 0 0.101 0.115 -20.007 20.007 0.000 792 22 gamma 91 666 0 0 0 0 0 -0.139 -0.174 -32.286 32.287 0.000 793 22 gamma 91 666 0 0 0 0 0 -0.192 0.204 -9.474 9.478 0.000 794 22 gamma 91 671 0 0 0 0 0 -0.073 -0.034 -0.076 0.111 0.000 795 22 gamma 91 671 0 0 0 0 0 -0.025 -0.139 0.000 0.142 0.000 796 22 gamma 91 672 0 0 0 0 0 0.228 0.148 4.060 4.069 0.000 797 22 gamma 91 672 0 0 0 0 0 0.035 -0.007 1.605 1.605 0.000 798 22 gamma 91 673 0 0 0 0 0 0.152 0.005 1.718 1.725 0.000 799 22 gamma 91 673 0 0 0 0 0 0.125 -0.039 3.518 3.520 0.000 800 22 gamma 91 674 0 0 0 0 0 0.207 -0.040 2.705 2.713 0.000 801 22 gamma 91 674 0 0 0 0 0 0.041 -0.047 0.309 0.315 0.000 802 22 gamma 91 685 0 0 0 0 0 0.107 -0.021 -0.473 0.486 0.000 803 22 gamma 91 685 0 0 0 0 0 -0.013 -0.076 -0.535 0.540 0.000 804 211 pi+ 91 686 0 0 0 0 0 0.119 0.212 0.086 0.293 0.140 805 -211 pi- 91 686 0 0 0 0 0 -0.036 -0.337 1.149 1.206 0.140 806 2212 p+ 91 688 0 0 0 0 0 -0.749 -1.497 83.462 83.484 0.938 807 -211 pi- 91 688 0 0 0 0 0 -0.281 -0.332 21.664 21.669 0.140 808 22 gamma 91 694 0 0 0 0 0 0.236 -0.007 -1.122 1.146 0.000 809 22 gamma 91 694 0 0 0 0 0 0.128 -0.049 -1.269 1.276 0.000 810 22 gamma 91 695 0 0 0 0 0 0.236 -0.179 -2.303 2.322 0.000 811 22 gamma 91 695 0 0 0 0 0 1.472 -0.728 -12.372 12.481 0.000 812 22 gamma 91 702 0 0 0 0 0 -0.092 0.139 1.787 1.795 0.000 813 22 gamma 91 702 0 0 0 0 0 -0.064 -0.023 0.551 0.555 0.000 814 22 gamma 91 703 0 0 0 0 0 -0.023 0.062 0.475 0.480 0.000 815 22 gamma 91 703 0 0 0 0 0 0.196 0.477 4.203 4.234 0.000 816 111 (pi0) -91 760 0 823 824 0 0 2.827 -3.917 -43.260 43.529 0.135 817 111 (pi0) -91 760 0 825 826 0 0 0.902 -1.374 -15.508 15.596 0.135 818 111 (pi0) -91 760 0 827 828 0 0 0.745 -1.218 -12.885 12.964 0.135 819 211 pi+ 91 761 0 0 0 0 0 1.055 -1.050 -14.069 14.149 0.140 820 111 (pi0) -91 761 0 829 830 0 0 -0.069 -0.210 -1.508 1.530 0.135 821 22 gamma 91 781 0 0 0 0 0 -0.890 -0.024 -2.179 2.354 0.000 822 22 gamma 91 781 0 0 0 0 0 -0.363 -0.095 -0.875 0.953 0.000 823 22 gamma 91 816 0 0 0 0 0 2.212 -3.136 -34.673 34.884 0.000 824 22 gamma 91 816 0 0 0 0 0 0.615 -0.782 -8.588 8.645 0.000 825 22 gamma 91 817 0 0 0 0 0 0.639 -1.040 -11.932 11.994 0.000 826 22 gamma 91 817 0 0 0 0 0 0.263 -0.334 -3.577 3.602 0.000 827 22 gamma 91 818 0 0 0 0 0 0.707 -1.080 -11.577 11.649 0.000 828 22 gamma 91 818 0 0 0 0 0 0.037 -0.138 -1.307 1.315 0.000 829 22 gamma 91 820 0 0 0 0 0 0.030 -0.083 -0.350 0.361 0.000 830 22 gamma 91 820 0 0 0 0 0 -0.099 -0.127 -1.158 1.169 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 0.000 1960.000 1960.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Error in StringFragmentation::fragmentToJunction: caught in junction flavour loop PYTHIA Error in Pythia::next: hadronLevel failed; try again PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | f fbar -> gamma*/Z0 221 | 4539 1000 1000 | 4.856e-06 9.444e-08 | | | | | | sum | 4539 1000 1000 | 4.856e-06 9.444e-08 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Error in Pythia::next: hadronLevel failed; try again | | 1 Error in StringFragmentation::fragmentToJunction: caught in junction flavour loop | | 4 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:00 dN/dpTZ 8.40*10^ 1 7 8.10*10^ 1 X3X 7.80*10^ 1 XXX7 7.50*10^ 1 XXXX 7.20*10^ 1 XXXX 6.90*10^ 1 XXXX 6.60*10^ 1 XXXX 6.30*10^ 1 XXXX 6.00*10^ 1 XXXX 5.70*10^ 1 XXXX 5.40*10^ 1 XXXXX7 5.10*10^ 1 XXXXXX 3 4.80*10^ 1 XXXXXX X 4.50*10^ 1 XXXXXX3 X 4.20*10^ 1 XXXXXXX3X 3.90*10^ 1 XXXXXXXXX3 3.60*10^ 1 XXXXXXXXXX 3.30*10^ 1 XXXXXXXXXX33 3.00*10^ 1 XXXXXXXXXXXX 3 2.70*10^ 1 XXXXXXXXXXXX3 X 2.40*10^ 1 XXXXXXXXXXXXX3 X 2.10*10^ 1 XXXXXXXXXXXXXX7 X 7 1.80*10^ 1 3XXXXXXXXXXXXXXX3X X 1.50*10^ 1 XXXXXXXXXXXXXXXXXXX3 3XX 3 1.20*10^ 1 XXXXXXXXXXXXXXXXXXXX3XXX 3 X 0.90*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXX 7XXXX 0.60*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXX3XXXXX73 77 3 0.30*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7XXXXXX33 333X373 3 3 3 3 73337 3 3 37 3 333 3 Contents *10^ 1 1878755444333222121111120010100000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 6193743309711520685303504809395435523333341100111312101000101010211120000010100001200000000100111010 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 0 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 1000 Mean = 1.2549e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+03 Rms = 1.3548e+01 Overflow = 0.0000e+00 High edge = 1.0000e+02 pythia8-8.1.80.orig/examples/outref/out040000644000175000017500000052545112217346170016370 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:01:04 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | non-diffractive 101 | 5.584e+01 | | A B -> A B elastic 102 | 3.210e+01 | | A B -> X B single diffractive 103 | 5.628e+00 | | A B -> A X single diffractive 104 | 5.628e+00 | | A B -> X X double diffractive 105 | 9.472e+00 | | A B -> A X B central diffractive 106 | 8.179e-01 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 55.84 mb | | | | pT0 = 2.74 gives sigmaInteraction = 351.67 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction XB | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.86 gives sigmaInteraction = 7.43 mb: rejected | | pT0 = 0.77 gives sigmaInteraction = 11.74 mb: accepted | | diffractive mass = 6.117e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.15 gives sigmaInteraction = 11.49 mb: accepted | | diffractive mass = 3.742e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.53 gives sigmaInteraction = 15.70 mb: accepted | | diffractive mass = 2.289e+03 GeV and sigmaNorm = 10.000 mb | | pT0 = 2.05 gives sigmaInteraction = 29.09 mb: accepted | | diffractive mass = 1.400e+04 GeV and sigmaNorm = 10.000 mb | | pT0 = 2.74 gives sigmaInteraction = 59.82 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* PYTHIA Warning in MultipartonInteractions::init: maximum increased by factor 5.153 *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction AX | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.86 gives sigmaInteraction = 7.41 mb: rejected | | pT0 = 0.77 gives sigmaInteraction = 11.88 mb: accepted | | diffractive mass = 6.117e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.15 gives sigmaInteraction = 11.40 mb: accepted | | diffractive mass = 3.742e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.53 gives sigmaInteraction = 15.59 mb: accepted | | diffractive mass = 2.289e+03 GeV and sigmaNorm = 10.000 mb | | pT0 = 2.05 gives sigmaInteraction = 28.72 mb: accepted | | diffractive mass = 1.400e+04 GeV and sigmaNorm = 10.000 mb | | pT0 = 2.74 gives sigmaInteraction = 59.51 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | diffraction AXB | | | | diffractive mass = 1.000e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 0.86 gives sigmaInteraction = 1.60 mb: rejected | | pT0 = 0.77 gives sigmaInteraction = 2.43 mb: rejected | | pT0 = 0.70 gives sigmaInteraction = 3.67 mb: rejected | | pT0 = 0.63 gives sigmaInteraction = 5.61 mb: rejected | | pT0 = 0.56 gives sigmaInteraction = 8.69 mb: rejected | | pT0 = 0.51 gives sigmaInteraction = 13.62 mb: accepted | | diffractive mass = 6.117e+01 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.15 gives sigmaInteraction = 1.42 mb: rejected | | pT0 = 1.03 gives sigmaInteraction = 1.90 mb: rejected | | pT0 = 0.93 gives sigmaInteraction = 2.56 mb: rejected | | pT0 = 0.84 gives sigmaInteraction = 3.50 mb: rejected | | pT0 = 0.75 gives sigmaInteraction = 4.80 mb: rejected | | pT0 = 0.68 gives sigmaInteraction = 6.77 mb: rejected | | pT0 = 0.61 gives sigmaInteraction = 9.69 mb: rejected | | pT0 = 0.55 gives sigmaInteraction = 14.11 mb: accepted | | diffractive mass = 3.742e+02 GeV and sigmaNorm = 10.000 mb | | pT0 = 1.53 gives sigmaInteraction = 2.32 mb: rejected | | pT0 = 1.38 gives sigmaInteraction = 2.80 mb: rejected | | pT0 = 1.24 gives sigmaInteraction = 3.40 mb: rejected | | pT0 = 1.12 gives sigmaInteraction = 4.09 mb: rejected | | pT0 = 1.01 gives sigmaInteraction = 4.90 mb: rejected | | pT0 = 0.91 gives sigmaInteraction = 5.98 mb: rejected | | pT0 = 0.82 gives sigmaInteraction = 7.32 mb: rejected | | pT0 = 0.73 gives sigmaInteraction = 9.10 mb: rejected | | pT0 = 0.66 gives sigmaInteraction = 11.64 mb: accepted | | diffractive mass = 2.289e+03 GeV and sigmaNorm = 10.000 mb | | pT0 = 2.05 gives sigmaInteraction = 4.65 mb: rejected | | pT0 = 1.85 gives sigmaInteraction = 5.48 mb: rejected | | pT0 = 1.66 gives sigmaInteraction = 6.45 mb: rejected | | pT0 = 1.49 gives sigmaInteraction = 7.63 mb: rejected | | pT0 = 1.35 gives sigmaInteraction = 8.65 mb: rejected | | pT0 = 1.21 gives sigmaInteraction = 10.04 mb: rejected | | pT0 = 1.09 gives sigmaInteraction = 11.40 mb: accepted | | diffractive mass = 1.400e+04 GeV and sigmaNorm = 10.000 mb | | pT0 = 2.74 gives sigmaInteraction = 7.96 mb: rejected | | pT0 = 2.47 gives sigmaInteraction = 9.41 mb: rejected | | pT0 = 2.22 gives sigmaInteraction = 11.18 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Diffraction:PomFlux | 5 | 1 1 5 | | Init:showChangedParticleData | off | on | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 2 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.16000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:ecmRef | 1960.000 | 1800.000 1.00000 | | MultipartonInteractions:pT0Ref | 2.00000 | 2.15000 0.50000 10.00000 | | Next:numberCount | 500 | 1000 0 | | Next:numberShowEvent | 0 | 1 0 | | Next:numberShowInfo | 3 | 1 0 | | Next:numberShowProcess | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SoftQCD:all | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. Process A B -> X X double diffractive with code 105 is 2 -> 2. It has s = 1.960e+08, t = -3.805e-01, u = -1.959e+08, pT = 6.165e-01, m3 = 1.370e+00, m4 = 2.445e+02, theta = 8.810e-05, phi = 1.782e+00. Diffractive system on side B: In 1: id = -3, x = 2.334e-01, pdf = 3.309e-03 at Q2 = 4.420e-01. In 2: id = 21, x = 7.165e-04, pdf = 9.323e+00 at same Q2. Subprocess q g -> q g with code 113 is 2 -> 2. It has sHat = 9.991e+00, tHat = -4.635e-01, uHat = -9.527e+00, pTHat = 6.648e-01, m3Hat = 0.000e+00, m4Hat = 0.000e+00, thetaHat = 4.342e-01, phiHat = 5.910e+00. alphaEM = 7.480e-03, alphaS = 4.257e-01 at Q2 = 2.526e+00. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. In 1: id = 21, x = 3.752e-02, pdf = 6.724e+00 at Q2 = 5.299e+01. In 2: id = 21, x = 1.634e-04, pdf = 9.730e+01 at same Q2. Process non-diffractive with code 101 is 2 -> 2. Subprocess g g -> g g with code 111 is 2 -> 2. It has sHat = 1.202e+03, tHat = -5.555e+01, uHat = -1.146e+03, pTHat = 7.279e+00, m3Hat = 0.000e+00, m4Hat = 0.000e+00, thetaHat = 4.334e-01, phiHat = 4.883e-01. alphaEM = 7.606e-03, alphaS = 2.271e-01 at Q2 = 6.049e+01. Impact parameter b = 1.171e+00 gives enhancement factor = 2.380e-01. Max pT scale for MPI = 7.279e+00, ISR = 7.279e+00, FSR = 7.279e+00. Number of MPI = 4, ISR = 8, FSRproc = 61, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. Process A B -> A B elastic with code 102 is 2 -> 2. It has s = 1.960e+08, t = -1.745e-01, u = -1.960e+08, pT = 4.177e-01, m3 = 9.383e-01, m4 = 9.383e-01, theta = 5.967e-05, phi = 4.726e+00. -------- End PYTHIA Info Listing ------------------------------------ PYTHIA Warning in SpaceShower::pT2nextQCD: weight above unity PYTHIA Error in BeamRemnants::setKinematics: kinematics construction failed PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame PYTHIA Error in Pythia::check: unmatched particle energy/momentum/mass PYTHIA Error in Pythia::next: check of event revealed problems Pythia::next(): 500 events have been generated *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | non-diffractive 101 | 520 520 520 | 5.584e+01 3.536e-07 | | A B -> A B elastic 102 | 289 289 289 | 3.210e+01 0.000e+00 | | A B -> X B single diffractive 103 | 41 41 41 | 5.628e+00 3.356e-08 | | A B -> A X single diffractive 104 | 60 60 60 | 5.628e+00 0.000e+00 | | A B -> X X double diffractive 105 | 84 84 84 | 9.472e+00 0.000e+00 | | A B -> A X B central diffractive 106 | 6 6 6 | 8.179e-01 4.302e-09 | | | | | | sum | 1000 1000 1000 | 1.095e+02 3.552e-07 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 6 Error in BeamRemnants::setKinematics: kinematics construction failed | | 3 Error in Pythia::check: unmatched particle energy/momentum/mass | | 1 Error in Pythia::next: check of event revealed problems | | 3 Warning in MultipartonInteractions::init: maximum increased | | 11 Warning in SpaceShower::pT2nextQCD: weight above unity | | 2 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:01 rapidity of charged particles; all 1.40*10^ 3 2 X 5 1.35*10^ 3 X X7 76X 1 1.30*10^ 3 2X X4X 79XX6XXXXX7 4 1.25*10^ 3 4XXXXXXXXXXXXXXXXXX6 X67 1.20*10^ 3 3 14XXXXXXXXXXXXXXXXXXXX8XXX431 1.15*10^ 3 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1 1.10*10^ 3 22XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3X 5 1.05*10^ 3 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 2 1.00*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX1X 0.95*10^ 3 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 0.90*10^ 3 574XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1 0.85*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8X 0.80*10^ 3 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 0.75*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.70*10^ 3 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX1 0.65*10^ 3 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9 0.60*10^ 3 9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX92 0.55*10^ 3 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.50*10^ 3 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6 0.45*10^ 3 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.40*10^ 3 27XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.35*10^ 3 6 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX72 0.30*10^ 3 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX22 3 0.25*10^ 3 X 3777XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX82 X 0.20*10^ 3 X 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5221 X 0.15*10^ 3 7X 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 X9 0.10*10^ 3 XX2 9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX754XX 0.05*10^ 3 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2 Contents *10^ 3 0000000000000000000000000000001111111111111111111111111111111111111110100000000000000000000000000000 *10^ 2 0120001112222232334455667888890001111122223232223323332322122211101009098877665544333222211111000210 *10^ 1 0366594561333439682649256078742562645615956704899383379082962366560475113593549583831664176652876640 *10^ 0 9601231153375818278815255234017823785888802128358703138768299694643876259303333816741022271061568659 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 72558 Mean = -2.5779e-02 Underflow = 1.9000e+01 Low edge = -1.0000e+01 All chan = 7.2521e+04 Rms = 3.9062e+00 Overflow = 1.8000e+01 High edge = 1.0000e+01 2013-09-20 16:01 number of charged particles; all 3.24*10^ 2 9 3.12*10^ 2 X 3.00*10^ 2 X 2.88*10^ 2 X 2.76*10^ 2 X 2.64*10^ 2 X 2.52*10^ 2 X 2.40*10^ 2 X 2.28*10^ 2 X 2.16*10^ 2 X 2.04*10^ 2 X 1.92*10^ 2 X 1.80*10^ 2 X 1.68*10^ 2 X 1.56*10^ 2 X 1.44*10^ 2 X 1.32*10^ 2 X 1.20*10^ 2 X 1.08*10^ 2 X 0.96*10^ 2 X 0.84*10^ 2 X 4 0.72*10^ 2 X X 0.60*10^ 2 X X72 0.48*10^ 2 X 3 6XXX 0.36*10^ 2 X7X8XXXX8 4 0.24*10^ 2 XXXXXXXXX9X7771 1 0.12*10^ 2 XXXXXXXXXXXXXXX5XX878548635355 331343414133522 13432321 1131 2 1 Contents *10^ 2 3000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 2343475532222210110000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 3204377043901036239896597363660431353515133622013532321011310020100000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 1000 Mean = 7.3316e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+03 Rms = 9.7856e+01 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 number of charged particles; single diffraction 2.50*10^ 1 X 2.40*10^ 1 X 2.30*10^ 1 XX 2.20*10^ 1 XX 2.10*10^ 1 XX 2.00*10^ 1 XX 1.90*10^ 1 XXX 1.80*10^ 1 XXX 1.70*10^ 1 XXX 1.60*10^ 1 XXX 1.50*10^ 1 XXX 1.40*10^ 1 XXX 1.30*10^ 1 XXX 1.20*10^ 1 XXX 1.10*10^ 1 XXX 1.00*10^ 1 XXX 0.90*10^ 1 XXXX 0.80*10^ 1 XXXX 0.70*10^ 1 XXXX 0.60*10^ 1 XXXXX 0.50*10^ 1 XXXXXX 0.40*10^ 1 XXXXXXX 0.30*10^ 1 XXXXXXX X 0.20*10^ 1 XXXXXXX XXX 0.10*10^ 1 XXXXXXX XXX X XX Contents *10^ 1 2210000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 5399654022300101100000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 101 Mean = 2.4807e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0100e+02 Rms = 2.6021e+01 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 number of charged particles, double diffractive 1.84*10^ 1 55 1.76*10^ 1 XX 1.68*10^ 1 XX 1.60*10^ 1 XX 1.52*10^ 1 XX 1.44*10^ 1 XX5 1.36*10^ 1 XXX 1.28*10^ 1 XXX 1.20*10^ 1 XXX 1.12*10^ 1 XXX 1.04*10^ 1 XXX 0.96*10^ 1 XXX 0.88*10^ 1 XXX 0.80*10^ 1 XXXX 0.72*10^ 1 XXXX 0.64*10^ 1 5XXXX5 0.56*10^ 1 XXXXXX 0.48*10^ 1 XXXXXX 0.40*10^ 1 XXXXXX X 0.32*10^ 1 XXXXXX7 X 0.24*10^ 1 XXXXXXX 5 X 5 0.16*10^ 1 XXXXXXX2X X2 X 2 0.08*10^ 1 XXXXXXXXX XX X X Contents *10^ 1 0011100000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 6888463120410200000100000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 84 Mean = 3.4071e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 8.4000e+01 Rms = 2.6103e+01 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 number of charged particles, central diffractive 3.00*10^ 0 X 2.88*10^ 0 X 2.76*10^ 0 X 2.64*10^ 0 X 2.52*10^ 0 X 2.40*10^ 0 X 2.28*10^ 0 X 2.16*10^ 0 X 2.04*10^ 0 X 7 1.92*10^ 0 X X 1.80*10^ 0 X X 1.68*10^ 0 X X 1.56*10^ 0 X X 1.44*10^ 0 X X 1.32*10^ 0 X X 1.20*10^ 0 X X 1.08*10^ 0 X3X 0.96*10^ 0 XXX 0.84*10^ 0 XXX 0.72*10^ 0 XXX 0.60*10^ 0 XXX 0.48*10^ 0 XXX 0.36*10^ 0 XXX 0.24*10^ 0 XXX 0.12*10^ 0 XXX Contents *10^ 0 3120000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 6 Mean = 1.0167e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 6.0000e+00 Rms = 7.1802e+00 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 number of charged particles, non-diffractive 6.75*10^ 1 4 6.50*10^ 1 X 6.25*10^ 1 X 6.00*10^ 1 X 5.75*10^ 1 X 5.50*10^ 1 X 5.25*10^ 1 X 5.00*10^ 1 XX6 4.75*10^ 1 XXX 4.50*10^ 1 XXX 4.25*10^ 1 XXX 4.00*10^ 1 XXX 3.75*10^ 1 XXX 3.50*10^ 1 XXX 3.25*10^ 1 XXX 3.00*10^ 1 XXXX 2.75*10^ 1 XXXX 2.50*10^ 1 2XXXX 2.25*10^ 1 XXXXX48 4 2.00*10^ 1 XXXXXXX6X 1.75*10^ 1 XXXXXXXXX8 1.50*10^ 1 XXXXXXXXXX2 2 1.25*10^ 1 XXXXXXXXXXX 4X 1.00*10^ 1 XXXXXXXXXXX XX6 6 6 0.75*10^ 1 8XXXXXXXXXXX XXX8X4 X8 4 44 4 0.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXX2X2XX 62 2X2X X 22X 2X2 2 2 0.25*10^ 1 4XXXXXXXXXXXXXXXXXXXXXXXXXXX XX4XXXX4X4XXX88 4XXX8X84 44X4 8 4 Contents *10^ 1 0000265432212110110000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0017360901291735139796597363660431353515133622013532321011310020100000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 520 Mean = 1.2861e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 5.2000e+02 Rms = 1.0796e+02 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 (n_charged) all 8.70*10^-1 1 8.40*10^-1 X 8.10*10^-1 X 9 7.80*10^-1 X X 7.50*10^-1 X 6 6X 7.20*10^-1 5 9 X 6 9X XX51 6 6.90*10^-1 X 5X 2 X X8 8XX XXXX X 6.60*10^-1 X 7 XX X2X 5XX5XXX XXXX X 1 6.30*10^-1 X336X XX54XXX 3XXXXXXX XXXX X X 6.00*10^-1 2 45 3XXXXX1XXXXXXX XXXXXXXX XXXX X X 5.70*10^-1 11 X 1XX 6XXXXXXXXXXXXXX XXXXXXXX XXXX X X 5.40*10^-1 72XXX78X3XXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 5.10*10^-1 9 195XXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 4.80*10^-1 8 XXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 4.50*10^-1 5X987XXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 4.20*10^-1 3 69XXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 3.90*10^-1 7X8XXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 3.60*10^-1 8XXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 3.30*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 3.00*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 2.70*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 2.40*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 2.10*10^-1 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 1.80*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 1.50*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 1.20*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 0.90*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 0.60*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 0.30*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X Contents *10^-1 1333334444444544545555555555550557666656766668066766677078760070600000000000000000000000000000000000 *10^-2 9258980137444088093144433714880570101577111634004084813030090000300000000000000000000000000000000000 *10^-3 4930856663642711752604204592130974077045752474085653578066340060300000000000000000000000000000000000 *10^-4 1090637728215359610430493460270073573609376554026748193096830090700000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 2000 Mean = 2.7163e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 3.7153e-01 Rms = 1.3974e+02 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 (n_charged) single diffraction 6.25*10^-1 X 6.00*10^-1 X 5.75*10^-1 9 X 5.50*10^-1 X X 5.25*10^-1 X 6X 5.00*10^-1 X XX 4.75*10^-1 9 X XX 4.50*10^-1 6 3 X X XX 4.25*10^-1 X3 X5X X XX 4.00*10^-1 2XXX XXX X XX 3.75*10^-1 XXXX XXX X XX 3.50*10^-1 8XXXX XXX X XX 3.25*10^-1 8XXXXX XXX X XX 3.00*10^-1 3XXXXXX XXX X XX 2.75*10^-1 XXXXXXX XXX X XX 2.50*10^-1 XXXXXXX XXX X XX 2.25*10^-1 XXXXXXX XXX X XX 2.00*10^-1 XXXXXXX XXX X XX 1.75*10^-1 XXXXXXX XXX X XX 1.50*10^-1 XXXXXXX XXX X XX 1.25*10^-1 XXXXXXX XXX X XX 1.00*10^-1 XXXXXXX XXX X XX 0.75*10^-1 XXXXXXX XXX X XX 0.50*10^-1 XXXXXXX XXX X XX 0.25*10^-1 XXXXXXX XXX X XX Contents *10^-1 2333444044400505600000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 8247300031700701200000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 2159970022100304600000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-4 1170085068800501100000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 202 Mean = 6.8323e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 3.5162e-01 Rms = 4.1360e+01 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 (n_charged) double diffraction 5.00*10^-1 5 4.80*10^-1 X 4.60*10^-1 8 2 X 4.40*10^-1 X X X 4.20*10^-1 584 X X X 4.00*10^-1 XXX 7X X X 3.80*10^-1 343XXX5 XX X X 3.60*10^-1 73XXXXXXX XX X X 3.40*10^-1 XXXXXXXXX XX X X 3.20*10^-1 XXXXXXXXX XX X X 3.00*10^-1 XXXXXXXXX XX X X 2.80*10^-1 XXXXXXXXX XX X X 2.60*10^-1 XXXXXXXXX XX X X 2.40*10^-1 XXXXXXXXX XX X X 2.20*10^-1 XXXXXXXXX XX X X 2.00*10^-1 XXXXXXXXX XX X X 1.80*10^-1 XXXXXXXXX XX X X 1.60*10^-1 XXXXXXXXX XX X X 1.40*10^-1 XXXXXXXXX XX X X 1.20*10^-1 XXXXXXXXX XX X X 1.00*10^-1 XXXXXXXXX XX X X 0.80*10^-1 XXXXXXXXX XX X X 0.60*10^-1 XXXXXXXXX XX X X 0.40*10^-1 XXXXXXXXX XX X X 0.20*10^-1 XXXXXXXXX XX X X Contents *10^-1 3333344430340400000400000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 5466611070950400000900000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 4657505700350300000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-4 6988863270200300000100000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 168 Mean = 6.2144e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 3.7488e-01 Rms = 4.2650e+01 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 (n_charged) central diffraction 4.05*10^-1 X 3.90*10^-1 X 3.75*10^-1 X3 3.60*10^-1 XX 3.45*10^-1 XX7 3.30*10^-1 XXX 3.15*10^-1 XXX 3.00*10^-1 XXX 2.85*10^-1 XXX 2.70*10^-1 XXX 2.55*10^-1 XXX 2.40*10^-1 XXX 2.25*10^-1 XXX 2.10*10^-1 XXX 1.95*10^-1 XXX 1.80*10^-1 XXX 1.65*10^-1 XXX 1.50*10^-1 XXX 1.35*10^-1 XXX 1.20*10^-1 XXX 1.05*10^-1 XXX 0.90*10^-1 XXX 0.75*10^-1 XXX 0.60*10^-1 XXX 0.45*10^-1 XXX 0.30*10^-1 XXX 0.15*10^-1 XXX Contents *10^-1 4330000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0640000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 4500000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-4 8060000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 12 Mean = 1.1037e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 3.7678e-01 Rms = 6.5383e+00 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 (n_charged) non-diffractive 8.70*10^-1 1 8.40*10^-1 X 8.10*10^-1 X 9 7.80*10^-1 X X 7.50*10^-1 X 6 6X 7.20*10^-1 5 9 X 6 9X XX51 6 6.90*10^-1 X 5X 2 X X8 8XX XXXX X 6.60*10^-1 X 7 XX X2X 5XX5XXX XXXX X 1 6.30*10^-1 X336X XX54XXX 3XXXXXXX XXXX X X 6.00*10^-1 2 45 3XXXXX1XXXXXXX XXXXXXXX XXXX X X 5.70*10^-1 11 X 1XX 6XXXXXXXXXXXXXX XXXXXXXX XXXX X X 5.40*10^-1 73XXX78X3XXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 5.10*10^-1 X 65XXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 4.80*10^-1 X1 XX8XXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 4.50*10^-1 7XX87XXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 4.20*10^-1 86 69XXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 3.90*10^-1 XX7XXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 3.60*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 3.30*10^-1 8XXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 3.00*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 2.70*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 2.40*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 2.10*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 1.80*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 1.50*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 1.20*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 0.90*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 0.60*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X 0.30*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXXXXX XXXXXXXX XXXX X X Contents *10^-1 0034434444444544445555555555550557666656766668066766677078760070600000000000000000000000000000000000 *10^-2 0021080147544187993244433714880570101577111634004084813030090000300000000000000000000000000000000000 *10^-3 0033816609232115652004204592130974077045752474085653578066340060300000000000000000000000000000000000 *10^-4 0030037987455055810230493460270073573609376554026748193096830090700000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 1040 Mean = 2.7570e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 4.8071e-01 Rms = 1.3688e+02 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 log10(mass), by diffractive system 5.20*10^ 2 X 5.00*10^ 2 X 4.80*10^ 2 X 4.60*10^ 2 X 4.40*10^ 2 X 4.20*10^ 2 X 4.00*10^ 2 X 3.80*10^ 2 X 3.60*10^ 2 X 3.40*10^ 2 X 3.20*10^ 2 X 3.00*10^ 2 X 2.80*10^ 2 X 2.60*10^ 2 X 2.40*10^ 2 X 2.20*10^ 2 X 2.00*10^ 2 X 1.80*10^ 2 X 1.60*10^ 2 X 1.40*10^ 2 X 1.20*10^ 2 X 1.00*10^ 2 X 0.80*10^ 2 X 0.60*10^ 2 X 0.40*10^ 2 X 0.20*10^ 2 1737412322223134312111231121131331333121332323312 111312111111 111 111 1111 X Contents *10^ 2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000500000000000000000 *10^ 1 0010100000000000000000000000000000000000000000000000000000000000000000000000000000200000000000000000 *10^ 0 0137483454444536862421345234337266356734365454561401325142332320133023101111000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^-1 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^-2 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 795 Mean = 3.2218e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 7.9500e+02 Rms = 1.3729e+00 Overflow = 0.0000e+00 High edge = 5.0000e+00 2013-09-20 16:01 (log10(mass)) 1.30*10^ 2 4 6 1.25*10^ 2 X X 1.20*10^ 2 X8 X 1.15*10^ 2 XX X 1.10*10^ 2 8XX X 1.05*10^ 2 XXX X 1.00*10^ 2 XXX X 0.95*10^ 2 XXX X 0.90*10^ 2 4 XXX X 0.85*10^ 2 X 2 XXX X 0.80*10^ 2 8 X X XXX X 0.75*10^ 2 6 X X X XXXX X 0.70*10^ 2 X X X X XXXX X 0.65*10^ 2 X X3X 6 X XXXX X 0.60*10^ 2 X 5 XXX X X XXXX X 0.55*10^ 2 X X XXX X3X XXXX X 0.50*10^ 2 1 3X X XXX XXX XXXX X 0.45*10^ 2 X XX X6 XXX XXX XXXX X 0.40*10^ 2 X XX24 XX16 XXX XXX XXXX X 0.35*10^ 2 2 8 X XXXX7XXXX XXX XXX XXXX X 0.30*10^ 2 X 2 X82 8XXXXXXXXXXX XXX XXX XXXX X 0.25*10^ 2 X X X14 58 X8XXX XXXXXXXXXXXX XXX XXX XXXX X 0.20*10^ 2 8 4X8 X2 XXX53XXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 0.15*10^ 2 11 1X28XXX9XX7XXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 0.10*10^ 2 2 42X 5XX6XXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 0.05*10^ 2 232333326768XX9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X Contents *10^ 2 0000000000000000000000000000000000000000000000000000000000000000000000001110000000100000000000000000 *10^ 1 0000000000000000000010011011111311211222112222232202434733354330768065800217000000200000000000000000 *10^ 0 0111111113334554557605700809146184653402762405349609506367373580917031109795000000800000000000000000 *10^-1 0030367520500007800300756030009083087930376000800000706000770700070007000000000000200000000000000000 Low edge *10^ 0 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^-1 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^-2 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 1590 Mean = 2.8896e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 9.0399e+01 Rms = 8.5791e-01 Overflow = 0.0000e+00 High edge = 5.0000e+00 2013-09-20 16:01 _charged>(log10(mass)) 6.50*10^-1 2 6.25*10^-1 X 6.00*10^-1 1X 5.75*10^-1 XX 5.50*10^-1 6 XX 5.25*10^-1 3 X XX7 5.00*10^-1 3 X 63 3 X XXX 2 4.75*10^-1 X X XX X XX XXX X 4.50*10^-1 X 4 X 7 3 XX3 1 X XX XXX X 4.25*10^-1 X X X 8 2 X X 51 3XXX X 6 X8X XX XXX X 4.00*10^-1 X2 X X X X X X X 8 X 1 X XX 34 XXXX 9 X33X XXX XX XXX8 X 3.75*10^-1 XX X X X X X X X2 X X 8 3 2X8X9XX XX XXXX6X XXXX XXX 6XX XXXX X 3.50*10^-1 XX X X X9X5 X 9X7 7XX X 6X 26X X7XXXXXXX XX8 9XXXXXX3XXXX XXX XXX XXXX X 3.25*10^-1 XXXX6X XXXX X3XXX6XXX38X XX9XXX7XXXXXXXXX93XXX XXXXXXXXXXXX XXX XXX XXXX X 3.00*10^-1 XXXXXX8XXXX4XXXXXXXXXXXX5XXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 2.75*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 2.50*10^-1 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 2.25*10^-1 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 2.00*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 1.75*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 1.50*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 1.25*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 1.00*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 0.75*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 0.50*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X 0.25*10^-1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX XXX XXX XXXX X Contents *10^-1 0224334352434324334333433332334333333333343443333303444433343340444034505653000000400000000000000000 *10^-2 0028723109240380044414050298030234715457737102088404088369328810228067407219000000800000000000000000 *10^-3 0182945575060834862241156066090110076336022221616607682256362240701044007974000000000000000000000000 *10^-4 0931161193788481678927158724193325555697617848491109591256008880725030202469000000700000000000000000 Low edge *10^ 0 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^-1 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^-2 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 1590 Mean = 1.9995e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 4.4174e-01 Rms = 1.1221e+00 Overflow = 0.0000e+00 High edge = 5.0000e+00 2013-09-20 16:01 elastic |t| spectrum 6.75*10^ 1 8 6.50*10^ 1 X 6.25*10^ 1 X 6.00*10^ 1 X 5.75*10^ 1 X 5.50*10^ 1 X 5.25*10^ 1 X 5.00*10^ 1 XX 4.75*10^ 1 XX 4.50*10^ 1 XX 4.25*10^ 1 XX4 4.00*10^ 1 XXX 3.75*10^ 1 XXX 3.50*10^ 1 XXX 3.25*10^ 1 XXX 3.00*10^ 1 XXX 2.75*10^ 1 XXX 2.50*10^ 1 XXX6 2.25*10^ 1 XXXX4 2.00*10^ 1 XXXXX 1.75*10^ 1 XXXXX 4 1.50*10^ 1 XXXXX6 X 1.25*10^ 1 XXXXXX X8 1.00*10^ 1 XXXXXX6XX 0.75*10^ 1 XXXXXXXXX44 0.50*10^ 1 XXXXXXXXXXX 62 22 0.25*10^ 1 XXXXXXXXXXX8XX848XX 44 4 Contents *10^ 1 6542210110000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 7014149626624321233001100000100000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^-1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-2 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 289 Mean = 4.2855e-02 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 2.8900e+02 Rms = 4.5331e-02 Overflow = 0.0000e+00 High edge = 1.0000e+00 2013-09-20 16:01 elastic log10(|t|) spectrum 1.50*10^ 1 X X 1.44*10^ 1 X X 1.38*10^ 1 X X 1.32*10^ 1 7 X 7 X 1.26*10^ 1 X X X X 1.20*10^ 1 X X X X 1.14*10^ 1 3 X X X3 X3 1.08*10^ 1 X X X XX XX 1.02*10^ 1 X X7X7 7 XX XX 0.96*10^ 1 X XXXX X XX XX 0.90*10^ 1 X XXXXXXXXXX XX 0.84*10^ 1 3 X XXXXXXXXXX3 XX 0.78*10^ 1 X X XXXXXXXXXXX XX 0.72*10^ 1 7 7X7 X7 XXXXXXXXXXX XX77 0.66*10^ 1 X XXX XX XXXXXXXXXXX XXXX 0.60*10^ 1 XX X XXXXXXXXXXXXXXXXXXXXXXX 0.54*10^ 1 3 XX3X XXXXXXXXXXXXXXXXXXXXXXX3 3 0.48*10^ 1 X XXXX XXXXXXXXXXXXXXXXXXXXXXXX X 0.42*10^ 1 X 7XXXX XXXXXXXXXXXXXXXXXXXXXXXX X 0.36*10^ 1 X XXXXX XXXXXXXXXXXXXXXXXXXXXXXX X 0.30*10^ 1 X X XXXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.24*10^ 1 3 3 X 3 X XXXXX3XXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.18*10^ 1 X X X X X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.12*10^ 1 7 7 7 77 X X X7 77X X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX77 7 0.06*10^ 1 X X X XX X X XX XXX X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X Contents *10^ 1 0000000000000000000000000000000000000000000000000000000000000010011110101100011000000000000000000000 *10^ 0 0000000000000000001001000010110020020000000310112050467562787617630509093198651775335311010000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge ---------------------------------------------------------------------------------------------------- *10^ 0 5444444444444444444443333333333333333333322222222222222222222111111111111111111110000000000000000000 *10^-1 0998877665544332211009988776655443322110099887766554433221100998877665544332211009988776655443322110 *10^-2 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 289 Mean = -1.6459e+00 Underflow = 0.0000e+00 Low edge = -5.0000e+00 All chan = 2.8900e+02 Rms = 5.8431e-01 Overflow = 0.0000e+00 High edge = 0.0000e+00 2013-09-20 16:01 single diffractive |t| spectrum 1.92*10^ 1 8 1.84*10^ 1 X 1.76*10^ 1 X3 1.68*10^ 1 XX 1.60*10^ 1 XX 1.52*10^ 1 XX 1.44*10^ 1 XX5 1.36*10^ 1 XXX 1.28*10^ 1 XXX 1.20*10^ 1 XXX 1.12*10^ 1 XXX 1.04*10^ 1 XXX 0.96*10^ 1 XXX 0.88*10^ 1 XXX 0.80*10^ 1 XXX 0.72*10^ 1 XXX 0.64*10^ 1 XXX5 0.56*10^ 1 XXXX222 2 0.48*10^ 1 XXXXXXX X 0.40*10^ 1 XXXXXXXXX X 0.32*10^ 1 XXXXXXXXX X 0.24*10^ 1 XXXXXXXXX5X 5 5 5 5 0.16*10^ 1 XXXXXXXXXXX X2X 22 X X 22 2 2 0.08*10^ 1 XXXXXXXXXXX XXX XX X X XX X X Contents *10^ 1 1110000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 9746555452402120110002020001101000000000000001000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^-1 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^-2 0246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 101 Mean = 1.2485e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0100e+02 Rms = 1.5455e-01 Overflow = 0.0000e+00 High edge = 2.0000e+00 2013-09-20 16:01 double diffractive |t| spectrum 1.30*10^ 1 X 1.25*10^ 1 X 1.20*10^ 1 X 1.15*10^ 1 X 1.10*10^ 1 X 1.05*10^ 1 X 1.00*10^ 1 X X 0.95*10^ 1 X X 0.90*10^ 1 XX XX 0.85*10^ 1 XX XX 0.80*10^ 1 XX XX X 0.75*10^ 1 XX XX X 0.70*10^ 1 XX XX X 0.65*10^ 1 XX XX X 0.60*10^ 1 XX XX X 0.55*10^ 1 XX XX X 0.50*10^ 1 XXXXX XX 0.45*10^ 1 XXXXX XX 0.40*10^ 1 XXXXX XX X 0.35*10^ 1 XXXXX XX X 0.30*10^ 1 XXXXXXXX XX 0.25*10^ 1 XXXXXXXX XX 0.20*10^ 1 XXXXXXXXXXX X 0.15*10^ 1 XXXXXXXXXXX X 0.10*10^ 1 XXXXXXXXXXXX XX X X X X X X X X X 0.05*10^ 1 XXXXXXXXXXXX XX X X X X X X X X X Contents *10^ 1 0100100000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 9359035823410110000200001010001010000000000010010000000010000000000100000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^-1 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^-2 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 84 Mean = 4.2738e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 8.4000e+01 Rms = 6.0764e-01 Overflow = 0.0000e+00 High edge = 5.0000e+00 2013-09-20 16:01 central diffractive |t| spectrum 3.00*10^ 0 X 2.88*10^ 0 X 2.76*10^ 0 X 2.64*10^ 0 X 2.52*10^ 0 X 2.40*10^ 0 X 2.28*10^ 0 X 2.16*10^ 0 X 2.04*10^ 0 7X 77 1.92*10^ 0 XX XX 1.80*10^ 0 XX XX 1.68*10^ 0 XX XX 1.56*10^ 0 XX XX 1.44*10^ 0 XX XX 1.32*10^ 0 XX XX 1.20*10^ 0 XX XX 1.08*10^ 0 XX XX333 0.96*10^ 0 XX XXXXX 0.84*10^ 0 XX XXXXX 0.72*10^ 0 XX XXXXX 0.60*10^ 0 XX XXXXX 0.48*10^ 0 XX XXXXX 0.36*10^ 0 XX XXXXX 0.24*10^ 0 XX XXXXX 0.12*10^ 0 XX XXXXX Contents *10^ 0 2302211100000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^-1 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^-2 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 12 Mean = 1.7083e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.2000e+01 Rms = 1.1265e-01 Overflow = 0.0000e+00 High edge = 5.0000e+00 2013-09-20 16:01 diffractive mass spectrum 4.35*10^ 1 7 4.20*10^ 1 X 4.05*10^ 1 X 3.90*10^ 1 X 3.75*10^ 1 X 3.60*10^ 1 X 3.45*10^ 1 X 3.30*10^ 1 X 3.15*10^ 1 X 3.00*10^ 1 X 2.85*10^ 1 X 2.70*10^ 1 X 2.55*10^ 1 X 2.40*10^ 1 X 2.25*10^ 1 X 2.10*10^ 1 X 1.95*10^ 1 X 1.80*10^ 1 X 1.65*10^ 1 X 1.50*10^ 1 XX 1.35*10^ 1 XX 1.20*10^ 1 XX 1.05*10^ 1 XX 7 0.90*10^ 1 XXXX X 0.75*10^ 1 XXXX7X 0.60*10^ 1 XXXXXXX 0.45*10^ 1 XXXXXXX 7 77 0.30*10^ 1 XXXXXXX3X 3 3 XX 33 3 3 X3X3 3 3 3 3 3 3 3 3 33 3 0.15*10^ 1 XXXXXXXXX7X7X XX7777XX X7 X XXXX X 7X7 77X X777 X7 X X 77X 77 XX 7 X 7 7 7 7777 Contents *10^ 1 0410001000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0359970624121204411112202102000323202001210112021110000210020200112011022010200101000001000000001111 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 0 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 275 Mean = 2.0788e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.8400e+02 Rms = 2.5530e+01 Overflow = 9.1000e+01 High edge = 1.0000e+02 2013-09-20 16:01 log10(diffractive mass spectrum) 1.20*10^ 1 X 1.15*10^ 1 X 1.10*10^ 1 X 1.05*10^ 1 X 1.00*10^ 1 X 0.95*10^ 1 X 0.90*10^ 1 X X 0.85*10^ 1 X X 0.80*10^ 1 X X 0.75*10^ 1 X X 0.70*10^ 1 X X X 0.65*10^ 1 X X X 0.60*10^ 1 XXXX X XX X X X 0.55*10^ 1 XXXX X XX X X X 0.50*10^ 1 XXXXXX X XX XX XX XX X X XX 0.45*10^ 1 XXXXXX X XX XX XX XX X X XX 0.40*10^ 1 XXXXXX XXX X X XX X X XX XX XX XXXX X X X X XX X X 0.35*10^ 1 XXXXXX XXX X X XX X X XX XX XX XXXX X X X X XX X X 0.30*10^ 1 XXXXXX XXX XXXX XXXXX X XX XX XX XXXXXXXX X XXXXXX XX X X X X X XX X X 0.25*10^ 1 XXXXXX XXX XXXX XXXXX X XX XX XX XXXXXXXX X XXXXXX XX X X X X X XX X X 0.20*10^ 1 XXXXXXXXXX XXXXXXXXXXXX XX XXXXXX XXX XXXXXXXX XXXXXXXXXXX XX XX X XX XX XX XX XX 0.15*10^ 1 XXXXXXXXXX XXXXXXXXXXXX XX XXXXXX XXX XXXXXXXX XXXXXXXXXXX XX XX X XX XX XX XX XX 0.10*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX XXXXXXXXXXXXXX XXXX XX X XX XX 0.05*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX XXXXXXXXXXXXXX XXXX XX X XX XX Contents *10^ 1 0000010000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0069625624541433423673424122144223312561553345641426343352550320123141421321330011320230101101100000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^-1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^-2 0482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 275 Mean = 1.5153e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 2.7500e+02 Rms = 9.9381e-01 Overflow = 0.0000e+00 High edge = 4.0000e+00 2013-09-20 16:01 total pT_hard spectrum 2.32*10^ 2 6 2.24*10^ 2 X 2.16*10^ 2 X 2.08*10^ 2 X 2.00*10^ 2 X 1.92*10^ 2 X 1.84*10^ 2 X 1.76*10^ 2 X 1.68*10^ 2 X3 1.60*10^ 2 XX 1.52*10^ 2 XX 1.44*10^ 2 XX 1.36*10^ 2 XX 1.28*10^ 2 XX 1.20*10^ 2 XX 1.12*10^ 2 XX 1.04*10^ 2 XX 0.96*10^ 2 XX 0.88*10^ 2 XX 0.80*10^ 2 XX 0.72*10^ 2 XX 0.64*10^ 2 XX4 0.56*10^ 2 XXX 0.48*10^ 2 XXX 0.40*10^ 2 XXX 0.32*10^ 2 XXX 4 0.24*10^ 2 XXXX 4X4 4 1 0.16*10^ 2 XXXX 95 44XXXXX72X5 6X2X 4 5416 1562 1 0.08*10^ 2 XXXX959XX6XXXXXXXXXXX9XXXX6X9XXXX9XXXX663X15464956356341514313 3 413111 3313 1 13 1 13 1 1 Contents *10^ 2 2100000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 2652000110111112111110111101011010011100000000000000000000000000000000000000000000000000000000000000 *10^ 0 9294747525116697940927370651721937923055291435374524523141321202003121110022120010120010000001201010 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^ 0 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^-1 0246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 1000 Mean = 3.0613e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 9.9100e+02 Rms = 3.7220e+00 Overflow = 9.0000e+00 High edge = 2.0000e+01 2013-09-20 16:01 nondiffractive pT_hard spectrum 2.70*10^ 1 X 2.60*10^ 1 X 2.50*10^ 1 X 2.40*10^ 1 X 2.30*10^ 1 X 2.20*10^ 1 X 2.10*10^ 1 X 2.00*10^ 1 X 1.90*10^ 1 XXX X 1.80*10^ 1 XXX X 1.70*10^ 1 XXX X X 1.60*10^ 1 XXXXX X X X 1.50*10^ 1 XXXXX X X X 1.40*10^ 1 XXXXXX X X X 1.30*10^ 1 XXXXXX X XX X X X 1.20*10^ 1 X XXXXXX XX XX X X X XX 1.10*10^ 1 XX XXXXXXXX XX XX X X XX X XX 1.00*10^ 1 XX XXXXXXXXXXX XXXX X XX X XXX 0.90*10^ 1 XX XXXXXXXXXXX XXXX X XXXX XXXX X 0.80*10^ 1 XX XXXXXXXXXXX XXXX X XXXX XXXX X 0.70*10^ 1 XX XXXXXXXXXXXXXXXX XXXXXXXXXXX X X 0.60*10^ 1 XX XXXXXXXXXXXXXXXX XXXXXXXXXXX X X 0.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X X X X 0.40*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X X XXX XX X 0.30*10^ 1 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X XXXXXXX XX X X X X 0.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXXXXXX X XX X X X X XX X X X 0.10*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X XXXXXX XXXX X XX X XX X X Contents *10^ 1 0000000110111112111110111101011010011100000000000000000000000000000000000000000000000000000000000000 *10^ 0 0223225215116697940927370651721937923055291435374524523141321202003121110022120010120010000001201010 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^ 0 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^-1 0246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 520 Mean = 5.6832e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 5.1100e+02 Rms = 3.5529e+00 Overflow = 9.0000e+00 High edge = 2.0000e+01 2013-09-20 16:01 b impact parameter spectrum 2.50*10^ 1 X 2.40*10^ 1 X XX 2.30*10^ 1 X X XX 2.20*10^ 1 X X XX 2.10*10^ 1 XXX XX 2.00*10^ 1 XXX XX X 1.90*10^ 1 XXX XX X 1.80*10^ 1 X XXX XXX X X 1.70*10^ 1 X XXXX XXXX X X 1.60*10^ 1 X X XXXX XXXX X X 1.50*10^ 1 XX X X XXXX XXXX X XX 1.40*10^ 1 XXXX XXXXXXXXXXX X XX 1.30*10^ 1 XXXX XXXXXXXXXXXXXXXX 1.20*10^ 1 XXXXX XXXXXXXXXXXXXXXX 1.10*10^ 1 XXXXX XXXXXXXXXXXXXXXX 1.00*10^ 1 X XXXXXXXXXXXXXXXXXXXXXX 0.90*10^ 1 X X XXXXXXXXXXXXXXXXXXXXXXXXX 0.80*10^ 1 XXX XX XXXXXXXXXXXXXXXXXXXXXXXXX 0.70*10^ 1 XXX XXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.60*10^ 1 X XXXX XXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.50*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 0.40*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX 0.30*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 0.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X X 0.10*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXX X X X Contents *10^ 1 0000000000010001111111112221221112111000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0016569885807992554806474134548730358964345533012120300000010100000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^-1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^-2 0482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 520 Mean = 1.0048e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 5.2000e+02 Rms = 4.1770e-01 Overflow = 0.0000e+00 High edge = 4.0000e+00 2013-09-20 16:01 b enhancement spectrum 0.92*10^ 2 X 0.88*10^ 2 X 0.84*10^ 2 X 0.80*10^ 2 X 0.76*10^ 2 X 0.72*10^ 2 XX 0.68*10^ 2 XX 0.64*10^ 2 XX 0.60*10^ 2 XX 0.56*10^ 2 XXX 0.52*10^ 2 XXX 0.48*10^ 2 XXX 0.44*10^ 2 XXX 0.40*10^ 2 XXX X 0.36*10^ 2 XXX5X 0.32*10^ 2 XXXXX 0.28*10^ 2 XXXXX 0.24*10^ 2 XXXXX2 0.20*10^ 2 XXXXXX7 0.16*10^ 2 XXXXXXX 5 0.12*10^ 2 XXXXXXXXXX2525 0.08*10^ 2 XXXXXXXXXXXXXXX27 2 0.04*10^ 2 XXXXXXXXXXXXXXXXXX8X5838555X85 88 553 X33833383X 553 35833 853353 Contents *10^ 1 9753421111010100000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 2264019224909085743523132224320330221041131113140221012311032112100000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-1 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 520 Mean = 1.0177e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 5.2000e+02 Rms = 1.4340e+00 Overflow = 0.0000e+00 High edge = 1.0000e+01 2013-09-20 16:01 number of interactions 1.68*10^ 2 8 1.62*10^ 2 X 1.56*10^ 2 X 1.50*10^ 2 X 1.44*10^ 2 X 1.38*10^ 2 X 1.32*10^ 2 X 1.26*10^ 2 X 1.20*10^ 2 X 1.14*10^ 2 X 1.08*10^ 2 X 1.02*10^ 2 X 0.96*10^ 2 X 0.90*10^ 2 X7 0.84*10^ 2 XX 0.78*10^ 2 XX 0.72*10^ 2 XX 0.66*10^ 2 XX 0.60*10^ 2 XX3 0.54*10^ 2 XXX 0.48*10^ 2 XXX 0.42*10^ 2 XXX 0.36*10^ 2 XXX 0.30*10^ 2 XXX5 0.24*10^ 2 XXXX733 0.18*10^ 2 XXXXXXX 0.12*10^ 2 XXXXXXXXX 223 3 0.06*10^ 2 XXXXXXXXX5XXXX7X88X837722X257 52 2 2 Contents *10^ 2 0100000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0685222211000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0786720022377864655652441181340310101000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 1 0000000000011111111112222222222333333333344444444445555555555666666666677777777778888888888999999999 *10^ 0 0012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789012345678 *10^-1 5555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555555 Entries = 520 Mean = 5.8038e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 5.2000e+02 Rms = 7.1557e+00 Overflow = 0.0000e+00 High edge = 9.9500e+01 2013-09-20 16:01 pT spectrum for b < 0.5 4.05*10^ 0 7 7 7 3.90*10^ 0 X X X 3.75*10^ 0 X X X 3.60*10^ 0 X X X 3.45*10^ 0 X X X 3.30*10^ 0 X X X 3.15*10^ 0 X X X 3.00*10^ 0 X X X X X X X X 2.85*10^ 0 X X X X X X X X 2.70*10^ 0 X X X X X X X X 2.55*10^ 0 X X X X X X X X 2.40*10^ 0 X X X X X X X X 2.25*10^ 0 X X X X X X X X 2.10*10^ 0 X 3 X33 X3 3 X 3 X X X X 3 3 33 1.95*10^ 0 X X XXX XX X X X X X X X X X XX 1.80*10^ 0 X X XXX XX X X X X X X X X X XX 1.65*10^ 0 X X XXX XX X X X X X X X X X XX 1.50*10^ 0 X X XXX XX X X X X X X X X X XX 1.35*10^ 0 X X XXX XX X X X X X X X X X XX 1.20*10^ 0 X X XXX XX X X X X X X X X X XX 1.05*10^ 0 X 7 X XXX7XX7X X7X777X7X7 X77 X7X 7 X7 7 XX7 7 77 7 0.90*10^ 0 X X X XXXXXXXX XXXXXXXXXX XXX XXX X XX X XXX X XX X 0.75*10^ 0 X X X XXXXXXXX XXXXXXXXXX XXX XXX X XX X XXX X XX X 0.60*10^ 0 X X X XXXXXXXX XXXXXXXXXX XXX XXX X XX X XXX X XX X 0.45*10^ 0 X X X XXXXXXXX XXXXXXXXXX XXX XXX X XX X XXX X XX X 0.30*10^ 0 X X X XXXXXXXX XXXXXXXXXX XXX XXX X XX X XXX X XX X 0.15*10^ 0 X X X XXXXXXXX XXXXXXXXXX XXX XXX X XX X XXX X XX X Contents *10^ 0 0000000000000000000000000301020042213212031211141310411031200100002101000022100010110000000000100000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^ 0 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^-1 0246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 70 Mean = 9.8672e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 6.7000e+01 Rms = 3.2118e+00 Overflow = 3.0000e+00 High edge = 2.0000e+01 2013-09-20 16:01 pT spectrum for 0.5 < b < 1 1.00*10^ 1 X 0.96*10^ 1 X 0.92*10^ 1 X 5 0.88*10^ 1 X X 0.84*10^ 1 X X 0.80*10^ 1 X XX 0.76*10^ 1 X XX 0.72*10^ 1 5X 5 5 XX 55 0.68*10^ 1 XX X X XX XX 0.64*10^ 1 XX X X XX XX 0.60*10^ 1 XX X X X X XX XX 0.56*10^ 1 XX X X X X XX XX 0.52*10^ 1 XX X 5 X X X XX 5XX 0.48*10^ 1 XX X X X X X XX XXX 0.44*10^ 1 XX X X X X X XX XXX 0.40*10^ 1 XXXXXX XX X X X XXXX XXX 0.36*10^ 1 XXXXXX XX X X X XXXX XXX 0.32*10^ 1 XXXXXX5XX X55X X XXXX5XXX 5 5 5 0.28*10^ 1 XXXXXXXXX XXXX X XXXXXXXX X X X 0.24*10^ 1 XXXXXXXXX XXXX X XXXXXXXX X X X 0.20*10^ 1 X XXXXXXXXX XXXXXXXXXXXXXXXXX X X XXXXX X X X X 0.16*10^ 1 X XXXXXXXXX XXXXXXXXXXXXXXXXX X X XXXXX X X X X 0.12*10^ 1 5 5X 5XXXXXXXXX5XXXXXXXXXXXXXXXXX5 X X5XXXXX5X5 555 X55 X X 55 5 55 0.08*10^ 1 X XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXX X XXXXXXXXXX XXX XXX X X XX X XX 0.04*10^ 1 X XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXX X XXXXXXXXXX XXX XXX X X XX X XX Contents *10^ 1 0000000000000001000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0001000120014470463541633727289443577231030213222212101110021102000020110000010000000000000001100000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^ 0 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^-1 0246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 176 Mean = 6.2688e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.7300e+02 Rms = 3.1882e+00 Overflow = 3.0000e+00 High edge = 2.0000e+01 2013-09-20 16:01 pT spectrum for 1 < b < 1.5 1.50*10^ 1 X 1.44*10^ 1 X 1.38*10^ 1 X 1.32*10^ 1 7X 1.26*10^ 1 XX 1.20*10^ 1 XX 1.14*10^ 1 3XX 3 1.08*10^ 1 XXX X 1.02*10^ 1 XXX 7 X 0.96*10^ 1 XXX X X 0.90*10^ 1 X XXX X X 0.84*10^ 1 3X3XXX3 X X 0.78*10^ 1 XXXXXXX X X 0.72*10^ 1 7 7XXXXXXX X7 7X 0.66*10^ 1 X XXXXXXXX XX XX 0.60*10^ 1 XX XXXXXXXXXXX XX X 0.54*10^ 1 XX XXXXXXXXXXX3XX3 33 X 0.48*10^ 1 XX XXXXXXXXXXXXXXX XX X 0.42*10^ 1 7XX XXXXXXXXXXXXXXX7 XX 7 X 0.36*10^ 1 XXX XXXXXXXXXXXXXXXX XX X X 0.30*10^ 1 XXX XXXXXXXXXXXXXXXXXXX XX XXX X 0.24*10^ 1 33333XXX XXXXXXXXXXXXXXXXXXX33XX3 XXX 33X 3 0.18*10^ 1 XXXXXXXX XXXXXXXXXXXXXXXXXXXXXXXX XXX XXX X 0.12*10^ 1 XXXXXXXX7XXXXXXXXXXXXXXXXXXXXXXXX7XXX XXX 77 77 X 77 7 7 7 7 7 7 0.06*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX XX XX X XX X X X X X X Contents *10^ 1 0000000000000011100100010000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0222224671789813586075715433322552143602230011011002011000100000001000000000010000000010000000001010 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^ 0 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^-1 0246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 225 Mean = 4.4486e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 2.2200e+02 Rms = 2.9310e+00 Overflow = 3.0000e+00 High edge = 2.0000e+01 2013-09-20 16:01 pT spectrum for 1.5 < b 5.00*10^ 0 X 4.80*10^ 0 X 4.60*10^ 0 X 4.40*10^ 0 X 4.20*10^ 0 X 4.00*10^ 0 X XX X X X 3.80*10^ 0 X XX X X X 3.60*10^ 0 X XX X X X 3.40*10^ 0 X XX X X X 3.20*10^ 0 X XX X X X 3.00*10^ 0 X XX XX X X X 2.80*10^ 0 X XX XX X X X 2.60*10^ 0 X XX XX X X X 2.40*10^ 0 X XX XX X X X 2.20*10^ 0 X XX XX X X X 2.00*10^ 0 XXXXXXX X X XXX X 1.80*10^ 0 XXXXXXX X X XXX X 1.60*10^ 0 XXXXXXX X X XXX X 1.40*10^ 0 XXXXXXX X X XXX X 1.20*10^ 0 XXXXXXX X X XXX X 1.00*10^ 0 XXXXXXXXXX XXXX XXX X X X X 0.80*10^ 0 XXXXXXXXXX XXXX XXX X X X X 0.60*10^ 0 XXXXXXXXXX XXXX XXX X X X X 0.40*10^ 0 XXXXXXXXXX XXXX XXX X X X X 0.20*10^ 0 XXXXXXXXXX XXXX XXX X X X X Contents *10^ 0 0000001524423414001411032200200000100010000000000000000000000000000000000000000000010000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^ 0 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^-1 0246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 49 Mean = 3.4878e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 4.9000e+01 Rms = 2.4201e+00 Overflow = 0.0000e+00 High edge = 2.0000e+01 2013-09-20 16:01 b spectrum for pT < 2 5.00*10^ 0 X 4.80*10^ 0 X 4.60*10^ 0 X 4.40*10^ 0 X 4.20*10^ 0 X 4.00*10^ 0 X X X 3.80*10^ 0 X X X 3.60*10^ 0 X X X 3.40*10^ 0 X X X 3.20*10^ 0 X X X 3.00*10^ 0 X XX XX X X 2.80*10^ 0 X XX XX X X 2.60*10^ 0 X XX XX X X 2.40*10^ 0 X XX XX X X 2.20*10^ 0 X XX XX X X 2.00*10^ 0 XX XX XXXXXX X X 1.80*10^ 0 XX XX XXXXXX X X 1.60*10^ 0 XX XX XXXXXX X X 1.40*10^ 0 XX XX XXXXXX X X 1.20*10^ 0 XX XX XXXXXX X X 1.00*10^ 0 X X XX XXXXXXXXXXX X XX X X X 0.80*10^ 0 X X XX XXXXXXXXXXX X XX X X X 0.60*10^ 0 X X XX XXXXXXXXXXX X XX X X X 0.40*10^ 0 X X XX XXXXXXXXXXX X XX X X X 0.20*10^ 0 X X XX XXXXXXXXXXX X XX X X X Contents *10^ 0 0000000000000000000010102301134135222402003100001000100000010000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^-1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^-2 0482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 44 Mean = 1.3682e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 4.4000e+01 Rms = 3.0410e-01 Overflow = 0.0000e+00 High edge = 4.0000e+00 2013-09-20 16:01 b spectrum for 2 < pT < 5 1.50*10^ 1 X 1.44*10^ 1 X33 3 1.38*10^ 1 XXX X 1.32*10^ 1 XXX X7 1.26*10^ 1 XXX XX 1.20*10^ 1 XXX XX X 1.14*10^ 1 XXX XX 3 X 1.08*10^ 1 XXX XX X X 1.02*10^ 1 7XXX XX X 7 X 0.96*10^ 1 XXXX XX X X X 0.90*10^ 1 XXXXXXXXXXX X 0.84*10^ 1 XXXXXXXXXXX X 0.78*10^ 1 XXXXXXXXXXX X 0.72*10^ 1 XXXXXXXXXXX77X 0.66*10^ 1 XXXXXXXXXXXXXX 0.60*10^ 1 X X X XXXXXXXXXXXXXX X 0.54*10^ 1 X X X3XXXXXXXXXXXXXX X 0.48*10^ 1 X X XXXXXXXXXXXXXXXX X 0.42*10^ 1 X7X XXXXXXXXXXXXXXXX X 0.36*10^ 1 XXX XXXXXXXXXXXXXXXX X 0.30*10^ 1 X XXX XXXXXXXXXXXXXXXXXX X XX 0.24*10^ 1 X 3XXX3XXXXXXXXXXXXXXXXXX33X XX3 3 0.18*10^ 1 X XXXXXXXXXXXXXXXXXXXXXXXXXX XXX X 0.12*10^ 1 7X7XXXXXXXXXXXXXXXXXXXXXXXXXX7XXX 77 X 7 7 0.06*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX X X X Contents *10^ 1 0000000000000000000000011110110101001000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000000000131264626505449439190772362231332011020100000000100000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^-1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^-2 0482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 221 Mean = 1.1869e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 2.2100e+02 Rms = 3.0981e-01 Overflow = 0.0000e+00 High edge = 4.0000e+00 2013-09-20 16:01 b spectrum for 5 < pT < 15 1.30*10^ 1 X 1.25*10^ 1 X 1.20*10^ 1 X 1.15*10^ 1 X 1.10*10^ 1 XX X 1.05*10^ 1 XX X 1.00*10^ 1 X XX XX 0.95*10^ 1 X XX XX 0.90*10^ 1 X X XXXXX X 0.85*10^ 1 X X XXXXX X 0.80*10^ 1 X X XXXXX X X X 0.75*10^ 1 X X XXXXX X X X 0.70*10^ 1 X X X XXXXX XXXX X XX 0.65*10^ 1 X X X XXXXX XXXX X XX 0.60*10^ 1 X XXX XXXXXXXXXXXXXXX X XX 0.55*10^ 1 X XXX XXXXXXXXXXXXXXX X XX 0.50*10^ 1 X XXXX XXXXXXXXXXXXXXX X XX X X X 0.45*10^ 1 X XXXX XXXXXXXXXXXXXXX X XX X X X 0.40*10^ 1 XXXXXX XXXXXXXXXXXXXXXXXXXXXX XXX 0.35*10^ 1 XXXXXX XXXXXXXXXXXXXXXXXXXXXX XXX 0.30*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXX 0.25*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXX 0.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXX 0.15*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXXXX 0.10*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX X X X 0.05*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XXX X X X Contents *10^ 1 0000000000010001101100000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0016469653606761390169777484874515453200011101000100100000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^-1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^-2 0482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 231 Mean = 7.8762e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 2.3100e+02 Rms = 3.9193e-01 Overflow = 0.0000e+00 High edge = 4.0000e+00 2013-09-20 16:01 b spectrum for 15 < pT 3.00*10^ 0 X 2.88*10^ 0 X 2.76*10^ 0 X 2.64*10^ 0 X 2.52*10^ 0 X 2.40*10^ 0 X 2.28*10^ 0 X 2.16*10^ 0 X 2.04*10^ 0 7X77 7 1.92*10^ 0 XXXX X 1.80*10^ 0 XXXX X 1.68*10^ 0 XXXX X 1.56*10^ 0 XXXX X 1.44*10^ 0 XXXX X 1.32*10^ 0 XXXX X 1.20*10^ 0 XXXX X 1.08*10^ 0 3 XXXX 33 3333 3 X33 33 3 0.96*10^ 0 X XXXX XX XXXX X XXX XX X 0.84*10^ 0 X XXXX XX XXXX X XXX XX X 0.72*10^ 0 X XXXX XX XXXX X XXX XX X 0.60*10^ 0 X XXXX XX XXXX X XXX XX X 0.48*10^ 0 X XXXX XX XXXX X XXX XX X 0.36*10^ 0 X XXXX XX XXXX X XXX XX X 0.24*10^ 0 X XXXX XX XXXX X XXX XX X 0.12*10^ 0 X XXXX XX XXXX X XXX XX X Contents *10^ 0 0000100232201100000111100010211000011000100000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 0 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^-1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^-2 0482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 24 Mean = 7.5167e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 2.4000e+01 Rms = 4.2763e-01 Overflow = 0.0000e+00 High edge = 4.0000e+00 pythia8-8.1.80.orig/examples/outref/out070000644000175000017500000027133212217346171016370 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:02:04 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide e+ with e- at a CM energy of 5.000e+02 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | GenericResonance 9001 | 4.088e-01 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eCM | 500.00000 | 14000.000 10.00000 | | Beams:idA | -11 | 2212 | | Beams:idB | 11 | 2212 | | Main:timesAllowErrors | 5 | 10 0 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberCount | 100 | 1000 0 | | PDF:lepton | off | on | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products 13 mu- mu+ 2 -3 0 0.10566 0.00000 0.00000 0.00000 6.58654e+05 0 1 0 1 0 0 1 1.0000000 22 -12 11 14 130 K_L0 1 0 0 0.49761 0.00000 0.00000 0.00000 1.53300e+04 0 1 0 1 0 0 1 0.1952278 0 111 111 111 1 1 0.1254178 0 211 -211 111 2 1 0.2027688 22 -12 11 211 3 1 0.2027688 22 12 -11 -211 4 1 0.1352191 22 -14 13 211 5 1 0.1352191 22 14 -13 -211 6 1 0.0019673 0 211 -211 7 1 0.0008641 0 111 111 8 1 0.0005471 0 22 22 211 pi+ pi- 1 3 0 0.13957 0.00000 0.00000 0.00000 7.80450e+03 0 1 0 1 0 0 1 0.9998770 0 -13 14 1 1 0.0001230 0 -11 12 321 K+ K- 1 3 0 0.49368 0.00000 0.00000 0.00000 3.71300e+03 0 1 0 1 0 0 1 0.6355250 0 -13 14 1 1 0.0000158 0 -11 12 2 1 0.2066081 0 211 111 3 1 0.0559022 0 211 211 -211 4 1 0.0176107 0 211 111 111 5 1 0.0507020 22 12 -11 111 6 1 0.0335313 22 14 -13 111 7 1 0.0000220 0 -11 12 111 111 8 1 0.0000409 0 -11 12 211 -211 9 1 0.0000140 0 -13 14 111 111 10 1 0.0000280 0 -13 14 211 -211 2112 n0 nbar0 2 0 0 0.93957 0.00000 0.00000 0.00000 2.65500e+14 0 1 0 1 0 0 1 1.0000000 22 -12 11 2212 999999 GeneralResonance 1 0 0 500.00000 1.00000 0.00000 0.00000 0.00000e+00 1 1 0 1 0 0 1 0.2000000 101 1 -1 1 1 0.2000000 101 6 -6 2 1 0.2000000 101 15 -15 3 1 0.2000000 101 24 -24 4 1 0.2000000 101 25 25 -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = -11, pz = 2.500e+02, e = 2.500e+02, m = 5.110e-04. Beam B: id = 11, pz = -2.500e+02, e = 2.500e+02, m = 5.110e-04. In 1: id = -11, x = 1.000e+00, pdf = 1.000e+00 at Q2 = 2.500e+05. In 2: id = 11, x = 1.000e+00, pdf = 1.000e+00 at same Q2. Subprocess GenericResonance with code 9001 is 2 -> 1. It has sHat = 2.500e+05. alphaEM = 7.971e-03, alphaS = 1.067e-01 at Q2 = 2.500e+05. Impact parameter b = 0.000e+00 gives enhancement factor = 1.000e+00. Max pT scale for MPI = 5.000e+02, ISR = 5.000e+02, FSR = 5.000e+02. Number of MPI = 1, ISR = 0, FSRproc = 0, FSRreson = 20. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 500.000 500.000 1 -11 (e+) -12 0 0 3 0 0 0 0.000 0.000 250.000 250.000 0.001 2 11 (e-) -12 0 0 4 0 0 0 0.000 0.000 -250.000 250.000 0.001 3 -11 (e+) -21 1 0 5 0 0 0 0.000 0.000 250.000 250.000 0.000 4 11 (e-) -21 2 0 5 0 0 0 0.000 0.000 -250.000 250.000 0.000 5 999999 (GeneralResonance) -22 3 4 6 7 0 0 0.000 0.000 0.000 500.000 500.000 6 24 (W+) -22 5 0 8 9 0 0 -125.579 -97.357 176.267 250.835 81.238 7 -24 (W-) -22 5 0 10 11 0 0 125.579 97.357 -176.267 249.165 75.927 8 -1 dbar 23 6 0 0 0 0 101 1.570 -37.647 43.395 57.472 0.330 9 4 c 23 6 0 0 0 101 0 -127.148 -59.710 132.872 193.363 1.500 10 1 d 23 7 0 0 0 102 0 78.044 58.729 -52.070 110.686 0.330 11 -2 ubar 23 7 0 0 0 0 102 47.535 38.628 -124.196 138.479 0.330 Charge sum: 0.000 Momentum sum: 0.000 0.000 -0.000 500.000 500.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 500.000 500.000 1 -11 (e+) -12 0 0 3 0 0 0 0.000 0.000 250.000 250.000 0.001 2 11 (e-) -12 0 0 4 0 0 0 0.000 0.000 -250.000 250.000 0.001 3 -11 (e+) -21 1 0 5 0 0 0 0.000 0.000 250.000 250.000 0.000 4 11 (e-) -21 2 0 5 0 0 0 0.000 0.000 -250.000 250.000 0.000 5 999999 (GeneralResonance) -22 3 4 6 7 0 0 0.000 0.000 0.000 500.000 500.000 6 24 (W+) -22 5 0 8 9 0 0 -125.579 -97.357 176.267 250.835 81.238 7 -24 (W-) -22 5 0 31 32 0 0 125.579 97.357 -176.267 249.165 75.927 8 -1 (dbar) -23 6 0 12 12 0 101 1.570 -37.647 43.395 57.472 0.330 9 4 (c) -23 6 0 10 11 101 0 -127.148 -59.710 132.872 193.363 1.500 10 4 (c) -51 9 0 101 101 103 0 -104.864 -51.013 108.474 159.272 1.500 11 21 (g) -51 9 0 13 14 101 103 -22.277 -8.862 24.588 34.342 0.000 12 -1 (dbar) -52 8 8 15 15 0 101 1.563 -37.483 43.205 57.221 0.330 13 21 (g) -51 11 0 16 17 104 103 -19.739 -6.895 20.051 28.969 0.000 14 21 (g) -51 11 0 18 18 101 104 -2.500 -2.880 5.589 6.767 0.000 15 -1 (dbar) -52 12 12 24 24 0 101 1.525 -36.570 42.153 55.827 0.330 16 21 (g) -51 13 0 30 30 107 103 -17.811 -5.833 18.426 26.283 0.000 17 21 (g) -51 13 0 19 20 104 107 -2.203 -1.378 2.238 3.430 0.000 18 21 (g) -52 14 14 21 21 101 104 -2.225 -2.564 4.976 6.023 0.000 19 21 (g) -51 17 0 28 29 109 107 -0.414 -0.093 0.941 1.032 0.000 20 21 (g) -51 17 0 105 105 104 109 -3.023 -2.706 4.055 5.736 0.000 21 21 (g) -52 18 18 22 23 101 104 -0.992 -1.143 2.218 2.685 0.000 22 21 (g) -51 21 0 106 106 110 104 -1.229 -2.019 2.849 3.702 0.000 23 21 (g) -51 21 0 25 26 101 110 0.332 -1.396 1.987 2.451 0.000 24 -1 (dbar) -52 15 15 27 27 0 101 1.429 -34.298 39.534 52.359 0.330 25 21 (g) -51 23 0 107 107 111 110 -0.096 -3.361 4.411 5.546 0.000 26 21 (g) -51 23 0 108 108 101 111 0.871 -8.862 10.045 13.423 0.000 27 -1 (dbar) -52 24 24 109 109 0 101 0.986 -23.471 27.066 35.840 0.330 28 21 (g) -51 19 0 104 104 109 112 -2.572 -0.876 3.642 4.543 0.000 29 21 (g) -51 19 0 103 103 112 107 -2.194 -0.643 1.802 2.911 0.000 30 21 (g) -52 16 16 102 102 107 103 -13.459 -4.408 13.924 19.861 0.000 31 1 (d) -23 7 0 33 34 102 0 78.044 58.729 -52.070 110.686 0.330 32 -2 (ubar) -23 7 0 35 35 0 102 47.535 38.628 -124.196 138.479 0.330 33 1 (d) -51 31 0 42 43 114 0 72.548 56.133 -47.919 103.492 0.330 34 21 (g) -51 31 0 36 37 102 114 5.977 2.987 -5.410 8.597 0.000 35 -2 (ubar) -52 32 32 38 38 0 102 47.053 38.237 -122.938 137.076 0.330 36 21 (g) -51 34 0 44 44 117 114 6.667 3.196 -7.498 10.531 0.000 37 21 (g) -51 34 0 41 41 102 117 0.146 0.470 -0.095 0.501 0.000 38 -2 (ubar) -52 35 35 39 40 0 102 46.217 37.558 -120.754 134.642 0.330 39 -2 (ubar) -51 38 0 86 86 0 118 40.465 32.702 -103.914 116.212 0.330 40 21 (g) -51 38 0 47 47 118 102 5.762 4.887 -16.846 18.463 0.000 41 21 (g) -52 37 37 45 46 102 117 0.136 0.440 -0.088 0.469 0.000 42 1 (d) -51 33 0 48 49 119 0 71.354 55.193 -46.856 101.653 0.330 43 21 (g) -51 33 0 50 50 114 119 1.644 1.156 -1.568 2.549 0.000 44 21 (g) -52 36 36 54 55 117 114 6.218 2.981 -6.993 9.821 0.000 45 21 (g) -51 41 0 56 56 120 117 0.243 0.035 -1.650 1.669 0.000 46 21 (g) -51 41 0 53 53 102 120 1.101 1.429 -1.970 2.671 0.000 47 21 (g) -52 40 40 51 52 118 102 4.554 3.862 -13.314 14.591 0.000 48 1 (d) -51 42 0 74 74 121 0 17.388 13.095 -10.881 24.338 0.330 49 21 (g) -51 42 0 69 70 119 121 54.262 42.306 -36.258 77.774 0.000 50 21 (g) -52 43 43 71 71 114 119 1.348 0.948 -1.286 2.090 0.000 51 21 (g) -51 47 0 85 85 118 122 2.324 1.650 -4.932 5.696 0.000 52 21 (g) -51 47 0 62 62 122 102 2.566 2.648 -8.983 9.711 0.000 53 21 (g) -52 46 46 60 61 102 120 0.765 0.992 -1.369 1.856 0.000 54 21 (g) -51 44 0 78 78 123 114 3.547 1.410 -4.559 5.946 0.000 55 21 (g) -51 44 0 59 59 117 123 2.706 1.576 -2.675 4.119 0.000 56 21 (g) -52 45 45 57 58 120 117 0.208 0.030 -1.409 1.425 0.000 57 21 (g) -51 56 0 65 65 120 124 0.846 -0.083 -1.582 1.796 0.000 58 21 (g) -51 56 0 80 80 124 117 0.237 0.622 -0.692 0.960 0.000 59 21 (g) -52 55 55 79 79 117 123 1.831 1.066 -1.810 2.787 0.000 60 21 (g) -51 53 0 63 64 126 120 0.498 1.199 -2.551 2.863 0.000 61 21 (g) -51 53 0 66 67 102 126 1.173 0.728 -1.989 2.421 0.000 62 21 (g) -52 52 52 84 84 122 102 1.660 1.713 -5.812 6.283 0.000 63 21 (g) -51 60 0 68 68 126 127 0.253 0.892 -2.433 2.604 0.000 64 21 (g) -51 60 0 72 0 127 120 0.691 0.263 -0.953 1.207 0.000 65 21 (g) -52 57 57 72 0 120 124 0.400 -0.039 -0.747 0.848 0.000 66 21 (g) -51 61 0 83 83 102 128 0.058 0.362 -1.338 1.388 0.000 67 21 (g) -51 61 0 73 0 128 126 1.300 1.019 -2.433 2.941 0.000 68 21 (g) -52 63 63 73 0 126 127 0.068 0.239 -0.651 0.696 0.000 69 21 (g) -51 49 0 75 75 129 121 49.903 38.829 -33.685 71.642 0.000 70 21 (g) -51 49 0 76 76 119 129 4.595 3.642 -2.798 6.497 0.000 71 21 (g) -52 50 50 77 77 114 119 1.112 0.782 -1.061 1.724 0.000 72 21 (g) -73 64 65 81 81 127 124 1.091 0.224 -1.700 2.055 0.301 73 21 (g) -73 67 68 82 82 128 127 1.368 1.258 -3.084 3.637 0.517 74 1 (d) -71 48 48 87 100 121 0 17.388 13.095 -10.881 24.338 0.330 75 21 (g) -71 69 69 87 100 129 121 49.903 38.829 -33.685 71.642 0.000 76 21 (g) -71 70 70 87 100 119 129 4.595 3.642 -2.798 6.497 0.000 77 21 (g) -71 71 71 87 100 114 119 1.112 0.782 -1.061 1.724 0.000 78 21 (g) -71 54 54 87 100 123 114 3.547 1.410 -4.559 5.946 0.000 79 21 (g) -71 59 59 87 100 117 123 1.831 1.066 -1.810 2.787 0.000 80 21 (g) -71 58 58 87 100 124 117 0.237 0.622 -0.692 0.960 0.000 81 21 (g) -71 72 72 87 100 127 124 1.091 0.224 -1.700 2.055 0.301 82 21 (g) -71 73 73 87 100 128 127 1.368 1.258 -3.084 3.637 0.517 83 21 (g) -71 66 66 87 100 102 128 0.058 0.362 -1.338 1.388 0.000 84 21 (g) -71 62 62 87 100 122 102 1.660 1.713 -5.812 6.283 0.000 85 21 (g) -71 51 51 87 100 118 122 2.324 1.650 -4.932 5.696 0.000 86 -2 (ubar) -71 39 39 87 100 0 118 40.465 32.702 -103.914 116.212 0.330 87 -211 (pi-) -83 74 86 149 150 0 0 24.222 19.115 -15.946 34.733 0.140 88 321 (K+) -83 74 86 151 152 0 0 8.099 6.118 -5.450 11.531 0.494 89 -321 (K-) -83 74 86 153 154 0 0 30.813 23.279 -19.889 43.441 0.494 90 321 (K+) -83 74 86 155 156 0 0 8.138 6.891 -6.362 12.427 0.494 91 -313 (K*bar0) -83 74 86 124 125 0 0 2.154 0.805 -1.839 3.065 0.851 92 -211 (pi-) -83 74 86 157 158 0 0 3.811 1.982 -5.066 6.643 0.140 93 213 (rho+) -84 74 86 126 127 0 0 1.166 0.921 -1.206 1.989 0.544 94 -211 (pi-) -84 74 86 159 160 0 0 0.864 0.593 -0.814 1.334 0.140 95 321 (K+) -84 74 86 161 162 0 0 0.669 0.270 -1.936 2.124 0.494 96 -313 (K*bar0) -84 74 86 128 129 0 0 1.439 1.564 -3.816 4.460 0.901 97 111 (pi0) -84 74 86 163 164 0 0 4.224 3.111 -11.048 12.231 0.135 98 113 (rho0) -84 74 86 130 131 0 0 5.876 5.354 -15.755 17.687 1.187 99 -211 (pi-) -84 74 86 165 166 0 0 5.716 4.169 -14.170 15.839 0.140 100 221 (eta) -84 74 86 167 169 0 0 28.386 23.188 -72.971 81.661 0.548 101 4 (c) -71 10 10 110 123 103 0 -104.864 -51.013 108.474 159.272 1.500 102 21 (g) -71 30 30 110 123 107 103 -13.459 -4.408 13.924 19.861 0.000 103 21 (g) -71 29 29 110 123 112 107 -2.194 -0.643 1.802 2.911 0.000 104 21 (g) -71 28 28 110 123 109 112 -2.572 -0.876 3.642 4.543 0.000 105 21 (g) -71 20 20 110 123 104 109 -3.023 -2.706 4.055 5.736 0.000 106 21 (g) -71 22 22 110 123 110 104 -1.229 -2.019 2.849 3.702 0.000 107 21 (g) -71 25 25 110 123 111 110 -0.096 -3.361 4.411 5.546 0.000 108 21 (g) -71 26 26 110 123 101 111 0.871 -8.862 10.045 13.423 0.000 109 -1 (dbar) -71 27 27 110 123 0 101 0.986 -23.471 27.066 35.840 0.330 110 423 (D*0) -83 101 109 170 171 0 0 -80.063 -38.765 83.186 121.806 2.007 111 213 (rho+) -83 101 109 132 133 0 0 -15.309 -7.144 15.851 23.180 0.813 112 -211 (pi-) -83 101 109 172 173 0 0 -2.233 -0.982 2.106 3.226 0.140 113 113 (rho0) -83 101 109 134 135 0 0 -7.030 -3.093 6.683 10.222 0.906 114 323 (K*+) -83 101 109 136 137 0 0 -8.524 -3.616 9.363 13.190 0.755 115 -311 (Kbar0) -83 101 109 138 138 0 0 -7.140 -2.347 7.416 10.570 0.498 116 113 (rho0) -84 101 109 139 140 0 0 -1.381 -1.093 1.999 2.735 0.616 117 223 (omega) -84 101 109 174 176 0 0 -3.752 -2.700 5.120 6.942 0.785 118 -213 (rho-) -84 101 109 141 142 0 0 -1.357 -1.349 1.801 2.719 0.699 119 321 (K+) -84 101 109 177 178 0 0 -0.202 -4.263 5.401 6.901 0.494 120 -323 (K*-) -84 101 109 143 144 0 0 0.374 -2.981 3.600 4.763 0.834 121 211 (pi+) -84 101 109 179 180 0 0 -0.073 -0.302 0.425 0.544 0.140 122 221 (eta) -84 101 109 181 183 0 0 0.251 -14.965 17.705 23.190 0.548 123 113 (rho0) -84 101 109 145 146 0 0 0.860 -13.756 15.611 20.847 0.957 124 -321 (K-) -91 91 0 184 186 0 0 1.925 0.835 -1.763 2.785 0.494 125 211 (pi+) -91 91 0 187 188 0 0 0.229 -0.030 -0.076 0.281 0.140 126 211 (pi+) -91 93 0 189 190 0 0 0.331 0.055 -0.369 0.518 0.140 127 111 (pi0) -91 93 0 191 192 0 0 0.835 0.866 -0.837 1.472 0.135 128 -321 (K-) -91 96 0 193 194 0 0 1.096 1.414 -3.451 3.918 0.494 129 211 (pi+) -91 96 0 195 196 0 0 0.344 0.150 -0.365 0.541 0.140 130 211 (pi+) -91 98 0 197 198 0 0 1.532 1.881 -5.676 6.174 0.140 131 -211 (pi-) -91 98 0 199 200 0 0 4.344 3.473 -10.079 11.513 0.140 132 211 (pi+) -91 111 0 201 202 0 0 -6.252 -3.324 6.529 9.632 0.140 133 111 (pi0) -91 111 0 203 204 0 0 -9.056 -3.820 9.323 13.548 0.135 134 211 (pi+) -91 113 0 205 206 0 0 -0.465 -0.169 0.702 0.870 0.140 135 -211 (pi-) -91 113 0 207 208 0 0 -6.565 -2.925 5.982 9.352 0.140 136 311 (K0) -91 114 0 147 147 0 0 -5.470 -2.150 5.845 8.304 0.498 137 211 (pi+) -91 114 0 209 210 0 0 -3.055 -1.466 3.518 4.886 0.140 138 310 (K_S0) -91 115 115 211 212 0 0 -7.140 -2.347 7.416 10.570 0.498 139 211 (pi+) -91 116 0 213 214 0 0 -0.757 -0.369 0.639 1.067 0.140 140 -211 (pi-) -91 116 0 215 216 0 0 -0.624 -0.724 1.360 1.668 0.140 141 -211 (pi-) -91 118 0 217 218 0 0 -0.136 -0.495 0.589 0.794 0.140 142 111 (pi0) -91 118 0 219 220 0 0 -1.221 -0.855 1.212 1.925 0.135 143 -311 (Kbar0) -91 120 0 148 148 0 0 0.209 -1.122 1.370 1.851 0.498 144 -211 (pi-) -91 120 0 221 222 0 0 0.165 -1.859 2.230 2.911 0.140 145 211 (pi+) -91 123 0 223 224 0 0 0.699 -5.047 5.436 7.452 0.140 146 -211 (pi-) -91 123 0 225 226 0 0 0.161 -8.709 10.175 13.395 0.140 147 310 (K_S0) -91 136 136 227 228 0 0 -5.470 -2.150 5.845 8.304 0.498 148 130 (K_L0) -91 143 143 229 231 0 0 0.209 -1.122 1.370 1.851 0.498 149 13 (mu-) -91 87 0 232 234 0 0 21.051 16.639 -13.886 30.213 0.106 150 -14 nu_mubar 91 87 0 0 0 0 0 3.171 2.476 -2.059 4.520 0.000 151 -13 (mu+) -91 88 0 235 237 0 0 5.945 4.345 -4.154 8.454 0.106 152 14 nu_mu 91 88 0 0 0 0 0 2.154 1.773 -1.297 3.077 0.000 153 13 (mu-) -91 89 0 238 240 0 0 17.734 13.618 -11.341 25.072 0.106 154 -14 nu_mubar 91 89 0 0 0 0 0 13.079 9.661 -8.548 18.370 0.000 155 211 (pi+) -91 90 0 241 242 0 0 5.254 4.571 -4.346 8.210 0.140 156 111 (pi0) -91 90 0 243 244 0 0 2.885 2.319 -2.016 4.217 0.135 157 13 (mu-) -91 92 0 245 247 0 0 3.285 1.729 -4.346 5.716 0.106 158 -14 nu_mubar 91 92 0 0 0 0 0 0.526 0.253 -0.720 0.927 0.000 159 13 (mu-) -91 94 0 248 250 0 0 0.750 0.546 -0.722 1.181 0.106 160 -14 nu_mubar 91 94 0 0 0 0 0 0.114 0.046 -0.092 0.154 0.000 161 211 (pi+) -91 95 0 251 252 0 0 0.105 0.046 -0.155 0.238 0.140 162 111 (pi0) -91 95 0 253 254 0 0 0.564 0.224 -1.780 1.886 0.135 163 22 gamma 91 97 0 0 0 0 0 1.805 1.274 -4.537 5.046 0.000 164 22 gamma 91 97 0 0 0 0 0 2.419 1.837 -6.511 7.184 0.000 165 13 (mu-) -91 99 0 255 257 0 0 4.786 3.489 -11.798 13.201 0.106 166 -14 nu_mubar 91 99 0 0 0 0 0 0.930 0.679 -2.373 2.638 0.000 167 211 (pi+) -91 100 0 258 259 0 0 9.118 7.417 -23.416 26.201 0.140 168 -211 (pi-) -91 100 0 260 261 0 0 9.772 8.148 -25.123 28.162 0.140 169 111 (pi0) -91 100 0 262 263 0 0 9.496 7.623 -24.432 27.299 0.135 170 421 (D0) -91 110 0 264 266 0 0 -78.856 -38.089 81.930 119.937 1.865 171 22 gamma 91 110 0 0 0 0 0 -1.207 -0.676 1.256 1.869 0.000 172 13 (mu-) -91 112 0 267 269 0 0 -1.645 -0.695 1.526 2.352 0.106 173 -14 nu_mubar 91 112 0 0 0 0 0 -0.588 -0.287 0.580 0.874 0.000 174 211 (pi+) -91 117 0 270 271 0 0 -1.611 -0.958 2.337 2.999 0.140 175 -211 (pi-) -91 117 0 272 273 0 0 -0.667 -0.666 0.790 1.238 0.140 176 111 (pi0) -91 117 0 274 275 0 0 -1.474 -1.076 1.992 2.705 0.135 177 -13 (mu+) -91 119 0 276 278 0 0 -0.008 -0.216 0.239 0.339 0.106 178 14 nu_mu 91 119 0 0 0 0 0 -0.194 -4.046 5.162 6.562 0.000 179 -13 (mu+) -91 121 0 279 281 0 0 -0.030 -0.188 0.251 0.332 0.106 180 14 nu_mu 91 121 0 0 0 0 0 -0.042 -0.114 0.174 0.212 0.000 181 211 (pi+) -91 122 0 282 283 0 0 0.048 -5.176 6.098 8.000 0.140 182 -211 (pi-) -91 122 0 284 285 0 0 0.090 -7.888 9.321 12.212 0.140 183 111 (pi0) -91 122 0 286 287 0 0 0.114 -1.901 2.286 2.978 0.135 184 -211 (pi-) -91 124 0 288 289 0 0 0.634 0.170 -0.542 0.862 0.140 185 -211 (pi-) -91 124 0 290 291 0 0 0.718 0.324 -0.596 0.998 0.140 186 211 (pi+) -91 124 0 292 293 0 0 0.573 0.341 -0.625 0.925 0.140 187 -13 (mu+) -91 125 0 294 296 0 0 0.207 -0.001 -0.074 0.244 0.106 188 14 nu_mu 91 125 0 0 0 0 0 0.022 -0.029 -0.002 0.037 0.000 189 -13 (mu+) -91 126 0 297 299 0 0 0.312 0.042 -0.366 0.494 0.106 190 14 nu_mu 91 126 0 0 0 0 0 0.019 0.013 -0.002 0.024 0.000 191 22 gamma 91 127 0 0 0 0 0 0.676 0.753 -0.660 1.208 0.000 192 22 gamma 91 127 0 0 0 0 0 0.159 0.112 -0.177 0.264 0.000 193 -211 (pi-) -91 128 0 300 301 0 0 0.866 0.886 -2.079 2.425 0.140 194 111 (pi0) -91 128 0 302 303 0 0 0.229 0.528 -1.372 1.494 0.135 195 -13 (mu+) -91 129 0 304 306 0 0 0.191 0.086 -0.216 0.319 0.106 196 14 nu_mu 91 129 0 0 0 0 0 0.152 0.064 -0.149 0.222 0.000 197 -13 (mu+) -91 130 0 307 309 0 0 1.146 1.454 -4.335 4.715 0.106 198 14 nu_mu 91 130 0 0 0 0 0 0.386 0.427 -1.341 1.459 0.000 199 13 (mu-) -91 131 0 310 312 0 0 3.198 2.521 -7.399 8.446 0.106 200 -14 nu_mubar 91 131 0 0 0 0 0 1.147 0.952 -2.681 3.067 0.000 201 -13 (mu+) -91 132 0 313 315 0 0 -5.002 -2.650 5.258 7.727 0.106 202 14 nu_mu 91 132 0 0 0 0 0 -1.250 -0.674 1.271 1.906 0.000 203 22 gamma 91 133 0 0 0 0 0 -6.129 -2.566 6.219 9.101 0.000 204 22 gamma 91 133 0 0 0 0 0 -2.927 -1.254 3.104 4.447 0.000 205 -13 (mu+) -91 134 0 316 318 0 0 -0.384 -0.126 0.527 0.672 0.106 206 14 nu_mu 91 134 0 0 0 0 0 -0.081 -0.043 0.175 0.197 0.000 207 13 (mu-) -91 135 0 319 321 0 0 -6.210 -2.757 5.677 8.855 0.106 208 -14 nu_mubar 91 135 0 0 0 0 0 -0.356 -0.168 0.304 0.497 0.000 209 -13 (mu+) -91 137 0 322 324 0 0 -2.820 -1.378 3.261 4.527 0.106 210 14 nu_mu 91 137 0 0 0 0 0 -0.235 -0.088 0.257 0.360 0.000 211 211 (pi+) -91 138 0 325 326 0 0 -6.226 -1.958 6.486 9.202 0.140 212 -211 (pi-) -91 138 0 327 328 0 0 -0.914 -0.390 0.929 1.367 0.140 213 -13 (mu+) -91 139 0 329 331 0 0 -0.582 -0.317 0.499 0.836 0.106 214 14 nu_mu 91 139 0 0 0 0 0 -0.175 -0.053 0.140 0.231 0.000 215 13 (mu-) -91 140 0 332 334 0 0 -0.557 -0.620 1.147 1.422 0.106 216 -14 nu_mubar 91 140 0 0 0 0 0 -0.067 -0.104 0.213 0.246 0.000 217 13 (mu-) -91 141 0 335 337 0 0 -0.097 -0.300 0.350 0.482 0.106 218 -14 nu_mubar 91 141 0 0 0 0 0 -0.040 -0.195 0.240 0.311 0.000 219 22 gamma 91 142 0 0 0 0 0 -0.628 -0.426 0.532 0.927 0.000 220 22 gamma 91 142 0 0 0 0 0 -0.592 -0.429 0.680 0.999 0.000 221 13 (mu-) -91 144 0 338 340 0 0 0.119 -1.290 1.508 1.991 0.106 222 -14 nu_mubar 91 144 0 0 0 0 0 0.046 -0.569 0.722 0.921 0.000 223 -13 (mu+) -91 145 0 341 343 0 0 0.633 -4.606 4.994 6.824 0.106 224 14 nu_mu 91 145 0 0 0 0 0 0.066 -0.441 0.442 0.628 0.000 225 13 (mu-) -91 146 0 344 346 0 0 0.138 -7.422 8.627 11.382 0.106 226 -14 nu_mubar 91 146 0 0 0 0 0 0.023 -1.287 1.548 2.013 0.000 227 211 (pi+) -91 147 0 347 348 0 0 -2.610 -1.004 2.495 3.750 0.140 228 -211 (pi-) -91 147 0 349 350 0 0 -2.859 -1.146 3.351 4.554 0.140 229 -14 nu_mubar 91 148 0 0 0 0 0 0.098 -0.464 0.719 0.861 0.000 230 13 (mu-) -91 148 0 351 353 0 0 0.118 -0.151 0.212 0.304 0.106 231 211 (pi+) -91 148 0 354 355 0 0 -0.007 -0.508 0.439 0.686 0.140 232 -12 nu_ebar 91 149 0 0 0 0 0 14.956 11.821 -9.857 21.461 0.000 233 11 e- 91 149 0 0 0 0 0 0.637 0.492 -0.401 0.900 0.001 234 14 nu_mu 91 149 0 0 0 0 0 5.457 4.325 -3.628 7.852 0.000 235 12 nu_e 91 151 0 0 0 0 0 2.995 2.189 -2.039 4.233 0.000 236 -11 e+ 91 151 0 0 0 0 0 2.112 1.539 -1.530 3.029 0.001 237 -14 nu_mubar 91 151 0 0 0 0 0 0.837 0.617 -0.584 1.192 0.000 238 -12 nu_ebar 91 153 0 0 0 0 0 8.343 6.442 -5.351 11.821 0.000 239 11 e- 91 153 0 0 0 0 0 9.055 6.910 -5.784 12.775 0.001 240 14 nu_mu 91 153 0 0 0 0 0 0.335 0.266 -0.206 0.475 0.000 241 -13 (mu+) -91 155 0 356 358 0 0 3.924 3.384 -3.256 6.121 0.106 242 14 nu_mu 91 155 0 0 0 0 0 1.329 1.187 -1.091 2.089 0.000 243 22 gamma 91 156 0 0 0 0 0 1.651 1.404 -1.213 2.483 0.000 244 22 gamma 91 156 0 0 0 0 0 1.234 0.915 -0.803 1.734 0.000 245 -12 nu_ebar 91 157 0 0 0 0 0 1.101 0.575 -1.473 1.926 0.000 246 11 e- 91 157 0 0 0 0 0 1.866 0.959 -2.414 3.198 0.001 247 14 nu_mu 91 157 0 0 0 0 0 0.317 0.196 -0.459 0.591 0.000 248 -12 nu_ebar 91 159 0 0 0 0 0 0.356 0.276 -0.363 0.578 0.000 249 11 e- 91 159 0 0 0 0 0 0.081 0.029 -0.086 0.122 0.001 250 14 nu_mu 91 159 0 0 0 0 0 0.313 0.241 -0.274 0.481 0.000 251 -13 (mu+) -91 161 0 359 361 0 0 0.084 0.017 -0.088 0.162 0.106 252 14 nu_mu 91 161 0 0 0 0 0 0.021 0.029 -0.067 0.076 0.000 253 22 gamma 91 162 0 0 0 0 0 0.043 0.046 -0.294 0.301 0.000 254 22 gamma 91 162 0 0 0 0 0 0.522 0.179 -1.486 1.585 0.000 255 -12 nu_ebar 91 165 0 0 0 0 0 0.700 0.500 -1.646 1.857 0.000 256 11 e- 91 165 0 0 0 0 0 2.318 1.689 -5.807 6.476 0.001 257 14 nu_mu 91 165 0 0 0 0 0 1.768 1.301 -4.345 4.868 0.000 258 -13 (mu+) -91 167 0 362 364 0 0 8.092 6.616 -20.819 23.296 0.106 259 14 nu_mu 91 167 0 0 0 0 0 1.027 0.801 -2.597 2.905 0.000 260 13 (mu-) -91 168 0 365 367 0 0 9.146 7.600 -23.498 26.336 0.106 261 -14 nu_mubar 91 168 0 0 0 0 0 0.626 0.548 -1.625 1.826 0.000 262 22 gamma 91 169 0 0 0 0 0 0.397 0.296 -0.950 1.071 0.000 263 22 gamma 91 169 0 0 0 0 0 9.099 7.327 -23.482 26.227 0.000 264 310 (K_S0) -91 170 0 368 369 0 0 -42.992 -20.174 44.702 65.221 0.498 265 211 (pi+) -91 170 0 370 371 0 0 -1.952 -0.860 2.119 3.010 0.140 266 -211 (pi-) -91 170 0 372 373 0 0 -33.911 -17.055 35.109 51.706 0.140 267 -12 nu_ebar 91 172 0 0 0 0 0 -0.371 -0.135 0.313 0.504 0.000 268 11 e- 91 172 0 0 0 0 0 -0.670 -0.315 0.603 0.954 0.001 269 14 nu_mu 91 172 0 0 0 0 0 -0.605 -0.244 0.610 0.893 0.000 270 -13 (mu+) -91 174 0 374 376 0 0 -1.603 -0.955 2.334 2.991 0.106 271 14 nu_mu 91 174 0 0 0 0 0 -0.008 -0.003 0.003 0.009 0.000 272 13 (mu-) -91 175 0 377 379 0 0 -0.474 -0.471 0.525 0.857 0.106 273 -14 nu_mubar 91 175 0 0 0 0 0 -0.193 -0.195 0.264 0.381 0.000 274 22 gamma 91 176 0 0 0 0 0 -0.721 -0.451 0.968 1.289 0.000 275 22 gamma 91 176 0 0 0 0 0 -0.752 -0.625 1.025 1.417 0.000 276 12 nu_e 91 177 0 0 0 0 0 -0.019 -0.128 0.125 0.180 0.000 277 -11 e+ 91 177 0 0 0 0 0 -0.003 -0.091 0.075 0.118 0.001 278 -14 nu_mubar 91 177 0 0 0 0 0 0.014 0.002 0.039 0.042 0.000 279 12 nu_e 91 179 0 0 0 0 0 0.017 -0.056 0.075 0.095 0.000 280 -11 e+ 91 179 0 0 0 0 0 -0.001 -0.063 0.031 0.070 0.001 281 -14 nu_mubar 91 179 0 0 0 0 0 -0.046 -0.070 0.145 0.168 0.000 282 -13 (mu+) -91 181 0 380 382 0 0 0.061 -4.559 5.400 7.068 0.106 283 14 nu_mu 91 181 0 0 0 0 0 -0.013 -0.617 0.698 0.932 0.000 284 13 (mu-) -91 182 0 383 385 0 0 0.071 -7.471 8.850 11.582 0.106 285 -14 nu_mubar 91 182 0 0 0 0 0 0.019 -0.417 0.471 0.629 0.000 286 22 gamma 91 183 0 0 0 0 0 0.113 -0.893 1.029 1.367 0.000 287 22 gamma 91 183 0 0 0 0 0 0.001 -1.008 1.257 1.611 0.000 288 13 (mu-) -91 184 0 386 388 0 0 0.455 0.149 -0.412 0.640 0.106 289 -14 nu_mubar 91 184 0 0 0 0 0 0.179 0.021 -0.130 0.222 0.000 290 13 (mu-) -91 185 0 389 391 0 0 0.594 0.268 -0.455 0.802 0.106 291 -14 nu_mubar 91 185 0 0 0 0 0 0.125 0.056 -0.141 0.196 0.000 292 -13 (mu+) -91 186 0 392 394 0 0 0.544 0.297 -0.576 0.853 0.106 293 14 nu_mu 91 186 0 0 0 0 0 0.029 0.044 -0.049 0.072 0.000 294 12 nu_e 91 187 0 0 0 0 0 0.005 -0.010 -0.032 0.034 0.000 295 -11 e+ 91 187 0 0 0 0 0 0.112 -0.016 -0.024 0.116 0.001 296 -14 nu_mubar 91 187 0 0 0 0 0 0.090 0.025 -0.018 0.095 0.000 297 12 nu_e 91 189 0 0 0 0 0 0.069 -0.015 -0.128 0.146 0.000 298 -11 e+ 91 189 0 0 0 0 0 0.004 -0.001 -0.016 0.017 0.001 299 -14 nu_mubar 91 189 0 0 0 0 0 0.239 0.058 -0.222 0.331 0.000 300 13 (mu-) -91 193 0 395 397 0 0 0.631 0.606 -1.471 1.714 0.106 301 -14 nu_mubar 91 193 0 0 0 0 0 0.236 0.280 -0.609 0.710 0.000 302 22 gamma 91 194 0 0 0 0 0 0.240 0.491 -1.215 1.332 0.000 303 22 gamma 91 194 0 0 0 0 0 -0.011 0.037 -0.157 0.162 0.000 304 12 nu_e 91 195 0 0 0 0 0 0.061 0.059 -0.095 0.128 0.000 305 -11 e+ 91 195 0 0 0 0 0 0.004 -0.004 -0.036 0.036 0.001 306 -14 nu_mubar 91 195 0 0 0 0 0 0.126 0.032 -0.085 0.156 0.000 307 12 nu_e 91 197 0 0 0 0 0 0.179 0.241 -0.778 0.834 0.000 308 -11 e+ 91 197 0 0 0 0 0 0.964 1.212 -3.542 3.866 0.001 309 -14 nu_mubar 91 197 0 0 0 0 0 0.004 0.001 -0.015 0.016 0.000 310 -12 nu_ebar 91 199 0 0 0 0 0 1.991 1.586 -4.657 5.308 0.000 311 11 e- 91 199 0 0 0 0 0 0.736 0.607 -1.708 1.956 0.001 312 14 nu_mu 91 199 0 0 0 0 0 0.470 0.329 -1.034 1.182 0.000 313 12 nu_e 91 201 0 0 0 0 0 -1.280 -0.694 1.312 1.960 0.000 314 -11 e+ 91 201 0 0 0 0 0 -3.632 -1.898 3.841 5.617 0.001 315 -14 nu_mubar 91 201 0 0 0 0 0 -0.090 -0.058 0.105 0.149 0.000 316 12 nu_e 91 205 0 0 0 0 0 0.000 -0.002 0.028 0.028 0.000 317 -11 e+ 91 205 0 0 0 0 0 -0.016 -0.003 0.044 0.046 0.001 318 -14 nu_mubar 91 205 0 0 0 0 0 -0.368 -0.120 0.455 0.598 0.000 319 -12 nu_ebar 91 207 0 0 0 0 0 -0.532 -0.238 0.488 0.760 0.000 320 11 e- 91 207 0 0 0 0 0 -0.236 -0.108 0.192 0.323 0.001 321 14 nu_mu 91 207 0 0 0 0 0 -5.441 -2.411 4.998 7.772 0.000 322 12 nu_e 91 209 0 0 0 0 0 -0.251 -0.119 0.258 0.379 0.000 323 -11 e+ 91 209 0 0 0 0 0 -2.158 -1.070 2.495 3.468 0.001 324 -14 nu_mubar 91 209 0 0 0 0 0 -0.411 -0.189 0.507 0.680 0.000 325 -13 (mu+) -91 211 0 398 400 0 0 -4.665 -1.437 4.861 6.890 0.106 326 14 nu_mu 91 211 0 0 0 0 0 -1.561 -0.521 1.625 2.313 0.000 327 13 (mu-) -91 212 0 401 403 0 0 -0.759 -0.324 0.811 1.162 0.106 328 -14 nu_mubar 91 212 0 0 0 0 0 -0.154 -0.066 0.118 0.205 0.000 329 12 nu_e 91 213 0 0 0 0 0 -0.160 -0.040 0.102 0.194 0.000 330 -11 e+ 91 213 0 0 0 0 0 -0.356 -0.239 0.332 0.542 0.001 331 -14 nu_mubar 91 213 0 0 0 0 0 -0.066 -0.038 0.065 0.100 0.000 332 -12 nu_ebar 91 215 0 0 0 0 0 -0.027 -0.059 0.078 0.102 0.000 333 11 e- 91 215 0 0 0 0 0 -0.138 -0.172 0.264 0.345 0.001 334 14 nu_mu 91 215 0 0 0 0 0 -0.392 -0.388 0.805 0.976 0.000 335 -12 nu_ebar 91 217 0 0 0 0 0 -0.011 -0.006 0.003 0.013 0.000 336 11 e- 91 217 0 0 0 0 0 -0.074 -0.292 0.344 0.458 0.001 337 14 nu_mu 91 217 0 0 0 0 0 -0.012 -0.002 0.002 0.012 0.000 338 -12 nu_ebar 91 221 0 0 0 0 0 0.089 -0.692 0.865 1.111 0.000 339 11 e- 91 221 0 0 0 0 0 -0.001 -0.005 0.002 0.005 0.001 340 14 nu_mu 91 221 0 0 0 0 0 0.031 -0.593 0.641 0.874 0.000 341 12 nu_e 91 223 0 0 0 0 0 0.075 -0.432 0.456 0.633 0.000 342 -11 e+ 91 223 0 0 0 0 0 0.085 -0.765 0.791 1.103 0.001 343 -14 nu_mubar 91 223 0 0 0 0 0 0.472 -3.409 3.747 5.088 0.000 344 -12 nu_ebar 91 225 0 0 0 0 0 -0.011 -0.581 0.658 0.877 0.000 345 11 e- 91 225 0 0 0 0 0 0.032 -1.984 2.282 3.024 0.001 346 14 nu_mu 91 225 0 0 0 0 0 0.118 -4.857 5.687 7.480 0.000 347 -13 (mu+) -91 227 0 404 406 0 0 -2.068 -0.767 1.984 2.968 0.106 348 14 nu_mu 91 227 0 0 0 0 0 -0.542 -0.238 0.511 0.782 0.000 349 13 (mu-) -91 228 0 407 409 0 0 -2.478 -0.996 2.864 3.917 0.106 350 -14 nu_mubar 91 228 0 0 0 0 0 -0.381 -0.150 0.487 0.636 0.000 351 -12 nu_ebar 91 230 0 0 0 0 0 0.037 0.008 0.041 0.056 0.000 352 11 e- 91 230 0 0 0 0 0 0.071 -0.110 0.126 0.182 0.001 353 14 nu_mu 91 230 0 0 0 0 0 0.010 -0.048 0.044 0.066 0.000 354 -13 (mu+) -91 231 0 410 412 0 0 -0.016 -0.466 0.427 0.641 0.106 355 14 nu_mu 91 231 0 0 0 0 0 0.009 -0.042 0.012 0.045 0.000 356 12 nu_e 91 241 0 0 0 0 0 0.538 0.488 -0.487 0.874 0.000 357 -11 e+ 91 241 0 0 0 0 0 0.751 0.648 -0.640 1.181 0.001 358 -14 nu_mubar 91 241 0 0 0 0 0 2.635 2.248 -2.129 4.066 0.000 359 12 nu_e 91 251 0 0 0 0 0 0.065 0.013 -0.045 0.080 0.000 360 -11 e+ 91 251 0 0 0 0 0 0.021 0.010 0.012 0.026 0.001 361 -14 nu_mubar 91 251 0 0 0 0 0 -0.002 -0.006 -0.055 0.056 0.000 362 12 nu_e 91 258 0 0 0 0 0 1.639 1.311 -4.139 4.641 0.000 363 -11 e+ 91 258 0 0 0 0 0 5.721 4.722 -14.780 16.537 0.001 364 -14 nu_mubar 91 258 0 0 0 0 0 0.732 0.582 -1.901 2.118 0.000 365 -12 nu_ebar 91 260 0 0 0 0 0 3.054 2.543 -7.930 8.870 0.000 366 11 e- 91 260 0 0 0 0 0 1.052 0.904 -2.724 3.057 0.001 367 14 nu_mu 91 260 0 0 0 0 0 5.039 4.152 -12.844 14.409 0.000 368 211 (pi+) -91 264 0 413 414 0 0 -38.520 -18.100 40.136 58.500 0.140 369 -211 (pi-) -91 264 0 415 416 0 0 -4.472 -2.074 4.566 6.721 0.140 370 -13 (mu+) -91 265 0 417 419 0 0 -1.271 -0.575 1.360 1.952 0.106 371 14 nu_mu 91 265 0 0 0 0 0 -0.681 -0.285 0.759 1.059 0.000 372 13 (mu-) -91 266 0 420 422 0 0 -28.034 -14.081 29.051 42.757 0.106 373 -14 nu_mubar 91 266 0 0 0 0 0 -5.877 -2.973 6.058 8.949 0.000 374 12 nu_e 91 270 0 0 0 0 0 -0.895 -0.552 1.299 1.671 0.000 375 -11 e+ 91 270 0 0 0 0 0 0.000 -0.004 0.003 0.005 0.001 376 -14 nu_mubar 91 270 0 0 0 0 0 -0.709 -0.399 1.032 1.314 0.000 377 -12 nu_ebar 91 272 0 0 0 0 0 -0.093 -0.072 0.067 0.136 0.000 378 11 e- 91 272 0 0 0 0 0 -0.150 -0.160 0.135 0.258 0.001 379 14 nu_mu 91 272 0 0 0 0 0 -0.232 -0.239 0.323 0.464 0.000 380 12 nu_e 91 282 0 0 0 0 0 0.053 -2.532 3.009 3.932 0.000 381 -11 e+ 91 282 0 0 0 0 0 0.034 -1.560 1.838 2.411 0.001 382 -14 nu_mubar 91 282 0 0 0 0 0 -0.025 -0.468 0.552 0.724 0.000 383 -12 nu_ebar 91 284 0 0 0 0 0 0.045 -2.731 3.186 4.196 0.000 384 11 e- 91 284 0 0 0 0 0 0.041 -3.200 3.802 4.969 0.001 385 14 nu_mu 91 284 0 0 0 0 0 -0.015 -1.540 1.862 2.417 0.000 386 -12 nu_ebar 91 288 0 0 0 0 0 0.082 0.001 -0.082 0.117 0.000 387 11 e- 91 288 0 0 0 0 0 0.189 0.055 -0.122 0.232 0.001 388 14 nu_mu 91 288 0 0 0 0 0 0.183 0.092 -0.207 0.292 0.000 389 -12 nu_ebar 91 290 0 0 0 0 0 0.136 0.032 -0.083 0.162 0.000 390 11 e- 91 290 0 0 0 0 0 0.211 0.123 -0.137 0.280 0.001 391 14 nu_mu 91 290 0 0 0 0 0 0.246 0.113 -0.235 0.359 0.000 392 12 nu_e 91 292 0 0 0 0 0 -0.003 0.004 -0.006 0.008 0.000 393 -11 e+ 91 292 0 0 0 0 0 0.049 0.010 -0.054 0.074 0.001 394 -14 nu_mubar 91 292 0 0 0 0 0 0.498 0.283 -0.516 0.771 0.000 395 -12 nu_ebar 91 300 0 0 0 0 0 0.034 0.066 -0.135 0.154 0.000 396 11 e- 91 300 0 0 0 0 0 0.386 0.316 -0.815 0.955 0.001 397 14 nu_mu 91 300 0 0 0 0 0 0.210 0.224 -0.521 0.605 0.000 398 12 nu_e 91 325 0 0 0 0 0 -1.257 -0.378 1.358 1.889 0.000 399 -11 e+ 91 325 0 0 0 0 0 -0.926 -0.276 0.979 1.375 0.001 400 -14 nu_mubar 91 325 0 0 0 0 0 -2.482 -0.783 2.524 3.625 0.000 401 -12 nu_ebar 91 327 0 0 0 0 0 -0.053 -0.006 0.036 0.064 0.000 402 11 e- 91 327 0 0 0 0 0 -0.551 -0.219 0.602 0.845 0.001 403 14 nu_mu 91 327 0 0 0 0 0 -0.156 -0.100 0.174 0.254 0.000 404 12 nu_e 91 347 0 0 0 0 0 -0.121 -0.042 0.098 0.161 0.000 405 -11 e+ 91 347 0 0 0 0 0 -0.027 -0.021 0.026 0.043 0.001 406 -14 nu_mubar 91 347 0 0 0 0 0 -1.920 -0.704 1.860 2.765 0.000 407 -12 nu_ebar 91 349 0 0 0 0 0 -0.670 -0.274 0.800 1.079 0.000 408 11 e- 91 349 0 0 0 0 0 -0.548 -0.208 0.567 0.816 0.001 409 14 nu_mu 91 349 0 0 0 0 0 -1.261 -0.514 1.496 2.023 0.000 410 12 nu_e 91 354 0 0 0 0 0 0.017 -0.012 0.010 0.023 0.000 411 -11 e+ 91 354 0 0 0 0 0 -0.025 -0.330 0.285 0.437 0.001 412 -14 nu_mubar 91 354 0 0 0 0 0 -0.008 -0.124 0.132 0.181 0.000 413 -13 (mu+) -91 368 0 423 425 0 0 -26.996 -12.688 28.092 40.975 0.106 414 14 nu_mu 91 368 0 0 0 0 0 -11.524 -5.412 12.043 17.525 0.000 415 13 (mu-) -91 369 0 426 428 0 0 -3.277 -1.552 3.359 4.944 0.106 416 -14 nu_mubar 91 369 0 0 0 0 0 -1.195 -0.523 1.207 1.777 0.000 417 12 nu_e 91 370 0 0 0 0 0 -0.256 -0.111 0.250 0.375 0.000 418 -11 e+ 91 370 0 0 0 0 0 -0.231 -0.066 0.236 0.336 0.001 419 -14 nu_mubar 91 370 0 0 0 0 0 -0.785 -0.397 0.875 1.240 0.000 420 -12 nu_ebar 91 372 0 0 0 0 0 -13.555 -6.768 14.010 20.636 0.000 421 11 e- 91 372 0 0 0 0 0 -11.302 -5.731 11.738 17.273 0.001 422 14 nu_mu 91 372 0 0 0 0 0 -3.177 -1.583 3.302 4.848 0.000 423 12 nu_e 91 413 0 0 0 0 0 -12.741 -6.021 13.247 19.340 0.000 424 -11 e+ 91 413 0 0 0 0 0 -5.024 -2.319 5.221 7.607 0.001 425 -14 nu_mubar 91 413 0 0 0 0 0 -9.231 -4.348 9.625 14.027 0.000 426 -12 nu_ebar 91 415 0 0 0 0 0 -2.334 -1.121 2.447 3.562 0.000 427 11 e- 91 415 0 0 0 0 0 -0.885 -0.404 0.845 1.289 0.001 428 14 nu_mu 91 415 0 0 0 0 0 -0.058 -0.027 0.067 0.092 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 -0.000 500.000 500.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- Pythia::next(): 100 events have been generated PYTHIA Warning in TimeShower::pTnext: negative dipole mass. Pythia::next(): 200 events have been generated PYTHIA Warning in TimeShower::findMEcorr: ME weight above PS one Pythia::next(): 300 events have been generated Pythia::next(): 400 events have been generated Pythia::next(): 500 events have been generated Pythia::next(): 600 events have been generated Pythia::next(): 700 events have been generated Pythia::next(): 800 events have been generated Pythia::next(): 900 events have been generated *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | GenericResonance 9001 | 1053 1000 1000 | 3.894e-01 4.871e-10 | | | | | | sum | 1053 1000 1000 | 3.894e-01 4.871e-10 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 3 Warning in TimeShower::findMEcorr: ME weight above PS one | | 2 Warning in TimeShower::pTnext: negative dipole mass. | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:02 energy spectrum of photons 2.90*10^ 4 X 2.80*10^ 4 X 2.70*10^ 4 X 2.60*10^ 4 X 2.50*10^ 4 X 2.40*10^ 4 X 2.30*10^ 4 X 2.20*10^ 4 X 2.10*10^ 4 X 2.00*10^ 4 X 1.90*10^ 4 X 1.80*10^ 4 X 1.70*10^ 4 X 1.60*10^ 4 X 1.50*10^ 4 X 1.40*10^ 4 X 1.30*10^ 4 X 1.20*10^ 4 X 1.10*10^ 4 X 1.00*10^ 4 X 0.90*10^ 4 X 0.80*10^ 4 X 0.70*10^ 4 X 0.60*10^ 4 X 0.50*10^ 4 X4 0.40*10^ 4 XX 0.30*10^ 4 XX 0.20*10^ 4 XX8 0.10*10^ 4 XXXX643221111 Contents *10^ 4 2000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 3 9411000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0480632111000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0400288870887543433232221211011010100010000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000000000000000000000000000000000111111111111111111111111111111111111111122222222222222222222 *10^ 1 0000111122223333444455556666777788889999000011112222333344445555666677778888999900001111222233334444 *10^ 0 0358035803580358035803580358035803580358035803580358035803580358035803580358035803580358035803580358 Entries = 38660 Mean = 3.4410e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 3.8660e+04 Rms = 7.9886e+00 Overflow = 0.0000e+00 High edge = 2.5000e+02 2013-09-20 16:02 energy spectrum of e+ and e- 3.12*10^ 4 8 3.00*10^ 4 X 2.88*10^ 4 X 2.76*10^ 4 X 2.64*10^ 4 X 2.52*10^ 4 X 2.40*10^ 4 X 2.28*10^ 4 X 2.16*10^ 4 X 2.04*10^ 4 X 1.92*10^ 4 X 1.80*10^ 4 X 1.68*10^ 4 X 1.56*10^ 4 X 1.44*10^ 4 X 1.32*10^ 4 X 1.20*10^ 4 X 1.08*10^ 4 X 0.96*10^ 4 X 0.84*10^ 4 X 0.72*10^ 4 X 0.60*10^ 4 X 0.48*10^ 4 X 0.36*10^ 4 X4 0.24*10^ 4 XX 0.12*10^ 4 XX95321111 Contents *10^ 4 3000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 3 0210000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 9815321110000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 4417228218544243322221211101111011001011010000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000000000000000000000000000000000111111111111111111111111111111111111111122222222222222222222 *10^ 1 0000111122223333444455556666777788889999000011112222333344445555666677778888999900001111222233334444 *10^ 0 0358035803580358035803580358035803580358035803580358035803580358035803580358035803580358035803580358 Entries = 37010 Mean = 2.9886e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 3.7010e+04 Rms = 9.1781e+00 Overflow = 0.0000e+00 High edge = 2.5000e+02 2013-09-20 16:02 energy spectrum of p and pbar 9.00*10^ 2 9 8.70*10^ 2 X 8.40*10^ 2 X 8.10*10^ 2 6X 7.80*10^ 2 XX 7.50*10^ 2 XX 7.20*10^ 2 XX 6.90*10^ 2 XX 6.60*10^ 2 XX 6.30*10^ 2 XX 6.00*10^ 2 XX 5.70*10^ 2 XX 5.40*10^ 2 XX 5.10*10^ 2 XX 4.80*10^ 2 XX9 4.50*10^ 2 XXX 4.20*10^ 2 XXX 3.90*10^ 2 XXX 3.60*10^ 2 XXX 3.30*10^ 2 XXX 3.00*10^ 2 XXX8 2.70*10^ 2 XXXX 2.40*10^ 2 XXXX 2.10*10^ 2 XXXX7 1.80*10^ 2 XXXXX 1.50*10^ 2 XXXXX7 1.20*10^ 2 XXXXXX62 0.90*10^ 2 XXXXXXXX2 0.60*10^ 2 XXXXXXXXX453 0.30*10^ 2 XXXXXXXXXXXXX9X7544332212121121 111 11 11 1 1 Contents *10^ 2 7842211000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 9979040964432232111000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 7675009553589602531987646262463142212211022021100121000100000000001000100000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000000000000000000000000000000000111111111111111111111111111111111111111122222222222222222222 *10^ 1 0000111122223333444455556666777788889999000011112222333344445555666677778888999900001111222233334444 *10^ 0 0358035803580358035803580358035803580358035803580358035803580358035803580358035803580358035803580358 Entries = 3440 Mean = 1.0111e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 3.4400e+03 Rms = 1.4563e+01 Overflow = 0.0000e+00 High edge = 2.5000e+02 2013-09-20 16:02 energy spectrum of neutrinos 9.00*10^ 4 5 8.70*10^ 4 X 8.40*10^ 4 X 8.10*10^ 4 X 7.80*10^ 4 X 7.50*10^ 4 X 7.20*10^ 4 X 6.90*10^ 4 X 6.60*10^ 4 X 6.30*10^ 4 X 6.00*10^ 4 X 5.70*10^ 4 X 5.40*10^ 4 X 5.10*10^ 4 X 4.80*10^ 4 X 4.50*10^ 4 X 4.20*10^ 4 X 3.90*10^ 4 X 3.60*10^ 4 X 3.30*10^ 4 X 3.00*10^ 4 X 2.70*10^ 4 X 2.40*10^ 4 X 2.10*10^ 4 X 1.80*10^ 4 X 1.50*10^ 4 X 1.20*10^ 4 X 0.90*10^ 4 X5 0.60*10^ 4 XX 0.30*10^ 4 XXX5321111 Contents *10^ 4 8000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 3 8721000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 4585963322111000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0661108440432977554444332224323221222211221111111111111111111011101111101011011000001000000000000000 Low edge *10^ 2 0000000000000000000000000000000000000000111111111111111111111111111111111111111122222222222222222222 *10^ 1 0000111122223333444455556666777788889999000011112222333344445555666677778888999900001111222233334444 *10^ 0 0358035803580358035803580358035803580358035803580358035803580358035803580358035803580358035803580358 Entries = 104636 Mean = 3.1320e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0464e+05 Rms = 1.0935e+01 Overflow = 0.0000e+00 High edge = 2.5000e+02 pythia8-8.1.80.orig/examples/outref/out240000644000175000017500000034537412217346175016403 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:07:11 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *----------------------- SusyLesHouches SUSY/BSM Interface ------------------------* | Last Change 01 Aug 2012 - P. Skands | Parsing: cmssm.spc *------------------------------------------------------------------------------------* | | Spectrum Calculator was: SOFTSUSY version: 3.3.0 | Read SLHA spectrum from: cmssm.spc | | ~g m | 1000021 1146.878 | | ~d m ~dL ~sL ~bL ~dR ~sR ~bR | 1000001 1055.611 1.000 0.000 0.000 0.000 0.000 0.000 | 1000003 1055.608 0.000 1.000 0.000 0.000 0.000 0.000 | 1000005 965.462 0.000 0.000 0.976 0.000 0.000 0.218 | 2000001 1011.023 0.000 0.000 0.000 1.000 0.000 0.000 | 2000003 1011.020 0.000 0.000 0.000 0.000 1.000 0.000 | 2000005 1007.759 0.000 0.000 -0.218 0.000 0.000 0.976 | | ~u m ~uL ~cL ~tL ~uR ~cR ~tR | 1000002 1052.787 1.000 0.000 0.000 0.000 0.000 0.000 | 1000004 1052.784 0.000 1.000 0.000 0.000 0.000 0.000 | 1000006 803.541 0.000 0.000 0.425 0.000 0.000 0.905 | 2000002 1014.342 0.000 0.000 0.000 1.000 0.000 0.000 | 2000004 1014.340 0.000 0.000 0.000 0.000 1.000 0.000 | 2000006 1011.028 0.000 0.000 0.905 0.000 0.000 -0.425 | | ~e m ~eL ~muL ~tauL ~eR ~muR ~tauR | 1000011 361.778 1.000 0.000 0.000 0.000 0.000 0.000 | 1000013 361.862 0.000 1.000 0.000 0.000 0.000 0.000 | 1000015 222.692 0.000 0.000 0.143 0.000 0.000 0.990 | 2000011 229.875 0.000 0.000 0.000 1.000 0.000 0.000 | 2000013 229.864 0.000 0.000 0.000 0.000 1.000 0.000 | 2000015 362.940 0.000 0.000 0.990 0.000 0.000 -0.143 | | ~nu m ~nu_e ~nu_mu ~nu_tau | 1000012 352.903 1.000 0.000 0.000 | 1000014 352.900 0.000 1.000 0.000 | 1000016 351.731 0.000 0.000 1.000 | | ~chi0 m ~B ~W_3 ~H_1 ~H_2 | 1000022 204.168 0.996 -0.017 0.082 -0.034 | 1000023 386.197 0.037 0.971 -0.196 0.130 | 1000025 -639.639 -0.033 0.048 0.703 0.708 | 1000035 653.033 -0.076 0.232 0.678 -0.693 | | ~chi+ m U: ~W ~H | V: ~W ~H | 1000024 386.332 0.961 -0.277 | 0.983 -0.186 | 1000037 652.680 0.277 0.961 | 0.186 0.983 | | Higgs | alpha -0.107 | mu 634.226 (DRbar running value at Q = 873.811 GeV) | tan(beta) 9.669 (DRbar running value at Q = 873.811 GeV) | v 244.044 (DRbar running value at Q = 873.811 GeV) | mA 5.400e+05 (DRbar running value at Q = 873.811 GeV) | | Gauge | g' 0.362 (DRbar running value at Q = 873.811 GeV) | g 0.643 (DRbar running value at Q = 873.811 GeV) | g3 1.061 (DRbar running value at Q = 873.811 GeV) | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.000e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> gluino gluino 1201 | 6.686e-11 | | q qbar -> gluino gluino 1202 | 8.648e-12 | | q g -> ~d_L gluino + c.c. 1203 | 9.987e-11 | | q g -> ~u_L gluino + c.c. 1204 | 2.532e-10 | | q g -> ~s_L gluino + c.c. 1205 | 5.542e-12 | | q g -> ~c_L gluino + c.c. 1206 | 4.809e-12 | | q g -> ~b_1 gluino + c.c. 1207 | 1.847e-12 | | q g -> ~t_1 gluino + c.c. 1208 | 0.000e+00 | | q g -> ~d_R gluino + c.c. 1209 | 1.152e-10 | | q g -> ~u_R gluino + c.c. 1210 | 2.847e-10 | | q g -> ~s_R gluino + c.c. 1211 | 6.152e-12 | | q g -> ~c_R gluino + c.c. 1212 | 5.453e-12 | | q g -> ~b_2 gluino + c.c. 1213 | 1.691e-12 | | q g -> ~t_2 gluino + c.c. 1214 | 0.000e+00 | | g g -> ~d_L ~d_Lbar 1215 | 3.904e-12 | | g g -> ~u_L ~u_Lbar 1216 | 3.966e-12 | | g g -> ~s_L ~s_Lbar 1217 | 3.904e-12 | | g g -> ~c_L ~c_Lbar 1218 | 3.966e-12 | | g g -> ~b_1 ~b_1bar 1219 | 7.970e-12 | | g g -> ~t_1 ~t_1bar 1220 | 3.448e-11 | | g g -> ~d_R ~d_Rbar 1221 | 5.208e-12 | | g g -> ~u_R ~u_Rbar 1222 | 5.067e-12 | | g g -> ~s_R ~s_Rbar 1223 | 5.208e-12 | | g g -> ~c_R ~c_Rbar 1224 | 5.067e-12 | | g g -> ~b_2 ~b_2bar 1225 | 5.351e-12 | | g g -> ~t_2 ~t_2bar 1226 | 5.208e-12 | | q qbar' -> ~d_L ~d_Lbar 1231 | 5.535e-12 | | q qbar' -> ~d_L ~s_Lbar 1232 | 1.202e-12 | | q qbar' -> ~s_L ~d_Lbar 1233 | 1.269e-13 | | q qbar' -> ~d_L ~b_1bar 1234 | 4.254e-13 | | q qbar' -> ~b_1 ~d_Lbar 1235 | 4.958e-14 | | q qbar' -> ~d_L ~d_Rbar 1236 | 1.183e-11 | | q qbar' -> ~d_R ~d_Lbar 1237 | 1.183e-11 | | q qbar' -> ~d_L ~s_Rbar 1238 | 5.439e-12 | | q qbar' -> ~s_R ~d_Lbar 1239 | 7.506e-13 | | q qbar' -> ~d_L ~b_2bar 1240 | 1.353e-12 | | q qbar' -> ~b_2 ~d_Lbar 1241 | 1.863e-13 | | q qbar' -> ~u_L ~u_Lbar 1242 | 8.272e-12 | | q qbar' -> ~u_L ~c_Lbar 1243 | 1.276e-12 | | q qbar' -> ~c_L ~u_Lbar 1244 | 3.840e-14 | | q qbar' -> ~u_L ~t_1bar 1245 | 0.000e+00 | | q qbar' -> ~t_1 ~u_Lbar 1246 | 0.000e+00 | | q qbar' -> ~u_L ~u_Rbar 1247 | 1.957e-11 | | q qbar' -> ~u_R ~u_Lbar 1248 | 1.957e-11 | | q qbar' -> ~u_L ~c_Rbar 1249 | 5.675e-12 | | q qbar' -> ~c_R ~u_Lbar 1250 | 2.094e-13 | | q qbar' -> ~u_L ~t_2bar 1251 | 0.000e+00 | | q qbar' -> ~t_2 ~u_Lbar 1252 | 0.000e+00 | | q qbar' -> ~u_L ~d_Lbar + c.c. 1253 | 6.631e-12 | | q qbar' -> ~u_L ~s_Lbar + c.c. 1254 | 3.144e-12 | | q qbar' -> ~u_L ~b_1bar + c.c. 1255 | 1.133e-12 | | q qbar' -> ~u_L ~d_Rbar + c.c. 1256 | 3.640e-11 | | q qbar' -> ~u_L ~s_Rbar + c.c. 1257 | 1.337e-11 | | q qbar' -> ~u_L ~b_2bar + c.c. 1258 | 3.506e-12 | | q qbar' -> ~s_L ~s_Lbar 1259 | 3.172e-12 | | q qbar' -> ~s_L ~b_1bar 1260 | 2.275e-14 | | q qbar' -> ~b_1 ~s_Lbar 1261 | 2.275e-14 | | q qbar' -> ~s_L ~d_Rbar 1262 | 7.506e-13 | | q qbar' -> ~d_R ~s_Lbar 1263 | 5.434e-12 | | q qbar' -> ~s_L ~s_Rbar 1264 | 3.433e-13 | | q qbar' -> ~s_R ~s_Lbar 1265 | 3.433e-13 | | q qbar' -> ~s_L ~b_2bar 1266 | 8.524e-14 | | q qbar' -> ~b_2 ~s_Lbar 1267 | 8.524e-14 | | q qbar' -> ~c_L ~c_Lbar 1268 | 3.230e-12 | | q qbar' -> ~c_L ~t_1bar 1269 | 0.000e+00 | | q qbar' -> ~t_1 ~c_Lbar 1270 | 0.000e+00 | | q qbar' -> ~c_L ~u_Rbar 1271 | 2.094e-13 | | q qbar' -> ~u_R ~c_Lbar 1272 | 5.675e-12 | | q qbar' -> ~c_L ~c_Rbar 1273 | 6.322e-14 | | q qbar' -> ~c_R ~c_Lbar 1274 | 6.322e-14 | | q qbar' -> ~c_L ~t_2bar 1275 | 0.000e+00 | | q qbar' -> ~t_2 ~c_Lbar 1276 | 0.000e+00 | | q qbar' -> ~c_L ~d_Lbar + c.c. 1277 | 5.431e-13 | | q qbar' -> ~c_L ~s_Lbar + c.c. 1278 | 2.458e-13 | | q qbar' -> ~c_L ~b_1bar + c.c. 1279 | 1.950e-14 | | q qbar' -> ~c_L ~d_Rbar + c.c. 1280 | 2.688e-12 | | q qbar' -> ~c_L ~s_Rbar + c.c. 1281 | 2.980e-13 | | q qbar' -> ~c_L ~b_2bar + c.c. 1282 | 7.446e-14 | | q qbar' -> ~b_1 ~b_1bar 1283 | 6.031e-12 | | q qbar' -> ~b_1 ~d_Rbar 1284 | 2.707e-13 | | q qbar' -> ~d_R ~b_1bar 1285 | 1.848e-12 | | q qbar' -> ~b_1 ~s_Rbar 1286 | 1.238e-13 | | q qbar' -> ~s_R ~b_1bar 1287 | 1.238e-13 | | q qbar' -> ~b_1 ~b_2bar 1288 | 3.186e-14 | | q qbar' -> ~b_2 ~b_1bar 1289 | 3.186e-14 | | q qbar' -> ~t_1 ~t_1bar 1290 | 2.071e-11 | | q qbar' -> ~t_1 ~u_Rbar 1291 | 0.000e+00 | | q qbar' -> ~u_R ~t_1bar 1292 | 0.000e+00 | | q qbar' -> ~t_1 ~c_Rbar 1293 | 0.000e+00 | | q qbar' -> ~c_R ~t_1bar 1294 | 0.000e+00 | | q qbar' -> ~t_1 ~t_2bar 1295 | 2.488e-14 | | q qbar' -> ~t_2 ~t_1bar 1296 | 2.488e-14 | | q qbar' -> ~t_1 ~d_Lbar + c.c. 1297 | 6.914e-18 | | q qbar' -> ~t_1 ~s_Lbar + c.c. 1298 | 1.807e-16 | | q qbar' -> ~t_1 ~b_1bar + c.c. 1299 | 1.391e-13 | | q qbar' -> ~t_1 ~d_Rbar + c.c. 1300 | 0.000e+00 | | q qbar' -> ~t_1 ~s_Rbar + c.c. 1301 | 0.000e+00 | | q qbar' -> ~t_1 ~b_2bar + c.c. 1302 | 5.923e-15 | | q qbar' -> ~d_R ~d_Rbar 1303 | 7.954e-12 | | q qbar' -> ~d_R ~s_Rbar 1304 | 1.579e-12 | | q qbar' -> ~s_R ~d_Rbar 1305 | 1.767e-13 | | q qbar' -> ~d_R ~b_2bar 1306 | 4.273e-13 | | q qbar' -> ~b_2 ~d_Rbar 1307 | 4.985e-14 | | q qbar' -> ~u_R ~u_Rbar 1308 | 1.081e-11 | | q qbar' -> ~u_R ~c_Rbar 1309 | 1.614e-12 | | q qbar' -> ~c_R ~u_Rbar 1310 | 4.900e-14 | | q qbar' -> ~u_R ~t_2bar 1311 | 0.000e+00 | | q qbar' -> ~t_2 ~u_Rbar 1312 | 0.000e+00 | | q qbar' -> ~u_R ~d_Lbar + c.c. 1313 | 3.568e-11 | | q qbar' -> ~u_R ~s_Lbar + c.c. 1314 | 1.310e-11 | | q qbar' -> ~u_R ~b_1bar + c.c. 1315 | 4.656e-12 | | q qbar' -> ~u_R ~d_Rbar + c.c. 1316 | 1.096e-11 | | q qbar' -> ~u_R ~s_Rbar + c.c. 1317 | 4.050e-12 | | q qbar' -> ~u_R ~b_2bar + c.c. 1318 | 1.116e-12 | | q qbar' -> ~s_R ~s_Rbar 1319 | 4.367e-12 | | q qbar' -> ~s_R ~b_2bar 1320 | 2.288e-14 | | q qbar' -> ~b_2 ~s_Rbar 1321 | 2.288e-14 | | q qbar' -> ~c_R ~c_Rbar 1322 | 4.195e-12 | | q qbar' -> ~c_R ~t_2bar 1323 | 0.000e+00 | | q qbar' -> ~t_2 ~c_Rbar 1324 | 0.000e+00 | | q qbar' -> ~c_R ~d_Lbar + c.c. 1325 | 2.629e-12 | | q qbar' -> ~c_R ~s_Lbar + c.c. 1326 | 2.905e-13 | | q qbar' -> ~c_R ~b_1bar + c.c. 1327 | 1.066e-13 | | q qbar' -> ~c_R ~d_Rbar + c.c. 1328 | 7.100e-13 | | q qbar' -> ~c_R ~s_Rbar + c.c. 1329 | 6.643e-14 | | q qbar' -> ~c_R ~b_2bar + c.c. 1330 | 1.885e-14 | | q qbar' -> ~b_2 ~b_2bar 1331 | 4.391e-12 | | q qbar' -> ~t_2 ~t_2bar 1332 | 4.335e-12 | | q qbar' -> ~t_2 ~d_Lbar + c.c. 1333 | 1.478e-17 | | q qbar' -> ~t_2 ~s_Lbar + c.c. 1334 | 3.863e-16 | | q qbar' -> ~t_2 ~b_1bar + c.c. 1335 | 2.939e-13 | | q qbar' -> ~t_2 ~d_Rbar + c.c. 1336 | 0.000e+00 | | q qbar' -> ~t_2 ~s_Rbar + c.c. 1337 | 0.000e+00 | | q qbar' -> ~t_2 ~b_2bar + c.c. 1338 | 1.256e-14 | | q q' -> ~d_L ~d_L + c.c. 1351 | 3.095e-11 | | q q' -> ~d_L ~s_L + c.c. 1352 | 5.091e-12 | | q q' -> ~d_L ~b_1 + c.c. 1353 | 1.750e-12 | | q q' -> ~d_L ~d_R + c.c. 1354 | 1.853e-11 | | q q' -> ~d_L ~s_R + c.c. 1355 | 1.117e-12 | | q q' -> ~d_L ~b_2 + c.c. 1356 | 3.196e-13 | | q q' -> ~u_L ~u_L + c.c. 1357 | 1.768e-10 | | q q' -> ~u_L ~c_L + c.c. 1358 | 5.593e-12 | | q q' -> ~u_L ~t_1 + c.c. 1359 | 0.000e+00 | | q q' -> ~u_L ~u_R + c.c. 1360 | 1.326e-10 | | q q' -> ~u_L ~c_R + c.c. 1361 | 1.320e-12 | | q q' -> ~u_L ~t_2 + c.c. 1362 | 0.000e+00 | | q q' -> ~u_L ~d_L + c.c. 1363 | 2.627e-10 | | q q' -> ~u_L ~s_L + c.c. 1364 | 1.227e-11 | | q q' -> ~u_L ~b_1 + c.c. 1365 | 1.448e-12 | | q q' -> ~u_L ~d_R + c.c. 1366 | 7.694e-11 | | q q' -> ~u_L ~s_R + c.c. 1367 | 3.637e-12 | | q q' -> ~u_L ~b_2 + c.c. 1368 | 3.140e-12 | | q q' -> ~s_L ~s_L + c.c. 1369 | 2.507e-13 | | q q' -> ~s_L ~b_1 + c.c. 1370 | 2.005e-13 | | q q' -> ~s_L ~d_R + c.c. 1371 | 1.117e-12 | | q q' -> ~s_L ~s_R + c.c. 1372 | 1.035e-13 | | q q' -> ~s_L ~b_2 + c.c. 1373 | 3.007e-14 | | q q' -> ~c_L ~c_L + c.c. 1374 | 4.725e-14 | | q q' -> ~c_L ~t_1 + c.c. 1375 | 0.000e+00 | | q q' -> ~c_L ~u_R + c.c. 1376 | 1.320e-12 | | q q' -> ~c_L ~c_R + c.c. 1377 | 1.883e-14 | | q q' -> ~c_L ~t_2 + c.c. 1378 | 0.000e+00 | | q q' -> ~c_L ~d_L + c.c. 1379 | 3.443e-12 | | q q' -> ~c_L ~s_L + c.c. 1380 | 4.460e-13 | | q q' -> ~c_L ~b_1 + c.c. 1381 | 2.704e-14 | | q q' -> ~c_L ~d_R + c.c. 1382 | 6.293e-13 | | q q' -> ~c_L ~s_R + c.c. 1383 | 5.762e-14 | | q q' -> ~c_L ~b_2 + c.c. 1384 | 6.626e-14 | | q q' -> ~b_1 ~b_1 + c.c. 1385 | 3.379e-14 | | q q' -> ~b_1 ~d_R + c.c. 1386 | 4.254e-13 | | q q' -> ~b_1 ~s_R + c.c. 1387 | 4.209e-14 | | q q' -> ~b_1 ~b_2 + c.c. 1388 | 1.120e-14 | | q q' -> ~t_1 ~t_1 + c.c. 1389 | 0.000e+00 | | q q' -> ~t_1 ~u_R + c.c. 1390 | 0.000e+00 | | q q' -> ~t_1 ~c_R + c.c. 1391 | 0.000e+00 | | q q' -> ~t_1 ~t_2 + c.c. 1392 | 0.000e+00 | | q q' -> ~t_1 ~d_L + c.c. 1393 | 5.210e-13 | | q q' -> ~t_1 ~s_L + c.c. 1394 | 3.952e-14 | | q q' -> ~t_1 ~b_1 + c.c. 1395 | 2.092e-16 | | q q' -> ~t_1 ~d_R + c.c. 1396 | 0.000e+00 | | q q' -> ~t_1 ~s_R + c.c. 1397 | 0.000e+00 | | q q' -> ~t_1 ~b_2 + c.c. 1398 | 8.814e-17 | | q q' -> ~d_R ~d_R + c.c. 1399 | 2.921e-11 | | q q' -> ~d_R ~s_R + c.c. 1400 | 6.828e-12 | | q q' -> ~d_R ~b_2 + c.c. 1401 | 1.726e-12 | | q q' -> ~u_R ~u_R + c.c. 1402 | 1.632e-10 | | q q' -> ~u_R ~c_R + c.c. 1403 | 7.168e-12 | | q q' -> ~u_R ~t_2 + c.c. 1404 | 0.000e+00 | | q q' -> ~u_R ~d_L + c.c. 1405 | 7.596e-11 | | q q' -> ~u_R ~s_L + c.c. 1406 | 3.565e-12 | | q q' -> ~u_R ~b_1 + c.c. 1407 | 4.093e-12 | | q q' -> ~u_R ~d_R + c.c. 1408 | 2.227e-10 | | q q' -> ~u_R ~s_R + c.c. 1409 | 1.511e-11 | | q q' -> ~u_R ~b_2 + c.c. 1410 | 1.422e-12 | | q q' -> ~s_R ~s_R + c.c. 1411 | 2.789e-13 | | q q' -> ~s_R ~b_2 + c.c. 1412 | 1.982e-13 | | q q' -> ~c_R ~c_R + c.c. 1413 | 5.488e-14 | | q q' -> ~c_R ~t_2 + c.c. 1414 | 0.000e+00 | | q q' -> ~c_R ~d_L + c.c. 1415 | 6.156e-13 | | q q' -> ~c_R ~s_L + c.c. 1416 | 5.616e-14 | | q q' -> ~c_R ~b_1 + c.c. 1417 | 9.308e-14 | | q q' -> ~c_R ~d_R + c.c. 1418 | 3.088e-12 | | q q' -> ~c_R ~s_R + c.c. 1419 | 3.507e-13 | | q q' -> ~c_R ~b_2 + c.c. 1420 | 2.650e-14 | | q q' -> ~b_2 ~b_2 + c.c. 1421 | 1.763e-14 | | q q' -> ~t_2 ~t_2 + c.c. 1422 | 0.000e+00 | | q q' -> ~t_2 ~d_L + c.c. 1423 | 9.649e-15 | | q q' -> ~t_2 ~s_L + c.c. 1424 | 6.991e-16 | | q q' -> ~t_2 ~b_1 + c.c. 1425 | 6.713e-18 | | q q' -> ~t_2 ~d_R + c.c. 1426 | 0.000e+00 | | q q' -> ~t_2 ~s_R + c.c. 1427 | 0.000e+00 | | q q' -> ~t_2 ~b_2 + c.c. 1428 | 4.185e-18 | | q g -> ~chi_10 ~d_L + c.c. (q=d,s,b) 1431 | 1.224e-12 | | q g -> ~chi_10 ~u_L + c.c. (q=u,c) 1432 | 1.921e-12 | | q g -> ~chi_10 ~s_L + c.c. (q=d,s,b) 1433 | 1.941e-13 | | q g -> ~chi_10 ~c_L + c.c. (q=u,c) 1434 | 6.698e-14 | | q g -> ~chi_10 ~b_1 + c.c. (q=d,s,b) 1435 | 1.212e-13 | | q g -> ~chi_10 ~t_1 + c.c. (q=u,c) 1436 | 0.000e+00 | | q g -> ~chi_10 ~d_R + c.c. (q=d,s,b) 1437 | 5.120e-12 | | q g -> ~chi_10 ~u_R + c.c. (q=u,c) 1438 | 4.477e-11 | | q g -> ~chi_10 ~s_R + c.c. (q=d,s,b) 1439 | 8.356e-13 | | q g -> ~chi_10 ~c_R + c.c. (q=u,c) 1440 | 1.632e-12 | | q g -> ~chi_10 ~b_2 + c.c. (q=d,s,b) 1441 | 2.295e-13 | | q g -> ~chi_10 ~t_2 + c.c. (q=u,c) 1442 | 0.000e+00 | | q g -> ~chi_20 ~d_L + c.c. (q=d,s,b) 1443 | 1.529e-11 | | q g -> ~chi_20 ~u_L + c.c. (q=u,c) 1444 | 3.445e-11 | | q g -> ~chi_20 ~s_L + c.c. (q=d,s,b) 1445 | 2.477e-12 | | q g -> ~chi_20 ~c_L + c.c. (q=u,c) 1446 | 1.238e-12 | | q g -> ~chi_20 ~b_1 + c.c. (q=d,s,b) 1447 | 1.144e-12 | | q g -> ~chi_20 ~t_1 + c.c. (q=u,c) 1448 | 0.000e+00 | | q g -> ~chi_20 ~d_R + c.c. (q=d,s,b) 1449 | 4.006e-15 | | q g -> ~chi_20 ~u_R + c.c. (q=u,c) 1450 | 3.384e-14 | | q g -> ~chi_20 ~s_R + c.c. (q=d,s,b) 1451 | 6.682e-16 | | q g -> ~chi_20 ~c_R + c.c. (q=u,c) 1452 | 1.267e-15 | | q g -> ~chi_20 ~b_2 + c.c. (q=d,s,b) 1453 | 2.381e-14 | | q g -> ~chi_20 ~t_2 + c.c. (q=u,c) 1454 | 0.000e+00 | | q g -> ~chi_30 ~d_L + c.c. (q=d,s,b) 1455 | 2.318e-14 | | q g -> ~chi_30 ~u_L + c.c. (q=u,c) 1456 | 2.919e-14 | | q g -> ~chi_30 ~s_L + c.c. (q=d,s,b) 1457 | 3.248e-15 | | q g -> ~chi_30 ~c_L + c.c. (q=u,c) 1458 | 8.947e-16 | | q g -> ~chi_30 ~b_1 + c.c. (q=d,s,b) 1459 | 1.950e-14 | | q g -> ~chi_30 ~t_1 + c.c. (q=u,c) 1460 | 0.000e+00 | | q g -> ~chi_30 ~d_R + c.c. (q=d,s,b) 1461 | 1.469e-15 | | q g -> ~chi_30 ~u_R + c.c. (q=u,c) 1462 | 1.202e-14 | | q g -> ~chi_30 ~s_R + c.c. (q=d,s,b) 1463 | 2.115e-16 | | q g -> ~chi_30 ~c_R + c.c. (q=u,c) 1464 | 3.829e-16 | | q g -> ~chi_30 ~b_2 + c.c. (q=d,s,b) 1465 | 1.913e-14 | | q g -> ~chi_30 ~t_2 + c.c. (q=u,c) 1466 | 0.000e+00 | | q g -> ~chi_40 ~d_L + c.c. (q=d,s,b) 1467 | 4.575e-13 | | q g -> ~chi_40 ~u_L + c.c. (q=u,c) 1468 | 7.574e-13 | | q g -> ~chi_40 ~s_L + c.c. (q=d,s,b) 1469 | 6.356e-14 | | q g -> ~chi_40 ~c_L + c.c. (q=u,c) 1470 | 2.296e-14 | | q g -> ~chi_40 ~b_1 + c.c. (q=d,s,b) 1471 | 3.417e-14 | | q g -> ~chi_40 ~t_1 + c.c. (q=u,c) 1472 | 0.000e+00 | | q g -> ~chi_40 ~d_R + c.c. (q=d,s,b) 1473 | 7.373e-15 | | q g -> ~chi_40 ~u_R + c.c. (q=u,c) 1474 | 6.033e-14 | | q g -> ~chi_40 ~s_R + c.c. (q=d,s,b) 1475 | 1.053e-15 | | q g -> ~chi_40 ~c_R + c.c. (q=u,c) 1476 | 1.901e-15 | | q g -> ~chi_40 ~b_2 + c.c. (q=d,s,b) 1477 | 2.470e-14 | | q g -> ~chi_40 ~t_2 + c.c. (q=u,c) 1478 | 0.000e+00 | | q g -> ~chi_1+ ~d_L + c.c. (q=u,c) 1491 | 1.641e-10 | | q g -> ~chi_1- ~u_L + c.c. (q=d,s,b) 1492 | 7.747e-11 | | q g -> ~chi_1+ ~s_L + c.c. (q=u,c) 1493 | 1.336e-11 | | q g -> ~chi_1- ~c_L + c.c. (q=d,s,b) 1494 | 1.601e-11 | | q g -> ~chi_1+ ~b_1 + c.c. (q=u,c) 1495 | 2.013e-14 | | q g -> ~chi_1- ~t_1 + c.c. (q=d,s,b) 1496 | 1.699e-11 | | q g -> ~chi_1+ ~d_R + c.c. (q=u,c) 1497 | 0.000e+00 | | q g -> ~chi_1- ~u_R + c.c. (q=d,s,b) 1498 | 0.000e+00 | | q g -> ~chi_1+ ~s_R + c.c. (q=u,c) 1499 | 0.000e+00 | | q g -> ~chi_1- ~c_R + c.c. (q=d,s,b) 1500 | 0.000e+00 | | q g -> ~chi_1+ ~b_2 + c.c. (q=u,c) 1501 | 4.107e-16 | | q g -> ~chi_1- ~t_2 + c.c. (q=d,s,b) 1502 | 1.342e-13 | | q g -> ~chi_2+ ~d_L + c.c. (q=u,c) 1503 | 6.029e-12 | | q g -> ~chi_2- ~u_L + c.c. (q=d,s,b) 1504 | 2.940e-12 | | q g -> ~chi_2+ ~s_L + c.c. (q=u,c) 1505 | 4.897e-13 | | q g -> ~chi_2- ~c_L + c.c. (q=d,s,b) 1506 | 5.471e-13 | | q g -> ~chi_2+ ~b_1 + c.c. (q=u,c) 1507 | 4.155e-16 | | q g -> ~chi_2- ~t_1 + c.c. (q=d,s,b) 1508 | 1.021e-11 | | q g -> ~chi_2+ ~d_R + c.c. (q=u,c) 1509 | 0.000e+00 | | q g -> ~chi_2- ~u_R + c.c. (q=d,s,b) 1510 | 0.000e+00 | | q g -> ~chi_2+ ~s_R + c.c. (q=u,c) 1511 | 0.000e+00 | | q g -> ~chi_2- ~c_R + c.c. (q=d,s,b) 1512 | 0.000e+00 | | q g -> ~chi_2+ ~b_2 + c.c. (q=u,c) 1513 | 4.349e-16 | | q g -> ~chi_2- ~t_2 + c.c. (q=d,s,b) 1514 | 2.826e-13 | | q qbar' -> ~chi_10 ~chi_10 1551 | 4.787e-12 | | q qbar' -> ~chi_10 ~chi_20 1552 | 5.546e-13 | | q qbar' -> ~chi_20 ~chi_20 1553 | 4.096e-12 | | q qbar' -> ~chi_10 ~chi_30 1554 | 1.743e-13 | | q qbar' -> ~chi_20 ~chi_30 1555 | 6.627e-13 | | q qbar' -> ~chi_30 ~chi_30 1556 | 3.653e-17 | | q qbar' -> ~chi_10 ~chi_40 1557 | 4.754e-14 | | q qbar' -> ~chi_20 ~chi_40 1558 | 1.863e-13 | | q qbar' -> ~chi_30 ~chi_40 1559 | 3.969e-12 | | q qbar' -> ~chi_40 ~chi_40 1560 | 2.161e-15 | | q qbar' -> ~chi_1+ ~chi_10 1571 | 1.274e-12 | | q qbar' -> ~chi_1- ~chi_10 1572 | 5.117e-13 | | q qbar' -> ~chi_2+ ~chi_10 1573 | 3.393e-13 | | q qbar' -> ~chi_2- ~chi_10 1574 | 1.329e-13 | | q qbar' -> ~chi_1+ ~chi_20 1575 | 1.045e-10 | | q qbar' -> ~chi_1- ~chi_20 1576 | 4.886e-11 | | q qbar' -> ~chi_2+ ~chi_20 1577 | 4.795e-14 | | q qbar' -> ~chi_2- ~chi_20 1578 | 1.499e-14 | | q qbar' -> ~chi_1+ ~chi_30 1579 | 9.421e-13 | | q qbar' -> ~chi_1- ~chi_30 1580 | 3.659e-13 | | q qbar' -> ~chi_2+ ~chi_30 1581 | 5.862e-12 | | q qbar' -> ~chi_2- ~chi_30 1582 | 1.969e-12 | | q qbar' -> ~chi_1+ ~chi_40 1583 | 5.646e-14 | | q qbar' -> ~chi_1- ~chi_40 1584 | 1.778e-14 | | q qbar' -> ~chi_2+ ~chi_40 1585 | 5.747e-12 | | q qbar' -> ~chi_2- ~chi_40 1586 | 1.920e-12 | | q qbar' -> ~chi_1+ ~chi_1- 1591 | 7.640e-11 | | q qbar' -> ~chi_1+ ~chi_2- 1592 | 3.566e-13 | | q qbar' -> ~chi_2+ ~chi_1- 1593 | 3.566e-13 | | q qbar' -> ~chi_2+ ~chi_2- 1594 | 4.106e-12 | | q q' -> ~d_L* + c.c 2011 | 0.000e+00 | | q q' -> ~u_L* + c.c 2012 | 0.000e+00 | | q q' -> ~s_L* + c.c 2013 | 0.000e+00 | | q q' -> ~c_L* + c.c 2014 | 0.000e+00 | | q q' -> ~b_1* + c.c 2015 | 0.000e+00 | | q q' -> ~t_1* + c.c 2016 | 0.000e+00 | | q q' -> ~d_R* + c.c 2021 | 0.000e+00 | | q q' -> ~u_R* + c.c 2022 | 0.000e+00 | | q q' -> ~s_R* + c.c 2023 | 0.000e+00 | | q q' -> ~c_R* + c.c 2024 | 0.000e+00 | | q q' -> ~b_2* + c.c 2025 | 0.000e+00 | | q q' -> ~t_2* + c.c 2026 | 0.000e+00 | | q qbar' -> ~g ~chi_10 1601 | 1.400e-11 | | q qbar' -> ~g ~chi_20 1602 | 1.421e-11 | | q qbar' -> ~g ~chi_30 1603 | 8.572e-14 | | q qbar' -> ~g ~chi_40 1604 | 3.152e-13 | | q qbar' -> ~g ~chi_1+ + c.c 1621 | 3.160e-11 | | q qbar' -> ~g ~chi_2+ + c.c 1622 | 8.012e-13 | | q qbar' -> ~e_L- ~e_L+ 1651 | 7.499e-12 | | q qbar' -> ~e_L- ~mu_L+ 1652 | 0.000e+00 | | q qbar' -> ~mu_L- ~e_L+ 1653 | 0.000e+00 | | q qbar' -> ~e_L- ~tau_1+ 1654 | 0.000e+00 | | q qbar' -> ~tau_1- ~e_L+ 1655 | 0.000e+00 | | q qbar' -> ~e_L- ~e_R+ 1656 | 0.000e+00 | | q qbar' -> ~e_R- ~e_L+ 1657 | 0.000e+00 | | q qbar' -> ~e_L- ~mu_R+ 1658 | 0.000e+00 | | q qbar' -> ~mu_R- ~e_L+ 1659 | 0.000e+00 | | q qbar' -> ~e_L- ~tau_2+ 1660 | 0.000e+00 | | q qbar' -> ~tau_2- ~e_L+ 1661 | 0.000e+00 | | q qbar' -> ~nu_eL ~nu_eLbar 1662 | 8.156e-12 | | q qbar' -> ~nu_eL ~nu_muLbar 1663 | 0.000e+00 | | q qbar' -> ~nu_muL ~nu_eLbar 1664 | 0.000e+00 | | q qbar' -> ~nu_eL ~nu_tauLbar 1665 | 0.000e+00 | | q qbar' -> ~nu_tauL ~nu_eLbar 1666 | 0.000e+00 | | q qbar' -> ~nu_eL ~nu_eRbar 1667 | 0.000e+00 | | q qbar' -> ~nu_eR ~nu_eLbar 1668 | 0.000e+00 | | q qbar' -> ~nu_eL ~nu_muRbar 1669 | 0.000e+00 | | q qbar' -> ~nu_muR ~nu_eLbar 1670 | 0.000e+00 | | q qbar' -> ~nu_eL ~nu_tauRbar 1671 | 0.000e+00 | | q qbar' -> ~nu_tauR ~nu_eLbar 1672 | 0.000e+00 | | q qbar' -> ~nu_eL ~e_L+ + c.c. 1673 | 2.925e-11 | | q qbar' -> ~nu_eL ~mu_L+ + c.c. 1674 | 0.000e+00 | | q qbar' -> ~nu_eL ~tau_1+ + c.c. 1675 | 0.000e+00 | | q qbar' -> ~nu_eL ~e_R+ + c.c. 1676 | 0.000e+00 | | q qbar' -> ~nu_eL ~mu_R+ + c.c. 1677 | 0.000e+00 | | q qbar' -> ~nu_eL ~tau_2+ + c.c. 1678 | 0.000e+00 | | q qbar' -> ~mu_L- ~mu_L+ 1679 | 7.491e-12 | | q qbar' -> ~mu_L- ~tau_1+ 1680 | 0.000e+00 | | q qbar' -> ~tau_1- ~mu_L+ 1681 | 0.000e+00 | | q qbar' -> ~mu_L- ~e_R+ 1682 | 0.000e+00 | | q qbar' -> ~e_R- ~mu_L+ 1683 | 0.000e+00 | | q qbar' -> ~mu_L- ~mu_R+ 1684 | 0.000e+00 | | q qbar' -> ~mu_R- ~mu_L+ 1685 | 0.000e+00 | | q qbar' -> ~mu_L- ~tau_2+ 1686 | 0.000e+00 | | q qbar' -> ~tau_2- ~mu_L+ 1687 | 0.000e+00 | | q qbar' -> ~nu_muL ~nu_muLbar 1688 | 8.156e-12 | | q qbar' -> ~nu_muL ~nu_tauLbar 1689 | 0.000e+00 | | q qbar' -> ~nu_tauL ~nu_muLbar 1690 | 0.000e+00 | | q qbar' -> ~nu_muL ~nu_eRbar 1691 | 0.000e+00 | | q qbar' -> ~nu_eR ~nu_muLbar 1692 | 0.000e+00 | | q qbar' -> ~nu_muL ~nu_muRbar 1693 | 0.000e+00 | | q qbar' -> ~nu_muR ~nu_muLbar 1694 | 0.000e+00 | | q qbar' -> ~nu_muL ~nu_tauRbar 1695 | 0.000e+00 | | q qbar' -> ~nu_tauR ~nu_muLbar 1696 | 0.000e+00 | | q qbar' -> ~nu_muL ~e_L+ + c.c. 1697 | 0.000e+00 | | q qbar' -> ~nu_muL ~mu_L+ + c.c. 1698 | 2.924e-11 | | q qbar' -> ~nu_muL ~tau_1+ + c.c. 1699 | 0.000e+00 | | q qbar' -> ~nu_muL ~e_R+ + c.c. 1700 | 0.000e+00 | | q qbar' -> ~nu_muL ~mu_R+ + c.c. 1701 | 0.000e+00 | | q qbar' -> ~nu_muL ~tau_2+ + c.c. 1702 | 0.000e+00 | | q qbar' -> ~tau_1- ~tau_1+ 1703 | 2.396e-11 | | q qbar' -> ~tau_1- ~e_R+ 1704 | 0.000e+00 | | q qbar' -> ~e_R- ~tau_1+ 1705 | 0.000e+00 | | q qbar' -> ~tau_1- ~mu_R+ 1706 | 0.000e+00 | | q qbar' -> ~mu_R- ~tau_1+ 1707 | 0.000e+00 | | q qbar' -> ~tau_1- ~tau_2+ 1708 | 1.002e-11 | | q qbar' -> ~tau_2- ~tau_1+ 1709 | 1.002e-11 | | q qbar' -> ~nu_tauL ~nu_tauLbar 1710 | 8.273e-12 | | q qbar' -> ~nu_tauL ~nu_eRbar 1711 | 0.000e+00 | | q qbar' -> ~nu_eR ~nu_tauLbar 1712 | 0.000e+00 | | q qbar' -> ~nu_tauL ~nu_muRbar 1713 | 0.000e+00 | | q qbar' -> ~nu_muR ~nu_tauLbar 1714 | 0.000e+00 | | q qbar' -> ~nu_tauL ~nu_tauRbar 1715 | 0.000e+00 | | q qbar' -> ~nu_tauR ~nu_tauLbar 1716 | 0.000e+00 | | q qbar' -> ~nu_tauL ~e_L+ + c.c. 1717 | 0.000e+00 | | q qbar' -> ~nu_tauL ~mu_L+ + c.c. 1718 | 0.000e+00 | | q qbar' -> ~nu_tauL ~tau_1+ + c.c. 1719 | 1.416e-12 | | q qbar' -> ~nu_tauL ~e_R+ + c.c. 1720 | 0.000e+00 | | q qbar' -> ~nu_tauL ~mu_R+ + c.c. 1721 | 0.000e+00 | | q qbar' -> ~nu_tauL ~tau_2+ + c.c. 1722 | 2.866e-11 | | q qbar' -> ~e_R- ~e_R+ 1723 | 2.156e-11 | | q qbar' -> ~e_R- ~mu_R+ 1724 | 0.000e+00 | | q qbar' -> ~mu_R- ~e_R+ 1725 | 0.000e+00 | | q qbar' -> ~e_R- ~tau_2+ 1726 | 0.000e+00 | | q qbar' -> ~tau_2- ~e_R+ 1727 | 0.000e+00 | | q qbar' -> ~nu_eR ~nu_eRbar 1728 | 0.000e+00 | | q qbar' -> ~nu_eR ~nu_muRbar 1729 | 0.000e+00 | | q qbar' -> ~nu_muR ~nu_eRbar 1730 | 0.000e+00 | | q qbar' -> ~nu_eR ~nu_tauRbar 1731 | 0.000e+00 | | q qbar' -> ~nu_tauR ~nu_eRbar 1732 | 0.000e+00 | | q qbar' -> ~nu_eR ~e_L+ + c.c. 1733 | 0.000e+00 | | q qbar' -> ~nu_eR ~mu_L+ + c.c. 1734 | 0.000e+00 | | q qbar' -> ~nu_eR ~tau_1+ + c.c. 1735 | 0.000e+00 | | q qbar' -> ~nu_eR ~e_R+ + c.c. 1736 | 0.000e+00 | | q qbar' -> ~nu_eR ~mu_R+ + c.c. 1737 | 0.000e+00 | | q qbar' -> ~nu_eR ~tau_2+ + c.c. 1738 | 0.000e+00 | | q qbar' -> ~mu_R- ~mu_R+ 1739 | 2.156e-11 | | q qbar' -> ~mu_R- ~tau_2+ 1740 | 0.000e+00 | | q qbar' -> ~tau_2- ~mu_R+ 1741 | 0.000e+00 | | q qbar' -> ~nu_muR ~nu_muRbar 1742 | 0.000e+00 | | q qbar' -> ~nu_muR ~nu_tauRbar 1743 | 0.000e+00 | | q qbar' -> ~nu_tauR ~nu_muRbar 1744 | 0.000e+00 | | q qbar' -> ~nu_muR ~e_L+ + c.c. 1745 | 0.000e+00 | | q qbar' -> ~nu_muR ~mu_L+ + c.c. 1746 | 0.000e+00 | | q qbar' -> ~nu_muR ~tau_1+ + c.c. 1747 | 0.000e+00 | | q qbar' -> ~nu_muR ~e_R+ + c.c. 1748 | 0.000e+00 | | q qbar' -> ~nu_muR ~mu_R+ + c.c. 1749 | 0.000e+00 | | q qbar' -> ~nu_muR ~tau_2+ + c.c. 1750 | 0.000e+00 | | q qbar' -> ~tau_2- ~tau_2+ 1751 | 7.169e-12 | | q qbar' -> ~nu_tauR ~nu_tauRbar 1752 | 0.000e+00 | | q qbar' -> ~nu_tauR ~e_L+ + c.c. 1753 | 0.000e+00 | | q qbar' -> ~nu_tauR ~mu_L+ + c.c. 1754 | 0.000e+00 | | q qbar' -> ~nu_tauR ~tau_1+ + c.c. 1755 | 0.000e+00 | | q qbar' -> ~nu_tauR ~e_R+ + c.c. 1756 | 0.000e+00 | | q qbar' -> ~nu_tauR ~mu_R+ + c.c. 1757 | 0.000e+00 | | q qbar' -> ~nu_tauR ~tau_2+ + c.c. 1758 | 0.000e+00 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eCM | 10000.000 | 14000.000 10.00000 | | HadronLevel:Hadronize | off | on | | HiggsA3:coup2d | 9.66950 | 1.00000 | | HiggsA3:coup2H1Z | -0.0037460 | 1.00000 | | HiggsA3:coup2H2Z | 0.99999 | 1.00000 | | HiggsA3:coup2l | 0.10342 | 1.00000 | | HiggsA3:coup2u | 0.10342 | 1.00000 | | HiggsH1:coup2d | 1.03622 | 1.00000 | | HiggsH1:coup2Hchg | 0.56046 | 0.0 | | HiggsH1:coup2l | 0.99961 | 1.00000 | | HiggsH1:coup2u | 0.99961 | 1.00000 | | HiggsH1:coup2W | 0.99999 | 1.00000 | | HiggsH1:coup2Z | 0.99999 | 1.00000 | | HiggsH2:coup2A3A3 | 0.20390 | 1.00000 | | HiggsH2:coup2d | 9.66568 | 1.00000 | | HiggsH2:coup2H1H1 | -0.61823 | 1.00000 | | HiggsH2:coup2Hchg | 0.19822 | 0.0 | | HiggsH2:coup2HchgW | 0.99999 | 0.0 | | HiggsH2:coup2l | -0.10716 | 1.00000 | | HiggsH2:coup2u | -0.10716 | 1.00000 | | HiggsH2:coup2W | -0.0037460 | 1.00000 | | HiggsH2:coup2Z | -0.0037460 | 1.00000 | | HiggsHchg:coup2H1W | -0.0037460 | 1.00000 | | HiggsHchg:coup2H2W | 0.99999 | 0.0 | | HiggsHchg:tanBeta | 9.66950 | 5.00000 | | Init:showChangedParticleData | off | on | | Main:numberOfEvents | 10000 | 1000 0 | | Main:timesAllowErrors | 3 | 10 0 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberCount | 500 | 1000 0 | | Next:numberShowEvent | 2 | 1 0 | | Next:numberShowInfo | 2 | 1 0 | | Next:numberShowProcess | 2 | 1 0 | | PartonLevel:FSR | off | on | | PartonLevel:ISR | off | on | | PartonLevel:MPI | off | on | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SLHA:file | cmssm.spc | void | | SpaceShower:rapidityOrder | on | off | | SUSY:all | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* PYTHIA Warning in TauDecays::decay: unknown tau production, assuming unpolarized and uncorrelated -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 5.000e+03, e = 5.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -5.000e+03, e = 5.000e+03, m = 9.383e-01. In 1: id = 1, x = 3.634e-01, pdf = 6.633e-02 at Q2 = 1.768e+06. In 2: id = 21, x = 3.261e-01, pdf = 3.111e-02 at same Q2. Subprocess q g -> ~d_L gluino + c.c. with code 1203 is 2 -> 2. It has sHat = 1.185e+07, tHat = -8.315e+06, uHat = -1.108e+06, pTHat = 8.086e+02, m3Hat = 1.056e+03, m4Hat = 1.147e+03, thetaHat = 2.484e+00, phiHat = 5.302e+00. alphaEM = 8.065e-03, alphaS = 9.533e-02 at Q2 = 1.866e+06. Impact parameter b = 0.000e+00 gives enhancement factor = 1.000e+00. Max pT scale for MPI = 1.000e+04, ISR = 1.000e+04, FSR = 1.000e+04. Number of MPI = 1, ISR = 0, FSRproc = 0, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 10000.000 10000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 5000.000 5000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -5000.000 5000.000 0.938 3 1 (d) -21 1 0 5 6 101 0 0.000 0.000 1817.122 1817.122 0.000 4 21 (g) -21 2 0 5 6 102 101 0.000 0.000 -1630.731 1630.731 0.000 5 1000001 (~d_L) -22 3 4 7 8 103 0 449.937 -671.837 -956.559 1638.026 1055.611 6 1000021 (~g) -22 3 4 9 10 102 103 -449.937 671.837 1142.950 1809.827 1146.878 7 -1000024 (~chi_1-) -22 5 0 11 12 0 0 445.589 -543.567 -143.348 814.749 386.332 8 2 u 23 5 0 0 0 103 0 4.348 -128.271 -813.211 823.277 0.330 9 -1000006 (~t_1bar) -22 6 0 13 14 0 103 -494.915 664.865 739.528 1370.973 803.541 10 6 (t) -22 6 0 15 16 102 0 44.978 6.972 403.422 438.854 166.648 11 1000015 (~tau_1-) -22 7 0 17 18 0 0 195.745 -146.141 -30.618 331.968 222.692 12 -16 nu_taubar 23 7 0 0 0 0 0 249.844 -397.426 -112.730 482.781 0.000 13 1000023 (~chi_20) -22 9 0 19 20 0 0 -281.147 146.239 111.762 511.926 386.197 14 -6 (tbar) -22 9 0 21 22 0 103 -213.769 518.626 627.766 859.046 170.884 15 24 (W+) -22 10 0 23 24 0 0 47.040 -35.397 144.008 175.951 82.186 16 5 b 23 10 0 0 0 102 0 -2.062 42.369 259.414 262.903 4.800 17 1000022 ~chi_10 23 11 0 0 0 0 0 165.829 -132.490 -13.425 294.818 204.168 18 15 tau- 23 11 0 0 0 0 0 29.916 -13.651 -17.194 37.150 1.777 19 -1000015 (~tau_1+) -22 13 0 25 26 0 0 -230.778 204.446 5.079 380.361 222.692 20 15 tau- 23 13 0 0 0 0 0 -50.369 -58.206 106.684 131.566 1.777 21 -24 (W-) -22 14 0 27 28 0 0 -136.824 468.148 543.140 733.935 75.994 22 -5 bbar 23 14 0 0 0 0 103 -76.945 50.477 84.625 125.112 4.800 23 -3 sbar 23 15 0 0 0 0 104 -17.266 -21.515 78.036 82.770 0.500 24 4 c 23 15 0 0 0 104 0 64.307 -13.882 65.973 93.181 1.500 25 1000022 ~chi_10 23 19 0 0 0 0 0 -205.250 184.740 -12.375 343.648 204.168 26 -15 tau+ 23 19 0 0 0 0 0 -25.528 19.706 17.454 36.712 1.777 27 3 s 23 21 0 0 0 105 0 -139.371 411.117 454.576 628.555 0.500 28 -4 cbar 23 21 0 0 0 0 105 2.547 57.031 88.564 105.380 1.500 Charge sum: -0.333 Momentum sum: -0.000 0.000 186.391 3447.853 3442.811 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 10000.000 10000.000 1 2212 (p+) -12 0 0 7 0 0 0 0.000 0.000 5000.000 5000.000 0.938 2 2212 (p+) -12 0 0 8 0 0 0 0.000 0.000 -5000.000 5000.000 0.938 3 1 (d) -21 7 7 5 6 101 0 0.000 0.000 1817.122 1817.122 0.000 4 21 (g) -21 8 8 5 6 102 101 0.000 0.000 -1630.731 1630.731 0.000 5 1000001 (~d_L) -22 3 4 9 9 103 0 449.937 -671.837 -956.559 1638.026 1055.611 6 1000021 (~g) -22 3 4 10 10 102 103 -449.937 671.837 1142.950 1809.827 1146.878 7 1 (d) -61 1 0 3 3 101 0 2.244 -1.332 1817.121 1817.123 0.000 8 21 (g) -61 2 0 4 4 102 101 0.007 -2.317 -1630.731 1630.732 0.000 9 1000001 (~d_L) -62 5 5 14 15 103 0 450.364 -673.931 -956.605 1639.030 1055.611 10 1000021 (~g) -62 6 6 16 17 102 103 -448.112 670.282 1142.995 1808.826 1146.878 11 2203 uu_1 63 1 0 0 0 0 101 -2.244 1.332 3182.580 3182.581 0.771 12 2 u 63 2 0 0 0 101 0 0.082 0.887 -0.466 1.058 0.330 13 2103 ud_1 63 2 0 0 0 0 102 -0.090 1.431 -3368.505 3368.505 0.771 14 -1000024 (~chi_1-) -22 9 0 18 19 0 0 445.802 -544.608 -143.371 815.564 386.332 15 2 u 23 9 0 0 0 103 0 4.562 -129.323 -813.234 823.465 0.330 16 -1000006 (~t_1bar) -22 10 0 20 21 0 103 -493.533 663.687 739.562 1369.922 803.541 17 6 (t) -22 10 0 22 23 102 0 45.421 6.595 403.433 438.904 166.648 18 1000015 (~tau_1-) -22 14 0 24 25 0 0 195.832 -146.565 -30.628 332.207 222.692 19 -16 nu_taubar 23 14 0 0 0 0 0 249.970 -398.043 -112.743 483.357 0.000 20 1000023 (~chi_20) -22 16 0 26 27 0 0 -280.631 145.800 111.775 511.520 386.197 21 -6 (tbar) -22 16 0 28 29 0 103 -212.903 517.888 627.787 858.402 170.884 22 24 (W+) -22 17 0 30 31 0 0 47.218 -35.549 144.013 176.033 82.186 23 5 b 23 17 0 0 0 102 0 -1.797 42.143 259.420 262.871 4.800 24 1000022 ~chi_10 23 18 0 0 0 0 0 165.906 -132.867 -13.433 295.031 204.168 25 15 (tau-) -23 18 0 36 39 0 0 29.926 -13.698 -17.195 37.176 1.777 26 -1000015 (~tau_1+) -22 20 0 32 33 0 0 -230.394 204.119 5.088 379.953 222.692 27 15 (tau-) -23 20 0 40 41 0 0 -50.236 -58.320 106.687 131.568 1.777 28 -24 (W-) -22 21 0 34 35 0 0 -136.084 467.518 543.159 733.409 75.994 29 -5 bbar 23 21 0 0 0 0 103 -76.819 50.370 84.628 124.993 4.800 30 -3 sbar 23 22 0 0 0 0 104 -17.183 -21.586 78.038 82.773 0.500 31 4 c 23 22 0 0 0 104 0 64.401 -13.962 65.975 93.260 1.500 32 1000022 ~chi_10 23 26 0 0 0 0 0 -204.904 184.445 -12.366 343.282 204.168 33 -15 (tau+) -23 26 0 42 44 0 0 -25.491 19.675 17.455 36.670 1.777 34 3 s 23 28 0 0 0 105 0 -138.737 410.577 454.592 628.073 0.500 35 -4 cbar 23 28 0 0 0 0 105 2.653 56.941 88.567 105.336 1.500 36 16 nu_tau 91 25 0 0 0 0 0 8.054 -3.164 -4.894 9.941 0.000 37 -211 pi- 91 25 0 0 0 0 0 5.662 -2.323 -3.015 6.824 0.140 38 -211 pi- 91 25 0 0 0 0 0 3.574 -1.881 -2.157 4.581 0.140 39 211 pi+ 91 25 0 0 0 0 0 12.635 -6.330 -7.129 15.830 0.140 40 16 nu_tau 91 27 0 0 0 0 0 -17.060 -20.340 38.108 46.443 0.000 41 -211 pi- 91 27 0 0 0 0 0 -33.176 -37.980 68.579 85.125 0.140 42 -16 nu_taubar 91 33 0 0 0 0 0 -7.817 5.326 4.842 10.627 0.000 43 -11 e+ 91 33 0 0 0 0 0 -7.503 6.610 5.846 11.583 0.001 44 12 nu_e 91 33 0 0 0 0 0 -10.171 7.738 6.766 14.461 0.000 Charge sum: 2.000 Momentum sum: -0.000 0.000 0.000 10000.000 10000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 5.000e+03, e = 5.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -5.000e+03, e = 5.000e+03, m = 9.383e-01. In 1: id = 2, x = 4.426e-01, pdf = 1.300e-01 at Q2 = 7.366e+05. In 2: id = -2, x = 6.737e-02, pdf = 1.234e-01 at same Q2. Subprocess q qbar' -> ~t_1 ~t_1bar with code 1290 is 2 -> 2. It has sHat = 2.982e+06, tHat = -1.008e+06, uHat = -6.828e+05, pTHat = 3.016e+02, m3Hat = 8.035e+02, m4Hat = 8.035e+02, thetaHat = 1.873e+00, phiHat = 1.277e+00. alphaEM = 8.021e-03, alphaS = 1.003e-01 at Q2 = 7.366e+05. Impact parameter b = 0.000e+00 gives enhancement factor = 1.000e+00. Max pT scale for MPI = 1.000e+04, ISR = 1.000e+04, FSR = 1.000e+04. Number of MPI = 1, ISR = 0, FSRproc = 0, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 10000.000 10000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 5000.000 5000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -5000.000 5000.000 0.938 3 2 (u) -21 1 0 5 6 101 0 0.000 0.000 2213.233 2213.233 0.000 4 -2 (ubar) -21 2 0 5 6 0 102 0.000 0.000 -336.827 336.827 0.000 5 1000006 (~t_1) -22 3 4 7 8 101 0 87.388 288.624 799.217 1172.760 803.541 6 -1000006 (~t_1bar) -22 3 4 9 10 0 102 -87.388 -288.624 1077.188 1377.299 803.541 7 1000037 (~chi_2+) -22 5 0 11 12 0 0 -38.447 215.107 752.133 1019.532 652.680 8 5 b 23 5 0 0 0 101 0 125.834 73.517 47.084 153.229 4.800 9 -1000037 (~chi_2-) -22 6 0 13 14 0 0 28.338 -223.184 1021.884 1233.228 652.680 10 -5 bbar 23 6 0 0 0 0 102 -115.725 -65.440 55.304 144.071 4.800 11 1000023 (~chi_20) -22 7 0 15 16 0 0 -178.929 219.140 705.554 852.638 386.197 12 24 (W+) -22 7 0 17 18 0 0 140.482 -4.033 46.580 166.893 77.020 13 1000022 ~chi_10 23 9 0 0 0 0 0 -245.105 -228.347 704.778 806.608 204.168 14 -24 (W-) -22 9 0 19 20 0 0 273.443 5.163 317.106 426.621 81.558 15 -1000013 (~mu_L+) -22 11 0 21 22 0 0 -188.127 194.949 654.969 795.818 361.862 16 13 mu- 23 11 0 0 0 0 0 9.198 24.191 50.584 56.821 0.106 17 -13 mu+ 23 12 0 0 0 0 0 144.414 -11.909 54.732 154.896 0.106 18 14 nu_mu 23 12 0 0 0 0 0 -3.931 7.876 -8.152 11.998 0.000 19 3 s 23 14 0 0 0 103 0 8.594 -4.915 -3.618 10.553 0.500 20 -4 cbar 23 14 0 0 0 0 103 264.848 10.079 320.724 416.068 1.500 21 1000022 ~chi_10 23 15 0 0 0 0 0 13.993 109.556 355.301 424.408 204.168 22 -13 mu+ 23 15 0 0 0 0 0 -202.120 85.393 299.668 371.410 0.106 Charge sum: 0.000 Momentum sum: -0.000 0.000 1876.406 2550.060 1726.820 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 10000.000 10000.000 1 2212 (p+) -12 0 0 7 0 0 0 0.000 0.000 5000.000 5000.000 0.938 2 2212 (p+) -12 0 0 8 0 0 0 0.000 0.000 -5000.000 5000.000 0.938 3 2 (u) -21 7 7 5 6 101 0 0.000 0.000 2213.233 2213.233 0.000 4 -2 (ubar) -21 8 8 5 6 0 102 0.000 0.000 -336.827 336.827 0.000 5 1000006 (~t_1) -22 3 4 9 9 101 0 87.388 288.624 799.217 1172.760 803.541 6 -1000006 (~t_1bar) -22 3 4 10 10 0 102 -87.388 -288.624 1077.188 1377.299 803.541 7 2 (u) -61 1 0 3 3 101 0 -1.187 1.580 2213.234 2213.235 0.000 8 -2 (ubar) -61 2 0 4 4 0 102 0.254 1.574 -336.825 336.829 0.000 9 1000006 (~t_1) -62 5 5 15 16 101 0 87.000 290.201 799.847 1173.550 803.541 10 -1000006 (~t_1bar) -62 6 6 17 18 0 102 -87.932 -287.048 1076.562 1376.515 803.541 11 2103 ud_1 63 1 0 0 0 0 101 1.187 -1.580 2786.762 2786.763 0.771 12 2203 uu_1 63 2 0 0 0 0 105 -0.138 -0.411 -1625.949 1625.950 0.771 13 1 d 63 2 0 0 0 102 0 0.268 -0.854 -2718.161 2718.161 0.330 14 2 u 63 2 0 0 0 105 0 -0.383 -0.308 -319.061 319.062 0.330 15 1000037 (~chi_2+) -22 9 0 19 20 0 0 -38.784 216.478 752.681 1020.238 652.680 16 5 b 23 9 0 0 0 101 0 125.784 73.723 47.166 153.311 4.800 17 -1000037 (~chi_2-) -22 10 0 21 22 0 0 27.850 -221.772 1021.324 1232.498 652.680 18 -5 bbar 23 10 0 0 0 0 102 -115.782 -65.276 55.239 144.017 4.800 19 1000023 (~chi_20) -22 15 0 23 24 0 0 -179.212 220.286 706.011 853.372 386.197 20 24 (W+) -22 15 0 25 26 0 0 140.427 -3.808 46.669 166.867 77.020 21 1000022 ~chi_10 23 17 0 0 0 0 0 -245.424 -227.424 704.412 806.124 204.168 22 -24 (W-) -22 17 0 27 28 0 0 273.274 5.652 316.912 426.375 81.558 23 -1000013 (~mu_L+) -22 19 0 29 30 0 0 -188.391 196.019 655.396 796.494 361.862 24 13 mu- 23 19 0 0 0 0 0 9.179 24.267 50.615 56.877 0.106 25 -13 mu+ 23 20 0 0 0 0 0 144.362 -11.701 54.815 154.862 0.106 26 14 nu_mu 23 20 0 0 0 0 0 -3.935 7.892 -8.146 12.005 0.000 27 3 s 23 22 0 0 0 103 0 8.590 -4.903 -3.623 10.545 0.500 28 -4 cbar 23 22 0 0 0 0 103 264.684 10.555 320.535 415.829 1.500 29 1000022 ~chi_10 23 23 0 0 0 0 0 13.852 110.127 355.529 424.742 204.168 30 -13 mu+ 23 23 0 0 0 0 0 -202.243 85.892 299.867 371.753 0.106 Charge sum: 2.000 Momentum sum: -0.000 0.000 -0.000 10000.000 10000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- Pythia::next(): 500 events have been generated Pythia::next(): 1000 events have been generated Pythia::next(): 1500 events have been generated Pythia::next(): 2000 events have been generated Pythia::next(): 2500 events have been generated Pythia::next(): 3000 events have been generated Pythia::next(): 3500 events have been generated Pythia::next(): 4000 events have been generated Pythia::next(): 4500 events have been generated Pythia::next(): 5000 events have been generated Pythia::next(): 5500 events have been generated Pythia::next(): 6000 events have been generated Pythia::next(): 6500 events have been generated PYTHIA Warning in TauDecays::decay: maximum decay weight exceeded in tau decay Pythia::next(): 7000 events have been generated Pythia::next(): 7500 events have been generated Pythia::next(): 8000 events have been generated Pythia::next(): 8500 events have been generated Pythia::next(): 9000 events have been generated Pythia::next(): 9500 events have been generated *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> gluino gluino 1201 | 1651 115 115 | 4.882e-12 2.488e-13 | | q qbar -> gluino gluino 1202 | 201 17 17 | 8.404e-13 1.114e-13 | | q g -> ~d_L gluino + c.c. 1203 | 2549 224 224 | 9.102e-12 3.400e-13 | | q g -> ~u_L gluino + c.c. 1204 | 6235 767 767 | 3.102e-11 6.489e-13 | | q g -> ~s_L gluino + c.c. 1205 | 146 13 13 | 5.127e-13 8.725e-14 | | q g -> ~c_L gluino + c.c. 1206 | 99 9 9 | 3.261e-13 7.975e-14 | | q g -> ~b_1 gluino + c.c. 1207 | 44 4 4 | 1.782e-13 4.422e-14 | | q g -> ~d_R gluino + c.c. 1209 | 2837 272 272 | 1.078e-11 3.800e-13 | | q g -> ~u_R gluino + c.c. 1210 | 6933 956 956 | 3.593e-11 6.918e-13 | | q g -> ~s_R gluino + c.c. 1211 | 154 8 8 | 4.461e-13 7.965e-14 | | q g -> ~c_R gluino + c.c. 1212 | 130 10 10 | 3.607e-13 7.190e-14 | | q g -> ~b_2 gluino + c.c. 1213 | 46 1 1 | 7.399e-14 7.399e-14 | | g g -> ~d_L ~d_Lbar 1215 | 98 7 7 | 3.502e-13 6.828e-14 | | g g -> ~u_L ~u_Lbar 1216 | 90 4 4 | 2.876e-13 7.058e-14 | | g g -> ~s_L ~s_Lbar 1217 | 91 8 8 | 2.633e-13 6.472e-14 | | g g -> ~c_L ~c_Lbar 1218 | 100 6 6 | 2.196e-13 4.836e-14 | | g g -> ~b_1 ~b_1bar 1219 | 213 23 23 | 7.391e-13 9.568e-14 | | g g -> ~t_1 ~t_1bar 1220 | 883 84 84 | 3.370e-12 2.065e-13 | | g g -> ~d_R ~d_Rbar 1221 | 149 14 14 | 3.504e-13 5.540e-14 | | g g -> ~u_R ~u_Rbar 1222 | 131 6 6 | 3.313e-13 6.070e-14 | | g g -> ~s_R ~s_Rbar 1223 | 135 10 10 | 4.643e-13 8.214e-14 | | g g -> ~c_R ~c_Rbar 1224 | 123 5 5 | 2.483e-13 4.908e-14 | | g g -> ~b_2 ~b_2bar 1225 | 130 9 9 | 4.352e-13 7.029e-14 | | g g -> ~t_2 ~t_2bar 1226 | 120 8 8 | 4.123e-13 7.975e-14 | | q qbar' -> ~d_L ~d_Lbar 1231 | 133 9 9 | 3.634e-13 6.987e-14 | | q qbar' -> ~d_L ~s_Lbar 1232 | 19 1 1 | 5.104e-14 5.104e-14 | | q qbar' -> ~s_L ~d_Lbar 1233 | 4 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~d_L ~b_1bar 1234 | 13 3 3 | 8.869e-14 3.011e-14 | | q qbar' -> ~b_1 ~d_Lbar 1235 | 3 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~d_L ~d_Rbar 1236 | 299 22 22 | 9.269e-13 1.067e-13 | | q qbar' -> ~d_R ~d_Lbar 1237 | 296 22 22 | 8.301e-13 1.010e-13 | | q qbar' -> ~d_L ~s_Rbar 1238 | 153 15 15 | 5.031e-13 7.639e-14 | | q qbar' -> ~s_R ~d_Lbar 1239 | 15 1 1 | 2.900e-14 2.900e-14 | | q qbar' -> ~d_L ~b_2bar 1240 | 38 4 4 | 9.724e-14 3.258e-14 | | q qbar' -> ~b_2 ~d_Lbar 1241 | 5 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~u_L ~u_Lbar 1242 | 186 20 20 | 6.584e-13 9.239e-14 | | q qbar' -> ~u_L ~c_Lbar 1243 | 26 3 3 | 1.147e-13 4.715e-14 | | q qbar' -> ~c_L ~u_Lbar 1244 | 1 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~u_L ~u_Rbar 1247 | 485 56 56 | 2.135e-12 1.653e-13 | | q qbar' -> ~u_R ~u_Lbar 1248 | 480 59 59 | 2.527e-12 1.831e-13 | | q qbar' -> ~u_L ~c_Rbar 1249 | 126 13 13 | 5.586e-13 8.431e-14 | | q qbar' -> ~c_R ~u_Lbar 1250 | 3 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~u_L ~d_Lbar + c.c. 1253 | 182 15 15 | 4.225e-13 6.502e-14 | | q qbar' -> ~u_L ~s_Lbar + c.c. 1254 | 84 8 8 | 3.241e-13 6.939e-14 | | q qbar' -> ~u_L ~b_1bar + c.c. 1255 | 26 2 2 | 1.111e-13 3.832e-14 | | q qbar' -> ~u_L ~d_Rbar + c.c. 1256 | 922 82 82 | 3.629e-12 2.070e-13 | | q qbar' -> ~u_L ~s_Rbar + c.c. 1257 | 327 29 29 | 1.300e-12 1.326e-13 | | q qbar' -> ~u_L ~b_2bar + c.c. 1258 | 82 11 11 | 4.472e-13 8.597e-14 | | q qbar' -> ~s_L ~s_Lbar 1259 | 71 2 2 | 1.787e-13 4.790e-14 | | q qbar' -> ~s_L ~b_1bar 1260 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~b_1 ~s_Lbar 1261 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~s_L ~d_Rbar 1262 | 18 1 1 | 3.265e-14 3.265e-14 | | q qbar' -> ~d_R ~s_Lbar 1263 | 142 13 13 | 5.337e-13 7.946e-14 | | q qbar' -> ~s_L ~s_Rbar 1264 | 7 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~s_R ~s_Lbar 1265 | 7 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~s_L ~b_2bar 1266 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~b_2 ~s_Lbar 1267 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~c_L ~c_Lbar 1268 | 71 4 4 | 1.913e-13 5.480e-14 | | q qbar' -> ~c_L ~u_Rbar 1271 | 2 1 1 | 4.928e-14 4.928e-14 | | q qbar' -> ~u_R ~c_Lbar 1272 | 146 19 19 | 7.175e-13 1.046e-13 | | q qbar' -> ~c_L ~c_Rbar 1273 | 2 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~c_R ~c_Lbar 1274 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~c_L ~d_Lbar + c.c. 1277 | 15 3 3 | 5.104e-14 2.816e-14 | | q qbar' -> ~c_L ~s_Lbar + c.c. 1278 | 8 2 2 | 3.882e-14 2.144e-14 | | q qbar' -> ~c_L ~b_1bar + c.c. 1279 | 1 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~c_L ~d_Rbar + c.c. 1280 | 64 6 6 | 2.837e-13 5.964e-14 | | q qbar' -> ~c_L ~s_Rbar + c.c. 1281 | 3 1 1 | 1.223e-14 1.223e-14 | | q qbar' -> ~c_L ~b_2bar + c.c. 1282 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~b_1 ~b_1bar 1283 | 168 19 19 | 5.671e-13 8.214e-14 | | q qbar' -> ~b_1 ~d_Rbar 1284 | 6 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~d_R ~b_1bar 1285 | 39 4 4 | 2.234e-13 5.246e-14 | | q qbar' -> ~b_1 ~s_Rbar 1286 | 1 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~s_R ~b_1bar 1287 | 3 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~b_1 ~b_2bar 1288 | 2 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~b_2 ~b_1bar 1289 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~t_1 ~t_1bar 1290 | 522 44 44 | 2.037e-12 1.666e-13 | | q qbar' -> ~t_1 ~t_2bar 1295 | 3 1 1 | 2.927e-15 2.927e-15 | | q qbar' -> ~t_2 ~t_1bar 1296 | 1 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~t_1 ~d_Lbar + c.c. 1297 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~t_1 ~s_Lbar + c.c. 1298 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~t_1 ~b_1bar + c.c. 1299 | 2 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~t_1 ~b_2bar + c.c. 1302 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~d_R ~d_Rbar 1303 | 212 18 18 | 6.504e-13 9.108e-14 | | q qbar' -> ~d_R ~s_Rbar 1304 | 43 3 3 | 1.250e-13 4.102e-14 | | q qbar' -> ~s_R ~d_Rbar 1305 | 3 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~d_R ~b_2bar 1306 | 13 1 1 | 1.497e-14 1.497e-14 | | q qbar' -> ~b_2 ~d_Rbar 1307 | 1 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~u_R ~u_Rbar 1308 | 260 18 18 | 9.704e-13 1.172e-13 | | q qbar' -> ~u_R ~c_Rbar 1309 | 36 4 4 | 1.974e-13 6.095e-14 | | q qbar' -> ~c_R ~u_Rbar 1310 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~u_R ~d_Lbar + c.c. 1313 | 899 89 89 | 3.923e-12 2.252e-13 | | q qbar' -> ~u_R ~s_Lbar + c.c. 1314 | 296 34 34 | 1.509e-12 1.539e-13 | | q qbar' -> ~u_R ~b_1bar + c.c. 1315 | 117 13 13 | 4.795e-13 7.920e-14 | | q qbar' -> ~u_R ~d_Rbar + c.c. 1316 | 232 18 18 | 9.181e-13 1.153e-13 | | q qbar' -> ~u_R ~s_Rbar + c.c. 1317 | 97 6 6 | 3.911e-13 7.772e-14 | | q qbar' -> ~u_R ~b_2bar + c.c. 1318 | 21 2 2 | 1.612e-13 6.008e-14 | | q qbar' -> ~s_R ~s_Rbar 1319 | 112 7 7 | 2.530e-13 4.330e-14 | | q qbar' -> ~s_R ~b_2bar 1320 | 1 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~b_2 ~s_Rbar 1321 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~c_R ~c_Rbar 1322 | 106 9 9 | 2.972e-13 6.910e-14 | | q qbar' -> ~c_R ~d_Lbar + c.c. 1325 | 58 5 5 | 2.284e-13 6.652e-14 | | q qbar' -> ~c_R ~s_Lbar + c.c. 1326 | 11 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~c_R ~b_1bar + c.c. 1327 | 4 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~c_R ~d_Rbar + c.c. 1328 | 16 2 2 | 3.367e-14 1.749e-14 | | q qbar' -> ~c_R ~s_Rbar + c.c. 1329 | 3 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~c_R ~b_2bar + c.c. 1330 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~b_2 ~b_2bar 1331 | 108 5 5 | 2.758e-13 5.615e-14 | | q qbar' -> ~t_2 ~t_2bar 1332 | 97 9 9 | 4.210e-13 8.380e-14 | | q qbar' -> ~t_2 ~d_Lbar + c.c. 1333 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~t_2 ~s_Lbar + c.c. 1334 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~t_2 ~b_1bar + c.c. 1335 | 5 2 2 | 7.943e-14 2.984e-14 | | q qbar' -> ~t_2 ~b_2bar + c.c. 1338 | 1 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~d_L ~d_L + c.c. 1351 | 715 71 71 | 3.112e-12 1.984e-13 | | q q' -> ~d_L ~s_L + c.c. 1352 | 136 15 15 | 3.449e-13 6.230e-14 | | q q' -> ~d_L ~b_1 + c.c. 1353 | 44 5 5 | 2.097e-13 5.414e-14 | | q q' -> ~d_L ~d_R + c.c. 1354 | 453 46 46 | 1.767e-12 1.567e-13 | | q q' -> ~d_L ~s_R + c.c. 1355 | 21 3 3 | 1.623e-13 6.049e-14 | | q q' -> ~d_L ~b_2 + c.c. 1356 | 7 1 1 | 9.679e-15 9.679e-15 | | q q' -> ~u_L ~u_L + c.c. 1357 | 4520 542 542 | 2.102e-11 4.986e-13 | | q q' -> ~u_L ~c_L + c.c. 1358 | 139 15 15 | 5.313e-13 8.662e-14 | | q q' -> ~u_L ~u_R + c.c. 1360 | 3272 374 374 | 1.494e-11 4.618e-13 | | q q' -> ~u_L ~c_R + c.c. 1361 | 37 2 2 | 6.931e-14 2.819e-14 | | q q' -> ~u_L ~d_L + c.c. 1363 | 6568 691 691 | 2.810e-11 5.920e-13 | | q q' -> ~u_L ~s_L + c.c. 1364 | 325 40 40 | 1.545e-12 1.409e-13 | | q q' -> ~u_L ~b_1 + c.c. 1365 | 31 6 6 | 2.013e-13 4.909e-14 | | q q' -> ~u_L ~d_R + c.c. 1366 | 1831 130 130 | 5.250e-12 2.709e-13 | | q q' -> ~u_L ~s_R + c.c. 1367 | 87 4 4 | 2.076e-13 3.797e-14 | | q q' -> ~u_L ~b_2 + c.c. 1368 | 67 9 9 | 4.841e-13 8.633e-14 | | q q' -> ~s_L ~s_L + c.c. 1369 | 12 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~s_L ~b_1 + c.c. 1370 | 3 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~s_L ~d_R + c.c. 1371 | 35 3 3 | 8.292e-14 2.361e-14 | | q q' -> ~s_L ~s_R + c.c. 1372 | 2 1 1 | 1.165e-14 1.165e-14 | | q q' -> ~s_L ~b_2 + c.c. 1373 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_L ~c_L + c.c. 1374 | 1 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_L ~u_R + c.c. 1376 | 33 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_L ~c_R + c.c. 1377 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_L ~d_L + c.c. 1379 | 84 14 14 | 3.186e-13 5.501e-14 | | q q' -> ~c_L ~s_L + c.c. 1380 | 12 1 1 | 4.926e-14 4.926e-14 | | q q' -> ~c_L ~b_1 + c.c. 1381 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_L ~d_R + c.c. 1382 | 13 2 2 | 1.043e-13 3.403e-14 | | q q' -> ~c_L ~s_R + c.c. 1383 | 1 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_L ~b_2 + c.c. 1384 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~b_1 ~b_1 + c.c. 1385 | 1 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~b_1 ~d_R + c.c. 1386 | 10 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~b_1 ~s_R + c.c. 1387 | 1 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~b_1 ~b_2 + c.c. 1388 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~t_1 ~d_L + c.c. 1393 | 11 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~t_1 ~s_L + c.c. 1394 | 2 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~t_1 ~b_1 + c.c. 1395 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~t_1 ~b_2 + c.c. 1398 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~d_R ~d_R + c.c. 1399 | 727 93 93 | 3.226e-12 1.997e-13 | | q q' -> ~d_R ~s_R + c.c. 1400 | 173 9 9 | 5.179e-13 7.595e-14 | | q q' -> ~d_R ~b_2 + c.c. 1401 | 46 3 3 | 1.156e-13 3.463e-14 | | q q' -> ~u_R ~u_R + c.c. 1402 | 3978 540 540 | 2.227e-11 5.286e-13 | | q q' -> ~u_R ~c_R + c.c. 1403 | 174 16 16 | 6.968e-13 9.604e-14 | | q q' -> ~u_R ~d_L + c.c. 1405 | 1823 137 137 | 5.493e-12 2.749e-13 | | q q' -> ~u_R ~s_L + c.c. 1406 | 73 5 5 | 2.935e-13 6.540e-14 | | q q' -> ~u_R ~b_1 + c.c. 1407 | 109 17 17 | 5.458e-13 8.747e-14 | | q q' -> ~u_R ~d_R + c.c. 1408 | 5546 590 590 | 2.249e-11 5.283e-13 | | q q' -> ~u_R ~s_R + c.c. 1409 | 377 42 42 | 1.523e-12 1.378e-13 | | q q' -> ~u_R ~b_2 + c.c. 1410 | 35 4 4 | 1.988e-13 5.565e-14 | | q q' -> ~s_R ~s_R + c.c. 1411 | 9 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~s_R ~b_2 + c.c. 1412 | 2 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_R ~c_R + c.c. 1413 | 3 1 1 | 1.226e-14 1.226e-14 | | q q' -> ~c_R ~d_L + c.c. 1415 | 18 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_R ~s_L + c.c. 1416 | 4 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_R ~b_1 + c.c. 1417 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_R ~d_R + c.c. 1418 | 82 5 5 | 2.366e-13 6.518e-14 | | q q' -> ~c_R ~s_R + c.c. 1419 | 6 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~c_R ~b_2 + c.c. 1420 | 2 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~b_2 ~b_2 + c.c. 1421 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~t_2 ~d_L + c.c. 1423 | 1 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~t_2 ~s_L + c.c. 1424 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~t_2 ~b_1 + c.c. 1425 | 0 0 0 | 0.000e+00 0.000e+00 | | q q' -> ~t_2 ~b_2 + c.c. 1428 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_10 ~d_L + c.c. (q=d,s,b) 1431 | 23 5 5 | 1.619e-13 5.543e-14 | | q g -> ~chi_10 ~u_L + c.c. (q=u,c) 1432 | 46 2 2 | 1.586e-13 4.322e-14 | | q g -> ~chi_10 ~s_L + c.c. (q=d,s,b) 1433 | 9 1 1 | 3.399e-14 3.399e-14 | | q g -> ~chi_10 ~c_L + c.c. (q=u,c) 1434 | 1 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_10 ~b_1 + c.c. (q=d,s,b) 1435 | 3 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_10 ~d_R + c.c. (q=d,s,b) 1437 | 118 19 19 | 7.660e-13 9.908e-14 | | q g -> ~chi_10 ~u_R + c.c. (q=u,c) 1438 | 1117 149 149 | 5.885e-12 2.734e-13 | | q g -> ~chi_10 ~s_R + c.c. (q=d,s,b) 1439 | 16 1 1 | 1.990e-14 1.990e-14 | | q g -> ~chi_10 ~c_R + c.c. (q=u,c) 1440 | 41 3 3 | 1.572e-13 5.527e-14 | | q g -> ~chi_10 ~b_2 + c.c. (q=d,s,b) 1441 | 9 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_20 ~d_L + c.c. (q=d,s,b) 1443 | 367 39 39 | 2.187e-12 1.832e-13 | | q g -> ~chi_20 ~u_L + c.c. (q=u,c) 1444 | 829 114 114 | 4.786e-12 2.575e-13 | | q g -> ~chi_20 ~s_L + c.c. (q=d,s,b) 1445 | 54 4 4 | 1.191e-13 3.232e-14 | | q g -> ~chi_20 ~c_L + c.c. (q=u,c) 1446 | 31 1 1 | 7.297e-14 7.297e-14 | | q g -> ~chi_20 ~b_1 + c.c. (q=d,s,b) 1447 | 34 1 1 | 6.194e-14 6.194e-14 | | q g -> ~chi_20 ~d_R + c.c. (q=d,s,b) 1449 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_20 ~u_R + c.c. (q=u,c) 1450 | 1 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_20 ~s_R + c.c. (q=d,s,b) 1451 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_20 ~c_R + c.c. (q=u,c) 1452 | 1 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_20 ~b_2 + c.c. (q=d,s,b) 1453 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_30 ~d_L + c.c. (q=d,s,b) 1455 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_30 ~u_L + c.c. (q=u,c) 1456 | 1 1 1 | 1.037e-14 1.037e-14 | | q g -> ~chi_30 ~s_L + c.c. (q=d,s,b) 1457 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_30 ~c_L + c.c. (q=u,c) 1458 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_30 ~b_1 + c.c. (q=d,s,b) 1459 | 1 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_30 ~d_R + c.c. (q=d,s,b) 1461 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_30 ~u_R + c.c. (q=u,c) 1462 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_30 ~s_R + c.c. (q=d,s,b) 1463 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_30 ~c_R + c.c. (q=u,c) 1464 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_30 ~b_2 + c.c. (q=d,s,b) 1465 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_40 ~d_L + c.c. (q=d,s,b) 1467 | 16 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_40 ~u_L + c.c. (q=u,c) 1468 | 25 4 4 | 8.633e-14 2.528e-14 | | q g -> ~chi_40 ~s_L + c.c. (q=d,s,b) 1469 | 3 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_40 ~c_L + c.c. (q=u,c) 1470 | 2 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_40 ~b_1 + c.c. (q=d,s,b) 1471 | 1 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_40 ~d_R + c.c. (q=d,s,b) 1473 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_40 ~u_R + c.c. (q=u,c) 1474 | 1 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_40 ~s_R + c.c. (q=d,s,b) 1475 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_40 ~c_R + c.c. (q=u,c) 1476 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_40 ~b_2 + c.c. (q=d,s,b) 1477 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_1+ ~d_L + c.c. (q=u,c) 1491 | 3962 553 553 | 2.249e-11 5.607e-13 | | q g -> ~chi_1- ~u_L + c.c. (q=d,s,b) 1492 | 1877 212 212 | 9.513e-12 3.826e-13 | | q g -> ~chi_1+ ~s_L + c.c. (q=u,c) 1493 | 358 32 32 | 1.696e-12 1.439e-13 | | q g -> ~chi_1- ~c_L + c.c. (q=d,s,b) 1494 | 416 37 37 | 1.438e-12 1.394e-13 | | q g -> ~chi_1+ ~b_1 + c.c. (q=u,c) 1495 | 1 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_1- ~t_1 + c.c. (q=d,s,b) 1496 | 412 34 34 | 1.547e-12 1.470e-13 | | q g -> ~chi_1+ ~b_2 + c.c. (q=u,c) 1501 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_1- ~t_2 + c.c. (q=d,s,b) 1502 | 5 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_2+ ~d_L + c.c. (q=u,c) 1503 | 153 23 23 | 8.935e-13 1.114e-13 | | q g -> ~chi_2- ~u_L + c.c. (q=d,s,b) 1504 | 87 11 11 | 3.109e-13 6.047e-14 | | q g -> ~chi_2+ ~s_L + c.c. (q=u,c) 1505 | 18 1 1 | 2.442e-14 2.442e-14 | | q g -> ~chi_2- ~c_L + c.c. (q=d,s,b) 1506 | 17 4 4 | 9.385e-14 3.551e-14 | | q g -> ~chi_2+ ~b_1 + c.c. (q=u,c) 1507 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_2- ~t_1 + c.c. (q=d,s,b) 1508 | 249 22 22 | 8.811e-13 1.172e-13 | | q g -> ~chi_2+ ~b_2 + c.c. (q=u,c) 1513 | 0 0 0 | 0.000e+00 0.000e+00 | | q g -> ~chi_2- ~t_2 + c.c. (q=d,s,b) 1514 | 5 1 1 | 7.155e-14 7.155e-14 | | q qbar' -> ~chi_10 ~chi_10 1551 | 141 18 18 | 5.072e-13 7.939e-14 | | q qbar' -> ~chi_10 ~chi_20 1552 | 15 1 1 | 5.193e-14 5.193e-14 | | q qbar' -> ~chi_20 ~chi_20 1553 | 96 14 14 | 4.952e-13 8.264e-14 | | q qbar' -> ~chi_10 ~chi_30 1554 | 5 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_20 ~chi_30 1555 | 19 3 3 | 1.044e-13 2.704e-14 | | q qbar' -> ~chi_30 ~chi_30 1556 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_10 ~chi_40 1557 | 1 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_20 ~chi_40 1558 | 2 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_30 ~chi_40 1559 | 96 14 14 | 5.551e-13 8.107e-14 | | q qbar' -> ~chi_40 ~chi_40 1560 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_1+ ~chi_10 1571 | 37 3 3 | 1.152e-13 3.228e-14 | | q qbar' -> ~chi_1- ~chi_10 1572 | 11 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_2+ ~chi_10 1573 | 9 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_2- ~chi_10 1574 | 3 1 1 | 3.414e-15 3.414e-15 | | q qbar' -> ~chi_1+ ~chi_20 1575 | 2569 487 487 | 1.878e-11 5.000e-13 | | q qbar' -> ~chi_1- ~chi_20 1576 | 1167 184 184 | 7.588e-12 3.225e-13 | | q qbar' -> ~chi_2+ ~chi_20 1577 | 3 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_2- ~chi_20 1578 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_1+ ~chi_30 1579 | 22 6 6 | 1.903e-13 5.345e-14 | | q qbar' -> ~chi_1- ~chi_30 1580 | 8 1 1 | 5.394e-14 5.394e-14 | | q qbar' -> ~chi_2+ ~chi_30 1581 | 152 33 33 | 1.260e-12 1.191e-13 | | q qbar' -> ~chi_2- ~chi_30 1582 | 52 11 11 | 3.765e-13 7.035e-14 | | q qbar' -> ~chi_1+ ~chi_40 1583 | 2 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_1- ~chi_40 1584 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar' -> ~chi_2+ ~chi_40 1585 | 153 24 24 | 9.079e-13 1.014e-13 | | q qbar' -> ~chi_2- ~chi_40 1586 | 48 8 8 | 2.566e-13 5.910e-14 | | q qbar' -> ~chi_1+ ~chi_1- 1591 | 1939 332 332 | 1.381e-11 4.219e-13 | | q qbar' -> ~chi_1+ ~chi_2- 1592 | 4 1 1 | 1.088e-13 1.088e-13 | | q qbar' -> ~chi_2+ ~chi_1- 1593 | 6 1 1 | 5.438e-14 5.438e-14 | | q qbar' -> ~chi_2+ ~chi_2- 1594 | 100 15 15 | 6.950e-13 9.517e-14 | | q qbar' -> ~g ~chi_10 1601 | 320 46 46 | 1.731e-12 1.606e-13 | | q qbar' -> ~g ~chi_20 1602 | 355 34 34 | 1.219e-12 1.290e-13 | | q qbar' -> ~g ~chi_30 1603 | 5 1 1 | 2.819e-14 2.819e-14 | | q qbar' -> ~g ~chi_40 1604 | 8 2 2 | 5.032e-14 2.277e-14 | | q qbar' -> ~g ~chi_1+ + c.c 1621 | 753 88 88 | 3.683e-12 2.281e-13 | | q qbar' -> ~g ~chi_2+ + c.c 1622 | 21 3 3 | 1.034e-13 4.189e-14 | | q qbar' -> ~e_L- ~e_L+ 1651 | 199 21 21 | 9.264e-13 1.068e-13 | | q qbar' -> ~nu_eL ~nu_eLbar 1662 | 211 21 21 | 8.296e-13 1.017e-13 | | q qbar' -> ~nu_eL ~e_L+ + c.c. 1673 | 758 70 70 | 3.207e-12 2.072e-13 | | q qbar' -> ~mu_L- ~mu_L+ 1679 | 172 24 24 | 9.285e-13 1.075e-13 | | q qbar' -> ~nu_muL ~nu_muLbar 1688 | 215 24 24 | 8.491e-13 1.036e-13 | | q qbar' -> ~nu_muL ~mu_L+ + c.c. 1698 | 709 86 86 | 3.400e-12 2.181e-13 | | q qbar' -> ~tau_1- ~tau_1+ 1703 | 603 87 87 | 3.053e-12 2.072e-13 | | q qbar' -> ~tau_1- ~tau_2+ 1708 | 256 35 35 | 1.282e-12 1.310e-13 | | q qbar' -> ~tau_2- ~tau_1+ 1709 | 236 26 26 | 9.915e-13 1.206e-13 | | q qbar' -> ~nu_tauL ~nu_tauLbar 1710 | 210 22 22 | 9.464e-13 1.138e-13 | | q qbar' -> ~nu_tauL ~tau_1+ + c.c. 1719 | 30 2 2 | 1.813e-13 5.629e-14 | | q qbar' -> ~nu_tauL ~tau_2+ + c.c. 1722 | 738 83 83 | 3.133e-12 2.091e-13 | | q qbar' -> ~e_R- ~e_R+ 1723 | 518 55 55 | 3.009e-12 2.179e-13 | | q qbar' -> ~mu_R- ~mu_R+ 1739 | 531 66 66 | 2.545e-12 1.887e-13 | | q qbar' -> ~tau_2- ~tau_2+ 1751 | 159 16 16 | 7.287e-13 9.916e-14 | | | | | | sum | 86891 10000 10000 | 4.012e-10 2.314e-12 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Warning in TauDecays::decay: maximum decay weight exceeded in tau decay | | 9600 Warning in TauDecays::decay: unknown tau production, assuming unpolarized and uncorrelated | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:07 deviation from energy-momentum conservation 1.00*10^ 4 X 0.96*10^ 4 X 0.92*10^ 4 X 0.88*10^ 4 X 0.84*10^ 4 X 0.80*10^ 4 X 0.76*10^ 4 X 0.72*10^ 4 X 0.68*10^ 4 X 0.64*10^ 4 X 0.60*10^ 4 X 0.56*10^ 4 X 0.52*10^ 4 X 0.48*10^ 4 X 0.44*10^ 4 X 0.40*10^ 4 X 0.36*10^ 4 X 0.32*10^ 4 X 0.28*10^ 4 X 0.24*10^ 4 X 0.20*10^ 4 X 0.16*10^ 4 X 0.12*10^ 4 X 0.08*10^ 4 X 0.04*10^ 4 X Contents *10^ 4 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^-3 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-4 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-5 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 10000 Mean = 5.0000e-05 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+04 Rms = 0.0000e+00 Overflow = 0.0000e+00 High edge = 1.0000e-02 2013-09-20 16:07 final particle multiplicity 6.25*10^ 3 5 6.00*10^ 3 X 5.75*10^ 3 X 5.50*10^ 3 X 5.25*10^ 3 X 5.00*10^ 3 X 4.75*10^ 3 X 4.50*10^ 3 X 4.25*10^ 3 X 4.00*10^ 3 X 3.75*10^ 3 X 3.50*10^ 3 X 3.25*10^ 3 X 3.00*10^ 3 X 2.75*10^ 3 X 2.50*10^ 3 X8 2.25*10^ 3 XX 2.00*10^ 3 XX 1.75*10^ 3 XX 1.50*10^ 3 XX 1.25*10^ 3 9XX 1.00*10^ 3 XXX 0.75*10^ 3 XXX 0.50*10^ 3 XXX 0.25*10^ 3 XXX8 Contents *10^ 3 1620000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 2141000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 1259100000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 5717000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 10000 Mean = 1.2828e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+04 Rms = 5.2267e+00 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:07 dn/dy for particles 7.80*10^ 3 561 7.50*10^ 3 XXX 7.20*10^ 3 8XXX 6.90*10^ 3 2XXXX7 6.60*10^ 3 XXXXXX 6.30*10^ 3 XXXXXX1 6.00*10^ 3 6XXXXXXX 5.70*10^ 3 XXXXXXXX 5.40*10^ 3 XXXXXXXX 5.10*10^ 3 5XXXXXXXX7 4.80*10^ 3 XXXXXXXXXX 4.50*10^ 3 XXXXXXXXXX 4.20*10^ 3 4XXXXXXXXXXX 3.90*10^ 3 XXXXXXXXXXXX 3.60*10^ 3 XXXXXXXXXXXX 3.30*10^ 3 7XXXXXXXXXXXX6 3.00*10^ 3 XXXXXXXXXXXXXX 2.70*10^ 3 1XXXXXXXXXXXXXX 2.40*10^ 3 XXXXXXXXXXXXXXX8 2.10*10^ 3 XXXXXXXXXXXXXXXX 2 1.80*10^ 3 37X4 9XXXXXXXXXXXXXXXXX 5X92 1.50*10^ 3 XXXX2 1XXXXXXXXXXXXXXXXXX3 3XXXX 1.20*10^ 3 8XXXXX1 XXXXXXXXXXXXXXXXXXXX2 3XXXXX8 0.90*10^ 3 XXXXXXX4 8XXXXXXXXXXXXXXXXXXXXX 2XXXXXXX 0.60*10^ 3 9XXXXXXXX74211 14XXXXXXXXXXXXXXXXXXXXXXXX4 2237XXXXXXXX7 0.30*10^ 3 18XXXXXXXXXXXXXX9887655543433333457XXXXXXXXXXXXXXXXXXXXXXXXXXXX654343333445566588XXXXXXXXXXXXXXX71 Contents *10^ 3 0000111111000000000000000000000000000000112344567777665432110000000000000000000000000000001111110000 *10^ 2 0025157862975433322221111101100001123458274209861665800113829542111010000111111122323335692687515200 *10^ 1 0237480115211272253317553290098872501293473115845682020875096928952829889214568634085790778458431130 *10^ 0 9583718081395035766336745067414562886247221048773380693714603495485712337399251227293066285073864187 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 128105 Mean = 9.2795e-03 Underflow = 3.0000e+00 Low edge = -1.0000e+01 All chan = 1.2810e+05 Rms = 4.0874e+00 Overflow = 3.0000e+00 High edge = 1.0000e+01 pythia8-8.1.80.orig/examples/outref/out080000644000175000017500000005645412217346171016377 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:02:07 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* PYTHIA Error in Pythia::check: unmatched particle energy/momentum/mass PYTHIA Abort from Pythia::next: check of event revealed problems PYTHIA Warning in MultipartonInteractions::pTfirst: weight above unity PYTHIA Warning in MultipartonInteractions::pTnext: weight above unity PYTHIA Warning in PhaseSpace2to2tauyz::trialKin: maximum for cross section violated 2013-09-20 16:02 pTHat distribution, unweighted 1.35*10^ 4 47 1.30*10^ 4 XX 1.25*10^ 4 XX5 1.20*10^ 4 XXX 1.15*10^ 4 XXX 1.10*10^ 4 7XXX 1.05*10^ 4 XXXX8 1.00*10^ 4 XXXXX 0.95*10^ 4 XXXXX 0.90*10^ 4 XXXXX 0.85*10^ 4 XXXXX7 0.80*10^ 4 XXXXXX 0.75*10^ 4 XXXXXX 0.70*10^ 4 XXXXXX 0.65*10^ 4 XXXXXX3 0.60*10^ 4 XXXXXXX 0.55*10^ 4 XXXXXXX 0.50*10^ 4 4XXXXXXX3 0.45*10^ 4 XXXXXXXXX 0.40*10^ 4 XXXXXXXXX 0.35*10^ 4 XXXXXXXXX8 0.30*10^ 4 XXXXXXXXXX2 1 0.25*10^ 4 XXXXXXXXXXX X77663412 0.20*10^ 4 2XXXXXXXXXXX7 XXXXXXXXXX9X7764433221 2 0.15*10^ 4 XXXXXXXXXXXXX82 XXXXXXXXXXXXXXXXXXXXXXXX9999866554443432212 1 1 0.10*10^ 4 XXXXXXXXXXXXXXX73 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9XX9X899767777666666464534444334232 0.05*10^ 4 XXXXXXXXXXXXXXXXXX87XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 4 0011111000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 3 1403320864321110000022222222211211111111111111111111111111111111101000000000000000000000000000000000 *10^ 2 6681323316358308643353333120199088776666554544444322222111111000090999999888888788888776766677666666 *10^ 1 0849369744984893689536720727394246929732849975330283701849610682473839056525553921021289479810558231 Low edge *10^ 1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 0 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 198410 Mean = 2.8628e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.9841e+05 Rms = 2.7496e+01 Overflow = 0.0000e+00 High edge = 1.0000e+02 2013-09-20 16:02 pTHat distribution, weighted 7.80*10^ 0 36 7.50*10^ 0 XX 7.20*10^ 0 XX5 6.90*10^ 0 XXX 6.60*10^ 0 XXX 6.30*10^ 0 8XXX 6.00*10^ 0 XXXX9 5.70*10^ 0 XXXXX 5.40*10^ 0 XXXXX 5.10*10^ 0 XXXXX1 4.80*10^ 0 XXXXXX 4.50*10^ 0 XXXXXX 4.20*10^ 0 XXXXXX 3.90*10^ 0 XXXXXX 3.60*10^ 0 XXXXXX8 3.30*10^ 0 XXXXXXX 3.00*10^ 0 XXXXXXX 2.70*10^ 0 XXXXXXXX9 2.40*10^ 0 XXXXXXXXX 2.10*10^ 0 XXXXXXXXX5 1.80*10^ 0 XXXXXXXXXX 1.50*10^ 0 XXXXXXXXXX9 1.20*10^ 0 1XXXXXXXXXXX5 0.90*10^ 0 XXXXXXXXXXXXX61 0.60*10^ 0 XXXXXXXXXXXXXXX63 0.30*10^ 0 XXXXXXXXXXXXXXXXX97754332221111111 Contents *10^ 0 0267775432111000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 9625609856940764322111100000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 1939757137485927772952087554322211111000000000000000000000000000000000000000000000000000000000000000 *10^-3 8550167642929398753682241700695386420987665544333222222111111111111100000000000000000000000000000000 Low edge *10^ 1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 0 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 198410 Mean = 6.4833e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 5.7587e+01 Rms = 4.5420e+00 Overflow = 0.0000e+00 High edge = 1.0000e+02 2013-09-20 16:02 pTHat distribution, pT3*weighted 2.32*10^ 3 5 2.24*10^ 3 XXX 2.16*10^ 3 XXXX 2.08*10^ 3 2XXXX8 2.00*10^ 3 XXXXXX2 1.92*10^ 3 XXXXXXX8 1.84*10^ 3 XXXXXXXX2 1.76*10^ 3 XXXXXXXXX2 1.68*10^ 3 5XXXXXXXXXX 1.60*10^ 3 XXXXXXXXXXX 1.52*10^ 3 XXXXXXXXXXX4 1 1.44*10^ 3 XXXXXXXXXXXX6X 1.36*10^ 3 XXXXXXXXXXXXXXX 1.28*10^ 3 XXXXXXXXXXXXXXX1 1.20*10^ 3 7XXXXXXXXXXXXXXXX6 1.12*10^ 3 XXXXXXXXXXXXXXXXXX6 1.04*10^ 3 XXXXXXXXXXXXXXXXXXX9 0.96*10^ 3 XXXXXXXXXXXXXXXXXXXX76 0.88*10^ 3 XXXXXXXXXXXXXXXXXXXXXX43 0.80*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXX3 0.72*10^ 3 8XXXXXXXXXXXXXXXXXXXXXXXXX89 0.64*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXX872 0.56*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX741 0.48*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9641 1 0.40*10^ 3 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8X6421 0.32*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX753311 0.24*10^ 3 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX989765442212 0.16*10^ 3 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9X8896565554443432312 1 1 0.08*10^ 3 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9X998 Contents *10^ 3 0000011222222111111111111000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0013716012220997644432100998877766555444443433333222222222222111111111111111111111111010000000000000 *10^ 1 0103073158446307971561683323240021731965308065431986644323200998867655444322221111000908988888777776 *10^ 0 0264879973345989432030585962332953350082088462019504786440062230053219389046428141897408334252658018 Low edge *10^ 1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 0 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 198410 Mean = 2.6198e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 5.5321e+04 Rms = 2.0367e+01 Overflow = 0.0000e+00 High edge = 1.0000e+02 2013-09-20 16:02 pTHat distribution, pT5*weighted 7.80*10^ 5 5 31 1 5 6 2X 45 7.50*10^ 5 X1359X1 5 31 XX472X29 X6 X XX 153 654XX X 3 3 2 7.20*10^ 5 4 15543XXXXXXX73X6XX8XXXXXXXX7XX7X7XX4 9XXX3XXXXX X X XX X 6.90*10^ 5 3 X 9756XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9XXXXXXXXXX9X4X2X9XX77X283 6.60*10^ 5 7 X68XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 6.30*10^ 5 73XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 6.00*10^ 5 1 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 5.70*10^ 5 4X6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 5.40*10^ 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 5.10*10^ 5 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 4.80*10^ 5 4 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 4.50*10^ 5 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 4.20*10^ 5 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 3.90*10^ 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 3.60*10^ 5 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 3.30*10^ 5 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 3.00*10^ 5 9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 2.70*10^ 5 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 2.40*10^ 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 2.10*10^ 5 9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.80*10^ 5 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.50*10^ 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.20*10^ 5 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.90*10^ 5 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.60*10^ 5 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.30*10^ 5 15XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 5 0000000112223344444555566666666766666667777777777777777777777777777777777767777677777676766677667666 *10^ 4 0000136150492502658575802152645068877890000622345210303216533252406306058081232933366857269831782687 *10^ 3 0004469366763207113129910009863307249934430449571320690150209715895897950267338894215711850609915650 *10^ 2 0073729915282568553762509363666124250498630610340131010821375286150481746106674538387245101336655432 Low edge *10^ 1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 0 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 198410 Mean = 5.7207e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 6.0914e+07 Rms = 2.4918e+01 Overflow = 0.0000e+00 High edge = 1.0000e+02 pythia8-8.1.80.orig/examples/outref/out010000644000175000017500000050727612217346170016372 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:00:09 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 8.000e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> g g 111 | 2.223e+00 | | g g -> q qbar (uds) 112 | 2.283e-02 | | q g -> q g 113 | 1.242e+00 | | q q(bar)' -> q q(bar)' 114 | 1.294e-01 | | q qbar -> g g 115 | 9.369e-04 | | q qbar -> q' qbar' (uds) 116 | 4.182e-04 | | g g -> c cbar 121 | 7.525e-03 | | q qbar -> c cbar 122 | 1.386e-04 | | g g -> b bbar 123 | 6.766e-03 | | q qbar -> b bbar 124 | 1.311e-04 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 52.12 mb | | | | pT0 = 2.77 gives sigmaInteraction = 218.38 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eCM | 8000.000 | 14000.000 10.00000 | | HardQCD:all | on | off | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:pTHatMin | 20.00000 | 0.0 0.0 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 4.000e+03, e = 4.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -4.000e+03, e = 4.000e+03, m = 9.383e-01. In 1: id = 21, x = 1.513e-02, pdf = 5.952e+00 at Q2 = 4.117e+02. In 2: id = 21, x = 3.405e-02, pdf = 3.148e+00 at same Q2. Subprocess g g -> g g with code 111 is 2 -> 2. It has sHat = 3.297e+04, tHat = -4.170e+02, uHat = -3.255e+04, pTHat = 2.029e+01, m3Hat = 0.000e+00, m4Hat = 0.000e+00, thetaHat = 2.254e-01, phiHat = 5.974e-01. alphaEM = 7.687e-03, alphaS = 1.794e-01 at Q2 = 4.117e+02. Impact parameter b = 7.973e-01 gives enhancement factor = 1.255e+00. Max pT scale for MPI = 2.029e+01, ISR = 2.029e+01, FSR = 2.029e+01. Number of MPI = 5, ISR = 12, FSRproc = 88, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 8000.000 8000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 4000.000 4000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -4000.000 4000.000 0.938 3 21 (g) -21 1 0 5 6 101 102 0.000 0.000 60.516 60.516 0.000 4 21 (g) -21 2 0 5 6 103 104 0.000 0.000 -136.203 136.203 0.000 5 21 g 23 3 4 0 0 101 104 16.776 11.413 58.028 61.473 0.000 6 21 g 23 3 4 0 0 103 102 -16.776 -11.413 -133.715 135.246 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 -75.687 196.719 181.576 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 8000.000 8000.000 1 2212 (p+) -12 0 0 378 0 0 0 0.000 0.000 4000.000 4000.000 0.938 2 2212 (p+) -12 0 0 379 0 0 0 0.000 0.000 -4000.000 4000.000 0.938 3 21 (g) -21 7 0 5 6 101 102 0.000 0.000 60.516 60.516 0.000 4 21 (g) -21 8 8 5 6 103 104 0.000 0.000 -136.203 136.203 0.000 5 21 (g) -23 3 4 9 9 101 104 16.776 11.413 58.028 61.473 0.000 6 21 (g) -23 3 4 10 10 103 102 -16.776 -11.413 -133.715 135.246 0.000 7 21 (g) -41 45 45 11 3 101 105 0.000 -0.000 87.477 87.477 0.000 8 21 (g) -42 44 44 4 4 103 104 -0.000 0.000 -136.203 136.203 0.000 9 21 (g) -44 5 5 42 43 101 104 3.197 16.909 59.903 62.326 0.000 10 21 (g) -44 6 6 48 48 103 102 -16.950 -11.342 -132.057 133.623 0.000 11 21 (g) -43 7 0 49 49 102 105 13.753 -5.567 23.428 27.731 0.000 12 21 (g) -31 16 0 14 15 106 107 0.000 0.000 0.145 0.145 0.000 13 21 (g) -31 17 17 14 15 108 109 0.000 0.000 -347.224 347.224 0.000 14 21 (g) -33 12 13 18 18 106 109 1.555 -5.730 -268.304 268.369 0.000 15 21 (g) -33 12 13 19 19 108 107 -1.555 5.730 -78.776 79.000 0.000 16 21 (g) -41 158 158 20 12 110 107 0.000 0.000 3.328 3.328 0.000 17 21 (g) -42 159 0 13 13 108 109 -0.000 0.000 -347.224 347.224 0.000 18 21 (g) -44 14 14 39 40 106 109 1.641 -6.968 -337.266 337.342 0.000 19 21 (g) -44 15 15 161 161 108 107 -1.263 1.520 -7.432 7.690 0.000 20 21 (g) -43 16 0 41 41 110 106 -0.378 5.447 0.802 5.519 0.000 21 21 (g) -31 34 0 23 24 112 113 0.000 0.000 5.572 5.572 0.000 22 3 (s) -31 35 35 23 24 111 0 0.000 0.000 -8.431 8.431 0.000 23 21 (g) -33 21 22 36 36 111 113 -0.302 5.197 -5.968 7.920 0.000 24 3 (s) -33 21 22 37 37 112 0 0.302 -5.197 3.109 6.084 0.500 25 21 (g) -31 29 0 27 28 114 115 0.000 0.000 8.447 8.447 0.000 26 21 (g) -31 30 30 27 28 116 117 0.000 0.000 -57.392 57.392 0.000 27 21 (g) -33 25 26 31 31 114 117 -3.593 -3.713 -56.473 56.709 0.000 28 21 (g) -33 25 26 32 32 116 115 3.593 3.713 7.528 9.131 0.000 29 21 (g) -41 58 58 33 25 114 118 0.000 -0.000 270.561 270.561 0.000 30 21 (g) -42 59 0 26 26 116 117 -0.000 -0.000 -57.392 57.392 0.000 31 21 (g) -44 27 27 60 60 114 117 -3.640 -3.765 -57.246 57.485 0.000 32 21 (g) -44 28 28 61 61 116 115 0.323 0.028 8.437 8.443 0.000 33 21 (g) -43 29 0 62 62 115 118 3.316 3.737 261.978 262.026 0.000 34 21 (g) -41 176 176 38 21 119 113 0.000 0.000 25.199 25.199 0.000 35 3 (s) -42 287 287 22 22 111 0 -0.000 0.000 -8.431 8.431 0.000 36 21 (g) -44 23 23 174 175 111 113 -1.039 5.205 -5.314 7.511 0.000 37 3 (s) -44 24 24 106 107 112 0 -3.173 -5.159 3.390 6.959 0.500 38 21 (g) -43 34 0 108 108 119 112 4.212 -0.046 18.692 19.161 0.000 39 21 (g) -51 18 0 111 111 120 109 5.118 -4.553 -277.928 278.013 0.000 40 21 (g) -51 18 0 66 66 106 120 -3.486 -2.282 -59.318 59.465 0.000 41 21 (g) -52 20 20 64 65 110 106 -0.369 5.314 0.782 5.384 0.000 42 21 (g) -51 9 0 47 47 101 121 4.956 11.722 49.695 51.299 0.000 43 21 (g) -51 9 0 50 50 121 104 -1.759 5.187 9.912 11.324 0.000 44 21 (g) -53 46 0 8 8 103 104 -0.000 0.000 -136.500 136.500 0.000 45 21 (g) -42 73 73 7 7 101 105 0.000 -0.000 87.477 87.477 0.000 46 21 (g) -41 57 57 51 44 122 104 -0.000 0.000 -156.361 156.361 0.000 47 21 (g) -44 42 42 76 76 101 121 4.973 11.717 49.627 51.233 0.000 48 21 (g) -44 10 10 52 53 103 102 -14.149 -12.286 -132.385 133.704 0.000 49 21 (g) -44 11 11 54 54 102 105 13.798 -5.582 23.550 27.860 0.000 50 21 (g) -44 43 43 79 79 121 104 -1.744 5.182 9.857 11.272 0.000 51 21 (g) -43 46 0 55 56 122 103 -2.878 0.970 -19.534 19.769 0.000 52 21 (g) -51 48 0 77 77 103 123 -12.080 -11.554 -97.066 98.495 0.000 53 21 (g) -51 48 0 81 81 123 102 -2.022 -0.752 -35.238 35.304 0.000 54 21 (g) -52 49 49 71 72 102 105 13.751 -5.563 23.470 27.765 0.000 55 -4 (cbar) -51 51 0 80 80 0 103 -2.431 1.643 -83.837 83.901 1.500 56 4 (c) -51 51 0 82 82 122 0 -0.447 -0.673 -8.457 8.627 1.500 57 21 (g) -53 75 75 46 46 122 104 0.000 -0.000 -229.120 229.120 0.000 58 21 (g) -42 96 96 29 29 114 118 -0.000 0.000 270.561 270.561 0.000 59 21 (g) -41 97 0 63 30 116 124 0.000 -0.000 -84.113 84.113 0.000 60 21 (g) -44 31 31 98 98 114 117 -5.685 -2.173 -57.223 57.546 0.000 61 21 (g) -44 32 32 99 99 116 115 0.323 0.028 8.429 8.435 0.000 62 21 (g) -44 33 33 100 100 115 118 3.316 3.738 261.882 261.929 0.000 63 21 (g) -43 59 0 101 101 117 124 2.047 -1.593 -26.639 26.765 0.000 64 21 (g) -51 41 0 162 162 110 125 -2.136 2.780 1.197 3.705 0.000 65 21 (g) -51 41 0 155 156 125 106 1.630 2.444 -2.764 4.033 0.000 66 21 (g) -52 40 40 109 110 106 120 -3.348 -2.191 -56.970 57.110 0.000 67 21 (g) -31 88 0 69 70 126 127 0.000 0.000 0.370 0.370 0.000 68 21 (g) -31 89 89 69 70 127 128 0.000 0.000 -207.796 207.796 0.000 69 21 (g) -33 67 68 90 90 126 129 1.410 1.554 -2.654 3.383 0.000 70 21 (g) -33 67 68 91 91 129 128 -1.410 -1.554 -204.771 204.782 0.000 71 21 (g) -51 54 0 78 78 102 130 10.707 -5.874 17.752 21.547 0.000 72 21 (g) -51 54 0 83 83 130 105 3.044 0.311 9.118 9.618 0.000 73 21 (g) -53 74 0 45 45 101 105 0.000 -0.000 90.877 90.877 0.000 74 21 (g) -41 124 124 84 73 101 131 -0.000 0.000 108.941 108.941 0.000 75 21 (g) -42 125 0 57 57 122 104 0.000 -0.000 -229.120 229.120 0.000 76 21 (g) -44 47 47 126 126 101 121 3.975 11.731 49.682 51.202 0.000 77 21 (g) -44 52 52 87 87 103 123 -12.094 -11.553 -97.161 98.590 0.000 78 21 (g) -44 71 71 95 95 102 130 10.318 -5.868 17.862 21.446 0.000 79 21 (g) -44 50 50 129 129 121 104 -1.953 5.185 9.841 11.294 0.000 80 -4 (cbar) -44 55 55 130 130 0 103 -2.432 1.643 -83.841 83.906 1.500 81 21 (g) -44 53 53 85 86 123 102 -2.023 -0.752 -35.250 35.316 0.000 82 4 (c) -44 56 56 132 132 122 0 -0.448 -0.673 -8.459 8.629 1.500 83 21 (g) -44 72 72 93 94 130 105 2.859 0.313 9.150 9.591 0.000 84 21 (g) -43 74 0 134 134 105 131 1.799 -0.026 17.997 18.087 0.000 85 21 (g) -51 81 0 131 131 132 102 -1.344 -1.250 -33.974 34.023 0.000 86 21 (g) -51 81 0 135 135 123 132 -4.724 -3.367 -33.777 34.271 0.000 87 21 (g) -52 77 77 127 127 103 123 -8.049 -7.689 -64.660 65.611 0.000 88 21 (g) -41 482 482 92 67 126 133 -0.000 -0.000 46.605 46.605 0.000 89 21 (g) -42 359 359 68 68 127 128 0.000 0.000 -207.796 207.796 0.000 90 21 (g) -44 69 69 103 104 126 129 1.045 -0.055 -0.376 1.112 0.000 91 21 (g) -44 70 70 105 105 129 128 -1.416 -1.577 -207.031 207.042 0.000 92 21 (g) -43 88 0 357 358 127 133 0.371 1.632 46.216 46.246 0.000 93 21 (g) -51 83 0 133 133 134 105 0.931 -0.716 0.686 1.360 0.000 94 21 (g) -51 83 0 136 136 130 134 5.821 -1.185 15.203 16.322 0.000 95 21 (g) -52 78 78 128 128 102 130 6.425 -3.654 11.123 13.355 0.000 96 21 (g) -42 114 114 58 58 114 118 -0.000 -0.000 270.561 270.561 0.000 97 21 (g) -41 139 139 102 59 135 124 0.000 0.000 -109.702 109.702 0.000 98 21 (g) -44 60 60 112 113 114 117 -5.352 -1.153 -57.261 57.522 0.000 99 21 (g) -44 61 61 141 141 116 115 0.323 0.028 8.429 8.435 0.000 100 21 (g) -44 62 62 142 142 115 118 3.316 3.738 261.894 261.941 0.000 101 21 (g) -44 63 63 120 120 117 124 2.201 -1.118 -26.648 26.762 0.000 102 21 (g) -43 97 0 144 144 135 116 -0.488 -1.496 -25.555 25.603 0.000 103 2 (u) -51 90 0 484 484 126 0 -1.307 0.035 -6.924 7.054 0.330 104 -2 (ubar) -51 90 0 117 117 0 129 2.280 -0.171 -4.096 4.703 0.330 105 21 (g) -52 91 91 115 116 129 128 -1.343 -1.496 -196.386 196.397 0.000 106 3 (s) -51 37 0 185 185 137 0 -3.485 -4.685 4.842 7.602 0.500 107 21 (g) -51 37 0 179 179 112 137 0.628 -0.478 -0.053 0.791 0.000 108 21 (g) -52 38 38 177 178 119 112 3.897 -0.043 17.294 17.727 0.000 109 21 (g) -51 66 0 157 157 106 138 -3.334 -2.433 -81.066 81.171 0.000 110 21 (g) -51 66 0 165 165 138 120 0.487 -0.205 -3.180 3.223 0.000 111 21 (g) -52 39 39 160 160 120 109 4.616 -4.106 -250.653 250.729 0.000 112 21 (g) -51 98 0 118 119 139 117 -5.287 0.142 -48.891 49.177 0.000 113 21 (g) -51 98 0 145 145 114 139 -0.066 -1.295 -8.307 8.408 0.000 114 21 (g) -53 138 0 96 96 114 118 0.000 -0.000 270.624 270.624 0.000 115 21 (g) -51 105 0 221 221 140 128 -0.611 -2.253 -129.221 129.242 0.000 116 21 (g) -51 105 0 171 172 129 140 -0.663 0.752 -67.283 67.291 0.000 117 -2 (ubar) -52 104 104 173 173 0 129 2.211 -0.166 -3.978 4.567 0.330 118 21 (g) -51 112 0 140 140 139 141 -0.633 -0.122 -1.647 1.768 0.000 119 21 (g) -51 112 0 123 123 141 117 -4.315 0.092 -51.342 51.523 0.000 120 21 (g) -52 101 101 121 122 117 124 1.863 -0.946 -22.550 22.647 0.000 121 21 (g) -51 120 0 143 143 142 124 1.275 0.556 -15.939 16.000 0.000 122 21 (g) -51 120 0 147 147 117 142 -0.212 -1.485 -16.127 16.197 0.000 123 21 (g) -52 119 119 146 146 141 117 -3.515 0.075 -41.826 41.974 0.000 124 21 (g) -42 242 242 74 74 101 131 -0.000 0.000 108.941 108.941 0.000 125 21 (g) -41 379 379 137 75 122 143 0.000 -0.000 -549.282 549.282 0.000 126 21 (g) -44 76 76 240 241 101 121 3.977 11.728 49.662 51.183 0.000 127 21 (g) -44 87 87 152 153 103 123 -7.854 -7.959 -64.657 65.617 0.000 128 21 (g) -44 95 95 149 150 102 130 6.429 -3.659 11.140 13.372 0.000 129 21 (g) -44 79 79 189 190 121 104 -1.951 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143.692 0.000 541 21 (g) -71 505 505 543 550 120 170 1.001 -2.494 -87.713 87.755 0.517 542 -3 (sbar) -71 502 502 543 550 0 120 -0.134 1.074 -309.087 309.089 0.500 543 4214 (Sigma*_c+) -83 538 542 877 878 0 0 0.156 -0.368 -26.411 26.537 2.546 544 113 (rho0) -83 538 542 768 769 0 0 -0.202 -0.576 -9.379 9.435 0.817 545 -2212 pbar- 83 538 542 0 0 0 0 1.603 -1.623 -81.957 81.994 0.938 546 111 (pi0) -83 538 542 879 880 0 0 1.524 -0.413 -45.607 45.635 0.135 547 111 (pi0) -84 538 542 881 882 0 0 -0.096 0.023 -40.604 40.604 0.135 548 2212 p+ 84 538 542 0 0 0 0 1.772 -2.422 -116.413 116.456 0.938 549 -2112 nbar0 84 538 542 0 0 0 0 -0.439 -0.203 -157.170 157.173 0.940 550 311 (K0) -84 538 542 770 770 0 0 0.008 0.472 -115.772 115.774 0.498 551 1 (d) -71 437 437 560 573 147 0 -0.443 0.461 -4.603 4.659 0.330 552 21 (g) -71 511 511 560 573 138 147 0.813 -0.249 -11.780 11.821 0.494 553 21 (g) -71 385 385 560 573 132 138 -1.025 -0.846 -12.976 13.044 0.000 554 21 (g) -71 404 404 560 573 172 132 -3.205 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-0.263 -16.395 16.409 0.140 815 111 (pi0) -91 666 0 1001 1002 0 0 0.397 -0.367 -17.047 17.056 0.135 816 211 pi+ 91 668 0 0 0 0 0 0.263 -0.120 -1.080 1.127 0.140 817 -211 pi- 91 668 0 0 0 0 0 -0.161 0.430 -0.942 1.057 0.140 818 -211 pi- 91 670 0 0 0 0 0 0.086 0.255 -0.024 0.304 0.140 819 111 (pi0) -91 670 0 1003 1004 0 0 -0.813 0.269 -0.120 0.875 0.135 820 211 pi+ 91 673 0 0 0 0 0 -0.238 -0.382 -0.777 0.909 0.140 821 -211 pi- 91 673 0 0 0 0 0 0.073 0.419 0.150 0.472 0.140 822 211 pi+ 91 678 0 0 0 0 0 -0.102 2.218 -3.007 3.740 0.140 823 111 (pi0) -91 678 0 1005 1006 0 0 0.054 0.117 -0.079 0.203 0.135 824 211 pi+ 91 680 0 0 0 0 0 -0.111 -0.140 -0.695 0.731 0.140 825 111 (pi0) -91 680 0 1007 1008 0 0 -0.487 0.783 -2.247 2.433 0.135 826 -211 pi- 91 684 0 0 0 0 0 0.092 -0.092 -0.106 0.218 0.140 827 111 (pi0) -91 684 0 1009 1010 0 0 -0.662 0.144 0.299 0.752 0.135 828 310 (K_S0) -91 686 686 1011 1012 0 0 0.399 0.348 2.540 2.642 0.498 829 130 K_L0 91 687 687 0 0 0 0 -0.812 0.804 2.189 2.519 0.498 830 -211 pi- 91 688 0 0 0 0 0 -0.249 1.518 5.099 5.327 0.140 831 111 (pi0) -91 688 0 1013 1014 0 0 0.333 0.768 1.733 1.929 0.135 832 211 pi+ 91 691 0 0 0 0 0 0.967 3.450 13.619 14.083 0.140 833 111 (pi0) -91 691 0 1015 1016 0 0 -0.060 0.436 3.258 3.290 0.135 834 211 pi+ 91 694 0 0 0 0 0 0.153 0.225 9.439 9.444 0.140 835 111 (pi0) -91 694 0 1017 1018 0 0 0.012 0.442 65.086 65.087 0.135 836 211 pi+ 91 695 0 0 0 0 0 0.045 0.048 1.087 1.098 0.140 837 -211 pi- 91 695 0 0 0 0 0 0.939 0.821 60.147 60.160 0.140 838 -211 pi- 91 697 0 0 0 0 0 0.136 0.947 45.174 45.185 0.140 839 111 (pi0) -91 697 0 1019 1020 0 0 -0.037 -0.064 8.213 8.215 0.135 840 211 pi+ 91 707 0 0 0 0 0 -0.131 -0.433 1.843 1.903 0.140 841 -211 pi- 91 707 0 0 0 0 0 0.167 -0.066 5.944 5.948 0.140 842 211 pi+ 91 727 0 0 0 0 0 -0.121 0.006 22.449 22.450 0.140 843 -211 pi- 91 727 0 0 0 0 0 0.764 -1.167 487.188 487.190 0.140 844 211 pi+ 91 729 0 0 0 0 0 0.301 -0.595 99.733 99.735 0.140 845 -211 pi- 91 729 0 0 0 0 0 0.184 0.344 40.385 40.387 0.140 846 -211 pi- 91 731 0 0 0 0 0 -0.175 -0.276 16.228 16.232 0.140 847 111 (pi0) -91 731 0 1021 1022 0 0 0.027 0.359 13.359 13.364 0.135 848 -211 pi- 91 733 0 0 0 0 0 0.591 0.254 5.599 5.637 0.140 849 111 (pi0) -91 733 0 1023 1024 0 0 -0.067 -0.022 10.575 10.577 0.135 850 130 K_L0 91 736 736 0 0 0 0 -0.224 0.065 0.190 0.581 0.498 851 211 pi+ 91 742 0 0 0 0 0 0.037 -0.006 -0.249 0.288 0.140 852 111 (pi0) -91 742 0 1025 1026 0 0 -0.548 0.583 -5.235 5.297 0.135 853 2212 p+ 91 744 0 0 0 0 0 0.317 0.140 -6.789 6.862 0.938 854 111 (pi0) -91 744 0 1027 1028 0 0 0.322 -0.096 -1.207 1.260 0.135 855 211 pi+ 91 747 0 0 0 0 0 -0.366 -0.401 -26.929 26.935 0.140 856 -211 pi- 91 747 0 0 0 0 0 0.133 -0.201 -3.134 3.146 0.140 857 -211 pi- 91 751 0 0 0 0 0 -0.569 -0.169 -26.872 26.879 0.140 858 111 (pi0) -91 751 0 1029 1030 0 0 -0.302 0.105 -2.871 2.892 0.135 859 311 (K0) -91 752 0 876 876 0 0 -0.175 -0.076 -6.239 6.262 0.498 860 211 pi+ 91 752 0 0 0 0 0 0.252 -0.251 -7.856 7.866 0.140 861 211 pi+ 91 754 0 0 0 0 0 -0.361 -0.731 -11.313 11.343 0.140 862 -211 pi- 91 754 0 0 0 0 0 0.111 0.154 -2.586 2.596 0.140 863 310 (K_S0) -91 756 756 1031 1032 0 0 0.086 -0.697 -9.779 9.817 0.498 864 130 K_L0 91 757 757 0 0 0 0 -1.042 0.321 -6.027 6.145 0.498 865 310 (K_S0) -91 758 758 1033 1034 0 0 -0.291 -0.867 -4.010 4.143 0.498 866 -321 K- 91 760 0 0 0 0 0 0.249 -0.030 0.792 0.966 0.494 867 211 pi+ 91 760 0 0 0 0 0 0.044 -0.067 -0.119 0.200 0.140 868 211 pi+ 91 763 0 0 0 0 0 -0.226 0.205 0.568 0.659 0.140 869 -211 pi- 91 763 0 0 0 0 0 0.322 -0.227 0.005 0.418 0.140 870 211 pi+ 91 764 0 0 0 0 0 -0.292 -0.748 60.726 60.731 0.140 871 -211 pi- 91 764 0 0 0 0 0 0.297 0.368 15.306 15.314 0.140 872 211 pi+ 91 765 0 0 0 0 0 -0.355 0.200 110.134 110.135 0.140 873 111 (pi0) -91 765 0 1035 1037 0 0 0.587 -0.108 355.758 355.758 0.135 874 -211 pi- 91 766 0 0 0 0 0 -0.261 -0.252 554.605 554.606 0.140 875 111 (pi0) -91 766 0 1038 1039 0 0 -0.748 0.083 683.590 683.590 0.135 876 310 (K_S0) -91 859 859 1040 1041 0 0 -0.175 -0.076 -6.239 6.262 0.498 877 4122 (Lambda_c+) -91 543 0 1042 1044 0 0 -0.004 -0.481 -24.273 24.385 2.286 878 111 (pi0) -91 543 0 1045 1046 0 0 0.160 0.114 -2.139 2.152 0.135 879 22 gamma 91 546 0 0 0 0 0 0.909 -0.312 -28.160 28.176 0.000 880 22 gamma 91 546 0 0 0 0 0 0.615 -0.101 -17.447 17.459 0.000 881 22 gamma 91 547 0 0 0 0 0 0.015 -0.016 -1.463 1.463 0.000 882 22 gamma 91 547 0 0 0 0 0 -0.112 0.039 -39.141 39.141 0.000 883 22 gamma 91 567 0 0 0 0 0 -0.119 -0.122 -1.089 1.103 0.000 884 22 gamma 91 567 0 0 0 0 0 -0.137 -0.267 -1.137 1.176 0.000 885 22 gamma 91 572 0 0 0 0 0 -0.336 -0.008 -6.851 6.859 0.000 886 22 gamma 91 572 0 0 0 0 0 -0.741 -0.206 -14.163 14.184 0.000 887 -421 (Dbar0) -91 573 0 1047 1049 0 0 -2.496 0.071 -80.617 80.678 1.865 888 -211 pi- 91 573 0 0 0 0 0 -0.187 -0.037 -6.149 6.153 0.140 889 22 gamma 91 580 0 0 0 0 0 -0.283 -0.332 -1.658 1.714 0.000 890 22 gamma 91 580 0 0 0 0 0 -0.071 -0.236 -0.895 0.928 0.000 891 211 pi+ 91 581 0 0 0 0 0 -0.357 -0.248 -8.044 8.057 0.140 892 -211 pi- 91 581 0 0 0 0 0 0.039 -0.085 -10.143 10.144 0.140 893 111 (pi0) -91 581 0 1050 1051 0 0 -0.181 -0.128 -3.157 3.168 0.135 894 22 gamma 91 582 0 0 0 0 0 -0.026 0.222 -58.194 58.195 0.000 895 22 gamma 91 582 0 0 0 0 0 0.059 0.167 -75.926 75.926 0.000 896 22 gamma 91 583 0 0 0 0 0 0.023 -0.094 -28.692 28.692 0.000 897 22 gamma 91 583 0 0 0 0 0 0.073 0.025 -38.035 38.035 0.000 898 111 (pi0) -91 586 0 1052 1053 0 0 0.549 0.083 -538.981 538.982 0.135 899 22 gamma 91 586 0 0 0 0 0 -0.082 0.255 -817.376 817.376 0.000 900 211 pi+ 91 604 0 0 0 0 0 0.095 -0.167 0.370 0.440 0.140 901 -211 pi- 91 604 0 0 0 0 0 -0.517 -0.317 0.917 1.108 0.140 902 111 (pi0) -91 604 0 1054 1055 0 0 -0.041 -0.021 0.498 0.518 0.135 903 22 gamma 91 607 0 0 0 0 0 -0.009 0.033 0.084 0.090 0.000 904 22 gamma 91 607 0 0 0 0 0 0.000 -0.118 0.651 0.662 0.000 905 22 gamma 91 608 0 0 0 0 0 0.045 -0.069 0.292 0.303 0.000 906 22 gamma 91 608 0 0 0 0 0 -0.058 -0.077 0.905 0.910 0.000 907 22 gamma 91 609 0 0 0 0 0 0.314 0.001 0.793 0.853 0.000 908 22 gamma 91 609 0 0 0 0 0 -0.213 -0.155 0.580 0.637 0.000 909 211 pi+ 91 610 0 0 0 0 0 -0.056 -0.115 0.148 0.241 0.140 910 -211 pi- 91 610 0 0 0 0 0 0.096 0.099 0.274 0.337 0.140 911 111 (pi0) -91 610 0 1056 1057 0 0 -0.275 -0.346 1.003 1.104 0.135 912 22 gamma 91 616 0 0 0 0 0 0.719 -0.081 2.643 2.740 0.000 913 22 gamma 91 616 0 0 0 0 0 0.202 -0.402 1.450 1.518 0.000 914 22 gamma 91 624 0 0 0 0 0 -0.085 -0.087 -0.053 0.133 0.000 915 22 gamma 91 624 0 0 0 0 0 -0.029 -0.258 -0.006 0.260 0.000 916 -2112 nbar0 91 626 0 0 0 0 0 -1.024 0.669 0.101 1.546 0.940 917 211 pi+ 91 626 0 0 0 0 0 -0.430 0.268 -0.194 0.560 0.140 918 22 gamma 91 628 0 0 0 0 0 -0.006 0.132 -0.395 0.416 0.000 919 22 gamma 91 628 0 0 0 0 0 0.144 0.181 -0.488 0.540 0.000 920 22 gamma 91 629 0 0 0 0 0 -0.072 -0.188 -0.624 0.656 0.000 921 22 gamma 91 629 0 0 0 0 0 0.059 -0.090 -0.297 0.315 0.000 922 2112 n0 91 663 0 0 0 0 0 -0.370 0.514 -236.113 236.116 0.940 923 -211 pi- 91 663 0 0 0 0 0 -0.161 0.033 -107.023 107.024 0.140 924 -2112 nbar0 91 664 0 0 0 0 0 0.068 -0.176 -49.655 49.664 0.940 925 211 pi+ 91 664 0 0 0 0 0 -0.134 0.075 -20.722 20.723 0.140 926 22 gamma 91 665 0 0 0 0 0 -0.746 0.485 -47.404 47.412 0.000 927 22 gamma 91 665 0 0 0 0 0 0.017 -0.070 -1.314 1.316 0.000 928 22 gamma 91 667 0 0 0 0 0 0.210 -0.100 -4.450 4.456 0.000 929 22 gamma 91 667 0 0 0 0 0 -0.263 0.155 -3.620 3.633 0.000 930 2212 p+ 91 674 0 0 0 0 0 0.517 0.466 -0.487 1.266 0.938 931 -211 pi- 91 674 0 0 0 0 0 0.057 0.204 -0.084 0.267 0.140 932 -2112 nbar0 91 675 0 0 0 0 0 -0.371 2.098 -2.246 3.235 0.940 933 211 pi+ 91 675 0 0 0 0 0 -0.280 0.348 -0.544 0.718 0.140 934 22 gamma 91 677 0 0 0 0 0 0.178 -0.057 -0.508 0.541 0.000 935 22 gamma 91 677 0 0 0 0 0 0.360 -0.049 -0.576 0.681 0.000 936 22 gamma 91 681 0 0 0 0 0 0.059 -0.021 -0.867 0.869 0.000 937 22 gamma 91 681 0 0 0 0 0 0.158 0.131 -1.466 1.480 0.000 938 111 (pi0) -91 696 0 1058 1059 0 0 1.018 0.707 48.939 48.955 0.135 939 22 gamma 91 696 0 0 0 0 0 0.411 -0.169 11.842 11.851 0.000 940 22 gamma 91 698 0 0 0 0 0 -0.119 -0.239 16.569 16.571 0.000 941 22 gamma 91 698 0 0 0 0 0 0.037 -0.044 3.479 3.479 0.000 942 22 gamma 91 699 0 0 0 0 0 0.018 -0.008 0.924 0.924 0.000 943 22 gamma 91 699 0 0 0 0 0 1.236 0.525 51.195 51.213 0.000 944 22 gamma 91 705 0 0 0 0 0 0.203 -0.035 4.249 4.254 0.000 945 22 gamma 91 705 0 0 0 0 0 0.477 0.108 8.551 8.565 0.000 946 111 (pi0) -91 706 0 1060 1061 0 0 -0.043 0.245 1.042 1.080 0.135 947 111 (pi0) -91 706 0 1062 1063 0 0 0.093 0.263 1.835 1.861 0.135 948 111 (pi0) -91 706 0 1064 1065 0 0 -0.029 0.359 1.058 1.126 0.135 949 211 pi+ 91 708 0 0 0 0 0 -0.164 0.189 0.341 0.445 0.140 950 -211 pi- 91 708 0 0 0 0 0 0.052 -0.132 0.507 0.544 0.140 951 111 (pi0) -91 708 0 1066 1067 0 0 -0.086 -0.114 0.022 0.198 0.135 952 211 pi+ 91 710 0 0 0 0 0 0.383 -0.073 -0.530 0.673 0.140 953 -211 pi- 91 710 0 0 0 0 0 0.565 -0.056 -0.357 0.685 0.140 954 111 (pi0) -91 710 0 1068 1069 0 0 0.155 -0.150 0.043 0.258 0.135 955 22 gamma 91 711 0 0 0 0 0 0.065 -0.035 -0.424 0.431 0.000 956 22 gamma 91 711 0 0 0 0 0 -0.024 -0.090 -1.483 1.486 0.000 957 111 (pi0) -91 728 0 1070 1071 0 0 -0.136 0.057 52.752 52.752 0.135 958 111 (pi0) -91 728 0 1072 1073 0 0 -0.162 0.171 30.949 30.950 0.135 959 111 (pi0) -91 728 0 1074 1075 0 0 -0.009 0.035 46.577 46.577 0.135 960 211 pi+ 91 735 0 0 0 0 0 -0.016 0.284 0.269 0.416 0.140 961 -211 pi- 91 735 0 0 0 0 0 -0.129 0.092 0.964 0.987 0.140 962 111 (pi0) -91 735 0 1076 1077 0 0 -0.002 -0.091 0.501 0.527 0.135 963 211 pi+ 91 739 0 0 0 0 0 -0.230 -0.248 -0.280 0.461 0.140 964 -211 pi- 91 739 0 0 0 0 0 0.073 0.025 -0.331 0.367 0.140 965 111 (pi0) -91 739 0 1078 1079 0 0 -0.328 0.050 -0.222 0.421 0.135 966 22 gamma 91 741 0 0 0 0 0 -0.011 -0.024 0.045 0.052 0.000 967 22 gamma 91 741 0 0 0 0 0 0.039 -0.328 0.017 0.331 0.000 968 22 gamma 91 743 0 0 0 0 0 0.646 0.194 -5.895 5.934 0.000 969 22 gamma 91 743 0 0 0 0 0 0.471 0.183 -5.496 5.519 0.000 970 -2112 nbar0 91 746 0 0 0 0 0 1.062 0.216 -15.157 15.224 0.940 971 -211 pi- 91 746 0 0 0 0 0 0.003 -0.092 -1.681 1.690 0.140 972 111 (pi0) -91 759 0 1080 1081 0 0 0.026 0.002 -0.480 0.499 0.135 973 111 (pi0) -91 759 0 1082 1083 0 0 -0.079 -0.160 -0.699 0.734 0.135 974 221 (eta) -91 759 0 1084 1086 0 0 -0.269 -0.033 -0.923 1.107 0.548 975 113 (rho0) -91 762 0 1087 1088 0 0 0.362 0.054 2.826 2.955 0.782 976 22 gamma 91 762 0 0 0 0 0 -0.032 -0.124 0.203 0.240 0.000 977 211 pi+ 91 770 0 0 0 0 0 0.152 0.046 -30.657 30.658 0.140 978 -211 pi- 91 770 0 0 0 0 0 -0.144 0.426 -85.115 85.116 0.140 979 22 gamma 91 772 0 0 0 0 0 -0.190 -0.078 -1.842 1.854 0.000 980 22 gamma 91 772 0 0 0 0 0 -0.273 -0.032 -1.500 1.525 0.000 981 22 gamma 91 774 0 0 0 0 0 -0.035 -0.098 -0.174 0.202 0.000 982 22 gamma 91 774 0 0 0 0 0 -0.004 -0.025 -0.405 0.406 0.000 983 22 gamma 91 786 0 0 0 0 0 0.008 -0.092 -1.053 1.057 0.000 984 22 gamma 91 786 0 0 0 0 0 0.191 -0.196 -1.852 1.872 0.000 985 22 gamma 91 788 0 0 0 0 0 -0.287 0.119 -79.788 79.789 0.000 986 22 gamma 91 788 0 0 0 0 0 0.009 0.030 -6.351 6.351 0.000 987 22 gamma 91 792 0 0 0 0 0 -0.112 -0.119 0.080 0.182 0.000 988 22 gamma 91 792 0 0 0 0 0 -0.060 -0.018 -0.047 0.079 0.000 989 22 gamma 91 794 0 0 0 0 0 0.158 0.339 1.107 1.169 0.000 990 22 gamma 91 794 0 0 0 0 0 0.048 0.167 0.863 0.880 0.000 991 22 gamma 91 798 0 0 0 0 0 0.145 -0.074 0.149 0.221 0.000 992 22 gamma 91 798 0 0 0 0 0 0.320 -0.418 0.394 0.657 0.000 993 22 gamma 91 802 0 0 0 0 0 0.350 0.001 0.657 0.744 0.000 994 22 gamma 91 802 0 0 0 0 0 0.752 -0.198 1.428 1.626 0.000 995 22 gamma 91 806 0 0 0 0 0 0.377 -0.164 1.117 1.190 0.000 996 22 gamma 91 806 0 0 0 0 0 0.979 -0.613 2.734 2.968 0.000 997 211 pi+ 91 811 0 0 0 0 0 0.155 0.910 -0.173 0.950 0.140 998 -211 pi- 91 811 0 0 0 0 0 -0.044 0.052 -0.030 0.158 0.140 999 22 gamma 91 813 0 0 0 0 0 -0.068 0.115 -10.457 10.458 0.000 1000 22 gamma 91 813 0 0 0 0 0 0.041 0.202 -23.526 23.527 0.000 1001 22 gamma 91 815 0 0 0 0 0 0.174 -0.186 -6.053 6.058 0.000 1002 22 gamma 91 815 0 0 0 0 0 0.223 -0.181 -10.994 10.998 0.000 1003 22 gamma 91 819 0 0 0 0 0 -0.295 0.076 0.019 0.306 0.000 1004 22 gamma 91 819 0 0 0 0 0 -0.518 0.192 -0.139 0.570 0.000 1005 22 gamma 91 823 0 0 0 0 0 0.070 0.124 -0.102 0.175 0.000 1006 22 gamma 91 823 0 0 0 0 0 -0.016 -0.006 0.023 0.028 0.000 1007 22 gamma 91 825 0 0 0 0 0 -0.306 0.403 -1.349 1.441 0.000 1008 22 gamma 91 825 0 0 0 0 0 -0.180 0.381 -0.898 0.992 0.000 1009 22 gamma 91 827 0 0 0 0 0 -0.052 0.043 0.059 0.090 0.000 1010 22 gamma 91 827 0 0 0 0 0 -0.610 0.101 0.240 0.663 0.000 1011 211 pi+ 91 828 0 0 0 0 0 0.038 0.305 1.147 1.196 0.140 1012 -211 pi- 91 828 0 0 0 0 0 0.361 0.044 1.393 1.446 0.140 1013 22 gamma 91 831 0 0 0 0 0 0.163 0.535 1.128 1.259 0.000 1014 22 gamma 91 831 0 0 0 0 0 0.170 0.233 0.605 0.670 0.000 1015 22 gamma 91 833 0 0 0 0 0 -0.040 0.237 1.284 1.306 0.000 1016 22 gamma 91 833 0 0 0 0 0 -0.020 0.200 1.974 1.984 0.000 1017 22 gamma 91 835 0 0 0 0 0 -0.043 0.125 13.833 13.834 0.000 1018 22 gamma 91 835 0 0 0 0 0 0.055 0.317 51.252 51.253 0.000 1019 22 gamma 91 839 0 0 0 0 0 -0.001 -0.047 7.596 7.596 0.000 1020 22 gamma 91 839 0 0 0 0 0 -0.036 -0.017 0.617 0.619 0.000 1021 22 gamma 91 847 0 0 0 0 0 0.071 0.306 11.356 11.360 0.000 1022 22 gamma 91 847 0 0 0 0 0 -0.044 0.053 2.003 2.004 0.000 1023 22 gamma 91 849 0 0 0 0 0 -0.002 -0.021 0.254 0.255 0.000 1024 22 gamma 91 849 0 0 0 0 0 -0.065 -0.000 10.322 10.322 0.000 1025 22 gamma 91 852 0 0 0 0 0 -0.537 0.584 -5.030 5.092 0.000 1026 22 gamma 91 852 0 0 0 0 0 -0.011 -0.001 -0.205 0.205 0.000 1027 22 gamma 91 854 0 0 0 0 0 0.161 -0.068 -0.847 0.865 0.000 1028 22 gamma 91 854 0 0 0 0 0 0.161 -0.029 -0.359 0.395 0.000 1029 22 gamma 91 858 0 0 0 0 0 -0.219 0.009 -1.720 1.734 0.000 1030 22 gamma 91 858 0 0 0 0 0 -0.083 0.096 -1.151 1.158 0.000 1031 211 pi+ 91 863 0 0 0 0 0 -0.082 -0.050 -2.572 2.578 0.140 1032 -211 pi- 91 863 0 0 0 0 0 0.167 -0.647 -7.207 7.239 0.140 1033 211 pi+ 91 865 0 0 0 0 0 -0.281 -0.748 -2.671 2.791 0.140 1034 -211 pi- 91 865 0 0 0 0 0 -0.010 -0.119 -1.340 1.352 0.140 1035 22 gamma 91 873 0 0 0 0 0 0.090 -0.021 89.809 89.809 0.000 1036 11 e- 91 873 0 0 0 0 0 0.280 -0.047 151.734 151.734 0.001 1037 -11 e+ 91 873 0 0 0 0 0 0.217 -0.041 114.214 114.215 0.001 1038 22 gamma 91 875 0 0 0 0 0 -0.509 0.117 483.961 483.961 0.000 1039 22 gamma 91 875 0 0 0 0 0 -0.239 -0.033 199.629 199.629 0.000 1040 211 pi+ 91 876 0 0 0 0 0 -0.205 -0.184 -2.592 2.610 0.140 1041 -211 pi- 91 876 0 0 0 0 0 0.029 0.108 -3.648 3.652 0.140 1042 311 (K0) -91 877 0 1089 1089 0 0 -0.156 0.210 -4.757 4.791 0.498 1043 211 pi+ 91 877 0 0 0 0 0 0.036 -0.232 -6.193 6.199 0.140 1044 3322 (Xi0) -91 877 0 1090 1091 0 0 0.117 -0.459 -13.322 13.395 1.315 1045 22 gamma 91 878 0 0 0 0 0 0.014 -0.027 -0.158 0.161 0.000 1046 22 gamma 91 878 0 0 0 0 0 0.146 0.140 -1.981 1.991 0.000 1047 313 (K*0) -91 887 0 1092 1093 0 0 -0.936 -0.431 -38.165 38.189 0.873 1048 -211 pi- 91 887 0 0 0 0 0 -1.496 0.376 -36.039 36.072 0.140 1049 211 pi+ 91 887 0 0 0 0 0 -0.064 0.125 -6.414 6.417 0.140 1050 22 gamma 91 893 0 0 0 0 0 -0.124 -0.150 -2.152 2.161 0.000 1051 22 gamma 91 893 0 0 0 0 0 -0.057 0.022 -1.005 1.007 0.000 1052 22 gamma 91 898 0 0 0 0 0 0.147 0.067 -117.199 117.199 0.000 1053 22 gamma 91 898 0 0 0 0 0 0.403 0.017 -421.783 421.783 0.000 1054 22 gamma 91 902 0 0 0 0 0 -0.022 0.056 0.163 0.174 0.000 1055 22 gamma 91 902 0 0 0 0 0 -0.019 -0.077 0.335 0.344 0.000 1056 22 gamma 91 911 0 0 0 0 0 -0.219 -0.340 0.856 0.947 0.000 1057 22 gamma 91 911 0 0 0 0 0 -0.056 -0.005 0.147 0.157 0.000 1058 22 gamma 91 938 0 0 0 0 0 0.846 0.551 37.954 37.968 0.000 1059 22 gamma 91 938 0 0 0 0 0 0.172 0.156 10.985 10.988 0.000 1060 22 gamma 91 946 0 0 0 0 0 -0.036 0.260 1.016 1.049 0.000 1061 22 gamma 91 946 0 0 0 0 0 -0.007 -0.015 0.026 0.031 0.000 1062 22 gamma 91 947 0 0 0 0 0 0.006 0.043 0.089 0.099 0.000 1063 22 gamma 91 947 0 0 0 0 0 0.088 0.220 1.746 1.762 0.000 1064 22 gamma 91 948 0 0 0 0 0 0.039 0.268 0.747 0.795 0.000 1065 22 gamma 91 948 0 0 0 0 0 -0.068 0.091 0.311 0.331 0.000 1066 22 gamma 91 951 0 0 0 0 0 -0.040 -0.111 0.065 0.134 0.000 1067 22 gamma 91 951 0 0 0 0 0 -0.047 -0.004 -0.043 0.064 0.000 1068 22 gamma 91 954 0 0 0 0 0 0.175 -0.138 0.058 0.230 0.000 1069 22 gamma 91 954 0 0 0 0 0 -0.020 -0.012 -0.015 0.028 0.000 1070 22 gamma 91 957 0 0 0 0 0 -0.114 -0.020 25.522 25.522 0.000 1071 22 gamma 91 957 0 0 0 0 0 -0.022 0.077 27.230 27.230 0.000 1072 22 gamma 91 958 0 0 0 0 0 -0.145 0.115 28.005 28.006 0.000 1073 22 gamma 91 958 0 0 0 0 0 -0.017 0.056 2.944 2.944 0.000 1074 22 gamma 91 959 0 0 0 0 0 -0.044 0.069 36.755 36.755 0.000 1075 22 gamma 91 959 0 0 0 0 0 0.035 -0.034 9.821 9.822 0.000 1076 22 gamma 91 962 0 0 0 0 0 -0.057 -0.001 0.172 0.182 0.000 1077 22 gamma 91 962 0 0 0 0 0 0.055 -0.090 0.329 0.345 0.000 1078 22 gamma 91 965 0 0 0 0 0 -0.049 -0.032 -0.075 0.095 0.000 1079 22 gamma 91 965 0 0 0 0 0 -0.280 0.082 -0.146 0.326 0.000 1080 22 gamma 91 972 0 0 0 0 0 0.028 0.004 -0.011 0.031 0.000 1081 22 gamma 91 972 0 0 0 0 0 -0.003 -0.002 -0.468 0.468 0.000 1082 22 gamma 91 973 0 0 0 0 0 0.000 0.006 -0.230 0.230 0.000 1083 22 gamma 91 973 0 0 0 0 0 -0.080 -0.166 -0.469 0.504 0.000 1084 211 pi+ 91 974 0 0 0 0 0 -0.282 0.086 -0.492 0.590 0.140 1085 -211 pi- 91 974 0 0 0 0 0 0.100 -0.075 -0.298 0.352 0.140 1086 22 gamma 91 974 0 0 0 0 0 -0.086 -0.044 -0.134 0.165 0.000 1087 211 pi+ 91 975 0 0 0 0 0 0.140 0.376 1.087 1.167 0.140 1088 -211 pi- 91 975 0 0 0 0 0 0.221 -0.322 1.739 1.788 0.140 1089 130 K_L0 91 1042 1042 0 0 0 0 -0.156 0.210 -4.757 4.791 0.498 1090 3122 (Lambda0) -91 1044 0 1094 1095 0 0 0.041 -0.517 -11.510 11.575 1.116 1091 111 (pi0) -91 1044 0 1096 1097 0 0 0.075 0.058 -1.812 1.820 0.135 1092 311 (K0) -91 1047 0 1098 1098 0 0 -0.383 -0.113 -24.544 24.553 0.498 1093 111 (pi0) -91 1047 0 1099 1100 0 0 -0.553 -0.318 -13.621 13.636 0.135 1094 2212 p+ 91 1090 0 0 0 0 0 0.084 -0.380 -10.180 10.230 0.938 1095 -211 pi- 91 1090 0 0 0 0 0 -0.043 -0.137 -1.330 1.345 0.140 1096 22 gamma 91 1091 0 0 0 0 0 -0.028 -0.003 -0.123 0.126 0.000 1097 22 gamma 91 1091 0 0 0 0 0 0.104 0.061 -1.689 1.694 0.000 1098 130 K_L0 91 1092 1092 0 0 0 0 -0.383 -0.113 -24.544 24.553 0.498 1099 22 gamma 91 1093 0 0 0 0 0 -0.538 -0.272 -12.720 12.734 0.000 1100 22 gamma 91 1093 0 0 0 0 0 -0.015 -0.046 -0.901 0.902 0.000 Charge sum: 2.000 Momentum sum: 0.000 -0.000 0.000 8000.000 8000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> g g 111 | 553 56 56 | 2.248e-01 1.685e-02 | | g g -> q qbar (uds) 112 | 10 2 2 | 5.643e-03 2.037e-03 | | q g -> q g 113 | 330 41 41 | 1.376e-01 1.213e-02 | | q q(bar)' -> q q(bar)' 114 | 36 1 1 | 1.321e-02 1.321e-02 | | q qbar -> g g 115 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar -> q' qbar' (uds) 116 | 0 0 0 | 0.000e+00 0.000e+00 | | g g -> c cbar 121 | 3 0 0 | 0.000e+00 0.000e+00 | | q qbar -> c cbar 122 | 0 0 0 | 0.000e+00 0.000e+00 | | g g -> b bbar 123 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar -> b bbar 124 | 0 0 0 | 0.000e+00 0.000e+00 | | | | | | sum | 932 100 100 | 3.812e-01 2.469e-02 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 0 no errors or warnings to report | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:00 charged multiplicity 8.10*10^ 0 7 7 7.80*10^ 0 X X 7.50*10^ 0 X X 7.20*10^ 0 X 3 X 6.90*10^ 0 X X X 6.60*10^ 0 X X X 6.30*10^ 0 X X X 6.00*10^ 0 XX X X 5.70*10^ 0 XX X X 5.40*10^ 0 XX X X 5.10*10^ 0 77 7 XX X X 4.80*10^ 0 XX X XX X X 4.50*10^ 0 XX X XX X X 4.20*10^ 0 333XX X 3XX X X 3.90*10^ 0 XXXXX X XXX X X 3.60*10^ 0 XXXXX X XXX X X 3.30*10^ 0 XXXXX X XXX X X 3.00*10^ 0 XXXXXXXXXXXXXX XXXXX 2.70*10^ 0 XXXXXXXXXXXXXX XXXXX 2.40*10^ 0 XXXXXXXXXXXXXX XXXXX 2.10*10^ 0 7 XXXXXXXXXXXXXX7XXXXX 7 77 1.80*10^ 0 X XXXXXXXXXXXXXXXXXXXX X XX 1.50*10^ 0 X XXXXXXXXXXXXXXXXXXXX X XX 1.20*10^ 0 3 X3XXXXXXXXXXXXXXXXXXXX3X3XX3 3 0.90*10^ 0 X XXXXXXXXXXXXXXXXXXXXXXXXXXXX X 0.60*10^ 0 X XXXXXXXXXXXXXXXXXXXXXXXXXXXX X 0.30*10^ 0 X XXXXXXXXXXXXXXXXXXXXXXXXXXXX X Contents *10^ 0 0000001021444553353486372338331212210010000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 100 Mean = 1.6654e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+02 Rms = 5.6949e+01 Overflow = 0.0000e+00 High edge = 7.9950e+02 pythia8-8.1.80.orig/examples/outref/out110000644000175000017500000044721712217346171016372 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:03:34 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with pbar- at a CM energy of 1.960e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | Les Houches User Process(es) 9999 | 5.480e-09 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 40.89 mb | | | | pT0 = 2.12 gives sigmaInteraction = 136.66 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:frameType | 4 | 1 1 5 | | Beams:LHEF | ttbar.lhe | void | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- LHA initialization information ------------ beam kind energy pdfgrp pdfset A 2212 980.000 0 7 B -2212 980.000 0 7 Event weighting strategy = 3 Processes, with strategy-dependent cross section info number xsec (pb) xerr (pb) xmax (pb) 81 5.2201e+00 5.3841e-01 1.0000e+00 82 2.6026e-01 1.0625e-01 1.0000e+00 -------- End LHA initialization information -------- -------- LHA event information and listing ---------------------------------------------------------------------- process = 81 weight = 1.0000e+00 scale = 1.7331e+02 (GeV) alpha_em = 7.8198e-03 alpha_strong = 1.1567e-01 Participating Particles no id stat mothers colours p_x p_y p_z e m tau spin 1 2 -1 0 0 101 0 0.000 0.000 108.382 108.382 0.000 0.000 9.000 2 -2 -1 0 0 0 102 0.000 0.000 -279.761 279.761 0.000 0.000 9.000 3 6 2 1 2 101 0 33.629 8.912 -110.596 212.418 177.987 0.000 9.000 4 -6 2 1 2 0 102 -33.629 -8.912 -60.783 175.725 161.166 0.000 9.000 5 24 2 3 0 0 0 -30.885 -12.140 -4.785 86.623 79.871 0.000 9.000 6 5 1 3 0 101 0 64.514 21.052 -105.811 125.794 4.800 0.000 9.000 7 -24 2 4 0 0 0 -50.940 34.881 -75.292 126.217 80.315 0.000 9.000 8 -5 1 4 0 0 102 17.311 -43.792 14.509 49.507 4.800 0.000 9.000 9 -1 1 5 0 0 103 18.584 9.166 18.652 27.882 0.330 0.000 9.000 10 2 1 5 0 103 0 -49.469 -21.306 -23.437 58.741 0.330 0.000 9.000 11 13 1 7 0 0 0 9.691 39.074 -25.560 47.687 0.106 0.000 9.000 12 -14 1 7 0 0 0 -60.632 -4.194 -49.732 78.530 0.000 0.000 9.000 pdf: id1 = 2 id2 = -2 x1 = 1.106e-01 x2 = 2.855e-01 scalePDF = 1.733e+02 pdf1 = 5.530e-01 pdf2 = 3.572e-01 -------- End LHA event information and listing ------------------------------------------------------------------ -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 9.800e+02, e = 9.800e+02, m = 9.383e-01. Beam B: id = -2212, pz = -9.800e+02, e = 9.800e+02, m = 9.383e-01. In 1: id = 2, x = 1.106e-01, pdf = 5.530e-01 at Q2 = 3.004e+04. In 2: id = -2, x = 2.855e-01, pdf = 3.572e-01 at same Q2. Process Les Houches User Process(es) with code 9999 is 2 -> 2. Subprocess user process 81 with code 81 is 2 -> 2. It has sHat = 1.213e+05, tHat = -3.834e+04, uHat = -2.529e+04, pTHat = 3.479e+01, m3Hat = 1.780e+02, m4Hat = 1.612e+02, thetaHat = 2.065e+00, phiHat = 2.590e-01. alphaEM = 7.820e-03, alphaS = 1.157e-01 at Q2 = 3.004e+04. Impact parameter b = 6.777e-01 gives enhancement factor = 1.623e+00. Max pT scale for MPI = 1.960e+03, ISR = 1.960e+03, FSR = 1.960e+03. Number of MPI = 6, ISR = 12, FSRproc = 46, FSRreson = 25. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 1960.000 1960.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 980.000 980.000 0.938 2 -2212 (pbar-) -12 0 0 4 0 0 0 0.000 0.000 -980.000 980.000 0.938 3 2 (u) -21 1 0 5 6 101 0 0.000 0.000 108.382 108.382 0.000 4 -2 (ubar) -21 2 0 5 6 0 102 0.000 0.000 -279.761 279.761 0.000 5 6 (t) -22 3 4 7 8 101 0 33.629 8.912 -110.596 212.418 177.987 6 -6 (tbar) -22 3 4 9 10 0 102 -33.629 -8.912 -60.783 175.725 161.166 7 24 (W+) -22 5 0 11 12 0 0 -30.885 -12.140 -4.785 86.623 79.871 8 5 b 23 5 0 0 0 101 0 64.514 21.052 -105.811 125.794 4.800 9 -24 (W-) -22 6 0 13 14 0 0 -50.940 34.881 -75.292 126.217 80.315 10 -5 bbar 23 6 0 0 0 0 102 17.311 -43.792 14.509 49.507 4.800 11 -1 dbar 23 7 0 0 0 0 103 18.584 9.166 18.652 27.882 0.330 12 2 u 23 7 0 0 0 103 0 -49.469 -21.306 -23.437 58.741 0.330 13 13 mu- 23 9 0 0 0 0 0 9.691 39.074 -25.560 47.687 0.106 14 -14 nu_mubar 23 9 0 0 0 0 0 -60.632 -4.194 -49.732 78.530 0.000 Charge sum: 0.000 Momentum sum: -0.000 0.000 -171.379 388.143 348.258 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 1960.000 1960.000 1 2212 (p+) -12 0 0 253 0 0 0 0.000 0.000 980.000 980.000 0.938 2 -2212 (pbar-) -12 0 0 254 0 0 0 0.000 0.000 -980.000 980.000 0.938 3 2 (u) -21 7 0 5 6 101 0 0.000 0.000 108.382 108.382 0.000 4 -2 (ubar) -21 8 8 5 6 0 102 0.000 0.000 -279.761 279.761 0.000 5 6 (t) -22 3 4 9 9 101 0 33.629 8.912 -110.596 212.418 177.987 6 -6 (tbar) -22 3 4 10 10 0 102 -33.629 -8.912 -60.783 175.725 161.166 7 2 (u) -41 12 0 11 3 104 0 -0.000 -0.000 168.342 168.342 0.000 8 -2 (ubar) -42 13 13 4 4 0 102 0.000 0.000 -279.761 279.761 0.000 9 6 (t) -44 5 5 14 14 101 0 8.224 2.686 -31.426 180.947 177.987 10 -6 (tbar) -44 6 6 15 15 0 102 -62.308 -15.939 -4.803 173.591 161.166 11 21 (g) -43 7 0 16 16 104 101 54.085 13.253 -75.191 93.565 0.000 12 2 (u) -41 18 0 17 7 105 0 -0.000 0.000 179.905 179.905 0.000 13 -2 (ubar) -42 19 19 8 8 0 102 0.000 -0.000 -279.761 279.761 0.000 14 6 (t) -44 9 9 20 20 101 0 3.364 3.157 -29.071 180.405 177.987 15 -6 (tbar) -44 10 10 21 21 0 102 -67.794 -15.407 -4.752 175.586 161.166 16 21 (g) -44 11 11 22 22 104 101 53.488 13.311 -72.383 90.981 0.000 17 21 (g) -43 12 0 23 23 105 104 10.942 -1.061 6.350 12.695 0.000 18 2 (u) -41 25 25 24 12 106 0 -0.000 -0.000 196.445 196.445 0.000 19 -2 (ubar) -42 26 0 13 13 0 102 0.000 0.000 -279.761 279.761 0.000 20 6 (t) -44 14 14 27 27 101 0 5.076 4.129 -28.906 180.438 177.987 21 -6 (tbar) -44 15 15 28 28 0 102 -65.862 -14.310 -3.672 174.729 161.166 22 21 (g) -44 16 16 29 29 104 101 53.698 13.431 -72.955 91.577 0.000 23 21 (g) -44 17 17 30 30 105 104 11.157 -0.939 6.248 12.822 0.000 24 21 (g) -43 18 0 31 31 106 105 -4.069 -2.310 15.968 16.640 0.000 25 2 (u) -42 80 0 18 18 106 0 0.000 -0.000 196.445 196.445 0.000 26 -2 (ubar) -41 81 81 32 19 0 102 -0.000 0.000 -320.933 320.933 0.000 27 6 (t) -44 20 20 42 42 101 0 6.300 3.562 -28.967 180.474 177.987 28 -6 (tbar) -44 21 21 83 83 0 102 -64.818 -14.794 -4.095 174.389 161.166 29 21 (g) -44 22 22 37 38 104 101 54.660 12.985 -72.717 91.892 0.000 30 21 (g) -44 23 23 39 39 105 104 11.195 -0.957 6.310 12.887 0.000 31 21 (g) -44 24 24 60 61 106 105 -4.065 -2.312 15.943 16.615 0.000 32 22 (gamma) -43 26 0 87 87 0 0 -3.272 1.516 -40.963 41.121 0.000 33 21 (g) -31 50 0 35 36 107 108 0.000 0.000 1.018 1.018 0.000 34 21 (g) -31 51 51 35 36 109 110 0.000 0.000 -12.621 12.621 0.000 35 21 (g) -33 33 34 52 52 107 110 -2.397 -2.660 -6.118 7.089 0.000 36 21 (g) -33 33 34 53 53 109 108 2.397 2.660 -5.485 6.551 0.000 37 21 (g) -51 29 0 40 41 111 101 17.011 3.115 -16.922 24.196 0.000 38 21 (g) -51 29 0 45 45 104 111 37.961 9.843 -55.619 68.054 0.000 39 21 (g) -52 30 30 43 44 105 104 10.884 -0.930 6.135 12.528 0.000 40 21 (g) -51 37 0 84 84 111 112 4.861 0.666 -9.134 10.369 0.000 41 21 (g) -51 37 0 89 89 112 101 11.428 2.330 -7.189 13.701 0.000 42 6 (t) -52 27 27 82 82 101 0 7.022 3.681 -29.566 180.600 177.987 43 21 (g) -51 39 0 62 62 105 113 9.206 0.457 6.390 11.216 0.000 44 21 (g) -51 39 0 90 90 113 104 4.013 -0.782 -3.676 5.498 0.000 45 21 (g) -52 38 38 88 88 104 111 35.626 9.238 -52.199 63.869 0.000 46 -1 (dbar) -31 55 55 48 49 0 114 0.000 0.000 2.592 2.592 0.000 47 -4 (cbar) -31 56 0 48 49 0 115 0.000 0.000 -5.456 5.456 0.000 48 -1 (dbar) -33 46 47 57 57 0 115 -0.301 -2.455 1.425 2.874 0.330 49 -4 (cbar) -33 46 47 58 58 0 114 0.301 2.455 -4.290 5.174 1.500 50 21 (g) -41 63 63 54 33 107 116 0.000 0.000 1.428 1.428 0.000 51 21 (g) -42 64 0 34 34 109 110 0.000 -0.000 -12.621 12.621 0.000 52 21 (g) -44 35 35 65 65 107 110 -2.434 -2.642 -4.062 5.423 0.000 53 21 (g) -44 36 36 66 66 109 108 2.357 2.680 -3.517 5.011 0.000 54 21 (g) -43 50 0 67 67 108 116 0.077 -0.037 -3.614 3.615 0.000 55 -1 (dbar) -42 297 297 46 46 0 114 0.000 -0.000 2.592 2.592 0.000 56 21 (g) -41 298 298 59 47 117 115 -0.000 0.000 -8.928 8.928 0.000 57 -1 (dbar) -44 48 48 299 299 0 115 -0.351 -2.295 0.627 2.428 0.330 58 -4 (cbar) -44 49 49 300 300 0 114 -0.026 3.501 -5.264 6.497 1.500 59 4 (c) -43 56 0 301 301 117 0 0.377 -1.205 -1.700 2.595 1.500 60 21 (g) -51 31 0 86 86 106 118 -4.246 -0.832 14.360 14.998 0.000 61 21 (g) -51 31 0 91 91 118 105 1.564 -1.411 2.543 3.302 0.000 62 21 (g) -52 43 43 85 85 105 113 7.823 0.388 5.430 9.531 0.000 63 21 (g) -42 69 0 50 50 107 116 0.000 0.000 1.428 1.428 0.000 64 21 (g) -41 70 70 68 51 109 119 -0.000 -0.000 -37.626 37.626 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0.202 425 21 (g) -73 319 422 613 613 127 120 -0.609 1.652 -0.066 1.784 0.281 426 21 (g) -73 306 313 620 620 168 169 -0.223 -2.313 6.669 7.073 0.401 427 21 (g) -73 314 331 614 614 162 127 -0.752 -0.794 0.288 1.215 0.442 428 21 (g) -73 305 326 430 0 122 116 0.305 -1.261 0.156 1.309 0.072 429 21 (g) -73 321 333 432 0 133 109 0.100 -0.244 -5.488 5.496 0.139 430 21 (g) -73 318 428 565 565 161 116 0.568 -1.854 -0.000 1.976 0.381 431 21 (g) -73 362 364 573 573 195 197 3.634 -19.845 9.422 22.272 0.471 432 21 (g) -73 327 429 570 570 147 109 0.563 -0.328 -30.468 30.480 0.581 433 21 (g) -73 290 296 515 515 138 158 -0.440 -2.293 -4.534 5.100 0.075 434 -4 (cbar) -73 300 332 518 518 0 145 0.461 4.669 -6.195 7.929 1.575 435 21 (g) -73 285 322 516 516 107 138 0.148 0.621 -1.801 1.913 0.080 436 21 (g) -73 289 329 437 0 145 131 -0.809 0.198 -1.371 1.615 0.187 437 21 (g) -73 328 436 517 517 145 107 -1.196 0.634 -2.562 2.942 0.504 438 -3 (sbar) -73 257 275 457 457 0 112 6.567 1.240 -11.066 12.947 0.709 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-8.498 10.269 0.140 468 311 (K0) -84 449 457 649 649 0 0 1.228 0.332 -1.187 1.809 0.498 469 1 (d) -71 258 258 479 490 105 0 3.087 -0.188 3.028 4.340 0.330 470 21 (g) -71 264 264 479 490 154 105 1.009 -0.663 0.909 1.511 0.000 471 21 (g) -71 276 276 479 490 118 154 0.334 -0.941 2.146 2.367 0.000 472 21 (g) -71 259 259 479 490 163 118 -0.065 0.178 0.250 0.313 0.000 473 21 (g) -71 278 278 479 490 137 163 -1.548 -0.569 5.358 5.606 0.000 474 21 (g) -71 270 270 479 490 134 137 -2.127 0.182 8.419 8.685 0.000 475 21 (g) -71 266 266 479 490 173 134 -0.019 0.162 5.485 5.487 0.000 476 21 (g) -71 282 282 479 490 106 173 -0.871 0.182 5.560 5.631 0.000 477 21 (g) -71 265 265 479 490 124 106 -0.549 0.991 12.566 12.617 0.000 478 -2 (ubar) -71 337 337 479 490 0 124 -0.012 -0.030 9.655 9.661 0.330 479 111 (pi0) -83 469 478 721 722 0 0 0.378 -0.100 0.245 0.481 0.135 480 -211 pi- 83 469 478 0 0 0 0 1.560 -0.100 1.591 2.235 0.140 481 211 pi+ 83 469 478 0 0 0 0 0.299 0.209 0.173 0.427 0.140 482 -213 (rho-) 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2.269 5.391 0.330 497 -311 (Kbar0) -83 491 496 655 655 0 0 14.853 3.821 -21.940 26.773 0.498 498 -211 pi- 83 491 496 0 0 0 0 3.597 1.294 -4.798 6.136 0.140 499 113 (rho0) -83 491 496 656 657 0 0 8.040 1.758 -11.460 14.132 0.808 500 111 (pi0) -83 491 496 729 730 0 0 2.016 0.645 -3.455 4.054 0.135 501 211 pi+ 83 491 496 0 0 0 0 1.296 0.231 -1.678 2.137 0.140 502 -213 (rho-) -83 491 496 658 659 0 0 3.857 0.636 -4.494 6.003 0.748 503 211 pi+ 83 491 496 0 0 0 0 0.783 -0.262 -1.064 1.354 0.140 504 -211 pi- 83 491 496 0 0 0 0 0.140 0.027 -0.106 0.226 0.140 505 111 (pi0) -83 491 496 731 732 0 0 1.267 0.763 0.322 1.520 0.135 506 213 (rho+) -83 491 496 660 661 0 0 1.552 -0.470 -0.441 1.861 0.800 507 311 (K0) -83 491 496 662 662 0 0 0.568 -0.363 -0.584 1.021 0.498 508 -323 (K*-) -84 491 496 663 664 0 0 2.640 0.496 0.935 2.969 0.851 509 211 pi+ 84 491 496 0 0 0 0 0.322 -0.267 0.093 0.450 0.140 510 -2101 (ud_0bar) -71 338 338 519 532 114 0 0.040 -0.136 -561.172 561.172 0.579 511 21 (g) -71 288 288 519 532 143 114 -0.291 0.031 -3.823 3.834 0.000 512 21 (g) -71 294 294 519 532 155 143 -1.524 0.277 -6.007 6.204 0.000 513 21 (g) -71 292 292 519 532 110 155 -0.632 -0.191 -6.358 6.392 0.000 514 21 (g) -71 295 295 519 532 158 110 -1.081 -1.169 -3.634 3.967 0.000 515 21 (g) -71 433 433 519 532 138 158 -0.440 -2.293 -4.534 5.100 0.075 516 21 (g) -71 435 435 519 532 107 138 0.148 0.621 -1.801 1.913 0.080 517 21 (g) -71 437 437 519 532 145 107 -1.196 0.634 -2.562 2.942 0.504 518 -4 (cbar) -71 434 434 519 532 0 145 0.461 4.669 -6.195 7.929 1.575 519 -2212 pbar- 83 510 518 0 0 0 0 0.149 0.195 -352.948 352.950 0.938 520 113 (rho0) -83 510 518 665 666 0 0 -0.145 -0.608 -162.679 162.682 0.722 521 211 pi+ 83 510 518 0 0 0 0 -0.197 0.354 -3.349 3.376 0.140 522 -213 (rho-) -83 510 518 667 668 0 0 -0.570 0.211 -41.494 41.505 0.772 523 211 pi+ 83 510 518 0 0 0 0 -0.005 -0.036 -0.167 0.221 0.140 524 111 (pi0) -83 510 518 733 734 0 0 -0.679 0.374 -6.914 6.958 0.135 525 2112 n0 84 510 518 0 0 0 0 -1.425 -0.945 -9.528 9.726 0.940 526 -2112 nbar0 84 510 518 0 0 0 0 -0.174 -1.327 -3.596 3.951 0.940 527 331 (eta') -84 510 518 735 737 0 0 -0.631 -0.249 -3.168 3.379 0.958 528 111 (pi0) -84 510 518 738 739 0 0 0.177 -0.203 -0.864 0.915 0.135 529 1114 (Delta-) -84 510 518 669 670 0 0 -1.025 -0.235 -3.152 3.638 1.482 530 211 pi+ 84 510 518 0 0 0 0 -0.047 0.055 -0.069 0.172 0.140 531 -2212 pbar- 84 510 518 0 0 0 0 0.311 1.250 -2.664 3.104 0.938 532 -423 (D*bar0) -84 510 518 740 741 0 0 -0.253 3.608 -5.494 6.877 2.007 533 2 (u) -71 413 413 547 563 203 0 -26.340 -8.532 1.255 27.717 0.330 534 21 (g) -71 412 412 547 563 216 203 -7.849 -3.768 0.929 8.756 0.000 535 21 (g) -71 411 411 547 563 201 216 -6.786 -2.568 0.090 7.256 0.000 536 21 (g) -71 400 400 547 563 209 201 -6.308 -3.046 -1.174 7.103 0.000 537 21 (g) -71 405 405 547 563 212 209 -6.441 -2.643 -0.006 6.962 0.000 538 21 (g) -71 406 406 547 563 205 212 -0.937 -0.796 0.092 1.233 0.000 539 21 (g) -71 414 414 547 563 217 205 -1.248 -1.111 1.168 2.039 0.000 540 21 (g) -71 442 442 547 563 214 217 -0.481 -0.606 0.459 1.081 0.598 541 21 (g) -71 440 440 547 563 208 214 -0.114 -0.157 1.003 1.090 0.380 542 21 (g) -71 441 441 547 563 200 208 0.821 1.277 6.022 6.231 0.509 543 21 (g) -71 403 403 547 563 210 200 -0.367 1.119 3.094 3.311 0.000 544 21 (g) -71 402 402 547 563 202 210 0.409 0.612 3.628 3.702 0.000 545 21 (g) -71 391 391 547 563 206 202 1.091 0.266 2.463 2.707 0.000 546 -1 (dbar) -71 390 390 547 563 0 206 11.056 5.269 14.175 18.736 0.330 547 321 K+ 83 533 546 0 0 0 0 -18.910 -5.842 0.719 19.811 0.494 548 -311 (Kbar0) -83 533 546 671 671 0 0 -18.377 -7.222 1.109 19.783 0.498 549 111 (pi0) -83 533 546 742 743 0 0 -3.634 -1.898 -0.666 4.156 0.135 550 -211 pi- 83 533 546 0 0 0 0 -6.110 -2.686 0.744 6.717 0.140 551 113 (rho0) -83 533 546 672 673 0 0 -4.244 -2.010 -0.633 4.799 0.759 552 2212 p+ 83 533 546 0 0 0 0 -3.566 -1.835 0.353 4.134 0.938 553 -2212 pbar- 84 533 546 0 0 0 0 -0.939 -0.708 0.900 1.753 0.938 554 211 pi+ 84 533 546 0 0 0 0 -0.308 -0.371 1.071 1.183 0.140 555 3122 (Lambda0) -84 533 546 744 745 0 0 0.360 0.255 2.466 2.743 1.116 556 -3122 (Lambdabar0) -84 533 546 746 747 0 0 -0.226 0.370 0.931 1.516 1.116 557 111 (pi0) -84 533 546 748 749 0 0 -0.239 -0.038 0.983 1.021 0.135 558 -211 pi- 84 533 546 0 0 0 0 0.061 0.125 2.301 2.309 0.140 559 213 (rho+) -84 533 546 674 675 0 0 1.012 1.065 4.809 5.146 1.092 560 221 (eta) -84 533 546 750 752 0 0 0.148 0.368 0.709 0.979 0.548 561 -213 (rho-) -84 533 546 676 677 0 0 2.744 1.778 5.159 6.153 0.739 562 211 pi+ 84 533 546 0 0 0 0 0.402 -0.248 0.508 0.708 0.140 563 113 (rho0) -84 533 546 678 679 0 0 8.335 4.211 11.732 15.011 0.697 564 1 (d) -71 336 336 581 610 116 0 0.587 -0.111 0.801 1.052 0.330 565 21 (g) -71 430 430 581 610 161 116 0.568 -1.854 -0.000 1.976 0.381 566 21 (g) -71 323 323 581 610 174 161 0.488 -1.047 -1.693 2.049 0.000 567 21 (g) -71 287 287 581 610 141 174 1.293 0.143 -5.256 5.414 0.000 568 21 (g) -71 291 291 581 610 108 141 0.473 0.150 -0.135 0.515 0.000 569 21 (g) -71 286 286 581 610 109 108 3.218 0.765 -3.404 4.746 0.000 570 21 (g) -71 432 432 581 610 147 109 0.563 -0.328 -30.468 30.480 0.581 571 21 (g) -71 330 330 581 610 102 147 0.624 1.055 -13.037 13.095 0.000 572 21 (g) -71 365 365 581 610 197 102 -0.361 -1.331 0.650 1.524 0.000 573 21 (g) -71 431 431 581 610 195 197 3.634 -19.845 9.422 22.272 0.471 574 21 (g) -71 363 363 581 610 192 195 1.115 -4.953 2.568 5.689 0.000 575 21 (g) -71 354 354 581 610 190 192 0.010 -1.494 0.405 1.548 0.000 576 21 (g) -71 353 353 581 610 193 190 -0.562 -2.087 1.942 2.905 0.000 577 21 (g) -71 355 355 581 610 194 193 0.318 -1.054 1.433 1.807 0.000 578 21 (g) -71 367 367 581 610 198 194 -0.806 -2.210 0.972 2.545 0.000 579 21 (g) -71 368 368 581 610 191 198 -0.223 -2.597 0.400 2.637 0.000 580 -5 (bbar) -71 369 369 581 610 0 191 3.220 -9.065 12.796 16.713 4.800 581 -211 pi- 83 564 580 0 0 0 0 0.184 0.082 0.190 0.310 0.140 582 213 (rho+) -83 564 580 680 681 0 0 0.673 -1.565 0.345 1.949 0.882 583 223 (omega) -83 564 580 753 755 0 0 0.828 -0.557 -0.546 1.375 0.773 584 -213 (rho-) -83 564 580 682 683 0 0 0.282 -0.564 -1.198 1.589 0.832 585 213 (rho+) -83 564 580 684 685 0 0 0.124 0.316 -1.362 1.587 0.739 586 2112 n0 83 564 580 0 0 0 0 2.222 0.080 -3.198 4.007 0.940 587 331 (eta') -83 564 580 756 758 0 0 0.573 -0.339 -4.764 4.905 0.957 588 -2112 nbar0 83 564 580 0 0 0 0 0.989 -0.017 -1.371 1.934 0.940 589 2112 n0 83 564 580 0 0 0 0 0.822 0.294 -4.001 4.201 0.940 590 -2112 nbar0 83 564 580 0 0 0 0 0.239 -0.015 -4.961 5.055 0.940 591 -213 (rho-) -83 564 580 686 687 0 0 -0.050 0.361 -4.971 5.032 0.689 592 331 (eta') -83 564 580 759 760 0 0 0.715 0.382 -14.086 14.142 0.958 593 213 (rho+) -83 564 580 688 689 0 0 -0.076 -0.032 -5.459 5.507 0.717 594 111 (pi0) -83 564 580 761 762 0 0 -0.116 -0.053 -4.384 4.388 0.135 595 -213 (rho-) -83 564 580 690 691 0 0 0.055 -0.208 -0.886 1.238 0.837 596 223 (omega) -83 564 580 763 765 0 0 0.329 0.371 -1.065 1.413 0.784 597 211 pi+ 83 564 580 0 0 0 0 -0.212 -0.543 -0.000 0.599 0.140 598 -213 (rho-) -83 564 580 692 693 0 0 0.420 -0.960 -0.696 1.909 1.437 599 213 (rho+) -83 564 580 694 695 0 0 0.029 -2.098 0.925 2.411 0.743 600 111 (pi0) -83 564 580 766 767 0 0 0.247 -0.804 0.645 1.069 0.135 601 3112 (Sigma-) -83 564 580 768 769 0 0 1.103 -11.241 4.982 12.403 1.197 602 323 (K*+) -84 564 580 696 697 0 0 1.511 -4.818 3.332 6.117 0.898 603 -2112 nbar0 84 564 580 0 0 0 0 0.472 -5.523 2.502 6.154 0.940 604 221 (eta) -84 564 580 770 772 0 0 -0.093 -1.248 0.501 1.455 0.548 605 2112 n0 84 564 580 0 0 0 0 0.217 -3.176 1.485 3.636 0.940 606 -2212 pbar- 84 564 580 0 0 0 0 -0.030 -2.615 2.230 3.562 0.938 607 111 (pi0) -84 564 580 773 774 0 0 0.425 -0.488 0.616 0.903 0.135 608 321 K+ 84 564 580 0 0 0 0 -0.405 -1.403 1.152 1.924 0.494 609 -321 K- 84 564 580 0 0 0 0 0.162 -0.456 0.713 0.993 0.494 610 523 (B*+) -84 564 580 775 776 0 0 2.516 -9.023 10.724 15.202 5.325 611 4 (c) -71 301 301 622 641 117 0 0.455 -0.792 -1.401 2.247 1.500 612 21 (g) -71 293 293 622 641 120 117 0.158 1.111 -0.686 1.315 0.000 613 21 (g) -71 425 425 622 641 127 120 -0.609 1.652 -0.066 1.784 0.281 614 21 (g) -71 427 427 622 641 162 127 -0.752 -0.794 0.288 1.215 0.442 615 21 (g) -71 309 309 622 641 164 162 -0.378 -0.105 1.364 1.419 0.000 616 21 (g) -71 424 424 622 641 123 164 -0.179 0.343 6.289 6.304 0.202 617 21 (g) -71 334 334 622 641 144 123 0.895 0.871 22.592 22.626 0.000 618 21 (g) -71 310 310 622 641 153 144 0.186 -0.103 15.609 15.611 0.000 619 21 (g) -71 423 423 622 641 169 153 -0.490 -1.264 34.535 34.562 0.139 620 21 (g) -71 426 426 622 641 168 169 -0.223 -2.313 6.669 7.073 0.401 621 2101 (ud_0) -71 335 335 622 641 0 168 0.425 -0.059 615.024 615.024 0.579 622 433 (D*_s+) -83 611 621 777 778 0 0 0.266 1.148 -1.414 2.802 2.112 623 -321 K- 83 611 621 0 0 0 0 -0.357 -0.249 -0.038 0.659 0.494 624 2212 p+ 83 611 621 0 0 0 0 -0.362 -0.602 0.009 1.172 0.938 625 -2112 nbar0 83 611 621 0 0 0 0 0.067 0.408 0.027 1.027 0.940 626 111 (pi0) -83 611 621 779 780 0 0 -0.543 0.892 -0.138 1.062 0.135 627 -211 pi- 83 611 621 0 0 0 0 -0.028 -0.248 2.135 2.154 0.140 628 223 (omega) -83 611 621 781 783 0 0 -0.029 0.230 5.882 5.938 0.778 629 111 (pi0) -83 611 621 784 785 0 0 0.535 0.254 3.815 3.863 0.135 630 211 pi+ 83 611 621 0 0 0 0 -0.292 -0.427 2.066 2.134 0.140 631 113 (rho0) -83 611 621 698 699 0 0 0.071 0.857 9.346 9.418 0.783 632 113 (rho0) -84 611 621 700 701 0 0 0.147 -0.758 28.200 28.223 0.837 633 -211 pi- 84 611 621 0 0 0 0 -0.155 -0.081 4.248 4.254 0.140 634 211 pi+ 84 611 621 0 0 0 0 0.134 -0.047 10.003 10.005 0.140 635 2112 n0 84 611 621 0 0 0 0 0.162 -0.249 5.617 5.703 0.940 636 223 (omega) -84 611 621 786 787 0 0 -0.535 -1.197 11.050 11.155 0.784 637 -2212 pbar- 84 611 621 0 0 0 0 -0.244 -1.132 9.324 9.443 0.938 638 321 K+ 84 611 621 0 0 0 0 0.240 0.052 1.905 1.983 0.494 639 -323 (K*-) -84 611 621 702 703 0 0 -0.085 -0.170 142.667 142.670 0.920 640 111 (pi0) -84 611 621 788 789 0 0 0.207 -0.369 23.259 23.263 0.135 641 2212 p+ 84 611 621 0 0 0 0 0.290 0.234 442.252 442.253 0.938 642 211 pi+ 91 445 0 0 0 0 0 -0.191 0.167 2.155 2.175 0.140 643 -211 pi- 91 445 0 0 0 0 0 0.434 -0.345 12.975 12.988 0.140 644 310 (K_S0) -91 448 448 790 791 0 0 -1.013 -1.241 0.965 1.935 0.498 645 211 pi+ 91 460 0 0 0 0 0 1.922 1.226 -1.567 2.769 0.140 646 111 (pi0) -91 460 0 792 793 0 0 -0.100 -0.067 -0.508 0.539 0.135 647 -211 pi- 91 463 0 0 0 0 0 1.000 0.665 -1.468 1.902 0.140 648 111 (pi0) -91 463 0 794 795 0 0 1.446 0.217 -1.023 1.789 0.135 649 130 K_L0 91 468 468 0 0 0 0 1.228 0.332 -1.187 1.809 0.498 650 -211 pi- 91 482 0 0 0 0 0 1.148 -0.640 2.023 2.416 0.140 651 111 (pi0) -91 482 0 796 797 0 0 0.268 -0.391 0.630 0.800 0.135 652 310 (K_S0) -91 485 485 798 799 0 0 -1.740 -0.054 9.461 9.632 0.498 653 -321 K- 91 489 0 0 0 0 0 -0.320 0.587 7.442 7.488 0.494 654 211 pi+ 91 489 0 0 0 0 0 -0.075 -0.134 3.887 3.892 0.140 655 130 K_L0 91 497 497 0 0 0 0 14.853 3.821 -21.940 26.773 0.498 656 211 pi+ 91 499 0 0 0 0 0 3.657 0.441 -5.349 6.496 0.140 657 -211 pi- 91 499 0 0 0 0 0 4.383 1.317 -6.111 7.636 0.140 658 -211 pi- 91 502 0 0 0 0 0 0.879 0.403 -1.323 1.644 0.140 659 111 (pi0) -91 502 0 800 801 0 0 2.978 0.233 -3.172 4.359 0.135 660 211 pi+ 91 506 0 0 0 0 0 0.102 0.103 -0.189 0.276 0.140 661 111 (pi0) -91 506 0 802 803 0 0 1.449 -0.573 -0.252 1.584 0.135 662 310 (K_S0) -91 507 507 804 805 0 0 0.568 -0.363 -0.584 1.021 0.498 663 -311 (Kbar0) -91 508 0 704 704 0 0 1.746 0.467 0.398 1.916 0.498 664 -211 pi- 91 508 0 0 0 0 0 0.894 0.029 0.537 1.052 0.140 665 211 pi+ 91 520 0 0 0 0 0 0.049 -0.226 -17.326 17.328 0.140 666 -211 pi- 91 520 0 0 0 0 0 -0.194 -0.382 -145.353 145.354 0.140 667 -211 pi- 91 522 0 0 0 0 0 -0.400 -0.038 -35.479 35.482 0.140 668 111 (pi0) -91 522 0 806 807 0 0 -0.170 0.249 -6.014 6.023 0.135 669 2112 n0 91 529 0 0 0 0 0 -1.220 -0.277 -2.592 3.028 0.940 670 -211 pi- 91 529 0 0 0 0 0 0.195 0.041 -0.560 0.611 0.140 671 130 K_L0 91 548 548 0 0 0 0 -18.377 -7.222 1.109 19.783 0.498 672 211 pi+ 91 551 0 0 0 0 0 -2.886 -1.440 -0.111 3.230 0.140 673 -211 pi- 91 551 0 0 0 0 0 -1.359 -0.570 -0.521 1.569 0.140 674 211 pi+ 91 559 0 0 0 0 0 0.184 0.666 0.990 1.215 0.140 675 111 (pi0) -91 559 0 808 809 0 0 0.828 0.400 3.819 3.931 0.135 676 -211 pi- 91 561 0 0 0 0 0 0.947 1.015 2.116 2.535 0.140 677 111 (pi0) -91 561 0 810 811 0 0 1.797 0.763 3.043 3.618 0.135 678 211 pi+ 91 563 0 0 0 0 0 7.281 3.677 10.522 13.314 0.140 679 -211 pi- 91 563 0 0 0 0 0 1.054 0.534 1.210 1.697 0.140 680 211 pi+ 91 582 0 0 0 0 0 0.088 -0.282 0.418 0.531 0.140 681 111 (pi0) -91 582 0 812 813 0 0 0.585 -1.283 -0.073 1.418 0.135 682 -211 pi- 91 584 0 0 0 0 0 0.030 -0.707 -0.775 1.059 0.140 683 111 (pi0) -91 584 0 814 815 0 0 0.251 0.143 -0.423 0.530 0.135 684 211 pi+ 91 585 0 0 0 0 0 0.264 0.260 -1.323 1.381 0.140 685 111 (pi0) -91 585 0 816 817 0 0 -0.140 0.056 -0.039 0.206 0.135 686 -211 pi- 91 591 0 0 0 0 0 0.226 0.141 -1.035 1.078 0.140 687 111 (pi0) -91 591 0 818 819 0 0 -0.276 0.220 -3.936 3.954 0.135 688 211 pi+ 91 593 0 0 0 0 0 0.100 0.148 -4.504 4.509 0.140 689 111 (pi0) -91 593 0 820 821 0 0 -0.176 -0.180 -0.956 0.997 0.135 690 -211 pi- 91 595 0 0 0 0 0 -0.002 0.300 -0.276 0.431 0.140 691 111 (pi0) -91 595 0 822 823 0 0 0.057 -0.508 -0.610 0.807 0.135 692 -211 pi- 91 598 0 0 0 0 0 -0.201 0.088 -0.630 0.682 0.140 693 111 (pi0) -91 598 0 824 825 0 0 0.621 -1.048 -0.065 1.227 0.135 694 211 pi+ 91 599 0 0 0 0 0 -0.219 -1.305 0.818 1.562 0.140 695 111 (pi0) -91 599 0 826 827 0 0 0.248 -0.793 0.107 0.849 0.135 696 311 (K0) -91 602 0 705 705 0 0 0.478 -1.579 1.217 2.109 0.498 697 211 pi+ 91 602 0 0 0 0 0 1.034 -3.240 2.116 4.007 0.140 698 211 pi+ 91 631 0 0 0 0 0 0.094 0.569 2.704 2.768 0.140 699 -211 pi- 91 631 0 0 0 0 0 -0.022 0.288 6.643 6.650 0.140 700 211 pi+ 91 632 0 0 0 0 0 0.174 -0.720 12.727 12.750 0.140 701 -211 pi- 91 632 0 0 0 0 0 -0.027 -0.038 15.472 15.473 0.140 702 -321 K- 91 639 0 0 0 0 0 0.033 -0.024 130.287 130.288 0.494 703 111 (pi0) -91 639 0 828 829 0 0 -0.118 -0.145 12.380 12.383 0.135 704 130 K_L0 91 663 663 0 0 0 0 1.746 0.467 0.398 1.916 0.498 705 130 K_L0 91 696 696 0 0 0 0 0.478 -1.579 1.217 2.109 0.498 706 130 K_L0 91 447 0 0 0 0 0 0.206 0.049 3.334 3.378 0.498 707 310 (K_S0) -91 447 0 830 831 0 0 0.252 0.034 5.437 5.466 0.498 708 -511 (Bbar0) -91 458 0 832 834 0 0 46.643 17.053 -58.650 77.033 5.280 709 22 gamma 91 458 0 0 0 0 0 0.006 0.013 -0.025 0.029 0.000 710 22 gamma 91 461 0 0 0 0 0 3.550 0.262 -3.187 4.778 0.000 711 22 gamma 91 461 0 0 0 0 0 0.807 -0.005 -0.728 1.087 0.000 712 22 gamma 91 462 0 0 0 0 0 0.653 0.269 -0.355 0.791 0.000 713 22 gamma 91 462 0 0 0 0 0 0.761 0.406 -0.301 0.914 0.000 714 22 gamma 91 464 0 0 0 0 0 0.381 -0.002 -0.481 0.613 0.000 715 22 gamma 91 464 0 0 0 0 0 0.433 -0.118 -0.433 0.623 0.000 716 22 gamma 91 465 0 0 0 0 0 0.138 -0.085 -0.152 0.223 0.000 717 22 gamma 91 465 0 0 0 0 0 -0.004 0.010 0.019 0.022 0.000 718 111 (pi0) -91 466 0 835 836 0 0 0.380 0.131 -0.865 0.963 0.135 719 111 (pi0) -91 466 0 837 838 0 0 0.300 0.114 -0.415 0.541 0.135 720 111 (pi0) -91 466 0 839 840 0 0 0.360 -0.063 -0.462 0.604 0.135 721 22 gamma 91 479 0 0 0 0 0 0.025 -0.048 0.051 0.074 0.000 722 22 gamma 91 479 0 0 0 0 0 0.354 -0.052 0.194 0.407 0.000 723 211 pi+ 91 484 0 0 0 0 0 -0.048 -0.040 0.577 0.597 0.140 724 -211 pi- 91 484 0 0 0 0 0 -0.158 -0.019 0.478 0.523 0.140 725 221 (eta) -91 484 0 841 843 0 0 0.130 -0.389 1.701 1.833 0.548 726 211 pi+ 91 488 0 0 0 0 0 -0.118 0.122 1.447 1.463 0.140 727 -211 pi- 91 488 0 0 0 0 0 -0.103 -0.113 1.997 2.007 0.140 728 221 (eta) -91 488 0 844 846 0 0 -0.287 0.262 7.212 7.243 0.548 729 22 gamma 91 500 0 0 0 0 0 1.800 0.587 -3.009 3.555 0.000 730 22 gamma 91 500 0 0 0 0 0 0.216 0.057 -0.447 0.499 0.000 731 22 gamma 91 505 0 0 0 0 0 1.262 0.760 0.331 1.510 0.000 732 22 gamma 91 505 0 0 0 0 0 0.005 0.004 -0.008 0.010 0.000 733 22 gamma 91 524 0 0 0 0 0 -0.015 -0.005 -0.062 0.065 0.000 734 22 gamma 91 524 0 0 0 0 0 -0.664 0.380 -6.851 6.894 0.000 735 211 pi+ 91 527 0 0 0 0 0 -0.302 0.045 -0.844 0.908 0.140 736 -211 pi- 91 527 0 0 0 0 0 -0.020 -0.082 -0.629 0.650 0.140 737 221 (eta) -91 527 0 847 848 0 0 -0.310 -0.213 -1.695 1.820 0.548 738 22 gamma 91 528 0 0 0 0 0 0.103 -0.198 -0.709 0.743 0.000 739 22 gamma 91 528 0 0 0 0 0 0.074 -0.005 -0.155 0.172 0.000 740 -421 (Dbar0) -91 532 0 849 853 0 0 -0.332 3.494 -5.417 6.718 1.865 741 22 gamma 91 532 0 0 0 0 0 0.078 0.115 -0.077 0.159 0.000 742 22 gamma 91 549 0 0 0 0 0 -3.307 -1.693 -0.578 3.760 0.000 743 22 gamma 91 549 0 0 0 0 0 -0.327 -0.205 -0.088 0.396 0.000 744 2212 p+ 91 555 0 0 0 0 0 0.369 0.298 2.109 2.357 0.938 745 -211 pi- 91 555 0 0 0 0 0 -0.009 -0.043 0.357 0.386 0.140 746 -2212 pbar- 91 556 0 0 0 0 0 -0.240 0.388 0.883 1.367 0.938 747 211 pi+ 91 556 0 0 0 0 0 0.014 -0.018 0.047 0.149 0.140 748 22 gamma 91 557 0 0 0 0 0 -0.246 -0.009 0.903 0.935 0.000 749 22 gamma 91 557 0 0 0 0 0 0.007 -0.029 0.080 0.086 0.000 750 111 (pi0) -91 560 0 854 855 0 0 0.019 0.260 0.302 0.422 0.135 751 111 (pi0) -91 560 0 856 857 0 0 -0.028 0.104 0.154 0.231 0.135 752 111 (pi0) -91 560 0 858 859 0 0 0.157 0.003 0.252 0.326 0.135 753 211 pi+ 91 583 0 0 0 0 0 0.234 -0.064 -0.190 0.338 0.140 754 -211 pi- 91 583 0 0 0 0 0 0.437 -0.588 -0.255 0.788 0.140 755 111 (pi0) -91 583 0 860 861 0 0 0.158 0.095 -0.101 0.249 0.135 756 211 pi+ 91 587 0 0 0 0 0 0.062 -0.061 -1.537 1.545 0.140 757 -211 pi- 91 587 0 0 0 0 0 0.029 -0.086 -0.802 0.819 0.140 758 221 (eta) -91 587 0 862 864 0 0 0.482 -0.192 -2.426 2.541 0.548 759 113 (rho0) -91 592 0 865 866 0 0 0.351 0.093 -7.014 7.054 0.662 760 22 gamma 91 592 0 0 0 0 0 0.365 0.289 -7.072 7.087 0.000 761 22 gamma 91 594 0 0 0 0 0 -0.029 0.027 -0.355 0.358 0.000 762 22 gamma 91 594 0 0 0 0 0 -0.087 -0.081 -4.028 4.030 0.000 763 211 pi+ 91 596 0 0 0 0 0 0.324 0.126 -0.617 0.722 0.140 764 -211 pi- 91 596 0 0 0 0 0 -0.007 -0.071 -0.051 0.165 0.140 765 111 (pi0) -91 596 0 867 868 0 0 0.011 0.316 -0.397 0.526 0.135 766 22 gamma 91 600 0 0 0 0 0 0.187 -0.738 0.558 0.944 0.000 767 22 gamma 91 600 0 0 0 0 0 0.060 -0.066 0.087 0.125 0.000 768 2112 n0 91 601 0 0 0 0 0 0.752 -8.023 3.386 8.791 0.940 769 -211 pi- 91 601 0 0 0 0 0 0.351 -3.218 1.596 3.612 0.140 770 111 (pi0) -91 604 0 869 871 0 0 -0.060 -0.284 0.007 0.320 0.135 771 111 (pi0) -91 604 0 872 873 0 0 0.052 -0.239 0.144 0.314 0.135 772 111 (pi0) -91 604 0 874 875 0 0 -0.085 -0.725 0.350 0.821 0.135 773 22 gamma 91 607 0 0 0 0 0 0.415 -0.494 0.615 0.892 0.000 774 22 gamma 91 607 0 0 0 0 0 0.010 0.006 0.001 0.012 0.000 775 521 (B+) -91 610 0 876 879 0 0 2.453 -8.886 10.545 14.969 5.279 776 22 gamma 91 610 0 0 0 0 0 0.063 -0.137 0.178 0.234 0.000 777 431 (D_s+) -91 622 0 880 881 0 0 0.277 1.132 -1.485 2.727 1.968 778 22 gamma 91 622 0 0 0 0 0 -0.012 0.017 0.072 0.074 0.000 779 22 gamma 91 626 0 0 0 0 0 -0.224 0.403 0.004 0.461 0.000 780 22 gamma 91 626 0 0 0 0 0 -0.320 0.488 -0.142 0.601 0.000 781 211 pi+ 91 628 0 0 0 0 0 -0.231 0.167 1.774 1.802 0.140 782 -211 pi- 91 628 0 0 0 0 0 0.167 0.190 2.529 2.546 0.140 783 111 (pi0) -91 628 0 882 883 0 0 0.035 -0.126 1.579 1.590 0.135 784 22 gamma 91 629 0 0 0 0 0 0.071 0.088 0.827 0.835 0.000 785 22 gamma 91 629 0 0 0 0 0 0.464 0.166 2.988 3.028 0.000 786 111 (pi0) -91 636 0 884 885 0 0 -0.679 -1.198 10.109 10.203 0.135 787 22 gamma 91 636 0 0 0 0 0 0.144 0.001 0.941 0.952 0.000 788 22 gamma 91 640 0 0 0 0 0 0.192 -0.240 14.310 14.314 0.000 789 22 gamma 91 640 0 0 0 0 0 0.015 -0.129 8.948 8.949 0.000 790 111 (pi0) -91 644 0 886 887 0 0 -0.551 -0.654 0.272 0.908 0.135 791 111 (pi0) -91 644 0 888 889 0 0 -0.462 -0.587 0.693 1.028 0.135 792 22 gamma 91 646 0 0 0 0 0 0.031 -0.014 -0.058 0.067 0.000 793 22 gamma 91 646 0 0 0 0 0 -0.132 -0.053 -0.450 0.472 0.000 794 22 gamma 91 648 0 0 0 0 0 0.490 0.079 -0.426 0.654 0.000 795 22 gamma 91 648 0 0 0 0 0 0.956 0.138 -0.597 1.135 0.000 796 22 gamma 91 651 0 0 0 0 0 0.128 -0.124 0.149 0.232 0.000 797 22 gamma 91 651 0 0 0 0 0 0.141 -0.266 0.481 0.567 0.000 798 111 (pi0) -91 652 0 890 891 0 0 -0.368 0.138 1.955 1.998 0.135 799 111 (pi0) -91 652 0 892 893 0 0 -1.372 -0.193 7.506 7.634 0.135 800 22 gamma 91 659 0 0 0 0 0 0.219 -0.005 -0.275 0.352 0.000 801 22 gamma 91 659 0 0 0 0 0 2.758 0.238 -2.897 4.007 0.000 802 22 gamma 91 661 0 0 0 0 0 0.409 -0.168 -0.010 0.442 0.000 803 22 gamma 91 661 0 0 0 0 0 1.040 -0.405 -0.241 1.142 0.000 804 211 pi+ 91 662 0 0 0 0 0 0.260 -0.224 -0.050 0.374 0.140 805 -211 pi- 91 662 0 0 0 0 0 0.308 -0.139 -0.534 0.647 0.140 806 22 gamma 91 668 0 0 0 0 0 -0.139 0.084 -2.848 2.853 0.000 807 22 gamma 91 668 0 0 0 0 0 -0.031 0.165 -3.166 3.170 0.000 808 22 gamma 91 675 0 0 0 0 0 0.580 0.226 2.738 2.808 0.000 809 22 gamma 91 675 0 0 0 0 0 0.248 0.173 1.081 1.122 0.000 810 22 gamma 91 677 0 0 0 0 0 0.159 0.044 0.318 0.358 0.000 811 22 gamma 91 677 0 0 0 0 0 1.638 0.719 2.725 3.260 0.000 812 22 gamma 91 681 0 0 0 0 0 0.477 -1.061 -0.111 1.169 0.000 813 22 gamma 91 681 0 0 0 0 0 0.108 -0.221 0.038 0.249 0.000 814 22 gamma 91 683 0 0 0 0 0 0.018 -0.025 -0.035 0.047 0.000 815 22 gamma 91 683 0 0 0 0 0 0.234 0.169 -0.388 0.483 0.000 816 22 gamma 91 685 0 0 0 0 0 -0.138 0.082 -0.061 0.172 0.000 817 22 gamma 91 685 0 0 0 0 0 -0.001 -0.026 0.022 0.034 0.000 818 22 gamma 91 687 0 0 0 0 0 -0.110 0.010 -1.116 1.121 0.000 819 22 gamma 91 687 0 0 0 0 0 -0.166 0.210 -2.820 2.833 0.000 820 22 gamma 91 689 0 0 0 0 0 -0.001 -0.030 -0.315 0.316 0.000 821 22 gamma 91 689 0 0 0 0 0 -0.176 -0.150 -0.641 0.681 0.000 822 22 gamma 91 691 0 0 0 0 0 0.029 -0.057 -0.147 0.161 0.000 823 22 gamma 91 691 0 0 0 0 0 0.028 -0.450 -0.463 0.647 0.000 824 22 gamma 91 693 0 0 0 0 0 0.359 -0.622 -0.105 0.725 0.000 825 22 gamma 91 693 0 0 0 0 0 0.262 -0.426 0.039 0.502 0.000 826 22 gamma 91 695 0 0 0 0 0 0.121 -0.197 0.050 0.237 0.000 827 22 gamma 91 695 0 0 0 0 0 0.127 -0.596 0.057 0.612 0.000 828 22 gamma 91 703 0 0 0 0 0 -0.055 -0.106 3.884 3.886 0.000 829 22 gamma 91 703 0 0 0 0 0 -0.062 -0.040 8.496 8.496 0.000 830 211 pi+ 91 707 0 0 0 0 0 0.350 0.014 3.213 3.235 0.140 831 -211 pi- 91 707 0 0 0 0 0 -0.098 0.021 2.224 2.230 0.140 832 -413 (D*-) -91 708 0 894 895 0 0 18.084 6.506 -23.447 30.384 2.010 833 413 (D*+) -91 708 0 896 897 0 0 18.702 7.779 -23.755 31.283 2.010 834 -311 (Kbar0) -91 708 0 898 898 0 0 9.857 2.768 -11.448 15.366 0.498 835 22 gamma 91 718 0 0 0 0 0 0.309 0.159 -0.704 0.786 0.000 836 22 gamma 91 718 0 0 0 0 0 0.071 -0.028 -0.161 0.178 0.000 837 22 gamma 91 719 0 0 0 0 0 0.007 0.025 -0.095 0.099 0.000 838 22 gamma 91 719 0 0 0 0 0 0.293 0.089 -0.319 0.443 0.000 839 22 gamma 91 720 0 0 0 0 0 0.110 0.042 -0.158 0.197 0.000 840 22 gamma 91 720 0 0 0 0 0 0.250 -0.105 -0.304 0.407 0.000 841 111 (pi0) -91 725 0 899 900 0 0 0.071 -0.128 0.262 0.329 0.135 842 111 (pi0) -91 725 0 901 902 0 0 0.075 -0.133 1.087 1.106 0.135 843 111 (pi0) -91 725 0 903 904 0 0 -0.017 -0.128 0.351 0.398 0.135 844 211 pi+ 91 728 0 0 0 0 0 -0.023 0.066 1.241 1.251 0.140 845 -211 pi- 91 728 0 0 0 0 0 -0.077 0.163 1.718 1.733 0.140 846 111 (pi0) -91 728 0 905 906 0 0 -0.187 0.032 4.253 4.259 0.135 847 22 gamma 91 737 0 0 0 0 0 -0.291 -0.378 -1.433 1.510 0.000 848 22 gamma 91 737 0 0 0 0 0 -0.019 0.165 -0.262 0.310 0.000 849 -311 (Kbar0) -91 740 0 907 907 0 0 -0.300 1.214 -2.506 2.845 0.498 850 -211 pi- 91 740 0 0 0 0 0 0.050 0.261 -0.262 0.398 0.140 851 -211 pi- 91 740 0 0 0 0 0 -0.070 0.713 -1.394 1.573 0.140 852 211 pi+ 91 740 0 0 0 0 0 -0.038 0.677 -0.982 1.202 0.140 853 211 pi+ 91 740 0 0 0 0 0 0.027 0.629 -0.272 0.699 0.140 854 22 gamma 91 750 0 0 0 0 0 -0.042 0.024 0.035 0.059 0.000 855 22 gamma 91 750 0 0 0 0 0 0.060 0.237 0.268 0.362 0.000 856 22 gamma 91 751 0 0 0 0 0 -0.040 0.041 0.157 0.167 0.000 857 22 gamma 91 751 0 0 0 0 0 0.012 0.063 -0.003 0.064 0.000 858 22 gamma 91 752 0 0 0 0 0 0.081 0.062 0.082 0.131 0.000 859 22 gamma 91 752 0 0 0 0 0 0.077 -0.059 0.170 0.196 0.000 860 22 gamma 91 755 0 0 0 0 0 -0.009 0.018 0.021 0.029 0.000 861 22 gamma 91 755 0 0 0 0 0 0.167 0.077 -0.122 0.220 0.000 862 211 pi+ 91 758 0 0 0 0 0 0.225 0.053 -1.018 1.053 0.140 863 -211 pi- 91 758 0 0 0 0 0 0.033 -0.120 -0.476 0.512 0.140 864 111 (pi0) -91 758 0 908 909 0 0 0.224 -0.124 -0.932 0.976 0.135 865 211 pi+ 91 759 0 0 0 0 0 0.379 0.295 -5.152 5.176 0.140 866 -211 pi- 91 759 0 0 0 0 0 -0.028 -0.202 -1.862 1.878 0.140 867 22 gamma 91 765 0 0 0 0 0 0.036 0.162 -0.296 0.339 0.000 868 22 gamma 91 765 0 0 0 0 0 -0.024 0.154 -0.101 0.186 0.000 869 22 gamma 91 770 0 0 0 0 0 -0.086 -0.126 -0.029 0.155 0.000 870 11 e- 91 770 0 0 0 0 0 0.016 -0.078 0.026 0.084 0.001 871 -11 e+ 91 770 0 0 0 0 0 0.010 -0.080 0.010 0.082 0.001 872 22 gamma 91 771 0 0 0 0 0 -0.005 -0.177 0.148 0.230 0.000 873 22 gamma 91 771 0 0 0 0 0 0.056 -0.062 -0.003 0.084 0.000 874 22 gamma 91 772 0 0 0 0 0 -0.034 -0.530 0.192 0.565 0.000 875 22 gamma 91 772 0 0 0 0 0 -0.051 -0.195 0.157 0.256 0.000 876 -421 (Dbar0) -91 775 0 910 914 0 0 -0.002 -1.386 1.896 2.999 1.865 877 211 pi+ 91 775 0 0 0 0 0 0.794 -3.981 4.949 6.403 0.140 878 113 (rho0) -91 775 0 915 916 0 0 1.362 -2.990 2.463 4.182 0.795 879 111 (pi0) -91 775 0 917 918 0 0 0.298 -0.529 1.237 1.385 0.135 880 221 (eta) -91 777 0 919 921 0 0 1.036 0.466 -0.927 1.565 0.548 881 211 pi+ 91 777 0 0 0 0 0 -0.759 0.666 -0.558 1.162 0.140 882 22 gamma 91 783 0 0 0 0 0 0.035 -0.101 1.539 1.543 0.000 883 22 gamma 91 783 0 0 0 0 0 -0.000 -0.026 0.040 0.048 0.000 884 22 gamma 91 786 0 0 0 0 0 -0.108 -0.306 2.322 2.344 0.000 885 22 gamma 91 786 0 0 0 0 0 -0.571 -0.892 7.787 7.859 0.000 886 22 gamma 91 790 0 0 0 0 0 -0.234 -0.179 0.092 0.309 0.000 887 22 gamma 91 790 0 0 0 0 0 -0.316 -0.475 0.180 0.599 0.000 888 22 gamma 91 791 0 0 0 0 0 -0.334 -0.334 0.385 0.610 0.000 889 22 gamma 91 791 0 0 0 0 0 -0.128 -0.253 0.307 0.418 0.000 890 22 gamma 91 798 0 0 0 0 0 -0.342 0.159 1.863 1.901 0.000 891 22 gamma 91 798 0 0 0 0 0 -0.025 -0.021 0.091 0.097 0.000 892 22 gamma 91 799 0 0 0 0 0 -0.814 -0.109 4.081 4.163 0.000 893 22 gamma 91 799 0 0 0 0 0 -0.558 -0.084 3.425 3.471 0.000 894 -421 (Dbar0) -91 832 0 922 923 0 0 16.541 5.922 -21.451 27.791 1.865 895 -211 pi- 91 832 0 0 0 0 0 1.543 0.584 -1.996 2.593 0.140 896 411 (D+) -91 833 0 924 926 0 0 17.728 7.385 -22.507 29.646 1.870 897 111 (pi0) -91 833 0 927 928 0 0 0.974 0.394 -1.249 1.637 0.135 898 130 K_L0 91 834 834 0 0 0 0 9.857 2.768 -11.448 15.366 0.498 899 22 gamma 91 841 0 0 0 0 0 0.107 -0.066 0.146 0.193 0.000 900 22 gamma 91 841 0 0 0 0 0 -0.036 -0.061 0.116 0.136 0.000 901 22 gamma 91 842 0 0 0 0 0 0.066 -0.115 0.462 0.481 0.000 902 22 gamma 91 842 0 0 0 0 0 0.010 -0.018 0.625 0.626 0.000 903 22 gamma 91 843 0 0 0 0 0 -0.002 -0.004 -0.012 0.013 0.000 904 22 gamma 91 843 0 0 0 0 0 -0.015 -0.124 0.364 0.385 0.000 905 22 gamma 91 846 0 0 0 0 0 -0.095 -0.018 3.123 3.124 0.000 906 22 gamma 91 846 0 0 0 0 0 -0.092 0.051 1.130 1.134 0.000 907 310 (K_S0) -91 849 849 929 930 0 0 -0.300 1.214 -2.506 2.845 0.498 908 22 gamma 91 864 0 0 0 0 0 0.133 -0.126 -0.458 0.494 0.000 909 22 gamma 91 864 0 0 0 0 0 0.091 0.002 -0.474 0.483 0.000 910 321 K+ 91 876 0 0 0 0 0 0.028 -0.652 0.622 1.028 0.494 911 -211 pi- 91 876 0 0 0 0 0 -0.010 0.219 0.034 0.262 0.140 912 -211 pi- 91 876 0 0 0 0 0 0.062 -0.456 0.336 0.586 0.140 913 211 pi+ 91 876 0 0 0 0 0 -0.076 -0.162 0.625 0.665 0.140 914 111 (pi0) -91 876 0 931 932 0 0 -0.006 -0.335 0.280 0.457 0.135 915 211 pi+ 91 878 0 0 0 0 0 1.384 -2.498 1.974 3.475 0.140 916 -211 pi- 91 878 0 0 0 0 0 -0.022 -0.491 0.489 0.708 0.140 917 22 gamma 91 879 0 0 0 0 0 0.293 -0.415 1.017 1.137 0.000 918 22 gamma 91 879 0 0 0 0 0 0.005 -0.114 0.220 0.248 0.000 919 111 (pi0) -91 880 0 933 934 0 0 0.244 0.093 -0.210 0.361 0.135 920 111 (pi0) -91 880 0 935 936 0 0 0.561 0.102 -0.429 0.726 0.135 921 111 (pi0) -91 880 0 937 938 0 0 0.231 0.272 -0.289 0.478 0.135 922 313 (K*0) -91 894 0 939 940 0 0 9.926 4.080 -12.912 16.813 0.887 923 113 (rho0) -91 894 0 941 942 0 0 6.614 1.842 -8.540 10.977 0.658 924 311 (K0) -91 896 0 943 943 0 0 14.911 6.008 -19.575 25.335 0.498 925 211 pi+ 91 896 0 0 0 0 0 1.725 0.854 -1.612 2.515 0.140 926 111 (pi0) -91 896 0 944 945 0 0 1.092 0.524 -1.319 1.796 0.135 927 22 gamma 91 897 0 0 0 0 0 0.812 0.272 -1.010 1.324 0.000 928 22 gamma 91 897 0 0 0 0 0 0.162 0.122 -0.239 0.313 0.000 929 111 (pi0) -91 907 0 946 947 0 0 -0.070 0.951 -1.657 1.916 0.135 930 111 (pi0) -91 907 0 948 949 0 0 -0.230 0.263 -0.850 0.929 0.135 931 22 gamma 91 914 0 0 0 0 0 0.019 -0.012 0.063 0.067 0.000 932 22 gamma 91 914 0 0 0 0 0 -0.025 -0.324 0.217 0.391 0.000 933 22 gamma 91 919 0 0 0 0 0 0.173 0.000 -0.094 0.197 0.000 934 22 gamma 91 919 0 0 0 0 0 0.071 0.092 -0.116 0.164 0.000 935 22 gamma 91 920 0 0 0 0 0 0.551 0.120 -0.422 0.704 0.000 936 22 gamma 91 920 0 0 0 0 0 0.010 -0.018 -0.007 0.022 0.000 937 22 gamma 91 921 0 0 0 0 0 0.207 0.157 -0.229 0.347 0.000 938 22 gamma 91 921 0 0 0 0 0 0.023 0.115 -0.059 0.131 0.000 939 311 (K0) -91 922 0 950 950 0 0 5.516 2.169 -6.740 8.990 0.498 940 111 (pi0) -91 922 0 951 952 0 0 4.410 1.911 -6.172 7.824 0.135 941 211 pi+ 91 923 0 0 0 0 0 5.141 1.538 -6.987 8.810 0.140 942 -211 pi- 91 923 0 0 0 0 0 1.473 0.305 -1.553 2.167 0.140 943 130 K_L0 91 924 924 0 0 0 0 14.911 6.008 -19.575 25.335 0.498 944 22 gamma 91 926 0 0 0 0 0 0.503 0.245 -0.511 0.758 0.000 945 22 gamma 91 926 0 0 0 0 0 0.588 0.279 -0.808 1.038 0.000 946 22 gamma 91 929 0 0 0 0 0 -0.091 0.496 -0.790 0.937 0.000 947 22 gamma 91 929 0 0 0 0 0 0.021 0.455 -0.867 0.979 0.000 948 22 gamma 91 930 0 0 0 0 0 -0.095 0.114 -0.204 0.252 0.000 949 22 gamma 91 930 0 0 0 0 0 -0.135 0.149 -0.646 0.677 0.000 950 310 (K_S0) -91 939 939 953 954 0 0 5.516 2.169 -6.740 8.990 0.498 951 22 gamma 91 940 0 0 0 0 0 1.229 0.539 -1.822 2.263 0.000 952 22 gamma 91 940 0 0 0 0 0 3.181 1.372 -4.350 5.561 0.000 953 211 pi+ 91 950 0 0 0 0 0 3.494 1.438 -4.568 5.930 0.140 954 -211 pi- 91 950 0 0 0 0 0 2.023 0.731 -2.172 3.060 0.140 Charge sum: 0.000 Momentum sum: -0.000 0.000 0.000 1960.000 1960.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Warning in TimeShower::findMEcorr: ME weight above PS one PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again PYTHIA Abort from Pythia::next: reached end of Les Houches Events File *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | Les Houches User Process(es) 9999 | 100 100 100 | 5.480e-09 5.488e-10 | | ... whereof user classification code 81 | 94 94 94 | | | ... whereof user classification code 82 | 6 6 6 | | | | | | | sum | 100 100 100 | 5.480e-09 5.488e-10 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Abort from Pythia::next: reached end of Les Houches Events File | | 1 Error in Pythia::next: hadronLevel failed; try again | | 1 Error in StringFragmentation::fragment: stuck in joining | | 2 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | 1 Warning in TimeShower::findMEcorr: ME weight above PS one | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:03 charged particle multiplicity 8.10*10^ 0 7 7 7.80*10^ 0 X X 7.50*10^ 0 X X 7.20*10^ 0 X X 6.90*10^ 0 X X 6.60*10^ 0 X X 6.30*10^ 0 X X 6.00*10^ 0 X X X 5.70*10^ 0 X X X 5.40*10^ 0 X X X 5.10*10^ 0 X7X X7 4.80*10^ 0 XXX XX 4.50*10^ 0 XXX XX 4.20*10^ 0 333XXX 3 XX 3.90*10^ 0 XXXXXX X XX 3.60*10^ 0 XXXXXX X XX 3.30*10^ 0 XXXXXX X XX 3.00*10^ 0 X XX XXXXXXX X XX XX X X X 2.70*10^ 0 X XX XXXXXXX X XX XX X X X 2.40*10^ 0 X XX XXXXXXX X XX XX X X X 2.10*10^ 0 7X XX XXXXXXX X XX XX 7X7X X 7 1.80*10^ 0 XX XX XXXXXXX X XX XX XXXX X X 1.50*10^ 0 XX XX XXXXXXX X XX XX XXXX X X 1.20*10^ 0 3 3333XX33XX3XXXXXXX3X3XX3XX3XXXX 3 X3X 3 3 3 0.90*10^ 0 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X XXX X X X 0.60*10^ 0 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X XXX X X X 0.30*10^ 0 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X XXX X X X Contents *10^ 0 0000000000000010111123113313444858131431651232301031200010100000000000000000001000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^ 1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^ 0 1482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 100 Mean = 1.3990e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+02 Rms = 4.0906e+01 Overflow = 0.0000e+00 High edge = 3.9950e+02 pythia8-8.1.80.orig/examples/outref/out270000644000175000017500000037161212217346175016400 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:08:23 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* |------------------------- | KK mass is: 4000.000 |------------------------- *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | f fbar -> mu+ mu- (s-channel gamma_KK/Z_KK) 5073 | 7.047e-11 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 57.54 mb | | | | pT0 = 3.08 gives sigmaInteraction = 273.02 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | ExtraDimensionsTEV:ffbar2mu+mu- | on | off | | ExtraDimensionsTEV:nMax | 100.00000 | 10.00000 1.00000 100.00000 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:mHatMax | 8000.000 | -1.00000 | | PhaseSpace:mHatMin | 1000.000 | 4.00000 0.0 | | Random:seed | 0 | -1 900000000 | | Random:setSeed | on | off | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products 5000023 Z_KK 3 0 0 4.000e+03 2.400e+02 1.000e+03 8.000e+03 0.00000e+00 0 0 0 1 0 -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. In 1: id = -2, x = 6.093e-02, pdf = 1.356e-01 at Q2 = 2.884e+06. In 2: id = 2, x = 2.415e-01, pdf = 3.464e-01 at same Q2. Subprocess f fbar -> mu+ mu- (s-channel gamma_KK/Z_KK) with code 5073 is 2 -> 2. It has sHat = 2.884e+06, tHat = -1.027e+06, uHat = -1.857e+06, pTHat = 8.133e+02, m3Hat = 1.057e-01, m4Hat = 1.057e-01, thetaHat = 1.279e+00, phiHat = 3.371e+00. alphaEM = 8.086e-03, alphaS = 9.318e-02 at Q2 = 2.884e+06. Impact parameter b = 6.396e-01 gives enhancement factor = 1.818e+00. Max pT scale for MPI = 1.400e+04, ISR = 1.400e+04, FSR = 1.400e+04. Number of MPI = 7, ISR = 11, FSRproc = 49, FSRreson = 1. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 -2 (ubar) -21 1 0 5 0 0 101 0.000 0.000 426.483 426.483 0.000 4 2 (u) -21 2 0 5 0 101 0 0.000 0.000 -1690.760 1690.760 0.000 5 5000023 (Z_KK) -22 3 4 6 7 0 0 0.000 0.000 -1264.277 2117.242 1698.328 6 -13 mu+ 23 5 0 0 0 0 0 -792.004 -184.798 -327.636 876.793 0.106 7 13 mu- 23 5 0 0 0 0 0 792.004 184.798 -936.641 1240.450 0.106 Charge sum: 0.000 Momentum sum: 0.000 0.000 -1264.277 2117.242 1698.328 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 251 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 252 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 -2 (ubar) -21 6 6 5 0 0 101 0.000 0.000 426.483 426.483 0.000 4 2 (u) -21 7 0 5 0 101 0 0.000 0.000 -1690.760 1690.760 0.000 5 5000023 (Z_KK) -22 3 4 8 8 0 0 0.000 0.000 -1264.277 2117.242 1698.328 6 -2 (ubar) -42 16 16 3 3 0 101 -0.000 -0.000 426.483 426.483 0.000 7 2 (u) -41 28 28 9 4 102 0 0.000 0.000 -1970.674 1970.674 0.000 8 5000023 (Z_KK) -44 5 5 71 71 0 0 7.494 69.221 -1290.656 2134.235 1698.328 9 21 (g) -43 7 0 14 15 102 101 -7.494 -69.221 -253.535 262.922 0.000 10 21 (g) -31 21 21 12 13 103 104 0.000 0.000 319.901 319.901 0.000 11 21 (g) -31 22 0 12 13 105 106 0.000 0.000 -0.439 0.439 0.000 12 21 (g) -33 10 11 23 23 103 106 -5.066 -1.351 303.388 303.433 0.000 13 21 (g) -33 10 11 24 24 105 104 5.066 1.351 16.074 16.907 0.000 14 21 (g) -51 9 0 26 27 102 107 -3.033 -54.696 -210.067 217.092 0.000 15 21 (g) -51 9 0 73 73 107 101 -4.460 -14.525 -43.357 45.942 0.000 16 -2 (ubar) -53 69 0 6 6 0 101 -0.000 -0.000 426.595 426.595 0.000 17 21 (g) -31 29 0 19 20 109 110 0.000 0.000 5.887 5.887 0.000 18 1 (d) -31 30 30 19 20 108 0 0.000 0.000 -70.807 70.807 0.000 19 21 (g) -33 17 18 31 31 108 110 0.102 -3.969 5.154 6.506 0.000 20 1 (d) -33 17 18 32 32 109 0 -0.102 3.969 -70.074 70.188 0.330 21 21 (g) -42 42 42 10 10 103 104 0.000 0.000 319.901 319.901 0.000 22 1 (d) -41 97 97 25 11 105 0 -0.000 -0.000 -0.558 0.558 0.000 23 21 (g) -44 12 12 47 48 103 106 -5.174 -1.417 296.927 296.975 0.000 24 21 (g) -44 13 13 40 41 105 104 3.064 0.124 4.826 5.718 0.000 25 1 (d) -43 22 0 78 78 106 0 2.111 1.293 17.590 17.766 0.330 26 21 (g) -51 14 0 72 72 111 107 -3.749 -46.099 -169.589 175.783 0.000 27 21 (g) -51 14 0 74 74 102 111 0.716 -8.597 -44.344 45.176 0.000 28 2 (u) -53 70 70 7 7 102 0 0.000 0.000 -1974.541 1974.541 0.000 29 21 (g) -41 34 0 33 17 109 112 0.000 0.000 42.484 42.484 0.000 30 1 (d) -42 35 35 18 18 108 0 0.000 -0.000 -70.807 70.807 0.000 31 21 (g) -44 19 19 36 36 108 110 -0.468 -2.150 5.638 6.052 0.000 32 1 (d) -44 20 20 37 37 109 0 -0.108 3.987 -70.518 70.631 0.330 33 21 (g) -43 29 0 38 38 110 112 0.576 -1.837 36.556 36.607 0.000 34 1 (d) -41 55 55 39 29 109 0 -0.000 0.000 120.487 120.487 0.000 35 1 (d) -42 56 0 30 30 108 0 -0.000 0.000 -70.807 70.807 0.000 36 21 (g) -44 31 31 57 57 108 110 -0.541 -1.923 5.677 6.018 0.000 37 1 (d) -44 32 32 58 58 109 0 -0.109 3.989 -70.568 70.682 0.330 38 21 (g) -44 33 33 59 59 110 112 0.116 -0.419 36.595 36.597 0.000 39 1 (d) -43 34 0 60 60 112 0 0.534 -1.647 77.977 77.997 0.330 40 21 (g) -51 24 0 99 99 105 113 1.351 -0.483 0.940 1.715 0.000 41 21 (g) -51 24 0 101 101 113 104 1.713 0.607 14.113 14.230 0.000 42 21 (g) -53 49 49 21 21 103 104 -0.000 0.000 330.128 330.128 0.000 43 21 (g) -31 50 50 45 46 114 115 0.000 0.000 9.641 9.641 0.000 44 21 (g) -31 51 0 45 46 116 117 0.000 0.000 -0.715 0.715 0.000 45 21 (g) -33 43 44 52 52 114 117 0.228 -1.313 8.924 9.023 0.000 46 21 (g) -33 43 44 53 53 116 115 -0.228 1.313 0.003 1.333 0.000 47 21 (g) -51 23 0 76 77 118 106 -5.196 -1.031 362.134 362.173 0.000 48 21 (g) -51 23 0 102 102 103 118 0.021 -0.386 7.675 7.684 0.000 49 21 (g) -53 96 0 42 42 103 104 0.000 0.000 403.010 403.010 0.000 50 21 (g) -42 86 0 43 43 114 115 -0.000 0.000 9.641 9.641 0.000 51 21 (g) -41 68 68 54 44 116 119 0.000 -0.000 -53.120 53.120 0.000 52 21 (g) -44 45 45 88 88 114 117 0.144 -1.302 8.167 8.271 0.000 53 21 (g) -44 46 46 66 67 116 115 -1.355 1.461 0.713 2.117 0.000 54 21 (g) -43 51 0 90 90 117 119 1.212 -0.159 -52.359 52.374 0.000 55 1 (d) -42 146 146 34 34 109 0 -0.000 0.000 120.487 120.487 0.000 56 1 (d) -41 176 176 61 35 120 0 0.000 -0.000 -83.987 83.987 0.000 57 21 (g) -44 36 36 93 94 108 110 -0.543 -1.921 5.669 6.011 0.000 58 1 (d) -44 37 37 144 145 109 0 -0.918 4.682 -70.559 70.721 0.330 59 21 (g) -44 38 38 117 117 110 112 0.116 -0.419 36.584 36.587 0.000 60 1 (d) -44 39 39 290 290 112 0 0.534 -1.647 77.949 77.969 0.330 61 21 (g) -43 56 0 95 95 120 108 0.811 -0.695 -13.144 13.187 0.000 62 21 (g) -31 225 0 64 65 121 122 0.000 0.000 1.341 1.341 0.000 63 21 (g) -31 226 226 64 65 123 121 0.000 0.000 -5.178 5.178 0.000 64 21 (g) -33 62 63 156 157 123 124 0.896 0.475 -4.927 5.030 0.000 65 21 (g) -33 62 63 158 158 124 122 -0.896 -0.475 1.090 1.489 0.000 66 21 (g) -51 53 0 89 89 125 115 -1.536 1.933 -0.364 2.496 0.000 67 21 (g) -51 53 0 91 91 116 125 0.181 -0.472 0.166 0.532 0.000 68 21 (g) -53 87 87 51 51 116 119 0.000 0.000 -54.032 54.032 0.000 69 -2 (ubar) -41 251 251 75 16 0 126 -0.000 -0.000 478.737 478.737 0.000 70 2 (u) -42 179 179 28 28 102 0 0.000 0.000 -1974.541 1974.541 0.000 71 5000023 (Z_KK) -44 8 8 253 253 0 0 6.549 68.988 -1290.624 2134.205 1698.328 72 21 (g) -44 26 26 139 139 111 107 -3.756 -46.101 -169.606 175.800 0.000 73 21 (g) -44 15 15 131 132 107 101 -4.463 -14.526 -43.365 45.951 0.000 74 21 (g) -44 27 27 137 138 102 111 0.715 -8.597 -44.346 45.177 0.000 75 21 (g) -43 69 0 133 133 101 126 0.956 0.236 52.136 52.146 0.000 76 21 (g) -51 47 0 98 98 118 127 -1.783 0.602 99.033 99.051 0.000 77 21 (g) -51 47 0 79 80 127 106 -3.350 -1.595 263.608 263.634 0.000 78 1 (d) -52 25 25 81 81 106 0 2.048 1.254 17.082 17.253 0.330 79 21 (g) -51 77 0 103 103 127 128 -2.450 -0.150 161.674 161.693 0.000 80 21 (g) -51 77 0 104 104 128 106 -0.834 -1.404 102.468 102.481 0.000 81 1 (d) -52 78 78 100 100 106 0 1.981 1.214 16.547 16.713 0.330 82 21 (g) -31 330 330 84 85 130 129 0.000 0.000 13.228 13.228 0.000 83 21 (g) -31 331 331 84 85 132 131 0.000 0.000 -0.296 0.296 0.000 84 21 (g) -33 82 83 332 332 132 129 0.668 -0.617 12.472 12.505 0.000 85 21 (g) -33 82 83 333 333 130 131 -0.668 0.617 0.460 1.019 0.000 86 21 (g) -41 121 121 92 50 114 133 0.000 -0.000 10.205 10.205 0.000 87 21 (g) -42 122 0 68 68 116 119 -0.000 0.000 -54.032 54.032 0.000 88 21 (g) -44 52 52 112 113 114 117 -0.037 -0.609 8.265 8.287 0.000 89 21 (g) -44 66 66 120 120 125 115 -1.559 2.023 -0.447 2.593 0.000 90 21 (g) -44 54 54 114 114 117 119 1.212 -0.158 -51.978 51.992 0.000 91 21 (g) -44 67 67 118 119 116 125 0.173 -0.443 0.191 0.512 0.000 92 21 (g) -43 86 0 127 127 115 133 0.212 -0.813 0.142 0.852 0.000 93 21 (g) -51 57 0 115 116 134 110 -0.865 -2.340 4.595 5.229 0.000 94 21 (g) -51 57 0 159 160 108 134 0.335 0.406 0.853 1.003 0.000 95 21 (g) -52 61 61 174 175 120 108 0.798 -0.683 -12.923 12.966 0.000 96 21 (g) -41 270 270 105 49 103 135 0.000 0.000 440.160 440.160 0.000 97 1 (d) -42 271 271 22 22 105 0 0.000 -0.000 -0.558 0.558 0.000 98 21 (g) -44 76 76 272 272 118 127 -1.899 0.760 99.960 99.981 0.000 99 21 (g) -44 40 40 273 273 105 113 1.349 -0.481 0.957 1.722 0.000 100 1 (d) -44 81 81 108 108 106 0 1.962 1.240 16.704 16.868 0.330 101 21 (g) -44 41 41 134 135 113 104 1.696 0.630 14.247 14.362 0.000 102 21 (g) -44 48 48 276 276 103 118 0.012 -0.374 7.747 7.756 0.000 103 21 (g) -44 79 79 150 151 127 128 -2.640 0.108 163.188 163.210 0.000 104 21 (g) -44 80 80 106 107 128 106 -0.954 -1.240 103.429 103.441 0.000 105 21 (g) -43 96 0 136 136 104 135 0.473 -0.645 33.369 33.379 0.000 106 21 (g) -51 104 0 109 110 128 136 -0.294 0.456 7.888 7.907 0.000 107 21 (g) -51 104 0 111 111 136 106 -0.420 -1.544 97.503 97.516 0.000 108 1 (d) -52 100 100 274 274 106 0 1.722 1.089 14.742 14.886 0.330 109 21 (g) -51 106 0 152 152 128 137 -0.831 -0.854 54.676 54.689 0.000 110 21 (g) -51 106 0 281 281 137 136 0.293 0.415 9.724 9.738 0.000 111 21 (g) -52 107 107 280 280 136 106 -0.177 -0.649 40.991 40.997 0.000 112 21 (g) -51 88 0 123 123 114 138 0.344 -0.328 8.207 8.221 0.000 113 21 (g) -51 88 0 128 128 138 117 -0.361 -0.284 -0.788 0.912 0.000 114 21 (g) -52 90 90 125 125 117 119 1.192 -0.155 -51.133 51.147 0.000 115 21 (g) -51 93 0 161 161 134 139 -1.195 -2.536 6.220 6.823 0.000 116 21 (g) -51 93 0 218 218 139 110 0.342 0.152 2.248 2.279 0.000 117 21 (g) -52 59 59 236 237 110 112 0.104 -0.375 32.711 32.714 0.000 118 21 (g) -51 91 0 126 126 116 140 -0.292 0.103 0.735 0.798 0.000 119 21 (g) -51 91 0 129 129 140 125 -0.206 0.326 -0.736 0.831 0.000 120 21 (g) -52 89 89 124 124 125 115 -0.888 1.152 -0.254 1.477 0.000 121 21 (g) -42 304 304 86 86 114 133 -0.000 0.000 10.205 10.205 0.000 122 21 (g) -41 305 305 130 87 116 141 0.000 0.000 -819.442 819.442 0.000 123 21 (g) -44 112 112 147 148 114 138 0.344 -0.328 8.208 8.221 0.000 124 21 (g) -44 120 120 209 209 125 115 -0.877 1.149 -0.263 1.469 0.000 125 21 (g) -44 114 114 155 155 117 119 1.864 -0.332 -51.136 51.171 0.000 126 21 (g) -44 118 118 233 234 116 140 -0.292 0.102 0.733 0.795 0.000 127 21 (g) -44 92 92 207 208 115 133 0.217 -0.814 0.145 0.855 0.000 128 21 (g) -44 113 113 149 149 138 117 -0.350 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495 735 736 0 0 -0.160 0.489 -5.539 5.585 0.498 587 -211 pi- 91 496 0 0 0 0 0 -0.176 0.033 -7.465 7.468 0.140 588 111 (pi0) -91 496 0 737 738 0 0 0.061 0.419 -5.053 5.072 0.135 589 211 pi+ 91 498 0 0 0 0 0 0.069 -0.277 -2.977 2.994 0.140 590 -211 pi- 91 498 0 0 0 0 0 0.227 0.334 -20.749 20.754 0.140 591 211 pi+ 91 506 0 0 0 0 0 0.073 0.121 -219.396 219.396 0.140 592 -211 pi- 91 506 0 0 0 0 0 0.084 -0.340 -34.431 34.433 0.140 593 -211 pi- 91 515 0 0 0 0 0 -0.515 0.504 -16.333 16.349 0.140 594 111 (pi0) -91 515 0 739 740 0 0 -0.377 0.636 -7.210 7.249 0.135 595 211 pi+ 91 517 0 0 0 0 0 -0.278 -0.349 -1.341 1.420 0.140 596 111 (pi0) -91 517 0 741 742 0 0 -0.058 0.335 -1.953 1.987 0.135 597 -211 pi- 91 518 0 0 0 0 0 0.262 -0.053 -0.607 0.678 0.140 598 111 (pi0) -91 518 0 743 744 0 0 -0.260 -0.245 -0.398 0.552 0.135 599 211 pi+ 91 526 0 0 0 0 0 0.345 0.261 0.734 0.864 0.140 600 111 (pi0) -91 526 0 745 746 0 0 0.141 -0.032 2.482 2.490 0.135 601 -211 pi- 91 527 0 0 0 0 0 0.293 0.255 2.496 2.530 0.140 602 111 (pi0) -91 527 0 747 748 0 0 0.801 -0.635 2.779 2.964 0.135 603 -3122 (Lambdabar0) -91 530 0 749 750 0 0 0.017 -0.299 91.477 91.484 1.116 604 -211 pi- 91 530 0 0 0 0 0 0.193 -0.049 36.098 36.099 0.140 605 211 pi+ 91 532 0 0 0 0 0 -0.361 0.235 35.329 35.332 0.140 606 -211 pi- 91 532 0 0 0 0 0 0.142 0.250 79.188 79.189 0.140 607 2112 n0 91 536 0 0 0 0 0 0.374 0.431 1779.575 1779.575 0.940 608 211 pi+ 91 536 0 0 0 0 0 0.039 0.452 604.498 604.499 0.140 609 310 (K_S0) -91 552 552 751 752 0 0 -0.217 -0.684 28.860 28.873 0.498 610 211 pi+ 91 382 0 0 0 0 0 0.413 0.059 2.033 2.080 0.140 611 -211 pi- 91 382 0 0 0 0 0 0.308 -0.228 2.982 3.010 0.140 612 111 (pi0) -91 382 0 753 754 0 0 0.270 -0.361 1.658 1.724 0.135 613 111 (pi0) -91 383 0 755 756 0 0 -0.189 0.200 1.166 1.206 0.135 614 111 (pi0) -91 383 0 757 758 0 0 -0.199 0.117 1.492 1.516 0.135 615 111 (pi0) -91 383 0 759 760 0 0 -0.303 0.065 0.817 0.884 0.135 616 22 gamma 91 384 0 0 0 0 0 0.183 -0.606 3.222 3.284 0.000 617 22 gamma 91 384 0 0 0 0 0 0.127 -0.264 1.131 1.169 0.000 618 22 gamma 91 387 0 0 0 0 0 0.072 -0.097 0.031 0.125 0.000 619 22 gamma 91 387 0 0 0 0 0 0.108 0.032 0.014 0.113 0.000 620 22 gamma 91 399 0 0 0 0 0 0.365 0.202 3.886 3.908 0.000 621 22 gamma 91 399 0 0 0 0 0 0.684 0.396 5.822 5.875 0.000 622 22 gamma 91 402 0 0 0 0 0 0.132 0.071 1.790 1.796 0.000 623 22 gamma 91 402 0 0 0 0 0 0.157 0.011 4.020 4.023 0.000 624 211 pi+ 91 414 0 0 0 0 0 0.014 -0.504 11.972 11.983 0.140 625 -211 pi- 91 414 0 0 0 0 0 0.113 -0.254 8.089 8.095 0.140 626 111 (pi0) -91 414 0 761 762 0 0 -0.066 -0.111 6.029 6.032 0.135 627 2112 n0 91 415 0 0 0 0 0 0.653 -0.178 11.269 11.329 0.940 628 211 pi+ 91 415 0 0 0 0 0 0.192 -0.125 1.214 1.243 0.140 629 -2112 nbar0 91 416 0 0 0 0 0 0.552 -0.202 3.516 3.686 0.940 630 -211 pi- 91 416 0 0 0 0 0 -0.093 -0.120 0.686 0.717 0.140 631 22 gamma 91 419 0 0 0 0 0 0.312 -1.035 22.537 22.563 0.000 632 22 gamma 91 419 0 0 0 0 0 0.067 -0.177 2.952 2.958 0.000 633 22 gamma 91 423 0 0 0 0 0 -0.001 -0.128 0.702 0.713 0.000 634 22 gamma 91 423 0 0 0 0 0 0.133 -0.265 2.725 2.741 0.000 635 22 gamma 91 424 0 0 0 0 0 0.102 0.230 0.196 0.319 0.000 636 22 gamma 91 424 0 0 0 0 0 0.067 0.212 0.037 0.225 0.000 637 22 gamma 91 426 0 0 0 0 0 -0.021 0.040 -0.132 0.140 0.000 638 22 gamma 91 426 0 0 0 0 0 -0.097 0.018 -0.016 0.101 0.000 639 2212 p+ 91 431 0 0 0 0 0 0.018 0.351 356.887 356.888 0.938 640 111 (pi0) -91 431 0 763 764 0 0 0.123 -0.013 154.223 154.223 0.135 641 -2112 nbar0 91 432 0 0 0 0 0 0.145 0.726 415.564 415.565 0.940 642 -211 pi- 91 432 0 0 0 0 0 -0.073 -0.057 71.821 71.822 0.140 643 211 pi+ 91 433 0 0 0 0 0 0.016 0.032 4.856 4.858 0.140 644 -211 pi- 91 433 0 0 0 0 0 0.107 -0.123 32.944 32.945 0.140 645 111 (pi0) -91 433 0 765 766 0 0 -0.113 -0.175 6.278 6.283 0.135 646 211 pi+ 91 439 0 0 0 0 0 -0.153 0.361 -0.961 1.047 0.140 647 -211 pi- 91 439 0 0 0 0 0 -0.124 -0.016 -0.162 0.248 0.140 648 111 (pi0) -91 439 0 767 768 0 0 0.192 0.132 -0.655 0.708 0.135 649 211 pi+ 91 466 0 0 0 0 0 0.033 -0.045 0.160 0.219 0.140 650 -211 pi- 91 466 0 0 0 0 0 -0.166 0.021 0.166 0.274 0.140 651 111 (pi0) -91 466 0 769 770 0 0 -0.127 -0.207 0.208 0.347 0.135 652 211 pi+ 91 471 0 0 0 0 0 -0.042 -0.025 -0.295 0.330 0.140 653 -211 pi- 91 471 0 0 0 0 0 -0.194 -0.103 -0.239 0.353 0.140 654 111 (pi0) -91 471 0 771 772 0 0 0.277 -0.250 -0.194 0.442 0.135 655 22 gamma 91 477 0 0 0 0 0 -1.155 -3.159 -10.384 10.916 0.000 656 22 gamma 91 477 0 0 0 0 0 -0.133 -0.394 -0.781 0.884 0.000 657 22 gamma 91 480 0 0 0 0 0 0.007 -0.012 -0.039 0.042 0.000 658 22 gamma 91 480 0 0 0 0 0 -0.498 -2.631 -8.442 8.857 0.000 659 211 pi+ 91 482 0 0 0 0 0 -0.245 -2.855 -9.609 10.028 0.140 660 -211 pi- 91 482 0 0 0 0 0 -0.248 -5.174 -18.767 19.469 0.140 661 111 (pi0) -91 482 0 773 774 0 0 -0.537 -3.378 -11.609 12.103 0.135 662 22 gamma 91 483 0 0 0 0 0 -0.206 -2.598 -10.338 10.662 0.000 663 22 gamma 91 483 0 0 0 0 0 -0.257 -2.328 -8.870 9.174 0.000 664 2112 n0 91 488 0 0 0 0 0 0.141 -2.064 -9.892 10.149 0.940 665 -211 pi- 91 488 0 0 0 0 0 -0.056 -0.058 -0.897 0.911 0.140 666 -2112 nbar0 91 489 0 0 0 0 0 -0.273 -1.293 -6.104 6.316 0.940 667 211 pi+ 91 489 0 0 0 0 0 -0.093 -0.706 -2.185 2.302 0.140 668 211 pi+ 91 497 0 0 0 0 0 0.091 0.248 -3.398 3.411 0.140 669 -211 pi- 91 497 0 0 0 0 0 0.178 0.547 -11.978 11.993 0.140 670 111 (pi0) -91 497 0 775 776 0 0 0.495 0.195 -9.514 9.530 0.135 671 211 pi+ 91 499 0 0 0 0 0 0.169 -0.164 -6.204 6.210 0.140 672 -211 pi- 91 499 0 0 0 0 0 0.494 0.059 -21.379 21.385 0.140 673 111 (pi0) -91 499 0 777 778 0 0 0.404 -0.263 -29.074 29.079 0.135 674 22 gamma 91 500 0 0 0 0 0 -0.244 0.086 -28.712 28.713 0.000 675 22 gamma 91 500 0 0 0 0 0 -0.194 0.041 -12.404 12.405 0.000 676 211 pi+ 91 502 0 0 0 0 0 -0.563 -0.715 -113.262 113.266 0.140 677 -211 pi- 91 502 0 0 0 0 0 -0.008 -0.067 -10.673 10.674 0.140 678 111 (pi0) -91 502 0 779 780 0 0 -0.058 -0.105 -48.843 48.843 0.135 679 22 gamma 91 504 0 0 0 0 0 0.026 -0.110 -29.477 29.477 0.000 680 22 gamma 91 504 0 0 0 0 0 -0.121 -0.140 -58.315 58.315 0.000 681 22 gamma 91 507 0 0 0 0 0 -0.226 -0.368 -129.752 129.753 0.000 682 22 gamma 91 507 0 0 0 0 0 -0.255 -0.265 -142.982 142.983 0.000 683 211 pi+ 91 516 0 0 0 0 0 -0.008 0.177 -1.002 1.028 0.140 684 -211 pi- 91 516 0 0 0 0 0 -0.182 0.219 -1.343 1.380 0.140 685 111 (pi0) -91 516 0 781 782 0 0 0.014 0.435 -2.712 2.750 0.135 686 2112 n0 91 521 0 0 0 0 0 0.962 0.025 3.548 3.795 0.940 687 211 pi+ 91 521 0 0 0 0 0 0.033 0.043 1.000 1.011 0.140 688 -2112 nbar0 91 522 0 0 0 0 0 0.062 -0.257 6.622 6.694 0.940 689 -211 pi- 91 522 0 0 0 0 0 -0.096 -0.246 2.987 3.002 0.140 690 211 pi+ 91 523 0 0 0 0 0 -0.088 0.134 1.300 1.318 0.140 691 -211 pi- 91 523 0 0 0 0 0 0.131 0.065 2.341 2.349 0.140 692 111 (pi0) -91 523 0 783 784 0 0 -0.047 -0.009 1.334 1.342 0.135 693 211 pi+ 91 528 0 0 0 0 0 0.158 -0.016 0.868 0.893 0.140 694 -211 pi- 91 528 0 0 0 0 0 0.594 -0.273 0.868 1.095 0.140 695 111 (pi0) -91 528 0 785 786 0 0 0.126 0.108 0.291 0.361 0.135 696 2212 p+ 91 529 0 0 0 0 0 0.351 0.397 9.959 10.017 0.938 697 111 (pi0) -91 529 0 787 788 0 0 -0.096 0.175 3.702 3.710 0.135 698 22 gamma 91 531 0 0 0 0 0 -0.161 -0.172 44.680 44.680 0.000 699 22 gamma 91 531 0 0 0 0 0 0.027 -0.020 8.010 8.010 0.000 700 211 pi+ 91 535 0 0 0 0 0 -0.011 0.173 224.072 224.072 0.140 701 -211 pi- 91 535 0 0 0 0 0 -0.120 0.151 256.174 256.174 0.140 702 111 (pi0) -91 535 0 789 790 0 0 -0.024 0.026 437.127 437.127 0.135 703 22 gamma 91 539 0 0 0 0 0 0.386 -0.079 -374.053 374.053 0.000 704 22 gamma 91 539 0 0 0 0 0 0.188 -0.032 -294.165 294.165 0.000 705 22 gamma 91 545 0 0 0 0 0 -0.006 0.001 0.062 0.063 0.000 706 22 gamma 91 545 0 0 0 0 0 -0.779 -0.164 46.444 46.451 0.000 707 22 gamma 91 547 0 0 0 0 0 -0.190 0.039 12.277 12.279 0.000 708 22 gamma 91 547 0 0 0 0 0 -0.024 0.049 8.772 8.772 0.000 709 22 gamma 91 549 0 0 0 0 0 -0.195 -0.040 9.321 9.323 0.000 710 22 gamma 91 549 0 0 0 0 0 -0.298 -0.241 20.169 20.173 0.000 711 2212 p+ 91 550 0 0 0 0 0 -0.454 0.307 81.582 81.589 0.938 712 -211 pi- 91 550 0 0 0 0 0 -0.103 0.161 13.222 13.224 0.140 713 22 gamma 91 551 0 0 0 0 0 0.043 0.096 2.760 2.762 0.000 714 22 gamma 91 551 0 0 0 0 0 0.034 -0.047 1.426 1.427 0.000 715 22 gamma 91 555 0 0 0 0 0 0.232 -0.408 7.162 7.177 0.000 716 22 gamma 91 555 0 0 0 0 0 0.319 -0.374 9.230 9.243 0.000 717 22 gamma 91 557 0 0 0 0 0 -0.089 0.008 0.583 0.590 0.000 718 22 gamma 91 557 0 0 0 0 0 -0.135 -0.083 0.404 0.434 0.000 719 22 gamma 91 563 0 0 0 0 0 0.006 -0.011 2.080 2.080 0.000 720 22 gamma 91 563 0 0 0 0 0 0.264 0.299 26.269 26.272 0.000 721 22 gamma 91 565 0 0 0 0 0 -0.059 0.143 -0.201 0.254 0.000 722 22 gamma 91 565 0 0 0 0 0 0.039 0.014 -0.011 0.043 0.000 723 22 gamma 91 569 0 0 0 0 0 0.258 -0.211 -0.498 0.599 0.000 724 22 gamma 91 569 0 0 0 0 0 0.142 -0.009 -0.197 0.244 0.000 725 22 gamma 91 571 0 0 0 0 0 -0.049 0.008 -0.005 0.050 0.000 726 22 gamma 91 571 0 0 0 0 0 -0.270 0.091 -0.419 0.507 0.000 727 22 gamma 91 575 0 0 0 0 0 -0.738 -4.509 -15.101 15.777 0.000 728 22 gamma 91 575 0 0 0 0 0 -0.327 -1.805 -6.345 6.604 0.000 729 22 gamma 91 577 0 0 0 0 0 -0.374 -3.989 -14.614 15.153 0.000 730 22 gamma 91 577 0 0 0 0 0 -0.254 -3.931 -14.639 15.160 0.000 731 22 gamma 91 583 0 0 0 0 0 -0.011 0.006 -0.069 0.070 0.000 732 22 gamma 91 583 0 0 0 0 0 0.293 0.567 -2.169 2.261 0.000 733 -2212 pbar- 91 584 0 0 0 0 0 -0.088 0.909 -9.812 9.899 0.938 734 211 pi+ 91 584 0 0 0 0 0 -0.036 0.333 -3.060 3.082 0.140 735 111 (pi0) -91 586 0 791 792 0 0 -0.152 0.009 -2.139 2.148 0.135 736 111 (pi0) -91 586 0 793 794 0 0 -0.008 0.480 -3.400 3.437 0.135 737 22 gamma 91 588 0 0 0 0 0 -0.002 0.299 -2.944 2.959 0.000 738 22 gamma 91 588 0 0 0 0 0 0.063 0.120 -2.109 2.113 0.000 739 22 gamma 91 594 0 0 0 0 0 -0.061 0.069 -0.565 0.573 0.000 740 22 gamma 91 594 0 0 0 0 0 -0.316 0.567 -6.645 6.677 0.000 741 22 gamma 91 596 0 0 0 0 0 0.022 0.012 -0.285 0.286 0.000 742 22 gamma 91 596 0 0 0 0 0 -0.080 0.323 -1.668 1.701 0.000 743 22 gamma 91 598 0 0 0 0 0 -0.212 -0.242 -0.289 0.433 0.000 744 22 gamma 91 598 0 0 0 0 0 -0.048 -0.003 -0.109 0.119 0.000 745 22 gamma 91 600 0 0 0 0 0 0.113 -0.082 1.800 1.805 0.000 746 22 gamma 91 600 0 0 0 0 0 0.028 0.050 0.682 0.685 0.000 747 22 gamma 91 602 0 0 0 0 0 0.322 -0.242 1.286 1.347 0.000 748 22 gamma 91 602 0 0 0 0 0 0.479 -0.394 1.493 1.617 0.000 749 -2112 nbar0 91 603 0 0 0 0 0 0.091 -0.210 81.197 81.203 0.940 750 111 (pi0) -91 603 0 795 796 0 0 -0.074 -0.088 10.280 10.281 0.135 751 211 pi+ 91 609 0 0 0 0 0 -0.262 -0.659 24.606 24.617 0.140 752 -211 pi- 91 609 0 0 0 0 0 0.046 -0.026 4.254 4.257 0.140 753 22 gamma 91 612 0 0 0 0 0 0.275 -0.295 1.375 1.433 0.000 754 22 gamma 91 612 0 0 0 0 0 -0.005 -0.066 0.284 0.291 0.000 755 22 gamma 91 613 0 0 0 0 0 -0.006 -0.013 0.016 0.022 0.000 756 22 gamma 91 613 0 0 0 0 0 -0.183 0.213 1.150 1.184 0.000 757 22 gamma 91 614 0 0 0 0 0 -0.211 0.102 1.457 1.476 0.000 758 22 gamma 91 614 0 0 0 0 0 0.012 0.016 0.035 0.040 0.000 759 22 gamma 91 615 0 0 0 0 0 -0.280 0.037 0.791 0.840 0.000 760 22 gamma 91 615 0 0 0 0 0 -0.023 0.028 0.027 0.045 0.000 761 22 gamma 91 626 0 0 0 0 0 -0.096 -0.033 2.947 2.949 0.000 762 22 gamma 91 626 0 0 0 0 0 0.030 -0.078 3.082 3.083 0.000 763 22 gamma 91 640 0 0 0 0 0 0.077 0.021 135.075 135.075 0.000 764 22 gamma 91 640 0 0 0 0 0 0.046 -0.034 19.148 19.148 0.000 765 22 gamma 91 645 0 0 0 0 0 0.016 -0.056 2.693 2.694 0.000 766 22 gamma 91 645 0 0 0 0 0 -0.129 -0.119 3.585 3.589 0.000 767 22 gamma 91 648 0 0 0 0 0 0.084 0.067 -0.484 0.496 0.000 768 22 gamma 91 648 0 0 0 0 0 0.108 0.065 -0.171 0.212 0.000 769 22 gamma 91 651 0 0 0 0 0 -0.025 -0.075 0.151 0.170 0.000 770 22 gamma 91 651 0 0 0 0 0 -0.103 -0.132 0.057 0.177 0.000 771 22 gamma 91 654 0 0 0 0 0 0.026 -0.009 -0.065 0.071 0.000 772 22 gamma 91 654 0 0 0 0 0 0.251 -0.241 -0.129 0.371 0.000 773 22 gamma 91 661 0 0 0 0 0 -0.316 -2.292 -7.702 8.042 0.000 774 22 gamma 91 661 0 0 0 0 0 -0.221 -1.086 -3.906 4.061 0.000 775 22 gamma 91 670 0 0 0 0 0 0.456 0.153 -7.757 7.772 0.000 776 22 gamma 91 670 0 0 0 0 0 0.039 0.042 -1.757 1.758 0.000 777 22 gamma 91 673 0 0 0 0 0 0.151 -0.170 -11.594 11.596 0.000 778 22 gamma 91 673 0 0 0 0 0 0.253 -0.093 -17.481 17.483 0.000 779 22 gamma 91 678 0 0 0 0 0 0.030 -0.071 -14.318 14.319 0.000 780 22 gamma 91 678 0 0 0 0 0 -0.087 -0.034 -34.524 34.524 0.000 781 22 gamma 91 685 0 0 0 0 0 0.032 0.059 -0.225 0.235 0.000 782 22 gamma 91 685 0 0 0 0 0 -0.017 0.376 -2.487 2.515 0.000 783 22 gamma 91 692 0 0 0 0 0 -0.072 -0.051 0.649 0.655 0.000 784 22 gamma 91 692 0 0 0 0 0 0.024 0.042 0.685 0.687 0.000 785 22 gamma 91 695 0 0 0 0 0 0.154 0.087 0.255 0.310 0.000 786 22 gamma 91 695 0 0 0 0 0 -0.029 0.022 0.036 0.051 0.000 787 22 gamma 91 697 0 0 0 0 0 0.025 0.083 1.100 1.104 0.000 788 22 gamma 91 697 0 0 0 0 0 -0.121 0.092 2.602 2.606 0.000 789 22 gamma 91 702 0 0 0 0 0 0.052 0.030 147.575 147.575 0.000 790 22 gamma 91 702 0 0 0 0 0 -0.076 -0.004 289.552 289.552 0.000 791 22 gamma 91 735 0 0 0 0 0 0.008 0.037 -0.575 0.577 0.000 792 22 gamma 91 735 0 0 0 0 0 -0.160 -0.028 -1.563 1.572 0.000 793 22 gamma 91 736 0 0 0 0 0 -0.004 0.020 -0.040 0.045 0.000 794 22 gamma 91 736 0 0 0 0 0 -0.005 0.460 -3.361 3.392 0.000 795 22 gamma 91 750 0 0 0 0 0 -0.036 -0.060 9.399 9.399 0.000 796 22 gamma 91 750 0 0 0 0 0 -0.038 -0.028 0.880 0.882 0.000 Charge sum: 2.000 Momentum sum: 0.000 0.000 -0.000 14000.000 14000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- Event: 0 PYTHIA Warning in PhaseSpace2to2tauyz::trialKin: maximum for cross section violated Event: 10 Event: 20 Event: 30 PYTHIA Warning in SpaceShower::pT2nextQCD: weight above unity Event: 40 PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame Event: 50 Event: 60 Event: 70 Event: 80 Event: 90 Event: 100 Event: 110 Event: 120 Event: 130 Event: 140 Event: 150 Event: 160 Event: 170 Event: 180 Event: 190 Event: 200 Event: 210 Event: 220 Event: 230 Event: 240 Event: 250 Event: 260 Event: 270 Event: 280 Event: 290 Event: 300 Event: 310 Event: 320 Event: 330 Event: 340 Event: 350 Event: 360 Event: 370 Event: 380 Event: 390 Event: 400 Event: 410 Event: 420 Event: 430 Event: 440 Event: 450 Event: 460 Event: 470 Event: 480 Event: 490 *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | f fbar -> mu+ mu- (s-channel gamma_KK/Z_KK) 5073 | 7476 500 500 | 5.224e-12 1.671e-13 | | | | | | sum | 7476 500 500 | 5.224e-12 1.671e-13 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 79 Warning in PhaseSpace2to2tauyz::trialKin: maximum for cross section violated | | 6 Warning in SpaceShower::pT2nextQCD: weight above unity | | 3 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:08 dN/dmHat 4.60*10^ 1 5 4.40*10^ 1 X 4.20*10^ 1 X 4.00*10^ 1 X 3.80*10^ 1 X 3.60*10^ 1 X 3.40*10^ 1 X 3.20*10^ 1 X 3.00*10^ 1 X 2.80*10^ 1 X X 2.60*10^ 1 X X 2.40*10^ 1 X X 2.20*10^ 1 X X 2.00*10^ 1 X X 1.80*10^ 1 X X 1.60*10^ 1 XX 5X 1.40*10^ 1 XX XX 1.20*10^ 1 XX XX 1.00*10^ 1 XX5 XX 0.80*10^ 1 XXX XXX 0.60*10^ 1 XXX XXXX 0.40*10^ 1 XXXX XXXXX5 0.20*10^ 1 XXXX 5 5 X 5XXXXXX Contents *10^ 1 41000000000000000000120000000000000000000000000000 *10^ 0 56940100010002000148586300000000000000000000000000 *10^-1 00000000000000000000000000000000000000000000000000 *10^-2 00000000000000000000000000000000000000000000000000 Low edge *10^ 3 11111111222222233333334444444555555566666667777777 *10^ 2 01245789124568912356890235679023467901346780134578 *10^ 1 04826048260482604826048260482604826048260482604826 Entries = 143 Mean = 2.4563e+03 Underflow = 0.0000e+00 Low edge = 1.0000e+03 All chan = 1.4300e+02 Rms = 1.3764e+03 Overflow = 0.0000e+00 High edge = 8.0000e+03 2013-09-20 16:08 (dN/dpT)_mu^- 1.50*10^ 1 X 1.44*10^ 1 X 1.38*10^ 1 X 1.32*10^ 1 7X 1.26*10^ 1 XX 1.20*10^ 1 XX 1.14*10^ 1 XX 1.08*10^ 1 XX 1.02*10^ 1 XX 0.96*10^ 1 XX 0.90*10^ 1 XX 0.84*10^ 1 XX3 0.78*10^ 1 XXX 0.72*10^ 1 7 XXX 0.66*10^ 1 X XXX 0.60*10^ 1 XXXXXX X X 0.54*10^ 1 3 XXXXXX X 3 X 0.48*10^ 1 X XXXXXX X X X 0.42*10^ 1 X XXXXXX X X 777X 777 0.36*10^ 1 X XXXXXX X X XXXX XXX 0.30*10^ 1 X XXXXXXXXXX X XX XXXX XXX 0.24*10^ 1 3X3XXXXXXXXXX33 3 33 X 3 XX3XXXX XXX 0.18*10^ 1 XXXXXXXXXXXXXXX X XX X X XXXXXXX XXX 0.12*10^ 1 XXXXXXXXXXXXXXX77X77XX7X7X XXXXXXX7 XXX77 0.06*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXX XXXXXXXX XXXXX Contents *10^ 1 00000000011000000000000000000000000000000000000000 *10^ 0 02325376635836221121122151203324446104441100000000 *10^-1 00000000000000000000000000000000000000000000000000 *10^-2 00000000000000000000000000000000000000000000000000 Low edge *10^ 3 00000000000000000000111111111111111111112222222222 *10^ 2 00112233445566778899001122334455667788990011223344 *10^ 1 05050505050505050505050505050505050505050505050505 Entries = 143 Mean = 9.0467e+02 Underflow = 0.0000e+00 Low edge = 1.0000e+00 All chan = 1.4300e+02 Rms = 5.8691e+02 Overflow = 0.0000e+00 High edge = 2.5010e+03 |----------------------------------------| | CPU Runtime = 1.4423e+01 sec |----------------------------------------| pythia8-8.1.80.orig/examples/outref/out200000644000175000017500000003705412217346174016367 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:06:28 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 8.000e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | f fbar -> gamma*/Z0 gamma*/Z0 231 | 2.815e-07 | | f fbar' -> Z0 W+- (no gamma*!) 232 | 3.934e-07 | | f fbar -> W+ W- 233 | 4.239e-07 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:eCM | 8000.000 | 14000.000 10.00000 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PartonLevel:all | off | on | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | WeakDoubleBoson:all | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products 23 Z0 3 0 0 91.18760 2.50687 50.00000 0.00000 0.00000e+00 1 1 0 0 0 0 1 0.1541199 0 1 -1 1 1 0.1195484 0 2 -2 2 1 0.1541093 0 3 -3 3 1 0.1193873 0 4 -4 4 1 0.1523969 0 5 -5 5 1 0.0335122 0 11 -11 6 1 0.0666593 0 12 -12 7 1 0.0335119 0 13 -13 8 1 0.0666593 0 14 -14 9 1 0.0334363 0 15 -15 10 1 0.0666593 0 16 -16 24 W+ W- 3 3 0 80.38500 2.09454 50.00000 0.00000 0.00000e+00 1 1 0 1 0 0 1 0.3206876 0 -1 2 1 1 0.0174315 0 -1 4 2 1 0.0174549 0 -3 2 3 1 0.3199453 0 -3 4 4 1 0.0000053 0 -5 2 5 1 0.0005990 0 -5 4 6 1 0.1079853 0 -11 12 7 1 0.1079850 0 -13 14 8 1 0.1079062 0 -15 16 -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 4.000e+03, e = 4.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -4.000e+03, e = 4.000e+03, m = 9.383e-01. In 1: id = -2, x = 2.691e-02, pdf = 2.754e-01 at Q2 = 7.519e+03. In 2: id = 2, x = 7.693e-02, pdf = 5.689e-01 at same Q2. Subprocess f fbar -> W+ W- with code 233 is 2 -> 2. It has sHat = 1.325e+05, tHat = -1.507e+03, uHat = -1.171e+05, pTHat = 3.117e+01, m3Hat = 8.092e+01, m4Hat = 8.546e+01, thetaHat = 1.938e-01, phiHat = 1.501e-01. alphaEM = 7.815e-03, alphaS = 1.356e-01 at Q2 = 7.888e+03. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 8000.000 8000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 4000.000 4000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -4000.000 4000.000 0.938 3 -2 (ubar) -21 1 0 5 6 0 101 0.000 0.000 107.632 107.632 0.000 4 2 (u) -21 2 0 5 6 101 0 0.000 0.000 -307.734 307.734 0.000 5 -24 (W-) -22 3 4 7 8 0 0 30.817 4.660 81.766 119.184 80.918 6 24 (W+) -22 3 4 9 10 0 0 -30.817 -4.660 -281.867 296.183 85.461 7 3 s 23 5 0 0 0 102 0 -22.069 20.172 18.067 34.938 0.500 8 -4 cbar 23 5 0 0 0 0 102 52.886 -15.512 63.699 84.246 1.500 9 -3 sbar 23 6 0 0 0 0 103 25.512 0.448 -157.437 159.492 0.500 10 4 c 23 6 0 0 0 103 0 -56.330 -5.109 -124.430 136.690 1.500 Charge sum: -0.000 Momentum sum: -0.000 -0.000 -200.102 415.366 363.990 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | f fbar -> gamma*/Z0 gamma*/Z0 231 | 565 11 11 | 5.030e-09 8.097e-10 | | f fbar' -> Z0 W+- (no gamma*!) 232 | 807 22 22 | 1.295e-08 1.168e-09 | | f fbar -> W+ W- 233 | 816 67 67 | 3.613e-08 2.036e-09 | | | | | | sum | 2188 100 100 | 5.410e-08 2.483e-09 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 0 no errors or warnings to report | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* pythia8-8.1.80.orig/examples/outref/out150000644000175000017500000145112612217346173016373 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:04:49 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> b bbar 123 | 4.851e-04 | | q qbar -> b bbar 124 | 1.273e-05 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 57.54 mb | | | | pT0 = 3.08 gives sigmaInteraction = 270.61 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | HadronLevel:all | off | on | | HardQCD:gg2bbbar | on | off | | HardQCD:qqbar2bbbar | on | off | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:pTHatMin | 50.00000 | 0.0 0.0 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. In 1: id = 21, x = 1.786e-03, pdf = 2.497e+01 at Q2 = 2.975e+03. In 2: id = 21, x = 3.709e-02, pdf = 2.784e+00 at same Q2. Subprocess g g -> b bbar with code 123 is 2 -> 2. It has sHat = 1.299e+04, tHat = -8.347e+03, uHat = -4.593e+03, pTHat = 5.433e+01, m3Hat = 4.800e+00, m4Hat = 4.800e+00, thetaHat = 1.865e+00, phiHat = 4.259e+00. alphaEM = 7.772e-03, alphaS = 1.475e-01 at Q2 = 2.975e+03. Impact parameter b = 5.577e-01 gives enhancement factor = 2.133e+00. Max pT scale for MPI = 5.454e+01, ISR = 5.454e+01, FSR = 5.454e+01. Number of MPI = 11, ISR = 25, FSRproc = 148, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 21 (g) -21 1 0 5 6 101 102 0.000 0.000 12.504 12.504 0.000 4 21 (g) -21 2 0 5 6 103 101 0.000 0.000 -259.631 259.631 0.000 5 5 b 23 3 4 0 0 103 0 -23.822 -48.832 -162.906 171.794 4.800 6 -5 bbar 23 3 4 0 0 0 102 23.822 48.832 -84.221 100.341 4.800 Charge sum: 0.000 Momentum sum: 0.000 0.000 -247.126 272.135 113.956 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 689 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 690 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 21 (g) -21 7 0 5 6 101 102 0.000 0.000 12.504 12.504 0.000 4 21 (g) -21 8 8 5 6 103 101 0.000 0.000 -259.631 259.631 0.000 5 5 (b) -23 3 4 9 9 103 0 -23.822 -48.832 -162.906 171.794 4.800 6 -5 (bbar) -23 3 4 10 10 0 102 23.822 48.832 -84.221 100.341 4.800 7 21 (g) -41 19 19 11 3 101 104 -0.000 0.000 39.271 39.271 0.000 8 21 (g) -42 20 0 4 4 103 101 0.000 -0.000 -259.631 259.631 0.000 9 5 (b) -44 5 5 21 21 103 0 -21.502 -58.844 -197.178 206.948 4.800 10 -5 (bbar) -44 6 6 14 14 0 102 28.030 30.674 -40.521 58.237 4.800 11 21 (g) -43 7 0 12 13 102 104 -6.528 28.170 17.340 33.717 0.000 12 21 (g) -51 11 0 23 23 105 104 -4.289 35.160 13.248 37.817 0.000 13 21 (g) -51 11 0 24 24 102 105 1.490 -2.967 -1.312 3.570 0.000 14 -5 (bbar) -52 10 10 22 22 0 102 24.301 26.652 -35.117 50.568 4.800 15 21 (g) -31 30 30 17 18 106 107 0.000 0.000 2.089 2.089 0.000 16 21 (g) -31 31 0 17 18 108 109 0.000 0.000 -40.605 40.605 0.000 17 21 (g) -33 15 16 32 32 106 109 -5.271 2.348 -2.620 6.338 0.000 18 21 (g) -33 15 16 33 33 108 107 5.271 -2.348 -35.895 36.356 0.000 19 21 (g) -42 39 0 7 7 101 104 0.000 0.000 39.271 39.271 0.000 20 21 (g) -41 40 40 25 8 110 101 -0.000 -0.000 -2118.222 2118.222 0.000 21 5 (b) -44 9 9 41 41 103 0 -25.900 -59.396 -197.028 207.465 4.800 22 -5 (bbar) -44 14 14 42 42 0 102 23.369 26.535 -35.458 50.304 4.800 23 21 (g) -44 12 12 43 43 105 104 -4.556 35.126 13.213 37.805 0.000 24 21 (g) -44 13 13 44 44 102 105 1.437 -2.974 -1.327 3.559 0.000 25 21 (g) -43 20 0 45 45 110 103 5.651 0.710 -1858.352 1858.360 0.000 26 21 (g) -31 169 169 28 29 111 112 0.000 0.000 2.954 2.954 0.000 27 21 (g) -31 170 0 28 29 112 113 0.000 0.000 -108.527 108.527 0.000 28 21 (g) -33 26 27 50 51 111 114 -3.510 -3.184 0.966 4.836 0.000 29 21 (g) -33 26 27 52 52 114 113 3.510 3.184 -106.539 106.644 0.000 30 21 (g) -42 57 0 15 15 106 107 -0.000 0.000 2.089 2.089 0.000 31 21 (g) -41 58 58 34 16 108 115 0.000 -0.000 -436.847 436.847 0.000 32 21 (g) -44 17 17 59 59 106 109 -5.741 2.548 -2.735 6.851 0.000 33 21 (g) -44 18 18 60 60 108 107 1.483 -0.737 -38.639 38.674 0.000 34 21 (g) -43 31 0 61 61 109 115 4.258 -1.811 -393.385 393.412 0.000 35 21 (g) -31 140 140 37 38 116 117 0.000 0.000 8.016 8.016 0.000 36 21 (g) -31 117 117 37 38 118 119 0.000 0.000 -158.050 158.050 0.000 37 21 (g) -33 35 36 115 116 116 119 4.298 1.465 7.338 8.629 0.000 38 21 (g) -33 35 36 143 143 118 117 -4.298 -1.465 -157.371 157.437 0.000 39 21 (g) -41 111 111 46 19 120 104 0.000 0.000 126.873 126.873 0.000 40 21 (g) -42 220 220 20 20 110 101 -0.000 -0.000 -2118.222 2118.222 0.000 41 5 (b) -44 21 21 87 88 103 0 -26.048 -59.959 -200.592 211.030 4.800 42 -5 (bbar) -44 22 22 47 48 0 102 23.158 25.735 -33.717 48.564 4.800 43 21 (g) -44 23 23 109 110 105 104 -5.279 32.379 14.964 36.058 0.000 44 21 (g) -44 24 24 49 49 102 105 1.405 -3.094 -1.470 3.703 0.000 45 21 (g) -44 25 25 89 89 110 103 5.651 0.709 -1858.079 1858.088 0.000 46 21 (g) -43 39 0 218 219 120 101 1.112 4.230 87.544 87.653 0.000 47 -5 (bbar) -51 42 0 494 494 0 121 19.248 23.644 -26.875 40.925 4.800 48 21 (g) -51 42 0 270 270 121 102 4.207 1.437 -7.152 8.421 0.000 49 21 (g) -52 44 44 177 177 102 105 1.108 -2.441 -1.159 2.920 0.000 50 21 (g) -51 28 0 171 171 111 122 -5.861 -3.158 -2.235 7.023 0.000 51 21 (g) -51 28 0 173 173 122 114 2.545 0.149 -2.678 3.697 0.000 52 21 (g) -52 29 29 172 172 114 113 3.316 3.008 -100.660 100.760 0.000 53 21 (g) -31 135 0 55 56 124 123 0.000 0.000 11.539 11.539 0.000 54 21 (g) -31 136 136 55 56 126 125 0.000 0.000 -1.040 1.040 0.000 55 21 (g) -33 53 54 137 137 126 123 -2.560 2.042 7.299 8.000 0.000 56 21 (g) -33 53 54 138 138 124 125 2.560 -2.042 3.200 4.579 0.000 57 21 (g) -41 70 0 62 30 106 127 0.000 -0.000 10.503 10.503 0.000 58 21 (g) -42 71 71 31 31 108 115 0.000 0.000 -436.847 436.847 0.000 59 21 (g) -44 32 32 63 64 106 109 -2.561 2.039 0.768 3.363 0.000 60 21 (g) -44 33 33 73 73 108 107 1.511 -0.741 -39.741 39.777 0.000 61 21 (g) -44 34 34 65 65 109 115 4.279 -1.814 -395.460 395.487 0.000 62 21 (g) -43 57 0 75 75 107 127 -3.228 0.516 8.088 8.724 0.000 63 21 (g) -51 59 0 72 72 106 128 -0.863 0.694 1.866 2.170 0.000 64 21 (g) -51 59 0 76 76 128 109 -1.494 1.259 -19.895 19.991 0.000 65 21 (g) -52 61 61 74 74 109 115 4.075 -1.728 -376.662 376.688 0.000 66 21 (g) -31 100 100 68 69 130 129 0.000 0.000 147.656 147.656 0.000 67 21 (g) -31 101 0 68 69 129 131 0.000 0.000 -0.074 0.074 0.000 68 21 (g) -33 66 67 102 102 132 131 0.140 2.977 41.847 41.953 0.000 69 21 (g) -33 66 67 103 103 130 132 -0.140 -2.977 105.735 105.777 0.000 70 21 (g) -41 121 0 77 57 133 127 -0.000 0.000 44.612 44.612 0.000 71 21 (g) -42 122 122 58 58 108 115 0.000 -0.000 -436.847 436.847 0.000 72 21 (g) -44 63 63 123 123 106 128 -1.429 0.757 1.696 2.343 0.000 73 21 (g) -44 60 60 112 113 108 107 1.506 -0.741 -39.493 39.529 0.000 74 21 (g) -44 65 65 125 125 109 115 4.072 -1.728 -375.829 375.855 0.000 75 21 (g) -44 62 62 114 114 107 127 -5.586 0.777 7.466 9.357 0.000 76 21 (g) -44 64 64 127 127 128 109 -1.508 1.260 -20.113 20.208 0.000 77 21 (g) -43 70 0 128 128 133 106 2.946 -0.325 34.038 34.167 0.000 78 21 (g) -31 82 0 80 81 135 134 0.000 0.000 620.787 620.787 0.000 79 21 (g) -31 83 83 80 81 137 136 0.000 0.000 -0.212 0.212 0.000 80 21 (g) -33 78 79 84 84 137 134 -2.748 -0.995 10.037 10.453 0.000 81 21 (g) -33 78 79 85 85 135 136 2.748 0.995 610.539 610.546 0.000 82 2 (u) -41 90 90 86 78 135 0 -0.000 -0.000 1009.161 1009.161 0.000 83 21 (g) -42 91 0 79 79 137 136 0.000 0.000 -0.212 0.212 0.000 84 21 (g) -44 80 80 92 92 137 134 -2.769 -1.033 10.414 10.826 0.000 85 21 (g) -44 81 81 93 93 135 136 1.497 -1.267 632.886 632.889 0.000 86 2 (u) -43 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101.463 101.467 0.000 775 21 (g) -61 1 0 636 636 123 112 0.339 0.653 3.626 3.700 0.000 776 21 (g) -61 2 0 272 272 115 250 -0.283 -2.951 -178.984 179.009 0.000 777 21 g 62 509 509 0 0 111 270 -3.064 -1.803 -0.638 3.612 0.000 778 21 g 62 274 274 0 0 114 231 1.536 1.312 -92.513 92.535 0.000 779 21 g 62 516 516 0 0 264 167 1.150 -0.070 -2.636 2.877 0.000 780 21 g 62 631 631 0 0 115 309 0.552 -0.353 -37.555 37.561 0.000 781 3 s 62 277 277 0 0 167 0 -0.398 0.163 -0.950 1.157 0.500 782 -3 sbar 62 278 278 0 0 0 145 0.731 1.074 -5.700 5.867 0.500 783 21 g 62 589 589 0 0 191 117 -0.558 0.027 -0.387 0.680 0.000 784 21 g 62 613 613 0 0 301 142 0.447 -0.686 -1.074 1.351 0.000 785 21 g 62 434 434 0 0 211 111 -0.398 -0.371 0.167 0.569 0.000 786 21 g 62 591 591 0 0 237 199 -0.524 -0.135 -0.069 0.545 0.000 787 21 g 62 615 615 0 0 261 319 -0.127 0.119 -0.569 0.595 0.000 788 21 g 62 508 508 0 0 122 320 0.050 -0.600 -0.406 0.726 0.000 789 21 g 62 517 517 0 0 209 262 -0.120 -0.235 -0.629 0.682 0.000 790 21 g 62 590 590 0 0 289 237 -0.663 0.009 0.462 0.808 0.000 791 21 g 62 614 614 0 0 252 197 0.505 0.163 -0.442 0.691 0.000 792 21 g 62 634 634 0 0 309 160 0.978 -0.627 -19.973 20.006 0.000 793 21 g 62 635 635 0 0 310 118 -0.043 -0.284 -12.444 12.447 0.000 794 21 (g) -61 1 0 546 546 151 151 3.299 1.241 9.346 9.988 0.000 795 21 (g) -61 2 0 660 660 227 227 -1.907 0.707 -317.312 317.319 0.000 796 21 g 62 619 619 0 0 304 179 1.650 0.921 0.550 1.968 0.000 797 21 g 62 549 549 0 0 184 304 -1.164 -0.478 -18.945 18.987 0.000 798 21 g 62 598 598 0 0 147 122 0.163 -0.990 -0.215 1.026 0.000 799 21 g 62 658 658 0 0 119 258 -0.653 -0.642 -1.847 2.061 0.000 800 21 g 62 552 552 0 0 160 310 -0.002 -0.038 -0.956 0.957 0.000 801 21 g 62 553 553 0 0 179 116 0.207 0.204 0.138 0.321 0.000 802 21 g 62 554 554 0 0 118 246 -0.275 0.035 -15.338 15.340 0.000 803 -1 dbar 62 555 555 0 0 0 184 -0.742 -0.306 -9.771 9.810 0.330 804 21 g 62 609 609 0 0 231 189 0.116 0.455 -27.301 27.305 0.000 805 21 g 62 557 557 0 0 195 188 -1.231 -0.045 -40.938 40.957 0.000 806 1 d 62 558 558 0 0 188 0 -0.503 -0.738 -39.507 39.518 0.330 807 21 g 62 559 559 0 0 200 233 -0.117 0.349 -16.835 16.839 0.000 808 21 g 62 621 621 0 0 116 276 2.539 2.146 1.856 3.807 0.000 809 21 g 62 561 561 0 0 246 195 -1.551 -0.057 -59.736 59.756 0.000 810 21 g 62 562 562 0 0 117 289 -0.415 0.141 0.272 0.516 0.000 811 21 g 62 607 607 0 0 189 176 0.289 0.495 -47.632 47.635 0.000 812 21 g 62 564 564 0 0 225 131 -0.079 0.288 -5.383 5.391 0.000 813 21 g 62 565 565 0 0 267 158 1.360 -0.935 1.513 2.239 0.000 814 21 g 62 566 566 0 0 274 114 0.154 0.025 -7.086 7.088 0.000 815 21 g 62 567 567 0 0 276 223 0.539 0.439 0.618 0.930 0.000 816 21 g 62 599 599 0 0 293 288 0.107 0.069 0.214 0.249 0.000 817 21 g 62 608 608 0 0 298 250 -0.195 -0.253 -22.207 22.209 0.000 818 21 g 62 620 620 0 0 223 284 1.158 0.587 1.161 1.742 0.000 819 21 g 62 659 659 0 0 319 252 0.038 0.276 -0.592 0.654 0.000 820 -1 (dbar) -61 1 0 135 135 0 123 0.000 -1.440 733.311 733.313 0.000 821 21 (g) -61 2 0 360 360 123 149 0.872 4.003 2.737 4.927 0.000 822 21 g 62 358 358 0 0 123 124 0.082 1.419 5.089 5.284 0.000 823 21 g 62 594 594 0 0 152 112 0.740 0.781 6.998 7.081 0.000 824 -1 dbar 62 583 583 0 0 0 149 -1.368 -2.913 683.574 683.582 0.330 825 21 g 62 646 646 0 0 220 267 1.822 -1.330 5.829 6.250 0.000 826 21 g 62 580 580 0 0 284 278 0.756 0.103 0.612 0.978 0.000 827 21 g 62 592 592 0 0 175 308 -0.413 -0.029 1.716 1.765 0.000 828 21 g 62 359 359 0 0 126 137 -1.537 3.174 9.016 9.681 0.000 829 21 g 62 368 368 0 0 168 290 0.078 0.286 0.602 0.671 0.000 830 21 g 62 648 648 0 0 234 301 0.046 -0.028 -0.023 0.059 0.000 831 21 g 62 585 585 0 0 124 240 0.179 0.579 1.521 1.638 0.000 832 21 g 62 584 584 0 0 285 314 0.251 0.083 19.484 19.486 0.000 833 21 g 62 593 593 0 0 290 143 0.189 0.412 0.698 0.833 0.000 834 21 g 62 647 647 0 0 314 241 0.047 0.025 0.932 0.933 0.000 835 21 (g) -61 1 0 679 679 324 324 1.181 0.629 147.792 147.798 0.000 836 21 (g) -61 2 0 680 680 129 129 -0.269 0.152 -9.839 9.844 0.000 837 3 s 62 681 681 0 0 132 0 0.961 3.903 73.410 73.522 0.500 838 1 d 62 682 682 0 0 130 0 0.444 -0.757 30.685 30.700 0.330 839 21 g 62 683 683 0 0 142 248 0.084 -0.602 -0.857 1.051 0.000 840 -3 sbar 62 684 684 0 0 0 144 -0.252 0.852 10.710 10.759 0.500 841 21 g 62 685 685 0 0 270 147 -0.165 -1.094 -0.349 1.160 0.000 842 -1 dbar 62 686 686 0 0 0 208 -0.107 -1.252 32.309 32.335 0.330 843 21 g 62 687 687 0 0 248 209 -0.063 -0.607 -1.136 1.289 0.000 844 21 g 62 688 688 0 0 131 274 0.009 0.338 -6.819 6.827 0.000 845 2 (u) -61 1 0 90 90 112 0 -4.448 -0.211 1008.258 1008.268 0.000 846 -2 (ubar) -61 2 0 91 91 0 112 1.623 -2.951 3.569 4.907 0.000 847 21 g 62 515 515 0 0 203 201 0.243 -1.724 8.414 8.592 0.000 848 21 g 62 93 93 0 0 135 153 -1.318 -1.423 641.025 641.028 0.000 849 2 u 62 154 154 0 0 155 0 1.423 1.919 208.088 208.102 0.330 850 -2 ubar 62 316 316 0 0 0 155 -0.182 0.175 -0.297 0.511 0.330 851 21 g 62 477 477 0 0 253 224 -2.226 0.150 118.273 118.294 0.000 852 21 g 62 479 479 0 0 241 203 0.722 -0.006 10.013 10.039 0.000 853 21 g 62 446 446 0 0 193 239 -0.632 -0.620 3.441 3.554 0.000 854 21 g 62 322 322 0 0 137 303 -0.117 0.096 0.633 0.651 0.000 855 21 g 62 513 513 0 0 201 220 0.238 -0.870 3.388 3.506 0.000 856 21 g 62 445 445 0 0 134 132 -0.362 -0.240 5.928 5.944 0.000 857 21 g 62 478 478 0 0 180 139 -0.222 -0.310 8.108 8.117 0.000 858 21 g 62 514 514 0 0 263 134 -0.395 -0.310 4.811 4.837 0.000 859 21 (g) -61 1 0 301 301 156 156 0.315 1.243 288.766 288.769 0.000 860 21 (g) -61 2 0 302 302 141 141 -0.613 3.307 -187.958 187.989 0.000 861 21 g 62 346 346 0 0 210 285 -0.257 0.474 147.304 147.305 0.000 862 4 c 62 573 573 0 0 140 0 1.830 2.389 22.518 22.767 1.500 863 -4 cbar 62 305 305 0 0 0 312 1.018 -0.953 -0.360 2.079 1.500 864 21 g 62 420 420 0 0 176 200 -0.933 2.910 -140.299 140.332 0.000 865 21 g 62 571 571 0 0 199 211 -0.386 -0.381 0.344 0.643 0.000 866 21 g 62 471 471 0 0 207 298 -0.211 0.156 -5.973 5.979 0.000 867 21 g 62 437 437 0 0 224 238 -0.243 -0.288 26.149 26.152 0.000 868 21 g 62 512 512 0 0 139 253 -0.482 0.100 14.154 14.162 0.000 869 21 g 62 421 421 0 0 233 207 -0.800 1.004 -37.189 37.212 0.000 870 21 g 62 436 436 0 0 238 135 -0.367 -0.292 76.340 76.341 0.000 871 21 g 62 630 630 0 0 251 264 0.368 -0.368 -2.049 2.114 0.000 872 21 g 62 628 628 0 0 308 193 -0.053 -0.026 0.272 0.278 0.000 873 21 g 62 572 572 0 0 278 293 0.437 0.034 0.363 0.569 0.000 874 21 g 62 629 629 0 0 262 119 -0.219 -0.210 -0.765 0.823 0.000 875 21 (g) -61 1 0 667 667 260 250 -1.442 0.101 874.855 874.856 0.000 876 1 (d) -61 2 0 668 668 250 0 -1.237 -0.832 -25.369 25.412 0.000 877 4 c 62 669 669 0 0 144 0 0.978 -2.747 34.477 34.632 1.500 878 21 g 62 670 670 0 0 143 157 -0.568 0.897 1.696 2.001 0.000 879 -4 cbar 62 671 671 0 0 0 259 -0.812 0.987 118.688 118.704 1.500 880 1 d 62 672 672 0 0 260 0 -0.342 -0.138 -18.583 18.590 0.330 881 21 g 62 673 673 0 0 249 279 -0.096 0.183 -0.104 0.231 0.000 882 21 g 62 674 674 0 0 239 263 -0.139 -0.103 0.334 0.376 0.000 883 21 g 62 675 675 0 0 311 261 -0.799 0.257 -4.492 4.570 0.000 884 21 g 62 676 676 0 0 145 225 0.197 0.165 -1.832 1.850 0.000 885 21 g 62 677 677 0 0 312 152 0.131 0.032 0.886 0.896 0.000 886 21 g 62 678 678 0 0 153 210 -1.229 -0.264 718.416 718.418 0.000 887 21 (g) -61 1 0 338 338 250 159 0.044 -0.759 98.896 98.899 0.000 888 2 (u) -61 2 0 339 339 159 0 -0.994 -0.924 -2.693 3.016 0.000 889 21 g 62 340 340 0 0 157 126 -1.665 1.562 4.696 5.222 0.000 890 2 u 62 468 468 0 0 250 0 0.607 -0.630 -0.797 1.229 0.330 891 21 g 62 501 501 0 0 208 180 -0.159 -0.891 27.608 27.622 0.000 892 21 g 62 622 622 0 0 305 130 0.315 -0.325 23.589 23.593 0.000 893 21 g 62 661 661 0 0 320 174 -0.267 -1.361 -1.068 1.751 0.000 894 21 g 62 624 624 0 0 259 305 0.123 -0.445 39.705 39.708 0.000 895 21 g 62 663 663 0 0 303 175 -0.355 -0.004 1.029 1.089 0.000 896 21 g 62 617 617 0 0 288 140 0.407 0.166 1.258 1.333 0.000 897 21 g 62 623 623 0 0 240 168 0.035 0.070 0.177 0.193 0.000 898 21 g 62 662 662 0 0 158 249 0.008 0.175 0.006 0.175 0.000 899 -2 (ubar) -61 1 0 202 202 0 149 1.357 -0.369 0.408 1.464 0.000 900 21 (g) -61 2 0 203 203 149 173 -0.024 -2.490 -17.901 18.073 0.000 901 -2 ubar 62 292 292 0 0 0 173 2.259 -0.727 -1.824 3.011 0.330 902 21 g 62 498 498 0 0 258 251 -0.758 -2.406 -13.663 13.894 0.000 903 21 g 62 574 574 0 0 197 234 0.502 0.113 -0.234 0.565 0.000 904 21 g 62 576 576 0 0 174 311 -0.287 0.012 -1.593 1.619 0.000 905 21 g 62 575 575 0 0 279 191 -0.382 0.150 -0.179 0.448 0.000 906 2101 ud_0 63 1 0 0 0 0 260 0.118 -0.582 2607.221 2607.221 0.579 907 1 d 63 1 0 0 0 104 0 -0.465 -0.868 155.761 155.765 0.330 908 2 u 63 1 0 0 0 159 0 0.537 -0.098 388.118 388.119 0.330 909 2101 ud_0 63 2 0 0 0 0 123 1.213 -0.132 -2020.435 2020.435 0.579 910 2 u 63 2 0 0 0 173 0 0.755 -0.789 -1532.390 1532.390 0.330 911 -1 dbar 63 2 0 0 0 0 159 0.524 -0.346 -34.610 34.618 0.330 Charge sum: 2.000 Momentum sum: 0.000 -0.000 0.000 14000.000 14000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 689 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 690 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 21 (g) -21 7 0 5 6 101 102 0.000 0.000 12.504 12.504 0.000 4 21 (g) -21 8 8 5 6 103 101 0.000 0.000 -259.631 259.631 0.000 5 5 (b) -23 3 4 9 9 103 0 -23.822 -48.832 -162.906 171.794 4.800 6 -5 (bbar) -23 3 4 10 10 0 102 23.822 48.832 -84.221 100.341 4.800 7 21 (g) -41 19 19 11 3 101 104 -0.000 0.000 39.271 39.271 0.000 8 21 (g) -42 20 0 4 4 103 101 0.000 -0.000 -259.631 259.631 0.000 9 5 (b) -44 5 5 21 21 103 0 -21.502 -58.844 -197.178 206.948 4.800 10 -5 (bbar) -44 6 6 14 14 0 102 28.030 30.674 -40.521 58.237 4.800 11 21 (g) -43 7 0 12 13 102 104 -6.528 28.170 17.340 33.717 0.000 12 21 (g) -51 11 0 23 23 105 104 -4.289 35.160 13.248 37.817 0.000 13 21 (g) -51 11 0 24 24 102 105 1.490 -2.967 -1.312 3.570 0.000 14 -5 (bbar) -52 10 10 22 22 0 102 24.301 26.652 -35.117 50.568 4.800 15 21 (g) -31 30 30 17 18 106 107 0.000 0.000 2.089 2.089 0.000 16 21 (g) -31 31 0 17 18 108 109 0.000 0.000 -40.605 40.605 0.000 17 21 (g) -33 15 16 32 32 106 109 -5.271 2.348 -2.620 6.338 0.000 18 21 (g) -33 15 16 33 33 108 107 5.271 -2.348 -35.895 36.356 0.000 19 21 (g) -42 39 0 7 7 101 104 0.000 0.000 39.271 39.271 0.000 20 21 (g) -41 40 40 25 8 110 101 -0.000 -0.000 -2118.222 2118.222 0.000 21 5 (b) -44 9 9 41 41 103 0 -25.900 -59.396 -197.028 207.465 4.800 22 -5 (bbar) -44 14 14 42 42 0 102 23.369 26.535 -35.458 50.304 4.800 23 21 (g) -44 12 12 43 43 105 104 -4.556 35.126 13.213 37.805 0.000 24 21 (g) -44 13 13 44 44 102 105 1.437 -2.974 -1.327 3.559 0.000 25 21 (g) -43 20 0 45 45 110 103 5.651 0.710 -1858.352 1858.360 0.000 26 21 (g) -31 169 169 28 29 111 112 0.000 0.000 2.954 2.954 0.000 27 21 (g) -31 170 0 28 29 112 113 0.000 0.000 -108.527 108.527 0.000 28 21 (g) -33 26 27 50 51 111 114 -3.510 -3.184 0.966 4.836 0.000 29 21 (g) -33 26 27 52 52 114 113 3.510 3.184 -106.539 106.644 0.000 30 21 (g) -42 57 0 15 15 106 107 -0.000 0.000 2.089 2.089 0.000 31 21 (g) -41 58 58 34 16 108 115 0.000 -0.000 -436.847 436.847 0.000 32 21 (g) -44 17 17 59 59 106 109 -5.741 2.548 -2.735 6.851 0.000 33 21 (g) -44 18 18 60 60 108 107 1.483 -0.737 -38.639 38.674 0.000 34 21 (g) -43 31 0 61 61 109 115 4.258 -1.811 -393.385 393.412 0.000 35 21 (g) -31 140 140 37 38 116 117 0.000 0.000 8.016 8.016 0.000 36 21 (g) -31 117 117 37 38 118 119 0.000 0.000 -158.050 158.050 0.000 37 21 (g) -33 35 36 115 116 116 119 4.298 1.465 7.338 8.629 0.000 38 21 (g) -33 35 36 143 143 118 117 -4.298 -1.465 -157.371 157.437 0.000 39 21 (g) -41 111 111 46 19 120 104 0.000 0.000 126.873 126.873 0.000 40 21 (g) -42 220 220 20 20 110 101 -0.000 -0.000 -2118.222 2118.222 0.000 41 5 (b) -44 21 21 87 88 103 0 -26.048 -59.959 -200.592 211.030 4.800 42 -5 (bbar) -44 22 22 47 48 0 102 23.158 25.735 -33.717 48.564 4.800 43 21 (g) -44 23 23 109 110 105 104 -5.279 32.379 14.964 36.058 0.000 44 21 (g) -44 24 24 49 49 102 105 1.405 -3.094 -1.470 3.703 0.000 45 21 (g) -44 25 25 89 89 110 103 5.651 0.709 -1858.079 1858.088 0.000 46 21 (g) -43 39 0 218 219 120 101 1.112 4.230 87.544 87.653 0.000 47 -5 (bbar) -51 42 0 494 494 0 121 19.248 23.644 -26.875 40.925 4.800 48 21 (g) -51 42 0 270 270 121 102 4.207 1.437 -7.152 8.421 0.000 49 21 (g) -52 44 44 177 177 102 105 1.108 -2.441 -1.159 2.920 0.000 50 21 (g) -51 28 0 171 171 111 122 -5.861 -3.158 -2.235 7.023 0.000 51 21 (g) -51 28 0 173 173 122 114 2.545 0.149 -2.678 3.697 0.000 52 21 (g) -52 29 29 172 172 114 113 3.316 3.008 -100.660 100.760 0.000 53 21 (g) -31 135 0 55 56 124 123 0.000 0.000 11.539 11.539 0.000 54 21 (g) -31 136 136 55 56 126 125 0.000 0.000 -1.040 1.040 0.000 55 21 (g) -33 53 54 137 137 126 123 -2.560 2.042 7.299 8.000 0.000 56 21 (g) -33 53 54 138 138 124 125 2.560 -2.042 3.200 4.579 0.000 57 21 (g) -41 70 0 62 30 106 127 0.000 -0.000 10.503 10.503 0.000 58 21 (g) -42 71 71 31 31 108 115 0.000 0.000 -436.847 436.847 0.000 59 21 (g) -44 32 32 63 64 106 109 -2.561 2.039 0.768 3.363 0.000 60 21 (g) -44 33 33 73 73 108 107 1.511 -0.741 -39.741 39.777 0.000 61 21 (g) -44 34 34 65 65 109 115 4.279 -1.814 -395.460 395.487 0.000 62 21 (g) -43 57 0 75 75 107 127 -3.228 0.516 8.088 8.724 0.000 63 21 (g) -51 59 0 72 72 106 128 -0.863 0.694 1.866 2.170 0.000 64 21 (g) -51 59 0 76 76 128 109 -1.494 1.259 -19.895 19.991 0.000 65 21 (g) -52 61 61 74 74 109 115 4.075 -1.728 -376.662 376.688 0.000 66 21 (g) -31 100 100 68 69 130 129 0.000 0.000 147.656 147.656 0.000 67 21 (g) -31 101 0 68 69 129 131 0.000 0.000 -0.074 0.074 0.000 68 21 (g) -33 66 67 102 102 132 131 0.140 2.977 41.847 41.953 0.000 69 21 (g) -33 66 67 103 103 130 132 -0.140 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80 92 92 137 134 -2.769 -1.033 10.414 10.826 0.000 85 21 (g) -44 81 81 93 93 135 136 1.497 -1.267 632.886 632.889 0.000 86 2 (u) -43 82 0 94 94 134 0 1.272 2.300 365.648 365.658 0.330 87 5 (b) -51 41 0 183 183 138 0 -21.777 -55.057 -178.043 187.691 4.800 88 21 (g) -51 41 0 132 133 103 138 -4.260 -4.900 -26.278 27.068 0.000 89 21 (g) -52 45 45 134 134 110 103 5.640 0.708 -1854.350 1854.358 0.000 90 2 (u) -42 845 845 82 82 135 0 0.000 -0.000 1009.161 1009.161 0.000 91 -2 (ubar) -41 846 846 95 83 0 136 -0.000 0.000 -0.672 0.672 0.000 92 21 (g) -44 84 84 156 156 137 134 -1.485 -3.178 14.590 15.006 0.000 93 21 (g) -44 85 85 848 848 135 136 1.506 -1.283 636.929 636.932 0.000 94 2 (u) -44 86 86 154 155 134 0 1.302 2.250 353.739 353.749 0.330 95 -2 (ubar) -43 91 0 316 316 0 137 -1.323 2.211 3.231 4.146 0.330 96 21 (g) -31 157 157 98 99 140 141 0.000 0.000 288.194 288.194 0.000 97 4 (c) -31 158 0 98 99 139 0 0.000 0.000 -0.124 0.124 0.000 98 21 (g) -33 96 97 159 159 139 141 -1.668 -1.571 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-0.021 0.745 9.780 9.821 0.498 976 1 (d) -71 956 956 978 980 259 0 0.882 -1.527 93.979 94.001 0.950 977 -4 (cbar) -71 879 879 978 980 0 259 -0.812 0.987 118.688 118.704 1.500 978 -211 pi- 83 976 977 0 0 0 0 -0.008 -1.207 73.375 73.385 0.140 979 111 (pi0) -84 976 977 1596 1597 0 0 0.341 0.654 36.044 36.052 0.135 980 -423 (D*bar0) -84 976 977 1598 1599 0 0 -0.264 0.013 103.248 103.268 2.007 981 1 (d) -71 720 720 983 985 121 0 3.109 0.922 -5.058 6.017 0.330 982 -5 (bbar) -71 692 692 983 985 0 121 18.271 22.469 -25.510 38.891 4.800 983 -211 pi- 83 981 982 0 0 0 0 2.507 0.515 -3.558 4.386 0.140 984 211 pi+ 84 981 982 0 0 0 0 1.875 2.540 -3.217 4.509 0.140 985 513 (B*0) -84 981 982 1600 1601 0 0 16.998 20.337 -23.793 36.013 5.325 986 1 (d) -71 914 914 992 1000 296 0 0.075 2.072 1.616 2.678 0.513 987 21 (g) -71 916 916 992 1000 105 296 -0.022 0.597 -0.154 0.789 0.492 988 21 (g) -71 707 707 992 1000 192 105 0.948 -1.038 -0.697 1.569 0.000 989 21 (g) -71 694 694 992 1000 243 192 0.624 0.572 -0.622 1.050 0.000 990 21 (g) -71 915 915 992 1000 102 243 -0.366 -0.273 -0.345 0.628 0.259 991 -1 (dbar) -71 697 697 992 1000 0 102 1.197 1.421 -1.950 2.714 0.330 992 111 (pi0) -83 986 991 1602 1603 0 0 -0.081 0.546 0.519 0.770 0.135 993 111 (pi0) -83 986 991 1604 1605 0 0 0.179 0.882 0.207 0.933 0.135 994 111 (pi0) -83 986 991 1606 1607 0 0 0.103 0.195 0.340 0.427 0.135 995 -213 (rho-) -83 986 991 1392 1393 0 0 -0.041 0.413 0.590 1.107 0.839 996 213 (rho+) -83 986 991 1394 1395 0 0 0.262 0.437 -0.425 1.010 0.762 997 223 (omega) -84 986 991 1608 1610 0 0 0.119 -0.184 -0.752 1.084 0.749 998 111 (pi0) -84 986 991 1611 1612 0 0 0.978 -0.285 -0.881 1.354 0.135 999 -213 (rho-) -84 986 991 1396 1397 0 0 0.438 0.961 -1.261 1.933 1.015 1000 211 pi+ 84 986 991 0 0 0 0 0.500 0.386 -0.489 0.811 0.140 1001 2 (u) -71 693 693 1005 1012 256 0 -2.888 12.984 6.648 14.874 0.330 1002 21 (g) -71 727 727 1005 1012 315 256 0.254 1.119 0.580 1.286 0.000 1003 21 (g) -71 913 913 1005 1012 162 315 -1.583 7.047 3.595 8.079 0.425 1004 -1 (dbar) -71 708 708 1005 1012 0 162 -1.491 -0.736 -0.335 1.728 0.330 1005 211 pi+ 83 1001 1004 0 0 0 0 -1.809 9.565 4.653 10.791 0.140 1006 311 (K0) -83 1001 1004 1398 1398 0 0 -0.784 2.314 1.170 2.754 0.498 1007 -311 (Kbar0) -83 1001 1004 1399 1399 0 0 0.092 1.143 0.962 1.578 0.498 1008 -211 pi- 83 1001 1004 0 0 0 0 -1.142 5.663 2.506 6.299 0.140 1009 2212 p+ 84 1001 1004 0 0 0 0 -0.495 1.109 0.911 1.784 0.938 1010 -2112 nbar0 84 1001 1004 0 0 0 0 -0.516 0.188 0.129 1.096 0.940 1011 -211 pi- 84 1001 1004 0 0 0 0 -1.218 0.605 0.215 1.384 0.140 1012 211 pi+ 84 1001 1004 0 0 0 0 0.163 -0.173 -0.057 0.282 0.140 1013 111 (pi0) -83 849 850 1613 1614 0 0 0.595 0.788 79.069 79.075 0.135 1014 113 (rho0) -83 849 850 1400 1401 0 0 0.537 1.064 112.688 112.696 0.654 1015 211 pi+ 83 849 850 0 0 0 0 0.518 0.126 13.973 13.984 0.140 1016 311 (K0) -84 849 850 1402 1402 0 0 -0.276 0.157 1.732 1.830 0.498 1017 -323 (K*-) -84 849 850 1403 1404 0 0 -0.132 -0.040 0.329 1.027 0.963 1018 2 (u) -71 890 890 1026 1037 250 0 0.607 -0.630 -0.797 1.229 0.330 1019 21 (g) -71 817 817 1026 1037 298 250 -0.195 -0.253 -22.207 22.209 0.000 1020 21 (g) -71 965 965 1026 1037 233 298 -1.012 1.161 -43.163 43.191 0.207 1021 21 (g) -71 962 962 1026 1037 176 233 -1.050 3.258 -157.134 157.172 0.015 1022 21 (g) -71 966 966 1026 1037 231 176 0.405 0.950 -74.933 74.941 0.235 1023 21 (g) -71 967 967 1026 1037 274 231 1.690 1.337 -99.599 99.623 0.303 1024 21 (g) -71 963 963 1026 1037 225 274 -0.070 0.626 -12.202 12.218 0.100 1025 -3 (sbar) -71 964 964 1026 1037 0 225 0.927 1.239 -7.532 7.717 0.657 1026 113 (rho0) -83 1018 1025 1405 1406 0 0 0.382 -0.532 -2.453 2.667 0.814 1027 211 pi+ 83 1018 1025 0 0 0 0 -0.530 0.485 -7.876 7.910 0.140 1028 111 (pi0) -83 1018 1025 1615 1616 0 0 0.614 -0.632 -2.044 2.230 0.135 1029 223 (omega) -83 1018 1025 1617 1619 0 0 -0.611 0.655 -37.582 37.601 0.781 1030 -211 pi- 83 1018 1025 0 0 0 0 -0.401 1.261 -78.147 78.159 0.140 1031 111 (pi0) -83 1018 1025 1620 1621 0 0 -0.784 2.145 -102.919 102.945 0.135 1032 211 pi+ 84 1018 1025 0 0 0 0 1.281 0.797 -66.261 66.279 0.140 1033 -211 pi- 84 1018 1025 0 0 0 0 -0.347 0.606 -21.290 21.302 0.140 1034 213 (rho+) -84 1018 1025 1407 1408 0 0 0.848 1.317 -76.875 76.905 1.492 1035 -211 pi- 84 1018 1025 0 0 0 0 -0.154 0.255 -4.881 4.893 0.140 1036 113 (rho0) -84 1018 1025 1409 1410 0 0 0.874 0.623 -8.403 8.502 0.720 1037 323 (K*+) -84 1018 1025 1411 1412 0 0 0.131 0.709 -8.834 8.908 0.889 1038 1 (d) -71 907 907 1040 1047 104 0 -0.465 -0.868 155.761 155.765 0.330 1039 -2 (ubar) -71 699 699 1040 1047 0 104 0.493 7.716 2.864 8.252 0.330 1040 331 (eta') -83 1038 1039 1622 1624 0 0 -0.263 -1.081 105.810 105.820 0.958 1041 223 (omega) -83 1038 1039 1625 1627 0 0 -0.134 0.665 25.757 25.778 0.787 1042 -213 (rho-) -83 1038 1039 1413 1414 0 0 0.213 -0.176 17.983 18.004 0.826 1043 211 pi+ 83 1038 1039 0 0 0 0 -0.621 -0.016 3.096 3.161 0.140 1044 111 (pi0) -83 1038 1039 1628 1629 0 0 0.263 0.378 1.021 1.128 0.135 1045 -213 (rho-) -83 1038 1039 1415 1416 0 0 0.161 0.177 2.317 2.490 0.878 1046 211 pi+ 83 1038 1039 0 0 0 0 0.165 0.010 0.020 0.217 0.140 1047 -213 (rho-) -84 1038 1039 1417 1418 0 0 0.244 6.891 2.621 7.419 0.791 1048 2 (u) -71 910 910 1050 1060 173 0 0.755 -0.789 -1532.390 1532.390 0.330 1049 -2 (ubar) -71 901 901 1050 1060 0 173 2.259 -0.727 -1.824 3.011 0.330 1050 321 K+ 83 1048 1049 0 0 0 0 -0.159 -0.294 -604.775 604.776 0.494 1051 -313 (K*bar0) -83 1048 1049 1419 1420 0 0 0.363 -0.213 -357.605 357.606 0.873 1052 111 (pi0) -83 1048 1049 1630 1631 0 0 0.156 -0.032 -58.261 58.262 0.135 1053 223 (omega) -83 1048 1049 1632 1634 0 0 0.515 -0.164 -465.649 465.650 0.784 1054 113 (rho0) -83 1048 1049 1421 1422 0 0 -0.306 -0.150 -21.958 21.975 0.804 1055 311 (K0) -83 1048 1049 1423 1423 0 0 0.179 -0.160 -3.999 4.037 0.498 1056 333 (phi) -83 1048 1049 1635 1636 0 0 0.067 -0.070 -13.408 13.447 1.021 1057 -321 K- 84 1048 1049 0 0 0 0 0.867 0.717 -3.595 3.799 0.494 1058 221 (eta) -84 1048 1049 1637 1639 0 0 0.067 -0.901 -1.418 1.768 0.548 1059 111 (pi0) -84 1048 1049 1640 1641 0 0 0.560 0.429 -2.283 2.393 0.135 1060 221 (eta) -84 1048 1049 1642 1643 0 0 0.705 -0.677 -1.263 1.688 0.548 1061 4 (c) -71 862 862 1068 1076 140 0 1.830 2.389 22.518 22.767 1.500 1062 21 (g) -71 959 959 1068 1076 293 140 0.514 0.236 1.473 1.582 0.123 1063 21 (g) -71 957 957 1068 1076 284 293 1.192 0.137 0.975 1.547 0.035 1064 21 (g) -71 960 960 1068 1076 276 284 1.698 1.025 1.779 2.672 0.203 1065 21 (g) -71 958 958 1068 1076 179 276 2.745 2.350 1.995 4.129 0.103 1066 21 (g) -71 796 796 1068 1076 304 179 1.650 0.921 0.550 1.968 0.000 1067 -1 (dbar) -71 961 961 1068 1076 0 304 -1.906 -0.784 -28.716 28.797 0.605 1068 421 (D0) -83 1061 1067 1644 1645 0 0 1.376 1.148 11.066 11.364 1.865 1069 213 (rho+) -83 1061 1067 1424 1425 0 0 0.863 0.776 11.609 11.733 1.245 1070 113 (rho0) -83 1061 1067 1426 1427 0 0 3.178 2.514 4.255 5.928 0.782 1071 113 (rho0) -83 1061 1067 1428 1429 0 0 2.910 1.387 1.308 3.671 1.173 1072 2114 (Delta0) -83 1061 1067 1430 1431 0 0 1.027 1.110 0.471 2.051 1.304 1073 213 (rho+) -84 1061 1067 1432 1433 0 0 0.062 -0.279 -0.718 0.983 0.608 1074 -2224 (Deltabar--) -84 1061 1067 1434 1435 0 0 -0.379 0.296 -8.616 8.735 1.360 1075 211 pi+ 84 1061 1067 0 0 0 0 -0.521 0.331 -1.483 1.613 0.140 1076 223 (omega) -84 1061 1067 1646 1648 0 0 -0.793 -1.009 -17.319 17.384 0.782 1077 5 (b) -71 691 691 1088 1102 138 0 -18.074 -45.409 -148.550 156.458 4.800 1078 21 (g) -71 711 711 1088 1102 206 138 -1.005 -1.254 -5.911 6.126 0.000 1079 21 (g) -71 709 709 1088 1102 202 206 -1.320 -6.342 -25.473 26.283 0.000 1080 21 (g) -71 725 725 1088 1102 277 202 -0.551 -1.175 -3.129 3.388 0.000 1081 21 (g) -71 703 703 1088 1102 164 277 -0.969 -1.984 -9.299 9.558 0.000 1082 21 (g) -71 698 698 1088 1102 269 164 -3.535 -4.979 -20.739 21.620 0.000 1083 21 (g) -71 722 722 1088 1102 150 269 -0.538 -0.089 -2.176 2.243 0.000 1084 21 (g) -71 700 700 1088 1102 166 150 0.806 -0.372 -24.934 24.950 0.000 1085 21 (g) -71 912 912 1088 1102 275 166 -0.009 1.039 -99.564 99.569 0.145 1086 21 (g) -71 713 713 1088 1102 205 275 0.203 -0.175 -122.047 122.047 0.000 1087 -2 (ubar) -71 710 710 1088 1102 0 205 0.463 0.719 -172.943 172.946 0.330 1088 -513 (B*bar0) -83 1077 1087 1649 1650 0 0 -15.101 -37.120 -124.475 130.875 5.325 1089 -211 pi- 83 1077 1087 0 0 0 0 -0.765 -2.032 -6.614 6.962 0.140 1090 113 (rho0) -83 1077 1087 1436 1437 0 0 -2.970 -8.352 -27.182 28.605 0.902 1091 211 pi+ 83 1077 1087 0 0 0 0 -0.845 -2.693 -8.427 8.888 0.140 1092 311 (K0) -83 1077 1087 1438 1438 0 0 -2.604 -3.325 -16.031 16.585 0.498 1093 -321 K- 83 1077 1087 0 0 0 0 -0.753 -1.830 -7.608 7.877 0.494 1094 211 pi+ 83 1077 1087 0 0 0 0 -0.153 -1.435 -5.766 5.945 0.140 1095 223 (omega) -83 1077 1087 1651 1652 0 0 -0.779 -1.598 -7.272 7.526 0.768 1096 -213 (rho-) -83 1077 1087 1439 1440 0 0 -0.850 -2.125 -8.494 8.833 0.795 1097 323 (K*+) -84 1077 1087 1441 1442 0 0 -0.524 -0.520 -8.478 8.558 0.897 1098 -311 (Kbar0) -84 1077 1087 1443 1443 0 0 0.213 -0.673 -5.186 5.258 0.498 1099 113 (rho0) -84 1077 1087 1444 1445 0 0 -0.347 1.238 -44.853 44.878 0.786 1100 -211 pi- 84 1077 1087 0 0 0 0 -0.196 -0.710 -39.014 39.021 0.140 1101 213 (rho+) -84 1077 1087 1446 1447 0 0 0.892 1.226 -228.877 228.884 0.884 1102 -213 (rho-) -84 1077 1087 1448 1449 0 0 0.252 -0.071 -96.488 96.491 0.751 1103 21 (g) -71 773 773 1123 1168 204 316 -0.214 -0.101 -0.984 1.012 0.000 1104 21 (g) -71 745 745 1123 1168 101 204 0.439 0.190 -25.827 25.832 0.000 1105 21 (g) -71 728 728 1123 1168 317 101 0.287 0.180 3.024 3.043 0.000 1106 21 (g) -71 971 971 1123 1168 216 317 -1.523 0.806 35.354 35.401 0.565 1107 21 (g) -71 696 696 1123 1168 265 216 0.314 1.273 16.202 16.255 0.000 1108 21 (g) -71 721 721 1123 1168 120 265 0.322 1.527 36.457 36.491 0.000 1109 21 (g) -71 760 760 1123 1168 236 120 -0.221 1.139 3.650 3.830 0.000 1110 21 (g) -71 744 744 1123 1168 181 236 -0.602 -0.043 1.958 2.049 0.000 1111 21 (g) -71 970 970 1123 1168 281 181 -3.880 -0.587 4.178 5.758 0.549 1112 21 (g) -71 767 767 1123 1168 292 281 -0.159 -0.015 1.314 1.324 0.000 1113 21 (g) -71 768 768 1123 1168 107 292 -0.464 0.377 0.403 0.721 0.000 1114 21 (g) -71 766 766 1123 1168 272 107 0.225 -0.141 -0.161 0.311 0.000 1115 21 (g) -71 738 738 1123 1168 245 272 -0.190 0.529 -0.935 1.091 0.000 1116 21 (g) -71 762 762 1123 1168 186 245 0.317 -0.531 -0.350 0.711 0.000 1117 21 (g) -71 747 747 1123 1168 148 186 1.492 0.079 -4.529 4.769 0.000 1118 21 (g) -71 968 968 1123 1168 242 148 0.879 0.248 -4.360 4.460 0.218 1119 21 (g) -71 969 969 1123 1168 299 242 -0.926 0.728 -8.103 8.198 0.403 1120 21 (g) -71 770 770 1123 1168 146 299 -0.032 0.126 -9.735 9.736 0.000 1121 21 (g) -71 732 732 1123 1168 183 146 -0.902 -0.827 -9.888 9.963 0.000 1122 21 (g) -71 751 751 1123 1168 316 183 0.053 -0.510 -13.369 13.378 0.000 1123 211 pi+ 83 1103 1122 0 0 0 0 0.246 -0.273 -0.116 0.410 0.140 1124 -213 (rho-) -83 1103 1122 1450 1451 0 0 -0.189 0.739 -1.007 1.493 0.795 1125 223 (omega) -83 1103 1122 1653 1655 0 0 -0.071 -0.282 0.759 1.126 0.779 1126 211 pi+ 83 1103 1122 0 0 0 0 0.197 0.014 0.301 0.386 0.140 1127 2112 n0 83 1103 1122 0 0 0 0 -0.146 0.132 1.441 1.732 0.940 1128 111 (pi0) -83 1103 1122 1656 1657 0 0 -0.116 -0.270 3.589 3.604 0.135 1129 -3122 (Lambdabar0) -83 1103 1122 1658 1659 0 0 -0.395 1.156 15.277 15.366 1.116 1130 -321 K- 83 1103 1122 0 0 0 0 -0.212 1.349 35.338 35.368 0.494 1131 211 pi+ 83 1103 1122 0 0 0 0 -0.036 0.052 3.062 3.066 0.140 1132 311 (K0) -83 1103 1122 1452 1452 0 0 -0.142 0.069 4.795 4.823 0.498 1133 -313 (K*bar0) -83 1103 1122 1453 1454 0 0 -0.126 1.251 11.909 12.007 0.877 1134 111 (pi0) -83 1103 1122 1660 1661 0 0 0.245 0.269 5.079 5.094 0.135 1135 -213 (rho-) -83 1103 1122 1455 1456 0 0 -0.550 -0.228 3.521 3.640 0.703 1136 213 (rho+) -83 1103 1122 1457 1458 0 0 -0.327 -0.019 3.307 3.442 0.897 1137 2112 n0 83 1103 1122 0 0 0 0 -0.615 0.267 2.766 2.997 0.940 1138 111 (pi0) -83 1103 1122 1662 1663 0 0 -0.129 -0.102 2.755 2.763 0.135 1139 -2112 nbar0 83 1103 1122 0 0 0 0 -0.395 0.873 2.781 3.088 0.940 1140 313 (K*0) -83 1103 1122 1459 1460 0 0 -1.388 -0.008 2.673 3.144 0.900 1141 -321 K- 83 1103 1122 0 0 0 0 -0.241 -0.578 0.215 0.826 0.494 1142 211 pi+ 83 1103 1122 0 0 0 0 -0.621 0.290 0.583 0.911 0.140 1143 -211 pi- 83 1103 1122 0 0 0 0 -0.541 -0.247 0.183 0.637 0.140 1144 111 (pi0) -83 1103 1122 1664 1665 0 0 0.435 0.427 0.291 0.689 0.135 1145 211 pi+ 83 1103 1122 0 0 0 0 -0.347 -0.324 0.136 0.513 0.140 1146 223 (omega) -83 1103 1122 1666 1667 0 0 -0.141 0.279 -0.418 0.944 0.786 1147 -211 pi- 84 1103 1122 0 0 0 0 0.723 0.209 -1.450 1.640 0.140 1148 211 pi+ 84 1103 1122 0 0 0 0 0.371 0.372 -1.986 2.059 0.140 1149 111 (pi0) -84 1103 1122 1668 1669 0 0 -0.668 -0.504 -2.381 2.527 0.135 1150 111 (pi0) -84 1103 1122 1670 1671 0 0 0.277 -0.133 -2.141 2.167 0.135 1151 2112 n0 84 1103 1122 0 0 0 0 1.172 0.331 -3.348 3.684 0.940 1152 -2212 pbar- 84 1103 1122 0 0 0 0 -0.300 -0.299 -9.227 9.284 0.938 1153 211 pi+ 84 1103 1122 0 0 0 0 0.044 0.124 -0.691 0.717 0.140 1154 -211 pi- 84 1103 1122 0 0 0 0 -0.021 0.055 -1.993 1.999 0.140 1155 111 (pi0) -84 1103 1122 1672 1673 0 0 0.073 -0.018 -1.643 1.651 0.135 1156 211 pi+ 84 1103 1122 0 0 0 0 -0.770 0.063 -7.638 7.678 0.140 1157 111 (pi0) -84 1103 1122 1674 1675 0 0 0.216 0.059 -2.692 2.705 0.135 1158 -211 pi- 84 1103 1122 0 0 0 0 0.034 -0.279 -4.047 4.059 0.140 1159 211 pi+ 84 1103 1122 0 0 0 0 -0.301 -0.059 -9.395 9.402 0.140 1160 -211 pi- 84 1103 1122 0 0 0 0 0.184 0.061 -1.994 2.009 0.140 1161 221 (eta) -84 1103 1122 1676 1678 0 0 -0.168 -0.018 -6.591 6.615 0.548 1162 111 (pi0) -84 1103 1122 1679 1680 0 0 -0.331 -0.070 -3.837 3.854 0.135 1163 211 pi+ 84 1103 1122 0 0 0 0 0.143 -0.204 -3.538 3.549 0.140 1164 -211 pi- 84 1103 1122 0 0 0 0 0.119 -0.117 -1.642 1.657 0.140 1165 211 pi+ 84 1103 1122 0 0 0 0 0.003 0.134 -0.361 0.410 0.140 1166 -213 (rho-) -84 1103 1122 1461 1462 0 0 -0.145 -0.102 -5.781 5.835 0.771 1167 213 (rho+) -84 1103 1122 1463 1464 0 0 0.223 -0.035 -2.447 2.578 0.780 1168 -211 pi- 84 1103 1122 0 0 0 0 -0.057 0.044 -0.099 0.186 0.140 1169 2 (u) -71 712 712 1175 1192 103 0 -0.199 0.422 -67.684 67.686 0.330 1170 21 (g) -71 716 716 1175 1192 228 103 0.174 0.454 -206.627 206.627 0.000 1171 21 (g) -71 695 695 1175 1192 255 228 2.012 0.864 -674.756 674.759 0.000 1172 21 (g) -71 718 718 1175 1192 112 255 1.462 -0.157 -550.188 550.190 0.000 1173 21 (g) -71 917 917 1175 1192 312 112 0.871 0.813 7.884 7.977 0.214 1174 -4 (cbar) -71 863 863 1175 1192 0 312 1.018 -0.953 -0.360 2.079 1.500 1175 211 pi+ 83 1169 1174 0 0 0 0 -0.028 -0.120 -34.333 34.333 0.140 1176 111 (pi0) -83 1169 1174 1681 1682 0 0 0.069 0.209 -69.119 69.119 0.135 1177 -213 (rho-) -83 1169 1174 1465 1466 0 0 0.897 0.873 -393.756 393.758 0.726 1178 113 (rho0) -83 1169 1174 1467 1468 0 0 0.790 0.260 -403.772 403.774 1.029 1179 211 pi+ 83 1169 1174 0 0 0 0 0.499 0.401 -153.205 153.206 0.140 1180 -211 pi- 83 1169 1174 0 0 0 0 0.026 -0.174 -62.498 62.499 0.140 1181 211 pi+ 83 1169 1174 0 0 0 0 1.117 0.045 -275.940 275.943 0.140 1182 -213 (rho-) -84 1169 1174 1469 1470 0 0 0.012 0.284 -29.616 29.623 0.576 1183 2212 p+ 84 1169 1174 0 0 0 0 -0.110 -0.371 -49.948 49.958 0.938 1184 213 (rho+) -84 1169 1174 1471 1472 0 0 -0.270 0.289 -16.144 16.174 0.886 1185 -2224 (Deltabar--) -84 1169 1174 1473 1474 0 0 0.472 -0.143 -5.423 5.594 1.280 1186 323 (K*+) -84 1169 1174 1475 1476 0 0 -0.002 0.050 -5.145 5.222 0.893 1187 -321 K- 84 1169 1174 0 0 0 0 0.443 0.500 3.805 3.895 0.494 1188 323 (K*+) -84 1169 1174 1477 1478 0 0 0.130 0.131 0.605 1.091 0.889 1189 -321 K- 84 1169 1174 0 0 0 0 -0.182 -0.208 0.170 0.591 0.494 1190 111 (pi0) -84 1169 1174 1683 1684 0 0 0.234 -0.228 0.790 0.866 0.135 1191 323 (K*+) -84 1169 1174 1479 1480 0 0 0.438 -0.090 0.301 1.060 0.913 1192 -431 (D_s-) -84 1169 1174 1685 1686 0 0 0.803 -0.263 1.497 2.614 1.968 1193 2 (u) -71 908 908 1195 1205 159 0 0.537 -0.098 388.118 388.119 0.330 1194 -1 (dbar) -71 911 911 1195 1205 0 159 0.524 -0.346 -34.610 34.618 0.330 1195 211 pi+ 83 1193 1194 0 0 0 0 0.545 0.181 211.134 211.135 0.140 1196 -211 pi- 83 1193 1194 0 0 0 0 -0.295 -0.262 87.346 87.347 0.140 1197 111 (pi0) -83 1193 1194 1687 1688 0 0 0.205 0.095 31.941 31.942 0.135 1198 113 (rho0) -83 1193 1194 1481 1482 0 0 -0.155 -0.198 34.933 34.965 1.471 1199 213 (rho+) -84 1193 1194 1483 1484 0 0 0.327 0.084 10.728 10.758 0.737 1200 -213 (rho-) -84 1193 1194 1485 1486 0 0 0.099 0.049 4.799 4.852 0.704 1201 111 (pi0) -84 1193 1194 1689 1690 0 0 -0.428 0.182 2.558 2.603 0.135 1202 211 pi+ 84 1193 1194 0 0 0 0 0.072 -0.306 3.288 3.306 0.140 1203 311 (K0) -84 1193 1194 1487 1487 0 0 0.128 0.681 0.804 1.172 0.498 1204 333 (phi) -84 1193 1194 1691 1692 0 0 -0.041 -0.539 -0.780 1.392 1.018 1205 -313 (K*bar0) -84 1193 1194 1488 1489 0 0 0.603 -0.410 -33.243 33.264 0.920 1206 1 (d) -71 880 880 1208 1223 260 0 -0.342 -0.138 -18.583 18.590 0.330 1207 2101 (ud_0) -71 906 906 1208 1223 0 260 0.118 -0.582 2607.221 2607.221 0.579 1208 223 (omega) -83 1206 1207 1693 1695 0 0 -0.280 -0.109 -14.511 14.536 0.781 1209 113 (rho0) -83 1206 1207 1490 1491 0 0 -0.241 -0.063 -1.821 2.051 0.909 1210 -213 (rho-) -83 1206 1207 1492 1493 0 0 0.075 0.217 -1.108 1.365 0.764 1211 113 (rho0) -83 1206 1207 1494 1495 0 0 0.016 0.325 -0.089 0.844 0.774 1212 211 pi+ 83 1206 1207 0 0 0 0 -0.105 -0.770 0.589 0.985 0.140 1213 -211 pi- 83 1206 1207 0 0 0 0 -0.097 0.351 0.740 0.837 0.140 1214 211 pi+ 83 1206 1207 0 0 0 0 0.390 -0.093 0.448 0.617 0.140 1215 1114 (Delta-) -83 1206 1207 1496 1497 0 0 -0.282 0.204 10.192 10.316 1.558 1216 -3112 (Sigmabar+) -83 1206 1207 1696 1697 0 0 0.135 -0.488 17.793 17.840 1.197 1217 -321 K- 84 1206 1207 0 0 0 0 0.264 0.082 30.199 30.204 0.494 1218 211 pi+ 84 1206 1207 0 0 0 0 -0.269 0.468 37.554 37.558 0.140 1219 -213 (rho-) -84 1206 1207 1498 1499 0 0 -0.042 -0.090 222.715 222.717 0.836 1220 211 pi+ 84 1206 1207 0 0 0 0 0.311 -0.346 237.113 237.113 0.140 1221 -211 pi- 84 1206 1207 0 0 0 0 -0.533 -0.007 136.274 136.276 0.140 1222 111 (pi0) -84 1206 1207 1698 1699 0 0 0.624 -0.100 312.893 312.893 0.135 1223 2212 p+ 84 1206 1207 0 0 0 0 -0.189 -0.301 1599.658 1599.659 0.938 1224 3 (s) -71 781 781 1254 1301 167 0 -0.398 0.163 -0.950 1.157 0.500 1225 21 (g) -71 779 779 1254 1301 264 167 1.150 -0.070 -2.636 2.877 0.000 1226 21 (g) -71 871 871 1254 1301 251 264 0.368 -0.368 -2.049 2.114 0.000 1227 21 (g) -71 902 902 1254 1301 258 251 -0.758 -2.406 -13.663 13.894 0.000 1228 21 (g) -71 929 929 1254 1301 209 258 -0.992 -1.086 -3.241 3.566 0.226 1229 21 (g) -71 927 927 1254 1301 142 209 0.021 -1.209 -1.993 2.340 0.206 1230 21 (g) -71 784 784 1254 1301 301 142 0.447 -0.686 -1.074 1.351 0.000 1231 21 (g) -71 932 932 1254 1301 252 301 1.054 0.247 -0.699 1.315 0.263 1232 21 (g) -71 928 928 1254 1301 261 252 -0.089 0.394 -1.161 1.249 0.221 1233 21 (g) -71 921 921 1254 1301 174 261 -1.086 0.269 -6.085 6.189 0.132 1234 21 (g) -71 931 931 1254 1301 122 174 -0.217 -1.961 -1.474 2.477 0.262 1235 21 (g) -71 933 933 1254 1301 270 122 -0.002 -2.084 -0.564 2.187 0.344 1236 21 (g) -71 777 777 1254 1301 111 270 -3.064 -1.803 -0.638 3.612 0.000 1237 21 (g) -71 923 923 1254 1301 199 111 -0.785 -0.752 0.511 1.211 0.162 1238 21 (g) -71 786 786 1254 1301 237 199 -0.524 -0.135 -0.069 0.545 0.000 1239 21 (g) -71 924 924 1254 1301 117 237 -1.078 0.151 0.734 1.324 0.172 1240 21 (g) -71 926 926 1254 1301 279 117 -0.940 0.177 -0.566 1.128 0.189 1241 21 (g) -71 922 922 1254 1301 158 279 -0.088 0.358 -0.097 0.406 0.141 1242 21 (g) -71 813 813 1254 1301 267 158 1.360 -0.935 1.513 2.239 0.000 1243 21 (g) -71 825 825 1254 1301 220 267 1.822 -1.330 5.829 6.250 0.000 1244 21 (g) -71 934 934 1254 1301 203 220 0.481 -2.594 11.802 12.098 0.346 1245 21 (g) -71 919 919 1254 1301 314 203 0.769 0.020 10.945 10.972 0.108 1246 21 (g) -71 832 832 1254 1301 285 314 0.251 0.083 19.484 19.486 0.000 1247 21 (g) -71 861 861 1254 1301 210 285 -0.257 0.474 147.304 147.305 0.000 1248 21 (g) -71 886 886 1254 1301 153 210 -1.229 -0.264 718.416 718.418 0.000 1249 21 (g) -71 848 848 1254 1301 135 153 -1.318 -1.423 641.025 641.028 0.000 1250 21 (g) -71 935 935 1254 1301 224 135 -0.610 -0.580 102.489 102.493 0.379 1251 21 (g) -71 851 851 1254 1301 253 224 -2.226 0.150 118.273 118.294 0.000 1252 21 (g) -71 868 868 1254 1301 139 253 -0.482 0.100 14.154 14.162 0.000 1253 -1 (dbar) -71 930 930 1254 1301 0 139 -0.487 -2.453 68.024 68.074 0.732 1254 -311 (Kbar0) -83 1224 1253 1500 1500 0 0 0.263 -0.087 -0.859 1.031 0.498 1255 111 (pi0) -83 1224 1253 1700 1701 0 0 0.142 -0.090 -0.283 0.356 0.135 1256 223 (omega) -83 1224 1253 1702 1704 0 0 -0.011 -0.071 -2.964 3.064 0.772 1257 113 (rho0) -83 1224 1253 1501 1502 0 0 -0.120 -0.057 -2.425 2.550 0.777 1258 -211 pi- 83 1224 1253 0 0 0 0 0.173 -1.197 -4.736 4.890 0.140 1259 213 (rho+) -83 1224 1253 1503 1504 0 0 -0.418 -0.816 -5.773 5.916 0.913 1260 113 (rho0) -83 1224 1253 1505 1506 0 0 -0.192 -1.407 -4.608 4.872 0.697 1261 -213 (rho-) -83 1224 1253 1507 1508 0 0 0.004 -0.885 -2.099 2.458 0.923 1262 211 pi+ 83 1224 1253 0 0 0 0 -0.191 -0.058 -0.172 0.299 0.140 1263 -211 pi- 83 1224 1253 0 0 0 0 0.363 -0.328 -0.431 0.667 0.140 1264 213 (rho+) -83 1224 1253 1509 1510 0 0 0.377 -0.098 -2.238 2.556 1.172 1265 -213 (rho-) -83 1224 1253 1511 1512 0 0 -0.375 -0.382 -2.385 2.529 0.650 1266 113 (rho0) -83 1224 1253 1513 1514 0 0 0.418 0.281 -1.649 1.885 0.761 1267 211 pi+ 83 1224 1253 0 0 0 0 -0.027 -0.041 -0.221 0.266 0.140 1268 313 (K*0) -83 1224 1253 1515 1516 0 0 -0.215 -0.109 -1.030 1.418 0.944 1269 -321 K- 83 1224 1253 0 0 0 0 -0.465 -0.476 -1.246 1.497 0.494 1270 2212 p+ 83 1224 1253 0 0 0 0 0.287 -0.783 -1.006 1.609 0.938 1271 -2212 pbar- 83 1224 1253 0 0 0 0 -0.936 -1.340 -1.066 2.165 0.938 1272 211 pi+ 83 1224 1253 0 0 0 0 -0.532 -0.617 -0.505 0.968 0.140 1273 111 (pi0) -83 1224 1253 1705 1706 0 0 -0.077 -0.541 -0.525 0.770 0.135 1274 111 (pi0) -83 1224 1253 1707 1708 0 0 -1.119 -0.862 0.324 1.456 0.135 1275 311 (K0) -83 1224 1253 1517 1517 0 0 -0.200 -0.366 0.157 0.668 0.498 1276 3122 (Lambda0) -83 1224 1253 1709 1710 0 0 -2.381 -0.108 -0.199 2.639 1.116 1277 111 (pi0) -83 1224 1253 1711 1712 0 0 -0.270 -0.505 0.644 0.872 0.135 1278 -2212 pbar- 83 1224 1253 0 0 0 0 -1.366 -0.119 0.184 1.671 0.938 1279 211 pi+ 83 1224 1253 0 0 0 0 0.383 -0.325 -0.243 0.575 0.140 1280 113 (rho0) -84 1224 1253 1518 1519 0 0 1.167 -0.621 3.224 3.567 0.764 1281 111 (pi0) -84 1224 1253 1713 1714 0 0 0.287 -0.037 0.816 0.876 0.135 1282 2112 n0 84 1224 1253 0 0 0 0 0.666 -1.532 5.492 5.817 0.940 1283 -2212 pbar- 84 1224 1253 0 0 0 0 0.782 0.291 4.057 4.247 0.938 1284 211 pi+ 84 1224 1253 0 0 0 0 0.273 -1.599 12.115 12.224 0.140 1285 223 (omega) -84 1224 1253 1715 1717 0 0 0.476 -0.190 11.356 11.395 0.787 1286 -211 pi- 84 1224 1253 0 0 0 0 0.078 -0.266 1.762 1.789 0.140 1287 323 (K*+) -84 1224 1253 1520 1521 0 0 -0.181 -0.288 18.774 18.801 0.952 1288 -321 K- 84 1224 1253 0 0 0 0 0.142 0.188 37.478 37.482 0.494 1289 211 pi+ 84 1224 1253 0 0 0 0 -0.096 0.340 51.093 51.095 0.140 1290 111 (pi0) -84 1224 1253 1718 1719 0 0 -0.090 -0.265 10.273 10.278 0.135 1291 -211 pi- 84 1224 1253 0 0 0 0 0.036 0.255 37.940 37.941 0.140 1292 2212 p+ 84 1224 1253 0 0 0 0 0.111 -0.416 195.119 195.122 0.938 1293 113 (rho0) -84 1224 1253 1522 1523 0 0 -0.246 -0.014 217.769 217.771 0.757 1294 -2114 (Deltabar0) -84 1224 1253 1524 1525 0 0 -1.764 -0.556 642.298 642.302 1.523 1295 -213 (rho-) -84 1224 1253 1526 1527 0 0 -0.368 -0.486 238.661 238.663 0.794 1296 223 (omega) -84 1224 1253 1720 1722 0 0 -1.654 -0.005 142.918 142.930 0.784 1297 213 (rho+) -84 1224 1253 1528 1529 0 0 -0.340 -0.436 44.338 44.347 0.711 1298 -213 (rho-) -84 1224 1253 1530 1531 0 0 -0.305 -0.806 70.969 70.983 1.111 1299 213 (rho+) -84 1224 1253 1532 1533 0 0 -0.286 -1.253 59.843 59.863 0.846 1300 113 (rho0) -84 1224 1253 1534 1535 0 0 -1.104 -0.293 49.125 49.145 0.814 1301 111 (pi0) -84 1224 1253 1723 1724 0 0 -0.005 -0.182 3.474 3.481 0.135 1302 3 (s) -71 837 837 1311 1331 132 0 0.961 3.903 73.410 73.522 0.500 1303 21 (g) -71 949 949 1311 1331 263 132 -0.757 -0.550 10.739 10.781 0.169 1304 21 (g) -71 951 951 1311 1331 193 263 -0.771 -0.723 3.776 3.930 0.267 1305 21 (g) -71 953 953 1311 1331 137 193 -0.936 0.038 3.650 3.783 0.327 1306 21 (g) -71 828 828 1311 1331 126 137 -1.537 3.174 9.016 9.681 0.000 1307 21 (g) -71 954 954 1311 1331 143 126 -2.233 2.459 6.392 7.223 0.523 1308 21 (g) -71 952 952 1311 1331 124 143 0.481 1.347 2.999 3.335 0.287 1309 21 (g) -71 822 822 1311 1331 123 124 0.082 1.419 5.089 5.284 0.000 1310 2101 (ud_0) -71 909 909 1311 1331 0 123 1.213 -0.132 -2020.435 2020.435 0.579 1311 -313 (K*bar0) -83 1302 1310 1536 1537 0 0 0.717 2.547 52.113 52.187 0.875 1312 111 (pi0) -83 1302 1310 1725 1726 0 0 0.439 1.073 15.490 15.534 0.135 1313 113 (rho0) -83 1302 1310 1538 1539 0 0 -0.832 -0.143 10.350 10.439 1.067 1314 -213 (rho-) -83 1302 1310 1540 1541 0 0 -1.147 0.332 9.452 9.562 0.823 1315 211 pi+ 83 1302 1310 0 0 0 0 -0.084 -0.093 0.103 0.214 0.140 1316 113 (rho0) -83 1302 1310 1542 1543 0 0 -0.352 -0.436 3.721 3.870 0.900 1317 311 (K0) -83 1302 1310 1544 1544 0 0 -1.197 1.409 5.501 5.825 0.498 1318 -313 (K*bar0) -83 1302 1310 1545 1546 0 0 -1.418 2.397 6.543 7.196 1.104 1319 -211 pi- 83 1302 1310 0 0 0 0 -0.342 0.309 1.091 1.193 0.140 1320 2212 p+ 83 1302 1310 0 0 0 0 -0.824 1.495 3.831 4.298 0.938 1321 -2112 nbar0 84 1302 1310 0 0 0 0 0.449 0.821 3.644 3.878 0.940 1322 223 (omega) -84 1302 1310 1727 1729 0 0 0.030 0.618 1.505 1.787 0.738 1323 -211 pi- 84 1302 1310 0 0 0 0 0.299 0.611 1.243 1.424 0.140 1324 113 (rho0) -84 1302 1310 1547 1548 0 0 -0.387 0.064 -3.280 3.398 0.797 1325 111 (pi0) -84 1302 1310 1730 1731 0 0 0.010 0.060 -0.022 0.150 0.135 1326 213 (rho+) -84 1302 1310 1549 1550 0 0 -0.046 -0.203 -2.039 2.222 0.860 1327 113 (rho0) -84 1302 1310 1551 1552 0 0 -0.125 0.658 -3.404 3.560 0.800 1328 -213 (rho-) -84 1302 1310 1553 1554 0 0 0.324 -0.813 -55.429 55.445 0.984 1329 113 (rho0) -84 1302 1310 1555 1556 0 0 -0.674 0.420 -47.147 47.159 0.676 1330 211 pi+ 84 1302 1310 0 0 0 0 0.929 -0.076 -457.213 457.214 0.140 1331 2112 n0 84 1302 1310 0 0 0 0 0.733 -0.117 -1451.417 1451.418 0.940 1332 1 (d) -71 806 806 1356 1390 188 0 -0.503 -0.738 -39.507 39.518 0.330 1333 21 (g) -71 937 937 1356 1390 246 188 -2.782 -0.102 -100.675 100.713 0.202 1334 21 (g) -71 943 943 1356 1390 160 246 -0.319 -0.286 -28.737 28.744 0.440 1335 21 (g) -71 792 792 1356 1390 309 160 0.978 -0.627 -19.973 20.006 0.000 1336 21 (g) -71 780 780 1356 1390 115 309 0.552 -0.353 -37.555 37.561 0.000 1337 21 (g) -71 938 938 1356 1390 266 115 2.272 0.162 -138.511 138.529 0.208 1338 21 (g) -71 758 758 1356 1390 109 266 2.534 0.005 -237.260 237.274 0.000 1339 21 (g) -71 735 735 1356 1390 169 109 -0.559 0.915 -4.292 4.424 0.000 1340 21 (g) -71 764 764 1356 1390 257 169 -0.628 0.821 -9.040 9.099 0.000 1341 21 (g) -71 939 939 1356 1390 229 257 -0.390 0.471 -1.522 1.654 0.213 1342 21 (g) -71 754 754 1356 1390 221 229 0.426 -0.469 -1.739 1.851 0.000 1343 21 (g) -71 757 757 1356 1390 230 221 -0.175 -0.857 -0.580 1.050 0.000 1344 21 (g) -71 945 945 1356 1390 235 230 0.234 0.763 -1.564 1.848 0.575 1345 21 (g) -71 941 941 1356 1390 177 235 0.017 -0.234 0.435 0.619 0.374 1346 21 (g) -71 731 731 1356 1390 307 177 -0.748 0.488 0.659 1.110 0.000 1347 21 (g) -71 942 942 1356 1390 254 307 -1.382 0.040 0.165 1.458 0.432 1348 21 (g) -71 750 750 1356 1390 106 254 0.297 0.239 -0.042 0.383 0.000 1349 21 (g) -71 736 736 1356 1390 133 106 1.231 0.369 23.038 23.074 0.000 1350 21 (g) -71 772 772 1356 1390 313 133 0.383 -0.225 16.176 16.182 0.000 1351 21 (g) -71 742 742 1356 1390 322 313 -0.181 -0.055 32.072 32.072 0.000 1352 21 (g) -71 774 774 1356 1390 218 322 0.897 0.130 101.463 101.467 0.000 1353 21 (g) -71 940 940 1356 1390 294 218 1.910 -0.290 153.514 153.527 0.220 1354 21 (g) -71 944 944 1356 1390 149 294 0.614 0.549 200.943 200.945 0.512 1355 -1 (dbar) -71 824 824 1356 1390 0 149 -1.368 -2.913 683.574 683.582 0.330 1356 -213 (rho-) -83 1332 1355 1557 1558 0 0 -1.320 -0.800 -68.531 68.558 1.095 1357 111 (pi0) -83 1332 1355 1732 1733 0 0 -1.925 -0.331 -83.710 83.733 0.135 1358 221 (eta) -83 1332 1355 1734 1736 0 0 -0.298 -0.453 -12.006 12.031 0.548 1359 111 (pi0) -83 1332 1355 1737 1738 0 0 1.146 0.020 -51.575 51.588 0.135 1360 323 (K*+) -83 1332 1355 1559 1560 0 0 2.331 -0.129 -163.292 163.311 0.937 1361 -311 (Kbar0) -83 1332 1355 1561 1561 0 0 0.203 -0.046 -18.445 18.453 0.498 1362 111 (pi0) -83 1332 1355 1739 1740 0 0 0.654 -0.154 -74.541 74.544 0.135 1363 -211 pi- 83 1332 1355 0 0 0 0 1.334 0.181 -77.654 77.666 0.140 1364 213 (rho+) -83 1332 1355 1562 1563 0 0 0.533 -0.003 -23.080 23.091 0.452 1365 111 (pi0) -83 1332 1355 1741 1742 0 0 0.452 -0.316 -25.293 25.300 0.135 1366 -213 (rho-) -83 1332 1355 1564 1565 0 0 -1.168 0.720 -10.623 10.739 0.769 1367 321 K+ 83 1332 1355 0 0 0 0 0.205 0.210 -1.482 1.590 0.494 1368 -311 (Kbar0) -83 1332 1355 1566 1566 0 0 -0.309 0.274 -2.384 2.471 0.498 1369 113 (rho0) -83 1332 1355 1567 1568 0 0 0.044 0.338 -3.350 3.440 0.701 1370 -211 pi- 83 1332 1355 0 0 0 0 -0.381 0.247 -0.644 0.801 0.140 1371 223 (omega) -83 1332 1355 1743 1745 0 0 0.315 0.429 -1.994 2.206 0.778 1372 323 (K*+) -83 1332 1355 1569 1570 0 0 -0.569 -0.368 -0.013 1.117 0.888 1373 -323 (K*-) -83 1332 1355 1571 1572 0 0 0.008 -0.469 -1.380 1.716 0.905 1374 213 (rho+) -83 1332 1355 1573 1574 0 0 -0.301 0.693 -0.401 1.212 0.859 1375 -211 pi- 83 1332 1355 0 0 0 0 0.293 0.054 -0.039 0.331 0.140 1376 211 pi+ 84 1332 1355 0 0 0 0 -1.568 0.084 0.959 1.846 0.140 1377 111 (pi0) -84 1332 1355 1746 1747 0 0 0.052 0.037 0.263 0.302 0.135 1378 -211 pi- 84 1332 1355 0 0 0 0 0.275 -0.210 0.605 0.711 0.140 1379 211 pi+ 84 1332 1355 0 0 0 0 -0.049 0.312 4.237 4.251 0.140 1380 111 (pi0) -84 1332 1355 1748 1749 0 0 -0.027 0.056 2.019 2.024 0.135 1381 2114 (Delta0) -84 1332 1355 1575 1576 0 0 0.391 -0.330 5.272 5.429 1.190 1382 111 (pi0) -84 1332 1355 1750 1751 0 0 0.050 0.489 2.746 2.793 0.135 1383 -2112 nbar0 84 1332 1355 0 0 0 0 0.286 -0.002 18.603 18.629 0.940 1384 111 (pi0) -84 1332 1355 1752 1753 0 0 1.418 -0.205 91.972 91.983 0.135 1385 -211 pi- 84 1332 1355 0 0 0 0 0.132 -0.043 8.456 8.458 0.140 1386 111 (pi0) -84 1332 1355 1754 1755 0 0 0.428 0.154 26.403 26.407 0.135 1387 211 pi+ 84 1332 1355 0 0 0 0 0.125 -0.338 236.532 236.533 0.140 1388 113 (rho0) -84 1332 1355 1577 1578 0 0 0.542 0.052 129.032 129.036 0.881 1389 223 (omega) -84 1332 1355 1756 1757 0 0 0.797 0.107 127.188 127.193 0.788 1390 113 (rho0) -84 1332 1355 1579 1580 0 0 -0.791 -2.459 557.195 557.202 1.061 1391 310 (K_S0) -91 975 975 1758 1759 0 0 -0.021 0.745 9.780 9.821 0.498 1392 -211 pi- 91 995 0 0 0 0 0 -0.170 0.571 0.196 0.643 0.140 1393 111 (pi0) -91 995 0 1760 1761 0 0 0.129 -0.158 0.394 0.464 0.135 1394 211 pi+ 91 996 0 0 0 0 0 0.032 -0.153 -0.275 0.346 0.140 1395 111 (pi0) -91 996 0 1762 1763 0 0 0.230 0.590 -0.150 0.665 0.135 1396 -211 pi- 91 999 0 0 0 0 0 0.019 0.819 -1.209 1.467 0.140 1397 111 (pi0) -91 999 0 1764 1765 0 0 0.419 0.142 -0.052 0.466 0.135 1398 130 K_L0 91 1006 1006 0 0 0 0 -0.784 2.314 1.170 2.754 0.498 1399 310 (K_S0) -91 1007 1007 1766 1767 0 0 0.092 1.143 0.962 1.578 0.498 1400 211 pi+ 91 1014 0 0 0 0 0 0.564 0.644 59.092 59.099 0.140 1401 -211 pi- 91 1014 0 0 0 0 0 -0.027 0.420 53.596 53.598 0.140 1402 130 K_L0 91 1016 1016 0 0 0 0 -0.276 0.157 1.732 1.830 0.498 1403 -311 (Kbar0) -91 1017 0 1581 1581 0 0 -0.173 0.218 -0.018 0.570 0.498 1404 -211 pi- 91 1017 0 0 0 0 0 0.041 -0.258 0.347 0.457 0.140 1405 211 pi+ 91 1026 0 0 0 0 0 0.366 -0.654 -1.371 1.568 0.140 1406 -211 pi- 91 1026 0 0 0 0 0 0.016 0.121 -1.083 1.098 0.140 1407 211 pi+ 91 1034 0 0 0 0 0 0.302 0.030 -43.035 43.036 0.140 1408 111 (pi0) -91 1034 0 1768 1769 0 0 0.546 1.287 -33.840 33.869 0.135 1409 211 pi+ 91 1036 0 0 0 0 0 0.876 0.612 -6.090 6.184 0.140 1410 -211 pi- 91 1036 0 0 0 0 0 -0.002 0.011 -2.313 2.317 0.140 1411 311 (K0) -91 1037 0 1582 1582 0 0 0.159 0.617 -8.444 8.482 0.498 1412 211 pi+ 91 1037 0 0 0 0 0 -0.027 0.093 -0.391 0.426 0.140 1413 -211 pi- 91 1042 0 0 0 0 0 0.507 -0.145 10.820 10.834 0.140 1414 111 (pi0) -91 1042 0 1770 1771 0 0 -0.293 -0.030 7.163 7.170 0.135 1415 -211 pi- 91 1045 0 0 0 0 0 0.143 -0.170 0.176 0.316 0.140 1416 111 (pi0) -91 1045 0 1772 1773 0 0 0.018 0.347 2.142 2.174 0.135 1417 -211 pi- 91 1047 0 0 0 0 0 -0.026 5.959 2.274 6.379 0.140 1418 111 (pi0) -91 1047 0 1774 1775 0 0 0.270 0.932 0.347 1.040 0.135 1419 -311 (Kbar0) -91 1051 0 1583 1583 0 0 0.530 -0.160 -262.679 262.680 0.498 1420 111 (pi0) -91 1051 0 1776 1777 0 0 -0.167 -0.054 -94.926 94.926 0.135 1421 211 pi+ 91 1054 0 0 0 0 0 -0.515 -0.009 -17.442 17.450 0.140 1422 -211 pi- 91 1054 0 0 0 0 0 0.209 -0.141 -4.516 4.525 0.140 1423 310 (K_S0) -91 1055 1055 1778 1779 0 0 0.179 -0.160 -3.999 4.037 0.498 1424 211 pi+ 91 1069 0 0 0 0 0 0.493 1.041 9.549 9.619 0.140 1425 111 (pi0) -91 1069 0 1780 1781 0 0 0.369 -0.265 2.060 2.114 0.135 1426 211 pi+ 91 1070 0 0 0 0 0 0.690 0.605 0.581 1.096 0.140 1427 -211 pi- 91 1070 0 0 0 0 0 2.488 1.909 3.674 4.832 0.140 1428 211 pi+ 91 1071 0 0 0 0 0 1.225 0.828 0.040 1.485 0.140 1429 -211 pi- 91 1071 0 0 0 0 0 1.685 0.559 1.267 2.186 0.140 1430 2112 n0 91 1072 0 0 0 0 0 0.474 0.784 0.148 1.321 0.940 1431 111 (pi0) -91 1072 0 1782 1783 0 0 0.552 0.327 0.322 0.731 0.135 1432 211 pi+ 91 1073 0 0 0 0 0 -0.033 0.122 -0.064 0.199 0.140 1433 111 (pi0) -91 1073 0 1784 1785 0 0 0.095 -0.401 -0.654 0.784 0.135 1434 -2212 pbar- 91 1074 0 0 0 0 0 0.008 0.389 -5.745 5.834 0.938 1435 -211 pi- 91 1074 0 0 0 0 0 -0.387 -0.093 -2.871 2.902 0.140 1436 211 pi+ 91 1090 0 0 0 0 0 -2.274 -5.926 -20.516 21.476 0.140 1437 -211 pi- 91 1090 0 0 0 0 0 -0.696 -2.427 -6.666 7.129 0.140 1438 310 (K_S0) -91 1092 1092 1786 1787 0 0 -2.604 -3.325 -16.031 16.585 0.498 1439 -211 pi- 91 1096 0 0 0 0 0 -0.617 -1.137 -3.479 3.714 0.140 1440 111 (pi0) -91 1096 0 1788 1789 0 0 -0.233 -0.988 -5.015 5.119 0.135 1441 311 (K0) -91 1097 0 1584 1584 0 0 -0.200 -0.274 -6.741 6.768 0.498 1442 211 pi+ 91 1097 0 0 0 0 0 -0.323 -0.246 -1.737 1.790 0.140 1443 130 K_L0 91 1098 1098 0 0 0 0 0.213 -0.673 -5.186 5.258 0.498 1444 211 pi+ 91 1099 0 0 0 0 0 -0.451 0.993 -40.496 40.511 0.140 1445 -211 pi- 91 1099 0 0 0 0 0 0.105 0.245 -4.356 4.367 0.140 1446 211 pi+ 91 1101 0 0 0 0 0 0.743 0.966 -120.696 120.703 0.140 1447 111 (pi0) -91 1101 0 1790 1791 0 0 0.149 0.261 -108.181 108.182 0.135 1448 -211 pi- 91 1102 0 0 0 0 0 0.271 0.169 -21.969 21.972 0.140 1449 111 (pi0) -91 1102 0 1792 1793 0 0 -0.019 -0.240 -74.519 74.519 0.135 1450 -211 pi- 91 1124 0 0 0 0 0 -0.309 0.007 -0.227 0.408 0.140 1451 111 (pi0) -91 1124 0 1794 1795 0 0 0.120 0.732 -0.780 1.085 0.135 1452 130 K_L0 91 1132 1132 0 0 0 0 -0.142 0.069 4.795 4.823 0.498 1453 -321 K- 91 1133 0 0 0 0 0 -0.322 1.097 9.931 10.009 0.494 1454 211 pi+ 91 1133 0 0 0 0 0 0.196 0.154 1.978 1.998 0.140 1455 -211 pi- 91 1135 0 0 0 0 0 -0.391 0.185 1.571 1.636 0.140 1456 111 (pi0) -91 1135 0 1796 1797 0 0 -0.159 -0.412 1.950 2.004 0.135 1457 211 pi+ 91 1136 0 0 0 0 0 0.122 0.324 1.187 1.245 0.140 1458 111 (pi0) -91 1136 0 1798 1799 0 0 -0.448 -0.343 2.120 2.198 0.135 1459 321 K+ 91 1140 0 0 0 0 0 -0.652 -0.190 1.031 1.329 0.494 1460 -211 pi- 91 1140 0 0 0 0 0 -0.736 0.182 1.642 1.814 0.140 1461 -211 pi- 91 1166 0 0 0 0 0 -0.228 -0.290 -1.642 1.688 0.140 1462 111 (pi0) -91 1166 0 1800 1801 0 0 0.082 0.188 -4.139 4.147 0.135 1463 211 pi+ 91 1167 0 0 0 0 0 0.335 -0.313 -1.341 1.424 0.140 1464 111 (pi0) -91 1167 0 1802 1803 0 0 -0.113 0.278 -1.107 1.154 0.135 1465 -211 pi- 91 1177 0 0 0 0 0 0.397 -0.012 -109.026 109.026 0.140 1466 111 (pi0) -91 1177 0 1804 1805 0 0 0.501 0.885 -284.730 284.732 0.135 1467 211 pi+ 91 1178 0 0 0 0 0 0.413 -0.052 -334.897 334.898 0.140 1468 -211 pi- 91 1178 0 0 0 0 0 0.377 0.312 -68.875 68.877 0.140 1469 -211 pi- 91 1182 0 0 0 0 0 -0.047 0.414 -18.376 18.381 0.140 1470 111 (pi0) -91 1182 0 1806 1807 0 0 0.059 -0.130 -11.240 11.242 0.135 1471 211 pi+ 91 1184 0 0 0 0 0 0.116 0.214 -1.690 1.713 0.140 1472 111 (pi0) -91 1184 0 1808 1809 0 0 -0.386 0.075 -14.454 14.460 0.135 1473 -2212 pbar- 91 1185 0 0 0 0 0 0.409 -0.377 -4.243 4.381 0.938 1474 -211 pi- 91 1185 0 0 0 0 0 0.064 0.234 -1.180 1.213 0.140 1475 311 (K0) -91 1186 0 1585 1585 0 0 -0.024 -0.249 -2.900 2.953 0.498 1476 211 pi+ 91 1186 0 0 0 0 0 0.022 0.299 -2.245 2.269 0.140 1477 311 (K0) -91 1188 0 1586 1586 0 0 0.316 0.129 0.222 0.643 0.498 1478 211 pi+ 91 1188 0 0 0 0 0 -0.186 0.002 0.383 0.448 0.140 1479 311 (K0) -91 1191 0 1587 1587 0 0 0.189 -0.205 0.442 0.722 0.498 1480 211 pi+ 91 1191 0 0 0 0 0 0.249 0.115 -0.141 0.338 0.140 1481 211 pi+ 91 1198 0 0 0 0 0 -0.092 -0.770 13.001 13.025 0.140 1482 -211 pi- 91 1198 0 0 0 0 0 -0.063 0.572 21.932 21.940 0.140 1483 211 pi+ 91 1199 0 0 0 0 0 0.531 0.003 7.746 7.765 0.140 1484 111 (pi0) -91 1199 0 1810 1811 0 0 -0.204 0.081 2.982 2.993 0.135 1485 -211 pi- 91 1200 0 0 0 0 0 -0.111 -0.096 3.945 3.950 0.140 1486 111 (pi0) -91 1200 0 1812 1813 0 0 0.210 0.145 0.854 0.902 0.135 1487 130 K_L0 91 1203 1203 0 0 0 0 0.128 0.681 0.804 1.172 0.498 1488 -311 (Kbar0) -91 1205 0 1588 1588 0 0 0.421 -0.001 -24.030 24.039 0.498 1489 111 (pi0) -91 1205 0 1814 1815 0 0 0.183 -0.409 -9.213 9.225 0.135 1490 211 pi+ 91 1209 0 0 0 0 0 0.091 0.038 -1.613 1.622 0.140 1491 -211 pi- 91 1209 0 0 0 0 0 -0.333 -0.101 -0.208 0.429 0.140 1492 -211 pi- 91 1210 0 0 0 0 0 0.288 0.190 -0.200 0.423 0.140 1493 111 (pi0) -91 1210 0 1816 1817 0 0 -0.213 0.027 -0.908 0.942 0.135 1494 211 pi+ 91 1211 0 0 0 0 0 -0.182 -0.071 0.187 0.304 0.140 1495 -211 pi- 91 1211 0 0 0 0 0 0.198 0.396 -0.276 0.540 0.140 1496 2112 n0 91 1215 0 0 0 0 0 -0.238 0.528 5.434 5.545 0.940 1497 -211 pi- 91 1215 0 0 0 0 0 -0.044 -0.324 4.758 4.771 0.140 1498 -211 pi- 91 1219 0 0 0 0 0 0.150 0.262 149.335 149.335 0.140 1499 111 (pi0) -91 1219 0 1818 1819 0 0 -0.192 -0.352 73.380 73.381 0.135 1500 130 K_L0 91 1254 1254 0 0 0 0 0.263 -0.087 -0.859 1.031 0.498 1501 211 pi+ 91 1257 0 0 0 0 0 -0.191 0.227 -1.932 1.959 0.140 1502 -211 pi- 91 1257 0 0 0 0 0 0.071 -0.284 -0.493 0.590 0.140 1503 211 pi+ 91 1259 0 0 0 0 0 -0.333 -0.216 -0.793 0.897 0.140 1504 111 (pi0) -91 1259 0 1820 1821 0 0 -0.085 -0.600 -4.980 5.019 0.135 1505 211 pi+ 91 1260 0 0 0 0 0 0.206 -0.279 -1.242 1.297 0.140 1506 -211 pi- 91 1260 0 0 0 0 0 -0.398 -1.128 -3.366 3.575 0.140 1507 -211 pi- 91 1261 0 0 0 0 0 -0.307 -0.124 -1.099 1.156 0.140 1508 111 (pi0) -91 1261 0 1822 1823 0 0 0.311 -0.761 -1.001 1.302 0.135 1509 211 pi+ 91 1264 0 0 0 0 0 0.242 -0.050 0.025 0.285 0.140 1510 111 (pi0) -91 1264 0 1824 1825 0 0 0.135 -0.048 -2.262 2.271 0.135 1511 -211 pi- 91 1265 0 0 0 0 0 -0.311 -0.526 -1.928 2.027 0.140 1512 111 (pi0) -91 1265 0 1826 1827 0 0 -0.063 0.144 -0.457 0.502 0.135 1513 211 pi+ 91 1266 0 0 0 0 0 0.459 -0.109 -0.987 1.103 0.140 1514 -211 pi- 91 1266 0 0 0 0 0 -0.041 0.390 -0.661 0.782 0.140 1515 321 K+ 91 1268 0 0 0 0 0 -0.108 -0.208 -1.079 1.210 0.494 1516 -211 pi- 91 1268 0 0 0 0 0 -0.107 0.099 0.049 0.208 0.140 1517 130 K_L0 91 1275 1275 0 0 0 0 -0.200 -0.366 0.157 0.668 0.498 1518 211 pi+ 91 1280 0 0 0 0 0 0.022 0.074 0.561 0.583 0.140 1519 -211 pi- 91 1280 0 0 0 0 0 1.145 -0.694 2.663 2.984 0.140 1520 311 (K0) -91 1287 0 1589 1589 0 0 0.098 -0.068 6.101 6.122 0.498 1521 211 pi+ 91 1287 0 0 0 0 0 -0.279 -0.220 12.673 12.679 0.140 1522 211 pi+ 91 1293 0 0 0 0 0 0.053 0.009 178.407 178.407 0.140 1523 -211 pi- 91 1293 0 0 0 0 0 -0.299 -0.023 39.362 39.364 0.140 1524 -2112 nbar0 91 1294 0 0 0 0 0 -1.168 0.096 409.075 409.078 0.940 1525 111 (pi0) -91 1294 0 1828 1829 0 0 -0.595 -0.652 233.222 233.224 0.135 1526 -211 pi- 91 1295 0 0 0 0 0 -0.419 -0.182 64.168 64.170 0.140 1527 111 (pi0) -91 1295 0 1830 1831 0 0 0.050 -0.304 174.493 174.494 0.135 1528 211 pi+ 91 1297 0 0 0 0 0 0.093 0.035 3.769 3.772 0.140 1529 111 (pi0) -91 1297 0 1832 1833 0 0 -0.433 -0.470 40.570 40.575 0.135 1530 -211 pi- 91 1298 0 0 0 0 0 -0.354 -0.244 57.127 57.129 0.140 1531 111 (pi0) -91 1298 0 1834 1835 0 0 0.049 -0.562 13.842 13.854 0.135 1532 211 pi+ 91 1299 0 0 0 0 0 -0.142 -0.611 13.869 13.883 0.140 1533 111 (pi0) -91 1299 0 1836 1837 0 0 -0.144 -0.643 45.974 45.979 0.135 1534 211 pi+ 91 1300 0 0 0 0 0 -0.743 -0.025 40.588 40.595 0.140 1535 -211 pi- 91 1300 0 0 0 0 0 -0.361 -0.268 8.537 8.550 0.140 1536 -321 K- 91 1311 0 0 0 0 0 0.510 1.121 27.383 27.415 0.494 1537 211 pi+ 91 1311 0 0 0 0 0 0.207 1.426 24.730 24.772 0.140 1538 211 pi+ 91 1313 0 0 0 0 0 -0.059 -0.248 6.594 6.600 0.140 1539 -211 pi- 91 1313 0 0 0 0 0 -0.773 0.105 3.756 3.839 0.140 1540 -211 pi- 91 1314 0 0 0 0 0 -0.544 -0.236 4.206 4.249 0.140 1541 111 (pi0) -91 1314 0 1838 1839 0 0 -0.603 0.568 5.246 5.313 0.135 1542 211 pi+ 91 1316 0 0 0 0 0 -0.574 -0.328 1.719 1.847 0.140 1543 -211 pi- 91 1316 0 0 0 0 0 0.222 -0.108 2.002 2.022 0.140 1544 130 K_L0 91 1317 1317 0 0 0 0 -1.197 1.409 5.501 5.825 0.498 1545 -311 (Kbar0) -91 1318 0 1590 1590 0 0 -0.534 1.735 4.201 4.603 0.498 1546 111 (pi0) -91 1318 0 1840 1841 0 0 -0.884 0.663 2.342 2.593 0.135 1547 211 pi+ 91 1324 0 0 0 0 0 0.046 -0.048 -2.366 2.371 0.140 1548 -211 pi- 91 1324 0 0 0 0 0 -0.433 0.112 -0.914 1.027 0.140 1549 211 pi+ 91 1326 0 0 0 0 0 0.013 -0.517 -1.307 1.412 0.140 1550 111 (pi0) -91 1326 0 1842 1843 0 0 -0.059 0.314 -0.732 0.810 0.135 1551 211 pi+ 91 1327 0 0 0 0 0 0.028 -0.094 -0.202 0.265 0.140 1552 -211 pi- 91 1327 0 0 0 0 0 -0.153 0.753 -3.202 3.295 0.140 1553 -211 pi- 91 1328 0 0 0 0 0 0.386 -0.891 -31.983 31.998 0.140 1554 111 (pi0) -91 1328 0 1844 1845 0 0 -0.062 0.078 -23.446 23.447 0.135 1555 211 pi+ 91 1329 0 0 0 0 0 -0.634 0.096 -35.688 35.694 0.140 1556 -211 pi- 91 1329 0 0 0 0 0 -0.040 0.324 -11.459 11.464 0.140 1557 -211 pi- 91 1356 0 0 0 0 0 -1.080 -0.055 -36.471 36.487 0.140 1558 111 (pi0) -91 1356 0 1846 1847 0 0 -0.241 -0.745 -32.061 32.071 0.135 1559 311 (K0) -91 1360 0 1591 1591 0 0 1.927 0.149 -135.532 135.547 0.498 1560 211 pi+ 91 1360 0 0 0 0 0 0.405 -0.278 -27.759 27.764 0.140 1561 310 (K_S0) -91 1361 1361 1848 1849 0 0 0.203 -0.046 -18.445 18.453 0.498 1562 211 pi+ 91 1364 0 0 0 0 0 0.131 0.091 -3.984 3.989 0.140 1563 111 (pi0) -91 1364 0 1850 1851 0 0 0.402 -0.095 -19.096 19.101 0.135 1564 -211 pi- 91 1366 0 0 0 0 0 -1.130 0.714 -7.999 8.111 0.140 1565 111 (pi0) -91 1366 0 1852 1853 0 0 -0.038 0.006 -2.624 2.628 0.135 1566 130 K_L0 91 1368 1368 0 0 0 0 -0.309 0.274 -2.384 2.471 0.498 1567 211 pi+ 91 1369 0 0 0 0 0 0.329 0.220 -2.239 2.278 0.140 1568 -211 pi- 91 1369 0 0 0 0 0 -0.285 0.118 -1.111 1.162 0.140 1569 311 (K0) -91 1372 0 1592 1592 0 0 -0.404 -0.406 0.227 0.792 0.498 1570 211 pi+ 91 1372 0 0 0 0 0 -0.165 0.039 -0.239 0.325 0.140 1571 -311 (Kbar0) -91 1373 0 1593 1593 0 0 -0.150 -0.526 -0.768 1.066 0.498 1572 -211 pi- 91 1373 0 0 0 0 0 0.158 0.057 -0.613 0.650 0.140 1573 211 pi+ 91 1374 0 0 0 0 0 -0.472 0.747 -0.214 0.920 0.140 1574 111 (pi0) -91 1374 0 1854 1855 0 0 0.171 -0.054 -0.187 0.292 0.135 1575 2112 n0 91 1381 0 0 0 0 0 0.259 -0.443 4.185 4.320 0.940 1576 111 (pi0) -91 1381 0 1856 1857 0 0 0.132 0.113 1.087 1.109 0.135 1577 211 pi+ 91 1388 0 0 0 0 0 0.070 -0.217 12.705 12.708 0.140 1578 -211 pi- 91 1388 0 0 0 0 0 0.473 0.269 116.326 116.328 0.140 1579 211 pi+ 91 1390 0 0 0 0 0 -0.694 -2.417 544.040 544.045 0.140 1580 -211 pi- 91 1390 0 0 0 0 0 -0.098 -0.042 13.155 13.156 0.140 1581 310 (K_S0) -91 1403 1403 1858 1859 0 0 -0.173 0.218 -0.018 0.570 0.498 1582 310 (K_S0) -91 1411 1411 1860 1861 0 0 0.159 0.617 -8.444 8.482 0.498 1583 130 K_L0 91 1419 1419 0 0 0 0 0.530 -0.160 -262.679 262.680 0.498 1584 310 (K_S0) -91 1441 1441 1862 1863 0 0 -0.200 -0.274 -6.741 6.768 0.498 1585 310 (K_S0) -91 1475 1475 1864 1865 0 0 -0.024 -0.249 -2.900 2.953 0.498 1586 310 (K_S0) -91 1477 1477 1866 1867 0 0 0.316 0.129 0.222 0.643 0.498 1587 130 K_L0 91 1479 1479 0 0 0 0 0.189 -0.205 0.442 0.722 0.498 1588 130 K_L0 91 1488 1488 0 0 0 0 0.421 -0.001 -24.030 24.039 0.498 1589 130 K_L0 91 1520 1520 0 0 0 0 0.098 -0.068 6.101 6.122 0.498 1590 310 (K_S0) -91 1545 1545 1868 1869 0 0 -0.534 1.735 4.201 4.603 0.498 1591 130 K_L0 91 1559 1559 0 0 0 0 1.927 0.149 -135.532 135.547 0.498 1592 130 K_L0 91 1569 1569 0 0 0 0 -0.404 -0.406 0.227 0.792 0.498 1593 130 K_L0 91 1571 1571 0 0 0 0 -0.150 -0.526 -0.768 1.066 0.498 1594 421 (D0) -91 974 0 1870 1871 0 0 0.723 -2.435 33.026 33.176 1.865 1595 211 pi+ 91 974 0 0 0 0 0 0.024 -0.205 2.381 2.394 0.140 1596 22 gamma 91 979 0 0 0 0 0 0.228 0.515 29.336 29.342 0.000 1597 22 gamma 91 979 0 0 0 0 0 0.113 0.139 6.708 6.711 0.000 1598 -421 (Dbar0) -91 980 0 1872 1874 0 0 -0.282 0.034 96.388 96.406 1.865 1599 111 (pi0) -91 980 0 1875 1876 0 0 0.019 -0.021 6.860 6.862 0.135 1600 511 (B0) -91 985 0 1877 1879 0 0 16.927 20.219 -23.620 35.793 5.280 1601 22 gamma 91 985 0 0 0 0 0 0.071 0.117 -0.173 0.220 0.000 1602 22 gamma 91 992 0 0 0 0 0 -0.050 0.071 0.045 0.098 0.000 1603 22 gamma 91 992 0 0 0 0 0 -0.031 0.475 0.474 0.672 0.000 1604 22 gamma 91 993 0 0 0 0 0 0.187 0.616 0.152 0.662 0.000 1605 22 gamma 91 993 0 0 0 0 0 -0.008 0.266 0.055 0.272 0.000 1606 22 gamma 91 994 0 0 0 0 0 0.037 0.100 0.274 0.294 0.000 1607 22 gamma 91 994 0 0 0 0 0 0.066 0.095 0.066 0.133 0.000 1608 211 pi+ 91 997 0 0 0 0 0 0.135 -0.334 -0.465 0.604 0.140 1609 -211 pi- 91 997 0 0 0 0 0 -0.010 -0.012 -0.215 0.257 0.140 1610 111 (pi0) -91 997 0 1880 1881 0 0 -0.007 0.162 -0.071 0.222 0.135 1611 22 gamma 91 998 0 0 0 0 0 0.552 -0.092 -0.470 0.730 0.000 1612 22 gamma 91 998 0 0 0 0 0 0.426 -0.194 -0.412 0.623 0.000 1613 22 gamma 91 1013 0 0 0 0 0 0.446 0.487 53.265 53.269 0.000 1614 22 gamma 91 1013 0 0 0 0 0 0.149 0.301 25.804 25.806 0.000 1615 22 gamma 91 1028 0 0 0 0 0 0.537 -0.506 -1.601 1.763 0.000 1616 22 gamma 91 1028 0 0 0 0 0 0.076 -0.126 -0.444 0.468 0.000 1617 211 pi+ 91 1029 0 0 0 0 0 -0.001 0.192 -5.183 5.188 0.140 1618 -211 pi- 91 1029 0 0 0 0 0 -0.127 0.180 -17.945 17.947 0.140 1619 111 (pi0) -91 1029 0 1882 1883 0 0 -0.483 0.283 -14.454 14.466 0.135 1620 22 gamma 91 1031 0 0 0 0 0 -0.085 0.164 -7.135 7.137 0.000 1621 22 gamma 91 1031 0 0 0 0 0 -0.699 1.981 -95.785 95.808 0.000 1622 211 pi+ 91 1040 0 0 0 0 0 0.092 -0.346 31.053 31.055 0.140 1623 -211 pi- 91 1040 0 0 0 0 0 -0.116 -0.251 19.581 19.584 0.140 1624 221 (eta) -91 1040 0 1884 1886 0 0 -0.238 -0.484 55.176 55.181 0.548 1625 211 pi+ 91 1041 0 0 0 0 0 0.158 0.213 11.297 11.300 0.140 1626 -211 pi- 91 1041 0 0 0 0 0 -0.153 0.143 2.805 2.816 0.140 1627 111 (pi0) -91 1041 0 1887 1888 0 0 -0.139 0.310 11.656 11.661 0.135 1628 22 gamma 91 1044 0 0 0 0 0 0.158 0.112 0.427 0.469 0.000 1629 22 gamma 91 1044 0 0 0 0 0 0.105 0.266 0.594 0.659 0.000 1630 22 gamma 91 1052 0 0 0 0 0 -0.007 -0.040 -7.272 7.272 0.000 1631 22 gamma 91 1052 0 0 0 0 0 0.162 0.009 -50.989 50.990 0.000 1632 211 pi+ 91 1053 0 0 0 0 0 0.115 -0.235 -156.952 156.952 0.140 1633 -211 pi- 91 1053 0 0 0 0 0 0.111 0.124 -47.666 47.666 0.140 1634 111 (pi0) -91 1053 0 1889 1890 0 0 0.288 -0.053 -261.031 261.032 0.135 1635 321 K+ 91 1056 0 0 0 0 0 0.115 0.067 -6.759 6.778 0.494 1636 -321 K- 91 1056 0 0 0 0 0 -0.048 -0.137 -6.649 6.669 0.494 1637 111 (pi0) -91 1058 0 1891 1892 0 0 0.144 -0.313 -0.615 0.717 0.135 1638 111 (pi0) -91 1058 0 1893 1894 0 0 -0.024 -0.369 -0.605 0.722 0.135 1639 111 (pi0) -91 1058 0 1895 1896 0 0 -0.052 -0.219 -0.198 0.329 0.135 1640 22 gamma 91 1059 0 0 0 0 0 0.042 0.088 -0.334 0.347 0.000 1641 22 gamma 91 1059 0 0 0 0 0 0.519 0.341 -1.949 2.046 0.000 1642 22 gamma 91 1060 0 0 0 0 0 0.498 -0.734 -1.128 1.435 0.000 1643 22 gamma 91 1060 0 0 0 0 0 0.207 0.057 -0.135 0.253 0.000 1644 -313 (K*bar0) -91 1068 0 1897 1898 0 0 1.211 0.890 5.134 5.423 0.888 1645 111 (pi0) -91 1068 0 1899 1900 0 0 0.165 0.257 5.931 5.941 0.135 1646 211 pi+ 91 1076 0 0 0 0 0 -0.418 -0.134 -4.338 4.362 0.140 1647 -211 pi- 91 1076 0 0 0 0 0 -0.353 -0.595 -8.069 8.100 0.140 1648 111 (pi0) -91 1076 0 1901 1902 0 0 -0.021 -0.281 -4.912 4.922 0.135 1649 -511 (Bbar0) -91 1088 0 1903 1905 0 0 -14.919 -36.745 -123.301 129.630 5.280 1650 22 gamma 91 1088 0 0 0 0 0 -0.182 -0.375 -1.174 1.245 0.000 1651 111 (pi0) -91 1095 0 1906 1907 0 0 -0.141 -0.107 -1.925 1.938 0.135 1652 22 gamma 91 1095 0 0 0 0 0 -0.638 -1.491 -5.348 5.588 0.000 1653 211 pi+ 91 1125 0 0 0 0 0 0.107 -0.231 0.000 0.290 0.140 1654 -211 pi- 91 1125 0 0 0 0 0 -0.138 -0.063 0.399 0.449 0.140 1655 111 (pi0) -91 1125 0 1908 1909 0 0 -0.040 0.012 0.360 0.386 0.135 1656 22 gamma 91 1128 0 0 0 0 0 -0.134 -0.154 2.112 2.122 0.000 1657 22 gamma 91 1128 0 0 0 0 0 0.019 -0.116 1.477 1.482 0.000 1658 -2212 pbar- 91 1129 0 0 0 0 0 -0.294 0.902 13.111 13.179 0.938 1659 211 pi+ 91 1129 0 0 0 0 0 -0.101 0.253 2.165 2.187 0.140 1660 22 gamma 91 1134 0 0 0 0 0 0.193 0.274 4.501 4.513 0.000 1661 22 gamma 91 1134 0 0 0 0 0 0.052 -0.005 0.578 0.581 0.000 1662 22 gamma 91 1138 0 0 0 0 0 -0.051 -0.031 0.294 0.300 0.000 1663 22 gamma 91 1138 0 0 0 0 0 -0.078 -0.071 2.461 2.463 0.000 1664 22 gamma 91 1144 0 0 0 0 0 0.183 0.122 0.160 0.272 0.000 1665 22 gamma 91 1144 0 0 0 0 0 0.252 0.305 0.131 0.417 0.000 1666 211 pi+ 91 1146 0 0 0 0 0 0.170 0.265 -0.486 0.596 0.140 1667 -211 pi- 91 1146 0 0 0 0 0 -0.311 0.014 0.068 0.348 0.140 1668 22 gamma 91 1149 0 0 0 0 0 -0.203 -0.080 -0.622 0.659 0.000 1669 22 gamma 91 1149 0 0 0 0 0 -0.465 -0.425 -1.758 1.868 0.000 1670 22 gamma 91 1150 0 0 0 0 0 0.034 -0.073 -0.379 0.387 0.000 1671 22 gamma 91 1150 0 0 0 0 0 0.243 -0.060 -1.762 1.779 0.000 1672 22 gamma 91 1155 0 0 0 0 0 0.038 -0.071 -0.610 0.615 0.000 1673 22 gamma 91 1155 0 0 0 0 0 0.035 0.053 -1.034 1.036 0.000 1674 22 gamma 91 1157 0 0 0 0 0 0.144 -0.008 -1.075 1.085 0.000 1675 22 gamma 91 1157 0 0 0 0 0 0.071 0.067 -1.617 1.620 0.000 1676 111 (pi0) -91 1161 0 1910 1911 0 0 0.055 -0.023 -2.262 2.267 0.135 1677 111 (pi0) -91 1161 0 1912 1913 0 0 -0.090 0.097 -2.676 2.683 0.135 1678 111 (pi0) -91 1161 0 1914 1915 0 0 -0.133 -0.092 -1.652 1.666 0.135 1679 22 gamma 91 1162 0 0 0 0 0 -0.101 0.040 -1.282 1.286 0.000 1680 22 gamma 91 1162 0 0 0 0 0 -0.229 -0.110 -2.555 2.568 0.000 1681 22 gamma 91 1176 0 0 0 0 0 0.062 0.093 -17.890 17.890 0.000 1682 22 gamma 91 1176 0 0 0 0 0 0.007 0.116 -51.229 51.229 0.000 1683 22 gamma 91 1190 0 0 0 0 0 0.053 -0.058 0.075 0.109 0.000 1684 22 gamma 91 1190 0 0 0 0 0 0.181 -0.170 0.715 0.757 0.000 1685 -313 (K*bar0) -91 1192 0 1916 1917 0 0 1.033 0.214 0.479 1.458 0.884 1686 -211 pi- 91 1192 0 0 0 0 0 -0.230 -0.477 1.018 1.156 0.140 1687 22 gamma 91 1197 0 0 0 0 0 0.023 -0.014 1.015 1.015 0.000 1688 22 gamma 91 1197 0 0 0 0 0 0.182 0.109 30.927 30.927 0.000 1689 22 gamma 91 1201 0 0 0 0 0 -0.256 0.174 1.506 1.537 0.000 1690 22 gamma 91 1201 0 0 0 0 0 -0.172 0.008 1.052 1.066 0.000 1691 130 K_L0 91 1204 0 0 0 0 0 -0.092 -0.237 -0.470 0.730 0.498 1692 310 (K_S0) -91 1204 0 1918 1919 0 0 0.050 -0.303 -0.310 0.662 0.498 1693 211 pi+ 91 1208 0 0 0 0 0 -0.134 -0.180 -3.986 3.995 0.140 1694 -211 pi- 91 1208 0 0 0 0 0 -0.101 -0.169 -7.083 7.087 0.140 1695 111 (pi0) -91 1208 0 1920 1921 0 0 -0.045 0.240 -3.443 3.454 0.135 1696 -2112 nbar0 91 1216 0 0 0 0 0 0.105 -0.282 15.945 15.976 0.940 1697 211 pi+ 91 1216 0 0 0 0 0 0.029 -0.206 1.847 1.864 0.140 1698 22 gamma 91 1222 0 0 0 0 0 0.391 -0.128 201.005 201.006 0.000 1699 22 gamma 91 1222 0 0 0 0 0 0.233 0.028 111.887 111.887 0.000 1700 22 gamma 91 1255 0 0 0 0 0 0.016 -0.026 -0.175 0.178 0.000 1701 22 gamma 91 1255 0 0 0 0 0 0.126 -0.065 -0.108 0.178 0.000 1702 211 pi+ 91 1256 0 0 0 0 0 -0.029 -0.114 -0.205 0.274 0.140 1703 -211 pi- 91 1256 0 0 0 0 0 0.012 -0.127 -1.337 1.350 0.140 1704 111 (pi0) -91 1256 0 1922 1923 0 0 0.005 0.171 -1.423 1.439 0.135 1705 22 gamma 91 1273 0 0 0 0 0 -0.104 -0.487 -0.436 0.662 0.000 1706 22 gamma 91 1273 0 0 0 0 0 0.027 -0.053 -0.090 0.108 0.000 1707 22 gamma 91 1274 0 0 0 0 0 -0.683 -0.448 0.161 0.832 0.000 1708 22 gamma 91 1274 0 0 0 0 0 -0.436 -0.414 0.163 0.623 0.000 1709 2212 p+ 91 1276 0 0 0 0 0 -2.001 -0.105 -0.267 2.229 0.938 1710 -211 pi- 91 1276 0 0 0 0 0 -0.379 -0.003 0.068 0.410 0.140 1711 22 gamma 91 1277 0 0 0 0 0 -0.244 -0.342 0.503 0.655 0.000 1712 22 gamma 91 1277 0 0 0 0 0 -0.027 -0.163 0.141 0.217 0.000 1713 22 gamma 91 1281 0 0 0 0 0 0.202 -0.004 0.375 0.426 0.000 1714 22 gamma 91 1281 0 0 0 0 0 0.085 -0.033 0.440 0.450 0.000 1715 211 pi+ 91 1285 0 0 0 0 0 -0.007 -0.041 3.287 3.290 0.140 1716 -211 pi- 91 1285 0 0 0 0 0 -0.078 -0.074 1.903 1.911 0.140 1717 111 (pi0) -91 1285 0 1924 1925 0 0 0.561 -0.075 6.166 6.193 0.135 1718 22 gamma 91 1290 0 0 0 0 0 -0.061 -0.163 8.305 8.307 0.000 1719 22 gamma 91 1290 0 0 0 0 0 -0.030 -0.103 1.969 1.972 0.000 1720 211 pi+ 91 1296 0 0 0 0 0 -0.421 0.244 37.148 37.152 0.140 1721 -211 pi- 91 1296 0 0 0 0 0 -0.902 -0.051 72.825 72.831 0.140 1722 111 (pi0) -91 1296 0 1926 1927 0 0 -0.331 -0.198 32.945 32.947 0.135 1723 22 gamma 91 1301 0 0 0 0 0 -0.034 -0.114 1.143 1.149 0.000 1724 22 gamma 91 1301 0 0 0 0 0 0.029 -0.067 2.331 2.332 0.000 1725 22 gamma 91 1312 0 0 0 0 0 -0.003 0.006 0.291 0.291 0.000 1726 22 gamma 91 1312 0 0 0 0 0 0.443 1.067 15.199 15.243 0.000 1727 211 pi+ 91 1322 0 0 0 0 0 -0.115 0.012 0.327 0.373 0.140 1728 -211 pi- 91 1322 0 0 0 0 0 0.178 0.101 0.282 0.376 0.140 1729 111 (pi0) -91 1322 0 1928 1929 0 0 -0.033 0.506 0.896 1.038 0.135 1730 22 gamma 91 1325 0 0 0 0 0 0.070 0.016 -0.021 0.075 0.000 1731 22 gamma 91 1325 0 0 0 0 0 -0.060 0.044 -0.002 0.075 0.000 1732 22 gamma 91 1357 0 0 0 0 0 -1.376 -0.224 -62.244 62.260 0.000 1733 22 gamma 91 1357 0 0 0 0 0 -0.548 -0.106 -21.466 21.473 0.000 1734 211 pi+ 91 1358 0 0 0 0 0 -0.132 -0.298 -5.146 5.158 0.140 1735 -211 pi- 91 1358 0 0 0 0 0 -0.100 -0.055 -5.121 5.125 0.140 1736 111 (pi0) -91 1358 0 1930 1931 0 0 -0.066 -0.100 -1.739 1.748 0.135 1737 22 gamma 91 1359 0 0 0 0 0 0.608 -0.028 -29.783 29.789 0.000 1738 22 gamma 91 1359 0 0 0 0 0 0.538 0.048 -21.793 21.799 0.000 1739 22 gamma 91 1362 0 0 0 0 0 0.234 -0.122 -29.282 29.283 0.000 1740 22 gamma 91 1362 0 0 0 0 0 0.419 -0.031 -45.259 45.261 0.000 1741 22 gamma 91 1365 0 0 0 0 0 0.136 -0.173 -10.411 10.414 0.000 1742 22 gamma 91 1365 0 0 0 0 0 0.316 -0.143 -14.882 14.886 0.000 1743 211 pi+ 91 1371 0 0 0 0 0 -0.184 0.118 -0.618 0.670 0.140 1744 -211 pi- 91 1371 0 0 0 0 0 0.337 0.136 -0.628 0.738 0.140 1745 111 (pi0) -91 1371 0 1932 1933 0 0 0.162 0.175 -0.749 0.797 0.135 1746 22 gamma 91 1377 0 0 0 0 0 0.056 -0.024 0.217 0.225 0.000 1747 22 gamma 91 1377 0 0 0 0 0 -0.004 0.062 0.046 0.077 0.000 1748 22 gamma 91 1380 0 0 0 0 0 0.053 0.022 0.571 0.574 0.000 1749 22 gamma 91 1380 0 0 0 0 0 -0.080 0.035 1.447 1.450 0.000 1750 22 gamma 91 1382 0 0 0 0 0 0.042 0.319 1.421 1.457 0.000 1751 22 gamma 91 1382 0 0 0 0 0 0.008 0.169 1.325 1.336 0.000 1752 22 gamma 91 1384 0 0 0 0 0 1.406 -0.215 90.642 90.653 0.000 1753 22 gamma 91 1384 0 0 0 0 0 0.012 0.011 1.330 1.330 0.000 1754 22 gamma 91 1386 0 0 0 0 0 0.399 0.099 23.405 23.409 0.000 1755 22 gamma 91 1386 0 0 0 0 0 0.029 0.055 2.998 2.998 0.000 1756 111 (pi0) -91 1389 0 1934 1935 0 0 0.083 -0.087 5.988 5.991 0.135 1757 22 gamma 91 1389 0 0 0 0 0 0.714 0.194 121.200 121.202 0.000 1758 111 (pi0) -91 1391 0 1936 1937 0 0 0.025 0.103 3.997 4.001 0.135 1759 111 (pi0) -91 1391 0 1938 1939 0 0 -0.046 0.642 5.782 5.820 0.135 1760 22 gamma 91 1393 0 0 0 0 0 0.077 -0.046 0.061 0.108 0.000 1761 22 gamma 91 1393 0 0 0 0 0 0.052 -0.112 0.333 0.356 0.000 1762 22 gamma 91 1395 0 0 0 0 0 0.166 0.264 -0.040 0.315 0.000 1763 22 gamma 91 1395 0 0 0 0 0 0.063 0.326 -0.110 0.350 0.000 1764 22 gamma 91 1397 0 0 0 0 0 0.295 0.145 -0.080 0.338 0.000 1765 22 gamma 91 1397 0 0 0 0 0 0.124 -0.003 0.028 0.127 0.000 1766 111 (pi0) -91 1399 0 1940 1941 0 0 0.150 0.855 0.881 1.244 0.135 1767 111 (pi0) -91 1399 0 1942 1943 0 0 -0.058 0.289 0.082 0.334 0.135 1768 22 gamma 91 1408 0 0 0 0 0 0.249 0.556 -13.173 13.187 0.000 1769 22 gamma 91 1408 0 0 0 0 0 0.298 0.731 -20.666 20.681 0.000 1770 22 gamma 91 1414 0 0 0 0 0 -0.041 -0.018 2.578 2.578 0.000 1771 22 gamma 91 1414 0 0 0 0 0 -0.252 -0.013 4.585 4.592 0.000 1772 22 gamma 91 1416 0 0 0 0 0 0.053 0.152 0.678 0.697 0.000 1773 22 gamma 91 1416 0 0 0 0 0 -0.035 0.195 1.464 1.477 0.000 1774 22 gamma 91 1418 0 0 0 0 0 0.143 0.702 0.270 0.766 0.000 1775 22 gamma 91 1418 0 0 0 0 0 0.127 0.230 0.077 0.274 0.000 1776 22 gamma 91 1420 0 0 0 0 0 -0.137 -0.033 -40.361 40.361 0.000 1777 22 gamma 91 1420 0 0 0 0 0 -0.030 -0.021 -54.565 54.565 0.000 1778 211 pi+ 91 1423 0 0 0 0 0 0.137 -0.295 -2.598 2.622 0.140 1779 -211 pi- 91 1423 0 0 0 0 0 0.042 0.135 -1.401 1.415 0.140 1780 22 gamma 91 1425 0 0 0 0 0 0.364 -0.272 2.053 2.102 0.000 1781 22 gamma 91 1425 0 0 0 0 0 0.006 0.007 0.008 0.012 0.000 1782 22 gamma 91 1431 0 0 0 0 0 0.488 0.240 0.298 0.619 0.000 1783 22 gamma 91 1431 0 0 0 0 0 0.065 0.087 0.025 0.111 0.000 1784 22 gamma 91 1433 0 0 0 0 0 -0.028 -0.160 -0.223 0.276 0.000 1785 22 gamma 91 1433 0 0 0 0 0 0.123 -0.240 -0.430 0.508 0.000 1786 211 pi+ 91 1438 0 0 0 0 0 -1.513 -1.678 -9.066 9.345 0.140 1787 -211 pi- 91 1438 0 0 0 0 0 -1.091 -1.647 -6.964 7.240 0.140 1788 22 gamma 91 1440 0 0 0 0 0 -0.215 -0.901 -4.735 4.825 0.000 1789 22 gamma 91 1440 0 0 0 0 0 -0.018 -0.087 -0.280 0.294 0.000 1790 22 gamma 91 1447 0 0 0 0 0 0.110 0.227 -100.954 100.955 0.000 1791 22 gamma 91 1447 0 0 0 0 0 0.039 0.034 -7.227 7.227 0.000 1792 22 gamma 91 1449 0 0 0 0 0 -0.054 -0.211 -68.295 68.296 0.000 1793 22 gamma 91 1449 0 0 0 0 0 0.035 -0.028 -6.223 6.223 0.000 1794 22 gamma 91 1451 0 0 0 0 0 0.091 0.586 -0.537 0.800 0.000 1795 22 gamma 91 1451 0 0 0 0 0 0.029 0.146 -0.242 0.284 0.000 1796 22 gamma 91 1456 0 0 0 0 0 -0.165 -0.254 1.223 1.260 0.000 1797 22 gamma 91 1456 0 0 0 0 0 0.006 -0.158 0.726 0.743 0.000 1798 22 gamma 91 1458 0 0 0 0 0 -0.295 -0.296 1.451 1.510 0.000 1799 22 gamma 91 1458 0 0 0 0 0 -0.153 -0.046 0.669 0.688 0.000 1800 22 gamma 91 1462 0 0 0 0 0 0.041 0.038 -2.312 2.313 0.000 1801 22 gamma 91 1462 0 0 0 0 0 0.042 0.150 -1.827 1.834 0.000 1802 22 gamma 91 1464 0 0 0 0 0 -0.062 0.080 -0.188 0.214 0.000 1803 22 gamma 91 1464 0 0 0 0 0 -0.051 0.198 -0.918 0.941 0.000 1804 22 gamma 91 1466 0 0 0 0 0 0.258 0.384 -145.421 145.422 0.000 1805 22 gamma 91 1466 0 0 0 0 0 0.243 0.500 -139.309 139.310 0.000 1806 22 gamma 91 1470 0 0 0 0 0 0.053 -0.018 -7.032 7.033 0.000 1807 22 gamma 91 1470 0 0 0 0 0 0.006 -0.112 -4.208 4.209 0.000 1808 22 gamma 91 1472 0 0 0 0 0 -0.377 0.063 -12.343 12.349 0.000 1809 22 gamma 91 1472 0 0 0 0 0 -0.009 0.012 -2.111 2.111 0.000 1810 22 gamma 91 1484 0 0 0 0 0 -0.097 -0.004 0.668 0.675 0.000 1811 22 gamma 91 1484 0 0 0 0 0 -0.107 0.085 2.314 2.318 0.000 1812 22 gamma 91 1486 0 0 0 0 0 0.151 0.028 0.538 0.560 0.000 1813 22 gamma 91 1486 0 0 0 0 0 0.059 0.116 0.316 0.342 0.000 1814 22 gamma 91 1489 0 0 0 0 0 0.114 -0.368 -7.207 7.217 0.000 1815 22 gamma 91 1489 0 0 0 0 0 0.069 -0.041 -2.006 2.008 0.000 1816 22 gamma 91 1493 0 0 0 0 0 -0.216 0.002 -0.876 0.902 0.000 1817 22 gamma 91 1493 0 0 0 0 0 0.003 0.025 -0.032 0.040 0.000 1818 22 gamma 91 1499 0 0 0 0 0 -0.106 -0.153 23.046 23.046 0.000 1819 22 gamma 91 1499 0 0 0 0 0 -0.086 -0.199 50.335 50.335 0.000 1820 22 gamma 91 1504 0 0 0 0 0 0.002 -0.303 -2.878 2.894 0.000 1821 22 gamma 91 1504 0 0 0 0 0 -0.087 -0.297 -2.102 2.125 0.000 1822 22 gamma 91 1508 0 0 0 0 0 0.052 -0.207 -0.184 0.281 0.000 1823 22 gamma 91 1508 0 0 0 0 0 0.259 -0.554 -0.817 1.021 0.000 1824 22 gamma 91 1510 0 0 0 0 0 0.083 -0.083 -0.973 0.980 0.000 1825 22 gamma 91 1510 0 0 0 0 0 0.052 0.035 -1.289 1.290 0.000 1826 22 gamma 91 1512 0 0 0 0 0 -0.082 0.133 -0.455 0.481 0.000 1827 22 gamma 91 1512 0 0 0 0 0 0.018 0.011 -0.002 0.021 0.000 1828 22 gamma 91 1525 0 0 0 0 0 -0.209 -0.328 99.385 99.385 0.000 1829 22 gamma 91 1525 0 0 0 0 0 -0.386 -0.324 133.838 133.839 0.000 1830 22 gamma 91 1527 0 0 0 0 0 -0.008 0.006 19.477 19.477 0.000 1831 22 gamma 91 1527 0 0 0 0 0 0.058 -0.311 155.016 155.017 0.000 1832 22 gamma 91 1529 0 0 0 0 0 -0.174 -0.284 19.432 19.435 0.000 1833 22 gamma 91 1529 0 0 0 0 0 -0.259 -0.187 21.138 21.140 0.000 1834 22 gamma 91 1531 0 0 0 0 0 -0.040 -0.209 4.442 4.447 0.000 1835 22 gamma 91 1531 0 0 0 0 0 0.090 -0.352 9.400 9.407 0.000 1836 22 gamma 91 1533 0 0 0 0 0 -0.102 -0.185 13.105 13.107 0.000 1837 22 gamma 91 1533 0 0 0 0 0 -0.042 -0.458 32.869 32.872 0.000 1838 22 gamma 91 1541 0 0 0 0 0 -0.329 0.395 3.077 3.120 0.000 1839 22 gamma 91 1541 0 0 0 0 0 -0.274 0.173 2.169 2.193 0.000 1840 22 gamma 91 1546 0 0 0 0 0 -0.412 0.329 1.271 1.376 0.000 1841 22 gamma 91 1546 0 0 0 0 0 -0.472 0.334 1.071 1.217 0.000 1842 22 gamma 91 1550 0 0 0 0 0 0.002 0.220 -0.365 0.426 0.000 1843 22 gamma 91 1550 0 0 0 0 0 -0.061 0.094 -0.367 0.384 0.000 1844 22 gamma 91 1554 0 0 0 0 0 -0.096 0.079 -14.173 14.173 0.000 1845 22 gamma 91 1554 0 0 0 0 0 0.033 -0.001 -9.273 9.273 0.000 1846 22 gamma 91 1558 0 0 0 0 0 -0.022 -0.030 -0.759 0.760 0.000 1847 22 gamma 91 1558 0 0 0 0 0 -0.219 -0.715 -31.302 31.310 0.000 1848 211 pi+ 91 1561 0 0 0 0 0 -0.085 0.011 -3.014 3.018 0.140 1849 -211 pi- 91 1561 0 0 0 0 0 0.288 -0.057 -15.431 15.434 0.140 1850 22 gamma 91 1563 0 0 0 0 0 0.412 -0.090 -18.181 18.186 0.000 1851 22 gamma 91 1563 0 0 0 0 0 -0.010 -0.005 -0.916 0.916 0.000 1852 22 gamma 91 1565 0 0 0 0 0 -0.021 0.030 -2.501 2.502 0.000 1853 22 gamma 91 1565 0 0 0 0 0 -0.017 -0.024 -0.123 0.126 0.000 1854 22 gamma 91 1574 0 0 0 0 0 -0.004 0.018 -0.063 0.065 0.000 1855 22 gamma 91 1574 0 0 0 0 0 0.175 -0.072 -0.124 0.227 0.000 1856 22 gamma 91 1576 0 0 0 0 0 0.052 0.128 0.647 0.662 0.000 1857 22 gamma 91 1576 0 0 0 0 0 0.080 -0.015 0.439 0.447 0.000 1858 111 (pi0) -91 1581 0 1944 1945 0 0 0.106 0.098 0.096 0.220 0.135 1859 111 (pi0) -91 1581 0 1946 1947 0 0 -0.278 0.120 -0.114 0.351 0.135 1860 211 pi+ 91 1582 0 0 0 0 0 0.192 0.373 -3.130 3.161 0.140 1861 -211 pi- 91 1582 0 0 0 0 0 -0.033 0.243 -5.314 5.321 0.140 1862 111 (pi0) -91 1584 0 1948 1949 0 0 0.104 -0.169 -3.464 3.472 0.135 1863 111 (pi0) -91 1584 0 1950 1951 0 0 -0.304 -0.105 -3.277 3.295 0.135 1864 211 pi+ 91 1585 0 0 0 0 0 0.023 -0.296 -1.139 1.185 0.140 1865 -211 pi- 91 1585 0 0 0 0 0 -0.047 0.047 -1.761 1.768 0.140 1866 211 pi+ 91 1586 0 0 0 0 0 0.121 0.190 0.283 0.388 0.140 1867 -211 pi- 91 1586 0 0 0 0 0 0.195 -0.061 -0.061 0.255 0.140 1868 211 pi+ 91 1590 0 0 0 0 0 -0.346 0.989 2.888 3.075 0.140 1869 -211 pi- 91 1590 0 0 0 0 0 -0.188 0.745 1.313 1.528 0.140 1870 311 (K0) -91 1594 0 1952 1952 0 0 1.027 -2.272 31.618 31.720 0.498 1871 111 (pi0) -91 1594 0 1953 1954 0 0 -0.304 -0.163 1.408 1.456 0.135 1872 313 (K*0) -91 1598 0 1955 1956 0 0 0.127 0.065 73.744 73.750 0.905 1873 -211 pi- 91 1598 0 0 0 0 0 -0.401 0.215 14.934 14.942 0.140 1874 211 pi+ 91 1598 0 0 0 0 0 -0.008 -0.246 7.709 7.715 0.140 1875 22 gamma 91 1599 0 0 0 0 0 0.042 -0.050 1.718 1.719 0.000 1876 22 gamma 91 1599 0 0 0 0 0 -0.024 0.029 5.143 5.143 0.000 1877 14 nu_mu 91 1600 0 0 0 0 0 1.561 0.744 -1.082 2.040 0.000 1878 -13 mu+ 91 1600 0 0 0 0 0 0.643 1.390 -2.532 2.961 0.106 1879 -413 (D*-) -91 1600 0 1957 1958 0 0 14.723 18.085 -20.006 30.791 2.010 1880 22 gamma 91 1610 0 0 0 0 0 -0.023 0.180 -0.044 0.186 0.000 1881 22 gamma 91 1610 0 0 0 0 0 0.016 -0.018 -0.027 0.036 0.000 1882 22 gamma 91 1619 0 0 0 0 0 -0.246 0.197 -9.249 9.254 0.000 1883 22 gamma 91 1619 0 0 0 0 0 -0.237 0.086 -5.205 5.211 0.000 1884 111 (pi0) -91 1624 0 1959 1960 0 0 -0.096 -0.352 31.382 31.385 0.135 1885 111 (pi0) -91 1624 0 1961 1962 0 0 -0.152 -0.031 12.956 12.957 0.135 1886 111 (pi0) -91 1624 0 1963 1964 0 0 0.009 -0.102 10.838 10.839 0.135 1887 22 gamma 91 1627 0 0 0 0 0 -0.079 0.266 7.616 7.621 0.000 1888 22 gamma 91 1627 0 0 0 0 0 -0.060 0.044 4.040 4.040 0.000 1889 22 gamma 91 1634 0 0 0 0 0 0.218 -0.098 -194.808 194.808 0.000 1890 22 gamma 91 1634 0 0 0 0 0 0.071 0.045 -66.224 66.224 0.000 1891 22 gamma 91 1637 0 0 0 0 0 0.148 -0.306 -0.514 0.616 0.000 1892 22 gamma 91 1637 0 0 0 0 0 -0.004 -0.006 -0.101 0.101 0.000 1893 22 gamma 91 1638 0 0 0 0 0 0.019 -0.307 -0.410 0.512 0.000 1894 22 gamma 91 1638 0 0 0 0 0 -0.043 -0.062 -0.195 0.209 0.000 1895 22 gamma 91 1639 0 0 0 0 0 0.038 -0.109 -0.121 0.168 0.000 1896 22 gamma 91 1639 0 0 0 0 0 -0.090 -0.110 -0.077 0.161 0.000 1897 -311 (Kbar0) -91 1644 0 1965 1965 0 0 1.205 0.793 4.086 4.362 0.498 1898 111 (pi0) -91 1644 0 1966 1967 0 0 0.006 0.097 1.048 1.061 0.135 1899 22 gamma 91 1645 0 0 0 0 0 0.183 0.211 4.595 4.604 0.000 1900 22 gamma 91 1645 0 0 0 0 0 -0.018 0.047 1.336 1.337 0.000 1901 22 gamma 91 1648 0 0 0 0 0 0.026 0.002 -0.432 0.433 0.000 1902 22 gamma 91 1648 0 0 0 0 0 -0.047 -0.283 -4.480 4.489 0.000 1903 4312 (Xi'_c0) -91 1649 0 1968 1969 0 0 -13.005 -28.944 -97.811 102.862 2.578 1904 211 pi+ 91 1649 0 0 0 0 0 -0.819 -4.351 -13.491 14.200 0.140 1905 -2212 pbar- 91 1649 0 0 0 0 0 -1.095 -3.449 -12.000 12.569 0.938 1906 22 gamma 91 1651 0 0 0 0 0 -0.102 -0.128 -1.727 1.735 0.000 1907 22 gamma 91 1651 0 0 0 0 0 -0.040 0.022 -0.197 0.202 0.000 1908 22 gamma 91 1655 0 0 0 0 0 -0.016 -0.060 0.199 0.209 0.000 1909 22 gamma 91 1655 0 0 0 0 0 -0.024 0.072 0.160 0.178 0.000 1910 22 gamma 91 1676 0 0 0 0 0 0.003 -0.025 -0.073 0.077 0.000 1911 22 gamma 91 1676 0 0 0 0 0 0.051 0.002 -2.189 2.190 0.000 1912 22 gamma 91 1677 0 0 0 0 0 -0.092 -0.000 -1.272 1.275 0.000 1913 22 gamma 91 1677 0 0 0 0 0 0.002 0.097 -1.405 1.408 0.000 1914 22 gamma 91 1678 0 0 0 0 0 -0.023 0.034 -0.255 0.258 0.000 1915 22 gamma 91 1678 0 0 0 0 0 -0.110 -0.127 -1.397 1.407 0.000 1916 -311 (Kbar0) -91 1685 0 1970 1970 0 0 0.257 0.030 0.268 0.622 0.498 1917 111 (pi0) -91 1685 0 1971 1972 0 0 0.776 0.184 0.211 0.836 0.135 1918 211 pi+ 91 1692 0 0 0 0 0 0.068 -0.264 0.013 0.307 0.140 1919 -211 pi- 91 1692 0 0 0 0 0 -0.017 -0.038 -0.324 0.355 0.140 1920 22 gamma 91 1695 0 0 0 0 0 -0.042 0.139 -1.164 1.173 0.000 1921 22 gamma 91 1695 0 0 0 0 0 -0.004 0.100 -2.279 2.281 0.000 1922 22 gamma 91 1704 0 0 0 0 0 -0.015 0.135 -0.585 0.601 0.000 1923 22 gamma 91 1704 0 0 0 0 0 0.020 0.036 -0.838 0.839 0.000 1924 22 gamma 91 1717 0 0 0 0 0 0.226 0.007 1.882 1.896 0.000 1925 22 gamma 91 1717 0 0 0 0 0 0.335 -0.082 4.284 4.298 0.000 1926 22 gamma 91 1722 0 0 0 0 0 -0.265 -0.194 23.347 23.349 0.000 1927 22 gamma 91 1722 0 0 0 0 0 -0.066 -0.005 9.598 9.598 0.000 1928 22 gamma 91 1729 0 0 0 0 0 0.052 0.160 0.274 0.322 0.000 1929 22 gamma 91 1729 0 0 0 0 0 -0.085 0.345 0.622 0.717 0.000 1930 22 gamma 91 1736 0 0 0 0 0 -0.070 -0.130 -1.528 1.535 0.000 1931 22 gamma 91 1736 0 0 0 0 0 0.004 0.030 -0.211 0.213 0.000 1932 22 gamma 91 1745 0 0 0 0 0 0.064 0.150 -0.351 0.387 0.000 1933 22 gamma 91 1745 0 0 0 0 0 0.098 0.025 -0.397 0.410 0.000 1934 22 gamma 91 1756 0 0 0 0 0 0.008 -0.014 3.950 3.950 0.000 1935 22 gamma 91 1756 0 0 0 0 0 0.075 -0.073 2.038 2.041 0.000 1936 22 gamma 91 1758 0 0 0 0 0 -0.015 -0.029 0.662 0.663 0.000 1937 22 gamma 91 1758 0 0 0 0 0 0.040 0.132 3.335 3.338 0.000 1938 22 gamma 91 1759 0 0 0 0 0 0.026 0.412 3.333 3.359 0.000 1939 22 gamma 91 1759 0 0 0 0 0 -0.071 0.230 2.449 2.461 0.000 1940 22 gamma 91 1766 0 0 0 0 0 0.161 0.843 0.878 1.227 0.000 1941 22 gamma 91 1766 0 0 0 0 0 -0.011 0.012 0.003 0.016 0.000 1942 22 gamma 91 1767 0 0 0 0 0 0.015 0.002 -0.017 0.022 0.000 1943 22 gamma 91 1767 0 0 0 0 0 -0.073 0.287 0.098 0.312 0.000 1944 22 gamma 91 1858 0 0 0 0 0 0.126 0.103 0.107 0.195 0.000 1945 22 gamma 91 1858 0 0 0 0 0 -0.021 -0.005 -0.011 0.024 0.000 1946 22 gamma 91 1859 0 0 0 0 0 -0.188 0.079 -0.141 0.249 0.000 1947 22 gamma 91 1859 0 0 0 0 0 -0.090 0.041 0.027 0.102 0.000 1948 22 gamma 91 1862 0 0 0 0 0 -0.027 -0.002 -0.441 0.442 0.000 1949 22 gamma 91 1862 0 0 0 0 0 0.131 -0.167 -3.023 3.030 0.000 1950 22 gamma 91 1863 0 0 0 0 0 -0.035 -0.016 -0.126 0.132 0.000 1951 22 gamma 91 1863 0 0 0 0 0 -0.269 -0.089 -3.150 3.163 0.000 1952 310 (K_S0) -91 1870 1870 1973 1974 0 0 1.027 -2.272 31.618 31.720 0.498 1953 22 gamma 91 1871 0 0 0 0 0 -0.198 -0.171 1.074 1.106 0.000 1954 22 gamma 91 1871 0 0 0 0 0 -0.106 0.008 0.334 0.350 0.000 1955 321 K+ 91 1872 0 0 0 0 0 0.044 -0.190 60.017 60.020 0.494 1956 -211 pi- 91 1872 0 0 0 0 0 0.083 0.256 13.727 13.730 0.140 1957 -421 (Dbar0) -91 1879 0 1975 1977 0 0 13.680 16.764 -18.522 28.543 1.865 1958 -211 pi- 91 1879 0 0 0 0 0 1.043 1.321 -1.484 2.249 0.140 1959 22 gamma 91 1884 0 0 0 0 0 -0.029 -0.294 26.099 26.101 0.000 1960 22 gamma 91 1884 0 0 0 0 0 -0.067 -0.057 5.283 5.284 0.000 1961 22 gamma 91 1885 0 0 0 0 0 -0.006 0.038 3.964 3.965 0.000 1962 22 gamma 91 1885 0 0 0 0 0 -0.145 -0.069 8.991 8.993 0.000 1963 22 gamma 91 1886 0 0 0 0 0 -0.052 -0.082 8.046 8.047 0.000 1964 22 gamma 91 1886 0 0 0 0 0 0.061 -0.020 2.791 2.792 0.000 1965 130 K_L0 91 1897 1897 0 0 0 0 1.205 0.793 4.086 4.362 0.498 1966 22 gamma 91 1898 0 0 0 0 0 -0.013 0.123 0.635 0.647 0.000 1967 22 gamma 91 1898 0 0 0 0 0 0.019 -0.026 0.413 0.414 0.000 1968 4132 (Xi_c0) -91 1903 0 1978 1979 0 0 -12.358 -27.452 -92.484 97.292 2.471 1969 22 gamma 91 1903 0 0 0 0 0 -0.647 -1.492 -5.327 5.569 0.000 1970 310 (K_S0) -91 1916 1916 1980 1981 0 0 0.257 0.030 0.268 0.622 0.498 1971 22 gamma 91 1917 0 0 0 0 0 0.776 0.186 0.219 0.828 0.000 1972 22 gamma 91 1917 0 0 0 0 0 -0.000 -0.003 -0.008 0.008 0.000 1973 211 pi+ 91 1952 0 0 0 0 0 0.143 -0.652 7.335 7.367 0.140 1974 -211 pi- 91 1952 0 0 0 0 0 0.885 -1.620 24.283 24.353 0.140 1975 321 K+ 91 1957 0 0 0 0 0 2.742 3.446 -4.447 6.278 0.494 1976 -211 pi- 91 1957 0 0 0 0 0 2.253 2.315 -2.700 4.212 0.140 1977 111 (pi0) -91 1957 0 1982 1983 0 0 8.685 11.002 -11.375 18.052 0.135 1978 -311 (Kbar0) -91 1968 0 1984 1984 0 0 -5.561 -10.205 -35.005 36.887 0.498 1979 3122 (Lambda0) -91 1968 0 1985 1986 0 0 -6.797 -17.247 -57.479 60.405 1.116 1980 111 (pi0) -91 1970 0 1987 1988 0 0 0.206 -0.068 0.346 0.430 0.135 1981 111 (pi0) -91 1970 0 1989 1990 0 0 0.051 0.098 -0.078 0.191 0.135 1982 22 gamma 91 1977 0 0 0 0 0 6.344 8.078 -8.265 13.184 0.000 1983 22 gamma 91 1977 0 0 0 0 0 2.340 2.925 -3.110 4.869 0.000 1984 130 K_L0 91 1978 1978 0 0 0 0 -5.561 -10.205 -35.005 36.887 0.498 1985 2212 p+ 91 1979 0 0 0 0 0 -5.319 -13.638 -45.593 47.895 0.938 1986 -211 pi- 91 1979 0 0 0 0 0 -1.478 -3.608 -11.886 12.510 0.140 1987 22 gamma 91 1980 0 0 0 0 0 0.178 -0.104 0.248 0.323 0.000 1988 22 gamma 91 1980 0 0 0 0 0 0.029 0.036 0.098 0.108 0.000 1989 22 gamma 91 1981 0 0 0 0 0 0.052 0.128 -0.083 0.161 0.000 1990 22 gamma 91 1981 0 0 0 0 0 -0.001 -0.030 0.004 0.030 0.000 Charge sum: 2.000 Momentum sum: 0.000 -0.000 0.000 14000.000 14000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> b bbar 123 | 460 98 98 | 1.145e-04 5.744e-06 | | q qbar -> b bbar 124 | 10 2 2 | 3.810e-06 9.896e-07 | | | | | | sum | 470 100 100 | 1.183e-04 5.829e-06 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 0 no errors or warnings to report | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:04 number of b quarks in an event 9.00*10^ 1 7 8.70*10^ 1 X 8.40*10^ 1 X 8.10*10^ 1 X 7.80*10^ 1 X 7.50*10^ 1 X 7.20*10^ 1 X 6.90*10^ 1 X 6.60*10^ 1 X 6.30*10^ 1 X 6.00*10^ 1 X 5.70*10^ 1 X 5.40*10^ 1 X 5.10*10^ 1 X 4.80*10^ 1 X 4.50*10^ 1 X 4.20*10^ 1 X 3.90*10^ 1 X 3.60*10^ 1 X 3.30*10^ 1 X 3.00*10^ 1 X 2.70*10^ 1 X 2.40*10^ 1 X 2.10*10^ 1 X 1.80*10^ 1 X 1.50*10^ 1 X 1.20*10^ 1 X 7 0.90*10^ 1 X X 0.60*10^ 1 X X 0.30*10^ 1 X X Contents *10^ 1 0080100000 *10^ 0 0090100000 *10^-1 0000000000 *10^-2 0000000000 Low edge - *10^ 0 0012345678 *10^-1 5555555555 *10^-2 0000000000 Entries = 100 Mean = 2.2200e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+02 Rms = 6.2578e-01 Overflow = 0.0000e+00 High edge = 9.5000e+00 2013-09-20 16:04 number of times same event is used 4.05*10^ 1 7 3.90*10^ 1 X 3.75*10^ 1 X 3.60*10^ 1 X 3.45*10^ 1 X 3.30*10^ 1 X 3.15*10^ 1 X 3.00*10^ 1 X 2.85*10^ 1 X 2.70*10^ 1 X3 2.55*10^ 1 XX 2.40*10^ 1 XX 2.25*10^ 1 XX 2.10*10^ 1 XX 1.95*10^ 1 XX7 1.80*10^ 1 XXX 1.65*10^ 1 XXX 1.50*10^ 1 XXX 1.35*10^ 1 XXX 1.20*10^ 1 XXX 1.05*10^ 1 XXX 0.90*10^ 1 XXX 0.75*10^ 1 XXX 0.60*10^ 1 XXXX3 0.45*10^ 1 XXXXX 0.30*10^ 1 XXXXXX 0.15*10^ 1 XXXXXX 7 Contents *10^ 1 4210000000 *10^ 0 0696530100 *10^-1 0000000000 *10^-2 0000000000 Low edge - *10^ 0 0012345678 *10^-1 5555555555 *10^-2 0000000000 Entries = 100 Mean = 1.2400e+00 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+02 Rms = 1.4361e+00 Overflow = 0.0000e+00 High edge = 9.5000e+00 2013-09-20 16:04 mass of opposite-sign muon pair 1.62*10^ 1 7 1.56*10^ 1 X 1.50*10^ 1 X 1.44*10^ 1 X 1.38*10^ 1 X 1.32*10^ 1 X7 1.26*10^ 1 XX 1.20*10^ 1 XX 1.14*10^ 1 XX 1.08*10^ 1 XX 1.02*10^ 1 XX 0.96*10^ 1 XX 0.90*10^ 1 XX 0.84*10^ 1 XX 3 0.78*10^ 1 XX X 0.72*10^ 1 XX7X 7 0.66*10^ 1 XXXX X 0.60*10^ 1 XXXX X 0.54*10^ 1 XXXX X3 0.48*10^ 1 XXXX XX 0.42*10^ 1 XXXX XX 7 0.36*10^ 1 XXXX XX X 0.30*10^ 1 XXXXXXXXX X 0.24*10^ 1 XXXXXXXXX 3 X 3 3 0.18*10^ 1 XXXXXXXXX X X X X 0.12*10^ 1 XXXXXXXXX 7X7X777 77X 7X7 7 7 777 7 7 7 7 7 0.06*10^ 1 XXXXXXXXX XXXXXXX XXX XXX X X XXX X X X X X Contents *10^ 1 1100000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 6378375340121311101120121010100001110010000000000010000000000000000000100000000001001000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 0 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 94 Mean = 1.0681e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 9.4000e+01 Rms = 1.5925e+01 Overflow = 0.0000e+00 High edge = 1.0000e+02 2013-09-20 16:04 mass of same-sign muon pair 9.00*10^ 0 X 8.70*10^ 0 X 8.40*10^ 0 X 8.10*10^ 0 X 7.80*10^ 0 X 7.50*10^ 0 X 7.20*10^ 0 3 X 6.90*10^ 0 X X 6.60*10^ 0 X X 6.30*10^ 0 X X 6.00*10^ 0 X XX 5.70*10^ 0 X XX 5.40*10^ 0 X XX 5.10*10^ 0 X7XX 7 7 4.80*10^ 0 XXXX X X 4.50*10^ 0 XXXX X X 4.20*10^ 0 XXXX 3X X 3 3.90*10^ 0 XXXX XX X X 3.60*10^ 0 XXXX XX X X 3.30*10^ 0 XXXX XX X X 3.00*10^ 0 XXXX XX X X 2.70*10^ 0 XXXX XX X X 2.40*10^ 0 XXXX XX X X 2.10*10^ 0 XXXX77XX7 X7 7 X777 7 7 1.80*10^ 0 XXXXXXXXX XX X XXXX X X 1.50*10^ 0 XXXXXXXXX XX X XXXX X X 1.20*10^ 0 XXXXXXXXX3XX3 333X XXXX3 3 X33 33 33333 X 33 3 3 3 0.90*10^ 0 XXXXXXXXXXXXX XXXX XXXXX X XXX XX XXXXX X XX X X X 0.60*10^ 0 XXXXXXXXXXXXX XXXX XXXXX X XXX XX XXXXX X XX X X X 0.30*10^ 0 XXXXXXXXXXXXX XXXX XXXXX X XXX XX XXXXX X XX X X X Contents *10^ 0 7596224521521011120422210100211011001111102000000011001000000010000000000000000000000000000000000001 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 1 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^ 0 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 87 Mean = 1.5919e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 8.6000e+01 Rms = 1.7240e+01 Overflow = 1.0000e+00 High edge = 1.0000e+02 pythia8-8.1.80.orig/examples/outref/out250000644000175000017500000103134612217346175016374 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:07:54 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *----------------------- SusyLesHouches SUSY/BSM Interface ------------------------* | Last Change 01 Aug 2012 - P. Skands | Parsing: main25.lhe | (SLHA::readFile) line 15 - storing QNUMBERS for id = 9000006 sextet *------------------------------------------------------------------------------------* | | Spectrum Calculator was: unknown version: unknown | Read spectrum from: main25.lhe | | ~g m | 1000021 70.000 | | ~d m ~dL ~sL ~bL ~dR ~sR ~bR | 1000001 10000.000 1.000 0.000 0.000 0.000 0.000 0.000 | 1000003 10000.000 0.000 1.000 0.000 0.000 0.000 0.000 | 1000005 10000.000 0.000 0.000 0.938 0.000 0.000 0.346 | 2000001 10000.000 0.000 0.000 0.000 1.000 0.000 0.000 | 2000003 10000.000 0.000 0.000 0.000 0.000 1.000 0.000 | 2000005 10000.000 0.000 0.000 -0.346 0.000 0.000 0.938 | | ~u m ~uL ~cL ~tL ~uR ~cR ~tR | 1000002 1000.000 1.000 0.000 0.000 0.000 0.000 0.000 | 1000004 1000.000 0.000 1.000 0.000 0.000 0.000 0.000 | 1000006 10000.000 0.000 0.000 0.553 0.000 0.000 0.833 | 2000002 1000.000 0.000 0.000 0.000 1.000 0.000 0.000 | 2000004 1000.000 0.000 0.000 0.000 0.000 1.000 0.000 | 2000006 10000.000 0.000 0.000 0.833 0.000 0.000 -0.553 | | ~e m ~eL ~muL ~tauL ~eR ~muR ~tauR | 1000011 20275.952 1.000 0.000 0.000 0.000 0.000 0.000 | 1000013 20275.952 0.000 1.000 0.000 0.000 0.000 0.000 | 1000015 23451.856 0.000 0.000 0.282 0.000 0.000 0.959 | 2000011 24407.125 0.000 0.000 0.000 1.000 0.000 0.000 | 2000013 24407.125 0.000 0.000 0.000 0.000 1.000 0.000 | 2000015 20668.792 0.000 0.000 0.959 0.000 0.000 -0.282 | | ~nu m ~nu_e ~nu_mu ~nu_tau | 1000012 18508.967 1.000 0.000 0.000 | 1000014 18508.967 0.000 1.000 0.000 | 1000016 28454.038 0.000 0.000 1.000 | | ~chi0 m ~B ~W_3 ~H_1 ~H_2 | 1000022 40.000 1.000 0.000 0.000 0.000 | 1000023 60.000 0.000 1.000 0.000 0.000 | 1000025 70.000 0.000 0.000 1.000 0.000 | 1000035 80.000 0.000 0.000 0.000 1.000 | | ~chi+ m U: ~W ~H | V: ~W ~H | 1000024 18169.250 0.915 -0.402 | 0.972 -0.236 | 1000037 27832.806 0.402 0.915 | 0.236 0.972 | | Higgs | alpha -0.114 | mu 355.826 (DRbar running value at Q = 464.669 GeV) | tan(beta) 9.749 (DRbar running value at Q = 464.669 GeV) | v 245.016 (DRbar running value at Q = 464.669 GeV) | mA 1.651e+05 (DRbar running value at Q = 464.669 GeV) | | Gauge | g' absent | g absent | g3 1.099 (DRbar running value at Q = 464.669 GeV) | *------------------------------------------------------------------------------------* | (SLHA::initSUSY) Warning: Block GAUGE not found or incomplete; using sin(thetaW) at mZ *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 8.000e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | Les Houches User Process(es) 9999 | 3.886e-06 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:frameType | 4 | 1 1 5 | | Beams:LHEF | main25.lhe | void | | HiggsA3:coup2d | 9.74916 | 1.00000 | | HiggsA3:coup2H1Z | -0.0117056 | 1.00000 | | HiggsA3:coup2H2Z | 0.99993 | 1.00000 | | HiggsA3:coup2l | 0.10257 | 1.00000 | | HiggsA3:coup2u | 0.10257 | 1.00000 | | HiggsH1:coup2d | 1.11405 | 1.00000 | | HiggsH1:coup2Hchg | 0.58110 | 0.0 | | HiggsH1:coup2l | 0.99873 | 1.00000 | | HiggsH1:coup2u | 0.99873 | 1.00000 | | HiggsH1:coup2W | 0.99993 | 1.00000 | | HiggsH1:coup2Z | 0.99993 | 1.00000 | | HiggsH2:coup2A3A3 | 0.20999 | 1.00000 | | HiggsH2:coup2d | 9.73678 | 1.00000 | | HiggsH2:coup2H1H1 | -0.65016 | 1.00000 | | HiggsH2:coup2Hchg | 0.19199 | 0.0 | | HiggsH2:coup2HchgW | 0.99993 | 0.0 | | HiggsH2:coup2l | -0.11427 | 1.00000 | | HiggsH2:coup2u | -0.11427 | 1.00000 | | HiggsH2:coup2W | -0.0117056 | 1.00000 | | HiggsH2:coup2Z | -0.0117056 | 1.00000 | | HiggsHchg:coup2H1W | -0.0117056 | 1.00000 | | HiggsHchg:coup2H2W | 0.99993 | 0.0 | | HiggsHchg:tanBeta | 9.74916 | 5.00000 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | PartonLevel:FSR | off | on | | PartonLevel:ISR | off | on | | PartonLevel:MPI | off | on | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products 25 h0(H_1) 1 0 0 110.86439 0.00265 110.73203 110.99675 0.00000e+00 1 1 0 0 0 0 1 0.0000012 0 1 -1 1 1 0.0000003 0 2 -2 2 1 0.0003017 0 3 -3 3 1 0.0428676 0 4 -4 4 1 0.7490199 0 5 -5 5 1 0.0000000 0 6 -6 6 1 0.0000000 0 11 -11 7 1 0.0003065 0 13 -13 8 1 0.0865412 0 15 -15 9 1 0.0626901 0 21 21 10 1 0.0024906 0 22 22 11 1 0.0005018 0 22 23 12 1 0.0043239 0 23 23 13 1 0.0509551 0 24 -24 14 1 0.0000000 103 1000022 1000022 15 1 0.0000000 103 1000023 1000022 16 1 0.0000000 103 1000023 1000023 17 1 0.0000000 103 1000025 1000022 18 1 0.0000000 103 1000025 1000023 19 1 0.0000000 103 1000025 1000025 20 1 0.0000000 103 1000035 1000022 21 1 0.0000000 103 1000035 1000023 22 1 0.0000000 103 1000035 1000025 23 1 0.0000000 103 1000035 1000035 24 1 0.0000000 103 1000024 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-2000014 71 1 0.0000000 103 -1000014 2000014 72 1 0.0000000 103 1000015 -1000015 73 1 0.0000000 103 2000015 -2000015 74 1 0.0000000 103 1000015 -2000015 75 1 0.0000000 103 -1000015 2000015 76 1 0.0000000 103 1000016 -1000016 77 1 0.0000000 103 2000016 -2000016 78 1 0.0000000 103 1000016 -2000016 79 1 0.0000000 103 -1000016 2000016 37 H+ H- 1 3 0 406.25628 0.00000 50.00000 0.00000 0.00000e+00 1 0 0 1 0 0 1 0.0000000 0 -1 2 1 1 0.0000000 0 -3 4 2 1 0.0000000 0 -5 6 3 1 0.0000000 0 -11 12 4 1 0.0000000 0 -13 14 5 1 0.0000000 0 -15 16 6 1 0.0000000 0 24 25 7 1 0.0000000 103 1000022 1000024 8 1 0.0000000 103 1000022 1000037 9 1 0.0000000 103 1000023 1000024 10 1 0.0000000 103 1000023 1000037 11 1 0.0000000 103 1000025 1000024 12 1 0.0000000 103 1000025 1000037 13 1 0.0000000 103 1000035 1000024 14 1 0.0000000 103 1000035 1000037 15 1 0.0000000 103 1000006 -1000005 16 1 0.0000000 103 2000006 -1000005 17 1 0.0000000 103 1000006 -2000005 18 1 0.0000000 103 2000006 -2000005 19 1 0.0000000 103 -1000001 1000002 20 1 0.0000000 103 -1000003 1000004 21 1 0.0000000 103 -1000011 1000012 22 1 0.0000000 103 -1000013 1000014 23 1 0.0000000 103 -1000015 1000016 24 1 0.0000000 103 -2000015 1000016 1000001 ~d_L ~d_Lbar 1 -1 1 1.000e+04 6.882e-04 5.000e+01 0.000e+00 0.00000e+00 1 1 0 1 0 0 1 0.0000000 103 1000039 1 1 1 0.0000000 103 1000039 3 2 1 0.0000000 103 1000039 5 3 1 0.0000000 103 -1000024 2 4 1 0.0000000 103 -1000037 2 5 1 0.0000000 103 -1000024 4 6 1 0.0000000 103 -1000037 4 7 1 0.0000000 103 -1000024 6 8 1 0.0000000 103 -1000037 6 9 1 0.0000192 103 1000022 1 10 1 0.0000000 103 1000022 3 11 1 0.0000000 103 1000022 5 12 1 0.0005732 103 1000023 1 13 1 0.0000000 103 1000023 3 14 1 0.0000000 103 1000023 5 15 1 0.0000000 103 1000025 1 16 1 0.0000000 103 1000025 3 17 1 0.0000000 103 1000025 5 18 1 0.0000000 103 1000035 1 19 1 0.0000000 103 1000035 3 20 1 0.0000000 103 1000035 5 21 1 0.0000000 103 1000002 -24 22 1 0.0000000 103 1000004 -24 23 1 0.0000000 103 1000006 -24 24 1 0.0000000 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-24 26 1 0.0000000 103 2000005 -24 27 1 0.0000000 103 1000001 -37 28 1 0.0000000 103 1000003 -37 29 1 0.0000000 103 1000005 -37 30 1 0.0000000 103 2000001 -37 31 1 0.0000000 103 2000003 -37 32 1 0.0000000 103 2000005 -37 33 1 0.9994060 103 1000021 2 34 1 0.0000000 103 1000021 4 35 1 0.0000000 103 1000021 6 36 1 0.0000000 103 -11 1 37 1 0.0000000 103 -11 3 38 1 0.0000000 103 -11 5 39 1 0.0000000 103 -13 1 40 1 0.0000000 103 -13 3 41 1 0.0000000 103 -13 5 42 1 0.0000000 103 -15 1 43 1 0.0000000 103 -15 3 44 1 0.0000000 103 -15 5 45 1 0.0000000 103 -1 -3 46 1 0.0000000 103 -1 -5 47 1 0.0000000 103 -3 -5 1000003 ~s_L ~s_Lbar 1 -1 1 1.000e+04 4.077e-07 5.000e+01 0.000e+00 0.00000e+00 1 1 0 1 0 0 1 0.0000000 103 1000039 1 1 1 0.0000000 103 1000039 3 2 1 0.0000000 103 1000039 5 3 1 0.0000000 103 -1000024 2 4 1 0.0000000 103 -1000037 2 5 1 0.0000000 103 -1000024 4 6 1 0.0000000 103 -1000037 4 7 1 0.0000000 103 -1000024 6 8 1 0.0000000 103 -1000037 6 9 1 0.0000000 103 1000022 1 10 1 0.0323351 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PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- LHA initialization information ------------ beam kind energy pdfgrp pdfset A 2212 4000.000 0 10042 B 2212 4000.000 0 10042 Event weighting strategy = 3 Processes, with strategy-dependent cross section info number xsec (pb) xerr (pb) xmax (pb) 661 3.8860e+03 4.0300e+00 3.8944e-02 -------- End LHA initialization information -------- Begin event # 0 -------- LHA event information and listing ---------------------------------------------------------------------- process = 1 weight = 3.1703e+00 scale = 3.4814e+02 (GeV) alpha_em = 7.8165e-03 alpha_strong = 1.0722e-01 Participating Particles no id stat mothers colours p_x p_y p_z e m tau spin 1 -1 -1 0 0 0 501 0.000 0.000 477.456 477.456 0.000 0.000 1.000 2 -3 -1 0 0 0 502 0.000 0.000 -63.461 63.461 0.000 0.000 1.000 3 1000006 2 1 2 503 0 0.000 0.000 413.995 540.917 348.137 0.000 0.000 4 6 1 3 3 503 0 55.020 55.099 352.628 400.466 173.100 0.000 -1.000 5 1000022 1 3 3 0 0 -55.020 -55.099 61.367 140.451 99.486 0.000 -1.000 -------- End LHA event information and listing ------------------------------------------------------------------ -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 4.000e+03, e = 4.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -4.000e+03, e = 4.000e+03, m = 9.383e-01. In 1: id = -1, x = 1.194e-01, pdf = 0.000e+00 at Q2 = 1.212e+05. In 2: id = -3, x = 1.587e-02, pdf = 0.000e+00 at same Q2. Process Les Houches User Process(es) with code 9999 is 2 -> 1. Subprocess user process 1 with code 1 is 2 -> 1. It has sHat = 1.212e+05. alphaEM = 7.817e-03, alphaS = 1.072e-01 at Q2 = 1.212e+05. Impact parameter b = 0.000e+00 gives enhancement factor = 1.000e+00. Max pT scale for MPI = 8.000e+03, ISR = 8.000e+03, FSR = 8.000e+03. Number of MPI = 1, ISR = 0, FSRproc = 0, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 8000.000 8000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 4000.000 4000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -4000.000 4000.000 0.938 3 -1 (dbar) -21 1 0 5 0 0 501 0.000 0.000 477.456 477.456 0.000 4 -3 (sbar) -21 2 0 5 0 0 502 0.000 0.000 -63.461 63.461 0.000 5 1000006 (~t_1) -22 3 4 6 7 503 0 0.000 0.000 413.995 540.917 348.137 6 6 (t) -22 5 0 8 9 503 0 55.020 55.099 352.628 400.466 173.100 7 1000022 ~chi_10 23 5 0 0 0 0 0 -55.020 -55.099 61.367 140.451 99.486 8 24 (W+) -22 6 0 10 11 0 0 -1.788 89.132 266.062 291.369 78.483 9 5 b 23 6 0 0 0 503 0 56.808 -34.033 86.566 109.097 4.800 10 -13 mu+ 23 8 0 0 0 0 0 34.570 45.829 175.063 184.235 0.106 11 14 nu_mu 23 8 0 0 0 0 0 -36.358 43.303 90.998 107.134 0.000 Charge sum: 0.667 Momentum sum: 0.000 0.000 413.995 540.917 348.137 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 8000.000 8000.000 1 2212 (p+) -12 0 0 6 0 0 0 0.000 0.000 4000.000 4000.000 0.938 2 2212 (p+) -12 0 0 7 0 0 0 0.000 0.000 -4000.000 4000.000 0.938 3 -1 (dbar) -21 6 6 5 0 0 501 0.000 0.000 477.456 477.456 0.000 4 -3 (sbar) -21 7 7 5 0 0 502 0.000 0.000 -63.461 63.461 0.000 5 1000006 (~t_1) -22 3 4 8 8 503 0 0.000 0.000 413.995 540.917 348.137 6 -1 (dbar) -61 1 0 3 3 0 501 2.185 0.481 477.450 477.456 0.000 7 -3 (sbar) -61 2 0 4 4 0 502 2.255 -2.931 -63.411 63.519 0.000 8 1000006 (~t_1) -62 5 5 15 16 503 0 4.441 -2.450 414.039 540.974 348.137 9 2203 (uu_1) -63 1 0 26 26 0 504 -0.863 0.113 3042.849 3042.849 0.771 10 1 (d) -63 1 0 31 31 501 0 -0.678 0.185 74.561 74.565 0.330 11 1 (d) -63 1 0 25 25 504 0 -0.644 -0.779 405.078 405.080 0.330 12 2203 (uu_1) -63 2 0 22 22 0 507 -0.987 0.707 -2462.035 2462.035 0.771 13 1 (d) -63 2 0 30 30 502 0 -0.622 1.249 -751.170 751.171 0.330 14 3 (s) -63 2 0 21 21 507 0 -0.646 0.975 -723.324 723.325 0.500 15 6 (t) -22 8 0 17 18 503 0 58.308 53.284 352.661 400.715 173.100 16 1000022 ~chi_10 23 8 0 0 0 0 0 -53.868 -55.734 61.379 140.260 99.486 17 24 (W+) -22 15 0 19 20 0 0 0.602 87.813 266.085 290.985 78.483 18 5 (b) -23 15 0 32 32 503 0 57.706 -34.528 86.575 109.729 4.800 19 -13 mu+ 23 17 0 0 0 0 0 36.083 44.994 175.078 184.334 0.106 20 14 nu_mu 23 17 0 0 0 0 0 -35.481 42.819 91.007 106.652 0.000 21 3 (s) -71 14 14 23 24 507 0 -0.646 0.975 -723.324 723.325 0.500 22 2203 (uu_1) -71 12 12 23 24 0 507 -0.987 0.707 -2462.035 2462.035 0.771 23 -311 (Kbar0) -82 21 22 52 52 0 0 -1.529 1.402 -2041.142 2041.143 0.498 24 2212 p+ 82 21 22 0 0 0 0 -0.104 0.281 -1144.216 1144.216 0.938 25 1 (d) -71 11 11 27 29 504 0 -0.644 -0.779 405.078 405.080 0.330 26 2203 (uu_1) -71 9 9 27 29 0 504 -0.863 0.113 3042.849 3042.849 0.771 27 313 (K*0) -83 25 26 53 54 0 0 -0.584 -0.150 823.125 823.125 0.926 28 -311 (Kbar0) -84 25 26 55 55 0 0 -0.581 0.301 1248.931 1248.931 0.498 29 2212 p+ 84 25 26 0 0 0 0 -0.343 -0.818 1375.872 1375.872 0.938 30 1 (d) -71 13 13 33 51 502 0 -0.622 1.249 -751.170 751.171 0.330 31 1 (d) -71 10 10 33 51 501 0 -0.678 0.185 74.561 74.565 0.330 32 5 (b) -71 18 18 33 51 503 0 57.706 -34.528 86.575 109.729 4.800 33 -213 (rho-) -85 30 32 56 57 0 0 -0.053 0.267 62.949 62.962 1.268 34 111 (pi0) -85 30 32 64 65 0 0 -0.315 0.423 4.214 4.249 0.135 35 211 pi+ 85 30 32 0 0 0 0 -0.509 -0.850 3.025 3.186 0.140 36 111 (pi0) -85 30 32 66 67 0 0 0.842 -0.241 0.680 1.117 0.135 37 -513 (B*bar0) -86 30 32 68 69 0 0 52.532 -31.891 78.611 99.924 5.325 38 111 (pi0) -86 30 32 70 71 0 0 1.679 -0.566 2.724 3.253 0.135 39 -211 pi- 86 30 32 0 0 0 0 1.578 -1.106 2.881 3.469 0.140 40 211 pi+ 86 30 32 0 0 0 0 0.553 -0.316 0.490 0.815 0.140 41 -211 pi- 83 30 32 0 0 0 0 -0.048 0.155 -166.382 166.382 0.140 42 213 (rho+) -83 30 32 58 59 0 0 -0.455 0.498 -264.592 264.594 0.717 43 221 (eta) -83 30 32 72 74 0 0 -0.151 0.362 -198.388 198.389 0.548 44 223 (omega) -83 30 32 75 77 0 0 -0.262 -0.102 -27.833 27.845 0.781 45 311 (K0) -84 30 32 60 60 0 0 0.293 0.513 -84.627 84.630 0.498 46 -311 (Kbar0) -84 30 32 61 61 0 0 -0.477 0.122 -4.626 4.679 0.498 47 2112 n0 84 30 32 0 0 0 0 0.534 -0.064 -3.361 3.531 0.940 48 111 (pi0) -84 30 32 78 79 0 0 0.113 -0.154 -0.747 0.782 0.135 49 -2212 pbar- 84 30 32 0 0 0 0 -0.022 -0.257 1.394 1.700 0.938 50 2214 (Delta+) -84 30 32 62 63 0 0 0.156 0.069 2.007 2.350 1.210 51 -211 pi- 84 30 32 0 0 0 0 0.417 0.045 1.547 1.609 0.140 52 130 K_L0 91 23 23 0 0 0 0 -1.529 1.402 -2041.142 2041.143 0.498 53 321 K+ 91 27 0 0 0 0 0 -0.718 -0.091 585.519 585.520 0.494 54 -211 pi- 91 27 0 0 0 0 0 0.134 -0.059 237.605 237.605 0.140 55 130 K_L0 91 28 28 0 0 0 0 -0.581 0.301 1248.931 1248.931 0.498 56 -211 pi- 91 33 0 0 0 0 0 -0.221 0.645 52.049 52.054 0.140 57 111 (pi0) -91 33 0 80 81 0 0 0.168 -0.378 10.899 10.908 0.135 58 211 pi+ 91 42 0 0 0 0 0 -0.304 0.518 -112.046 112.048 0.140 59 111 (pi0) -91 42 0 82 83 0 0 -0.151 -0.020 -152.546 152.546 0.135 60 130 K_L0 91 45 45 0 0 0 0 0.293 0.513 -84.627 84.630 0.498 61 130 K_L0 91 46 46 0 0 0 0 -0.477 0.122 -4.626 4.679 0.498 62 2212 p+ 91 50 0 0 0 0 0 0.321 0.019 1.760 2.020 0.938 63 111 (pi0) -91 50 0 84 85 0 0 -0.164 0.050 0.247 0.330 0.135 64 22 gamma 91 34 0 0 0 0 0 -0.305 0.415 4.193 4.224 0.000 65 22 gamma 91 34 0 0 0 0 0 -0.010 0.008 0.021 0.025 0.000 66 22 gamma 91 36 0 0 0 0 0 0.717 -0.178 0.514 0.899 0.000 67 22 gamma 91 36 0 0 0 0 0 0.126 -0.063 0.166 0.217 0.000 68 -511 (Bbar0) -91 37 0 86 88 0 0 52.177 -31.703 78.036 99.222 5.280 69 22 gamma 91 37 0 0 0 0 0 0.355 -0.189 0.575 0.702 0.000 70 22 gamma 91 38 0 0 0 0 0 1.015 -0.396 1.594 1.930 0.000 71 22 gamma 91 38 0 0 0 0 0 0.665 -0.171 1.130 1.322 0.000 72 211 pi+ 91 43 0 0 0 0 0 -0.027 0.074 -25.859 25.860 0.140 73 -211 pi- 91 43 0 0 0 0 0 -0.158 0.238 -103.510 103.510 0.140 74 111 (pi0) -91 43 0 89 90 0 0 0.034 0.049 -69.019 69.020 0.135 75 211 pi+ 91 44 0 0 0 0 0 -0.112 0.169 -5.981 5.986 0.140 76 -211 pi- 91 44 0 0 0 0 0 -0.117 -0.171 -4.847 4.853 0.140 77 111 (pi0) -91 44 0 91 92 0 0 -0.033 -0.099 -17.004 17.005 0.135 78 22 gamma 91 48 0 0 0 0 0 0.121 -0.074 -0.353 0.380 0.000 79 22 gamma 91 48 0 0 0 0 0 -0.009 -0.081 -0.394 0.402 0.000 80 22 gamma 91 57 0 0 0 0 0 0.027 -0.163 3.043 3.047 0.000 81 22 gamma 91 57 0 0 0 0 0 0.142 -0.216 7.857 7.861 0.000 82 22 gamma 91 59 0 0 0 0 0 -0.012 0.012 -76.583 76.583 0.000 83 22 gamma 91 59 0 0 0 0 0 -0.139 -0.032 -75.963 75.963 0.000 84 22 gamma 91 63 0 0 0 0 0 -0.184 0.056 0.241 0.308 0.000 85 22 gamma 91 63 0 0 0 0 0 0.020 -0.006 0.006 0.022 0.000 86 -411 (D-) -91 68 0 93 95 0 0 12.790 -8.302 18.627 24.145 1.870 87 -311 (Kbar0) -91 68 0 96 96 0 0 2.698 -1.818 3.974 5.160 0.498 88 411 (D+) -91 68 0 97 98 0 0 36.690 -21.583 55.434 69.917 1.870 89 22 gamma 91 74 0 0 0 0 0 0.056 0.060 -66.140 66.140 0.000 90 22 gamma 91 74 0 0 0 0 0 -0.022 -0.011 -2.879 2.879 0.000 91 22 gamma 91 77 0 0 0 0 0 0.011 -0.006 -10.772 10.772 0.000 92 22 gamma 91 77 0 0 0 0 0 -0.044 -0.093 -6.232 6.233 0.000 93 13 mu- 91 86 0 0 0 0 0 1.912 -1.727 2.819 3.821 0.106 94 -14 nu_mubar 91 86 0 0 0 0 0 1.699 -0.696 2.142 2.821 0.000 95 313 (K*0) -91 86 0 99 100 0 0 9.179 -5.879 13.667 17.504 0.883 96 310 (K_S0) -91 87 87 101 102 0 0 2.698 -1.818 3.974 5.160 0.498 97 20213 (a_1(1260)+) -91 88 0 103 104 0 0 28.457 -16.792 42.859 54.134 1.342 98 311 (K0) -91 88 0 105 105 0 0 8.232 -4.790 12.575 15.783 0.498 99 321 K+ 91 95 0 0 0 0 0 8.123 -5.367 12.359 15.741 0.494 100 -211 pi- 91 95 0 0 0 0 0 1.056 -0.512 1.308 1.763 0.140 101 111 (pi0) -91 96 0 106 107 0 0 0.795 -0.523 1.468 1.755 0.135 102 111 (pi0) -91 96 0 108 109 0 0 1.902 -1.295 2.507 3.406 0.135 103 213 (rho+) -91 97 0 110 111 0 0 17.830 -10.692 26.768 33.908 1.000 104 111 (pi0) -91 97 0 112 113 0 0 10.628 -6.100 16.091 20.226 0.135 105 310 (K_S0) -91 98 98 114 115 0 0 8.232 -4.790 12.575 15.783 0.498 106 22 gamma 91 101 0 0 0 0 0 0.476 -0.331 0.772 0.965 0.000 107 22 gamma 91 101 0 0 0 0 0 0.320 -0.193 0.696 0.789 0.000 108 22 gamma 91 102 0 0 0 0 0 0.901 -0.559 1.080 1.514 0.000 109 22 gamma 91 102 0 0 0 0 0 1.001 -0.735 1.427 1.892 0.000 110 211 pi+ 91 103 0 0 0 0 0 15.091 -9.074 22.109 28.265 0.140 111 111 (pi0) -91 103 0 116 117 0 0 2.738 -1.618 4.659 5.643 0.135 112 22 gamma 91 104 0 0 0 0 0 9.004 -5.223 13.684 17.193 0.000 113 22 gamma 91 104 0 0 0 0 0 1.623 -0.877 2.406 3.032 0.000 114 111 (pi0) -91 105 0 118 119 0 0 4.591 -2.505 7.147 8.858 0.135 115 111 (pi0) -91 105 0 120 121 0 0 3.641 -2.286 5.428 6.925 0.135 116 22 gamma 91 111 0 0 0 0 0 1.614 -0.881 2.651 3.226 0.000 117 22 gamma 91 111 0 0 0 0 0 1.124 -0.737 2.008 2.417 0.000 118 22 gamma 91 114 0 0 0 0 0 1.051 -0.592 1.557 1.969 0.000 119 22 gamma 91 114 0 0 0 0 0 3.541 -1.913 5.591 6.889 0.000 120 22 gamma 91 115 0 0 0 0 0 3.049 -1.970 4.602 5.861 0.000 121 22 gamma 91 115 0 0 0 0 0 0.592 -0.316 0.826 1.064 0.000 Charge sum: 2.000 Momentum sum: 0.000 0.000 -0.000 8000.000 8000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- Begin event # 1 Begin event # 2 Begin event # 3 Begin event # 4 Begin event # 5 Begin event # 6 Begin event # 7 Begin event # 8 Begin event # 9 Begin event # 10 Begin event # 11 Begin event # 12 Begin event # 13 Begin event # 14 Begin event # 15 Begin event # 16 Begin event # 17 Begin event # 18 Begin event # 19 Begin event # 20 PYTHIA Abort from Pythia::next: reached end of Les Houches Events File *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | Les Houches User Process(es) 9999 | 20 20 20 | 3.886e-06 4.030e-09 | | ... whereof user classification code 0 | 2 2 2 | | | ... whereof user classification code 1 | 4 4 4 | | | ... whereof user classification code 2 | 2 2 2 | | | ... whereof user classification code 3 | 2 2 2 | | | ... whereof user classification code 4 | 8 8 8 | | | ... whereof user classification code 6 | 2 2 2 | | | | | | | sum | 20 20 20 | 3.886e-06 4.030e-09 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Abort from Pythia::next: reached end of Les Houches Events File | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:07 charged particle multiplicity 3.00*10^ 0 X X 2.88*10^ 0 X X 2.76*10^ 0 X X 2.64*10^ 0 X X 2.52*10^ 0 X X 2.40*10^ 0 X X 2.28*10^ 0 X X 2.16*10^ 0 X X 2.04*10^ 0 7 X7 7 X 1.92*10^ 0 X XX X X 1.80*10^ 0 X XX X X 1.68*10^ 0 X XX X X 1.56*10^ 0 X XX X X 1.44*10^ 0 X XX X X 1.32*10^ 0 X XX X X 1.20*10^ 0 X XX X X 1.08*10^ 0 3X333 XX 3X3 33X 0.96*10^ 0 XXXXX XX XXX XXX 0.84*10^ 0 XXXXX XX XXX XXX 0.72*10^ 0 XXXXX XX XXX XXX 0.60*10^ 0 XXXXX XX XXX XXX 0.48*10^ 0 XXXXX XX XXX XXX 0.36*10^ 0 XXXXX XX XXX XXX 0.24*10^ 0 XXXXX XX XXX XXX 0.12*10^ 0 XXXXX XX XXX XXX Contents *10^ 0 0000012111032001210113000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^ 1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^ 0 1482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 20 Mean = 5.4300e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 2.0000e+01 Rms = 2.1302e+01 Overflow = 0.0000e+00 High edge = 3.9950e+02 pythia8-8.1.80.orig/examples/outref/out120000644000175000017500000040252412217346172016364 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:03:37 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with pbar- at a CM energy of 1.960e+03 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> t tbar 601 | 7.731e-09 | | q qbar -> t tbar 602 | 1.009e-07 | | Les Houches User Process(es) 9999 | 5.480e-09 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 40.89 mb | | | | pT0 = 2.12 gives sigmaInteraction = 136.61 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | Beams:frameType | 4 | 1 1 5 | | Beams:LHEF | ttbar.lhe | void | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberShowEvent | 0 | 1 0 | | Next:numberShowInfo | 0 | 1 0 | | Next:numberShowLHA | 0 | 1 0 | | Next:numberShowProcess | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | Top:gg2ttbar | on | off | | Top:qqbar2ttbar | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products 6 t tbar 2 2 1 175.00000 1.40771 86.00000 0.00000 0.00000e+00 1 1 0 1 0 0 1 0.0000664 0 24 1 1 1 0.0017360 0 24 3 2 1 0.9981976 0 24 5 3 0 0.0000000 0 37 5 -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- LHA initialization information ------------ beam kind energy pdfgrp pdfset A 2212 980.000 0 7 B -2212 980.000 0 7 Event weighting strategy = 3 Processes, with strategy-dependent cross section info number xsec (pb) xerr (pb) xmax (pb) 81 5.2201e+00 5.3841e-01 1.0000e+00 82 2.6026e-01 1.0625e-01 1.0000e+00 -------- End LHA initialization information -------- -------- LHA event information and listing ---------------------------------------------------------------------- process = 81 weight = 1.0000e+00 scale = 1.7331e+02 (GeV) alpha_em = 7.8198e-03 alpha_strong = 1.1567e-01 Participating Particles no id stat mothers colours p_x p_y p_z e m tau spin 1 2 -1 0 0 101 0 0.000 0.000 108.382 108.382 0.000 0.000 9.000 2 -2 -1 0 0 0 102 0.000 0.000 -279.761 279.761 0.000 0.000 9.000 3 6 2 1 2 101 0 33.629 8.912 -110.596 212.418 177.987 0.000 9.000 4 -6 2 1 2 0 102 -33.629 -8.912 -60.783 175.725 161.166 0.000 9.000 5 24 2 3 0 0 0 -30.885 -12.140 -4.785 86.623 79.871 0.000 9.000 6 5 1 3 0 101 0 64.514 21.052 -105.811 125.794 4.800 0.000 9.000 7 -24 2 4 0 0 0 -50.940 34.881 -75.292 126.217 80.315 0.000 9.000 8 -5 1 4 0 0 102 17.311 -43.792 14.509 49.507 4.800 0.000 9.000 9 -1 1 5 0 0 103 18.584 9.166 18.652 27.882 0.330 0.000 9.000 10 2 1 5 0 103 0 -49.469 -21.306 -23.437 58.741 0.330 0.000 9.000 11 13 1 7 0 0 0 9.691 39.074 -25.560 47.687 0.106 0.000 9.000 12 -14 1 7 0 0 0 -60.632 -4.194 -49.732 78.530 0.000 0.000 9.000 pdf: id1 = 2 id2 = -2 x1 = 1.106e-01 x2 = 2.855e-01 scalePDF = 1.733e+02 pdf1 = 5.530e-01 pdf2 = 3.572e-01 -------- End LHA event information and listing ------------------------------------------------------------------ -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 9.800e+02, e = 9.800e+02, m = 9.383e-01. Beam B: id = -2212, pz = -9.800e+02, e = 9.800e+02, m = 9.383e-01. In 1: id = 2, x = 1.106e-01, pdf = 5.530e-01 at Q2 = 3.004e+04. In 2: id = -2, x = 2.855e-01, pdf = 3.572e-01 at same Q2. Process Les Houches User Process(es) with code 9999 is 2 -> 2. Subprocess user process 81 with code 81 is 2 -> 2. It has sHat = 1.213e+05, tHat = -3.834e+04, uHat = -2.529e+04, pTHat = 3.479e+01, m3Hat = 1.780e+02, m4Hat = 1.612e+02, thetaHat = 2.065e+00, phiHat = 2.590e-01. alphaEM = 7.820e-03, alphaS = 1.157e-01 at Q2 = 3.004e+04. Impact parameter b = 5.609e-01 gives enhancement factor = 2.001e+00. Max pT scale for MPI = 1.960e+03, ISR = 1.960e+03, FSR = 1.960e+03. Number of MPI = 6, ISR = 10, FSRproc = 38, FSRreson = 32. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 1960.000 1960.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 980.000 980.000 0.938 2 -2212 (pbar-) -12 0 0 4 0 0 0 0.000 0.000 -980.000 980.000 0.938 3 2 (u) -21 1 0 5 6 101 0 0.000 0.000 108.382 108.382 0.000 4 -2 (ubar) -21 2 0 5 6 0 102 0.000 0.000 -279.761 279.761 0.000 5 6 (t) -22 3 4 7 8 101 0 33.629 8.912 -110.596 212.418 177.987 6 -6 (tbar) -22 3 4 9 10 0 102 -33.629 -8.912 -60.783 175.725 161.166 7 24 (W+) -22 5 0 11 12 0 0 -30.885 -12.140 -4.785 86.623 79.871 8 5 b 23 5 0 0 0 101 0 64.514 21.052 -105.811 125.794 4.800 9 -24 (W-) -22 6 0 13 14 0 0 -50.940 34.881 -75.292 126.217 80.315 10 -5 bbar 23 6 0 0 0 0 102 17.311 -43.792 14.509 49.507 4.800 11 -1 dbar 23 7 0 0 0 0 103 18.584 9.166 18.652 27.882 0.330 12 2 u 23 7 0 0 0 103 0 -49.469 -21.306 -23.437 58.741 0.330 13 13 mu- 23 9 0 0 0 0 0 9.691 39.074 -25.560 47.687 0.106 14 -14 nu_mubar 23 9 0 0 0 0 0 -60.632 -4.194 -49.732 78.530 0.000 Charge sum: 0.000 Momentum sum: -0.000 0.000 -171.379 388.143 348.258 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 1960.000 1960.000 1 2212 (p+) -12 0 0 208 0 0 0 0.000 0.000 980.000 980.000 0.938 2 -2212 (pbar-) -12 0 0 209 0 0 0 0.000 0.000 -980.000 980.000 0.938 3 2 (u) -21 7 0 5 6 101 0 0.000 0.000 108.382 108.382 0.000 4 -2 (ubar) -21 8 8 5 6 0 102 0.000 0.000 -279.761 279.761 0.000 5 6 (t) -22 3 4 9 9 101 0 33.629 8.912 -110.596 212.418 177.987 6 -6 (tbar) -22 3 4 10 10 0 102 -33.629 -8.912 -60.783 175.725 161.166 7 21 (g) -41 12 12 11 3 101 104 0.000 0.000 374.349 374.349 0.000 8 -2 (ubar) -42 13 0 4 4 0 102 -0.000 0.000 -279.761 279.761 0.000 9 6 (t) -44 5 5 14 14 101 0 37.313 3.657 -111.094 213.136 177.987 10 -6 (tbar) -44 6 6 15 15 0 102 -29.470 -14.843 -59.875 175.066 161.166 11 -2 (ubar) -43 7 0 16 16 0 104 -7.843 11.187 265.557 265.908 0.330 12 21 (g) -42 18 18 7 7 101 104 -0.000 0.000 374.349 374.349 0.000 13 -2 (ubar) -41 19 0 17 8 0 105 0.000 -0.000 -293.514 293.514 0.000 14 6 (t) -44 9 9 20 20 101 0 42.821 0.472 -111.969 214.593 177.987 15 -6 (tbar) -44 10 10 21 21 0 102 -25.479 -17.151 -61.439 175.193 161.166 16 -2 (ubar) -44 11 11 22 22 0 104 -7.837 11.183 263.416 263.770 0.330 17 21 (g) -43 13 0 23 23 102 105 -9.505 5.497 -9.173 14.307 0.000 18 21 (g) -42 25 0 12 12 101 104 0.000 -0.000 374.349 374.349 0.000 19 -2 (ubar) -41 26 26 24 13 0 106 -0.000 0.000 -333.188 333.188 0.000 20 6 (t) -44 14 14 27 27 101 0 40.104 3.097 -112.490 214.362 177.987 21 -6 (tbar) -44 15 15 28 28 0 102 -27.448 -15.249 -61.505 175.337 161.166 22 -2 (ubar) -44 16 16 29 29 0 104 -7.840 11.186 263.337 263.692 0.330 23 21 (g) -44 17 17 30 30 102 105 -9.700 5.685 -9.061 14.440 0.000 24 21 (g) -43 19 0 31 31 105 106 4.884 -4.720 -39.120 39.706 0.000 25 2 (u) -41 39 39 32 18 101 0 -0.000 -0.000 614.980 614.980 0.000 26 -2 (ubar) -42 40 0 19 19 0 106 -0.000 -0.000 -333.188 333.188 0.000 27 6 (t) -44 20 20 41 41 101 0 40.316 3.411 -112.575 214.452 177.987 28 -6 (tbar) -44 21 21 42 42 0 102 -27.211 -14.899 -61.394 175.231 161.166 29 -2 (ubar) -44 22 22 35 35 0 104 -6.743 12.807 263.326 263.724 0.330 30 21 (g) -44 23 23 44 44 102 105 -9.689 5.702 -9.058 14.437 0.000 31 21 (g) -44 24 24 45 45 105 106 4.885 -4.718 -39.115 39.700 0.000 32 2 (u) -43 25 0 33 34 104 0 -1.558 -2.303 240.607 240.624 0.330 33 2 (u) -51 32 0 46 46 107 0 1.233 -0.732 98.520 98.531 0.330 34 21 (g) 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537 144 109 0.057 0.202 -25.522 25.523 0.000 467 21 (g) -71 231 231 495 537 151 144 -0.314 1.199 -29.472 29.498 0.000 468 21 (g) -71 404 404 495 537 125 151 1.089 0.270 -16.586 16.634 0.584 469 21 (g) -71 257 257 495 537 137 125 -1.552 -0.653 -22.627 22.689 0.000 470 21 (g) -71 403 403 495 537 139 137 -0.193 -1.125 -8.396 8.482 0.395 471 21 (g) -71 221 221 495 537 150 139 0.209 -0.963 -20.789 20.813 0.000 472 21 (g) -71 400 400 495 537 143 150 -0.109 0.569 -6.525 6.553 0.192 473 21 (g) -71 271 271 495 537 156 143 -0.479 2.680 -8.040 8.488 0.000 474 21 (g) -71 269 269 495 537 133 156 -0.673 0.666 -3.371 3.501 0.000 475 21 (g) -71 279 279 495 537 167 133 0.961 0.392 -5.193 5.295 0.000 476 21 (g) -71 214 214 495 537 135 167 1.399 -1.964 -15.743 15.926 0.000 477 21 (g) -71 242 242 495 537 164 135 0.077 -0.510 -2.171 2.231 0.000 478 21 (g) -71 227 227 495 537 105 164 1.872 -1.441 -12.123 12.352 0.000 479 21 (g) -71 270 270 495 537 120 105 0.107 -0.459 -0.680 0.827 0.000 480 21 (g) -71 262 262 495 537 116 120 -0.832 -0.491 -2.275 2.472 0.000 481 21 (g) -71 401 401 495 537 138 116 -1.210 -0.260 -4.562 4.732 0.222 482 21 (g) -71 230 230 495 537 140 138 -1.964 0.814 -3.100 3.759 0.000 483 21 (g) -71 220 220 495 537 115 140 -0.950 0.883 -1.339 1.864 0.000 484 21 (g) -71 213 213 495 537 126 115 -1.243 0.009 0.017 1.243 0.000 485 21 (g) -71 228 228 495 537 136 126 -0.978 1.294 -2.216 2.747 0.000 486 21 (g) -71 222 222 495 537 162 136 -0.435 0.461 0.105 0.643 0.000 487 21 (g) -71 399 399 495 537 130 162 -1.273 1.182 -1.315 2.181 0.099 488 21 (g) -71 223 223 495 537 157 130 -0.226 -0.136 -0.363 0.449 0.000 489 21 (g) -71 236 236 495 537 102 157 -0.601 0.246 0.162 0.670 0.000 490 21 (g) -71 330 330 495 537 192 102 1.023 -3.646 0.445 3.813 0.000 491 21 (g) -71 329 329 495 537 190 192 0.316 -2.753 0.886 2.909 0.000 492 21 (g) -71 402 402 495 537 193 190 3.990 -13.909 4.147 15.055 0.243 493 21 (g) -71 332 332 495 537 187 193 0.136 -1.546 0.336 1.588 0.000 494 -5 (bbar) -71 331 331 495 537 0 187 12.453 -23.528 8.148 28.250 4.800 495 211 pi+ 83 465 494 0 0 0 0 -0.045 -0.331 0.508 0.623 0.140 496 -211 pi- 83 465 494 0 0 0 0 -0.437 -0.017 0.082 0.466 0.140 497 223 (omega) -83 465 494 679 681 0 0 0.105 -0.390 0.000 0.881 0.783 498 321 K+ 83 465 494 0 0 0 0 0.093 0.135 -0.332 0.617 0.494 499 -323 (K*-) -83 465 494 603 604 0 0 -0.342 -0.338 0.234 1.144 1.011 500 211 pi+ 83 465 494 0 0 0 0 -0.114 -0.280 -0.897 0.957 0.140 501 221 (eta) -83 465 494 682 684 0 0 0.303 -0.188 -2.205 2.300 0.548 502 -211 pi- 83 465 494 0 0 0 0 -0.110 0.132 -0.204 0.301 0.140 503 211 pi+ 83 465 494 0 0 0 0 -0.006 0.919 -21.741 21.761 0.140 504 223 (omega) -83 465 494 685 687 0 0 0.354 -0.031 -7.670 7.718 0.784 505 111 (pi0) -83 465 494 688 689 0 0 -0.044 0.057 -5.103 5.105 0.135 506 -213 (rho-) -83 465 494 605 606 0 0 -0.631 -0.080 -22.414 22.443 0.943 507 113 (rho0) -83 465 494 607 608 0 0 -0.066 0.389 -10.996 11.045 0.962 508 113 (rho0) -83 465 494 609 610 0 0 0.034 -0.549 -11.752 11.787 0.727 509 213 (rho+) -83 465 494 611 612 0 0 0.214 -0.276 -16.918 16.942 0.846 510 -211 pi- 83 465 494 0 0 0 0 -0.524 -0.071 -4.788 4.819 0.140 511 113 (rho0) -83 465 494 613 614 0 0 -0.511 -0.837 -17.701 17.762 1.096 512 113 (rho0) -83 465 494 615 616 0 0 0.321 1.084 -4.888 5.076 0.769 513 213 (rho+) -83 465 494 617 618 0 0 -0.191 1.033 -8.154 8.273 0.923 514 313 (K*0) -83 465 494 619 620 0 0 -0.583 1.833 -8.115 8.385 0.874 515 -313 (K*bar0) -83 465 494 621 622 0 0 1.411 -1.977 -12.321 12.589 0.875 516 111 (pi0) -83 465 494 690 691 0 0 0.789 -0.285 -4.039 4.127 0.135 517 -211 pi- 83 465 494 0 0 0 0 0.245 0.166 -1.469 1.505 0.140 518 211 pi+ 83 465 494 0 0 0 0 0.223 -1.257 -6.309 6.439 0.140 519 -213 (rho-) -83 465 494 623 624 0 0 0.663 -0.763 -6.952 7.117 1.143 520 113 (rho0) -84 465 494 625 626 0 0 -0.286 -0.363 -4.032 4.128 0.754 521 211 pi+ 84 465 494 0 0 0 0 -0.214 0.142 -0.048 0.296 0.140 522 2112 n0 84 465 494 0 0 0 0 -1.231 -0.159 -3.208 3.566 0.940 523 -2212 pbar- 84 465 494 0 0 0 0 -0.715 0.315 -1.930 2.284 0.938 524 211 pi+ 84 465 494 0 0 0 0 -1.663 -0.018 -1.897 2.527 0.140 525 111 (pi0) -84 465 494 692 693 0 0 0.042 0.052 -0.177 0.233 0.135 526 -211 pi- 84 465 494 0 0 0 0 -0.783 0.684 -0.963 1.425 0.140 527 111 (pi0) -84 465 494 694 695 0 0 -0.576 0.361 -0.910 1.144 0.135 528 223 (omega) -84 465 494 696 698 0 0 -1.000 0.699 -0.575 1.558 0.781 529 2114 (Delta0) -84 465 494 627 628 0 0 -1.238 1.199 -1.534 2.642 1.288 530 211 pi+ 84 465 494 0 0 0 0 -0.418 0.549 -0.062 0.706 0.140 531 -2212 pbar- 84 465 494 0 0 0 0 -0.096 -0.343 -0.364 1.067 0.938 532 213 (rho+) -84 465 494 629 630 0 0 -0.349 -0.719 -0.018 1.081 0.727 533 2212 p+ 84 465 494 0 0 0 0 -0.078 -0.928 -0.131 1.329 0.938 534 -213 (rho-) -84 465 494 631 632 0 0 1.533 -5.550 1.796 6.102 0.922 535 -2214 (Deltabar-) -84 465 494 633 634 0 0 1.601 -5.352 1.560 5.930 1.238 536 223 (omega) -84 465 494 699 701 0 0 2.084 -7.072 2.233 7.743 0.787 537 523 (B*+) -84 465 494 702 703 0 0 12.248 -25.175 8.307 29.684 5.325 538 21 (g) -71 266 266 556 582 121 163 -0.356 -0.421 8.196 8.214 0.000 539 21 (g) -71 249 249 556 582 163 141 0.111 -0.457 1.836 1.895 0.000 540 21 (g) -71 387 387 556 582 141 154 0.423 0.136 1.651 1.715 0.138 541 21 (g) -71 389 389 556 582 154 148 -1.835 1.790 6.297 6.815 0.471 542 21 (g) -71 252 252 556 582 148 112 -0.003 0.393 1.419 1.472 0.000 543 21 (g) -71 246 246 556 582 112 111 0.751 2.332 5.092 5.651 0.000 544 21 (g) -71 251 251 556 582 111 155 0.967 0.137 0.215 1.000 0.000 545 21 (g) -71 248 248 556 582 155 101 1.199 -0.829 -0.388 1.509 0.000 546 21 (g) -71 313 313 556 582 101 186 3.292 0.392 -5.085 6.070 0.000 547 21 (g) -71 312 312 556 582 186 185 1.764 0.614 -1.994 2.732 0.000 548 21 (g) -71 388 388 556 582 185 176 5.622 3.146 -10.902 12.665 0.179 549 21 (g) -71 391 391 556 582 176 184 12.832 4.446 -23.262 26.941 0.561 550 21 (g) -71 307 307 556 582 184 182 5.488 1.220 -8.250 9.984 0.000 551 21 (g) -71 390 390 556 582 182 180 2.122 1.017 -4.312 4.936 0.493 552 21 (g) -71 294 294 556 582 180 178 0.075 0.010 0.101 0.126 0.000 553 5 (b) -71 314 314 556 582 178 0 35.879 5.774 -53.089 64.515 4.800 554 1 (d) -71 275 275 556 582 146 0 1.896 -0.781 -0.446 2.124 0.330 555 1 (d) -71 280 280 556 582 170 0 0.552 -0.841 267.637 267.639 0.330 556 -213 (rho-) -85 538 555 635 636 0 0 0.856 -0.569 0.093 1.573 1.187 557 211 pi+ 85 538 555 0 0 0 0 0.464 0.157 0.364 0.626 0.140 558 223 (omega) -85 538 555 704 706 0 0 0.457 -0.523 0.719 1.271 0.785 559 313 (K*0) -85 538 555 637 638 0 0 -0.392 0.467 6.090 6.178 0.841 560 -213 (rho-) -86 538 555 639 640 0 0 -0.086 0.021 125.828 125.830 0.635 561 323 (K*+) -86 538 555 641 642 0 0 0.608 -0.780 112.643 112.651 0.872 562 -321 K- 86 538 555 0 0 0 0 0.330 -0.371 23.527 23.537 0.494 563 -521 (B-) -83 538 555 707 709 0 0 32.391 5.205 -47.762 58.184 5.279 564 3212 (Sigma0) -83 538 555 710 711 0 0 7.806 1.569 -12.001 14.451 1.193 565 113 (rho0) -83 538 555 643 644 0 0 1.916 1.044 -3.497 4.192 0.763 566 -3112 (Sigmabar+) -83 538 555 712 713 0 0 6.459 2.552 -11.917 13.845 1.197 567 311 (K0) -83 538 555 645 645 0 0 3.293 1.085 -5.808 6.782 0.498 568 -313 (K*bar0) -83 538 555 646 647 0 0 9.763 3.818 -17.623 20.525 0.907 569 2112 n0 83 538 555 0 0 0 0 3.296 0.513 -4.033 5.317 0.940 570 -2112 nbar0 83 538 555 0 0 0 0 0.598 -0.137 -1.141 1.600 0.940 571 -211 pi- 83 538 555 0 0 0 0 2.363 0.429 -2.246 3.291 0.140 572 213 (rho+) -83 538 555 648 649 0 0 0.061 -0.008 -0.411 0.894 0.791 573 -211 pi- 83 538 555 0 0 0 0 -0.092 0.136 -0.087 0.232 0.140 574 321 K+ 83 538 555 0 0 0 0 1.059 0.054 -0.067 1.172 0.494 575 -323 (K*-) -84 538 555 650 651 0 0 0.310 0.710 2.810 3.044 0.878 576 223 (omega) -84 538 555 714 715 0 0 0.112 0.309 0.748 1.132 0.783 577 211 pi+ 84 538 555 0 0 0 0 -0.839 0.452 2.217 2.417 0.140 578 -211 pi- 84 538 555 0 0 0 0 0.468 0.385 0.986 1.165 0.140 579 223 (omega) -84 538 555 716 718 0 0 0.142 0.849 2.842 3.074 0.794 580 211 pi+ 84 538 555 0 0 0 0 0.033 0.207 0.819 0.857 0.140 581 3114 (Sigma*-) -84 538 555 652 653 0 0 -0.429 1.406 4.603 5.032 1.405 582 213 (rho+) -84 538 555 654 655 0 0 -0.168 -0.899 7.020 7.129 0.846 583 -211 pi- 91 425 0 0 0 0 0 -0.128 -0.173 6.860 6.865 0.140 584 111 (pi0) -91 425 0 719 720 0 0 0.112 0.622 29.978 29.985 0.135 585 211 pi+ 91 429 0 0 0 0 0 -1.674 2.523 65.348 65.419 0.140 586 -211 pi- 91 429 0 0 0 0 0 -0.096 0.211 3.044 3.055 0.140 587 211 pi+ 91 430 0 0 0 0 0 -0.543 0.591 19.318 19.335 0.140 588 -211 pi- 91 430 0 0 0 0 0 -0.718 1.881 31.261 31.326 0.140 589 211 pi+ 91 431 0 0 0 0 0 -2.217 4.173 78.473 78.615 0.140 590 -211 pi- 91 431 0 0 0 0 0 -2.004 1.876 56.471 56.538 0.140 591 211 pi+ 91 451 0 0 0 0 0 -1.907 -0.863 -1.457 2.554 0.140 592 -211 pi- 91 451 0 0 0 0 0 -1.479 -0.456 -0.493 1.630 0.140 593 211 pi+ 91 452 0 0 0 0 0 -0.654 -0.059 -0.225 0.708 0.140 594 111 (pi0) -91 452 0 721 722 0 0 -0.731 -0.775 -0.732 1.300 0.135 595 -211 pi- 91 454 0 0 0 0 0 -0.076 -0.026 -0.095 0.187 0.140 596 111 (pi0) -91 454 0 723 724 0 0 -1.199 -1.518 0.014 1.939 0.135 597 311 (K0) -91 455 0 656 656 0 0 -0.172 -0.724 0.430 0.993 0.498 598 211 pi+ 91 455 0 0 0 0 0 -0.363 -0.426 0.814 0.998 0.140 599 -311 (Kbar0) -91 456 0 657 657 0 0 1.035 -0.260 1.162 1.654 0.498 600 -211 pi- 91 456 0 0 0 0 0 0.664 -0.708 0.636 1.169 0.140 601 211 pi+ 91 462 0 0 0 0 0 5.247 2.698 5.667 8.182 0.140 602 -211 pi- 91 462 0 0 0 0 0 0.458 0.491 0.625 0.928 0.140 603 -311 (Kbar0) -91 499 0 658 658 0 0 -0.093 0.170 0.149 0.554 0.498 604 -211 pi- 91 499 0 0 0 0 0 -0.250 -0.508 0.085 0.589 0.140 605 -211 pi- 91 506 0 0 0 0 0 -0.553 -0.198 -6.586 6.614 0.140 606 111 (pi0) -91 506 0 725 726 0 0 -0.078 0.118 -15.828 15.829 0.135 607 211 pi+ 91 507 0 0 0 0 0 -0.057 -0.232 -6.310 6.316 0.140 608 -211 pi- 91 507 0 0 0 0 0 -0.009 0.621 -4.685 4.729 0.140 609 211 pi+ 91 508 0 0 0 0 0 -0.141 -0.619 -7.208 7.237 0.140 610 -211 pi- 91 508 0 0 0 0 0 0.175 0.070 -4.545 4.551 0.140 611 211 pi+ 91 509 0 0 0 0 0 0.304 -0.348 -16.028 16.035 0.140 612 111 (pi0) -91 509 0 727 728 0 0 -0.090 0.072 -0.890 0.907 0.135 613 211 pi+ 91 511 0 0 0 0 0 -0.829 -0.595 -11.212 11.259 0.140 614 -211 pi- 91 511 0 0 0 0 0 0.318 -0.242 -6.490 6.503 0.140 615 211 pi+ 91 512 0 0 0 0 0 -0.109 0.059 -0.302 0.355 0.140 616 -211 pi- 91 512 0 0 0 0 0 0.430 1.024 -4.586 4.721 0.140 617 211 pi+ 91 513 0 0 0 0 0 0.230 0.625 -2.631 2.717 0.140 618 111 (pi0) -91 513 0 729 730 0 0 -0.420 0.409 -5.523 5.556 0.135 619 321 K+ 91 514 0 0 0 0 0 -0.592 1.501 -7.332 7.523 0.494 620 -211 pi- 91 514 0 0 0 0 0 0.009 0.332 -0.783 0.862 0.140 621 -311 (Kbar0) -91 515 0 659 659 0 0 0.518 -1.105 -6.814 6.941 0.498 622 111 (pi0) -91 515 0 731 732 0 0 0.893 -0.872 -5.507 5.648 0.135 623 -211 pi- 91 519 0 0 0 0 0 0.588 -1.043 -5.473 5.605 0.140 624 111 (pi0) -91 519 0 733 734 0 0 0.075 0.280 -1.479 1.513 0.135 625 211 pi+ 91 520 0 0 0 0 0 -0.143 -0.346 -3.801 3.822 0.140 626 -211 pi- 91 520 0 0 0 0 0 -0.143 -0.018 -0.231 0.306 0.140 627 2112 n0 91 529 0 0 0 0 0 -0.635 0.630 -1.077 1.686 0.940 628 111 (pi0) -91 529 0 735 736 0 0 -0.603 0.568 -0.457 0.956 0.135 629 211 pi+ 91 532 0 0 0 0 0 -0.301 -0.464 0.304 0.646 0.140 630 111 (pi0) -91 532 0 737 738 0 0 -0.049 -0.255 -0.321 0.435 0.135 631 -211 pi- 91 534 0 0 0 0 0 0.334 -0.477 0.335 0.687 0.140 632 111 (pi0) -91 534 0 739 740 0 0 1.199 -5.073 1.461 5.415 0.135 633 -2112 nbar0 91 535 0 0 0 0 0 1.050 -3.982 1.339 4.431 0.940 634 -211 pi- 91 535 0 0 0 0 0 0.550 -1.370 0.220 1.500 0.140 635 -211 pi- 91 556 0 0 0 0 0 0.075 0.332 0.061 0.373 0.140 636 111 (pi0) -91 556 0 741 742 0 0 0.781 -0.901 0.032 1.200 0.135 637 321 K+ 91 559 0 0 0 0 0 -0.290 0.590 4.588 4.661 0.494 638 -211 pi- 91 559 0 0 0 0 0 -0.101 -0.123 1.502 1.517 0.140 639 -211 pi- 91 560 0 0 0 0 0 0.150 0.216 69.883 69.884 0.140 640 111 (pi0) -91 560 0 743 744 0 0 -0.236 -0.195 55.946 55.947 0.135 641 311 (K0) -91 561 0 660 660 0 0 0.573 -0.652 68.635 68.643 0.498 642 211 pi+ 91 561 0 0 0 0 0 0.035 -0.128 44.008 44.008 0.140 643 211 pi+ 91 565 0 0 0 0 0 0.279 -0.072 -0.395 0.508 0.140 644 -211 pi- 91 565 0 0 0 0 0 1.637 1.116 -3.102 3.683 0.140 645 130 K_L0 91 567 567 0 0 0 0 3.293 1.085 -5.808 6.782 0.498 646 -311 (Kbar0) -91 568 0 661 661 0 0 8.970 3.340 -16.163 18.792 0.498 647 111 (pi0) -91 568 0 745 746 0 0 0.793 0.478 -1.460 1.734 0.135 648 211 pi+ 91 572 0 0 0 0 0 -0.110 0.263 -0.443 0.545 0.140 649 111 (pi0) -91 572 0 747 748 0 0 0.172 -0.271 0.032 0.349 0.135 650 -311 (Kbar0) -91 575 0 662 662 0 0 0.141 0.784 2.262 2.449 0.498 651 -211 pi- 91 575 0 0 0 0 0 0.169 -0.074 0.549 0.595 0.140 652 3122 (Lambda0) -91 581 0 749 750 0 0 -0.546 1.357 4.270 4.650 1.116 653 -211 pi- 91 581 0 0 0 0 0 0.117 0.049 0.332 0.382 0.140 654 211 pi+ 91 582 0 0 0 0 0 0.009 -0.424 1.111 1.197 0.140 655 111 (pi0) -91 582 0 751 752 0 0 -0.176 -0.475 5.909 5.932 0.135 656 310 (K_S0) -91 597 597 753 754 0 0 -0.172 -0.724 0.430 0.993 0.498 657 130 K_L0 91 599 599 0 0 0 0 1.035 -0.260 1.162 1.654 0.498 658 130 K_L0 91 603 603 0 0 0 0 -0.093 0.170 0.149 0.554 0.498 659 310 (K_S0) -91 621 621 755 756 0 0 0.518 -1.105 -6.814 6.941 0.498 660 130 K_L0 91 641 641 0 0 0 0 0.573 -0.652 68.635 68.643 0.498 661 130 K_L0 91 646 646 0 0 0 0 8.970 3.340 -16.163 18.792 0.498 662 310 (K_S0) -91 650 650 757 758 0 0 0.141 0.784 2.262 2.449 0.498 663 211 pi+ 91 407 0 0 0 0 0 -0.031 0.216 -49.106 49.106 0.140 664 -211 pi- 91 407 0 0 0 0 0 0.153 0.063 -14.299 14.301 0.140 665 111 (pi0) -91 407 0 759 760 0 0 0.528 0.239 -74.069 74.071 0.135 666 22 gamma 91 421 0 0 0 0 0 0.026 -0.221 15.317 15.318 0.000 667 22 gamma 91 421 0 0 0 0 0 0.919 -1.360 53.131 53.157 0.000 668 22 gamma 91 422 0 0 0 0 0 0.671 -0.073 31.123 31.130 0.000 669 22 gamma 91 422 0 0 0 0 0 0.065 -0.001 26.141 26.142 0.000 670 211 pi+ 91 428 0 0 0 0 0 -0.130 -0.055 6.246 6.250 0.140 671 -211 pi- 91 428 0 0 0 0 0 -0.142 0.085 4.591 4.596 0.140 672 111 (pi0) -91 428 0 761 762 0 0 -0.103 0.048 1.599 1.609 0.135 673 321 K+ 91 449 0 0 0 0 0 -12.513 -4.181 -7.301 15.087 0.494 674 -321 K- 91 449 0 0 0 0 0 -18.495 -6.068 -10.902 22.315 0.494 675 22 gamma 91 453 0 0 0 0 0 -0.186 0.270 0.020 0.328 0.000 676 22 gamma 91 453 0 0 0 0 0 0.232 0.010 -0.220 0.320 0.000 677 2212 p+ 91 460 0 0 0 0 0 0.968 -0.064 1.245 1.836 0.938 678 -211 pi- 91 460 0 0 0 0 0 0.337 0.031 0.392 0.536 0.140 679 211 pi+ 91 497 0 0 0 0 0 0.221 -0.375 0.004 0.457 0.140 680 -211 pi- 91 497 0 0 0 0 0 -0.143 0.048 -0.116 0.236 0.140 681 111 (pi0) -91 497 0 763 764 0 0 0.026 -0.064 0.112 0.188 0.135 682 211 pi+ 91 501 0 0 0 0 0 0.065 -0.013 -0.330 0.365 0.140 683 -211 pi- 91 501 0 0 0 0 0 0.228 -0.129 -1.581 1.608 0.140 684 111 (pi0) -91 501 0 765 766 0 0 0.010 -0.046 -0.294 0.327 0.135 685 211 pi+ 91 504 0 0 0 0 0 0.227 0.252 -2.459 2.486 0.140 686 -211 pi- 91 504 0 0 0 0 0 0.014 -0.028 -2.309 2.313 0.140 687 111 (pi0) -91 504 0 767 768 0 0 0.113 -0.255 -2.902 2.919 0.135 688 22 gamma 91 505 0 0 0 0 0 -0.046 -0.019 -3.648 3.648 0.000 689 22 gamma 91 505 0 0 0 0 0 0.002 0.075 -1.455 1.457 0.000 690 22 gamma 91 516 0 0 0 0 0 0.404 -0.145 -1.738 1.790 0.000 691 22 gamma 91 516 0 0 0 0 0 0.385 -0.141 -2.301 2.337 0.000 692 22 gamma 91 525 0 0 0 0 0 0.017 0.010 0.021 0.029 0.000 693 22 gamma 91 525 0 0 0 0 0 0.026 0.042 -0.198 0.204 0.000 694 22 gamma 91 527 0 0 0 0 0 -0.187 0.107 -0.397 0.451 0.000 695 22 gamma 91 527 0 0 0 0 0 -0.389 0.255 -0.513 0.693 0.000 696 211 pi+ 91 528 0 0 0 0 0 -0.475 0.222 -0.259 0.601 0.140 697 -211 pi- 91 528 0 0 0 0 0 -0.004 0.093 -0.240 0.293 0.140 698 111 (pi0) -91 528 0 769 770 0 0 -0.521 0.383 -0.076 0.665 0.135 699 211 pi+ 91 536 0 0 0 0 0 0.856 -2.353 0.647 2.590 0.140 700 -211 pi- 91 536 0 0 0 0 0 0.272 -0.972 0.498 1.134 0.140 701 111 (pi0) -91 536 0 771 772 0 0 0.955 -3.747 1.088 4.019 0.135 702 521 (B+) -91 537 0 773 777 0 0 12.147 -25.025 8.216 29.482 5.279 703 22 gamma 91 537 0 0 0 0 0 0.102 -0.149 0.091 0.202 0.000 704 211 pi+ 91 558 0 0 0 0 0 0.540 -0.236 0.538 0.810 0.140 705 -211 pi- 91 558 0 0 0 0 0 -0.077 -0.172 0.156 0.282 0.140 706 111 (pi0) -91 558 0 778 779 0 0 -0.006 -0.115 0.024 0.179 0.135 707 -12 nu_ebar 91 563 0 0 0 0 0 0.334 0.214 -0.223 0.455 0.000 708 11 e- 91 563 0 0 0 0 0 5.291 2.199 -9.374 10.987 0.001 709 423 (D*0) -91 563 0 780 781 0 0 26.766 2.792 -38.165 46.742 2.007 710 3122 (Lambda0) -91 564 0 782 783 0 0 7.577 1.584 -11.685 14.061 1.116 711 22 gamma 91 564 0 0 0 0 0 0.229 -0.016 -0.316 0.390 0.000 712 -2112 nbar0 91 566 0 0 0 0 0 4.202 1.612 -7.877 9.121 0.940 713 211 pi+ 91 566 0 0 0 0 0 2.258 0.939 -4.040 4.724 0.140 714 111 (pi0) -91 576 0 784 785 0 0 -0.055 -0.174 0.529 0.575 0.135 715 22 gamma 91 576 0 0 0 0 0 0.167 0.483 0.220 0.557 0.000 716 211 pi+ 91 579 0 0 0 0 0 0.218 0.104 0.413 0.499 0.140 717 -211 pi- 91 579 0 0 0 0 0 0.089 0.478 1.631 1.708 0.140 718 111 (pi0) -91 579 0 786 787 0 0 -0.164 0.267 0.798 0.868 0.135 719 22 gamma 91 584 0 0 0 0 0 0.030 0.489 22.873 22.878 0.000 720 22 gamma 91 584 0 0 0 0 0 0.082 0.134 7.105 7.107 0.000 721 22 gamma 91 594 0 0 0 0 0 -0.534 -0.527 -0.580 0.949 0.000 722 22 gamma 91 594 0 0 0 0 0 -0.197 -0.248 -0.152 0.351 0.000 723 22 gamma 91 596 0 0 0 0 0 -0.744 -0.858 0.049 1.137 0.000 724 22 gamma 91 596 0 0 0 0 0 -0.455 -0.660 -0.035 0.803 0.000 725 22 gamma 91 606 0 0 0 0 0 -0.081 0.141 -15.074 15.075 0.000 726 22 gamma 91 606 0 0 0 0 0 0.003 -0.022 -0.754 0.754 0.000 727 22 gamma 91 612 0 0 0 0 0 -0.030 0.038 -0.751 0.753 0.000 728 22 gamma 91 612 0 0 0 0 0 -0.059 0.033 -0.138 0.154 0.000 729 22 gamma 91 618 0 0 0 0 0 -0.342 0.248 -3.798 3.821 0.000 730 22 gamma 91 618 0 0 0 0 0 -0.078 0.160 -1.725 1.735 0.000 731 22 gamma 91 622 0 0 0 0 0 0.889 -0.851 -5.342 5.482 0.000 732 22 gamma 91 622 0 0 0 0 0 0.004 -0.021 -0.165 0.166 0.000 733 22 gamma 91 624 0 0 0 0 0 0.100 0.118 -0.661 0.678 0.000 734 22 gamma 91 624 0 0 0 0 0 -0.025 0.163 -0.818 0.835 0.000 735 22 gamma 91 628 0 0 0 0 0 -0.456 0.349 -0.287 0.642 0.000 736 22 gamma 91 628 0 0 0 0 0 -0.148 0.220 -0.170 0.314 0.000 737 22 gamma 91 630 0 0 0 0 0 -0.035 0.000 -0.058 0.067 0.000 738 22 gamma 91 630 0 0 0 0 0 -0.014 -0.255 -0.264 0.367 0.000 739 22 gamma 91 632 0 0 0 0 0 0.880 -3.785 1.148 4.052 0.000 740 22 gamma 91 632 0 0 0 0 0 0.319 -1.288 0.313 1.363 0.000 741 22 gamma 91 636 0 0 0 0 0 0.387 -0.452 -0.051 0.597 0.000 742 22 gamma 91 636 0 0 0 0 0 0.394 -0.449 0.084 0.603 0.000 743 22 gamma 91 640 0 0 0 0 0 -0.035 0.015 3.771 3.771 0.000 744 22 gamma 91 640 0 0 0 0 0 -0.201 -0.210 52.175 52.176 0.000 745 22 gamma 91 647 0 0 0 0 0 0.393 0.313 -0.758 0.909 0.000 746 22 gamma 91 647 0 0 0 0 0 0.400 0.164 -0.702 0.825 0.000 747 22 gamma 91 649 0 0 0 0 0 0.157 -0.176 -0.026 0.238 0.000 748 22 gamma 91 649 0 0 0 0 0 0.014 -0.095 0.057 0.112 0.000 749 2212 p+ 91 652 0 0 0 0 0 -0.416 1.045 3.591 3.878 0.938 750 -211 pi- 91 652 0 0 0 0 0 -0.129 0.313 0.680 0.772 0.140 751 22 gamma 91 655 0 0 0 0 0 -0.148 -0.467 5.343 5.366 0.000 752 22 gamma 91 655 0 0 0 0 0 -0.028 -0.007 0.566 0.566 0.000 753 211 pi+ 91 656 0 0 0 0 0 0.026 -0.169 0.302 0.374 0.140 754 -211 pi- 91 656 0 0 0 0 0 -0.198 -0.555 0.128 0.619 0.140 755 211 pi+ 91 659 0 0 0 0 0 0.020 -0.173 -1.828 1.842 0.140 756 -211 pi- 91 659 0 0 0 0 0 0.498 -0.933 -4.986 5.099 0.140 757 111 (pi0) -91 662 0 788 789 0 0 -0.064 0.052 0.270 0.313 0.135 758 111 (pi0) -91 662 0 790 791 0 0 0.205 0.732 1.992 2.136 0.135 759 22 gamma 91 665 0 0 0 0 0 0.131 0.029 -24.098 24.098 0.000 760 22 gamma 91 665 0 0 0 0 0 0.397 0.210 -49.971 49.973 0.000 761 22 gamma 91 672 0 0 0 0 0 -0.120 0.062 1.532 1.538 0.000 762 22 gamma 91 672 0 0 0 0 0 0.017 -0.014 0.067 0.070 0.000 763 22 gamma 91 681 0 0 0 0 0 0.005 -0.104 0.065 0.123 0.000 764 22 gamma 91 681 0 0 0 0 0 0.021 0.041 0.047 0.066 0.000 765 22 gamma 91 684 0 0 0 0 0 0.013 -0.011 0.011 0.020 0.000 766 22 gamma 91 684 0 0 0 0 0 -0.003 -0.035 -0.305 0.307 0.000 767 22 gamma 91 687 0 0 0 0 0 -0.023 -0.100 -1.064 1.069 0.000 768 22 gamma 91 687 0 0 0 0 0 0.136 -0.155 -1.838 1.850 0.000 769 22 gamma 91 698 0 0 0 0 0 -0.050 0.001 -0.027 0.057 0.000 770 22 gamma 91 698 0 0 0 0 0 -0.471 0.382 -0.049 0.608 0.000 771 22 gamma 91 701 0 0 0 0 0 0.126 -0.363 0.084 0.393 0.000 772 22 gamma 91 701 0 0 0 0 0 0.829 -3.384 1.004 3.626 0.000 773 -421 (Dbar0) -91 702 0 792 795 0 0 2.891 -6.173 2.435 7.475 1.865 774 211 pi+ 91 702 0 0 0 0 0 1.643 -3.569 0.734 3.999 0.140 775 -211 pi- 91 702 0 0 0 0 0 1.982 -4.946 1.331 5.495 0.140 776 211 pi+ 91 702 0 0 0 0 0 2.523 -4.920 2.803 6.201 0.140 777 111 (pi0) -91 702 0 796 797 0 0 3.108 -5.417 0.912 6.313 0.135 778 22 gamma 91 706 0 0 0 0 0 0.018 0.027 0.011 0.034 0.000 779 22 gamma 91 706 0 0 0 0 0 -0.024 -0.142 0.013 0.145 0.000 780 421 (D0) -91 709 0 798 799 0 0 25.327 2.617 -36.126 44.237 1.865 781 111 (pi0) -91 709 0 800 801 0 0 1.439 0.175 -2.039 2.505 0.135 782 2212 p+ 91 710 0 0 0 0 0 6.888 1.373 -10.524 12.687 0.938 783 -211 pi- 91 710 0 0 0 0 0 0.689 0.211 -1.161 1.374 0.140 784 22 gamma 91 714 0 0 0 0 0 0.022 -0.132 0.254 0.287 0.000 785 22 gamma 91 714 0 0 0 0 0 -0.077 -0.042 0.274 0.288 0.000 786 22 gamma 91 718 0 0 0 0 0 -0.107 0.250 0.561 0.623 0.000 787 22 gamma 91 718 0 0 0 0 0 -0.058 0.017 0.237 0.245 0.000 788 22 gamma 91 757 0 0 0 0 0 -0.065 0.092 0.159 0.195 0.000 789 22 gamma 91 757 0 0 0 0 0 0.001 -0.040 0.111 0.118 0.000 790 22 gamma 91 758 0 0 0 0 0 0.191 0.628 1.821 1.936 0.000 791 22 gamma 91 758 0 0 0 0 0 0.014 0.104 0.170 0.200 0.000 792 -311 (Kbar0) -91 773 0 802 802 0 0 1.075 -2.057 1.295 2.704 0.498 793 -311 (Kbar0) -91 773 0 803 803 0 0 0.370 -1.286 0.263 1.451 0.498 794 -211 pi- 91 773 0 0 0 0 0 0.265 -0.467 0.126 0.569 0.140 795 211 pi+ 91 773 0 0 0 0 0 1.182 -2.364 0.751 2.751 0.140 796 22 gamma 91 777 0 0 0 0 0 0.850 -1.539 0.203 1.770 0.000 797 22 gamma 91 777 0 0 0 0 0 2.257 -3.878 0.710 4.543 0.000 798 321 K+ 91 780 0 0 0 0 0 14.132 1.702 -21.473 25.768 0.494 799 -321 K- 91 780 0 0 0 0 0 11.195 0.915 -14.652 18.469 0.494 800 22 gamma 91 781 0 0 0 0 0 0.659 0.063 -0.819 1.053 0.000 801 22 gamma 91 781 0 0 0 0 0 0.780 0.111 -1.220 1.452 0.000 802 310 (K_S0) -91 792 792 804 805 0 0 1.075 -2.057 1.295 2.704 0.498 803 130 K_L0 91 793 793 0 0 0 0 0.370 -1.286 0.263 1.451 0.498 804 111 (pi0) -91 802 0 806 807 0 0 0.365 -1.145 0.697 1.396 0.135 805 111 (pi0) -91 802 0 808 809 0 0 0.709 -0.912 0.598 1.308 0.135 806 22 gamma 91 804 0 0 0 0 0 0.051 -0.172 0.163 0.242 0.000 807 22 gamma 91 804 0 0 0 0 0 0.315 -0.973 0.534 1.153 0.000 808 22 gamma 91 805 0 0 0 0 0 0.137 -0.146 0.052 0.207 0.000 809 22 gamma 91 805 0 0 0 0 0 0.573 -0.765 0.547 1.101 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 0.000 1960.000 1960.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame PYTHIA Warning in TimeShower::findMEcorr: ME weight above PS one PYTHIA Abort from Pythia::next: reached end of Les Houches Events File *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> t tbar 601 | 244 9 9 | 2.680e-10 3.892e-11 | | q qbar -> t tbar 602 | 3400 165 165 | 5.666e-09 1.937e-10 | | Les Houches User Process(es) 9999 | 200 200 200 | 5.480e-09 5.488e-10 | | ... whereof user classification code 81 | 192 192 192 | | | ... whereof user classification code 82 | 8 8 8 | | | | | | | sum | 3844 374 374 | 1.141e-08 5.833e-10 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 2 Abort from Pythia::next: reached end of Les Houches Events File | | 4 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | 1 Warning in TimeShower::findMEcorr: ME weight above PS one | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:03 charged particle multiplicity 1.84*10^ 1 5 5 1.76*10^ 1 3 X 3X 1.68*10^ 1 X X XX 1.60*10^ 1 X X XXXX 1.52*10^ 1 X X XXXX8 1.44*10^ 1 X5 X 5 XXXXX5 1.36*10^ 1 3 XX X X XXXXXX 3 1.28*10^ 1 X XX X X XXXXXX X 1.20*10^ 1 X XXX X XX XXXXXX X 1.12*10^ 1 8X XXX8X8XX XXXXXX X 8 1.04*10^ 1 XX XXXXXXXX XXXXXX5X X 0.96*10^ 1 XX XXXXXXXX XXXXXXXX X 0.88*10^ 1 XX XXXXXXXX XXXXXXXX X 0.80*10^ 1 XX XXXXXXXXXXXXXXXXXXX XX 0.72*10^ 1 XX8XXXXXXXXXXXXXXXXXXX XX 0.64*10^ 1 XXXXXXXXXXXXXXXXXXXXXX5XX 5 0.56*10^ 1 22 XXXXXXXXXXXXXXXXXXXXXXXXX 2X2 2 0.48*10^ 1 XX XXXXXXXXXXXXXXXXXXXXXXXXX XXX X 0.40*10^ 1 XXX XXXXXXXXXXXXXXXXXXXXXXXXXXX XXX X 0.32*10^ 1 XXX7XXXXXXXXXXXXXXXXXXXXXXXXXXX7XXX X7 0.24*10^ 1 5 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 5 5 0.16*10^ 1 X2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2XX22X22X 2 2 0.08*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X Contents *10^ 1 0000000000000000000011011111111011111111010000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000000002145534413727418124866785403816883565153112112000010100000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000000000000000111111111111111111111111122222222222222222222222223333333333333333333333333 *10^ 1 0001122233444556667788899000112223344455666778889900011222334445566677888990001122233444556667788899 *10^ 0 1482604826048260482604826048260482604826048260482604826048260482604826048260482604826048260482604826 Entries = 374 Mean = 1.3026e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 3.7400e+02 Rms = 3.8280e+01 Overflow = 0.0000e+00 High edge = 3.9950e+02 pythia8-8.1.80.orig/examples/outref/out030000644000175000017500000014435512217346170016367 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:00:21 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> g g 111 | 1.252e-01 | | g g -> q qbar (uds) 112 | 1.483e-03 | | q g -> q g 113 | 1.005e-01 | | q q(bar)' -> q q(bar)' 114 | 1.148e-02 | | q qbar -> g g 115 | 8.118e-05 | | q qbar -> q' qbar' (uds) 116 | 3.858e-05 | | g g -> c cbar 121 | 4.935e-04 | | q qbar -> c cbar 122 | 1.285e-05 | | g g -> b bbar 123 | 4.851e-04 | | q qbar -> b bbar 124 | 1.273e-05 | | q g -> q gamma (udscb) 201 | 3.386e-05 | | q qbar -> g gamma 202 | 2.496e-06 | | g g -> g gamma 203 | 1.124e-08 | | f fbar -> gamma gamma 204 | 2.014e-08 | | g g -> gamma gamma 205 | 9.624e-09 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 57.54 mb | | | | pT0 = 3.17 gives sigmaInteraction = 253.30 mb: accepted | | | | x-dependent matter profile: a1 = 0.15, a0 = 0.26, bStep = 0.02 | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | HardQCD:all | on | off | | Init:showChangedParticleData | off | on | | Main:timesAllowErrors | 3 | 10 0 | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 4 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | Next:numberCount | 100 | 1000 0 | | Next:numberShowEvent | 0 | 1 0 | | ParticleDecays:limitTau0 | on | off | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:pTHatMin | 50.00000 | 0.0 0.0 | | PromptPhoton:all | on | off | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | Tune:pp | 6 | 5 -1 13 | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. In 1: id = 21, x = 2.271e-02, pdf = 4.363e+00 at Q2 = 2.822e+03. In 2: id = 21, x = 8.902e-03, pdf = 9.011e+00 at same Q2. Subprocess g g -> g g with code 111 is 2 -> 2. It has sHat = 3.963e+04, tHat = -3.058e+03, uHat = -3.657e+04, pTHat = 5.312e+01, m3Hat = 0.000e+00, m4Hat = 0.000e+00, thetaHat = 5.630e-01, phiHat = 5.710e+00. alphaEM = 7.770e-03, alphaS = 1.482e-01 at Q2 = 2.822e+03. Impact parameter b = 6.620e-01 gives enhancement factor = 1.796e+00. Max pT scale for MPI = 5.312e+01, ISR = 5.312e+01, FSR = 5.312e+01. Number of MPI = 12, ISR = 36, FSRproc = 192, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 21 (g) -21 1 0 5 6 101 102 0.000 0.000 158.976 158.976 0.000 4 21 (g) -21 2 0 5 6 103 104 0.000 0.000 -62.317 62.317 0.000 5 21 g 23 3 4 0 0 101 104 44.625 -28.817 141.901 151.518 0.000 6 21 g 23 3 4 0 0 103 102 -44.625 28.817 -45.242 69.775 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 96.659 221.293 199.066 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Warning in MultipartonInteractions::pTnext: weight above unity PYTHIA Error in StringFragmentation::fragment: stuck in joining PYTHIA Error in Pythia::next: hadronLevel failed; try again Pythia::next(): 100 events have been generated Pythia::next(): 200 events have been generated Pythia::next(): 300 events have been generated Pythia::next(): 400 events have been generated PYTHIA Error in Pythia::check: unmatched particle energy/momentum/mass PYTHIA Error in Pythia::next: check of event revealed problems Pythia::next(): 500 events have been generated Pythia::next(): 600 events have been generated PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame PYTHIA Warning in SpaceShower::pT2nextQCD: weight above unity Pythia::next(): 700 events have been generated Pythia::next(): 800 events have been generated Pythia::next(): 900 events have been generated *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> g g 111 | 4405 534 534 | 1.599e-02 3.416e-04 | | g g -> q qbar (uds) 112 | 41 6 6 | 3.491e-04 5.508e-05 | | q g -> q g 113 | 3502 400 400 | 1.137e-02 3.188e-04 | | q q(bar)' -> q q(bar)' 114 | 349 47 47 | 1.532e-03 1.281e-04 | | q qbar -> g g 115 | 3 1 1 | 2.552e-05 2.552e-05 | | q qbar -> q' qbar' (uds) 116 | 4 2 2 | 1.507e-05 7.424e-06 | | g g -> c cbar 121 | 20 4 4 | 6.811e-05 2.401e-05 | | q qbar -> c cbar 122 | 0 0 0 | 0.000e+00 0.000e+00 | | g g -> b bbar 123 | 20 5 5 | 1.312e-04 2.577e-05 | | q qbar -> b bbar 124 | 1 0 0 | 0.000e+00 0.000e+00 | | q g -> q gamma (udscb) 201 | 1 1 1 | 1.238e-05 1.238e-05 | | q qbar -> g gamma 202 | 0 0 0 | 0.000e+00 0.000e+00 | | g g -> g gamma 203 | 0 0 0 | 0.000e+00 0.000e+00 | | f fbar -> gamma gamma 204 | 0 0 0 | 0.000e+00 0.000e+00 | | g g -> gamma gamma 205 | 0 0 0 | 0.000e+00 0.000e+00 | | | | | | sum | 8346 1000 1000 | 2.950e-02 4.897e-04 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Error in Pythia::check: unmatched particle energy/momentum/mass | | 1 Error in Pythia::next: check of event revealed problems | | 2 Error in Pythia::next: hadronLevel failed; try again | | 2 Error in StringFragmentation::fragment: stuck in joining | | 1 Warning in MultipartonInteractions::pTnext: weight above unity | | 2 Warning in SpaceShower::pT2nextQCD: weight above unity | | 1 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:01 process pT scale 3.24*10^ 2 9 3.12*10^ 2 X 3.00*10^ 2 X 2.88*10^ 2 X 2.76*10^ 2 X 2.64*10^ 2 X 2.52*10^ 2 X 2.40*10^ 2 X 2.28*10^ 2 X 2.16*10^ 2 X1 2.04*10^ 2 XX 1.92*10^ 2 XX 1.80*10^ 2 XX 1.68*10^ 2 XX 1.56*10^ 2 XX 1.44*10^ 2 XX 1.32*10^ 2 XX9 1.20*10^ 2 XXX 1.08*10^ 2 XXX3 0.96*10^ 2 XXXX 0.84*10^ 2 XXXX 0.72*10^ 2 XXXX 0.60*10^ 2 XXXXX2 0.48*10^ 2 XXXXXX 0.36*10^ 2 XXXXXX9 0.24*10^ 2 XXXXXXX8322 0.12*10^ 2 XXXXXXXXXXX32413 1321121 1 1 1 Contents *10^ 2 0000000000321000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0000000000203965321110000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0000000000351901526444251401321121010001000000001000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 2 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^ 1 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^ 0 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 1000 Mean = 6.5165e+01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+03 Rms = 1.8220e+01 Overflow = 0.0000e+00 High edge = 5.0000e+02 2013-09-20 16:01 final particle multiplicity 4.50*10^ 1 3 3 4.35*10^ 1 X X 4.20*10^ 1 X X 4.05*10^ 1 X 7 X 3.90*10^ 1 X 3XXX X 3.75*10^ 1 X7 XXXX X 7 3.60*10^ 1 XX3 XXXXXXX3X 3.45*10^ 1 XXX 7XXXXXXXXX 3.30*10^ 1 3 XXX XXXXXXXXXX 3.15*10^ 1 7 X7XXX7XXXXXXXXXX 3.00*10^ 1 X XXXXXXXXXXXXXXXX 2.85*10^ 1 X XXXXXXXXXXXXXXXX 2.70*10^ 1 X XXXXXXXXXXXXXXXX 2.55*10^ 1 X XXXXXXXXXXXXXXXX 2.40*10^ 1 X XXXXXXXXXXXXXXXX X X 2.25*10^ 1 X XXXXXXXXXXXXXXXX7X X7 2.10*10^ 1 3 X XXXXXXXXXXXXXXXXXXX3XX 1.95*10^ 1 7X X7XXXXXXXXXXXXXXXXXXXXXX 1.80*10^ 1 XXX XXXXXXXXXXXXXXXXXXXXXXXX 1.65*10^ 1 XXX XXXXXXXXXXXXXXXXXXXXXXXX 1.50*10^ 1 XXX3XXXXXXXXXXXXXXXXXXXXXXXX 1.35*10^ 1 77 XXXXXXXXXXXXXXXXXXXXXXXXXXXX 7 1.20*10^ 1 3XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 3 1.05*10^ 1 XXX7XXXXXXXXXXXXXXXXXXXXXXXXXXXXX X X7 0.90*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 0.75*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 7 0.60*10^ 1 XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X3 0.45*10^ 1 7XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX XX 0.30*10^ 1 XXX3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.15*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7777 7 Contents *10^ 1 0000000000011111211312334333333433433322222101011000000000000000000000000000000000000000000000000000 *10^ 0 0000000466213309084191214751489096465724042293610663751111000000000100000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^ 3 0000000000000000000000000000000000000000000000000000000000000001111111111111111111111111111111111111 *10^ 2 0000001111111222222333333444444555555566666677777788888899999990000001111112222223333333444444555555 *10^ 1 0235680134689124679024578023568013468912467902457802356801346891246790245780235680134689124679024578 Entries = 1000 Mean = 4.8196e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+03 Rms = 1.5817e+02 Overflow = 0.0000e+00 High edge = 1.5995e+03 2013-09-20 16:01 charged particle multiplicity 4.60*10^ 1 5 X X 4.40*10^ 1 X 5X X 4.20*10^ 1 X XX XX 4.00*10^ 1 5 XX XXX 5XX 3.80*10^ 1 X XX XXXX XXX 3.60*10^ 1 X XX XXXX XXX 3.40*10^ 1 X XXXXXXXXXXX 3.20*10^ 1 5X XXXXXXXXXXX 3.00*10^ 1 XXXXXXXXXXXXXX5X 2.80*10^ 1 XXXXXXXXXXXXXXXX XX 2.60*10^ 1 X XXXXXXXXXXXXXXXX5XX 2.40*10^ 1 XX XXXXXXXXXXXXXXXXXXX X 2.20*10^ 1 XXX5XXXXXXXXXXXXXXXXXXX X 2.00*10^ 1 5 XXXXXXXXXXXXXXXXXXXXXXXXX 1.80*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXX 1.60*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXX 1.40*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 5 1.00*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X5 0.80*10^ 1 55XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 5 0.60*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X 5 0.40*10^ 1 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 5 0.20*10^ 1 5XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5XX5 5 Contents *10^ 1 0000000000111111222233344344433344232222210100000000000000000000000000000000000000000000000000000000 *10^ 0 0000001377022498642119005436084962905880408197474512310000000010000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000111111111111222222222222233333333333344444444444445555555555556666666666666777777777777 *10^ 1 0012344567889012234566789001234456788901223456678900123445678890122345667890012344567889012234566789 *10^ 0 1864208642086420864208642086420864208642086420864208642086420864208642086420864208642086420864208642 Entries = 1000 Mean = 2.2395e+02 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+03 Rms = 7.3543e+01 Overflow = 0.0000e+00 High edge = 7.9950e+02 2013-09-20 16:01 dn/dy for charged particles 2.70*10^ 1 2 2.60*10^ 1 35X7X44 4 2.50*10^ 1 29XXXXXXX97X 2.40*10^ 1 67XXXXXXXXXXXXXX5 2.30*10^ 1 23XXXXXXXXXXXXXXXXXX8 2.20*10^ 1 15XXXXXXXXXXXXXXXXXXXXX5 2.10*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXX61 2.00*10^ 1 9XXXXXXXXXXXXXXXXXXXXXXXXXXX1 1.90*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.80*10^ 1 56XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 1.70*10^ 1 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX33 1.60*10^ 1 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 1.50*10^ 1 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX1 1.40*10^ 1 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 1.30*10^ 1 9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 1.20*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.10*10^ 1 9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 1.00*10^ 1 49XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 0.90*10^ 1 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 0.80*10^ 1 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.70*10^ 1 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 0.60*10^ 1 17XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX62 0.50*10^ 1 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 0.40*10^ 1 39XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX92 0.30*10^ 1 156XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX74 0.20*10^ 1 2458XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX98641 0.10*10^ 1 1113358XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX87543111 Contents *10^ 1 0000000000000000000000000011111111111222222222222222222222222222111111111110000000000000000000000000 *10^ 0 0000000001111222334556789902234567799112233344555565544543321000976654322009876554332211111000000000 *10^-1 0001235891348146283178363890866274509042257918259713396304085600053331760942775622916397641875331000 *10^-2 4684854166550192759510458722624877921981554858819278829959454590931290571978931407366837211221641965 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 223422 Mean = -1.0577e-02 Underflow = 2.0000e-02 Low edge = -1.0000e+01 All chan = 1.1171e+03 Rms = 3.2450e+00 Overflow = 3.0000e-02 High edge = 1.0000e+01 2013-09-20 16:01 dn/d(eta) for charged particles 2.40*10^ 1 4 22 2.32*10^ 1 2541X538385 72XX534 2.24*10^ 1 85XXXXXXXXXXX9XXXXXXX 2.16*10^ 1 67XXXXXXXXXXXXXXXXXXXXX3 2.08*10^ 1 3XXXXXXXXXXXXXXXXXXXXXXXX625 2.00*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.92*10^ 1 7XXXXXXXXXXXXXXXXXXXXXXXXXXXX9 1.84*10^ 1 1XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX6 1.76*10^ 1 6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.68*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 1.60*10^ 1 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 1.52*10^ 1 9XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 1.44*10^ 1 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 1.36*10^ 1 28XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 1.28*10^ 1 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 1.20*10^ 1 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9 1.12*10^ 1 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 1.04*10^ 1 7XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.96*10^ 1 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX8 0.88*10^ 1 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.80*10^ 1 2XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX3 0.72*10^ 1 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.64*10^ 1 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.56*10^ 1 3XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4 0.48*10^ 1 4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX5 0.40*10^ 1 26XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX7 0.32*10^ 1 27XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX41 0.24*10^ 1 47XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX42 0.16*10^ 1 549XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX9521 0.08*10^ 1 224578XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX895432 Contents *10^ 1 0000000000000000000000001111111111112222222222222222222222222222111111111111000000000000000000000000 *10^ 0 0000000111112223345567890012345577880112222223223232222332221000986654332100987655433221111100000000 *10^-1 1124568114591594730873312549411726492232058755860607396337670523107688955891434661472749765298664321 *10^-2 6881461829605730227253420877281354385551354526156776050487022007087830274886813912291145544047381137 Low edge -------------------------------------------------- *10^ 1 1000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0999998888877777666665555544444333332222211111000000000111112222233333444445555566666777778888899999 *10^-1 0864208642086420864208642086420864208642086420864202468024680246802468024680246802468024680246802468 Entries = 223422 Mean = -1.1071e-02 Underflow = 3.4500e-01 Low edge = -1.0000e+01 All chan = 1.1164e+03 Rms = 3.4151e+00 Overflow = 3.2500e-01 High edge = 1.0000e+01 2013-09-20 16:01 dn/dpT for charged particles 3.00*10^ 2 1 2.90*10^ 2 X 2.80*10^ 2 X 2.70*10^ 2 X 2.60*10^ 2 7X7 2.50*10^ 2 XXX 2.40*10^ 2 XXX 2.30*10^ 2 XXX 2.20*10^ 2 XXX2 2.10*10^ 2 XXXX 2.00*10^ 2 XXXX 1.90*10^ 2 XXXX 1.80*10^ 2 XXXX2 1.70*10^ 2 XXXXX 1.60*10^ 2 XXXXX 1.50*10^ 2 XXXXX 1.40*10^ 2 XXXXX6 1.30*10^ 2 6XXXXXX 1.20*10^ 2 XXXXXXX 1.10*10^ 2 XXXXXXX7 1.00*10^ 2 XXXXXXXX 0.90*10^ 2 XXXXXXXX5 0.80*10^ 2 XXXXXXXXX 0.70*10^ 2 XXXXXXXXXX 0.60*10^ 2 XXXXXXXXXX7 0.50*10^ 2 XXXXXXXXXXX92 0.40*10^ 2 XXXXXXXXXXXXX71 0.30*10^ 2 XXXXXXXXXXXXXXX73 0.20*10^ 2 XXXXXXXXXXXXXXXXXX86421 0.10*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXX97766554444333322232222221111111111111111111111111111111 1 11 1 Contents *10^ 2 1222211100000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 2595173086544332211111100000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 6707215749791616397532099876655444433222222221211111111111111110011000000000000000000000000000000000 *10^-1 4152165179106745586975967647451731294889541629198754543220111119800777778767966564556544534434443333 Low edge *10^ 0 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-1 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 223422 Mean = 8.3081e-01 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 2.2179e+03 Rms = 1.1040e+00 Overflow = 1.6300e+01 High edge = 1.0000e+01 2013-09-20 16:01 deviation from energy-momentum conservation 1.00*10^ 3 X 0.96*10^ 3 X 0.92*10^ 3 X 0.88*10^ 3 X 0.84*10^ 3 X 0.80*10^ 3 X 0.76*10^ 3 X 0.72*10^ 3 X 0.68*10^ 3 X 0.64*10^ 3 X 0.60*10^ 3 X 0.56*10^ 3 X 0.52*10^ 3 X 0.48*10^ 3 X 0.44*10^ 3 X 0.40*10^ 3 X 0.36*10^ 3 X 0.32*10^ 3 X 0.28*10^ 3 X 0.24*10^ 3 X 0.20*10^ 3 X 0.16*10^ 3 X 0.12*10^ 3 X 0.08*10^ 3 X 0.04*10^ 3 X Contents *10^ 2 9000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 9000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 0 8000010010000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge *10^-7 0000000000111111111122222222223333333333444444444455555555556666666666777777777788888888889999999999 *10^-8 0123456789012345678901234567890123456789012345678901234567890123456789012345678901234567890123456789 *10^-9 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 1000 Mean = 5.1300e-09 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 1.0000e+03 Rms = 2.9805e-09 Overflow = 0.0000e+00 High edge = 1.0000e-06 pythia8-8.1.80.orig/examples/outref/out180000644000175000017500000157310012217346173016373 0ustar sunsun *------------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------* | | | | | | | | | | | PPP Y Y TTTTT H H III A Welcome to the Lund Monte Carlo! | | | | P P Y Y T H H I A A This is PYTHIA version 8.180 | | | | PPP Y T HHHHH I AAAAA Last date of change: 20 Sep 2013 | | | | P Y T H H I A A | | | | P Y T H H III A A Now is 20 Sep 2013 at 16:05:50 | | | | | | | | Torbjorn Sjostrand; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | phone: + 46 - 46 - 222 48 16; e-mail: torbjorn@thep.lu.se | | | | Jesper Roy Christiansen; Department of Astronomy and Theoretical Physics, | | | | Lund University, Solvegatan 14A, SE-223 62 Lund, Sweden; | | | | e-mail: Jesper.Roy.Christiansen@thep.lu.se | | | | Nishita Desai; Department of Physics and Astronomy, University College | | | | London, Gower Street, London, WC1E 6BT, United Kingdom; | | | | e-mail: Nishita.Desai@cern.ch | | | | Philip Ilten; School of Physics, Uniiversity College Dublin, | | | | Belfield, Dublin 4, Ireland; | | | | e-mail: philten@cern.ch | | | | Stephen Mrenna; Computing Division, Simulations Group, | | | | Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA; | | | | phone: + 1 - 630 - 840 - 2556; e-mail: mrenna@fnal.gov | | | | Stefan Prestel; Theory Group, DESY, | | | | Notkestrasse 85, D-22607 Hamburg, Germany; | | | | phone: + 49 - 40 - 8998-4250; e-mail: stefan.prestel@thep.lu.se | | | | Peter Skands; Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland; | | | | phone: + 41 - 22 - 767 2447; e-mail: peter.skands@cern.ch | | | | Stefan Ask; former author; e-mail: ask.stefan@gmail.com | | | | Richard Corke; former author; e-mail: r.corke@errno.net | | | | | | | | The main program reference is the 'Brief Introduction to PYTHIA 8.1', | | | | T. Sjostrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 85 | | | | [arXiv:0710.3820] | | | | | | | | The main physics reference is the 'PYTHIA 6.4 Physics and Manual', | | | | T. Sjostrand, S. Mrenna and P. Skands, JHEP05 (2006) 026 [hep-ph/0603175]. | | | | | | | | An archive of program versions and documentation is found on the web: | | | | http://www.thep.lu.se/~torbjorn/Pythia.html | | | | | | | | This program is released under the GNU General Public Licence version 2. | | | | Please respect the MCnet Guidelines for Event Generator Authors and Users. | | | | | | | | Disclaimer: this program comes without any guarantees. | | | | Beware of errors and use common sense when interpreting results. | | | | | | | | Copyright (C) 2013 Torbjorn Sjostrand | | | | | | | | | | | *------------------------------------------------------------------------------* | | | *------------------------------------------------------------------------------------* *------- PYTHIA Process Initialization --------------------------* | | | We collide p+ with p+ at a CM energy of 1.400e+04 GeV | | | |------------------------------------------------------------------| | | | | Subprocess Code | Estimated | | | max (mb) | | | | |------------------------------------------------------------------| | | | | g g -> g g 111 | 5.045e-03 | | g g -> q qbar (uds) 112 | 7.366e-05 | | q g -> q g 113 | 7.288e-03 | | q q(bar)' -> q q(bar)' 114 | 9.156e-04 | | q qbar -> g g 115 | 6.857e-06 | | q qbar -> q' qbar' (uds) 116 | 3.497e-06 | | g g -> c cbar 121 | 2.454e-05 | | q qbar -> c cbar 122 | 1.165e-06 | | g g -> b bbar 123 | 2.443e-05 | | q qbar -> b bbar 124 | 1.163e-06 | | | *------- End PYTHIA Process Initialization -----------------------* *------- PYTHIA Multiparton Interactions Initialization ---------* | | | sigmaNonDiffractive = 57.54 mb | | | | pT0 = 3.08 gives sigmaInteraction = 271.14 mb: accepted | | | *------- End PYTHIA Multiparton Interactions Initialization -----* *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings (changes only) --------------------------------* | | | Name | Now | Default Min Max | | | | | | BeamRemnants:reconnectRange | 1.50000 | 10.00000 0.0 10.00000 | | HardQCD:all | on | off | | MultipartonInteractions:alphaSvalue | 0.13500 | 0.12700 0.0600000 0.25000 | | MultipartonInteractions:bProfile | 3 | 1 0 4 | | MultipartonInteractions:ecmPow | 0.19000 | 0.24000 0.0 0.50000 | | MultipartonInteractions:expPow | 2.00000 | 1.00000 0.40000 10.00000 | | MultipartonInteractions:pT0Ref | 2.08500 | 2.15000 0.50000 10.00000 | | Next:numberShowEvent | 0 | 1 0 | | Next:numberShowInfo | 0 | 1 0 | | Next:numberShowProcess | 0 | 1 0 | | PDF:pSet | 8 | 2 1 16 | | PhaseSpace:pTHatMin | 100.00000 | 0.0 0.0 | | SigmaDiffractive:dampen | on | off | | SigmaDiffractive:maxAX | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXB | 65.00000 | 15.00000 0.0 | | SigmaDiffractive:maxXX | 65.00000 | 15.00000 0.0 | | SigmaProcess:alphaSvalue | 0.13500 | 0.12650 0.0600000 0.25000 | | SigmaTotal:zeroAXB | on | off | | SpaceShower:rapidityOrder | on | off | | | *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec Settings -------------------------------------------* -------- PYTHIA Particle Data Table (changed only) ------------------------------------------------------------------------------ id name antiName spn chg col m0 mWidth mMin mMax tau0 res dec ext vis wid no onMode bRatio meMode products no particle data has been changed from its default value -------- End PYTHIA Particle Data Table ----------------------------------------------------------------------------------------- -------- PYTHIA Info Listing ---------------------------------------- Beam A: id = 2212, pz = 7.000e+03, e = 7.000e+03, m = 9.383e-01. Beam B: id = 2212, pz = -7.000e+03, e = 7.000e+03, m = 9.383e-01. In 1: id = 21, x = 1.695e-02, pdf = 5.545e+00 at Q2 = 1.210e+04. In 2: id = 21, x = 2.642e-02, pdf = 3.742e+00 at same Q2. Subprocess g g -> g g with code 111 is 2 -> 2. It has sHat = 8.781e+04, tHat = -7.331e+04, uHat = -1.450e+04, pTHat = 1.100e+02, m3Hat = 0.000e+00, m4Hat = 0.000e+00, thetaHat = 2.305e+00, phiHat = 7.739e-01. alphaEM = 7.834e-03, alphaS = 1.310e-01 at Q2 = 1.210e+04. Impact parameter b = 3.992e-01 gives enhancement factor = 2.738e+00. Max pT scale for MPI = 1.100e+02, ISR = 1.100e+02, FSR = 1.100e+02. Number of MPI = 14, ISR = 29, FSRproc = 301, FSRreson = 0. -------- End PYTHIA Info Listing ------------------------------------ -------- PYTHIA Event Listing (hard process) ----------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 3 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 4 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 21 (g) -21 1 0 5 6 102 101 0.000 0.000 118.684 118.684 0.000 4 21 (g) -21 2 0 5 6 104 103 0.000 0.000 -184.958 184.958 0.000 5 21 g 23 3 4 0 0 104 101 78.679 76.889 -134.832 174.017 0.000 6 21 g 23 3 4 0 0 102 103 -78.679 -76.889 68.559 129.625 0.000 Charge sum: 0.000 Momentum sum: 0.000 0.000 -66.273 303.642 296.321 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (complete event) --------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 0 90 (system) -11 0 0 0 0 0 0 0.000 0.000 0.000 14000.000 14000.000 1 2212 (p+) -12 0 0 1212 0 0 0 0.000 0.000 7000.000 7000.000 0.938 2 2212 (p+) -12 0 0 1213 0 0 0 0.000 0.000 -7000.000 7000.000 0.938 3 21 (g) -21 7 0 5 6 102 101 0.000 0.000 118.684 118.684 0.000 4 21 (g) -21 8 8 5 6 104 103 0.000 0.000 -184.958 184.958 0.000 5 21 (g) -23 3 4 9 9 104 101 78.679 76.889 -134.832 174.017 0.000 6 21 (g) -23 3 4 10 10 102 103 -78.679 -76.889 68.559 129.625 0.000 7 21 (g) -41 14 14 11 3 102 105 0.000 0.000 157.862 157.862 0.000 8 21 (g) -42 16 0 4 4 104 103 -0.000 0.000 -184.958 184.958 0.000 9 21 (g) -44 5 5 17 17 104 101 82.514 71.305 -113.068 157.090 0.000 10 21 (g) -44 6 6 12 13 102 103 -59.283 -105.133 78.609 144.038 0.000 11 21 (g) -43 7 0 19 19 101 105 -23.231 33.829 7.363 41.692 0.000 12 21 (g) -51 10 0 18 18 106 103 -60.827 -105.645 80.967 146.344 0.000 13 21 (g) -51 10 0 20 20 102 106 1.544 0.512 25.376 25.429 0.000 14 21 (g) -53 15 15 7 7 102 105 0.000 0.000 185.597 185.597 0.000 15 21 (g) -42 25 25 14 14 102 105 0.000 0.000 185.597 185.597 0.000 16 21 (g) -41 26 0 21 8 107 103 -0.000 -0.000 -203.631 203.631 0.000 17 21 (g) -44 9 9 27 27 104 101 77.194 60.569 -121.942 156.517 0.000 18 21 (g) -44 12 12 24 24 106 103 -62.114 -108.243 81.872 149.258 0.000 19 21 (g) -44 11 11 29 29 101 105 -23.907 32.464 5.277 40.661 0.000 20 21 (g) -44 13 13 22 23 102 106 1.543 0.510 24.569 24.623 0.000 21 21 (g) -43 16 0 31 31 107 104 7.284 14.700 -7.810 18.170 0.000 22 21 (g) -51 20 0 30 30 102 108 -4.613 4.813 18.967 20.105 0.000 23 21 (g) -51 20 0 32 32 108 106 -9.655 -31.854 26.441 42.509 0.000 24 21 (g) -52 18 18 28 28 106 103 -46.304 -80.692 61.033 111.267 0.000 25 21 (g) -42 62 0 15 15 102 105 0.000 0.000 185.597 185.597 0.000 26 2 (u) -41 63 63 33 16 107 0 -0.000 -0.000 -648.985 648.985 0.000 27 21 (g) -44 17 17 39 39 104 101 85.991 61.635 -119.389 159.521 0.000 28 21 (g) -44 24 24 36 36 106 103 -44.717 -80.500 59.109 109.424 0.000 29 21 (g) -44 19 19 37 38 101 105 -22.789 32.600 4.599 40.040 0.000 30 21 (g) -44 22 22 67 67 102 108 -4.577 4.817 18.808 19.948 0.000 31 21 (g) -44 21 21 68 68 107 104 8.104 14.800 -7.541 18.482 0.000 32 21 (g) -44 23 23 69 69 108 106 -9.147 -31.792 25.954 42.048 0.000 33 2 (u) -43 26 0 34 35 103 0 -12.866 -1.560 -444.929 445.118 0.330 34 2 (u) -51 33 0 70 70 109 0 -20.645 -5.357 -427.313 427.845 0.330 35 21 (g) -51 33 0 71 71 103 109 7.237 2.821 -16.900 18.600 0.000 36 21 (g) -52 28 28 65 65 106 103 -44.175 -79.524 58.393 108.098 0.000 37 21 (g) -51 29 0 66 66 110 105 -19.419 14.316 2.648 24.270 0.000 38 21 (g) -51 29 0 72 72 101 110 -1.103 19.909 -1.196 19.975 0.000 39 21 (g) -52 27 27 64 64 104 101 83.725 60.011 -116.242 155.317 0.000 40 1 (d) -31 53 53 42 43 111 0 0.000 0.000 83.571 83.571 0.000 41 21 (g) -31 54 0 42 43 112 113 0.000 0.000 -10.026 10.026 0.000 42 1 (d) -33 40 41 55 55 112 0 6.229 5.692 81.539 81.975 0.330 43 21 (g) -33 40 41 56 56 111 113 -6.229 -5.692 -7.993 11.623 0.000 44 21 (g) -31 48 48 46 47 115 114 0.000 0.000 7.145 7.145 0.000 45 21 (g) -31 49 0 46 47 116 115 0.000 0.000 -103.394 103.394 0.000 46 21 (g) -33 44 45 50 50 117 114 -7.645 -1.592 4.815 9.174 0.000 47 21 (g) -33 44 45 51 51 116 117 7.645 1.592 -101.064 101.365 0.000 48 21 (g) -42 355 355 44 44 115 114 0.000 -0.000 7.145 7.145 0.000 49 21 (g) -41 366 0 52 45 118 115 0.000 0.000 -204.282 204.282 0.000 50 21 (g) -44 46 46 102 102 117 114 -7.756 -1.632 4.823 9.278 0.000 51 21 (g) -44 47 47 100 101 116 117 2.484 -0.263 -103.426 103.457 0.000 52 21 (g) -43 49 0 231 231 118 116 5.272 1.895 -98.533 98.692 0.000 53 1 (d) -42 296 0 40 40 111 0 -0.000 0.000 83.571 83.571 0.000 54 21 (g) -41 138 138 57 41 119 113 0.000 -0.000 -22.925 22.925 0.000 55 1 (d) -44 42 42 94 95 112 0 6.117 5.727 79.171 79.614 0.330 56 21 (g) -44 43 43 136 137 111 113 -11.266 -4.093 -6.356 13.568 0.000 57 21 (g) -43 54 0 96 96 119 112 5.149 -1.634 -12.170 13.315 0.000 58 21 (g) -31 506 506 60 61 121 120 0.000 0.000 60.285 60.285 0.000 59 21 (g) -31 441 441 60 61 123 122 0.000 0.000 -0.476 0.476 0.000 60 21 (g) -33 58 59 504 505 123 120 3.895 3.567 24.915 25.468 0.000 61 21 (g) -33 58 59 439 440 121 122 -3.895 -3.567 34.895 35.292 0.000 62 21 (g) -41 143 0 73 25 102 124 0.000 0.000 446.669 446.669 0.000 63 2 (u) -42 144 144 26 26 107 0 -0.000 0.000 -648.985 648.985 0.000 64 21 (g) -44 39 39 135 135 104 101 83.996 59.529 -116.072 155.150 0.000 65 21 (g) -44 36 36 99 99 106 103 -43.021 -81.575 57.714 108.794 0.000 66 21 (g) -44 37 37 147 147 110 105 -19.232 13.985 2.958 23.962 0.000 67 21 (g) -44 30 30 76 76 102 108 -4.308 4.340 18.897 19.862 0.000 68 21 (g) -44 31 31 149 149 107 104 8.180 14.665 -7.414 18.356 0.000 69 21 (g) -44 32 32 74 75 108 106 -8.676 -32.630 25.623 42.385 0.000 70 2 (u) -44 34 34 123 123 109 0 -20.641 -5.363 -427.194 427.726 0.330 71 21 (g) -44 35 35 97 98 103 109 7.249 2.800 -16.914 18.614 0.000 72 21 (g) -44 38 38 133 134 101 110 -0.973 19.677 -0.943 19.724 0.000 73 21 (g) -43 62 0 154 154 105 124 -2.573 4.572 261.028 261.080 0.000 74 21 (g) -51 69 0 150 150 125 106 -6.990 -19.697 10.880 23.563 0.000 75 21 (g) -51 69 0 155 155 108 125 -2.182 -12.433 16.917 21.108 0.000 76 21 (g) -52 67 67 148 148 102 108 -3.812 3.840 16.723 17.577 0.000 77 21 (g) -31 81 0 79 80 127 126 0.000 0.000 82.106 82.106 0.000 78 21 (g) -31 82 82 79 80 126 128 0.000 0.000 -1.914 1.914 0.000 79 21 (g) -33 77 78 83 83 129 128 -4.305 -1.464 0.946 4.644 0.000 80 21 (g) -33 77 78 84 84 127 129 4.305 1.464 79.246 79.377 0.000 81 21 (g) -41 222 222 85 77 130 126 0.000 -0.000 207.996 207.996 0.000 82 21 (g) -42 223 0 78 78 126 128 -0.000 -0.000 -1.914 1.914 0.000 83 21 (g) -44 79 79 224 224 129 128 -4.170 -1.436 1.252 4.585 0.000 84 21 (g) -44 80 80 105 105 127 129 8.128 2.244 82.599 83.028 0.000 85 21 (g) -43 81 0 103 104 130 127 -3.958 -0.808 122.231 122.297 0.000 86 21 (g) -31 128 0 88 89 131 132 0.000 0.000 29.206 29.206 0.000 87 21 (g) -31 129 129 88 89 133 131 0.000 0.000 -0.486 0.486 0.000 88 21 (g) -33 86 87 130 130 133 134 3.429 1.436 11.937 12.502 0.000 89 21 (g) -33 86 87 131 131 134 132 -3.429 -1.436 16.784 17.190 0.000 90 21 (g) -31 106 0 92 93 135 136 0.000 0.000 21.355 21.355 0.000 91 21 (g) -31 107 107 92 93 136 137 0.000 0.000 -7.709 7.709 0.000 92 21 (g) -33 90 91 108 108 135 138 -1.872 2.845 20.834 21.111 0.000 93 21 (g) -33 90 91 109 109 138 137 1.872 -2.845 -7.187 7.953 0.000 94 1 (d) -51 55 0 298 298 139 0 1.947 5.431 66.681 66.931 0.330 95 21 (g) -51 55 0 301 301 112 139 4.278 0.262 12.234 12.963 0.000 96 21 (g) -52 57 57 300 300 119 112 5.041 -1.600 -11.914 13.035 0.000 97 21 (g) -51 71 0 121 122 140 109 7.921 -0.519 -15.784 17.667 0.000 98 21 (g) -51 71 0 156 156 103 140 -1.294 2.140 -0.296 2.519 0.000 99 21 (g) -52 65 65 146 146 106 103 -42.399 -80.396 56.880 107.222 0.000 100 21 (g) -51 51 0 229 230 116 141 -2.943 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934.608 0.000 115 21 (g) -42 245 245 106 106 135 143 -0.000 0.000 852.131 852.131 0.000 116 21 (g) -41 246 0 120 107 136 148 0.000 -0.000 -8.022 8.022 0.000 117 21 (g) -44 108 108 247 247 135 138 -0.546 5.624 19.824 20.613 0.000 118 21 (g) -44 109 109 248 248 138 137 3.181 -4.998 -6.192 8.570 0.000 119 21 (g) -44 110 110 249 249 136 143 -1.280 -2.951 823.263 823.269 0.000 120 21 (g) -43 116 0 250 250 137 148 -1.356 2.325 7.215 7.701 0.000 121 21 (g) -51 97 0 152 152 140 149 2.722 1.751 -3.730 4.938 0.000 122 21 (g) -51 97 0 157 157 149 109 4.791 -2.376 -20.509 21.195 0.000 123 2 (u) -52 70 70 151 151 109 0 -20.233 -5.257 -418.739 419.261 0.330 124 21 (g) -31 1522 1522 126 127 150 151 0.000 0.000 27.147 27.147 0.000 125 21 (g) -31 1523 1523 126 127 151 152 0.000 0.000 -9.566 9.566 0.000 126 21 (g) -33 124 125 218 218 150 153 2.271 -2.031 26.816 26.988 0.000 127 21 (g) -33 124 125 216 217 153 152 -2.271 2.031 -9.235 9.725 0.000 128 1 (d) -41 160 160 132 86 131 0 0.000 0.000 1767.396 1767.396 0.000 129 21 (g) -42 161 0 87 87 133 131 -0.000 -0.000 -0.486 0.486 0.000 130 21 (g) -44 88 88 162 162 133 134 2.276 0.952 14.072 14.286 0.000 131 21 (g) -44 89 89 163 163 134 132 -5.031 -2.109 19.334 20.089 0.000 132 1 (d) -43 128 0 164 164 132 0 2.755 1.157 1733.504 1733.507 0.330 133 21 (g) -51 72 0 153 153 154 110 -2.340 16.488 0.126 16.654 0.000 134 21 (g) -51 72 0 158 158 101 154 4.683 5.539 -5.652 9.196 0.000 135 21 (g) -52 64 64 145 145 104 101 80.679 57.179 -111.489 149.025 0.000 136 21 (g) -51 56 0 299 299 111 155 -3.018 -4.088 -3.238 6.025 0.000 137 21 (g) -51 56 0 267 268 155 113 -8.249 -0.005 -5.476 9.901 0.000 138 21 (g) -53 269 269 54 54 119 113 -0.000 -0.000 -25.284 25.284 0.000 139 21 (g) -31 282 0 141 142 156 157 0.000 0.000 180.278 180.278 0.000 140 21 (g) -31 283 283 141 142 158 159 0.000 0.000 -0.173 0.173 0.000 141 21 (g) -33 139 140 284 284 156 159 -1.367 -2.450 168.083 168.107 0.000 142 21 (g) -33 139 140 285 285 158 157 1.367 2.450 12.022 12.345 0.000 143 2 (u) -41 587 587 159 62 102 0 -0.000 -0.000 1770.428 1770.428 0.000 144 2 (u) -42 237 237 63 63 107 0 -0.000 0.000 -648.985 648.985 0.000 145 21 (g) -44 135 135 198 199 104 101 80.771 57.108 -111.577 149.113 0.000 146 21 (g) -44 99 99 171 171 106 103 -41.997 -80.708 56.831 107.272 0.000 147 21 (g) -44 66 66 166 167 110 105 -19.166 13.933 3.032 23.889 0.000 148 21 (g) -44 76 76 406 406 102 108 -3.728 3.775 16.739 17.560 0.000 149 21 (g) -44 68 68 200 200 107 104 8.207 14.644 -7.406 18.348 0.000 150 21 (g) -44 74 74 669 670 125 106 -6.905 -19.763 10.860 23.584 0.000 151 2 (u) -44 123 123 465 466 109 0 -20.231 -5.258 -418.696 419.217 0.330 152 21 (g) -44 121 121 177 177 140 149 2.725 1.749 -3.733 4.941 0.000 153 21 (g) -44 133 133 168 168 154 110 -2.299 16.456 0.164 16.617 0.000 154 21 (g) -44 73 73 307 307 105 124 -1.294 3.578 261.042 261.070 0.000 155 21 (g) -44 75 75 404 405 108 125 -2.088 -12.506 16.899 21.126 0.000 156 21 (g) -44 98 98 169 170 103 140 -1.289 2.136 -0.289 2.511 0.000 157 21 (g) -44 122 122 175 176 149 109 4.792 -2.378 -20.525 21.211 0.000 158 21 (g) -44 134 134 183 184 101 154 4.692 5.533 -5.653 9.196 0.000 159 2 (u) -43 143 0 398 399 124 0 -2.189 1.702 1323.754 1323.757 0.330 160 1 (d) -42 190 190 128 128 131 0 0.000 0.000 1767.396 1767.396 0.000 161 21 (g) -41 191 0 165 129 133 160 -0.000 -0.000 -2.690 2.690 0.000 162 21 (g) -44 130 130 192 192 133 134 1.796 0.579 8.164 8.380 0.000 163 21 (g) -44 131 131 174 174 134 132 -6.721 -3.419 37.179 37.936 0.000 164 1 (d) -44 132 132 172 173 132 0 2.750 1.152 1720.704 1720.707 0.330 165 21 (g) -43 161 0 195 195 131 160 2.175 1.688 -1.343 3.063 0.000 166 21 (g) -51 147 0 305 306 161 105 -7.622 7.665 -1.304 10.888 0.000 167 21 (g) -51 147 0 564 565 110 161 -11.844 8.414 4.357 15.168 0.000 168 21 (g) -52 153 153 185 185 154 110 -1.999 14.310 0.142 14.450 0.000 169 21 (g) -51 156 0 444 444 162 140 0.321 1.719 -0.652 1.866 0.000 170 21 (g) -51 156 0 442 443 103 162 -5.179 -6.442 5.193 9.762 0.000 171 21 (g) -52 146 146 671 671 106 103 -38.428 -73.849 52.001 98.155 0.000 172 1 (d) -51 164 0 194 194 163 0 0.668 -0.689 1529.580 1529.580 0.330 173 21 (g) -51 164 0 196 196 132 163 1.942 1.770 191.896 191.914 0.000 174 21 (g) -52 163 163 193 193 134 132 -6.581 -3.348 36.407 37.149 0.000 175 21 (g) -51 157 0 467 467 164 109 3.028 -1.296 -18.244 18.539 0.000 176 21 (g) -51 157 0 1098 1099 149 164 3.567 0.076 -4.751 5.941 0.000 177 21 (g) -52 152 152 1103 1103 140 149 0.922 0.592 -1.263 1.672 0.000 178 21 (g) -41 221 221 182 111 165 145 0.000 -0.000 79.667 79.667 0.000 179 21 (g) -42 426 426 112 112 146 147 -0.000 0.000 -961.777 961.777 0.000 180 21 (g) -44 113 113 213 214 144 147 4.809 1.128 -63.578 63.770 0.000 181 21 (g) -44 114 114 219 220 146 145 -2.467 -1.979 -898.081 898.087 0.000 182 21 (g) -43 178 0 215 215 165 144 -2.341 0.851 79.549 79.588 0.000 183 21 (g) -51 158 0 584 584 101 166 2.937 0.925 -1.768 3.551 0.000 184 21 (g) -51 158 0 252 253 166 154 1.373 7.339 -3.858 8.404 0.000 185 21 (g) -52 168 168 254 254 154 110 -1.617 11.578 0.115 11.691 0.000 186 21 (g) -31 205 0 188 189 167 168 0.000 0.000 59.243 59.243 0.000 187 -1 (dbar) -31 206 206 188 189 0 167 0.000 0.000 -5.637 5.637 0.000 188 21 (g) -33 186 187 207 207 169 168 2.201 -0.528 58.989 59.032 0.000 189 -1 (dbar) -33 186 187 208 208 0 169 -2.201 0.528 -5.382 5.848 0.330 190 1 (d) -42 1076 1076 160 160 131 0 -0.000 -0.000 1767.396 1767.396 0.000 191 21 (g) -41 674 674 197 161 170 160 0.000 0.000 -47.532 47.532 0.000 192 21 (g) -44 162 162 276 277 133 134 1.752 0.500 7.607 7.822 0.000 193 21 (g) -44 174 174 212 212 134 132 -6.731 -3.620 39.015 39.757 0.000 194 1 (d) -44 172 172 275 275 163 0 0.668 -0.689 1529.266 1529.266 0.330 195 21 (g) -44 165 165 672 673 131 160 1.287 0.072 -2.015 2.392 0.000 196 21 (g) -44 173 173 210 211 132 163 1.939 1.763 190.803 190.821 0.000 197 21 (g) -43 191 0 401 402 170 133 1.085 1.973 -44.813 44.869 0.000 198 21 (g) -51 145 0 513 514 171 101 72.144 49.002 -96.645 130.178 0.000 199 21 (g) -51 145 0 257 257 104 171 9.021 8.808 -15.287 19.815 0.000 200 21 (g) -52 149 149 235 236 107 104 7.813 13.941 -7.051 17.468 0.000 201 -2 (ubar) -31 451 451 203 204 0 172 0.000 0.000 0.869 0.869 0.000 202 21 (g) -31 452 0 203 204 174 173 0.000 0.000 -31.151 31.151 0.000 203 -2 (ubar) -33 201 202 453 453 0 173 0.664 2.088 -0.653 2.311 0.330 204 21 (g) -33 201 202 454 454 174 172 -0.664 -2.088 -29.629 29.710 0.000 205 21 (g) -41 518 518 209 186 175 168 0.000 -0.000 70.006 70.006 0.000 206 -1 (dbar) -42 1550 1550 187 187 0 167 -0.000 0.000 -5.637 5.637 0.000 207 21 (g) -44 188 188 377 378 169 168 3.376 1.084 60.273 60.378 0.000 208 -1 (dbar) -44 189 189 379 379 0 169 -2.196 0.535 -5.240 5.716 0.330 209 21 (g) -43 205 0 516 517 175 167 -1.180 -1.619 9.336 9.549 0.000 210 21 (g) -51 196 0 273 274 176 163 1.264 3.080 115.548 115.596 0.000 211 21 (g) -51 196 0 232 233 132 176 0.260 -1.540 77.658 77.673 0.000 212 21 (g) -52 193 193 234 234 134 132 -6.316 -3.397 36.613 37.309 0.000 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0.056 0.000 1248 21 (g) -62 762 762 1798 1798 326 247 -0.177 -0.331 -8.856 8.864 0.000 1249 21 (g) -62 1097 1097 2096 2096 104 393 2.601 2.126 -4.105 5.304 0.000 1250 21 (g) -62 843 843 1642 0 357 264 4.691 3.020 -6.184 8.329 0.000 1251 21 (g) -62 837 837 1620 0 355 381 -0.027 0.052 -0.013 0.060 0.000 1252 21 (g) -62 828 828 2163 2163 352 153 0.496 0.528 0.324 0.793 0.000 1253 21 (g) -62 845 845 2093 2093 171 278 2.525 2.167 -3.644 4.935 0.000 1254 21 (g) -62 951 951 2077 2077 397 321 -1.147 2.540 0.371 2.812 0.000 1255 21 (g) -62 911 911 1624 0 109 429 -0.123 0.176 -1.544 1.559 0.000 1256 21 (g) -62 1188 1188 1633 0 281 478 -0.596 0.467 -0.087 0.762 0.000 1257 21 (g) -62 1160 1160 2089 2089 438 343 9.906 6.819 -13.897 18.378 0.000 1258 21 (g) -62 971 971 1606 0 102 121 -0.362 -0.179 1.997 2.038 0.000 1259 21 (g) -62 839 839 1769 1769 273 292 -0.141 0.046 1.139 1.148 0.000 1260 3 (s) -62 711 711 1652 0 297 0 -0.010 0.358 425.723 425.724 0.500 1261 21 (g) -62 986 986 2171 2171 305 313 -5.486 -12.138 7.457 15.266 0.000 1262 21 (g) -62 697 697 2170 2170 313 106 -5.510 -11.173 8.262 14.948 0.000 1263 21 (g) -62 872 872 1740 0 314 364 -3.541 2.615 -0.074 4.403 0.000 1264 -3 (sbar) -62 712 712 1628 0 0 462 0.168 0.821 352.306 352.307 0.500 1265 21 (g) -62 909 909 1799 1799 383 326 -4.237 -0.199 -73.895 74.016 0.000 1266 21 (g) -62 1010 1010 1643 0 327 424 -0.131 -0.054 1.372 1.379 0.000 1267 21 (g) -62 813 813 2085 2085 331 344 0.017 0.841 -1.313 1.559 0.000 1268 21 (g) -62 918 918 1640 0 337 386 -0.294 0.896 -0.521 1.077 0.000 1269 21 (g) -62 1088 1088 1902 1902 418 472 0.113 0.018 0.022 0.116 0.000 1270 21 (g) -62 808 808 1721 0 342 363 -8.656 -16.438 11.045 21.613 0.000 1271 21 (g) -62 814 814 2084 2084 344 166 0.027 1.693 -0.504 1.767 0.000 1272 21 (g) -62 1016 1016 1676 0 350 266 0.202 -0.452 0.848 0.982 0.000 1273 21 (g) -62 829 829 1723 0 246 262 -0.032 -0.410 0.021 0.412 0.000 1274 21 (g) -62 838 838 1768 1768 292 402 -1.877 2.523 9.680 10.178 0.000 1275 21 (g) -62 844 844 2092 2092 278 357 0.796 0.181 -0.527 0.971 0.000 1276 21 (g) -62 865 865 1780 1780 364 161 0.025 0.095 0.076 0.124 0.000 1277 -1 (dbar) -62 871 871 1740 0 0 314 -2.270 1.525 0.333 2.775 0.330 1278 21 (g) -62 874 874 2080 2080 154 366 0.102 1.606 -0.420 1.663 0.000 1279 21 (g) -62 1071 1071 2103 2103 439 188 0.449 0.045 -0.365 0.581 0.000 1280 21 (g) -62 910 910 1625 0 282 383 -0.060 -0.173 -4.421 4.425 0.000 1281 21 (g) -62 916 916 2097 2097 385 104 3.415 4.432 -4.383 7.107 0.000 1282 21 (g) -62 919 919 2082 2082 386 189 0.734 1.777 -0.617 2.019 0.000 1283 21 (g) -62 1116 1116 1623 0 453 394 -0.377 -0.672 0.210 0.799 0.000 1284 21 (g) -62 952 952 2078 2078 110 397 0.012 -0.023 0.143 0.145 0.000 1285 21 (g) -62 955 955 2166 2166 241 398 -0.802 -1.577 0.623 1.876 0.000 1286 21 (g) -62 970 970 1615 0 288 137 -0.780 0.722 5.586 5.686 0.000 1287 21 (g) -62 1019 1019 1728 0 408 305 -0.386 -1.676 0.840 1.914 0.000 1288 21 (g) -62 1009 1009 1650 0 416 461 0.170 0.983 16.663 16.693 0.000 1289 21 (g) -62 1012 1012 2101 2101 233 417 0.288 1.348 -0.682 1.538 0.000 1290 21 (g) -62 1015 1015 1678 0 105 474 0.349 -0.396 4.450 4.481 0.000 1291 -2 (ubar) -62 1018 1018 1728 0 0 408 -1.909 -5.716 2.605 6.574 0.330 1292 21 (g) -62 1158 1158 2087 2087 468 200 0.880 0.233 -0.010 0.910 0.000 1293 21 (g) -62 1069 1069 2090 2090 287 438 7.744 5.360 -9.721 13.534 0.000 1294 21 (g) -62 1072 1072 2104 2104 182 439 0.537 0.411 0.447 0.811 0.000 1295 21 (g) -62 1087 1087 1697 0 340 454 -0.258 0.061 38.897 38.898 0.000 1296 21 (g) -62 1096 1096 1637 0 248 447 2.093 2.353 -3.953 5.054 0.000 1297 21 (g) -62 1136 1136 1719 0 448 480 0.049 -0.121 -0.057 0.143 0.000 1298 21 (g) -62 1102 1102 1733 0 149 440 2.884 0.496 -4.982 5.778 0.000 1299 21 (g) -62 1114 1114 1830 1830 232 452 -0.347 -0.583 0.932 1.153 0.000 1300 21 (g) -62 1128 1128 1621 0 458 370 -1.143 -2.945 3.536 4.741 0.000 1301 21 (g) -62 1129 1129 1619 0 125 185 -0.033 -2.118 2.640 3.385 0.000 1302 21 (g) -62 1135 1135 1727 0 164 177 0.238 -0.227 -3.630 3.645 0.000 1303 21 (g) -62 1150 1150 1681 0 465 210 0.059 -0.122 -0.068 0.152 0.000 1304 21 (g) -62 1159 1159 1631 0 101 468 1.772 0.819 -1.768 2.634 0.000 1305 21 (g) -62 1189 1189 2075 2075 478 284 -2.713 1.728 1.289 3.465 0.000 1306 1 (d) -61 1 0 732 732 172 0 0.746 -1.762 489.953 489.956 0.000 1307 21 (g) -61 2 0 733 733 208 113 -2.950 0.956 -794.305 794.311 0.000 1308 1 (d) -62 734 734 1982 1982 259 0 2.332 4.396 46.776 47.041 0.330 1309 2 (u) -62 978 978 2006 2006 283 0 -0.284 -0.309 -0.592 0.797 0.330 1310 1 (d) -62 923 923 2285 2285 119 0 3.520 -0.810 -4.237 5.578 0.330 1311 21 (g) -62 1157 1157 1661 0 218 463 0.696 -0.157 1.421 1.590 0.000 1312 21 (g) -62 1133 1133 1940 1940 155 194 -4.036 0.512 -3.865 5.611 0.000 1313 21 (g) -62 912 912 1666 0 384 319 -0.258 0.007 0.075 0.268 0.000 1314 21 (g) -62 882 882 2015 2015 172 371 -0.288 -0.385 22.189 22.195 0.000 1315 21 (g) -62 1131 1131 1942 1942 206 459 -0.378 -0.221 -0.010 0.438 0.000 1316 -1 (dbar) -62 842 842 1992 1992 0 112 1.518 -0.694 -6.425 6.646 0.330 1317 21 (g) -62 800 800 1664 0 301 111 0.146 0.260 16.979 16.982 0.000 1318 21 (g) -62 990 990 1662 0 356 410 -0.345 0.127 0.195 0.416 0.000 1319 21 (g) -62 893 893 1669 0 330 260 -0.450 -0.643 -0.562 0.965 0.000 1320 21 (g) -62 992 992 1988 1988 250 267 -0.081 0.447 0.938 1.042 0.000 1321 21 (g) -62 834 834 1663 0 354 256 -0.164 -0.002 -0.061 0.175 0.000 1322 21 (g) -62 1166 1166 1660 0 139 259 0.781 0.473 12.722 12.755 0.000 1323 21 (g) -62 749 749 1943 1943 260 206 -2.421 -0.169 -1.701 2.963 0.000 1324 21 (g) -62 957 957 1987 1987 267 399 2.311 -0.109 4.051 4.665 0.000 1325 21 (g) -62 751 751 1663 0 256 283 -0.224 0.192 0.126 0.320 0.000 1326 21 (g) -62 836 836 2009 2009 339 286 -0.503 0.186 13.890 13.901 0.000 1327 21 (g) -62 1058 1058 1664 0 415 301 0.162 -0.005 3.537 3.541 0.000 1328 21 (g) -62 754 754 1666 0 319 113 0.047 0.174 0.133 0.224 0.000 1329 21 (g) -62 816 816 2289 2289 208 345 -2.616 0.222 -558.124 558.131 0.000 1330 21 (g) -62 980 980 1665 0 221 375 -0.220 -0.229 -0.338 0.463 0.000 1331 21 (g) -62 914 914 1667 0 194 335 0.045 -0.056 -0.170 0.184 0.000 1332 21 (g) -62 799 799 2010 2010 111 339 0.346 0.408 5.792 5.817 0.000 1333 21 (g) -62 999 999 2288 2288 345 413 -0.244 0.533 -35.512 35.517 0.000 1334 21 (g) -62 835 835 2008 2008 286 354 0.155 -0.442 2.794 2.833 0.000 1335 21 (g) -62 885 885 1991 1991 112 372 0.321 -0.640 0.025 0.717 0.000 1336 21 (g) -62 1007 1007 2014 2014 371 213 -1.733 -0.983 298.354 298.361 0.000 1337 21 (g) -62 886 886 1662 0 372 356 0.079 0.358 -0.154 0.397 0.000 1338 21 (g) -62 892 892 1668 0 375 330 -0.021 -0.705 -0.246 0.747 0.000 1339 21 (g) -62 913 913 1667 0 335 384 -0.708 -1.067 -1.460 1.942 0.000 1340 21 (g) -62 1001 1001 2286 2286 387 119 0.288 -0.086 -2.525 2.543 0.000 1341 21 (g) -62 958 958 1986 1986 399 218 0.362 0.274 0.350 0.573 0.000 1342 -2 (ubar) -62 979 979 1665 0 0 221 -0.670 -1.565 -1.155 2.083 0.330 1343 21 (g) -62 991 991 1989 1989 410 250 0.192 -0.183 1.392 1.417 0.000 1344 21 (g) -62 1000 1000 2287 2287 413 387 -0.782 0.331 -170.102 170.105 0.000 1345 21 (g) -62 1056 1056 2013 2013 213 434 0.052 0.073 0.484 0.492 0.000 1346 21 (g) -62 1057 1057 2012 2012 434 415 0.164 -0.679 41.987 41.993 0.000 1347 21 (g) -62 1132 1132 1941 1941 459 155 -0.820 0.086 -1.353 1.585 0.000 1348 21 (g) -62 1164 1164 1984 1984 467 470 1.055 0.666 5.025 5.177 0.000 1349 21 (g) -62 1156 1156 1661 0 463 467 0.448 -0.363 2.223 2.297 0.000 1350 21 (g) -62 1165 1165 1660 0 470 139 0.017 -0.028 2.782 2.782 0.000 1351 21 (g) -61 1 0 591 591 115 159 2.436 1.088 9.698 10.059 0.000 1352 21 (g) -61 2 0 592 592 167 115 0.869 -2.110 -338.565 338.572 0.000 1353 21 (g) -62 983 983 1614 0 324 315 -1.334 -0.028 1.593 2.078 0.000 1354 21 (g) -62 780 780 2225 2225 272 333 0.004 0.242 -7.522 7.526 0.000 1355 21 (g) -62 678 678 2220 2220 118 308 3.640 0.868 -64.706 64.814 0.000 1356 21 (g) -62 663 663 2230 2230 303 212 2.553 -0.638 -30.920 31.032 0.000 1357 21 (g) -62 1092 1092 2222 2222 446 180 0.610 0.593 -7.998 8.043 0.000 1358 21 (g) -62 1110 1110 2228 2228 263 451 0.264 -1.374 -20.268 20.316 0.000 1359 21 (g) -62 599 599 1616 0 198 274 -0.199 0.315 -0.790 0.873 0.000 1360 21 (g) -62 651 651 2231 2231 212 299 0.353 0.231 -2.374 2.411 0.000 1361 21 (g) -62 1109 1109 1736 0 219 320 -0.832 0.053 0.069 0.836 0.000 1362 21 (g) -62 602 602 2219 2219 222 118 1.149 -0.222 -25.745 25.771 0.000 1363 21 (g) -62 1031 1031 1616 0 228 198 0.265 0.342 -2.220 2.261 0.000 1364 21 (g) -62 604 604 2218 2218 167 222 1.227 -0.290 -108.231 108.238 0.000 1365 21 (g) -62 1206 1206 2227 2227 486 263 -0.335 -0.075 -0.743 0.818 0.000 1366 21 (g) -62 906 906 2224 2224 382 272 -0.939 0.176 -2.957 3.107 0.000 1367 21 (g) -62 1154 1154 1612 0 274 117 0.182 -0.894 -0.552 1.066 0.000 1368 21 (g) -62 1041 1041 1738 0 426 159 0.064 -0.123 0.914 0.925 0.000 1369 21 (g) -62 1029 1029 2232 2232 299 422 0.181 0.178 -11.596 11.599 0.000 1370 21 (g) -62 1112 1112 1610 0 141 303 0.151 -0.145 -5.276 5.280 0.000 1371 21 (g) -62 1094 1094 1613 0 308 116 0.141 0.056 -8.257 8.258 0.000 1372 1 (d) -62 1107 1107 2238 2238 407 0 -1.548 -0.520 1.479 2.228 0.330 1373 21 (g) -62 977 977 1737 0 320 114 -0.735 -0.330 0.886 1.197 0.000 1374 21 (g) -62 1152 1152 2236 2236 466 324 -0.333 -0.345 0.931 1.047 0.000 1375 21 (g) -62 1208 1208 1611 0 333 191 -0.655 0.277 -5.661 5.705 0.000 1376 21 (g) -62 907 907 2223 2223 180 382 -0.161 0.064 -4.756 4.759 0.000 1377 21 (g) -62 1043 1043 1735 0 114 405 0.027 -0.002 -0.009 0.029 0.000 1378 21 (g) -62 982 982 1614 0 315 407 -0.462 0.258 0.327 0.622 0.000 1379 21 (g) -62 1030 1030 2233 2233 422 228 -0.653 -0.057 -10.183 10.204 0.000 1380 21 (g) -62 1042 1042 1735 0 405 426 0.475 0.701 0.852 1.201 0.000 1381 21 (g) -62 1093 1093 1613 0 116 446 0.377 -0.297 -5.893 5.912 0.000 1382 -1 (dbar) -62 1108 1108 1736 0 0 219 -0.243 -0.111 0.285 0.511 0.330 1383 21 (g) -62 1111 1111 1610 0 451 141 0.276 0.029 -3.954 3.964 0.000 1384 21 (g) -62 1153 1153 1612 0 117 466 0.203 -0.403 -0.089 0.460 0.000 1385 21 (g) -62 1207 1207 1611 0 191 486 -0.409 0.449 -5.504 5.537 0.000 1386 21 (g) -61 1 0 848 848 122 122 -3.183 0.013 69.212 69.285 0.000 1387 21 (g) -61 2 0 683 683 120 120 -3.018 -1.671 4.623 5.768 0.000 1388 21 (g) -62 504 504 1912 1912 123 237 1.336 1.375 5.296 5.633 0.000 1389 21 (g) -62 846 846 2213 2213 358 437 -2.252 -1.071 16.904 17.087 0.000 1390 21 (g) -62 1104 1104 1615 0 450 288 -0.599 0.029 2.520 2.591 0.000 1391 21 (g) -62 505 505 2049 2049 261 279 0.361 1.354 10.586 10.678 0.000 1392 21 (g) -62 682 682 1694 0 309 245 -0.890 -0.937 5.827 5.969 0.000 1393 21 (g) -62 1106 1106 1646 0 240 338 -1.063 -0.494 9.787 9.857 0.000 1394 21 (g) -62 847 847 1607 0 121 473 -1.745 -1.232 9.367 9.607 0.000 1395 21 (g) -62 1105 1105 1646 0 338 193 -1.349 -0.681 13.546 13.630 0.000 1396 21 (g) -61 1 0 615 615 128 128 0.012 -0.766 208.103 208.105 0.000 1397 21 (g) -61 2 0 1127 1127 126 126 1.800 -1.158 -243.121 243.131 0.000 1398 21 (g) -62 617 617 1717 0 129 162 -0.249 -0.128 0.231 0.362 0.000 1399 2 (u) -62 692 692 1900 1900 127 0 1.095 -0.167 10.050 10.117 0.330 1400 21 (g) -62 619 619 2212 2212 130 358 0.192 -0.661 39.615 39.621 0.000 1401 21 (g) -62 1173 1173 1881 1881 142 257 -1.309 0.190 20.143 20.186 0.000 1402 2 (u) -62 1025 1025 1692 0 179 0 0.987 -0.537 -3.053 3.270 0.330 1403 21 (g) -62 1038 1038 1678 0 425 105 0.288 -0.453 3.608 3.648 0.000 1404 21 (g) -62 1061 1061 1718 0 211 277 -0.211 0.152 -0.162 0.307 0.000 1405 21 (g) -62 624 624 1693 0 285 444 -0.211 0.217 11.213 11.217 0.000 1406 21 (g) -62 1059 1059 1618 0 201 306 -1.226 -0.686 -0.263 1.430 0.000 1407 21 (g) -62 863 863 1709 0 215 270 -0.088 -0.035 3.943 3.945 0.000 1408 21 (g) -62 881 881 1721 0 363 103 -0.236 -0.440 0.278 0.572 0.000 1409 21 (g) -62 628 628 1706 0 291 223 0.362 0.118 4.811 4.826 0.000 1410 -2 (ubar) -62 629 629 1630 0 0 150 0.565 1.013 -4.428 4.589 0.330 1411 21 (g) -62 1040 1040 1672 0 252 181 0.156 -0.315 4.032 4.047 0.000 1412 21 (g) -62 879 879 1621 0 370 453 -0.380 -0.647 0.787 1.088 0.000 1413 21 (g) -62 632 632 1649 0 187 236 -0.268 0.024 8.459 8.463 0.000 1414 21 (g) -62 638 638 1712 0 207 184 1.242 0.510 20.708 20.752 0.000 1415 21 (g) -62 634 634 1709 0 270 156 -0.533 -0.373 44.360 44.364 0.000 1416 21 (g) -62 972 972 1715 0 294 146 1.434 -0.691 -196.381 196.387 0.000 1417 -2 (ubar) -62 637 637 1852 1852 0 291 2.159 0.880 12.864 13.078 0.330 1418 21 (g) -62 1175 1175 1698 0 311 142 -0.535 0.470 12.023 12.044 0.000 1419 21 (g) -62 862 862 1686 0 216 350 0.351 -0.268 0.726 0.850 0.000 1420 21 (g) -62 880 880 1622 0 269 435 -0.961 -0.107 0.172 0.983 0.000 1421 21 (g) -62 1187 1187 1637 0 393 248 0.436 0.409 -0.894 1.075 0.000 1422 21 (g) -62 1023 1023 1715 0 310 294 0.023 -0.039 -16.806 16.806 0.000 1423 21 (g) -62 1024 1024 1742 0 420 377 0.669 0.164 -8.523 8.551 0.000 1424 21 (g) -62 1039 1039 1698 0 243 311 -0.148 0.210 6.084 6.090 0.000 1425 21 (g) -62 1060 1060 1622 0 435 201 -1.851 -0.649 0.613 2.055 0.000 1426 21 (g) -62 1185 1185 1741 0 477 186 0.009 0.113 -9.294 9.294 0.000 1427 21 (g) -62 1174 1174 1607 0 473 450 -0.157 -0.079 0.604 0.629 0.000 1428 21 (g) -62 1186 1186 2153 2153 457 164 0.208 -0.118 -0.540 0.590 0.000 1429 1 (d) -61 1 0 1076 1076 160 0 1.039 -0.636 1767.471 1767.471 0.000 1430 21 (g) -61 2 0 674 674 115 160 3.186 0.462 -49.721 49.825 0.000 1431 2 (u) -62 965 965 1878 1878 133 0 -0.754 0.868 4.304 4.467 0.330 1432 21 (g) -62 561 561 1720 0 134 241 -0.142 -0.145 0.169 0.264 0.000 1433 1 (d) -62 641 641 2035 2035 115 0 0.035 -0.868 536.011 536.012 0.330 1434 21 (g) -62 1074 1074 1733 0 440 449 1.834 -0.001 -3.458 3.914 0.000 1435 21 (g) -62 938 938 1655 0 176 254 0.045 1.394 106.303 106.312 0.000 1436 3 (s) -62 699 699 1702 0 170 0 2.561 1.644 -26.323 26.503 0.500 1437 21 (g) -62 1053 1053 1659 0 424 187 -0.634 -0.082 6.723 6.754 0.000 1438 21 (g) -62 1181 1181 1671 0 132 226 0.057 -0.157 2.600 2.606 0.000 1439 21 (g) -62 1121 1121 1696 0 391 374 0.020 0.232 9.301 9.303 0.000 1440 21 (g) -62 1067 1067 1680 0 379 348 0.090 -0.053 0.080 0.131 0.000 1441 21 (g) -62 1077 1077 1652 0 304 297 -0.245 0.010 151.246 151.246 0.000 1442 -2 (ubar) -62 902 902 2052 2052 0 411 0.588 -0.259 4.155 4.217 0.330 1443 21 (g) -62 1122 1122 2210 2210 225 400 0.658 -0.016 92.949 92.952 0.000 1444 21 (g) -62 924 924 1725 0 388 140 -0.233 0.315 -0.159 0.423 0.000 1445 21 (g) -62 1119 1119 1697 0 454 300 -0.275 0.150 35.443 35.444 0.000 1446 21 (g) -62 1065 1065 1608 0 437 316 -2.070 -0.706 10.919 11.136 0.000 1447 21 (g) -62 831 831 1626 0 271 231 -0.269 -0.000 -0.918 0.957 0.000 1448 21 (g) -62 1179 1179 1675 0 280 132 0.198 -0.349 7.416 7.426 0.000 1449 21 (g) -62 1124 1124 1605 0 295 195 0.289 -0.251 67.559 67.560 0.000 1450 21 (g) -62 960 960 2211 2211 400 130 -0.003 -0.276 57.982 57.983 0.000 1451 21 (g) -62 667 667 1655 0 254 229 -0.188 0.786 72.807 72.811 0.000 1452 21 (g) -62 673 673 1618 0 306 232 -0.131 -0.099 -0.037 0.168 0.000 1453 -3 (sbar) -62 926 926 1690 0 0 268 1.872 0.779 -14.180 14.332 0.500 1454 21 (g) -62 963 963 1677 0 353 379 0.735 -0.437 0.139 0.866 0.000 1455 21 (g) -62 889 889 1693 0 374 285 -0.212 0.315 12.481 12.486 0.000 1456 21 (g) -62 901 901 1684 0 197 425 0.261 -1.066 8.129 8.203 0.000 1457 21 (g) -62 925 925 1626 0 231 360 -0.591 0.161 -2.364 2.442 0.000 1458 21 (g) -62 937 937 1714 0 196 409 0.790 -0.206 27.487 27.499 0.000 1459 21 (g) -62 1140 1140 1628 0 462 487 0.028 0.102 36.624 36.624 0.000 1460 21 (g) -62 964 964 1724 0 401 419 -0.266 0.096 -0.088 0.296 0.000 1461 21 (g) -62 1052 1052 1648 0 421 240 -0.073 0.106 1.703 1.707 0.000 1462 21 (g) -62 1050 1050 1713 0 431 175 -0.751 -0.827 29.103 29.124 0.000 1463 21 (g) -62 1051 1051 1679 0 181 280 0.207 -0.260 4.655 4.666 0.000 1464 21 (g) -62 1142 1142 1708 0 432 445 -0.024 -0.172 4.700 4.703 0.000 1465 21 (g) -62 1066 1066 1699 0 257 309 -0.801 -0.951 5.920 6.050 0.000 1466 21 (g) -62 1075 1075 1635 0 131 275 -0.132 0.213 -0.631 0.679 0.000 1467 21 (g) -62 1078 1078 1605 0 441 295 0.438 -0.367 103.902 103.903 0.000 1468 21 (g) -62 1120 1120 2044 2044 163 176 0.631 0.396 68.083 68.087 0.000 1469 21 (g) -62 1123 1123 2208 2208 455 441 0.665 -0.597 287.102 287.103 0.000 1470 21 (g) -62 1141 1141 1673 0 296 298 0.092 -0.025 0.471 0.481 0.000 1471 21 (g) -62 1180 1180 1648 0 475 421 -0.074 0.428 9.443 9.453 0.000 1472 21 (g) -61 1 0 245 245 148 148 0.922 2.187 851.900 851.903 0.000 1473 21 (g) -61 2 0 905 905 143 143 -3.327 -0.791 -8.177 8.864 0.000 1474 1 (d) -62 359 359 1766 1766 135 0 -0.874 0.134 3.950 4.061 0.330 1475 21 (g) -62 1194 1194 1719 0 480 390 0.284 -0.939 -0.694 1.202 0.000 1476 21 (g) -62 270 270 1609 0 195 225 1.319 -1.470 353.505 353.511 0.000 1477 21 (g) -62 935 935 1703 0 361 318 -0.057 0.141 0.584 0.603 0.000 1478 21 (g) -62 1148 1148 1617 0 381 108 -0.108 0.009 0.087 0.140 0.000 1479 -1 (dbar) -62 456 456 1887 1887 0 340 -0.347 -0.572 182.811 182.812 0.330 1480 -1 (dbar) -62 995 995 1834 1834 0 355 -0.289 2.553 6.748 7.228 0.330 1481 1 (d) -62 783 783 1844 1844 334 0 -1.197 0.586 176.651 176.657 0.330 1482 21 (g) -62 789 789 1685 0 336 192 -0.090 -0.450 4.467 4.491 0.000 1483 21 (g) -62 1004 1004 1674 0 136 365 -0.042 -0.213 0.837 0.864 0.000 1484 21 (g) -62 1163 1163 1726 0 258 485 -0.049 -0.983 -0.638 1.173 0.000 1485 21 (g) -62 1161 1161 1722 0 469 392 -0.303 0.109 -0.291 0.434 0.000 1486 21 (g) -62 993 993 1654 0 411 423 0.189 0.878 4.558 4.645 0.000 1487 21 (g) -62 1169 1169 1704 0 318 135 -0.071 0.632 2.009 2.108 0.000 1488 21 (g) -62 784 784 1885 1885 251 341 -0.660 1.127 93.780 93.789 0.000 1489 21 (g) -62 790 790 1656 0 253 416 0.426 0.627 8.584 8.617 0.000 1490 21 (g) -62 1196 1196 1638 0 471 110 -0.072 0.480 0.113 0.498 0.000 1491 1 (d) -62 933 933 2217 2217 137 0 -1.297 1.750 4.808 5.289 0.330 1492 21 (g) -62 904 904 1634 0 188 378 0.032 0.639 0.283 0.700 0.000 1493 21 (g) -62 931 931 1730 0 390 258 1.117 -4.147 -3.505 5.544 0.000 1494 -1 (dbar) -62 934 934 1771 1771 0 403 -0.106 0.407 1.155 1.273 0.330 1495 21 (g) -62 994 994 1682 0 307 216 0.325 0.382 0.710 0.869 0.000 1496 21 (g) -62 1146 1146 1695 0 464 325 -0.610 -0.161 1.382 1.519 0.000 1497 21 (g) -62 1147 1147 1632 0 414 182 -0.384 0.582 0.914 1.150 0.000 1498 21 (g) -62 1162 1162 1723 0 262 352 0.135 -0.559 0.014 0.575 0.000 1499 21 (g) -62 1168 1168 1680 0 348 123 0.289 0.023 0.632 0.695 0.000 1500 21 (g) -62 1195 1195 1670 0 138 238 0.034 -0.171 0.268 0.320 0.000 1501 21 (g) -61 1 0 770 770 147 147 -0.841 -2.488 99.575 99.609 0.000 1502 21 (g) -61 2 0 524 524 145 145 -0.136 -2.557 -975.772 975.775 0.000 1503 21 (g) -62 424 424 1727 0 177 362 1.640 -1.147 -18.884 18.990 0.000 1504 3 (s) -62 219 219 1964 1964 146 0 -1.263 -0.625 -543.420 543.422 0.500 1505 21 (g) -62 849 849 1683 0 322 165 -0.003 -0.463 6.352 6.369 0.000 1506 -3 (sbar) -62 323 323 1627 0 0 244 -0.238 -0.316 -12.039 12.056 0.500 1507 -3 (sbar) -62 768 768 1817 1817 0 328 -0.462 -2.422 -187.505 187.522 0.500 1508 21 (g) -62 1172 1172 1695 0 325 133 -0.121 0.011 0.254 0.281 0.000 1509 3 (s) -62 358 358 2150 2150 144 0 -0.371 1.604 -2.602 3.119 0.500 1510 21 (g) -62 357 357 1705 0 220 273 -1.346 0.530 2.142 2.584 0.000 1511 21 (g) -62 1083 1083 1813 1813 235 430 1.674 -0.134 -23.329 23.390 0.000 1512 21 (g) -62 1049 1049 1690 0 268 367 0.500 0.402 -3.935 3.987 0.000 1513 21 (g) -62 1137 1137 1650 0 461 475 0.134 0.385 8.739 8.748 0.000 1514 21 (g) -62 730 730 1683 0 165 336 -0.256 -1.033 16.991 17.025 0.000 1515 21 (g) -62 1170 1170 1647 0 279 302 0.179 0.518 5.176 5.205 0.000 1516 21 (g) -62 769 769 1816 1816 328 477 -0.868 -1.286 -167.196 167.203 0.000 1517 21 (g) -62 1139 1139 1711 0 359 215 -1.904 -1.324 51.936 51.988 0.000 1518 21 (g) -62 1085 1085 1742 0 430 420 0.382 0.000 -4.121 4.138 0.000 1519 21 (g) -62 1084 1084 1702 0 443 170 1.228 0.422 -11.968 12.038 0.000 1520 21 (g) -62 1138 1138 1643 0 193 327 -0.458 -0.233 5.132 5.157 0.000 1521 21 (g) -62 1171 1171 1688 0 472 296 0.577 0.066 2.082 2.161 0.000 1522 21 (g) -61 1 0 124 124 152 152 -0.889 0.228 27.039 27.054 0.000 1523 21 (g) -61 2 0 125 125 151 151 2.113 -0.340 -9.446 9.685 0.000 1524 21 (g) -62 648 648 1630 0 150 178 0.017 0.017 -0.078 0.082 0.000 1525 21 (g) -62 289 289 1639 0 178 173 0.699 1.496 -5.182 5.439 0.000 1526 21 (g) -62 1182 1182 1674 0 238 136 -0.021 -0.187 0.476 0.512 0.000 1527 21 (g) -62 869 869 1685 0 192 329 -0.355 -0.857 6.354 6.422 0.000 1528 21 (g) -62 876 876 1691 0 367 183 0.333 0.162 -1.254 1.308 0.000 1529 21 (g) -62 810 810 1671 0 226 322 0.017 -0.078 1.348 1.351 0.000 1530 21 (g) -62 1203 1203 1724 0 153 401 -0.545 0.020 -0.028 0.546 0.000 1531 21 (g) -62 812 812 1677 0 289 353 0.254 -0.110 0.001 0.277 0.000 1532 21 (g) -62 708 708 1673 0 298 127 1.186 -0.112 6.826 6.929 0.000 1533 21 (g) -62 867 867 1606 0 316 102 -0.866 -0.380 4.749 4.842 0.000 1534 21 (g) -62 1205 1205 1633 0 321 281 -0.211 0.213 -0.076 0.309 0.000 1535 21 (g) -62 811 811 1631 0 343 101 0.158 0.087 -0.185 0.259 0.000 1536 21 (g) -62 868 868 1684 0 365 197 0.033 -0.681 6.008 6.047 0.000 1537 21 (g) -62 1184 1184 1636 0 200 436 0.873 0.578 -0.669 1.243 0.000 1538 21 (g) -62 1183 1183 1716 0 476 388 -0.222 0.286 -0.211 0.419 0.000 1539 21 (g) -62 1204 1204 1726 0 485 457 -0.128 -0.567 -0.485 0.757 0.000 1540 21 (g) -61 1 0 1193 1193 159 160 0.668 -0.233 219.141 219.142 0.000 1541 1 (d) -61 2 0 526 526 160 0 -2.289 1.354 5.502 6.112 0.000 1542 21 (g) -62 1089 1089 1845 1845 156 334 -1.363 -2.147 175.466 175.485 0.000 1543 21 (g) -62 528 528 2050 2050 158 261 -0.060 3.457 21.461 21.738 0.000 1544 21 (g) -62 1191 1191 1645 0 157 158 -0.067 0.433 2.299 2.340 0.000 1545 1 (d) -62 989 989 1738 0 159 0 -0.437 0.049 0.477 0.728 0.330 1546 21 (g) -62 1091 1091 1707 0 409 479 0.198 -0.057 4.220 4.225 0.000 1547 21 (g) -62 1090 1090 1708 0 445 431 -0.231 -0.369 12.414 12.422 0.000 1548 21 (g) -62 1192 1192 1707 0 479 432 0.339 -0.243 8.306 8.316 0.000 1549 21 (g) -61 1 0 806 806 167 168 0.031 2.110 102.228 102.250 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1.716 0.000 1564 21 (g) -61 2 0 1046 1046 172 310 1.389 1.821 -43.877 43.937 0.000 1565 -2 (ubar) -62 939 939 1966 1966 0 310 -0.099 1.208 0.023 1.256 0.330 1566 21 (g) -62 852 852 1814 1814 174 235 0.690 -0.735 -21.296 21.320 0.000 1567 21 (g) -62 1082 1082 1625 0 429 282 -0.030 -0.221 -3.923 3.929 0.000 1568 21 (g) -62 941 941 1635 0 173 131 -0.212 0.388 -1.826 1.879 0.000 1569 21 (g) -62 694 694 1731 0 312 144 0.457 -0.030 -1.997 2.049 0.000 1570 21 (g) -62 853 853 1624 0 360 109 -0.202 0.358 -2.573 2.606 0.000 1571 21 (g) -62 940 940 1718 0 392 211 -0.517 0.228 -0.357 0.668 0.000 1572 21 (g) -62 1080 1080 1627 0 244 271 -0.428 -0.274 -4.237 4.267 0.000 1573 21 (g) -62 1081 1081 1745 0 442 174 0.259 0.012 -7.674 7.679 0.000 1574 21 (g) -61 1 0 860 860 227 227 -0.155 1.471 478.799 478.802 0.000 1575 21 (g) -61 2 0 716 716 205 205 2.549 2.091 -44.725 44.846 0.000 1576 21 (g) -62 858 858 1734 0 362 460 0.573 -0.169 -4.690 4.728 0.000 1577 21 (g) -62 948 948 1619 0 185 458 0.014 -0.188 0.212 0.284 0.000 1578 21 (g) -62 1211 1211 1701 0 300 251 -0.372 0.598 80.116 80.119 0.000 1579 21 (g) -62 896 896 1741 0 186 442 -0.018 0.036 -1.152 1.153 0.000 1580 21 (g) -62 996 996 1644 0 412 124 -0.066 0.329 51.667 51.668 0.000 1581 21 (g) -62 1178 1178 1710 0 184 169 0.183 0.079 5.637 5.641 0.000 1582 21 (g) -62 1209 1209 1653 0 229 239 0.049 1.059 150.203 150.206 0.000 1583 21 (g) -62 1199 1199 1743 0 377 317 0.652 0.344 -8.375 8.408 0.000 1584 21 (g) -62 859 859 1692 0 183 179 1.282 -0.023 -3.260 3.503 0.000 1585 2 (u) -62 1197 1197 1743 0 317 0 1.786 0.552 -18.701 18.797 0.330 1586 21 (g) -62 1202 1202 1722 0 396 469 -0.711 0.104 -0.818 1.088 0.000 1587 21 (g) -62 998 998 1703 0 402 361 -0.237 0.476 1.811 1.888 0.000 1588 21 (g) -62 997 997 1649 0 236 163 -0.792 0.081 35.939 35.947 0.000 1589 21 (g) -62 1200 1200 1739 0 483 346 -0.151 0.271 0.093 0.324 0.000 1590 21 (g) -62 1177 1177 1672 0 474 252 0.163 -0.248 3.086 3.101 0.000 1591 -2 (ubar) -62 1198 1198 1747 1747 0 443 0.463 0.111 -6.310 6.337 0.330 1592 21 (g) -62 1201 1201 1732 0 419 396 -0.820 -0.153 -0.731 1.109 0.000 1593 21 (g) -62 1210 1210 1629 0 487 230 0.395 0.302 149.347 149.348 0.000 1594 21 (g) -61 1 0 319 319 208 115 0.977 -0.099 0.947 1.365 0.000 1595 -2 (ubar) -61 2 0 320 320 0 208 1.262 1.628 -2.349 3.125 0.000 1596 21 (g) -62 321 321 1915 1915 210 289 1.518 -0.844 -0.821 1.921 0.000 1597 -2 (ubar) -62 322 322 2036 2036 0 115 0.722 2.373 -0.582 2.569 0.330 1598 2 (u) -63 1 0 2239 2239 160 0 -0.727 0.213 13.171 13.197 0.330 1599 -1 (dbar) -63 1 0 2290 2290 0 208 -0.084 -0.011 820.448 820.448 0.330 1600 2 (u) -63 1 0 1869 1869 168 0 -1.410 -0.305 54.716 54.736 0.330 1601 2103 (ud_1) -63 2 0 1788 1788 0 491 -0.115 -0.638 -3681.704 3681.704 0.771 1602 -1 (dbar) -63 2 0 2016 2016 0 172 0.024 0.198 -0.662 0.767 0.330 1603 1 (d) -63 2 0 1937 1937 113 0 -0.182 -0.124 -132.321 132.321 0.330 1604 2 (u) -63 2 0 1787 1787 491 0 -0.547 -0.204 -15.751 15.766 0.330 1605 21 (g) -73 1449 1467 1609 0 441 195 0.727 -0.618 171.461 171.463 0.016 1606 21 (g) -73 1258 1533 1608 0 316 121 -1.228 -0.559 6.746 6.880 0.030 1607 21 (g) -73 1394 1427 2215 2215 121 450 -1.902 -1.311 9.971 10.236 0.169 1608 21 (g) -73 1446 1606 2214 2214 437 121 -3.299 -1.265 17.665 18.016 0.176 1609 21 (g) -73 1476 1605 2209 2209 441 225 2.046 -2.087 524.966 524.974 0.187 1610 21 (g) -73 1370 1383 2229 2229 451 303 0.427 -0.116 -9.230 9.244 0.246 1611 21 (g) -73 1375 1385 2226 2226 333 486 -1.064 0.726 -11.164 11.242 0.294 1612 21 (g) -73 1367 1384 2235 2235 274 466 0.385 -1.297 -0.640 1.526 0.298 1613 21 (g) -73 1371 1381 2221 2221 308 446 0.518 -0.241 -14.150 14.171 0.515 1614 21 (g) -73 1353 1378 2237 2237 324 407 -1.796 0.230 1.920 2.700 0.570 1615 21 (g) -73 1286 1390 2216 2216 450 137 -1.379 0.751 8.106 8.277 0.573 1616 21 (g) -73 1359 1363 2234 2234 228 274 0.066 0.657 -3.010 3.135 0.577 1617 21 (g) -73 1240 1478 1620 0 381 269 -0.393 0.014 0.242 0.463 0.040 1618 21 (g) -73 1406 1452 1831 1831 201 232 -1.357 -0.785 -0.301 1.597 0.068 1619 21 (g) -73 1301 1577 1828 1828 125 458 -0.020 -2.307 2.853 3.669 0.075 1620 21 (g) -73 1251 1617 1833 1833 355 269 -0.420 0.066 0.229 0.523 0.201 1621 21 (g) -73 1300 1412 1827 1827 458 453 -1.523 -3.592 4.323 5.829 0.258 1622 21 (g) -73 1420 1425 1832 1832 269 201 -2.812 -0.757 0.785 3.038 0.360 1623 2 (u) -73 1219 1283 1826 1826 453 0 -1.696 -4.529 2.507 5.489 0.676 1624 21 (g) -73 1255 1570 1801 1801 360 429 -0.325 0.534 -4.118 4.165 0.049 1625 21 (g) -73 1280 1567 1800 1800 429 383 -0.090 -0.394 -8.344 8.354 0.077 1626 21 (g) -73 1447 1457 1802 1802 271 360 -0.860 0.161 -3.282 3.398 0.119 1627 -3 (sbar) -73 1506 1572 1803 1803 0 271 -0.666 -0.591 -16.276 16.323 0.864 1628 -3 (sbar) -73 1264 1459 1629 0 0 487 0.196 0.922 388.930 388.931 0.529 1629 -3 (sbar) -73 1593 1628 1751 1751 0 230 0.591 1.225 538.277 538.279 0.813 1630 -2 (ubar) -73 1410 1524 1639 0 0 178 0.582 1.030 -4.506 4.671 0.338 1631 21 (g) -73 1304 1535 2088 2088 343 468 1.930 0.906 -1.953 2.892 0.066 1632 21 (g) -73 1234 1497 2105 2105 107 182 -0.469 0.744 1.092 1.405 0.086 1633 21 (g) -73 1256 1534 2076 2076 321 478 -0.807 0.679 -0.163 1.071 0.089 1634 21 (g) -73 1218 1492 2102 2102 188 233 0.036 1.084 0.382 1.156 0.113 1635 21 (g) -73 1466 1568 1641 0 173 275 -0.344 0.601 -2.457 2.558 0.160 1636 21 (g) -73 1227 1537 2086 2086 200 331 2.345 1.449 -2.020 3.422 0.178 1637 21 (g) -73 1296 1421 2095 2095 393 447 2.529 2.762 -4.847 6.129 0.231 1638 21 (g) -73 1222 1490 2079 2079 366 110 -0.440 4.568 0.416 4.614 0.238 1639 -2 (ubar) -73 1525 1630 2107 2107 0 173 1.281 2.526 -9.688 10.110 0.571 1640 21 (g) -73 1232 1268 2083 2083 166 386 -0.858 4.297 -1.949 4.809 0.355 1641 21 (g) -73 1556 1635 2106 2106 173 107 -0.853 1.005 -3.665 3.930 0.521 1642 21 (g) -73 1214 1250 2091 2091 357 287 50.538 34.649 -68.522 91.925 0.576 1643 21 (g) -73 1266 1520 1651 0 193 424 -0.589 -0.287 6.503 6.536 0.022 1644 21 (g) -73 1243 1580 1653 0 239 124 -0.204 2.029 311.000 311.006 0.089 1645 21 (g) -73 1544 1562 1654 0 423 158 -0.068 0.754 3.693 3.771 0.090 1646 21 (g) -73 1393 1395 1651 0 240 193 -2.412 -1.175 23.334 23.488 0.104 1647 21 (g) -73 1515 1557 1656 0 279 253 1.102 2.429 24.091 24.239 0.142 1648 21 (g) -73 1461 1471 1658 0 475 240 -0.146 0.535 11.146 11.161 0.156 1649 21 (g) -73 1413 1588 2045 2045 187 163 -1.060 0.105 44.398 44.411 0.168 1650 21 (g) -73 1288 1513 1658 0 416 475 0.304 1.368 25.402 25.441 0.190 1651 21 (g) -73 1643 1646 1659 0 240 424 -3.001 -1.462 29.837 30.024 0.215 1652 3 (s) -73 1260 1441 1657 0 304 0 -0.255 0.367 576.969 576.970 0.736 1653 21 (g) -73 1582 1644 2042 2042 229 124 -0.155 3.088 461.202 461.213 0.264 1654 21 (g) -73 1486 1645 2051 2051 411 158 0.122 1.632 8.251 8.416 0.284 1655 21 (g) -73 1435 1451 2043 2043 176 229 -0.143 2.180 179.110 179.123 0.335 1656 21 (g) -73 1489 1647 2048 2048 279 416 1.528 3.056 32.675 32.856 0.435 1657 3 (s) -73 1239 1652 2041 2041 124 0 -0.939 0.706 873.687 873.689 1.207 1658 21 (g) -73 1648 1650 2047 2047 416 240 0.158 1.903 36.548 36.602 0.566 1659 21 (g) -73 1437 1651 2046 2046 240 187 -3.635 -1.544 36.561 36.778 0.580 1660 21 (g) -73 1322 1350 1983 1983 470 259 0.798 0.445 15.504 15.537 0.433 1661 21 (g) -73 1311 1349 1985 1985 218 467 1.144 -0.520 3.644 3.887 0.498 1662 21 (g) -73 1318 1337 1990 1990 372 410 -0.266 0.485 0.040 0.813 0.595 1663 21 (g) -73 1321 1325 2007 2007 354 283 -0.387 0.189 0.065 0.495 0.235 1664 21 (g) -73 1317 1327 2011 2011 415 111 0.308 0.256 20.516 20.522 0.316 1665 -2 (ubar) -73 1330 1342 1668 0 0 375 -0.890 -1.794 -1.493 2.547 0.499 1666 21 (g) -73 1313 1328 1938 1938 384 113 -0.211 0.181 0.208 0.492 0.349 1667 21 (g) -73 1331 1339 1939 1939 194 384 -0.663 -1.123 -1.630 2.126 0.404 1668 -2 (ubar) -73 1338 1665 1669 0 0 330 -0.910 -2.499 -1.739 3.294 0.868 1669 -2 (ubar) -73 1319 1668 1944 1944 0 260 -1.360 -3.141 -2.301 4.258 1.061 1670 21 (g) -73 1500 1558 1676 0 266 238 0.065 -0.283 0.430 0.519 0.017 1671 21 (g) -73 1438 1529 1675 0 132 322 0.073 -0.235 3.949 3.956 0.018 1672 21 (g) -73 1411 1590 1679 0 474 181 0.319 -0.564 7.118 7.148 0.050 1673 21 (g) -73 1470 1532 1688 0 296 127 1.278 -0.137 7.297 7.410 0.076 1674 21 (g) -73 1483 1526 1909 1909 238 365 -0.063 -0.399 1.313 1.376 0.084 1675 21 (g) -73 1448 1671 1687 0 280 322 0.272 -0.584 11.364 11.383 0.086 1676 21 (g) -73 1272 1670 1686 0 350 238 0.267 -0.736 1.278 1.501 0.092 1677 21 (g) -73 1454 1531 1914 1914 289 379 0.989 -0.547 0.140 1.143 0.099 1678 21 (g) -73 1290 1403 1907 1907 425 474 0.637 -0.849 8.059 8.130 0.146 1679 21 (g) -73 1463 1672 1687 0 474 280 0.526 -0.824 11.773 11.814 0.148 1680 21 (g) -73 1440 1499 1913 1913 379 123 0.378 -0.030 0.712 0.826 0.180 1681 -1 (dbar) -73 1303 1560 1916 1916 0 210 -0.053 -0.126 0.076 0.529 0.505 1682 21 (g) -73 1237 1495 1689 0 242 216 0.421 0.700 1.051 1.345 0.195 1683 21 (g) -73 1505 1514 1905 1905 322 336 -0.259 -1.496 23.343 23.394 0.196 1684 21 (g) -73 1456 1536 1908 1908 365 425 0.294 -1.746 14.137 14.250 0.223 1685 21 (g) -73 1482 1527 1904 1904 336 329 -0.445 -1.308 10.822 10.913 0.262 1686 21 (g) -73 1419 1676 1910 1910 216 238 0.618 -1.003 2.004 2.351 0.350 1687 21 (g) -73 1675 1679 1906 1906 474 322 0.798 -1.408 23.137 23.197 0.402 1688 21 (g) -73 1521 1673 1901 1901 472 127 1.854 -0.071 9.379 9.571 0.443 1689 21 (g) -73 1245 1682 1911 1911 237 216 0.647 1.640 2.701 3.258 0.457 1690 -3 (sbar) -73 1453 1512 1691 0 0 367 2.372 1.181 -18.115 18.320 0.667 1691 -3 (sbar) -73 1528 1690 1755 1755 0 183 2.704 1.343 -19.369 19.627 0.978 1692 2 (u) -73 1402 1584 1754 1754 183 0 2.269 -0.559 -6.313 6.773 0.747 1693 21 (g) -73 1405 1455 1700 0 374 444 -0.424 0.532 23.693 23.703 0.072 1694 21 (g) -73 1223 1392 1699 0 309 464 -0.980 -1.028 6.284 6.443 0.095 1695 21 (g) -73 1496 1508 1879 1879 464 133 -0.731 -0.150 1.636 1.801 0.098 1696 21 (g) -73 1439 1559 1884 1884 341 374 0.186 0.624 25.992 26.001 0.099 1697 21 (g) -73 1295 1445 1701 0 340 300 -0.534 0.211 74.339 74.342 0.107 1698 21 (g) -73 1418 1424 1882 1882 243 142 -0.683 0.680 18.107 18.133 0.177 1699 21 (g) -73 1465 1694 1880 1880 257 464 -1.782 -1.979 12.204 12.492 0.182 1700 21 (g) -73 1246 1693 1883 1883 374 243 -1.170 1.080 52.901 52.925 0.249 1701 21 (g) -73 1578 1697 1886 1886 340 251 -0.906 0.809 154.456 154.461 0.435 1702 3 (s) -73 1436 1519 1746 1746 443 0 3.789 2.066 -38.291 38.541 0.778 1703 21 (g) -73 1477 1587 1704 0 402 318 -0.294 0.617 2.395 2.491 0.039 1704 21 (g) -73 1487 1703 1767 1767 402 135 -0.366 1.250 4.404 4.598 0.234 1705 21 (g) -73 1217 1510 1770 1770 403 273 -1.862 0.927 3.275 3.891 0.303 1706 21 (g) -73 1409 1551 1712 0 291 207 1.529 0.562 22.026 22.086 0.069 1707 21 (g) -73 1546 1548 1714 0 409 432 0.537 -0.300 12.526 12.541 0.100 1708 21 (g) -73 1464 1547 1713 0 432 431 -0.255 -0.541 17.114 17.125 0.115 1709 21 (g) -73 1407 1415 1846 1846 215 156 -0.622 -0.408 48.303 48.309 0.138 1710 21 (g) -73 1554 1581 1850 1850 184 196 1.295 0.128 34.114 34.139 0.175 1711 21 (g) -73 1517 1555 1847 1847 175 215 -2.223 -1.607 59.988 60.051 0.207 1712 21 (g) -73 1414 1706 1851 1851 291 184 2.771 1.073 42.734 42.838 0.223 1713 21 (g) -73 1462 1708 1848 1848 432 175 -1.006 -1.368 46.217 46.249 0.317 1714 21 (g) -73 1458 1707 1849 1849 196 432 1.327 -0.506 40.013 40.040 0.440 1715 21 (g) -73 1416 1422 1965 1965 310 146 1.457 -0.730 -213.186 213.193 0.348 1716 21 (g) -73 1225 1538 1725 0 277 388 -0.885 1.210 -0.943 1.771 0.040 1717 21 (g) -73 1247 1398 1729 0 129 246 -0.273 -0.155 0.273 0.418 0.044 1718 21 (g) -73 1404 1571 2160 2160 392 277 -0.728 0.380 -0.519 0.975 0.080 1719 21 (g) -73 1297 1475 1730 0 448 390 0.333 -1.060 -0.751 1.344 0.091 1720 21 (g) -73 1230 1432 2167 2167 103 241 -1.868 -2.399 2.700 4.067 0.099 1721 21 (g) -73 1270 1408 2168 2168 342 103 -8.893 -16.878 11.323 22.185 0.106 1722 21 (g) -73 1485 1586 1732 0 396 392 -1.013 0.213 -1.108 1.522 0.124 1723 21 (g) -73 1273 1498 2164 2164 246 352 0.104 -0.969 0.035 0.987 0.153 1724 21 (g) -73 1460 1530 2162 2162 153 419 -0.811 0.116 -0.116 0.842 0.157 1725 21 (g) -73 1444 1716 2159 2159 277 140 -1.118 1.525 -1.101 2.194 0.159 1726 21 (g) -73 1484 1539 2154 2154 258 457 -0.177 -1.550 -1.123 1.930 0.172 1727 21 (g) -73 1302 1503 1734 0 164 362 1.878 -1.374 -22.514 22.635 0.177 1728 -2 (ubar) -73 1287 1291 2172 2172 0 305 -2.295 -7.392 3.445 8.487 0.513 1729 21 (g) -73 1244 1717 2165 2165 398 246 -2.211 -1.853 1.772 3.399 0.306 1730 21 (g) -73 1493 1719 2155 2155 448 258 1.450 -5.208 -4.256 6.888 0.332 1731 21 (g) -73 1226 1569 2151 2151 460 144 2.894 -0.996 -14.431 14.756 0.353 1732 21 (g) -73 1592 1722 2161 2161 419 392 -1.833 0.061 -1.839 2.631 0.417 1733 21 (g) -73 1298 1434 2157 2157 149 449 4.719 0.494 -8.440 9.692 0.446 1734 21 (g) -73 1576 1727 2152 2152 164 460 2.451 -1.543 -27.204 27.363 0.512 1735 21 (g) -73 1377 1380 1760 1760 114 426 0.502 0.699 0.843 1.230 0.249 1736 -1 (dbar) -73 1361 1382 1737 0 0 320 -1.075 -0.058 0.354 1.348 0.730 1737 -1 (dbar) -73 1373 1736 1761 1761 0 114 -1.809 -0.388 1.240 2.545 1.231 1738 1 (d) -73 1368 1545 1759 1759 426 0 -0.373 -0.074 1.391 1.653 0.807 1739 21 (g) -73 1242 1589 1778 1778 204 346 -0.736 1.206 0.474 1.491 0.039 1740 -1 (dbar) -73 1263 1277 1781 1781 0 364 -5.811 4.140 0.259 7.177 0.733 1741 21 (g) -73 1426 1579 1745 0 477 442 -0.009 0.149 -10.446 10.447 0.082 1742 21 (g) -73 1423 1518 1744 0 430 377 1.052 0.164 -12.644 12.689 0.141 1743 2 (u) -73 1583 1585 1744 0 377 0 2.438 0.895 -27.076 27.205 0.476 1744 2 (u) -73 1742 1743 1812 1812 430 0 3.490 1.059 -39.720 39.894 0.742 1745 21 (g) -73 1573 1741 1815 1815 477 174 0.251 0.160 -18.120 18.126 0.347 1746 3 (s) -71 1702 1702 1748 1749 443 0 3.789 2.066 -38.291 38.541 0.778 1747 -2 (ubar) -71 1591 1591 1748 1749 0 443 0.463 0.111 -6.310 6.337 0.330 1748 -311 (Kbar0) -82 1746 1747 2312 2312 0 0 3.242 1.768 -29.040 29.278 0.498 1749 -211 pi- 82 1746 1747 0 0 0 0 1.010 0.409 -15.561 15.600 0.140 1750 2 (u) -71 1228 1228 1752 1753 230 0 -0.372 0.331 155.482 155.483 0.330 1751 -3 (sbar) -71 1629 1629 1752 1753 0 230 0.591 1.225 538.277 538.279 0.813 1752 111 (pi0) -82 1750 1751 2599 2600 0 0 0.514 1.026 402.617 402.619 0.135 1753 323 (K*+) -82 1750 1751 2313 2314 0 0 -0.295 0.530 291.141 291.143 0.832 1754 2 (u) -71 1692 1692 1756 1758 183 0 2.269 -0.559 -6.313 6.773 0.747 1755 -3 (sbar) -71 1691 1691 1756 1758 0 183 2.704 1.343 -19.369 19.627 0.978 1756 331 (eta') -83 1754 1755 2601 2603 0 0 2.253 0.234 -7.612 7.999 0.958 1757 211 pi+ 83 1754 1755 0 0 0 0 0.758 -0.437 -2.512 2.664 0.140 1758 313 (K*0) -84 1754 1755 2315 2316 0 0 1.962 0.987 -15.558 15.737 0.884 1759 1 (d) -71 1738 1738 1762 1765 426 0 -0.373 -0.074 1.391 1.653 0.807 1760 21 (g) -71 1735 1735 1762 1765 114 426 0.502 0.699 0.843 1.230 0.249 1761 -1 (dbar) -71 1737 1737 1762 1765 0 114 -1.809 -0.388 1.240 2.545 1.231 1762 -213 (rho-) -83 1759 1761 2317 2318 0 0 0.198 0.299 1.175 1.568 0.974 1763 111 (pi0) -83 1759 1761 2604 2605 0 0 -0.741 0.063 1.313 1.515 0.135 1764 223 (omega) -83 1759 1761 2606 2608 0 0 -1.443 -0.379 0.831 1.895 0.821 1765 211 pi+ 84 1759 1761 0 0 0 0 0.306 0.255 0.154 0.449 0.140 1766 1 (d) -71 1474 1474 1772 1776 135 0 -0.874 0.134 3.950 4.061 0.330 1767 21 (g) -71 1704 1704 1772 1776 402 135 -0.366 1.250 4.404 4.598 0.234 1768 21 (g) -71 1274 1274 1772 1776 292 402 -1.877 2.523 9.680 10.178 0.000 1769 21 (g) -71 1259 1259 1772 1776 273 292 -0.141 0.046 1.139 1.148 0.000 1770 21 (g) -71 1705 1705 1772 1776 403 273 -1.862 0.927 3.275 3.891 0.303 1771 -1 (dbar) -71 1494 1494 1772 1776 0 403 -0.106 0.407 1.155 1.273 0.330 1772 113 (rho0) -83 1766 1771 2319 2320 0 0 -1.446 2.095 8.783 9.188 0.891 1773 223 (omega) -83 1766 1771 2609 2611 0 0 -1.066 1.341 7.978 8.197 0.779 1774 -211 pi- 84 1766 1771 0 0 0 0 -1.241 0.598 1.962 2.401 0.140 1775 211 pi+ 84 1766 1771 0 0 0 0 -0.157 0.429 1.074 1.175 0.140 1776 113 (rho0) -84 1766 1771 2321 2322 0 0 -1.315 0.823 3.805 4.188 0.809 1777 1 (d) -71 1561 1561 1782 1786 346 0 0.065 -0.287 -0.512 0.677 0.330 1778 21 (g) -71 1739 1739 1782 1786 204 346 -0.736 1.206 0.474 1.491 0.039 1779 21 (g) -71 1216 1216 1782 1786 161 204 -2.507 2.135 -0.093 3.294 0.000 1780 21 (g) -71 1276 1276 1782 1786 364 161 0.025 0.095 0.076 0.124 0.000 1781 -1 (dbar) -71 1740 1740 1782 1786 0 364 -5.811 4.140 0.259 7.177 0.733 1782 111 (pi0) -83 1777 1781 2612 2613 0 0 -0.265 0.355 0.413 0.620 0.135 1783 111 (pi0) -83 1777 1781 2614 2615 0 0 -0.881 0.472 -0.254 1.040 0.135 1784 111 (pi0) -84 1777 1781 2616 2617 0 0 0.399 0.731 -0.396 0.932 0.135 1785 -211 pi- 84 1777 1781 0 0 0 0 -3.617 2.123 0.759 4.264 0.140 1786 213 (rho+) -84 1777 1781 2323 2324 0 0 -4.602 3.608 -0.317 5.906 0.769 1787 2 (u) -71 1604 1604 1789 1796 491 0 -0.547 -0.204 -15.751 15.766 0.330 1788 2103 (ud_1) -71 1601 1601 1789 1796 0 491 -0.115 -0.638 -3681.704 3681.704 0.771 1789 321 K+ 83 1787 1788 0 0 0 0 -0.218 -0.059 -29.304 29.309 0.494 1790 -311 (Kbar0) -83 1787 1788 2325 2325 0 0 -0.442 -0.400 -151.397 151.399 0.498 1791 111 (pi0) -83 1787 1788 2618 2619 0 0 0.238 0.303 -85.496 85.497 0.135 1792 -211 pi- 83 1787 1788 0 0 0 0 0.040 0.177 -7.576 7.579 0.140 1793 213 (rho+) -83 1787 1788 2326 2327 0 0 -0.050 -0.093 -255.367 255.369 0.986 1794 111 (pi0) -84 1787 1788 2620 2621 0 0 -0.347 0.005 -817.805 817.805 0.135 1795 2112 n0 84 1787 1788 0 0 0 0 0.173 -0.355 -779.726 779.727 0.940 1796 223 (omega) -84 1787 1788 2622 2624 0 0 -0.056 -0.419 -1570.785 1570.785 0.783 1797 2 (u) -71 1220 1220 1804 1811 247 0 -15.561 -5.138 -331.260 331.665 0.330 1798 21 (g) -71 1248 1248 1804 1811 326 247 -0.177 -0.331 -8.856 8.864 0.000 1799 21 (g) -71 1265 1265 1804 1811 383 326 -4.237 -0.199 -73.895 74.016 0.000 1800 21 (g) -71 1625 1625 1804 1811 429 383 -0.090 -0.394 -8.344 8.354 0.077 1801 21 (g) -71 1624 1624 1804 1811 360 429 -0.325 0.534 -4.118 4.165 0.049 1802 21 (g) -71 1626 1626 1804 1811 271 360 -0.860 0.161 -3.282 3.398 0.119 1803 -3 (sbar) -71 1627 1627 1804 1811 0 271 -0.666 -0.591 -16.276 16.323 0.864 1804 223 (omega) -83 1797 1803 2625 2626 0 0 -10.093 -2.796 -208.802 209.066 0.785 1805 223 (omega) -84 1797 1803 2627 2629 0 0 -3.914 -1.454 -92.173 92.271 0.814 1806 2114 (Delta0) -84 1797 1803 2328 2329 0 0 -3.473 -1.154 -63.757 63.874 1.270 1807 211 pi+ 84 1797 1803 0 0 0 0 0.128 -0.149 -5.795 5.800 0.140 1808 -2214 (Deltabar-) -84 1797 1803 2330 2331 0 0 -2.403 0.321 -32.926 33.037 1.207 1809 211 pi+ 84 1797 1803 0 0 0 0 -0.678 -0.397 -23.269 23.282 0.140 1810 221 (eta) -84 1797 1803 2630 2631 0 0 -0.977 0.140 -5.200 5.321 0.548 1811 311 (K0) -84 1797 1803 2332 2332 0 0 -0.504 -0.467 -14.109 14.134 0.498 1812 2 (u) -71 1744 1744 1818 1825 430 0 3.490 1.059 -39.720 39.894 0.742 1813 21 (g) -71 1511 1511 1818 1825 235 430 1.674 -0.134 -23.329 23.390 0.000 1814 21 (g) -71 1566 1566 1818 1825 174 235 0.690 -0.735 -21.296 21.320 0.000 1815 21 (g) -71 1745 1745 1818 1825 477 174 0.251 0.160 -18.120 18.126 0.347 1816 21 (g) -71 1516 1516 1818 1825 328 477 -0.868 -1.286 -167.196 167.203 0.000 1817 -3 (sbar) -71 1507 1507 1818 1825 0 328 -0.462 -2.422 -187.505 187.522 0.500 1818 213 (rho+) -83 1812 1817 2333 2334 0 0 1.227 0.009 -14.316 14.382 0.635 1819 -213 (rho-) -83 1812 1817 2335 2336 0 0 2.695 -0.135 -43.465 43.562 1.103 1820 223 (omega) -83 1812 1817 2632 2634 0 0 0.974 0.623 -18.943 18.994 0.784 1821 211 pi+ 83 1812 1817 0 0 0 0 0.750 0.058 -7.767 7.804 0.140 1822 -211 pi- 83 1812 1817 0 0 0 0 0.153 -0.021 -4.927 4.932 0.140 1823 113 (rho0) -84 1812 1817 2337 2338 0 0 -0.449 -1.150 -156.879 156.887 0.878 1824 221 (eta) -84 1812 1817 2635 2637 0 0 -0.207 -1.989 -120.220 120.238 0.548 1825 321 K+ 84 1812 1817 0 0 0 0 -0.368 -0.753 -90.650 90.655 0.494 1826 2 (u) -71 1623 1623 1835 1843 453 0 -1.696 -4.529 2.507 5.489 0.676 1827 21 (g) -71 1621 1621 1835 1843 458 453 -1.523 -3.592 4.323 5.829 0.258 1828 21 (g) -71 1619 1619 1835 1843 125 458 -0.020 -2.307 2.853 3.669 0.075 1829 21 (g) -71 1224 1224 1835 1843 452 125 -1.007 -8.219 11.688 14.324 0.000 1830 21 (g) -71 1299 1299 1835 1843 232 452 -0.347 -0.583 0.932 1.153 0.000 1831 21 (g) -71 1618 1618 1835 1843 201 232 -1.357 -0.785 -0.301 1.597 0.068 1832 21 (g) -71 1622 1622 1835 1843 269 201 -2.812 -0.757 0.785 3.038 0.360 1833 21 (g) -71 1620 1620 1835 1843 355 269 -0.420 0.066 0.229 0.523 0.201 1834 -1 (dbar) -71 1480 1480 1835 1843 0 355 -0.289 2.553 6.748 7.228 0.330 1835 223 (omega) -83 1826 1834 2638 2640 0 0 -0.729 -2.512 1.580 3.155 0.784 1836 213 (rho+) -83 1826 1834 2339 2340 0 0 -1.602 -4.335 3.598 5.896 0.679 1837 311 (K0) -83 1826 1834 2341 2341 0 0 -0.990 -1.938 3.146 3.858 0.498 1838 333 (phi) -83 1826 1834 2641 2642 0 0 -0.557 -7.414 8.668 11.465 1.018 1839 333 (phi) -84 1826 1834 2643 2644 0 0 -0.882 -2.601 4.805 5.629 1.027 1840 -311 (Kbar0) -84 1826 1834 2342 2342 0 0 -2.216 -1.260 0.483 2.642 0.498 1841 113 (rho0) -84 1826 1834 2343 2344 0 0 -0.464 -0.208 0.471 1.026 0.757 1842 -213 (rho-) -84 1826 1834 2345 2346 0 0 -1.116 -0.762 0.058 1.543 0.743 1843 213 (rho+) -84 1826 1834 2347 2348 0 0 -0.913 2.879 6.956 7.637 0.902 1844 1 (d) -71 1481 1481 1853 1868 334 0 -1.197 0.586 176.651 176.657 0.330 1845 21 (g) -71 1542 1542 1853 1868 156 334 -1.363 -2.147 175.466 175.485 0.000 1846 21 (g) -71 1709 1709 1853 1868 215 156 -0.622 -0.408 48.303 48.309 0.138 1847 21 (g) -71 1711 1711 1853 1868 175 215 -2.223 -1.607 59.988 60.051 0.207 1848 21 (g) -71 1713 1713 1853 1868 432 175 -1.006 -1.368 46.217 46.249 0.317 1849 21 (g) -71 1714 1714 1853 1868 196 432 1.327 -0.506 40.013 40.040 0.440 1850 21 (g) -71 1710 1710 1853 1868 184 196 1.295 0.128 34.114 34.139 0.175 1851 21 (g) -71 1712 1712 1853 1868 291 184 2.771 1.073 42.734 42.838 0.223 1852 -2 (ubar) -71 1417 1417 1853 1868 0 291 2.159 0.880 12.864 13.078 0.330 1853 -213 (rho-) -83 1844 1852 2349 2350 0 0 -1.463 0.160 191.421 191.430 0.962 1854 111 (pi0) -83 1844 1852 2645 2646 0 0 -0.381 -0.877 70.785 70.791 0.135 1855 2212 p+ 83 1844 1852 0 0 0 0 -1.064 -0.750 60.966 60.987 0.938 1856 -2212 pbar- 83 1844 1852 0 0 0 0 -0.656 -0.443 62.482 62.494 0.938 1857 211 pi+ 83 1844 1852 0 0 0 0 -0.928 -1.680 64.343 64.372 0.140 1858 111 (pi0) -83 1844 1852 2647 2648 0 0 0.076 0.220 6.142 6.148 0.135 1859 221 (eta) -83 1844 1852 2649 2651 0 0 -0.168 -0.589 17.294 17.313 0.548 1860 -211 pi- 83 1844 1852 0 0 0 0 -0.163 -0.070 9.939 9.941 0.140 1861 211 pi+ 83 1844 1852 0 0 0 0 -0.533 -0.965 26.513 26.536 0.140 1862 -211 pi- 83 1844 1852 0 0 0 0 0.274 0.331 9.211 9.222 0.140 1863 113 (rho0) -83 1844 1852 2351 2352 0 0 0.147 -0.522 31.850 31.861 0.586 1864 211 pi+ 83 1844 1852 0 0 0 0 0.353 -0.402 12.138 12.150 0.140 1865 111 (pi0) -84 1844 1852 2652 2653 0 0 1.132 0.695 19.437 19.482 0.135 1866 111 (pi0) -84 1844 1852 2654 2655 0 0 1.992 1.071 16.071 16.230 0.135 1867 -213 (rho-) -84 1844 1852 2353 2354 0 0 1.879 -0.018 27.070 27.156 1.048 1868 221 (eta) -84 1844 1852 2656 2658 0 0 0.644 0.469 10.689 10.733 0.548 1869 2 (u) -71 1600 1600 1871 1877 168 0 -1.410 -0.305 54.716 54.736 0.330 1870 -1 (dbar) -71 1552 1552 1871 1877 0 168 -2.006 1.947 -2.893 4.037 0.330 1871 321 K+ 83 1869 1870 0 0 0 0 -0.089 -0.228 14.461 14.472 0.494 1872 -311 (Kbar0) -83 1869 1870 2355 2355 0 0 -0.449 0.192 14.461 14.477 0.498 1873 -211 pi- 83 1869 1870 0 0 0 0 -0.980 -0.506 18.143 18.177 0.140 1874 211 pi+ 84 1869 1870 0 0 0 0 0.392 0.282 1.931 1.995 0.140 1875 2114 (Delta0) -84 1869 1870 2356 2357 0 0 -0.188 -0.082 4.337 4.492 1.151 1876 -213 (rho-) -84 1869 1870 2358 2359 0 0 -0.431 -0.078 0.759 1.441 1.144 1877 -1114 (Deltabar+) -84 1869 1870 2360 2361 0 0 -1.672 2.061 -2.269 3.719 1.280 1878 2 (u) -71 1431 1431 1888 1899 133 0 -0.754 0.868 4.304 4.467 0.330 1879 21 (g) -71 1695 1695 1888 1899 464 133 -0.731 -0.150 1.636 1.801 0.098 1880 21 (g) -71 1699 1699 1888 1899 257 464 -1.782 -1.979 12.204 12.492 0.182 1881 21 (g) -71 1401 1401 1888 1899 142 257 -1.309 0.190 20.143 20.186 0.000 1882 21 (g) -71 1698 1698 1888 1899 243 142 -0.683 0.680 18.107 18.133 0.177 1883 21 (g) -71 1700 1700 1888 1899 374 243 -1.170 1.080 52.901 52.925 0.249 1884 21 (g) -71 1696 1696 1888 1899 341 374 0.186 0.624 25.992 26.001 0.099 1885 21 (g) -71 1488 1488 1888 1899 251 341 -0.660 1.127 93.780 93.789 0.000 1886 21 (g) -71 1701 1701 1888 1899 340 251 -0.906 0.809 154.456 154.461 0.435 1887 -1 (dbar) -71 1479 1479 1888 1899 0 340 -0.347 -0.572 182.811 182.812 0.330 1888 113 (rho0) -83 1878 1887 2362 2363 0 0 -1.115 0.664 5.400 5.606 0.763 1889 213 (rho+) -83 1878 1887 2364 2365 0 0 -0.900 -1.260 12.676 12.802 0.907 1890 -213 (rho-) -83 1878 1887 2366 2367 0 0 -1.194 0.111 4.653 4.862 0.743 1891 223 (omega) -83 1878 1887 2659 2661 0 0 -0.899 0.253 19.530 19.568 0.771 1892 111 (pi0) -83 1878 1887 2662 2663 0 0 -0.616 -0.296 3.268 3.342 0.135 1893 211 pi+ 84 1878 1887 0 0 0 0 0.067 0.514 23.825 23.831 0.140 1894 111 (pi0) -84 1878 1887 2664 2665 0 0 -0.046 -0.133 9.929 9.931 0.135 1895 113 (rho0) -84 1878 1887 2368 2369 0 0 -1.181 0.663 29.840 29.880 0.745 1896 223 (omega) -84 1878 1887 2666 2668 0 0 -0.504 1.216 116.341 116.351 0.784 1897 111 (pi0) -84 1878 1887 2669 2670 0 0 -0.099 -0.065 1.543 1.553 0.135 1898 313 (K*0) -84 1878 1887 2370 2371 0 0 -0.992 1.470 185.552 185.563 0.989 1899 -311 (Kbar0) -84 1878 1887 2372 2372 0 0 -0.677 -0.460 153.776 153.779 0.498 1900 2 (u) -71 1399 1399 1917 1936 127 0 1.095 -0.167 10.050 10.117 0.330 1901 21 (g) -71 1688 1688 1917 1936 472 127 1.854 -0.071 9.379 9.571 0.443 1902 21 (g) -71 1269 1269 1917 1936 418 472 0.113 0.018 0.022 0.116 0.000 1903 21 (g) -71 1553 1553 1917 1936 329 418 -0.893 -1.103 10.266 10.364 0.000 1904 21 (g) -71 1685 1685 1917 1936 336 329 -0.445 -1.308 10.822 10.913 0.262 1905 21 (g) -71 1683 1683 1917 1936 322 336 -0.259 -1.496 23.343 23.394 0.196 1906 21 (g) -71 1687 1687 1917 1936 474 322 0.798 -1.408 23.137 23.197 0.402 1907 21 (g) -71 1678 1678 1917 1936 425 474 0.637 -0.849 8.059 8.130 0.146 1908 21 (g) -71 1684 1684 1917 1936 365 425 0.294 -1.746 14.137 14.250 0.223 1909 21 (g) -71 1674 1674 1917 1936 238 365 -0.063 -0.399 1.313 1.376 0.084 1910 21 (g) -71 1686 1686 1917 1936 216 238 0.618 -1.003 2.004 2.351 0.350 1911 21 (g) -71 1689 1689 1917 1936 237 216 0.647 1.640 2.701 3.258 0.457 1912 21 (g) -71 1388 1388 1917 1936 123 237 1.336 1.375 5.296 5.633 0.000 1913 21 (g) -71 1680 1680 1917 1936 379 123 0.378 -0.030 0.712 0.826 0.180 1914 21 (g) -71 1677 1677 1917 1936 289 379 0.989 -0.547 0.140 1.143 0.099 1915 21 (g) -71 1596 1596 1917 1936 210 289 1.518 -0.844 -0.821 1.921 0.000 1916 -1 (dbar) -71 1681 1681 1917 1936 0 210 -0.053 -0.126 0.076 0.529 0.505 1917 113 (rho0) -83 1900 1916 2373 2374 0 0 1.677 0.057 11.148 11.302 0.797 1918 211 pi+ 83 1900 1916 0 0 0 0 0.484 -0.905 5.625 5.720 0.140 1919 331 (eta') -83 1900 1916 2671 2673 0 0 0.127 0.222 4.821 4.922 0.958 1920 331 (eta') -83 1900 1916 2674 2676 0 0 -0.240 -0.987 14.869 14.934 0.958 1921 -213 (rho-) -83 1900 1916 2375 2376 0 0 0.350 -1.129 12.126 12.215 0.875 1922 213 (rho+) -83 1900 1916 2377 2378 0 0 0.367 -1.257 13.216 13.304 0.787 1923 2112 n0 83 1900 1916 0 0 0 0 -0.551 -2.070 23.872 23.986 0.940 1924 -2212 pbar- 83 1900 1916 0 0 0 0 0.430 -1.133 9.604 9.726 0.938 1925 223 (omega) -83 1900 1916 2677 2679 0 0 0.585 -1.115 12.109 12.199 0.784 1926 321 K+ 84 1900 1916 0 0 0 0 0.288 -0.228 1.006 1.180 0.494 1927 -321 K- 84 1900 1916 0 0 0 0 -0.101 0.223 1.830 1.911 0.494 1928 211 pi+ 84 1900 1916 0 0 0 0 0.343 -0.629 2.799 2.893 0.140 1929 -211 pi- 84 1900 1916 0 0 0 0 0.472 0.829 2.251 2.449 0.140 1930 213 (rho+) -84 1900 1916 2379 2380 0 0 0.821 0.232 2.570 2.989 1.265 1931 3212 (Sigma0) -84 1900 1916 2680 2681 0 0 0.680 0.330 1.858 2.333 1.193 1932 -3222 (Sigmabar-) -84 1900 1916 2682 2683 0 0 1.134 0.395 0.748 1.848 1.189 1933 113 (rho0) -84 1900 1916 2381 2382 0 0 0.284 -0.199 0.279 0.910 0.794 1934 113 (rho0) -84 1900 1916 2383 2384 0 0 1.260 -0.701 -0.155 1.791 1.052 1935 211 pi+ 84 1900 1916 0 0 0 0 0.209 -0.101 0.110 0.292 0.140 1936 111 (pi0) -84 1900 1916 2684 2685 0 0 -0.053 0.102 -0.049 0.184 0.135 1937 1 (d) -71 1603 1603 1945 1963 113 0 -0.182 -0.124 -132.321 132.321 0.330 1938 21 (g) -71 1666 1666 1945 1963 384 113 -0.211 0.181 0.208 0.492 0.349 1939 21 (g) -71 1667 1667 1945 1963 194 384 -0.663 -1.123 -1.630 2.126 0.404 1940 21 (g) -71 1312 1312 1945 1963 155 194 -4.036 0.512 -3.865 5.611 0.000 1941 21 (g) -71 1347 1347 1945 1963 459 155 -0.820 0.086 -1.353 1.585 0.000 1942 21 (g) -71 1315 1315 1945 1963 206 459 -0.378 -0.221 -0.010 0.438 0.000 1943 21 (g) -71 1323 1323 1945 1963 260 206 -2.421 -0.169 -1.701 2.963 0.000 1944 -2 (ubar) -71 1669 1669 1945 1963 0 260 -1.360 -3.141 -2.301 4.258 1.061 1945 -211 pi- 83 1937 1944 0 0 0 0 -0.360 -0.306 -48.132 48.135 0.140 1946 111 (pi0) -83 1937 1944 2686 2687 0 0 0.316 0.374 -12.477 12.487 0.135 1947 213 (rho+) -83 1937 1944 2385 2386 0 0 0.163 -0.246 -21.107 21.128 0.899 1948 -213 (rho-) -83 1937 1944 2387 2388 0 0 -0.083 -0.025 -19.827 19.846 0.856 1949 211 pi+ 83 1937 1944 0 0 0 0 -0.216 0.089 -2.455 2.470 0.140 1950 223 (omega) -83 1937 1944 2688 2690 0 0 0.054 -0.231 -15.288 15.309 0.771 1951 221 (eta) -83 1937 1944 2691 2693 0 0 -0.084 0.314 -2.013 2.112 0.548 1952 223 (omega) -83 1937 1944 2694 2696 0 0 0.137 -0.234 -6.638 6.682 0.714 1953 -211 pi- 83 1937 1944 0 0 0 0 -0.226 0.059 -0.173 0.322 0.140 1954 113 (rho0) -83 1937 1944 2389 2390 0 0 -0.505 -0.094 -4.226 4.337 0.827 1955 213 (rho+) -84 1937 1944 2391 2392 0 0 -0.641 -0.072 -1.630 1.964 0.886 1956 2112 n0 84 1937 1944 0 0 0 0 -1.120 0.153 -0.809 1.678 0.940 1957 -2212 pbar- 84 1937 1944 0 0 0 0 -1.442 -1.062 -1.735 2.664 0.938 1958 211 pi+ 84 1937 1944 0 0 0 0 -1.469 -0.074 -1.315 1.978 0.140 1959 -211 pi- 84 1937 1944 0 0 0 0 -0.074 0.172 -0.157 0.281 0.140 1960 213 (rho+) -84 1937 1944 2393 2394 0 0 -2.468 -0.365 -2.546 3.669 0.866 1961 223 (omega) -84 1937 1944 2697 2699 0 0 -0.624 -0.290 -0.445 1.129 0.776 1962 -213 (rho-) -84 1937 1944 2395 2396 0 0 -1.063 -1.019 -1.217 2.168 1.025 1963 111 (pi0) -84 1937 1944 2700 2701 0 0 -0.365 -1.141 -0.781 1.437 0.135 1964 3 (s) -71 1504 1504 1967 1981 146 0 -1.263 -0.625 -543.420 543.422 0.500 1965 21 (g) -71 1715 1715 1967 1981 310 146 1.457 -0.730 -213.186 213.193 0.348 1966 -2 (ubar) -71 1565 1565 1967 1981 0 310 -0.099 1.208 0.023 1.256 0.330 1967 -321 K- 83 1964 1966 0 0 0 0 0.062 -0.292 -150.752 150.753 0.494 1968 321 K+ 83 1964 1966 0 0 0 0 -0.571 -0.209 -226.021 226.022 0.494 1969 -321 K- 83 1964 1966 0 0 0 0 0.180 -0.295 -154.279 154.280 0.494 1970 211 pi+ 83 1964 1966 0 0 0 0 -0.070 -0.035 -43.537 43.537 0.140 1971 223 (omega) -83 1964 1966 2702 2704 0 0 -0.050 -0.112 -39.459 39.467 0.792 1972 111 (pi0) -83 1964 1966 2705 2706 0 0 0.279 -0.314 -62.515 62.517 0.135 1973 111 (pi0) -83 1964 1966 2707 2708 0 0 -0.370 0.032 -8.910 8.919 0.135 1974 -213 (rho-) -83 1964 1966 2397 2398 0 0 0.705 -0.039 -48.492 48.506 0.927 1975 111 (pi0) -83 1964 1966 2709 2710 0 0 -0.336 0.048 -1.352 1.401 0.135 1976 211 pi+ 84 1964 1966 0 0 0 0 0.501 -0.286 -7.733 7.756 0.140 1977 -211 pi- 84 1964 1966 0 0 0 0 0.077 0.484 -1.968 2.033 0.140 1978 113 (rho0) -84 1964 1966 2399 2400 0 0 0.225 -0.046 -7.436 7.503 0.968 1979 213 (rho+) -84 1964 1966 2401 2402 0 0 -0.193 0.030 -1.792 2.055 0.986 1980 -211 pi- 84 1964 1966 0 0 0 0 -0.068 0.625 -2.133 2.228 0.140 1981 223 (omega) -84 1964 1966 2711 2713 0 0 -0.278 0.261 -0.203 0.895 0.784 1982 1 (d) -71 1308 1308 1993 2005 259 0 2.332 4.396 46.776 47.041 0.330 1983 21 (g) -71 1660 1660 1993 2005 470 259 0.798 0.445 15.504 15.537 0.433 1984 21 (g) -71 1348 1348 1993 2005 467 470 1.055 0.666 5.025 5.177 0.000 1985 21 (g) -71 1661 1661 1993 2005 218 467 1.144 -0.520 3.644 3.887 0.498 1986 21 (g) -71 1341 1341 1993 2005 399 218 0.362 0.274 0.350 0.573 0.000 1987 21 (g) -71 1324 1324 1993 2005 267 399 2.311 -0.109 4.051 4.665 0.000 1988 21 (g) -71 1320 1320 1993 2005 250 267 -0.081 0.447 0.938 1.042 0.000 1989 21 (g) -71 1343 1343 1993 2005 410 250 0.192 -0.183 1.392 1.417 0.000 1990 21 (g) -71 1662 1662 1993 2005 372 410 -0.266 0.485 0.040 0.813 0.595 1991 21 (g) -71 1335 1335 1993 2005 112 372 0.321 -0.640 0.025 0.717 0.000 1992 -1 (dbar) -71 1316 1316 1993 2005 0 112 1.518 -0.694 -6.425 6.646 0.330 1993 -211 pi- 83 1982 1992 0 0 0 0 0.268 0.647 6.083 6.125 0.140 1994 211 pi+ 83 1982 1992 0 0 0 0 1.777 3.242 36.357 36.544 0.140 1995 113 (rho0) -83 1982 1992 2403 2404 0 0 0.920 0.473 7.118 7.236 0.794 1996 223 (omega) -83 1982 1992 2714 2716 0 0 0.606 0.535 10.290 10.338 0.570 1997 -213 (rho-) -83 1982 1992 2405 2406 0 0 0.479 -0.072 2.077 2.264 0.760 1998 211 pi+ 84 1982 1992 0 0 0 0 0.747 -0.324 6.218 6.272 0.140 1999 -211 pi- 84 1982 1992 0 0 0 0 1.236 0.963 2.928 3.324 0.140 2000 213 (rho+) -84 1982 1992 2407 2408 0 0 0.611 0.072 2.295 2.485 0.726 2001 -213 (rho-) -84 1982 1992 2409 2410 0 0 -0.173 -0.109 0.957 1.258 0.790 2002 211 pi+ 84 1982 1992 0 0 0 0 1.700 -0.000 2.723 3.213 0.140 2003 313 (K*0) -84 1982 1992 2411 2412 0 0 -0.376 -0.038 0.501 1.101 0.904 2004 -311 (Kbar0) -84 1982 1992 2413 2413 0 0 0.525 0.230 0.069 0.762 0.498 2005 113 (rho0) -84 1982 1992 2414 2415 0 0 1.367 -1.052 -6.297 6.593 0.917 2006 2 (u) -71 1309 1309 2017 2034 283 0 -0.284 -0.309 -0.592 0.797 0.330 2007 21 (g) -71 1663 1663 2017 2034 354 283 -0.387 0.189 0.065 0.495 0.235 2008 21 (g) -71 1334 1334 2017 2034 286 354 0.155 -0.442 2.794 2.833 0.000 2009 21 (g) -71 1326 1326 2017 2034 339 286 -0.503 0.186 13.890 13.901 0.000 2010 21 (g) -71 1332 1332 2017 2034 111 339 0.346 0.408 5.792 5.817 0.000 2011 21 (g) -71 1664 1664 2017 2034 415 111 0.308 0.256 20.516 20.522 0.316 2012 21 (g) -71 1346 1346 2017 2034 434 415 0.164 -0.679 41.987 41.993 0.000 2013 21 (g) -71 1345 1345 2017 2034 213 434 0.052 0.073 0.484 0.492 0.000 2014 21 (g) -71 1336 1336 2017 2034 371 213 -1.733 -0.983 298.354 298.361 0.000 2015 21 (g) -71 1314 1314 2017 2034 172 371 -0.288 -0.385 22.189 22.195 0.000 2016 -1 (dbar) -71 1602 1602 2017 2034 0 172 0.024 0.198 -0.662 0.767 0.330 2017 223 (omega) -83 2006 2016 2717 2719 0 0 -0.331 -0.053 0.022 0.850 0.781 2018 213 (rho+) -83 2006 2016 2416 2417 0 0 0.204 -0.038 0.758 1.096 0.764 2019 -211 pi- 83 2006 2016 0 0 0 0 -0.196 -0.352 0.275 0.507 0.140 2020 113 (rho0) -83 2006 2016 2418 2419 0 0 -0.271 0.198 2.137 2.466 1.182 2021 3212 (Sigma0) -83 2006 2016 2720 2721 0 0 0.217 0.293 11.481 11.549 1.193 2022 -3112 (Sigmabar+) -83 2006 2016 2722 2723 0 0 -0.010 0.073 12.423 12.481 1.197 2023 313 (K*0) -83 2006 2016 2420 2421 0 0 -0.268 -0.727 18.854 18.894 0.963 2024 -311 (Kbar0) -83 2006 2016 2422 2422 0 0 -0.619 -0.214 164.494 164.496 0.498 2025 -213 (rho-) -83 2006 2016 2423 2424 0 0 -0.234 -0.536 66.962 66.975 1.201 2026 213 (rho+) -83 2006 2016 2425 2426 0 0 -0.119 0.079 88.534 88.541 1.103 2027 -211 pi- 84 2006 2016 0 0 0 0 -0.273 -0.512 8.367 8.388 0.140 2028 111 (pi0) -84 2006 2016 2724 2725 0 0 -0.092 0.202 9.956 9.959 0.135 2029 223 (omega) -84 2006 2016 2726 2728 0 0 -0.298 0.388 10.132 10.174 0.783 2030 221 (eta) -84 2006 2016 2729 2731 0 0 0.067 -0.008 6.539 6.563 0.548 2031 213 (rho+) -84 2006 2016 2427 2428 0 0 -0.211 -0.113 2.517 2.690 0.917 2032 -211 pi- 84 2006 2016 0 0 0 0 -0.021 -0.326 0.457 0.579 0.140 2033 111 (pi0) -84 2006 2016 2732 2733 0 0 0.434 -0.026 0.075 0.462 0.135 2034 213 (rho+) -84 2006 2016 2429 2430 0 0 -0.127 0.185 0.836 1.503 1.229 2035 1 (d) -71 1433 1433 2037 2040 115 0 0.035 -0.868 536.011 536.012 0.330 2036 -2 (ubar) -71 1597 1597 2037 2040 0 115 0.722 2.373 -0.582 2.569 0.330 2037 311 (K0) -83 2035 2036 2431 2431 0 0 -0.482 -0.730 392.264 392.266 0.498 2038 -313 (K*bar0) -83 2035 2036 2432 2433 0 0 0.531 0.163 112.618 112.623 0.893 2039 113 (rho0) -84 2035 2036 2434 2435 0 0 -0.117 -0.086 31.141 31.152 0.807 2040 -213 (rho-) -84 2035 2036 2436 2437 0 0 0.825 2.157 -0.594 2.540 0.877 2041 3 (s) -71 1657 1657 2053 2073 124 0 -0.939 0.706 873.687 873.689 1.207 2042 21 (g) -71 1653 1653 2053 2073 229 124 -0.155 3.088 461.202 461.213 0.264 2043 21 (g) -71 1655 1655 2053 2073 176 229 -0.143 2.180 179.110 179.123 0.335 2044 21 (g) -71 1468 1468 2053 2073 163 176 0.631 0.396 68.083 68.087 0.000 2045 21 (g) -71 1649 1649 2053 2073 187 163 -1.060 0.105 44.398 44.411 0.168 2046 21 (g) -71 1659 1659 2053 2073 240 187 -3.635 -1.544 36.561 36.778 0.580 2047 21 (g) -71 1658 1658 2053 2073 416 240 0.158 1.903 36.548 36.602 0.566 2048 21 (g) -71 1656 1656 2053 2073 279 416 1.528 3.056 32.675 32.856 0.435 2049 21 (g) -71 1391 1391 2053 2073 261 279 0.361 1.354 10.586 10.678 0.000 2050 21 (g) -71 1543 1543 2053 2073 158 261 -0.060 3.457 21.461 21.738 0.000 2051 21 (g) -71 1654 1654 2053 2073 411 158 0.122 1.632 8.251 8.416 0.284 2052 -2 (ubar) -71 1442 1442 2053 2073 0 411 0.588 -0.259 4.155 4.217 0.330 2053 -313 (K*bar0) -83 2041 2052 2438 2439 0 0 -0.242 0.426 316.496 316.498 0.911 2054 -213 (rho-) -83 2041 2052 2440 2441 0 0 -0.535 1.247 678.613 678.616 1.249 2055 213 (rho+) -83 2041 2052 2442 2443 0 0 -0.559 1.531 185.564 185.573 0.774 2056 -211 pi- 83 2041 2052 0 0 0 0 0.994 1.637 202.807 202.817 0.140 2057 211 pi+ 83 2041 2052 0 0 0 0 -0.689 0.407 118.436 118.438 0.140 2058 -211 pi- 83 2041 2052 0 0 0 0 0.129 0.678 29.029 29.037 0.140 2059 211 pi+ 83 2041 2052 0 0 0 0 -0.496 0.195 62.578 62.580 0.140 2060 111 (pi0) -83 2041 2052 2734 2735 0 0 0.048 0.001 0.778 0.792 0.135 2061 223 (omega) -83 2041 2052 2736 2738 0 0 -0.251 0.178 13.909 13.935 0.783 2062 -211 pi- 83 2041 2052 0 0 0 0 -1.689 -0.463 24.785 24.847 0.140 2063 211 pi+ 83 2041 2052 0 0 0 0 0.018 -0.060 4.249 4.252 0.140 2064 2112 n0 83 2041 2052 0 0 0 0 -1.808 -0.320 21.305 21.404 0.940 2065 111 (pi0) -84 2041 2052 2739 2740 0 0 0.191 0.856 22.699 22.716 0.135 2066 -2114 (Deltabar0) -84 2041 2052 2444 2445 0 0 0.146 0.401 11.478 11.560 1.303 2067 113 (rho0) -84 2041 2052 2446 2447 0 0 0.522 1.759 21.809 21.897 0.716 2068 223 (omega) -84 2041 2052 2741 2743 0 0 0.222 1.923 17.124 17.251 0.785 2069 311 (K0) -84 2041 2052 2448 2448 0 0 0.603 2.320 17.308 17.480 0.498 2070 -323 (K*-) -84 2041 2052 2449 2450 0 0 0.504 0.834 8.341 8.448 0.919 2071 213 (rho+) -84 2041 2052 2451 2452 0 0 0.138 0.914 8.185 8.283 0.872 2072 223 (omega) -84 2041 2052 2744 2746 0 0 0.162 1.192 9.443 9.551 0.778 2073 -211 pi- 84 2041 2052 0 0 0 0 -0.011 0.416 1.780 1.833 0.140 2074 1 (d) -71 1229 1229 2108 2149 284 0 -7.014 5.609 2.220 9.258 0.330 2075 21 (g) -71 1305 1305 2108 2149 478 284 -2.713 1.728 1.289 3.465 0.000 2076 21 (g) -71 1633 1633 2108 2149 321 478 -0.807 0.679 -0.163 1.071 0.089 2077 21 (g) -71 1254 1254 2108 2149 397 321 -1.147 2.540 0.371 2.812 0.000 2078 21 (g) -71 1284 1284 2108 2149 110 397 0.012 -0.023 0.143 0.145 0.000 2079 21 (g) -71 1638 1638 2108 2149 366 110 -0.440 4.568 0.416 4.614 0.238 2080 21 (g) -71 1278 1278 2108 2149 154 366 0.102 1.606 -0.420 1.663 0.000 2081 21 (g) -71 1235 1235 2108 2149 189 154 0.695 3.129 -0.134 3.208 0.000 2082 21 (g) -71 1282 1282 2108 2149 386 189 0.734 1.777 -0.617 2.019 0.000 2083 21 (g) -71 1640 1640 2108 2149 166 386 -0.858 4.297 -1.949 4.809 0.355 2084 21 (g) -71 1271 1271 2108 2149 344 166 0.027 1.693 -0.504 1.767 0.000 2085 21 (g) -71 1267 1267 2108 2149 331 344 0.017 0.841 -1.313 1.559 0.000 2086 21 (g) -71 1636 1636 2108 2149 200 331 2.345 1.449 -2.020 3.422 0.178 2087 21 (g) -71 1292 1292 2108 2149 468 200 0.880 0.233 -0.010 0.910 0.000 2088 21 (g) -71 1631 1631 2108 2149 343 468 1.930 0.906 -1.953 2.892 0.066 2089 21 (g) -71 1257 1257 2108 2149 438 343 9.906 6.819 -13.897 18.378 0.000 2090 21 (g) -71 1293 1293 2108 2149 287 438 7.744 5.360 -9.721 13.534 0.000 2091 21 (g) -71 1642 1642 2108 2149 357 287 50.538 34.649 -68.522 91.925 0.576 2092 21 (g) -71 1275 1275 2108 2149 278 357 0.796 0.181 -0.527 0.971 0.000 2093 21 (g) -71 1253 1253 2108 2149 171 278 2.525 2.167 -3.644 4.935 0.000 2094 21 (g) -71 1233 1233 2108 2149 447 171 1.626 2.244 -2.330 3.621 0.000 2095 21 (g) -71 1637 1637 2108 2149 393 447 2.529 2.762 -4.847 6.129 0.231 2096 21 (g) -71 1249 1249 2108 2149 104 393 2.601 2.126 -4.105 5.304 0.000 2097 21 (g) -71 1281 1281 2108 2149 385 104 3.415 4.432 -4.383 7.107 0.000 2098 21 (g) -71 1236 1236 2108 2149 190 385 0.339 1.000 -1.199 1.598 0.000 2099 21 (g) -71 1238 1238 2108 2149 217 190 1.900 2.472 -2.700 4.124 0.000 2100 21 (g) -71 1241 1241 2108 2149 417 217 2.673 4.223 -3.219 5.945 0.000 2101 21 (g) -71 1289 1289 2108 2149 233 417 0.288 1.348 -0.682 1.538 0.000 2102 21 (g) -71 1634 1634 2108 2149 188 233 0.036 1.084 0.382 1.156 0.113 2103 21 (g) -71 1279 1279 2108 2149 439 188 0.449 0.045 -0.365 0.581 0.000 2104 21 (g) -71 1294 1294 2108 2149 182 439 0.537 0.411 0.447 0.811 0.000 2105 21 (g) -71 1632 1632 2108 2149 107 182 -0.469 0.744 1.092 1.405 0.086 2106 21 (g) -71 1641 1641 2108 2149 173 107 -0.853 1.005 -3.665 3.930 0.521 2107 -2 (ubar) -71 1639 1639 2108 2149 0 173 1.281 2.526 -9.688 10.110 0.571 2108 111 (pi0) -83 2074 2107 2747 2748 0 0 -2.152 1.626 1.096 2.914 0.135 2109 -213 (rho-) -83 2074 2107 2453 2454 0 0 -3.793 3.036 0.829 4.996 0.820 2110 321 K+ 83 2074 2107 0 0 0 0 -3.297 2.798 0.727 4.413 0.494 2111 -311 (Kbar0) -83 2074 2107 2455 2455 0 0 -0.861 0.993 0.699 1.570 0.498 2112 3112 (Sigma-) -83 2074 2107 2749 2750 0 0 -0.687 2.346 0.294 2.738 1.197 2113 -3212 (Sigmabar0) -83 2074 2107 2751 2752 0 0 -0.408 2.996 -0.039 3.251 1.193 2114 113 (rho0) -83 2074 2107 2456 2457 0 0 -0.317 1.840 -0.175 2.037 0.797 2115 323 (K*+) -83 2074 2107 2458 2459 0 0 0.016 2.822 0.159 2.969 0.908 2116 -321 K- 83 2074 2107 0 0 0 0 0.547 1.900 -0.249 2.053 0.494 2117 213 (rho+) -83 2074 2107 2460 2461 0 0 -0.171 3.751 -1.289 4.071 0.902 2118 -211 pi- 83 2074 2107 0 0 0 0 -0.102 0.108 -0.130 0.242 0.140 2119 323 (K*+) -83 2074 2107 2462 2463 0 0 0.643 1.589 -1.227 2.316 0.961 2120 -321 K- 83 2074 2107 0 0 0 0 -0.019 1.077 -0.485 1.280 0.494 2121 211 pi+ 83 2074 2107 0 0 0 0 -0.363 1.647 -1.044 1.988 0.140 2122 111 (pi0) -84 2074 2107 2753 2754 0 0 1.521 1.046 -1.086 2.146 0.135 2123 2112 n0 84 2074 2107 0 0 0 0 2.746 2.104 -3.503 5.012 0.940 2124 -2112 nbar0 84 2074 2107 0 0 0 0 4.558 2.759 -5.123 7.451 0.940 2125 221 (eta) -84 2074 2107 2755 2757 0 0 3.211 2.272 -3.667 5.406 0.548 2126 111 (pi0) -84 2074 2107 2758 2759 0 0 2.140 1.330 -2.299 3.414 0.135 2127 -211 pi- 84 2074 2107 0 0 0 0 7.480 4.987 -9.940 13.404 0.140 2128 111 (pi0) -84 2074 2107 2760 2761 0 0 1.916 1.273 -2.089 3.110 0.135 2129 2224 (Delta++) -84 2074 2107 2464 2465 0 0 14.913 9.950 -21.937 28.357 1.223 2130 -213 (rho-) -84 2074 2107 2466 2467 0 0 7.739 5.355 -9.794 13.603 0.754 2131 -2114 (Deltabar0) -84 2074 2107 2468 2469 0 0 24.008 16.741 -33.061 44.174 1.286 2132 223 (omega) -84 2074 2107 2762 2764 0 0 3.420 2.691 -4.430 6.258 0.777 2133 111 (pi0) -84 2074 2107 2765 2766 0 0 2.526 2.547 -3.924 5.318 0.135 2134 223 (omega) -84 2074 2107 2767 2769 0 0 2.354 1.809 -3.820 4.900 0.776 2135 -213 (rho-) -84 2074 2107 2470 2471 0 0 4.755 4.813 -6.113 9.191 1.156 2136 213 (rho+) -84 2074 2107 2472 2473 0 0 2.126 2.656 -3.231 4.749 0.735 2137 -211 pi- 84 2074 2107 0 0 0 0 -0.038 0.774 -0.563 0.968 0.140 2138 111 (pi0) -84 2074 2107 2770 2771 0 0 0.325 0.610 -0.331 0.778 0.135 2139 113 (rho0) -84 2074 2107 2474 2475 0 0 3.229 3.896 -4.783 7.022 0.907 2140 213 (rho+) -84 2074 2107 2476 2477 0 0 0.802 1.342 -1.041 2.043 0.802 2141 -211 pi- 84 2074 2107 0 0 0 0 0.980 1.513 -0.855 2.000 0.140 2142 213 (rho+) -84 2074 2107 2478 2479 0 0 1.195 2.142 -1.939 3.287 1.014 2143 313 (K*0) -84 2074 2107 2480 2481 0 0 0.217 1.473 0.693 1.867 0.887 2144 -311 (Kbar0) -84 2074 2107 2482 2482 0 0 -0.009 0.076 -0.027 0.504 0.498 2145 -211 pi- 84 2074 2107 0 0 0 0 0.534 0.110 0.576 0.805 0.140 2146 113 (rho0) -84 2074 2107 2483 2484 0 0 -0.694 1.327 -3.173 3.617 0.878 2147 113 (rho0) -84 2074 2107 2485 2486 0 0 0.745 1.608 -5.977 6.408 1.481 2148 211 pi+ 84 2074 2107 0 0 0 0 -0.130 0.335 -2.498 2.527 0.140 2149 -211 pi- 84 2074 2107 0 0 0 0 0.019 0.559 -1.447 1.557 0.140 2150 3 (s) -71 1509 1509 2173 2207 144 0 -0.371 1.604 -2.602 3.119 0.500 2151 21 (g) -71 1731 1731 2173 2207 460 144 2.894 -0.996 -14.431 14.756 0.353 2152 21 (g) -71 1734 1734 2173 2207 164 460 2.451 -1.543 -27.204 27.363 0.512 2153 21 (g) -71 1428 1428 2173 2207 457 164 0.208 -0.118 -0.540 0.590 0.000 2154 21 (g) -71 1726 1726 2173 2207 258 457 -0.177 -1.550 -1.123 1.930 0.172 2155 21 (g) -71 1730 1730 2173 2207 448 258 1.450 -5.208 -4.256 6.888 0.332 2156 21 (g) -71 1231 1231 2173 2207 449 448 1.292 0.010 -1.321 1.848 0.000 2157 21 (g) -71 1733 1733 2173 2207 149 449 4.719 0.494 -8.440 9.692 0.446 2158 21 (g) -71 1221 1221 2173 2207 140 149 0.395 0.253 -0.542 0.717 0.000 2159 21 (g) -71 1725 1725 2173 2207 277 140 -1.118 1.525 -1.101 2.194 0.159 2160 21 (g) -71 1718 1718 2173 2207 392 277 -0.728 0.380 -0.519 0.975 0.080 2161 21 (g) -71 1732 1732 2173 2207 419 392 -1.833 0.061 -1.839 2.631 0.417 2162 21 (g) -71 1724 1724 2173 2207 153 419 -0.811 0.116 -0.116 0.842 0.157 2163 21 (g) -71 1252 1252 2173 2207 352 153 0.496 0.528 0.324 0.793 0.000 2164 21 (g) -71 1723 1723 2173 2207 246 352 0.104 -0.969 0.035 0.987 0.153 2165 21 (g) -71 1729 1729 2173 2207 398 246 -2.211 -1.853 1.772 3.399 0.306 2166 21 (g) -71 1285 1285 2173 2207 241 398 -0.802 -1.577 0.623 1.876 0.000 2167 21 (g) -71 1720 1720 2173 2207 103 241 -1.868 -2.399 2.700 4.067 0.099 2168 21 (g) -71 1721 1721 2173 2207 342 103 -8.893 -16.878 11.323 22.185 0.106 2169 21 (g) -71 1215 1215 2173 2207 106 342 -21.019 -40.618 29.247 54.286 0.000 2170 21 (g) -71 1262 1262 2173 2207 313 106 -5.510 -11.173 8.262 14.948 0.000 2171 21 (g) -71 1261 1261 2173 2207 305 313 -5.486 -12.138 7.457 15.266 0.000 2172 -2 (ubar) -71 1728 1728 2173 2207 0 305 -2.295 -7.392 3.445 8.487 0.513 2173 -311 (Kbar0) -83 2150 2172 2487 2487 0 0 0.072 0.323 -0.936 1.110 0.498 2174 -213 (rho-) -83 2150 2172 2488 2489 0 0 0.653 -0.195 -3.687 3.867 0.948 2175 321 K+ 83 2150 2172 0 0 0 0 -0.073 1.090 -2.815 3.060 0.494 2176 -323 (K*-) -83 2150 2172 2490 2491 0 0 1.008 -0.498 -9.056 9.169 0.894 2177 213 (rho+) -83 2150 2172 2492 2493 0 0 1.672 -0.739 -11.814 11.981 0.782 2178 113 (rho0) -83 2150 2172 2494 2495 0 0 0.997 -0.420 -6.602 6.736 0.786 2179 -211 pi- 83 2150 2172 0 0 0 0 0.106 -0.338 -4.335 4.351 0.140 2180 211 pi+ 83 2150 2172 0 0 0 0 0.302 -0.305 -2.883 2.918 0.140 2181 -213 (rho-) -83 2150 2172 2496 2497 0 0 0.004 -0.576 -1.957 2.171 0.745 2182 2212 p+ 83 2150 2172 0 0 0 0 0.447 -0.916 -1.877 2.333 0.938 2183 111 (pi0) -83 2150 2172 2772 2773 0 0 1.095 -2.407 -1.708 3.151 0.135 2184 -2114 (Deltabar0) -83 2150 2172 2498 2499 0 0 0.310 -2.275 -2.574 3.679 1.280 2185 223 (omega) -83 2150 2172 2774 2776 0 0 1.680 0.015 -2.105 2.804 0.779 2186 -211 pi- 83 2150 2172 0 0 0 0 0.683 -0.079 -2.193 2.302 0.140 2187 323 (K*+) -83 2150 2172 2500 2501 0 0 1.394 0.169 -1.145 2.069 0.999 2188 -313 (K*bar0) -83 2150 2172 2502 2503 0 0 0.622 0.050 -2.104 2.370 0.894 2189 -213 (rho-) -83 2150 2172 2504 2505 0 0 1.179 0.545 -2.718 3.208 1.104 2190 211 pi+ 83 2150 2172 0 0 0 0 0.078 -0.060 -0.577 0.602 0.140 2191 113 (rho0) -83 2150 2172 2506 2507 0 0 -0.942 0.731 -0.872 1.644 0.720 2192 -213 (rho-) -83 2150 2172 2508 2509 0 0 -0.292 0.286 -0.491 1.084 0.876 2193 211 pi+ 83 2150 2172 0 0 0 0 -2.043 0.764 -1.493 2.647 0.140 2194 111 (pi0) -84 2150 2172 2777 2778 0 0 -0.007 -0.294 0.402 0.515 0.135 2195 221 (eta) -84 2150 2172 2779 2781 0 0 -0.130 0.091 -0.122 0.583 0.548 2196 313 (K*0) -84 2150 2172 2510 2511 0 0 -0.203 -0.139 0.131 0.921 0.878 2197 -313 (K*bar0) -84 2150 2172 2512 2513 0 0 -1.098 -1.835 1.121 2.575 0.893 2198 -213 (rho-) -84 2150 2172 2514 2515 0 0 -2.118 -2.431 1.619 3.686 0.753 2199 2224 (Delta++) -84 2150 2172 2516 2517 0 0 -6.478 -11.832 8.821 16.160 1.177 2200 -211 pi- 84 2150 2172 0 0 0 0 -1.774 -4.053 2.647 5.158 0.140 2201 -2212 pbar- 84 2150 2172 0 0 0 0 -8.616 -16.252 12.018 21.992 0.938 2202 211 pi+ 84 2150 2172 0 0 0 0 -3.552 -6.057 4.109 8.137 0.140 2203 113 (rho0) -84 2150 2172 2518 2519 0 0 -16.986 -34.508 24.347 45.535 1.143 2204 223 (omega) -84 2150 2172 2782 2784 0 0 -1.766 -4.207 2.747 5.384 0.792 2205 -211 pi- 84 2150 2172 0 0 0 0 -2.037 -4.680 2.647 5.752 0.140 2206 111 (pi0) -84 2150 2172 2785 2786 0 0 -0.492 -1.493 0.757 1.749 0.135 2207 113 (rho0) -84 2150 2172 2520 2521 0 0 -2.806 -6.917 3.851 8.435 0.773 2208 21 (g) -71 1469 1469 2240 2284 455 441 0.665 -0.597 287.102 287.103 0.000 2209 21 (g) -71 1609 1609 2240 2284 441 225 2.046 -2.087 524.966 524.974 0.187 2210 21 (g) -71 1443 1443 2240 2284 225 400 0.658 -0.016 92.949 92.952 0.000 2211 21 (g) -71 1450 1450 2240 2284 400 130 -0.003 -0.276 57.982 57.983 0.000 2212 21 (g) -71 1400 1400 2240 2284 130 358 0.192 -0.661 39.615 39.621 0.000 2213 21 (g) -71 1389 1389 2240 2284 358 437 -2.252 -1.071 16.904 17.087 0.000 2214 21 (g) -71 1608 1608 2240 2284 437 121 -3.299 -1.265 17.665 18.016 0.176 2215 21 (g) -71 1607 1607 2240 2284 121 450 -1.902 -1.311 9.971 10.236 0.169 2216 21 (g) -71 1615 1615 2240 2284 450 137 -1.379 0.751 8.106 8.277 0.573 2217 1 (d) -71 1491 1491 2240 2284 137 0 -1.297 1.750 4.808 5.289 0.330 2218 21 (g) -71 1364 1364 2240 2284 167 222 1.227 -0.290 -108.231 108.238 0.000 2219 21 (g) -71 1362 1362 2240 2284 222 118 1.149 -0.222 -25.745 25.771 0.000 2220 21 (g) -71 1355 1355 2240 2284 118 308 3.640 0.868 -64.706 64.814 0.000 2221 21 (g) -71 1613 1613 2240 2284 308 446 0.518 -0.241 -14.150 14.171 0.515 2222 21 (g) -71 1357 1357 2240 2284 446 180 0.610 0.593 -7.998 8.043 0.000 2223 21 (g) -71 1376 1376 2240 2284 180 382 -0.161 0.064 -4.756 4.759 0.000 2224 21 (g) -71 1366 1366 2240 2284 382 272 -0.939 0.176 -2.957 3.107 0.000 2225 21 (g) -71 1354 1354 2240 2284 272 333 0.004 0.242 -7.522 7.526 0.000 2226 21 (g) -71 1611 1611 2240 2284 333 486 -1.064 0.726 -11.164 11.242 0.294 2227 21 (g) -71 1365 1365 2240 2284 486 263 -0.335 -0.075 -0.743 0.818 0.000 2228 21 (g) -71 1358 1358 2240 2284 263 451 0.264 -1.374 -20.268 20.316 0.000 2229 21 (g) -71 1610 1610 2240 2284 451 303 0.427 -0.116 -9.230 9.244 0.246 2230 21 (g) -71 1356 1356 2240 2284 303 212 2.553 -0.638 -30.920 31.032 0.000 2231 21 (g) -71 1360 1360 2240 2284 212 299 0.353 0.231 -2.374 2.411 0.000 2232 21 (g) -71 1369 1369 2240 2284 299 422 0.181 0.178 -11.596 11.599 0.000 2233 21 (g) -71 1379 1379 2240 2284 422 228 -0.653 -0.057 -10.183 10.204 0.000 2234 21 (g) -71 1616 1616 2240 2284 228 274 0.066 0.657 -3.010 3.135 0.577 2235 21 (g) -71 1612 1612 2240 2284 274 466 0.385 -1.297 -0.640 1.526 0.298 2236 21 (g) -71 1374 1374 2240 2284 466 324 -0.333 -0.345 0.931 1.047 0.000 2237 21 (g) -71 1614 1614 2240 2284 324 407 -1.796 0.230 1.920 2.700 0.570 2238 1 (d) -71 1372 1372 2240 2284 407 0 -1.548 -0.520 1.479 2.228 0.330 2239 2 (u) -71 1598 1598 2240 2284 160 0 -0.727 0.213 13.171 13.197 0.330 2240 211 pi+ 85 2208 2239 0 0 0 0 -0.147 0.503 8.840 8.856 0.140 2241 223 (omega) -86 2208 2239 2787 2789 0 0 -1.444 1.307 7.806 8.085 0.802 2242 113 (rho0) -86 2208 2239 2522 2523 0 0 -1.046 -0.534 4.340 4.561 0.768 2243 -211 pi- 86 2208 2239 0 0 0 0 -0.349 -0.087 0.593 0.707 0.140 2244 221 (eta) -86 2208 2239 2790 2792 0 0 -0.658 0.299 5.866 5.936 0.548 2245 211 pi+ 86 2208 2239 0 0 0 0 -0.833 0.516 2.528 2.715 0.140 2246 313 (K*0) -86 2208 2239 2524 2525 0 0 -3.016 -1.334 19.446 19.744 0.893 2247 -323 (K*-) -86 2208 2239 2526 2527 0 0 -2.000 -1.045 13.018 13.244 0.911 2248 221 (eta) -86 2208 2239 2793 2795 0 0 0.123 -0.397 11.569 11.589 0.548 2249 113 (rho0) -86 2208 2239 2528 2529 0 0 -0.014 -0.263 81.995 82.002 1.053 2250 113 (rho0) -86 2208 2239 2530 2531 0 0 -0.340 -0.040 11.798 11.828 0.774 2251 211 pi+ 86 2208 2239 0 0 0 0 0.023 -0.263 27.551 27.552 0.140 2252 2112 n0 86 2208 2239 0 0 0 0 0.558 -0.834 153.045 153.051 0.940 2253 -2212 pbar- 86 2208 2239 0 0 0 0 0.787 -0.637 307.153 307.156 0.938 2254 2212 p+ 86 2208 2239 0 0 0 0 1.391 -1.065 304.118 304.125 0.938 2255 -2112 nbar0 86 2208 2239 0 0 0 0 -0.129 -0.349 89.508 89.514 0.940 2256 311 (K0) -83 2208 2239 2532 2532 0 0 -1.767 -0.544 1.978 2.753 0.498 2257 -313 (K*bar0) -83 2208 2239 2533 2534 0 0 -0.361 -0.600 0.391 1.188 0.876 2258 3112 (Sigma-) -83 2208 2239 2796 2797 0 0 -1.034 0.248 1.338 2.087 1.197 2259 -3112 (Sigmabar+) -83 2208 2239 2798 2799 0 0 -0.225 -0.040 -1.020 1.589 1.197 2260 111 (pi0) -83 2208 2239 2800 2801 0 0 -0.167 0.022 0.008 0.216 0.135 2261 313 (K*0) -83 2208 2239 2535 2536 0 0 -0.241 -0.550 -1.562 1.922 0.945 2262 -313 (K*bar0) -83 2208 2239 2537 2538 0 0 -0.119 0.008 -1.918 2.115 0.885 2263 -211 pi- 83 2208 2239 0 0 0 0 0.319 -0.118 -0.481 0.605 0.140 2264 323 (K*+) -83 2208 2239 2539 2540 0 0 0.293 0.254 -4.389 4.493 0.879 2265 -323 (K*-) -83 2208 2239 2541 2542 0 0 0.190 0.474 -11.350 11.397 0.900 2266 2212 p+ 83 2208 2239 0 0 0 0 0.838 0.058 -19.884 19.924 0.938 2267 -2212 pbar- 83 2208 2239 0 0 0 0 0.413 -1.031 -13.665 13.742 0.938 2268 3222 (Sigma+) -83 2208 2239 2802 2803 0 0 1.469 -0.736 -26.245 26.324 1.189 2269 -3222 (Sigmabar-) -83 2208 2239 2804 2805 0 0 -0.171 -0.482 -10.418 10.498 1.189 2270 213 (rho+) -84 2208 2239 2543 2544 0 0 -1.216 0.513 -12.812 12.894 0.611 2271 113 (rho0) -84 2208 2239 2545 2546 0 0 0.499 0.888 -8.481 8.573 0.731 2272 313 (K*0) -84 2208 2239 2547 2548 0 0 -0.854 -0.306 -12.774 12.838 0.896 2273 3112 (Sigma-) -84 2208 2239 2806 2807 0 0 2.284 0.645 -33.651 33.756 1.197 2274 223 (omega) -84 2208 2239 2808 2810 0 0 2.392 0.234 -61.180 61.232 0.785 2275 -1114 (Deltabar+) -84 2208 2239 2549 2550 0 0 1.095 0.177 -61.509 61.532 1.245 2276 -211 pi- 84 2208 2239 0 0 0 0 0.541 -0.633 -16.615 16.636 0.140 2277 213 (rho+) -84 2208 2239 2551 2552 0 0 -0.253 0.169 -9.287 9.316 0.675 2278 111 (pi0) -84 2208 2239 2811 2812 0 0 0.410 0.107 -2.300 2.342 0.135 2279 313 (K*0) -84 2208 2239 2553 2554 0 0 -0.167 0.024 -20.917 20.936 0.891 2280 -313 (K*bar0) -84 2208 2239 2555 2556 0 0 0.550 -0.206 -3.210 3.388 0.910 2281 -213 (rho-) -84 2208 2239 2557 2558 0 0 -0.307 -0.006 -1.603 1.794 0.744 2282 223 (omega) -84 2208 2239 2813 2815 0 0 0.273 -0.043 5.103 5.172 0.791 2283 2214 (Delta+) -84 2208 2239 2559 2560 0 0 -0.414 0.334 11.845 11.913 1.153 2284 -211 pi- 84 2208 2239 0 0 0 0 0.077 -0.417 6.810 6.824 0.140 2285 1 (d) -71 1310 1310 2291 2311 119 0 3.520 -0.810 -4.237 5.578 0.330 2286 21 (g) -71 1340 1340 2291 2311 387 119 0.288 -0.086 -2.525 2.543 0.000 2287 21 (g) -71 1344 1344 2291 2311 413 387 -0.782 0.331 -170.102 170.105 0.000 2288 21 (g) -71 1333 1333 2291 2311 345 413 -0.244 0.533 -35.512 35.517 0.000 2289 21 (g) -71 1329 1329 2291 2311 208 345 -2.616 0.222 -558.124 558.131 0.000 2290 -1 (dbar) -71 1599 1599 2291 2311 0 208 -0.084 -0.011 820.448 820.448 0.330 2291 223 (omega) -83 2285 2290 2816 2818 0 0 3.694 -0.745 -4.925 6.250 0.784 2292 -213 (rho-) -83 2285 2290 2561 2562 0 0 0.006 0.162 -12.446 12.468 0.723 2293 211 pi+ 83 2285 2290 0 0 0 0 -0.742 -0.003 -149.289 149.291 0.140 2294 -211 pi- 83 2285 2290 0 0 0 0 -0.883 0.224 -60.614 60.621 0.140 2295 213 (rho+) -83 2285 2290 2563 2564 0 0 0.095 -0.415 -68.126 68.132 0.832 2296 111 (pi0) -83 2285 2290 2819 2820 0 0 -0.148 0.606 -93.071 93.073 0.135 2297 -213 (rho-) -83 2285 2290 2565 2566 0 0 -0.798 0.115 -173.221 173.227 1.146 2298 213 (rho+) -83 2285 2290 2567 2568 0 0 -0.468 0.310 -138.021 138.027 1.131 2299 113 (rho0) -83 2285 2290 2569 2570 0 0 -0.612 -0.310 -48.918 48.935 1.094 2300 -213 (rho-) -83 2285 2290 2571 2572 0 0 0.058 0.165 -5.852 5.920 0.882 2301 113 (rho0) -84 2285 2290 2573 2574 0 0 -0.226 -0.004 -6.639 6.679 0.692 2302 213 (rho+) -84 2285 2290 2575 2576 0 0 0.501 0.306 -7.981 8.036 0.724 2303 113 (rho0) -84 2285 2290 2577 2578 0 0 -0.321 -0.307 -0.608 1.064 0.752 2304 113 (rho0) -84 2285 2290 2579 2580 0 0 0.283 0.261 -0.077 0.768 0.659 2305 -211 pi- 84 2285 2290 0 0 0 0 -0.126 -0.304 3.297 3.316 0.140 2306 211 pi+ 84 2285 2290 0 0 0 0 -0.141 0.208 1.337 1.368 0.140 2307 223 (omega) -84 2285 2290 2821 2823 0 0 0.086 0.116 15.943 15.963 0.784 2308 113 (rho0) -84 2285 2290 2581 2582 0 0 -0.181 -0.265 17.567 17.591 0.857 2309 -213 (rho-) -84 2285 2290 2583 2584 0 0 0.072 0.370 364.594 364.595 0.773 2310 211 pi+ 84 2285 2290 0 0 0 0 -0.302 -0.174 249.643 249.643 0.140 2311 113 (rho0) -84 2285 2290 2585 2586 0 0 0.237 -0.137 167.353 167.355 0.767 2312 310 (K_S0) -91 1748 1748 2824 2825 0 0 3.242 1.768 -29.040 29.278 0.498 2313 311 (K0) -91 1753 0 2587 2587 0 0 -0.231 0.221 236.130 236.131 0.498 2314 211 pi+ 91 1753 0 0 0 0 0 -0.064 0.309 55.011 55.012 0.140 2315 321 K+ 91 1758 0 0 0 0 0 1.448 0.909 -10.404 10.555 0.494 2316 -211 pi- 91 1758 0 0 0 0 0 0.514 0.078 -5.154 5.182 0.140 2317 -211 pi- 91 1762 0 0 0 0 0 0.011 0.493 0.204 0.551 0.140 2318 111 (pi0) -91 1762 0 2826 2827 0 0 0.187 -0.194 0.971 1.017 0.135 2319 211 pi+ 91 1772 0 0 0 0 0 -0.986 0.741 4.617 4.781 0.140 2320 -211 pi- 91 1772 0 0 0 0 0 -0.461 1.354 4.166 4.407 0.140 2321 211 pi+ 91 1776 0 0 0 0 0 -1.112 0.940 3.378 3.681 0.140 2322 -211 pi- 91 1776 0 0 0 0 0 -0.203 -0.117 0.427 0.507 0.140 2323 211 pi+ 91 1786 0 0 0 0 0 -3.612 3.167 -0.271 4.813 0.140 2324 111 (pi0) -91 1786 0 2828 2829 0 0 -0.990 0.441 -0.046 1.093 0.135 2325 310 (K_S0) -91 1790 1790 2830 2831 0 0 -0.442 -0.400 -151.397 151.399 0.498 2326 211 pi+ 91 1793 0 0 0 0 0 0.433 0.043 -98.238 98.239 0.140 2327 111 (pi0) -91 1793 0 2832 2833 0 0 -0.483 -0.136 -157.129 157.130 0.135 2328 2112 n0 91 1806 0 0 0 0 0 -1.953 -0.770 -37.364 37.435 0.940 2329 111 (pi0) -91 1806 0 2834 2835 0 0 -1.520 -0.384 -26.393 26.440 0.135 2330 -2112 nbar0 91 1808 0 0 0 0 0 -1.886 0.051 -25.315 25.403 0.940 2331 -211 pi- 91 1808 0 0 0 0 0 -0.517 0.270 -7.611 7.634 0.140 2332 130 K_L0 91 1811 1811 0 0 0 0 -0.504 -0.467 -14.109 14.134 0.498 2333 211 pi+ 91 1818 0 0 0 0 0 0.529 0.266 -7.534 7.559 0.140 2334 111 (pi0) -91 1818 0 2836 2837 0 0 0.698 -0.257 -6.782 6.824 0.135 2335 -211 pi- 91 1819 0 0 0 0 0 1.160 -0.436 -13.842 13.898 0.140 2336 111 (pi0) -91 1819 0 2838 2839 0 0 1.535 0.301 -29.622 29.664 0.135 2337 211 pi+ 91 1823 0 0 0 0 0 -0.540 -0.274 -68.136 68.139 0.140 2338 -211 pi- 91 1823 0 0 0 0 0 0.091 -0.876 -88.743 88.747 0.140 2339 211 pi+ 91 1836 0 0 0 0 0 -0.836 -1.755 1.199 2.288 0.140 2340 111 (pi0) -91 1836 0 2840 2841 0 0 -0.766 -2.580 2.399 3.608 0.135 2341 130 K_L0 91 1837 1837 0 0 0 0 -0.990 -1.938 3.146 3.858 0.498 2342 310 (K_S0) -91 1840 1840 2842 2843 0 0 -2.216 -1.260 0.483 2.642 0.498 2343 211 pi+ 91 1841 0 0 0 0 0 -0.304 -0.036 0.627 0.712 0.140 2344 -211 pi- 91 1841 0 0 0 0 0 -0.159 -0.172 -0.156 0.314 0.140 2345 -211 pi- 91 1842 0 0 0 0 0 -0.591 -0.682 0.275 0.953 0.140 2346 111 (pi0) -91 1842 0 2844 2845 0 0 -0.525 -0.080 -0.217 0.589 0.135 2347 211 pi+ 91 1843 0 0 0 0 0 -0.248 0.133 0.888 0.942 0.140 2348 111 (pi0) -91 1843 0 2846 2847 0 0 -0.665 2.746 6.068 6.695 0.135 2349 -211 pi- 91 1853 0 0 0 0 0 -0.808 0.222 151.818 151.821 0.140 2350 111 (pi0) -91 1853 0 2848 2849 0 0 -0.656 -0.061 39.603 39.609 0.135 2351 211 pi+ 91 1863 0 0 0 0 0 -0.139 -0.417 17.207 17.213 0.140 2352 -211 pi- 91 1863 0 0 0 0 0 0.286 -0.105 14.643 14.647 0.140 2353 -211 pi- 91 1867 0 0 0 0 0 0.587 0.065 15.597 15.609 0.140 2354 111 (pi0) -91 1867 0 2850 2851 0 0 1.292 -0.083 11.473 11.547 0.135 2355 310 (K_S0) -91 1872 1872 2852 2853 0 0 -0.449 0.192 14.461 14.477 0.498 2356 2112 n0 91 1875 0 0 0 0 0 -0.006 -0.068 3.443 3.569 0.940 2357 111 (pi0) -91 1875 0 2854 2855 0 0 -0.182 -0.014 0.895 0.923 0.135 2358 -211 pi- 91 1876 0 0 0 0 0 0.354 0.055 0.409 0.561 0.140 2359 111 (pi0) -91 1876 0 2856 2857 0 0 -0.785 -0.133 0.350 0.880 0.135 2360 -2112 nbar0 91 1877 0 0 0 0 0 -1.173 1.723 -2.025 3.054 0.940 2361 211 pi+ 91 1877 0 0 0 0 0 -0.498 0.338 -0.244 0.664 0.140 2362 211 pi+ 91 1888 0 0 0 0 0 -1.047 0.330 4.484 4.618 0.140 2363 -211 pi- 91 1888 0 0 0 0 0 -0.068 0.335 0.916 0.988 0.140 2364 211 pi+ 91 1889 0 0 0 0 0 -0.536 -1.163 11.169 11.243 0.140 2365 111 (pi0) -91 1889 0 2858 2859 0 0 -0.365 -0.097 1.507 1.559 0.135 2366 -211 pi- 91 1890 0 0 0 0 0 -0.697 -0.150 3.478 3.553 0.140 2367 111 (pi0) -91 1890 0 2860 2861 0 0 -0.496 0.261 1.175 1.309 0.135 2368 211 pi+ 91 1895 0 0 0 0 0 -0.506 0.631 19.298 19.316 0.140 2369 -211 pi- 91 1895 0 0 0 0 0 -0.675 0.032 10.541 10.564 0.140 2370 311 (K0) -91 1898 0 2588 2588 0 0 -1.018 1.025 155.398 155.406 0.498 2371 111 (pi0) -91 1898 0 2862 2863 0 0 0.026 0.445 30.154 30.157 0.135 2372 310 (K_S0) -91 1899 1899 2864 2865 0 0 -0.677 -0.460 153.776 153.779 0.498 2373 211 pi+ 91 1917 0 0 0 0 0 0.206 0.191 3.285 3.300 0.140 2374 -211 pi- 91 1917 0 0 0 0 0 1.471 -0.134 7.863 8.002 0.140 2375 -211 pi- 91 1921 0 0 0 0 0 -0.138 -0.413 2.029 2.080 0.140 2376 111 (pi0) -91 1921 0 2866 2867 0 0 0.488 -0.716 10.097 10.135 0.135 2377 211 pi+ 91 1922 0 0 0 0 0 0.145 0.040 1.695 1.708 0.140 2378 111 (pi0) -91 1922 0 2868 2869 0 0 0.222 -1.297 11.521 11.597 0.135 2379 211 pi+ 91 1930 0 0 0 0 0 0.309 -0.508 0.916 1.101 0.140 2380 111 (pi0) -91 1930 0 2870 2871 0 0 0.512 0.740 1.654 1.888 0.135 2381 211 pi+ 91 1933 0 0 0 0 0 0.283 0.182 -0.074 0.372 0.140 2382 -211 pi- 91 1933 0 0 0 0 0 0.001 -0.381 0.353 0.538 0.140 2383 211 pi+ 91 1934 0 0 0 0 0 0.448 -0.607 -0.475 0.903 0.140 2384 -211 pi- 91 1934 0 0 0 0 0 0.812 -0.093 0.321 0.889 0.140 2385 211 pi+ 91 1947 0 0 0 0 0 -0.169 -0.465 -9.837 9.850 0.140 2386 111 (pi0) -91 1947 0 2872 2873 0 0 0.332 0.219 -11.270 11.278 0.135 2387 -211 pi- 91 1948 0 0 0 0 0 -0.114 0.365 -6.858 6.870 0.140 2388 111 (pi0) -91 1948 0 2874 2875 0 0 0.031 -0.389 -12.969 12.976 0.135 2389 211 pi+ 91 1954 0 0 0 0 0 -0.696 -0.097 -2.746 2.838 0.140 2390 -211 pi- 91 1954 0 0 0 0 0 0.191 0.003 -1.480 1.499 0.140 2391 211 pi+ 91 1955 0 0 0 0 0 -0.688 -0.157 -1.647 1.797 0.140 2392 111 (pi0) -91 1955 0 2876 2877 0 0 0.047 0.084 0.017 0.167 0.135 2393 211 pi+ 91 1960 0 0 0 0 0 -1.189 0.182 -0.898 1.508 0.140 2394 111 (pi0) -91 1960 0 2878 2879 0 0 -1.279 -0.547 -1.648 2.161 0.135 2395 -211 pi- 91 1962 0 0 0 0 0 0.144 -0.196 -0.400 0.488 0.140 2396 111 (pi0) -91 1962 0 2880 2881 0 0 -1.208 -0.823 -0.817 1.680 0.135 2397 -211 pi- 91 1974 0 0 0 0 0 -0.108 -0.014 -22.923 22.923 0.140 2398 111 (pi0) -91 1974 0 2882 2883 0 0 0.814 -0.026 -25.569 25.582 0.135 2399 211 pi+ 91 1978 0 0 0 0 0 -0.065 -0.096 -6.638 6.641 0.140 2400 -211 pi- 91 1978 0 0 0 0 0 0.290 0.050 -0.798 0.862 0.140 2401 211 pi+ 91 1979 0 0 0 0 0 0.090 -0.225 -0.073 0.289 0.140 2402 111 (pi0) -91 1979 0 2884 2885 0 0 -0.283 0.255 -1.719 1.765 0.135 2403 211 pi+ 91 1995 0 0 0 0 0 -0.074 0.213 1.303 1.329 0.140 2404 -211 pi- 91 1995 0 0 0 0 0 0.993 0.260 5.815 5.907 0.140 2405 -211 pi- 91 1997 0 0 0 0 0 0.548 -0.286 1.354 1.495 0.140 2406 111 (pi0) -91 1997 0 2886 2887 0 0 -0.069 0.214 0.723 0.769 0.135 2407 211 pi+ 91 2000 0 0 0 0 0 0.310 -0.213 1.700 1.747 0.140 2408 111 (pi0) -91 2000 0 2888 2889 0 0 0.301 0.285 0.596 0.738 0.135 2409 -211 pi- 91 2001 0 0 0 0 0 -0.346 -0.135 0.957 1.036 0.140 2410 111 (pi0) -91 2001 0 2890 2891 0 0 0.174 0.026 0.000 0.221 0.135 2411 321 K+ 91 2003 0 0 0 0 0 -0.535 -0.128 0.309 0.801 0.494 2412 -211 pi- 91 2003 0 0 0 0 0 0.159 0.089 0.192 0.299 0.140 2413 130 K_L0 91 2004 2004 0 0 0 0 0.525 0.230 0.069 0.762 0.498 2414 211 pi+ 91 2005 0 0 0 0 0 0.360 -0.824 -2.780 2.925 0.140 2415 -211 pi- 91 2005 0 0 0 0 0 1.007 -0.228 -3.516 3.667 0.140 2416 211 pi+ 91 2018 0 0 0 0 0 -0.004 -0.353 0.278 0.471 0.140 2417 111 (pi0) -91 2018 0 2892 2893 0 0 0.208 0.315 0.480 0.625 0.135 2418 211 pi+ 91 2020 0 0 0 0 0 -0.298 0.179 2.251 2.282 0.140 2419 -211 pi- 91 2020 0 0 0 0 0 0.027 0.019 -0.114 0.183 0.140 2420 321 K+ 91 2023 0 0 0 0 0 0.073 -0.131 9.696 9.710 0.494 2421 -211 pi- 91 2023 0 0 0 0 0 -0.341 -0.596 9.158 9.185 0.140 2422 130 K_L0 91 2024 2024 0 0 0 0 -0.619 -0.214 164.494 164.496 0.498 2423 -211 pi- 91 2025 0 0 0 0 0 0.381 0.080 30.030 30.033 0.140 2424 111 (pi0) -91 2025 0 2894 2895 0 0 -0.615 -0.615 36.931 36.942 0.135 2425 211 pi+ 91 2026 0 0 0 0 0 -0.427 -0.285 62.542 62.544 0.140 2426 111 (pi0) -91 2026 0 2896 2897 0 0 0.308 0.364 25.992 25.997 0.135 2427 211 pi+ 91 2031 0 0 0 0 0 -0.206 -0.417 2.103 2.158 0.140 2428 111 (pi0) -91 2031 0 2898 2899 0 0 -0.005 0.304 0.414 0.532 0.135 2429 211 pi+ 91 2034 0 0 0 0 0 -0.411 -0.094 0.966 1.063 0.140 2430 111 (pi0) -91 2034 0 2900 2901 0 0 0.284 0.279 -0.130 0.440 0.135 2431 310 (K_S0) -91 2037 2037 2902 2903 0 0 -0.482 -0.730 392.264 392.266 0.498 2432 -311 (Kbar0) -91 2038 0 2589 2589 0 0 0.132 0.313 68.132 68.135 0.498 2433 111 (pi0) -91 2038 0 2904 2905 0 0 0.399 -0.150 44.486 44.488 0.135 2434 211 pi+ 91 2039 0 0 0 0 0 0.308 0.013 9.684 9.690 0.140 2435 -211 pi- 91 2039 0 0 0 0 0 -0.425 -0.099 21.457 21.462 0.140 2436 -211 pi- 91 2040 0 0 0 0 0 0.244 0.108 0.064 0.308 0.140 2437 111 (pi0) -91 2040 0 2906 2907 0 0 0.581 2.049 -0.657 2.233 0.135 2438 -321 K- 91 2053 0 0 0 0 0 -0.052 0.012 214.423 214.424 0.494 2439 211 pi+ 91 2053 0 0 0 0 0 -0.190 0.415 102.073 102.074 0.140 2440 -211 pi- 91 2054 0 0 0 0 0 -0.140 -0.156 38.018 38.019 0.140 2441 111 (pi0) -91 2054 0 2908 2909 0 0 -0.395 1.403 640.596 640.597 0.135 2442 211 pi+ 91 2055 0 0 0 0 0 0.043 0.054 7.734 7.736 0.140 2443 111 (pi0) -91 2055 0 2910 2911 0 0 -0.603 1.477 177.829 177.837 0.135 2444 -2212 pbar- 91 2066 0 0 0 0 0 0.166 0.155 6.272 6.346 0.938 2445 211 pi+ 91 2066 0 0 0 0 0 -0.020 0.246 5.206 5.214 0.140 2446 211 pi+ 91 2067 0 0 0 0 0 0.005 1.028 9.860 9.914 0.140 2447 -211 pi- 91 2067 0 0 0 0 0 0.517 0.731 11.949 11.983 0.140 2448 130 K_L0 91 2069 2069 0 0 0 0 0.603 2.320 17.308 17.480 0.498 2449 -321 K- 91 2070 0 0 0 0 0 0.089 0.301 2.562 2.628 0.494 2450 111 (pi0) -91 2070 0 2912 2913 0 0 0.414 0.533 5.780 5.821 0.135 2451 211 pi+ 91 2071 0 0 0 0 0 -0.069 0.981 5.799 5.884 0.140 2452 111 (pi0) -91 2071 0 2914 2915 0 0 0.207 -0.066 2.386 2.399 0.135 2453 -211 pi- 91 2109 0 0 0 0 0 -3.443 2.581 0.912 4.401 0.140 2454 111 (pi0) -91 2109 0 2916 2917 0 0 -0.350 0.455 -0.083 0.596 0.135 2455 310 (K_S0) -91 2111 2111 2918 2919 0 0 -0.861 0.993 0.699 1.570 0.498 2456 211 pi+ 91 2114 0 0 0 0 0 -0.209 1.487 0.164 1.516 0.140 2457 -211 pi- 91 2114 0 0 0 0 0 -0.108 0.353 -0.340 0.521 0.140 2458 321 K+ 91 2115 0 0 0 0 0 0.009 1.524 -0.202 1.615 0.494 2459 111 (pi0) -91 2115 0 2920 2921 0 0 0.007 1.298 0.362 1.354 0.135 2460 211 pi+ 91 2117 0 0 0 0 0 0.327 2.159 -0.734 2.308 0.140 2461 111 (pi0) -91 2117 0 2922 2923 0 0 -0.498 1.592 -0.554 1.763 0.135 2462 311 (K0) -91 2119 0 2590 2590 0 0 0.541 1.254 -0.574 1.563 0.498 2463 211 pi+ 91 2119 0 0 0 0 0 0.102 0.335 -0.653 0.754 0.140 2464 2212 p+ 91 2129 0 0 0 0 0 13.718 9.168 -20.409 26.261 0.938 2465 211 pi+ 91 2129 0 0 0 0 0 1.195 0.781 -1.528 2.096 0.140 2466 -211 pi- 91 2130 0 0 0 0 0 1.014 0.523 -1.404 1.815 0.140 2467 111 (pi0) -91 2130 0 2924 2925 0 0 6.724 4.832 -8.390 11.789 0.135 2468 -2112 nbar0 91 2131 0 0 0 0 0 17.846 12.208 -24.718 32.854 0.940 2469 111 (pi0) -91 2131 0 2926 2927 0 0 6.162 4.533 -8.344 11.320 0.135 2470 -211 pi- 91 2135 0 0 0 0 0 4.106 3.864 -4.551 7.248 0.140 2471 111 (pi0) -91 2135 0 2928 2929 0 0 0.648 0.949 -1.561 1.943 0.135 2472 211 pi+ 91 2136 0 0 0 0 0 1.559 1.556 -1.765 2.826 0.140 2473 111 (pi0) -91 2136 0 2930 2931 0 0 0.568 1.099 -1.466 1.923 0.135 2474 211 pi+ 91 2139 0 0 0 0 0 3.127 3.849 -4.597 6.763 0.140 2475 -211 pi- 91 2139 0 0 0 0 0 0.102 0.047 -0.186 0.258 0.140 2476 211 pi+ 91 2140 0 0 0 0 0 0.924 1.085 -0.764 1.623 0.140 2477 111 (pi0) -91 2140 0 2932 2933 0 0 -0.122 0.258 -0.277 0.420 0.135 2478 211 pi+ 91 2142 0 0 0 0 0 0.990 2.123 -1.505 2.788 0.140 2479 111 (pi0) -91 2142 0 2934 2935 0 0 0.205 0.019 -0.434 0.499 0.135 2480 321 K+ 91 2143 0 0 0 0 0 0.141 1.111 0.209 1.242 0.494 2481 -211 pi- 91 2143 0 0 0 0 0 0.076 0.362 0.484 0.625 0.140 2482 130 K_L0 91 2144 2144 0 0 0 0 -0.009 0.076 -0.027 0.504 0.498 2483 211 pi+ 91 2146 0 0 0 0 0 0.058 0.387 -0.345 0.540 0.140 2484 -211 pi- 91 2146 0 0 0 0 0 -0.752 0.940 -2.828 3.076 0.140 2485 211 pi+ 91 2147 0 0 0 0 0 0.035 0.630 -0.557 0.853 0.140 2486 -211 pi- 91 2147 0 0 0 0 0 0.710 0.978 -5.420 5.555 0.140 2487 130 K_L0 91 2173 2173 0 0 0 0 0.072 0.323 -0.936 1.110 0.498 2488 -211 pi- 91 2174 0 0 0 0 0 0.425 -0.447 -1.226 1.380 0.140 2489 111 (pi0) -91 2174 0 2936 2937 0 0 0.229 0.252 -2.461 2.488 0.135 2490 -311 (Kbar0) -91 2176 0 2591 2591 0 0 0.504 -0.178 -6.495 6.536 0.498 2491 -211 pi- 91 2176 0 0 0 0 0 0.504 -0.320 -2.561 2.633 0.140 2492 211 pi+ 91 2177 0 0 0 0 0 1.273 -0.192 -7.390 7.503 0.140 2493 111 (pi0) -91 2177 0 2938 2939 0 0 0.399 -0.547 -4.424 4.478 0.135 2494 211 pi+ 91 2178 0 0 0 0 0 0.718 0.087 -3.351 3.431 0.140 2495 -211 pi- 91 2178 0 0 0 0 0 0.279 -0.507 -3.251 3.305 0.140 2496 -211 pi- 91 2181 0 0 0 0 0 -0.137 -0.430 -1.842 1.902 0.140 2497 111 (pi0) -91 2181 0 2940 2941 0 0 0.141 -0.146 -0.114 0.269 0.135 2498 -2112 nbar0 91 2184 0 0 0 0 0 0.376 -1.906 -2.444 3.260 0.940 2499 111 (pi0) -91 2184 0 2942 2943 0 0 -0.065 -0.369 -0.130 0.419 0.135 2500 321 K+ 91 2187 0 0 0 0 0 0.261 -0.051 -0.350 0.661 0.494 2501 111 (pi0) -91 2187 0 2944 2945 0 0 1.134 0.220 -0.795 1.408 0.135 2502 -311 (Kbar0) -91 2188 0 2592 2592 0 0 0.152 0.218 -0.950 1.105 0.498 2503 111 (pi0) -91 2188 0 2946 2947 0 0 0.471 -0.168 -1.155 1.265 0.135 2504 -211 pi- 91 2189 0 0 0 0 0 0.374 0.723 -1.711 1.900 0.140 2505 111 (pi0) -91 2189 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-2.422 0.968 2.784 0.140 2521 -211 pi- 91 2207 0 0 0 0 0 -1.844 -4.495 2.883 5.651 0.140 2522 211 pi+ 91 2242 0 0 0 0 0 -0.799 -0.701 3.208 3.383 0.140 2523 -211 pi- 91 2242 0 0 0 0 0 -0.246 0.167 1.132 1.179 0.140 2524 321 K+ 91 2246 0 0 0 0 0 -2.702 -1.177 15.948 16.226 0.494 2525 -211 pi- 91 2246 0 0 0 0 0 -0.314 -0.157 3.497 3.518 0.140 2526 -311 (Kbar0) -91 2247 0 2593 2593 0 0 -1.421 -0.899 8.119 8.306 0.498 2527 -211 pi- 91 2247 0 0 0 0 0 -0.579 -0.145 4.900 4.938 0.140 2528 211 pi+ 91 2249 0 0 0 0 0 0.209 -0.574 36.689 36.694 0.140 2529 -211 pi- 91 2249 0 0 0 0 0 -0.223 0.311 45.306 45.308 0.140 2530 211 pi+ 91 2250 0 0 0 0 0 -0.188 -0.350 8.261 8.272 0.140 2531 -211 pi- 91 2250 0 0 0 0 0 -0.151 0.311 3.537 3.556 0.140 2532 130 K_L0 91 2256 2256 0 0 0 0 -1.767 -0.544 1.978 2.753 0.498 2533 -311 (Kbar0) -91 2257 0 2594 2594 0 0 -0.256 -0.530 0.018 0.771 0.498 2534 111 (pi0) -91 2257 0 2954 2955 0 0 -0.105 -0.069 0.373 0.416 0.135 2535 311 (K0) -91 2261 0 2595 2595 0 0 -0.109 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pi+ 91 2275 0 0 0 0 0 -0.072 -0.005 -6.359 6.361 0.140 2551 211 pi+ 91 2277 0 0 0 0 0 -0.309 -0.113 -2.955 2.976 0.140 2552 111 (pi0) -91 2277 0 2966 2967 0 0 0.056 0.282 -6.332 6.340 0.135 2553 321 K+ 91 2279 0 0 0 0 0 0.015 0.058 -18.868 18.875 0.494 2554 -211 pi- 91 2279 0 0 0 0 0 -0.183 -0.034 -2.049 2.062 0.140 2555 -321 K- 91 2280 0 0 0 0 0 0.406 -0.300 -3.002 3.083 0.494 2556 211 pi+ 91 2280 0 0 0 0 0 0.144 0.094 -0.208 0.304 0.140 2557 -211 pi- 91 2281 0 0 0 0 0 -0.183 -0.005 -1.594 1.610 0.140 2558 111 (pi0) -91 2281 0 2968 2969 0 0 -0.124 -0.001 -0.009 0.184 0.135 2559 2112 n0 91 2283 0 0 0 0 0 -0.371 0.368 11.161 11.213 0.940 2560 211 pi+ 91 2283 0 0 0 0 0 -0.043 -0.034 0.684 0.700 0.140 2561 -211 pi- 91 2292 0 0 0 0 0 -0.290 0.155 -4.056 4.072 0.140 2562 111 (pi0) -91 2292 0 2970 2971 0 0 0.296 0.008 -8.389 8.396 0.135 2563 211 pi+ 91 2295 0 0 0 0 0 0.313 0.046 -39.738 39.739 0.140 2564 111 (pi0) -91 2295 0 2972 2973 0 0 -0.218 -0.462 -28.388 28.393 0.135 2565 -211 pi- 91 2297 0 0 0 0 0 -0.208 -0.011 -138.070 138.070 0.140 2566 111 (pi0) -91 2297 0 2974 2975 0 0 -0.590 0.126 -35.151 35.156 0.135 2567 211 pi+ 91 2298 0 0 0 0 0 0.249 0.021 -12.326 12.329 0.140 2568 111 (pi0) -91 2298 0 2976 2977 0 0 -0.717 0.288 -125.695 125.697 0.135 2569 211 pi+ 91 2299 0 0 0 0 0 0.190 -0.375 -22.739 22.743 0.140 2570 -211 pi- 91 2299 0 0 0 0 0 -0.802 0.065 -26.180 26.193 0.140 2571 -211 pi- 91 2300 0 0 0 0 0 -0.383 0.009 -2.970 2.998 0.140 2572 111 (pi0) -91 2300 0 2978 2979 0 0 0.441 0.156 -2.882 2.923 0.135 2573 211 pi+ 91 2301 0 0 0 0 0 -0.181 -0.040 -0.694 0.732 0.140 2574 -211 pi- 91 2301 0 0 0 0 0 -0.044 0.035 -5.944 5.946 0.140 2575 211 pi+ 91 2302 0 0 0 0 0 0.288 -0.184 -3.837 3.854 0.140 2576 111 (pi0) -91 2302 0 2980 2981 0 0 0.213 0.490 -4.145 4.181 0.135 2577 211 pi+ 91 2303 0 0 0 0 0 0.212 -0.054 -0.252 0.362 0.140 2578 -211 pi- 91 2303 0 0 0 0 0 -0.532 -0.253 -0.356 0.702 0.140 2579 211 pi+ 91 2304 0 0 0 0 0 0.425 0.296 0.034 0.537 0.140 2580 -211 pi- 91 2304 0 0 0 0 0 -0.141 -0.034 -0.112 0.230 0.140 2581 211 pi+ 91 2308 0 0 0 0 0 0.103 -0.461 7.034 7.051 0.140 2582 -211 pi- 91 2308 0 0 0 0 0 -0.284 0.196 10.534 10.540 0.140 2583 -211 pi- 91 2309 0 0 0 0 0 0.090 0.524 165.822 165.823 0.140 2584 111 (pi0) -91 2309 0 2982 2983 0 0 -0.018 -0.153 198.773 198.773 0.135 2585 211 pi+ 91 2311 0 0 0 0 0 0.288 -0.168 34.487 34.489 0.140 2586 -211 pi- 91 2311 0 0 0 0 0 -0.051 0.031 132.867 132.867 0.140 2587 310 (K_S0) -91 2313 2313 2984 2985 0 0 -0.231 0.221 236.130 236.131 0.498 2588 310 (K_S0) -91 2370 2370 2986 2987 0 0 -1.018 1.025 155.398 155.406 0.498 2589 310 (K_S0) -91 2432 2432 2988 2989 0 0 0.132 0.313 68.132 68.135 0.498 2590 130 K_L0 91 2462 2462 0 0 0 0 0.541 1.254 -0.574 1.563 0.498 2591 130 K_L0 91 2490 2490 0 0 0 0 0.504 -0.178 -6.495 6.536 0.498 2592 130 K_L0 91 2502 2502 0 0 0 0 0.152 0.218 -0.950 1.105 0.498 2593 130 K_L0 91 2526 2526 0 0 0 0 -1.421 -0.899 8.119 8.306 0.498 2594 130 K_L0 91 2533 2533 0 0 0 0 -0.256 -0.530 0.018 0.771 0.498 2595 130 K_L0 91 2535 2535 0 0 0 0 -0.109 -0.650 -1.477 1.692 0.498 2596 310 (K_S0) -91 2537 2537 2990 2991 0 0 0.068 -0.200 -0.885 1.037 0.498 2597 130 K_L0 91 2541 2541 0 0 0 0 0.020 0.203 -3.679 3.718 0.498 2598 130 K_L0 91 2547 2547 0 0 0 0 -0.695 -0.177 -6.454 6.512 0.498 2599 22 gamma 91 1752 0 0 0 0 0 0.410 0.879 324.113 324.115 0.000 2600 22 gamma 91 1752 0 0 0 0 0 0.105 0.147 78.504 78.504 0.000 2601 211 pi+ 91 1756 0 0 0 0 0 0.607 -0.062 -1.576 1.696 0.140 2602 -211 pi- 91 1756 0 0 0 0 0 0.262 0.008 -0.837 0.888 0.140 2603 221 (eta) -91 1756 0 2992 2993 0 0 1.384 0.288 -5.199 5.415 0.548 2604 22 gamma 91 1763 0 0 0 0 0 -0.056 0.040 0.096 0.118 0.000 2605 22 gamma 91 1763 0 0 0 0 0 -0.686 0.023 1.217 1.398 0.000 2606 211 pi+ 91 1764 0 0 0 0 0 -1.015 -0.051 0.528 1.154 0.140 2607 -211 pi- 91 1764 0 0 0 0 0 -0.358 -0.320 0.309 0.588 0.140 2608 111 (pi0) -91 1764 0 2994 2995 0 0 -0.069 -0.007 -0.007 0.152 0.135 2609 211 pi+ 91 1773 0 0 0 0 0 -0.525 0.572 2.937 3.041 0.140 2610 -211 pi- 91 1773 0 0 0 0 0 -0.579 0.494 3.550 3.634 0.140 2611 111 (pi0) -91 1773 0 2996 2997 0 0 0.038 0.275 1.491 1.522 0.135 2612 22 gamma 91 1782 0 0 0 0 0 -0.248 0.235 0.297 0.452 0.000 2613 22 gamma 91 1782 0 0 0 0 0 -0.017 0.120 0.116 0.168 0.000 2614 22 gamma 91 1783 0 0 0 0 0 -0.422 0.289 -0.169 0.539 0.000 2615 22 gamma 91 1783 0 0 0 0 0 -0.459 0.183 -0.085 0.501 0.000 2616 22 gamma 91 1784 0 0 0 0 0 0.300 0.427 -0.214 0.564 0.000 2617 22 gamma 91 1784 0 0 0 0 0 0.099 0.304 -0.182 0.368 0.000 2618 22 gamma 91 1791 0 0 0 0 0 0.233 0.217 -71.825 71.826 0.000 2619 22 gamma 91 1791 0 0 0 0 0 0.005 0.085 -13.671 13.671 0.000 2620 22 gamma 91 1794 0 0 0 0 0 -0.207 -0.056 -407.856 407.856 0.000 2621 22 gamma 91 1794 0 0 0 0 0 -0.140 0.061 -409.949 409.949 0.000 2622 211 pi+ 91 1796 0 0 0 0 0 -0.052 -0.418 -649.166 649.166 0.140 2623 -211 pi- 91 1796 0 0 0 0 0 0.098 -0.117 -598.595 598.595 0.140 2624 111 (pi0) -91 1796 0 2998 2999 0 0 -0.101 0.116 -323.024 323.024 0.135 2625 111 (pi0) -91 1804 0 3000 3001 0 0 -2.587 -1.005 -51.963 52.038 0.135 2626 22 gamma 91 1804 0 0 0 0 0 -7.506 -1.791 -156.838 157.028 0.000 2627 211 pi+ 91 1805 0 0 0 0 0 -1.620 -0.800 -42.084 42.123 0.140 2628 -211 pi- 91 1805 0 0 0 0 0 -1.892 -0.655 -42.328 42.376 0.140 2629 111 (pi0) -91 1805 0 3002 3003 0 0 -0.401 0.000 -7.761 7.772 0.135 2630 22 gamma 91 1810 0 0 0 0 0 -0.110 0.028 -0.115 0.162 0.000 2631 22 gamma 91 1810 0 0 0 0 0 -0.867 0.111 -5.085 5.159 0.000 2632 211 pi+ 91 1820 0 0 0 0 0 0.431 0.335 -10.664 10.678 0.140 2633 -211 pi- 91 1820 0 0 0 0 0 0.051 -0.058 -2.041 2.047 0.140 2634 111 (pi0) -91 1820 0 3004 3005 0 0 0.491 0.346 -6.238 6.269 0.135 2635 211 pi+ 91 1824 0 0 0 0 0 -0.152 -0.819 -44.223 44.231 0.140 2636 -211 pi- 91 1824 0 0 0 0 0 0.023 -0.607 -33.473 33.479 0.140 2637 111 (pi0) -91 1824 0 3006 3007 0 0 -0.078 -0.563 -42.524 42.528 0.135 2638 211 pi+ 91 1835 0 0 0 0 0 -0.074 -0.974 0.454 1.086 0.140 2639 -211 pi- 91 1835 0 0 0 0 0 -0.224 -0.794 0.739 1.117 0.140 2640 111 (pi0) -91 1835 0 3008 3009 0 0 -0.430 -0.743 0.387 0.952 0.135 2641 130 K_L0 91 1838 0 0 0 0 0 -0.250 -3.458 3.892 5.236 0.498 2642 310 (K_S0) -91 1838 0 3010 3011 0 0 -0.307 -3.956 4.776 6.229 0.498 2643 130 K_L0 91 1839 0 0 0 0 0 -0.516 -1.253 2.546 2.926 0.498 2644 310 (K_S0) -91 1839 0 3012 3013 0 0 -0.366 -1.348 2.259 2.702 0.498 2645 22 gamma 91 1854 0 0 0 0 0 -0.021 -0.137 12.745 12.746 0.000 2646 22 gamma 91 1854 0 0 0 0 0 -0.360 -0.740 58.040 58.046 0.000 2647 22 gamma 91 1858 0 0 0 0 0 0.038 0.153 2.438 2.443 0.000 2648 22 gamma 91 1858 0 0 0 0 0 0.038 0.067 3.704 3.705 0.000 2649 111 (pi0) -91 1859 0 3014 3015 0 0 -0.045 -0.136 6.900 6.903 0.135 2650 111 (pi0) -91 1859 0 3016 3017 0 0 -0.074 -0.195 6.823 6.828 0.135 2651 111 (pi0) -91 1859 0 3018 3019 0 0 -0.050 -0.258 3.570 3.583 0.135 2652 22 gamma 91 1865 0 0 0 0 0 0.182 0.057 2.805 2.811 0.000 2653 22 gamma 91 1865 0 0 0 0 0 0.951 0.639 16.632 16.671 0.000 2654 22 gamma 91 1866 0 0 0 0 0 0.147 0.089 0.994 1.009 0.000 2655 22 gamma 91 1866 0 0 0 0 0 1.845 0.982 15.077 15.221 0.000 2656 111 (pi0) -91 1868 0 3020 3021 0 0 0.128 0.053 3.785 3.790 0.135 2657 111 (pi0) -91 1868 0 3022 3023 0 0 0.304 0.147 3.355 3.374 0.135 2658 111 (pi0) -91 1868 0 3024 3025 0 0 0.213 0.269 3.550 3.569 0.135 2659 211 pi+ 91 1891 0 0 0 0 0 -0.748 0.067 13.981 14.002 0.140 2660 -211 pi- 91 1891 0 0 0 0 0 -0.169 0.123 2.407 2.420 0.140 2661 111 (pi0) -91 1891 0 3026 3027 0 0 0.018 0.063 3.142 3.146 0.135 2662 22 gamma 91 1892 0 0 0 0 0 -0.560 -0.296 3.111 3.175 0.000 2663 22 gamma 91 1892 0 0 0 0 0 -0.056 -0.001 0.157 0.167 0.000 2664 22 gamma 91 1894 0 0 0 0 0 -0.082 -0.035 3.932 3.933 0.000 2665 22 gamma 91 1894 0 0 0 0 0 0.036 -0.098 5.997 5.998 0.000 2666 211 pi+ 91 1896 0 0 0 0 0 -0.272 0.461 52.390 52.393 0.140 2667 -211 pi- 91 1896 0 0 0 0 0 0.031 0.122 5.971 5.974 0.140 2668 111 (pi0) -91 1896 0 3028 3029 0 0 -0.263 0.633 57.980 57.985 0.135 2669 22 gamma 91 1897 0 0 0 0 0 -0.075 -0.031 0.335 0.345 0.000 2670 22 gamma 91 1897 0 0 0 0 0 -0.024 -0.034 1.208 1.209 0.000 2671 211 pi+ 91 1919 0 0 0 0 0 -0.013 -0.056 0.436 0.462 0.140 2672 -211 pi- 91 1919 0 0 0 0 0 0.082 0.146 0.728 0.760 0.140 2673 221 (eta) -91 1919 0 3030 3031 0 0 0.058 0.132 3.657 3.701 0.548 2674 211 pi+ 91 1920 0 0 0 0 0 -0.027 -0.148 2.042 2.052 0.140 2675 -211 pi- 91 1920 0 0 0 0 0 0.090 -0.347 3.471 3.492 0.140 2676 221 (eta) -91 1920 0 3032 3034 0 0 -0.304 -0.491 9.356 9.390 0.548 2677 211 pi+ 91 1925 0 0 0 0 0 0.141 -0.216 1.492 1.520 0.140 2678 -211 pi- 91 1925 0 0 0 0 0 0.082 -0.010 2.297 2.303 0.140 2679 111 (pi0) -91 1925 0 3035 3036 0 0 0.362 -0.888 8.320 8.376 0.135 2680 3122 (Lambda0) -91 1931 0 3037 3038 0 0 0.707 0.336 1.860 2.306 1.116 2681 22 gamma 91 1931 0 0 0 0 0 -0.027 -0.006 -0.002 0.028 0.000 2682 -2112 nbar0 91 1932 0 0 0 0 0 1.094 0.214 0.639 1.592 0.940 2683 -211 pi- 91 1932 0 0 0 0 0 0.040 0.181 0.108 0.256 0.140 2684 22 gamma 91 1936 0 0 0 0 0 -0.018 -0.000 -0.072 0.074 0.000 2685 22 gamma 91 1936 0 0 0 0 0 -0.035 0.102 0.023 0.110 0.000 2686 22 gamma 91 1946 0 0 0 0 0 0.276 0.377 -11.405 11.415 0.000 2687 22 gamma 91 1946 0 0 0 0 0 0.040 -0.003 -1.072 1.073 0.000 2688 211 pi+ 91 1950 0 0 0 0 0 -0.050 0.063 -0.938 0.952 0.140 2689 -211 pi- 91 1950 0 0 0 0 0 0.030 -0.081 -3.029 3.034 0.140 2690 111 (pi0) -91 1950 0 3039 3040 0 0 0.074 -0.213 -11.320 11.323 0.135 2691 22 gamma 91 1951 0 0 0 0 0 -0.292 0.043 -0.949 0.994 0.000 2692 11 e- 91 1951 0 0 0 0 0 0.028 0.032 -0.131 0.138 0.001 2693 -11 e+ 91 1951 0 0 0 0 0 0.180 0.239 -0.934 0.980 0.001 2694 211 pi+ 91 1952 0 0 0 0 0 -0.039 -0.156 -1.177 1.196 0.140 2695 -211 pi- 91 1952 0 0 0 0 0 -0.061 0.111 -1.941 1.950 0.140 2696 111 (pi0) -91 1952 0 3041 3042 0 0 0.237 -0.189 -3.520 3.536 0.135 2697 211 pi+ 91 1961 0 0 0 0 0 -0.352 -0.252 -0.086 0.463 0.140 2698 -211 pi- 91 1961 0 0 0 0 0 -0.161 0.119 -0.009 0.244 0.140 2699 111 (pi0) -91 1961 0 3043 3044 0 0 -0.111 -0.157 -0.350 0.422 0.135 2700 22 gamma 91 1963 0 0 0 0 0 -0.093 -0.436 -0.347 0.565 0.000 2701 22 gamma 91 1963 0 0 0 0 0 -0.272 -0.706 -0.434 0.872 0.000 2702 211 pi+ 91 1971 0 0 0 0 0 -0.158 -0.268 -18.558 18.561 0.140 2703 -211 pi- 91 1971 0 0 0 0 0 0.096 0.175 -6.855 6.860 0.140 2704 111 (pi0) -91 1971 0 3045 3046 0 0 0.012 -0.020 -14.045 14.046 0.135 2705 22 gamma 91 1972 0 0 0 0 0 0.012 -0.094 -14.127 14.127 0.000 2706 22 gamma 91 1972 0 0 0 0 0 0.268 -0.220 -48.389 48.390 0.000 2707 22 gamma 91 1973 0 0 0 0 0 -0.096 0.021 -1.247 1.251 0.000 2708 22 gamma 91 1973 0 0 0 0 0 -0.274 0.011 -7.663 7.668 0.000 2709 22 gamma 91 1975 0 0 0 0 0 -0.347 0.049 -1.338 1.383 0.000 2710 22 gamma 91 1975 0 0 0 0 0 0.010 -0.001 -0.014 0.018 0.000 2711 211 pi+ 91 1981 0 0 0 0 0 -0.206 0.107 -0.180 0.325 0.140 2712 -211 pi- 91 1981 0 0 0 0 0 0.136 0.223 -0.079 0.307 0.140 2713 111 (pi0) -91 1981 0 3047 3048 0 0 -0.208 -0.069 0.055 0.263 0.135 2714 211 pi+ 91 1996 0 0 0 0 0 0.216 0.282 3.334 3.356 0.140 2715 -211 pi- 91 1996 0 0 0 0 0 0.353 0.176 5.733 5.748 0.140 2716 111 (pi0) -91 1996 0 3049 3050 0 0 0.037 0.078 1.224 1.234 0.135 2717 211 pi+ 91 2017 0 0 0 0 0 -0.138 0.080 -0.178 0.277 0.140 2718 -211 pi- 91 2017 0 0 0 0 0 -0.309 -0.114 0.119 0.377 0.140 2719 111 (pi0) -91 2017 0 3051 3052 0 0 0.116 -0.019 0.081 0.197 0.135 2720 3122 (Lambda0) -91 2021 0 3053 3054 0 0 0.260 0.322 11.172 11.235 1.116 2721 22 gamma 91 2021 0 0 0 0 0 -0.043 -0.029 0.309 0.314 0.000 2722 -2112 nbar0 91 2022 0 0 0 0 0 0.051 -0.122 10.210 10.254 0.940 2723 211 pi+ 91 2022 0 0 0 0 0 -0.061 0.195 2.213 2.226 0.140 2724 22 gamma 91 2028 0 0 0 0 0 0.003 0.136 6.612 6.613 0.000 2725 22 gamma 91 2028 0 0 0 0 0 -0.095 0.066 3.344 3.346 0.000 2726 211 pi+ 91 2029 0 0 0 0 0 -0.032 0.091 5.863 5.865 0.140 2727 -211 pi- 91 2029 0 0 0 0 0 -0.186 0.049 2.829 2.839 0.140 2728 111 (pi0) -91 2029 0 3055 3056 0 0 -0.080 0.248 1.440 1.469 0.135 2729 211 pi+ 91 2030 0 0 0 0 0 -0.095 -0.008 2.948 2.953 0.140 2730 -211 pi- 91 2030 0 0 0 0 0 0.091 -0.088 1.928 1.937 0.140 2731 111 (pi0) -91 2030 0 3057 3058 0 0 0.071 0.087 1.664 1.673 0.135 2732 22 gamma 91 2033 0 0 0 0 0 0.259 -0.063 0.092 0.282 0.000 2733 22 gamma 91 2033 0 0 0 0 0 0.175 0.036 -0.017 0.180 0.000 2734 22 gamma 91 2060 0 0 0 0 0 0.001 -0.009 -0.002 0.009 0.000 2735 22 gamma 91 2060 0 0 0 0 0 0.048 0.010 0.781 0.782 0.000 2736 211 pi+ 91 2061 0 0 0 0 0 -0.265 -0.062 4.988 4.997 0.140 2737 -211 pi- 91 2061 0 0 0 0 0 -0.088 0.312 5.753 5.764 0.140 2738 111 (pi0) -91 2061 0 3059 3060 0 0 0.102 -0.071 3.168 3.173 0.135 2739 22 gamma 91 2065 0 0 0 0 0 0.011 0.228 4.828 4.833 0.000 2740 22 gamma 91 2065 0 0 0 0 0 0.180 0.627 17.872 17.884 0.000 2741 211 pi+ 91 2068 0 0 0 0 0 -0.082 0.349 2.526 2.555 0.140 2742 -211 pi- 91 2068 0 0 0 0 0 0.229 1.484 12.617 12.707 0.140 2743 111 (pi0) -91 2068 0 3061 3062 0 0 0.075 0.090 1.980 1.988 0.135 2744 211 pi+ 91 2072 0 0 0 0 0 0.067 0.401 1.615 1.672 0.140 2745 -211 pi- 91 2072 0 0 0 0 0 -0.038 0.087 1.807 1.815 0.140 2746 111 (pi0) -91 2072 0 3063 3064 0 0 0.133 0.704 6.020 6.064 0.135 2747 22 gamma 91 2108 0 0 0 0 0 -0.639 0.483 0.393 0.892 0.000 2748 22 gamma 91 2108 0 0 0 0 0 -1.513 1.143 0.703 2.022 0.000 2749 2112 n0 91 2112 0 0 0 0 0 -0.707 2.109 0.132 2.418 0.940 2750 -211 pi- 91 2112 0 0 0 0 0 0.020 0.237 0.162 0.320 0.140 2751 -3122 (Lambdabar0) -91 2113 0 3065 3066 0 0 -0.320 2.694 0.003 2.933 1.116 2752 22 gamma 91 2113 0 0 0 0 0 -0.087 0.302 -0.042 0.317 0.000 2753 22 gamma 91 2122 0 0 0 0 0 0.081 0.096 -0.066 0.142 0.000 2754 22 gamma 91 2122 0 0 0 0 0 1.440 0.950 -1.020 2.004 0.000 2755 111 (pi0) -91 2125 0 3067 3068 0 0 0.692 0.621 -0.988 1.364 0.135 2756 111 (pi0) -91 2125 0 3069 3070 0 0 1.157 0.819 -1.206 1.866 0.135 2757 111 (pi0) -91 2125 0 3071 3072 0 0 1.362 0.832 -1.473 2.176 0.135 2758 22 gamma 91 2126 0 0 0 0 0 1.830 1.188 -2.010 2.966 0.000 2759 22 gamma 91 2126 0 0 0 0 0 0.311 0.143 -0.289 0.447 0.000 2760 22 gamma 91 2128 0 0 0 0 0 0.220 0.149 -0.302 0.402 0.000 2761 22 gamma 91 2128 0 0 0 0 0 1.696 1.124 -1.787 2.708 0.000 2762 211 pi+ 91 2132 0 0 0 0 0 1.345 1.349 -2.231 2.937 0.140 2763 -211 pi- 91 2132 0 0 0 0 0 1.257 0.817 -1.401 2.056 0.140 2764 111 (pi0) -91 2132 0 3073 3074 0 0 0.818 0.525 -0.799 1.265 0.135 2765 22 gamma 91 2133 0 0 0 0 0 1.694 1.685 -2.522 3.475 0.000 2766 22 gamma 91 2133 0 0 0 0 0 0.832 0.862 -1.402 1.844 0.000 2767 211 pi+ 91 2134 0 0 0 0 0 0.975 1.005 -1.714 2.217 0.140 2768 -211 pi- 91 2134 0 0 0 0 0 1.202 0.697 -1.634 2.150 0.140 2769 111 (pi0) -91 2134 0 3075 3076 0 0 0.177 0.107 -0.472 0.533 0.135 2770 22 gamma 91 2138 0 0 0 0 0 0.266 0.375 -0.246 0.522 0.000 2771 22 gamma 91 2138 0 0 0 0 0 0.059 0.235 -0.084 0.256 0.000 2772 22 gamma 91 2183 0 0 0 0 0 0.490 -0.938 -0.644 1.239 0.000 2773 22 gamma 91 2183 0 0 0 0 0 0.605 -1.469 -1.064 1.912 0.000 2774 211 pi+ 91 2185 0 0 0 0 0 0.246 0.021 -0.634 0.694 0.140 2775 -211 pi- 91 2185 0 0 0 0 0 0.613 0.141 -0.460 0.792 0.140 2776 111 (pi0) -91 2185 0 3077 3078 0 0 0.821 -0.146 -1.011 1.318 0.135 2777 22 gamma 91 2194 0 0 0 0 0 -0.059 -0.115 0.224 0.259 0.000 2778 22 gamma 91 2194 0 0 0 0 0 0.051 -0.178 0.178 0.257 0.000 2779 211 pi+ 91 2195 0 0 0 0 0 0.060 0.121 -0.127 0.232 0.140 2780 -211 pi- 91 2195 0 0 0 0 0 -0.125 0.009 0.042 0.192 0.140 2781 111 (pi0) -91 2195 0 3079 3080 0 0 -0.065 -0.038 -0.037 0.159 0.135 2782 211 pi+ 91 2204 0 0 0 0 0 -0.266 -1.112 0.551 1.277 0.140 2783 -211 pi- 91 2204 0 0 0 0 0 -1.232 -2.704 1.820 3.488 0.140 2784 111 (pi0) -91 2204 0 3081 3082 0 0 -0.268 -0.390 0.376 0.619 0.135 2785 22 gamma 91 2206 0 0 0 0 0 -0.484 -1.347 0.677 1.583 0.000 2786 22 gamma 91 2206 0 0 0 0 0 -0.008 -0.145 0.080 0.166 0.000 2787 211 pi+ 91 2241 0 0 0 0 0 -0.625 0.714 4.389 4.493 0.140 2788 -211 pi- 91 2241 0 0 0 0 0 -0.176 0.286 0.839 0.914 0.140 2789 111 (pi0) -91 2241 0 3083 3084 0 0 -0.644 0.307 2.578 2.679 0.135 2790 111 (pi0) -91 2244 0 3085 3086 0 0 -0.259 0.015 2.472 2.489 0.135 2791 111 (pi0) -91 2244 0 3087 3088 0 0 -0.134 0.132 1.981 1.995 0.135 2792 111 (pi0) -91 2244 0 3089 3090 0 0 -0.265 0.152 1.413 1.452 0.135 2793 111 (pi0) -91 2248 0 3091 3092 0 0 -0.007 -0.040 3.730 3.733 0.135 2794 111 (pi0) -91 2248 0 3093 3094 0 0 -0.006 -0.216 5.449 5.455 0.135 2795 111 (pi0) -91 2248 0 3095 3096 0 0 0.136 -0.141 2.389 2.401 0.135 2796 2112 n0 91 2258 0 0 0 0 0 -0.632 0.064 0.886 1.439 0.940 2797 -211 pi- 91 2258 0 0 0 0 0 -0.403 0.184 0.452 0.648 0.140 2798 -2112 nbar0 91 2259 0 0 0 0 0 -0.331 -0.009 -0.681 1.207 0.940 2799 211 pi+ 91 2259 0 0 0 0 0 0.106 -0.032 -0.339 0.383 0.140 2800 22 gamma 91 2260 0 0 0 0 0 -0.161 -0.008 0.046 0.168 0.000 2801 22 gamma 91 2260 0 0 0 0 0 -0.006 0.029 -0.038 0.049 0.000 2802 2112 n0 91 2268 0 0 0 0 0 0.971 -0.442 -19.743 19.794 0.940 2803 211 pi+ 91 2268 0 0 0 0 0 0.498 -0.294 -6.502 6.530 0.140 2804 -2212 pbar- 91 2269 0 0 0 0 0 -0.140 -0.526 -7.672 7.749 0.938 2805 111 (pi0) -91 2269 0 3097 3098 0 0 -0.031 0.044 -2.745 2.749 0.135 2806 2112 n0 91 2273 0 0 0 0 0 1.542 0.311 -22.873 22.946 0.940 2807 -211 pi- 91 2273 0 0 0 0 0 0.742 0.333 -10.779 10.810 0.140 2808 211 pi+ 91 2274 0 0 0 0 0 0.192 -0.117 -8.226 8.230 0.140 2809 -211 pi- 91 2274 0 0 0 0 0 0.992 0.255 -25.343 25.364 0.140 2810 111 (pi0) -91 2274 0 3099 3100 0 0 1.208 0.096 -27.612 27.638 0.135 2811 22 gamma 91 2278 0 0 0 0 0 -0.003 0.012 -0.021 0.025 0.000 2812 22 gamma 91 2278 0 0 0 0 0 0.413 0.095 -2.278 2.317 0.000 2813 211 pi+ 91 2282 0 0 0 0 0 -0.010 -0.225 1.418 1.442 0.140 2814 -211 pi- 91 2282 0 0 0 0 0 -0.051 0.019 0.595 0.614 0.140 2815 111 (pi0) -91 2282 0 3101 3102 0 0 0.334 0.163 3.090 3.116 0.135 2816 211 pi+ 91 2291 0 0 0 0 0 1.039 -0.324 -1.693 2.018 0.140 2817 -211 pi- 91 2291 0 0 0 0 0 0.977 -0.294 -1.009 1.442 0.140 2818 111 (pi0) -91 2291 0 3103 3104 0 0 1.677 -0.127 -2.223 2.791 0.135 2819 22 gamma 91 2296 0 0 0 0 0 -0.001 0.279 -43.102 43.103 0.000 2820 22 gamma 91 2296 0 0 0 0 0 -0.147 0.328 -49.968 49.970 0.000 2821 211 pi+ 91 2307 0 0 0 0 0 0.088 0.175 6.979 6.984 0.140 2822 -211 pi- 91 2307 0 0 0 0 0 0.103 -0.211 3.348 3.359 0.140 2823 111 (pi0) -91 2307 0 3105 3106 0 0 -0.104 0.152 5.615 5.620 0.135 2824 211 pi+ 91 2312 0 0 0 0 0 1.129 0.610 -11.676 11.747 0.140 2825 -211 pi- 91 2312 0 0 0 0 0 2.113 1.158 -17.364 17.531 0.140 2826 22 gamma 91 2318 0 0 0 0 0 0.174 -0.201 0.759 0.804 0.000 2827 22 gamma 91 2318 0 0 0 0 0 0.013 0.007 0.212 0.213 0.000 2828 22 gamma 91 2324 0 0 0 0 0 -0.792 0.367 -0.089 0.877 0.000 2829 22 gamma 91 2324 0 0 0 0 0 -0.198 0.074 0.043 0.216 0.000 2830 211 pi+ 91 2325 0 0 0 0 0 0.032 -0.143 -56.063 56.063 0.140 2831 -211 pi- 91 2325 0 0 0 0 0 -0.474 -0.257 -95.334 95.336 0.140 2832 22 gamma 91 2327 0 0 0 0 0 -0.222 0.007 -65.042 65.043 0.000 2833 22 gamma 91 2327 0 0 0 0 0 -0.262 -0.143 -92.087 92.088 0.000 2834 22 gamma 91 2329 0 0 0 0 0 -1.281 -0.321 -22.999 23.037 0.000 2835 22 gamma 91 2329 0 0 0 0 0 -0.239 -0.063 -3.394 3.403 0.000 2836 22 gamma 91 2334 0 0 0 0 0 0.653 -0.226 -6.506 6.542 0.000 2837 22 gamma 91 2334 0 0 0 0 0 0.045 -0.032 -0.276 0.281 0.000 2838 22 gamma 91 2336 0 0 0 0 0 0.606 0.160 -12.859 12.874 0.000 2839 22 gamma 91 2336 0 0 0 0 0 0.929 0.141 -16.764 16.790 0.000 2840 22 gamma 91 2340 0 0 0 0 0 -0.600 -1.977 1.915 2.817 0.000 2841 22 gamma 91 2340 0 0 0 0 0 -0.165 -0.603 0.484 0.790 0.000 2842 211 pi+ 91 2342 0 0 0 0 0 -1.474 -0.858 0.129 1.716 0.140 2843 -211 pi- 91 2342 0 0 0 0 0 -0.743 -0.402 0.354 0.926 0.140 2844 22 gamma 91 2346 0 0 0 0 0 -0.384 -0.033 -0.095 0.396 0.000 2845 22 gamma 91 2346 0 0 0 0 0 -0.141 -0.047 -0.122 0.193 0.000 2846 22 gamma 91 2348 0 0 0 0 0 -0.543 1.989 4.401 4.860 0.000 2847 22 gamma 91 2348 0 0 0 0 0 -0.122 0.757 1.667 1.835 0.000 2848 22 gamma 91 2350 0 0 0 0 0 -0.614 -0.057 34.307 34.313 0.000 2849 22 gamma 91 2350 0 0 0 0 0 -0.042 -0.004 5.296 5.296 0.000 2850 22 gamma 91 2354 0 0 0 0 0 0.883 -0.110 7.563 7.616 0.000 2851 22 gamma 91 2354 0 0 0 0 0 0.408 0.027 3.910 3.931 0.000 2852 211 pi+ 91 2355 0 0 0 0 0 -0.426 0.083 12.589 12.597 0.140 2853 -211 pi- 91 2355 0 0 0 0 0 -0.022 0.110 1.872 1.880 0.140 2854 22 gamma 91 2357 0 0 0 0 0 -0.075 -0.070 0.326 0.341 0.000 2855 22 gamma 91 2357 0 0 0 0 0 -0.106 0.055 0.569 0.581 0.000 2856 22 gamma 91 2359 0 0 0 0 0 -0.752 -0.098 0.339 0.831 0.000 2857 22 gamma 91 2359 0 0 0 0 0 -0.032 -0.035 0.011 0.049 0.000 2858 22 gamma 91 2365 0 0 0 0 0 -0.132 0.027 0.586 0.601 0.000 2859 22 gamma 91 2365 0 0 0 0 0 -0.233 -0.125 0.921 0.958 0.000 2860 22 gamma 91 2367 0 0 0 0 0 -0.450 0.276 1.068 1.192 0.000 2861 22 gamma 91 2367 0 0 0 0 0 -0.046 -0.015 0.107 0.117 0.000 2862 22 gamma 91 2371 0 0 0 0 0 -0.001 0.089 3.205 3.206 0.000 2863 22 gamma 91 2371 0 0 0 0 0 0.028 0.356 26.948 26.951 0.000 2864 211 pi+ 91 2372 0 0 0 0 0 -0.464 -0.407 130.375 130.376 0.140 2865 -211 pi- 91 2372 0 0 0 0 0 -0.213 -0.053 23.401 23.403 0.140 2866 22 gamma 91 2376 0 0 0 0 0 0.095 -0.225 3.268 3.277 0.000 2867 22 gamma 91 2376 0 0 0 0 0 0.393 -0.491 6.829 6.858 0.000 2868 22 gamma 91 2378 0 0 0 0 0 0.129 -0.385 3.576 3.599 0.000 2869 22 gamma 91 2378 0 0 0 0 0 0.093 -0.911 7.945 7.998 0.000 2870 22 gamma 91 2380 0 0 0 0 0 0.410 0.656 1.472 1.663 0.000 2871 22 gamma 91 2380 0 0 0 0 0 0.102 0.084 0.183 0.225 0.000 2872 22 gamma 91 2386 0 0 0 0 0 0.091 -0.005 -2.471 2.473 0.000 2873 22 gamma 91 2386 0 0 0 0 0 0.240 0.223 -8.799 8.805 0.000 2874 22 gamma 91 2388 0 0 0 0 0 -0.001 -0.121 -6.220 6.221 0.000 2875 22 gamma 91 2388 0 0 0 0 0 0.032 -0.268 -6.749 6.755 0.000 2876 22 gamma 91 2392 0 0 0 0 0 -0.004 -0.022 -0.032 0.039 0.000 2877 22 gamma 91 2392 0 0 0 0 0 0.051 0.106 0.049 0.128 0.000 2878 22 gamma 91 2394 0 0 0 0 0 -0.360 -0.220 -0.484 0.642 0.000 2879 22 gamma 91 2394 0 0 0 0 0 -0.919 -0.326 -1.164 1.519 0.000 2880 22 gamma 91 2396 0 0 0 0 0 -0.010 0.005 -0.005 0.012 0.000 2881 22 gamma 91 2396 0 0 0 0 0 -1.198 -0.828 -0.812 1.667 0.000 2882 22 gamma 91 2398 0 0 0 0 0 0.257 -0.065 -7.418 7.423 0.000 2883 22 gamma 91 2398 0 0 0 0 0 0.557 0.039 -18.150 18.159 0.000 2884 22 gamma 91 2402 0 0 0 0 0 -0.229 0.262 -1.537 1.576 0.000 2885 22 gamma 91 2402 0 0 0 0 0 -0.053 -0.007 -0.182 0.190 0.000 2886 22 gamma 91 2406 0 0 0 0 0 -0.101 0.108 0.476 0.498 0.000 2887 22 gamma 91 2406 0 0 0 0 0 0.032 0.106 0.247 0.270 0.000 2888 22 gamma 91 2408 0 0 0 0 0 0.213 0.139 0.435 0.504 0.000 2889 22 gamma 91 2408 0 0 0 0 0 0.088 0.146 0.160 0.234 0.000 2890 22 gamma 91 2410 0 0 0 0 0 0.113 0.062 0.047 0.137 0.000 2891 22 gamma 91 2410 0 0 0 0 0 0.061 -0.036 -0.047 0.084 0.000 2892 22 gamma 91 2417 0 0 0 0 0 0.123 0.073 0.195 0.242 0.000 2893 22 gamma 91 2417 0 0 0 0 0 0.084 0.242 0.285 0.383 0.000 2894 22 gamma 91 2424 0 0 0 0 0 -0.577 -0.606 34.320 34.330 0.000 2895 22 gamma 91 2424 0 0 0 0 0 -0.037 -0.009 2.611 2.612 0.000 2896 22 gamma 91 2426 0 0 0 0 0 -0.008 0.016 2.247 2.247 0.000 2897 22 gamma 91 2426 0 0 0 0 0 0.316 0.348 23.745 23.750 0.000 2898 22 gamma 91 2428 0 0 0 0 0 0.018 0.269 0.272 0.383 0.000 2899 22 gamma 91 2428 0 0 0 0 0 -0.023 0.035 0.142 0.148 0.000 2900 22 gamma 91 2430 0 0 0 0 0 0.260 0.252 -0.157 0.395 0.000 2901 22 gamma 91 2430 0 0 0 0 0 0.024 0.027 0.027 0.045 0.000 2902 211 pi+ 91 2431 0 0 0 0 0 -0.246 -0.148 190.156 190.156 0.140 2903 -211 pi- 91 2431 0 0 0 0 0 -0.236 -0.581 202.108 202.109 0.140 2904 22 gamma 91 2433 0 0 0 0 0 0.384 -0.163 39.517 39.519 0.000 2905 22 gamma 91 2433 0 0 0 0 0 0.015 0.013 4.969 4.969 0.000 2906 22 gamma 91 2437 0 0 0 0 0 0.403 1.543 -0.542 1.684 0.000 2907 22 gamma 91 2437 0 0 0 0 0 0.178 0.506 -0.115 0.549 0.000 2908 22 gamma 91 2441 0 0 0 0 0 -0.328 1.299 583.638 583.639 0.000 2909 22 gamma 91 2441 0 0 0 0 0 -0.067 0.104 56.958 56.958 0.000 2910 22 gamma 91 2443 0 0 0 0 0 -0.023 0.040 8.179 8.179 0.000 2911 22 gamma 91 2443 0 0 0 0 0 -0.580 1.437 169.651 169.658 0.000 2912 22 gamma 91 2450 0 0 0 0 0 0.052 0.021 0.312 0.318 0.000 2913 22 gamma 91 2450 0 0 0 0 0 0.362 0.511 5.467 5.503 0.000 2914 22 gamma 91 2452 0 0 0 0 0 0.056 -0.022 1.392 1.394 0.000 2915 22 gamma 91 2452 0 0 0 0 0 0.151 -0.044 0.993 1.006 0.000 2916 22 gamma 91 2454 0 0 0 0 0 -0.341 0.428 -0.108 0.558 0.000 2917 22 gamma 91 2454 0 0 0 0 0 -0.009 0.027 0.025 0.038 0.000 2918 211 pi+ 91 2455 0 0 0 0 0 -0.315 0.674 0.401 0.856 0.140 2919 -211 pi- 91 2455 0 0 0 0 0 -0.547 0.319 0.298 0.713 0.140 2920 22 gamma 91 2459 0 0 0 0 0 0.027 0.410 0.055 0.414 0.000 2921 22 gamma 91 2459 0 0 0 0 0 -0.020 0.888 0.307 0.940 0.000 2922 22 gamma 91 2461 0 0 0 0 0 -0.338 0.857 -0.312 0.973 0.000 2923 22 gamma 91 2461 0 0 0 0 0 -0.160 0.735 -0.242 0.790 0.000 2924 22 gamma 91 2467 0 0 0 0 0 4.078 3.010 -5.152 7.227 0.000 2925 22 gamma 91 2467 0 0 0 0 0 2.646 1.822 -3.238 4.561 0.000 2926 22 gamma 91 2469 0 0 0 0 0 1.481 1.033 -1.919 2.635 0.000 2927 22 gamma 91 2469 0 0 0 0 0 4.681 3.500 -6.425 8.685 0.000 2928 22 gamma 91 2471 0 0 0 0 0 0.594 0.917 -1.451 1.816 0.000 2929 22 gamma 91 2471 0 0 0 0 0 0.055 0.032 -0.110 0.127 0.000 2930 22 gamma 91 2473 0 0 0 0 0 0.034 0.110 -0.089 0.146 0.000 2931 22 gamma 91 2473 0 0 0 0 0 0.534 0.989 -1.377 1.778 0.000 2932 22 gamma 91 2477 0 0 0 0 0 -0.007 0.171 -0.151 0.229 0.000 2933 22 gamma 91 2477 0 0 0 0 0 -0.115 0.086 -0.126 0.191 0.000 2934 22 gamma 91 2479 0 0 0 0 0 -0.014 -0.003 -0.085 0.086 0.000 2935 22 gamma 91 2479 0 0 0 0 0 0.219 0.022 -0.349 0.413 0.000 2936 22 gamma 91 2489 0 0 0 0 0 0.028 -0.015 -0.207 0.209 0.000 2937 22 gamma 91 2489 0 0 0 0 0 0.201 0.268 -2.254 2.278 0.000 2938 22 gamma 91 2493 0 0 0 0 0 0.096 -0.063 -0.957 0.964 0.000 2939 22 gamma 91 2493 0 0 0 0 0 0.303 -0.484 -3.467 3.514 0.000 2940 22 gamma 91 2497 0 0 0 0 0 0.150 -0.070 -0.060 0.176 0.000 2941 22 gamma 91 2497 0 0 0 0 0 -0.008 -0.076 -0.054 0.093 0.000 2942 22 gamma 91 2499 0 0 0 0 0 -0.045 -0.035 0.007 0.057 0.000 2943 22 gamma 91 2499 0 0 0 0 0 -0.021 -0.334 -0.138 0.362 0.000 2944 22 gamma 91 2501 0 0 0 0 0 0.376 0.030 -0.204 0.429 0.000 2945 22 gamma 91 2501 0 0 0 0 0 0.757 0.191 -0.591 0.980 0.000 2946 22 gamma 91 2503 0 0 0 0 0 0.434 -0.119 -1.070 1.161 0.000 2947 22 gamma 91 2503 0 0 0 0 0 0.037 -0.049 -0.085 0.105 0.000 2948 22 gamma 91 2505 0 0 0 0 0 0.003 -0.014 -0.033 0.036 0.000 2949 22 gamma 91 2505 0 0 0 0 0 0.802 -0.164 -0.973 1.272 0.000 2950 22 gamma 91 2509 0 0 0 0 0 -0.354 0.487 -0.448 0.751 0.000 2951 22 gamma 91 2509 0 0 0 0 0 0.004 0.027 -0.053 0.060 0.000 2952 22 gamma 91 2515 0 0 0 0 0 -1.782 -1.695 1.412 2.836 0.000 2953 22 gamma 91 2515 0 0 0 0 0 -0.044 -0.060 0.021 0.077 0.000 2954 22 gamma 91 2534 0 0 0 0 0 -0.125 -0.015 0.258 0.287 0.000 2955 22 gamma 91 2534 0 0 0 0 0 0.020 -0.055 0.115 0.129 0.000 2956 22 gamma 91 2536 0 0 0 0 0 -0.138 0.122 -0.093 0.207 0.000 2957 22 gamma 91 2536 0 0 0 0 0 0.006 -0.022 0.007 0.024 0.000 2958 22 gamma 91 2538 0 0 0 0 0 -0.012 0.109 -0.364 0.380 0.000 2959 22 gamma 91 2538 0 0 0 0 0 -0.175 0.099 -0.668 0.698 0.000 2960 22 gamma 91 2540 0 0 0 0 0 0.070 -0.125 -0.601 0.618 0.000 2961 22 gamma 91 2540 0 0 0 0 0 -0.047 -0.070 -0.674 0.679 0.000 2962 22 gamma 91 2544 0 0 0 0 0 -0.357 0.180 -3.784 3.805 0.000 2963 22 gamma 91 2544 0 0 0 0 0 -0.422 0.374 -5.997 6.023 0.000 2964 22 gamma 91 2548 0 0 0 0 0 -0.137 -0.028 -3.199 3.202 0.000 2965 22 gamma 91 2548 0 0 0 0 0 -0.023 -0.102 -3.122 3.124 0.000 2966 22 gamma 91 2552 0 0 0 0 0 0.064 0.279 -5.159 5.167 0.000 2967 22 gamma 91 2552 0 0 0 0 0 -0.008 0.003 -1.173 1.173 0.000 2968 22 gamma 91 2558 0 0 0 0 0 -0.081 -0.027 -0.066 0.108 0.000 2969 22 gamma 91 2558 0 0 0 0 0 -0.043 0.026 0.057 0.076 0.000 2970 22 gamma 91 2562 0 0 0 0 0 0.085 -0.055 -3.281 3.283 0.000 2971 22 gamma 91 2562 0 0 0 0 0 0.212 0.063 -5.108 5.113 0.000 2972 22 gamma 91 2564 0 0 0 0 0 0.008 -0.005 -0.154 0.154 0.000 2973 22 gamma 91 2564 0 0 0 0 0 -0.226 -0.456 -28.234 28.239 0.000 2974 22 gamma 91 2566 0 0 0 0 0 -0.244 0.118 -16.395 16.397 0.000 2975 22 gamma 91 2566 0 0 0 0 0 -0.346 0.008 -18.756 18.760 0.000 2976 22 gamma 91 2568 0 0 0 0 0 -0.221 0.151 -38.600 38.601 0.000 2977 22 gamma 91 2568 0 0 0 0 0 -0.496 0.138 -87.095 87.096 0.000 2978 22 gamma 91 2572 0 0 0 0 0 0.383 0.149 -2.178 2.216 0.000 2979 22 gamma 91 2572 0 0 0 0 0 0.058 0.008 -0.704 0.707 0.000 2980 22 gamma 91 2576 0 0 0 0 0 0.225 0.397 -3.518 3.547 0.000 2981 22 gamma 91 2576 0 0 0 0 0 -0.012 0.093 -0.627 0.634 0.000 2982 22 gamma 91 2584 0 0 0 0 0 -0.068 -0.075 135.841 135.841 0.000 2983 22 gamma 91 2584 0 0 0 0 0 0.050 -0.078 62.932 62.932 0.000 2984 211 pi+ 91 2587 0 0 0 0 0 -0.045 0.141 35.030 35.031 0.140 2985 -211 pi- 91 2587 0 0 0 0 0 -0.186 0.080 201.100 201.100 0.140 2986 111 (pi0) -91 2588 0 3107 3109 0 0 -0.800 0.584 90.842 90.848 0.135 2987 111 (pi0) -91 2588 0 3110 3111 0 0 -0.219 0.441 64.556 64.558 0.135 2988 211 pi+ 91 2589 0 0 0 0 0 0.049 0.160 57.053 57.054 0.140 2989 -211 pi- 91 2589 0 0 0 0 0 0.083 0.153 11.079 11.081 0.140 2990 211 pi+ 91 2596 0 0 0 0 0 0.115 0.087 -0.473 0.514 0.140 2991 -211 pi- 91 2596 0 0 0 0 0 -0.047 -0.287 -0.412 0.524 0.140 2992 22 gamma 91 2603 0 0 0 0 0 0.142 0.198 -1.295 1.318 0.000 2993 22 gamma 91 2603 0 0 0 0 0 1.243 0.091 -3.903 4.098 0.000 2994 22 gamma 91 2608 0 0 0 0 0 -0.037 0.060 0.018 0.073 0.000 2995 22 gamma 91 2608 0 0 0 0 0 -0.032 -0.068 -0.025 0.079 0.000 2996 22 gamma 91 2611 0 0 0 0 0 -0.051 0.090 0.461 0.473 0.000 2997 22 gamma 91 2611 0 0 0 0 0 0.088 0.185 1.029 1.049 0.000 2998 22 gamma 91 2624 0 0 0 0 0 -0.088 0.069 -295.579 295.579 0.000 2999 22 gamma 91 2624 0 0 0 0 0 -0.013 0.047 -27.446 27.446 0.000 3000 22 gamma 91 2625 0 0 0 0 0 -1.037 -0.334 -20.670 20.698 0.000 3001 22 gamma 91 2625 0 0 0 0 0 -1.550 -0.671 -31.294 31.340 0.000 3002 22 gamma 91 2629 0 0 0 0 0 -0.237 -0.040 -3.536 3.544 0.000 3003 22 gamma 91 2629 0 0 0 0 0 -0.164 0.040 -4.225 4.228 0.000 3004 22 gamma 91 2634 0 0 0 0 0 0.103 0.080 -2.007 2.012 0.000 3005 22 gamma 91 2634 0 0 0 0 0 0.388 0.266 -4.231 4.257 0.000 3006 22 gamma 91 2637 0 0 0 0 0 -0.056 -0.167 -17.288 17.289 0.000 3007 22 gamma 91 2637 0 0 0 0 0 -0.022 -0.396 -25.236 25.239 0.000 3008 22 gamma 91 2640 0 0 0 0 0 -0.394 -0.590 0.343 0.788 0.000 3009 22 gamma 91 2640 0 0 0 0 0 -0.037 -0.154 0.044 0.164 0.000 3010 211 pi+ 91 2642 0 0 0 0 0 -0.291 -1.554 1.735 2.351 0.140 3011 -211 pi- 91 2642 0 0 0 0 0 -0.016 -2.402 3.040 3.877 0.140 3012 211 pi+ 91 2644 0 0 0 0 0 0.072 -0.374 0.644 0.761 0.140 3013 -211 pi- 91 2644 0 0 0 0 0 -0.438 -0.974 1.615 1.942 0.140 3014 22 gamma 91 2649 0 0 0 0 0 -0.021 -0.047 0.631 0.633 0.000 3015 22 gamma 91 2649 0 0 0 0 0 -0.024 -0.089 6.269 6.270 0.000 3016 22 gamma 91 2650 0 0 0 0 0 -0.091 -0.166 4.175 4.179 0.000 3017 22 gamma 91 2650 0 0 0 0 0 0.018 -0.029 2.648 2.648 0.000 3018 22 gamma 91 2651 0 0 0 0 0 0.013 -0.180 2.789 2.795 0.000 3019 22 gamma 91 2651 0 0 0 0 0 -0.062 -0.078 0.782 0.788 0.000 3020 22 gamma 91 2656 0 0 0 0 0 0.105 0.096 2.553 2.556 0.000 3021 22 gamma 91 2656 0 0 0 0 0 0.023 -0.043 1.232 1.233 0.000 3022 22 gamma 91 2657 0 0 0 0 0 0.215 0.162 2.708 2.722 0.000 3023 22 gamma 91 2657 0 0 0 0 0 0.089 -0.015 0.646 0.653 0.000 3024 22 gamma 91 2658 0 0 0 0 0 0.222 0.202 2.811 2.827 0.000 3025 22 gamma 91 2658 0 0 0 0 0 -0.010 0.067 0.738 0.741 0.000 3026 22 gamma 91 2661 0 0 0 0 0 -0.016 -0.023 0.180 0.182 0.000 3027 22 gamma 91 2661 0 0 0 0 0 0.034 0.086 2.962 2.964 0.000 3028 22 gamma 91 2668 0 0 0 0 0 -0.252 0.580 55.609 55.613 0.000 3029 22 gamma 91 2668 0 0 0 0 0 -0.011 0.053 2.371 2.372 0.000 3030 22 gamma 91 2673 0 0 0 0 0 -0.193 0.121 0.775 0.808 0.000 3031 22 gamma 91 2673 0 0 0 0 0 0.251 0.011 2.882 2.893 0.000 3032 211 pi+ 91 2676 0 0 0 0 0 -0.161 -0.105 1.715 1.732 0.140 3033 -211 pi- 91 2676 0 0 0 0 0 -0.026 -0.083 2.450 2.456 0.140 3034 111 (pi0) -91 2676 0 3112 3113 0 0 -0.116 -0.304 5.190 5.202 0.135 3035 22 gamma 91 2679 0 0 0 0 0 0.273 -0.737 7.164 7.207 0.000 3036 22 gamma 91 2679 0 0 0 0 0 0.088 -0.151 1.156 1.169 0.000 3037 2212 p+ 91 2680 0 0 0 0 0 0.703 0.264 1.586 1.990 0.938 3038 -211 pi- 91 2680 0 0 0 0 0 0.004 0.072 0.274 0.316 0.140 3039 22 gamma 91 2690 0 0 0 0 0 0.017 -0.024 -0.341 0.342 0.000 3040 22 gamma 91 2690 0 0 0 0 0 0.057 -0.189 -10.979 10.981 0.000 3041 22 gamma 91 2696 0 0 0 0 0 0.116 -0.172 -2.415 2.424 0.000 3042 22 gamma 91 2696 0 0 0 0 0 0.120 -0.017 -1.105 1.112 0.000 3043 22 gamma 91 2699 0 0 0 0 0 -0.134 -0.094 -0.206 0.263 0.000 3044 22 gamma 91 2699 0 0 0 0 0 0.022 -0.063 -0.144 0.158 0.000 3045 22 gamma 91 2704 0 0 0 0 0 -0.060 -0.009 -7.776 7.776 0.000 3046 22 gamma 91 2704 0 0 0 0 0 0.073 -0.010 -6.269 6.269 0.000 3047 22 gamma 91 2713 0 0 0 0 0 -0.075 -0.087 0.058 0.129 0.000 3048 22 gamma 91 2713 0 0 0 0 0 -0.133 0.019 -0.003 0.134 0.000 3049 22 gamma 91 2716 0 0 0 0 0 -0.018 0.029 0.957 0.958 0.000 3050 22 gamma 91 2716 0 0 0 0 0 0.054 0.049 0.266 0.276 0.000 3051 22 gamma 91 2719 0 0 0 0 0 0.126 -0.012 0.012 0.127 0.000 3052 22 gamma 91 2719 0 0 0 0 0 -0.010 -0.008 0.069 0.070 0.000 3053 2212 p+ 91 2720 0 0 0 0 0 0.226 0.363 9.217 9.275 0.938 3054 -211 pi- 91 2720 0 0 0 0 0 0.034 -0.041 1.954 1.960 0.140 3055 22 gamma 91 2728 0 0 0 0 0 -0.055 0.247 1.397 1.420 0.000 3056 22 gamma 91 2728 0 0 0 0 0 -0.025 0.000 0.043 0.049 0.000 3057 22 gamma 91 2731 0 0 0 0 0 -0.039 0.024 0.571 0.573 0.000 3058 22 gamma 91 2731 0 0 0 0 0 0.111 0.063 1.093 1.100 0.000 3059 22 gamma 91 2738 0 0 0 0 0 -0.023 -0.041 0.484 0.486 0.000 3060 22 gamma 91 2738 0 0 0 0 0 0.124 -0.031 2.684 2.687 0.000 3061 22 gamma 91 2743 0 0 0 0 0 0.101 0.092 1.866 1.871 0.000 3062 22 gamma 91 2743 0 0 0 0 0 -0.026 -0.002 0.114 0.117 0.000 3063 22 gamma 91 2746 0 0 0 0 0 -0.026 0.055 0.500 0.504 0.000 3064 22 gamma 91 2746 0 0 0 0 0 0.159 0.649 5.520 5.560 0.000 3065 -2112 nbar0 91 2751 0 0 0 0 0 -0.321 2.538 0.030 2.725 0.940 3066 111 (pi0) -91 2751 0 3114 3115 0 0 0.000 0.156 -0.027 0.208 0.135 3067 22 gamma 91 2755 0 0 0 0 0 0.357 0.405 -0.599 0.807 0.000 3068 22 gamma 91 2755 0 0 0 0 0 0.335 0.216 -0.389 0.557 0.000 3069 22 gamma 91 2756 0 0 0 0 0 0.636 0.522 -0.739 1.106 0.000 3070 22 gamma 91 2756 0 0 0 0 0 0.521 0.297 -0.467 0.760 0.000 3071 22 gamma 91 2757 0 0 0 0 0 0.253 0.218 -0.294 0.445 0.000 3072 22 gamma 91 2757 0 0 0 0 0 1.109 0.615 -1.178 1.731 0.000 3073 22 gamma 91 2764 0 0 0 0 0 0.026 -0.001 -0.045 0.052 0.000 3074 22 gamma 91 2764 0 0 0 0 0 0.792 0.526 -0.754 1.213 0.000 3075 22 gamma 91 2769 0 0 0 0 0 0.018 -0.006 0.003 0.019 0.000 3076 22 gamma 91 2769 0 0 0 0 0 0.159 0.113 -0.475 0.513 0.000 3077 22 gamma 91 2776 0 0 0 0 0 0.251 -0.076 -0.235 0.352 0.000 3078 22 gamma 91 2776 0 0 0 0 0 0.570 -0.070 -0.776 0.966 0.000 3079 22 gamma 91 2781 0 0 0 0 0 -0.068 -0.068 0.017 0.098 0.000 3080 22 gamma 91 2781 0 0 0 0 0 0.003 0.030 -0.054 0.061 0.000 3081 22 gamma 91 2784 0 0 0 0 0 -0.089 -0.210 0.240 0.331 0.000 3082 22 gamma 91 2784 0 0 0 0 0 -0.179 -0.180 0.135 0.288 0.000 3083 22 gamma 91 2789 0 0 0 0 0 -0.209 0.168 1.027 1.061 0.000 3084 22 gamma 91 2789 0 0 0 0 0 -0.435 0.138 1.551 1.617 0.000 3085 22 gamma 91 2790 0 0 0 0 0 -0.170 -0.021 2.012 2.019 0.000 3086 22 gamma 91 2790 0 0 0 0 0 -0.090 0.036 0.460 0.470 0.000 3087 22 gamma 91 2791 0 0 0 0 0 -0.128 0.135 1.979 1.987 0.000 3088 22 gamma 91 2791 0 0 0 0 0 -0.006 -0.003 0.003 0.007 0.000 3089 22 gamma 91 2792 0 0 0 0 0 -0.055 0.005 0.101 0.115 0.000 3090 22 gamma 91 2792 0 0 0 0 0 -0.210 0.147 1.312 1.337 0.000 3091 22 gamma 91 2793 0 0 0 0 0 0.013 -0.080 3.111 3.112 0.000 3092 22 gamma 91 2793 0 0 0 0 0 -0.021 0.040 0.619 0.621 0.000 3093 22 gamma 91 2794 0 0 0 0 0 -0.031 -0.208 5.238 5.242 0.000 3094 22 gamma 91 2794 0 0 0 0 0 0.026 -0.008 0.211 0.213 0.000 3095 22 gamma 91 2795 0 0 0 0 0 0.079 -0.123 1.010 1.020 0.000 3096 22 gamma 91 2795 0 0 0 0 0 0.056 -0.018 1.379 1.381 0.000 3097 22 gamma 91 2805 0 0 0 0 0 0.041 0.010 -0.349 0.351 0.000 3098 22 gamma 91 2805 0 0 0 0 0 -0.072 0.034 -2.397 2.398 0.000 3099 22 gamma 91 2810 0 0 0 0 0 1.146 0.097 -25.377 25.403 0.000 3100 22 gamma 91 2810 0 0 0 0 0 0.062 -0.002 -2.234 2.235 0.000 3101 22 gamma 91 2815 0 0 0 0 0 0.044 0.069 0.955 0.959 0.000 3102 22 gamma 91 2815 0 0 0 0 0 0.291 0.094 2.135 2.157 0.000 3103 22 gamma 91 2818 0 0 0 0 0 0.157 0.024 -0.183 0.242 0.000 3104 22 gamma 91 2818 0 0 0 0 0 1.520 -0.150 -2.040 2.549 0.000 3105 22 gamma 91 2823 0 0 0 0 0 -0.068 0.040 0.991 0.994 0.000 3106 22 gamma 91 2823 0 0 0 0 0 -0.036 0.112 4.624 4.626 0.000 3107 22 gamma 91 2986 0 0 0 0 0 -0.076 0.110 13.170 13.171 0.000 3108 11 e- 91 2986 0 0 0 0 0 -0.548 0.357 58.663 58.666 0.001 3109 -11 e+ 91 2986 0 0 0 0 0 -0.176 0.117 19.009 19.010 0.001 3110 22 gamma 91 2987 0 0 0 0 0 -0.016 0.003 6.170 6.170 0.000 3111 22 gamma 91 2987 0 0 0 0 0 -0.203 0.438 58.386 58.388 0.000 3112 22 gamma 91 3034 0 0 0 0 0 0.017 -0.001 0.509 0.510 0.000 3113 22 gamma 91 3034 0 0 0 0 0 -0.133 -0.303 4.681 4.693 0.000 3114 22 gamma 91 3066 0 0 0 0 0 0.068 0.077 -0.014 0.103 0.000 3115 22 gamma 91 3066 0 0 0 0 0 -0.067 0.079 -0.012 0.105 0.000 Charge sum: 2.000 Momentum sum: -0.000 0.000 0.000 14000.000 14000.000 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- -------- PYTHIA Event Listing (filtered) --------------------------------------------------------------------------------------- no id name status mothers daughters colours p_x p_y p_z e m 1774 -211 pi- 84 1766 1771 0 0 0 0 -1.241 0.598 1.962 2.401 0.140 1785 -211 pi- 84 1777 1781 0 0 0 0 -3.617 2.123 0.759 4.264 0.140 1918 211 pi+ 83 1900 1916 0 0 0 0 0.484 -0.905 5.625 5.720 0.140 1924 -2212 pbar- 83 1900 1916 0 0 0 0 0.430 -1.133 9.604 9.726 0.938 1957 -2212 pbar- 84 1937 1944 0 0 0 0 -1.442 -1.062 -1.735 2.664 0.938 1958 211 pi+ 84 1937 1944 0 0 0 0 -1.469 -0.074 -1.315 1.978 0.140 1994 211 pi+ 83 1982 1992 0 0 0 0 1.777 3.242 36.357 36.544 0.140 1999 -211 pi- 84 1982 1992 0 0 0 0 1.236 0.963 2.928 3.324 0.140 2002 211 pi+ 84 1982 1992 0 0 0 0 1.700 -0.000 2.723 3.213 0.140 2110 321 K+ 83 2074 2107 0 0 0 0 -3.297 2.798 0.727 4.413 0.494 2116 -321 K- 83 2074 2107 0 0 0 0 0.547 1.900 -0.249 2.053 0.494 2120 -321 K- 83 2074 2107 0 0 0 0 -0.019 1.077 -0.485 1.280 0.494 2121 211 pi+ 83 2074 2107 0 0 0 0 -0.363 1.647 -1.044 1.988 0.140 2127 -211 pi- 84 2074 2107 0 0 0 0 7.480 4.987 -9.940 13.404 0.140 2141 -211 pi- 84 2074 2107 0 0 0 0 0.980 1.513 -0.855 2.000 0.140 2175 321 K+ 83 2150 2172 0 0 0 0 -0.073 1.090 -2.815 3.060 0.494 2182 2212 p+ 83 2150 2172 0 0 0 0 0.447 -0.916 -1.877 2.333 0.938 2193 211 pi+ 83 2150 2172 0 0 0 0 -2.043 0.764 -1.493 2.647 0.140 2200 -211 pi- 84 2150 2172 0 0 0 0 -1.774 -4.053 2.647 5.158 0.140 2201 -2212 pbar- 84 2150 2172 0 0 0 0 -8.616 -16.252 12.018 21.992 0.938 2202 211 pi+ 84 2150 2172 0 0 0 0 -3.552 -6.057 4.109 8.137 0.140 2205 -211 pi- 84 2150 2172 0 0 0 0 -2.037 -4.680 2.647 5.752 0.140 2315 321 K+ 91 1758 0 0 0 0 0 1.448 0.909 -10.404 10.555 0.494 2319 211 pi+ 91 1772 0 0 0 0 0 -0.986 0.741 4.617 4.781 0.140 2320 -211 pi- 91 1772 0 0 0 0 0 -0.461 1.354 4.166 4.407 0.140 2321 211 pi+ 91 1776 0 0 0 0 0 -1.112 0.940 3.378 3.681 0.140 2323 211 pi+ 91 1786 0 0 0 0 0 -3.612 3.167 -0.271 4.813 0.140 2339 211 pi+ 91 1836 0 0 0 0 0 -0.836 -1.755 1.199 2.288 0.140 2362 211 pi+ 91 1888 0 0 0 0 0 -1.047 0.330 4.484 4.618 0.140 2364 211 pi+ 91 1889 0 0 0 0 0 -0.536 -1.163 11.169 11.243 0.140 2374 -211 pi- 91 1917 0 0 0 0 0 1.471 -0.134 7.863 8.002 0.140 2393 211 pi+ 91 1960 0 0 0 0 0 -1.189 0.182 -0.898 1.508 0.140 2404 -211 pi- 91 1995 0 0 0 0 0 0.993 0.260 5.815 5.907 0.140 2415 -211 pi- 91 2005 0 0 0 0 0 1.007 -0.228 -3.516 3.667 0.140 2446 211 pi+ 91 2067 0 0 0 0 0 0.005 1.028 9.860 9.914 0.140 2453 -211 pi- 91 2109 0 0 0 0 0 -3.443 2.581 0.912 4.401 0.140 2456 211 pi+ 91 2114 0 0 0 0 0 -0.209 1.487 0.164 1.516 0.140 2458 321 K+ 91 2115 0 0 0 0 0 0.009 1.524 -0.202 1.615 0.494 2460 211 pi+ 91 2117 0 0 0 0 0 0.327 2.159 -0.734 2.308 0.140 2464 2212 p+ 91 2129 0 0 0 0 0 13.718 9.168 -20.409 26.261 0.938 2465 211 pi+ 91 2129 0 0 0 0 0 1.195 0.781 -1.528 2.096 0.140 2466 -211 pi- 91 2130 0 0 0 0 0 1.014 0.523 -1.404 1.815 0.140 2470 -211 pi- 91 2135 0 0 0 0 0 4.106 3.864 -4.551 7.248 0.140 2472 211 pi+ 91 2136 0 0 0 0 0 1.559 1.556 -1.765 2.826 0.140 2474 211 pi+ 91 2139 0 0 0 0 0 3.127 3.849 -4.597 6.763 0.140 2476 211 pi+ 91 2140 0 0 0 0 0 0.924 1.085 -0.764 1.623 0.140 2478 211 pi+ 91 2142 0 0 0 0 0 0.990 2.123 -1.505 2.788 0.140 2480 321 K+ 91 2143 0 0 0 0 0 0.141 1.111 0.209 1.242 0.494 2484 -211 pi- 91 2146 0 0 0 0 0 -0.752 0.940 -2.828 3.076 0.140 2486 -211 pi- 91 2147 0 0 0 0 0 0.710 0.978 -5.420 5.555 0.140 2492 211 pi+ 91 2177 0 0 0 0 0 1.273 -0.192 -7.390 7.503 0.140 2507 -211 pi- 91 2191 0 0 0 0 0 -0.868 0.730 -0.515 1.253 0.140 2512 -321 K- 91 2197 0 0 0 0 0 -0.662 -1.063 0.350 1.391 0.494 2516 2212 p+ 91 2199 0 0 0 0 0 -6.022 -10.955 8.293 15.031 0.938 2518 211 pi+ 91 2203 0 0 0 0 0 -10.921 -22.498 15.225 29.279 0.140 2519 -211 pi- 91 2203 0 0 0 0 0 -6.065 -12.010 9.121 16.255 0.140 2520 211 pi+ 91 2207 0 0 0 0 0 -0.962 -2.422 0.968 2.784 0.140 2521 -211 pi- 91 2207 0 0 0 0 0 -1.844 -4.495 2.883 5.651 0.140 2522 211 pi+ 91 2242 0 0 0 0 0 -0.799 -0.701 3.208 3.383 0.140 2524 321 K+ 91 2246 0 0 0 0 0 -2.702 -1.177 15.948 16.226 0.494 2606 211 pi+ 91 1764 0 0 0 0 0 -1.015 -0.051 0.528 1.154 0.140 2742 -211 pi- 91 2068 0 0 0 0 0 0.229 1.484 12.617 12.707 0.140 2762 211 pi+ 91 2132 0 0 0 0 0 1.345 1.349 -2.231 2.937 0.140 2763 -211 pi- 91 2132 0 0 0 0 0 1.257 0.817 -1.401 2.056 0.140 2767 211 pi+ 91 2134 0 0 0 0 0 0.975 1.005 -1.714 2.217 0.140 2768 -211 pi- 91 2134 0 0 0 0 0 1.202 0.697 -1.634 2.150 0.140 2782 211 pi+ 91 2204 0 0 0 0 0 -0.266 -1.112 0.551 1.277 0.140 2783 -211 pi- 91 2204 0 0 0 0 0 -1.232 -2.704 1.820 3.488 0.140 2816 211 pi+ 91 2291 0 0 0 0 0 1.039 -0.324 -1.693 2.018 0.140 2817 -211 pi- 91 2291 0 0 0 0 0 0.977 -0.294 -1.009 1.442 0.140 2824 211 pi+ 91 2312 0 0 0 0 0 1.129 0.610 -11.676 11.747 0.140 2825 -211 pi- 91 2312 0 0 0 0 0 2.113 1.158 -17.364 17.531 0.140 2842 211 pi+ 91 2342 0 0 0 0 0 -1.474 -0.858 0.129 1.716 0.140 3010 211 pi+ 91 2642 0 0 0 0 0 -0.291 -1.554 1.735 2.351 0.140 3011 -211 pi- 91 2642 0 0 0 0 0 -0.016 -2.402 3.040 3.877 0.140 3013 -211 pi- 91 2644 0 0 0 0 0 -0.438 -0.974 1.615 1.942 0.140 -------- End PYTHIA Event Listing ----------------------------------------------------------------------------------------------- PYTHIA Warning in SpaceShower::pT2nextQCD: weight above unity PYTHIA Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame *------- PYTHIA Event and Cross Section Statistics -------------------------------------------------------------* | | | Subprocess Code | Number of events | sigma +- delta | | | Tried Selected Accepted | (estimated) (mb) | | | | | |-----------------------------------------------------------------------------------------------------------------| | | | | | g g -> g g 111 | 320 37 37 | 7.072e-04 5.376e-05 | | g g -> q qbar (uds) 112 | 1 0 0 | 0.000e+00 0.000e+00 | | q g -> q g 113 | 463 51 51 | 6.500e-04 5.345e-05 | | q q(bar)' -> q q(bar)' 114 | 73 12 12 | 9.137e-05 1.667e-05 | | q qbar -> g g 115 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar -> q' qbar' (uds) 116 | 2 0 0 | 0.000e+00 0.000e+00 | | g g -> c cbar 121 | 0 0 0 | 0.000e+00 0.000e+00 | | q qbar -> c cbar 122 | 0 0 0 | 0.000e+00 0.000e+00 | | g g -> b bbar 123 | 1 0 0 | 0.000e+00 0.000e+00 | | q qbar -> b bbar 124 | 0 0 0 | 0.000e+00 0.000e+00 | | | | | | sum | 860 100 100 | 1.449e-03 7.762e-05 | | | *------- End PYTHIA Event and Cross Section Statistics ----------------------------------------------------------* *------- PYTHIA Error and Warning Messages Statistics ----------------------------------------------------------* | | | times message | | | | 1 Warning in SpaceShower::pT2nextQCD: weight above unity | | 1 Warning in StringFragmentation::fragmentToJunction: bad convergence junction rest frame | | | *------- End PYTHIA Error and Warning Messages Statistics ------------------------------------------------------* 2013-09-20 16:05 selected charged multiplicity 8.10*10^ 0 7 7.80*10^ 0 X 7.50*10^ 0 X 7.20*10^ 0 X 6.90*10^ 0 X 6.60*10^ 0 X 6.30*10^ 0 X 6.00*10^ 0 X X X 5.70*10^ 0 X X X 5.40*10^ 0 X X X 5.10*10^ 0 X X7 7X 7 4.80*10^ 0 X XX XX X 4.50*10^ 0 X XX XX X 4.20*10^ 0 3X XX 3XX3 33 X33 3.90*10^ 0 XX XX XXXX XX XXX 3.60*10^ 0 XX XX XXXX XX XXX 3.30*10^ 0 XX XX XXXX XX XXX 3.00*10^ 0 XX XXXXXXX XXXXXXXXX X 2.70*10^ 0 XX XXXXXXX XXXXXXXXX X 2.40*10^ 0 XX XXXXXXX XXXXXXXXX X 2.10*10^ 0 7 77 XX XXXXXXX XXXXXXXXX X 1.80*10^ 0 X XX XX XXXXXXX XXXXXXXXX X 1.50*10^ 0 X XX XX XXXXXXX XXXXXXXXX X 1.20*10^ 0 3 33 33X XX3XX XXXXXXX3XXXXXXXXX33X 3 33 3 0.90*10^ 0 X XX XXX XXXXX XXXXXXXXXXXXXXXXXXXX X XX X 0.60*10^ 0 X XX XXX XXXXX XXXXXXXXXXXXXXXXXXXX X XX X 0.30*10^ 0 X XX XXX XXXXX XXXXXXXXXXXXXXXXXXXX X XX X Contents *10^ 0 0000101101120221460853456413443354431130101101000000000000000000000000000000000000000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^-3 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge - *10^ 2 0000000000000000000000000000000000000000000000000011111111111111111111111111111111111111111111111111 *10^ 1 0000011111222223333344444555556666677777888889999900000111112222233333444445555566666777778888899999 *10^ 0 1246802468024680246802468024680246802468024680246802468024680246802468024680246802468024680246802468 Entries = 100 Mean = 4.9760e+01 Underflow = 0.0000e+00 Low edge = -5.0000e-01 All chan = 1.0000e+02 Rms = 1.7061e+01 Overflow = 0.0000e+00 High edge = 1.9950e+02 2013-09-20 16:05 selected charged eta distribution 1.50*10^ 2 4 1.45*10^ 2 X 1.40*10^ 2 X 1.35*10^ 2 X 1.30*10^ 2 6X 2 1.25*10^ 2 XX X2 1.20*10^ 2 8 XX8 XX8 1.15*10^ 2 X 4 XXX2XXX 1.10*10^ 2 68 X 2X 6XXXXXXX 1.05*10^ 2 XX44 X XX6 4 XXXXXXXX 1.00*10^ 2 XXXX X XXX XX XXXXXXXX 0.95*10^ 2 6 XXXX8X XXX8 XX XXXXXXXX 0.90*10^ 2 X4 XXXXXX8XXXX XXXXXXXXXXX 4 0.85*10^ 2 XX 8 4XXXXXXXXXXX8 4XXXXXXXXXXX X 6 2 0.80*10^ 2 XX 24X4XXXXXXXXXXXXX XXXXXXXXXXXX X X 2X 0.75*10^ 2 4 4XX XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX X46488X XX 0.70*10^ 2 X XXX4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXX2XXXXXXX XX 0.65*10^ 2 6X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 6XXX 0.60*10^ 2 XX6XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 2 0.55*10^ 2 6 8XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX62X 4 0.50*10^ 2 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX4X 0.45*10^ 2 X XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.40*10^ 2 X66 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.35*10^ 2 XXX4XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.30*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.25*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.20*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.15*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.10*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX 0.05*10^ 2 XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX Contents *10^ 2 0000000000000000000000000000000000000111101011100001101111111100000000000000000000000000000000000000 *10^ 1 0000000000000000000053335675798677878000091801098780090241122168777778666785554500000000000000000000 *10^ 0 0000000000000000000038824328237767472892249962344520208879161967232443035613167200000000000000000000 *10^-1 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Low edge -------------------------------------------------- *10^ 0 5444444444433333333332222222222111111111100000000000000000001111111111222222222233333333334444444444 *10^-1 0987654321098765432109876543210987654321098765432101234567890123456789012345678901234567890123456789 *10^-2 0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 Entries = 4978 Mean = 2.8626e-02 Underflow = 0.0000e+00 Low edge = -5.0000e+00 All chan = 4.9780e+03 Rms = 1.5341e+00 Overflow = 0.0000e+00 High edge = 5.0000e+00 2013-09-20 16:05 selected charged pT distribution 1.62*10^ 3 4 1.56*10^ 3 X 1.50*10^ 3 X 1.44*10^ 3 X 1.38*10^ 3 X 1.32*10^ 3 X 1.26*10^ 3 X 1.20*10^ 3 X 1.14*10^ 3 X 1.08*10^ 3 X 1.02*10^ 3 X 0.96*10^ 3 X 0.90*10^ 3 X 0.84*10^ 3 X3 0.78*10^ 3 XX 0.72*10^ 3 XX 0.66*10^ 3 XX 0.60*10^ 3 XX 0.54*10^ 3 XX4 0.48*10^ 3 XXX 0.42*10^ 3 XXX2 0.36*10^ 3 XXXX 0.30*10^ 3 XXXX5 0.24*10^ 3 XXXXX 0.18*10^ 3 XXXXXX85 0.12*10^ 3 XXXXXXXX6721 0.06*10^ 3 XXXXXXXXXXXX9885654323342332122112111111111 1 11 1 1 1 11 1 1 Contents *10^ 3 0010000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 2 0057532111010000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 *10^ 1 0089067765907654423322111211110110010000000000000000000000000000000000000000000000000000000000000000 *10^ 0 0056692991542435796120168626537026536745853552525322426011240121451321112022113002022000101001100021 Low edge *10^ 1 0000000000000000000011111111111111111111222222222222222222223333333333333333333344444444444444444444 *10^ 0 0011223344556677889900112233445566778899001122334455667788990011223344556677889900112233445566778899 *10^-1 0505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505050505 Entries = 4978 Mean = 3.8763e+00 Underflow = 0.0000e+00 Low edge = 0.0000e+00 All chan = 4.9600e+03 Rms = 5.1252e+00 Overflow = 1.8000e+01 High edge = 5.0000e+01 pythia8-8.1.80.orig/examples/main04.cc0000644000175000017500000002034612217346163015560 0ustar sunsun// main04.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how to generate and study "total cross section" processes, // i.e. elastic, single and double diffractive, and the "minimum-bias" rest. // All input is specified in the main06.cmnd file. // Note that the "total" cross section does NOT include // the Coulomb contribution to elastic scattering, as switched on here. #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== int main() { // Generator. Shorthand for the event. Pythia pythia; Event& event = pythia.event; // Read in commands from external file. pythia.readFile("main04.cmnd"); // Extract settings to be used in the main program. int nEvent = pythia.mode("Main:numberOfEvents"); int nAbort = pythia.mode("Main:timesAllowErrors"); // Initialize. pythia.init(); // Book histograms: multiplicities and mean transverse momenta. Hist yChg("rapidity of charged particles; all", 100, -10., 10.); Hist nChg("number of charged particles; all", 100, -0.5, 799.5); Hist nChgSD("number of charged particles; single diffraction", 100, -0.5, 799.5); Hist nChgDD("number of charged particles, double diffractive", 100, -0.5, 799.5); Hist nChgCD("number of charged particles, central diffractive", 100, -0.5, 799.5); Hist nChgND("number of charged particles, non-diffractive", 100, -0.5, 799.5); Hist pTnChg("(n_charged) all", 100, -0.5, 799.5); Hist pTnChgSD("(n_charged) single diffraction", 100, -0.5, 799.5); Hist pTnChgDD("(n_charged) double diffraction", 100, -0.5, 799.5); Hist pTnChgCD("(n_charged) central diffraction", 100, -0.5, 799.5); Hist pTnChgND("(n_charged) non-diffractive ", 100, -0.5, 799.5); // Book histograms: ditto as function of separate subsystem mass. Hist mLogInel("log10(mass), by diffractive system", 100, 0., 5.); Hist nChgmLog("(log10(mass))", 100, 0., 5.); Hist pTmLog("_charged>(log10(mass))", 100, 0., 5.); // Book histograms: elastic/diffractive. Hist tSpecEl("elastic |t| spectrum", 100, 0., 1.); Hist tSpecElLog("elastic log10(|t|) spectrum", 100, -5., 0.); Hist tSpecSD("single diffractive |t| spectrum", 100, 0., 2.); Hist tSpecDD("double diffractive |t| spectrum", 100, 0., 5.); Hist tSpecCD("central diffractive |t| spectrum", 100, 0., 5.); Hist mSpec("diffractive mass spectrum", 100, 0., 100.); Hist mLogSpec("log10(diffractive mass spectrum)", 100, 0., 4.); // Book histograms: inelastic nondiffractive. double pTmax = 20.; double bMax = 4.; Hist pTspec("total pT_hard spectrum", 100, 0., pTmax); Hist pTspecND("nondiffractive pT_hard spectrum", 100, 0., pTmax); Hist bSpec("b impact parameter spectrum", 100, 0., bMax); Hist enhanceSpec("b enhancement spectrum", 100, 0., 10.); Hist number("number of interactions", 100, -0.5, 99.5); Hist pTb1("pT spectrum for b < 0.5", 100, 0., pTmax); Hist pTb2("pT spectrum for 0.5 < b < 1", 100, 0., pTmax); Hist pTb3("pT spectrum for 1 < b < 1.5", 100, 0., pTmax); Hist pTb4("pT spectrum for 1.5 < b", 100, 0., pTmax); Hist bpT1("b spectrum for pT < 2", 100, 0., bMax); Hist bpT2("b spectrum for 2 < pT < 5", 100, 0., bMax); Hist bpT3("b spectrum for 5 < pT < 15", 100, 0., bMax); Hist bpT4("b spectrum for 15 < pT", 100, 0., bMax); // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if too many failures. if (!pythia.next()) { if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Extract event classification. int code = pythia.info.code(); // Charged multiplicity and mean pT: all and by event class. int nch = 0; double pTsum = 0.; for (int i = 1; i < event.size(); ++i) if (event[i].isFinal() && event[i].isCharged()) { yChg.fill( event[i].y() ); ++nch; pTsum += event[i].pT(); } nChg.fill( nch ); if (nch > 0) pTnChg.fill( nch, pTsum/nch); if (code == 103 || code == 104) { nChgSD.fill( nch ); if (nch > 0) pTnChgSD.fill( nch, pTsum/nch); } else if (code == 105) { nChgDD.fill( nch ); if (nch > 0) pTnChgDD.fill( nch, pTsum/nch); } else if (code == 106) { nChgCD.fill( nch ); if (nch > 0) pTnChgCD.fill( nch, pTsum/nch); } else if (code == 101) { nChgND.fill( nch ); if (nch > 0) pTnChgND.fill( nch, pTsum/nch); double mLog = log10( event[0].m() ); mLogInel.fill( mLog ); nChgmLog.fill( mLog, nch ); if (nch > 0) pTmLog.fill( mLog, pTsum / nch ); } // Charged multiplicity and mean pT: per diffractive system. for (int iDiff = 0; iDiff < 3; ++iDiff) if ( (iDiff == 0 && pythia.info.isDiffractiveA()) || (iDiff == 1 && pythia.info.isDiffractiveB()) || (iDiff == 2 && pythia.info.isDiffractiveC()) ) { int ndiff = 0; double pTdiff = 0.; int nDoc = (iDiff < 2) ? 4 : 5; for (int i = nDoc + 1; i < event.size(); ++i) if (event[i].isFinal() && event[i].isCharged()) { // Trace back final particle to see which system it comes from. int k = i; do k = event[k].mother1(); while (k > nDoc); if (k == iDiff + 3) { ++ndiff; pTdiff += event[i].pT(); } } // Study diffractive mass spectrum. double mDiff = event[iDiff+3].m(); double mLog = log10( mDiff); mLogInel.fill( mLog ); nChgmLog.fill( mLog, ndiff ); if (ndiff > 0) pTmLog.fill( mLog, pTdiff / ndiff ); mSpec.fill( mDiff ); mLogSpec.fill( mLog ); } // Study pT spectrum of all hard collisions, no distinction. double pT = pythia.info.pTHat(); pTspec.fill( pT ); // Study t distribution of elastic/diffractive events. if (code > 101) { double tAbs = abs(pythia.info.tHat()); if (code == 102) { tSpecEl.fill(tAbs); tSpecElLog.fill(log10(tAbs)); } else if (code == 103 || code == 104) tSpecSD.fill(tAbs); else if (code == 105) tSpecDD.fill(tAbs); else if (code == 106) { double t1Abs = abs( (event[3].p() - event[1].p()).m2Calc() ); double t2Abs = abs( (event[4].p() - event[2].p()).m2Calc() ); tSpecCD.fill(t1Abs); tSpecCD.fill(t2Abs); } // Study nondiffractive inelastic events in (pT, b) space. } else { double b = pythia.info.bMPI(); double enhance = pythia.info.enhanceMPI(); int nMPI = pythia.info.nMPI(); pTspecND.fill( pT ); bSpec.fill( b ); enhanceSpec.fill( enhance ); number.fill( nMPI ); if (b < 0.5) pTb1.fill( pT ); else if (b < 1.0) pTb2.fill( pT ); else if (b < 1.5) pTb3.fill( pT ); else pTb4.fill( pT ); if (pT < 2.) bpT1.fill( b ); else if (pT < 5.) bpT2.fill( b ); else if (pT < 15.) bpT3.fill( b ); else bpT4.fill( b ); } // End of event loop. } // Final statistics and histograms. pythia.stat(); pTnChg /= nChg; pTnChgSD /= nChgSD; pTnChgDD /= nChgDD; pTnChgCD /= nChgCD; pTnChgND /= nChgND; nChgmLog /= mLogInel; pTmLog /= mLogInel; cout << yChg << nChg << nChgSD << nChgDD << nChgCD << nChgND << pTnChg << pTnChgSD << pTnChgDD << pTnChgCD << pTnChgND << mLogInel << nChgmLog << pTmLog << tSpecEl << tSpecElLog << tSpecSD << tSpecDD << tSpecCD << mSpec << mLogSpec << pTspec << pTspecND << bSpec << enhanceSpec << number << pTb1 << pTb2 << pTb3 << pTb4 << bpT1 << bpT2 << bpT3 << bpT4; // Done. return 0; } pythia8-8.1.80.orig/examples/main08.cmnd0000644000175000017500000000136512217346164016121 0ustar sunsun! File: main08.cmnd ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! Names are case-insensitive - but spellings-sensitive! ! The changes here are illustrative, not always physics-motivated. ! The current file is input for subruns with consecutive pT ranges. Main:numberOfSubruns = 5 Main:subrun = 0 PhaseSpace:pTHatMin = 100. PhaseSpace:pTHatMax = 150. Main:subrun = 1 PhaseSpace:pTHatMin = 150. PhaseSpace:pTHatMax = 250. Main:subrun = 2 PhaseSpace:pTHatMin = 250. PhaseSpace:pTHatMax = 400. Main:subrun = 3 PhaseSpace:pTHatMin = 400. PhaseSpace:pTHatMax = 600. Main:subrun = 4 PhaseSpace:pTHatMin = 600. PhaseSpace:pTHatMax = 0. ! 0. means open-ended pythia8-8.1.80.orig/examples/README0000644000175000017500000001173712217346206015043 0ustar sunsun---------------------------------------------------------------------- BASIC INSTRUCTIONS FOR RUNNING TEST PROGRAMS 1) You are supposed to have already compiled PYTHIA 8, as described in the README file of the mother directory. For the moment we assume that you will NOT use the HepMC, LHAPDF, or FastJet libraries. 2) You are now ready to test run the first thirty of the mainNN examples, see the manual page "Sample main program" for details. Type "gmake mainNN" to build an executable "mainNN.exe". Type "./mainNN.exe > output" to run this executable. Then study the output file. The existing files outNN are examples of possible outputs from several runs, so that you can compare. 3) If you want to run your own programs from this directory you can edit the "Makefile", adding the name of your main program to the already existing ones. Note that different cases exist, depending on which external libraries are to be linked. There is no main00, but this name is defined in the Makefile, so it can be used for simple first tests. 4) With ./runmains all the 27 first mainXX program will be run, plus main31, to get a thorough test of the installation. The runmains file can easily be edited to run the others as well, but then you should first link to the appropriate external libraries. The outref subdirectory contains the output of such a run, if you want to compare with what you obtain. 5) Type "gmake clean" to clean up the examples directory (but not the output files). ---------------------------------------------------------------------- ADVANCED INSTRUCTIONS FOR RUNNING TEST PROGRAMS 1) If you want to be able to run examples linked to HepMC you should already have set that up with the "./configure" command in the mother directory. If not, you can go back and do it now. This will create files "config.csh" and "config.sh" in the current directory. 2) If you are going to run examples linked with LHAPDF and/or FastJet, or if you want to move (all or parts of) the current examples subdirectory to a location separate from the rest of the library, you should as a first step run the script "configure" in the current directory. You can use command-line arguments to set up the desired library links. The possible options are: --help : prints a brief summary of the options described here. --enable-debug : turns on debugging flags and turns off optimization --enable-shared : use shared library (not yet implemented; default no) --lcgplatform=name : LCG platform name (can be part of path to external librtaries; default is x86_64-slc5-gcc43-opt) --with-pythia8=p8path : path to the pythia81xx installation directory, where the programs in this examples directory can find libraries, includes and parameters (default is ..) --with-lhapdf=lhapdfpath : the path to your local copy of the LHAPDF library (must be version 5.3 or higher) --with-lhapdfversion=v : a simpler alternative to the above, valid if you are using the CERN AFS MCGenerators area; then you do not need to specify the full path but only the version, e.g. =5.3.0 (must be version 5.3 or higher) --with-lhapdflibname=n : lhapdf library name line (default is -lLHAPDF) --with-lhapdfsets=path : path to the LHAPDF data files (default is lhapdfpath/../PDFsets, CERN AFS default is lhapdfpath/../../../share/PDFsets) --with-fastjet=path : path to FastJet (default = /usr/local) --with-fastjetversion=v : FastJet version (simplified alternative when using CERN AFS external, e.g. =2.3.3) When "configure" is run it will create or append to the config.csh and config.sh files. 3) Before running the examples using external libraries for the first time, type "source config.csh" if you use the csh or tcsh shell, or "source config.sh" otherwise. (Use "echo $SHELL" if uncertain.) This will set or append the environment variables LD_LIBRARY_PATH, needed to find the HepMC libraries. (Eventually also LHAPDF and FastJet libraries, if shared ones are used. Default, if taken from CERN AFS MCGenerators, is archive.) It will also set the variable LHAPATH, needed to find the LHAPDF data files. 4) If you want to change to other LHAPDF or FastJet or versions, you have to rerun the script "configure" and again "source" one of the config.* files. In case of using shared libraries (these will be taken if both shared and archive ones are on the same path) pay attention to the variable LD_LIBRARY_PATH: subsequent commands "source" will add new items to it, not substitute the old ones. As a result, the wrong version can still be loaded at runtime, which can cause relocation errors. A simple solution is to repeat the "configure" and "source" steps in a new window, i.e. in a new clean copy of the shell. ---------------------------------------------------------------------- pythia8-8.1.80.orig/examples/softsusy.spc0000644000175000017500000001377112217346206016571 0ustar sunsun# SOFTSUSY1.9 # B.C. Allanach, Comput. Phys. Commun. 143 (2002) 305-331, hep-ph/0104145 Block SPINFO # Program information 1 SOFTSUSY # spectrum calculator 2 1.9.1 # version number Block MODSEL # Select model 1 1 # sugra Block SMINPUTS # Standard Model inputs 1 1.27934000e+02 # alpha_em^(-1)(MZ) SM MSbar 2 1.16637000e-05 # G_Fermi 3 1.17200000e-01 # alpha_s(MZ)MSbar 4 9.11876000e+01 # MZ(pole) 5 4.25000000e+00 # Mb(mb) 6 1.74300000e+02 # Mtop(pole) 7 1.77700000e+00 # Mtau(pole) Block MINPAR # SUSY breaking input parameters 3 1.00000000e+01 # tanb 4 1.00000000e+00 # sign(mu) 1 1.00000000e+02 # m0 2 2.50000000e+02 # m12 5 -1.00000000e+02 # A0 # Low energy data in SOFTSUSY: MIXING=-1 TOLERANCE=1.00000000e-03 # mgut=2.45916471e+16 GeV Block MASS # Mass spectrum #PDG code mass particle 24 8.04191121e+01 # MW 25 1.10762378e+02 # h0 35 4.00599584e+02 # H0 36 4.00231463e+02 # A0 37 4.08513284e+02 # H+ 1000001 5.72700955e+02 # ~d_L 1000002 5.67251814e+02 # ~u_L 1000003 5.72700955e+02 # ~s_L 1000004 5.67251814e+02 # ~c_L 1000005 5.15211952e+02 # ~b_1 1000006 3.95920984e+02 # ~t_1 1000011 2.04276615e+02 # ~e_L 1000012 1.88657729e+02 # ~nue_L 1000013 2.04276615e+02 # ~mu_L 1000014 1.88657729e+02 # ~numu_L 1000015 1.36227147e+02 # ~stau_1 1000016 1.87773326e+02 # ~nu_tau_L 1000021 6.07604198e+02 # ~g 1000022 9.72852615e+01 # ~neutralino(1) 1000023 1.80961862e+02 # ~neutralino(2) 1000024 1.80378828e+02 # ~chargino(1) 1000025 -3.64435115e+02 # ~neutralino(3) 1000035 3.83135773e+02 # ~neutralino(4) 1000037 3.83371870e+02 # ~chargino(2) 2000001 5.46070490e+02 # ~d_R 2000002 5.46999685e+02 # ~u_R 2000003 5.46070490e+02 # ~s_R 2000004 5.46999685e+02 # ~c_R 2000005 5.43966766e+02 # ~b_2 2000006 5.85698733e+02 # ~t_2 2000011 1.45526717e+02 # ~e_R 2000013 1.45526717e+02 # ~mu_R 2000015 2.08222793e+02 # ~stau_2 # Higgs mixing Block alpha # Effective Higgs mixing parameter -1.13732831e-01 # alpha Block stopmix # stop mixing matrix 1 1 5.38083886e-01 # O_{11} 1 2 8.42891293e-01 # O_{12} 2 1 8.42891293e-01 # O_{21} 2 2 -5.38083886e-01 # O_{22} Block sbotmix # sbottom mixing matrix 1 1 9.47744273e-01 # O_{11} 1 2 3.19031021e-01 # O_{12} 2 1 -3.19031021e-01 # O_{21} 2 2 9.47744273e-01 # O_{22} Block staumix # stau mixing matrix 1 1 2.80956141e-01 # O_{11} 1 2 9.59720609e-01 # O_{12} 2 1 9.59720609e-01 # O_{21} 2 2 -2.80956141e-01 # O_{22} Block nmix # neutralino mixing matrix 1 1 9.86066377e-01 # N_{1,1} 1 2 -5.46292061e-02 # N_{1,2} 1 3 1.47649927e-01 # N_{1,3} 1 4 -5.37424305e-02 # N_{1,4} 2 1 1.02062420e-01 # N_{2,1} 2 2 9.42721210e-01 # N_{2,2} 2 3 -2.74985600e-01 # N_{2,3} 2 4 1.58880154e-01 # N_{2,4} 3 1 -6.04575099e-02 # N_{3,1} 3 2 8.97030908e-02 # N_{3,2} 3 3 6.95501068e-01 # N_{3,3} 3 4 7.10335491e-01 # N_{3,4} 4 1 -1.16624405e-01 # N_{4,1} 4 2 3.16616055e-01 # N_{4,2} 4 3 6.47194471e-01 # N_{4,3} 4 4 -6.83587843e-01 # N_{4,4} Block Umix # chargino U mixing matrix 1 1 9.15531658e-01 # U_{1,1} 1 2 -4.02245924e-01 # U_{1,2} 2 1 4.02245924e-01 # U_{2,1} 2 2 9.15531658e-01 # U_{2,2} Block Vmix # chargino V mixing matrix 1 1 9.72345994e-01 # V_{1,1} 1 2 -2.33545003e-01 # V_{1,2} 2 1 2.33545003e-01 # V_{2,1} 2 2 9.72345994e-01 # V_{2,2} Block gauge Q= 4.64231969e+02 1 3.60968173e-01 # g'(Q)MSSM DRbar 2 6.46474399e-01 # g(Q)MSSM DRbar 3 1.09626470e+00 # g3(Q)MSSM DRbar Block yu Q= 4.64231969e+02 3 3 8.89731484e-01 # Yt(Q)MSSM DRbar Block yd Q= 4.64231969e+02 3 3 1.39732269e-01 # Yb(Q)MSSM DRbar Block ye Q= 4.64231969e+02 3 3 1.00914051e-01 # Ytau(Q)MSSM DRbar Block hmix Q= 4.64231969e+02 # Higgs mixing parameters 1 3.58339654e+02 # mu(Q)MSSM DRbar 2 9.75145219e+00 # tan beta(Q)MSSM DRbar 3 2.44923803e+02 # higgs vev(Q)MSSM DRbar 4 1.67100152e+05 # mA^2(Q)MSSM DRbar Block msoft Q=4.64231969e+02 # MSSM DRbar SUSY breaking parameters 1 1.01439997e+02 # M_1(Q) 2 1.91579315e+02 # M_2(Q) 3 5.86586195e+02 # M_3(Q) 21 3.23914077e+04 # mH1^2(Q) 22 -1.29413007e+05 # mH2^2(Q) 31 1.99042560e+02 # meL(Q) 32 1.99042560e+02 # mmuL(Q) 33 1.98204510e+02 # mtauL(Q) 34 1.38811933e+02 # meR(Q) 35 1.38811933e+02 # mmuR(Q) 36 1.36392545e+02 # mtauR(Q) 41 5.50815976e+02 # mqL1(Q) 42 5.50815976e+02 # mqL2(Q) 43 4.99361608e+02 # mqL3(Q) 44 5.28861326e+02 # muR(Q) 45 5.28861326e+02 # mcR(Q) 46 4.18454191e+02 # mtR(Q) 47 5.26100270e+02 # mdR(Q) 48 5.26100270e+02 # msR(Q) 49 5.22780488e+02 # mbR(Q) Block au Q= 4.64231969e+02 1 1 0.00000000e+00 # Au(Q)MSSM DRbar 2 2 0.00000000e+00 # Ac(Q)MSSM DRbar 3 3 -5.04520155e+02 # At(Q)MSSM DRbar Block ad Q= 4.64231969e+02 1 1 0.00000000e+00 # Ad(Q)MSSM DRbar 2 2 0.00000000e+00 # As(Q)MSSM DRbar 3 3 -7.97104366e+02 # Ab(Q)MSSM DRbar Block ae Q= 4.64231969e+02 1 1 0.00000000e+00 # Ae(Q)MSSM DRbar 2 2 0.00000000e+00 # Amu(Q)MSSM DRbar 3 3 -2.56146632e+02 # Atau(Q)MSSM DRbar pythia8-8.1.80.orig/examples/main26.cc0000644000175000017500000001672512217346165015574 0ustar sunsun// main26.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a test program for the extra dimensions processes. // Author: Stefan Ask (Stefan DOT Ask AT cern DOT ch) // Documentation: S. Ask et al., arXiv:0809.4750 and arXiv:0912.4233 #include "Pythia8/Pythia.h" using namespace Pythia8; // The main program. int main() { // Test cases // 1 = Jet + G (real G emission) // 2 = Jet + U (real U emission) // 3 = Z + G (real G emission) // 4 = Z + U (real U emission) // 5 = gamma gamma (LED G* exchange) // 6 = l lbar (LED U* exchange). // Note: charged leptons only! // 7 = Z_KK/gamma_KK (TEV ED resonance) // 8 = G* (RS resonance, SM on the TeV brane) // 9 = kk-gluon* (RS resonance) int nTest = 1; // Number of events to generate. Max number of errors. int nEvent = 1000; int nAbort = 50; // Pythia generator. Pythia pythia; // PYTHIA paramters: pythia.readString("PhaseSpace:showViolation = off"); // Test case parameters if (nTest == 1) { pythia.readString("ExtraDimensionsLED:monojet = on"); pythia.readString("ExtraDimensionsLED:n = 4"); pythia.readString("ExtraDimensionsLED:MD = 4000."); pythia.readString("ExtraDimensionsLED:CutOffmode = 3"); pythia.readString("ExtraDimensionsLED:t = 2"); pythia.readString("5000039:m0 = 2500."); pythia.readString("5000039:mWidth = 1500."); pythia.readString("5000039:mMin = 1."); pythia.readString("5000039:mMax = 13990."); pythia.readString("PhaseSpace:pTHatMin = 700."); } else if (nTest == 2){ pythia.readString("ExtraDimensionsUnpart:gg2Ug = off"); pythia.readString("ExtraDimensionsUnpart:qg2Uq = on"); pythia.readString("ExtraDimensionsUnpart:qqbar2Ug = on"); pythia.readString("ExtraDimensionsUnpart:spinU = 1"); pythia.readString("ExtraDimensionsUnpart:dU = 1.2"); pythia.readString("ExtraDimensionsUnpart:LambdaU = 1000"); pythia.readString("ExtraDimensionsUnpart:lambda = 1.0"); pythia.readString("ExtraDimensionsUnpart:CutOffmode = 0"); pythia.readString("5000039:m0 = 300."); pythia.readString("5000039:mWidth = 500."); pythia.readString("5000039:mMin = 1."); pythia.readString("5000039:mMax = 13990."); pythia.readString("PhaseSpace:pTHatMin = 700."); } else if (nTest == 3){ pythia.readString("ExtraDimensionsLED:ffbar2GZ = on"); pythia.readString("ExtraDimensionsLED:n = 6"); pythia.readString("ExtraDimensionsLED:MD = 2000."); pythia.readString("ExtraDimensionsLED:CutOffmode = 1"); pythia.readString("5000039:m0 = 3000."); pythia.readString("5000039:mWidth = 1500."); pythia.readString("5000039:mMin = 1."); pythia.readString("5000039:mMax = 13990."); pythia.readString("PhaseSpace:pTHatMin = 50."); } else if (nTest == 4){ pythia.readString("ExtraDimensionsUnpart:ffbar2UZ = on"); pythia.readString("ExtraDimensionsUnpart:spinU = 1"); pythia.readString("ExtraDimensionsUnpart:dU = 2.0"); pythia.readString("ExtraDimensionsUnpart:LambdaU = 1000"); pythia.readString("ExtraDimensionsUnpart:lambda = 1.000"); pythia.readString("ExtraDimensionsUnpart:CutOffmode = 0"); pythia.readString("5000039:m0 = 500."); pythia.readString("5000039:mWidth = 1000."); pythia.readString("5000039:mMin = 1."); pythia.readString("5000039:mMax = 13990."); pythia.readString("PhaseSpace:pTHatMin = 50."); } else if (nTest == 5){ pythia.readString("ExtraDimensionsLED:ffbar2gammagamma = on"); pythia.readString("ExtraDimensionsLED:gg2gammagamma = on"); pythia.readString("ExtraDimensionsLED:LambdaT = 3300."); pythia.readString("PhaseSpace:mHatMin = 800."); } else if (nTest == 6){ pythia.readString("ExtraDimensionsUnpart:ffbar2llbar = on"); pythia.readString("ExtraDimensionsUnpart:gg2llbar = off"); pythia.readString("ExtraDimensionsUnpart:spinU = 1"); pythia.readString("ExtraDimensionsUnpart:dU = 1.3"); pythia.readString("ExtraDimensionsUnpart:LambdaU = 1000"); pythia.readString("ExtraDimensionsUnpart:lambda = 1.0"); pythia.readString("ExtraDimensionsUnpart:gXX = 0"); pythia.readString("ExtraDimensionsUnpart:gXY = 0"); pythia.readString("PhaseSpace:mHatMin = 300."); } else if (nTest == 7){ pythia.readString("ExtraDimensionsTEV:ffbar2mu+mu- = on"); pythia.readString("ExtraDimensionsTEV:gmZmode = 3"); pythia.readString("ExtraDimensionsTEV:nMax = 100"); pythia.readString("ExtraDimensionsTEV:mStar = 4000"); pythia.readString("PhaseSpace:mHatMin = 1000"); pythia.readString("PhaseSpace:mHatMax = 6000"); pythia.readString("5000023:isResonance = false"); } else if (nTest == 8){ pythia.readString("ExtraDimensionsG*:all = on"); } else if (nTest == 9){ pythia.readString("ExtraDimensionsG*:qqbar2KKgluon* = on"); pythia.readString("ExtraDimensionsG*:KKintMode = 2"); pythia.readString("ExtraDimensionsG*:KKgqR = -0.2"); pythia.readString("ExtraDimensionsG*:KKgqL = -0.2"); pythia.readString("ExtraDimensionsG*:KKgbR = -0.2"); pythia.readString("ExtraDimensionsG*:KKgbL = 1.0"); pythia.readString("ExtraDimensionsG*:KKgtR = 5.0"); pythia.readString("ExtraDimensionsG*:KKgtL = 1.0"); pythia.readString("5100021:m0 = 2000"); } // Switch off sophisticated tau treatment: not yet matched to SUSY. pythia.readString("ParticleDecays:sophisticatedTau = 0"); // Initialization for LHC. pythia.readString("Beams:eCM = 14000."); pythia.init(); // Validation histograms Hist hEtjet("dN/dETjet: monojet check", 100, 0., 7000.); Hist hMass("dN/m: graviton mass spectrum", 100, 0., 7000.); // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if many failures. if (!pythia.next()) { if (++iAbort < nAbort) continue; std::cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Checked particle index int tmp_monojet = -1; // Particle loop for (int iPart = 0; iPart < pythia.event.size(); ++iPart) { // From hard process (inital = 21, interm.=22, final=23 state) if (pythia.event[iPart].statusAbs() == 22) { // Find Z_KK/gamma_KK or kk-gluon if( pythia.event[iPart].idAbs() == 5000023 || pythia.event[iPart].idAbs() == 5100021 || pythia.event[iPart].idAbs() == 5100039){ hMass.fill( pythia.event[iPart].m() ); } } else if ( pythia.event[iPart].statusAbs() == 23 ) { // Find graviton/unparticle if( pythia.event[iPart].idAbs() == 5000039){ hMass.fill( pythia.event[iPart].m() ); } // Find mono-jets if (nTest == 1 || nTest == 2) { if ( pythia.event[iPart].idAbs() <= 6 || pythia.event[iPart].idAbs() == 21 ){ if (tmp_monojet >= 0) { std::cout << "More than one (hard process) mono-jet ! \n"; } else { tmp_monojet = iPart; } } } } } // Validation mono-jet wrt G.Giudice et al. paper [hep-ph/9811291v2] if (tmp_monojet >= 0) { double tmp_eta = pythia.event[tmp_monojet].eta(); double tmp_et = pythia.event[tmp_monojet].eT(); double tmp_et_cut = 1000; if ( tmp_et >= tmp_et_cut && abs(tmp_eta) < 3 ) { hEtjet.fill( fabs(tmp_et) ); } } } // Final statistics. pythia.stat(); cout << hMass << hEtjet; return 0; } pythia8-8.1.80.orig/examples/main10.cc0000644000175000017500000001112312217346164015547 0ustar sunsun// main10.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Example how you can use UserHooks to trace pT spectrum through program, // and veto undesirable jet multiplicities. #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // Put histograms here to make them global, so they can be used both // in MyUserHooks and in the main program. Hist pTtrial("trial pT spectrum", 100, 0., 400.); Hist pTselect("selected pT spectrum (before veto)", 100, 0., 400.); Hist pTaccept("accepted pT spectrum (after veto)", 100, 0., 400.); Hist nPartonsB("number of partons before veto", 20, -0.5, 19.5); Hist nJets("number of jets before veto", 20, -0.5, 19.5); Hist nPartonsA("number of partons after veto", 20, -0.5, 19.5); Hist nFSRatISR("number of FSR emissions at first ISR emission", 20, -0.5, 19.5); //========================================================================== // Write own derived UserHooks class. class MyUserHooks : public UserHooks { public: // Constructor creates anti-kT jet finder with (-1, R, pTmin, etaMax). MyUserHooks() { slowJet = new SlowJet(-1, 0.7, 10., 5.); } // Destructor deletes anti-kT jet finder. ~MyUserHooks() {delete slowJet;} // Allow process cross section to be modified... virtual bool canModifySigma() {return true;} // ...which gives access to the event at the trial level, before selection. virtual double multiplySigmaBy(const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool inEvent) { // All events should be 2 -> 2, but kill them if not. if (sigmaProcessPtr->nFinal() != 2) return 0.; // Extract the pT for 2 -> 2 processes in the event generation chain // (inEvent = false for initialization). if (inEvent) { pTHat = phaseSpacePtr->pTHat(); // Fill histogram of pT spectrum. pTtrial.fill( pTHat ); } // Here we do not modify 2 -> 2 cross sections. return 1.; } // Allow a veto for the interleaved evolution in pT. virtual bool canVetoPT() {return true;} // Do the veto test at a pT scale of 5 GeV. virtual double scaleVetoPT() {return 5.;} // Access the event in the interleaved evolution. virtual bool doVetoPT(int iPos, const Event& event) { // iPos <= 3 for interleaved evolution; skip others. if (iPos > 3) return false; // Fill histogram of pT spectrum at this stage. pTselect.fill(pTHat); // Extract a copy of the partons in the hardest system. subEvent(event); nPartonsB.fill( workEvent.size() ); // Find number of jets with given conditions. slowJet->analyze(event); int nJet = slowJet->sizeJet(); nJets.fill( nJet ); // Veto events which do not have exactly three jets. if (nJet != 3) return true; // Statistics of survivors. nPartonsA.fill( workEvent.size() ); pTaccept.fill(pTHat); // Do not veto events that got this far. return false; } // Allow a veto after (by default) first step. virtual bool canVetoStep() {return true;} // Access the event in the interleaved evolution after first step. virtual bool doVetoStep( int iPos, int nISR, int nFSR, const Event& ) { // Only want to study what happens at first ISR emission if (iPos == 2 && nISR == 1) nFSRatISR.fill( nFSR ); // Not intending to veto any events here. return false; } private: // The anti-kT (or kT, C/A) jet finder. SlowJet* slowJet; // Save the pThat scale. double pTHat; }; //========================================================================== int main() { // Generator. Pythia pythia; // Process selection. No need to study hadron level. pythia.readString("HardQCD:all = on"); pythia.readString("PhaseSpace:pTHatMin = 50."); pythia.readString("HadronLevel:all = off"); // Set up to do a user veto and send it in. MyUserHooks* myUserHooks = new MyUserHooks(); pythia.setUserHooksPtr( myUserHooks); // Tevatron initialization. pythia.readString("Beams:idB = -2212"); pythia.readString("Beams:eCM = 1960."); pythia.init(); // Begin event loop. for (int iEvent = 0; iEvent < 1000; ++iEvent) { // Generate events. pythia.next(); // End of event loop. } // Statistics. Histograms. pythia.stat(); cout << pTtrial << pTselect << pTaccept << nPartonsB << nJets << nPartonsA << nFSRatISR; // Done. delete myUserHooks; return 0; } pythia8-8.1.80.orig/examples/main84.cc0000644000175000017500000003353712217346167015602 0ustar sunsun// main84.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This program is written by Stefan Prestel. // It illustrates how to do CKKW-L merging, // see the Matrix Element Merging page in the online manual. #include #include "Pythia8/Pythia.h" #include "Pythia8/Pythia8ToHepMC.h" #include "HepMC/GenEvent.h" #include "HepMC/IO_GenEvent.h" using namespace Pythia8; // Functions for histogramming #include "fastjet/PseudoJet.hh" #include "fastjet/ClusterSequence.hh" #include "fastjet/CDFMidPointPlugin.hh" #include "fastjet/CDFJetCluPlugin.hh" #include "fastjet/D0RunIIConePlugin.hh" //========================================================================== // Find the Durham kT separation of the clustering from // nJetMin --> nJetMin-1 jets in te input event double pTfirstJet( const Event& event, int nJetMin, double Rparam) { double yPartonMax = 4.; // Fastjet analysis - select algorithm and parameters fastjet::Strategy strategy = fastjet::Best; fastjet::RecombinationScheme recombScheme = fastjet::E_scheme; fastjet::JetDefinition *jetDef = NULL; // For hadronic collision, use hadronic Durham kT measure if(event[3].colType() != 0 || event[4].colType() != 0) jetDef = new fastjet::JetDefinition(fastjet::kt_algorithm, Rparam, recombScheme, strategy); // For e+e- collision, use e+e- Durham kT measure else jetDef = new fastjet::JetDefinition(fastjet::ee_kt_algorithm, recombScheme, strategy); // Fastjet input std::vector fjInputs; // Reset Fastjet input fjInputs.resize(0); // Loop over event record to decide what to pass to FastJet for (int i = 0; i < event.size(); ++i) { // (Final state && coloured+photons) only! if ( !event[i].isFinal() || event[i].isLepton() || event[i].id() == 23 || abs(event[i].id()) == 24 || abs(event[i].y()) > yPartonMax) continue; // Store as input to Fastjet fjInputs.push_back( fastjet::PseudoJet (event[i].px(), event[i].py(), event[i].pz(),event[i].e() ) ); } // Do nothing for empty input if (int(fjInputs.size()) == 0) { delete jetDef; return 0.0; } // Run Fastjet algorithm fastjet::ClusterSequence clustSeq(fjInputs, *jetDef); // Extract kT of first clustering double pTFirst = sqrt(clustSeq.exclusive_dmerge_max(nJetMin-1)); delete jetDef; // Return kT return pTFirst; } //========================================================================== int main( int argc, char* argv[] ){ // Check that correct number of command-line arguments if (argc != 6) { cerr << " Unexpected number of command-line arguments. \n You are" << " expected to provide the arguments" << endl << " 1. Input file for settings" << endl << " 2. Name of output HepMC file" << endl << " 3. Maximal number of additional jets" << " (not used internally in Pythia, only used to construct the full" << " name of lhe files with additional jets, and to label output" << " histograms)" << endl << " 4. Full name of the input LHE file (with path" << " , without any _0.lhe suffix)" << endl << " 5. Path for output histogram files" << endl << " Program stopped. " << endl; return 1; } Pythia pythia; // First argument: Get input from an input file pythia.readFile(argv[1]); int nEvent = pythia.mode("Main:numberOfEvents"); // Interface for conversion from Pythia8::Event to HepMC event. // Will fill cross section and event weight directly in this program, // so switch it off for normal conversion routine. HepMC::Pythia8ToHepMC ToHepMC; ToHepMC.set_store_xsec(false); // Specify file where HepMC events will be stored. HepMC::IO_GenEvent ascii_io(argv[2], std::ios::out); // Third argument: Maximal number of additional jets int njet = atoi(argv[3]); // Read input and output paths string iPath = string(argv[4]); string oPath = string(argv[5]); // To write correctly normalized events to hepmc file, first get // a reasonable accurate of the cross section int njetCounterEstimate = njet; vector xsecEstimate; vector nTrialEstimate; vector nAcceptEstimate; pythia.readString("Random:setSeed = on"); pythia.readString("Random:seed = 42390964"); while(njetCounterEstimate >= 0) { // Number of runs int nRun = 1; double nTrial = 0.; double nAccept = 0.; int countEvents = 0; // Run pythia nRun times with the same lhe file to get nRun times // higher statistics in the histograms for(int n = 1; n <= nRun ; ++n ) { // Get process and events from LHE file, initialize only the // first time bool skipInit = false; if(n > 1){ skipInit = true; pythia.readString("Main:LHEFskipInit = on"); } // From njet, choose LHE file stringstream in; in << "_" << njetCounterEstimate << ".lhe"; string LHEfile = iPath + in.str(); pythia.readString("HadronLevel:all = off"); // Read in ME configurations pythia.init(LHEfile,skipInit); for( int iEvent=0; iEvent 0 ) njetCounterEstimate--; else break; } // end loop over different jet multiplicities cout << endl << "Finished estimating cross section" << endl; for(int i=0; i < int(xsecEstimate.size()); ++i) cout << " Cross section estimate for " << njet-i << " jets :" << scientific << setprecision(8) << xsecEstimate[i] << endl; for(int i=0; i < int(nTrialEstimate.size()); ++i) cout << " Trial events for " << njet-i << " jets :" << scientific << setprecision(3) << nTrialEstimate[i] << " Accepted events for " << njet-i << " jets :" << scientific << setprecision(3) << nAcceptEstimate[i] << endl; cout << endl; // Now start merging procedure int njetCounter = njet; Hist histPTFirstSum("pT of first jet",100,0.,100.); Hist histPTSecondSum("pT of second jet",100,0.,100.); pythia.readString("Random:setSeed = on"); pythia.readString("Random:seed = 42390964"); // Sum of event weights double sigma = 0.0; double sigma2 = 0.0; while(njetCounter >= 0) { cout << " Path to lhe files: " << iPath << "_*" << endl; cout << " Output written to: " << oPath << "'name'.dat" << endl; // Set up histograms of pT of the first jet Hist histPTFirst("pT of first jet",100,0.,200.); Hist histPTSecond("pT of second jet",100,0.,200.); Hist histPTThird("pT of third jet",100,0.,200.); Hist histPTFourth("pT of fourth jet",50,0.,100.); Hist histPTFifth("pT of fifth jet",30,0.,50.); Hist histPTSixth("pT of sixth jet",30,0.,50.); // Number of runs int nRun = 1; // Number of tried events int nTriedEvents = 0; // Number of accepted events int nAccepEvents = 0; // Run pythia nRun times with the same lhe file to get nRun times // higher statistics in the histograms for(int n = 1; n <= nRun ; ++n ) { // Get process and events from LHE file, initialize only the // first time bool skipInit = false; if(n > 1){ skipInit = true; pythia.readString("Main:LHEFskipInit = on"); } // From njet, choose LHE file stringstream in; in << "_" << njetCounter << ".lhe"; string LHEfile = iPath + in.str(); cout << endl << endl << "\t LHE FILE FOR + " << njetCounter << " JET SAMPLE READ FROM " << LHEfile << endl << endl; cout << "Normalise with xsection " << xsecEstimate[njet-njetCounter] << endl << endl; pythia.readString("HadronLevel:all = on"); // Read in ME configurations pythia.init(LHEfile,skipInit); if(pythia.flag("Main:showChangedSettings")) { pythia.settings.listChanged(); } for( int iEvent=0; iEvent 0.){ // Construct new empty HepMC event and fill it. // Units will be as chosen for HepMC build, but can be changed // by arguments, e.g. GenEvt( HepMC::Units::GEV, HepMC::Units::MM) HepMC::GenEvent* hepmcevt = new HepMC::GenEvent(); double normhepmc = 1.* xsecEstimate[njet-njetCounter] * nTrialEstimate[njet-njetCounter] / nAcceptEstimate[njet-njetCounter] * 1./ (double(nRun)*double(nEvent)); sigma += weight*normhepmc; sigma2 += pow(weight*normhepmc,2); // Set event weight hepmcevt->weights().push_back(weight*normhepmc); // Fill summed histograms histPTFirstSum.fill( pTfirst, weight*normhepmc); histPTSecondSum.fill( pTsecnd, weight*normhepmc); // Fill HepMC event, with PDF info. ToHepMC.fill_next_event( pythia, hepmcevt ); // Report cross section to hepmc HepMC::GenCrossSection xsec; xsec.set_cross_section( sigma*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } } // if( pythia.next() ) if(nTriedEvents%10000 == 0) cout << nTriedEvents << endl; } // end loop over events to generate // print cross section, errors pythia.stat(); } // end outer loop to rerun pythia with the same lhe file // Normalise histograms for this particular multiplicity double norm = 1. * pythia.info.sigmaGen() * double(nTriedEvents)/double(nAccepEvents) * 1./ (double(nRun)*double(nEvent)); histPTFirst *= norm; histPTSecond *= norm; histPTThird *= norm; histPTFourth *= norm; histPTFifth *= norm; histPTSixth *= norm; // Write histograms for this particular multiplicity to file ofstream write; stringstream suffix; suffix << njet << "_" << njetCounter; suffix << "_wv.dat"; write.open( (char*)(oPath + "PTjet1_" + suffix.str()).c_str()); histPTFirst.table(write); write.close(); write.open( (char*)(oPath + "PTjet2_" + suffix.str()).c_str()); histPTSecond.table(write); write.close(); write.open( (char*)(oPath + "PTjet3_" + suffix.str()).c_str()); histPTThird.table(write); write.close(); write.open( (char*)(oPath + "PTjet4_" + suffix.str()).c_str()); histPTFourth.table(write); write.close(); write.open( (char*)(oPath + "PTjet5_" + suffix.str()).c_str()); histPTFifth.table(write); write.close(); write.open( (char*)(oPath + "PTjet6_" + suffix.str()).c_str()); histPTSixth.table(write); write.close(); histPTFirst.null(); histPTSecond.null(); histPTThird.null(); histPTFourth.null(); histPTFifth.null(); histPTSixth.null(); // Restart with ME of a reduced the number of jets if( njetCounter > 0 ) njetCounter--; else break; } // end loop over different jet multiplicities // Since the histograms have been filled with the correct weight for // each jet multiplicity, no normalisation is needed. // Write summed histograms to file. ofstream writeSum; stringstream suffixSum; suffixSum << njet << "_wv.dat"; writeSum.open( (char*)(oPath + "PTjet1Sum_" + suffixSum.str()).c_str()); histPTFirstSum.table(writeSum); writeSum.close(); writeSum.open( (char*)(oPath + "PTjet2Sum_" + suffixSum.str()).c_str()); histPTSecondSum.table(writeSum); writeSum.close(); for(int i=0; i < int(xsecEstimate.size()); ++i) cout << " Cross section estimate for " << njet-i << " jets :" << scientific << setprecision(8) << xsecEstimate[i] << endl; for(int i=0; i < int(nTrialEstimate.size()); ++i) cout << " Trial events for " << njet-i << " jets :" << scientific << setprecision(3) << nTrialEstimate[i] << " Accepted events for " << njet-i << " jets :" << scientific << setprecision(3) << nAcceptEstimate[i] << endl; cout << endl; cout << "Histogrammed cross section for " << iPath << " with " << njet << " additional jets is " << scientific << setprecision(8) << sigma << " error " << sqrt(sigma2) << endl; return 0; } pythia8-8.1.80.orig/examples/w_production_tree_1.lhe0000644000175000017500000062032512217346211020623 0ustar sunsun
      # MG version : 5.1.5.5 #************************************************************ #* MadGraph 5 * #* * #* * * * #* * * * * * #* * * * * 5 * * * * * #* * * * * * #* * * * #* * #* * #* VERSION 1.5.5 2012-11-18 * #* * #* The MadGraph Development Team - Please visit us at * #* https://server06.fynu.ucl.ac.be/projects/madgraph * #* * #************************************************************ #* * #* Command File for MadGraph 5 * #* * #* run as ./bin/mg5 filename * #* * #************************************************************ set group_subprocesses Auto set ignore_six_quark_processes False set gauge unitary set complex_mass_scheme False import model sm define p = g u c d s u~ c~ d~ s~ define j = g u c d s u~ c~ d~ s~ define l+ = e+ mu+ define l- = e- mu- define vl = ve vm vt define vl~ = ve~ vm~ vt~ # Specify process(es) to run generate p p > w+ j , w+ > e+ ve QED=2 @1 add process p p > w- j , w- > e- ve~ QED=2 @2 # Output processes to MadEvent directory output -f #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # proc_card.dat * #********************************************************************* # * # This Files is generated by MADGRAPH 5 * # * # WARNING: This Files is generated for MADEVENT (compatibility issue)* # This files is NOT a valid MG4 proc_card.dat * # Running this in MG4 will NEVER reproduce the result of MG5* # * #********************************************************************* #********************************************************************* # Process(es) requested : mg2 input * #********************************************************************* # Begin PROCESS # This is TAG. Do not modify this line p p > w+ j , w+ > e+ ve @1 #Process # Be carefull the coupling are here in MG5 convention QED=2 end_coup # End the couplings input done # this tells MG there are no more procs # End PROCESS # This is TAG. Do not modify this line #********************************************************************* # Model information * #********************************************************************* # Begin MODEL # This is TAG. Do not modify this line sm # End MODEL # This is TAG. Do not modify this line #********************************************************************* # Start multiparticle definitions * #********************************************************************* # Begin MULTIPARTICLES # This is TAG. Do not modify this line # End MULTIPARTICLES # This is TAG. Do not modify this line ###################################################################### ## PARAM_CARD AUTOMATICALY GENERATED BY MG5 FOLLOWING UFO MODEL #### ###################################################################### ## ## ## Width set on Auto will be computed following the information ## ## present in the decay.py files of the model. By default, ## ## this is only 1->2 decay modes. ## ## ## ###################################################################### ################################### ## INFORMATION FOR MASS ################################### Block mass 5 4.700000e+00 # MB 6 1.730000e+02 # MT 15 1.777000e+00 # MTA 23 9.118800e+01 # MZ 25 1.200000e+02 # MH ## Not dependent paramater. ## Those values should be edited following the ## analytical expression. MG5 ignore those values ## but they are important for interfacing the output of MG5 ## to external program such as Pythia. 1 0.000000 # d : 0.0 2 0.000000 # u : 0.0 3 0.000000 # s : 0.0 4 0.000000 # c : 0.0 11 0.000000 # e- : 0.0 12 0.000000 # ve : 0.0 13 0.000000 # mu- : 0.0 14 0.000000 # vm : 0.0 16 0.000000 # vt : 0.0 21 0.000000 # g : 0.0 22 0.000000 # a : 0.0 24 80.419002 # w+ : cmath.sqrt(MZ__exp__2/2. + cmath.sqrt(MZ__exp__4/4. - (aEW*cmath.pi*MZ__exp__2)/(Gf*sqrt__2))) ################################### ## INFORMATION FOR SMINPUTS ################################### Block sminputs 1 1.325070e+02 # aEWM1 2 1.166390e-05 # Gf 3 1.180000e-01 # aS ################################### ## INFORMATION FOR YUKAWA ################################### Block yukawa 5 4.200000e+00 # ymb 6 1.645000e+02 # ymt 15 1.777000e+00 # ymtau ################################### ## INFORMATION FOR DECAY ################################### DECAY 6 1.491500e+00 # WT DECAY 23 2.441404e+00 # WZ DECAY 24 2.047600e+00 # WW DECAY 25 5.753088e-03 # WH ## Not dependent paramater. ## Those values should be edited following the ## analytical expression. MG5 ignore those values ## but they are important for interfacing the output of MG5 ## to external program such as Pythia. DECAY 1 0.000000 # d : 0.0 DECAY 2 0.000000 # u : 0.0 DECAY 3 0.000000 # s : 0.0 DECAY 4 0.000000 # c : 0.0 DECAY 5 0.000000 # b : 0.0 DECAY 11 0.000000 # e- : 0.0 DECAY 12 0.000000 # ve : 0.0 DECAY 13 0.000000 # mu- : 0.0 DECAY 14 0.000000 # vm : 0.0 DECAY 15 0.000000 # ta- : 0.0 DECAY 16 0.000000 # vt : 0.0 DECAY 21 0.000000 # g : 0.0 DECAY 22 0.000000 # a : 0.0 #********************************************************************* # MadGraph/MadEvent * # http://madgraph.hep.uiuc.edu * # * # run_card.dat * # * # This file is used to set the parameters of the run. * # * # Some notation/conventions: * # * # Lines starting with a '# ' are info or comments * # * # mind the format: value = variable ! comment * #********************************************************************* # #******************* # Running parameters #******************* # #********************************************************************* # Tag name for the run (one word) * #********************************************************************* tag_1 = run_tag ! name of the run #********************************************************************* # Run to generate the grid pack * #********************************************************************* .false. = gridpack !True = setting up the grid pack #********************************************************************* # Number of events and rnd seed * # Warning: Do not generate more than 1M events in a single run * # If you want to run Pythia, avoid more than 50k events in a run. * #********************************************************************* 1000 = nevents ! Number of unweighted events requested 396 = iseed ! rnd seed (0=assigned automatically=default)) #********************************************************************* # Collider type and energy * # lpp: 0=No PDF, 1=proton, -1=antiproton, 2=photon from proton, * # 3=photon from electron * #********************************************************************* 1 = lpp1 ! beam 1 type 1 = lpp2 ! beam 2 type 3500 = ebeam1 ! beam 1 total energy in GeV 3500 = ebeam2 ! beam 2 total energy in GeV #********************************************************************* # Beam polarization from -100 (left-handed) to 100 (right-handed) * #********************************************************************* 0 = polbeam1 ! beam polarization for beam 1 0 = polbeam2 ! beam polarization for beam 2 #********************************************************************* # PDF CHOICE: this automatically fixes also alpha_s and its evol. * #********************************************************************* 'lhapdf' = pdlabel ! PDF set 10042 = lhaid ! PDF set cteq6m #********************************************************************* # Renormalization and factorization scales * #********************************************************************* T = fixed_ren_scale ! if .true. use fixed ren scale T = fixed_fac_scale ! if .true. use fixed fac scale 91.1880 = scale ! fixed ren scale 80.4 = dsqrt_q2fact1 ! fixed fact scale for pdf1 80.4 = dsqrt_q2fact2 ! fixed fact scale for pdf2 1 = scalefact ! scale factor for event-by-event scales #********************************************************************* # Matching - Warning! ickkw > 1 is still beta #********************************************************************* 0 = ickkw ! 0 no matching, 1 MLM, 2 CKKW matching 1 = highestmult ! for ickkw=2, highest mult group 1 = ktscheme ! for ickkw=1, 1 Durham kT, 2 Pythia pTE 1 = alpsfact ! scale factor for QCD emission vx F = chcluster ! cluster only according to channel diag F = pdfwgt ! for ickkw=1, perform pdf reweighting #********************************************************************* # Automatic ptj and mjj cuts if xqcut > 0 # (turn off for VBF and single top processes) #********************************************************** F = auto_ptj_mjj ! Automatic setting of ptj and mjj #********************************************************** # #********************************** # BW cutoff (M+/-bwcutoff*Gamma) #********************************** 5 = bwcutoff ! (M+/-bwcutoff*Gamma) #********************************************************** # Apply pt/E/eta/dr/mij cuts on decay products or not # (note that etmiss/ptll/ptheavy/ht/sorted cuts always apply) #********************************************************** F = cut_decays ! Cut decay products #************************************************************* # Number of helicities to sum per event (0 = all helicities) # 0 gives more stable result, but longer run time (needed for # long decay chains e.g.). # Use >=2 if most helicities contribute, e.g. pure QCD. #************************************************************* 0 = nhel ! Number of helicities used per event #******************* # Standard Cuts #******************* # #********************************************************************* # Minimum and maximum pt's (for max, -1 means no cut) * #********************************************************************* 5 = ptj ! minimum pt for the jets 0 = ptb ! minimum pt for the b 0 = pta ! minimum pt for the photons 0 = ptl ! minimum pt for the charged leptons 0 = misset ! minimum missing Et (sum of neutrino's momenta) 0 = ptheavy ! minimum pt for one heavy final state 0 = ptonium ! minimum pt for the quarkonium states -1 = ptjmax ! maximum pt for the jets -1 = ptbmax ! maximum pt for the b -1 = ptamax ! maximum pt for the photons -1 = ptlmax ! maximum pt for the charged leptons -1 = missetmax ! maximum missing Et (sum of neutrino's momenta) #********************************************************************* # Minimum and maximum E's (in the lab frame) * #********************************************************************* 0 = ej ! minimum E for the jets 0 = eb ! minimum E for the b 0 = ea ! minimum E for the photons 0 = el ! minimum E for the charged leptons -1 = ejmax ! maximum E for the jets -1 = ebmax ! maximum E for the b -1 = eamax ! maximum E for the photons -1 = elmax ! maximum E for the charged leptons #********************************************************************* # Maximum and minimum absolute rapidity (for max, -1 means no cut) * #********************************************************************* -1 = etaj ! max rap for the jets -1 = etab ! max rap for the b -1 = etaa ! max rap for the photons -1 = etal ! max rap for the charged leptons -1 = etaonium ! max rap for the quarkonium states 0 = etajmin ! min rap for the jets 0 = etabmin ! min rap for the b 0 = etaamin ! min rap for the photons 0 = etalmin ! main rap for the charged leptons #********************************************************************* # Minimum and maximum DeltaR distance * #********************************************************************* 1d-2 = drjj ! min distance between jets 0 = drbb ! min distance between b's 0 = drll ! min distance between leptons 0 = draa ! min distance between gammas 0 = drbj ! min distance between b and jet 0 = draj ! min distance between gamma and jet 0 = drjl ! min distance between jet and lepton 0 = drab ! min distance between gamma and b 0 = drbl ! min distance between b and lepton 0 = dral ! min distance between gamma and lepton -1 = drjjmax ! max distance between jets -1 = drbbmax ! max distance between b's -1 = drllmax ! max distance between leptons -1 = draamax ! max distance between gammas -1 = drbjmax ! max distance between b and jet -1 = drajmax ! max distance between gamma and jet -1 = drjlmax ! max distance between jet and lepton -1 = drabmax ! max distance between gamma and b -1 = drblmax ! max distance between b and lepton -1 = dralmax ! maxdistance between gamma and lepton #********************************************************************* # Minimum and maximum invariant mass for pairs * #********************************************************************* 5.0 = mmjj ! min invariant mass of a jet pair 0 = mmbb ! min invariant mass of a b pair 0 = mmaa ! min invariant mass of gamma gamma pair 0 = mmll ! min invariant mass of l+l- (same flavour) lepton pair -1 = mmjjmax ! max invariant mass of a jet pair -1 = mmbbmax ! max invariant mass of a b pair -1 = mmaamax ! max invariant mass of gamma gamma pair -1 = mmllmax ! max invariant mass of l+l- (same flavour) lepton pair #********************************************************************* # Minimum and maximum invariant mass for all letpons * #********************************************************************* 0 = mmnl ! min invariant mass for all letpons (l+- and vl) -1 = mmnlmax ! max invariant mass for all letpons (l+- and vl) #********************************************************************* # Minimum and maximum pt for 4-momenta sum of leptons * #********************************************************************* 0 = ptllmin ! Minimum pt for 4-momenta sum of leptons(l and vl) -1 = ptllmax ! Maximum pt for 4-momenta sum of leptons(l and vl) #********************************************************************* # Inclusive cuts * #********************************************************************* 0 = xptj ! minimum pt for at least one jet 0 = xptb ! minimum pt for at least one b 0 = xpta ! minimum pt for at least one photon 0 = xptl ! minimum pt for at least one charged lepton #********************************************************************* # Control the pt's of the jets sorted by pt * #********************************************************************* 0 = ptj1min ! minimum pt for the leading jet in pt 0 = ptj2min ! minimum pt for the second jet in pt 0 = ptj3min ! minimum pt for the third jet in pt 0 = ptj4min ! minimum pt for the fourth jet in pt -1 = ptj1max ! maximum pt for the leading jet in pt -1 = ptj2max ! maximum pt for the second jet in pt -1 = ptj3max ! maximum pt for the third jet in pt -1 = ptj4max ! maximum pt for the fourth jet in pt 0 = cutuse ! reject event if fails any (0) / all (1) jet pt cuts #********************************************************************* # Control the pt's of leptons sorted by pt * #********************************************************************* 0 = ptl1min ! minimum pt for the leading lepton in pt 0 = ptl2min ! minimum pt for the second lepton in pt 0 = ptl3min ! minimum pt for the third lepton in pt 0 = ptl4min ! minimum pt for the fourth lepton in pt -1 = ptl1max ! maximum pt for the leading lepton in pt -1 = ptl2max ! maximum pt for the second lepton in pt -1 = ptl3max ! maximum pt for the third lepton in pt -1 = ptl4max ! maximum pt for the fourth lepton in pt #********************************************************************* # Control the Ht(k)=Sum of k leading jets * #********************************************************************* 0 = htjmin ! minimum jet HT=Sum(jet pt) -1 = htjmax ! maximum jet HT=Sum(jet pt) 0 = ihtmin !inclusive Ht for all partons (including b) -1 = ihtmax !inclusive Ht for all partons (including b) 0 = ht2min ! minimum Ht for the two leading jets 0 = ht3min ! minimum Ht for the three leading jets 0 = ht4min ! minimum Ht for the four leading jets -1 = ht2max ! maximum Ht for the two leading jets -1 = ht3max ! maximum Ht for the three leading jets -1 = ht4max ! maximum Ht for the four leading jets #********************************************************************* # WBF cuts * #********************************************************************* 0 = xetamin ! minimum rapidity for two jets in the WBF case 0 = deltaeta ! minimum rapidity for two jets in the WBF case #********************************************************************* # maximal pdg code for quark to be considered as a light jet * # (otherwise b cuts are applied) * #********************************************************************* 4 = maxjetflavor ! Maximum jet pdg code #********************************************************************* # Jet measure cuts * #********************************************************************* 2.0 = xqcut ! minimum kt jet measure between partons #********************************************************************* 0d0 = kt_durham ! minimum durham kt jet measure between partons 0.4 = d_parameter ! D parameter for hadronic kT F = do_kt_durham ! T: enable durham kt cut 15 = pt_pythia ! minimum pythia pt jet measure between partons 1 = njets_requested ! number of jets above the pythia pt cut T = do_pt_pythia ! T: enable pythia pt cut #********************************************************************* # Number of Events : 1000 # Integrated weight (pb) : .26047E+04 # Truncated wgt (pb) : .00000E+00 # Unit wgt : .26047E+01
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0.98128962049E+01 0.00000000000E+00 0. 1. 2 -1 0 0 502 0 0.00000000000E+00 0.00000000000E+00 -0.10737474277E+04 0.10737474277E+04 0.00000000000E+00 0. -1. 24 2 1 2 0 0 -0.20265182728E+02 -0.78878866688E+02 -0.44455629128E+03 0.45885082526E+03 0.79254214316E+02 0. 0. -11 1 3 3 0 0 -0.16043041007E+02 -0.91975595412E+02 -0.42369586730E+03 0.43386066575E+03 0.00000000000E+00 0. 1. 12 1 3 3 0 0 -0.42221417211E+01 0.13096728724E+02 -0.20860423983E+02 0.24990159518E+02 0.00000000000E+00 0. -1. 1 1 1 2 501 0 0.20265182728E+02 0.78878866688E+02 -0.61937824016E+03 0.62470949859E+03 0.00000000000E+00 0. -1. 6 1 0.2604700E+01 0.8040000E+02 0.7957747E-01 0.1297830E+00 21 -1 0 0 501 502 0.00000000000E+00 0.00000000000E+00 0.12917414194E+02 0.12917414194E+02 0.00000000000E+00 0. -1. -1 -1 0 0 0 501 0.00000000000E+00 0.00000000000E+00 -0.24745109320E+03 0.24745109320E+03 0.00000000000E+00 0. 1. 24 2 1 2 0 0 -0.58168744876E+01 -0.23097485672E+02 -0.20770541054E+03 0.22449252849E+03 0.81780363839E+02 0. 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      pythia8-8.1.80.orig/examples/main27.cc0000644000175000017500000001232112217346165015561 0ustar sunsun// main27.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Kaluza-Klein gamma*/Z resonances in TeV-sized extra dimensions. #include #include #include #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Generator. Pythia pythia; ParticleData& pdt = pythia.particleData; // Pick new random number seed for each run, based on clock. pythia.readString("Random:setSeed = on"); pythia.readString("Random:seed = 0"); // Process selection. // ANY COMBINATION OF THE PROCESSES FLAGS BELOW IS ALLOWED // HERE WE SWITCH ON ONLY THE MU+MU- FINAL STATE. // TO SWITCH ALL POSSIBLE FINAL STATES ON, UNCOMMENT ALL // THE RELEVANT LINES BELOW: //pythia.readString("ExtraDimensionsTEV:ffbar2e+e- = on"); pythia.readString("ExtraDimensionsTEV:ffbar2mu+mu- = on"); //pythia.readString("ExtraDimensionsTEV:ffbar2tau+tau- = on"); //pythia.readString("ExtraDimensionsTEV:ffbar2uubar = on"); //pythia.readString("ExtraDimensionsTEV:ffbar2ddbar = on"); //pythia.readString("ExtraDimensionsTEV:ffbar2ccbar = on"); //pythia.readString("ExtraDimensionsTEV:ffbar2ssbar = on"); //pythia.readString("ExtraDimensionsTEV:ffbar2bbbar = on"); //pythia.readString("ExtraDimensionsTEV:ffbar2ttbar = on"); //pythia.readString("ExtraDimensionsTEV:ffbar2nuenuebar = on"); //pythia.readString("ExtraDimensionsTEV:ffbar2numunumubar = on"); //pythia.readString("ExtraDimensionsTEV:ffbar2nutaunutaubar = on"); // Pick KK mass. double newMass = 4000.; // GeV cout << "|-------------------------" << endl; cout << "| KK mass is: " << newMass << endl; cout << "|-------------------------" << endl; stringstream strm; string sNewMass, sNewWidth, sNewLowBound, sNewHighBound; // Manually set the mass and therefore the width // and the phase space for the sampling strm.clear(); strm << newMass; strm >> sNewMass; strm.clear(); strm << newMass / pdt.m0(5000023) * pdt.mWidth(5000023); strm >> sNewWidth; strm.clear(); strm << newMass/4.; strm >> sNewLowBound; strm.clear(); strm << newMass*2.; strm >> sNewHighBound; // Feed in KK state information and other generation specifics. pythia.readString("5000023:m0 = " + sNewMass); pythia.readString("5000023:mWidth = " + sNewWidth); pythia.readString("5000023:mMin = " + sNewLowBound); pythia.readString("5000023:mMax = " + sNewHighBound); ////////////////////////////////////////////////////////////////////////// pythia.readString("5000023:isResonance = false"); // THIS IS MANDATORY // ////////////////////////////////////////////////////////////////////////// // 0=(gm+Z), 1=(gm), 2=(Z), 3=(gm+Z+gmKK+ZKK), 4=(m+Z+gmKK), 5=(m+Z+ZKK) pythia.readString("ExtraDimensionsTEV:gmZmode = 3"); // min=0, max=100, default=10 pythia.readString("ExtraDimensionsTEV:nMax = 100"); pythia.readString("ExtraDimensionsTEV:mStar = " + sNewMass); pythia.readString("PhaseSpace:mHatMin = " + sNewLowBound); pythia.readString("PhaseSpace:mHatMax = " + sNewHighBound); // Initialize for LHC. pythia.readString("Beams:eCM = 14000."); pythia.init(); // Histograms. Hist mHatHisto("dN/dmHat", 50, newMass/4., newMass*2.); Hist pTmuHisto("(dN/dpT)_mu^-", 50, 1., 2501.); vector moms; // Measure the cpu runtime. clock_t start, stop; double t = 0.0; // Depending on operating system, either of lines below gives warning. //assert((start = clock()) != -1); // Start timer; clock_t signed. //assert((start = clock()) != -1u); // Start timer; clock_t unsigned. // Simpler option, not using assert. start = clock(); // Begin event loop. Generate event. Skip if error. List first one. for (int iEvent = 0 ; iEvent < 500 ; ++iEvent) { if (!pythia.next()) continue; // Begin event analysis. bool isZ = false; bool ismu = false; int iZ = 0; int imu = 0; for (int i = 0 ; i < pythia.event.size() ; ++i) { // find the most recent Z if (pythia.event[i].id() == 5000023) { iZ = i; isZ = true; } // find the final muon who's first mother is the Z if (pythia.event[i].id() == 13 && pythia.event[i].isFinal()) { moms.clear(); moms = pythia.event.motherList(i); for (int m = 0 ; m < int(moms.size()) ; m++) { if( pythia.event[ moms[m] ].id() == 5000023 ) { imu = i; ismu = true; break; } // end if 5000023 } // end for moms.size() } // end if final muon } // end for event.size() if(isZ && ismu) { mHatHisto.fill( pythia.event[iZ].m() ); pTmuHisto.fill( pythia.event[imu].pT() ); } if(iEvent%10 == 0) cout << "Event: " << iEvent << endl << flush; } // end for iEvent<500 // Done. Print results. stop = clock(); // Stop timer t = (double) (stop-start)/CLOCKS_PER_SEC; pythia.stat(); cout << mHatHisto; cout << pTmuHisto; cout << "\n" << "|----------------------------------------|" << endl; cout << "| CPU Runtime = " << t << " sec" << endl; cout << "|----------------------------------------|" << "\n" << endl; return 0; } pythia8-8.1.80.orig/examples/main82.cmnd0000644000175000017500000000107612217346167016125 0ustar sunsun! main82.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. // specify statistics parameters Main:numberOfEvents = 100 // number of events generated // specify shower options HadronLevel:all = off SpaceShower:MEafterFirst = off TimeShower:MEafterFirst = off Merging:doUserMerging = on Merging:Process = pp>e+ve Merging:TMS = 30. Merging:nJetMax = 2 // specify PDF set PDF:useLHAPDF = on PDF:LHAPDFset = cteq6ll.LHpdf pythia8-8.1.80.orig/examples/main85.cc0000644000175000017500000002173112217346167015574 0ustar sunsun// main85.cc is a part of the PYTHIA event generator. // Copyright (C) 2011 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This program is written by Stefan Prestel. // It illustrates how to do CKKW-L merging, // see the Matrix Element Merging page in the online manual. #include "Pythia8/Pythia.h" #include "Pythia8/Pythia8ToHepMC.h" #include "HepMC/GenEvent.h" #include "HepMC/IO_GenEvent.h" // Following line to be used with HepMC 2.04 onwards. #include "HepMC/Units.h" using namespace Pythia8; //========================================================================== // Example main programm to illustrate merging int main( int argc, char* argv[] ){ // Check that correct number of command-line arguments if (argc != 4) { cerr << " Unexpected number of command-line arguments ("< xsecLO; vector nAcceptLO; cout << endl << endl << endl; cout << "Start estimating ckkwl tree level cross section" << endl; while(njetcounterLO >= 0) { // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathTree+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathTree + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); pythia.settings.mode("Merging:nRequested", njetcounterLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Start generation loop for( int iEvent=0; iEvent 0 ) njetcounterLO--; else break; } // end loop over different jet multiplicities //----------------------------------------------------------------------------- //----------------------------------------------------------------------------- // Switch off cross section estimation. pythia.settings.flag("Merging:doXSectionEstimate", false); // Switch showering and multiple interaction back on. pythia.settings.flag("PartonLevel:FSR",fsr); pythia.settings.flag("PartonLevel:ISR",isr); pythia.settings.flag("HadronLevel:all",had); pythia.settings.flag("PartonLevel:MPI",mpi); // Declare sample cross section for output. double sigmaTemp = 0.; vector sampleXStree; // Cross section an error. double sigmaTotal = 0.; double errorTotal = 0.; int sizeLO = int(xsecLO.size()); njetcounterLO = nMaxLO; iPathTree = iPath + "_tree"; while(njetcounterLO >= 0){ // From njetcounter, choose LHE file stringstream in; in << "_" << njetcounterLO << ".lhe"; #ifdef GZIPSUPPORT if(access( (iPathTree+in.str()+".gz").c_str(), F_OK) != -1) in << ".gz"; #endif string LHEfile = iPathTree + in.str(); LHAupLHEF lhareader((char*)(LHEfile).c_str()); cout << endl << endl << endl << "Start tree level treatment for " << njetcounterLO << " jets" << endl; pythia.settings.mode("Merging:nRequested", njetcounterLO); pythia.settings.word("Beams:LHEF", LHEfile); pythia.init(&lhareader); // Remember position in vector of cross section estimates. int iNow = sizeLO-1-njetcounterLO; // Start generation loop for( int iEvent=0; iEventweights().push_back(weight*normhepmc); // Fill HepMC event ToHepMC.fill_next_event( pythia, hepmcevt ); // Add the weight of the current event to the cross section. sigmaTotal += weight*normhepmc; sigmaTemp += weight*normhepmc; errorTotal += pow2(weight*normhepmc); // Report cross section to hepmc HepMC::GenCrossSection xsec; xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 ); hepmcevt->set_cross_section( xsec ); // Write the HepMC event to file. Done with it. ascii_io << hepmcevt; delete hepmcevt; } // end loop over events to generate // print cross section, errors pythia.stat(); // Save sample cross section for output. sampleXStree.push_back(sigmaTemp); sigmaTemp = 0.; // Restart with ME of a reduced the number of jets if( njetcounterLO > 0 ) njetcounterLO--; else break; } // Print cross section information. cout << endl << endl; cout << " *---------------------------------------------------*" << endl; cout << " | |" << endl; cout << " | Sample cross sections after CKKW-L merging |" << endl; cout << " | |" << endl; cout << " | Leading order cross sections (mb): |" << endl; for (int i = 0; i < int(sampleXStree.size()); ++i) cout << " | " << sampleXStree.size()-1-i << "-jet: " << setw(17) << scientific << setprecision(6) << sampleXStree[i] << " |" << endl; cout << " | |" << endl; cout << " |---------------------------------------------------|" << endl; cout << " |---------------------------------------------------|" << endl; cout << " | Inclusive cross sections: |" << endl; cout << " | |" << endl; cout << " | CKKW-L merged inclusive cross section: |" << endl; cout << " | " << setw(17) << scientific << setprecision(6) << sigmaTotal << " +- " << setw(17) << sqrt(errorTotal) << " mb " << " |" << endl; cout << " | |" << endl; cout << " | LO inclusive cross section: |" << endl; cout << " | " << setw(17) << scientific << setprecision(6) << xsecLO.back() << " mb |" << endl; cout << " | |" << endl; cout << " *---------------------------------------------------*" << endl; cout << endl << endl; // Done return 0; } pythia8-8.1.80.orig/examples/main18.cc0000644000175000017500000001650612217346164015571 0ustar sunsun// main18.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how to write an event filter. // No new functionality is involved - all could be done in the main program // - but the division of tasks may be more convenient for recurrent cuts. #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // The EventFilter class. // The constructor takes the following arguments // select = 1 : keep only final particles. // = 2 : keep only final visible particles (i.e. not neutrinos). // = 3 : keep only final charged particles. // etaMax (default = 50) : keep only particles with pseudorapidity // |eta| < etaMax. // pTminCharged (default = 0) : keep a charged particle only if // its transverse momentum pT < pTminCharged. // pTminNeutral (default = 0) : keep a neutral particle only if // its transverse momentum pT < pTminNeutral. // Main methods: // filter( event) takes an event record as input and analyzes it. // size() returns the number of particles kept. // index(i) returns the index in the full event of the i'th kept particle. // particlePtr(i) returns a pointer to the i'th kept particle. // particleRef(i) returns a reference to the i'th kept particle. // list() gives a listing of the kept particles only. class EventFilter { public: // Constructor sets properties of filter. EventFilter( int selectIn, double etaMaxIn = 50., double pTminChargedIn = 0., double pTminNeutralIn = 0.) : select(selectIn), etaMax(etaMaxIn), pTminCharged(pTminChargedIn), pTminNeutral(pTminNeutralIn) {} // Analysis of each new event to find acceptable particles. void filter(Event& event); // Return size of array, and index of a particle. int size() const {return keptPtrs.size();} int index(int i) const {return keptIndx[i];} // Return pointer or reference to a particle. Particle* particlePtr(int i) {return keptPtrs[i];} Particle& particleRef(int i) {return *keptPtrs[i];} // List kept particles only. void list(ostream& os = cout); private: // Filter properties, set by constructor. int select; double etaMax, pTminCharged, pTminNeutral; // Kept particle indices and pointers, referring to original event. vector keptIndx; vector keptPtrs; }; //-------------------------------------------------------------------------- // The filter method. void EventFilter::filter(Event& event) { // Reset arrays in preparation for new event. keptIndx.resize(0); keptPtrs.resize(0); // Loop over all particles in the event record. for (int i = 0; i < event.size(); ++i) { // Skip if particle kind selection criteria not fulfilled. if (!event[i].isFinal()) continue; if (select == 2 && !event[i].isVisible()) continue; bool isCharged = event[i].isCharged(); if (select == 3 && !isCharged) continue; // Skip if too large pseudorapidity. if (abs(event[i].eta()) > etaMax) continue; // Skip if too small pT. if (isCharged && event[i].pT() < pTminCharged) continue; else if (!isCharged && event[i].pT() < pTminNeutral) continue; // Add particle to vectors of indices and pointers. keptIndx.push_back( i ); keptPtrs.push_back( &event[i] ); // End of particle loop. Done. } } //-------------------------------------------------------------------------- // The list method: downscaled version of Event::list. void EventFilter::list(ostream& os) { // Header. os << "\n -------- PYTHIA Event Listing (filtered) ------------------" << "-----------------------------------------------------------------" << "----\n \n no id name status mothers " << " daughters colours p_x p_y p_z e " << " m \n"; // At high energy switch to scientific format for momenta. double eSum = 0.; for (int iKept = 0; iKept < size(); ++iKept) eSum += keptPtrs[iKept]->e(); bool useFixed = (eSum < 1e5); // Listing of kept particles in event. for (int iKept = 0; iKept < size(); ++iKept) { int i = keptIndx[iKept]; Particle& pt = *keptPtrs[iKept]; // Basic line for a particle, always printed. os << setw(6) << i << setw(10) << pt.id() << " " << left << setw(18) << pt.nameWithStatus(18) << right << setw(4) << pt.status() << setw(6) << pt.mother1() << setw(6) << pt.mother2() << setw(6) << pt.daughter1() << setw(6) << pt.daughter2() << setw(6) << pt.col() << setw(6) << pt.acol() << ( (useFixed) ? fixed : scientific ) << setprecision(3) << setw(11) << pt.px() << setw(11) << pt.py() << setw(11) << pt.pz() << setw(11) << pt.e() << setw(11) << pt.m() << "\n"; } // Listing finished. os << "\n -------- End PYTHIA Event Listing ----------------------------" << "-------------------------------------------------------------------" << endl; } //========================================================================== // Use the EventFilter method to plot some event properties. int main() { // Number of events to generate, to list, to allow aborts. int nEvent = 100; int nList = 1; int nAbort = 3; // Declare generator. Pythia pythia; // Hard QCD events with pThat > 100. pythia.readString("HardQCD:all = on"); pythia.readString("PhaseSpace:pTHatMin = 100."); // No automatic event listings - do it manually below. pythia.readString("Next:numberShowInfo = 0"); pythia.readString("Next:numberShowProcess = 0"); pythia.readString("Next:numberShowEvent = 0"); // Initialization for LHC. pythia.init(); // Values for filter. int select = 3; double etaMax = 3.; double pTminChg = 1.; // Declare Event Filter according to specification. EventFilter filter( select, etaMax, pTminChg); // Histograms. Hist nCharged( "selected charged multiplicity", 100, -0.5, 199.5); Hist etaCharged( "selected charged eta distribution", 100, -5.0, 5.0); Hist pTCharged( "selected charged pT distribution", 100, 0.0, 50.0); // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if too many failures. if (!pythia.next()) { if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Find final charged particles with |eta| < 3 and pT > 1 GeV. filter.filter( pythia.event); // List first few events, both complete and after filtering. if (iEvent < nList) { pythia.info.list(); pythia.process.list(); pythia.event.list(); filter.list(); } // Analyze selected particle sample. nCharged.fill( filter.size() ); for (int i = 0; i < filter.size(); ++i) { // Use both reference and pointer notation to illustrate freedom. etaCharged.fill( filter.particleRef(i).eta() ); pTCharged.fill( filter.particlePtr(i)->pT() ); } // End of event loop. } // Final statistics. pythia.stat(); // Histograms. cout << nCharged << etaCharged << pTCharged; // Done. return 0; } pythia8-8.1.80.orig/examples/main61.cmnd0000644000175000017500000000522212217346166016116 0ustar sunsun! File: main61.cmnd ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! Names are case-insensitive - but spellings-sensitive! ! The changes here are illustrative, not always physics-motivated. ! 1) Settings that will be used in a main program. Main:numberOfEvents = 200 ! number of events to generate Main:timesAllowErrors = 3 ! abort run after this many flawed events ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showAllSettings = off ! list all settings Init:showChangedParticleData = on ! list changed particle data Init:showAllParticleData = off ! list all particle data Next:numberCount = 1000 ! print message every n events Next:numberShowLHA = 1 ! print LHA information n times Next:numberShowInfo = 1 ! print event information n times Next:numberShowProcess = 1 ! print process record n times Next:numberShowEvent = 1 ! print event record n times Stat:showPartonLevel = on ! additional statistics on MPI ! 3) Beam parameter settings. Values below agree with default ones. Beams:idA = 2212 ! first beam, p = 2212, pbar = -2212 Beams:idB = 2212 ! second beam, p = 2212, pbar = -2212 Beams:eCM = 14000. ! CM energy of collision ! 4) PDF settings. Default is to use internal PDFs PDF:useLHAPDF = on ! some pdf sets examples: cteq61.LHpdf cteq61.LHgrid MRST2004nlo.LHgrid PDF:LHAPDFset = MRST2001lo.LHgrid ! Allow extrapolation of PDF's beyond x and Q2 boundaries, at own risk. ! Default behaviour is to freeze PDF's at boundaries. PDF:extrapolateLHAPDF = on ! 5a) Pick processes and kinematics cuts. Charmonium:gg2QQbar[3S1(1)]g = on ! colour singlet charmonium production Charmonium:gg2QQbar[3P0(1)]g = on ! " Charmonium:gg2QQbar[3P1(1)]g = on ! " Charmonium:gg2QQbar[3P2(1)]g = on ! " PhaseSpace:pTHatMin = 20. ! minimum pT of hard process ! 5b) Alternative beam and process selection from a Les Houches Event File. ! NOTE: to use this option, comment out the lines in section 5a above ! and uncomment the ones below. Section 3 is ignored for frameType = 4. #Beams:frameType = 4 ! read info from a LHEF #Beams:LHEF = ttbar.lhe ! the LHEF to read from ! 6) Other settings. Can be expanded as desired. ! Note: may overwrite some of the values above, so watch out. #Tune:pp = 6 ! use Tune 4Cx #ParticleDecays:limitTau0 = on ! set long-lived particle stable ... #ParticleDecays:tau0Max = 10 ! ... if c*tau0 > 10 mm pythia8-8.1.80.orig/examples/main03.cmnd0000644000175000017500000000520112217346163016104 0ustar sunsun! main03.cmnd. ! This file contains commands to be read in for a Pythia8 run. ! Lines not beginning with a letter or digit are comments. ! Names are case-insensitive - but spellings-sensitive! ! The settings here are illustrative, not always physics-motivated. ! 1) Settings used in the main program. Main:numberOfEvents = 1000 ! number of events to generate Main:timesAllowErrors = 3 ! how many aborts before run stops ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showChangedParticleData = off ! list changed particle data Next:numberCount = 100 ! print message every n events Next:numberShowInfo = 1 ! print event information n times Next:numberShowProcess = 1 ! print process record n times Next:numberShowEvent = 0 ! print event record n times ! 3) Beam parameter settings. Values below agree with default ones. Beams:idA = 2212 ! first beam, p = 2212, pbar = -2212 Beams:idB = 2212 ! second beam, p = 2212, pbar = -2212 Beams:eCM = 14000. ! CM energy of collision ! 4) Settings for the hard-process generation. ! Example 1: QCD + prompt photon production; must set pTmin. HardQCD:all = on ! switch on all QCD jet + jet processes PromptPhoton:all = on ! swich on gamma + jet and gamma + gamma PhaseSpace:pTHatMin = 50. ! minimal pT scale in process ! Example 2: t-tbar production. #Top:gg2ttbar = on ! g g -> t tbar #Top:qqbar2ttbar = on ! q qbar -> t tbar ! Example 3: Z0 production; should set mMin. #WeakSingleBoson:ffbar2gmZ = on ! q qbar -> gamma*/Z0 #PhaseSpace:mHatMin = 50. ! Example 4: gauge boson pair production; set pTmin. Not yet complete. #WeakDoubleBoson:ffbar2ZW = on ! q qbar -> Z0 W+- #WeakDoubleBoson:ffbar2WW = on ! q qbar -> W+ W- #PhaseSpace:pTHatMin = 20. ! minimal pT scale in process ! 5) Switch on/off the key event generation steps. #PartonLevel:MPI = off ! no multiparton interactions #PartonLevel:ISR = off ! no initial-state radiation #PartonLevel:FSR = off ! no final-state radiation #HadronLevel:Hadronize = off ! no hadronization #HadronLevel:Decay = off ! no decays ! 6) Other settings. Can be expanded as desired. #Tune:preferLHAPDF = off ! use internal PDFs when LHAPDF not linked Tune:pp = 6 ! use Tune 4Cx ParticleDecays:limitTau0 = on ! set long-lived particle stable ... ParticleDecays:tau0Max = 10 ! ... if c*tau0 > 10 mm pythia8-8.1.80.orig/examples/main21.cc0000644000175000017500000003107312217346165015560 0ustar sunsun// main21.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates how to feed in a single particle (including a resonance) // or a toy parton-level configurations. #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // Single-particle gun. The particle must be a colour singlet. // Input: flavour, energy, direction (theta, phi). // If theta < 0 then random choice over solid angle. // Optional final argument to put particle at rest => E = m. void fillParticle(int id, double ee, double thetaIn, double phiIn, Event& event, ParticleData& pdt, Rndm& rndm, bool atRest = false) { // Reset event record to allow for new event. event.reset(); // Select particle mass; where relevant according to Breit-Wigner. double mm = pdt.mSel(id); double pp = sqrtpos(ee*ee - mm*mm); // Special case when particle is supposed to be at rest. if (atRest) { ee = mm; pp = 0.; } // Angles as input or uniform in solid angle. double cThe, sThe, phi; if (thetaIn >= 0.) { cThe = cos(thetaIn); sThe = sin(thetaIn); phi = phiIn; } else { cThe = 2. * rndm.flat() - 1.; sThe = sqrtpos(1. - cThe * cThe); phi = 2. * M_PI * rndm.flat(); } // Store the particle in the event record. event.append( id, 1, 0, 0, pp * sThe * cos(phi), pp * sThe * sin(phi), pp * cThe, ee, mm); } //========================================================================== // Simple method to do the filling of partons into the event record. void fillPartons(int type, double ee, Event& event, ParticleData& pdt, Rndm& rndm) { // Reset event record to allow for new event. event.reset(); // Information on a q qbar system, to be hadronized. if (type == 1) { int id = 2; double mm = pdt.m0(id); double pp = sqrtpos(ee*ee - mm*mm); event.append( id, 23, 101, 0, 0., 0., pp, ee, mm); event.append( -id, 23, 0, 101, 0., 0., -pp, ee, mm); // Information on a g g system, to be hadronized. } else if (type == 2) { event.append( 21, 23, 101, 102, 0., 0., ee, ee); event.append( 21, 23, 102, 101, 0., 0., -ee, ee); // Information on a g g g system, to be hadronized. } else if (type == 3) { event.append( 21, 23, 101, 102, 0., 0., ee, ee); event.append( 21, 23, 102, 103, 0.8 * ee, 0., -0.6 * ee, ee); event.append( 21, 23, 103, 101, -0.8 * ee, 0., -0.6 * ee, ee); // Information on a q q q junction system, to be hadronized. } else if (type == 4 || type == 5) { // Need a colour singlet mother parton to define junction origin. event.append( 1000022, -21, 0, 0, 2, 4, 0, 0, 0., 0., 1.01 * ee, 1.01 * ee); // The three endpoint q q q; the minimal system. double rt75 = sqrt(0.75); event.append( 2, 23, 1, 0, 0, 0, 101, 0, 0., 0., 1.01 * ee, 1.01 * ee); event.append( 2, 23, 1, 0, 0, 0, 102, 0, rt75 * ee, 0., -0.5 * ee, ee ); event.append( 1, 23, 1, 0, 0, 0, 103, 0, -rt75 * ee, 0., -0.5 * ee, ee ); // Define the qqq configuration as starting point for adding gluons. if (type == 5) { int colNow[4] = {0, 101, 102, 103}; Vec4 pQ[4]; pQ[1] = Vec4(0., 0., 1., 0.); pQ[2] = Vec4( rt75, 0., -0.5, 0.); pQ[3] = Vec4(-rt75, 0., -0.5, 0.); // Minimal cos(q-g opening angle), allows more or less nasty events. double cosThetaMin =0.; // Add a few gluons (almost) at random. for (int nglu = 0; nglu < 5; ++nglu) { int iq = 1 + int( 2.99999 * rndm.flat() ); double px, py, pz, e, prod; do { e = ee * rndm.flat(); double cThe = 2. * rndm.flat() - 1.; double phi = 2. * M_PI * rndm.flat(); px = e * sqrt(1. - cThe*cThe) * cos(phi); py = e * sqrt(1. - cThe*cThe) * sin(phi); pz = e * cThe; prod = ( px * pQ[iq].px() + py * pQ[iq].py() + pz * pQ[iq].pz() ) / e; } while (prod < cosThetaMin); int colNew = 104 + nglu; event.append( 21, 23, 1, 0, 0, 0, colNew, colNow[iq], px, py, pz, e, 0.); colNow[iq] = colNew; } // Update daughter range of mother. event[1].daughters(1, event.size() - 1); } // Information on a q q qbar qbar dijunction system, to be hadronized. } else if (type >= 6) { // The two fictitious beam remnant particles; needed for junctions. event.append( 2212, -12, 0, 0, 3, 5, 0, 0, 0., 0., ee, ee, 0.); event.append(-2212, -12, 0, 0, 6, 8, 0, 0, 0., 0., ee, ee, 0.); // Opening angle between "diquark" legs. double theta = 0.2; double cThe = cos(theta); double sThe = sin(theta); // Set one colour depending on whether more gluons or not. int acol = (type == 6) ? 103 : 106; // The four endpoint q q qbar qbar; the minimal system. // Two additional fictitious partons to make up original beams. event.append( 2, 23, 1, 0, 0, 0, 101, 0, ee * sThe, 0., ee * cThe, ee, 0.); event.append( 1, 23, 1, 0, 0, 0, 102, 0, -ee * sThe, 0., ee * cThe, ee, 0.); event.append( 2, -21, 1, 0, 0, 0, 103, 0, 0., 0., ee , ee, 0.); event.append( -2, 23, 2, 0, 0, 0, 0, 104, ee * sThe, 0., -ee * cThe, ee, 0.); event.append( -1, 23, 2, 0, 0, 0, 0, 105, -ee * sThe, 0., -ee * cThe, ee, 0.); event.append( -2, -21, 2, 0, 0, 0, 0, acol, 0., 0., -ee , ee, 0.); // Add extra gluons on string between junctions. if (type == 7) { event.append( 21, 23, 5, 8, 0, 0, 103, 106, 0., ee, 0., ee, 0.); } else if (type == 8) { event.append( 21, 23, 5, 8, 0, 0, 103, 108, 0., ee, 0., ee, 0.); event.append( 21, 23, 5, 8, 0, 0, 108, 106, 0.,-ee, 0., ee, 0.); } else if (type == 9) { event.append( 21, 23, 5, 8, 0, 0, 103, 107, 0., ee, 0., ee, 0.); event.append( 21, 23, 5, 8, 0, 0, 107, 108, ee, 0., 0., ee, 0.); event.append( 21, 23, 5, 8, 0, 0, 108, 106, 0.,-ee, 0., ee, 0.); } else if (type == 10) { event.append( 21, 23, 5, 8, 0, 0, 103, 107, 0., ee, 0., ee, 0.); event.append( 21, 23, 5, 8, 0, 0, 107, 108, ee, 0., 0., ee, 0.); event.append( 21, 23, 5, 8, 0, 0, 108, 109, 0.,-ee, 0., ee, 0.); event.append( 21, 23, 5, 8, 0, 0, 109, 106,-ee, 0., 0., ee, 0.); } // No more cases: done. } } //========================================================================== int main() { // Pick kind of events to generate: // 0 = single-particle gun. // 1 = q qbar. // 2 = g g. // 3 = g g g. // 4 = minimal q q q junction topology. // 5 = q q q junction topology with gluons on the strings. // 6 = q q qbar qbar dijunction topology, no gluons. // 7 - 10 : ditto, but with 1 - 4 gluons on string between junctions. // 11 : single-resonance gun. int type = 11; // Set particle species and energy for single-particle gun. int idGun = (type == 0) ? 15 : 25; double eeGun = (type == 0) ? 20. : 125.; bool atRest = (type == 0) ? false : true; // Set typical energy per parton. double ee = 20.0; // Set number of events to generate and to list. int nEvent = 10000; int nList = 3; // Generator; shorthand for event and particleData. Pythia pythia; Event& event = pythia.event; ParticleData& pdt = pythia.particleData; // Key requirement: switch off ProcessLevel, and thereby also PartonLevel. pythia.readString("ProcessLevel:all = off"); // Also allow resonance decays, with showers in them pythia.readString("Standalone:allowResDec = on"); // Optionally switch off decays. //pythia.readString("HadronLevel:Decay = off"); // Switch off automatic event listing in favour of manual. pythia.readString("Next:numberShowInfo = 0"); pythia.readString("Next:numberShowProcess = 0"); pythia.readString("Next:numberShowEvent = 0"); // Initialize. pythia.init(); // Book histograms. Hist epCons("deviation from energy-momentum conservation",100,0.,1e-4); Hist chgCons("deviation from charge conservation",57,-9.5,9.5); Hist nFinal("final particle multiplicity",100,-0.5,99.5); Hist dnparticledp("dn/dp for particles",100,0.,ee); Hist status85("multiplicity status code 85",50,-0.5,49.5); Hist status86("multiplicity status code 86",50,-0.5,49.5); Hist status83("multiplicity status code 83",50,-0.5,49.5); Hist status84("multiplicity status code 84",50,-0.5,49.5); Hist dndtheta("particle flow in event plane",100,-M_PI,M_PI); Hist dedtheta("energy flow in event plane",100,-M_PI,M_PI); Hist dpartondtheta("parton flow in event plane",100,-M_PI,M_PI); Hist dndyAnti("dn/dy primaries antijunction",100, -10., 10.); Hist dndyJun("dn/dy primaries junction",100, -10., 10.); Hist dndySum("dn/dy all primaries",100, -10., 10.); // Begin of event loop. for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Set up single particle, with random direction in solid angle. if (type == 0 || type == 11) fillParticle( idGun, eeGun, -1., 0., event, pdt, pythia.rndm, atRest); // Set up parton-level configuration. else fillPartons( type, ee, event, pdt, pythia.rndm); // Generate events. Quit if failure. if (!pythia.next()) { cout << " Event generation aborted prematurely, owing to error!\n"; break; } // List first few events. if (iEvent < nList) { event.list(); // Also list junctions. event.listJunctions(); } // Initialize statistics. Vec4 pSum = - event[0].p(); double chargeSum = 0.; if (type == 0) chargeSum = -event[1].charge(); if (type == 4 || type == 5) chargeSum = -1; int nFin = 0; int n85 = 0; int n86 = 0; int n83 = 0; int n84 = 0; // Loop over all particles. for (int i = 0; i < event.size(); ++i) { int status = event[i].statusAbs(); // Find any unrecognized particle codes. int id = event[i].id(); if (id == 0 || !pdt.isParticle(id)) cout << " Error! Unknown code id = " << id << "\n"; // Find particles with E-p mismatch. double eCalc = event[i].eCalc(); if (abs(eCalc/event[i].e() - 1.) > 1e-6) cout << " e mismatch, i = " << i << " e_nominal = " << event[i].e() << " e-from-p = " << eCalc << " m-from-e " << event[i].mCalc() << "\n"; // Parton flow in event plane. if (status == 71 || status == 72) { double thetaXZ = event[i].thetaXZ(); dpartondtheta.fill(thetaXZ); } // Origin of primary hadrons. if (status == 85) ++n85; if (status == 86) ++n86; if (status == 83) ++n83; if (status == 84) ++n84; // Flow of primary hadrons in the event plane. if (status > 80 && status < 90) { double eAbs = event[i].e(); if (eAbs < 0.) {cout << " e < 0 line " << i; event.list();} double thetaXZ = event[i].thetaXZ(); dndtheta.fill(thetaXZ); dedtheta.fill(thetaXZ, eAbs); // Rapidity distribution of primary hadrons. double y = event[i].y(); dndySum.fill(y); if (type >= 6) { int motherId = event[event[i].mother1()].id(); if (motherId > 0 ) dndyJun.fill(event[i].y()); else dndyAnti.fill(event[i].y()); } } // Study final-state particles. if (event[i].isFinal()) { pSum += event[i].p(); chargeSum += event[i].charge(); nFin++; double pAbs = event[i].pAbs(); dnparticledp.fill(pAbs); } } // Fill histograms once for each event. double epDev = abs(pSum.e()) + abs(pSum.px()) + abs(pSum.py()) + abs(pSum.pz()); epCons.fill(epDev); chgCons.fill(chargeSum); nFinal.fill(nFin); status85.fill(n85); status86.fill(n86); status83.fill(n83); status84.fill(n84); if (epDev > 1e-3 || abs(chargeSum) > 0.1) event.list(); // End of event loop. } // Print statistics, histograms and done. pythia.stat(); cout << epCons << chgCons << nFinal << dnparticledp << dndtheta << dedtheta << dpartondtheta << dndySum; if (type >= 4) cout << status85 << status86 << status83 << status84; if (type >= 6) cout << dndyJun << dndyAnti; // Done. return 0; } pythia8-8.1.80.orig/examples/main17.cc0000644000175000017500000001342612217346164015566 0ustar sunsun// main17.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates // (a) how to use UserHooks to regularize onium cross section for pT -> 0, // (b) how decays could be handled externally. #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // A derived class to do J/psi decays. class JpsiDecay : public DecayHandler { public: // Constructor. JpsiDecay(ParticleData* pdtPtrIn, Rndm* rndmPtrIn) {times = 0; pdtPtr = pdtPtrIn; rndmPtr = rndmPtrIn;} // Routine for doing the decay. bool decay(vector& idProd, vector& mProd, vector& pProd, int iDec, const Event& event); private: // Count number of times JpsiDecay is called. int times; // Pointer to the particle data table. ParticleData* pdtPtr; // Pointer to the random number generator. Rndm* rndmPtr; }; //-------------------------------------------------------------------------- // The actual J/psi decay routine. // Not intended for realism, just to illustrate the principles. bool JpsiDecay::decay(vector& idProd, vector& mProd, vector& pProd, int iDec, const Event& event) { // Always do decay J/psi -> mu+ mu-; store the muons. idProd.push_back(-13); idProd.push_back(13); // Muon mass(es), here from Pythia tables, also stored. double mMuon = pdtPtr->m0(13); mProd.push_back(mMuon); mProd.push_back(mMuon); // Calculate muon energy and momentum in J/psi rest frame. double eMuon = 0.5 * mProd[0]; double pAbsMuon = sqrt(eMuon * eMuon - mMuon * mMuon); // Assume decay angles isotropic in rest frame. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(max(0., 1. - cosTheta * cosTheta)); double phi = 2. * M_PI * rndmPtr->flat(); double pxMuon = pAbsMuon * sinTheta * cos(phi); double pyMuon = pAbsMuon * sinTheta * sin(phi); double pzMuon = pAbsMuon * cosTheta; // Define mu+ and mu- four-vectors in the J/psi rest frame. Vec4 pMuPlus( pxMuon, pyMuon, pzMuon, eMuon); Vec4 pMuMinus( -pxMuon, -pyMuon, -pzMuon, eMuon); // Boost them by velocity vector of the J/psi mother and store. pMuPlus.bst(pProd[0]); pMuMinus.bst(pProd[0]); pProd.push_back(pMuPlus); pProd.push_back(pMuMinus); // Print message the first few times, to show that it works. if (times++ < 10) { int iMother = event[iDec].mother1(); int idMother = event[iMother].id(); cout << "\n J/psi decay performed, J/psi in line " << iDec << ", mother id = " << idMother << "\n"; } // Done return true; } //========================================================================== int main() { // Number of events to generate and to list. Max number of errors. int nEvent = 2000; int nList = 2; int nAbort = 5; // Pythia generator. Pythia pythia; // Initialization for charmonium (singlet+octet) production at the LHC. pythia.readString("Charmonium:all = on"); pythia.readString("Beams:eCM = 7000."); // Normally cutoff at pTHat = 1, but push it lower combined with dampening. pythia.readString("PhaseSpace:pTHatMin = 0.5"); pythia.readString("PhaseSpace:pTHatMinDiverge = 0.5"); // Set up to do a user veto and send it in. // First argument: multiplies the pT0 of multiparton interactions // to define the pT dampeing scale. // Second argument: howe many powers of alpha_strong to // reweight with new (larger) argument. // Third argument: choice of process scale two different ways; // probably does not make much difference. // See "User Hooks" in manual for detail on SuppressSmallPT. UserHooks* oniumUserHook = new SuppressSmallPT( 1., 3, false); pythia.setUserHooksPtr( oniumUserHook); // A class to do J/psi decays externally. DecayHandler* handleDecays = new JpsiDecay(&pythia.particleData, &pythia.rndm); // The list of particles the class can handle. vector handledParticles; handledParticles.push_back(443); // Hand pointer and list to Pythia. pythia.setDecayPtr( handleDecays, handledParticles); // Switch off automatic event listing in favour of manual. pythia.readString("Next:numberShowInfo = 0"); pythia.readString("Next:numberShowProcess = 0"); pythia.readString("Next:numberShowEvent = 0"); // Initialization. pythia.init(); // Book histograms. Hist pThard("pTHat of hard subprocess", 100, 0., 50.); Hist pTJPsi("pT of J/Psi", 100, 0., 50.); // Begin event loop. int iList = 0; int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if many failures. if (!pythia.next()) { if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Histogram pThard spectrum of process. double pTHat = pythia.info.pTHat(); pThard.fill( pTHat ); // Look for event with externally handled decays. bool externalDecay = false; for (int i = 0; i < pythia.event.size(); ++i) { int status = pythia.event[i].statusAbs(); if (status == 93 || status == 94) {externalDecay = true; break;} } // List first few events with external decay. if (externalDecay && ++iList <= nList) { pythia.process.list(); pythia.event.list(); } // Histogram pT spectrum of J/Psi. for (int i = 0; i < pythia.event.size(); ++i) if (pythia.event[i].id() == 443) pTJPsi.fill( pythia.event[i].pT() ); // End of event loop. } // Final statistics. Print histograms. pythia.stat(); cout << pThard << pTJPsi; // Done. delete handleDecays; delete oniumUserHook; return 0; } pythia8-8.1.80.orig/examples/GeneratorInput.h0000644000175000017500000012054212217346163017277 0ustar sunsun// GeneratorInput.h is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Primary Author: Richard Corke // Secondary Author: Stephen Mrenna // This file provides the following classes: // AlpgenPar: a class for parsing ALPGEN parameter files // and reading back out the values // LHAupAlpgen: an LHAup derived class for reading in ALPGEN // format event files // AlpgenHooks: a UserHooks derived class for providing // 'Alpgen:*' user options // MadgraphPar: a class for parsing MadGraph parameter files // and reading back out the values // Example usage is shown in main32.cc, and further details // can be found in the 'Jet Matching Style' manual page. // Minor changes were made by the secondary author for integration // with Madgraph-style matching, and Madgraph input was added. #ifndef Pythia8_GeneratorInput_H #define Pythia8_GeneratorInput_H // Includes and namespace #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // AlpgenPar: Class to parse ALPGEN parameter files and make them // available through a simple interface class AlpgenPar { public: // Constructor AlpgenPar(Info *infoPtrIn = NULL) : infoPtr(infoPtrIn) {} // Parse as incoming ALPGEN parameter file (passed as string) bool parse(const string paramStr); // Parse an incoming parameter line void extractRunParam(string line); // Check if a parameter exists bool haveParam(const string ¶mIn) { return (params.find(paramIn) == params.end()) ? false : true; } // Get a parameter as a double or integer. // Caller should have already checked existance of the parameter. double getParam(const string ¶mIn) { return (haveParam(paramIn)) ? params[paramIn] : 0.; } int getParamAsInt(const string ¶mIn) { return (haveParam(paramIn)) ? int(params[paramIn]) : 0.; } // Print parameters read from the '.par' file void printParams(); private: // Warn if a parameter is going to be overwriten void warnParamOverwrite(const string ¶mIn, double val); // Simple string trimmer static string trim(string s); // Storage for parameters map params; // Info pointer if provided Info* infoPtr; // Constants static const double ZEROTHRESHOLD; }; //========================================================================== // LHAupAlpgen: LHAup derived class for reading in ALPGEN format // event files. class LHAupAlpgen : public LHAup { public: // Constructor and destructor. LHAupAlpgen(const char *baseFNin, Info *infoPtrIn = NULL); ~LHAupAlpgen() { closeFile(isUnw, ifsUnw); } // Override fileFound routine from LHAup. bool fileFound() { return (isUnw != NULL); } // Override setInit/setEvent routines from LHAup. bool setInit(); bool setEvent(int, double); // Print list of particles; mainly intended for debugging void printParticles(); private: // Add resonances to incoming event. bool addResonances(); // Rescale momenta to remove any imbalances. bool rescaleMomenta(); // Class variables string baseFN, parFN, unwFN; // Incoming filenames AlpgenPar alpgenPar; // Parameter database int lprup; // Process code double ebmupA, ebmupB; // Beam energies int ihvy1, ihvy2; // Heavy flavours for certain processes double mb; // Bottom mass ifstream ifsUnw; // Input file stream for 'unw' file istream* isUnw; // Input stream for 'unw' file vector myParticles; // Local storage for particles // Constants static const bool LHADEBUG, LHADEBUGRESCALE; static const double ZEROTHRESHOLD, EWARNTHRESHOLD, PTWARNTHRESHOLD, INCOMINGMIN; }; //========================================================================== // AlpgenHooks: provides Alpgen file reading options. // Note that it is defined with virtual inheritance, so that it can // be combined with other UserHooks classes, see e.g. main32.cc. class AlpgenHooks : virtual public UserHooks { public: // Constructor and destructor AlpgenHooks(Pythia &pythia); ~AlpgenHooks() { if (LHAagPtr) delete LHAagPtr; } // Override initAfterBeams routine from UserHooks bool initAfterBeams(); private: // LHAupAlpgen pointer LHAupAlpgen* LHAagPtr; }; //========================================================================== // MadgraphPar: Class to parse the Madgraph header parameters and // make them available through a simple interface class MadgraphPar { public: // Constructor MadgraphPar(Info *infoPtrIn = NULL) : infoPtr(infoPtrIn) {} // Parse an incoming Madgraph parameter file string bool parse(const string paramStr); // Parse an incoming parameter line void extractRunParam(string line); // Check if a parameter exists bool haveParam(const string ¶mIn) { return (params.find(paramIn) == params.end()) ? false : true; } // Get a parameter as a double or integer. // Caller should have already checked existance of the parameter. double getParam(const string ¶mIn) { return (haveParam(paramIn)) ? params[paramIn] : 0.; } int getParamAsInt(const string ¶mIn) { return (haveParam(paramIn)) ? int(params[paramIn]) : 0.; } // Print parameters read from the '.par' file void printParams(); private: // Warn if a parameter is going to be overwriten void warnParamOverwrite(const string ¶mIn, double val); // Simple string trimmer static string trim(string s); // Storage for parameters map params; // Info pointer if provided Info *infoPtr; // Constants static const double ZEROTHRESHOLD; }; //========================================================================== // Main implementation of AlpgenPar class. // This may be split out to a separate C++ file if desired, // but currently included here for ease of use. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // A zero threshold value for double comparisons. const double AlpgenPar::ZEROTHRESHOLD = 1e-10; //-------------------------------------------------------------------------- // Warn if e/pT imbalance greater than these values // Parse an incoming Alpgen parameter file string bool AlpgenPar::parse(const string paramStr) { // Read par file in blocks: // 0 - process information // 1 - run parameters // 2 - cross sections int block = 0; // Loop over incoming lines stringstream paramStream(paramStr); string line; while (getline(paramStream, line)) { // Change to 'run parameters' block if (line.find("run parameters") != string::npos) { block = 1; // End of 'run parameters' block } else if (line.find("end parameters") != string::npos) { block = 2; // Do not extract anything from block 0 so far } else if (block == 0) { // Block 1 or 2: extract parameters } else { extractRunParam(line); } } // while (getline(paramStream, line)) return true; } //-------------------------------------------------------------------------- // Parse an incoming parameter line void AlpgenPar::extractRunParam(string line) { // Extract information to the right of the final '!' character size_t idx = line.rfind("!"); if (idx == string::npos) return; string paramName = trim(line.substr(idx + 1)); string paramVal = trim(line.substr(0, idx)); istringstream iss(paramVal); // Special case: 'hard process code' - single integer input double val; if (paramName == "hard process code") { iss >> val; warnParamOverwrite("hpc", val); params["hpc"] = val; // Special case: 'Crosssection +- error (pb)' - two double values } else if (paramName.find("Crosssection") == 0) { double xerrup; iss >> val >> xerrup; warnParamOverwrite("xsecup", val); warnParamOverwrite("xerrup", val); params["xsecup"] = val; params["xerrup"] = xerrup; // Special case: 'unwtd events, lum (pb-1)' - integer and double values } else if (paramName.find("unwtd events") == 0) { int nevent; iss >> nevent >> val; warnParamOverwrite("nevent", val); warnParamOverwrite("lum", val); params["nevent"] = nevent; params["lum"] = val; // Special case: 'mc,mb,...' - split on ',' for name and ' ' for values } else if (paramName.find(",") != string::npos) { // Simple tokeniser string paramNameNow; istringstream issName(paramName); while (getline(issName, paramNameNow, ',')) { iss >> val; warnParamOverwrite(paramNameNow, val); params[paramNameNow] = val; } // Default case: assume integer and double on the left } else { int paramIdx; iss >> paramIdx >> val; warnParamOverwrite(paramName, val); params[paramName] = val; } } //-------------------------------------------------------------------------- // Print parameters read from the '.par' file void AlpgenPar::printParams() { // Loop over all stored parameters and print cout << fixed << setprecision(3) << endl << " *------- Alpgen parameters -------*" << endl; for (map < string, double >::iterator it = params.begin(); it != params.end(); ++it) cout << " | " << left << setw(13) << it->first << " | " << right << setw(13) << it->second << " |" << endl; cout << " *-----------------------------------*" << endl; } //-------------------------------------------------------------------------- // Warn if a parameter is going to be overwriten void AlpgenPar::warnParamOverwrite(const string ¶mIn, double val) { // Check if present and if new value is different if (haveParam(paramIn) && abs(getParam(paramIn) - val) > ZEROTHRESHOLD) { if (infoPtr) infoPtr->errorMsg("Warning in LHAupAlpgen::" "warnParamOverwrite: overwriting existing parameter", paramIn); } } //-------------------------------------------------------------------------- // Simple string trimmer string AlpgenPar::trim(string s) { // Remove whitespace in incoming string size_t i; if ((i = s.find_last_not_of(" \t\r\n")) != string::npos) s = s.substr(0, i + 1); if ((i = s.find_first_not_of(" \t\r\n")) != string::npos) s = s.substr(i); return s; } //========================================================================== // Main implementation of LHAupAlpgen class. // This may be split out to a separate C++ file if desired, // but currently included here for ease of use. // ---------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Debug flag to print all particles in each event. const bool LHAupAlpgen::LHADEBUG = false; // Debug flag to print particles when an e/p imbalance is found. const bool LHAupAlpgen::LHADEBUGRESCALE = false; // A zero threshold value for double comparisons. const double LHAupAlpgen::ZEROTHRESHOLD = 1e-10; // Warn if e/pT imbalance greater than these values const double LHAupAlpgen::EWARNTHRESHOLD = 3e-3; const double LHAupAlpgen::PTWARNTHRESHOLD = 1e-3; // If incoming e/pZ is 0, it is reset to this value const double LHAupAlpgen::INCOMINGMIN = 1e-3; // ---------------------------------------------------------------------- // Constructor. Opens parameter file and parses then opens event file. LHAupAlpgen::LHAupAlpgen(const char* baseFNin, Info* infoPtrIn) : baseFN(baseFNin), alpgenPar(infoPtrIn), isUnw(NULL) { // Set the info pointer if given if (infoPtrIn) setPtr(infoPtrIn); // Read in '_unw.par' file to get parameters ifstream ifsPar; istream* isPar = NULL; // Try gzip file first then normal file afterwards #ifdef GZIPSUPPORT parFN = baseFN + "_unw.par.gz"; isPar = openFile(parFN.c_str(), ifsPar); if (!ifsPar.is_open()) closeFile(isPar, ifsPar); #endif if (isPar == NULL) { parFN = baseFN + "_unw.par"; isPar = openFile(parFN.c_str(), ifsPar); if (!ifsPar.is_open()) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::LHAupAlpgen: " "cannot open parameter file", parFN); closeFile(isPar, ifsPar); return; } } // Read entire contents into string and close file string paramStr((istreambuf_iterator(isPar->rdbuf())), istreambuf_iterator()); // Make sure we reached EOF and not other error if (ifsPar.bad()) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::LHAupAlpgen: " "cannot read parameter file", parFN); return; } closeFile(isPar, ifsPar); // Parse file and set LHEF header alpgenPar.parse(paramStr); if (infoPtr) setInfoHeader("AlpgenPar", paramStr); // Open '.unw' events file (with possible gzip support) #ifdef GZIPSUPPORT unwFN = baseFN + ".unw.gz"; isUnw = openFile(unwFN.c_str(), ifsUnw); if (!ifsUnw.is_open()) closeFile(isUnw, ifsUnw); #endif if (isUnw == NULL) { unwFN = baseFN + ".unw"; isUnw = openFile(unwFN.c_str(), ifsUnw); if (!ifsUnw.is_open()) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::LHAupAlpgen: " "cannot open event file", unwFN); closeFile(isUnw, ifsUnw); } } } // ---------------------------------------------------------------------- // setInit is a virtual method that must be finalised here. // Sets up beams, strategy and processes. bool LHAupAlpgen::setInit() { // Check that all required parameters are present if (!alpgenPar.haveParam("ih2") || !alpgenPar.haveParam("ebeam") || !alpgenPar.haveParam("hpc") || !alpgenPar.haveParam("xsecup") || !alpgenPar.haveParam("xerrup")) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::setInit: " "missing input parameters"); return false; } // Beam IDs int ih2 = alpgenPar.getParamAsInt("ih2"); int idbmupA = 2212; int idbmupB = (ih2 == 1) ? 2212 : -2212; // Beam energies double ebeam = alpgenPar.getParam("ebeam"); ebmupA = ebeam; ebmupB = ebmupA; // PDF group and set (at the moment not set) int pdfgupA = 0, pdfsupA = 0; int pdfgupB = 0, pdfsupB = 0; // Strategy is for unweighted events and xmaxup not important int idwtup = 3; double xmaxup = 0.; // Get hard process code lprup = alpgenPar.getParamAsInt("hpc"); // Check for unsupported processes if (lprup == 7 || lprup == 8 || lprup == 13) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::setInit: " "process not implemented"); return false; } // Depending on the process code, get heavy flavour information: // 6 = QQbar + jets // 7 = QQbar + Q'Qbar' + jets // 8 = QQbar + Higgs + jets // 16 = QQbar + gamma + jets if (lprup == 6 || lprup == 7 || lprup == 8 || lprup == 16) { if (!alpgenPar.haveParam("ihvy")) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::setInit: " "heavy flavour information not present"); return false; } ihvy1 = alpgenPar.getParamAsInt("ihvy"); } else ihvy1 = -1; if (lprup == 7) { if (!alpgenPar.haveParam("ihvy2")) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::setInit: " "heavy flavour information not present"); return false; } ihvy2 = alpgenPar.getParamAsInt("ihvy2"); } else ihvy2 = -1; // For single top (process 13), get b mass to set incoming mb = -1.; if (lprup == 13) { if (!alpgenPar.haveParam("mb")) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::setInit: " "heavy flavour information not present"); return false; } mb = alpgenPar.getParam("mb"); } // Set the beams setBeamA(idbmupA, ebmupA, pdfgupA, pdfsupA); setBeamB(idbmupB, ebmupB, pdfgupB, pdfsupB); setStrategy(idwtup); // Add the process double xsecup = alpgenPar.getParam("xsecup"); double xerrup = alpgenPar.getParam("xerrup"); addProcess(lprup, xsecup, xerrup, xmaxup); xSecSumSave = xsecup; xErrSumSave = xerrup; // All okay return true; } // ---------------------------------------------------------------------- // setEvent is a virtual method that must be finalised here. // Read in an event from the 'unw' file and setup. bool LHAupAlpgen::setEvent(int, double) { // Read in the first line of the event int nEvent, iProc, nParton; double Swgt, Sq; string line; if (!getline(*isUnw, line)) { // Read was bad if (ifsUnw.bad()) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::setEvent: " "could not read events from file"); return false; } // End of file reached if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::setEvent: " "end of file reached"); return false; } istringstream iss1(line); iss1 >> nEvent >> iProc >> nParton >> Swgt >> Sq; // Set the process details (ignore alphaQED and alphaQCD parameters) double wgtT = Swgt, scaleT = Sq; setProcess(lprup, wgtT, scaleT); // Incoming flavour and x information for later int id1T, id2T; double x1T, x2T; // Temporary storage for read in parton information int idT, statusT, mother1T, mother2T, col1T, col2T; double pxT, pyT, pzT, eT, mT; // Leave tau and spin as default values double tauT = 0., spinT = 9.; // Store particles locally at first so that resonances can be added myParticles.clear(); // Now read in partons for (int i = 0; i < nParton; i++) { // Get the next line if (!getline(*isUnw, line)) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::setEvent: " "could not read events from file"); return false; } istringstream iss2(line); // Incoming (flavour, colour, anticolour, pz) if (i < 2) { // Note that mothers will be set automatically by Pythia, and LHA // status -1 is for an incoming parton iss2 >> idT >> col1T >> col2T >> pzT; statusT = -1; mother1T = mother2T = 0; pxT = pyT = mT = 0.; eT = abs(pzT); // Adjust when zero pz/e if (pzT == 0.) { pzT = (i == 0) ? INCOMINGMIN : -INCOMINGMIN; eT = INCOMINGMIN; } // Outgoing (flavour, colour, anticolour, px, py, pz, mass) } else { // Note that mothers 1 and 2 corresport to the incoming partons, // as set above, and LHA status +1 is for outgoing final state iss2 >> idT >> col1T >> col2T >> pxT >> pyT >> pzT >> mT; statusT = 1; mother1T = 1; mother2T = 2; eT = sqrt(max(0., pxT*pxT + pyT*pyT + pzT*pzT + mT*mT)); } // Add particle myParticles.push_back(LHAParticle( idT, statusT, mother1T, mother2T, col1T, col2T, pxT, pyT, pzT, eT, mT, tauT, spinT,-1.)); } // Add resonances if required if (!addResonances()) return false; // Rescale momenta if required (must be done after full event // reconstruction in addResonances) if (!rescaleMomenta()) return false; // Pass particles on to Pythia for (size_t i = 0; i < myParticles.size(); i++) addParticle(myParticles[i]); // Set incoming flavour/x information and done id1T = myParticles[0].idPart; x1T = myParticles[0].ePart / ebmupA; id2T = myParticles[1].idPart; x2T = myParticles[1].ePart / ebmupA; setIdX(id1T, id2T, x1T, x2T); setPdf(id1T, id2T, x1T, x2T, 0., 0., 0., false); return true; } // ---------------------------------------------------------------------- // Print list of particles; mainly intended for debugging void LHAupAlpgen::printParticles() { cout << endl << "---- LHAupAlpgen particle listing begin ----" << endl; cout << scientific << setprecision(6); for (int i = 0; i < int(myParticles.size()); i++) { cout << setw(5) << i << setw(5) << myParticles[i].idPart << setw(5) << myParticles[i].statusPart << setw(15) << myParticles[i].pxPart << setw(15) << myParticles[i].pyPart << setw(15) << myParticles[i].pzPart << setw(15) << myParticles[i].ePart << setw(15) << myParticles[i].mPart << setw(5) << myParticles[i].mother1Part - 1 << setw(5) << myParticles[i].mother2Part - 1 << setw(5) << myParticles[i].col1Part << setw(5) << myParticles[i].col2Part << endl; } cout << "---- LHAupAlpgen particle listing end ----" << endl; } // ---------------------------------------------------------------------- // Routine to add resonances to an incoming event based on the // hard process code (now stored in lprup). bool LHAupAlpgen::addResonances() { // Temporary storage for resonance information int idT, statusT, mother1T, mother2T, col1T, col2T; double pxT, pyT, pzT, eT, mT; // Leave tau and spin as default values double tauT = 0., spinT = 9.; // Alpgen process dependent parts. Processes: // 1 = W + QQbar + jets // 2 = Z/gamma* + QQbar + jets // 3 = W + jets // 4 = Z/gamma* + jets // 10 = W + c + jets // 14 = W + gamma + jets // 15 = W + QQbar + gamma + jets // When QQbar = ttbar, tops are not decayed in these processes. // Explicitly reconstruct W/Z resonances; assumption is that the // decay products are the last two particles. if (lprup <= 4 || lprup == 10 || lprup == 14 || lprup == 15) { // Decay products are the last two entries int i1 = myParticles.size() - 1, i2 = i1 - 1; // Follow 'alplib/alpsho.f' procedure to get ID if (myParticles[i1].idPart + myParticles[i2].idPart == 0) idT = 0; else idT = - (myParticles[i1].idPart % 2) - (myParticles[i2].idPart % 2); idT = (idT > 0) ? 24 : (idT < 0) ? -24 : 23; // Check that we get the expected resonance type; Z/gamma* if (lprup == 2 || lprup == 4) { if (idT != 23) { if (infoPtr) infoPtr->errorMsg("Error in " "LHAupAlpgen::addResonances: wrong resonance type in event"); return false; } // W's } else { if (abs(idT) != 24) { if (infoPtr) infoPtr->errorMsg("Error in " "LHAupAlpgen::addResonances: wrong resonance type in event"); return false; } } // Remaining input statusT = 2; mother1T = 1; mother2T = 2; col1T = col2T = 0; pxT = myParticles[i1].pxPart + myParticles[i2].pxPart; pyT = myParticles[i1].pyPart + myParticles[i2].pyPart; pzT = myParticles[i1].pzPart + myParticles[i2].pzPart; eT = myParticles[i1].ePart + myParticles[i2].ePart; mT = sqrt(eT*eT - pxT*pxT - pyT*pyT - pzT*pzT); myParticles.push_back(LHAParticle( idT, statusT, mother1T, mother2T, col1T, col2T, pxT, pyT, pzT, eT, mT, tauT, spinT, -1.)); // Update decay product mothers (note array size as if from 1) myParticles[i1].mother1Part = myParticles[i2].mother1Part = myParticles.size(); myParticles[i1].mother2Part = myParticles[i2].mother2Part = 0; // Processes: // 5 = nW + mZ + j gamma + lH + jets // 6 = QQbar + jets (QQbar = ttbar) // 8 = QQbar + Higgs + jets (QQbar = ttbar) // 13 = top + q (topprc = 1) // 13 = top + b (topprc = 2) // 13 = top + W + jets (topprc = 3) // 13 = top + W + b (topprc = 4) // 16 = QQbar + gamma + jets (QQbar = ttbar) // // When tops are present, they are decayed to Wb (both the W and b // are not given), with this W also decaying (decay products given). // The top is marked intermediate, the (intermediate) W is // reconstructed from its decay products, and the decay product mothers // updated. The final-state b is reconstructed from (top - W). // // W/Z resonances are given, as well as their decay products. The // W/Z is marked intermediate, and the decay product mothers updated. // // It is always assumed that decay products are at the end. // For processes 5 and 13, it is also assumed that the decay products // are in the same order as the resonances. // For processes 6, 8 and 16, the possibility of the decay products // being out-of-order is also taken into account. } else if ( ((lprup == 6 || lprup == 8 || lprup == 16) && ihvy1 == 6) || lprup == 5 || lprup == 13) { // Go backwards through the particles looking for W/Z/top int idx = myParticles.size() - 1; for (int i = myParticles.size() - 1; i > -1; i--) { // W or Z if (myParticles[i].idPart == 23 || abs(myParticles[i].idPart) == 24) { // Check that decay products and resonance match up int flav; if (myParticles[idx].idPart + myParticles[idx - 1].idPart == 0) flav = 0; else flav = - (myParticles[idx].idPart % 2) - (myParticles[idx - 1].idPart % 2); flav = (flav > 0) ? 24 : (flav < 0) ? -24 : 23; if (flav != myParticles[i].idPart) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::addResonance: " "resonance does not match decay products"); return false; } // Update status/mothers myParticles[i].statusPart = 2; myParticles[idx ].mother1Part = i + 1; myParticles[idx--].mother2Part = 0; myParticles[idx ].mother1Part = i + 1; myParticles[idx--].mother2Part = 0; // Top } else if (abs(myParticles[i].idPart) == 6) { // Check that decay products and resonance match up int flav; if (myParticles[idx].idPart + myParticles[idx - 1].idPart == 0) flav = 0; else flav = - (myParticles[idx].idPart % 2) - (myParticles[idx - 1].idPart % 2); flav = (flav > 0) ? 24 : (flav < 0) ? -24 : 23; bool outOfOrder = false, wrongFlavour = false;; if ( abs(flav) != 24 || (flav == 24 && myParticles[i].idPart != 6) || (flav == -24 && myParticles[i].idPart != -6) ) { // Processes 5 and 13, order should always be correct if (lprup == 5 || lprup == 13) { wrongFlavour = true; // Processes 6, 8 and 16, can have out of order decay products } else { // Go back two decay products and retry idx -= 2; if (myParticles[idx].idPart + myParticles[idx - 1].idPart == 0) flav = 0; else flav = - (myParticles[idx].idPart % 2) - (myParticles[idx - 1].idPart % 2); flav = (flav > 0) ? 24 : (flav < 0) ? -24 : 23; // If still the wrong flavour then error if ( abs(flav) != 24 || (flav == 24 && myParticles[i].idPart != 6) || (flav == -24 && myParticles[i].idPart != -6) ) wrongFlavour = true; else outOfOrder = true; } // Error if wrong flavour if (wrongFlavour) { if (infoPtr) infoPtr->errorMsg("Error in LHAupAlpgen::addResonance: " "resonance does not match decay products"); return false; } } // Mark t/tbar as now intermediate myParticles[i].statusPart = 2; // New intermediate W+/W- idT = flav; statusT = 2; mother1T = i + 1; mother2T = 0; col1T = col2T = 0; pxT = myParticles[idx].pxPart + myParticles[idx - 1].pxPart; pyT = myParticles[idx].pyPart + myParticles[idx - 1].pyPart; pzT = myParticles[idx].pzPart + myParticles[idx - 1].pzPart; eT = myParticles[idx].ePart + myParticles[idx - 1].ePart; mT = sqrt(eT*eT - pxT*pxT - pyT*pyT - pzT*pzT); myParticles.push_back(LHAParticle( idT, statusT, mother1T, mother2T, col1T, col2T, pxT, pyT, pzT, eT, mT, tauT, spinT, -1.)); // Update the decay product mothers myParticles[idx ].mother1Part = myParticles.size(); myParticles[idx--].mother2Part = 0; myParticles[idx ].mother1Part = myParticles.size(); myParticles[idx--].mother2Part = 0; // New final-state b/bbar idT = (flav == 24) ? 5 : -5; statusT = 1; // Colour from top col1T = myParticles[i].col1Part; col2T = myParticles[i].col2Part; // Momentum from (t/tbar - W+/W-) pxT = myParticles[i].pxPart - myParticles.back().pxPart; pyT = myParticles[i].pyPart - myParticles.back().pyPart; pzT = myParticles[i].pzPart - myParticles.back().pzPart; eT = myParticles[i].ePart - myParticles.back().ePart; mT = sqrt(eT*eT - pxT*pxT - pyT*pyT - pzT*pzT); myParticles.push_back(LHAParticle( idT, statusT, mother1T, mother2T, col1T, col2T, pxT, pyT, pzT, eT, mT, tauT, spinT, -1.)); // If decay products were out of order, reset idx to point // at correct decay products if (outOfOrder) idx += 4; } // if (abs(myParticles[i].idPart) == 6) } // for (i) // Processes: // 7 = QQbar + Q'Qbar' + jets (tops are not decayed) // 9 = jets // 11 = gamma + jets // 12 = Higgs + jets } else if (lprup == 7 || lprup == 9 || lprup == 11 || lprup == 12) { // Nothing to do for these processes } // For single top, set incoming b mass if necessary if (lprup == 13) for (int i = 0; i < 2; i++) if (abs(myParticles[i].idPart) == 5) { myParticles[i].mPart = mb; myParticles[i].ePart = sqrt(pow2(myParticles[i].pzPart) + pow2(mb)); } // Debug output and done. if (LHADEBUG) printParticles(); return true; } // ---------------------------------------------------------------------- // Routine to rescale momenta to remove any imbalances. The routine // assumes that any imbalances are due to decimal output/rounding // effects, and are therefore small. // // First any px/py imbalances are fixed by adjusting all outgoing // particles px/py and also updating their energy so mass is fixed. // Because incoming pT is zero, changes should be limited to ~0.001. // // Second, any pz/e imbalances are fixed by scaling the incoming beams // (again, no changes to masses required). Because incoming pz/e is not // zero, effects can be slightly larger ~0.002/0.003. bool LHAupAlpgen::rescaleMomenta() { // Total momenta in/out int nOut = 0; Vec4 pIn, pOut; for (int i = 0; i < int(myParticles.size()); i++) { Vec4 pNow = Vec4(myParticles[i].pxPart, myParticles[i].pyPart, myParticles[i].pzPart, myParticles[i].ePart); if (i < 2) pIn += pNow; else if (myParticles[i].statusPart == 1) { nOut++; pOut += pNow; } } // pT out to match pT in. Split any imbalances over all outgoing // particles, and scale energies also to keep m^2 fixed. if (abs(pOut.pT() - pIn.pT()) > ZEROTHRESHOLD) { // Differences in px/py double pxDiff = (pOut.px() - pIn.px()) / nOut, pyDiff = (pOut.py() - pIn.py()) / nOut; // Warn if resulting changes above warning threshold if (pxDiff > PTWARNTHRESHOLD || pyDiff > PTWARNTHRESHOLD) { if (infoPtr) infoPtr->errorMsg("Warning in LHAupAlpgen::setEvent: " "large pT imbalance in incoming event"); // Debug printout if (LHADEBUGRESCALE) { printParticles(); cout << "pxDiff = " << pxDiff << ", pyDiff = " << pyDiff << endl; } } // Adjust all final-state outgoing pOut.reset(); for (int i = 2; i < int(myParticles.size()); i++) { if (myParticles[i].statusPart != 1) continue; myParticles[i].pxPart -= pxDiff; myParticles[i].pyPart -= pyDiff; myParticles[i].ePart = sqrt(max(0., pow2(myParticles[i].pxPart) + pow2(myParticles[i].pyPart) + pow2(myParticles[i].pzPart) + pow2(myParticles[i].mPart))); pOut += Vec4(myParticles[i].pxPart, myParticles[i].pyPart, myParticles[i].pzPart, myParticles[i].ePart); } } // Differences in E/pZ and scaling factors double de = (pOut.e() - pIn.e()); double dp = (pOut.pz() - pIn.pz()); double a = 1 + (de + dp) / 2. / myParticles[0].ePart; double b = 1 + (de - dp) / 2. / myParticles[1].ePart; // Warn if resulting energy changes above warning threshold. // Change in pz less than or equal to change in energy (incoming b // quark can have mass at this stage for process 13). Note that for // very small incoming momenta, the relative adjustment may be large, // but still small in absolute terms. if (abs(a - 1.) * myParticles[0].ePart > EWARNTHRESHOLD || abs(b - 1.) * myParticles[1].ePart > EWARNTHRESHOLD) { if (infoPtr) infoPtr->errorMsg("Warning in LHAupAlpgen::setEvent: " "large rescaling factor"); // Debug printout if (LHADEBUGRESCALE) { printParticles(); cout << "de = " << de << ", dp = " << dp << ", a = " << a << ", b = " << b << endl << "Absolute energy change for incoming 0 = " << abs(a - 1.) * myParticles[0].ePart << endl << "Absolute energy change for incoming 1 = " << abs(b - 1.) * myParticles[1].ePart << endl; } } myParticles[0].ePart *= a; myParticles[0].pzPart *= a; myParticles[1].ePart *= b; myParticles[1].pzPart *= b; // Recalculate resonance four vectors for (int i = 0; i < int(myParticles.size()); i++) { if (myParticles[i].statusPart != 2) continue; // Only mothers stored in LHA, so go through all Vec4 resVec; for (int j = 0; j < int(myParticles.size()); j++) { if (myParticles[j].mother1Part - 1 != i) continue; resVec += Vec4(myParticles[j].pxPart, myParticles[j].pyPart, myParticles[j].pzPart, myParticles[j].ePart); } myParticles[i].pxPart = resVec.px(); myParticles[i].pyPart = resVec.py(); myParticles[i].pzPart = resVec.pz(); myParticles[i].ePart = resVec.e(); } return true; } //========================================================================== // Main implementation of AlpgenHooks class. // This may be split out to a separate C++ file if desired, // but currently included here for ease of use. // ---------------------------------------------------------------------- // Constructor: provides the 'Alpgen:file' option by directly // changing the Pythia 'Beams' settings AlpgenHooks::AlpgenHooks(Pythia &pythia) : LHAagPtr(NULL) { // If LHAupAlpgen needed, construct and pass to Pythia string agFile = pythia.settings.word("Alpgen:file"); if (agFile != "void") { LHAagPtr = new LHAupAlpgen(agFile.c_str(), &pythia.info); pythia.settings.mode("Beams:frameType", 5); pythia.setLHAupPtr(LHAagPtr); } } // ---------------------------------------------------------------------- // Initialisation routine which is called by pythia.init(). // This happens after the local pointers have been assigned and after // Pythia has processed the Beam information (and therefore LHEF header // information has been read in), but before any other internal // initialisation. Provides the remaining 'Alpgen:*' options. bool AlpgenHooks::initAfterBeams() { // Read in ALPGEN specific configuration variables bool setMasses = settingsPtr->flag("Alpgen:setMasses"); bool setNjet = settingsPtr->flag("Alpgen:setNjet"); bool setMLM = settingsPtr->flag("Alpgen:setMLM"); // If ALPGEN parameters are present, then parse in AlpgenPar object AlpgenPar par(infoPtr); string parStr = infoPtr->header("AlpgenPar"); if (!parStr.empty()) { par.parse(parStr); par.printParams(); } // Set masses if requested if (setMasses) { if (par.haveParam("mc")) particleDataPtr->m0(4, par.getParam("mc")); if (par.haveParam("mb")) particleDataPtr->m0(5, par.getParam("mb")); if (par.haveParam("mt")) particleDataPtr->m0(6, par.getParam("mt")); if (par.haveParam("mz")) particleDataPtr->m0(23, par.getParam("mz")); if (par.haveParam("mw")) particleDataPtr->m0(24, par.getParam("mw")); if (par.haveParam("mh")) particleDataPtr->m0(25, par.getParam("mh")); } // Set MLM:nJets if requested if (setNjet) { if (par.haveParam("njets")) settingsPtr->mode("JetMatching:nJet", par.getParamAsInt("njets")); else infoPtr->errorMsg("Warning in AlpgenHooks:init: " "no ALPGEN nJet parameter found"); } // Set MLM merging parameters if requested if (setMLM) { if (par.haveParam("ptjmin") && par.haveParam("drjmin") && par.haveParam("etajmax")) { double ptjmin = par.getParam("ptjmin"); ptjmin = max(ptjmin + 5., 1.2 * ptjmin); settingsPtr->parm("JetMatching:eTjetMin", ptjmin); settingsPtr->parm("JetMatching:coneRadius", par.getParam("drjmin")); settingsPtr->parm("JetMatching:etaJetMax", par.getParam("etajmax")); // Warn if setMLM requested, but parameters not present } else { infoPtr->errorMsg("Warning in AlpgenHooks:init: " "no ALPGEN merging parameters found"); } } // Initialisation complete. return true; } //========================================================================== // Main implementation of MadgraphPar class. // This may be split out to a separate C++ file if desired, // but currently included here for ease of use. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // A zero threshold value for double comparisons. const double MadgraphPar::ZEROTHRESHOLD = 1e-10; //-------------------------------------------------------------------------- // Parse an incoming Madgraph parameter file string bool MadgraphPar::parse(const string paramStr) { // Loop over incoming lines stringstream paramStream(paramStr); string line; while ( getline(paramStream, line) ) extractRunParam(line); return true; } //-------------------------------------------------------------------------- // Parse an incoming parameter line void MadgraphPar::extractRunParam(string line) { // Extract information to the right of the final '!' character size_t idz = line.find("#"); if ( !(idz == string::npos) ) return; size_t idx = line.find("="); size_t idy = line.find("!"); if (idy == string::npos) idy = line.size(); if (idx == string::npos) return; string paramName = trim( line.substr( idx + 1, idy - idx - 1) ); string paramVal = trim( line.substr( 0, idx) ); replace( paramVal.begin(), paramVal.end(), 'd', 'e'); // Simple tokeniser istringstream iss(paramVal); double val; if (paramName.find(",") != string::npos) { string paramNameNow; istringstream issName( paramName); while ( getline(issName, paramNameNow, ',') ) { iss >> val; warnParamOverwrite( paramNameNow, val); params[paramNameNow] = val; } // Default case: assume integer and double on the left } else { iss >> val; warnParamOverwrite( paramName, val); params[paramName] = val; } } //-------------------------------------------------------------------------- // Print parameters read from the '.par' file void MadgraphPar::printParams() { // Loop over all stored parameters and print cout << endl << " *-------- Madgraph parameters --------*" << endl; for (map::iterator it = params.begin(); it != params.end(); ++it) cout << " | " << left << setw(15) << it->first << " | " << right << setw(15) << it->second << " |" << endl; cout << " *---------------------------------------*" << endl; } //-------------------------------------------------------------------------- // Warn if a parameter is going to be overwriten void MadgraphPar::warnParamOverwrite(const string ¶mIn, double val) { // Check if present and if new value is different if (haveParam(paramIn) && abs(getParam(paramIn) - val) > ZEROTHRESHOLD) { if (infoPtr) infoPtr->errorMsg("Warning in LHAupAlpgen::" "warnParamOverwrite: overwriting existing parameter", paramIn); } } //-------------------------------------------------------------------------- // Simple string trimmer string MadgraphPar::trim(string s) { // Remove whitespace in incoming string size_t i; if ( (i = s.find_last_not_of(" \t\r\n")) != string::npos) s = s.substr(0, i + 1); if ( (i = s.find_first_not_of(" \t\r\n")) != string::npos) s = s.substr(i); return s; } //========================================================================== #endif // Pythia8_GeneratorInput_H pythia8-8.1.80.orig/examples/main22.cc0000644000175000017500000002113612217346165015560 0ustar sunsun// main22.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Simple illustration how to provide (a) your own resonance-width class, // and (b) your own cross-section class, with instances handed in to Pythia. // The hypothetical scenario is that top would have been so long-lived // that a toponium resonance Theta could form. Then production could // proceed via q qbar -> gamma*/Z* -> Theta, with decay either to // a fermion pair or (dominantly) to three gluons. // The implementation is not physically correct in any number of ways, // but should exemplify the strategy needed for realistic cases. #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // The ResonanceTheta class handles a toponium resonance. class ResonanceTheta : public ResonanceWidths { public: // Constructor. ResonanceTheta(int idResIn) {initBasic(idResIn);} private: // Locally stored properties and couplings. double normTheta2qqbar, normTheta2llbar, normTheta2ggg; // Initialize constants. virtual void initConstants(); // Calculate various common prefactors for the current mass. // Superfluous here, so skipped. //virtual void calcPreFac(bool = false); // Calculate width for currently considered channel. virtual void calcWidth(bool = false); }; //-------------------------------------------------------------------------- // Initialize constants. void ResonanceTheta::initConstants() { // Dummy normalization of couplings to the allowed decay channels. normTheta2qqbar = 0.0001; normTheta2llbar = 0.0001; normTheta2ggg = 0.001; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceTheta::calcWidth(bool) { // Expression for Theta -> q qbar (q up to b). Colour factor. if (id1Abs < 6) widNow = 3. * normTheta2qqbar * mHat; // Expression for Theta -> l lbar (l = e, mu, tau). else if (id1Abs == 11 || id1Abs == 13 || id1Abs == 15) widNow = normTheta2llbar * mHat; // Expression for Theta -> g g g. Colour factor. else if (id1Abs == 21) widNow = 8. * normTheta2ggg * mHat; } //========================================================================== // A derived class for q qbar -> Theta (toponium bound state). class Sigma1qqbar2Theta : public Sigma1Process { public: // Constructor. Sigma1qqbar2Theta() {} // Initialize process. virtual void initProc(); // Calculate flavour-independent parts of cross section. virtual void sigmaKin(); // Evaluate sigmaHat(sHat). Assumed flavour-independent so simple. virtual double sigmaHat() {return sigma;} // Select flavour, colour and anticolour. virtual void setIdColAcol(); // Evaluate weight for decay angles. virtual double weightDecay( Event& process, int iResBeg, int iResEnd); // Info on the subprocess. virtual string name() const {return "q qbar -> Theta";} virtual int code() const {return 621;} virtual string inFlux() const {return "qqbarSame";} virtual int resonanceA() const {return 663;} private: // Store flavour-specific process information and standard prefactor. int idTheta; double mRes, GammaRes, m2Res, GamMRat, normTheta2qqbar, sigma; // Pointer to properties of Theta, to access decay width. ParticleDataEntry* particlePtr; }; //-------------------------------------------------------------------------- // Initialize process. void Sigma1qqbar2Theta::initProc() { // Store Theta mass and width for propagator. idTheta = 663; mRes = particleDataPtr->m0(idTheta); GammaRes = particleDataPtr->mWidth(idTheta); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Same normlization as in ResonanceTheta for coupling strength. normTheta2qqbar = 0.0001; // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(idTheta); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat); first step when inflavours unknown. void Sigma1qqbar2Theta::sigmaKin() { // Incoming width with colour factor. double widthIn = normTheta2qqbar * mH / 3.; // Breit-Wigner, including some (guessed) spin factors. double sigBW = 12. * M_PI / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); // Outgoing width: only includes channels left open. double widthOut = particlePtr->resWidthOpen(663, mH); // Total answer. sigma = widthIn * sigBW * widthOut; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1qqbar2Theta::setIdColAcol() { // Flavours trivial. setId( id1, id2, idTheta); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 1, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for Theta -> g g g. double Sigma1qqbar2Theta::weightDecay( Event& process, int iResBeg, int iResEnd) { // Should be Theta decay. (This is only option here, so overkill.) if (iResEnd != iResBeg || process[iResBeg].idAbs() != idTheta) return 1.; // Should be decay to three gluons. int i1 = process[iResBeg].daughter1(); int i2 = i1 + 1; int i3 = i2 + 1; if (i3 != process[iResBeg].daughter2() || process[i1].id() != 21) return 1.; // Energy fractions x_i = 2 E_i/m_Theta of gluons in Theta rest frame. double x1 = 2. * process[i1].p() * process[iResBeg].p() / process[iResBeg].m2(); double x2 = 2. * process[i2].p() * process[iResBeg].p() / process[iResBeg].m2(); double x3 = 2. * process[i3].p() * process[iResBeg].p() / process[iResBeg].m2(); // Matrix-element expression for Theta -> g g g. double wtME = pow2( (1. - x1) / (x2 * x3) ) + pow2( (1. - x2) / (x1 * x3) ) + pow2( (1. - x3) / (x1 * x2) ); double wtMEmax = 2.; return wtME / wtMEmax; } //========================================================================== int main() { // Number of events to generate. Max number of errors. // Warning: generation of complete events is much slower than if you use // PartonLevel:all = off to only get cross sections, so adjust nEvent. int nEvent = 1000; int nAbort = 5; // Pythia generator. Pythia pythia; // Create the toponium resonance and a few production/decay channels. // Warning: many more exist, e.g. weak ones of one top quark. // Note: to obtain the correct width for the Breit-Wigner you must // include all channels, but you only need leave those on that you // want to study. pythia.readString("663:new = Theta void 3 0 0 342.0 0.2 300. 400. 0."); pythia.readString("663:addChannel = 1 0. 0 1 -1"); pythia.readString("663:addChannel = 1 0. 0 2 -2"); pythia.readString("663:addChannel = 1 0. 0 3 -3"); pythia.readString("663:addChannel = 1 0. 0 4 -4"); pythia.readString("663:addChannel = 1 0. 0 5 -5"); pythia.readString("663:addChannel = 1 0. 0 11 -11"); pythia.readString("663:addChannel = 1 0. 0 13 -13"); pythia.readString("663:addChannel = 1 0. 0 15 -15"); pythia.readString("663:addChannel = 1 0. 0 21 21 21"); // Create instance of a class to calculate the width of Theta to the // above channels. Hand in pointer to Pythia. // Note: Pythia will automatically delete this pointer, // along with all other resonances. ResonanceWidths* resonanceTheta = new ResonanceTheta(663); pythia.setResonancePtr(resonanceTheta); // Create instance of a class to generate the q qbar -> Theta process // from an external matrix element. Hand in pointer to Pythia. SigmaProcess* sigma1Theta = new Sigma1qqbar2Theta(); pythia.setSigmaPtr(sigma1Theta); // Optionally only compare cross sections. //pythia.readString("PartonLevel:all = off"); pythia.readString("Check:nErrList = 2"); // Initialization for LHC. pythia.init(); // Book histogram. Hist mTheta("Theta mass", 100, 300., 400.); // Begin event loop. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Quit if many failures. if (!pythia.next()) { if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Fill Theta mass. End of event loop. mTheta.fill( pythia.process[5].m() ); } // Final statistics. Print histogram. pythia.stat(); cout << mTheta; // Done. delete sigma1Theta; return 0; } pythia8-8.1.80.orig/examples/main32.cmnd0000644000175000017500000000616212217346166016120 0ustar sunsun! 1) Settings used in the main program. Main:numberOfEvents = -1 ! number of events to generate (-1 for all) Main:timesAllowErrors = 3 ! how many aborts before run stops Main:spareMode1 = 0 ! skip n events at beginning of file ! 2) Settings related to output in init(), next() and stat(). Init:showChangedSettings = on ! list changed settings Init:showChangedParticleData = on ! list changed particle data Next:numberCount = 10 ! print message every n events Next:numberShowInfo = 1 ! print event information n times Next:numberShowProcess = 1 ! print process record n times Next:numberShowEvent = 1 ! print event record n times ! 3) Enable matching JetMatching:merge = on ! Madgraph run: Beams:LHEF = w+_production_lhc_2.lhe Beams:frameType = 4 JetMatching:scheme = 1 JetMatching:setMad = off JetMatching:qCut = 20.0 JetMatching:coneRadius = 1.0 JetMatching:etaJetMax = 10.0 JetMatching:nJetMax = 3 ! Alpgen run ! Alpgen:file = main32 ! Alpgen:setMLM = on ! JetMatching:scheme = 2 ! JetMatching:nJetMax = 3 ! Alpgen file + Madgraph matching scheme ! Alpgen:file = main32 ! JetMatching:scheme = 1 ! JetMatching:qCut = 20.0 ! JetMatching:coneRadius = 1.0 ! JetMatching:etaJetMax = 10.0 ! LHEF + Alpgen matching scheme ! Beams:LHEF = w+_production_lhc_2.lhe ! Beams:frameType = 4 ! JetMatching:scheme = 2 ! JetMatching:slowJetPower = 1 ! JetMatching:jetAlgorithm = 1 ! JetMatching:eTjetMin = 20.0 ! JetMatching:coneRadius = 1.0 ! JetMatching:exclusive = 1 ! 4) Examples of further possible MLM settings. ! Default is CellJet algorithm with merging parameters set based on ! read in matrix element cuts. Exclusive/inclusive mode is set ! based on the read in value of 'MLM:nJet', and 'MLM:nJetMax' above. ! MLM master settings !Alpgen:file = main32 !Alpgen:setMLM = on !JetMatching:scheme = 2 !JetMatching:nJetMax = 3 ! Pick custom merging parameters ! Alpgen:file = main32 ! Alpgen:setMLM = off ! JetMatching:scheme = 2 ! JetMatching:nJetMax = 3 ! JetMatching:eTjetMin = 30.0 ! JetMatching:coneRadius = 1.0 ! JetMatching:etaJetMax = 2.0 ! JetMatching:exclusive = 0 ! Disable automatic setting of Alpgen masses ! Alpgen:setMasses = off ! Anti-kT algorithm with ghost particle jet matching ! Alpgen:file = main32 ! Alpgen:setMLM = on ! JetMatching:scheme = 2 ! JetMatching:jetAlgorithm = 2 ! JetMatching:slowJetPower = -1 ! JetMatching:jetMatch = 2 ! JetMatching:jetAllow = 2 ! Anti-kT algorithm with deltaR matching with factor 1. ! Alpgen:file = main32 ! Alpgen:setMLM = on ! JetMatching:scheme = 2 ! JetMatching:jetAlgorithm = 2 ! JetMatching:slowJetPower = -1 ! JetMatching:coneMatchLight = 1.0 ! JetMatching:coneMatchHeavy = 1.0 ! kT algorithm with ghost particle jet matching ! Alpgen:file = main32 ! Alpgen:setMLM = on ! JetMatching:scheme = 2 ! JetMatching:jetAlgorithm = 2 ! JetMatching:slowJetPower = 1 ! JetMatching:jetMatch = 2 ! 5) Other settings HadronLevel:all = off ! switch off hadronisation for testing only pythia8-8.1.80.orig/examples/runmains0000755000175000017500000000702712217346206015742 0ustar sunsun# runmains is a part of the PYTHIA event generator. # Copyright (C) 2013 Torbjorn Sjostrand. # PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. # Please respect the MCnet Guidelines, see GUIDELINES for details. # Simple script to run all the mainXX test programs # Several of the ones from main31 and higher need linkage to external # libraries, however, and therefore the execution exits before them by default. # If you want to change that behaviour, comment out the "exit" line. # The subdirectory outref contains output from reference run. echo echo Now begin main01 make main01 time ./main01.exe > out01 echo echo Now begin main02 make main02 time ./main02.exe > out02 echo echo Now begin main03 make main03 time ./main03.exe > out03 echo echo Now begin main04 make main04 time ./main04.exe > out04 echo echo Now begin main05 make main05 time ./main05.exe > out05 echo echo Now begin main06 make main06 time ./main06.exe > out06 echo echo Now begin main07 make main07 time ./main07.exe > out07 echo echo Now begin main08 make main08 time ./main08.exe > out08 echo echo Now begin main09 make main09 time ./main09.exe > out09 echo echo Now begin main10 make main10 time ./main10.exe > out10 echo echo Now begin main11 make main11 time ./main11.exe > out11 echo echo Now begin main12 make main12 time ./main12.exe > out12 echo echo Now begin main13 make main13 time ./main13.exe > out13 echo echo Now begin main14 make main14 time ./main14.exe > out14 echo echo Now begin main15 make main15 time ./main15.exe > out15 echo echo Now begin main16 make main16 time ./main16.exe main16.cmnd > out16 echo echo Now begin main17 make main17 time ./main17.exe > out17 echo echo Now begin main18 make main18 time ./main18.exe > out18 echo echo Now begin main19 make main19 time ./main19.exe > out19 echo echo Now begin main20 make main20 time ./main20.exe > out20 echo echo Now begin main21 make main21 time ./main21.exe > out21 echo echo Now begin main22 make main22 time ./main22.exe > out22 echo echo Now begin main23 make main23 time ./main23.exe > out23 echo echo Now begin main24 make main24 time ./main24.exe > out24 echo echo Now begin main25 make main25 time ./main25.exe > out25 echo echo Now begin main26 make main26 time ./main26.exe > out26 echo echo Now begin main27 make main27 time ./main27.exe > out27 echo echo Now begin main28 make main28 time ./main28.exe > out28 # This code section stops the testing before the mainXX programs # that need access to various external libraries (+ main31). # If you have ensured such linkage, feel free to comment out # the exit command below, to have the program continue to the end. echo echo The testing stops here! echo Further checks require that you have external libraries linked, echo and edit this runmains file, by removing a single exit line. exit echo echo Now begin main31 make main31 time ./main31.exe > out31 echo echo Now begin main41 make main41 time ./main41.exe > out41 echo echo Now begin main42 make main42 time ./main42.exe main42.cmnd hepmcout42.dat > out42 echo echo Now begin main51 make main51 time ./main51.exe > out51 echo echo Now begin main52 make main52 time ./main52.exe > out52 echo echo Now begin main53 make main53 time ./main53.exe > out53 echo echo Now begin main61 make main61 time ./main61.exe main61.cmnd hepmcout61.dat > out61 echo echo Now begin main62 make main62 time ./main62.exe main62.cmnd hepmcout62.dat > out62 echo echo Now begin main71 make main71 time ./main71.exe > out71 echo echo Now begin main72 make main72 time ./main72.exe > out72 pythia8-8.1.80.orig/examples/main32.unw0000644000175000017500000012247412217346166016015 0ustar sunsun 1 2 7 0.100000E+01 0.913894E+02 21 1 2 494.433 2 4 0 -134.303 1 1 0 -31.630 -7.872 -29.353 0.000 21 4 3 10.953 -12.331 -25.249 0.000 21 3 2 -23.009 4.580 452.654 0.000 12 0 0 7.647 46.153 -21.012 0.000 -11 0 0 36.039 -30.529 -16.910 0.001 2 3 7 0.100000E+01 0.880429E+02 2 4 0 349.728 21 2 3 -18.858 1 1 0 7.697 -22.874 68.583 0.000 21 2 1 -19.464 -3.449 82.529 0.000 21 4 3 17.535 1.904 6.417 0.000 12 0 0 18.279 13.756 161.993 0.000 -11 0 0 -24.046 10.663 11.348 0.001 3 4 7 0.100000E+01 0.112976E+03 21 2 1 842.354 21 4 3 -21.462 2 4 0 -18.296 5.741 51.846 0.000 -1 0 1 13.149 21.360 5.672 0.000 21 2 3 -31.541 -65.611 412.625 0.000 11 0 0 55.633 2.779 184.391 0.001 -12 0 0 -18.944 35.732 166.359 0.000 4 22 7 0.100000E+01 0.115675E+03 2 3 0 284.300 21 1 2 -309.384 1 1 0 -78.216 16.795 1.157 0.000 1 3 0 11.917 11.566 -196.160 0.000 -1 0 2 15.193 -2.680 -63.199 0.000 12 0 0 44.314 -50.193 139.315 0.000 -11 0 0 6.791 24.512 93.803 0.001 5 3 7 0.100000E+01 0.138202E+03 2 4 0 180.688 21 2 3 -273.996 1 1 0 -103.367 35.809 62.327 0.000 21 2 1 2.852 -20.242 -150.770 0.000 21 4 3 7.897 -13.617 -45.672 0.000 12 0 0 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1558.828 21 1 2 -11.822 1 1 0 -40.652 4.308 312.495 0.000 21 4 3 48.999 15.238 246.082 0.000 21 3 2 -15.445 -1.261 3.887 0.000 12 0 0 21.190 26.907 540.499 0.000 -11 0 0 -14.092 -45.193 444.043 0.001 69 3 7 0.100000E+01 0.938644E+02 -1 0 1 302.874 21 3 4 -23.228 -2 0 4 11.711 28.671 47.806 0.000 21 2 1 -15.601 -27.045 69.746 0.000 21 3 2 -18.148 -8.945 20.032 0.000 -11 0 0 -2.961 -24.476 109.752 0.001 12 0 0 24.998 31.795 32.310 0.000 70 3 7 0.100000E+01 0.913656E+02 2 4 0 215.744 21 1 2 -44.020 1 1 0 20.099 17.371 25.839 0.000 21 3 2 -7.701 -21.625 -13.078 0.000 21 4 3 14.393 -20.991 36.812 0.000 12 0 0 -41.461 40.451 50.553 0.000 -11 0 0 14.670 -15.206 71.597 0.001 71 18 7 0.100000E+01 0.103045E+03 2 1 0 515.781 21 3 2 -260.985 2 1 0 -7.948 42.700 12.593 0.000 2 3 0 -14.157 -26.609 458.454 0.000 -3 0 2 25.659 -26.416 -176.388 0.000 -12 0 0 -18.651 -32.451 -16.962 0.000 11 0 0 15.097 42.776 -22.902 0.001 72 3 7 0.100000E+01 0.170605E+03 1 1 0 1638.618 21 4 3 -22.237 2 4 0 79.650 -67.423 311.501 0.000 21 2 3 10.391 18.374 15.529 0.000 21 1 2 -106.260 3.462 906.897 0.000 11 0 0 29.784 59.185 229.574 0.001 -12 0 0 -13.565 -13.598 152.881 0.000 73 3 7 0.100000E+01 0.954169E+02 2 4 0 839.815 21 3 4 -41.729 1 1 0 -16.913 35.382 50.523 0.000 21 3 2 -16.531 -5.202 -7.029 0.000 21 2 1 -5.148 -27.791 -9.502 0.000 12 0 0 -15.092 21.171 155.803 0.000 -11 0 0 53.685 -23.560 608.291 0.001 74 2 7 0.100000E+01 0.943919E+02 21 4 3 24.164 1 1 0 -1350.954 2 4 0 -3.871 31.709 -128.865 0.000 21 2 3 -26.448 -21.254 5.617 0.000 21 1 2 13.216 9.810 -132.321 0.000 11 0 0 -1.750 -42.308 -897.260 0.001 -12 0 0 18.853 22.043 -173.961 0.000 75 3 7 0.100000E+01 0.868100E+02 2 4 0 457.303 21 2 3 -57.307 1 1 0 -15.307 1.926 -0.930 0.000 21 4 3 24.392 0.649 -8.916 0.000 21 2 1 -2.716 -15.098 -25.640 0.000 12 0 0 -2.823 -17.185 378.826 0.000 -11 0 0 -3.547 29.708 56.655 0.001 76 2 7 0.100000E+01 0.965438E+02 21 2 3 92.438 2 4 0 -2426.760 1 1 0 8.471 20.777 -270.555 0.000 21 4 3 -28.285 3.920 -181.294 0.000 21 2 1 38.296 -8.251 85.690 0.000 12 0 0 -13.239 -36.983 -1805.412 0.000 -11 0 0 -5.243 20.537 -162.752 0.001 77 2 7 0.100000E+01 0.921950E+02 21 3 4 81.517 2 4 0 -394.344 1 1 0 29.376 -2.757 -11.651 0.000 21 3 2 -23.826 14.707 21.652 0.000 21 2 1 -1.684 19.374 35.231 0.000 12 0 0 7.433 -19.229 -349.051 0.000 -11 0 0 -11.299 -12.095 -9.008 0.001 78 15 7 0.100000E+01 0.910668E+02 2 1 0 232.623 1 3 0 -644.423 1 1 0 -35.477 -6.422 -614.520 0.000 1 2 0 13.042 -11.288 0.705 0.000 21 3 2 14.705 3.517 -9.409 0.000 -11 0 0 -9.363 -31.030 76.884 0.001 12 0 0 17.094 45.223 134.540 0.000 79 2 7 0.100000E+01 0.126244E+03 21 1 2 269.188 -3 0 1 -360.973 -4 0 4 82.930 -24.820 30.417 0.000 21 3 2 21.301 16.878 175.199 0.000 21 4 3 -34.376 -7.526 8.392 0.000 -11 0 0 -21.157 15.960 -247.776 0.001 12 0 0 -48.698 -0.492 -58.017 0.000 80 2 7 0.100000E+01 0.122003E+03 21 4 3 167.373 3 1 0 -90.909 4 4 0 -33.034 -37.941 40.460 0.000 21 2 3 51.748 53.836 19.028 0.000 21 1 2 8.717 -15.316 -12.665 0.000 11 0 0 -17.279 -29.097 48.616 0.001 -12 0 0 -10.151 28.518 -18.975 0.000 81 6 7 0.100000E+01 0.114382E+03 1 1 0 601.315 -3 0 2 -541.018 2 3 0 -54.579 31.554 113.762 0.000 -3 0 3 31.059 -16.757 -416.186 0.000 21 1 2 6.655 36.766 -107.938 0.000 11 0 0 14.457 8.738 277.226 0.001 -12 0 0 2.409 -60.301 193.432 0.000 82 4 7 0.100000E+01 0.941121E+02 21 4 3 169.148 21 2 1 -83.217 4 4 0 -16.358 3.107 14.029 0.000 -3 0 1 31.389 -25.421 15.875 0.000 21 2 3 16.076 14.923 91.917 0.000 11 0 0 13.166 -13.946 -38.989 0.001 -12 0 0 -44.273 21.338 3.100 0.000 83 14 7 0.100000E+01 0.154573E+03 1 3 0 153.496 2 2 0 -699.341 1 1 0 -42.892 -52.024 118.389 0.000 1 3 0 86.989 8.022 -171.416 0.000 21 2 1 17.372 70.329 -182.957 0.000 -11 0 0 15.416 -23.241 -103.258 0.001 12 0 0 -76.885 -3.086 -206.603 0.000 84 6 7 0.100000E+01 0.108344E+03 -4 0 3 152.882 -1 0 2 -360.630 -3 0 1 -16.288 41.716 16.044 0.000 -1 0 3 -9.677 15.692 -232.645 0.000 21 1 2 -48.676 23.586 -59.057 0.000 -12 0 0 79.135 -29.297 37.526 0.000 11 0 0 -4.493 -51.698 30.383 0.001 85 3 7 0.100000E+01 0.145997E+03 3 1 0 177.228 21 4 3 -1248.476 4 4 0 -67.825 -41.504 -24.385 0.000 21 1 2 64.618 -60.578 103.092 0.000 21 2 3 14.647 21.575 -1055.988 0.000 11 0 0 -3.939 95.791 -62.253 0.001 -12 0 0 -7.501 -15.284 -31.716 0.000 86 4 7 0.100000E+01 0.888261E+02 21 4 3 237.301 21 2 1 -53.091 2 4 0 20.808 7.957 29.556 0.000 -1 0 1 -22.917 11.274 -31.383 0.000 21 2 3 -16.016 4.217 17.662 0.000 11 0 0 24.934 -39.598 47.901 0.001 -12 0 0 -6.809 16.150 120.473 0.000 87 6 7 0.100000E+01 0.104023E+03 1 1 0 1613.255 2 2 0 -929.523 4 3 0 -19.352 -18.030 204.373 0.000 2 1 0 -53.846 -15.548 -888.801 0.000 21 2 3 -21.801 -6.129 -32.365 0.000 11 0 0 83.863 35.489 1379.230 0.001 -12 0 0 11.136 4.218 21.295 0.000 88 7 7 0.100000E+01 0.112080E+03 -4 0 2 42.646 2 3 0 -347.655 1 1 0 -12.371 -26.272 -87.013 0.000 -4 0 1 -39.460 56.000 -26.134 0.000 21 3 2 21.759 9.216 -33.969 0.000 12 0 0 20.849 -52.490 -157.670 0.000 -11 0 0 9.222 13.545 -0.223 0.001 89 2 7 0.100000E+01 0.104816E+03 21 1 2 24.262 2 4 0 -960.583 1 1 0 -16.105 -50.790 -131.872 0.000 21 3 2 10.600 25.599 -4.807 0.000 21 4 3 1.180 30.186 -576.559 0.000 12 0 0 -6.447 36.761 -103.628 0.000 -11 0 0 10.772 -41.757 -119.455 0.001 90 4 7 0.100000E+01 0.101129E+03 21 3 4 188.115 21 1 2 -154.297 3 1 0 27.291 -19.947 -8.507 0.000 -4 0 4 -3.520 -46.074 87.027 0.000 21 3 2 -18.689 -11.516 -86.993 0.000 12 0 0 31.436 29.645 40.231 0.000 -11 0 0 -36.519 47.892 2.061 0.001 91 2 7 0.100000E+01 0.148014E+03 21 2 3 459.010 2 4 0 -349.121 1 1 0 -90.119 -8.143 47.456 0.000 21 2 1 78.772 26.601 351.394 0.000 21 4 3 6.792 -17.160 12.940 0.000 12 0 0 -6.141 -56.402 -155.607 0.000 -11 0 0 10.696 55.103 -146.294 0.001 92 3 7 0.100000E+01 0.106489E+03 -1 0 1 135.317 21 3 4 -168.934 -2 0 4 -28.810 -45.665 -0.668 0.000 21 3 2 36.106 19.336 -51.762 0.000 21 2 1 8.092 14.646 -64.487 0.000 -11 0 0 -42.027 22.224 73.132 0.001 12 0 0 26.639 -10.542 10.167 0.000 93 4 7 0.100000E+01 0.117977E+03 21 1 2 184.184 21 3 4 -104.699 3 1 0 -23.566 3.976 30.378 0.000 -4 0 4 -78.269 22.002 -11.281 0.000 21 3 2 -12.072 -11.151 6.914 0.000 12 0 0 -6.084 3.847 24.419 0.000 -11 0 0 119.991 -18.674 29.054 0.001 94 14 7 0.100000E+01 0.873307E+02 2 1 0 425.884 1 2 0 -93.622 2 3 0 18.387 9.329 381.776 0.000 2 1 0 -15.621 -1.389 -2.551 0.000 21 2 3 15.485 -15.767 -28.390 0.000 -12 0 0 -29.377 -2.596 25.303 0.000 11 0 0 11.126 10.422 -43.876 0.001 95 2 7 0.100000E+01 0.107594E+03 21 3 2 53.913 1 1 0 -1811.007 2 4 0 -27.322 -16.459 -151.148 0.000 21 3 4 49.636 -22.398 35.230 0.000 21 1 2 -17.503 28.640 -537.929 0.000 11 0 0 22.131 -21.086 -797.593 0.001 -12 0 0 -26.943 31.303 -305.654 0.000 96 2 7 0.100000E+01 0.961263E+02 21 3 4 219.883 -3 0 1 -144.401 -4 0 4 19.957 30.480 -19.531 0.000 21 2 1 -9.658 -23.210 50.592 0.000 21 3 2 -17.011 -22.899 137.766 0.000 -11 0 0 7.402 47.844 -73.203 0.001 12 0 0 -0.689 -32.215 -20.142 0.000 97 13 7 0.100000E+01 0.116027E+03 1 1 0 386.205 1 3 0 -56.748 1 2 0 27.887 -6.410 -16.802 0.000 2 3 0 -30.170 -12.644 39.674 0.000 21 1 2 -55.132 45.459 196.693 0.000 11 0 0 12.031 27.619 30.614 0.001 -12 0 0 45.385 -54.025 79.277 0.000 98 3 7 0.100000E+01 0.106926E+03 2 4 0 750.171 21 1 2 -15.110 1 1 0 -50.271 31.465 187.219 0.000 21 3 2 -22.571 -9.275 79.372 0.000 21 4 3 28.304 7.214 135.628 0.000 12 0 0 31.986 11.816 261.924 0.000 -11 0 0 12.552 -41.221 70.919 0.001 99 3 7 0.100000E+01 0.898455E+02 2 4 0 47.398 21 1 2 -378.559 1 1 0 22.192 -20.849 -4.260 0.000 21 3 2 11.280 -14.190 -249.586 0.000 21 4 3 1.163 -18.651 -3.637 0.000 12 0 0 -34.718 -11.438 -20.947 0.000 -11 0 0 0.083 65.129 -52.731 0.001 100 14 7 0.100000E+01 0.145454E+03 2 1 0 317.837 1 2 0 -472.856 2 3 0 -28.677 -35.576 241.321 0.000 2 1 0 1.790 102.682 -48.392 0.000 21 2 3 -43.259 -13.550 16.049 0.000 -12 0 0 39.776 -16.103 -50.445 0.000 11 0 0 30.371 -37.452 -313.552 0.001 pythia8-8.1.80.orig/examples/main08.cc0000644000175000017500000001566612217346164015576 0ustar sunsun// main08.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This is a simple test program. // It illustrates methods to emphasize generation at high pT. #include "Pythia8/Pythia.h" using namespace Pythia8; int main() { // Different modes are illustrated for setting the pT ranges. // 1 : Hardcoded in the main program. // 2 : Using the Main:subrun keyword in a separate command file. // A third method instead biases selection continuously. // 3 : Bias high-pT selection by a pT^4 factor. // Matching also to low-pT processes is more complicated. // 4 : Matching between low- and high-pT. (No diffraction.) // 5: As 4, but bias high-pT selection by a pT^4 factor. int mode = 5; // Number of events to generate per bin. int nEvent = 100000; // One does not need complete events to study pThard spectrum only. bool completeEvents = false; // Optionally minimize output (almost) to final results. bool smallOutput = true; // Book histograms. int nRange = 100; double pTrange = (mode < 4) ? 1000. : 100.; Hist pTraw("pTHat distribution, unweighted", nRange, 0., pTrange); Hist pTnorm("pTHat distribution, weighted", nRange, 0., pTrange); Hist pTpow3("pTHat distribution, pT3*weighted", nRange, 0., pTrange); Hist pTpow5("pTHat distribution, pT5*weighted", nRange, 0., pTrange); Hist pTnormPart("pTHat distribution, weighted", nRange, 0., pTrange); Hist pTpow3Part("pTHat distribution, pT3*weighted", nRange, 0., pTrange); Hist pTpow5Part("pTHat distribution, pT5*weighted", nRange, 0., pTrange); // Generator. Pythia pythia; // Shorthand for some public members of pythia (also static ones). Settings& settings = pythia.settings; Info& info = pythia.info; // Optionally limit output to minimal one. if (smallOutput) { pythia.readString("Init:showProcesses = off"); pythia.readString("Init:showMultipartonInteractions = off"); pythia.readString("Init:showChangedSettings = off"); pythia.readString("Init:showChangedParticleData = off"); pythia.readString("Next:numberCount = 1000000000"); pythia.readString("Next:numberShowInfo = 0"); pythia.readString("Next:numberShowProcess = 0"); pythia.readString("Next:numberShowEvent = 0"); } // Number of bins to use. In mode 2 read from main08.cmnd file. int nBin = 5; if (mode == 2) { pythia.readFile("main08.cmnd"); nBin = pythia.mode("Main:numberOfSubruns"); } else if (mode == 3) nBin = 1; else if (mode == 4) nBin = 4; else if (mode == 5) nBin = 2; // Mode 1: set up five pT bins - last one open-ended. double pTlimit[6] = {100., 150., 250., 400., 600., 0.}; // Modes 4 & 5: set up pT bins for range [0, 100]. The lowest bin // is generated with soft processes, to regularize pT -> 0 blowup. // Warning: if pTlimitLow[1] is picked too low there will be a // visible discontinuity, since soft processes are generated with // dampening and "Sudakov" for pT -> 0, while hard processes are not. double pTlimitLow[6] = {0., 20., 40., 70., 100.}; double pTlimitTwo[3] = {0., 20., 100.}; // Loop over number of bins, i.e. number of subruns. for (int iBin = 0; iBin < nBin; ++iBin) { // Normally HardQCD, but in two cases nonDiffractive. // Need MPI on in nonDiffractive to get first interaction, but not else. if (mode > 3 && iBin == 0) { pythia.readString("HardQCD:all = off"); pythia.readString("SoftQCD:nonDiffractive = on"); if (!completeEvents) { pythia.readString("PartonLevel:all = on"); pythia.readString("PartonLevel:ISR = off"); pythia.readString("PartonLevel:FSR = off"); pythia.readString("HadronLevel:all = off"); } } else { pythia.readString("HardQCD:all = on"); pythia.readString("SoftQCD:nonDiffractive = off"); if (!completeEvents) pythia.readString("PartonLevel:all = off"); } // Mode 1: hardcoded here. Use settings.parm for non-string input. if (mode == 1) { settings.parm("PhaseSpace:pTHatMin", pTlimit[iBin]); settings.parm("PhaseSpace:pTHatMax", pTlimit[iBin + 1]); } // Mode 2: subruns stored in the main08.cmnd file. else if (mode == 2) pythia.readFile("main08.cmnd", iBin); // Mode 3: The whole range in one step, but pT-weighted. else if (mode == 3) { settings.parm("PhaseSpace:pTHatMin", pTlimit[0]); settings.parm("PhaseSpace:pTHatMax", 0.); pythia.readString("PhaseSpace:bias2Selection = on"); pythia.readString("PhaseSpace:bias2SelectionPow = 4."); pythia.readString("PhaseSpace:bias2SelectionRef = 100."); } // Mode 4: hardcoded here. Use settings.parm for non-string input. else if (mode == 4) { settings.parm("PhaseSpace:pTHatMin", pTlimitLow[iBin]); settings.parm("PhaseSpace:pTHatMax", pTlimitLow[iBin + 1]); } // Mode 5: hardcoded here. Use settings.parm for non-string input. // Hard processes in one step, but pT-weighted. else if (mode == 5) { settings.parm("PhaseSpace:pTHatMin", pTlimitTwo[iBin]); settings.parm("PhaseSpace:pTHatMax", pTlimitTwo[iBin + 1]); if (iBin == 1) { pythia.readString("PhaseSpace:bias2Selection = on"); pythia.readString("PhaseSpace:bias2SelectionPow = 4."); pythia.readString("PhaseSpace:bias2SelectionRef = 20."); } } // Initialize for LHC at 14 TeV. pythia.readString("Beams:eCM = 14000."); pythia.init(); // Reset local histograms (that need to be rescaled before added). pTnormPart.null(); pTpow3Part.null(); pTpow5Part.null(); // Begin event loop. for (int iEvent = 0; iEvent < nEvent; ++iEvent) { // Generate events. Skip if failure. if (!pythia.next()) continue; // Soft events have no upper pT limit. They therefore overlap // with hard events, and the overlap must be removed by hand. // No overlap for elastic/diffraction, which is only part of soft. double pTHat = info.pTHat(); if (mode > 3 && iBin == 0 && info.isNonDiffractive() && pTHat > pTlimitLow[1]) continue; // Fill hard scale of event. double weight = info.weight(); pTraw.fill( pTHat ); pTnormPart.fill( pTHat, weight); pTpow3Part.fill( pTHat, weight * pow3(pTHat) ); pTpow5Part.fill( pTHat, weight * pow5(pTHat) ); // End of event loop. Statistics. } if (!smallOutput) pythia.stat(); // Normalize to cross section for each case, and add to sum. double sigmaNorm = (info.sigmaGen() / info.weightSum()) * (nRange / pTrange); pTnorm += sigmaNorm * pTnormPart; pTpow3 += sigmaNorm * pTpow3Part; pTpow5 += sigmaNorm * pTpow5Part; // End of pT-bin loop. } // Output histograms. cout << pTraw << pTnorm << pTpow3 << pTpow5; // Done. return 0; } pythia8-8.1.80.orig/examples/main23.cc0000644000175000017500000002640512217346165015565 0ustar sunsun// main23.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Example how to write a derived class for beam momentum and vertex spread, // with an instance handed to Pythia for internal generation. // Also how to write a derived class for external random numbers, // and how to write a derived class for external parton distributions. // Warning: the parameters are not realistic. #include "Pythia8/Pythia.h" using namespace Pythia8; //========================================================================== // A derived class to set beam momentum and interaction vertex spread. class MyBeamShape : public BeamShape { public: // Constructor. MyBeamShape() {} // Initialize beam parameters. // In this particular example we will reuse the existing settings names // but with modified meaning, so init() in the base class can be kept. //virtual void init( Settings& settings, Rndm* rndmPtrIn); // Set the two beam momentum deviations and the beam vertex. virtual void pick(); }; //-------------------------------------------------------------------------- // Set the two beam momentum deviations and the beam vertex. // Note that momenta are in units of GeV and vertices in mm, // always with c = 1, so that e.g. time is in mm/c. void MyBeamShape::pick() { // Reset all values. deltaPxA = deltaPyA = deltaPzA = deltaPxB = deltaPyB = deltaPzB = vertexX = vertexY = vertexZ = vertexT = 0.; // Set beam A transverse momentum deviation by a two-dimensional Gaussian. if (allowMomentumSpread) { double totalDev, gauss; do { totalDev = 0.; if (sigmaPxA > 0.) { gauss = rndmPtr->gauss(); deltaPxA = sigmaPxA * gauss; totalDev += gauss * gauss; } if (sigmaPyA > 0.) { gauss = rndmPtr->gauss(); deltaPyA = sigmaPyA * gauss; totalDev += gauss * gauss; } } while (totalDev > maxDevA * maxDevA); // Set beam A longitudinal momentum as a triangular shape. // Reuse sigmaPzA to represent maximum deviation in this case. if (sigmaPzA > 0.) { deltaPzA = sigmaPzA * ( 1. - sqrt(rndmPtr->flat()) ); if (rndmPtr->flat() < 0.5) deltaPzA = -deltaPzA; } // Set beam B transverse momentum deviation by a two-dimensional Gaussian. do { totalDev = 0.; if (sigmaPxB > 0.) { gauss = rndmPtr->gauss(); deltaPxB = sigmaPxB * gauss; totalDev += gauss * gauss; } if (sigmaPyB > 0.) { gauss = rndmPtr->gauss(); deltaPyB = sigmaPyB * gauss; totalDev += gauss * gauss; } } while (totalDev > maxDevB * maxDevB); // Set beam B longitudinal momentum as a triangular shape. // Reuse sigmaPzB to represent maximum deviation in this case. if (sigmaPzB > 0.) { deltaPzB = sigmaPzB * ( 1. - sqrt(rndmPtr->flat()) ); if (rndmPtr->flat() < 0.5) deltaPzB = -deltaPzB; } } // Set beam vertex location by a two-dimensional Gaussian. if (allowVertexSpread) { double totalDev, gauss; do { totalDev = 0.; if (sigmaVertexX > 0.) { gauss = rndmPtr->gauss(); vertexX = sigmaVertexX * gauss; totalDev += gauss * gauss; } if (sigmaVertexY > 0.) { gauss = rndmPtr->gauss(); vertexY = sigmaVertexY * gauss; totalDev += gauss * gauss; } } while (totalDev > maxDevVertex * maxDevVertex); // Set beam B longitudinal momentum as a triangular shape. // This corresponds to two step-function beams colliding. // Reuse sigmaVertexZ to represent maximum deviation in this case. if (sigmaVertexZ > 0.) { vertexZ = sigmaVertexZ * ( 1. - sqrt(rndmPtr->flat()) ); if (rndmPtr->flat() < 0.5) vertexZ = -vertexZ; // Set beam collision time flat between +-(sigmaVertexZ - |vertexZ|). // This corresponds to two step-function beams colliding (with v = c). vertexT = (2. * rndmPtr->flat() - 1.) * (sigmaVertexZ - abs(vertexZ)); } // Add offset to beam vertex. vertexX += offsetX; vertexY += offsetY; vertexZ += offsetZ; vertexT += offsetT; } } //========================================================================== // A derived class to generate random numbers. // A guranteed VERY STUPID generator, just to show principles. class stupidRndm : public RndmEngine { public: // Constructor. stupidRndm() { init();} // Routine for generating a random number. double flat(); private: // Initialization. void init(); // State of the generator. double value, exp10; }; //-------------------------------------------------------------------------- // Initialization method for the random numbers. void stupidRndm::init() { // Initial values. value = 0.5; exp10 = exp(10.); } //-------------------------------------------------------------------------- // Generation method for the random numbers. double stupidRndm::flat() { // Update counter. Add to current value. do { value *= exp10; value += M_PI; value -= double(int(value)); if (value < 0.) value += 1.; } while (value <= 0. || value >= 1.); // Return new value. return value; } //========================================================================== // A simple scaling PDF. Not realistic; only to check that it works. class Scaling : public PDF { public: // Constructor. Scaling(int idBeamIn = 2212) : PDF(idBeamIn) {} private: // Update PDF values. void xfUpdate(int id, double x, double Q2); }; //-------------------------------------------------------------------------- // No dependence on Q2, so leave out name for last argument. void Scaling::xfUpdate(int, double x, double ) { // Valence quarks, carrying 60% of the momentum. double dv = 4. * x * pow3(1. - x); double uv = 2. * dv; // Gluons and sea quarks carrying the rest. double gl = 2. * pow5(1. - x); double sea = 0.4 * pow5(1. - x); // Update values xg = gl; xu = uv + 0.18 * sea; xd = dv + 0.18 * sea; xubar = 0.18 * sea; xdbar = 0.18 * sea; xs = 0.08 * sea; xc = 0.04 * sea; xb = 0.02 * sea; // Subdivision of valence and sea. xuVal = uv; xuSea = xubar; xdVal = dv; xdSea = xdbar; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //========================================================================== int main() { // Number of events to generate. Max number of errors. int nEvent = 10000; int nAbort = 5; // Pythia generator. Pythia pythia; // Process selection. pythia.readString("HardQCD:all = on"); pythia.readString("PhaseSpace:pTHatMin = 20."); // LHC with acollinear beams in the x plane. // Use that default is pp with pz = +-7000 GeV, so this need not be set. pythia.readString("Beams:frameType = 3"); pythia.readString("Beams:pxA = 1."); pythia.readString("Beams:pxB = 1."); // A class to generate beam parameters according to own parametrization. BeamShape* myBeamShape = new MyBeamShape(); // Hand pointer to Pythia. // If you comment this out you get internal Gaussian-style implementation. pythia.setBeamShapePtr( myBeamShape); // Set up beam spread parameters - reused by MyBeamShape. pythia.readString("Beams:allowMomentumSpread = on"); pythia.readString("Beams:sigmapxA = 0.1"); pythia.readString("Beams:sigmapyA = 0.1"); pythia.readString("Beams:sigmapzA = 5."); pythia.readString("Beams:sigmapxB = 0.1"); pythia.readString("Beams:sigmapyB = 0.1"); pythia.readString("Beams:sigmapzB = 5."); // Set up beam vertex parameters - reused by MyBeamShape. pythia.readString("Beams:allowVertexSpread = on"); pythia.readString("Beams:sigmaVertexX = 0.3"); pythia.readString("Beams:sigmaVertexY = 0.3"); pythia.readString("Beams:sigmaVertexZ = 50."); // In MyBeamShape the time width is not an independent parameter. //pythia.readString("Beams:sigmaTime = 50."); // Optionally simplify generation. pythia.readString("PartonLevel:all = off"); // A class to do random numbers externally. Hand pointer to Pythia. RndmEngine* badRndm = new stupidRndm(); pythia.setRndmEnginePtr( badRndm); // Two classes to do the two PDFs externally. Hand pointers to Pythia. PDF* pdfAPtr = new Scaling(2212); PDF* pdfBPtr = new Scaling(2212); pythia.setPDFPtr( pdfAPtr, pdfBPtr); // Initialization. pythia.init(); // Read out nominal energy. double eCMnom = pythia.info.eCM(); // Histograms. Hist eCM("center-of-mass energy deviation", 100, -20., 20.); Hist pXsum("net pX offset", 100, -1.0, 1.0); Hist pYsum("net pY offset", 100, -1.0, 1.0); Hist pZsum("net pZ offset", 100, -10., 10.); Hist pZind("individual abs(pZ) offset", 100, -10., 10.); Hist vtxX("vertex x position", 100, -1.0, 1.0); Hist vtxY("vertex y position", 100, -1.0, 1.0); Hist vtxZ("vertex z position", 100, -100., 100.); Hist vtxT("vertex time", 100, -100., 100.); Hist vtxZT("vertex |x| + |t|", 100, 0., 100.); // Begin event loop. Generate event. int iAbort = 0; for (int iEvent = 0; iEvent < nEvent; ++iEvent) { if (!pythia.next()) { // List faulty events and quit if many failures. pythia.info.list(); pythia.process.list(); //pythia.event.list(); if (++iAbort < nAbort) continue; cout << " Event generation aborted prematurely, owing to error!\n"; break; } // Fill histograms. double eCMnow = pythia.info.eCM(); eCM.fill( eCMnow - eCMnom); pXsum.fill( pythia.process[0].px() - 2. ); pYsum.fill( pythia.process[0].py() ); pZsum.fill( pythia.process[0].pz() ); pZind.fill( pythia.process[1].pz() - 7000. ); pZind.fill( -pythia.process[2].pz() - 7000. ); vtxX.fill( pythia.process[0].xProd() ); vtxY.fill( pythia.process[0].yProd() ); vtxZ.fill( pythia.process[0].zProd() ); vtxT.fill( pythia.process[0].tProd() ); double absSum = abs(pythia.process[0].zProd()) + abs(pythia.process[0].tProd()); vtxZT.fill( absSum ); // End of event loop. Statistics. Histograms. } pythia.stat(); cout << eCM << pXsum << pYsum << pZsum << pZind << vtxX << vtxY << vtxZ << vtxT << vtxZT; // Study standard Pythia random number generator. Hist rndmDist("standard random number distribution", 100, 0., 1.); Hist rndmCorr("standard random number correlation", 100, 0., 1.); double rndmNow; double rndmOld = pythia.rndm.flat(); for (int i = 0; i < 100000; ++i) { rndmNow = pythia.rndm.flat(); rndmDist.fill(rndmNow); rndmCorr.fill( abs(rndmNow - rndmOld) ); rndmOld = rndmNow; } cout << rndmDist << rndmCorr; // Study bad "new" random number generator. Hist rndmDist2("stupid random number distribution", 100, 0., 1.); Hist rndmCorr2("stupid random number correlation", 100, 0., 1.); rndmOld = pythia.rndm.flat(); for (int i = 0; i < 100000; ++i) { rndmNow = pythia.rndm.flat(); rndmDist2.fill(rndmNow); rndmCorr2.fill( abs(rndmNow - rndmOld) ); rndmOld = rndmNow; } cout << rndmDist2 << rndmCorr2; // Done. delete myBeamShape; delete badRndm; delete pdfAPtr; delete pdfBPtr; return 0; } pythia8-8.1.80.orig/README.HepMC0000644000175000017500000000311712217346244014153 0ustar sunsunHow to install HepMC on your laptop (Linux/Mac OSX) and link to Pythia As of Pythia 8.175 support for older HepMC versions have been dropped, so you have to use HepMC version 2.06 (or later), Here is an example for HepMC 2.06.08 that works for me, but it comes with no guarantee. 1) Create a directory where you want to do the installation, e.g. mkdir hepmc and move to it cd hepmc 2) Open http://lcgapp.cern.ch/project/simu/HepMC/download in a browser, scroll down to "HepMC 2.06.08" and pick the version relevant for your platform from the list to the right. 3) In the pop-up menu pick "Save to file" and then the above hepmc directory. You should now have the appropriate version in that directory, e.g. HepMC-2.06.08-x86_64-mac106-gcc42-opt.tar.gz on a current Mac. 4) Unpack with tar -xzf file.tar.gz with "file" the name of the downloaded file. This will create a new directory, e.g. x86_64-mac106-gcc42-opt/, where ready-to-use libraries can be found. 5) Now move to your pythia8175 (or later) directory and configure with ./configure --with-hepmc=mypath/hepmc/newdir --with-hepmcversion=2.06.08 where "mypath" is the absolute path to the hepmc directory (use pwd if in doubt) and "newdir" is the name of the new directory created in step 4. 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/usr/bin/env bash ## Pythia path variables based on args given to configure prefix=@prefix@ datadir=@datadir@ includedir=$prefix/include libdir=$prefix/lib ## External path variables, also calculated by configure hepmcpath=@HEPMCPATH@ enablegzip=@ENABLEGZIP@ zlibpath=@ZLIBPATH@ boostincpath=@BOOSTINCPATH@ boostlibpath=@BOOSTLIBPATH@ tmp=$(echo $* | egrep -- '--\|-\') if test $# -eq 0 || test -n "$tmp"; then echo "pythia8-config: configuration tool for the Pythia8 event generator library" echo echo "Usage: $( basename $0 ) [--help|-h] | " echo " [--{prefix,datadir,libdir,includedir}] | " echo " [--{cxxflags,ldflags,libs}]" echo "Options:" echo " --help | -h : show this help message" echo echo " --prefix : show the installation prefix (cf. autoconf)" echo " --includedir : show the path to the directory containing the Pythia8 headers" echo " --libdir : show the path to the directory containing the Pythia8 libraries" echo " --datadir : show the path to the directory containing Pythia8 data" echo " --xmldoc : show the path to the xmldoc config directory" echo echo " --cppflags : returns a -I flags string for insertion into CPPFLAGS" echo " --cxxflags : returns a -I flags string for insertion into CPPFLAGS" echo " --ldflags : returns a -L/-l flags string for insertion into LDFLAGS or LIBS" echo " --libs : returns a -L/-l flags string for insertion into LDFLAGS or LIBS" echo " --hepmc : include HepMC -I/-L/-l flags in above output" echo " --lhapdf : LHAPDF will be used: do not include the lhapdfdummy library" exit 0 fi OUT="" ## Paths tmp=$( echo "$*" | egrep -- '--\') test -n "$tmp" && OUT="$OUT $prefix" tmp=$( echo "$*" | egrep -- '--\') test -n "$tmp" && OUT="$OUT $includedir" tmp=$( echo "$*" | egrep -- '--\') test -n "$tmp" && OUT="$OUT $libdir" tmp=$( echo "$*" | egrep -- '--\') test -n "$tmp" && OUT="$OUT $datadir" tmp=$( echo "$*" | egrep -- '--\') test -n "$tmp" && OUT="$OUT $datadir/xmldoc" ## "Pre-rolled" build flag strings tmp=$( echo "$*" | egrep -- '--\') if test -n "$tmp"; then test -n "$includedir" && OUT="$OUT -I${includedir}" tmp=$( echo "$*" | egrep -- '--\') test -n "$tmp" && test -n "$hepmcpath" && OUT="$OUT -I${hepmcpath}/include" test "$enablegzip" = "yes" && OUT="$OUT -I${boostincpath}" fi tmp=$( echo "$*" | egrep -- '--\') if test -n "$tmp"; then test -n "$libdir" && OUT="$OUT -L${libdir} -lpythia8" tmp=$( echo "$*" | egrep -- '--\') test -n "$tmp" && test -n "$hepmcpath" && OUT="$OUT -lhepmcinterface -L${hepmcpath}/lib -lHepMC" tmp=$( echo "$*" | egrep -- '--\') test -n "$tmp" || OUT="$OUT -llhapdfdummy" test "$enablegzip" = "yes" && OUT="$OUT -L${boostlibpath} -lboost_iostreams -L${zlibpath}/lib -lz" fi echo $OUT pythia8-8.1.80.orig/configure0000755000175000017500000003452412217346162014254 0ustar sunsun#!/bin/sh # # Configuration script, to be run before compilation # # Author: M. Kirsanov # # User-changeable part ------------------------------- # #LCG platform. Can be needed if external libraries are specified if [ x$MYLCGPLATFORM = x ]; then export MYLCGPLATFORM=x86_64-slc5-gcc43-opt fi # Defaults export COMPMODE=OPT export SHAREDLIBS=no export ENABLEGZIP=no export INSTALLDIR=. export DATADIR= for arg in $* ; do if [ "x$arg" = "x--enable-debug" ] ; then COMPMODE=DBG elif [ "x$arg" = "x--enable-shared" ] ; then SHAREDLIBS=yes elif [ "x$arg" = "x--enable-64bits" ] ; then ENABLE64=-m64 elif [ "x$arg" = "x--enable-gzip" ] ; then ENABLEGZIP=yes elif [ "x$arg" = "x--help" ] ; then echo "Usage: ./configure [options] , where options are:" echo "--help : prints this help" echo "--enable-debug : turns on debugging flags and turns off optimization" echo "--enable-shared : turns on shared library creation (default no)" echo "--enable-64bits : turns on 64 bits compilation flags" echo "--lcgplatform=name : LCG platform name, default is x86_64-slc5-gcc43-opt" echo "--installdir=name : install directory, default is . " echo "--prefix=name : install directory (equivalent to --installdir)" echo "--datadir=name : data directory (for xmldoc), default is install directory" echo "--with-hepmc=path : path to HepMC library to build interface (default is not build)" echo "--with-hepmcversion=v : HepMC version (simplified alternative when using CERN AFS LCG external, e.g. =2.06.08)" echo "--enable-gzip : turns on support for reading in gzipped files (default no)" echo " (experimental feature, see README for more details)" echo "--with-boost=path : path to boost installation (default /usr) (required for gzip support)" echo "--with-zlib=path : path to zlib (default /usr/lib) (required for gzip support)" echo echo "Use the following environment variables to force the configuration process or add flags:" echo "USRCXXFLAGS - to add flags. Use this variable to add -fPIC to the compilation flags for the static libraries" echo "USRLDFLAGSSHARED - to add flags to the shared library build command" echo "USRSHAREDSUFFIX - to force shared libraries suffix to be like this (default on MacOSX is dylib)" echo exit elif [ x`echo x${arg} | grep "="` != x ] ; then option=`echo ${arg} | awk -F = '{print $1}'` value=`echo ${arg} | awk -F = '{print $2}'` if [ "x${option}" = "x--lcgplatform" ] ; then MYLCGPLATFORM=${value} elif [ "x${option}" = "x--installdir" ] ; then INSTALLDIR=${value} elif [ "x${option}" = "x--prefix" ] ; then INSTALLDIR=${value} elif [ "x${option}" = "x--datadir" ] ; then DATADIR=${value} elif [ "x${option}" = "x--with-hepmcversion" ] ; then HEPMCVERSION=${value} elif [ "x${option}" = "x--with-hepmc" ] ; then HEPMCLOCATION=${value} elif [ "x${option}" = "x--with-boost" ] ; then BOOSTLOCATION=${value} elif [ "x${option}" = "x--with-zlib" ] ; then ZLIBLOCATION=${value} else echo "${arg}: wrong option. Ignored." >&2 fi fi done echo compilation mode is $COMPMODE echo sharedlibs = $SHAREDLIBS if [ "x${DATADIR}" = "x" ] ; then DATADIR=${INSTALLDIR} fi # Environment variables for building HepMC interface library. Note that # the HepMC interface library is used by the examples main41, main42, .. . # Attention: if you have already run these examples and you change HepMC # version you should reset your LD_LIBRARY_PATH # The default values here correspond to CERN AFS lcg external # if [ "x${HEPMCVERSION}" != "x" ] ; then if [ "x${HEPMCLOCATION}" = "x" ] ; then export HEPMCLOCATION=/afs/cern.ch/sw/lcg/external/HepMC/${HEPMCVERSION}/${MYLCGPLATFORM} fi fi # If you want to assign these variables by hand: # #export HEPMCVERSION=2.04.00 #export HEPMCLOCATION=/afs/cern.ch/sw/lcg/external/HepMC/${HEPMCVERSION}/${MYLCGPLATFORM} if [ "x${HEPMCVERSION}" = "x" ] ; then if [ "x${HEPMCLOCATION}" != "x" ] ; then # try to find out which HepMC version test1=`echo $HEPMCLOCATION | grep \/1.` test2=`echo $HEPMCLOCATION | grep \/2.` echo $test1 echo $test2 if [ "x${test1}" != "x" ] ; then echo "Warning: HepMC 1 cannot be used anymore; Please use HepMC 2" echo " The interface will not be built" export HEPMCLOCATION= fi if [ "x${test2}" != "x" ] ; then export HEPMCVERSION=2.`echo $HEPMCLOCATION | awk -F \/2. '{print $2}' | awk -F \/ '{print $1}'` fi fi fi if [ "x${HEPMCVERSION}" != "x" ] ; then export HEPMCMAINVERSION=`echo ${HEPMCVERSION} | awk -F . '{print$1}'` if [ ${HEPMCMAINVERSION} = 1 ] ; then echo "Warning: HepMC 1 cannot be used anymore; Please use HepMC 2" echo " The interface will not be built" export HEPMCLOCATION= fi fi if [ "x${HEPMCLOCATION}" != "x" ] ; then if [ "x${HEPMCVERSION}" = "x" ] ; then echo "Warning: hepmc specified, but cannot find out which HepMC version" echo "Warning: if you specify HepMC 1 the compilation of interface will fail" fi fi # # User-changeable part, experts ----------------------------- # # Switch off -Wshadow when gzip support is enabled WSHADOW="-Wshadow" if [ "x${ENABLEGZIP}" = "xyes" ]; then WSHADOW="" fi # export FFLAGS_OPT="-O2 -Wuninitialized" # -Wuninitialized outputs many irrelevant warnings and therefore obscurs export FFLAGS_OPT="-O2" export FFLAGS_DBG=-g export CFLAGS_OPT="-O2" export CFLAGS_DBG=-g export CXXFLAGS_OPT="-O2 -ansi -pedantic -W -Wall ${WSHADOW} ${ENABLE64}" export CXXFLAGS_DBG="-g -ansi -pedantic -W -Wall ${WSHADOW} ${ENABLE64}" # # Find platform. # export ARCH0="`uname`" export ARCH=${ARCH0} export theGcc=`gcc -dumpversion | awk -F . '{print $1}'` if [ ${theGcc} = 4 ]; then export ARCH=${ARCH}-gcc4 fi echo Platform is $ARCH #default platform settings: export FCCOPY=$FC if [ x$FC = x ]; then export FC=g77 fi if [ x$CC = x ]; then export CC=gcc fi export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" export FLIBS="-lfrtbegin -lg2c" if [ ${COMPMODE} = OPT ]; then export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" fi if [ ${COMPMODE} = DBG ]; then export FFLAGS="${FFLAGS_DBG}" export CFLAGS="${CFLAGS_DBG}" export CXXFLAGS="${CXXFLAGS_DBG}" fi LDFLAGSSHARED="${CXXFLAGS} -fPIC -shared" LDFLAGLIBNAME="-Wl,-soname" SHAREDSUFFIX=so if [ $ARCH = Linux ]; then if [ x$FCCOPY = x ]; then export FC=g77 fi export FFLAGS="${FFLAGS_OPT} -Wno-globals" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" export FLIBS="-lfrtbegin -lg2c" if [ ${COMPMODE} = OPT ]; then export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" fi if [ ${COMPMODE} = DBG ]; then export FFLAGS="${FFLAGS_DBG} -Wno-globals" export CFLAGS="${CFLAGS_DBG}" export CXXFLAGS="${CXXFLAGS_DBG}" fi LDFLAGSSHARED="${CXXFLAGS} -fPIC -shared" LDFLAGLIBNAME="-Wl,-soname" SHAREDSUFFIX=so fi # Linux platform with gcc4: new Fortran90 compiler. if [ $ARCH = Linux-gcc4 ]; then if [ x$FCCOPY = x ]; then export FC=gfortran fi export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" export FLIBS="-lgfortran -lgfortranbegin" if [ ${COMPMODE} = OPT ]; then export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" fi if [ ${COMPMODE} = DBG ]; then export FFLAGS="${FFLAGS_DBG}" export CFLAGS="${CFLAGS_DBG}" export CXXFLAGS="${CXXFLAGS_DBG}" fi LDFLAGSSHARED="${CXXFLAGS} -fPIC -shared" LDFLAGLIBNAME="-Wl,-soname" SHAREDSUFFIX=so fi # Mac-OSX with gcc4 if [ $ARCH = Darwin-gcc4 ]; then if [ x$FCCOPY = x ]; then export FC=gfortran fi export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" export FLIBS="-lgfortran" if [ ${COMPMODE} = OPT ]; then export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" fi if [ ${COMPMODE} = DBG ]; then export FFLAGS="${FFLAGS_DBG}" export CFLAGS="${CFLAGS_DBG}" export CXXFLAGS="${CXXFLAGS_DBG}" fi LDFLAGSSHARED="${CXXFLAGS} -dynamiclib -single_module -flat_namespace -undefined suppress" LDFLAGLIBNAME="-Wl,-dylib_install_name" SHAREDSUFFIX=dylib fi # Mac-OSX with gcc3; is not tested if [ $ARCH = Darwin ]; then if [ x$FCCOPY = x ]; then export FC=g77 fi export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" export FLIBS="-lfrtbegin -lg2c" if [ ${COMPMODE} = OPT ]; then export FFLAGS="${FFLAGS_OPT}" export CFLAGS="${CFLAGS_OPT}" export CXXFLAGS="${CXXFLAGS_OPT}" fi if [ ${COMPMODE} = DBG ]; then export FFLAGS="${FFLAGS_DBG}" export CFLAGS="${CFLAGS_DBG}" export CXXFLAGS="${CXXFLAGS_DBG}" fi LDFLAGSSHARED="${CXXFLAGS} -dynamiclib -single_module -flat_namespace -undefined suppress" LDFLAGLIBNAME="-Wl,-dylib_install_name" SHAREDSUFFIX=dylib fi CXXFLAGS="${CXXFLAGS} $USRCXXFLAGS" LDFLAGSSHARED="${LDFLAGSSHARED} $USRLDFLAGSSHARED" if [ "x${USRSHAREDSUFFIX}" != "x" ] ; then SHAREDSUFFIX="${USRSHAREDSUFFIX}" fi #Platform & opt/dbg - independent flags and variables: # # End of the user-changeable part --------------------------- # # Checks # if [ $?HEPMCLOCATION ]; then if [ x${HEPMCLOCATION} != x ]; then if [ ! -d ${HEPMCLOCATION}/include ]; then echo "Warning: bad HEPMCLOCATION: directory ${HEPMCLOCATION}/include does not exist" echo " The interface will not be built" export HEPMCLOCATION= fi if [ ! -d ${HEPMCLOCATION}/lib ]; then echo "Warning: bad HEPMCLOCATION: directory ${HEPMCLOCATION}/lib does not exist" echo " The interface will not be built" export HEPMCLOCATION= fi fi fi # gzip support - do after SHAREDSUFFIX is set if [ "x${ENABLEGZIP}" = "xyes" ]; then # Default locations if none given if [ "x${BOOSTLOCATION}" = "x" ]; then BOOSTLOCATION=/usr fi if [ "x${ZLIBLOCATION}" = "x" ]; then ZLIBLOCATION=/usr/lib fi # Check for Boost and zlib if [ "x${ENABLEGZIP}" = "xyes" ] ; then if [ ! -d "${BOOSTLOCATION}/include/boost/iostreams" ]; then echo "Error: cannot find required Boost include files; gzip support disabled" ENABLEGZIP=no fi # Some systems have Boost only under lib64? for i in lib lib64; do if [ -f "${BOOSTLOCATION}/$i/libboost_iostreams.${SHAREDSUFFIX}" ]; then BOOSTLIBLOCATION=${BOOSTLOCATION}/$i break fi done if [ "x${ENABLEGZIP}" = "xyes" -a x"${BOOSTLIBLOCATION}" = x ]; then echo "Error: cannot find required Boost library files; gzip support disabled" ENABLEGZIP=no fi if [ "x${ENABLEGZIP}" = "xyes" -a ! -f "${ZLIBLOCATION}/libz.${SHAREDSUFFIX}" ]; then echo "Error: cannot find zlib; gzip support disabled" ENABLEGZIP=no fi fi # Add flags if [ "x${ENABLEGZIP}" = "xyes" ] ; then echo gzip support is enabled CXXFLAGS="${CXXFLAGS} -DGZIPSUPPORT -I${BOOSTLOCATION}/include" fi fi rm -f config.mk echo SHELL = /bin/sh > config.mk echo ARCH = ${ARCH} >> config.mk echo MYLCGPLATFORM = ${MYLCGPLATFORM} >> config.mk echo SHAREDLIBS = ${SHAREDLIBS} >> config.mk echo FC = ${FC} >> config.mk echo CC = ${CC} >> config.mk echo FFLAGS = ${FFLAGS} >> config.mk echo CFLAGS = ${CFLAGS} >> config.mk echo CXXFLAGS = ${CXXFLAGS} >> config.mk echo FLIBS = ${FLIBS} >> config.mk echo LDFLAGSSHARED = ${LDFLAGSSHARED} >> config.mk echo LDFLAGLIBNAME = ${LDFLAGLIBNAME} >> config.mk echo SHAREDSUFFIX = ${SHAREDSUFFIX} >> config.mk echo INSTALLDIR = ${INSTALLDIR} >> config.mk echo DATADIR = ${DATADIR} >> config.mk # if [ x${HEPMCLOCATION} != x ]; then if [ x${HEPMCVERSION} != x ]; then echo HEPMCVERSION = ${HEPMCVERSION} >> config.mk fi echo HEPMCLOCATION = ${HEPMCLOCATION} >> config.mk fi # # # rm -f examples/config.sh rm -f examples/config.csh if [ x${HEPMCLOCATION} != x ]; then if [ $ARCH0 != Darwin ]; then echo "#!/bin/csh" > examples/config.csh echo 'if( ! $?LD_LIBRARY_PATH ) then' >> examples/config.csh echo " setenv LD_LIBRARY_PATH ${HEPMCLOCATION}/lib" >> examples/config.csh echo "else" >> examples/config.csh echo " setenv LD_LIBRARY_PATH" '${LD_LIBRARY_PATH}'":${HEPMCLOCATION}/lib" >> examples/config.csh echo "endif" >> examples/config.csh echo "#!/bin/sh" > examples/config.sh echo 'if [ ! $?LD_LIBRARY_PATH ]; then' >> examples/config.sh echo " export LD_LIBRARY_PATH=${HEPMCLOCATION}/lib" >> examples/config.sh echo fi >> examples/config.sh echo 'if [ $?LD_LIBRARY_PATH ]; then' >> examples/config.sh echo " export LD_LIBRARY_PATH="'${LD_LIBRARY_PATH}'":${HEPMCLOCATION}/lib" >> examples/config.sh echo fi >> examples/config.sh else echo "#!/bin/csh" > examples/config.csh echo 'if( ! $?DYLD_LIBRARY_PATH ) then' >> examples/config.csh echo " setenv DYLD_LIBRARY_PATH ${HEPMCLOCATION}/lib" >> examples/config.csh echo "else" >> examples/config.csh echo " setenv DYLD_LIBRARY_PATH" '${DYLD_LIBRARY_PATH}'":${HEPMCLOCATION}/lib" >> examples/config.csh echo "endif" >> examples/config.csh echo "#!/bin/sh" > examples/config.sh echo 'if [ ! $?DYLD_LIBRARY_PATH ]; then' >> examples/config.sh echo " export DYLD_LIBRARY_PATH=${HEPMCLOCATION}/lib" >> examples/config.sh echo fi >> examples/config.sh echo 'if [ $?DYLD_LIBRARY_PATH ]; then' >> examples/config.sh echo " export DYLD_LIBRARY_PATH="'${DYLD_LIBRARY_PATH}'":${HEPMCLOCATION}/lib" >> examples/config.sh echo fi >> examples/config.sh fi fi # gzip support - write locations into config.mk if [ "x${ENABLEGZIP}" = "xyes" ] ; then echo "ENABLEGZIP = yes" >> config.mk echo "BOOSTLOCATION = ${BOOSTLOCATION}" >> config.mk echo "BOOSTLIBLOCATION = ${BOOSTLIBLOCATION}" >> config.mk echo "ZLIBLOCATION = ${ZLIBLOCATION}" >> config.mk fi # Substitute into pythia8-config script mkdir -p bin sed -e "s:@prefix@:$INSTALLDIR:" -e "s:@datadir@:$DATADIR:" \ -e "s:@HEPMCPATH@:$HEPMCLOCATION:" \ -e "s:@ENABLEGZIP@:$ENABLEGZIP:" \ -e "s:@ZLIBPATH@:$ZLIBLOCATION:" \ -e "s:@BOOSTINCPATH@:$BOOSTLOCATION:" \ -e "s:@BOOSTLIBPATH@:$BOOSTLIBLOCATION:" \ pythia8-config.in > bin/pythia8-config chmod +x bin/pythia8-config pythia8-8.1.80.orig/AUTHORS0000644000175000017500000000056612217364012013406 0ustar sunsunAUTHORS: Torbjorn Sjostrand Jesper Roy Christiansen Nishita Desai Philip Ilten Stephen Mrenna Stefan Prestel Peter Skands FORMER AUTHORS: Stefan Ask Richard Corke pythia8-8.1.80.orig/src/0000755000175000017500000000000012217616062013123 5ustar sunsunpythia8-8.1.80.orig/src/PartonSystems.cc0000644000175000017500000000700412217346246016272 0ustar sunsun// PartonSystems.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // PartonSystem and PartonSystems classes. #include "Pythia8/PartonSystems.h" namespace Pythia8 { //========================================================================== // The PartonSystems class. //-------------------------------------------------------------------------- // Replace the index of an incoming or outgoing parton by a new index. void PartonSystems::replace(int iSys, int iPosOld, int iPosNew) { if (systems[iSys].iInA == iPosOld) { systems[iSys].iInA = iPosNew; return; } if (systems[iSys].iInB == iPosOld) { systems[iSys].iInB = iPosNew; return; } for (int i = 0; i < sizeOut(iSys); ++i) if (systems[iSys].iOut[i] == iPosOld) { systems[iSys].iOut[i] = iPosNew; return; } } //-------------------------------------------------------------------------- // Return index of any parton in system, list starting with beam remnants. int PartonSystems::getAll(int iSys, int iMem) const { if (hasInAB(iSys)) { if (iMem == 0) return systems[iSys].iInA; if (iMem == 1) return systems[iSys].iInB; return systems[iSys].iOut[iMem - 2]; } else return systems[iSys].iOut[iMem]; } //-------------------------------------------------------------------------- // Find system of given outgoing parton, optionally also incoming one. int PartonSystems::getSystemOf(int iPos, bool alsoIn) const { // Loop over systems and over final-state members in each system. for (int iSys = 0; iSys < sizeSys(); ++iSys) { if (alsoIn) { if (systems[iSys].iInA == iPos) return iSys; if (systems[iSys].iInB == iPos) return iSys; } for (int iMem = 0; iMem < sizeOut(iSys); ++iMem) if (systems[iSys].iOut[iMem] == iPos) return iSys; } // Failure signalled by return value -1. return -1; } //-------------------------------------------------------------------------- // Get the iMem index of iOut for an index into the event record int PartonSystems::getIndexOfOut(int iSys, int iPos) const { for (int iMem = 0; iMem < sizeOut(iSys); ++iMem) if (systems[iSys].iOut[iMem] == iPos) return iMem; // Failure signalled by return value -1. return -1; } //-------------------------------------------------------------------------- // Print members in systems; for debug mainly. void PartonSystems::list(ostream& os) const { // Header. os << "\n -------- PYTHIA Parton Systems Listing -------------------" << "--------------------------------- " << "\n \n no inA inB out members \n"; // Loop over system list and over members in each system. for (int iSys = 0; iSys < sizeSys(); ++iSys) { os << " " << setw(3) << iSys << " " << setw(4) << systems[iSys].iInA << " " << setw(4) << systems[iSys].iInB; for (int iMem = 0; iMem < sizeOut(iSys); ++iMem) { if (iMem%16 == 0 && iMem > 0) os << "\n "; os << " " << setw(4) << systems[iSys].iOut[iMem]; } os << "\n"; } // Alternative if no systems. Done. if (sizeSys() == 0) os << " no systems defined \n"; os << "\n -------- End PYTHIA Parton Systems Listing ---------------" << "---------------------------------" << endl; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SLHAinterface.cc0000644000175000017500000004102412217346251016043 0ustar sunsun// SLHAinterface.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // Main authors of this file: N. Desai, P. Skands // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. #include "Pythia8/SLHAinterface.h" namespace Pythia8 { //========================================================================== // The SLHAinterface class. //-------------------------------------------------------------------------- // Initialize and switch to SUSY couplings if reading SLHA spectrum. void SLHAinterface::init( Settings& settings, Rndm* rndmPtr, Couplings* couplingsPtrIn, ParticleData* particleDataPtr, bool& useSLHAcouplings) { // Initialize SLHA couplingsPtr to PYTHIA one by default couplingsPtr = couplingsPtrIn; useSLHAcouplings = false; // Check if SUSY couplings need to be read in if( !initSLHA(settings, particleDataPtr)) infoPtr->errorMsg("Error in SLHAinterface::init: " "Could not read SLHA file"); // SLHA sets isSUSY flag to tell us if there was an SLHA SUSY spectrum if (couplingsPtr->isSUSY) { // Initialize the derived SUSY couplings class (SM first, then SUSY) coupSUSY.init( settings, rndmPtr); coupSUSY.initSUSY(&slha, &settings, particleDataPtr); // Switch couplingsPtr to point to the derived class // and tell PYTHIA to use it couplingsPtr = (Couplings *) &coupSUSY; useSLHAcouplings = true; } } //-------------------------------------------------------------------------- // Initialize SUSY Les Houches Accord data. bool SLHAinterface::initSLHA(Settings& settings, ParticleData* particleDataPtr) { // Error and warning prefixes for this method string errPref = "Error in SLHAinterface::initSLHA(): "; string warnPref = "Warning in SLHAinterface::initSLHA(): "; string infoPref = "Info from SLHAinterface::initSLHA(): "; // Initial and settings values. int ifailLHE = 1; int ifailSpc = 1; int readFrom = settings.mode("SLHA:readFrom"); string lhefFile = settings.word("Beams:LHEF"); string lhefHeader = settings.word("Beams:LHEFheader"); string slhaFile = settings.word("SLHA:file"); int verboseSLHA = settings.mode("SLHA:verbose"); bool slhaUseDec = settings.flag("SLHA:useDecayTable"); // Set internal data members meMode = settings.mode("SLHA:meMode"); // No SUSY by default couplingsPtr->isSUSY = false; // Option with no SLHA read-in at all. if (readFrom == 0) return true; // First check LHEF header (if reading from LHEF) if (readFrom == 1) { if (lhefHeader != "void") ifailLHE = slha.readFile(lhefHeader, verboseSLHA, slhaUseDec ); else if (lhefFile != "void") ifailLHE = slha.readFile(lhefFile, verboseSLHA, slhaUseDec ); } // If LHEF read successful, everything needed should already be ready if (ifailLHE == 0) { ifailSpc = 0; couplingsPtr->isSUSY = true; // If no LHEF file or no SLHA info in header, read from SLHA:file } else { lhefFile = "void"; if ( settings.word("SLHA:file") == "none" || settings.word("SLHA:file") == "void" || settings.word("SLHA:file") == "" || settings.word("SLHA:file") == " ") return true; ifailSpc = slha.readFile(slhaFile,verboseSLHA, slhaUseDec); } // In case of problems, print error and fail init. if (ifailSpc != 0) { infoPtr->errorMsg(errPref + "problem reading SLHA file", slhaFile); return false; } else { couplingsPtr->isSUSY = true; } // Check spectrum for consistency. Switch off SUSY if necessary. ifailSpc = slha.checkSpectrum(); // ifail >= 1 : no MODSEL found -> don't switch on SUSY if (ifailSpc == 1) { // no SUSY, but MASS ok couplingsPtr->isSUSY = false; infoPtr->errorMsg(infoPref + "No MODSEL found, keeping internal SUSY switched off"); } else if (ifailSpc >= 2) { // no SUSY, but problems infoPtr->errorMsg(warnPref + "Problem with SLHA MASS or QNUMBERS."); couplingsPtr->isSUSY = false; } // ifail = 0 : MODSEL found, spectrum OK else if (ifailSpc == 0) { // Print spectrum. Done. slha.printSpectrum(0); } else if (ifailSpc < 0) { infoPtr->errorMsg(warnPref + "Problem with SLHA spectrum.", "\n Only using masses and switching off SUSY."); settings.flag("SUSY:all", false); couplingsPtr->isSUSY = false; slha.printSpectrum(ifailSpc); } // Import qnumbers if ( (ifailSpc == 1 || ifailSpc == 0) && slha.qnumbers.size() > 0) { for (int iQnum=0; iQnum < int(slha.qnumbers.size()); iQnum++) { // Always use positive id codes int id = abs(slha.qnumbers[iQnum](0)); ostringstream idCode; idCode << id; if (particleDataPtr->isParticle(id)) { infoPtr->errorMsg(warnPref + "ignoring QNUMBERS", "for id = " + idCode.str() + " (already exists)", true); } else { int qEM3 = slha.qnumbers[iQnum](1); int nSpins = slha.qnumbers[iQnum](2); int colRep = slha.qnumbers[iQnum](3); int hasAnti = slha.qnumbers[iQnum](4); // Translate colRep to PYTHIA colType int colType = 0; if (colRep == 3) colType = 1; else if (colRep == -3) colType = -1; else if (colRep == 8) colType = 2; else if (colRep == 6) colType = 3; else if (colRep == -6) colType = -3; // Default name: PDG code string name, antiName; ostringstream idStream; idStream<addParticle(id, name, nSpins, qEM3, colType); } else { particleDataPtr->addParticle(id, name, antiName, nSpins, qEM3, colType); } } } } // Import mass spectrum. bool keepSM = settings.flag("SLHA:keepSM"); double minMassSM = settings.parm("SLHA:minMassSM"); bool allowUserOverride = settings.flag("SLHA:allowUserOverride"); vector idModified; if (ifailSpc == 1 || ifailSpc == 0) { // Loop through to update particle data. int id = slha.mass.first(); ostringstream idCode; idCode << id; for (int i = 1; i <= slha.mass.size() ; i++) { double mass = abs(slha.mass(id)); // Ignore masses for known SM particles or particles with // default masses < minMassSM; overwrite masses for rest. if (keepSM && (id < 25 || (id > 80 && id < 1000000))) ; else if (id < 1000000 && particleDataPtr->m0(id) < minMassSM) { infoPtr->errorMsg(warnPref + "ignoring MASS entry", "for id = " + idCode.str() + " (m0 < SLHA:minMassSM)", true); } // Also ignore SLHA mass values if user has already set // a different value and is allowed to override them. else if (allowUserOverride && particleDataPtr->hasChanged(id)) { ostringstream mValue; mValue << particleDataPtr->m0(id); infoPtr->errorMsg(warnPref + "keeping user mass", "for id = " + idCode.str() + ", m0 = " + mValue.str(), true); idModified.push_back(id); } else { particleDataPtr->m0(id,mass); idModified.push_back(id); } // Go to next MASS entry id = slha.mass.next(); }; } // Update decay data. for (int iTable=0; iTable < int(slha.decays.size()); iTable++) { // Pointer to this SLHA table LHdecayTable* slhaTable=&(slha.decays[iTable]); // Extract ID and create pointer to corresponding particle data object int idRes = slhaTable->getId(); ostringstream idCode; idCode << idRes; ParticleDataEntry* particlePtr = particleDataPtr->particleDataEntryPtr(idRes); // Ignore decay channels for known SM particles or particles with // default masses < minMassSM; overwrite masses for rest. if (keepSM && (idRes < 25 || (idRes > 80 && idRes < 1000000))) continue; else if (idRes < 1000000 && particleDataPtr->m0(idRes) < minMassSM) { infoPtr->errorMsg(warnPref + "ignoring DECAY table", "for id = " + idCode.str() + " (m0 < SLHA:minMassSM)", true); continue; } // Extract and store total width (absolute value, neg -> switch off) double widRes = abs(slhaTable->getWidth()); double pythiaMinWidth = settings.parm("ResonanceWidths:minWidth"); if (widRes > 0. && widRes < pythiaMinWidth) { infoPtr->errorMsg(warnPref + "forcing width = 0 ","for id = " + idCode.str() + " (width < ResonanceWidths:minWidth)" , true); widRes = 0.0; } particlePtr->setMWidth(widRes); // Set lifetime in mm for displaced vertex calculations // (convert GeV^-1 to mm) if (widRes > 0.) { double decayLength = 1.97e-13/widRes; particlePtr->setTau0(decayLength); // Reset decay table of the particle. Allow decays, treat as resonance. if (slhaTable->size() > 0) { particlePtr->clearChannels(); particleDataPtr->mayDecay(idRes,true); particleDataPtr->isResonance(idRes,true); } else { infoPtr->errorMsg(warnPref + "empty DECAY table ","for id = " + idCode.str() + " (total width provided but no branching fractions)", true); } } // Reset to stable if width <= 0.0 else { particleDataPtr->mayDecay(idRes,false); } // Set initial minimum mass. double brWTsum = 0.; double massWTsum = 0.; // Loop over SLHA channels, import into Pythia, treating channels // with negative branching fractions as having the equivalent positive // branching fraction, but being switched off for this run for (int iChannel=0 ; iChannelsize(); iChannel++) { LHdecayChannel slhaChannel = slhaTable->getChannel(iChannel); double brat = slhaChannel.getBrat(); vector idDa = slhaChannel.getIdDa(); if (idDa.size() >= 9) { infoPtr->errorMsg(errPref + "max number of DECAY products is 8"); } else if (idDa.size() <= 1) { infoPtr->errorMsg(errPref + "min number of DECAY products is 2"); } else { int onMode = 1; if (brat < 0.0) onMode = 0; int meModeNow = meMode; // Check phase space, including margin ~ sqrt(sum(widths^2)) double massSum(0.); double widSqSum = pow2(widRes); int nDa = idDa.size(); for (int jDa=0; jDam0( idDa[jDa] ); widSqSum += pow2(particleDataPtr->mWidth( idDa[jDa] )); } double deltaM = particleDataPtr->m0(idRes) - massSum; // Negative mass difference: intrinsically off shell if (onMode == 1 && brat > 0.0 && deltaM < 0.) { // String containing decay name ostringstream errCode; errCode << idRes <<" ->"; for (int jDa=0; jDa 100. * sqrt(widSqSum)) { infoPtr->errorMsg(warnPref + "switched off DECAY mode", ": " + errCode.str()+" (too far off shell)",true); onMode = 0; } // If ~ OK within fluctuations else { // Ignore user-selected meMode if (meModeNow != 100) { infoPtr->errorMsg(warnPref + "adding off shell DECAY mode", ": "+errCode.str()+" (forced meMode = 100)",true); meModeNow = 100; } else { infoPtr->errorMsg(warnPref + "adding off shell DECAY mode", errCode.str(), true); } } } // Branching-ratio-weighted average mass in decay. brWTsum += abs(brat); massWTsum += abs(brat) * massSum; // Add channel int id0 = idDa[0]; int id1 = idDa[1]; int id2 = (idDa.size() >= 3) ? idDa[2] : 0; int id3 = (idDa.size() >= 4) ? idDa[3] : 0; int id4 = (idDa.size() >= 5) ? idDa[4] : 0; int id5 = (idDa.size() >= 6) ? idDa[5] : 0; int id6 = (idDa.size() >= 7) ? idDa[6] : 0; int id7 = (idDa.size() >= 8) ? idDa[7] : 0; particlePtr->addChannel(onMode,abs(brat),meModeNow, id0,id1,id2,id3,id4,id5,id6,id7); } } // Set minimal mass, but always below nominal one. if (slhaTable->size() > 0) { double massAvg = massWTsum / brWTsum; double massMin = min( massAvg, particlePtr->m0()) ; particlePtr->setMMin(massMin); } // Add to list of particles that have been modified idModified.push_back(idRes); } // Sanity check of all decay tables with modified MASS or DECAY info for (int iMod = 0; iMod < int(idModified.size()); ++iMod) { int id = idModified[iMod]; ostringstream idCode; idCode << id; ParticleDataEntry* particlePtr = particleDataPtr->particleDataEntryPtr(id); double m0 = particlePtr->m0(); double wid = particlePtr->mWidth(); // Always set massless particles stable if (m0 <= 0.0 && (wid > 0.0 || particlePtr->mayDecay())) { infoPtr->errorMsg(warnPref + "massless particle forced stable"," id = " + idCode.str(), true); particlePtr->setMWidth(0.0); particlePtr->setMayDecay(false); continue; } // Declare zero-width particles to be stable if (wid == 0.0 && particlePtr->mayDecay()) { particlePtr->setMayDecay(false); continue; } // Check at least one on-shell channel is available double mSumMin = 10. * m0; int nChannels = particlePtr->sizeChannels(); for (int iChannel=0; iChannelchannel(iChannel); if (channel.onMode() <= 0) continue; int nProd = channel.multiplicity(); double mSum = 0.; for (int iDa = 0; iDa < nProd; ++iDa) { int idDa = channel.product(iDa); mSum += particleDataPtr->m0(idDa); } mSumMin = min(mSumMin, mSum); } // Require at least one on-shell channel if (mSumMin > m0) { infoPtr->errorMsg(warnPref + "particle forced stable"," id = " + idCode.str() + " (no on-shell decay channels)", true); particlePtr->setMWidth(0.0); particlePtr->setMayDecay(false); continue; } else { // mMin: lower cutoff on Breit-Wigner: default is mMin = m0 - 5*Gamma // (User is allowed to specify a lower value if desired.) // Increase minimum if needed to ensure at least one channel on shell double mMin = min(particlePtr->mMin(), max(0.0,m0 - 5.*wid)); mMin = max(mSumMin,mMin); particlePtr->setMMin(mMin); } } return true; } //-------------------------------------------------------------------------- // Initialize SLHA blocks SMINPUTS and MASS from PYTHIA SM parameter values. // E.g., to make sure that there are no important unfilled entries void SLHAinterface::pythia2slha(ParticleData* particleDataPtr) { // Initialize block SMINPUTS. string blockName = "sminputs"; double mZ = particleDataPtr->m0(23); slha.set(blockName,1,1.0/couplingsPtr->alphaEM(pow2(mZ))); slha.set(blockName,2,couplingsPtr->GF()); slha.set(blockName,3,couplingsPtr->alphaS(pow2(mZ))); slha.set(blockName,4,mZ); // b mass (should be running mass, here pole for time being) slha.set(blockName,5,particleDataPtr->m0(5)); slha.set(blockName,6,particleDataPtr->m0(6)); slha.set(blockName,7,particleDataPtr->m0(15)); slha.set(blockName,8,particleDataPtr->m0(16)); slha.set(blockName,11,particleDataPtr->m0(11)); slha.set(blockName,12,particleDataPtr->m0(12)); slha.set(blockName,13,particleDataPtr->m0(13)); slha.set(blockName,14,particleDataPtr->m0(14)); // Force 3 lightest quarks massless slha.set(blockName,21,double(0.0)); slha.set(blockName,22,double(0.0)); slha.set(blockName,23,double(0.0)); // c mass (should be running mass, here pole for time being) slha.set(blockName,24,particleDataPtr->m0(4)); // Initialize block MASS. blockName = "mass"; int id = 1; int count = 0; while (particleDataPtr->nextId(id) > id) { slha.set(blockName,id,particleDataPtr->m0(id)); id = particleDataPtr->nextId(id); ++count; if (count > 10000) { infoPtr->errorMsg("Error in SLHAinterface::pythia2slha(): " "encountered infinite loop when saving mass block"); break; } } } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaOnia.cc0000644000175000017500000005023612217346251015307 0ustar sunsun// SigmaOnia.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // charmonia/bottomonia simulation classes. #include "Pythia8/SigmaOnia.h" namespace Pythia8 { //========================================================================== // Sigma2gg2QQbar3S11g class. // Cross section g g -> QQbar[3S1(1)] g (Q = c or b). //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2QQbar3S11g::initProc() { // Produced state. Process name. Onium matrix element. idHad = (idNew == 4) ? 443 : 553; nameSave = (idNew == 4) ? "g g -> ccbar[3S1(1)] g" : "g g -> bbbar[3S1(1)] g"; oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:OJpsi3S11") : settingsPtr->parm("Bottomonium:OUpsilon3S11"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat); no explicit flavour dependence. void Sigma2gg2QQbar3S11g::sigmaKin() { // Calculate kinematics dependence. double stH = sH + tH; double tuH = tH + uH; double usH = uH + sH; double sig = (10. * M_PI / 81.) * m3 * ( pow2(sH * tuH) + pow2(tH * usH) + pow2(uH * stH) ) / pow2( stH * tuH * usH ); // Answer. sigma = (M_PI/sH2) * pow3(alpS) * oniumME * sig; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2QQbar3S11g::setIdColAcol() { // Flavours are trivial. setId( id1, id2, idHad, 21); // Two orientations of colour flow.. setColAcol( 1, 2, 2, 3, 0, 0, 1, 3); if (rndmPtr->flat() > 0.5) swapColAcol(); } //========================================================================== // Sigma2gg2QQbar3PJ1g class. // Cross section g g -> QQbar[3PJ(1)] g (Q = c or b, J = 0, 1 or 2). //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2QQbar3PJ1g::initProc() { // Produced state. Process name. Onium matrix element. idHad = 0; nameSave = "illegal process"; if (jSave == 0) { idHad = (idNew == 4) ? 10441 : 10551; nameSave = (idNew == 4) ? "g g -> ccbar[3P0(1)] g" : "g g -> bbbar[3P0(1)] g"; } else if (jSave == 1) { idHad = (idNew == 4) ? 20443 : 20553; nameSave = (idNew == 4) ? "g g -> ccbar[3P1(1)] g" : "g g -> bbbar[3P1(1)] g"; } else if (jSave == 2) { idHad = (idNew == 4) ? 445 : 555; nameSave = (idNew == 4) ? "g g -> ccbar[3P2(1)] g" : "g g -> bbbar[3P2(1)] g"; } oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:Ochic03P01") : settingsPtr->parm("Bottomonium:Ochib03P01"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat); no explicit flavour dependence. void Sigma2gg2QQbar3PJ1g::sigmaKin() { // Useful derived kinematics quantities. double pRat = (sH * uH + uH * tH + tH * sH)/ sH2; double qRat = tH * uH / sH2; double rRat = s3 / sH; double pRat2 = pRat * pRat; double pRat3 = pRat2 * pRat; double pRat4 = pRat3 * pRat; double qRat2 = qRat * qRat; double qRat3 = qRat2 * qRat; double qRat4 = qRat3 * qRat; double rRat2 = rRat * rRat; double rRat3 = rRat2 * rRat; double rRat4 = rRat3 * rRat; // Calculate kinematics dependence. double sig = 0.; if (jSave == 0) { sig = (8. * M_PI / (9. * m3 * sH)) * ( 9. * rRat2 * pRat4 * (rRat4 - 2. * rRat2 * pRat + pRat2) - 6. * rRat * pRat3 * qRat * (2. * rRat4 - 5. * rRat2 * pRat + pRat2) - pRat2 * qRat2 * (rRat4 + 2. * rRat2 * pRat - pRat2) + 2. * rRat * pRat * qRat3 * (rRat2 - pRat) + 6. * rRat2 * qRat4) / (qRat * pow4(qRat - rRat * pRat)); } else if (jSave == 1) { sig = (8. * M_PI / (3.* m3 * sH)) * pRat2 * (rRat * pRat2 * (rRat2 - 4. * pRat) + 2. * qRat * (-rRat4 + 5. * rRat2 * pRat + pRat2) - 15. * rRat * qRat2) / pow4(qRat - rRat * pRat); } else if (jSave == 2) { sig = (8. * M_PI / (9. * m3 * sH)) * (12. * rRat2 * pRat4 * (rRat4 - 2. * rRat2 * pRat + pRat2) - 3. * rRat * pRat3 * qRat * (8. * rRat4 - rRat2 * pRat + 4. * pRat2) + 2. * pRat2 * qRat2 * (-7. * rRat4 + 43. * rRat2 * pRat + pRat2) + rRat * pRat * qRat3 * (16. * rRat2 - 61. * pRat) + 12. * rRat2 * qRat4) / (qRat * pow4(qRat-rRat * pRat)); } // Answer. sigma = (M_PI/sH2) * pow3(alpS) * oniumME * sig; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2QQbar3PJ1g::setIdColAcol() { // Flavours are trivial. setId( id1, id2, idHad, 21); // Two orientations of colour flow. setColAcol( 1, 2, 2, 3, 0, 0, 1, 3); if (rndmPtr->flat() > 0.5) swapColAcol(); } //========================================================================== // Sigma2qg2QQbar3PJ1q class. // Cross section q g -> QQbar[3PJ(1)] q (Q = c or b, J = 0, 1 or 2). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2QQbar3PJ1q::initProc() { // Produced state. Process name. Onium matrix element. idHad = 0; nameSave = "illegal process"; if (jSave == 0) { idHad = (idNew == 4) ? 10441 : 10551; nameSave = (idNew == 4) ? "q g -> ccbar[3P0(1)] q" : "q g -> bbbar[3P0(1)] q"; } else if (jSave == 1) { idHad = (idNew == 4) ? 20443 : 20553; nameSave = (idNew == 4) ? "q g -> ccbar[3P1(1)] q" : "q g -> bbbar[3P1(1)] q"; } else if (jSave == 2) { idHad = (idNew == 4) ? 445 : 555; nameSave = (idNew == 4) ? "q g -> ccbar[3P2(1)] q" : "q g -> bbbar[3P2(1)] q"; } oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:Ochic03P01") : settingsPtr->parm("Bottomonium:Ochib03P01"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat); no explicit flavour dependence. void Sigma2qg2QQbar3PJ1q::sigmaKin() { // Calculate kinematics dependence. double usH = uH + sH; double sig = 0.; if (jSave == 0) { sig = - (16. * M_PI / 81.) * pow2(tH - 3. * s3) * (sH2 + uH2) / (m3 * tH * pow4(usH)); } else if (jSave == 1) { sig = - (32. * M_PI / 27.) * (4. * s3 * sH * uH + tH * (sH2 + uH2)) / (m3 * pow4(usH)); } else if (jSave == 2) { sig = - (32. *M_PI / 81.) * ( (6. * s3*s3 + tH2) * pow2(usH) - 2. * sH * uH * (tH2 + 6. * s3 * usH)) / (m3 * tH * pow4(usH)); } // Answer. sigma = (M_PI/sH2) * pow3(alpS) * oniumME * sig; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2QQbar3PJ1q::setIdColAcol() { // Flavours are trivial. int idq = (id2 == 21) ? id1 : id2; setId( id1, id2, idHad, idq); // tH defined between q_in and q_out: must swap tHat <-> uHat if q g in. swapTU = (id2 == 21); // Colour flow topologies. Swap when antiquarks. if (id2 == 21) setColAcol( 1, 0, 2, 1, 0, 0, 2, 0); else setColAcol( 2, 1, 1, 0, 0, 0, 2, 0); if (idq < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2QQbar3PJ1g class. // Cross section q qbar -> QQbar[3PJ(1)] g (Q = c or b, J = 0, 1 or 2). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2QQbar3PJ1g::initProc() { // Produced state. Process name. Onium matrix element. idHad = 0; nameSave = "illegal process"; if (jSave == 0) { idHad = (idNew == 4) ? 10441 : 10551; nameSave = (idNew == 4) ? "q qbar -> ccbar[3P0(1)] g" : "q qbar -> bbbar[3P0(1)] g"; } else if (jSave == 1) { idHad = (idNew == 4) ? 20443 : 20553; nameSave = (idNew == 4) ? "q qbar -> ccbar[3P1(1)] g" : "q qbar -> bbbar[3P1(1)] g"; } else if (jSave == 2) { idHad = (idNew == 4) ? 445 : 555; nameSave = (idNew == 4) ? "q qbar -> ccbar[3P2(1)] g" : "q qbar -> bbbar[3P2(1)] g"; } oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:Ochic03P01") : settingsPtr->parm("Bottomonium:Ochib03P01"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat); no explicit flavour dependence. void Sigma2qqbar2QQbar3PJ1g::sigmaKin() { // Calculate kinematics dependence. double tuH = tH + uH; double sig = 0.; if (jSave == 0) { sig =(128. * M_PI / 243.) * pow2(sH - 3. * s3) * (tH2 + uH2) / (m3 * sH * pow4(tuH)); } else if (jSave == 1) { sig = (256. * M_PI / 81.) * (4. * s3 * tH * uH + sH * (tH2 + uH2)) / (m3 * pow4(tuH)); } else if (jSave == 2) { sig = (256. * M_PI / 243.) * ( (6. * s3*s3 + sH2) * pow2(tuH) - 2. * tH * uH * (sH2 + 6. * s3 * tuH) )/ (m3 * sH * pow4(tuH)); } // Answer. sigma = (M_PI/sH2) * pow3(alpS) * oniumME * sig; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2QQbar3PJ1g::setIdColAcol() { // Flavours are trivial. setId( id1, id2, idHad, 21); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 0, 0, 1, 2); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2gg2QQbarX8g class. // Cross section g g -> QQbar[X(8)] g (Q = c or b, X = 3S1, 1S0 or 3PJ). //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2QQbarX8g::initProc() { // Produced state. Process name. Onium matrix element. idHad = 0; nameSave = "illegal process"; if (stateSave == 0) { idHad = (idNew == 4) ? 9900443 : 9900553; nameSave = (idNew == 4) ? "g g -> ccbar[3S1(8)] g" : "g g -> bbbar[3S1(8)] g"; oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:OJpsi3S18") : settingsPtr->parm("Bottomonium:OUpsilon3S18"); } else if (stateSave == 1) { idHad = (idNew == 4) ? 9900441 : 9900551; nameSave = (idNew == 4) ? "g g -> ccbar[1S0(8)] g" : "g g -> bbbar[1S0(8)] g"; oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:OJpsi1S08") : settingsPtr->parm("Bottomonium:OUpsilon1S08"); } else if (stateSave == 2) { idHad = (idNew == 4) ? 9910441 : 9910551; nameSave = (idNew == 4) ? "g g -> ccbar[3PJ(8)] g" : "g g -> bbbar[3PJ(8)] g"; oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:OJpsi3P08") : settingsPtr->parm("Bottomonium:OUpsilon3P08"); } } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat); no explicit flavour dependence. void Sigma2gg2QQbarX8g::sigmaKin() { // Calculate kinematics dependence. double stH = sH + tH; double tuH = tH + uH; double usH = uH + sH; double sig = 0.; if (stateSave == 0) { sig = (M_PI / 72.) * m3 * ( 27. * (pow2(stH) + pow2(tuH) + pow2(usH)) / (s3*s3) - 16. ) * ( pow2(sH * tuH) + pow2(tH * usH) + pow2(uH * stH) ) / pow2( stH * tuH * usH ); } else if (stateSave == 1) { sig = (5. * M_PI / 16.) * m3 * ( pow2(uH / (tuH * usH)) + pow2(sH / (stH * usH)) + pow2(tH / (stH * tuH)) ) * ( 12. + (pow4(stH) + pow4(tuH) + pow4(usH)) / (s3 * sH * tH * uH) ); } else if (stateSave == 2) { double sH3 = sH2 * sH; double sH4 = sH3 * sH; double sH5 = sH4 * sH; double sH6 = sH5 * sH; double sH7 = sH6 * sH; double sH8 = sH7 * sH; double tH3 = tH2 * tH; double tH4 = tH3 * tH; double tH5 = tH4 * tH; double tH6 = tH5 * tH; double tH7 = tH6 * tH; double tH8 = tH7 * tH; double ssttH = sH * sH + sH * tH + tH * tH; sig = 5. * M_PI * (3. * sH * tH * stH * pow4(ssttH) - s3 * pow2(ssttH) * (7. * sH6 + 36. * sH5 * tH + 45. * sH4 * tH2 + 28. * sH3 * tH3 + 45. * sH2 * tH4 + 36. * sH * tH5 + 7. * tH6) + pow2(s3) * stH * (35. *sH8 + 169. * sH7 * tH + 299. * sH6 * tH2 + 401. * sH5 * tH3 + 418. * sH4 * tH4 + 401. * sH3 * tH5 + 299. * sH2 * tH6 + 169. * sH * tH7 + 35. * tH8) - pow3(s3) * (84. *sH8+432. *sH7*tH+905. *sH6*tH2 + 1287. * sH5 * tH3 + 1436. * sH4 * tH4 +1287. * sH3 * tH5 + 905. * sH2 * tH6 + 432. * sH * tH7 + 84. * tH8) + pow4(s3) * stH * (126. * sH6 + 451. * sH5 * tH +677. * sH4 * tH2 + 836. * sH3 * tH3 + 677. * sH2 * tH4 + 451. * sH * tH5 + 126. * tH6) - pow5(s3) * 3. * (42. * sH6 + 171. * sH5 * tH + 304. * sH4 * tH2 + 362. * sH3 * tH3 + 304. * sH2 * tH4 + 171. * sH * tH5 + 42. * tH6) + pow3(s3 * s3) * 2. * stH * (42. * sH4 + 106. * sH3 * tH + 119. * sH2 * tH2 + 106. * sH * tH3 + 42. * tH4) - pow4(s3) * pow3(s3) * (35. * sH4 + 99. * sH3 * tH + 120. * sH2 * tH2 + 99. * sH * tH3 + 35. * tH4) + pow4(s3 * s3) * 7. * stH * ssttH) / (sH * tH * uH * s3 * m3 * pow3(stH * tuH * usH)); } // Answer. sigma = (M_PI/sH2) * pow3(alpS) * oniumME * sig; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2QQbarX8g::setIdColAcol() { // Flavours are trivial. setId( id1, id2, idHad, 21); // Split total contribution into different colour flows just like in // g g -> g g (with kinematics recalculated for massless partons). double sHr = - (tH + uH); double sH2r = sHr * sHr; double sigTS = tH2/sH2r + 2.*tH/sHr + 3. + 2.*sHr/tH + sH2r/tH2; double sigUS = uH2/sH2r + 2.*uH/sHr + 3. + 2.*sHr/uH + sH2r/uH2; double sigTU = tH2/uH2 + 2.*tH/uH + 3. + 2.*uH/tH + uH2/tH2; double sigSum = sigTS + sigUS + sigTU; // Three colour flow topologies, each with two orientations. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 2, 2, 3, 1, 4, 4, 3); else if (sigRand < sigTS + sigUS) setColAcol( 1, 2, 3, 1, 3, 4, 4, 2); else setColAcol( 1, 2, 3, 4, 1, 4, 3, 2); if (rndmPtr->flat() > 0.5) swapColAcol(); } //========================================================================== // Sigma2qg2QQbarX8q class. // Cross section q g -> QQbar[X(8)] q (Q = c or b, X = 3S1, 1S0 or 3PJ). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2QQbarX8q::initProc() { // Produced state. Process name. Onium matrix element. idHad = 0; nameSave = "illegal process"; if (stateSave == 0) { idHad = (idNew == 4) ? 9900443 : 9900553; nameSave = (idNew == 4) ? "q g -> ccbar[3S1(8)] q" : "q g -> bbbar[3S1(8)] q"; oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:OJpsi3S18") : settingsPtr->parm("Bottomonium:OUpsilon3S18"); } else if (stateSave == 1) { idHad = (idNew == 4) ? 9900441 : 9900551; nameSave = (idNew == 4) ? "q g -> ccbar[1S0(8)] q" : "q g -> bbbar[1S0(8)] q"; oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:OJpsi1S08") : settingsPtr->parm("Bottomonium:OUpsilon1S08"); } else if (stateSave == 2) { idHad = (idNew == 4) ? 9910441 : 9910551; nameSave = (idNew == 4) ? "q g -> ccbar[3PJ(8)] q" : "q g -> bbbar[3PJ(8)] q"; oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:OJpsi3P08") : settingsPtr->parm("Bottomonium:OUpsilon3P08"); } } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat); no explicit flavour dependence. void Sigma2qg2QQbarX8q::sigmaKin() { // Calculate kinematics dependence. double stH = sH + tH; double tuH = tH + uH; double usH = uH + sH; double stH2 = stH * stH; double tuH2 = tuH * tuH; double usH2 = usH * usH; double sig = 0.; if (stateSave == 0) { sig = - (M_PI / 27.)* (4. * (sH2 + uH2) - sH * uH) * (stH2 +tuH2) / (s3 * m3 * sH * uH * usH2); } else if (stateSave == 1) { sig = - (5. * M_PI / 18.) * (sH2 + uH2) / (m3 * tH * usH2); } else if (stateSave == 2) { sig = - (10. * M_PI / 9.) * ( (7. * usH + 8. * tH) * (sH2 + uH2) + 4. * tH * (2. * pow2(s3) - stH2 - tuH2) ) / (s3 * m3 * tH * usH2 * usH); } // Answer. sigma = (M_PI/sH2) * pow3(alpS) * oniumME * sig; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2QQbarX8q::setIdColAcol() { // Flavours are trivial. int idq = (id2 == 21) ? id1 : id2; setId( id1, id2, idHad, idq); // tH defined between q_in and q_out: must swap tHat <-> uHat if q g in. swapTU = (id2 == 21); // Split total contribution into different colour flows just like in // q g -> q g (with kinematics recalculated for massless partons). double sHr = - (tH + uH); double sH2r = sHr * sHr; double sigTS = uH2/tH2 - (4./9.) * uH/sHr; double sigTU = sH2r/tH2 - (4./9.) * sHr/uH; double sigSum = sigTS + sigTU; // Two colour flow topologies. Swap if first is gluon, or when antiquark. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 0, 2, 1, 2, 3, 3, 0); else setColAcol( 1, 0, 2, 3, 1, 3, 2, 0); if (id1 == 21) swapCol12(); if (idq < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2QQbarX8g class. // Cross section q qbar -> QQbar[X(8)] g (Q = c or b, X = 3S1, 1S0 or 3PJ). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2QQbarX8g::initProc() { // Produced state. Process name. Onium matrix element. idHad = 0; nameSave = "illegal process"; if (stateSave == 0) { idHad = (idNew == 4) ? 9900443 : 9900553; nameSave = (idNew == 4) ? "q qbar -> ccbar[3S1(8)] g" : "q qbar -> bbbar[3S1(8)] g"; oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:OJpsi3S18") : settingsPtr->parm("Bottomonium:OUpsilon3S18"); } else if (stateSave == 1) { idHad = (idNew == 4) ? 9900441 : 9900551; nameSave = (idNew == 4) ? "q qbar -> ccbar[1S0(8)] g" : "q qbar -> bbbar[1S0(8)] g"; oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:OJpsi1S08") : settingsPtr->parm("Bottomonium:OUpsilon1S08"); } else if (stateSave == 2) { idHad = (idNew == 4) ? 9910441 : 9910551; nameSave = (idNew == 4) ? "q qbar -> ccbar[3PJ(8)] g" : "q qbar -> bbbar[3PJ(8)] g"; oniumME = (idNew == 4) ? settingsPtr->parm("Charmonium:OJpsi3P08") : settingsPtr->parm("Bottomonium:OUpsilon3P08"); } } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat); no explicit flavour dependence. void Sigma2qqbar2QQbarX8g::sigmaKin() { // Calculate kinematics dependence. double stH = sH + tH; double tuH = tH + uH; double usH = uH + sH; double stH2 = stH * stH; double tuH2 = tuH * tuH; double usH2 = usH * usH; double sig = 0.; if (stateSave == 0) { sig = (8. * M_PI / 81.) * (4. * (tH2 + uH2) - tH * uH) * (stH2 + usH2) / (s3 * m3 * tH * uH * tuH2); } else if (stateSave == 1) { sig = (20. * M_PI / 27.) * (tH2 + uH2) / (m3 * sH * tuH2); } else if (stateSave == 2) { sig = (80. * M_PI / 27.) * ( (7. * tuH + 8. * sH) * (tH2 + uH2) + 4. * sH * (2. * pow2(s3) - stH2 -usH2) ) / (s3 * m3 * sH * tuH2 * tuH); } // Answer. sigma = (M_PI/sH2) * pow3(alpS) * oniumME * sig; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2QQbarX8g::setIdColAcol() { // Flavours are trivial. setId( id1, id2, idHad, 21); // Split total contribution into different colour flows just like in // q qbar -> g g (with kinematics recalculated for massless partons). double sHr = - (tH + uH); double sH2r = sHr * sHr; double sigTS = (4. / 9.) * uH / tH - uH2 / sH2r; double sigUS = (4. / 9.) * tH / uH - tH2 / sH2r; double sigSum = sigTS + sigUS; // Two colour flow topologies. Swap if first is antiquark. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 0, 0, 2, 1, 3, 3, 2); else setColAcol( 1, 0, 0, 2, 3, 2, 1, 3); if (id1 < 0) swapColAcol(); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/TauDecays.cc0000644000175000017500000006225512217346252015327 0ustar sunsun// TauDecays.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Philip Ilten, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the TauDecays class. #include "Pythia8/TauDecays.h" namespace Pythia8 { //========================================================================== // The TauDecays class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of times to try a decay channel. const int TauDecays::NTRYCHANNEL = 10; // Number of times to try a decay sampling. const int TauDecays::NTRYDECAY = 10000; //const int TauDecays::NTRYDECAY = 100000; // These numbers are hardwired empirical parameters, // intended to speed up the M-generator. const double TauDecays::WTCORRECTION[11] = { 1., 1., 1., 2., 5., 15., 60., 250., 1250., 7000., 50000. }; //-------------------------------------------------------------------------- // Initialize the TauDecays class with the necessary pointers to info, // particle data, random numbers, and Standard Model couplings. // Additionally, the necessary matrix elements are initialized with the // Standard Model couplings, and particle data pointers. void TauDecays::init(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, Couplings* couplingsPtrIn) { // Set the pointers. infoPtr = infoPtrIn; settingsPtr = settingsPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; couplingsPtr = couplingsPtrIn; // Initialize the hard matrix elements. hmeTwoFermions2W2TwoFermions .initPointers(particleDataPtr, couplingsPtr); hmeTwoFermions2Z2TwoFermions .initPointers(particleDataPtr, couplingsPtr); hmeTwoFermions2Gamma2TwoFermions .initPointers(particleDataPtr, couplingsPtr); hmeTwoFermions2GammaZ2TwoFermions.initPointers(particleDataPtr, couplingsPtr); hmeZ2TwoFermions .initPointers(particleDataPtr, couplingsPtr); hmeHiggsEven2TwoFermions .initPointers(particleDataPtr, couplingsPtr); hmeHiggsOdd2TwoFermions .initPointers(particleDataPtr, couplingsPtr); hmeHiggsCharged2TwoFermions .initPointers(particleDataPtr, couplingsPtr); hmeUnpolarized .initPointers(particleDataPtr, couplingsPtr); // Initialize the tau decay matrix elements. hmeTau2Meson .initPointers(particleDataPtr, couplingsPtr); hmeTau2TwoLeptons .initPointers(particleDataPtr, couplingsPtr); hmeTau2TwoMesonsViaVector .initPointers(particleDataPtr, couplingsPtr); hmeTau2TwoMesonsViaVectorScalar.initPointers(particleDataPtr, couplingsPtr); hmeTau2ThreePions .initPointers(particleDataPtr, couplingsPtr); hmeTau2ThreeMesonsWithKaons .initPointers(particleDataPtr, couplingsPtr); hmeTau2ThreeMesonsGeneric .initPointers(particleDataPtr, couplingsPtr); hmeTau2TwoPionsGamma .initPointers(particleDataPtr, couplingsPtr); hmeTau2FourPions .initPointers(particleDataPtr, couplingsPtr); hmeTau2FivePions .initPointers(particleDataPtr, couplingsPtr); hmeTau2PhaseSpace .initPointers(particleDataPtr, couplingsPtr); // User selected tau decay mode. tauModeSave = settingsPtr->mode("ParticleDecays:sophisticatedTau"); // User selected tau decay mother. tauMotherSave = settingsPtr->mode("ParticleDecays:tauMother"); // User selected tau polarization. polSave = settingsPtr->parm("ParticleDecays:tauPolarization"); // Parameters to determine if correlated partner should decay. limitTau0 = settingsPtr->flag("ParticleDecays:limitTau0"); tau0Max = settingsPtr->parm("ParticleDecays:tau0Max"); limitTau = settingsPtr->flag("ParticleDecays:limitTau"); tauMax = settingsPtr->parm("ParticleDecays:tauMax"); limitRadius = settingsPtr->flag("ParticleDecays:limitRadius"); rMax = settingsPtr->parm("ParticleDecays:rMax"); limitCylinder = settingsPtr->flag("ParticleDecays:limitCylinder"); xyMax = settingsPtr->parm("ParticleDecays:xyMax"); zMax = settingsPtr->parm("ParticleDecays:zMax"); limitDecay = limitTau0 || limitTau || limitRadius || limitCylinder; } //-------------------------------------------------------------------------- // Main method of the TauDecays class. Pass the index of the tau requested // to be decayed along with the event record in which the tau exists. The // tau is then decayed with proper spin correlations as well any partner. // The children of the decays are written to the event record, and if the // decays were succesful, a return value of true is supplied. bool TauDecays::decay(int idxOut1, Event& event) { // User selected tau decay mode, mother, and polarization. tauMode = tauModeSave; tauMother = tauMotherSave; polarization = polSave; // Set the first outgoing particle of the hard process. out1 = HelicityParticle(event[idxOut1]); out1.idx = idxOut1; // Begin PS April 2012. // Check if this tau already has helicity information (eg from LHEF). bool hasHelicity = false; double helicityNow = 0.; if (tauMode >= 1 && abs(out1.pol()) <= 1.001) { hasHelicity = true; helicityNow = out1.pol(); } // End PS April 2012. // Find the mediator of the hard process. Create temporary copy. int idxMediator = out1.mother1(); int idxFirstOut1 = idxOut1; while(idxMediator > 0 && event[idxMediator].id() == out1.id()) { idxFirstOut1 = idxMediator; idxMediator = event[idxMediator].mother1(); } Particle medTmp = event[idxMediator]; // Find and set up the incoming particles of the hard process. int idxIn1 = medTmp.mother1(); int idxIn2 = medTmp.mother2(); while(idxIn1 > 0 && event[idxIn1].id() == medTmp.id()) { idxIn1 = event[idxIn1].mother1(); idxIn2 = event[idxIn2].mother2(); } in1 = HelicityParticle(event[idxIn1]); in1.idx = idxIn1; in1.direction = -1; in2 = HelicityParticle(event[idxIn2]); in2.idx = idxIn2; in2.direction = -1; // Find and set up the second outgoing particle of the hard process. int idxOut2 = (medTmp.daughter1() == idxFirstOut1) ? medTmp.daughter2() : medTmp.daughter1(); while (idxOut2 > 0 && event[idxOut2].daughter1() != 0 && event[event[idxOut2].daughter1()].id() == event[idxOut2].id()) { idxOut2 = event[idxOut2].daughter1(); } out2 = HelicityParticle(event[idxOut2]); out2.idx = idxOut2; // Set up the mediator. Special case for dipole shower, // where a massless photon can branch to a tau pair. if (medTmp.id() == 22 && out2.idAbs() == 15 && medTmp.m() < out1.m() + out2.m()) { Vec4 pTmp = out1.p() + out2.p(); medTmp.p( pTmp); medTmp.m( pTmp.mCalc() ); } mediator = HelicityParticle(medTmp); mediator.idx = idxMediator; mediator.direction = -1; // Set the particles vector. particles.clear(); particles.push_back(in1); particles.push_back(in2); particles.push_back(out1); particles.push_back(out2); // Set the hard matrix element. // Polarized tau (decayed one by one). if (hasHelicity) { correlated = false; // Produced from a W. } else if (abs(mediator.id()) == 24) { // Produced from quarks: s-channel. if (abs(in1.id()) <= 18 && abs(in2.id()) <= 18) hardME = hmeTwoFermions2W2TwoFermions.initChannel(particles); // Produced from quarks: t-channel. else if (abs(in1.id()) <= 18 || abs(in2.id()) <= 18) { bool fermion = (abs(in1.id()) <= 18) ? 0 : 1; particles[!fermion] = (event[particles[fermion].daughter1()].id() == mediator.id()) ? HelicityParticle(event[particles[fermion].daughter2()]) : HelicityParticle(event[particles[fermion].daughter1()]); particles[!fermion].direction = 1; if (abs(particles[!fermion].id()) <= 18) hardME = hmeTwoFermions2W2TwoFermions.initChannel(particles); else { infoPtr->errorMsg("Warning in TauDecays::decay: unknown " "tau production, assuming unpolarized and uncorrelated"); hardME = hmeUnpolarized.initChannel(particles); } // Unknown W production: assume negative helicity. } else if (tauMode == 1) { tauMode = 3; polarization = -1; } correlated = false; // Produced from a photon. } else if (abs(mediator.id()) == 22 && abs(in1.id()) <= 18) { particles.push_back(mediator); hardME = hmeTwoFermions2Gamma2TwoFermions.initChannel(particles); correlated = true; // Produced from a photon/Z. } else if (abs(mediator.id()) == 23 && abs(in1.id()) <= 18) { particles.push_back(mediator); if (settingsPtr->mode("WeakZ0:gmZmode") == 0) hardME = hmeTwoFermions2GammaZ2TwoFermions.initChannel(particles); else if (settingsPtr->mode("WeakZ0:gmZmode") == 1) hardME = hmeTwoFermions2Gamma2TwoFermions.initChannel(particles); else if (settingsPtr->mode("WeakZ0:gmZmode") == 2) hardME = hmeTwoFermions2Z2TwoFermions.initChannel(particles); correlated = true; // Unkown Z production: assume unpolarized Z. } else if (abs(mediator.id()) == 23) { particles[1] = mediator; hardME = hmeZ2TwoFermions.initChannel(particles); correlated = true; // Produced from a CP even Higgs. } else if (abs(mediator.id()) == 25 || abs(mediator.id()) == 35) { hardME = hmeHiggsEven2TwoFermions.initChannel(particles); correlated = true; // Produced from a CP odd Higgs. } else if (abs(mediator.id()) == 36) { hardME = hmeHiggsOdd2TwoFermions.initChannel(particles); correlated = true; // Produced from a charged Higgs. } else if (abs(mediator.id()) == 37) { hardME = hmeHiggsCharged2TwoFermions.initChannel(particles); correlated = false; // Produced from a D or B hadron decay with a single tau. } else if ((abs(mediator.id()) == 411 || abs(mediator.id()) == 431 || abs(mediator.id()) == 511 || abs(mediator.id()) == 521 || abs(mediator.id()) == 531 || abs(mediator.id()) == 541 || (abs(mediator.id()) > 5100 && abs(mediator.id()) < 5600) ) && abs(out2.id()) == 16) { int idBmother = (mediator.id() > 0) ? -5 : 5; if (abs(mediator.id()) > 5100) idBmother = -idBmother; particles[0] = HelicityParticle( idBmother, 0, 0, 0, 0, 0, 0, 0, 0., 0., 0., 0., 0., 0., particleDataPtr); particles[1] = HelicityParticle( -idBmother, 0, 0, 0, 0, 0, 0, 0, 0., 0., 0., 0., 0., 0., particleDataPtr); particles[0].idx = 0; particles[1].idx = 1; // D or B meson decays into neutrino + tau + meson. if (mediator.daughter1() + 2 == mediator.daughter2()) { particles[0].p(mediator.p()); particles[1].direction = 1; particles[1].id(-particles[1].id()); particles[1].p(particles[0].p() - particles[2].p() - particles[3].p()); } // D or B meson decays into neutrino + tau. else { particles[0].p(mediator.p()/2); particles[1].p(mediator.p()/2); } hardME = hmeTwoFermions2W2TwoFermions.initChannel(particles); correlated = false; // Produced from a virtual photon with correlated taus. } else if (abs(out1.id()) == 15 && abs(out2.id()) == 15) { particles.push_back(mediator); particles[0] = HelicityParticle(-1, 0, 0, 0, 0, 0, 0, 0, mediator.p()/2, 0., 0., particleDataPtr); particles[1] = HelicityParticle(1, 0, 0, 0, 0, 0, 0, 0, mediator.p()/2, 0., 0., particleDataPtr); particles[0].direction = -1; particles[1].direction = -1; particles[0].idx = 0; particles[1].idx = 0; hardME = hmeTwoFermions2Gamma2TwoFermions.initChannel(particles); correlated = true; // Produced from an unknown process, assume unpolarized and uncorrelated. } else { if (tauMode <= 1) infoPtr->errorMsg("Warning in TauDecays::decay: unknown " "tau production, assuming unpolarized and uncorrelated"); hardME = hmeUnpolarized.initChannel(particles); correlated = false; } // Check if correlated partner should decay. if (correlated) { // Check vertex is within limits. if (limitTau0 && out2.tau0() > tau0Max) correlated = false; else if (limitTau && out2.tau() > tauMax) correlated = false; else if (limitRadius && pow2(out2.xDec()) + pow2(out2.yDec()) + pow2(out2.zDec()) > pow2(rMax)) correlated = false; else if (limitCylinder && (pow2(out2.xDec()) + pow2(out2.yDec()) > pow2(xyMax) || abs(out2.zDec()) > zMax)) correlated = false; // Check partner can decay. else if (!out2.canDecay()) correlated = false; else if (!out2.mayDecay()) correlated = false; // Check partner is compatible with hard matrix element (only leptons). else if (out2.idAbs() < 11 || out2.idAbs() > 16) { infoPtr->errorMsg("Warning in TauDecays::decay: incompatible " "correlated partner in tau decay"); correlated = false; } // Undecay correlated partner if already decayed. else if (!out2.isFinal()) event.undoDecay(out2.idx); } // Pick the first tau to decay. HelicityParticle* tau; int idx; if (correlated) idx = (rndmPtr->flat() < 0.5) ? 2 : 3; else idx = (abs(particles[2].id()) == 15) ? 2 : 3; tau = &particles[idx]; // Calculate the density matrix and decay the tau. if ( (tauMode == 2 && abs(mediator.id()) == tauMother) || tauMode == 3 ) { tau->rho[0][0] = (tau->id() > 0) ? (1 - polarization) / 2 : (1 + polarization) / 2; tau->rho[1][1] = (tau->id() > 0) ? (1 + polarization) / 2 : (1 - polarization) / 2; correlated = false; } // Begin PS April 2012. // Else use tau helicity provided by event record (LHEF). else if (hasHelicity) { tau->rho[0][0] = (1. - helicityNow) / 2.; tau->rho[1][1] = (1. + helicityNow) / 2.; } // End PS April 2012. // Else compute density matrix according to matrix element. else hardME->calculateRho(idx, particles); vector children = createChildren(*tau); if (children.size() == 0) return false; // Decay the first tau. bool accepted = false; int tries = 0; while (!accepted) { isotropicDecay(children); double decayWeight = decayME->decayWeight(children); double decayWeightMax = decayME->decayWeightMax(children); accepted = (rndmPtr->flat() < decayWeight / decayWeightMax); if (decayWeight > decayWeightMax) infoPtr->errorMsg("Warning in TauDecays::decay: maximum " "decay weight exceeded in tau decay"); if (tries > NTRYDECAY) { infoPtr->errorMsg("Warning in TauDecays::decay: maximum " "number of decay attempts exceeded"); break; } ++tries; } writeDecay(event,children); // If a correlated second tau exists, decay that tau as well. if (correlated) { idx = (idx == 2) ? 3 : 2; // Calculate the first tau decay matrix. decayME->calculateD(children); // Update the decay matrix for the tau. (*tau).D = children[0].D; // Switch the taus. tau = &particles[idx]; // Calculate second tau's density matrix. hardME->calculateRho(idx, particles); // Decay the second tau. children.clear(); children = createChildren(*tau); if (children.size() == 0) return false; accepted = false; tries = 0; while (!accepted) { isotropicDecay(children); double decayWeight = decayME->decayWeight(children); double decayWeightMax = decayME->decayWeightMax(children); accepted = (rndmPtr->flat() < decayWeight / decayWeightMax); if (decayWeight > decayWeightMax) infoPtr->errorMsg("Warning in TauDecays::decay: maximum " "decay weight exceeded in correlated tau decay"); if (tries > NTRYDECAY) { infoPtr->errorMsg("Warning in TauDecays::decay: maximum " "number of decay attempts exceeded"); break; } ++tries; } writeDecay(event,children); } // Done. return true; } //-------------------------------------------------------------------------- // Given a HelicityParticle parent, select the decay channel and return // a vector of HelicityParticles containing the children, with the parent // particle duplicated in the first entry of the vector. vector TauDecays::createChildren(HelicityParticle parent) { // Initial values. int meMode = 0; vector children; // Set the parent as incoming. parent.direction = -1; // Setup decay data for the decaying particle. ParticleDataEntry decayData = parent.particleDataEntry(); // Initialize the decay data. if (!decayData.preparePick(parent.id())) return children; // Try to pick a decay channel. bool decayed = false; int decayTries = 0; while (!decayed && decayTries < NTRYCHANNEL) { // Pick a decay channel. DecayChannel decayChannel = decayData.pickChannel(); meMode = decayChannel.meMode(); int decayMult = decayChannel.multiplicity(); // Select children masses. bool allowed = false; int channelTries = 0; while (!allowed && channelTries < NTRYCHANNEL) { children.resize(0); children.push_back(parent); for (int i = 0; i < decayMult; ++i) { // Grab child ID. int childId = decayChannel.product(i); // Flip sign for anti-particle decay. if (parent.id() < 0 && particleDataPtr->hasAnti(childId)) childId = -childId; // Grab child mass. double childMass = particleDataPtr->mSel(childId); // Push back the child into the children vector. children.push_back( HelicityParticle(childId, 91, parent.idx, 0, 0, 0, 0, 0, 0., 0., 0., 0.,childMass, 0., particleDataPtr) ); } // Check there is enough phase space for decay. if (decayMult > 1) { double massDiff = parent.m(); for (int i = 0; i < decayMult; ++i) massDiff -= children[i].m(); // For now we just check kinematically available. if (massDiff > 0) { allowed = true; decayed = true; } } // End pick a channel. ++channelTries; } ++decayTries; } // Swap the children ordering for muons. if (parent.idAbs() == 13 && children.size() == 4 && meMode == 22) swap(children[1], children[3]); // Set the decay matrix element. // Two body decays. if (children.size() == 3) { if (meMode == 1521) decayME = hmeTau2Meson.initChannel(children); else decayME = hmeTau2PhaseSpace.initChannel(children); } // Three body decays. else if (children.size() == 4) { // Leptonic decay. if (meMode == 1531 || (parent.idAbs() == 13 && meMode == 22)) decayME = hmeTau2TwoLeptons.initChannel(children); // Two meson decay via vector meson. else if (meMode == 1532) decayME = hmeTau2TwoMesonsViaVector.initChannel(children); // Two meson decay via vector or scalar meson. else if (meMode == 1533) decayME = hmeTau2TwoMesonsViaVectorScalar.initChannel(children); // Flat phase space. else decayME = hmeTau2PhaseSpace.initChannel(children); } // Four body decays. else if (children.size() == 5) { // Three pion CLEO decay. if (meMode == 1541) decayME = hmeTau2ThreePions.initChannel(children); // Three meson decay with one or more kaons decay. else if (meMode == 1542) decayME = hmeTau2ThreeMesonsWithKaons.initChannel(children); // Generic three meson decay. else if (meMode == 1543) decayME = hmeTau2ThreeMesonsGeneric.initChannel(children); // Two pions and photon decay. else if (meMode == 1544) decayME = hmeTau2TwoPionsGamma.initChannel(children); // Flat phase space. else decayME = hmeTau2PhaseSpace.initChannel(children); } // Five body decays. else if (children.size() == 6) { // Four pion Novosibirsk current. if (meMode == 1551) decayME = hmeTau2FourPions.initChannel(children); // Flat phase space. else decayME = hmeTau2PhaseSpace.initChannel(children); } // Six body decays. else if (children.size() == 7) { // Four pion Novosibirsk current. if (meMode == 1561) decayME = hmeTau2FivePions.initChannel(children); // Flat phase space. else decayME = hmeTau2PhaseSpace.initChannel(children); } // Flat phase space. else decayME = hmeTau2PhaseSpace.initChannel(children); // Done. return children; } //-------------------------------------------------------------------------- // N-body decay using the M-generator algorithm described in // "Monte Carlo Phase Space" by F. James in CERN 68-15, May 1968. Taken // from ParticleDecays::mGenerator but modified to handle spin particles. // Given a vector of HelicityParticles where the first particle is // the mother, the remaining particles are decayed isotropically. void TauDecays::isotropicDecay(vector& children) { // Mother and sum daughter masses. int decayMult = children.size() - 1; double m0 = children[0].m(); double mSum = children[1].m(); for (int i = 2; i <= decayMult; ++i) mSum += children[i].m(); double mDiff = m0 - mSum; // Begin setup of intermediate invariant masses. vector mInv; for (int i = 0; i <= decayMult; ++i) mInv.push_back( children[i].m()); // Calculate the maximum weight in the decay. double wtPS; double wtPSmax = 1. / WTCORRECTION[decayMult]; double mMax = mDiff + children[decayMult].m(); double mMin = 0.; for (int i = decayMult - 1; i > 0; --i) { mMax += children[i].m(); mMin += children[i+1].m(); double mNow = children[i].m(); wtPSmax *= 0.5 * sqrtpos( (mMax - mMin - mNow) * (mMax + mMin + mNow) * (mMax + mMin - mNow) * (mMax - mMin + mNow) ) / mMax; } // Begin loop to find the set of intermediate invariant masses. vector rndmOrd; do { wtPS = 1.; // Find and order random numbers in descending order. rndmOrd.clear(); rndmOrd.push_back(1.); for (int i = 1; i < decayMult - 1; ++i) { double random = rndmPtr->flat(); rndmOrd.push_back(random); for (int j = i - 1; j > 0; --j) { if (random > rndmOrd[j]) swap( rndmOrd[j], rndmOrd[j+1] ); else break; } } rndmOrd.push_back(0.); // Translate into intermediate masses and find weight. for (int i = decayMult - 1; i > 0; --i) { mInv[i] = mInv[i+1] + children[i].m() + (rndmOrd[i-1] - rndmOrd[i]) * mDiff; wtPS *= 0.5 * sqrtpos( (mInv[i] - mInv[i+1] - children[i].m()) * (mInv[i] + mInv[i+1] + children[i].m()) * (mInv[i] + mInv[i+1] - children[i].m()) * (mInv[i] - mInv[i+1] + children[i].m()) ) / mInv[i]; } // If rejected, try again with new invariant masses. } while ( wtPS < rndmPtr->flat() * wtPSmax ); // Perform two-particle decays in the respective rest frame. vector pInv(decayMult + 1); for (int i = 1; i < decayMult; ++i) { double pAbs = 0.5 * sqrtpos( (mInv[i] - mInv[i+1] - children[i].m()) * (mInv[i] + mInv[i+1] + children[i].m()) * (mInv[i] + mInv[i+1] - children[i].m()) * (mInv[i] - mInv[i+1] + children[i].m()) ) / mInv[i]; // Isotropic angles give three-momentum. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(1. - cosTheta*cosTheta); double phi = 2. * M_PI * rndmPtr->flat(); double pX = pAbs * sinTheta * cos(phi); double pY = pAbs * sinTheta * sin(phi); double pZ = pAbs * cosTheta; // Calculate energies, fill four-momenta. double eHad = sqrt( children[i].m()*children[i].m() + pAbs*pAbs); double eInv = sqrt( mInv[i+1]*mInv[i+1] + pAbs*pAbs); children[i].p( pX, pY, pZ, eHad); pInv[i+1].p( -pX, -pY, -pZ, eInv); } // Boost decay products to the mother rest frame. children[decayMult].p( pInv[decayMult] ); for (int iFrame = decayMult - 1; iFrame > 1; --iFrame) for (int i = iFrame; i <= decayMult; ++i) children[i].bst( pInv[iFrame], mInv[iFrame]); // Boost decay products to the current frame. pInv[1].p( children[0].p() ); for (int i = 1; i <= decayMult; ++i) children[i].bst( pInv[1], mInv[1] ); // Done. return; } //-------------------------------------------------------------------------- // Write the vector of HelicityParticles to the event record, excluding the // first particle. Set the lifetime and production vertex of the particles // and mark the first particle of the vector as decayed. void TauDecays::writeDecay(Event& event, vector& children) { // Set additional information and append children to event. int decayMult = children.size() - 1; Vec4 decayVertex = children[0].vDec(); for (int i = 1; i <= decayMult; i++) { // Set child lifetime. children[i].tau(children[i].tau0() * rndmPtr->exp()); // Set child production vertex. children[i].vProd(decayVertex); // Append child to record. children[i].idx = event.append(children[i]); } // Mark the parent as decayed and set children. event[children[0].idx].statusNeg(); event[children[0].idx].daughters(children[1].idx, children[decayMult].idx); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/LesHouches.cc0000644000175000017500000006402612217346246015510 0ustar sunsun// LesHouches.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the LHAup and // LHAupLHEF classes. #include "Pythia8/LesHouches.h" // Access time information. #include // GZIP support. #ifdef GZIPSUPPORT // For GCC versions >= 4.6, can switch off shadow warnings. #if (defined GZIPSUPPORT && ((__GNUC__ * 100) + __GNUC_MINOR__) >= 406) #pragma GCC diagnostic ignored "-Wshadow" #endif // Boost includes. #include "boost/iostreams/filtering_stream.hpp" #include "boost/iostreams/filter/gzip.hpp" // Switch shadow warnings back on. #if (defined GZIPSUPPORT && ((__GNUC__ * 100) + __GNUC_MINOR__) >= 406) #pragma GCC diagnostic warning "-Wshadow" #endif #endif // GZIPSUPPORT namespace Pythia8 { //========================================================================== // LHAup class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // LHA convention with cross section in pb may require conversion from mb. const double LHAup::CONVERTMB2PB = 1e9; //-------------------------------------------------------------------------- // Print the initialization info; to check it worked. void LHAup::listInit(ostream& os) { // Header. os << "\n -------- LHA initialization information ------------ \n"; // Beam info. os << fixed << setprecision(3) << "\n beam kind energy pdfgrp pdfset \n" << " A " << setw(6) << idBeamASave << setw(12) << eBeamASave << setw(8) << pdfGroupBeamASave << setw(8) << pdfSetBeamASave << "\n" << " B " << setw(6) << idBeamBSave << setw(12) << eBeamBSave << setw(8) << pdfGroupBeamBSave << setw(8) << pdfSetBeamBSave << "\n"; // Event weighting strategy. os << "\n Event weighting strategy = " << setw(2) << strategySave << "\n" ; // Process list. os << scientific << setprecision(4) << "\n Processes, with strategy-dependent cross section info \n" << " number xsec (pb) xerr (pb) xmax (pb) \n" ; for (int ip = 0; ip < int(processes.size()); ++ip) { os << setw(8) << processes[ip].idProc << setw(15) << processes[ip].xSecProc << setw(15) << processes[ip].xErrProc << setw(15) << processes[ip].xMaxProc << "\n"; } // Finished. os << "\n -------- End LHA initialization information -------- \n"; } //-------------------------------------------------------------------------- // Print the event info; to check it worked. void LHAup::listEvent(ostream& os) { // Header. os << "\n -------- LHA event information and listing -------------" << "--------------------------------------------------------- \n"; // Basic event info. os << scientific << setprecision(4) << "\n process = " << setw(8) << idProc << " weight = " << setw(12) << weightProc << " scale = " << setw(12) << scaleProc << " (GeV) \n" << " " << " alpha_em = " << setw(12) << alphaQEDProc << " alpha_strong = " << setw(12) << alphaQCDProc << "\n"; // Particle list os << fixed << setprecision(3) << "\n Participating Particles \n" << " no id stat mothers colours p_x " << "p_y p_z e m tau spin \n" ; for (int ip = 1; ip < int(particles.size()); ++ip) { os << setw(6) << ip << setw(10) << particles[ip].idPart << setw(5) << particles[ip].statusPart << setw(6) << particles[ip].mother1Part << setw(6) << particles[ip].mother2Part << setw(6) << particles[ip].col1Part << setw(6) << particles[ip].col2Part << setw(11) << particles[ip].pxPart << setw(11) << particles[ip].pyPart << setw(11) << particles[ip].pzPart << setw(11) << particles[ip].ePart << setw(11) << particles[ip].mPart << setw(8) << particles[ip].tauPart << setw(8) << particles[ip].spinPart << "\n"; } // PDF info - optional. if (pdfIsSetSave) os << "\n pdf: id1 =" << setw(5) << id1pdfSave << " id2 =" << setw(5) << id2pdfSave << " x1 =" << scientific << setw(10) << x1pdfSave << " x2 =" << setw(10) << x2pdfSave << " scalePDF =" << setw(10) << scalePDFSave << " pdf1 =" << setw(10) << pdf1Save << " pdf2 =" << setw(10) << pdf2Save << "\n"; // Finished. os << "\n -------- End LHA event information and listing ---------" << "--------------------------------------------------------- \n"; } //-------------------------------------------------------------------------- // Open and write header to a Les Houches Event File. bool LHAup::openLHEF(string fileNameIn) { // Open file for writing. Reset it to be empty. fileName = fileNameIn; const char* cstring = fileName.c_str(); osLHEF.open(cstring, ios::out | ios::trunc); if (!osLHEF) { infoPtr->errorMsg("Error in LHAup::openLHEF:" " could not open file", fileName); return false; } // Read out current date and time. time_t t = time(0); strftime(dateNow,12,"%d %b %Y",localtime(&t)); strftime(timeNow,9,"%H:%M:%S",localtime(&t)); // Write header. osLHEF << "\n" << "" << endl; // Done. return true; } //-------------------------------------------------------------------------- // Write initialization information to a Les Houches Event File. bool LHAup::initLHEF() { // Write information on beams. osLHEF << "\n" << scientific << setprecision(6) << " " << idBeamASave << " " << idBeamBSave << " " << eBeamASave << " " << eBeamBSave << " " << pdfGroupBeamASave << " " << pdfGroupBeamBSave << " " << pdfSetBeamASave << " " << pdfSetBeamBSave << " " << strategySave << " " << processes.size() << "\n"; // Write information on all the subprocesses. for (int ip = 0; ip < int(processes.size()); ++ip) osLHEF << " " << setw(13) << processes[ip].xSecProc << " " << setw(13) << processes[ip].xErrProc << " " << setw(13) << processes[ip].xMaxProc << " " << setw(6) << processes[ip].idProc << "\n"; // Done. osLHEF << "" << endl; return true; } //-------------------------------------------------------------------------- // Write event information to a Les Houches Event File. // Normal mode is to line up event info in columns, but the non-verbose // altnernative saves space at the expense of human readability. bool LHAup::eventLHEF(bool verbose) { // Default verbose option. if (verbose) { // Write information on process as such. osLHEF << "\n" << scientific << setprecision(6) << " " << setw(5) << particles.size() - 1 << " " << setw(5) << idProc << " " << setw(13) << weightProc << " " << setw(13) << scaleProc << " " << setw(13) << alphaQEDProc << " " << setw(13) << alphaQCDProc << "\n"; // Write information on the particles, excluding zeroth. for (int ip = 1; ip < int(particles.size()); ++ip) { LHAParticle& ptNow = particles[ip]; osLHEF << " " << setw(8) << ptNow.idPart << " " << setw(5) << ptNow.statusPart << " " << setw(5) << ptNow.mother1Part << " " << setw(5) << ptNow.mother2Part << " " << setw(5) << ptNow.col1Part << " " << setw(5) << ptNow.col2Part << setprecision(10) << " " << setw(17) << ptNow.pxPart << " " << setw(17) << ptNow.pyPart << " " << setw(17) << ptNow.pzPart << " " << setw(17) << ptNow.ePart << " " << setw(17) << ptNow.mPart << setprecision(6); if (ptNow.tauPart == 0.) osLHEF << " 0."; else osLHEF << " " << setw(13) << ptNow.tauPart; if (ptNow.spinPart == 9.) osLHEF << " 9."; else osLHEF << " " << setw(13) << ptNow.spinPart; osLHEF << "\n"; } // Optionally write information on PDF values at hard interaction. if (pdfIsSetSave) osLHEF << "#pdf" << " " << setw(4) << id1pdfSave << " " << setw(4) << id2pdfSave << " " << setw(13) << x1pdfSave << " " << setw(13) << x2pdfSave << " " << setw(13) << scalePDFSave << " " << setw(13) << pdf1Save << " " << setw(13) << pdf2Save << "\n"; // Alternative non-verbose option. } else { // Write information on process as such. osLHEF << "\n" << scientific << setprecision(6) << particles.size() - 1 << " " << idProc << " " << weightProc << " " << scaleProc << " " << alphaQEDProc << " " << alphaQCDProc << "\n"; // Write information on the particles, excluding zeroth. for (int ip = 1; ip < int(particles.size()); ++ip) { LHAParticle& ptNow = particles[ip]; osLHEF << ptNow.idPart << " " << ptNow.statusPart << " " << ptNow.mother1Part << " " << ptNow.mother2Part << " " << ptNow.col1Part << " " << ptNow.col2Part << setprecision(10) << " " << ptNow.pxPart << " " << ptNow.pyPart << " " << ptNow.pzPart << " " << ptNow.ePart << " " << ptNow.mPart << setprecision(6); if (ptNow.tauPart == 0.) osLHEF << " 0."; else osLHEF << " " << setw(13) << ptNow.tauPart; if (ptNow.spinPart == 9.) osLHEF << " 9."; else osLHEF << " " << setw(13) << ptNow.spinPart; osLHEF << "\n"; } // Optionally write information on PDF values at hard interaction. if (pdfIsSetSave) osLHEF << "#pdf" << " " << id1pdfSave << " " << id2pdfSave << " " << x1pdfSave << " " << x2pdfSave << " " << scalePDFSave << " " << pdf1Save << " " << pdf2Save << "\n"; } // Done. osLHEF << "" << endl; return true; } //-------------------------------------------------------------------------- // Write end of a Les Houches Event File and close it. bool LHAup::closeLHEF(bool updateInit) { // Write an end to the file. osLHEF << "" << endl; osLHEF.close(); // Optionally update the cross section information. if (updateInit) { const char* cstring = fileName.c_str(); osLHEF.open(cstring, ios::in | ios::out); // Rewrite header; identically with what openLHEF did. osLHEF << "\n" << "" << endl; // Redo initialization information. initLHEF(); osLHEF.close(); } // Done. return true; } //-------------------------------------------------------------------------- // Read in initialization information from a Les Houches Event File. bool LHAup::setInitLHEF(istream& is, bool readHeaders) { // Check that first line is consistent with proper LHEF file. string line; if (!getline(is, line)) return false; if (line.find("" : ") tag // is found first on a line. string tag = " "; do { if (!getline(is, line)) return false; if (line.find_first_not_of(" \n\t\v\b\r\f\a") != string::npos) { istringstream getfirst(line); getfirst >> tag; if (!getfirst) return false; } } while (tag != "" && tag != " headerMap; // Loop over lines until an tag is found. bool read = true, newKey = false; string key = "base"; vector < string > keyVec; while (true) { if (!getline(is, line)) return false; // Check if this line is a tag; '<' as first character, // '>' as last character, exclusing whitespace size_t pos1 = line.find_first_not_of(" \n\t\v\b\r\f\a"); size_t pos2 = line.find_last_not_of(" \n\t\v\b\r\f\a"); if (pos1 != string::npos && line[pos1] == '<' && pos2 != string::npos && line[pos2] == '>' && pos1 < pos2) { // Only take the first word of the tag tag = line.substr(pos1 + 1, pos2 - pos1 - 1); istringstream getfirst(tag); getfirst >> tag; // Tag present, so handle here if (getfirst) { // Exit condition if (tag == "init") break; // End of header block; keep reading until tag, // but do not store any further information else if (tag == "/header") { read = false; continue; // Opening tag } else if (tag[0] != '/') { keyVec.push_back(tag); newKey = true; continue; // Closing tag that matches current key } else if (tag == "/" + keyVec.back()) { keyVec.pop_back(); newKey = true; continue; } } // if (getfirst) } // At this point we have a line that is not a tag; if no longer // reading headers then keep going if (!read) continue; // Check for key change if (newKey) { if (keyVec.empty()) key = "base"; else key = keyVec[0]; for (size_t i = 1; i < keyVec.size(); i++) key += "." + keyVec[i]; newKey = false; } // Append information to local storage headerMap[key] += line + "\n"; } // while (true) // Copy information to info using LHAup::setInfoHeader for (map < string, string >::iterator it = headerMap.begin(); it != headerMap.end(); it++) setInfoHeader(it->first, it->second); } // if (readHeaders == true && tag == headerTag) // Read in beam and strategy info, and store it. int idbmupA, idbmupB; double ebmupA, ebmupB; int pdfgupA, pdfgupB, pdfsupA, pdfsupB, idwtup, nprup; if (!getline(is, line)) return false; istringstream getbms(line); getbms >> idbmupA >> idbmupB >> ebmupA >> ebmupB >> pdfgupA >> pdfgupB >> pdfsupA >> pdfsupB >> idwtup >> nprup; if (!getbms) return false; setBeamA(idbmupA, ebmupA, pdfgupA, pdfsupA); setBeamB(idbmupB, ebmupB, pdfgupB, pdfsupB); setStrategy(idwtup); // Read in process info, one process at a time, and store it. double xsecup, xerrup, xmaxup; xSecSumSave = 0.; xErrSumSave = 0.; int lprup; for (int ip = 0; ip < nprup; ++ip) { if (!getline(is, line)) return false; istringstream getpro(line); getpro >> xsecup >> xerrup >> xmaxup >> lprup ; if (!getpro) return false; addProcess(lprup, xsecup, xerrup, xmaxup); xSecSumSave += xsecup; xErrSumSave += pow2(xerrup); } xErrSumSave = sqrt(xErrSumSave); // Reading worked. return true; } //-------------------------------------------------------------------------- // Read in event information from a Les Houches Event File, // into a staging area where it can be reused by setOldEventLHEF. bool LHAup::setNewEventLHEF(istream& is, double mRecalculate ) { // Loop over lines until an > tag; if (!getfirst) return false; } } while (tag != "" && tag != "> nupSave >> idprupSave >> xwgtupSave >> scalupSave >> aqedupSave >> aqcdupSave; if (!getpro) return false; // Reset particlesSave vector, add slot-0 empty particle. particlesSave.clear(); particlesSave.push_back( LHAParticle() ); // Read in particle info one by one, and store it. // Note unusual C++ loop range, to better reflect LHA/Fortran standard. // (Recall that process(...) above added empty particle at index 0.) int idup, istup, mothup1, mothup2, icolup1, icolup2; double pup1, pup2, pup3, pup4, pup5, vtimup, spinup; bool doRecalculate = (mRecalculate > 0.); for (int ip = 1; ip <= nupSave; ++ip) { if (!getline(is, line)) return false; istringstream getall(line); getall >> idup >> istup >> mothup1 >> mothup2 >> icolup1 >> icolup2 >> pup1 >> pup2 >> pup3 >> pup4 >> pup5 >> vtimup >> spinup; if (!getall) return false; // Optionally recalculate mass from four-momentum. if (doRecalculate && pup5 > mRecalculate) pup5 = sqrtpos( pup4*pup4 - pup1*pup1 - pup2*pup2 - pup3*pup3); particlesSave.push_back( LHAParticle( idup, istup, mothup1, mothup2, icolup1, icolup2, pup1, pup2, pup3, pup4, pup5, vtimup, spinup, -1.) ); } // Flavour and x values of hard-process initiators. id1InSave = particlesSave[1].idPart; id2InSave = particlesSave[2].idPart; x1InSave = (eBeamASave > 0.) ? particlesSave[1].ePart / eBeamASave : 0.; x2InSave = (eBeamBSave > 0.) ? particlesSave[2].ePart / eBeamBSave : 0.; // Continue parsing till . Look for optional info on the way. getPDFSave = false; getScale = false; do { if (!getline(is, line)) return false; istringstream getinfo(line); getinfo >> tag; if (!getinfo) return false; // Extract PDF info if present. if (tag == "#pdf" && !getPDFSave) { getinfo >> id1pdfInSave >> id2pdfInSave >> x1pdfInSave >> x2pdfInSave >> scalePDFInSave >> pdf1InSave >> pdf2InSave; if (!getinfo) return false; getPDFSave = true; // Extract scale info if present. } else if (tag == "#" && !getScale) { double scaleIn = 0; for (int i = 3; i < int(particlesSave.size()); ++i) if (particlesSave[i].statusPart == 1) { if ( !(getinfo >> scaleIn) ) return false; particlesSave[i].scalePart = scaleIn; } if (!getinfo) return false; getScale = true; } } while (tag != "" && tag != "setstate(std::ios_base::badbit); // Check filename ending to decide which filters to apply. else { const char *last = strrchr(fn, '.'); if (last && strncmp(last, ".gz", 3) == 0) fis->push(boost::iostreams::gzip_decompressor()); fis->push(ifs); } return (istream *) fis; #endif // GZIPSUPPORT } //-------------------------------------------------------------------------- // Companion method to 'openFile', above. // Correctly deallocates memory if required before closing the file. void LHAup::closeFile(istream *&is, ifstream &ifs) { // If the istream pointer is not NULL and is not the // same as the ifstream, then delete pointer. if (is && is != &ifs) delete is; is = NULL; // Close the file if (ifs.is_open()) ifs.close(); } //========================================================================== // LHAupLHEF class. //-------------------------------------------------------------------------- // Constructor. LHAupLHEF::LHAupLHEF(const char* fileIn, const char* headerIn, bool readHeadersIn) : is(NULL), isHead(NULL), readHeaders(readHeadersIn) { // Open LHEF and optionally header file as well. Note that both // are opened here so that initialisation can be aborted if // either of the files is missing, see fileFound(). is = openFile(fileIn, ifs); isHead = (headerIn == NULL) ? is : openFile(headerIn, ifsHead); } //-------------------------------------------------------------------------- // Destructor. LHAupLHEF::~LHAupLHEF() { // Close files closeAllFiles(); } //========================================================================== // LHAupFromPYTHIA8 class. //-------------------------------------------------------------------------- // Read in initialization information from PYTHIA 8. bool LHAupFromPYTHIA8::setInit() { // Read in beam from Info class. Parton density left empty. int idbmupA = infoPtr->idA(); int idbmupB = infoPtr->idB(); double ebmupA = infoPtr->eA(); double ebmupB = infoPtr->eB(); int pdfgupA = 0; int pdfgupB = 0; int pdfsupA = 0; int pdfsupB = 0; setBeamA(idbmupA, ebmupA, pdfgupA, pdfsupA); setBeamB(idbmupB, ebmupB, pdfgupB, pdfsupB); // Currently only one allowed strategy. int idwtup = 3; setStrategy(idwtup); // Only one process with dummy information. (Can overwrite at the end.) int lprup = 9999; double xsecup = 1.; double xerrup = 0.; double xmaxup = 1.; addProcess(lprup, xsecup, xerrup, xmaxup); // Done. return true; } //-------------------------------------------------------------------------- // Read in event information from PYTHIA 8. bool LHAupFromPYTHIA8::setEvent( int, double ) { // Read process information from Info class, and store it. // Note: renormalization scale here, factorization further down. // For now always convert to process 9999, instead of infoPtr->code(). int idprup = 9999; double xwgtup = infoPtr->weight(); double scalup = infoPtr->QRen(); double aqedup = infoPtr->alphaEM(); double aqcdup = infoPtr->alphaS(); setProcess(idprup, xwgtup, scalup, aqedup, aqcdup); // Read in particle info one by one, excluding zero and beams, and store it. // Note unusual C++ loop range, to better reflect LHA/Fortran standard. int nup = processPtr->size() - 3; int idup, statusup, istup, mothup1, mothup2, icolup1, icolup2; double pup1, pup2, pup3, pup4, pup5, vtimup, spinup; for (int ip = 1; ip <= nup; ++ip) { Particle& particle = (*processPtr)[ip + 2]; idup = particle.id(); // Convert from PYTHIA8 to LHA status codes. statusup = particle.status(); if (ip < 3) istup = -1; else if (statusup < 0) istup = 2; else istup = 1; mothup1 = max(0, particle.mother1() - 2); mothup2 = max(0, particle.mother2() - 2); icolup1 = particle.col(); icolup2 = particle.acol(); pup1 = particle.px(); pup2 = particle.py(); pup3 = particle.pz(); pup4 = particle.e(); pup5 = particle.m(); vtimup = particle.tau(); spinup = particle.pol(); addParticle(idup, istup, mothup1, mothup2, icolup1, icolup2, pup1, pup2, pup3, pup4, pup5, vtimup, spinup, -1.) ; } // Extract hard-process initiator information from Info class, and store it. int id1up = infoPtr->id1(); int id2up = infoPtr->id2(); double x1up = infoPtr->x1(); double x2up = infoPtr->x2(); setIdX( id1up, id2up, x1up, x2up); // Also extract pdf information from Info class, and store it. int id1pdfup = infoPtr->id1pdf(); int id2pdfup = infoPtr->id2pdf(); double x1pdfup = infoPtr->x1pdf(); double x2pdfup = infoPtr->x2pdf(); double scalePDFup = infoPtr->QFac(); double pdf1up = infoPtr->pdf1(); double pdf2up = infoPtr->pdf2(); setPdf(id1pdfup, id2pdfup, x1pdfup, x2pdfup, scalePDFup, pdf1up, pdf2up, true); // Done. return true; } //-------------------------------------------------------------------------- // Update cross-section information at the end of the run. bool LHAupFromPYTHIA8::updateSigma() { // Read out information from PYTHIA 8 and send it in to LHA. double sigGen = CONVERTMB2PB * infoPtr->sigmaGen(); double sigErr = CONVERTMB2PB * infoPtr->sigmaErr(); setXSec(0, sigGen); setXErr(0, sigErr); // Done. return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/MiniStringFragmentation.cc0000644000175000017500000002630212217346246020243 0ustar sunsun// MiniStringFragmentation.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the . // MiniStringFragmentation class #include "Pythia8/MiniStringFragmentation.h" namespace Pythia8 { //========================================================================== // The MiniStringFragmentation class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Since diffractive by definition is > 1 particle, try hard. const int MiniStringFragmentation::NTRYDIFFRACTIVE = 200; // After one-body fragmentation failed, try two-body once more. const int MiniStringFragmentation::NTRYLASTRESORT = 100; // Loop try to combine available endquarks to valid hadron. const int MiniStringFragmentation::NTRYFLAV = 10; //-------------------------------------------------------------------------- // Initialize and save pointers. void MiniStringFragmentation::init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, StringFlav* flavSelPtrIn, StringPT* pTSelPtrIn, StringZ* zSelPtrIn) { // Save pointers. infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; flavSelPtr = flavSelPtrIn; pTSelPtr = pTSelPtrIn; zSelPtr = zSelPtrIn; // Initialize the MiniStringFragmentation class proper. nTryMass = settings.mode("MiniStringFragmentation:nTry"); // Initialize the b parameter of the z spectrum, used when joining jets. bLund = zSelPtr->bAreaLund(); } //-------------------------------------------------------------------------- // Do the fragmentation: driver routine. bool MiniStringFragmentation::fragment(int iSub, ColConfig& colConfig, Event& event, bool isDiff) { // Junction topologies not yet considered - is very rare. iParton = colConfig[iSub].iParton; if (iParton.front() < 0) { infoPtr->errorMsg("Error in MiniStringFragmentation::fragment: " "very low-mass junction topologies not yet handled"); return false; } // Read in info on system to be treated. flav1 = FlavContainer( event[ iParton.front() ].id() ); flav2 = FlavContainer( event[ iParton.back() ].id() ); pSum = colConfig[iSub].pSum; mSum = colConfig[iSub].mass; m2Sum = mSum*mSum; isClosed = colConfig[iSub].isClosed; // Do not want diffractive systems to easily collapse to one particle. int nTryFirst = (isDiff) ? NTRYDIFFRACTIVE : nTryMass; // First try to produce two particles from the system. if (ministring2two( nTryFirst, event)) return true; // If this fails, then form one hadron and shuffle momentum. if (ministring2one( iSub, colConfig, event)) return true; // If also this fails, then try harder to produce two particles. if (ministring2two( NTRYLASTRESORT, event)) return true; // Else complete failure. infoPtr->errorMsg("Error in MiniStringFragmentation::fragment: " "no 1- or 2-body state found above mass threshold"); return false; } //-------------------------------------------------------------------------- // Attempt to produce two particles from the ministring. bool MiniStringFragmentation::ministring2two( int nTry, Event& event) { // Properties of the produced hadrons. int idHad1 = 0; int idHad2 = 0; double mHad1 = 0.; double mHad2 = 0.; double mHadSum = 0.; // Allow a few attempts to find a particle pair with low enough masses. for (int iTry = 0; iTry < nTry; ++iTry) { // For closed gluon loop need to pick an initial flavour. if (isClosed) do { int idStart = flavSelPtr->pickLightQ(); FlavContainer flavStart(idStart, 1); flavStart = flavSelPtr->pick( flavStart); flav1 = flavSelPtr->pick( flavStart); flav2.anti(flav1); } while (flav1.id == 0 || flav1.nPop > 0); // Create a new q qbar flavour to form two hadrons. // Start from a diquark, if any. do { FlavContainer flav3 = (flav1.isDiquark() || (!flav2.isDiquark() && rndmPtr->flat() < 0.5) ) ? flavSelPtr->pick( flav1) : flavSelPtr->pick( flav2).anti(); idHad1 = flavSelPtr->combine( flav1, flav3); idHad2 = flavSelPtr->combine( flav2, flav3.anti()); } while (idHad1 == 0 || idHad2 == 0); // Check whether the mass sum fits inside the available phase space. mHad1 = particleDataPtr->mSel(idHad1); mHad2 = particleDataPtr->mSel(idHad2); mHadSum = mHad1 + mHad2; if (mHadSum < mSum) break; } if (mHadSum >= mSum) return false; // Define an effective two-parton string, by splitting intermediate // gluon momenta in proportion to their closeness to either endpoint. Vec4 pSum1 = event[ iParton.front() ].p(); Vec4 pSum2 = event[ iParton.back() ].p(); if (iParton.size() > 2) { Vec4 pEnd1 = pSum1; Vec4 pEnd2 = pSum2; Vec4 pEndSum = pEnd1 + pEnd2; for (int i = 1; i < int(iParton.size()) - 1 ; ++i) { Vec4 pNow = event[ iParton[i] ].p(); double ratio = (pEnd2 * pNow) / (pEndSum * pNow); pSum1 += ratio * pNow; pSum2 += (1. - ratio) * pNow; } } // Set up a string region based on the two effective endpoints. StringRegion region; region.setUp( pSum1, pSum2); // Generate an isotropic decay in the ministring rest frame, // suppressed at large pT by a fragmentation pT Gaussian. double pAbs2 = 0.25 * ( pow2(m2Sum - mHad1*mHad1 - mHad2*mHad2) - pow2(2. * mHad1 * mHad2) ) / m2Sum; double pT2 = 0.; do { double cosTheta = rndmPtr->flat(); pT2 = (1. - pow2(cosTheta)) * pAbs2; } while (pTSelPtr->suppressPT2(pT2) < rndmPtr->flat() ); // Construct the forward-backward asymmetry of the two particles. double mT21 = mHad1*mHad1 + pT2; double mT22 = mHad2*mHad2 + pT2; double lambda = sqrtpos( pow2(m2Sum - mT21 - mT22) - 4. * mT21 * mT22 ); double probReverse = 1. / (1. + exp( min( 50., bLund * lambda) ) ); // Construct kinematics, as viewed in the transverse rest frame. double xpz1 = 0.5 * lambda/ m2Sum; if (probReverse > rndmPtr->flat()) xpz1 = -xpz1; double xmDiff = (mT21 - mT22) / m2Sum; double xe1 = 0.5 * (1. + xmDiff); double xe2 = 0.5 * (1. - xmDiff ); // Distribute pT isotropically in angle. double phi = 2. * M_PI * rndmPtr->flat(); double pT = sqrt(pT2); double px = pT * cos(phi); double py = pT * sin(phi); // Translate this into kinematics in the string frame. Vec4 pHad1 = region.pHad( xe1 + xpz1, xe1 - xpz1, px, py); Vec4 pHad2 = region.pHad( xe2 - xpz1, xe2 + xpz1, -px, -py); // Add produced particles to the event record. int iFirst = event.append( idHad1, 82, iParton.front(), iParton.back(), 0, 0, 0, 0, pHad1, mHad1); int iLast = event.append( idHad2, 82, iParton.front(), iParton.back(), 0, 0, 0, 0, pHad2, mHad2); // Set decay vertex when this is displaced. if (event[iParton.front()].hasVertex()) { Vec4 vDec = event[iParton.front()].vDec(); event[iFirst].vProd( vDec ); event[iLast].vProd( vDec ); } // Set lifetime of hadrons. event[iFirst].tau( event[iFirst].tau0() * rndmPtr->exp() ); event[iLast].tau( event[iLast].tau0() * rndmPtr->exp() ); // Mark original partons as hadronized and set their daughter range. for (int i = 0; i < int(iParton.size()); ++i) { event[ iParton[i] ].statusNeg(); event[ iParton[i] ].daughters(iFirst, iLast); } // Successfully done. return true; } //-------------------------------------------------------------------------- // Attempt to produce one particle from a ministring. // Current algorithm: find the system with largest invariant mass // relative to the existing one, and boost that system appropriately. // Try more sophisticated alternatives later?? (Z0 mass shifted??) // Also, if problems, attempt several times to obtain closer mass match?? bool MiniStringFragmentation::ministring2one( int iSub, ColConfig& colConfig, Event& event) { // Cannot handle qq + qbarqbar system. if (abs(flav1.id) > 100 && abs(flav2.id) > 100) return false; // For closed gluon loop need to pick an initial flavour. if (isClosed) do { int idStart = flavSelPtr->pickLightQ(); FlavContainer flavStart(idStart, 1); flav1 = flavSelPtr->pick( flavStart); flav2 = flav1.anti(); } while (abs(flav1.id) > 100); // Select hadron flavour from available quark flavours. int idHad = 0; for (int iTryFlav = 0; iTryFlav < NTRYFLAV; ++iTryFlav) { idHad = flavSelPtr->combine( flav1, flav2); if (idHad != 0) break; } if (idHad == 0) return false; // Find mass. double mHad = particleDataPtr->mSel(idHad); // Find the untreated parton system which combines to the largest // squared mass above mimimum required. int iMax = -1; double deltaM2 = mHad*mHad - mSum*mSum; double delta2Max = 0.; for (int iRec = iSub + 1; iRec < colConfig.size(); ++iRec) { double delta2Rec = 2. * (pSum * colConfig[iRec].pSum) - deltaM2 - 2. * mHad * colConfig[iRec].mass; if (delta2Rec > delta2Max) { iMax = iRec; delta2Max = delta2Rec;} } if (iMax == -1) return false; // Construct kinematics of the hadron and recoiling system. Vec4& pRec = colConfig[iMax].pSum; double mRec = colConfig[iMax].mass; double vecProd = pSum * pRec; double coefOld = mSum*mSum + vecProd; double coefNew = mHad*mHad + vecProd; double coefRec = mRec*mRec + vecProd; double coefSum = coefOld + coefNew; double sHat = coefOld + coefRec; double root = sqrtpos( (pow2(coefSum) - 4. * sHat * mHad*mHad) / (pow2(vecProd) - pow2(mSum * mRec)) ); double k2 = 0.5 * (coefOld * root - coefSum) / sHat; double k1 = (coefRec * k2 + 0.5 * deltaM2) / coefOld; Vec4 pHad = (1. + k1) * pSum - k2 * pRec; Vec4 pRecNew = (1. + k2) * pRec - k1 * pSum; // Add the produced particle to the event record. int iHad = event.append( idHad, 81, iParton.front(), iParton.back(), 0, 0, 0, 0, pHad, mHad); // Set decay vertex when this is displaced. if (event[iParton.front()].hasVertex()) { Vec4 vDec = event[iParton.front()].vDec(); event[iHad].vProd( vDec ); } // Set lifetime of hadron. event[iHad].tau( event[iHad].tau0() * rndmPtr->exp() ); // Mark original partons as hadronized and set their daughter range. for (int i = 0; i < int(iParton.size()); ++i) { event[ iParton[i] ].statusNeg(); event[ iParton[i] ].daughters(iHad, iHad); } // Copy down recoiling system, with boosted momentum. Update current partons. RotBstMatrix M; M.bst(pRec, pRecNew); for (int i = 0; i < colConfig[iMax].size(); ++i) { int iOld = colConfig[iMax].iParton[i]; // Do not touch negative iOld = beginning of new junction leg. if (iOld >= 0) { int iNew = event.copy(iOld, 72); event[iNew].rotbst(M); colConfig[iMax].iParton[i] = iNew; } } colConfig[iMax].pSum = pRecNew; colConfig[iMax].isCollected = true; // Successfully done. return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/Info.cc0000644000175000017500000002353412217346246014340 0ustar sunsun// Info.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the Info class. #include "Pythia8/Info.h" namespace Pythia8 { //========================================================================== // Info class. // This class contains a mixed bag of information on the event generation // activity, especially on the current subprocess properties. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of times the same error message will be repeated at most. const int Info::TIMESTOPRINT = 1; // LHA convention with cross section in pb may require conversion from mb. const double Info::CONVERTMB2PB = 1e9; //-------------------------------------------------------------------------- // List (almost) all information currently set. void Info::list(ostream& os) const { // Header and beam info. os << "\n -------- PYTHIA Info Listing ------------------------" << "---------------- \n \n" << scientific << setprecision(3) << " Beam A: id = " << setw(6) << idASave << ", pz = " << setw(10) << pzASave << ", e = " << setw(10) << eASave << ", m = " << setw(10) << mASave << ".\n" << " Beam B: id = " << setw(6) << idBSave << ", pz = " << setw(10) << pzBSave << ", e = " << setw(10) << eBSave << ", m = " << setw(10) << mBSave << ".\n\n"; // Done if no subprocess has been defined. if (codeSave == 0 && nFinalSave == 0) { os << " No process has been set; something must have gone wrong! \n" << "\n -------- End PYTHIA Info Listing --------------------" << "----------------" << endl; return; } // Colliding parton info. if (isRes) { os << " In 1: id = " << setw(4) << id1pdfSave[0] << ", x = " << setw(10) << x1pdfSave[0] << ", pdf = " << setw(10) << pdf1Save[0] << " at Q2 = " << setw(10) << Q2FacSave[0] << ".\n" << " In 2: id = " << setw(4) << id2pdfSave[0] << ", x = " << setw(10) << x2pdfSave[0] << ", pdf = " << setw(10) << pdf2Save[0] << " at same Q2.\n"; bool matchIdX = true; if (id1pdfSave[0] != id1Save[0] || id2pdfSave[0] != id2Save[0]) matchIdX = false; if (abs(x1pdfSave[0] - x1Save[0]) > 1e-4 * x1Save[0]) matchIdX = false; if (abs(x2pdfSave[0] - x2Save[0]) > 1e-4 * x2Save[0]) matchIdX = false; if (!matchIdX) os << " Warning: above flavour/x info does not match" << " incoming partons in event!\n"; os << "\n"; } // Process name and code. os << ((isRes && !hasSubSave[0]) ? " Subprocess " : " Process ") << nameSave << " with code " << codeSave << " is 2 -> " << nFinalSave << ".\n"; // Subprocess name and code for nondiffractive processes. if (hasSubSave[0]) os << " Subprocess " << nameSubSave[0] << " with code " << codeSubSave[0] << " is 2 -> " << nFinalSubSave[0] << ".\n"; // Process-type-specific kinematics information. if ( isRes && nFinalSave == 1) os << " It has sHat = " << setw(10) << sH[0] << ".\n"; else if ( isRes && nFinalSave == 2) os << " It has sHat = " << setw(10) << sH[0] << ", tHat = " << setw(10) << tH[0] << ", uHat = " << setw(10) << uH[0] << ",\n" << " pTHat = " << setw(10) << pTH[0] << ", m3Hat = " << setw(10) << m3H[0] << ", m4Hat = " << setw(10) << m4H[0] << ",\n" << " thetaHat = " << setw(10) << thetaH[0] << ", phiHat = " << setw(10) << phiH[0] << ".\n"; else if ( nFinalSave == 2) os << " It has s = " << setw(10) << sH[0] << ", t = " << setw(10) << tH[0] << ", u = " << setw(10) << uH[0] << ",\n" << " pT = " << setw(10) << pTH[0] << ", m3 = " << setw(10) << m3H[0] << ", m4 = " << setw(10) << m4H[0] << ",\n" << " theta = " << setw(10) << thetaH[0] << ", phi = " << setw(10) << phiH[0] << ".\n"; else if ( isRes && nFinalSave == 3) os << " It has sHat = " << setw(10) << sH[0] << ", = " << setw(10) << pTH[0] << ".\n"; else if ( nFinalSave == 3) os << " It has s = " << setw(10) << sH[0] << ", t_A = " << setw(10) << tH[0] << ", t_B = " << setw(10) << uH[0] << ",\n" << " = " << setw(10) << pTH[0] << ".\n"; // Couplings. if (isRes) os << " alphaEM = " << setw(10) << alphaEMSave[0] << ", alphaS = " << setw(10) << alphaSSave[0] << " at Q2 = " << setw(10) << Q2RenSave[0] << ".\n"; // Diffractive subsystems. for (int iDS = 1; iDS < 4; ++iDS) if (id1Save[iDS] != 0) { if (iDS == 1) os << "\n Diffractive system on side A: \n"; if (iDS == 2) os << "\n Diffractive system on side B: \n"; if (iDS == 3) os << "\n Central diffractive system: \n"; os << " In 1: id = " << setw(4) << id1pdfSave[iDS] << ", x = " << setw(10) << x1pdfSave[iDS] << ", pdf = " << setw(10) << pdf1Save[iDS] << " at Q2 = " << setw(10) << Q2FacSave[iDS] << ".\n" << " In 2: id = " << setw(4) << id2pdfSave[iDS] << ", x = " << setw(10) << x2pdfSave[iDS] << ", pdf = " << setw(10) << pdf2Save[iDS] << " at same Q2.\n"; os << " Subprocess " << nameSubSave[iDS] << " with code " << codeSubSave[iDS] << " is 2 -> " << nFinalSubSave[iDS] << ".\n"; if (nFinalSubSave[iDS] == 1) os << " It has sHat = " << setw(10) << sH[iDS] << ".\n"; else if (nFinalSubSave[iDS] == 2) os << " It has sHat = " << setw(10) << sH[iDS] << ", tHat = " << setw(10) << tH[iDS] << ", uHat = " << setw(10) << uH[iDS] << ",\n" << " pTHat = " << setw(10) << pTH[iDS] << ", m3Hat = " << setw(10) << m3H[iDS] << ", m4Hat = " << setw(10) << m4H[iDS] << ",\n" << " thetaHat = " << setw(10) << thetaH[iDS] << ", phiHat = " << setw(10) << phiH[iDS] << ".\n"; os << " alphaEM = " << setw(10) << alphaEMSave[iDS] << ", alphaS = " << setw(10) << alphaSSave[iDS] << " at Q2 = " << setw(10) << Q2RenSave[iDS] << ".\n"; } // Impact parameter. if (bIsSet) os << "\n Impact parameter b = " << setw(10) << bMPISave << " gives enhancement factor = " << setw(10) << enhanceMPISave << ".\n"; // Multiparton interactions and shower evolution. if (evolIsSet) os << " Max pT scale for MPI = " << setw(10) << pTmaxMPISave << ", ISR = " << setw(10) << pTmaxISRSave << ", FSR = " << setw(10) << pTmaxISRSave << ".\n Number of MPI = " << setw(5) << nMPISave << ", ISR = " << setw(5) << nISRSave << ", FSRproc = " << setw(5) << nFSRinProcSave << ", FSRreson = " << setw(5) << nFSRinResSave << ".\n"; // Listing finished. os << "\n -------- End PYTHIA Info Listing --------------------" << "----------------" << endl; } //-------------------------------------------------------------------------- // Event weight and accumulated weight. double Info::weight() const { return (abs(lhaStrategySave) == 4) ? CONVERTMB2PB * weightSave : weightSave; } double Info::weightSum() const {return (abs(lhaStrategySave) == 4) ? CONVERTMB2PB * wtAccSum : wtAccSum; } //-------------------------------------------------------------------------- // Print a message the first few times. Insert in database. void Info::errorMsg(string messageIn, string extraIn, bool showAlways, ostream& os) { // Recover number of times message occured. Also inserts new string. int times = messages[messageIn]; ++messages[messageIn]; // Print message the first few times. if (times < TIMESTOPRINT || showAlways) os << " PYTHIA " << messageIn << " " << extraIn << endl; } //-------------------------------------------------------------------------- // Provide total number of errors/aborts/warnings experienced to date. int Info::errorTotalNumber() { int nTot = 0; for ( map::iterator messageEntry = messages.begin(); messageEntry != messages.end(); ++messageEntry) nTot += messageEntry->second; return nTot; } //-------------------------------------------------------------------------- // Print statistics on errors/aborts/warnings. void Info::errorStatistics(ostream& os) { // Header. os << "\n *------- PYTHIA Error and Warning Messages Statistics " << "----------------------------------------------------------* \n" << " | " << " | \n" << " | times message " << " | \n" << " | " << " | \n"; // Loop over all messages map::iterator messageEntry = messages.begin(); if (messageEntry == messages.end()) os << " | 0 no errors or warnings to report " << " | \n"; while (messageEntry != messages.end()) { // Message printout. string temp = messageEntry->first; int len = temp.length(); temp.insert( len, max(0, 102 - len), ' '); os << " | " << setw(6) << messageEntry->second << " " << temp << " | \n"; ++messageEntry; } // Done. os << " | " << " | \n" << " *------- End PYTHIA Error and Warning Messages Statistics" << " ------------------------------------------------------* " << endl; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/FJcore.cc0000644000175000017500000050064012217346245014612 0ustar sunsun// fjcore -- extracted from FastJet v3.0.5 (http://fastjet.fr) // // fjcore constitutes a digest of the main FastJet functionality. // The files fjcore.hh and fjcore.cc are meant to provide easy access to these // core functions, in the form of single files and without the need of a full // FastJet installation: // // g++ main.cc fjcore.cc // // with main.cc including fjcore.hh. // // The results are expected to be identical to those obtained by linking to // the full FastJet distribution. // // NOTE THAT, IN ORDER TO MAKE IT POSSIBLE FOR FJCORE AND THE FULL FASTJET // TO COEXIST, THE FORMER USES THE "fjcore" NAMESPACE INSTEAD OF "fastjet". // // In particular, fjcore provides: // // - access to all native pp and ee algorithms, kt, anti-kt, C/A. // For C/A, the NlnN method is available, while anti-kt and kt // are limited to the N^2 one (still the fastest for N < 20k particles) // - access to selectors, for implementing cuts and selections // - access to all functionalities related to pseudojets (e.g. a jet's // structure or user-defined information) // // Instead, it does NOT provide: // // - jet areas functionality // - background estimation // - access to other algorithms via plugins // - interface to CGAL // - fastjet tools, e.g. filters, taggers // // If these functionalities are needed, the full FastJet installation must be // used. The code will be fully compatible, with the sole replacement of the // header files and of the fjcore namespace with the fastjet one. // // fjcore.hh and fjcore.cc are not meant to be human-readable. // For documentation, see the full FastJet manual and doxygen at http://fastjet.fr // // Like FastJet, fjcore is released under the terms of the GNU General Public // License version 2 (GPLv2). If you use this code as part of work towards a // scientific publication, whether directly or contained within another program // (e.g. Delphes, SpartyJet, Rivet, LHC collaboration software frameworks, // etc.), you should include a citation to // // EPJC72(2012)1896 [arXiv:1111.6097] (FastJet User Manual) // and, optionally, Phys.Lett.B641 (2006) 57 [arXiv:hep-ph/0512210] // // Copyright (c) 2005-2013, Matteo Cacciari, Gavin P. Salam and Gregory Soyez // //---------------------------------------------------------------------- // This file is part of FastJet. // // FastJet is free software; you can redistribute it and/or modify // it under the terms of the GNU General Public License as published by // the Free Software Foundation; either version 2 of the License, or // (at your option) any later version. // // The algorithms that underlie FastJet have required considerable // development and are described in hep-ph/0512210. If you use // FastJet as part of work towards a scientific publication, please // include a citation to the FastJet paper. // // FastJet is distributed in the hope that it will be useful, // but WITHOUT ANY WARRANTY; without even the implied warranty of // MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the // GNU General Public License for more details. // // You should have received a copy of the GNU General Public License // along with FastJet. If not, see . //---------------------------------------------------------------------- // //#include "fjcore.hh" // For inclusion in Pythia8 line above is replaced by line below. #include "Pythia8/FJcore.h" #ifndef __FJCORE_VERSION_HH__ #define __FJCORE_VERSION_HH__ #include FJCORE_BEGIN_NAMESPACE const char* fastjet_version = FJCORE_PACKAGE_VERSION; FJCORE_END_NAMESPACE #endif // __FJCORE_VERSION_HH__ #ifndef __FJCORE_CLUSTERQUENCE_N2_ICC__ #define __FJCORE_CLUSTERQUENCE_N2_ICC__ FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh template void ClusterSequence::_simple_N2_cluster() { int n = _jets.size(); BJ * briefjets = new BJ[n]; BJ * jetA = briefjets, * jetB; for (int i = 0; i< n; i++) { _bj_set_jetinfo(jetA, i); jetA++; // move on to next entry of briefjets } BJ * tail = jetA; // a semaphore for the end of briefjets BJ * head = briefjets; // a nicer way of naming start for (jetA = head + 1; jetA != tail; jetA++) { _bj_set_NN_crosscheck(jetA, head, jetA); } double * diJ = new double[n]; jetA = head; for (int i = 0; i < n; i++) { diJ[i] = _bj_diJ(jetA); jetA++; // have jetA follow i } int history_location = n-1; while (tail != head) { double diJ_min = diJ[0]; int diJ_min_jet = 0; for (int i = 1; i < n; i++) { if (diJ[i] < diJ_min) {diJ_min_jet = i; diJ_min = diJ[i];} } history_location++; jetA = & briefjets[diJ_min_jet]; jetB = static_cast(jetA->NN); diJ_min *= _invR2; if (jetB != NULL) { if (jetA < jetB) {std::swap(jetA,jetB);} int nn; // new jet index _do_ij_recombination_step(jetA->_jets_index, jetB->_jets_index, diJ_min, nn); _bj_set_jetinfo(jetB, nn); } else { _do_iB_recombination_step(jetA->_jets_index, diJ_min); } tail--; n--; *jetA = *tail; diJ[jetA - head] = diJ[tail-head]; for (BJ * jetI = head; jetI != tail; jetI++) { if (jetI->NN == jetA || jetI->NN == jetB) { _bj_set_NN_nocross(jetI, head, tail); diJ[jetI-head] = _bj_diJ(jetI); // update diJ } if (jetB != NULL) { double dist = _bj_dist(jetI,jetB); if (dist < jetI->NN_dist) { if (jetI != jetB) { jetI->NN_dist = dist; jetI->NN = jetB; diJ[jetI-head] = _bj_diJ(jetI); // update diJ... } } if (dist < jetB->NN_dist) { if (jetI != jetB) { jetB->NN_dist = dist; jetB->NN = jetI;} } } if (jetI->NN == tail) {jetI->NN = jetA;} } if (jetB != NULL) {diJ[jetB-head] = _bj_diJ(jetB);} } delete[] diJ; delete[] briefjets; } FJCORE_END_NAMESPACE #endif // __FJCORE_CLUSTERQUENCE_N2_ICC__ #ifndef __FJCORE_DYNAMICNEARESTNEIGHBOURS_HH__ #define __FJCORE_DYNAMICNEARESTNEIGHBOURS_HH__ #include #include #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class EtaPhi { public: double first, second; EtaPhi() {} EtaPhi(double a, double b) {first = a; second = b;} void sanitize() { if (second < 0) second += twopi; if (second >= twopi) second -= twopi; } }; class DnnError { public: DnnError() {;}; DnnError(const std::string & message_in) { _message = message_in; std::cerr << message_in << std::endl;}; std::string message() const {return _message;}; private: std::string _message; }; class DynamicNearestNeighbours { public: virtual int NearestNeighbourIndex(const int & ii) const = 0; virtual double NearestNeighbourDistance(const int & ii) const = 0; virtual bool Valid(const int & index) const = 0; virtual void RemoveAndAddPoints(const std::vector & indices_to_remove, const std::vector & points_to_add, std::vector & indices_added, std::vector & indices_of_updated_neighbours) = 0; inline void RemovePoint (const int & index, std::vector & indices_of_updated_neighbours) { std::vector indices_added; std::vector points_to_add; std::vector indices_to_remove(1); indices_to_remove[0] = index; RemoveAndAddPoints(indices_to_remove, points_to_add, indices_added, indices_of_updated_neighbours );}; inline void RemoveCombinedAddCombination( const int & index1, const int & index2, const EtaPhi & newpoint, int & index3, std::vector & indices_of_updated_neighbours) { std::vector indices_added(1); std::vector points_to_add(1); std::vector indices_to_remove(2); indices_to_remove[0] = index1; indices_to_remove[1] = index2; points_to_add[0] = newpoint; RemoveAndAddPoints(indices_to_remove, points_to_add, indices_added, indices_of_updated_neighbours ); index3 = indices_added[0]; }; virtual ~DynamicNearestNeighbours () {} }; FJCORE_END_NAMESPACE #endif // __FJCORE_DYNAMICNEARESTNEIGHBOURS_HH__ #ifndef __FJCORE_SEARCHTREE_HH__ #define __FJCORE_SEARCHTREE_HH__ #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh template class SearchTree { public: class Node; class circulator; class const_circulator; SearchTree(const std::vector & init); SearchTree(const std::vector & init, unsigned int max_size); void remove(unsigned node_index); void remove(typename SearchTree::Node * node); void remove(typename SearchTree::circulator & circ); circulator insert(const T & value); const Node & operator[](int i) const {return _nodes[i];}; unsigned int size() const {return _nodes.size() - _available_nodes.size();} void verify_structure(); void verify_structure_linear() const; void verify_structure_recursive(const Node * , const Node * , const Node * ) const; void print_elements(); #ifdef __FJCORE_SEARCHTREE_TRACK_DEPTH inline unsigned int max_depth() const {return _max_depth;}; #else inline unsigned int max_depth() const {return 0;}; #endif int loc(const Node * node) const ; Node * _find_predecessor(const Node *); Node * _find_successor(const Node *); const Node & operator[](unsigned int i) const {return _nodes[i];}; const_circulator somewhere() const; circulator somewhere(); private: void _initialize(const std::vector & init); std::vector _nodes; std::vector _available_nodes; Node * _top_node; unsigned int _n_removes; void _do_initial_connections(unsigned int this_one, unsigned int scale, unsigned int left_edge, unsigned int right_edge, unsigned int depth); #ifdef __FJCORE_SEARCHTREE_TRACK_DEPTH unsigned int _max_depth; #endif }; template class SearchTree::Node{ public: Node() {}; /// default constructor bool treelinks_null() const { return ((parent==0) && (left==0) && (right==0));}; inline void nullify_treelinks() { parent = NULL; left = NULL; right = NULL; }; void reset_parents_link_to_me(Node * XX); T value; Node * left; Node * right; Node * parent; Node * successor; Node * predecessor; }; template void SearchTree::Node::reset_parents_link_to_me(typename SearchTree::Node * XX) { if (parent == NULL) {return;} if (parent->right == this) {parent->right = XX;} else {parent->left = XX;} } template class SearchTree::circulator{ public: template friend class SearchTree::const_circulator; friend class SearchTree; circulator() : _node(NULL) {} circulator(Node * node) : _node(node) {} const T * operator->() const {return &(_node->value);} T * operator->() {return &(_node->value);} const T & operator*() const {return _node->value;} T & operator*() {return _node->value;} circulator & operator++() { _node = _node->successor; return *this;} circulator operator++(int) { circulator tmp = *this; _node = _node->successor; return tmp;} circulator & operator--() { _node = _node->predecessor; return *this;} circulator operator--(int) { circulator tmp = *this; _node = _node->predecessor; return tmp;} circulator next() const { return circulator(_node->successor);} circulator previous() const { return circulator(_node->predecessor);} bool operator!=(const circulator & other) const {return other._node != _node;} bool operator==(const circulator & other) const {return other._node == _node;} private: Node * _node; }; template class SearchTree::const_circulator{ public: const_circulator() : _node(NULL) {} const_circulator(const Node * node) : _node(node) {} const_circulator(const circulator & circ) :_node(circ._node) {} const T * operator->() {return &(_node->value);} const T & operator*() const {return _node->value;} const_circulator & operator++() { _node = _node->successor; return *this;} const_circulator operator++(int) { const_circulator tmp = *this; _node = _node->successor; return tmp;} const_circulator & operator--() { _node = _node->predecessor; return *this;} const_circulator operator--(int) { const_circulator tmp = *this; _node = _node->predecessor; return tmp;} const_circulator next() const { return const_circulator(_node->successor);} const_circulator previous() const { return const_circulator(_node->predecessor);} bool operator!=(const const_circulator & other) const {return other._node != _node;} bool operator==(const const_circulator & other) const {return other._node == _node;} private: const Node * _node; }; template SearchTree::SearchTree(const std::vector & init, unsigned int max_size) : _nodes(max_size) { _available_nodes.reserve(max_size); _available_nodes.resize(max_size - init.size()); for (unsigned int i = init.size(); i < max_size; i++) { _available_nodes[i-init.size()] = &(_nodes[i]); } _initialize(init); } template SearchTree::SearchTree(const std::vector & init) : _nodes(init.size()), _available_nodes(0) { _available_nodes.reserve(init.size()); _initialize(init); } template void SearchTree::_initialize(const std::vector & init) { _n_removes = 0; unsigned n = init.size(); assert(n>=1); #ifdef __FJCORE_SEARCHTREE_TRACK_DEPTH _max_depth = 0; #endif for (unsigned int i = 1; i inline int SearchTree::loc(const Node * node) const {return node == NULL? -999 : node - &(_nodes[0]);} template void SearchTree::_do_initial_connections( unsigned int this_one, unsigned int scale, unsigned int left_edge, unsigned int right_edge, unsigned int depth ) { #ifdef __FJCORE_SEARCHTREE_TRACK_DEPTH _max_depth = max(depth, _max_depth); #endif unsigned int ref_new_scale = (scale+1)/2; unsigned new_scale = ref_new_scale; bool did_child = false; while(true) { int left = this_one - new_scale; // be careful here to use signed int... if (left >= static_cast(left_edge) && _nodes[left].treelinks_null() ) { _nodes[left].parent = &(_nodes[this_one]); _nodes[this_one].left = &(_nodes[left]); _do_initial_connections(left, new_scale, left_edge, this_one, depth+1); did_child = true; break; } unsigned int old_new_scale = new_scale; new_scale = (old_new_scale + 1)/2; if (new_scale == old_new_scale) break; } if (!did_child) {_nodes[this_one].left = NULL;} new_scale = ref_new_scale; did_child = false; while(true) { unsigned int right = this_one + new_scale; if (right < right_edge && _nodes[right].treelinks_null()) { _nodes[right].parent = &(_nodes[this_one]); _nodes[this_one].right = &(_nodes[right]); _do_initial_connections(right, new_scale, this_one+1,right_edge,depth+1); did_child = true; break; } unsigned int old_new_scale = new_scale; new_scale = (old_new_scale + 1)/2; if (new_scale == old_new_scale) break; } if (!did_child) {_nodes[this_one].right = NULL;} } template void SearchTree::remove(unsigned int node_index) { remove(&(_nodes[node_index])); } template void SearchTree::remove(circulator & circ) { remove(circ._node); } template void SearchTree::remove(typename SearchTree::Node * node) { assert(size() > 1); // switch this to throw...? assert(!node->treelinks_null()); node->predecessor->successor = node->successor; node->successor->predecessor = node->predecessor; if (node->left == NULL && node->right == NULL) { node->reset_parents_link_to_me(NULL); } else if (node->left != NULL && node->right == NULL){ node->reset_parents_link_to_me(node->left); node->left->parent = node->parent; if (_top_node == node) {_top_node = node->left;} } else if (node->left == NULL && node->right != NULL){ node->reset_parents_link_to_me(node->right); node->right->parent = node->parent; if (_top_node == node) {_top_node = node->right;} } else { Node * replacement; bool use_predecessor = (_n_removes % 2 == 1); if (use_predecessor) { replacement = node->predecessor; assert(replacement->right == NULL); // guaranteed if it's our predecessor if (replacement != node->left) { if (replacement->left != NULL) { replacement->left->parent = replacement->parent;} replacement->reset_parents_link_to_me(replacement->left); replacement->left = node->left; } replacement->parent = node->parent; replacement->right = node->right; } else { replacement = node->successor; assert(replacement->left == NULL); // guaranteed if it's our successor if (replacement != node->right) { if (replacement->right != NULL) { replacement->right->parent = replacement->parent;} replacement->reset_parents_link_to_me(replacement->right); replacement->right = node->right; } replacement->parent = node->parent; replacement->left = node->left; } node->reset_parents_link_to_me(replacement); if (node->left != replacement) {node->left->parent = replacement;} if (node->right != replacement) {node->right->parent = replacement;} if (_top_node == node) {_top_node = replacement;} } node->nullify_treelinks(); node->predecessor = NULL; node->successor = NULL; _n_removes++; _available_nodes.push_back(node); } template typename SearchTree::circulator SearchTree::insert(const T & value) { assert(_available_nodes.size() > 0); Node * node = _available_nodes.back(); _available_nodes.pop_back(); node->value = value; Node * location = _top_node; Node * old_location = NULL; bool on_left = true; // (init not needed -- but soothes g++4) #ifdef __FJCORE_SEARCHTREE_TRACK_DEPTH unsigned int depth = 0; #endif while(location != NULL) { #ifdef __FJCORE_SEARCHTREE_TRACK_DEPTH depth++; #endif old_location = location; on_left = value < location->value; if (on_left) {location = location->left;} else {location = location->right;} } #ifdef __FJCORE_SEARCHTREE_TRACK_DEPTH _max_depth = max(depth, _max_depth); #endif node->parent = old_location; if (on_left) {node->parent->left = node;} else {node->parent->right = node;} node->left = NULL; node->right = NULL; node->predecessor = _find_predecessor(node); if (node->predecessor != NULL) { node->successor = node->predecessor->successor; node->predecessor->successor = node; node->successor->predecessor = node; } else { node->successor = _find_successor(node); assert(node->successor != NULL); // can only happen if we're sole element node->predecessor = node->successor->predecessor; node->successor->predecessor = node; node->predecessor->successor = node; } return circulator(node); } template void SearchTree::verify_structure() { verify_structure_linear(); const Node * left_limit = _top_node; while (left_limit->left != NULL) {left_limit = left_limit->left;} const Node * right_limit = _top_node; while (right_limit->right != NULL) {right_limit = right_limit->right;} verify_structure_recursive(_top_node, left_limit, right_limit); } template void SearchTree::verify_structure_recursive( const typename SearchTree::Node * element, const typename SearchTree::Node * left_limit, const typename SearchTree::Node * right_limit) const { assert(!(element->value < left_limit->value)); assert(!(right_limit->value < element->value)); const Node * left = element->left; if (left != NULL) { assert(!(element->value < left->value)); if (left != left_limit) { verify_structure_recursive(left, left_limit, element);} } const Node * right = element->right; if (right != NULL) { assert(!(right->value < element->value)); if (right != right_limit) { verify_structure_recursive(right, element, right_limit);} } } template void SearchTree::verify_structure_linear() const { unsigned n_top = 0; unsigned n_null = 0; for(unsigned i = 0; i < _nodes.size(); i++) { const typename SearchTree::Node * node = &(_nodes[i]); if (node->treelinks_null()) {n_null++; continue;} if (node->parent == NULL) { n_top++; } else { assert((node->parent->left == node) ^ (node->parent->right == node)); } if (node->left != NULL) { assert(!(node->value < node->left->value ));} if (node->right != NULL) { assert(!(node->right->value < node->value ));} } assert(n_top == 1 || (n_top == 0 && size() <= 1) ); assert(n_null == _available_nodes.size() || (n_null == _available_nodes.size() + 1 && size() == 1)); } template typename SearchTree::Node * SearchTree::_find_predecessor(const typename SearchTree::Node * node) { typename SearchTree::Node * newnode; if (node->left != NULL) { newnode = node->left; while(newnode->right != NULL) {newnode = newnode->right;} return newnode; } else { const typename SearchTree::Node * lastnode = node; newnode = node->parent; while(newnode != NULL) { if (newnode->right == lastnode) {return newnode;} lastnode = newnode; newnode = newnode->parent; } return newnode; } } template typename SearchTree::Node * SearchTree::_find_successor(const typename SearchTree::Node * node) { typename SearchTree::Node * newnode; if (node->right != NULL) { newnode = node->right; while(newnode->left != NULL) {newnode = newnode->left;} return newnode; } else { const typename SearchTree::Node * lastnode = node; newnode = node->parent; while(newnode != NULL) { if (newnode->left == lastnode) {return newnode;} lastnode = newnode; newnode = newnode->parent; } return newnode; } } template void SearchTree::print_elements() { typename SearchTree::Node * base_node = &(_nodes[0]); typename SearchTree::Node * node = base_node; int n = _nodes.size(); for(; node - base_node < n ; node++) { printf("%4d parent:%4d left:%4d right:%4d pred:%4d succ:%4d value:%10.6f\n",loc(node), loc(node->parent), loc(node->left), loc(node->right), loc(node->predecessor),loc(node->successor),node->value); } } template typename SearchTree::circulator SearchTree::somewhere() { return circulator(_top_node); } template typename SearchTree::const_circulator SearchTree::somewhere() const { return const_circulator(_top_node); } FJCORE_END_NAMESPACE #endif // __FJCORE_SEARCHTREE_HH__ #ifndef __FJCORE_MINHEAP__HH__ #define __FJCORE_MINHEAP__HH__ #include #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class MinHeap { public: MinHeap (const std::vector & values, unsigned int max_size) : _heap(max_size) {_initialise(values);}; MinHeap (const std::vector & values) : _heap(values.size()) {_initialise(values);}; inline unsigned int minloc() const { return (_heap[0].minloc) - &(_heap[0]);}; inline double minval() const {return _heap[0].minloc->value;}; inline double operator[](int i) const {return _heap[i].value;}; void remove(unsigned int loc) { update(loc,std::numeric_limits::max());}; void update(unsigned int, double); private: struct ValueLoc{ double value; ValueLoc * minloc; }; std::vector _heap; void _initialise(const std::vector & values); }; FJCORE_END_NAMESPACE #endif // __FJCORE_MINHEAP__HH__ #ifndef __FJCORE_CLOSESTPAIR2DBASE__HH__ #define __FJCORE_CLOSESTPAIR2DBASE__HH__ #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class Coord2D { public: double x, y; Coord2D() {}; Coord2D(double a, double b): x(a), y(b) {}; Coord2D operator-(const Coord2D & other) const { return Coord2D(x - other.x, y - other.y);}; Coord2D operator+(const Coord2D & other) const { return Coord2D(x + other.x, y + other.y);}; Coord2D operator*(double factor) const {return Coord2D(factor*x,factor*y);}; friend Coord2D operator*(double factor, const Coord2D & coord) { return Coord2D(factor*coord.x,factor*coord.y); } Coord2D operator/(double divisor) const { return Coord2D(x / divisor, y / divisor);}; friend double distance2(const Coord2D & a, const Coord2D & b) { double dx = a.x - b.x, dy = a.y-b.y; return dx*dx+dy*dy; }; double distance2(const Coord2D & b) const { double dx = x - b.x, dy = y-b.y; return dx*dx+dy*dy; }; }; class ClosestPair2DBase { public: virtual void closest_pair(unsigned int & ID1, unsigned int & ID2, double & distance2) const = 0; virtual void remove(unsigned int ID) = 0; virtual unsigned int insert(const Coord2D & position) = 0; virtual unsigned int replace(unsigned int ID1, unsigned int ID2, const Coord2D & position) { remove(ID1); remove(ID2); unsigned new_ID = insert(position); return(new_ID); }; virtual void replace_many(const std::vector & IDs_to_remove, const std::vector & new_positions, std::vector & new_IDs) { for(unsigned i = 0; i < IDs_to_remove.size(); i++) { remove(IDs_to_remove[i]);} new_IDs.resize(0); for(unsigned i = 0; i < new_positions.size(); i++) { new_IDs.push_back(insert(new_positions[i]));} } virtual unsigned int size() = 0; virtual ~ClosestPair2DBase() {}; }; FJCORE_END_NAMESPACE #endif // __FJCORE_CLOSESTPAIR2DBASE__HH__ #ifndef __FJCORE_CLOSESTPAIR2D__HH__ #define __FJCORE_CLOSESTPAIR2D__HH__ #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh class ClosestPair2D : public ClosestPair2DBase { public: ClosestPair2D(const std::vector & positions, const Coord2D & left_corner, const Coord2D & right_corner) { _initialize(positions, left_corner, right_corner, positions.size()); }; ClosestPair2D(const std::vector & positions, const Coord2D & left_corner, const Coord2D & right_corner, const unsigned int max_size) { _initialize(positions, left_corner, right_corner, max_size); }; void closest_pair(unsigned int & ID1, unsigned int & ID2, double & distance2) const; void remove(unsigned int ID); unsigned int insert(const Coord2D &); virtual unsigned int replace(unsigned int ID1, unsigned int ID2, const Coord2D & position); virtual void replace_many(const std::vector & IDs_to_remove, const std::vector & new_positions, std::vector & new_IDs); inline void print_tree_depths(std::ostream & outdev) const { outdev << _trees[0]->max_depth() << " " << _trees[1]->max_depth() << " " << _trees[2]->max_depth() << "\n"; }; unsigned int size(); private: void _initialize(const std::vector & positions, const Coord2D & left_corner, const Coord2D & right_corner, const unsigned int max_size); static const unsigned int _nshift = 3; class Point; // will be defined below template class triplet { public: inline const T & operator[](unsigned int i) const {return _contents[i];}; inline T & operator[](unsigned int i) {return _contents[i];}; private: T _contents[_nshift]; }; class Shuffle { public: unsigned int x, y; Point * point; bool operator<(const Shuffle &) const; void operator+=(unsigned int shift) {x += shift; y+= shift;}; }; typedef SearchTree Tree; typedef Tree::circulator circulator; typedef Tree::const_circulator const_circulator; triplet > _trees; std::auto_ptr _heap; std::vector _points; std::stack _available_points; std::vector _points_under_review; static const unsigned int _remove_heap_entry = 1; static const unsigned int _review_heap_entry = 2; static const unsigned int _review_neighbour = 4; void _add_label(Point * point, unsigned int review_flag); void _set_label(Point * point, unsigned int review_flag); void _deal_with_points_to_review(); void _remove_from_search_tree(Point * point_to_remove); void _insert_into_search_tree(Point * new_point); void _point2shuffle(Point & , Shuffle & , unsigned int shift); Coord2D _left_corner; double _range; int _ID(const Point *) const; triplet _shifts; // absolute shifts triplet _rel_shifts; // shifts relative to previous shift unsigned int _cp_search_range; }; class ClosestPair2D::Point { public: Coord2D coord; Point * neighbour; double neighbour_dist2; triplet circ; unsigned int review_flag; double distance2(const Point & other) const { return coord.distance2(other.coord); }; }; inline bool floor_ln2_less(unsigned x, unsigned y) { if (x>y) return false; return (x < (x^y)); // beware of operator precedence... } inline int ClosestPair2D::_ID(const Point * point) const { return point - &(_points[0]); } inline unsigned int ClosestPair2D::size() { return _points.size() - _available_points.size(); } FJCORE_END_NAMESPACE #endif // __FJCORE_CLOSESTPAIR2D__HH__ #include #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh const unsigned int huge_unsigned = 4294967295U; const unsigned int twopow31 = 2147483648U; using namespace std; void ClosestPair2D::_point2shuffle(Point & point, Shuffle & shuffle, unsigned int shift) { Coord2D renorm_point = (point.coord - _left_corner)/_range; assert(renorm_point.x >=0); assert(renorm_point.x <=1); assert(renorm_point.y >=0); assert(renorm_point.y <=1); shuffle.x = static_cast(twopow31 * renorm_point.x) + shift; shuffle.y = static_cast(twopow31 * renorm_point.y) + shift; shuffle.point = &point; } bool ClosestPair2D::Shuffle::operator<(const Shuffle & q) const { if (floor_ln2_less(x ^ q.x, y ^ q.y)) { return (y < q.y); } else { return (x < q.x); } } void ClosestPair2D::_initialize(const std::vector & positions, const Coord2D & left_corner, const Coord2D & right_corner, unsigned int max_size) { unsigned int n_positions = positions.size(); assert(max_size >= n_positions); _points.resize(max_size); for (unsigned int i = n_positions; i < max_size; i++) { _available_points.push(&(_points[i])); } _left_corner = left_corner; _range = max((right_corner.x - left_corner.x), (right_corner.y - left_corner.y)); vector shuffles(n_positions); for (unsigned int i = 0; i < n_positions; i++) { _points[i].coord = positions[i]; _points[i].neighbour_dist2 = numeric_limits::max(); _points[i].review_flag = 0; _point2shuffle(_points[i], shuffles[i], 0); } for (unsigned ishift = 0; ishift < _nshift; ishift++) { _shifts[ishift] = static_cast(((twopow31*1.0)*ishift)/_nshift); if (ishift == 0) {_rel_shifts[ishift] = 0;} else {_rel_shifts[ishift] = _shifts[ishift] - _shifts[ishift-1];} } _cp_search_range = 30; _points_under_review.reserve(_nshift * _cp_search_range); for (unsigned int ishift = 0; ishift < _nshift; ishift++) { if (ishift > 0) { unsigned rel_shift = _rel_shifts[ishift]; for (unsigned int i = 0; i < shuffles.size(); i++) { shuffles[i] += rel_shift; } } sort(shuffles.begin(), shuffles.end()); _trees[ishift] = auto_ptr(new Tree(shuffles, max_size)); circulator circ = _trees[ishift]->somewhere(), start=circ; unsigned int CP_range = min(_cp_search_range, n_positions-1); do { Point * this_point = circ->point; this_point->circ[ishift] = circ; circulator other = circ; for (unsigned i=0; i < CP_range; i++) { ++other; double dist2 = this_point->distance2(*other->point); if (dist2 < this_point->neighbour_dist2) { this_point->neighbour_dist2 = dist2; this_point->neighbour = other->point; } } } while (++circ != start); } vector mindists2(n_positions); for (unsigned int i = 0; i < n_positions; i++) { mindists2[i] = _points[i].neighbour_dist2;} _heap = auto_ptr(new MinHeap(mindists2, max_size)); } void ClosestPair2D::closest_pair(unsigned int & ID1, unsigned int & ID2, double & distance2) const { ID1 = _heap->minloc(); ID2 = _ID(_points[ID1].neighbour); distance2 = _points[ID1].neighbour_dist2; if (ID1 > ID2) std::swap(ID1,ID2); } inline void ClosestPair2D::_add_label(Point * point, unsigned int review_flag) { if (point->review_flag == 0) _points_under_review.push_back(point); point->review_flag |= review_flag; } inline void ClosestPair2D::_set_label(Point * point, unsigned int review_flag) { if (point->review_flag == 0) _points_under_review.push_back(point); point->review_flag = review_flag; } void ClosestPair2D::remove(unsigned int ID) { Point * point_to_remove = & (_points[ID]); _remove_from_search_tree(point_to_remove); _deal_with_points_to_review(); } void ClosestPair2D::_remove_from_search_tree(Point * point_to_remove) { _available_points.push(point_to_remove); _set_label(point_to_remove, _remove_heap_entry); unsigned int CP_range = min(_cp_search_range, size()-1); for (unsigned int ishift = 0; ishift < _nshift; ishift++) { circulator removed_circ = point_to_remove->circ[ishift]; circulator right_end = removed_circ.next(); _trees[ishift]->remove(removed_circ); circulator left_end = right_end, orig_right_end = right_end; for (unsigned int i = 0; i < CP_range; i++) {left_end--;} if (size()-1 < _cp_search_range) { left_end--; right_end--; } do { Point * left_point = left_end->point; if (left_point->neighbour == point_to_remove) { // we'll deal with it later... _add_label(left_point, _review_neighbour); } else { // check to see if right point has become its closest neighbour double dist2 = left_point->distance2(*right_end->point); if (dist2 < left_point->neighbour_dist2) { left_point->neighbour = right_end->point; left_point->neighbour_dist2 = dist2; // NB: (LESSER) REVIEW NEEDED HERE TOO... _add_label(left_point, _review_heap_entry); } } ++right_end; } while (++left_end != orig_right_end); } // ishift... } void ClosestPair2D::_deal_with_points_to_review() { unsigned int CP_range = min(_cp_search_range, size()-1); while(_points_under_review.size() > 0) { Point * this_point = _points_under_review.back(); _points_under_review.pop_back(); if (this_point->review_flag & _remove_heap_entry) { assert(!(this_point->review_flag ^ _remove_heap_entry)); _heap->remove(_ID(this_point)); } else { if (this_point->review_flag & _review_neighbour) { this_point->neighbour_dist2 = numeric_limits::max(); // among all three shifts for (unsigned int ishift = 0; ishift < _nshift; ishift++) { circulator other = this_point->circ[ishift]; // among points within CP_range for (unsigned i=0; i < CP_range; i++) { ++other; double dist2 = this_point->distance2(*other->point); if (dist2 < this_point->neighbour_dist2) { this_point->neighbour_dist2 = dist2; this_point->neighbour = other->point; } } } } _heap->update(_ID(this_point), this_point->neighbour_dist2); } this_point->review_flag = 0; } } unsigned int ClosestPair2D::insert(const Coord2D & new_coord) { assert(_available_points.size() > 0); Point * new_point = _available_points.top(); _available_points.pop(); new_point->coord = new_coord; _insert_into_search_tree(new_point); _deal_with_points_to_review(); return _ID(new_point); } unsigned int ClosestPair2D::replace(unsigned int ID1, unsigned int ID2, const Coord2D & position) { Point * point_to_remove = & (_points[ID1]); _remove_from_search_tree(point_to_remove); point_to_remove = & (_points[ID2]); _remove_from_search_tree(point_to_remove); Point * new_point = _available_points.top(); _available_points.pop(); new_point->coord = position; _insert_into_search_tree(new_point); _deal_with_points_to_review(); return _ID(new_point); } void ClosestPair2D::replace_many( const std::vector & IDs_to_remove, const std::vector & new_positions, std::vector & new_IDs) { for (unsigned int i = 0; i < IDs_to_remove.size(); i++) { _remove_from_search_tree(& (_points[IDs_to_remove[i]])); } new_IDs.resize(0); for (unsigned int i = 0; i < new_positions.size(); i++) { Point * new_point = _available_points.top(); _available_points.pop(); new_point->coord = new_positions[i]; _insert_into_search_tree(new_point); new_IDs.push_back(_ID(new_point)); } _deal_with_points_to_review(); } void ClosestPair2D::_insert_into_search_tree(Point * new_point) { _set_label(new_point, _review_heap_entry); new_point->neighbour_dist2 = numeric_limits::max(); unsigned int CP_range = min(_cp_search_range, size()-1); for (unsigned ishift = 0; ishift < _nshift; ishift++) { Shuffle new_shuffle; _point2shuffle(*new_point, new_shuffle, _shifts[ishift]); circulator new_circ = _trees[ishift]->insert(new_shuffle); new_point->circ[ishift] = new_circ; circulator right_edge = new_circ; right_edge++; circulator left_edge = new_circ; for (unsigned int i = 0; i < CP_range; i++) {left_edge--;} do { Point * left_point = left_edge->point; Point * right_point = right_edge->point; double new_dist2 = left_point->distance2(*new_point); if (new_dist2 < left_point->neighbour_dist2) { left_point->neighbour_dist2 = new_dist2; left_point->neighbour = new_point; _add_label(left_point, _review_heap_entry); } new_dist2 = new_point->distance2(*right_point); if (new_dist2 < new_point->neighbour_dist2) { new_point->neighbour_dist2 = new_dist2; new_point->neighbour = right_point; } if (left_point->neighbour == right_point) { _add_label(left_point, _review_neighbour); } right_edge++; } while (++left_edge != new_circ); } } FJCORE_END_NAMESPACE #include #include #include #include #include #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; std::ostream * ClusterSequence::_fastjet_banner_ostr = &cout; ClusterSequence::~ClusterSequence () { if (_structure_shared_ptr()){ ClusterSequenceStructure* csi = dynamic_cast(_structure_shared_ptr()); assert(csi != NULL); csi->set_associated_cs(NULL); if (_deletes_self_when_unused) { _structure_shared_ptr.set_count(_structure_shared_ptr.use_count() + _structure_use_count_after_construction); } } } void ClusterSequence::signal_imminent_self_deletion() const { assert(_deletes_self_when_unused); _deletes_self_when_unused = false; } void ClusterSequence::_initialise_and_run ( const JetDefinition & jet_def_in, const bool & writeout_combinations) { _decant_options(jet_def_in, writeout_combinations); _initialise_and_run_no_decant(); } void ClusterSequence::_initialise_and_run_no_decant () { _fill_initial_history(); if (n_particles() == 0) return; if (_jet_algorithm == plugin_algorithm) { _plugin_activated = true; _jet_def.plugin()->run_clustering( (*this) ); _plugin_activated = false; _update_structure_use_count(); return; } else if (_jet_algorithm == ee_kt_algorithm || _jet_algorithm == ee_genkt_algorithm) { _strategy = N2Plain; if (_jet_algorithm == ee_kt_algorithm) { assert(_Rparam > 2.0); _invR2 = 1.0; } else { if (_Rparam > pi) { // choose a value that ensures that back-to-back particles will // always recombine //_R2 = 4.0000000000001; _R2 = 2 * ( 3.0 + cos(_Rparam) ); } else { _R2 = 2 * ( 1.0 - cos(_Rparam) ); } _invR2 = 1.0/_R2; } _simple_N2_cluster_EEBriefJet(); return; } else if (_jet_algorithm == undefined_jet_algorithm) { throw Error("A ClusterSequence cannot be created with an uninitialised JetDefinition"); } if (_strategy == Best) { int N = _jets.size(); if (min(1.0,max(0.1,_Rparam)*3.3)*N <= 30) { _strategy = N2Plain; } else if (N > 6200/pow(_Rparam,2.0) && _jet_def.jet_algorithm() == cambridge_algorithm) { _strategy = NlnNCam; #ifndef __FJCORE_DROP_CGAL } else if ((N > 16000/pow(_Rparam,1.15) && _jet_def.jet_algorithm() != antikt_algorithm) || N > 35000/pow(_Rparam,1.15)) { _strategy = NlnN; #endif // __FJCORE_DROP_CGAL } else if (N <= 450) { _strategy = N2Tiled; } else { _strategy = N2MinHeapTiled; } } if (_Rparam >= twopi) { if ( _strategy == NlnN || _strategy == NlnN3pi || _strategy == NlnNCam || _strategy == NlnNCam2pi2R || _strategy == NlnNCam4pi) { #ifdef __FJCORE_DROP_CGAL _strategy = N2MinHeapTiled; #else _strategy = NlnN4pi; #endif } if (_jet_def.strategy() != Best && _strategy != _jet_def.strategy()) { ostringstream oss; oss << "Cluster strategy " << strategy_string(_jet_def.strategy()) << " automatically changed to " << strategy_string() << " because the former is not supported for R = " << _Rparam << " >= 2pi"; _changed_strategy_warning.warn(oss.str()); } } if (_strategy == N2Plain) { this->_simple_N2_cluster_BriefJet(); } else if (_strategy == N2Tiled) { this->_faster_tiled_N2_cluster(); } else if (_strategy == N2MinHeapTiled) { this->_minheap_faster_tiled_N2_cluster(); } else if (_strategy == NlnN) { this->_delaunay_cluster(); } else if (_strategy == NlnNCam) { this->_CP2DChan_cluster_2piMultD(); } else if (_strategy == NlnN3pi || _strategy == NlnN4pi ) { this->_delaunay_cluster(); } else if (_strategy == N3Dumb ) { this->_really_dumb_cluster(); } else if (_strategy == N2PoorTiled) { this->_tiled_N2_cluster(); } else if (_strategy == NlnNCam4pi) { this->_CP2DChan_cluster(); } else if (_strategy == NlnNCam2pi2R) { this->_CP2DChan_cluster_2pi2R(); } else { ostringstream err; err << "Unrecognised value for strategy: "<<_strategy; throw Error(err.str()); } } bool ClusterSequence::_first_time = true; int ClusterSequence::_n_exclusive_warnings = 0; string fastjet_version_string() { return "FastJet version "+string(fastjet_version)+" [fjcore]"; } void ClusterSequence::print_banner() { if (!_first_time) {return;} _first_time = false; ostream * ostr = _fastjet_banner_ostr; if (!ostr) return; (*ostr) << "#--------------------------------------------------------------------------\n"; (*ostr) << "# FastJet release " << fastjet_version << " [fjcore]" << endl; (*ostr) << "# M. Cacciari, G.P. Salam and G. Soyez \n"; (*ostr) << "# A software package for jet finding and analysis at colliders \n"; (*ostr) << "# http://fastjet.fr \n"; (*ostr) << "# \n"; (*ostr) << "# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package\n"; (*ostr) << "# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210]. \n"; (*ostr) << "# \n"; (*ostr) << "# FastJet is provided without warranty under the terms of the GNU GPLv2.\n"; (*ostr) << "# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code"; #ifndef __FJCORE_DROP_CGAL (*ostr) << ",\n# CGAL "; #else (*ostr) << "\n# "; #endif // __FJCORE_DROP_CGAL (*ostr) << "and 3rd party plugin jet algorithms. See COPYING file for details.\n"; (*ostr) << "#--------------------------------------------------------------------------\n"; ostr->flush(); } void ClusterSequence::_decant_options(const JetDefinition & jet_def_in, const bool & writeout_combinations) { _jet_def = jet_def_in; _writeout_combinations = writeout_combinations; _structure_shared_ptr.reset(new ClusterSequenceStructure(this)); _decant_options_partial(); } void ClusterSequence::_decant_options_partial() { print_banner(); _jet_algorithm = _jet_def.jet_algorithm(); _Rparam = _jet_def.R(); _R2 = _Rparam*_Rparam; _invR2 = 1.0/_R2; _strategy = _jet_def.strategy(); _plugin_activated = false; _update_structure_use_count(); // make sure it's correct already here } void ClusterSequence::_fill_initial_history () { _jets.reserve(_jets.size()*2); _history.reserve(_jets.size()*2); _Qtot = 0; for (int i = 0; i < static_cast(_jets.size()) ; i++) { history_element element; element.parent1 = InexistentParent; element.parent2 = InexistentParent; element.child = Invalid; element.jetp_index = i; element.dij = 0.0; element.max_dij_so_far = 0.0; _history.push_back(element); _jet_def.recombiner()->preprocess(_jets[i]); _jets[i].set_cluster_hist_index(i); _set_structure_shared_ptr(_jets[i]); _Qtot += _jets[i].E(); } _initial_n = _jets.size(); _deletes_self_when_unused = false; } string ClusterSequence::strategy_string (Strategy strategy_in) const { string strategy; switch(strategy_in) { case NlnN: strategy = "NlnN"; break; case NlnN3pi: strategy = "NlnN3pi"; break; case NlnN4pi: strategy = "NlnN4pi"; break; case N2Plain: strategy = "N2Plain"; break; case N2Tiled: strategy = "N2Tiled"; break; case N2MinHeapTiled: strategy = "N2MinHeapTiled"; break; case N2PoorTiled: strategy = "N2PoorTiled"; break; case N3Dumb: strategy = "N3Dumb"; break; case NlnNCam4pi: strategy = "NlnNCam4pi"; break; case NlnNCam2pi2R: strategy = "NlnNCam2pi2R"; break; case NlnNCam: strategy = "NlnNCam"; break; // 2piMultD case plugin_strategy: strategy = "plugin strategy"; break; default: strategy = "Unrecognized"; } return strategy; } double ClusterSequence::jet_scale_for_algorithm( const PseudoJet & jet) const { if (_jet_algorithm == kt_algorithm) {return jet.kt2();} else if (_jet_algorithm == cambridge_algorithm) {return 1.0;} else if (_jet_algorithm == antikt_algorithm) { double kt2=jet.kt2(); return kt2 > 1e-300 ? 1.0/kt2 : 1e300; } else if (_jet_algorithm == genkt_algorithm) { double kt2 = jet.kt2(); double p = jet_def().extra_param(); if (p <= 0 && kt2 < 1e-300) kt2 = 1e-300; // dodgy safety check return pow(kt2, p); } else if (_jet_algorithm == cambridge_for_passive_algorithm) { double kt2 = jet.kt2(); double lim = _jet_def.extra_param(); if (kt2 < lim*lim && kt2 != 0.0) { return 1.0/kt2; } else {return 1.0;} } else {throw Error("Unrecognised jet algorithm");} } void ClusterSequence::transfer_from_sequence(const ClusterSequence & from_seq, const FunctionOfPseudoJet * action_on_jets){ if (will_delete_self_when_unused()) throw(Error("cannot use CS::transfer_from_sequence after a call to delete_self_when_unused()")); _jet_def = from_seq._jet_def ; _writeout_combinations = from_seq._writeout_combinations ; _initial_n = from_seq._initial_n ; _Rparam = from_seq._Rparam ; _R2 = from_seq._R2 ; _invR2 = from_seq._invR2 ; _strategy = from_seq._strategy ; _jet_algorithm = from_seq._jet_algorithm ; _plugin_activated = from_seq._plugin_activated ; if (action_on_jets) _jets = (*action_on_jets)(from_seq._jets); else _jets = from_seq._jets; _history = from_seq._history; _extras = from_seq._extras; if (_structure_shared_ptr()) { if (_deletes_self_when_unused) throw Error("transfer_from_sequence cannot be used for a cluster sequence that deletes self when unused"); ClusterSequenceStructure* csi = dynamic_cast(_structure_shared_ptr()); assert(csi != NULL); csi->set_associated_cs(NULL); } _structure_shared_ptr.reset(new ClusterSequenceStructure(this)); _update_structure_use_count(); for (unsigned int i=0; i<_jets.size(); i++){ _jets[i].set_cluster_hist_index(from_seq._jets[i].cluster_hist_index()); _set_structure_shared_ptr(_jets[i]); } } void ClusterSequence::plugin_record_ij_recombination( int jet_i, int jet_j, double dij, const PseudoJet & newjet, int & newjet_k) { plugin_record_ij_recombination(jet_i, jet_j, dij, newjet_k); int tmp_index = _jets[newjet_k].cluster_hist_index(); _jets[newjet_k] = newjet; _jets[newjet_k].set_cluster_hist_index(tmp_index); _set_structure_shared_ptr(_jets[newjet_k]); } vector ClusterSequence::inclusive_jets (const double & ptmin) const{ double dcut = ptmin*ptmin; int i = _history.size() - 1; // last jet vector jets_local; if (_jet_algorithm == kt_algorithm) { while (i >= 0) { if (_history[i].max_dij_so_far < dcut) {break;} if (_history[i].parent2 == BeamJet && _history[i].dij >= dcut) { // for beam jets int parent1 = _history[i].parent1; jets_local.push_back(_jets[_history[parent1].jetp_index]);} i--; } } else if (_jet_algorithm == cambridge_algorithm) { while (i >= 0) { if (_history[i].parent2 != BeamJet) {break;} int parent1 = _history[i].parent1; const PseudoJet & jet = _jets[_history[parent1].jetp_index]; if (jet.perp2() >= dcut) {jets_local.push_back(jet);} i--; } } else if (_jet_algorithm == plugin_algorithm || _jet_algorithm == ee_kt_algorithm || _jet_algorithm == antikt_algorithm || _jet_algorithm == genkt_algorithm || _jet_algorithm == ee_genkt_algorithm || _jet_algorithm == cambridge_for_passive_algorithm) { while (i >= 0) { if (_history[i].parent2 == BeamJet) { int parent1 = _history[i].parent1; const PseudoJet & jet = _jets[_history[parent1].jetp_index]; if (jet.perp2() >= dcut) {jets_local.push_back(jet);} } i--; } } else {throw Error("cs::inclusive_jets(...): Unrecognized jet algorithm");} return jets_local; } int ClusterSequence::n_exclusive_jets (const double & dcut) const { int i = _history.size() - 1; // last jet while (i >= 0) { if (_history[i].max_dij_so_far <= dcut) {break;} i--; } int stop_point = i + 1; int njets = 2*_initial_n - stop_point; return njets; } vector ClusterSequence::exclusive_jets (const double & dcut) const { int njets = n_exclusive_jets(dcut); return exclusive_jets(njets); } vector ClusterSequence::exclusive_jets (const int & njets) const { if (njets > _initial_n) { ostringstream err; err << "Requested " << njets << " exclusive jets, but there were only " << _initial_n << " particles in the event"; throw Error(err.str()); } return exclusive_jets_up_to(njets); } vector ClusterSequence::exclusive_jets_up_to (const int & njets) const { if (( _jet_def.jet_algorithm() != kt_algorithm) && ( _jet_def.jet_algorithm() != cambridge_algorithm) && ( _jet_def.jet_algorithm() != ee_kt_algorithm) && (((_jet_def.jet_algorithm() != genkt_algorithm) && (_jet_def.jet_algorithm() != ee_genkt_algorithm)) || (_jet_def.extra_param() <0)) && ((_jet_def.jet_algorithm() != plugin_algorithm) || (!_jet_def.plugin()->exclusive_sequence_meaningful())) && (_n_exclusive_warnings < 5)) { _n_exclusive_warnings++; cerr << "FastJet WARNING: dcut and exclusive jets for jet-finders other than kt should be interpreted with care." << endl; } int stop_point = 2*_initial_n - njets; if (stop_point < _initial_n) stop_point = _initial_n; if (2*_initial_n != static_cast(_history.size())) { ostringstream err; err << "2*_initial_n != _history.size() -- this endangers internal assumptions!\n"; throw Error(err.str()); } vector jets_local; for (unsigned int i = stop_point; i < _history.size(); i++) { int parent1 = _history[i].parent1; if (parent1 < stop_point) { jets_local.push_back(_jets[_history[parent1].jetp_index]); } int parent2 = _history[i].parent2; if (parent2 < stop_point && parent2 > 0) { jets_local.push_back(_jets[_history[parent2].jetp_index]); } } if (int(jets_local.size()) != min(_initial_n, njets)) { ostringstream err; err << "ClusterSequence::exclusive_jets: size of returned vector (" <= 0); if (njets >= _initial_n) {return 0.0;} return _history[2*_initial_n-njets-1].dij; } double ClusterSequence::exclusive_dmerge_max (const int & njets) const { assert(njets >= 0); if (njets >= _initial_n) {return 0.0;} return _history[2*_initial_n-njets-1].max_dij_so_far; } std::vector ClusterSequence::exclusive_subjets (const PseudoJet & jet, const double & dcut) const { set subhist; get_subhist_set(subhist, jet, dcut, 0); vector subjets; subjets.reserve(subhist.size()); for (set::iterator elem = subhist.begin(); elem != subhist.end(); elem++) { subjets.push_back(_jets[(*elem)->jetp_index]); } return subjets; } int ClusterSequence::n_exclusive_subjets(const PseudoJet & jet, const double & dcut) const { set subhist; get_subhist_set(subhist, jet, dcut, 0); return subhist.size(); } std::vector ClusterSequence::exclusive_subjets (const PseudoJet & jet, int nsub) const { vector subjets = exclusive_subjets_up_to(jet, nsub); if (int(subjets.size()) < nsub) { ostringstream err; err << "Requested " << nsub << " exclusive subjets, but there were only " << subjets.size() << " particles in the jet"; throw Error(err.str()); } return subjets; } std::vector ClusterSequence::exclusive_subjets_up_to (const PseudoJet & jet, int nsub) const { set subhist; vector subjets; if (nsub < 0) throw Error("Requested a negative number of subjets. This is nonsensical."); if (nsub == 0) return subjets; get_subhist_set(subhist, jet, -1.0, nsub); subjets.reserve(subhist.size()); for (set::iterator elem = subhist.begin(); elem != subhist.end(); elem++) { subjets.push_back(_jets[(*elem)->jetp_index]); } return subjets; } double ClusterSequence::exclusive_subdmerge(const PseudoJet & jet, int nsub) const { set subhist; get_subhist_set(subhist, jet, -1.0, nsub); set::iterator highest = subhist.end(); highest--; return (*highest)->dij; } double ClusterSequence::exclusive_subdmerge_max(const PseudoJet & jet, int nsub) const { set subhist; get_subhist_set(subhist, jet, -1.0, nsub); set::iterator highest = subhist.end(); highest--; return (*highest)->max_dij_so_far; } void ClusterSequence::get_subhist_set(set & subhist, const PseudoJet & jet, double dcut, int maxjet) const { assert(contains(jet)); subhist.clear(); subhist.insert(&(_history[jet.cluster_hist_index()])); int njet = 1; while (true) { set::iterator highest = subhist.end(); assert (highest != subhist.begin()); highest--; const history_element* elem = *highest; if (njet == maxjet) break; if (elem->parent1 < 0) break; if (elem->max_dij_so_far <= dcut) break; subhist.erase(highest); subhist.insert(&(_history[elem->parent1])); subhist.insert(&(_history[elem->parent2])); njet++; } } bool ClusterSequence::object_in_jet(const PseudoJet & object, const PseudoJet & jet) const { assert(contains(object) && contains(jet)); const PseudoJet * this_object = &object; const PseudoJet * childp; while(true) { if (this_object->cluster_hist_index() == jet.cluster_hist_index()) { return true; } else if (has_child(*this_object, childp)) { this_object = childp; } else { return false; } } } bool ClusterSequence::has_parents(const PseudoJet & jet, PseudoJet & parent1, PseudoJet & parent2) const { const history_element & hist = _history[jet.cluster_hist_index()]; assert ((hist.parent1 >= 0 && hist.parent2 >= 0) || (hist.parent1 < 0 && hist.parent2 < 0)); if (hist.parent1 < 0) { parent1 = PseudoJet(0.0,0.0,0.0,0.0); parent2 = parent1; return false; } else { parent1 = _jets[_history[hist.parent1].jetp_index]; parent2 = _jets[_history[hist.parent2].jetp_index]; if (parent1.perp2() < parent2.perp2()) std::swap(parent1,parent2); return true; } } bool ClusterSequence::has_child(const PseudoJet & jet, PseudoJet & child) const { const PseudoJet * childp; bool res = has_child(jet, childp); if (res) { child = *childp; return true; } else { child = PseudoJet(0.0,0.0,0.0,0.0); return false; } } bool ClusterSequence::has_child(const PseudoJet & jet, const PseudoJet * & childp) const { const history_element & hist = _history[jet.cluster_hist_index()]; if (hist.child >= 0 && _history[hist.child].jetp_index >= 0) { childp = &(_jets[_history[hist.child].jetp_index]); return true; } else { childp = NULL; return false; } } bool ClusterSequence::has_partner(const PseudoJet & jet, PseudoJet & partner) const { const history_element & hist = _history[jet.cluster_hist_index()]; if (hist.child >= 0 && _history[hist.child].parent2 >= 0) { const history_element & child_hist = _history[hist.child]; if (child_hist.parent1 == jet.cluster_hist_index()) { partner = _jets[_history[child_hist.parent2].jetp_index]; } else { partner = _jets[_history[child_hist.parent1].jetp_index]; } return true; } else { partner = PseudoJet(0.0,0.0,0.0,0.0); return false; } } vector ClusterSequence::constituents (const PseudoJet & jet) const { vector subjets; add_constituents(jet, subjets); return subjets; } void ClusterSequence::print_jets_for_root(const std::vector & jets_in, ostream & ostr) const { for (unsigned i = 0; i < jets_in.size(); i++) { ostr << i << " " << jets_in[i].px() << " " << jets_in[i].py() << " " << jets_in[i].pz() << " " << jets_in[i].E() << endl; vector cst = constituents(jets_in[i]); for (unsigned j = 0; j < cst.size() ; j++) { ostr << " " << j << " " << cst[j].rap() << " " << cst[j].phi() << " " << cst[j].perp() << endl; } ostr << "#END" << endl; } } void ClusterSequence::print_jets_for_root(const std::vector & jets_in, const std::string & filename, const std::string & comment ) const { std::ofstream ostr(filename.c_str()); if (comment != "") ostr << "# " << comment << endl; print_jets_for_root(jets_in, ostr); } vector ClusterSequence::particle_jet_indices( const vector & jets_in) const { vector indices(n_particles()); for (unsigned ipart = 0; ipart < n_particles(); ipart++) indices[ipart] = -1; for (unsigned ijet = 0; ijet < jets_in.size(); ijet++) { vector jet_constituents(constituents(jets_in[ijet])); for (unsigned ip = 0; ip < jet_constituents.size(); ip++) { unsigned iclust = jet_constituents[ip].cluster_hist_index(); unsigned ipart = history()[iclust].jetp_index; indices[ipart] = ijet; } } return indices; } void ClusterSequence::add_constituents ( const PseudoJet & jet, vector & subjet_vector) const { int i = jet.cluster_hist_index(); int parent1 = _history[i].parent1; int parent2 = _history[i].parent2; if (parent1 == InexistentParent) { subjet_vector.push_back(_jets[i]); return; } add_constituents(_jets[_history[parent1].jetp_index], subjet_vector); if (parent2 != BeamJet) { add_constituents(_jets[_history[parent2].jetp_index], subjet_vector); } } void ClusterSequence::_add_step_to_history ( const int & step_number, const int & parent1, const int & parent2, const int & jetp_index, const double & dij) { history_element element; element.parent1 = parent1; element.parent2 = parent2; element.jetp_index = jetp_index; element.child = Invalid; element.dij = dij; element.max_dij_so_far = max(dij,_history[_history.size()-1].max_dij_so_far); _history.push_back(element); int local_step = _history.size()-1; assert(local_step == step_number); assert(parent1 >= 0); _history[parent1].child = local_step; if (parent2 >= 0) {_history[parent2].child = local_step;} if (jetp_index != Invalid) { assert(jetp_index >= 0); _jets[jetp_index].set_cluster_hist_index(local_step); _set_structure_shared_ptr(_jets[jetp_index]); } if (_writeout_combinations) { cout << local_step << ": " << parent1 << " with " << parent2 << "; y = "<< dij< ClusterSequence::unique_history_order() const { valarray lowest_constituent(_history.size()); int hist_n = _history.size(); lowest_constituent = hist_n; // give it a large number for (int i = 0; i < hist_n; i++) { lowest_constituent[i] = min(lowest_constituent[i],i); if (_history[i].child > 0) lowest_constituent[_history[i].child] = min(lowest_constituent[_history[i].child],lowest_constituent[i]); } valarray extracted(_history.size()); extracted = false; vector unique_tree; unique_tree.reserve(_history.size()); for (unsigned i = 0; i < n_particles(); i++) { if (!extracted[i]) { unique_tree.push_back(i); extracted[i] = true; _extract_tree_children(i, extracted, lowest_constituent, unique_tree); } } return unique_tree; } void ClusterSequence::_extract_tree_children( int position, valarray & extracted, const valarray & lowest_constituent, vector & unique_tree) const { if (!extracted[position]) { _extract_tree_parents(position,extracted,lowest_constituent,unique_tree); } int child = _history[position].child; if (child >= 0) _extract_tree_children(child,extracted,lowest_constituent,unique_tree); } vector ClusterSequence::unclustered_particles() const { vector unclustered; for (unsigned i = 0; i < n_particles() ; i++) { if (_history[i].child == Invalid) unclustered.push_back(_jets[_history[i].jetp_index]); } return unclustered; } vector ClusterSequence::childless_pseudojets() const { vector unclustered; for (unsigned i = 0; i < _history.size() ; i++) { if ((_history[i].child == Invalid) && (_history[i].parent2 != BeamJet)) unclustered.push_back(_jets[_history[i].jetp_index]); } return unclustered; } bool ClusterSequence::contains(const PseudoJet & jet) const { return jet.cluster_hist_index() >= 0 && jet.cluster_hist_index() < int(_history.size()) && jet.has_valid_cluster_sequence() && jet.associated_cluster_sequence() == this; } void ClusterSequence::_extract_tree_parents( int position, valarray & extracted, const valarray & lowest_constituent, vector & unique_tree) const { if (!extracted[position]) { int parent1 = _history[position].parent1; int parent2 = _history[position].parent2; if (parent1 >= 0 && parent2 >= 0) { if (lowest_constituent[parent1] > lowest_constituent[parent2]) std::swap(parent1, parent2); } if (parent1 >= 0 && !extracted[parent1]) _extract_tree_parents(parent1,extracted,lowest_constituent,unique_tree); if (parent2 >= 0 && !extracted[parent2]) _extract_tree_parents(parent2,extracted,lowest_constituent,unique_tree); unique_tree.push_back(position); extracted[position] = true; } } void ClusterSequence::_do_ij_recombination_step( const int & jet_i, const int & jet_j, const double & dij, int & newjet_k) { PseudoJet newjet(false); _jet_def.recombiner()->recombine(_jets[jet_i], _jets[jet_j], newjet); _jets.push_back(newjet); newjet_k = _jets.size()-1; int newstep_k = _history.size(); _jets[newjet_k].set_cluster_hist_index(newstep_k); int hist_i = _jets[jet_i].cluster_hist_index(); int hist_j = _jets[jet_j].cluster_hist_index(); _add_step_to_history(newstep_k, min(hist_i, hist_j), max(hist_i,hist_j), newjet_k, dij); } void ClusterSequence::_do_iB_recombination_step( const int & jet_i, const double & diB) { int newstep_k = _history.size(); _add_step_to_history(newstep_k,_jets[jet_i].cluster_hist_index(),BeamJet, Invalid, diB); } LimitedWarning ClusterSequence::_changed_strategy_warning; void ClusterSequence::_set_structure_shared_ptr(PseudoJet & j) { j.set_structure_shared_ptr(_structure_shared_ptr); _update_structure_use_count(); } void ClusterSequence::_update_structure_use_count() { _structure_use_count_after_construction = _structure_shared_ptr.use_count(); } void ClusterSequence::delete_self_when_unused() { int new_count = _structure_shared_ptr.use_count() - _structure_use_count_after_construction; if (new_count <= 0) { throw Error("delete_self_when_unused may only be called if at least one object outside the CS (e.g. a jet) is already associated with the CS"); } _structure_shared_ptr.set_count(new_count); _deletes_self_when_unused = true; } FJCORE_END_NAMESPACE #include #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; namespace Private { class MirrorInfo{ public: int orig, mirror; MirrorInfo(int a, int b) : orig(a), mirror(b) {}; MirrorInfo() {}; }; bool make_mirror(Coord2D & point, double Dlim) { if (point.y < Dlim) {point.y += twopi; return true;} if (twopi-point.y < Dlim) {point.y -= twopi; return true;} return false; } } using namespace Private; void ClusterSequence::_CP2DChan_limited_cluster (double Dlim) { unsigned int n = _initial_n; vector coordIDs(2*n); // coord IDs of a given jetID vector jetIDs(2*n); // jet ID for a given coord ID vector coords(2*n); // our coordinates (and copies) double Dlim4mirror = min(Dlim,pi); double minrap = numeric_limits::max(); double maxrap = -minrap; int coord_index = -1; int n_active = 0; for (unsigned jet_i = 0; jet_i < _jets.size(); jet_i++) { if (_history[_jets[jet_i].cluster_hist_index()].child != Invalid || (_jets[jet_i].E() == abs(_jets[jet_i].pz()) && _jets[jet_i].perp2() == 0.0) ) {continue;} n_active++; coordIDs[jet_i].orig = ++coord_index; coords[coord_index] = Coord2D(_jets[jet_i].rap(), _jets[jet_i].phi_02pi()); jetIDs[coord_index] = jet_i; minrap = min(coords[coord_index].x,minrap); maxrap = max(coords[coord_index].x,maxrap); Coord2D mirror_point(coords[coord_index]); if (make_mirror(mirror_point, Dlim4mirror)) { coordIDs[jet_i].mirror = ++coord_index; coords[coord_index] = mirror_point; jetIDs[coord_index] = jet_i; } else { coordIDs[jet_i].mirror = Invalid; } } coords.resize(coord_index+1); Coord2D left_edge(minrap-1.0, -3.15); // a security margin below -pi Coord2D right_edge(maxrap+1.0, 9.45); // a security margin above 3*pi ClosestPair2D cp(coords, left_edge, right_edge); vector new_points(2); vector cIDs_to_remove(4); vector new_cIDs(2); do { unsigned int cID1, cID2; double distance2; cp.closest_pair(cID1,cID2,distance2); if (distance2 > Dlim*Dlim) {break;} distance2 *= _invR2; int jet_i = jetIDs[cID1]; int jet_j = jetIDs[cID2]; assert (jet_i != jet_j); // to catch issue of recombining with mirror point int newjet_k; _do_ij_recombination_step(jet_i, jet_j, distance2, newjet_k); if (--n_active == 1) {break;} cIDs_to_remove.resize(0); cIDs_to_remove.push_back(coordIDs[jet_i].orig); cIDs_to_remove.push_back(coordIDs[jet_j].orig); if (coordIDs[jet_i].mirror != Invalid) cIDs_to_remove.push_back(coordIDs[jet_i].mirror); if (coordIDs[jet_j].mirror != Invalid) cIDs_to_remove.push_back(coordIDs[jet_j].mirror); Coord2D new_point(_jets[newjet_k].rap(),_jets[newjet_k].phi_02pi()); new_points.resize(0); new_points.push_back(new_point); if (make_mirror(new_point, Dlim4mirror)) new_points.push_back(new_point); //< same warning as before concerning the mirroring cp.replace_many(cIDs_to_remove, new_points, new_cIDs); coordIDs[newjet_k].orig = new_cIDs[0]; jetIDs[new_cIDs[0]] = newjet_k; if (new_cIDs.size() == 2) { coordIDs[newjet_k].mirror = new_cIDs[1]; jetIDs[new_cIDs[1]] = newjet_k; } else {coordIDs[newjet_k].mirror = Invalid;} } while(true); } void ClusterSequence::_CP2DChan_cluster_2pi2R () { if (_jet_algorithm != cambridge_algorithm) throw Error("CP2DChan clustering method called for a jet-finder that is not the cambridge algorithm"); _CP2DChan_limited_cluster(_Rparam); _do_Cambridge_inclusive_jets(); } void ClusterSequence::_CP2DChan_cluster_2piMultD () { if (_Rparam >= 0.39) { _CP2DChan_limited_cluster(min(_Rparam/2,0.3)); } _CP2DChan_cluster_2pi2R (); } void ClusterSequence::_CP2DChan_cluster () { if (_jet_algorithm != cambridge_algorithm) throw Error("_CP2DChan_cluster called for a jet-finder that is not the cambridge algorithm"); unsigned int n = _jets.size(); vector coordIDs(2*n); // link from original to mirror indices vector jetIDs(2*n); // link from mirror to original indices vector coords(2*n); // our coordinates (and copies) double minrap = numeric_limits::max(); double maxrap = -minrap; int coord_index = 0; for (unsigned i = 0; i < n; i++) { if (_jets[i].E() == abs(_jets[i].pz()) && _jets[i].perp2() == 0.0) { coordIDs[i] = MirrorInfo(BeamJet,BeamJet); } else { coordIDs[i].orig = coord_index; coordIDs[i].mirror = coord_index+1; coords[coord_index] = Coord2D(_jets[i].rap(), _jets[i].phi_02pi()); coords[coord_index+1] = Coord2D(_jets[i].rap(), _jets[i].phi_02pi()+twopi); jetIDs[coord_index] = i; jetIDs[coord_index+1] = i; minrap = min(coords[coord_index].x,minrap); maxrap = max(coords[coord_index].x,maxrap); coord_index += 2; } } for (unsigned i = n; i < 2*n; i++) {coordIDs[i].orig = Invalid;} coords.resize(coord_index); Coord2D left_edge(minrap-1.0, 0.0); Coord2D right_edge(maxrap+1.0, 2*twopi); ClosestPair2D cp(coords, left_edge, right_edge); vector new_points(2); vector cIDs_to_remove(4); vector new_cIDs(2); do { unsigned int cID1, cID2; double distance2; cp.closest_pair(cID1,cID2,distance2); distance2 *= _invR2; if (distance2 > 1.0) {break;} int jet_i = jetIDs[cID1]; int jet_j = jetIDs[cID2]; assert (jet_i != jet_j); // to catch issue of recombining with mirror point int newjet_k; _do_ij_recombination_step(jet_i, jet_j, distance2, newjet_k); cIDs_to_remove[0] = coordIDs[jet_i].orig; cIDs_to_remove[1] = coordIDs[jet_i].mirror; cIDs_to_remove[2] = coordIDs[jet_j].orig; cIDs_to_remove[3] = coordIDs[jet_j].mirror; new_points[0] = Coord2D(_jets[newjet_k].rap(),_jets[newjet_k].phi_02pi()); new_points[1] = Coord2D(_jets[newjet_k].rap(),_jets[newjet_k].phi_02pi()+twopi); new_cIDs[0] = cp.replace(cIDs_to_remove[0], cIDs_to_remove[2], new_points[0]); new_cIDs[1] = cp.replace(cIDs_to_remove[1], cIDs_to_remove[3], new_points[1]); coordIDs[jet_i].orig = Invalid; coordIDs[jet_j].orig = Invalid; coordIDs[newjet_k] = MirrorInfo(new_cIDs[0], new_cIDs[1]); jetIDs[new_cIDs[0]] = newjet_k; jetIDs[new_cIDs[1]] = newjet_k; n--; if (n == 1) {break;} } while(true); _do_Cambridge_inclusive_jets(); } void ClusterSequence::_do_Cambridge_inclusive_jets () { unsigned int n = _history.size(); for (unsigned int hist_i = 0; hist_i < n; hist_i++) { if (_history[hist_i].child == Invalid) { _do_iB_recombination_step(_history[hist_i].jetp_index, 1.0); } } } FJCORE_END_NAMESPACE #include #include #include #include #include #include #ifndef __FJCORE_DROP_CGAL // in case we do not have the code for CGAL #include "fastjet/internal/Dnn4piCylinder.hh" #include "fastjet/internal/Dnn3piCylinder.hh" #include "fastjet/internal/Dnn2piCylinder.hh" #endif // __FJCORE_DROP_CGAL FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; void ClusterSequence::_delaunay_cluster () { int n = _jets.size(); vector points(n); // recall EtaPhi is just a typedef'd pair for (int i = 0; i < n; i++) { points[i] = EtaPhi(_jets[i].rap(),_jets[i].phi_02pi()); points[i].sanitize(); // make sure things are in the right range } auto_ptr DNN; #ifndef __FJCORE_DROP_CGAL // strategy = NlnN* are not supported if we drop CGAL... bool verbose = false; bool ignore_nearest_is_mirror = (_Rparam < twopi); if (_strategy == NlnN4pi) { DNN.reset(new Dnn4piCylinder(points,verbose)); } else if (_strategy == NlnN3pi) { DNN.reset(new Dnn3piCylinder(points,ignore_nearest_is_mirror,verbose)); } else if (_strategy == NlnN) { DNN.reset(new Dnn2piCylinder(points,ignore_nearest_is_mirror,verbose)); } else #else if (_strategy == NlnN4pi || _strategy == NlnN3pi || _strategy == NlnN) { ostringstream err; err << "ERROR: Requested strategy "<first; SmallestDijPair = DijMap.begin()->second; jet_i = SmallestDijPair.first; jet_j = SmallestDijPair.second; DijMap.erase(DijMap.begin()); recombine_with_beam = (jet_j == BeamJet); if (!recombine_with_beam) {Valid2 = DNN->Valid(jet_j);} else {Valid2 = true;} } while ( !DNN->Valid(jet_i) || !Valid2); if (! recombine_with_beam) { int nn; // will be index of new jet _do_ij_recombination_step(jet_i, jet_j, SmallestDij, nn); EtaPhi newpoint(_jets[nn].rap(), _jets[nn].phi_02pi()); newpoint.sanitize(); // make sure it is in correct range points.push_back(newpoint); } else { _do_iB_recombination_step(jet_i, SmallestDij); } if (i == n-1) {break;} vector updated_neighbours; if (! recombine_with_beam) { int point3; DNN->RemoveCombinedAddCombination(jet_i, jet_j, points[points.size()-1], point3, updated_neighbours); if (static_cast (point3) != points.size()-1) { throw Error("INTERNAL ERROR: point3 != points.size()-1");} } else { DNN->RemovePoint(jet_i, updated_neighbours); } vector::iterator it = updated_neighbours.begin(); for (; it != updated_neighbours.end(); ++it) { int ii = *it; _add_ktdistance_to_map(ii, DijMap, DNN.get()); } } // end clustering loop } void ClusterSequence::_add_ktdistance_to_map( const int & ii, DistMap & DijMap, const DynamicNearestNeighbours * DNN) { double yiB = jet_scale_for_algorithm(_jets[ii]); if (yiB == 0.0) { DijMap.insert(DijEntry(yiB, TwoVertices(ii,-1))); } else { double DeltaR2 = DNN->NearestNeighbourDistance(ii) * _invR2; if (DeltaR2 > 1.0) { DijMap.insert(DijEntry(yiB, TwoVertices(ii,-1))); } else { double kt2i = jet_scale_for_algorithm(_jets[ii]); int jj = DNN->NearestNeighbourIndex(ii); if (kt2i <= jet_scale_for_algorithm(_jets[jj])) { double dij = DeltaR2 * kt2i; DijMap.insert(DijEntry(dij, TwoVertices(ii,jj))); } } } } FJCORE_END_NAMESPACE #include #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; void ClusterSequence::_really_dumb_cluster () { vector jetsp(_jets.size()); vector indices(_jets.size()); for (size_t i = 0; i<_jets.size(); i++) { jetsp[i] = & _jets[i]; indices[i] = i; } for (int n = jetsp.size(); n > 0; n--) { int ii, jj; double ymin = jet_scale_for_algorithm(*(jetsp[0])); ii = 0; jj = -2; for (int i = 0; i < n; i++) { double yiB = jet_scale_for_algorithm(*(jetsp[i])); if (yiB < ymin) { ymin = yiB; ii = i; jj = -2;} } for (int i = 0; i < n-1; i++) { for (int j = i+1; j < n; j++) { //double y = jetsp[i]->kt_distance(*jetsp[j])*_invR2; double y = min(jet_scale_for_algorithm(*(jetsp[i])), jet_scale_for_algorithm(*(jetsp[j]))) * jetsp[i]->plain_distance(*jetsp[j])*_invR2; if (y < ymin) {ymin = y; ii = i; jj = j;} } } int newn = 2*jetsp.size() - n; if (jj >= 0) { int nn; // new jet index _do_ij_recombination_step(jetsp[ii]-&_jets[0], jetsp[jj]-&_jets[0], ymin, nn); jetsp[ii] = &_jets[nn]; jetsp[jj] = jetsp[n-1]; indices[ii] = newn; indices[jj] = indices[n-1]; } else { _do_iB_recombination_step(jetsp[ii]-&_jets[0], ymin); jetsp[ii] = jetsp[n-1]; indices[ii] = indices[n-1]; } } } FJCORE_END_NAMESPACE #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; template<> inline void ClusterSequence::_bj_set_jetinfo( EEBriefJet * const jetA, const int _jets_index) const { double E = _jets[_jets_index].E(); double scale = E*E; // the default energy scale for the kt alg double p = jet_def().extra_param(); // in case we're ee_genkt switch (_jet_algorithm) { case ee_kt_algorithm: assert(_Rparam > 2.0); // force this to be true! [not best place, but works] break; case ee_genkt_algorithm: if (p <= 0 && scale < 1e-300) scale = 1e-300; // same dodgy safety as genkt scale = pow(scale,p); break; default: throw Error("Unrecognised jet algorithm"); } jetA->kt2 = scale; // "kt2" might one day be renamed as "scale" or some such double norm = _jets[_jets_index].modp2(); if (norm > 0) { norm = 1.0/sqrt(norm); jetA->nx = norm * _jets[_jets_index].px(); jetA->ny = norm * _jets[_jets_index].py(); jetA->nz = norm * _jets[_jets_index].pz(); } else { jetA->nx = 0.0; jetA->ny = 0.0; jetA->nz = 1.0; } jetA->_jets_index = _jets_index; jetA->NN_dist = _R2; jetA->NN = NULL; } template<> double ClusterSequence::_bj_dist( const EEBriefJet * const jeta, const EEBriefJet * const jetb) const { double dist = 1.0 - jeta->nx*jetb->nx - jeta->ny*jetb->ny - jeta->nz*jetb->nz; dist *= 2; // distance is _2_*min(Ei^2,Ej^2)*(1-cos theta) return dist; } void ClusterSequence::_simple_N2_cluster_BriefJet() { _simple_N2_cluster(); } void ClusterSequence::_simple_N2_cluster_EEBriefJet() { _simple_N2_cluster(); } FJCORE_END_NAMESPACE #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; ClusterSequenceStructure::~ClusterSequenceStructure(){ if (_associated_cs != NULL && _associated_cs->will_delete_self_when_unused()) { _associated_cs->signal_imminent_self_deletion(); delete _associated_cs; } } bool ClusterSequenceStructure::has_valid_cluster_sequence() const{ return (_associated_cs != NULL); } const ClusterSequence* ClusterSequenceStructure::associated_cluster_sequence() const{ return _associated_cs; } const ClusterSequence * ClusterSequenceStructure::validated_cs() const { if (!_associated_cs) throw Error("you requested information about the internal structure of a jet, but its associated ClusterSequence has gone out of scope."); return _associated_cs; } bool ClusterSequenceStructure::has_partner(const PseudoJet &reference, PseudoJet &partner) const{ return validated_cs()->has_partner(reference, partner); } bool ClusterSequenceStructure::has_child(const PseudoJet &reference, PseudoJet &child) const{ return validated_cs()->has_child(reference, child); } bool ClusterSequenceStructure::has_parents(const PseudoJet &reference, PseudoJet &parent1, PseudoJet &parent2) const{ return validated_cs()->has_parents(reference, parent1, parent2); } bool ClusterSequenceStructure::object_in_jet(const PseudoJet &reference, const PseudoJet &jet) const{ if ((!has_associated_cluster_sequence()) || (!jet.has_associated_cluster_sequence())) throw Error("you requested information about the internal structure of a jet, but it is not associated with a ClusterSequence or its associated ClusterSequence has gone out of scope."); if (reference.associated_cluster_sequence() != jet.associated_cluster_sequence()) return false; return validated_cs()->object_in_jet(reference, jet); } bool ClusterSequenceStructure::has_constituents() const{ if (!has_associated_cluster_sequence()) throw Error("you requested information about the internal structure of a jet, but it is not associated with a ClusterSequence or its associated ClusterSequence has gone out of scope."); return true; } vector ClusterSequenceStructure::constituents(const PseudoJet &reference) const{ return validated_cs()->constituents(reference); } bool ClusterSequenceStructure::has_exclusive_subjets() const{ if (!has_associated_cluster_sequence()) throw Error("you requested information about the internal structure of a jet, but it is not associated with a ClusterSequence or its associated ClusterSequence has gone out of scope."); return true; } std::vector ClusterSequenceStructure::exclusive_subjets (const PseudoJet &reference, const double & dcut) const { return validated_cs()->exclusive_subjets(reference, dcut); } int ClusterSequenceStructure::n_exclusive_subjets(const PseudoJet &reference, const double & dcut) const { return validated_cs()->n_exclusive_subjets(reference, dcut); } std::vector ClusterSequenceStructure::exclusive_subjets_up_to (const PseudoJet &reference, int nsub) const { return validated_cs()->exclusive_subjets_up_to(reference, nsub); } double ClusterSequenceStructure::exclusive_subdmerge(const PseudoJet &reference, int nsub) const { return validated_cs()->exclusive_subdmerge(reference, nsub); } double ClusterSequenceStructure::exclusive_subdmerge_max(const PseudoJet &reference, int nsub) const { return validated_cs()->exclusive_subdmerge_max(reference, nsub); } bool ClusterSequenceStructure::has_pieces(const PseudoJet &reference) const{ PseudoJet dummy1, dummy2; return has_parents(reference, dummy1, dummy2); } vector ClusterSequenceStructure::pieces(const PseudoJet &reference) const{ PseudoJet j1, j2; vector res; if (has_parents(reference, j1, j2)){ res.push_back(j1); res.push_back(j2); } return res; } FJCORE_END_NAMESPACE #include #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; void ClusterSequence::_bj_remove_from_tiles(TiledJet * const jet) { Tile * tile = & _tiles[jet->tile_index]; if (jet->previous == NULL) { tile->head = jet->next; } else { jet->previous->next = jet->next; } if (jet->next != NULL) { jet->next->previous = jet->previous; } } void ClusterSequence::_initialise_tiles() { double default_size = max(0.1,_Rparam); _tile_size_eta = default_size; _n_tiles_phi = max(3,int(floor(twopi/default_size))); _tile_size_phi = twopi / _n_tiles_phi; // >= _Rparam and fits in 2pi _tiles_eta_min = 0.0; _tiles_eta_max = 0.0; const double maxrap = 7.0; for(unsigned int i = 0; i < _jets.size(); i++) { double eta = _jets[i].rap(); if (abs(eta) < maxrap) { if (eta < _tiles_eta_min) {_tiles_eta_min = eta;} if (eta > _tiles_eta_max) {_tiles_eta_max = eta;} } } _tiles_ieta_min = int(floor(_tiles_eta_min/_tile_size_eta)); _tiles_ieta_max = int(floor( _tiles_eta_max/_tile_size_eta)); _tiles_eta_min = _tiles_ieta_min * _tile_size_eta; _tiles_eta_max = _tiles_ieta_max * _tile_size_eta; _tiles.resize((_tiles_ieta_max-_tiles_ieta_min+1)*_n_tiles_phi); for (int ieta = _tiles_ieta_min; ieta <= _tiles_ieta_max; ieta++) { for (int iphi = 0; iphi < _n_tiles_phi; iphi++) { Tile * tile = & _tiles[_tile_index(ieta,iphi)]; tile->head = NULL; // first element of tiles points to itself tile->begin_tiles[0] = tile; Tile ** pptile = & (tile->begin_tiles[0]); pptile++; tile->surrounding_tiles = pptile; if (ieta > _tiles_ieta_min) { // with the itile subroutine, we can safely run tiles from // idphi=-1 to idphi=+1, because it takes care of // negative and positive boundaries for (int idphi = -1; idphi <=+1; idphi++) { *pptile = & _tiles[_tile_index(ieta-1,iphi+idphi)]; pptile++; } } *pptile = & _tiles[_tile_index(ieta,iphi-1)]; pptile++; tile->RH_tiles = pptile; *pptile = & _tiles[_tile_index(ieta,iphi+1)]; pptile++; if (ieta < _tiles_ieta_max) { for (int idphi = -1; idphi <= +1; idphi++) { *pptile = & _tiles[_tile_index(ieta+1,iphi+idphi)]; pptile++; } } tile->end_tiles = pptile; tile->tagged = false; } } } int ClusterSequence::_tile_index(const double & eta, const double & phi) const { int ieta, iphi; if (eta <= _tiles_eta_min) {ieta = 0;} else if (eta >= _tiles_eta_max) {ieta = _tiles_ieta_max-_tiles_ieta_min;} else { ieta = int(((eta - _tiles_eta_min) / _tile_size_eta)); if (ieta > _tiles_ieta_max-_tiles_ieta_min) { ieta = _tiles_ieta_max-_tiles_ieta_min;} } iphi = int((phi+twopi)/_tile_size_phi) % _n_tiles_phi; return (iphi + ieta * _n_tiles_phi); } inline void ClusterSequence::_tj_set_jetinfo( TiledJet * const jet, const int _jets_index) { _bj_set_jetinfo<>(jet, _jets_index); jet->tile_index = _tile_index(jet->eta, jet->phi); Tile * tile = &_tiles[jet->tile_index]; jet->previous = NULL; jet->next = tile->head; if (jet->next != NULL) {jet->next->previous = jet;} tile->head = jet; } void ClusterSequence::_print_tiles(TiledJet * briefjets ) const { for (vector::const_iterator tile = _tiles.begin(); tile < _tiles.end(); tile++) { cout << "Tile " << tile - _tiles.begin()<<" = "; vector list; for (TiledJet * jetI = tile->head; jetI != NULL; jetI = jetI->next) { list.push_back(jetI-briefjets); } sort(list.begin(),list.end()); for (unsigned int i = 0; i < list.size(); i++) {cout <<" "< & tile_union, int & n_near_tiles) const { for (Tile * const * near_tile = _tiles[tile_index].begin_tiles; near_tile != _tiles[tile_index].end_tiles; near_tile++){ tile_union[n_near_tiles] = *near_tile - & _tiles[0]; n_near_tiles++; } } inline void ClusterSequence::_add_untagged_neighbours_to_tile_union( const int tile_index, vector & tile_union, int & n_near_tiles) { for (Tile ** near_tile = _tiles[tile_index].begin_tiles; near_tile != _tiles[tile_index].end_tiles; near_tile++){ if (! (*near_tile)->tagged) { (*near_tile)->tagged = true; tile_union[n_near_tiles] = *near_tile - & _tiles[0]; n_near_tiles++; } } } void ClusterSequence::_tiled_N2_cluster() { _initialise_tiles(); int n = _jets.size(); TiledJet * briefjets = new TiledJet[n]; TiledJet * jetA = briefjets, * jetB; TiledJet oldB; oldB.tile_index=0; // prevents a gcc warning vector tile_union(3*n_tile_neighbours); for (int i = 0; i< n; i++) { _tj_set_jetinfo(jetA, i); jetA++; // move on to next entry of briefjets } TiledJet * tail = jetA; // a semaphore for the end of briefjets TiledJet * head = briefjets; // a nicer way of naming start vector::const_iterator tile; for (tile = _tiles.begin(); tile != _tiles.end(); tile++) { for (jetA = tile->head; jetA != NULL; jetA = jetA->next) { for (jetB = tile->head; jetB != jetA; jetB = jetB->next) { double dist = _bj_dist(jetA,jetB); if (dist < jetA->NN_dist) {jetA->NN_dist = dist; jetA->NN = jetB;} if (dist < jetB->NN_dist) {jetB->NN_dist = dist; jetB->NN = jetA;} } } for (Tile ** RTile = tile->RH_tiles; RTile != tile->end_tiles; RTile++) { for (jetA = tile->head; jetA != NULL; jetA = jetA->next) { for (jetB = (*RTile)->head; jetB != NULL; jetB = jetB->next) { double dist = _bj_dist(jetA,jetB); if (dist < jetA->NN_dist) {jetA->NN_dist = dist; jetA->NN = jetB;} if (dist < jetB->NN_dist) {jetB->NN_dist = dist; jetB->NN = jetA;} } } } } double * diJ = new double[n]; jetA = head; for (int i = 0; i < n; i++) { diJ[i] = _bj_diJ(jetA); jetA++; // have jetA follow i } int history_location = n-1; while (tail != head) { double diJ_min = diJ[0]; int diJ_min_jet = 0; for (int i = 1; i < n; i++) { if (diJ[i] < diJ_min) {diJ_min_jet = i; diJ_min = diJ[i];} } history_location++; jetA = & briefjets[diJ_min_jet]; jetB = jetA->NN; diJ_min *= _invR2; if (jetB != NULL) { if (jetA < jetB) {std::swap(jetA,jetB);} int nn; // new jet index _do_ij_recombination_step(jetA->_jets_index, jetB->_jets_index, diJ_min, nn); _bj_remove_from_tiles(jetA); oldB = * jetB; // take a copy because we will need it... _bj_remove_from_tiles(jetB); _tj_set_jetinfo(jetB, nn); // also registers the jet in the tiling } else { _do_iB_recombination_step(jetA->_jets_index, diJ_min); _bj_remove_from_tiles(jetA); } int n_near_tiles = 0; _add_neighbours_to_tile_union(jetA->tile_index, tile_union, n_near_tiles); if (jetB != NULL) { bool sort_it = false; if (jetB->tile_index != jetA->tile_index) { sort_it = true; _add_neighbours_to_tile_union(jetB->tile_index,tile_union,n_near_tiles); } if (oldB.tile_index != jetA->tile_index && oldB.tile_index != jetB->tile_index) { sort_it = true; _add_neighbours_to_tile_union(oldB.tile_index,tile_union,n_near_tiles); } if (sort_it) { // sort the tiles before then compressing the list sort(tile_union.begin(), tile_union.begin()+n_near_tiles); // and now condense the list int nnn = 1; for (int i = 1; i < n_near_tiles; i++) { if (tile_union[i] != tile_union[nnn-1]) { tile_union[nnn] = tile_union[i]; nnn++; } } n_near_tiles = nnn; } } tail--; n--; if (jetA == tail) { } else { *jetA = *tail; diJ[jetA - head] = diJ[tail-head]; if (jetA->previous == NULL) { _tiles[jetA->tile_index].head = jetA; } else { jetA->previous->next = jetA; } if (jetA->next != NULL) {jetA->next->previous = jetA;} } for (int itile = 0; itile < n_near_tiles; itile++) { Tile * tile_ptr = &_tiles[tile_union[itile]]; for (TiledJet * jetI = tile_ptr->head; jetI != NULL; jetI = jetI->next) { // see if jetI had jetA or jetB as a NN -- if so recalculate the NN if (jetI->NN == jetA || (jetI->NN == jetB && jetB != NULL)) { jetI->NN_dist = _R2; jetI->NN = NULL; // now go over tiles that are neighbours of I (include own tile) for (Tile ** near_tile = tile_ptr->begin_tiles; near_tile != tile_ptr->end_tiles; near_tile++) { // and then over the contents of that tile for (TiledJet * jetJ = (*near_tile)->head; jetJ != NULL; jetJ = jetJ->next) { double dist = _bj_dist(jetI,jetJ); if (dist < jetI->NN_dist && jetJ != jetI) { jetI->NN_dist = dist; jetI->NN = jetJ; } } } diJ[jetI-head] = _bj_diJ(jetI); // update diJ } // check whether new jetB is closer than jetI's current NN and // if need to update things if (jetB != NULL) { double dist = _bj_dist(jetI,jetB); if (dist < jetI->NN_dist) { if (jetI != jetB) { jetI->NN_dist = dist; jetI->NN = jetB; diJ[jetI-head] = _bj_diJ(jetI); // update diJ... } } if (dist < jetB->NN_dist) { if (jetI != jetB) { jetB->NN_dist = dist; jetB->NN = jetI;} } } } } if (jetB != NULL) {diJ[jetB-head] = _bj_diJ(jetB);} for (Tile ** near_tile = _tiles[tail->tile_index].begin_tiles; near_tile!= _tiles[tail->tile_index].end_tiles; near_tile++){ for (TiledJet * jetJ = (*near_tile)->head; jetJ != NULL; jetJ = jetJ->next) { if (jetJ->NN == tail) {jetJ->NN = jetA;} } } if (jetB != NULL) {diJ[jetB-head] = _bj_diJ(jetB);} } delete[] diJ; delete[] briefjets; } void ClusterSequence::_faster_tiled_N2_cluster() { _initialise_tiles(); int n = _jets.size(); TiledJet * briefjets = new TiledJet[n]; TiledJet * jetA = briefjets, * jetB; TiledJet oldB; oldB.tile_index=0; // prevents a gcc warning vector tile_union(3*n_tile_neighbours); for (int i = 0; i< n; i++) { _tj_set_jetinfo(jetA, i); jetA++; // move on to next entry of briefjets } TiledJet * head = briefjets; // a nicer way of naming start vector::const_iterator tile; for (tile = _tiles.begin(); tile != _tiles.end(); tile++) { for (jetA = tile->head; jetA != NULL; jetA = jetA->next) { for (jetB = tile->head; jetB != jetA; jetB = jetB->next) { double dist = _bj_dist(jetA,jetB); if (dist < jetA->NN_dist) {jetA->NN_dist = dist; jetA->NN = jetB;} if (dist < jetB->NN_dist) {jetB->NN_dist = dist; jetB->NN = jetA;} } } for (Tile ** RTile = tile->RH_tiles; RTile != tile->end_tiles; RTile++) { for (jetA = tile->head; jetA != NULL; jetA = jetA->next) { for (jetB = (*RTile)->head; jetB != NULL; jetB = jetB->next) { double dist = _bj_dist(jetA,jetB); if (dist < jetA->NN_dist) {jetA->NN_dist = dist; jetA->NN = jetB;} if (dist < jetB->NN_dist) {jetB->NN_dist = dist; jetB->NN = jetA;} } } } } struct diJ_plus_link { double diJ; // the distance TiledJet * jet; // the jet (i) for which we've found this distance }; diJ_plus_link * diJ = new diJ_plus_link[n]; jetA = head; for (int i = 0; i < n; i++) { diJ[i].diJ = _bj_diJ(jetA); // kt distance * R^2 diJ[i].jet = jetA; // our compact diJ table will not be in jetA->diJ_posn = i; // one-to-one corresp. with non-compact jets, jetA++; // have jetA follow i } int history_location = n-1; while (n > 0) { diJ_plus_link * best, *stop; // pointers a bit faster than indices double diJ_min = diJ[0].diJ; // initialise the best one here. best = diJ; // and here stop = diJ+n; for (diJ_plus_link * here = diJ+1; here != stop; here++) { if (here->diJ < diJ_min) {best = here; diJ_min = here->diJ;} } history_location++; jetA = best->jet; jetB = jetA->NN; diJ_min *= _invR2; if (jetB != NULL) { if (jetA < jetB) {std::swap(jetA,jetB);} int nn; // new jet index _do_ij_recombination_step(jetA->_jets_index, jetB->_jets_index, diJ_min, nn); _bj_remove_from_tiles(jetA); oldB = * jetB; // take a copy because we will need it... _bj_remove_from_tiles(jetB); _tj_set_jetinfo(jetB, nn); // cause jetB to become _jets[nn] } else { _do_iB_recombination_step(jetA->_jets_index, diJ_min); _bj_remove_from_tiles(jetA); } int n_near_tiles = 0; _add_untagged_neighbours_to_tile_union(jetA->tile_index, tile_union, n_near_tiles); if (jetB != NULL) { if (jetB->tile_index != jetA->tile_index) { _add_untagged_neighbours_to_tile_union(jetB->tile_index, tile_union,n_near_tiles); } if (oldB.tile_index != jetA->tile_index && oldB.tile_index != jetB->tile_index) { _add_untagged_neighbours_to_tile_union(oldB.tile_index, tile_union,n_near_tiles); } } n--; diJ[n].jet->diJ_posn = jetA->diJ_posn; diJ[jetA->diJ_posn] = diJ[n]; for (int itile = 0; itile < n_near_tiles; itile++) { Tile * tile_ptr = &_tiles[tile_union[itile]]; tile_ptr->tagged = false; // reset tag, since we're done with unions for (TiledJet * jetI = tile_ptr->head; jetI != NULL; jetI = jetI->next) { // see if jetI had jetA or jetB as a NN -- if so recalculate the NN if (jetI->NN == jetA || (jetI->NN == jetB && jetB != NULL)) { jetI->NN_dist = _R2; jetI->NN = NULL; // now go over tiles that are neighbours of I (include own tile) for (Tile ** near_tile = tile_ptr->begin_tiles; near_tile != tile_ptr->end_tiles; near_tile++) { // and then over the contents of that tile for (TiledJet * jetJ = (*near_tile)->head; jetJ != NULL; jetJ = jetJ->next) { double dist = _bj_dist(jetI,jetJ); if (dist < jetI->NN_dist && jetJ != jetI) { jetI->NN_dist = dist; jetI->NN = jetJ; } } } diJ[jetI->diJ_posn].diJ = _bj_diJ(jetI); // update diJ kt-dist } // check whether new jetB is closer than jetI's current NN and // if jetI is closer than jetB's current (evolving) nearest // neighbour. Where relevant update things if (jetB != NULL) { double dist = _bj_dist(jetI,jetB); if (dist < jetI->NN_dist) { if (jetI != jetB) { jetI->NN_dist = dist; jetI->NN = jetB; diJ[jetI->diJ_posn].diJ = _bj_diJ(jetI); // update diJ... } } if (dist < jetB->NN_dist) { if (jetI != jetB) { jetB->NN_dist = dist; jetB->NN = jetI;} } } } } if (jetB != NULL) {diJ[jetB->diJ_posn].diJ = _bj_diJ(jetB);} } delete[] diJ; delete[] briefjets; } void ClusterSequence::_minheap_faster_tiled_N2_cluster() { _initialise_tiles(); int n = _jets.size(); TiledJet * briefjets = new TiledJet[n]; TiledJet * jetA = briefjets, * jetB; TiledJet oldB; oldB.tile_index=0; // prevents a gcc warning vector tile_union(3*n_tile_neighbours); for (int i = 0; i< n; i++) { _tj_set_jetinfo(jetA, i); jetA++; // move on to next entry of briefjets } TiledJet * head = briefjets; // a nicer way of naming start vector::const_iterator tile; for (tile = _tiles.begin(); tile != _tiles.end(); tile++) { for (jetA = tile->head; jetA != NULL; jetA = jetA->next) { for (jetB = tile->head; jetB != jetA; jetB = jetB->next) { double dist = _bj_dist(jetA,jetB); if (dist < jetA->NN_dist) {jetA->NN_dist = dist; jetA->NN = jetB;} if (dist < jetB->NN_dist) {jetB->NN_dist = dist; jetB->NN = jetA;} } } for (Tile ** RTile = tile->RH_tiles; RTile != tile->end_tiles; RTile++) { for (jetA = tile->head; jetA != NULL; jetA = jetA->next) { for (jetB = (*RTile)->head; jetB != NULL; jetB = jetB->next) { double dist = _bj_dist(jetA,jetB); if (dist < jetA->NN_dist) {jetA->NN_dist = dist; jetA->NN = jetB;} if (dist < jetB->NN_dist) {jetB->NN_dist = dist; jetB->NN = jetA;} } } } } vector diJs(n); for (int i = 0; i < n; i++) { diJs[i] = _bj_diJ(&briefjets[i]); briefjets[i].label_minheap_update_done(); } MinHeap minheap(diJs); vector jets_for_minheap; jets_for_minheap.reserve(n); int history_location = n-1; while (n > 0) { double diJ_min = minheap.minval() *_invR2; jetA = head + minheap.minloc(); history_location++; jetB = jetA->NN; if (jetB != NULL) { if (jetA < jetB) {std::swap(jetA,jetB);} int nn; // new jet index _do_ij_recombination_step(jetA->_jets_index, jetB->_jets_index, diJ_min, nn); _bj_remove_from_tiles(jetA); oldB = * jetB; // take a copy because we will need it... _bj_remove_from_tiles(jetB); _tj_set_jetinfo(jetB, nn); // cause jetB to become _jets[nn] } else { _do_iB_recombination_step(jetA->_jets_index, diJ_min); _bj_remove_from_tiles(jetA); } minheap.remove(jetA-head); int n_near_tiles = 0; _add_untagged_neighbours_to_tile_union(jetA->tile_index, tile_union, n_near_tiles); if (jetB != NULL) { if (jetB->tile_index != jetA->tile_index) { _add_untagged_neighbours_to_tile_union(jetB->tile_index, tile_union,n_near_tiles); } if (oldB.tile_index != jetA->tile_index && oldB.tile_index != jetB->tile_index) { // GS: the line below generates a warning that oldB.tile_index // may be used uninitialised. However, to reach this point, we // ned jetB != NULL (see test a few lines above) and is jetB // !=NULL, one would have gone through "oldB = *jetB before // (see piece of code ~20 line above), so the index is // initialised. We do not do anything to avoid the warning to // avoid any potential speed impact. _add_untagged_neighbours_to_tile_union(oldB.tile_index, tile_union,n_near_tiles); } jetB->label_minheap_update_needed(); jets_for_minheap.push_back(jetB); } for (int itile = 0; itile < n_near_tiles; itile++) { Tile * tile_ptr = &_tiles[tile_union[itile]]; tile_ptr->tagged = false; // reset tag, since we're done with unions for (TiledJet * jetI = tile_ptr->head; jetI != NULL; jetI = jetI->next) { // see if jetI had jetA or jetB as a NN -- if so recalculate the NN if (jetI->NN == jetA || (jetI->NN == jetB && jetB != NULL)) { jetI->NN_dist = _R2; jetI->NN = NULL; // label jetI as needing heap action... if (!jetI->minheap_update_needed()) { jetI->label_minheap_update_needed(); jets_for_minheap.push_back(jetI);} // now go over tiles that are neighbours of I (include own tile) for (Tile ** near_tile = tile_ptr->begin_tiles; near_tile != tile_ptr->end_tiles; near_tile++) { // and then over the contents of that tile for (TiledJet * jetJ = (*near_tile)->head; jetJ != NULL; jetJ = jetJ->next) { double dist = _bj_dist(jetI,jetJ); if (dist < jetI->NN_dist && jetJ != jetI) { jetI->NN_dist = dist; jetI->NN = jetJ; } } } } // check whether new jetB is closer than jetI's current NN and // if jetI is closer than jetB's current (evolving) nearest // neighbour. Where relevant update things if (jetB != NULL) { double dist = _bj_dist(jetI,jetB); if (dist < jetI->NN_dist) { if (jetI != jetB) { jetI->NN_dist = dist; jetI->NN = jetB; // label jetI as needing heap action... if (!jetI->minheap_update_needed()) { jetI->label_minheap_update_needed(); jets_for_minheap.push_back(jetI);} } } if (dist < jetB->NN_dist) { if (jetI != jetB) { jetB->NN_dist = dist; jetB->NN = jetI;} } } } } while (jets_for_minheap.size() > 0) { TiledJet * jetI = jets_for_minheap.back(); jets_for_minheap.pop_back(); minheap.update(jetI-head, _bj_diJ(jetI)); jetI->label_minheap_update_done(); } n--; } delete[] briefjets; } FJCORE_END_NAMESPACE FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; CompositeJetStructure::CompositeJetStructure(const std::vector & initial_pieces, const JetDefinition::Recombiner * recombiner) : _pieces(initial_pieces){ if (recombiner){}; // ugly trick to prevent a gcc warning _area_4vector_ptr = 0; } std::string CompositeJetStructure::description() const{ string str = "Composite PseudoJet"; return str; } bool CompositeJetStructure::has_constituents() const{ return _pieces.size()!=0; } std::vector CompositeJetStructure::constituents(const PseudoJet & /*jet*/) const{ vector all_constituents; for (unsigned i = 0; i < _pieces.size(); i++) { if (_pieces[i].has_constituents()){ vector constits = _pieces[i].constituents(); copy(constits.begin(), constits.end(), back_inserter(all_constituents)); } else { all_constituents.push_back(_pieces[i]); } } return all_constituents; } std::vector CompositeJetStructure::pieces(const PseudoJet & /*jet*/) const{ return _pieces; } FJCORE_END_NAMESPACE // defined in fastjet/internal/base.hh #include #ifdef FJCORE_HAVE_EXECINFO_H #include #include #endif FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; bool Error::_print_errors = true; bool Error::_print_backtrace = false; ostream * Error::_default_ostr = & cerr; Error::Error(const std::string & message_in) { _message = message_in; if (_print_errors && _default_ostr){ ostringstream oss; oss << "fjcore::Error: "<< message_in << endl; #ifdef FJCORE_HAVE_EXECINFO_H if (_print_backtrace){ void * array[10]; char ** messages; int size = backtrace(array, 10); messages = backtrace_symbols(array, size); oss << "stack:" << endl; for (int i = 1; i < size && messages != NULL; ++i){ oss << " #" << i << ": " << messages[i] << endl; } free(messages); } #endif *_default_ostr << oss.str(); _default_ostr->flush(); } } FJCORE_END_NAMESPACE #include #include using namespace std; FJCORE_BEGIN_NAMESPACE FJCORE_END_NAMESPACE #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; const double JetDefinition::max_allowable_R = 1000.0; JetDefinition::JetDefinition(JetAlgorithm jet_algorithm_in, double R_in, Strategy strategy_in, RecombinationScheme recomb_scheme_in, int nparameters) : _jet_algorithm(jet_algorithm_in), _Rparam(R_in), _strategy(strategy_in) { if (_jet_algorithm == ee_kt_algorithm) { _Rparam = 4.0; // introduce a fictional R that ensures that } else { if (R_in > max_allowable_R) { ostringstream oss; oss << "Requested R = " << R_in << " for jet definition is larger than max_allowable_R = " << max_allowable_R; throw Error(oss.str()); } } switch (jet_algorithm_in) { case ee_kt_algorithm: if (nparameters != 0) { ostringstream oss; oss << "ee_kt_algorithm should be constructed with 0 parameters but was called with " << nparameters << " parameter(s)\n"; throw Error(oss.str()); } break; case genkt_algorithm: case ee_genkt_algorithm: if (nparameters != 2) { ostringstream oss; oss << "(ee_)genkt_algorithm should be constructed with 2 parameters but was called with " << nparameters << " parameter(s)\n"; throw Error(oss.str()); } break; default: if (nparameters != 1) { ostringstream oss; oss << "The jet algorithm you requested (" << jet_algorithm_in << ") should be constructed with 1 parameter but was called with " << nparameters << " parameter(s)\n"; throw Error(oss.str()); } } assert (_strategy != plugin_strategy); _plugin = NULL; set_recombination_scheme(recomb_scheme_in); set_extra_param(0.0); // make sure it's defined } string JetDefinition::description() const { ostringstream name; if (jet_algorithm() == plugin_algorithm) { return plugin()->description(); } else if (jet_algorithm() == kt_algorithm) { name << "Longitudinally invariant kt algorithm with R = " << R(); name << " and " << recombiner()->description(); } else if (jet_algorithm() == cambridge_algorithm) { name << "Longitudinally invariant Cambridge/Aachen algorithm with R = " << R() ; name << " and " << recombiner()->description(); } else if (jet_algorithm() == antikt_algorithm) { name << "Longitudinally invariant anti-kt algorithm with R = " << R() ; name << " and " << recombiner()->description(); } else if (jet_algorithm() == genkt_algorithm) { name << "Longitudinally invariant generalised kt algorithm with R = " << R() << ", p = " << extra_param(); name << " and " << recombiner()->description(); } else if (jet_algorithm() == cambridge_for_passive_algorithm) { name << "Longitudinally invariant Cambridge/Aachen algorithm with R = " << R() << "and a special hack whereby particles with kt < " << extra_param() << "are treated as passive ghosts"; } else if (jet_algorithm() == ee_kt_algorithm) { name << "e+e- kt (Durham) algorithm (NB: no R)"; name << " with " << recombiner()->description(); } else if (jet_algorithm() == ee_genkt_algorithm) { name << "e+e- generalised kt algorithm with R = " << R() << ", p = " << extra_param(); name << " and " << recombiner()->description(); } else if (jet_algorithm() == undefined_jet_algorithm) { name << "uninitialised JetDefinition (jet_algorithm=undefined_jet_algorithm)" ; } else { throw Error("JetDefinition::description(): unrecognized jet_algorithm"); } return name.str(); } void JetDefinition::set_recombination_scheme( RecombinationScheme recomb_scheme) { _default_recombiner = JetDefinition::DefaultRecombiner(recomb_scheme); if (_recombiner_shared()) _recombiner_shared.reset(); _recombiner = 0; } bool JetDefinition::has_same_recombiner(const JetDefinition &other_jd) const{ const RecombinationScheme & scheme = recombination_scheme(); if (other_jd.recombination_scheme() != scheme) return false; return (scheme != external_scheme) || (recombiner() == other_jd.recombiner()); } void JetDefinition::delete_recombiner_when_unused(){ if (_recombiner == 0){ throw Error("tried to call JetDefinition::delete_recombiner_when_unused() for a JetDefinition without a user-defined recombination scheme"); } _recombiner_shared.reset(_recombiner); } void JetDefinition::delete_plugin_when_unused(){ if (_plugin == 0){ throw Error("tried to call JetDefinition::delete_plugin_when_unused() for a JetDefinition without a plugin"); } _plugin_shared.reset(_plugin); } string JetDefinition::DefaultRecombiner::description() const { switch(_recomb_scheme) { case E_scheme: return "E scheme recombination"; case pt_scheme: return "pt scheme recombination"; case pt2_scheme: return "pt2 scheme recombination"; case Et_scheme: return "Et scheme recombination"; case Et2_scheme: return "Et2 scheme recombination"; case BIpt_scheme: return "boost-invariant pt scheme recombination"; case BIpt2_scheme: return "boost-invariant pt2 scheme recombination"; default: ostringstream err; err << "DefaultRecombiner: unrecognized recombination scheme " << _recomb_scheme; throw Error(err.str()); } } void JetDefinition::DefaultRecombiner::recombine( const PseudoJet & pa, const PseudoJet & pb, PseudoJet & pab) const { double weighta, weightb; switch(_recomb_scheme) { case E_scheme: pab.reset(pa.px()+pb.px(), pa.py()+pb.py(), pa.pz()+pb.pz(), pa.E ()+pb.E ()); return; case pt_scheme: case Et_scheme: case BIpt_scheme: weighta = pa.perp(); weightb = pb.perp(); break; case pt2_scheme: case Et2_scheme: case BIpt2_scheme: weighta = pa.perp2(); weightb = pb.perp2(); break; default: ostringstream err; err << "DefaultRecombiner: unrecognized recombination scheme " << _recomb_scheme; throw Error(err.str()); } double perp_ab = pa.perp() + pb.perp(); if (perp_ab != 0.0) { // weights also non-zero... double y_ab = (weighta * pa.rap() + weightb * pb.rap())/(weighta+weightb); double phi_a = pa.phi(), phi_b = pb.phi(); if (phi_a - phi_b > pi) phi_b += twopi; if (phi_a - phi_b < -pi) phi_b -= twopi; double phi_ab = (weighta * phi_a + weightb * phi_b)/(weighta+weightb); pab.reset_PtYPhiM(perp_ab,y_ab,phi_ab); } else { // weights are zero pab.reset(0.0, 0.0, 0.0, 0.0); } } void JetDefinition::DefaultRecombiner::preprocess(PseudoJet & p) const { switch(_recomb_scheme) { case E_scheme: case BIpt_scheme: case BIpt2_scheme: break; case pt_scheme: case pt2_scheme: { double newE = sqrt(p.perp2()+p.pz()*p.pz()); p.reset_momentum(p.px(), p.py(), p.pz(), newE); } break; case Et_scheme: case Et2_scheme: { double rescale = p.E()/sqrt(p.perp2()+p.pz()*p.pz()); p.reset_momentum(rescale*p.px(), rescale*p.py(), rescale*p.pz(), p.E()); } break; default: ostringstream err; err << "DefaultRecombiner: unrecognized recombination scheme " << _recomb_scheme; throw Error(err.str()); } } void JetDefinition::Plugin::set_ghost_separation_scale(double /*scale*/) const { throw Error("set_ghost_separation_scale not supported"); } PseudoJet join(const vector & pieces, const JetDefinition::Recombiner & recombiner){ PseudoJet result; // automatically initialised to 0 if (pieces.size()>0){ result = pieces[0]; for (unsigned int i=1; i(cj_struct)); return result; } PseudoJet join(const PseudoJet & j1, const JetDefinition::Recombiner & recombiner){ return join(vector(1,j1), recombiner); } PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const JetDefinition::Recombiner & recombiner){ vector pieces; pieces.push_back(j1); pieces.push_back(j2); return join(pieces, recombiner); } PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3, const JetDefinition::Recombiner & recombiner){ vector pieces; pieces.push_back(j1); pieces.push_back(j2); pieces.push_back(j3); return join(pieces, recombiner); } PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3, const PseudoJet & j4, const JetDefinition::Recombiner & recombiner){ vector pieces; pieces.push_back(j1); pieces.push_back(j2); pieces.push_back(j3); pieces.push_back(j4); return join(pieces, recombiner); } FJCORE_END_NAMESPACE #include #include using namespace std; FJCORE_BEGIN_NAMESPACE ostream * LimitedWarning::_default_ostr = &cerr; std::list< LimitedWarning::Summary > LimitedWarning::_global_warnings_summary; int LimitedWarning::_max_warn_default = 5; void LimitedWarning::warn(const std::string & warning) { warn(warning, _default_ostr); } void LimitedWarning::warn(const std::string & warning, std::ostream * ostr) { if (_this_warning_summary == 0) { _global_warnings_summary.push_back(Summary(warning, 0)); _this_warning_summary = & (_global_warnings_summary.back()); } if (_n_warn_so_far < _max_warn) { ostringstream warnstr; warnstr << "WARNING: "; warnstr << warning; _n_warn_so_far++; if (_n_warn_so_far == _max_warn) warnstr << " (LAST SUCH WARNING)"; warnstr << std::endl; if (ostr) { (*ostr) << warnstr.str(); ostr->flush(); // get something written to file even if the program aborts } } if (_this_warning_summary->second < numeric_limits::max()) { _this_warning_summary->second++; } } string LimitedWarning::summary() { ostringstream str; for (list

      ::const_iterator it = _global_warnings_summary.begin(); it != _global_warnings_summary.end(); it++) { str << it->second << " times: " << it->first << endl; } return str.str(); } FJCORE_END_NAMESPACE #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; void MinHeap::_initialise(const std::vector & values){ for (unsigned i = values.size(); i < _heap.size(); i++) { _heap[i].value = std::numeric_limits::max(); _heap[i].minloc = &(_heap[i]); } for (unsigned i = 0; i < values.size(); i++) { _heap[i].value = values[i]; _heap[i].minloc = &(_heap[i]); } for (unsigned i = _heap.size()-1; i > 0; i--) { ValueLoc * parent = &(_heap[(i-1)/2]); ValueLoc * here = &(_heap[i]); if (here->minloc->value < parent->minloc->value) { parent->minloc = here->minloc; } } } void MinHeap::update(unsigned int loc, double new_value) { assert(loc < _heap.size()); ValueLoc * start = &(_heap[loc]); if (start->minloc != start && !(new_value < start->minloc->value)) { start->value = new_value; return; } start->value = new_value; start->minloc = start; bool change_made = true; ValueLoc * heap_end = (&(_heap[0])) + _heap.size(); while(change_made) { ValueLoc * here = &(_heap[loc]); change_made = false; if (here->minloc == start) { here->minloc = here; change_made = true; } ValueLoc * child = &(_heap[2*loc+1]); if (child < heap_end && child->minloc->value < here->minloc->value ) { here->minloc = child->minloc; change_made = true;} child++; if (child < heap_end && child->minloc->value < here->minloc->value ) { here->minloc = child->minloc; change_made = true;} if (loc == 0) {break;} loc = (loc-1)/2; } } FJCORE_END_NAMESPACE #include #include #include #include #include #include FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh using namespace std; PseudoJet::PseudoJet(const double px_in, const double py_in, const double pz_in, const double E_in) { _E = E_in ; _px = px_in; _py = py_in; _pz = pz_in; this->_finish_init(); _reset_indices(); } void PseudoJet::_finish_init () { _kt2 = this->px()*this->px() + this->py()*this->py(); _phi = pseudojet_invalid_phi; _rap = pseudojet_invalid_rap; } void PseudoJet::_set_rap_phi() const { if (_kt2 == 0.0) { _phi = 0.0; } else { _phi = atan2(this->py(),this->px()); } if (_phi < 0.0) {_phi += twopi;} if (_phi >= twopi) {_phi -= twopi;} // can happen if phi=-|eps<1e-15|? if (this->E() == abs(this->pz()) && _kt2 == 0) { double MaxRapHere = MaxRap + abs(this->pz()); if (this->pz() >= 0.0) {_rap = MaxRapHere;} else {_rap = -MaxRapHere;} } else { double effective_m2 = max(0.0,m2()); // force non tachyonic mass double E_plus_pz = _E + abs(_pz); // the safer of p+, p- _rap = 0.5*log((_kt2 + effective_m2)/(E_plus_pz*E_plus_pz)); if (_pz > 0) {_rap = - _rap;} } } valarray PseudoJet::four_mom() const { valarray mom(4); mom[0] = _px; mom[1] = _py; mom[2] = _pz; mom[3] = _E ; return mom; } double PseudoJet::operator () (int i) const { switch(i) { case X: return px(); case Y: return py(); case Z: return pz(); case T: return e(); default: ostringstream err; err << "PseudoJet subscripting: bad index (" << i << ")"; throw Error(err.str()); } return 0.; } double PseudoJet::pseudorapidity() const { if (px() == 0.0 && py() ==0.0) return MaxRap; if (pz() == 0.0) return 0.0; double theta = atan(perp()/pz()); if (theta < 0) theta += pi; return -log(tan(theta/2)); } PseudoJet operator+ (const PseudoJet & jet1, const PseudoJet & jet2) { return PseudoJet(jet1.px()+jet2.px(), jet1.py()+jet2.py(), jet1.pz()+jet2.pz(), jet1.E() +jet2.E() ); } PseudoJet operator- (const PseudoJet & jet1, const PseudoJet & jet2) { return PseudoJet(jet1.px()-jet2.px(), jet1.py()-jet2.py(), jet1.pz()-jet2.pz(), jet1.E() -jet2.E() ); } PseudoJet operator* (double coeff, const PseudoJet & jet) { PseudoJet coeff_times_jet(jet); coeff_times_jet *= coeff; return coeff_times_jet; } PseudoJet operator* (const PseudoJet & jet, double coeff) { return coeff*jet; } PseudoJet operator/ (const PseudoJet & jet, double coeff) { return (1.0/coeff)*jet; } void PseudoJet::operator*=(double coeff) { _px *= coeff; _py *= coeff; _pz *= coeff; _E *= coeff; _kt2*= coeff*coeff; } void PseudoJet::operator/=(double coeff) { (*this) *= 1.0/coeff; } void PseudoJet::operator+=(const PseudoJet & other_jet) { _px += other_jet._px; _py += other_jet._py; _pz += other_jet._pz; _E += other_jet._E ; _finish_init(); // we need to recalculate phi,rap,kt2 } void PseudoJet::operator-=(const PseudoJet & other_jet) { _px -= other_jet._px; _py -= other_jet._py; _pz -= other_jet._pz; _E -= other_jet._E ; _finish_init(); // we need to recalculate phi,rap,kt2 } bool operator==(const PseudoJet & a, const PseudoJet & b) { if (a.px() != b.px()) return false; if (a.py() != b.py()) return false; if (a.pz() != b.pz()) return false; if (a.E () != b.E ()) return false; if (a.user_index() != b.user_index()) return false; if (a.cluster_hist_index() != b.cluster_hist_index()) return false; if (a.user_info_ptr() != b.user_info_ptr()) return false; if (a.structure_ptr() != b.structure_ptr()) return false; return true; } bool operator==(const PseudoJet & jet, const double val) { if (val != 0) throw Error("comparing a PseudoJet with a non-zero constant (double) is not allowed."); return (jet.px() == 0 && jet.py() == 0 && jet.pz() == 0 && jet.E() == 0); } PseudoJet & PseudoJet::boost(const PseudoJet & prest) { if (prest.px() == 0.0 && prest.py() == 0.0 && prest.pz() == 0.0) return *this; double m_local = prest.m(); assert(m_local != 0); double pf4 = ( px()*prest.px() + py()*prest.py() + pz()*prest.pz() + E()*prest.E() )/m_local; double fn = (pf4 + E()) / (prest.E() + m_local); _px += fn*prest.px(); _py += fn*prest.py(); _pz += fn*prest.pz(); _E = pf4; _finish_init(); // we need to recalculate phi,rap,kt2 return *this; } PseudoJet & PseudoJet::unboost(const PseudoJet & prest) { if (prest.px() == 0.0 && prest.py() == 0.0 && prest.pz() == 0.0) return *this; double m_local = prest.m(); assert(m_local != 0); double pf4 = ( -px()*prest.px() - py()*prest.py() - pz()*prest.pz() + E()*prest.E() )/m_local; double fn = (pf4 + E()) / (prest.E() + m_local); _px -= fn*prest.px(); _py -= fn*prest.py(); _pz -= fn*prest.pz(); _E = pf4; _finish_init(); // we need to recalculate phi,rap,kt2 return *this; } bool have_same_momentum(const PseudoJet & jeta, const PseudoJet & jetb) { return jeta.px() == jetb.px() && jeta.py() == jetb.py() && jeta.pz() == jetb.pz() && jeta.E() == jetb.E(); } void PseudoJet::set_cached_rap_phi(double rap_in, double phi_in) { _rap = rap_in; _phi = phi_in; if (_phi >= twopi) _phi -= twopi; if (_phi < 0) _phi += twopi; } void PseudoJet::reset_momentum_PtYPhiM(double pt_in, double y_in, double phi_in, double m_in) { assert(phi_in < 2*twopi && phi_in > -twopi); double ptm = (m_in == 0) ? pt_in : sqrt(pt_in*pt_in+m_in*m_in); double exprap = exp(y_in); double pminus = ptm/exprap; double pplus = ptm*exprap; double px_local = pt_in*cos(phi_in); double py_local = pt_in*sin(phi_in); reset_momentum(px_local,py_local,0.5*(pplus-pminus),0.5*(pplus+pminus)); set_cached_rap_phi(y_in,phi_in); } PseudoJet PtYPhiM(double pt, double y, double phi, double m) { assert(phi < 2*twopi && phi > -twopi); double ptm = (m == 0) ? pt : sqrt(pt*pt+m*m); double exprap = exp(y); double pminus = ptm/exprap; double pplus = ptm*exprap; double px = pt*cos(phi); double py = pt*sin(phi); PseudoJet mom(px,py,0.5*(pplus-pminus),0.5*(pplus+pminus)); mom.set_cached_rap_phi(y,phi); return mom; } double PseudoJet::kt_distance(const PseudoJet & other) const { double distance = min(_kt2, other._kt2); double dphi = abs(phi() - other.phi()); if (dphi > pi) {dphi = twopi - dphi;} double drap = rap() - other.rap(); distance = distance * (dphi*dphi + drap*drap); return distance; } double PseudoJet::plain_distance(const PseudoJet & other) const { double dphi = abs(phi() - other.phi()); if (dphi > pi) {dphi = twopi - dphi;} double drap = rap() - other.rap(); return (dphi*dphi + drap*drap); } double PseudoJet::delta_phi_to(const PseudoJet & other) const { double dphi = other.phi() - phi(); if (dphi > pi) dphi -= twopi; if (dphi < -pi) dphi += twopi; return dphi; } string PseudoJet::description() const{ if (!_structure()) return "standard PseudoJet (with no associated clustering information)"; return _structure()->description(); } bool PseudoJet::has_associated_cluster_sequence() const{ return (_structure()) && (_structure->has_associated_cluster_sequence()); } const ClusterSequence* PseudoJet::associated_cluster_sequence() const{ if (! has_associated_cluster_sequence()) return NULL; return _structure->associated_cluster_sequence(); } bool PseudoJet::has_valid_cluster_sequence() const{ return (_structure()) && (_structure->has_valid_cluster_sequence()); } const ClusterSequence * PseudoJet::validated_cs() const { return validated_structure_ptr()->validated_cs(); } void PseudoJet::set_structure_shared_ptr(const SharedPtr &structure_in){ _structure = structure_in; } bool PseudoJet::has_structure() const{ return _structure(); } const PseudoJetStructureBase* PseudoJet::structure_ptr() const { if (!_structure()) return NULL; return _structure(); } PseudoJetStructureBase* PseudoJet::structure_non_const_ptr(){ if (!_structure()) return NULL; return _structure(); } const PseudoJetStructureBase* PseudoJet::validated_structure_ptr() const { if (!_structure()) throw Error("Trying to access the structure of a PseudoJet which has no associated structure"); return _structure(); } const SharedPtr & PseudoJet::structure_shared_ptr() const { return _structure; } bool PseudoJet::has_partner(PseudoJet &partner) const{ return validated_structure_ptr()->has_partner(*this, partner); } bool PseudoJet::has_child(PseudoJet &child) const{ return validated_structure_ptr()->has_child(*this, child); } bool PseudoJet::has_parents(PseudoJet &parent1, PseudoJet &parent2) const{ return validated_structure_ptr()->has_parents(*this, parent1, parent2); } bool PseudoJet::contains(const PseudoJet &constituent) const{ return validated_structure_ptr()->object_in_jet(constituent, *this); } bool PseudoJet::is_inside(const PseudoJet &jet) const{ return validated_structure_ptr()->object_in_jet(*this, jet); } bool PseudoJet::has_constituents() const{ return (_structure()) && (_structure->has_constituents()); } vector PseudoJet::constituents() const{ return validated_structure_ptr()->constituents(*this); } bool PseudoJet::has_exclusive_subjets() const{ return (_structure()) && (_structure->has_exclusive_subjets()); } std::vector PseudoJet::exclusive_subjets (const double & dcut) const { return validated_structure_ptr()->exclusive_subjets(*this, dcut); } int PseudoJet::n_exclusive_subjets(const double & dcut) const { return validated_structure_ptr()->n_exclusive_subjets(*this, dcut); } std::vector PseudoJet::exclusive_subjets_up_to (int nsub) const { return validated_structure_ptr()->exclusive_subjets_up_to(*this, nsub); } std::vector PseudoJet::exclusive_subjets (int nsub) const { vector subjets = exclusive_subjets_up_to(nsub); if (int(subjets.size()) < nsub) { ostringstream err; err << "Requested " << nsub << " exclusive subjets, but there were only " << subjets.size() << " particles in the jet"; throw Error(err.str()); } return subjets; } double PseudoJet::exclusive_subdmerge(int nsub) const { return validated_structure_ptr()->exclusive_subdmerge(*this, nsub); } double PseudoJet::exclusive_subdmerge_max(int nsub) const { return validated_structure_ptr()->exclusive_subdmerge_max(*this, nsub); } bool PseudoJet::has_pieces() const{ return ((_structure()) && (_structure->has_pieces(*this))); } std::vector PseudoJet::pieces() const{ return validated_structure_ptr()->pieces(*this); } PseudoJet::InexistentUserInfo::InexistentUserInfo() : Error("you attempted to perform a dynamic cast of a PseudoJet's extra info, but the extra info pointer was null") {} void sort_indices(vector & indices, const vector & values) { IndexedSortHelper index_sort_helper(&values); sort(indices.begin(), indices.end(), index_sort_helper); } template vector objects_sorted_by_values( const vector & objects, const vector & values) { assert(objects.size() == values.size()); vector indices(values.size()); for (size_t i = 0; i < indices.size(); i++) {indices[i] = i;} sort_indices(indices, values); vector objects_sorted(objects.size()); for (size_t i = 0; i < indices.size(); i++) { objects_sorted[i] = objects[indices[i]]; } return objects_sorted; } vector sorted_by_pt(const vector & jets) { vector minus_kt2(jets.size()); for (size_t i = 0; i < jets.size(); i++) {minus_kt2[i] = -jets[i].kt2();} return objects_sorted_by_values(jets, minus_kt2); } vector sorted_by_rapidity(const vector & jets) { vector rapidities(jets.size()); for (size_t i = 0; i < jets.size(); i++) {rapidities[i] = jets[i].rap();} return objects_sorted_by_values(jets, rapidities); } vector sorted_by_E(const vector & jets) { vector energies(jets.size()); for (size_t i = 0; i < jets.size(); i++) {energies[i] = -jets[i].E();} return objects_sorted_by_values(jets, energies); } vector sorted_by_pz(const vector & jets) { vector pz(jets.size()); for (size_t i = 0; i < jets.size(); i++) {pz[i] = jets[i].pz();} return objects_sorted_by_values(jets, pz); } PseudoJet join(const vector & pieces){ PseudoJet result; // automatically initialised to 0 for (unsigned int i=0; i(cj_struct)); return result; } PseudoJet join(const PseudoJet & j1){ return join(vector(1,j1)); } PseudoJet join(const PseudoJet & j1, const PseudoJet & j2){ vector pieces; pieces.push_back(j1); pieces.push_back(j2); return join(pieces); } PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3){ vector pieces; pieces.push_back(j1); pieces.push_back(j2); pieces.push_back(j3); return join(pieces); } PseudoJet join(const PseudoJet & j1, const PseudoJet & j2, const PseudoJet & j3, const PseudoJet & j4){ vector pieces; pieces.push_back(j1); pieces.push_back(j2); pieces.push_back(j3); pieces.push_back(j4); return join(pieces); } FJCORE_END_NAMESPACE using namespace std; FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh const ClusterSequence* PseudoJetStructureBase::associated_cluster_sequence() const{ return NULL; } const ClusterSequence * PseudoJetStructureBase::validated_cs() const{ throw Error("This PseudoJet structure is not associated with a valid ClusterSequence"); } bool PseudoJetStructureBase::has_partner(const PseudoJet & /*reference */, PseudoJet & /*partner*/) const{ throw Error("This PseudoJet structure has no implementation for has_partner"); } bool PseudoJetStructureBase::has_child(const PseudoJet & /*reference*/, PseudoJet & /*child*/) const{ throw Error("This PseudoJet structure has no implementation for has_child"); } bool PseudoJetStructureBase::has_parents(const PseudoJet & /*reference*/, PseudoJet &/*parent1*/, PseudoJet &/*parent2*/) const{ throw Error("This PseudoJet structure has no implementation for has_parents"); } bool PseudoJetStructureBase::object_in_jet(const PseudoJet & /*reference*/, const PseudoJet & /*jet*/) const{ throw Error("This PseudoJet structure has no implementation for is_inside"); } vector PseudoJetStructureBase::constituents(const PseudoJet &/*reference*/) const{ throw Error("This PseudoJet structure has no implementation for constituents"); } vector PseudoJetStructureBase::exclusive_subjets (const PseudoJet & /*reference*/, const double & /*dcut*/) const{ throw Error("This PseudoJet structure has no implementation for exclusive_subjets"); } int PseudoJetStructureBase::n_exclusive_subjets(const PseudoJet & /*reference*/, const double & /*dcut*/) const{ throw Error("This PseudoJet structure has no implementation for n_exclusive_subjets"); } vector PseudoJetStructureBase::exclusive_subjets_up_to (const PseudoJet & /*reference*/, int /*nsub*/) const{ throw Error("This PseudoJet structure has no implementation for exclusive_subjets"); } double PseudoJetStructureBase::exclusive_subdmerge(const PseudoJet & /*reference*/, int /*nsub*/) const{ throw Error("This PseudoJet structure has no implementation for exclusive_submerge"); } double PseudoJetStructureBase::exclusive_subdmerge_max(const PseudoJet & /*reference*/, int /*nsub*/) const{ throw Error("This PseudoJet structure has no implementation for exclusive_submerge_max"); } std::vector PseudoJetStructureBase::pieces(const PseudoJet & /*reference*/) const{ throw Error("This PseudoJet structure has no implementation for pieces"); } FJCORE_END_NAMESPACE #include #include using namespace std; FJCORE_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh std::vector Selector::operator()(const std::vector & jets) const { std::vector result; const SelectorWorker * worker_local = validated_worker(); if (worker_local->applies_jet_by_jet()) { for (std::vector::const_iterator jet = jets.begin(); jet != jets.end(); jet++) { if (worker_local->pass(*jet)) result.push_back(*jet); } } else { std::vector jetptrs(jets.size()); for (unsigned i = 0; i < jets.size(); i++) { jetptrs[i] = & jets[i]; } worker_local->terminator(jetptrs); for (unsigned i = 0; i < jetptrs.size(); i++) { if (jetptrs[i]) result.push_back(jets[i]); } } return result; } unsigned int Selector::count(const std::vector & jets) const { unsigned n = 0; const SelectorWorker * worker_local = validated_worker(); if (worker_local->applies_jet_by_jet()) { for (unsigned i = 0; i < jets.size(); i++) { if (worker_local->pass(jets[i])) n++; } } else { std::vector jetptrs(jets.size()); for (unsigned i = 0; i < jets.size(); i++) { jetptrs[i] = & jets[i]; } worker_local->terminator(jetptrs); for (unsigned i = 0; i < jetptrs.size(); i++) { if (jetptrs[i]) n++; } } return n; } void Selector::sift(const std::vector & jets, std::vector & jets_that_pass, std::vector & jets_that_fail ) const { const SelectorWorker * worker_local = validated_worker(); jets_that_pass.clear(); jets_that_fail.clear(); if (worker_local->applies_jet_by_jet()) { for (unsigned i = 0; i < jets.size(); i++) { if (worker_local->pass(jets[i])) { jets_that_pass.push_back(jets[i]); } else { jets_that_fail.push_back(jets[i]); } } } else { std::vector jetptrs(jets.size()); for (unsigned i = 0; i < jets.size(); i++) { jetptrs[i] = & jets[i]; } worker_local->terminator(jetptrs); for (unsigned i = 0; i < jetptrs.size(); i++) { if (jetptrs[i]) { jets_that_pass.push_back(jets[i]); } else { jets_that_fail.push_back(jets[i]); } } } } bool SelectorWorker::has_finite_area() const { if (! is_geometric()) return false; double rapmin, rapmax; get_rapidity_extent(rapmin, rapmax); return (rapmax != std::numeric_limits::infinity()) && (-rapmin != std::numeric_limits::infinity()); } class SW_Identity : public SelectorWorker { public: SW_Identity(){} virtual bool pass(const PseudoJet &) const { return true; } virtual void terminator(vector &) const { return; } virtual string description() const { return "Identity";} virtual bool is_geometric() const { return true;} }; Selector SelectorIdentity() { return Selector(new SW_Identity); } class SW_Not : public SelectorWorker { public: SW_Not(const Selector & s) : _s(s) {} virtual SelectorWorker* copy(){ return new SW_Not(*this);} virtual bool pass(const PseudoJet & jet) const { if (!applies_jet_by_jet()) throw Error("Cannot apply this selector worker to an individual jet"); return ! _s.pass(jet); } virtual bool applies_jet_by_jet() const {return _s.applies_jet_by_jet();} virtual void terminator(vector & jets) const { if (applies_jet_by_jet()){ SelectorWorker::terminator(jets); return; } vector s_jets = jets; _s.worker()->terminator(s_jets); for (unsigned int i=0; i & jets) const { if (applies_jet_by_jet()){ SelectorWorker::terminator(jets); return; } vector s1_jets = jets; _s1.worker()->terminator(s1_jets); _s2.worker()->terminator(jets); for (unsigned int i=0; i & jets) const { if (applies_jet_by_jet()){ SelectorWorker::terminator(jets); return; } vector s1_jets = jets; _s1.worker()->terminator(s1_jets); _s2.worker()->terminator(jets); for (unsigned int i=0; i & jets) const { if (applies_jet_by_jet()){ SelectorWorker::terminator(jets); return; } _s2.worker()->terminator(jets); _s1.worker()->terminator(jets); } virtual string description() const { ostringstream ostr; ostr << "(" << _s1.description() << " * " << _s2.description() << ")"; return ostr.str(); } }; Selector operator*(const Selector & s1, const Selector & s2) { return Selector(new SW_Mult(s1,s2)); } class QuantityBase{ public: QuantityBase(double q) : _q(q){} virtual ~QuantityBase(){} virtual double operator()(const PseudoJet & jet ) const =0; virtual string description() const =0; virtual bool is_geometric() const { return false;} virtual double comparison_value() const {return _q;} virtual double description_value() const {return comparison_value();} protected: double _q; }; class QuantitySquareBase : public QuantityBase{ public: QuantitySquareBase(double sqrtq) : QuantityBase(sqrtq*sqrtq), _sqrtq(sqrtq){} virtual double description_value() const {return _sqrtq;} protected: double _sqrtq; }; template class SW_QuantityMin : public SelectorWorker{ public: SW_QuantityMin(double qmin) : _qmin(qmin) {} virtual bool pass(const PseudoJet & jet) const {return _qmin(jet) >= _qmin.comparison_value();} virtual string description() const { ostringstream ostr; ostr << _qmin.description() << " >= " << _qmin.description_value(); return ostr.str(); } virtual bool is_geometric() const { return _qmin.is_geometric();} protected: QuantityType _qmin; ///< the cut }; template class SW_QuantityMax : public SelectorWorker { public: SW_QuantityMax(double qmax) : _qmax(qmax) {} virtual bool pass(const PseudoJet & jet) const {return _qmax(jet) <= _qmax.comparison_value();} virtual string description() const { ostringstream ostr; ostr << _qmax.description() << " <= " << _qmax.description_value(); return ostr.str(); } virtual bool is_geometric() const { return _qmax.is_geometric();} protected: QuantityType _qmax; ///< the cut }; template class SW_QuantityRange : public SelectorWorker { public: SW_QuantityRange(double qmin, double qmax) : _qmin(qmin), _qmax(qmax) {} virtual bool pass(const PseudoJet & jet) const { double q = _qmin(jet); // we could identically use _qmax return (q >= _qmin.comparison_value()) && (q <= _qmax.comparison_value()); } virtual string description() const { ostringstream ostr; ostr << _qmin.description_value() << " <= " << _qmin.description() << " <= " << _qmax.description_value(); return ostr.str(); } virtual bool is_geometric() const { return _qmin.is_geometric();} protected: QuantityType _qmin; // the lower cut QuantityType _qmax; // the upper cut }; class QuantityPt2 : public QuantitySquareBase{ public: QuantityPt2(double pt) : QuantitySquareBase(pt){} virtual double operator()(const PseudoJet & jet ) const { return jet.perp2();} virtual string description() const {return "pt";} }; Selector SelectorPtMin(double ptmin) { return Selector(new SW_QuantityMin(ptmin)); } Selector SelectorPtMax(double ptmax) { return Selector(new SW_QuantityMax(ptmax)); } Selector SelectorPtRange(double ptmin, double ptmax) { return Selector(new SW_QuantityRange(ptmin, ptmax)); } class QuantityEt2 : public QuantitySquareBase{ public: QuantityEt2(double Et) : QuantitySquareBase(Et){} virtual double operator()(const PseudoJet & jet ) const { return jet.Et2();} virtual string description() const {return "Et";} }; Selector SelectorEtMin(double Etmin) { return Selector(new SW_QuantityMin(Etmin)); } Selector SelectorEtMax(double Etmax) { return Selector(new SW_QuantityMax(Etmax)); } Selector SelectorEtRange(double Etmin, double Etmax) { return Selector(new SW_QuantityRange(Etmin, Etmax)); } class QuantityE : public QuantityBase{ public: QuantityE(double E) : QuantityBase(E){} virtual double operator()(const PseudoJet & jet ) const { return jet.E();} virtual string description() const {return "E";} }; Selector SelectorEMin(double Emin) { return Selector(new SW_QuantityMin(Emin)); } Selector SelectorEMax(double Emax) { return Selector(new SW_QuantityMax(Emax)); } Selector SelectorERange(double Emin, double Emax) { return Selector(new SW_QuantityRange(Emin, Emax)); } class QuantityM2 : public QuantitySquareBase{ public: QuantityM2(double m) : QuantitySquareBase(m){} virtual double operator()(const PseudoJet & jet ) const { return jet.m2();} virtual string description() const {return "mass";} }; Selector SelectorMassMin(double mmin) { return Selector(new SW_QuantityMin(mmin)); } Selector SelectorMassMax(double mmax) { return Selector(new SW_QuantityMax(mmax)); } Selector SelectorMassRange(double mmin, double mmax) { return Selector(new SW_QuantityRange(mmin, mmax)); } class QuantityRap : public QuantityBase{ public: QuantityRap(double rap) : QuantityBase(rap){} virtual double operator()(const PseudoJet & jet ) const { return jet.rap();} virtual string description() const {return "rap";} virtual bool is_geometric() const { return true;} }; class SW_RapMin : public SW_QuantityMin{ public: SW_RapMin(double rapmin) : SW_QuantityMin(rapmin){} virtual void get_rapidity_extent(double &rapmin, double & rapmax) const{ rapmax = std::numeric_limits::max(); rapmin = _qmin.comparison_value(); } }; class SW_RapMax : public SW_QuantityMax{ public: SW_RapMax(double rapmax) : SW_QuantityMax(rapmax){} virtual void get_rapidity_extent(double &rapmin, double & rapmax) const{ rapmax = _qmax.comparison_value(); rapmin = -std::numeric_limits::max(); } }; class SW_RapRange : public SW_QuantityRange{ public: SW_RapRange(double rapmin, double rapmax) : SW_QuantityRange(rapmin, rapmax){ assert(rapmin<=rapmax); } virtual void get_rapidity_extent(double &rapmin, double & rapmax) const{ rapmax = _qmax.comparison_value(); rapmin = _qmin.comparison_value(); } virtual bool has_known_area() const { return true;} ///< the area is analytically known virtual double known_area() const { return twopi * (_qmax.comparison_value()-_qmin.comparison_value()); } }; Selector SelectorRapMin(double rapmin) { return Selector(new SW_RapMin(rapmin)); } Selector SelectorRapMax(double rapmax) { return Selector(new SW_RapMax(rapmax)); } Selector SelectorRapRange(double rapmin, double rapmax) { return Selector(new SW_RapRange(rapmin, rapmax)); } class QuantityAbsRap : public QuantityBase{ public: QuantityAbsRap(double absrap) : QuantityBase(absrap){} virtual double operator()(const PseudoJet & jet ) const { return abs(jet.rap());} virtual string description() const {return "|rap|";} virtual bool is_geometric() const { return true;} }; class SW_AbsRapMax : public SW_QuantityMax{ public: SW_AbsRapMax(double absrapmax) : SW_QuantityMax(absrapmax){} virtual void get_rapidity_extent(double &rapmin, double & rapmax) const{ rapmax = _qmax.comparison_value(); rapmin = -_qmax.comparison_value(); } virtual bool has_known_area() const { return true;} ///< the area is analytically known virtual double known_area() const { return twopi * 2 * _qmax.comparison_value(); } }; class SW_AbsRapRange : public SW_QuantityRange{ public: SW_AbsRapRange(double absrapmin, double absrapmax) : SW_QuantityRange(absrapmin, absrapmax){} virtual void get_rapidity_extent(double &rapmin, double & rapmax) const{ rapmax = _qmax.comparison_value(); rapmin = -_qmax.comparison_value(); } virtual bool has_known_area() const { return true;} ///< the area is analytically known virtual double known_area() const { return twopi * 2 * (_qmax.comparison_value()-max(_qmin.comparison_value(),0.0)); // this should handle properly absrapmin<0 } }; Selector SelectorAbsRapMin(double absrapmin) { return Selector(new SW_QuantityMin(absrapmin)); } Selector SelectorAbsRapMax(double absrapmax) { return Selector(new SW_AbsRapMax(absrapmax)); } Selector SelectorAbsRapRange(double rapmin, double rapmax) { return Selector(new SW_AbsRapRange(rapmin, rapmax)); } class QuantityEta : public QuantityBase{ public: QuantityEta(double eta) : QuantityBase(eta){} virtual double operator()(const PseudoJet & jet ) const { return jet.eta();} virtual string description() const {return "eta";} }; Selector SelectorEtaMin(double etamin) { return Selector(new SW_QuantityMin(etamin)); } Selector SelectorEtaMax(double etamax) { return Selector(new SW_QuantityMax(etamax)); } Selector SelectorEtaRange(double etamin, double etamax) { return Selector(new SW_QuantityRange(etamin, etamax)); } class QuantityAbsEta : public QuantityBase{ public: QuantityAbsEta(double abseta) : QuantityBase(abseta){} virtual double operator()(const PseudoJet & jet ) const { return abs(jet.eta());} virtual string description() const {return "|eta|";} virtual bool is_geometric() const { return true;} }; Selector SelectorAbsEtaMin(double absetamin) { return Selector(new SW_QuantityMin(absetamin)); } Selector SelectorAbsEtaMax(double absetamax) { return Selector(new SW_QuantityMax(absetamax)); } Selector SelectorAbsEtaRange(double absetamin, double absetamax) { return Selector(new SW_QuantityRange(absetamin, absetamax)); } class SW_PhiRange : public SelectorWorker { public: SW_PhiRange(double phimin, double phimax) : _phimin(phimin), _phimax(phimax){ assert(_phimin<_phimax); assert(_phimin>-twopi); assert(_phimax<2*twopi); _phispan = _phimax - _phimin; } virtual bool pass(const PseudoJet & jet) const { double dphi=jet.phi()-_phimin; if (dphi >= twopi) dphi -= twopi; if (dphi < 0) dphi += twopi; return (dphi <= _phispan); } virtual string description() const { ostringstream ostr; ostr << _phimin << " <= phi <= " << _phimax; return ostr.str(); } virtual bool is_geometric() const { return true;} protected: double _phimin; // the lower cut double _phimax; // the upper cut double _phispan; // the span of the range }; Selector SelectorPhiRange(double phimin, double phimax) { return Selector(new SW_PhiRange(phimin, phimax)); } class SW_RapPhiRange : public SW_And{ public: SW_RapPhiRange(double rapmin, double rapmax, double phimin, double phimax) : SW_And(SelectorRapRange(rapmin, rapmax), SelectorPhiRange(phimin, phimax)){ _known_area = ((phimax-phimin > twopi) ? twopi : phimax-phimin) * (rapmax-rapmin); } virtual double known_area() const{ return _known_area; } protected: double _known_area; }; Selector SelectorRapPhiRange(double rapmin, double rapmax, double phimin, double phimax) { return Selector(new SW_RapPhiRange(rapmin, rapmax, phimin, phimax)); } class SW_NHardest : public SelectorWorker { public: SW_NHardest(unsigned int n) : _n(n) {}; virtual bool pass(const PseudoJet &) const { if (!applies_jet_by_jet()) throw Error("Cannot apply this selector worker to an individual jet"); return false; } virtual void terminator(vector & jets) const { if (jets.size() < _n) return; vector minus_pt2(jets.size()); vector indices(jets.size()); for (unsigned int i=0; iperp2() : 0.0; } IndexedSortHelper sort_helper(& minus_pt2); partial_sort(indices.begin(), indices.begin()+_n, indices.end(), sort_helper); for (unsigned int i=_n; i= _radius_in2); } virtual string description() const { ostringstream ostr; ostr << sqrt(_radius_in2) << " <= distance from the centre <= " << sqrt(_radius_out2); return ostr.str(); } virtual void get_rapidity_extent(double & rapmin, double & rapmax) const{ if (! _is_initialised) throw Error("To use a SelectorDoughnut (or any selector that requires a reference), you first have to call set_reference(...)"); rapmax = _reference.rap()+sqrt(_radius_out2); rapmin = _reference.rap()-sqrt(_radius_out2); } virtual bool is_geometric() const { return true;} ///< implies a finite area virtual bool has_finite_area() const { return true;} ///< regardless of the reference virtual bool has_known_area() const { return true;} ///< the area is analytically known virtual double known_area() const { return pi * (_radius_out2-_radius_in2); } protected: double _radius_in2, _radius_out2; }; Selector SelectorDoughnut(const double & radius_in, const double & radius_out) { return Selector(new SW_Doughnut(radius_in, radius_out)); } class SW_Strip : public SW_WithReference { public: SW_Strip(const double &delta) : _delta(delta) {} virtual SelectorWorker* copy(){ return new SW_Strip(*this);} virtual bool pass(const PseudoJet & jet) const { if (! _is_initialised) throw Error("To use a SelectorStrip (or any selector that requires a reference), you first have to call set_reference(...)"); return abs(jet.rap()-_reference.rap()) <= _delta; } virtual string description() const { ostringstream ostr; ostr << "|rap - rap_reference| <= " << _delta; return ostr.str(); } virtual void get_rapidity_extent(double & rapmin, double & rapmax) const{ if (! _is_initialised) throw Error("To use a SelectorStrip (or any selector that requires a reference), you first have to call set_reference(...)"); rapmax = _reference.rap()+_delta; rapmin = _reference.rap()-_delta; } virtual bool is_geometric() const { return true;} ///< implies a finite area virtual bool has_finite_area() const { return true;} ///< regardless of the reference virtual bool has_known_area() const { return true;} ///< the area is analytically known virtual double known_area() const { return twopi * 2 * _delta; } protected: double _delta; }; Selector SelectorStrip(const double & half_width) { return Selector(new SW_Strip(half_width)); } class SW_Rectangle : public SW_WithReference { public: SW_Rectangle(const double &delta_rap, const double &delta_phi) : _delta_rap(delta_rap), _delta_phi(delta_phi) {} virtual SelectorWorker* copy(){ return new SW_Rectangle(*this);} virtual bool pass(const PseudoJet & jet) const { if (! _is_initialised) throw Error("To use a SelectorRectangle (or any selector that requires a reference), you first have to call set_reference(...)"); return (abs(jet.rap()-_reference.rap()) <= _delta_rap) && (abs(jet.delta_phi_to(_reference)) <= _delta_phi); } virtual string description() const { ostringstream ostr; ostr << "|rap - rap_reference| <= " << _delta_rap << " && |phi - phi_reference| <= " << _delta_phi ; return ostr.str(); } virtual void get_rapidity_extent(double & rapmin, double & rapmax) const{ if (! _is_initialised) throw Error("To use a SelectorRectangle (or any selector that requires a reference), you first have to call set_reference(...)"); rapmax = _reference.rap()+_delta_rap; rapmin = _reference.rap()-_delta_rap; } virtual bool is_geometric() const { return true;} ///< implies a finite area virtual bool has_finite_area() const { return true;} ///< regardless of the reference virtual bool has_known_area() const { return true;} ///< the area is analytically known virtual double known_area() const { return 4 * _delta_rap * _delta_phi; } protected: double _delta_rap, _delta_phi; }; Selector SelectorRectangle(const double & half_rap_width, const double & half_phi_width) { return Selector(new SW_Rectangle(half_rap_width, half_phi_width)); } class SW_PtFractionMin : public SW_WithReference { public: SW_PtFractionMin(double fraction) : _fraction2(fraction*fraction){} virtual SelectorWorker* copy(){ return new SW_PtFractionMin(*this);} virtual bool pass(const PseudoJet & jet) const { if (! _is_initialised) throw Error("To use a SelectorPtFractionMin (or any selector that requires a reference), you first have to call set_reference(...)"); return (jet.perp2() >= _fraction2*_reference.perp2()); } virtual string description() const { ostringstream ostr; ostr << "pt >= " << sqrt(_fraction2) << "* pt_ref"; return ostr.str(); } protected: double _fraction2; }; Selector SelectorPtFractionMin(double fraction){ return Selector(new SW_PtFractionMin(fraction)); } class SW_IsZero : public SelectorWorker { public: SW_IsZero(){} virtual bool pass(const PseudoJet & jet) const { return jet==0; } virtual string description() const { return "zero";} }; Selector SelectorIsZero(){ return Selector(new SW_IsZero()); } Selector & Selector::operator &=(const Selector & b){ _worker.reset(new SW_And(*this, b)); return *this; } Selector & Selector::operator |=(const Selector & b){ _worker.reset(new SW_Or(*this, b)); return *this; } FJCORE_END_NAMESPACE // defined in fastjet/internal/base.hh pythia8-8.1.80.orig/src/SigmaCompositeness.cc0000644000175000017500000006171012217346250017252 0ustar sunsun// SigmaCompositeness.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // compositeness simulation classes. #include "Pythia8/SigmaCompositeness.h" namespace Pythia8 { //========================================================================== // Sigma1qg2qStar class. // Cross section for q g -> q^* (excited quark state). //-------------------------------------------------------------------------- // Initialize process. void Sigma1qg2qStar::initProc() { // Set up process properties from the chosen quark flavour. idRes = 4000000 + idq; codeSave = 4000 + idq; if (idq == 1) nameSave = "d g -> d^*"; else if (idq == 2) nameSave = "u g -> u^*"; else if (idq == 3) nameSave = "s g -> s^*"; else if (idq == 4) nameSave = "c g -> c^*"; else nameSave = "b g -> b^*"; // Store q* mass and width for propagator. mRes = particleDataPtr->m0(idRes); GammaRes = particleDataPtr->mWidth(idRes); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Locally stored properties and couplings. Lambda = settingsPtr->parm("ExcitedFermion:Lambda"); coupFcol = settingsPtr->parm("ExcitedFermion:coupFcol"); // Set pointer to particle properties and decay table. qStarPtr = particleDataPtr->particleDataEntryPtr(idRes); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1qg2qStar::sigmaKin() { // Incoming width for correct quark. widthIn = pow3(mH) * alpS * pow2(coupFcol) / (3. * pow2(Lambda)); // Set up Breit-Wigner. sigBW = M_PI/ ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat) for specific incoming flavours. double Sigma1qg2qStar::sigmaHat() { // Identify whether correct incoming flavours. int idqNow = (id2 == 21) ? id1 : id2; if (abs(idqNow) != idq) return 0.; // Outgoing width and total sigma. Done. return widthIn * sigBW * qStarPtr->resWidthOpen(idqNow, mH); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1qg2qStar::setIdColAcol() { // Flavours. int idqNow = (id2 == 21) ? id1 : id2; int idqStar = (idqNow > 0) ? idRes : -idRes; setId( id1, id2, idqStar); // Colour flow topology. if (id1 == idqNow) setColAcol( 1, 0, 2, 1, 2, 0); else setColAcol( 2, 1, 1, 0, 2, 0); if (idqNow < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for q* decay angle. double Sigma1qg2qStar::weightDecay( Event& process, int iResBeg, int iResEnd) { // q* should sit in entry 5. Sequential Z/W decay assumed isotropic. if (iResBeg != 5 || iResEnd != 5) return 1.; // Sign of asymmetry. int sideIn = (process[3].idAbs() < 20) ? 1 : 2; int sideOut = (process[6].idAbs() < 20) ? 1 : 2; double eps = (sideIn == sideOut) ? 1. : -1.; // Phase space factors. double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double betaf = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); // Reconstruct decay angle. Default isotropic decay. double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * betaf); double wt = 1.; double wtMax = 1.; // Decay q* -> q (g/gamma) or q (Z^0/W^+-). int idBoson = (sideOut == 1) ? process[7].idAbs() : process[6].idAbs(); if (idBoson == 21 || idBoson == 22) { wt = 1. + eps * cosThe; wtMax = 2.; } else if (idBoson == 23 || idBoson == 24) { double mrB = (sideOut == 1) ? mr2 : mr1; double ratB = (1. - 0.5 * mrB) / (1 + 0.5 * mrB); wt = 1. + eps * cosThe * ratB; wtMax = 1. + ratB; } // Done. return (wt / wtMax); } //========================================================================== // Sigma1lgm2lStar class. // Cross section for l gamma -> l^* (excited lepton state). //-------------------------------------------------------------------------- // Initialize process. void Sigma1lgm2lStar::initProc() { // Set up process properties from the chosen lepton flavour. idRes = 4000000 + idl; codeSave = 4000 + idl; if (idl == 11) nameSave = "e gamma -> e^*"; else if (idl == 13) nameSave = "mu gamma -> mu^*"; else nameSave = "tau gamma -> tau^*"; // Store l* mass and width for propagator. mRes = particleDataPtr->m0(idRes); GammaRes = particleDataPtr->mWidth(idRes); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Locally stored properties and couplings. Lambda = settingsPtr->parm("ExcitedFermion:Lambda"); double coupF = settingsPtr->parm("ExcitedFermion:coupF"); double coupFp = settingsPtr->parm("ExcitedFermion:coupFprime"); coupChg = -0.5 * coupF - 0.5 * coupFp; // Set pointer to particle properties and decay table. qStarPtr = particleDataPtr->particleDataEntryPtr(idRes); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1lgm2lStar::sigmaKin() { // Incoming width for correct lepton. widthIn = pow3(mH) * alpEM * pow2(coupChg) / pow2(Lambda); // Set up Breit-Wigner. sigBW = M_PI/ ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat) for specific incoming flavours. double Sigma1lgm2lStar::sigmaHat() { // Identify whether correct incoming flavours. int idlNow = (id2 == 22) ? id1 : id2; if (abs(idlNow) != idl) return 0.; // Outgoing width and total sigma. Done. return widthIn * sigBW * qStarPtr->resWidthOpen(idlNow, mH); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1lgm2lStar::setIdColAcol() { // Flavours. int idlNow = (id2 == 22) ? id1 : id2; int idlStar = (idlNow > 0) ? idRes : -idRes; setId( id1, id2, idlStar); // No colour flow. setColAcol( 0, 0, 0, 0, 0, 0); } //-------------------------------------------------------------------------- // Evaluate weight for l* decay angle. double Sigma1lgm2lStar::weightDecay( Event& process, int iResBeg, int iResEnd) { // l* should sit in entry 5. Sequential Z/W decay assumed isotropic. if (iResBeg != 5 || iResEnd != 5) return 1.; // Sign of asymmetry. int sideIn = (process[3].idAbs() < 20) ? 1 : 2; int sideOut = (process[6].idAbs() < 20) ? 1 : 2; double eps = (sideIn == sideOut) ? 1. : -1.; // Phase space factors. double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double betaf = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); // Reconstruct decay angle. Default isotropic decay. double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * betaf); double wt = 1.; double wtMax = 1.; // Decay l* -> l gamma or l (Z^0/W^+-). int idBoson = (sideOut == 1) ? process[7].idAbs() : process[6].idAbs(); if (idBoson == 22) { wt = 1. + eps * cosThe; wtMax = 2.; } else if (idBoson == 23 || idBoson == 24) { double mrB = (sideOut == 1) ? mr2 : mr1; double ratB = (1. - 0.5 * mrB) / (1 + 0.5 * mrB); wt = 1. + eps * cosThe * ratB; wtMax = 1. + ratB; } // Done. return (wt / wtMax); } //========================================================================== // Sigma2qq2qStarq class. // Cross section for q q' -> q^* q' (excited quark state). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qq2qStarq::initProc() { // Set up process properties from the chosen quark flavour. idRes = 4000000 + idq; codeSave = 4020 + idq; if (idq == 1) nameSave = "q q -> d^* q"; else if (idq == 2) nameSave = "q q -> u^* q"; else if (idq == 3) nameSave = "q q -> s^* q"; else if (idq == 4) nameSave = "q q -> c^* q"; else nameSave = "q q -> b^* q"; // Locally stored properties and couplings. Lambda = settingsPtr->parm("ExcitedFermion:Lambda"); preFac = M_PI / pow4(Lambda); // Secondary open width fractions. openFracPos = particleDataPtr->resOpenFrac( idRes); openFracNeg = particleDataPtr->resOpenFrac(-idRes); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2qq2qStarq::sigmaKin() { // Two possible expressions, for like or unlike sign. sigmaA = preFac * (1. - s3 / sH); sigmaB = preFac * (-uH) * (sH + tH) / sH2; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat) for specific incoming flavours. double Sigma2qq2qStarq::sigmaHat() { // Identify different allowed incoming flavour combinations. int id1Abs = abs(id1); int id2Abs = abs(id2); double open1 = (id1 > 0) ? openFracPos : openFracNeg; double open2 = (id2 > 0) ? openFracPos : openFracNeg; double sigma = 0.; if (id1 * id2 > 0) { if (id1Abs == idq) sigma += (4./3.) * sigmaA * open1; if (id2Abs == idq) sigma += (4./3.) * sigmaA * open2; } else if (id1Abs == idq && id2 == -id1) sigma = (8./3.) * sigmaB * (open1 + open2); else if (id2 == -id1) sigma = sigmaB * (open1 + open2); else if (id1Abs == idq) sigma = sigmaB * open1; else if (id2Abs == idq) sigma = sigmaB * open2; // Done. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qq2qStarq::setIdColAcol() { // Flavours: either side may have been excited. int idAbs1 = abs(id1); int idAbs2 = abs(id2); double open1 = 0.; double open2 = 0.; if (idAbs1 == idq) open1 = (id1 > 0) ? openFracPos : openFracNeg; if (idAbs2 == idq) open2 = (id2 > 0) ? openFracPos : openFracNeg; if (open1 == 0. && open2 == 0.) { open1 = (id1 > 0) ? openFracPos : openFracNeg; open2 = (id2 > 0) ? openFracPos : openFracNeg; } bool excite1 = (open1 > 0.); if (open1 > 0. && open2 > 0.) excite1 = (rndmPtr->flat() * (open1 + open2) < open1); // Always excited quark in slot 3 so colour flow flipped or not. if (excite1) { id3 = (id1 > 0) ? idRes : -idRes; id4 = id2; // Special case for s-channel like production. if ((idAbs1 == idAbs2) && (id1 * id2 < 0)) { id4 = (id3 > 0) ? -idq : idq; } if (id1 * id2 > 0) setColAcol( 1, 0, 2, 0, 1, 0, 2, 0); else setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); if (id1 < 0) swapColAcol(); } else { id3 = (id2 > 0) ? idRes : -idRes; id4 = id1; // Special case for s-channel like production. if ((idAbs1 == idAbs2) && (id1 * id2 < 0)) { id4 = (id3 > 0) ? -idq : idq; } swapTU = true; if (id1 * id2 > 0) setColAcol( 1, 0, 2, 0, 2, 0, 1, 0); else setColAcol( 1, 0, 0, 2, 0, 2, 1, 0); if (id1 < 0) swapColAcol(); } setId( id1, id2, id3, id4); } //-------------------------------------------------------------------------- // Evaluate weight for q* decay angle. // SA: Angles dist. for decay q* -> q V, based on Eq. 1.7 // in CERN Yellow Reports 90-10 vol.2, p. 1014 to 1021. double Sigma2qq2qStarq::weightDecay( Event& process, int iResBeg, int iResEnd) { // q* should sit in entry 5. Sequential Z/W decay assumed isotropic. if (iResBeg != 5 && iResEnd != 5) return 1.; // Phase space factors. double mr1 = pow2(process[7].m() / process[5].m()); double mr2 = pow2(process[8].m() / process[5].m()); // Reconstruct decay angle in q* CoM frame. int idAbs3 = process[7].idAbs(); Vec4 pQStarCom = (idAbs3 < 20) ? process[7].p() : process[8].p(); pQStarCom.bstback(process[5].p()); double cosThe = costheta(pQStarCom, process[5].p()); double wt = 1.; // Decay q* -> q (g/gamma) or q (Z^0/W^+-). int idBoson = (idAbs3 < 20) ? process[8].idAbs() : process[7].idAbs(); if (idBoson == 21 || idBoson == 22) { wt = 0.5 * (1. + cosThe); } else if (idBoson == 23 || idBoson == 24) { double mrB = (idAbs3 < 20) ? mr2 : mr1; double kTrm = 0.5 * (mrB * (1. - cosThe)); wt = (1. + cosThe + kTrm) / (2 + mrB); } // Done. return wt; } //========================================================================== // Sigma2qqbar2lStarlbar class. // Cross section for q qbar -> l^* lbar (excited lepton state). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2lStarlbar::initProc() { // Set up process properties from the chosen lepton flavour. idRes = 4000000 + idl; codeSave = 4020 + idl; if (idl == 11) nameSave = "q qbar -> e^*+- e^-+"; else if (idl == 12) nameSave = "q qbar -> nu_e^* nu_ebar"; else if (idl == 13) nameSave = "q qbar -> mu^*+- mu^-+"; else if (idl == 14) nameSave = "q qbar -> nu_mu^* nu_mubar"; else if (idl == 15) nameSave = "q qbar -> tau^*+- tau^-+"; else nameSave = "q qbar -> nu_tau^* nu_taubar"; // Secondary open width fractions. openFracPos = particleDataPtr->resOpenFrac( idRes); openFracNeg = particleDataPtr->resOpenFrac(-idRes); // Locally stored properties and couplings. Lambda = settingsPtr->parm("ExcitedFermion:Lambda"); preFac = (M_PI / pow4(Lambda)) * (openFracPos + openFracNeg) / 3.; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2qqbar2lStarlbar::sigmaKin() { // Only one possible expressions sigma = preFac * (-uH) * (sH + tH) / sH2; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2lStarlbar::setIdColAcol() { // Flavours: either lepton or antilepton may be excited. if (rndmPtr->flat() * (openFracPos + openFracNeg) < openFracPos) { setId( id1, id2, idRes, -idl); if (id1 < 0) swapTU = true; } else { setId( id1, id2, -idRes, idl); if (id1 > 0) swapTU = true; } // Colour flow trivial. if (id1 > 0) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 1, 1, 0, 0, 0, 0, 0); } //-------------------------------------------------------------------------- // Evaluate weight for l* decay angle. // SA: Angles dist. for decay l* -> l V, based on Eq. 1.7 // in CERN Yellow Reports 90-10 vol.2, p. 1014 to 1021. double Sigma2qqbar2lStarlbar::weightDecay( Event& process, int iResBeg, int iResEnd) { // l* should sit in entry 5. Sequential Z/W decay assumed isotropic. if (iResBeg != 5 && iResEnd != 5) return 1.; // Phase space factors. double mr1 = pow2(process[7].m() / process[5].m()); double mr2 = pow2(process[8].m() / process[5].m()); // Reconstruct decay angle in l* CoM frame. int idAbs3 = process[7].idAbs(); Vec4 pLStarCom = (idAbs3 < 20) ? process[7].p() : process[8].p(); pLStarCom.bstback(process[5].p()); double cosThe = costheta(pLStarCom, process[5].p()); double wt = 1.; // Decay, l* -> l + gamma/Z^0/W^+-). int idBoson = (idAbs3 < 20) ? process[8].idAbs() : process[7].idAbs(); if (idBoson == 22) { wt = 0.5 * (1. + cosThe); } else if (idBoson == 23 || idBoson == 24) { double mrB = (idAbs3 < 20) ? mr2 : mr1; double kTrm = 0.5 * (mrB * (1. - cosThe)); wt = (1. + cosThe + kTrm) / (2 + mrB); } // Done. return wt; } //========================================================================== // Sigma2QCqq2qq class. // Cross section for q q -> q q (quark contact interactions). //-------------------------------------------------------------------------- // Initialize process. void Sigma2QCqq2qq::initProc() { qCLambda2 = settingsPtr->parm("ContactInteractions:Lambda"); qCetaLL = settingsPtr->mode("ContactInteractions:etaLL"); qCetaRR = settingsPtr->mode("ContactInteractions:etaRR"); qCetaLR = settingsPtr->mode("ContactInteractions:etaLR"); qCLambda2 *= qCLambda2; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2QCqq2qq::sigmaKin() { // Calculate kinematics dependence for different terms. sigT = (4./9.) * (sH2 + uH2) / tH2; sigU = (4./9.) * (sH2 + tH2) / uH2; sigTU = - (8./27.) * sH2 / (tH * uH); sigST = - (8./27.) * uH2 / (sH * tH); sigQCSTU = sH2 * (1 / tH + 1 / uH); sigQCUTS = uH2 * (1 / tH + 1 / sH); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2QCqq2qq::sigmaHat() { // Terms from QC contact interactions. double sigQCLL = 0; double sigQCRR = 0; double sigQCLR = 0; // Combine cross section terms; factor 1/2 when identical quarks. // q q -> q q if (id2 == id1) { // SM terms. sigSum = 0.5 * (sigT + sigU + sigTU); // Contact terms. sigQCLL = (8./9.) * alpS * (qCetaLL/qCLambda2) * sigQCSTU + (8./3.) * pow2(qCetaLL/qCLambda2) * sH2; sigQCRR = (8./9.) * alpS * (qCetaRR/qCLambda2) * sigQCSTU + (8./3.) * pow2(qCetaRR/qCLambda2) * sH2; sigQCLR = 2. * (uH2 + tH2) * pow2(qCetaLR/qCLambda2); sigQCLL /= 2; sigQCRR /= 2; sigQCLR /= 2; // q qbar -> q qbar, without pure s-channel term. } else if (id2 == -id1) { // SM terms. sigSum = sigT + sigST; // Contact terms, minus the terms included in qqbar2qqbar. sigQCLL = (8./9.) * alpS * (qCetaLL/qCLambda2) * sigQCUTS + (5./3.) * pow2(qCetaLL/qCLambda2) * uH2; sigQCRR = (8./9.) * alpS * (qCetaRR/qCLambda2) * sigQCUTS + (5./3.) * pow2(qCetaRR/qCLambda2) * uH2; sigQCLR = 2. * sH2 * pow2(qCetaLR/qCLambda2); // q q' -> q q' or q qbar' -> q qbar' } else { // SM terms. sigSum = sigT; // Contact terms. if (id1 * id2 > 0) { sigQCLL = pow2(qCetaLL/qCLambda2) * sH2; sigQCRR = pow2(qCetaRR/qCLambda2) * sH2; sigQCLR = 2 * pow2(qCetaLR/qCLambda2) * uH2; } else { sigQCLL = pow2(qCetaLL/qCLambda2) * uH2; sigQCRR = pow2(qCetaRR/qCLambda2) * uH2; sigQCLR = 2 * pow2(qCetaLR/qCLambda2) * sH2; } } // Answer. double sigma = (M_PI/sH2) * ( pow2(alpS) * sigSum + sigQCLL + sigQCRR + sigQCLR ); return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2QCqq2qq::setIdColAcol() { // Outgoing = incoming flavours. setId( id1, id2, id1, id2); // Colour flow topologies. Swap when antiquarks. if (id1 * id2 > 0) setColAcol( 1, 0, 2, 0, 2, 0, 1, 0); else setColAcol( 1, 0, 0, 1, 2, 0, 0, 2); if (id2 == id1 && (sigT + sigU) * rndmPtr->flat() > sigT) setColAcol( 1, 0, 2, 0, 1, 0, 2, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2QCqqbar2qqbar class. // Cross section for q qbar -> q' qbar' (quark contact interactions). //-------------------------------------------------------------------------- // Initialize process. void Sigma2QCqqbar2qqbar::initProc() { qCnQuarkNew = settingsPtr->mode("ContactInteractions:nQuarkNew"); qCLambda2 = settingsPtr->parm("ContactInteractions:Lambda"); qCetaLL = settingsPtr->mode("ContactInteractions:etaLL"); qCetaRR = settingsPtr->mode("ContactInteractions:etaRR"); qCetaLR = settingsPtr->mode("ContactInteractions:etaLR"); qCLambda2 *= qCLambda2; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2QCqqbar2qqbar::sigmaKin() { // Pick new flavour. idNew = 1 + int( qCnQuarkNew * rndmPtr->flat() ); mNew = particleDataPtr->m0(idNew); m2New = mNew*mNew; // Calculate kinematics dependence. double sigQC = 0.; sigS = 0.; if (sH > 4. * m2New) { sigS = (4./9.) * (tH2 + uH2) / sH2; sigQC = pow2(qCetaLL/qCLambda2) * uH2 + pow2(qCetaRR/qCLambda2) * uH2 + 2 * pow2(qCetaLR/qCLambda2) * tH2; } // Answer is proportional to number of outgoing flavours. sigma = (M_PI / sH2) * qCnQuarkNew * ( pow2(alpS) * sigS + sigQC); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2QCqqbar2qqbar::setIdColAcol() { // Set outgoing flavours ones. id3 = (id1 > 0) ? idNew : -idNew; setId( id1, id2, id3, -id3); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2QCffbar2llbar class. // Cross section for f fbar -> l lbar (contact interactions). //-------------------------------------------------------------------------- // Initialize process. void Sigma2QCffbar2llbar::initProc() { qCLambda2 = settingsPtr->parm("ContactInteractions:Lambda"); qCetaLL = settingsPtr->mode("ContactInteractions:etaLL"); qCetaRR = settingsPtr->mode("ContactInteractions:etaRR"); qCetaLR = settingsPtr->mode("ContactInteractions:etaLR"); qCLambda2 *= qCLambda2; // Process name. if (idNew == 11) nameNew = "f fbar -> (QC) -> e- e+"; if (idNew == 13) nameNew = "f fbar -> (QC) -> mu- mu+"; if (idNew == 15) nameNew = "f fbar -> (QC) -> tau- tau+"; // Kinematics. qCmNew = particleDataPtr->m0(idNew); qCmNew2 = qCmNew * qCmNew; qCmZ = particleDataPtr->m0(23); qCmZ2 = qCmZ * qCmZ; qCGZ = particleDataPtr->mWidth(23); qCGZ2 = qCGZ * qCGZ; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2QCffbar2llbar::sigmaKin() { qCPropGm = 1./sH; double denomPropZ = pow2(sH - qCmZ2) + qCmZ2 * qCGZ2; qCrePropZ = (sH - qCmZ2) / denomPropZ; qCimPropZ = -qCmZ * qCGZ / denomPropZ; sigma0 = 0.; if (sH > 4. * qCmNew2) sigma0 = 1./(16. * M_PI * sH2); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. double Sigma2QCffbar2llbar::sigmaHat() { // Incoming fermion flavor. int idAbs = abs(id1); // Couplings and constants. double tmPe2QfQl = 4. * M_PI * alpEM * couplingsPtr->ef(idAbs) * couplingsPtr->ef(idNew); double tmPgvf = 0.25 * couplingsPtr->vf(idAbs); double tmPgaf = 0.25 * couplingsPtr->af(idAbs); double tmPgLf = tmPgvf + tmPgaf; double tmPgRf = tmPgvf - tmPgaf; double tmPgvl = 0.25 * couplingsPtr->vf(idNew); double tmPgal = 0.25 * couplingsPtr->af(idNew); double tmPgLl = tmPgvl + tmPgal; double tmPgRl = tmPgvl - tmPgal; double tmPe2s2c2 = 4. * M_PI * alpEM / (couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); // Complex amplitudes. complex I(0., 1.); complex meLL(0., 0.); complex meRR(0., 0.); complex meLR(0., 0.); complex meRL(0., 0.); // Amplitudes, M = gamma + Z + CI. meLL = tmPe2QfQl * qCPropGm + tmPe2s2c2 * tmPgLf * tmPgLl * (qCrePropZ + I * qCimPropZ) + 4. * M_PI * qCetaLL / qCLambda2; meRR = tmPe2QfQl * qCPropGm + tmPe2s2c2 * tmPgRf * tmPgRl * (qCrePropZ + I * qCimPropZ) + 4. * M_PI * qCetaRR / qCLambda2; meLR = tmPe2QfQl * qCPropGm + tmPe2s2c2 * tmPgLf * tmPgRl * (qCrePropZ + I * qCimPropZ) + 4. * M_PI * qCetaLR / qCLambda2; meRL = tmPe2QfQl * qCPropGm + tmPe2s2c2 * tmPgRf * tmPgLl * (qCrePropZ + I * qCimPropZ) + 4. * M_PI * qCetaLR / qCLambda2; double sigma = sigma0 * uH2 * real(meLL*conj(meLL)); sigma += sigma0 * uH2 * real(meRR*conj(meRR)); sigma += sigma0 * tH2 * real(meLR*conj(meLR)); sigma += sigma0 * tH2 * real(meRL*conj(meRL)); // If f fbar are quarks. if (idAbs < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2QCffbar2llbar::setIdColAcol() { // Flavours trivial. setId(id1, id2, idNew, -idNew); // tH defined between f and f': must swap tHat <-> uHat if id1 is fbar. swapTU = (id2 > 0); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/HadronScatter.cc0000644000175000017500000011206512217346245016203 0ustar sunsun// HadronScatter.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. #include "Pythia8/HadronScatter.h" namespace Pythia8 { //========================================================================== // The SigmaPartialWave class // Reads in tables of partial wave data to provide dSigma/dCos(theta) // The generic classes of process are: // process = 0 (pi-pi), 1 (pi-K), 2 (pi-N) // Subprocesses are defined (along with isospin coefficients) in: // setupSubprocesses(); // Individual subprocesses are selected using: // setSubprocess(subprocess); or setSubprocess(PDG1, PDG2); // Internally, there are two std::map's, to convert between: // subprocess <==> PDG1, PDG2 // // Data are read in from files: // Lines starting with a '#' are comments // Lines starting with 'set' provide options: // set eType [Wcm | Tlab] - energy bins in Wcm or Tlab // set eUnit [MeV | GeV] - energy unit // set input [eta,delta | Sn,delta | Tr,Ti | mod,phi ] // - format of columns in partial waves // set dUnit [deg | rad] - unit of phase shifts // set norm [0 | 1] - normalisation // Column headers give L,2I[,2J] (2J for e.g. piN) // Input types: Sn,delta -> Sn = 1 - eta^2 // mod,phi -> amplitude T_L = |T_L| exp(i phi_L) // Normalisation: 0 -> dSigma/dOmega = 1 / k^2 |T_L|^2 // 1 -> dSigma/dOmega = 16 / s |T_L|^2 // // Internally data is stored as (J = 0 for spinless): // pwData[L * LSHIFT + 2I * ISHIFT + J][energy_bin_centre] = T // where the energy is Wcm in GeV. // // This is stored using std::map's, to take into account that not all // L,I,J states are always present (e.g. negligable contributions or // conservation rules) and that bin sizes are not fixed. // // Re[T] and Im[T] are interpolated between bins and extrapolated down to // threshold from the first two bins. Above energy_bin_centre of the final // bin, no extrapolation is done and the final bin value is always used. // // A simple scheme to provide correct distributions for cos(theta) at a // given CM energy is included. Efficiency is not too bad, but can likely // be greatly improved. // // For each subprocess, a grid in bins of Wcm and cos(theta) is setup with: // setupGrid(); // The size of the grid is set by the constants: // const double SigmaPartialWave::WCMBIN; // const double SigmaPartialWave::CTBIN; // For each bin of (Wcm, ct), the maximum sigma elastic is found by // splitting this bin into subbins multiple times, controlled by: // const int SigmaPartialWave::SUBBIN; // const int SigmaPartialWave::ITER // With the final maxium sigma elastic given by this value multipled by // a safety factor: // const double SigmaPartialWave::GRIDSAFETY // // To pick values of cos(theta) for a given CM energy, a: // pickCosTheta(Wcm); // function is provided. The above grid is used as an overestimate, to // pick properly distributed values of cos(theta). //-------------------------------------------------------------------------- // Constants // pwData[L * LSHIFT + 2I * ISHIFT + J] const int SigmaPartialWave::LSHIFT = 1000000; const int SigmaPartialWave::ISHIFT = 1000; // Convert GeV^-2 to mb const double SigmaPartialWave::CONVERT2MB = 0.389380; // Size of bin in Wcm and cos(theta) const double SigmaPartialWave::WCMBIN = 0.005; const double SigmaPartialWave::CTBIN = 0.2; // Number of subbins and iterations const int SigmaPartialWave::SUBBIN = 2; const int SigmaPartialWave::ITER = 2; // Safety value to add on to grid maxima const double SigmaPartialWave::MASSSAFETY = 0.001; const double SigmaPartialWave::GRIDSAFETY = 0.05; //-------------------------------------------------------------------------- // Perform initialization and store pointers. bool SigmaPartialWave::init(int processIn, string xmlPath, string filename, Info *infoPtrIn, ParticleData *particleDataPtrIn, Rndm *rndmPtrIn) { // Store incoming pointers infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; // Check incoming process is okay if (processIn < 0 || processIn > 2) { infoPtr->errorMsg("Error in SigmaPartialWave::init: " "unknown process"); return false; } process = processIn; // Setup subprocesses and isospin coefficients setupSubprocesses(); setSubprocess(0); // Read in partial-wave data if (!readFile(xmlPath, filename)) return false; // Setup vector for Legendre polynomials PlVec.resize(Lmax); if (Lmax > 0) PlVec[0] = 1.; // And derivatives if needed if (process == 2) { PlpVec.resize(Lmax); if (Lmax > 0) PlpVec[0] = 0.; if (Lmax > 1) PlpVec[1] = 1.; } // Setup grid for integration setupGrid(); return true; } //-------------------------------------------------------------------------- // Read input data file bool SigmaPartialWave::readFile(string xmlPath, string filename) { // Create full path and open file string fullPath = xmlPath + filename; ifstream ifs(fullPath.c_str()); if (!ifs.good()) { infoPtr->errorMsg("Error in SigmaPartialWave::init: " "could not read data file"); return false; } // Default unit settings int eType = 0; // 0 = Wcm, 1 = Tlab int eUnit = 0; // 0 = GeV, 1 = MeV int input = 0; // 0 = eta, delta; 1 = Sn, delta (Sn = 1 - eta^2); // 2 = Treal, Tim, 3 = mod, phi int dUnit = 0; // 0 = deg, 1 = rad norm = 0; // 0 = standard, 1 = sqrt(s) / sqrt(s - 4Mpi^2) // Once we have a header line, each column corresponds to // values of L, I and J. Lmax = Imax = 0; binMax = 0.; vector < int > Lvec, Ivec, Jvec; // Parse the file string line; while (ifs.good()) { // Get line, convert to lowercase and strip leading whitespace getline(ifs, line); for (unsigned int i = 0; i < line.length(); i++) line[i] = tolower(line[i]); string::size_type startPos = line.find_first_not_of(" "); if (startPos != string::npos) line = line.substr(startPos); // Skip blank lines and lines that start with '#' if (line.length() == 0 || line[0] == '#') continue; // Tokenise line on whitespace (spaces or tabs) string lineT = line; vector < string > token; while (true) { startPos = lineT.find_first_of(" "); token.push_back(lineT.substr(0, startPos)); if (startPos == string::npos) break; startPos = lineT.find_first_not_of(" ", startPos + 1); if (startPos == string::npos) break; lineT = lineT.substr(startPos); } // Settings if (token[0] == "set") { bool badSetting = false; // eType if (token[1] == "etype") { if (token[2] == "wcm") eType = 0; else if (token[2] == "tlab") eType = 1; else badSetting = true; // eUnit } else if (token[1] == "eunit") { if (token[2] == "gev") eUnit = 0; else if (token[2] == "mev") eUnit = 1; else badSetting = true; // input } else if (token[1] == "input") { if (token[2] == "eta,delta") input = 0; else if (token[2] == "sn,delta") input = 1; else if (token[2] == "tr,ti") input = 2; else if (token[2] == "mod,phi") input = 3; else badSetting = true; // dUnit } else if (token[1] == "dunit") { if (token[2] == "deg") dUnit = 0; else if (token[2] == "rad") dUnit = 1; else badSetting = true; // norm } else if (token[1] == "norm") { if (token[2] == "0") norm = 0; else if (token[2] == "1") norm = 1; else badSetting = true; } // Bad setting if (badSetting) { infoPtr->errorMsg("Error in SigmaPartialWave::init: " "bad setting line"); return false; } continue; } // Header line if (line.substr(0, 1).find_first_of("0123456789.") != 0) { // Clear current stored L,2I,2J values Lvec.clear(); Ivec.clear(); Jvec.clear(); // Parse header bool badHeader = false; for (unsigned int i = 1; i < token.size(); i++) { // Extract L startPos = token[i].find_first_of(","); if (startPos == string::npos) { badHeader = true; break; } string Lstr = token[i].substr(0, startPos); token[i] = token[i].substr(startPos + 1); // Extract 2I string Istr; startPos = token[i].find_first_of(", "); if (startPos == string::npos) { Istr = token[i]; token[i] = ""; } else { Istr = token[i].substr(0, startPos); token[i] = token[i].substr(startPos + 1); } // Extract 2J string Jstr("0"); if (token[i].length() != 0) Jstr = token[i]; // Convert to integers and store int L, I, J; stringstream Lss(Lstr); Lss >> L; stringstream Iss(Istr); Iss >> I; stringstream Jss(Jstr); Jss >> J; if (Lss.fail() || Iss.fail() || Jss.fail()) { badHeader = true; break; } Lvec.push_back(L); Ivec.push_back(I); Jvec.push_back(J); Lmax = max(Lmax, L); Imax = max(Imax, I); } if (badHeader) { infoPtr->errorMsg("Error in SigmaPartialWave::init: " "malformed header line"); return false; } // Data line } else { bool badData = false; // Check there are the correct number of columns if (token.size() != 2 * Lvec.size() + 1) badData = true; // Extract energy double eNow = 0.; if (!badData) { stringstream eSS(token[0]); eSS >> eNow; if (eSS.fail()) badData = true; // Convert to GeV if needed if (eUnit == 1) eNow *= 1e-3; // Convert to Wcm if needed if (eType == 1) eNow = sqrt(2. * mB * eNow + pow2(mA + mB)); binMax = max(binMax, eNow); } // Extract eta/phase shifts if (!badData) { for (unsigned int i = 1; i < token.size(); i += 2) { // L,2I,2J int LIJidx = (i - 1) / 2; int L = Lvec[LIJidx]; int I = Ivec[LIJidx]; int J = Jvec[LIJidx]; double i1, i2; stringstream i1SS(token[i]); i1SS >> i1; stringstream i2SS(token[i + 1]); i2SS >> i2; if (i1SS.fail() || i2SS.fail()) { badData = true; break; } // Sn to eta if (input == 1) i1 = sqrt(1. - i1); // Degrees to radians if ((input == 0 || input == 1 || input == 3) && dUnit == 0) i2 *= M_PI / 180.; // Convert to Treal and Timg complex T(0., 0.); if (input == 0 || input == 1) { T = (i1 * exp(2. * complex(0., 1.) * i2) - 1.) / 2. / complex(0., 1.); } else if (input == 2) { T = complex(i1, i2); } else if (input == 3) { T = i1 * exp(complex(0., 1.) * i2); } // Store pwData[L * LSHIFT + I * ISHIFT + J][eNow] = T; } } if (badData) { infoPtr->errorMsg("Error in SigmaPartialWave::init: " "malformed data line"); return false; } } } // Make sure it was EOF that caused us to end if (!ifs.eof()) { ifs.close(); return false; } // Maximum values of L and I Lmax++; Imax++; return true; } //-------------------------------------------------------------------------- // Setup isospin coefficients and subprocess mapping void SigmaPartialWave::setupSubprocesses() { // Setup isospin coefficients switch (process) { // pi-pi case 0: // Map subprocess to incoming subprocessMax = 6; sp2in[0] = pair < int, int > ( 211, 211); sp2in[1] = pair < int, int > ( 211, -211); sp2in[2] = pair < int, int > ( 211, 111); sp2in[3] = pair < int, int > ( 111, 111); sp2in[4] = pair < int, int > (-211, 111); sp2in[5] = pair < int, int > (-211, -211); // Incoming to subprocess for (int i = 0; i < subprocessMax; i++) in2sp[sp2in[i]] = i; // Isospin coefficients isoCoeff[0][0] = 0.; isoCoeff[0][2] = 0.; isoCoeff[0][4] = 1.; isoCoeff[1][0] = 1./3.; isoCoeff[1][2] = 1./2.; isoCoeff[1][4] = 1./6.; isoCoeff[2][0] = 0.; isoCoeff[2][2] = 1./2.; isoCoeff[2][4] = 1./2.; isoCoeff[3][0] = 1./3.; isoCoeff[3][2] = 0.; isoCoeff[3][4] = 2./3.; isoCoeff[4][0] = 0.; isoCoeff[4][2] = 1./2.; isoCoeff[4][4] = 1./2.; isoCoeff[5][0] = 0.; isoCoeff[5][2] = 0.; isoCoeff[5][4] = 1.; break; // pi-K and pi-N case 1: case 2: int id1, id2; if (process == 1) { id1 = 321; id2 = 311; } else { id1 = 2212; id2 = 2112; } // Map subprocess to incoming subprocessMax = 12; sp2in[0] = pair < int, int > ( 211, id1); sp2in[1] = pair < int, int > ( 211, id2); sp2in[2] = pair < int, int > ( 111, id1); sp2in[3] = pair < int, int > ( 111, id2); sp2in[4] = pair < int, int > (-211, id1); sp2in[5] = pair < int, int > (-211, id2); // Isospin coefficients isoCoeff[0][1] = 0.; isoCoeff[0][3] = 1.; isoCoeff[1][1] = 2. / 3.; isoCoeff[1][3] = 1. / 3.; isoCoeff[2][1] = 1. / 3.; isoCoeff[2][3] = 2. / 3.; isoCoeff[3][1] = 1. / 3.; isoCoeff[3][3] = 2. / 3.; isoCoeff[4][1] = 2. / 3.; isoCoeff[4][3] = 1. / 3.; isoCoeff[5][1] = 0.; isoCoeff[5][3] = 1.; // Antiparticles for (int i = 0; i < 6; i++) { id1 = ((sp2in[i].first == 111) ? +1 : -1) * sp2in[i].first; sp2in[i + 6] = pair < int, int > (id1, -sp2in[i].second); isoCoeff[i + 6] = isoCoeff[i]; } // Map incoming to subprocess for (int i = 0; i < subprocessMax; i++) in2sp[sp2in[i]] = i; break; } return; } //-------------------------------------------------------------------------- // Setup grids for integration void SigmaPartialWave::setupGrid() { // Reset sigma maximum sigElMax = 0.; // Go through each subprocess gridMax.resize(subprocessMax); gridNorm.resize(subprocessMax); for (int sp = 0; sp < subprocessMax; sp++) { // Setup subprocess setSubprocess(sp); // Bins in Wcm int nBin1 = int( (binMax - mA - mB) / WCMBIN ); gridMax[subprocess].resize(nBin1); gridNorm[subprocess].resize(nBin1); for (int n1 = 0; n1 < nBin1; n1++) { // Bin lower and upper double bl1 = mA + mB + double(n1) * WCMBIN; double bu1 = bl1 + WCMBIN; // Bins in cos(theta) int nBin2 = int( 2. / CTBIN ); gridMax[subprocess][n1].resize(nBin2); for (int n2 = 0; n2 < nBin2; n2++) { // Bin lower and upper double bl2 = -1. + double(n2) * CTBIN; double bu2 = bl2 + CTBIN; // Find maximum double maxSig = 0.; double bl3 = bl1, bu3 = bu1, bl4 = bl2, bu4 = bu2; for (int iter = 0; iter < ITER; iter++) { int i3Save = -1, i4Save = -1; double step3 = (bu3 - bl3) / double(SUBBIN); double step4 = (bu4 - bl4) / double(SUBBIN); for (int i3 = 0; i3 <= SUBBIN; i3++) { double Wcm = bl3 + double(i3) * step3; for (int i4 = 0; i4 <= SUBBIN; i4++) { double ct = bl4 + double(i4) * step4; double ds = dSigma(Wcm, ct); if (ds > maxSig) { i3Save = i3; i4Save = i4; maxSig = ds; } } } // Set new min/max if (i3Save == -1 && i4Save == -1) break; if (i3Save > -1) { bl3 = bl3 + ((i3Save == 0) ? 0. : i3Save - 1.) * step3; bu3 = bl3 + ((i3Save == SUBBIN) ? 1. : 2.) * step3; } if (i4Save > -1) { bl4 = bl4 + ((i4Save == 0) ? 0. : i4Save - 1.) * step4; bu4 = bl4 + ((i4Save == SUBBIN) ? 1. : 2.) * step4; } } // for (iter) // Save maximum value gridMax[subprocess][n1][n2] = maxSig * (1. + GRIDSAFETY); gridNorm[subprocess][n1] += maxSig * (1. + GRIDSAFETY) * CTBIN; sigElMax = max(sigElMax, maxSig); } // for (n2) } // for (n1) } // for (sp) return; } //-------------------------------------------------------------------------- // Pick a cos(theta) value double SigmaPartialWave::pickCosTheta(double Wcm) { // Find grid bin in Wcm int WcmBin = int((Wcm - mA - mB) / WCMBIN); if (WcmBin < 0) WcmBin = 0; if (WcmBin >= int(gridMax[subprocess].size())) WcmBin = int(gridMax[subprocess].size() - 1); // Pick a value of cos(theta) double ct, wgt; do { // Sample from overestimate and inverse double y = rndmPtr->flat() * gridNorm[subprocess][WcmBin]; double sum = 0.; int ctBin; for (ctBin = 0; ctBin < int(2. / CTBIN); ctBin++) { if (sum + CTBIN * gridMax[subprocess][WcmBin][ctBin] > y) break; sum += CTBIN * gridMax[subprocess][WcmBin][ctBin]; } // Linear interpolation double x1 = -1. + CTBIN * double(ctBin); double y1 = sum; double x2 = x1 + CTBIN; double y2 = sum + CTBIN * gridMax[subprocess][WcmBin][ctBin]; ct = (x2 - x1) / (y2 - y1) * (y - y1) + x1; wgt = dSigma(Wcm, ct) / gridMax[subprocess][WcmBin][ctBin]; if (wgt >= 1.) { infoPtr->errorMsg("Warning in SigmaPartialWave::pickCosTheta: " "weight above unity"); break; } } while (wgt <= rndmPtr->flat()); return ct; } //-------------------------------------------------------------------------- // Set subprocess bool SigmaPartialWave::setSubprocess(int spIn) { if (sp2in.find(spIn) == sp2in.end()) return false; subprocess = spIn; pair < int, int > in = sp2in[spIn]; idA = in.first; mA = particleDataPtr->m0(idA); idB = in.second; mB = particleDataPtr->m0(idB); return true; } bool SigmaPartialWave::setSubprocess(int idAin, int idBin) { pair < int, int > in = pair < int, int > (idAin, idBin); if (in2sp.find(in) == in2sp.end()) { // Try the other way around as well swap(in.first, in.second); if (in2sp.find(in) == in2sp.end()) return false; } subprocess = in2sp[in]; idA = idAin; mA = particleDataPtr->m0(idA); idB = idBin; mB = particleDataPtr->m0(idB); return true; } //-------------------------------------------------------------------------- // Calculate: mode = 0 (sigma elastic), 1 (sigma total), 2 (dSigma/dcTheta) double SigmaPartialWave::sigma(int mode, double Wcm, double cTheta) { // Below threshold, return 0 if (Wcm < (mA + mB + MASSSAFETY)) return 0.; // Return values complex amp[2] = { complex(0., 0.) }; double sig = 0.; // Kinematic variables double s = pow2(Wcm); double k2 = (s - pow2(mB + mA)) * (s - pow2(mB - mA)) / 4. / s; // Precompute all required Pl and Pl' values double sTheta = 0.; if (mode == 2) { if (process == 2) sTheta = sqrt(1. - pow2(cTheta)); legendreP(cTheta, ((process == 2) ? true : false)); } // Loop over L for (int L = 0; L < Lmax; L++) { // Loop over J (only J = 0 for spinless) complex ampJ[2] = { complex(0., 0.) }; int Jstart = (process != 2) ? 0 : 2 * L - 1; int Jend = (process != 2) ? 1 : 2 * L + 2; int Jstep = (process != 2) ? 1 : 2; int Jcount = 0; for (int J = Jstart; J < Jend; J += Jstep, Jcount++) { // Loop over isospin coefficients for (int I = 0; I < Imax; I++) { if (isoCoeff[subprocess][I] == 0.) continue; // Check wave exists int LIJ = L * LSHIFT + I * ISHIFT + J; if (pwData.find(LIJ) == pwData.end()) continue; // Extrapolation / interpolation (not for last bin) map < double, complex >::iterator it = pwData[LIJ].upper_bound(Wcm); if (it == pwData[LIJ].begin()) ++it; double ar, ai; if (it == pwData[LIJ].end()) { ar = (--it)->second.real(); ai = it->second.imag(); } else { double eA = it->first; complex ampA = (it--)->second; double eB = it->first; complex ampB = it->second; ar = (ampA.real() - ampB.real()) / (eA - eB) * (Wcm - eB) + ampB.real(); ai = (ampA.imag() - ampB.imag()) / (eA - eB) * (Wcm - eB) + ampB.imag(); } // Isospin sum ampJ[Jcount] += isoCoeff[subprocess][I] * complex(ar, ai); } } // Partial wave sum. Sigma elastic if (mode == 0) { if (process == 0 || process == 1) { sig += (2. * L + 1.) * (ampJ[0] * conj(ampJ[0])).real(); } else if (process == 2) { sig += ( (L + 0.) * (ampJ[0] * conj(ampJ[0])).real() + (L + 1.) * (ampJ[1] * conj(ampJ[1])).real() ); } // Sigma total } else if (mode == 1) { if (process == 0 || process == 1) { sig += (2. * L + 1.) * ampJ[0].imag(); } else if (process == 2) { sig += ( (L + 0.) * ampJ[0].imag() + (L + 1.) * ampJ[1].imag() ); } // dSigma } else if (mode == 2) { if (process == 0 || process == 1) { amp[0] += (2. * L + 1.) * ampJ[0] * PlVec[L]; } else if (process == 2) { amp[0] += ((L + 0.) * ampJ[0] + double(L + 1.) * ampJ[1]) * PlVec[L]; amp[1] += complex(0., 1.) * (ampJ[1] - ampJ[0]) * sTheta * PlpVec[L]; } } } // for (L) // Normalisation and return if (mode == 0 || mode == 1) { if (norm == 0) sig *= 4. * M_PI / k2 * CONVERT2MB; else if (norm == 1) sig *= 64. * M_PI / s * CONVERT2MB; } else if (mode == 2) { sig = (amp[0] * conj(amp[0])).real() + (amp[1] * conj(amp[1])).real(); if (norm == 0) sig *= 2. * M_PI / k2 * CONVERT2MB; else if (norm == 1) sig *= 32. * M_PI / s * CONVERT2MB; } // Half for identical return ((idA == idB) ? 0.5 : 1.) * sig; } //-------------------------------------------------------------------------- // Bonnet's recursion formula for Legendre polynomials and derivatives void SigmaPartialWave::legendreP(double ct, bool deriv) { if (Lmax > 1) PlVec[1] = ct; for (int L = 2; L < Lmax; L++) { PlVec[L] = ( (2. * L - 1.) * ct * PlVec[L - 1] - (L - 1.) * PlVec[L - 2] ) / double(L); if (deriv) PlpVec[L] = ( (2. * L - 1.) * (PlVec[L - 1] + ct * PlpVec[L - 1]) - (L - 1.) * PlpVec[L - 2] ) / double(L); } return; } //========================================================================== // HadronScatter class //-------------------------------------------------------------------------- // Perform initialization and store pointers. bool HadronScatter::init(Info* infoPtrIn, Settings& settings, Rndm *rndmPtrIn, ParticleData *particleDataPtr) { // Save incoming pointers infoPtr = infoPtrIn; rndmPtr = rndmPtrIn; // Main settings doHadronScatter = settings.flag("HadronScatter:scatter"); afterDecay = settings.flag("HadronScatter:afterDecay"); allowDecayProd = settings.flag("HadronScatter:allowDecayProd"); scatterRepeat = settings.flag("HadronScatter:scatterRepeat"); // Hadron selection hadronSelect = settings.mode("HadronScatter:hadronSelect"); Npar = settings.parm("HadronScatter:N"); kPar = settings.parm("HadronScatter:k"); pPar = settings.parm("HadronScatter:p"); // Scattering probability scatterProb = settings.mode("HadronScatter:scatterProb"); jPar = settings.parm("HadronScatter:j"); rMax = settings.parm("HadronScatter:rMax"); rMax2 = rMax * rMax; doTile = settings.flag("HadronScatter:tile"); // String fragmentation and MPI settings pTsigma = 2.0 * settings.parm("StringPT:sigma"); pTsigma2 = pTsigma * pTsigma; double pT0ref = settings.parm("MultipartonInteractions:pT0ref"); double eCMref = settings.parm("MultipartonInteractions:eCMref"); double eCMpow = settings.parm("MultipartonInteractions:eCMpow"); double eCMnow = infoPtr->eCM(); pT0MPI = pT0ref * pow(eCMnow / eCMref, eCMpow); // Tiling double mp2 = particleDataPtr->m0(111) * particleDataPtr->m0(111); double eA = infoPtr->eA(); double eB = infoPtr->eB(); double pzA = sqrt(eA * eA - mp2); double pzB = -sqrt(eB * eB - mp2); yMax = 0.5 * log((eA + pzA) / (eA - pzA)); yMin = 0.5 * log((eB + pzB) / (eB - pzB)); // Size in y and phi if (doTile) { ytMax = int((yMax - yMin) / rMax); ytSize = (yMax - yMin) / double(ytMax); ptMax = int(2. * M_PI / rMax); ptSize = 2. * M_PI / double(ptMax); } else { ytMax = 1; ytSize = yMax - yMin; ptMax = 1; ptSize = 2. * M_PI; } // Initialise tiles tile.resize(ytMax); for (int yt = 0; yt < ytMax; yt++) tile[yt].resize(ptMax); // Find path to data files, i.e. xmldoc directory location. // Environment variable takes precedence, else use constructor input. // XXX - as in Pythia.cc, but not passed around in e.g. Info/Settings, // so redo here string xmlPath = ""; const char* PYTHIA8DATA = "PYTHIA8DATA"; char* envPath = getenv(PYTHIA8DATA); if (envPath != 0 && *envPath != '\0') { int i = 0; while (*(envPath+i) != '\0') xmlPath += *(envPath+(i++)); } else xmlPath = "../xmldoc"; if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; // Hadron scattering partial wave cross sections if ( !sigmaPW[0].init(0, xmlPath, "pipi-Froggatt.dat", infoPtr, particleDataPtr, rndmPtr) ) return false; if ( !sigmaPW[1].init(1, xmlPath, "piK-Estabrooks.dat", infoPtr, particleDataPtr, rndmPtr) ) return false; if ( !sigmaPW[2].init(2, xmlPath, "piN-SAID-WI08.dat", infoPtr, particleDataPtr, rndmPtr) ) return false; sigElMax = 0.; sigElMax = max(sigElMax, sigmaPW[0].getSigmaElMax()); sigElMax = max(sigElMax, sigmaPW[1].getSigmaElMax()); sigElMax = max(sigElMax, sigmaPW[2].getSigmaElMax()); // DEBUG debugOutput(); return true; } //-------------------------------------------------------------------------- // Debug output void HadronScatter::debugOutput() { // Print settings cout << "Hadron scattering:" << endl << " scatter = " << ((doHadronScatter) ? "on" : "off") << endl << " afterDecay = " << ((afterDecay) ? "on" : "off") << endl << " allowDecayProd = " << ((allowDecayProd) ? "on" : "off") << endl << " scatterRepeat = " << ((scatterRepeat) ? "on" : "off") << endl << " tile = " << ((doTile) ? "on" : "off") << endl << " yMin = " << yMin << endl << " yMax = " << yMax << endl << " ytMax = " << ytMax << endl << " ytSize = " << ytSize << endl << " ptMax = " << ptMax << endl << " ptSize = " << ptSize << endl << endl << " hadronSelect = " << hadronSelect << endl << " N = " << Npar << endl << " k = " << kPar << endl << " p = " << pPar << endl << endl << " scatterProb = " << scatterProb << endl << " j = " << jPar << endl << " rMax = " << rMax << endl << endl << " pTsigma = " << pTsigma2 << endl << " pT0MPI = " << pT0MPI << endl << endl << " sigElMax = " << sigElMax << endl << endl; return; } //-------------------------------------------------------------------------- // Perform hadron scattering void HadronScatter::scatter(Event& event) { // Reset tiles for (int yt = 0; yt < ytMax; yt++) for (int pt = 0; pt < ptMax; pt++) tile[yt][pt].clear(); // Generate list of hadrons which can take part in the scattering for (int i = 0; i < event.size(); i++) if (event[i].isFinal() && event[i].isHadron() && canScatter(event, i)) tile[yTile(event, i)][pTile(event, i)].insert(HSIndex(i, i)); // Generate all pairwise interaction probabilities vector < HadronScatterPair > scatterList; // For each tile and for each hadron in the tile do pairing for (int pt1 = 0; pt1 < ptMax; pt1++) for (int yt1 = 0; yt1 < ytMax; yt1++) for (set < HSIndex >::iterator si1 = tile[yt1][pt1].begin(); si1 != tile[yt1][pt1].end(); si1++) tileIntProb(scatterList, event, *si1, yt1, pt1, false); // Sort by ordering measure (largest to smallest) sort(scatterList.rbegin(), scatterList.rend()); // Reset list of things that have scattered if (scatterRepeat) scattered.clear(); // Do scatterings while (scatterList.size() > 0) { // Check still valid and scatter HadronScatterPair &hsp = scatterList[0]; if (!event[hsp.i1.second].isFinal() || !event[hsp.i2.second].isFinal()) { scatterList.erase(scatterList.begin()); continue; } // Remove old entries in tiles and scatter tile[hsp.yt1][hsp.pt1].erase(hsp.i1); tile[hsp.yt2][hsp.pt2].erase(hsp.i2); hadronScatter(event, hsp); // Store new indices for later HSIndex iNew1 = hsp.i1, iNew2 = hsp.i2; // Check if hadrons can scatter again bool resort = false; if (scatterRepeat) { // Check for new scatters of iNew1 and iNew2 HSIndex iNew = iNew1; for (int i = 0; i < 2; i++) { if (canScatter(event, iNew.second)) { // If both can scatter again, make sure they can't scatter // with each other if (i == 1) scattered.insert(HSIndex(min(iNew1.first, iNew2.first), max(iNew1.first, iNew2.first))); int yt = yTile(event, iNew.second); int pt = pTile(event, iNew.second); resort = tileIntProb(scatterList, event, iNew, yt, pt, true); tile[yt][pt].insert(iNew); } iNew = iNew2; } // for (i) } // if (scatterRepeat) // Remove the old entry and onto next scatterList.erase(scatterList.begin()); // Resort list if anything added if (resort) sort(scatterList.rbegin(), scatterList.rend()); } // while (scatterList.size() > 0) // Done. return; } //-------------------------------------------------------------------------- // Criteria for if a hadron is allowed to scatter or not bool HadronScatter::canScatter(Event& event, int i) { // Probability to accept double p = 0.; // Pions, K+, K-, p+, pbar- only if (scatterProb == 1 || scatterProb == 2) if (event[i].idAbs() != 111 && event[i].idAbs() != 211 && event[i].idAbs() != 321 && event[i].idAbs() != 2212) return false; // Probability switch (hadronSelect) { case 0: double t1 = exp( - event[i].pT2() / 2. / pTsigma2); double t2 = pow(pT0MPI, pPar) / pow(pT0MPI * pT0MPI + event[i].pT2(), pPar / 2.); p = Npar * t1 / ( (1 - kPar) * t1 + kPar * t2 ); break; } // Return true/false if (p > rndmPtr->flat()) return true; else return false; } //-------------------------------------------------------------------------- // Probability for scattering bool HadronScatter::doesScatter(Event& event, const HSIndex &i1, const HSIndex &i2) { Particle &p1 = event[i1.second]; Particle &p2 = event[i2.second]; // Can't come from the same decay if (!allowDecayProd && event[i1.first].mother1() == event[i2.first].mother1() && event[event[i1.first].mother1()].isHadron()) return false; // Check that the two hadrons have not already scattered if (scatterRepeat && scattered.find(HSIndex(min(i1.first, i2.first), max(i1.first, i2.first))) != scattered.end()) return false; // K-K, p-p and K-p not allowed int id1 = min(p1.idAbs(), p2.idAbs()); int id2 = max(p1.idAbs(), p2.idAbs()); if (scatterProb == 1 || scatterProb == 2) { if ((id1 == 321 || id1 == 2212) && id1 == id2) return false; if (id1 == 321 && id2 == 2212) return false; } // Distance in y - phi space double dy = p1.y() - p2.y(); double dp = abs(p1.phi() - p2.phi()); if (dp > M_PI) dp = 2 * M_PI - dp; double dr2 = dy * dy + dp * dp; double p = max(0., 1. - dr2 / rMax2); // Additional factor depending on scatterProb if (scatterProb == 0 || scatterProb == 1) { p *= jPar; // Additional pair dependent probability } else if (scatterProb == 2) { // Wcm and which partial wave amplitude to use double Wcm = (p1.p() + p2.p()).mCalc(); int pw = 0; if ((id1 == 111 || id1 == 211) && (id2 == 111 || id2 == 211)) pw = 0; else if ((id1 == 111 || id1 == 211) && id2 == 321) pw = 1; else if ((id1 == 111 || id1 == 211) && id2 == 2212) pw = 2; else { infoPtr->errorMsg("Error in HadronScatter::doesScatter:" "unknown subprocess"); } if (!sigmaPW[pw].setSubprocess(p1.id(), p2.id())) { infoPtr->errorMsg("Error in HadronScatter::doesScatter:" "setSubprocess failed"); } else { p *= 1 - exp(-jPar * sigmaPW[pw].sigmaEl(Wcm)); } } // Return true/false return (p > rndmPtr->flat()); } //-------------------------------------------------------------------------- // Calculate ordering measure double HadronScatter::measure(Event& event, int idx1, int idx2) { Particle &p1 = event[idx1]; Particle &p2 = event[idx2]; return abs(p1.pT() / p1.mT() - p2.pT() / p2.mT()); } //-------------------------------------------------------------------------- // Scatter a pair bool HadronScatter::hadronScatter(Event& event, HadronScatterPair &hsp) { bool doSwap = (0.5 < rndmPtr->flat()) ? true : false; if (doSwap) swap(hsp.i1, hsp.i2); Particle &p1 = event[hsp.i1.second]; Particle &p2 = event[hsp.i2.second]; // Pick theta and phi (always flat) double ct = 0., phi = 2 * M_PI * rndmPtr->flat(); // Flat for all flavours if (scatterProb == 0 || scatterProb == 1) { ct = 2. * rndmPtr->flat() - 1.; // pi-pi, pi-K and pi-p only using partial wave amplitudes } else if (scatterProb == 2) { // Wcm and which partial wave amplitude to use int id1 = min(p1.idAbs(), p2.idAbs()); int id2 = max(p1.idAbs(), p2.idAbs()); double Wcm = (p1.p() + p2.p()).mCalc(); int pw = 0; if ((id1 == 111 || id1 == 211) && (id2 == 111 || id2 == 211)) pw = 0; else if ((id1 == 111 || id1 == 211) && id2 == 321) pw = 1; else if ((id1 == 111 || id1 == 211) && id2 == 2212) pw = 2; else { infoPtr->errorMsg("Error in HadronScatter::hadronScatter:" "unknown subprocess"); } sigmaPW[pw].setSubprocess(p1.id(), p2.id()); ct = sigmaPW[pw].pickCosTheta(Wcm); } // Rotation RotBstMatrix sMat; sMat.toCMframe(p1.p(), p2.p()); sMat.rot(acos(ct), phi); sMat.fromCMframe(p1.p(), p2.p()); Vec4 v1 = p1.p(), v2 = p2.p(); v1.rotbst(sMat); v2.rotbst(sMat); // Update event record int iNew1 = event.copy(hsp.i1.second, 98); event[iNew1].p(v1); event[iNew1].e(event[iNew1].eCalc()); event[hsp.i1.second].statusNeg(); int iNew2 = event.copy(hsp.i2.second, 98); event[iNew2].p(v2); event[iNew2].e(event[iNew2].eCalc()); event[hsp.i2.second].statusNeg(); // New indices in event record hsp.i1.second = iNew1; hsp.i2.second = iNew2; if (doSwap) swap(hsp.i1, hsp.i2); return true; } //-------------------------------------------------------------------------- // Calculate pair interaction probabilities in nearest-neighbour tiles // (yt1, pt1) represents centre cell (8): // 7 | 0 | 1 // ----------- // 6 | 8 | 2 // ----------- // 5 | 4 | 3 bool HadronScatter::tileIntProb(vector < HadronScatterPair > &hsp, Event &event, const HSIndex &i1, int yt1, int pt1, bool doAll) { // Track if a new pair is added bool pairAdded = false; // Special handling for pairing in own tile if (!doAll) { set < HSIndex >::iterator si2 = tile[yt1][pt1].find(i1); while (++si2 != tile[yt1][pt1].end()) // Calculate if scatters if (doesScatter(event, i1, *si2)) { double m = measure(event, i1.second, si2->second); hsp.push_back(HadronScatterPair(i1, yt1, pt1, *si2, yt1, pt1, m)); } } // And the rest int tileMax = (doAll) ? 9 : 4; for (int tileNow = 0; tileNow < tileMax; tileNow++) { // New (yt, pt) coordinate int yt2 = yt1, pt2 = pt1; switch (tileNow) { case 0: ++pt2; break; case 1: ++yt2; ++pt2; break; case 2: ++yt2; break; case 3: ++yt2; --pt2; break; case 4: --pt2; break; case 5: --yt2; --pt2; break; case 6: --yt2; break; case 7: --yt2; ++pt2; break; } // Limit in rapidity tiles if (yt2 < 0 || yt2 >= ytMax) continue; // Wraparound for phi tiles if (pt2 < 0) { pt2 = ptMax - 1; if (pt2 == pt1 || pt2 == pt1 + 1) continue; } else if (pt2 >= ptMax) { pt2 = 0; if (pt2 == pt1 || pt2 == pt1 - 1) continue; } // Interaction probability for (set < HSIndex >::iterator si2 = tile[yt2][pt2].begin(); si2 != tile[yt2][pt2].end(); si2++) { // Calculate if scatters if (doesScatter(event, i1, *si2)) { double m = measure(event, i1.second, si2->second); hsp.push_back(HadronScatterPair(i1, yt1, pt1, *si2, yt2, pt2, m)); pairAdded = true; } } } return pairAdded; } //========================================================================== } // namespace Pythia8 pythia8-8.1.80.orig/src/BeamParticle.cc0000644000175000017500000007467312217346244016005 0ustar sunsun// BeamParticle.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // BeamParticle class. #include "Pythia8/BeamParticle.h" namespace Pythia8 { //========================================================================== // The BeamParticle class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // A lepton that takes (almost) the full beam energy does not leave a remnant. const double BeamParticle::XMINUNRESOLVED = 1. - 1e-10; //-------------------------------------------------------------------------- // Initialize data on a beam particle and save pointers. void BeamParticle::init( int idIn, double pzIn, double eIn, double mIn, Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn,PDF* pdfInPtr, PDF* pdfHardInPtr, bool isUnresolvedIn, StringFlav* flavSelPtrIn) { // Store input pointers (and one bool) for future use. infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; pdfBeamPtr = pdfInPtr; pdfHardBeamPtr = pdfHardInPtr; isUnresolvedBeam = isUnresolvedIn; flavSelPtr = flavSelPtrIn; // Maximum quark kind in allowed incoming beam hadrons. maxValQuark = settings.mode("BeamRemnants:maxValQuark"); // Power of (1-x)^power/sqrt(x) for remnant valence quark distribution. valencePowerMeson = settings.parm("BeamRemnants:valencePowerMeson"); valencePowerUinP = settings.parm("BeamRemnants:valencePowerUinP"); valencePowerDinP = settings.parm("BeamRemnants:valencePowerDinP"); // Enhancement factor of x of diquark. valenceDiqEnhance = settings.parm("BeamRemnants:valenceDiqEnhance"); // Assume g(x) ~ (1-x)^power/x to constrain companion to sea quark. companionPower = settings.mode("BeamRemnants:companionPower"); // Assume g(x) ~ (1-x)^power/x to constrain companion to sea quark. companionPower = settings.mode("BeamRemnants:companionPower"); // Allow or not more than one valence quark to be kicked out. allowJunction = settings.flag("BeamRemnants:allowJunction"); // For low-mass diffractive system kick out q/g = norm / mass^power. pickQuarkNorm = settings.parm("Diffraction:pickQuarkNorm"); pickQuarkPower = settings.parm("Diffraction:pickQuarkPower"); // Width of primordial kT distribution in low-mass diffractive systems. diffPrimKTwidth = settings.parm("Diffraction:primKTwidth"); // Suppress large masses of beam remnant in low-mass diffractive systems. diffLargeMassSuppress = settings.parm("Diffraction:largeMassSuppress"); // Store info on the incoming beam. idBeam = idIn; initBeamKind(); pBeam = Vec4( 0., 0., pzIn, eIn); mBeam = mIn; } //-------------------------------------------------------------------------- // Initialize kind and valence flavour content of incoming beam. // For recognized hadrons one can generate multiparton interactions. // Dynamic choice of meson valence flavours in newValenceContent below. void BeamParticle::initBeamKind() { // Reset. idBeamAbs = abs(idBeam); isLeptonBeam = false; isHadronBeam = false; isMesonBeam = false; isBaryonBeam = false; nValKinds = 0; // Check for leptons. if (idBeamAbs > 10 && idBeamAbs < 17) { nValKinds = 1; nVal[0] = 1; idVal[0] = idBeam; isLeptonBeam = true; } // Done if cannot be lowest-lying hadron state. if (idBeamAbs < 101 || idBeamAbs > 9999) return; // Resolve valence content for assumed Pomeron. if (idBeamAbs == 990) { isMesonBeam = true; nValKinds = 2; nVal[0] = 1 ; nVal[1] = 1 ; newValenceContent(); // Resolve valence content for assumed meson. Flunk unallowed codes. } else if (idBeamAbs < 1000) { int id1 = idBeamAbs/100; int id2 = (idBeamAbs/10)%10; if ( id1 < 1 || id1 > maxValQuark || id2 < 1 || id2 > maxValQuark ) return; isMesonBeam = true; // Store valence content of a confirmed meson. nValKinds = 2; nVal[0] = 1 ; nVal[1] = 1; if (id1%2 == 0) { idVal[0] = id1; idVal[1] = -id2; } else { idVal[0] = id2; idVal[1] = -id1; } newValenceContent(); // Resolve valence content for assumed baryon. Flunk unallowed codes. } else { int id1 = idBeamAbs/1000; int id2 = (idBeamAbs/100)%10; int id3 = (idBeamAbs/10)%10; if ( id1 < 1 || id1 > maxValQuark || id2 < 1 || id2 > maxValQuark || id3 < 1 || id3 > maxValQuark) return; if (id2 > id1 || id3 > id1) return; isBaryonBeam = true; // Store valence content of a confirmed baryon. nValKinds = 1; idVal[0] = id1; nVal[0] = 1; if (id2 == id1) ++nVal[0]; else { nValKinds = 2; idVal[1] = id2; nVal[1] = 1; } if (id3 == id1) ++nVal[0]; else if (id3 == id2) ++nVal[1]; else { idVal[nValKinds] = id3; nVal[nValKinds] = 1; ++nValKinds; } } // Flip flavours for antimeson or antibaryon, and then done. if (idBeam < 0) for (int i = 0; i < nValKinds; ++i) idVal[i] = -idVal[i]; isHadronBeam = true; Q2ValFracSav = -1.; } //-------------------------------------------------------------------------- // Dynamic choice of meson valence flavours for pi0, K0S, K0L, Pomeron. void BeamParticle::newValenceContent() { // A pi0 oscillates between d dbar and u ubar. if (idBeam == 111) { idVal[0] = (rndmPtr->flat() < 0.5) ? 1 : 2; idVal[1] = -idVal[0]; // A K0S or K0L oscillates between d sbar and s dbar. } else if (idBeam == 130 || idBeam == 310) { idVal[0] = (rndmPtr->flat() < 0.5) ? 1 : 3; idVal[1] = (idVal[0] == 1) ? -3 : -1; // For a Pomeron split gluon remnant into d dbar or u ubar. } else if (idBeam == 990) { idVal[0] = (rndmPtr->flat() < 0.5) ? 1 : 2; idVal[1] = -idVal[0]; // Other hadrons so far do not require any event-by-event change. } else return; // Propagate change to PDF routine(s). pdfBeamPtr->newValenceContent( idVal[0], idVal[1]); if (pdfHardBeamPtr != pdfBeamPtr && pdfHardBeamPtr != 0) pdfHardBeamPtr->newValenceContent( idVal[0], idVal[1]); } //-------------------------------------------------------------------------- double BeamParticle::xMax(int iSkip) { // Minimum requirement on remaining energy > nominal mass for hadron. double xLeft = 1.; if (isHadron()) xLeft -= m() / e(); if (size() == 0) return xLeft; // Subtract what was carried away by initiators (to date). for (int i = 0; i < size(); ++i) if (i != iSkip && resolved[i].isFromBeam()) xLeft -= resolved[i].x(); return xLeft; } //-------------------------------------------------------------------------- // Parton distributions, reshaped to take into account previous // multiparton interactions. By picking a non-negative iSkip value, // one particular interaction is skipped, as needed for ISR double BeamParticle::xfModified(int iSkip, int idIn, double x, double Q2) { // Initial values. idSave = idIn; iSkipSave = iSkip; xqVal = 0.; xqgSea = 0.; xqCompSum = 0.; // Fast procedure for first interaction. if (size() == 0) { if (x >= 1.) return 0.; bool canBeVal = false; for (int i = 0; i < nValKinds; ++i) if (idIn == idVal[i]) canBeVal = true; if (canBeVal) { xqVal = xfVal( idIn, x, Q2); xqgSea = xfSea( idIn, x, Q2); } else xqgSea = xf( idIn, x, Q2); // More complicated procedure for non-first interaction. } else { // Sum up the x already removed, and check that remaining x is enough. double xUsed = 0.; for (int i = 0; i < size(); ++i) if (i != iSkip) xUsed += resolved[i].x(); double xLeft = 1. - xUsed; if (x >= xLeft) return 0.; double xRescaled = x / xLeft; // Calculate total and remaining amount of x carried by valence quarks. double xValTot = 0.; double xValLeft = 0.; for (int i = 0; i < nValKinds; ++i) { nValLeft[i] = nVal[i]; for (int j = 0; j < size(); ++j) if (j != iSkip && resolved[j].isValence() && resolved[j].id() == idVal[i]) --nValLeft[i]; double xValNow = xValFrac(i, Q2); xValTot += nVal[i] * xValNow; xValLeft += nValLeft[i] * xValNow; } // Calculate total amount of x carried by unmatched companion quarks. double xCompAdded = 0.; for (int i = 0; i < size(); ++i) if (i != iSkip && resolved[i].isUnmatched()) xCompAdded += xCompFrac( resolved[i].x() / (xLeft + resolved[i].x()) ) // Typo warning: extrafactor missing in Skands&Sjostrand article; // for companion refers to fraction of x left INCLUDING sea quark. // To be modified further?? * (1. + resolved[i].x() / xLeft); // Calculate total rescaling factor and pdf for sea and gluon. double rescaleGS = max( 0., (1. - xValLeft - xCompAdded) / (1. - xValTot) ); xqgSea = rescaleGS * xfSea( idIn, xRescaled, Q2); // Find valence part and rescale it to remaining number of quarks. for (int i = 0; i < nValKinds; ++i) if (idIn == idVal[i] && nValLeft[i] > 0) xqVal = xfVal( idIn, xRescaled, Q2) * double(nValLeft[i]) / double(nVal[i]); // Find companion part, by adding all companion contributions. for (int i = 0; i < size(); ++i) if (i != iSkip && resolved[i].id() == -idIn && resolved[i].isUnmatched()) { double xsRescaled = resolved[i].x() / (xLeft + resolved[i].x()); double xcRescaled = x / (xLeft + resolved[i].x()); double xqCompNow = xCompDist( xcRescaled, xsRescaled); resolved[i].xqCompanion( xqCompNow); xqCompSum += xqCompNow; } } // Add total, but only return relevant part for ISR. More cases?? // Watch out, e.g. g can come from either kind of quark.?? xqgTot = xqVal + xqgSea + xqCompSum; if (iSkip >= 0) { if (resolved[iSkip].isValence()) return xqVal; if (resolved[iSkip].isUnmatched()) return xqgSea + xqCompSum; } return xqgTot; } //-------------------------------------------------------------------------- // Decide whether a quark extracted from the beam is of valence, sea or // companion kind; in the latter case also pick its companion. // Assumes xfModified has already been called. int BeamParticle::pickValSeaComp() { // If parton already has a companion than reset code for this. int oldCompanion = resolved[iSkipSave].companion(); if (oldCompanion >= 0) resolved[oldCompanion].companion(-2); // Default assignment is sea. int vsc = -2; // For gluons or photons no sense of valence or sea. if (idSave == 21 || idSave == 22) vsc = -1; // For lepton beam assume same-kind lepton inside is valence. else if (isLeptonBeam && idSave == idBeam) vsc = -3; // Decide if valence or sea quark. else { double xqRndm = xqgTot * rndmPtr->flat(); if (xqRndm < xqVal) vsc = -3; else if (xqRndm < xqVal + xqgSea) vsc = -2; // If not either, loop over all possible companion quarks. else { xqRndm -= xqVal + xqgSea; for (int i = 0; i < size(); ++i) if (i != iSkipSave && resolved[i].id() == -idSave && resolved[i].isUnmatched()) { xqRndm -= resolved[i].xqCompanion(); if (xqRndm < 0.) vsc = i; break; } } } // Bookkeep assignment; for sea--companion pair both ways. resolved[iSkipSave].companion(vsc); if (vsc >= 0) resolved[vsc].companion(iSkipSave); // Done; return code for choice (to distinguish valence/sea in Info). return vsc; } //-------------------------------------------------------------------------- // Fraction of hadron momentum sitting in a valence quark distribution. // Based on hardcoded parametrizations of CTEQ 5L numbers. double BeamParticle::xValFrac(int j, double Q2) { // Only recalculate when required. if (Q2 != Q2ValFracSav) { Q2ValFracSav = Q2; // Q2-dependence of log-log form; assume fixed Lambda = 0.2. double llQ2 = log( log( max( 1., Q2) / 0.04 )); // Fractions carried by u and d in proton. uValInt = 0.48 / (1. + 1.56 * llQ2); dValInt = 0.385 / (1. + 1.60 * llQ2); } // Baryon with three different quark kinds: (2 * u + d) / 3 of proton. if (isBaryonBeam && nValKinds == 3) return (2. * uValInt + dValInt) / 3.; // Baryon with one or two identical: like d or u of proton. if (isBaryonBeam && nVal[j] == 1) return dValInt; if (isBaryonBeam && nVal[j] == 2) return uValInt; // Meson: (2 * u + d) / 2 of proton so same total valence quark fraction. return 0.5 * (2. * uValInt + dValInt); } //-------------------------------------------------------------------------- // The momentum integral of a companion quark, with its partner at x_s, // using an approximate gluon density like (1 - x_g)^power / x_g. // The value corresponds to an unrescaled range between 0 and 1 - x_s. double BeamParticle::xCompFrac(double xs) { // Select case by power of gluon (1-x_g) shape. switch (companionPower) { case 0: return xs * ( 5. + xs * (-9. - 2. * xs * (-3. + xs)) + 3. * log(xs) ) / ( (-1. + xs) * (2. + xs * (-1. + 2. * xs)) ); case 1: return -1. -3. * xs + ( 2. * pow2(-1. + xs) * (1. + xs + xs*xs)) / ( 2. + xs*xs * (xs - 3.) + 3. * xs * log(xs) ); case 2: return xs * ( (1. - xs) * (19. + xs * (43. + 4. * xs)) + 6. * log(xs) * (1. + 6. * xs + 4.*xs*xs) ) / ( 4. * ( (xs - 1.) * (1. + xs * (4. + xs) ) - 3. * xs * log(xs) * (1 + xs) ) ); case 3: return 3. * xs * ( (xs - 1.) * (7. + xs * (28. + 13. * xs)) - 2. * log(xs) * (1. + xs * (9. + 2. * xs * (6. + xs))) ) / ( 4. + 27. * xs - 31. * pow3(xs) + 6. * xs * log(xs) * (3. + 2. * xs * (3.+xs)) ); default: return ( -9. * xs * (xs*xs - 1.) * (5. + xs * (24. + xs)) + 12. * xs * log(xs) * (1. + 2. * xs) * (1. + 2. * xs * (5. + 2. * xs)) ) / ( 8. * (1. + 2. * xs) * ((xs - 1.) * (1. + xs * (10. + xs)) - 6. * xs * log(xs) * (1. + xs)) ); } } //-------------------------------------------------------------------------- // The x*f pdf of a companion quark at x_c, with its sea partner at x_s, // using an approximate gluon density like (1 - x_g)^power / x_g. // The value corresponds to an unrescaled range between 0 and 1 - x_s. double BeamParticle::xCompDist(double xc, double xs) { // Mother gluon momentum fraction. Check physical limit. double xg = xc + xs; if (xg > 1.) return 0.; // Common factor, including splitting kernel and part of gluon density // (and that it is x_c * f that is coded). double fac = 3. * xc * xs * (xc*xc + xs*xs) / pow4(xg); // Select case by power of gluon (1-x_g) shape. switch (companionPower) { case 0: return fac / ( 2. - xs * (3. - xs * (3. - 2. * xs)) ); case 1: return fac * (1. - xg) / ( 2. + xs*xs * (-3. + xs) + 3. * xs * log(xs) ); case 2: return fac * pow2(1. - xg) / ( 2. * ((1. - xs) * (1. + xs * (4. + xs)) + 3. * xs * (1. + xs) * log(xs)) ); case 3: return fac * pow3(1. - xg) * 2. / ( 4. + 27. * xs - 31. * pow3(xs) + 6. * xs * log(xs) * (3. + 2. * xs * (3. + xs)) ); default: return fac * pow4(1. - xg) / ( 2. * (1. + 2. * xs) * ((1. - xs) * (1. + xs * (10. + xs)) + 6. * xs * log(xs) * (1. + xs)) ); } } //-------------------------------------------------------------------------- // Add required extra remnant flavour content. Also initial colours. bool BeamParticle::remnantFlavours(Event& event) { // A baryon will have a junction, unless a diquark is formed later. hasJunctionBeam = (isBaryon()); // Store how many hard-scattering partons were removed from beam. nInit = size(); // Find remaining valence quarks. for (int i = 0; i < nValKinds; ++i) { nValLeft[i] = nVal[i]; for (int j = 0; j < nInit; ++j) if (resolved[j].isValence() && resolved[j].id() == idVal[i]) --nValLeft[i]; // Add remaining valence quarks to record. Partly temporary values. for (int k = 0; k < nValLeft[i]; ++k) append(0, idVal[i], 0., -3); } // If at least two valence quarks left in baryon remnant then form diquark. int nInitPlusVal = size(); if (isBaryon() && nInitPlusVal - nInit >= 2) { // If three, pick two at random to form diquark, else trivial. int iQ1 = nInit; int iQ2 = nInit + 1; if (nInitPlusVal - nInit == 3) { double pickDq = 3. * rndmPtr->flat(); if (pickDq > 1.) iQ2 = nInit + 2; if (pickDq > 2.) iQ1 = nInit + 1; } // Pick spin 0 or 1 according to SU(6) wave function factors. int idDq = flavSelPtr->makeDiquark( resolved[iQ1].id(), resolved[iQ2].id(), idBeam); // Overwrite with diquark flavour and remove one slot. No more junction. resolved[iQ1].id(idDq); if (nInitPlusVal - nInit == 3 && iQ2 == nInit + 1) resolved[nInit + 1].id( resolved[nInit + 2].id() ); resolved.pop_back(); hasJunctionBeam = false; } // Find companion quarks to unmatched sea quarks. for (int i = 0; i < nInit; ++i) if (resolved[i].isUnmatched()) { // Add companion quark to record; and bookkeep both ways. append(0, -resolved[i].id(), 0., i); resolved[i].companion(size() - 1); } // If no other remnants found, add a gluon or photon to carry momentum. if (size() == nInit) { int idRemnant = (isHadronBeam) ? 21 : 22; append(0, idRemnant, 0., -1); } // Set initiator and remnant masses. for (int i = 0; i < size(); ++i) { if (i < nInit) resolved[i].m(0.); else resolved[i].m( particleDataPtr->m0( resolved[i].id() ) ); } // For debug purposes: reject beams with resolved junction topology. if (hasJunctionBeam && !allowJunction) return false; // Pick initial colours for remnants. for (int i = nInit; i < size(); ++i) { int colType = particleDataPtr->colType( resolved[i].id() ); int col = (colType == 1 || colType == 2) ? event.nextColTag() : 0; int acol = (colType == -1 || colType == 2) ? event.nextColTag() : 0; resolved[i].cols( col, acol); } // Done. return true; } //-------------------------------------------------------------------------- // Correlate all initiators and remnants to make a colour singlet. bool BeamParticle::remnantColours(Event& event, vector& colFrom, vector& colTo) { // No colours in lepton beams so no need to do anything. if (isLeptonBeam) return true; // Copy initiator colour info from the event record to the beam. for (int i = 0; i < size(); ++i) { int j = resolved[i].iPos(); resolved[i].cols( event[j].col(), event[j].acol()); } // Find number and position of valence quarks, of gluons, and // of sea-companion pairs (counted as gluons) in the beam remnants. // Skip gluons with same colour as anticolour and rescattering partons. vector iVal; vector iGlu; for (int i = 0; i < size(); ++i) if (resolved[i].isFromBeam()) { if ( resolved[i].isValence() ) iVal.push_back(i); else if ( resolved[i].isCompanion() && resolved[i].companion() > i ) iGlu.push_back(i); else if ( resolved[i].id() == 21 && resolved[i].col() != resolved[i].acol() ) iGlu.push_back(i); } // Pick a valence quark to which gluons are attached. // Do not resolve quarks in diquark. (More sophisticated??) int iValSel= iVal[0]; if (iVal.size() == 2) { if ( abs(resolved[iValSel].id()) > 10 ) iValSel = iVal[1]; } else { double rndmValSel = 3. * rndmPtr->flat(); if (rndmValSel > 1.) iValSel= iVal[1]; if (rndmValSel > 2.) iValSel= iVal[2]; } // This valence quark defines initial (anti)colour. int iBeg = iValSel; bool hasCol = (resolved[iBeg].col() > 0); int begCol = (hasCol) ? resolved[iBeg].col() : resolved[iBeg].acol(); // Do random stepping through gluon/(sea+companion) list. vector iGluRndm; for (int i = 0; i < int(iGlu.size()); ++i) iGluRndm.push_back( iGlu[i] ); for (int iOrder = 0; iOrder < int(iGlu.size()); ++iOrder) { int iRndm = int( double(iGluRndm.size()) * rndmPtr->flat()); int iGluSel = iGluRndm[iRndm]; iGluRndm[iRndm] = iGluRndm[iGluRndm.size() - 1]; iGluRndm.pop_back(); // Find matching anticolour/colour to current colour/anticolour. int iEnd = iGluSel; int endCol = (hasCol) ? resolved[iEnd].acol() : resolved[iEnd].col(); // Not gluon but sea+companion pair: go to other. if (endCol == 0) { iEnd = resolved[iEnd].companion(); endCol = (hasCol) ? resolved[iEnd].acol() : resolved[iEnd].col(); } // Collapse this colour-anticolour pair to the lowest one. if (begCol < endCol) { if (hasCol) resolved[iEnd].acol(begCol); else resolved[iEnd].col(begCol); colFrom.push_back(endCol); colTo.push_back(begCol); } else { if (hasCol) resolved[iBeg].col(endCol); else resolved[iBeg].acol(endCol); colFrom.push_back(begCol); colTo.push_back(endCol); } // Pick up the other colour of the recent gluon and repeat. iBeg = iEnd; begCol = (hasCol) ? resolved[iBeg].col() : resolved[iBeg].acol(); // Not gluon but sea+companion pair: go to other. if (begCol == 0) { iBeg = resolved[iBeg].companion(); begCol = (hasCol) ? resolved[iBeg].col() : resolved[iBeg].acol(); } // At end of gluon/(sea+companion) list. } // Now begin checks, and also finding junction information. // Loop through remnant partons; isolate all colours and anticolours. vector colList; vector acolList; for (int i = 0; i < size(); ++i) if ( resolved[i].isFromBeam() ) if ( resolved[i].col() != resolved[i].acol() ) { if (resolved[i].col() > 0) colList.push_back( resolved[i].col() ); if (resolved[i].acol() > 0) acolList.push_back( resolved[i].acol() ); } // Remove all matching colour-anticolour pairs. bool foundPair = true; while (foundPair && colList.size() > 0 && acolList.size() > 0) { foundPair = false; for (int iCol = 0; iCol < int(colList.size()); ++iCol) { for (int iAcol = 0; iAcol < int(acolList.size()); ++iAcol) { if (acolList[iAcol] == colList[iCol]) { colList[iCol] = colList.back(); colList.pop_back(); acolList[iAcol] = acolList.back(); acolList.pop_back(); foundPair = true; break; } } if (foundPair) break; } } // Usually one unmatched pair left to collapse. if (colList.size() == 1 && acolList.size() == 1) { int finalFrom = max( colList[0], acolList[0]); int finalTo = min( colList[0], acolList[0]); for (int i = 0; i < size(); ++i) if ( resolved[i].isFromBeam() ) { if (resolved[i].col() == finalFrom) resolved[i].col(finalTo); if (resolved[i].acol() == finalFrom) resolved[i].acol(finalTo); } colFrom.push_back(finalFrom); colTo.push_back(finalTo); // Store an (anti)junction when three (anti)coloured daughters. } else if (hasJunctionBeam && colList.size() == 3 && acolList.size() == 0) { event.appendJunction( 1, colList[0], colList[1], colList[2]); junCol[0] = colList[0]; junCol[1] = colList[1]; junCol[2] = colList[2]; } else if (hasJunctionBeam && acolList.size() == 3 && colList.size() == 0) { event.appendJunction( 2, acolList[0], acolList[1], acolList[2]); junCol[0] = acolList[0]; junCol[1] = acolList[1]; junCol[2] = acolList[2]; // Any other nonvanishing values indicate failure. } else if (colList.size() > 0 || acolList.size() > 0) { infoPtr->errorMsg("Error in BeamParticle::remnantColours: " "leftover unmatched colours"); return false; } // Store colour assignment of beam particles. for (int i = nInit; i < size(); ++i) event[resolved[i].iPos()].cols( resolved[i].col(), resolved[i].acol() ); // Done. return true; } //-------------------------------------------------------------------------- // Pick unrescaled x values for beam remnant sharing. double BeamParticle::xRemnant( int i) { double x = 0.; // Calculation of x of valence quark or diquark, for latter as sum. if (resolved[i].isValence()) { // Resolve diquark into sum of two quarks. int id1 = resolved[i].id(); int id2 = 0; if (abs(id1) > 10) { id2 = (id1 > 0) ? (id1/100)%10 : -(((-id1)/100)%10); id1 = (id1 > 0) ? id1/1000 : -((-id1)/1000); } // Loop over (up to) two quarks; add their contributions. for (int iId = 0; iId < 2; ++iId) { int idNow = (iId == 0) ? id1 : id2; if (idNow == 0) break; double xPart = 0.; // Assume form (1-x)^a / sqrt(x). double xPow = valencePowerMeson; if (isBaryonBeam) { if (nValKinds == 3 || nValKinds == 1) xPow = (3. * rndmPtr->flat() < 2.) ? valencePowerUinP : valencePowerDinP ; else if (nValence(idNow) == 2) xPow = valencePowerUinP; else xPow = valencePowerDinP; } do xPart = pow2( rndmPtr->flat() ); while ( pow(1. - xPart, xPow) < rndmPtr->flat() ); // End loop over (up to) two quarks. Possibly enhancement for diquarks. x += xPart; } if (id2 != 0) x *= valenceDiqEnhance; // Calculation of x of sea quark, based on companion association. } else if (resolved[i].isCompanion()) { // Find rescaled x value of companion. double xLeft = 1.; for (int iInit = 0; iInit < nInit; ++iInit) if (resolved[iInit].isFromBeam()) xLeft -= resolved[iInit].x(); double xCompanion = resolved[ resolved[i].companion() ].x(); xCompanion /= (xLeft + xCompanion); // Now use ansatz q(x; x_c) < N/(x +x_c) to pick x. do x = pow( xCompanion, rndmPtr->flat()) - xCompanion; while ( pow( (1. - x - xCompanion) / (1. - xCompanion), companionPower) * (pow2(x) + pow2(xCompanion)) / pow2(x + xCompanion) < rndmPtr->flat() ); // Else, rarely, a single gluon remnant, so value does not matter. } else x = 1.; return x; } //-------------------------------------------------------------------------- // Print the list of resolved partons in a beam. void BeamParticle::list(ostream& os) const { // Header. os << "\n -------- PYTHIA Partons resolved in beam -----------------" << "-------------------------------------------------------------\n" << "\n i iPos id x comp xqcomp pTfact " << "colours p_x p_y p_z e m \n"; // Loop over list of removed partons and print it. double xSum = 0.; Vec4 pSum; for (int i = 0; i < size(); ++i) { ResolvedParton res = resolved[i]; os << fixed << setprecision(6) << setw(5) << i << setw(6) << res.iPos() << setw(8) << res.id() << setw(10) << res.x() << setw(6) << res.companion() << setw(10) << res.xqCompanion() << setw(10) << res.pTfactor() << setprecision(3) << setw(6) << res.col() << setw(6) << res.acol() << setw(11) << res.px() << setw(11) << res.py() << setw(11) << res.pz() << setw(11) << res.e() << setw(11) << res.m() << "\n"; // Also find sum of x and p values. if (res.companion() != -10) { xSum += res.x(); pSum += res.p(); } } // Print sum and endline. os << setprecision(6) << " x sum:" << setw(10) << xSum << setprecision(3) << " p sum:" << setw(11) << pSum.px() << setw(11) << pSum.py() << setw(11) << pSum.pz() << setw(11) << pSum.e() << "\n\n -------- End PYTHIA Partons resolved in beam -----------" << "---------------------------------------------------------------" << endl; } //-------------------------------------------------------------------------- // Test whether a lepton is to be considered as unresolved. bool BeamParticle::isUnresolvedLepton() { // Require record to consist of lepton with full energy plus a photon. if (!isLeptonBeam || resolved.size() > 2 || resolved[1].id() != 22 || resolved[0].x() < XMINUNRESOLVED) return false; return true; } //-------------------------------------------------------------------------- // For a diffractive system, decide whether to kick out gluon or quark. bool BeamParticle::pickGluon(double mDiff) { // Relative weight to pick a quark, assumed falling with energy. double probPickQuark = pickQuarkNorm / pow( mDiff, pickQuarkPower); return ( (1. + probPickQuark) * rndmPtr->flat() < 1. ); } //-------------------------------------------------------------------------- // Pick a valence quark at random. (Used for diffractive systems.) int BeamParticle::pickValence() { // Pick one valence quark at random. int nTotVal = (isBaryonBeam) ? 3 : 2; double rnVal = rndmPtr->flat() * nTotVal; int iVal = (rnVal < 1.) ? 1 : ( (rnVal < 2.) ? 2 : 3 ); // This valence in slot 1, the rest thereafter. idVal1 = 0; idVal2 = 0; idVal3 = 0; int iNow = 0; for (int i = 0; i < nValKinds; ++i) for (int j = 0; j < nVal[i]; ++j) { ++iNow; if (iNow == iVal) idVal1 = idVal[i]; else if ( idVal2 == 0) idVal2 = idVal[i]; else idVal3 = idVal[i]; } // Construct diquark if baryon. if (idVal3 != 0) idVal2 = flavSelPtr->makeDiquark( idVal2, idVal3); // Done. return idVal1; } //-------------------------------------------------------------------------- // Share lightcone momentum between two remnants in a diffractive system. double BeamParticle::zShare( double mDiff, double m1, double m2) { // Set up as valence in normal beam so can use xRemnant code. append(0, idVal1, 0., -3); append(0, idVal2, 0., -3); double m2Diff = mDiff*mDiff; // Begin to generate z and pT until acceptable solution. double wtAcc = 0.; do { double x1 = xRemnant(0); double x2 = xRemnant(0); zRel = x1 / (x1 + x2); pair gauss2 = rndmPtr->gauss2(); pxRel = diffPrimKTwidth * gauss2.first; pyRel = diffPrimKTwidth * gauss2.second; // Suppress large invariant masses of remnant system. double mTS1 = m1*m1 + pxRel*pxRel + pyRel*pyRel; double mTS2 = m2*m2 + pxRel*pxRel + pyRel*pyRel; double m2Sys = mTS1 / zRel + mTS2 / (1. - zRel); wtAcc = (m2Sys < m2Diff) ? pow( 1. - m2Sys / m2Diff, diffLargeMassSuppress) : 0.; } while (wtAcc < rndmPtr->flat()); // Done. return zRel; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/StringFragmentation.cc0000644000175000017500000013604712217346252017433 0ustar sunsun// StringFragmentation.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the StringEnd and // StringFragmentation classes. #include "Pythia8/StringFragmentation.h" namespace Pythia8 { //========================================================================== // The StringEnd class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // Avoid unphysical solutions to equation system. const double StringEnd::TINY = 1e-6; // Assume two (eX, eY) regions are related if pT2 differs by less. const double StringEnd::PT2SAME = 0.01; //-------------------------------------------------------------------------- // Set up initial endpoint values from input. void StringEnd::setUp(bool fromPosIn, int iEndIn, int idOldIn, int iMaxIn, double pxIn, double pyIn, double GammaIn, double xPosIn, double xNegIn) { // Simple transcription from input. fromPos = fromPosIn; iEnd = iEndIn; iMax = iMaxIn; flavOld = FlavContainer(idOldIn); pxOld = pxIn; pyOld = pyIn; GammaOld = GammaIn; iPosOld = (fromPos) ? 0 : iMax; iNegOld = (fromPos) ? iMax : 0; xPosOld = xPosIn; xNegOld = xNegIn; } //-------------------------------------------------------------------------- // Fragment off one hadron from the string system, in flavour and pT. void StringEnd::newHadron() { // Pick new flavour and form a new hadron. do { flavNew = flavSelPtr->pick( flavOld); idHad = flavSelPtr->combine( flavOld, flavNew); } while (idHad == 0); // Pick its transverse momentum. pair pxy = pTSelPtr->pxy(); pxNew = pxy.first; pyNew = pxy.second; pxHad = pxOld + pxNew; pyHad = pyOld + pyNew; // Pick its mass and thereby define its transverse mass. mHad = particleDataPtr->mSel(idHad); mT2Had = pow2(mHad) + pow2(pxHad) + pow2(pyHad); } //-------------------------------------------------------------------------- // Fragment off one hadron from the string system, in momentum space, // by taking steps from positive end. Vec4 StringEnd::kinematicsHadron( StringSystem& system) { // Pick fragmentation step z and calculate new Gamma. zHad = zSelPtr->zFrag( flavOld.id, flavNew.id, mT2Had); GammaNew = (1. - zHad) * (GammaOld + mT2Had / zHad); // Set up references that are direction-neutral; // ...Dir for direction of iteration and ...Inv for its inverse. int& iDirOld = (fromPos) ? iPosOld : iNegOld; int& iInvOld = (fromPos) ? iNegOld : iPosOld; int& iDirNew = (fromPos) ? iPosNew : iNegNew; int& iInvNew = (fromPos) ? iNegNew : iPosNew; double& xDirOld = (fromPos) ? xPosOld : xNegOld; double& xInvOld = (fromPos) ? xNegOld : xPosOld; double& xDirNew = (fromPos) ? xPosNew : xNegNew; double& xInvNew = (fromPos) ? xNegNew : xPosNew; double& xDirHad = (fromPos) ? xPosHad : xNegHad; double& xInvHad = (fromPos) ? xNegHad : xPosHad; // Start search for new breakup in the old region. iDirNew = iDirOld; iInvNew = iInvOld; Vec4 pTNew; // Each step corresponds to trying a new string region. for (int iStep = 0; ; ++iStep) { // Referance to current string region. StringRegion& region = system.region( iPosNew, iNegNew); // Now begin special section for rapid processing of low region. if (iStep == 0 && iPosOld + iNegOld == iMax) { // A first step within a low region is easy. if (mT2Had < zHad * xDirOld * (1. - xInvOld) * region.w2) { // Translate into x coordinates. xDirHad = zHad * xDirOld; xInvHad = mT2Had / (xDirHad * region.w2); xDirNew = xDirOld - xDirHad; xInvNew = xInvOld + xInvHad; // Find and return four-momentum of the produced particle. return region.pHad( xPosHad, xNegHad, pxHad, pyHad); // A first step out of a low region also OK, if there are more regions. // Negative energy signals failure, i.e. in last region. } else { --iInvNew; if (iInvNew < 0) return Vec4(0., 0., 0., -1.); // Momentum taken by stepping out of region. Continue to next region. xInvHad = 1. - xInvOld; xDirHad = 0.; pSoFar = region.pHad( xPosHad, xNegHad, pxOld, pyOld); continue; } // Else, for first step, take into account starting pT. } else if (iStep == 0) { pSoFar = region.pHad( 0., 0., pxOld, pyOld); pTNew = region.pHad( 0., 0., pxNew, pyNew); } // Now begin normal treatment of nontrivial regions. // Set up four-vectors in a region not visited before. if (!region.isSetUp) region.setUp( system.regionLowPos(iPosNew).pPos, system.regionLowNeg(iNegNew).pNeg, true); // If new region is vanishingly small, continue immediately to next. // Negative energy signals failure to do this, i.e. moved too low. if (region.isEmpty) { xDirHad = (iDirNew == iDirOld) ? xDirOld : 1.; xInvHad = 0.; pSoFar += region.pHad( xPosHad, xNegHad, 0., 0.); ++iDirNew; if (iDirNew + iInvNew > iMax) return Vec4(0., 0., 0., -1.); continue; } // Reexpress pTNew w.r.t. base vectors in new region, if possible. // Recall minus sign from normalization e_x^2 = e_y^2 = -1. double pxNewTemp = -pTNew * region.eX; double pyNewTemp = -pTNew * region.eY; if (abs( pxNewTemp * pxNewTemp + pyNewTemp * pyNewTemp - pxNew * pxNew - pyNew * pyNew) < PT2SAME) { pxNew = pxNewTemp; pyNew = pyNewTemp; } // Four-momentum taken so far, including new pT. Vec4 pTemp = pSoFar + region.pHad( 0., 0., pxNew, pyNew); // Derive coefficients for m2 expression. // cM2 * x+ + cM3 * x- + cM4 * x+ * x- = m^2 - cM1; double cM1 = pTemp.m2Calc(); double cM2 = 2. * (pTemp * region.pPos); double cM3 = 2. * (pTemp * region.pNeg); double cM4 = region.w2; if (!fromPos) swap( cM2, cM3); // Derive coefficients for Gamma expression. // cGam2 * x+ + cGam3 * x- + cGam4 * x+ * x- = Gamma_new - cGam1; double cGam1 = 0.; double cGam2 = 0.; double cGam3 = 0.; double cGam4 = 0.; for (int iInv = iInvNew; iInv <= iMax - iDirNew; ++iInv) { double xInv = 1.; if (iInv == iInvNew) xInv = (iInvNew == iInvOld) ? xInvOld : 0.; for (int iDir = iDirNew; iDir <= iMax - iInv; ++iDir) { double xDir = (iDir == iDirOld) ? xDirOld : 1.; int iPos = (fromPos) ? iDir : iInv; int iNeg = (fromPos) ? iInv : iDir; StringRegion& regionGam = system.region( iPos, iNeg); if (!regionGam.isSetUp) regionGam.setUp( system.regionLowPos(iPos).pPos, system.regionLowNeg(iNeg).pNeg, true); double w2 = regionGam.w2; cGam1 += xDir * xInv * w2; if (iDir == iDirNew) cGam2 -= xInv * w2; if (iInv == iInvNew) cGam3 += xDir * w2; if (iDir == iDirNew && iInv == iInvNew) cGam4 -= w2; } } // Solve (m2, Gamma) equation system => r2 * x-^2 + r1 * x- + r0 = 0. double cM0 = pow2(mHad) - cM1; double cGam0 = GammaNew - cGam1; double r2 = cM3 * cGam4 - cM4 * cGam3; double r1 = cM4 * cGam0 - cM0 * cGam4 + cM3 * cGam2 - cM2 * cGam3; double r0 = cM2 * cGam0 - cM0 * cGam2; double root = sqrtpos( r1*r1 - 4. * r2 * r0 ); if (abs(r2) < TINY || root < TINY) return Vec4(0., 0., 0., -1.); xInvHad = 0.5 * (root / abs(r2) - r1 / r2); xDirHad = (cM0 - cM3 * xInvHad) / (cM2 + cM4 * xInvHad); // Define position of new trial vertex. xDirNew = (iDirNew == iDirOld) ? xDirOld - xDirHad : 1. - xDirHad; xInvNew = (iInvNew == iInvOld) ? xInvOld + xInvHad : xInvHad; // Step up to new region if new x- > 1. if (xInvNew > 1.) { xInvHad = (iInvNew == iInvOld) ? 1. - xInvOld : 1.; xDirHad = 0.; pSoFar += region.pHad( xPosHad, xNegHad, 0., 0.); --iInvNew; if (iInvNew < 0) return Vec4(0., 0., 0., -1.); continue; // Step down to new region if new x+ < 0. } else if (xDirNew < 0.) { xDirHad = (iDirNew == iDirOld) ? xDirOld : 1.; xInvHad = 0.; pSoFar += region.pHad( xPosHad, xNegHad, 0., 0.); ++iDirNew; if (iDirNew + iInvNew > iMax) return Vec4(0., 0., 0., -1.); continue; } // Else we have found the correct region, and can return four-momentum. return pSoFar + region.pHad( xPosHad, xNegHad, pxNew, pyNew); // End of "infinite" loop of stepping to new region. } } //-------------------------------------------------------------------------- // Update string end information after a hadron has been removed. void StringEnd::update() { flavOld.anti(flavNew); iPosOld = iPosNew; iNegOld = iNegNew; pxOld = -pxNew; pyOld = -pyNew; GammaOld = GammaNew; xPosOld = xPosNew; xNegOld = xNegNew; } //========================================================================== // The StringFragmentation class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Maximum number of tries to (flavour-, energy) join the two string ends. const int StringFragmentation::NTRYFLAV = 10; const int StringFragmentation::NTRYJOIN = 30; // The last few times gradually increase the stop mass to make it easier. const int StringFragmentation::NSTOPMASS = 15; const double StringFragmentation::FACSTOPMASS = 1.05; // For closed string, pick a Gamma by taking a step with fictitious mass. const double StringFragmentation::CLOSEDM2MAX = 25.; const double StringFragmentation::CLOSEDM2FRAC = 0.1; // Do not allow too large argument to exp function. const double StringFragmentation::EXPMAX = 50.; // Matching criterion that p+ and p- not the same (can happen in gg loop). const double StringFragmentation::MATCHPOSNEG = 1e-6; // For pull on junction, do not trace too far down each leg. const double StringFragmentation::EJNWEIGHTMAX = 10.; // Iterate junction rest frame boost until convergence or too many tries. const double StringFragmentation::CONVJNREST = 1e-5; const int StringFragmentation::NTRYJNREST = 20; // Fail and try again when two legs combined to diquark (3 loops). const int StringFragmentation::NTRYJNMATCH = 20; const double StringFragmentation::EEXTRAJNMATCH = 0.5; const double StringFragmentation::MDIQUARKMIN = -2.0; // Consider junction-leg parton as massless if m2 tiny. const double StringFragmentation::M2MAXJRF = 1e-4; // Iterate junction rest frame equation until convergence or too many tries. const double StringFragmentation::CONVJRFEQ = 1e-12; const int StringFragmentation::NTRYJRFEQ = 40; //-------------------------------------------------------------------------- // Initialize and save pointers. void StringFragmentation::init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, StringFlav* flavSelPtrIn, StringPT* pTSelPtrIn, StringZ* zSelPtrIn) { // Save pointers. infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; flavSelPtr = flavSelPtrIn; pTSelPtr = pTSelPtrIn; zSelPtr = zSelPtrIn; // Initialize the StringFragmentation class. stopMass = zSelPtr->stopMass(); stopNewFlav = zSelPtr->stopNewFlav(); stopSmear = zSelPtr->stopSmear(); eNormJunction = settings.parm("StringFragmentation:eNormJunction"); eBothLeftJunction = settings.parm("StringFragmentation:eBothLeftJunction"); eMaxLeftJunction = settings.parm("StringFragmentation:eMaxLeftJunction"); eMinLeftJunction = settings.parm("StringFragmentation:eMinLeftJunction"); // Joining of nearby partons along the string. mJoin = settings.parm("FragmentationSystems:mJoin"); // Initialize the b parameter of the z spectrum, used when joining jets. bLund = zSelPtr->bAreaLund(); // Initialize the hadrons instance of an event record. hadrons.init( "(string fragmentation)", particleDataPtr); // Send on pointers to the two StringEnd instances. posEnd.init( particleDataPtr, flavSelPtr, pTSelPtr, zSelPtr); negEnd.init( particleDataPtr, flavSelPtr, pTSelPtr, zSelPtr); } //-------------------------------------------------------------------------- // Perform the fragmentation. bool StringFragmentation::fragment( int iSub, ColConfig& colConfig, Event& event) { // Find partons and their total four-momentum. iParton = colConfig[iSub].iParton; iPos = iParton[0]; if (iPos < 0) iPos = iParton[1]; int idPos = event[iPos].id(); iNeg = iParton.back(); int idNeg = event[iNeg].id(); pSum = colConfig[iSub].pSum; // Reset the local event record. hadrons.clear(); // For closed gluon string: pick first breakup region. isClosed = colConfig[iSub].isClosed; if (isClosed) iParton = findFirstRegion(iParton, event); // For junction topology: fragment off two of the string legs. // Then iParton overwritten to remaining leg + leftover diquark. pJunctionHadrons = 0.; hasJunction = colConfig[iSub].hasJunction; if (hasJunction && !fragmentToJunction(event)) return false; int junctionHadrons = hadrons.size(); if (hasJunction) { idPos = event[ iParton[0] ].id(); idNeg = event.back().id(); pSum -= pJunctionHadrons; } // Set up kinematics of string evolution ( = motion). system.setUp(iParton, event); stopMassNow = stopMass; int nExtraJoin = 0; // Fallback loop, when joining in the middle fails. Bailout if stuck. for ( int iTry = 0; ; ++iTry) { if (iTry > NTRYJOIN) { infoPtr->errorMsg("Error in StringFragmentation::fragment: " "stuck in joining"); if (hasJunction) ++nExtraJoin; if (nExtraJoin > 0) event.popBack(nExtraJoin); return false; } // After several failed tries join some (extra) nearby partons. if (iTry == NTRYJOIN / 3) nExtraJoin = extraJoin( 2., event); if (iTry == 2 * NTRYJOIN / 3) nExtraJoin += extraJoin( 4., event); // After several failed tries gradually allow larger stop mass. if (iTry > NTRYJOIN - NSTOPMASS) stopMassNow *= FACSTOPMASS; // Set up flavours of two string ends, and reset other info. setStartEnds(idPos, idNeg, system); pRem = pSum; // Begin fragmentation loop, interleaved from the two ends. bool fromPos; for ( ; ; ) { // Take a step either from the positive or the negative end. fromPos = (rndmPtr->flat() < 0.5); StringEnd& nowEnd = (fromPos) ? posEnd : negEnd; // Construct trial hadron and check that energy remains. nowEnd.newHadron(); if ( energyUsedUp(fromPos) ) break; // Construct kinematics of the new hadron and store it. Vec4 pHad = nowEnd.kinematicsHadron(system); int statusHad = (fromPos) ? 83 : 84; hadrons.append( nowEnd.idHad, statusHad, iPos, iNeg, 0, 0, 0, 0, pHad, nowEnd.mHad); if (pHad.e() < 0.) break; // Update string end and remaining momentum. nowEnd.update(); pRem -= pHad; // End of fragmentation loop. } // When done, join in the middle. If this works, then really done. if ( finalTwo(fromPos) ) break; // Else remove produced particles (except from first two junction legs) // and start all over. int newHadrons = hadrons.size() - junctionHadrons; hadrons.popBack(newHadrons); } // Junctions & extra joins: remove fictitious end, restore original partons. if (hasJunction) ++nExtraJoin; if (nExtraJoin > 0) { event.popBack(nExtraJoin); iParton = colConfig[iSub].iParton; } // Store the hadrons in the normal event record, ordered from one end. store(event); // Done. return true; } //-------------------------------------------------------------------------- // Find region where to put first string break for closed gluon loop. vector StringFragmentation::findFirstRegion(vector& iPartonIn, Event& event) { // Evaluate mass-squared for all adjacent gluon pairs. vector m2Pair; double m2Sum = 0.; int size = iPartonIn.size(); for (int i = 0; i < size; ++i) { double m2Now = 0.5 * event[ iPartonIn[i] ].p() * event[ iPartonIn[(i + 1)%size] ].p(); m2Pair.push_back(m2Now); m2Sum += m2Now; } // Pick breakup region with probability proportional to mass-squared. double m2Reg = m2Sum * rndmPtr->flat(); int iReg = -1; do m2Reg -= m2Pair[++iReg]; while (m2Reg > 0. && iReg < size - 1); // Create reordered parton list, with breakup string region duplicated. vector iPartonOut; for (int i = 0; i < size + 2; ++i) iPartonOut.push_back( iPartonIn[(i + iReg)%size] ); // Done. return iPartonOut; } //-------------------------------------------------------------------------- // Set flavours and momentum position for initial string endpoints. void StringFragmentation::setStartEnds( int idPos, int idNeg, StringSystem systemNow) { // Variables characterizing string endpoints: defaults for open string. double px = 0.; double py = 0.; double Gamma = 0.; double xPosFromPos = 1.; double xNegFromPos = 0.; double xPosFromNeg = 0.; double xNegFromNeg = 1.; // For closed gluon loop need to pick an initial flavour. if (isClosed) { do { int idTry = flavSelPtr->pickLightQ(); FlavContainer flavTry(idTry, 1); flavTry = flavSelPtr->pick( flavTry); flavTry = flavSelPtr->pick( flavTry); idPos = flavTry.id; idNeg = -idPos; } while (idPos == 0); // Also need pT and breakup vertex position in region. pair pxy = pTSelPtr->pxy(); px = pxy.first; py = pxy.second; double m2Region = systemNow.regionLowPos(0).w2; double m2Temp = min( CLOSEDM2MAX, CLOSEDM2FRAC * m2Region); do { double zTemp = zSelPtr->zFrag( idPos, idNeg, m2Temp); xPosFromPos = 1. - zTemp; xNegFromPos = m2Temp / (zTemp * m2Region); } while (xNegFromPos > 1.); Gamma = xPosFromPos * xNegFromPos * m2Region; xPosFromNeg = xPosFromPos; xNegFromNeg = xNegFromPos; } // Initialize two string endpoints. posEnd.setUp( true, iPos, idPos, systemNow.iMax, px, py, Gamma, xPosFromPos, xNegFromPos); negEnd.setUp( false, iNeg, idNeg, systemNow.iMax, -px, -py, Gamma, xPosFromNeg, xNegFromNeg); // For closed gluon loop can allow popcorn on one side but not both. if (isClosed) { flavSelPtr->assignPopQ(posEnd.flavOld); flavSelPtr->assignPopQ(negEnd.flavOld); if (rndmPtr->flat() < 0.5) posEnd.flavOld.nPop = 0; else negEnd.flavOld.nPop = 0; posEnd.flavOld.rank = 1; negEnd.flavOld.rank = 1; } // Done. } //-------------------------------------------------------------------------- // Check remaining energy-momentum whether it is OK to continue. bool StringFragmentation::energyUsedUp(bool fromPos) { // If remaining negative energy then abort right away. if (pRem.e() < 0.) return true; // Calculate W2_minimum and done if remaining W2 is below it. double wMin = stopMassNow + particleDataPtr->constituentMass(posEnd.flavOld.id) + particleDataPtr->constituentMass(negEnd.flavOld.id); if (fromPos) wMin += stopNewFlav * particleDataPtr->constituentMass(posEnd.flavNew.id); else wMin += stopNewFlav * particleDataPtr->constituentMass(negEnd.flavNew.id); wMin *= 1. + (2. * rndmPtr->flat() - 1.) * stopSmear; w2Rem = pRem.m2Calc(); if (w2Rem < pow2(wMin)) return true; // Else still enough energy left to continue iteration. return false; } //-------------------------------------------------------------------------- // Produce the final two partons to complete the system. bool StringFragmentation::finalTwo(bool fromPos) { // Check whether we went too far in p+-. if (pRem.e() < 0. || w2Rem < 0. || (hadrons.size() > 0 && hadrons.back().e() < 0.) ) return false; if ( posEnd.iPosOld > negEnd.iPosOld || negEnd.iNegOld > posEnd.iNegOld) return false; if ( posEnd.iPosOld == negEnd.iPosOld && posEnd.xPosOld < negEnd.xPosOld) return false; if ( posEnd.iNegOld == negEnd.iNegOld && posEnd.xNegOld > negEnd.xNegOld) return false; // Construct the final hadron from the leftover flavours. // Impossible to join two diquarks. Also break if stuck for other reason. FlavContainer flav1 = (fromPos) ? posEnd.flavNew.anti() : posEnd.flavOld; FlavContainer flav2 = (fromPos) ? negEnd.flavOld : negEnd.flavNew.anti(); if (flav1.isDiquark() && flav2.isDiquark()) return false; int idHad; for (int iTry = 0; iTry < NTRYFLAV; ++iTry) { idHad = flavSelPtr->combine( flav1, flav2); if (idHad != 0) break; } if (idHad == 0) return false; // Store the final particle and its new pT, and construct its mass. if (fromPos) { negEnd.idHad = idHad; negEnd.pxNew = -posEnd.pxNew; negEnd.pyNew = -posEnd.pyNew; negEnd.mHad = particleDataPtr->mSel(idHad); } else { posEnd.idHad = idHad; posEnd.pxNew = -negEnd.pxNew; posEnd.pyNew = -negEnd.pyNew; posEnd.mHad = particleDataPtr->mSel(idHad); } // String region in which to do the joining. StringRegion region = finalRegion(); if (region.isEmpty) return false; // Project remaining momentum along longitudinal and transverse directions. region.project( pRem); double pxRem = region.px() - posEnd.pxOld - negEnd.pxOld; double pyRem = region.py() - posEnd.pyOld - negEnd.pyOld; double xPosRem = region.xPos(); double xNegRem = region.xNeg(); // Share extra pT kick evenly between final two hadrons. posEnd.pxOld += 0.5 * pxRem; posEnd.pyOld += 0.5 * pyRem; negEnd.pxOld += 0.5 * pxRem; negEnd.pyOld += 0.5 * pyRem; // Construct new pT and mT of the final two particles. posEnd.pxHad = posEnd.pxOld + posEnd.pxNew; posEnd.pyHad = posEnd.pyOld + posEnd.pyNew; posEnd.mT2Had = pow2(posEnd.mHad) + pow2(posEnd.pxHad) + pow2(posEnd.pyHad); negEnd.pxHad = negEnd.pxOld + negEnd.pxNew; negEnd.pyHad = negEnd.pyOld + negEnd.pyNew; negEnd.mT2Had = pow2(negEnd.mHad) + pow2(negEnd.pxHad) + pow2(negEnd.pyHad); // Construct remaining system transverse mass. double wT2Rem = w2Rem + pow2( posEnd.pxHad + negEnd.pxHad) + pow2( posEnd.pyHad + negEnd.pyHad); // Check that kinematics possible. if ( sqrt(wT2Rem) < sqrt(posEnd.mT2Had) + sqrt(negEnd.mT2Had) ) return false; double lambda2 = pow2( wT2Rem - posEnd.mT2Had - negEnd.mT2Had) - 4. * posEnd.mT2Had * negEnd.mT2Had; if (lambda2 <= 0.) return false; // Construct kinematics, as viewed in the transverse rest frame. double lambda = sqrt(lambda2); double probReverse = 1. / (1. + exp( min( EXPMAX, bLund * lambda) ) ); double xpzPos = 0.5 * lambda/ wT2Rem; if (probReverse > rndmPtr->flat()) xpzPos = -xpzPos; double xmDiff = (posEnd.mT2Had - negEnd.mT2Had) / wT2Rem; double xePos = 0.5 * (1. + xmDiff); double xeNeg = 0.5 * (1. - xmDiff ); // Translate this into kinematics in the string frame. Vec4 pHadPos = region.pHad( (xePos + xpzPos) * xPosRem, (xePos - xpzPos) * xNegRem, posEnd.pxHad, posEnd.pyHad); Vec4 pHadNeg = region.pHad( (xeNeg - xpzPos) * xPosRem, (xeNeg + xpzPos) * xNegRem, negEnd.pxHad, negEnd.pyHad); // Add produced particles to the event record. hadrons.append( posEnd.idHad, 83, posEnd.iEnd, negEnd.iEnd, 0, 0, 0, 0, pHadPos, posEnd.mHad); hadrons.append( negEnd.idHad, 84, posEnd.iEnd, negEnd.iEnd, 0, 0, 0, 0, pHadNeg, negEnd.mHad); // It worked. return true; } //-------------------------------------------------------------------------- // Construct a special joining region for the final two hadrons. StringRegion StringFragmentation::finalRegion() { // Simple case when both string ends are in the same region. if (posEnd.iPosOld == negEnd.iPosOld && posEnd.iNegOld == negEnd.iNegOld) return system.region( posEnd.iPosOld, posEnd.iNegOld); // Start out with empty region. (Empty used for error returns.) StringRegion region; // Add up all remaining p+. Vec4 pPosJoin; if ( posEnd.iPosOld == negEnd.iPosOld) { double xPosJoin = posEnd.xPosOld - negEnd.xPosOld; if (xPosJoin < 0.) return region; pPosJoin = system.regionLowPos(posEnd.iPosOld).pHad( xPosJoin, 0., 0., 0.); } else { for (int iPosNow = posEnd.iPosOld; iPosNow <= negEnd.iPosOld; ++iPosNow) { if (iPosNow == posEnd.iPosOld) pPosJoin += system.regionLowPos(iPosNow).pHad( posEnd.xPosOld, 0., 0., 0.); else if (iPosNow == negEnd.iPosOld) pPosJoin += system.regionLowPos(iPosNow).pHad( 1. - negEnd.xPosOld, 0., 0., 0.); else pPosJoin += system.regionLowPos(iPosNow).pHad( 1., 0., 0., 0.); } } // Add up all remaining p-. Vec4 pNegJoin; if ( negEnd.iNegOld == posEnd.iNegOld) { double xNegJoin = negEnd.xNegOld - posEnd.xNegOld; if (xNegJoin < 0.) return region; pNegJoin = system.regionLowNeg(negEnd.iNegOld).pHad( 0., xNegJoin, 0., 0.); } else { for (int iNegNow = negEnd.iNegOld; iNegNow <= posEnd.iNegOld; ++iNegNow) { if (iNegNow == negEnd.iNegOld) pNegJoin += system.regionLowNeg(iNegNow).pHad( 0., negEnd.xNegOld, 0., 0.); else if (iNegNow == posEnd.iNegOld) pNegJoin += system.regionLowNeg(iNegNow).pHad( 0., 1. - posEnd.xNegOld, 0., 0.); else pNegJoin += system.regionLowNeg(iNegNow).pHad( 0., 1., 0., 0.); } } // For a closed gluon loop pPosJoin == pNegJoin and the above does not work. // So reshuffle; "perfect" for g g systems, OK in general. Vec4 pTest = pPosJoin - pNegJoin; if ( abs(pTest.px()) + abs(pTest.py()) + abs(pTest.pz()) + abs(pTest.e()) < MATCHPOSNEG * (pPosJoin.e() + pNegJoin.e()) ) { Vec4 delta = system.regionLowPos(posEnd.iPosOld + 1).pHad( 1., 0., 0., 0.) - system.regionLowNeg(negEnd.iNegOld + 1).pHad( 0., 1., 0., 0.); pPosJoin -= delta; pNegJoin += delta; } // Construct a new region from remaining p+ and p-. region.setUp( pPosJoin, pNegJoin); if (region.isEmpty) return region; // Project the existing pTold vectors onto the new directions. Vec4 pTposOld = system.region( posEnd.iPosOld, posEnd.iNegOld).pHad( 0., 0., posEnd.pxOld, posEnd.pyOld); region.project( pTposOld); posEnd.pxOld = region.px(); posEnd.pyOld = region.py(); Vec4 pTnegOld = system.region( negEnd.iPosOld, negEnd.iNegOld).pHad( 0., 0., negEnd.pxOld, negEnd.pyOld); region.project( pTnegOld); negEnd.pxOld = region.px(); negEnd.pyOld = region.py(); // Done. return region; } //-------------------------------------------------------------------------- // Store the hadrons in the normal event record, ordered from one end. void StringFragmentation::store(Event& event) { // Starting position. int iFirst = event.size(); // Copy straight over from first two junction legs. if (hasJunction) { for (int i = 0; i < hadrons.size(); ++i) if (hadrons[i].status() == 85 || hadrons[i].status() == 86) event.append( hadrons[i] ); } // Loop downwards, copying all from the positive end. for (int i = 0; i < hadrons.size(); ++i) if (hadrons[i].status() == 83) event.append( hadrons[i] ); // Loop upwards, copying all from the negative end. for (int i = hadrons.size() - 1; i >= 0 ; --i) if (hadrons[i].status() == 84) event.append( hadrons[i] ); int iLast = event.size() - 1; // Set decay vertex when this is displaced. if (event[posEnd.iEnd].hasVertex()) { Vec4 vDec = event[posEnd.iEnd].vDec(); for (int i = iFirst; i <= iLast; ++i) event[i].vProd( vDec ); } // Set lifetime of hadrons. for (int i = iFirst; i <= iLast; ++i) event[i].tau( event[i].tau0() * rndmPtr->exp() ); // Mark original partons as hadronized and set their daughter range. for (int i = 0; i < int(iParton.size()); ++i) if (iParton[i] >= 0) { event[ iParton[i] ].statusNeg(); event[ iParton[i] ].daughters(iFirst, iLast); } } //-------------------------------------------------------------------------- // Fragment off two of the string legs in to a junction. bool StringFragmentation::fragmentToJunction(Event& event) { // Identify range of partons on the three legs. // (Each leg begins with an iParton[i] = -(10 + 10*junctionNumber + leg), // and partons then appear ordered from the junction outwards.) int legBeg[3] = { 0, 0, 0}; int legEnd[3] = { 0, 0, 0}; int leg = -1; // PS (4/10/2011) Protect against invalid systems if (iParton[0] > 0) { infoPtr->errorMsg("Error in StringFragmentation::fragment" "ToJunction: iParton[0] not a valid junctionNumber"); return false; } for (int i = 0; i < int(iParton.size()); ++i) { if (iParton[i] < 0) { if (leg == 2) { infoPtr->errorMsg("Error in StringFragmentation::fragment" "ToJunction: unprocessed multi-junction system"); return false; } legBeg[++leg] = i + 1; } else legEnd[leg] = i; } // Iterate from system rest frame towards the junction rest frame (JRF). RotBstMatrix MtoJRF, Mstep; MtoJRF.bstback(pSum); Vec4 pWTinJRF[3]; int iter = 0; double errInCM = 0.; do { ++iter; // Find weighted sum of momenta on the three sides of the junction. for (leg = 0; leg < 3; ++ leg) { pWTinJRF[leg] = 0.; double eWeight = 0.; for (int i = legBeg[leg]; i <= legEnd[leg]; ++i) { Vec4 pTemp = event[ iParton[i] ].p(); pTemp.rotbst(MtoJRF); pWTinJRF[leg] += pTemp * exp(-eWeight); eWeight += pTemp.e() / eNormJunction; if (eWeight > EJNWEIGHTMAX) break; } } // Store original deviation from 120 degree topology. if (iter == 1) errInCM = pow2(costheta(pWTinJRF[0], pWTinJRF[1]) + 0.5) + pow2(costheta(pWTinJRF[0], pWTinJRF[2]) + 0.5) + pow2(costheta(pWTinJRF[1], pWTinJRF[2]) + 0.5); // Find new JRF from the set of weighted momenta. Mstep = junctionRestFrame( pWTinJRF[0], pWTinJRF[1], pWTinJRF[2]); // Fortran code will not take full step after the first few // iterations. How implement this in terms of an M matrix?? MtoJRF.rotbst( Mstep ); } while (iter < 3 || (Mstep.deviation() > CONVJNREST && iter < NTRYJNREST) ); // If final deviation from 120 degrees is bigger than in CM then revert. double errInJRF = pow2(costheta(pWTinJRF[0], pWTinJRF[1]) + 0.5) + pow2(costheta(pWTinJRF[0], pWTinJRF[2]) + 0.5) + pow2(costheta(pWTinJRF[1], pWTinJRF[2]) + 0.5); if (errInJRF > errInCM) { infoPtr->errorMsg("Warning in StringFragmentation::fragmentTo" "Junction: bad convergence junction rest frame"); MtoJRF.reset(); MtoJRF.bstback(pSum); } // Opposite operation: boost from JRF to original system. RotBstMatrix MfromJRF = MtoJRF; MfromJRF.invert(); // Sum leg four-momenta in original frame and in JRF. Vec4 pInLeg[3], pInJRF[3]; for (leg = 0; leg < 3; ++leg) { pInLeg[leg] = 0.; for (int i = legBeg[leg]; i <= legEnd[leg]; ++i) pInLeg[leg] += event[ iParton[i] ].p(); pInJRF[leg] = pInLeg[leg]; pInJRF[leg].rotbst(MtoJRF); } // Pick the two legs with lowest energy in JRF. int legMin = (pInJRF[0].e() < pInJRF[1].e()) ? 0 : 1; int legMax = 1 - legMin; if (pInJRF[2].e() < min(pInJRF[0].e(), pInJRF[1].e()) ) legMin = 2; else if (pInJRF[2].e() > max(pInJRF[0].e(), pInJRF[1].e()) ) legMax = 2; int legMid = 3 - legMin - legMax; // Save info on which status codes belong with the three legs. int iJunction = (-iParton[0]) / 10 - 1; event.statusJunction( iJunction, legMin, 85); event.statusJunction( iJunction, legMid, 86); event.statusJunction( iJunction, legMax, 83); // Temporarily copy the partons on the low-energy legs, into the JRF, // in reverse order, so (anti)quark leg end first. vector iPartonMin; for (int i = legEnd[legMin]; i >= legBeg[legMin]; --i) { int iNew = event.append( event[ iParton[i] ] ); event[iNew].rotbst(MtoJRF); iPartonMin.push_back( iNew ); } vector iPartonMid; for (int i = legEnd[legMid]; i >= legBeg[legMid]; --i) { int iNew = event.append( event[ iParton[i] ] ); event[iNew].rotbst(MtoJRF); iPartonMid.push_back( iNew ); } // Find final weighted sum of momenta on each of the two legs. double eWeight = 0.; pWTinJRF[legMin] = 0.; for (int i = iPartonMin.size() - 1; i >= 0; --i) { pWTinJRF[legMin] += event[ iPartonMin[i] ].p() * exp(-eWeight); eWeight += event[ iPartonMin[i] ].e() / eNormJunction; if (eWeight > EJNWEIGHTMAX) break; } eWeight = 0.; pWTinJRF[legMid] = 0.; for (int i = iPartonMid.size() - 1; i >= 0; --i) { pWTinJRF[legMid] += event[ iPartonMid[i] ].p() * exp(-eWeight); eWeight += event[ iPartonMid[i] ].e() / eNormJunction; if (eWeight > EJNWEIGHTMAX) break; } // Define fictitious opposing partons in JRF and store as string ends. Vec4 pOppose = pWTinJRF[legMin]; pOppose.flip3(); int idOppose = (rndmPtr->flat() > 0.5) ? 2 : 1; if (event[ iPartonMin[0] ].col() > 0) idOppose = -idOppose; int iOppose = event.append( idOppose, 77, 0, 0, 0, 0, 0, 0, pOppose, 0.); iPartonMin.push_back( iOppose); pOppose = pWTinJRF[legMid]; pOppose.flip3(); idOppose = (rndmPtr->flat() > 0.5) ? 2 : 1; if (event[ iPartonMid[0] ].col() > 0) idOppose = -idOppose; iOppose = event.append( idOppose, 77, 0, 0, 0, 0, 0, 0, pOppose, 0.); iPartonMid.push_back( iOppose); // Set up kinematics of string evolution in low-energy temporary systems. systemMin.setUp(iPartonMin, event); systemMid.setUp(iPartonMid, event); // Outer fallback loop, when too little energy left for third leg. int idMin = 0; int idMid = 0; Vec4 pDiquark; for ( int iTryOuter = 0; ; ++iTryOuter) { // Middle fallback loop, when much unused energy in leg remnants. double eLeftMin = 0.; double eLeftMid = 0.; for ( int iTryMiddle = 0; ; ++iTryMiddle) { // Loop over the two lowest-energy legs. for (int legLoop = 0; legLoop < 2; ++ legLoop) { int legNow = (legLoop == 0) ? legMin : legMid; // Read in properties specific to this leg. StringSystem& systemNow = (legLoop == 0) ? systemMin : systemMid; int idPos = (legLoop == 0) ? event[ iPartonMin[0] ].id() : event[ iPartonMid[0] ].id(); idOppose = (legLoop == 0) ? event[ iPartonMin.back() ].id() : event[ iPartonMid.back() ].id(); double eInJRF = pInJRF[legNow].e(); int statusHad = (legLoop == 0) ? 85 : 86; // Inner fallback loop, when a diquark comes in to junction. double eUsed = 0.; for ( int iTryInner = 0; ; ++iTryInner) { if (iTryInner > 2 * NTRYJNMATCH) { infoPtr->errorMsg("Error in StringFragmentation::fragment" "ToJunction: caught in junction flavour loop"); event.popBack( iPartonMin.size() + iPartonMid.size() ); return false; } bool needBaryon = (abs(idPos) > 10 && iTryInner > NTRYJNMATCH); double eExtra = (iTryInner > NTRYJNMATCH) ? EEXTRAJNMATCH : 0.; // Set up two string ends, and begin fragmentation loop. setStartEnds(idPos, idOppose, systemNow); eUsed = 0.; int nHadrons = 0; bool noNegE = true; for ( ; ; ++nHadrons) { // Construct trial hadron from positive end. posEnd.newHadron(); Vec4 pHad = posEnd.kinematicsHadron(systemNow); // Negative energy signals failure in construction. if (pHad.e() < 0. ) { noNegE = false; break; } // Break if passed system midpoint ( = junction) in energy. // Exceptions: small systems, and/or with diquark end. bool delayedBreak = false; if (eUsed + pHad.e() + eExtra > eInJRF) { if (nHadrons > 0 || !needBaryon) break; delayedBreak = true; } // Else construct kinematics of the new hadron and store it. hadrons.append( posEnd.idHad, statusHad, iPos, iNeg, 0, 0, 0, 0, pHad, posEnd.mHad); // Update string end and remaining momentum. posEnd.update(); eUsed += pHad.e(); // Delayed break in small systems, and/or with diquark end. if (delayedBreak) { ++nHadrons; break; } } // End of fragmentation loop. Inner loopback if ends on a diquark. if ( noNegE && abs(posEnd.flavOld.id) < 10 ) break; hadrons.popBack(nHadrons); } // End of one-leg fragmentation. Store end quark and remnant energy. if (legNow == legMin) { idMin = posEnd.flavOld.id; eLeftMin = eInJRF - eUsed; } else { idMid = posEnd.flavOld.id; eLeftMid = eInJRF - eUsed; } } // End of both-leg fragmentation. // Middle loopback if too much energy left. double eTrial = eBothLeftJunction + rndmPtr->flat() * eMaxLeftJunction; if (iTryMiddle > NTRYJNMATCH || ( min( eLeftMin, eLeftMid) < eBothLeftJunction && max( eLeftMin, eLeftMid) < eTrial ) ) break; hadrons.clear(); } // Boost hadrons away from the JRF to the original frame. for (int i = 0; i < hadrons.size(); ++i) { hadrons[i].rotbst(MfromJRF); // Recalculate energy to compensate for numerical precision loss // in iterative calculation of MfromJRF. hadrons[i].e( hadrons[i].eCalc() ); pJunctionHadrons += hadrons[i].p(); } // Outer loopback if combined diquark mass too negative // or too little energy left in third leg. pDiquark = pInLeg[legMin] + pInLeg[legMid] - pJunctionHadrons; double m2Left = m2( pInLeg[legMax], pDiquark); if (iTryOuter > NTRYJNMATCH || (pDiquark.mCalc() > MDIQUARKMIN && m2Left > eMinLeftJunction * pInLeg[legMax].e()) ) break; hadrons.clear(); pJunctionHadrons = 0.; } // Now found solution; no more loopback. Remove temporary parton copies. event.popBack( iPartonMin.size() + iPartonMid.size() ); // Construct and store an effective diquark string end from the // two remnant quark ends, for temporary usage. int idDiquark = flavSelPtr->makeDiquark( idMin, idMid); double mDiquark = pDiquark.mCalc(); int iDiquark = event.append( idDiquark, 78, 0, 0, 0, 0, 0, 0, pDiquark, mDiquark); // Find the partons on the last leg, again in reverse order. vector iPartonMax; for (int i = legEnd[legMax]; i >= legBeg[legMax]; --i) iPartonMax.push_back( iParton[i] ); iPartonMax.push_back( iDiquark ); // Recluster gluons nearby to diquark end when taken too much energy. int iPsize = iPartonMax.size(); double m0Diquark = event[iDiquark].m0(); while (iPsize > 2) { Vec4 pGluNear = event[ iPartonMax[iPsize - 2] ].p(); if ( (pDiquark + 0.5 * pGluNear).mCalc() > m0Diquark + mJoin ) break; pDiquark += pGluNear; event[iDiquark].p( pDiquark ); event[iDiquark].m( pDiquark.mCalc() ); iPartonMax.pop_back(); --iPsize; iPartonMax[iPsize - 1] = iDiquark; } // Modify parton list to remaining leg + remnant of the first two. iParton = iPartonMax; // Done. return true; } //-------------------------------------------------------------------------- // Find the boost matrix to the rest frame of a junction, // given the three respective endpoint four-momenta. RotBstMatrix StringFragmentation::junctionRestFrame(Vec4& p0, Vec4& p1, Vec4& p2) { // Calculate masses and other invariants. Vec4 pSumJun = p0 + p1 + p2; double sHat = pSumJun.m2Calc(); double pp[3][3]; pp[0][0] = p0.m2Calc(); pp[1][1] = p1.m2Calc(); pp[2][2] = p2.m2Calc(); pp[0][1] = pp[1][0] = p0 * p1; pp[0][2] = pp[2][0] = p0 * p2; pp[1][2] = pp[2][1] = p1 * p2; // Requirement (eiMax)_j = pi*pj/mj < (eiMax)_k = pi*pk/mk, used below, // here rewritten as pi*pj * mk < pi*pk * mj and squared. double eMax01 = pow2(pp[0][1]) * pp[2][2]; double eMax02 = pow2(pp[0][2]) * pp[1][1]; double eMax12 = pow2(pp[1][2]) * pp[0][0]; // Initially pick i to be the most massive parton. but allow other tries. int i = (pp[1][1] > pp[0][0]) ? 1 : 0; if (pp[2][2] > max(pp[0][0], pp[1][1])) i = 2; int j, k; double ei = 0.; double ej = 0.; double ek = 0.; for (int iTry = 0; iTry < 3; ++iTry) { // Pick j to give minimal eiMax, and k the third vector. if (i == 0) j = (eMax02 < eMax01) ? 2 : 1; else if (i == 1) j = (eMax12 < eMax01) ? 2 : 0; else j = (eMax12 < eMax02) ? 1 : 0; k = 3 - i - j; // Alternative names according to i, j, k conventions. double m2i = pp[i][i]; double m2j = pp[j][j]; double m2k = pp[k][k]; double pipj = pp[i][j]; double pipk = pp[i][k]; double pjpk = pp[j][k]; // Trivial to find new parton energies if all three partons are massless. if (m2i < M2MAXJRF) { ei = sqrt( 2. * pipk * pipj / (3. * pjpk) ); ej = sqrt( 2. * pjpk * pipj / (3. * pipk) ); ek = sqrt( 2. * pipk * pjpk / (3. * pipj) ); // Else find three-momentum range for parton i and values at extremes. } else { // Minimum when i is at rest. double piMin = 0.; double eiMin = sqrt(m2i); double ejMin = pipj / eiMin; double ekMin = pipk / eiMin; double pjMin = sqrtpos( ejMin*ejMin - m2j ); double pkMin = sqrtpos( ekMin*ekMin - m2k ); double fMin = ejMin * ekMin + 0.5 * pjMin * pkMin - pjpk; // Maximum estimated when j + k is at rest, alternatively j at rest. double eiMax = (pipj + pipk) / sqrt(m2j + m2k + 2. * pjpk); if (m2j > M2MAXJRF) eiMax = min( eiMax, pipj / sqrt(m2j) ); double piMax = sqrtpos( eiMax*eiMax - m2i ); double temp = eiMax*eiMax - 0.25 *piMax*piMax; double pjMax = (eiMax * sqrtpos( pipj*pipj - m2j * temp ) - 0.5 * piMax * pipj) / temp; double pkMax = (eiMax * sqrtpos( pipk*pipk - m2k * temp ) - 0.5 * piMax * pipk) / temp; double ejMax = sqrt(pjMax*pjMax + m2j); double ekMax = sqrt(pkMax*pkMax + m2k); double fMax = ejMax * ekMax + 0.5 * pjMax * pkMax - pjpk; // If unexpected values at upper endpoint then pick another parton. if (fMax > 0.) { int iPrel = (i + 1)%3; if (pp[iPrel][iPrel] > M2MAXJRF) {i = iPrel; continue;} ++iTry; iPrel = (i + 2)%3; if (iTry < 3 && pp[iPrel][iPrel] > M2MAXJRF) {i = iPrel; continue;} } // Start binary + linear search to find solution inside range. int iterMin = 0; int iterMax = 0; double pi = 0.5 * (piMin + piMax); for (int iter = 0; iter < NTRYJRFEQ; ++iter) { // Derive momentum of other two partons and distance to root. ei = sqrt(pi*pi + m2i); temp = ei*ei - 0.25 * pi*pi; double pj = (ei * sqrtpos( pipj*pipj - m2j * temp ) - 0.5 * pi * pipj) / temp; double pk = (ei * sqrtpos( pipk*pipk - m2k * temp ) - 0.5 * pi * pipk) / temp; ej = sqrt(pj*pj + m2j); ek = sqrt(pk*pk + m2k); double fNow = ej * ek + 0.5 * pj * pk - pjpk; // Replace lower or upper bound by new value. if (fNow > 0.) { ++iterMin; piMin = pi; fMin = fNow;} else {++iterMax; piMax = pi; fMax = fNow;} // Pick next i momentum to explore, hopefully closer to root. if (2 * iter < NTRYJRFEQ && (iterMin < 2 || iterMax < 2 || 4 * iter < NTRYJRFEQ)) { pi = 0.5 * (piMin + piMax); continue;} if (fMin < 0. || fMax > 0. || abs(fNow) < CONVJRFEQ * sHat) break; pi = piMin + (piMax - piMin) * fMin / (fMin - fMax); } // If arrived here then either succeeded or exhausted possibilities. } break; } // Now we know the energies in the junction rest frame. double eNew[3] = { 0., 0., 0.}; eNew[i] = ei; eNew[j] = ej; eNew[k] = ek; // Boost (copy of) partons to their rest frame. RotBstMatrix Mmove; Vec4 p0cm = p0; Vec4 p1cm = p1; Vec4 p2cm = p2; Mmove.bstback(pSumJun); p0cm.rotbst(Mmove); p1cm.rotbst(Mmove); p2cm.rotbst(Mmove); // Construct difference vectors and the boost to junction rest frame. Vec4 pDir01 = p0cm / p0cm.e() - p1cm / p1cm.e(); Vec4 pDir02 = p0cm / p0cm.e() - p2cm / p2cm.e(); double pDiff01 = pDir01.pAbs2(); double pDiff02 = pDir02.pAbs2(); double pDiff0102 = dot3(pDir01, pDir02); double eDiff01 = eNew[0] / p0cm.e() - eNew[1] / p1cm.e(); double eDiff02 = eNew[0] / p0cm.e() - eNew[2] / p2cm.e(); double denom = pDiff01 * pDiff02 - pDiff0102*pDiff0102; double coef01 = (eDiff01 * pDiff02 - eDiff02 * pDiff0102) / denom; double coef02 = (eDiff02 * pDiff01 - eDiff01 * pDiff0102) / denom; Vec4 vJunction = coef01 * pDir01 + coef02 * pDir02; vJunction.e( sqrt(1. + vJunction.pAbs2()) ); // Add two boosts, giving final result. Mmove.bst(vJunction); return Mmove; } //-------------------------------------------------------------------------- // When string fragmentation has failed several times, // try to join some more nearby partons. int StringFragmentation::extraJoin(double facExtra, Event& event) { // Keep on looping while pairs found below joining threshold. int nJoin = 0; int iPsize = iParton.size(); while (iPsize > 2) { // Look for the pair of neighbour partons (along string) with // the smallest invariant mass (subtracting quark masses). int iJoinMin = -1; double mJoinMin = 2. * facExtra * mJoin; for (int i = 0; i < iPsize - 1; ++i) { Particle& parton1 = event[ iParton[i] ]; Particle& parton2 = event[ iParton[i + 1] ]; Vec4 pSumNow; pSumNow += (parton2.isGluon()) ? 0.5 * parton1.p() : parton1.p(); pSumNow += (parton2.isGluon()) ? 0.5 * parton2.p() : parton2.p(); double mJoinNow = pSumNow.mCalc(); if (!parton1.isGluon()) mJoinNow -= parton1.m0(); if (!parton2.isGluon()) mJoinNow -= parton2.m0(); if (mJoinNow < mJoinMin) { iJoinMin = i; mJoinMin = mJoinNow; } } // Decide whether to join, if not finished. if (iJoinMin < 0 || mJoinMin > facExtra * mJoin) return nJoin; ++nJoin; // Create new joined parton. int iJoin1 = iParton[iJoinMin]; int iJoin2 = iParton[iJoinMin + 1]; int idNew = (event[iJoin1].isGluon()) ? event[iJoin2].id() : event[iJoin1].id(); int colNew = event[iJoin1].col(); int acolNew = event[iJoin2].acol(); if (colNew == acolNew) { colNew = event[iJoin2].col(); acolNew = event[iJoin1].acol(); } Vec4 pNew = event[iJoin1].p() + event[iJoin2].p(); // Append joined parton to event record and reduce parton list. int iNew = event.append( idNew, 73, min(iJoin1, iJoin2), max(iJoin1, iJoin2), 0, 0, colNew, acolNew, pNew, pNew.mCalc() ); iParton[iJoinMin] = iNew; for (int i = iJoinMin + 1; i < iPsize - 1; ++i) iParton[i] = iParton[i + 1]; iParton.pop_back(); --iPsize; // Done. } return nJoin; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/TimeShower.cc0000644000175000017500000052074612217346252015537 0ustar sunsun// TimeShower.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the TimeShower class. #include "Pythia8/TimeShower.h" namespace Pythia8 { //========================================================================== // The TimeShower class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // For small x approximate 1 - sqrt(1 - x) by x/2. const double TimeShower::SIMPLIFYROOT = 1e-8; // Do not allow x too close to 0 or 1 in matrix element expressions. // Warning: cuts into phase space for E_CM > 2 * pTmin * sqrt(1/XMARGIN), // i.e. will become problem roughly for E_CM > 10^6 GeV. const double TimeShower::XMARGIN = 1e-12; const double TimeShower::XMARGINCOMB = 1e-4; // Lower limit on PDF value in order to avoid division by zero. const double TimeShower::TINYPDF = 1e-10; // Big starting value in search for smallest invariant-mass pair. const double TimeShower::LARGEM2 = 1e20; // In g -> q qbar or gamma -> f fbar require m2_pair > this * m2_q/f. const double TimeShower::THRESHM2 = 4.004; // Never pick pT so low that alphaS is evaluated too close to Lambda_3. const double TimeShower::LAMBDA3MARGIN = 1.1; // Rescatter: rescattering + ISR + FSR + primordial kT can lead to // systems not locally conserving momentum. // Fix up momentum in intermediate systems with rescattering const bool TimeShower::FIXRESCATTER = true; // Veto negative energies when using FIXRESCATTER option. const bool TimeShower::VETONEGENERGY = false; // Do not allow too large time- or spacelike virtualities in fixing-up. const double TimeShower::MAXVIRTUALITYFRACTION = 0.5; // Do not allow too large negative spacelike energy in system rest frame. const double TimeShower::MAXNEGENERGYFRACTION = 0.7; //-------------------------------------------------------------------------- // Initialize alphaStrong, alphaEM and related pTmin parameters. void TimeShower::init( BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn) { // Store input pointers for future use. beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; // Main flags. doQCDshower = settingsPtr->flag("TimeShower:QCDshower"); doQEDshowerByQ = settingsPtr->flag("TimeShower:QEDshowerByQ"); doQEDshowerByL = settingsPtr->flag("TimeShower:QEDshowerByL"); doQEDshowerByGamma = settingsPtr->flag("TimeShower:QEDshowerByGamma"); doWeakShower = settingsPtr->flag("TimeShower:weakShower"); doMEcorrections = settingsPtr->flag("TimeShower:MEcorrections"); doMEafterFirst = settingsPtr->flag("TimeShower:MEafterFirst"); doPhiPolAsym = settingsPtr->flag("TimeShower:phiPolAsym"); doInterleave = settingsPtr->flag("TimeShower:interleave"); allowBeamRecoil = settingsPtr->flag("TimeShower:allowBeamRecoil"); dampenBeamRecoil = settingsPtr->flag("TimeShower:dampenBeamRecoil"); recoilToColoured = settingsPtr->flag("TimeShower:recoilToColoured"); // Matching in pT of hard interaction or MPI to shower evolution. pTmaxMatch = settingsPtr->mode("TimeShower:pTmaxMatch"); pTdampMatch = settingsPtr->mode("TimeShower:pTdampMatch"); pTmaxFudge = settingsPtr->parm("TimeShower:pTmaxFudge"); pTmaxFudgeMPI = settingsPtr->parm("TimeShower:pTmaxFudgeMPI"); pTdampFudge = settingsPtr->parm("TimeShower:pTdampFudge"); // Charm and bottom mass thresholds. mc = particleDataPtr->m0(4); mb = particleDataPtr->m0(5); m2c = mc * mc; m2b = mb * mb; // Parameters of scale choices. renormMultFac = settingsPtr->parm("TimeShower:renormMultFac"); factorMultFac = settingsPtr->parm("TimeShower:factorMultFac"); // Parameters of alphaStrong generation. alphaSvalue = settingsPtr->parm("TimeShower:alphaSvalue"); alphaSorder = settingsPtr->mode("TimeShower:alphaSorder"); alphaSnfmax = settingsPtr->mode("StandardModel:alphaSnfmax"); alphaSuseCMW = settingsPtr->flag("TimeShower:alphaSuseCMW"); alphaS2pi = 0.5 * alphaSvalue / M_PI; // Initialize alphaStrong generation. alphaS.init( alphaSvalue, alphaSorder, alphaSnfmax, alphaSuseCMW); // Lambda for 5, 4 and 3 flavours. Lambda3flav = alphaS.Lambda3(); Lambda4flav = alphaS.Lambda4(); Lambda5flav = alphaS.Lambda5(); Lambda5flav2 = pow2(Lambda5flav); Lambda4flav2 = pow2(Lambda4flav); Lambda3flav2 = pow2(Lambda3flav); // Parameters of QCD evolution. Warn if pTmin must be raised. nGluonToQuark = settingsPtr->mode("TimeShower:nGluonToQuark"); pTcolCutMin = settingsPtr->parm("TimeShower:pTmin"); if (pTcolCutMin > LAMBDA3MARGIN * Lambda3flav / sqrt(renormMultFac)) pTcolCut = pTcolCutMin; else { pTcolCut = LAMBDA3MARGIN * Lambda3flav / sqrt(renormMultFac); ostringstream newPTcolCut; newPTcolCut << fixed << setprecision(3) << pTcolCut; infoPtr->errorMsg("Warning in TimeShower::init: pTmin too low", ", raised to " + newPTcolCut.str() ); infoPtr->setTooLowPTmin(true); } pT2colCut = pow2(pTcolCut); // Parameters of alphaEM generation. alphaEMorder = settingsPtr->mode("TimeShower:alphaEMorder"); // Initialize alphaEM generation. alphaEM.init( alphaEMorder, settingsPtr); // Parameters of QED evolution. nGammaToQuark = settingsPtr->mode("TimeShower:nGammaToQuark"); nGammaToLepton = settingsPtr->mode("TimeShower:nGammaToLepton"); pTchgQCut = settingsPtr->parm("TimeShower:pTminChgQ"); pT2chgQCut = pow2(pTchgQCut); pTchgLCut = settingsPtr->parm("TimeShower:pTminChgL"); pT2chgLCut = pow2(pTchgLCut); mMaxGamma = settingsPtr->parm("TimeShower:mMaxGamma"); m2MaxGamma = pow2(mMaxGamma); // Parameters of weak evolution. weakMode = settingsPtr->mode("TimeShower:weakShowerMode"); pTweakCut = settingsPtr->parm("TimeShower:pTminWeak"); pT2weakCut = pow2(pTweakCut); weakEnhancement = settingsPtr->parm("TimeShower:weakShowerEnhancement"); singleWeakEmission = settingsPtr->flag("TimeShower:singleWeakEmission"); extraScaleTerm = settingsPtr->parm("TimeShower:extraScaleTerm"); dopTdampMass = settingsPtr->flag("TimeShower:dopTDampMass"); // Consisteny check for gamma -> f fbar variables. if (nGammaToQuark <= 0 && nGammaToLepton <= 0) doQEDshowerByGamma = false; // Possibility of a global recoil stategy, e.g. for MC@NLO. globalRecoil = settingsPtr->flag("TimeShower:globalRecoil"); nMaxGlobalRecoil = settingsPtr->mode("TimeShower:nMaxGlobalRecoil"); // Number of splittings produced with global recoil. nMaxGlobalBranch = settingsPtr->mode("TimeShower:nMaxGlobalBranch"); // Number of partons in Born-like events, to distinguish between S and H. nFinalBorn = settingsPtr->mode("TimeShower:nPartonsInBorn"); // Flag to allow to start from a scale smaller than scalup. globalRecoilMode = settingsPtr->mode("TimeShower:globalRecoilMode"); // Flag to allow to start from a scale smaller than scalup. limitMUQ = settingsPtr->flag("TimeShower:limitPTmaxGlobal"); // Fraction and colour factor of gluon emission off onium octat state. octetOniumFraction = settingsPtr->parm("TimeShower:octetOniumFraction"); octetOniumColFac = settingsPtr->parm("TimeShower:octetOniumColFac"); // Z0 and W+- properties needed for gamma/Z0 mixing and weak showers. mZ = particleDataPtr->m0(23); gammaZ = particleDataPtr->mWidth(23); thetaWRat = 1. / (16. * coupSMPtr->sin2thetaW() * coupSMPtr->cos2thetaW()); mW = particleDataPtr->m0(24); gammaW = particleDataPtr->mWidth(24); // May have to fix up recoils related to rescattering. allowRescatter = settingsPtr->flag("PartonLevel:MPI") && settingsPtr->flag("MultipartonInteractions:allowRescatter"); // Hidden Valley scenario with further shower activity. doHVshower = settingsPtr->flag("HiddenValley:FSR"); nCHV = settingsPtr->mode("HiddenValley:Ngauge"); alphaHVfix = settingsPtr->parm("HiddenValley:alphaFSR"); pThvCut = settingsPtr->parm("HiddenValley:pTminFSR"); pT2hvCut = pThvCut * pThvCut; CFHV = (nCHV == 1) ? 1. : (nCHV * nCHV - 1.)/(2. * nCHV); idHV = (nCHV == 1) ? 4900022 : 4900021; mHV = particleDataPtr->m0(idHV); brokenHVsym = (nCHV == 1 && mHV > 0.); // Possibility of two predetermined hard emissions in event. doSecondHard = settingsPtr->flag("SecondHard:generate"); // Possibility to allow user veto of emission step. canVetoEmission = (userHooksPtr != 0) ? userHooksPtr->canVetoFSREmission() : false; } //-------------------------------------------------------------------------- // Find whether to limit maximum scale of emissions. // Also allow for dampening at factorization or renormalization scale. bool TimeShower::limitPTmax( Event& event, double Q2Fac, double Q2Ren) { // Find whether to limit pT. Begin by user-set cases. bool dopTlimit = false; dopTlimit1 = dopTlimit2 = false; if (pTmaxMatch == 1) dopTlimit = dopTlimit1 = dopTlimit2 = true; else if (pTmaxMatch == 2) dopTlimit = dopTlimit1 = dopTlimit2 = false; // Look if any quark (u, d, s, c, b), gluon or photon in final state. else { int n21 = 0; for (int i = 5; i < event.size(); ++i) { if (event[i].status() == -21) ++n21; else if (n21 == 0) { int idAbs = event[i].idAbs(); if (idAbs <= 5 || idAbs == 21 || idAbs == 22) dopTlimit1 = true; } else if (n21 == 2) { int idAbs = event[i].idAbs(); if (idAbs <= 5 || idAbs == 21 || idAbs == 22) dopTlimit2 = true; } } dopTlimit = (doSecondHard) ? (dopTlimit1 && dopTlimit2) : dopTlimit1; } // Dampening at factorization or renormalization scale; only for hardest. dopTdamp = false; pT2damp = 0.; if ( !dopTlimit1 && (pTdampMatch == 1 || pTdampMatch == 2) ) { dopTdamp = true; pT2damp = pow2(pTdampFudge) * ((pTdampMatch == 1) ? Q2Fac : Q2Ren); } // Done. return dopTlimit; } //-------------------------------------------------------------------------- // Top-level routine to do a full time-like shower in resonance decay. int TimeShower::shower( int iBeg, int iEnd, Event& event, double pTmax, int nBranchMax) { // Add new system, automatically with two empty beam slots. int iSys = partonSystemsPtr->addSys(); // Loop over allowed range to find all final-state particles. Vec4 pSum; for (int i = iBeg; i <= iEnd; ++i) if (event[i].isFinal()) { partonSystemsPtr->addOut( iSys, i); pSum += event[i].p(); } partonSystemsPtr->setSHat( iSys, pSum.m2Calc() ); // Let prepare routine do the setup. dopTlimit1 = true; dopTlimit2 = true; dopTdamp = false; hasWeaklyRadiated = false; prepare( iSys, event, true); // Begin evolution down in pT from hard pT scale. int nBranch = 0; pTLastBranch = 0.; do { double pTtimes = pTnext( event, pTmax, 0.); // Do a final-state emission (if allowed). if (pTtimes > 0.) { if (branch( event)) { ++nBranch; pTLastBranch = pTtimes; } pTmax = pTtimes; } // Keep on evolving until nothing is left to be done. else pTmax = 0.; } while (pTmax > 0. && (nBranchMax <= 0 || nBranch < nBranchMax)); // Return number of emissions that were performed. return nBranch; } //-------------------------------------------------------------------------- // Top-level routine for QED radiation in hadronic decay to two leptons. // Intentionally only does photon radiation, i.e. no photon branchings. int TimeShower::showerQED( int i1, int i2, Event& event, double pTmax) { // Add new system, automatically with two empty beam slots. int iSys = partonSystemsPtr->addSys(); partonSystemsPtr->addOut( iSys, i1); partonSystemsPtr->addOut( iSys, i2); partonSystemsPtr->setSHat( iSys, m2(event[i1], event[i2]) ); // Charge type of two leptons tells whether MEtype is gamma*/Z0 or W+-. int iChg1 = event[i1].chargeType(); int iChg2 = event[i2].chargeType(); int MEtype = (iChg1 + iChg2 == 0) ? 102 : 101; // Fill dipole-ends list. dipEnd.resize(0); if (iChg1 != 0) dipEnd.push_back( TimeDipoleEnd(i1, i2, pTmax, 0, iChg1, 0, 0, 0, iSys, MEtype, i2) ); if (iChg2 != 0) dipEnd.push_back( TimeDipoleEnd(i2, i1, pTmax, 0, iChg2, 0, 0, 0, iSys, MEtype, i1) ); // Begin evolution down in pT from hard pT scale. int nBranch = 0; pTLastBranch = 0.; do { // Begin loop over all possible radiating dipole ends. dipSel = 0; iDipSel = -1; double pT2sel = 0.; for (int iDip = 0; iDip < int(dipEnd.size()); ++iDip) { TimeDipoleEnd& dip = dipEnd[iDip]; // Dipole properties. dip.mRad = event[dip.iRadiator].m(); dip.mRec = event[dip.iRecoiler].m(); dip.mDip = m( event[dip.iRadiator], event[dip.iRecoiler] ); dip.m2Rad = pow2(dip.mRad); dip.m2Rec = pow2(dip.mRec); dip.m2Dip = pow2(dip.mDip); // Find maximum evolution scale for dipole. dip.m2DipCorr = pow2(dip.mDip - dip.mRec) - dip.m2Rad; double pTbegDip = min( pTmax, dip.pTmax ); double pT2begDip = min( pow2(pTbegDip), 0.25 * dip.m2DipCorr); // Do QED evolution where relevant. dip.pT2 = 0.; if (pT2begDip > pT2sel) { pT2nextQED( pT2begDip, pT2sel, dip, event); // Update if found larger pT than current maximum. End dipole loop. if (dip.pT2 > pT2sel) { pT2sel = dip.pT2; dipSel = &dip; iDipSel = iDip; } } } double pTsel = (dipSel == 0) ? 0. : sqrt(pT2sel); // Do a final-state emission (if allowed). if (pTsel > 0.) { // Find initial radiator and recoiler particles in dipole branching. int iRadBef = dipSel->iRadiator; int iRecBef = dipSel->iRecoiler; Particle& radBef = event[iRadBef]; Particle& recBef = event[iRecBef]; Vec4 pRadBef = event[iRadBef].p(); Vec4 pRecBef = event[iRecBef].p(); // Construct kinematics in dipole rest frame; massless emitter. double pTorig = sqrt( dipSel->pT2); double eRadPlusEmt = 0.5 * (dipSel->m2Dip + dipSel->m2 - dipSel->m2Rec) / dipSel->mDip; double e2RadPlusEmt = pow2(eRadPlusEmt); double pzRadPlusEmt = 0.5 * sqrtpos( pow2(dipSel->m2Dip - dipSel->m2 - dipSel->m2Rec) - 4. * dipSel->m2 * dipSel->m2Rec ) / dipSel->mDip; double pT2corr = dipSel->m2 * (e2RadPlusEmt * dipSel->z * (1. - dipSel->z) - 0.25 * dipSel->m2) / pow2(pzRadPlusEmt); double pTcorr = sqrtpos( pT2corr ); double pzRad = (e2RadPlusEmt * dipSel->z - 0.5 * dipSel->m2) / pzRadPlusEmt; double pzEmt = (e2RadPlusEmt * (1. - dipSel->z) - 0.5 * dipSel->m2) / pzRadPlusEmt; double mRad = dipSel->mRad; double mEmt = 0.; // Kinematics reduction for radiator mass. double m2Ratio = dipSel->m2Rad / dipSel->m2; pTorig *= 1. - m2Ratio; pTcorr *= 1. - m2Ratio; pzRad += pzEmt * m2Ratio; pzEmt *= 1. - m2Ratio; // Store kinematics of branching in dipole rest frame. double phi = 2. * M_PI * rndmPtr->flat(); Vec4 pRad = Vec4( pTcorr * cos(phi), pTcorr * sin(phi), pzRad, sqrt( pow2(pTcorr) + pow2(pzRad) + pow2(mRad) ) ); Vec4 pEmt = Vec4( -pRad.px(), -pRad.py(), pzEmt, sqrt( pow2(pTcorr) + pow2(pzEmt) + pow2(mEmt) ) ); Vec4 pRec = Vec4( 0., 0., -pzRadPlusEmt, sqrt( pow2(pzRadPlusEmt) + dipSel->m2Rec ) ); // Rotate and boost dipole products to the event frame. RotBstMatrix M; M.fromCMframe(pRadBef, pRecBef); pRad.rotbst(M); pEmt.rotbst(M); pRec.rotbst(M); // Define new particles from dipole branching. Particle rad = Particle(radBef.id(), 51, iRadBef, 0, 0, 0, radBef.col(), radBef.acol(), pRad, mRad, pTsel); Particle emt = Particle(22, 51, iRadBef, 0, 0, 0, 0, 0, pEmt, mEmt, pTsel); Particle rec = Particle(recBef.id(), 52, iRecBef, iRecBef, 0, 0, recBef.col(), recBef.acol(), pRec, dipSel->mRec, pTsel); // ME corrections can lead to branching being rejected. if (dipSel->MEtype == 0 || findMEcorr( dipSel, rad, rec, emt, false) > rndmPtr->flat() ) { // Shower may occur at a displaced vertex, or for unstable particle. if (radBef.hasVertex()) { rad.vProd( radBef.vProd() ); emt.vProd( radBef.vProd() ); } if (recBef.hasVertex()) rec.vProd( recBef.vProd() ); rad.tau( event[iRadBef].tau() ); rec.tau( event[iRecBef].tau() ); // Put new particles into the event record. int iRad = event.append(rad); int iEmt = event.append(emt); event[iRadBef].statusNeg(); event[iRadBef].daughters( iRad, iEmt); int iRec = event.append(rec); event[iRecBef].statusNeg(); event[iRecBef].daughters( iRec, iRec); // Update to new dipole ends. dipSel->iRadiator = iRad; dipSel->iRecoiler = iRec; dipSel->pTmax = pTsel; // Update other dipoles that also involved the radiator or recoiler. for (int i = 0; i < int(dipEnd.size()); ++i) if (i != iDipSel) { if (dipEnd[i].iRadiator == iRadBef) dipEnd[i].iRadiator = iRad; if (dipEnd[i].iRecoiler == iRadBef) dipEnd[i].iRecoiler = iRad; if (dipEnd[i].iMEpartner == iRadBef) dipEnd[i].iMEpartner = iRad; if (dipEnd[i].iRadiator == iRecBef) dipEnd[i].iRadiator = iRec; if (dipEnd[i].iRecoiler == iRecBef) dipEnd[i].iRecoiler = iRec; if (dipEnd[i].iMEpartner == iRecBef) dipEnd[i].iMEpartner = iRec; } // Done with branching ++nBranch; pTLastBranch = pTsel; } pTmax = pTsel; } // Keep on evolving until nothing is left to be done. else pTmax = 0.; } while (pTmax > 0.); // Return number of emissions that were performed. return nBranch; } //-------------------------------------------------------------------------- // Global recoil: reset counters and store locations of outgoing partons. void TimeShower::prepareGlobal( Event& event) { // Global recoils: reset some counters. nGlobal = 0; nHard = 0; nProposed = 0; hardPartons.resize(0); // Global recoils: store positions of hard outgoing partons. // No global recoil for H events. if (globalRecoil) { for (int i = 0; i < event.size(); ++i) if (event[i].isFinal() && event[i].colType() != 0) hardPartons.push_back(i); nHard = hardPartons.size(); if (nFinalBorn > 0 && nHard > nFinalBorn) { hardPartons.resize(0); nHard = 0; } } } //-------------------------------------------------------------------------- // Prepare system for evolution; identify ME. void TimeShower::prepare( int iSys, Event& event, bool limitPTmaxIn, double pTfirstTrialIn) { // Reset number of proposed splittings. nProposed = 0; // Reset W/Z radiation flag at first call for new event. if (iSys == 0) hasWeaklyRadiated = false; // Reset dipole-ends list for first interaction and for resonance decays. int iInA = partonSystemsPtr->getInA(iSys); int iInB = partonSystemsPtr->getInB(iSys); if (iSys == 0 || iInA == 0) dipEnd.resize(0); int dipEndSizeBeg = dipEnd.size(); // No dipoles for 2 -> 1 processes. if (partonSystemsPtr->sizeOut(iSys) < 2) return; // In case of DPS overwrite limitPTmaxIn by saved value. if (doSecondHard && iSys == 0) limitPTmaxIn = dopTlimit1; if (doSecondHard && iSys == 1) limitPTmaxIn = dopTlimit2; // Loop through final state of system to find possible dipole ends. for (int i = 0; i < partonSystemsPtr->sizeOut(iSys); ++i) { int iRad = partonSystemsPtr->getOut( iSys, i); if (event[iRad].isFinal() && event[iRad].scale() > 0.) { // Identify colour octet onium state. Check whether QCD shower allowed. int idRad = event[iRad].id(); int idRadAbs = abs(idRad); bool isOctetOnium = ( idRad == 9900441 || idRad == 9900443 || idRad == 9910441 || idRad == 9900551 || idRad == 9900553 || idRad == 9910551 ); bool doQCD = doQCDshower; if (doQCD && isOctetOnium) doQCD = (rndmPtr->flat() < octetOniumFraction); // Find dipole end formed by colour index. int colTag = event[iRad].col(); if (doQCD && colTag > 0) setupQCDdip( iSys, i, colTag, 1, event, isOctetOnium, limitPTmaxIn); // Find dipole end formed by anticolour index. int acolTag = event[iRad].acol(); if (doQCD && acolTag > 0) setupQCDdip( iSys, i, acolTag, -1, event, isOctetOnium, limitPTmaxIn); // Find "charge-dipole" and "photon-dipole" ends. int chgType = event[iRad].chargeType(); bool doChgDip = (chgType != 0) && ( ( doQEDshowerByQ && event[iRad].isQuark() ) || ( doQEDshowerByL && event[iRad].isLepton() ) ); int gamType = (idRad == 22) ? 1 : 0; bool doGamDip = (gamType == 1) && doQEDshowerByGamma; if (doChgDip || doGamDip) setupQEDdip( iSys, i, chgType, gamType, event, limitPTmaxIn); // Find weak diple ends. if (doWeakShower && (event[iRad].isQuark() || event[iRad].isLepton())) { if(weakMode == 0 || weakMode == 1) setupWeakdip( iSys, i, 1, event, limitPTmaxIn); if(weakMode == 0 || weakMode == 2) setupWeakdip( iSys, i, 2, event, limitPTmaxIn); } // Find Hidden Valley dipole ends. bool isHVrad = (idRadAbs > 4900000 && idRadAbs < 4900007) || (idRadAbs > 4900010 && idRadAbs < 4900017) || idRadAbs == 4900101; if (doHVshower && isHVrad) setupHVdip( iSys, i, event, limitPTmaxIn); // End loop over system final state. Have now found the dipole ends. } } // Loop through dipole ends to find matrix element corrections. for (int iDip = dipEndSizeBeg; iDip < int(dipEnd.size()); ++iDip) findMEtype( event, dipEnd[iDip]); // Update dipole list after a multiparton interactions rescattering. if (iSys > 0 && ( (iInA > 0 && event[iInA].status() == -34) || (iInB > 0 && event[iInB].status() == -34) ) ) rescatterUpdate( iSys, event); // Set the maximum first trial emission's pT: pTfirstTrial = pTfirstTrialIn; } //-------------------------------------------------------------------------- // Update dipole list after a multiparton interactions rescattering. void TimeShower::rescatterUpdate( int iSys, Event& event) { // Loop over two incoming partons in system; find their rescattering mother. // (iOut is outgoing from old system = incoming iIn of rescattering system.) for (int iResc = 0; iResc < 2; ++iResc) { int iIn = (iResc == 0) ? partonSystemsPtr->getInA(iSys) : partonSystemsPtr->getInB(iSys); if (iIn == 0 || event[iIn].status() != -34) continue; int iOut = event[iIn].mother1(); // Loop over all dipoles. int dipEndSize = dipEnd.size(); for (int iDip = 0; iDip < dipEndSize; ++iDip) { TimeDipoleEnd& dipNow = dipEnd[iDip]; // Kill dipoles where rescattered parton is radiator. if (dipNow.iRadiator == iOut) { dipNow.colType = 0; dipNow.chgType = 0; dipNow.gamType = 0; continue; } // No matrix element for dipoles between scatterings. if (dipNow.iMEpartner == iOut) { dipNow.MEtype = 0; dipNow.iMEpartner = -1; } // Update dipoles where outgoing rescattered parton is recoiler. if (dipNow.iRecoiler == iOut) { int iRad = dipNow.iRadiator; // Colour dipole: recoil in final state, initial state or new. if (dipNow.colType > 0) { int colTag = event[iRad].col(); bool done = false; for (int i = 0; i < partonSystemsPtr->sizeOut(iSys); ++i) { int iRecNow = partonSystemsPtr->getOut( iSys, i); if (event[iRecNow].acol() == colTag) { dipNow.iRecoiler = iRecNow; dipNow.systemRec = iSys; dipNow.MEtype = 0; done = true; break; } } if (!done) { int iIn2 = (iResc == 0) ? partonSystemsPtr->getInB(iSys) : partonSystemsPtr->getInA(iSys); if (event[iIn2].col() == colTag) { dipNow.iRecoiler = iIn2; dipNow.systemRec = iSys; dipNow.MEtype = 0; int isrType = event[iIn2].mother1(); // This line in case mother is a rescattered parton. while (isrType > 2 + beamOffset) isrType = event[isrType].mother1(); if (isrType > 2) isrType -= beamOffset; dipNow.isrType = isrType; done = true; } } // If above options failed, then create new dipole. if (!done) { int iRadNow = partonSystemsPtr->getIndexOfOut(dipNow.system, iRad); if (iRadNow != -1) setupQCDdip(dipNow.system, iRadNow, event[iRad].col(), 1, event, dipNow.isOctetOnium, true); else infoPtr->errorMsg("Warning in TimeShower::rescatterUpdate: " "failed to locate radiator in system"); dipNow.colType = 0; dipNow.chgType = 0; dipNow.gamType = 0; infoPtr->errorMsg("Warning in TimeShower::rescatterUpdate: " "failed to locate new recoiling colour partner"); } // Anticolour dipole: recoil in final state, initial state or new. } else if (dipNow.colType < 0) { int acolTag = event[iRad].acol(); bool done = false; for (int i = 0; i < partonSystemsPtr->sizeOut(iSys); ++i) { int iRecNow = partonSystemsPtr->getOut( iSys, i); if (event[iRecNow].col() == acolTag) { dipNow.iRecoiler = iRecNow; dipNow.systemRec = iSys; dipNow.MEtype = 0; done = true; break; } } if (!done) { int iIn2 = (iResc == 0) ? partonSystemsPtr->getInB(iSys) : partonSystemsPtr->getInA(iSys); if (event[iIn2].acol() == acolTag) { dipNow.iRecoiler = iIn2; dipNow.systemRec = iSys; dipNow.MEtype = 0; int isrType = event[iIn2].mother1(); // This line in case mother is a rescattered parton. while (isrType > 2 + beamOffset) isrType = event[isrType].mother1(); if (isrType > 2) isrType -= beamOffset; dipNow.isrType = isrType; done = true; } } // If above options failed, then create new dipole. if (!done) { int iRadNow = partonSystemsPtr->getIndexOfOut(dipNow.system, iRad); if (iRadNow != -1) setupQCDdip(dipNow.system, iRadNow, event[iRad].acol(), -1, event, dipNow.isOctetOnium, true); else infoPtr->errorMsg("Warning in TimeShower::rescatterUpdate: " "failed to locate radiator in system"); dipNow.colType = 0; dipNow.chgType = 0; dipNow.gamType = 0; infoPtr->errorMsg("Warning in TimeShower::rescatterUpdate: " "failed to locate new recoiling colour partner"); } // Charge or photon dipoles: same flavour in final or initial state. } else if (dipNow.chgType != 0 || dipNow.gamType != 0) { int idTag = event[dipNow.iRecoiler].id(); bool done = false; for (int i = 0; i < partonSystemsPtr->sizeOut(iSys); ++i) { int iRecNow = partonSystemsPtr->getOut( iSys, i); if (event[iRecNow].id() == idTag) { dipNow.iRecoiler = iRecNow; dipNow.systemRec = iSys; dipNow.MEtype = 0; done = true; break; } } if (!done) { int iIn2 = (iResc == 0) ? partonSystemsPtr->getInB(iSys) : partonSystemsPtr->getInA(iSys); if (event[iIn2].id() == -idTag) { dipNow.iRecoiler = iIn2; dipNow.systemRec = iSys; dipNow.MEtype = 0; int isrType = event[iIn2].mother1(); // This line in case mother is a rescattered parton. while (isrType > 2 + beamOffset) isrType = event[isrType].mother1(); if (isrType > 2) isrType -= beamOffset; dipNow.isrType = isrType; done = true; } } // If above options failed, then create new dipole if (!done) { int iRadNow = partonSystemsPtr->getIndexOfOut(dipNow.system, iRad); if (iRadNow != -1) setupQEDdip(dipNow.system, iRadNow, dipNow.chgType, dipNow.gamType, event, true); else infoPtr->errorMsg("Warning in TimeShower::rescatterUpdate: " "failed to locate radiator in system"); dipNow.colType = 0; dipNow.chgType = 0; dipNow.gamType = 0; infoPtr->errorMsg("Warning in TimeShower::rescatterUpdate: " "failed to locate new recoiling charge partner"); } } } // End of loop over dipoles and two incoming sides. } } } //-------------------------------------------------------------------------- // Update dipole list after each ISR emission (so not used for resonances). void TimeShower::update( int iSys, Event& event) { // Start list of rescatterers that gave further changed systems in ISR. vector iRescatterer; // Find new and old positions of incoming partons in the system. vector iNew, iOld; iNew.push_back( partonSystemsPtr->getInA(iSys) ); iOld.push_back( event[iNew[0]].daughter2() ); iNew.push_back( partonSystemsPtr->getInB(iSys) ); iOld.push_back( event[iNew[1]].daughter2() ); // Ditto for outgoing partons, except the newly created one. int sizeOut = partonSystemsPtr->sizeOut(iSys) - 1; for (int i = 0; i < sizeOut; ++i) { int iNow = partonSystemsPtr->getOut(iSys, i); iNew.push_back( iNow ); iOld.push_back( event[iNow].mother1() ); // Add non-final to list of rescatterers. if (!event[iNow].isFinal()) iRescatterer.push_back( iNow ); } int iNewNew = partonSystemsPtr->getOut(iSys, sizeOut); // Swap beams to let 0 be side on which branching occured. if (event[iNew[0]].status() != -41) { swap( iNew[0], iNew[1]); swap( iOld[0], iOld[1]); } // Loop over all dipole ends belonging to the system // or to the recoil system, if different. for (int iDip = 0; iDip < int(dipEnd.size()); ++iDip) if (dipEnd[iDip].system == iSys || dipEnd[iDip].systemRec == iSys) { TimeDipoleEnd& dipNow = dipEnd[iDip]; // Replace radiator (always in final state so simple). for (int i = 2; i < 2 + sizeOut; ++i) if (dipNow.iRadiator == iOld[i]) { dipNow.iRadiator = iNew[i]; break; } // Replace ME partner (always in final state, if exists, so simple). for (int i = 2; i < 2 + sizeOut; ++i) if (dipNow.iMEpartner == iOld[i]) { dipNow.iMEpartner = iNew[i]; break; } // Recoiler: by default pick old one, only moved. Note excluded beam. int iRec = 0; if (dipNow.systemRec == iSys) { for (int i = 1; i < 2 + sizeOut; ++i) if (dipNow.iRecoiler == iOld[i]) { iRec = iNew[i]; break; } // QCD recoiler: check if colour hooks up with new final parton. if ( dipNow.colType > 0 && event[dipNow.iRadiator].col() == event[iNewNew].acol() ) { iRec = iNewNew; dipNow.isrType = 0; } if ( dipNow.colType < 0 && event[dipNow.iRadiator].acol() == event[iNewNew].col() ) { iRec = iNewNew; dipNow.isrType = 0; } // QCD recoiler: check if colour hooks up with new beam parton. if ( iRec == 0 && dipNow.colType > 0 && event[dipNow.iRadiator].col() == event[iNew[0]].col() ) iRec = iNew[0]; if ( iRec == 0 && dipNow.colType < 0 && event[dipNow.iRadiator].acol() == event[iNew[0]].acol() ) iRec = iNew[0]; // QED/photon recoiler: either to new particle or remains to beam. if ( iRec == 0 && (dipNow.chgType != 0 || dipNow.gamType != 0) ) { if ( event[iNew[0]].chargeType() == 0 ) { iRec = iNewNew; dipNow.isrType = 0; } else { iRec = iNew[0]; } } // Recoiler in another system: keep it as is. } else iRec = dipNow.iRecoiler; // Done. Kill dipole if failed to find new recoiler. dipNow.iRecoiler = iRec; if ( iRec == 0 && (dipNow.colType != 0 || dipNow.chgType != 0 || dipNow.gamType != 0) ) { dipNow.colType = 0; dipNow.chgType = 0; dipNow.gamType = 0; infoPtr->errorMsg("Error in TimeShower::update: " "failed to locate new recoiling partner"); } } // Find new dipole end formed by colour index. int colTag = event[iNewNew].col(); if (doQCDshower && colTag > 0) setupQCDdip( iSys, sizeOut, colTag, 1, event, false, true); // Find new dipole end formed by anticolour index. int acolTag = event[iNewNew].acol(); if (doQCDshower && acolTag > 0) setupQCDdip( iSys, sizeOut, acolTag, -1, event, false, true); // Find new "charge-dipole" and "photon-dipole" ends. int chgType = event[iNewNew].chargeType(); bool doChgDip = (chgType != 0) && ( ( doQEDshowerByQ && event[iNewNew].isQuark() ) || ( doQEDshowerByL && event[iNewNew].isLepton() ) ); int gamType = (event[iNewNew].id() == 22) ? 1 : 0; bool doGamDip = (gamType == 1) && doQEDshowerByGamma; if (doChgDip || doGamDip) setupQEDdip( iSys, sizeOut, chgType, gamType, event, true); // Start iterate over list of rescatterers - may be empty. int iRescNow = -1; while (++iRescNow < int(iRescatterer.size())) { // Identify systems that rescatterers belong to. int iOutNew = iRescatterer[iRescNow]; int iInNew = event[iOutNew].daughter1(); int iSysResc = partonSystemsPtr->getSystemOf(iInNew, true); // Find new and old positions of incoming partons in the system. iNew.resize(0); iOld.resize(0); iNew.push_back( partonSystemsPtr->getInA(iSysResc) ); iOld.push_back( event[iNew[0]].daughter1() ); iNew.push_back( partonSystemsPtr->getInB(iSysResc) ); iOld.push_back( event[iNew[1]].daughter1() ); // Ditto for outgoing partons. sizeOut = partonSystemsPtr->sizeOut(iSysResc); for (int i = 0; i < sizeOut; ++i) { int iNow = partonSystemsPtr->getOut(iSysResc, i); iNew.push_back( iNow ); iOld.push_back( event[iNow].mother1() ); // Add non-final to list of rescatterers. if (!event[iNow].isFinal()) iRescatterer.push_back( iNow ); } // Loop over all dipole ends belonging to the system // or to the recoil system, if different. for (int iDip = 0; iDip < int(dipEnd.size()); ++iDip) if (dipEnd[iDip].system == iSysResc || dipEnd[iDip].systemRec == iSysResc) { TimeDipoleEnd& dipNow = dipEnd[iDip]; // Replace radiator (always in final state so simple). for (int i = 2; i < 2 + sizeOut; ++i) if (dipNow.iRadiator == iOld[i]) { dipNow.iRadiator = iNew[i]; break; } // Replace ME partner (always in final state, if exists, so simple). for (int i = 2; i < 2 + sizeOut; ++i) if (dipNow.iMEpartner == iOld[i]) { dipNow.iMEpartner = iNew[i]; break; } // Replace recoiler. for (int i = 0; i < 2 + sizeOut; ++i) if (dipNow.iRecoiler == iOld[i]) { dipNow.iRecoiler = iNew[i]; break; } } // End iterate over list of rescatterers. } } //-------------------------------------------------------------------------- // Setup a dipole end for a QCD colour charge. void TimeShower::setupQCDdip( int iSys, int i, int colTag, int colSign, Event& event, bool isOctetOnium, bool limitPTmaxIn) { // Initial values. Find if allowed to hook up beams. int iRad = partonSystemsPtr->getOut(iSys, i); int iRec = 0; int sizeAllA = partonSystemsPtr->sizeAll(iSys); int sizeOut = partonSystemsPtr->sizeOut(iSys); int sizeAll = ( allowBeamRecoil ) ? sizeAllA : sizeOut; int sizeIn = sizeAll - sizeOut; int sizeInA = sizeAllA - sizeIn - sizeOut; int iOffset = i + sizeAllA - sizeOut; bool otherSystemRec = false; bool allowInitial = (partonSystemsPtr->hasInAB(iSys)) ? true : false; // PS dec 2010: possibility to allow for several recoilers and each with // flexible normalization bool isFlexible = false; double flexFactor = 1.0; vector iRecVec(0); // Colour: other end by same index in beam or opposite in final state. // Exclude rescattered incoming and not final outgoing. if (colSign > 0) for (int j = 0; j < sizeAll; ++j) if (j + sizeInA != iOffset) { int iRecNow = partonSystemsPtr->getAll(iSys, j + sizeInA); if ( ( j < sizeIn && event[iRecNow].col() == colTag && !event[iRecNow].isRescatteredIncoming() ) || ( j >= sizeIn && event[iRecNow].acol() == colTag && event[iRecNow].isFinal() ) ) { iRec = iRecNow; break; } } // Anticolour: other end by same index in beam or opposite in final state. // Exclude rescattered incoming and not final outgoing. if (colSign < 0) for (int j = 0; j < sizeAll; ++j) if (j + sizeInA != iOffset) { int iRecNow = partonSystemsPtr->getAll(iSys, j + sizeInA); if ( ( j < sizeIn && event[iRecNow].acol() == colTag && !event[iRecNow].isRescatteredIncoming() ) || ( j >= sizeIn && event[iRecNow].col() == colTag && event[iRecNow].isFinal() ) ) { iRec = iRecNow; break; } } // Resonance decays (= no instate): // other end to nearest recoiler in same system final state, // by (p_i + p_j)^2 - (m_i + m_j)^2 = 2 (p_i p_j - m_i m_j). // (junction colours more involved, so keep track if junction colour) bool hasJunction = false; if (iRec == 0 && !allowInitial) { for (int iJun = 0; iJun < event.sizeJunction(); ++ iJun) { // For types 1&2, all legs in final state // For types 3&4, two legs in final state // For types 5&6, one leg in final state int iBeg = (event.kindJunction(iJun)-1)/2; for (int iLeg = iBeg; iLeg < 3; ++iLeg) if (event.endColJunction( iJun, iLeg) == colTag) hasJunction = true; } double ppMin = LARGEM2; for (int j = 0; j < sizeOut; ++j) if (j != i) { int iRecNow = partonSystemsPtr->getOut(iSys, j); if (!event[iRecNow].isFinal()) continue; double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; } } } // If no success then look for matching (anti)colour anywhere in final state. if ( iRec == 0 || (!doInterleave && !event[iRec].isFinal()) ) { iRec = 0; for (int j = 0; j < event.size(); ++j) if (event[j].isFinal()) if ( (colSign > 0 && event[j].acol() == colTag) || (colSign < 0 && event[j].col() == colTag) ) { iRec = j; otherSystemRec = true; break; } // If no success then look for match to non-rescattered in initial state. if (iRec == 0 && allowInitial) { for (int iSysR = 0; iSysR < partonSystemsPtr->sizeSys(); ++iSysR) if (iSysR != iSys) { int j = partonSystemsPtr->getInA(iSysR); if (j > 0 && event[j].isRescatteredIncoming()) j = 0; if (j > 0 && ( (colSign > 0 && event[j].col() == colTag) || (colSign < 0 && event[j].acol() == colTag) ) ) { iRec = j; otherSystemRec = true; break; } j = partonSystemsPtr->getInB(iSysR); if (j > 0 && event[j].isRescatteredIncoming()) j = 0; if (j > 0 && ( (colSign > 0 && event[j].col() == colTag) || (colSign < 0 && event[j].acol() == colTag) ) ) { iRec = j; otherSystemRec = true; break; } } } } // Junctions (PS&ND dec 2010) // For types 1&2: all legs in final state // half-strength dipoles between all legs // For types 3&4, two legs in final state // full-strength dipole between final-state legs // For types 5&6, one leg in final state // no final-state dipole end if (hasJunction) { for (int iJun = 0; iJun < event.sizeJunction(); ++ iJun) { int kindJun = event.kindJunction(iJun); int iBeg = (kindJun-1)/2; for (int iLeg = iBeg; iLeg < 3; ++iLeg) { if (event.endColJunction( iJun, iLeg) == colTag) { // For types 5&6, no other leg to recoil against. Switch off if // no other particles at all, since radiation then handled by ISR. // Example: qq -> ~t* : no radiation off ~t* // Allow radiation + recoil if unconnected partners available // Example: qq -> ~t* -> tbar ~chi0 : allow radiation off tbar, // with ~chi0 as recoiler if (kindJun >= 5) { if (sizeOut == 1) return; else break; } // For junction types 3 & 4, span one full-strength dipole // (only look inside same decay system) else if (kindJun >= 3) { int iLegRec = 3-iLeg; int colTagRec = event.endColJunction( iJun, iLegRec); for (int j = 0; j < sizeOut; ++j) if (j != i) { int iRecNow = partonSystemsPtr->getOut(iSys, j); if (!event[iRecNow].isFinal()) continue; if ( (colSign > 0 && event[iRecNow].col() == colTagRec) || (colSign < 0 && event[iRecNow].acol() == colTagRec) ) { // Only accept if staying inside same system iRec = iRecNow; break; } } } // For junction types 1 & 2, span two half-strength dipoles // (only look inside same decay system) else { // Loop over two half-strength dipole connections for (int jLeg = 1; jLeg <= 2; jLeg++) { int iLegRec = (iLeg + jLeg) % 3; int colTagRec = event.endColJunction( iJun, iLegRec); for (int j = 0; j < sizeOut; ++j) if (j != i) { int iRecNow = partonSystemsPtr->getOut(iSys, j); if (!event[iRecNow].isFinal()) continue; if ( (colSign > 0 && event[iRecNow].col() == colTagRec) || (colSign < 0 && event[iRecNow].acol() == colTagRec) ) { // Store recoilers in temporary array iRecVec.push_back(iRecNow); // Set iRec != 0 for checks below iRec = iRecNow; } } } } // End if-then-else of junction kinds } // End if leg has right color tag } // End of loop over junction legs } // End loop over junctions } // End main junction if // If fail, then other end to nearest recoiler in same system final state, // by (p_i + p_j)^2 - (m_i + m_j)^2 = 2 (p_i p_j - m_i m_j). if (iRec == 0) { double ppMin = LARGEM2; for (int j = 0; j < sizeOut; ++j) if (j != i) { int iRecNow = partonSystemsPtr->getOut(iSys, j); if (!event[iRecNow].isFinal()) continue; double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; } } } // If fail, then other end to nearest recoiler in any system final state, // by (p_i + p_j)^2 - (m_i + m_j)^2 = 2 (p_i p_j - m_i m_j). if (iRec == 0) { double ppMin = LARGEM2; for (int iRecNow = 0; iRecNow < event.size(); ++iRecNow) if (iRecNow != iRad && event[iRecNow].isFinal()) { double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; otherSystemRec = true; ppMin = ppNow; } } } // PS dec 2010: make sure iRec is stored in iRecVec if (iRecVec.size() == 0 && iRec != 0) iRecVec.push_back(iRec); // Remove any zero recoilers from normalization int nRec = iRecVec.size(); for (unsigned int mRec = 0; mRec < iRecVec.size(); ++mRec) if (iRecVec[mRec] <= 0) nRec--; if (nRec >= 2) { isFlexible = true; flexFactor = 1.0/nRec; } // Check for failure to locate any recoiler if ( nRec <= 0 ) { infoPtr->errorMsg("Error in TimeShower::setupQCDdip: " "failed to locate any recoiling partner"); return; } // Store dipole colour end(s). for (unsigned int mRec = 0; mRec < iRecVec.size(); ++mRec) { iRec = iRecVec[mRec]; if (iRec <= 0) continue; // Max scale either by parton scale or by half dipole mass. double pTmax = event[iRad].scale(); if (limitPTmaxIn) { if (iSys == 0 || (iSys == 1 && doSecondHard)) pTmax *= pTmaxFudge; else if (sizeIn > 0) pTmax *= pTmaxFudgeMPI; } else pTmax = 0.5 * m( event[iRad], event[iRec]); int colType = (event[iRad].id() == 21) ? 2 * colSign : colSign; int isrType = (event[iRec].isFinal()) ? 0 : event[iRec].mother1(); // This line in case mother is a rescattered parton. while (isrType > 2 + beamOffset) isrType = event[isrType].mother1(); if (isrType > 2) isrType -= beamOffset; dipEnd.push_back( TimeDipoleEnd( iRad, iRec, pTmax, colType, 0, 0, 0, isrType, iSys, -1, -1, 0, isOctetOnium) ); // If hooked up with other system then find which. if (otherSystemRec) { int systemRec = partonSystemsPtr->getSystemOf(iRec, true); if (systemRec >= 0) dipEnd.back().systemRec = systemRec; dipEnd.back().MEtype = 0; } // PS dec 2010 // If non-unity (flexible) normalization, set normalization factor if (isFlexible) { dipEnd.back().isFlexible = true; dipEnd.back().flexFactor = flexFactor; } } } //-------------------------------------------------------------------------- // Setup a dipole end for a QED colour charge or a photon. // No failsafe choice of recoiler, so gradually widen search. void TimeShower::setupQEDdip( int iSys, int i, int chgType, int gamType, Event& event, bool limitPTmaxIn) { // Initial values. Find if allowed to hook up beams. int iRad = partonSystemsPtr->getOut(iSys, i); int idRad = event[iRad].id(); int iRec = 0; int sizeAllA = partonSystemsPtr->sizeAll(iSys); int sizeOut = partonSystemsPtr->sizeOut(iSys); int sizeAll = ( allowBeamRecoil ) ? sizeAllA : sizeOut; int sizeIn = sizeAll - sizeOut; int sizeInA = sizeAllA - sizeIn - sizeOut; int iOffset = i + sizeAllA - sizeOut; double ppMin = LARGEM2; bool hasRescattered = false; bool otherSystemRec = false; // Find nearest same- (opposide-) flavour recoiler in initial (final) // state of same system, excluding rescattered (in or out) partons. // Also find if system is involved in rescattering. // Note: (p_i + p_j)2 - (m_i + m_j)2 = 2 (p_i p_j - m_i m_j). for (int j = 0; j < sizeAll; ++j) if (j + sizeInA != iOffset) { int iRecNow = partonSystemsPtr->getAll(iSys, j + sizeInA); if ( (j < sizeIn && !event[iRecNow].isRescatteredIncoming()) || (j >= sizeIn && event[iRecNow].isFinal()) ) { if ( (j < sizeIn && event[iRecNow].id() == idRad) || (j >= sizeIn && event[iRecNow].id() == -idRad) ) { double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; } } } else hasRescattered = true; } // If rescattering then find nearest opposite-flavour recoiler // anywhere in final state. if (iRec == 0 && hasRescattered) { for (int iRecNow = 0; iRecNow < event.size(); ++iRecNow) if (event[iRecNow].id() == -idRad && event[iRecNow].isFinal()) { double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; otherSystemRec = true; } } } // Find nearest recoiler in same system, charge-squared-weighted, // including initial state, but excluding rescatterer. if (iRec == 0) for (int j = 0; j < sizeAll; ++j) if (j + sizeInA != iOffset) { int iRecNow = partonSystemsPtr->getAll(iSys, j + sizeInA); int chgTypeRecNow = event[iRecNow].chargeType(); if (chgTypeRecNow == 0) continue; if ( (j < sizeIn && !event[iRecNow].isRescatteredIncoming()) || (j >= sizeIn && event[iRecNow].isFinal()) ) { double ppNow = (event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m()) / pow2(chgTypeRecNow); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; } } } // If rescattering then find nearest recoiler in the final state, // charge-squared-weighted. if (iRec == 0 && hasRescattered) { for (int iRecNow = 0; iRecNow < event.size(); ++iRecNow) if (iRecNow != iRad && event[iRecNow].isFinal()) { int chgTypeRecNow = event[iRecNow].chargeType(); if (chgTypeRecNow != 0 && event[iRecNow].isFinal()) { double ppNow = (event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m()) / pow2(chgTypeRecNow); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; otherSystemRec = true; } } } } // Find any nearest recoiler in final state of same system. if (iRec == 0) for (int j = 0; j < sizeOut; ++j) if (j != i) { int iRecNow = partonSystemsPtr->getOut(iSys, j); double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; } } // Find any nearest recoiler in final state. if (iRec == 0) for (int iRecNow = 0; iRecNow < event.size(); ++iRecNow) if (iRecNow != iRad && event[iRecNow].isFinal()) { double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; otherSystemRec = true; } } // Fill charge-dipole or photon-dipole end. if (iRec > 0) { // Max scale either by parton scale or by half dipole mass. double pTmax = event[iRad].scale(); if (limitPTmaxIn) { if (iSys == 0 || (iSys == 1 && doSecondHard)) pTmax *= pTmaxFudge; else if (sizeIn > 0) pTmax *= pTmaxFudgeMPI; } else pTmax = 0.5 * m( event[iRad], event[iRec]); int isrType = (event[iRec].isFinal()) ? 0 : event[iRec].mother1(); // This line in case mother is a rescattered parton. while (isrType > 2 + beamOffset) isrType = event[isrType].mother1(); if (isrType > 2) isrType -= beamOffset; dipEnd.push_back( TimeDipoleEnd(iRad, iRec, pTmax, 0, chgType, gamType, 0, isrType, iSys, -1) ); // If hooked up with other system then find which. if (otherSystemRec) { int systemRec = partonSystemsPtr->getSystemOf(iRec); if (systemRec >= 0) dipEnd.back().systemRec = systemRec; dipEnd.back().MEtype = 0; } // Failure to find other end of dipole. } else { infoPtr->errorMsg("Error in TimeShower::setupQEDdip: " "failed to locate any recoiling partner"); } } //-------------------------------------------------------------------------- // Setup a dipole end for weak W or Z emission. void TimeShower::setupWeakdip( int iSys, int i, int weakType, Event& event, bool limitPTmaxIn) { // Initial values. Find if allowed to hook up beams. int iRad = partonSystemsPtr->getOut(iSys, i); int idRad = event[iRad].id(); int iRec = 0; int sizeAllA = partonSystemsPtr->sizeAll(iSys); int sizeOut = partonSystemsPtr->sizeOut(iSys); int sizeAll = ( allowBeamRecoil ) ? sizeAllA : sizeOut; int sizeIn = sizeAll - sizeOut; int sizeInA = sizeAllA - sizeIn - sizeOut; int iOffset = i + sizeAllA - sizeOut; double ppMin = LARGEM2; bool hasRescattered = false; bool otherSystemRec = false; // Find nearest same- (opposide-) flavour recoiler in initial (final) // state of same system, excluding rescattered (in or out) partons. // Also find if system is involved in rescattering. // Note: (p_i + p_j)2 - (m_i + m_j)2 = 2 (p_i p_j - m_i m_j). for (int j = 0; j < sizeAll; ++j) if (j + sizeInA != iOffset) { int iRecNow = partonSystemsPtr->getAll(iSys, j + sizeInA); if ( (j < sizeIn && !event[iRecNow].isRescatteredIncoming()) || (j >= sizeIn && event[iRecNow].isFinal()) ) { if ( (j < sizeIn && event[iRecNow].id() == idRad) || (j >= sizeIn && event[iRecNow].id() == -idRad) ) { double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; } } } else hasRescattered = true; } // If rescattering then find nearest opposite-flavour recoiler // anywhere in final state. if (iRec == 0 && hasRescattered) { for (int iRecNow = 0; iRecNow < event.size(); ++iRecNow) if (event[iRecNow].id() == -idRad && event[iRecNow].isFinal()) { double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; otherSystemRec = true; } } } // Need to change it to weak-charge instead of charge. // Find nearest recoiler in same system, weak-charge-squared-weighted, // including initial state, but excluding rescatterer. if (iRec == 0) for (int j = 0; j < sizeAll; ++j) if (j + sizeInA != iOffset) { int iRecNow = partonSystemsPtr->getAll(iSys, j + sizeInA); int weakTypeRecNow = 0; if(abs(event[iRecNow].id()) >= 20) weakTypeRecNow = 0; else if(weakType == 1) weakTypeRecNow = 1; else if(weakType == 2) weakTypeRecNow = coupSMPtr->af2(abs(event[iRecNow].id())) + coupSMPtr->vf2(abs(event[iRecNow].id())); if (weakTypeRecNow == 0) continue; if ( (j < sizeIn && !event[iRecNow].isRescatteredIncoming()) || (j >= sizeIn && event[iRecNow].isFinal()) ) { double ppNow = (event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m()) / pow2(weakTypeRecNow); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; } } } // If rescattering then find nearest recoiler in the final state, // weak-charge-squared-weighted. if (iRec == 0 && hasRescattered) { for (int iRecNow = 0; iRecNow < event.size(); ++iRecNow) if (iRecNow != iRad && event[iRecNow].isFinal()) { int weakTypeRecNow = 0; if(abs(event[iRecNow].id()) >= 20) weakTypeRecNow = 0; else if(weakType == 1) weakTypeRecNow = 1; else if(weakType == 2) weakTypeRecNow = coupSMPtr->af2(abs(event[iRecNow].id())) + coupSMPtr->vf2(abs(event[iRecNow].id())); if (weakTypeRecNow != 0 && event[iRecNow].isFinal()) { double ppNow = (event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m()) / pow2(weakTypeRecNow); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; otherSystemRec = true; } } } } // Find any nearest recoiler in final state of same system. if (iRec == 0) for (int j = 0; j < sizeOut; ++j) if (j != i) { int iRecNow = partonSystemsPtr->getOut(iSys, j); double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; } } // Find any nearest recoiler in final state. if (iRec == 0) for (int iRecNow = 0; iRecNow < event.size(); ++iRecNow) if (iRecNow != iRad && event[iRecNow].isFinal()) { double ppNow = event[iRecNow].p() * event[iRad].p() - event[iRecNow].m() * event[iRad].m(); if (ppNow < ppMin) { iRec = iRecNow; ppMin = ppNow; otherSystemRec = true; } } // Fill in weak dipole-end. if (iRec > 0) { // Max scale either by parton scale or by half dipole mass. double pTmax = event[iRad].scale(); if (limitPTmaxIn) { if (iSys == 0) pTmax *= pTmaxFudge; if (iSys > 0 && sizeIn > 0) pTmax *= pTmaxFudgeMPI; } else pTmax = 0.5 * m( event[iRad], event[iRec]); int isrType = (event[iRec].isFinal()) ? 0 : event[iRec].mother1(); // This line in case mother is a rescattered parton. while (isrType > 2 + beamOffset) isrType = event[isrType].mother1(); if (isrType > 2) isrType -= beamOffset; // No right-handed W emission. int weakPol = (rndmPtr->flat() > 0.5) ? -1 : 1; if (weakType == 1 && weakPol == 1) return; dipEnd.push_back( TimeDipoleEnd(iRad, iRec, pTmax, 0, 0, 0, weakType, isrType, iSys, -1, -1, weakPol) ); // If hooked up with other system then find which. if (otherSystemRec) { int systemRec = partonSystemsPtr->getSystemOf(iRec); if (systemRec >= 0) dipEnd.back().systemRec = systemRec; dipEnd.back().MEtype = 0; } // Failure to find other end of dipole. } else { infoPtr->errorMsg("Error in TimeShower::setupWeakdip: " "failed to locate any recoiling partner"); } } //-------------------------------------------------------------------------- // Setup a dipole end for a Hidden Valley colour charge. void TimeShower::setupHVdip( int iSys, int i, Event& event, bool limitPTmaxIn) { // Initial values. int iRad = partonSystemsPtr->getOut(iSys, i); int iRec = 0; int idRad = event[iRad].id(); int sizeOut = partonSystemsPtr->sizeOut(iSys); // Hidden Valley colour positive for positive id, and vice versa. // Find opposte HV colour in final state of same system. for (int j = 0; j < sizeOut; ++j) if (j != i) { int iRecNow = partonSystemsPtr->getOut(iSys, j); int idRec = event[iRecNow].id(); if ( (abs(idRec) > 4900000 && abs(idRec) < 4900017) && idRad * idRec < 0) { iRec = iRecNow; break; } } // Else find heaviest other final-state in same system. // (Intended for decays; should mainly be two-body so unique.) double mMax = -sqrt(LARGEM2); if (iRec == 0) for (int j = 0; j < sizeOut; ++j) if (j != i) { int iRecNow = partonSystemsPtr->getOut(iSys, j); if (event[iRecNow].m() > mMax) { iRec = iRecNow; mMax = event[iRecNow].m(); } } // Set up dipole end, or report failure. if (iRec > 0) { // Max scale either by parton scale or by half dipole mass. double pTmax = event[iRad].scale(); if (limitPTmaxIn) { if (iSys == 0 || (iSys == 1 && doSecondHard)) pTmax *= pTmaxFudge; } else pTmax = 0.5 * m( event[iRad], event[iRec]); int colvType = (event[iRad].id() > 0) ? 1 : -1; dipEnd.push_back( TimeDipoleEnd( iRad, iRec, pTmax, 0, 0, 0, 0, 0, iSys, -1, -1, 0, false, true, colvType) ); } else infoPtr->errorMsg("Error in TimeShower::setupHVdip: " "failed to locate any recoiling partner"); } //-------------------------------------------------------------------------- // Select next pT in downwards evolution of the existing dipoles. double TimeShower::pTnext( Event& event, double pTbegAll, double pTendAll, bool isFirstTrial) { // Begin loop over all possible radiating dipole ends. dipSel = 0; iDipSel = -1; double pT2sel = pTendAll * pTendAll; for (int iDip = 0; iDip < int(dipEnd.size()); ++iDip) { TimeDipoleEnd& dip = dipEnd[iDip]; // Check if global recoil should be used. useLocalRecoilNow = !(globalRecoil && dip.system == 0 && partonSystemsPtr->sizeOut(0) <= nMaxGlobalRecoil); // Do not use global recoil if the radiator line has already branched. if (globalRecoilMode == 1) { if (globalRecoil) useLocalRecoilNow = true; for (int iHard = 0; iHard < int(hardPartons.size()); ++iHard) if ( event[dip.iRadiator].isAncestor(hardPartons[iHard]) ) useLocalRecoilNow = false; // Check if global recoil should be used. if ( !globalRecoil || nGlobal >= nMaxGlobalBranch ) useLocalRecoilNow = true; // Switch off global recoil after first trial emission. } else if (globalRecoilMode == 2) { useLocalRecoilNow = !(globalRecoil && dip.system == 0 && nGlobal <= nMaxGlobalBranch); int nFinal = 0; for (int k = 0; k < int(event.size()); ++k) if ( event[k].isFinal() && event[k].colType() != 0) nFinal++; bool isFirst = (nHard == nFinal); // Switch off global recoil after first emission if ( globalRecoil && doInterleave && !isFirst ) useLocalRecoilNow = true; if ( globalRecoil && nProposed > 0 ) useLocalRecoilNow = true; // No global recoil for H-events. if ( nFinalBorn > 0 && nHard > nFinalBorn ) useLocalRecoilNow = true; } // Dipole properties; normal local recoil. dip.mRad = event[dip.iRadiator].m(); if (useLocalRecoilNow) { dip.mRec = event[dip.iRecoiler].m(); dip.mDip = m( event[dip.iRadiator], event[dip.iRecoiler] ); // Dipole properties, alternative global recoil. Squares. } else { Vec4 pSumGlobal; for (int i = 0; i < partonSystemsPtr->sizeOut( dip.system); ++i) { int ii = partonSystemsPtr->getOut( dip.system, i); if (ii != dip.iRadiator) pSumGlobal += event[ii].p(); } dip.mRec = pSumGlobal.mCalc(); dip.mDip = m( event[dip.iRadiator].p(), pSumGlobal); } dip.m2Rad = pow2(dip.mRad); dip.m2Rec = pow2(dip.mRec); dip.m2Dip = pow2(dip.mDip); // Find maximum evolution scale for dipole. dip.m2DipCorr = pow2(dip.mDip - dip.mRec) - dip.m2Rad; double pTbegDip; // Calculate the weak corrections needed for the different // ordering used for weak showers. double weakCorrection = 0.; if (dip.weakType == 1) weakCorrection = extraScaleTerm * pow2(mW); else if (dip.weakType == 2) weakCorrection = extraScaleTerm * pow2(mZ); // If first trial, allow weak showers to start at higher scale. if (isFirstTrial) pTbegAll = sqrt(pow2(pTbegAll) + weakCorrection); // If the scale got above the initial max scale for QCD/QED, // set it back to the initial max scale. // This can happen if first emission is a high pT W/Z particle, // because W/Z emissions are allowed to start at the scale pT2 + mW2(mZ2). if (dip.weakType == 0) { if (pTbegAll > pTfirstTrial) pTbegDip = min( pTfirstTrial, dip.pTmax ); else pTbegDip = min( pTbegAll, dip.pTmax ); } // Special scales for weak (for different competition). else { pTbegDip = min(sqrt(pow2(pTbegAll) - weakCorrection), dip.pTmax); pT2sel -= weakCorrection; } double pT2begDip = min( pow2(pTbegDip), 0.25 * dip.m2DipCorr); // For global recoil, always set the starting scale for first emission. bool isFirstWimpy = !useLocalRecoilNow && (pTmaxMatch == 1) && (nProposed == 0 || isFirstTrial); double muQ = (infoPtr->scalup() > 0.) ? infoPtr->scalup() : infoPtr->QFac(); if (isFirstWimpy && !limitMUQ) pT2begDip = pow2(muQ); else if (isFirstWimpy && limitMUQ) { // Find mass of colour dipole. double mS = event[dip.iRecoiler].m(); double mD = m( event[dip.iRadiator], event[dip.iRecoiler] ); double m2DC = pow2(mD - mS) - pow2(dip.mRad); // Choose minimal scale. pT2begDip = min( pow2(muQ), min(pow2(pTbegDip), 0.25 * m2DC) ); } // Do not try splitting if the corrected dipole mass is negative. dip.pT2 = 0.; if (dip.m2DipCorr < 0.) { infoPtr->errorMsg("Warning in TimeShower::pTnext: " "negative dipole mass."); continue; } // Do QCD, QED, weak or HV evolution if it makes sense. if (pT2begDip > pT2sel) { if (dip.colType != 0) pT2nextQCD(pT2begDip, pT2sel, dip, event); else if (dip.chgType != 0 || dip.gamType != 0) pT2nextQED(pT2begDip, pT2sel, dip, event); else if (dip.weakType != 0) pT2nextWeak(pT2begDip, pT2sel, dip, event); else if (dip.colvType != 0) pT2nextHV(pT2begDip, pT2sel, dip, event); // Update if found larger pT than current maximum. if (dip.weakType == 0 && dip.pT2 > pT2sel) { pT2sel = dip.pT2; dipSel = &dip; iDipSel = iDip; } // Special update case for weak emissions: need to add the mass // to the evolution variable. The middle cut is needed, // to tell if the evolution of the shower was stopped or not. // (Normally the stop sets pT2 to zero, but for massive emissions // this will still give a pT2sel.) if (dip.weakType != 0 && dip.pT2 > pT2weakCut / 2. && dip.pT2 + weakCorrection > pT2sel) { pT2sel = dip.pT2; dipSel = &dip; iDipSel = iDip; } } // Cleanup for weak corrections. if (dip.weakType != 0) { pT2sel += weakCorrection; if (isFirstTrial) pTbegAll = sqrt(pow2(pTbegAll) - weakCorrection); } } // Update the number of proposed timelike emissions. if (dipSel != 0) ++nProposed; // Return nonvanishing value if found pT bigger than already found. return (dipSel == 0) ? 0. : sqrt(pT2sel); } //-------------------------------------------------------------------------- // Evolve a QCD dipole end. void TimeShower::pT2nextQCD(double pT2begDip, double pT2sel, TimeDipoleEnd& dip, Event& event) { // Lower cut for evolution. Return if no evolution range. double pT2endDip = max( pT2sel, pT2colCut ); if (pT2begDip < pT2endDip) return; // Upper estimate for matrix element weighting and colour factor. // Special cases for triplet recoiling against gluino and octet onia. // Note that g -> g g and g -> q qbar are split on two sides. int colTypeAbs = abs(dip.colType); double wtPSglue = 2.; double colFac = (colTypeAbs == 1) ? 4./3. : 3./2.; if (dip.MEgluinoRec) colFac = 3.; if (dip.isOctetOnium) colFac *= 0.5 * octetOniumColFac; // PS dec 2010. Include possibility for flexible normalization, // e.g., for dipoles stretched to junctions or to switch off radiation. if (dip.isFlexible) colFac *= dip.flexFactor; double wtPSqqbar = (colTypeAbs == 2) ? 0.25 * nGluonToQuark : 0.; // Variables used inside evolution loop. (Mainly dummy start values.) dip.pT2 = pT2begDip; int nFlavour = 3; double zMinAbs = 0.5; double pT2min = pT2endDip; double b0 = 4.5; double Lambda2 = Lambda3flav2; double emitCoefGlue = 0.; double emitCoefQqbar = 0.; double emitCoefTot = 0.; double wt = 0.; bool mustFindRange = true; // Begin evolution loop towards smaller pT values. do { // Initialize evolution coefficients at the beginning and // reinitialize when crossing c and b flavour thresholds. if (mustFindRange) { // Determine overestimated z range; switch at c and b masses. if (dip.pT2 > m2b) { nFlavour = 5; pT2min = max( m2b, pT2endDip); b0 = 23./6.; Lambda2 = Lambda5flav2; } else if (dip.pT2 > m2c) { nFlavour = 4; pT2min = max( m2c, pT2endDip); b0 = 25./6.; Lambda2 = Lambda4flav2; } else { nFlavour = 3; pT2min = pT2endDip; b0 = 27./6.; Lambda2 = Lambda3flav2; } // A change of renormalization scale expressed by a change of Lambda. Lambda2 /= renormMultFac; zMinAbs = 0.5 - sqrtpos( 0.25 - pT2min / dip.m2DipCorr ); if (zMinAbs < SIMPLIFYROOT) zMinAbs = pT2min / dip.m2DipCorr; // Find emission coefficients for X -> X g and g -> q qbar. emitCoefGlue = wtPSglue * colFac * log(1. / zMinAbs - 1.); emitCoefTot = emitCoefGlue; if (colTypeAbs == 2 && event[dip.iRadiator].id() == 21) { emitCoefQqbar = wtPSqqbar * (1. - 2. * zMinAbs); emitCoefTot += emitCoefQqbar; } // Initialization done for current range. mustFindRange = false; } // Pick pT2 (in overestimated z range) for fixed alpha_strong. if (alphaSorder == 0) { dip.pT2 = dip.pT2 * pow( rndmPtr->flat(), 1. / (alphaS2pi * emitCoefTot) ); // Ditto for first-order alpha_strong. } else if (alphaSorder == 1) { dip.pT2 = Lambda2 * pow( dip.pT2 / Lambda2, pow( rndmPtr->flat(), b0 / emitCoefTot) ); // For second order reject by second term in alpha_strong expression. } else { do dip.pT2 = Lambda2 * pow( dip.pT2 / Lambda2, pow( rndmPtr->flat(), b0 / emitCoefTot) ); while (alphaS.alphaS2OrdCorr(renormMultFac * dip.pT2) < rndmPtr->flat() && dip.pT2 > pT2min); } wt = 0.; // If crossed c or b thresholds: continue evolution from threshold. if (nFlavour == 5 && dip.pT2 < m2b) { mustFindRange = true; dip.pT2 = m2b; } else if ( nFlavour == 4 && dip.pT2 < m2c) { mustFindRange = true; dip.pT2 = m2c; // Abort evolution if below cutoff scale, or below another branching. } else { if ( dip.pT2 < pT2endDip) { dip.pT2 = 0.; return; } // Pick kind of branching: X -> X g or g -> q qbar. dip.flavour = 21; dip.mFlavour = 0.; if (colTypeAbs == 2 && emitCoefQqbar > rndmPtr->flat() * emitCoefTot) dip.flavour = 0; // Pick z: either dz/(1-z) or flat dz. if (dip.flavour == 21) { dip.z = 1. - zMinAbs * pow( 1. / zMinAbs - 1., rndmPtr->flat() ); } else { dip.z = zMinAbs + (1. - 2. * zMinAbs) * rndmPtr->flat(); } // Do not accept branching if outside allowed z range. double zMin = 0.5 - sqrtpos( 0.25 - dip.pT2 / dip.m2DipCorr ); if (zMin < SIMPLIFYROOT) zMin = dip.pT2 / dip.m2DipCorr; dip.m2 = dip.m2Rad + dip.pT2 / (dip.z * (1. - dip.z)); if (dip.z > zMin && dip.z < 1. - zMin && dip.m2 * dip.m2Dip < dip.z * (1. - dip.z) * pow2(dip.m2Dip + dip.m2 - dip.m2Rec) ) { // Flavour choice for g -> q qbar. if (dip.flavour == 0) { dip.flavour = min(5, 1 + int(nGluonToQuark * rndmPtr->flat())); dip.mFlavour = particleDataPtr->m0(dip.flavour); } // No z weight, except threshold, if to do ME corrections later on. if (dip.MEtype > 0) { wt = 1.; if (dip.flavour < 10 && dip.m2 < THRESHM2 * pow2(dip.mFlavour)) wt = 0.; // z weight for X -> X g. } else if (dip.flavour == 21 && (colTypeAbs == 1 || colTypeAbs == 3) ) { wt = (1. + pow2(dip.z)) / wtPSglue; } else if (dip.flavour == 21) { wt = (1. + pow3(dip.z)) / wtPSglue; // z weight for g -> q qbar. } else { double beta = sqrtpos( 1. - 4. * pow2(dip.mFlavour) / dip.m2 ); wt = beta * ( pow2(dip.z) + pow2(1. - dip.z) ); } // Suppression factors for dipole to beam remnant. if (dip.isrType != 0 && useLocalRecoilNow) { BeamParticle& beam = (dip.isrType == 1) ? *beamAPtr : *beamBPtr; int iSysRec = dip.systemRec; double xOld = beam[iSysRec].x(); double xNew = xOld * (1. + (dip.m2 - dip.m2Rad) / (dip.m2Dip - dip.m2Rad)); double xMaxAbs = beam.xMax(iSysRec); if (xMaxAbs < 0.) { infoPtr->errorMsg("Warning in TimeShower::pT2nextQCD: " "xMaxAbs negative"); return; } // Firstly reduce by PDF ratio. if (xNew > xMaxAbs) wt = 0.; else { int idRec = event[dip.iRecoiler].id(); double pdfOld = max ( TINYPDF, beam.xfISR( iSysRec, idRec, xOld, factorMultFac * dip.pT2) ); double pdfNew = beam.xfISR( iSysRec, idRec, xNew, factorMultFac * dip.pT2); wt *= min( 1., pdfNew / pdfOld); } // Secondly optionally reduce by 4 pT2_hard / (4 pT2_hard + m2). if (dampenBeamRecoil) { double pTpT = sqrt(event[dip.iRadiator].pT2() * dip.pT2); wt *= pTpT / (pTpT + dip.m2); } } // Optional dampening of large pT values in hard system. if (dopTdamp && dip.system == 0 && dip.MEtype == 0) wt *= pT2damp / (dip.pT2 + pT2damp); } } // Iterate until acceptable pT (or have fallen below pTmin). } while (wt < rndmPtr->flat()); } //-------------------------------------------------------------------------- // Evolve a QED dipole end, either charged or photon. void TimeShower::pT2nextQED(double pT2begDip, double pT2sel, TimeDipoleEnd& dip, Event& event) { // Lower cut for evolution. Return if no evolution range. double pT2chgCut = (dip.chgType != 0 && abs(dip.chgType) != 3) ? pT2chgQCut : pT2chgLCut; double pT2endDip = max( pT2sel, pT2chgCut ); if (pT2begDip < pT2endDip) return; // Emission of photon or photon branching. bool hasCharge = (dip.chgType != 0); // Default values. double wtPSgam = 0.; double chg2Sum = 0.; double chg2SumL = 0.; double chg2SumQ = 0.; double zMinAbs = 0.; double emitCoefTot = 0.; // alpha_em at maximum scale provides upper estimate. double alphaEMmax = alphaEM.alphaEM(renormMultFac * pT2begDip); double alphaEM2pi = alphaEMmax / (2. * M_PI); // Emission: upper estimate for matrix element weighting; charge factor. if (hasCharge) { wtPSgam = 2.; double chg2 = pow2(dip.chgType / 3.); // Determine overestimated z range. Find evolution coefficient. zMinAbs = 0.5 - sqrtpos( 0.25 - pT2endDip / dip.m2DipCorr ); if (zMinAbs < SIMPLIFYROOT) zMinAbs = pT2endDip / dip.m2DipCorr; emitCoefTot = alphaEM2pi * chg2 * wtPSgam * log(1. / zMinAbs - 1.); // Branching: sum of squared charge factors for lepton and quark daughters. } else { chg2SumL = max(0, min(3, nGammaToLepton)); if (nGammaToQuark > 4) chg2SumQ = 11. / 9.; else if (nGammaToQuark > 3) chg2SumQ = 10. / 9.; else if (nGammaToQuark > 2) chg2SumQ = 6. / 9.; else if (nGammaToQuark > 1) chg2SumQ = 5. / 9.; else if (nGammaToQuark > 0) chg2SumQ = 1. / 9.; // Total sum of squared charge factors. Find evolution coefficient. chg2Sum = chg2SumL + 3. * chg2SumQ; emitCoefTot = alphaEM2pi * chg2Sum; } // Variables used inside evolution loop. dip.pT2 = pT2begDip; double wt; // Begin evolution loop towards smaller pT values. do { // Pick pT2 (in overestimated z range). dip.pT2 = dip.pT2 * pow(rndmPtr->flat(), 1. / emitCoefTot); wt = 0.; // Abort evolution if below cutoff scale, or below another branching. if ( dip.pT2 < pT2endDip) { dip.pT2 = 0.; return; } // Pick z according to dz/(1-z) or flat. if (hasCharge) dip.z = 1. - zMinAbs * pow( 1. / zMinAbs - 1., rndmPtr->flat() ); else dip.z = rndmPtr->flat(); // Do not accept branching if outside allowed z range. double zMin = 0.5 - sqrtpos( 0.25 - dip.pT2 / dip.m2DipCorr ); if (zMin < SIMPLIFYROOT) zMin = dip.pT2 / dip.m2DipCorr; if (dip.z <= zMin || dip.z >= 1. - zMin) continue; dip.m2 = dip.m2Rad + dip.pT2 / (dip.z * (1. - dip.z)); if (dip.m2 * dip.m2Dip < dip.z * (1. - dip.z) * pow2(dip.m2Dip + dip.m2 - dip.m2Rec) // For gamma -> f fbar also impose maximum mass. && (hasCharge || dip.m2 < m2MaxGamma) ) { // Photon emission: unique flavour choice. if (hasCharge) { dip.flavour = 22; dip.mFlavour = 0.; // Photon branching: either lepton or quark flavour choice. } else { if (rndmPtr->flat() * chg2Sum < chg2SumL) dip.flavour = 9 + 2 * min(3, 1 + int(chg2SumL * rndmPtr->flat())); else { double rndmQ = 9. * chg2SumQ * rndmPtr->flat(); if (rndmQ < 1.) dip.flavour = 1; else if (rndmQ < 5.) dip.flavour = 2; else if (rndmQ < 6.) dip.flavour = 3; else if (rndmQ < 10.) dip.flavour = 4; else dip.flavour = 5; } dip.mFlavour = particleDataPtr->m0(dip.flavour); } // No z weight, except threshold, if to do ME corrections later on. if (dip.MEtype > 0) { wt = 1.; if (dip.flavour < 20 && dip.m2 < THRESHM2 * pow2(dip.mFlavour)) wt = 0.; // z weight for X -> X gamma. } else if (hasCharge) { wt = (1. + pow2(dip.z)) / wtPSgam; // z weight for gamma -> f fbar. } else { double beta = sqrtpos( 1. - 4. * pow2(dip.mFlavour) / dip.m2 ); wt = beta * ( pow2(dip.z) + pow2(1. - dip.z) ); } // Correct to current value of alpha_EM. double alphaEMnow = alphaEM.alphaEM(renormMultFac * dip.pT2); wt *= (alphaEMnow / alphaEMmax); // Suppression factors for dipole to beam remnant. if (dip.isrType != 0 && useLocalRecoilNow) { BeamParticle& beam = (dip.isrType == 1) ? *beamAPtr : *beamBPtr; int iSys = dip.system; double xOld = beam[iSys].x(); double xNew = xOld * (1. + (dip.m2 - dip.m2Rad) / (dip.m2Dip - dip.m2Rad)); double xMaxAbs = beam.xMax(iSys); if (xMaxAbs < 0.) { infoPtr->errorMsg("Warning in TimeShower::pT2nextQED: " "xMaxAbs negative"); return; } // Firstly reduce by PDF ratio. if (xNew > xMaxAbs) wt = 0.; else { int idRec = event[dip.iRecoiler].id(); double pdfOld = max ( TINYPDF, beam.xfISR( iSys, idRec, xOld, factorMultFac * dip.pT2) ); double pdfNew = beam.xfISR( iSys, idRec, xNew, factorMultFac * dip.pT2); wt *= min( 1., pdfNew / pdfOld); } // Secondly optionally reduce by 4 pT2_hard / (4 pT2_hard + m2). if (dampenBeamRecoil) { double pT24 = 4. * event[dip.iRadiator].pT2(); wt *= pT24 / (pT24 + dip.m2); } } // Optional dampening of large pT values in hard system. if (dopTdamp && dip.system == 0 && dip.MEtype == 0) wt *= pT2damp / (dip.pT2 + pT2damp); } // Iterate until acceptable pT (or have fallen below pTmin). } while (wt < rndmPtr->flat()); } //-------------------------------------------------------------------------- // Evolve a weak-emission dipole end. void TimeShower::pT2nextWeak(double pT2begDip, double pT2sel, TimeDipoleEnd& dip, Event& event) { // Lower cut for evolution. Return if no evolution range. double pT2endDip = max( pT2sel, pT2weakCut ); if (pT2begDip < pT2endDip) return; // Default values. double wtPSgam = 0.; double zMinAbs = 0.; double emitCoefTot = 0.; // alpha_em at maximum scale provides upper estimate. double alphaEMmax = alphaEM.alphaEM(renormMultFac * pT2begDip); double alphaEM2pi = alphaEMmax / (2. * M_PI); // Emission: upper estimate for matrix element weighting; charge factor. wtPSgam = 8.; // Determine overestimated z range. Find evolution coefficient. zMinAbs = 0.5 - sqrtpos( 0.25 - pT2endDip / dip.m2DipCorr ); if (zMinAbs < SIMPLIFYROOT) zMinAbs = pT2endDip / dip.m2DipCorr; // Determine weak coupling. double weakCoupling = 0.; // W-radiation, with additional factor of two, from only having // left-handed fermions. if(dip.weakType == 1) weakCoupling = 2. * alphaEM2pi / (4. * coupSMPtr->sin2thetaW()); // Z-radiation, split between left and right fermions. else if (dip.weakType == 2 && dip.weakPol == -1) weakCoupling = alphaEM2pi * thetaWRat * pow2(2. * coupSMPtr->lf( event[dip.iRadiator].idAbs() )); else weakCoupling = alphaEM2pi * thetaWRat * pow2(2. * coupSMPtr->rf( event[dip.iRadiator].idAbs() )); // Variables used inside evolution loop. emitCoefTot = weakEnhancement * weakCoupling * wtPSgam * log(1. / zMinAbs - 1.); dip.pT2 = pT2begDip; double wt; // Begin evolution loop towards smaller pT values. do { // Pick pT2 (in overestimated z range). dip.pT2 = dip.pT2 * pow(rndmPtr->flat(), 1. / emitCoefTot); wt = 0.; // Abort evolution if below cutoff scale, or below another branching. if ( dip.pT2 < pT2endDip) {dip.pT2 = 0.; return; } // Pick z according to dz/(1-z) or flat. dip.z = 1. - zMinAbs * pow( 1. / zMinAbs - 1., rndmPtr->flat() ); // Do not accept branching if outside allowed z range. double zMin = 0.5 - sqrtpos( 0.25 - dip.pT2 / dip.m2DipCorr ); if (zMin < SIMPLIFYROOT) zMin = dip.pT2 / dip.m2DipCorr; dip.m2 = dip.m2Rad + dip.pT2 / (dip.z * (1. - dip.z)); if (dip.z > zMin && dip.z < 1. - zMin && dip.m2 * dip.m2Dip < dip.z * (1. - dip.z) * pow2(dip.m2Dip + dip.m2 - dip.m2Rec) ) { // Check whether emission of W+ or W-, or else Z0. if (dip.weakType == 1) { dip.flavour = (event[dip.iRadiator].id() > 0) ? 24 : -24; if (event[dip.iRadiator].idAbs() % 2 == 1) dip.flavour = -dip.flavour; } else if (dip.weakType == 2) dip.flavour = 23; // Set mass of emitted particle, with Breit-Wigner distribution. dip.mFlavour = particleDataPtr->mSel( dip.flavour); // No z weight, except threshold, if to do ME corrections later on. // Here no pure shower mode exists, always needs ME corrections. if (dip.MEtype > 0) wt = 1.; // Correct to current value of alpha_EM. double alphaEMnow = alphaEM.alphaEM(renormMultFac * dip.pT2); wt *= (alphaEMnow / alphaEMmax); // Suppression factors for dipole to beam remnant. if (dip.isrType != 0 && useLocalRecoilNow) { BeamParticle& beam = (dip.isrType == 1) ? *beamAPtr : *beamBPtr; int iSys = dip.system; double xOld = beam[iSys].x(); double xNew = xOld * (1. + (dip.m2 - dip.m2Rad) / (dip.m2Dip - dip.m2Rad)); double xMaxAbs = beam.xMax(iSys); if (xMaxAbs < 0.) { infoPtr->errorMsg("Warning in TimeShower::pT2nextQED: " "xMaxAbs negative"); return; } // Firstly reduce by PDF ratio. if (xNew > xMaxAbs) wt = 0.; else { int idRec = event[dip.iRecoiler].id(); double pdfOld = max ( TINYPDF, beam.xfISR( iSys, idRec, xOld, factorMultFac * dip.pT2) ); double pdfNew = beam.xfISR( iSys, idRec, xNew, factorMultFac * dip.pT2); wt *= min( 1., pdfNew / pdfOld); } // Secondly optionally reduce by 4 pT2_hard / (4 pT2_hard + m2). if (dampenBeamRecoil) { double pT24 = 4. * event[dip.iRadiator].pT2(); wt *= pT24 / (pT24 + dip.m2); } } } // Optional dampening of large pT values in hard system. if (dopTdamp && dip.system == 0) wt *= pT2damp / (dip.pT2 + pT2damp); // Extra dampening of low pT values. if (dopTdampMass) wt *= (dip.pT2 + 0.25 * pow2(dip.mFlavour)) / (dip.pT2 + 1. * pow2(dip.mFlavour)); // Iterate until acceptable pT (or have fallen below pTmin). } while (wt < rndmPtr->flat()); } //-------------------------------------------------------------------------- // Evolve a Hidden Valley dipole end. void TimeShower::pT2nextHV(double pT2begDip, double pT2sel, TimeDipoleEnd& dip, Event& ) { // Lower cut for evolution. Return if no evolution range. double pT2endDip = max( pT2sel, pT2hvCut ); if (pT2begDip < pT2endDip) return; // C_F * alpha_HV/2 pi. int colvTypeAbs = abs(dip.colvType); double colvFac = (colvTypeAbs == 1) ? CFHV : 0.5 * nCHV; double alphaHV2pi = colvFac * (alphaHVfix / (2. * M_PI)); // Determine overestimated z range. Find evolution coefficient. double zMinAbs = 0.5 - sqrtpos( 0.25 - pT2endDip / dip.m2DipCorr ); if (zMinAbs < SIMPLIFYROOT) zMinAbs = pT2endDip / dip.m2DipCorr; double emitCoefTot = alphaHV2pi * 2. * log(1. / zMinAbs - 1.); // Variables used inside evolution loop. dip.pT2 = pT2begDip; double wt; // Begin evolution loop towards smaller pT values. do { // Pick pT2 (in overestimated z range). dip.pT2 = dip.pT2 * pow(rndmPtr->flat(), 1. / emitCoefTot); wt = 0.; // Abort evolution if below cutoff scale, or below another branching. if ( dip.pT2 < pT2endDip) { dip.pT2 = 0.; return; } // Pick z according to dz/(1-z). dip.z = 1. - zMinAbs * pow( 1. / zMinAbs - 1., rndmPtr->flat() ); // Do not accept branching if outside allowed z range. double zMin = 0.5 - sqrtpos( 0.25 - dip.pT2 / dip.m2DipCorr ); if (zMin < SIMPLIFYROOT) zMin = dip.pT2 / dip.m2DipCorr; dip.m2 = dip.m2Rad + dip.pT2 / (dip.z * (1. - dip.z)); if (dip.z > zMin && dip.z < 1. - zMin && dip.m2 * dip.m2Dip < dip.z * (1. - dip.z) * pow2(dip.m2Dip + dip.m2 - dip.m2Rec) ) { // HV gamma or gluon emission: unique flavour choice. dip.flavour = idHV; dip.mFlavour = mHV; // No z weight, except threshold, if to do ME corrections later on. if (dip.MEtype > 0) wt = 1.; // z weight for X -> X g_HV. else if (colvTypeAbs == 1) wt = (1. + pow2(dip.z)) / 2.; else wt = (1. + pow3(dip.z)) / 2.; } // Optional dampening of large pT values in hard system. if (dopTdamp && dip.system == 0 && dip.MEtype == 0) wt *= pT2damp / (dip.pT2 + pT2damp); // Iterate until acceptable pT (or have fallen below pTmin). } while (wt < rndmPtr->flat()); } //-------------------------------------------------------------------------- // ME corrections and kinematics that may give failure. // Notation: radBef, recBef = radiator, recoiler before emission, // rad, rec, emt = radiator, recoiler, emitted efter emission. // (rad, emt distinguished by colour flow for g -> q qbar.) bool TimeShower::branch( Event& event, bool isInterleaved) { // Check if global recoil should be used. useLocalRecoilNow = !(globalRecoil && dipSel->system == 0 && partonSystemsPtr->sizeOut(0) <= nMaxGlobalRecoil); // Do not use global recoil if the radiator line has already branched. if (globalRecoilMode == 1) { if ( globalRecoil ) useLocalRecoilNow = true; for (int iHard = 0; iHard < int(hardPartons.size()); ++iHard) if ( event[dipSel->iRadiator].isAncestor(hardPartons[iHard]) ) useLocalRecoilNow = false; // Check if global recoil should be used. if ( !globalRecoil || nGlobal >= nMaxGlobalBranch ) useLocalRecoilNow = true; // Switch off global recoil after first trial emission } else if (globalRecoilMode == 2) { useLocalRecoilNow = !(globalRecoil && dipSel->system == 0 && nGlobal <= nMaxGlobalBranch); int nFinal = 0; for (int i = 0; i < int(event.size()); ++i) if ( event[i].isFinal() && event[i].colType() != 0) nFinal++; bool isFirst = (nHard == nFinal); if ( globalRecoil && doInterleave && !isFirst ) useLocalRecoilNow = true; if ( globalRecoil && nProposed > 1 ) useLocalRecoilNow = true; // No global recoil for H-events. if ( nFinalBorn > 0 && nHard > nFinalBorn ) useLocalRecoilNow = true; } // Check if the first emission should be studied for removal. bool canMergeFirst = (mergingHooksPtr != 0) ? mergingHooksPtr->canVetoEmission() : false; // Find initial radiator and recoiler particles in dipole branching. int iRadBef = dipSel->iRadiator; int iRecBef = dipSel->iRecoiler; Particle& radBef = event[iRadBef]; Particle& recBef = event[iRecBef]; // Find their momenta, with special sum for global recoil. Vec4 pRadBef = event[iRadBef].p(); Vec4 pRecBef; vector iGRecBef, iGRec; if (useLocalRecoilNow) pRecBef = event[iRecBef].p(); else { for (int i = 0; i < partonSystemsPtr->sizeOut( dipSel->system); ++i) { int iG = partonSystemsPtr->getOut( dipSel->system, i); if (iG != dipSel->iRadiator) { iGRecBef.push_back(iG); pRecBef += event[iG].p(); } } } // Default flavours and colour tags for new particles in dipole branching. int idRad = radBef.id(); int idEmt = dipSel->flavour; int colRad = radBef.col(); int acolRad = radBef.acol(); int colEmt = 0; int acolEmt = 0; iSysSel = dipSel->system; int iSysSelRec = dipSel->systemRec; // Default OK for photon, photon_HV or gluon_HV emission. if (dipSel->flavour == 22 || dipSel->flavour == idHV) { // New colour tag required for gluon emission. } else if (dipSel->flavour == 21 && dipSel->colType > 0) { colEmt = colRad; colRad = event.nextColTag(); acolEmt = colRad; } else if (dipSel->flavour == 21) { acolEmt = acolRad; acolRad = event.nextColTag(); colEmt = acolRad; // New flavours for g -> q qbar; split colours. } else if (dipSel->colType > 0) { idEmt = dipSel->flavour ; idRad = -idEmt; colEmt = colRad; colRad = 0; } else if (dipSel->colType < 0) { idEmt = -dipSel->flavour ; idRad = -idEmt; acolEmt = acolRad; acolRad = 0; // New flavours for gamma -> f fbar, and maybe also colours. } else if (dipSel->gamType == 1 && rndmPtr->flat() > 0.5) { idEmt = -dipSel->flavour ; idRad = -idEmt; if (idRad < 10) colRad = event.nextColTag(); acolEmt = colRad; } else if (dipSel->gamType == 1) { idEmt = dipSel->flavour ; idRad = -idEmt; if (idEmt < 10) colEmt = event.nextColTag(); acolRad = colEmt; } // Change fermion flavour by W emissions. int idRadSv = idRad; if (abs(idEmt) == 24) { if (rndmPtr->flat() > coupSMPtr->V2CKMsum(idRad)) return false; idRad = coupSMPtr->V2CKMpick(idRad); } // Construct kinematics in dipole rest frame: // begin simple (like g -> g g). double pTorig = sqrt( dipSel->pT2); double eRadPlusEmt = 0.5 * (dipSel->m2Dip + dipSel->m2 - dipSel->m2Rec) / dipSel->mDip; double e2RadPlusEmt = pow2(eRadPlusEmt); double pzRadPlusEmt = 0.5 * sqrtpos( pow2(dipSel->m2Dip - dipSel->m2 - dipSel->m2Rec) - 4. * dipSel->m2 * dipSel->m2Rec ) / dipSel->mDip; double pT2corr = dipSel->m2 * (e2RadPlusEmt * dipSel->z * (1. - dipSel->z) - 0.25 * dipSel->m2) / pow2(pzRadPlusEmt); double pTcorr = sqrtpos( pT2corr ); double pzRad = (e2RadPlusEmt * dipSel->z - 0.5 * dipSel->m2) / pzRadPlusEmt; double pzEmt = (e2RadPlusEmt * (1. - dipSel->z) - 0.5 * dipSel->m2) / pzRadPlusEmt; // Radiator flavour changed if W emission, so find new mass. double mRad = (idRad == idRadSv) ? dipSel->mRad : particleDataPtr->m0(idRad); double m2Rad = pow2(mRad); double mEmt = 0.; // Kinematics reduction for f -> f W/Z when m_f > 0 (and m_W/Z > 0) // or q -> q gamma_v when m_q > 0 and m_gamma_v > 0. if ( dipSel->weakType != 0 || (abs(dipSel->colvType) == 1 && dipSel->mFlavour > 0.) ) { mEmt = dipSel->mFlavour; if (pow2(mRad + mEmt) > dipSel->m2) return false; double m2Emt = pow2(mEmt); double lambda = sqrtpos( pow2(dipSel->m2 - m2Rad - m2Emt) - 4. * m2Rad * m2Emt ); kRad = 0.5 * (dipSel->m2 - lambda + m2Emt - m2Rad) / dipSel->m2; kEmt = 0.5 * (dipSel->m2 - lambda + m2Rad - m2Emt) / dipSel->m2; pTorig *= 1. - kRad - kEmt; pTcorr *= 1. - kRad - kEmt; double pzMove = kRad * pzRad - kEmt * pzEmt; pzRad -= pzMove; pzEmt += pzMove; // Kinematics reduction for q -> q g/gamma/g_HV when m_q > 0. } else if (abs(dipSel->colType) == 1 || dipSel->chgType != 0 || abs(dipSel->colvType) == 1) { pTorig *= 1. - dipSel->m2Rad / dipSel->m2; pTcorr *= 1. - dipSel->m2Rad / dipSel->m2; pzRad += pzEmt * dipSel->m2Rad / dipSel->m2; pzEmt *= 1. - dipSel->m2Rad / dipSel->m2; // Kinematics reduction for g -> q qbar or gamma -> f fbar when m_f > 0; } else if (abs(dipSel->flavour) < 20) { mEmt = dipSel->mFlavour; mRad = mEmt; double beta = sqrtpos( 1. - 4. * pow2(mEmt) / dipSel->m2 ); pTorig *= beta; pTcorr *= beta; pzRad = 0.5 * ( (1. + beta) * pzRad + (1. - beta) * pzEmt ); pzEmt = pzRadPlusEmt - pzRad; } // Reject g emission where mass effects have reduced pT below cutoff. if (idEmt == 21 && pTorig < pTcolCut) return false; // Find rest frame and angles of original dipole. RotBstMatrix M; M.fromCMframe(pRadBef, pRecBef); // Evaluate coefficient of azimuthal asymmetry from gluon polarization. findAsymPol( event, dipSel); // Begin construction of new dipole kinematics: pick azimuthal angle. Vec4 pRad, pEmt, pRec; double wtPhi = 1.; do { double phi = 2. * M_PI * rndmPtr->flat(); // Define kinematics of branching in dipole rest frame. pRad = Vec4( pTcorr * cos(phi), pTcorr * sin(phi), pzRad, sqrt( pow2(pTcorr) + pow2(pzRad) + pow2(mRad) ) ); pEmt = Vec4( -pRad.px(), -pRad.py(), pzEmt, sqrt( pow2(pTcorr) + pow2(pzEmt) + pow2(mEmt) ) ); pRec = Vec4( 0., 0., -pzRadPlusEmt, sqrt( pow2(pzRadPlusEmt) + dipSel->m2Rec ) ); // Rotate and boost dipole products to the event frame. pRad.rotbst(M); pEmt.rotbst(M); pRec.rotbst(M); // Azimuthal phi weighting: loop to new phi value if required. if (dipSel->asymPol != 0.) { Vec4 pAunt = event[dipSel->iAunt].p(); double cosPhi = cosphi( pRad, pAunt, pRadBef ); wtPhi = ( 1. + dipSel->asymPol * (2. * pow2(cosPhi) - 1.) ) / ( 1. + abs(dipSel->asymPol) ); } } while (wtPhi < rndmPtr->flat()) ; // Kinematics when recoiler is initial-state parton. int isrTypeNow = dipSel->isrType; int isrTypeSave = isrTypeNow; if (!useLocalRecoilNow) isrTypeNow = 0; if (isrTypeNow != 0) pRec = 2. * recBef.p() - pRec; // PS dec 2010: check if radiator has flexible normalization bool isFlexible = dipSel->isFlexible; // Define new particles from dipole branching. double pTsel = sqrt(dipSel->pT2); Particle rad = Particle(idRad, 51, iRadBef, 0, 0, 0, colRad, acolRad, pRad, mRad, pTsel); Particle emt = Particle(idEmt, 51, iRadBef, 0, 0, 0, colEmt, acolEmt, pEmt, mEmt, pTsel); // Recoiler either in final or in initial state Particle rec = (isrTypeNow == 0) ? Particle(recBef.id(), 52, iRecBef, iRecBef, 0, 0, recBef.col(), recBef.acol(), pRec, dipSel->mRec, pTsel) : Particle(recBef.id(), -53, 0, 0, iRecBef, iRecBef, recBef.col(), recBef.acol(), pRec, 0., 0.); // Special checks to set weak particles status equal to 56. // This is needed for decaying the particles. Also set polarisation. if (rec.idAbs() == 23 || rec.idAbs() == 24) rec.status(56); if (rad.idAbs() == 23 || rad.idAbs() == 24) rad.status(56); if (emt.idAbs() == 23 || emt.idAbs() == 24) { emt.status(56); event[iRadBef].pol( dipSel->weakPol ); rad.pol( dipSel->weakPol ); } // ME corrections can lead to branching being rejected. if (dipSel->MEtype > 0) { Particle& partner = (dipSel->iMEpartner == iRecBef) ? rec : event[dipSel->iMEpartner]; if ( findMEcorr( dipSel, rad, partner, emt) < rndmPtr->flat() ) return false; } // Rescatter: if the recoiling partner is not in the same system // as the radiator, fix up intermediate systems (can lead // to emissions being vetoed) if (allowRescatter && FIXRESCATTER && isInterleaved && iSysSel != iSysSelRec) { Vec4 pNew = rad.p() + emt.p(); if (!rescatterPropagateRecoil(event, pNew)) return false; } // Save properties to be restored in case of user-hook veto of emission. int eventSizeOld = event.size(); int iRadStatusV = event[iRadBef].status(); int iRadDau1V = event[iRadBef].daughter1(); int iRadDau2V = event[iRadBef].daughter2(); int iRecStatusV = event[iRecBef].status(); int iRecMot1V = event[iRecBef].mother1(); int iRecMot2V = event[iRecBef].mother2(); int iRecDau1V = event[iRecBef].daughter1(); int iRecDau2V = event[iRecBef].daughter2(); int beamOff1 = 1 + beamOffset; int beamOff2 = 2 + beamOffset; int ev1Dau1V = event[beamOff1].daughter1(); int ev2Dau1V = event[beamOff2].daughter1(); // Shower may occur at a displaced vertex. if (radBef.hasVertex()) { rad.vProd( radBef.vProd() ); emt.vProd( radBef.vProd() ); } if (recBef.hasVertex()) rec.vProd( recBef.vProd() ); // Put new particles into the event record. // Mark original dipole partons as branched and set daughters/mothers. int iRad = event.append(rad); int iEmt = event.append(emt); event[iRadBef].statusNeg(); event[iRadBef].daughters( iRad, iEmt); int iRec = 0; if (useLocalRecoilNow) { iRec = event.append(rec); if (isrTypeNow == 0) { event[iRecBef].statusNeg(); event[iRecBef].daughters( iRec, iRec); } else { event[iRecBef].mothers( iRec, iRec); event[iRec].mothers( iRecMot1V, iRecMot2V); if (iRecMot1V == beamOff1) event[beamOff1].daughter1( iRec); if (iRecMot1V == beamOff2) event[beamOff2].daughter1( iRec); } // Global recoil: need to find relevant rotation+boost for recoilers: // boost+rotate to rest frame, boost along z axis, rotate+boost back. } else { RotBstMatrix MG = M; MG.invert(); double pzRecBef = -0.5 * sqrtpos( pow2(dipSel->m2Dip - dipSel->m2Rad - dipSel->m2Rec) - 4. * dipSel->m2Rad * dipSel->m2Rec ) / dipSel->mDip; double eRecBef = sqrt( pow2(pzRecBef) + dipSel->m2Rec); double pzRecAft = -pzRadPlusEmt; double eRecAft = sqrt( pow2(pzRecAft) + dipSel->m2Rec); MG.bst( Vec4(0., 0., pzRecBef, eRecBef), Vec4(0., 0., pzRecAft, eRecAft) ); MG.rotbst( M); // Global recoil: copy particles, and rotate+boost momenta (not vertices). for (int iG = 0; iG < int(iGRecBef.size()); ++iG) { iRec = event.copy( iGRecBef[iG], 52); iGRec.push_back( iRec); Vec4 pGRec = event[iRec].p(); pGRec.rotbst( MG); event[iRec].p( pGRec); } } // Allow veto of branching. If so restore event record to before emission. bool inResonance = (partonSystemsPtr->getInA(iSysSel) == 0) ? true : false; if ( (canVetoEmission && userHooksPtr->doVetoFSREmission( eventSizeOld, event, iSysSel, inResonance)) || (canMergeFirst && mergingHooksPtr->doVetoEmission( event )) ) { event.popBack( event.size() - eventSizeOld); event[iRadBef].status( iRadStatusV); event[iRadBef].daughters( iRadDau1V, iRadDau2V); if (useLocalRecoilNow && isrTypeNow == 0) { event[iRecBef].status( iRecStatusV); event[iRecBef].daughters( iRecDau1V, iRecDau2V); } else if (useLocalRecoilNow) { event[iRecBef].mothers( iRecMot1V, iRecMot2V); if (iRecMot1V == beamOff1) event[beamOff1].daughter1( ev1Dau1V); if (iRecMot1V == beamOff2) event[beamOff2].daughter1( ev2Dau1V); } else { for (int iG = 0; iG < int(iGRecBef.size()); ++iG) { event[iGRecBef[iG]].statusPos(); event[iGRecBef[iG]].daughters( 0, 0); } } return false; } // For global recoil restore the one nominal recoiler, for bookkeeping. if (!useLocalRecoilNow) { iRec = iRecBef; for (int iG = 0; iG < int(iGRecBef.size()); ++iG) if (iGRecBef[iG] == iRecBef) iRec = iGRec[iG]; } // For initial-state recoiler also update beam and sHat info. if (isrTypeNow != 0) { BeamParticle& beamRec = (isrTypeNow == 1) ? *beamAPtr : *beamBPtr; double xOld = beamRec[iSysSelRec].x(); double xRec = 2. * pRec.e() / (beamAPtr->e() + beamBPtr->e()); beamRec[iSysSelRec].iPos( iRec); beamRec[iSysSelRec].x( xRec); partonSystemsPtr->setSHat( iSysSelRec, partonSystemsPtr->getSHat(iSysSelRec) * xRec / xOld); } // For global recoil: if everything went as expected, remove the line // from the list of "hard lines" that are allowed to use global recoil. if ( !useLocalRecoilNow || nGlobal >= nMaxGlobalBranch) { bool doRemove=true; while ( doRemove ) { bool hasRemoved = false; for (int iHard = 0; iHard < int(hardPartons.size()); ++iHard) if ( event[dipSel->iRadiator].isAncestor(hardPartons[iHard]) ) { hardPartons.erase( hardPartons.begin() + iHard ); hasRemoved = true; break; } doRemove = hasRemoved; } } // Update number of splittings that have been produced with global recoil. if ( !useLocalRecoilNow ) ++nGlobal; // Photon emission: update to new dipole ends; add new photon "dipole". if (dipSel->flavour == 22) { dipSel->iRadiator = iRad; dipSel->iRecoiler = iRec; // When recoiler was uncharged particle, in resonance decays, // assign recoil to emitted photons. if (recoilToColoured && inResonance && event[iRec].chargeType() == 0) dipSel->iRecoiler = iEmt; dipSel->pTmax = pTsel; if (doQEDshowerByGamma) dipEnd.push_back( TimeDipoleEnd(iEmt, iRad, pTsel, 0, 0, 1, 0, 0, iSysSel, 0) ); // Gluon emission: update both dipole ends and add two new ones. } else if (dipSel->flavour == 21) { dipSel->iRadiator = iRad; dipSel->iRecoiler = iEmt; dipSel->systemRec = iSysSel; dipSel->isrType = 0; dipSel->pTmax = pTsel; // Optionally also kill ME corrections after first emission. if (!doMEafterFirst) dipSel->MEtype = 0; // PS dec 2010: check normalization of radiating dipole // Dipole corresponding to the newly created color tag has normal strength double flexFactor = (isFlexible) ? dipSel->flexFactor : 1.0; dipSel->isFlexible = false; for (int i = 0; i < int(dipEnd.size()); ++i) { if (dipEnd[i].iRadiator == iRecBef && dipEnd[i].iRecoiler == iRadBef && dipEnd[i].colType != 0) { dipEnd[i].iRadiator = iRec; dipEnd[i].iRecoiler = iEmt; // Optionally also kill ME corrections after first emission. if (!doMEafterFirst) dipEnd[i].MEtype = 0; // Strive to match colour to anticolour inside closed system. if ( !isFlexible && dipEnd[i].colType * dipSel->colType > 0) dipEnd[i].iRecoiler = iRad; dipEnd[i].pTmax = pTsel; // PS dec 2010: if the (iRadBef,iRecBef) dipole was flexible, the // same should be true for this (opposite) end. If so, this end keeps // the modified normalization, so we shouldn't need to do anything. } } int colType = (dipSel->colType > 0) ? 2 : -2 ; // When recoiler was uncoloured particle, in resonance decays, // assign recoil to coloured particle. int iRecMod = iRec; if (recoilToColoured && inResonance && event[iRec].col() == 0 && event[iRec].acol() == 0) iRecMod = iRad; dipEnd.push_back( TimeDipoleEnd(iEmt, iRecMod, pTsel, colType, 0, 0, 0, isrTypeSave, iSysSel, 0)); dipEnd.back().systemRec = iSysSelRec; // PS dec 2010: the (iEmt,iRec) dipole "inherits" flexible normalization if (isFlexible) { dipEnd.back().isFlexible = true; dipEnd.back().flexFactor = flexFactor; } dipEnd.push_back( TimeDipoleEnd(iEmt, iRad, pTsel, -colType, 0, 0, 0, 0, iSysSel, 0)); // Gluon branching to q qbar: update current dipole and other of gluon. } else if (dipSel->colType != 0) { for (int i = 0; i < int(dipEnd.size()); ++i) { // Strive to match colour to anticolour inside closed system. if ( !isFlexible && dipEnd[i].iRecoiler == iRadBef && dipEnd[i].colType * dipSel->colType < 0 ) dipEnd[i].iRecoiler = iEmt; if (dipEnd[i].iRadiator == iRadBef && abs(dipEnd[i].colType) == 2) { dipEnd[i].colType /= 2; if (dipEnd[i].system != dipEnd[i].systemRec) continue; // Note: gluino -> quark + squark gives a deeper radiation dip than // the more obvious alternative photon decay, so is more realistic. dipEnd[i].MEtype = 66; if (&dipEnd[i] == dipSel) dipEnd[i].iMEpartner = iRad; else dipEnd[i].iMEpartner = iEmt; } } dipSel->iRadiator = iEmt; dipSel->iRecoiler = iRec; dipSel->pTmax = pTsel; // Gluon branching to q qbar: also add two charge dipole ends. // Note: gluino -> quark + squark gives a deeper radiation dip than // the more obvious alternative photon decay, so is more realistic. if (doQEDshowerByQ) { int chgType = event[iRad].chargeType(); dipEnd.push_back( TimeDipoleEnd(iRad, iEmt, pTsel, 0, chgType, 0, 0, 0, iSysSel, 66, iEmt)); dipEnd.push_back( TimeDipoleEnd(iEmt, iRad, pTsel, 0, -chgType, 0, 0, 0, iSysSel, 66, iRad)); } // Gluon branching to q qbar: also add weak dipoles. // Randomly decided whether to use left or right quarks. if (doWeakShower && (!hasWeaklyRadiated || !singleWeakEmission)) { int weakPol = (rndmPtr->flat() > 0.5) ? -1 : 1; if ((weakMode == 0 || weakMode == 1) && weakPol == -1) { dipEnd.push_back( TimeDipoleEnd(iRad, iEmt, pTsel, 0, 0, 0, 1, 0, iSysSel, 201, iEmt, weakPol) ); dipEnd.push_back( TimeDipoleEnd(iEmt, iRad, pTsel, 0, 0, 0, 1, 0, iSysSel, 201, iRad, weakPol) ); } if (weakMode == 0 || weakMode == 2) { dipEnd.push_back( TimeDipoleEnd(iRad, iEmt, pTsel, 0, 0, 0, 2, 0, iSysSel, 202, iEmt, weakPol) ); dipEnd.push_back( TimeDipoleEnd(iEmt, iRad, pTsel, 0, 0, 0, 2, 0, iSysSel, 202, iRad, weakPol) ); } } // Photon branching to f fbar: inactivate photon "dipole"; // optionally add new charge and colour dipole ends. // (But not W or Z ends, since W/Z are heavier than gamma*.) } else if (dipSel->gamType != 0) { dipSel->gamType = 0; int chgType = event[iRad].chargeType(); int colType = event[iRad].colType(); // MEtype = 102 for charge in vector decay. if ( chgType != 0 && ( ( doQEDshowerByQ && colType != 0 ) || ( doQEDshowerByL && colType == 0 ) ) ) { dipEnd.push_back( TimeDipoleEnd(iRad, iEmt, pTsel, 0, chgType, 0, 0, 0, iSysSel, 102, iEmt) ); dipEnd.push_back( TimeDipoleEnd(iEmt, iRad, pTsel, 0, -chgType, 0, 0, 0, iSysSel, 102, iRad) ); } // MEtype = 11 for colour in vector decay. if (colType != 0 && doQCDshower) { dipEnd.push_back( TimeDipoleEnd(iRad, iEmt, pTsel, colType, 0, 0, 0, 0, iSysSel, 11, iEmt) ); dipEnd.push_back( TimeDipoleEnd(iEmt, iRad, pTsel, -colType, 0, 0, 0, 0, iSysSel, 11, iRad) ); } // Photon_HV emission: update to new dipole ends. } else if (dipSel->flavour == 4900022) { dipSel->iRadiator = iRad; dipSel->iRecoiler = iRec; dipSel->pTmax = pTsel; // Gluon_HV emission: update to new dipole ends. } else if (dipSel->flavour == 4900021) { dipSel->iRadiator = iRad; dipSel->iRecoiler = iEmt; dipSel->pTmax = pTsel; for (int i = 0; i < int(dipEnd.size()); ++i) if (dipEnd[i].iRadiator == iRecBef && dipEnd[i].iRecoiler == iRadBef && dipEnd[i].isHiddenValley) { dipEnd[i].iRadiator = iRec; dipEnd[i].iRecoiler = iEmt; dipEnd[i].pTmax = pTsel; } int colvType = (dipSel->colvType > 0) ? 2 : -2 ; dipEnd.push_back( TimeDipoleEnd(iEmt, iRec, pTsel, 0, 0, 0, 0, isrTypeSave, iSysSel, 0, -1, 0, false, true, colvType) ); dipEnd.back().systemRec = iSysSelRec; dipEnd.push_back( TimeDipoleEnd(iEmt, iRad, pTsel, 0, 0, 0, 0, 0, iSysSel, 0, -1, 0, false, true, -colvType) ); // W/Z emission, if only a single weak emission is allowed. } else if (dipSel->weakType != 0) { hasWeaklyRadiated = true; if (singleWeakEmission) for (int i = 0; i < int(dipEnd.size()); ++i) dipEnd[i].weakType = 0; } // Copy or set lifetime for new final state. if (event[iRad].id() == event[iRadBef].id()) { event[iRad].tau( event[iRadBef].tau() ); } else { event[iRad].tau( event[iRad].tau0() * rndmPtr->exp() ); event[iEmt].tau( event[iEmt].tau0() * rndmPtr->exp() ); } event[iRec].tau( event[iRecBef].tau() ); // Now update other dipoles that also involved the radiator or recoiler. for (int i = 0; i < int(dipEnd.size()); ++i) { // PS dec 2010: if radiator was flexible and now is normal, there may // be other flexible dipoles that need updating. if (isFlexible && !dipSel->isFlexible && dipEnd[i].isFlexible) { if (dipEnd[i].iRecoiler == iRadBef) dipEnd[i].iRecoiler = iEmt; if (dipEnd[i].iRadiator == iRadBef) { dipEnd[i].iRadiator = iEmt; if (dipEnd[i].colType == 1 && dipSel->flavour == 21) dipEnd[i].colType = 2; if (dipEnd[i].colType ==-1 && dipSel->flavour == 21) dipEnd[i].colType =-2; } } if (dipEnd[i].iRadiator == iRadBef) dipEnd[i].iRadiator = iRad; if (dipEnd[i].iRecoiler == iRadBef) dipEnd[i].iRecoiler = iRad; if (dipEnd[i].iMEpartner == iRadBef) dipEnd[i].iMEpartner = iRad; if (useLocalRecoilNow) { if (dipEnd[i].iRadiator == iRecBef) dipEnd[i].iRadiator = iRec; if (dipEnd[i].iRecoiler == iRecBef) dipEnd[i].iRecoiler = iRec; if (dipEnd[i].iMEpartner == iRecBef) dipEnd[i].iMEpartner = iRec; } else { for (int iG = 0; iG < int(iGRecBef.size()); ++iG) { if (dipEnd[i].iRadiator == iGRecBef[iG]) dipEnd[i].iRadiator = iGRec[iG]; if (dipEnd[i].iRecoiler == iGRecBef[iG]) dipEnd[i].iRecoiler = iGRec[iG]; if (dipEnd[i].iMEpartner == iGRecBef[iG]) dipEnd[i].iMEpartner = iGRec[iG]; } } } // PS Apr 2011 // Update any junctions downstream of this branching (if necessary) // (This happens, e.g., via LHEF, when adding showers to intermediate // coloured resonances whose decays involved junctions) for (int iJun = 0; iJun < event.sizeJunction(); iJun++) { // Number of incoming colour lines for this junction. int nIncoming = (event.kindJunction(iJun)-1)/2; // Check radiator colour or anticolour, depending on junction kind // (if junction, incoming = anticolours, and vice versa) int colChk = 0; colChk = ( event.kindJunction(iJun) % 2 == 0 ) ? event[iRadBef].col() : event[iRadBef].acol(); // Loop over incoming junction ends for (int iCol = 0; iCol < nIncoming; iCol++) { int colJun = event.colJunction( iJun, iCol); // If match, update junction end with new upstream (anti)colour if (colJun == colChk) { int colNew = 0; if ( event.kindJunction(iJun) % 2 == 0 ) colNew = colRad; else colNew = acolRad; event.colJunction( iJun, iCol, colNew ); } } } // Finally update the list of all partons in all systems. partonSystemsPtr->replace(iSysSel, iRadBef, iRad); partonSystemsPtr->addOut(iSysSel, iEmt); if (useLocalRecoilNow) partonSystemsPtr->replace(iSysSelRec, iRecBef, iRec); else { for (int iG = 0; iG < int(iGRecBef.size()); ++iG) partonSystemsPtr->replace(iSysSel, iGRecBef[iG], iGRec[iG]); } // Done. return true; } //-------------------------------------------------------------------------- // Rescatter: If a dipole stretches between two different systems, those // systems will no longer locally conserve momentum. These // imbalances become problematic when ISR or primordial kT // is switched on as these steps involve Lorentz boosts. // // 'rescatterPropagateRecoil' tries to fix momentum in all // systems by propogating recoil momentum through all // intermediate systems. As the momentum transfer is already // defined, this can lead to internal lines gaining a // virtuality. // Useful definitions for a pair of integers and a vector of pairs typedef pair < int, int > pairInt; typedef vector < pairInt > vectorPairInt; //-------------------------------------------------------------------------- // findParentSystems // Utility routine to find all parent systems of a given system // Returns a vector of pairs of integers with: // a) The system index, including the starting system (negative // if (b) points to a parent system, positive if (b) points // to a daughter system // b) The event record index that is the path out of the system // (if forwards == false, this is an incoming parton to the // system, and is +ve if side A or -ve if side B, // if forwards == true, this is an outgoing parton from the // system). // Returns as empty vector on failure // Note: this assumes single rescattering only and therefore only // one possible parent system inline vectorPairInt findParentSystems(const int sys, Event& event, PartonSystems* partonSystemsPtr, bool forwards) { vectorPairInt parentSystems; parentSystems.reserve(10); int iSysCur = sys; while (true) { // Get two incoming partons int iInA = partonSystemsPtr->getInA(iSysCur); int iInB = partonSystemsPtr->getInB(iSysCur); // Check if either of these links to another system int iIn = 0; if (event[iInA].isRescatteredIncoming()) iIn = iInA; if (event[iInB].isRescatteredIncoming()) iIn = -iInB; // Save the current system to the vector parentSystems.push_back( pairInt(-iSysCur, iIn) ); if (iIn == 0) break; int iInAbs = abs(iIn); int iMother = event[iInAbs].mother1(); iSysCur = partonSystemsPtr->getSystemOf(iMother); if (iSysCur == -1) { parentSystems.clear(); break; } } // while (true) // If forwards is set, change all event record indices to go to daughter // systems rather than parent systems if (forwards) { vectorPairInt::reverse_iterator rit; for (rit = parentSystems.rbegin(); rit < (parentSystems.rend() - 1); ++rit) { pairInt &cur = *rit; pairInt &next = *(rit + 1); cur.first = -cur.first; cur.second = (next.second < 0) ? -event[abs(next.second)].mother1() : event[abs(next.second)].mother1(); } } return parentSystems; } //-------------------------------------------------------------------------- // rescatterPropagateRecoil // Fix up momentum in all intermediate systems when radiator and recoiler // systems are different. The strategy is to look at all parent systems // from the radiator system and the recoiler system and find where they // intersect. bool TimeShower::rescatterPropagateRecoil( Event& event, Vec4& pNew) { // Some useful variables for later int iRadBef = dipSel->iRadiator; iSysSel = dipSel->system; int iSysSelRec = dipSel->systemRec; Vec4 pImbal = pNew - event[iRadBef].p(); // Store changes locally at first in case we veto the branching // eventMod stores index into the event record and new 4-vector vector < pair < int, Vec4 > > eventMod; eventMod.reserve(10); // systemMod stores system index (iSys) and system-parton index (iMem) // iMem >= 0 - index into outgoing partons (iOut) // iMem == -1 - incoming A // iMem == -2 - incoming B vectorPairInt systemMod; systemMod.reserve(10); // Find all parent systems from radiating and recoiling systems vectorPairInt radParent = findParentSystems(iSysSel, event, partonSystemsPtr, false); vectorPairInt recParent = findParentSystems(iSysSelRec, event, partonSystemsPtr, true); if (radParent.size() == 0 || recParent.size() == 0) { // This should never happen infoPtr->errorMsg("Error in TimeShower::rescatterPropagateRecoil: " "couldn't find parent system; branching vetoed"); return false; } // Find the system that connects radiating and recoiling system bool foundPath = false; unsigned int iRadP = 0; unsigned int iRecP = 0; for (iRadP = 0; iRadP < radParent.size(); iRadP++) { for (iRecP = 0; iRecP < recParent.size(); iRecP++) if (abs(radParent[iRadP].first) == abs(recParent[iRecP].first)) { foundPath = true; break; } if (foundPath) break; } if (!foundPath) { // Can fail e.g. for QED dipoles where there is no connection // between radiator and recoiler systems infoPtr->errorMsg("Warning in TimeShower::rescatterPropagateRecoil: " "couldn't find recoil path; branching vetoed"); return false; } // Join together to form complete path from radiating system // to recoiling system vectorPairInt path; if (radParent.size() > 1) path.assign(radParent.begin(), radParent.begin() + iRadP); if (recParent.size() > 1) path.insert(path.end(), recParent.rend() - iRecP - 1, recParent.rend() - 1); // Follow the path fixing up momenta as we go for (unsigned int i = 0; i < path.size(); i++) { // Line out of the current system bool isIncoming = (path[i].first < 0) ? true : false; int iSysCur = abs(path[i].first); bool isIncomingA = (path[i].second > 0) ? true : false; int iLink = abs(path[i].second); int iMemCur; if (isIncoming) iMemCur = (isIncomingA) ? -1 : -2; else { iMemCur = -1; for (int j = 0; j < partonSystemsPtr->sizeOut(iSysCur); j++) if (partonSystemsPtr->getOut(iSysCur, j) == iLink) { iMemCur = j; break; } if (iMemCur == -1) { // This should never happen infoPtr->errorMsg("Error in TimeShower::rescatterPropagateRecoil: " "couldn't find parton system; branching vetoed"); return false; } } Vec4 pMod = (isIncoming) ? event[iLink].p() + pImbal : event[iLink].p() - pImbal; eventMod.push_back(pair (iLink, pMod)); systemMod.push_back(pairInt(iSysCur, iMemCur)); // Calculate sHat of iSysCur int iInCurA = partonSystemsPtr->getInA(iSysCur); int iInCurB = partonSystemsPtr->getInB(iSysCur); Vec4 pTotCur = event[iInCurA].p() + event[iInCurB].p(); // If iMemCur is -1 or -2, then we must have changed the sHat of iSysCur if (iMemCur < 0) pTotCur += (isIncoming) ? pImbal : -pImbal; double sHatCur = pTotCur.m2Calc(); // The fixed-up incoming and outgoing partons should not have // too large a virtuality in relation to the system mass-square. if (abs(pMod.m2Calc()) > MAXVIRTUALITYFRACTION * sHatCur) { infoPtr->errorMsg("Warning in TimeShower::rescatterPropagateRecoil: " "virtuality much larger than sHat; branching vetoed"); return false; } // Outgoing ones should also not have too large negative energy // in the rest frame of the system. if (!isIncoming && pMod * pTotCur < -MAXNEGENERGYFRACTION * sHatCur) { infoPtr->errorMsg("Warning in TimeShower::rescatterPropagateRecoil: " "rest frame energy too negative; branching vetoed"); return false; } // Veto negative sHat. if (sHatCur < 0.0) { infoPtr->errorMsg("Warning in TimeShower::rescatterPropagateRecoil: " "sHat became negative; branching vetoed"); return false; } // Line into the new current system iLink = (isIncoming) ? event[iLink].mother1() : event[iLink].daughter1(); iSysCur = partonSystemsPtr->getSystemOf(iLink, true); if (!isIncoming) iMemCur = (isIncomingA) ? -1 : -2; else { iMemCur = -1; for (int j = 0; j < partonSystemsPtr->sizeOut(iSysCur); j++) if (partonSystemsPtr->getOut(iSysCur, j) == iLink) { iMemCur = j; break; } if (iMemCur == -1) { // This should never happen infoPtr->errorMsg("Error in TimeShower::rescatterPropagateRecoil: " "couldn't find parton system; branching vetoed"); return false; } } pMod = (isIncoming) ? event[iLink].p() + pImbal : event[iLink].p() - pImbal; eventMod.push_back(pair (iLink, pMod)); systemMod.push_back(pairInt(iSysCur, iMemCur)); // Calculate sHat of iSysCur iInCurA = partonSystemsPtr->getInA(iSysCur); iInCurB = partonSystemsPtr->getInB(iSysCur); pTotCur = event[iInCurA].p() + event[iInCurB].p(); // If iMemCur is -1 or -2, then we must have changed the sHat of iSysCur if (iMemCur < 0) pTotCur += (isIncoming) ? pImbal : -pImbal; sHatCur = pTotCur.m2Calc(); // The fixed-up incoming and outgoing partons should not have // too large a virtuality in relation to the system mass-square. if (abs(pMod.m2Calc()) > MAXVIRTUALITYFRACTION * sHatCur) { infoPtr->errorMsg("Warning in TimeShower::rescatterPropagateRecoil: " "virtuality much larger than sHat; branching vetoed"); return false; } // Outgoing ones should also not have too large negative energy // in the rest frame of the system. if (!isIncoming && pMod * pTotCur < -MAXNEGENERGYFRACTION * sHatCur) { infoPtr->errorMsg("Warning in TimeShower::rescatterPropagateRecoil: " "rest frame energy too negative; branching vetoed"); return false; } // Veto negative sHat if (sHatCur < 0.0) { infoPtr->errorMsg("Warning in TimeShower::rescatterPropagateRecoil: " "sHat became negative; branching vetoed"); return false; } // Do negative energy veto if (VETONEGENERGY && pMod.e() < 0.0) { infoPtr->errorMsg("Warning in TimeShower::rescatterPropagateRecoil: " "energy became negative; branching vetoed"); return false; } } // for (unsigned int i = 0; i < path.size(); i++) // If no vetos by this point, apply the changes to the event record // An incoming particle with changed momentum is given status code -54, // an outgoing particle with changed momentum is given status code -55 for (unsigned int i = 0; i < eventMod.size(); i++) { int idx = eventMod[i].first; Vec4 &pMod = eventMod[i].second; int iSys = systemMod[i].first; int iMem = systemMod[i].second; // If incoming to a process then set the copy to be the mother if (event[idx].isRescatteredIncoming()) { int mother1 = event[idx].mother1(); idx = event.copy(idx, -54); event[mother1].daughters(idx, idx); // Update beam information if necessary double eCM = sqrt(m2( beamAPtr->p(), beamBPtr->p())); if (iMem == -1) { partonSystemsPtr->setInA(iSys, idx); (*beamAPtr)[iSys].x((pMod.e() + pMod.pz()) / eCM); (*beamAPtr)[iSys].m(pMod.mCalc()); (*beamAPtr)[iSys].p(pMod); (*beamAPtr)[iSys].iPos(idx); } else if (iMem == -2) { partonSystemsPtr->setInB(iSys, idx); (*beamBPtr)[iSys].x((pMod.e() - pMod.pz()) / eCM); (*beamBPtr)[iSys].m(pMod.mCalc()); (*beamBPtr)[iSys].p(pMod); (*beamBPtr)[iSys].iPos(idx); } else { // This should never happen infoPtr->errorMsg("Error in TimeShower::rescatterPropagateRecoil: " "internal bookeeping error"); } // Otherwise set the new event record entry to be the daughter } else { int daughter1 = event[idx].daughter1(); idx = event.copy(idx, 55); event[idx].statusNeg(); event[daughter1].mothers(idx, idx); partonSystemsPtr->setOut(iSys, iMem, idx); } event[idx].p( eventMod[i].second ); event[idx].m( event[idx].mCalc() ); } return true; } //-------------------------------------------------------------------------- // Find class of QCD ME correction. // MEtype classification follow codes in Norrbin article, // additionally -1 = try to find type, 0 = no ME corrections. // Warning: not yet tried out to do a correct assignment in // arbitrary multiparton configurations! ?? void TimeShower::findMEtype( Event& event, TimeDipoleEnd& dip) { // Initial value. Mark if no ME corrections to be applied. bool setME = true; if (!doMEcorrections) setME = false; int iMother = event[dip.iRadiator].mother1(); int iMother2 = event[dip.iRadiator].mother2(); // Allow ME corrections for Hidden Valley pair in 2 -> 2. if (dip.isHiddenValley && event[dip.iRecoiler].id() == -event[dip.iRadiator].id()); // Allow ME corrections for all weak branchings. else if (dip.weakType != 0); // Else no ME corrections in 2 -> n processes. else { if (iMother2 != iMother && iMother2 != 0) setME = false; if (event[dip.iRecoiler].mother1() != iMother) setME = false; if (event[dip.iRecoiler].mother2() != iMother2) setME = false; } // No ME corrections for recoiler in initial state. if (event[dip.iRecoiler].status() < 0) setME = false; // No ME corrections for recoiler not in same system if (dip.system != dip.systemRec) setME = false; // Done if no ME to be set. if (!setME) { dip.MEtype = 0; return; } // If no ME partner set, assume it is the recoiler. if (dip.iMEpartner < 0) dip.iMEpartner = dip.iRecoiler; // Now begin processing of colour dipole, including Hidden Valley. if (dip.colType != 0 || dip.colvType != 0) { bool isHiddenColour = (dip.colvType != 0); // Find daughter types (may or may not be used later on). int idDau1 = event[dip.iRadiator].id(); int idDau2 = event[dip.iMEpartner].id(); int dau1Type = findMEparticle(idDau1, isHiddenColour); int dau2Type = findMEparticle(idDau2, isHiddenColour); int minDauType = min(dau1Type, dau2Type); int maxDauType = max(dau1Type, dau2Type); // Reorder dipole ends in kinematics. Split ME expression in two sides. dip.MEorder = (dau2Type >= dau1Type); dip.MEsplit = (maxDauType <= 6); dip.MEgluinoRec = false; // If type already set (or set not to have) then done. if (minDauType == 0 && dip.MEtype < 0) dip.MEtype = 0; if (dip.MEtype >= 0) return; dip.MEtype = 0; // For H -> gg -> ggg we found that DGLAP kernels do better than eikonal. if (dau1Type == 4 && dau2Type == 4) return; // Find mother type. int idMother = 0; if ( event[dip.iRecoiler].mother1() == iMother && iMother >= 0) idMother = event[iMother].id(); int motherType = (idMother != 0) ? findMEparticle(idMother, isHiddenColour) : 0; // When a mother if not known then use colour and spin content to guess. if (motherType == 0) { int col1 = event[dip.iRadiator].col(); int acol1 = event[dip.iRadiator].acol(); int col2 = event[dip.iMEpartner].col(); int acol2 = event[dip.iMEpartner].acol(); // spinT = 0/1 = integer or half-integer. int spinT = ( event[dip.iRadiator].spinType() + event[dip.iMEpartner].spinType() )%2; // Colour singlet mother. if ( col1 == acol2 && acol1 == col2 ) motherType = (spinT == 0) ? 7 : 9; // Colour octet mother. else if ( (col1 == acol2 && acol1 != 0 && col2 != 0) || (acol1 == col2 && col1 != 0 && acol2 != 0) ) motherType = (spinT == 0) ? 4 : 5; // Colour triplet mother. else if ( (col1 == acol2 && acol1 != col2) || (acol1 == col2 && col1 != acol2) ) motherType = (spinT == 0) ? 2 : 1; // If no colours are matched then cannot have common mother, so done. else return; } // Now start from default, which is eikonal ME corrections, // and try to find matching ME cases below. int MEkind = 0; int MEcombi = 4; dip.MEmix = 0.5; // Hidden Valley with massive gamma_v covered by two special cases. if (isHiddenColour && brokenHVsym) { MEkind = (dau2Type == 0 || dau2Type > 6) ? 30 : 31; dip.MEtype = 5 * MEkind + 1; return; } // Triplet recoiling against gluino needs enhanced radiation // to match to matrix elements. dip.MEgluinoRec = (dau1Type >= 1 && dau1Type <= 3 && dau2Type == 5); // Vector/axial vector -> q + qbar. if (minDauType == 1 && maxDauType == 1 && (motherType == 4 || motherType == 7) ) { MEkind = 2; if (idMother == 21 || idMother == 22) MEcombi = 1; else if (idMother == 23 || idDau1 + idDau2 == 0) { MEcombi = 3; dip.MEmix = gammaZmix( event, iMother, dip.iRadiator, dip.iRecoiler ); } else if (idMother == 24) MEcombi = 4; } // For chi -> chi q qbar, use V/A -> q qbar as first approximation. else if (minDauType == 1 && maxDauType == 1 && motherType == 9) MEkind = 2; // q -> q + V. else if (minDauType == 1 && maxDauType == 7 && motherType == 1) MEkind = 3; if (idDau1 == 22 || idDau2 == 22) MEcombi = 1; // Scalar/pseudoscalar -> q + qbar; q -> q + S. else if (minDauType == 1 && maxDauType == 1 && motherType == 8) { MEkind = 4; if (idMother == 25 || idMother == 35 || idMother == 37) MEcombi = 1; else if (idMother == 36) MEcombi = 2; } else if (minDauType == 1 && maxDauType == 8 && motherType == 1) MEkind = 5; // V -> ~q + ~qbar; ~q -> ~q + V; S -> ~q + ~qbar; ~q -> ~q + S. else if (minDauType == 2 && maxDauType == 2 && (motherType == 4 || motherType == 7) ) MEkind = 6; else if (minDauType == 2 && (maxDauType == 4 || maxDauType == 7) && motherType == 2) MEkind = 7; else if (minDauType == 2 && maxDauType == 2 && motherType == 8) MEkind = 8; else if (minDauType == 2 && maxDauType == 8 && motherType == 2) MEkind = 9; // chi -> q + ~qbar; ~q -> q + chi; q -> ~q + chi. else if (minDauType == 1 && maxDauType == 2 && motherType == 9) MEkind = 10; else if (minDauType == 1 && maxDauType == 9 && motherType == 2) MEkind = 11; else if (minDauType == 2 && maxDauType == 9 && motherType == 1) MEkind = 12; // ~g -> q + ~qbar; ~q -> q + ~g; q -> ~q + ~g. else if (minDauType == 1 && maxDauType == 2 && motherType == 5) MEkind = 13; else if (minDauType == 1 && maxDauType == 5 && motherType == 2) MEkind = 14; else if (minDauType == 2 && maxDauType == 5 && motherType == 1) MEkind = 15; // In cases where coloured spin 1 particle involved use spin 0. // V_coloured -> q + l. else if (minDauType == 1 && maxDauType == 9 && motherType == 3) MEkind = 11; // q -> V_coloured + l; else if (minDauType == 3 && maxDauType == 9 && motherType == 1) MEkind = 12; // g (+V, S) -> ~g + ~g (eikonal approximation). else if (minDauType == 5 && maxDauType == 5) MEkind = 16; // Save ME type and gamma_5 admixture. dip.MEtype = 5 * MEkind + MEcombi; // Now begin processing of charge dipole - still primitive. } else if (dip.chgType != 0) { // Set defaults for QED case; then possibly done. dip.MEorder = true; dip.MEsplit = true; if (dip.MEtype >= 0) return; // So far only ME corrections for q qbar or l lbar. int idDau1 = event[dip.iRadiator].id(); int idDau2 = event[dip.iMEpartner].id(); if (abs(idDau1) < 9 && abs(idDau2) < 9 && idDau1 * idDau2 < 0) ; else if (abs(idDau1) > 10 && abs(idDau1) < 19 && abs(idDau2) > 10 && abs(idDau2) < 19 && idDau1 * idDau2 < 0) ; else { dip.MEtype = 0; return; } // Distinguish charge sum != 0 or = 0; in latter assume vector source. dip.MEtype = 101; if (idDau1 + idDau2 == 0) dip.MEtype = 102; dip.MEmix = 1.; } // Weak ME corrections. else if (dip.weakType == 1) dip.MEtype = 201; else if (dip.weakType == 2) dip.MEtype = 202; } //-------------------------------------------------------------------------- // Find type of particle for ME type: 0 = unknown, 1 = quark, 2 = squark, // 3 = spare triplet, 4 = gluon, 5 = gluino, 6 = spare octet, // 7 = vector boson, 8 = colourless scalar, 9 = colourless spin 1/2. int TimeShower::findMEparticle( int id, bool isHiddenColour) { // find colour and spin of particle. int type = 0; int colType = abs(particleDataPtr->colType(id)); int spinType = particleDataPtr->spinType(id); // For hidden valley particle treat HV colour as normal one. // Note: no need to assign gv/gammav since not in ME. if (isHiddenColour) { colType = 0; int idAbs = abs(id); if ( (idAbs > 4900000 && idAbs < 4900007) || (idAbs > 4900010 && idAbs < 4900017) || idAbs == 4900101) colType = 1; } // Find particle type from colour and spin. if (colType == 1 && spinType == 2) type = 1; else if (colType == 1 && spinType == 1) type = 2; else if (colType == 1) type = 3; else if (colType == 2 && spinType == 3) type = 4; else if (colType == 2 && spinType == 2) type = 5; else if (colType == 2) type = 6; else if (colType == 0 && spinType == 3) type = 7; else if (colType == 0 && spinType == 1) type = 8; else if (colType == 0 && spinType == 2) type = 9; // Done. return type; } //-------------------------------------------------------------------------- // Find mixture of V and A in gamma/Z: energy- and flavour-dependent. double TimeShower::gammaZmix( Event& event, int iRes, int iDau1, int iDau2) { // Try to identify initial flavours; use e+e- as default. int idIn1 = -11; int idIn2 = 11; int iIn1 = (iRes >= 0) ? event[iRes].mother1() : -1; int iIn2 = (iRes >= 0) ? event[iRes].mother2() : -1; if (iIn1 >=0) idIn1 = event[iIn1].id(); if (iIn2 >=0) idIn2 = event[iIn1].id(); // In processes f + g/gamma -> f + Z only need find one fermion. if (idIn1 == 21 || idIn1 == 22) idIn1 = -idIn2; if (idIn2 == 21 || idIn2 == 22) idIn2 = -idIn1; // Initial flavours and couplings; return if don't make sense. if (idIn1 + idIn2 != 0 ) return 0.5; int idInAbs = abs(idIn1); if (idInAbs == 0 || idInAbs > 18 ) return 0.5; double ei = coupSMPtr->ef(idInAbs); double vi = coupSMPtr->vf(idInAbs); double ai = coupSMPtr->af(idInAbs); // Final flavours and couplings; return if don't make sense. if (event[iDau1].id() + event[iDau2].id() != 0) return 0.5; int idOutAbs = abs(event[iDau1].id()); if (idOutAbs == 0 || idOutAbs >18 ) return 0.5; double ef = coupSMPtr->ef(idOutAbs); double vf = coupSMPtr->vf(idOutAbs); double af = coupSMPtr->af(idOutAbs); // Calculate prefactors for interference and resonance part. Vec4 psum = event[iDau1].p() + event[iDau2].p(); double sH = psum.m2Calc(); double intNorm = 2. * thetaWRat * sH * (sH - mZ*mZ) / ( pow2(sH - mZ*mZ) + pow2(sH * gammaZ / mZ) ); double resNorm = pow2(thetaWRat * sH) / ( pow2(sH - mZ*mZ) + pow2(sH * gammaZ / mZ) ); // Calculate vector and axial expressions and find mix. double vect = ei*ei * ef*ef + ei*vi * intNorm * ef*vf + (vi*vi + ai*ai) * resNorm * vf*vf; double axiv = (vi*vi + ai*ai) * resNorm * af*af; return vect / (vect + axiv); } //-------------------------------------------------------------------------- // Set up to calculate QCD ME correction with calcMEcorr. // Normally for primary particles, but also from g/gamma -> f fbar. double TimeShower::findMEcorr(TimeDipoleEnd* dip, Particle& rad, Particle& partner, Particle& emt, bool cutEdge) { // Initial values and matrix element kind. double wtME = 1.; double wtPS = 1.; int MEkind = dip->MEtype / 5; int MEcombi = dip->MEtype % 5; // Construct ME variables. Vec4 sum = rad.p() + partner.p() + emt.p(); double eCMME = sum.mCalc(); double x1 = 2. * (sum * rad.p()) / pow2(eCMME); double x2 = 2. * (sum * partner.p()) / pow2(eCMME); double r1 = rad.m() / eCMME; double r2 = partner.m() / eCMME; double r3 = 0.; // Evaluate kinematics for Hidden Valley with massive gamma_v. double gammavCorr = 1.; if (dip->colvType != 0 && brokenHVsym) { r3 = emt.m() / eCMME; double x3Tmp = 2. - x1 - x2; gammavCorr = x3Tmp / (x3Tmp - kRad * (x1 + x3Tmp)); // For Q_v Qbar_v pair correct kinematics to common average mass. if (MEkind == 31) { double m2Pair = (rad.p() + partner.p()).m2Calc(); double m2Avg = 0.5 * (rad.m2() + partner.m2()) - 0.25 * pow2(rad.m2() - partner.m2()) / m2Pair; r1 = sqrt(m2Avg) / eCMME; r2 = r1; double xShift = 0.5 * (x1 + x2) * (partner.m2() - rad.m2()) / m2Pair; x1 += xShift; x2 -= xShift; } } // Derived ME variables, suitably protected. double x1minus, x2minus, x3; if (cutEdge) { x1minus = max(XMARGIN, 1. + r1*r1 - r2*r2 - x1); x2minus = max(XMARGIN, 1. + r2*r2 - r1*r1 - x2) ; x3 = max(XMARGIN, 2. - x1 - x2); } else { x1minus = max(XMARGIN*XMARGIN, 1. + r1*r1 - r2*r2 - x1); x2minus = max(XMARGIN*XMARGIN, 1. + r2*r2 - r1*r1 - x2) ; x3 = max(XMARGIN*XMARGIN, 2. - x1 - x2); } // Begin processing of QCD dipoles. if (dip->colType !=0 || dip->colvType != 0) { // Evaluate normal ME, for proper order of particles. if (dip->MEorder) wtME = calcMEcorr(MEkind, MEcombi, dip->MEmix, x1, x2, r1, r2, r3, cutEdge); else wtME = calcMEcorr(MEkind, MEcombi, dip->MEmix, x2, x1, r2, r1, r3, cutEdge); // Split up total ME when two radiating particles. if (dip->MEsplit) wtME = wtME * x1minus / x3; // Evaluate shower rate to be compared with. wtPS = 2. / ( x3 * x2minus ); if (dip->MEgluinoRec) wtPS *= 9./4.; if (dip->colvType != 0 && brokenHVsym) wtPS *= gammavCorr; // For generic charge combination currently only massless expression. // (Masses included only to respect phase space boundaries.) } else if (dip->chgType !=0 && dip->MEtype == 101) { double chg1 = particleDataPtr->charge(rad.id()); double chg2 = particleDataPtr->charge(partner.id()); wtME = (x1*x1 + x2*x2) * pow2( chg1 * x1minus / x3 - chg2 * x2minus / x3 ); wtPS = 2. * ( chg1*chg1 * x1minus / x3 + chg2*chg2 * x2minus / x3 ); // For flavour neutral system assume vector source and include masses. } else if (dip->chgType !=0 && dip->MEtype == 102) { wtME = calcMEcorr(2, 1, dip->MEmix, x1, x2, r1, r2, 0., cutEdge) * x1minus / x3; wtPS = 2. / ( x3 * x2minus ); } // For W-emissions and Z-emissions: // currently using same matrix element for W and Z. else if (dip->MEtype == 202 || dip->MEtype == 201) { r3 = emt.m() / eCMME; wtME = calcMEcorr(32, 1, dip->MEmix, x1, x2, r1, r2, r3, cutEdge) * x1minus / x3; wtPS = 8. / (x3 * x2minus); wtPS *= x3 / (x3 - kRad * (x1 + x3)); } // Return ratio of actual ME to assumed PS rate of emission. if (wtME > wtPS) infoPtr->errorMsg("Warning in TimeShower::findMEcorr: " "ME weight above PS one"); return wtME / wtPS; } //-------------------------------------------------------------------------- // Matrix elements for gluon (or photon) emission from // a two-body state; to be used by the parton shower routine. // Here x_i = 2 E_i/E_cm, r_i = m_i/E_cm and // 1/sigma_0 d(sigma)/d(x_1)d(x_2) = (alpha-strong/2 pi) * C_F * (this), // i.e. normalization is such that one recovers the familiar // (x_1^2 + x_2^2)/((1-x_1)*(1-x_2)) for the massless case. // Coupling structure: // kind = 1 : eikonal soft-gluon expression (spin-independent) // = 2 : V -> q qbar (V = vector/axial vector colour singlet) // = 3 : q -> q V // = 4 : S -> q qbar (S = scalar/pseudoscalar colour singlet) // = 5 : q -> q S // = 6 : V -> ~q ~qbar (~q = squark) // = 7 : ~q -> ~q V // = 8 : S -> ~q ~qbar // = 9 : ~q -> ~q S // = 10 : chi -> q ~qbar (chi = neutralino/chargino) // = 11 : ~q -> q chi // = 12 : q -> ~q chi // = 13 : ~g -> q ~qbar // = 14 : ~q -> q ~g // = 15 : q -> ~q ~g // = 16 : (9/4)*(eikonal) for gg -> ~g ~g // = 30 : Dv -> d qv (Dv= hidden valley fermion, qv= valley scalar) // = 31 : S -> Dv Dvbar (S=scalar color singlet) // Note that the order of the decay products is important. // combi = 1 : pure non-gamma5, i.e. vector/scalar/... // = 2 : pure gamma5, i.e. axial vector/pseudoscalar/.... // = 3 : mixture mix*(combi=1) + (1-mix)*(combi=2) // = 4 : mixture (combi=1) +- (combi=2) double TimeShower::calcMEcorr( int kind, int combiIn, double mixIn, double x1, double x2, double r1, double r2, double r3, bool cutEdge) { // Frequent variable combinations. double x3 = 2. - x1 - x2; double x1s = x1 * x1; double x2s = x2 * x2; double x3s = x3 * x3; double x1c = x1 * x1s; double x2c = x2 * x2s; double x3c = x3 * x3s; double r1s = r1 * r1; double r2s = r2 * r2; double r1c = r1 * r1s; double r2c = r2 * r2s; double r1q = r1s * r1s; double r2q = r2s * r2s; double prop1 = 1. + r1s - r2s - x1; double prop2 = 1. + r2s - r1s - x2; double prop1s = prop1 * prop1; double prop2s = prop2 * prop2; double prop12 = prop1 * prop2; double prop13 = prop1 * x3; double prop23 = prop2 * x3; // Special case: Hidden-Valley massive photon. double r3s = r3 * r3; double prop3 = r3s - x3; double prop3s = prop3 * prop3; if (kind == 30) prop13 = prop1 * prop3; // Check input values. Return zero outside allowed phase space. if (cutEdge) { if (x1 - 2.*r1 < XMARGIN || prop1 < XMARGIN) return 0.; if (x2 - 2.*r2 < XMARGIN || prop2 < XMARGIN) return 0.; // Limits not worked out for r3 > 0. if (kind != 30 && kind != 31) { if (x1 + x2 - 1. - pow2(r1+r2) < XMARGIN) return 0.; // Note: equivalent rewritten form 4. * ( (1. - x1) * (1. - x2) // * (1. - r1s - r2s - x3) + r1s * (1. - x2s - x3) + r2s // * (1. - x1s - x3) - pow2(r1s - r2s) ) gives about same result. if ( (x1s - 4.*r1s) * (x2s - 4.*r2s) - pow2( 2. * (1. - x1 - x2 + r1s + r2s) + x1*x2 ) < XMARGIN * (XMARGINCOMB + r1 + r2) ) return 0.; } } // Initial values; phase space. int combi = max(1, min(4, combiIn) ); double mix = max(0., min(1., mixIn) ); bool isSet1 = false; bool isSet2 = false; bool isSet4 = false; double ps = sqrtpos( pow2(1. - r1*r1 - r2*r2) - pow2(2. * r1 * r2) ); double rLO = 0., rFO = 0., rLO1 = 0., rFO1 = 0., rLO2 = 0., rFO2 = 0., rLO4 = 0., rFO4 = 0.; double offset = 0; // Select which kind of ME to use. switch (kind) { // case 1 is equal to default, i.e. eikonal expression. // V -> q qbar (V = gamma*/Z0/W+-/...). case 2: if (combi == 1 || combi == 3) { rLO1 = ps*(2.-r1s-r1q+6.*r1*r2-r2s+2.*r1s*r2s-r2q)/2.; rFO1 = -(3.+6.*r1s+r1q-6.*r1*r2+6.*r1c*r2-2.*r2s-6.*r1s*r2s +6.*r1*r2c+r2q-3.*x1+6.*r1*r2*x1+2.*r2s*x1+x1s-2.*r1s*x1s +3.*r1s*x3+6.*r1*r2*x3-r2s*x3-2.*x1*x3-5.*r1s*x1*x3 +r2s*x1*x3+x1s*x3-3.*x3s-3.*r1s*x3s+r2s*x3s +2.*x1*x3s+x3c-x2) /prop2s -2.*(-3.+r1s-6.*r1*r2+6.*r1c*r2+3.*r2s-4.*r1s*r2s +6.*r1*r2c+2.*x1+3.*r1s*x1+r2s*x1-x1s-r1s*x1s -r2s*x1s+4.*x3+2.*r1s*x3+3.*r1*r2*x3-r2s*x3-3.*x1*x3 -2.*r1s*x1*x3+x1s*x3-x3s-r1s*x3s+r1*r2*x3s+x1*x3s) /prop12 -(-1.+2.*r1s+r1q+6.*r1*r2+6.*r1c*r2-2.*r2s-6.*r1s*r2s +6.*r1*r2c+r2q-x1-2.*r1s*x1-6.*r1*r2*x1+8.*r2s*x1+x1s -2.*r2s*x1s-r1s*x3+r2s*x3-r1s*x1*x3+r2s*x1*x3+x1s*x3+x2) /prop1s; rFO1 = rFO1/2.; isSet1 = true; } if (combi == 2 || combi == 3) { rLO2 = ps*(2.-r1s-r1q-6.*r1*r2-r2s+2.*r1s*r2s-r2q)/2.; rFO2 = -(3.+6.*r1s+r1q+6.*r1*r2-6.*r1c*r2-2.*r2s-6.*r1s*r2s -6.*r1*r2c+r2q-3.*x1-6.*r1*r2*x1+2.*r2s*x1+x1s-2.*r1s*x1s +3.*r1s*x3-6.*r1*r2*x3-r2s*x3-2.*x1*x3-5.*r1s*x1*x3 +r2s*x1*x3+x1s*x3-3.*x3s-3.*r1s*x3s+r2s*x3s+2.*x1*x3s+x3c-x2) /prop2s -2.*(-3+r1s+6.*r1*r2-6.*r1c*r2+3.*r2s-4.*r1s*r2s-6.*r1*r2c +2.*x1+3.*r1s*x1+r2s*x1-x1s-r1s*x1s-r2s*x1s+4.*x3+2.*r1s*x3 -3.*r1*r2*x3-r2s*x3-3.*x1*x3-2.*r1s*x1*x3+x1s*x3-x3s-r1s*x3s -r1*r2*x3s+x1*x3s) /prop12 -(-1.+2.*r1s+r1q-6.*r1*r2-6.*r1c*r2-2.*r2s-6.*r1s*r2s -6.*r1*r2c+r2q-x1-2.*r1s*x1+6.*r1*r2*x1+8.*r2s*x1+x1s -2.*r2s*x1s-r1s*x3+r2s*x3-r1s*x1*x3+r2s*x1*x3+x1s*x3+x2) /prop1s; rFO2 = rFO2/2.; isSet2 = true; } if (combi == 4) { rLO4 = ps*(2.-r1s-r1q-r2s+2.*r1s*r2s-r2q)/2.; rFO4 = (1.-r1q+6.*r1s*r2s-r2q+x1+3.*r1s*x1-9.*r2s*x1-3.*x1s -r1s*x1s+3.*r2s*x1s+x1c-x2-r1s*x2+r2s*x2-r1s*x1*x2+r2s*x1*x2 +x1s*x2) /prop1s -2.*(1.+r1s+r2s-4.*r1s*r2s+r1s*x1+2.*r2s*x1-x1s-r2s*x1s +2.*r1s*x2+r2s*x2-3.*x1*x2+x1s*x2-x2s-r1s*x2s+x1*x2s) /prop12 +(1.-r1q+6.*r1s*r2s-r2q-x1+r1s*x1-r2s*x1+x2-9.*r1s*x2 +3.*r2s*x2+r1s*x1*x2-r2s*x1*x2-3.*x2s+3.*r1s*x2s-r2s*x2s +x1*x2s+x2c) /prop2s; rFO4 = rFO4/2.; isSet4 = true; } break; // q -> q V. case 3: if (combi == 1 || combi == 3) { rLO1 = ps*(1.-2.*r1s+r1q+r2s-6.*r1*r2s+r1s*r2s-2.*r2q); rFO1 = -2.*(-1.+r1-2.*r1s+2.*r1c-r1q+pow5(r1)-r2s+r1*r2s -5.*r1s*r2s+r1c*r2s-2.*r1*r2q+2.*x1-2.*r1*x1+2.*r1s*x1 -2.*r1c*x1+2.*r2s*x1+5.*r1*r2s*x1+r1s*r2s*x1+2.*r2q*x1 -x1s+r1*x1s-r2s*x1s+3.*x2+4.*r1s*x2+r1q*x2+2.*r2s*x2 +2.*r1s*r2s*x2-4.*x1*x2-2.*r1s*x1*x2-r2s*x1*x2+x1s*x2 -2.*x2s-2.*r1s*x2s+x1*x2s) /prop23 +(2.*r2s+6.*r1*r2s-6.*r1s*r2s+6.*r1c*r2s+2.*r2q+6.*r1*r2q -r2s*x1+r1s*r2s*x1-r2q*x1+x2-r1q*x2-3.*r2s*x2-6.*r1*r2s*x2 +9.*r1s*r2s*x2-2.*r2q*x2-x1*x2+r1s*x1*x2-x2s-3.*r1s*x2s +2.*r2s*x2s+x1*x2s) /prop2s +(-4.-8.*r1s-4.*r1q+4.*r2s-4.*r1s*r2s+8.*r2q+9.*x1+10.*r1s*x1 +r1q*x1-3.*r2s*x1+6.*r1*r2s*x1+r1s*r2s*x1-2.*r2q*x1-6.*x1s- 2.*r1s*x1s+x1c+7.*x2+8.*r1s*x2+r1q*x2-7.*r2s*x2+6.*r1*r2s*x2 +r1s*r2s*x2-2.*r2q*x2-9.*x1*x2-3.*r1s*x1*x2+2.*r2s*x1*x2 +2.*x1s*x2-3.*x2s-r1s*x2s+2.*r2s*x2s+x1*x2s) /x3s; isSet1 = true; } if (combi == 2 || combi == 3) { rLO2 = ps*(1.-2.*r1s+r1q+r2s+6.*r1*r2s+r1s*r2s-2.*r2q); rFO2 = 2*(1.+r1+2.*r1s+2.*r1c+r1q+pow5(r1)+r2s+r1*r2s +5.*r1s*r2s+r1c*r2s-2.*r1*r2q-2.*x1-2.*r1*x1-2.*r1s*x1 -2.*r1c*x1-2.*r2s*x1+5.*r1*r2s*x1-r1s*r2s*x1-2.*r2q*x1+x1s +r1*x1s+r2s*x1s-3.*x2-4.*r1s*x2-r1q*x2-2.*r2s*x2 -2.*r1s*r2s*x2+4.*x1*x2+2.*r1s*x1*x2+r2s*x1*x2-x1s*x2 +2.*x2s+2.*r1s*x2s-x1*x2s) /prop23 +(2.*r2s-6.*r1*r2s-6.*r1s*r2s-6.*r1c*r2s+2.*r2q-6.*r1*r2q -r2s*x1+r1s*r2s*x1-r2q*x1+x2-r1q*x2-3.*r2s*x2+6.*r1*r2s*x2 +9.*r1s*r2s*x2-2.*r2q*x2-x1*x2+r1s*x1*x2-x2s-3.*r1s*x2s +2.*r2s*x2s+x1*x2s) /prop2s +(-4.-8.*r1s-4.*r1q+4.*r2s-4.*r1s*r2s+8.*r2q+9.*x1+10.*r1s*x1 +r1q*x1-3.*r2s*x1-6.*r1*r2s*x1+r1s*r2s*x1-2.*r2q*x1-6.*x1s -2.*r1s*x1s+x1c+7.*x2+8.*r1s*x2+r1q*x2-7.*r2s*x2-6.*r1*r2s*x2 +r1s*r2s*x2-2.*r2q*x2-9.*x1*x2-3.*r1s*x1*x2+2.*r2s*x1*x2 +2.*x1s*x2-3.*x2s-r1s*x2s+2.*r2s*x2s+x1*x2s) /x3s; isSet2 = true; } if (combi == 4) { rLO4 = ps*(1.-2.*r1s+r1q+r2s+r1s*r2s-2.*r2q); rFO4 = 2*(1.+2.*r1s+r1q+r2s+5.*r1s*r2s-2.*x1-2.*r1s*x1 -2.*r2s*x1-r1s*r2s*x1-2.*r2q*x1+x1s+r2s*x1s-3.*x2-4.*r1s*x2 -r1q*x2-2.*r2s*x2-2.*r1s*r2s*x2+4.*x1*x2+2.*r1s*x1*x2+r2s*x1*x2 -x1s*x2+2.*x2s+2.*r1s*x2s-x1*x2s) /prop23 +(2.*r2s-6.*r1s*r2s+2.*r2q-r2s*x1+r1s*r2s*x1-r2q*x1+x2-r1q*x2 -3.*r2s*x2+9.*r1s*r2s*x2-2.*r2q*x2-x1*x2+r1s*x1*x2-x2s-3.*r1s*x2s +2.*r2s*x2s+x1*x2s) /prop2s +(-4.-8.*r1s-4.*r1q+4.*r2s-4.*r1s*r2s+8.*r2q+9.*x1+10.*r1s*x1 +r1q*x1-3.*r2s*x1+r1s*r2s*x1-2.*r2q*x1-6.*x1s-2.*r1s*x1s+x1c +7.*x2+8.*r1s*x2+r1q*x2-7.*r2s*x2+r1s*r2s*x2-2.*r2q*x2-9.*x1*x2 -3.*r1s*x1*x2+2.*r2s*x1*x2+2.*x1s*x2-3.*x2s-r1s*x2s+2.*r2s*x2s +x1*x2s) /x3s; isSet4 = true; } break; // S -> q qbar (S = h0/H0/A0/H+-/...). case 4: if (combi == 1 || combi == 3) { rLO1 = ps*(1.-r1s-r2s-2.*r1*r2); rFO1 = -(-1.+r1q-2.*r1*r2-2.*r1c*r2-6.*r1s*r2s-2.*r1*r2c+r2q+x1 -r1s*x1+2.*r1*r2*x1+3.*r2s*x1+x2+r1s*x2-r2s*x2-x1*x2) /prop1s -2.*(r1s+r1q-2.*r1c*r2+r2s-6.*r1s*r2s-2.*r1*r2c+r2q-r1s*x1 +r1*r2*x1+2.*r2s*x1+2.*r1s*x2+r1*r2*x2-r2s*x2-x1*x2) /prop12 -(-1.+r1q-2.*r1*r2-2.*r1c*r2-6.*r1s*r2s-2.*r1*r2c+r2q+x1-r1s*x1 +r2s*x1+x2+3.*r1s*x2+2.*r1*r2*x2-r2s*x2-x1*x2) /prop2s; isSet1 = true; } if (combi == 2 || combi == 3) { rLO2 = ps*(1.-r1s-r2s+2.*r1*r2); rFO2 = -(-1.+r1q+2.*r1*r2+2.*r1c*r2-6.*r1s*r2s+2.*r1*r2c+r2q+x1 -r1s*x1-2.*r1*r2*x1+3.*r2s*x1+x2+r1s*x2-r2s*x2-x1*x2) /prop1s -(-1.+r1q+2.*r1*r2+2.*r1c*r2-6.*r1s*r2s+2.*r1*r2c+r2q+x1 -r1s*x1+r2s*x1+x2+3.*r1s*x2-2.*r1*r2*x2-r2s*x2-x1*x2) /prop2s +2.*(-r1s-r1q-2.*r1c*r2-r2s+6.*r1s*r2s-2.*r1*r2c-r2q+r1s*x1 +r1*r2*x1-2.*r2s*x1-2.*r1s*x2+r1*r2*x2+r2s*x2+x1*x2) /prop12; isSet2 = true; } if (combi == 4) { rLO4 = ps*(1.-r1s-r2s); rFO4 = -(-1.+r1q-6.*r1s*r2s+r2q+x1-r1s*x1+3.*r2s*x1+x2 +r1s*x2-r2s*x2-x1*x2) /prop1s -2.*(r1s+r1q+r2s-6.*r1s*r2s+r2q-r1s*x1 +2.*r2s*x1+2.*r1s*x2-r2s*x2-x1*x2) /prop12 -(-1.+r1q-6.*r1s*r2s+r2q+x1-r1s*x1+r2s*x1 +x2+3.*r1s*x2-r2s*x2-x1*x2) /prop2s; isSet4 = true; } break; // q -> q S. case 5: if (combi == 1 || combi == 3) { rLO1 = ps*(1.+r1s-r2s+2.*r1); rFO1 = (4.-4.*r1s+4.*r2s-3.*x1-2.*r1*x1+r1s*x1-r2s*x1-5.*x2 -2.*r1*x2+r1s*x2-r2s*x2+x1*x2+x2s) /x3s -2.*(3.-r1-5.*r1s-r1c+3.*r2s+r1*r2s-2.*x1-r1*x1 +r1s*x1-4.*x2+2.*r1s*x2-r2s*x2+x1*x2+x2s) /prop23 +(2.-2.*r1-6.*r1s-2.*r1c+2.*r2s-2.*r1*r2s-x1+r1s*x1 -r2s*x1-3.*x2+2.*r1*x2+3.*r1s*x2-r2s*x2+x1*x2+x2s) /prop2s; isSet1 = true; } if (combi == 2 || combi == 3) { rLO2 = ps*(1.+r1s-r2s-2.*r1); rFO2 = (4.-4.*r1s+4.*r2s-3.*x1+2.*r1*x1+r1s*x1-r2s*x1-5.*x2 +2.*r1*x2+r1s*x2-r2s*x2+x1*x2+x2s) /x3s -2.*(3.+r1-5.*r1s+r1c+3.*r2s-r1*r2s-2.*x1+r1*x1 +r1s*x1-4.*x2+2.*r1s*x2-r2s*x2+x1*x2+x2s) /prop23 +(2.+2.*r1-6.*r1s+2.*r1c+2.*r2s+2.*r1*r2s-x1+r1s*x1 -r2s*x1-3.*x2-2.*r1*x2+3.*r1s*x2-r2s*x2+x1*x2+x2s) /prop2s; isSet2 = true; } if (combi == 4) { rLO4 = ps*(1.+r1s-r2s); rFO4 = (4.-4.*r1s+4.*r2s-3.*x1+r1s*x1-r2s*x1-5.*x2+r1s*x2 -r2s*x2+x1*x2+x2s) /x3s -2.*(3.-5.*r1s+3.*r2s-2.*x1+r1s*x1-4.*x2+2.*r1s*x2 -r2s*x2+x1*x2+x2s) /prop23 +(2.-6.*r1s+2.*r2s-x1+r1s*x1-r2s*x1-3.*x2+3.*r1s*x2 -r2s*x2+x1*x2+x2s) /prop2s; isSet4 = true; } break; // V -> ~q ~qbar (~q = squark). case 6: rLO1 = ps*(1.-2.*r1s+r1q-2.*r2s-2.*r1s*r2s+r2q); rFO1 = 2.*3.+(1.+r1s+r2s-x1)*(4.*r1s-x1s) /prop1s +2.*(-1.-3.*r1s-r2s+x1+x1s*0.5+x2-x1*x2*0.5) /prop1 +(1.+r1s+r2s-x2)*(4.*r2s-x2s) /prop2s +2.*(-1.-r1s-3.*r2s+x1+x2-x1*x2*0.5+x2s*0.5) /prop2 -(-4.*r1s-4.*r1q-4.*r2s-8.*r1s*r2s-4.*r2q+2.*x1+6.*r1s*x1 +6.*r2s*x1-2.*x1s+2.*x2+6.*r1s*x2+6.*r2s*x2-4.*x1*x2 -2.*r1s*x1*x2-2.*r2s*x1*x2+x1s*x2-2.*x2s+x1*x2s) /prop12; isSet1 = true; break; // ~q -> ~q V. case 7: rLO1 = ps*(1.-2.*r1s+r1q-2.*r2s-2.*r1s*r2s+r2q); rFO1 = 16.*r2s-8.*(4.*r2s+2.*r2s*x1+x2+r1s*x2+r2s*x2-x1*x2 -2.*x2s) /(3.*prop2) +8.*(1.+r1s+r2s-x2)*(4.*r2s-x2s) /(3.*prop2s) +8.*(x1+x2)*(-1.-2.*r1s-r1q-2.*r2s+2.*r1s*r2s-r2q+2.*x1 +2.*r1s*x1+2.*r2s*x1-x1s+2.*x2+2.*r1s*x2+2.*r2s*x2-2.*x1*x2-x2s) /(3.*x3s) +8.*(-1.-r1s+r2s-x1)*(2.*r2s*x1+x2+r1s*x2+r2s*x2-x1*x2-x2s) /(3.*prop2*x3) -8.*(1.+2.*r1s+r1q+2.*r2s-2.*r1s*r2s+r2q-2.*x1-2.*r1s*x1 -4.*r2s*x1+x1s-3.*x2-3.*r1s*x2-3.*r2s*x2+3.*x1*x2+2.*x2s) /(3.*x3); rFO1 = 3.*rFO1/8.; isSet1 = true; break; // S -> ~q ~qbar. case 8: rLO1 = ps; rFO1 = (-1.-2.*r1s-r1q-2.*r2s+2.*r1s*r2s-r2q+2.*x1+2.*r1s*x1 +2.*r2s*x1-x1s-r2s*x1s+2.*x2+2.*r1s*x2+2.*r2s*x2-3.*x1*x2 -r1s*x1*x2-r2s*x1*x2+x1s*x2-x2s-r1s*x2s+x1*x2s) /(prop1s*prop2s); rFO1 = 2.*rFO1; isSet1 = true; break; // ~q -> ~q S. case 9: rLO1 = ps; rFO1 = (-1.-r1s-r2s+x2) /prop2s +(1.+r1s-r2s+x1) /prop23 -(x1+x2) /x3s; isSet1 = true; break; // chi -> q ~qbar (chi = neutralino/chargino). case 10: if (combi == 1 || combi == 3) { rLO1 = ps*(1.+r1s-r2s+2.*r1); rFO1 = (2.*r1+x1)*(-1.-r1s-r2s+x1) /prop1s +2.*(-1.-r1s-2.*r1c-r2s-2.*r1*r2s+3.*x1*0.5+r1*x1 -r1s*x1*0.5-r2s*x1*0.5+x2+r1*x2+r1s*x2-x1*x2*0.5) /prop12 +(2.-2.*r1-6.*r1s-2.*r1c+2.*r2s-2.*r1*r2s-x1+r1s*x1 -r2s*x1-3.*x2+2.*r1*x2+3.*r1s*x2-r2s*x2+x1*x2+x2s) /prop2s; isSet1 = true; } if (combi == 2 || combi == 3) { rLO2 = ps*(1.-2.*r1+r1s-r2s); rFO2 = (2.*r1-x1)*(1.+r1s+r2s-x1) /prop1s +2.*(-1.-r1s+2.*r1c-r2s+2.*r1*r2s+3.*x1*0.5-r1*x1 -r1s*x1*0.5-r2s*x1*0.5+x2-r1*x2+r1s*x2-x1*x2*0.5) /prop12 +(2.+2.*r1-6.*r1s+2.*r1c+2.*r2s+2.*r1*r2s-x1+r1s*x1 -r2s*x1-3.*x2-2.*r1*x2+3.*r1s*x2-r2s*x2+x1*x2+x2s)/ prop2s; isSet2 = true; } if (combi == 4) { rLO4 = ps*(1.+r1s-r2s); rFO4 = x1*(-1.-r1s-r2s+x1) /prop1s +2.*(-1.-r1s-r2s+3.*x1*0.5-r1s*x1*0.5-r2s*x1*0.5 +x2+r1s*x2-x1*x2*0.5) /prop12 +(2.-6.*r1s+2.*r2s-x1+r1s*x1-r2s*x1-3.*x2+3.*r1s*x2 -r2s*x2+x1*x2+x2s) /prop2s; isSet4 = true; } break; // ~q -> q chi. case 11: if (combi == 1 || combi == 3) { rLO1 = ps*(1.-pow2(r1+r2)); rFO1 = (1.+r1s+2.*r1*r2+r2s-x1-x2)*(x1+x2) /x3s -(-1.+r1q-2.*r1*r2-2.*r1c*r2-6.*r1s*r2s-2.*r1*r2c+r2q+x1 -r1s*x1+r2s*x1+x2+3.*r1s*x2+2.*r1*r2*x2-r2s*x2-x1*x2) /prop2s +(-1.-2.*r1s-r1q-2.*r1*r2-2.*r1c*r2+2.*r1*r2c+r2q+x1+r1s*x1 -2.*r1*r2*x1-3.*r2s*x1+2.*r1s*x2-2.*r2s*x2+x1*x2+x2s) /prop23; isSet1 = true; } if (combi == 2 || combi == 3) { rLO2 = ps*(1.-pow2(r1-r2)); rFO2 = (1.+r1s-2.*r1*r2+r2s-x1-x2)*(x1+x2) /x3s -(-1.+r1q+2.*r1*r2+2.*r1c*r2-6.*r1s*r2s+2.*r1*r2c+r2q+x1 -r1s*x1+r2s*x1+x2+3.*r1s*x2-2.*r1*r2*x2-r2s*x2-x1*x2) /prop2s +(-1.-2.*r1s-r1q+2.*r1*r2+2.*r1c*r2-2.*r1*r2c+r2q+x1+r1s*x1 +2.*r1*r2*x1-3.*r2s*x1+2.*r1s*x2-2.*r2s*x2+x1*x2+x2s) /prop23; isSet2 = true; } if (combi == 4) { rLO4 = ps*(1.-r1s-r2s); rFO4 = (1.+r1s+r2s-x1-x2)*(x1+x2) /x3s -(-1.+r1q-6.*r1s*r2s+r2q+x1-r1s*x1+r2s*x1+x2 +3.*r1s*x2-r2s*x2-x1*x2) /prop2s +(-1.-2.*r1s-r1q+r2q+x1+r1s*x1-3.*r2s*x1 +2.*r1s*x2-2.*r2s*x2+x1*x2+x2s) /prop23; isSet4 = true; } break; // q -> ~q chi. case 12: if (combi == 1 || combi == 3) { rLO1 = ps*(1.-r1s+r2s+2.*r2); rFO1 = (2.*r2+x2)*(-1.-r1s-r2s+x2) /prop2s +(4.+4.*r1s-4.*r2s-5.*x1-r1s*x1-2.*r2*x1+r2s*x1+x1s -3.*x2-r1s*x2-2.*r2*x2+r2s*x2+x1*x2) /x3s +2.*(-1.-r1s+r2+r1s*r2-r2s-r2c+x1+r2*x1+r2s*x1+2.*x2 +r1s*x2-x1*x2*0.5-x2s*0.5) /prop23; isSet1 = true; } if (combi == 2 || combi == 3) { rLO2 = ps*(1.-r1s+r2s-2.*r2); rFO2 = (2.*r2-x2)*(1.+r1s+r2s-x2) /prop2s +(4.+4.*r1s-4.*r2s-5.*x1-r1s*x1+2.*r2*x1+r2s*x1+x1s -3.*x2-r1s*x2+2.*r2*x2+r2s*x2+x1*x2) /x3s +2.*(-1.-r1s-r2-r1s*r2-r2s+r2c+x1-r2*x1+r2s*x1+2.*x2 +r1s*x2-x1*x2*0.5-x2s*0.5) /prop23; isSet2 = true; } if (combi == 4) { rLO4 = ps*(1.-r1s+r2s); rFO4 = x2*(-1.-r1s-r2s+x2) /prop2s +(4.+4.*r1s-4.*r2s-5.*x1-r1s*x1+r2s*x1+x1s -3.*x2-r1s*x2+r2s*x2+x1*x2) /x3s +2.*(-1.-r1s-r2s+x1+r2s*x1+2.*x2 +r1s*x2-x1*x2*0.5-x2s*0.5) /prop23; isSet4 = true; } break; // ~g -> q ~qbar. case 13: if (combi == 1 || combi == 3) { rLO1 = ps*(1.+r1s-r2s+2.*r1); rFO1 = 4.*(2.*r1+x1)*(-1.-r1s-r2s+x1) /(3.*prop1s) -(-1.-r1s-2.*r1c-r2s-2.*r1*r2s+3.*x1*0.5+r1*x1-r1s*x1*0.5 -r2s*x1*0.5+x2+r1*x2+r1s*x2-x1*x2*0.5) /(3.*prop12) +3.*(-1.+r1-r1s-r1c-r2s+r1*r2s+2.*x1+r2s*x1-x1s*0.5+x2+r1*x2 +r1s*x2-x1*x2*0.5) /prop13 +3.*(4.-4.*r1s+4.*r2s-3.*x1-2.*r1*x1+r1s*x1-r2s*x1-5.*x2 -2.*r1*x2+r1s*x2-r2s*x2+x1*x2+x2s) /x3s -3.*(3.-r1-5.*r1s-r1c+3.*r2s+r1*r2s-2.*x1-r1*x1+r1s*x1 -4.*x2+2.*r1s*x2-r2s*x2+x1*x2+x2s) /prop23 +4.*(2.-2.*r1-6.*r1s-2.*r1c+2.*r2s-2.*r1*r2s-x1+r1s*x1-r2s*x1 -3.*x2+2.*r1*x2+3.*r1s*x2-r2s*x2+x1*x2+x2s) /(3.*prop2s); rFO1 = 3.*rFO1/4.; isSet1 = true; } if (combi == 2 || combi == 3) { rLO2 = ps*(1.+r1s-r2s-2.*r1); rFO2 = 4.*(2.*r1-x1)*(1.+r1s+r2s-x1) /(3.*prop1s) +3.*(-1.-r1-r1s+r1c-r2s-r1*r2s+2.*x1+r2s*x1-x1s*0.5 +x2-r1*x2+r1s*x2-x1*x2*0.5) /prop13 +(2.+2.*r1s-4.*r1c+2.*r2s-4.*r1*r2s-3.*x1+2.*r1*x1 +r1s*x1+r2s*x1-2.*x2+2.*r1*x2-2.*r1s*x2+x1*x2) /(6.*prop12) +3.*(4.-4.*r1s+4.*r2s-3.*x1+2.*r1*x1+r1s*x1-r2s*x1-5.*x2 +2.*r1*x2+r1s*x2-r2s*x2+x1*x2+x2s) /x3s -3.*(3.+r1-5.*r1s+r1c+3.*r2s-r1*r2s-2.*x1+r1*x1+r1s*x1-4.*x2 +2.*r1s*x2-r2s*x2+x1*x2+x2s) /prop23 +4.*(2.+2.*r1-6.*r1s+2.*r1c+2.*r2s+2.*r1*r2s-x1+r1s*x1-r2s*x1 -3.*x2-2.*r1*x2+3.*r1s*x2-r2s*x2+x1*x2+x2s) /(3.*prop2s); rFO2 = 3.*rFO2/4.; isSet2 = true; } if (combi == 4) { rLO4 = ps*(1.+r1s-r2s); rFO4 = 8.*x1*(-1.-r1s-r2s+x1) /(3.*prop1s) +6.*(-1-r1s-r2s+2.*x1+r2s*x1-x1s*0.5+x2+r1s*x2-x1*x2*0.5) /prop13 +(2.+2.*r1s+2.*r2s-3.*x1+r1s*x1+r2s*x1-2.*x2-2.*r1s*x2+x1*x2) /(3.*prop12) +6.*(4.-4.*r1s+4.*r2s-3.*x1+r1s*x1-r2s*x1-5.*x2+r1s*x2-r2s*x2 +x1*x2+x2s) /x3s -6.*(3.-5.*r1s+3.*r2s-2.*x1+r1s*x1-4.*x2+2.*r1s*x2-r2s*x2+x1*x2+x2s) /prop23 +8.*(2.-6.*r1s+2.*r2s-x1+r1s*x1-r2s*x1-3.*x2+3.*r1s*x2-r2s*x2 +x1*x2+x2s) /(3.*prop2s); rFO4 = 3.*rFO4/8.; isSet4 = true; } break; // ~q -> q ~g. case 14: if (combi == 1 || combi == 3) { rLO1 = ps*(1.-r1s-r2s-2.*r1*r2); rFO1 = 64.*(1.+r1s+2.*r1*r2+r2s-x1-x2)*(x1+x2) /(9.*x3s) -16.*(-1.+r1q-2.*r1*r2-2.*r1c*r2-6.*r1s*r2s-2.*r1*r2c+r2q +x1-r1s*x1+2.*r1*r2*x1+3.*r2s*x1+x2+r1s*x2-r2s*x2-x1*x2) /prop1s -16.*(r1s+r1q-2.*r1c*r2+r2s-6.*r1s*r2s-2.*r1*r2c+r2q-r1s*x1 +r1*r2*x1+2.*r2s*x1+2.*r1s*x2+r1*r2*x2-r2s*x2-x1*x2) /prop12 -64.*(-1.+r1q-2.*r1*r2-2.*r1c*r2-6.*r1s*r2s-2.*r1*r2c+r2q+x1 -r1s*x1+r2s*x1+x2+3.*r1s*x2+2.*r1*r2*x2-r2s*x2-x1*x2) /(9.*prop2s) +8.*(-1.+r1q-2.*r1*r2+2.*r1c*r2-2.*r2s-2.*r1*r2c-r2q-2.*r1s*x1 +2.*r2s*x1+x1s+x2-3.*r1s*x2-2.*r1*r2*x2+r2s*x2+x1*x2) /prop13 -8.*(-1.-2.*r1s-r1q-2.*r1*r2-2.*r1c*r2+2.*r1*r2c+r2q+x1+r1s*x1 -2.*r1*r2*x1-3.*r2s*x1+2.*r1s*x2-2.*r2s*x2+x1*x2+x2s) /(9.*prop23); rFO1 = 9.*rFO1/64.; isSet1 = true; } if (combi == 2 || combi == 3) { rLO2 = ps*(1.-r1s-r2s+2.*r1*r2); rFO2 = 64.*(1.+r1s-2.*r1*r2+r2s-x1-x2)*(x1+x2) /(9.*x3s) -16.*(-1.+r1q+2.*r1*r2+2.*r1c*r2-6.*r1s*r2s+2.*r1*r2c+r2q+x1 -r1s*x1-2.*r1*r2*x1+3.*r2s*x1+x2+r1s*x2-r2s*x2-x1*x2) /prop1s -64.*(-1.+r1q+2.*r1*r2+2.*r1c*r2-6.*r1s*r2s+2.*r1*r2c+r2q+x1 -r1s*x1+r2s*x1+x2+3.*r1s*x2-2.*r1*r2*x2-r2s*x2-x1*x2) /(9.*prop2s) +16.*(-r1s-r1q-2.*r1c*r2-r2s+6.*r1s*r2s-2.*r1*r2c-r2q+r1s*x1 +r1*r2*x1-2.*r2s*x1-2.*r1s*x2+r1*r2*x2+r2s*x2+x1*x2) /prop12 +8.*(-1.+r1q+2.*r1*r2-2.*r1c*r2-2.*r2s+2.*r1*r2c-r2q-2.*r1s*x1 +2.*r2s*x1+x1s+x2-3.*r1s*x2+2.*r1*r2*x2+r2s*x2+x1*x2) /prop13 -8.*(-1.-2.*r1s-r1q+2.*r1*r2+2.*r1c*r2-2.*r1*r2c+r2q+x1+r1s*x1+ 2.*r1*r2*x1-3.*r2s*x1+2.*r1s*x2-2.*r2s*x2+x1*x2+x2s) /(9.*prop23); rFO2 = 9.*rFO2/64.; isSet2 = true; } if (combi == 4) { rLO4 = ps*(1.-r1s-r2s); rFO4 = 128.*(1.+r1s+r2s-x1-x2)*(x1+x2) /(9.*x3s) -32*(-1.+r1q-6.*r1s*r2s+r2q+x1-r1s*x1+3.*r2s*x1+x2 +r1s*x2-r2s*x2-x1*x2) /prop1s -32.*(r1s+r1q+r2s-6.*r1s*r2s+r2q-r1s*x1+2.*r2s*x1+2.*r1s*x2 -r2s*x2-x1*x2) /prop12 -128.*(-1.+r1q-6.*r1s*r2s+r2q+x1-r1s*x1+r2s*x1+x2+3.*r1s*x2 -r2s*x2-x1*x2) /(9.*prop2s) +16.*(-1.+r1q-2.*r2s-r2q-2.*r1s*x1+2.*r2s*x1+x1s +x2-3.*r1s*x2+r2s*x2+x1*x2) /prop13 -16.*(-1.-2.*r1s-r1q+r2q+x1+r1s*x1-3.*r2s*x1 +2.*r1s*x2-2.*r2s*x2+x1*x2+x2s) /(9.*prop23); rFO4 = 9.*rFO4/128.; isSet4 = true; } break; // q -> ~q ~g. case 15: if (combi == 1 || combi == 3) { rLO1 = ps*(1.-r1s+r2s+2.*r2); rFO1 = 32*(2.*r2+x2)*(-1.-r1s-r2s+x2) /(9.*prop2s) +8.*(-1.-r1s-2.*r1s*r2-r2s-2.*r2c+x1+r2*x1+r2s*x1 +3.*x2*0.5-r1s*x2*0.5+r2*x2-r2s*x2*0.5-x1*x2*0.5) /prop12 +8.*(2.+2.*r1s-2.*r2-2.*r1s*r2-6.*r2s-2.*r2c-3.*x1-r1s*x1 +2.*r2*x1+3.*r2s*x1+x1s-x2-r1s*x2+r2s*x2+x1*x2) /prop1s +32.*(4.+4.*r1s-4.*r2s-5.*x1-r1s*x1-2.*r2*x1+r2s*x1+x1s -3.*x2-r1s*x2-2.*r2*x2+r2s*x2+x1*x2) /(9.*x3s) -8.*(3.+3.*r1s-r2+r1s*r2-5.*r2s-r2c-4.*x1-r1s*x1 +2.*r2s*x1+x1s-2.*x2-r2*x2+r2s*x2+x1*x2) /prop13 -8.*(-1.-r1s+r2+r1s*r2-r2s-r2c+x1+r2*x1+r2s*x1+2.*x2+r1s*x2 -x1*x2*0.5-x2s*0.5) /(9.*prop23); rFO1 = 9.*rFO1/32.; isSet1 = true; } if (combi == 2 || combi == 3) { rLO2 = ps*(1.-r1s+r2s-2.*r2); rFO2 = 32*(2.*r2-x2)*(1.+r1s+r2s-x2) /(9.*prop2s) +8.*(-1.-r1s+2.*r1s*r2-r2s+2.*r2c+x1-r2*x1+r2s*x1 +3.*x2*0.5-r1s*x2*0.5-r2*x2-r2s*x2*0.5-x1*x2*0.5) /prop12 +8.*(2.+2.*r1s+2.*r2+2.*r1s*r2-6.*r2s+2.*r2c-3.*x1-r1s*x1 -2.*r2*x1+3.*r2s*x1+x1s-x2-r1s*x2+r2s*x2+x1*x2) /prop1s -8.*(3.+3.*r1s+r2-r1s*r2-5.*r2s+r2c-4.*x1-r1s*x1+2.*r2s*x1+x1s -2.*x2+r2*x2+r2s*x2+x1*x2) /prop13 +32*(4.+4.*r1s-4.*r2s-5.*x1-r1s*x1+2.*r2*x1+r2s*x1 +x1s-3.*x2-r1s*x2+2.*r2*x2+r2s*x2+x1*x2) /(9.*x3s) -8.*(-1.-r1s-r2-r1s*r2-r2s+r2c+x1-r2*x1+r2s*x1+2.*x2+r1s*x2 -x1*x2*0.5-x2s*0.5) /(9.*prop23); rFO2 = 9.*rFO2/32.; isSet2 = true; } if (combi == 4) { rLO4 = ps*(1.-r1s+r2s); rFO4 = 64.*x2*(-1.-r1s-r2s+x2) /(9.*prop2s) +16.*(-1.-r1s-r2s+x1+r2s*x1+3.*x2*0.5-r1s*x2*0.5 -r2s*x2*0.5-x1*x2*0.5) /prop12 -16.*(3.+3.*r1s-5.*r2s-4.*x1-r1s*x1+2.*r2s*x1+x1s-2.*x2+r2s*x2 +x1*x2) /prop13 +64.*(4.+4.*r1s-4.*r2s-5.*x1-r1s*x1+r2s*x1+x1s-3.*x2 -r1s*x2+r2s*x2+x1*x2) /(9.*x3s) +16.*(2.+2.*r1s-6.*r2s-3.*x1-r1s*x1+3.*r2s*x1+x1s -x2-r1s*x2+r2s*x2+x1*x2) /prop1s -16.*(-1.-r1s-r2s+x1+r2s*x1+2.*x2+r1s*x2-x1*x2*0.5-x2s*0.5) /(9.*prop23); rFO4 = 9.*rFO4/64.; isSet4 = true; } break; // g -> ~g ~g. Use (9/4)*eikonal. May be changed in the future. case 16: rLO = ps; if (combi == 2) offset = x3s; else if (combi == 3) offset = mix * x3s; else if (combi == 4) offset = 0.5 * x3s; rFO = ps * 4.5 * ( (x1+x2-1.+offset-r1s-r2s)/prop12 - r1s/prop2s - r2s/prop1s ); break; // Dv -> qv d. case 30: rLO = ps*(1.-r1s+r2s+2.*r2); rFO = ( 0.5*r3s + 2.*r1q + 0.5*r2s*r3s + r2*r3s - 2.*r1s - 0.5*r1s*r3s - 2.*r1s*r2s - 4.*r1s*r2 ) / prop2s + ( -2. + 2.*r2q + 2.*r1q + 2.*r2s*r3s - 4.*r2 + 2.*r2*r3s + 4.*r2*r2s - 4.*r1s*r2s - 4.*r1s*r2 ) /prop23 + ( -2. - 0.5*r3s - 2.*r2s - 4.*r2 + 2.*r1s ) / prop2 + ( -2. - r3s - 2.*r2s - r2s*r3s - 4.*r2 - 2.*r2*r3s + 2.*r1s + r1s*r3s ) / prop3s + ( -1. - r3s - r2s - 4.*r2 + r1s - x2 ) / prop3 + 1.; break; // S -> Dv Dvbar case 31: rLO = ps*(1.-4.*r1s); rFO = (r3s + 2.*r1s) * (-1. + 4.*r1s) * (1./prop1s + 1./prop2s) + (-1. + 8.*r1s - x2) / prop1 + (-1. + 8.*r1s - x1) / prop2 + 2. * (1. - 6.*r1s + 8.*r1q + 4.*r3s*r1s) / prop12 + 2.; break; // q -> q~ W case 32: rLO = 1.; rFO = (2. * r3s * r3s + 2. * r3s * (x1 + x2) + x1s + x2s) / prop12 - r3s / prop1s - r3s / prop2s; break; // q -> q Z case 33: rLO = 1.; rFO = (2. * r3s * r3s + 2. * r3s * (x1 + x2) + x1s + x2s) / prop12 - r3s / prop1s - r3s / prop2s; break; // Eikonal expression for kind == 1; also acts as default. default: rLO = ps; if (combi == 2) offset = x3s; else if (combi == 3) offset = mix * x3s; else if (combi == 4) offset = 0.5 * x3s; rFO = ps * 2. * ( (x1+x2-1.+offset-r1s-r2s)/prop12 - r1s/prop2s - r2s/prop1s ); break; // End of ME cases. } // Find relevant leading and first order expressions. if (combi == 1 && isSet1) { rLO = rLO1; rFO = rFO1; } else if (combi == 2 && isSet2) { rLO = rLO2; rFO = rFO2; } else if (combi == 3 && isSet1 && isSet2) { rLO = mix * rLO1 + (1.-mix) * rLO2; rFO = mix * rFO1 + (1.-mix) * rFO2; } else if (isSet4) { rLO = rLO4; rFO = rFO4; } else if (combi == 4 && isSet1 && isSet2) { rLO = 0.5 * (rLO1 + rLO2); rFO = 0.5 * (rFO1 + rFO2); } else if (isSet1) { rLO = rLO1; rFO = rFO1; } // Return ratio of first to leading order cross section. return rFO / rLO; } //-------------------------------------------------------------------------- // Find coefficient of azimuthal asymmetry from gluon polarization. void TimeShower::findAsymPol( Event& event, TimeDipoleEnd* dip) { // Default is no asymmetry. Only gluons are studied. dip->asymPol = 0.; dip->iAunt = 0; int iRad = dip->iRadiator; if (!doPhiPolAsym || event[iRad].id() != 21) return; // Trace grandmother via possibly intermediate recoil copies. int iMother = event.iTopCopy(iRad); int iGrandM = event[iMother].mother1(); // If grandmother in initial state of hard scattering, // then only keep gg and qq initial states. int statusGrandM = event[iGrandM].status(); bool isHardProc = (statusGrandM == -21 || statusGrandM == -31); if (isHardProc) { if (event[iGrandM + 1].status() != statusGrandM) return; if (event[iGrandM].isGluon() && event[iGrandM + 1].isGluon()); else if (event[iGrandM].isQuark() && event[iGrandM + 1].isQuark()); else return; } // Set aunt by history or, for hard scattering, by colour flow. if (isHardProc) dip->iAunt = dip->iRecoiler; else dip->iAunt = (event[iGrandM].daughter1() == iMother) ? event[iGrandM].daughter2() : event[iGrandM].daughter1(); // Coefficient from gluon production (approximate z by energy). // For hard process arbitrarily put z = 1/2. double zProd = (isHardProc) ? 0.5 : event[iRad].e() / (event[iRad].e() + event[dip->iAunt].e()); if (event[iGrandM].isGluon()) dip->asymPol = pow2( (1. - zProd) / (1. - zProd * (1. - zProd) ) ); else dip->asymPol = 2. * (1. - zProd) / (1. + pow2(1. - zProd) ); // Coefficients from gluon decay. if (dip->flavour == 21) dip->asymPol *= pow2( (1. - dip->z) / (1. - dip->z * (1. - dip->z) ) ); else dip->asymPol *= -2. * dip->z *( 1. - dip->z ) / (1. - 2. * dip->z * (1. - dip->z) ); } //-------------------------------------------------------------------------- // Print the list of dipoles. void TimeShower::list(ostream& os) const { // Header. os << "\n -------- PYTHIA TimeShower Dipole Listing ----------------" << "------------------------------------------------------- \n \n " << " i rad rec pTmax col chg gam weak oni hv is" << "r sys sysR type MErec mix ord spl ~gR pol \n" << fixed << setprecision(3); // Loop over dipole list and print it. for (int i = 0; i < int(dipEnd.size()); ++i) os << setw(5) << i << setw(7) << dipEnd[i].iRadiator << setw(7) << dipEnd[i].iRecoiler << setw(12) << dipEnd[i].pTmax << setw(5) << dipEnd[i].colType << setw(5) << dipEnd[i].chgType << setw(5) << dipEnd[i].gamType << setw(5) << dipEnd[i].weakType << setw(5) << dipEnd[i].isOctetOnium << setw(5) << dipEnd[i].isHiddenValley << setw(5) << dipEnd[i].isrType << setw(5) << dipEnd[i].system << setw(5) << dipEnd[i].systemRec << setw(5) << dipEnd[i].MEtype << setw(7) << dipEnd[i].iMEpartner << setw(8) << dipEnd[i].MEmix << setw(5) << dipEnd[i].MEorder << setw(5) << dipEnd[i].MEsplit << setw(5) << dipEnd[i].MEgluinoRec << setw(5) << dipEnd[i].weakPol << "\n"; // Done. os << "\n -------- End PYTHIA TimeShower Dipole Listing ------------" << "-------------------------------------------------------" << endl; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/ResonanceDecays.cc0000644000175000017500000007533712217346247016524 0ustar sunsun// ResonanceDecays.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for // the ResonanceDecays class. #include "Pythia8/ResonanceDecays.h" namespace Pythia8 { //========================================================================== // The ResonanceDecays class. // Do all resonance decays sequentially. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of tries to pick a decay channel. const int ResonanceDecays::NTRYCHANNEL = 10; // Number of tries to pick a set of daughter masses. const int ResonanceDecays::NTRYMASSES = 10000; // Mass above threshold for allowed decays. const double ResonanceDecays::MSAFETY = 0.1; // When constrainted kinematics cut high-mass tail of Breit-Wigner. const double ResonanceDecays::WIDTHCUT = 5.; // Small number (relative to 1) to protect against roundoff errors. const double ResonanceDecays::TINY = 1e-10; // Forbid small Breit-Wigner mass range, as mapped onto atan range. const double ResonanceDecays::TINYBWRANGE = 1e-8; // These numbers are hardwired empirical parameters, // intended to speed up the M-generator. const double ResonanceDecays::WTCORRECTION[11] = { 1., 1., 1., 2., 5., 15., 60., 250., 1250., 7000., 50000. }; //-------------------------------------------------------------------------- bool ResonanceDecays::next( Event& process, int iDecNow) { // Loop over all entries to find resonances that should decay. // (Except for iDecNow > 0, where only it will be handled.) int iDec = iDecNow; do { Particle& decayer = process[iDec]; if (decayer.isFinal() && decayer.canDecay() && decayer.mayDecay() && decayer.isResonance() ) { // Fill the decaying particle in slot 0 of arrays. id0 = decayer.id(); m0 = decayer.m(); idProd.resize(0); mProd.resize(0); idProd.push_back( id0 ); mProd.push_back( m0 ); // Mother flavour - relevant for gamma*/Z0 mixing. (Not always??) int idIn = process[decayer.mother1()].id(); // Prepare decay selection. if (!decayer.particleDataEntry().preparePick(id0, m0, idIn)) { ostringstream osWarn; osWarn << "for id = " << id0; infoPtr->errorMsg("Error in ResonanceDecays::next:" " no open decay channel", osWarn.str()); return false; } // Pick a decay channel; allow up to ten tries. bool foundChannel = false; for (int iTryChannel = 0; iTryChannel < NTRYCHANNEL; ++iTryChannel) { // Pick decay channel. Find multiplicity. DecayChannel& channel = decayer.particleDataEntry().pickChannel(); mult = channel.multiplicity(); // Read out flavours. idProd.resize(1); int idNow; for (int i = 1; i <= mult; ++i) { idNow = channel.product(i - 1); if (id0 < 0 && particleDataPtr->hasAnti(idNow)) idNow = -idNow; idProd.push_back( idNow); } // Pick masses. Pick new channel if fail. if (!pickMasses()) continue; foundChannel = true; break; } // Failed to find acceptable decays. if (!foundChannel) { ostringstream osWarn; osWarn << "for id = " << id0; infoPtr->errorMsg("Error in ResonanceDecays::next:" " failed to find workable decay channel", osWarn.str()); return false; } // Select colours in decay. if (!pickColours(iDec, process)) return false; // Select four-momenta in decay, boosted to lab frame. pProd.resize(0); pProd.push_back( decayer.p() ); if (!pickKinematics()) return false; // Append decay products to the process event record. Set lifetimes. int iFirst = process.size(); for (int i = 1; i <= mult; ++i) { process.append( idProd[i], 23, iDec, 0, 0, 0, cols[i], acols[i], pProd[i], mProd[i], m0); } int iLast = process.size() - 1; // Set decay vertex when this is displaced. if (process[iDec].hasVertex() || process[iDec].tau() > 0.) { Vec4 vDec = process[iDec].vDec(); for (int i = iFirst; i <= iLast; ++i) process[i].vProd( vDec ); } // Set lifetime of daughters. for (int i = iFirst; i <= iLast; ++i) process[i].tau( process[i].tau0() * rndmPtr->exp() ); // Modify mother status and daughters. decayer.status(-22); decayer.daughters(iFirst, iLast); // End of loop over all entries. } } while (iDecNow == 0 && ++iDec < process.size()); // Done. return true; } //-------------------------------------------------------------------------- // Select masses of decay products. bool ResonanceDecays::pickMasses() { // Arrays with properties of particles. Fill with dummy values for mother. vector useBW; vector m0BW, mMinBW, mMaxBW, widthBW; double mMother = mProd[0]; double m2Mother = mMother * mMother; useBW.push_back( false ); m0BW.push_back( mMother ); mMinBW.push_back( mMother ); mMaxBW.push_back( mMother ); widthBW.push_back( 0. ); // Loop throught products for masses and widths. Set nominal mass. bool useBWNow; double m0Now, mMinNow, mMaxNow, widthNow; for (int i = 1; i <= mult; ++i) { useBWNow = particleDataPtr->useBreitWigner( idProd[i] ); m0Now = particleDataPtr->m0( idProd[i] ); mMinNow = particleDataPtr->m0Min( idProd[i] ); mMaxNow = particleDataPtr->m0Max( idProd[i] ); if (useBWNow && mMaxNow < mMinNow) mMaxNow = mMother; widthNow = particleDataPtr->mWidth( idProd[i] ); useBW.push_back( useBWNow ); m0BW.push_back( m0Now ); mMinBW.push_back( mMinNow ); mMaxBW.push_back( mMaxNow ); widthBW.push_back( widthNow ); mProd.push_back( m0Now ); } // Find number of Breit-Wigners and summed (minimal) masses. int nBW = 0; double mSum = 0.; double mSumMin = 0.; for (int i = 1; i <= mult; ++i) { if (useBW[i]) ++nBW; mSum += max( m0BW[i], mMinBW[i]); mSumMin += mMinBW[i]; } // If sum of minimal masses above mother mass then give up. if (mSumMin + MSAFETY > mMother) return false; // If sum of masses below and no Breit-Wigners then done. if (mSum + 0.5 * MSAFETY < mMother && nBW == 0) return true; // Else if below then retry Breit-Wigners, with simple treshold. if (mSum + MSAFETY < mMother) { double wtMax = 2. * sqrtpos(1. - mSum*mSum / m2Mother); double wt; for (int iTryMasses = 0; iTryMasses <= NTRYMASSES; ++ iTryMasses) { if (iTryMasses == NTRYMASSES) return false; mSum = 0.; for (int i = 1; i <= mult; ++i) { if (useBW[i]) mProd[i] = particleDataPtr->mSel( idProd[i] ); mSum += mProd[i]; } wt = (mSum + 0.5 * MSAFETY < mMother) ? sqrtpos(1. - mSum*mSum / m2Mother) : 0.; if (wt > rndmPtr->flat() * wtMax) break; } return true; } // From now on some particles will have to be forced off shell. // Order Breit-Wigners in decreasing widths. Sum of other masses. vector iBW; double mSum0 = 0.; for (int i = 1; i <= mult; ++i) { if (useBW[i]) iBW.push_back(i); else mSum0 += mProd[i]; } for (int i = 1; i < nBW; ++i) { for (int j = i - 1; j >= 0; --j) { if (widthBW[iBW[j+1]] > widthBW[iBW[j]]) swap (iBW[j+1], iBW[j]); else break; } } // Do all but broadest two in increasing-width order. Includes only one. if (nBW != 2) { int iMin = (nBW == 1) ? 0 : 2; for (int i = nBW - 1; i >= iMin; --i) { int iBWi = iBW[i]; // Find allowed mass range of current resonance. double mMax = mMother - mSum0 - MSAFETY; if (nBW != 1) for (int j = 0; j < i; ++j) mMax -= mMinBW[iBW[j]]; mMax = min( mMaxBW[iBWi], mMax ); double mMin = min( mMinBW[iBWi], mMax - MSAFETY); if (mMin < 0.) return false; // Parameters for Breit-Wigner choice, with constrained mass range. double m2Nom = pow2( m0BW[iBWi] ); double m2Max = mMax * mMax; double m2Min = mMin * mMin; double mmWid = m0BW[iBWi] * widthBW[iBWi]; double atanMin = atan( (m2Min - m2Nom) / mmWid ); double atanMax = atan( (m2Max - m2Nom) / mmWid ); double atanDif = atanMax - atanMin; // Fail if too narrow mass range; e.g. out in tail of Breit-Wigner. if (atanDif < TINYBWRANGE) return false; // Retry mass according to Breit-Wigner, with simple threshold factor. double mr1 = mSum0*mSum0 / m2Mother; double mr2 = m2Min / m2Mother; double wtMax = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2 ); double m2Now, wt; for (int iTryMasses = 0; iTryMasses <= NTRYMASSES; ++ iTryMasses) { if (iTryMasses == NTRYMASSES) return false; m2Now = m2Nom + mmWid * tan(atanMin + rndmPtr->flat() * atanDif); mr2 = m2Now / m2Mother; wt = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2 ); if (wt > rndmPtr->flat() * wtMax) break; } // Prepare to iterate for more. Done for one Breit-Wigner. mProd[iBWi] = sqrt(m2Now); mSum0 += mProd[iBWi]; } if (nBW == 1) return true; } // Left to do two broadest Breit-Wigners correlated, i.e. more realistic. int iBW1 = iBW[0]; int iBW2 = iBW[1]; int idMother = abs(idProd[0]); int idDau1 = abs(idProd[iBW1]); int idDau2 = abs(idProd[iBW2]); // In some cases known phase-space behaviour; else simple beta factor. int psMode = 1 ; if ( (idMother == 25 || idMother == 35) && idDau1 < 19 && idDau2 == idDau1 ) psMode = 3; if ( (idMother == 25 || idMother == 35 ) && (idDau1 == 23 || idDau1 == 24) && idDau2 == idDau1 ) psMode = 5; if ( idMother == 36 && (idDau1 == 23 || idDau1 == 24) && idDau2 == idDau1 ) psMode = 6; // Find allowed mass ranges. Ensure that they are not closed. double mRem = mMother - mSum0 - MSAFETY; double mMax1 = min( mMaxBW[iBW1], mRem - mMinBW[iBW2] ); double mMin1 = min( mMinBW[iBW1], mMax1 - MSAFETY); double mMax2 = min( mMaxBW[iBW2], mRem - mMinBW[iBW1] ); double mMin2 = min( mMinBW[iBW2], mMax2 - MSAFETY); // At least one range must extend below half remaining mass. if (mMin1 + mMin2 > mRem) return false; double mMid = 0.5 * mRem; bool hasMid1 = (mMin1 < mMid); bool hasMid2 = (mMin2 < mMid); if (!hasMid1 && !hasMid2) return false; // Parameters for Breit-Wigner choice, with constrained mass range. double m2Nom1 = pow2( m0BW[iBW1] ); double m2Max1 = mMax1 * mMax1; double m2Min1 = mMin1 * mMin1; double m2Mid1 = min( mMid * mMid, m2Max1); double mmWid1 = m0BW[iBW1] * widthBW[iBW1]; double atanMin1 = atan( (m2Min1 - m2Nom1) / mmWid1 ); double atanMax1 = atan( (m2Max1 - m2Nom1) / mmWid1 ); double atanMid1 = (hasMid1) ? atan( (m2Mid1 - m2Nom1) / mmWid1 ) : 0.; double m2Nom2 = pow2( m0BW[iBW2] ); double m2Max2 = mMax2 * mMax2; double m2Min2 = mMin2 * mMin2; double m2Mid2 = min( mMid * mMid, m2Max2); double mmWid2 = m0BW[iBW2] * widthBW[iBW2]; double atanMin2 = atan( (m2Min2 - m2Nom2) / mmWid2 ); double atanMax2 = atan( (m2Max2 - m2Nom2) / mmWid2 ); double atanMid2 = (hasMid2) ? atan( (m2Mid2 - m2Nom2) / mmWid2 ) : 0.; // Relative weight to pick either below half remaining mass. double probLow1 = (hasMid1) ? 1. : 0.; if (hasMid1 && hasMid2) { double intLow1 = (atanMid1 - atanMin1) * (atanMax2 - atanMin2); double intLow2 = (atanMax1 - atanMin1) * (atanMid2 - atanMin2); probLow1 = intLow1 / (intLow1 + intLow2); } // Maximum matrix element times phase space weight. double m2Rem = mRem * mRem; double mr1 = m2Min1 / m2Rem; double mr2 = m2Min2 / m2Rem; double psMax = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2 ); double wtMax = 1.; if (psMode == 1) wtMax = psMax; else if (psMode == 2) wtMax = psMax * psMax; else if (psMode == 3) wtMax = pow3(psMax); else if (psMode == 5) wtMax = psMax * (pow2(1. - mr1 - mr2) + 8. * mr1 * mr2); else if (psMode == 6) wtMax = pow3(psMax); // Retry mass according to Breit-Wigners, with simple threshold factor. double atanDif1, atanDif2, m2Now1, m2Now2, mNow1, mNow2, ps, wt; for (int iTryMasses = 0; iTryMasses <= NTRYMASSES; ++ iTryMasses) { if (iTryMasses == NTRYMASSES) return false; // Pick either below half remaining mass. bool pickLow1 = false; if (rndmPtr->flat() < probLow1) { atanDif1 = atanMid1 - atanMin1; atanDif2 = atanMax2 - atanMin2; pickLow1 = true; } else { atanDif1 = atanMax1 - atanMin1; atanDif2 = atanMid2 - atanMin2; } m2Now1 = m2Nom1 + mmWid1 * tan(atanMin1 + rndmPtr->flat() * atanDif1); m2Now2 = m2Nom2 + mmWid2 * tan(atanMin2 + rndmPtr->flat() * atanDif2); mNow1 = sqrt(m2Now1); mNow2 = sqrt(m2Now2); // Check that intended mass ordering is fulfilled. bool rejectRegion = (pickLow1) ? (mNow1 > mNow2) : (mNow2 > mNow1); if (rejectRegion) continue; // Threshold weight. mr1 = m2Now1 / m2Rem; mr2 = m2Now2 / m2Rem; wt = 0.; if (mNow1 + mNow2 + MSAFETY < mMother) { ps = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2 ); wt = 1.; if (psMode == 1) wt = ps; else if (psMode == 2) wt = ps * ps; else if (psMode == 3) wt = pow3(ps); else if (psMode == 5) wt = ps * (pow2(1. - mr1 - mr2) + 8. * mr1 * mr2); else if (psMode == 6) wt = pow3(ps)*mr1*mr2; } if (wt > rndmPtr->flat() * wtMax) break; } mProd[iBW1] = mNow1; mProd[iBW2] = mNow2; // Done. return true; } //-------------------------------------------------------------------------- // Select colours of decay products. bool ResonanceDecays::pickColours(int iDec, Event& process) { // Reset or create arrays with colour info. cols.resize(0); acols.resize(0); vector iTriplet, iAtriplet, iOctet, iDipCol, iDipAcol; // Mother colours already known. int col0 = process[iDec].col(); int acol0 = process[iDec].acol(); int colType0 = process[iDec].colType(); cols.push_back( col0); acols.push_back(acol0); // Loop through all daughters. int colTypeNow; for (int i = 1; i <= mult; ++i) { // Daughter colours initially empty, so that all is set for singlet. cols.push_back(0); acols.push_back(0); // Find character (singlet, triplet, antitriplet, octet) of daughters. colTypeNow = particleDataPtr->colType( idProd[i] ); if (colTypeNow == 0); else if (colTypeNow == 1) iTriplet.push_back(i); else if (colTypeNow == -1) iAtriplet.push_back(i); else if (colTypeNow == 2) iOctet.push_back(i); // Add two entries for sextets; else if (colTypeNow == 3) { iTriplet.push_back(i); iTriplet.push_back(i); } else if (colTypeNow == -3) { iAtriplet.push_back(i); iAtriplet.push_back(i); } else { infoPtr->errorMsg("Error in ResonanceDecays::pickColours:" " unknown colour type encountered"); return false; } } // Check excess of colours and anticolours in final over initial state. int nCol = iTriplet.size(); if (colType0 == 1 || colType0 == 2) nCol -= 1; else if (colType0 == 3) nCol -= 2; int nAcol = iAtriplet.size(); if (colType0 == -1 || colType0 == 2) nAcol -= 1; else if (colType0 == -3) nAcol -= 2; // If net creation of three colours then find junction kind: // mother is 1 = singlet, triplet, or sextet (no incoming RPV tags) // 3 = antitriplet, octet, or antisextet (acol0 = incoming RPV tag) // 5 = not applicable to decays (needs two incoming RPV tags) if (nCol - nAcol == 3) { int kindJun = (colType0 == 0 || colType0 == 1 || colType0 == 3) ? 1 : 3; // Set colours in three junction legs and store junction. int colJun[3]; colJun[0] = (kindJun == 1) ? process.nextColTag() : acol0; colJun[1] = process.nextColTag(); colJun[2] = process.nextColTag(); process.appendJunction( kindJun, colJun[0], colJun[1], colJun[2]); // Loop over three legs. Remove an incoming anticolour on first leg. for (int leg = 0; leg < 3; ++leg) { if (leg == 0 && kindJun != 1) acol0 = 0; // Pick final-state triplets to carry these new colours. else { int pickT = (iTriplet.size() == 1) ? 0 : int( TINY + rndmPtr->flat() * (iTriplet.size() - TINY) ); int iPickT = iTriplet[pickT]; cols[iPickT] = colJun[leg]; // Remove matched triplet and store new colour dipole ends. iTriplet[pickT] = iTriplet.back(); iTriplet.pop_back(); iDipCol.push_back(iPickT); iDipAcol.push_back(0); } } // Update colour counter. Done with junction. nCol -= 3; } // If net creation of three anticolours then find antijunction kind: // mother is 2 = singlet, antitriplet, or antisextet (no incoming RPV tags) // 4 = triplet, octet, or sextet (col0 = incoming RPV tag) // 6 = not applicable to decays (needs two incoming RPV tags) if (nAcol - nCol == 3) { int kindJun = (colType0 == 0 || colType0 == -1 || colType0 == -3) ? 2 : 4; // Set anticolours in three antijunction legs and store antijunction. int acolJun[3]; acolJun[0] = (kindJun == 2) ? process.nextColTag() : col0; acolJun[1] = process.nextColTag(); acolJun[2] = process.nextColTag(); process.appendJunction( kindJun, acolJun[0], acolJun[1], acolJun[2]); // Loop over three legs. Remove an incoming colour on first leg. for (int leg = 0; leg < 3; ++leg) { if (leg == 0 && kindJun != 2) col0 = 0; // Pick final-state antitriplets to carry these new anticolours. else { int pickA = (iAtriplet.size() == 1) ? 0 : int( TINY + rndmPtr->flat() * (iAtriplet.size() - TINY) ); int iPickA = iAtriplet[pickA]; acols[iPickA] = acolJun[leg]; // Remove matched antitriplet and store new colour dipole ends. iAtriplet[pickA] = iAtriplet.back(); iAtriplet.pop_back(); iDipCol.push_back(0); iDipAcol.push_back(iPickA); } } // Update anticolour counter. Done with antijunction. nAcol -= 3; } // If colours and anticolours do not match now then unphysical. if (nCol != nAcol) { infoPtr->errorMsg("Error in ResonanceDecays::pickColours:" " inconsistent colour tags"); return false; } // Pick final-state triplet (if any) to carry initial colour. if (col0 > 0 && iTriplet.size() > 0) { int pickT = (iTriplet.size() == 1) ? 0 : int( TINY + rndmPtr->flat() * (iTriplet.size() - TINY) ); int iPickT = iTriplet[pickT]; cols[iPickT] = col0; // Remove matched triplet and store new colour dipole ends. col0 = 0; iTriplet[pickT] = iTriplet.back(); iTriplet.pop_back(); iDipCol.push_back(iPickT); iDipAcol.push_back(0); } // Pick final-state antitriplet (if any) to carry initial anticolour. if (acol0 > 0 && iAtriplet.size() > 0) { int pickA = (iAtriplet.size() == 1) ? 0 : int( TINY + rndmPtr->flat() * (iAtriplet.size() - TINY) ); int iPickA = iAtriplet[pickA]; acols[iPickA] = acol0; // Remove matched antitriplet and store new colour dipole ends. acol0 = 0; iAtriplet[pickA] = iAtriplet.back(); iAtriplet.pop_back(); iDipCol.push_back(0); iDipAcol.push_back(iPickA); } // Sextets: second final-state triplet (if any) if (acol0 < 0 && iTriplet.size() > 0) { int pickT = (iTriplet.size() == 1) ? 0 : int( TINY + rndmPtr->flat() * (iTriplet.size() - TINY) ); int iPickT = iTriplet[pickT]; cols[iPickT] = -acol0; // Remove matched antitriplet and store new colour dipole ends. acol0 = 0; iTriplet[pickT] = iTriplet.back(); iTriplet.pop_back(); iDipCol.push_back(iPickT); iDipAcol.push_back(0); } // Sextets: second final-state antitriplet (if any) if (col0 < 0 && iAtriplet.size() > 0) { int pickA = (iAtriplet.size() == 1) ? 0 : int( TINY + rndmPtr->flat() * (iAtriplet.size() - TINY) ); int iPickA = iAtriplet[pickA]; acols[iPickA] = -col0; // Remove matched triplet and store new colour dipole ends. col0 = 0; iAtriplet[pickA] = iAtriplet.back(); iAtriplet.pop_back(); iDipCol.push_back(0); iDipAcol.push_back(iPickA); } // Error checks that amount of leftover colours and anticolours match. if ( (iTriplet.size() != iAtriplet.size()) || (col0 != 0 && acol0 == 0) || (col0 == 0 && acol0 != 0) ) { infoPtr->errorMsg("Error in ResonanceDecays::pickColours:" " inconsistent colour tags"); return false; } // Match triplets to antitriplets in the final state. for (int pickT = 0; pickT < int(iTriplet.size()); ++pickT) { int iPickT = iTriplet[pickT]; int pickA = (iAtriplet.size() == 1) ? 0 : int( TINY + rndmPtr->flat() * (iAtriplet.size() - TINY) ); int iPickA = iAtriplet[pickA]; // Connect pair with new colour tag. cols[iPickT] = process.nextColTag(); acols[iPickA] = cols[iPickT]; // Remove matched antitriplet and store new colour dipole ends. iAtriplet[pickT] = iAtriplet.back(); iAtriplet.pop_back(); iDipCol.push_back(iPickT); iDipAcol.push_back(iPickA); } // If no octets are around then matching is done. if (col0 == 0 && acol0 == 0 && iOctet.size() == 0) return true; // If initial-state octet remains then store as (first!) new dipole. if (col0 != 0) { iDipCol.push_back(0); iDipAcol.push_back(0); } // Now attach all final-state octets at random to existing dipoles. for (int i = 0; i < int(iOctet.size()); ++i) { int iOct = iOctet[i]; // If no dipole then start new one. (Happens for singlet -> octets.) if (iDipCol.size() == 0) { cols[iOct] = process.nextColTag(); acols[iOct] = cols[iOct] ; iDipCol.push_back(iOct); iDipAcol.push_back(iOct); } // Else attach to existing dipole picked at random. else { int pickDip = (iDipCol.size() == 1) ? 0 : int( TINY + rndmPtr->flat() * (iDipCol.size() - TINY) ); // Case with dipole in initial state: reattach existing colours. if (iDipCol[pickDip] == 0 && iDipAcol[pickDip] == 0) { cols[iOct] = col0; acols[iOct] = acol0; iDipAcol[pickDip] = iOct; iDipCol.push_back(iOct); iDipAcol.push_back(0); // Case with dipole from colour in initial state: also new colour. } else if (iDipAcol[pickDip] == 0) { int iPickCol = iDipCol[pickDip]; cols[iOct] = cols[iPickCol]; acols[iOct] = process.nextColTag(); cols[iPickCol] = acols[iOct]; iDipCol[pickDip] = iOct; iDipCol.push_back(iPickCol); iDipAcol.push_back(iOct); // Remaining cases with dipole from anticolour in initial state // or dipole inside final state: also new colour. } else { int iPickAcol = iDipAcol[pickDip]; acols[iOct] = acols[iPickAcol]; cols[iOct] = process.nextColTag(); acols[iPickAcol] = cols[iOct]; iDipAcol[pickDip] = iOct; iDipCol.push_back(iOct); iDipAcol.push_back(iPickAcol); } } } // Must now have at least two dipoles (no 1 -> 8 or 8 -> 1). if (iDipCol.size() < 2) { infoPtr->errorMsg("Error in ResonanceDecays::pickColours:" " inconsistent colour tags"); return false; } // Done. return true; } //-------------------------------------------------------------------------- // Select decay products momenta isotropically in phase space. // Process-dependent angular distributions may be imposed in SigmaProcess. bool ResonanceDecays::pickKinematics() { // Description of two-body decays as simple special case. if (mult == 2) { // Masses. m0 = mProd[0]; double m1 = mProd[1]; double m2 = mProd[2]; // Energies and absolute momentum in the rest frame. double e1 = 0.5 * (m0*m0 + m1*m1 - m2*m2) / m0; double e2 = 0.5 * (m0*m0 + m2*m2 - m1*m1) / m0; double pAbs = 0.5 * sqrtpos( (m0 - m1 - m2) * (m0 + m1 + m2) * (m0 + m1 - m2) * (m0 - m1 + m2) ) / m0; // Pick isotropic angles to give three-momentum. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(1. - cosTheta*cosTheta); double phi = 2. * M_PI * rndmPtr->flat(); double pX = pAbs * sinTheta * cos(phi); double pY = pAbs * sinTheta * sin(phi); double pZ = pAbs * cosTheta; // Fill four-momenta in mother rest frame and then boost to lab frame. pProd.push_back( Vec4( pX, pY, pZ, e1) ); pProd.push_back( Vec4( -pX, -pY, -pZ, e2) ); pProd[1].bst( pProd[0] ); pProd[2].bst( pProd[0] ); // Done for two-body decay. return true; } // Description of three-body decays as semi-simple special case. if (mult == 3) { // Masses. m0 = mProd[0]; double m1 = mProd[1]; double m2 = mProd[2]; double m3 = mProd[3]; double mDiff = m0 - (m1 + m2 + m3); // Kinematical limits for 2+3 mass. Maximum phase-space weight. double m23Min = m2 + m3; double m23Max = m0 - m1; double p1Max = 0.5 * sqrtpos( (m0 - m1 - m23Min) * (m0 + m1 + m23Min) * (m0 + m1 - m23Min) * (m0 - m1 + m23Min) ) / m0; double p23Max = 0.5 * sqrtpos( (m23Max - m2 - m3) * (m23Max + m2 + m3) * (m23Max + m2 - m3) * (m23Max - m2 + m3) ) / m23Max; double wtPSmax = 0.5 * p1Max * p23Max; // Pick an intermediate mass m23 flat in the allowed range. double wtPS, m23, p1Abs, p23Abs; do { m23 = m23Min + rndmPtr->flat() * mDiff; // Translate into relative momenta and find phase-space weight. p1Abs = 0.5 * sqrtpos( (m0 - m1 - m23) * (m0 + m1 + m23) * (m0 + m1 - m23) * (m0 - m1 + m23) ) / m0; p23Abs = 0.5 * sqrtpos( (m23 - m2 - m3) * (m23 + m2 + m3) * (m23 + m2 - m3) * (m23 - m2 + m3) ) / m23; wtPS = p1Abs * p23Abs; // If rejected, try again with new invariant masses. } while ( wtPS < rndmPtr->flat() * wtPSmax ); // Set up m23 -> m2 + m3 isotropic in its rest frame. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(1. - cosTheta*cosTheta); double phi = 2. * M_PI * rndmPtr->flat(); double pX = p23Abs * sinTheta * cos(phi); double pY = p23Abs * sinTheta * sin(phi); double pZ = p23Abs * cosTheta; double e2 = sqrt( m2*m2 + p23Abs*p23Abs); double e3 = sqrt( m3*m3 + p23Abs*p23Abs); Vec4 p2( pX, pY, pZ, e2); Vec4 p3( -pX, -pY, -pZ, e3); // Set up 0 -> 1 + 23 isotropic in its rest frame. cosTheta = 2. * rndmPtr->flat() - 1.; sinTheta = sqrt(1. - cosTheta*cosTheta); phi = 2. * M_PI * rndmPtr->flat(); pX = p1Abs * sinTheta * cos(phi); pY = p1Abs * sinTheta * sin(phi); pZ = p1Abs * cosTheta; double e1 = sqrt( m1*m1 + p1Abs*p1Abs); double e23 = sqrt( m23*m23 + p1Abs*p1Abs); pProd.push_back( Vec4( pX, pY, pZ, e1) ); // Boost 2 + 3 to the 0 rest frame and then boost to lab frame. Vec4 p23( -pX, -pY, -pZ, e23); p2.bst( p23 ); p3.bst( p23 ); pProd.push_back( p2 ); pProd.push_back( p3 ); pProd[1].bst( pProd[0] ); pProd[2].bst( pProd[0] ); pProd[3].bst( pProd[0] ); // Done for three-body decay. return true; } // Do a multibody decay using the M-generator algorithm. // Mother and sum daughter masses. m0 = mProd[0]; double mSum = mProd[1]; for (int i = 2; i <= mult; ++i) mSum += mProd[i]; double mDiff = m0 - mSum; // Begin setup of intermediate invariant masses. vector mInv; for (int i = 0; i <= mult; ++i) mInv.push_back( mProd[i]); // Calculate the maximum weight in the decay. double wtPSmax = 1. / WTCORRECTION[mult]; double mMax = mDiff + mProd[mult]; double mMin = 0.; for (int i = mult - 1; i > 0; --i) { mMax += mProd[i]; mMin += mProd[i+1]; double mNow = mProd[i]; wtPSmax *= 0.5 * sqrtpos( (mMax - mMin - mNow) * (mMax + mMin + mNow) * (mMax + mMin - mNow) * (mMax - mMin + mNow) ) / mMax; } // Begin loop to find the set of intermediate invariant masses. vector rndmOrd; double wtPS; do { wtPS = 1.; // Find and order random numbers in descending order. rndmOrd.resize(0); rndmOrd.push_back(1.); for (int i = 1; i < mult - 1; ++i) { double rndm = rndmPtr->flat(); rndmOrd.push_back(rndm); for (int j = i - 1; j > 0; --j) { if (rndm > rndmOrd[j]) swap( rndmOrd[j], rndmOrd[j+1] ); else break; } } rndmOrd.push_back(0.); // Translate into intermediate masses and find weight. for (int i = mult - 1; i > 0; --i) { mInv[i] = mInv[i+1] + mProd[i] + (rndmOrd[i-1] - rndmOrd[i]) * mDiff; wtPS *= 0.5 * sqrtpos( (mInv[i] - mInv[i+1] - mProd[i]) * (mInv[i] + mInv[i+1] + mProd[i]) * (mInv[i] + mInv[i+1] - mProd[i]) * (mInv[i] - mInv[i+1] + mProd[i]) ) / mInv[i]; } // If rejected, try again with new invariant masses. } while ( wtPS < rndmPtr->flat() * wtPSmax ); // Perform two-particle decays in the respective rest frame. vector pInv; pInv.resize(mult + 1); for (int i = 1; i < mult; ++i) { double pAbs = 0.5 * sqrtpos( (mInv[i] - mInv[i+1] - mProd[i]) * (mInv[i] + mInv[i+1] + mProd[i]) * (mInv[i] + mInv[i+1] - mProd[i]) * (mInv[i] - mInv[i+1] + mProd[i]) ) / mInv[i]; // Isotropic angles give three-momentum. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(1. - cosTheta*cosTheta); double phi = 2. * M_PI * rndmPtr->flat(); double pX = pAbs * sinTheta * cos(phi); double pY = pAbs * sinTheta * sin(phi); double pZ = pAbs * cosTheta; // Calculate energies, fill four-momenta. double eHad = sqrt( mProd[i]*mProd[i] + pAbs*pAbs); double eInv = sqrt( mInv[i+1]*mInv[i+1] + pAbs*pAbs); pProd.push_back( Vec4( pX, pY, pZ, eHad) ); pInv[i+1].p( -pX, -pY, -pZ, eInv); } pProd.push_back( pInv[mult] ); // Boost decay products to the mother rest frame and on to lab frame. pInv[1] = pProd[0]; for (int iFrame = mult - 1; iFrame > 0; --iFrame) for (int i = iFrame; i <= mult; ++i) pProd[i].bst(pInv[iFrame]); // Done for multibody decay. return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/BeamShape.cc0000644000175000017500000001124212217346245015262 0ustar sunsun// BeamShape.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the BeamShape class. #include "Pythia8/BeamShape.h" namespace Pythia8 { //========================================================================== // The BeamShape class. //-------------------------------------------------------------------------- // Initialize beam parameters. void BeamShape::init( Settings& settings, Rndm* rndmPtrIn) { // Save pointer. rndmPtr = rndmPtrIn; // Main flags. allowMomentumSpread = settings.flag("Beams:allowMomentumSpread"); allowVertexSpread = settings.flag("Beams:allowVertexSpread"); // Parameters for beam A momentum spread. sigmaPxA = settings.parm("Beams:sigmaPxA"); sigmaPyA = settings.parm("Beams:sigmaPyA"); sigmaPzA = settings.parm("Beams:sigmaPzA"); maxDevA = settings.parm("Beams:maxDevA"); // Parameters for beam B momentum spread. sigmaPxB = settings.parm("Beams:sigmaPxB"); sigmaPyB = settings.parm("Beams:sigmaPyB"); sigmaPzB = settings.parm("Beams:sigmaPzB"); maxDevB = settings.parm("Beams:maxDevB"); // Parameters for beam vertex spread. sigmaVertexX = settings.parm("Beams:sigmaVertexX"); sigmaVertexY = settings.parm("Beams:sigmaVertexY"); sigmaVertexZ = settings.parm("Beams:sigmaVertexZ"); maxDevVertex = settings.parm("Beams:maxDevVertex"); sigmaTime = settings.parm("Beams:sigmaTime"); maxDevTime = settings.parm("Beams:maxDevTime"); // Parameters for beam vertex offset. offsetX = settings.parm("Beams:offsetVertexX"); offsetY = settings.parm("Beams:offsetVertexY"); offsetZ = settings.parm("Beams:offsetVertexZ"); offsetT = settings.parm("Beams:offsetTime"); } //-------------------------------------------------------------------------- // Set the two beam momentum deviations and the beam vertex. void BeamShape::pick() { // Reset all values. deltaPxA = deltaPyA = deltaPzA = deltaPxB = deltaPyB = deltaPzB = vertexX = vertexY = vertexZ = vertexT = 0.; // Set beam A momentum deviation by a three-dimensional Gaussian. if (allowMomentumSpread) { double totalDev, gauss; do { totalDev = 0.; if (sigmaPxA > 0.) { gauss = rndmPtr->gauss(); deltaPxA = sigmaPxA * gauss; totalDev += gauss * gauss; } if (sigmaPyA > 0.) { gauss = rndmPtr->gauss(); deltaPyA = sigmaPyA * gauss; totalDev += gauss * gauss; } if (sigmaPzA > 0.) { gauss = rndmPtr->gauss(); deltaPzA = sigmaPzA * gauss; totalDev += gauss * gauss; } } while (totalDev > maxDevA * maxDevA); // Set beam B momentum deviation by a three-dimensional Gaussian. do { totalDev = 0.; if (sigmaPxB > 0.) { gauss = rndmPtr->gauss(); deltaPxB = sigmaPxB * gauss; totalDev += gauss * gauss; } if (sigmaPyB > 0.) { gauss = rndmPtr->gauss(); deltaPyB = sigmaPyB * gauss; totalDev += gauss * gauss; } if (sigmaPzB > 0.) { gauss = rndmPtr->gauss(); deltaPzB = sigmaPzB * gauss; totalDev += gauss * gauss; } } while (totalDev > maxDevB * maxDevB); } // Set beam vertex location by a three-dimensional Gaussian. if (allowVertexSpread) { double totalDev, gauss; do { totalDev = 0.; if (sigmaVertexX > 0.) { gauss = rndmPtr->gauss(); vertexX = sigmaVertexX * gauss; totalDev += gauss * gauss; } if (sigmaVertexY > 0.) { gauss = rndmPtr->gauss(); vertexY = sigmaVertexY * gauss; totalDev += gauss * gauss; } if (sigmaVertexZ > 0.) { gauss = rndmPtr->gauss(); vertexZ = sigmaVertexZ * gauss; totalDev += gauss * gauss; } } while (totalDev > maxDevVertex * maxDevVertex); // Set beam collision time by a Gaussian. if (sigmaTime > 0.) { do gauss = rndmPtr->gauss(); while (abs(gauss) > maxDevTime); vertexT = sigmaTime * gauss; } // Add offset to beam vertex. vertexX += offsetX; vertexY += offsetY; vertexZ += offsetZ; vertexT += offsetT; } } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/BeamRemnants.cc0000644000175000017500000013205412217346245016016 0ustar sunsun// BeamRemnants.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // BeamRemnants class. #include "Pythia8/BeamRemnants.h" namespace Pythia8 { //========================================================================== // The BeamDipole class is purely internal to reconnectColours. class BeamDipole { public: // Constructor. BeamDipole( int colIn = 0, int iColIn = 0, int iAcolIn = 0) : col(colIn), iCol(iColIn), iAcol(iAcolIn) {} // Members. int col, iCol, iAcol; double p1p2; }; //========================================================================== // The BeamRemnants class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // If same (anti)colour appears twice in final state, repair or reject. const bool BeamRemnants::ALLOWCOLOURTWICE = true; // Maximum number of tries to match colours and kinematics in the event. const int BeamRemnants::NTRYCOLMATCH = 10; const int BeamRemnants::NTRYKINMATCH = 10; // Overall correction step for energy-momentum conservation; only // becomes relevant in rescattering scenarios when FSR dipole emissions // and primordial kT is added. Should hopefully not be needed. const bool BeamRemnants::CORRECTMISMATCH = false; //-------------------------------------------------------------------------- // Initialization. bool BeamRemnants::init( Info* infoPtrIn, Settings& settings, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, PartonSystems* partonSystemsPtrIn) { // Save pointers. infoPtr = infoPtrIn; rndmPtr = rndmPtrIn; beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; partonSystemsPtr = partonSystemsPtrIn; // Width of primordial kT distribution. doPrimordialKT = settings.flag("BeamRemnants:primordialKT"); primordialKTsoft = settings.parm("BeamRemnants:primordialKTsoft"); primordialKThard = settings.parm("BeamRemnants:primordialKThard"); primordialKTremnant = settings.parm("BeamRemnants:primordialKTremnant"); halfScaleForKT = settings.parm("BeamRemnants:halfScaleForKT"); halfMassForKT = settings.parm("BeamRemnants:halfMassForKT"); // Handling of rescattering kinematics uncertainties from primodial kT. allowRescatter = settings.flag("MultipartonInteractions:allowRescatter"); doRescatterRestoreY = settings.flag("BeamRemnants:rescatterRestoreY"); // Parameters for colour reconnection scenario, partly borrowed from // multiparton interactions not to introduce too many new ones. doReconnect = settings.flag("BeamRemnants:reconnectColours"); reconnectRange = settings.parm("BeamRemnants:reconnectRange"); pT0Ref = settings.parm("MultipartonInteractions:pT0Ref"); ecmRef = settings.parm("MultipartonInteractions:ecmRef"); ecmPow = settings.parm("MultipartonInteractions:ecmPow"); // Total and squared CM energy at nominal energy. eCM = infoPtr->eCM(); sCM = eCM * eCM; // The MPI pT0 smoothening scale and its reconnection-strength combination. pT0 = pT0Ref * pow(eCM / ecmRef, ecmPow); pT20Rec = pow2(reconnectRange * pT0); // Done. return true; } //-------------------------------------------------------------------------- // Select the flavours/kinematics/colours of the two beam remnants. // Notation: iPar = all partons, iSys = matched systems of two beams, // iRem = additional partons in remnants. bool BeamRemnants::add( Event& event) { // Update to current CM energy. eCM = infoPtr->eCM(); sCM = eCM * eCM; // Check that flavour bookkept in event and in beam particles agree. for (int i = 0; i < beamAPtr->size(); ++i) { int j = (*beamAPtr)[i].iPos(); if ((*beamAPtr)[i].id() != event[j].id()) { infoPtr->errorMsg("Error in BeamRemnants::add: " "event and beam flavours do not match"); return false; } } for (int i = 0; i < beamBPtr->size(); ++i) { int j = (*beamBPtr)[i].iPos(); if ((*beamBPtr)[i].id() != event[j].id()) { infoPtr->errorMsg("Error in BeamRemnants::add: " "event and beam flavours do not match"); return false; } } // Number of scattering subsystems. Size of event record before treatment. nSys = partonSystemsPtr->sizeSys(); oldSize = event.size(); // Add required extra remnant flavour content. // Start all over if fails (in option where junctions not allowed). if ( !beamAPtr->remnantFlavours(event) || !beamBPtr->remnantFlavours(event) ) { infoPtr->errorMsg("Error in BeamRemnants::add:" " remnant flavour setup failed"); return false; } // Do the kinematics of the collision subsystems and two beam remnants. if (!setKinematics(event)) return false; // Allow colour reconnections. if (doReconnect) reconnectColours(event); // Save current modifiable colour configuration for fast restoration. vector colSave; vector acolSave; for (int i = oldSize; i < event.size(); ++i) { colSave.push_back( event[i].col() ); acolSave.push_back( event[i].acol() ); } event.saveJunctionSize(); // Allow several tries to match colours of initiators and remnants. // Frequent "failures" since shortcutting colours separately on // the two event sides may give "colour singlet gluons" etc. bool physical = true; for (int iTry = 0; iTry < NTRYCOLMATCH; ++iTry) { physical = true; // Reset list of colour "collapses" (transformations). colFrom.resize(0); colTo.resize(0); // First process each set of beam colours on its own. if (!beamAPtr->remnantColours(event, colFrom, colTo)) physical = false; if (!beamBPtr->remnantColours(event, colFrom, colTo)) physical = false; // Then check that colours and anticolours are matched in whole event. if ( physical && !checkColours(event) ) physical = false; // If no problems then done, else restore and loop. if (physical) break; for (int i = oldSize; i < event.size(); ++i) event[i].cols( colSave[i - oldSize], acolSave[i - oldSize] ); event.restoreJunctionSize(); infoPtr->errorMsg("Warning in BeamRemnants::add:" " colour tracing failed; will try again"); } // If no solution after several tries then failed. if (!physical) { infoPtr->errorMsg("Error in BeamRemnants::add:" " colour tracing failed after several attempts"); return false; } // Done. return true; } //-------------------------------------------------------------------------- // Set up trial transverse and longitudinal kinematics for each beam // separately. Final decisions involve comparing the two beams. bool BeamRemnants::setKinematics( Event& event) { // References to beams to simplify indexing. BeamParticle& beamA = *beamAPtr; BeamParticle& beamB = *beamBPtr; // Nothing to do for lepton-lepton scattering with all energy already used. if ( beamA.isUnresolvedLepton() && beamB.isUnresolvedLepton() ) return true; // Check that has not already used up beams. if ( (!beamA.isLepton() && beamA.xMax(-1) <= 0.) || (!beamB.isLepton() && beamB.xMax(-1) <= 0.) ) { infoPtr->errorMsg("Error in BeamRemnants::setKinematics:" " no momentum left for beam remnants"); return false; } // Last beam-status particles. Offset relative to normal beam locations. int nBeams = 3; for (int i = 3; i < event.size(); ++i) if (event[i].statusAbs() < 20) nBeams = i + 1; int nOffset = nBeams - 3; // Reserve space for extra information on the systems and beams. int nMaxBeam = max( beamA.size(), beamB.size() ); vector sHatSys(nMaxBeam); vector kTwidth(nMaxBeam); vector kTcomp(nMaxBeam); vector Msys(nSys); // Loop over all subsystems. Default values. Find invariant mass. double kTcompSumA = 0.; double kTcompSumB = 0.; for (int iSys = 0; iSys < nSys; ++iSys) { double kTwidthNow = 0.; double mHatDamp = 1.; int iInA = partonSystemsPtr->getInA(iSys); int iInB = partonSystemsPtr->getInB(iSys); double sHatNow = (event[iInA].p() + event[iInB].p()).m2Calc(); // Allow primordial kT reduction for small-mass and small-pT systems // (for hardest interaction pT -> renormalization scale so also 2 -> 1). if (doPrimordialKT) { double mHat = sqrt(sHatNow); mHatDamp = mHat / (mHat + halfMassForKT); double scale = (iSys == 0) ? infoPtr->QRen(iDS) : partonSystemsPtr->getPTHat(iSys); kTwidthNow = ( (halfScaleForKT * primordialKTsoft + scale * primordialKThard) / (halfScaleForKT + scale) ) * mHatDamp; } // Store properties of compensation systems and total compensation power. // Rescattered partons do not compensate, but may be massive. sHatSys[iSys] = sHatNow; kTwidth[iSys] = kTwidthNow ; kTcomp[iSys] = mHatDamp; if (beamA[iSys].isFromBeam()) kTcompSumA += mHatDamp; else beamA[iSys].m( event[iInA].m() ); if (beamB[iSys].isFromBeam()) kTcompSumB += mHatDamp; else beamB[iSys].m( event[iInB].m() ); } // Primordial kT and compensation power among remnants. double kTwidthNow = (doPrimordialKT) ? primordialKTremnant : 0.; for (int iRem = nSys; iRem < nMaxBeam; ++iRem) { sHatSys[iRem] = 0.; kTwidth[iRem] = kTwidthNow ; kTcomp[iRem] = 1.; } kTcompSumA += beamA.size() - nSys; kTcompSumB += beamB.size() - nSys; // Allow ten tries to construct kinematics (but normally works first). bool physical; double xSum[2], xInvM[2], w2Beam[2], wPosRem, wNegRem, w2Rem; for (int iTry = 0; iTry < NTRYKINMATCH; ++iTry) { physical = true; // Loop over the two beams. for (int iBeam = 0; iBeam < 2; ++iBeam) { BeamParticle& beam = (iBeam == 0) ? beamA : beamB; int nPar = beam.size(); // Generate Gaussian pT for initiator partons inside hadrons. // Store/restore rescattered parton momenta before primordial kT. if (beam.isHadron() && doPrimordialKT) { double pxSum = 0.; double pySum = 0.; for (int iPar = 0; iPar < nPar; ++iPar) { if ( beam[iPar].isFromBeam() ) { pair gauss2 = rndmPtr->gauss2(); double px = kTwidth[iPar] * gauss2.first; double py = kTwidth[iPar] * gauss2.second; beam[iPar].px(px); beam[iPar].py(py); pxSum += px; pySum += py; } else { int iInAB = (iBeam == 0) ? partonSystemsPtr->getInA(iPar) : partonSystemsPtr->getInB(iPar); beam[iPar].p( event[iInAB].p() ); } } // Share recoil between all initiator partons, rescatterers excluded. double kTcompSum = (iBeam == 0) ? kTcompSumA : kTcompSumB; for (int iPar = 0; iPar < nPar; ++iPar) if (beam[iPar].isFromBeam() ) { beam[iPar].px( beam[iPar].px() - pxSum * kTcomp[iPar] / kTcompSum ); beam[iPar].py( beam[iPar].py() - pySum * kTcomp[iPar] / kTcompSum ); } // Without primordial kT: still need to store rescattered partons. } else if (beam.isHadron()) { for (int iPar = 0; iPar < nPar; ++iPar) if ( !beam[iPar].isFromBeam() ) { int iInAB = (iBeam == 0) ? partonSystemsPtr->getInA(iPar) : partonSystemsPtr->getInB(iPar); beam[iPar].p( event[iInAB].p() ); } } // Pick unrescaled x values for remnants. Sum up (unscaled) p+ and p-. xSum[iBeam] = 0.; xInvM[iBeam] = 0.; for (int iRem = nSys; iRem < nPar; ++iRem) { double xPrel = beam.xRemnant( iRem); beam[iRem].x(xPrel); xSum[iBeam] += xPrel; xInvM[iBeam] += beam[iRem].mT2()/xPrel; } // Squared transverse mass for each beam, using lightcone x. w2Beam[iBeam] = xSum[iBeam] * xInvM[iBeam]; // End separate treatment of the two beams. } // Recalculate kinematics of initiator systems with primordial kT. wPosRem = eCM; wNegRem = eCM; for (int iSys = 0; iSys < nSys; ++iSys) { int iA = beamA[iSys].iPos(); int iB = beamB[iSys].iPos(); double sHat = sHatSys[iSys]; // Classify system: rescattering on either or both sides? bool normalA = beamA[iSys].isFromBeam(); bool normalB = beamB[iSys].isFromBeam(); bool normalSys = normalA && normalB; bool doubleRes = !normalA && !normalB; // Check whether final-state system momentum matches initial-state one. if (allowRescatter && CORRECTMISMATCH) { Vec4 pInitial = event[iA].p() + event[iB].p(); Vec4 pFinal; for (int iMem = 0; iMem < partonSystemsPtr->sizeOut(iSys); ++iMem) { int iAB = partonSystemsPtr->getOut(iSys, iMem); if (event[iAB].isFinal()) pFinal += event[iAB].p(); } // Scale down primordial kT from side A if p+ increased. if (normalA && pFinal.pPos() > pInitial.pPos()) beamA[iSys].scalePT( pInitial.pPos() / pFinal.pPos() ); // Scale down primordial kT from side B if p- increased. if (normalB && pFinal.pNeg() > pInitial.pNeg()) beamB[iSys].scalePT( pInitial.pNeg() / pFinal.pNeg() ); } // Rescatter: possible change in sign of lightcone momentum of a // rescattered parton. If this happens, try to pick // new primordial kT values if (allowRescatter && (event[iA].pPos() / beamA[iSys].pPos() < 0 || event[iB].pNeg() / beamB[iSys].pNeg() < 0) ) { infoPtr->errorMsg("Warning in BeamRemnants::setKinematics:" " change in lightcone momentum sign; retrying kinematics"); physical = false; break; } // Begin kinematics of partons after primordial kT has been added. double sHatTAft = sHat + pow2( beamA[iSys].px() + beamB[iSys].px()) + pow2( beamA[iSys].py() + beamB[iSys].py()); double w2A = beamA[iSys].mT2(); double w2B = beamB[iSys].mT2(); double w2Diff = sHatTAft - w2A - w2B; double lambda = pow2(w2Diff) - 4. * w2A * w2B; // Too large transverse momenta means that kinematics will not work. if (lambda <= 0.) { physical = false; break; } double lamRoot = sqrtpos( lambda ); // Mirror solution if the two incoming have reverse rapidity ordering. if (allowRescatter && doubleRes && (event[iA].pPos() * event[iB].pNeg() < event[iA].pNeg() * event[iB].pPos()) ) lamRoot = -lamRoot; // Two procedures, which agree for normal scattering, separate here. // First option keeps rapidity (and mass) of system unchanged by // primordial kT, by modification of rescattered parton. if (normalSys || doRescatterRestoreY || doubleRes) { // Find kinematics of initial system: transverse mass, and // longitudinal momentum carried by all or rescattered partons. double sHatTBef = sHat; double wPosBef, wNegBef, wPosBefRes, wNegBefRes; // Normal scattering. if (normalSys) { wPosBef = beamA[iSys].x() * eCM; wNegBef = beamB[iSys].x() * eCM; wPosBefRes = 0.; wNegBefRes = 0.; // Rescattering on side A. } else if (normalB) { sHatTBef += event[iA].pT2(); wPosBef = event[iA].pPos(); wNegBef = event[iA].pNeg() + beamB[iSys].x() * eCM; wPosBefRes = beamA[iSys].pPos(); wNegBefRes = beamA[iSys].pNeg(); // Rescattering on side B. } else if (normalA) { sHatTBef += event[iB].pT2(); wPosBef = beamA[iSys].x() * eCM + event[iB].pPos(); wNegBef = event[iB].pNeg(); wPosBefRes = beamB[iSys].pPos(); wNegBefRes = beamB[iSys].pNeg(); // Rescattering on both sides. } else { sHatTBef += pow2( event[iA].px() + event[iB].px()) + pow2( event[iA].py() + event[iB].py()); wPosBef = event[iA].pPos() + event[iB].pPos(); wNegBef = event[iA].pNeg() + event[iB].pNeg(); wPosBefRes = beamA[iSys].pPos() + beamB[iSys].pPos(); wNegBefRes = beamA[iSys].pNeg() + beamB[iSys].pNeg(); } // Rescale outgoing momenta to keep same mass and rapidity of system // as originally, and solve for kinematics. double rescale = sqrt(sHatTAft / sHatTBef); double wPosAft = rescale * wPosBef; double wNegAft = rescale * wNegBef; wPosRem -= wPosAft - wPosBefRes; wNegRem -= wNegAft - wNegBefRes; double wPosA = 0.5 * (sHatTAft + w2A - w2B + lamRoot) / wNegAft; double wNegB = 0.5 * (sHatTAft + w2B - w2A + lamRoot) / wPosAft; // Store modified beam parton momenta. beamA[iSys].e( 0.5 * (wPosA + w2A / wPosA) ); beamA[iSys].pz( 0.5 * (wPosA - w2A / wPosA) ); beamB[iSys].e( 0.5 * (w2B / wNegB + wNegB) ); beamB[iSys].pz( 0.5 * (w2B / wNegB - wNegB) ); // Second option keeps rescattered parton (and system mass) unchanged // by primordial kT, by modification of system rapidity. } else { // Rescattering on side A: preserve already scattered parton. if (normalB) { double wPosA = beamA[iSys].pPos(); double wNegB = 0.5 * (w2Diff + lamRoot) / wPosA; beamB[iSys].e( 0.5 * (w2B / wNegB + wNegB) ); beamB[iSys].pz( 0.5 * (w2B / wNegB - wNegB) ); wPosRem -= w2B / wNegB; wNegRem -= wNegB; // Rescattering on side B: preserve already scattered parton. } else if (normalA) { double wNegB = beamB[iSys].pNeg(); double wPosA = 0.5 * (w2Diff + lamRoot) / wNegB; beamA[iSys].e( 0.5 * (wPosA + w2A / wPosA) ); beamA[iSys].pz( 0.5 * (wPosA - w2A / wPosA) ); wPosRem -= wPosA; wNegRem -= w2A / wPosA; // Primordial kT in double rescattering does change the mass of // the system without any possible fix in this framework, which // leads to incorrect boosts. Current choice is therefore always // to handle it with the first procedure, where mass is retained. } else { } } // Construct system rotation and boost caused by primordial kT. Msys[iSys].reset(); Msys[iSys].toCMframe( event[iA].p(), event[iB].p() ); Msys[iSys].fromCMframe( beamA[iSys].p(), beamB[iSys].p() ); // Boost rescattered partons in subsequent beam A list. for (int iSys2 = iSys + 1; iSys2 < nSys; ++iSys2) { if (!beamA[iSys2].isFromBeam()) { int iBefResc = event[ beamA[iSys2].iPos() ].mother1(); for (int iMem = 0; iMem < partonSystemsPtr->sizeOut(iSys); ++iMem) if (partonSystemsPtr->getOut(iSys, iMem) == iBefResc) { Vec4 pTemp = event[iBefResc].p(); pTemp.rotbst( Msys[iSys] ); beamA[iSys2].p( pTemp ); } } // Boost rescattered partons in subsequent beam B list. if (!beamB[iSys2].isFromBeam()) { int iBefResc = event[ beamB[iSys2].iPos() ].mother1(); for (int iMem = 0; iMem < partonSystemsPtr->sizeOut(iSys); ++iMem) if (partonSystemsPtr->getOut(iSys, iMem) == iBefResc) { Vec4 pTemp = event[iBefResc].p(); pTemp.rotbst( Msys[iSys] ); beamB[iSys2].p( pTemp ); } } } } // Check that remaining momentum is enough for remnants. if (wPosRem < 0. || wNegRem < 0.) physical = false; w2Rem = wPosRem * wNegRem; if (sqrtpos(w2Rem) < sqrt(w2Beam[0]) + sqrt(w2Beam[1])) physical = false; // End of loop over ten tries. Do not loop when solution found. if (physical) break; } // If no solution after ten tries then failed. if (!physical) { infoPtr->errorMsg("Error in BeamRemnants::setKinematics:" " kinematics construction failed"); return false; } // For successful initiator kinematics process whole systems. Vec4 pSumOut; for (int iSys = 0; iSys < nSys; ++iSys) { // Copy initiators and their systems and boost them accordingly. // Update subsystem and beams info on new positions of partons. // Update daughter info of mothers, i.e. of beams, for hardest interaction. if (beamA[iSys].isFromBeam()) { int iA = beamA[iSys].iPos(); int iAcopy = event.copy(iA, -61); event[iAcopy].rotbst(Msys[iSys]); partonSystemsPtr->setInA(iSys, iAcopy); beamA[iSys].iPos( iAcopy); if (iSys == 0) { int mother = event[iAcopy].mother1(); event[mother].daughter1(iAcopy); } } if (beamB[iSys].isFromBeam()) { int iB = beamB[iSys].iPos(); int iBcopy = event.copy(iB, -61); event[iBcopy].rotbst(Msys[iSys]); partonSystemsPtr->setInB(iSys, iBcopy); beamB[iSys].iPos( iBcopy); if (iSys == 0) { int mother = event[iBcopy].mother1(); event[mother].daughter1(iBcopy); } } for (int iMem = 0; iMem < partonSystemsPtr->sizeOut(iSys); ++iMem) { int iAB = partonSystemsPtr->getOut(iSys, iMem); if (event[iAB].isFinal()) { int iABcopy = event.copy(iAB, 62); event[iABcopy].rotbst(Msys[iSys]); partonSystemsPtr->setOut(iSys, iMem, iABcopy); pSumOut += event[iABcopy].p(); } } } // Colour dipoles spanning systems gives mismatch between FSR recoils // and primordial kT boosts. if (allowRescatter && CORRECTMISMATCH) { // Find summed pT of beam remnants = - wanted pT of systems. double pxBeams = 0.; double pyBeams = 0.; for (int iRem = nSys; iRem < beamA.size(); ++iRem) { pxBeams += beamA[iRem].px(); pyBeams += beamA[iRem].py(); } for (int iRem = nSys; iRem < beamB.size(); ++iRem) { pxBeams += beamB[iRem].px(); pyBeams += beamB[iRem].py(); } // Boost all final partons in systems transversely, and also their sum. Vec4 pSumTo( -pxBeams, -pyBeams, pSumOut.pz(), sqrt( pow2(pxBeams) + pow2(pyBeams) + pow2(pSumOut.pz()) + pSumOut.m2Calc() ) ); RotBstMatrix Mmismatch; Mmismatch.bst( pSumOut, pSumTo); for (int iSys = 0; iSys < nSys; ++iSys) for (int iMem = 0; iMem < partonSystemsPtr->sizeOut(iSys); ++iMem) { int iAB = partonSystemsPtr->getOut(iSys, iMem); if (event[iAB].isFinal()) event[iAB].rotbst(Mmismatch); } pSumOut.rotbst(Mmismatch); // Reset energy and momentum sum, to be compensated by beam remnants. wPosRem = eCM - (pSumOut.e() + pSumOut.pz()); wNegRem = eCM - (pSumOut.e() - pSumOut.pz()); w2Rem = wPosRem * wNegRem; if ( wPosRem < 0. || wNegRem < 0. || sqrtpos(w2Rem) < sqrt(w2Beam[0]) + sqrt(w2Beam[1])) { infoPtr->errorMsg("Error in BeamRemnants::setKinematics:" " kinematics construction failed owing to recoil mismatch"); return false; } } // Construct x rescaling factors for the two remants. double lambdaRoot = sqrtpos( pow2(w2Rem - w2Beam[0] - w2Beam[1]) - 4. * w2Beam[0] * w2Beam[1] ); double rescaleA = (w2Rem + w2Beam[0] - w2Beam[1] + lambdaRoot) / (2. * w2Rem * xSum[0]) ; double rescaleB = (w2Rem + w2Beam[1] - w2Beam[0] + lambdaRoot) / (2. * w2Rem * xSum[1]) ; // Construct energy and pz for remnants in first beam. for (int iRem = nSys; iRem < beamA.size(); ++iRem) { double pPos = rescaleA * beamA[iRem].x() * wPosRem; double pNeg = beamA[iRem].mT2() / pPos; beamA[iRem].e( 0.5 * (pPos + pNeg) ); beamA[iRem].pz( 0.5 * (pPos - pNeg) ); // Add these partons to the normal event record. int iNew = event.append( beamA[iRem].id(), 63, 1 + nOffset, 0, 0, 0, beamA[iRem].col(), beamA[iRem].acol(), beamA[iRem].p(), beamA[iRem].m() ); beamA[iRem].iPos( iNew); } // Construct energy and pz for remnants in second beam. for (int iRem = nSys; iRem < beamB.size(); ++iRem) { double pNeg = rescaleB * beamB[iRem].x() * wNegRem; double pPos = beamB[iRem].mT2() / pNeg; beamB[iRem].e( 0.5 * (pPos + pNeg) ); beamB[iRem].pz( 0.5 * (pPos - pNeg) ); // Add these partons to the normal event record. int iNew = event.append( beamB[iRem].id(), 63, 2 + nOffset, 0, 0, 0, beamB[iRem].col(), beamB[iRem].acol(), beamB[iRem].p(), beamB[iRem].m() ); beamB[iRem].iPos( iNew); } // Done. return true; } //-------------------------------------------------------------------------- // Allow colour reconnections by mergings of collision subsystems. // iRec is system that may be reconnected, by moving its gluons to iSys, // where minimal pT (or equivalently Lambda) is used to pick location. // Therefore all dipoles in iSys have to be found, and all gluons in iRec. // Matching q-qbar pairs are treated by analogy with gluons. // Note: owing to rescatterings some outgoing partons must be skipped. bool BeamRemnants::reconnectColours( Event& event) { // References to beams to simplify indexing. BeamParticle& beamA = *beamAPtr; BeamParticle& beamB = *beamBPtr; // Prepare record of which systems should be merged onto another. // The iSys system must have colour in final state to attach to it. vector iMerge(nSys); vector hasColour(nSys); for (int iSys = 0; iSys < nSys; ++iSys) { iMerge[iSys] = iSys; bool hasCol = false; for (int iMem = 0; iMem < partonSystemsPtr->sizeOut(iSys); ++iMem) { int iNow = partonSystemsPtr->getOut( iSys, iMem); if (event[iNow].isFinal() && (event[iNow].col() > 0 || event[iNow].acol() > 0) ) { hasCol = true; break; } } hasColour[iSys] = hasCol; } // Loop over systems to decide which should be reconnected. for (int iRec = nSys - 1; iRec > 0; --iRec) { // Determine reconnection strength from pT scale of system. double pT2Rec = pow2( partonSystemsPtr->getPTHat(iRec) ); double probRec = pT20Rec / (pT20Rec + pT2Rec); // Loop over other systems iSys at higher pT scale and // decide whether to reconnect the iRec gluons onto one of them. for (int iSys = iRec - 1; iSys >= 0; --iSys) if (hasColour[iSys] && probRec > rndmPtr->flat()) { // The iRec system and all merged with it to be merged with iSys. iMerge[iRec] = iSys; for (int iRec2 = iRec + 1; iRec2 < nSys; ++iRec2) if (iMerge[iRec2] == iRec) iMerge[iRec2] = iSys; // Once a system has been merged do not test it anymore. break; } } // Loop over systems. Check whether other systems to be merged with it. for (int iSys = 0; iSys < nSys; ++iSys) { int nMerge = 0; for (int iRec = iSys + 1; iRec < nSys; ++iRec) if (iMerge[iRec] == iSys) ++nMerge; if (nMerge == 0) continue; // Incoming partons not counted if rescattered. int iInASys = partonSystemsPtr->getInA(iSys); bool hasInA = (beamA[iSys].isFromBeam()); int iInBSys = partonSystemsPtr->getInB(iSys); bool hasInB = (beamB[iSys].isFromBeam()); // Begin find dipoles in iSys system. vector dipoles; int sizeOut = partonSystemsPtr->sizeOut(iSys); for (int iMem = 0; iMem < sizeOut; ++iMem) { // Find colour dipoles to beam remnant. int iNow = partonSystemsPtr->getOut( iSys, iMem); if (!event[iNow].isFinal()) continue; int col = event[iNow].col(); if (col > 0) { if (hasInA && event[iInASys].col() == col) dipoles.push_back( BeamDipole( col, iNow, iInASys ) ); else if (hasInB && event[iInBSys].col() == col) dipoles.push_back( BeamDipole( col, iNow, iInBSys ) ); // Find colour dipole between final-state partons. else for (int iMem2 = 0; iMem2 < sizeOut; ++iMem2) if (iMem2 != iMem) { int iNow2 = partonSystemsPtr->getOut( iSys, iMem2); if (!event[iNow2].isFinal()) continue; if (event[iNow2].acol() == col) { dipoles.push_back( BeamDipole( col, iNow, iNow2) ); break; } } } // Find anticolour dipoles to beam remnant. int acol = event[iNow].acol(); if (acol > 0) { if (hasInA && event[iInASys].acol() == acol) dipoles.push_back( BeamDipole( acol, iInASys, iNow ) ); else if (hasInB && event[iInBSys].acol() == acol) dipoles.push_back( BeamDipole( acol, iInBSys, iNow ) ); } } // Skip mergings if no dipoles found. if (dipoles.size() == 0) continue; // Find dipole sizes. for (int iDip = 0; iDip < int(dipoles.size()); ++iDip) dipoles[iDip].p1p2 = event[dipoles[iDip].iCol].p() * event[dipoles[iDip].iAcol].p(); // Loop over systems iRec to be merged with iSys. for (int iRec = iSys + 1; iRec < nSys; ++iRec) { if (iMerge[iRec] != iSys) continue; // Information on iRec. Vectors for gluons and anything else. int sizeRec = partonSystemsPtr->sizeOut(iRec); int iInARec = partonSystemsPtr->getInA(iRec); int iInBRec = partonSystemsPtr->getInB(iRec); int nGluRec = 0; vector iGluRec; vector pT2GluRec; int nAnyRec = 0; vector iAnyRec; vector freeAnyRec; // Copy of gluon positions in descending order. for (int iMem = 0; iMem < sizeRec; ++iMem) { int iNow = partonSystemsPtr->getOut( iRec, iMem); if (!event[iNow].isFinal()) continue; if (event[iNow].isGluon()) { ++nGluRec; iGluRec.push_back( iNow ); pT2GluRec.push_back( event[iNow].pT2() ); for (int i = nGluRec - 1; i > 1; --i) { if (pT2GluRec[i - 1] > pT2GluRec[i]) break; swap( iGluRec[i - 1], iGluRec[i] ); swap( pT2GluRec[i - 1], pT2GluRec[i] ); } // Copy of anything else, mainly quarks, in no particular order. } else { ++nAnyRec; iAnyRec.push_back( iNow ); freeAnyRec.push_back( true ); } } // For each gluon in iRec now find the dipole that gives the smallest // (pGlu * pI) (pGlu * pJ) / (pI * pJ), i.e. minimal pT (and Lambda). for (int iGRec = 0; iGRec < nGluRec; ++iGRec) { int iGlu = iGluRec[iGRec]; Vec4 pGlu = event[iGlu].p(); int iDipMin = 0; double pT2DipMin = sCM; for (int iDip = 0; iDip < int(dipoles.size()); ++iDip) { double pT2Dip = (pGlu * event[dipoles[iDip].iCol].p()) * (pGlu * event[dipoles[iDip].iAcol].p()) / dipoles[iDip].p1p2; if (pT2Dip < pT2DipMin) { iDipMin = iDip; pT2DipMin = pT2Dip; } } // Attach the gluon to the dipole, i.e. split the dipole in two. int colGlu = event[iGlu].col(); int acolGlu = event[iGlu].acol(); int colDip = dipoles[iDipMin].col; int iColDip = dipoles[iDipMin].iCol; int iAcolDip = dipoles[iDipMin].iAcol; event[iGlu].acol( colDip ); if (event[iAcolDip].acol() == colDip) event[iAcolDip].acol( colGlu ); else event[iAcolDip].col( colGlu ); dipoles[iDipMin].iAcol = iGlu; dipoles[iDipMin].p1p2 = event[iColDip].p() * pGlu; dipoles.push_back( BeamDipole( colGlu, iGlu, iAcolDip ) ); dipoles.back().p1p2 = pGlu * event[iAcolDip].p(); // Remove gluon from old system: reconnect colours. for (int i = oldSize; i < event.size(); ++i) if (i != iGlu && i != iAcolDip) { if (event[i].isFinal()) { if (event[i].acol() == colGlu) event[i].acol( acolGlu ); } else { if (event[i].col() == colGlu) event[i].col( acolGlu ); } } // Update any junction legs that match reconnected dipole. for (int iJun = 0; iJun < event.sizeJunction(); ++iJun) { // Only junctions need to be updated, not antijunctions. if (event.kindJunction(iJun) % 2 == 0) continue; for (int leg = 0; leg < 3; ++leg) { int col = event.colJunction(iJun, leg); if (col == colDip) event.colJunction(iJun, leg, colGlu); } } } // See if any matching quark-antiquark pairs among the rest. for (int iQRec = 0; iQRec < nAnyRec; ++iQRec) { int iQ = iAnyRec[iQRec]; int idQ = event[iQ].id(); if (freeAnyRec[iQRec] && idQ > 0 && idQ < 6) for (int iQbarRec = 0; iQbarRec < nAnyRec; ++iQbarRec) { int iQbar = iAnyRec[iQbarRec]; if (freeAnyRec[iQbarRec] && event[iQbar].id() == -idQ) { // Check that these can be traced back to same gluon splitting. // For now also avoid qqbar pairs produced in rescatterings.?? int iTopQ = event.iTopCopyId(iQ); int iTopQbar = event.iTopCopyId(iQbar); int iMother = event[iTopQ].mother1(); if (event[iTopQbar].mother1() == iMother && event[iMother].isGluon() && event[iMother].status() != -34 && event[iMother + 1].status() != -34 ) { // Now find the dipole that gives the smallest // ((pQ + pQbar) * pI) ((pQ + pQbar) * pJ) / (pI * pJ). Vec4 pGlu = event[iQ].p() + event[iQbar].p(); int iDipMin = 0; double pT2DipMin = sCM; for (int iDip = 0; iDip < int(dipoles.size()); ++iDip) { double pT2Dip = (pGlu * event[dipoles[iDip].iCol].p()) * (pGlu * event[dipoles[iDip].iAcol].p()) / dipoles[iDip].p1p2; if (pT2Dip < pT2DipMin) { iDipMin = iDip; pT2DipMin = pT2Dip; } } // Attach the q-qbar pair to the dipole, i.e. split the dipole. int colGlu = event[iQ].col(); int acolGlu = event[iQbar].acol(); int colDip = dipoles[iDipMin].col; int iColDip = dipoles[iDipMin].iCol; int iAcolDip = dipoles[iDipMin].iAcol; event[iQbar].acol( colDip ); if (event[iAcolDip].acol() == colDip) event[iAcolDip].acol( colGlu ); else event[iAcolDip].col( colGlu ); dipoles[iDipMin].iAcol = iQbar; dipoles[iDipMin].p1p2 = event[iColDip].p() * event[iQbar].p(); dipoles.push_back( BeamDipole( colGlu, iQ, iAcolDip ) ); dipoles.back().p1p2 = event[iQ].p() * event[iAcolDip].p(); // Remove q-qbar pair from old system: reconnect colours. freeAnyRec[iQRec] = false; freeAnyRec[iQbarRec] = false; for (int i = oldSize; i < event.size(); ++i) if (i != iQRec && i != iQbarRec && i != iColDip && i != iAcolDip) { if (event[i].isFinal()) { if (event[i].acol() == colGlu) event[i].acol( acolGlu ); } else { if (event[i].col() == colGlu) event[i].col( acolGlu ); } } // Update any junction legs that match reconnected dipole. for (int iJun = 0; iJun < event.sizeJunction(); ++iJun) { // Only junctions need to be updated, not antijunctions. if (event.kindJunction(iJun) % 2 == 0) continue; for (int leg = 0; leg < 3; ++leg) { int col = event.colJunction(iJun, leg); if (col == colDip) event.colJunction(iJun, leg, colGlu); } } // Done with processing of q-qbar pairs. } } } } // If only two beam gluons left of system, set their colour = anticolour. // Used by BeamParticle::remnantColours to skip irrelevant gluons. if ( event[iInARec].isGluon() && !event[iInARec].isRescatteredIncoming() && event[iInBRec].isGluon() && !event[iInBRec].isRescatteredIncoming() && event[iInARec].col() == event[iInBRec].acol() && event[iInARec].acol() == event[iInBRec].col() ) { event[iInARec].acol( event[iInARec].col() ); event[iInBRec].acol( event[iInBRec].col() ); } // End of loops over iRec and iSys systems. } } // Done. return true; } //-------------------------------------------------------------------------- // Collapse colours and check that they are consistent. bool BeamRemnants::checkColours( Event& event) { // No colours in lepton beams so no need to do anything. if (beamAPtr->isLepton() && beamBPtr->isLepton()) return true; // Remove ambiguities when one colour collapses two ways. // Resolve chains where one colour is mapped to another. for (int iCol = 1; iCol < int(colFrom.size()); ++iCol) for (int iColRef = 0; iColRef < iCol; ++iColRef) { if (colFrom[iCol] == colFrom[iColRef]) { colFrom[iCol] = colTo[iCol]; colTo[iCol] = colTo[iColRef]; } if (colTo[iCol] == colFrom[iColRef]) colTo[iCol] = colTo[iColRef]; } // Transform event record colours from beam remnant colour collapses. for (int i = oldSize; i < event.size(); ++i) { int col = event[i].col(); int acol = event[i].acol(); for (int iCol = 0; iCol < int(colFrom.size()); ++iCol) { if (col == colFrom[iCol]) {col = colTo[iCol]; event[i].col(col);} if (acol == colFrom[iCol]) {acol = colTo[iCol]; event[i].acol(acol);} } } // Transform junction colours from beam remnant colour collapses. for (int iJun = 0; iJun < event.sizeJunction(); ++iJun) for (int leg = 0; leg < 3; ++leg) { int col = event.colJunction(iJun, leg); for (int iCol = 0; iCol < int(colFrom.size()); ++iCol) { if (col == colFrom[iCol]) { col = colTo[iCol]; event.colJunction(iJun, leg, col); } } } // Arrays for current colours and anticolours, and for singlet gluons. vector colList; vector acolList; vector iSingletGluon; // Find current colours and anticolours in the event record. for (int i = oldSize; i < event.size(); ++i) if (event[i].isFinal()) { int id = event[i].id(); int col = event[i].col(); int acol = event[i].acol(); int colType = event[i].colType(); // Quarks must have colour set, antiquarks anticolour, gluons both. if ( (id > 0 && id < 9 && (col <= 0 || acol != 0) ) || (id < 0 && id > -9 && (col != 0 || acol <= 0) ) || (id == 21 && (col <= 0 || acol <= 0) ) ) { infoPtr->errorMsg("Error in BeamRemnants::checkColours: " "q/qbar/g has wrong colour slots set"); return false; } // Sextets must have one positive and one negative tag if ( (colType == 3 && (col <= 0 || acol >= 0)) || (colType == -3 && (col >= 0 || acol <= 0)) ) { infoPtr->errorMsg("Error in BeamRemnants::checkColours: " "sextet has wrong colours"); } // Save colours/anticolours, and position of colour singlet gluons. if ( col > 0) colList.push_back( col ); if (acol > 0) acolList.push_back( acol ); if (col > 0 && acol == col) iSingletGluon.push_back(i); // Colour sextets if ( col < 0) acolList.push_back( -col ); if (acol < 0) colList.push_back( -acol ); } // Run though list of singlet gluons and put them on final-state dipole // (i,j) that offers smallest (p_g p_i) * (p_g p_j) / (p_i p_j). for (int iS = 0; iS < int(iSingletGluon.size()); ++iS) { int iGlu = iSingletGluon[iS]; int iAcolDip = -1; double pT2DipMin = sCM; for (int iC = oldSize; iC < event.size(); ++iC) if (iC != iGlu && event[iC].isFinal()) { int colDip = event[iC].col(); if (colDip > 0 && event[iC].acol() !=colDip) for (int iA = oldSize; iA < event.size(); ++iA) if (iA != iGlu && iA != iC && event[iA].isFinal() && event[iA].acol() == colDip && event[iA].col() !=colDip) { double pT2Dip = (event[iGlu].p() * event[iC].p()) * (event[iGlu].p() * event[iA].p()) / (event[iC].p() * event[iA].p()); if (pT2Dip < pT2DipMin) { iAcolDip = iA; pT2DipMin = pT2Dip; } } } // Fail if no dipole. Else insert singlet gluon onto relevant dipole. if (iAcolDip == -1) return false; event[iGlu].acol( event[iAcolDip].acol() ); event[iAcolDip].acol( event[iGlu].col() ); // Update any junction legs that match reconnected dipole. for (int iJun = 0; iJun < event.sizeJunction(); ++iJun) { // Only junctions need to be updated, not antijunctions. if (event.kindJunction(iJun) % 2 == 0) continue; for (int leg = 0; leg < 3; ++leg) { int col = event.colJunction(iJun, leg); if (col == event[iGlu].acol()) event.colJunction(iJun, leg, event[iGlu].col()); } } } // Check that not the same colour or anticolour appears twice. for (int iCol = 0; iCol < int(colList.size()) - 1; ++iCol) { int col = colList[iCol]; for (int iCol2 = iCol + 1; iCol2 < int(colList.size()); ++iCol2) if (colList[iCol2] == col) { infoPtr->errorMsg("Warning in BeamRemnants::checkColours:" " colour appears twice"); if (!ALLOWCOLOURTWICE) return false; } } for (int iAcol = 0; iAcol < int(acolList.size()) - 1; ++iAcol) { int acol = acolList[iAcol]; for (int iAcol2 = iAcol + 1; iAcol2 < int(acolList.size()); ++iAcol2) if (acolList[iAcol2] == acol) { infoPtr->errorMsg("Warning in BeamRemnants::checkColours:" " anticolour appears twice"); if (!ALLOWCOLOURTWICE) return false; } } // Remove all matching colour-anticolour pairs. bool foundPair = true; while (foundPair && colList.size() > 0 && acolList.size() > 0) { foundPair = false; for (int iCol = 0; iCol < int(colList.size()); ++iCol) { for (int iAcol = 0; iAcol < int(acolList.size()); ++iAcol) { if (acolList[iAcol] == colList[iCol]) { colList[iCol] = colList.back(); colList.pop_back(); acolList[iAcol] = acolList.back(); acolList.pop_back(); foundPair = true; break; } } if (foundPair) break; } } // Check that remaining (anti)colours are accounted for by junctions. for (int iJun = 0; iJun < event.sizeJunction(); ++iJun) { int kindJun = event.kindJunction(iJun); for (int leg = 0; leg < 3; ++leg) { int colEnd = event.colJunction(iJun, leg); // Junction connected to three colours. if (kindJun == 1) { for (int iCol = 0; iCol < int(colList.size()); ++iCol) if (colList[iCol] == colEnd) { // Found colour match: remove and exit. colList[iCol] = colList.back(); colList.pop_back(); break; } } // Junction connected to three anticolours. else if (kindJun == 2) { for (int iAcol = 0; iAcol < int(acolList.size()); ++iAcol) if (acolList[iAcol] == colEnd) { // Found colour match: remove and exit. acolList[iAcol] = acolList.back(); acolList.pop_back(); break; } } // Other junction types else if ( kindJun == 3 || kindJun == 5) { for (int iCol = 0; iCol < int(colList.size()); ++iCol) if (colList[iCol] == colEnd) { // Found colour match: remove and exit. colList[iCol] = colList.back(); colList.pop_back(); break; } } // Other antijunction types else if ( kindJun == 4 || kindJun == 6) { for (int iAcol = 0; iAcol < int(acolList.size()); ++iAcol) if (acolList[iAcol] == colEnd) { // Found colour match: remove and exit. acolList[iAcol] = acolList.back(); acolList.pop_back(); break; } } // End junction check. } } // Repair step - sometimes needed when rescattering allowed. if (colList.size() > 0 || acolList.size() > 0) { infoPtr->errorMsg("Warning in BeamRemnants::checkColours:" " need to repair unmatched colours"); } while (colList.size() > 0 && acolList.size() > 0) { // Replace one colour and one anticolour index by a new common one. int colMatch = colList.back(); int acolMatch = acolList.back(); int colNew = event.nextColTag(); colList.pop_back(); acolList.pop_back(); for (int i = oldSize; i < event.size(); ++i) if (event[i].isFinal() && event[i].col() == colMatch) { event[i].col( colNew); break; } for (int i = oldSize; i < event.size(); ++i) if (event[i].isFinal() && event[i].acol() == acolMatch) { event[i].acol( colNew); break; } } // Done. return (colList.size() == 0 && acolList.size() == 0); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/BoseEinstein.cc0000644000175000017500000002447512217346245016040 0ustar sunsun// BoseEinstein.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the BoseEinsten class. #include "Pythia8/BoseEinstein.h" namespace Pythia8 { //========================================================================== // The BoseEinstein class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Enumeration of id codes and table for particle species considered. const int BoseEinstein::IDHADRON[9] = { 211, -211, 111, 321, -321, 130, 310, 221, 331 }; const int BoseEinstein::ITABLE[9] = { 0, 0, 0, 1, 1, 1, 1, 2, 3 }; // Distance between table entries, normalized to min( 2*mass, QRef). const double BoseEinstein::STEPSIZE = 0.05; // Skip shift for two extremely close particles, to avoid instabilities. const double BoseEinstein::Q2MIN = 1e-8; // Parameters of energy compensation procedure: maximally allowed // relative energy error, iterative stepsize, and number of iterations. const double BoseEinstein::COMPRELERR = 1e-10; const double BoseEinstein::COMPFACMAX = 1000.; const int BoseEinstein::NCOMPSTEP = 10; //-------------------------------------------------------------------------- // Find settings. Precalculate table used to find momentum shifts. bool BoseEinstein::init(Info* infoPtrIn, Settings& settings, ParticleData& particleData) { // Save pointer. infoPtr = infoPtrIn; // Main flags. doPion = settings.flag("BoseEinstein:Pion"); doKaon = settings.flag("BoseEinstein:Kaon"); doEta = settings.flag("BoseEinstein:Eta"); // Shape of Bose-Einstein enhancement/suppression. lambda = settings.parm("BoseEinstein:lambda"); QRef = settings.parm("BoseEinstein:QRef"); // Multiples and inverses (= "radii") of distance parameters in Q-space. QRef2 = 2. * QRef; QRef3 = 3. * QRef; R2Ref = 1. / (QRef * QRef); R2Ref2 = 1. / (QRef2 * QRef2); R2Ref3 = 1. / (QRef3 * QRef3); // Masses of particles with Bose-Einstein implemented. for (int iSpecies = 0; iSpecies < 9; ++iSpecies) mHadron[iSpecies] = particleData.m0( IDHADRON[iSpecies] ); // Pair pi, K, eta and eta' masses for use in tables. mPair[0] = 2. * mHadron[0]; mPair[1] = 2. * mHadron[3]; mPair[2] = 2. * mHadron[7]; mPair[3] = 2. * mHadron[8]; // Loop over the four required tables. Local variables. double Qnow, Q2now, centerCorr; for (int iTab = 0; iTab < 4; ++iTab) { m2Pair[iTab] = mPair[iTab] * mPair[iTab]; // Step size and number of steps in normal table. deltaQ[iTab] = STEPSIZE * min(mPair[iTab], QRef); nStep[iTab] = min( 199, 1 + int(3. * QRef / deltaQ[iTab]) ); maxQ[iTab] = (nStep[iTab] - 0.1) * deltaQ[iTab]; centerCorr = deltaQ[iTab] * deltaQ[iTab] / 12.; // Construct normal table recursively in Q space. shift[iTab][0] = 0.; for (int i = 1; i <= nStep[iTab]; ++i) { Qnow = deltaQ[iTab] * (i - 0.5); Q2now = Qnow * Qnow; shift[iTab][i] = shift[iTab][i - 1] + exp(-Q2now * R2Ref) * deltaQ[iTab] * (Q2now + centerCorr) / sqrt(Q2now + m2Pair[iTab]); } // Step size and number of steps in compensation table. deltaQ3[iTab] = STEPSIZE * min(mPair[iTab], QRef3); nStep3[iTab] = min( 199, 1 + int(9. * QRef / deltaQ3[iTab]) ); maxQ3[iTab] = (nStep3[iTab] - 0.1) * deltaQ3[iTab]; centerCorr = deltaQ3[iTab] * deltaQ3[iTab] / 12.; // Construct compensation table recursively in Q space. shift3[iTab][0] = 0.; for (int i = 1; i <= nStep3[iTab]; ++i) { Qnow = deltaQ3[iTab] * (i - 0.5); Q2now = Qnow * Qnow; shift3[iTab][i] = shift3[iTab][i - 1] + exp(-Q2now * R2Ref3) * deltaQ3[iTab] * (Q2now + centerCorr) / sqrt(Q2now + m2Pair[iTab]); } } // Done. return true; } //-------------------------------------------------------------------------- // Perform Bose-Einstein corrections on an event. bool BoseEinstein::shiftEvent( Event& event) { // Reset list of identical particles. hadronBE.resize(0); // Loop over all hadron species with BE effects. nStored[0] = 0; for (int iSpecies = 0; iSpecies < 9; ++iSpecies) { nStored[iSpecies + 1] = nStored[iSpecies]; if (!doPion && iSpecies <= 2) continue; if (!doKaon && iSpecies >= 3 && iSpecies <= 6) continue; if (!doEta && iSpecies >= 7) continue; // Properties of current hadron species. int idNow = IDHADRON[ iSpecies ]; int iTab = ITABLE[ iSpecies ]; // Loop through event record to store copies of current species. for (int i = 0; i < event.size(); ++i) if ( event[i].id() == idNow && event[i].isFinal() ) hadronBE.push_back( BoseEinsteinHadron( idNow, i, event[i].p(), event[i].m() ) ); nStored[iSpecies + 1] = hadronBE.size(); // Loop through pairs of identical particles and find shifts. for (int i1 = nStored[iSpecies]; i1 < nStored[iSpecies+1] - 1; ++i1) for (int i2 = i1 + 1; i2 < nStored[iSpecies+1]; ++i2) shiftPair( i1, i2, iTab); } // Must have at least two pairs to carry out compensation. if (nStored[9] < 2) return true; // Shift momenta and recalculate energies. double eSumOriginal = 0.; double eSumShifted = 0.; double eDiffByComp = 0.; for (int i = 0; i < nStored[9]; ++i) { eSumOriginal += hadronBE[i].p.e(); hadronBE[i].p += hadronBE[i].pShift; hadronBE[i].p.e( sqrt( hadronBE[i].p.pAbs2() + hadronBE[i].m2 ) ); eSumShifted += hadronBE[i].p.e(); eDiffByComp += dot3( hadronBE[i].pComp, hadronBE[i].p) / hadronBE[i].p.e(); } // Iterate compensation shift until convergence. int iStep = 0; while ( abs(eSumShifted - eSumOriginal) > COMPRELERR * eSumOriginal && abs(eSumShifted - eSumOriginal) < COMPFACMAX * abs(eDiffByComp) && iStep < NCOMPSTEP ) { ++iStep; double compFac = (eSumOriginal - eSumShifted) / eDiffByComp; eSumShifted = 0.; eDiffByComp = 0.; for (int i = 0; i < nStored[9]; ++i) { hadronBE[i].p += compFac * hadronBE[i].pComp; hadronBE[i].p.e( sqrt( hadronBE[i].p.pAbs2() + hadronBE[i].m2 ) ); eSumShifted += hadronBE[i].p.e(); eDiffByComp += dot3( hadronBE[i].pComp, hadronBE[i].p) / hadronBE[i].p.e(); } } // Error if no convergence, and then return without doing BE shift. // However, not grave enough to kill event, so return true. if ( abs(eSumShifted - eSumOriginal) > COMPRELERR * eSumOriginal ) { infoPtr->errorMsg("Warning in BoseEinstein::shiftEvent: " "no consistent BE shift topology found, so skip BE"); return true; } // Store new particle copies with shifted momenta. for (int i = 0; i < nStored[9]; ++i) { int iNew = event.copy( hadronBE[i].iPos, 99); event[ iNew ].p( hadronBE[i].p ); } // Done. return true; } //-------------------------------------------------------------------------- // Calculate shift and (unnormalized) compensation for pair. void BoseEinstein::shiftPair( int i1, int i2, int iTab) { // Calculate old relative momentum. double Q2old = m2(hadronBE[i1].p, hadronBE[i2].p) - m2Pair[iTab]; if (Q2old < Q2MIN) return; double Qold = sqrt(Q2old); double psFac = sqrt(Q2old + m2Pair[iTab]) / Q2old; // Calculate new relative momentum for normal shift. double Qmove = 0.; if (Qold < deltaQ[iTab]) Qmove = Qold / 3.; else if (Qold < maxQ[iTab]) { double realQbin = Qold / deltaQ[iTab]; int intQbin = int( realQbin ); double inter = (pow3(realQbin) - pow3(intQbin)) / (3 * intQbin * (intQbin + 1) + 1); Qmove = ( shift[iTab][intQbin] + inter * (shift[iTab][intQbin + 1] - shift[iTab][intQbin]) ) * psFac; } else Qmove = shift[iTab][nStep[iTab]] * psFac; double Q2new = Q2old * pow( Qold / (Qold + 3. * lambda * Qmove), 2. / 3.); // Calculate corresponding three-momentum shift. double Q2Diff = Q2new - Q2old; double p2DiffAbs = (hadronBE[i1].p - hadronBE[i2].p).pAbs2(); double p2AbsDiff = hadronBE[i1].p.pAbs2() - hadronBE[i2].p.pAbs2(); double eSum = hadronBE[i1].p.e() + hadronBE[i2].p.e(); double eDiff = hadronBE[i1].p.e() - hadronBE[i2].p.e(); double sumQ2E = Q2Diff + eSum * eSum; double rootA = eSum * eDiff * p2AbsDiff - p2DiffAbs * sumQ2E; double rootB = p2DiffAbs * sumQ2E - p2AbsDiff * p2AbsDiff; double factor = 0.5 * ( rootA + sqrtpos(rootA * rootA + Q2Diff * (sumQ2E - eDiff * eDiff) * rootB) ) / rootB; // Add shifts to sum. (Energy component dummy.) Vec4 pDiff = factor * (hadronBE[i1].p - hadronBE[i2].p); hadronBE[i1].pShift += pDiff; hadronBE[i2].pShift -= pDiff; // Calculate new relative momentum for compensation shift. double Qmove3 = 0.; if (Qold < deltaQ3[iTab]) Qmove3 = Qold / 3.; else if (Qold < maxQ3[iTab]) { double realQbin = Qold / deltaQ3[iTab]; int intQbin = int( realQbin ); double inter = (pow3(realQbin) - pow3(intQbin)) / (3 * intQbin * (intQbin + 1) + 1); Qmove3 = ( shift3[iTab][intQbin] + inter * (shift3[iTab][intQbin + 1] - shift3[iTab][intQbin]) ) * psFac; } else Qmove3 = shift3[iTab][nStep3[iTab]] *psFac; double Q2new3 = Q2old * pow( Qold / (Qold + 3. * lambda * Qmove3), 2. / 3.); // Calculate corresponding three-momentum shift. Q2Diff = Q2new3 - Q2old; sumQ2E = Q2Diff + eSum * eSum; rootA = eSum * eDiff * p2AbsDiff - p2DiffAbs * sumQ2E; rootB = p2DiffAbs * sumQ2E - p2AbsDiff * p2AbsDiff; factor = 0.5 * ( rootA + sqrtpos(rootA * rootA + Q2Diff * (sumQ2E - eDiff * eDiff) * rootB) ) / rootB; // Extra dampening factor to go from BE_3 to BE_32. factor *= 1. - exp(-Q2old * R2Ref2); // Add shifts to sum. (Energy component dummy.) pDiff = factor * (hadronBE[i1].p - hadronBE[i2].p); hadronBE[i1].pComp += pDiff; hadronBE[i2].pComp -= pDiff; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/HadronLevel.cc0000644000175000017500000010476612217346245015656 0ustar sunsun// HadronLevel.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the HadronLevel class. #include "Pythia8/HadronLevel.h" namespace Pythia8 { //========================================================================== // The HadronLevel class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // For breaking J-J string, pick a Gamma by taking a step with fictitious mass. const double HadronLevel::JJSTRINGM2MAX = 25.; const double HadronLevel::JJSTRINGM2FRAC = 0.1; // Iterate junction rest frame boost until convergence or too many tries. const double HadronLevel::CONVJNREST = 1e-5; const int HadronLevel::NTRYJNREST = 20; // Typical average transvere primary hadron mass . const double HadronLevel::MTHAD = 0.9; //-------------------------------------------------------------------------- // Find settings. Initialize HadronLevel classes as required. bool HadronLevel::init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, Couplings* couplingsPtrIn, TimeShower* timesDecPtr, RHadrons* rHadronsPtrIn, DecayHandler* decayHandlePtr, vector handledParticles) { // Save pointers. infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; couplingsPtr = couplingsPtrIn; rHadronsPtr = rHadronsPtrIn; // Main flags. doHadronize = settings.flag("HadronLevel:Hadronize"); doDecay = settings.flag("HadronLevel:Decay"); doBoseEinstein = settings.flag("HadronLevel:BoseEinstein"); // Boundary mass between string and ministring handling. mStringMin = settings.parm("HadronLevel:mStringMin"); // For junction processing. eNormJunction = settings.parm("StringFragmentation:eNormJunction"); // Allow R-hadron formation. allowRH = settings.flag("RHadrons:allow"); // Particles that should decay or not before Bose-Einstein stage. widthSepBE = settings.parm("BoseEinstein:widthSep"); // Hadron scattering --rjc doHadronScatter = settings.flag("HadronScatter:scatter"); hsAfterDecay = settings.flag("HadronScatter:afterDecay"); // Initialize auxiliary fragmentation classes. flavSel.init(settings, rndmPtr); pTSel.init(settings, *particleDataPtr, rndmPtr); zSel.init(settings, *particleDataPtr, rndmPtr); // Initialize auxiliary administrative class. colConfig.init(infoPtr, settings, &flavSel); // Initialize string and ministring fragmentation. stringFrag.init(infoPtr, settings, particleDataPtr, rndmPtr, &flavSel, &pTSel, &zSel); ministringFrag.init(infoPtr, settings, particleDataPtr, rndmPtr, &flavSel, &pTSel, &zSel); // Initialize particle decays. decays.init(infoPtr, settings, particleDataPtr, rndmPtr, couplingsPtr, timesDecPtr, &flavSel, decayHandlePtr, handledParticles); // Initialize BoseEinstein. boseEinstein.init(infoPtr, settings, *particleDataPtr); // Initialize HadronScatter --rjc if (doHadronScatter) hadronScatter.init(infoPtr, settings, rndmPtr, particleDataPtr); // Initialize Hidden-Valley fragmentation, if necessary. useHiddenValley = hiddenvalleyFrag.init(infoPtr, settings, particleDataPtr, rndmPtr); // Send flavour and z selection pointers to R-hadron machinery. rHadronsPtr->fragPtrs( &flavSel, &zSel); // Done. return true; } //-------------------------------------------------------------------------- // Hadronize and decay the next parton-level. bool HadronLevel::next( Event& event) { // Do Hidden-Valley fragmentation, if necessary. if (useHiddenValley) hiddenvalleyFrag.fragment(event); // Colour-octet onia states must be decayed to singlet + gluon. if (!decayOctetOnia(event)) return false; // Possibility of hadronization inside decay, but then no BE second time. // Hadron scattering, first pass only --rjc bool moreToDo, firstPass = true; bool doBoseEinsteinNow = doBoseEinstein; do { moreToDo = false; // First part: string fragmentation. if (doHadronize) { // Find the complete colour singlet configuration of the event. if (!findSinglets( event)) return false; // Fragment off R-hadrons, if necessary. if (allowRH && !rHadronsPtr->produce( colConfig, event)) return false; // Process all colour singlet (sub)system for (int iSub = 0; iSub < colConfig.size(); ++iSub) { // Collect sequentially all partons in a colour singlet subsystem. colConfig.collect(iSub, event); // String fragmentation of each colour singlet (sub)system. if ( colConfig[iSub].massExcess > mStringMin ) { if (!stringFrag.fragment( iSub, colConfig, event)) return false; // Low-mass string treated separately. Tell if diffractive system. } else { bool isDiff = infoPtr->isDiffractiveA() || infoPtr->isDiffractiveB(); if (!ministringFrag.fragment( iSub, colConfig, event, isDiff)) return false; } } } // Hadron scattering --rjc if (doHadronScatter && !hsAfterDecay && firstPass) hadronScatter.scatter(event); // Second part: sequential decays of short-lived particles (incl. K0). if (doDecay) { // Loop through all entries to find those that should decay. int iDec = 0; do { Particle& decayer = event[iDec]; if ( decayer.isFinal() && decayer.canDecay() && decayer.mayDecay() && (decayer.mWidth() > widthSepBE || decayer.idAbs() == 311) ) { decays.decay( iDec, event); if (decays.moreToDo()) moreToDo = true; } } while (++iDec < event.size()); } // Hadron scattering --rjc if (doHadronScatter && hsAfterDecay && firstPass) hadronScatter.scatter(event); // Third part: include Bose-Einstein effects among current particles. if (doBoseEinsteinNow) { if (!boseEinstein.shiftEvent(event)) return false; doBoseEinsteinNow = false; } // Fourth part: sequential decays also of long-lived particles. if (doDecay) { // Loop through all entries to find those that should decay. int iDec = 0; do { Particle& decayer = event[iDec]; if ( decayer.isFinal() && decayer.canDecay() && decayer.mayDecay() ) { decays.decay( iDec, event); if (decays.moreToDo()) moreToDo = true; } } while (++iDec < event.size()); } // Normally done first time around, but sometimes not (e.g. Upsilon). } while (moreToDo); // Done. return true; } //-------------------------------------------------------------------------- // Allow more decays if on/off switches changed. // Note: does not do sequential hadronization, e.g. for Upsilon. bool HadronLevel::moreDecays( Event& event) { // Colour-octet onia states must be decayed to singlet + gluon. if (!decayOctetOnia(event)) return false; // Loop through all entries to find those that should decay. int iDec = 0; do { if ( event[iDec].isFinal() && event[iDec].canDecay() && event[iDec].mayDecay() ) decays.decay( iDec, event); } while (++iDec < event.size()); // Done. return true; } //-------------------------------------------------------------------------- // Decay colour-octet onium states. bool HadronLevel::decayOctetOnia(Event& event) { // Onium states to be decayed. int idOnium[6] = { 9900443, 9900441, 9910441, 9900553, 9900551, 9910551 }; // Loop over particles and identify onia. for (int iDec = 0; iDec < event.size(); ++iDec) if (event[iDec].isFinal()) { int id = event[iDec].id(); bool isOnium = false; for (int j = 0; j < 6; ++j) if (id == idOnium[j]) isOnium = true; // Decay any onia encountered. if (isOnium) { if (!decays.decay( iDec, event)) return false; // Set colour flow by hand: gluon inherits octet-onium state. int iGlu = event.size() - 1; event[iGlu].cols( event[iDec].col(), event[iDec].acol() ); } } // Done. return true; } //-------------------------------------------------------------------------- // Trace colour flow in the event to form colour singlet subsystems. bool HadronLevel::findSinglets(Event& event) { // Find a list of final partons and of all colour ends and gluons. iColEnd.resize(0); iAcolEnd.resize(0); iColAndAcol.resize(0); for (int i = 0; i < event.size(); ++i) if (event[i].isFinal()) { if (event[i].col() > 0 && event[i].acol() > 0) iColAndAcol.push_back(i); else if (event[i].col() > 0) iColEnd.push_back(i); else if (event[i].acol() > 0) iAcolEnd.push_back(i); } // Begin arrange the partons into separate colour singlets. colConfig.clear(); iPartonJun.resize(0); iPartonAntiJun.resize(0); // No need to do anything if no final partons. if (iColEnd.size() == 0 && iAcolEnd.size() == 0 && iColAndAcol.size() == 0) return true; // Junctions: loop over them, and identify kind. for (int iJun = 0; iJun < event.sizeJunction(); ++iJun) if (event.remainsJunction(iJun)) { event.remainsJunction(iJun, false); int kindJun = event.kindJunction(iJun); iParton.resize(0); // Loop over junction legs. for (int iCol = 0; iCol < 3; ++iCol) { int indxCol = event.colJunction(iJun, iCol); iParton.push_back( -(10 + 10 * iJun + iCol) ); // Junctions: find color ends. if (kindJun % 2 == 1 && !traceFromAcol(indxCol, event, iJun, iCol)) return false; // Antijunctions: find anticolor ends. if (kindJun % 2 == 0 && !traceFromCol(indxCol, event, iJun, iCol)) return false; } // Reject triple- and higher-junction systems (physics not implemented). int otherJun = 0; for (int i = 0; i < int(iParton.size()); ++i) if (iParton[i] < 0 && abs(iParton[i]) / 10 != iJun + 1) { if (otherJun == 0) otherJun = abs(iParton[i]) / 10; else if (abs(iParton[i]) / 10 != otherJun) { infoPtr->errorMsg("Error in HadronLevel::findSinglets: " "too many junction-junction connections"); return false; } } // Keep in memory a junction hooked up with an antijunction, // else store found single-junction system. int nNeg = 0; for (int i = 0; i < int(iParton.size()); ++i) if (iParton[i] < 0) ++nNeg; if (nNeg > 3 && kindJun % 2 == 1) { for (int i = 0; i < int(iParton.size()); ++i) iPartonJun.push_back(iParton[i]); } else if (nNeg > 3 && kindJun % 2 == 0) { for (int i = 0; i < int(iParton.size()); ++i) iPartonAntiJun.push_back(iParton[i]); } else { // A junction may be eliminated by insert if two quarks are nearby. int nJunOld = event.sizeJunction(); if (!colConfig.insert(iParton, event)) return false; if (event.sizeJunction() < nJunOld) --iJun; } } // Split junction-antijunction system into two, and store those. // (Only one system in extreme cases, and then second empty.) if (iPartonJun.size() > 0 && iPartonAntiJun.size() > 0) { if (!splitJunctionPair(event)) return false; if (!colConfig.insert(iPartonJun, event)) return false; if (iPartonAntiJun.size() > 0) if (!colConfig.insert(iPartonAntiJun, event)) return false; // Error if only one of junction and antijuction left here. } else if (iPartonJun.size() > 0 || iPartonAntiJun.size() > 0) { infoPtr->errorMsg("Error in HadronLevel::findSinglets: " "unmatched (anti)junction"); return false; } // Open strings: pick up each colour end and trace to its anticolor end. for (int iEnd = 0; iEnd < int(iColEnd.size()); ++iEnd) { iParton.resize(0); iParton.push_back( iColEnd[iEnd] ); int indxCol = event[ iColEnd[iEnd] ].col(); if (!traceFromCol(indxCol, event)) return false; // Store found open string system. Analyze its properties. if (!colConfig.insert(iParton, event)) return false; } // Closed strings : begin at any gluon and trace until back at it. while (iColAndAcol.size() > 0) { iParton.resize(0); iParton.push_back( iColAndAcol[0] ); int indxCol = event[ iColAndAcol[0] ].col(); int indxAcol = event[ iColAndAcol[0] ].acol(); iColAndAcol[0] = iColAndAcol.back(); iColAndAcol.pop_back(); if (!traceInLoop(indxCol, indxAcol, event)) return false; // Store found closed string system. Analyze its properties. if (!colConfig.insert(iParton, event)) return false; } // Done. return true; } //-------------------------------------------------------------------------- // Trace a colour line, from a colour to an anticolour. bool HadronLevel::traceFromCol(int indxCol, Event& event, int iJun, int iCol) { // Junction kind, if any. int kindJun = (iJun >= 0) ? event.kindJunction(iJun) : 0; // Begin to look for a matching anticolour. int loop = 0; int loopMax = iColAndAcol.size() + 2; bool hasFound = false; do { ++loop; hasFound= false; // First check list of matching anticolour ends. for (int i = 0; i < int(iAcolEnd.size()); ++i) if (event[ iAcolEnd[i] ].acol() == indxCol) { iParton.push_back( iAcolEnd[i] ); indxCol = 0; iAcolEnd[i] = iAcolEnd.back(); iAcolEnd.pop_back(); hasFound = true; break; } // Then check list of intermediate gluons. if (!hasFound) for (int i = 0; i < int(iColAndAcol.size()); ++i) if (event[ iColAndAcol[i] ].acol() == indxCol) { iParton.push_back( iColAndAcol[i] ); // Update to new colour. Remove gluon. indxCol = event[ iColAndAcol[i] ].col(); if (kindJun > 0) event.endColJunction(iJun, iCol, indxCol); iColAndAcol[i] = iColAndAcol.back(); iColAndAcol.pop_back(); hasFound = true; break; } // In a pinch, check list of opposite-sign junction end colours. // Store in iParton list as -(10 + 10 * iAntiJun + iAntiLeg). if (!hasFound && kindJun % 2 == 0 && event.sizeJunction() > 1) for (int iAntiJun = 0; iAntiJun < event.sizeJunction(); ++iAntiJun) if (iAntiJun != iJun && event.kindJunction(iAntiJun) %2 == 1) for (int iColAnti = 0; iColAnti < 3; ++iColAnti) if (event.endColJunction(iAntiJun, iColAnti) == indxCol) { iParton.push_back( -(10 + 10 * iAntiJun + iColAnti) ); indxCol = 0; hasFound = true; break; } // Keep on tracing via gluons until reached end of leg. } while (hasFound && indxCol > 0 && loop < loopMax); // Something went wrong in colour tracing. if (!hasFound || loop == loopMax) { infoPtr->errorMsg("Error in HadronLevel::traceFromCol: " "colour tracing failed"); return false; } // Done. return true; } //-------------------------------------------------------------------------- // Trace a colour line, from an anticolour to a colour. bool HadronLevel::traceFromAcol(int indxCol, Event& event, int iJun, int iCol) { // Junction kind, if any. int kindJun = (iJun >= 0) ? event.kindJunction(iJun) : 0; // Begin to look for a matching colour. int loop = 0; int loopMax = iColAndAcol.size() + 2; bool hasFound = false; do { ++loop; hasFound= false; // First check list of matching colour ends. for (int i = 0; i < int(iColEnd.size()); ++i) if (event[ iColEnd[i] ].col() == indxCol) { iParton.push_back( iColEnd[i] ); indxCol = 0; iColEnd[i] = iColEnd.back(); iColEnd.pop_back(); hasFound = true; break; } // Then check list of intermediate gluons. if (!hasFound) for (int i = 0; i < int(iColAndAcol.size()); ++i) if (event[ iColAndAcol[i] ].col() == indxCol) { iParton.push_back( iColAndAcol[i] ); // Update to new colour. Remove gluon. indxCol = event[ iColAndAcol[i] ].acol(); if (kindJun > 0) event.endColJunction(iJun, iCol, indxCol); iColAndAcol[i] = iColAndAcol.back(); iColAndAcol.pop_back(); hasFound = true; break; } // In a pinch, check list of opposite-sign junction end colours. // Store in iParton list as -(10 + 10 * iAntiJun + iLeg). if (!hasFound && kindJun % 2 == 1 && event.sizeJunction() > 1) for (int iAntiJun = 0; iAntiJun < event.sizeJunction(); ++iAntiJun) if (iAntiJun != iJun && event.kindJunction(iAntiJun) % 2 == 0) for (int iColAnti = 0; iColAnti < 3; ++iColAnti) if (event.endColJunction(iAntiJun, iColAnti) == indxCol) { iParton.push_back( -(10 + 10 * iAntiJun + iColAnti) ); indxCol = 0; hasFound = true; break; } // Keep on tracing via gluons until reached end of leg. } while (hasFound && indxCol > 0 && loop < loopMax); // Something went wrong in colour tracing. if (!hasFound || loop == loopMax) { infoPtr->errorMsg("Error in HadronLevel::traceFromAcol: " "colour tracing failed"); return false; } // Done. return true; } //-------------------------------------------------------------------------- // Trace a colour loop, from a colour back to the anticolour of the same. bool HadronLevel::traceInLoop(int indxCol, int indxAcol, Event& event) { // Move around until back where begun. int loop = 0; int loopMax = iColAndAcol.size() + 2; bool hasFound = false; do { ++loop; hasFound= false; // Check list of gluons. for (int i = 0; i < int(iColAndAcol.size()); ++i) if (event[ iColAndAcol[i] ].acol() == indxCol) { iParton.push_back( iColAndAcol[i] ); indxCol = event[ iColAndAcol[i] ].col(); iColAndAcol[i] = iColAndAcol.back(); iColAndAcol.pop_back(); hasFound = true; break; } } while (hasFound && indxCol != indxAcol && loop < loopMax); // Something went wrong in colour tracing. if (!hasFound || loop == loopMax) { infoPtr->errorMsg("Error in HadronLevel::traceInLoop: " "colour tracing failed"); return false; } // Done. return true; } //-------------------------------------------------------------------------- // Split junction-antijunction system into two, or simplify other way. bool HadronLevel::splitJunctionPair(Event& event) { // Construct separate index arrays for the three junction legs. int identJun = (-iPartonJun[0])/10; iJunLegA.resize(0); iJunLegB.resize(0); iJunLegC.resize(0); int leg = -1; for (int i = 0; i < int(iPartonJun.size()); ++ i) { if ( (-iPartonJun[i])/10 == identJun) ++leg; if (leg == 0) iJunLegA.push_back( iPartonJun[i] ); else if (leg == 1) iJunLegB.push_back( iPartonJun[i] ); else iJunLegC.push_back( iPartonJun[i] ); } // Construct separate index arrays for the three antijunction legs. int identAnti = (-iPartonAntiJun[0])/10; iAntiLegA.resize(0); iAntiLegB.resize(0); iAntiLegC.resize(0); leg = -1; for (int i = 0; i < int(iPartonAntiJun.size()); ++ i) { if ( (-iPartonAntiJun[i])/10 == identAnti) ++leg; if (leg == 0) iAntiLegA.push_back( iPartonAntiJun[i] ); else if (leg == 1) iAntiLegB.push_back( iPartonAntiJun[i] ); else iAntiLegC.push_back( iPartonAntiJun[i] ); } // Find interjunction legs, i.e. between junction and antijunction. int nMatch = 0; int legJun[3], legAnti[3], nGluLeg[3]; if (iJunLegA.back() < 0) { legJun[nMatch] = 0; legAnti[nMatch] = (-iJunLegA.back())%10; ++nMatch;} if (iJunLegB.back() < 0) { legJun[nMatch] = 1; legAnti[nMatch] = (-iJunLegB.back())%10; ++nMatch;} if (iJunLegC.back() < 0) { legJun[nMatch] = 2; legAnti[nMatch] = (-iJunLegC.back())%10; ++nMatch;} // Loop over interjunction legs. for (int iMatch = 0; iMatch < nMatch; ++iMatch) { vector& iJunLeg = (legJun[iMatch] == 0) ? iJunLegA : ( (legJun[iMatch] == 1) ? iJunLegB : iJunLegC ); vector& iAntiLeg = (legAnti[iMatch] == 0) ? iAntiLegA : ( (legAnti[iMatch] == 1) ? iAntiLegB : iAntiLegC ); // Find number of gluons on each. Do nothing for now if none. nGluLeg[iMatch] = iJunLeg.size() + iAntiLeg.size() - 4; if (nGluLeg[iMatch] == 0) continue; // Else pick up the gluons on the interjunction leg in order. iGluLeg.resize(0); for (int i = 1; i < int(iJunLeg.size()) - 1; ++i) iGluLeg.push_back( iJunLeg[i] ); for (int i = int(iAntiLeg.size()) - 2; i > 0; --i) iGluLeg.push_back( iAntiLeg[i] ); // Remove those gluons from the junction/antijunction leg lists. iJunLeg.resize(1); iAntiLeg.resize(1); // Pick a new quark at random; for simplicity no diquarks. int idQ = flavSel.pickLightQ(); int colQ, acolQ; // If one gluon on leg, split it into a collinear q-qbar pair. if (iGluLeg.size() == 1) { // Store the new q qbar pair, sharing gluon colour and momentum. colQ = event[ iGluLeg[0] ].col(); acolQ = event[ iGluLeg[0] ].acol(); Vec4 pQ = 0.5 * event[ iGluLeg[0] ].p(); double mQ = 0.5 * event[ iGluLeg[0] ].m(); int iQ = event.append( idQ, 75, iGluLeg[0], 0, 0, 0, colQ, 0, pQ, mQ ); int iQbar = event.append( -idQ, 75, iGluLeg[0], 0, 0, 0, 0, acolQ, pQ, mQ ); // Mark split gluon and update junction and antijunction legs. event[ iGluLeg[0] ].statusNeg(); event[ iGluLeg[0] ].daughters( iQ, iQbar); iJunLeg.push_back(iQ); iAntiLeg.push_back(iQbar); // If several gluons on the string, decide which g-g region to split up. } else { // Evaluate mass-squared for all adjacent gluon pairs. m2Pair.resize(0); double m2Sum = 0.; for (int i = 0; i < int(iGluLeg.size()) - 1; ++i) { double m2Now = 0.5 * event[ iGluLeg[i] ].p() * event[ iGluLeg[i + 1] ].p(); m2Pair.push_back(m2Now); m2Sum += m2Now; } // Pick breakup region with probability proportional to mass-squared. double m2Reg = m2Sum * rndmPtr->flat(); int iReg = -1; do m2Reg -= m2Pair[++iReg]; while (m2Reg > 0. && iReg < int(iGluLeg.size()) - 1); m2Reg = m2Pair[iReg]; // Pick breaking point of string in chosen region (symmetrically). double m2Temp = min( JJSTRINGM2MAX, JJSTRINGM2FRAC * m2Reg); double xPos = 0.5; double xNeg = 0.5; do { double zTemp = zSel.zFrag( idQ, 0, m2Temp); xPos = 1. - zTemp; xNeg = m2Temp / (zTemp * m2Reg); } while (xNeg > 1.); if (rndmPtr->flat() > 0.5) swap(xPos, xNeg); // Pick up two "mother" gluons of breakup. Mark them decayed. Particle& gJun = event[ iGluLeg[iReg] ]; Particle& gAnti = event[ iGluLeg[iReg + 1] ]; gJun.statusNeg(); gAnti.statusNeg(); int dau1 = event.size(); gJun.daughters(dau1, dau1 + 3); gAnti.daughters(dau1, dau1 + 3); int mother1 = min( iGluLeg[iReg], iGluLeg[iReg + 1]); int mother2 = max( iGluLeg[iReg], iGluLeg[iReg + 1]); // Can keep one of old colours but need one new so unambiguous. colQ = gJun.acol(); acolQ = event.nextColTag(); // Store copied gluons with reduced momenta. int iGjun = event.append( 21, 75, mother1, mother2, 0, 0, gJun.col(), gJun.acol(), (1. - 0.5 * xPos) * gJun.p(), (1. - 0.5 * xPos) * gJun.m()); int iGanti = event.append( 21, 75, mother1, mother2, 0, 0, acolQ, gAnti.acol(), (1. - 0.5 * xNeg) * gAnti.p(), (1. - 0.5 * xNeg) * gAnti.m()); // Store the new q qbar pair with remaining momenta. int iQ = event.append( idQ, 75, mother1, mother2, 0, 0, colQ, 0, 0.5 * xNeg * gAnti.p(), 0.5 * xNeg * gAnti.m() ); int iQbar = event.append( -idQ, 75, mother1, mother2, 0, 0, 0, acolQ, 0.5 * xPos * gJun.p(), 0.5 * xPos * gJun.m() ); // Update junction and antijunction legs with gluons and quarks. for (int i = 0; i < iReg; ++i) iJunLeg.push_back( iGluLeg[i] ); iJunLeg.push_back(iGjun); iJunLeg.push_back(iQ); for (int i = int(iGluLeg.size()) - 1; i > iReg + 1; --i) iAntiLeg.push_back( iGluLeg[i] ); iAntiLeg.push_back(iGanti); iAntiLeg.push_back(iQbar); } // Update end colours for both g -> q qbar and g g -> g g q qbar. event.endColJunction(identJun - 1, legJun[iMatch], colQ); event.endColJunction(identAnti - 1, legAnti[iMatch], acolQ); } // Update list of interjunction legs after splittings above. int iMatchUp = 0; while (iMatchUp < nMatch) { if (nGluLeg[iMatchUp] > 0) { for (int i = iMatchUp; i < nMatch - 1; ++i) { legJun[i] = legJun[i + 1]; legAnti[i] = legAnti[i + 1]; nGluLeg[i] = nGluLeg[i + 1]; } --nMatch; } else ++iMatchUp; } // Should not ever have three empty interjunction legs. if (nMatch == 3) { infoPtr->errorMsg("Error in HadronLevel::splitJunctionPair: " "three empty junction-junction legs"); return false; } // If two legs are empty, then collapse system to a single string. if (nMatch == 2) { int legJunLeft = 3 - legJun[0] - legJun[1]; int legAntiLeft = 3 - legAnti[0] - legAnti[1]; vector& iJunLeg = (legJunLeft == 0) ? iJunLegA : ( (legJunLeft == 1) ? iJunLegB : iJunLegC ); vector& iAntiLeg = (legAntiLeft == 0) ? iAntiLegA : ( (legAntiLeft == 1) ? iAntiLegB : iAntiLegC ); iPartonJun.resize(0); for (int i = int(iJunLeg.size()) - 1; i > 0; --i) iPartonJun.push_back( iJunLeg[i] ); for (int i = 1; i < int(iAntiLeg.size()); ++i) iPartonJun.push_back( iAntiLeg[i] ); // Match up the colours where the strings are joined. int iColJoin = iJunLeg[1]; int iAcolJoin = iAntiLeg[1]; event[iAcolJoin].acol( event[iColJoin].col() ); // Other string system empty. Remove junctions from their list. Done. iPartonAntiJun.resize(0); event.eraseJunction( max(identJun, identAnti) - 1); event.eraseJunction( min(identJun, identAnti) - 1); return true; } // If one leg is empty then, depending on string length, either // (a) annihilate junction and antijunction into two simple strings, or // (b) split the empty leg by borrowing energy from nearby legs. if (nMatch == 1) { // Identify the two external legs of either junction. vector& iJunLeg0 = (legJun[0] == 0) ? iJunLegB : iJunLegA; vector& iJunLeg1 = (legJun[0] == 2) ? iJunLegB : iJunLegC; vector& iAntiLeg0 = (legAnti[0] == 0) ? iAntiLegB : iAntiLegA; vector& iAntiLeg1 = (legAnti[0] == 2) ? iAntiLegB : iAntiLegC; // Simplified procedure: mainly study first parton on each leg. Vec4 pJunLeg0 = event[ iJunLeg0[1] ].p(); Vec4 pJunLeg1 = event[ iJunLeg1[1] ].p(); Vec4 pAntiLeg0 = event[ iAntiLeg0[1] ].p(); Vec4 pAntiLeg1 = event[ iAntiLeg1[1] ].p(); // Starting frame hopefully intermediate to two junction directions. Vec4 pStart = pJunLeg0 / pJunLeg0.e() + pJunLeg1 / pJunLeg1.e() + pAntiLeg0 / pAntiLeg0.e() + pAntiLeg1 / pAntiLeg1.e(); // Loop over iteration to junction/antijunction rest frames (JRF/ARF). RotBstMatrix MtoJRF, MtoARF; Vec4 pInJRF[3], pInARF[3]; for (int iJun = 0; iJun < 2; ++iJun) { int offset = (iJun == 0) ? 0 : 2; // Iterate from system rest frame towards the junction rest frame. RotBstMatrix MtoRF, Mstep; MtoRF.bstback(pStart); Vec4 pInRF[4]; int iter = 0; do { ++iter; // Find rest-frame momenta on the three sides of the junction. // Only consider first parton on each leg, for simplicity. pInRF[0 + offset] = pJunLeg0; pInRF[1 + offset] = pJunLeg1; pInRF[2 - offset] = pAntiLeg0; pInRF[3 - offset] = pAntiLeg1; for (int i = 0; i < 4; ++i) pInRF[i].rotbst(MtoRF); // For third side add both legs beyond other junction, weighted. double wt2 = 1. - exp( -pInRF[2].e() / eNormJunction); double wt3 = 1. - exp( -pInRF[3].e() / eNormJunction); pInRF[2] = wt2 * pInRF[2] + wt3 * pInRF[3]; // Find new junction rest frame from the set of momenta. Mstep = stringFrag.junctionRestFrame( pInRF[0], pInRF[1], pInRF[2]); MtoRF.rotbst( Mstep ); } while (iter < 3 || (Mstep.deviation() > CONVJNREST && iter < NTRYJNREST) ); // Store final boost and rest-frame (weighted) momenta. if (iJun == 0) { MtoJRF = MtoRF; for (int i = 0; i < 3; ++i) pInJRF[i] = pInRF[i]; } else { MtoARF = MtoRF; for (int i = 0; i < 3; ++i) pInARF[i] = pInRF[i]; } } // Opposite operations: boost from JRF/ARF to original system. RotBstMatrix MfromJRF = MtoJRF; MfromJRF.invert(); RotBstMatrix MfromARF = MtoARF; MfromARF.invert(); // Velocity vectors of junctions and momentum of legs in lab frame. Vec4 vJun(0., 0., 0., 1.); vJun.rotbst(MfromJRF); Vec4 vAnti(0., 0., 0., 1.); vAnti.rotbst(MfromARF); Vec4 pLabJ[3], pLabA[3]; for (int i = 0; i < 3; ++i) { pLabJ[i] = pInJRF[i]; pLabJ[i].rotbst(MfromJRF); pLabA[i] = pInARF[i]; pLabA[i].rotbst(MfromARF); } // Calculate Lambda-measure length of three possible topologies. double vJvA = vJun * vAnti; double vJvAe2y = vJvA + sqrt(vJvA*vJvA - 1.); double LambdaJA = (2. * pInJRF[0].e()) * (2. * pInJRF[1].e()) * (2. * pInARF[0].e()) * (2. * pInARF[1].e()) * vJvAe2y; double Lambda00 = (2. * pLabJ[0] * pLabA[0]) * (2. * pLabJ[1] * pLabA[1]); double Lambda01 = (2. * pLabJ[0] * pLabA[1]) * (2. * pLabJ[1] * pLabA[0]); // Case when either topology without junctions is the shorter one. if (LambdaJA > min( Lambda00, Lambda01)) { vector& iAntiMatch0 = (Lambda00 < Lambda01) ? iAntiLeg0 : iAntiLeg1; vector& iAntiMatch1 = (Lambda00 < Lambda01) ? iAntiLeg1 : iAntiLeg0; // Define two quark-antiquark strings. iPartonJun.resize(0); for (int i = int(iJunLeg0.size()) - 1; i > 0; --i) iPartonJun.push_back( iJunLeg0[i] ); for (int i = 1; i < int(iAntiMatch0.size()); ++i) iPartonJun.push_back( iAntiMatch0[i] ); iPartonAntiJun.resize(0); for (int i = int(iJunLeg1.size()) - 1; i > 0; --i) iPartonAntiJun.push_back( iJunLeg1[i] ); for (int i = 1; i < int(iAntiMatch1.size()); ++i) iPartonAntiJun.push_back( iAntiMatch1[i] ); // Match up the colours where the strings are joined. int iColJoin = iJunLeg0[1]; int iAcolJoin = iAntiMatch0[1]; event[iAcolJoin].acol( event[iColJoin].col() ); iColJoin = iJunLeg1[1]; iAcolJoin = iAntiMatch1[1]; event[iAcolJoin].acol( event[iColJoin].col() ); // Remove junctions from their list. Done. event.eraseJunction( max(identJun, identAnti) - 1); event.eraseJunction( min(identJun, identAnti) - 1); return true; } // Case where junction and antijunction to be separated. // Shuffle (p+/p-) momentum of order between systems, // times 2/3 for 120 degree in JRF, times 1/2 for two legs, // but not more than half of what nearest parton carries. double eShift = MTHAD / (3. * sqrt(vJvAe2y)); double fracJ0 = min(0.5, eShift / pInJRF[0].e()); double fracJ1 = min(0.5, eShift / pInJRF[0].e()); Vec4 pFromJun = fracJ0 * pJunLeg0 + fracJ1 * pJunLeg1; double fracA0 = min(0.5, eShift / pInARF[0].e()); double fracA1 = min(0.5, eShift / pInARF[0].e()); Vec4 pFromAnti = fracA0 * pAntiLeg0 + fracA1 * pAntiLeg1; // Pick a new quark at random; for simplicity no diquarks. int idQ = flavSel.pickLightQ(); // Copy junction partons with scaled-down momenta and update legs. int mother1 = min(iJunLeg0[1], iJunLeg1[1]); int mother2 = max(iJunLeg0[1], iJunLeg1[1]); int iNew1 = event.copy(iJunLeg0[1], 76); event[iNew1].rescale5(1. - fracJ0); iJunLeg0[1] = iNew1; int iNew2 = event.copy(iJunLeg1[1], 76); event[iNew2].rescale5(1. - fracJ1); iJunLeg1[1] = iNew2; // Update junction colour and store quark with antijunction momentum. // Store history as 2 -> 3 step for consistency. int colQ = event.nextColTag(); event.endColJunction(identJun - 1, legJun[0], colQ); int iNewJ = event.append( idQ, 76, mother1, mother2, 0, 0, colQ, 0, pFromAnti, pFromAnti.mCalc() ); event[mother1].daughters( iNew1, iNewJ); event[mother2].daughters( iNew1, iNewJ); event[iNew1].mothers( mother1, mother2); event[iNew2].mothers( mother1, mother2); // Copy anti junction partons with scaled-down momenta and update legs. mother1 = min(iAntiLeg0[1], iAntiLeg1[1]); mother2 = max(iAntiLeg0[1], iAntiLeg1[1]); iNew1 = event.copy(iAntiLeg0[1], 76); event[iNew1].rescale5(1. - fracA0); iAntiLeg0[1] = iNew1; iNew2 = event.copy(iAntiLeg1[1], 76); event[iNew2].rescale5(1. - fracA1); iAntiLeg1[1] = iNew2; // Update antijunction anticolour and store antiquark with junction // momentum. Store history as 2 -> 3 step for consistency. int acolQ = event.nextColTag(); event.endColJunction(identAnti - 1, legAnti[0], acolQ); int iNewA = event.append( -idQ, 76, mother1, mother2, 0, 0, 0, acolQ, pFromJun, pFromJun.mCalc() ); event[mother1].daughters( iNew1, iNewA); event[mother2].daughters( iNew1, iNewA); event[iNew1].mothers( mother1, mother2); event[iNew2].mothers( mother1, mother2); // Bookkeep new quark and antiquark on third legs. if (legJun[0] == 0) iJunLegA[1] = iNewJ; else if (legJun[0] == 1) iJunLegB[1] = iNewJ; else iJunLegC[1] = iNewJ; if (legAnti[0] == 0) iAntiLegA[1] = iNewA; else if (legAnti[0] == 1) iAntiLegB[1] = iNewA; else iAntiLegC[1] = iNewA; // Done with splitting junction from antijunction. } // Put together new junction parton list. iPartonJun.resize(0); for (int i = 0; i < int(iJunLegA.size()); ++i) iPartonJun.push_back( iJunLegA[i] ); for (int i = 0; i < int(iJunLegB.size()); ++i) iPartonJun.push_back( iJunLegB[i] ); for (int i = 0; i < int(iJunLegC.size()); ++i) iPartonJun.push_back( iJunLegC[i] ); // Put together new antijunction parton list. iPartonAntiJun.resize(0); for (int i = 0; i < int(iAntiLegA.size()); ++i) iPartonAntiJun.push_back( iAntiLegA[i] ); for (int i = 0; i < int(iAntiLegB.size()); ++i) iPartonAntiJun.push_back( iAntiLegB[i] ); for (int i = 0; i < int(iAntiLegC.size()); ++i) iPartonAntiJun.push_back( iAntiLegC[i] ); // Now the two junction systems are separated and can be stored. return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaGeneric.cc0000644000175000017500000003360512217346250015775 0ustar sunsun// SigmaGeneric.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Johan Bijnens, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for various generic // production processes, to be used as building blocks for some BSM processes. // Currently represented by QCD pair production of colour triplet objects, // with spin either 0, 1/2 or 1. // Cross sections are only provided for fixed m3 = m4, so do some gymnastics: // i) s34Avg picked so that beta34 same when s3, s4 -> s34Avg. // ii) tHQ = tH - mQ^2 = -0.5 sH (1 - beta34 cos(thetaH)) for m3 = m4 = mQ, // but tH - uH = sH beta34 cos(thetaH) also for m3 != m4, so use // tH, uH selected for m3 != m4 to derive tHQ, uHQ valid for m3 = m4. #include "Pythia8/SigmaGeneric.h" namespace Pythia8 { //========================================================================== // Sigma2gg2qGqGbar class. // Cross section for g g -> qG qGbar (generic quark of spin 0, 1/2 or 1). //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2qGqGbar::initProc() { // Number of colours. Anomalous coupling kappa - 1 used for vector state. nCHV = settingsPtr->mode("HiddenValley:Ngauge"); kappam1 = settingsPtr->parm("HiddenValley:kappa") - 1.; hasKappa = (abs(kappam1) > 1e-8); // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(idNew, -idNew); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2gg2qGqGbar::sigmaKin() { // Modified Mandelstam variables for massive kinematics with m3 = m4. double delta = 0.25 * pow2(s3 - s4) / sH; double s34Avg = 0.5 * (s3 + s4) - delta; double tHavg = tH - delta; double uHavg = uH - delta; double tHQ = -0.5 * (sH - tH + uH); double uHQ = -0.5 * (sH + tH - uH); double tHQ2 = tHQ * tHQ; double uHQ2 = uHQ * uHQ; // Evaluate cross section for spin 0 colour triplet. if (spinSave == 0) { sigSum = 0.5 * ( 7. / 48. + 3. * pow2(uHavg - tHavg) / (16. * sH2) ) * ( 1. + 2. * s34Avg * tHavg / pow2(tHavg - s34Avg) + 2. * s34Avg * uHavg / pow2(uHavg - s34Avg) + 4. * pow2(s34Avg) / ((tHavg - s34Avg) * (uHavg - s34Avg)) ); // Equal probability for two possible colour flows. sigTS = 0.5 * sigSum; sigUS = sigTS; } // Evaluate cross section for spin 1/2 colour triplet. else if (spinSave == 1) { double tumHQ = tHQ * uHQ - s34Avg * sH; sigTS = ( uHQ / tHQ - 2.25 * uHQ2 / sH2 + 4.5 * s34Avg * tumHQ / ( sH * tHQ2) + 0.5 * s34Avg * (tHQ + s34Avg) / tHQ2 - s34Avg*s34Avg / (sH * tHQ) ) / 6.; sigUS = ( tHQ / uHQ - 2.25 * tHQ2 / sH2 + 4.5 * s34Avg * tumHQ / ( sH * uHQ2) + 0.5 * s34Avg * (uHQ + s34Avg) / uHQ2 - s34Avg*s34Avg / (sH * uHQ) ) / 6.; sigSum = sigTS + sigUS; } // Evaluate cross section for spin 1 colour triplet. else { double tmu = tHavg - uHavg; double s34Pos = s34Avg / sH; double s34Pos2 = s34Pos * s34Pos; double s34Neg = sH / s34Avg; double s34Neg2 = s34Neg * s34Neg; sigSum = pow2(tmu) * sH2 * (241./1536. - 1./32. * s34Pos + 9./16. * s34Pos2) + pow4(tmu) * (37./512. + 9./64. * s34Pos) + pow6(tmu) * (9./512. / sH2) + sH2 * sH2 * (133./1536. - 7./64. * s34Pos + 7./16. * s34Pos2); // Anomalous coupling. if (hasKappa) sigSum += pow2(tmu) * sH2 * (kappam1 * (143./384. - 7./3072 * s34Neg) + pow2(kappam1) * (- 1./768. * s34Neg + 185./768.) + pow3(kappam1) * (- 7./3072. * s34Neg2 - 25./3072. * s34Neg + 67./1536.) + pow4(kappam1) * (- 37./49152. * s34Neg2 - 25./6144. * s34Neg + 5./1536.) ) + pow4(tmu) * (kappam1 * 3./32. + pow2(kappam1) * (7./6144. * s34Neg2 - 7./768. * s34Neg + 3./128.) + pow3(kappam1) * (7./6144. * s34Neg2 - 7./1536. * s34Neg) + pow4(kappam1) * (- 1./49152. * s34Neg2 + 5./6144. * s34Neg) ) + pow6(tmu) * pow4(kappam1) * 13./49152. / pow2(s34Avg) + sH2 * sH2 * ( kappam1 * 77./384. + pow2(kappam1) * (7./6144. * s34Neg2 + 1./96.* s34Neg + 39./256.) + pow3(kappam1) * (7./6144. * s34Neg2 + 13./1024. * s34Neg + 61./1536.) + pow4(kappam1) * (25./49152. * s34Neg2 + 5./1536. * s34Neg + 1./512.) ); // Equal probability for two possible colour flows. sigSum /= pow2( (uHavg-s34Avg) * (tHavg-s34Avg) ); sigTS = 0.5 * sigSum; sigUS = sigTS; } // Final answer, with common factors. sigma = (M_PI / sH2) * pow2(alpS) * sigSum * nCHV * openFracPair; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2qGqGbar::setIdColAcol() { // Flavours trivial. setId( 21, 21, idNew, -idNew); // Two colour flow topologies. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 2, 2, 3, 1, 0, 0, 3); else setColAcol( 1, 2, 3, 1, 3, 0, 0, 2); } //========================================================================== // Sigma2qqbar2qGqGbar class. // Cross section for q qbar -> qG qGbar (generic quark of spin 0, 1/2 or 1). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2qGqGbar::initProc() { // Number of colours. Coupling kappa used for vector state. nCHV = settingsPtr->mode("HiddenValley:Ngauge"); kappa = settingsPtr->parm("HiddenValley:kappa"); // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(idNew, -idNew); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2qGqGbar::sigmaKin() { // Modified Mandelstam variables for massive kinematics with m3 = m4. double delta = 0.25 * pow2(s3 - s4) / sH; double s34Avg = 0.5 * (s3 + s4) - delta; double tHavg = tH - delta; double uHavg = uH - delta; double tHQ = -0.5 * (sH - tH + uH); double uHQ = -0.5 * (sH + tH - uH); double tHQ2 = tHQ * tHQ; double uHQ2 = uHQ * uHQ; // Evaluate cross section for spin 0 colour triplet. if (spinSave == 0) { sigSum = (1./9.) * (sH * (sH - 4. * s34Avg) - pow2(uHavg - tHavg)) / sH2; } // Evaluate cross section for spin 1/2 colour triplet. else if (spinSave == 1) { sigSum = (4./9.) * ((tHQ2 + uHQ2) / sH2 + 2. * s34Avg / sH); } // Evaluate cross section for spin 1 colour triplet. else { double tuH34 = (tHavg + uHavg) / s34Avg; sigSum = (1./9.) * ( pow2(1. + kappa) * sH * s34Avg * (pow2(tuH34) - 4.) + (tHavg * uHavg - pow2(s34Avg)) * (8. + 2. * (1. - pow2(kappa)) * tuH34 + pow2(kappa) * pow2(tuH34)) ) / sH2; } // Final answer, with common factors. sigma = (M_PI / sH2) * pow2(alpS) * sigSum * nCHV * openFracPair; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2qGqGbar::setIdColAcol() { // Flavours trivial. setId( id1, id2, idNew, -idNew); // tH defined between f and qG: must swap tHat <-> uHat if qbar q in. swapTU = (id1 < 0); // Colour flow topologies. if (id1 > 0) setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); else setColAcol( 0, 2, 1, 0, 1, 0, 0, 2); } //========================================================================== // Sigma2ffbar2fGfGbar class. // Cross section for f fbar -> qG qGbar (generic quark of spin 0, 1/2 or 1) // via gamma^*/Z^* s-channel exchange. Still under development!! ?? //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2fGfGbar::initProc() { // Charge and number of colours. Coupling kappa used for vector state. if (settingsPtr->flag("HiddenValley:doKinMix")) eQHV2 = pow2(settingsPtr->parm("HiddenValley:kinMix")); else eQHV2 = pow2( particleDataPtr->charge(idNew) ); nCHV = settingsPtr->mode("HiddenValley:Ngauge"); kappa = settingsPtr->parm("HiddenValley:kappa"); // Coloured or uncoloured particle. hasColour = (particleDataPtr->colType(idNew) != 0); colFac = (hasColour) ? 3. : 1.; // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(idNew, -idNew); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2fGfGbar::sigmaKin() { // Modified Mandelstam variables for massive kinematics with m3 = m4. double delta = 0.25 * pow2(s3 - s4) / sH; double s34Avg = 0.5 * (s3 + s4) - delta; double tHavg = tH - delta; double uHavg = uH - delta; double tHQ = -0.5 * (sH - tH + uH); double uHQ = -0.5 * (sH + tH - uH); double tHQ2 = tHQ * tHQ; double uHQ2 = uHQ * uHQ; // Evaluate cross section for spin 0 colour triplet. if (spinSave == 0) { sigSum = 0.5 * (sH * (sH - 4. * s34Avg) - pow2(uHavg - tHavg)) / sH2; } // Evaluate cross section for spin 1/2 colour triplet. else if (spinSave == 1) { sigSum = 2. * ((tHQ2 + uHQ2) / sH2 + 2. * s34Avg / sH); } // Evaluate cross section for spin 1 colour triplet. else { double tuH34 = (tHavg + uHavg) / s34Avg; sigSum = 0.5 * ( pow2(1. + kappa) * sH * s34Avg * (pow2(tuH34) - 4.) + (tHavg * uHavg - pow2(s34Avg)) * (8. + 2. * (1. - pow2(kappa)) * tuH34 + pow2(kappa) * pow2(tuH34)) ) / sH2; } // Final-state charge factors. sigSum *= colFac * eQHV2 * (1. + alpS / M_PI); // Final answer, except for initial-state weight sigma0 = (M_PI / sH2) * pow2(alpEM) * sigSum * nCHV * openFracPair; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2fGfGbar::sigmaHat() { // Charge and colour factors. double eNow = couplingsPtr->ef( abs(id1) ); double sigma = sigma0 * pow2(eNow); if (abs(id1) < 9) sigma /= 3.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2fGfGbar::setIdColAcol() { // Flavours trivial. setId( id1, id2, idNew, -idNew); // tH defined between f and qG: must swap tHat <-> uHat if fbar f in. swapTU = (id1 < 0); // Colour flow topologies. if (hasColour) { if (id1 > 0 && id1 < 7) setColAcol( 1, 0, 0, 1, 2, 0, 0, 2); else if (id1 > -7 && id1 < 0) setColAcol( 0, 1, 1, 0, 2, 0, 0, 2); else setColAcol( 0, 0, 0, 0, 1, 0, 0, 1); } else { if (id1 > 0 && id1 < 7) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else if (id1 > -7 && id1 < 0) setColAcol( 0, 1, 1, 0, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); } } //========================================================================== // Sigma1ffbar2Zv class. // Cross section for f fbar -> Zv, where Zv couples both to the SM and // to a hidden sector. Primitive coupling structure. //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2Zv::initProc() { // Store Zv mass and width for propagator. idZv = 4900023; mRes = particleDataPtr->m0(idZv); GammaRes = particleDataPtr->mWidth(idZv); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(idZv); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat); first step when inflavours unknown. void Sigma1ffbar2Zv::sigmaKin() { // Breit-Wigner, including some (guessed) spin factors. double sigBW = 12. * M_PI / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); // Outgoing width: only includes channels left open. double widthOut = particlePtr->resWidthOpen(663, mH); // Temporary answer. sigOut = sigBW * widthOut; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat); second step when inflavours known. double Sigma1ffbar2Zv::sigmaHat() { // Incoming quark or lepton; for former need two 1/3 colour factors. int id1Abs = abs(id1); double widthIn = particlePtr->resWidthChan( mH, id1Abs, -id1Abs); if (id1Abs < 6) widthIn /= 9.; return widthIn * sigOut; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2Zv::setIdColAcol() { // Flavours trivial. setId( id1, id2, idZv); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 6) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma1ffbar2Zv::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying resonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Z' itself angular distribution as if gamma*. if (iResBeg == 5 && iResEnd == 5) { double mr = 4. * pow2(process[6].m()) / sH; double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * sqrtpos(1. - mr)); double wt = 1. + pow2(cosThe) + mr * (1. - pow2(cosThe)); return 0.5 * wt; } // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/Basics.cc0000644000175000017500000011545212217346244014650 0ustar sunsun// Basics.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the Rndm, Vec4, // RotBstMatrix and Hist classes, and some related global functions. #include "Pythia8/Basics.h" // Access time information. #include namespace Pythia8 { //========================================================================== // Rndm class. // This class handles random number generation according to the // Marsaglia-Zaman-Tsang algorithm //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // The default seed, i.e. the Marsaglia-Zaman random number sequence. const int Rndm::DEFAULTSEED = 19780503; //-------------------------------------------------------------------------- // Method to pass in pointer for external random number generation. bool Rndm::rndmEnginePtr( RndmEngine* rndmEngPtrIn) { // Save pointer. if (rndmEngPtrIn == 0) return false; rndmEngPtr = rndmEngPtrIn; useExternalRndm = true; // Done. return true; } //-------------------------------------------------------------------------- // Initialize, normally at construction or in first call. void Rndm::init(int seedIn) { // Pick seed in convenient way. Assure it to be non-negative. int seed = seedIn; if (seedIn < 0) seed = DEFAULTSEED; else if (seedIn == 0) seed = int(time(0)); if (seed < 0) seed = -seed; // Unpack seed. int ij = (seed/30082) % 31329; int kl = seed % 30082; int i = (ij/177) % 177 + 2; int j = ij % 177 + 2; int k = (kl/169) % 178 + 1; int l = kl % 169; // Initialize random number array. for (int ii = 0; ii < 97; ++ii) { double s = 0.; double t = 0.5; for (int jj = 0; jj < 48; ++jj) { int m = (( (i*j)%179 )*k) % 179; i = j; j = k; k = m; l = (53*l+1) % 169; if ( (l*m) % 64 >= 32) s += t; t *= 0.5; } u[ii] = s; } // Initialize other variables. double twom24 = 1.; for (int i24 = 0; i24 < 24; ++i24) twom24 *= 0.5; c = 362436. * twom24; cd = 7654321. * twom24; cm = 16777213. * twom24; i97 = 96; j97 = 32; // Finished. initRndm = true; seedSave = seed; sequence = 0; } //-------------------------------------------------------------------------- // Generate next random number uniformly between 0 and 1. double Rndm::flat() { // Use external random number generator if such has been linked. if (useExternalRndm) return rndmEngPtr->flat(); // Ensure that already initialized. if (!initRndm) init(DEFAULTSEED); // Find next random number and update saved state. ++sequence; double uni; do { uni = u[i97] - u[j97]; if (uni < 0.) uni += 1.; u[i97] = uni; if (--i97 < 0) i97 = 96; if (--j97 < 0) j97 = 96; c -= cd; if (c < 0.) c += cm; uni -= c; if(uni < 0.) uni += 1.; } while (uni <= 0. || uni >= 1.); return uni; } //-------------------------------------------------------------------------- // Pick one option among vector of (positive) probabilities. int Rndm::pick(const vector& prob) { double work = 0.; for (int i = 0; i < int(prob.size()); ++i) work += prob[i]; work *= flat(); int index = -1; do work -= prob[++index]; while (work > 0. && index < int(prob.size())); return index; } //-------------------------------------------------------------------------- // Save current state of the random number generator to a binary file. bool Rndm::dumpState(string fileName) { // Open file as output stream. const char* fn = fileName.c_str(); ofstream ofs(fn, ios::binary); if (!ofs.good()) { cout << " Rndm::dumpState: could not open output file" << endl; return false; } // Write the state of the generator on the file. ofs.write((char *) &seedSave, sizeof(int)); ofs.write((char *) &sequence, sizeof(long)); ofs.write((char *) &i97, sizeof(int)); ofs.write((char *) &j97, sizeof(int)); ofs.write((char *) &c, sizeof(double)); ofs.write((char *) &cd, sizeof(double)); ofs.write((char *) &cm, sizeof(double)); ofs.write((char *) &u, sizeof(double) * 97); // Write confirmation on cout. cout << " PYTHIA Rndm::dumpState: seed = " << seedSave << ", sequence no = " << sequence << endl; return true; } //-------------------------------------------------------------------------- // Read in the state of the random number generator from a binary file. bool Rndm::readState(string fileName) { // Open file as input stream. const char* fn = fileName.c_str(); ifstream ifs(fn, ios::binary); if (!ifs.good()) { cout << " Rndm::readState: could not open input file" << endl; return false; } // Read the state of the generator from the file. ifs.read((char *) &seedSave, sizeof(int)); ifs.read((char *) &sequence, sizeof(long)); ifs.read((char *) &i97, sizeof(int)); ifs.read((char *) &j97, sizeof(int)); ifs.read((char *) &c, sizeof(double)); ifs.read((char *) &cd, sizeof(double)); ifs.read((char *) &cm, sizeof(double)); ifs.read((char *) &u, sizeof(double) *97); // Write confirmation on cout. cout << " PYTHIA Rndm::readState: seed " << seedSave << ", sequence no = " << sequence << endl; return true; } //========================================================================== // Vec4 class. // This class implements four-vectors, in energy-momentum space. // (But could also be used to hold space-time four-vectors.) //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Small number to avoid division by zero. const double Vec4::TINY = 1e-20; //-------------------------------------------------------------------------- // Rotation (simple). void Vec4::rot(double thetaIn, double phiIn) { double cthe = cos(thetaIn); double sthe = sin(thetaIn); double cphi = cos(phiIn); double sphi = sin(phiIn); double tmpx = cthe * cphi * xx - sphi * yy + sthe * cphi * zz; double tmpy = cthe * sphi * xx + cphi * yy + sthe * sphi * zz; double tmpz = -sthe * xx + cthe * zz; xx = tmpx; yy = tmpy; zz = tmpz; } //-------------------------------------------------------------------------- // Azimuthal rotation phi around an arbitrary axis (nz, ny, nz). void Vec4::rotaxis(double phiIn, double nx, double ny, double nz) { double norm = 1./sqrt(nx*nx + ny*ny + nz*nz); nx *= norm; ny *= norm; nz *= norm; double cphi = cos(phiIn); double sphi = sin(phiIn); double comb = (nx * xx + ny * yy + nz * zz) * (1. - cphi); double tmpx = cphi * xx + comb * nx + sphi * (ny * zz - nz * yy); double tmpy = cphi * yy + comb * ny + sphi * (nz * xx - nx * zz); double tmpz = cphi * zz + comb * nz + sphi * (nx * yy - ny * xx); xx = tmpx; yy = tmpy; zz = tmpz; } //-------------------------------------------------------------------------- // Azimuthal rotation phi around an arbitrary (3-vector component of) axis. void Vec4::rotaxis(double phiIn, const Vec4& n) { double nx = n.xx; double ny = n.yy; double nz = n.zz; double norm = 1./sqrt(nx*nx + ny*ny + nz*nz); nx *= norm; ny *=norm; nz *=norm; double cphi = cos(phiIn); double sphi = sin(phiIn); double comb = (nx * xx + ny * yy + nz * zz) * (1. - cphi); double tmpx = cphi * xx + comb * nx + sphi * (ny * zz - nz * yy); double tmpy = cphi * yy + comb * ny + sphi * (nz * xx - nx * zz); double tmpz = cphi * zz + comb * nz + sphi * (nx * yy - ny * xx); xx = tmpx; yy = tmpy; zz = tmpz; } //-------------------------------------------------------------------------- // Boost (simple). void Vec4::bst(double betaX, double betaY, double betaZ) { double beta2 = betaX*betaX + betaY*betaY + betaZ*betaZ; double gamma = 1. / sqrt(1. - beta2); double prod1 = betaX * xx + betaY * yy + betaZ * zz; double prod2 = gamma * (gamma * prod1 / (1. + gamma) + tt); xx += prod2 * betaX; yy += prod2 * betaY; zz += prod2 * betaZ; tt = gamma * (tt + prod1); } //-------------------------------------------------------------------------- // Boost (simple, given gamma). void Vec4::bst(double betaX, double betaY, double betaZ, double gamma) { double prod1 = betaX * xx + betaY * yy + betaZ * zz; double prod2 = gamma * (gamma * prod1 / (1. + gamma) + tt); xx += prod2 * betaX; yy += prod2 * betaY; zz += prod2 * betaZ; tt = gamma * (tt + prod1); } //-------------------------------------------------------------------------- // Boost given by a Vec4 p. void Vec4::bst(const Vec4& pIn) { double betaX = pIn.xx / pIn.tt; double betaY = pIn.yy / pIn.tt; double betaZ = pIn.zz / pIn.tt; double beta2 = betaX*betaX + betaY*betaY + betaZ*betaZ; double gamma = 1. / sqrt(1. - beta2); double prod1 = betaX * xx + betaY * yy + betaZ * zz; double prod2 = gamma * (gamma * prod1 / (1. + gamma) + tt); xx += prod2 * betaX; yy += prod2 * betaY; zz += prod2 * betaZ; tt = gamma * (tt + prod1); } //-------------------------------------------------------------------------- // Boost given by a Vec4 p and double m. void Vec4::bst(const Vec4& pIn, double mIn) { double betaX = pIn.xx / pIn.tt; double betaY = pIn.yy / pIn.tt; double betaZ = pIn.zz / pIn.tt; double gamma = pIn.tt / mIn; double prod1 = betaX * xx + betaY * yy + betaZ * zz; double prod2 = gamma * (gamma * prod1 / (1. + gamma) + tt); xx += prod2 * betaX; yy += prod2 * betaY; zz += prod2 * betaZ; tt = gamma * (tt + prod1); } //-------------------------------------------------------------------------- // Boost given by a Vec4 p; boost in opposite direction. void Vec4::bstback(const Vec4& pIn) { double betaX = -pIn.xx / pIn.tt; double betaY = -pIn.yy / pIn.tt; double betaZ = -pIn.zz / pIn.tt; double beta2 = betaX*betaX + betaY*betaY + betaZ*betaZ; double gamma = 1. / sqrt(1. - beta2); double prod1 = betaX * xx + betaY * yy + betaZ * zz; double prod2 = gamma * (gamma * prod1 / (1. + gamma) + tt); xx += prod2 * betaX; yy += prod2 * betaY; zz += prod2 * betaZ; tt = gamma * (tt + prod1); } //-------------------------------------------------------------------------- // Boost given by a Vec4 p and double m; boost in opposite direction. void Vec4::bstback(const Vec4& pIn, double mIn) { double betaX = -pIn.xx / pIn.tt; double betaY = -pIn.yy / pIn.tt; double betaZ = -pIn.zz / pIn.tt; double gamma = pIn.tt / mIn; double prod1 = betaX * xx + betaY * yy + betaZ * zz; double prod2 = gamma * (gamma * prod1 / (1. + gamma) + tt); xx += prod2 * betaX; yy += prod2 * betaY; zz += prod2 * betaZ; tt = gamma * (tt + prod1); } //-------------------------------------------------------------------------- // Arbitrary combination of rotations and boosts defined by 4 * 4 matrix. void Vec4::rotbst(const RotBstMatrix& M) { double x = xx; double y = yy; double z = zz; double t = tt; tt = M.M[0][0] * t + M.M[0][1] * x + M.M[0][2] * y + M.M[0][3] * z; xx = M.M[1][0] * t + M.M[1][1] * x + M.M[1][2] * y + M.M[1][3] * z; yy = M.M[2][0] * t + M.M[2][1] * x + M.M[2][2] * y + M.M[2][3] * z; zz = M.M[3][0] * t + M.M[3][1] * x + M.M[3][2] * y + M.M[3][3] * z; } //-------------------------------------------------------------------------- // The invariant mass of two four-vectors. double m(const Vec4& v1, const Vec4& v2) { double m2 = pow2(v1.tt + v2.tt) - pow2(v1.xx + v2.xx) - pow2(v1.yy + v2.yy) - pow2(v1.zz + v2.zz); return (m2 > 0.) ? sqrt(m2) : 0.; } //-------------------------------------------------------------------------- // The squared invariant mass of two four-vectors. double m2(const Vec4& v1, const Vec4& v2) { double m2 = pow2(v1.tt + v2.tt) - pow2(v1.xx + v2.xx) - pow2(v1.yy + v2.yy) - pow2(v1.zz + v2.zz); return m2; } //-------------------------------------------------------------------------- // The scalar product of two three-vectors. double dot3(const Vec4& v1, const Vec4& v2) { return v1.xx*v2.xx + v1.yy*v2.yy + v1.zz*v2.zz; } //-------------------------------------------------------------------------- // The cross product of two three-vectors. Vec4 cross3(const Vec4& v1, const Vec4& v2) { Vec4 v; v.xx = v1.yy * v2.zz - v1.zz * v2.yy; v.yy = v1.zz * v2.xx - v1.xx * v2.zz; v.zz = v1.xx * v2.yy - v1.yy * v2.xx; return v; } //-------------------------------------------------------------------------- // Opening angle between two three-vectors. double theta(const Vec4& v1, const Vec4& v2) { double cthe = (v1.xx * v2.xx + v1.yy * v2.yy + v1.zz * v2.zz) / sqrt( (v1.xx*v1.xx + v1.yy*v1.yy + v1.zz*v1.zz) * (v2.xx*v2.xx + v2.yy*v2.yy + v2.zz*v2.zz) ); cthe = max(-1., min(1., cthe)); return acos(cthe); } //-------------------------------------------------------------------------- // Cosine of the opening angle between two three-vectors. double costheta(const Vec4& v1, const Vec4& v2) { double cthe = (v1.xx * v2.xx + v1.yy * v2.yy + v1.zz * v2.zz) / sqrt( (v1.xx*v1.xx + v1.yy*v1.yy + v1.zz*v1.zz) * (v2.xx*v2.xx + v2.yy*v2.yy + v2.zz*v2.zz) ); cthe = max(-1., min(1., cthe)); return cthe; } //-------------------------------------------------------------------------- // Azimuthal angle between two three-vectors. double phi(const Vec4& v1, const Vec4& v2) { double cphi = (v1.xx * v2.xx + v1.yy * v2.yy) / sqrt( max( Vec4::TINY, (v1.xx*v1.xx + v1.yy*v1.yy) * (v2.xx*v2.xx + v2.yy*v2.yy) )); cphi = max(-1., min(1., cphi)); return acos(cphi); } //-------------------------------------------------------------------------- // Cosine of the azimuthal angle between two three-vectors. double cosphi(const Vec4& v1, const Vec4& v2) { double cphi = (v1.xx * v2.xx + v1.yy * v2.yy) / sqrt( max( Vec4::TINY, (v1.xx*v1.xx + v1.yy*v1.yy) * (v2.xx*v2.xx + v2.yy*v2.yy) )); cphi = max(-1., min(1., cphi)); return cphi; } //-------------------------------------------------------------------------- // Azimuthal angle between two three-vectors around a third. double phi(const Vec4& v1, const Vec4& v2, const Vec4& n) { double nx = n.xx; double ny = n.yy; double nz = n.zz; double norm = 1. / sqrt(nx*nx + ny*ny + nz*nz); nx *= norm; ny *=norm; nz *=norm; double v1s = v1.xx * v1.xx + v1.yy * v1.yy + v1.zz * v1.zz; double v2s = v2.xx * v2.xx + v2.yy * v2.yy + v2.zz * v2.zz; double v1v2 = v1.xx * v2.xx + v1.yy * v2.yy + v1.zz * v2.zz; double v1n = v1.xx * nx + v1.yy * ny + v1.zz * nz; double v2n = v2.xx * nx + v2.yy * ny + v2.zz * nz; double cphi = (v1v2 - v1n * v2n) / sqrt( max( Vec4::TINY, (v1s - v1n*v1n) * (v2s - v2n*v2n) )); cphi = max(-1., min(1., cphi)); return acos(cphi); } //-------------------------------------------------------------------------- // Cosine of the azimuthal angle between two three-vectors around a third. double cosphi(const Vec4& v1, const Vec4& v2, const Vec4& n) { double nx = n.xx; double ny = n.yy; double nz = n.zz; double norm = 1. / sqrt(nx*nx + ny*ny + nz*nz); nx *= norm; ny *=norm; nz *=norm; double v1s = v1.xx * v1.xx + v1.yy * v1.yy + v1.zz * v1.zz; double v2s = v2.xx * v2.xx + v2.yy * v2.yy + v2.zz * v2.zz; double v1v2 = v1.xx * v2.xx + v1.yy * v2.yy + v1.zz * v2.zz; double v1n = v1.xx * nx + v1.yy * ny + v1.zz * nz; double v2n = v2.xx * nx + v2.yy * ny + v2.zz * nz; double cphi = (v1v2 - v1n * v2n) / sqrt( max( Vec4::TINY, (v1s - v1n*v1n) * (v2s - v2n*v2n) )); cphi = max(-1., min(1., cphi)); return cphi; } //-------------------------------------------------------------------------- // Distance in cylindrical (y, phi) coordinates. double RRapPhi(const Vec4& v1, const Vec4& v2) { double dRap = abs(v1.rap() - v2.rap()); double dPhi = abs(v1.phi() - v2.phi()); if (dPhi > M_PI) dPhi = 2. * M_PI - dPhi; return sqrt(dRap*dRap + dPhi*dPhi); } //-------------------------------------------------------------------------- // Distance in cylindrical (eta, phi) coordinates. double REtaPhi(const Vec4& v1, const Vec4& v2) { double dEta = abs(v1.eta() - v2.eta()); double dPhi = abs(v1.phi() - v2.phi()); if (dPhi > M_PI) dPhi = 2. * M_PI - dPhi; return sqrt(dEta*dEta + dPhi*dPhi); } //-------------------------------------------------------------------------- // Print a four-vector: also operator overloading with friend. ostream& operator<<(ostream& os, const Vec4& v) { os << fixed << setprecision(3) << " " << setw(9) << v.xx << " " << setw(9) << v.yy << " " << setw(9) << v.zz << " " << setw(9) << v.tt << " (" << setw(9) << v.mCalc() << ")\n"; return os; } //========================================================================== // RotBstMatrix class. // This class implements 4 * 4 matrices that encode an arbitrary combination // of rotations and boosts, that can be applied to Vec4 four-vectors. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Small number to avoid division by zero. const double RotBstMatrix::TINY = 1e-20; //-------------------------------------------------------------------------- // Rotate by polar angle theta and azimuthal angle phi. void RotBstMatrix::rot(double theta, double phi) { // Set up rotation matrix. double cthe = cos(theta); double sthe = sin(theta); double cphi = cos(phi); double sphi = sin(phi); double Mrot[4][4] = { {1., 0., 0., 0.}, {0., cthe * cphi, - sphi, sthe * cphi}, {0., cthe * sphi, cphi, sthe * sphi}, {0., -sthe, 0., cthe } }; // Rotate current matrix accordingly. double Mtmp[4][4]; for (int i = 0; i < 4; ++i) for (int j = 0; j < 4; ++j) Mtmp[i][j] = M[i][j]; for (int i = 0; i < 4; ++i) for (int j = 0; j < 4; ++j) M[i][j] = Mrot[i][0] * Mtmp[0][j] + Mrot[i][1] * Mtmp[1][j] + Mrot[i][2] * Mtmp[2][j] + Mrot[i][3] * Mtmp[3][j]; } //-------------------------------------------------------------------------- // Rotate so that vector originally along z axis becomes parallel with p. void RotBstMatrix::rot(const Vec4& p) { double theta = p.theta(); double phi = p.phi(); rot(0., -phi); rot(theta, phi); } //-------------------------------------------------------------------------- // Boost with velocity vector (betaX, betaY, betaZ). void RotBstMatrix::bst(double betaX, double betaY, double betaZ) { // Set up boost matrix. double gm = 1. / sqrt( max( TINY, 1. - betaX*betaX - betaY*betaY - betaZ*betaZ ) ); double gf = gm*gm / (1. + gm); double Mbst[4][4] = { { gm, gm*betaX, gm*betaY, gm*betaZ }, { gm*betaX, 1. + gf*betaX*betaX, gf*betaX*betaY, gf*betaX*betaZ }, { gm*betaY, gf*betaY*betaX, 1. + gf*betaY*betaY, gf*betaY*betaZ }, { gm*betaZ, gf*betaZ*betaX, gf*betaZ*betaY, 1. + gf*betaZ*betaZ } }; // Boost current matrix correspondingly. double Mtmp[4][4]; for (int i = 0; i < 4; ++i) for (int j = 0; j < 4; ++j) Mtmp[i][j] = M[i][j]; for (int i = 0; i < 4; ++i) for (int j = 0; j < 4; ++j) M[i][j] = Mbst[i][0] * Mtmp[0][j] + Mbst[i][1] * Mtmp[1][j] + Mbst[i][2] * Mtmp[2][j] + Mbst[i][3] * Mtmp[3][j]; } //-------------------------------------------------------------------------- // Boost so that vector originally at rest obtains same velocity as p. void RotBstMatrix::bst(const Vec4& p) { double betaX = p.px() / p.e(); double betaY = p.py() / p.e(); double betaZ = p.pz() / p.e(); bst(betaX, betaY, betaZ); } //-------------------------------------------------------------------------- // Boost so vector originally with same velocity as p is brought to rest. void RotBstMatrix::bstback(const Vec4& p) { double betaX = -p.px() / p.e(); double betaY = -p.py() / p.e(); double betaZ = -p.pz() / p.e(); bst(betaX, betaY, betaZ); } //-------------------------------------------------------------------------- // Boost that transforms p1 to p2, where p1^2 = p2^2 is assumed. void RotBstMatrix::bst(const Vec4& p1, const Vec4& p2) { double eSum = p1.e() + p2.e(); double betaX = (p2.px() - p1.px()) / eSum; double betaY = (p2.py() - p1.py()) / eSum; double betaZ = (p2.pz() - p1.pz()) / eSum; double fac = 2. / (1. + betaX*betaX + betaY*betaY + betaZ*betaZ); betaX *= fac; betaY *= fac; betaZ *= fac; bst(betaX, betaY, betaZ); } //-------------------------------------------------------------------------- // Boost and rotation that transforms from p1 and p2 // to their rest frame with p1 along +z axis. void RotBstMatrix::toCMframe(const Vec4& p1, const Vec4& p2) { Vec4 pSum = p1 + p2; Vec4 dir = p1; dir.bstback(pSum); double theta = dir.theta(); double phi = dir.phi(); bstback(pSum); rot(0., -phi); rot(-theta, phi); } //-------------------------------------------------------------------------- // Rotation and boost that transforms from rest frame of p1 and p2 // with p1 along +z axis to actual frame of p1 and p2. (Inverse of above.) void RotBstMatrix::fromCMframe(const Vec4& p1, const Vec4& p2) { Vec4 pSum = p1 + p2; Vec4 dir = p1; dir.bstback(pSum); double theta = dir.theta(); double phi = dir.phi(); rot(0., -phi); rot(theta, phi); bst(pSum); } //-------------------------------------------------------------------------- // Combine existing rotation/boost matrix with another one. void RotBstMatrix::rotbst(const RotBstMatrix& Mrb) { double Mtmp[4][4]; for (int i = 0; i < 4; ++i) for (int j = 0; j < 4; ++j) Mtmp[i][j] = M[i][j]; for (int i = 0; i < 4; ++i) for (int j = 0; j < 4; ++j) M[i][j] = Mrb.M[i][0] * Mtmp[0][j] + Mrb.M[i][1] * Mtmp[1][j] + Mrb.M[i][2] * Mtmp[2][j] + Mrb.M[i][3] * Mtmp[3][j]; } //-------------------------------------------------------------------------- // Invert the rotation and boost. void RotBstMatrix::invert() { double Mtmp[4][4]; for (int i = 0; i < 4; ++i) for (int j = 0; j < 4; ++j) Mtmp[i][j] = M[i][j]; for (int i = 0; i < 4; ++i) for (int j = 0; j < 4; ++j) M[i][j] = ( (i == 0 && j > 0) || (i > 0 && j == 0) ) ? - Mtmp[j][i] : Mtmp[j][i]; } //-------------------------------------------------------------------------- // Reset to diagonal matrix. void RotBstMatrix::reset() { for (int i = 0; i < 4; ++i) for (int j = 0; j < 4; ++j) M[i][j] = (i==j) ? 1. : 0.; } //-------------------------------------------------------------------------- // Crude estimate deviation from unit matrix. double RotBstMatrix::deviation() const { double devSum = 0.; for (int i = 0; i < 4; ++i) for (int j = 0; j < 4; ++j) devSum += (i==j) ? abs(M[i][j] - 1.) : abs(M[i][j]); return devSum; } //-------------------------------------------------------------------------- // Print a rotation and boost matrix: operator overloading with friend. ostream& operator<<(ostream& os, const RotBstMatrix& M) { os << fixed << setprecision(5) << " Rotation/boost matrix: \n"; for (int i = 0; i <4; ++i) os << setw(10) << M.M[i][0] << setw(10) << M.M[i][1] << setw(10) << M.M[i][2] << setw(10) << M.M[i][3] << "\n"; return os; } //========================================================================== // Hist class. // This class handles a single histogram at a time // (or a vector of histograms). //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Maximum number of bins in a histogram. const int Hist::NBINMAX = 1000; // Maximum number of columns that can be printed for a histogram. const int Hist::NCOLMAX = 100; // Maximum number of lines a histogram can use at output. const int Hist::NLINES = 30; // Tolerance in deviation of xMin and xMax between two histograms. const double Hist::TOLERANCE = 0.001; // Small and large numbers to avoid division by zero and overflow. const double Hist::TINY = 1e-20; const double Hist::LARGE = 1e20; // When minbin/maxbin < SMALLFRAC the y scale goes down to zero. const double Hist::SMALLFRAC = 0.1; // Constants for printout: fixed steps on y scale; filling characters. const double DYAC[] = {0.04, 0.05, 0.06, 0.08, 0.10, 0.12, 0.15, 0.20, 0.25, 0.30}; const char NUMBER[] = {'0', '1', '2', '3', '4', '5', '6', '7', '8', '9', 'X' }; //-------------------------------------------------------------------------- // Book a histogram. void Hist::book(string titleIn, int nBinIn, double xMinIn, double xMaxIn) { title = titleIn; nBin = nBinIn; if (nBinIn < 1) nBin = 1; if (nBinIn > NBINMAX) nBin = NBINMAX; xMin = xMinIn; xMax = xMaxIn; dx = (xMax - xMin)/nBin; res.resize(nBin); null(); } //-------------------------------------------------------------------------- // Reset bin contents. void Hist::null() { nFill = 0; under = 0.; inside = 0.; over = 0.; for (int ix = 0; ix < nBin; ++ix) res[ix] = 0.; } //-------------------------------------------------------------------------- // Fill bin with weight. void Hist::fill(double x, double w) { ++nFill; int iBin = int(floor((x - xMin)/dx)); if (iBin < 0) under += w; else if (iBin >= nBin) over += w; else {inside += w; res[iBin] += w; } } //-------------------------------------------------------------------------- // Print a histogram: also operator overloading with friend. ostream& operator<<(ostream& os, const Hist& h) { // Do not print empty histograms. if (h.nFill <= 0) return os; // Write time and title. time_t t = time(0); char date[18]; strftime(date,18,"%Y-%m-%d %H:%M",localtime(&t)); os << "\n\n " << date << " " << h.title << "\n\n"; // Group bins, where required, to make printout have fewer columns. // Avoid overflow. int nGroup = 1 + (h.nBin - 1) / Hist::NCOLMAX; int nCol = 1 + (h.nBin - 1) / nGroup; vector resCol(nCol); for (int iCol = 0; iCol < nCol; ++iCol) { resCol[iCol] = 0.; for (int ix = nGroup * iCol; ix < min( h.nBin, nGroup * (iCol + 1)); ++ix) resCol[iCol] += h.res[ix]; resCol[iCol] = max( -Hist::LARGE, min( Hist::LARGE, resCol[iCol] ) ); } // Find minimum and maximum bin content. double yMin = resCol[0]; double yMax = resCol[0]; for (int iCol = 1; iCol < nCol; ++iCol) { if (resCol[iCol] < yMin) yMin = resCol[iCol]; if (resCol[iCol] > yMax) yMax = resCol[iCol]; } // Determine scale and step size for y axis. if (yMax - yMin > Hist::NLINES * DYAC[0] * 1e-9) { if (yMin > 0. && yMin < Hist::SMALLFRAC * yMax) yMin = 0.; if (yMax < 0. && yMax > Hist::SMALLFRAC * yMin) yMax = 0.; int iPowY = int(floor( log10(yMax - yMin) )); if (yMax - yMin < Hist::NLINES * DYAC[0] * pow(10.,iPowY)) iPowY = iPowY - 1; if (yMax - yMin > Hist::NLINES * DYAC[9] * pow(10.,iPowY)) iPowY = iPowY + 1; double nLinePow = Hist::NLINES * pow(10.,iPowY); double delY = DYAC[0]; for (int idel = 0; idel < 9; ++idel) if (yMax - yMin >= nLinePow * DYAC[idel]) delY = DYAC[idel+1]; double dy = delY * pow(10.,iPowY); // Convert bin contents to integer form; fractional fill in top row. vector row(nCol); vector frac(nCol); for (int iCol = 0; iCol < nCol ; ++iCol) { double cta = abs(resCol[iCol]) / dy; row[iCol] = int(cta + 0.95); if(resCol[iCol] < 0.) row[iCol] = - row[iCol]; frac[iCol] = int(10. * (cta + 1.05 - floor(cta + 0.95))); } int rowMin = int(abs(yMin)/dy + 0.95); if ( yMin < 0) rowMin = - rowMin; int rowMax = int(abs(yMax)/dy + 0.95); if ( yMax < 0) rowMax = - rowMax; // Print histogram row by row. os << fixed << setprecision(2); for (int iRow = rowMax; iRow >= rowMin; iRow--) if (iRow != 0) { os << " " << setw(10) << iRow*delY << "*10^" << setw(2) << iPowY << " "; for (int iCol = 0; iCol < nCol ; ++iCol) { if (iRow == row[iCol]) os << NUMBER[frac[iCol]]; else if (iRow * (row[iCol] - iRow) > 0) os << NUMBER[10]; else os << " "; } os << "\n"; } os << "\n"; // Print sign and value of bin contents double maxim = log10(max(yMax, -yMin)); int iPowBin = int(floor(maxim + 0.0001)); os << " Contents "; for (int iCol = 0; iCol < nCol ; ++iCol) { if (resCol[iCol] < - pow(10., iPowBin - 4)) os << "-"; else os << " "; row[iCol] = int(abs(resCol[iCol]) * pow(10., 3 - iPowBin) + 0.5); } os << "\n"; for (int iRow = 3; iRow >= 0; iRow--) { os << " *10^" << setw(2) << iPowBin + iRow - 3 << " "; int mask = int( pow(10., iRow) + 0.5); for (int iCol = 0; iCol < nCol ; ++iCol) { os << NUMBER[(row[iCol] / mask) % 10]; } os << "\n"; } os << "\n"; // Print sign and value of lower bin edge. maxim = log10( max( -h.xMin, h.xMax - h.dx)); int iPowExp = int(floor(maxim + 0.0001)); os << " Low edge "; for (int iCol = 0; iCol < nCol ; ++iCol) { if (h.xMin + iCol * nGroup * h.dx < - pow(10., iPowExp - 3)) os << "-"; else os << " "; row[iCol] = int(abs(h.xMin + iCol * nGroup * h.dx) * pow(10., 2 - iPowExp) + 0.5); } os << "\n"; for (int iRow = 2; iRow >= 0; iRow--) { os << " *10^" << setw(2) << iPowExp + iRow - 2 << " "; int mask = int( pow(10., iRow) + 0.5); for (int iCol = 0; iCol < nCol ; ++iCol) os << NUMBER[(row[iCol] / mask) % 10]; os << "\n"; } os << "\n"; // Print explanation if histogram cannot be shown. } else os << " Histogram not shown since lowest value" << scientific << setprecision(4) << setw(12) << yMin << " and highest value" << setw(12) << yMax << " are too close \n \n"; // Calculate and print statistics. double cSum = 0.; double cxSum = 0.; double cxxSum = 0.; for (int ix = 0; ix < h.nBin ; ++ix) { double cta = abs(h.res[ix]); double x = h.xMin + (ix + 0.5) * h.dx; cSum = cSum + cta; cxSum = cxSum + cta * x; cxxSum = cxxSum + cta * x * x; } double xmean = cxSum / max(cSum, Hist::TINY); double rms = sqrtpos( cxxSum / max(cSum, Hist::TINY) - xmean*xmean ); os << scientific << setprecision(4) << " Entries =" << setw(12) << h.nFill << " Mean =" << setw(12) << xmean << " Underflow =" << setw(12) << h.under << " Low edge =" << setw(12) << h.xMin << "\n" << " All chan =" << setw(12) << h.inside << " Rms =" << setw(12) << rms << " Overflow =" << setw(12) << h.over << " High edge =" << setw(12) << h.xMax << endl; return os; } //-------------------------------------------------------------------------- // Print histogram contents as a table (e.g. for Gnuplot). void Hist::table(ostream& os) const { // Print histogram vector bin by bin, with mean x as first column. os << scientific << setprecision(4); for (int ix = 0; ix < nBin; ++ix) os << setw(12) << xMin + (ix + 0.5) * dx << setw(12) << res[ix] << "\n"; } //-------------------------------------------------------------------------- // Print a table out of two histograms with same x axis (e.g. for Gnuplot). void table(const Hist& h1, const Hist& h2, ostream& os) { // Require histogram x axes to agree. if (h1.nBin != h2.nBin || abs(h1.xMin - h2.xMin) > Hist::TOLERANCE * h1.dx || abs(h1.xMax - h2.xMax) > Hist::TOLERANCE * h1.dx) return; // Print histogram vectors bin by bin, with mean x as first column. os << scientific << setprecision(4); for (int ix = 0; ix < h1.nBin; ++ix) os << setw(12) << h1.xMin + (ix + 0.5) * h1.dx << setw(12) << h1.res[ix] << setw(12) << h2.res[ix] << "\n"; } void table(const Hist& h1, const Hist& h2, string fileName) { ofstream streamName(fileName.c_str()); table( h1, h2, streamName); } //-------------------------------------------------------------------------- // Get content of specific bin. // Special values are bin 0 for underflow and bin nBin+1 for overflow. // All other bins outside proper histogram range return 0. double Hist::getBinContent(int iBin) { if (iBin > 0 && iBin <= nBin) return res[iBin - 1]; else if (iBin == 0) return under; else if (iBin == nBin + 1) return over; else return 0.; } //-------------------------------------------------------------------------- // Check whether another histogram has same size and limits. bool Hist::sameSize(const Hist& h) const { if (nBin == h.nBin && abs(xMin - h.xMin) < TOLERANCE * dx && abs(xMax - h.xMax) < TOLERANCE * dx) return true; else return false; } //-------------------------------------------------------------------------- // Take 10-logarithm or natural logarithm of contents bin by bin. void Hist::takeLog(bool tenLog) { // Find smallest positive bin content, and put min a bit below. double yMin = Hist::LARGE; for (int ix = 0; ix < nBin; ++ix) if (res[ix] > Hist::TINY && res[ix] < yMin ) yMin = res[ix]; yMin *= 0.8; // Take 10-logarithm bin by bin, but ensure positivity. if (tenLog) { for (int ix = 0; ix < nBin; ++ix) res[ix] = log10( max( yMin, res[ix]) ); under = log10( max( yMin, under) ); inside = log10( max( yMin, inside) ); over = log10( max( yMin, over) ); // Take natural logarithm bin by bin, but ensure positivity. } else { for (int ix = 0; ix < nBin; ++ix) res[ix] = log( max( yMin, res[ix]) ); under = log( max( yMin, under) ); inside = log( max( yMin, inside) ); over = log( max( yMin, over) ); } } //-------------------------------------------------------------------------- // Take square root of contents bin by bin; set 0 for negative content. void Hist::takeSqrt() { for (int ix = 0; ix < nBin; ++ix) res[ix] = sqrtpos(res[ix]); under = sqrtpos(under); inside = sqrtpos(inside); over = sqrtpos(over); } //-------------------------------------------------------------------------- // Add histogram to existing one. Hist& Hist::operator+=(const Hist& h) { if (!sameSize(h)) return *this; nFill += h.nFill; under += h.under; inside += h.inside; over += h.over; for (int ix = 0; ix < nBin; ++ix) res[ix] += h.res[ix]; return *this; } //-------------------------------------------------------------------------- // Subtract histogram from existing one. Hist& Hist::operator-=(const Hist& h) { if (!sameSize(h)) return *this; nFill += h.nFill; under -= h.under; inside -= h.inside; over -= h.over; for (int ix = 0; ix < nBin; ++ix) res[ix] -= h.res[ix]; return *this; } //-------------------------------------------------------------------------- // Multiply existing histogram by another one. Hist& Hist::operator*=(const Hist& h) { if (!sameSize(h)) return *this; nFill += h.nFill; under *= h.under; inside *= h.inside; over *= h.over; for (int ix = 0; ix < nBin; ++ix) res[ix] *= h.res[ix]; return *this; } //-------------------------------------------------------------------------- // Divide existing histogram by another one. Hist& Hist::operator/=(const Hist& h) { if (!sameSize(h)) return *this; nFill += h.nFill; under = (abs(h.under) < Hist::TINY) ? 0. : under/h.under; inside = (abs(h.inside) < Hist::TINY) ? 0. : inside/h.inside; over = (abs(h.over) < Hist::TINY) ? 0. : over/h.over; for (int ix = 0; ix < nBin; ++ix) res[ix] = (abs(h.res[ix]) < Hist::TINY) ? 0. : res[ix]/h.res[ix]; return *this; } //-------------------------------------------------------------------------- // Add constant offset to histogram. Hist& Hist::operator+=(double f) { under += f; inside += nBin * f; over += f; for (int ix = 0; ix < nBin; ++ix) res[ix] += f; return *this; } //-------------------------------------------------------------------------- // Subtract constant offset from histogram. Hist& Hist::operator-=(double f) { under -= f; inside -= nBin * f; over -= f; for (int ix = 0; ix < nBin; ++ix) res[ix] -= f; return *this; } //-------------------------------------------------------------------------- // Multiply histogram by constant. Hist& Hist::operator*=(double f) { under *= f; inside *= f; over *= f; for (int ix = 0; ix < nBin; ++ix) res[ix] *= f; return *this; } //-------------------------------------------------------------------------- // Divide histogram by constant. Hist& Hist::operator/=(double f) { if (abs(f) > Hist::TINY) { under /= f; inside /= f; over /= f; for (int ix = 0; ix < nBin; ++ix) res[ix] /= f; // Set empty contents when division by zero. } else { under = 0.; inside = 0.; over = 0.; for (int ix = 0; ix < nBin; ++ix) res[ix] = 0.; } return *this; } //-------------------------------------------------------------------------- // Implementation of operator overloading with friends. Hist operator+(double f, const Hist& h1) { Hist h = h1; return h += f;} Hist operator+(const Hist& h1, double f) { Hist h = h1; return h += f;} Hist operator+(const Hist& h1, const Hist& h2) { Hist h = h1; return h += h2;} Hist operator-(double f, const Hist& h1) { Hist h = h1; h.under = f - h1.under; h.inside = h1.nBin * f - h1.inside; h.over = f - h1.over; for (int ix = 0; ix < h1.nBin; ++ix) h.res[ix] = f - h1.res[ix]; return h;} Hist operator-(const Hist& h1, double f) { Hist h = h1; return h -= f;} Hist operator-(const Hist& h1, const Hist& h2) { Hist h = h1; return h -= h2;} Hist operator*(double f, const Hist& h1) { Hist h = h1; return h *= f;} Hist operator*(const Hist& h1, double f) { Hist h = h1; return h *= f;} Hist operator*(const Hist& h1, const Hist& h2) { Hist h = h1; return h *= h2;} Hist operator/(double f, const Hist& h1) { Hist h = h1; h.under = (abs(h1.under) < Hist::TINY) ? 0. : f/h1.under; h.inside = (abs(h1.inside) < Hist::TINY) ? 0. : f/h1.inside; h.over = (abs(h1.over) < Hist::TINY) ? 0. : f/h1.over; for (int ix = 0; ix < h1.nBin; ++ix) h.res[ix] = (abs(h1.res[ix]) < Hist::TINY) ? 0. : f/h1.res[ix]; return h; } Hist operator/(const Hist& h1, double f) { Hist h = h1; return h /= f;} Hist operator/(const Hist& h1, const Hist& h2) { Hist h = h1; return h /= h2;} //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/HelicityBasics.cc0000644000175000017500000002341512217346245016341 0ustar sunsun// HelicityBasics.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Philip Ilten, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for helper classes // used in tau decays. #include "Pythia8/HelicityBasics.h" namespace Pythia8 { //========================================================================== // Wave4 class. // Friend methods to it. //-------------------------------------------------------------------------- // complex * Wave4. Wave4 operator*(complex s, const Wave4& w) { return Wave4( s * w.val[0], s * w.val[1], s * w.val[2], s * w.val[3]); } //-------------------------------------------------------------------------- // double * Wave4. Wave4 operator*(double s, const Wave4& w) { return Wave4( s * w.val[0], s * w.val[1], s * w.val[2], s * w.val[3]); } //-------------------------------------------------------------------------- // Complex conjugate. Wave4 conj(Wave4 w) { w(0) = conj(w(0)); w(1) = conj(w(1)); w(2) = conj(w(2)); w(3) = conj(w(3)); return w; } //-------------------------------------------------------------------------- // Permutation operator. Wave4 epsilon(Wave4 w1, Wave4 w2, Wave4 w3) { Wave4 w4; w4(0) = -(w1(1) * w2(2) * w3(3)) + (w1(1) * w2(3) * w3(2)) + (w1(2) * w2(1) * w3(3)) - (w1(2) * w2(3) * w3(1)) - (w1(3) * w2(1) * w3(2)) + (w1(3) * w2(2) * w3(1)); w4(1) = -(w1(0) * w2(2) * w3(3)) + (w1(0) * w2(3) * w3(2)) + (w1(2) * w2(0) * w3(3)) - (w1(2) * w2(3) * w3(0)) - (w1(3) * w2(0) * w3(2)) + (w1(3) * w2(2) * w3(0)); w4(2) = (w1(0) * w2(1) * w3(3)) - (w1(0) * w2(3) * w3(1)) - (w1(1) * w2(0) * w3(3)) + (w1(1) * w2(3) * w3(0)) + (w1(3) * w2(0) * w3(1)) - (w1(3) * w2(1) * w3(0)); w4(3) = -(w1(0) * w2(1) * w3(2)) + (w1(0) * w2(2) * w3(1)) + (w1(1) * w2(0) * w3(2)) - (w1(1) * w2(2) * w3(0)) - (w1(2) * w2(0) * w3(1)) + (w1(2) * w2(1) * w3(0)); return w4; } //-------------------------------------------------------------------------- // Invariant squared mass for REAL Wave4 (to save time). double m2(Wave4 w) { return real(w(0)) * real(w(0)) - real(w(1)) * real(w(1)) - real(w(2)) * real(w(2)) - real(w(3)) * real(w(3)); } double m2(Wave4 w1, Wave4 w2) { return real(w1(0)) * real(w2(0)) - real(w1(1)) * real(w2(1)) - real(w1(2)) * real(w2(2)) - real(w1(3)) * real(w2(3)); } //-------------------------------------------------------------------------- // Print a Wave4 vector. ostream& operator<< (ostream& os, Wave4 w) { os << left << setprecision(2); for (int i = 0; i < 4; i++) os << setw(20) << w.val[i]; os << "\n"; return os; } //========================================================================== // Constructor for the GammaMatrix class. Gamma(1) through Gamma(3) give the // corresponding gamma matrices using the Weyl basis as outlined in the HELAS // paper. Gamma(4) gives the +--- metric, while Gamma(5) gives the gamma^5 // matrix. GammaMatrix::GammaMatrix(int mu) { COMPLEXZERO = complex( 0., 0.); if (mu == 0) { val[0] = 1.; val[1] = 1.; val[2] = 1.; val[3] = 1.; index[0] = 2; index[1] = 3; index[2] = 0; index[3] = 1; } else if (mu == 1) { val[0] = -1.; val[1] = -1.; val[2] = 1.; val[3] = 1.; index[0] = 3; index[1] = 2; index[2] = 1; index[3] = 0; } else if (mu == 2) { val[0] = complex(0.,-1.); val[1] = complex(0.,1.); val[2] = complex(0.,1.); val[3] = complex(0.,-1.); index[0] = 3; index[1] = 2; index[2] = 1; index[3] = 0; } else if (mu == 3) { val[0] = -1.; val[1] = 1.; val[2] = 1.; val[3] = -1.; index[0] = 2; index[1] = 3; index[2] = 0; index[3] = 1; } else if (mu == 4) { val[0] = 1.; val[1] = -1.; val[2] = -1.; val[3] = -1.; index[0] = 0; index[1] = 1; index[2] = 2; index[3] = 3; } else if (mu == 5) { val[0] = -1.; val[1] = -1.; val[2] = 1.; val[3] = 1.; index[0] = 0; index[1] = 1; index[2] = 2; index[3] = 3; } } //-------------------------------------------------------------------------- // Wave4 * GammaMatrix. Wave4 operator*(Wave4 w, GammaMatrix g) { complex w0 = w(g.index[0]); complex w1 = w(g.index[1]); complex w2 = w(g.index[2]); complex w3 = w(g.index[3]); w(0) = w0 * g.val[0]; w(1) = w1 * g.val[1]; w(2) = w2 * g.val[2]; w(3) = w3 * g.val[3]; return w; } //-------------------------------------------------------------------------- // Scalar * GammaMatrix. GammaMatrix operator*(complex s, GammaMatrix g) { g.val[0] = s * g.val[0]; g.val[1] = s*g.val[1]; g.val[2] = s * g.val[2]; g.val[3] = s*g.val[3]; return g; } //-------------------------------------------------------------------------- // I * Scalar - Gamma5. GammaMatrix operator-(complex s, GammaMatrix g) { g.val[0] = s - g.val[0]; g.val[1] = s - g.val[1]; g.val[2] = s - g.val[2]; g.val[3] = s - g.val[3]; return g; } //-------------------------------------------------------------------------- // I * Scalar + Gamma5. GammaMatrix operator+(complex s, GammaMatrix g) { g.val[0] = s + g.val[0]; g.val[1] = s + g.val[1]; g.val[2] = s + g.val[2]; g.val[3] = s + g.val[3]; return g; } //-------------------------------------------------------------------------- // Print GammaMatrix. ostream& operator<< (ostream& os, GammaMatrix g) { os << left << setprecision(2); for (int i = 0; i < 4; i++) { for (int j = 0; j < 4; j++) os << setw(20) << g(i,j); os << "\n"; } return os; } //========================================================================== // Weyl helicity wave functions for spin 1/2 fermions and spin 1 boson. // This is the basis as given by the HELAS collaboration on page 122 of // "HELas: HELicity Amplitude Subroutines for Feynman Diagram Evaluations" // by H. Murayama, I. Watanabe, K. Hagiwara. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // The spinors become ill-defined for p -> -pz and the polarization vectors // become ill-defined when pT -> 0. For these special cases limits are used // and are triggered when the difference of the approached quantity falls // below the variable TOLERANCE. const double HelicityParticle::TOLERANCE = 0.000001; //-------------------------------------------------------------------------- // Return wave vector for given helicity. Wave4 HelicityParticle::wave(int h) { // Create wave vector to return. Wave4 w; // Fermion (spin 1/2) spinor. if (spinType() == 2) { // Calculate helicity independent normalization. double P = pAbs(); double n = sqrtpos(2*P*(P+pz())); bool aligned = (abs(P+pz()) < TOLERANCE); // Calculate eigenspinor basis. vector< vector > xi(2, vector(2)); // Helicity -1 xi[0][0] = aligned ? -1 : complex(-px(),py())/n; xi[0][1] = aligned ? 0 : (P+pz())/n; // Helicity +1 xi[1][0] = aligned ? 0 : (P+pz())/n; xi[1][1] = aligned ? 1 : complex(px(),py())/n; // Calculate helicity dependent normalization. vector omega(2); omega[0] = sqrtpos(e()-P); omega[1] = sqrtpos(e()+P); vector hsign(2,1); hsign[0] = -1; // Create particle spinor. if (this->id() > 0) { w(0) = omega[!h] * xi[h][0]; w(1) = omega[!h] * xi[h][1]; w(2) = omega[h] * xi[h][0]; w(3) = omega[h] * xi[h][1]; // Create anti-particle spinor. } else { w(0) = hsign[!h] * omega[h] * xi[!h][0]; w(1) = hsign[!h] * omega[h] * xi[!h][1]; w(2) = hsign[h] * omega[!h] * xi[!h][0]; w(3) = hsign[h] * omega[!h] * xi[!h][1]; } // Boson (spin 1) polarization vector. } else if (spinType() == 3) { double P = pAbs(); double PT = pT(); // Create helicity +1 or -1 polarization vector. if (h >= 0 && h <= 1) { double hsign = h ? -1 : 1; if (PT > TOLERANCE) { w(0) = 0; w(1) = complex(hsign * px() * pz() / (P * PT), -py() / PT); w(2) = complex(hsign * py() * pz() / (P * PT), px() / PT); w(3) = complex(-hsign * PT / P, 0); } else { w(0) = 0; w(1) = hsign * pz(); w(2) = 0; w(3) = 0; } // Create helicity 0 polarization vector (ensure boson massive). } else if (h == 2 && m() > TOLERANCE) { w(0) = P / m(); w(1) = px() * e() / (m() * P); w(2) = py() * e() / (m() * P); w(3) = pz() * e() / (m() * P); } // Unknown wave function. } else { w(0) = 0; w(1) = 0; w(2) = 0; w(3) = 0; } // Done. return w; } //-------------------------------------------------------------------------- // Bar of a wave function. Wave4 HelicityParticle::waveBar(int h) { if (spinType() == 2) return conj(wave(h)) * GammaMatrix(0); else return conj(wave(h)); } //-------------------------------------------------------------------------- // Normalize the rho or D matrices. void HelicityParticle::normalize(vector< vector >& matrix) { complex trace = 0; for (unsigned int i = 0; i < matrix.size(); i++) trace += matrix[i][i]; for (unsigned int i = 0; i < matrix.size(); i++) { for (unsigned int j = 0; j < matrix.size(); j++) { if (trace != complex(0,0)) matrix[i][j] /= trace; else matrix[i][j] = 1 / static_cast(matrix.size()); } } } //-------------------------------------------------------------------------- // Return the number of spin states. int HelicityParticle::spinStates() { int sT = spinType(); if (sT == 0) return 1; else if (sT != 2 && m() < TOLERANCE) return sT - 1; else return sT; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/ProcessContainer.cc0000644000175000017500000033221212217346247016723 0ustar sunsun// ProcessContainer.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // ProcessContainer and SetupContainers classes. #include "Pythia8/ProcessContainer.h" // Internal headers for special processes. #include "Pythia8/SigmaCompositeness.h" #include "Pythia8/SigmaEW.h" #include "Pythia8/SigmaExtraDim.h" #include "Pythia8/SigmaGeneric.h" #include "Pythia8/SigmaHiggs.h" #include "Pythia8/SigmaLeftRightSym.h" #include "Pythia8/SigmaLeptoquark.h" #include "Pythia8/SigmaNewGaugeBosons.h" #include "Pythia8/SigmaOnia.h" #include "Pythia8/SigmaQCD.h" #include "Pythia8/SigmaSUSY.h" namespace Pythia8 { //========================================================================== // ProcessContainer class. // Information allowing the generation of a specific process. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of event tries to check maximization finding reliability. const int ProcessContainer::N12SAMPLE = 100; // Ditto, but increased for 2 -> 3 processes. const int ProcessContainer::N3SAMPLE = 1000; //-------------------------------------------------------------------------- // Initialize phase space and counters. // Argument isFirst distinguishes two hard processes in same event. bool ProcessContainer::init(bool isFirst, Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtr, BeamParticle* beamBPtr, Couplings* couplingsPtr, SigmaTotal* sigmaTotPtr, ResonanceDecays* resDecaysPtrIn, SLHAinterface* slhaInterfacePtr, UserHooks* userHooksPtrIn) { // Extract info about current process from SigmaProcess object. isLHA = sigmaProcessPtr->isLHA(); isNonDiff = sigmaProcessPtr->isNonDiff(); isResolved = sigmaProcessPtr->isResolved(); isDiffA = sigmaProcessPtr->isDiffA(); isDiffB = sigmaProcessPtr->isDiffB(); isDiffC = sigmaProcessPtr->isDiffC(); isQCD3body = sigmaProcessPtr->isQCD3body(); int nFin = sigmaProcessPtr->nFinal(); lhaStrat = (isLHA) ? lhaUpPtr->strategy() : 0; lhaStratAbs = abs(lhaStrat); allowNegSig = sigmaProcessPtr->allowNegativeSigma(); // Flag for maximum violation handling. increaseMaximum = settings.flag("PhaseSpace:increaseMaximum"); // Pick and create phase space generator. Send pointers where required. if (isLHA) phaseSpacePtr = new PhaseSpaceLHA(); else if (isNonDiff) phaseSpacePtr = new PhaseSpace2to2nondiffractive(); else if (!isResolved && !isDiffA && !isDiffB && !isDiffC ) phaseSpacePtr = new PhaseSpace2to2elastic(); else if (!isResolved && !isDiffA && !isDiffB && isDiffC) phaseSpacePtr = new PhaseSpace2to3diffractive(); else if (!isResolved) phaseSpacePtr = new PhaseSpace2to2diffractive( isDiffA, isDiffB); else if (nFin == 1) phaseSpacePtr = new PhaseSpace2to1tauy(); else if (nFin == 2) phaseSpacePtr = new PhaseSpace2to2tauyz(); else if (isQCD3body) phaseSpacePtr = new PhaseSpace2to3yyycyl(); else phaseSpacePtr = new PhaseSpace2to3tauycyl(); // Store pointers and perform simple initialization. infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; resDecaysPtr = resDecaysPtrIn; userHooksPtr = userHooksPtrIn; canVetoResDecay = (userHooksPtr != 0) ? userHooksPtr->canVetoResonanceDecays() : false; if (isLHA) { sigmaProcessPtr->setLHAPtr(lhaUpPtr); phaseSpacePtr->setLHAPtr(lhaUpPtr); } sigmaProcessPtr->init(infoPtr, &settings, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr, sigmaTotPtr, slhaInterfacePtr); phaseSpacePtr->init( isFirst, sigmaProcessPtr, infoPtr, &settings, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr, sigmaTotPtr, userHooksPtr); // Reset cross section statistics. nTry = 0; nSel = 0; nAcc = 0; nTryStat = 0; sigmaMx = 0.; sigmaSum = 0.; sigma2Sum = 0.; sigmaNeg = 0.; sigmaAvg = 0.; sigmaFin = 0.; deltaFin = 0.; wtAccSum = 0.; // Initialize process and allowed incoming partons. sigmaProcessPtr->initProc(); if (!sigmaProcessPtr->initFlux()) return false; // Find maximum of differential cross section * phasespace. bool physical = phaseSpacePtr->setupSampling(); sigmaMx = phaseSpacePtr->sigmaMax(); double sigmaHalfWay = sigmaMx; // Separate signed maximum needed for LHA with negative weight. sigmaSgn = phaseSpacePtr->sigmaSumSigned(); // Check maximum by a few events, and extrapolate a further increase. if (physical & !isLHA) { int nSample = (nFin < 3) ? N12SAMPLE : N3SAMPLE; for (int iSample = 0; iSample < nSample; ++iSample) { bool test = false; while (!test) test = phaseSpacePtr->trialKin(false); if (iSample == nSample/2) sigmaHalfWay = phaseSpacePtr->sigmaMax(); } double sigmaFullWay = phaseSpacePtr->sigmaMax(); sigmaMx = (sigmaHalfWay > 0.) ? pow2(sigmaFullWay) / sigmaHalfWay : sigmaFullWay; phaseSpacePtr->setSigmaMax(sigmaMx); } // Allow Pythia to overwrite Les Houches lifetime input. setLifetime = settings.mode("LesHouches:setLifetime"); // Done. return physical; } //-------------------------------------------------------------------------- // Generate a trial event; selected or not. bool ProcessContainer::trialProcess() { // Loop over tries only occurs for Les Houches strategy = +-2. for (int iTry = 0; ; ++iTry) { // Generate a trial phase space point, if meaningful. if (sigmaMx == 0.) return false; infoPtr->setEndOfFile(false); bool repeatSame = (iTry > 0); bool physical = phaseSpacePtr->trialKin(true, repeatSame); // Note if at end of Les Houches file, else do statistics. if (isLHA && !physical) infoPtr->setEndOfFile(true); else { ++nTry; // Statistics for separate Les Houches process codes. Insert new codes. if (isLHA) { int codeLHANow = lhaUpPtr->idProcess(); int iFill = -1; for (int i = 0; i < int(codeLHA.size()); ++i) if (codeLHANow == codeLHA[i]) iFill = i; if (iFill >= 0) { ++nTryLHA[iFill]; } else { codeLHA.push_back(codeLHANow); nTryLHA.push_back(1); nSelLHA.push_back(0); nAccLHA.push_back(0); for (int i = int(codeLHA.size()) - 1; i > 0; --i) { if (codeLHA[i] < codeLHA[i - 1]) { swap(codeLHA[i], codeLHA[i - 1]); swap(nTryLHA[i], nTryLHA[i - 1]); swap(nSelLHA[i], nSelLHA[i - 1]); swap(nAccLHA[i], nAccLHA[i - 1]); } else break; } } } } // Possibly fail, else cross section. if (!physical) return false; double sigmaNow = phaseSpacePtr->sigmaNow(); // Tell if this event comes with weight from cross section. double sigmaWeight = 1.; if (!isLHA && !increaseMaximum && sigmaNow > sigmaMx) sigmaWeight = sigmaNow / sigmaMx; if ( lhaStrat < 0 && sigmaNow < 0.) sigmaWeight = -1.; if ( lhaStratAbs == 4) sigmaWeight = sigmaNow; // Also compensating weight from biased phase-space selection. double biasWeight = phaseSpacePtr->biasSelectionWeight(); weightNow = sigmaWeight * biasWeight; infoPtr->setWeight( weightNow, lhaStrat); // Check that not negative cross section when not allowed. if (!allowNegSig) { if (sigmaNow < sigmaNeg) { infoPtr->errorMsg("Warning in ProcessContainer::trialProcess: neg" "ative cross section set 0", "for " + sigmaProcessPtr->name() ); sigmaNeg = sigmaNow; } if (sigmaNow < 0.) sigmaNow = 0.; } // Cross section of process may come with a weight. Update sum. double sigmaAdd = sigmaNow * biasWeight; if (lhaStratAbs == 2 || lhaStratAbs == 3) sigmaAdd = sigmaSgn; sigmaSum += sigmaAdd; sigma2Sum += pow2(sigmaAdd); // Check if maximum violated. newSigmaMx = phaseSpacePtr->newSigmaMax(); if (newSigmaMx) sigmaMx = phaseSpacePtr->sigmaMax(); // Select or reject trial point. Statistics. bool select = true; if (lhaStratAbs < 3) select = (newSigmaMx || rndmPtr->flat() * abs(sigmaMx) < abs(sigmaNow)); if (select) { ++nSel; if (isLHA) { int codeLHANow = lhaUpPtr->idProcess(); int iFill = -1; for (int i = 0; i < int(codeLHA.size()); ++i) if (codeLHANow == codeLHA[i]) iFill = i; if (iFill >= 0) ++nSelLHA[iFill]; } } if (select || lhaStratAbs != 2) return select; } } //-------------------------------------------------------------------------- // Accumulate statistics after user veto, including LHA code. void ProcessContainer::accumulate() { ++nAcc; wtAccSum += weightNow; if (isLHA) { int codeLHANow = lhaUpPtr->idProcess(); int iFill = -1; for (int i = 0; i < int(codeLHA.size()); ++i) if (codeLHANow == codeLHA[i]) iFill = i; if (iFill >= 0) ++nAccLHA[iFill]; } } //-------------------------------------------------------------------------- // Pick flavours and colour flow of process. bool ProcessContainer::constructState() { // Construct flavour and colours for selected event. if (isResolved && !isNonDiff) sigmaProcessPtr->pickInState(); sigmaProcessPtr->setIdColAcol(); // Done. return true; } //-------------------------------------------------------------------------- // Give the hard subprocess with kinematics. bool ProcessContainer::constructProcess( Event& process, bool isHardest) { // Construct kinematics from selected phase space point. if (!phaseSpacePtr->finalKin()) return false; int nFin = sigmaProcessPtr->nFinal(); // Basic info on process. if (isHardest) infoPtr->setType( name(), code(), nFin, isNonDiff, isResolved, isDiffA, isDiffB, isDiffC, isLHA); // Let hard process record begin with the event as a whole and // the two incoming beam particles. process.append( 90, -11, 0, 0, 0, 0, 0, 0, Vec4(0., 0., 0., infoPtr->eCM()), infoPtr->eCM(), 0. ); process.append( infoPtr->idA(), -12, 0, 0, 0, 0, 0, 0, Vec4(0., 0., infoPtr->pzA(), infoPtr->eA()), infoPtr->mA(), 0. ); process.append( infoPtr->idB(), -12, 0, 0, 0, 0, 0, 0, Vec4(0., 0., infoPtr->pzB(), infoPtr->eB()), infoPtr->mB(), 0. ); // For nondiffractive process no interaction selected so far, so done. if (isNonDiff) return true; // Entries 3 and 4, now to be added, come from 1 and 2. process[1].daughter1(3); process[2].daughter1(4); double scale = 0.; double scalup = 0.; // For DiffC entries 3 - 5 come jointly from 1 and 2 (to keep HepMC happy). if (isDiffC) { process[1].daughters(3, 5); process[2].daughters(3, 5); } // Insert the subprocess partons - resolved processes. int idRes = sigmaProcessPtr->idSChannel(); if (isResolved && !isLHA) { // NOAM: Mothers and daughters without/with intermediate state. int m_M1 = 3; int m_M2 = 4; int m_D1 = 5; int m_D2 = (nFin == 1) ? 0 : 4 + nFin; if (idRes != 0) { m_M1 = 5; m_M2 = 0; m_D1 = 5; m_D2 = 0; } // Find scale from which to begin MPI/ISR/FSR evolution. scale = sqrt(Q2Fac()); process.scale( scale ); // Loop over incoming and outgoing partons. int colOffset = process.lastColTag(); for (int i = 1; i <= 2 + nFin; ++i) { // Read out particle info from SigmaProcess object. int id = sigmaProcessPtr->id(i); int status = (i <= 2) ? -21 : 23; int mother1 = (i <= 2) ? i : m_M1 ; int mother2 = (i <= 2) ? 0 : m_M2 ; int daughter1 = (i <= 2) ? m_D1 : 0; int daughter2 = (i <= 2) ? m_D2 : 0; int col = sigmaProcessPtr->col(i); if (col > 0) col += colOffset; else if (col < 0) col -= colOffset; int acol = sigmaProcessPtr->acol(i); if (acol > 0) acol += colOffset; else if (acol < 0) acol -= colOffset; // Append to process record. int iNow = process.append( id, status, mother1, mother2, daughter1, daughter2, col, acol, phaseSpacePtr->p(i), phaseSpacePtr->m(i), scale); // NOAM: If there is an intermediate state, insert the it in // the process record after the two incoming particles. if (i == 2 && idRes != 0) { // Sign of intermediate state: go by charge. if (particleDataPtr->hasAnti(idRes) && process[3].chargeType() + process[4].chargeType() < 0) idRes *= -1; // The colour configuration of the intermediate state has to be // resolved separately. col = 0; acol = 0; int m_col1 = sigmaProcessPtr->col(1); int m_acol1 = sigmaProcessPtr->acol(1); int m_col2 = sigmaProcessPtr->col(2); int m_acol2 = sigmaProcessPtr->acol(2); if (m_col1 == m_acol2 && m_col2 != m_acol1) { col = m_col2; acol = m_acol1; } else if (m_col2 == m_acol1 && m_col1 != m_acol2) { col = m_col1; acol = m_acol2; } if ( col > 0) col += colOffset; else if ( col < 0) col -= colOffset; if (acol > 0) acol += colOffset; else if (acol < 0) acol -= colOffset; // Insert the intermediate state into the event record. Vec4 pIntMed = phaseSpacePtr->p(1) + phaseSpacePtr->p(2); process.append( idRes, -22, 3, 4, 6, 5 + nFin, col, acol, pIntMed, pIntMed.mCalc(), scale); } // Pick lifetime where relevant, else not. if (process[iNow].tau0() > 0.) process[iNow].tau( process[iNow].tau0() * rndmPtr->exp() ); } } // Insert the outgoing particles - unresolved processes. else if (!isLHA) { int id3 = sigmaProcessPtr->id(3); int status3 = (id3 == process[1].id()) ? 14 : 15; process.append( id3, status3, 1, 0, 0, 0, 0, 0, phaseSpacePtr->p(3), phaseSpacePtr->m(3)); int id4 = sigmaProcessPtr->id(4); int status4 = (id4 == process[2].id()) ? 14 : 15; process.append( id4, status4, 2, 0, 0, 0, 0, 0, phaseSpacePtr->p(4), phaseSpacePtr->m(4)); // For central diffraction: two scattered protons inserted so far, // but modify mothers, add also centrally-produced hadronic system. if (isDiffC) { process[3].mothers( 1, 2); process[4].mothers( 1, 2); int id5 = sigmaProcessPtr->id(5); int status5 = 15; process.append( id5, status5, 1, 2, 0, 0, 0, 0, phaseSpacePtr->p(5), phaseSpacePtr->m(5)); } } // Insert the outgoing particles - Les Houches Accord processes. else { // Since LHA partons may be out of order, determine correct one. // (Recall that zeroth particle is empty.) vector newPos; newPos.reserve(lhaUpPtr->sizePart()); newPos.push_back(0); for (int iNew = 0; iNew < lhaUpPtr->sizePart(); ++iNew) { // For iNew == 0 look for the two incoming partons, then for // partons having them as mothers, and so on layer by layer. for (int i = 1; i < lhaUpPtr->sizePart(); ++i) if (lhaUpPtr->mother1(i) == newPos[iNew]) newPos.push_back(i); if (int(newPos.size()) <= iNew) break; } // Find scale from which to begin MPI/ISR/FSR evolution. scalup = lhaUpPtr->scale(); scale = scalup; double scalePr = (scale < 0.) ? sqrt(Q2Fac()) : scale; process.scale( scalePr); // Copy over info from LHA event to process, in proper order. for (int i = 1; i < lhaUpPtr->sizePart(); ++i) { int iOld = newPos[i]; int id = lhaUpPtr->id(iOld); // Translate from LHA status codes. int lhaStatus = lhaUpPtr->status(iOld); int status = -21; if (lhaStatus == 2 || lhaStatus == 3) status = -22; if (lhaStatus == 1) status = 23; // Find where mothers have been moved by reordering. int mother1Old = lhaUpPtr->mother1(iOld); int mother2Old = lhaUpPtr->mother2(iOld); int mother1 = 0; int mother2 = 0; for (int im = 1; im < i; ++im) { if (mother1Old == newPos[im]) mother1 = im + 2; if (mother2Old == newPos[im]) mother2 = im + 2; } if (i <= 2) mother1 = i; // Ensure that second mother = 0 except for bona fide carbon copies. if (mother1 > 0 && mother2 == mother1) { int sister1 = process[mother1].daughter1(); int sister2 = process[mother1].daughter2(); if (sister2 != sister1 && sister2 != 0) mother2 = 0; } // Find daughters and where they have been moved by reordering. // (Values shifted two steps to account for inserted beams.) int daughter1 = 0; int daughter2 = 0; for (int im = i + 1; im < lhaUpPtr->sizePart(); ++im) { if (lhaUpPtr->mother1(newPos[im]) == iOld || lhaUpPtr->mother2(newPos[im]) == iOld) { if (daughter1 == 0 || im + 2 < daughter1) daughter1 = im + 2; if (daughter2 == 0 || im + 2 > daughter2) daughter2 = im + 2; } } // For 2 -> 1 hard scatterings reset second daughter to 0. if (daughter2 == daughter1) daughter2 = 0; // Colour trivial, except reset irrelevant colour indices. int colType = particleDataPtr->colType(id); int col1 = (colType == 1 || colType == 2 || abs(colType) == 3) ? lhaUpPtr->col1(iOld) : 0; int col2 = (colType == -1 || colType == 2 || abs(colType) == 3) ? lhaUpPtr->col2(iOld) : 0; // Momentum trivial. double px = lhaUpPtr->px(iOld); double py = lhaUpPtr->py(iOld); double pz = lhaUpPtr->pz(iOld); double e = lhaUpPtr->e(iOld); double m = lhaUpPtr->m(iOld); // Polarization. double pol = lhaUpPtr->spin(iOld); // Allow scale setting for generic partons. double scaleShow = lhaUpPtr->scale(iOld); // For resonance decay products use resonance mass as scale. double scaleNow = scalePr; if (mother1 > 4) scaleNow = process[mother1].m(); if (scaleShow >= 0.0) scaleNow = scaleShow; // Store Les Houches Accord partons. int iNow = process.append( id, status, mother1, mother2, daughter1, daughter2, col1, col2, Vec4(px, py, pz, e), m, scaleNow, pol); // Check if need to store lifetime. double tau = lhaUpPtr->tau(iOld); if ( (setLifetime == 1 && abs(id) == 15) || setLifetime == 2) tau = process[iNow].tau0() * rndmPtr->exp(); if (tau > 0.) process[iNow].tau(tau); } } // Loop through decay chains and set secondary vertices when needed. for (int i = 3; i < process.size(); ++i) { int iMother = process[i].mother1(); // If sister to already assigned vertex then assign same. if ( process[i - 1].mother1() == iMother && process[i - 1].hasVertex() ) process[i].vProd( process[i - 1].vProd() ); // Else if mother already has vertex and/or lifetime then assign. else if ( process[iMother].hasVertex() || process[iMother].tau() > 0.) process[i].vProd( process[iMother].vDec() ); } // Further info on process. Reset quantities that may or may not be known. int id1Now = process[3].id(); int id2Now = process[4].id(); int id1pdf = 0; int id2pdf = 0; double x1pdf = 0.; double x2pdf = 0.; double pdf1 = 0.; double pdf2 = 0.; double tHat = 0.; double uHat = 0.; double pTHatL = 0.; double m3 = 0.; double m4 = 0.; double theta = 0.; double phi = 0.; double x1Now, x2Now, Q2FacNow, alphaEM, alphaS, Q2Ren, sHat; // Internally generated and stored information. if (!isLHA) { id1pdf = id1Now; id2pdf = id2Now; x1Now = phaseSpacePtr->x1(); x2Now = phaseSpacePtr->x2(); x1pdf = x1Now; x2pdf = x2Now; pdf1 = sigmaProcessPtr->pdf1(); pdf2 = sigmaProcessPtr->pdf2(); Q2FacNow = sigmaProcessPtr->Q2Fac(); alphaEM = sigmaProcessPtr->alphaEMRen(); alphaS = sigmaProcessPtr->alphaSRen(); Q2Ren = sigmaProcessPtr->Q2Ren(); sHat = phaseSpacePtr->sHat(); tHat = phaseSpacePtr->tHat(); uHat = phaseSpacePtr->uHat(); pTHatL = phaseSpacePtr->pTHat(); m3 = phaseSpacePtr->m(3); m4 = phaseSpacePtr->m(4); theta = phaseSpacePtr->thetaHat(); phi = phaseSpacePtr->phiHat(); } // Les Houches Accord process partly available, partly to be constructed. else { x1Now = 2. * process[3].e() / infoPtr->eCM(); x2Now = 2. * process[4].e() / infoPtr->eCM(); Q2FacNow = (scale < 0.) ? sigmaProcessPtr->Q2Fac() : pow2(scale); alphaEM = lhaUpPtr->alphaQED(); if (alphaEM < 0.001) alphaEM = sigmaProcessPtr->alphaEMRen(); alphaS = lhaUpPtr->alphaQCD(); if (alphaS < 0.001) alphaS = sigmaProcessPtr->alphaSRen(); Q2Ren = (scale < 0.) ? sigmaProcessPtr->Q2Ren() : pow2(scale); Vec4 pSum = process[3].p() + process[4].p(); sHat = pSum * pSum; int nFinLH = 0; double pTLH = 0.; for (int i = 5; i < process.size(); ++i) if (process[i].mother1() == 3 && process[i].mother2() == 4) { ++nFinLH; pTLH += process[i].pT(); } if (nFinLH > 0) pTHatL = pTLH / nFinLH; // Read info on parton densities if provided. id1pdf = lhaUpPtr->id1pdf(); id2pdf = lhaUpPtr->id2pdf(); x1pdf = lhaUpPtr->x1pdf(); x2pdf = lhaUpPtr->x2pdf(); if (lhaUpPtr->pdfIsSet()) { pdf1 = lhaUpPtr->pdf1(); pdf2 = lhaUpPtr->pdf2(); Q2FacNow = pow2(lhaUpPtr->scalePDF()); } // Reconstruct kinematics of 2 -> 2 processes from momenta. if (nFin == 2) { Vec4 pDifT = process[3].p() - process[5].p(); tHat = pDifT * pDifT; Vec4 pDifU = process[3].p() - process[6].p(); uHat = pDifU * pDifU; pTHatL = process[5].pT(); m3 = process[5].m(); m4 = process[6].m(); Vec4 p5 = process[5].p(); p5.bstback(pSum); theta = p5.theta(); phi = process[5].phi(); } } // Store information. if (isHardest) { infoPtr->setPDFalpha( 0, id1pdf, id2pdf, x1pdf, x2pdf, pdf1, pdf2, Q2FacNow, alphaEM, alphaS, Q2Ren, scalup); infoPtr->setKin( 0, id1Now, id2Now, x1Now, x2Now, sHat, tHat, uHat, pTHatL, m3, m4, theta, phi); } infoPtr->setTypeMPI( code(), pTHatL); // For Les Houches event store subprocess classification. if (isLHA) { int codeSub = lhaUpPtr->idProcess(); ostringstream nameSub; nameSub << "user process " << codeSub; infoPtr->setSubType( 0, nameSub.str(), codeSub, nFin); } // Done. return true; } //-------------------------------------------------------------------------- // Give the hard resonance decay chain from Les Houches input. // Note: mildly modified copy of some constructProcess code; to streamline. bool ProcessContainer::constructDecays( Event& process) { // Let hard process record begin with the event as a whole. process.clear(); process.append( 90, -11, 0, 0, 0, 0, 0, 0, Vec4(0., 0., 0., 0.), 0., 0. ); // Since LHA partons may be out of order, determine correct one. // (Recall that zeroth particle is empty.) vector newPos; newPos.reserve(lhaUpPtr->sizePart()); newPos.push_back(0); for (int iNew = 0; iNew < lhaUpPtr->sizePart(); ++iNew) { // For iNew == 0 look for the two incoming partons, then for // partons having them as mothers, and so on layer by layer. for (int i = 1; i < lhaUpPtr->sizePart(); ++i) if (lhaUpPtr->mother1(i) == newPos[iNew]) newPos.push_back(i); if (int(newPos.size()) <= iNew) break; } // Find scale from which to begin MPI/ISR/FSR evolution. double scale = lhaUpPtr->scale(); process.scale( scale); Vec4 pSum; // Copy over info from LHA event to process, in proper order. for (int i = 1; i < lhaUpPtr->sizePart(); ++i) { int iOld = newPos[i]; int id = lhaUpPtr->id(iOld); // Translate from LHA status codes. int lhaStatus = lhaUpPtr->status(iOld); int status = -21; if (lhaStatus == 2 || lhaStatus == 3) status = -22; if (lhaStatus == 1) status = 23; // Find where mothers have been moved by reordering. int mother1Old = lhaUpPtr->mother1(iOld); int mother2Old = lhaUpPtr->mother2(iOld); int mother1 = 0; int mother2 = 0; for (int im = 1; im < i; ++im) { if (mother1Old == newPos[im]) mother1 = im; if (mother2Old == newPos[im]) mother2 = im; } // Ensure that second mother = 0 except for bona fide carbon copies. if (mother1 > 0 && mother2 == mother1) { int sister1 = process[mother1].daughter1(); int sister2 = process[mother1].daughter2(); if (sister2 != sister1 && sister2 != 0) mother2 = 0; } // Find daughters and where they have been moved by reordering. int daughter1 = 0; int daughter2 = 0; for (int im = i + 1; im < lhaUpPtr->sizePart(); ++im) { if (lhaUpPtr->mother1(newPos[im]) == iOld || lhaUpPtr->mother2(newPos[im]) == iOld) { if (daughter1 == 0 || im < daughter1) daughter1 = im; if (daughter2 == 0 || im > daughter2) daughter2 = im; } } // For 2 -> 1 hard scatterings reset second daughter to 0. if (daughter2 == daughter1) daughter2 = 0; // Colour trivial, except reset irrelevant colour indices. int colType = particleDataPtr->colType(id); int col1 = (colType == 1 || colType == 2 || abs(colType) == 3) ? lhaUpPtr->col1(iOld) : 0; int col2 = (colType == -1 || colType == 2 || abs(colType) == 3) ? lhaUpPtr->col2(iOld) : 0; // Momentum trivial. double px = lhaUpPtr->px(iOld); double py = lhaUpPtr->py(iOld); double pz = lhaUpPtr->pz(iOld); double e = lhaUpPtr->e(iOld); double m = lhaUpPtr->m(iOld); if (status > 0) pSum += Vec4( px, py, pz, e); // Polarization. double pol = lhaUpPtr->spin(iOld); // For resonance decay products use resonance mass as scale. double scaleNow = scale; if (mother1 > 0) scaleNow = process[mother1].m(); // Store Les Houches Accord partons. int iNow = process.append( id, status, mother1, mother2, daughter1, daughter2, col1, col2, Vec4(px, py, pz, e), m, scaleNow, pol); // Check if need to store lifetime. double tau = lhaUpPtr->tau(iOld); if ( (setLifetime == 1 && abs(id) == 15) || setLifetime == 2) tau = process[iNow].tau0() * rndmPtr->exp(); if (tau > 0.) process[iNow].tau(tau); } // Update four-momentum of system as a whole. process[0].p( pSum); process[0].m( pSum.mCalc()); // Loop through decay chains and set secondary vertices when needed. for (int i = 1; i < process.size(); ++i) { int iMother = process[i].mother1(); // If sister to already assigned vertex then assign same. if ( process[i - 1].mother1() == iMother && process[i - 1].hasVertex() && i > 1) process[i].vProd( process[i - 1].vProd() ); // Else if mother already has vertex and/or lifetime then assign. else if ( process[iMother].hasVertex() || process[iMother].tau() > 0.) process[i].vProd( process[iMother].vDec() ); } // Done. return true; } //-------------------------------------------------------------------------- // Handle resonance decays. bool ProcessContainer::decayResonances( Event& process) { // Save current event-record size and status codes. process.saveSize(); vector statusSave( process.size()); for (int i = 0; i < process.size(); ++i) statusSave[i] = process[i].status(); bool physical = true; bool newChain = false; bool newFlavours = false; // Do loop over user veto. do { // Do sequential chain of uncorrelated isotropic decays. do { physical = resDecaysPtr->next( process); if (!physical) return false; // Check whether flavours should be correlated. // (Currently only relevant for f fbar -> gamma*/Z0 gamma*/Z0.) newFlavours = ( sigmaProcessPtr->weightDecayFlav( process) < rndmPtr->flat() ); // Reset the decay chains if have to redo. if (newFlavours) { process.restoreSize(); for (int i = 0; i < process.size(); ++i) process[i].status( statusSave[i]); } // Loop back where required to generate new decays with new flavours. } while (newFlavours); // Correct to nonisotropic decays. phaseSpacePtr->decayKinematics( process); // Optionally user hooks check/veto on decay chain. if (canVetoResDecay) newChain = userHooksPtr->doVetoResonanceDecays( process); // Reset the decay chains if have to redo. if (newChain) { process.restoreSize(); for (int i = 0; i < process.size(); ++i) process[i].status( statusSave[i]); } // Loop back where required to generate new decay chain. } while(newChain); // Done. return true; } //-------------------------------------------------------------------------- // Reset event generation statistics; but NOT maximum of cross section. void ProcessContainer::reset() { nTry = 0; nSel = 0; nAcc = 0; nTryStat = 0; sigmaSum = 0.; sigma2Sum = 0.; sigmaNeg = 0.; sigmaAvg = 0.; sigmaFin = 0.; deltaFin = 0.; wtAccSum = 0.; } //-------------------------------------------------------------------------- // Estimate integrated cross section and its uncertainty. void ProcessContainer::sigmaDelta() { // Initial values. No analysis meaningful unless accepted events. nTryStat = nTry; sigmaAvg = 0.; sigmaFin = 0.; deltaFin = 0.; if (nAcc == 0) return; // Average value. No error analysis unless at least two events. double nTryInv = 1. / nTry; double nSelInv = 1. / nSel; double nAccInv = 1. / nAcc; sigmaAvg = sigmaSum * nTryInv; double fracAcc = nAcc * nSelInv; sigmaFin = sigmaAvg * fracAcc; deltaFin = sigmaFin; if (nAcc == 1) return; // Estimated error. Quadratic sum of cross section term and // binomial from accept/reject step. double delta2Sig = (lhaStratAbs != 3) ? (sigma2Sum * nTryInv - pow2(sigmaAvg)) * nTryInv / pow2(sigmaAvg) : pow2( lhaUpPtr->xErrSum() / lhaUpPtr->xSecSum()); double delta2Veto = (nSel - nAcc) * nAccInv * nSelInv; double delta2Sum = delta2Sig + delta2Veto; deltaFin = sqrtpos(delta2Sum) * sigmaFin; } //========================================================================== // SetupContainer class. // Turns list of user-desired processes into a vector of containers. //-------------------------------------------------------------------------- // Main routine to initialize list of processes. bool SetupContainers::init(vector& containerPtrs, Settings& settings, ParticleData* particleDataPtr, Couplings* couplings) { // Reset process list, if filled in previous subrun. if (containerPtrs.size() > 0) { for (int i = 0; i < int(containerPtrs.size()); ++i) delete containerPtrs[i]; containerPtrs.clear(); } SigmaProcess* sigmaPtr; // Set up requested objects for soft QCD processes. bool softQCD = settings.flag("SoftQCD:all"); bool inelastic = settings.flag("SoftQCD:inelastic"); if (softQCD || inelastic || settings.flag("SoftQCD:nonDiffractive")) { sigmaPtr = new Sigma0nonDiffractive; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (softQCD || settings.flag("SoftQCD:elastic")) { sigmaPtr = new Sigma0AB2AB; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (softQCD || inelastic || settings.flag("SoftQCD:singleDiffractive")) { sigmaPtr = new Sigma0AB2XB; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma0AB2AX; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (softQCD || inelastic || settings.flag("SoftQCD:doubleDiffractive")) { sigmaPtr = new Sigma0AB2XX; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (softQCD || inelastic || settings.flag("SoftQCD:centralDiffractive")) { sigmaPtr = new Sigma0AB2AXB; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for hard QCD processes. bool hardQCD = settings.flag("HardQCD:all"); if (hardQCD || settings.flag("HardQCD:gg2gg")) { sigmaPtr = new Sigma2gg2gg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD || settings.flag("HardQCD:gg2qqbar")) { sigmaPtr = new Sigma2gg2qqbar; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD || settings.flag("HardQCD:qg2qg")) { sigmaPtr = new Sigma2qg2qg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD || settings.flag("HardQCD:qq2qq")) { sigmaPtr = new Sigma2qq2qq; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD || settings.flag("HardQCD:qqbar2gg")) { sigmaPtr = new Sigma2qqbar2gg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD || settings.flag("HardQCD:qqbar2qqbarNew")) { sigmaPtr = new Sigma2qqbar2qqbarNew; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for c cbar and b bbar, also hard QCD. bool hardccbar = settings.flag("HardQCD:hardccbar"); if (hardQCD || hardccbar || settings.flag("HardQCD:gg2ccbar")) { sigmaPtr = new Sigma2gg2QQbar(4, 121); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD || hardccbar || settings.flag("HardQCD:qqbar2ccbar")) { sigmaPtr = new Sigma2qqbar2QQbar(4, 122); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } bool hardbbbar = settings.flag("HardQCD:hardbbbar"); if (hardQCD || hardbbbar || settings.flag("HardQCD:gg2bbbar")) { sigmaPtr = new Sigma2gg2QQbar(5, 123); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD || hardbbbar || settings.flag("HardQCD:qqbar2bbbar")) { sigmaPtr = new Sigma2qqbar2QQbar(5, 124); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for hard QCD 2 -> 3 processes. bool hardQCD3parton = settings.flag("HardQCD:3parton"); if (hardQCD3parton || settings.flag("HardQCD:gg2ggg")) { sigmaPtr = new Sigma3gg2ggg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD3parton || settings.flag("HardQCD:qqbar2ggg")) { sigmaPtr = new Sigma3qqbar2ggg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD3parton || settings.flag("HardQCD:qg2qgg")) { sigmaPtr = new Sigma3qg2qgg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD3parton || settings.flag("HardQCD:qq2qqgDiff")) { sigmaPtr = new Sigma3qq2qqgDiff; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD3parton || settings.flag("HardQCD:qq2qqgSame")) { sigmaPtr = new Sigma3qq2qqgSame; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD3parton || settings.flag("HardQCD:qqbar2qqbargDiff")) { sigmaPtr = new Sigma3qqbar2qqbargDiff; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD3parton || settings.flag("HardQCD:qqbar2qqbargSame")) { sigmaPtr = new Sigma3qqbar2qqbargSame; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD3parton || settings.flag("HardQCD:gg2qqbarg")) { sigmaPtr = new Sigma3gg2qqbarg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD3parton || settings.flag("HardQCD:qg2qqqbarDiff")) { sigmaPtr = new Sigma3qg2qqqbarDiff; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hardQCD3parton || settings.flag("HardQCD:qg2qqqbarSame")) { sigmaPtr = new Sigma3qg2qqqbarSame; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for prompt photon processes. bool promptPhotons = settings.flag("PromptPhoton:all"); if (promptPhotons || settings.flag("PromptPhoton:qg2qgamma")) { sigmaPtr = new Sigma2qg2qgamma; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (promptPhotons || settings.flag("PromptPhoton:qqbar2ggamma")) { sigmaPtr = new Sigma2qqbar2ggamma; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (promptPhotons || settings.flag("PromptPhoton:gg2ggamma")) { sigmaPtr = new Sigma2gg2ggamma; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (promptPhotons || settings.flag("PromptPhoton:ffbar2gammagamma")) { sigmaPtr = new Sigma2ffbar2gammagamma; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (promptPhotons || settings.flag("PromptPhoton:gg2gammagamma")) { sigmaPtr = new Sigma2gg2gammagamma; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for weak gauge boson t-channel exchange. bool weakBosonExchanges = settings.flag("WeakBosonExchange:all"); if (weakBosonExchanges || settings.flag("WeakBosonExchange:ff2ff(t:gmZ)")) { sigmaPtr = new Sigma2ff2fftgmZ; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakBosonExchanges || settings.flag("WeakBosonExchange:ff2ff(t:W)")) { sigmaPtr = new Sigma2ff2fftW; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for weak gauge boson processes. bool weakSingleBosons = settings.flag("WeakSingleBoson:all"); if (weakSingleBosons || settings.flag("WeakSingleBoson:ffbar2gmZ")) { sigmaPtr = new Sigma1ffbar2gmZ; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakSingleBosons || settings.flag("WeakSingleBoson:ffbar2W")) { sigmaPtr = new Sigma1ffbar2W; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested object for s-channel gamma exchange. // Subset of gamma*/Z0 above, intended for multiparton interactions. if (settings.flag("WeakSingleBoson:ffbar2ffbar(s:gm)")) { sigmaPtr = new Sigma2ffbar2ffbarsgm; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for weak gauge boson pair processes. bool weakDoubleBosons = settings.flag("WeakDoubleBoson:all"); if (weakDoubleBosons || settings.flag("WeakDoubleBoson:ffbar2gmZgmZ")) { sigmaPtr = new Sigma2ffbar2gmZgmZ; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakDoubleBosons || settings.flag("WeakDoubleBoson:ffbar2ZW")) { sigmaPtr = new Sigma2ffbar2ZW; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakDoubleBosons || settings.flag("WeakDoubleBoson:ffbar2WW")) { sigmaPtr = new Sigma2ffbar2WW; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for weak gauge boson + parton processes. bool weakBosonAndPartons = settings.flag("WeakBosonAndParton:all"); if (weakBosonAndPartons || settings.flag("WeakBosonAndParton:qqbar2gmZg")) { sigmaPtr = new Sigma2qqbar2gmZg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakBosonAndPartons || settings.flag("WeakBosonAndParton:qg2gmZq")) { sigmaPtr = new Sigma2qg2gmZq; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakBosonAndPartons || settings.flag("WeakBosonAndParton:ffbar2gmZgm")) { sigmaPtr = new Sigma2ffbar2gmZgm; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakBosonAndPartons || settings.flag("WeakBosonAndParton:fgm2gmZf")) { sigmaPtr = new Sigma2fgm2gmZf; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakBosonAndPartons || settings.flag("WeakBosonAndParton:qqbar2Wg")) { sigmaPtr = new Sigma2qqbar2Wg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakBosonAndPartons || settings.flag("WeakBosonAndParton:qg2Wq")) { sigmaPtr = new Sigma2qg2Wq; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakBosonAndPartons || settings.flag("WeakBosonAndParton:ffbar2Wgm")) { sigmaPtr = new Sigma2ffbar2Wgm; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (weakBosonAndPartons || settings.flag("WeakBosonAndParton:fgm2Wf")) { sigmaPtr = new Sigma2fgm2Wf; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for photon collision processes. bool photonCollisions = settings.flag("PhotonCollision:all"); if (photonCollisions || settings.flag("PhotonCollision:gmgm2qqbar")) { sigmaPtr = new Sigma2gmgm2ffbar(1, 261); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (photonCollisions || settings.flag("PhotonCollision:gmgm2ccbar")) { sigmaPtr = new Sigma2gmgm2ffbar(4, 262); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (photonCollisions || settings.flag("PhotonCollision:gmgm2bbbar")) { sigmaPtr = new Sigma2gmgm2ffbar(5, 263); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (photonCollisions || settings.flag("PhotonCollision:gmgm2ee")) { sigmaPtr = new Sigma2gmgm2ffbar(11, 264); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (photonCollisions || settings.flag("PhotonCollision:gmgm2mumu")) { sigmaPtr = new Sigma2gmgm2ffbar(13, 265); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (photonCollisions || settings.flag("PhotonCollision:gmgm2tautau")) { sigmaPtr = new Sigma2gmgm2ffbar(15, 266); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for charmonium production bool charmoniums = settings.flag("Charmonium:all"); if (charmoniums || settings.flag("Charmonium:gg2QQbar[3S1(1)]g")) { sigmaPtr = new Sigma2gg2QQbar3S11g(4, 401); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:gg2QQbar[3P0(1)]g")) { sigmaPtr = new Sigma2gg2QQbar3PJ1g(4, 0, 402); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:gg2QQbar[3P1(1)]g")) { sigmaPtr = new Sigma2gg2QQbar3PJ1g(4, 1, 403); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:gg2QQbar[3P2(1)]g")) { sigmaPtr = new Sigma2gg2QQbar3PJ1g(4, 2, 404); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qg2QQbar[3P0(1)]q")) { sigmaPtr = new Sigma2qg2QQbar3PJ1q(4, 0, 405); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qg2QQbar[3P1(1)]q")) { sigmaPtr = new Sigma2qg2QQbar3PJ1q(4, 1, 406); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qg2QQbar[3P2(1)]q")) { sigmaPtr = new Sigma2qg2QQbar3PJ1q(4, 2, 407); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qqbar2QQbar[3P0(1)]g")) { sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(4, 0, 408); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qqbar2QQbar[3P1(1)]g")) { sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(4, 1, 409); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qqbar2QQbar[3P2(1)]g")) { sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(4, 2, 410); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:gg2QQbar[3S1(8)]g")) { sigmaPtr = new Sigma2gg2QQbarX8g(4, 0, 411); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:gg2QQbar[1S0(8)]g")) { sigmaPtr = new Sigma2gg2QQbarX8g(4, 1, 412); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:gg2QQbar[3PJ(8)]g")) { sigmaPtr = new Sigma2gg2QQbarX8g(4, 2, 413); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qg2QQbar[3S1(8)]q")) { sigmaPtr = new Sigma2qg2QQbarX8q(4, 0, 414); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qg2QQbar[1S0(8)]q")) { sigmaPtr = new Sigma2qg2QQbarX8q(4, 1, 415); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qg2QQbar[3PJ(8)]q")) { sigmaPtr = new Sigma2qg2QQbarX8q(4, 2, 416); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qqbar2QQbar[3S1(8)]g")) { sigmaPtr = new Sigma2qqbar2QQbarX8g(4, 0, 417); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qqbar2QQbar[1S0(8)]g")) { sigmaPtr = new Sigma2qqbar2QQbarX8g(4, 1, 418); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (charmoniums || settings.flag("Charmonium:qqbar2QQbar[3PJ(8)]g")) { sigmaPtr = new Sigma2qqbar2QQbarX8g(4, 2, 419); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for bottomonium production bool bottomoniums = settings.flag("Bottomonium:all"); if (bottomoniums || settings.flag("Bottomonium:gg2QQbar[3S1(1)]g")) { sigmaPtr = new Sigma2gg2QQbar3S11g(5, 501); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:gg2QQbar[3P0(1)]g")) { sigmaPtr = new Sigma2gg2QQbar3PJ1g(5, 0, 502); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:gg2QQbar[3P1(1)]g")) { sigmaPtr = new Sigma2gg2QQbar3PJ1g(5, 1, 503); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:gg2QQbar[3P2(1)]g")) { sigmaPtr = new Sigma2gg2QQbar3PJ1g(5, 2, 504); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qg2QQbar[3P0(1)]q")) { sigmaPtr = new Sigma2qg2QQbar3PJ1q(5, 0, 505); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qg2QQbar[3P1(1)]q")) { sigmaPtr = new Sigma2qg2QQbar3PJ1q(5, 1, 506); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qg2QQbar[3P2(1)]q")) { sigmaPtr = new Sigma2qg2QQbar3PJ1q(5, 2, 507); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qqbar2QQbar[3P0(1)]g")) { sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(5, 0, 508); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qqbar2QQbar[3P1(1)]g")) { sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(5, 1, 509); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qqbar2QQbar[3P2(1)]g")) { sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(5, 2, 510); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:gg2QQbar[3S1(8)]g")) { sigmaPtr = new Sigma2gg2QQbarX8g(5, 0, 511); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:gg2QQbar[1S0(8)]g")) { sigmaPtr = new Sigma2gg2QQbarX8g(5, 1, 512); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:gg2QQbar[3PJ(8)]g")) { sigmaPtr = new Sigma2gg2QQbarX8g(5, 2, 513); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qg2QQbar[3S1(8)]q")) { sigmaPtr = new Sigma2qg2QQbarX8q(5, 0, 514); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qg2QQbar[1S0(8)]q")) { sigmaPtr = new Sigma2qg2QQbarX8q(5, 1, 515); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qg2QQbar[3PJ(8)]q")) { sigmaPtr = new Sigma2qg2QQbarX8q(5, 2, 516); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qqbar2QQbar[3S1(8)]g")) { sigmaPtr = new Sigma2qqbar2QQbarX8g(5, 0, 517); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qqbar2QQbar[1S0(8)]g")) { sigmaPtr = new Sigma2qqbar2QQbarX8g(5, 1, 518); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bottomoniums || settings.flag("Bottomonium:qqbar2QQbar[3PJ(8)]g")) { sigmaPtr = new Sigma2qqbar2QQbarX8g(5, 2, 519); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for top production bool tops = settings.flag("Top:all"); if (tops || settings.flag("Top:gg2ttbar")) { sigmaPtr = new Sigma2gg2QQbar(6, 601); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (tops || settings.flag("Top:qqbar2ttbar")) { sigmaPtr = new Sigma2qqbar2QQbar(6, 602); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (tops || settings.flag("Top:qq2tq(t:W)")) { sigmaPtr = new Sigma2qq2QqtW(6, 603); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (tops || settings.flag("Top:ffbar2ttbar(s:gmZ)")) { sigmaPtr = new Sigma2ffbar2FFbarsgmZ(6, 604); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (tops || settings.flag("Top:ffbar2tqbar(s:W)")) { sigmaPtr = new Sigma2ffbar2FfbarsW(6, 0, 605); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (tops || settings.flag("Top:gmgm2ttbar")) { sigmaPtr = new Sigma2gmgm2ffbar(6, 606); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for fourth-generation b' production bool bPrimes = settings.flag("FourthBottom:all"); if (bPrimes || settings.flag("FourthBottom:gg2bPrimebPrimebar")) { sigmaPtr = new Sigma2gg2QQbar(7, 801); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bPrimes || settings.flag("FourthBottom:qqbar2bPrimebPrimebar")) { sigmaPtr = new Sigma2qqbar2QQbar(7, 802); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bPrimes || settings.flag("FourthBottom:qq2bPrimeq(t:W)")) { sigmaPtr = new Sigma2qq2QqtW(7, 803); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bPrimes || settings.flag("FourthBottom:ffbar2bPrimebPrimebar(s:gmZ)")) { sigmaPtr = new Sigma2ffbar2FFbarsgmZ(7, 804); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bPrimes || settings.flag("FourthBottom:ffbar2bPrimeqbar(s:W)")) { sigmaPtr = new Sigma2ffbar2FfbarsW(7, 0, 805); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (bPrimes || settings.flag("FourthBottom:ffbar2bPrimetbar(s:W)")) { sigmaPtr = new Sigma2ffbar2FfbarsW(7, 6, 806); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for fourth-generation t' production bool tPrimes = settings.flag("FourthTop:all"); if (tPrimes || settings.flag("FourthTop:gg2tPrimetPrimebar")) { sigmaPtr = new Sigma2gg2QQbar(8, 821); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (tPrimes || settings.flag("FourthTop:qqbar2tPrimetPrimebar")) { sigmaPtr = new Sigma2qqbar2QQbar(8, 822); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (tPrimes || settings.flag("FourthTop:qq2tPrimeq(t:W)")) { sigmaPtr = new Sigma2qq2QqtW(8, 823); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (tPrimes || settings.flag("FourthTop:ffbar2tPrimetPrimebar(s:gmZ)")) { sigmaPtr = new Sigma2ffbar2FFbarsgmZ(8, 824); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (tPrimes || settings.flag("FourthTop:ffbar2tPrimeqbar(s:W)")) { sigmaPtr = new Sigma2ffbar2FfbarsW(8, 0, 825); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for two different fourth-generation fermions. if (bPrimes || tPrimes || settings.flag("FourthPair:ffbar2tPrimebPrimebar(s:W)")) { sigmaPtr = new Sigma2ffbar2FfbarsW(8, 7, 841); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("FourthPair:ffbar2tauPrimenuPrimebar(s:W)")) { sigmaPtr = new Sigma2ffbar2FfbarsW(17, 18, 842); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Flag for global choice between SM and BSM Higgses. bool useBSMHiggses = settings.flag("Higgs:useBSM"); // Set up requested objects for Standard-Model Higgs production. if (!useBSMHiggses) { bool HiggsesSM = settings.flag("HiggsSM:all"); if (HiggsesSM || settings.flag("HiggsSM:ffbar2H")) { sigmaPtr = new Sigma1ffbar2H(0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesSM || settings.flag("HiggsSM:gg2H")) { sigmaPtr = new Sigma1gg2H(0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesSM || settings.flag("HiggsSM:gmgm2H")) { sigmaPtr = new Sigma1gmgm2H(0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesSM || settings.flag("HiggsSM:ffbar2HZ")) { sigmaPtr = new Sigma2ffbar2HZ(0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesSM || settings.flag("HiggsSM:ffbar2HW")) { sigmaPtr = new Sigma2ffbar2HW(0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesSM || settings.flag("HiggsSM:ff2Hff(t:ZZ)")) { sigmaPtr = new Sigma3ff2HfftZZ(0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesSM || settings.flag("HiggsSM:ff2Hff(t:WW)")) { sigmaPtr = new Sigma3ff2HfftWW(0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesSM || settings.flag("HiggsSM:gg2Httbar")) { sigmaPtr = new Sigma3gg2HQQbar(6,0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesSM || settings.flag("HiggsSM:qqbar2Httbar")) { sigmaPtr = new Sigma3qqbar2HQQbar(6,0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Further Standard-Model Higgs processes, not included in "all". if (settings.flag("HiggsSM:qg2Hq")) { sigmaPtr = new Sigma2qg2Hq(4,0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2Hq(5,0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsSM:gg2Hbbbar")) { sigmaPtr = new Sigma3gg2HQQbar(5,0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsSM:qqbar2Hbbbar")) { sigmaPtr = new Sigma3qqbar2HQQbar(5,0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsSM:gg2Hg(l:t)")) { sigmaPtr = new Sigma2gg2Hglt(0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsSM:qg2Hq(l:t)")) { sigmaPtr = new Sigma2qg2Hqlt(0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsSM:qqbar2Hg(l:t)")) { sigmaPtr = new Sigma2qqbar2Hglt(0); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } // Common switch for the group of Higgs production BSM. if (useBSMHiggses) { bool HiggsesBSM = settings.flag("HiggsBSM:all"); // Set up requested objects for BSM H1 production. bool HiggsesH1 = settings.flag("HiggsBSM:allH1"); if (HiggsesBSM || HiggsesH1 || settings.flag("HiggsBSM:ffbar2H1")) { sigmaPtr = new Sigma1ffbar2H(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH1 || settings.flag("HiggsBSM:gg2H1")) { sigmaPtr = new Sigma1gg2H(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH1 || settings.flag("HiggsBSM:gmgm2H1")) { sigmaPtr = new Sigma1gmgm2H(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH1 || settings.flag("HiggsBSM:ffbar2H1Z")) { sigmaPtr = new Sigma2ffbar2HZ(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH1 || settings.flag("HiggsBSM:ffbar2H1W")) { sigmaPtr = new Sigma2ffbar2HW(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH1 || settings.flag("HiggsBSM:ff2H1ff(t:ZZ)")) { sigmaPtr = new Sigma3ff2HfftZZ(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH1 || settings.flag("HiggsBSM:ff2H1ff(t:WW)")) { sigmaPtr = new Sigma3ff2HfftWW(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH1 || settings.flag("HiggsBSM:gg2H1ttbar")) { sigmaPtr = new Sigma3gg2HQQbar(6,1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH1 || settings.flag("HiggsBSM:qqbar2H1ttbar")) { sigmaPtr = new Sigma3qqbar2HQQbar(6,1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Further BSM H1 processes, not included in "all". if (settings.flag("HiggsBSM:qg2H1q")) { sigmaPtr = new Sigma2qg2Hq(4,1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2Hq(5,1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:gg2H1bbbar")) { sigmaPtr = new Sigma3gg2HQQbar(5,1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:qqbar2H1bbbar")) { sigmaPtr = new Sigma3qqbar2HQQbar(5,1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:gg2H1g(l:t)")) { sigmaPtr = new Sigma2gg2Hglt(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:qg2H1q(l:t)")) { sigmaPtr = new Sigma2qg2Hqlt(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:qqbar2H1g(l:t)")) { sigmaPtr = new Sigma2qqbar2Hglt(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for BSM H2 production. bool HiggsesH2 = settings.flag("HiggsBSM:allH2"); if (HiggsesBSM || HiggsesH2 || settings.flag("HiggsBSM:ffbar2H2")) { sigmaPtr = new Sigma1ffbar2H(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH2 || settings.flag("HiggsBSM:gg2H2")) { sigmaPtr = new Sigma1gg2H(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH2 || settings.flag("HiggsBSM:gmgm2H2")) { sigmaPtr = new Sigma1gmgm2H(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH2 || settings.flag("HiggsBSM:ffbar2H2Z")) { sigmaPtr = new Sigma2ffbar2HZ(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH2 || settings.flag("HiggsBSM:ffbar2H2W")) { sigmaPtr = new Sigma2ffbar2HW(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH2 || settings.flag("HiggsBSM:ff2H2ff(t:ZZ)")) { sigmaPtr = new Sigma3ff2HfftZZ(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH2 || settings.flag("HiggsBSM:ff2H2ff(t:WW)")) { sigmaPtr = new Sigma3ff2HfftWW(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH2 || settings.flag("HiggsBSM:gg2H2ttbar")) { sigmaPtr = new Sigma3gg2HQQbar(6,2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesH2 || settings.flag("HiggsBSM:qqbar2H2ttbar")) { sigmaPtr = new Sigma3qqbar2HQQbar(6,2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Further BSM H2 processes, not included in "all". if (settings.flag("HiggsBSM:qg2H2q")) { sigmaPtr = new Sigma2qg2Hq(4,2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2Hq(5,2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:gg2H2bbbar")) { sigmaPtr = new Sigma3gg2HQQbar(5,2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:qqbar2H2bbbar")) { sigmaPtr = new Sigma3qqbar2HQQbar(5,2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:gg2H2g(l:t)")) { sigmaPtr = new Sigma2gg2Hglt(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:qg2H2q(l:t)")) { sigmaPtr = new Sigma2qg2Hqlt(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:qqbar2H2g(l:t)")) { sigmaPtr = new Sigma2qqbar2Hglt(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for BSM A3 production. bool HiggsesA3 = settings.flag("HiggsBSM:allA3"); if (HiggsesBSM || HiggsesA3 || settings.flag("HiggsBSM:ffbar2A3")) { sigmaPtr = new Sigma1ffbar2H(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesA3 || settings.flag("HiggsBSM:gg2A3")) { sigmaPtr = new Sigma1gg2H(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesA3 || settings.flag("HiggsBSM:gmgm2A3")) { sigmaPtr = new Sigma1gmgm2H(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesA3 || settings.flag("HiggsBSM:ffbar2A3Z")) { sigmaPtr = new Sigma2ffbar2HZ(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesA3 || settings.flag("HiggsBSM:ffbar2A3W")) { sigmaPtr = new Sigma2ffbar2HW(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesA3 || settings.flag("HiggsBSM:ff2A3ff(t:ZZ)")) { sigmaPtr = new Sigma3ff2HfftZZ(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesA3 || settings.flag("HiggsBSM:ff2A3ff(t:WW)")) { sigmaPtr = new Sigma3ff2HfftWW(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesA3 || settings.flag("HiggsBSM:gg2A3ttbar")) { sigmaPtr = new Sigma3gg2HQQbar(6,3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesA3 || settings.flag("HiggsBSM:qqbar2A3ttbar")) { sigmaPtr = new Sigma3qqbar2HQQbar(6,3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Further BSM A3 processes, not included in "all". if (settings.flag("HiggsBSM:qg2A3q")) { sigmaPtr = new Sigma2qg2Hq(4,3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2Hq(5,3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:gg2A3bbbar")) { sigmaPtr = new Sigma3gg2HQQbar(5,3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:qqbar2A3bbbar")) { sigmaPtr = new Sigma3qqbar2HQQbar(5,3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:gg2A3g(l:t)")) { sigmaPtr = new Sigma2gg2Hglt(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:qg2A3q(l:t)")) { sigmaPtr = new Sigma2qg2Hqlt(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("HiggsBSM:qqbar2A3g(l:t)")) { sigmaPtr = new Sigma2qqbar2Hglt(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for Charged Higgs production bool HiggsesChg = settings.flag("HiggsBSM:allH+-"); if (HiggsesBSM || HiggsesChg || settings.flag("HiggsBSM:ffbar2H+-")) { sigmaPtr = new Sigma1ffbar2Hchg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesChg || settings.flag("HiggsBSM:bg2H+-t")) { sigmaPtr = new Sigma2qg2Hchgq(6, 1062, "b g -> H+- t"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for Higgs pair-production bool HiggsesPairs = settings.flag("HiggsBSM:allHpair"); if (HiggsesBSM || HiggsesPairs || settings.flag("HiggsBSM:ffbar2A3H1")) { sigmaPtr = new Sigma2ffbar2A3H12(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesPairs || settings.flag("HiggsBSM:ffbar2A3H2")) { sigmaPtr = new Sigma2ffbar2A3H12(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesPairs || settings.flag("HiggsBSM:ffbar2H+-H1")) { sigmaPtr = new Sigma2ffbar2HchgH12(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesPairs || settings.flag("HiggsBSM:ffbar2H+-H2")) { sigmaPtr = new Sigma2ffbar2HchgH12(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (HiggsesBSM || HiggsesPairs || settings.flag("HiggsBSM:ffbar2H+H-")) { sigmaPtr = new Sigma2ffbar2HposHneg(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } // Set up requested objects for SUSY pair processes. if (couplings->isSUSY) { CoupSUSY* coupSUSY = (CoupSUSY *) couplings; bool SUSYs = settings.flag("SUSY:all"); bool nmssm = settings.flag("SLHA:NMSSM"); // Preselected SUSY codes. setupIdVecs( settings); // MSSM: 4 neutralinos int nNeut = 4; if (nmssm) nNeut = 5; // Gluino-gluino if (SUSYs || settings.flag("SUSY:gg2gluinogluino")) { // Skip if outgoing codes not asked for if (allowIdVals( 1000021, 1000021)) { sigmaPtr = new Sigma2gg2gluinogluino(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } if (SUSYs || settings.flag("SUSY:qqbar2gluinogluino")) { // Skip if outgoing codes not asked for if (allowIdVals( 1000021, 1000021)) { sigmaPtr = new Sigma2qqbar2gluinogluino(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } // Gluino-squark if (SUSYs || settings.flag("SUSY:qg2squarkgluino")) { int iproc = 1202; for (int idx = 1; idx <= 6; ++idx) { for (int iso = 1; iso <= 2; ++iso) { iproc++; int id3 = iso + ((idx <= 3) ? 1000000+2*(idx-1) : 2000000+2*(idx-4)); int id4 = 1000021; // Skip if outgoing codes not asked for if (!allowIdVals( id3, id4)) continue; sigmaPtr = new Sigma2qg2squarkgluino(id3,iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } // Squark-antisquark (gg initiated) if (SUSYs || settings.flag("SUSY:gg2squarkantisquark")) { int iproc = 1214; for (int idx = 1; idx <= 6; ++idx) { for (int iso = 1; iso <= 2; ++iso) { iproc++; int id = iso + ((idx <= 3) ? 1000000+2*(idx-1) : 2000000+2*(idx-4)); // Skip if outgoing codes not asked for if (!allowIdVals( id, id)) continue; sigmaPtr = new Sigma2gg2squarkantisquark(id,iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } // Squark-antisquark (qqbar initiated) if (SUSYs || settings.flag("SUSY:qqbar2squarkantisquark")) { int iproc = 1230; for (int idx = 1; idx <= 6; ++idx) { for (int iso = 1; iso <= 2; ++iso) { for (int jso = iso; jso >= 1; --jso) { for (int jdx = 1; jdx <= 6; ++jdx) { if (iso == jso && jdx < idx) continue; int id1 = iso + ((idx <= 3) ? 1000000+2*(idx-1) : 2000000+2*(idx-4)); int id2 = jso + ((jdx <= 3) ? 1000000+2*(jdx-1) : 2000000+2*(jdx-4)); // Update process number counter (for ~q~q, +2 if not self-conj) //if (iproc == 1302) iproc=1310; iproc++; if (iso == jso && id1 != id2) iproc++; // Skip if outgoing codes not asked for if (!allowIdVals( id1, id2)) continue; if (iso == jso && id1 != id2) { sigmaPtr = new Sigma2qqbar2squarkantisquark(id1,-id2,iproc-1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2squarkantisquark(id2,-id1,iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } else { sigmaPtr = new Sigma2qqbar2squarkantisquark(id1,-id2,iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } } } } // Squark-squark if (SUSYs || settings.flag("SUSY:qq2squarksquark")) { int iproc = 1350; for (int idx = 1; idx <= 6; ++idx) { for (int iso = 1; iso <= 2; ++iso) { for (int jso = iso; jso >= 1; jso--) { for (int jdx = 1; jdx <= 6; ++jdx) { if (iso == jso && jdx < idx) continue; iproc++; int id1 = iso + ((idx <= 3) ? 1000000+2*(idx-1) : 2000000+2*(idx-4)); int id2 = jso + ((jdx <= 3) ? 1000000+2*(jdx-1) : 2000000+2*(jdx-4)); // Skip if outgoing codes not asked for if (!allowIdVals( id1, id2)) continue; sigmaPtr = new Sigma2qq2squarksquark(id1,id2,iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } } } // Neutralino + squark if (SUSYs || settings.flag("SUSY:qg2chi0squark")) { int iproc = 1430; for (int iNeut= 1; iNeut <= nNeut; iNeut++) { for (int idx = 1; idx <= 6; idx++) { bool isUp = false; for (int iso = 1; iso <= 2; iso++) { if (iso == 2) isUp = true; iproc++; int id3 = coupSUSY->idNeut(iNeut); int id4 = iso + ((idx <= 3) ? 1000000+2*(idx-1) : 2000000+2*(idx-4)); // Skip if outgoing codes not asked for if (!allowIdVals( id3, id4)) continue; sigmaPtr = new Sigma2qg2chi0squark(iNeut,idx,isUp,iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } } // Chargino + squark if (SUSYs || settings.flag("SUSY:qg2chi+-squark")) { int iproc = 1490; for (int iChar = 1; iChar <= 2; iChar++) { for (int idx = 1; idx <= 6; idx++) { bool isUp = false; for (int iso = 1; iso <= 2; iso++) { if (iso == 2) isUp = true; iproc++; int id3 = coupSUSY->idChar(iChar); int id4 = iso + ((idx <= 3) ? 1000000+2*(idx-1) : 2000000+2*(idx-4)); // Skip if outgoing codes not asked for if (!allowIdVals( id3, id4)) continue; sigmaPtr = new Sigma2qg2charsquark(iChar,idx,isUp,iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } } // Neutralino pairs if (SUSYs || settings.flag("SUSY:qqbar2chi0chi0")) { int iproc = 1550; for (int iNeut2 = 1; iNeut2 <= nNeut; iNeut2++) { for (int iNeut1 = 1; iNeut1 <= iNeut2; iNeut1++) { iproc++; // Skip if outgoing codes not asked for if (!allowIdVals( coupSUSY->idNeut(iNeut1), coupSUSY->idNeut(iNeut2) ) ) continue; sigmaPtr = new Sigma2qqbar2chi0chi0(iNeut1, iNeut2,iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } // Neutralino-Chargino if (SUSYs || settings.flag("SUSY:qqbar2chi+-chi0")) { int iproc = 1570; for (int iNeut = 1; iNeut <= nNeut; iNeut++) { for (int iChar = 1; iChar <= 2; ++iChar) { iproc += 2; // Skip if outgoing codes not asked for if (!allowIdVals( coupSUSY->idNeut(iNeut), coupSUSY->idChar(iChar) ) ) continue; sigmaPtr = new Sigma2qqbar2charchi0( iChar, iNeut, iproc-1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2charchi0(-iChar, iNeut, iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } // Chargino-Chargino if (SUSYs || settings.flag("SUSY:qqbar2chi+chi-")) { int iproc = 1590; for (int i = 1; i <= 2; ++i) { for (int j = 1; j <= 2; ++j) { iproc++; // Skip if outgoing codes not asked for if (!allowIdVals( coupSUSY->idChar(i), coupSUSY->idChar(j) ) ) continue; sigmaPtr = new Sigma2qqbar2charchar( i,-j, iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } // RPV squark production if(SUSYs || settings.flag("SUSY:qq2antisquark")) { for (int idx = 1; idx <= 6; ++idx) { for (int iso = 1; iso <= 2; ++iso) { int id1 = iso + ((idx <= 3) ? 1000000+2*(idx-1) : 2000000+2*(idx-4)); // Skip if outgoing code not asked for if (!allowIdVals( id1, 0)) continue; sigmaPtr = new Sigma1qq2antisquark(id1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } // Neutralino-gluino if (SUSYs || settings.flag("SUSY:qqbar2chi0gluino")) { int iproc = 1600; for (int iNeut = 1; iNeut <= nNeut; iNeut++) { iproc++; // Skip if outgoing codes not asked for if (!allowIdVals( coupSUSY->idNeut(iNeut), 1000021)) continue; sigmaPtr = new Sigma2qqbar2chi0gluino(iNeut, iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } // Chargino-Gluino if (SUSYs || settings.flag("SUSY:qqbar2chi+-gluino")) { int iproc = 1620; for (int iChar = 1; iChar <= 2; ++iChar) { iproc ++; // Skip if outgoing codes not asked for if (!allowIdVals( coupSUSY->idChar(iChar), 1000021)) continue; sigmaPtr = new Sigma2qqbar2chargluino( iChar, iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } // Slepton-antislepton (qqbar initiated); Currently no RH sneutrinos if (SUSYs || settings.flag("SUSY:qqbar2sleptonantislepton")) { int iproc = 1650; for (int idx = 1; idx <= 6; ++idx) { for (int iso = 1; iso <= 2; ++iso) { for (int jso = iso; jso >= 1; --jso) { for (int jdx = 1; jdx <= 6; ++jdx) { if (iso == jso && jdx < idx) continue; int id1 = iso + ((idx <= 3) ? 1000010+2*(idx-1) : 2000010+2*(idx-4)); int id2 = jso + ((jdx <= 3) ? 1000010+2*(jdx-1) : 2000010+2*(jdx-4)); // Update process number counter iproc++; if (iso == jso && id1 != id2) iproc++; // Skip if outgoing codes not asked for if (!allowIdVals( id1, id2)) continue; if (iso == jso && id1 != id2) { sigmaPtr = new Sigma2qqbar2sleptonantislepton(id1,-id2,iproc-1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2sleptonantislepton(id2,-id1,iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } else { sigmaPtr = new Sigma2qqbar2sleptonantislepton(id1,-id2,iproc); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } } } } } } } // End of SUSY processes. // Set up requested objects for New-Gauge-Boson processes. if (settings.flag("NewGaugeBoson:ffbar2gmZZprime")) { sigmaPtr = new Sigma1ffbar2gmZZprime(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("NewGaugeBoson:ffbar2Wprime")) { sigmaPtr = new Sigma1ffbar2Wprime(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("NewGaugeBoson:ffbar2R0")) { sigmaPtr = new Sigma1ffbar2Rhorizontal(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for Left-Right-Symmetry processes. bool leftrights = settings.flag("LeftRightSymmmetry:all"); if (leftrights || settings.flag("LeftRightSymmmetry:ffbar2ZR")) { sigmaPtr = new Sigma1ffbar2ZRight(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:ffbar2WR")) { sigmaPtr = new Sigma1ffbar2WRight(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:ll2HL")) { sigmaPtr = new Sigma1ll2Hchgchg(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:lgm2HLe")) { sigmaPtr = new Sigma2lgm2Hchgchgl(1, 11); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:lgm2HLmu")) { sigmaPtr = new Sigma2lgm2Hchgchgl(1, 13); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:lgm2HLtau")) { sigmaPtr = new Sigma2lgm2Hchgchgl(1, 15); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:ff2HLff")) { sigmaPtr = new Sigma3ff2HchgchgfftWW(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:ffbar2HLHL")) { sigmaPtr = new Sigma2ffbar2HchgchgHchgchg(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:ll2HR")) { sigmaPtr = new Sigma1ll2Hchgchg(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:lgm2HRe")) { sigmaPtr = new Sigma2lgm2Hchgchgl(2, 11); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:lgm2HRmu")) { sigmaPtr = new Sigma2lgm2Hchgchgl(2, 13); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:lgm2HRtau")) { sigmaPtr = new Sigma2lgm2Hchgchgl(2, 15); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:ff2HRff")) { sigmaPtr = new Sigma3ff2HchgchgfftWW(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leftrights || settings.flag("LeftRightSymmmetry:ffbar2HRHR")) { sigmaPtr = new Sigma2ffbar2HchgchgHchgchg(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for leptoquark LQ processes. bool leptoquarks = settings.flag("LeptoQuark:all"); if (leptoquarks || settings.flag("LeptoQuark:ql2LQ")) { sigmaPtr = new Sigma1ql2LeptoQuark; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leptoquarks || settings.flag("LeptoQuark:qg2LQl")) { sigmaPtr = new Sigma2qg2LeptoQuarkl; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leptoquarks || settings.flag("LeptoQuark:gg2LQLQbar")) { sigmaPtr = new Sigma2gg2LQLQbar; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (leptoquarks || settings.flag("LeptoQuark:qqbar2LQLQbar")) { sigmaPtr = new Sigma2qqbar2LQLQbar; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for excited-fermion processes. bool excitedfermions = settings.flag("ExcitedFermion:all"); if (excitedfermions || settings.flag("ExcitedFermion:dg2dStar")) { sigmaPtr = new Sigma1qg2qStar(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:ug2uStar")) { sigmaPtr = new Sigma1qg2qStar(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:sg2sStar")) { sigmaPtr = new Sigma1qg2qStar(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:cg2cStar")) { sigmaPtr = new Sigma1qg2qStar(4); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:bg2bStar")) { sigmaPtr = new Sigma1qg2qStar(5); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:egm2eStar")) { sigmaPtr = new Sigma1lgm2lStar(11); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:mugm2muStar")) { sigmaPtr = new Sigma1lgm2lStar(13); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:taugm2tauStar")) { sigmaPtr = new Sigma1lgm2lStar(15); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qq2dStarq")) { sigmaPtr = new Sigma2qq2qStarq(1); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qq2uStarq")) { sigmaPtr = new Sigma2qq2qStarq(2); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qq2sStarq")) { sigmaPtr = new Sigma2qq2qStarq(3); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qq2cStarq")) { sigmaPtr = new Sigma2qq2qStarq(4); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qq2bStarq")) { sigmaPtr = new Sigma2qq2qStarq(5); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qqbar2eStare")) { sigmaPtr = new Sigma2qqbar2lStarlbar(11); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qqbar2nueStarnue")) { sigmaPtr = new Sigma2qqbar2lStarlbar(12); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qqbar2muStarmu")) { sigmaPtr = new Sigma2qqbar2lStarlbar(13); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qqbar2numuStarnumu")) { sigmaPtr = new Sigma2qqbar2lStarlbar(14); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qqbar2tauStartau")) { sigmaPtr = new Sigma2qqbar2lStarlbar(15); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (excitedfermions || settings.flag("ExcitedFermion:qqbar2nutauStarnutau")) { sigmaPtr = new Sigma2qqbar2lStarlbar(16); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for contact interaction processes. if (settings.flag("ContactInteractions:QCqq2qq")) { sigmaPtr = new Sigma2QCqq2qq(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ContactInteractions:QCqqbar2qqbar")) { sigmaPtr = new Sigma2QCqqbar2qqbar(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ContactInteractions:QCffbar2eebar")) { sigmaPtr = new Sigma2QCffbar2llbar(11, 4003); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ContactInteractions:QCffbar2mumubar")) { sigmaPtr = new Sigma2QCffbar2llbar(13, 4004); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ContactInteractions:QCffbar2tautaubar")) { sigmaPtr = new Sigma2QCffbar2llbar(15, 4005); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set spin of particles in the Hidden Valley scenario. int spinFv = settings.mode("HiddenValley:spinFv"); for (int i = 1; i < 7; ++i) { if (particleDataPtr->spinType( 4900000 + i) != spinFv + 1) particleDataPtr->spinType( 4900000 + i, spinFv + 1); if (particleDataPtr->spinType( 4900010 + i) != spinFv + 1) particleDataPtr->spinType( 4900010 + i, spinFv + 1); } if (spinFv != 1) { if (particleDataPtr->spinType( 4900101) != 2) particleDataPtr->spinType( 4900101, 2); } else { int spinqv = settings.mode("HiddenValley:spinqv"); if (particleDataPtr->spinType( 4900101) != 2 * spinqv + 1) particleDataPtr->spinType( 4900101, 2 * spinqv + 1); } // Set up requested objects for HiddenValley processes. bool hiddenvalleys = settings.flag("HiddenValley:all"); if (hiddenvalleys || settings.flag("HiddenValley:gg2DvDvbar")) { sigmaPtr = new Sigma2gg2qGqGbar( 4900001, 4901, spinFv, "g g -> Dv Dvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:gg2UvUvbar")) { sigmaPtr = new Sigma2gg2qGqGbar( 4900002, 4902, spinFv, "g g -> Uv Uvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:gg2SvSvbar")) { sigmaPtr = new Sigma2gg2qGqGbar( 4900003, 4903, spinFv, "g g -> Sv Svbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:gg2CvCvbar")) { sigmaPtr = new Sigma2gg2qGqGbar( 4900004, 4904, spinFv, "g g -> Cv Cvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:gg2BvBvbar")) { sigmaPtr = new Sigma2gg2qGqGbar( 4900005, 4905, spinFv, "g g -> Bv Bvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:gg2TvTvbar")) { sigmaPtr = new Sigma2gg2qGqGbar( 4900006, 4906, spinFv, "g g -> Tv Tvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:qqbar2DvDvbar")) { sigmaPtr = new Sigma2qqbar2qGqGbar( 4900001, 4911, spinFv, "q qbar -> Dv Dvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:qqbar2UvUvbar")) { sigmaPtr = new Sigma2qqbar2qGqGbar( 4900002, 4912, spinFv, "q qbar -> Uv Uvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:qqbar2SvSvbar")) { sigmaPtr = new Sigma2qqbar2qGqGbar( 4900003, 4913, spinFv, "q qbar -> Sv Svbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:qqbar2CvCvbar")) { sigmaPtr = new Sigma2qqbar2qGqGbar( 4900004, 4914, spinFv, "q qbar -> Cv Cvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:qqbar2BvBvbar")) { sigmaPtr = new Sigma2qqbar2qGqGbar( 4900005, 4915, spinFv, "q qbar -> Bv Bvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:qqbar2TvTvbar")) { sigmaPtr = new Sigma2qqbar2qGqGbar( 4900006, 4916, spinFv, "q qbar -> Tv Tvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2DvDvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900001, 4921, spinFv, "f fbar -> Dv Dvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2UvUvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900002, 4922, spinFv, "f fbar -> Uv Uvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2SvSvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900003, 4923, spinFv, "f fbar -> Sv Svbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2CvCvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900004, 4924, spinFv, "f fbar -> Cv Cvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2BvBvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900005, 4925, spinFv, "f fbar -> Bv Bvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2TvTvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900006, 4926, spinFv, "f fbar -> Tv Tvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2EvEvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900011, 4931, spinFv, "f fbar -> Ev Evbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2nuEvnuEvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900012, 4932, spinFv, "f fbar -> nuEv nuEvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2MUvMUvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900013, 4933, spinFv, "f fbar -> MUv MUvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2nuMUvnuMUvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900014, 4934, spinFv, "f fbar -> nuMUv nuMUvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2TAUvTAUvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900015, 4935, spinFv, "f fbar -> TAUv TAUvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2nuTAUvnuTAUvbar")) { sigmaPtr = new Sigma2ffbar2fGfGbar( 4900016, 4936, spinFv, "f fbar -> nuTAUv nuTAUvbar"); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (hiddenvalleys || settings.flag("HiddenValley:ffbar2Zv")) { sigmaPtr = new Sigma1ffbar2Zv(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for RS extra-dimensional G* processes. bool extraDimGstars = settings.flag("ExtraDimensionsG*:all"); if (extraDimGstars || settings.flag("ExtraDimensionsG*:gg2G*")) { sigmaPtr = new Sigma1gg2GravitonStar; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (extraDimGstars || settings.flag("ExtraDimensionsG*:ffbar2G*")) { sigmaPtr = new Sigma1ffbar2GravitonStar; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsG*:gg2G*g")) { sigmaPtr = new Sigma2gg2GravitonStarg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsG*:qg2G*q")) { sigmaPtr = new Sigma2qg2GravitonStarq; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsG*:qqbar2G*g")) { sigmaPtr = new Sigma2qqbar2GravitonStarg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for RS extra-dimensional KKgluon processes. if (settings.flag("ExtraDimensionsG*:qqbar2KKgluon*")) { sigmaPtr = new Sigma1qqbar2KKgluonStar; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // NOAM: Set up requested objects for TEV extra-dimensional processes. if (settings.flag("ExtraDimensionsTEV:ffbar2ddbar")) { sigmaPtr = new Sigma2ffbar2TEVffbar(1, 5061); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2uubar")) { sigmaPtr = new Sigma2ffbar2TEVffbar(2, 5062); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2ssbar")) { sigmaPtr = new Sigma2ffbar2TEVffbar(3, 5063); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2ccbar")) { sigmaPtr = new Sigma2ffbar2TEVffbar(4, 5064); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2bbbar")) { sigmaPtr = new Sigma2ffbar2TEVffbar(5, 5065); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2ttbar")) { sigmaPtr = new Sigma2ffbar2TEVffbar(6, 5066); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2e+e-")) { sigmaPtr = new Sigma2ffbar2TEVffbar(11, 5071); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2nuenuebar")) { sigmaPtr = new Sigma2ffbar2TEVffbar(12, 5072); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2mu+mu-")) { sigmaPtr = new Sigma2ffbar2TEVffbar(13, 5073); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2numunumubar")) { sigmaPtr = new Sigma2ffbar2TEVffbar(14, 5074); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2tau+tau-")) { sigmaPtr = new Sigma2ffbar2TEVffbar(15, 5075); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsTEV:ffbar2nutaunutaubar")) { sigmaPtr = new Sigma2ffbar2TEVffbar(16, 5076); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for large extra-dimensional G processes. bool extraDimLEDmono = settings.flag("ExtraDimensionsLED:monojet"); if (extraDimLEDmono || settings.flag("ExtraDimensionsLED:gg2Gg")) { sigmaPtr = new Sigma2gg2LEDUnparticleg( true ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (extraDimLEDmono || settings.flag("ExtraDimensionsLED:qg2Gq")) { sigmaPtr = new Sigma2qg2LEDUnparticleq( true ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (extraDimLEDmono || settings.flag("ExtraDimensionsLED:qqbar2Gg")) { sigmaPtr = new Sigma2qqbar2LEDUnparticleg( true ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsLED:ffbar2GZ")) { sigmaPtr = new Sigma2ffbar2LEDUnparticleZ( true ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsLED:ffbar2Ggamma")) { sigmaPtr = new Sigma2ffbar2LEDUnparticlegamma( true ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsLED:ffbar2gammagamma")) { sigmaPtr = new Sigma2ffbar2LEDgammagamma( true ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsLED:gg2gammagamma")) { sigmaPtr = new Sigma2gg2LEDgammagamma( true ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsLED:ffbar2llbar")) { sigmaPtr = new Sigma2ffbar2LEDllbar( true ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsLED:gg2llbar")) { sigmaPtr = new Sigma2gg2LEDllbar( true ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } bool extraDimLEDdij = settings.flag("ExtraDimensionsLED:dijets"); if (extraDimLEDdij || settings.flag("ExtraDimensionsLED:gg2DJgg")) { sigmaPtr = new Sigma2gg2LEDgg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (extraDimLEDdij || settings.flag("ExtraDimensionsLED:gg2DJqqbar")) { sigmaPtr = new Sigma2gg2LEDqqbar; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (extraDimLEDdij || settings.flag("ExtraDimensionsLED:qg2DJqg")) { sigmaPtr = new Sigma2qg2LEDqg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (extraDimLEDdij || settings.flag("ExtraDimensionsLED:qq2DJqq")) { sigmaPtr = new Sigma2qq2LEDqq; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (extraDimLEDdij || settings.flag("ExtraDimensionsLED:qqbar2DJgg")) { sigmaPtr = new Sigma2qqbar2LEDgg; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (extraDimLEDdij || settings.flag("ExtraDimensionsLED:qqbar2DJqqbarNew")) { sigmaPtr = new Sigma2qqbar2LEDqqbarNew; containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Set up requested objects for unparticle processes. bool extraDimUnpartmono = settings.flag("ExtraDimensionsUnpart:monojet"); if (extraDimUnpartmono || settings.flag("ExtraDimensionsUnpart:gg2Ug")) { sigmaPtr = new Sigma2gg2LEDUnparticleg( false ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (extraDimUnpartmono || settings.flag("ExtraDimensionsUnpart:qg2Uq")) { sigmaPtr = new Sigma2qg2LEDUnparticleq( false ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (extraDimUnpartmono || settings.flag("ExtraDimensionsUnpart:qqbar2Ug")) { sigmaPtr = new Sigma2qqbar2LEDUnparticleg( false ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsUnpart:ffbar2UZ")) { sigmaPtr = new Sigma2ffbar2LEDUnparticleZ( false ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsUnpart:ffbar2Ugamma")) { sigmaPtr = new Sigma2ffbar2LEDUnparticlegamma( false ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsUnpart:ffbar2gammagamma")) { sigmaPtr = new Sigma2ffbar2LEDgammagamma( false ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsUnpart:gg2gammagamma")) { sigmaPtr = new Sigma2gg2LEDgammagamma( false ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsUnpart:ffbar2llbar")) { sigmaPtr = new Sigma2ffbar2LEDllbar( false ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } if (settings.flag("ExtraDimensionsUnpart:gg2llbar")) { sigmaPtr = new Sigma2gg2LEDllbar( false ); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); } // Done. return true; } //-------------------------------------------------------------------------- // Routine to initialize list of second hard processes. bool SetupContainers::init2(vector& container2Ptrs, Settings& settings) { // Reset process list, if filled in previous subrun. if (container2Ptrs.size() > 0) { for (int i = 0; i < int(container2Ptrs.size()); ++i) delete container2Ptrs[i]; container2Ptrs.clear(); } SigmaProcess* sigmaPtr; // Two hard QCD jets. if (settings.flag("SecondHard:TwoJets")) { sigmaPtr = new Sigma2gg2gg; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2qqbar; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2qg; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qq2qq; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2gg; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2qqbarNew; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbar(4, 121); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbar(4, 122); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbar(5, 123); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbar(5, 124); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // A prompt photon and a hard jet. if (settings.flag("SecondHard:PhotonAndJet")) { sigmaPtr = new Sigma2qg2qgamma; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2ggamma; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2ggamma; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // Two prompt photons. if (settings.flag("SecondHard:TwoPhotons")) { sigmaPtr = new Sigma2ffbar2gammagamma; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2gammagamma; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // Charmonium production. if (settings.flag("SecondHard:Charmonium")) { sigmaPtr = new Sigma2gg2QQbar3S11g(4, 401); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbar3PJ1g(4, 0, 402); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbar3PJ1g(4, 1, 403); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbar3PJ1g(4, 2, 404); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbar3PJ1q(4, 0, 405); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbar3PJ1q(4, 1, 406); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbar3PJ1q(4, 2, 407); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(4, 0, 408); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(4, 1, 409); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(4, 2, 410); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbarX8g(4, 0, 411); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbarX8g(4, 1, 412); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbarX8g(4, 2, 413); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbarX8q(4, 0, 414); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbarX8q(4, 1, 415); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbarX8q(4, 2, 416); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbarX8g(4, 0, 417); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbarX8g(4, 1, 418); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbarX8g(4, 2, 419); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // Bottomonium production. if (settings.flag("SecondHard:Bottomonium")) { sigmaPtr = new Sigma2gg2QQbar3S11g(5, 501); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbar3PJ1g(5, 0, 502); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbar3PJ1g(5, 1, 503); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbar3PJ1g(5, 2, 504); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbar3PJ1q(5, 0, 505); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbar3PJ1q(5, 1, 506); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbar3PJ1q(5, 2, 507); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(5, 0, 508); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(5, 1, 509); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbar3PJ1g(5, 2, 510); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbarX8g(5, 0, 511); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbarX8g(5, 1, 512); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2gg2QQbarX8g(5, 2, 513); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbarX8q(5, 0, 514); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbarX8q(5, 1, 515); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2QQbarX8q(5, 2, 516); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbarX8g(5, 0, 517); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbarX8g(5, 1, 518); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbarX8g(5, 2, 519); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // A single gamma*/Z0. if (settings.flag("SecondHard:SingleGmZ")) { sigmaPtr = new Sigma1ffbar2gmZ; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // A single W+-. if (settings.flag("SecondHard:SingleW")) { sigmaPtr = new Sigma1ffbar2W; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // A gamma*/Z0 and a hard jet. if (settings.flag("SecondHard:GmZAndJet")) { sigmaPtr = new Sigma2qqbar2gmZg; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2gmZq; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // A W+- and a hard jet. if (settings.flag("SecondHard:WAndJet")) { sigmaPtr = new Sigma2qqbar2Wg; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qg2Wq; container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // Top pair production. if (settings.flag("SecondHard:TopPair")) { sigmaPtr = new Sigma2gg2QQbar(6, 601); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbar(6, 602); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2ffbar2FFbarsgmZ(6, 604); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // Single top production. if (settings.flag("SecondHard:SingleTop")) { sigmaPtr = new Sigma2qq2QqtW(6, 603); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2ffbar2FfbarsW(6, 0, 605); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // Two b jets - already part of TwoJets sample above. if (settings.flag("SecondHard:TwoBJets")) { sigmaPtr = new Sigma2gg2QQbar(5, 123); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); sigmaPtr = new Sigma2qqbar2QQbar(5, 124); container2Ptrs.push_back( new ProcessContainer(sigmaPtr) ); } // Done. return true; } //-------------------------------------------------------------------------- // Set up arrays of allowed outgoing SUSY particles. void SetupContainers::setupIdVecs( Settings& settings) { // First array either none, one or many particles. idVecA.resize(0); if (settings.mode("SUSY:idA") != 0) { idVecA.push_back( abs(settings.mode("SUSY:idA")) ); } else { vector idTmpA = settings.mvec("SUSY:idVecA"); for (int i = 0; i < int(idTmpA.size()); ++i) if (idTmpA[i] != 0) idVecA.push_back( abs(idTmpA[i]) ); } nVecA = idVecA.size(); // Second array either none, one or many particles. idVecB.resize(0); if (settings.mode("SUSY:idB") != 0) { idVecB.push_back( abs(settings.mode("SUSY:idB")) ); } else { vector idTmpB = settings.mvec("SUSY:idVecB"); for (int i = 0; i < int(idTmpB.size()); ++i) if (idTmpB[i] != 0) idVecB.push_back( abs(idTmpB[i]) ); } nVecB = idVecB.size(); } //-------------------------------------------------------------------------- // Check final state for allowed outgoing SUSY particles. // Normally check two codes, but allow for only one. bool SetupContainers::allowIdVals( int idCheck1, int idCheck2) { // If empty arrays or id's no need for checks. Else need absolute values. if (nVecA == 0 && nVecB == 0) return true; if (idCheck1 == 0 && idCheck2 == 0) return true; int idChk1 = abs(idCheck1); int idChk2 = abs(idCheck2); // If only one outgoing particle then check idVecA and idVecB. if (idChk1 == 0) swap(idChk1, idChk2); if (idChk2 == 0) { for (int i = 0; i < nVecA; ++i) if (idChk1 == idVecA[i]) return true; for (int i = 0; i < nVecB; ++i) if (idChk1 == idVecB[i]) return true; return false; } // If empty array idVecB then compare with idVecA. if (nVecB == 0) { for (int i = 0; i < nVecA; ++i) if (idChk1 == idVecA[i] || idChk2 == idVecA[i]) return true; return false; } // If empty array idVecA then compare with idVecB. if (nVecA == 0) { for (int i = 0; i < nVecB; ++i) if (idChk1 == idVecB[i] || idChk2 == idVecB[i]) return true; return false; } // Else check that pair matches allowed combinations. for (int i = 0; i < nVecA; ++i) for (int j = 0; j < nVecB; ++j) if ( (idChk1 == idVecA[i] && idChk2 == idVecB[j]) || (idChk2 == idVecA[i] && idChk1 == idVecB[j]) ) return true; return false; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SusyResonanceWidths.cc0000644000175000017500000012304012217346252017417 0ustar sunsun// SusyResonanceWidths.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand // Authors: N. Desai, P. Skands // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // SUSY Resonance widths classes. #include "Pythia8/SusyResonanceWidths.h" #include "Pythia8/SusyCouplings.h" #include "Pythia8/ParticleData.h" #include "Pythia8/PythiaComplex.h" namespace Pythia8 { //========================================================================== // WidthFunctions Class // Contains functions to be integrated for calculating the 3-body // decay widths //-------------------------------------------------------------------------- void WidthFunction::init( ParticleData* particleDataPtrIn, CoupSUSY* coupSUSYPtrIn) { particleDataPtr = particleDataPtrIn; coupSUSYPtr = coupSUSYPtrIn; } //-------------------------------------------------------------------------- void WidthFunction::setInternal2(int idResIn, int id1In, int id2In, int id3In, int idIntIn) { // Res -> 1,2,3 idRes = idResIn; id1 = id1In; id2 = id2In; id3 = id3In; idInt = idIntIn; mRes = particleDataPtr->m0(idRes); m1 = particleDataPtr->m0(id1); m2 = particleDataPtr->m0(id2); m3 = particleDataPtr->m0(id3); // Internal propagator mInt = particleDataPtr->m0(idInt); gammaInt = particleDataPtr->mWidth(idInt); return; } //-------------------------------------------------------------------------- double WidthFunction::function(double) { cout<<"Warning using dummy width function"<m0(idInt); gammaInt = particleDataPtr->mWidth(idInt); iX = coupSUSYPtr->typeNeut(idRes); iQ = (id3+1)/2; iSq = (idInt>1000000)? 3 + (idInt%10+1)/2 : (idInt%10+1)/2; isSqDown = (idInt % 2 == 1)? true : false; m1 = particleDataPtr->m0(id1); m2 = particleDataPtr->m0(id2); m3 = particleDataPtr->m0(id3); return; } //-------------------------------------------------------------------------- void Upsilon::setInternal (int idResIn, int id1In, int id2In, int id3In, int idIntIn, int idInt2In) { setInternal2(idResIn, id1In, id2In, id3In, idIntIn); idInt2 = idInt2In; mInt = particleDataPtr->m0(idInt); gammaInt = particleDataPtr->mWidth(idInt); mInt2 = particleDataPtr->m0(idInt2); gammaInt2 = particleDataPtr->mWidth(idInt2); iX = coupSUSYPtr->typeNeut(idRes); iQ = (id3+1)/2; iSq = (idInt>1000000)? 3 + (idInt%10+1)/2 : (idInt%10+1)/2; iSq2 = (idInt2>1000000)? 3 + (idInt2%10+1)/2 : (idInt2%10+1)/2; isSqDown = (idIntIn % 2 == 1)? true : false; m1 = particleDataPtr->m0(id1); m2 = particleDataPtr->m0(id2); m3 = particleDataPtr->m0(id3); return; } //-------------------------------------------------------------------------- void Phi::setInternal (int idResIn, int id1In, int id2In, int id3In, int idIntIn, int idInt2In) { setInternal2(idResIn, id1In, id2In, id3In, idIntIn); idInt2 = idInt2In; mInt = particleDataPtr->m0(idInt); gammaInt = particleDataPtr->mWidth(idInt); mInt2 = particleDataPtr->m0(idInt2); gammaInt2 = particleDataPtr->mWidth(idInt2); iX = coupSUSYPtr->typeNeut(idRes); iQ = (id3+1)/2; iSq = (idInt>1000000)? 3 + (idInt%10+1)/2 : (idInt%10+1)/2; iSq2 = (idInt2>1000000)? 3 + (idInt2%10+1)/2 : (idInt2%10+1)/2; isSqDown = (idIntIn % 2 == 1)? true : false; m1 = particleDataPtr->m0(id1); m2 = particleDataPtr->m0(id2); m3 = particleDataPtr->m0(id3); return; } //-------------------------------------------------------------------------- double Psi::function(double m12sq) { double R, factor1, factor2, value; // Check that the propagators are offshell if (m12sq > pow2(mInt) || abs(m12sq - pow2(mInt)) < gammaInt) return 0; R = 1.0/(pow2(m12sq-pow2(mInt)) + pow2(gammaInt*mInt)); if (isSqDown){ factor1 = (norm(coupSUSYPtr->LsddX[iSq][iQ][iX]) + norm(coupSUSYPtr->RsddX[iSq][iQ][iX]))* (mRes*mRes + m3*m3 - m12sq); factor2 = 4.0 * real(coupSUSYPtr->LsddX[iSq][iQ][iX] * conj(coupSUSYPtr->RsddX[iSq][iQ][iX])) * m3 * mRes; } else { factor1 = (norm(coupSUSYPtr->LsuuX[iSq][iQ][iX]) + norm(coupSUSYPtr->RsuuX[iSq][iQ][iX]))* (mRes*mRes + m3*m3 - m12sq); factor2 = 4.0 * real(coupSUSYPtr->LsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->RsuuX[iSq][iQ][iX])) * m3 * mRes; } value = R * (m12sq - m1*m1 - m2*m2) * (factor1+factor2); return value; } //-------------------------------------------------------------------------- double Upsilon::function(double m12sq) { double R1,R2, S, factor1, factor2, value; // Check that the propagators are offshell if (m12sq > pow2(mInt) || abs(m12sq - pow2(mInt)) < gammaInt) return 0; if (m12sq > pow2(mInt2) || abs(m12sq - pow2(mInt2)) < gammaInt2) return 0; R1 = 1.0/(pow2(m12sq-pow2(mInt)) + pow2(gammaInt*mInt)); R2 = 1.0/(pow2(m12sq-pow2(mInt2)) + pow2(gammaInt2*mInt2)); S = R1 * R2 * ((m12sq - pow2(mInt)) * (m12sq - pow2(mInt2)) + gammaInt * mInt * gammaInt2 * mInt2); if (isSqDown){ factor1 = real(coupSUSYPtr->LsddX[iSq][iQ][iX] * conj(coupSUSYPtr->LsddX[iSq2][iQ][iX])) + real(coupSUSYPtr->RsddX[iSq][iQ][iX] * conj(coupSUSYPtr->RsddX[iSq2][iQ][iX])); factor2 = real(coupSUSYPtr->LsddX[iSq][iQ][iX] * conj(coupSUSYPtr->RsddX[iSq2][iQ][iX])) + real(coupSUSYPtr->RsddX[iSq][iQ][iX] * conj(coupSUSYPtr->LsddX[iSq2][iQ][iX])); }else{ factor1 = real(coupSUSYPtr->LsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->LsuuX[iSq2][iQ][iX])) + real(coupSUSYPtr->RsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->RsuuX[iSq2][iQ][iX])); factor2 = real(coupSUSYPtr->LsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->RsuuX[iSq2][iQ][iX])) + real(coupSUSYPtr->RsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->LsuuX[iSq2][iQ][iX])); } value = S * (m12sq - pow2(m1) - pow2(m2)) * ( factor1 * (pow2(mRes) + pow2(m3) - m12sq) + 2.0 * factor2 * m3 * mRes); // cout<<"I1: "< pow2(mInt) || abs(m12sq - pow2(mInt)) < gammaInt) return 0; double m23max, m23min, E2, E3; E2 = (m12sq - pow2(m1) - pow2(m2))/(2.0 * sqrt(m12sq)); E3 = (pow2(mRes) - m12sq - pow2(m3))/(2.0 * sqrt(m12sq)); m23max = pow2(E2+E3) - (sqrt(E2*E2 - m2*m2) - sqrt(E3*E3 - m3*m3)) ; m23min = pow2(E2+E3) - (sqrt(E2*E2 - m2*m2) + sqrt(E3*E3 - m3*m3)) ; if (E2 < m2 || E3 < m3){ cout <<"Error in Phi:function"< pow2(mInt2) || abs(m23sq - pow2(mInt2)) < gammaInt2) return 0; double R1, R2, S, factor1, factor2, factor3, factor4, value, fac; int iQ2; R1 = 1.0/(pow2(m12sq-pow2(mInt)) + pow2(gammaInt*mInt)); R2 = 1.0/(pow2(m12sq-pow2(mInt2)) + pow2(gammaInt2*mInt2)); S = R1 * R2 * ((m12sq - pow2(mInt)) * (m12sq - pow2(mInt2)) + gammaInt * mInt * gammaInt2 * mInt2); fac = 1.0; if (isSqDown){ // Only factor is when both d_i and d_j are near. iQ2 = (id1%2 == 1)? (id1+1)/2 : (id2+1)/2; if (mRes > mInt2 + particleDataPtr->m0(iQ2)) fac = 0.; factor1 = m1 * m3 * real(coupSUSYPtr->LsddX[iSq][iQ][iX] * conj(coupSUSYPtr->LsddX[iSq2][iQ2][iX])) * (m12sq + m23sq - pow2(m1) - pow2(m3)); factor2 = m1 * mRes * real(coupSUSYPtr->RsddX[iSq][iQ][iX] * conj(coupSUSYPtr->LsddX[iSq2][iQ2][iX])) * (m23sq - pow2(m2) - pow2(m3)); factor3 = m3 * mRes * real(coupSUSYPtr->LsddX[iSq][iQ][iX] * conj(coupSUSYPtr->RsddX[iSq2][iQ2][iX])) * (m12sq - pow2(m1) - pow2(m2)); factor4 = m3 * mRes * real(coupSUSYPtr->RsddX[iSq][iQ][iX] * conj(coupSUSYPtr->RsddX[iSq2][iQ2][iX])) * (m12sq * m23sq - pow2(m1 * m3) - pow2(m2 * mRes)); }else{ // Factor A: u and d_1 iQ2 = (id1+1)/2; if (mRes > mInt2 + particleDataPtr->m0(iQ2)) fac = 0.; factor1 = m1 * m3 * real(coupSUSYPtr->LsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->LsddX[iSq2][iQ2][iX])) * (m12sq + m23sq - pow2(m1) - pow2(m3)); factor2 = m1 * mRes * real(coupSUSYPtr->RsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->LsddX[iSq2][iQ2][iX])) * (m23sq - pow2(m2) - pow2(m3)); factor3 = m3 * mRes * real(coupSUSYPtr->LsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->RsddX[iSq2][iQ2][iX])) * (m12sq - pow2(m1) - pow2(m2)); factor4 = m3 * mRes * real(coupSUSYPtr->RsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->RsddX[iSq2][iQ2][iX])) * (m12sq * m23sq - pow2(m1 * m3) - pow2(m2 * mRes)); // Factor B: u and d_2; change 1 <=> 2 iQ2 = (id2+1)/2; if (mRes > mInt2 + particleDataPtr->m0(iQ2)) fac = 0.; factor1 += m2 * m3 * real(coupSUSYPtr->LsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->LsddX[iSq2][iQ2][iX])) * (m12sq + m23sq - pow2(m2) - pow2(m3)); factor2 += m2 * mRes * real(coupSUSYPtr->RsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->LsddX[iSq2][iQ2][iX])) * (m23sq - pow2(m1) - pow2(m3)); factor3 += m3 * mRes * real(coupSUSYPtr->LsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->RsddX[iSq2][iQ2][iX])) * (m12sq - pow2(m2) - pow2(m1)); factor4 += m3 * mRes * real(coupSUSYPtr->RsuuX[iSq][iQ][iX] * conj(coupSUSYPtr->RsddX[iSq2][iQ2][iX])) * (m12sq * m23sq - pow2(m2 * m3) - pow2(m1 * mRes)); } value = S * (factor1 + factor2 + factor3 + factor4); // cout<<"I1: "< xhi ) { cerr<<" (integrateGauss:) -> xhi < xlo"<isSUSY) { coupSUSYPtr = (CoupSUSY *) couplingsPtr; return true; } return false; } //-------------------------------------------------------------------------- bool SUSYResonanceWidths::allowCalc(){ // Check if decay calculations at all possible if ( !couplingsPtr->isSUSY ) return false; // Next check if SLHA decay tables are ignored (= always do calculation) if ( !settingsPtr->flag("SLHA:useDecayTable") ) return true; // Next check if decay table was read in via SLHA and takes precedence for ( int iDec = 1; iDec < int((coupSUSYPtr->slhaPtr)->decays.size()); ++iDec) if ( (coupSUSYPtr->slhaPtr)->decays[iDec].getId() == abs(idRes) ) { if (DBSUSY) cout<<"Using external decay table for:"<alphaS(mHat * mHat ); alpEM = coupSUSYPtr->alphaEM(mHat * mHat); s2W = coupSUSYPtr->sin2W; } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceSquark::calcPreFac(bool) { // Common coupling factors. preFac = 1.0 / (s2W * pow(mHat,3)); } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceSquark::calcWidth(bool) { // Squark type -- in u_i/d_i and generation int ksusy = 1000000; bool idown = (abs(idRes)%2 == 0 ? false : true); int isq = (abs(idRes)/ksusy == 2) ? (abs(idRes)%10+1)/2 + 3: (abs(idRes)%10+1)/2; // int isqgen = (abs(idRes)%10 + 1)/2; // Check that mass is above threshold. if (ps == 0.) return; else{ // Two-body decays kinFac = (mHat * mHat - mf1 * mf1 - mf2 * mf2); double fac = 0.0 , wid = 0.0; //RPV decays //Case 1a: UDD-type if (id1Abs < 7 && id2Abs < 7){ // Quark generations int iq1 = (id1Abs + 1)/2; int iq2 = (id2Abs + 1)/2; // Check for RPV UDD couplings if (!coupSUSYPtr->isUDD) {widNow = 0; return;} // ~q -> q_i + q_j fac = 2.0 * kinFac / (16.0 * M_PI * pow(mHat,3)); wid = 0.0; if (idown) { if ((id1Abs+id2Abs)%2 == 1){ if (id1Abs%2==1) for (int isq2 = 1; isq2 < 4; isq2++) wid += norm(coupSUSYPtr->rvUDD[iq2][iq1][isq2] * coupSUSYPtr->Rdsq[isq][isq2+3]); else for (int isq2 = 1; isq2 < 4; isq2++) wid += norm(coupSUSYPtr->rvUDD[iq1][iq2][isq2] * coupSUSYPtr->Rdsq[isq][isq2+3]); } } else { if ((id1Abs+id2Abs)%2 != 0) widNow = 0.0; else for (int isq2 = 1; isq2 < 4; isq2++) wid += norm(coupSUSYPtr->rvUDD[isq2][iq1][iq2] * coupSUSYPtr->Rusq[isq][isq2+3]); } } //Case 1b: LQD-type else if (id1Abs < 17 && id2Abs < 7){ if (!coupSUSYPtr->isLQD) {widNow = 0; return;} int ilep = (id1Abs - 9)/2; int iq = (id2Abs + 1)/2; fac = kinFac / (16.0 * M_PI * pow(mHat,3)); wid = 0.0; if (idown){ if (iq%2 == 0){ // q is up-type; ~q is right-handed down type for (int isq2=1; isq2<3; isq2++) wid += norm(coupSUSYPtr->Rdsq[isq][isq2+3] * coupSUSYPtr->rvLQD[ilep][iq][isq2]); }else{ //q is down type; ~q left-handed down-type for (int isq2=1; isq2<3; isq2++) wid += norm(coupSUSYPtr->Rdsq[isq][isq2] * coupSUSYPtr->rvLQD[ilep][isq2][isq2]); } } else{ if (iq%2 == 0) {widNow = 0.0; return;} // q is down type; ~q is left-handed up-type for (int isq2=1; isq2<3; isq2++) wid += norm(coupSUSYPtr->Rusq[isq][isq2] * coupSUSYPtr->rvLQD[ilep][isq2][iq]); } } //Case 2: quark + gaugino else if (id1Abs > ksusy && id2Abs < 7) { int iq = (id2Abs + 1)/2; // ~q -> ~g + q if (id1Abs == 1000021 && idRes%10 == id2Abs) { // Removed factor of s2W in denominator: strong process -- no EW fac = 2.0 * alpS / (3.0 * pow3(mHat)); if (idown) wid = kinFac * (norm(coupSUSYPtr->LsddG[isq][iq]) + norm(coupSUSYPtr->RsddG[isq][iq])) - 4.0 * mHat * mf2 * real(coupSUSYPtr->LsddG[isq][iq] * conj(coupSUSYPtr->RsddG[isq][iq])); else wid = kinFac * (norm(coupSUSYPtr->LsuuG[isq][iq]) + norm(coupSUSYPtr->RsuuG[isq][iq])) - 4.0 * mHat * mf2 * real(coupSUSYPtr->LsuuG[isq][iq] * conj(coupSUSYPtr->RsuuG[isq][iq])); } else for (int i=1; i<6 ; i++){ // ~q -> ~chi0 + q if (coupSUSYPtr->idNeut(i)==id1Abs && idRes%2 == id2Abs%2){ fac = alpEM * preFac / (2.0 * (1 - s2W)); if (idown) wid = kinFac * (norm(coupSUSYPtr->LsddX[isq][iq][i]) + norm(coupSUSYPtr->RsddX[isq][iq][i])) - 4.0 * mHat * mf2 * real(coupSUSYPtr->LsddX[isq][iq][i] * conj(coupSUSYPtr->RsddX[isq][iq][i])); else wid = kinFac * (norm(coupSUSYPtr->LsuuX[isq][iq][i]) + norm(coupSUSYPtr->RsuuX[isq][iq][i])) - 4.0 * mHat * mf2 * real(coupSUSYPtr->LsuuX[isq][iq][i] * conj(coupSUSYPtr->RsuuX[isq][iq][i])); } // ~q -> chi- + q else if (i < 3 && coupSUSYPtr->idChar(i)==id1Abs && idRes%2 != id2Abs%2){ fac = alpEM * preFac / (4.0 * (1 - s2W)); if (idown) wid = kinFac * (norm(coupSUSYPtr->LsduX[isq][iq][i]) + norm(coupSUSYPtr->RsduX[isq][iq][i])) - 4.0 * mHat * mf2 * real(coupSUSYPtr->LsduX[isq][iq][i] * conj(coupSUSYPtr->RsduX[isq][iq][i])); else wid = kinFac * (norm(coupSUSYPtr->LsudX[isq][iq][i]) + norm(coupSUSYPtr->RsudX[isq][iq][i])) - 4.0 * mHat * mf2 * real(coupSUSYPtr->LsudX[isq][iq][i] * conj(coupSUSYPtr->RsudX[isq][iq][i])); } } } //Case 3: ~q_i -> ~q_j + Z/W else if (id1Abs > ksusy && id1Abs%100 < 7 && (id2Abs == 23 || id2Abs == 24)){ // factor of lambda^(3/2) = ps^(3/2) ; fac = alpEM * preFac/(16.0 * pow2(particleDataPtr->m0(id2Abs)) * (1.0 - s2W)) * pow2(ps) ; int isq2 = (id1Abs/ksusy == 2) ? (id1Abs%10+1)/2 + 3: (id1Abs%10+1)/2; if (id2Abs == 23 && id1Abs%2 == idRes%2){ if (idown) wid = norm(coupSUSYPtr->LsdsdZ[isq][isq2] + coupSUSYPtr->RsdsdZ[isq][isq2]); else wid = norm(coupSUSYPtr->LsusuZ[isq][isq2] + coupSUSYPtr->RsusuZ[isq][isq2]); } else if (id2Abs == 24 && id1Abs%2 != idRes%2){ if (idown) wid = norm(coupSUSYPtr->LsusdW[isq2][isq]); else wid = norm(coupSUSYPtr->LsusdW[isq][isq2]); } } // TODO: Case ~q_i -> ~q_j + h/H widNow = fac * wid * ps; if (DBSUSY) cout<alphaS(mHat * mHat); return; } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceGluino::calcPreFac(bool) { // Common coupling factors. preFac = alpS /( 8.0 * pow(mHat,3)); return; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceGluino::calcWidth(bool) { widNow = 0.0; if (ps == 0.) return; kinFac = (mHat * mHat - mf1 * mf1 + mf2 * mf2); if (id1Abs > 1000000 && (id1Abs % 100) < 7 && id2Abs < 7) { int isq = (abs(id1Abs)/1000000 == 2) ? (abs(id1Abs)%10+1)/2 + 3 : (abs(id1Abs)%10+1)/2; bool idown = id2Abs%2; int iq = (id2Abs + 1)/2; // ~g -> ~q + q if (idown){ widNow = kinFac * (norm(coupSUSYPtr->LsddG[isq][iq]) + norm(coupSUSYPtr->RsddG[isq][iq])) + 4.0 * mHat * mf2 * real(coupSUSYPtr->LsddG[isq][iq] * conj(coupSUSYPtr->RsddG[isq][iq])); } else{ widNow = kinFac * (norm(coupSUSYPtr->LsuuG[isq][iq]) + norm(coupSUSYPtr->RsuuG[isq][iq])) + 4.0 * mHat * mf2 * real(coupSUSYPtr->LsuuG[isq][iq] * conj(coupSUSYPtr->RsuuG[isq][iq])); } widNow = widNow * preFac * ps; if (DBSUSY) { cout<<"Gluino:: id1:"<alphaEM(mHat * mHat); s2W = coupSUSYPtr->sin2W; // Initialize functions for calculating 3-body widths psi.init(particleDataPtr,coupSUSYPtr); phi.init(particleDataPtr,coupSUSYPtr); upsil.init(particleDataPtr,coupSUSYPtr); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceNeut::calcPreFac(bool){ // Common coupling factors. preFac = alpEM / (8.0 * s2W * pow(mHat,3)); return; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceNeut::calcWidth(bool){ widNow = 0.0; if (ps ==0.) return; else if (mult ==2){ // Two-body decays kinFac = mHat * mHat - mf1 * mf1 + mf2 * mf2; kinFac2 = pow(mHat,4) + pow(mf1,4) - 2.0 * pow(mf2,4) + pow2(mHat) * pow2(mf2) + pow2(mf1) * pow2(mf2) - 2.0 * pow2(mHat) * pow2(mf1); // Stable lightest neutralino if (idRes == 1000022) return; double fac = 0.0; int iNeut1 = coupSUSYPtr->typeNeut(idRes); int iNeut2 = coupSUSYPtr->typeNeut(id1Abs); int iChar1 = coupSUSYPtr->typeChar(id1Abs); if (iNeut2>0 && id2Abs == 23){ // ~chi0_i -> chi0_j + Z fac = kinFac2 * (norm(coupSUSYPtr->OLpp[iNeut1][iNeut2]) + norm(coupSUSYPtr->ORpp[iNeut1][iNeut2])); fac -= 12.0 * mHat * mf1 * pow2(mf2) * real(coupSUSYPtr->OLpp[iNeut1][iNeut2] * conj(coupSUSYPtr->ORpp[iNeut1][iNeut2])); fac /= pow2(mf2) * (1.0 - s2W); } else if (iChar1>0 && id2Abs==24){ // ~chi0_i -> chi+_j + W- (or c.c.) fac = kinFac2 * (norm(coupSUSYPtr->OL[iNeut1][iChar1]) + norm(coupSUSYPtr->OR[iNeut1][iChar1])); fac -= 12.0 * mHat * mf1 * pow2(mf2) * real(coupSUSYPtr->OL[iNeut1][iChar1] * conj(coupSUSYPtr->OR[iNeut1][iChar1])); fac /= pow2(mf2); } else if (id1Abs > 1000000 && id1Abs%100 < 7 && id2Abs < 7){ // ~chi0_k -> ~q + q bool idown = (id1Abs%2 == 1); int iq = (id2Abs + 1 )/ 2; int isq = (abs(id1Abs)/1000000 == 2) ? (abs(id1Abs)%10+1)/2 + 3 : (abs(id1Abs)%10+1)/2; if (idown){ fac = kinFac * (norm(coupSUSYPtr->LsddX[isq][iq][iNeut1]) + norm(coupSUSYPtr->RsddX[isq][iq][iNeut1])); fac += 4.0 * mHat * mf2 * real(coupSUSYPtr->LsddX[isq][iq][iNeut1] * conj(coupSUSYPtr->RsddX[isq][iq][iNeut1])); } else{ fac = kinFac * (norm(coupSUSYPtr->LsuuX[isq][iq][iNeut1]) + norm(coupSUSYPtr->RsuuX[isq][iq][iNeut1])); fac += 4.0 * mHat * mf2 * real(coupSUSYPtr->LsuuX[isq][iq][iNeut1] * conj(coupSUSYPtr->RsuuX[isq][iq][iNeut1])); } // Extra multiplicative factor of 3 over sleptons fac *= 6.0/(1 - s2W); } else if (id1Abs > 1000000 && id1Abs%100 > 10 && id1Abs%100 < 17 && id2Abs < 17){ // ~chi0_k -> ~l + l bool idown = id2Abs%2; int il = (id2Abs - 9)/ 2; int isl = (abs(id1Abs)/1000000 == 2) ? (abs(id1Abs)%10+1)/2 + 3 : (abs(id1Abs)%10+1)/2; if (idown){ fac = kinFac * (norm(coupSUSYPtr->LsllX[isl][il][iNeut1]) + norm(coupSUSYPtr->RsllX[isl][il][iNeut1])); fac += 4.0 * mHat * mf2 * real(coupSUSYPtr->LsllX[isl][il][iNeut1] * conj(coupSUSYPtr->RsllX[isl][il][iNeut1])); } else{ fac = kinFac * (norm(coupSUSYPtr->LsvvX[isl][il][iNeut1])); } fac *= 2.0/(1 - s2W); } // TODO: Decays in higgs // Final width for 2-body decays widNow = fac * preFac * ps ; if (DBSUSY) { cout<isUDD) return; if (id1Abs < 7 && id2Abs < 7 && id3Abs < 7){ // Check that quarks compatible with UDD structure if ((id1Abs+id2Abs+id3Abs)%2 == 1) return; double rvfac,m12min,m12max,integral; int idInt; // Loop over mass eigenstate in actual propagator for (int idIntRes = 1; idIntRes <= 6; idIntRes++){ // Right handed field in the UDD coupling for (int iSq = 1; iSq <= 3; iSq++){ double m1, m2, m3, mixfac1(0.), mixfac2(0.), mixfac3(0.); int itemp1,itemp2,itemp3; // up/down-type internal lines for (int itype = 1; itype<=3; itype++){ //itype = 1: up //itype = 2: down1 //itype = 3: down2 if (itype ==1 ) idInt = coupSUSYPtr->idSup(idIntRes); else idInt = coupSUSYPtr->idSdown(idIntRes); if (id1Abs%2 == 0){ if (itype == 1){ itemp3 = id1Abs; itemp1 = id2Abs; itemp2 = id3Abs; rvfac = pow2( coupSUSYPtr->rvUDD[iSq][(id2Abs+1)/2][(id3Abs+1)/2]); }else if (itype ==2){ itemp3 = id2Abs; itemp1 = id1Abs; itemp2 = id3Abs; rvfac = pow2( coupSUSYPtr->rvUDD[(id1Abs+1)/2][iSq][(id3Abs+1)/2]); } else{ itemp3 = id3Abs; itemp1 = id1Abs; itemp2 = id2Abs; rvfac = pow2( coupSUSYPtr->rvUDD[(id1Abs+1)/2][(id2Abs+1)/2][iSq]); } }else if (id2Abs%2 == 0){ if (itype==1){ itemp3 = id2Abs; itemp1 = id1Abs; itemp2 = id3Abs; rvfac = pow2( coupSUSYPtr->rvUDD[iSq][(id1Abs+1)/2][(id3Abs+1)/2]); }else if (itype ==2){ itemp3 = id1Abs; itemp1 = id2Abs; itemp2 = id3Abs; rvfac = pow2( coupSUSYPtr->rvUDD[(id2Abs+1)/2][iSq][(id3Abs+1)/2]); } else{ itemp3 = id3Abs; itemp1 = id2Abs; itemp2 = id1Abs; rvfac = pow2( coupSUSYPtr->rvUDD[(id2Abs+1)/2][(id2Abs+1)/2][iSq]); } }else{ if (itype==1){ itemp3 = id3Abs; itemp1 = id1Abs; itemp2 = id2Abs; rvfac = pow2( coupSUSYPtr->rvUDD[iSq][(id1Abs+1)/2][(id2Abs+1)/2]); }else if (itype ==2){ itemp3 = id2Abs; itemp1 = id1Abs; itemp2 = id3Abs; rvfac = pow2( coupSUSYPtr->rvUDD[(id3Abs+1)/2][iSq][(id2Abs+1)/2]); } else{ itemp3 = id3Abs; itemp1 = id1Abs; itemp2 = id2Abs; rvfac = pow2( coupSUSYPtr->rvUDD[(id3Abs+1)/2][(id1Abs+1)/2][iSq]); } } m1 = particleDataPtr->m0(itemp1); m2 = particleDataPtr->m0(itemp2); m3 = particleDataPtr->m0(itemp3); m12min = pow2(m1+m2); m12max = pow2(mHat-m3); // Ignore mode when 2-body decay is possible if (mRes > particleDataPtr->m0(idInt) + particleDataPtr->m0(itemp3)) continue; // Single diagram squared terms psi.setInternal(idRes, itemp1, itemp2, itemp3, idInt, 0); // Mixing with R-states if (itype == 1) mixfac1 = norm(coupSUSYPtr->Rusq[idIntRes][iSq+3]); else mixfac1 = norm(coupSUSYPtr->Rdsq[idIntRes][iSq+3]); if (abs(rvfac * mixfac1) > 1.0e-8) { integral = integrateGauss(&psi,m12min,m12max,1.0e-4); widNow += rvfac * mixfac1 * integral; // if (DBSUSY || idRes == 1000023) // cout << scientific << setw(10) <<"Psi: intRes: "<idSup(idIntRes2); mixfac2 = 2.0 * real(coupSUSYPtr->Rusq[idIntRes][iSq+3] * conj(coupSUSYPtr->Rusq[idIntRes2][iSq+3])); } else { idInt2 = coupSUSYPtr->idSdown(idIntRes2); mixfac2 = 2.0 * real(coupSUSYPtr->Rdsq[idIntRes][iSq+3] * conj(coupSUSYPtr->Rdsq[idIntRes2][iSq+3])); } // Ignore mode when 2-body decay is possible if (mRes > particleDataPtr->m0(idInt2) + particleDataPtr->m0(itemp3)) continue; upsil.setInternal(idRes,itemp1, itemp2,itemp3,idInt,idInt2); if (abs(rvfac * mixfac2) > 0.0) { integral = integrateGauss(&upsil,m12min,m12max,1.0e-4); widNow += rvfac * mixfac2 * integral; // if (DBSUSY || idRes == 1000023) // cout << scientific << setw(10) <<"Upsilon: intRes: " // <idSdown(idIntRes2); mixfac3 = 2.0 * real(coupSUSYPtr->Rusq[idIntRes][iSq+3] * conj(coupSUSYPtr->Rdsq[idIntRes2][iSq2+3])); } else { idInt2 = coupSUSYPtr->idSdown(idIntRes2); mixfac3 = 2.0 * real(coupSUSYPtr->Rdsq[idIntRes][iSq+3] * conj(coupSUSYPtr->Rdsq[idIntRes2][iSq2+3])); } if (abs(rvfac * mixfac3) > 0.0) { phi.setInternal(idRes,itemp1, itemp2,itemp3,idInt,idInt2); //integral = 0; //if (idIntRes == 2 && iSq2 ==4) integral = integrateGauss(&phi,m12min,m12max,1.0e-4); widNow -= rvfac * mixfac2 * integral; } } } } } } } // Normalisation. Extra factor of 2 to account for the fact that // d_i, d_j will always be ordered in ascending order. N_c! = 6 widNow *= 12.0 /(pow3(2.0 * M_PI * mHat) * 32.0); } return; } //========================================================================== // Class ResonanceChar // Derived class for Neutralino Resonances // Decays into higgses/sleptons not yet implemented //-------------------------------------------------------------------------- void ResonanceChar::initConstants(){ alpEM = coupSUSYPtr->alphaEM(mHat * mHat); s2W = coupSUSYPtr->sin2W; return; } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceChar::calcPreFac(bool){ preFac = alpEM / (8.0 * s2W * pow(mHat,3)); return; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceChar::calcWidth(bool){ widNow = 0.0; if (ps == 0.) return; if (mult ==2){ double fac = 0.0; kinFac = mHat * mHat - mf1 * mf1 + mf2 * mf2; kinFac2 = pow(mHat,4) + pow(mf1,4) - 2.0 * pow(mf2,4) + pow2(mHat) * pow2(mf2) + pow2(mf1) * pow2(mf2) - 2.0 * pow2(mHat) * pow2(mf1); int idChar1 = coupSUSYPtr->typeChar(idRes); int idChar2 = coupSUSYPtr->typeChar(id1Abs); int idNeut1 = coupSUSYPtr->typeNeut(id1Abs); if (idChar2>0 && id2Abs == 23){ // ~chi_i -> chi_j + Z fac = kinFac2 * (norm(coupSUSYPtr->OLp[idChar1][idChar2]) + norm(coupSUSYPtr->ORp[idChar1][idChar2])); fac -= 12.0 * mHat * mf1 * pow2(mf2) * real(coupSUSYPtr->OLp[idChar1][idChar2] * conj(coupSUSYPtr->ORp[idChar1][idChar2])); fac /= pow2(mf2) * (1.0 - s2W); } else if (idNeut1>0 && id2Abs==24){ // ~chi_i -> chi0_j + W- (or c.c.) fac = kinFac2 * (norm(coupSUSYPtr->OL[idNeut1][idChar1]) + norm(coupSUSYPtr->OR[idNeut1][idChar1])); fac -= 12.0 * mHat * mf1 * pow2(mf2) * real(coupSUSYPtr->OL[idNeut1][idChar1] * conj(coupSUSYPtr->OR[idNeut1][idChar1])); fac /= pow2(mf2); } else if (id1Abs > 1000000 && id1Abs%100 < 7 && id2Abs < 7){ // ~chi0_k -> ~q + q bool idown = (id1Abs%2 == 1); int iq = (id2Abs + 1 )/ 2; int isq = (abs(id1Abs)/1000000 == 2) ? (abs(id1Abs)%10+1)/2 + 3 : (abs(id1Abs)%10+1)/2; if (idown){ fac = kinFac * (norm(coupSUSYPtr->LsduX[isq][iq][idChar1]) + norm(coupSUSYPtr->RsduX[isq][iq][idChar1])); fac += 4.0 * mHat * mf2 * real(coupSUSYPtr->LsduX[isq][iq][idChar1] * conj(coupSUSYPtr->RsduX[isq][iq][idChar1])); } else{ fac = kinFac * (norm(coupSUSYPtr->LsudX[isq][iq][idChar1]) + norm(coupSUSYPtr->RsudX[isq][iq][idChar1])); fac += 4.0 * mHat * mf2 * real(coupSUSYPtr->LsudX[isq][iq][idChar1] * conj(coupSUSYPtr->RsudX[isq][iq][idChar1])); } fac *= 6.0/(1 - s2W); } else if (id1Abs > 1000000 && id1Abs%100 > 10 && id1Abs%100 < 17 && id2Abs < 17){ // ~chi+_k -> ~l + l bool idown = id2Abs%2; int il = (id2Abs - 9)/ 2; int isl = (abs(id1Abs)/1000000 == 2) ? (abs(id1Abs)%10+1)/2 + 3 : (abs(id1Abs)%10+1)/2; if (idown){ fac = kinFac * (norm(coupSUSYPtr->LslvX[isl][il][idChar1]) + norm(coupSUSYPtr->RslvX[isl][il][idChar1])); fac += 4.0 * mHat * mf2 * real(coupSUSYPtr->LslvX[isl][il][idChar1] * conj(coupSUSYPtr->RslvX[isl][il][idChar1])); } else{ fac = kinFac * (norm(coupSUSYPtr->LsvlX[isl][il][idChar1])); } fac *= 2.0/(1 - s2W); } // TODO: Decays in higgs widNow = fac * preFac * ps ; if (DBSUSY) { cout<alphaEM(mHat * mHat); s2W = coupSUSYPtr->sin2W; } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceSlepton::calcPreFac(bool) { // Common coupling factors. preFac = 1.0 / (s2W * pow(mHat,3)); } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceSlepton::calcWidth(bool) { // Slepton type -- in u_i/d_i and generation int ksusy = 1000000; int isl = (abs(idRes)/ksusy == 2) ? (abs(idRes)%10+1)/2 + 3 : (abs(idRes)%10+1)/2; int il = (id2Abs-9)/2; bool islep = idRes%2; // Check that mass is above threshold. if (ps == 0.) return; else{ // Two-body decays kinFac = (mHat * mHat - mf1 * mf1 - mf2 * mf2); double fac = 0.0 , wid = 0.0; //Case 1: RPV: To be implemented //Case 2: slepton + gaugino if (id1Abs > ksusy && id2Abs > 10 && id2Abs < 17) { for (int i=1; i<6 ; i++){ // ~ell/~nu -> ~chi0 + ell/nu if (coupSUSYPtr->idNeut(i)==id1Abs && idRes%2 == id2Abs%2){ fac = alpEM * preFac / (2.0 * (1 - s2W)); if (islep) wid = kinFac * (norm(coupSUSYPtr->LsllX[isl][il][i]) + norm(coupSUSYPtr->RsllX[isl][il][i])) - 4.0 * mHat * mf2 * real(coupSUSYPtr->LsllX[isl][il][i] * conj(coupSUSYPtr->RsllX[isl][il][i])); else wid = kinFac * (norm(coupSUSYPtr->LsvvX[isl][il][i]) + norm(coupSUSYPtr->RsvvX[isl][il][i])) - 4.0 * mHat * mf2 * real(coupSUSYPtr->LsvvX[isl][il][i] * conj(coupSUSYPtr->RsvvX[isl][il][i])); } // ~ell/~nu -> ~chi- + nu/ell else if (i < 3 && coupSUSYPtr->idChar(i)==id1Abs && idRes%2 != id2Abs%2){ fac = alpEM * preFac / (4.0 * (1 - s2W)); if (islep) wid = kinFac * (norm(coupSUSYPtr->LslvX[isl][il][i]) + norm(coupSUSYPtr->RslvX[isl][il][i])) - 4.0 * mHat * mf2 * real(coupSUSYPtr->LslvX[isl][il][i] * conj(coupSUSYPtr->RslvX[isl][il][i])); else wid = kinFac * (norm(coupSUSYPtr->LslvX[isl][il][i]) + norm(coupSUSYPtr->RslvX[isl][il][i])) - 4.0 * mHat * mf2 * real(coupSUSYPtr->LslvX[isl][il][i] * conj(coupSUSYPtr->RslvX[isl][il][i])); } } } //Case 3: ~l_i -> ~l_j + Z/W else if (id1Abs > ksusy+10 && id1Abs%100 < 17 && (id2Abs == 23 || id2Abs == 24)){ // factor of lambda^(3/2) = ps^3; fac = alpEM * preFac/(16.0 * pow2(mf2) * (1.0 - s2W)) * pow2(ps) ; int isl2 = (id1Abs/ksusy == 2) ? (id1Abs%10+1)/2 + 3: (id1Abs%10+1)/2; if (id2Abs == 23 && id1Abs%2 == idRes%2){ if (islep) wid = norm(coupSUSYPtr->LslslZ[isl][isl2] + coupSUSYPtr->RslslZ[isl][isl2]); else wid = norm(coupSUSYPtr->LsvsvZ[isl][isl2] + coupSUSYPtr->RsvsvZ[isl][isl2]); } else if (id2Abs == 24 && id1Abs%2 != idRes%2){ if (islep) wid = norm(coupSUSYPtr->LslsvW[isl2][isl]); else wid = norm(coupSUSYPtr->LslsvW[isl][isl2]); } } // TODO: Case ~l_i -> ~l_j + h/H widNow = fac * wid * ps; if (DBSUSY) cout< xhi) { cerr<<" (integrateGauss:) -> xhi < xlo"<function(zmi+dz) + widthFn->function(zmi-dz)); } s8 *= zmr; double s16=0.0; for (int i=0;i<8;i++) { double dz = zmr * x16[i]; s16 += w16[i]*(widthFn->function(zmi+dz) + widthFn->function(zmi-dz)); } s16 *= zmr; if (abs(s16-s8) < tol*(1+abs(s16))) { //precision in this bin OK, add to cumulative and go to next nextbin=true; sum += s16; //next bin: LO = end of current, HI = end of integration region. zlo=zhi; zhi=xhi; if ( zlo == zhi ) nextbin = false; } else { //precision in this bin not OK, subdivide. if (1.0 + c*abs(zmr) == 1.0) { cerr << " (integrateGauss:) too high accuracy required"<eCM(); } //-------------------------------------------------------------------------- // Function to print information. void Merging::statistics( ostream& os ) { // Recall switch to enfore merging scale cut. bool enforceCutOnLHE = settingsPtr->flag("Merging:enforceCutOnLHE"); // Recall merging scale value. double tmsval = mergingHooksPtr->tms(); bool printBanner = enforceCutOnLHE && tmsNowMin > TMSMISMATCH*tmsval; // Reset minimal tms value. tmsNowMin = infoPtr->eCM(); if (!printBanner) return; // Header. os << "\n *------- PYTHIA Matrix Element Merging Information ------" << "-------------------------------------------------------*\n" << " | " << " |\n"; // Print warning if the minimal tms value of any event was significantly // above the desired merging scale value. os << " | Warning in Merging::statistics: All Les Houches events" << " significantly above Merging:TMS cut. Please check. |\n"; // Listing finished. os << " | " << " |\n" << " *------- End PYTHIA Matrix Element Merging Information -----" << "-----------------------------------------------------*" << endl; } //-------------------------------------------------------------------------- // Function to steer different merging prescriptions. int Merging::mergeProcess(Event& process){ int vetoCode = 1; // Possibility to apply merging scale to an input event. bool applyTMSCut = settingsPtr->flag("Merging:doXSectionEstimate"); if ( applyTMSCut && cutOnProcess(process) ) return -1; // Done if only a cut should be applied. if ( applyTMSCut ) return 1; // Possibility to perform CKKW-L merging on this event. if ( mergingHooksPtr->doCKKWLMerging() ) vetoCode = mergeProcessCKKWL(process); // Possibility to perform UMEPS merging on this event. if ( mergingHooksPtr->doUMEPSMerging() ) vetoCode = mergeProcessUMEPS(process); // Possibility to perform NL3 NLO merging on this event. if ( mergingHooksPtr->doNL3Merging() ) vetoCode = mergeProcessNL3(process); // Possibility to perform UNLOPS merging on this event. if ( mergingHooksPtr->doUNLOPSMerging() ) vetoCode = mergeProcessUNLOPS(process); return vetoCode; } //-------------------------------------------------------------------------- // Function to perform CKKW-L merging on this event. int Merging::mergeProcessCKKWL( Event& process) { // Ensure that merging hooks to not veto events in the trial showers. mergingHooksPtr->doIgnoreStep(true); // For pp > h, allow cut on state, so that underlying processes // can be clustered to gg > h if ( mergingHooksPtr->getProcessString().compare("pp>h") == 0 ) mergingHooksPtr->allowCutOnRecState(true); // For now, prefer construction of ordered histories. mergingHooksPtr->orderHistories(true); // Reset weight of the event. double wgt = 1.0; mergingHooksPtr->setWeightCKKWL(1.); mergingHooksPtr->muMI(-1.); // Prepare process record for merging. If Pythia has already decayed // resonances used to define the hard process, remove resonance decay // products. Event newProcess( mergingHooksPtr->bareEvent( process, true) ); // Store candidates for the splitting V -> qqbar'. mergingHooksPtr->storeHardProcessCandidates( newProcess); // Check if event passes the merging scale cut. double tmsval = mergingHooksPtr->tms(); // Get merging scale in current event. double tmsnow = mergingHooksPtr->tmsNow( newProcess ); // Calculate number of clustering steps. int nSteps = mergingHooksPtr->getNumberOfClusteringSteps( newProcess); // Reset the minimal tms value, if necessary. tmsNowMin = (nSteps == 0) ? 0. : min(tmsNowMin, tmsnow); // Enfore merging scale cut if the event did not pass the merging scale // criterion. bool enforceCutOnLHE = settingsPtr->flag("Merging:enforceCutOnLHE"); if ( enforceCutOnLHE && nSteps > 0 && tmsnow < tmsval ) { string message="Warning in Merging::mergeProcessCKKWL: Les Houches Event"; message+=" fails merging scale cut. Reject event."; infoPtr->errorMsg(message); mergingHooksPtr->setWeightCKKWL(0.); return -1; } // Get random number to choose a path. double RN = rndmPtr->flat(); // Set dummy process scale. newProcess.scale(0.0); // Generate all histories. History FullHistory( nSteps, 0.0, newProcess, Clustering(), mergingHooksPtr, (*beamAPtr), (*beamBPtr), particleDataPtr, infoPtr, true, true, true, true, 1.0, 0); // Project histories onto desired branches, e.g. only ordered paths. FullHistory.projectOntoDesiredHistories(); // Calculate CKKWL weight: // Perform reweighting with Sudakov factors, save alpha_s ratios and // PDF ratio weights. wgt = FullHistory.weightTREE( trialPartonLevelPtr, mergingHooksPtr->AlphaS_FSR(), mergingHooksPtr->AlphaS_ISR(), RN); // Event with production scales set for further (trial) showering // and starting conditions for the shower. FullHistory.getStartingConditions( RN, process ); // If necessary, reattach resonance decay products. mergingHooksPtr->reattachResonanceDecays(process); // Allow to dampen histories in which the lowest multiplicity reclustered // state does not pass the lowest multiplicity cut of the matrix element. double dampWeight = mergingHooksPtr->dampenIfFailCuts( FullHistory.lowestMultProc(RN) ); // Save the weight of the event for histogramming. Only change the // event weight after trial shower on the matrix element // multiplicity event (= in doVetoStep). wgt *= dampWeight; // Set QCD 2->2 starting scale different from arbitrary scale in LHEF! // --> Set to minimal mT of partons. int nFinal = 0; double muf = process[0].e(); for ( int i=0; i < process.size(); ++i ) if ( process[i].isFinal() && (process[i].colType() != 0 || process[i].id() == 22 ) ) { nFinal++; muf = min( muf, abs(process[i].mT()) ); } // For pure QCD dijet events (only!), set the process scale to the // transverse momentum of the outgoing partons. if ( nSteps == 0 && nFinal == 2 && ( mergingHooksPtr->getProcessString().compare("pp>jj") == 0 || mergingHooksPtr->getProcessString().compare("pp>aj") == 0) ) process.scale(muf); // Save the weight of the event for histogramming. mergingHooksPtr->setWeightCKKWL(wgt); // Allow merging hooks to veto events from now on. mergingHooksPtr->doIgnoreStep(false); // If no-emission probability is zero. if ( wgt == 0. ) return 0; // Done return 1; } //-------------------------------------------------------------------------- // Function to perform UMEPS merging on this event. int Merging::mergeProcessUMEPS( Event& process) { // Initialise which part of UMEPS merging is applied. bool doUMEPSTree = settingsPtr->flag("Merging:doUMEPSTree"); bool doUMEPSSubt = settingsPtr->flag("Merging:doUMEPSSubt"); // Save number of looping steps mergingHooksPtr->nReclusterSave = settingsPtr->mode("Merging:nRecluster"); int nRecluster = settingsPtr->mode("Merging:nRecluster"); // Ensure that merging hooks does not remove emissions. mergingHooksPtr->doIgnoreEmissions(true); // For pp > h, allow cut on state, so that underlying processes // can be clustered to gg > h if ( mergingHooksPtr->getProcessString().compare("pp>h") == 0 ) mergingHooksPtr->allowCutOnRecState(true); // For now, prefer construction of ordered histories. mergingHooksPtr->orderHistories(true); // Reset weights of the event. double wgt = 1.; mergingHooksPtr->setWeightCKKWL(1.); mergingHooksPtr->muMI(-1.); // Prepare process record for merging. If Pythia has already decayed // resonances used to define the hard process, remove resonance decay // products. Event newProcess( mergingHooksPtr->bareEvent( process, true) ); // Store candidates for the splitting V -> qqbar'. mergingHooksPtr->storeHardProcessCandidates( newProcess ); // Check if event passes the merging scale cut. double tmsval = mergingHooksPtr->tms(); // Get merging scale in current event. double tmsnow = mergingHooksPtr->tmsNow( newProcess ); // Calculate number of clustering steps. int nSteps = mergingHooksPtr->getNumberOfClusteringSteps( newProcess ); // Reset the minimal tms value, if necessary. tmsNowMin = (nSteps == 0) ? 0. : min(tmsNowMin, tmsnow); // Get random number to choose a path. double RN = rndmPtr->flat(); // Set dummy process scale. newProcess.scale(0.0); // Generate all histories. History FullHistory( nSteps, 0.0, newProcess, Clustering(), mergingHooksPtr, (*beamAPtr), (*beamBPtr), particleDataPtr, infoPtr, true, true, true, true, 1.0, 0); // Project histories onto desired branches, e.g. only ordered paths. FullHistory.projectOntoDesiredHistories(); // Do not apply cut if the configuration could not be projected onto an // underlying born configuration. bool applyCut = nSteps > 0 && FullHistory.select(RN)->nClusterings() > 0; // Enfore merging scale cut if the event did not pass the merging scale // criterion. bool enforceCutOnLHE = settingsPtr->flag("Merging:enforceCutOnLHE"); if ( enforceCutOnLHE && applyCut && tmsnow < tmsval ) { string message="Warning in Merging::mergeProcessUMEPS: Les Houches Event"; message+=" fails merging scale cut. Reject event."; infoPtr->errorMsg(message); mergingHooksPtr->setWeightCKKWL(0.); return -1; } // Check reclustering steps to correctly apply MPI. int nPerformed = 0; if ( nSteps > 0 && doUMEPSSubt && !FullHistory.getFirstClusteredEventAboveTMS( RN, nRecluster, newProcess, nPerformed, false ) ) { // Discard if the state could not be reclustered to a state above TMS. mergingHooksPtr->setWeightCKKWL(0.); return -1; } mergingHooksPtr->nMinMPI(nSteps - nPerformed); // Calculate CKKWL weight: // Perform reweighting with Sudakov factors, save alpha_s ratios and // PDF ratio weights. if ( doUMEPSTree ) { wgt = FullHistory.weight_UMEPS_TREE( trialPartonLevelPtr, mergingHooksPtr->AlphaS_FSR(), mergingHooksPtr->AlphaS_ISR(), RN ); } else { wgt = FullHistory.weight_UMEPS_SUBT( trialPartonLevelPtr, mergingHooksPtr->AlphaS_FSR(), mergingHooksPtr->AlphaS_ISR(), RN ); } // Event with production scales set for further (trial) showering // and starting conditions for the shower. if ( doUMEPSTree ) FullHistory.getStartingConditions( RN, process ); // Do reclustering (looping) steps. else FullHistory.getFirstClusteredEventAboveTMS( RN, nRecluster, process, nPerformed, true ); // Allow to dampen histories in which the lowest multiplicity reclustered // state does not pass the lowest multiplicity cut of the matrix element double dampWeight = mergingHooksPtr->dampenIfFailCuts( FullHistory.lowestMultProc(RN) ); // Save the weight of the event for histogramming. Only change the // event weight after trial shower on the matrix element // multiplicity event (= in doVetoStep) wgt *= dampWeight; // Save the weight of the event for histogramming. mergingHooksPtr->setWeightCKKWL(wgt); // Set QCD 2->2 starting scale different from arbitrary scale in LHEF! // --> Set to minimal mT of partons. int nFinal = 0; double muf = process[0].e(); for ( int i=0; i < process.size(); ++i ) if ( process[i].isFinal() && (process[i].colType() != 0 || process[i].id() == 22 ) ) { nFinal++; muf = min( muf, abs(process[i].mT()) ); } // For pure QCD dijet events (only!), set the process scale to the // transverse momentum of the outgoing partons. // Calculate number of clustering steps. int nStepsNew = mergingHooksPtr->getNumberOfClusteringSteps( process ); if ( nStepsNew == 0 && ( mergingHooksPtr->getProcessString().compare("pp>jj") == 0 || mergingHooksPtr->getProcessString().compare("pp>aj") == 0) ) process.scale(muf); // Reset hard process candidates (changed after clustering a parton). mergingHooksPtr->storeHardProcessCandidates( process ); // If necessary, reattach resonance decay products. mergingHooksPtr->reattachResonanceDecays(process); // Allow merging hooks to remove emissions from now on. mergingHooksPtr->doIgnoreEmissions(false); // If no-emission probability is zero. if ( wgt == 0. ) return 0; // Done return 1; } //-------------------------------------------------------------------------- // Function to perform NL3 NLO merging on this event. int Merging::mergeProcessNL3( Event& process) { // Initialise which part of NL3 merging is applied. bool doNL3Tree = settingsPtr->flag("Merging:doNL3Tree"); bool doNL3Loop = settingsPtr->flag("Merging:doNL3Loop"); bool doNL3Subt = settingsPtr->flag("Merging:doNL3Subt"); // Save number of looping steps. int nRequested = settingsPtr->mode("Merging:nRequested"); // Ensure that hooks (NL3 part) to not remove emissions. mergingHooksPtr->doIgnoreEmissions(true); // Ensure that hooks (CKKWL part) to not veto events in trial showers. mergingHooksPtr->doIgnoreStep(true); // For pp > h, allow cut on state, so that underlying processes // can be clustered to gg > h if ( mergingHooksPtr->getProcessString().compare("pp>h") == 0) mergingHooksPtr->allowCutOnRecState(true); // For now, prefer construction of ordered histories. mergingHooksPtr->orderHistories(true); // Reset weight of the event double wgt = 1.; mergingHooksPtr->setWeightCKKWL(1.); // Reset the O(alphaS)-term of the CKKW-L weight. double wgtFIRST = 0.; mergingHooksPtr->setWeightFIRST(0.); mergingHooksPtr->muMI(-1.); // Prepare process record for merging. If Pythia has already decayed // resonances used to define the hard process, remove resonance decay // products. Event newProcess( mergingHooksPtr->bareEvent( process, true) ); // Store candidates for the splitting V -> qqbar' mergingHooksPtr->storeHardProcessCandidates( newProcess); // Check if event passes the merging scale cut. double tmsval = mergingHooksPtr->tms(); // Get merging scale in current event. double tmsnow = mergingHooksPtr->tmsNow( newProcess ); // Calculate number of clustering steps int nSteps = mergingHooksPtr->getNumberOfClusteringSteps( newProcess); // Reset the minimal tms value, if necessary. tmsNowMin = (nSteps == 0) ? 0. : min(tmsNowMin, tmsnow); // Enfore merging scale cut if the event did not pass the merging scale // criterion. bool enforceCutOnLHE = settingsPtr->flag("Merging:enforceCutOnLHE"); if ( enforceCutOnLHE && nSteps > 0 && nSteps == nRequested && tmsnow < tmsval ) { string message="Warning in Merging::mergeProcessNL3: Les Houches Event"; message+=" fails merging scale cut. Reject event."; infoPtr->errorMsg(message); mergingHooksPtr->setWeightCKKWL(0.); mergingHooksPtr->setWeightFIRST(0.); return -1; } // Get random number to choose a path. double RN = rndmPtr->flat(); // Set dummy process scale. newProcess.scale(0.0); // Generate all histories History FullHistory( nSteps, 0.0, newProcess, Clustering(), mergingHooksPtr, (*beamAPtr), (*beamBPtr), particleDataPtr, infoPtr, true, true, true, true, 1.0, 0); // Project histories onto desired branches, e.g. only ordered paths. FullHistory.projectOntoDesiredHistories(); // Discard states that cannot be projected unto a state with one less jet. if ( nSteps > 0 && doNL3Subt && FullHistory.select(RN)->nClusterings() == 0 ){ mergingHooksPtr->setWeightCKKWL(0.); mergingHooksPtr->setWeightFIRST(0.); return -1; } // Potentially recluster real emission jets for powheg input containing // "too many" jets, i.e. real-emission kinematics. bool containsRealKin = nSteps > nRequested && nSteps > 0; // Perform one reclustering for real emission kinematics, then apply merging // scale cut on underlying Born kinematics. if ( containsRealKin ) { Event dummy = Event(); // Initialise temporary output of reclustering. dummy.clear(); dummy.init( "(hard process-modified)", particleDataPtr ); dummy.clear(); // Recluster once. if ( !FullHistory.getClusteredEvent( RN, nSteps, dummy )) { mergingHooksPtr->setWeightCKKWL(0.); mergingHooksPtr->setWeightFIRST(0.); return -1; } double tnowNew = mergingHooksPtr->tmsNow( dummy ); // Veto if underlying Born kinematics do not pass merging scale cut. if ( enforceCutOnLHE && nSteps > 0 && nRequested > 0 && tnowNew < tmsval ) { mergingHooksPtr->setWeightCKKWL(0.); mergingHooksPtr->setWeightFIRST(0.); return -1; } } // Remember number of jets, to include correct MPI no-emission probabilities. if ( doNL3Subt || containsRealKin ) mergingHooksPtr->nMinMPI(nSteps - 1); else mergingHooksPtr->nMinMPI(nSteps); // Calculate weight // Do LO or first part of NLO tree-level reweighting if( doNL3Tree ) { // Perform reweighting with Sudakov factors, save as ratios and // PDF ratio weights wgt = FullHistory.weightTREE( trialPartonLevelPtr, mergingHooksPtr->AlphaS_FSR(), mergingHooksPtr->AlphaS_ISR(), RN); } else if( doNL3Loop || doNL3Subt ) { // No reweighting, just set event scales properly and incorporate MPI // no-emission probabilities. wgt = FullHistory.weightLOOP( trialPartonLevelPtr, RN); } // Event with production scales set for further (trial) showering // and starting conditions for the shower if ( !doNL3Subt && !containsRealKin ) FullHistory.getStartingConditions(RN, process); // For sutraction of nSteps-additional resolved partons from // the nSteps-1 parton phase space, recluster the last parton // in nSteps-parton events, and sutract later else { // Function to return the reclustered event if ( !FullHistory.getClusteredEvent( RN, nSteps, process )) { mergingHooksPtr->setWeightCKKWL(0.); mergingHooksPtr->setWeightFIRST(0.); return -1; } } // Allow to dampen histories in which the lowest multiplicity reclustered // state does not pass the lowest multiplicity cut of the matrix element double dampWeight = mergingHooksPtr->dampenIfFailCuts( FullHistory.lowestMultProc(RN) ); // Save the weight of the event for histogramming. Only change the // event weight after trial shower on the matrix element // multiplicity event (= in doVetoStep) wgt *= dampWeight; // For tree level samples in NL3, rescale with k-Factor if (doNL3Tree ){ // Find k-factor double kFactor = 1.; if( nSteps > mergingHooksPtr->nMaxJetsNLO() ) kFactor = mergingHooksPtr->kFactor( mergingHooksPtr->nMaxJetsNLO() ); else kFactor = mergingHooksPtr->kFactor(nSteps); // For NLO merging, rescale CKKW-L weight with k-factor wgt *= kFactor; } // Save the weight of the event for histogramming mergingHooksPtr->setWeightCKKWL(wgt); // Check if we need to subtract the O(\alpha_s)-term. If the number // of additional partons is larger than the number of jets for // which loop matrix elements are available, do standard CKKW-L bool doOASTree = doNL3Tree && nSteps <= mergingHooksPtr->nMaxJetsNLO(); // Now begin NLO part for tree-level events if ( doOASTree ) { // Calculate the O(\alpha_s)-term of the CKKWL weight wgtFIRST = FullHistory.weightFIRST( trialPartonLevelPtr, mergingHooksPtr->AlphaS_FSR(), mergingHooksPtr->AlphaS_ISR(), RN, rndmPtr ); // If necessary, also dampen the O(\alpha_s)-term wgtFIRST *= dampWeight; // Set the subtractive weight to the value calculated so far mergingHooksPtr->setWeightFIRST(wgtFIRST); // Subtract the O(\alpha_s)-term from the CKKW-L weight // If PDF contributions have not been included, subtract these later wgt = wgt - wgtFIRST; } // Set qcd 2->2 starting scale different from arbirtrary scale in LHEF! // --> Set to pT of partons double pT = 0.; for( int i=0; i < process.size(); ++i) if(process[i].isFinal() && process[i].colType() != 0) { pT = sqrt(pow(process[i].px(),2) + pow(process[i].py(),2)); break; } // For pure QCD dijet events (only!), set the process scale to the // transverse momentum of the outgoing partons. if ( nSteps == 0 && mergingHooksPtr->getProcessString().compare("pp>jj") == 0) process.scale(pT); // Reset hard process candidates (changed after clustering a parton). mergingHooksPtr->storeHardProcessCandidates( process ); // If necessary, reattach resonance decay products. mergingHooksPtr->reattachResonanceDecays(process); // Allow merging hooks (NL3 part) to remove emissions from now on. mergingHooksPtr->doIgnoreEmissions(false); // Allow merging hooks (CKKWL part) to veto events from now on. mergingHooksPtr->doIgnoreStep(false); // Done return 1; } //-------------------------------------------------------------------------- // Function to perform UNLOPS merging on this event. int Merging::mergeProcessUNLOPS( Event& process) { // Initialise which part of UNLOPS merging is applied. bool nloTilde = settingsPtr->flag("Merging:doUNLOPSTilde"); bool doUNLOPSTree = settingsPtr->flag("Merging:doUNLOPSTree"); bool doUNLOPSLoop = settingsPtr->flag("Merging:doUNLOPSLoop"); bool doUNLOPSSubt = settingsPtr->flag("Merging:doUNLOPSSubt"); bool doUNLOPSSubtNLO = settingsPtr->flag("Merging:doUNLOPSSubtNLO"); // Save number of looping steps mergingHooksPtr->nReclusterSave = settingsPtr->mode("Merging:nRecluster"); int nRecluster = settingsPtr->mode("Merging:nRecluster"); int nRequested = settingsPtr->mode("Merging:nRequested"); // Ensure that merging hooks to not remove emissions mergingHooksPtr->doIgnoreEmissions(true); // For now, prefer construction of ordered histories. mergingHooksPtr->orderHistories(true); // For pp > h, allow cut on state, so that underlying processes // can be clustered to gg > h if ( mergingHooksPtr->getProcessString().compare("pp>h") == 0) mergingHooksPtr->allowCutOnRecState(true); // Reset weight of the event. double wgt = 1.; mergingHooksPtr->setWeightCKKWL(1.); // Reset the O(alphaS)-term of the UMEPS weight. double wgtFIRST = 0.; mergingHooksPtr->setWeightFIRST(0.); mergingHooksPtr->muMI(-1.); // Prepare process record for merging. If Pythia has already decayed // resonances used to define the hard process, remove resonance decay // products. Event newProcess( mergingHooksPtr->bareEvent( process, true) ); // Store candidates for the splitting V -> qqbar' mergingHooksPtr->storeHardProcessCandidates( newProcess ); // Check if event passes the merging scale cut. double tmsval = mergingHooksPtr->tms(); // Get merging scale in current event. double tmsnow = mergingHooksPtr->tmsNow( newProcess ); // Calculate number of clustering steps int nSteps = mergingHooksPtr->getNumberOfClusteringSteps( newProcess); // Reset the minimal tms value, if necessary. tmsNowMin = (nSteps == 0) ? 0. : min(tmsNowMin, tmsnow); // Get random number to choose a path. double RN = rndmPtr->flat(); // Set dummy process scale. newProcess.scale(0.0); // Generate all histories History FullHistory( nSteps, 0.0, newProcess, Clustering(), mergingHooksPtr, (*beamAPtr), (*beamBPtr), particleDataPtr, infoPtr, true, true, true, true, 1.0, 0); // Project histories onto desired branches, e.g. only ordered paths. FullHistory.projectOntoDesiredHistories(); // Do not apply cut if the configuration could not be projected onto an // underlying born configuration. bool applyCut = nSteps > 0 && FullHistory.select(RN)->nClusterings() > 0; // Enfore merging scale cut if the event did not pass the merging scale // criterion. bool enforceCutOnLHE = settingsPtr->flag("Merging:enforceCutOnLHE"); if ( enforceCutOnLHE && applyCut && nSteps == nRequested && tmsnow < tmsval ) { string message="Warning in Merging::mergeProcessUNLOPS: Les Houches Event"; message+=" fails merging scale cut. Reject event."; infoPtr->errorMsg(message); mergingHooksPtr->setWeightCKKWL(0.); mergingHooksPtr->setWeightFIRST(0.); return -1; } // Potentially recluster real emission jets for powheg input containing // "too many" jets, i.e. real-emission kinematics. bool containsRealKin = nSteps > nRequested && nSteps > 0; if ( containsRealKin ) nRecluster += nSteps - nRequested; // Remove real emission events without underlying Born configuration from // the loop sample, since such states will be taken care of by tree-level // samples. if ( doUNLOPSLoop && containsRealKin && FullHistory.select(RN)->nClusterings() == 0 ) { mergingHooksPtr->setWeightCKKWL(0.); mergingHooksPtr->setWeightFIRST(0.); return -1; } // Discard if the state could not be reclustered to any state above TMS. int nPerformed = 0; if ( nSteps > 0 && ( doUNLOPSSubt || doUNLOPSSubtNLO || containsRealKin ) && !FullHistory.getFirstClusteredEventAboveTMS( RN, nRecluster, newProcess, nPerformed, false ) ) { mergingHooksPtr->setWeightCKKWL(0.); mergingHooksPtr->setWeightFIRST(0.); return -1; } // Check reclustering steps to correctly apply MPI. mergingHooksPtr->nMinMPI(nSteps - nPerformed); // Perform one reclustering for real emission kinematics, then apply merging // scale cut on underlying Born kinematics. if ( containsRealKin ) { Event dummy = Event(); // Initialise temporary output of reclustering. dummy.clear(); dummy.init( "(hard process-modified)", particleDataPtr ); dummy.clear(); // Recluster once. FullHistory.getClusteredEvent( RN, nSteps, dummy ); double tnowNew = mergingHooksPtr->tmsNow( dummy ); // Veto if underlying Born kinematics do not pass merging scale cut. if ( enforceCutOnLHE && nSteps > 0 && nRequested > 0 && tnowNew < tmsval ) { mergingHooksPtr->setWeightCKKWL(0.); mergingHooksPtr->setWeightFIRST(0.); return -1; } } // Calculate weights. // Do LO or first part of NLO tree-level reweighting if( doUNLOPSTree ) { // Perform reweighting with Sudakov factors, save as ratios and // PDF ratio weights wgt = FullHistory.weight_UNLOPS_TREE( trialPartonLevelPtr, mergingHooksPtr->AlphaS_FSR(), mergingHooksPtr->AlphaS_ISR(), RN); } else if( doUNLOPSLoop ) { // No reweighting, just set event scales properly wgt = FullHistory.weight_UNLOPS_LOOP( trialPartonLevelPtr, RN); } else if( doUNLOPSSubtNLO ) { // The standard prescripition contains no real-emission parts // No reweighting, just set event scales properly wgt = FullHistory.weight_UNLOPS_SUBTNLO( trialPartonLevelPtr, RN); } else if( doUNLOPSSubt ) { // The standard prescripition contains no subtraction parts // No reweighting, just set event scales properly wgt = FullHistory.weight_UNLOPS_SUBT( trialPartonLevelPtr, mergingHooksPtr->AlphaS_FSR(), mergingHooksPtr->AlphaS_ISR(), RN); } // Event with production scales set for further (trial) showering // and starting conditions for the shower. if (!doUNLOPSSubt && !doUNLOPSSubtNLO && !containsRealKin ) FullHistory.getStartingConditions(RN, process); // Do reclustering (looping) steps. else FullHistory.getFirstClusteredEventAboveTMS( RN, nRecluster, process, nPerformed, true ); // Allow to dampen histories in which the lowest multiplicity reclustered // state does not pass the lowest multiplicity cut of the matrix element double dampWeight = mergingHooksPtr->dampenIfFailCuts( FullHistory.lowestMultProc(RN) ); // Save the weight of the event for histogramming. Only change the // event weight after trial shower on the matrix element // multiplicity event (= in doVetoStep) wgt *= dampWeight; // For tree-level or subtractive sammples, rescale with k-Factor if ( doUNLOPSTree || doUNLOPSSubt ){ // Find k-factor double kFactor = 1.; if ( nSteps > mergingHooksPtr->nMaxJetsNLO() ) kFactor = mergingHooksPtr->kFactor( mergingHooksPtr->nMaxJetsNLO() ); else kFactor = mergingHooksPtr->kFactor(nSteps); // For NLO merging, rescale CKKW-L weight with k-factor wgt *= (nRecluster == 2 && nloTilde) ? 1. : kFactor; } // Save the weight of the event for histogramming mergingHooksPtr->setWeightCKKWL(wgt); // Check if we need to subtract the O(\alpha_s)-term. If the number // of additional partons is larger than the number of jets for // which loop matrix elements are available, do standard UMEPS. int nMaxNLO = mergingHooksPtr->nMaxJetsNLO(); bool doOASTree = doUNLOPSTree && nSteps <= nMaxNLO; bool doOASSubt = doUNLOPSSubt && nSteps <= nMaxNLO+1 && nSteps > 0 && nMaxNLO != 0; // Now begin NLO part for tree-level events if ( doOASTree || doOASSubt ) { // Calculate terms in expansion of the CKKW-L weight. int order = ( nSteps == 1 ) ? 1 : -1; if ( nSteps == 2 && nRecluster == 1 && nloTilde ) order = 0; wgtFIRST = FullHistory.weight_UNLOPS_CORRECTION( order, trialPartonLevelPtr, mergingHooksPtr->AlphaS_FSR(), mergingHooksPtr->AlphaS_ISR(), RN, rndmPtr ); // Second reclustering term if ( nSteps == 1 && doUNLOPSSubt && nloTilde ) wgtFIRST += 1.; // If necessary, also dampen the O(\alpha_s)-term wgtFIRST *= dampWeight; // Set the subtractive weight to the value calculated so far mergingHooksPtr->setWeightFIRST(wgtFIRST); // Subtract the O(\alpha_s)-term from the CKKW-L weight // If PDF contributions have not been included, subtract these later wgt = wgt - wgtFIRST; } // Do not subtract the O(as)-term if more than one reclustering has been // performed. if ( nPerformed > nRecluster ) mergingHooksPtr->setWeightFIRST(0.); // Set QCD 2->2 starting scale different from arbitrary scale in LHEF! // --> Set to minimal mT of partons. int nFinal = 0; double muf = process[0].e(); for ( int i=0; i < process.size(); ++i ) if ( process[i].isFinal() && (process[i].colType() != 0 || process[i].id() == 22 ) ) { nFinal++; muf = min( muf, abs(process[i].mT()) ); } // For pure QCD dijet events (only!), set the process scale to the // transverse momentum of the outgoing partons. if ( nSteps == 0 && nFinal == 2 && ( mergingHooksPtr->getProcessString().compare("pp>jj") == 0 || mergingHooksPtr->getProcessString().compare("pp>aj") == 0) ) process.scale(muf); // Reset hard process candidates (changed after clustering a parton). mergingHooksPtr->storeHardProcessCandidates( process ); // Check if resonance structure has been changed // (e.g. because of clustering W/Z/gluino) vector oldResonance; for ( int i=0; i < newProcess.size(); ++i ) if ( newProcess[i].status() == 22 ) oldResonance.push_back(newProcess[i].id()); vector newResonance; for ( int i=0; i < process.size(); ++i ) if ( process[i].status() == 22 ) newResonance.push_back(process[i].id()); // Compare old and new resonances for ( int i=0; i < int(oldResonance.size()); ++i ) for ( int j=0; j < int(newResonance.size()); ++j ) if ( newResonance[j] == oldResonance[i] ) { oldResonance[i] = 99; break; } bool hasNewResonances = (newResonance.size() != oldResonance.size()); for ( int i=0; i < int(oldResonance.size()); ++i ) hasNewResonances = (oldResonance[i] != 99); // If necessary, reattach resonance decay products. if (!hasNewResonances) mergingHooksPtr->reattachResonanceDecays(process); // Allow merging hooks to remove emissions from now on. mergingHooksPtr->doIgnoreEmissions(false); // If no-emission probability is zero. if ( wgt == 0. ) return 0; // If the resonance structure of the process has changed due to reclustering, // redo the resonance decays in Pythia::next() if (hasNewResonances) return 2; // Done return 1; } //-------------------------------------------------------------------------- // Function to apply the merging scale cut on an input event. bool Merging::cutOnProcess( Event& process) { // Save number of looping steps mergingHooksPtr->nReclusterSave = settingsPtr->mode("Merging:nRecluster"); int nRequested = settingsPtr->mode("Merging:nRequested"); // For now, prefer construction of ordered histories. mergingHooksPtr->orderHistories(true); // For pp > h, allow cut on state, so that underlying processes // can be clustered to gg > h if ( mergingHooksPtr->getProcessString().compare("pp>h") == 0) mergingHooksPtr->allowCutOnRecState(true); // Prepare process record for merging. If Pythia has already decayed // resonances used to define the hard process, remove resonance decay // products. Event newProcess( mergingHooksPtr->bareEvent( process, true) ); // Store candidates for the splitting V -> qqbar' mergingHooksPtr->storeHardProcessCandidates( newProcess ); // Check if event passes the merging scale cut. double tmsval = mergingHooksPtr->tms(); // Get merging scale in current event. double tmsnow = mergingHooksPtr->tmsNow( newProcess ); // Calculate number of clustering steps int nSteps = mergingHooksPtr->getNumberOfClusteringSteps( newProcess); // Reset the minimal tms value, if necessary. tmsNowMin = (nSteps == 0) ? 0. : min(tmsNowMin, tmsnow); // Potentially recluster real emission jets for powheg input containing // "too many" jets, i.e. real-emission kinematics. bool containsRealKin = nSteps > nRequested && nSteps > 0; // Get random number to choose a path. double RN = rndmPtr->flat(); // Set dummy process scale. newProcess.scale(0.0); // Generate all histories History FullHistory( nSteps, 0.0, newProcess, Clustering(), mergingHooksPtr, (*beamAPtr), (*beamBPtr), particleDataPtr, infoPtr, true, true, true, true, 1.0, 0); // Project histories onto desired branches, e.g. only ordered paths. FullHistory.projectOntoDesiredHistories(); // Remove real emission events without underlying Born configuration from // the loop sample, since such states will be taken care of by tree-level // samples. if ( containsRealKin && FullHistory.select(RN)->nClusterings() == 0 ) return true; // Do not apply cut if the configuration could not be projected onto an // underlying born configuration. if ( nSteps > 0 && FullHistory.select(RN)->nClusterings() == 0 ) return false; // Now enfore merging scale cut if the event did not pass the merging scale // criterion. if ( nSteps > 0 && nSteps == nRequested && tmsnow < tmsval ) { string message="Warning in Merging::cutOnProcess: Les Houches Event"; message+=" fails merging scale cut. Reject event."; infoPtr->errorMsg(message); return true; } // Cut if no history passes the cut on the lowest-multiplicity state. double dampWeight = mergingHooksPtr->dampenIfFailCuts( FullHistory.lowestMultProc(RN) ); if ( dampWeight == 0. ) return true; // Done if no real-emission jets are present. if ( !containsRealKin ) return false; // Now cut on events that contain an additional real-emission jet. // Perform one reclustering for real emission kinematics, then apply merging // scale cut on underlying Born kinematics. if ( containsRealKin ) { Event dummy = Event(); // Initialise temporary output of reclustering. dummy.clear(); dummy.init( "(hard process-modified)", particleDataPtr ); dummy.clear(); // Recluster once. FullHistory.getClusteredEvent( RN, nSteps, dummy ); double tnowNew = mergingHooksPtr->tmsNow( dummy ); // Veto if underlying Born kinematics do not pass merging scale cut. if ( nSteps > 0 && nRequested > 0 && tnowNew < tmsval ) return true; } // Done if only interested in cross section estimate after cuts. return false; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/Event.cc0000644000175000017500000011432412217346245014523 0ustar sunsun// Event.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // Particle and Event classes, and some related global functions. #include "Pythia8/Event.h" namespace Pythia8 { //========================================================================== // Particle class. // This class holds info on a particle in general. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Small number to avoid division by zero. const double Particle::TINY = 1e-20; //-------------------------------------------------------------------------- // Set pointer to the particle data species of the particle. void Particle::setPDEPtr(ParticleDataEntry* pdePtrIn) { pdePtr = pdePtrIn; if (pdePtrIn != 0 || evtPtr == 0) return; pdePtr = (*evtPtr).particleDataPtr->particleDataEntryPtr( idSave);} //-------------------------------------------------------------------------- // Functions for rapidity and pseudorapidity. double Particle::y() const { double temp = log( ( pSave.e() + abs(pSave.pz()) ) / max( TINY, mT() ) ); return (pSave.pz() > 0) ? temp : -temp; } double Particle::eta() const { double temp = log( ( pSave.pAbs() + abs(pSave.pz()) ) / max( TINY, pT() ) ); return (pSave.pz() > 0) ? temp : -temp; } //-------------------------------------------------------------------------- // Method to find the index of the particle in the event record. int Particle::index() const { if (evtPtr == 0) return -1; return (long(this) - long(&((*evtPtr)[0]))) / sizeof(Particle); } //-------------------------------------------------------------------------- // Convert internal Pythia status codes to the HepMC status conventions. int Particle::statusHepMC() const { // Positive codes are final particles. Status -12 are beam particles. if (statusSave > 0) return 1; if (statusSave == -12) return 4; if (evtPtr == 0) return 0; // Hadrons, muons, taus that decay normally are status 2. if (isHadron() || abs(idSave) == 13 || abs(idSave) == 15) { // Particle should not decay into itself (e.g. Bose-Einstein). if ( (*evtPtr)[daughter1Save].id() != idSave) { int statusDau = (*evtPtr)[daughter1Save].statusAbs(); if (statusDau > 90 && statusDau < 95) return 2; } } // Other acceptable negative codes as their positive counterpart. if (statusSave <= -11 && statusSave >= -200) return -statusSave; // Unacceptable codes as 0. return 0; } //-------------------------------------------------------------------------- // Trace the first and last copy of one and the same particle. int Particle::iTopCopy() const { if (evtPtr == 0) return -1; int iUp = index(); while ( iUp > 0 && (*evtPtr)[iUp].mother2() == (*evtPtr)[iUp].mother1() && (*evtPtr)[iUp].mother1() > 0) iUp = (*evtPtr)[iUp].mother1(); return iUp; } int Particle::iBotCopy() const { if (evtPtr == 0) return -1; int iDn = index(); while ( iDn > 0 && (*evtPtr)[iDn].daughter2() == (*evtPtr)[iDn].daughter1() && (*evtPtr)[iDn].daughter1() > 0) iDn = (*evtPtr)[iDn].daughter1(); return iDn; } //-------------------------------------------------------------------------- // Trace the first and last copy of one and the same particle, // also through shower branchings, making use of flavour matches. // Stops tracing when this gives ambiguities. int Particle::iTopCopyId() const { if (evtPtr == 0) return -1; int iUp = index(); for ( ; ; ) { int mother1up = (*evtPtr)[iUp].mother1(); int id1up = (mother1up > 0) ? (*evtPtr)[mother1up].id() : 0; int mother2up = (*evtPtr)[iUp].mother2(); int id2up = (mother2up > 0) ? (*evtPtr)[mother2up].id() : 0; if (mother2up != mother1up && id2up == id1up) break; if (id1up == idSave) { iUp = mother1up; continue; } if (id2up == idSave) { iUp = mother2up; continue; } break; } return iUp; } int Particle::iBotCopyId() const { if (evtPtr == 0) return -1; int iDn = index(); for ( ; ; ) { int daughter1dn = (*evtPtr)[iDn].daughter1(); int id1dn = (daughter1dn > 0) ? (*evtPtr)[daughter1dn].id() : 0; int daughter2dn = (*evtPtr)[iDn].daughter2(); int id2dn = (daughter2dn > 0) ? (*evtPtr)[daughter2dn].id() : 0; if (daughter2dn != daughter1dn && id2dn == id1dn) break; if (id1dn == idSave) { iDn = daughter1dn; continue; } if (id2dn == idSave) { iDn = daughter2dn; continue; } break; } return iDn; } //-------------------------------------------------------------------------- // Find complete list of mothers. vector Particle::motherList() const { // Vector of all the mothers; created empty. Done if no event pointer. vector motherVec; if (evtPtr == 0) return motherVec; // Special cases in the beginning, where the meaning of zero is unclear. int statusSaveAbs = abs(statusSave); if (statusSaveAbs == 11 || statusSaveAbs == 12) ; else if (mother1Save == 0 && mother2Save == 0) motherVec.push_back(0); // One mother or a carbon copy else if (mother2Save == 0 || mother2Save == mother1Save) motherVec.push_back(mother1Save); // A range of mothers from string fragmentation. else if ( (statusSaveAbs > 80 && statusSaveAbs < 90) || (statusSaveAbs > 100 && statusSaveAbs < 107) ) for (int iRange = mother1Save; iRange <= mother2Save; ++iRange) motherVec.push_back(iRange); // Two separate mothers. else { motherVec.push_back( min(mother1Save, mother2Save) ); motherVec.push_back( max(mother1Save, mother2Save) ); } // Done. return motherVec; } //-------------------------------------------------------------------------- // Find complete list of daughters. vector Particle::daughterList() const { // Vector of all the daughters; created empty. Done if no event pointer. vector daughterVec; if (evtPtr == 0) return daughterVec; // Simple cases: no or one daughter. if (daughter1Save == 0 && daughter2Save == 0) ; else if (daughter2Save == 0 || daughter2Save == daughter1Save) daughterVec.push_back(daughter1Save); // A range of daughters. else if (daughter2Save > daughter1Save) for (int iRange = daughter1Save; iRange <= daughter2Save; ++iRange) daughterVec.push_back(iRange); // Two separated daughters. else { daughterVec.push_back(daughter2Save); daughterVec.push_back(daughter1Save); } // Special case for two incoming beams: attach further // initiators and remnants that have beam as mother. if (abs(statusSave) == 12 || abs(statusSave) == 13) { int i = index(); for (int iDau = i + 1; iDau < evtPtr->size(); ++iDau) if ((*evtPtr)[iDau].mother1() == i) { bool isIn = false; for (int iIn = 0; iIn < int(daughterVec.size()); ++iIn) if (iDau == daughterVec[iIn]) isIn = true; if (!isIn) daughterVec.push_back(iDau); } } // Done. return daughterVec; } //-------------------------------------------------------------------------- // Find complete list of sisters. Optionally traces up with iTopCopy // and down with iBotCopy to give sisters at same level of evolution. vector Particle::sisterList(bool traceTopBot) const { // Vector of all the sisters; created empty. vector sisterVec; if (evtPtr == 0 || abs(statusSave) == 11) return sisterVec; // Find all daughters of the mother. int iUp = (traceTopBot) ? iTopCopy() : index(); int iMother = (*evtPtr)[iUp].mother1(); vector daughterVec = (*evtPtr)[iMother].daughterList(); // Copy all daughters, excepting the input particle itself. for (int j = 0; j < int(daughterVec.size()); ++j) { int iDau = daughterVec[j]; if (iDau != iUp) { int iDn = (traceTopBot) ? (*evtPtr)[iDau].iBotCopy() : iDau; sisterVec.push_back( iDn); } } // Done. return sisterVec; } //-------------------------------------------------------------------------- // Check whether a given particle is an arbitrarily-steps-removed // mother to another. For the parton -> hadron transition, only // first-rank hadrons are associated with the respective end quark. bool Particle::isAncestor(int iAncestor) const { // Begin loop to trace upwards from the daughter. if (evtPtr == 0) return false; int iUp = index(); int sizeNow = (*evtPtr).size(); for ( ; ; ) { // If positive match then done. if (iUp == iAncestor) return true; // If out of range then failed to find match. if (iUp <= 0 || iUp > sizeNow) return false; // If unique mother then keep on moving up the chain. int mother1up = (*evtPtr)[iUp].mother1(); int mother2up = (*evtPtr)[iUp].mother2(); if (mother2up == mother1up || mother2up == 0) {iUp = mother1up; continue;} // If many mothers, except hadronization, then fail tracing. int statusUp = (*evtPtr)[iUp].statusAbs(); if (statusUp < 81 || statusUp > 86) return false; // For hadronization step, fail if not first rank, else move up. if (statusUp == 82) { iUp = (iUp + 1 < sizeNow && (*evtPtr)[iUp + 1].mother1() == mother1up) ? mother1up : mother2up; continue; } if (statusUp == 83) { if ((*evtPtr)[iUp - 1].mother1() == mother1up) return false; iUp = mother1up; continue; } if (statusUp == 84) { if (iUp + 1 < sizeNow && (*evtPtr)[iUp + 1].mother1() == mother1up) return false; iUp = mother1up; continue; } // Fail for ministring -> one hadron and for junctions. return false; } // End of loop. Should never reach beyond here. return false; } //-------------------------------------------------------------------------- // Recursively remove the decay products of a particle, update it to be // undecayed, and update all mother/daughter indices to be correct. // Warning: assumes that decay chains are nicely ordered. bool Particle::undoDecay() { // Do not remove daughters of a parton, i.e. entry carrying colour. if (evtPtr == 0) return false; int i = index(); if (i < 0 || i >= int((*evtPtr).size())) return false; if (colSave != 0 || acolSave != 0) return false; // Find range of daughters to remove. int dau1 = daughter1Save; if (dau1 == 0) return false; int dau2 = daughter2Save; if (dau2 == 0) dau2 = dau1; // Refuse if any of the daughters have other mothers. for (int j = dau1; j <= dau2; ++j) if ((*evtPtr)[j].mother1() != i || ((*evtPtr)[j].mother2() != i && (*evtPtr)[j].mother2() != 0) ) return false; // Initialize range arrays for daughters and granddaughters. vector dauBeg, dauEnd; dauBeg.push_back( dau1); dauEnd.push_back( dau2); // Begin recursive search through all decay chains. int iRange = 0; do { for (int j = dauBeg[iRange]; j <= dauEnd[iRange]; ++j) if ((*evtPtr)[j].status() < 0) { // Find new daughter range, if present. dau1 = (*evtPtr)[j].daughter1(); if (dau1 == 0) return false; dau2 = (*evtPtr)[j].daughter2(); if (dau2 == 0) dau2 = dau1; // Check if the range duplicates or contradicts existing ones. bool isNew = true; for (int iR = 0; iR < int(dauBeg.size()); ++iR) { if (dau1 == dauBeg[iR] && dau2 == dauEnd[iR]) isNew = false; else if (dau1 >= dauBeg[iR] && dau1 <= dauEnd[iR]) return false; else if (dau2 >= dauBeg[iR] && dau2 <= dauEnd[iR]) return false; } // Add new range where relevant. Keep ranges ordered. if (isNew) { dauBeg.push_back( dau1); dauEnd.push_back( dau2); for (int iR = int(dauBeg.size()) - 1; iR > 0; --iR) { if (dauBeg[iR] < dauBeg[iR - 1]) { swap( dauBeg[iR], dauBeg[iR - 1]); swap( dauEnd[iR], dauEnd[iR - 1]); } else break; } } // End of recursive search all decay chains. } } while (++iRange < int(dauBeg.size())); // Join adjacent ranges to reduce number of erase steps. if (int(dauBeg.size()) > 1) { int iRJ = 0; do { if (dauEnd[iRJ] + 1 == dauBeg[iRJ + 1]) { for (int iRB = iRJ + 1; iRB < int(dauBeg.size()) - 1; ++iRB) dauBeg[iRB] = dauBeg[iRB + 1]; for (int iRE = iRJ; iRE < int(dauEnd.size()) - 1; ++iRE) dauEnd[iRE] = dauEnd[iRE + 1]; dauBeg.pop_back(); dauEnd.pop_back(); } else ++iRJ; } while (iRJ < int(dauBeg.size()) - 1); } // Iterate over relevant ranges, from bottom up. for (int iR = int(dauBeg.size()) - 1; iR >= 0; --iR) { dau1 = dauBeg[iR]; dau2 = dauEnd[iR]; int nRem = dau2 - dau1 + 1; // Remove daughters in each range. (*evtPtr).remove( dau1, dau2); // Update subsequent history to account for removed indices. for (int j = 0; j < int((*evtPtr).size()); ++j) { if ((*evtPtr)[j].mother1() > dau2) (*evtPtr)[j].mother1( (*evtPtr)[j].mother1() - nRem ); if ((*evtPtr)[j].mother2() > dau2) (*evtPtr)[j].mother2( (*evtPtr)[j].mother2() - nRem ); if ((*evtPtr)[j].daughter1() > dau2) (*evtPtr)[j].daughter1( (*evtPtr)[j].daughter1() - nRem ); if ((*evtPtr)[j].daughter2() > dau2) (*evtPtr)[j].daughter2( (*evtPtr)[j].daughter2() - nRem ); } } // Update mother that has been undecayed. statusSave = abs(statusSave); daughter1Save = 0; daughter2Save = 0; // Done. return true; } //-------------------------------------------------------------------------- // Particle name, with status but imposed maximum length -> may truncate. string Particle::nameWithStatus(int maxLen) const { if (pdePtr == 0) return " "; string temp = (statusSave > 0) ? pdePtr->name(idSave) : "(" + pdePtr->name(idSave) + ")"; while (int(temp.length()) > maxLen) { // Remove from end, excluding closing bracket and charge. int iRem = temp.find_last_not_of(")+-0"); temp.erase(iRem, 1); } return temp; } //-------------------------------------------------------------------------- // Add offsets to mother and daughter pointers (must be non-negative). void Particle::offsetHistory( int minMother, int addMother, int minDaughter, int addDaughter) { if (addMother < 0 || addDaughter < 0) return; if ( mother1Save > minMother ) mother1Save += addMother; if ( mother2Save > minMother ) mother2Save += addMother; if (daughter1Save > minDaughter) daughter1Save += addDaughter; if (daughter2Save > minDaughter) daughter2Save += addDaughter; } //-------------------------------------------------------------------------- // Add offsets to colour and anticolour (must be positive). void Particle::offsetCol( int addCol) { if (addCol < 0) return; if ( colSave > 0) colSave += addCol; if (acolSave > 0) acolSave += addCol; } //-------------------------------------------------------------------------- // Invariant mass of a pair and its square. // (Not part of class proper, but tightly linked.) double m(const Particle& pp1, const Particle& pp2) { double m2 = pow2(pp1.e() + pp2.e()) - pow2(pp1.px() + pp2.px()) - pow2(pp1.py() + pp2.py()) - pow2(pp1.pz() + pp2.pz()); return (m2 > 0. ? sqrt(m2) : 0.); } double m2(const Particle& pp1, const Particle& pp2) { double m2 = pow2(pp1.e() + pp2.e()) - pow2(pp1.px() + pp2.px()) - pow2(pp1.py() + pp2.py()) - pow2(pp1.pz() + pp2.pz()); return m2; } //========================================================================== // Event class. // This class holds info on the complete event record. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Maxmimum number of mothers or daughter indices per line in listing. const int Event::IPERLINE = 20; //-------------------------------------------------------------------------- // Copy all information from one event record to another. Event& Event::operator=( const Event& oldEvent) { // Do not copy if same. if (this != &oldEvent) { // Reset all current info in the event. clear(); // Copy particle data table; needed for individual particles. particleDataPtr = oldEvent.particleDataPtr; // Copy all the particles one by one. for (int i = 0; i < oldEvent.size(); ++i) append( oldEvent[i] ); // Copy all the junctions one by one. for (int i = 0; i < oldEvent.sizeJunction(); ++i) appendJunction( oldEvent.getJunction(i) ); // Copy all other values. startColTag = oldEvent.startColTag; maxColTag = oldEvent.maxColTag; savedSize = oldEvent.savedSize; savedJunctionSize = oldEvent.savedJunctionSize; scaleSave = oldEvent.scaleSave; scaleSecondSave = oldEvent.scaleSecondSave; headerList = oldEvent.headerList; // Done. } return *this; } //-------------------------------------------------------------------------- // Add a copy of an existing particle at the end of the event record; // return index. Three cases, depending on sign of new status code: // Positive: copy is viewed as daughter, status of original is negated. // Negative: copy is viewed as mother, status of original is unchanged. // Zero: the new is a perfect carbon copy (maybe to be changed later). int Event::copy(int iCopy, int newStatus) { // Protect against attempt to copy negative entries (e.g., junction codes) // or entries beyond end of record. if (iCopy < 0 || iCopy >= size()) return -1; // Simple carbon copy. entry.push_back(entry[iCopy]); int iNew = entry.size() - 1; // Set up to make new daughter of old. if (newStatus > 0) { entry[iCopy].daughters(iNew,iNew); entry[iCopy].statusNeg(); entry[iNew].mothers(iCopy, iCopy); entry[iNew].status(newStatus); // Set up to make new mother of old. } else if (newStatus < 0) { entry[iCopy].mothers(iNew,iNew); entry[iNew].daughters(iCopy, iCopy); entry[iNew].status(newStatus); } // Done. return iNew; } //-------------------------------------------------------------------------- // Print an event - special cases that rely on the general method. // Not inline to make them directly callable in (some) debuggers. void Event::list() const { list(false, false, cout); } void Event::list(ostream& os) const { list(false, false, os); } void Event::list(bool showScaleAndVertex, bool showMothersAndDaughters) const { list(showScaleAndVertex, showMothersAndDaughters, cout); } //-------------------------------------------------------------------------- // Print an event. void Event::list(bool showScaleAndVertex, bool showMothersAndDaughters, ostream& os) const { // Header. os << "\n -------- PYTHIA Event Listing " << headerList << "----------" << "-------------------------------------------------\n \n no " << " id name status mothers daughters colou" << "rs p_x p_y p_z e m \n"; if (showScaleAndVertex) os << " scale pol " << " xProd yProd zProd tProd " << " tau\n"; // At high energy switch to scientific format for momenta. bool useFixed = (entry[0].e() < 1e5); // Listing of complete event. Vec4 pSum; double chargeSum = 0.; for (int i = 0; i < int(entry.size()); ++i) { const Particle& pt = entry[i]; // Basic line for a particle, always printed. os << setw(6) << i << setw(10) << pt.id() << " " << left << setw(18) << pt.nameWithStatus(18) << right << setw(4) << pt.status() << setw(6) << pt.mother1() << setw(6) << pt.mother2() << setw(6) << pt.daughter1() << setw(6) << pt.daughter2() << setw(6) << pt.col() << setw(6) << pt.acol() << ( (useFixed) ? fixed : scientific ) << setprecision(3) << setw(11) << pt.px() << setw(11) << pt.py() << setw(11) << pt.pz() << setw(11) << pt.e() << setw(11) << pt.m() << "\n"; // Optional extra line for scale value, polarization and production vertex. if (showScaleAndVertex) os << " " << setw(11) << pt.scale() << " " << fixed << setprecision(3) << setw(11) << pt.pol() << " " << scientific << setprecision(3) << setw(11) << pt.xProd() << setw(11) << pt.yProd() << setw(11) << pt.zProd() << setw(11) << pt.tProd() << setw(11) << pt.tau() << "\n"; // Optional extra line, giving a complete list of mothers and daughters. if (showMothersAndDaughters) { int linefill = 2; os << " mothers:"; vector allMothers = motherList(i); for (int j = 0; j < int(allMothers.size()); ++j) { os << " " << allMothers[j]; if (++linefill == IPERLINE) {os << "\n "; linefill = 0;} } os << "; daughters:"; vector allDaughters = daughterList(i); for (int j = 0; j < int(allDaughters.size()); ++j) { os << " " << allDaughters[j]; if (++linefill == IPERLINE) {os << "\n "; linefill = 0;} } if (linefill !=0) os << "\n"; } // Extra blank separation line when each particle spans more than one line. if (showScaleAndVertex || showMothersAndDaughters) os << "\n"; // Statistics on momentum and charge. if (entry[i].status() > 0) { pSum += entry[i].p(); chargeSum += entry[i].charge(); } } // Line with sum charge, momentum, energy and invariant mass. os << fixed << setprecision(3) << " " << "Charge sum:" << setw(7) << chargeSum << " Momentum sum:" << ( (useFixed) ? fixed : scientific ) << setprecision(3) << setw(11) << pSum.px() << setw(11) << pSum.py() << setw(11) << pSum.pz() << setw(11) << pSum.e() << setw(11) << pSum.mCalc() << "\n"; // Listing finished. os << "\n -------- End PYTHIA Event Listing ----------------------------" << "-------------------------------------------------------------------" << endl; } //-------------------------------------------------------------------------- // Recursively remove the decay products of particle i, update it to be // undecayed, and update all mother/daughter indices to be correct. // Warning: assumes that decay chains are nicely ordered. bool Event::undoDecay(int i) { // Do not remove daughters of a parton, i.e. entry carrying colour. if (i < 0 || i >= int(entry.size())) return false; if (entry[i].col() != 0 || entry[i].acol() != 0) return false; // Find range of daughters to remove. int dau1 = entry[i].daughter1(); if (dau1 == 0) return false; int dau2 = entry[i].daughter2(); if (dau2 == 0) dau2 = dau1; // Refuse if any of the daughters have other mothers. for (int j = dau1; j <= dau2; ++j) if (entry[j].mother1() != i || (entry[j].mother2() != i && entry[j].mother2() != 0) ) return false; // Initialize range arrays for daughters and granddaughters. vector dauBeg, dauEnd; dauBeg.push_back( dau1); dauEnd.push_back( dau2); // Begin recursive search through all decay chains. int iRange = 0; do { for (int j = dauBeg[iRange]; j <= dauEnd[iRange]; ++j) if (entry[j].status() < 0) { // Find new daughter range, if present. dau1 = entry[j].daughter1(); if (dau1 == 0) return false; dau2 = entry[j].daughter2(); if (dau2 == 0) dau2 = dau1; // Check if the range duplicates or contradicts existing ones. bool isNew = true; for (int iR = 0; iR < int(dauBeg.size()); ++iR) { if (dau1 == dauBeg[iR] && dau2 == dauEnd[iR]) isNew = false; else if (dau1 >= dauBeg[iR] && dau1 <= dauEnd[iR]) return false; else if (dau2 >= dauBeg[iR] && dau2 <= dauEnd[iR]) return false; } // Add new range where relevant. Keep ranges ordered. if (isNew) { dauBeg.push_back( dau1); dauEnd.push_back( dau2); for (int iR = int(dauBeg.size()) - 1; iR > 0; --iR) { if (dauBeg[iR] < dauBeg[iR - 1]) { swap( dauBeg[iR], dauBeg[iR - 1]); swap( dauEnd[iR], dauEnd[iR - 1]); } else break; } } // End of recursive search all decay chains. } } while (++iRange < int(dauBeg.size())); // Join adjacent ranges to reduce number of erase steps. if (int(dauBeg.size()) > 1) { int iRJ = 0; do { if (dauEnd[iRJ] + 1 == dauBeg[iRJ + 1]) { for (int iRB = iRJ + 1; iRB < int(dauBeg.size()) - 1; ++iRB) dauBeg[iRB] = dauBeg[iRB + 1]; for (int iRE = iRJ; iRE < int(dauEnd.size()) - 1; ++iRE) dauEnd[iRE] = dauEnd[iRE + 1]; dauBeg.pop_back(); dauEnd.pop_back(); } else ++iRJ; } while (iRJ < int(dauBeg.size()) - 1); } // Iterate over relevant ranges, from bottom up. for (int iR = int(dauBeg.size()) - 1; iR >= 0; --iR) { dau1 = dauBeg[iR]; dau2 = dauEnd[iR]; int nRem = dau2 - dau1 + 1; // Remove daughters in each range. entry.erase( entry.begin() + dau1, entry.begin() + dau2 + 1); // Update subsequent history to account for removed indices. for (int j = 0; j < int(entry.size()); ++j) { if (entry[j].mother1() > dau2) entry[j].mother1( entry[j].mother1() - nRem ); if (entry[j].mother2() > dau2) entry[j].mother2( entry[j].mother2() - nRem ); if (entry[j].daughter1() > dau2) entry[j].daughter1( entry[j].daughter1() - nRem ); if (entry[j].daughter2() > dau2) entry[j].daughter2( entry[j].daughter2() - nRem ); } } // Update mother that has been undecayed. entry[i].statusPos(); entry[i].daughters(); // Done. return true; } //-------------------------------------------------------------------------- // Find complete list of mothers. vector Event::motherList(int i) const { // Vector of all the mothers; created empty. vector mothers; // Read out the two official mother indices and status code. int mother1 = entry[i].mother1(); int mother2 = entry[i].mother2(); int statusAbs = entry[i].statusAbs(); // Special cases in the beginning, where the meaning of zero is unclear. if (statusAbs == 11 || statusAbs == 12) ; else if (mother1 == 0 && mother2 == 0) mothers.push_back(0); // One mother or a carbon copy else if (mother2 == 0 || mother2 == mother1) mothers.push_back(mother1); // A range of mothers from string fragmentation. else if ( (statusAbs > 80 && statusAbs < 90) || (statusAbs > 100 && statusAbs < 107) ) for (int iRange = mother1; iRange <= mother2; ++iRange) mothers.push_back(iRange); // Two separate mothers. else { mothers.push_back( min(mother1, mother2) ); mothers.push_back( max(mother1, mother2) ); } // Done. return mothers; } //-------------------------------------------------------------------------- // Find complete list of daughters. vector Event::daughterList(int i) const { // Vector of all the daughters; created empty. vector daughters; // Read out the two official daughter indices. int daughter1 = entry[i].daughter1(); int daughter2 = entry[i].daughter2(); // Simple cases: no or one daughter. if (daughter1 == 0 && daughter2 == 0) ; else if (daughter2 == 0 || daughter2 == daughter1) daughters.push_back(daughter1); // A range of daughters. else if (daughter2 > daughter1) for (int iRange = daughter1; iRange <= daughter2; ++iRange) daughters.push_back(iRange); // Two separated daughters. else { daughters.push_back(daughter2); daughters.push_back(daughter1); } // Special case for two incoming beams: attach further // initiators and remnants that have beam as mother. if (entry[i].statusAbs() == 12 || entry[i].statusAbs() == 13) for (int iDau = i + 1; iDau < size(); ++iDau) if (entry[iDau].mother1() == i) { bool isIn = false; for (int iIn = 0; iIn < int(daughters.size()); ++iIn) if (iDau == daughters[iIn]) isIn = true; if (!isIn) daughters.push_back(iDau); } // Done. return daughters; } //-------------------------------------------------------------------------- // Convert internal Pythia status codes to the HepMC status conventions. int Event::statusHepMC(int i) const { // Positive codes are final particles. Status -12 are beam particles. int statusNow = entry[i].status(); if (statusNow > 0) return 1; if (statusNow == -12) return 4; // Hadrons, muons, taus that decay normally are status 2. int idNow = entry[i].id(); if (entry[i].isHadron() || abs(idNow) == 13 || abs(idNow) == 15) { int iDau = entry[i].daughter1(); // Particle should not decay into itself (e.g. Bose-Einstein). if ( entry[iDau].id() != idNow) { int statusDau = entry[ iDau ].statusAbs(); if (statusDau > 90 && statusDau < 95) return 2; } } // Other acceptable negative codes as their positive counterpart. if (statusNow <= -11 && statusNow >= -200) return -statusNow; // Unacceptable codes as 0. return 0; } //-------------------------------------------------------------------------- // Trace the first and last copy of one and the same particle. int Event::iTopCopy( int i) const { int iUp = i; while ( iUp > 0 && entry[iUp].mother2() == entry[iUp].mother1() && entry[iUp].mother1() > 0) iUp = entry[iUp].mother1(); return iUp; } int Event::iBotCopy( int i) const { int iDn = i; while ( iDn > 0 && entry[iDn].daughter2() == entry[iDn].daughter1() && entry[iDn].daughter1() > 0) iDn = entry[iDn].daughter1(); return iDn; } //-------------------------------------------------------------------------- // Trace the first and last copy of one and the same particle, // also through shower branchings, making use of flavour matches. // Stops tracing when this gives ambiguities. int Event::iTopCopyId( int i) const { int id = entry[i].id(); int iUp = i; for ( ; ; ) { int mother1 = entry[iUp].mother1(); int id1 = (mother1 > 0) ? entry[mother1].id() : 0; int mother2 = entry[iUp].mother2(); int id2 = (mother2 > 0) ? entry[mother2].id() : 0; if (mother2 != mother1 && id2 == id1) break; if (id1 == id) { iUp = mother1; continue; } if (id2 == id) { iUp = mother2; continue; } break; } return iUp; } int Event::iBotCopyId( int i) const { int id = entry[i].id(); int iDn = i; for ( ; ; ) { int daughter1 = entry[iDn].daughter1(); int id1 = (daughter1 > 0) ? entry[daughter1].id() : 0; int daughter2 = entry[iDn].daughter2(); int id2 = (daughter2 > 0) ? entry[daughter2].id() : 0; if (daughter2 != daughter1 && id2 == id1) break; if (id1 == id) { iDn = daughter1; continue; } if (id2 == id) { iDn = daughter2; continue; } break; } return iDn; } //-------------------------------------------------------------------------- // Find complete list of sisters. vector Event::sisterList(int i) const { // Vector of all the sisters; created empty. vector sisters; if (entry[i].statusAbs() == 11) return sisters; // Find mother and all its daughters. int iMother = entry[i].mother1(); vector daughters = daughterList(iMother); // Copy all daughters, excepting the input particle itself. for (int j = 0; j < int(daughters.size()); ++j) if (daughters[j] != i) sisters.push_back( daughters[j] ); // Done. return sisters; } //-------------------------------------------------------------------------- // Find complete list of sisters. Traces up with iTopCopy and // down with iBotCopy to give sisters at same level of evolution. // Should this not give any final particles, the search is widened. vector Event::sisterListTopBot(int i, bool widenSearch) const { // Vector of all the sisters; created empty. vector sisters; if (entry[i].statusAbs() == 11) return sisters; // Trace up to first copy of current particle. int iUp = iTopCopy(i); // Find mother and all its daughters. int iMother = entry[iUp].mother1(); vector daughters = daughterList(iMother); // Trace all daughters down, excepting the input particle itself. for (int jD = 0; jD < int(daughters.size()); ++jD) if (daughters[jD] != iUp) sisters.push_back( iBotCopy( daughters[jD] ) ); // Prune any non-final particles from list. int jP = 0; while (jP < int(sisters.size())) { if (entry[sisters[jP]].status() > 0) ++jP; else { sisters[jP] = sisters.back(); sisters.pop_back(); } } // If empty list then restore immediate daughters. if (sisters.size() == 0 && widenSearch) { for (int jR = 0; jR < int(daughters.size()); ++jR) if (daughters[jR] != iUp) sisters.push_back( iBotCopy( daughters[jR] ) ); // Then trace all daughters, not only bottom copy. for (int jT = 0; jT < int(sisters.size()); ++jT) { daughters = daughterList( sisters[jT] ); for (int k = 0; k < int(daughters.size()); ++k) sisters.push_back( daughters[k] ); } // And then prune any non-final particles from list. int jN = 0; while (jN < int(sisters.size())) { if (entry[sisters[jN]].status() > 0) ++jN; else { sisters[jN] = sisters.back(); sisters.pop_back(); } } } // Done. return sisters; } //-------------------------------------------------------------------------- // Check whether a given particle is an arbitrarily-steps-removed // mother to another. For the parton -> hadron transition, only // first-rank hadrons are associated with the respective end quark. bool Event::isAncestor(int i, int iAncestor) const { // Begin loop to trace upwards from the daughter. int iUp = i; for ( ; ; ) { // If positive match then done. if (iUp == iAncestor) return true; // If out of range then failed to find match. if (iUp <= 0 || iUp > size()) return false; // If unique mother then keep on moving up the chain. int mother1 = entry[iUp].mother1(); int mother2 = entry[iUp].mother2(); if (mother2 == mother1 || mother2 == 0) {iUp = mother1; continue;} // If many mothers, except hadronization, then fail tracing. int status = entry[iUp].statusAbs(); if (status < 81 || status > 86) return false; // For hadronization step, fail if not first rank, else move up. if (status == 82) { iUp = (iUp + 1 < size() && entry[iUp + 1].mother1() == mother1) ? mother1 : mother2; continue; } if (status == 83) { if (entry[iUp - 1].mother1() == mother1) return false; iUp = mother1; continue; } if (status == 84) { if (iUp + 1 < size() && entry[iUp + 1].mother1() == mother1) return false; iUp = mother1; continue; } // Fail for ministring -> one hadron and for junctions. return false; } // End of loop. Should never reach beyond here. return false; } //-------------------------------------------------------------------------- // Erase junction stored in specified slot and move up the ones under. void Event::eraseJunction(int i) { for (int j = i; j < int(junction.size()) - 1; ++j) junction[j] = junction[j + 1]; junction.pop_back(); } //-------------------------------------------------------------------------- // Print the junctions in an event. void Event::listJunctions(ostream& os) const { // Header. os << "\n -------- PYTHIA Junction Listing " << headerList.substr(0,30) << "\n \n no kind col0 col1 col2 " << "endc0 endc1 endc2 stat0 stat1 stat2\n"; // Loop through junctions in event and list them. for (int i = 0; i < sizeJunction(); ++i) os << setw(6) << i << setw(6) << kindJunction(i) << setw(6) << colJunction(i, 0) << setw(6) << colJunction(i, 1) << setw(6) << colJunction(i, 2) << setw(6) << endColJunction(i, 0) << setw(6) << endColJunction(i, 1) << setw(6) << endColJunction(i, 2) << setw(6) << statusJunction(i, 0) << setw(6) << statusJunction(i, 1) << setw(6) << statusJunction(i, 2) << "\n"; // Alternative if no junctions. Listing finished. if (sizeJunction() == 0) os << " no junctions present \n"; os << "\n -------- End PYTHIA Junction Listing --------------------" << "------" << endl; } //-------------------------------------------------------------------------- // Operator overloading allows to append one event to an existing one. Event& Event::operator+=( const Event& addEvent) { // Find offsets. One less since won't copy line 0. int offsetIdx = entry.size() - 1; int offsetCol = maxColTag; // Add energy to zeroth line and calculate new invariant mass. entry[0].p( entry[0].p() + addEvent[0].p() ); entry[0].m( entry[0].mCalc() ); // Read out particles from line 1 (not 0) onwards. Particle temp; for (int i = 1; i < addEvent.size(); ++i) { temp = addEvent[i]; // Add offset to nonzero mother, daughter and colour indices. if (temp.mother1() > 0) temp.mother1( temp.mother1() + offsetIdx ); if (temp.mother2() > 0) temp.mother2( temp.mother2() + offsetIdx ); if (temp.daughter1() > 0) temp.daughter1( temp.daughter1() + offsetIdx ); if (temp.daughter2() > 0) temp.daughter2( temp.daughter2() + offsetIdx ); if (temp.col() > 0) temp.col( temp.col() + offsetCol ); if (temp.acol() > 0) temp.acol( temp.acol() + offsetCol ); // Append particle to summed event. append( temp ); } // Read out junctions one by one. Junction tempJ; int begCol, endCol; for (int i = 0; i < addEvent.sizeJunction(); ++i) { tempJ = addEvent.getJunction(i); // Add colour offsets to all three legs. for (int j = 0; j < 3; ++j) { begCol = tempJ.col(j); endCol = tempJ.endCol(j); if (begCol > 0) begCol += offsetCol; if (endCol > 0) endCol += offsetCol; tempJ.cols( j, begCol, endCol); } // Append junction to summed event. appendJunction( tempJ ); } // Set header that indicates character as sum of events. headerList = "(combination of several events) -------"; // Done. return *this; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/UserHooks.cc0000644000175000017500000002365212217346252015365 0ustar sunsun// UserHooks.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the UserHooks class. // Note: compilation crashes if PhaseSpace.h is moved to UserHooks.h. #include "Pythia8/PhaseSpace.h" #include "Pythia8/UserHooks.h" namespace Pythia8 { //========================================================================== // The UserHooks class. //-------------------------------------------------------------------------- // multiplySigmaBy allows the user to introduce a multiplicative factor // that modifies the cross section of a hard process. Since it is called // from before the event record is generated in full, the normal analysis // does not work. The code here provides a rather extensive summary of // which methods actually do work. It is a convenient starting point for // writing your own derived routine. double UserHooks::multiplySigmaBy( const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool inEvent) { // Process code, necessary when some to be treated differently. //int code = sigmaProcessPtr->code(); // Final multiplicity, i.e. whether 2 -> 1 or 2 -> 2. //int nFinal = sigmaProcessPtr->nFinal(); // Incoming x1 and x2 to the hard collision, and factorization scale. //double x1 = phaseSpacePtr->x1(); //double x2 = phaseSpacePtr->x2(); //double Q2Fac = sigmaProcessPtr->Q2Fac(); // Renormalization scale and assumed alpha_strong and alpha_EM. //double Q2Ren = sigmaProcessPtr->Q2Ren(); //double alphaS = sigmaProcessPtr->alphaSRen(); //double alphaEM = sigmaProcessPtr->alphaEMRen(); // Subprocess mass-square. //double sHat = phaseSpacePtr->sHat(); // Now methods only relevant for 2 -> 2. //if (nFinal == 2) { // Mandelstam variables and hard-process pT. //double tHat = phaseSpacePtr->tHat(); //double uHat = phaseSpacePtr->uHat(); //double pTHat = phaseSpacePtr->pTHat(); // Masses of the final-state particles. (Here 0 for light quarks.) //double m3 = sigmaProcessPtr->m(3); //double m4 = sigmaProcessPtr->m(4); //} // Dummy statement to avoid compiler warnings. return ((inEvent && sigmaProcessPtr->code() == 0 && phaseSpacePtr->sHat() < 0.) ? 0. : 1.); } //-------------------------------------------------------------------------- // biasSelectionBy allows the user to introduce a multiplicative factor // that modifies the cross section of a hard process. The event is assigned // a wegith that is the inverse of the selection bias, such that the // cross section is unchanged. Since it is called from before the // event record is generated in full, the normal analysis does not work. // The code here provides a rather extensive summary of which methods // actually do work. It is a convenient starting point for writing // your own derived routine. double UserHooks::biasSelectionBy( const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool inEvent) { // Process code, necessary when some to be treated differently. //int code = sigmaProcessPtr->code(); // Final multiplicity, i.e. whether 2 -> 1 or 2 -> 2. //int nFinal = sigmaProcessPtr->nFinal(); // Incoming x1 and x2 to the hard collision, and factorization scale. //double x1 = phaseSpacePtr->x1(); //double x2 = phaseSpacePtr->x2(); //double Q2Fac = sigmaProcessPtr->Q2Fac(); // Renormalization scale and assumed alpha_strong and alpha_EM. //double Q2Ren = sigmaProcessPtr->Q2Ren(); //double alphaS = sigmaProcessPtr->alphaSRen(); //double alphaEM = sigmaProcessPtr->alphaEMRen(); // Subprocess mass-square. //double sHat = phaseSpacePtr->sHat(); // Now methods only relevant for 2 -> 2. //if (nFinal == 2) { // Mandelstam variables and hard-process pT. //double tHat = phaseSpacePtr->tHat(); //double uHat = phaseSpacePtr->uHat(); //double pTHat = phaseSpacePtr->pTHat(); // Masses of the final-state particles. (Here 0 for light quarks.) //double m3 = sigmaProcessPtr->m(3); //double m4 = sigmaProcessPtr->m(4); //} // Insert here your calculation of the selection bias. // Here illustrated by a weighting up of events at high pT. //selBias = pow4(phaseSpacePtr->pTHat()); // Return the selBias weight. // Warning: if you use another variable than selBias // the compensating weight will not be set correctly. //return selBias; // Dummy statement to avoid compiler warnings. return ((inEvent && sigmaProcessPtr->code() == 0 && phaseSpacePtr->sHat() < 0.) ? 0. : 1.); } //-------------------------------------------------------------------------- // omitResonanceDecays omits resonance decay chains from process record. void UserHooks::omitResonanceDecays(const Event& process, bool finalOnly) { // Reset work event to be empty workEvent.clear(); // Loop through all partons. Beam particles should be copied. for (int i = 0; i < process.size(); ++i) { bool doCopy = false; bool isFinal = false; if (i < 3) doCopy = true; // Daughters of beams should normally be copied. else { int iMother = process[i].mother1(); if (iMother == 1 || iMother == 2) doCopy = true; // Granddaughters of beams should normally be copied and are final. else if (iMother > 2) { int iGrandMother = process[iMother].mother1(); if (iGrandMother == 1 || iGrandMother == 2) { doCopy = true; isFinal = true; } } } // Optionally non-final are not copied. if (finalOnly && !isFinal) doCopy = false; // Do copying and modify status/daughters of final. if (doCopy) { int iNew = workEvent.append( process[i]); if (isFinal) { workEvent[iNew].statusPos(); workEvent[iNew].daughters( 0, 0); // When final only : no mothers; position in full event as daughters. if (finalOnly) { workEvent[iNew].mothers( 0, 0); workEvent[iNew].daughters( i, i); } } } } } //-------------------------------------------------------------------------- // subEvent extracts currently resolved partons in the hard process. void UserHooks::subEvent(const Event& event, bool isHardest) { // Reset work event to be empty. workEvent.clear(); // At the PartonLevel final partons are bookkept by subsystem. if (partonSystemsPtr->sizeSys() > 0) { // Find which subsystem to study. int iSys = 0; if (!isHardest) iSys = partonSystemsPtr->sizeSys() - 1; // Loop through all the final partons of the given subsystem. for (int i = 0; i < partonSystemsPtr->sizeOut(iSys); ++i) { int iOld = partonSystemsPtr->getOut( iSys, i); // Copy partons to work event. int iNew = workEvent.append( event[iOld]); // No mothers. Position in full event as daughters. workEvent[iNew].mothers( 0, 0); workEvent[iNew].daughters( iOld, iOld); } // At the ProcessLevel no subsystems have been defined. } else { // Loop through all partons, and copy all final ones. for (int iOld = 0; iOld < event.size(); ++iOld) if (event[iOld].isFinal()) { int iNew = workEvent.append( event[iOld]); // No mothers. Position in full event as daughters. workEvent[iNew].mothers( 0, 0); workEvent[iNew].daughters( iOld, iOld); } } } //========================================================================== // The SuppressSmallPT class, derived from UserHooks. //-------------------------------------------------------------------------- // Modify event weight at the trial level, before selection. double SuppressSmallPT::multiplySigmaBy( const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool ) { // Need to initialize first time this method is called. if (!isInit) { // Calculate pT0 as for multiparton interactions. // Fudge factor allows offset relative to MPI framework. double eCM = phaseSpacePtr->ecm(); double pT0Ref = settingsPtr->parm("MultipartonInteractions:pT0Ref"); double ecmRef = settingsPtr->parm("MultipartonInteractions:ecmRef"); double ecmPow = settingsPtr->parm("MultipartonInteractions:ecmPow"); double pT0 = pT0timesMPI * pT0Ref * pow(eCM / ecmRef, ecmPow); pT20 = pT0 * pT0; // Initialize alpha_strong object as for multiparton interactions, // alternatively as for hard processes. double alphaSvalue; int alphaSorder; int alphaSnfmax = settingsPtr->mode("StandardModel:alphaSnfmax"); if (useSameAlphaSasMPI) { alphaSvalue = settingsPtr->parm("MultipartonInteractions:alphaSvalue"); alphaSorder = settingsPtr->mode("MultipartonInteractions:alphaSorder"); } else { alphaSvalue = settingsPtr->parm("SigmaProcess:alphaSvalue"); alphaSorder = settingsPtr->mode("SigmaProcess:alphaSorder"); } alphaS.init( alphaSvalue, alphaSorder, alphaSnfmax, false); // Initialization finished. isInit = true; } // Only modify 2 -> 2 processes. int nFinal = sigmaProcessPtr->nFinal(); if (nFinal != 2) return 1.; // pT scale of process. Weight pT^4 / (pT^2 + pT0^2)^2 double pTHat = phaseSpacePtr->pTHat(); double pT2 = pTHat * pTHat; double wt = pow2( pT2 / (pT20 + pT2) ); if (numberAlphaS > 0) { // Renormalization scale and assumed alpha_strong. double Q2RenOld = sigmaProcessPtr->Q2Ren(); double alphaSOld = sigmaProcessPtr->alphaSRen(); // Reweight to new alpha_strong at new scale. double Q2RenNew = pT20 + Q2RenOld; double alphaSNew = alphaS.alphaS(Q2RenNew); wt *= pow( alphaSNew / alphaSOld, numberAlphaS); } // End weight calculation. return wt; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaQCD.cc0000644000175000017500000013366412217346251015037 0ustar sunsun// SigmaQCD.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // QCD simulation classes. #include "Pythia8/SigmaQCD.h" namespace Pythia8 { //========================================================================== // Sigma0AB2AB class. // Cross section for elastic scattering A B -> A B. //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma0AB2AB::setIdColAcol() { // Flavours and colours are trivial. setId( idA, idB, idA, idB); setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); } //========================================================================== // Sigma0AB2XB class. // Cross section for single diffractive scattering A B -> X B. //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma0AB2XB::setIdColAcol() { // Flavours and colours are trivial. int idX = 10* (abs(idA) / 10) + 9900000; if (idA < 0) idX = -idX; setId( idA, idB, idX, idB); setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); } //========================================================================== // Sigma0AB2AX class. // Cross section for single diffractive scattering A B -> A X. //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma0AB2AX::setIdColAcol() { // Flavours and colours are trivial. int idX = 10* (abs(idB) / 10) + 9900000; if (idB < 0) idX = -idX; setId( idA, idB, idA, idX); setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); } //========================================================================== // Sigma0AB2XX class. // Cross section for double diffractive scattering A B -> X X. //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma0AB2XX::setIdColAcol() { // Flavours and colours are trivial. int idX1 = 10* (abs(idA) / 10) + 9900000; if (idA < 0) idX1 = -idX1; int idX2 = 10* (abs(idB) / 10) + 9900000; if (idB < 0) idX2 = -idX2; setId( idA, idB, idX1, idX2); setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); } //========================================================================== // Sigma0AB2AXB class. // Cross section for central scattering A B -> A X B. //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma0AB2AXB::setIdColAcol() { // Central diffractive state represented by rho_diffr0. Colours trivial. int idX = 9900110; setId( idA, idB, idA, idB,idX); setColAcol( 0, 0, 0, 0, 0, 0, 0, 0, 0, 0); } //========================================================================== // Sigma2gg2gg class. // Cross section for g g -> g g. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2gg2gg::sigmaKin() { // Calculate kinematics dependence. sigTS = (9./4.) * (tH2 / sH2 + 2. * tH / sH + 3. + 2. * sH / tH + sH2 / tH2); sigUS = (9./4.) * (uH2 / sH2 + 2. * uH / sH + 3. + 2. * sH / uH + sH2 / uH2); sigTU = (9./4.) * (tH2 / uH2 + 2. * tH / uH + 3. + 2. * uH / tH + uH2 / tH2); sigSum = sigTS + sigUS + sigTU; // Answer contains factor 1/2 from identical gluons. sigma = (M_PI / sH2) * pow2(alpS) * 0.5 * sigSum; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2gg::setIdColAcol() { // Flavours are trivial. setId( id1, id2, 21, 21); // Three colour flow topologies, each with two orientations. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 2, 2, 3, 1, 4, 4, 3); else if (sigRand < sigTS + sigUS) setColAcol( 1, 2, 3, 1, 3, 4, 4, 2); else setColAcol( 1, 2, 3, 4, 1, 4, 3, 2); if (rndmPtr->flat() > 0.5) swapColAcol(); } //========================================================================== // Sigma2gg2qqbar class. // Cross section for g g -> q qbar (q = u, d, s, i.e. almost massless). //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2qqbar::initProc() { // Read number of quarks to be considered in massless approximation. nQuarkNew = settingsPtr->mode("HardQCD:nQuarkNew"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2gg2qqbar::sigmaKin() { // Pick new flavour. idNew = 1 + int( nQuarkNew * rndmPtr->flat() ); mNew = particleDataPtr->m0(idNew); m2New = mNew*mNew; // Calculate kinematics dependence. sigTS = 0.; sigUS = 0.; if (sH > 4. * m2New) { sigTS = (1./6.) * uH / tH - (3./8.) * uH2 / sH2; sigUS = (1./6.) * tH / uH - (3./8.) * tH2 / sH2; } sigSum = sigTS + sigUS; // Answer is proportional to number of outgoing flavours. sigma = (M_PI / sH2) * pow2(alpS) * nQuarkNew * sigSum; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2qqbar::setIdColAcol() { // Flavours are trivial. setId( id1, id2, idNew, -idNew); // Two colour flow topologies. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 2, 2, 3, 1, 0, 0, 3); else setColAcol( 1, 2, 3, 1, 3, 0, 0, 2); } //========================================================================== // Sigma2qg2qg class. // Cross section for q g -> q g. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2qg2qg::sigmaKin() { // Calculate kinematics dependence. sigTS = uH2 / tH2 - (4./9.) * uH / sH; sigTU = sH2 / tH2 - (4./9.) * sH / uH; sigSum = sigTS + sigTU; // Answer. sigma = (M_PI / sH2) * pow2(alpS) * sigSum; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2qg::setIdColAcol() { // Outgoing = incoming flavours. setId( id1, id2, id1, id2); // Two colour flow topologies. Swap if first is gluon, or when antiquark. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 0, 2, 1, 3, 0, 2, 3); else setColAcol( 1, 0, 2, 3, 2, 0, 1, 3); if (id1 == 21) swapCol1234(); if (id1 < 0 || id2 < 0) swapColAcol(); } //========================================================================== // Sigma2qq2qq class. // Cross section for q qbar' -> q qbar' or q q' -> q q' // (qbar qbar' -> qbar qbar'), q' may be same as q. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qq2qq::sigmaKin() { // Calculate kinematics dependence for different terms. sigT = (4./9.) * (sH2 + uH2) / tH2; sigU = (4./9.) * (sH2 + tH2) / uH2; sigTU = - (8./27.) * sH2 / (tH * uH); sigST = - (8./27.) * uH2 / (sH * tH); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qq2qq::sigmaHat() { // Combine cross section terms; factor 1/2 when identical quarks. if (id2 == id1) sigSum = 0.5 * (sigT + sigU + sigTU); else if (id2 == -id1) sigSum = sigT + sigST; else sigSum = sigT; // Answer. return (M_PI/sH2) * pow2(alpS) * sigSum; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qq2qq::setIdColAcol() { // Outgoing = incoming flavours. setId( id1, id2, id1, id2); // Colour flow topologies. Swap when antiquarks. if (id1 * id2 > 0) setColAcol( 1, 0, 2, 0, 2, 0, 1, 0); else setColAcol( 1, 0, 0, 1, 2, 0, 0, 2); if (id2 == id1 && (sigT + sigU) * rndmPtr->flat() > sigT) setColAcol( 1, 0, 2, 0, 1, 0, 2, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2gg class. // Cross section for q qbar -> g g. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2qqbar2gg::sigmaKin() { // Calculate kinematics dependence. sigTS = (32./27.) * uH / tH - (8./3.) * uH2 / sH2; sigUS = (32./27.) * tH / uH - (8./3.) * tH2 / sH2; sigSum = sigTS + sigUS; // Answer contains factor 1/2 from identical gluons. sigma = (M_PI / sH2) * pow2(alpS) * 0.5 * sigSum; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2gg::setIdColAcol() { // Outgoing flavours trivial. setId( id1, id2, 21, 21); // Two colour flow topologies. Swap if first is antiquark. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 0, 0, 2, 1, 3, 3, 2); else setColAcol( 1, 0, 0, 2, 3, 2, 1, 3); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2qqbarNew class. // Cross section q qbar -> q' qbar'. //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2qqbarNew::initProc() { // Read number of quarks to be considered in massless approximation. nQuarkNew = settingsPtr->mode("HardQCD:nQuarkNew"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2qqbar2qqbarNew::sigmaKin() { // Pick new flavour. idNew = 1 + int( nQuarkNew * rndmPtr->flat() ); mNew = particleDataPtr->m0(idNew); m2New = mNew*mNew; // Calculate kinematics dependence. sigS = 0.; if (sH > 4. * m2New) sigS = (4./9.) * (tH2 + uH2) / sH2; // Answer is proportional to number of outgoing flavours. sigma = (M_PI / sH2) * pow2(alpS) * nQuarkNew * sigS; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2qqbarNew::setIdColAcol() { // Set outgoing flavours ones. id3 = (id1 > 0) ? idNew : -idNew; setId( id1, id2, id3, -id3); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2gg2QQbar class. // Cross section g g -> Q Qbar (Q = c, b or t). // Only provided for fixed m3 = m4 so do some gymnastics: // i) s34Avg picked so that beta34 same when s3, s4 -> s34Avg. // ii) tHQ = tH - mQ^2 = -0.5 sH (1 - beta34 cos(thetaH)) for m3 = m4 = mQ, // but tH - uH = sH beta34 cos(thetaH) also for m3 != m4, so use // tH, uH selected for m3 != m4 to derive tHQ, uHQ valid for m3 = m4. //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2QQbar::initProc() { // Process name. nameSave = "g g -> Q Qbar"; if (idNew == 4) nameSave = "g g -> c cbar"; if (idNew == 5) nameSave = "g g -> b bbar"; if (idNew == 6) nameSave = "g g -> t tbar"; if (idNew == 7) nameSave = "g g -> b' b'bar"; if (idNew == 8) nameSave = "g g -> t' t'bar"; // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(idNew, -idNew); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2gg2QQbar::sigmaKin() { // Modified Mandelstam variables for massive kinematics with m3 = m4. double s34Avg = 0.5 * (s3 + s4) - 0.25 * pow2(s3 - s4) / sH; double tHQ = -0.5 * (sH - tH + uH); double uHQ = -0.5 * (sH + tH - uH); double tHQ2 = tHQ * tHQ; double uHQ2 = uHQ * uHQ; // Calculate kinematics dependence. double tumHQ = tHQ * uHQ - s34Avg * sH; sigTS = ( uHQ / tHQ - 2.25 * uHQ2 / sH2 + 4.5 * s34Avg * tumHQ / ( sH * tHQ2) + 0.5 * s34Avg * (tHQ + s34Avg) / tHQ2 - s34Avg*s34Avg / (sH * tHQ) ) / 6.; sigUS = ( tHQ / uHQ - 2.25 * tHQ2 / sH2 + 4.5 * s34Avg * tumHQ / ( sH * uHQ2) + 0.5 * s34Avg * (uHQ + s34Avg) / uHQ2 - s34Avg*s34Avg / (sH * uHQ) ) / 6.; sigSum = sigTS + sigUS; // Answer. sigma = (M_PI / sH2) * pow2(alpS) * sigSum * openFracPair; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2QQbar::setIdColAcol() { // Flavours are trivial. setId( id1, id2, idNew, -idNew); // Two colour flow topologies. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 2, 2, 3, 1, 0, 0, 3); else setColAcol( 1, 2, 3, 1, 3, 0, 0, 2); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles of W in top decay. double Sigma2gg2QQbar::weightDecay( Event& process, int iResBeg, int iResEnd) { // For top decay hand over to standard routine, else done. if (idNew == 6 && process[process[iResBeg].mother1()].idAbs() == 6) return weightTopDecay( process, iResBeg, iResEnd); else return 1.; } //========================================================================== // Sigma2qqbar2QQbar class. // Cross section q qbar -> Q Qbar (Q = c, b or t). // Only provided for fixed m3 = m4 so do some gymnastics: // i) s34Avg picked so that beta34 same when s3, s4 -> s34Avg. // ii) tHQ = tH - mQ^2 = -0.5 sH (1 - beta34 cos(thetaH)) for m3 = m4 = mQ, // but tH - uH = sH beta34 cos(thetaH) also for m3 != m4, so use // tH, uH selected for m3 != m4 to derive tHQ, uHQ valid for m3 = m4. //-------------------------------------------------------------------------- // Initialize process, especially parton-flux object. void Sigma2qqbar2QQbar::initProc() { // Process name. nameSave = "q qbar -> Q Qbar"; if (idNew == 4) nameSave = "q qbar -> c cbar"; if (idNew == 5) nameSave = "q qbar -> b bbar"; if (idNew == 6) nameSave = "q qbar -> t tbar"; if (idNew == 7) nameSave = "q qbar -> b' b'bar"; if (idNew == 8) nameSave = "q qbar -> t' t'bar"; // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(idNew, -idNew); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2qqbar2QQbar::sigmaKin() { // Modified Mandelstam variables for massive kinematics with m3 = m4. double s34Avg = 0.5 * (s3 + s4) - 0.25 * pow2(s3 - s4) / sH; double tHQ = -0.5 * (sH - tH + uH); double uHQ = -0.5 * (sH + tH - uH); double tHQ2 = tHQ * tHQ; double uHQ2 = uHQ * uHQ; // Calculate kinematics dependence. double sigS = (4./9.) * ((tHQ2 + uHQ2) / sH2 + 2. * s34Avg / sH); // Answer. sigma = (M_PI / sH2) * pow2(alpS) * sigS * openFracPair; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2QQbar::setIdColAcol() { // Set outgoing flavours. id3 = (id1 > 0) ? idNew : -idNew; setId( id1, id2, id3, -id3); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles of W in top decay. double Sigma2qqbar2QQbar::weightDecay( Event& process, int iResBeg, int iResEnd) { // For top decay hand over to standard routine, else done. if (idNew == 6 && process[process[iResBeg].mother1()].idAbs() == 6) return weightTopDecay( process, iResBeg, iResEnd); else return 1.; } //========================================================================== // Sigma3gg2ggg class. // Cross section for g g -> g g g. //-------------------------------------------------------------------------- // Evaluate |M|^2 - no incoming flavour dependence. void Sigma3gg2ggg::sigmaKin() { // Calculate all four-vector products. Vec4 p1cm( 0., 0., 0.5 * mH, 0.5 * mH); Vec4 p2cm( 0., 0., -0.5 * mH, 0.5 * mH); pp[1][2] = p1cm * p2cm; pp[1][3] = p1cm * p3cm; pp[1][4] = p1cm * p4cm; pp[1][5] = p1cm * p5cm; pp[2][3] = p2cm * p3cm; pp[2][4] = p2cm * p4cm; pp[2][5] = p2cm * p5cm; pp[3][4] = p3cm * p4cm; pp[3][5] = p3cm * p5cm; pp[4][5] = p4cm * p5cm; for (int i = 1; i < 5; ++i) for (int j = i + 1; j < 6; ++j) pp[j][i] = pp[i][j]; // Cross section, in three main sections. double num1 = cycle(1,2,3,4,5) + cycle(1,2,3,5,4) + cycle(1,2,4,3,5) + cycle(1,2,4,5,3) + cycle(1,2,5,3,4) + cycle(1,2,5,4,3) + cycle(1,3,2,4,5) + cycle(1,3,2,5,4) + cycle(1,3,4,2,5) + cycle(1,3,5,2,4) + cycle(1,4,2,3,5) + cycle(1,4,3,2,5); double num2 = pow4(pp[1][2]) + pow4(pp[1][3]) + pow4(pp[1][4]) + pow4(pp[1][5]) + pow4(pp[2][3]) + pow4(pp[2][4]) + pow4(pp[2][5]) + pow4(pp[3][4]) + pow4(pp[3][5]) + pow4(pp[4][5]); double den = pp[1][2] * pp[1][3] * pp[1][4] * pp[1][5] * pp[2][3] * pp[2][4] * pp[2][5] * pp[3][4] * pp[3][5] * pp[4][5]; // Answer has a factor 6 due to identical gluons // This is cancelled by phase space factor (1 / 6) sigma = pow3(4. * M_PI * alpS) * (27./16.) * num1 * num2 / den; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3gg2ggg::setIdColAcol() { // Flavours are trivial. setId( id1, id2, 21, 21, 21); // Three colour flow topologies, each with two orientations. /* double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 2, 2, 3, 1, 4, 4, 3); else if (sigRand < sigTS + sigUS) setColAcol( 1, 2, 3, 1, 3, 4, 4, 2); else setColAcol( 1, 2, 3, 4, 1, 4, 3, 2); if (rndmPtr->flat() > 0.5) swapColAcol(); */ // Temporary solution. setColAcol( 1, 2, 2, 3, 1, 4, 4, 5, 5, 3); } //========================================================================== // Sigma3qqbar2ggg class. // Cross section for q qbar -> g g g. //-------------------------------------------------------------------------- // Evaluate |M|^2 - no incoming flavour dependence. void Sigma3qqbar2ggg::sigmaKin() { // Setup four-vectors pCM[0] = Vec4( 0., 0., 0.5 * mH, 0.5 * mH); pCM[1] = Vec4( 0., 0., -0.5 * mH, 0.5 * mH); pCM[2] = p3cm; pCM[3] = p4cm; pCM[4] = p5cm; // Calculate |M|^2 // Answer has a factor 6 due to identical gluons, // which is cancelled by phase space factor (1 / 6) sigma = m2Calc(); } //-------------------------------------------------------------------------- // |M|^2 inline double Sigma3qqbar2ggg::m2Calc() { // Calculate four-products double sHnow = (pCM[0] + pCM[1]).m2Calc(); double sHhalf = sH / 2.; // qbar (p+) + q(p-) -> g(k1) g(k2) g(k3) // a_i = (p+ . ki), i = 1, 2, 3 // b_i = (p- . ki), i = 1, 2, 3 a[0] = pCM[0] * pCM[2]; a[1] = pCM[0] * pCM[3]; a[2] = pCM[0] * pCM[4]; b[0] = pCM[1] * pCM[2]; b[1] = pCM[1] * pCM[3]; b[2] = pCM[1] * pCM[4]; pp[0][1] = pCM[2] * pCM[3]; pp[1][2] = pCM[3] * pCM[4]; pp[2][0] = pCM[4] * pCM[2]; // ab[i][j] = a_i * b_j + a_j * b_i ab[0][1] = a[0] * b[1] + a[1] * b[0]; ab[1][2] = a[1] * b[2] + a[2] * b[1]; ab[2][0] = a[2] * b[0] + a[0] * b[2]; // Cross section double num1 = a[0] * b[0] * (a[0] * a[0] + b[0] * b[0]) + a[1] * b[1] * (a[1] * a[1] + b[1] * b[1]) + a[2] * b[2] * (a[2] * a[2] + b[2] * b[2]); double den1 = a[0] * a[1] * a[2] * b[0] * b[1] * b[2]; double num2 = - ( ab[0][1] / pp[0][1] ) - ( ab[1][2] / pp[1][2] ) - ( ab[2][0] / pp[2][0] ); double num3 = a[2] * b[2] * ab[0][1] / (pp[1][2] * pp[2][0] ) + a[0] * b[0] * ab[1][2] / (pp[2][0] * pp[0][1] ) + a[1] * b[1] * ab[2][0] / (pp[0][1] * pp[1][2] ); // Final answer return pow3(4. * M_PI * alpS) * (8. / 324.) * (num1 / den1) * ( sHhalf + 9. * (sHhalf + num2) + (2. * 81. / sHnow) * num3 ); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3qqbar2ggg::setIdColAcol(){ // Flavours are trivial. setId( id1, id2, 21, 21, 21); // Temporary solution. setColAcol( 1, 0, 0, 2, 1, 3, 3, 4, 4, 2); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Map a final state configuration inline void Sigma3qqbar2ggg::mapFinal() { switch (config) { case 0: pCM[2] = p3cm; pCM[3] = p4cm; pCM[4] = p5cm; break; case 1: pCM[2] = p3cm; pCM[3] = p5cm; pCM[4] = p4cm; break; case 2: pCM[2] = p4cm; pCM[3] = p3cm; pCM[4] = p5cm; break; case 3: pCM[2] = p4cm; pCM[3] = p5cm; pCM[4] = p3cm; break; case 4: pCM[2] = p5cm; pCM[3] = p3cm; pCM[4] = p4cm; break; case 5: pCM[2] = p5cm; pCM[3] = p4cm; pCM[4] = p3cm; break; } } //========================================================================== // Sigma3qg2qgg class. // Cross section for q g -> q g g. // Crossed relation from q qbar -> g g g: // qbar(p+) q(p-) -> g(k1) g(k2) g(k3) //-------------------------------------------------------------------------- // Evaluate |M|^2 - no incoming flavour dependence // Note: two different contributions from gq and qg incoming void Sigma3qg2qgg::sigmaKin() { // Pick a final state configuration pickFinal(); // gq and qg incoming for (int i = 0; i < 2; i++) { // Map incoming four-vectors to p+, p-, k1, k2, k3 pCM[0] = Vec4( 0., 0., 0.5 * mH, 0.5 * mH); pCM[1] = Vec4( 0., 0., -0.5 * mH, 0.5 * mH); mapFinal(); // Crossing swap(pCM[i], pCM[2]); // |M|^2 // XXX - Extra factor of (3) from selecting a final state // configuration (already a factor of 2 in the original // answer due to two identical final state gluons)??? // Extra factor of (3 / 8) as average over incoming gluon sigma[i] = 3. * (3. / 8.) * m2Calc(); } // for (int i = 0; i < 2; i++) } //-------------------------------------------------------------------------- // Evaluate |M|^2 - incoming flavour dependence // Pick from two configurations calculated previously double Sigma3qg2qgg::sigmaHat() { // gq or qg incoming return (id1 == 21) ? sigma[0] : sigma[1]; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3qg2qgg::setIdColAcol(){ // Outgoing flavours; only need to know where the quark is int qIdx = config / 2; int idTmp[3] = { 21, 21, 21 }; idTmp[qIdx] = (id1 == 21) ? id2 : id1; setId( id1, id2, idTmp[0], idTmp[1], idTmp[2]); // Temporary solution if (qIdx == 0) setColAcol(1, 0, 2, 1, 4, 0, 3, 4, 2, 3); else if (qIdx == 1) setColAcol(1, 0, 2, 1, 3, 4, 4, 0, 2, 3); else setColAcol(1, 0, 2, 1, 3, 4, 2, 3, 4, 0); // gq or qg incoming if (id1 == 21) { swap( colSave[1], colSave[2]); swap(acolSave[1], acolSave[2]); } // qbar rather than q incoming if (id1 < 0 || id2 < 0) swapColAcol(); } //========================================================================== // Sigma3gg2qqbarg class. // Cross section for g g -> q qbar g // Crossed relation from q qbar -> g g g //-------------------------------------------------------------------------- // Initialize process. void Sigma3gg2qqbarg::initProc() { // Read number of quarks to be considered in massless approximation. nQuarkNew = settingsPtr->mode("HardQCD:nQuarkNew"); } //-------------------------------------------------------------------------- // Evaluate |M|^2 - no incoming flavour dependence. void Sigma3gg2qqbarg::sigmaKin() { // Incoming four-vectors pCM[0] = Vec4( 0., 0., 0.5 * mH, 0.5 * mH); pCM[1] = Vec4( 0., 0., -0.5 * mH, 0.5 * mH); // Pick and map a final state configuration pickFinal(); mapFinal(); // Crossing swap(pCM[0], pCM[2]); swap(pCM[1], pCM[3]); // |M|^2 // Extra factor of (6.) from picking a final state configuration // Extra factor of nQuarkNew // Extra factor of (3. / 8.) ^ 2 as averaging over two incoming gluons sigma = 6. * nQuarkNew * (3. / 8.) * (3. / 8.) * m2Calc(); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3gg2qqbarg::setIdColAcol(){ // Pick new flavour int idNew = 1 + int( nQuarkNew * rndmPtr->flat() ); // Outgoing flavours; easiest just to map by hand switch (config) { case 0: id3 = idNew; id4 = -idNew; id5 = 21; break; case 1: id3 = idNew; id4 = 21; id5 = -idNew; break; case 2: id3 = -idNew; id4 = idNew; id5 = 21; break; case 3: id3 = 21; id4 = idNew; id5 = -idNew; break; case 4: id3 = -idNew; id4 = 21; id5 = idNew; break; case 5: id3 = 21; id4 = -idNew; id5 = idNew; break; } setId(id1, id2, id3, id4, id5); // Temporary solution switch (config) { case 0: setColAcol( 1, 2, 2, 3, 4, 0, 0, 3, 1, 4 ); break; case 1: setColAcol( 1, 2, 2, 3, 4, 0, 1, 4, 0, 3 ); break; case 2: setColAcol( 1, 2, 2, 3, 0, 3, 4, 0, 1, 4 ); break; case 3: setColAcol( 1, 2, 2, 3, 1, 4, 4, 0, 0, 3 ); break; case 4: setColAcol( 1, 2, 2, 3, 0, 3, 1, 4, 4, 0 ); break; case 5: setColAcol( 1, 2, 2, 3, 1, 4, 0, 3, 4, 0 ); break; } } //========================================================================== // Sigma3qq2qqgDiff class. // Cross section for q q' -> q q' g, q != q' //-------------------------------------------------------------------------- // Evaluate |M|^2 - no incoming flavour dependence void Sigma3qq2qqgDiff::sigmaKin() { // q1(p+) q2(p-) -> q1(q+) q2(q-) g(k) // Incoming four-vectors pCM[0] = Vec4( 0., 0., 0.5 * mH, 0.5 * mH); pCM[1] = Vec4( 0., 0., -0.5 * mH, 0.5 * mH); // Pick and map a final state configuration pickFinal(); mapFinal(); // |M|^2 // Extra factor of (6.) from picking a final state configuration sigma = 6. * m2Calc(); } //-------------------------------------------------------------------------- // |M|^2 inline double Sigma3qq2qqgDiff::m2Calc() { // Four-products s = (pCM[0] + pCM[1]).m2Calc(); t = (pCM[0] - pCM[2]).m2Calc(); u = (pCM[0] - pCM[3]).m2Calc(); up = (pCM[1] - pCM[2]).m2Calc(); sp = (pCM[2] + pCM[3]).m2Calc(); tp = (pCM[1] - pCM[3]).m2Calc(); // |M|^2 double num1 = (s * s + sp * sp + u * u + up * up) / (t * tp); double den1 = (pCM[0] * pCM[4]) * (pCM[1] * pCM[4]) * (pCM[2] * pCM[4]) * (pCM[3] * pCM[4]); double num2 = (u + up) * (s * sp + t * tp - u * up) + u * (s * t + sp * tp) + up * (s * tp + sp * t); double num3 = (s + sp) * (s * sp - t * tp - u * up) + 2. * t * tp * (u + up) + 2. * u * up * (t + tp); // (N^2 - 1)^2 / 4N^3 = 16. / 27. // (N^2 - 1) / 4N^3 = 2. / 27. return (1. / 8.) * pow3(4. * M_PI * alpS) * num1 / den1 * ( (16. / 27.) * num2 - (2. / 27.) * num3 ); } //-------------------------------------------------------------------------- // Evaluate |M|^2 - incoming flavour dependence double Sigma3qq2qqgDiff::sigmaHat() { // Different incoming flavours only if (abs(id1) == abs(id2)) return 0.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3qq2qqgDiff::setIdColAcol(){ // Outgoing flavours; easiest just to map by hand switch (config) { case 0: id3 = id1; id4 = id2; id5 = 21; break; case 1: id3 = id1; id4 = 21; id5 = id2; break; case 2: id3 = id2; id4 = id1; id5 = 21; break; case 3: id3 = 21; id4 = id1; id5 = id2; break; case 4: id3 = id2; id4 = 21; id5 = id1; break; case 5: id3 = 21; id4 = id2; id5 = id1; break; } setId(id1, id2, id3, id4, id5); // Temporary solution; id1 and id2 can be q/qbar independently int cols[5][2]; if (id1 > 0) { cols[0][0] = 1; cols[0][1] = 0; cols[2][0] = 1; cols[2][1] = 0; } else { cols[0][0] = 0; cols[0][1] = 1; cols[2][0] = 0; cols[2][1] = 1; } if (id2 > 0) { cols[1][0] = 2; cols[1][1] = 0; cols[3][0] = 3; cols[3][1] = 0; cols[4][0] = 2; cols[4][1] = 3; } else { cols[1][0] = 0; cols[1][1] = 2; cols[3][0] = 0; cols[3][1] = 3; cols[4][0] = 3; cols[4][1] = 2; } // Map correct final state configuration int i3 = 0, i4 = 0, i5 = 0; switch (config) { case 0: i3 = 2; i4 = 3; i5 = 4; break; case 1: i3 = 2; i4 = 4; i5 = 3; break; case 2: i3 = 3; i4 = 2; i5 = 4; break; case 3: i3 = 4; i4 = 2; i5 = 3; break; case 4: i3 = 3; i4 = 4; i5 = 2; break; case 5: i3 = 4; i4 = 3; i5 = 2; break; } // Put colours in place setColAcol(cols[0][0], cols[0][1], cols[1][0], cols[1][1], cols[i3][0], cols[i3][1], cols[i4][0], cols[i4][1], cols[i5][0], cols[i5][1]); } //-------------------------------------------------------------------------- // Map a final state configuration inline void Sigma3qq2qqgDiff::mapFinal() { switch (config) { case 0: pCM[2] = p3cm; pCM[3] = p4cm; pCM[4] = p5cm; break; case 1: pCM[2] = p3cm; pCM[3] = p5cm; pCM[4] = p4cm; break; case 2: pCM[2] = p4cm; pCM[3] = p3cm; pCM[4] = p5cm; break; case 3: pCM[2] = p4cm; pCM[3] = p5cm; pCM[4] = p3cm; break; case 4: pCM[2] = p5cm; pCM[3] = p3cm; pCM[4] = p4cm; break; case 5: pCM[2] = p5cm; pCM[3] = p4cm; pCM[4] = p3cm; break; } } //========================================================================== // Sigma3qqbar2qqbargDiff // Cross section for q qbar -> q' qbar' g // Crossed relation from q q' -> q q' g, q != q' //-------------------------------------------------------------------------- // Initialize process. void Sigma3qqbar2qqbargDiff::initProc() { // Read number of quarks to be considered in massless approximation. nQuarkNew = settingsPtr->mode("HardQCD:nQuarkNew"); } //-------------------------------------------------------------------------- // Evaluate |M|^2 - no incoming flavour dependence. void Sigma3qqbar2qqbargDiff::sigmaKin() { // Overall 6 possibilities for final state ordering // To keep symmetry between final states, always map to: // 1) q1(p+) qbar1(p-) -> qbar2(q+) q2(q-) g(k) // 2) qbar1(p+) q1(p-) -> q2(q+) qbar2(q-) g(k) // Crossing p- and q+ gives: // 1) q1(p+) q2(-q+) -> q1(-p-) q2(q-) g(k) // 2) qbar1(p+) qbar2(-q+) -> qbar1(-p-) qbar2(q-) g(k) // Incoming four-vectors pCM[0] = Vec4( 0., 0., 0.5 * mH, 0.5 * mH); pCM[1] = Vec4( 0., 0., -0.5 * mH, 0.5 * mH); // Pick and map a final state configuration pickFinal(); mapFinal(); // Crossing swap(pCM[1], pCM[2]); pCM[1] = -pCM[1]; pCM[2] = -pCM[2]; // |M|^2 // Extra factor of (6.) from picking a final state configuration // Extra factor of (nQuarkNew - 1) from new q/qbar pairs // XXX - Extra factor of (2.) from second possible crossing??? sigma = 6. * (nQuarkNew - 1) * 2. * m2Calc(); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3qqbar2qqbargDiff::setIdColAcol(){ // Pick new q qbar flavour with incoming flavour disallowed int idNew = 1 + int( (nQuarkNew - 1) * rndmPtr->flat() ); if (idNew >= abs(id1)) ++idNew; // For qbar q incoming, q+ is always mapped to q2 // For q qbar incoming, q+ is always mapped to qbar2 if (id1 > 0) idNew = -idNew; // Outgoing flavours; easiest just to map by hand switch (config) { case 0: id3 = idNew; id4 = -idNew; id5 = 21; break; case 1: id3 = idNew; id4 = 21; id5 = -idNew; break; case 2: id3 = -idNew; id4 = idNew; id5 = 21; break; case 3: id3 = 21; id4 = idNew; id5 = -idNew; break; case 4: id3 = -idNew; id4 = 21; id5 = idNew; break; case 5: id3 = 21; id4 = -idNew; id5 = idNew; break; } setId(id1, id2, id3, id4, id5); // Temporary solution; start with q qbar -> qbar q g int cols[5][2]; cols[0][0] = 1; cols[0][1] = 0; cols[1][0] = 0; cols[1][1] = 2; cols[2][0] = 0; cols[2][1] = 3; cols[3][0] = 1; cols[3][1] = 0; cols[4][0] = 3; cols[4][1] = 2; // Map into correct place int i3 = 0, i4 = 0, i5 = 0; switch (config) { case 0: i3 = 2; i4 = 3; i5 = 4; break; case 1: i3 = 2; i4 = 4; i5 = 3; break; case 2: i3 = 3; i4 = 2; i5 = 4; break; case 3: i3 = 4; i4 = 2; i5 = 3; break; case 4: i3 = 3; i4 = 4; i5 = 2; break; case 5: i3 = 4; i4 = 3; i5 = 2; break; } setColAcol(cols[0][0], cols[0][1], cols[1][0], cols[1][1], cols[i3][0], cols[i3][1], cols[i4][0], cols[i4][1], cols[i5][0], cols[i5][1]); // Swap for qbar q incoming if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma3qg2qqqbarDiff class. // Cross section for q g -> q q' qbar' // Crossed relation from q q' -> q q' g, q != q' // q1(p+) q2(p-) -> q1(q+) q2(q-) g(k) //-------------------------------------------------------------------------- // Initialize process. void Sigma3qg2qqqbarDiff::initProc() { // Read number of quarks to be considered in massless approximation. nQuarkNew = settingsPtr->mode("HardQCD:nQuarkNew"); } //-------------------------------------------------------------------------- // Evaluate |M|^2 - no incoming flavour dependence void Sigma3qg2qqqbarDiff::sigmaKin() { // Pick a final state configuration pickFinal(); // gq or qg incoming for (int i = 0; i < 2; i++) { // Map incoming four-vectors pCM[0] = Vec4( 0., 0., 0.5 * mH, 0.5 * mH); pCM[1] = Vec4( 0., 0., -0.5 * mH, 0.5 * mH); mapFinal(); // Crossing (note extra -ve sign in total sigma) swap(pCM[i], pCM[4]); pCM[i] = -pCM[i]; pCM[4] = -pCM[4]; // |M|^2 // Extra factor of (6) from picking a final state configuration // Extra factor of (3 / 8) as averaging over incoming gluon // Extra factor of (nQuarkNew - 1) due to new q/qbar pair sigma[i] = -6. * (3. / 8.) * (nQuarkNew - 1) * m2Calc(); } } //-------------------------------------------------------------------------- // Evaluate |M|^2 - incoming flavour dependence double Sigma3qg2qqqbarDiff::sigmaHat() { // gq or qg incoming return (id1 == 21) ? sigma[0] : sigma[1]; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3qg2qqqbarDiff::setIdColAcol(){ // Pick new q qbar flavour with incoming flavour disallowed int sigmaIdx = (id1 == 21) ? 0 : 1; int idIn = (id1 == 21) ? id2 : id1; int idNew = 1 + int( (nQuarkNew - 1) * rndmPtr->flat() ); if (idNew >= abs(idIn)) ++idNew; // qbar instead of q incoming means swap outgoing q/qbar pair int id3Tmp = idIn, id4Tmp = idNew, id5Tmp = -idNew; if (idIn < 0) swap(id4Tmp, id5Tmp); // If g q incoming rather than q g, idIn and idNew // should be exchanged (see sigmaKin) if (sigmaIdx == 0) swap(id3Tmp, id4Tmp); // Outgoing flavours; now just map as if q g incoming switch (config) { case 0: id3 = id3Tmp; id4 = id4Tmp; id5 = id5Tmp; break; case 1: id3 = id3Tmp; id4 = id5Tmp; id5 = id4Tmp; break; case 2: id3 = id4Tmp; id4 = id3Tmp; id5 = id5Tmp; break; case 3: id3 = id5Tmp; id4 = id3Tmp; id5 = id4Tmp; break; case 4: id3 = id4Tmp; id4 = id5Tmp; id5 = id3Tmp; break; case 5: id3 = id5Tmp; id4 = id4Tmp; id5 = id3Tmp; break; } setId(id1, id2, id3, id4, id5); // Temporary solution; start with either // g q1 -> q1 q2 qbar2 // g qbar1 -> qbar1 qbar2 q2 int cols[5][2]; cols[0][0] = 1; cols[0][1] = 2; if (idIn > 0) { cols[1][0] = 3; cols[1][1] = 0; cols[2][0] = 1; cols[2][1] = 0; cols[3][0] = 3; cols[3][1] = 0; cols[4][0] = 0; cols[4][1] = 2; } else { cols[1][0] = 0; cols[1][1] = 3; cols[2][0] = 0; cols[2][1] = 2; cols[3][0] = 0; cols[3][1] = 3; cols[4][0] = 1; cols[4][1] = 0; } // Swap incoming if q/qbar g instead if (id2 == 21) { swap(cols[0][0], cols[1][0]); swap(cols[0][1], cols[1][1]); } // Map final state int i3 = 0, i4 = 0, i5 = 0; if (sigmaIdx == 0) { switch (config) { case 0: i3 = 3; i4 = 2; i5 = 4; break; case 1: i3 = 3; i4 = 4; i5 = 2; break; case 2: i3 = 2; i4 = 3; i5 = 4; break; case 3: i3 = 4; i4 = 3; i5 = 2; break; case 4: i3 = 2; i4 = 4; i5 = 3; break; case 5: i3 = 4; i4 = 2; i5 = 3; break; } } else { switch (config) { case 0: i3 = 2; i4 = 3; i5 = 4; break; case 1: i3 = 2; i4 = 4; i5 = 3; break; case 2: i3 = 3; i4 = 2; i5 = 4; break; case 3: i3 = 4; i4 = 2; i5 = 3; break; case 4: i3 = 3; i4 = 4; i5 = 2; break; case 5: i3 = 4; i4 = 3; i5 = 2; break; } } setColAcol(cols[0][0], cols[0][1], cols[1][0], cols[1][1], cols[i3][0], cols[i3][1], cols[i4][0], cols[i4][1], cols[i5][0], cols[i5][1]); } //========================================================================== // Sigma3qq2qqgSame class. // Cross section for q q' -> q q' g, q == q'. //-------------------------------------------------------------------------- // Evaluate |M|^2 - no incoming flavour dependence void Sigma3qq2qqgSame::sigmaKin() { // q1(p+) q2(p-) -> q1(q+) q2(q-) g(k) // Incoming four-vectors pCM[0] = Vec4( 0., 0., 0.5 * mH, 0.5 * mH); pCM[1] = Vec4( 0., 0., -0.5 * mH, 0.5 * mH); // Pick/map a final state configuration pickFinal(); mapFinal(); // |M|^2 // Extra factor (3) from picking final state configuration // (original answer already has a factor 2 from identical // quarks in the final state) sigma = 3. * m2Calc(); } //-------------------------------------------------------------------------- // |M|^2 inline double Sigma3qq2qqgSame::m2Calc() { // Four-products s = (pCM[0] + pCM[1]).m2Calc(); t = (pCM[0] - pCM[2]).m2Calc(); u = (pCM[0] - pCM[3]).m2Calc(); sp = (pCM[2] + pCM[3]).m2Calc(); tp = (pCM[1] - pCM[3]).m2Calc(); up = (pCM[1] - pCM[2]).m2Calc(); // |M|^2 ssp = s * sp; ttp = t * tp; uup = u * up; s_sp = s + sp; t_tp = t + tp; u_up = u + up; double den1 = (pCM[0] * pCM[4]) * (pCM[1] * pCM[4]) * (pCM[2] * pCM[4]) * (pCM[3] * pCM[4]); double fac1 = s * (t * u + tp * up) + sp * (t * up + tp * u); double fac2 = ssp - ttp - uup; double fac3 = 2. * (ttp * u_up + uup * t_tp); double num1 = u_up * (ssp + ttp - uup) + fac1; double num2 = s_sp * fac2 + fac3; double num3 = (s * s + sp * sp + u * u + up * up) / (t * tp); double num4 = t_tp * (ssp - ttp + uup) + fac1; double num5 = (s * s + sp * sp + t * t + tp * tp) / (u * up); double num6 = s_sp * fac2 - fac3 - 2. * fac1; double num7 = (s * s + sp * sp) * fac2; double den7 = (ttp * uup); // C1 = (N^2 - 1)^2 / 4N^3 = 16. / 27. // C2 = (N^2 - 1) / 4N^3 = 2. / 27. // C3 = (N^4 - 1) / 8N^4 = 10. / 81. // C4 = (N^2 - 1)^2 / 8N^4 = 8. / 81. return (1. / 8.) * pow3(4. * M_PI * alpS) * ( ( (16. / 27.) * num1 - (2. / 27.) * num2 ) * num3 + ( (16. / 27.) * num4 - (2. / 27.) * num2 ) * num5 + ( (10. / 81.) * num2 + (8. / 81.) * num6 ) * ( num7 / den7 ) ) / den1; } //-------------------------------------------------------------------------- // Evaluate |M|^2 - incoming flavour dependence double Sigma3qq2qqgSame::sigmaHat() { // q q / qbar qbar incoming states only if (id1 != id2) return 0.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3qq2qqgSame::setIdColAcol(){ // Need to know where the gluon was mapped (pCM[4]) int gIdx = 0; switch (config) { case 3: case 5: gIdx = 0; break; case 1: case 4: gIdx = 1; break; case 0: case 2: gIdx = 2; break; } // Outgoing flavours int idTmp[3] = { id1, id1, id1 }; idTmp[gIdx] = 21; setId(id1, id2, idTmp[0], idTmp[1], idTmp[2]); // Temporary solution; start with q q -> q q g setColAcol(1, 0, 2, 0, 1, 0, 3, 0, 2, 3); // Map gluon swap( colSave[5], colSave[gIdx + 3]); swap(acolSave[5], acolSave[gIdx + 3]); // Swap if qbar qbar incoming if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Map a final state configuration inline void Sigma3qq2qqgSame::mapFinal() { switch (config) { case 0: pCM[2] = p3cm; pCM[3] = p4cm; pCM[4] = p5cm; break; case 1: pCM[2] = p3cm; pCM[3] = p5cm; pCM[4] = p4cm; break; case 2: pCM[2] = p4cm; pCM[3] = p3cm; pCM[4] = p5cm; break; case 3: pCM[2] = p4cm; pCM[3] = p5cm; pCM[4] = p3cm; break; case 4: pCM[2] = p5cm; pCM[3] = p3cm; pCM[4] = p4cm; break; case 5: pCM[2] = p5cm; pCM[3] = p4cm; pCM[4] = p3cm; break; } } //========================================================================== // Sigma3qqbar2qqbargSame class. // Cross section for q qbar -> q qbar g // Crossed relation from q(bar) q(bar) -> q(bar) q(bar) g: // q1(p+) q2(p-) -> q1(q+) q2(q-) g(k) //-------------------------------------------------------------------------- // Evaluate |M|^2 - no incoming flavour dependence void Sigma3qqbar2qqbargSame::sigmaKin() { // Incoming four-vectors pCM[0] = Vec4( 0., 0., 0.5 * mH, 0.5 * mH); pCM[1] = Vec4( 0., 0., -0.5 * mH, 0.5 * mH); // Pick and map a final state configuration pickFinal(); mapFinal(); // Crossing swap(pCM[1], pCM[3]); pCM[1] = -pCM[1]; pCM[3] = -pCM[3]; // |M|^2 // Extra factor of (6) from picking a final state configuration sigma = 6. * m2Calc(); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3qqbar2qqbargSame::setIdColAcol(){ // Outgoing flavours; easiest to map by hand switch (config) { case 0: id3 = id1; id4 = id2; id5 = 21; break; case 1: id3 = id1; id4 = 21; id5 = id2; break; case 2: id3 = id2; id4 = id1; id5 = 21; break; case 3: id3 = 21; id4 = id1; id5 = id2; break; case 4: id3 = id2; id4 = 21; id5 = id1; break; case 5: id3 = 21; id4 = id2; id5 = id1; break; } setId(id1, id2, id3, id4, id5); // Temporary solution; start with q qbar -> q qbar g int cols[5][2]; cols[0][0] = 1; cols[0][1] = 0; cols[1][0] = 0; cols[1][1] = 2; cols[2][0] = 1; cols[2][1] = 0; cols[3][0] = 0; cols[3][1] = 3; cols[4][0] = 3; cols[4][1] = 2; // Map final state int i3 = 0, i4 = 0, i5 = 0; switch (config) { case 0: i3 = 2; i4 = 3; i5 = 4; break; case 1: i3 = 2; i4 = 4; i5 = 3; break; case 2: i3 = 3; i4 = 2; i5 = 4; break; case 3: i3 = 4; i4 = 2; i5 = 3; break; case 4: i3 = 3; i4 = 4; i5 = 2; break; case 5: i3 = 4; i4 = 3; i5 = 2; break; } setColAcol(cols[0][0], cols[0][1], cols[1][0], cols[1][1], cols[i3][0], cols[i3][1], cols[i4][0], cols[i4][1], cols[i5][0], cols[i5][1]); // Swap for qbar q incoming if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma3qg2qqqbarSame class. // Cross section for q g -> q q qbar. // Crossed relation from q(bar) q(bar) -> q(bar) q(bar) g: // q1(p+) q1(p-) -> q1(q+) q1(q-) g(k) //-------------------------------------------------------------------------- // Evaluate |M|^2 - no incoming flavour dependence void Sigma3qg2qqqbarSame::sigmaKin() { // Pick a final state configuration pickFinal(); // gq and qg incoming for (int i = 0; i < 2; i++) { // Map incoming four-vectors pCM[0] = Vec4( 0., 0., 0.5 * mH, 0.5 * mH); pCM[1] = Vec4( 0., 0., -0.5 * mH, 0.5 * mH); mapFinal(); // Crossing (note extra -ve sign in total sigma) swap(pCM[i], pCM[4]); pCM[i] = -pCM[i]; pCM[4] = -pCM[4]; // |M|^2 // XXX - Extra factor of (3) from picking a final state configuration??? // Extra factor of (3 / 8) as averaging over incoming gluon sigma[i] = -3. * (3. / 8.) * m2Calc(); } } //-------------------------------------------------------------------------- // Evaluate |M|^2 - incoming flavour dependence double Sigma3qg2qqqbarSame::sigmaHat() { // gq or qg incoming return (id1 == 21) ? sigma[0] : sigma[1]; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3qg2qqqbarSame::setIdColAcol(){ // Pick outgoing flavour configuration int idIn = (id1 == 21) ? id2 : id1; // Outgoing flavours; easiest just to map by hand switch (config) { case 0: id3 = idIn; id4 = idIn; id5 = -idIn; break; case 1: id3 = idIn; id4 = -idIn; id5 = idIn; break; case 2: id3 = idIn; id4 = idIn; id5 = -idIn; break; case 3: id3 = -idIn; id4 = idIn; id5 = idIn; break; case 4: id3 = idIn; id4 = -idIn; id5 = idIn; break; case 5: id3 = -idIn; id4 = idIn; id5 = idIn; break; } setId(id1, id2, id3, id4, id5); // Temporary solution; start with either // g q1 -> q1 q2 qbar2 // g qbar1 -> qbar1 qbar2 q2 int cols[5][2]; cols[0][0] = 1; cols[0][1] = 2; if (idIn > 0) { cols[1][0] = 3; cols[1][1] = 0; cols[2][0] = 1; cols[2][1] = 0; cols[3][0] = 3; cols[3][1] = 0; cols[4][0] = 0; cols[4][1] = 2; } else { cols[1][0] = 0; cols[1][1] = 3; cols[2][0] = 0; cols[2][1] = 2; cols[3][0] = 0; cols[3][1] = 3; cols[4][0] = 1; cols[4][1] = 0; } // Swap incoming if q/qbar g instead if (id2 == 21) { swap(cols[0][0], cols[1][0]); swap(cols[0][1], cols[1][1]); } // Map final state int i3 = 0, i4 = 0, i5 = 0; switch (config) { case 0: i3 = 2; i4 = 3; i5 = 4; break; case 1: i3 = 2; i4 = 4; i5 = 3; break; case 2: i3 = 3; i4 = 2; i5 = 4; break; case 3: i3 = 4; i4 = 2; i5 = 3; break; case 4: i3 = 3; i4 = 4; i5 = 2; break; case 5: i3 = 4; i4 = 3; i5 = 2; break; } setColAcol(cols[0][0], cols[0][1], cols[1][0], cols[1][1], cols[i3][0], cols[i3][1], cols[i4][0], cols[i4][1], cols[i5][0], cols[i5][1]); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaNewGaugeBosons.cc0000644000175000017500000006403212217346251017306 0ustar sunsun// SigmaNewGaugeBosons.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // leptoquark simulation classes. #include "Pythia8/SigmaNewGaugeBosons.h" namespace Pythia8 { //========================================================================== // Sigma1ffbarZprimeWprime class. // Collects common methods for f fbar -> Z'/W' -> WW/WZ -> 4 fermions. // Copied from SigmaEW for gauge-boson-pair production. //-------------------------------------------------------------------------- // Calculate and store internal products. void Sigma1ffbarZprimeWprime::setupProd( Event& process, int i1, int i2, int i3, int i4, int i5, int i6) { // Store incoming and outgoing momenta, pRot[1] = process[i1].p(); pRot[2] = process[i2].p(); pRot[3] = process[i3].p(); pRot[4] = process[i4].p(); pRot[5] = process[i5].p(); pRot[6] = process[i6].p(); // Do random rotation to avoid accidental zeroes in HA expressions. bool smallPT = false; do { smallPT = false; double thetaNow = acos(2. * rndmPtr->flat() - 1.); double phiNow = 2. * M_PI * rndmPtr->flat(); for (int i = 1; i <= 6; ++i) { pRot[i].rot( thetaNow, phiNow); if (pRot[i].pT2() < 1e-4 * pRot[i].pAbs2()) smallPT = true; } } while (smallPT); // Calculate internal products. for (int i = 1; i < 6; ++i) { for (int j = i + 1; j <= 6; ++j) { hA[i][j] = sqrt( (pRot[i].e() - pRot[i].pz()) * (pRot[j].e() + pRot[j].pz()) / pRot[i].pT2() ) * complex( pRot[i].px(), pRot[i].py() ) - sqrt( (pRot[i].e() + pRot[i].pz()) * (pRot[j].e() - pRot[j].pz()) / pRot[j].pT2() ) * complex( pRot[j].px(), pRot[j].py() ); hC[i][j] = conj( hA[i][j] ); if (i <= 2) { hA[i][j] *= complex( 0., 1.); hC[i][j] *= complex( 0., 1.); } hA[j][i] = - hA[i][j]; hC[j][i] = - hC[i][j]; } } } //-------------------------------------------------------------------------- // Evaluate the F function of Gunion and Kunszt. complex Sigma1ffbarZprimeWprime::fGK(int j1, int j2, int j3, int j4, int j5, int j6) { return 4. * hA[j1][j3] * hC[j2][j6] * ( hA[j1][j5] * hC[j1][j4] + hA[j3][j5] * hC[j3][j4] ); } //-------------------------------------------------------------------------- // Evaluate the Xi function of Gunion and Kunszt. double Sigma1ffbarZprimeWprime::xiGK( double tHnow, double uHnow, double s3now, double s4now) { return - 4. * s3now * s4now + tHnow * (3. * tHnow + 4. * uHnow) + tHnow * tHnow * ( tHnow * uHnow / (s3now * s4now) - 2. * (1. / s3now + 1./s4now) * (tHnow + uHnow) + 2. * (s3now / s4now + s4now / s3now) ); } //-------------------------------------------------------------------------- // Evaluate the Xj function of Gunion and Kunszt. double Sigma1ffbarZprimeWprime::xjGK( double tHnow, double uHnow, double s3now, double s4now) { return 8. * pow2(s3now + s4now) - 8. * (s3now + s4now) * (tHnow + uHnow) - 6. * tHnow * uHnow - 2. * tHnow * uHnow * ( tHnow * uHnow / (s3now * s4now) - 2. * (1. / s3now + 1. / s4now) * (tHnow + uHnow) + 2. * (s3now / s4now + s4now / s3now) ); } //========================================================================== // Sigma1ffbar2gmZZprime class. // Cross section for f fbar -> gamma*/Z0/Z'0 (f is quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2gmZZprime::initProc() { // Allow to pick only parts of full gamma*/Z0/Z'0 expression. gmZmode = settingsPtr->mode("Zprime:gmZmode"); // Store Z'0 mass and width for propagator. mRes = particleDataPtr->m0(32); GammaRes = particleDataPtr->mWidth(32); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; sin2tW = couplingsPtr->sin2thetaW(); cos2tW = 1. - sin2tW; thetaWRat = 1. / (16. * sin2tW * cos2tW); // Properties of Z0 resonance also needed. mZ = particleDataPtr->m0(23); GammaZ = particleDataPtr->mWidth(23); m2Z = mZ*mZ; GamMRatZ = GammaZ / mZ; // Ensure that arrays initially are empty. for (int i = 0; i < 20; ++i) afZp[i] = 0.; for (int i = 0; i < 20; ++i) vfZp[i] = 0.; // Store first-generation axial and vector couplings. afZp[1] = settingsPtr->parm("Zprime:ad"); afZp[2] = settingsPtr->parm("Zprime:au"); afZp[11] = settingsPtr->parm("Zprime:ae"); afZp[12] = settingsPtr->parm("Zprime:anue"); vfZp[1] = settingsPtr->parm("Zprime:vd"); vfZp[2] = settingsPtr->parm("Zprime:vu"); vfZp[11] = settingsPtr->parm("Zprime:ve"); vfZp[12] = settingsPtr->parm("Zprime:vnue"); // Second and third generation could be carbon copy of this... if (settingsPtr->flag("Zprime:universality")) { for (int i = 3; i <= 6; ++i) { afZp[i] = afZp[i-2]; vfZp[i] = vfZp[i-2]; afZp[i+10] = afZp[i+8]; vfZp[i+10] = vfZp[i+8]; } // ... or could have different couplings. } else { afZp[3] = settingsPtr->parm("Zprime:as"); afZp[4] = settingsPtr->parm("Zprime:ac"); afZp[5] = settingsPtr->parm("Zprime:ab"); afZp[6] = settingsPtr->parm("Zprime:at"); afZp[13] = settingsPtr->parm("Zprime:amu"); afZp[14] = settingsPtr->parm("Zprime:anumu"); afZp[15] = settingsPtr->parm("Zprime:atau"); afZp[16] = settingsPtr->parm("Zprime:anutau"); vfZp[3] = settingsPtr->parm("Zprime:vs"); vfZp[4] = settingsPtr->parm("Zprime:vc"); vfZp[5] = settingsPtr->parm("Zprime:vb"); vfZp[6] = settingsPtr->parm("Zprime:vt"); vfZp[13] = settingsPtr->parm("Zprime:vmu"); vfZp[14] = settingsPtr->parm("Zprime:vnumu"); vfZp[15] = settingsPtr->parm("Zprime:vtau"); vfZp[16] = settingsPtr->parm("Zprime:vnutau"); } // Coupling for Z' -> W+ W- and decay angular admixture. coupZpWW = settingsPtr->parm("Zprime:coup2WW"); anglesZpWW = settingsPtr->parm("Zprime:anglesWW"); // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(32); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1ffbar2gmZZprime::sigmaKin() { // Common coupling factors. double colQ = 3. * (1. + alpS / M_PI); // Reset quantities to sum. Declare variables in loop. gamSum = 0.; gamZSum = 0.; ZSum = 0.; gamZpSum = 0.; ZZpSum = 0.; ZpSum = 0.; int idAbs, onMode; double mf, mr, ps, kinFacA, kinFacV, ef, af, vf, apf, vpf, ef2, efvf, vaf2, efvpf, vafvapf, vapf2, colf; // Loop over all open Z'0 decay channels. for (int i = 0; i < particlePtr->sizeChannels(); ++i) { onMode = particlePtr->channel(i).onMode(); if (onMode != 1 && onMode != 2) continue; idAbs = abs( particlePtr->channel(i).product(0) ); // Contributions from three fermion generations. if ( (idAbs > 0 && idAbs < 7) || ( idAbs > 10 && idAbs < 17) ) { mf = particleDataPtr->m0(idAbs); // Check that above threshold. if (mH > 2. * mf + MASSMARGIN) { mr = pow2(mf / mH); ps = sqrtpos(1. - 4. * mr); // Couplings of gamma^*/Z^0/Z'^0 to final flavour ef = couplingsPtr->ef(idAbs); af = couplingsPtr->af(idAbs); vf = couplingsPtr->vf(idAbs); apf = afZp[idAbs]; vpf = vfZp[idAbs]; // Combine couplings with kinematical factors. kinFacA = pow3(ps); kinFacV = ps * (1. + 2. * mr); ef2 = ef * ef * kinFacV; efvf = ef * vf * kinFacV; vaf2 = vf * vf * kinFacV + af * af * kinFacA; efvpf = ef * vpf * kinFacV; vafvapf = vf * vpf * kinFacV + af * apf * kinFacA; vapf2 = vpf * vpf * kinFacV + apf * apf * kinFacA; // Colour factor. Additionally secondary width for top. colf = (idAbs < 9) ? colQ : 1.; if (idAbs == 6) colf *= particleDataPtr->resOpenFrac(6, -6); // Store sum of combinations. gamSum += colf * ef2; gamZSum += colf * efvf; ZSum += colf * vaf2; gamZpSum += colf * efvpf; ZZpSum += colf * vafvapf; ZpSum += colf * vapf2; } // Optional contribution from W+ W-. } else if (idAbs == 24) { mf = particleDataPtr->m0(idAbs); if (mH > 2. * mf + MASSMARGIN) { mr = pow2(mf / mH); ps = sqrtpos(1. - 4. * mr); ZpSum += pow2(coupZpWW * cos2tW) * pow3(ps) * (1. + 20. * mr + 12. * mr*mr) * particleDataPtr->resOpenFrac(24, -24); } } } // Calculate prefactors for gamma/Z0/Z'0 cross section terms. double propZ = sH / ( pow2(sH - m2Z) + pow2(sH * GamMRatZ) ); double propZp = sH / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); gamNorm = 4. * M_PI * pow2(alpEM) / (3. * sH); gamZNorm = gamNorm * 2. * thetaWRat * (sH - m2Z) * propZ; ZNorm = gamNorm * pow2(thetaWRat) * sH * propZ; gamZpNorm = gamNorm * 2. * thetaWRat * (sH - m2Res) * propZp; ZZpNorm = gamNorm * 2. * pow2(thetaWRat) * ((sH - m2Z) * (sH - m2Res) + sH * GamMRatZ * sH * GamMRat) * propZ * propZp; ZpNorm = gamNorm * pow2(thetaWRat) * sH * propZp; // Optionally only keep some of gamma*, Z0 and Z' terms. if (gmZmode == 1) {gamZNorm = 0; ZNorm = 0.; gamZpNorm = 0.; ZZpNorm = 0.; ZpNorm = 0.;} if (gmZmode == 2) {gamNorm = 0.; gamZNorm = 0.; gamZpNorm = 0.; ZZpNorm = 0.; ZpNorm = 0.;} if (gmZmode == 3) {gamNorm = 0.; gamZNorm = 0.; ZNorm = 0.; gamZpNorm = 0.; ZZpNorm = 0.;} if (gmZmode == 4) {gamZpNorm = 0.; ZZpNorm = 0.; ZpNorm = 0.;} if (gmZmode == 5) {gamZNorm = 0.; ZNorm = 0.; ZZpNorm = 0.;} if (gmZmode == 6) {gamNorm = 0.; gamZNorm = 0.; gamZpNorm = 0.;} } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma1ffbar2gmZZprime::sigmaHat() { // Couplings to an incoming flavour. int idAbs = abs(id1); double ei = couplingsPtr->ef(idAbs); double ai = couplingsPtr->af(idAbs); double vi = couplingsPtr->vf(idAbs); double api = afZp[idAbs]; double vpi = vfZp[idAbs]; double ei2 = ei * ei; double eivi = ei * vi; double vai2 = vi * vi + ai * ai; double eivpi = ei * vpi; double vaivapi = vi * vpi + ai * api;; double vapi2 = vpi * vpi + api * api; // Combine gamma, interference and Z0 parts. double sigma = ei2 * gamNorm * gamSum + eivi * gamZNorm * gamZSum + vai2 * ZNorm * ZSum + eivpi * gamZpNorm * gamZpSum + vaivapi * ZZpNorm * ZZpSum + vapi2 * ZpNorm * ZpSum; // Colour factor. Answer. if (idAbs < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2gmZZprime::setIdColAcol() { // Flavours trivial. setId( id1, id2, 32); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for gamma*/Z0/Z'0 decay angle. double Sigma1ffbar2gmZZprime::weightDecay( Event& process, int iResBeg, int iResEnd) { // Default values, in- and out-flavours in process. double wt = 1.; double wtMax = 1.; int idInAbs = process[3].idAbs(); int idOutAbs = process[6].idAbs(); // Angular weight for outgoing fermion pair. if (iResBeg == 5 && iResEnd == 5 && (idOutAbs < 7 || ( idOutAbs > 10 && idOutAbs < 17)) ) { // Couplings for in- and out-flavours. double ei = couplingsPtr->ef(idInAbs); double vi = couplingsPtr->vf(idInAbs); double ai = couplingsPtr->af(idInAbs); double vpi = vfZp[idInAbs]; double api = afZp[idInAbs]; double ef = couplingsPtr->ef(idOutAbs); double vf = couplingsPtr->vf(idOutAbs); double af = couplingsPtr->af(idOutAbs); double vpf = vfZp[idOutAbs]; double apf = afZp[idOutAbs]; // Phase space factors. (One power of beta left out in formulae.) double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double ps = sqrtpos(pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); double mrAvg = 0.5 * (mr1 + mr2) - 0.25 * pow2(mr1 - mr2); // Coefficients of angular expression. double coefTran = ei*ei * gamNorm * ef*ef + ei * vi * gamZNorm * ef * vf + (vi*vi + ai*ai) * ZNorm * (vf*vf + ps*ps * af*af) + ei * vpi * gamZpNorm * ef * vpf + (vi * vpi + ai * api) * ZZpNorm * (vf * vpf + ps*ps * af * apf) + (vpi*vpi + api*api) * ZpNorm * (vpf*vpf + ps*ps * apf*apf); double coefLong = 4. * mrAvg * ( ei*ei * gamNorm * ef*ef + ei * vi * gamZNorm * ef * vf + (vi*vi + ai*ai) * ZNorm * vf*vf + ei * vpi * gamZpNorm * ef * vpf + (vi * vpi + ai * api) * ZZpNorm * vf * vpf + (vpi*vpi + api*api) * ZpNorm * vpf*vpf ); double coefAsym = ps * ( ei * ai * gamZNorm * ef * af + 4. * vi * ai * ZNorm * vf * af + ei * api * gamZpNorm * ef * apf + (vi * api + vpi * ai) * ZZpNorm * (vf * apf + vpf * af) + 4. * vpi * api * ZpNorm * vpf * apf ); // Flip asymmetry for in-fermion + out-antifermion. if (process[3].id() * process[6].id() < 0) coefAsym = -coefAsym; // Reconstruct decay angle and weight for it. double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * ps); wt = coefTran * (1. + pow2(cosThe)) + coefLong * (1. - pow2(cosThe)) + 2. * coefAsym * cosThe; wtMax = 2. * (coefTran + abs(coefAsym)); } // Angular weight for Z' -> W+ W-. else if (iResBeg == 5 && iResEnd == 5 && idOutAbs == 24) { double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double ps = sqrtpos(pow2(1. - mr1 -mr2) - 4. * mr1 * mr2); double cCos2 = - (1./16.) * ps*ps * (1. - 2. * mr1 - 2. * mr2 + mr1*mr1 + mr2*mr2 + 10. * mr1 * mr2); double cFlat = -cCos2 + 0.5 * (mr1 + mr2) * (1. - 2. * mr1 - 2. * mr2 + pow2(mr1 - mr2)); // Reconstruct decay angle and weight for it. double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * ps); wt = cFlat + cCos2 * cosThe*cosThe; wtMax = cFlat + max(0., cCos2); } // Angular weight for f + fbar -> Z' -> W+ + W- -> 4 fermions. else if (iResBeg == 6 && iResEnd == 7 && idOutAbs == 24) { // Order so that fbar(1) f(2) -> f'(3) fbar'(4) f"(5) fbar"(6). // with f' fbar' from W- and f" fbar" from W+. int i1 = (process[3].id() < 0) ? 3 : 4; int i2 = 7 - i1; int i3 = (process[8].id() > 0) ? 8 : 9; int i4 = 17 - i3; int i5 = (process[10].id() > 0) ? 10 : 11; int i6 = 21 - i5; if (process[6].id() > 0) {swap(i3, i5); swap(i4, i6);} // Decay distribution like in f fbar -> Z^* -> W+ W-. if (rndmPtr->flat() > anglesZpWW) { // Set up four-products and internal products. setupProd( process, i1, i2, i3, i4, i5, i6); // tHat and uHat of fbar f -> W- W+, and their squared masses. int iNeg = (process[6].id() < 0) ? 6 : 7; int iPos = 13 - iNeg; double tHres = (process[i1].p() - process[iNeg].p()).m2Calc(); double uHres = (process[i1].p() - process[iPos].p()).m2Calc(); double s3now = process[iNeg].m2(); double s4now = process[iPos].m2(); // Kinematics combinations (norm(x) = |x|^2). double fGK135 = norm(fGK( 1, 2, 3, 4, 5, 6) - fGK( 1, 2, 5, 6, 3, 4) ); double fGK253 = norm(fGK( 2, 1, 5, 6, 3, 4) - fGK( 2, 1, 3, 4, 5, 6) ); double xiT = xiGK( tHres, uHres, s3now, s4now); double xiU = xiGK( uHres, tHres, s3now, s4now); double xjTU = xjGK( tHres, uHres, s3now, s4now); // Couplings of incoming (anti)fermion. Combine with kinematics. int idAbs = process[i1].idAbs(); double li = 0.5 * (vfZp[idAbs] + afZp[idAbs]); double ri = 0.5 * (vfZp[idAbs] - afZp[idAbs]); wt = li*li * fGK135 + ri*ri * fGK253; wtMax = 4. * s3now * s4now * (li*li + ri*ri) * (xiT + xiU - xjTU); // Decay distribution like in f fbar -> h^0 -> W+ W-. } else { double p35 = 2. * process[i3].p() * process[i5].p(); double p46 = 2. * process[i4].p() * process[i6].p(); wt = 16. * p35 * p46; wtMax = sH2; } } // Angular weight in top decay by standard routine. else if (process[process[iResBeg].mother1()].idAbs() == 6) return weightTopDecay( process, iResBeg, iResEnd); // Done. return (wt / wtMax); } //========================================================================== // Sigma1ffbar2Wprime class. // Cross section for f fbar' -> W'+- (f is quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2Wprime::initProc() { // Store W+- mass and width for propagator. mRes = particleDataPtr->m0(34); GammaRes = particleDataPtr->mWidth(34); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; thetaWRat = 1. / (12. * couplingsPtr->sin2thetaW()); // Axial and vector couplings of fermions. aqWp = settingsPtr->parm("Wprime:aq"); vqWp = settingsPtr->parm("Wprime:vq"); alWp = settingsPtr->parm("Wprime:al"); vlWp = settingsPtr->parm("Wprime:vl"); // Coupling for W' -> W Z and decay angular admixture. coupWpWZ = settingsPtr->parm("Wprime:coup2WZ"); anglesWpWZ = settingsPtr->parm("Wprime:anglesWZ"); // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(34); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1ffbar2Wprime::sigmaKin() { // Set up Breit-Wigner. Cross section for W+ and W- separately. double sigBW = 12. * M_PI / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); double preFac = alpEM * thetaWRat * mH; sigma0Pos = preFac * sigBW * particlePtr->resWidthOpen(34, mH); sigma0Neg = preFac * sigBW * particlePtr->resWidthOpen(-34, mH); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma1ffbar2Wprime::sigmaHat() { // Secondary width for W+ or W-. CKM and colour factors. int idUp = (abs(id1)%2 == 0) ? id1 : id2; double sigma = (idUp > 0) ? sigma0Pos : sigma0Neg; if (abs(id1) < 7) sigma *= couplingsPtr->V2CKMid(abs(id1), abs(id2)) / 3.; // Couplings. if (abs(id1) < 7) sigma *= 0.5 * (aqWp * aqWp + vqWp * vqWp); else sigma *= 0.5 * (alWp * alWp + vlWp * vlWp); // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2Wprime::setIdColAcol() { // Sign of outgoing W. int sign = 1 - 2 * (abs(id1)%2); if (id1 < 0) sign = -sign; setId( id1, id2, 34 * sign); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for W decay angle. double Sigma1ffbar2Wprime::weightDecay( Event& process, int iResBeg, int iResEnd) { // Default values, in- and out-flavours in process. double wt = 1.; double wtMax = 1.; int idInAbs = process[3].idAbs(); int idOutAbs = process[6].idAbs(); // Angular weight for outgoing fermion pair. if (iResBeg == 5 && iResEnd == 5 && (idOutAbs < 7 || ( idOutAbs > 10 && idOutAbs < 17)) ) { // Couplings for in- and out-flavours. double ai = (idInAbs < 9) ? aqWp : alWp; double vi = (idInAbs < 9) ? vqWp : vlWp; double af = (idOutAbs < 9) ? aqWp : alWp; double vf = (idOutAbs < 9) ? vqWp : vlWp; // Asymmetry expression. double coefAsym = 8. * vi * ai * vf * af / ((vi*vi + ai*ai) * (vf*vf + af*af)); // Flip asymmetry for in-fermion + out-antifermion. if (process[3].id() * process[6].id() < 0) coefAsym = -coefAsym; // Phase space factors. double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double ps = sqrtpos(pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); // Reconstruct decay angle and weight for it. double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * ps); wt = 1. + coefAsym * cosThe + cosThe * cosThe; wtMax = 2. + abs(coefAsym); } // Angular weight for W' -> W Z. else if (iResBeg == 5 && iResEnd == 5 && idOutAbs == 24) { double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double ps = sqrtpos(pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); double cCos2 = - (1./16.) * ps*ps * (1. - 2. * mr1 - 2. * mr2 + mr1*mr1 + mr2*mr2 + 10. * mr1 * mr2); double cFlat = -cCos2 + 0.5 * (mr1 + mr2) * (1. - 2. * mr1 - 2. * mr2 + pow2(mr1 - mr2)); // Reconstruct decay angle and weight for it. double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * ps); wt = cFlat + cCos2 * cosThe*cosThe; wtMax = cFlat + max(0., cCos2); } // Angular weight for f + fbar -> W' -> W + Z -> 4 fermions. else if (iResBeg == 6 && iResEnd == 7 && (idOutAbs == 24 || idOutAbs == 23)) { // Order so that fbar(1) f(2) -> f'(3) fbar'(4) f"(5) fbar"(6). // with f' fbar' from W and f" fbar" from Z. int i1 = (process[3].id() < 0) ? 3 : 4; int i2 = 7 - i1; int i3 = (process[8].id() > 0) ? 8 : 9; int i4 = 17 - i3; int i5 = (process[10].id() > 0) ? 10 : 11; int i6 = 21 - i5; if (process[6].id() == 23) {swap(i3, i5); swap(i4, i6);} // Decay distribution like in f fbar -> Z^* -> W+ W-. if (rndmPtr->flat() > anglesWpWZ) { // Set up four-products and internal products. setupProd( process, i1, i2, i3, i4, i5, i6); // tHat and uHat of fbar f -> W Z, and their squared masses. int iW = (process[6].id() == 23) ? 7 : 6; int iZ = 13 - iW; double tHres = (process[i1].p() - process[iW].p()).m2Calc(); double uHres = (process[i1].p() - process[iZ].p()).m2Calc(); double s3now = process[iW].m2(); double s4now = process[iZ].m2(); // Kinematics combinations (norm(x) = |x|^2). double fGK135 = norm(fGK( 1, 2, 3, 4, 5, 6) - fGK( 1, 2, 5, 6, 3, 4) ); double fGK136 = norm(fGK( 1, 2, 3, 4, 6, 5) - fGK( 1, 2, 6, 5, 3, 4) ); double xiT = xiGK( tHres, uHres, s3now, s4now); double xiU = xiGK( uHres, tHres, s3now, s4now); double xjTU = xjGK( tHres, uHres, s3now, s4now); // Couplings of outgoing fermion from Z. Combine with kinematics. int idAbs = process[i5].idAbs(); double lfZ = couplingsPtr->lf(idAbs); double rfZ = couplingsPtr->rf(idAbs); wt = lfZ*lfZ * fGK135 + rfZ*rfZ * fGK136; wtMax = 4. * s3now * s4now * (lfZ*lfZ + rfZ*rfZ) * (xiT + xiU - xjTU); // Decay distribution like in f fbar -> H^+- -> W+- Z0. } else { double p35 = 2. * process[i3].p() * process[i5].p(); double p46 = 2. * process[i4].p() * process[i6].p(); wt = 16. * p35 * p46; wtMax = sH2; } } // Angular weight in top decay by standard routine. else if (process[process[iResBeg].mother1()].idAbs() == 6) return weightTopDecay( process, iResBeg, iResEnd); // Done. return (wt / wtMax); } //========================================================================== // Sigma1ffbar2Rhorizontal class. // Cross section for f fbar' -> R^0 (f is a quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2Rhorizontal::initProc() { // Store R^0 mass and width for propagator. mRes = particleDataPtr->m0(41); GammaRes = particleDataPtr->mWidth(41); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; thetaWRat = 1. / (12. * couplingsPtr->sin2thetaW()); // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(41); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1ffbar2Rhorizontal::sigmaKin() { // Set up Breit-Wigner. Cross section for W+ and W- separately. double sigBW = 12. * M_PI / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); double preFac = alpEM * thetaWRat * mH; sigma0Pos = preFac * sigBW * particlePtr->resWidthOpen(41, mH); sigma0Neg = preFac * sigBW * particlePtr->resWidthOpen(-41, mH); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma1ffbar2Rhorizontal::sigmaHat() { // Check for allowed flavour combinations, one generation apart. if (id1 * id2 > 0 || abs(id1 + id2) != 2) return 0.; // Find whether R0 or R0bar. Colour factors. double sigma = (id1 + id2 > 0) ? sigma0Pos : sigma0Neg; if (abs(id1) < 7) sigma /= 3.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2Rhorizontal::setIdColAcol() { // Outgoing R0 or R0bar. id3 = (id1 +id2 > 0) ? 41 : -41; setId( id1, id2, id3); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/MultipartonInteractions.cc0000644000175000017500000027073312217346246020353 0ustar sunsun// MultipartonInteractions.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // SigmaMultiparton and MultipartonInteractions classes. #include "Pythia8/MultipartonInteractions.h" // Internal headers for special processes. #include "Pythia8/SigmaQCD.h" #include "Pythia8/SigmaEW.h" #include "Pythia8/SigmaOnia.h" namespace Pythia8 { //========================================================================== // The SigmaMultiparton class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // The sum of outgoing masses must not be too close to the cm energy. const double SigmaMultiparton::MASSMARGIN = 0.1; // Fraction of time not the dominant "gluon t-channel" process is picked. const double SigmaMultiparton::OTHERFRAC = 0.2; //-------------------------------------------------------------------------- // Initialize the generation process for given beams. bool SigmaMultiparton::init(int inState, int processLevel, Info* infoPtr, Settings* settingsPtr, ParticleData* particleDataPtr, Rndm* rndmPtrIn, BeamParticle* beamAPtr, BeamParticle* beamBPtr, Couplings* couplingsPtr) { // Store input pointer for future use. rndmPtr = rndmPtrIn; // Reset vector sizes (necessary in case of re-initialization). if (sigmaT.size() > 0) { for (int i = 0; i < int(sigmaT.size()); ++i) delete sigmaT[i]; sigmaT.resize(0); } if (sigmaU.size() > 0) { for (int i = 0; i < int(sigmaU.size()); ++i) delete sigmaU[i]; sigmaU.resize(0); } // Always store mimimal set of processes:QCD 2 -> 2 t-channel. // Gluon-gluon instate. if (inState == 0) { sigmaT.push_back( new Sigma2gg2gg() ); sigmaU.push_back( new Sigma2gg2gg() ); // Quark-gluon instate. } else if (inState == 1) { sigmaT.push_back( new Sigma2qg2qg() ); sigmaU.push_back( new Sigma2qg2qg() ); // Quark-(anti)quark instate. } else { sigmaT.push_back( new Sigma2qq2qq() ); sigmaU.push_back( new Sigma2qq2qq() ); } // Normally store QCD processes to new flavour. if (processLevel > 0) { if (inState == 0) { sigmaT.push_back( new Sigma2gg2qqbar() ); sigmaU.push_back( new Sigma2gg2qqbar() ); sigmaT.push_back( new Sigma2gg2QQbar(4, 121) ); sigmaU.push_back( new Sigma2gg2QQbar(4, 121) ); sigmaT.push_back( new Sigma2gg2QQbar(5, 123) ); sigmaU.push_back( new Sigma2gg2QQbar(5, 123) ); } else if (inState == 2) { sigmaT.push_back( new Sigma2qqbar2gg() ); sigmaU.push_back( new Sigma2qqbar2gg() ); sigmaT.push_back( new Sigma2qqbar2qqbarNew() ); sigmaU.push_back( new Sigma2qqbar2qqbarNew() ); sigmaT.push_back( new Sigma2qqbar2QQbar(4, 122) ); sigmaU.push_back( new Sigma2qqbar2QQbar(4, 122) ); sigmaT.push_back( new Sigma2qqbar2QQbar(5, 124) ); sigmaU.push_back( new Sigma2qqbar2QQbar(5, 124) ); } } // Optionally store electroweak processes, mainly photon production. if (processLevel > 1) { if (inState == 0) { sigmaT.push_back( new Sigma2gg2ggamma() ); sigmaU.push_back( new Sigma2gg2ggamma() ); sigmaT.push_back( new Sigma2gg2gammagamma() ); sigmaU.push_back( new Sigma2gg2gammagamma() ); } else if (inState == 1) { sigmaT.push_back( new Sigma2qg2qgamma() ); sigmaU.push_back( new Sigma2qg2qgamma() ); } else if (inState == 2) { sigmaT.push_back( new Sigma2qqbar2ggamma() ); sigmaU.push_back( new Sigma2qqbar2ggamma() ); sigmaT.push_back( new Sigma2ffbar2gammagamma() ); sigmaU.push_back( new Sigma2ffbar2gammagamma() ); sigmaT.push_back( new Sigma2ffbar2ffbarsgm() ); sigmaU.push_back( new Sigma2ffbar2ffbarsgm() ); } if (inState >= 2) { sigmaT.push_back( new Sigma2ff2fftgmZ() ); sigmaU.push_back( new Sigma2ff2fftgmZ() ); sigmaT.push_back( new Sigma2ff2fftW() ); sigmaU.push_back( new Sigma2ff2fftW() ); } } // Optionally store charmonium and bottomonium production. if (processLevel > 2) { if (inState == 0) { sigmaT.push_back( new Sigma2gg2QQbar3S11g(4, 401) ); sigmaU.push_back( new Sigma2gg2QQbar3S11g(4, 401) ); sigmaT.push_back( new Sigma2gg2QQbar3PJ1g(4, 0, 402) ); sigmaU.push_back( new Sigma2gg2QQbar3PJ1g(4, 0, 402) ); sigmaT.push_back( new Sigma2gg2QQbar3PJ1g(4, 1, 403) ); sigmaU.push_back( new Sigma2gg2QQbar3PJ1g(4, 1, 403) ); sigmaT.push_back( new Sigma2gg2QQbar3PJ1g(4, 2, 404) ); sigmaU.push_back( new Sigma2gg2QQbar3PJ1g(4, 2, 404) ); sigmaT.push_back( new Sigma2gg2QQbarX8g(4, 0, 411) ); sigmaU.push_back( new Sigma2gg2QQbarX8g(4, 0, 411) ); sigmaT.push_back( new Sigma2gg2QQbarX8g(4, 1, 412) ); sigmaU.push_back( new Sigma2gg2QQbarX8g(4, 1, 412) ); sigmaT.push_back( new Sigma2gg2QQbarX8g(4, 2, 413) ); sigmaU.push_back( new Sigma2gg2QQbarX8g(4, 2, 413) ); sigmaT.push_back( new Sigma2gg2QQbar3S11g(5, 501) ); sigmaU.push_back( new Sigma2gg2QQbar3S11g(5, 501) ); sigmaT.push_back( new Sigma2gg2QQbar3PJ1g(5, 0, 502) ); sigmaU.push_back( new Sigma2gg2QQbar3PJ1g(5, 0, 502) ); sigmaT.push_back( new Sigma2gg2QQbar3PJ1g(5, 1, 503) ); sigmaU.push_back( new Sigma2gg2QQbar3PJ1g(5, 1, 503) ); sigmaT.push_back( new Sigma2gg2QQbar3PJ1g(5, 2, 504) ); sigmaU.push_back( new Sigma2gg2QQbar3PJ1g(5, 2, 504) ); sigmaT.push_back( new Sigma2gg2QQbarX8g(5, 0, 511) ); sigmaU.push_back( new Sigma2gg2QQbarX8g(5, 0, 511) ); sigmaT.push_back( new Sigma2gg2QQbarX8g(5, 1, 512) ); sigmaU.push_back( new Sigma2gg2QQbarX8g(5, 1, 512) ); sigmaT.push_back( new Sigma2gg2QQbarX8g(5, 2, 513) ); sigmaU.push_back( new Sigma2gg2QQbarX8g(5, 2, 513) ); } else if (inState == 1) { sigmaT.push_back( new Sigma2qg2QQbar3PJ1q(4, 0, 405) ); sigmaU.push_back( new Sigma2qg2QQbar3PJ1q(4, 0, 405) ); sigmaT.push_back( new Sigma2qg2QQbar3PJ1q(4, 1, 406) ); sigmaU.push_back( new Sigma2qg2QQbar3PJ1q(4, 1, 406) ); sigmaT.push_back( new Sigma2qg2QQbar3PJ1q(4, 2, 407) ); sigmaU.push_back( new Sigma2qg2QQbar3PJ1q(4, 2, 407) ); sigmaT.push_back( new Sigma2qg2QQbarX8q(4, 0, 414) ); sigmaU.push_back( new Sigma2qg2QQbarX8q(4, 0, 414) ); sigmaT.push_back( new Sigma2qg2QQbarX8q(4, 1, 415) ); sigmaU.push_back( new Sigma2qg2QQbarX8q(4, 1, 415) ); sigmaT.push_back( new Sigma2qg2QQbarX8q(4, 2, 416) ); sigmaU.push_back( new Sigma2qg2QQbarX8q(4, 2, 416) ); sigmaT.push_back( new Sigma2qg2QQbar3PJ1q(5, 0, 505) ); sigmaU.push_back( new Sigma2qg2QQbar3PJ1q(5, 0, 505) ); sigmaT.push_back( new Sigma2qg2QQbar3PJ1q(5, 1, 506) ); sigmaU.push_back( new Sigma2qg2QQbar3PJ1q(5, 1, 506) ); sigmaT.push_back( new Sigma2qg2QQbar3PJ1q(5, 2, 507) ); sigmaU.push_back( new Sigma2qg2QQbar3PJ1q(5, 2, 507) ); sigmaT.push_back( new Sigma2qg2QQbarX8q(5, 0, 514) ); sigmaU.push_back( new Sigma2qg2QQbarX8q(5, 0, 514) ); sigmaT.push_back( new Sigma2qg2QQbarX8q(5, 1, 515) ); sigmaU.push_back( new Sigma2qg2QQbarX8q(5, 1, 515) ); sigmaT.push_back( new Sigma2qg2QQbarX8q(5, 2, 516) ); sigmaU.push_back( new Sigma2qg2QQbarX8q(5, 2, 516) ); } else if (inState == 2) { sigmaT.push_back( new Sigma2qqbar2QQbar3PJ1g(4, 0, 408) ); sigmaU.push_back( new Sigma2qqbar2QQbar3PJ1g(4, 0, 408) ); sigmaT.push_back( new Sigma2qqbar2QQbar3PJ1g(4, 1, 409) ); sigmaU.push_back( new Sigma2qqbar2QQbar3PJ1g(4, 1, 409) ); sigmaT.push_back( new Sigma2qqbar2QQbar3PJ1g(4, 2, 410) ); sigmaU.push_back( new Sigma2qqbar2QQbar3PJ1g(4, 2, 410) ); sigmaT.push_back( new Sigma2qqbar2QQbarX8g(4, 0, 417) ); sigmaU.push_back( new Sigma2qqbar2QQbarX8g(4, 0, 417) ); sigmaT.push_back( new Sigma2qqbar2QQbarX8g(4, 1, 418) ); sigmaU.push_back( new Sigma2qqbar2QQbarX8g(4, 1, 418) ); sigmaT.push_back( new Sigma2qqbar2QQbarX8g(4, 2, 419) ); sigmaU.push_back( new Sigma2qqbar2QQbarX8g(4, 2, 419) ); sigmaT.push_back( new Sigma2qqbar2QQbar3PJ1g(5, 0, 508) ); sigmaU.push_back( new Sigma2qqbar2QQbar3PJ1g(5, 0, 508) ); sigmaT.push_back( new Sigma2qqbar2QQbar3PJ1g(5, 1, 509) ); sigmaU.push_back( new Sigma2qqbar2QQbar3PJ1g(5, 1, 509) ); sigmaT.push_back( new Sigma2qqbar2QQbar3PJ1g(5, 2, 510) ); sigmaU.push_back( new Sigma2qqbar2QQbar3PJ1g(5, 2, 510) ); sigmaT.push_back( new Sigma2qqbar2QQbarX8g(5, 0, 517) ); sigmaU.push_back( new Sigma2qqbar2QQbarX8g(5, 0, 517) ); sigmaT.push_back( new Sigma2qqbar2QQbarX8g(5, 1, 518) ); sigmaU.push_back( new Sigma2qqbar2QQbarX8g(5, 1, 518) ); sigmaT.push_back( new Sigma2qqbar2QQbarX8g(5, 2, 519) ); sigmaU.push_back( new Sigma2qqbar2QQbarX8g(5, 2, 519) ); } } // Resize arrays to match sizes above. nChan = sigmaT.size(); needMasses.resize(nChan); m3Fix.resize(nChan); m4Fix.resize(nChan); sHatMin.resize(nChan); sigmaTval.resize(nChan); sigmaUval.resize(nChan); // Initialize the processes. for (int i = 0; i < nChan; ++i) { sigmaT[i]->init( infoPtr, settingsPtr, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr); sigmaT[i]->initProc(); sigmaU[i]->init( infoPtr, settingsPtr, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr); sigmaU[i]->initProc(); // Prepare for massive kinematics (but fixed masses!) where required. needMasses[i] = false; int id3Mass = sigmaT[i]->id3Mass(); int id4Mass = sigmaT[i]->id4Mass(); m3Fix[i] = 0.; m4Fix[i] = 0.; if (id3Mass > 0 || id4Mass > 0) { needMasses[i] = true; m3Fix[i] = particleDataPtr->m0(id3Mass); m4Fix[i] = particleDataPtr->m0(id4Mass); } sHatMin[i] = pow2( m3Fix[i] + m4Fix[i] + MASSMARGIN); } // Done. return true; } //-------------------------------------------------------------------------- // Calculate cross section summed over possibilities. double SigmaMultiparton::sigma( int id1, int id2, double x1, double x2, double sHat, double tHat, double uHat, double alpS, double alpEM, bool restore, bool pickOtherIn) { // Choose either the dominant process (in slot 0) or the rest of them. if (restore) pickOther = pickOtherIn; else pickOther = (rndmPtr->flat() < OTHERFRAC); // Iterate over all subprocesses. sigmaTsum = 0.; sigmaUsum = 0.; for (int i = 0; i < nChan; ++i) { sigmaTval[i] = 0.; sigmaUval[i] = 0.; // Skip the not chosen processes. if (i == 0 && pickOther) continue; if (i > 0 && !pickOther) continue; // t-channel-sampling contribution. if (sHat > sHatMin[i]) { sigmaT[i]->set2KinMPI( x1, x2, sHat, tHat, uHat, alpS, alpEM, needMasses[i], m3Fix[i], m4Fix[i]); sigmaTval[i] = sigmaT[i]->sigmaHatWrap(id1, id2); sigmaT[i]->pickInState(id1, id2); // Correction factor for tHat rescaling in massive kinematics. if (needMasses[i]) sigmaTval[i] *= sigmaT[i]->sHBetaMPI() / sHat; sigmaTsum += sigmaTval[i]; } // u-channel-sampling contribution. if (sHat > sHatMin[i]) { sigmaU[i]->set2KinMPI( x1, x2, sHat, uHat, tHat, alpS, alpEM, needMasses[i], m3Fix[i], m4Fix[i]); sigmaUval[i] = sigmaU[i]->sigmaHatWrap( id1, id2); sigmaU[i]->pickInState(id1, id2); // Correction factor for tHat rescaling in massive kinematics. if (needMasses[i]) sigmaUval[i] *= sigmaU[i]->sHBetaMPI() / sHat; sigmaUsum += sigmaUval[i]; } // Average of t- and u-channel sampling; corrected for not selected channels. } double sigmaAvg = 0.5 * (sigmaTsum + sigmaUsum); if (pickOther) sigmaAvg /= OTHERFRAC; if (!pickOther) sigmaAvg /= (1. - OTHERFRAC); return sigmaAvg; } //-------------------------------------------------------------------------- // Return one subprocess, picked according to relative cross sections. SigmaProcess* SigmaMultiparton::sigmaSel() { // Decide between t- and u-channel-sampled kinematics. pickedU = (rndmPtr->flat() * (sigmaTsum + sigmaUsum) < sigmaUsum); // Pick one of t-channel-sampled processes. if (!pickedU) { double sigmaRndm = sigmaTsum * rndmPtr->flat(); int iPick = -1; do sigmaRndm -= sigmaTval[++iPick]; while (sigmaRndm > 0.); return sigmaT[iPick]; // Pick one of u-channel-sampled processes. } else { double sigmaRndm = sigmaUsum * rndmPtr->flat(); int iPick = -1; do sigmaRndm -= sigmaUval[++iPick]; while (sigmaRndm > 0.); return sigmaU[iPick]; } } //========================================================================== // The MultipartonInteractions class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Factorization scale pT2 by default, but could be shifted to pT2 + pT02. // (A priori possible, but problems for flavour threshold interpretation.) const bool MultipartonInteractions::SHIFTFACSCALE = false; // Pick one parton to represent rescattering cross section to speed up. const bool MultipartonInteractions::PREPICKRESCATTER = true; // Naive upper estimate of cross section too pessimistic, so reduce by this. const double MultipartonInteractions::SIGMAFUDGE = 0.8; // The r value above, picked to allow a flatter correct/trial cross section. const double MultipartonInteractions::RPT20 = 0.25; // Reduce pT0 by factor pT0STEP if sigmaInt < SIGMASTEP * sigmaND. const double MultipartonInteractions::PT0STEP = 0.9; const double MultipartonInteractions::SIGMASTEP = 1.1; // Stop if pT0 or pTmin fall below this, or alpha_s blows up. const double MultipartonInteractions::PT0MIN = 0.2; // Refuse too low expPow in impact parameter profile. const double MultipartonInteractions::EXPPOWMIN = 0.4; // Define low-b region by interaction rate above given number. const double MultipartonInteractions::PROBATLOWB = 0.6; // Basic step size for b integration; sometimes modified. const double MultipartonInteractions::BSTEP = 0.01; // Stop b integration when integrand dropped enough. const double MultipartonInteractions::BMAX = 1e-8; // Do not allow too large argument to exp function. const double MultipartonInteractions::EXPMAX = 50.; // Convergence criterion for k iteration. const double MultipartonInteractions::KCONVERGE = 1e-7; // Conversion of GeV^{-2} to mb for cross section. const double MultipartonInteractions::CONVERT2MB = 0.389380; // Stay away from division by zero in Jacobian for tHat -> pT2. const double MultipartonInteractions::ROOTMIN = 0.01; // No need to reinitialize parameters if energy close to previous. const double MultipartonInteractions::ECMDEV = 0.01; // Settings for x-dependent matter profile: // Number of bins in b (with these settings, no bStep increase and // reintegration needed with a1 ~ 0.20 up to ECM ~ 40TeV). const int MultipartonInteractions::XDEP_BBIN = 500; // Initial value of a0. const double MultipartonInteractions::XDEP_A0 = 1.0; // Width of form ( XDEP_A1 + a1 * log(1 / x) ). const double MultipartonInteractions::XDEP_A1 = 1.0; // Initial step size in b and increment. const double MultipartonInteractions::XDEP_BSTEP = 0.02; const double MultipartonInteractions::XDEP_BSTEPINC = 0.01; // Overlap-weighted cross section in last bin of b must be beneath // XDEP_CUTOFF * sigmaInt. const double MultipartonInteractions::XDEP_CUTOFF = 1e-4; // a0 is calculated in units of sqrt(mb), so convert to fermi. const double MultipartonInteractions::XDEP_SMB2FM = sqrt(0.1); // Only write warning when weight clearly above unity. const double MultipartonInteractions::WTACCWARN = 1.1; //-------------------------------------------------------------------------- // Initialize the generation process for given beams. bool MultipartonInteractions::init( bool doMPIinit, int iDiffSysIn, Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtr, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, Couplings* couplingsPtrIn, PartonSystems* partonSystemsPtrIn, SigmaTotal* sigmaTotPtrIn, UserHooks* userHooksPtrIn, ostream& os) { // Store input pointers for future use. Done if no initialization. iDiffSys = iDiffSysIn; infoPtr = infoPtrIn; rndmPtr = rndmPtrIn; beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; couplingsPtr = couplingsPtrIn; partonSystemsPtr = partonSystemsPtrIn; sigmaTotPtr = sigmaTotPtrIn; userHooksPtr = userHooksPtrIn; if (!doMPIinit) return false; // If both beams are baryons then softer PDF's than for mesons/Pomerons. hasBaryonBeams = ( beamAPtr->isBaryon() && beamBPtr->isBaryon() ); // Matching in pT of hard interaction to further interactions. pTmaxMatch = settings.mode("MultipartonInteractions:pTmaxMatch"); // Parameters of alphaStrong generation. alphaSvalue = settings.parm("MultipartonInteractions:alphaSvalue"); alphaSorder = settings.mode("MultipartonInteractions:alphaSorder"); alphaSnfmax = settings.mode("StandardModel:alphaSnfmax"); // Parameters of alphaEM generation. alphaEMorder = settings.mode("MultipartonInteractions:alphaEMorder"); // Parameters of cross section generation. Kfactor = settings.parm("MultipartonInteractions:Kfactor"); // Regularization of QCD evolution for pT -> 0. pT0Ref = settings.parm("MultipartonInteractions:pT0Ref"); ecmRef = settings.parm("MultipartonInteractions:ecmRef"); ecmPow = settings.parm("MultipartonInteractions:ecmPow"); pTmin = settings.parm("MultipartonInteractions:pTmin"); // Impact parameter profile: nondiffractive topologies. if (iDiffSys == 0) { bProfile = settings.mode("MultipartonInteractions:bProfile"); coreRadius = settings.parm("MultipartonInteractions:coreRadius"); coreFraction = settings.parm("MultipartonInteractions:coreFraction"); expPow = settings.parm("MultipartonInteractions:expPow"); expPow = max(EXPPOWMIN, expPow); // x-dependent impact parameter profile. a1 = settings.parm("MultipartonInteractions:a1"); // Impact parameter profile: diffractive topologies. } else { bProfile = settings.mode("Diffraction:bProfile"); coreRadius = settings.parm("Diffraction:coreRadius"); coreFraction = settings.parm("Diffraction:coreFraction"); expPow = settings.parm("Diffraction:expPow"); expPow = max(EXPPOWMIN, expPow); } // Common choice of "pT" scale for determining impact parameter. bSelScale = settings.mode("MultipartonInteractions:bSelScale"); // Process sets to include in machinery. processLevel = settings.mode("MultipartonInteractions:processLevel"); // Parameters of rescattering description. allowRescatter = settings.flag("MultipartonInteractions:allowRescatter"); allowDoubleRes = settings.flag("MultipartonInteractions:allowDoubleRescatter"); rescatterMode = settings.mode("MultipartonInteractions:rescatterMode"); ySepResc = settings.parm("MultipartonInteractions:ySepRescatter"); deltaYResc = settings.parm("MultipartonInteractions:deltaYRescatter"); // Rescattering not yet implemented for x-dependent impact profile. if (bProfile == 4) allowRescatter = false; // A global recoil FSR stategy restricts rescattering. globalRecoilFSR = settings.flag("TimeShower:globalRecoil"); nMaxGlobalRecoilFSR = settings.mode("TimeShower:nMaxGlobalRecoil"); // Various other parameters. nQuarkIn = settings.mode("MultipartonInteractions:nQuarkIn"); nSample = settings.mode("MultipartonInteractions:nSample"); // Optional dampening at small pT's when large multiplicities. enhanceScreening = settings.mode("MultipartonInteractions:enhanceScreening"); // Parameters for diffractive systems. sigmaPomP = settings.parm("Diffraction:sigmaRefPomP"); mPomP = settings.parm("Diffraction:mRefPomP"); pPomP = settings.parm("Diffraction:mPowPomP"); mMinPertDiff = settings.parm("Diffraction:mMinPert"); // Possibility to allow user veto of MPI canVetoMPI = (userHooksPtr != 0) ? userHooksPtr->canVetoMPIEmission() : false; // Some common combinations for double Gaussian, as shorthand. if (bProfile == 2) { fracA = pow2(1. - coreFraction); fracB = 2. * coreFraction * (1. - coreFraction); fracC = pow2(coreFraction); radius2B = 0.5 * (1. + pow2(coreRadius)); radius2C = pow2(coreRadius); // Some common combinations for exp(b^pow), as shorthand. } else if (bProfile == 3) { hasLowPow = (expPow < 2.); expRev = 2. / expPow - 1.; } // Initialize alpha_strong generation. alphaS.init( alphaSvalue, alphaSorder, alphaSnfmax, false); double Lambda3 = alphaS.Lambda3(); // Initialize alphaEM generation. alphaEM.init( alphaEMorder, &settings); // Attach matrix-element calculation objects. sigma2gg.init( 0, processLevel, infoPtr, &settings, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr); sigma2qg.init( 1, processLevel, infoPtr, &settings, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr); sigma2qqbarSame.init( 2, processLevel, infoPtr, &settings, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr); sigma2qq.init( 3, processLevel, infoPtr, &settings, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr); // Calculate invariant mass of system. eCM = infoPtr->eCM(); sCM = eCM * eCM; mMaxPertDiff = eCM; eCMsave = eCM; // Get the total inelastic and nondiffractive cross section. if (!sigmaTotPtr->hasSigmaTot()) return false; bool isNonDiff = (iDiffSys == 0); sigmaND = sigmaTotPtr->sigmaND(); double sigmaMaxViol = 0.; // Output initialization info - first part. bool showMPI = settings.flag("Init:showMultipartonInteractions"); if (showMPI) { os << "\n *------- PYTHIA Multiparton Interactions Initialization " << "---------* \n" << " | " << " | \n"; if (isNonDiff) os << " | sigmaNonDiffractive = " << fixed << setprecision(2) << setw(7) << sigmaND << " mb | \n"; else if (iDiffSys == 1) os << " | diffraction XB " << " | \n"; else if (iDiffSys == 2) os << " | diffraction AX " << " | \n"; else if (iDiffSys == 3) os << " | diffraction AXB " << " | \n"; os << " | " << " | \n"; } // For diffraction need to cover range of diffractive masses. nStep = (iDiffSys == 0) ? 1 : 5; eStepSize = (nStep < 2) ? 1. : log(mMaxPertDiff / mMinPertDiff) / (nStep - 1.); for (int iStep = 0; iStep < nStep; ++iStep) { // Update and output current diffractive mass and // fictitious Pomeron-proton cross section for normalization. if (nStep > 1) { eCM = mMinPertDiff * pow( mMaxPertDiff / mMinPertDiff, iStep / (nStep - 1.) ); sCM = eCM * eCM; sigmaND = sigmaPomP * pow( eCM / mPomP, pPomP); if (showMPI) os << " | diffractive mass = " << scientific << setprecision(3) << setw(9) << eCM << " GeV and sigmaNorm = " << fixed << setw(6) << sigmaND << " mb | \n"; } // Set current pT0 scale. pT0 = pT0Ref * pow(eCM / ecmRef, ecmPow); // The pT0 value may need to be decreased, if sigmaInt < sigmaND. double pT4dSigmaMaxBeg = 0.; for ( ; ; ) { // Derived pT kinematics combinations. pT20 = pT0*pT0; pT2min = pTmin*pTmin; pTmax = 0.5*eCM; pT2max = pTmax*pTmax; pT20R = RPT20 * pT20; pT20minR = pT2min + pT20R; pT20maxR = pT2max + pT20R; pT20min0maxR = pT20minR * pT20maxR; pT2maxmin = pT2max - pT2min; // Provide upper estimate of interaction rate d(Prob)/d(pT2). upperEnvelope(); // Setup binning in b for x-dependent matter profile. if (bProfile == 4) { sigmaIntWgt.resize(XDEP_BBIN); sigmaSumWgt.resize(XDEP_BBIN); bstepNow = XDEP_BSTEP; } // Integrate the parton-parton interaction cross section. pT4dSigmaMaxBeg = pT4dSigmaMax; jetCrossSection(); // If the overlap-weighted cross section has not fallen below // cutoff, then increase bin size in b and reintegrate. while (bProfile == 4 && sigmaIntWgt[XDEP_BBIN - 1] > XDEP_CUTOFF * sigmaInt) { bstepNow += XDEP_BSTEPINC; jetCrossSection(); } // Sufficiently big SigmaInt or reduce pT0; maybe also pTmin. if (sigmaInt > SIGMASTEP * sigmaND) break; if (showMPI) os << fixed << setprecision(2) << " | pT0 = " << setw(5) << pT0 << " gives sigmaInteraction = " << setw(7) << sigmaInt << " mb: rejected | \n"; if (pTmin > pT0) pTmin *= PT0STEP; pT0 *= PT0STEP; // Give up if pT0 and pTmin fall too low. if ( max(pT0, pTmin) < max(PT0MIN, Lambda3) ) { infoPtr->errorMsg("Error in MultipartonInteractions::init:" " failed to find acceptable pT0 and pTmin"); infoPtr->setTooLowPTmin(true); return false; } } // Output for accepted pT0. if (showMPI) os << fixed << setprecision(2) << " | pT0 = " << setw(5) << pT0 << " gives sigmaInteraction = "<< setw(7) << sigmaInt << " mb: accepted | \n"; // Calculate factor relating matter overlap and interaction rate. overlapInit(); // Maximum violation relative to first estimate. sigmaMaxViol = max( sigmaMaxViol, pT4dSigmaMax / pT4dSigmaMaxBeg); // Save values calculated. if (nStep > 1) { pT0Save[iStep] = pT0; pT4dSigmaMaxSave[iStep] = pT4dSigmaMax; pT4dProbMaxSave[iStep] = pT4dProbMax; sigmaIntSave[iStep] = sigmaInt; for (int j = 0; j <= 100; ++j) sudExpPTSave[iStep][j] = sudExpPT[j]; zeroIntCorrSave[iStep] = zeroIntCorr; normOverlapSave[iStep] = normOverlap; kNowSave[iStep] = kNow; bAvgSave[iStep] = bAvg; bDivSave[iStep] = bDiv; probLowBSave[iStep] = probLowB; fracAhighSave[iStep] = fracAhigh; fracBhighSave[iStep] = fracBhigh; fracChighSave[iStep] = fracBhigh; fracABChighSave[iStep] = fracABChigh; cDivSave[iStep] = cDiv; cMaxSave[iStep] = cMax; } // End of loop over diffractive masses. } // Output details for x-dependent matter profile. if (bProfile == 4 && showMPI) os << " | " << " | \n" << fixed << setprecision(2) << " | x-dependent matter profile: a1 = " << a1 << ", " << "a0 = " << a0now * XDEP_SMB2FM << ", bStep = " << bstepNow << " | \n"; // End initialization printout. if (showMPI) os << " | " << " | \n" << " *------- End PYTHIA Multiparton Interactions Initialization" << " -----* " << endl; // Amount of violation from upperEnvelope to jetCrossSection. if (sigmaMaxViol > 1.) { ostringstream osWarn; osWarn << "by factor " << fixed << setprecision(3) << sigmaMaxViol; infoPtr->errorMsg("Warning in MultipartonInteractions::init:" " maximum increased", osWarn.str()); } // Reset statistics. SigmaMultiparton* dSigma; for (int i = 0; i < 4; ++i) { if (i == 0) dSigma = &sigma2gg; else if (i == 1) dSigma = &sigma2qg; else if (i == 2) dSigma = &sigma2qqbarSame; else dSigma = &sigma2qq; int nProc = dSigma->nProc(); for (int iProc = 0; iProc < nProc; ++iProc) nGen[ dSigma->codeProc(iProc) ] = 0; } // Additional setup for x-dependent matter profile. if (bProfile == 4) { sigmaIntWgt.clear(); sigmaSumWgt.clear(); } // No preselection of sea/valence content and initialise a0. vsc1 = 0; vsc2 = 0; // Done. return true; } //-------------------------------------------------------------------------- // Reset impact parameter choice and update the CM energy. // For diffraction also interpolate parameters to current CM energy. void MultipartonInteractions::reset( ) { // Reset impact parameter choice. bIsSet = false; bSetInFirst = false; // Update CM energy. Done if not diffraction and not new energy. eCM = infoPtr->eCM(); sCM = eCM * eCM; if (nStep == 1 || abs( eCM / eCMsave - 1.) < ECMDEV) return; // Set fictitious Pomeron-proton cross section for diffractive system. sigmaND = sigmaPomP * pow( eCM / mPomP, pPomP); // Current interpolation point. eCMsave = eCM; eStepSave = log(eCM / mMinPertDiff) / eStepSize; iStepFrom = max( 0, min( nStep - 2, int( eStepSave) ) ); iStepTo = iStepFrom + 1; eStepTo = max( 0., min( 1., eStepSave - iStepFrom) ); eStepFrom = 1. - eStepTo; // Update pT0 and combinations derived from it. pT0 = eStepFrom * pT0Save[iStepFrom] + eStepTo * pT0Save[iStepTo]; pT20 = pT0*pT0; pT2min = pTmin*pTmin; pTmax = 0.5*eCM; pT2max = pTmax*pTmax; pT20R = RPT20 * pT20; pT20minR = pT2min + pT20R; pT20maxR = pT2max + pT20R; pT20min0maxR = pT20minR * pT20maxR; pT2maxmin = pT2max - pT2min; // Update other parameters used in pT choice. pT4dSigmaMax = eStepFrom * pT4dSigmaMaxSave[iStepFrom] + eStepTo * pT4dSigmaMaxSave[iStepTo]; pT4dProbMax = eStepFrom * pT4dProbMaxSave[iStepFrom] + eStepTo * pT4dProbMaxSave[iStepTo]; sigmaInt = eStepFrom * sigmaIntSave[iStepFrom] + eStepTo * sigmaIntSave[iStepTo]; for (int j = 0; j <= 100; ++j) sudExpPT[j] = eStepFrom * sudExpPTSave[iStepFrom][j] + eStepTo * sudExpPTSave[iStepTo][j]; // Update parameters related to the impact-parameter picture. zeroIntCorr = eStepFrom * zeroIntCorrSave[iStepFrom] + eStepTo * zeroIntCorrSave[iStepTo]; normOverlap = eStepFrom * normOverlapSave[iStepFrom] + eStepTo * normOverlapSave[iStepTo]; kNow = eStepFrom * kNowSave[iStepFrom] + eStepTo * kNowSave[iStepTo]; bAvg = eStepFrom * bAvgSave[iStepFrom] + eStepTo * bAvgSave[iStepTo]; bDiv = eStepFrom * bDivSave[iStepFrom] + eStepTo * bDivSave[iStepTo]; probLowB = eStepFrom * probLowBSave[iStepFrom] + eStepTo * probLowBSave[iStepTo]; fracAhigh = eStepFrom * fracAhighSave[iStepFrom] + eStepTo * fracAhighSave[iStepTo]; fracBhigh = eStepFrom * fracBhighSave[iStepFrom] + eStepTo * fracBhighSave[iStepTo]; fracChigh = eStepFrom * fracChighSave[iStepFrom] + eStepTo * fracChighSave[iStepTo]; fracABChigh = eStepFrom * fracABChighSave[iStepFrom] + eStepTo * fracABChighSave[iStepTo]; cDiv = eStepFrom * cDivSave[iStepFrom] + eStepTo * cDivSave[iStepTo]; cMax = eStepFrom * cMaxSave[iStepFrom] + eStepTo * cMaxSave[iStepTo]; } //-------------------------------------------------------------------------- // Select first = hardest pT in nondiffractive process. // Requires separate treatment at low and high b values. void MultipartonInteractions::pTfirst() { // Pick impact parameter and thereby interaction rate enhancement. // This is not used for the x-dependent matter profile, which // instead uses trial interactions. if (bProfile == 4) isAtLowB = false; else overlapFirst(); bSetInFirst = true; double WTacc; // At low b values evolve downwards with Sudakov. if (isAtLowB) { pT2 = pT2max; do { // Pick a pT using a quick-and-dirty cross section estimate. pT2 = fastPT2(pT2); // If fallen below lower cutoff then need to restart at top. if (pT2 < pT2min) { pT2 = pT2max; WTacc = 0.; // Else pick complete kinematics and evaluate cross-section correction. } else { WTacc = sigmaPT2scatter(true) / dSigmaApprox; if (WTacc > WTACCWARN) infoPtr->errorMsg("Warning in " "MultipartonInteractions::pTfirst: weight above unity"); } // Loop until acceptable pT and acceptable kinematics. } while (WTacc < rndmPtr->flat() || !dSigmaDtSel->final2KinMPI()); // At high b values make preliminary pT choice without Sudakov factor. } else { while (true) { do { pT2 = pT20min0maxR / (pT20minR + rndmPtr->flat() * pT2maxmin) - pT20R; // Evaluate upper estimate of cross section for this pT2 choice. dSigmaApprox = pT4dSigmaMax / pow2(pT2 + pT20R); // Pick complete kinematics and evaluate cross-section correction. WTacc = sigmaPT2scatter(true) / dSigmaApprox; // Evaluate and include Sudakov factor. if (bProfile != 4) WTacc *= sudakov( pT2, enhanceB); // Warn for weight above unity if (WTacc > WTACCWARN) infoPtr->errorMsg("Warning in " "MultipartonInteractions::pTfirst: weight above unity"); // Loop until acceptable pT and acceptable kinematics. } while (WTacc < rndmPtr->flat() || !dSigmaDtSel->final2KinMPI()); // For x-dependent matter profile, use trial interactions to // generate Sudakov, otherwise done. if (bProfile != 4) break; else { // Save details of the original hard interaction. pT2Save = pT2; id1Save = id1; id2Save = id2; x1Save = x1; x2Save = x2; sHatSave = sHat; tHatSave = tHat; uHatSave = uHat; alpSsave = alpS; alpEMsave = alpEM; pT2FacSave = pT2Fac; pT2RenSave = pT2Ren; xPDF1nowSave = xPDF1now; xPDF2nowSave = xPDF2now; // Save accepted kinematics and pointer to SigmaProcess. dSigmaDtSel->saveKin(); dSigmaDtSelSave = dSigmaDtSel; // Put x1, x2 information into beam pointers to get correct // PDF rescaling in trial interaction (for hard process, can // be sea or valence, not companion). beamAPtr->append( 0, id1, x1); beamAPtr->xfISR( 0, id1, x1, pT2Fac * pT2Fac); vsc1 = beamAPtr->pickValSeaComp(); beamBPtr->append( 0, id2, x2); beamBPtr->xfISR( 0, id2, x2, pT2Fac * pT2Fac); vsc2 = beamBPtr->pickValSeaComp(); // Pick b according to O(b, x1, x2). double w1 = XDEP_A1 + a1 * log(1. / x1); double w2 = XDEP_A1 + a1 * log(1. / x2); double fac = a02now * (w1 * w1 + w2 * w2); double expb2 = rndmPtr->flat(); b2now = - fac * log(expb2); bNow = sqrt(b2now); // Enhancement factor for the hard process and overestimate // for fastPT2. Note that existing framework has a (1. / sigmaND) // present. enhanceB = sigmaND / M_PI / fac * expb2; enhanceBmax = sigmaND / 2. / M_PI / a02now * exp( -b2now / 2. / a2max ); // Trial interaction with dummy event. Event evDummy; double pTtrial = pTnext(pTmax, pTmin, evDummy); // Restore beams. beamAPtr->clear(); beamBPtr->clear(); // Accept if fallen beneath factorisation scale. if (pTtrial < sqrt(pT2FacSave)) { // Restore previous values and original sigma. swap(pT2, pT2Save); swap(pT2Fac, pT2FacSave); swap(pT2Ren, pT2RenSave); swap(id1, id1Save); swap(id2, id2Save); swap(x1, x1Save); swap(x2, x2Save); swap(sHat, sHatSave); swap(tHat, tHatSave); swap(uHat, uHatSave); swap(alpS, alpSsave); swap(alpEM, alpEMsave); swap(xPDF1now, xPDF1nowSave); swap(xPDF2now, xPDF2nowSave); if (dSigmaDtSel == dSigmaDtSelSave) dSigmaDtSel->swapKin(); else swap(dSigmaDtSel, dSigmaDtSelSave); // Accept. bIsSet = true; break; } } // if (bProfile == 4) } // while (true) // End handling for high b. } } //-------------------------------------------------------------------------- // Set up kinematics for first = hardest pT in nondiffractive process. void MultipartonInteractions::setupFirstSys( Event& process) { // Last beam-status particles. Offset relative to normal beam locations. int sizeProc = process.size(); int nBeams = 3; for (int i = 3; i < sizeProc; ++i) if (process[i].statusAbs() < 20) nBeams = i + 1; int nOffset = nBeams - 3; // Remove any partons of previous failed interactions. if (sizeProc > nBeams) { process.popBack( sizeProc - nBeams); process.initColTag(); } // Entries 3 and 4, now to be added, come from 1 and 2. process[1 + nOffset].daughter1(3 + nOffset); process[2 + nOffset].daughter1(4 + nOffset); // Negate beam status, if not already done. (Case with offset beams.) process[1 + nOffset].statusNeg(); process[2 + nOffset].statusNeg(); // Loop over four partons and offset info relative to subprocess itself. int colOffset = process.lastColTag(); for (int i = 1; i <= 4; ++i) { Particle parton = dSigmaDtSel->getParton(i); if (i <= 2 ) parton.mothers( i + nOffset, 0); else parton.mothers( 3 + nOffset, 4 + nOffset); if (i <= 2 ) parton.daughters( 5 + nOffset, 6 + nOffset); else parton.daughters( 0, 0); int col = parton.col(); if (col > 0) parton.col( col + colOffset); int acol = parton.acol(); if (acol > 0) parton.acol( acol + colOffset); // Put the partons into the event record. process.append(parton); } // Set scale from which to begin evolution. process.scale( sqrt(pT2Fac) ); // Info on subprocess - specific to mimimum-bias events. string nameSub = dSigmaDtSel->name(); int codeSub = dSigmaDtSel->code(); int nFinalSub = dSigmaDtSel->nFinal(); double pTMPI = dSigmaDtSel->pTMPIFin(); infoPtr->setSubType( iDiffSys, nameSub, codeSub, nFinalSub); if (iDiffSys == 0) infoPtr->setTypeMPI( codeSub, pTMPI, 0, 0, enhanceB / zeroIntCorr); // Further standard info on process. infoPtr->setPDFalpha( iDiffSys, id1, id2, x1, x2, xPDF1now, xPDF2now, pT2Fac, alpEM, alpS, pT2Ren, 0.); double m3 = dSigmaDtSel->m(3); double m4 = dSigmaDtSel->m(4); double theta = dSigmaDtSel->thetaMPI(); double phi = dSigmaDtSel->phiMPI(); infoPtr->setKin( iDiffSys, id1, id2, x1, x2, sHat, tHat, uHat, sqrt(pT2), m3, m4, theta, phi); } //-------------------------------------------------------------------------- // Find whether to limit maximum scale of emissions. bool MultipartonInteractions::limitPTmax( Event& event) { // User-set cases. if (pTmaxMatch == 1) return true; if (pTmaxMatch == 2) return false; // Look if only quarks (u, d, s, c, b), gluons and photons in final state. bool onlyQGP1 = true; bool onlyQGP2 = true; int n21 = 0; for (int i = 5; i < event.size(); ++i) { if (event[i].status() == -21) ++n21; else if (n21 == 0) { int idAbs = event[i].idAbs(); if (idAbs > 5 && idAbs != 21 && idAbs != 22) onlyQGP1 = false; } else if (n21 == 2) { int idAbs = event[i].idAbs(); if (idAbs > 5 && idAbs != 21 && idAbs != 22) onlyQGP2 = false; } } // If two hard interactions then limit if one only contains q/g/gamma. bool onlyQGP = (n21 == 2) ? (onlyQGP1 || onlyQGP2) : onlyQGP1; return (onlyQGP); } //-------------------------------------------------------------------------- // Select next pT in downwards evolution. double MultipartonInteractions::pTnext( double pTbegAll, double pTendAll, Event& event) { // Initial values. bool pickRescatter, acceptKin; double dSigmaScatter, dSigmaRescatter, WTacc; double pT2end = pow2( max(pTmin, pTendAll) ); // With the x-dependent matter profile, it is possible to reuse // values that have been stored during trial interactions for a // slight speedup. bIsSet is false during trial interactions, // counter 21 in case partonLevel is retried and counter 22 for // the first pass through partonLevel. if (bProfile == 4 && bIsSet && infoPtr->getCounter(21) == 1 && infoPtr->getCounter(22) == 1) { // Minimum bias. if (bSetInFirst) { if (pT2Save < pT2end) return 0.; pT2 = pT2Save; pT2Fac = pT2FacSave; pT2Ren = pT2RenSave; id1 = id1Save; id2 = id2Save; x1 = x1Save; x2 = x2Save; sHat = sHatSave; tHat = tHatSave; uHat = uHatSave; alpS = alpSsave; alpEM = alpEMsave; xPDF1now = xPDF1nowSave; xPDF2now = xPDF2nowSave; if (dSigmaDtSel == dSigmaDtSelSave) dSigmaDtSel->swapKin(); else dSigmaDtSel = dSigmaDtSelSave; return sqrt(pT2); // Hard process. } else { return (pT2 < pT2end) ? 0. : sqrt(pT2); } } // Do not allow rescattering while sill FSR with global recoil. bool allowRescatterNow = allowRescatter; if (globalRecoilFSR && partonSystemsPtr->sizeOut(0) <= nMaxGlobalRecoilFSR) allowRescatterNow = false; // Initial pT2 value. pT2 = pow2(pTbegAll); // Find the set of already scattered partons on the two sides. if (allowRescatterNow) findScatteredPartons( event); // Pick a pT2 using a quick-and-dirty cross section estimate. do { do { pT2 = fastPT2(pT2); if (pT2 < pT2end) return 0.; // Initial values: no rescattering. i1Sel = 0; i2Sel = 0; dSigmaSum = 0.; pickRescatter = false; // Pick complete kinematics and evaluate interaction cross-section. dSigmaScatter = sigmaPT2scatter(false); // Also cross section from rescattering if allowed. dSigmaRescatter = (allowRescatterNow) ? sigmaPT2rescatter( event) : 0.; // Normalize to dSigmaApprox, which was set in fastPT2 above. WTacc = (dSigmaScatter + dSigmaRescatter) / dSigmaApprox; if (WTacc > WTACCWARN) infoPtr->errorMsg("Warning in " "MultipartonInteractions::pTnext: weight above unity"); // Idea suggested by Gosta Gustafson: increased screening in events // with large activity can be simulated by pT0_eff = sqrt(n) * pT0. if (enhanceScreening > 0) { int nSysNow = infoPtr->nMPI() + 1; if (enhanceScreening == 2) nSysNow += infoPtr->nISR(); double WTscreen = pow2( (pT2 + pT20) / (pT2 + nSysNow * pT20) ); WTacc *= WTscreen; } // x-dependent matter profile overlap weighting. if (bProfile == 4) { double w1 = XDEP_A1 + a1 * log(1. / x1); double w2 = XDEP_A1 + a1 * log(1. / x2); double fac = a02now * (w1 * w1 + w2 * w2); // Correct enhancement factor and weight enhanceBnow = sigmaND / M_PI / fac * exp( - b2now / fac); double oWgt = enhanceBnow / enhanceBmax; if (oWgt > 1.0000000001) infoPtr->errorMsg("Warning in Multiparton" "Interactions::pTnext: overlap weight above unity"); WTacc *= oWgt; } // Decide whether to keep the event based on weight. } while (WTacc < rndmPtr->flat()); // When rescattering possible: new interaction or rescattering? if (allowRescatterNow) { pickRescatter = (i1Sel > 0 || i2Sel > 0); // Restore kinematics for selected scattering/rescattering. id1 = id1Sel; id2 = id2Sel; x1 = x1Sel; x2 = x2Sel; sHat = sHatSel; tHat = tHatSel; uHat = uHatSel; sigma2Sel->sigma( id1, id2, x1, x2, sHat, tHat, uHat, alpS, alpEM, true, pickOtherSel); } // Pick one of the possible channels summed above. dSigmaDtSel = sigma2Sel->sigmaSel(); if (sigma2Sel->swapTU()) swap( tHat, uHat); // Decide to keep event based on kinematics (normally always OK). // Rescattering: need to provide incoming four-vectors and masses. if (pickRescatter) { Vec4 p1Res = (i1Sel == 0) ? 0.5 * eCM * x1Sel * Vec4( 0., 0., 1., 1.) : event[i1Sel].p(); Vec4 p2Res = (i2Sel == 0) ? 0.5 * eCM * x2Sel * Vec4( 0., 0., -1., 1.) : event[i2Sel].p(); double m1Res = (i1Sel == 0) ? 0. : event[i1Sel].m(); double m2Res = (i2Sel == 0) ? 0. : event[i2Sel].m(); acceptKin = dSigmaDtSel->final2KinMPI( i1Sel, i2Sel, p1Res, p2Res, m1Res, m2Res); // New interaction: already stored values enough. } else acceptKin = dSigmaDtSel->final2KinMPI(); } while (!acceptKin); // Done. return sqrt(pT2); } //-------------------------------------------------------------------------- // Set up the kinematics of the 2 -> 2 scattering process, // and store the scattering in the event record. bool MultipartonInteractions::scatter( Event& event) { // Last beam-status particles. Offset relative to normal beam locations. int sizeProc = event.size(); int nBeams = 3; for (int i = 3; i < sizeProc; ++i) if (event[i].statusAbs() < 20) nBeams = i + 1; int nOffset = nBeams - 3; // Loop over four partons and offset info relative to subprocess itself. int motherOffset = event.size(); int colOffset = event.lastColTag(); for (int i = 1; i <= 4; ++i) { Particle parton = dSigmaDtSel->getParton(i); if (i <= 2 ) parton.mothers( i + nOffset, 0); else parton.mothers( motherOffset, motherOffset + 1); if (i <= 2 ) parton.daughters( motherOffset + 2, motherOffset + 3); else parton.daughters( 0, 0); int col = parton.col(); if (col > 0) parton.col( col + colOffset); int acol = parton.acol(); if (acol > 0) parton.acol( acol + colOffset); // Put the partons into the event record. event.append(parton); } // Allow veto of MPI. If so restore event record to before scatter. if (canVetoMPI && userHooksPtr->doVetoMPIEmission(sizeProc, event)) { event.popBack(event.size() - sizeProc); return false; } // Store participating partons as a new set in list of all systems. int iSys = partonSystemsPtr->addSys(); partonSystemsPtr->setInA(iSys, motherOffset); partonSystemsPtr->setInB(iSys, motherOffset + 1); partonSystemsPtr->addOut(iSys, motherOffset + 2); partonSystemsPtr->addOut(iSys, motherOffset + 3); partonSystemsPtr->setSHat(iSys, sHat); // Tag double rescattering graphs that annihilate one initial colour. bool annihil1 = false; bool annihil2 = false; if (i1Sel > 0 && i2Sel > 0) { if (event[motherOffset].col() == event[motherOffset + 1].acol() && event[motherOffset].col() > 0) annihil1 = true; if (event[motherOffset].acol() == event[motherOffset + 1].col() && event[motherOffset].acol() > 0) annihil2 = true; } // Beam remnant A: add scattered partons to list. BeamParticle& beamA = *beamAPtr; int iA = beamA.append( motherOffset, id1, x1); // Find whether incoming partons are valence or sea, so prepared for ISR. if (i1Sel == 0) { beamA.xfISR( iA, id1, x1, pT2); beamA.pickValSeaComp(); // Remove rescattered parton from final state and change history. // Propagate existing colour labels throught graph. } else { beamA[iA].companion(-10); event[i1Sel].statusNeg(); event[i1Sel].daughters( motherOffset, motherOffset); event[motherOffset].mothers( i1Sel, i1Sel); int colOld = event[i1Sel].col(); if (colOld > 0) { int colNew = event[motherOffset].col(); for (int i = motherOffset; i < motherOffset + 4; ++i) { if (event[i].col() == colNew) event[i].col( colOld); if (event[i].acol() == colNew) event[i].acol( colOld); } } int acolOld = event[i1Sel].acol(); if (acolOld > 0) { int acolNew = event[motherOffset].acol(); for (int i = motherOffset; i < motherOffset + 4; ++i) { if (event[i].col() == acolNew) event[i].col( acolOld); if (event[i].acol() == acolNew) event[i].acol( acolOld); } } } // Beam remnant B: add scattered partons to list. BeamParticle& beamB = *beamBPtr; int iB = beamB.append( motherOffset + 1, id2, x2); // Find whether incoming partons are valence or sea, so prepared for ISR. if (i2Sel == 0) { beamB.xfISR( iB, id2, x2, pT2); beamB.pickValSeaComp(); // Remove rescattered parton from final state and change history. // Propagate existing colour labels throught graph. } else { beamB[iB].companion(-10); event[i2Sel].statusNeg(); event[i2Sel].daughters( motherOffset + 1, motherOffset + 1); event[motherOffset + 1].mothers( i2Sel, i2Sel); int colOld = event[i2Sel].col(); if (colOld > 0) { int colNew = event[motherOffset + 1].col(); for (int i = motherOffset; i < motherOffset + 4; ++i) { if (event[i].col() == colNew) event[i].col( colOld); if (event[i].acol() == colNew) event[i].acol( colOld); } } int acolOld = event[i2Sel].acol(); if (acolOld > 0) { int acolNew = event[motherOffset + 1].acol(); for (int i = motherOffset; i < motherOffset + 4; ++i) { if (event[i].col() == acolNew) event[i].col( acolOld); if (event[i].acol() == acolNew) event[i].acol( acolOld); } } } // Annihilating colour in double rescattering requires relabelling // of one colour into the other in the whole preceding event. if (annihil1 || annihil2) { int colLeft = (annihil1) ? event[motherOffset].col() : event[motherOffset].acol(); int mother1 = event[motherOffset].mother1(); int mother2 = event[motherOffset + 1].mother1(); int colLost = (annihil1) ? event[mother1].col() + event[mother2].acol() - colLeft : event[mother1].acol() + event[mother2].col() - colLeft; for (int i = 0; i < motherOffset; ++i) { if (event[i].col() == colLost) event[i].col( colLeft ); if (event[i].acol() == colLost) event[i].acol( colLeft ); } } // Store info on subprocess code and rescattered partons. int codeMPI = dSigmaDtSel->code(); double pTMPI = dSigmaDtSel->pTMPIFin(); if (iDiffSys == 0) infoPtr->setTypeMPI( codeMPI, pTMPI, i1Sel, i2Sel, enhanceBnow / zeroIntCorr); partonSystemsPtr->setPTHat(iSys, pTMPI); // Done. return true; } //-------------------------------------------------------------------------- // Determine constant in d(Prob)/d(pT2) < const / (pT2 + r * pT20)^2. void MultipartonInteractions::upperEnvelope() { // Initially determine constant in jet cross section upper estimate // d(sigma_approx)/d(pT2) < const / (pT2 + r * pT20)^2. pT4dSigmaMax = 0.; // Loop thorough allowed pT range logarithmically evenly. for (int iPT = 0; iPT < 100; ++iPT) { double pT = pTmin * pow( pTmax/pTmin, 0.01 * (iPT + 0.5) ); pT2 = pT*pT; pT2shift = pT2 + pT20; pT2Ren = pT2shift; pT2Fac = (SHIFTFACSCALE) ? pT2shift : pT2; xT = 2. * pT / eCM; // Evaluate parton density sums at x1 = x2 = xT. double xPDF1sumMax = (9./4.) * beamAPtr->xf(21, xT, pT2Fac); for (int id = 1; id <= nQuarkIn; ++id) xPDF1sumMax += beamAPtr->xf( id, xT, pT2Fac) + beamAPtr->xf(-id, xT, pT2Fac); double xPDF2sumMax = (9./4.) * beamBPtr->xf(21, xT, pT2Fac); for (int id = 1; id <= nQuarkIn; ++id) xPDF2sumMax += beamBPtr->xf( id, xT, pT2Fac) + beamBPtr->xf(-id, xT, pT2Fac); // Evaluate alpha_strong and _EM, matrix element and phase space volume. alpS = alphaS.alphaS(pT2Ren); alpEM = alphaEM.alphaEM(pT2Ren); double dSigmaPartonApprox = CONVERT2MB * Kfactor * 0.5 * M_PI * pow2(alpS / pT2shift); double yMax = log(1./xT + sqrt(1./(xT*xT) - 1.)); double volumePhSp = pow2(2. * yMax); // Final comparison to determine upper estimate. double dSigmaApproxNow = SIGMAFUDGE * xPDF1sumMax * xPDF2sumMax * dSigmaPartonApprox * volumePhSp; double pT4dSigmaNow = pow2(pT2 + pT20R) * dSigmaApproxNow; if ( pT4dSigmaNow > pT4dSigmaMax) pT4dSigmaMax = pT4dSigmaNow; } // Get wanted constant by dividing by the nondiffractive cross section. pT4dProbMax = pT4dSigmaMax / sigmaND; } //-------------------------------------------------------------------------- // Integrate the parton-parton interaction cross section, // using stratified Monte Carlo sampling. // Store result in pT bins for use as Sudakov form factors. void MultipartonInteractions::jetCrossSection() { // Common factor from bin size in dpT2 / (pT2 + r * pT20)^2 and statistics. double sigmaFactor = (1. / pT20minR - 1. / pT20maxR) / (100. * nSample); // Reset overlap-weighted cross section for x-dependent matter profile. if (bProfile == 4) for (int bBin = 0; bBin < XDEP_BBIN; bBin++) sigmaIntWgt[bBin] = 0.; // Loop through allowed pT range evenly in dpT2 / (pT2 + r * pT20)^2. sigmaInt = 0.; double dSigmaMax = 0.; sudExpPT[100] = 0.; for (int iPT = 99; iPT >= 0; --iPT) { double sigmaSum = 0.; // Reset pT-binned overlap-weigted integration. if (bProfile == 4) for (int bBin = 0; bBin < XDEP_BBIN; bBin++) sigmaSumWgt[bBin] = 0.; // In each pT bin sample a number of random pT values. for (int iSample = 0; iSample < nSample; ++iSample) { double mappedPT2 = 1. - 0.01 * (iPT + rndmPtr->flat()); pT2 = pT20min0maxR / (pT20minR + mappedPT2 * pT2maxmin) - pT20R; // Evaluate cross section dSigma/dpT2 in phase space point. double dSigma = sigmaPT2scatter(true); // Multiply by (pT2 + r * pT20)^2 to compensate for pT sampling. Sum. dSigma *= pow2(pT2 + pT20R); sigmaSum += dSigma; if (dSigma > dSigmaMax) dSigmaMax = dSigma; // Overlap-weighted cross section for x-dependent matter profile. // Note that dSigma can be 0. when points are rejected. if (bProfile == 4 && dSigma > 0.) { double w1 = XDEP_A1 + a1 * log(1. / x1); double w2 = XDEP_A1 + a1 * log(1. / x2); double fac = XDEP_A0 * XDEP_A0 * (w1 * w1 + w2 * w2); double b = 0.5 * bstepNow; for (int bBin = 0; bBin < XDEP_BBIN; bBin++) { double wgt = exp( - b * b / fac ) / fac / M_PI; sigmaSumWgt[bBin] += dSigma * wgt; b += bstepNow; } } } // Store total cross section and exponent of Sudakov. sigmaSum *= sigmaFactor; sigmaInt += sigmaSum; sudExpPT[iPT] = sudExpPT[iPT + 1] + sigmaSum / sigmaND; // Sum overlap-weighted cross section if (bProfile == 4) for (int bBin = 0; bBin < XDEP_BBIN; bBin++) { sigmaSumWgt[bBin] *= sigmaFactor; sigmaIntWgt[bBin] += sigmaSumWgt[bBin]; } // End of loop over pT values. } // Update upper estimate of differential cross section. Done. if (dSigmaMax > pT4dSigmaMax) { pT4dSigmaMax = dSigmaMax; pT4dProbMax = dSigmaMax / sigmaND; } } //-------------------------------------------------------------------------- // Evaluate "Sudakov form factor" for not having a harder interaction // at the selected b value, given the pT scale of the event. double MultipartonInteractions::sudakov(double pT2sud, double enhance) { // Find bin the pT2 scale falls in. double xBin = (pT2sud - pT2min) * pT20maxR / (pT2maxmin * (pT2sud + pT20R)); xBin = max(1e-6, min(100. - 1e-6, 100. * xBin) ); int iBin = int(xBin); // Interpolate inside bin. Optionally include enhancement factor. double sudExp = sudExpPT[iBin] + (xBin - iBin) * (sudExpPT[iBin + 1] - sudExpPT[iBin]); return exp( -enhance * sudExp); } //-------------------------------------------------------------------------- // Pick a trial next pT, based on a simple upper estimate of the // d(sigma)/d(pT2) spectrum. double MultipartonInteractions::fastPT2( double pT2beg) { // Use d(Prob)/d(pT2) < pT4dProbMax / (pT2 + r * pT20)^2. double pT20begR = pT2beg + pT20R; double pT4dProbMaxNow = pT4dProbMax * enhanceBmax; double pT2try = pT4dProbMaxNow * pT20begR / (pT4dProbMaxNow - pT20begR * log(rndmPtr->flat())) - pT20R; // Save cross section associated with ansatz above. Done. dSigmaApprox = pT4dSigmaMax / pow2(pT2try + pT20R); return pT2try; } //-------------------------------------------------------------------------- // Calculate the actual cross section to decide whether fast choice is OK. // Select flavours and kinematics for interaction at given pT. // Slightly different treatment for first interaction and subsequent ones. double MultipartonInteractions::sigmaPT2scatter(bool isFirst) { // Derive recormalization and factorization scales, amd alpha_strong/em. pT2shift = pT2 + pT20; pT2Ren = pT2shift; pT2Fac = (SHIFTFACSCALE) ? pT2shift : pT2; alpS = alphaS.alphaS(pT2Ren); alpEM = alphaEM.alphaEM(pT2Ren); // Derive rapidity limits from chosen pT2. xT = 2. * sqrt(pT2) / eCM; if (xT >= 1.) return 0.; xT2 = xT*xT; double yMax = log(1./xT + sqrt(1./xT2 - 1.)); // Select rapidities y3 and y4 of the two produced partons. double y3 = yMax * (2. * rndmPtr->flat() - 1.); double y4 = yMax * (2. * rndmPtr->flat() - 1.); y = 0.5 * (y3 + y4); // Reject some events at large rapidities to improve efficiency. // (Works for baryons, not pions or Pomerons if they have hard PDF's.) double WTy = (hasBaryonBeams) ? (1. - pow2(y3/yMax)) * (1. - pow2(y4/yMax)) : 1.; if (WTy < rndmPtr->flat()) return 0.; // Failure if x1 or x2 exceed what is left in respective beam. x1 = 0.5 * xT * (exp(y3) + exp(y4)); x2 = 0.5 * xT * (exp(-y3) + exp(-y4)); if (isFirst) { if (x1 > 1. || x2 > 1.) return 0.; } else { if (x1 > beamAPtr->xMax() || x2 > beamBPtr->xMax()) return 0.; } tau = x1 * x2; // Begin evaluate parton densities at actual x1 and x2. double xPDF1[21]; double xPDF1sum = 0.; double xPDF2[21]; double xPDF2sum = 0.; // For first interaction use normal densities. if (isFirst) { for (int id = -nQuarkIn; id <= nQuarkIn; ++id) { if (id == 0) xPDF1[10] = (9./4.) * beamAPtr->xf(21, x1, pT2Fac); else xPDF1[id+10] = beamAPtr->xf(id, x1, pT2Fac); xPDF1sum += xPDF1[id+10]; } for (int id = -nQuarkIn; id <= nQuarkIn; ++id) { if (id == 0) xPDF2[10] = (9./4.) * beamBPtr->xf(21, x2, pT2Fac); else xPDF2[id+10] = beamBPtr->xf(id, x2, pT2Fac); xPDF2sum += xPDF2[id+10]; } // For subsequent interactions use rescaled densities. } else { for (int id = -nQuarkIn; id <= nQuarkIn; ++id) { if (id == 0) xPDF1[10] = (9./4.) * beamAPtr->xfMPI(21, x1, pT2Fac); else xPDF1[id+10] = beamAPtr->xfMPI(id, x1, pT2Fac); xPDF1sum += xPDF1[id+10]; } for (int id = -nQuarkIn; id <= nQuarkIn; ++id) { if (id == 0) xPDF2[10] = (9./4.) * beamBPtr->xfMPI(21, x2, pT2Fac); else xPDF2[id+10] = beamBPtr->xfMPI(id, x2, pT2Fac); xPDF2sum += xPDF2[id+10]; } } // Select incoming flavours according to actual PDF's. id1 = -nQuarkIn - 1; double temp = xPDF1sum * rndmPtr->flat(); do { xPDF1now = xPDF1[(++id1) + 10]; temp -= xPDF1now; } while (temp > 0. && id1 < nQuarkIn); if (id1 == 0) id1 = 21; id2 = -nQuarkIn-1; temp = xPDF2sum * rndmPtr->flat(); do { xPDF2now = xPDF2[(++id2) + 10]; temp -= xPDF2now;} while (temp > 0. && id2 < nQuarkIn); if (id2 == 0) id2 = 21; // Assign pointers to processes relevant for incoming flavour choice: // g + g, q + g, q + qbar (same flavour), q + q(bar) (the rest). // Factor 4./9. per incoming gluon to compensate for preweighting. SigmaMultiparton* sigma2Tmp; double gluFac = 1.; if (id1 == 21 && id2 == 21) { sigma2Tmp = &sigma2gg; gluFac = 16. / 81.; } else if (id1 == 21 || id2 == 21) { sigma2Tmp = &sigma2qg; gluFac = 4. / 9.; } else if (id1 == -id2) sigma2Tmp = &sigma2qqbarSame; else sigma2Tmp = &sigma2qq; // Prepare to generate differential cross sections. sHat = tau * sCM; double root = sqrtpos(1. - xT2 / tau); tHat = -0.5 * sHat * (1. - root); uHat = -0.5 * sHat * (1. + root); // Evaluate cross sections, include possibility of K factor. // Use kinematics for two symmetrical configurations (tHat <-> uHat). // (Not necessary, but makes for better MC efficiency.) double dSigmaPartonCorr = Kfactor * gluFac * sigma2Tmp->sigma( id1, id2, x1, x2, sHat, tHat, uHat, alpS, alpEM); // Combine cross section, pdf's and phase space integral. double volumePhSp = pow2(2. * yMax) / WTy; double dSigmaScat = dSigmaPartonCorr * xPDF1sum * xPDF2sum * volumePhSp; // Dampen cross section at small pT values; part of formalism. // Use pT2 corrected for massive kinematics at this step.?? // double pT2massive = dSigmaDtSel->pT2MPI(); double pT2massive = pT2; dSigmaScat *= pow2( pT2massive / (pT2massive + pT20) ); // Sum up total contribution for all scatterings and rescatterings. dSigmaSum += dSigmaScat; // Save values for comparison with rescattering processes. i1Sel = 0; i2Sel = 0; id1Sel = id1; id2Sel = id2; x1Sel = x1; x2Sel = x2; sHatSel = sHat; tHatSel = tHat; uHatSel = uHat; sigma2Sel = sigma2Tmp; pickOtherSel = sigma2Tmp->pickedOther(); // For first interaction: pick one of the possible channels summed above. if (isFirst) { dSigmaDtSel = sigma2Tmp->sigmaSel(); if (sigma2Tmp->swapTU()) swap( tHat, uHat); } // Done. return dSigmaScat; } //-------------------------------------------------------------------------- // Find the partons that are allowed to rescatter. void MultipartonInteractions::findScatteredPartons( Event& event) { // Reset arrays. scatteredA.resize(0); scatteredB.resize(0); double yTmp, probA, probB; // Loop though the event record and catch "final" partons. for (int i = 0; i < event.size(); ++i) if (event[i].isFinal() && (event[i].idAbs() <= nQuarkIn || event[i].id() == 21)) { yTmp = event[i].y(); // Different strategies to determine which partons may rescatter. switch(rescatterMode) { // Case 0: step function at origin case 0: if ( yTmp > 0.) scatteredA.push_back( i); if (-yTmp > 0.) scatteredB.push_back( i); break; // Case 1: step function as ySepResc. case 1: if ( yTmp > ySepResc) scatteredA.push_back( i); if (-yTmp > ySepResc) scatteredB.push_back( i); break; // Case 2: linear rise from ySep - deltaY to ySep + deltaY. case 2: probA = 0.5 * (1. + ( yTmp - ySepResc) / deltaYResc); if (probA > rndmPtr->flat()) scatteredA.push_back( i); probB = 0.5 * (1. + (-yTmp - ySepResc) / deltaYResc); if (probB > rndmPtr->flat()) scatteredB.push_back( i); break; // Case 3: rise like (1/2) * ( 1 + tanh((y - ySep) / deltaY) ). // Use that (1/2) (1 + tanh(x)) = 1 / (1 + exp(-2x)). case 3: probA = 1. / (1. + exp(-2. * ( yTmp - ySepResc) / deltaYResc)); if (probA > rndmPtr->flat()) scatteredA.push_back( i); probB = 1. / (1. + exp(-2. * (-yTmp - ySepResc) / deltaYResc)); if (probB > rndmPtr->flat()) scatteredB.push_back( i); break; // Case 4 and undefined values: all partons can rescatter. default: scatteredA.push_back( i); scatteredB.push_back( i); break; // End of loop over partons. Done. } } } //-------------------------------------------------------------------------- // Rescattering contribution summed over all already scattered partons. // Calculate the actual cross section to decide whether fast choice is OK. // Select flavours and kinematics for interaction at given pT. double MultipartonInteractions::sigmaPT2rescatter( Event& event) { // Derive xT scale from chosen pT2. xT = 2. * sqrt(pT2) / eCM; if (xT >= 1.) return 0.; xT2 = xT*xT; // Pointer to cross section and total rescatter contribution. SigmaMultiparton* sigma2Tmp; double dSigmaResc = 0.; // Normally save time by picking one random scattered parton from side A. int nScatA = scatteredA.size(); int iScatA = -1; if (PREPICKRESCATTER && nScatA > 0) iScatA = min( nScatA - 1, int( rndmPtr->flat() * double(nScatA) ) ); // Loop over all already scattered partons from side A. for (int iScat = 0; iScat < nScatA; ++iScat) { if (PREPICKRESCATTER && iScat != iScatA) continue; int iA = scatteredA[iScat]; int id1Tmp = event[iA].id(); // Calculate maximum possible sHat and check whether big enough. double x1Tmp = event[iA].pPos() / eCM; double sHatMax = x1Tmp * beamBPtr->xMax() * sCM; if (sHatMax < 4. * pT2) continue; // Select rapidity separation between two produced partons. double dyMax = log( sqrt(0.25 * sHatMax / pT2) * (1. + sqrtpos(1. - 4. * pT2 / sHatMax)) ); double dy = dyMax * (2. * rndmPtr->flat() - 1.); // Reconstruct kinematical variables, especially x2. // Incoming c/b masses handled better if tau != x1 * x2. double m2Tmp = event[iA].m2(); double sHatTmp = m2Tmp + 4. * pT2 * pow2(cosh(dy)); double x2Tmp = (sHatTmp - m2Tmp) /(x1Tmp * sCM); double tauTmp = sHatTmp / sCM; double root = sqrtpos(1. - xT2 / tauTmp); double tHatTmp = -0.5 * sHatTmp * (1. - root); double uHatTmp = -0.5 * sHatTmp * (1. + root); // Begin evaluate parton densities at actual x2. double xPDF2[21]; double xPDF2sum = 0.; // Use rescaled densities, with preweighting 9/4 for gluons. for (int id = -nQuarkIn; id <= nQuarkIn; ++id) { if (id == 0) xPDF2[10] = (9./4.) * beamBPtr->xfMPI(21, x2Tmp, pT2Fac); else xPDF2[id+10] = beamBPtr->xfMPI(id, x2Tmp, pT2Fac); xPDF2sum += xPDF2[id+10]; } // Select incoming flavour according to actual PDF's. int id2Tmp = -nQuarkIn - 1; double temp = xPDF2sum * rndmPtr->flat(); do { xPDF2now = xPDF2[(++id2Tmp) + 10]; temp -= xPDF2now;} while (temp > 0. && id2Tmp < nQuarkIn); if (id2Tmp == 0) id2Tmp = 21; // Assign pointers to processes relevant for incoming flavour choice: // g + g, q + g, q + qbar (same flavour), q + q(bar) (the rest). // Factor 4./9. for incoming gluon 2 to compensate for preweighting. if (id1Tmp == 21 && id2Tmp == 21) sigma2Tmp = &sigma2gg; else if (id1Tmp == 21 || id2Tmp == 21) sigma2Tmp = &sigma2qg; else if (id1Tmp == -id2Tmp) sigma2Tmp = &sigma2qqbarSame; else sigma2Tmp = &sigma2qq; double gluFac = (id2Tmp == 21) ? 4. / 9. : 1.; // Evaluate cross sections, include possibility of K factor. // Use kinematics for two symmetrical configurations (tHat <-> uHat). // (Not necessary, but makes for better MC efficiency.) double dSigmaPartonCorr = Kfactor * gluFac * sigma2Tmp->sigma( id1Tmp, id2Tmp, x1Tmp, x2Tmp, sHatTmp, tHatTmp, uHatTmp, alpS, alpEM); // Combine cross section, pdf's and phase space integral. double volumePhSp = 4. *dyMax; double dSigmaCorr = dSigmaPartonCorr * xPDF2sum * volumePhSp; // Dampen cross section at small pT values; part of formalism. // Use pT2 corrected for massive kinematics at this step. //?? double pT2massive = dSigmaDtSel->pT2MPI(); double pT2massive = pT2; dSigmaCorr *= pow2( pT2massive / (pT2massive + pT20) ); // Compensate for prepicked rescattering if appropriate. if (PREPICKRESCATTER) dSigmaCorr *= nScatA; // Sum up total contribution for all scatterings or rescattering only. dSigmaSum += dSigmaCorr; dSigmaResc += dSigmaCorr; // Determine whether current rescattering should be selected. if (dSigmaCorr > rndmPtr->flat() * dSigmaSum) { i1Sel = iA; i2Sel = 0; id1Sel = id1Tmp; id2Sel = id2Tmp; x1Sel = x1Tmp; x2Sel = x2Tmp; sHatSel = sHatTmp; tHatSel = tHatTmp; uHatSel = uHatTmp; sigma2Sel = sigma2Tmp; pickOtherSel = sigma2Tmp->pickedOther(); } } // Normally save time by picking one random scattered parton from side B. int nScatB = scatteredB.size(); int iScatB = -1; if (PREPICKRESCATTER && nScatB > 0) iScatB = min( nScatB - 1, int( rndmPtr->flat() * double(nScatB) ) ); // Loop over all already scattered partons from side B. for (int iScat = 0; iScat < nScatB; ++iScat) { if (PREPICKRESCATTER && iScat != iScatB) continue; int iB = scatteredB[iScat]; int id2Tmp = event[iB].id(); // Calculate maximum possible sHat and check whether big enough. double x2Tmp = event[iB].pNeg() / eCM; double sHatMax = beamAPtr->xMax() * x2Tmp * sCM; if (sHatMax < 4. * pT2) continue; // Select rapidity separation between two produced partons. double dyMax = log( sqrt(0.25 * sHatMax / pT2) * (1. + sqrtpos(1. - 4. * pT2 / sHatMax)) ); double dy = dyMax * (2. * rndmPtr->flat() - 1.); // Reconstruct kinematical variables, especially x1. // Incoming c/b masses handled better if tau != x1 * x2. double m2Tmp = event[iB].m2(); double sHatTmp = m2Tmp + 4. * pT2 * pow2(cosh(dy)); double x1Tmp = (sHatTmp - m2Tmp) /(x2Tmp * sCM); double tauTmp = sHatTmp / sCM; double root = sqrtpos(1. - xT2 / tauTmp); double tHatTmp = -0.5 * sHatTmp * (1. - root); double uHatTmp = -0.5 * sHatTmp * (1. + root); // Begin evaluate parton densities at actual x1. double xPDF1[21]; double xPDF1sum = 0.; // Use rescaled densities, with preweighting 9/4 for gluons. for (int id = -nQuarkIn; id <= nQuarkIn; ++id) { if (id == 0) xPDF1[10] = (9./4.) * beamAPtr->xfMPI(21, x1Tmp, pT2Fac); else xPDF1[id+10] = beamAPtr->xfMPI(id, x1Tmp, pT2Fac); xPDF1sum += xPDF1[id+10]; } // Select incoming flavour according to actual PDF's. int id1Tmp = -nQuarkIn - 1; double temp = xPDF1sum * rndmPtr->flat(); do { xPDF1now = xPDF1[(++id1Tmp) + 10]; temp -= xPDF1now;} while (temp > 0. && id1Tmp < nQuarkIn); if (id1Tmp == 0) id1Tmp = 21; // Assign pointers to processes relevant for incoming flavour choice: // g + g, q + g, q + qbar (same flavour), q + q(bar) (the rest). // Factor 4./9. for incoming gluon 2 to compensate for preweighting. if (id1Tmp == 21 && id2Tmp == 21) sigma2Tmp = &sigma2gg; else if (id1Tmp == 21 || id2Tmp == 21) sigma2Tmp = &sigma2qg; else if (id1Tmp == -id2Tmp) sigma2Tmp = &sigma2qqbarSame; else sigma2Tmp = &sigma2qq; double gluFac = (id1Tmp == 21) ? 4. / 9. : 1.; // Evaluate cross sections, include possibility of K factor. // Use kinematics for two symmetrical configurations (tHat <-> uHat). // (Not necessary, but makes for better MC efficiency.) double dSigmaPartonCorr = Kfactor * gluFac * sigma2Tmp->sigma( id1Tmp, id2Tmp, x1Tmp, x2Tmp, sHatTmp, tHatTmp, uHatTmp, alpS, alpEM); // Combine cross section, pdf's and phase space integral. double volumePhSp = 4. *dyMax; double dSigmaCorr = dSigmaPartonCorr * xPDF1sum * volumePhSp; // Dampen cross section at small pT values; part of formalism. // Use pT2 corrected for massive kinematics at this step. //?? double pT2massive = dSigmaDtSel->pT2MPI(); double pT2massive = pT2; dSigmaCorr *= pow2( pT2massive / (pT2massive + pT20) ); // Compensate for prepicked rescattering if appropriate. if (PREPICKRESCATTER) dSigmaCorr *= nScatB; // Sum up total contribution for all scatterings or rescattering only. dSigmaSum += dSigmaCorr; dSigmaResc += dSigmaCorr; // Determine whether current rescattering should be selected. if (dSigmaCorr > rndmPtr->flat() * dSigmaSum) { i1Sel = 0; i2Sel = iB; id1Sel = id1Tmp; id2Sel = id2Tmp; x1Sel = x1Tmp; x2Sel = x2Tmp; sHatSel = sHatTmp; tHatSel = tHatTmp; uHatSel = uHatTmp; sigma2Sel = sigma2Tmp; pickOtherSel = sigma2Tmp->pickedOther(); } } // Double rescatter: loop over already scattered partons from both sides. // As before, allow to use only one parton per side to speed up. if (allowDoubleRes) { for (int iScat1 = 0; iScat1 < nScatA; ++iScat1) { if (PREPICKRESCATTER && iScat1 != iScatA) continue; int iA = scatteredA[iScat1]; int id1Tmp = event[iA].id(); for (int iScat2 = 0; iScat2 < nScatB; ++iScat2) { if (PREPICKRESCATTER && iScat2 != iScatB) continue; int iB = scatteredB[iScat2]; int id2Tmp = event[iB].id(); // Calculate current sHat and check whether big enough. double sHatTmp = (event[iA].p() + event[iB].p()).m2Calc(); if (sHatTmp < 4. * pT2) continue; // Reconstruct other kinematical variables. (x values not needed.) double x1Tmp = event[iA].pPos() / eCM; double x2Tmp = event[iB].pNeg() / eCM; double tauTmp = sHatTmp / sCM; double root = sqrtpos(1. - xT2 / tauTmp); double tHatTmp = -0.5 * sHatTmp * (1. - root); double uHatTmp = -0.5 * sHatTmp * (1. + root); // Assign pointers to processes relevant for incoming flavour choice: // g + g, q + g, q + qbar (same flavour), q + q(bar) (the rest). if (id1Tmp == 21 && id2Tmp == 21) sigma2Tmp = &sigma2gg; else if (id1Tmp == 21 || id2Tmp == 21) sigma2Tmp = &sigma2qg; else if (id1Tmp == -id2Tmp) sigma2Tmp = &sigma2qqbarSame; else sigma2Tmp = &sigma2qq; // Evaluate cross sections, include possibility of K factor. // Use kinematics for two symmetrical configurations (tHat <-> uHat). // (Not necessary, but makes for better MC efficiency.) double dSigmaPartonCorr = Kfactor * sigma2Tmp->sigma( id1Tmp, id2Tmp, x1Tmp, x2Tmp, sHatTmp, tHatTmp, uHatTmp, alpS, alpEM); // Combine cross section and Jacobian tHat -> pT2 // (with safety minvalue). double dSigmaCorr = dSigmaPartonCorr / max(ROOTMIN, root); // Dampen cross section at small pT values; part of formalism. // Use pT2 corrected for massive kinematics at this step. //?? double pT2massive = dSigmaDtSel->pT2MPI(); double pT2massive = pT2; dSigmaCorr *= pow2( pT2massive / (pT2massive + pT20) ); // Compensate for prepicked rescattering if appropriate. if (PREPICKRESCATTER) dSigmaCorr *= nScatA * nScatB; // Sum up total contribution for all scatterings or rescattering only. dSigmaSum += dSigmaCorr; dSigmaResc += dSigmaCorr; // Determine whether current rescattering should be selected. if (dSigmaCorr > rndmPtr->flat() * dSigmaSum) { i1Sel = iA; i2Sel = iB; id1Sel = id1Tmp; id2Sel = id2Tmp; x1Sel = x1Tmp; x2Sel = x2Tmp; sHatSel = sHatTmp; tHatSel = tHatTmp; uHatSel = uHatTmp; sigma2Sel = sigma2Tmp; pickOtherSel = sigma2Tmp->pickedOther(); } } } } // Done. return dSigmaResc; } //-------------------------------------------------------------------------- // Calculate factor relating matter overlap and interaction rate, // i.e. k in = k * overlap(b) (neglecting // n_int = 0 corrections and energy-momentum conservation effects). void MultipartonInteractions::overlapInit() { // Initial values for iteration. Step size of b integration. nAvg = sigmaInt / sigmaND; kNow = 0.5; int stepDir = 1; double deltaB = BSTEP; if (bProfile == 2) deltaB *= min( 0.5, 2.5 * coreRadius); if (bProfile == 3) deltaB *= max(1., pow(2. / expPow, 1. / expPow)); // Further variables, with dummy initial values. double nNow = 0.; double kLow = 0.; double nLow = 0.; double kHigh = 0.; double nHigh = 0.; double overlapNow = 0.; double probNow = 0.; double overlapInt = 0.5; double probInt = 0.; double probOverlapInt = 0.; double bProbInt = 0.; normPi = 1. / (2. * M_PI); // Subdivision into low-b and high-b region by interaction rate. bool pastBDiv = false; double overlapHighB = 0.; // For x-dependent matter profile, try to find a0 rather than k. // Existing framework is used, but with substitutions: // a0 tuned according to Int( Pint(b), d^2b ) = sigmaND, // nAvg = sigmaND, kNow = a0now, kLow = a0low, kHigh = a0high, // nNow = probInt, nLow = probIntLow, nHigh = probIntHigh. double rescale2 = 1.; if (bProfile == 4) { nAvg = sigmaND; kNow = XDEP_A0 / 2.0; } // First close k into an interval by binary steps, // then find k by successive interpolation. do { if (stepDir == 1) kNow *= 2.; else if (stepDir == -1) kNow *= 0.5; else kNow = kLow + (nAvg - nLow) * (kHigh - kLow) / (nHigh - nLow); // Overlap trivial if no impact parameter dependence. if (bProfile <= 0 || bProfile > 4) { probInt = 0.5 * M_PI * (1. - exp(-kNow)); probOverlapInt = probInt / M_PI; bProbInt = probInt; // Ratio of b-integrated k * overlap / (1 - exp( - k * overlap)). nNow = M_PI * kNow * overlapInt / probInt; // Else integrate overlap over impact parameter. } else if (bProfile < 4) { // Reset integrals. overlapInt = (bProfile == 3) ? 0. : 0.5; probInt = 0.; probOverlapInt = 0.; bProbInt = 0.; pastBDiv = false; overlapHighB = 0.; // Step in b space. double b = -0.5 * deltaB; double bArea = 0.; do { b += deltaB; bArea = 2. * M_PI * b * deltaB; // Evaluate overlap at current b value. if (bProfile == 1) { overlapNow = normPi * exp( -b*b); } else if (bProfile == 2) { overlapNow = normPi * ( fracA * exp( -min(EXPMAX, b*b)) + fracB * exp( -min(EXPMAX, b*b / radius2B)) / radius2B + fracC * exp( -min(EXPMAX, b*b / radius2C)) / radius2C ); } else { overlapNow = normPi * exp( -pow( b, expPow)); overlapInt += bArea * overlapNow; } if (pastBDiv) overlapHighB += bArea * overlapNow; // Calculate interaction probability and integrate. probNow = 1. - exp( -min(EXPMAX, M_PI * kNow * overlapNow)); probInt += bArea * probNow; probOverlapInt += bArea * overlapNow * probNow; bProbInt += b * bArea * probNow; // Check when interaction probability has dropped sufficiently. if (!pastBDiv && probNow < PROBATLOWB) { bDiv = b + 0.5 * deltaB; pastBDiv = true; } // Continue out in b until overlap too small. } while (b < 1. || b * probNow > BMAX); // Ratio of b-integrated k * overlap / (1 - exp( - k * overlap)). nNow = M_PI * kNow * overlapInt / probInt; // x-dependent matter profile. } else if (bProfile == 4) { rescale2 = pow2(kNow / XDEP_A0); probInt = 0.; double b = 0.5 * bstepNow; for (int bBin = 0; bBin < XDEP_BBIN; bBin++) { double bArea = 2. * M_PI * b * bstepNow; double pIntNow = 1 - exp( -min(EXPMAX, sigmaIntWgt[bBin] / rescale2) ); probInt += bArea * rescale2 * pIntNow; b += bstepNow; } nNow = probInt; } // Replace lower or upper limit of k. if (nNow < nAvg) { kLow = kNow; nLow = nNow; if (stepDir == -1) stepDir = 0; } else { kHigh = kNow; nHigh = nNow; if (stepDir == 1) stepDir = -1; } // Continue iteration until convergence. } while (abs(nNow - nAvg) > KCONVERGE * nAvg); // Save relevant final numbers for overlap values. if (bProfile >= 0 && bProfile < 4) { double avgOverlap = probOverlapInt / probInt; zeroIntCorr = probOverlapInt / overlapInt; normOverlap = normPi * zeroIntCorr / avgOverlap; bAvg = bProbInt / probInt; // Values for x-dependent matter profile. } else if (bProfile == 4) { // bAvg = Int(b * Pint(b), d2b) / sigmaND. // zeroIntCorr = Int( * Pint(b), d2b) / sigmaInt. bAvg = 0.; zeroIntCorr = 0.; double b = 0.5 * bstepNow; for (int bBin = 0; bBin < XDEP_BBIN; bBin++) { double bArea = 2. * M_PI * b * bstepNow; double pIntNow = 1. - exp( -min(EXPMAX, sigmaIntWgt[bBin] / rescale2) ); bAvg += sqrt(rescale2) * b * bArea * rescale2 * pIntNow; zeroIntCorr += bArea * sigmaIntWgt[bBin] * pIntNow; b += bstepNow; } bAvg /= nNow; zeroIntCorr /= sigmaInt; // Other required values. a0now = kNow; infoPtr->seta0MPI(a0now * XDEP_SMB2FM); a02now = a0now * a0now; double xMin = 2. * pTmin / infoPtr->eCM(); a2max = a0now * (XDEP_A1 + a1 * log(1. / xMin)); a2max *= a2max; } // Relative rates for preselection of low-b and high-b region. // Other useful combinations for subsequent selection. if (bProfile > 0 && bProfile <= 3) { probLowB = M_PI * bDiv*bDiv; double probHighB = M_PI * kNow * overlapHighB; if (bProfile == 1) probHighB = M_PI * kNow * 0.5 * exp( -bDiv*bDiv); else if (bProfile == 2) { fracAhigh = fracA * exp( -bDiv*bDiv); fracBhigh = fracB * exp( -bDiv*bDiv / radius2B); fracChigh = fracC * exp( -bDiv*bDiv / radius2C); fracABChigh = fracAhigh + fracBhigh + fracChigh; probHighB = M_PI * kNow * 0.5 * fracABChigh; } else { cDiv = pow( bDiv, expPow); cMax = max(2. * expRev, cDiv); } probLowB /= (probLowB + probHighB); } } //-------------------------------------------------------------------------- // Pick impact parameter and interaction rate enhancement beforehand, // i.e. before even the hardest interaction for minimum-bias events. void MultipartonInteractions::overlapFirst() { // Trivial values if no impact parameter dependence. if (bProfile <= 0 || bProfile > 4) { bNow = bAvg; enhanceB = zeroIntCorr; bIsSet = true; isAtLowB = true; return; } // Preliminary choice between and inside low-b and high-b regions. double overlapNow = 0.; double probAccept = 0.; do { // Treatment in low-b region: pick b flat in area. if (rndmPtr->flat() < probLowB) { isAtLowB = true; bNow = bDiv * sqrt(rndmPtr->flat()); // Evaluate overlap and from that acceptance probability. if (bProfile == 1) overlapNow = normPi * exp( -bNow*bNow); else if (bProfile == 2) overlapNow = normPi * ( fracA * exp( -bNow*bNow) + fracB * exp( -bNow*bNow / radius2B) / radius2B + fracC * exp( -bNow*bNow / radius2C) / radius2C ); else overlapNow = normPi * exp( -pow( bNow, expPow)); probAccept = 1. - exp( -min(EXPMAX, M_PI * kNow * overlapNow)); // Treatment in high-b region: pick b according to overlap. } else { isAtLowB = false; // For simple and double Gaussian pick b according to exp(-b^2 / r^2). if (bProfile == 1) { bNow = sqrt(bDiv*bDiv - log(rndmPtr->flat())); overlapNow = normPi * exp( -min(EXPMAX, bNow*bNow)); } else if (bProfile == 2) { double pickFrac = rndmPtr->flat() * fracABChigh; if (pickFrac < fracAhigh) bNow = sqrt(bDiv*bDiv - log(rndmPtr->flat())); else if (pickFrac < fracAhigh + fracBhigh) bNow = sqrt(bDiv*bDiv - radius2B * log(rndmPtr->flat())); else bNow = sqrt(bDiv*bDiv - radius2C * log(rndmPtr->flat())); overlapNow = normPi * ( fracA * exp( -min(EXPMAX, bNow*bNow)) + fracB * exp( -min(EXPMAX, bNow*bNow / radius2B)) / radius2B + fracC * exp( -min(EXPMAX, bNow*bNow / radius2C)) / radius2C ); // For exp( - b^expPow) transform to variable c = b^expPow so that // f(b) = b * exp( - b^expPow) -> f(c) = c^r * exp(-c) with r = expRev. // case hasLowPow: expPow < 2 <=> r > 0: preselect according to // f(c) < N exp(-c/2) and then accept with N' * c^r * exp(-c/2). } else if (hasLowPow) { double cNow, acceptC; do { cNow = cDiv - 2. * log(rndmPtr->flat()); acceptC = pow(cNow / cMax, expRev) * exp( -0.5 * (cNow - cMax)); } while (acceptC < rndmPtr->flat()); bNow = pow( cNow, 1. / expPow); overlapNow = normPi * exp( -cNow); // case !hasLowPow: expPow >= 2 <=> - 1 < r < 0: preselect according to // f(c) < N exp(-c) and then accept with N' * c^r. } else { double cNow, acceptC; do { cNow = cDiv - log(rndmPtr->flat()); acceptC = pow(cNow / cDiv, expRev); } while (acceptC < rndmPtr->flat()); bNow = pow( cNow, 1. / expPow); overlapNow = normPi * exp( -cNow); } double temp = M_PI * kNow *overlapNow; probAccept = (1. - exp( -min(EXPMAX, temp))) / temp; } // Confirm choice of b value. Derive enhancement factor. } while (probAccept < rndmPtr->flat()); // Same enhancement for hardest process and all subsequent MPI enhanceB = enhanceBmax = enhanceBnow = (normOverlap / normPi) * overlapNow; // Done. bIsSet = true; } //-------------------------------------------------------------------------- // Pick impact parameter and interaction rate enhancement afterwards, // i.e. after a hard interaction is known but before rest of MPI treatment. void MultipartonInteractions::overlapNext(Event& event, double pTscale) { // Default, valid for bProfile = 0. Also initial Sudakov. enhanceB = zeroIntCorr; if (bProfile <= 0 || bProfile > 4) return; // Alternative choices of event scale for Sudakov in (pT, b) space. if (bSelScale == 1) { vector mmT; for (int i = 5; i < event.size(); ++i) if (event[i].isFinal()) { mmT.push_back( event[i].m() + event[i].mT() ); for (int j = int(mmT.size()) - 1; j > 0; --j) if (mmT[j] > mmT[j - 1]) swap( mmT[j], mmT[j - 1] ); } pTscale = 0.5 * mmT[0]; for (int j = 1; j < int(mmT.size()); ++j) pTscale += mmT[j] / (j + 1.); } else if (bSelScale == 2) pTscale = event.scale(); double pT2scale = pTscale*pTscale; // Use trial interaction for x-dependent matter profile. if (bProfile == 4) { double pTtrial = 0.; do { // Pick b according to wanted O(b, x1, x2). double expb2 = rndmPtr->flat(); double w1 = XDEP_A1 + a1 * log(1. / infoPtr->x1()); double w2 = XDEP_A1 + a1 * log(1. / infoPtr->x2()); double fac = a02now * (w1 * w1 + w2 * w2); b2now = - fac * log(expb2); bNow = sqrt(b2now); // Enhancement factor for the hard process and overestimate // for fastPT2. Note that existing framework has a (1. / sigmaND) // present. enhanceB = sigmaND / M_PI / fac * expb2; enhanceBmax = sigmaND / 2. / M_PI / a02now * exp( -b2now / 2. / a2max ); // Trial interaction. Keep going until pTtrial < pTscale. pTtrial = pTnext(pTmax, pTmin, event); } while (pTtrial > pTscale); bIsSet = true; return; } // Begin loop over pT-dependent rejection of b value. do { // Flat enhancement distribution for simple Gaussian. if (bProfile == 1) { double expb2 = rndmPtr->flat(); // Same enhancement for hardest process and all subsequent MPI. enhanceB = enhanceBmax = enhanceBnow = normOverlap * expb2; bNow = sqrt( -log(expb2)); // For double Gaussian go the way via b, according to each Gaussian. } else if (bProfile == 2) { double bType = rndmPtr->flat(); double b2 = -log( rndmPtr->flat() ); if (bType < fracA) ; else if (bType < fracA + fracB) b2 *= radius2B; else b2 *= radius2C; // Same enhancement for hardest process and all subsequent MPI. enhanceB = enhanceBmax = enhanceBnow = normOverlap * ( fracA * exp( -min(EXPMAX, b2)) + fracB * exp( -min(EXPMAX, b2 / radius2B)) / radius2B + fracC * exp( -min(EXPMAX, b2 / radius2C)) / radius2C ); bNow = sqrt(b2); // For exp( - b^expPow) transform to variable c = b^expPow so that // f(b) = b * exp( - b^expPow) -> f(c) = c^r * exp(-c) with r = expRev. // case hasLowPow: expPow < 2 <=> r > 0: // f(c) < r^r exp(-r) for c < 2r, < (2r)^r exp(-r-c/2) for c > 2r. } else if (bProfile == 3 && hasLowPow) { double cNow, acceptC; double probLowC = expRev / (expRev + pow(2., expRev) * exp( - expRev)); do { if (rndmPtr->flat() < probLowC) { cNow = 2. * expRev * rndmPtr->flat(); acceptC = pow( cNow / expRev, expRev) * exp(expRev - cNow); } else { cNow = 2. * (expRev - log( rndmPtr->flat() )); acceptC = pow(0.5 * cNow / expRev, expRev) * exp(expRev - 0.5 * cNow); } } while (acceptC < rndmPtr->flat()); // Same enhancement for hardest process and all subsequent MPI. enhanceB = enhanceBmax = enhanceBnow = normOverlap *exp(-cNow); bNow = pow( cNow, 1. / expPow); // case !hasLowPow: expPow >= 2 <=> - 1 < r < 0: // f(c) < c^r for c < 1, f(c) < exp(-c) for c > 1. } else if (bProfile == 3 && !hasLowPow) { double cNow, acceptC; double probLowC = expPow / (2. * exp(-1.) + expPow); do { if (rndmPtr->flat() < probLowC) { cNow = pow( rndmPtr->flat(), 0.5 * expPow); acceptC = exp(-cNow); } else { cNow = 1. - log( rndmPtr->flat() ); acceptC = pow( cNow, expRev); } } while (acceptC < rndmPtr->flat()); // Same enhancement for hardest process and all subsequent MPI. enhanceB = enhanceBmax = enhanceBnow = normOverlap * exp(-cNow); bNow = pow( cNow, 1. / expPow); } // Evaluate "Sudakov form factor" for not having a harder interaction. } while (sudakov(pT2scale, enhanceB) < rndmPtr->flat()); // Done. bIsSet = true; } //-------------------------------------------------------------------------- // Printe statistics on number of multiparton-interactions processes. void MultipartonInteractions::statistics(bool resetStat, ostream& os) { // Header. os << "\n *------- PYTHIA Multiparton Interactions Statistics -----" << "---*\n" << " | " << " |\n" << " | Note: excludes hardest subprocess if already listed above " << " |\n" << " | " << " |\n" << " | Subprocess Code | Times" << " |\n" << " | | " << " |\n" << " |------------------------------------------------------------" << "-|\n" << " | | " << " |\n"; // Loop over existing processes. Sum of all subprocesses. int numberSum = 0; for ( map::iterator iter = nGen.begin(); iter != nGen.end(); ++iter) { int code = iter -> first; int number = iter->second; numberSum += number; // Find process name that matches code. string name = " "; bool foundName = false; SigmaMultiparton* dSigma; for (int i = 0; i < 4; ++i) { if (i == 0) dSigma = &sigma2gg; else if (i == 1) dSigma = &sigma2qg; else if (i == 2) dSigma = &sigma2qqbarSame; else dSigma = &sigma2qq; int nProc = dSigma->nProc(); for (int iProc = 0; iProc < nProc; ++iProc) if (dSigma->codeProc(iProc) == code) { name = dSigma->nameProc(iProc); foundName = true; } if (foundName) break; } // Print individual process info. os << " | " << left << setw(40) << name << right << setw(5) << code << " | " << setw(11) << number << " |\n"; } // Print summed process info. os << " | " << " |\n" << " | " << left << setw(45) << "sum" << right << " | " << setw(11) << numberSum << " |\n"; // Listing finished. os << " | | " << " |\n" << " *------- End PYTHIA Multiparton Interactions Statistics ----" << "-*" << endl; // Optionally reset statistics contents. if (resetStat) resetStatistics(); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/HelicityMatrixElements.cc0000644000175000017500000023412012217346245020073 0ustar sunsun// HelicityMatrixElements.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Philip Ilten, Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for physics classes // used in tau decays. #include "Pythia8/HelicityMatrixElements.h" namespace Pythia8 { //========================================================================== // The HelicityMatrixElements class. //-------------------------------------------------------------------------- // Initialize the helicity matrix element. void HelicityMatrixElement::initPointers(ParticleData* particleDataPtrIn, Couplings* couplingsPtrIn) { particleDataPtr = particleDataPtrIn; couplingsPtr = couplingsPtrIn; for(int i = 0; i <= 5; i++) gamma.push_back(GammaMatrix(i)); } //-------------------------------------------------------------------------- // Initialize the channel for the helicity matrix element. HelicityMatrixElement* HelicityMatrixElement::initChannel( vector& p) { pID.clear(); pM.clear(); for(int i = 0; i < static_cast(p.size()); i++) { pID.push_back(p[i].id()); pM.push_back(p[i].m()); } initConstants(); return this; } //-------------------------------------------------------------------------- // Calculate a particle's decay matrix. void HelicityMatrixElement::calculateD(vector& p) { // Reset the D matrix to zero. for (int i = 0; i < p[0].spinStates(); i++) { for (int j = 0; j < p[0].spinStates(); j++) { p[0].D[i][j] = 0; } } // Initialize the wave functions. initWaves(p); // Create the helicity vectors. vector h1(p.size(),0); vector h2(p.size(),0); // Call the recursive sub-method. calculateD(p, h1, h2, 0); // Normalize the decay matrix. p[0].normalize(p[0].D); } //-------------------------------------------------------------------------- // Recursive sub-method for calculating a particle's decay matrix. void HelicityMatrixElement::calculateD(vector& p, vector& h1, vector& h2, unsigned int i) { if (i < p.size()) { for (h1[i] = 0; h1[i] < p[i].spinStates(); h1[i]++) { for (h2[i] = 0; h2[i] < p[i].spinStates(); h2[i]++) { calculateD(p, h1, h2, i+1); } } } else { p[0].D[h1[0]][h2[0]] += calculateME(h1) * conj(calculateME(h2)) * calculateProductD(p, h1, h2); } } //-------------------------------------------------------------------------- // Calculate a particle's helicity density matrix. void HelicityMatrixElement::calculateRho(unsigned int idx, vector& p) { // Reset the rho matrix to zero. for (int i = 0; i < p[idx].spinStates(); i++) { for (int j = 0; j < p[idx].spinStates(); j++) { p[idx].rho[i][j] = 0; } } // Initialize the wave functions. initWaves(p); // Create the helicity vectors. vector h1(p.size(),0); vector h2(p.size(),0); // Call the recursive sub-method. calculateRho(idx, p, h1, h2, 0); // Normalize the density matrix. p[idx].normalize(p[idx].rho); } //-------------------------------------------------------------------------- // Recursive sub-method for calculating a particle's helicity density matrix. void HelicityMatrixElement::calculateRho(unsigned int idx, vector& p, vector& h1, vector& h2, unsigned int i) { if (i < p.size()) { for (h1[i] = 0; h1[i] < p[i].spinStates(); h1[i]++) { for (h2[i] = 0; h2[i] < p[i].spinStates(); h2[i]++) { calculateRho(idx, p, h1, h2, i+1); } } } else { // Calculate rho from a hard process. if (p[1].direction < 0) p[idx].rho[h1[idx]][h2[idx]] += p[0].rho[h1[0]][h2[0]] * p[1].rho[h1[1]][h2[1]] * calculateME(h1)*conj(calculateME(h2)) * calculateProductD(idx, 2, p, h1, h2); // Calculate rho from a decay. else p[idx].rho[h1[idx]][h2[idx]] += p[0].rho[h1[0]][h2[0]] * calculateME(h1)*conj(calculateME(h2)) * calculateProductD(idx, 1, p, h1, h2); return; } } //-------------------------------------------------------------------------- // Calculate a decay's weight. double HelicityMatrixElement::decayWeight(vector& p) { complex weight = complex(0,0); // Initialize the wave functions. initWaves(p); // Create the helicity vectors. vector h1(p.size(),0); vector h2(p.size(),0); // Call the recursive sub-method. decayWeight(p, h1, h2, weight, 0); return real(weight); } //-------------------------------------------------------------------------- // Recursive sub-method for calculating a decay's weight. void HelicityMatrixElement::decayWeight(vector& p, vector& h1, vector& h2, complex& weight, unsigned int i) { if (i < p.size()) { for (h1[i] = 0; h1[i] < p[i].spinStates(); h1[i]++) { for (h2[i] = 0; h2[i] < p[i].spinStates(); h2[i]++) { decayWeight(p, h1, h2, weight, i+1); } } } else { weight += p[0].rho[h1[0]][h2[0]] * calculateME(h1) * conj(calculateME(h2)) * calculateProductD(p, h1, h2); } } //-------------------------------------------------------------------------- // Calculate the product of the decay matrices (hard process). complex HelicityMatrixElement::calculateProductD(unsigned int idx, unsigned int start, vector& p, vector& h1, vector& h2) { complex answer(1,0); for (unsigned int i = start; i < p.size(); i++) { if (i != idx) { answer *= p[i].D[h1[i]][h2[i]]; } } return answer; } //-------------------------------------------------------------------------- // Calculate the product of the decay matrices (decay process). complex HelicityMatrixElement::calculateProductD( vector& p, vector& h1, vector& h2) { complex answer(1,0); for (unsigned int i = 1; i < p.size(); i++) { answer *= p[i].D[h1[i]][h2[i]]; } return answer; } //-------------------------------------------------------------------------- // Initialize a fermion line. void HelicityMatrixElement::setFermionLine(int position, HelicityParticle& p0, HelicityParticle& p1) { vector< Wave4 > u0, u1; // First particle is incoming and particle, or outgoing and anti-particle. if (p0.id()*p0.direction < 0) { pMap[position] = position; pMap[position+1] = position+1; for (int h = 0; h < p0.spinStates(); h++) u0.push_back(p0.wave(h)); for (int h = 0; h < p1.spinStates(); h++) u1.push_back(p1.waveBar(h)); } // First particle is outgoing and particle, or incoming and anti-particle. else { pMap[position] = position+1; pMap[position+1] = position; for (int h = 0; h < p0.spinStates(); h++) u1.push_back(p0.waveBar(h)); for (int h = 0; h < p1.spinStates(); h++) u0.push_back(p1.wave(h)); } u.push_back(u0); u.push_back(u1); } //-------------------------------------------------------------------------- // Return a fixed width Breit-Wigner. complex HelicityMatrixElement::breitWigner(double s, double M, double G) { return (-M*M + complex(0, 1) * M * G) / (s - M*M + complex(0, 1) * M * G); } //-------------------------------------------------------------------------- // Return an s-wave BreitWigner. complex HelicityMatrixElement::sBreitWigner(double m0, double m1, double s, double M, double G) { double gs = sqrtpos((s - pow2(m0+m1)) * (s - pow2(m0-m1))) / (2*sqrtpos(s)); double gM = sqrtpos((M*M - pow2(m0+m1)) * (M*M - pow2(m0-m1))) / (2*M); return M*M / (M*M - s - complex(0,1)*G*M*M/sqrtpos(s)*(gs/gM)); } //-------------------------------------------------------------------------- // Return a p-wave BreitWigner. complex HelicityMatrixElement::pBreitWigner(double m0, double m1, double s, double M, double G) { double gs = sqrtpos((s - pow2(m0+m1)) * (s - pow2(m0-m1))) / (2*sqrtpos(s)); double gM = sqrtpos((M*M - pow2(m0+m1)) * (M*M - pow2(m0-m1))) / (2*M); return M*M / (M*M - s - complex(0,1)*G*M*M/sqrtpos(s)*pow3(gs/gM)); } //-------------------------------------------------------------------------- // Return a d-wave BreitWigner. complex HelicityMatrixElement::dBreitWigner(double m0, double m1, double s, double M, double G) { double gs = sqrtpos((s - pow2(m0+m1)) * (s - pow2(m0-m1))) / (2*sqrtpos(s)); double gM = sqrtpos((M*M - pow2(m0+m1)) * (M*M - pow2(m0-m1))) / (2*M); return M*M / (M*M - s - complex(0,1)*G*M*M/sqrtpos(s)*pow5(gs/gM)); } //========================================================================== // Helicity matrix element for two fermions -> W -> two fermions. This matrix // element handles s-channel hard processes in addition to t-channel, assuming // the first two particles are a fermion line and the second two particles // are a fermion line. This matrix element is not scaled with respect to W // propagator energy as currently this matrix element is used only for // calculating helicity density matrices. //-------------------------------------------------------------------------- // Initialize spinors for the helicity matrix element. void HMETwoFermions2W2TwoFermions::initWaves(vector& p) { u.clear(); pMap.resize(4); setFermionLine(0,p[0],p[1]); setFermionLine(2,p[2],p[3]); } //-------------------------------------------------------------------------- // Return element for the helicity matrix element. complex HMETwoFermions2W2TwoFermions::calculateME(vector h) { complex answer(0,0); for (int mu = 0; mu <= 3; mu++) { answer += (u[1][h[pMap[1]]] * gamma[mu] * (1 - gamma[5]) * u[0][h[pMap[0]]]) * gamma[4](mu,mu) * (u[3][h[pMap[3]]] * gamma[mu] * (1 - gamma[5]) * u[2][h[pMap[2]]]); } return answer; } //========================================================================== // Helicity matrix element for two fermions -> photon -> two fermions. This // matrix element can be combined with the Z matrix element to provide full // interference effects. // p0Q: charge of the incoming fermion line // p2Q: charge of the outgoing fermion line // s: center of mass energy //-------------------------------------------------------------------------- // Initialize wave functions for the helicity matrix element. void HMETwoFermions2Gamma2TwoFermions::initWaves( vector& p) { u.clear(); pMap.resize(4); setFermionLine(0, p[0], p[1]); setFermionLine(2, p[2], p[3]); s = max( 1., pow2(p[4].m())); p0Q = p[0].charge(); p2Q = p[2].charge(); } //-------------------------------------------------------------------------- // Return element for the helicity matrix element. complex HMETwoFermions2Gamma2TwoFermions::calculateME(vector h) { complex answer(0,0); for (int mu = 0; mu <= 3; mu++) { answer += (u[1][h[pMap[1]]] * gamma[mu] * u[0][h[pMap[0]]]) * gamma[4](mu,mu) * (u[3][h[pMap[3]]] * gamma[mu] * u[2][h[pMap[2]]]); } return p0Q*p2Q * answer / s; } //========================================================================== // Helicity matrix element for two fermions -> Z -> two fermions. This matrix // element can be combined with the photon matrix element to provide full // interference effects. // Note that there is a double contraction in the Z matrix element, which can // be very time consuming. If the two incoming fermions are oriented along // the z-axis, their helicities must be opposite for a non-zero matrix element // term. Consequently, this check is made to help speed up the matrix element. // sin2W: sine of the Weinberg angle // cos2W: cosine of the Weinberg angle // zM: on-shell mass of the Z // zG: on-shell width of the Z // p0CA: axial coupling of particle 0 to the Z // p2CA: axial coupling of particle 2 to the Z // p0CV: vector coupling of particle 0 to the Z // p2CV: vector coupling of particle 2 to the Z // zaxis: true if the incoming fermions are oriented along the z-axis //-------------------------------------------------------------------------- // Initialize the constant for the helicity matrix element. void HMETwoFermions2Z2TwoFermions::initConstants() { // Set the Weinberg angle. sin2W = couplingsPtr->sin2thetaW(); cos2W = couplingsPtr->cos2thetaW(); // Set the on-shell Z mass and width. zG = particleDataPtr->mWidth(23); zM = particleDataPtr->m0(23); // Set the vector and axial couplings to the fermions. p0CA = couplingsPtr->af(abs(pID[0])); p2CA = couplingsPtr->af(abs(pID[2])); p0CV = couplingsPtr->vf(abs(pID[0])); p2CV = couplingsPtr->vf(abs(pID[2])); } //-------------------------------------------------------------------------- // Initialize wave functions for the helicity matrix element. void HMETwoFermions2Z2TwoFermions::initWaves(vector& p) { vector< Wave4 > u4; u.clear(); pMap.resize(4); setFermionLine(0, p[0], p[1]); setFermionLine(2, p[2], p[3]); u4.push_back(Wave4(p[2].p() + p[3].p())); u.push_back(u4); // Center of mass energy. s = max( 1., pow2(p[4].m())); // Check if incoming fermions are oriented along z-axis. zaxis = (p[0].pAbs() == fabs(p[0].pz())) && (p[1].pAbs() == fabs(p[1].pz())); } //-------------------------------------------------------------------------- // Return element for helicity matrix element. complex HMETwoFermions2Z2TwoFermions::calculateME(vector h) { complex answer(0,0); // Return zero if correct helicity conditions. if (h[0] == h[1] && zaxis) return answer; for (int mu = 0; mu <= 3; mu++) { for (int nu = 0; nu <= 3; nu++) { answer += (u[1][h[pMap[1]]] * gamma[mu] * (p0CV - p0CA * gamma[5]) * u[0][h[pMap[0]]]) * (gamma[4](mu,nu) - gamma[4](mu,mu)*u[4][0](mu) * gamma[4](nu,nu) * u[4][0](nu) / (zM*zM)) * (u[3][h[pMap[3]]] * gamma[nu] * (p2CV - p2CA * gamma[5]) * u[2][h[pMap[2]]]); } } return answer / (16 * pow2(sin2W * cos2W) * (s - zM*zM + complex(0, s*zG/zM))); } //========================================================================== // Helicity matrix element for two fermions -> photon/Z -> two fermions. Full // interference is obtained by combining the photon and Z helicity matrix // elements. // In general the initPointers and initChannel methods should not be // redeclared. //-------------------------------------------------------------------------- // Initialize the matrix element. void HMETwoFermions2GammaZ2TwoFermions::initPointers( ParticleData* particleDataPtrIn, Couplings* couplingsPtrIn) { zHME.initPointers(particleDataPtrIn, couplingsPtrIn); gHME.initPointers(particleDataPtrIn, couplingsPtrIn); } //-------------------------------------------------------------------------- // Initialize the channel for the helicity matrix element. HelicityMatrixElement* HMETwoFermions2GammaZ2TwoFermions::initChannel( vector& p) { zHME.initChannel(p); zHME.initChannel(p); return this; } //-------------------------------------------------------------------------- // Initialize wave functions for the helicity matrix element. void HMETwoFermions2GammaZ2TwoFermions::initWaves( vector& p) { zHME.initWaves(p); gHME.initWaves(p); } //-------------------------------------------------------------------------- // Return element for the helicity matrix element. complex HMETwoFermions2GammaZ2TwoFermions::calculateME(vector h) { return zHME.calculateME(h) + gHME.calculateME(h); } //========================================================================== // Helicity matrix element for Z -> two fermions. // Helicity matrix element for Z -> two fermions. This matrix element is used // when the production of the Z is from an unknown process. // p2CA: axial coupling of particle 2 to the Z // p2CV: vector coupling of particle 2 to the Z //-------------------------------------------------------------------------- // Initialize the constant for the helicity matrix element. void HMEZ2TwoFermions::initConstants() { // Set the vector and axial couplings to the fermions. p2CA = couplingsPtr->af(abs(pID[2])); p2CV = couplingsPtr->vf(abs(pID[2])); } //-------------------------------------------------------------------------- // Initialize wave functions for the helicity matrix element. void HMEZ2TwoFermions::initWaves(vector& p) { u.clear(); pMap.resize(4); // Initialize Z wave function. vector< Wave4 > u1; pMap[1] = 1; for (int h = 0; h < p[pMap[1]].spinStates(); h++) u1.push_back(p[pMap[1]].wave(h)); u.push_back(u1); // Initialize fermion wave functions. setFermionLine(2, p[2], p[3]); } //-------------------------------------------------------------------------- // Return element for helicity matrix element. complex HMEZ2TwoFermions::calculateME(vector h) { complex answer(0,0); for (int mu = 0; mu <= 3; mu++) { answer += u[0][h[pMap[1]]](mu) * (u[2][h[pMap[3]]] * gamma[mu] * (p2CV - p2CA * gamma[5]) * u[1][h[pMap[2]]]); } return answer; } //========================================================================== // Helicity matrix element for the decay of a CP even Higgs to two fermions. // All SM and MSSM Higgses couple to fermions with a vertex factor of // (pfCV - pfCA * gamma[5]) where pf indicates the type of fermion line. For // simplicity for the SM and MSSM CP even Higgses pfCV is set to one, and // pfCA to zero, as this matrix element is used only for calculating helicity // density matrices. // p2CA: in the SM and MSSM this coupling is zero // p2CV: in the SM and MSSM this coupling is given by: // i * g_w * m_f / (2 * m_W) // * -1 for the SM H // * -sin(alpha) / sin(beta) for H^0 u-type // * -cos(alpha) / cos(beta) for H^0 d-type // * -cos(alpha) / sin(beta) for h^0 u-type // * sin(alpha) / cos(beta) for h^0 d-type //-------------------------------------------------------------------------- // Initialize wave functions for the helicity matrix element. void HMEHiggsEven2TwoFermions::initWaves(vector& p) { u.clear(); pMap.resize(4); p2CA = 0; p2CV = 1; setFermionLine(2, p[2], p[3]); } //-------------------------------------------------------------------------- // Return element for the helicity matrix element. complex HMEHiggsEven2TwoFermions::calculateME(vector h) { return (u[1][h[pMap[3]]] * (p2CV - p2CA * gamma[5]) * u[0][h[pMap[2]]]); } //========================================================================== // Helicity matrix element for the decay of a CP odd Higgs to two fermions. // See HMEHiggsEven2TwoFermions for more details. For the MSSM CP odd Higgs // pfCA is set to one and pfCV is set to zero. // p2CA: in the MSSM this coupling is given by: // -g_w * m_f / (2 * m_W) // * cot(beta) for A^0 u-type // * tan(beta) for A^0 d-type // p2CV: in the MSSM this coupling is zero //-------------------------------------------------------------------------- // Initialize wave functions for the helicity matrix element. void HMEHiggsOdd2TwoFermions::initWaves(vector& p) { u.clear(); pMap.resize(4); p2CA = 1; p2CV = 0; setFermionLine(2, p[2], p[3]); } //-------------------------------------------------------------------------- // Return element for the helicity matrix element. complex HMEHiggsOdd2TwoFermions::calculateME(vector h) { return (u[1][h[pMap[3]]] * (p2CV - p2CA * gamma[5]) * u[0][h[pMap[2]]]); } //========================================================================== // Helicity matrix element for the decay of a charged Higgs to two fermions. // See HMEHiggsEven2TwoFermions for more details. For the MSSM charged Higgs // pfCA is set to +/- one given an H^+/- and pfCV is set to one. // p2CA: in the MSSM this coupling is given by: // i * g / (sqrt(8.) * m_W) * (m_d * tan(beta) + m_u * cot(beta)) // p2CV: in the MSSM this coupling is given by: // +/- i * g / (sqrt(8.) * m_W) * (m_d * tan(beta) - m_u * cot(beta)) //-------------------------------------------------------------------------- // Initialize wave functions for the helicity matrix element. void HMEHiggsCharged2TwoFermions::initWaves(vector& p) { u.clear(); pMap.resize(4); p2CV = 1; if (pID[3] == 15 || pID[3] == -16) p2CA = 1; else p2CA = -1; setFermionLine(2, p[2], p[3]); } //-------------------------------------------------------------------------- // Return element for the helicity matrix element. complex HMEHiggsCharged2TwoFermions::calculateME(vector h) { return (u[1][h[pMap[3]]] * (p2CV - p2CA * gamma[5]) * u[0][h[pMap[2]]]); } //========================================================================== // Helicity matrix element which provides an unpolarized helicity // density matrix. This matrix element is used for unkown hard processes. // Note that calculateRho is redefined for this special case, but that in // general calculateRho should not be redefined. //-------------------------------------------------------------------------- // Calculate a particle's helicity density matrix. void HMEUnpolarized::calculateRho(unsigned int idx, vector& p) { for (int i = 0; i < p[idx].spinStates(); i++ ) { for (int j = 1; j < p[idx].spinStates(); j++) { if (i == j) p[idx].rho[i][j] = 1.0 / static_cast(p[idx].spinStates()); else p[idx].rho[i][j] = 0; } } } //========================================================================== // Base class for all tau decay matrix elements. This class derives from // the HelicityMatrixElement class and redefines some of the virtual functions. // One new method, initHadronicCurrent is defined which initializes the // hadronic current in the initWaves method. For each tau decay matrix element // the hadronic current method must be redefined accordingly, but initWaves // should not be redefined. //-------------------------------------------------------------------------- // Initialize wave functions for the helicity matrix element. void HMETauDecay::initWaves(vector& p) { u.clear(); pMap.resize(p.size()); setFermionLine(0, p[0], p[1]); initHadronicCurrent(p); } //-------------------------------------------------------------------------- // Return element for the helicity matrix element. complex HMETauDecay::calculateME(vector h) { complex answer(0,0); for (int mu = 0; mu <= 3; mu++) { answer += (u[1][h[pMap[1]]] * gamma[mu] * (1 - gamma[5]) * u[0][h[pMap[0]]]) * gamma[4](mu,mu) * u[2][0](mu); } return answer; } //-------------------------------------------------------------------------- // Return the maximum decay weight for the helicity matrix element. double HMETauDecay::decayWeightMax(vector& p) { // Determine the maximum on-diagonal element of rho. double on = real(p[0].rho[0][0]) > real(p[0].rho[1][1]) ? real(p[0].rho[0][0]) : real(p[0].rho[1][1]); // Determine the maximum off-diagonal element of rho. double off = fabs(real(p[0].rho[0][1])) + fabs(imag(p[0].rho[0][1])); return DECAYWEIGHTMAX * (on + off); } //-------------------------------------------------------------------------- // Calculate complex resonance weights given a phase and amplitude vector. void HMETauDecay::calculateResonanceWeights(vector& phase, vector& amplitude, vector& weight) { for (unsigned int i = 0; i < phase.size(); i++) weight.push_back(amplitude[i] * (cos(phase[i]) + complex(0,1) * sin(phase[i]))); } //========================================================================== // Tau decay matrix element for tau decay into a single scalar meson. // The maximum decay weight for this matrix element can be found analytically // to be 4 * m_tau^2 * (m_tau^2 - m_meson^2). However, because m_tau >> m_meson // for the relevant tau decay channels, this expression is approximated by // m_tau^4. //-------------------------------------------------------------------------- // Initialize constants for the helicity matrix element. void HMETau2Meson::initConstants() { DECAYWEIGHTMAX = 4*pow4(pM[0]); } //-------------------------------------------------------------------------- // Initialize the hadronic current for the helicity matrix element. void HMETau2Meson::initHadronicCurrent(vector& p) { vector< Wave4 > u2; pMap[2] = 2; u2.push_back(Wave4(p[2].p())); u.push_back(u2); } //========================================================================== // Tau decay matrix element for tau decay into two leptons. Because there is // no hadronic current, but rather a leptonic current, the calculateME and // initWaves methods must be redefined. //-------------------------------------------------------------------------- // Initialize constants for the helicity matrix element. void HMETau2TwoLeptons::initConstants() { DECAYWEIGHTMAX = 16*pow4(pM[0]); } //-------------------------------------------------------------------------- // Initialize spinors for the helicity matrix element. void HMETau2TwoLeptons::initWaves(vector& p) { u.clear(); pMap.resize(4); setFermionLine(0,p[0],p[1]); setFermionLine(2,p[2],p[3]); } //-------------------------------------------------------------------------- // Return element for the helicity matrix element. complex HMETau2TwoLeptons::calculateME(vector h) { complex answer(0,0); for (int mu = 0; mu <= 3; mu++) { answer += (u[1][h[pMap[1]]] * gamma[mu] * (1 - gamma[5]) * u[0][h[pMap[0]]]) * gamma[4](mu,mu) * (u[3][h[pMap[3]]] * gamma[mu] * (1 - gamma[5]) * u[2][h[pMap[2]]]); } return answer; } //========================================================================== // Tau decay matrix element for tau decay into two mesons through an // intermediate vector meson. This matrix element is used for pi^0 + pi^- // decays (rho resonances), K^0 + K^- decays (rho resonances), and eta + K^- // decays (K^* resonances). Note that for the rho resonances the pi^0 + pi^- // running width dominates while for the K^* resonances the pi^- + K^0 running // width dominates. // vecM: on-shell masses for the vector resonances // vecG: on-shell widths for the vector resonances // vecP: phases used to calculate vector resonance weights // vecA: amplitudes used to calculate vector resonance weights // vecW: vector resonance weights //-------------------------------------------------------------------------- // Initialize constants for the helicity matrix element. void HMETau2TwoMesonsViaVector::initConstants() { // Clear the vectors from previous decays. vecM.clear(); vecG.clear(); vecP.clear(); vecA.clear(); vecW.clear(); // Decay through K^* resonances (eta + K^- decay). if (abs(pID[2]) == 221) { DECAYWEIGHTMAX = 10; pM[2] = particleDataPtr->m0(211); pM[3] = particleDataPtr->m0(311); vecM.push_back(0.8921); vecM.push_back(1.700); vecG.push_back(0.0513); vecG.push_back(0.235); vecP.push_back(0); vecP.push_back(M_PI); vecA.push_back(1); vecA.push_back(0.038); } // Decay through rho resonances (pi^0 + pi^- and K^0 + K^- decays). else { if (abs(pID[2]) == 111) DECAYWEIGHTMAX = 800; else if (abs(pID[2]) == 311) DECAYWEIGHTMAX = 6; pM[2] = particleDataPtr->m0(111); pM[3] = particleDataPtr->m0(211); vecM.push_back(0.7746); vecM.push_back(1.4080); vecM.push_back(1.700); vecG.push_back(0.1490); vecG.push_back(0.5020); vecG.push_back(0.235); vecP.push_back(0); vecP.push_back(M_PI); vecP.push_back(0); vecA.push_back(1.0); vecA.push_back(0.167); vecA.push_back(0.050); } calculateResonanceWeights(vecP, vecA, vecW); } //-------------------------------------------------------------------------- // Initialize the hadronic current for the helicity matrix element. void HMETau2TwoMesonsViaVector::initHadronicCurrent( vector& p) { vector< Wave4 > u2; Wave4 u3(p[3].p() - p[2].p()); Wave4 u4(p[2].p() + p[3].p()); double s1 = m2(u3, u4); double s2 = m2(u4); complex sumBW = 0; for (unsigned int i = 0; i < vecW.size(); i++) sumBW += vecW[i] * pBreitWigner(pM[2], pM[3], s2, vecM[i], vecG[i]); u2.push_back((u3 - s1 / s2 * u4) * sumBW); u.push_back(u2); } //========================================================================== // Tau decay matrix element for tau decay into two mesons through both // intermediate vector and scalar mesons. // scaC: scalar coupling constant // scaM: on-shell masses for the scalar resonances // scaG: on-shell widths for the scalar resonances // scaP: phases used to calculate scalar resonance weights // scaA: amplitudes used to calculate scalar resonance weights // scaW: scalar resonance weights // vecC: scalar coupling constant // vecM: on-shell masses for the vector resonances // vecG: on-shell widths for the vector resonances // vecP: phases used to calculate vector resonance weights // vecA: amplitudes used to calculate vector resonance weights // vecW: vector resonance weights //-------------------------------------------------------------------------- // Initialize constants for the helicity matrix element. void HMETau2TwoMesonsViaVectorScalar::initConstants() { DECAYWEIGHTMAX = 5400; // Clear the vectors from previous decays. scaM.clear(); scaG.clear(); scaP.clear(); scaA.clear(); scaW.clear(); vecM.clear(); vecG.clear(); vecP.clear(); vecA.clear(); vecW.clear(); // Scalar resonance parameters. scaC = 0.465; scaM.push_back(0.878); scaG.push_back(0.499); scaP.push_back(0); scaA.push_back(1); calculateResonanceWeights(scaP, scaA, scaW); // Vector resonance parameters. vecC = 1; vecM.push_back(0.89547); vecM.push_back(1.414); vecG.push_back(0.04619); vecG.push_back(0.232); vecP.push_back(0); vecP.push_back(1.4399); vecA.push_back(1); vecA.push_back(0.075); calculateResonanceWeights(vecP, vecA, vecW); } //-------------------------------------------------------------------------- // Initialize the hadronic current for the helicity matrix element. void HMETau2TwoMesonsViaVectorScalar::initHadronicCurrent( vector& p) { vector< Wave4 > u2; Wave4 u3(p[3].p() - p[2].p()); Wave4 u4(p[2].p() + p[3].p()); double s1 = m2(u3,u4); double s2 = m2(u4); complex scaSumBW = 0; complex scaSumW = 0; complex vecSumBW = 0; complex vecSumW = 0; complex vecSumBWM = 0; for (unsigned int i = 0; i < scaW.size(); i++) { scaSumBW += scaW[i] * sBreitWigner(pM[2], pM[3], s2, scaM[i], scaG[i]); scaSumW += scaW[i]; } for (unsigned int i = 0; i < vecW.size(); i++) { vecSumBW += vecW[i] * pBreitWigner(pM[2], pM[3], s2, vecM[i], vecG[i]); vecSumBWM += vecW[i] * pBreitWigner(pM[2], pM[3], s2, vecM[i], vecG[i]) / pow2(vecM[i]); vecSumW += vecW[i]; } u2.push_back(vecC * (vecSumBW * u3 - s1 * vecSumBWM * u4) / vecSumW + scaC * u4 * scaSumBW / scaSumW); u.push_back(u2); } //========================================================================== // Tau decay matrix element for tau decay into three mesons. This matrix // element provides a base class for all implemented three meson decays. // mode: three meson decay mode of the tau // initMode(): initialize the decay mode // initResonances(): initialize the resonance constants // s1, s2, s3, s4: center-of-mass energies // q, q2, q3, q4: summed and individual hadronic momentum four-vectors // a1BW: stored value of a1BreitWigner for speed // a1PhaseSpace(s): phase space factor for the a1 // a1BreitWigner(s): Breit-Wigner for the a1 // T(m0, m1, s, M, G, W): sum weighted p-wave Breit-Wigners // T(s, M, G, W): sum weighted fixed width Breit-Wigners // F1(), F2(), F3(), F4(): sub-current form factors //-------------------------------------------------------------------------- // Initialize constants for the helicity matrix element. void HMETau2ThreeMesons::initConstants() { initMode(); initResonances(); } //-------------------------------------------------------------------------- // Initialize the hadronic current for the helicity matrix element. void HMETau2ThreeMesons::initHadronicCurrent(vector& p) { vector< Wave4 > u2; // Initialize the momenta. initMomenta(p); // Calculate the center of mass energies. s1 = m2(q); s2 = m2(q3 + q4); s3 = m2(q2 + q4); s4 = m2(q2 + q3); // Calculate the form factors. a1BW = a1BreitWigner(s1); complex f1 = F1(); complex f2 = F2(); complex f3 = F3(); complex f4 = F4(); // Calculate the hadronic current. Wave4 u3 = (f3 - f2) * q2 + (f1 - f3) * q3 + (f2 - f1) * q4; u3 = u3 - (u3 * gamma[4] * q / s1) * q; if (f4 != complex(0, 0)) u3 = u3 + complex(0, 1) * f4 * epsilon(q2, q3, q4); u2.push_back(u3); u.push_back(u2); } //-------------------------------------------------------------------------- // Initialize the tau decay mode. void HMETau2ThreeMesons::initMode() { if (abs(pID[2]) == 111 && abs(pID[3]) == 111 && abs(pID[4]) == 211) mode = Pi0Pi0Pim; else if (abs(pID[2]) == 211 && abs(pID[3]) == 211 && abs(pID[4]) == 211) mode = PimPimPip; else if (abs(pID[2]) == 111 && abs(pID[3]) == 211 && abs(pID[4]) == 311) mode = Pi0PimK0b; else if (abs(pID[2]) == 211 && abs(pID[3]) == 211 && abs(pID[4]) == 321) mode = PimPipKm; else if (abs(pID[2]) == 111 && abs(pID[3]) == 211 && abs(pID[4]) == 221) mode = Pi0PimEta; else if (abs(pID[2]) == 211 && abs(pID[3]) == 321 && abs(pID[4]) == 321) mode = PimKmKp; else if (abs(pID[2]) == 111 && abs(pID[3]) == 311 && abs(pID[4]) == 321) mode = Pi0K0Km; else if (abs(pID[2]) == 130 && abs(pID[3]) == 211 && abs(pID[4]) == 310) mode = KlPimKs; else if (abs(pID[2]) == 111 && abs(pID[3]) == 111 && abs(pID[4]) == 321) mode = Pi0Pi0Km; else if (abs(pID[2]) == 130 && abs(pID[3]) == 130 && abs(pID[4]) == 211) mode = KlKlPim; else if (abs(pID[2]) == 211 && abs(pID[3]) == 310 && abs(pID[4]) == 310) mode = PimKsKs; else if (abs(pID[2]) == 211 && abs(pID[3]) == 311 && abs(pID[4]) == 311) mode = PimK0bK0; else mode = Uknown; } //-------------------------------------------------------------------------- // Initialize the momenta for the helicity matrix element. void HMETau2ThreeMesons::initMomenta(vector& p) { q = Wave4(p[2].p() + p[3].p() + p[4].p()); // pi-, pi-, pi+ decay and pi0, pi0, pi- decay. if (mode == PimPimPip || mode == Pi0Pi0Pim) { q2 = Wave4(p[2].p()); q3 = Wave4(p[3].p()); q4 = Wave4(p[4].p()); // K-, pi-, K+ decay. } else if (mode == PimKmKp) { q2 = Wave4(p[3].p()); q3 = Wave4(p[2].p()); q4 = Wave4(p[4].p()); // K0, pi-, Kbar0 decay. } else if (mode == PimK0bK0) { q2 = Wave4(p[3].p()); q3 = Wave4(p[2].p()); q4 = Wave4(p[4].p()); // K_S0, pi-, K_S0 decay. } else if (mode == PimKsKs) { q2 = Wave4(p[3].p()); q3 = Wave4(p[2].p()); q4 = Wave4(p[4].p()); // K_L0, pi-, K_L0 decay. } else if (mode == KlKlPim) { q2 = Wave4(p[2].p()); q3 = Wave4(p[4].p()); q4 = Wave4(p[3].p()); // K_S0, pi-, K_L0 decay. } else if (mode == KlPimKs) { q2 = Wave4(p[4].p()); q3 = Wave4(p[3].p()); q4 = Wave4(p[2].p()); } // K-, pi0, K0 decay. else if (mode == Pi0K0Km) { q2 = Wave4(p[4].p()); q3 = Wave4(p[2].p()); q4 = Wave4(p[3].p()); } // pi0, pi0, K- decay. else if (mode == Pi0Pi0Km) { q2 = Wave4(p[2].p()); q3 = Wave4(p[3].p()); q4 = Wave4(p[4].p()); } // K-, pi-, pi+ decay. else if (mode == PimPipKm) { q2 = Wave4(p[4].p()); q3 = Wave4(p[2].p()); q4 = Wave4(p[3].p()); } // pi-, Kbar0, pi0 decay. else if (mode == Pi0PimK0b) { q2 = Wave4(p[3].p()); q3 = Wave4(p[4].p()); q4 = Wave4(p[2].p()); } // pi-, pi0, eta decay. else if (mode == Pi0PimEta) { q2 = Wave4(p[3].p()); q3 = Wave4(p[2].p()); q4 = Wave4(p[4].p()); } } //-------------------------------------------------------------------------- // Return the phase space factor for the a1. Implements equation 3.16 of Z. // Phys. C48 (1990) 445-452. double HMETau2ThreeMesons::a1PhaseSpace(double s) { double piM = 0.13957; // Mass of the charged pion. double rhoM = 0.773; // Mass of the rho. if (s < pow2(3 * piM)) return 0; else if (s < pow2(rhoM + piM)) { double sum = (s - 9 * piM * piM); return 4.1 * sum * sum * sum * (1 - 3.3 * sum + 5.8 * sum * sum); } else return s * (1.623 + 10.38 / s - 9.32 / (s * s) + 0.65 / (s * s * s)); } //-------------------------------------------------------------------------- // Return the Breit-Wigner for the a1. Implements equation 3.18 // of Z. Phys. C48 (1990) 445-452. complex HMETau2ThreeMesons::a1BreitWigner(double s) { double a1M = 1.251; // Mass of the a1. double a1G = 0.475; // Width of the a1. return a1M * a1M / (a1M * a1M - s - complex(0,1) * a1M * a1G * a1PhaseSpace(s) / a1PhaseSpace(a1M * a1M)); } //-------------------------------------------------------------------------- // Return summed weighted running p Breit-Wigner resonances. complex HMETau2ThreeMesons::T(double m0, double m1, double s, vector &M, vector &G, vector &W) { complex num(0, 0); double den(0); for (unsigned int i = 0; i < M.size(); i++) { num += W[i] * pBreitWigner(m0, m1, s, M[i], G[i]); den += W[i]; } return num / den; } //-------------------------------------------------------------------------- // Return summed weighted fixed width Breit-Wigner resonances. complex HMETau2ThreeMesons::T(double s, vector &M, vector &G, vector &W) { complex num(0, 0); double den(0); for (unsigned int i = 0; i < M.size(); i++) { num += W[i] * breitWigner(s, M[i], G[i]); den += W[i]; } return num / den; } //========================================================================== // Tau decay matrix element for tau decay into three pions. This matrix element // is taken from the Herwig++ implementation based on the CLEO fits. // rhoM: on-shell masses for the rho resonances // rhoG: on-shell widths for the rho resonances // rhoPp: p-wave phase for the rho coupling to the a1 // rhoAp: p-wave amplitude for the rho coupling to the a1 // rhoPd: d-wave phase for the rho coupling to the a1 // rhoAd: d-wave amplitude for the rho coupling to the a1 // f0M: f0 on-shell mass // f0G: f0 on-shell width // f0P: phase for the coupling of the f0 to the a1 // f0A: amplitude for the coupling of the f0 to the a1 // f2M: f2 on-shell mass // f2G: f2 on-shell width // f2P: phase for the coupling of the f2 to the a1 // f2P: amplitude for the coupling of the f2 to the a1 // sigM: sigma on-shell mass // sigG: sigma on-shell width // sigP: phase for the coupling of the sigma to the a1 // sigA: amplitude for the coupling of the sigma to the a1 //-------------------------------------------------------------------------- // Initialize resonance constants for the helicity matrix element. void HMETau2ThreePions::initResonances() { // Three charged pion decay. if (mode == PimPimPip) DECAYWEIGHTMAX = 6000; // Two neutral and one charged pion decay. else DECAYWEIGHTMAX = 3000; // Clear the vectors from previous decays. rhoM.clear(); rhoG.clear(); rhoPp.clear(); rhoAp.clear(); rhoWp.clear(); rhoPd.clear(); rhoAd.clear(); rhoWd.clear(); // Rho parameters. rhoM.push_back(.7743); rhoM.push_back(1.370); rhoM.push_back(1.720); rhoG.push_back(.1491); rhoG.push_back(.386); rhoG.push_back(.250); rhoPp.push_back(0); rhoPp.push_back(3.11018); rhoPp.push_back(0); rhoAp.push_back(1); rhoAp.push_back(0.12); rhoAp.push_back(0); rhoPd.push_back(-0.471239); rhoPd.push_back(1.66504); rhoPd.push_back(0); rhoAd.push_back(3.7e-07); rhoAd.push_back(8.7e-07); rhoAd.push_back(0); // Scalar and tensor parameters. f0M = 1.186; f2M = 1.275; sigM = 0.860; f0G = 0.350; f2G = 0.185; sigG = 0.880; f0P = -1.69646; f2P = 1.75929; sigP = 0.722566; f0A = 0.77; f2A = 7.1e-07; sigA = 2.1; // Calculate the weights from the phases and amplitudes. calculateResonanceWeights(rhoPp, rhoAp, rhoWp); calculateResonanceWeights(rhoPd, rhoAd, rhoWd); f0W = f0A * (cos(f0P) + complex(0,1) * sin(f0P)); f2W = f2A * (cos(f2P) + complex(0,1) * sin(f2P)); sigW = sigA * (cos(sigP) + complex(0,1) * sin(sigP)); } //-------------------------------------------------------------------------- // Return the first form factor. complex HMETau2ThreePions::F1() { complex answer(0,0); // Three charged pion decay. if (mode == PimPimPip) { for (unsigned int i = 0; i < rhoM.size(); i++) { answer += - rhoWp[i] * pBreitWigner(pM[3], pM[4], s2, rhoM[i], rhoG[i]) - rhoWd[i] / 3.0 * pBreitWigner(pM[2], pM[4], s3, rhoM[i], rhoG[i]) * (s2 - s4); } answer += -2.0 / 3.0 * (sigW * sBreitWigner(pM[2], pM[4], s3, sigM, sigG) + f0W * sBreitWigner(pM[2], pM[4], s3, f0M, f0G)); answer += f2W * (0.5 * (s4 - s3) * dBreitWigner(pM[3], pM[4], s2, f2M, f2G) - 1.0 / (18 * s3) * (4 * pow2(pM[2]) - s3) * (s1 + s3 - pow2(pM[2])) * dBreitWigner(pM[2], pM[4], s3, f2M, f2G)); } // Two neutral and one charged pion decay. else { for (unsigned int i = 0; i < rhoM.size(); i++) { answer += rhoWp[i] * pBreitWigner(pM[3], pM[4], s2, rhoM[i], rhoG[i]) - rhoWd[i] / 3.0 * pBreitWigner(pM[2], pM[4], s3, rhoM[i], rhoG[i]) * (s4 - s2 - pow2(pM[4]) + pow2(pM[2])); } answer += 2.0 / 3.0 * (sigW * sBreitWigner(pM[2], pM[3], s4, sigM, sigG) + f0W * sBreitWigner(pM[2], pM[3], s4, f0M, f0G)); answer += f2W / (18 * s4) * (s1 - pow2(pM[4]) + s4) * (4 * pow2(pM[2]) - s4) * dBreitWigner(pM[2], pM[3], s4, f2M, f2G); } return a1BW * answer; } //-------------------------------------------------------------------------- // Return the second form factor. complex HMETau2ThreePions::F2() { complex answer(0,0); // Three charged pion decay. if (mode == PimPimPip) { for (unsigned int i = 0; i < rhoM.size(); i++) { answer += -rhoWp[i] * pBreitWigner(pM[2], pM[4], s3, rhoM[i], rhoG[i]) - rhoWd[i] / 3.0 * pBreitWigner(pM[3], pM[4], s2, rhoM[i], rhoG[i]) * (s3 - s4); } answer += -2.0 / 3.0 * (sigW * sBreitWigner(pM[3], pM[4], s2, sigM, sigG) + f0W * sBreitWigner(pM[3], pM[4], s2, f0M, f0G)); answer += f2W * (0.5 * (s4 - s2) * dBreitWigner(pM[2], pM[4], s3, f2M, f2G) - 1.0 / (18 * s2) * (4 * pow2(pM[2]) - s2) * (s1 + s2 - pow2(pM[2])) * dBreitWigner(pM[3], pM[4], s2, f2M, f2G)); } // Two neutral and one charged pion decay. else { for (unsigned int i = 0; i < rhoM.size(); i++) { answer += -rhoWp[i] / 3.0 * pBreitWigner(pM[2], pM[4], s3, rhoM[i], rhoG[i]) - rhoWd[i] * pBreitWigner(pM[3], pM[4], s2, rhoM[i], rhoG[i]) * (s4 - s3 - pow2(pM[4]) + pow2(pM[3])); } answer += 2.0 / 3.0 * (sigW * sBreitWigner(pM[2], pM[3], s4, sigM, sigG) + f0W * sBreitWigner(pM[2], pM[3], s4, f0M, f0G)); answer += f2W / (18 * s4) * (s1 - pow2(pM[4]) + s4) * (4 * pow2(pM[2]) - s4) * dBreitWigner(pM[2], pM[3], s4, f2M, f2G); } return -a1BW * answer; } //-------------------------------------------------------------------------- // Return the third form factor. complex HMETau2ThreePions::F3() { complex answer(0,0); // Three charged pion decay. if (mode == PimPimPip) { for (unsigned int i = 0; i < rhoM.size(); i++) { answer += -rhoWd[i] * (1.0 / 3.0 * (s3 - s4) * pBreitWigner(pM[3], pM[4], s2, rhoM[i], rhoG[i]) - 1.0 / 3.0 * (s2 - s4) * pBreitWigner(pM[2], pM[4], s3, rhoM[i], rhoG[i])); } answer += -2.0 / 3.0 * (sigW * sBreitWigner(pM[3], pM[4], s2, sigM, sigG) + f0W * sBreitWigner(pM[3], pM[4], s2, f0M, f0G)); answer += 2.0 / 3.0 * (sigW * sBreitWigner(pM[2], pM[4], s3, sigM, sigG) + f0W * sBreitWigner(pM[2], pM[4], s3, f0M, f0G)); answer += f2W * (-1.0 / (18 * s2) * (4 * pow2(pM[2]) - s2) * (s1 + s2 - pow2(pM[2])) * dBreitWigner(pM[3], pM[4], s2, f2M, f2G) + 1.0 / (18 * s3) * (4 * pow2(pM[2]) - s3) * (s1 + s3 - pow2(pM[2])) * dBreitWigner(pM[2], pM[4], s3, f2M, f2G)); } // Two neutral and one charged pion decay. else { for (unsigned int i = 0; i < rhoM.size(); i++) { answer += rhoWd[i] * (-1.0 / 3.0 * (s4 - s3 - pow2(pM[4]) + pow2(pM[3])) * pBreitWigner(pM[3], pM[4], s2, rhoM[i], rhoG[i]) + 1.0 / 3.0 * (s4 - s2 - pow2(pM[4]) + pow2(pM[2])) * pBreitWigner(pM[2], pM[4], s3, rhoM[i], rhoG[i])); } answer += -f2W / 2.0 * (s2 - s3) * dBreitWigner(pM[2], pM[3], s4, f2M, f2G); } return a1BW * answer; } //-------------------------------------------------------------------------- // Return the running width for the a1 (multiplied by a factor of a1M). double HMETau2ThreePions::a1PhaseSpace(double s) { double picM = 0.1753; // (m_pi^- + m_pi^- + m_pi^+)^2 double pinM = 0.1676; // (m_pi^0 + m_pi^0 + m_pi^-)^2 double kM = 0.496; // K mass. double ksM = 0.894; // K^* mass. double picG = 0; // Width contribution from three charged pions. double pinG = 0; // Width contribution from two neutral one charged. double kG = 0; // Width contributions from s-wave K K^*. double piW = pow2(0.2384)/1.0252088; // Overall weight factor. double kW = pow2(4.7621); // K K^* width weight factor. // Three charged pion width contribution. if (s < picM) picG = 0; else if (s < 0.823) picG = 5.80900 * pow3(s - picM) * (1.0 - 3.00980 * (s - picM) + 4.5792 * pow2(s - picM)); else picG = -13.91400 + 27.67900 * s - 13.39300 * pow2(s) + 3.19240 * pow3(s) - 0.10487 * pow4(s); // Two neutral and one charged pion width contribution. if (s < pinM) pinG = 0; else if (s < 0.823) pinG = 6.28450 * pow3(s - pinM) * (1.0 - 2.95950 * (s - pinM) + 4.33550 * pow2(s - pinM)); else pinG = -15.41100 + 32.08800 * s - 17.66600 * pow2(s) + 4.93550 * pow3(s) - 0.37498 * pow4(s); // K and K^* width contribution. if (s > pow2(ksM + kM)) kG = 0.5 * sqrt((s - pow2(ksM + kM)) * (s - pow2(ksM - kM))) / s; return piW*(picG + pinG + kW*kG); } //-------------------------------------------------------------------------- // Return the Breit-Wigner for the a1. complex HMETau2ThreePions::a1BreitWigner(double s) { double a1M = 1.331; // Mass of the a1. return a1M*a1M/(a1M*a1M - s - complex(0,1)*a1PhaseSpace(s)); } //========================================================================== // Tau decay matrix element for tau decay into three mesons with kaons. // The form factors are taken from hep-ph/9503474. // rhoMa(v): on-shell masses for the axial (vector) rho resonances // rhoGa(v): widths for the axial (vector) rho resonances // rhoWa(v): weights for the axial (vector) rho resonances // kstarXa(v): on-shell masses, widths, and weights for the K* resonances // k1Xa(b): on-shell masses, width, and weight for the K1 resonances, // the a constants are for K1 -> K* pi, K* -> K pi // the b constants are for K1 -> rho K, rho -> pi pi // omegaX: on-shell masses, width, and weights for the omega reosnances // kM: kaon mass // piM: charged pion mass // piW: pion coupling, f_W //-------------------------------------------------------------------------- // Initialize resonance constants for the helicity matrix element. void HMETau2ThreeMesonsWithKaons::initResonances() { // K-, pi-, K+ decay. if (mode == PimKmKp) DECAYWEIGHTMAX = 130; // K0, pi-, Kbar0 decay. else if (mode == PimK0bK0) DECAYWEIGHTMAX = 115; // K_S0, pi-, K_S0 and K_L0, pi-, K_L0 decay. else if (mode == PimKsKs || mode == KlKlPim) DECAYWEIGHTMAX = 230; // K_S0, pi-, K_L0 decay. else if (mode == KlPimKs) DECAYWEIGHTMAX = 230; // K-, pi0, K0 decay. else if (mode == Pi0K0Km) DECAYWEIGHTMAX = 125; // pi0, pi0, K- decay. else if (mode == Pi0Pi0Km) DECAYWEIGHTMAX = 2.5e4; // K-, pi-, pi+ decay. else if (mode == PimPipKm) DECAYWEIGHTMAX = 1.8e4; // pi-, Kbar0, pi0 decay. else if (mode == Pi0PimK0b) DECAYWEIGHTMAX = 3.9e4; // Clear the vectors from previous decays. rhoMa.clear(); rhoGa.clear(); rhoWa.clear(); rhoMv.clear(); rhoGv.clear(); rhoWv.clear(); kstarMa.clear(); kstarGa.clear(); kstarWa.clear(); kstarMv.clear(); kstarGv.clear(); kstarWv.clear(); k1Ma.clear(); k1Ga.clear(); k1Wa.clear(); k1Mb.clear(); k1Gb.clear(); k1Wb.clear(); omegaM.clear(); omegaG.clear(); omegaW.clear(); // Rho parameters. rhoMa.push_back(0.773); rhoGa.push_back(0.145); rhoWa.push_back(1); rhoMa.push_back(1.370); rhoGa.push_back(0.510); rhoWa.push_back(-0.145); rhoMv.push_back(0.773); rhoGv.push_back(0.145); rhoWv.push_back(1); rhoMv.push_back(1.500); rhoGv.push_back(0.220); rhoWv.push_back(-6.5 / 26.0); rhoMv.push_back(1.750); rhoGv.push_back(0.120); rhoWv.push_back(-1.0 / 26.0); // Kstar parameters. kstarMa.push_back(0.892); kstarGa.push_back(0.050); kstarMa.push_back(1.412); kstarGa.push_back(0.227); kstarWa.push_back(1); kstarWa.push_back(-0.135); kstarMv.push_back(0.892); kstarGv.push_back(0.050); kstarMv.push_back(1.412); kstarGv.push_back(0.227); kstarMv.push_back(1.714); kstarGv.push_back(0.323); kstarWv.push_back(1); kstarWv.push_back(-6.5 / 26.0); kstarWv.push_back(-1.0 / 26.0); // K1 parameters. k1Ma.push_back(1.270); k1Ga.push_back(0.090); k1Wa.push_back(0.33); k1Ma.push_back(1.402); k1Ga.push_back(0.174); k1Wa.push_back(1); k1Mb.push_back(1.270); k1Gb.push_back(0.090); k1Wb.push_back(1); // Omega and phi parameters. omegaM.push_back(0.782); omegaG.push_back(0.00843); omegaW.push_back(1); omegaM.push_back(1.020); omegaG.push_back(0.00443); omegaW.push_back(0.05); // Kaon and pion parameters kM = 0.49765; piM = 0.13957; piW = 0.0942; } //-------------------------------------------------------------------------- // Return the first form factor. complex HMETau2ThreeMesonsWithKaons::F1() { complex answer; // K-, pi-, K+ decay. if (mode == PimKmKp) answer = a1BW * T(piM, kM, s2, kstarMa, kstarGa, kstarWa) / 2.0; // K0, pi-, Kbar0 decay. else if (mode == PimK0bK0) answer = a1BW * T(piM, kM, s2, kstarMa, kstarGa, kstarWa) / 2.0; // K_S0, pi-, K_S0 decay and K_L0, pi-, K_L0 decay. else if (mode == PimKsKs || mode == KlKlPim) answer = -a1BW * (T(piM, kM, s2, kstarMa, kstarGa, kstarWa) + T(piM, kM, s4, kstarMa, kstarGa, kstarWa)) / 2.0; // K_S0, pi-, K_L0 decay. else if (mode == KlPimKs) answer = a1BW * (T(piM, kM, s2, kstarMa, kstarGa, kstarWa) - T(piM, kM, s4, kstarMa, kstarGa, kstarWa)) / 2.0; // K-, pi0, K0 decay. else if (mode == Pi0K0Km) answer = a1BW * (T(piM, kM, s2, kstarMa, kstarGa, kstarWa) - T(piM, kM, s4, kstarMa, kstarGa, kstarWa)) / 2.0; // pi0, pi0, K- decay. else if (mode == Pi0Pi0Km) answer = T(s1, k1Ma, k1Ga, k1Wa) * T(piM, kM, s2, kstarMa, kstarGa, kstarWa); // K-, pi-, pi+ decay. else if (mode == PimPipKm) answer = T(s1, k1Mb, k1Gb, k1Wb) * T(piM, piM, s2, rhoMa, rhoGa, rhoWa); // pi-, Kbar0, pi0 decay. else if (mode == Pi0PimK0b) answer = T(s1, k1Ma, k1Ga, k1Wa) * (T(piM, kM, s2, kstarMa, kstarGa, kstarWa) - T(piM, kM, s4, kstarMa, kstarGa, kstarWa)); return -1.0 / 3.0 * answer; } //-------------------------------------------------------------------------- // Return the second form factor. complex HMETau2ThreeMesonsWithKaons::F2() { complex answer; // K-, pi-, K+ decay. if (mode == PimKmKp) answer = a1BW * T(piM, piM, s3, rhoMa, rhoGa, rhoWa) / 2.0; // K0, pi-, Kbar0 decay. else if (mode == PimK0bK0) answer = a1BW * T(piM, piM, s3, rhoMa, rhoGa, rhoWa) / 2.0; // K_S0, pi-, K_S0 decay and K_L0, pi-, K_L0 decay. else if (mode == PimKsKs || mode == KlKlPim) answer = a1BW * T(piM, kM, s4, kstarMa, kstarGa, kstarWa) / 2.0; // K_S0, pi-, K_L0 decay. else if (mode == KlPimKs) answer = a1BW * (2.0 * T(piM, piM, s3, rhoMa, rhoGa, rhoWa) + T(piM, kM, s4, kstarMa, kstarGa, kstarWa)) / 2.0; // K-, pi0, K0 decay. else if (mode == Pi0K0Km) answer = a1BW * (2.0 * T(piM, piM, s3, rhoMa, rhoGa, rhoWa) + T(piM, kM, s4, kstarMa, kstarGa, kstarWa)) / 2.0; // pi0, pi0, K- decay. else if (mode == Pi0Pi0Km) answer = T(s1, k1Ma, k1Ga, k1Wa) * T(piM, kM, s3, kstarMa, kstarGa, kstarWa); // K-, pi-, pi+ decay. else if (mode == PimPipKm) answer = T(s1, k1Ma, k1Ga, k1Wa) * T(piM, kM, s3, kstarMa, kstarGa, kstarWa); // pi-, Kbar0, pi0 decay. else if (mode == Pi0PimK0b) answer = 2.0 * T(s1, k1Mb, k1Gb, k1Wb) * T(piM, piM, s3, rhoMa, rhoGa, rhoWa) + T(s1, k1Ma, k1Ga, k1Wa) * T(piM, kM, s4, kstarMa, kstarGa, kstarWa); return 1.0 / 3.0 * answer; } //-------------------------------------------------------------------------- // Return the fourth form factor. complex HMETau2ThreeMesonsWithKaons::F4() { complex answer; // K-, pi-, K+ decay. if (mode == PimKmKp) answer = (sqrt(2.) - 1) * T(piM, piM, s1, rhoMv, rhoGv, rhoWv) * (sqrt(2.) * T(s3, omegaM, omegaG, omegaW) + T(piM, kM, s2, kstarMa, kstarGa, kstarWa)); // K0, pi-, Kbar0 decay. else if (mode == PimK0bK0) answer = -(sqrt(2.) - 1) * T(piM, piM, s1, rhoMv, rhoGv, rhoWv) * (sqrt(2.) * T(s3, omegaM, omegaG, omegaW) + T(piM, kM, s2, kstarMa, kstarGa, kstarWa)); // K_S0, pi-, K_S0 decay and K_L0, pi-, K_L0 decay. else if (mode == PimKsKs || mode == KlKlPim) answer = (sqrt(2.) - 1) * T(piM, piM, s1, rhoMv, rhoGv, rhoWv) * (T(piM, kM, s2, kstarMa, kstarGa, kstarWa) - T(piM, kM, s4, kstarMa, kstarGa, kstarWa)); // K_S0, pi-, K_L0 decay. else if (mode == KlPimKs) answer = -(sqrt(2.) - 1) * T(piM, piM, s1, rhoMv, rhoGv, rhoWv) * (2 * sqrt(2.) * T(s3, omegaM, omegaG, omegaW) + T(piM, kM, s2, kstarMa, kstarGa, kstarWa) + T(piM, kM, s4, kstarMa, kstarGa, kstarWa)); // K-, pi0, K0 decay. else if (mode == Pi0K0Km) answer = -(sqrt(2.) - 1) * T(piM, piM, s1, rhoMv, rhoGv, rhoWv) * (T(piM, kM, s4, kstarMa, kstarGa, kstarWa) - T(piM, kM, s2, kstarMa, kstarGa, kstarWa)); // pi0, pi0, K- decay. else if (mode == Pi0Pi0Km) answer = T(piM, kM, s1, kstarMv, kstarGv, kstarWv) * (T(piM, kM, s2, kstarMa, kstarGa, kstarWa) - T(piM, kM, s3, kstarMa, kstarGa, kstarWa)); // K-, pi-, pi+ decay. else if (mode == PimPipKm) answer = -T(piM, kM, s1, kstarMv, kstarGv, kstarWv) * (T(piM, piM, s2, rhoMa, rhoGa, rhoWa) + T(piM, kM, s3, kstarMa, kstarGa, kstarWa)); // pi-, Kbar0, pi0 decay. else if (mode == Pi0PimK0b) answer = T(piM, kM, s1, kstarMv, kstarGv, kstarWv) * (2.0 * T(piM, piM, s3, rhoMa, rhoGa, rhoWa) + T(piM, kM, s2, kstarMa, kstarGa, kstarWa) + T(piM, kM, s4, kstarMa, kstarGa, kstarWa)); return 1.0 / (8.0 * M_PI * M_PI * piW * piW) * answer; } //========================================================================== // Tau decay matrix element for tau decay into three mesons. The form // factors are taken from Comp. Phys. Com. 76 (1993) 361-380. // rhoMa(v): on-shell masses for the axial (vector) rho resonances // rhoGa(v): widths for the axial (vector) rho resonances // rhoWa(v): weights for the axial (vector) rho resonances // kstarX: on-shell masses, widths, and weights for the K* resonances // k1X: on-shell masses, width, and weight for the K1 resonances // kM: kaon mass // piM: charged pion mass // piW: pion coupling, f_W //-------------------------------------------------------------------------- // Initialize resonances for the helicity matrix element. void HMETau2ThreeMesonsGeneric::initResonances() { // pi-, pi-, pi+ decay and pi0, pi0, pi- decay. if (mode == PimPimPip || mode == Pi0Pi0Pim) DECAYWEIGHTMAX = 1.3e4; // K-, pi-, K+ decay. else if (mode == PimKmKp) DECAYWEIGHTMAX = 330; // K0, pi-, Kbar0 decay. else if (mode == PimK0bK0) DECAYWEIGHTMAX = 300; // K-, pi0, K0 decay. else if (mode == Pi0K0Km) DECAYWEIGHTMAX = 40; // pi0, pi0, K- decay. else if (mode == Pi0Pi0Km) DECAYWEIGHTMAX = 9.4e4; // K-, pi-, pi+ decay. else if (mode == PimPipKm) DECAYWEIGHTMAX = 9.0e3; // pi-, Kbar0, pi0 decay. else if (mode == Pi0PimK0b) DECAYWEIGHTMAX = 1.2e4; // pi-, pi0, eta decay. else if (mode == Pi0PimEta) DECAYWEIGHTMAX = 360; // Clear the vectors from previous decays. rhoMa.clear(); rhoGa.clear(); rhoWa.clear(); rhoMv.clear(); rhoGv.clear(); rhoWv.clear(); kstarM.clear(); kstarG.clear(); kstarW.clear(); k1M.clear(); k1G.clear(); k1W.clear(); // Rho parameters. rhoMa.push_back(0.773); rhoGa.push_back(0.145); rhoWa.push_back(1); rhoMa.push_back(1.370); rhoGa.push_back(0.510); rhoWa.push_back(-0.145); rhoMv.push_back(0.773); rhoGv.push_back(0.145); rhoWv.push_back(-26); rhoMv.push_back(1.5); rhoGv.push_back(0.220); rhoWv.push_back(6.5); rhoMv.push_back(1.75); rhoGv.push_back(0.120); rhoWv.push_back(1); // Kaon parameters. kstarM.push_back(0.892); kstarG.push_back(0.0513); kstarW.push_back(1); k1M.push_back(1.402); k1G.push_back(0.174); k1W.push_back(1); // Kaon and pion parameters kM = 0.49765; piM = 0.13957; piW = 0.0942; } //-------------------------------------------------------------------------- // Return the first form factor. complex HMETau2ThreeMesonsGeneric::F1() { complex answer; // pi-, pi-, pi+ decay and pi0, pi0, pi- decay. if (mode == PimPimPip || mode == Pi0Pi0Pim) answer = a1BW * T(piM, piM, s2, rhoMa, rhoGa, rhoWa); // K-, pi-, K+ decay. else if (mode == PimKmKp) answer = -a1BW * T(piM, kM, s2, kstarM, kstarG, kstarW) / 3.0; // K0, pi-, Kbar0 decay. else if (mode == PimK0bK0) answer = -a1BW * T(piM, kM, s2, kstarM, kstarG, kstarW) / 3.0; // K-, pi0, K0 decay. else if (mode == Pi0K0Km) answer = 0; // pi0, pi0, K- decay. else if (mode == Pi0Pi0Km) answer = T(s1, k1M, k1G, k1W) * T(piM, kM, s2, kstarM, kstarG, kstarW); // K-, pi-, pi+ decay. else if (mode == PimPipKm) answer = -T(s1, k1M, k1G, k1W) * T(piM, piM, s2, rhoMa, rhoGa, rhoWa) / 3.0; // pi-, Kbar0, pi0 decay. else if (mode == Pi0PimK0b) answer = 0; // pi-, pi0, eta decay. else if (mode == Pi0PimEta) answer = 0; return answer; } //-------------------------------------------------------------------------- // Return the second form factor. complex HMETau2ThreeMesonsGeneric::F2() { complex answer; // pi-, pi-, pi+ decay and pi0, pi0, pi- decay. if (mode == PimPimPip || mode == Pi0Pi0Pim) answer = -a1BW * T(piM, piM, s3, rhoMa, rhoGa, rhoWa); // K-, pi-, K+ decay. else if (mode == PimKmKp) answer = a1BW * T(piM, piM, s3, rhoMa, rhoGa, rhoWa) / 3.0; // K0, pi-, Kbar0 decay. else if (mode == PimK0bK0) answer = a1BW * T(piM, piM, s3, rhoMa, rhoGa, rhoWa) / 3.0; // K-, pi0, K0 decay. else if (mode == Pi0K0Km) answer = a1BW * T(piM, piM, s3, rhoMa, rhoGa, rhoWa); // pi0, pi0, K- decay. else if (mode == Pi0Pi0Km) answer = -T(s1, k1M, k1G, k1W) * T(piM, kM, s3, kstarM, kstarG, kstarW); // K-, pi-, pi+ decay. else if (mode == PimPipKm) answer = T(s1, k1M, k1G, k1W) * T(piM, kM, s3, kstarM, kstarG, kstarW) / 3.0; // pi-, Kbar0, pi0 decay. else if (mode == Pi0PimK0b) answer = T(s1, k1M, k1G, k1W) * T(piM, piM, s3, rhoMa, rhoGa, rhoWa); // pi-, pi0, eta decay. else if (mode == Pi0PimEta) answer = 0; return answer; } //-------------------------------------------------------------------------- // Return the fourth form factor. complex HMETau2ThreeMesonsGeneric::F4() { complex answer; // pi-, pi-, pi+ decay and pi0, pi0, pi- decay. if (mode == PimPimPip || mode == Pi0Pi0Pim) answer = 0; // K-, pi-, K+ decay. else if (mode == PimKmKp) answer = T(piM, piM, s1, rhoMv, rhoGv, rhoWv) * (T(piM, piM, s3, rhoMa, rhoGa, rhoWa) - 0.2 * T(piM, kM, s2, kstarM, kstarG, kstarW)) * (1.25); // K0, pi-, Kbar0 decay. else if (mode == PimK0bK0) answer = -T(piM, piM, s1, rhoMv, rhoGv, rhoWv) * (T(piM, piM, s3, rhoMa, rhoGa, rhoWa) - 0.2 * T(piM, kM, s2, kstarM, kstarG, kstarW)) * (1.25); // K-, pi0, K0 decay. else if (mode == Pi0K0Km) answer = 0; // pi0, pi0, K- decay. else if (mode == Pi0Pi0Km) answer = 0; // K-, pi-, pi+ decay. else if (mode == PimPipKm) answer = -T(piM, kM, s1, kstarM, kstarG, kstarW) * (T(piM, piM, s2, rhoMa, rhoGa, rhoWa) - 0.2 * T(piM, kM, s3, kstarM, kstarG, kstarW)) * (1.25); // pi-, Kbar0, pi0 decay. else if (mode == Pi0PimK0b) answer = 2.0 * T(piM, kM, s1, kstarM, kstarG, kstarW) * (T(piM, piM, s3, rhoMa, rhoGa, rhoWa) - 0.2 * T(piM, kM, s2, kstarM, kstarG, kstarW)) * (1.25); // pi-, pi0, eta decay. else if (mode == Pi0PimEta) answer = T(piM, piM, s1, rhoMv, rhoGv, rhoWv) * T(piM, piM, s4, rhoMa, rhoGa, rhoWa); return 1.0 / (4.0 * M_PI * M_PI * piW * piW) * answer; } //========================================================================== // Tau decay matrix element for tau decay into two pions with a photons taken // from Comp. Phys. Com. 76 (1993) 361-380. Because a photon is in the final // state the matrix element is reimplented to handle the two spin states. // F(s, M, G, W): form factor for resonance // rhoM: on-shell mass of the rho resonances // rhoG: width of the rho resonances // rhoW: weight of the rho resonances // omegaX: on-shell mass, width, and weight of the omega resonances // piM: charged pion mass //-------------------------------------------------------------------------- // Initialize constants for the helicity matrix element. void HMETau2TwoPionsGamma::initConstants() { DECAYWEIGHTMAX = 4e4; // Clear the vectors from previous decays. rhoM.clear(); rhoG.clear(); rhoW.clear(); omegaM.clear(); omegaG.clear(); omegaW.clear(); // Set parameters. rhoM.push_back(0.773); rhoG.push_back(0.145); rhoW.push_back(1); rhoM.push_back(1.7); rhoG.push_back(0.26); rhoW.push_back(-0.1); omegaM.push_back(0.782); omegaG.push_back(0.0085); omegaW.push_back(1); piM = 0.13957; } //-------------------------------------------------------------------------- // Initialize wave functions for the helicity matrix element. void HMETau2TwoPionsGamma::initWaves(vector& p) { // Calculate the hadronic current. u.clear(); pMap.resize(p.size()); setFermionLine(0, p[0], p[1]); // Calculate the hadronic current. vector< Wave4 > u2; Wave4 q(p[2].p() + p[3].p() + p[4].p()); Wave4 q2(p[2].p()), q3(p[3].p()), q4(p[4].p()); double s1 = m2(q); double s2 = m2(q3 + q2); complex f = F(s1, rhoM, rhoG, rhoW) * F(0, rhoM, rhoG, rhoW) * F(s2, omegaM, omegaG, omegaW); double q4q2 = m2(q4, q2); double q4q3 = m2(q4, q3); double q3q2 = m2(q3, q2); for (int h = 0; h < 2; h++) { Wave4 e = p[2].wave(h); complex q4e = q4*gamma[4]*e; complex q3e = q3*gamma[4]*e; u2.push_back(f * (e * (piM*piM*q4q2 - q3q2*(q4q3 - q4q2)) - q3 * (q3e*q4q2 - q4e*q3q2) + q2 * (q3e*q4q3 - q4e*(piM*piM + q3q2)))); } u.push_back(u2); } //-------------------------------------------------------------------------- // Return element for the helicity matrix element. complex HMETau2TwoPionsGamma::calculateME(vector h) { complex answer(0,0); for (int mu = 0; mu <= 3; mu++) { answer += (u[1][h[pMap[1]]] * gamma[mu] * (1 - gamma[5]) * u[0][h[pMap[0]]]) * gamma[4](mu,mu) * u[2][h[2]](mu); } return answer; } //-------------------------------------------------------------------------- // Return the form factor. complex HMETau2TwoPionsGamma::F(double s, vector M, vector G, vector W) { complex answer(0, 0); for (unsigned int i = 0; i < M.size(); i++) answer += W[i] / (M[i]*M[i] - s - complex(0, 1) * M[i] * G[i]); return answer; } //========================================================================== // Tau decay matrix element for tau decay into pions using the Novosibirsk // model of Comp. Phys. Com. 174 (2006) 818-835. // G(i,s): G-factor for index 1, 2, or 3 // tX(q,q1,q2,q3,q4): combined resonance current // a1D(s): a1 Breit-Wigner denominator // rhoD(s): rho Breit-Wigner denominator // sigD(s): sigma Breit-Wigner denominator // omeD(s): omega Breit-Wigner denominator // a1FormFactor(s): form factor for the a1 resonance // rhoFormFactor1(2)(s): form factor for the rho resonance // omeFormFactor(s): form factor for the omega resonance // sigM: on-shell mass of the sigma resonance // sigG: width of the sigma resonance // sigA: amplitude of the sigma resonance // sigP: phase of the sigma resonance // sigW: weight of the sigma resonance (from amplitude and weight) // omeX: mass, width, amplitude, phase, and weight of the omega resonance // a1X: mass and width of the a1 resonance // rhoX: mass and width of the rho resonance // picM: charge pion mass // pinM: neutral pion mass // lambda2: a1 form factor cut-off //-------------------------------------------------------------------------- // Initialize constants for the helicity matrix element. void HMETau2FourPions::initConstants() { if (abs(pID[3]) == 111) DECAYWEIGHTMAX = 5e8; else DECAYWEIGHTMAX = 5e9; pinM = particleDataPtr->m0(111); picM = particleDataPtr->m0(211); sigM = 0.8; omeM = 0.782; a1M = 1.23; rhoM = 0.7761; sigG = 0.8; omeG = 0.00841; a1G = 0.45; rhoG = 0.1445; sigP = 0.43585; omeP = 0.0; sigA = 1.39987; omeA = 1.0; sigW = sigA*(cos(sigP)+complex(0,1)*sin(sigP)); omeW = omeA*(cos(omeP)+complex(0,1)*sin(omeP)); lambda2 = 1.2; } //-------------------------------------------------------------------------- // Initialize the hadronic current for the helicity matrix element. void HMETau2FourPions::initHadronicCurrent(vector& p) { vector< Wave4 > u2; // Create pion momenta. Wave4 q(p[2].p() + p[3].p() + p[4].p()+ p[5].p()); Wave4 q2(p[2].p()), q3(p[3].p()), q4(p[4].p()), q5(p[5].p()); // Calculate the four pion system energy. double s = m2(q); // Create the hadronic current for the 3 neutral pion channel. if (abs(pID[3]) == 111) u2.push_back(G(1,s)*(t1(q,q3,q4,q5,q2) + t1(q,q3,q2,q5,q4) + t1(q,q4,q3,q5,q2) + t1(q,q4,q2,q5,q3) + t1(q,q2,q3,q5,q4) + t1(q,q2,q4,q5,q3) + t2(q,q3,q5,q4,q2) + t2(q,q4,q5,q3,q2) + t2(q,q2,q5,q4,q3) - t2(q,q5,q3,q4,q2) - t2(q,q5,q4,q3,q2) - t2(q,q5,q2,q4,q3))); // Create the hadronic current for the 3 charged pion channel. else if (abs(pID[3]) == 211) u2.push_back(G(2,s)*(t1(q,q3,q5,q4,q2) + t1(q,q4,q5,q3,q2) + t1(q,q3,q4,q5,q2) + t1(q,q4,q3,q5,q2) + t1(q,q2,q4,q3,q5) + t1(q,q2,q3,q4,q5) + t2(q,q2,q4,q3,q5) + t2(q,q2,q3,q4,q5) - t2(q,q3,q2,q4,q5) - t2(q,q4,q2,q3,q5)) + G(3,s)*(t3(q,q3,q5,q4,q2) + t3(q,q4,q5,q3,q2) - t3(q,q3,q4,q5,q2) - t3(q,q4,q3,q5,q2) - t3(q,q3,q2,q4,q5) - t3(q,q4,q2,q3,q5))); u.push_back(u2); } //-------------------------------------------------------------------------- // Return the first t-vector. Wave4 HMETau2FourPions::t1(Wave4 &q, Wave4 &q1, Wave4 &q2, Wave4 &q3, Wave4 &q4) { Wave4 a1Q(q2 + q3 + q4); Wave4 rhoQ(q3 + q4); double a1S = m2(a1Q); double rhoS = m2(rhoQ); // Needed to match Herwig++. double gM = sqrtpos(rhoM*rhoM - 4*picM*picM) * (rhoM*rhoM - 4*picM*picM) / rhoM; double dm = (rhoFormFactor1(0) - rhoFormFactor1(rhoM*rhoM) + rhoM*rhoM * rhoFormFactor2(rhoM*rhoM)) / gM; return - a1FormFactor(a1S) / (a1D(a1S) * rhoD(rhoS)) * pow2(a1M) * (rhoM*rhoM + rhoM*rhoG*dm) * (m2(q,a1Q) * (m2(q3,a1Q) * q4 - m2(q4,a1Q) * q3) + (m2(q,q4) * m2(q1,q3) - m2(q,q3) * m2(q1,q4)) * a1Q); } //-------------------------------------------------------------------------- // Return the second t-vector. Wave4 HMETau2FourPions::t2(Wave4 &q, Wave4 &/*q1*/, Wave4 &q2, Wave4 &q3, Wave4 &q4) { Wave4 a1Q(q2 + q3 + q4); Wave4 sigQ(q3 + q4); double a1S = m2(a1Q); double sigS = m2(sigQ); return sigW * a1FormFactor(a1S) / (a1D(a1S) * sigD(sigS)) * pow2(a1M) * pow2(sigM) * (m2(q,a1Q) * a1S * q2 - m2(q,q2) * a1S * a1Q); } //-------------------------------------------------------------------------- // Return the third t-vector. Wave4 HMETau2FourPions::t3(Wave4 &q, Wave4 &q1, Wave4 &q2, Wave4 &q3, Wave4 &q4) { Wave4 omeQ(q2 + q3 + q4); Wave4 rhoQ(q3 + q4); double omeS = m2(omeQ); double rhoS = m2(rhoQ); // Needed to match Herwig++. double gM = sqrtpos(rhoM*rhoM - 4*picM*picM) * (rhoM*rhoM - 4*picM*picM) / rhoM; double dm = (rhoFormFactor1(0) - rhoFormFactor1(rhoM*rhoM) + rhoM*rhoM * rhoFormFactor2(rhoM*rhoM)) / gM; return omeW * omeFormFactor(omeS) / (omeD(omeS) * rhoD(rhoS)) * pow2(omeM) * (rhoM*rhoM + rhoM*rhoG*dm) * ((m2(q,q3) * m2(q1,q4) - m2(q,q4) * m2(q1,q3)) * q2 + (m2(q,q4) * m2(q1,q2) - m2(q,q2) * m2(q1,q4)) * q3 + (m2(q,q2) * m2(q1,q3) - m2(q,q3) * m2(q1,q2)) * q4); } //-------------------------------------------------------------------------- // Return the D function for the a1(1260). complex HMETau2FourPions::a1D(double s) { // rG is defined as the running width. double rG = 0; // The rho and pion cut off thresholds defined in the fit. double piM = 0.16960; double rM = 0.83425; // Fit of width below three pion mass threshold. if (s < piM) rG = 0; // Fit of width below pion and rho mass threshold. else if (s < rM) rG = 0.003052*pow3(s - piM)*(1.0 + 151.088*(s - piM) + 174.495*pow2(s - piM)); // Fit of width above pion and rho mass threshold. else rG = 2.60817 - 2.47790*s + 0.66539*pow2(s) - 0.0678183*pow3(s) + 1.66577*(s-1.23701)/s; return s - a1M*a1M + complex(0,1) * sqrtpos(s) * rG; } //-------------------------------------------------------------------------- // Return the D function for the rho(770). complex HMETau2FourPions::rhoD(double s) { double gQ = sqrtpos(s - 4*picM*picM) * (s - 4*picM*picM) / sqrtpos(s); double gM = sqrtpos(rhoM*rhoM - 4*picM*picM) * (rhoM*rhoM - 4*picM*picM) / rhoM; double dm = (rhoFormFactor1(s) - rhoFormFactor1(rhoM*rhoM) - (s - rhoM*rhoM) * rhoFormFactor2(rhoM*rhoM)) / gM; // Ensure complex part is zero below available channel. if (s < 4*picM*picM) gQ = 0; return s - rhoM*rhoM - rhoM*rhoG*dm + complex(0,1)*rhoM*rhoG*(gQ/gM); } //-------------------------------------------------------------------------- // Return the D function for the sigma(800) (just s-wave running width). complex HMETau2FourPions::sigD(double s) { // Sigma decay to two neutral pions for three neutral pion channel. double piM = abs(pID[3]) == 111 ? pinM : picM; double gQ = sqrtpos(1.0 - 4*piM*piM/s); double gM = sqrtpos(1.0 - 4*piM*piM/(sigM*sigM)); return s - sigM*sigM + complex(0,1)*sigM*sigG*gQ/gM; } //-------------------------------------------------------------------------- // Return the D function for the omega(782). complex HMETau2FourPions::omeD(double s) { double g = 0; double q = sqrtpos(s); double x = q - omeM; // Fit of width given in TAUOLA. if (s < 1) g = 1 + 17.560*x + 141.110*pow2(x) + 894.884*pow3(x) + 4977.35*pow4(x) + 7610.66*pow5(x) - 42524.4*pow6(x); else g = -1333.26 + 4860*q - 6000.81*pow2(q) + 2504.97*pow3(q); if (g < 0) g = 0; return s - omeM*omeM + complex(0,1)*omeM*omeG*g; } //-------------------------------------------------------------------------- // Return the form factor for the a1. double HMETau2FourPions::a1FormFactor(double s) { return pow2((1.0 + a1M*a1M/lambda2) / (1.0 + s/lambda2)); } //-------------------------------------------------------------------------- // Return the form factor for the rho(770) (equivalent to h(s) in TAUOLA). double HMETau2FourPions::rhoFormFactor1(double s) { double f = 0.; if (s > 4. * picM * picM) { double thr = sqrtpos(1 - 4. * picM * picM / s); f = thr * log((1. + thr) / (1. - thr)) * (s - 4. * picM * picM) / M_PI; } else if (s < 0.0000001) f = -8. * picM * picM / M_PI; return f; } //-------------------------------------------------------------------------- // Return the form factor for the rho(770) (equivalent to h(s) derivative). double HMETau2FourPions::rhoFormFactor2(double s) { double f = sqrtpos(1 - 4*picM*picM/s); if (s > 4*picM*picM) f = f / (M_PI * s) * (s*f + (2*picM*picM + s)*log((1 + f) / (1 - f))); else f = 0; return f; } //-------------------------------------------------------------------------- // Return the form factor for the omega(782). double HMETau2FourPions::omeFormFactor(double /*s*/) { return 1.0; } //-------------------------------------------------------------------------- // Return the G-functions given in TAUOLA using a piece-wise fit. double HMETau2FourPions::G(int i, double s) { // Break points for the fits. double s0(0), s1(0), s2(0), s3(0), s4(0), s5(0); // Parameters for the fits. double a1(0), b1(0); double a2(0), b2(0), c2(0), d2(0), e2(0); double a3(0), b3(0), c3(0), d3(0), e3(0); double a4(0), b4(0); double a5(0), b5(0); // Three neutral pion parameters. if (i == 1) { s0 = 0.614403; s1 = 0.656264; s2 = 1.57896; s3 = 3.08198; s4 = 3.12825; s5 = 3.17488; a1 = -23383.7; b1 = 38059.2; a2 = 230.368; b2 = -4.39368; c2 = 687.002; d2 = -732.581; e2 = 207.087; a3 = 1633.92; b3 = -2596.21; c3 = 1703.08; d3 = -501.407; e3 = 54.5919; a4 = -2982.44; b4 = 986.009; a5 = 6948.99; b5 = -2188.74; } // Three charged pion parameters. else if (i == 2) { s0 = 0.614403; s1 = 0.635161; s2 = 2.30794; s3 = 3.08198; s4 = 3.12825; s5 = 3.17488; a1 = -54171.5; b1 = 88169.3; a2 = 454.638; b2 = -3.07152; c2 = -48.7086; d2 = 81.9702; e2 = -24.0564; a3 = -162.421; b3 = 308.977; c3 = -27.7887; d3 = -48.5957; e3 = 10.6168; a4 = -2650.29; b4 = 879.776; a5 = 6936.99; b5 = -2184.97; } // Omega mediated three charged pion parameters. else if (i == 3) { s0 = 0.81364; s1 = 0.861709; s2 = 1.92621; s3 = 3.08198; s4 = 3.12825; s5 = 3.17488; a1 = -84888.9; b1 = 104332; a2 = 2698.15; b2 = -3.08302; c2 = 1936.11; d2 = -1254.59; e2 = 201.291; a3 = 7171.65; b3 = -6387.9; c3 = 3056.27; d3 = -888.63; e3 = 108.632; a4 = -5607.48; b4 = 1917.27; a5 = 26573; b5 = -8369.76; } // Return the appropriate fit. if (s < s0) return 0.0; else if (s < s1) return a1 + b1*s; else if (s < s2) return a2*pow(s,b2) + c2*pow2(s) + d2*pow3(s) + e2*pow4(s); else if (s < s3) return a3 + b3*s + c3*pow2(s) + d3*pow3(s) + e3*pow4(s); else if (s < s4) return a4 + b4*s; else if (s < s5) return a5 + b5*s; else return 0.0; } //========================================================================== // Tau decay matrix element for tau decay into five pions using the model given // in hep-ph/0602162v1. // Ja(q,q1,q2,q3,q4,q5): current through rho and omega resonances // Jb(q,q1,q2,q3,q4,q5): current through a1 and sigma resonances // breitWigner(s,M,G): s-wave Breit-Wigner assuming massless products // a1M: on-shell mass of the a1 resonance // a1G: width of the a1 resonance // rhoX: mass and width of the rho resonance // omegaX: mass, width, and weight of the omega resonance // sigmaX: mass, width, and weight of the sigma resonance //-------------------------------------------------------------------------- // Initialize constants for the helicity matrix element. void HMETau2FivePions::initConstants() { // pi-, pi-, pi+, pi+, pi- decay. if (abs(pID[2]) == 211 && abs(pID[3]) == 211 && abs(pID[4]) == 211 && abs(pID[5]) == 211 && abs(pID[6]) == 211) DECAYWEIGHTMAX = 4e4; // pi+, pi-, pi0, pi-, pi0 decay. else if (abs(pID[2]) == 111 && abs(pID[3]) == 111 && abs(pID[4]) == 211 && abs(pID[5]) == 211 && abs(pID[6]) == 211) DECAYWEIGHTMAX = 1e7; // pi0, pi0, pi-, pi0, pi0 decay. else if (abs(pID[2]) == 111 && abs(pID[3]) == 111 && abs(pID[4]) == 111 && abs(pID[5]) == 111 && abs(pID[6]) == 211) DECAYWEIGHTMAX = 1e5; // Set resonances. a1M = 1.260; a1G = 0.400; rhoM = 0.776; rhoG = 0.150; omegaM = 0.782; omegaG = 0.0085; omegaW = 11.5; sigmaM = 0.800; sigmaG = 0.600; sigmaW = 1; } //-------------------------------------------------------------------------- // Initialize the hadronic current for the helicity matrix element. void HMETau2FivePions::initHadronicCurrent(vector& p) { vector< Wave4 > u2; Wave4 q(p[2].p() + p[3].p() + p[4].p() + p[5].p() + p[6].p()); Wave4 q2(p[2].p()), q3(p[3].p()), q4(p[4].p()), q5(p[5].p()), q6(p[6].p()); // pi-, pi-, pi+, pi+, pi- decay. if (abs(pID[2]) == 211 && abs(pID[3]) == 211 && abs(pID[4]) == 211 && abs(pID[5]) == 211 && abs(pID[6]) == 211) u2.push_back(Jb(q, q2, q3, q5, q6, q4) + Jb(q, q4, q3, q5, q6, q2) + Jb(q, q2, q4, q5, q6, q3) + Jb(q, q2, q3, q6, q5, q4) + Jb(q, q4, q3, q6, q5, q2) + Jb(q, q2, q4, q6, q5, q3)); // pi+, pi-, pi0, pi-, pi0 decay. else if (abs(pID[2]) == 111 && abs(pID[3]) == 111 && abs(pID[4]) == 211 && abs(pID[5]) == 211 && abs(pID[6]) == 211) u2.push_back(Ja(q, q6, q4, q2, q5, q3) + Ja(q, q6, q5, q2, q4, q3) + Ja(q, q6, q4, q3, q5, q2) + Ja(q, q6, q5, q3, q4, q2) + Jb(q, q4, q5, q6, q2, q3) + Jb(q, q2, q3, q4, q6, q5) + Jb(q, q2, q3, q5, q6, q4)); // pi0, pi0, pi-, pi0, pi0 decay. else if (abs(pID[2]) == 111 && abs(pID[3]) == 111 && abs(pID[4]) == 111 && abs(pID[5]) == 111 && abs(pID[6]) == 211) u2.push_back(Jb(q, q2, q3, q6, q4, q5) + Jb(q, q5, q3, q6, q4, q2) + Jb(q, q3, q4, q6, q2, q5) + Jb(q, q2, q4, q6, q3, q5) + Jb(q, q2, q5, q6, q4, q3) + Jb(q, q4, q5, q6, q2, q3)); u.push_back(u2); } //-------------------------------------------------------------------------- // Return the omega-rho hadronic current. Wave4 HMETau2FivePions::Ja(Wave4 &q, Wave4 &q1, Wave4 &q2, Wave4 &q3, Wave4 &q4, Wave4 &q5) { Wave4 j = epsilon(q1, q2, q3); return omegaW * (breitWigner(m2(q), a1M, a1G) * breitWigner(m2(q1 + q2 + q3), omegaM, omegaG) * breitWigner(m2(q4 + q5), rhoM, rhoG) * epsilon(q4 - q5, j, q) * (breitWigner(m2(q2 + q3), rhoM, rhoG) + breitWigner(m2(q1 + q3), rhoM, rhoG) + breitWigner(m2(q1 + q2), rhoM, rhoG))); } //-------------------------------------------------------------------------- // Return the a1-sigma hadronic current. Wave4 HMETau2FivePions::Jb(Wave4 &q, Wave4 &q1, Wave4 &q2, Wave4 &q3, Wave4 &q4, Wave4 &q5) { double s = m2(q); Wave4 a1Q = q1 + q2 + q3; double a1S = m2(a1Q); Wave4 j = (m2(q2, q1 - q3) / a1S * a1Q - q1 + q3) * breitWigner(m2(q1 + q3), rhoM, rhoG) + (m2(q1, q2 - q3) / a1S * a1Q - q2 + q3) * breitWigner(m2(q2 + q3), rhoM, rhoG); j = (j * gamma[4] * q / s) * q - j; return sigmaW * (breitWigner(s, a1M, a1G) * breitWigner(a1S, a1M, a1G) * breitWigner(m2(q4 + q5), sigmaM, sigmaG) * j); } complex HMETau2FivePions::breitWigner(double s, double M, double G) { return M * M / (M * M - s - complex(0, 1) * M * G); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/Settings.cc0000644000175000017500000020040512217346250015232 0ustar sunsun// Settings.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the Settings class. #include "Pythia8/Settings.h" // Allow string and character manipulation. #include namespace Pythia8 { //========================================================================== // Settings class. // This class contains flags, modes, parms and words used in generation. //-------------------------------------------------------------------------- // Read in database from specific file. bool Settings::init(string startFile, bool append, ostream& os) { // Don't initialize if it has already been done and not in append mode. if (isInit && !append) return true; int nError = 0; // List of files to be checked. Start with input file. vector files; files.push_back(startFile); // If nontrivial startfile path, then use that for other files as well. string pathName = ""; if (startFile.rfind("/") != string::npos) pathName = startFile.substr(0, startFile.rfind("/") + 1); // Loop over files. Open them for read. for (int i = 0; i < int(files.size()); ++i) { const char* cstring = files[i].c_str(); ifstream is(cstring); // Check that instream is OK. if (!is.good()) { os << "\n PYTHIA Error: settings file " << files[i] << " not found" << endl; return false; } // Read in one line at a time. string line; while ( getline(is, line) ) { // Get first word of a line, to interpret it as tag. istringstream getfirst(line); string tag; getfirst >> tag; // Skip ahead if not interesting. Only look for new files in startfile. if (tag != ". while (line.find(">") == string::npos) { string addLine; getline(is, addLine); line += " " + addLine; } // Remove extra blanks before an = sign. while (line.find(" =") != string::npos) line.erase( line.find(" ="), 1); // Add file also to be read. if (tag == " value = intVectorAttributeValue( line, "default="); int minVal = intAttributeValue( line, "min="); int maxVal = intAttributeValue( line, "max="); addMVec( name, value, hasMin, hasMax, minVal, maxVal); // Check for occurence of a double vector and add to pvec map. } else if (tag == " value = doubleVectorAttributeValue( line, "default="); double minVal = doubleAttributeValue( line, "min="); double maxVal = doubleAttributeValue( line, "max="); addPVec( name, value, hasMin, hasMax, minVal, maxVal); } // End of loop over lines in input file and loop over files. }; }; // Set up default e+e- and pp tunes, if positive. int eeTune = mode("Tune:ee"); if (eeTune > 0) initTuneEE( eeTune); int ppTune = mode("Tune:pp"); if (ppTune > 0) initTunePP( ppTune); // Done. if (nError > 0) return false; isInit = true; return true; } //-------------------------------------------------------------------------- // Overwrite existing database by reading from specific file. bool Settings::reInit(string startFile, ostream& os) { // Reset maps to empty. flags.clear(); modes.clear(); parms.clear(); words.clear(); mvecs.clear(); pvecs.clear(); // Then let normal init do the rest. isInit = false; return init(startFile, false, os); } //-------------------------------------------------------------------------- // Read in updates from a character string, like a line of a file. // Is used by readString (and readFile) in Pythia. bool Settings::readString(string line, bool warn, ostream& os) { // If empty line then done. if (line.find_first_not_of(" \n\t\v\b\r\f\a") == string::npos) return true; // If first character is not a letter, then taken to be a comment line. string lineNow = line; int firstChar = lineNow.find_first_not_of(" \n\t\v\b\r\f\a"); if (!isalpha(lineNow[firstChar])) return true; // Replace an equal sign by a blank to make parsing simpler. while (lineNow.find("=") != string::npos) { int firstEqual = lineNow.find_first_of("="); lineNow.replace(firstEqual, 1, " "); } // Get first word of a line. istringstream splitLine(lineNow); string name; splitLine >> name; // Replace two colons by one (:: -> :) to allow for such mistakes. while (name.find("::") != string::npos) { int firstColonColon = name.find_first_of("::"); name.replace(firstColonColon, 2, ":"); } // Check whether this is in the database. int inDataBase = 0; if (isFlag(name)) inDataBase = 1; else if (isMode(name)) inDataBase = 2; else if (isParm(name)) inDataBase = 3; else if (isWord(name)) inDataBase = 4; else if (isMVec(name)) inDataBase = 5; else if (isPVec(name)) inDataBase = 6; // For backwards compatibility: multiple -> multiparton, MI -> MPI, // minBias -> nonDiffractive. if (inDataBase == 0) { bool retry = false; string nameLower = toLower(name); if (nameLower.find("multiple") != string::npos) { int firstMI = nameLower.find_first_of("multiple"); name.replace(firstMI, 8, "Multiparton"); retry = true; } if (!retry && nameLower.find("mi") != string::npos) { int firstMI = nameLower.find_first_of("mi"); name.replace(firstMI, 2, "MPI"); retry = true; } if (!retry && nameLower.find("minbias") != string::npos) { int firstMB = nameLower.find_first_of("minbias"); name.replace(firstMB, 7, "nonDiffractive"); retry = true; } if (retry) { if (isFlag(name)) inDataBase = 1; else if (isMode(name)) inDataBase = 2; else if (isParm(name)) inDataBase = 3; else if (isWord(name)) inDataBase = 4; else if (isMVec(name)) inDataBase = 5; else if (isPVec(name)) inDataBase = 6; } } // Warn and done if not in database. if (inDataBase == 0) { if (warn) os << "\n PYTHIA Error: input string not found in settings" << " databases::\n " << line << endl; readingFailedSave = true; return false; } // Find value. Warn if none found. string valueString; splitLine >> valueString; if (!splitLine) { if (warn) os << "\n PYTHIA Error: variable recognized, but its value" << " not meaningful:\n " << line << endl; readingFailedSave = true; return false; } // Update flag map; allow many ways to say yes. if (inDataBase == 1) { bool value = boolString(valueString); flag(name, value); // Update mode map. } else if (inDataBase == 2) { istringstream modeData(valueString); int value; modeData >> value; if (!modeData) { if (warn) os << "\n PYTHIA Error: variable recognized, but its value" << " not meaningful:\n " << line << endl; readingFailedSave = true; return false; } mode(name, value); // Update parm map. } else if (inDataBase == 3) { istringstream parmData(valueString); double value; parmData >> value; if (!parmData) { if (warn) os << "\n PYTHIA Error: variable recognized, but its value" << " not meaningful:\n " << line << endl; readingFailedSave = true; return false; } parm(name, value); // Update word map. } else if (inDataBase == 4) { word(name, valueString); // Update mvec map. } else if (inDataBase == 5) { istringstream mvecData(valueString); vector value(intVectorAttributeValue( "value=\"" + valueString + "\"", "value=")); if (!mvecData) { if (warn) os << "\n PYTHIA Error: variable recognized, but its value" << " not meaningful:\n " << line << endl; readingFailedSave = true; return false; } mvec(name, value); // Update pvec map. } else if (inDataBase == 6) { istringstream pvecData(valueString); vector value(doubleVectorAttributeValue( "value=\"" + valueString + "\"", "value=")); if (!pvecData) { if (warn) os << "\n PYTHIA Error: variable recognized, but its value" << " not meaningful:\n " << line << endl; readingFailedSave = true; return false; } pvec(name, value); } // Done. return true; } //-------------------------------------------------------------------------- // Write updates or everything to user-defined file. bool Settings::writeFile(string toFile, bool writeAll) { // Open file for writing. const char* cstring = toFile.c_str(); ofstream os(cstring); if (!os) { infoPtr->errorMsg("Error in Settings::writeFile:" " could not open file", toFile); return false; } // Hand over real work to next method. return writeFile( os, writeAll); } //-------------------------------------------------------------------------- // Write updates or everything to user-defined stream (or file). bool Settings::writeFile(ostream& os, bool writeAll) { // Write simple header as comment. if (writeAll) os << "! List of all current PYTHIA "; else os << "! List of all modified PYTHIA "; os << fixed << setprecision(3) << parm("Pythia:versionNumber") << " settings.\n"; // Iterators for the flag, mode and parm tables. map::iterator flagEntry = flags.begin(); map::iterator modeEntry = modes.begin(); map::iterator parmEntry = parms.begin(); map::iterator wordEntry = words.begin(); map::iterator mvecEntry = mvecs.begin(); map::iterator pvecEntry = pvecs.begin(); // Loop while there is something left to do. while (flagEntry != flags.end() || modeEntry != modes.end() || parmEntry != parms.end() || wordEntry != words.end() || mvecEntry != mvecs.end() || pvecEntry != pvecs.end() ) { // Check if a flag is next in lexigraphical order; if so print it. if ( flagEntry != flags.end() && ( modeEntry == modes.end() || flagEntry->first < modeEntry->first ) && ( parmEntry == parms.end() || flagEntry->first < parmEntry->first ) && ( wordEntry == words.end() || flagEntry->first < wordEntry->first ) && ( mvecEntry == mvecs.end() || flagEntry->first < mvecEntry->first ) && ( pvecEntry == pvecs.end() || flagEntry->first < pvecEntry->first ) ) { string state[2] = {"off", "on"}; bool valNow = flagEntry->second.valNow; bool valDefault = flagEntry->second.valDefault; if ( writeAll || valNow != valDefault ) os << flagEntry->second.name << " = " << state[valNow] << "\n"; ++flagEntry; // Else check if mode is next, and if so print it. } else if ( modeEntry != modes.end() && ( parmEntry == parms.end() || modeEntry->first < parmEntry->first ) && ( wordEntry == words.end() || modeEntry->first < wordEntry->first ) && ( mvecEntry == mvecs.end() || modeEntry->first < mvecEntry->first ) && ( pvecEntry == pvecs.end() || modeEntry->first < pvecEntry->first ) ) { int valNow = modeEntry->second.valNow; int valDefault = modeEntry->second.valDefault; if ( writeAll || valNow != valDefault ) os << modeEntry->second.name << " = " << valNow << "\n"; ++modeEntry; // Else check if parm is next, and if so print it; // fixed or scientific depending on value. } else if ( parmEntry != parms.end() && ( wordEntry == words.end() || parmEntry->first < wordEntry->first ) && ( mvecEntry == mvecs.end() || parmEntry->first < mvecEntry->first ) && ( pvecEntry == pvecs.end() || parmEntry->first < pvecEntry->first ) ) { double valNow = parmEntry->second.valNow; double valDefault = parmEntry->second.valDefault; if ( writeAll || valNow != valDefault ) { os << parmEntry->second.name << " = "; if ( valNow == 0. ) os << fixed << setprecision(1); else if ( abs(valNow) < 0.001 ) os << scientific << setprecision(4); else if ( abs(valNow) < 0.1 ) os << fixed << setprecision(7); else if ( abs(valNow) < 1000. ) os << fixed << setprecision(5); else if ( abs(valNow) < 1000000. ) os << fixed << setprecision(3); else os << scientific << setprecision(4); os << valNow << "\n"; } ++parmEntry; // Else check if word is next, and if so print it. } else if ( wordEntry != words.end() && ( mvecEntry == mvecs.end() || wordEntry->first < mvecEntry->first ) && ( pvecEntry == pvecs.end() || wordEntry->first < pvecEntry->first ) ) { string valNow = wordEntry->second.valNow; string valDefault = wordEntry->second.valDefault; if ( writeAll || valNow != valDefault ) os << wordEntry->second.name << " = " << valNow << "\n"; ++wordEntry; // Else check if mvec is next, and if so print it. } else if ( mvecEntry != mvecs.end() && ( pvecEntry == pvecs.end() || mvecEntry->first < pvecEntry->first ) ) { vector valNow = mvecEntry->second.valNow; vector valDefault = mvecEntry->second.valDefault; if ( writeAll || valNow != valDefault ) { os << mvecEntry->second.name << " = "; for (vector::iterator val = valNow.begin(); val != --valNow.end(); ++val) os << *val << ","; os << *(--valNow.end()) << "\n"; } ++mvecEntry; // Else print pvec; fixed or scientific depending on value. } else { vector valNow = pvecEntry->second.valNow; vector valDefault = pvecEntry->second.valDefault; if ( writeAll || valNow != valDefault ) { os << pvecEntry->second.name << " = "; for (vector::iterator val = valNow.begin(); val != --valNow.end(); ++val) { if ( *val == 0. ) os << fixed << setprecision(1); else if ( abs(*val) < 0.001 ) os << scientific << setprecision(4); else if ( abs(*val) < 0.1 ) os << fixed << setprecision(7); else if ( abs(*val) < 1000. ) os << fixed << setprecision(5); else if ( abs(*val) < 1000000. ) os << fixed << setprecision(3); else os << scientific << setprecision(4); os << *val << ","; } os << *(--valNow.end()) << "\n"; } ++pvecEntry; } } ; // Done. return true; } //-------------------------------------------------------------------------- // Print out table of database in lexigraphical order. void Settings::list(bool doListAll, bool doListString, string match, ostream& os) { // Table header; output for bool as off/on. if (doListAll) os << "\n *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Set" << "tings (all) -----------------------------------------* \n"; else if (!doListString) os << "\n *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Set" << "tings (changes only) --------------------------------* \n" ; else os << "\n *------- PYTHIA Flag + Mode + Parm + Word + MVec + PVec Set" << "tings (with requested string) -----------------------* \n" ; os << " | " << " | \n" << " | Name | " << " Now | Default Min Max | \n" << " | | " << " | | \n"; // Convert input string to lowercase for match. match = toLower(match); if (match == "") match = " "; // Iterators for the flag, mode and parm tables. map::iterator flagEntry = flags.begin(); map::iterator modeEntry = modes.begin(); map::iterator parmEntry = parms.begin(); map::iterator wordEntry = words.begin(); map::iterator mvecEntry = mvecs.begin(); map::iterator pvecEntry = pvecs.begin(); // Loop while there is something left to do. while (flagEntry != flags.end() || modeEntry != modes.end() || parmEntry != parms.end() || wordEntry != words.end() || mvecEntry != mvecs.end() || pvecEntry != pvecs.end() ) { // Check if a flag is next in lexigraphical order; if so print it. if ( flagEntry != flags.end() && ( modeEntry == modes.end() || flagEntry->first < modeEntry->first ) && ( parmEntry == parms.end() || flagEntry->first < parmEntry->first ) && ( wordEntry == words.end() || flagEntry->first < wordEntry->first ) && ( mvecEntry == mvecs.end() || flagEntry->first < mvecEntry->first ) && ( pvecEntry == pvecs.end() || flagEntry->first < pvecEntry->first ) ) { string state[2] = {"off", "on"}; bool valNow = flagEntry->second.valNow; bool valDefault = flagEntry->second.valDefault; if ( doListAll || (!doListString && valNow != valDefault) || (doListString && flagEntry->first.find(match) != string::npos) ) os << " | " << setw(45) << left << flagEntry->second.name << " | " << setw(24) << right << state[valNow] << " | " << setw(12) << state[valDefault] << " | \n"; ++flagEntry; // Else check if mode is next, and if so print it. } else if ( modeEntry != modes.end() && ( parmEntry == parms.end() || modeEntry->first < parmEntry->first ) && ( wordEntry == words.end() || modeEntry->first < wordEntry->first ) && ( mvecEntry == mvecs.end() || modeEntry->first < mvecEntry->first ) && ( pvecEntry == pvecs.end() || modeEntry->first < pvecEntry->first ) ) { int valNow = modeEntry->second.valNow; int valDefault = modeEntry->second.valDefault; if ( doListAll || (!doListString && valNow != valDefault) || (doListString && modeEntry->first.find(match) != string::npos) ) { os << " | " << setw(45) << left << modeEntry->second.name << " | " << setw(24) << right << valNow << " | " << setw(12) << valDefault; if (modeEntry->second.hasMin) os << setw(12) << modeEntry->second.valMin; else os << " "; if (modeEntry->second.hasMax) os << setw(12) << modeEntry->second.valMax; else os << " "; os << " | \n"; } ++modeEntry; // Else check if parm is next, and if so print it; // fixed or scientific depending on value. } else if ( parmEntry != parms.end() && ( wordEntry == words.end() || parmEntry->first < wordEntry->first ) && ( mvecEntry == mvecs.end() || parmEntry->first < mvecEntry->first ) && ( pvecEntry == pvecs.end() || parmEntry->first < pvecEntry->first ) ) { double valNow = parmEntry->second.valNow; double valDefault = parmEntry->second.valDefault; if ( doListAll || (!doListString && valNow != valDefault ) || (doListString && parmEntry->first.find(match) != string::npos) ) { os << " | " << setw(45) << left << parmEntry->second.name << right << " | "; for (int i = 0; i < 4; ++i) { if (i == 1) valNow = valDefault; if (i == 2) valNow = parmEntry->second.valMin; if (i == 3) valNow = parmEntry->second.valMax; if ( (i == 2 && !parmEntry->second.hasMin) || (i == 3 && !parmEntry->second.hasMax) ) os << " "; else if ( valNow == 0. ) os << fixed << setprecision(1) << setw(12) << valNow; else if ( abs(valNow) < 0.001 ) os << scientific << setprecision(4) << setw(12) << valNow; else if ( abs(valNow) < 0.1 ) os << fixed << setprecision(7) << setw(12) << valNow; else if ( abs(valNow) < 1000. ) os << fixed << setprecision(5) << setw(12) << valNow; else if ( abs(valNow) < 1000000. ) os << fixed << setprecision(3) << setw(12) << valNow; else os << scientific << setprecision(4) << setw(12) << valNow; if (i == 0) os << " | "; } os << " | \n"; } ++parmEntry; // Else check if word is next, and if so print it. } else if ( wordEntry != words.end() && ( mvecEntry == mvecs.end() || wordEntry->first < mvecEntry->first ) && ( pvecEntry == pvecs.end() || wordEntry->first < pvecEntry->first ) ) { string valNow = wordEntry->second.valNow; string valDefault = wordEntry->second.valDefault; int blankLeft = max(0, 60 - max(24, int(valNow.length()) ) - max(12, int(valDefault.length()) ) ); string blankPad( blankLeft, ' '); if ( doListAll || (!doListString && valNow != valDefault) || (doListString && wordEntry->first.find(match) != string::npos) ) os << " | " << setw(45) << left << wordEntry->second.name << " | " << setw(24) << right << valNow << " | " << setw(12) << valDefault << blankPad << " | \n"; ++wordEntry; // Else check if mvec is next, and if so print it. } else if ( mvecEntry != mvecs.end() && ( pvecEntry == pvecs.end() || mvecEntry->first < pvecEntry->first ) ) { vector valsNow = mvecEntry->second.valNow; vector valsDefault = mvecEntry->second.valDefault; int valNow(0), valDefault(0); if ( doListAll || (!doListString && valsNow != valsDefault ) || (doListString && mvecEntry->first.find(match) != string::npos) ) { for (unsigned int i = 0; i < valsNow.size() || i < valsDefault.size(); ++i) { if ( i == 0 ) os << " | " << setw(45) << left << mvecEntry->second.name << right << " | "; else os << " | " << setw(45) << " " << right << " | "; for (int j = 0; j < 4; ++j) { if (i < valsNow.size()) valNow = valsNow[i]; if (i < valsDefault.size()) valDefault = valsDefault[i]; if (j == 1) valNow = valDefault; if (j == 2) valNow = mvecEntry->second.valMin; if (j == 3) valNow = mvecEntry->second.valMax; if ( (j == 0 && i >= valsNow.size()) || (j == 1 && i >= valsDefault.size()) || (j == 2 && !mvecEntry->second.hasMin) || (j == 3 && !mvecEntry->second.hasMax) ) os << " "; else os << setw(12) << valNow; if (j == 0) os << " | "; } os << " | \n"; } } ++mvecEntry; // Else print pvec; fixed or scientific depending on value. } else { vector valsNow = pvecEntry->second.valNow; vector valsDefault = pvecEntry->second.valDefault; double valNow(0), valDefault(0); if ( doListAll || (!doListString && valsNow != valsDefault ) || (doListString && pvecEntry->first.find(match) != string::npos) ) { for (unsigned int i = 0; i < valsNow.size() || i < valsDefault.size(); ++i) { if ( i == 0 ) os << " | " << setw(45) << left << pvecEntry->second.name << right << " | "; else os << " | " << setw(45) << " " << right << " | "; for (int j = 0; j < 4; ++j) { if (i < valsNow.size()) valNow = valsNow[i]; if (i < valsDefault.size()) valDefault = valsDefault[i]; if (j == 1) valNow = valDefault; if (j == 2) valNow = pvecEntry->second.valMin; if (j == 3) valNow = pvecEntry->second.valMax; if ( (j == 0 && i >= valsNow.size()) || (j == 1 && i >= valsDefault.size()) || (j == 2 && !pvecEntry->second.hasMin) || (j == 3 && !pvecEntry->second.hasMax) ) os << " "; else if ( valNow == 0. ) os << fixed << setprecision(1) << setw(12) << valNow; else if ( abs(valNow) < 0.001 ) os << scientific << setprecision(4) << setw(12) << valNow; else if ( abs(valNow) < 0.1 ) os << fixed << setprecision(7) << setw(12) << valNow; else if ( abs(valNow) < 1000. ) os << fixed << setprecision(5) << setw(12) << valNow; else if ( abs(valNow) < 1000000. ) os << fixed << setprecision(3) << setw(12) << valNow; else os << scientific << setprecision(4) << setw(12) << valNow; if (j == 0) os << " | "; } os << " | \n"; } } ++pvecEntry; } } ; // End of loop over database contents. os << " | " << " | \n" << " *------- End PYTHIA Flag + Mode + Parm + Word + MVec + PVec " << "Settings -------------------------------------------* " << endl; } //-------------------------------------------------------------------------- // Reset all values to their defaults. void Settings::resetAll() { // Loop through the flags table, resetting all entries. for (map::iterator flagEntry = flags.begin(); flagEntry != flags.end(); ++flagEntry) { string name = flagEntry->first; resetFlag(name); } // Loop through the modes table, resetting all entries. for (map::iterator modeEntry = modes.begin(); modeEntry != modes.end(); ++modeEntry) { string name = modeEntry->first; resetMode(name); } // Loop through the parms table, resetting all entries. for (map::iterator parmEntry = parms.begin(); parmEntry != parms.end(); ++parmEntry) { string name = parmEntry->first; resetParm(name); } // Loop through the words table, resetting all entries. for (map::iterator wordEntry = words.begin(); wordEntry != words.end(); ++wordEntry) { string name = wordEntry->first; resetWord(name); } // Loop through the mvecs table, resetting all entries. for (map::iterator mvecEntry = mvecs.begin(); mvecEntry != mvecs.end(); ++mvecEntry) { string name = mvecEntry->first; resetMVec(name); } // Loop through the pvecs table, resetting all entries. for (map::iterator pvecEntry = pvecs.begin(); pvecEntry != pvecs.end(); ++pvecEntry) { string name = pvecEntry->first; resetPVec(name); } } //-------------------------------------------------------------------------- // Give back current value, with check that key exists. bool Settings::flag(string keyIn) { if (isFlag(keyIn)) return flags[toLower(keyIn)].valNow; infoPtr->errorMsg("Error in Settings::flag: unknown key", keyIn); return false; } int Settings::mode(string keyIn) { if (isMode(keyIn)) return modes[toLower(keyIn)].valNow; infoPtr->errorMsg("Error in Settings::mode: unknown key", keyIn); return 0; } double Settings::parm(string keyIn) { if (isParm(keyIn)) return parms[toLower(keyIn)].valNow; infoPtr->errorMsg("Error in Settings::parm: unknown key", keyIn); return 0.; } string Settings::word(string keyIn) { if (isWord(keyIn)) return words[toLower(keyIn)].valNow; infoPtr->errorMsg("Error in Settings::word: unknown key", keyIn); return " "; } vector Settings::mvec(string keyIn) { if (isMVec(keyIn)) return mvecs[toLower(keyIn)].valNow; infoPtr->errorMsg("Error in Settings::mvec: unknown key", keyIn); return vector(1, 0); } vector Settings::pvec(string keyIn) { if (isPVec(keyIn)) return pvecs[toLower(keyIn)].valNow; infoPtr->errorMsg("Error in Settings::pvec: unknown key", keyIn); return vector(1, 0.); } //-------------------------------------------------------------------------- // Give back default value, with check that key exists. bool Settings::flagDefault(string keyIn) { if (isFlag(keyIn)) return flags[toLower(keyIn)].valDefault; infoPtr->errorMsg("Error in Settings::flagDefault: unknown key", keyIn); return false; } int Settings::modeDefault(string keyIn) { if (isMode(keyIn)) return modes[toLower(keyIn)].valDefault; infoPtr->errorMsg("Error in Settings::modeDefault: unknown key", keyIn); return 0; } double Settings::parmDefault(string keyIn) { if (isParm(keyIn)) return parms[toLower(keyIn)].valDefault; infoPtr->errorMsg("Error in Settings::parmDefault: unknown key", keyIn); return 0.; } string Settings::wordDefault(string keyIn) { if (isWord(keyIn)) return words[toLower(keyIn)].valDefault; infoPtr->errorMsg("Error in Settings::wordDefault: unknown key", keyIn); return " "; } vector Settings::mvecDefault(string keyIn) { if (isMVec(keyIn)) return mvecs[toLower(keyIn)].valDefault; infoPtr->errorMsg("Error in Settings::mvecDefault: unknown key", keyIn); return vector(1, 0); } vector Settings::pvecDefault(string keyIn) { if (isPVec(keyIn)) return pvecs[toLower(keyIn)].valDefault; infoPtr->errorMsg("Error in Settings::pvecDefault: unknown key", keyIn); return vector(1, 0.); } //-------------------------------------------------------------------------- // Get a map of entries whose names contain the string "match". map Settings::getFlagMap(string match) { // Make the match string lower case. Start with an empty map. match = toLower(match); map flagMap; // Loop over the flag map (using iterator). for (map::iterator flagEntry = flags.begin(); flagEntry != flags.end(); ++flagEntry) if (flagEntry->first.find(match) != string::npos) flagMap[flagEntry->first] = flagEntry->second; return flagMap; } map Settings::getModeMap(string match) { // Make the match string lower case. Start with an empty map. match = toLower(match); map modeMap; // Loop over the mode map (using iterator). for (map::iterator modeEntry = modes.begin(); modeEntry != modes.end(); ++modeEntry) if (modeEntry->first.find(match) != string::npos) modeMap[modeEntry->first] = modeEntry->second; return modeMap; } map Settings::getParmMap(string match) { // Make the match string lower case. Start with an empty map. match = toLower(match); map parmMap; // Loop over the parm map (using iterator). for (map::iterator parmEntry = parms.begin(); parmEntry != parms.end(); ++parmEntry) if (parmEntry->first.find(match) != string::npos) parmMap[parmEntry->first] = parmEntry->second; return parmMap; } map Settings::getWordMap(string match) { // Make the match string lower case. Start with an empty map. match = toLower(match); map wordMap; // Loop over the word map (using iterator). for (map::iterator wordEntry = words.begin(); wordEntry != words.end(); ++wordEntry) if (wordEntry->first.find(match) != string::npos) wordMap[wordEntry->first] = wordEntry->second; return wordMap; } map Settings::getMVecMap(string match) { // Make the match string lower case. Start with an empty map. match = toLower(match); map mvecMap; // Loop over the mvec map (using iterator). for (map::iterator mvecEntry = mvecs.begin(); mvecEntry != mvecs.end(); ++mvecEntry) if (mvecEntry->first.find(match) != string::npos) mvecMap[mvecEntry->first] = mvecEntry->second; return mvecMap; } map Settings::getPVecMap(string match) { // Make the match string lower case. Start with an empty map. match = toLower(match); map pvecMap; // Loop over the pvec map (using iterator). for (map::iterator pvecEntry = pvecs.begin(); pvecEntry != pvecs.end(); ++pvecEntry) if (pvecEntry->first.find(match) != string::npos) pvecMap[pvecEntry->first] = pvecEntry->second; return pvecMap; } //-------------------------------------------------------------------------- // Change current value, respecting limits. void Settings::flag(string keyIn, bool nowIn) { string keyLower = toLower(keyIn); if (isFlag(keyIn)) flags[keyLower].valNow = nowIn; // Print:quiet triggers a whole set of changes. if (keyLower == "print:quiet") printQuiet( nowIn); } void Settings:: mode(string keyIn, int nowIn) { if (isMode(keyIn)) { string keyLower = toLower(keyIn); Mode& modeNow = modes[keyLower]; if (modeNow.hasMin && nowIn < modeNow.valMin) modeNow.valNow = modeNow.valMin; else if (modeNow.hasMax && nowIn > modeNow.valMax) modeNow.valNow = modeNow.valMax; else modeNow.valNow = nowIn; // Tune:ee and Tune:pp each trigger a whole set of changes. if (keyLower == "tune:ee") initTuneEE( modeNow.valNow); if (keyLower == "tune:pp") initTunePP( modeNow.valNow); } } void Settings::parm(string keyIn, double nowIn) { if (isParm(keyIn)) { Parm& parmNow = parms[toLower(keyIn)]; if (parmNow.hasMin && nowIn < parmNow.valMin) parmNow.valNow = parmNow.valMin; else if (parmNow.hasMax && nowIn > parmNow.valMax) parmNow.valNow = parmNow.valMax; else parmNow.valNow = nowIn; } } void Settings::word(string keyIn, string nowIn) { if (isWord(keyIn)) words[toLower(keyIn)].valNow = nowIn; } void Settings::mvec(string keyIn, vector nowIn) { if (isMVec(keyIn)) { MVec& mvecNow = mvecs[toLower(keyIn)]; mvecNow.valNow.clear(); for(vector::iterator now = nowIn.begin(); now != nowIn.end(); now++) { if (mvecNow.hasMin && *now < mvecNow.valMin) mvecNow.valNow.push_back(mvecNow.valMin); else if (mvecNow.hasMax && *now > mvecNow.valMax) mvecNow.valNow.push_back(mvecNow.valMax); else mvecNow.valNow.push_back(*now); } } } void Settings::pvec(string keyIn, vector nowIn) { if (isPVec(keyIn)) { PVec& pvecNow = pvecs[toLower(keyIn)]; pvecNow.valNow.clear(); for(vector::iterator now = nowIn.begin(); now != nowIn.end(); now++) { if (pvecNow.hasMin && *now < pvecNow.valMin) pvecNow.valNow.push_back(pvecNow.valMin); else if (pvecNow.hasMax && *now > pvecNow.valMax) pvecNow.valNow.push_back(pvecNow.valMax); else pvecNow.valNow.push_back(*now); } } } //-------------------------------------------------------------------------- // Change current value, disregarding limits. void Settings::forceMode(string keyIn, int nowIn) { if (isMode(keyIn)) { string keyLower = toLower(keyIn); Mode& modeNow = modes[keyLower]; modeNow.valNow = nowIn; // Tune:ee and Tune:pp each trigger a whole set of changes. if (keyLower == "tune:ee") initTuneEE( modeNow.valNow); if (keyLower == "tune:pp") initTunePP( modeNow.valNow); } } void Settings::forceParm(string keyIn, double nowIn) { if (isParm(keyIn)) parms[toLower(keyIn)].valNow = nowIn; } void Settings::forceMVec(string keyIn, vector nowIn) { if (isMVec(keyIn)) mvecs[toLower(keyIn)].valNow = nowIn; } void Settings::forcePVec(string keyIn, vector nowIn) { if (isPVec(keyIn)) pvecs[toLower(keyIn)].valNow = nowIn; } //-------------------------------------------------------------------------- // Restore current value to default. void Settings::resetFlag(string keyIn) { if (isFlag(keyIn)) flags[toLower(keyIn)].valNow = flags[toLower(keyIn)].valDefault ; } void Settings::resetMode(string keyIn) { string keyLower = toLower(keyIn); if (isMode(keyIn)) modes[keyLower].valNow = modes[toLower(keyIn)].valDefault ; // For Tune:ee and Tune:pp must also restore variables involved in tunes. if (keyLower == "tune:ee") resetTuneEE(); if (keyLower == "tune:pp") resetTunePP(); } void Settings::resetParm(string keyIn) { if (isParm(keyIn)) parms[toLower(keyIn)].valNow = parms[toLower(keyIn)].valDefault ; } void Settings::resetWord(string keyIn) { if (isWord(keyIn)) words[toLower(keyIn)].valNow = words[toLower(keyIn)].valDefault ; } void Settings::resetMVec(string keyIn) { if (isMVec(keyIn)) mvecs[toLower(keyIn)].valNow = mvecs[toLower(keyIn)].valDefault ; } void Settings::resetPVec(string keyIn) { if (isPVec(keyIn)) pvecs[toLower(keyIn)].valNow = pvecs[toLower(keyIn)].valDefault ; } //-------------------------------------------------------------------------- // Regulate level of printout by overall change of settings. void Settings::printQuiet(bool quiet) { // Switch off as much output as possible. if (quiet) { flag("Init:showProcesses", false ); flag("Init:showMultipartonInteractions", false ); flag("Init:showChangedSettings", false ); flag("Init:showAllSettings", false ); flag("Init:showChangedParticleData", false ); flag("Init:showChangedResonanceData", false ); flag("Init:showAllParticleData", false ); mode("Init:showOneParticleData", 0 ); mode("Next:numberCount", 0 ); mode("Next:numberShowLHA", 0 ); mode("Next:numberShowInfo", 0 ); mode("Next:numberShowProcess", 0 ); mode("Next:numberShowEvent", 0 ); // Restore ouput settings to default. } else { resetFlag("Init:showProcesses"); resetFlag("Init:showMultipartonInteractions"); resetFlag("Init:showChangedSettings"); resetFlag("Init:showAllSettings"); resetFlag("Init:showChangedParticleData"); resetFlag("Init:showChangedResonanceData"); resetFlag("Init:showAllParticleData"); resetMode("Init:showOneParticleData"); resetMode("Next:numberCount"); resetMode("Next:numberShowLHA"); resetMode("Next:numberShowInfo"); resetMode("Next:numberShowProcess"); resetMode("Next:numberShowEvent"); } } //-------------------------------------------------------------------------- // Restore all e+e- settings to their original values. void Settings::resetTuneEE() { resetParm("StringFlav:probStoUD"); resetParm("StringFlav:probQQtoQ"); resetParm("StringFlav:probSQtoQQ"); resetParm("StringFlav:probQQ1toQQ0"); resetParm("StringFlav:mesonUDvector"); resetParm("StringFlav:mesonSvector"); resetParm("StringFlav:mesonCvector"); resetParm("StringFlav:mesonBvector"); resetParm("StringFlav:etaSup"); resetParm("StringFlav:etaPrimeSup"); resetParm("StringFlav:popcornSpair"); resetParm("StringFlav:popcornSmeson"); resetParm("StringZ:aLund"); resetParm("StringZ:bLund"); resetParm("StringZ:rFactB"); resetParm("StringPT:sigma"); resetParm("TimeShower:alphaSvalue"); resetParm("TimeShower:pTmin"); resetParm("TimeShower:pTminChgQ"); } //-------------------------------------------------------------------------- // Restore all pp settings to their original values. void Settings::resetTunePP() { resetMode("PDF:pSet"); resetFlag("PDF:useLHAPDF"); resetParm("SigmaProcess:alphaSvalue"); resetFlag("SigmaTotal:zeroAXB"); resetFlag("SigmaDiffractive:dampen"); resetParm("SigmaDiffractive:maxXB"); resetParm("SigmaDiffractive:maxAX"); resetParm("SigmaDiffractive:maxXX"); resetFlag("TimeShower:dampenBeamRecoil"); resetFlag("TimeShower:phiPolAsym"); resetParm("SpaceShower:alphaSvalue"); resetFlag("SpaceShower:samePTasMPI"); resetParm("SpaceShower:pT0Ref"); resetParm("SpaceShower:ecmRef"); resetParm("SpaceShower:ecmPow"); resetFlag("SpaceShower:rapidityOrder"); resetFlag("SpaceShower:phiPolAsym"); resetFlag("SpaceShower:phiIntAsym"); resetParm("MultipartonInteractions:alphaSvalue"); resetParm("MultipartonInteractions:pT0Ref"); resetParm("MultipartonInteractions:ecmRef"); resetParm("MultipartonInteractions:ecmPow"); resetMode("MultipartonInteractions:bProfile"); resetParm("MultipartonInteractions:expPow"); resetParm("MultipartonInteractions:a1"); resetParm("BeamRemnants:primordialKTsoft"); resetParm("BeamRemnants:primordialKThard"); resetParm("BeamRemnants:halfScaleForKT"); resetParm("BeamRemnants:halfMassForKT"); resetParm("BeamRemnants:reconnectRange"); } //-------------------------------------------------------------------------- // Set the values related to a tune of e+e- data, // i.e. mainly for final-state radiation and hadronization. void Settings::initTuneEE( int eeTune) { // Restore all e+e- settings to their original values. // Is first step for setting up a specific tune. if (eeTune != 0) resetTuneEE(); // Old flavour and FSR defaults carried over from very old JETSET tune, // only with alphaS roughly tuned for "new" pT-ordered shower. if (eeTune == 1) { parm("StringFlav:probStoUD", 0.30 ); parm("StringFlav:probQQtoQ", 0.10 ); parm("StringFlav:probSQtoQQ", 0.40 ); parm("StringFlav:probQQ1toQQ0", 0.05 ); parm("StringFlav:mesonUDvector", 1.00 ); parm("StringFlav:mesonSvector", 1.50 ); parm("StringFlav:mesonCvector", 2.50 ); parm("StringFlav:mesonBvector", 3.00 ); parm("StringFlav:etaSup", 1.00 ); parm("StringFlav:etaPrimeSup", 0.40 ); parm("StringFlav:popcornSpair", 0.50 ); parm("StringFlav:popcornSmeson", 0.50 ); parm("StringZ:aLund", 0.30 ); parm("StringZ:bLund", 0.58 ); parm("StringZ:rFactB", 1.00 ); parm("StringPT:sigma", 0.36 ); parm("TimeShower:alphaSvalue", 0.137 ); parm("TimeShower:pTmin", 0.5 ); parm("TimeShower:pTminChgQ", 0.5 ); } // Marc Montull's tune to particle composition at LEP1 (August 2007). else if (eeTune == 2) { parm("StringFlav:probStoUD", 0.22 ); parm("StringFlav:probQQtoQ", 0.08 ); parm("StringFlav:probSQtoQQ", 0.75 ); parm("StringFlav:probQQ1toQQ0", 0.025 ); parm("StringFlav:mesonUDvector", 0.5 ); parm("StringFlav:mesonSvector", 0.6 ); parm("StringFlav:mesonCvector", 1.5 ); parm("StringFlav:mesonBvector", 2.5 ); parm("StringFlav:etaSup", 0.60 ); parm("StringFlav:etaPrimeSup", 0.15 ); parm("StringFlav:popcornSpair", 1.0 ); parm("StringFlav:popcornSmeson", 1.0 ); parm("StringZ:aLund", 0.76 ); parm("StringZ:bLund", 0.58 ); // kept fixed parm("StringZ:rFactB", 1.00 ); // kept fixed parm("StringPT:sigma", 0.36 ); // kept fixed parm("TimeShower:alphaSvalue", 0.137 ); // kept fixed parm("TimeShower:pTmin", 0.5 ); // kept fixed parm("TimeShower:pTminChgQ", 0.5 ); // kept fixed } // Full e+e- tune of flavours and FSR to LEP1 data within the // Rivet + Professor framework, by Hendrik Hoeth (June 2009). else if (eeTune == 3) { parm("StringFlav:probStoUD", 0.19 ); parm("StringFlav:probQQtoQ", 0.09 ); parm("StringFlav:probSQtoQQ", 1.00 ); parm("StringFlav:probQQ1toQQ0", 0.027 ); parm("StringFlav:mesonUDvector", 0.62 ); parm("StringFlav:mesonSvector", 0.725 ); parm("StringFlav:mesonCvector", 1.06 ); parm("StringFlav:mesonBvector", 3.0 ); parm("StringFlav:etaSup", 0.63 ); parm("StringFlav:etaPrimeSup", 0.12 ); parm("StringFlav:popcornSpair", 0.5 ); // kept fixed parm("StringFlav:popcornSmeson", 0.5 ); // kept fixed parm("StringZ:aLund", 0.3 ); // kept fixed parm("StringZ:bLund", 0.8 ); parm("StringZ:rFactB", 0.67 ); parm("StringPT:sigma", 0.304 ); parm("TimeShower:alphaSvalue", 0.1383); parm("TimeShower:pTmin", 0.4 ); // kept fixed (near limit) parm("TimeShower:pTminChgQ", 0.4 ); // kept same as pTmin } } //-------------------------------------------------------------------------- // Set the values related to a tune of pp/ppbar data, // i.e. mainly for initial-state radiation and multiparton interactions. void Settings::initTunePP( int ppTune) { // Restore all pp/ppbar settings to their original values. // Is first step for setting up a specific tune. if (ppTune != 0) resetTunePP(); // Decide whether to use LHAPFD where possible. bool preferLHAPDF = flag("Tune:preferLHAPDF"); // Old ISR and MPI defaults from early and primitive comparisons with data. if (ppTune == 1) { mode("PDF:pSet", 2 ); parm("SigmaProcess:alphaSvalue", 0.1265); flag("SigmaTotal:zeroAXB", true ); flag("SigmaDiffractive:dampen", false ); flag("TimeShower:dampenBeamRecoil", false ); flag("TimeShower:phiPolAsym", false ); parm("SpaceShower:alphaSvalue", 0.127 ); flag("SpaceShower:samePTasMPI", true ); parm("SpaceShower:pT0Ref", 2.2 ); parm("SpaceShower:ecmRef", 1800.0); parm("SpaceShower:ecmPow", 0.16 ); flag("SpaceShower:rapidityOrder", false ); flag("SpaceShower:phiPolAsym", false ); flag("SpaceShower:phiIntAsym", false ); parm("MultipartonInteractions:alphaSvalue", 0.127 ); parm("MultipartonInteractions:pT0Ref", 2.15 ); parm("MultipartonInteractions:ecmRef", 1800. ); parm("MultipartonInteractions:ecmPow", 0.16 ); mode("MultipartonInteractions:bProfile", 2 ); parm("BeamRemnants:primordialKTsoft", 0.4 ); parm("BeamRemnants:primordialKThard", 2.1 ); parm("BeamRemnants:halfScaleForKT", 7.0 ); parm("BeamRemnants:halfMassForKT", 2.0 ); parm("BeamRemnants:reconnectRange", 2.5 ); } // "Tune 1" simple first tune by Peter Skands to ISR and MPI, July 2009. else if (ppTune == 2) { mode("PDF:pSet", 2 ); parm("SigmaProcess:alphaSvalue", 0.1265); flag("SigmaTotal:zeroAXB", true ); flag("SigmaDiffractive:dampen", false ); flag("TimeShower:dampenBeamRecoil", false ); flag("TimeShower:phiPolAsym", false ); parm("SpaceShower:alphaSvalue", 0.137 ); flag("SpaceShower:samePTasMPI", false ); parm("SpaceShower:pT0Ref", 2.0 ); parm("SpaceShower:ecmRef", 1800.0); parm("SpaceShower:ecmPow", 0.0 ); flag("SpaceShower:rapidityOrder", false ); flag("SpaceShower:phiPolAsym", false ); flag("SpaceShower:phiIntAsym", false ); parm("MultipartonInteractions:alphaSvalue", 0.127 ); parm("MultipartonInteractions:pT0Ref", 2.25 ); parm("MultipartonInteractions:ecmRef", 1800. ); parm("MultipartonInteractions:ecmPow", 0.24 ); mode("MultipartonInteractions:bProfile", 1 ); parm("BeamRemnants:primordialKTsoft", 0.5 ); parm("BeamRemnants:primordialKThard", 2.0 ); parm("BeamRemnants:halfScaleForKT", 1.0 ); parm("BeamRemnants:halfMassForKT", 1.0 ); parm("BeamRemnants:reconnectRange", 10.0 ); } // Tune 2C, July 2010. else if (ppTune == 3) { mode("PDF:pSet", 8 ); parm("SigmaProcess:alphaSvalue", 0.135 ); flag("SigmaTotal:zeroAXB", true ); flag("SigmaDiffractive:dampen", false ); flag("TimeShower:dampenBeamRecoil", true ); flag("TimeShower:phiPolAsym", true ); parm("SpaceShower:alphaSvalue", 0.137 ); flag("SpaceShower:samePTasMPI", false ); parm("SpaceShower:pT0Ref", 2.0 ); parm("SpaceShower:ecmRef", 1800.0); parm("SpaceShower:ecmPow", 0.0 ); flag("SpaceShower:rapidityOrder", true ); flag("SpaceShower:phiPolAsym", true ); flag("SpaceShower:phiIntAsym", true ); parm("MultipartonInteractions:alphaSvalue", 0.135 ); parm("MultipartonInteractions:pT0Ref", 2.32 ); parm("MultipartonInteractions:ecmRef", 1800. ); parm("MultipartonInteractions:ecmPow", 0.21 ); mode("MultipartonInteractions:bProfile", 3 ); parm("MultipartonInteractions:expPow", 1.6 ); parm("BeamRemnants:primordialKTsoft", 0.5 ); parm("BeamRemnants:primordialKThard", 2.0 ); parm("BeamRemnants:halfScaleForKT", 1.0 ); parm("BeamRemnants:halfMassForKT", 1.0 ); parm("BeamRemnants:reconnectRange", 3.0 ); } // Tune 2M, July 2010. else if (ppTune == 4) { mode("PDF:pSet", 4 ); parm("SigmaProcess:alphaSvalue", 0.1265); flag("SigmaTotal:zeroAXB", true ); flag("SigmaDiffractive:dampen", false ); flag("TimeShower:dampenBeamRecoil", true ); flag("TimeShower:phiPolAsym", true ); parm("SpaceShower:alphaSvalue", 0.130 ); flag("SpaceShower:samePTasMPI", false ); parm("SpaceShower:pT0Ref", 2.0 ); parm("SpaceShower:ecmRef", 1800.0); parm("SpaceShower:ecmPow", 0.0 ); flag("SpaceShower:rapidityOrder", true ); flag("SpaceShower:phiPolAsym", true ); flag("SpaceShower:phiIntAsym", true ); parm("MultipartonInteractions:alphaSvalue", 0.127 ); parm("MultipartonInteractions:pT0Ref", 2.455 ); parm("MultipartonInteractions:ecmRef", 1800. ); parm("MultipartonInteractions:ecmPow", 0.26 ); mode("MultipartonInteractions:bProfile", 3 ); parm("MultipartonInteractions:expPow", 1.15 ); parm("BeamRemnants:primordialKTsoft", 0.5 ); parm("BeamRemnants:primordialKThard", 2.0 ); parm("BeamRemnants:halfScaleForKT", 1.0 ); parm("BeamRemnants:halfMassForKT", 1.0 ); parm("BeamRemnants:reconnectRange", 3.0 ); } // Tune 4C, October 2010. else if (ppTune == 5) { mode("PDF:pSet", 8 ); parm("SigmaProcess:alphaSvalue", 0.135 ); flag("SigmaTotal:zeroAXB", true ); flag("SigmaDiffractive:dampen", true ); parm("SigmaDiffractive:maxXB", 65.0 ); parm("SigmaDiffractive:maxAX", 65.0 ); parm("SigmaDiffractive:maxXX", 65.0 ); flag("TimeShower:dampenBeamRecoil", true ); flag("TimeShower:phiPolAsym", true ); parm("SpaceShower:alphaSvalue", 0.137 ); flag("SpaceShower:samePTasMPI", false ); parm("SpaceShower:pT0Ref", 2.0 ); parm("SpaceShower:ecmRef", 1800.0); parm("SpaceShower:ecmPow", 0.0 ); flag("SpaceShower:rapidityOrder", true ); flag("SpaceShower:phiPolAsym", true ); flag("SpaceShower:phiIntAsym", true ); parm("MultipartonInteractions:alphaSvalue", 0.135 ); parm("MultipartonInteractions:pT0Ref", 2.085 ); parm("MultipartonInteractions:ecmRef", 1800. ); parm("MultipartonInteractions:ecmPow", 0.19 ); mode("MultipartonInteractions:bProfile", 3 ); parm("MultipartonInteractions:expPow", 2.0 ); parm("BeamRemnants:primordialKTsoft", 0.5 ); parm("BeamRemnants:primordialKThard", 2.0 ); parm("BeamRemnants:halfScaleForKT", 1.0 ); parm("BeamRemnants:halfMassForKT", 1.0 ); parm("BeamRemnants:reconnectRange", 1.5 ); } // Tune 4Cx, January 2011. else if (ppTune == 6) { mode("PDF:pSet", 8 ); parm("SigmaProcess:alphaSvalue", 0.135 ); flag("SigmaTotal:zeroAXB", true ); flag("SigmaDiffractive:dampen", true ); parm("SigmaDiffractive:maxXB", 65.0 ); parm("SigmaDiffractive:maxAX", 65.0 ); parm("SigmaDiffractive:maxXX", 65.0 ); flag("TimeShower:dampenBeamRecoil", true ); flag("TimeShower:phiPolAsym", true ); parm("SpaceShower:alphaSvalue", 0.137 ); flag("SpaceShower:samePTasMPI", false ); parm("SpaceShower:pT0Ref", 2.0 ); parm("SpaceShower:ecmRef", 1800.0); parm("SpaceShower:ecmPow", 0.0 ); flag("SpaceShower:rapidityOrder", true ); flag("SpaceShower:phiPolAsym", true ); flag("SpaceShower:phiIntAsym", true ); parm("MultipartonInteractions:alphaSvalue", 0.135 ); parm("MultipartonInteractions:pT0Ref", 2.15 ); parm("MultipartonInteractions:ecmRef", 1800. ); parm("MultipartonInteractions:ecmPow", 0.19 ); mode("MultipartonInteractions:bProfile", 4 ); parm("MultipartonInteractions:a1", 0.15 ); parm("BeamRemnants:primordialKTsoft", 0.5 ); parm("BeamRemnants:primordialKThard", 2.0 ); parm("BeamRemnants:halfScaleForKT", 1.0 ); parm("BeamRemnants:halfMassForKT", 1.0 ); parm("BeamRemnants:reconnectRange", 1.5 ); } // Several ATLAS tunes in the A2 and AU2 series, see // ATLAS note ATL-PHYS-PUB-2012-003 (August 2012). else if (ppTune < 14) { parm("SigmaProcess:alphaSvalue", 0.135 ); flag("SigmaTotal:zeroAXB", true ); flag("SigmaDiffractive:dampen", true ); parm("SigmaDiffractive:maxXB", 65.0 ); parm("SigmaDiffractive:maxAX", 65.0 ); parm("SigmaDiffractive:maxXX", 65.0 ); flag("TimeShower:dampenBeamRecoil", true ); flag("TimeShower:phiPolAsym", true ); parm("SpaceShower:alphaSvalue", 0.137 ); flag("SpaceShower:samePTasMPI", false ); parm("SpaceShower:pT0Ref", 2.0 ); parm("SpaceShower:ecmRef", 1800.0); parm("SpaceShower:ecmPow", 0.0 ); flag("SpaceShower:rapidityOrder", false ); flag("SpaceShower:phiPolAsym", true ); flag("SpaceShower:phiIntAsym", true ); parm("MultipartonInteractions:alphaSvalue", 0.135 ); parm("MultipartonInteractions:ecmRef", 1800. ); mode("MultipartonInteractions:bProfile", 4 ); parm("BeamRemnants:primordialKTsoft", 0.5 ); parm("BeamRemnants:primordialKThard", 2.0 ); parm("BeamRemnants:halfScaleForKT", 1.0 ); parm("BeamRemnants:halfMassForKT", 1.0 ); // ATLAS MB tune A2-CTEQ6L1. if (ppTune == 7) { if (preferLHAPDF) { flag("PDF:useLHAPDF", true ); word("PDF:LHAPDFset", "cteq6ll.LHpdf"); } else mode("PDF:pSet", 8 ); parm("MultipartonInteractions:pT0Ref", 2.18 ); parm("MultipartonInteractions:ecmPow", 0.22 ); parm("MultipartonInteractions:a1", 0.06 ); parm("BeamRemnants:reconnectRange", 1.55 ); } // ATLAS MB tune A2-MSTW2008LO. else if (ppTune == 8) { if (preferLHAPDF) { flag("PDF:useLHAPDF", true ); word("PDF:LHAPDFset", "MSTW2008lo68cl.LHgrid"); } else mode("PDF:pSet", 5 ); parm("MultipartonInteractions:pT0Ref", 1.90 ); parm("MultipartonInteractions:ecmPow", 0.30 ); parm("MultipartonInteractions:a1", 0.03 ); parm("BeamRemnants:reconnectRange", 2.28 ); } // ATLAS UE tune AU2-CTEQ6L1. if (ppTune == 9) { if (preferLHAPDF) { flag("PDF:useLHAPDF", true ); word("PDF:LHAPDFset", "cteq6ll.LHpdf"); } else mode("PDF:pSet", 8 ); parm("MultipartonInteractions:pT0Ref", 2.13 ); parm("MultipartonInteractions:ecmPow", 0.21 ); parm("MultipartonInteractions:a1", 0.00 ); parm("BeamRemnants:reconnectRange", 2.21 ); } // ATLAS UE tune AU2-MSTW2008LO. else if (ppTune == 10) { if (preferLHAPDF) { flag("PDF:useLHAPDF", true ); word("PDF:LHAPDFset", "MSTW2008lo68cl.LHgrid"); } else mode("PDF:pSet", 5 ); parm("MultipartonInteractions:pT0Ref", 1.87 ); parm("MultipartonInteractions:ecmPow", 0.28 ); parm("MultipartonInteractions:a1", 0.01 ); parm("BeamRemnants:reconnectRange", 5.32 ); } // ATLAS UE tune AU2-CT10. else if (ppTune == 11) { flag("PDF:useLHAPDF", true ); word("PDF:LHAPDFset", "CT10.LHgrid"); parm("MultipartonInteractions:pT0Ref", 1.70 ); parm("MultipartonInteractions:ecmPow", 0.16 ); parm("MultipartonInteractions:a1", 0.10 ); parm("BeamRemnants:reconnectRange", 4.67 ); } // ATLAS UE tune AU2-MRST2007LO*. else if (ppTune == 12) { if (preferLHAPDF) { flag("PDF:useLHAPDF", true ); word("PDF:LHAPDFset", "MRST2007lomod.LHgrid"); } else mode("PDF:pSet", 3 ); parm("MultipartonInteractions:pT0Ref", 2.39 ); parm("MultipartonInteractions:ecmPow", 0.24 ); parm("MultipartonInteractions:a1", 0.01 ); parm("BeamRemnants:reconnectRange", 1.76 ); } // ATLAS UE tune AU2-MRST2007LO**. else if (ppTune == 13) { if (preferLHAPDF) { flag("PDF:useLHAPDF", true ); word("PDF:LHAPDFset", "MRSTMCal.LHgrid"); } else mode("PDF:pSet", 4 ); parm("MultipartonInteractions:pT0Ref", 2.57 ); parm("MultipartonInteractions:ecmPow", 0.23 ); parm("MultipartonInteractions:a1", 0.01 ); parm("BeamRemnants:reconnectRange", 1.47 ); } } } //-------------------------------------------------------------------------- // Convert string to lowercase for case-insensitive comparisons. // Also remove initial and trailing blanks, if any. string Settings::toLower(const string& name) { // Copy string without initial and trailing blanks. if (name.find_first_not_of(" \n\t\v\b\r\f\a") == string::npos) return ""; int firstChar = name.find_first_not_of(" \n\t\v\b\r\f\a"); int lastChar = name.find_last_not_of(" \n\t\v\b\r\f\a"); string temp = name.substr( firstChar, lastChar + 1 - firstChar); // Convert to lowercase letter by letter. for (int i = 0; i < int(temp.length()); ++i) temp[i] = tolower(temp[i]); return temp; } //-------------------------------------------------------------------------- // Allow several alternative inputs for true/false. bool Settings::boolString(string tag) { string tagLow = toLower(tag); return ( tagLow == "true" || tagLow == "1" || tagLow == "on" || tagLow == "yes" || tagLow == "ok" ); } //-------------------------------------------------------------------------- // Extract XML value string following XML attribute. string Settings::attributeValue(string line, string attribute) { if (line.find(attribute) == string::npos) return ""; int iBegAttri = line.find(attribute); int iBegQuote = line.find("\"", iBegAttri + 1); int iEndQuote = line.find("\"", iBegQuote + 1); return line.substr(iBegQuote + 1, iEndQuote - iBegQuote - 1); } //-------------------------------------------------------------------------- // Extract XML bool value following XML attribute. bool Settings::boolAttributeValue(string line, string attribute) { string valString = attributeValue(line, attribute); if (valString == "") return false; return boolString(valString); } //-------------------------------------------------------------------------- // Extract XML int value following XML attribute. int Settings::intAttributeValue(string line, string attribute) { string valString = attributeValue(line, attribute); if (valString == "") return 0; istringstream valStream(valString); int intVal; valStream >> intVal; return intVal; } //-------------------------------------------------------------------------- // Extract XML double value following XML attribute. double Settings::doubleAttributeValue(string line, string attribute) { string valString = attributeValue(line, attribute); if (valString == "") return 0.; istringstream valStream(valString); double doubleVal; valStream >> doubleVal; return doubleVal; } //-------------------------------------------------------------------------- // Extract XML int vector value following XML attribute. vector Settings::intVectorAttributeValue(string line, string attribute) { string valString = attributeValue(line, attribute); if (valString == "") return vector(1, 0); int intVal; vector vectorVal; size_t stringPos(0); while (stringPos != string::npos) { stringPos = valString.find(","); istringstream valStream(valString.substr(0, stringPos)); valString = valString.substr(stringPos + 1); valStream >> intVal; vectorVal.push_back(intVal); } return vectorVal; } //-------------------------------------------------------------------------- // Extract XML double vector value following XML attribute. vector Settings::doubleVectorAttributeValue(string line, string attribute) { string valString = attributeValue(line, attribute); if (valString == "") return vector(1, 0.); double doubleVal; vector vectorVal; size_t stringPos(0); while (stringPos != string::npos) { stringPos = valString.find(","); istringstream valStream(valString.substr(0, stringPos)); valString = valString.substr(stringPos + 1); valStream >> doubleVal; vectorVal.push_back(doubleVal); } return vectorVal; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/History.cc0000644000175000017500000076434012217346246015115 0ustar sunsun// History.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file is written by Stefan Prestel. // Function definitions (not found in the header) for the // Clustering and History classes. #include "Pythia8/History.h" namespace Pythia8 { //========================================================================== // The Clustering class. //-------------------------------------------------------------------------- // Declaration of Clustering class // This class holds information about one radiator, recoiler, // emitted system. // This class is a container class for History class use. // print for debug void Clustering::list() const { cout << " emt " << emitted << " rad " << emittor << " rec " << recoiler << " partner " << partner << " pTscale " << pTscale << endl; } //========================================================================== // The History class. // A History object represents an event in a given step in the CKKW-L // clustering procedure. It defines a tree-like recursive structure, // where the root node represents the state with n jets as given by // the matrix element generator, and is characterized by the member // variable mother being null. The leaves on the tree corresponds to a // fully clustered paths where the original n-jets has been clustered // down to the Born-level state. Also states which cannot be clustered // down to the Born-level are possible - these will be called // incomplete. The leaves are characterized by the vector of children // being empty. //-------------------------------------------------------------------------- // Number of trial emission to use for calculating the average number of // emissions const int History::NTRIAL = 1; //-------------------------------------------------------------------------- // Declaration of History class // The only constructor. Default arguments are used when creating // the initial history node. The \a depth is the maximum number of // clusterings requested. \a scalein is the scale at which the \a // statein was clustered (should be set to the merging scale for the // initial history node. \a beamAIn and beamBIn are needed to // calcutate PDF ratios, \a particleDataIn to have access to the // correct masses of particles. If \a isOrdered is true, the previous // clusterings has been ordered. \a is the PDF ratio for this // clustering (=1 for FSR clusterings). \a probin is the accumulated // probabilities for the previous clusterings, and \ mothin is the // previous history node (null for the initial node). History::History( int depth, double scalein, Event statein, Clustering c, MergingHooks* mergingHooksPtrIn, BeamParticle beamAIn, BeamParticle beamBIn, ParticleData* particleDataPtrIn, Info* infoPtrIn, bool isOrdered = true, bool isStronglyOrdered = true, bool isAllowed = true, bool isNextInInput = true, double probin = 1.0, History * mothin = 0) : state(statein), mother(mothin), sumpath(0.0), sumGoodBranches(0.0), sumBadBranches(0.0), foundOrderedPath(false), foundStronglyOrderedPath(false), foundAllowedPath(false), foundCompletePath(false), scale(scalein), nextInInput(isNextInInput), prob(probin), clusterIn(c), iReclusteredOld(0), doInclude(true), mergingHooksPtr(mergingHooksPtrIn), beamA(beamAIn), beamB(beamBIn), particleDataPtr(particleDataPtrIn), infoPtr(infoPtrIn) { // Initialise beam particles setupBeams(); // Update probability with PDF ratio if (mother && mergingHooksPtr->includeRedundant()) prob *= pdfForSudakov(); // Minimal scalar sum of pT used in Herwig to choose history // Keep track of scalar PT if (mother) { double acoll = (mother->state[clusterIn.emittor].isFinal()) ? mergingHooksPtr->herwigAcollFSR() : mergingHooksPtr->herwigAcollISR(); sumScalarPT = mother->sumScalarPT + acoll*scale; } else sumScalarPT = 0.0; // Remember reclustered radiator in lower multiplicity state if ( mother ) iReclusteredOld = mother->iReclusteredNew; // Check if more steps should be taken. int nFinalP = 0; int nFinalW = 0; for ( int i = 0; i < int(state.size()); ++i ) if ( state[i].isFinal() ) { if ( state[i].colType() != 0 ) nFinalP++; if ( state[i].idAbs() == 24 ) nFinalW++; } if ( mergingHooksPtr->doWClustering() && nFinalP == 2 && nFinalW == 0 ) depth = 0; // If this is not the fully clustered state, try to find possible // QCD clusterings. vector clusterings; if ( depth > 0 ) clusterings = getAllQCDClusterings(); // If necessary, try to find possible EW clusterings. vector clusteringsEW; if ( depth > 0 && mergingHooksPtr->doWClustering() ) clusteringsEW = getAllEWClusterings(); if ( !clusteringsEW.empty() ) { clusterings.resize(0); clusterings.insert( clusterings.end(), clusteringsEW.begin(), clusteringsEW.end() ); } // If necessary, try to find possible SQCD clusterings. vector clusteringsSQCD; if ( depth > 0 && mergingHooksPtr->doSQCDClustering() ) clusteringsSQCD = getAllSQCDClusterings(); if ( !clusteringsSQCD.empty() ) clusterings.insert( clusterings.end(), clusteringsSQCD.begin(), clusteringsSQCD.end() ); if ( clusterings.empty() && depth > 0) { string message="Warning in History::History: No clusterings"; message+=" found. History incomplete."; infoPtr->errorMsg(message); } // If no clusterings were found, the recursion is done and we // register this node. if ( clusterings.empty() ) { // Multiply with hard process matrix element. prob *= hardProcessME(state); registerPath( *this, isOrdered, isStronglyOrdered, isAllowed, depth == 0 ); return; } // Now we sort the possible clusterings so that we try the // smallest scale first. multimap sorted; for ( int i = 0, N = clusterings.size(); i < N; ++i ) { sorted.insert(make_pair(clusterings[i].pT(), &clusterings[i])); } for ( multimap::iterator it = sorted.begin(); it != sorted.end(); ++it ) { // If this path is not strongly ordered and we already have found an // ordered path, then we don't need to continue along this path. bool stronglyOrdered = isStronglyOrdered; if ( mergingHooksPtr->enforceStrongOrdering() && ( !stronglyOrdered || ( mother && ( it->first < mergingHooksPtr->scaleSeparationFactor()*scale ) ))) { if ( onlyStronglyOrderedPaths() ) continue; stronglyOrdered = false; } // Check if reclustering follows ordered sequence. bool ordered = isOrdered; if ( mergingHooksPtr->orderInRapidity() && mergingHooksPtr->orderHistories() ) { // Get new z value double z = getCurrentZ((*it->second).emittor, (*it->second).recoiler,(*it->second).emitted); // Get z value of splitting that produced this state double zOld = (!mother) ? 0. : mother->getCurrentZ(clusterIn.emittor, clusterIn.recoiler,clusterIn.emitted); // If this path is not ordered in pT and y, and we already have found // an ordered path, then we don't need to continue along this path. if ( !ordered || ( mother && (it->first < scale || it->first < pow(1. - z,2) / (z * (1. - zOld ))*scale ))) { if ( onlyOrderedPaths() ) continue; ordered = false; } } else if ( mergingHooksPtr->orderHistories() ) { // If this path is not ordered in pT and we already have found an // ordered path, then we don't need to continue along this path, unless // we have not yet found an allowed path. if ( !ordered || ( mother && (it->first < scale) ) ) { if ( onlyOrderedPaths() && onlyAllowedPaths() ) continue; ordered = false; } } // Check if reclustered state should be disallowed. bool doCut = mergingHooksPtr->canCutOnRecState() || mergingHooksPtr->allowCutOnRecState(); bool allowed = isAllowed; if ( doCut && mergingHooksPtr->doCutOnRecState(cluster(*it->second)) ) { if ( onlyAllowedPaths() ) continue; allowed = false; } // Perform the clustering and recurse and construct the next // history node. children.push_back(new History(depth - 1,it->first,cluster(*it->second), *it->second, mergingHooksPtr, beamA, beamB, particleDataPtr, infoPtr, ordered, stronglyOrdered, allowed, true, prob*getProb(*it->second), this )); } } //-------------------------------------------------------------------------- // Function to project all possible paths onto only the desired paths. bool History::projectOntoDesiredHistories() { // At the moment, only trim histories. return trimHistories(); } //-------------------------------------------------------------------------- // In the initial history node, select one of the paths according to // the probabilities. This function should be called for the initial // history node. // IN trialShower* : Previously initialised trialShower object, // to perform trial showering and as // repository of pointers to initialise alphaS // PartonSystems* : PartonSystems object needed to initialise // shower objects // OUT double : (Sukadov) , (alpha_S ratios) , (PDF ratios) double History::weightTREE(PartonLevel* trial, AlphaStrong * asFSR, AlphaStrong * asISR, double RN) { if ( mergingHooksPtr->canCutOnRecState() && !foundAllowedPath ) { string message="Warning in History::weightTREE: No allowed history"; message+=" found. Using disallowed history."; infoPtr->errorMsg(message); } if ( mergingHooksPtr->orderHistories() && !foundOrderedPath ) { string message="Warning in History::weightTREE: No ordered history"; message+=" found. Using unordered history."; infoPtr->errorMsg(message); } if ( mergingHooksPtr->canCutOnRecState() && mergingHooksPtr->orderHistories() && !foundAllowedPath && !foundOrderedPath ) { string message="Warning in History::weightTREE: No allowed or ordered"; message+=" history found."; infoPtr->errorMsg(message); } // Read alpha_S in ME calculation and maximal scale (eCM) double asME = infoPtr->alphaS(); double maxScale = (foundCompletePath) ? infoPtr->eCM() : mergingHooksPtr->muFinME(); // Select a path of clusterings History * selected = select(RN); // Set scales in the states to the scales pythia would have set selected->setScalesInHistory(); // Get weight. double asWeight = 1.; double pdfWeight = 1.; // Do trial shower, calculation of alpha_S ratios, PDF ratios double wt = selected->weightTree( trial, asME, maxScale, selected->clusterIn.pT(), asFSR, asISR, asWeight, pdfWeight ); // MPI no-emission probability int njetsMaxMPI = mergingHooksPtr->nMinMPI(); double mpiwt = selected->weightTreeEmissions( trial, -1, njetsMaxMPI, maxScale ); // Set hard process renormalisation scale to default Pythia value. bool resetScales = mergingHooksPtr->resetHardQRen(); // For pure QCD dijet events, evaluate the coupling of the hard process at // a more reasonable pT, rather than evaluation \alpha_s at a fixed // arbitrary scale. if ( resetScales && mergingHooksPtr->getProcessString().compare("pp>jj") == 0) { // Reset to a running coupling. Here we choose FSR for simplicity. double newQ2Ren = pow2( selected->hardRenScale(selected->state) ); double runningCoupling = (*asFSR).alphaS(newQ2Ren) / asME; asWeight *= pow2(runningCoupling); } // For prompt photon events, evaluate the coupling of the hard process at // a more reasonable pT, rather than evaluation \alpha_s at a fixed // arbitrary scale. if ( resetScales && mergingHooksPtr->getProcessString().compare("pp>aj") == 0) { // Reset to a running coupling. In prompt photon always ISR. double newQ2Ren = pow2( selected->hardRenScale(selected->state) ); double runningCoupling = (*asISR).alphaS( newQ2Ren + pow(mergingHooksPtr->pT0ISR(),2) ) / asME; asWeight *= runningCoupling; } // Done return (wt*asWeight*pdfWeight*mpiwt); } //-------------------------------------------------------------------------- // Function to return weight of virtual correction and subtractive events // for NL3 merging double History::weightLOOP(PartonLevel* trial, double RN ) { if ( mergingHooksPtr->canCutOnRecState() && !foundAllowedPath ) { string message="Warning in History::weightLOOP: No allowed history"; message+=" found. Using disallowed history."; infoPtr->errorMsg(message); } // Select a path of clusterings History * selected = select(RN); // Set scales in the states to the scales pythia would have set selected->setScalesInHistory(); // So far, no reweighting double wt = 1.; // Only reweighting with MPI no-emission probability double maxScale = (foundCompletePath) ? infoPtr->eCM() : mergingHooksPtr->muFinME(); int njetsMaxMPI = mergingHooksPtr->nMinMPI(); double mpiwt = selected->weightTreeEmissions( trial, -1, njetsMaxMPI, maxScale ); wt = mpiwt; // Done return wt; } //-------------------------------------------------------------------------- // Function to calculate O(\alpha_s)-term of CKKWL-weight for NLO merging double History::weightFIRST(PartonLevel* trial, AlphaStrong* asFSR, AlphaStrong* asISR, double RN, Rndm* rndmPtr ) { // Read alpha_S in ME calculation and maximal scale (eCM) double asME = infoPtr->alphaS(); double muR = mergingHooksPtr->muRinME(); double maxScale = (foundCompletePath) ? infoPtr->eCM() : mergingHooksPtr->muFinME(); // Pick path of clusterings History * selected = select(RN); // Set scales in the states to the scales pythia would have set selected->setScalesInHistory(); double nSteps = mergingHooksPtr->getNumberOfClusteringSteps(state); // Get the lowest order k-factor and add first two terms in expansion double kFactor = asME * mergingHooksPtr->k1Factor(nSteps); // If using Bbar, which includes a tree-level part, subtract an // additional one, i.e. the O(\as^0) contribution as well double wt = 1. + kFactor; // Calculate sum of O(alpha) terms wt += selected->weightFirst(trial,asME, muR, maxScale, asFSR, asISR, rndmPtr ); // Get starting scale for trial showers. double startingScale = (selected->mother) ? state.scale() : infoPtr->eCM(); // Count emissions: New variant // Generate true average, not only one-point bool fixpdf = true; bool fixas = true; double nWeight1 = 0.; for(int i=0; i < NTRIAL; ++i) { // Get number of emissions vector unresolvedEmissionTerm = countEmissions( trial, startingScale, mergingHooksPtr->tms(), 2, asME, asFSR, asISR, 3, fixpdf, fixas ); nWeight1 += unresolvedEmissionTerm[1]; } wt += nWeight1/double(NTRIAL); // Done return wt; } //-------------------------------------------------------------------------- double History::weight_UMEPS_TREE(PartonLevel* trial, AlphaStrong * asFSR, AlphaStrong * asISR, double RN) { // No difference to CKKW-L. Recycle CKKW-L function. return weightTREE( trial, asFSR, asISR, RN); } //-------------------------------------------------------------------------- // Function to return weight of virtual correction events for NLO merging double History::weight_UMEPS_SUBT(PartonLevel* trial, AlphaStrong * asFSR, AlphaStrong * asISR, double RN ) { // Read alpha_S in ME calculation and maximal scale (eCM) double asME = infoPtr->alphaS(); double maxScale = (foundCompletePath) ? infoPtr->eCM() : mergingHooksPtr->muFinME(); // Select a path of clusterings History * selected = select(RN); // Set scales in the states to the scales pythia would have set selected->setScalesInHistory(); // Get weight. double asWeight = 1.; double pdfWeight = 1.; // Do trial shower, calculation of alpha_S ratios, PDF ratios double sudakov = selected->weightTree(trial, asME, maxScale, selected->clusterIn.pT(), asFSR, asISR, asWeight, pdfWeight); // MPI no-emission probability. int njetsMaxMPI = mergingHooksPtr->nMinMPI()+1; double mpiwt = selected->weightTreeEmissions( trial, -1, njetsMaxMPI, maxScale ); // Set hard process renormalisation scale to default Pythia value. bool resetScales = mergingHooksPtr->resetHardQRen(); // For pure QCD dijet events, evaluate the coupling of the hard process at // a more reasonable pT, rather than evaluation \alpha_s at a fixed // arbitrary scale. if ( resetScales && mergingHooksPtr->getProcessString().compare("pp>jj") == 0) { // Reset to a running coupling. Here we choose FSR for simplicity. double newQ2Ren = pow2( selected->hardRenScale(selected->state) ); double runningCoupling = (*asFSR).alphaS(newQ2Ren) / asME; asWeight *= pow(runningCoupling,2); } // For prompt photon events, evaluate the coupling of the hard process at // a more reasonable pT, rather than evaluation \alpha_s at a fixed // arbitrary scale. if ( resetScales && mergingHooksPtr->getProcessString().compare("pp>aj") == 0) { // Reset to a running coupling. In prompt photon always ISR. double newQ2Ren = pow2( selected->hardRenScale(selected->state) ); double runningCoupling = (*asISR).alphaS( newQ2Ren + pow(mergingHooksPtr->pT0ISR(),2) ) / asME; asWeight *= runningCoupling; } // Done return (asWeight*pdfWeight*sudakov*mpiwt); } //-------------------------------------------------------------------------- double History::weight_UNLOPS_TREE(PartonLevel* trial, AlphaStrong * asFSR, AlphaStrong * asISR, double RN) { // Read alpha_S in ME calculation and maximal scale (eCM) double asME = infoPtr->alphaS(); double maxScale = (foundCompletePath) ? infoPtr->eCM() : mergingHooksPtr->muFinME(); // Select a path of clusterings History * selected = select(RN); // Set scales in the states to the scales pythia would have set selected->setScalesInHistory(); // Get weight. double asWeight = 1.; double pdfWeight = 1.; // Do trial shower, calculation of alpha_S ratios, PDF ratios double wt = selected->weightTree(trial, asME, maxScale, selected->clusterIn.pT(), asFSR, asISR, asWeight, pdfWeight); // MPI no-emission probability. int njetsMaxMPI = mergingHooksPtr->nMinMPI(); double mpiwt = selected->weightTreeEmissions( trial, -1, njetsMaxMPI, maxScale ); // Set hard process renormalisation scale to default Pythia value. bool resetScales = mergingHooksPtr->resetHardQRen(); // For pure QCD dijet events, evaluate the coupling of the hard process at // a more reasonable pT, rather than evaluation \alpha_s at a fixed // arbitrary scale. if ( resetScales && mergingHooksPtr->getProcessString().compare("pp>jj") == 0) { // Reset to a running coupling. Here we choose FSR for simplicity. double newQ2Ren = pow2( selected->hardRenScale(selected->state) ); double runningCoupling = (*asFSR).alphaS(newQ2Ren) / asME; asWeight *= pow(runningCoupling,2); } // For prompt photon events, evaluate the coupling of the hard process at // a more reasonable pT, rather than evaluation \alpha_s at a fixed // arbitrary scale. if ( resetScales && mergingHooksPtr->getProcessString().compare("pp>aj") == 0) { // Reset to a running coupling. In prompt photon always ISR. double newQ2Ren = pow2( selected->hardRenScale(selected->state) ); double runningCoupling = (*asISR).alphaS( newQ2Ren + pow(mergingHooksPtr->pT0ISR(),2) ) / asME; asWeight *= runningCoupling; } // Done return (wt*asWeight*pdfWeight*mpiwt); } //-------------------------------------------------------------------------- double History::weight_UNLOPS_LOOP(PartonLevel* trial, double RN ) { // No difference to default NL3 return weightLOOP(trial, RN ); } //-------------------------------------------------------------------------- double History::weight_UNLOPS_SUBT(PartonLevel* trial, AlphaStrong * asFSR, AlphaStrong * asISR, double RN ) { // Select a path of clusterings History * selected = select(RN); // Set scales in the states to the scales pythia would have set selected->setScalesInHistory(); // So far, no reweighting double wt = 1.; // Read alpha_S in ME calculation and maximal scale (eCM) double asME = infoPtr->alphaS(); double maxScale = (foundCompletePath) ? infoPtr->eCM() : mergingHooksPtr->muFinME(); // Only allow two clusterings if all intermediate states above the // merging scale. double nSteps = mergingHooksPtr->getNumberOfClusteringSteps(state); if ( nSteps == 2 && mergingHooksPtr->nRecluster() == 2 && ( !foundCompletePath || !selected->allIntermediateAboveRhoMS( mergingHooksPtr->tms() )) ) { return 0.; } // Get weights: alpha_S ratios and PDF ratios double asWeight = 1.; double pdfWeight = 1.; // Do trial shower, calculation of alpha_S ratios, PDF ratios double sudakov = selected->weightTree(trial, asME, maxScale, selected->clusterIn.pT(), asFSR, asISR, asWeight, pdfWeight); // MPI no-emission probability. int njetsMaxMPI = mergingHooksPtr->nMinMPI()+1; double mpiwt = selected->weightTreeEmissions( trial, -1, njetsMaxMPI, maxScale ); // Set weight wt = ( mergingHooksPtr->nRecluster() == 2 ) ? 1. : asWeight*pdfWeight*sudakov*mpiwt; // Done return wt; } //-------------------------------------------------------------------------- double History::weight_UNLOPS_SUBTNLO(PartonLevel* trial, double RN ) { // Select a path of clusterings History * selected = select(RN); // Set scales in the states to the scales pythia would have set selected->setScalesInHistory(); // So far, no reweighting double wt = 1.; // Only reweighting with MPI no-emission probability double maxScale = (foundCompletePath) ? infoPtr->eCM() : mergingHooksPtr->muFinME(); int njetsMaxMPI = mergingHooksPtr->nMinMPI()+1; double mpiwt = selected->weightTreeEmissions( trial, -1, njetsMaxMPI, maxScale ); wt = mpiwt; // Done return wt; } //-------------------------------------------------------------------------- // Function to calculate O(\alpha_s)-term of CKKWL-weight for NLO merging double History::weight_UNLOPS_CORRECTION( int order, PartonLevel* trial, AlphaStrong* asFSR, AlphaStrong* asISR, double RN, Rndm* rndmPtr ) { // Already done if no correction should be calculated if ( order < 0 ) return 0.; // Read alpha_S in ME calculation and maximal scale (eCM) double asME = infoPtr->alphaS(); double muR = mergingHooksPtr->muRinME(); double maxScale = (foundCompletePath) ? infoPtr->eCM() : mergingHooksPtr->muFinME(); // Pick path of clusterings History * selected = select(RN); // Set scales in the states to the scales pythia would have set selected->setScalesInHistory(); double nSteps = mergingHooksPtr->getNumberOfClusteringSteps(state); // Get the lowest order k-factor and add first two terms in expansion double kFactor = asME * mergingHooksPtr->k1Factor(nSteps); // If using Bbar, which includes a tree-level part, subtract an // additional one, i.e. the O(\as^0) contribution as well double wt = 1.; // If only O(\alpha_s^0)-term is to be calculated, done already. if ( order == 0 ) return wt; // Start by adding the O(\alpha_s^1)-term of the k-factor. wt += kFactor; // Calculate sum of O(\alpha_s^1)-terms of the ckkw-l weight WITHOUT // the O(\alpha_s^1)-term of the last no-emission probability. bool fixpdf = true; bool fixas = true; // Get first term in expansion of alpha_s ratios. double wA = selected->weightFirstALPHAS( asME, muR, asFSR, asISR ); // Add logarithm from \alpha_s expansion to weight. wt += (fixas) ? wA : 0.; // Generate true average, not only one-point. double nWeight = 0.; for ( int i=0; i < NTRIAL; ++i ) { // Get average number of emissions. double wE = selected->weightFirstEmissions(trial,asME, maxScale, asFSR, asISR, fixpdf, fixas ); // Add average number of emissions off reconstructed states to weight. nWeight += wE; // Get first term in expansion of PDF ratios. double pscale = selected->clusterIn.pT(); double wP = selected->weightFirstPDFs(asME, maxScale, pscale, rndmPtr); // Add integral of DGLAP shifted PDF ratios from \alpha_s expansion to wt. nWeight += (fixpdf) ? wP : 0.; } wt += nWeight/double(NTRIAL); // If O(\alpha_s^1)-term + O(\alpha_s^1)-term is to be calculated, done. if ( order == 1 ) return wt; // So far, no calculation of O(\alpha_s^2)-term return 0.; } //-------------------------------------------------------------------------- // Function to set the state with complete scales for evolution. void History::getStartingConditions( const double RN, Event& outState ) { // Select the history History * selected = select(RN); // Set scales in the states to the scales pythia would have set selected->setScalesInHistory(); // Copy the output state outState = state; // Set the scale of the lowest order process if (!selected->mother) { int nFinal = 0; for(int i=0; i < int(outState.size()); ++i) if (outState[i].isFinal()) nFinal++; if (nFinal <=2) outState.scale(mergingHooksPtr->muF()); // Save information on last splitting, to allow the next // emission in the shower to have smaller rapidity with // respect to the last ME splitting // For hard process, use dummy values if (mergingHooksPtr->getNumberOfClusteringSteps(state) == 0) { infoPtr->zNowISR(0.5); infoPtr->pT2NowISR(pow(state[0].e(),2)); infoPtr->hasHistory(true); // For incomplete process, try to use real values } else { infoPtr->zNowISR(selected->zISR()); infoPtr->pT2NowISR(pow(selected->pTISR(),2)); infoPtr->hasHistory(true); } } else { // Save information on last splitting, to allow the next // emission in the shower to have smaller rapidity with // respect to the last ME splitting infoPtr->zNowISR(selected->zISR()); infoPtr->pT2NowISR(pow(selected->pTISR(),2)); infoPtr->hasHistory(true); } // Save MPI starting scale if (mergingHooksPtr->getNumberOfClusteringSteps(state) == 0) mergingHooksPtr->muMI(infoPtr->eCM()); else mergingHooksPtr->muMI(outState.scale()); } //-------------------------------------------------------------------------- // Function to print the history that would be chosen from the number RN. void History::printHistory( const double RN ) { History * selected = select(RN); selected->printStates(); // Done } //-------------------------------------------------------------------------- // Function to print the states in a history, starting from the hard process. void History::printStates() { if ( !mother ) { state.list(); return; } // Print. state.list(); // Recurse mother->printStates(); // Done return; } //-------------------------------------------------------------------------- // Function to set the state with complete scales for evolution. bool History::getClusteredEvent( const double RN, int nSteps, Event& outState) { // Select history History * selected = select(RN); // Set scales in the states to the scales pythia would have set // (Only needed if not done before in calculation of weights or // setting of starting conditions) selected->setScalesInHistory(); // If the history does not allow for nSteps clusterings (e.g. because the // history is incomplete), return false if (nSteps > selected->nClusterings()) return false; // Return event with nSteps-1 additional partons (i.e. recluster the last // splitting) and copy the output state outState = selected->clusteredState(nSteps-1); // Done. return true; } //-------------------------------------------------------------------------- bool History::getFirstClusteredEventAboveTMS( const double RN, int nDesired, Event& process, int& nPerformed, bool doUpdate ) { // Do reclustering (looping) steps. Remember process scale. int nTried = nDesired - 1; // Get number of clustering steps. int nSteps = select(RN)->nClusterings(); // Set scales in the states to the scales pythia would have set. select(RN)->setScalesInHistory(); // Recluster until reclustered event is above the merging scale. Event dummy = Event(); do { // Initialise temporary output of reclustering. dummy.clear(); dummy.init( "(hard process-modified)", particleDataPtr ); dummy.clear(); // Recluster once more. nTried++; // If reclustered event does not exist, exit. if ( !getClusteredEvent( RN, nSteps-nTried+1, dummy ) ) return false; if ( nTried >= nSteps ) break; // Continue loop if reclustered event has unresolved partons. } while ( mergingHooksPtr->rhoms( dummy, false) < mergingHooksPtr->tms() ); // Update the hard process. if ( doUpdate ) process = dummy; // Failed to produce output state. if ( nTried > nSteps ) return false; nPerformed = nTried; if ( doUpdate ) { // Update to the actual number of steps. mergingHooksPtr->nReclusterSave = nPerformed; // Save MPI starting scale if (mergingHooksPtr->getNumberOfClusteringSteps(state) == 0) mergingHooksPtr->muMI(infoPtr->eCM()); else mergingHooksPtr->muMI(state.scale()); } // Done return true; } //-------------------------------------------------------------------------- // Calculate and return pdf ratio. double History::getPDFratio( int side, bool forSudakov, bool useHardPDFs, int flavNum, double xNum, double muNum, int flavDen, double xDen, double muDen) { // Do nothing for e+e- beams if ( abs(flavNum) > 10 && flavNum != 21 ) return 1.0; if ( abs(flavDen) > 10 && flavDen != 21 ) return 1.0; // Now calculate PDF ratio if necessary double pdfRatio = 1.0; // Get mother and daughter pdfs double pdfNum = 0.0; double pdfDen = 0.0; // Use hard process PDFs (i.e. PDFs NOT used in ISR, FSR or MPI). if ( useHardPDFs ) { if (side == 1) { if (forSudakov) pdfNum = mother->beamA.xfHard( flavNum, xNum, muNum*muNum); else pdfNum = beamA.xfHard( flavNum, xNum, muNum*muNum); if (forSudakov) pdfDen = max(1e-10, beamA.xfHard( flavDen, xDen, muDen*muDen)); else pdfDen = max(1e-10, beamA.xfHard( flavDen, xDen, muDen*muDen)); } else { if (forSudakov) pdfNum = mother->beamB.xfHard( flavNum, xNum, muNum*muNum); else pdfNum = beamB.xfHard( flavNum, xNum, muNum*muNum); if (forSudakov) pdfDen = max(1e-10,beamB.xfHard( flavDen, xDen, muDen*muDen)); else pdfDen = max(1e-10,beamB.xfHard( flavDen, xDen, muDen*muDen)); } // Use rescaled PDFs in the presence of multiparton interactions } else { if (side == 1) { if (forSudakov) pdfNum = mother->beamA.xfISR(0, flavNum, xNum, muNum*muNum); else pdfNum = beamA.xfISR(0, flavNum, xNum, muNum*muNum); if (forSudakov) pdfDen = max(1e-10, beamA.xfISR(0, flavDen, xDen, muDen*muDen)); else pdfDen = max(1e-10, beamA.xfISR(0, flavDen, xDen, muDen*muDen)); } else { if (forSudakov) pdfNum = mother->beamB.xfISR(0, flavNum, xNum, muNum*muNum); else pdfNum = beamB.xfISR(0, flavNum, xNum, muNum*muNum); if (forSudakov) pdfDen = max(1e-10,beamB.xfISR(0, flavDen, xDen, muDen*muDen)); else pdfDen = max(1e-10,beamB.xfISR(0, flavDen, xDen, muDen*muDen)); } } // Return ratio of pdfs if ( pdfNum > 1e-15 && pdfDen > 1e-10 ) { pdfRatio *= pdfNum / pdfDen; } else if ( pdfNum < pdfDen ) { pdfRatio = 0.; } else if ( pdfNum > pdfDen ) { pdfRatio = 1.; } // Done return pdfRatio; } //-------------------------------------------------------------------------- /*--------------- METHODS USED FOR ONLY ONE PATH OF HISTORY NODES ------- */ // Function to set all scales in the sequence of states. This is a // wrapper routine for setScales and setEventScales methods void History::setScalesInHistory() { // Find correct links from n+1 to n states (mother --> child), as // needed for enforcing ordered scale sequences vector ident; findPath(ident); // Set production scales in the states to the scales pythia would // have set and enforce ordering setScales(ident,true); // Set the overall event scales to the scale of the last branching setEventScales(); } //-------------------------------------------------------------------------- // Function to find the index (in the mother histories) of the // child history, thus providing a way access the path from both // initial history (mother == 0) and final history (all children == 0) // IN vector : The index of each child in the children vector // of the current history node will be saved in // this vector // NO OUTPUT void History::findPath(vector& out) { // If the initial and final nodes are identical, return if (!mother && int(children.size()) < 1) return; // Find the child by checking the children vector for the perfomed // clustering int iChild=-1; if ( mother ) { int size = int(mother->children.size()); // Loop through children and identify child chosen for ( int i=0; i < size; ++i) { if ( mother->children[i]->scale == scale && mother->children[i]->prob == prob && equalClustering(mother->children[i]->clusterIn,clusterIn)) { iChild = i; break; } } // Save the index of the child in the children vector and recurse if (iChild >-1) out.push_back(iChild); mother->findPath(out); } } //-------------------------------------------------------------------------- // Functions to set the parton production scales and enforce // ordering on the scales of the respective clusterings stored in // the History node: // Method will start from lowest multiplicity state and move to // higher states, setting the production scales the shower would // have used. // When arriving at the highest multiplicity, the method will switch // and go back in direction of lower states to check and enforce // ordering for unordered histories. // IN vector : Vector of positions of the chosen child // in the mother history to allow to move // in direction initial->final along path // bool : True: Move in direction low->high // multiplicity and set production scales // False: Move in direction high->low // multiplicity and check and enforce // ordering // NO OUTPUT void History::setScales( vector index, bool forward) { // First, set the scales of the hard process to the kinematial // limit (=s) if ( children.empty() && forward ) { // New "incomplete" configurations showered from mu if (!mother) { double scaleNew = 1.; if (mergingHooksPtr->incompleteScalePrescip()==0) { scaleNew = mergingHooksPtr->muF(); } else if (mergingHooksPtr->incompleteScalePrescip()==1) { Vec4 pOut; pOut.p(0.,0.,0.,0.); for(int i=0; iincompleteScalePrescip()==2) { scaleNew = state[0].e(); } scaleNew = max( mergingHooksPtr->pTcut(), scaleNew); state.scale(scaleNew); for(int i=3; i < int(state.size());++i) if (state[i].colType() != 0) state[i].scale(scaleNew); } else { // 2->2 with non-parton particles showered from eCM state.scale( state[0].e() ); // Count final partons bool isLEP = ( state[3].isLepton() && state[4].isLepton() ); int nFinal = 0; int nFinalPartons = 0; int nFinalPhotons = 0; for ( int i=0; i < int(state.size()); ++i ) { if ( state[i].isFinal() ) { nFinal++; if ( state[i].colType() != 0 ) nFinalPartons++; if ( state[i].id() == 22 ) nFinalPhotons++; } } bool isQCD = ( nFinal == 2 && nFinal == nFinalPartons ); bool isPPh = ( nFinal == 2 && nFinalPartons == 1 && nFinalPhotons == 1); // If 2->2, purely partonic, set event scale to kinematic pT if ( !isLEP && ( isQCD || isPPh ) ) state.scale( hardFacScale(state) ); } } // Set all particle production scales, starting from lowest // multiplicity (final) state if (mother && forward) { // When choosing splitting scale, beware of unordered splittings: double scaleNew = 1.; if (mergingHooksPtr->unorderedScalePrescip() == 0) { // Use larger scale as common splitting scale for mother and child scaleNew = max( mergingHooksPtr->pTcut(), max(scale,mother->scale)); } else if (mergingHooksPtr->unorderedScalePrescip() == 1) { // Use smaller scale as common splitting scale for mother and child if (scale < mother->scale) scaleNew *= max( mergingHooksPtr->pTcut(), min(scale,mother->scale)); else scaleNew *= max( mergingHooksPtr->pTcut(), max(scale,mother->scale)); } // Rescale the mother state partons to the clustering scales // that have been found along the path mother->state[clusterIn.emitted].scale(scaleNew); mother->state[clusterIn.emittor].scale(scaleNew); mother->state[clusterIn.recoiler].scale(scaleNew); // Find unchanged copies of partons in higher multiplicity states // and rescale those mother->scaleCopies(clusterIn.emitted, mother->state, scaleNew); mother->scaleCopies(clusterIn.emittor, mother->state, scaleNew); mother->scaleCopies(clusterIn.recoiler, mother->state, scaleNew); // Recurse mother->setScales(index,true); } // Now, check and correct ordering from the highest multiplicity // state backwards to all the clustered states if (!mother || !forward) { // Get index of child along the path int iChild = -1; if ( int(index.size()) > 0 ) { iChild = index.back(); index.pop_back(); } // Check that the reclustered scale is above the shower cut if (mother) { scale = max(mergingHooksPtr->pTcut(), scale); } // If this is NOT the 2->2 process, check and enforce ordering if (iChild != -1 && !children.empty()) { if (scale > children[iChild]->scale ) { if (mergingHooksPtr->unorderedScalePrescip() == 0) { // Use larger scale as common splitting scale for mother and child double scaleNew = max( mergingHooksPtr->pTcut(), max(scale,children[iChild]->scale)); // Enforce ordering in particle production scales for( int i = 0; i < int(children[iChild]->state.size()); ++i) if (children[iChild]->state[i].scale() == children[iChild]->scale) children[iChild]->state[i].scale(scaleNew); // Enforce ordering in saved clustering scale children[iChild]->scale = scaleNew; } else if ( mergingHooksPtr->unorderedScalePrescip() == 1) { // Use smaller scale as common splitting scale for mother & child double scaleNew = max(mergingHooksPtr->pTcut(), min(scale,children[iChild]->scale)); // Enforce ordering in particle production scales for( int i = 0; i < int(state.size()); ++i) if (state[i].scale() == scale) state[i].scale(scaleNew); // Enforce ordering in saved clustering scale scale = scaleNew; } // Just set the overall event scale to the minimal scale } else { double scalemin = state[0].e(); for( int i = 0; i < int(state.size()); ++i) if (state[i].colType() != 0) scalemin = max(mergingHooksPtr->pTcut(), min(scalemin,state[i].scale())); state.scale(scalemin); scale = max(mergingHooksPtr->pTcut(), scale); } //Recurse children[iChild]->setScales(index, false); } } } //-------------------------------------------------------------------------- // Function to find a particle in all higher multiplicity events // along the history path and set its production scale to the input // scale // IN int iPart : Parton in refEvent to be checked / rescaled // Event& refEvent : Reference event for iPart // double scale : Scale to be set as production scale for // unchanged copies of iPart in subsequent steps void History::scaleCopies(int iPart, const Event& refEvent, double rho) { // Check if any parton recently rescaled is found unchanged: // Same charge, colours in mother->state if ( mother ) { for( int i=0; i < mother->state.size(); ++i) { if ( ( mother->state[i].id() == refEvent[iPart].id() && mother->state[i].colType() == refEvent[iPart].colType() && mother->state[i].chargeType() == refEvent[iPart].chargeType() && mother->state[i].col() == refEvent[iPart].col() && mother->state[i].acol() == refEvent[iPart].acol() ) ) { // Rescale the unchanged parton mother->state[i].scale(rho); // Recurse if (mother->mother) mother->scaleCopies( iPart, refEvent, rho ); } // end if found unchanged parton case } // end loop over particle entries in event } } //-------------------------------------------------------------------------- // Functions to set the OVERALL EVENT SCALES [=state.scale()] to // the scale of the last clustering // NO INPUT // NO OUTPUT void History::setEventScales() { // Set the event scale to the scale of the last clustering, // except for the very lowest multiplicity state if (mother) { mother->state.scale(scale); // Recurse mother->setEventScales(); } } //-------------------------------------------------------------------------- // Functions to return the z value of the last ISR splitting // NO INPUT // OUTPUT double : z value of last ISR splitting in history double History::zISR() { // Do nothing for ME level state if (!mother) return 0.0; // Skip FSR splitting if (mother->state[clusterIn.emittor].isFinal()) return mother->zISR(); // Calculate z int rad = clusterIn.emittor; int rec = clusterIn.recoiler; int emt = clusterIn.emitted; double z = (mother->state[rad].p() + mother->state[rec].p() - mother->state[emt].p()).m2Calc() / (mother->state[rad].p() + mother->state[rec].p()).m2Calc(); // Recurse double znew = mother->zISR(); // Update z if (znew > 0.) z = znew; return z; } //-------------------------------------------------------------------------- // Functions to return the z value of the last FSR splitting // NO INPUT // OUTPUT double : z value of last FSR splitting in history double History::zFSR() { // Do nothing for ME level state if (!mother) return 0.0; // Skip ISR splitting if (!mother->state[clusterIn.emittor].isFinal()) return mother->zFSR(); // Calculate z int rad = clusterIn.emittor; int rec = clusterIn.recoiler; int emt = clusterIn.emitted; // Construct 2->3 variables for FSR Vec4 sum = mother->state[rad].p() + mother->state[rec].p() + mother->state[emt].p(); double m2Dip = sum.m2Calc(); double x1 = 2. * (sum * mother->state[rad].p()) / m2Dip; double x3 = 2. * (sum * mother->state[emt].p()) / m2Dip; // Calculate z of splitting for FSR double z = x1/(x1+x3); // Recurse double znew = mother->zFSR(); // Update z if (znew > 0.) z = znew; return z; } //-------------------------------------------------------------------------- // Functions to return the pT scale of the last FSR splitting // NO INPUT // OUTPUT double : pT scale of last FSR splitting in history double History::pTISR() { // Do nothing for ME level state if (!mother) return 0.0; // Skip FSR splitting if (mother->state[clusterIn.emittor].isFinal()) return mother->pTISR(); double pT = mother->state.scale(); // Recurse double pTnew = mother->pTISR(); // Update pT if (pTnew > 0.) pT = pTnew; return pT; } //-------------------------------------------------------------------------- // Functions to return the pT scale of the last FSR splitting // NO INPUT // OUTPUT double : pT scale of last FSR splitting in history double History::pTFSR() { // Do nothing for ME level state if (!mother) return 0.0; // Skip ISR splitting if (!mother->state[clusterIn.emittor].isFinal()) return mother->pTFSR(); double pT = mother->state.scale(); // Recurse double pTnew = mother->pTFSR(); // Update pT if (pTnew > 0.) pT = pTnew; return pT; } //-------------------------------------------------------------------------- // Function to return the depth of the history (i.e. the number of // reclustered splittings) // NO INPUT // OUTPUT int : Depth of history int History::nClusterings() { if (!mother) return 0; int w = mother->nClusterings(); w += 1; return w; } //-------------------------------------------------------------------------- // Functions to return the event after nSteps splittings of the 2->2 process // Example: nSteps = 1 -> return event with one additional parton // INPUT int : Number of splittings in the event, // as counted from core 2->2 process // OUTPUT Event : event with nSteps additional partons Event History::clusteredState(int nSteps) { // Save state Event outState = state; // As long as there are steps to do, recursively save state if (mother && nSteps > 0) outState = mother->clusteredState(nSteps - 1); // Done return outState; } //-------------------------------------------------------------------------- // Function to choose a path from all paths in the tree // according to their splitting probabilities // IN double : Random number // OUT History* : Leaf of history path chosen History * History::select(double rnd) { // No need to choose if no paths have been constructed. if ( goodBranches.empty() && badBranches.empty() ) return this; // Choose amongst paths allowed by projections. double sum = 0.; map selectFrom; if ( !goodBranches.empty() ) { selectFrom = goodBranches; sum = sumGoodBranches; } else { selectFrom = badBranches; sum = sumBadBranches; } if (mergingHooksPtr->pickBySumPT()) { // Find index of history with minimal sum of scalar pT int nFinal = 0; for (int i=0; i < state.size(); ++i) if (state[i].isFinal()) nFinal++; double iMin = 0.; double sumMin = (nFinal-2)*state[0].e(); for ( map::iterator it = selectFrom.begin(); it != selectFrom.end(); ++it ) { if (it->second->sumScalarPT < sumMin) { sumMin = it->second->sumScalarPT; iMin = it->first; } } // Choose history with smallest sum of scalar pT return selectFrom.lower_bound(iMin)->second; } else { // Choose history according to probability, be careful about upper bound if ( rnd != 1. ) { return selectFrom.upper_bound(sum*rnd)->second; } else { return selectFrom.lower_bound(sum*rnd)->second; } } // Done } //-------------------------------------------------------------------------- // Function to project paths onto desired paths. bool History::trimHistories() { // Do nothing if no paths have been constructed. if ( paths.empty() ) return false; // Loop through all constructed paths. Check all removal conditions. for ( map::iterator it = paths.begin(); it != paths.end(); ++it ) { // Check if history is allowed. if ( it->second->keep() && !it->second->keepHistory() ) it->second->remove(); } // Project onto desired / undesired branches. double sumold, sumnew, sumprob, mismatch; sumold = sumnew = sumprob = mismatch = 0.; // Loop through all constructed paths and store allowed paths. // Skip undesired paths. for ( map::iterator it = paths.begin(); it != paths.end(); ++it ) { // Update index sumnew = it->first; if ( it->second->keep() ) { // Fill branches with allowed paths. goodBranches.insert( make_pair( sumnew - mismatch, it->second) ); // Add probability of this path. sumGoodBranches = sumnew - mismatch; } else { // Update mismatch in probabilities resulting from not including this // path double mismatchOld = mismatch; mismatch += sumnew - sumold; // Fill branches with allowed paths. badBranches.insert( make_pair( mismatchOld + sumnew - sumold, it->second ) ); // Add probability of this path. sumBadBranches = mismatchOld + sumnew - sumold; } // remember index of this path in order to caclulate probability of // subsequent path. sumold = it->first; } // Done return !goodBranches.empty(); } //-------------------------------------------------------------------------- // Function implementing checks on a paths, deciding if the path is valid. bool History::keepHistory() { bool keepPath = true; // Tag unordered paths for removal. if ( mergingHooksPtr->getProcessString().compare("pp>jj") == 0 || mergingHooksPtr->getProcessString().compare("pp>aj") == 0 ) { // Tag unordered paths for removal. Include scale of hard 2->2 process // into the ordering definition. double maxScale = hardFacScale(state); keepPath = isOrderedPath( maxScale ); } //Done return keepPath; } //-------------------------------------------------------------------------- // Function to check if a path is ordered in evolution pT. bool History::isOrderedPath( double maxscale ) { double newscale = clusterIn.pT(); if ( !mother ) return true; bool ordered = mother->isOrderedPath(newscale); if ( !ordered || maxscale < newscale) return false; return ordered; } //-------------------------------------------------------------------------- // Function to check if all reconstucted states in a path pass the merging // scale cut. bool History::allIntermediateAboveRhoMS( double rhoms, bool good ) { // If one state below the merging scale has already been found, no need to // check further. if ( !good ) return false; // Check merging scale for states with more than 0 jets int nFinal = 0; for ( int i = 0; i < state.size(); ++i ) if ( state[i].isFinal() && state[i].colType() != 0 ) nFinal++; double rhoNew = (nFinal > 0 ) ? mergingHooksPtr->rhoms( state, false ) : state[0].e(); // Assume state from ME generator passes merging scale cut. if ( !mother ) return good; // Recurse. return good && mother->allIntermediateAboveRhoMS( rhoms, (rhoNew > rhoms) ); } //-------------------------------------------------------------------------- // Function to check if any ordered paths were found (and kept). bool History::foundAnyOrderedPaths() { //Do nothing if no paths were found if ( paths.empty() ) return false; double maxscale = infoPtr->eCM(); // Loop through paths. Divide probability into ordered and unordered pieces. for ( map::iterator it = paths.begin(); it != paths.end(); ++it ) if ( it->second->isOrderedPath(maxscale) ) return true; // Done return false; } //-------------------------------------------------------------------------- // For a full path, find the weight calculated from the ratio of // couplings, the no-emission probabilities, and possible PDF // ratios. This function should only be called for the last history // node of a full path. // IN TimeShower : Already initialised shower object to be used as // trial shower // double : alpha_s value used in ME calculation // double : Maximal mass scale of the problem (e.g. E_CM) // AlphaStrong: Initialised shower alpha_s object for FSR // alpha_s ratio calculation // AlphaStrong: Initialised shower alpha_s object for ISR // alpha_s ratio calculation (can be different from previous) double History::weightTree(PartonLevel* trial, double as0, double maxscale, double pdfScale, AlphaStrong * asFSR, AlphaStrong * asISR, double& asWeight, double& pdfWeight) { // Use correct scale double newScale = scale; // For ME state, just multiply by PDF ratios if ( !mother ) { int sideRad = (state[3].pz() > 0) ? 1 :-1; int sideRec = (state[4].pz() > 0) ? 1 :-1; // Calculate PDF first leg if (state[3].colType() != 0) { // Find x value and flavour double x = 2.*state[3].e() / state[0].e(); int flav = state[3].id(); // Find numerator/denominator scale double scaleNum = (children.empty()) ? hardFacScale(state) : maxscale; double scaleDen = mergingHooksPtr->muFinME(); // For initial parton, multiply by PDF ratio double ratio = getPDFratio(sideRad, false, false, flav, x, scaleNum, flav, x, scaleDen); pdfWeight *= ratio; } // Calculate PDF ratio for second leg if (state[4].colType() != 0) { // Find x value and flavour double x = 2.*state[4].e() / state[0].e(); int flav = state[4].id(); // Find numerator/denominator scale double scaleNum = (children.empty()) ? hardFacScale(state) : maxscale; double scaleDen = mergingHooksPtr->muFinME(); // For initial parton, multiply with PDF ratio double ratio = getPDFratio(sideRec, false, false, flav, x, scaleNum, flav, x, scaleDen); pdfWeight *= ratio; } return 1.0; } // Remember new PDF scale n case true sclae should be used for un-ordered // splittings. double newPDFscale = newScale; if (mergingHooksPtr->unorderedPDFscalePrescip() == 1) newPDFscale = clusterIn.pT(); // Recurse double w = mother->weightTree(trial, as0, newScale, newPDFscale, asFSR, asISR, asWeight, pdfWeight); // Do nothing for empty state if (state.size() < 3) return 1.0; // If up to now, trial shower was not successful, return zero if ( w < 1e-12 ) return 0.0; // Do trial shower on current state, return zero if not successful w *= doTrialShower(trial, 1, maxscale); if ( w < 1e-12 ) return 0.0; // Calculate alpha_s ratio for current state if ( asFSR && asISR ) { double asScale = pow2( newScale ); if (mergingHooksPtr->unorderedASscalePrescip() == 1) asScale = pow2( clusterIn.pT() ); bool FSR = mother->state[clusterIn.emittor].isFinal(); double alphaSinPS = (FSR) ? (*asFSR).alphaS(asScale) : (*asISR).alphaS(asScale + pow2(mergingHooksPtr->pT0ISR()) ); asWeight *= alphaSinPS / as0; } // Calculate pdf ratios: Get both sides of event int inP = 3; int inM = 4; int sideP = (mother->state[inP].pz() > 0) ? 1 :-1; int sideM = (mother->state[inM].pz() > 0) ? 1 :-1; if ( mother->state[inP].colType() != 0 ) { // Find x value and flavour double x = getCurrentX(sideP); int flav = getCurrentFlav(sideP); // Find numerator scale double scaleNum = (children.empty()) ? hardFacScale(state) : ( (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? pdfScale : maxscale ); double scaleDen = (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? clusterIn.pT() : newScale; // Multiply PDF ratio double ratio = getPDFratio(sideP, false, false, flav, x, scaleNum, flav, x, scaleDen); pdfWeight *= ratio; } if ( mother->state[inM].colType() != 0 ) { // Find x value and flavour double x = getCurrentX(sideM); int flav = getCurrentFlav(sideM); // Find numerator scale double scaleNum = (children.empty()) ? hardFacScale(state) : ( (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? pdfScale : maxscale ); double scaleDen = (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? clusterIn.pT() : newScale; // Multiply PDF ratio double ratio = getPDFratio(sideM, false, false, flav, x, scaleNum, flav, x, scaleDen); pdfWeight *= ratio; } // Done return w; } //-------------------------------------------------------------------------- // Function to return the \alpha_s-ratio part of the CKKWL weight of a path. double History::weightTreeALPHAS( double as0, AlphaStrong * asFSR, AlphaStrong * asISR ) { // For ME state, do nothing. if ( !mother ) return 1.; // Recurse double w = mother->weightTreeALPHAS( as0, asFSR, asISR ); // Do nothing for empty state if (state.size() < 3) return w; // Calculate alpha_s ratio for current state if ( asFSR && asISR ) { double asScale = pow2( scale ); if (mergingHooksPtr->unorderedASscalePrescip() == 1) asScale = pow2( clusterIn.pT() ); bool FSR = mother->state[clusterIn.emittor].isFinal(); double alphaSinPS = (FSR) ? (*asFSR).alphaS(asScale) : (*asISR).alphaS(asScale + pow2(mergingHooksPtr->pT0ISR()) ); w *= alphaSinPS / as0; } // Done return w; } //-------------------------------------------------------------------------- // Function to return the PDF-ratio part of the CKKWL weight of a path. double History::weightTreePDFs( double maxscale, double pdfScale ) { // Use correct scale double newScale = scale; // For ME state, just multiply by PDF ratios if ( !mother ) { double wt = 1.; int sideRad = (state[3].pz() > 0) ? 1 :-1; int sideRec = (state[4].pz() > 0) ? 1 :-1; // Calculate PDF first leg if (state[3].colType() != 0) { // Find x value and flavour double x = 2.*state[3].e() / state[0].e(); int flav = state[3].id(); // Find numerator/denominator scale double scaleNum = (children.empty()) ? hardFacScale(state) : maxscale; double scaleDen = mergingHooksPtr->muFinME(); // For initial parton, multiply by PDF ratio wt *= getPDFratio(sideRad, false, false, flav, x, scaleNum, flav, x, scaleDen); } // Calculate PDF ratio for second leg if (state[4].colType() != 0) { // Find x value and flavour double x = 2.*state[4].e() / state[0].e(); int flav = state[4].id(); // Find numerator/denominator scale double scaleNum = (children.empty()) ? hardFacScale(state) : maxscale; double scaleDen = mergingHooksPtr->muFinME(); // For initial parton, multiply with PDF ratio wt *= getPDFratio(sideRec, false, false, flav, x, scaleNum, flav, x, scaleDen); } return wt; } // Remember new PDF scale n case true sclae should be used for un-ordered // splittings. double newPDFscale = newScale; if ( mergingHooksPtr->unorderedPDFscalePrescip() == 1) newPDFscale = clusterIn.pT(); // Recurse double w = mother->weightTreePDFs( newScale, newPDFscale ); // Do nothing for empty state if (state.size() < 3) return w; // Calculate pdf ratios: Get both sides of event int inP = 3; int inM = 4; int sideP = (mother->state[inP].pz() > 0) ? 1 :-1; int sideM = (mother->state[inM].pz() > 0) ? 1 :-1; if ( mother->state[inP].colType() != 0 ) { // Find x value and flavour double x = getCurrentX(sideP); int flav = getCurrentFlav(sideP); // Find numerator scale double scaleNum = (children.empty()) ? hardFacScale(state) : ( (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? pdfScale : maxscale ); double scaleDen = (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? clusterIn.pT() : newScale; // Multiply PDF ratio double ratio = getPDFratio(sideP, false, false, flav, x, scaleNum, flav, x, scaleDen); w *= ratio; } if ( mother->state[inM].colType() != 0 ) { // Find x value and flavour double x = getCurrentX(sideM); int flav = getCurrentFlav(sideM); // Find numerator scale double scaleNum = (children.empty()) ? hardFacScale(state) : ( (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? pdfScale : maxscale ); double scaleDen = (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? clusterIn.pT() : newScale; // Multiply PDF ratio double ratio = getPDFratio(sideM, false, false, flav, x, scaleNum, flav, x, scaleDen); w *= ratio; } // Done return w; } //-------------------------------------------------------------------------- // Function to return the no-emission probability part of the CKKWL weight. double History::weightTreeEmissions( PartonLevel* trial, int type, int njetMax, double maxscale ) { // Use correct scale double newScale = scale; // For ME state, just multiply by PDF ratios if ( !mother ) return 1.0; // Recurse double w = mother->weightTreeEmissions( trial, type, njetMax, newScale ); // Do nothing for empty state if (state.size() < 3) return 1.0; // If up to now, trial shower was not successful, return zero if ( w < 1e-12 ) return 0.0; // If this node has too many jets, no not calculate no-emission probability. int njetNow = mergingHooksPtr->getNumberOfClusteringSteps( state) ; if (njetNow >= njetMax) return 1.0; // Do trial shower on current state, return zero if not successful w *= doTrialShower(trial, type, maxscale); if ( w < 1e-12 ) return 0.0; // Done return w; } //-------------------------------------------------------------------------- // Function to generate the O(\alpha_s)-term of the CKKWL-weight. double History::weightFirst(PartonLevel* trial, double as0, double muR, double maxscale, AlphaStrong * asFSR, AlphaStrong * asISR, Rndm* rndmPtr ) { // Use correct scale double newScale = scale; if ( !mother ) { double weight = 0.; // Calculate PDF first leg if (state[3].colType() != 0) { // Find x value and flavour double x = 2.*state[3].e() / state[0].e(); int flav = state[3].id(); // Find numerator/denominator scale double scaleNum = (children.empty()) ? hardFacScale(state) : maxscale; double scaleDen = mergingHooksPtr->muFinME(); // Monte Carlo integrand. double intPDF4 = monteCarloPDFratios(flav, x, scaleNum, scaleDen, mergingHooksPtr->muFinME(), as0, rndmPtr); weight += intPDF4; } // Calculate PDF ratio for second leg if (state[4].colType() != 0) { // Find x value and flavour double x = 2.*state[4].e() / state[0].e(); int flav = state[4].id(); // Find numerator/denominator scale double scaleNum = (children.empty()) ? hardFacScale(state) : maxscale; double scaleDen = mergingHooksPtr->muFinME(); // Monte Carlo integrand. double intPDF4 = monteCarloPDFratios(flav, x, scaleNum, scaleDen, mergingHooksPtr->muFinME(), as0, rndmPtr); weight += intPDF4; } return weight; } // Recurse double w = mother->weightFirst(trial, as0, muR, newScale, asFSR, asISR, rndmPtr ); // Do nothing for empty state if (state.size() < 3) return 0.0; // Find right scale double b = 1.; double asScale2 = newScale*newScale; int showerType = (mother->state[clusterIn.emittor].isFinal() ) ? 1 : -1; if (showerType == -1) { asScale2 += pow(mergingHooksPtr->pT0ISR(),2); b = 1.; } // Find summand beta_0 / 2 * ln(muR^2/t_i) due to as expansion. double NF = 4.; double BETA0 = 11. - 2./3.* NF; // For fixed \alpha_s in matrix element w += as0 / (2.*M_PI) * 0.5 * BETA0 * log( (muR*muR) / (b*asScale2) ); // Count emissions: New variant // Generate true average, not only one-point. bool fixpdf = true; bool fixas = true; double nWeight1 = 0.; double nWeight2 = 0.; for(int i=0; i < NTRIAL; ++i) { // Get number of emissions vector unresolvedEmissionTerm = countEmissions(trial, maxscale, newScale, 2, as0, asFSR, asISR, 3, fixpdf, fixas); nWeight1 += unresolvedEmissionTerm[1]; } w += nWeight1/double(NTRIAL) + nWeight2/double(NTRIAL); // Calculate pdf ratios: Get both sides of event int inP = 3; int inM = 4; int sideP = (mother->state[inP].pz() > 0) ? 1 :-1; int sideM = (mother->state[inM].pz() > 0) ? 1 :-1; if ( mother->state[inP].colType() != 0 ) { // Find x value and flavour double x = getCurrentX(sideP); int flav = getCurrentFlav(sideP); // Find numerator scale double scaleNum = (children.empty()) ? hardFacScale(state) : maxscale; // Monte Carlo integrand. double intPDF4 = monteCarloPDFratios(flav, x, scaleNum, newScale, mergingHooksPtr->muFinME(), as0, rndmPtr); w += intPDF4; } if ( mother->state[inM].colType() != 0 ) { // Find x value and flavour double x = getCurrentX(sideM); int flav = getCurrentFlav(sideM); // Find numerator scale double scaleNum = (children.empty()) ? hardFacScale(state) : maxscale; // Monte Carlo integrand. double intPDF4 = monteCarloPDFratios(flav, x, scaleNum, newScale, mergingHooksPtr->muFinME(), as0, rndmPtr); w += intPDF4; } // Done return w; } //-------------------------------------------------------------------------- // Function to generate the O(\alpha_s)-term of the \alpha_s-ratios // appearing in the CKKWL-weight. double History::weightFirstALPHAS( double as0, double muR, AlphaStrong * asFSR, AlphaStrong * asISR ) { // Use correct scale double newScale = scale; // Done if ( !mother ) return 0.; // Recurse double w = mother->weightFirstALPHAS( as0, muR, asFSR, asISR ); // Find right scale int showerType = (mother->state[clusterIn.emittor].isFinal() ) ? 1 : -1; double b = 1.; double asScale = pow2( newScale ); if ( mergingHooksPtr->unorderedASscalePrescip() == 1 ) asScale = pow2( clusterIn.pT() ); if (showerType == -1) { asScale += pow2( mergingHooksPtr->pT0ISR() ); b = 1.; } // Find summand beta_0 / 2 * ln(muR^2/t_i) due to as expansion. double NF = 4.; double BETA0 = 11. - 2./3.* NF; // For fixed \alpha_s in matrix element w += as0 / (2.*M_PI) * 0.5 * BETA0 * log( (muR*muR) / (b*asScale) ); // Done return w; } //-------------------------------------------------------------------------- // Function to generate the O(\alpha_s)-term of the PDF-ratios // appearing in the CKKWL-weight. double History::weightFirstPDFs( double as0, double maxscale, double pdfScale, Rndm* rndmPtr ) { // Use correct scale double newScale = scale; if ( !mother ) { double wt = 0.; // Calculate PDF first leg if (state[3].colType() != 0) { // Find x value and flavour double x = 2.*state[3].e() / state[0].e(); int flav = state[3].id(); // Find numerator/denominator scale double scaleNum = (children.empty()) ? hardFacScale(state) : maxscale; double scaleDen = mergingHooksPtr->muFinME(); // Monte Carlo integrand. wt += monteCarloPDFratios(flav, x, scaleNum, scaleDen, mergingHooksPtr->muFinME(), as0, rndmPtr); } // Calculate PDF ratio for second leg if (state[4].colType() != 0) { // Find x value and flavour double x = 2.*state[4].e() / state[0].e(); int flav = state[4].id(); // Find numerator/denominator scale double scaleNum = (children.empty()) ? hardFacScale(state) : maxscale; double scaleDen = mergingHooksPtr->muFinME(); // Monte Carlo integrand. wt += monteCarloPDFratios(flav, x, scaleNum, scaleDen, mergingHooksPtr->muFinME(), as0, rndmPtr); } // Done return wt; } // Remember new PDF scale n case true sclae should be used for un-ordered // splittings. double newPDFscale = newScale; if (mergingHooksPtr->unorderedPDFscalePrescip() == 1) newPDFscale = clusterIn.pT(); // Recurse double w = mother->weightFirstPDFs( as0, newScale, newPDFscale, rndmPtr); // Calculate pdf ratios: Get both sides of event int inP = 3; int inM = 4; int sideP = (mother->state[inP].pz() > 0) ? 1 :-1; int sideM = (mother->state[inM].pz() > 0) ? 1 :-1; if ( mother->state[inP].colType() != 0 ) { // Find x value and flavour double x = getCurrentX(sideP); int flav = getCurrentFlav(sideP); // Find numerator / denominator scales double scaleNum = (children.empty()) ? hardFacScale(state) : ( (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? pdfScale : maxscale ); double scaleDen = (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? clusterIn.pT() : newScale; // Monte Carlo integrand. w += monteCarloPDFratios(flav, x, scaleNum, scaleDen, mergingHooksPtr->muFinME(), as0, rndmPtr); } if ( mother->state[inM].colType() != 0 ) { // Find x value and flavour double x = getCurrentX(sideM); int flav = getCurrentFlav(sideM); // Find numerator / denominator scales double scaleNum = (children.empty()) ? hardFacScale(state) : ( (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? pdfScale : maxscale ); double scaleDen = (mergingHooksPtr->unorderedPDFscalePrescip() == 1) ? clusterIn.pT() : newScale; // Monte Carlo integrand. w += monteCarloPDFratios(flav, x, scaleNum, scaleDen, mergingHooksPtr->muFinME(), as0, rndmPtr); } // Done return w; } //-------------------------------------------------------------------------- // Function to generate the O(\alpha_s)-term of the no-emission // probabilities appearing in the CKKWL-weight. double History::weightFirstEmissions(PartonLevel* trial, double as0, double maxscale, AlphaStrong * asFSR, AlphaStrong * asISR, bool fixpdf, bool fixas ) { // Use correct scale double newScale = scale; if ( !mother ) return 0.0; // Recurse double w = mother->weightFirstEmissions(trial, as0, newScale, asFSR, asISR, fixpdf, fixas ); // Do nothing for empty state if (state.size() < 3) return 0.0; // Generate true average. double nWeight1 = 0.; double nWeight2 = 0.; for(int i=0; i < NTRIAL; ++i) { // Get number of emissions vector unresolvedEmissionTerm = countEmissions(trial, maxscale, newScale, 2, as0, asFSR, asISR, 3, fixpdf, fixas); nWeight1 += unresolvedEmissionTerm[1]; } w += nWeight1/double(NTRIAL) + nWeight2/double(NTRIAL); // Done return w; } //-------------------------------------------------------------------------- // Function to return the factorisation scale of the hard process in Pythia. double History::hardFacScale(const Event& event) { // Declare output scale. double hardscale = 0.; // If scale should not be reset, done. if ( !mergingHooksPtr->resetHardQFac() ) return mergingHooksPtr->muF(); // For pure QCD dijet events, calculate the hadronic cross section // of the hard process at the pT of the dijet system, rather than at fixed // arbitrary scale. if ( mergingHooksPtr->getProcessString().compare("pp>jj") == 0 || mergingHooksPtr->getProcessString().compare("pp>aj") == 0 ) { // Find the mT in the hard sub-process. vector mT; for ( int i=0; i < event.size(); ++i) if ( event[i].isFinal() && event[i].colType() != 0 ) mT.push_back( abs(event[i].mT2()) ); if ( int(mT.size()) != 2 ) hardscale = infoPtr->QFac(); else hardscale = sqrt( min( mT[0], mT[1] ) ); } else { hardscale = infoPtr->QFac(); } // Done return hardscale; } //-------------------------------------------------------------------------- // Function to return the factorisation scale of the hard process in Pythia. double History::hardRenScale(const Event& event) { // Declare output scale. double hardscale = 0.; // If scale should not be reset, done. if ( !mergingHooksPtr->resetHardQRen() ) return mergingHooksPtr->muR(); // For pure QCD dijet events, calculate the hadronic cross section // of the hard process at the pT of the dijet system, rather than at fixed // arbitrary scale. if ( mergingHooksPtr->getProcessString().compare("pp>jj") == 0 || mergingHooksPtr->getProcessString().compare("pp>aj") == 0 ) { // Find the mT in the hard sub-process. vector mT; for ( int i=0; i < event.size(); ++i) if ( event[i].isFinal() && ( event[i].colType() != 0 || event[i].id() == 22 ) ) mT.push_back( abs(event[i].mT()) ); if ( int(mT.size()) != 2 ) hardscale = infoPtr->QRen(); else hardscale = sqrt( mT[0]*mT[1] ); } else { hardscale = infoPtr->QRen(); } // Done return hardscale; } //-------------------------------------------------------------------------- // Perform a trial shower using the \a pythia object between // maxscale down to this scale and return the corresponding Sudakov // form factor. // IN trialShower : Shower object used as trial shower // double : Maximum scale for trial shower branching // OUT 0.0 : trial shower emission outside allowed pT range // 1.0 : trial shower successful (any emission was below // the minimal scale ) double History::doTrialShower( PartonLevel* trial, int type, double maxscaleIn, double minscaleIn ) { // Copy state to local process Event process = state; // Set starting scale. double startingScale = maxscaleIn; // Careful when setting shower starting scale for pure QCD and prompt // photon case. if ( mergingHooksPtr->getNumberOfClusteringSteps(process) == 0 && ( mergingHooksPtr->getProcessString().compare("pp>jj") == 0 || mergingHooksPtr->getProcessString().compare("pp>aj") == 0 ) ) startingScale = min( startingScale, hardFacScale(process) ); // Set output. bool doVeto = false; while ( true ) { // Reset trialShower object trial->resetTrial(); // Construct event to be showered Event event = Event(); event.init("(hard process-modified)", particleDataPtr); event.clear(); // Reset process scale so that shower starting scale is correctly set. process.scale(startingScale); doVeto = false; // Get pT before reclustering double minScale = (minscaleIn > 0.) ? minscaleIn : scale; // If the maximal scale and the minimal scale coincide (as would // be the case for the corrected scales of unordered histories), // do not generate Sudakov if (minScale >= startingScale) break; // Find z and pT values at which the current state was formed, to // ensure that the showers can order the next emission correctly in // rapidity, if required. // NOT CORRECTLY SET FOR HIGHEST MULTIPLICITY STATE! double z = ( mergingHooksPtr->getNumberOfClusteringSteps(state) == 0 || !mother ) ? 0.5 : mother->getCurrentZ(clusterIn.emittor,clusterIn.recoiler, clusterIn.emitted); // Store z and pT values at which the current state was formed infoPtr->zNowISR(z); infoPtr->pT2NowISR(pow(startingScale,2)); infoPtr->hasHistory(true); // Perform trial shower emission trial->next(process,event); // Get trial shower pT. double pTtrial = trial->pTLastInShower(); int typeTrial = trial->typeLastInShower(); // Clear parton systems. trial->resetTrial(); // Get veto (merging) scale value double vetoScale = (mother) ? 0. : mergingHooksPtr->tms(); // Get merging scale in current event double tnow = mergingHooksPtr->tmsNow( event ); // Done if evolution scale has fallen below minimum if ( pTtrial < minScale ) break; // Reset starting scale. startingScale = pTtrial; // Continue if this state is below the veto scale if ( tnow < vetoScale && vetoScale > 0. ) continue; // Retry if the trial emission was not allowed. if ( mergingHooksPtr->canVetoTrialEmission() && mergingHooksPtr->doVetoTrialEmission( process, event) ) continue; // Only consider allowed emissions for veto: // Only allow MPI for MPI no-emission probability. if ( type == -1 && typeTrial != 1 ) continue; // Only allow ISR or FSR for radiative no-emission probability. if ( type == 1 && !(typeTrial == 2 || typeTrial >= 3) ) continue; // Veto event if trial pT was above the next nodal scale. if ( pTtrial > minScale ) doVeto = true; //// For last no-emission probability, veto event if the trial state //// is above the merging scale, i.e. in the matrix element region. //if ( !mother && tnow > vetoScale && vetoScale > 0. ) doVeto = true; // For 2 -> 2 pure QCD state, do not allow multiparton interactions // above the kinematical pT of the 2 -> 2 state. if ( type == -1 && typeTrial == 1 && mergingHooksPtr->getNumberOfClusteringSteps(process) == 0 && ( mergingHooksPtr->getProcessString().compare("pp>jj") == 0 || mergingHooksPtr->getProcessString().compare("pp>aj") == 0 ) && pTtrial > hardFacScale(process) ) return 0.0; // If pT of trial emission was in suitable range (trial shower // successful), return false if ( pTtrial < minScale ) doVeto = false; // Done break; } // Done return ( (doVeto) ? 0. : 1. ); } //-------------------------------------------------------------------------- // Assume we have a vector of i elements containing indices into // another vector with N elements. Update the indices so that all // unique combinations (starting from 0,1,2,3, ...) are // covered. Return false when all combinations have been ehausted. bool History::updateind(vector & ind, int i, int N) { if ( i < 0 ) return false; if ( ++ind[i] < N ) return true; if ( !updateind(ind, i - 1, N - 1) ) return false; ind[i] = ind[i - 1] + 1; return true; } //-------------------------------------------------------------------------- // Return the expansion of the no-emission probability up to the Nth // term. Optionally calculate the the terms using fixed alphaS // and/or PDF ratios. vector History::countEmissions(PartonLevel* trial, double maxscale, double minscale, int showerType, double as0, AlphaStrong * asFSR, AlphaStrong * asISR, int N = 1, bool fixpdf = true, bool fixas = true) { if ( N < 0 ) return vector(); vector result(N+1); result[0] = 1.0; if ( N < 1 ) return result; // Copy state to local process Event process = state; double startingScale = maxscale; // Careful when setting shower starting scale for pure QCD and prompt // photon case. if ( mergingHooksPtr->getNumberOfClusteringSteps(process) == 0 && ( mergingHooksPtr->getProcessString().compare("pp>jj") == 0 || mergingHooksPtr->getProcessString().compare("pp>aj") == 0 ) ) startingScale = min( startingScale, hardFacScale(process) ); vector wts; while ( true ) { // Reset trialShower object trial->resetTrial(); // Construct event to be showered Event event = Event(); event.init("(hard process-modified)", particleDataPtr); event.clear(); // Reset process scale process.scale(startingScale); // If the maximal scale and the minimal scale coincide (as would // be the case for the corrected scales of unordered histories), // do not generate Sudakov if (minscale >= startingScale) return result; // Find z and pT values at which the current state was formed, to // ensure that the showers can order the next emission correctly in // rapidity, if required if ( mother ) { double z = ( mergingHooksPtr->getNumberOfClusteringSteps(state) == 0) ? 0.5 : mother->getCurrentZ(clusterIn.emittor,clusterIn.recoiler, clusterIn.emitted); // Store z and pT values at which the current state was formed infoPtr->zNowISR(z); infoPtr->pT2NowISR(pow(startingScale,2)); infoPtr->hasHistory(true); } // Perform trial shower emission trial->next(process,event); // Get trial shower pT double pTtrial = trial->pTLastInShower(); int typeTrial = trial->typeLastInShower(); // Clear parton systems. trial->resetTrial(); // Get veto (merging) scale value double vetoScale = (mother) ? 0. : mergingHooksPtr->tms(); // Get merging scale in current event double tnow = mergingHooksPtr->tmsNow( event ); // Save scale of current state. startingScale = pTtrial; // If the scale of the current state is below the minimal scale, exit. if ( pTtrial < minscale ) break; // If this state is below the merging scale, do not count emission. if ( tnow < vetoScale && vetoScale > 0. ) continue; // Retry if the trial emission was not allowed. if ( mergingHooksPtr->canVetoTrialEmission() && mergingHooksPtr->doVetoTrialEmission( process, event) ) continue; // Check if a new emission should be generated, either because // the latest emission was not of the desired kind or if the // emission was above the minimal scale double alphaSinPS = as0; double pdfs = 1.0; // Initial state splittings. if ( (showerType == -1 || showerType == 2) && typeTrial == 2 ) { // Get weight to translate to alpha_s at fixed renormalisation scale. if ( fixas ) alphaSinPS = (*asISR).alphaS(pTtrial*pTtrial); // Get weight to translate to PDFs at fixed factorisation scale. if ( fixpdf ) pdfs = pdfFactor( event, typeTrial, pTtrial, mergingHooksPtr->muFinME() ); // Final state splittings. } else if ( (showerType == 1 || showerType == 2) && typeTrial >= 3 ) { // Get weight to translate to alpha_s at fixed renormalisation scale. if ( fixas ) alphaSinPS = (*asFSR).alphaS(pTtrial*pTtrial); // Get weight to translate to PDFs at fixed factorisation scale. Needed // for final state splittings with initial state recoiler. if ( fixpdf ) pdfs = pdfFactor( event, typeTrial, pTtrial, mergingHooksPtr->muFinME() ); } // Save weight correcting to emission generated with fixed scales. if ( typeTrial == 2 || typeTrial >= 3 ) wts.push_back(as0/alphaSinPS*pdfs); } for ( int n = 1; n <= min(N, int(wts.size())); ++n ) { vector ind(N); for ( int i = 0; i < N; ++i ) ind[i] = i; do { double x = 1.0; for ( int j = 0; j < n; ++j ) x *= wts[ind[j]]; result[n] += x; } while ( updateind(ind, n - 1, wts.size()) ); if ( n%2 ) result[n] *= -1.0; } // Done return result; } //-------------------------------------------------------------------------- // Function to integrate PDF ratios between two scales over x and t, // where the PDFs are always evaluated at the lower t-integration limit double History::monteCarloPDFratios(int flav, double x, double maxScale, double minScale, double pdfScale, double asME, Rndm* rndmPtr) { // Perform numerical integration for PDF ratios // Prefactor is as/2PI double factor = asME / (2.*M_PI); // Scale integration just produces a multiplicative logarithm factor *= log(maxScale/minScale); // For identical scales, done if (factor == 0.) return 0.; // Declare constants double CF = 4./3.; double CA = 3.; double NF = 4.; double TR = 1./2.; double integral = 0.; double RN = rndmPtr->flat(); if (flav == 21) { double zTrial = pow(x,RN); integral = -log(x) * zTrial * integrand(flav, x, pdfScale, zTrial); integral += 1./6.*(11.*CA - 4.*NF*TR) + 2.*CA*log(1.-x); } else { double zTrial = x + RN*(1. - x); integral = (1.-x) * integrand(flav, x, pdfScale, zTrial); integral += 3./2.*CF + 2.*CF*log(1.-x); } // Done return (factor*integral); } /*--------------- METHODS USED FOR CONTRUCTION OF ALL HISTORIES --------- */ // Check if a ordered (and complete) path has been found in the // initial node, in which case we will no longer be interested in // any unordered paths. bool History::onlyOrderedPaths() { if ( !mother || foundOrderedPath ) return foundOrderedPath; return foundOrderedPath = mother->onlyOrderedPaths(); } //-------------------------------------------------------------------------- // Check if a STRONGLY ordered (and complete) path has been found in the // initial node, in which case we will no longer be interested in // any unordered paths. bool History::onlyStronglyOrderedPaths() { if ( !mother || foundStronglyOrderedPath ) return foundStronglyOrderedPath; return foundStronglyOrderedPath = mother->onlyStronglyOrderedPaths(); } //-------------------------------------------------------------------------- // Check if an allowed (according to user-criterion) path has been found in // the initial node, in which case we will no longer be interested in // any forbidden paths. bool History::onlyAllowedPaths() { if ( !mother || foundAllowedPath ) return foundAllowedPath; return foundAllowedPath = mother->onlyAllowedPaths(); } //-------------------------------------------------------------------------- // When a full path has been found, register it with the initial // history node. // IN History : History to be registered as path // bool : Specifying if clusterings so far were ordered // bool : Specifying if path is complete down to 2->2 process // OUT true if History object forms a plausible path (eg prob>0 ...) bool History::registerPath(History & l, bool isOrdered, bool isStronglyOrdered, bool isAllowed, bool isComplete) { // We are not interested in improbable paths. if ( l.prob <= 0.0) return false; // We only register paths in the initial node. if ( mother ) return mother->registerPath(l, isOrdered, isStronglyOrdered, isAllowed, isComplete); // Again, we are not interested in improbable paths. if ( sumpath == sumpath + l.prob ) return false; if ( mergingHooksPtr->canCutOnRecState() && foundAllowedPath && !isAllowed ) return false; if ( mergingHooksPtr->enforceStrongOrdering() && foundStronglyOrderedPath && !isStronglyOrdered ) return false; if ( mergingHooksPtr->orderHistories() && foundOrderedPath && !isOrdered ) { // Prefer complete or allowed paths to ordered paths. if ( (!foundCompletePath && isComplete) || (!foundAllowedPath && isAllowed) ) ; else return false; } if ( foundCompletePath && !isComplete ) return false; if ( !mergingHooksPtr->canCutOnRecState() && !mergingHooksPtr->allowCutOnRecState() ) foundAllowedPath = true; if ( mergingHooksPtr->canCutOnRecState() && isAllowed && isComplete) { if ( !foundAllowedPath || !foundCompletePath ) { // If this is the first complete, allowed path, discard the // old, disallowed or incomplete ones. paths.clear(); sumpath = 0.0; } foundAllowedPath = true; } if ( mergingHooksPtr->enforceStrongOrdering() && isStronglyOrdered && isComplete ) { if ( !foundStronglyOrderedPath || !foundCompletePath ) { // If this is the first complete, ordered path, discard the // old, non-ordered or incomplete ones. paths.clear(); sumpath = 0.0; } foundStronglyOrderedPath = true; foundCompletePath = true; } if ( mergingHooksPtr->orderHistories() && isOrdered && isComplete ) { if ( !foundOrderedPath || !foundCompletePath ) { // If this is the first complete, ordered path, discard the // old, non-ordered or incomplete ones. paths.clear(); sumpath = 0.0; } foundOrderedPath = true; foundCompletePath = true; } if ( isComplete ) { if ( !foundCompletePath ) { // If this is the first complete path, discard the old, // incomplete ones. paths.clear(); sumpath = 0.0; } foundCompletePath = true; } // Remember, if this path is ordered, even if no ordering is required if ( isOrdered ) { foundOrderedPath = true; } // Index path by probability sumpath += l.prob; paths[sumpath] = &l; return true; } //-------------------------------------------------------------------------- // For the history-defining state (and if necessary interfering // states), find all possible clusterings. // NO INPUT // OUT vector of all (rad,rec,emt) systems vector History::getAllQCDClusterings() { vector ret; // Initialise vectors to keep track of position of partons in the // history-defining state vector PosFinalPartn; vector PosInitPartn; vector PosFinalGluon; vector PosFinalQuark; vector PosFinalAntiq; vector PosInitGluon; vector PosInitQuark; vector PosInitAntiq; // Search event record for final state particles and store these in // quark, anti-quark and gluon vectors for ( int i=0; i < state.size(); ++i ) if ( state[i].isFinal() && state[i].colType() !=0 ) { // Store final partons if ( state[i].id() == 21 ) PosFinalGluon.push_back(i); else if ( state[i].idAbs() < 10 && state[i].id() > 0) PosFinalQuark.push_back(i); else if ( state[i].idAbs() < 10 && state[i].id() < 0) PosFinalAntiq.push_back(i); } else if (state[i].status() == -21 && state[i].colType() != 0 ) { // Store initial partons if ( state[i].id() == 21 ) PosInitGluon.push_back(i); else if ( state[i].idAbs() < 10 && state[i].id() > 0) PosInitQuark.push_back(i); else if ( state[i].idAbs() < 10 && state[i].id() < 0) PosInitAntiq.push_back(i); } // Get all clusterings for input state vector systems; systems = getQCDClusterings(state); ret.insert(ret.end(), systems.begin(), systems.end()); systems.resize(0); // If valid clusterings were found, return if ( !ret.empty() ) return ret; // If no clusterings have been found until now, try to find // clusterings of diagrams that interfere with the current one // (i.e. change the colours of the current event slightly and run // search again) else if ( ret.empty() && mergingHooksPtr->allowColourShuffling() ) { Event NewState = Event(state); // Start with changing final state quark colour for(int i = 0; i < int(PosFinalQuark.size()); ++i) { // Never change the hard process candidates if ( mergingHooksPtr->hardProcess.matchesAnyOutgoing(PosFinalQuark[i], NewState) ) continue; int col = NewState[PosFinalQuark[i]].col(); for(int j = 0; j < int(PosInitAntiq.size()); ++j) { // Now swap colours int acl = NewState[PosInitAntiq[j]].acol(); if ( col == acl ) continue; NewState[PosFinalQuark[i]].col(acl); NewState[PosInitAntiq[j]].acol(col); systems = getQCDClusterings(NewState); if (!systems.empty()) { state = NewState; NewState.clear(); ret.insert(ret.end(), systems.begin(), systems.end()); systems.resize(0); return ret; } } } // Now change final state antiquark anticolour for(int i = 0; i < int(PosFinalAntiq.size()); ++i) { // Never change the hard process candidates if ( mergingHooksPtr->hardProcess.matchesAnyOutgoing(PosFinalAntiq[i], NewState) ) continue; int acl = NewState[PosFinalAntiq[i]].acol(); for(int j = 0; j < int(PosInitQuark.size()); ++j) { // Now swap colours int col = NewState[PosInitQuark[j]].col(); if ( col == acl ) continue; NewState[PosFinalAntiq[i]].acol(col); NewState[PosInitQuark[j]].col(acl); systems = getQCDClusterings(NewState); if (!systems.empty()) { state = NewState; NewState.clear(); ret.insert(ret.end(), systems.begin(), systems.end()); systems.resize(0); return ret; } } } if ( !ret.empty() ) { string message="Warning in History::getAllQCDClusterings: Changed"; message+=" colour structure to allow at least one clustering."; infoPtr->errorMsg(message); } } // Done return ret; } //-------------------------------------------------------------------------- // For one given state, find all possible clusterings. // IN Event : state to be investigated // OUT vector of all (rad,rec,emt) systems in the state vector History::getQCDClusterings( const Event& event) { vector ret; // Initialise vectors to keep track of position of partons in the // input event vector PosFinalPartn; vector PosInitPartn; vector PosFinalGluon; vector PosFinalQuark; vector PosFinalAntiq; vector PosInitGluon; vector PosInitQuark; vector PosInitAntiq; // Search event record for final state particles and store these in // quark, anti-quark and gluon vectors for (int i=0; i < event.size(); ++i) if ( event[i].isFinal() && event[i].colType() !=0 ) { // Store final partons PosFinalPartn.push_back(i); if ( event[i].id() == 21 ) PosFinalGluon.push_back(i); else if ( event[i].idAbs() < 10 && event[i].id() > 0) PosFinalQuark.push_back(i); else if ( event[i].idAbs() < 10 && event[i].id() < 0) PosFinalAntiq.push_back(i); } else if ( event[i].status() == -21 && event[i].colType() != 0 ) { // Store initial partons PosInitPartn.push_back(i); if ( event[i].id() == 21 ) PosInitGluon.push_back(i); else if ( event[i].idAbs() < 10 && event[i].id() > 0) PosInitQuark.push_back(i); else if ( event[i].idAbs() < 10 && event[i].id() < 0) PosInitAntiq.push_back(i); } int nFiGluon = int(PosFinalGluon.size()); int nFiQuark = int(PosFinalQuark.size()); int nFiAntiq = int(PosFinalAntiq.size()); int nInGluon = int(PosInitGluon.size()); int nInQuark = int(PosInitQuark.size()); int nInAntiq = int(PosInitAntiq.size()); vector systems; // Find rad + emt + rec systems: // (1) Start from gluon and find all (rad,rec,emt=gluon) triples for (int i = 0; i < nFiGluon; ++i) { int EmtGluon = PosFinalGluon[i]; systems = findQCDTriple( EmtGluon, 2, event, PosFinalPartn, PosInitPartn); ret.insert(ret.end(), systems.begin(), systems.end()); systems.resize(0); } // For more than one quark-antiquark pair in final state, check for // g -> qqbar splittings bool check_g2qq = true; if ( ( ( nInQuark + nInAntiq == 0 ) && (nInGluon == 0) && (nFiQuark == 1) && (nFiAntiq == 1) ) || ( ( nFiQuark + nFiAntiq == 0) && (nInQuark == 1) && (nInAntiq == 1) ) ) check_g2qq = false; if ( check_g2qq ) { // (2) Start from quark and find all (rad,rec,emt=quark) triples // ( when g -> q qbar occured ) for( int i=0; i < nFiQuark; ++i) { int EmtQuark = PosFinalQuark[i]; systems = findQCDTriple( EmtQuark,1,event, PosFinalPartn, PosInitPartn); ret.insert(ret.end(), systems.begin(), systems.end()); systems.resize(0); } // (3) Start from anti-quark and find all (rad,rec,emt=anti-quark) // triples ( when g -> q qbar occured ) for( int i=0; i < nFiAntiq; ++i) { int EmtAntiq = PosFinalAntiq[i]; systems = findQCDTriple( EmtAntiq,1,event, PosFinalPartn, PosInitPartn); ret.insert(ret.end(), systems.begin(), systems.end()); systems.resize(0); } } return ret; } //-------------------------------------------------------------------------- // Function to construct (rad,rec,emt) triples from the event // IN int : Position of Emitted in event record for which // dipoles should be constructed // int : Colour topogy to be tested // 1= g -> qqbar, causing 2 -> 2 dipole splitting // 2= q(bar) -> q(bar) g && g -> gg, // causing a 2 -> 3 dipole splitting // Event : event record to be checked for ptential partners // OUT vector of all allowed radiator+recoiler+emitted triples vector History::findQCDTriple (int EmtTagIn, int colTopIn, const Event& event, vector PosFinalPartn, vector PosInitPartn ) { // Copy input parton tag int EmtTag = EmtTagIn; // Copy input colour topology tag // (1: g --> qqbar splitting present, 2:rest) int colTop = colTopIn; // Initialise FinalSize int FinalSize = int(PosFinalPartn.size()); int InitSize = int(PosInitPartn.size()); int Size = InitSize + FinalSize; vector clus; // Search final partons to find partons colour-connected to // event[EmtTag], choose radiator, then choose recoiler for ( int a = 0; a < Size; ++a ) { int i = (a < FinalSize)? a : (a - FinalSize) ; int iRad = (a < FinalSize)? PosFinalPartn[i] : PosInitPartn[i]; if ( event[iRad].col() == event[EmtTag].col() && event[iRad].acol() == event[EmtTag].acol() ) continue; if (iRad != EmtTag ) { int pTdef = event[iRad].isFinal() ? 1 : -1; int sign = (a < FinalSize)? 1 : -1 ; // First colour topology: g --> qqbar. Here, emt & rad should // have same flavour (causes problems for gamma->qqbar). if (colTop == 1) { if ( event[iRad].id() == -sign*event[EmtTag].id() ) { int col = -1; int acl = -1; if (event[iRad].id() < 0) { col = event[EmtTag].acol(); acl = event[iRad].acol(); } else { col = event[EmtTag].col(); acl = event[iRad].col(); } // Recoiler int iRec = 0; // Colour partner int iPartner = 0; if (col > 0) { // Find recoiler by colour iRec = FindCol(col,iRad,EmtTag,event,1,true); // In initial state splitting has final state colour partner, // Save both partner and recoiler if ( (sign < 0) && (event[iRec].isFinal()) ) { // Save colour recoiler iPartner = iRec; // Reset kinematic recoiler to initial state parton for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) iRec = PosInitPartn[l]; // For final state splittings, colour partner and recoiler are // identical } else { iPartner = iRec; } if ( iRec != 0 && iPartner != 0 && allowedClustering( iRad, EmtTag, iRec, iPartner, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iPartner, pTLund(event[iRad], event[EmtTag], event[iRec], pTdef) )); continue; } // Reset partner iPartner = 0; // Find recoiler by colour iRec = FindCol(col,iRad,EmtTag,event,2,true); // In initial state splitting has final state colour partner, // Save both partner and recoiler if ( (sign < 0) && (event[iRec].isFinal()) ) { // Save colour recoiler iPartner = iRec; // Reset kinematic recoiler to initial state parton for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) iRec = PosInitPartn[l]; // For final state splittings, colour partner and recoiler are // identical } else { iPartner = iRec; } if ( iRec != 0 && iPartner != 0 && allowedClustering( iRad, EmtTag, iRec, iPartner, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iPartner, pTLund(event[iRad], event[EmtTag], event[iRec], pTdef) )); continue; } } if (acl > 0) { // Reset partner iPartner = 0; // Find recoiler by colour iRec = FindCol(acl,iRad,EmtTag,event,1,true); // In initial state splitting has final state colour partner, // Save both partner and recoiler if ( (sign < 0) && (event[iRec].isFinal()) ) { // Save colour recoiler iPartner = iRec; // Reset kinematic recoiler to initial state parton for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) iRec = PosInitPartn[l]; // For final state splittings, colour partner and recoiler are // identical } else { iPartner = iRec; } if ( iRec != 0 && iPartner != 0 && allowedClustering( iRad, EmtTag, iRec, iPartner, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iPartner, pTLund(event[iRad], event[EmtTag], event[iRec], pTdef) )); continue; } // Reset partner iPartner = 0; // Find recoiler by colour iRec = FindCol(acl,iRad,EmtTag,event,2,true); // In initial state splitting has final state colour partner, // Save both partner and recoiler if ( (sign < 0) && (event[iRec].isFinal()) ) { // Save colour recoiler iPartner = iRec; // Reset kinematic recoiler to initial state parton for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) iRec = PosInitPartn[l]; // For final state splittings, colour partner and recoiler are // identical } else { iPartner = iRec; } if ( iRec != 0 && iPartner != 0 && allowedClustering( iRad, EmtTag, iRec, iPartner, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iPartner, pTLund(event[iRad], event[EmtTag], event[iRec], pTdef) )); continue; } } // Initial gluon splitting } else if ( event[iRad].id() == 21 &&( event[iRad].col() == event[EmtTag].col() || event[iRad].acol() == event[EmtTag].acol() )) { // For an initial state radiator, always set recoiler // to the other initial state parton (recoil is taken // by full remaining system, so this is just a // labelling for such a process) int RecInit = 0; for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) RecInit = PosInitPartn[l]; // Find the colour connected partner // Find colour index of radiator before splitting int col = getRadBeforeCol(iRad, EmtTag, event); int acl = getRadBeforeAcol(iRad, EmtTag, event); // Find the correct partner: If a colour line has split, // the partner is connected to the radiator before the splitting // by a colour line (same reasoning for anticolour). The colour // that split is the colour appearing twice in the // radiator + emitted pair. // Thus, if we remove a colour index with the clustering, // we should look for a colour partner, else look for // an anticolour partner int colRemove = (event[iRad].col() == event[EmtTag].col()) ? event[iRad].col() : 0; int iPartner = 0; if (colRemove > 0 && col > 0) iPartner = FindCol(col,iRad,EmtTag,event,1,true) + FindCol(col,iRad,EmtTag,event,2,true); else if (colRemove > 0 && acl > 0) iPartner = FindCol(acl,iRad,EmtTag,event,1,true) + FindCol(acl,iRad,EmtTag,event,2,true); if ( allowedClustering( iRad, EmtTag, RecInit, iPartner, event ) ) { clus.push_back( Clustering(EmtTag, iRad, RecInit, iPartner, pTLund(event[iRad],event[EmtTag],event[RecInit], pTdef) )); continue; } } // Second colour topology: Gluon emission } else { if ( (event[iRad].col() == event[EmtTag].acol()) || (event[iRad].acol() == event[EmtTag].col()) || (event[iRad].col() == event[EmtTag].col()) || (event[iRad].acol() == event[EmtTag].acol()) ) { // For the rest, choose recoiler to have a common colour // tag with radiator, while not being the "Emitted" int col = -1; int acl = -1; if (event[iRad].isFinal() ) { if ( event[iRad].id() < 0) { acl = event[EmtTag].acol(); col = event[iRad].col(); } else if ( event[iRad].id() > 0 && event[iRad].id() < 10) { col = event[EmtTag].col(); acl = event[iRad].acol(); } else { col = event[iRad].col(); acl = event[iRad].acol(); } int iRec = 0; if (col > 0) { iRec = FindCol(col,iRad,EmtTag,event,1,true); if ( (sign < 0) && (event[iRec].isFinal()) ) iRec = 0; if (iRec != 0 && allowedClustering( iRad, EmtTag, iRec, iRec, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iRec, pTLund(event[iRad],event[EmtTag],event[iRec], pTdef) )); continue; } iRec = FindCol(col,iRad,EmtTag,event,2,true); if ( (sign < 0) && (event[iRec].isFinal()) ) iRec = 0; if (iRec != 0 && allowedClustering( iRad, EmtTag, iRec, iRec, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iRec, pTLund(event[iRad],event[EmtTag],event[iRec], pTdef) )); continue; } } if (acl > 0) { iRec = FindCol(acl,iRad,EmtTag,event,1,true); if ( (sign < 0) && (event[iRec].isFinal()) ) iRec = 0; if (iRec != 0 && allowedClustering( iRad, EmtTag, iRec, iRec, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iRec, pTLund(event[iRad],event[EmtTag],event[iRec], pTdef) )); continue; } iRec = FindCol(acl,iRad,EmtTag,event,2,true); if ( (sign < 0) && (event[iRec].isFinal()) ) iRec = 0; if (iRec != 0 && allowedClustering( iRad, EmtTag, iRec, iRec, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iRec, pTLund(event[iRad],event[EmtTag],event[iRec], pTdef) )); continue; } } } else { // For an initial state radiator, always set recoiler // to the other initial state parton (recoil is taken // by full remaining system, so this is just a // labelling for such a process) int RecInit = 0; int iPartner = 0; for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) RecInit = PosInitPartn[l]; // Find the colour connected partner // Find colour index of radiator before splitting col = getRadBeforeCol(iRad, EmtTag, event); acl = getRadBeforeAcol(iRad, EmtTag, event); // Find the correct partner: If a colour line has split, // the partner is connected to the radiator before the splitting // by a colour line (same reasoning for anticolour). The colour // that split is the colour appearing twice in the // radiator + emitted pair. // Thus, if we remove a colour index with the clustering, // we should look for a colour partner, else look for // an anticolour partner int colRemove = (event[iRad].col() == event[EmtTag].col()) ? event[iRad].col() : 0; iPartner = (colRemove > 0) ? FindCol(col,iRad,EmtTag,event,1,true) + FindCol(col,iRad,EmtTag,event,2,true) : FindCol(acl,iRad,EmtTag,event,1,true) + FindCol(acl,iRad,EmtTag,event,2,true); if ( allowedClustering( iRad, EmtTag, RecInit, iPartner, event)) { clus.push_back( Clustering(EmtTag, iRad, RecInit, iPartner, pTLund(event[iRad],event[EmtTag],event[RecInit], pTdef))); continue; } } } } } } // Done return clus; } //-------------------------------------------------------------------------- // For the history-defining state (and if necessary interfering // states), find all possible clusterings. // NO INPUT // OUT vector of all (rad,rec,emt) systems vector History::getAllEWClusterings() { vector ret; // Get all clusterings for input state vector systems; systems = getEWClusterings(state); ret.insert(ret.end(), systems.begin(), systems.end()); // Done return ret; } //-------------------------------------------------------------------------- // For one given state, find all possible clusterings. // IN Event : state to be investigated // OUT vector of all (rad,rec,emt) systems in the state vector History::getEWClusterings( const Event& event) { vector ret; // Initialise vectors to keep track of position of partons in the // input event vector PosFinalPartn; vector PosInitPartn; vector PosFinalW; // Search event record for final state particles and store these in // quark, anti-quark and gluon vectors for ( int i=0; i < event.size(); ++i ) if ( event[i].isFinal() && abs(event[i].colType()) == 1 ) { // Store final partons PosFinalPartn.push_back(i); } else if ( event[i].status() == -21 && abs(event[i].colType()) == 1 ) { // Store initial partons PosInitPartn.push_back(i); } // Search event record for final W for ( int i=0; i < event.size(); ++i ) if ( event[i].isFinal() && event[i].idAbs() == 24 ) PosFinalW.push_back( i ); vector systems; // Find rad + emt + rec systems: // (1) Start from W boson and find all (rad,rec,emt=W) triples for ( int i = 0; i < int(PosFinalW.size()); ++i ) { int EmtW = PosFinalW[i]; systems = findEWTriple( EmtW, event, PosFinalPartn); ret.insert(ret.end(), systems.begin(), systems.end()); systems.resize(0); } return ret; } //-------------------------------------------------------------------------- // Function to construct (rad,rec,emt) triples from the event // IN int : Position of Emitted in event record for which // dipoles should be constructed // int : Colour topogy to be tested // 1= g -> qqbar, causing 2 -> 2 dipole splitting // 2= q(bar) -> q(bar) g && g -> gg, // causing a 2 -> 3 dipole splitting // Event : event record to be checked for ptential partners // OUT vector of all allowed radiator+recoiler+emitted triples vector History::findEWTriple ( int EmtTagIn, const Event& event, vector PosFinalPartn ) { // Copy input parton tag int EmtTag = EmtTagIn; // Copy input colour topology tag // (1: g --> qqbar splitting present, 2:rest) // Initialise FinalSize int FinalSize = int(PosFinalPartn.size()); vector clus; // Search final partons to find partons colour-connected to // event[EmtTag], choose radiator, then choose recoiler for ( int a = 0; a < FinalSize; ++a ) { int iRad = PosFinalPartn[a]; if (iRad != EmtTag ) { int pTdef = 1; // Find recoiler by flavour. int flavRad = event[iRad].id(); int flavEmt = event[EmtTag].id(); // Loop through final partons and try to find matching flavours. for ( int i = 0; i < FinalSize; ++i ) { int iRec = PosFinalPartn[i]; if ( i != a && flavEmt > 0 && event[iRec].id() == -flavRad - 1 ) clus.push_back( Clustering(EmtTag, iRad, iRec, iRec, pTLund(event[iRad],event[EmtTag],event[iRec], pTdef) ) ); } } } // Done return clus; } //-------------------------------------------------------------------------- // For the history-defining state (and if necessary interfering // states), find all possible clusterings. // NO INPUT // OUT vector of all (rad,rec,emt) systems vector History::getAllSQCDClusterings() { vector ret; // Get all clusterings for input state vector systems; systems = getSQCDClusterings(state); ret.insert(ret.end(), systems.begin(), systems.end()); // Done return ret; } //-------------------------------------------------------------------------- // For one given state, find all possible clusterings. // IN Event : state to be investigated // OUT vector of all (rad,rec,emt) systems in the state vector History::getSQCDClusterings( const Event& event) { vector ret; // Initialise vectors to keep track of position of partons in the // input event vector PosFinalPartn; vector PosInitPartn; vector PosFinalGluon; vector PosFinalQuark; vector PosFinalAntiq; vector PosInitGluon; vector PosInitQuark; vector PosInitAntiq; // Search event record for final state particles and store these in // quark, anti-quark and gluon vectors for (int i=0; i < event.size(); ++i) if ( event[i].isFinal() && event[i].colType() !=0 ) { // Store final partons PosFinalPartn.push_back(i); if ( event[i].id() == 21 || event[i].id() == 1000021) PosFinalGluon.push_back(i); else if ( (event[i].idAbs() < 10 && event[i].id() > 0) || (event[i].idAbs() < 1000010 && event[i].idAbs() > 1000000 && event[i].id() > 0) || (event[i].idAbs() < 2000010 && event[i].idAbs() > 2000000 && event[i].id() > 0)) PosFinalQuark.push_back(i); else if ( (event[i].idAbs() < 10 && event[i].id() < 0) || (event[i].idAbs() < 1000010 && event[i].idAbs() > 1000000 && event[i].id() < 0) || (event[i].idAbs() < 2000010 && event[i].idAbs() > 2000000 && event[i].id() < 0)) PosFinalAntiq.push_back(i); } else if ( event[i].status() == -21 && event[i].colType() != 0 ) { // Store initial partons PosInitPartn.push_back(i); if ( event[i].id() == 21 || event[i].id() == 1000021) PosInitGluon.push_back(i); else if ( (event[i].idAbs() < 10 && event[i].id() > 0) || (event[i].idAbs() < 1000010 && event[i].idAbs() > 1000000 && event[i].id() > 0) || (event[i].idAbs() < 2000010 && event[i].idAbs() > 2000000 && event[i].id() > 0)) PosInitQuark.push_back(i); else if ( (event[i].idAbs() < 10 && event[i].id() < 0) || (event[i].idAbs() < 1000010 && event[i].idAbs() > 1000000 && event[i].id() < 0) || (event[i].idAbs() < 2000010 && event[i].idAbs() > 2000000 && event[i].id() < 0)) PosInitAntiq.push_back(i); } int nFiGluon = int(PosFinalGluon.size()); int nFiQuark = int(PosFinalQuark.size()); int nFiAntiq = int(PosFinalAntiq.size()); int nInGluon = int(PosInitGluon.size()); int nInQuark = int(PosInitQuark.size()); int nInAntiq = int(PosInitAntiq.size()); vector systems; // Find rad + emt + rec systems: // (1) Start from gluon and find all (rad,rec,emt=gluon) triples for (int i = 0; i < nFiGluon; ++i) { int EmtGluon = PosFinalGluon[i]; systems = findSQCDTriple( EmtGluon, 2, event, PosFinalPartn, PosInitPartn); ret.insert(ret.end(), systems.begin(), systems.end()); systems.resize(0); } // For more than one quark-antiquark pair in final state, check for // g -> qqbar splittings bool check_g2qq = true; if ( ( ( nInQuark + nInAntiq == 0 ) && (nInGluon == 0) && (nFiQuark == 1) && (nFiAntiq == 1) ) || ( ( nFiQuark + nFiAntiq == 0) && (nInQuark == 1) && (nInAntiq == 1) ) ) check_g2qq = false; if ( check_g2qq ) { // (2) Start from quark and find all (rad,rec,emt=quark) triples // ( when g -> q qbar occured ) for( int i=0; i < nFiQuark; ++i) { int EmtQuark = PosFinalQuark[i]; systems = findSQCDTriple( EmtQuark,1,event, PosFinalPartn, PosInitPartn); ret.insert(ret.end(), systems.begin(), systems.end()); systems.resize(0); } // (3) Start from anti-quark and find all (rad,rec,emt=anti-quark) // triples ( when g -> q qbar occured ) for( int i=0; i < nFiAntiq; ++i) { int EmtAntiq = PosFinalAntiq[i]; systems = findSQCDTriple( EmtAntiq,1,event, PosFinalPartn, PosInitPartn); ret.insert(ret.end(), systems.begin(), systems.end()); systems.resize(0); } } return ret; } //-------------------------------------------------------------------------- // Function to construct (rad,rec,emt) triples from the event // IN int : Position of Emitted in event record for which // dipoles should be constructed // int : Colour topogy to be tested // 1= g -> qqbar, causing 2 -> 2 dipole splitting // 2= q(bar) -> q(bar) g && g -> gg, // causing a 2 -> 3 dipole splitting // Event : event record to be checked for ptential partners // OUT vector of all allowed radiator+recoiler+emitted triples vector History::findSQCDTriple (int EmtTagIn, int colTopIn, const Event& event, vector PosFinalPartn, vector PosInitPartn ) { // Copy input parton tag int EmtTag = EmtTagIn; // Copy input colour topology tag // (1: g --> qqbar splitting present, 2:rest) int colTop = colTopIn; // PDG numbering offset for squarks int offsetL = 1000000; int offsetR = 2000000; // Initialise FinalSize int FinalSize = int(PosFinalPartn.size()); int InitSize = int(PosInitPartn.size()); int Size = InitSize + FinalSize; vector clus; // Search final partons to find partons colour-connected to // event[EmtTag], choose radiator, then choose recoiler for ( int a = 0; a < Size; ++a ) { int i = (a < FinalSize)? a : (a - FinalSize) ; int iRad = (a < FinalSize)? PosFinalPartn[i] : PosInitPartn[i]; if ( event[iRad].col() == event[EmtTag].col() && event[iRad].acol() == event[EmtTag].acol() ) continue; // Save radiator flavour. int radID = event[iRad].id(); // Remember if radiator is BSM. bool isSQCDrad = (abs(radID) > offsetL); // Remember if emitted is BSM. bool isSQCDemt = (event[EmtTag].idAbs() > offsetL ); if (iRad != EmtTag ) { int pTdef = event[iRad].isFinal() ? 1 : -1; int sign = (a < FinalSize)? 1 : -1 ; // Disalllow clusterings resulting in an initial state sQCD parton! int radBefID = getRadBeforeFlav(iRad,EmtTag,event); if ( pTdef == -1 && abs(radBefID) > offsetL ) continue; // First colour topology: g --> qqbar. Here, emt & rad should // have same flavour (causes problems for gamma->qqbar). if (colTop == 1) { int emtSign = (event[EmtTag].id() < 0) ? -1 : 1; // Final gluino splitting. bool finalSplitting = false; if ( abs(radID) < 10 && radID == -sign*emtSign*(offsetL + event[EmtTag].idAbs()) ) finalSplitting = true; if ( abs(radID) < 10 && radID == -sign*emtSign*(offsetR + event[EmtTag].idAbs()) ) finalSplitting = true; if ( abs(radID) > offsetL && abs(radID) < offsetL+10 && radID == -sign*emtSign*( event[EmtTag].idAbs() - offsetL) ) finalSplitting = true; if ( abs(radID) > offsetR && abs(radID) < offsetR+10 && radID == -sign*emtSign*( event[EmtTag].idAbs() - offsetR) ) finalSplitting = true; // Initial gluon splitting. bool initialSplitting = false; if ( radID == 21 && ( ( event[EmtTag].idAbs() > offsetL && event[EmtTag].idAbs() < offsetL+10) || ( event[EmtTag].idAbs() > offsetR && event[EmtTag].idAbs() < offsetR+10) ) && ( event[iRad].col() == event[EmtTag].col() || event[iRad].acol() == event[EmtTag].acol() ) ) initialSplitting = true; if ( finalSplitting ) { int col = -1; int acl = -1; if ( radID < 0 && event[iRad].colType() == -1) { acl = event[EmtTag].acol(); col = event[iRad].acol(); } else if ( event[iRad].colType() == 1 ) { col = event[EmtTag].col(); acl = event[iRad].col(); } // Recoiler int iRec = 0; // Colour partner int iPartner = 0; if (col > 0) { // Find recoiler by colour iRec = FindCol(col,iRad,EmtTag,event,1,true); // In initial state splitting has final state colour partner, // Save both partner and recoiler if ( (sign < 0) && (event[iRec].isFinal()) ) { // Save colour recoiler iPartner = iRec; // Reset kinematic recoiler to initial state parton for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) iRec = PosInitPartn[l]; // For final state splittings, colour partner and recoiler are // identical } else { iPartner = iRec; } // Not interested in pure QCD triples here. if ( !isSQCDrad && !isSQCDemt && (event[iRec].idAbs() < 10 || event[iRec].id() == 21) ) iRec = 0; if ( iRec != 0 && iPartner != 0 && allowedClustering( iRad, EmtTag, iRec, iPartner, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iPartner, pTLund(event[iRad], event[EmtTag], event[iRec], pTdef) )); continue; } // Reset partner iPartner = 0; // Find recoiler by colour iRec = FindCol(col,iRad,EmtTag,event,2,true); // In initial state splitting has final state colour partner, // Save both partner and recoiler if ( (sign < 0) && (event[iRec].isFinal()) ) { // Save colour recoiler iPartner = iRec; // Reset kinematic recoiler to initial state parton for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) iRec = PosInitPartn[l]; // For final state splittings, colour partner and recoiler are // identical } else { iPartner = iRec; } // Not interested in pure QCD triples here. if ( !isSQCDrad && !isSQCDemt && (event[iRec].idAbs() < 10 || event[iRec].id() == 21) ) iRec = 0; if ( iRec != 0 && iPartner != 0 && allowedClustering( iRad, EmtTag, iRec, iPartner, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iPartner, pTLund(event[iRad], event[EmtTag], event[iRec], pTdef) )); continue; } } if (acl > 0) { // Reset partner iPartner = 0; // Find recoiler by colour iRec = FindCol(acl,iRad,EmtTag,event,1,true); // In initial state splitting has final state colour partner, // Save both partner and recoiler if ( (sign < 0) && (event[iRec].isFinal()) ) { // Save colour recoiler iPartner = iRec; // Reset kinematic recoiler to initial state parton for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) iRec = PosInitPartn[l]; // For final state splittings, colour partner and recoiler are // identical } else { iPartner = iRec; } // Not interested in pure QCD triples here. if ( !isSQCDrad && !isSQCDemt && (event[iRec].idAbs() < 10 || event[iRec].id() == 21) ) iRec = 0; if ( iRec != 0 && iPartner != 0 && allowedClustering( iRad, EmtTag, iRec, iPartner, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iPartner, pTLund(event[iRad], event[EmtTag], event[iRec], pTdef) )); continue; } // Reset partner iPartner = 0; // Find recoiler by colour iRec = FindCol(acl,iRad,EmtTag,event,2,true); // In initial state splitting has final state colour partner, // Save both partner and recoiler if ( (sign < 0) && (event[iRec].isFinal()) ) { // Save colour recoiler iPartner = iRec; // Reset kinematic recoiler to initial state parton for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) iRec = PosInitPartn[l]; // For final state splittings, colour partner and recoiler are // identical } else { iPartner = iRec; } // Not interested in pure QCD triples here. if ( !isSQCDrad && !isSQCDemt && (event[iRec].idAbs() < 10 || event[iRec].id() == 21) ) iRec = 0; if ( iRec != 0 && iPartner != 0 && allowedClustering( iRad, EmtTag, iRec, iPartner, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iPartner, pTLund(event[iRad], event[EmtTag], event[iRec], pTdef) )); continue; } } // Initial gluon splitting } else if ( initialSplitting ) { // SM splittings already taken care of in findQCDTriple. if ( !isSQCDrad && !isSQCDemt ) continue; // For an initial state radiator, always set recoiler // to the other initial state parton (recoil is taken // by full remaining system, so this is just a // labelling for such a process) int RecInit = 0; for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) RecInit = PosInitPartn[l]; // Find the colour connected partner // Find colour index of radiator before splitting int col = getRadBeforeCol(iRad, EmtTag, event); int acl = getRadBeforeAcol(iRad, EmtTag, event); // Find the correct partner: If a colour line has split, // the partner is connected to the radiator before the splitting // by a colour line (same reasoning for anticolour). The colour // that split is the colour appearing twice in the // radiator + emitted pair. // Thus, if we remove a colour index with the clustering, // we should look for a colour partner, else look for // an anticolour partner int colRemove = (event[iRad].col() == event[EmtTag].col()) ? event[iRad].col() : 0; int iPartner = 0; if (colRemove > 0 && col > 0) iPartner = FindCol(col,iRad,EmtTag,event,1,true) + FindCol(col,iRad,EmtTag,event,2,true); else if (colRemove > 0 && acl > 0) iPartner = FindCol(acl,iRad,EmtTag,event,1,true) + FindCol(acl,iRad,EmtTag,event,2,true); if ( allowedClustering( iRad, EmtTag, RecInit, iPartner, event ) ) { clus.push_back( Clustering(EmtTag, iRad, RecInit, iPartner, pTLund(event[iRad],event[EmtTag],event[RecInit], pTdef) )); continue; } } // Second colour topology: Gluino emission } else { if ( (event[iRad].col() == event[EmtTag].acol()) || (event[iRad].acol() == event[EmtTag].col()) || (event[iRad].col() == event[EmtTag].col()) || (event[iRad].acol() == event[EmtTag].acol()) ) { // For the rest, choose recoiler to have a common colour // tag with radiator, while not being the "Emitted" int col = -1; int acl = -1; if (event[iRad].isFinal() ) { if ( radID < 0 && event[iRad].colType() == -1) { acl = event[EmtTag].acol(); col = event[iRad].col(); } else if ( radID > 0 && event[iRad].colType() == 1 ) { col = event[EmtTag].col(); acl = event[iRad].acol(); } else { col = event[iRad].col(); acl = event[iRad].acol(); } int iRec = 0; if (col > 0) { iRec = FindCol(col,iRad,EmtTag,event,1,true); if ( (sign < 0) && (event[iRec].isFinal()) ) iRec = 0; // Not interested in pure QCD triples here. if ( !isSQCDrad && !isSQCDemt && (event[iRec].idAbs() < 10 || event[iRec].id() == 21) ) iRec = 0; if (iRec != 0 && allowedClustering( iRad, EmtTag, iRec, iRec, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iRec, pTLund(event[iRad],event[EmtTag],event[iRec], pTdef) )); continue; } iRec = FindCol(col,iRad,EmtTag,event,2,true); if ( (sign < 0) && (event[iRec].isFinal()) ) iRec = 0; // Not interested in pure QCD triples here. if ( !isSQCDrad && !isSQCDemt && (event[iRec].idAbs() < 10 || event[iRec].id() == 21) ) iRec = 0; if (iRec != 0 && allowedClustering( iRad, EmtTag, iRec, iRec, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iRec, pTLund(event[iRad],event[EmtTag],event[iRec], pTdef) )); continue; } } if (acl > 0) { iRec = FindCol(acl,iRad,EmtTag,event,1,true); if ( (sign < 0) && (event[iRec].isFinal()) ) iRec = 0; // Not interested in pure QCD triples here. if ( !isSQCDrad && !isSQCDemt && (event[iRec].idAbs() < 10 || event[iRec].id() == 21) ) iRec = 0; if (iRec != 0 && allowedClustering( iRad, EmtTag, iRec, iRec, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iRec, pTLund(event[iRad],event[EmtTag],event[iRec], pTdef) )); continue; } iRec = FindCol(acl,iRad,EmtTag,event,2,true); if ( (sign < 0) && (event[iRec].isFinal()) ) iRec = 0; // Not interested in pure QCD triples here. if ( !isSQCDrad && !isSQCDemt && (event[iRec].idAbs() < 10 || event[iRec].id() == 21) ) iRec = 0; if (iRec != 0 && allowedClustering( iRad, EmtTag, iRec, iRec, event) ) { clus.push_back( Clustering(EmtTag, iRad, iRec, iRec, pTLund(event[iRad],event[EmtTag],event[iRec], pTdef) )); continue; } } } else { // SM splittings already taken care of in findQCDTriple. Since // initial state splittings will not know if the true // colour-connected recoiler is a SM particle, any ISR splitting // of a SM particle will be included by findQCDTriple. To not // include the same splitting twice, continue for SM ISR radiator if ( !isSQCDrad || !isSQCDemt ) continue; // For an initial state radiator, always set recoiler // to the other initial state parton (recoil is taken // by full remaining system, so this is just a // labelling for such a process) int RecInit = 0; int iPartner = 0; for(int l = 0; l < int(PosInitPartn.size()); ++l) if (PosInitPartn[l] != iRad) RecInit = PosInitPartn[l]; // Find the colour connected partner // Find colour index of radiator before splitting col = getRadBeforeCol(iRad, EmtTag, event); acl = getRadBeforeAcol(iRad, EmtTag, event); // Find the correct partner: If a colour line has split, // the partner is connected to the radiator before the splitting // by a colour line (same reasoning for anticolour). The colour // that split is the colour appearing twice in the // radiator + emitted pair. // Thus, if we remove a colour index with the clustering, // we should look for a colour partner, else look for // an anticolour partner int colRemove = (event[iRad].col() == event[EmtTag].col()) ? event[iRad].col() : 0; iPartner = (colRemove > 0) ? FindCol(col,iRad,EmtTag,event,1,true) + FindCol(col,iRad,EmtTag,event,2,true) : FindCol(acl,iRad,EmtTag,event,1,true) + FindCol(acl,iRad,EmtTag,event,2,true); if ( allowedClustering( iRad, EmtTag, RecInit, iPartner, event)) { clus.push_back( Clustering(EmtTag, iRad, RecInit, iPartner, pTLund(event[iRad],event[EmtTag],event[RecInit], pTdef))); continue; } } } } } } // Done return clus; } //-------------------------------------------------------------------------- // Calculate and return the probability of a clustering. // IN Clustering : rad,rec,emt - System for which the splitting // probability should be calcuated // OUT splitting probability double History::getProb(const Clustering & SystemIn) { // Get local copies of input system int Rad = SystemIn.emittor; int Rec = SystemIn.recoiler; int Emt = SystemIn.emitted; // Initialise shower probability double showerProb = 0.0; // If the splitting resulted in disallowed evolution variable, // disallow the splitting if (SystemIn.pT() <= 0.) return 0.; // Initialise all combinatorical factors double CF = 4./3.; double NC = 3.; // Flavour is known when reclustring, thus n_f=1 double TR = 1./2.; // Split up in FSR and ISR bool isFSR = (state[Rad].isFinal() && state[Rec].isFinal()); bool isFSRinREC = (state[Rad].isFinal() && !state[Rec].isFinal()); bool isISR = !state[Rad].isFinal(); // Check if this is the clustering 2->3 to 2->2. // If so, use weight for joined evolution int nFinal = 0; for(int i=0; i < state.size(); ++i) if (state[i].isFinal()) nFinal++; bool isLast = (nFinal == (mergingHooksPtr->hardProcess.nQuarksOut() +mergingHooksPtr->hardProcess.nLeptonOut()+1)); if (isISR) { // Find incoming particles int inP = 0; int inM = 0; for(int i=0;i< int(state.size()); ++i) { if (state[i].mother1() == 1) inP = i; if (state[i].mother1() == 2) inM = i; } // Construct dipole mass, eCM and sHat = x1*x2*s Vec4 sum = state[Rad].p() + state[Rec].p() - state[Emt].p(); double m2Dip = sum.m2Calc(); double sHat = (state[inM].p() + state[inP].p()).m2Calc(); // Energy fraction z=E_q1/E_qi in branch q(i)q(2) -> q(1)g(3)q(2) double z1 = m2Dip / sHat; // Virtuality of the splittings Vec4 Q1( state[Rad].p() - state[Emt].p() ); Vec4 Q2( state[Rec].p() - state[Emt].p() ); // Q^2 for emission off radiator line double Q1sq = -Q1.m2Calc(); // pT^2 for emission off radiator line double pT1sq = pow(SystemIn.pT(),2); // Remember if massive particles involved: Mass corrections for // to g->QQ and Q->Qg splittings bool g2QQmassive = mergingHooksPtr->includeMassive() && state[Rad].id() == 21 && ( (state[Emt].idAbs() >= 4 && state[Emt].idAbs() < 7) || (state[Emt].idAbs() > 1000000 && state[Emt].idAbs() < 1000010 ) || (state[Emt].idAbs() > 2000000 && state[Emt].idAbs() < 2000010 )); bool Q2Qgmassive = mergingHooksPtr->includeMassive() && state[Emt].id() == 21 && ( (state[Rad].idAbs() >= 4 && state[Rad].idAbs() < 7) || (state[Rad].idAbs() > 1000000 && state[Rad].idAbs() < 1000010 ) || (state[Rad].idAbs() > 2000000 && state[Rad].idAbs() < 2000010 )); bool isMassive = mergingHooksPtr->includeMassive() && ( g2QQmassive || Q2Qgmassive || state[Emt].id() == 1000021); double m2Emt0 = pow(particleDataPtr->m0(state[Emt].id()),2); double m2Rad0 = pow(particleDataPtr->m0(state[Rad].id()),2); // Correction of virtuality for massive splittings if ( g2QQmassive) Q1sq += m2Emt0; else if (Q2Qgmassive) Q1sq += m2Rad0; // pT0 dependence!!! double pT0sq = pow(mergingHooksPtr->pT0ISR(),2); double Q2sq = -Q2.m2Calc(); // Correction of virtuality of other splitting bool g2QQmassiveRec = mergingHooksPtr->includeMassive() && state[Rec].id() == 21 && ( state[Emt].idAbs() >= 4 && state[Emt].idAbs() < 7); bool Q2QgmassiveRec = mergingHooksPtr->includeMassive() && state[Emt].id() == 21 && ( state[Rec].idAbs() >= 4 && state[Rec].idAbs() < 7); double m2Rec0 = pow(particleDataPtr->m0(state[Rad].id()),2); if ( g2QQmassiveRec) Q2sq += m2Emt0; else if (Q2QgmassiveRec) Q2sq += m2Rec0; bool hasJoinedEvol = (state[Emt].id() == 21 || state[Rad].id() == state[Rec].id()); // Initialise normalization factor multiplying the splitting // function numerator double fac = 1.; if ( mergingHooksPtr->pickByFull() || mergingHooksPtr->pickBySumPT()) { double facJoined = ( Q2sq + pT0sq/(1.-z1) ) * 1./(Q1sq*Q2sq + pT0sq*sHat + pow(pT0sq/(1.-z1),2)); double facSingle = mergingHooksPtr->nonJoinedNorm()*1./( pT1sq + pT0sq); fac = (hasJoinedEvol && isLast) ? facJoined : facSingle; } else if (mergingHooksPtr->pickByPoPT2()) { fac = 1./(pT1sq + pT0sq); } else { string message="Error in History::getProb: Scheme for calculating"; message+=" shower splitting probability is undefined."; infoPtr->errorMsg(message); } // Calculate shower splitting probability: // Splitting functions*normalization*ME reweighting factors // Calculate branching probability for q -> q g if ( state[Emt].id() == 21 && state[Rad].id() != 21) { // Find splitting kernel double num = CF*(1. + pow(z1,2)) / (1.-z1); if (isMassive) num -= CF * z1 * (1.-z1) * (m2Rad0/pT1sq); // Find ME reweighting factor double meReweighting = 1.; // Find the number of final state coloured particles, apart // from those coming from the hard process int nCol = 0; for(int i=0; i < state.size(); ++i) if (state[i].isFinal() && state[i].colType() != 0 && !mergingHooksPtr->hardProcess.matchesAnyOutgoing(i,state) ) nCol++; // For first splitting of single vector boson production, // apply ME corrections if (nCol == 1 && int(mergingHooksPtr->hardProcess.hardIntermediate.size()) == 1) { double sH = m2Dip / z1; double tH = -Q1sq; double uH = Q1sq - m2Dip * (1. - z1) / z1; double misMatch = (uH*tH - (uH + tH)*pT0sq/(1.-z1) + pow(pT0sq/(1.-z1),2) ) / (uH*tH); meReweighting *= (tH*tH + uH*uH + 2. * m2Dip * sH) / (sH*sH + m2Dip*m2Dip); meReweighting *= misMatch; } // Multiply factors showerProb = num*fac*meReweighting; // Calculate branching probability for g -> g g } else if ( state[Emt].id() == 21 && state[Rad].id() == 21) { // Calculate splitting kernel double num = 2.*NC*pow2(1. - z1*(1.-z1)) / (z1*(1.-z1)); // Include ME reweighting for higgs!! // Find ME reweighting factor double meReweighting = 1.; // Find the number of final state coloured particles, apart // from those coming from the hard process int nCol = 0; for(int i=0; i < state.size(); ++i) if (state[i].isFinal() && state[i].colType() != 0 && !mergingHooksPtr->hardProcess.matchesAnyOutgoing(i,state) ) nCol++; // For first splitting of single vector boson production, // apply ME corrections if ( nCol == 1 && mergingHooksPtr->getProcessString().compare("pp>h") == 0 && int(mergingHooksPtr->hardProcess.hardIntermediate.size()) == 1 ) { double sH = m2Dip / z1; double tH = -Q1sq; double uH = Q1sq - m2Dip * (1. - z1) / z1; meReweighting *= 0.5 * (pow4(sH) + pow4(tH) + pow4(uH) + pow4(m2Dip)) / pow2(sH*sH - m2Dip * (sH - m2Dip)); } // Multiply factors showerProb = num*fac*meReweighting; // Calculate branching probability for q -> g q } else if ( state[Emt].id() != 21 && state[Rad].id() != 21 ) { // Calculate splitting kernel double num = CF*(1. + pow2(1.-z1)) / z1; // Include ME reweighting for higgs!! // Find ME reweighting factor double meReweighting = 1.; // Find the number of final state coloured particles, apart // from those coming from the hard process int nCol = 0; for ( int i=0; i < state.size(); ++i ) if ( state[i].isFinal() && state[i].colType() != 0 && !mergingHooksPtr->hardProcess.matchesAnyOutgoing(i,state) ) nCol++; // For first splitting of single vector boson production, // apply ME corrections if (nCol == 1 && mergingHooksPtr->getProcessString().compare("pp>h") == 0 && int(mergingHooksPtr->hardProcess.hardIntermediate.size()) == 1) { double sH = m2Dip / z1; double uH = Q1sq - m2Dip * (1. - z1) / z1; meReweighting *= (sH*sH + uH*uH) / (sH*sH + pow2(sH -m2Dip)); } // Multiply factors showerProb = num*fac*meReweighting; // Calculate branching probability for g -> q qbar } else if ( state[Emt].id() != 21 && state[Rad].id() == 21 ) { // Calculate splitting kernel double num = TR * ( pow(z1,2) + pow(1.-z1,2) ); if (isMassive) num += TR * 2.*z1*(1.-z1)*(m2Emt0/pT1sq); // Calculate ME reweighting factor double meReweighting = 1.; // Find the number of final state coloured particles, apart // from those coming from the hard process int nCol = 0; for ( int i=0; i < state.size(); ++i ) if ( state[i].isFinal() && state[i].colType() != 0 && !mergingHooksPtr->hardProcess.matchesAnyOutgoing(i,state) ) nCol++; // For first splitting of single vector boson production, // apply ME corrections if (nCol == 1 && int(mergingHooksPtr->hardProcess.hardIntermediate.size()) == 1) { double sH = m2Dip / z1; double tH = -Q1sq; double uH = Q1sq - m2Dip * (1. - z1) / z1; swap( tH, uH); double misMatch = ( uH - pT0sq/(1.-z1) ) / uH; double me = (sH*sH + uH*uH + 2. * m2Dip * tH) / (pow2(sH - m2Dip) + m2Dip*m2Dip); // Weight with me/overestimate meReweighting *= me; meReweighting *= misMatch; } // Multiply factors showerProb = num*fac*meReweighting; // Print error if no kernel calculated } else { string message="Error in History::getProb: Splitting kernel undefined in ISR"; message+=" in clustering."; infoPtr->errorMsg(message); } // If corrected pT below zero in ISR, put probability to zero double m2Sister0 = pow(state[Emt].m0(),2); double pT2corr = (Q1sq - z1*(m2Dip + Q1sq)*(Q1sq + m2Sister0)/m2Dip); if (pT2corr < 0.) showerProb *= 1e-9; // If creating heavy quark by Q -> gQ then next need g -> Q + Qbar. // So minimum total mass2 is 4 * m2Sister, but use more to be safe. if ( state[Emt].id() == state[Rad].id() && ( state[Rad].idAbs() == 4 || state[Rad].idAbs() == 5 )) { double m2QQsister = 2.*4.*m2Sister0; double pT2QQcorr = Q1sq - z1*(m2Dip + Q1sq)*(Q1sq + m2QQsister) / m2Dip; if (pT2QQcorr < 0.0) showerProb *= 1e-9; } if (mergingHooksPtr->includeRedundant()) { // Initialise the spacelike shower alpha_S AlphaStrong* asISR = mergingHooksPtr->AlphaS_ISR(); double as = (*asISR).alphaS(pT1sq + pT0sq) / (2.*M_PI); // Multiply with alpha_S showerProb *= as; } // Done for ISR case, begin FSR case } else if (isFSR || isFSRinREC) { // Construct dipole mass Vec4 sum = state[Rad].p() + state[Rec].p() + state[Emt].p(); double m2Dip = sum.m2Calc(); // Construct 2->3 variables for FSR double x1 = 2. * (sum * state[Rad].p()) / m2Dip; double x2 = 2. * (sum * state[Rec].p()) / m2Dip; double prop1 = max(1e-12, 1. - x1); double prop2 = max(1e-12, 1. - x2); double x3 = max(1e-12, 2. - x1 - x2); // Energy fraction z=E_q1/E_qi in branch q(i)q(2) -> q(1)g(3)q(2) double z1 = x1/(x1 + x3); // Virtuality of the splittings Vec4 Q1( state[Rad].p() + state[Emt].p() ); Vec4 Q2( state[Rec].p() + state[Emt].p() ); // Q^2 for emission off radiator line double Q1sq = Q1.m2Calc(); // pT^2 for emission off radiator line double pT1sq = pow(SystemIn.pT(),2); // Q^2 for emission off recoiler line double Q2sq = Q2.m2Calc(); // Remember if radiator or recoiler is massive. bool isMassiveRad = ( state[Rad].idAbs() >= 4 && state[Rad].id() != 21 ); bool isMassiveRec = ( state[Rec].idAbs() >= 4 && state[Rec].id() != 21 ); // Correction of virtuality for massive splittings. double m2Rad0 = pow(particleDataPtr->m0(state[Rad].id()),2); double m2Rec0 = pow(particleDataPtr->m0(state[Rad].id()),2); if ( mergingHooksPtr->includeMassive() && isMassiveRad ) Q1sq -= m2Rad0; if ( mergingHooksPtr->includeMassive() && isMassiveRec ) Q2sq -= m2Rec0; // Initialise normalization factor multiplying the splitting // function numerator double fac = 1.; if ( mergingHooksPtr->pickByFull() || mergingHooksPtr->pickBySumPT()) { double facJoined = (1.-z1)/Q1sq * m2Dip/( Q1sq + Q2sq ); double facSingle = mergingHooksPtr->fsrInRecNorm() * 1./ pT1sq; fac = (!isFSRinREC && isLast) ? facJoined : facSingle; } else if (mergingHooksPtr->pickByPoPT2()) { fac = 1. / pT1sq; } else { string message="Error in History::getProb: Scheme for calculating"; message+=" shower splitting probability is undefined."; infoPtr->errorMsg(message); } // Calculate shower splitting probability: // Splitting functions*normalization*ME reweighting factors // Calculate branching probability for g -> g_1 g_2 if ( state[Emt].id() == 21 && state[Rad].id() == 21) { // Calculate splitting kernel double num = 0.5* NC * (1. + pow3(z1)) / (1.-z1); // Multiply factors showerProb = num*fac; // Calculate branching probability for q -> q g with quark recoiler } else if ( state[Emt].id() == 21 && state[Rad].id() != 21 && state[Rec].id() != 21) { // For a qqbar dipole in FSR, ME corrections exist and the // splitting function "z-weight" is set to 1.0 (only for 2->2 ??) double num = CF * 2./(1.-z1); // Find the number of final state coloured particles, apart // from those coming from the hard process int nCol = 0; for(int i=0; i < state.size(); ++i) if (state[i].isFinal() && state[i].colType() != 0 && !mergingHooksPtr->hardProcess.matchesAnyOutgoing(i,state) ) nCol++; // Calculate splitting kernel if ( nCol > 3 || int(mergingHooksPtr->hardProcess.hardIntermediate.size()) > 1) num = CF * (1. + pow2(z1)) /(1.-z1); // Calculate ME reweighting factor double meReweighting = 1.; // Correct if this is the process created by the first // FSR splitting of a 2->2 process if ( nCol == 3 && int(mergingHooksPtr->hardProcess.hardIntermediate.size()) == 1 ) { // Calculate the ME reweighting factor double ShowerRate1 = 2./( x3 * prop2 ); double meDividingFactor1 = prop1 / x3; double me = (pow(x1,2) + pow(x2,2))/(prop1*prop2); meReweighting = meDividingFactor1 * me / ShowerRate1; } // Multiply factors showerProb = num*fac*meReweighting; // Calculate branching probability for q1 -> q2 w+- with quark recoiler } else if ( state[Emt].idAbs() == 24 && state[Rad].id() != 21 && state[Rec].id() != 21 ) { double m2W = state[Emt].p().m2Calc(); double num = ( 3.*pow2(m2W / m2Dip) + 2.* (m2W/m2Dip)*(x1 + x2) + pow2(x1) + pow2(x2) ) / ( prop1*prop2 ) - (m2W/m2Dip) / pow2(prop1) - (m2W/m2Dip) / pow2(prop2); // Multiply factors showerProb = num*fac; // Calculate branching probability for q -> q g with gluon recoiler } else if ( state[Emt].id() == 21 && state[Rad].id() != 21 && state[Rec].id() == 21 ) { // For qg /qbarg dipoles, the splitting function is // calculated and not weighted by a ME correction factor // Shower splitting function double num = CF * (1. + pow2(z1)) / (1.-z1); showerProb = num*fac; // Calculate branching probability for g -> q qbar } else if ( state[Emt].id() != 21 ) { // Get flavour of quark / antiquark int flavour = state[Emt].id(); // Get correct masses for the quarks // (needed to calculate splitting function?) double mFlavour = particleDataPtr->m0(flavour); // Get mass of quark/antiquark pair double mDipole = m(state[Rad].p(), state[Emt].p()); // Factor determining if gluon decay was allowed double beta = sqrtpos( 1. - 4.*pow2(mFlavour)/pow2(mDipole) ); // Shower splitting function double num = 0.5*TR * ( z1*z1 + (1.-z1)*(1.-z1) ); if (beta <= 0.) beta = 0.; showerProb = num*fac*beta; // Print error if no kernel calculated } else { string message="Error in History::getProb: Splitting kernel undefined"; message+=" in FSR clustering."; infoPtr->errorMsg(message); } if (mergingHooksPtr->includeRedundant()) { // Initialise the spacelike shower alpha_S AlphaStrong* asFSR = mergingHooksPtr->AlphaS_FSR(); double as = (*asFSR).alphaS(pT1sq) / (2.*M_PI); // Multiply with alpha_S showerProb *= as; } // Done for FSR } else { string message="Error in History::getProb: Radiation could not be"; message+=" interpreted as FSR or ISR."; infoPtr->errorMsg(message); } if (showerProb <= 0.) showerProb = 0.; // // Different coupling constants for qcd and ew splittings // if ( state[Emt].colType() != 0 ) { // AlphaStrong* asFSR = mergingHooksPtr->AlphaS_FSR(); // double as = (*asFSR).alphaS(91.188*91.188) / (2.*M_PI); // showerProb *= as; // } else { // AlphaEM* aEMFSR = mergingHooksPtr->AlphaEM_FSR(); // double aEM = (*aEMFSR).alphaEM(91.188*91.188) / (2.*M_PI); // showerProb *= aEM; // } // Done return showerProb; } //-------------------------------------------------------------------------- // Set up the beams (fill the beam particles with the correct // current incoming particles) to allow calculation of splitting // probability. // For interleaved evolution, set assignments dividing PDFs into // sea and valence content. This assignment is, until a history path // is chosen and a first trial shower performed, not fully correct // (since content is chosen form too high x and too low scale). The // assignment used for reweighting will be corrected after trial // showering void History::setupBeams() { // Do nothing for empty event, possible if sequence of // clusterings was ill-advised in that it results in // colour-disconnected states if (state.size() < 4) return; // Do nothing for e+e- beams if ( state[3].colType() == 0 ) return; if ( state[4].colType() == 0 ) return; // Incoming partons to hard process are stored in slots 3 and 4. int inS = 0; int inP = 0; int inM = 0; for(int i=0;i< int(state.size()); ++i) { if (state[i].mother1() == 1) inP = i; if (state[i].mother1() == 2) inM = i; } // Save some info before clearing beams // Mothers of incoming partons companion code int motherPcompRes = -1; int motherMcompRes = -1; bool sameFlavP = false; bool sameFlavM = false; if (mother) { int inMotherP = 0; int inMotherM = 0; for(int i=0;i< int(mother->state.size()); ++i) { if (mother->state[i].mother1() == 1) inMotherP = i; if (mother->state[i].mother1() == 2) inMotherM = i; } sameFlavP = (state[inP].id() == mother->state[inMotherP].id()); sameFlavM = (state[inM].id() == mother->state[inMotherM].id()); motherPcompRes = (sameFlavP) ? beamA[0].companion() : -2; motherMcompRes = (sameFlavM) ? beamB[0].companion() : -2; } // Append the current incoming particles to the beam beamA.clear(); beamB.clear(); // Get energy of incoming particles double Ep = 2. * state[inP].e(); double Em = 2. * state[inM].e(); // If incoming partons are massive then recalculate to put them massless. if (state[inP].m() != 0. || state[inM].m() != 0.) { Ep = state[inP].pPos() + state[inM].pPos(); Em = state[inP].pNeg() + state[inM].pNeg(); } // Add incoming hard-scattering partons to list in beam remnants. double x1 = Ep / state[inS].m(); beamA.append( inP, state[inP].id(), x1); double x2 = Em / state[inS].m(); beamB.append( inM, state[inM].id(), x2); // Scale. For ME multiplicity history, put scale to mu_F // (since sea/valence quark content is chosen from this scale) double scalePDF = (mother) ? scale : infoPtr->QFac(); // Find whether incoming partons are valence or sea. Store. // Can I do better, e.g. by setting the scale to the hard process // scale (= M_W) or by replacing one of the x values by some x/z?? beamA.xfISR( 0, state[inP].id(), x1, scalePDF*scalePDF); if (!mother) { beamA.pickValSeaComp(); } else { beamA[0].companion(motherPcompRes); } beamB.xfISR( 0, state[inM].id(), x2, scalePDF*scalePDF); if (!mother) { beamB.pickValSeaComp(); } else { beamB[0].companion(motherMcompRes); } } //-------------------------------------------------------------------------- // Calculate the PDF ratio used in the argument of the no-emission // probability double History::pdfForSudakov() { // Do nothing for e+e- beams if ( state[3].colType() == 0 ) return 1.0; if ( state[4].colType() == 0 ) return 1.0; // Check if splittings was ISR or FSR bool FSR = ( mother->state[clusterIn.emittor].isFinal() && mother->state[clusterIn.recoiler].isFinal()); bool FSRinRec = ( mother->state[clusterIn.emittor].isFinal() && !mother->state[clusterIn.recoiler].isFinal()); // Done for pure FSR if (FSR) return 1.0; int iInMother = (FSRinRec)? clusterIn.recoiler : clusterIn.emittor; // Find side of event that was reclustered int side = ( mother->state[iInMother].pz() > 0 ) ? 1 : -1; int inP = 0; int inM = 0; for(int i=0;i< int(state.size()); ++i) { if (state[i].mother1() == 1) inP = i; if (state[i].mother1() == 2) inM = i; } // Save mother id int idMother = mother->state[iInMother].id(); // Find daughter position and id int iDau = (side == 1) ? inP : inM; int idDaughter = state[iDau].id(); // Get mother x value double xMother = 2. * mother->state[iInMother].e() / mother->state[0].e(); // Get daughter x value of daughter double xDaughter = 2.*state[iDau].e() / state[0].e(); // x1 before isr // Calculate pdf ratio double ratio = getPDFratio(side, true, false, idMother, xMother, scale, idDaughter, xDaughter, scale); // For FSR with incoming recoiler, maximally return 1.0, as // is done in Pythia::TimeShower. // For ISR, return ratio return ( (FSRinRec)? min(1.,ratio) : ratio); } //-------------------------------------------------------------------------- // Calculate the hard process matrix element to include in the selection // probability. double History::hardProcessME( const Event& event ) { // Get hard process. string process = mergingHooksPtr->getProcessString(); double result = 1.; if ( process.compare("pp>e+ve") == 0 || process.compare("pp>e-ve~") == 0 || process.compare("pp>LEPTONS,NEUTRINOS") == 0 ) { // Do nothing for incomplete process. int nFinal = 0; for ( int i=0; i < int(event.size()); ++i ) if ( event[i].isFinal() ) nFinal++; if ( nFinal != 2 ) return 1.; // Get W-boson mass and width. double mW = particleDataPtr->m0(24); double gW = particleDataPtr->mWidth(24) / mW; // Get incoming particles. int inP = (event[3].pz() > 0) ? 3 : 4; int inM = (event[3].pz() > 0) ? 4 : 3; // Get outgoing particles. int outP = 0; for ( int i=0; i < int(event.size()); ++i ) { if ( event[i].isFinal() && event[i].px() > 0 ) outP = i; } // Get Mandelstam variables. double sH = (event[inP].p() + event[inM].p()).m2Calc(); double tH = (event[inP].p() - event[outP].p()).m2Calc(); double uH = - sH - tH; // Return kinematic part of matrix element. result = ( 1. + (tH - uH)/sH ) / ( pow2(sH - mW*mW) + pow2(sH*gW) ); } else result = mergingHooksPtr->hardProcessME(event); return result; } //-------------------------------------------------------------------------- // Perform the clustering of the current state and return the // clustered state. // IN Clustering : rad,rec,emt triple to be clustered to two partons // OUT clustered state Event History::cluster( const Clustering & inSystem ) { // Initialise tags of particles to be changed int Rad = inSystem.emittor; int Rec = inSystem.recoiler; int Emt = inSystem.emitted; // Initialise eCM,mHat double eCM = state[0].e(); // Flags for type of radiation int radType = state[Rad].isFinal() ? 1 : -1; int recType = state[Rec].isFinal() ? 1 : -1; // Construct the clustered event Event NewEvent = Event(); NewEvent.init("(hard process-modified)", particleDataPtr); NewEvent.clear(); // Copy all unchanged particles to NewEvent for (int i = 0; i < state.size(); ++i) if ( i != Rad && i != Rec && i != Emt ) NewEvent.append( state[i] ); // Copy all the junctions one by one for (int i = 0; i < state.sizeJunction(); ++i) NewEvent.appendJunction( state.getJunction(i) ); // Find an appropriate scale for the hard process double mu = choseHardScale(state); // Initialise scales for new event NewEvent.saveSize(); NewEvent.saveJunctionSize(); NewEvent.scale(mu); NewEvent.scaleSecond(mu); // Set properties of radiator/recoiler after the clustering // Recoiler properties will be unchanged Particle RecBefore = Particle( state[Rec] ); RecBefore.setEvtPtr(&NewEvent); RecBefore.daughters(0,0); // Find flavour of radiator before splitting int radID = getRadBeforeFlav(Rad, Emt, state); int recID = state[Rec].id(); Particle RadBefore = Particle( state[Rad] ); RadBefore.setEvtPtr(&NewEvent); RadBefore.id(radID); RadBefore.daughters(0,0); // Put dummy values for colours RadBefore.cols(RecBefore.acol(),RecBefore.col()); // Reset status if the reclustered radiator is a resonance. if ( particleDataPtr->isResonance(radID) && radType == 1) RadBefore.status(state[Rad].status()); // Put mass for radiator and recoiler if (radType == 1 ) RadBefore.m(particleDataPtr->m0(radID)); else RadBefore.m(0.0); if (recType == 1 ) RecBefore.m(particleDataPtr->m0(recID)); else RecBefore.m(0.0); // Construct momenta and colours of clustered particles // ISR/FSR splittings are treated differently if ( radType + recType == 2 && state[Emt].idAbs() != 24 ) { // Clustering of final(rad)/final(rec) dipole splitting // Get eCM of (rad,rec,emt) triple Vec4 sum = state[Rad].p() + state[Rec].p() + state[Emt].p(); double eCMME = sum.mCalc(); // Define radiator and recoiler back-to-back in the dipole // rest frame [=(state[rad]+state[emt])+state[rec] rest frame] Vec4 Rad4mom; Vec4 Rec4mom; double mDsq = pow2(eCMME); // If possible, keep the invariant mass of the radiator. double mRsq = (radID == state[Rad].id() ) ? abs(state[Rad].p().m2Calc()) : pow2(particleDataPtr->m0(radID)); double mSsq = abs(state[Rec].p().m2Calc()); double a = 0.5*sqrt(mDsq); double b = 0.25*(mRsq - mSsq) / a; double c = sqrt(pow2(a) + pow2(b) - 2.*a*b - mSsq); Rad4mom.p( 0., 0., c, a+b); Rec4mom.p( 0., 0.,-c, a-b); // Find boost from Rad4mom+Rec4mom rest frame to event cm frame Vec4 old1 = Vec4(state[Rad].p() + state[Emt].p()); Vec4 old2 = Vec4(state[Rec].p()); RotBstMatrix fromCM; fromCM.fromCMframe(old1, old2); // Transform momenta Rad4mom.rotbst(fromCM); Rec4mom.rotbst(fromCM); RadBefore.p(Rad4mom); RecBefore.p(Rec4mom); } else if ( radType + recType == 2 && state[Emt].idAbs() == 24 ) { // Clustering of final(rad)/final(rec) dipole splitting // Get eCM of (rad,rec,emt) triple Vec4 sum = state[Rad].p() + state[Rec].p() + state[Emt].p(); double eCMME = sum.mCalc(); // Define radiator and recoiler back-to-back in the dipole // rest frame [=(state[rad]+state[emt])+state[rec] rest frame] Vec4 Rad4mom; Vec4 Rec4mom; double mDsq = pow2(eCMME); // If possible, keep the invariant mass of the radiator. double mRsq = (radID == state[Rad].id() ) ? abs(state[Rad].p().m2Calc()) : pow2(particleDataPtr->m0(radID)); double mSsq = abs(state[Rec].p().m2Calc()); double a = 0.5*sqrt(mDsq); double b = 0.25*(mRsq - mSsq) / a; double c = sqrt(pow2(a) + pow2(b) - 2.*a*b - mSsq); Rad4mom.p( 0., 0., c, a+b); Rec4mom.p( 0., 0.,-c, a-b); // Find boost from Rad4mom+Rec4mom rest frame to event cm frame Vec4 old1 = Vec4(state[Rad].p() + state[Emt].p()); Vec4 old2 = Vec4(state[Rec].p()); RotBstMatrix fromCM; fromCM.fromCMframe(old1, old2); // Transform momenta Rad4mom.rotbst(fromCM); Rec4mom.rotbst(fromCM); RadBefore.p(Rad4mom); RecBefore.p(Rec4mom); } else if ( radType + recType == 0 ) { // Clustering of final(rad)/initial(rec) dipole splitting // Get eCM of (rad,rec,emt) triple Vec4 sum = state[Rad].p() + state[Rec].p() + state[Emt].p(); double eCMME = sum.mCalc(); // Define radiator and recoiler back-to-back in the dipole // rest frame [=(state[rad]+state[emt])+state[rec] rest frame] Vec4 Rad4mom; Vec4 Rec4mom; double mDsq = pow2(eCMME); // If possible, keep the invariant mass of the radiator. double mRsq = (radID == state[Rad].id() ) ? abs(state[Rad].p().m2Calc()) : pow2(particleDataPtr->m0(radID)); double mSsq = abs(state[Rec].p().m2Calc()); double a = 0.5*sqrt(mDsq); double b = 0.25*(mRsq - mSsq) / a; double c = sqrt(pow2(a) + pow2(b) - 2.*a*b - mSsq); Rad4mom.p( 0., 0., c, a+b); Rec4mom.p( 0., 0.,-c, a-b); // Find boost from Rad4mom+Rec4mom rest frame to event cm frame Vec4 old1 = Vec4(state[Rad].p() + state[Emt].p()); Vec4 old2 = Vec4(state[Rec].p()); RotBstMatrix fromCM; fromCM.fromCMframe(old1, old2); // Transform momenta Rad4mom.rotbst(fromCM); Rec4mom.rotbst(fromCM); // Rescale recoiler momentum Rec4mom = 2.*state[Rec].p() - Rec4mom; RadBefore.p(Rad4mom); RecBefore.p(Rec4mom); // Set mass of initial recoiler to zero RecBefore.m( 0.0 ); } else { // Clustering of initial(rad)/initial(rec) dipole splitting // We want to cluster: Meaning doing the inverse of a process // ( pDaughter + pRecoiler -> pOut ) // ==> ( pMother + pPartner -> pOut' + pSister ) // produced by an initial state splitting. The matrix element // provides us with pMother, pPartner, pSister and pOut' Vec4 pMother( state[Rad].p() ); Vec4 pSister( state[Emt].p() ); Vec4 pPartner( state[Rec].p() ); Vec4 pDaughter( 0.,0.,0.,0. ); Vec4 pRecoiler( 0.,0.,0.,0. ); // Find side that radiates event (mother moving in // sign * p_z direction) int sign = state[Rad].pz() > 0 ? 1 : -1; // Find rotation by phi that would have been done for a // splitting daughter -> mother + sister double phi = pSister.phi(); // Find rotation with -phi RotBstMatrix rot_by_mphi; rot_by_mphi.rot(0.,-phi); // Find rotation with +phi RotBstMatrix rot_by_pphi; rot_by_pphi.rot(0.,phi); // Transform pMother and outgoing momenta pMother.rotbst( rot_by_mphi ); pSister.rotbst( rot_by_mphi ); pPartner.rotbst( rot_by_mphi ); for(int i=3; i< NewEvent.size(); ++i) NewEvent[i].rotbst( rot_by_mphi ); // Get mother and partner x values // x1 after isr double x1 = 2. * pMother.e() / eCM; // x2 after isr double x2 = 2. * pPartner.e() / eCM; pDaughter.p( pMother - pSister); pRecoiler.p( pPartner ); // Find boost from event cm frame to rest frame of // of-shell daughter + on-shell recoiler RotBstMatrix from_CM_to_DR; if (sign == 1) from_CM_to_DR.toCMframe(pDaughter, pRecoiler); else from_CM_to_DR.toCMframe(pRecoiler, pDaughter); // Transform all momenta pMother.rotbst( from_CM_to_DR ); pPartner.rotbst( from_CM_to_DR ); pSister.rotbst( from_CM_to_DR ); for(int i=3; i< NewEvent.size(); ++i) NewEvent[i].rotbst( from_CM_to_DR ); // Find theta angle between pMother and z-axis and undo // rotation that would have been done by shower double theta = pMother.theta(); if ( pMother.px() < 0. ) theta *= -1.; if (sign == -1) theta += M_PI; // Find rotation by +theta RotBstMatrix rot_by_ptheta; rot_by_ptheta.rot(theta, 0.); // Transform all momenta pMother.rotbst( rot_by_ptheta ); pPartner.rotbst( rot_by_ptheta ); pSister.rotbst( rot_by_ptheta ); for(int i=3; i< NewEvent.size(); ++i) NewEvent[i].rotbst( rot_by_ptheta ); // Find z of the splitting Vec4 qDip( pMother - pSister); Vec4 qAfter(pMother + pPartner); Vec4 qBefore(qDip + pPartner); double z = qBefore.m2Calc() / qAfter.m2Calc(); // Calculate new e_CM^2 double x1New = z*x1; // x1 before isr double x2New = x2; // x2 before isr double sHat = x1New*x2New*eCM*eCM; // Construct daughter and recoiler momenta pDaughter.p( 0., 0., sign*0.5*sqrt(sHat), 0.5*sqrt(sHat)); pRecoiler.p( 0., 0., -sign*0.5*sqrt(sHat), 0.5*sqrt(sHat)); // Find boost from current (daughter+recoiler rest frame) // frame to rest frame of daughter+unchanged recoiler to // recover the old x2 value RotBstMatrix from_DR_to_CM; from_DR_to_CM.bst( 0., 0., sign*( x1New - x2New ) / ( x1New + x2New ) ); // Correct for momentum mismatch by transforming all momenta pMother.rotbst( from_DR_to_CM ); pPartner.rotbst( from_DR_to_CM ); pSister.rotbst( from_DR_to_CM ); pDaughter.rotbst( from_DR_to_CM ); pRecoiler.rotbst( from_DR_to_CM ); for(int i=3; i< NewEvent.size(); ++i) NewEvent[i].rotbst( from_DR_to_CM ); // Transform pMother and outgoing momenta pMother.rotbst( rot_by_pphi ); pPartner.rotbst( rot_by_pphi ); pSister.rotbst( rot_by_pphi ); pDaughter.rotbst( rot_by_pphi ); pRecoiler.rotbst( rot_by_pphi ); for(int i=3; i< NewEvent.size(); ++i) NewEvent[i].rotbst( rot_by_pphi ); // Set momenta of particles to be attached to new event record RecBefore.p( pRecoiler ); RadBefore.p( pDaughter ); } // Put some dummy production scales for RecBefore, RadBefore RecBefore.scale(mu); RadBefore.scale(mu); // Append new recoiler and find new radiator colour NewEvent.append(RecBefore); // Assign the correct colour to re-clustered radiator. // Keep old radiator colours for electroweak emission. int emtID = state[Emt].id(); if ( emtID == 22 || emtID == 23 || abs(emtID) == 24 ) RadBefore.cols( state[Rad].col(), state[Rad].acol() ); // For QCD, carefully construct colour. else if ( !connectRadiator( RadBefore, radType, RecBefore, recType, NewEvent ) ) { // Could happen if previous clustering produced several colour // singlett subsystems in the event NewEvent.reset(); return NewEvent; } // Build the clustered event Event outState = Event(); outState.init("(hard process-modified)", particleDataPtr); outState.clear(); // Copy system and incoming beam particles to outState for (int i = 0; i < 3; ++i) outState.append( NewEvent[i] ); // Copy all the junctions one by one for (int i = 0; i < state.sizeJunction(); ++i) outState.appendJunction( state.getJunction(i) ); // Initialise scales for new event outState.saveSize(); outState.saveJunctionSize(); outState.scale(mu); outState.scaleSecond(mu); bool radAppended = false; bool recAppended = false; int size = int(outState.size()); // Save position of radiator in new event record int radPos = 0; // Append first incoming particle if ( RecBefore.mother1() == 1) { outState.append( RecBefore ); recAppended = true; } else if ( RadBefore.mother1() == 1 ) { radPos = outState.append( RadBefore ); radAppended = true; } else { // Find second incoming in input event int in1 = 0; for(int i=0; i < int(state.size()); ++i) if (state[i].mother1() == 1) in1 =i; outState.append( state[in1] ); size++; } // Append second incoming particle if ( RecBefore.mother1() == 2) { outState.append( RecBefore ); recAppended = true; } else if ( RadBefore.mother1() == 2 ) { radPos = outState.append( RadBefore ); radAppended = true; } else { // Find second incoming in input event int in2 = 0; for(int i=0; i < int(state.size()); ++i) if (state[i].mother1() == 2) in2 =i; outState.append( state[in2] ); size++; } // Append new recoiler if not done already if (!recAppended && !RecBefore.isFinal()) { recAppended = true; outState.append( RecBefore); } // Append new radiator if not done already if (!radAppended && !RadBefore.isFinal()) { radAppended = true; radPos = outState.append( RadBefore); } // Append intermediate particle // (careful not to append reclustered recoiler) for (int i = 0; i < int(NewEvent.size()-1); ++i) if (NewEvent[i].status() == -22) outState.append( NewEvent[i] ); // Append final state particles, resonances first for (int i = 0; i < int(NewEvent.size()-1); ++i) if (NewEvent[i].status() == 22) outState.append( NewEvent[i] ); // Then start appending partons if (!radAppended && RadBefore.statusAbs() == 22) radPos = outState.append(RadBefore); if (!recAppended) outState.append(RecBefore); if (!radAppended && RadBefore.statusAbs() != 22) radPos = outState.append(RadBefore); // Then partons (not reclustered recoiler) for(int i = 0; i < int(NewEvent.size()-1); ++i) if ( NewEvent[i].status() != 22 && NewEvent[i].colType() != 0 && NewEvent[i].isFinal()) outState.append( NewEvent[i] ); // Then the rest for(int i = 0; i < int(NewEvent.size()-1); ++i) if ( NewEvent[i].status() != 22 && NewEvent[i].colType() == 0 && NewEvent[i].isFinal() ) outState.append( NewEvent[i]); // Find intermediate and respective daughters vector PosIntermediate; vector PosDaughter1; vector PosDaughter2; for(int i=0; i < int(outState.size()); ++i) if (outState[i].status() == -22) { PosIntermediate.push_back(i); int d1 = outState[i].daughter1(); int d2 = outState[i].daughter2(); // Find daughters in output state int daughter1 = FindParticle( state[d1], outState); int daughter2 = FindParticle( state[d2], outState); // If both daughters found, done // Else put first final particle as first daughter // and last final particle as second daughter if (daughter1 > 0) PosDaughter1.push_back( daughter1); else { daughter1 = 0; while(!outState[daughter1].isFinal() ) daughter1++; PosDaughter1.push_back( daughter1); } if (daughter2 > 0) PosDaughter2.push_back( daughter2); else { daughter2 = outState.size()-1; while(!outState[daughter2].isFinal() ) daughter2--; PosDaughter2.push_back( daughter2); } } // Set daughters and mothers for(int i=0; i < int(PosIntermediate.size()); ++i) { outState[PosIntermediate[i]].daughters(PosDaughter1[i],PosDaughter2[i]); outState[PosDaughter1[i]].mother1(PosIntermediate[i]); outState[PosDaughter2[i]].mother1(PosIntermediate[i]); } // Find range of final state partons int minParFinal = int(outState.size()); int maxParFinal = 0; for(int i=0; i < int(outState.size()); ++i) if (outState[i].mother1() == 3 && outState[i].mother2() == 4) { minParFinal = min(i,minParFinal); maxParFinal = max(i,maxParFinal); } if (minParFinal == maxParFinal) maxParFinal = 0; outState[3].daughters(minParFinal,maxParFinal); outState[4].daughters(minParFinal,maxParFinal); // Update event properties outState.saveSize(); outState.saveJunctionSize(); // Almost there... // If an intermediate coloured parton exists which was directly // colour connected to the radiator before the splitting, and the // radiator before and after the splitting had only one colour, problems // will arise since the colour of the radiator will be changed, whereas // the intermediate parton still has the old colour. In effect, this // means that when setting up a event for trial showering, one colour will // be free. // Hence, check for an intermediate coloured triplet resonance has been // colour-connected to the "old" radiator. // Find resonance int iColRes = 0; if ( radType == -1 && state[Rad].colType() == 1) { // Find resonance connected to initial colour for(int i=0; i < int(state.size()); ++i) if ( i != Rad && i != Emt && i != Rec && state[i].status() == -22 && state[i].col() == state[Rad].col() ) iColRes = i; } else if ( radType == -1 && state[Rad].colType() == -1) { // Find resonance connected to initial anticolour for(int i=0; i < int(state.size()); ++i) if ( i != Rad && i != Emt && i != Rec && state[i].status() == -22 && state[i].acol() == state[Rad].acol() ) iColRes = i; } else if ( radType == 1 && state[Rad].colType() == 1) { // Find resonance connected to final state colour for(int i=0; i < int(state.size()); ++i) if ( i != Rad && i != Emt && i != Rec && state[i].status() == -22 && state[i].col() == state[Rad].col() ) iColRes = i; } else if ( radType == 1 && state[Rad].colType() == -1) { // Find resonance connected to final state anticolour for(int i=0; i < int(state.size()); ++i) if ( i != Rad && i != Emt && i != Rec && state[i].status() == -22 && state[i].acol() == state[Rad].acol() ) iColRes = i; } if (iColRes > 0) { // Now find this resonance in the reclustered state int iColResNow = FindParticle( state[iColRes], outState); // Find reclustered radiator colours int radCol = outState[radPos].col(); int radAcl = outState[radPos].acol(); // Find resonance radiator colours int resCol = outState[iColResNow].col(); int resAcl = outState[iColResNow].acol(); // Check if any of the reclustered radiators colours match the resonance bool matchesRes = (radCol > 0 && ( radCol == resCol || radCol == resAcl)) || (radAcl > 0 && ( radAcl == resCol || radAcl == resAcl)); // If a resonance has been found, but no colours match, change // the colour of the resonance if (!matchesRes && iColResNow > 0) { if ( radType == -1 && outState[radPos].colType() == 1) outState[iColResNow].col(radCol); else if ( radType ==-1 && outState[radPos].colType() ==-1) outState[iColResNow].acol(radAcl); else if ( radType == 1 && outState[radPos].colType() == 1) outState[iColResNow].col(radCol); else if ( radType == 1 && outState[radPos].colType() ==-1) outState[iColResNow].acol(radAcl); } // If a resonance has been found, but no colours match, and the position // of the resonance in the event record has been changed, update the // radiator mother if (!matchesRes && iColResNow > 0 && iColRes != iColResNow) outState[radPos].mother1(iColResNow); } // If event is not constructed properly, return false if ( !validEvent(outState) ) { outState.reset(); return outState; } // Remember position of reclustered radiator in state iReclusteredNew = radPos; // Done return outState; } //-------------------------------------------------------------------------- // Function to get the flavour of the radiator before the splitting // for clustering // IN int : Flavour of the radiator after the splitting // int : Flavour of the emitted after the splitting // OUT int : Flavour of the radiator before the splitting int History::getRadBeforeFlav(const int RadAfter, const int EmtAfter, const Event& event) { int type = event[RadAfter].isFinal() ? 1 :-1; int emtID = event[EmtAfter].id(); int radID = event[RadAfter].id(); int emtCOL = event[EmtAfter].col(); int radCOL = event[RadAfter].col(); int emtACL = event[EmtAfter].acol(); int radACL = event[RadAfter].acol(); bool colConnected = ((type == 1) && ( (emtCOL !=0 && (emtCOL ==radACL)) || (emtACL !=0 && (emtACL ==radCOL)) )) ||((type ==-1) && ( (emtCOL !=0 && (emtCOL ==radCOL)) || (emtACL !=0 && (emtACL ==radACL)) )); // QCD splittings // Gluon radiation if ( emtID == 21 ) return radID; // Final state gluon splitting if ( type == 1 && emtID == -radID && !colConnected ) return 21; // Initial state s-channel gluon splitting if ( type ==-1 && radID == 21 ) return -emtID; // Initial state t-channel gluon splitting if ( type ==-1 && !colConnected && emtID != 21 && radID != 21 && abs(emtID) < 10 && abs(radID) < 10) return 21; // SQCD splittings int radSign = (radID < 0) ? -1 : 1; int offsetL = 1000000; int offsetR = 2000000; // Gluino radiation if ( emtID == 1000021 ) { // Gluino radiation combined with quark yields squark. if (abs(radID) < 10 ) { int offset = offsetL; // Check if righthanded squark present. If so, make the reclustered // squark match. Works for squark pair production + gluino emission. for (int i=0; i < int(event.size()); ++i) if ( event[i].isFinal() && event[i].idAbs() < offsetR+10 && event[i].idAbs() > offsetR) offset = offsetR; return radSign*(abs(radID)+offset); } // Gluino radiation combined with squark yields quark. if (abs(radID) > offsetL && abs(radID) < offsetL+10 ) return radSign*(abs(radID)-offsetL); if (abs(radID) > offsetR && abs(radID) < offsetR+10 ) return radSign*(abs(radID)-offsetR); // Gluino radiation off gluon yields gluino. if (radID == 21 ) return emtID; } int emtSign = (emtID < 0) ? -1 : 1; // Get PDG numbering offsets. int emtOffset = 0; if ( abs(emtID) > offsetL && abs(emtID) < offsetL+10 ) emtOffset = offsetL; if ( abs(emtID) > offsetR && abs(emtID) < offsetR+10 ) emtOffset = offsetR; int radOffset = 0; if ( abs(radID) > offsetL && abs(radID) < offsetL+10 ) radOffset = offsetL; if ( abs(radID) > offsetR && abs(radID) < offsetR+10 ) radOffset = offsetR; // Final state gluino splitting if ( type == 1 && !colConnected ) { // Emitted squark, radiating quark. if ( emtOffset > 0 && radOffset == 0 && emtSign*(abs(emtID) - emtOffset) == -radID ) return 1000021; // Emitted quark, radiating squark. if ( emtOffset == 0 && radOffset > 0 && emtID == -radSign*(abs(radID) - radOffset) ) return 1000021; } // Initial state s-channel gluino splitting if ( type ==-1 && radID == 1000021 ) { // Quark entering underlying hard process. if ( emtOffset > 0 ) return -emtSign*(abs(emtID) - emtOffset); // Squark entering underlying hard process. else return -emtSign*(abs(emtID) + emtOffset); } // Initial state t-channel gluino splitting. if ( type ==-1 && ( (abs(emtID) > offsetL && abs(emtID) < offsetL+10) || (abs(emtID) > offsetR && abs(emtID) < offsetR+10)) && ( (abs(radID) > offsetL && abs(radID) < offsetL+10) || (abs(radID) > offsetR && abs(radID) < offsetR+10)) && emtSign*(abs(emtID)+emtOffset) == radSign*(abs(radID) - radOffset) && !colConnected ) { return 1000021; } // Electroweak splittings splittings // Photon / Z radiation: Calculate invariant mass of system double m2final = (event[RadAfter].p()+ event[EmtAfter].p()).m2Calc(); if ( emtID == 22 || emtID == 23 ) return radID; // Final state Photon splitting if ( type == 1 && emtID == -radID && colConnected && sqrt(m2final) <= 10. ) return 22; // Final state Photon splitting if ( type == 1 && emtID == -radID && colConnected && sqrt(m2final) > 10. ) return 23; // Initial state s-channel photon/ Z splitting if ( type ==-1 && (radID == 22 || radID == 23) ) return -emtID; // Initial state t-channel photon / Z splitting: Always bookkeep as photon if ( type ==-1 && abs(emtID) < 10 && abs(radID) < 10 && colConnected ) return 22; // W+ radiation // Final state W+ splitting if ( emtID == 24 && radID < 0 ) return radID + 1; if ( emtID == 24 && radID > 0 ) return radID + 1; // W- radiation // Final state W- splitting if ( emtID ==-24 && radID < 0 ) return radID - 1; if ( emtID ==-24 && radID > 0 ) return radID - 1; // Done. return 0; } //-------------------------------------------------------------------------- // Function to properly colour-connect the radiator to the rest of // the event, as needed during clustering // IN Particle& : Particle to be connected // Particle : Recoiler forming a dipole with Radiator // Event : event to which Radiator shall be appended // OUT true : Radiator could be connected to the event // false : Radiator could not be connected to the // event or the resulting event was // non-valid bool History::connectRadiator( Particle& Radiator, const int RadType, const Particle& Recoiler, const int RecType, const Event& event ) { // Start filling radiator colour indices with dummy values Radiator.cols( -1, -1 ); // Radiator should always be colour-connected to recoiler. // Three cases (rad = Anti-Quark, Quark, Gluon) to be considered if ( Radiator.colType() == -1 ) { // For final state antiquark radiator, the anticolour is fixed // by the final / initial state recoiler colour / anticolour if ( RadType + RecType == 2 ) Radiator.cols( 0, Recoiler.col()); else if ( RadType + RecType == 0 ) Radiator.cols( 0, Recoiler.acol()); // For initial state antiquark radiator, the anticolour is fixed // by the colour of the emitted gluon (which will be the // leftover anticolour of a final state particle or the leftover // colour of an initial state particle ( = the recoiler)) else { // Set colour of antiquark radiator to zero Radiator.col( 0 ); for (int i = 0; i < event.size(); ++i) { int col = event[i].col(); int acl = event[i].acol(); if ( event[i].isFinal()) { // Search for leftover anticolour in final / initial state if ( acl > 0 && FindCol(acl,i,0,event,1,true) == 0 && FindCol(acl,i,0,event,2,true) == 0 ) Radiator.acol(event[i].acol()); } else { // Search for leftover colour in initial / final state if ( col > 0 && FindCol(col,i,0,event,1,true) == 0 && FindCol(col,i,0,event,2,true) == 0 ) Radiator.acol(event[i].col()); } } // end loop over particles in event record } } else if ( Radiator.colType() == 1 ) { // For final state quark radiator, the colour is fixed // by the final / initial state recoiler anticolour / colour if ( RadType + RecType == 2 ) Radiator.cols( Recoiler.acol(), 0); else if ( RadType + RecType == 0 ) Radiator.cols( Recoiler.col(), 0); // For initial state quark radiator, the colour is fixed // by the anticolour of the emitted gluon (which will be the // leftover colour of a final state particle or the leftover // anticolour of an initial state particle ( = the recoiler)) else { // Set anticolour of quark radiator to zero Radiator.acol( 0 ); for (int i = 0; i < event.size(); ++i) { int col = event[i].col(); int acl = event[i].acol(); if ( event[i].isFinal()) { // Search for leftover colour in final / initial state if ( col > 0 && FindCol(col,i,0,event,1,true) == 0 && FindCol(col,i,0,event,2,true) == 0) Radiator.col(event[i].col()); } else { // Search for leftover anticolour in initial / final state if ( acl > 0 && FindCol(acl,i,0,event,1,true) == 0 && FindCol(acl,i,0,event,2,true) == 0) Radiator.col(event[i].acol()); } } // end loop over particles in event record } // end distinction between fsr / fsr+initial recoiler / isr } else if ( Radiator.colType() == 2 ) { // For a gluon radiator, one (anticolour) colour index is defined // by the recoiler colour (anticolour). // The remaining index is chosen to match the free index in the // event // Search for leftover colour (anticolour) in the final state for (int i = 0; i < event.size(); ++i) { int col = event[i].col(); int acl = event[i].acol(); int iEx = i; if ( event[i].isFinal()) { if ( col > 0 && FindCol(col,iEx,0,event,1,true) == 0 && FindCol(col,iEx,0,event,2,true) == 0) { if (Radiator.status() < 0 ) Radiator.col(event[i].col()); else Radiator.acol(event[i].col()); } if ( acl > 0 && FindCol(acl,iEx,0,event,2,true) == 0 && FindCol(acl,iEx,0,event,1,true) == 0 ) { if (Radiator.status() < 0 ) Radiator.acol(event[i].acol()); else Radiator.col(event[i].acol()); } } else { if ( col > 0 && FindCol(col,iEx,0,event,1,true) == 0 && FindCol(col,iEx,0,event,2,true) == 0) { if (Radiator.status() < 0 ) Radiator.acol(event[i].col()); else Radiator.col(event[i].col()); } if ( acl > 0 && (FindCol(acl,iEx,0,event,2,true) == 0 && FindCol(acl,iEx,0,event,1,true) == 0)) { if (Radiator.status() < 0 ) Radiator.col(event[i].acol()); else Radiator.acol(event[i].acol()); } } } // end loop over particles in event record } // end cases of different radiator colour type // If either colour or anticolour has not been set, return false if (Radiator.col() < 0 || Radiator.acol() < 0) return false; // Done return true; } //-------------------------------------------------------------------------- // Function to find a colour (anticolour) index in the input event // IN int col : Colour tag to be investigated // int iExclude1 : Identifier of first particle to be excluded // from search // int iExclude2 : Identifier of second particle to be excluded // from search // Event event : event to be searched for colour tag // int type : Tag to define if col should be counted as // colour (type = 1) [->find anti-colour index // contracted with col] // anticolour (type = 2) [->find colour index // contracted with col] // OUT int : Position of particle in event record // contraced with col [0 if col is free tag] int History::FindCol(int col, int iExclude1, int iExclude2, const Event& event, int type, bool isHardIn) { bool isHard = isHardIn; int index = 0; if (isHard) { // Search event record for matching colour & anticolour for(int n = 0; n < event.size(); ++n) { if ( n != iExclude1 && n != iExclude2 && event[n].colType() != 0 &&( event[n].status() > 0 // Check outgoing || event[n].status() == -21) ) { // Check incoming if ( event[n].acol() == col ) { index = -n; break; } if ( event[n].col() == col ) { index = n; break; } } } } else { // Search event record for matching colour & anticolour for(int n = 0; n < event.size(); ++n) { if ( n != iExclude1 && n != iExclude2 && event[n].colType() != 0 &&( event[n].status() == 43 // Check outgoing from ISR || event[n].status() == 51 // Check outgoing from FSR || event[n].status() == -41 // first initial || event[n].status() == -42) ) { // second initial if ( event[n].acol() == col ) { index = -n; break; } if ( event[n].col() == col ) { index = n; break; } } } } // if no matching colour / anticolour has been found, return false if ( type == 1 && index < 0) return abs(index); if ( type == 2 && index > 0) return abs(index); return 0; } //-------------------------------------------------------------------------- // Function to in the input event find a particle with quantum // numbers matching those of the input particle // IN Particle : Particle to be searched for // Event : Event to be searched in // OUT int : > 0 : Position of matching particle in event // < 0 : No match in event int History::FindParticle( const Particle& particle, const Event& event, bool checkStatus ) { int index = -1; for ( int i = int(event.size()) - 1; i > 0; --i ) if ( event[i].id() == particle.id() && event[i].colType() == particle.colType() && event[i].chargeType() == particle.chargeType() && event[i].col() == particle.col() && event[i].acol() == particle.acol() && event[i].charge() == particle.charge() ) { index = i; break; } if ( checkStatus && event[index].status() != particle.status() ) index = -1; return index; } //-------------------------------------------------------------------------- // Function to get the colour of the radiator before the splitting // for clustering // IN int : Position of the radiator after the splitting, in the event // int : Position of the emitted after the splitting, in the event // Event : Reference event // OUT int : Colour of the radiator before the splitting int History::getRadBeforeCol(const int rad, const int emt, const Event& event) { // Save type of splitting int type = (event[rad].isFinal()) ? 1 :-1; // Get flavour of radiator after potential clustering int radBeforeFlav = getRadBeforeFlav(rad,emt,event); // Get colours of the radiator before the potential clustering int radBeforeCol = -1; // Get reconstructed gluon colours if (radBeforeFlav == 21) { // Start with quark emissions in FSR if (type == 1 && event[emt].id() != 21) { radBeforeCol = (event[rad].col() > 0) ? event[rad].col() : event[emt].col(); // Quark emissions in ISR } else if (type == -1 && event[emt].id() != 21) { radBeforeCol = (event[rad].col() > 0) ? event[rad].col() : event[emt].acol(); //Gluon emissions in FSR } else if (type == 1 && event[emt].id() == 21) { // If emitted is a gluon, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].col() == event[emt].acol()) ? event[rad].acol() : event[rad].col(); radBeforeCol = (event[rad].col() == colRemove) ? event[emt].col() : event[rad].col(); //Gluon emissions in ISR } else if (type == -1 && event[emt].id() == 21) { // If emitted is a gluon, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].col() == event[emt].col()) ? event[rad].col() : event[rad].acol(); radBeforeCol = (event[rad].col() == colRemove) ? event[emt].acol() : event[rad].col(); } // Get reconstructed quark colours } else if ( radBeforeFlav != 21 && radBeforeFlav > 0) { // Quark emission in FSR if (type == 1 && event[emt].id() != 21) { // If radiating is a quark, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].col() == event[emt].acol()) ? event[rad].acol() : 0; radBeforeCol = (event[rad].col() == colRemove) ? event[emt].col() : event[rad].col(); //Gluon emissions in FSR } else if (type == 1 && event[emt].id() == 21) { // If emitted is a gluon, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].col() == event[emt].acol()) ? event[rad].col() : 0; radBeforeCol = (event[rad].col() == colRemove) ? event[emt].col() : event[rad].col(); //Quark emissions in ISR } else if (type == -1 && event[emt].id() != 21) { // If emitted is a quark, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].col() == event[emt].col()) ? event[rad].col() : 0; radBeforeCol = (event[rad].col() == colRemove) ? event[emt].acol() : event[rad].col(); //Gluon emissions in ISR } else if (type == -1 && event[emt].id() == 21) { // If emitted is a gluon, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].col() == event[emt].col()) ? event[rad].col() : 0; radBeforeCol = (event[rad].col() == colRemove) ? event[emt].acol() : event[rad].col(); } // Other particles are assumed uncoloured } else { radBeforeCol = 0; } return radBeforeCol; } //-------------------------------------------------------------------------- // Function to get the anticolour of the radiator before the splitting // for clustering // IN int : Position of the radiator after the splitting, in the event // int : Position of the emitted after the splitting, in the event // Event : Reference event // OUT int : Anticolour of the radiator before the splitting int History::getRadBeforeAcol(const int rad, const int emt, const Event& event) { // Save type of splitting int type = (event[rad].isFinal()) ? 1 :-1; // Get flavour of radiator after potential clustering int radBeforeFlav = getRadBeforeFlav(rad,emt,event); // Get colours of the radiator before the potential clustering int radBeforeAcl = -1; // Get reconstructed gluon colours if (radBeforeFlav == 21) { // Start with quark emissions in FSR if (type == 1 && event[emt].id() != 21) { radBeforeAcl = (event[rad].acol() > 0) ? event[rad].acol() : event[emt].acol(); // Quark emissions in ISR } else if (type == -1 && event[emt].id() != 21) { radBeforeAcl = (event[rad].acol() > 0) ? event[rad].acol() : event[emt].col(); //Gluon emissions in FSR } else if (type == 1 && event[emt].id() == 21) { // If emitted is a gluon, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].col() == event[emt].acol()) ? event[rad].acol() : event[rad].col(); radBeforeAcl = (event[rad].acol() == colRemove) ? event[emt].acol() : event[rad].acol(); //Gluon emissions in ISR } else if (type == -1 && event[emt].id() == 21) { // If emitted is a gluon, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].col() == event[emt].col()) ? event[rad].col() : event[rad].acol(); radBeforeAcl = (event[rad].acol() == colRemove) ? event[emt].col() : event[rad].acol(); } // Get reconstructed anti-quark colours } else if ( radBeforeFlav != 21 && radBeforeFlav < 0) { // Antiquark emission in FSR if (type == 1 && event[emt].id() != 21) { // If radiating is a antiquark, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].col() == event[emt].acol()) ? event[rad].acol() : 0; radBeforeAcl = (event[rad].acol() == colRemove) ? event[emt].acol() : event[rad].acol(); //Gluon emissions in FSR } else if (type == 1 && event[emt].id() == 21) { // If emitted is a gluon, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].acol() == event[emt].col()) ? event[rad].acol() : 0; radBeforeAcl = (event[rad].acol() == colRemove) ? event[emt].acol() : event[rad].acol(); //Antiquark emissions in ISR } else if (type == -1 && event[emt].id() != 21) { // If emitted is an antiquark, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].acol() == event[emt].acol()) ? event[rad].acol() : 0; radBeforeAcl = (event[rad].acol() == colRemove) ? event[emt].col() : event[rad].acol(); //Gluon emissions in ISR } else if (type == -1 && event[emt].id() == 21) { // If emitted is a gluon, remove the repeated index, and take // the remaining indices as colour and anticolour int colRemove = (event[rad].acol() == event[emt].acol()) ? event[rad].acol() : 0; radBeforeAcl = (event[rad].acol() == colRemove) ? event[emt].col() : event[rad].acol(); } // Other particles are considered uncoloured } else { radBeforeAcl = 0; } return radBeforeAcl; } //-------------------------------------------------------------------------- // Function to get the parton connected to in by a colour line // IN int : Position of parton for which partner should be found // Event : Reference event // OUT int : If a colour line connects the "in" parton with another // parton, return the Position of the partner, else return 0 int History::getColPartner(const int in, const Event& event) { if (event[in].col() == 0) return 0; int partner = 0; // Try to find anticolour index first partner = FindCol(event[in].col(),in,0,event,1,true); // If no anticolour index has been found, try colour if (partner == 0) partner = FindCol(event[in].col(),in,0,event,2,true); return partner; } //-------------------------------------------------------------------------- // Function to get the parton connected to in by an anticolour line // IN int : Position of parton for which partner should be found // Event : Reference event // OUT int : If an anticolour line connects the "in" parton with another // parton, return the Position of the partner, else return 0 int History::getAcolPartner(const int in, const Event& event) { if (event[in].acol() == 0) return 0; int partner = 0; // Try to find colour index first partner = FindCol(event[in].acol(),in,0,event,2,true); // If no colour index has been found, try anticolour if (partner == 0) partner = FindCol(event[in].acol(),in,0,event,1,true); return partner; } //-------------------------------------------------------------------------- // Function to get the list of partons connected to the particle // formed by reclusterinf emt and rad by colour and anticolour lines // IN int : Position of radiator in the clustering // IN int : Position of emitted in the clustering // Event : Reference event // OUT vector : List of positions of all partons that are connected // to the parton that will be formed // by clustering emt and rad. vector History::getReclusteredPartners(const int rad, const int emt, const Event& event) { // Save type int type = event[rad].isFinal() ? 1 : -1; // Get reclustered colours int radBeforeCol = getRadBeforeCol(rad, emt, event); int radBeforeAcl = getRadBeforeAcol(rad, emt, event); // Declare output vector partners; // Start with FSR clusterings if (type == 1) { for(int i=0; i < int(event.size()); ++i) { // Check all initial state partons if ( i != emt && i != rad && event[i].status() == -21 && event[i].col() > 0 && event[i].col() == radBeforeCol) partners.push_back(i); // Check all final state partons if ( i != emt && i != rad && event[i].isFinal() && event[i].acol() > 0 && event[i].acol() == radBeforeCol) partners.push_back(i); // Check all initial state partons if ( i != emt && i != rad && event[i].status() == -21 && event[i].acol() > 0 && event[i].acol() == radBeforeAcl) partners.push_back(i); // Check all final state partons if ( i != emt && i != rad && event[i].isFinal() && event[i].col() > 0 && event[i].col() == radBeforeAcl) partners.push_back(i); } // Start with ISR clusterings } else { for(int i=0; i < int(event.size()); ++i) { // Check all initial state partons if ( i != emt && i != rad && event[i].status() == -21 && event[i].acol() > 0 && event[i].acol() == radBeforeCol) partners.push_back(i); // Check all final state partons if ( i != emt && i != rad && event[i].isFinal() && event[i].col() > 0 && event[i].col() == radBeforeCol) partners.push_back(i); // Check all initial state partons if ( i != emt && i != rad && event[i].status() == -21 && event[i].col() > 0 && event[i].col() == radBeforeAcl) partners.push_back(i); // Check all final state partons if ( i != emt && i != rad && event[i].isFinal() && event[i].acol() > 0 && event[i].acol() == radBeforeAcl) partners.push_back(i); } } // Done return partners; } //-------------------------------------------------------------------------- // Function to extract a chain of colour-connected partons in // the event // IN int : Type of parton from which to start extracting a // parton chain. If the starting point is a quark // i.e. flavType = 1, a chain of partons that are // consecutively connected by colour-lines will be // extracted. If the starting point is an antiquark // i.e. flavType =-1, a chain of partons that are // consecutively connected by anticolour-lines // will be extracted. // IN int : Position of the parton from which a // colour-connected chain should be derived // IN Event : Refernence event // IN/OUT vector : Partons that should be excluded from the search. // OUT vector : Positions of partons along the chain // OUT bool : Found singlet / did not find singlet bool History::getColSinglet( const int flavType, const int iParton, const Event& event, vector& exclude, vector& colSinglet) { // If no possible flavour to start from has been found if (iParton < 0) return false; // If no further partner has been found in a previous iteration, // and the whole final state has been excluded, we're done if (iParton == 0) { // Count number of final state partons int nFinal = 0; for(int i=0; i < int(event.size()); ++i) if ( event[i].isFinal() && event[i].colType() != 0) nFinal++; // Get number of initial state partons in the list of // excluded partons int nExclude = int(exclude.size()); int nInitExclude = 0; if (!event[exclude[2]].isFinal()) nInitExclude++; if (!event[exclude[3]].isFinal()) nInitExclude++; // If the whole final state has been considered, return if (nFinal == nExclude - nInitExclude) return true; else return false; } // Declare colour partner int colP = 0; // Save the colour partner colSinglet.push_back(iParton); // Remove the partner from the list exclude.push_back(iParton); // When starting out from a quark line, follow the colour lines if (flavType == 1) colP = getColPartner(iParton,event); // When starting out from an antiquark line, follow the anticolour lines else colP = getAcolPartner(iParton,event); // Do not count excluded partons twice for(int i = 0; i < int(exclude.size()); ++i) if (colP == exclude[i]) return true; // Recurse return getColSinglet(flavType,colP,event,exclude,colSinglet); } //-------------------------------------------------------------------------- // Function to check that a set of partons forms a colour singlet // IN Event : Reference event // IN vector : Positions of the partons in the set // OUT bool : Is a colour singlet / is not bool History::isColSinglet( const Event& event, vector system ) { // Check if system forms a colour singlet for(int i=0; i < int(system.size()); ++i ) { // Match quark and gluon colours if ( system[i] > 0 && (event[system[i]].colType() == 1 || event[system[i]].colType() == 2) ) { for(int j=0; j < int(system.size()); ++j) // If flavour matches, remove both partons and continue if ( system[i] > 0 && system[j] > 0 && event[system[i]].col() == event[system[j]].acol()) { // Remove index and break system[i] = 0; system[j] = 0; break; } } // Match antiquark and gluon anticolours if ( system[i] > 0 && (event[system[i]].colType() == -1 || event[system[i]].colType() == 2) ) { for(int j=0; j < int(system.size()); ++j) // If flavour matches, remove both partons and continue if ( system[i] > 0 && system[j] > 0 && event[system[i]].acol() == event[system[j]].col()) { // Remove index and break system[i] = 0; system[j] = 0; break; } } } // The system is a colour singlet if for all colours, // an anticolour was found bool isColSing = true; for(int i=0; i < int(system.size()); ++i) if ( system[i] != 0 ) isColSing = false; // Return return isColSing; } //-------------------------------------------------------------------------- // Function to check that a set of partons forms a flavour singlet // IN Event : Reference event // IN vector : Positions of the partons in the set // IN int : Flavour of all the quarks in the set, if // all quarks in a set should have a fixed flavour // OUT bool : Is a flavour singlet / is not bool History::isFlavSinglet( const Event& event, vector system, int flav) { // If a decoupled colour singlet has been found, check if this is also // a flavour singlet // Check that each quark matches an antiquark for(int i=0; i < int(system.size()); ++i) if ( system[i] > 0 ) { for(int j=0; j < int(system.size()); ++j) { // If flavour of outgoing partons matches, // remove both partons and continue. // Skip all bosons if ( event[i].idAbs() != 21 && event[i].idAbs() != 22 && event[i].idAbs() != 23 && event[i].idAbs() != 24 && system[i] > 0 && system[j] > 0 && event[system[i]].isFinal() && event[system[j]].isFinal() && event[system[i]].id() == -1*event[system[j]].id()) { // If we want to check if only one flavour of quarks // exists if (abs(flav) > 0 && event[system[i]].idAbs() != flav) return false; // Remove index and break system[i] = 0; system[j] = 0; break; } // If flavour of outgoing and incoming partons match, // remove both partons and continue. // Skip all bosons if ( event[i].idAbs() != 21 && event[i].idAbs() != 22 && event[i].idAbs() != 23 && event[i].idAbs() != 24 && system[i] > 0 && system[j] > 0 && ( ( !event[system[i]].isFinal() && event[system[j]].isFinal()) ||( !event[system[j]].isFinal() && event[system[i]].isFinal()) ) && event[system[i]].id() == event[system[j]].id()) { // If we want to check if only one flavour of quarks // exists if (abs(flav) > 0 && event[system[i]].idAbs() != flav) return false; // Remove index and break system[i] = 0; system[j] = 0; break; } } } // The colour singlet is a flavour singlet if for all quarks, // an antiquark was found bool isFlavSing = true; for(int i=0; i < int(system.size()); ++i) if ( system[i] != 0 ) isFlavSing = false; // Return return isFlavSing; } //-------------------------------------------------------------------------- // Function to check if rad,emt,rec triple is allowed for clustering // IN int rad,emt,rec : Positions (in event record) of the three // particles considered for clustering // Event event : Reference event bool History::allowedClustering( int rad, int emt, int rec, int partner, const Event& event ) { // Declare output bool allowed = true; // CONSTRUCT SOME PROPERTIES FOR LATER INVESTIGATION // Check if the triple forms a colour singlett bool isSing = isSinglett(rad,emt,partner,event); int type = (event[rad].isFinal()) ? 1 :-1; // Get flavour of radiator after potential clustering int radBeforeFlav = getRadBeforeFlav(rad,emt,event); // Get colours of the radiator before the potential clustering int radBeforeCol = getRadBeforeCol(rad,emt,event); int radBeforeAcl = getRadBeforeAcol(rad,emt,event); // Get colour partner of reclustered parton vector radBeforeColP = getReclusteredPartners(rad, emt, event); // Count coloured partons in hard process int nPartonInHard = 0; for(int i=0; i < int(event.size()); ++i) // Check all final state partons if ( event[i].isFinal() && event[i].colType() != 0 && mergingHooksPtr->hardProcess.matchesAnyOutgoing(i, event) ) nPartonInHard++; // Count coloured final state partons in event, excluding // rad, rec, emt and hard process int nPartons = 0; for(int i=0; i < int(event.size()); ++i) // Check all final state partons if ( i!=emt && i!=rad && i!=rec && event[i].isFinal() && event[i].colType() != 0 && !mergingHooksPtr->hardProcess.matchesAnyOutgoing(i, event) ) nPartons++; // Count number of initial state partons int nInitialPartons = 0; for(int i=0; i < int(event.size()); ++i) if ( event[i].status() == -21 && event[i].colType() != 0 ) nInitialPartons++; // Get number of non-charged final state particles int nFinalEW = 0; for(int i=0; i < int(event.size()); ++i) if ( event[i].isFinal() &&( event[i].id() == 22 || event[i].id() == 23 || event[i].id() == 24 ||(event[i].idAbs() > 10 && event[i].idAbs() < 20) ||(event[i].idAbs() > 10 && event[i].idAbs() < 20) ||(event[i].idAbs() > 1000010 && event[i].idAbs() < 1000020) ||(event[i].idAbs() > 2000010 && event[i].idAbs() < 2000020) )) nFinalEW++; // Check if event after potential clustering contains an even // number of quarks and/or antiquarks // (otherwise no electroweak vertex could be formed!) // Get number of final quarks int nFinalQuark = 0; // Get number of excluded final state quarks as well int nFinalQuarkExc = 0; for(int i=0; i < int(event.size()); ++i) { if (i !=rad && i != emt && i != rec) { if (event[i].isFinal() && event[i].isQuark() ) { if ( !mergingHooksPtr->hardProcess.matchesAnyOutgoing(i,event) ) nFinalQuark++; else nFinalQuarkExc++; } } } // Add recoiler to number of final quarks if (event[rec].isFinal() && event[rec].isQuark()) nFinalQuark++; // Add radiator after clustering to number of final quarks if (event[rad].isFinal() && abs(radBeforeFlav) < 10) nFinalQuark++; // Get number of initial quarks int nInitialQuark = 0; if (type == 1) { if (event[rec].isFinal()) { if (event[3].isQuark()) nInitialQuark++; if (event[4].isQuark()) nInitialQuark++; } else { int iOtherIn = (rec == 3) ? 4 : 3; if (event[rec].isQuark()) nInitialQuark++; if (event[iOtherIn].isQuark()) nInitialQuark++; } } else { // Add recoiler to number of initial quarks if (event[rec].isQuark()) nInitialQuark++; // Add radiator after clustering to number of initial quarks if (abs(radBeforeFlav) < 10) nInitialQuark++; } // BEGIN CHECKING THE CLUSTERING // Check if colour is conserved vector unmatchedCol; vector unmatchedAcl; // Check all unmatched colours for ( int i = 0; i < event.size(); ++i) if ( i != emt && i != rad && (event[i].isFinal() || event[i].status() == -21) && event[i].colType() != 0 ) { int colP = getColPartner(i,event); int aclP = getAcolPartner(i,event); if (event[i].col() > 0 && (colP == emt || colP == rad || colP == 0) ) unmatchedCol.push_back(i); if (event[i].acol() > 0 && (aclP == emt || aclP == rad || aclP == 0) ) unmatchedAcl.push_back(i); } // If more than one colour or more than one anticolour are unmatched, // there is no way to make this clustering work if (int(unmatchedCol.size()) + int(unmatchedAcl.size()) > 2) return false; // If triple forms colour singlett, check that resulting state // matches hard core process if (isSing) allowed = false; if (isSing && (abs(radBeforeFlav)<10 && event[rec].isQuark()) ) allowed = true; // Never recluster any outgoing partons of the core V -> qqbar' splitting! if ( mergingHooksPtr->hardProcess.matchesAnyOutgoing(emt,event) ) { // Check if any other particle could replace "emt" as part of the candidate // core process. If so, replace emt with the new candidate and allow the // clustering. bool canReplace = mergingHooksPtr->hardProcess.findOtherCandidates(emt, event, true); if (canReplace) allowed = true; else allowed = false; } // Never allow clustering of any outgoing partons of the hard process // which would change the flavour of one of the hard process partons! if ( mergingHooksPtr->hardProcess.matchesAnyOutgoing(rad,event) && event[rad].id() != radBeforeFlav ) allowed = false; // If only gluons in initial state and no quarks in final state, // reject (no electroweak vertex can be formed) if (nFinalEW != 0 && nInitialQuark == 0 && nFinalQuark == 0 && nFinalQuarkExc == 0) allowed = false; if ( (nInitialQuark + nFinalQuark + nFinalQuarkExc)%2 != 0 ) allowed = false; // Do not allow final state splitting that produces only // allowed final state gluons, and has a colour-connected initial state // This means forbidding clusterings that do not allow for a // t-channel gluon, which is needed to have a quark-antiquark initial state. // Here, partons excluded from clustering are not counted as possible // partners to form a t-channel gluon if (event[3].col() == event[4].acol() && event[3].acol() == event[4].col() && nFinalQuark == 0) allowed = false; // No problems with gluon radiation if (event[emt].id() == 21) return allowed; // No problems with gluino radiation if (event[emt].id() == 1000021) return allowed; // Save all hard process candidates vector outgoingParticles; int nOut1 = int(mergingHooksPtr->hardProcess.PosOutgoing1.size()); for ( int i=0; i < nOut1; ++i ) { int iPos = mergingHooksPtr->hardProcess.PosOutgoing1[i]; outgoingParticles.push_back( mergingHooksPtr->hardProcess.state[iPos].id() ); } int nOut2 = int(mergingHooksPtr->hardProcess.PosOutgoing2.size()); for ( int i=0; i < nOut2; ++i ) { int iPos = mergingHooksPtr->hardProcess.PosOutgoing2[i]; outgoingParticles.push_back( mergingHooksPtr->hardProcess.state[iPos].id() ); } // Start more involved checks. g -> q_1 qbar_1 splittings are // particularly problematic if more than one quark of the emitted // flavour is present. // Count number of initial quarks of radiator or emitted flavour vector iInQuarkFlav; for(int i=0; i < int(event.size()); ++i) // Check all initial state partons if ( i != emt && i != rad && event[i].status() == -21 && event[i].idAbs() == event[emt].idAbs() ) iInQuarkFlav.push_back(i); // Count number of final quarks of radiator or emitted flavour vector iOutQuarkFlav; for(int i=0; i < int(event.size()); ++i) // Check all final state partons if ( i != emt && i != rad && event[i].isFinal() && event[i].idAbs() == event[emt].idAbs() ) { // Loop through final state hard particles. If one matches, remove the // matching one, and do not count. bool matchOut = false; for (int j = 0; j < int(outgoingParticles.size()); ++j) if ( event[i].idAbs() == abs(outgoingParticles[j])) { matchOut = true; outgoingParticles[j] = 99; } if (!matchOut) iOutQuarkFlav.push_back(i); } // Save number of potentially dangerous quarks int nInQuarkFlav = int(iInQuarkFlav.size()); int nOutQuarkFlav = int(iOutQuarkFlav.size()); // Easiest problem 0: // Radiator before splitting exactly matches the partner // after the splitting if ( event[partner].isFinal() && event[partner].id() == 21 && radBeforeFlav == 21 && event[partner].col() == radBeforeCol && event[partner].acol() == radBeforeAcl) return false; // If there are no ambiguities in qqbar pairs, return if (nInQuarkFlav + nOutQuarkFlav == 0) return allowed; // Save all quarks and gluons that will not change colour vector gluon; vector quark; vector antiq; vector partons; for(int i=0; i < int(event.size()); ++i) // Check initial and final state partons if ( i!=emt && i!=rad && event[i].colType() != 0 && (event[i].isFinal() || event[i].status() == -21) ) { // Save index partons.push_back(i); // Split into components if (event[i].colType() == 2) gluon.push_back(i); else if (event[i].colType() == 1) quark.push_back(i); else if (event[i].colType() == -1) antiq.push_back(i); } // We split up the test of the g->qq splitting into final state // and initial state problems bool isFSRg2qq = ((type == 1) && (event[rad].id() == -1*event[emt].id()) ); bool isISRg2qq = ((type ==-1) && (event[rad].id() == event[emt].id()) ); // First check general things about colour connections // Check that clustering does not produce a gluon that is exactly // matched in the final state, or does not have any colour connections if ( (isFSRg2qq || isISRg2qq) && int(quark.size()) + int(antiq.size()) + int(gluon.size()) > nPartonInHard ) { vector colours; vector anticolours; // Add the colour and anticolour of the gluon before the emission // to the list, bookkeep initial colour as final anticolour, and // initial anticolour as final colour if (type == 1) { colours.push_back(radBeforeCol); anticolours.push_back(radBeforeAcl); } else { colours.push_back(radBeforeAcl); anticolours.push_back(radBeforeCol); } // Now store gluon colours and anticolours. for(int i=0; i < int(gluon.size()); ++i) if (event[gluon[i]].isFinal()) { colours.push_back(event[gluon[i]].col()); anticolours.push_back(event[gluon[i]].acol()); } else { colours.push_back(event[gluon[i]].acol()); anticolours.push_back(event[gluon[i]].col()); } // Loop through colours and check if any match with // anticolours. If colour matches, remove from list for(int i=0; i < int(colours.size()); ++i) for(int j=0; j < int(anticolours.size()); ++j) if (colours[i] > 0 && anticolours[j] > 0 && colours[i] == anticolours[j]) { colours[i] = 0; anticolours[j] = 0; } // If all gluon anticolours and all colours matched, disallow // the clustering bool allMatched = true; for(int i=0; i < int(colours.size()); ++i) if (colours[i] != 0) allMatched = false; for(int i=0; i < int(anticolours.size()); ++i) if (anticolours[i] != 0) allMatched = false; if (allMatched) return false; // Now add the colours of the hard process, and check if all // colours match. for(int i=0; i < int(quark.size()); ++i) if ( event[quark[i]].isFinal() && mergingHooksPtr->hardProcess.matchesAnyOutgoing(quark[i], event) ) colours.push_back(event[quark[i]].col()); for(int i=0; i < int(antiq.size()); ++i) if ( event[antiq[i]].isFinal() && mergingHooksPtr->hardProcess.matchesAnyOutgoing(antiq[i], event) ) anticolours.push_back(event[antiq[i]].acol()); // Loop through colours again and check if any match with // anticolours. If colour matches, remove from list for(int i=0; i < int(colours.size()); ++i) for(int j=0; j < int(anticolours.size()); ++j) if (colours[i] > 0 && anticolours[j] > 0 && colours[i] == anticolours[j]) { colours[i] = 0; anticolours[j] = 0; } // Check if clustering would produce the hard process int nNotInHard = 0; for ( int i=0; i < int(quark.size()); ++i ) if ( !mergingHooksPtr->hardProcess.matchesAnyOutgoing( quark[i], event) ) nNotInHard++; for ( int i=0; i < int(antiq.size()); ++i ) if ( !mergingHooksPtr->hardProcess.matchesAnyOutgoing( antiq[i], event) ) nNotInHard++; for(int i=0; i < int(gluon.size()); ++i) if ( event[gluon[i]].isFinal() ) nNotInHard++; if ( type == 1 ) nNotInHard++; // If all colours are matched now, and since we have more quarks than // present in the hard process, disallow the clustering allMatched = true; for(int i=0; i < int(colours.size()); ++i) if (colours[i] != 0) allMatched = false; for(int i=0; i < int(anticolours.size()); ++i) if (anticolours[i] != 0) allMatched = false; if (allMatched && nNotInHard > 0) return false; } // FSR PROBLEMS if (isFSRg2qq && nInQuarkFlav + nOutQuarkFlav > 0) { // Easiest problem 1: // RECLUSTERED FINAL STATE GLUON MATCHES INITIAL STATE GLUON for(int i=0; i < int(gluon.size()); ++i) { if (!event[gluon[i]].isFinal() && event[gluon[i]].col() == radBeforeCol && event[gluon[i]].acol() == radBeforeAcl) return false; } // Easiest problem 2: // RECLUSTERED FINAL STATE GLUON MATCHES FINAL STATE GLUON for(int i=0; i < int(gluon.size()); ++i) { if (event[gluon[i]].isFinal() && event[gluon[i]].col() == radBeforeAcl && event[gluon[i]].acol() == radBeforeCol) return false; } // Easiest problem 3: // RECLUSTERED FINAL STATE GLUON MATCHES FINAL STATE Q-QBAR PAIR if ( int(radBeforeColP.size()) == 2 && event[radBeforeColP[0]].isFinal() && event[radBeforeColP[1]].isFinal() && event[radBeforeColP[0]].id() == -1*event[radBeforeColP[1]].id() ) { // This clustering is allowed if there is no colour in the // initial state if (nInitialPartons > 0) return false; } // Next-to-easiest problem 1: // RECLUSTERED FINAL STATE GLUON MATCHES ONE FINAL STARE Q_1 // AND ONE INITIAL STATE Q_1 if ( int(radBeforeColP.size()) == 2 && (( event[radBeforeColP[0]].status() == -21 && event[radBeforeColP[1]].isFinal()) ||( event[radBeforeColP[0]].isFinal() && event[radBeforeColP[1]].status() == -21)) && event[radBeforeColP[0]].id() == event[radBeforeColP[1]].id() ) { // In principle, clustering this splitting can disconnect // the colour lines of a graph. However, the colours can be connected // again if a final or initial partons of the correct flavour exists. // Check which of the partners are final / initial int incoming = (event[radBeforeColP[0]].isFinal()) ? radBeforeColP[1] : radBeforeColP[0]; int outgoing = (event[radBeforeColP[0]].isFinal()) ? radBeforeColP[0] : radBeforeColP[1]; // Loop through event to find "recovery partons" bool clusPossible = false; for(int i=0; i < int(event.size()); ++i) if ( i != emt && i != rad && i != incoming && i != outgoing && !mergingHooksPtr->hardProcess.matchesAnyOutgoing(i,event) ) { // Check if an incoming parton matches if ( event[i].status() == -21 && (event[i].id() == event[outgoing].id() ||event[i].id() == -1*event[incoming].id()) ) clusPossible = true; // Check if a final parton matches if ( event[i].isFinal() && (event[i].id() == -1*event[outgoing].id() ||event[i].id() == event[incoming].id()) ) clusPossible = true; } // There can be a further complication: If e.g. in // t-channel photon exchange topologies, both incoming // partons are quarks, and form colour singlets with any // number of final state partons, at least try to // recluster as much as possible. // For this, check if the incoming parton // connected to the radiator is connected to a // colour and flavour singlet vector excludeIn1; for(int i=0; i < 4; ++i) excludeIn1.push_back(0); vector colSingletIn1; int flavIn1Type = (event[incoming].id() > 0) ? 1 : -1; // Try finding colour singlets bool isColSingIn1 = getColSinglet(flavIn1Type,incoming,event, excludeIn1,colSingletIn1); // Check if colour singlet also is a flavour singlet bool isFlavSingIn1 = isFlavSinglet(event,colSingletIn1); // Check if the incoming parton not // connected to the radiator is connected to a // colour and flavour singlet int incoming2 = (incoming == 3) ? 4 : 3; vector excludeIn2; for(int i=0; i < 4; ++i) excludeIn2.push_back(0); vector colSingletIn2; int flavIn2Type = (event[incoming2].id() > 0) ? 1 : -1; // Try finding colour singlets bool isColSingIn2 = getColSinglet(flavIn2Type,incoming2,event, excludeIn2,colSingletIn2); // Check if colour singlet also is a flavour singlet bool isFlavSingIn2 = isFlavSinglet(event,colSingletIn2); // If no "recovery clustering" is possible, reject clustering if (!clusPossible && (!isColSingIn1 || !isFlavSingIn1 || !isColSingIn2 || !isFlavSingIn2)) return false; } // Next-to-easiest problem 2: // FINAL STATE Q-QBAR CLUSTERING DISCONNECTS SINGLETT SUBSYSTEM WITH // FINAL STATE Q-QBAR PAIR FROM GRAPH // Prepare to check for colour singlet combinations of final state quarks // Start by building a list of partons to exclude when checking for // colour singlet combinations int flav = event[emt].id(); vector exclude; exclude.push_back(emt); exclude.push_back(rad); exclude.push_back(radBeforeColP[0]); exclude.push_back(radBeforeColP[1]); vector colSinglet; // Now find parton from which to start checking colour singlets int iOther = -1; // Loop through event to find a parton of correct flavour for(int i=0; i < int(event.size()); ++i) // Check final state for parton equalling emitted flavour. // Exclude the colour system coupled to the clustering if ( i != emt && i != rad && i != radBeforeColP[0] && i != radBeforeColP[1] && event[i].isFinal() ) { // Stop if one parton of the correct flavour is found if (event[i].id() == flav) { iOther = i; break; } } // Save the type of flavour int flavType = (event[iOther].id() > 0) ? 1 : -1; // Try finding colour singlets bool isColSing = getColSinglet(flavType,iOther,event,exclude,colSinglet); // Check if colour singlet also is a flavour singlet bool isFlavSing = isFlavSinglet(event,colSinglet); // Nearly there... if (isColSing && isFlavSing) { // In a final check, ensure that the final state does not only // consist of colour singlets that are also flavour singlets // of the identical (!) flavours // Loop through event and save all final state partons vector allFinal; for(int i=0; i < int(event.size()); ++i) if ( event[i].isFinal() ) allFinal.push_back(i); // Check if all final partons form a colour singlet bool isFullColSing = isColSinglet(event,allFinal); // Check if all final partons form a flavour singlet bool isFullFlavSing = isFlavSinglet(event,allFinal,flav); // If all final quarks are of identical flavour, // no possible clustering should be discriminated. // Otherwise, disallow if (!isFullColSing || !isFullFlavSing) return false; } } // ISR PROBLEMS if (isISRg2qq && nInQuarkFlav + nOutQuarkFlav > 0) { // Easiest problem 1: // RECLUSTERED INITIAL STATE GLUON MATCHES FINAL STATE GLUON for(int i=0; i < int(gluon.size()); ++i) { if (event[gluon[i]].isFinal() && event[gluon[i]].col() == radBeforeCol && event[gluon[i]].acol() == radBeforeAcl) return false; } // Easiest problem 2: // RECLUSTERED INITIAL STATE GLUON MATCHES INITIAL STATE GLUON for(int i=0; i < int(gluon.size()); ++i) { if (event[gluon[i]].status() == -21 && event[gluon[i]].acol() == radBeforeCol && event[gluon[i]].col() == radBeforeAcl) return false; } // Next-to-easiest problem 1: // RECLUSTERED INITIAL STATE GLUON MATCHES FINAL STATE Q-QBAR PAIR if ( int(radBeforeColP.size()) == 2 && event[radBeforeColP[0]].isFinal() && event[radBeforeColP[1]].isFinal() && event[radBeforeColP[0]].id() == -1*event[radBeforeColP[1]].id() ) { // In principle, clustering this splitting can disconnect // the colour lines of a graph. However, the colours can be connected // again if final state partons of the correct (anti)flavour, or // initial state partons of the correct flavour exist // Loop through event to check bool clusPossible = false; for(int i=0; i < int(event.size()); ++i) if ( i != emt && i != rad && i != radBeforeColP[0] && i != radBeforeColP[1] && !mergingHooksPtr->hardProcess.matchesAnyOutgoing(i,event) ) { if (event[i].status() == -21 && ( event[radBeforeColP[0]].id() == event[i].id() || event[radBeforeColP[1]].id() == event[i].id() )) clusPossible = true; if (event[i].isFinal() && ( event[radBeforeColP[0]].id() == -1*event[i].id() || event[radBeforeColP[1]].id() == -1*event[i].id() )) clusPossible = true; } // There can be a further complication: If e.g. in // t-channel photon exchange topologies, both incoming // partons are quarks, and form colour singlets with any // number of final state partons, at least try to // recluster as much as possible. // For this, check if the incoming parton // connected to the radiator is connected to a // colour and flavour singlet int incoming1 = 3; vector excludeIn1; for(int i=0; i < 4; ++i) excludeIn1.push_back(0); vector colSingletIn1; int flavIn1Type = (event[incoming1].id() > 0) ? 1 : -1; // Try finding colour singlets bool isColSingIn1 = getColSinglet(flavIn1Type,incoming1,event, excludeIn1,colSingletIn1); // Check if colour singlet also is a flavour singlet bool isFlavSingIn1 = isFlavSinglet(event,colSingletIn1); // Check if the incoming parton not // connected to the radiator is connected to a // colour and flavour singlet int incoming2 = 4; vector excludeIn2; for(int i=0; i < 4; ++i) excludeIn2.push_back(0); vector colSingletIn2; int flavIn2Type = (event[incoming2].id() > 0) ? 1 : -1; // Try finding colour singlets bool isColSingIn2 = getColSinglet(flavIn2Type,incoming2,event, excludeIn2,colSingletIn2); // Check if colour singlet also is a flavour singlet bool isFlavSingIn2 = isFlavSinglet(event,colSingletIn2); // If no "recovery clustering" is possible, reject clustering if (!clusPossible && (!isColSingIn1 || !isFlavSingIn1 || !isColSingIn2 || !isFlavSingIn2)) return false; } } // Done return allowed; } //-------------------------------------------------------------------------- // Function to check if rad,emt,rec triple is results in // colour singlet radBefore+recBefore // IN int rad,emt,rec : Positions (in event record) of the three // particles considered for clustering // Event event : Reference event bool History::isSinglett( int rad, int emt, int rec, const Event& event ) { int radCol = event[rad].col(); int emtCol = event[emt].col(); int recCol = event[rec].col(); int radAcl = event[rad].acol(); int emtAcl = event[emt].acol(); int recAcl = event[rec].acol(); int recType = event[rec].isFinal() ? 1 : -1; bool isSing = false; if ( ( recType == -1 && radCol + emtCol == recCol && radAcl + emtAcl == recAcl) ||( recType == 1 && radCol + emtCol == recAcl && radAcl + emtAcl == recCol) ) isSing = true; return isSing; } //-------------------------------------------------------------------------- // Function to check if event is sensibly constructed: Meaning // that all colour indices are contracted and that the charge in // initial and final states matches // IN event : event to be checked // OUT TRUE : event is properly construced // FALSE : event not valid bool History::validEvent( const Event& event ) { // Check if event is coloured bool validColour = true; for ( int i = 0; i < event.size(); ++i) // Check colour of quarks if ( event[i].isFinal() && event[i].colType() == 1 // No corresponding anticolour in final state && ( FindCol(event[i].col(),i,0,event,1,true) == 0 // No corresponding colour in initial state && FindCol(event[i].col(),i,0,event,2,true) == 0 )) { validColour = false; break; // Check anticolour of antiquarks } else if ( event[i].isFinal() && event[i].colType() == -1 // No corresponding colour in final state && ( FindCol(event[i].acol(),i,0,event,2,true) == 0 // No corresponding anticolour in initial state && FindCol(event[i].acol(),i,0,event,1,true) == 0 )) { validColour = false; break; // No uncontracted colour (anticolour) charge of gluons } else if ( event[i].isFinal() && event[i].colType() == 2 // No corresponding anticolour in final state && ( FindCol(event[i].col(),i,0,event,1,true) == 0 // No corresponding colour in initial state && FindCol(event[i].col(),i,0,event,2,true) == 0 ) // No corresponding colour in final state && ( FindCol(event[i].acol(),i,0,event,2,true) == 0 // No corresponding anticolour in initial state && FindCol(event[i].acol(),i,0,event,1,true) == 0 )) { validColour = false; break; } // Check charge sum in initial and final state bool validCharge = true; double initCharge = event[3].charge() + event[4].charge(); double finalCharge = 0.0; for(int i = 0; i < event.size(); ++i) if (event[i].isFinal()) finalCharge += event[i].charge(); if (abs(initCharge-finalCharge) > 1e-12) validCharge = false; return (validColour && validCharge); } //-------------------------------------------------------------------------- // Function to check whether two clusterings are identical, used // for finding the history path in the mother -> children direction bool History::equalClustering( Clustering clus1 , Clustering clus2 ) { return ( (clus1.emittor == clus2.emittor) && (clus1.emitted == clus2.emitted) && (clus1.recoiler == clus2.recoiler) && (clus1.partner == clus2.partner) && (clus1.pT() == clus2.pT()) ); } //-------------------------------------------------------------------------- // Chose dummy scale for event construction. By default, choose // sHat for 2->Boson(->2)+ n partons processes and // M_Boson for 2->Boson(->) processes double History::choseHardScale( const Event& event ) const { // Get sHat double mHat = (event[3].p() + event[4].p()).mCalc(); // Find number of final state particles and bosons int nFinal = 0; int nFinBos= 0; int nBosons= 0; double mBos = 0.0; for(int i = 0; i < event.size(); ++i) if ( event[i].isFinal() ) { nFinal++; // Remember final state unstable bosons if ( event[i].idAbs() == 23 || event[i].idAbs() == 24 ) { nFinBos++; nBosons++; mBos += event[i].m(); } } else if ( abs(event[i].status()) == 22 && ( event[i].idAbs() == 23 || event[i].idAbs() == 24 )) { nBosons++; mBos += event[i].m(); // Real mass } // Return averaged boson masses if ( nBosons > 0 && (nFinal + nFinBos*2) <= 3) return (mBos / double(nBosons)); else return mHat; } //-------------------------------------------------------------------------- // If the state has an incoming hadron return the flavour of the // parton entering the hard interaction. Otherwise return 0 int History::getCurrentFlav(const int side) const { int in = (side == 1) ? 3 : 4; return state[in].id(); } //-------------------------------------------------------------------------- double History::getCurrentX(const int side) const { int in = (side == 1) ? 3 : 4; return ( 2.*state[in].e()/state[0].e() ); } //-------------------------------------------------------------------------- double History::getCurrentZ(const int rad, const int rec, const int emt) const { int type = state[rad].isFinal() ? 1 : -1; double z = 0.; if (type == 1) { // Construct 2->3 variables for FSR Vec4 sum = state[rad].p() + state[rec].p() + state[emt].p(); double m2Dip = sum.m2Calc(); double x1 = 2. * (sum * state[rad].p()) / m2Dip; double x3 = 2. * (sum * state[emt].p()) / m2Dip; // Calculate z of splitting, different for FSR z = x1/(x1+x3); } else { // Construct momenta of dipole before/after splitting for ISR Vec4 qBR(state[rad].p() - state[emt].p() + state[rec].p()); Vec4 qAR(state[rad].p() + state[rec].p()); // Calculate z of splitting, different for ISR z = (qBR.m2Calc())/( qAR.m2Calc()); } return z; } //-------------------------------------------------------------------------- // Function to compute "pythia pT separation" from Particle input double History::pTLund(const Particle& RadAfterBranch, const Particle& EmtAfterBranch, const Particle& RecAfterBranch, int ShowerType) { // Save type: 1 = FSR pT definition, else ISR definition int Type = ShowerType; // Calculate virtuality of splitting int sign = (Type==1) ? 1 : -1; Vec4 Q(RadAfterBranch.p() + sign*EmtAfterBranch.p()); double Qsq = sign * Q.m2Calc(); // Mass term of radiator: Consider all non-light quark or gluon radiators // massive partons. bool isMassive = ( RadAfterBranch.idAbs() >= 4 && RadAfterBranch.id() != 21 ); double m2Rad = ( mergingHooksPtr->includeMassive() && isMassive ) ? pow2( particleDataPtr->m0(RadAfterBranch.id()) ) : 0.; // Construct 2->3 variables for FSR Vec4 sum = RadAfterBranch.p() + RecAfterBranch.p() + EmtAfterBranch.p(); double m2Dip = sum.m2Calc(); double x1 = 2. * (sum * RadAfterBranch.p()) / m2Dip; double x3 = 2. * (sum * EmtAfterBranch.p()) / m2Dip; // Construct momenta of dipole before/after splitting for ISR Vec4 qBR(RadAfterBranch.p() - EmtAfterBranch.p() + RecAfterBranch.p()); Vec4 qAR(RadAfterBranch.p() + RecAfterBranch.p()); // Calculate z of splitting, different for FSR and ISR double z = (Type==1) ? x1/(x1+x3) : (qBR.m2Calc())/( qAR.m2Calc()); // Separation of splitting, different for FSR and ISR double pTpyth = (Type==1) ? z*(1.-z) : (1.-z); // pT^2 = separation*virtuality pTpyth *= (Qsq - sign*m2Rad); if ( pTpyth < 0. ) pTpyth = 0.; // Return pT return sqrt(pTpyth); } //-------------------------------------------------------------------------- // Function to return the position of the initial line before (or after) // a single (!) splitting. int History::posChangedIncoming(const Event& event, bool before) { // Check for initial state splittings. // Consider a splitting to exist if both mother and sister were found. // Find sister int iSister = 0; for (int i =0; i < event.size(); ++i) if (event[i].status() == 43) { iSister = i; break; } // Find mother int iMother = 0; if (iSister > 0) iMother = event[iSister].mother1(); // Initial state splitting has been found. if (iSister > 0 && iMother > 0) { // Find flavour, mother flavour int flavSister = event[iSister].id(); int flavMother = event[iMother].id(); // Find splitting flavour int flavDaughter = 0; if ( abs(flavMother) < 21 && flavSister == 21) flavDaughter = flavMother; else if ( flavMother == 21 && flavSister == 21) flavDaughter = flavMother; else if ( flavMother == 21 && abs(flavSister) < 21) flavDaughter = -1*flavSister; else if ( abs(flavMother) < 21 && abs(flavSister) < 21) flavDaughter = 21; // Find initial state (!) daughter int iDaughter = 0; for (int i =0; i < event.size(); ++i) if ( !event[i].isFinal() && event[i].mother1() == iMother && event[i].id() == flavDaughter ) iDaughter = i; // Done for initial state splitting. if ( !before ) return iMother; else return iDaughter; } // Check for final state splittings with initial state recoiler. // Consider a splitting to exist if both mother and daughter were found. // Find new mother iMother = 0; for (int i =0; i < event.size(); ++i) if ( abs(event[i].status()) == 53 || abs(event[i].status()) == 54) { iMother = i; break; } // Find daughter int iDaughter = 0; if (iMother > 0) iDaughter = event[iMother].daughter1(); // Done if final state splitting has been found. if (iDaughter > 0 && iMother > 0) { // Done for final state splitting. if ( !before ) return iMother; else return iDaughter; } // If no splitting has been found, return zero. return 0; } //-------------------------------------------------------------------------- // Function to give back the ratio of PDFs and PDF * splitting kernels needed // to convert a splitting at scale pdfScale, chosen with running PDFs, to a // splitting chosen with PDFs at a fixed scale mu. As needed to properly count // emissions. double History::pdfFactor( const Event& event, const int type, double pdfScale, double mu ) { double weight = 1.; // Final state splittings if (type >= 3) { // Find new mother int iMother = 0; for (int i =0; i < event.size(); ++i) if ( abs(event[i].status()) == 53 || abs(event[i].status()) == 54) { iMother = i; break; } int flavMother = event[iMother].id(); // Done if no initial state recoiler was found if ( iMother == 0 ) return 1.; // Find daughter int iDaughter = event[iMother].daughter1(); int flavDaughter = event[iDaughter].id(); // Find x values double xMother = 2.*event[iMother].e() / event[0].e(); double xDaughter = 2.*event[iDaughter].e() / event[0].e(); // Calculate PDF ratios int sideSplit = ( event[iMother].pz() > 0.) ? 1 : -1; double pdfDen1, pdfDen2, pdfNum1, pdfNum2; pdfDen1 = pdfDen2 = pdfNum1 = pdfNum2 = 1.; if ( sideSplit == 1 ) { // Find PDFs pdfDen1 = max(1e-15,beamA.xfISR(0, flavDaughter, xDaughter, pow2(mu)) ); pdfNum1 = beamA.xfISR(0, flavDaughter, xDaughter, pow2(pdfScale) ); pdfNum2 = beamA.xfISR(0, flavMother, xMother, pow2(mu) ); pdfDen2 = max(1e-15,beamA.xfISR(0,flavMother, xMother, pow2(pdfScale)) ); } else { // Find PDFs pdfDen1 = max(1e-15,beamB.xfISR(0, flavDaughter, xDaughter, pow2(mu)) ); pdfNum1 = beamB.xfISR(0, flavDaughter, xDaughter, pow2(pdfScale) ); pdfNum2 = beamB.xfISR(0, flavMother, xMother, pow2(mu) ); pdfDen2 = max(1e-15,beamB.xfISR(0,flavMother, xMother, pow2(pdfScale)) ); } // The magnitude of the PDF ratio in FSR is limited to one. If that was // the case, return one. if ( pdfDen2/pdfNum1 > 1. ) return 1.; // Calculate PDF weight to reweight emission to emission evaluated at // constant factorisation scale. No need to include the splitting kernel in // the weight, since it will drop out anyway. weight = (pdfNum1/pdfDen1) * (pdfNum2)/(pdfDen2); // Initial state splittings } else if (type == 2) { // Find sister int iSister = 0; for (int i =0; i < event.size(); ++i) if (event[i].status() == 43) { iSister = i; break; } int flavSister = event[iSister].id(); // Find mother int iMother = event[iSister].mother1(); int flavMother = event[iMother].id(); // Find splitting flavour int flavDaughter = 0; if ( abs(flavMother) < 21 && flavSister == 21) flavDaughter = flavMother; else if ( flavMother == 21 && flavSister == 21) flavDaughter = flavMother; else if ( flavMother == 21 && abs(flavSister) < 21) flavDaughter = -1*flavSister; else if ( abs(flavMother) < 21 && abs(flavSister) < 21) flavDaughter = 21; // Find x values double xMother = 2.*event[iMother].e() / event[0].e(); // Find initial state (!) daughter int iDaughter = 0; for (int i =0; i < event.size(); ++i) if ( !event[i].isFinal() && event[i].mother1() == iMother && event[i].id() == flavDaughter ) iDaughter = i; double xDaughter = 2.*event[iDaughter].e() / event[0].e(); // Calculate PDF weight to reweight emission to emission evaluated at // constant factorisation scale. No need to include the splitting kernel // in the weight, since it will drop out anyway. int sideSplit = ( event[iMother].pz() > 0.) ? 1 : -1; double ratio1 = getPDFratio( sideSplit, false, false, flavDaughter, xDaughter, pdfScale, flavDaughter, xDaughter, mu ); double ratio2 = getPDFratio( sideSplit, false, false, flavMother, xMother, mu, flavMother, xMother, pdfScale ); weight = ratio1*ratio2; // Do nothing for MPI } else { weight = 1.; } // Done return weight; } //-------------------------------------------------------------------------- // Function giving the product of splitting kernels and PDFs so that the // resulting flavour is given by flav. This is used as a helper routine // to dgauss double History::integrand(int flav, double x, double scaleInt, double z) { // Declare constants double CF = 4./3.; double TR = 1./2.; double CA = 3.; double result = 0.; // Integrate NLL sudakov remainder if (flav==0) { AlphaStrong* as = mergingHooksPtr->AlphaS_ISR(); double asNow = (*as).alphaS(z); result = 1./z *asNow*asNow* ( log(scaleInt/z) -3./2. ); // Integrand for PDF ratios. Careful about factors if 1/z, since formulae // are expressed in terms if f(x,mu), while Pythia uses x*f(x,mu)! } else if (flav==21) { double measure1 = 1./(1. - z); double measure2 = 1.; double integrand1 = 2.*CA * z * beamB.xf( 21,x/z,pow(scaleInt,2)) / beamB.xf( 21,x, pow(scaleInt,2)) - 2.*CA; double integrand2 = // G -> G terms 2.*CA *((1. -z)/z + z*(1.-z)) * beamB.xf( 21,x/z,pow(scaleInt,2)) / beamB.xf( 21,x, pow(scaleInt,2)) // G -> Q terms + CF * ((1+pow(1-z,2))/z) *( beamB.xf( 1, x/z,pow(scaleInt,2)) / beamB.xf( 21, x, pow(scaleInt,2)) + beamB.xf( -1, x/z,pow(scaleInt,2)) / beamB.xf( 21, x, pow(scaleInt,2)) + beamB.xf( 2, x/z,pow(scaleInt,2)) / beamB.xf( 21, x, pow(scaleInt,2)) + beamB.xf( -2, x/z,pow(scaleInt,2)) / beamB.xf( 21, x, pow(scaleInt,2)) + beamB.xf( 3, x/z,pow(scaleInt,2)) / beamB.xf( 21, x, pow(scaleInt,2)) + beamB.xf( -3, x/z,pow(scaleInt,2)) / beamB.xf( 21, x, pow(scaleInt,2)) + beamB.xf( 4, x/z,pow(scaleInt,2)) / beamB.xf( 21, x, pow(scaleInt,2)) + beamB.xf( -4, x/z,pow(scaleInt,2)) / beamB.xf( 21, x, pow(scaleInt,2)) ); // Done result = integrand1*measure1 + integrand2*measure2; } else { double measure1 = 1./(1. -z); double measure2 = 1.; // Q -> Q terms double integrand1 = CF * (1+pow(z,2)) * beamB.xf( flav, x/z, pow(scaleInt,2)) / beamB.xf( flav, x, pow(scaleInt,2)) - 2.*CF; // Q -> G terms double integrand2 = + TR * (pow(z,2) + pow(1-z,2)) * beamB.xf( 21, x/z, pow(scaleInt,2)) / beamB.xf( flav, x, pow(scaleInt,2)); // Done result = measure1*integrand1 + measure2*integrand2; } return result; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/FragmentationSystems.cc0000644000175000017500000004437012217346245017633 0ustar sunsun// FragmentationSystems.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // ColConfig, StringRegion and StringSystem classes. #include "Pythia8/FragmentationSystems.h" namespace Pythia8 { //========================================================================== // The ColConfig class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // A typical u/d constituent mass. const double ColConfig::CONSTITUENTMASS = 0.325; //-------------------------------------------------------------------------- // Initialize and save pointers. void ColConfig::init(Info* infoPtrIn, Settings& settings, StringFlav* flavSelPtrIn) { // Save pointers. infoPtr = infoPtrIn; flavSelPtr = flavSelPtrIn; // Joining of nearby partons along the string. mJoin = settings.parm("FragmentationSystems:mJoin"); // For consistency ensure that mJoin is bigger than in StringRegion. mJoin = max( mJoin, 2. * StringRegion::MJOIN); // Simplification of q q q junction topology to quark - diquark one. mJoinJunction = settings.parm("FragmentationSystems:mJoinJunction"); mStringMin = settings.parm("HadronLevel:mStringMin"); } //-------------------------------------------------------------------------- // Insert a new colour singlet system in ascending mass order. // Calculate its properties. Join nearby partons. bool ColConfig::insert( vector& iPartonIn, Event& event) { // Find momentum and invariant mass of system, minus endpoint masses. Vec4 pSumIn; double mSumIn = 0.; bool hasJunctionIn = false; int nJunctionLegs = 0; for (int i = 0; i < int(iPartonIn.size()); ++i) { if (iPartonIn[i] < 0) { hasJunctionIn = true; ++nJunctionLegs; } else { pSumIn += event[ iPartonIn[i] ].p(); if (!event[ iPartonIn[i] ].isGluon()) mSumIn += event[ iPartonIn[i] ].constituentMass(); } } double massIn = pSumIn.mCalc(); double massExcessIn = massIn - mSumIn; // Check for rare triple- and higher junction systems (like J-Jbar-J) if (nJunctionLegs >= 5) { infoPtr->errorMsg("Error in ColConfig::insert: " "junction topology too complicated; too many junction legs"); return false; } // Check that junction systems have at least three legs. else if (nJunctionLegs > 0 && nJunctionLegs <= 2) { infoPtr->errorMsg("Error in ColConfig::insert: " "junction topology inconsistent; too few junction legs"); return false; } // Check that momenta do not contain not-a-number. if (abs(massExcessIn) >= 0.); else { infoPtr->errorMsg("Error in ColConfig::insert: " "not-a-number system mass"); return false; } // Identify closed gluon loop. Assign "endpoint" masses as light quarks. bool isClosedIn = (iPartonIn[0] >= 0 && event[ iPartonIn[0] ].col() != 0 && event[ iPartonIn[0] ].acol() != 0 ); if (isClosedIn) massExcessIn -= 2. * CONSTITUENTMASS; // For junction topology: join two nearby legs into a diquark. if (hasJunctionIn && joinJunction( iPartonIn, event, massExcessIn)) hasJunctionIn = false; // Loop while > 2 partons left and hope of finding joining pair. bool hasJoined = true; while (hasJoined && iPartonIn.size() > 2) { // Look for the pair of neighbour partons (along string) with // the smallest invariant mass (subtracting quark masses). int iJoinMin = -1; double mJoinMin = 2. * mJoin; int nSize = iPartonIn.size(); int nPair = (isClosedIn) ? nSize : nSize - 1; for (int i = 0; i < nPair; ++i) { // Keep three legs of junction separate. if (iPartonIn[i] < 0 || iPartonIn[(i + 1)%nSize] < 0) continue; Particle& parton1 = event[ iPartonIn[i] ]; Particle& parton2 = event[ iPartonIn[(i + 1)%nSize] ]; // Avoid joining non-partons, e.g. gluino/squark for R-hadron. if (!parton1.isParton() || !parton2.isParton()) continue; Vec4 pSumNow; pSumNow += (parton1.isGluon()) ? 0.5 * parton1.p() : parton1.p(); pSumNow += (parton2.isGluon()) ? 0.5 * parton2.p() : parton2.p(); double mJoinNow = pSumNow.mCalc(); if (!parton1.isGluon()) mJoinNow -= parton1.m(); if (!parton2.isGluon()) mJoinNow -= parton2.m(); if (mJoinNow < mJoinMin) { iJoinMin = i; mJoinMin = mJoinNow; } } // If sufficiently nearby then join into one new parton. // Note: error sensitivity to mJoin indicates unstable precedure?? hasJoined = false; if (mJoinMin < mJoin) { int iJoin1 = iPartonIn[iJoinMin]; int iJoin2 = iPartonIn[(iJoinMin + 1)%nSize]; int idNew = (event[iJoin1].isGluon()) ? event[iJoin2].id() : event[iJoin1].id(); int colNew = event[iJoin1].col(); int acolNew = event[iJoin2].acol(); if (colNew == acolNew) { colNew = event[iJoin2].col(); acolNew = event[iJoin1].acol(); } Vec4 pNew = event[iJoin1].p() + event[iJoin2].p(); // Append joined parton to event record. int iNew = event.append( idNew, 73, min(iJoin1, iJoin2), max(iJoin1, iJoin2), 0, 0, colNew, acolNew, pNew, pNew.mCalc() ); // Displaced lifetime/vertex; mothers should be same but prefer quark. int iVtx = (event[iJoin1].isGluon()) ? iJoin2 : iJoin1; event[iNew].tau( event[iVtx].tau() ); if (event[iVtx].hasVertex()) event[iNew].vProd( event[iVtx].vProd() ); // Mark joined partons and reduce remaining system. event[iJoin1].statusNeg(); event[iJoin2].statusNeg(); event[iJoin1].daughter1(iNew); event[iJoin2].daughter1(iNew); if (iJoinMin == nSize - 1) iPartonIn[0] = iNew; else { iPartonIn[iJoinMin] = iNew; for (int i = iJoinMin + 1; i < nSize - 1; ++i) iPartonIn[i] = iPartonIn[i + 1]; } iPartonIn.pop_back(); // If joined,then loopback to look for more. hasJoined = true; } } // Store new colour singlet system at the end. singlets.push_back( ColSinglet(iPartonIn, pSumIn, massIn, massExcessIn, hasJunctionIn, isClosedIn) ); // Now move around, so that smallest mass excesses come first. int iInsert = singlets.size() - 1; for (int iSub = singlets.size() - 2; iSub >= 0; --iSub) { if (massExcessIn > singlets[iSub].massExcess) break; singlets[iSub + 1] = singlets[iSub]; iInsert = iSub; } if (iInsert < int(singlets.size()) - 1) singlets[iInsert] = ColSinglet(iPartonIn, pSumIn, massIn, massExcessIn, hasJunctionIn, isClosedIn); // Done. return true; } //-------------------------------------------------------------------------- // Join two legs of junction to a diquark for small invariant masses. // Note: for junction system, iPartonIn points to structure // (-code0) g...g.q0 (-code1) g...g.q1 (-code2) g...g.q2 bool ColConfig::joinJunction( vector& iPartonIn, Event& event, double massExcessIn) { // Find four-momentum and endpoint quarks and masses on the three legs. Vec4 pLeg[3]; double mLeg[3] = { 0., 0., 0.}; int idAbsLeg[3]; int leg = -1; for (int i = 0; i < int(iPartonIn.size()); ++ i) { if (iPartonIn[i] < 0) ++leg; else { pLeg[leg] += event[ iPartonIn[i] ].p(); mLeg[leg] = event[ iPartonIn[i] ].m(); idAbsLeg[leg] = event[ iPartonIn[i] ].idAbs(); } } // Calculate invariant mass of three pairs, minus endpoint masses. double m01 = (pLeg[0] + pLeg[1]).mCalc() - mLeg[0] - mLeg[1]; double m02 = (pLeg[0] + pLeg[2]).mCalc() - mLeg[0] - mLeg[2]; double m12 = (pLeg[1] + pLeg[2]).mCalc() - mLeg[1] - mLeg[2]; // Find lowest-mass pair not involving diquark. double mMin = mJoinJunction + 1.; int legA = -1; int legB = -1; if (m01 < mMin && idAbsLeg[0] < 9 && idAbsLeg[1] < 9) { mMin = m01; legA = 0; legB = 1; } if (m02 < mMin && idAbsLeg[0] < 9 && idAbsLeg[2] < 9) { mMin = m02; legA = 0; legB = 2; } if (m12 < mMin && idAbsLeg[1] < 9 && idAbsLeg[2] < 9) { mMin = m12; legA = 1; legB = 2; } int legC = 3 - legA - legB; // Nothing to do if no two legs have small invariant mass, and // system as a whole is above MiniStringFragmentation threshold. if (legA == -1 || (mMin > mJoinJunction && massExcessIn > mStringMin)) return false; // Construct separate index arrays for the three legs. vector iLegA, iLegB, iLegC; leg = -1; for (int i = 0; i < int(iPartonIn.size()); ++ i) { if (iPartonIn[i] < 0) ++leg; else if( leg == legA) iLegA.push_back( iPartonIn[i] ); else if( leg == legB) iLegB.push_back( iPartonIn[i] ); else if( leg == legC) iLegC.push_back( iPartonIn[i] ); } // First step: successively combine any gluons on the two legs. // (Presumably overkill; not likely to be (m)any extra gluons.) // (Do as successive binary joinings, so only need two mothers.) for (leg = 0; leg < 2; ++leg) { vector& iLegNow = (leg == 0) ? iLegA : iLegB; int sizeNow = iLegNow.size(); for (int i = sizeNow - 2; i >= 0; --i) { int iQ = iLegNow.back(); int iG = iLegNow[i]; int colNew = (event[iQ].id() > 0) ? event[iG].col() : 0; int acolNew = (event[iQ].id() < 0) ? event[iG].acol() : 0; Vec4 pNew = event[iQ].p() + event[iG].p(); int iNew = event.append( event[iQ].id(), 74, min(iQ, iG), max(iQ, iG), 0, 0, colNew, acolNew, pNew, pNew.mCalc() ); // Mark joined partons and update iLeg end. event[iQ].statusNeg(); event[iG].statusNeg(); event[iQ].daughter1(iNew); event[iG].daughter1(iNew); iLegNow.back() = iNew; } } // Second step: combine two quarks into a diquark. int iQA = iLegA.back(); int iQB = iLegB.back(); int idQA = event[iQA].id(); int idQB = event[iQB].id(); int idNew = flavSelPtr->makeDiquark( idQA, idQB ); // Diquark colour is opposite to parton closest to junction on third leg. int colNew = (idNew > 0) ? 0 : event[ iLegC[0] ].acol(); int acolNew = (idNew > 0) ? event[ iLegC[0] ].col() : 0; Vec4 pNew = pLeg[legA] + pLeg[legB]; int iNew = event.append( idNew, 74, min(iQA, iQB), max( iQA, iQB), 0, 0, colNew, acolNew, pNew, pNew.mCalc() ); // Mark joined partons and reduce remaining system. event[iQA].statusNeg(); event[iQB].statusNeg(); event[iQA].daughter1(iNew); event[iQB].daughter1(iNew); iPartonIn.resize(0); iPartonIn.push_back( iNew); for (int i = 0; i < int(iLegC.size()) ; ++i) iPartonIn.push_back( iLegC[i]); // Remove junction from event record list, identifying by colour. int iJun = -1; for (int i = 0; i < event.sizeJunction(); ++i) for (int j = 0; j < 3; ++ j) if ( event.colJunction(i,j) == max(colNew, acolNew) ) iJun = i; if (iJun >= 0) event.eraseJunction(iJun); // Done, having eliminated junction. return true; } //-------------------------------------------------------------------------- // Collect all partons of singlet to be consecutively ordered. void ColConfig::collect(int iSub, Event& event, bool skipTrivial) { // Check that all partons have positive energy. for (int i = 0; i < singlets[iSub].size(); ++i) { int iNow = singlets[iSub].iParton[i]; if (iNow > 0 && event[iNow].e() < 0.) infoPtr->errorMsg("Warning in ColConfig::collect: " "negative-energy parton encountered"); } // Partons may already have been collected, e.g. at ministring collapse. if (singlets[iSub].isCollected) return; singlets[iSub].isCollected = true; // Check if partons already "by chance" happen to be ordered. bool inOrder = true; for (int i = 0; i < singlets[iSub].size() - 1; ++i) { int iFirst = singlets[iSub].iParton[i]; if (iFirst < 0) continue; int iSecond = singlets[iSub].iParton[i + 1]; if (iSecond < 0) iSecond = singlets[iSub].iParton[i + 2]; if (iSecond != iFirst + 1) { inOrder = false; break;} } // Normally done if in order, but sometimes may need to copy anyway. if (inOrder && skipTrivial) return; // Copy down system. Update current partons. for (int i = 0; i < singlets[iSub].size(); ++i) { int iOld = singlets[iSub].iParton[i]; if (iOld < 0) continue; int iNew = event.copy(iOld, 71); singlets[iSub].iParton[i] = iNew; } // Done. } //-------------------------------------------------------------------------- // Find to which singlet system a particle belongs. int ColConfig::findSinglet(int i) { // Loop through all systems and all members in them. for (int iSub = 0; iSub < int(singlets.size()); ++iSub) for (int iMem = 0; iMem < singlets[iSub].size(); ++iMem) if (singlets[iSub].iParton[iMem] == i) return iSub; // Done without having found particle; return -1 = error code. return -1; } //-------------------------------------------------------------------------- // List all currently identified singlets. void ColConfig::list(ostream& os) const { // Header. Loop over all individual singlets. os << "\n -------- Colour Singlet Systems Listing -------------------\n"; for (int iSub = 0; iSub < int(singlets.size()); ++iSub) { // List all partons belonging to each singlet. os << " singlet " << iSub << " contains " ; for (int i = 0; i < singlets[iSub].size(); ++i) os << singlets[iSub].iParton[i] << " "; os << "\n"; // Done. } } //========================================================================== // The StringRegion class. // Currently a number of simplifications, in particular ?? // 1) No popcorn baryon production. // 2) Simplified treatment of pT in stepping and joining. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // If a string region is smaller thsan this it is assumed empty. const double StringRegion::MJOIN = 0.1; // Avoid division by zero. const double StringRegion::TINY = 1e-20; //-------------------------------------------------------------------------- // Set up four-vectors for longitudinal and transverse directions. void StringRegion::setUp(Vec4 p1, Vec4 p2, bool isMassless) { // Simple case: the two incoming four-vectors guaranteed massless. if (isMassless) { // Calculate w2, minimum value. Lightcone directions = input. w2 = 2. * (p1 * p2); if (w2 < MJOIN*MJOIN) {isSetUp = true; isEmpty = true; return;} pPos = p1; pNeg = p2; // Else allow possibility of masses for incoming partons (also gluons!). } else { // Generic four-momentum combinations. double m1Sq = p1 * p1; double m2Sq = p2 * p2; double p1p2 = p1 * p2; w2 = m1Sq + 2. * p1p2 + m2Sq; double rootSq = pow2(p1p2) - m1Sq * m2Sq; // If crazy kinematics (should not happen!) modify energies. if (w2 <= 0. || rootSq <= 0.) { if (m1Sq < 0.) m1Sq = 0.; p1.e( sqrt(m1Sq + p1.pAbs2()) ); if (m2Sq < 0.) m2Sq = 0.; p2.e( sqrt(m2Sq + p2.pAbs2()) ); p1p2 = p1 * p2; w2 = m1Sq + 2. * p1p2 + m2Sq; rootSq = pow2(p1p2) - m1Sq * m2Sq; } // If still small invariant mass then empty region (e.g. in gg system). if (w2 < MJOIN*MJOIN) {isSetUp = true; isEmpty = true; return;} // Find two lightconelike longitudinal four-vector directions. double root = sqrt( max(TINY, rootSq) ); double k1 = 0.5 * ( (m2Sq + p1p2) / root - 1.); double k2 = 0.5 * ( (m1Sq + p1p2) / root - 1.); pPos = (1. + k1) * p1 - k2 * p2; pNeg = (1. + k2) * p2 - k1 * p1; } // Find two spacelike transverse four-vector directions. // Begin by picking two sensible trial directions. Vec4 eDiff = pPos / pPos.e() - pNeg / pNeg.e(); double eDx = pow2( eDiff.px() ); double eDy = pow2( eDiff.py() ); double eDz = pow2( eDiff.pz() ); if (eDx < min(eDy, eDz)) { eX = Vec4( 1., 0., 0., 0.); eY = (eDy < eDz) ? Vec4( 0., 1., 0., 0.) : Vec4( 0., 0., 1., 0.); } else if (eDy < eDz) { eX = Vec4( 0., 1., 0., 0.); eY = (eDx < eDz) ? Vec4( 1., 0., 0., 0.) : Vec4( 0., 0., 1., 0.); } else { eX = Vec4( 0., 0., 1., 0.); eY = (eDx < eDy) ? Vec4( 1., 0., 0., 0.) : Vec4( 0., 1., 0., 0.); } // Then construct orthogonal linear combinations. double pPosNeg = pPos * pNeg; double kXPos = eX * pPos / pPosNeg; double kXNeg = eX * pNeg / pPosNeg; double kXX = 1. / sqrt( 1. + 2. * kXPos * kXNeg * pPosNeg ); double kYPos = eY * pPos / pPosNeg; double kYNeg = eY * pNeg / pPosNeg; double kYX = kXX * (kXPos * kYNeg + kXNeg * kYPos) * pPosNeg; double kYY = 1. / sqrt(1. + 2. * kYPos * kYNeg * pPosNeg - pow2(kYX)); eX = kXX * (eX - kXNeg * pPos - kXPos * pNeg); eY = kYY * (eY - kYNeg * pPos - kYPos * pNeg - kYX * eX); // Done. isSetUp = true; isEmpty = false; } //-------------------------------------------------------------------------- // Project a four-momentum onto (x+, x-, px, py). void StringRegion::project(Vec4 pIn) { // Perform projections by four-vector multiplication. xPosProj = 2. * (pIn * pNeg) / w2; xNegProj = 2. * (pIn * pPos) / w2; pxProj = - (pIn * eX); pyProj = - (pIn * eY); } //========================================================================== // The StringSystem class. //-------------------------------------------------------------------------- // Set up system from parton list. void StringSystem::setUp(vector& iSys, Event& event) { // Figure out how big the system is. (Closed gluon loops?) sizePartons = iSys.size(); sizeStrings = sizePartons - 1; sizeRegions = (sizeStrings * (sizeStrings + 1)) / 2; indxReg = 2 * sizeStrings + 1; iMax = sizeStrings - 1; // Reserve space for the required number of regions. system.clear(); system.resize(sizeRegions); // Set up the lowest-lying regions. for (int i = 0; i < sizeStrings; ++i) { Vec4 p1 = event[ iSys[i] ].p(); if ( event[ iSys[i] ].isGluon() ) p1 *= 0.5; Vec4 p2 = event[ iSys[i+1] ].p(); if ( event[ iSys[i+1] ].isGluon() ) p2 *= 0.5; system[ iReg(i, iMax - i) ].setUp( p1, p2, false); } } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaHiggs.cc0000644000175000017500000023317112217346251015463 0ustar sunsun// SigmaHiggs.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // Part of code written by Marc Montull, CERN summer student 2007. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // Higgs simulation classes. #include "Pythia8/SigmaHiggs.h" namespace Pythia8 { //========================================================================== // Sigma1ffbar2H class. // Cross section for f fbar -> H0 , H1, H2 or A3. // (f is quark or lepton, H0 SM Higgs and H1, H2, A3 BSM Higgses ). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2H::initProc() { // Properties specific to Higgs state. if (higgsType == 0) { nameSave = "f fbar -> H (SM)"; codeSave = 901; idRes = 25; } else if (higgsType == 1) { nameSave = "f fbar -> h0(H1)"; codeSave = 1001; idRes = 25; } else if (higgsType == 2) { nameSave = "f fbar -> H0(H2)"; codeSave = 1021; idRes = 35; } else if (higgsType == 3) { nameSave = "f fbar -> A0(A3)"; codeSave = 1041; idRes = 36; } // Find pointer to H0, H1, H2 or A3 depending on the value of idRes. HResPtr = particleDataPtr->particleDataEntryPtr(idRes); // Store H0, H1, H2 or A3 mass and width for propagator. mRes = HResPtr->m0(); GammaRes = HResPtr->mWidth(); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma1ffbar2H::sigmaKin() { // Set up Breit-Wigner. double width = HResPtr->resWidth(idRes, mH); sigBW = 4. * M_PI/ ( pow2(sH - m2Res) + pow2(mH * width) ); // Width out only includes open channels. widthOut = width * HResPtr->resOpenFrac(idRes); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma1ffbar2H::sigmaHat() { // Calculate mass-dependent incoming width, including colour factor. int idAbs = abs(id1); double widthIn = HResPtr->resWidthChan( mH, idAbs, -idAbs); if (idAbs < 9) widthIn /= 9.; // Done. return widthIn * sigBW * widthOut; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2H::setIdColAcol() { // Flavours trivial. setId( id1, id2, idRes); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma1ffbar2H::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma1gg2H class. // Cross section for g g -> H0, H1, H2 or A3 (H0 SM Higgs, H1, H2, A3 BSM). //-------------------------------------------------------------------------- // Initialize process. void Sigma1gg2H::initProc() { // Properties specific to Higgs state. if (higgsType == 0) { nameSave = "g g -> H (SM)"; codeSave = 902; idRes = 25; } else if (higgsType == 1) { nameSave = "g g -> h0(H1)"; codeSave = 1002; idRes = 25; } else if (higgsType == 2) { nameSave = "g g -> H0(H2)"; codeSave = 1022; idRes = 35; } else if (higgsType == 3) { nameSave = "g g -> A0(A3)"; codeSave = 1042; idRes = 36; } // Find pointer to H0, H1, H2 or A3 depending on idRes. HResPtr = particleDataPtr->particleDataEntryPtr(idRes); // Store H0, H1, H2 or A3 mass and width for propagator. mRes = HResPtr->m0(); GammaRes = HResPtr->mWidth(); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1gg2H::sigmaKin() { // Incoming width for gluons, gives colour factor of 1/8 * 1/8. double widthIn = HResPtr->resWidthChan( mH, 21, 21) / 64.; // Set up Breit-Wigner. double width = HResPtr->resWidth(idRes, mH); double sigBW = 8. * M_PI/ ( pow2(sH - m2Res) + pow2(mH * width) ); // Width out only includes open channels. double widthOut = width * HResPtr->resOpenFrac(idRes); // Done. sigma = widthIn * sigBW * widthOut; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1gg2H::setIdColAcol() { // Flavours trivial. setId( 21, 21, idRes); // Colour flow topology. setColAcol( 1, 2, 2, 1, 0, 0); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma1gg2H::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma1gmgm2H class. // Cross section for gamma gamma -> H0, H1, H2 or H3. // (H0 SM Higgs, H1, H2 and A3 BSM Higgses). //-------------------------------------------------------------------------- // Initialize process. void Sigma1gmgm2H::initProc() { // Properties specific to Higgs state. if (higgsType == 0) { nameSave = "gamma gamma -> H (SM)"; codeSave = 903; idRes = 25; } else if (higgsType == 1) { nameSave = "gamma gamma -> h0(H1)"; codeSave = 1003; idRes = 25; } else if (higgsType == 2) { nameSave = "gamma gamma -> H0(H2)"; codeSave = 1023; idRes = 35; } else if (higgsType == 3) { nameSave = "gamma gamma -> A0(A3)"; codeSave = 1043; idRes = 36; } // Find pointer to H0, H1, H2 or A3. HResPtr = particleDataPtr->particleDataEntryPtr(idRes); // Store H0, H1, H2 or A3 mass and width for propagator. mRes = HResPtr->m0(); GammaRes = HResPtr->mWidth(); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1gmgm2H::sigmaKin() { // Incoming width for photons. double widthIn = HResPtr->resWidthChan( mH, 22, 22); // Set up Breit-Wigner. double width = HResPtr->resWidth(idRes, mH); double sigBW = 8. * M_PI/ ( pow2(sH - m2Res) + pow2(mH * width) ); // Width out only includes open channels. double widthOut = width * HResPtr->resOpenFrac(idRes); // Done. sigma = widthIn * sigBW * widthOut; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1gmgm2H::setIdColAcol() { // Flavours trivial. setId( 22, 22, idRes); // Colour flow trivial. setColAcol( 0, 0, 0, 0, 0, 0); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma1gmgm2H::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma2ffbar2HZ class. // Cross section for f fbar -> H0 Z0, H1 Z0, H2 Z0 or A3 Z0. // (H0 SM Higgs, H1, H2 and A3 BSM Higgses). //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2HZ::initProc() { // Properties specific to Higgs state. if (higgsType == 0) { nameSave = "f fbar -> H0 Z0 (SM)"; codeSave = 904; idRes = 25; coup2Z = 1.; } else if (higgsType == 1) { nameSave = "f fbar -> h0(H1) Z0"; codeSave = 1004; idRes = 25; coup2Z = settingsPtr->parm("HiggsH1:coup2Z"); } else if (higgsType == 2) { nameSave = "f fbar -> H0(H2) Z0"; codeSave = 1024; idRes = 35; coup2Z = settingsPtr->parm("HiggsH2:coup2Z"); } else if (higgsType == 3) { nameSave = "f fbar -> A0(A3) ZO"; codeSave = 1044; idRes = 36; coup2Z = settingsPtr->parm("HiggsA3:coup2Z"); } // Store Z0 mass and width for propagator. Common coupling factor. mZ = particleDataPtr->m0(23); widZ = particleDataPtr->mWidth(23); mZS = mZ*mZ; mwZS = pow2(mZ * widZ); thetaWRat = 1. / (16. * couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(idRes, 23); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2HZ::sigmaKin() { // Evaluate differential cross section. sigma0 = (M_PI / sH2) * 8. * pow2(alpEM * thetaWRat * coup2Z) * (tH * uH - s3 * s4 + 2. * sH * s4) / (pow2(sH - mZS) + mwZS); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2HZ::sigmaHat() { // Coupling a_f^2 + v_f^2 to s-channel Z0 and colour factor. int idAbs = abs(id1); double sigma = sigma0 * couplingsPtr->vf2af2(idAbs); if (idAbs < 9) sigma /= 3.; // Secondary width for H0 and Z0 or H1 and Z0 or H2 and Z0 or A3 and Z0. sigma *= openFracPair; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2HZ::setIdColAcol() { // Flavours trivial. setId( id1, id2, idRes, 23); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma2ffbar2HZ::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // If not decay of Z0 created along with Higgs then done. if (iResBeg != 5 || iResEnd != 6) return 1.; // Order so that fbar(1) f(2) -> H() f'(3) fbar'(4). int i1 = (process[3].id() < 0) ? 3 : 4; int i2 = 7 - i1; int i3 = process[6].daughter1(); int i4 = process[6].daughter2(); if (process[i3].id() < 0) swap( i3, i4); // Find left- and righthanded couplings of fermion pairs. int idAbs = process[i1].idAbs(); double liS = pow2( couplingsPtr->lf(idAbs) ); double riS = pow2( couplingsPtr->rf(idAbs) ); idAbs = process[i3].idAbs(); double lfS = pow2( couplingsPtr->lf(idAbs) ); double rfS = pow2( couplingsPtr->rf(idAbs) ); // Evaluate relevant four-products. double pp13 = process[i1].p() * process[i3].p(); double pp14 = process[i1].p() * process[i4].p(); double pp23 = process[i2].p() * process[i3].p(); double pp24 = process[i2].p() * process[i4].p(); // Weight and maximum. double wt = (liS * lfS + riS * rfS) * pp13 * pp24 + (liS * rfS + riS * lfS) * pp14 * pp23; double wtMax = (liS + riS) * (lfS + rfS) * (pp13 + pp14) * (pp23 + pp24); // Done. return wt / wtMax; } //========================================================================== // Sigma2ffbar2HW class. // Cross section for f fbar -> H0 W+-, H1 W+-, H2 W+- or A3 W+-. // (H0 SM Higgs, H1, H2 and A3 BSM Higgses). //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2HW::initProc() { // Properties specific to Higgs state. if (higgsType == 0) { nameSave = "f fbar -> H0 W+- (SM)"; codeSave = 905; idRes = 25; coup2W = 1.; } else if (higgsType == 1) { nameSave = "f fbar -> h0(H1) W+-"; codeSave = 1005; idRes = 25; coup2W = settingsPtr->parm("HiggsH1:coup2W"); } else if (higgsType == 2) { nameSave = "f fbar -> H0(H2) W+-"; codeSave = 1025; idRes = 35; coup2W = settingsPtr->parm("HiggsH2:coup2W"); } else if (higgsType == 3) { nameSave = "f fbar -> A0(A3) W+-"; codeSave = 1045; idRes = 36; coup2W = settingsPtr->parm("HiggsA3:coup2W"); } // Store W+- mass and width for propagator. Common coupling factor. mW = particleDataPtr->m0(24); widW = particleDataPtr->mWidth(24); mWS = mW*mW; mwWS = pow2(mW * widW); thetaWRat = 1. / (4. * couplingsPtr->sin2thetaW()); // Secondary open width fractions. openFracPairPos = particleDataPtr->resOpenFrac(idRes, 24); openFracPairNeg = particleDataPtr->resOpenFrac(idRes, -24); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2HW::sigmaKin() { // Evaluate differential cross section. sigma0 = (M_PI / sH2) * 2. * pow2(alpEM * thetaWRat * coup2W) * (tH * uH - s3 * s4 + 2. * sH * s4) / (pow2(sH - mWS) + mwWS); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2HW::sigmaHat() { // CKM and colour factors. double sigma = sigma0; if (abs(id1) < 9) sigma *= couplingsPtr->V2CKMid(abs(id1), abs(id2)) / 3.; // Secondary width for H0 and W+-. int idUp = (abs(id1)%2 == 0) ? id1 : id2; sigma *= (idUp > 0) ? openFracPairPos : openFracPairNeg; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2HW::setIdColAcol() { // Sign of outgoing W. int sign = 1 - 2 * (abs(id1)%2); if (id1 < 0) sign = -sign; setId( id1, id2, idRes, 24 * sign); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma2ffbar2HW::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // If not decay of W+- created along with Higgs then done. if (iResBeg != 5 || iResEnd != 6) return 1.; // Order so that fbar(1) f(2) -> H() f'(3) fbar'(4). int i1 = (process[3].id() < 0) ? 3 : 4; int i2 = 7 - i1; int i3 = process[6].daughter1(); int i4 = process[6].daughter2(); if (process[i3].id() < 0) swap( i3, i4); // Evaluate relevant four-products. double pp13 = process[i1].p() * process[i3].p(); double pp14 = process[i1].p() * process[i4].p(); double pp23 = process[i2].p() * process[i3].p(); double pp24 = process[i2].p() * process[i4].p(); // Weight and maximum. double wt = pp13 * pp24; double wtMax = (pp13 + pp14) * (pp23 + pp24); // Done. return wt / wtMax; } //========================================================================== // Sigma3ff2HfftZZ class. // Cross section for f f' -> H f f' (Z0 Z0 fusion of SM or BSM Higgs). // (H can be H0 SM or H1, H2, A3 from BSM). //-------------------------------------------------------------------------- // Initialize process. void Sigma3ff2HfftZZ::initProc() { // Properties specific to Higgs state. if (higgsType == 0) { nameSave = "f f' -> H0 f f'(Z0 Z0 fusion) (SM)"; codeSave = 906; idRes = 25; coup2Z = 1.; } else if (higgsType == 1) { nameSave = "f f' -> h0(H1) f f' (Z0 Z0 fusion)"; codeSave = 1006; idRes = 25; coup2Z = settingsPtr->parm("HiggsH1:coup2Z"); } else if (higgsType == 2) { nameSave = "f f' -> H0(H2) f f' (Z0 Z0 fusion)"; codeSave = 1026; idRes = 35; coup2Z = settingsPtr->parm("HiggsH2:coup2Z"); } else if (higgsType == 3) { nameSave = "f f' -> A0(A3) f f' (Z0 Z0 fusion)"; codeSave = 1046; idRes = 36; coup2Z = settingsPtr->parm("HiggsA3:coup2Z"); } // Common fixed mass and coupling factor. mZS = pow2( particleDataPtr->m0(23) ); prefac = 0.25 * mZS * pow3( 4. * M_PI / (couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()) ); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(idRes); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma3ff2HfftZZ::sigmaKin() { // Required four-vector products. double pp12 = 0.5 * sH; double pp14 = 0.5 * mH * p4cm.pNeg(); double pp15 = 0.5 * mH * p5cm.pNeg(); double pp24 = 0.5 * mH * p4cm.pPos(); double pp25 = 0.5 * mH * p5cm.pPos(); double pp45 = p4cm * p5cm; // Propagator factors and two possible numerators. double prop = pow2( (2. * pp14 + mZS) * (2. * pp25 + mZS) ); sigma1 = prefac * pp12 * pp45 / prop; sigma2 = prefac * pp15 * pp24 / prop; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma3ff2HfftZZ::sigmaHat() { // Flavour-dependent coupling factors for two incoming flavours. int id1Abs = abs(id1); int id2Abs = abs(id2); double lf1S = pow2( couplingsPtr->lf(id1Abs) ); double rf1S = pow2( couplingsPtr->rf(id1Abs) ); double lf2S = pow2( couplingsPtr->lf(id2Abs) ); double rf2S = pow2( couplingsPtr->rf(id2Abs) ); double c1 = lf1S * lf2S + rf1S * rf2S; double c2 = lf1S * rf2S + rf1S * lf2S; // Combine couplings and kinematics factors. double sigma = pow3(alpEM) * (c1 * sigma1 + c2 * sigma2) * pow2(coup2Z); // Secondary width for H0, H1, H2 or A3. sigma *= openFrac; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3ff2HfftZZ::setIdColAcol() { // Trivial flavours: out = in. setId( id1, id2, idRes, id1, id2); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9 && abs(id2) < 9 && id1*id2 > 0) setColAcol( 1, 0, 2, 0, 0, 0, 1, 0, 2, 0); else if (abs(id1) < 9 && abs(id2) < 9) setColAcol( 1, 0, 0, 2, 0, 0, 1, 0, 0, 2); else if (abs(id1) < 9) setColAcol( 1, 0, 0, 0, 0, 0, 1, 0, 0, 0); else if (abs(id2) < 9) setColAcol( 0, 0, 1, 0, 0, 0, 0, 0, 1, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0, 0, 0); if ( (abs(id1) < 9 && id1 < 0) || (abs(id1) > 10 && id2 < 0) ) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma3ff2HfftZZ::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma3ff2HfftWW class. // Cross section for f_1 f_2 -> H0 f_3 f_4 (W+ W- fusion of SM or BSM Higgs). //-------------------------------------------------------------------------- // Initialize process. void Sigma3ff2HfftWW::initProc() { // Properties specific to Higgs state. if (higgsType == 0) { nameSave = "f_1 f_2 -> H0 f_3 f_4 (W+ W- fusion) (SM)"; codeSave = 907; idRes = 25; coup2W = 1.; } else if (higgsType == 1) { nameSave = "f_1 f_2 -> h0(H1) f_3 f_4 (W+ W- fusion)"; codeSave = 1007; idRes = 25; coup2W = settingsPtr->parm("HiggsH1:coup2W"); } else if (higgsType == 2) { nameSave = "f_1 f_2 -> H0(H2) f_3 f_4 (W+ W- fusion)"; codeSave = 1027; idRes = 35; coup2W = settingsPtr->parm("HiggsH2:coup2W"); } else if (higgsType == 3) { nameSave = "f_1 f_2 -> A0(A3) f_3 f_4 (W+ W- fusion)"; codeSave = 1047; idRes = 36; coup2W = settingsPtr->parm("HiggsA3:coup2W"); } // Common fixed mass and coupling factor. mWS = pow2( particleDataPtr->m0(24) ); prefac = mWS * pow3( 4. * M_PI / couplingsPtr->sin2thetaW() ); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(idRes); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma3ff2HfftWW::sigmaKin() { // Required four-vector products. double pp12 = 0.5 * sH; double pp14 = 0.5 * mH * p4cm.pNeg(); double pp25 = 0.5 * mH * p5cm.pPos(); double pp45 = p4cm * p5cm; // Cross section: kinematics part. Combine with couplings. double prop = pow2( (2. * pp14 + mWS) * (2. * pp25 + mWS) ); sigma0 = prefac * pp12 * pp45 * pow2(coup2W) / prop; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma3ff2HfftWW::sigmaHat() { // Some flavour combinations not possible. int id1Abs = abs(id1); int id2Abs = abs(id2); if ( (id1Abs%2 == id2Abs%2 && id1 * id2 > 0) || (id1Abs%2 != id2Abs%2 && id1 * id2 < 0) ) return 0.; // Basic cross section. CKM factors for final states. double sigma = sigma0 * pow3(alpEM) * couplingsPtr->V2CKMsum(id1Abs) * couplingsPtr->V2CKMsum(id2Abs); // Secondary width for H0, H1, H2 or A3. sigma *= openFrac; // Spin-state extra factor 2 per incoming neutrino. if (id1Abs == 12 || id1Abs == 14 || id1Abs == 16) sigma *= 2.; if (id2Abs == 12 || id2Abs == 14 || id2Abs == 16) sigma *= 2.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3ff2HfftWW::setIdColAcol() { // Pick out-flavours by relative CKM weights. id4 = couplingsPtr->V2CKMpick(id1); id5 = couplingsPtr->V2CKMpick(id2); setId( id1, id2, idRes, id4, id5); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9 && abs(id2) < 9 && id1*id2 > 0) setColAcol( 1, 0, 2, 0, 0, 0, 1, 0, 2, 0); else if (abs(id1) < 9 && abs(id2) < 9) setColAcol( 1, 0, 0, 2, 0, 0, 1, 0, 0, 2); else if (abs(id1) < 9) setColAcol( 1, 0, 0, 0, 0, 0, 1, 0, 0, 0); else if (abs(id2) < 9) setColAcol( 0, 0, 1, 0, 0, 0, 0, 0, 1, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0, 0, 0); if ( (abs(id1) < 9 && id1 < 0) || (abs(id1) > 10 && id2 < 0) ) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma3ff2HfftWW::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma3gg2HQQbar class. // Cross section for g g -> H0 Q Qbar (Q Qbar fusion of SM or BSM Higgs). //-------------------------------------------------------------------------- // Initialize process. void Sigma3gg2HQQbar::initProc() { // Properties specific to Higgs state for the "g g -> H ttbar" process. // (H can be H0 SM or H1, H2, A3 from BSM). if (higgsType == 0 && idNew == 6) { nameSave = "g g -> H t tbar (SM)"; codeSave = 908; idRes = 25; coup2Q = 1.; } else if (higgsType == 1 && idNew == 6) { nameSave = "g g -> h0(H1) t tbar"; codeSave = 1008; idRes = 25; coup2Q = settingsPtr->parm("HiggsH1:coup2u"); } else if (higgsType == 2 && idNew == 6) { nameSave = "g g -> H0(H2) t tbar"; codeSave = 1028; idRes = 35; coup2Q = settingsPtr->parm("HiggsH2:coup2u"); } else if (higgsType == 3 && idNew == 6) { nameSave = "g g -> A0(A3) t tbar"; codeSave = 1048; idRes = 36; coup2Q = settingsPtr->parm("HiggsA3:coup2u"); } // Properties specific to Higgs state for the "g g -> H b bbar" process. // (H can be H0 SM or H1, H2, A3 from BSM). if (higgsType == 0 && idNew == 5) { nameSave = "g g -> H b bbar (SM)"; codeSave = 912; idRes = 25; coup2Q = 1.; } else if (higgsType == 1 && idNew == 5) { nameSave = "g g -> h0(H1) b bbar"; codeSave = 1012; idRes = 25; coup2Q = settingsPtr->parm("HiggsH1:coup2d"); } else if (higgsType == 2 && idNew == 5) { nameSave = "g g -> H0(H2) b bbar"; codeSave = 1032; idRes = 35; coup2Q = settingsPtr->parm("HiggsH2:coup2d"); } else if (higgsType == 3 && idNew == 5) { nameSave = "g g -> A0(A3) b bbar"; codeSave = 1052; idRes = 36; coup2Q = settingsPtr->parm("HiggsA3:coup2d"); } // Common mass and coupling factors. double mWS = pow2(particleDataPtr->m0(24)); prefac = (4. * M_PI / couplingsPtr->sin2thetaW()) * pow2(4. * M_PI) * 0.25 / mWS; // Secondary open width fraction. openFracTriplet = particleDataPtr->resOpenFrac(idRes, idNew, -idNew); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma3gg2HQQbar::sigmaKin() { // Running mass of heavy quark. double mQ2run = pow2( particleDataPtr->mRun(idNew, mH) ); // Linear combination of p_Q and p_Qbar to ensure common mass. double mQ2 = m4 * m5; double epsi = 0.; if (m4 != m5) { double s45 = (p4cm + p5cm).m2Calc(); mQ2 = 0.5 * (s4 + s5) - 0.25 * pow2(s4 - s5) / s45; epsi = 0.5 * (s5 - s4) / s45; } // Set up kinematics: g(4) g(5) -> H(3) Q(1) Qbar(2) in outgoing sense. Vec4 pTemp[6]; pTemp[4] = Vec4( 0., 0., -0.5* mH, -0.5* mH); pTemp[5] = Vec4( 0., 0., 0.5* mH, -0.5* mH); pTemp[1] = p4cm + epsi * (p4cm + p5cm); pTemp[2] = p5cm - epsi * (p4cm + p5cm); pTemp[3] = p3cm; // Four-product combinations. double z1 = pTemp[1] * pTemp[2]; double z2 = pTemp[1] * pTemp[3]; double z3 = pTemp[1] * pTemp[4]; double z4 = pTemp[1] * pTemp[5]; double z5 = pTemp[2] * pTemp[3]; double z6 = pTemp[2] * pTemp[4]; double z7 = pTemp[2] * pTemp[5]; double z8 = pTemp[3] * pTemp[4]; double z9 = pTemp[3] * pTemp[5]; double z10 = pTemp[4] * pTemp[5]; // Powers required as shorthand in matriz elements. double mQ4 = mQ2 * mQ2; double mQ6 = mQ2 * mQ4; double z1S = z1 * z1; double z2S = z2 * z2; double z3S = z3 * z3; double z4S = z4 * z4; double z5S = z5 * z5; double z6S = z6 * z6; double z7S = z7 * z7; double z8S = z8 * z8; double z9S = z9 * z9; double z10S = z10 * z10; // Evaluate matriz elements for g + g -> Q + Qbar + H. // (H can be H0 SM or H1, H2, A3 from BSM). double fm[9][9]; fm[1][1] = 64*mQ6+16*mQ4*s3+32*mQ4*(z1+2*z2+z4+z9+2* z7+z5)+8*mQ2*s3*(-z1-z4+2*z7)+16*mQ2*(z2*z9+4*z2* z7+z2*z5-2*z4*z7-2*z9*z7)+8*s3*z4*z7-16*z2*z9*z7; fm[1][2] = 16*mQ6+8*mQ4*(-2*z1+z2-2*z3-2*z4-4*z10+z9-z8+2 *z7-4*z6+z5)+8*mQ2*(-2*z1*z2-2*z2*z4-2*z2*z10+z2*z7-2* z2*z6-2*z3*z7+2*z4*z7+4*z10*z7-z9*z7-z8*z7)+16*z2*z7*(z4+ z10); fm[1][3] = 16*mQ6-4*mQ4*s3+8*mQ4*(-2*z1+2*z2-2*z3-4* z4-8*z10+z9+z8-2*z7-4*z6+2*z5)-(4*mQ2*s3)*(z1+z4+z10 +z6)+8*mQ2*(-2*z1*z2-2*z1*z10+z1*z9+z1*z8-2*z1*z5+z2S -4*z2*z4-5*z2*z10+z2*z8-z2*z7-3*z2*z6+z2*z5+z3*z9+2*z3*z7 -z3*z5+z4*z8+2*z4*z6-3*z4*z5-5*z10*z5+z9*z8+z9*z6+z9*z5+ z8*z7-4*z6*z5+z5S)-(16*z2*z5)*(z1+z4+z10+z6); fm[1][4] = 16*mQ6+4*mQ4*s3+16*mQ4*(-z1+z2-z3-z4+z10- z9-z8+2*z7+2*z6-z5)+4*mQ2*s3*(z1+z3+z4+z10+2*z7+2*z6 )+8*mQ2*(4*z1*z10+4*z1*z7+4*z1*z6+2*z2*z10-z2*z9-z2*z8+ 4*z2*z7+4*z2*z6-z2*z5+4*z10*z5+4*z7*z5+4*z6*z5)-(8*s3* z1)*(z10+z7+z6)+16*z2*z5*(z10+z7+z6); fm[1][5] = 8*mQ4*(-2*z1-2*z4+z10-z9)+4*mQ2*(4*z1S-2*z1* z2+8*z1*z3+6*z1*z10-2*z1*z9+4*z1*z8+4*z1*z7+4*z1*z6+2*z1* z5+z2*z10+4*z3*z4-z3*z9+2*z3*z7+3*z4*z8-2*z4*z6+2*z4*z5-4 *z10*z7+3*z10*z5-3*z9*z6+3*z8*z7-4*z7S+4*z7*z5)+8*(z1S *z9-z1S*z8-z1*z2*z7+z1*z2*z6+z1*z3*z9+z1*z3*z5-z1*z4* z8-z1*z4*z5+z1*z10*z9+z1*z9*z7+z1*z9*z6-z1*z8*z7-z2*z3*z7 +z2*z4*z6-z2*z10*z7-z2*z7S+z3*z7*z5-z4*z10*z5-z4*z7*z5- z4*z6*z5); fm[1][6] = 16*mQ4*(-4*z1-z4+z9-z7)+4*mQ2*s3*(-2*z1-z4- z7)+16*mQ2*(-2*z1S-3*z1*z2-2*z1*z4-3*z1*z9-2*z1*z7-3* z1*z5-2*z2*z4-2*z7*z5)-8*s3*z4*z7+8*(-z1*z2*z9-2*z1*z2 *z5-z1*z9S-z1*z9*z5+z2S*z7-z2*z4*z5+z2*z9*z7-z2*z7*z5 +z4*z9*z5+z4*z5S); fm[1][7] = 8*mQ4*(2*z3+z4+3*z10+z9+2*z8+3*z7+6*z6)+2*mQ2* s3*(-2*z3-z4+3*z10+3*z7+6*z6)+4*mQ2*(4*z1*z10+4*z1* z7+8*z1*z6+6*z2*z10+z2*z9+2*z2*z8+6*z2*z7+12*z2*z6-8*z3* z7+4*z4*z7+4*z4*z6+4*z10*z5+4*z9*z7+4*z9*z6-8*z8*z7+4*z7* z5+8*z6*z5)+4*s3*(-z1*z10-z1*z7-2*z1*z6+2*z3*z7-z4*z7- z4*z6)+8*z2*(z10*z5+z9*z7+z9*z6-2*z8*z7+z7*z5+2*z6*z5); fm[1][8] = 8*mQ4*(2*z3+z4+3*z10+2*z9+z8+3*z7+6*z6)+2*mQ2* s3*(-2*z3-z4+2*z10+z7+2*z6)+4*mQ2*(4*z1*z10-2*z1*z9+ 2*z1*z8+4*z1*z7+8*z1*z6+5*z2*z10+2*z2*z9+z2*z8+4*z2*z7+8* z2*z6-z3*z9-8*z3*z7+2*z3*z5+2*z4*z9-z4*z8+4*z4*z7+4*z4*z6 +4*z4*z5+5*z10*z5+z9S-z9*z8+2*z9*z7+5*z9*z6+z9*z5-7*z8* z7+2*z8*z5+2*z7*z5+10*z6*z5)+2*s3*(-z1*z10+z3*z7-2*z4* z7+z4*z6)+4*(-z1*z9S+z1*z9*z8-2*z1*z9*z5-z1*z8*z5+2*z2* z10*z5+z2*z9*z7+z2*z9*z6-2*z2*z8*z7+3*z2*z6*z5+z3*z9*z5+ z3*z5S+z4*z9*z5-2*z4*z8*z5+2*z4*z5S); fm[2][2] = 16*mQ6+16*mQ4*(-z1+z3-z4-z10+z7-z6)+16*mQ2*( z3*z10+z3*z7+z3*z6+z4*z7+z10*z7)-16*z3*z10*z7; fm[2][3] = 16*mQ6+8*mQ4*(-2*z1+z2+2*z3-4*z4-4*z10-z9+z8-2 *z7-2*z6+z5)+8*mQ2*(-2*z1*z5+4*z3*z10-z3*z9-z3*z8-2*z3* z7+2*z3*z6+z3*z5-2*z4*z5-2*z10*z5-2*z6*z5)+16*z3*z5*(z10+ z6); fm[2][4] = 8*mQ4*(-2*z1-2*z3+z10-z8)+4*mQ2*(4*z1S-2*z1* z2+8*z1*z4+6*z1*z10+4*z1*z9-2*z1*z8+4*z1*z7+4*z1*z6+2*z1* z5+z2*z10+4*z3*z4+3*z3*z9-2*z3*z7+2*z3*z5-z4*z8+2*z4*z6-4 *z10*z6+3*z10*z5+3*z9*z6-3*z8*z7-4*z6S+4*z6*z5)+8*(-z1S *z9+z1S*z8+z1*z2*z7-z1*z2*z6-z1*z3*z9-z1*z3*z5+z1*z4 *z8+z1*z4*z5+z1*z10*z8-z1*z9*z6+z1*z8*z7+z1*z8*z6+z2*z3* z7-z2*z4*z6-z2*z10*z6-z2*z6S-z3*z10*z5-z3*z7*z5-z3*z6* z5+z4*z6*z5); fm[2][5] = 16*mQ4*z10+8*mQ2*(2*z1S+2*z1*z3+2*z1*z4+2*z1 *z10+2*z1*z7+2*z1*z6+z3*z7+z4*z6)+8*(-2*pow3(z1)-2*z1S*z3- 2*z1S*z4-2*z1S*z10-2*z1S*z7-2*z1S*z6-2*z1*z3*z4- z1*z3*z10-2*z1*z3*z6-z1*z4*z10-2*z1*z4*z7-z1*z10S-z1* z10*z7-z1*z10*z6-2*z1*z7*z6+z3S*z7-z3*z4*z7-z3*z4*z6+z3 *z10*z7+z3*z7S-z3*z7*z6+z4S*z6+z4*z10*z6-z4*z7*z6+z4* z6S); fm[2][6] = 8*mQ4*(-2*z1+z10-z9-2*z7)+4*mQ2*(4*z1S+2*z1* z2+4*z1*z3+4*z1*z4+6*z1*z10-2*z1*z9+4*z1*z8+8*z1*z6-2*z1* z5+4*z2*z4+3*z2*z10+2*z2*z7-3*z3*z9-2*z3*z7-4*z4S-4*z4* z10+3*z4*z8+2*z4*z6+z10*z5-z9*z6+3*z8*z7+4*z7*z6)+8*(z1S *z9-z1S*z8-z1*z2*z7+z1*z2*z6+z1*z3*z9+z1*z3*z5+z1*z4* z9-z1*z4*z8-z1*z4*z5+z1*z10*z9+z1*z9*z6-z1*z8*z7-z2*z3*z7 -z2*z4*z7+z2*z4*z6-z2*z10*z7+z3*z7*z5-z4S*z5-z4*z10*z5- z4*z6*z5); fm[2][7] = 8*mQ4*(z3+2*z4+3*z10+z7+2*z6)+4*mQ2*(-4*z1*z3- 2*z1*z4-2*z1*z10+z1*z9-z1*z8-4*z1*z7-2*z1*z6+z2*z3+2*z2* z4+3*z2*z10+z2*z7+2*z2*z6-6*z3*z4-6*z3*z10-2*z3*z9-2*z3* z7-4*z3*z6-z3*z5-6*z4S-6*z4*z10-3*z4*z9-z4*z8-4*z4*z7-2 *z4*z6-2*z4*z5-3*z10*z9-3*z10*z8-6*z10*z7-6*z10*z6+z10*z5 +z9*z7-2*z8*z7-2*z8*z6-6*z7*z6+z7*z5-6*z6S+2*z6*z5)+4*( -z1S*z9+z1S*z8-2*z1*z2*z10-3*z1*z2*z7-3*z1*z2*z6+z1* z3*z9-z1*z3*z5+z1*z4*z9+z1*z4*z8+z1*z4*z5+z1*z10*z9+z1* z10*z8-z1*z9*z6+z1*z8*z6+z2*z3*z7-3*z2*z4*z7-z2*z4*z6-3* z2*z10*z7-3*z2*z10*z6-3*z2*z7*z6-3*z2*z6S-2*z3*z4*z5-z3 *z10*z5-z3*z6*z5-z4S*z5-z4*z10*z5+z4*z6*z5); fm[2][8] = 8*mQ4*(z3+2*z4+3*z10+z7+2*z6)+4*mQ2*(-4*z1*z3- 2*z1*z4-2*z1*z10-z1*z9+z1*z8-4*z1*z7-2*z1*z6+z2*z3+2*z2* z4+z2*z10-z2*z7-2*z2*z6-6*z3*z4-6*z3*z10-2*z3*z9+z3*z8-2* z3*z7-4*z3*z6+z3*z5-6*z4S-6*z4*z10-2*z4*z9-4*z4*z7-2*z4 *z6+2*z4*z5-3*z10*z9-3*z10*z8-6*z10*z7-6*z10*z6+3*z10*z5- z9*z6-2*z8*z7-3*z8*z6-6*z7*z6+z7*z5-6*z6S+2*z6*z5)+4*( z1S*z9-z1S*z8-z1*z2*z7+z1*z2*z6-3*z1*z3*z5+z1*z4*z9- z1*z4*z8-3*z1*z4*z5+z1*z10*z9+z1*z10*z8-2*z1*z10*z5+z1*z9 *z6+z1*z8*z7+z1*z8*z6-z2*z4*z7+z2*z4*z6-z2*z10*z7-z2*z10* z6-2*z2*z7*z6-z2*z6S-3*z3*z4*z5-3*z3*z10*z5+z3*z7*z5-3* z3*z6*z5-3*z4S*z5-3*z4*z10*z5-z4*z6*z5); fm[3][3] = 64*mQ6+16*mQ4*s3+32*mQ4*(z1+z2+2*z3+z8+z6 +2*z5)+8*mQ2*s3*(-z1+2*z3-z6)+16*mQ2*(z2*z5-2*z3* z8-2*z3*z6+4*z3*z5+z8*z5)+8*s3*z3*z6-16*z3*z8*z5; fm[3][4] = 16*mQ4*(-4*z1-z3+z8-z6)+4*mQ2*s3*(-2*z1-z3- z6)+16*mQ2*(-2*z1S-3*z1*z2-2*z1*z3-3*z1*z8-2*z1*z6-3* z1*z5-2*z2*z3-2*z6*z5)-8*s3*z3*z6+8*(-z1*z2*z8-2*z1*z2 *z5-z1*z8S-z1*z8*z5+z2S*z6-z2*z3*z5+z2*z8*z6-z2*z6*z5 +z3*z8*z5+z3*z5S); fm[3][5] = 8*mQ4*(-2*z1+z10-z8-2*z6)+4*mQ2*(4*z1S+2*z1* z2+4*z1*z3+4*z1*z4+6*z1*z10+4*z1*z9-2*z1*z8+8*z1*z7-2*z1* z5+4*z2*z3+3*z2*z10+2*z2*z6-4*z3S-4*z3*z10+3*z3*z9+2*z3 *z7-3*z4*z8-2*z4*z6+z10*z5+3*z9*z6-z8*z7+4*z7*z6)+8*(-z1S *z9+z1S*z8+z1*z2*z7-z1*z2*z6-z1*z3*z9+z1*z3*z8-z1*z3 *z5+z1*z4*z8+z1*z4*z5+z1*z10*z8-z1*z9*z6+z1*z8*z7+z2*z3* z7-z2*z3*z6-z2*z4*z6-z2*z10*z6-z3S*z5-z3*z10*z5-z3*z7* z5+z4*z6*z5); fm[3][6] = 16*mQ6+4*mQ4*s3+16*mQ4*(-z1-z2+2*z3+2*z4+ z10-z9-z8-z7-z6+z5)+4*mQ2*s3*(z1+2*z3+2*z4+z10+z7+z6 )+8*mQ2*(4*z1*z3+4*z1*z4+4*z1*z10+4*z2*z3+4*z2*z4+4*z2* z10-z2*z5+4*z3*z5+4*z4*z5+2*z10*z5-z9*z5-z8*z5)-(8*s3* z1)*(z3+z4+z10)+16*z2*z5*(z3+z4+z10); fm[3][7] = 8*mQ4*(3*z3+6*z4+3*z10+z9+2*z8+2*z7+z6)+2*mQ2* s3*(z3+2*z4+2*z10-2*z7-z6)+4*mQ2*(4*z1*z3+8*z1*z4+4* z1*z10+2*z1*z9-2*z1*z8+2*z2*z3+10*z2*z4+5*z2*z10+2*z2*z9+ z2*z8+2*z2*z7+4*z2*z6-7*z3*z9+2*z3*z8-8*z3*z7+4*z3*z6+4* z3*z5+5*z4*z8+4*z4*z6+8*z4*z5+5*z10*z5-z9*z8-z9*z6+z9*z5+ z8S-z8*z7+2*z8*z6+2*z8*z5)+2*s3*(-z1*z10+z3*z7-2*z3* z6+z4*z6)+4*(-z1*z2*z9-2*z1*z2*z8+z1*z9*z8-z1*z8S+z2S *z7+2*z2S*z6+3*z2*z4*z5+2*z2*z10*z5-2*z2*z9*z6+z2*z8*z7 +z2*z8*z6-2*z3*z9*z5+z3*z8*z5+z4*z8*z5); fm[3][8] = 8*mQ4*(3*z3+6*z4+3*z10+2*z9+z8+2*z7+z6)+2*mQ2* s3*(3*z3+6*z4+3*z10-2*z7-z6)+4*mQ2*(4*z1*z3+8*z1*z4+ 4*z1*z10+4*z2*z3+8*z2*z4+4*z2*z10-8*z3*z9+4*z3*z8-8*z3*z7 +4*z3*z6+6*z3*z5+4*z4*z8+4*z4*z6+12*z4*z5+6*z10*z5+2*z9* z5+z8*z5)+4*s3*(-z1*z3-2*z1*z4-z1*z10+2*z3*z7-z3*z6-z4 *z6)+8*z5*(z2*z3+2*z2*z4+z2*z10-2*z3*z9+z3*z8+z4*z8); fm[4][4] = 64*mQ6+16*mQ4*s3+32*mQ4*(z1+2*z2+z3+z8+2* z6+z5)+8*mQ2*s3*(-z1-z3+2*z6)+16*mQ2*(z2*z8+4*z2* z6+z2*z5-2*z3*z6-2*z8*z6)+8*s3*z3*z6-16*z2*z8*z6; fm[4][5] = 16*mQ6+8*mQ4*(-2*z1+z2-2*z3-2*z4-4*z10-z9+z8-4 *z7+2*z6+z5)+8*mQ2*(-2*z1*z2-2*z2*z3-2*z2*z10-2*z2*z7+ z2*z6+2*z3*z6-2*z4*z6+4*z10*z6-z9*z6-z8*z6)+16*z2*z6*(z3+ z10); fm[4][6] = 16*mQ6-4*mQ4*s3+8*mQ4*(-2*z1+2*z2-4*z3-2* z4-8*z10+z9+z8-4*z7-2*z6+2*z5)-(4*mQ2*s3)*(z1+z3+z10 +z7)+8*mQ2*(-2*z1*z2-2*z1*z10+z1*z9+z1*z8-2*z1*z5+z2S -4*z2*z3-5*z2*z10+z2*z9-3*z2*z7-z2*z6+z2*z5+z3*z9+2*z3*z7 -3*z3*z5+z4*z8+2*z4*z6-z4*z5-5*z10*z5+z9*z8+z9*z6+z8*z7+ z8*z5-4*z7*z5+z5S)-(16*z2*z5)*(z1+z3+z10+z7); fm[4][7] = 8*mQ4*(-z3-2*z4-3*z10-2*z9-z8-6*z7-3*z6)+2*mQ2 *s3*(z3+2*z4-3*z10-6*z7-3*z6)+4*mQ2*(-4*z1*z10-8*z1* z7-4*z1*z6-6*z2*z10-2*z2*z9-z2*z8-12*z2*z7-6*z2*z6-4*z3* z7-4*z3*z6+8*z4*z6-4*z10*z5+8*z9*z6-4*z8*z7-4*z8*z6-8*z7* z5-4*z6*z5)+4*s3*(z1*z10+2*z1*z7+z1*z6+z3*z7+z3*z6-2* z4*z6)+8*z2*(-z10*z5+2*z9*z6-z8*z7-z8*z6-2*z7*z5-z6*z5); fm[4][8] = 8*mQ4*(-z3-2*z4-3*z10-z9-2*z8-6*z7-3*z6)+2*mQ2 *s3*(z3+2*z4-2*z10-2*z7-z6)+4*mQ2*(-4*z1*z10-2*z1*z9 +2*z1*z8-8*z1*z7-4*z1*z6-5*z2*z10-z2*z9-2*z2*z8-8*z2*z7-4 *z2*z6+z3*z9-2*z3*z8-4*z3*z7-4*z3*z6-4*z3*z5+z4*z8+8*z4* z6-2*z4*z5-5*z10*z5+z9*z8+7*z9*z6-2*z9*z5-z8S-5*z8*z7-2 *z8*z6-z8*z5-10*z7*z5-2*z6*z5)+2*s3*(z1*z10-z3*z7+2*z3 *z6-z4*z6)+4*(-z1*z9*z8+z1*z9*z5+z1*z8S+2*z1*z8*z5-2*z2 *z10*z5+2*z2*z9*z6-z2*z8*z7-z2*z8*z6-3*z2*z7*z5+2*z3*z9* z5-z3*z8*z5-2*z3*z5S-z4*z8*z5-z4*z5S); fm[5][5] = 16*mQ6+16*mQ4*(-z1-z3+z4-z10-z7+z6)+16*mQ2*( z3*z6+z4*z10+z4*z7+z4*z6+z10*z6)-16*z4*z10*z6; fm[5][6] = 16*mQ6+8*mQ4*(-2*z1+z2-4*z3+2*z4-4*z10+z9-z8-2 *z7-2*z6+z5)+8*mQ2*(-2*z1*z5-2*z3*z5+4*z4*z10-z4*z9-z4* z8+2*z4*z7-2*z4*z6+z4*z5-2*z10*z5-2*z7*z5)+16*z4*z5*(z10+ z7); fm[5][7] = 8*mQ4*(-2*z3-z4-3*z10-2*z7-z6)+4*mQ2*(2*z1*z3+ 4*z1*z4+2*z1*z10+z1*z9-z1*z8+2*z1*z7+4*z1*z6-2*z2*z3-z2* z4-3*z2*z10-2*z2*z7-z2*z6+6*z3S+6*z3*z4+6*z3*z10+z3*z9+ 3*z3*z8+2*z3*z7+4*z3*z6+2*z3*z5+6*z4*z10+2*z4*z8+4*z4*z7+ 2*z4*z6+z4*z5+3*z10*z9+3*z10*z8+6*z10*z7+6*z10*z6-z10*z5+ 2*z9*z7+2*z9*z6-z8*z6+6*z7S+6*z7*z6-2*z7*z5-z6*z5)+4*(- z1S*z9+z1S*z8+2*z1*z2*z10+3*z1*z2*z7+3*z1*z2*z6-z1*z3 *z9-z1*z3*z8-z1*z3*z5-z1*z4*z8+z1*z4*z5-z1*z10*z9-z1*z10* z8-z1*z9*z7+z1*z8*z7+z2*z3*z7+3*z2*z3*z6-z2*z4*z6+3*z2* z10*z7+3*z2*z10*z6+3*z2*z7S+3*z2*z7*z6+z3S*z5+2*z3*z4 *z5+z3*z10*z5-z3*z7*z5+z4*z10*z5+z4*z7*z5); fm[5][8] = 8*mQ4*(-2*z3-z4-3*z10-2*z7-z6)+4*mQ2*(2*z1*z3+ 4*z1*z4+2*z1*z10-z1*z9+z1*z8+2*z1*z7+4*z1*z6-2*z2*z3-z2* z4-z2*z10+2*z2*z7+z2*z6+6*z3S+6*z3*z4+6*z3*z10+2*z3*z8+ 2*z3*z7+4*z3*z6-2*z3*z5+6*z4*z10-z4*z9+2*z4*z8+4*z4*z7+2* z4*z6-z4*z5+3*z10*z9+3*z10*z8+6*z10*z7+6*z10*z6-3*z10*z5+ 3*z9*z7+2*z9*z6+z8*z7+6*z7S+6*z7*z6-2*z7*z5-z6*z5)+4*( z1S*z9-z1S*z8-z1*z2*z7+z1*z2*z6+z1*z3*z9-z1*z3*z8+3* z1*z3*z5+3*z1*z4*z5-z1*z10*z9-z1*z10*z8+2*z1*z10*z5-z1*z9 *z7-z1*z9*z6-z1*z8*z7-z2*z3*z7+z2*z3*z6+z2*z10*z7+z2*z10* z6+z2*z7S+2*z2*z7*z6+3*z3S*z5+3*z3*z4*z5+3*z3*z10*z5+ z3*z7*z5+3*z4*z10*z5+3*z4*z7*z5-z4*z6*z5); fm[6][6] = 64*mQ6+16*mQ4*s3+32*mQ4*(z1+z2+2*z4+z9+z7 +2*z5)+8*mQ2*s3*(-z1+2*z4-z7)+16*mQ2*(z2*z5-2*z4* z9-2*z4*z7+4*z4*z5+z9*z5)+8*s3*z4*z7-16*z4*z9*z5; fm[6][7] = 8*mQ4*(-6*z3-3*z4-3*z10-2*z9-z8-z7-2*z6)+2*mQ2 *s3*(-2*z3-z4-2*z10+z7+2*z6)+4*mQ2*(-8*z1*z3-4*z1*z4 -4*z1*z10+2*z1*z9-2*z1*z8-10*z2*z3-2*z2*z4-5*z2*z10-z2*z9 -2*z2*z8-4*z2*z7-2*z2*z6-5*z3*z9-4*z3*z7-8*z3*z5-2*z4*z9+ 7*z4*z8-4*z4*z7+8*z4*z6-4*z4*z5-5*z10*z5-z9S+z9*z8-2*z9 *z7+z9*z6-2*z9*z5+z8*z7-z8*z5)+2*s3*(z1*z10-z3*z7+2*z4 *z7-z4*z6)+4*(2*z1*z2*z9+z1*z2*z8+z1*z9S-z1*z9*z8-2* z2S*z7-z2S*z6-3*z2*z3*z5-2*z2*z10*z5-z2*z9*z7-z2*z9*z6+ 2*z2*z8*z7-z3*z9*z5-z4*z9*z5+2*z4*z8*z5); fm[6][8] = 8*mQ4*(-6*z3-3*z4-3*z10-z9-2*z8-z7-2*z6)+2*mQ2 *s3*(-6*z3-3*z4-3*z10+z7+2*z6)+4*mQ2*(-8*z1*z3-4*z1* z4-4*z1*z10-8*z2*z3-4*z2*z4-4*z2*z10-4*z3*z9-4*z3*z7-12* z3*z5-4*z4*z9+8*z4*z8-4*z4*z7+8*z4*z6-6*z4*z5-6*z10*z5-z9 *z5-2*z8*z5)+4*s3*(2*z1*z3+z1*z4+z1*z10+z3*z7+z4*z7-2* z4*z6)+8*z5*(-2*z2*z3-z2*z4-z2*z10-z3*z9-z4*z9+2*z4*z8); fm[7][7] = 72*mQ4*z10+18*mQ2*s3*z10+8*mQ2*(z1*z10+9* z2*z10+7*z3*z7+2*z3*z6+2*z4*z7+7*z4*z6+z10*z5+2*z9*z7+7* z9*z6+7*z8*z7+2*z8*z6)+2*s3*(-z1*z10-7*z3*z7-2*z3*z6-2 *z4*z7-7*z4*z6)+4*z2*(z10*z5+2*z9*z7+7*z9*z6+7*z8*z7+2*z8 *z6); fm[7][8] = 72*mQ4*z10+2*mQ2*s3*z10+4*mQ2*(2*z1*z10+ 10*z2*z10+7*z3*z9+2*z3*z8+14*z3*z7+4*z3*z6+2*z4*z9+7*z4* z8+4*z4*z7+14*z4*z6+10*z10*z5+z9S+7*z9*z8+2*z9*z7+7*z9* z6+z8S+7*z8*z7+2*z8*z6)+2*s3*(7*z1*z10-7*z3*z7-2*z3* z6-2*z4*z7-7*z4*z6)+2*(-2*z1*z9S-14*z1*z9*z8-2*z1*z8S +2*z2*z10*z5+2*z2*z9*z7+7*z2*z9*z6+7*z2*z8*z7+2*z2*z8*z6+ 7*z3*z9*z5+2*z3*z8*z5+2*z4*z9*z5+7*z4*z8*z5); fm[8][8] = 72*mQ4*z10+18*mQ2*s3*z10+8*mQ2*(z1*z10+z2 *z10+7*z3*z9+2*z3*z8+7*z3*z7+2*z3*z6+2*z4*z9+7*z4*z8+2*z4 *z7+7*z4*z6+9*z10*z5)+2*s3*(-z1*z10-7*z3*z7-2*z3*z6-2* z4*z7-7*z4*z6)+4*z5*(z2*z10+7*z3*z9+2*z3*z8+2*z4*z9+7*z4* z8); double fm99 = -4*mQ4*z10-mQ2*s3*z10+4*mQ2*(-z1*z10-z2*z10+ z3*z7+z4*z6-z10*z5+z9*z6+z8*z7)+s3*(z1*z10-z3*z7-z4*z6 )+2*z2*(-z10*z5+z9*z6+z8*z7); double fm910 = -4*mQ4*z10-mQ2*s3*z10+2*mQ2*(-2*z1*z10-2*z2* z10+2*z3*z9+2*z3*z7+2*z4*z6-2*z10*z5+z9*z8+2*z8*z7)+s3 *(z1*z10-z3*z7-z4*z6)+2*(-z1*z9*z8-z2*z10*z5+z2*z8*z7+z3* z9*z5); double fmxx = -4*mQ4*z10-mQ2*s3*z10+2*mQ2*(-2*z1*z10-2*z2* z10+2*z4*z8+2*z4*z6+2*z3*z7-2*z10*z5+z9*z8+2*z9*z6)+s3 *(z1*z10-z3*z7-z4*z6)+2*(-z1*z9*z8-z2*z10*z5+z2*z9*z6+z4* z8*z5); fm910 = 0.5*(fmxx+fm910); double fm1010 = -4*mQ4*z10-mQ2*s3*z10+4*mQ2*(-z1*z10-z2*z10+ z3*z7+z4*z6-z10*z5+z9*z3+z8*z4)+s3*(z1*z10-z3*z7-z4*z6 )+2*z5*(-z10*z2+z9*z3+z8*z4); fm[7][7] -= 2. * fm99; fm[7][8] -= 2. * fm910; fm[8][8] -= 2. * fm1010; // Propagators. double ss1 = (pTemp[1] + pTemp[3]).m2Calc() - mQ2; double ss2 = (pTemp[1] + pTemp[4]).m2Calc() - mQ2; double ss3 = (pTemp[1] + pTemp[5]).m2Calc() - mQ2; double ss4 = (pTemp[2] + pTemp[3]).m2Calc() - mQ2; double ss5 = (pTemp[2] + pTemp[4]).m2Calc() - mQ2; double ss6 = (pTemp[2] + pTemp[5]).m2Calc() - mQ2; double ss7 = sH; // Propagator combinations. double dz[9]; dz[1] = ss1 * ss6; dz[2] = ss2 * ss6; dz[3] = ss2 * ss4; dz[4] = ss1 * ss5; dz[5] = ss3 * ss5; dz[6] = ss3 * ss4; dz[7] = ss7 * ss1; dz[8] = ss7 * ss4; // Colour factors. double clr[9][9]; for (int i = 1; i < 4; ++i) for (int j = 1; j < 4; ++j) { clr[i][j] = 16. / 3.; clr[i][j+3] = -2. / 3.; clr[i+3][j] = -2. / 3.; clr[i+3][j+3] = 16. / 3.; } for (int i = 1; i < 4; ++i) for (int j = 1; j < 3; ++j) { clr[i][j+6] = -6.; clr[i+3][j+6] = 6.; clr[j+6][i] = -6.; clr[j+6][i+3] = 6.; } for (int i = 1; i < 3; ++i) for (int j = 1; j < 3; ++j) clr[i+6][j+6] = 12.; // Produce final result: matrix elements * colours * propagators. double wtSum = 0.; for (int i = 1; i < 9; ++i) for (int j = i; j < 9; ++j) { double fac = (j == i) ? 4. : 8.; wtSum += fm[i][j] * fac * clr[i][j] / (dz[i] * dz[j]); } wtSum *= -1./256.; // Combine factors. sigma = prefac * alpEM * pow2(alpS) * mQ2run * wtSum *pow2(coup2Q); // Secondary width for H, Q and Qbar (latter for top only). // (H can be H0 SM or H1, H2, A3 from BSM). sigma *= openFracTriplet; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3gg2HQQbar::setIdColAcol() { // Pick out-flavours by relative CKM weights. setId( id1, id2, idRes, idNew, -idNew); // Colour flow topologies. if (rndmPtr->flat() < 0.5) setColAcol( 1, 2, 2, 3, 0, 0, 1, 0, 0, 3); else setColAcol( 1, 2, 3, 1, 0, 0, 3, 0, 0, 2); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma3gg2HQQbar::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma3qqbar2HQQbar class. // Cross section for q qbar -> H0 Q Qbar (Q Qbar fusion of SM Higgs). // REDUCE output and part of the rest courtesy Z. Kunszt, // see Z. Kunszt, Nucl. Phys. B247 (1984) 339. //-------------------------------------------------------------------------- // Initialize process. void Sigma3qqbar2HQQbar::initProc() { // Properties specific to Higgs state for the "q qbar -> H ttbar" process. // (H can be H0 SM or H1, H2, A3 from BSM). if (higgsType == 0 && idNew == 6) { nameSave = "q qbar -> H t tbar (SM)"; codeSave = 909; idRes = 25; coup2Q = 1.; } else if (higgsType == 1 && idNew == 6) { nameSave = "q qbar -> h0(H1) t tbar"; codeSave = 1009; idRes = 25; coup2Q = settingsPtr->parm("HiggsH1:coup2u"); } else if (higgsType == 2 && idNew == 6) { nameSave = "q qbar -> H0(H2) t tbar"; codeSave = 1029; idRes = 35; coup2Q = settingsPtr->parm("HiggsH2:coup2u"); } else if (higgsType == 3 && idNew == 6) { nameSave = "q qbar -> A0(A3) t tbar"; codeSave = 1049; idRes = 36; coup2Q = settingsPtr->parm("HiggsA3:coup2u"); } // Properties specific to Higgs state for the "q qbar -> H b bbar" process. // (H can be H0 SM or H1, H2, A3 from BSM). if (higgsType == 0 && idNew == 5) { nameSave = "q qbar -> H b bbar (SM)"; codeSave = 913; idRes = 25; coup2Q = 1.; } else if (higgsType == 1 && idNew == 5) { nameSave = "q qbar -> h0(H1) b bbar"; codeSave = 1013; idRes = 25; coup2Q = settingsPtr->parm("HiggsH1:coup2d"); } else if (higgsType == 2 && idNew == 5) { nameSave = "q qbar -> H0(H2) b bbar"; codeSave = 1033; idRes = 35; coup2Q = settingsPtr->parm("HiggsH2:coup2d"); } else if (higgsType == 3 && idNew == 5) { nameSave = "q qbar -> A0(A3) b bbar"; codeSave = 1053; idRes = 36; coup2Q = settingsPtr->parm("HiggsA3:coup2d"); } // Common mass and coupling factors. double mWS = pow2(particleDataPtr->m0(24)); prefac = (4. * M_PI / couplingsPtr->sin2thetaW()) * pow2(4. * M_PI) * 0.25 / mWS; // Secondary open width fraction. openFracTriplet = particleDataPtr->resOpenFrac(idRes, idNew, -idNew); } //-------------------------------------------------------------------------- // Evaluate sigma(sHat), part independent of incoming flavour. void Sigma3qqbar2HQQbar::sigmaKin() { // Running mass of heavy quark. double mQ2run = pow2( particleDataPtr->mRun(idNew, mH) ); // Linear combination of p_Q and p_Qbar to ensure common mass. double mQ2 = m4 * m5; double epsi = 0.; if (m4 != m5) { double s45 = (p4cm + p5cm).m2Calc(); mQ2 = 0.5 * (s4 + s5) - 0.25 * pow2(s4 - s5) / s45; epsi = 0.5 * (s5 - s4) / s45; } // Set up kinematics: q(4) qbar(5) -> H(3) Q(1) Qbar(2) in outgoing sense. Vec4 pTemp[6]; pTemp[4] = Vec4( 0., 0., -0.5* mH, -0.5* mH); pTemp[5] = Vec4( 0., 0., 0.5* mH, -0.5* mH); pTemp[1] = p4cm + epsi * (p4cm + p5cm); pTemp[2] = p5cm - epsi * (p4cm + p5cm); pTemp[3] = p3cm; // Four-product combinations. double z1 = pTemp[1] * pTemp[2]; double z2 = pTemp[1] * pTemp[3]; double z3 = pTemp[1] * pTemp[4]; double z4 = pTemp[1] * pTemp[5]; double z5 = pTemp[2] * pTemp[3]; double z6 = pTemp[2] * pTemp[4]; double z7 = pTemp[2] * pTemp[5]; double z8 = pTemp[3] * pTemp[4]; double z9 = pTemp[3] * pTemp[5]; double z10 = pTemp[4] * pTemp[5]; // Powers required as shorthand in matriz elements. double mQ4 = mQ2 * mQ2; // Evaluate matrix elements for q + qbar -> Q + Qbar + H. // (H can be H0 SM or H1, H2, A3 from BSM). double a11 = -8.*mQ4*z10-2.*mQ2*s3*z10-(8.*mQ2)*(z2*z10+z3 *z7+z4*z6+z9*z6+z8*z7)+2.*s3*(z3*z7+z4*z6)-(4.*z2)*(z9 *z6+z8*z7); double a12 = -8.*mQ4*z10+4.*mQ2*(-z2*z10-z3*z9-2.*z3*z7-z4*z8- 2.*z4*z6-z10*z5-z9*z8-z9*z6-z8*z7)+2.*s3*(-z1*z10+z3*z7 +z4*z6)+2.*(2.*z1*z9*z8-z2*z9*z6-z2*z8*z7-z3*z9*z5-z4*z8* z5); double a22 = -8.*mQ4*z10-2.*mQ2*s3*z10-(8.*mQ2)*(z3*z9+z3* z7+z4*z8+z4*z6+z10*z5)+2.*s3*(z3*z7+z4*z6)-(4.*z5)*(z3 *z9+z4*z8); // Propagators and propagator combinations. double ss1 = (pTemp[1] + pTemp[3]).m2Calc() - mQ2; double ss4 = (pTemp[2] + pTemp[3]).m2Calc() - mQ2; double ss7 = sH; double dz7 = ss7 * ss1; double dz8 = ss7 * ss4; // Produce final result: matrix elements * propagators. a11 /= (dz7 * dz7); a12 /= (dz7 * dz8); a22 /= (dz8 * dz8); double wtSum = -(a11 + a22 + 2.*a12) * (8./9.); // Combine factors. sigma = prefac * alpEM * pow2(alpS) * mQ2run * wtSum * pow2(coup2Q); // Secondary width for H, Q and Qbar (latter for top only). // (H can be H0 SM or H1, H2, A3 from BSM). sigma *= openFracTriplet; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3qqbar2HQQbar::setIdColAcol() { // Pick out-flavours by relative CKM weights. setId( id1, id2, idRes, idNew, -idNew); // Colour flow topologies. if (id1 > 0) setColAcol( 1, 0, 0, 2, 0, 0, 1, 0, 0, 2); else setColAcol( 0, 1, 2, 0, 0, 0, 2, 0, 0, 1); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma3qqbar2HQQbar::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma2qg2Hq class. // Cross section for q g -> H q. // (H can be H0 SM or H1, H2, A3 from BSM). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2Hq::initProc() { // Properties specific to Higgs state for the "c g -> H c" process. // (H can be H0 SM or H1, H2, A3 from BSM). if (higgsType == 0 && idNew == 4) { nameSave = "c g -> H c (SM)"; codeSave = 911; idRes = 25; } else if (higgsType == 1 && idNew == 4) { nameSave = "c g -> h0(H1) c"; codeSave = 1011; idRes = 25; } else if (higgsType == 2 && idNew == 4) { nameSave = "c g -> H0(H2) c"; codeSave = 1031; idRes = 35; } else if (higgsType == 3 && idNew == 4) { nameSave = "c g -> A0(A3) c"; codeSave = 1051; idRes = 36; } // Properties specific to Higgs state for the "b g -> H b" process. // (H can be H0 SM or H1, H2, A3 from BSM). if (higgsType == 0 && idNew == 5) { nameSave = "b g -> H b (SM)"; codeSave = 911; idRes = 25; } else if (higgsType == 1 && idNew == 5) { nameSave = "b g -> h0(H1) b"; codeSave = 1011; idRes = 25; } else if (higgsType == 2 && idNew == 5) { nameSave = "b g -> H0(H2) b"; codeSave = 1031; idRes = 35; } else if (higgsType == 3 && idNew == 5) { nameSave = "b g -> A0(A3) b"; codeSave = 1051; idRes = 36; } // Standard parameters. m2W = pow2( particleDataPtr->m0(24) ); thetaWRat = 1. / (24. * couplingsPtr->sin2thetaW()); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(idRes); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2qg2Hq::sigmaKin() { // Running mass provides coupling. double m2Run = pow2( particleDataPtr->mRun(idNew, mH) ); // Cross section, including couplings and kinematics. sigma = (M_PI / sH2) * alpS * alpEM * thetaWRat * (m2Run/m2W) * (sH / (s4 - uH) + 2. * s4 * (s3 - uH) / pow2(s4 - uH) + (s4 - uH) / sH - 2. * s4 / (s4 - uH) + 2. * (s3 - uH) * (s3 - s4 - sH) / ((s4 - uH) * sH) ); // Include secondary width for H0, H1, H2 or A3. Done. sigma *= openFrac; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma2qg2Hq::sigmaHat() { // Check that specified flavour present. if (abs(id1) != idNew && abs(id2) != idNew) return 0.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2Hq::setIdColAcol() { // Flavour set up for q g -> H0 q. int idq = (id2 == 21) ? id1 : id2; setId( id1, id2, idRes, idq); // tH defined between f and f': must swap tHat <-> uHat if q g in. swapTU = (id2 == 21); // Colour flow topologies. Swap when antiquarks. if (id2 == 21) setColAcol( 1, 0, 2, 1, 0, 0, 2, 0); else setColAcol( 2, 1, 1, 0, 0, 0, 2, 0); if (idq < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma2qg2Hq::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma2gg2Hglt class. // Cross section for g g -> H g (H SM Higgs or BSM Higgs) via top loop. // (H can be H0 SM or H1, H2, A3 from BSM). //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2Hglt::initProc() { // Properties specific to Higgs state. if (higgsType == 0) { nameSave = "g g -> H g (SM; top loop)"; codeSave = 914; idRes = 25; } else if (higgsType == 1) { nameSave = "g g -> h0(H1) g (BSM; top loop)"; codeSave = 1014; idRes = 25; } else if (higgsType == 2) { nameSave = "g g -> H0(H2) g (BSM; top loop)"; codeSave = 1034; idRes = 35; } else if (higgsType == 3) { nameSave = "g g -> A0(A3) g (BSM; top loop)"; codeSave = 1054; idRes = 36; } // Normalization factor by g g -> H partial width. // (H can be H0 SM or H1, H2, A3 from BSM). double mHiggs = particleDataPtr->m0(idRes); widHgg = particleDataPtr->resWidthChan(idRes, mHiggs, 21, 21); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(idRes); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2gg2Hglt::sigmaKin() { // Evaluate cross section. Secondary width for H0, H1, H2 or A3. sigma = (M_PI / sH2) * (3. / 16.) * alpS * (widHgg / m3) * (sH2 * sH2 + tH2 * tH2 + uH2 * uH2 + pow4(s3)) / (sH * tH * uH * s3); sigma *= openFrac; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2Hglt::setIdColAcol() { // Flavour set up for g g -> H g trivial. // (H can be H0 SM or H1, H2, A3 from BSM). setId( 21, 21, idRes, 21); // Colour flow topologies: random choice between two mirrors. if (rndmPtr->flat() < 0.5) setColAcol( 1, 2, 2, 3, 0, 0, 1, 3); else setColAcol( 1, 2, 3, 1, 0, 0, 3, 2); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma2gg2Hglt::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma2qg2Hqlt class. // Cross section for q g -> H q (H SM or BSM Higgs) via top loop. // (H can be H0 SM or H1, H2, A3 from BSM). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2Hqlt::initProc() { // Properties specific to Higgs state. if (higgsType == 0) { nameSave = "q g -> H q (SM; top loop)"; codeSave = 915; idRes = 25; } else if (higgsType == 1) { nameSave = "q g -> h0(H1) q (BSM; top loop)"; codeSave = 1015; idRes = 25; } else if (higgsType == 2) { nameSave = "q g -> H0(H2) q (BSM; top loop)"; codeSave = 1035; idRes = 35; } else if (higgsType == 3) { nameSave = "q g -> A0(A3) q (BSM; top loop)"; codeSave = 1055; idRes = 36; } // Normalization factor by g g -> H partial width. // (H can be H0 SM or H1, H2, A3 from BSM). double mHiggs = particleDataPtr->m0(idRes); widHgg = particleDataPtr->resWidthChan(idRes, mHiggs, 21, 21); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(idRes); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat, part independent of incoming flavour). void Sigma2qg2Hqlt::sigmaKin() { // Evaluate cross section. Secondary width for H0, H1, H2 or A3. sigma = (M_PI / sH2) * (1. / 12.) * alpS * (widHgg / m3) * (sH2 + uH2) / (-tH * s3); sigma *= openFrac; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2Hqlt::setIdColAcol() { // Flavour set up for q g -> H q. // (H can be H0 SM or H1, H2, A3 from BSM). int idq = (id2 == 21) ? id1 : id2; setId( id1, id2, idRes, idq); // tH defined between f and f': must swap tHat <-> uHat if q g in. swapTU = (id2 == 21); // Colour flow topologies. Swap when antiquarks. if (id2 == 21) setColAcol( 1, 0, 2, 1, 0, 0, 2, 0); else setColAcol( 2, 1, 1, 0, 0, 0, 2, 0); if (idq < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma2qg2Hqlt::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma2qqbar2Hglt class. // Cross section for q qbar -> H g (H SM or BSM Higgs) via top loop. // (H can be H0 SM or H1, H2, A3 from BSM). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2Hglt::initProc() { // Properties specific to Higgs state. if (higgsType == 0) { nameSave = "q qbar -> H g (SM; top loop)"; codeSave = 916; idRes = 25; } else if (higgsType == 1) { nameSave = "q qbar -> h0(H1) g (BSM; top loop)"; codeSave = 1016; idRes = 25; } else if (higgsType == 2) { nameSave = "q qbar -> H0(H2) g (BSM; top loop)"; codeSave = 1036; idRes = 35; } else if (higgsType == 3) { nameSave = "q qbar -> A0(A3) g (BSM; top loop)"; codeSave = 1056; idRes = 36; } // Normalization factor by g g -> H partial width. // (H can be H0 SM or H1, H2, A3 from BSM). double mHiggs = particleDataPtr->m0(idRes); widHgg = particleDataPtr->resWidthChan(idRes, mHiggs, 21, 21); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(idRes); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2qqbar2Hglt::sigmaKin() { // Evaluate cross section. Secondary width for H0, H1, H2 or A3. sigma = (M_PI / sH2) * (2. / 9.) * alpS * (widHgg / m3) * (tH2 + uH2) / (sH * s3); sigma *= openFrac; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2Hglt::setIdColAcol() { // Flavours trivial. setId( id1, id2, idRes, 21); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 0, 0, 1, 2); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma2qqbar2Hglt::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma1ffbar2Hchg class. // Cross section for f fbar -> H+- (f is quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2Hchg::initProc() { // Find pointer to H+-. HResPtr = particleDataPtr->particleDataEntryPtr(37); // Store H+- mass and width for propagator. mRes = HResPtr->m0(); GammaRes = HResPtr->mWidth(); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Couplings. m2W = pow2(particleDataPtr->m0(24)); thetaWRat = 1. / (8. * couplingsPtr->sin2thetaW()); tan2Beta = pow2(settingsPtr->parm("HiggsHchg:tanBeta")); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma1ffbar2Hchg::sigmaKin() { // Set up Breit-Wigner. Width out only includes open channels. sigBW = 4. * M_PI / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); widthOutPos = HResPtr->resWidthOpen( 37, mH); widthOutNeg = HResPtr->resWidthOpen(-37, mH); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma1ffbar2Hchg::sigmaHat() { // Only allow generation-diagonal states. int id1Abs = abs(id1); int id2Abs = abs(id2); int idUp = max(id1Abs, id2Abs); int idDn = min(id1Abs, id2Abs); if (idUp%2 != 0 || idUp - idDn != 1) return 0.; // Calculate mass-dependent incoming width. Total cross section. double m2RunUp = pow2(particleDataPtr->mRun(idUp, mH)); double m2RunDn = pow2(particleDataPtr->mRun(idDn, mH)); double widthIn = alpEM * thetaWRat * (mH/m2W) * (m2RunDn * tan2Beta + m2RunUp / tan2Beta); int idUpChg = (id1Abs%2 == 0) ? id1 : id2; double sigma = (idUpChg > 0) ? widthIn * sigBW * widthOutPos : widthIn * sigBW * widthOutNeg; // Colour factor. Answer. if (idUp < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2Hchg::setIdColAcol() { // Charge of Higgs. Fill flavours. int idUpChg = (abs(id1)%2 == 0) ? id1 : id2; int idHchg = (idUpChg > 0) ? 37 : -37; setId( id1, id2, idHchg); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma1ffbar2Hchg::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma2qg2Hq class. // Cross section for q g -> H+- q'. //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2Hchgq::initProc() { // Standard parameters. m2W = pow2( particleDataPtr->m0(24) ); thetaWRat = 1. / (24. * couplingsPtr->sin2thetaW()); tan2Beta = pow2(settingsPtr->parm("HiggsHchg:tanBeta")); // Incoming flavour within same doublet. Uptype and downtype flavours. idOld = (idNew%2 == 0) ? idNew - 1 : idNew + 1; idUp = max(idOld, idNew); idDn = min(idOld, idNew); // Secondary open width fraction. openFracPos = (idOld%2 == 0) ? particleDataPtr->resOpenFrac( 37, idNew) : particleDataPtr->resOpenFrac(-37, idNew); openFracNeg = (idOld%2 == 0) ? particleDataPtr->resOpenFrac(-37, -idNew) : particleDataPtr->resOpenFrac( 37, -idNew); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2qg2Hchgq::sigmaKin() { // Running masses provides coupling. double m2RunUp = pow2(particleDataPtr->mRun(idUp, mH)); double m2RunDn = pow2(particleDataPtr->mRun(idDn, mH)); // Cross section, including couplings and kinematics. sigma = (M_PI / sH2) * alpS * alpEM * thetaWRat * (m2RunDn * tan2Beta + m2RunUp / tan2Beta) / m2W * (sH / (s4 - uH) + 2. * s4 * (s3 - uH) / pow2(s4 - uH) + (s4 - uH) / sH - 2. * s4 / (s4 - uH) + 2. * (s3 - uH) * (s3 - s4 - sH) / ((s4 - uH) * sH) ); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma2qg2Hchgq::sigmaHat() { // Check that specified flavour present. if (abs(id1) != idOld && abs(id2) != idOld) return 0.; // Answer. return (id1 == idOld || id2 == idOld) ? sigma * openFracPos : sigma * openFracNeg; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2Hchgq::setIdColAcol() { // Flavour set up for q g -> H+- q'. int idq = (id2 == 21) ? id1 : id2; id3 = ( (idq > 0 && idOld%2 == 0) || (idq < 0 && idOld%2 != 0) ) ? 37 : -37; id4 = (idq > 0) ? idNew : -idNew; setId( id1, id2, id3, id4); // tH defined between f and f': must swap tHat <-> uHat if q g in. swapTU = (id2 == 21); // Colour flow topologies. Swap when antiquarks. if (id2 == 21) setColAcol( 1, 0, 2, 1, 0, 0, 2, 0); else setColAcol( 2, 1, 1, 0, 0, 0, 2, 0); if (idq < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma2qg2Hchgq::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma2ffbar2A3H12 class. // Cross section for f fbar -> A0(H_3) h0(H_1) or A0(H_3) H0(H_2). //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2A3H12::initProc() { // Set up whether h0(H_1) or H0(H_2). higgs12 = (higgsType == 1) ? 25 : 35; codeSave = (higgsType == 1) ? 1081 : 1082; nameSave = (higgsType == 1) ? "f fbar -> A0(H3) h0(H1)" : "f fbar -> A0(H3) H0(H2)"; coupZA3H12 = (higgsType == 1) ? settingsPtr->parm("HiggsA3:coup2H1Z") : settingsPtr->parm("HiggsA3:coup2H2Z"); // Standard parameters. double mZ = particleDataPtr->m0(23); double GammaZ = particleDataPtr->mWidth(23); m2Z = mZ * mZ; mGammaZ = mZ * GammaZ; thetaWRat = 1. / (4. * couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(36, higgs12); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2ffbar2A3H12::sigmaKin() { // Common kinematics factora. sigma0 = (M_PI / sH2) * pow2(alpEM * thetaWRat * coupZA3H12) * (uH * tH - s3 * s4) / ( pow2(sH - m2Z) + pow2(mGammaZ) ); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma2ffbar2A3H12::sigmaHat() { // Couplings for incoming flavour. int idAbs = abs(id1); double lIn = couplingsPtr->lf(idAbs); double rIn = couplingsPtr->rf(idAbs); // Combine to total cross section. Colour factor. double sigma = (pow2(lIn) + pow2(rIn)) * sigma0 * openFrac; if (idAbs < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2A3H12::setIdColAcol() { // Flavours trivial setId( id1, id2, 36, higgs12); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma2ffbar2A3H12::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma2ffbar2HchgH12 class. // Cross section for f fbar -> H+- h0(H_1) or H+- H0(H_2). //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2HchgH12::initProc() { // Set up whether h0(H_1) or H0(H_2). higgs12 = (higgsType == 1) ? 25 : 35; codeSave = (higgsType == 1) ? 1083 : 1084; nameSave = (higgsType == 1) ? "f fbar' -> H+- h0(H1)" : "f fbar' -> H+- H0(H2)"; coupWHchgH12 = (higgsType == 1) ? settingsPtr->parm("HiggsHchg:coup2H1W") : settingsPtr->parm("HiggsHchg:coup2H2W"); // Standard parameters. double mW = particleDataPtr->m0(24); double GammaW = particleDataPtr->mWidth(24); m2W = mW * mW; mGammaW = mW * GammaW; thetaWRat = 1. / (2. * couplingsPtr->sin2thetaW()); // Secondary open width fraction. openFracPos = particleDataPtr->resOpenFrac( 37, higgs12); openFracNeg = particleDataPtr->resOpenFrac(-37, higgs12); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2ffbar2HchgH12::sigmaKin() { // Common kinematics factora. sigma0 = 0.5 * (M_PI / sH2) * pow2(alpEM * thetaWRat * coupWHchgH12) * (uH * tH - s3 * s4) / ( pow2(sH - m2W) + pow2(mGammaW) ); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma2ffbar2HchgH12::sigmaHat() { // Combine to total cross section. CKM and colour factor. int idUp = (abs(id1)%2 == 0) ? id1 : id2; double sigma = (idUp > 0) ? sigma0 * openFracPos : sigma0 * openFracNeg; if (abs(id1) < 9) sigma *= couplingsPtr->V2CKMid(abs(id1), abs(id2)) / 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2HchgH12::setIdColAcol() { // Charge of Higgs. Fill flavours. int idUpChg = (abs(id1)%2 == 0) ? id1 : id2; int idHchg = (idUpChg > 0) ? 37 : -37; setId( id1, id2, idHchg, higgs12); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma2ffbar2HchgH12::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma2ffbar2HposHneg class. // Cross section for q g -> H+- q'. //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2HposHneg::initProc() { // Standard parameters. double mZ = particleDataPtr->m0(23); double GammaZ = particleDataPtr->mWidth(23); m2Z = mZ * mZ; mGammaZ = mZ * GammaZ; thetaWRat = 1. / (4. * couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); // Charged Higgs coupling to gamma and Z0. eH = -1.; lH = -1. + 2. * couplingsPtr->sin2thetaW(); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(37, -37); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2ffbar2HposHneg::sigmaKin() { // Common kinematics factora. double preFac = M_PI * pow2(alpEM) * ((uH * tH - s3 * s4) / sH2); double propZ = 1. / ( pow2(sH - m2Z) + pow2(mGammaZ) ); // Separate parts for gamma*, interference and Z0. gamSig = preFac * 2. * pow2(eH) / sH2; intSig = preFac * 2. * eH * lH * thetaWRat * propZ * (sH - m2Z) / sH; resSig = preFac * pow2(lH * thetaWRat) * propZ; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma2ffbar2HposHneg::sigmaHat() { // Couplings for incoming flavour. int idAbs = abs(id1); double eIn = couplingsPtr->ef(idAbs); double lIn = couplingsPtr->lf(idAbs); double rIn = couplingsPtr->rf(idAbs); // Combine to total cross section. Colour factor. double sigma = (pow2(eIn) * gamSig + eIn * (lIn + rIn) * intSig + (pow2(lIn) + pow2(rIn)) * resSig) * openFrac; if (idAbs < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2HposHneg::setIdColAcol() { // Flavours trivial setId( id1, id2, 37, -37); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma2ffbar2HposHneg::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaTotal.cc0000644000175000017500000005331712217346251015507 0ustar sunsun// SigmaTotal.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the SigmaTotal class. #include "Pythia8/SigmaTotal.h" namespace Pythia8 { //========================================================================== // The SigmaTotal class. // Formulae are taken from: // G.A. Schuler and T. Sjostrand, Phys. Rev. D49 (1994) 2257, // Z. Phys. C73 (1997) 677 // which borrows some total cross sections from // A. Donnachie and P.V. Landshoff, Phys. Lett. B296 (1992) 227. // Implemented processes with their process number iProc: // = 0 : p + p; = 1 : pbar + p; // = 2 : pi+ + p; = 3 : pi- + p; = 4 : pi0/rho0 + p; // = 5 : phi + p; = 6 : J/psi + p; // = 7 : rho + rho; = 8 : rho + phi; = 9 : rho + J/psi; // = 10 : phi + phi; = 11 : phi + J/psi; = 12 : J/psi + J/psi. // = 13 : Pom + p (preliminary). // For now a neutron is treated like a proton. //-------------------------------------------------------------------------- // Definitions of static variables. // Note that a lot of parameters are hardcoded as const here, rather // than being interfaced for public change, since any changes would // have to be done in a globally consistent manner. Which basically // means a rewrite/replacement of the whole class. // Minimum threshold below which no cross sections will be defined. const double SigmaTotal::MMIN = 2.; // General constants in total cross section parametrization: // sigmaTot = X * s^epsilon + Y * s^eta (pomeron + reggeon). const double SigmaTotal::EPSILON = 0.0808; const double SigmaTotal::ETA = -0.4525; const double SigmaTotal::X[] = { 21.70, 21.70, 13.63, 13.63, 13.63, 10.01, 0.970, 8.56, 6.29, 0.609, 4.62, 0.447, 0.0434}; const double SigmaTotal::Y[] = { 56.08, 98.39, 27.56, 36.02, 31.79, 1.51, -0.146, 13.08, -0.62, -0.060, 0.030, -0.0028, 0.00028}; // Type of the two incoming hadrons as function of the process number: // = 0 : p/n ; = 1 : pi/rho/omega; = 2 : phi; = 3 : J/psi. const int SigmaTotal::IHADATABLE[] = { 0, 0, 1, 1, 1, 2, 3, 1, 1, 1, 2, 2, 3}; const int SigmaTotal::IHADBTABLE[] = { 0, 0, 0, 0, 0, 0, 0, 1, 2, 3, 2, 3, 3}; // Hadron-Pomeron coupling beta(t) = beta(0) * exp(b*t). const double SigmaTotal::BETA0[] = { 4.658, 2.926, 2.149, 0.208}; const double SigmaTotal::BHAD[] = { 2.3, 1.4, 1.4, 0.23}; // Pomeron trajectory alpha(t) = 1 + epsilon + alpha' * t const double SigmaTotal::ALPHAPRIME = 0.25; // Conversion coefficients = 1/(16pi) * (mb <-> GeV^2) * (G_3P)^n, // with n = 0 elastic, n = 1 single and n = 2 double diffractive. const double SigmaTotal::CONVERTEL = 0.0510925; const double SigmaTotal::CONVERTSD = 0.0336; const double SigmaTotal::CONVERTDD = 0.0084; // Diffractive mass spectrum starts at m + MMIN0 and has a low-mass // enhancement, factor cRes, up to around m + mRes0. const double SigmaTotal::MMIN0 = 0.28; const double SigmaTotal::CRES = 2.0; const double SigmaTotal::MRES0 = 1.062; // Parameters and coefficients for single diffractive scattering. const int SigmaTotal::ISDTABLE[] = { 0, 0, 1, 1, 1, 2, 3, 4, 5, 6, 7, 8, 9}; const double SigmaTotal::CSD[10][8] = { { 0.213, 0.0, -0.47, 150., 0.213, 0.0, -0.47, 150., } , { 0.213, 0.0, -0.47, 150., 0.267, 0.0, -0.47, 100., } , { 0.213, 0.0, -0.47, 150., 0.232, 0.0, -0.47, 110., } , { 0.213, 7.0, -0.55, 800., 0.115, 0.0, -0.47, 110., } , { 0.267, 0.0, -0.46, 75., 0.267, 0.0, -0.46, 75., } , { 0.232, 0.0, -0.46, 85., 0.267, 0.0, -0.48, 100., } , { 0.115, 0.0, -0.50, 90., 0.267, 6.0, -0.56, 420., } , { 0.232, 0.0, -0.48, 110., 0.232, 0.0, -0.48, 110., } , { 0.115, 0.0, -0.52, 120., 0.232, 6.0, -0.56, 470., } , { 0.115, 5.5, -0.58, 570., 0.115, 5.5, -0.58, 570. } }; // Parameters and coefficients for double diffractive scattering. const int SigmaTotal::IDDTABLE[] = { 0, 0, 1, 1, 1, 2, 3, 4, 5, 6, 7, 8, 9}; const double SigmaTotal::CDD[10][9] = { { 3.11, -7.34, 9.71, 0.068, -0.42, 1.31, -1.37, 35.0, 118., } , { 3.11, -7.10, 10.6, 0.073, -0.41, 1.17, -1.41, 31.6, 95., } , { 3.12, -7.43, 9.21, 0.067, -0.44, 1.41, -1.35, 36.5, 132., } , { 3.13, -8.18, -4.20, 0.056, -0.71, 3.12, -1.12, 55.2, 1298., } , { 3.11, -6.90, 11.4, 0.078, -0.40, 1.05, -1.40, 28.4, 78., } , { 3.11, -7.13, 10.0, 0.071, -0.41, 1.23, -1.34, 33.1, 105., } , { 3.12, -7.90, -1.49, 0.054, -0.64, 2.72, -1.13, 53.1, 995., } , { 3.11, -7.39, 8.22, 0.065, -0.44, 1.45, -1.36, 38.1, 148., } , { 3.18, -8.95, -3.37, 0.057, -0.76, 3.32, -1.12, 55.6, 1472., } , { 4.18, -29.2, 56.2, 0.074, -1.36, 6.67, -1.14, 116.2, 6532. } }; const double SigmaTotal::SPROTON = 0.880; // MBR parameters. Integration of MBR cross section. const int SigmaTotal::NINTEG = 1000; const int SigmaTotal::NINTEG2 = 40; const double SigmaTotal::HBARC2 = 0.38938; // MBR: form factor appoximation with two exponents, [FFB1,FFB2] = GeV^-2. const double SigmaTotal::FFA1 = 0.9; const double SigmaTotal::FFA2 = 0.1; const double SigmaTotal::FFB1 = 4.6; const double SigmaTotal::FFB2 = 0.6; //-------------------------------------------------------------------------- // Store pointer to Info and initialize data members. void SigmaTotal::init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn) { // Store pointers. infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; // Normalization of central diffractive cross section. zeroAXB = settings.flag("SigmaTotal:zeroAXB"); sigAXB2TeV = settings.parm("SigmaTotal:sigmaAXB2TeV"); // User-set values for cross sections. setTotal = settings.flag("SigmaTotal:setOwn"); sigTotOwn = settings.parm("SigmaTotal:sigmaTot"); sigElOwn = settings.parm("SigmaTotal:sigmaEl"); sigXBOwn = settings.parm("SigmaTotal:sigmaXB"); sigAXOwn = settings.parm("SigmaTotal:sigmaAX"); sigXXOwn = settings.parm("SigmaTotal:sigmaXX"); sigAXBOwn = settings.parm("SigmaTotal:sigmaAXB"); // User-set values to dampen diffractive cross sections. doDampen = settings.flag("SigmaDiffractive:dampen"); maxXBOwn = settings.parm("SigmaDiffractive:maxXB"); maxAXOwn = settings.parm("SigmaDiffractive:maxAX"); maxXXOwn = settings.parm("SigmaDiffractive:maxXX"); maxAXBOwn = settings.parm("SigmaDiffractive:maxAXB"); // User-set values for handling of elastic sacattering. setElastic = settings.flag("SigmaElastic:setOwn"); bSlope = settings.parm("SigmaElastic:bSlope"); rho = settings.parm("SigmaElastic:rho"); lambda = settings.parm("SigmaElastic:lambda"); tAbsMin = settings.parm("SigmaElastic:tAbsMin"); alphaEM0 = settings.parm("StandardModel:alphaEM0"); // Parameters for diffractive systems. sigmaPomP = settings.parm("Diffraction:sigmaRefPomP"); mPomP = settings.parm("Diffraction:mRefPomP"); pPomP = settings.parm("Diffraction:mPowPomP"); // Parameters for MBR model. PomFlux = settings.mode("Diffraction:PomFlux"); MBReps = settings.parm("Diffraction:MBRepsilon"); MBRalpha = settings.parm("Diffraction:MBRalpha"); MBRbeta0 = settings.parm("Diffraction:MBRbeta0"); MBRsigma0 = settings.parm("Diffraction:MBRsigma0"); m2min = settings.parm("Diffraction:MBRm2Min"); dyminSDflux = settings.parm("Diffraction:MBRdyminSDflux"); dyminDDflux = settings.parm("Diffraction:MBRdyminDDflux"); dyminCDflux = settings.parm("Diffraction:MBRdyminCDflux"); dyminSD = settings.parm("Diffraction:MBRdyminSD"); dyminDD = settings.parm("Diffraction:MBRdyminDD"); dyminCD = settings.parm("Diffraction:MBRdyminCD"); dyminSigSD = settings.parm("Diffraction:MBRdyminSigSD"); dyminSigDD = settings.parm("Diffraction:MBRdyminSigDD"); dyminSigCD = settings.parm("Diffraction:MBRdyminSigCD"); } //-------------------------------------------------------------------------- // Function that calculates the relevant properties. bool SigmaTotal::calc( int idA, int idB, double eCM) { // Derived quantities. alP2 = 2. * ALPHAPRIME; s0 = 1. / ALPHAPRIME; // Reset everything to zero to begin with. isCalc = false; sigTot = sigEl = sigXB = sigAX = sigXX = sigAXB = sigND = bEl = s = bA = bB = 0.; // Order flavour of incoming hadrons: idAbsA < idAbsB (restore later). int idAbsA = abs(idA); int idAbsB = abs(idB); bool swapped = false; if (idAbsA > idAbsB) { swap( idAbsA, idAbsB); swapped = true; } double sameSign = (idA * idB > 0); // Find process number. int iProc = -1; if (idAbsA > 1000) { iProc = (sameSign) ? 0 : 1; } else if (idAbsA > 100 && idAbsB > 1000) { iProc = (sameSign) ? 2 : 3; if (idAbsA/10 == 11 || idAbsA/10 == 22) iProc = 4; if (idAbsA > 300) iProc = 5; if (idAbsA > 400) iProc = 6; if (idAbsA > 900) iProc = 13; } else if (idAbsA > 100) { iProc = 7; if (idAbsB > 300) iProc = 8; if (idAbsB > 400) iProc = 9; if (idAbsA > 300) iProc = 10; if (idAbsA > 300 && idAbsB > 400) iProc = 11; if (idAbsA > 400) iProc = 12; } if (iProc == -1) return false; // Primitive implementation of Pomeron + p. if (iProc == 13) { s = eCM*eCM; sigTot = sigmaPomP * pow( eCM / mPomP, pPomP); sigND = sigTot; isCalc = true; return true; } // Find hadron masses and check that energy is enough. // For mesons use the corresponding vector meson masses. int idModA = (idAbsA > 1000) ? idAbsA : 10 * (idAbsA/10) + 3; int idModB = (idAbsB > 1000) ? idAbsB : 10 * (idAbsB/10) + 3; double mA = particleDataPtr->m0(idModA); double mB = particleDataPtr->m0(idModB); if (eCM < mA + mB + MMIN) { infoPtr->errorMsg("Error in SigmaTotal::calc: too low energy"); return false; } // Evaluate the total cross section. s = eCM*eCM; double sEps = pow( s, EPSILON); double sEta = pow( s, ETA); sigTot = X[iProc] * sEps + Y[iProc] * sEta; // Slope of hadron form factors. int iHadA = IHADATABLE[iProc]; int iHadB = IHADBTABLE[iProc]; bA = BHAD[iHadA]; bB = BHAD[iHadB]; // Elastic slope parameter and cross section. bEl = 2.*bA + 2.*bB + 4.*sEps - 4.2; sigEl = CONVERTEL * pow2(sigTot) / bEl; // Lookup coefficients for single and double diffraction. int iSD = ISDTABLE[iProc]; int iDD = IDDTABLE[iProc]; double sum1, sum2, sum3, sum4; // Single diffractive scattering A + B -> X + B cross section. mMinXBsave = mA + MMIN0; double sMinXB = pow2(mMinXBsave); mResXBsave = mA + MRES0; double sResXB = pow2(mResXBsave); double sRMavgXB = mResXBsave * mMinXBsave; double sRMlogXB = log(1. + sResXB/sMinXB); double sMaxXB = CSD[iSD][0] * s + CSD[iSD][1]; double BcorrXB = CSD[iSD][2] + CSD[iSD][3] / s; sum1 = log( (2.*bB + alP2 * log(s/sMinXB)) / (2.*bB + alP2 * log(s/sMaxXB)) ) / alP2; sum2 = CRES * sRMlogXB / (2.*bB + alP2 * log(s/sRMavgXB) + BcorrXB) ; sigXB = CONVERTSD * X[iProc] * BETA0[iHadB] * max( 0., sum1 + sum2); // Single diffractive scattering A + B -> A + X cross section. mMinAXsave = mB + MMIN0; double sMinAX = pow2(mMinAXsave); mResAXsave = mB + MRES0; double sResAX = pow2(mResAXsave); double sRMavgAX = mResAXsave * mMinAXsave; double sRMlogAX = log(1. + sResAX/sMinAX); double sMaxAX = CSD[iSD][4] * s + CSD[iSD][5]; double BcorrAX = CSD[iSD][6] + CSD[iSD][7] / s; sum1 = log( (2.*bA + alP2 * log(s/sMinAX)) / (2.*bA + alP2 * log(s/sMaxAX)) ) / alP2; sum2 = CRES * sRMlogAX / (2.*bA + alP2 * log(s/sRMavgAX) + BcorrAX) ; sigAX = CONVERTSD * X[iProc] * BETA0[iHadA] * max( 0., sum1 + sum2); // Order single diffractive correctly. if (swapped) { swap( bB, bA); swap( sigXB, sigAX); swap( mMinXBsave, mMinAXsave); swap( mResXBsave, mResAXsave); } // Double diffractive scattering A + B -> X1 + X2 cross section. double y0min = log( s * SPROTON / (sMinXB * sMinAX) ) ; double sLog = log(s); double Delta0 = CDD[iDD][0] + CDD[iDD][1] / sLog + CDD[iDD][2] / pow2(sLog); sum1 = (y0min * (log( max( 1e-10, y0min/Delta0) ) - 1.) + Delta0)/ alP2; if (y0min < 0.) sum1 = 0.; double sMaxXX = s * ( CDD[iDD][3] + CDD[iDD][4] / sLog + CDD[iDD][5] / pow2(sLog) ); double sLogUp = log( max( 1.1, s * s0 / (sMinXB * sRMavgAX) )); double sLogDn = log( max( 1.1, s * s0 / (sMaxXX * sRMavgAX) )); sum2 = CRES * log( sLogUp / sLogDn ) * sRMlogAX / alP2; sLogUp = log( max( 1.1, s * s0 / (sMinAX * sRMavgXB) )); sLogDn = log( max( 1.1, s * s0 / (sMaxXX * sRMavgXB) )); sum3 = CRES * log(sLogUp / sLogDn) * sRMlogXB / alP2; double BcorrXX = CDD[iDD][6] + CDD[iDD][7] / eCM + CDD[iDD][8] / s; sum4 = pow2(CRES) * sRMlogAX * sRMlogXB / max( 0.1, alP2 * log( s * s0 / (sRMavgAX * sRMavgXB) ) + BcorrXX); sigXX = CONVERTDD * X[iProc] * max( 0., sum1 + sum2 + sum3 + sum4); // Central diffractive scattering A + B -> A + X + B, only p and pbar. mMinAXBsave = 1.; if ( (idAbsA == 2212 || idAbsA == 2112) && (idAbsB == 2212 || idAbsB == 2112) && !zeroAXB) { double sMinAXB = pow2(mMinAXBsave); double sRefAXB = pow2(2000.); sigAXB = sigAXB2TeV * pow( log(0.06 * s / sMinAXB), 1.5 ) / pow( log(0.06 * sRefAXB / sMinAXB), 1.5 ); } // Option with user-requested damping of diffractive cross sections. if (doDampen) { sigXB = sigXB * maxXBOwn / (sigXB + maxXBOwn); sigAX = sigAX * maxAXOwn / (sigAX + maxAXOwn); sigXX = sigXX * maxXXOwn / (sigXX + maxXXOwn); sigAXB = sigAXB * maxAXBOwn / (sigAXB + maxAXBOwn); } // Calculate cross sections in MBR model. if (PomFlux == 5) calcMBRxsecs(idA, idB, eCM); // Option with user-set values for total and partial cross sections. // (Is not done earlier since want diffractive slopes anyway.) double sigNDOwn = sigTotOwn - sigElOwn - sigXBOwn - sigAXOwn - sigXXOwn - sigAXBOwn; double sigElMax = sigEl; if (setTotal && sigNDOwn > 0.) { sigTot = sigTotOwn; sigEl = sigElOwn; sigXB = sigXBOwn; sigAX = sigAXOwn; sigXX = sigXXOwn; sigAXB = sigAXBOwn; sigElMax = sigEl; // Sub-option to set elastic parameters, including Coulomb contribution. if (setElastic) { bEl = bSlope; sigEl = CONVERTEL * pow2(sigTot) * (1. + rho*rho) / bSlope; sigElMax = 2. * (sigEl * exp(-bSlope * tAbsMin) + alphaEM0 * alphaEM0 / (4. * CONVERTEL * tAbsMin) ); } } // Inelastic nondiffractive by unitarity. sigND = sigTot - sigEl - sigXB - sigAX - sigXX - sigAXB; if (sigND < 0.) infoPtr->errorMsg("Error in SigmaTotal::init: " "sigND < 0"); else if (sigND < 0.4 * sigTot) infoPtr->errorMsg("Warning in " "SigmaTotal::init: sigND suspiciously low"); // Upper estimate of elastic, including Coulomb term, where appropriate. sigEl = sigElMax; // Done. isCalc = true; return true; } //-------------------------------------------------------------------------- // Calculate parameters in the MBR model. bool SigmaTotal::calcMBRxsecs( int idA, int idB, double eCM) { // Local variables. double sigtot, sigel, sigsd, sigdd, sigdpe; // MBR parameters locally. double eps = MBReps; double alph = MBRalpha; double beta0gev = MBRbeta0; double beta0mb = beta0gev * sqrt(HBARC2); double sigma0mb = MBRsigma0; double sigma0gev = sigma0mb/HBARC2; double a1 = FFA1; double a2 = FFA2; double b1 = FFB1; double b2 = FFB2; // Calculate total and elastic cross sections. double ratio; if (eCM <= 1800.0) { double sign = (idA * idB > 0); sigtot = 16.79 * pow(s, 0.104) + 60.81 * pow(s, -0.32) - sign * 31.68 * pow(s, -0.54); ratio = 0.100 * pow(s, 0.06) + 0.421 * pow(s, -0.52) + sign * 0.160 * pow(s, -0.6); } else { double sigCDF = 80.03; double sCDF = pow2(1800.); double sF = pow2(22.); sigtot = sigCDF + ( pow2( log(s / sF)) - pow2( log(sCDF / sF)) ) * M_PI / (3.7 / HBARC2); ratio = 0.066 + 0.0119 * log(s); } sigel=sigtot*ratio; // Integrate SD, DD and DPE(CD) cross sections. // Each cross section is obtained from the ratio of two integrals: // the Regge cross section and the renormalized flux. double cflux, csig, c1, step, f; double dymin0 = 0.; // Calculate SD cross section. double dymaxSD = log(s / m2min); cflux = pow2(beta0gev) / (16. * M_PI); csig = cflux * sigma0mb; // SD flux. c1 = cflux; double fluxsd = 0.; step = (dymaxSD - dyminSDflux) / NINTEG; for (int i = 0; i < NINTEG; ++i) { double dy = dyminSDflux + (i + 0.5) * step; f = exp(2. * eps * dy) * ( (a1 / (b1 + 2. * alph * dy)) + (a2 / (b2 + 2. * alph * dy)) ); f *= 0.5 * (1. + erf( (dy - dyminSD) / dyminSigSD)); fluxsd = fluxsd + step * c1 * f; } if (fluxsd < 1.) fluxsd = 1.; // Regge cross section. c1 = csig * pow(s, eps); sigsd = 0.; sdpmax = 0.; step = (dymaxSD - dymin0) / NINTEG; for (int i = 0; i < NINTEG; ++i) { double dy = dymin0 + (i + 0.5) * step; f = exp(eps * dy) * ( (a1 / (b1 + 2. * alph * dy)) + (a2 / (b2 + 2. * alph * dy)) ); f *= 0.5 * (1. + erf( (dy - dyminSD) / dyminSigSD)); if (f > sdpmax) sdpmax = f; sigsd = sigsd + step * c1 * f; } sdpmax *= 1.01; sigsd /= fluxsd; // Calculate DD cross section. // Note: dymaxDD = ln(s * s0 /mMin^4) with s0 = 1 GeV^2. double dymaxDD = log(s / pow2(m2min)); cflux = sigma0gev / (16. * M_PI); csig = cflux * sigma0mb; // DD flux. c1 = cflux / (2. * alph); double fluxdd = 0.; step = (dymaxDD - dyminDDflux) / NINTEG; for (int i = 0; i < NINTEG; ++i) { double dy = dyminDDflux + (i + 0.5) * step; f = (dymaxDD - dy) * exp(2. * eps * dy) * ( exp(-2. * alph * dy * exp(-dy)) - exp(-2. * alph * dy * exp(dy)) ) / dy; f *= 0.5 * (1. + erf( (dy - dyminDD) / dyminSigDD)); fluxdd = fluxdd + step * c1 * f; } if (fluxdd < 1.) fluxdd = 1.; // Regge cross section. c1 = csig * pow(s, eps) / (2. * alph); ddpmax = 0.; sigdd = 0.; step = (dymaxDD - dymin0) / NINTEG; for (int i = 0; i < NINTEG; ++i) { double dy = dymin0 + (i + 0.5) * step; f = (dymaxDD - dy) * exp(eps * dy) * ( exp(-2. * alph * dy * exp(-dy)) - exp(-2. * alph * dy * exp(dy)) ) / dy; f *= 0.5 * (1. + erf( (dy - dyminDD) / dyminSigDD)); if (f > ddpmax) ddpmax = f; sigdd = sigdd + step * c1 * f; } ddpmax *= 1.01; sigdd /= fluxdd; // Calculate DPE (CD) cross section. double dymaxCD = log(s / m2min); cflux = pow4(beta0gev) / pow2(16. * M_PI); csig = cflux * pow2(sigma0mb / beta0mb); double dy1, dy2, f1, f2, step2; // DPE flux. c1 = cflux; double fluxdpe = 0.; step = (dymaxCD - dyminCDflux) / NINTEG; for (int i = 0; i < NINTEG; ++i) { double dy = dyminCDflux + (i + 0.5) * step; f = 0.; step2 = (dy - dyminCDflux) / NINTEG2; for (int j = 0; j < NINTEG2; ++j) { double yc = -0.5 * (dy - dyminCDflux) + (j + 0.5) * step2; dy1 = 0.5 * dy - yc; dy2 = 0.5 * dy + yc; f1 = exp(2. * eps * dy1) * ( (a1 / (b1 + 2. * alph * dy1)) + (a2 / (b2 + 2. * alph * dy1)) ); f2 = exp(2. * eps * dy2) * ( (a1 / (b1 + 2. * alph * dy2)) + (a2 / (b2 + 2. * alph * dy2)) ); f1 *= 0.5 * (1. + erf( (dy1 - 0.5 * dyminCD) / (dyminSigCD / sqrt(2.))) ); f2 *= 0.5 * (1. + erf( (dy2 - 0.5 *dyminCD) / (dyminSigCD / sqrt(2.))) ); f += f1 * f2 * step2; } fluxdpe += step * c1 * f; } if (fluxdpe < 1.) fluxdpe = 1.; // Regge cross section. c1 = csig * pow(s, eps); sigdpe = 0.; dpepmax = 0; step = (dymaxCD - dymin0) / NINTEG; for (int i = 0; i < NINTEG; ++i) { double dy = dymin0 + (i + 0.5) * step; f = 0.; step2 = (dy - dymin0) / NINTEG2; for (int j = 0; j < NINTEG2; ++j) { double yc = -0.5 * (dy - dymin0) + (j + 0.5) * step2; dy1 = 0.5 * dy - yc; dy2 = 0.5 * dy + yc; f1 = exp(eps * dy1) * ( (a1 / (b1 + 2. * alph * dy1)) + (a2 / (b2 + 2. * alph * dy1)) ); f2 = exp(eps * dy2) * ( (a1 / (b1 + 2. * alph * dy2)) + (a2 / (b2 + 2. * alph * dy2)) ); f1 *= 0.5 * (1. + erf( (dy1 - 0.5 * dyminCD) / (dyminSigCD / sqrt(2.))) ); f2 *= 0.5 * (1. + erf( (dy2 - 0.5 * dyminCD) /(dyminSigCD / sqrt(2.))) ); f += f1 * f2 * step2; } sigdpe += step * c1 * f; if ( f > dpepmax) dpepmax = f; } dpepmax *= 1.01; sigdpe /= fluxdpe; // Diffraction done. Now calculate total inelastic cross section. sigND = sigtot - (2. * sigsd + sigdd + sigel + sigdpe); sigTot = sigtot; sigEl = sigel; sigAX = sigsd; sigXB = sigsd; sigXX = sigdd; sigAXB = sigdpe; return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/PartonDistributions.cc0000644000175000017500000022731512217346246017476 0ustar sunsun// PartonDistributions.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the PDF, LHAPDF, // GRV94L, CTEQ5L, MSTWpdf, CTEQ6pdf, GRVpiL, PomFix, PomH1FitAB, // PomH1Jets, Lepton and NNPDF classes. #include "Pythia8/PartonDistributions.h" #include "Pythia8/LHAPDFInterface.h" namespace Pythia8 { //========================================================================== // Base class for parton distribution functions. //-------------------------------------------------------------------------- // Resolve valence content for assumed meson. Possibly modified later. void PDF::setValenceContent() { // Subdivide meson by flavour content. if (idBeamAbs < 100 || idBeamAbs > 1000) return; int idTmp1 = idBeamAbs/100; int idTmp2 = (idBeamAbs/10)%10; // Find which is quark and which antiquark. if (idTmp1%2 == 0) { idVal1 = idTmp1; idVal2 = -idTmp2; } else { idVal1 = idTmp2; idVal2 = -idTmp1; } if (idBeam < 0) { idVal1 = -idVal1; idVal2 = -idVal2; } // Special case for Pomeron, to start off. if (idBeamAbs == 990) { idVal1 = 1; idVal2 = -1; } } //-------------------------------------------------------------------------- // Standard parton densities. double PDF::xf(int id, double x, double Q2) { // Need to update if flavour, x or Q2 changed. // Use idSav = 9 to indicate that ALL flavours are up-to-date. // Assume that flavour and antiflavour always updated simultaneously. if ( (abs(idSav) != abs(id) && idSav != 9) || x != xSav || Q2 != Q2Sav) {idSav = id; xfUpdate(id, x, Q2); xSav = x; Q2Sav = Q2;} // Baryon and nondiagonal meson beams: only p, pbar, pi+, pi- for now. if (idBeamAbs == 2212 || idBeamAbs == 211) { int idNow = (idBeam > 0) ? id : -id; int idAbs = abs(id); if (idNow == 0 || idAbs == 21) return max(0., xg); if (idNow == 1) return max(0., xd); if (idNow == -1) return max(0., xdbar); if (idNow == 2) return max(0., xu); if (idNow == -2) return max(0., xubar); if (idNow == 3) return max(0., xs); if (idNow == -3) return max(0., xsbar); if (idAbs == 4) return max(0., xc); if (idAbs == 5) return max(0., xb); if (idAbs == 22) return max(0., xgamma); return 0.; // Baryon beams: n and nbar by isospin conjugation of p and pbar. } else if (idBeamAbs == 2112) { int idNow = (idBeam > 0) ? id : -id; int idAbs = abs(id); if (idNow == 0 || idAbs == 21) return max(0., xg); if (idNow == 1) return max(0., xu); if (idNow == -1) return max(0., xubar); if (idNow == 2) return max(0., xd); if (idNow == -2) return max(0., xdbar); if (idNow == 3) return max(0., xs); if (idNow == -3) return max(0., xsbar); if (idAbs == 4) return max(0., xc); if (idAbs == 5) return max(0., xb); if (idAbs == 22) return max(0., xgamma); return 0.; // Diagonal meson beams: only pi0, Pomeron for now. } else if (idBeam == 111 || idBeam == 990) { int idAbs = abs(id); if (id == 0 || idAbs == 21) return max(0., xg); if (id == idVal1 || id == idVal2) return max(0., xu); if (idAbs <= 2) return max(0., xubar); if (idAbs == 3) return max(0., xs); if (idAbs == 4) return max(0., xc); if (idAbs == 5) return max(0., xb); if (idAbs == 22) return max(0., xgamma); return 0.; // Lepton beam. } else { if (id == idBeam ) return max(0., xlepton); if (abs(id) == 22) return max(0., xgamma); return 0.; } } //-------------------------------------------------------------------------- // Only valence part of parton densities. double PDF::xfVal(int id, double x, double Q2) { // Need to update if flavour, x or Q2 changed. // Use idSav = 9 to indicate that ALL flavours are up-to-date. // Assume that flavour and antiflavour always updated simultaneously. if ( (abs(idSav) != abs(id) && idSav != 9) || x != xSav || Q2 != Q2Sav) {idSav = id; xfUpdate(id, x, Q2); xSav = x; Q2Sav = Q2;} // Baryon and nondiagonal meson beams: only p, pbar, n, nbar, pi+, pi-. if (idBeamAbs == 2212) { int idNow = (idBeam > 0) ? id : -id; if (idNow == 1) return max(0., xdVal); if (idNow == 2) return max(0., xuVal); return 0.; } else if (idBeamAbs == 2112) { int idNow = (idBeam > 0) ? id : -id; if (idNow == 1) return max(0., xuVal); if (idNow == 2) return max(0., xdVal); return 0.; } else if (idBeamAbs == 211) { int idNow = (idBeam > 0) ? id : -id; if (idNow == 2 || idNow == -1) return max(0., xuVal); return 0.; // Diagonal meson beams: only pi0, Pomeron for now. } else if (idBeam == 111 || idBeam == 990) { if (id == idVal1 || id == idVal2) return max(0., xuVal); return 0.; // Lepton beam. } else { if (id == idBeam) return max(0., xlepton); return 0.; } } //-------------------------------------------------------------------------- // Only sea part of parton densities. double PDF::xfSea(int id, double x, double Q2) { // Need to update if flavour, x or Q2 changed. // Use idSav = 9 to indicate that ALL flavours are up-to-date. // Assume that flavour and antiflavour always updated simultaneously. if ( (abs(idSav) != abs(id) && idSav != 9) || x != xSav || Q2 != Q2Sav) {idSav = id; xfUpdate(id, x, Q2); xSav = x; Q2Sav = Q2;} // Hadron beams. if (idBeamAbs > 100) { int idNow = (idBeam > 0) ? id : -id; int idAbs = abs(id); if (idNow == 0 || idAbs == 21) return max(0., xg); if (idBeamAbs == 2212) { if (idNow == 1) return max(0., xdSea); if (idNow == -1) return max(0., xdbar); if (idNow == 2) return max(0., xuSea); if (idNow == -2) return max(0., xubar); } else if (idBeamAbs == 2112) { if (idNow == 1) return max(0., xuSea); if (idNow == -1) return max(0., xubar); if (idNow == 2) return max(0., xdSea); if (idNow == -2) return max(0., xdbar); } else { if (idAbs <= 2) return max(0., xuSea); } if (idNow == 3) return max(0., xs); if (idNow == -3) return max(0., xsbar); if (idAbs == 4) return max(0., xc); if (idAbs == 5) return max(0., xb); if (idAbs == 22) return max(0., xgamma); return 0.; // Lepton beam. } else { if (abs(id) == 22) return max(0., xgamma); return 0.; } } //========================================================================== // Interface to the LHAPDF library. //-------------------------------------------------------------------------- // Define static member of the LHAPDF class. map< int, pair > LHAPDF::initializedSets; //-------------------------------------------------------------------------- // Static method to find the nSet number corresponding to a name and member. // Returns -1 if no such LHAPDF set has been initialized. int LHAPDF::findNSet(string setName, int member) { for (map >::const_iterator i = initializedSets.begin(); i != initializedSets.end(); ++i) { int iSet = i->first; string iName = i->second.first; int iMember = i->second.second; if (iName == setName && iMember == member) return iSet; } return -1; } //-------------------------------------------------------------------------- // Static method to return the lowest non-occupied nSet number. int LHAPDF::freeNSet() { for (int iSet = 1; iSet <= int(initializedSets.size()); ++iSet) { if (initializedSets.find(iSet) == initializedSets.end()) return iSet; } return initializedSets.size() + 1; } //-------------------------------------------------------------------------- // Initialize a parton density function from LHAPDF. void LHAPDF::init(string setName, int member, Info* infoPtr) { // Determine whether the pdf set contains the photon or not. // So far only MRST2004QED and NNPDF2.3QED. if ( setName == "MRST2004qed.LHgrid" || setName == "NNPDF23_lo_as_0130_qed.LHgrid" || setName == "NNPDF23_lo_as_0119_qed.LHgrid" || setName == "NNPDF23_nlo_as_0119_qed.LHgrid" || setName == "NNPDF23_nnlo_as_0119_qed.LHgrid" ) hasPhoton = true; else hasPhoton = false; // If already initialized then need not do anything further. pair initializedNameMember = initializedSets[nSet]; string initializedSetName = initializedNameMember.first; int initializedMember = initializedNameMember.second; if (setName == initializedSetName && member == initializedMember) return; // Initialize set. If first character is '/' then assume that name // is given with path, else not. if (setName[0] == '/') LHAPDFInterface::initPDFsetM( nSet, setName); else LHAPDFInterface::initPDFsetByNameM( nSet, setName); // Check that not dummy library was linked and put nSet negative. isSet = (nSet >= 0); if (!isSet) { if (infoPtr != 0) infoPtr->errorMsg("Error from LHAPDF::init: " "you try to use LHAPDF but did not link it"); else cout << " Error from LHAPDF::init: you try to use LHAPDF " << "but did not link it" << endl; } // Initialize member. LHAPDFInterface::initPDFM(nSet, member); // Do not collect statistics on under/overflow to save time and space. LHAPDFInterface::setPDFparm( "NOSTAT" ); LHAPDFInterface::setPDFparm( "LOWKEY" ); // Save values to avoid unnecessary reinitializations. if (nSet > 0) initializedSets[nSet] = make_pair(setName, member); } //-------------------------------------------------------------------------- // Allow optional extrapolation beyond boundaries. void LHAPDF::setExtrapolate(bool extrapol) { LHAPDFInterface::setPDFparm( (extrapol) ? "EXTRAPOLATE" : "18" ); } //-------------------------------------------------------------------------- // Give the parton distribution function set from LHAPDF. void LHAPDF::xfUpdate(int , double x, double Q2) { // Let LHAPDF do the evaluation of parton densities. double Q = sqrt( max( 0., Q2)); // Use special call if photon included in proton. if (hasPhoton) { LHAPDFInterface::evolvePDFPHOTONM( nSet, x, Q, xfArray, xPhoton); } // Else use default LHAPDF call. else { LHAPDFInterface::evolvePDFM( nSet, x, Q, xfArray); xPhoton=0.0; } // Update values. xg = xfArray[6]; xu = xfArray[8]; xd = xfArray[7]; xs = xfArray[9]; xubar = xfArray[4]; xdbar = xfArray[5]; xsbar = xfArray[3]; xc = xfArray[10]; xb = xfArray[11]; xgamma = xPhoton; // Subdivision of valence and sea. xuVal = xu - xubar; xuSea = xubar; xdVal = xd - xdbar; xdSea = xdbar; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //========================================================================== // Gives the GRV 94 L (leading order) parton distribution function set // in parametrized form. Authors: M. Glueck, E. Reya and A. Vogt. // Ref: M. Glueck, E. Reya and A. Vogt, Z.Phys. C67 (1995) 433. void GRV94L::xfUpdate(int , double x, double Q2) { // Common expressions. Constrain Q2 for which parametrization is valid. double mu2 = 0.23; double lam2 = 0.2322 * 0.2322; double s = (Q2 > mu2) ? log( log(Q2/lam2) / log(mu2/lam2) ) : 0.; double ds = sqrt(s); double s2 = s * s; double s3 = s2 * s; // uv : double nu = 2.284 + 0.802 * s + 0.055 * s2; double aku = 0.590 - 0.024 * s; double bku = 0.131 + 0.063 * s; double au = -0.449 - 0.138 * s - 0.076 * s2; double bu = 0.213 + 2.669 * s - 0.728 * s2; double cu = 8.854 - 9.135 * s + 1.979 * s2; double du = 2.997 + 0.753 * s - 0.076 * s2; double uv = grvv (x, nu, aku, bku, au, bu, cu, du); // dv : double nd = 0.371 + 0.083 * s + 0.039 * s2; double akd = 0.376; double bkd = 0.486 + 0.062 * s; double ad = -0.509 + 3.310 * s - 1.248 * s2; double bd = 12.41 - 10.52 * s + 2.267 * s2; double cd = 6.373 - 6.208 * s + 1.418 * s2; double dd = 3.691 + 0.799 * s - 0.071 * s2; double dv = grvv (x, nd, akd, bkd, ad, bd, cd, dd); // udb : double alx = 1.451; double bex = 0.271; double akx = 0.410 - 0.232 * s; double bkx = 0.534 - 0.457 * s; double agx = 0.890 - 0.140 * s; double bgx = -0.981; double cx = 0.320 + 0.683 * s; double dx = 4.752 + 1.164 * s + 0.286 * s2; double ex = 4.119 + 1.713 * s; double esx = 0.682 + 2.978 * s; double udb = grvw (x, s, alx, bex, akx, bkx, agx, bgx, cx, dx, ex, esx); // del : double ne = 0.082 + 0.014 * s + 0.008 * s2; double ake = 0.409 - 0.005 * s; double bke = 0.799 + 0.071 * s; double ae = -38.07 + 36.13 * s - 0.656 * s2; double be = 90.31 - 74.15 * s + 7.645 * s2; double ce = 0.; double de = 7.486 + 1.217 * s - 0.159 * s2; double del = grvv (x, ne, ake, bke, ae, be, ce, de); // sb : double sts = 0.; double als = 0.914; double bes = 0.577; double aks = 1.798 - 0.596 * s; double as = -5.548 + 3.669 * ds - 0.616 * s; double bs = 18.92 - 16.73 * ds + 5.168 * s; double dst = 6.379 - 0.350 * s + 0.142 * s2; double est = 3.981 + 1.638 * s; double ess = 6.402; double sb = grvs (x, s, sts, als, bes, aks, as, bs, dst, est, ess); // cb : double stc = 0.888; double alc = 1.01; double bec = 0.37; double akc = 0.; double ac = 0.; double bc = 4.24 - 0.804 * s; double dct = 3.46 - 1.076 * s; double ect = 4.61 + 1.49 * s; double esc = 2.555 + 1.961 * s; double chm = grvs (x, s, stc, alc, bec, akc, ac, bc, dct, ect, esc); // bb : double stb = 1.351; double alb = 1.00; double beb = 0.51; double akb = 0.; double ab = 0.; double bb = 1.848; double dbt = 2.929 + 1.396 * s; double ebt = 4.71 + 1.514 * s; double esb = 4.02 + 1.239 * s; double bot = grvs (x, s, stb, alb, beb, akb, ab, bb, dbt, ebt, esb); // gl : double alg = 0.524; double beg = 1.088; double akg = 1.742 - 0.930 * s; double bkg = - 0.399 * s2; double ag = 7.486 - 2.185 * s; double bg = 16.69 - 22.74 * s + 5.779 * s2; double cg = -25.59 + 29.71 * s - 7.296 * s2; double dg = 2.792 + 2.215 * s + 0.422 * s2 - 0.104 * s3; double eg = 0.807 + 2.005 * s; double esg = 3.841 + 0.316 * s; double gl = grvw (x, s, alg, beg, akg, bkg, ag, bg, cg, dg, eg, esg); // Update values xg = gl; xu = uv + 0.5*(udb - del); xd = dv + 0.5*(udb + del); xubar = 0.5*(udb - del); xdbar = 0.5*(udb + del); xs = sb; xsbar = sb; xc = chm; xb = bot; // Subdivision of valence and sea. xuVal = uv; xuSea = xubar; xdVal = dv; xdSea = xdbar; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //-------------------------------------------------------------------------- double GRV94L::grvv (double x, double n, double ak, double bk, double a, double b, double c, double d) { double dx = sqrt(x); return n * pow(x, ak) * (1. + a * pow(x, bk) + x * (b + c * dx)) * pow(1. - x, d); } //-------------------------------------------------------------------------- double GRV94L::grvw (double x, double s, double al, double be, double ak, double bk, double a, double b, double c, double d, double e, double es) { double lx = log(1./x); return (pow(x, ak) * (a + x * (b + x * c)) * pow(lx, bk) + pow(s, al) * exp(-e + sqrt(es * pow(s, be) * lx))) * pow(1. - x, d); } //-------------------------------------------------------------------------- double GRV94L::grvs (double x, double s, double sth, double al, double be, double ak, double ag, double b, double d, double e, double es) { if(s <= sth) { return 0.; } else { double dx = sqrt(x); double lx = log(1./x); return pow(s - sth, al) / pow(lx, ak) * (1. + ag * dx + b * x) * pow(1. - x, d) * exp(-e + sqrt(es * pow(s, be) * lx)); } } //========================================================================== // Gives the CTEQ 5 L (leading order) parton distribution function set // in parametrized form. Parametrization by J. Pumplin. // Ref: CTEQ Collaboration, H.L. Lai et al., Eur.Phys.J. C12 (2000) 375. // The range of (x, Q) covered by this parametrization of the QCD // evolved parton distributions is 1E-6 < x < 1, 1.1 GeV < Q < 10 TeV. // In the current implementation, densities are frozen at borders. void CTEQ5L::xfUpdate(int , double x, double Q2) { // Constrain x and Q2 to range for which parametrization is valid. double Q = sqrt( max( 1., min( 1e8, Q2) ) ); x = max( 1e-6, min( 1.-1e-10, x) ); // Derived kinematical quantities. double y = - log(x); double u = log( x / 0.00001); double x1 = 1. - x; double x1L = log(1. - x); double sumUbarDbar = 0.; // Parameters of parametrizations. const double Qmin[8] = { 0., 0., 0., 0., 0., 0., 1.3, 4.5}; const double alpha[8] = { 0.2987216, 0.3407552, 0.4491863, 0.2457668, 0.5293999, 0.3713141, 0.03712017, 0.004952010 }; const double ut1[8] = { 4.971265, 2.612618, -0.4656819, 3.862583, 0.1895615, 3.753257, 4.400772, 5.562568 }; const double ut2[8] = { -1.105128, -1.258304e5, -274.2390, -1.265969, -3.069097, -1.113085, -1.356116, -1.801317 }; const double am[8][9][3] = { // d. { { 0.5292616E+01, -0.2751910E+01, -0.2488990E+01 }, { 0.9714424E+00, 0.1011827E-01, -0.1023660E-01 }, { -0.1651006E+02, 0.7959721E+01, 0.8810563E+01 }, { -0.1643394E+02, 0.5892854E+01, 0.9348874E+01 }, { 0.3067422E+02, 0.4235796E+01, -0.5112136E+00 }, { 0.2352526E+02, -0.5305168E+01, -0.1169174E+02 }, { -0.1095451E+02, 0.3006577E+01, 0.5638136E+01 }, { -0.1172251E+02, -0.2183624E+01, 0.4955794E+01 }, { 0.1662533E-01, 0.7622870E-02, -0.4895887E-03 } }, // u. { { 0.9905300E+00, -0.4502235E+00, 0.1624441E+00 }, { 0.8867534E+00, 0.1630829E-01, -0.4049085E-01 }, { 0.8547974E+00, 0.3336301E+00, 0.1371388E+00 }, { 0.2941113E+00, -0.1527905E+01, 0.2331879E+00 }, { 0.3384235E+02, 0.3715315E+01, 0.8276930E+00 }, { 0.6230115E+01, 0.3134639E+01, -0.1729099E+01 }, { -0.1186928E+01, -0.3282460E+00, 0.1052020E+00 }, { -0.8545702E+01, -0.6247947E+01, 0.3692561E+01 }, { 0.1724598E-01, 0.7120465E-02, 0.4003646E-04 } }, // g. { { 0.1193572E+03, -0.3886845E+01, -0.1133965E+01 }, { -0.9421449E+02, 0.3995885E+01, 0.1607363E+01 }, { 0.4206383E+01, 0.2485954E+00, 0.2497468E+00 }, { 0.1210557E+03, -0.3015765E+01, -0.1423651E+01 }, { -0.1013897E+03, -0.7113478E+00, 0.2621865E+00 }, { -0.1312404E+01, -0.9297691E+00, -0.1562531E+00 }, { 0.1627137E+01, 0.4954111E+00, -0.6387009E+00 }, { 0.1537698E+00, -0.2487878E+00, 0.8305947E+00 }, { 0.2496448E-01, 0.2457823E-02, 0.8234276E-03 } }, // ubar + dbar. { { 0.2647441E+02, 0.1059277E+02, -0.9176654E+00 }, { 0.1990636E+01, 0.8558918E-01, 0.4248667E-01 }, { -0.1476095E+02, -0.3276255E+02, 0.1558110E+01 }, { -0.2966889E+01, -0.3649037E+02, 0.1195914E+01 }, { -0.1000519E+03, -0.2464635E+01, 0.1964849E+00 }, { 0.3718331E+02, 0.4700389E+02, -0.2772142E+01 }, { -0.1872722E+02, -0.2291189E+02, 0.1089052E+01 }, { -0.1628146E+02, -0.1823993E+02, 0.2537369E+01 }, { -0.1156300E+01, -0.1280495E+00, 0.5153245E-01 } }, // dbar/ubar. { { -0.6556775E+00, 0.2490190E+00, 0.3966485E-01 }, { 0.1305102E+01, -0.1188925E+00, -0.4600870E-02 }, { -0.2371436E+01, 0.3566814E+00, -0.2834683E+00 }, { -0.6152826E+01, 0.8339877E+00, -0.7233230E+00 }, { -0.8346558E+01, 0.2892168E+01, 0.2137099E+00 }, { 0.1279530E+02, 0.1021114E+00, 0.5787439E+00 }, { 0.5858816E+00, -0.1940375E+01, -0.4029269E+00 }, { -0.2795725E+02, -0.5263392E+00, 0.1290229E+01 }, { 0.0000000E+00, 0.0000000E+00, 0.0000000E+00 } }, // sbar. { { 0.1580931E+01, -0.2273826E+01, -0.1822245E+01 }, { 0.2702644E+01, 0.6763243E+00, 0.7231586E-02 }, { -0.1857924E+02, 0.3907500E+01, 0.5850109E+01 }, { -0.3044793E+02, 0.2639332E+01, 0.5566644E+01 }, { -0.4258011E+01, -0.5429244E+01, 0.4418946E+00 }, { 0.3465259E+02, -0.5532604E+01, -0.4904153E+01 }, { -0.1658858E+02, 0.2923275E+01, 0.2266286E+01 }, { -0.1149263E+02, 0.2877475E+01, -0.7999105E+00 }, { 0.0000000E+00, 0.0000000E+00, 0.0000000E+00 } }, // cbar. { { -0.8293661E+00, -0.3982375E+01, -0.6494283E-01 }, { 0.2754618E+01, 0.8338636E+00, -0.6885160E-01 }, { -0.1657987E+02, 0.1439143E+02, -0.6887240E+00 }, { -0.2800703E+02, 0.1535966E+02, -0.7377693E+00 }, { -0.6460216E+01, -0.4783019E+01, 0.4913297E+00 }, { 0.3141830E+02, -0.3178031E+02, 0.7136013E+01 }, { -0.1802509E+02, 0.1862163E+02, -0.4632843E+01 }, { -0.1240412E+02, 0.2565386E+02, -0.1066570E+02 }, { 0.0000000E+00, 0.0000000E+00, 0.0000000E+00 } }, // bbar. { { -0.6031237E+01, 0.1992727E+01, -0.1076331E+01 }, { 0.2933912E+01, 0.5839674E+00, 0.7509435E-01 }, { -0.8284919E+01, 0.1488593E+01, -0.8251678E+00 }, { -0.1925986E+02, 0.2805753E+01, -0.3015446E+01 }, { -0.9480483E+01, -0.9767837E+00, -0.1165544E+01 }, { 0.2193195E+02, -0.1788518E+02, 0.9460908E+01 }, { -0.1327377E+02, 0.1201754E+02, -0.6277844E+01 }, { 0.0000000E+00, 0.0000000E+00, 0.0000000E+00 }, { 0.0000000E+00, 0.0000000E+00, 0.0000000E+00 } } }; // Loop over 8 different parametrizations. Check if inside allowed region. for (int i = 0; i < 8; ++i) { double answer = 0.; if (Q > max(Qmin[i], alpha[i])) { // Evaluate answer. double tmp = log(Q / alpha[i]); double sb = log(tmp); double sb1 = sb - 1.2; double sb2 = sb1*sb1; double af[9]; for (int j = 0; j < 9; ++j) af[j] = am[i][j][0] + sb1 * am[i][j][1] + sb2 * am[i][j][2]; double part1 = af[1] * pow( y, 1. + 0.01 * af[4]) * (1. + af[8] * u); double part2 = af[0] * x1 + af[3] * x; double part3 = x * x1 * (af[5] + af[6] * x1 + af[7] * x * x1); double part4 = (ut2[i] < -100.) ? ut1[i] * x1L + af[2] * x1L : ut1[i] * x1L + af[2] * log(x1 + exp(ut2[i])); answer = x * exp( part1 + part2 + part3 + part4); answer *= 1. - Qmin[i] / Q; } // Store results. if (i == 0) xd = x * answer; else if (i == 1) xu = x * answer; else if (i == 2) xg = x * answer; else if (i == 3) sumUbarDbar = x * answer; else if (i == 4) { xubar = sumUbarDbar / (1. + answer); xdbar = sumUbarDbar * answer / (1. + answer); } else if (i == 5) {xs = x * answer; xsbar = xs;} else if (i == 6) xc = x * answer; else if (i == 7) xb = x * answer; } // Subdivision of valence and sea. xuVal = xu - xubar; xuSea = xubar; xdVal = xd - xdbar; xdSea = xdbar; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //========================================================================== // The MSTWpdf class. // MSTW 2008 PDF's, specifically the LO one. // Original C++ version by Jeppe Andersen. // Modified by Graeme Watt . //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of parton flavours, x and Q2 grid points, // bins below c and b thresholds. const int MSTWpdf::np = 12; const int MSTWpdf::nx = 64; const int MSTWpdf::nq = 48; const int MSTWpdf::nqc0 = 4; const int MSTWpdf::nqb0 = 14; // Range of (x, Q2) grid. const double MSTWpdf::xmin = 1e-6; const double MSTWpdf::xmax = 1.0; const double MSTWpdf::qsqmin = 1.0; const double MSTWpdf::qsqmax = 1e9; // Array of x values. const double MSTWpdf::xxInit[65] = {0., 1e-6, 2e-6, 4e-6, 6e-6, 8e-6, 1e-5, 2e-5, 4e-5, 6e-5, 8e-5, 1e-4, 2e-4, 4e-4, 6e-4, 8e-4, 1e-3, 2e-3, 4e-3, 6e-3, 8e-3, 1e-2, 1.4e-2, 2e-2, 3e-2, 4e-2, 6e-2, 8e-2, 0.10, 0.125, 0.15, 0.175, 0.20, 0.225, 0.25, 0.275, 0.30, 0.325, 0.35, 0.375, 0.40, 0.425, 0.45, 0.475, 0.50, 0.525, 0.55, 0.575, 0.60, 0.625, 0.65, 0.675, 0.70, 0.725, 0.75, 0.775, 0.80, 0.825, 0.85, 0.875, 0.90, 0.925, 0.95, 0.975, 1.0 }; // Array of Q values. const double MSTWpdf::qqInit[49] = {0., 1.0, 1.25, 1.5, 0., 0., 2.5, 3.2, 4.0, 5.0, 6.4, 8.0, 10., 12., 0., 0., 26.0, 40.0, 64.0, 1e2, 1.6e2, 2.4e2, 4e2, 6.4e2, 1e3, 1.8e3, 3.2e3, 5.6e3, 1e4, 1.8e4, 3.2e4, 5.6e4, 1e5, 1.8e5, 3.2e5, 5.6e5, 1e6, 1.8e6, 3.2e6, 5.6e6, 1e7, 1.8e7, 3.2e7, 5.6e7, 1e8, 1.8e8, 3.2e8, 5.6e8, 1e9 }; //-------------------------------------------------------------------------- // Initialize PDF: read in data grid from file and set up interpolation. void MSTWpdf::init(int iFitIn, string xmlPath, Info* infoPtr) { // Choice of fit among possibilities. Counters and temporary variables. iFit = iFitIn; int i,n,m,k,l,j; double dtemp; // Variables used for initialising c_ij array: double f[np+1][nx+1][nq+1]; double f1[np+1][nx+1][nq+1]; // derivative w.r.t. x double f2[np+1][nx+1][nq+1]; // derivative w.r.t. q double f12[np+1][nx+1][nq+1];// cross derivative double f21[np+1][nx+1][nq+1];// cross derivative int wt[16][16]={{1,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0}, {0,0,0,0,0,0,0,0,1,0,0,0,0,0,0,0}, {-3,0,0,3,0,0,0,0,-2,0,0,-1,0,0,0,0}, {2,0,0,-2,0,0,0,0,1,0,0,1,0,0,0,0}, {0,0,0,0,1,0,0,0,0,0,0,0,0,0,0,0}, {0,0,0,0,0,0,0,0,0,0,0,0,1,0,0,0}, {0,0,0,0,-3,0,0,3,0,0,0,0,-2,0,0,-1}, {0,0,0,0,2,0,0,-2,0,0,0,0,1,0,0,1}, {-3,3,0,0,-2,-1,0,0,0,0,0,0,0,0,0,0}, {0,0,0,0,0,0,0,0,-3,3,0,0,-2,-1,0,0}, {9,-9,9,-9,6,3,-3,-6,6,-6,-3,3,4,2,1,2}, {-6,6,-6,6,-4,-2,2,4,-3,3,3,-3,-2,-1,-1,-2}, {2,-2,0,0,1,1,0,0,0,0,0,0,0,0,0,0}, {0,0,0,0,0,0,0,0,2,-2,0,0,1,1,0,0}, {-6,6,-6,6,-3,-3,3,3,-4,4,2,-2,-2,-2,-1,-1}, {4,-4,4,-4,2,2,-2,-2,2,-2,-2,2,1,1,1,1}}; double xxd,d1d2,cl[16],x[16],d1,d2,y[5],y1[5],y2[5],y12[5]; double mc2,mb2,eps=1e-6; // q^2 grid points at mc2+eps, mb2+eps // Select which data file to read for current fit. if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; string fileName = " "; if (iFit == 1) fileName = "mrstlostar.00.dat"; if (iFit == 2) fileName = "mrstlostarstar.00.dat"; if (iFit == 3) fileName = "mstw2008lo.00.dat"; if (iFit == 4) fileName = "mstw2008nlo.00.dat"; // Open data file. ifstream data_file( (xmlPath + fileName).c_str() ); if (!data_file.good()) { if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " "did not find parametrization file ", fileName); else cout << " Error from MSTWpdf::init: " << "did not find parametrization file " << fileName << endl; isSet = false; return; } // Read distance, tolerance, heavy quark masses // and alphaS values from file. char comma; int nExtraFlavours; data_file.ignore(256,'\n'); data_file.ignore(256,'\n'); data_file.ignore(256,'='); data_file >> distance >> tolerance; data_file.ignore(256,'='); data_file >> mCharm; data_file.ignore(256,'='); data_file >> mBottom; data_file.ignore(256,'='); data_file >> alphaSQ0; data_file.ignore(256,'='); data_file >> alphaSMZ; data_file.ignore(256,'='); data_file >> alphaSorder >> comma >> alphaSnfmax; data_file.ignore(256,'='); data_file >> nExtraFlavours; data_file.ignore(256,'\n'); data_file.ignore(256,'\n'); data_file.ignore(256,'\n'); // Use c and b quark masses for outlay of qq array. for (int iqq = 0; iqq < 49; ++iqq) qq[iqq] = qqInit[iqq]; mc2=mCharm*mCharm; mb2=mBottom*mBottom; qq[4]=mc2; qq[5]=mc2+eps; qq[14]=mb2; qq[15]=mb2+eps; // Check that the heavy quark masses are sensible. if (mc2 < qq[3] || mc2 > qq[6]) { if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " "invalid mCharm"); else cout << " Error from MSTWpdf::init: invalid mCharm" << endl; isSet = false; return; } if (mb2 < qq[13] || mb2 > qq[16]) { if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " "invalid mBottom"); else cout << " Error from MSTWpdf::init: invalid mBottom" << endl; isSet = false; return; } // The nExtraFlavours variable is provided to aid compatibility // with future grids where, for example, a photon distribution // might be provided (cf. the MRST2004QED PDFs). if (nExtraFlavours < 0 || nExtraFlavours > 1) { if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " "invalid nExtraFlavours"); else cout << " Error from MSTWpdf::init: invalid nExtraFlavours" << endl; isSet = false; return; } // Now read in the grids from the grid file. for (n=1;n<=nx-1;n++) for (m=1;m<=nq;m++) { for (i=1;i<=9;i++) data_file >> f[i][n][m]; if (alphaSorder==2) { // only at NNLO data_file >> f[10][n][m]; // = chm-cbar data_file >> f[11][n][m]; // = bot-bbar } else { f[10][n][m] = 0.; // = chm-cbar f[11][n][m] = 0.; // = bot-bbar } if (nExtraFlavours>0) data_file >> f[12][n][m]; // = photon else f[12][n][m] = 0.; // photon if (data_file.eof()) { if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " "failed to read in data file"); else cout << " Error from MSTWpdf::init: failed to read in data file" << endl; isSet = false; return; } } // Check that ALL the file contents have been read in. data_file >> dtemp; if (!data_file.eof()) { if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " "failed to read in data file"); else cout << " Error from MSTWpdf::init: failed to read in data file" << endl; isSet = false; return; } // Close the datafile. data_file.close(); // PDFs are identically zero at x = 1. for (i=1;i<=np;i++) for (m=1;m<=nq;m++) f[i][nx][m]=0.0; // Set up the new array in log10(x) and log10(qsq). for (i=1;i<=nx;i++) xx[i]=log10(xxInit[i]); for (m=1;m<=nq;m++) qq[m]=log10(qq[m]); // Now calculate the derivatives used for bicubic interpolation. for (i=1;i<=np;i++) { // Start by calculating the first x derivatives // along the first x value: for (m=1;m<=nq;m++) { f1[i][1][m]=polderivative1(xx[1],xx[2],xx[3],f[i][1][m],f[i][2][m], f[i][3][m]); // Then along the rest (up to the last): for (k=2;kpow(10.,qq[nqc0]) && qsqpow(10.,qq[nqb0]) && qsqxmax) return 0.; if (qsqqsqmax) { interpolate=0; } if (f==0) ip=1; else if (f>=1 && f<=5) ip=f+1; else if (f<=-1 && f>=-5) ip=-f+1; else if (f>=7 && f<=11) ip=f; else if (f==13) ip=12; else if (abs(f)==6 || f==12) return 0.; else return 0.; // Interpolation in log10(x), log10(qsq): xxx=log10(x); qqq=log10(qsq); if (interpolate==1) { // do usual interpolation parton_pdf=parton_interpolate(ip,xxx,qqq); if (f<=-1 && f>=-5) // antiquark = quark - valence parton_pdf -= parton_interpolate(ip+5,xxx,qqq); } else if (interpolate==-1) { // extrapolate to low Q^2 if (x=-5) { // antiquark = quark - valence parton_pdf -= parton_extrapolate(ip+5,xxx,log10(qsqmin)); parton_pdf1 -= parton_extrapolate(ip+5,xxx,log10(1.01*qsqmin)); } } else { // do usual interpolation parton_pdf = parton_interpolate(ip,xxx,log10(qsqmin)); parton_pdf1 = parton_interpolate(ip,xxx,log10(1.01*qsqmin)); if (f<=-1 && f>=-5) { // antiquark = quark - valence parton_pdf -= parton_interpolate(ip+5,xxx,log10(qsqmin)); parton_pdf1 -= parton_interpolate(ip+5,xxx,log10(1.01*qsqmin)); } } // Calculate the anomalous dimension, dlog(xf)/dlog(qsq), // evaluated at qsqmin. Then extrapolate the PDFs to low // qsq < qsqmin by interpolating the anomalous dimenion between // the value at qsqmin and a value of 1 for qsq << qsqmin. // If value of PDF at qsqmin is very small, just set // anomalous dimension to 1 to prevent rounding errors. if (fabs(parton_pdf) >= 1.e-5) anom = max(-2.5, (parton_pdf1-parton_pdf)/parton_pdf/0.01); else anom = 1.; parton_pdf = parton_pdf*pow(qsq/qsqmin,anom*qsq/qsqmin+1.-qsq/qsqmin); } else { // extrapolate outside PDF grid to low x or high Q^2 parton_pdf = parton_extrapolate(ip,xxx,qqq); if (f<=-1 && f>=-5) // antiquark = quark - valence parton_pdf -= parton_extrapolate(ip+5,xxx,qqq); } return parton_pdf; } //-------------------------------------------------------------------------- // Interpolate PDF value inside data grid. double MSTWpdf::parton_interpolate(int ip, double xxx, double qqq) { double g, t, u; int n, m, l; n=locate(xx,nx,xxx); // 0: below xmin, nx: above xmax m=locate(qq,nq,qqq); // 0: below qsqmin, nq: above qsqmax t=(xxx-xx[n])/(xx[n+1]-xx[n]); u=(qqq-qq[m])/(qq[m+1]-qq[m]); // Assume PDF proportional to (1-x)^p as x -> 1. if (n==nx-1) { double g0=((c[ip][n][m][1][4]*u+c[ip][n][m][1][3])*u +c[ip][n][m][1][2])*u+c[ip][n][m][1][1]; // value at xx[n] double g1=((c[ip][n-1][m][1][4]*u+c[ip][n-1][m][1][3])*u +c[ip][n-1][m][1][2])*u+c[ip][n-1][m][1][1]; // value at xx[n-1] double p = 1.0; if (g0>0.0&&g1>0.0) p = log(g1/g0)/log((xx[n+1]-xx[n-1])/(xx[n+1]-xx[n])); if (p<=1.0) p=1.0; g=g0*pow((xx[n+1]-xxx)/(xx[n+1]-xx[n]),p); } // Usual interpolation. else { g=0.0; for (l=4;l>=1;l--) { g=t*g+((c[ip][n][m][l][4]*u+c[ip][n][m][l][3])*u +c[ip][n][m][l][2])*u+c[ip][n][m][l][1]; } } return g; } //-------------------------------------------------------------------------- // Extrapolate PDF value outside data grid. double MSTWpdf::parton_extrapolate(int ip, double xxx, double qqq) { double parton_pdf=0.; int n,m; n=locate(xx,nx,xxx); // 0: below xmin, nx: above xmax m=locate(qq,nq,qqq); // 0: below qsqmin, nq: above qsqmax if (n==0&&(m>0&&m1e-3 && f1>1e-3 ) { // if values are positive, keep them so f0=log(f0); f1=log(f1); parton_pdf=exp(f0+(f1-f0)/(xx[2]-xx[1])*(xxx-xx[1])); } else // otherwise just extrapolate in the value parton_pdf=f0+(f1-f0)/(xx[2]-xx[1])*(xxx-xx[1]); } if (n>0&&m==nq) { // if extrapolation into large q only double f0,f1; f0=parton_interpolate(ip,xxx,qq[nq]); f1=parton_interpolate(ip,xxx,qq[nq-1]); if ( f0>1e-3 && f1>1e-3 ) { // if values are positive, keep them so f0=log(f0); f1=log(f1); parton_pdf=exp(f0+(f0-f1)/(qq[nq]-qq[nq-1])*(qqq-qq[nq])); } else // otherwise just extrapolate in the value parton_pdf=f0+(f0-f1)/(qq[nq]-qq[nq-1])*(qqq-qq[nq]); } if (n==0&&m==nq) { // if extrapolation into large q AND small x double f0,f1; f0=parton_extrapolate(ip,xx[1],qqq); f1=parton_extrapolate(ip,xx[2],qqq); if ( f0>1e-3 && f1>1e-3 ) { // if values are positive, keep them so f0=log(f0); f1=log(f1); parton_pdf=exp(f0+(f1-f0)/(xx[2]-xx[1])*(xxx-xx[1])); } else // otherwise just extrapolate in the value parton_pdf=f0+(f1-f0)/(xx[2]-xx[1])*(xxx-xx[1]); } return parton_pdf; } //-------------------------------------------------------------------------- // Returns an integer j such that x lies inbetween xloc[j] and xloc[j+1]. // unit offset of increasing ordered array xloc assumed. // n is the length of the array (xloc[n] highest element). int MSTWpdf::locate(double xloc[],int n,double x) { int ju,jm,jl(0),j; ju=n+1; while (ju-jl>1) { jm=(ju+jl)/2; // compute a mid point. if ( x>= xloc[jm]) jl=jm; else ju=jm; } if (x==xloc[1]) j=1; else if (x==xloc[n]) j=n-1; else j=jl; return j; } //-------------------------------------------------------------------------- // Returns the estimate of the derivative at x1 obtained by a polynomial // interpolation using the three points (x_i,y_i). double MSTWpdf::polderivative1(double x1, double x2, double x3, double y1, double y2, double y3) { return (x3*x3*(y1-y2)+2.0*x1*(x3*(-y1+y2)+x2*(y1-y3))+x2*x2*(-y1+y3) +x1*x1*(-y2+y3))/((x1-x2)*(x1-x3)*(x2-x3)); } //-------------------------------------------------------------------------- // Returns the estimate of the derivative at x2 obtained by a polynomial // interpolation using the three points (x_i,y_i). double MSTWpdf::polderivative2(double x1, double x2, double x3, double y1, double y2, double y3) { return (x3*x3*(y1-y2)-2.0*x2*(x3*(y1-y2)+x1*(y2-y3))+x2*x2*(y1-y3) +x1*x1*(y2-y3))/((x1-x2)*(x1-x3)*(x2-x3)); } //-------------------------------------------------------------------------- // Returns the estimate of the derivative at x3 obtained by a polynomial // interpolation using the three points (x_i,y_i). double MSTWpdf::polderivative3(double x1, double x2, double x3, double y1, double y2, double y3) { return (x3*x3*(-y1+y2)+2.0*x2*x3*(y1-y3)+x1*x1*(y2-y3)+x2*x2*(-y1+y3) +2.0*x1*x3*(-y2+y3))/((x1-x2)*(x1-x3)*(x2-x3)); } //========================================================================== // The CTEQ6pdf class. // Code for handling CTEQ6L, CTEQ6L1, CTEQ66.00, CT09MC1, CT09MC2, (CT09MCS?). // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Stay away from xMin, xMax, Qmin, Qmax limits. const double CTEQ6pdf::EPSILON = 1e-6; // Assumed approximate power of small-x behaviour for interpolation. const double CTEQ6pdf::XPOWER = 0.3; //-------------------------------------------------------------------------- // Initialize PDF: read in data grid from file. void CTEQ6pdf::init(int iFitIn, string xmlPath, Info* infoPtr) { // Choice of fit among possibilities. iFit = iFitIn; // Select which data file to read for current fit. if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; string fileName = " "; if (iFit == 1) fileName = "cteq6l.tbl"; if (iFit == 2) fileName = "cteq6l1.tbl"; if (iFit == 3) fileName = "ctq66.00.pds"; if (iFit == 4) fileName = "ct09mc1.pds"; if (iFit == 5) fileName = "ct09mc2.pds"; if (iFit == 6) fileName = "ct09mcs.pds"; bool isPdsGrid = (iFit > 2); // Open data file. ifstream pdfgrid( (xmlPath + fileName).c_str() ); if (!pdfgrid.good()) { if (infoPtr != 0) infoPtr->errorMsg("Error from CTEQ6pdf::init: " "did not find parametrization file ", fileName); else cout << " Error from CTEQ6pdf::init: " << "did not find parametrization file " << fileName << endl; isSet = false; return; } // Read in common information. int iDum; double orderTmp, nQTmp, qTmp, rDum; string line; getline( pdfgrid, line); getline( pdfgrid, line); getline( pdfgrid, line); istringstream is1(line); is1 >> orderTmp >> nQTmp >> lambda >> mQ[1] >> mQ[2] >> mQ[3] >> mQ[4] >> mQ[5] >> mQ[6]; order = int(orderTmp + 0.5); nQuark = int(nQTmp + 0.5); getline( pdfgrid, line); // Read in information for the .pds grid format. if (isPdsGrid) { getline( pdfgrid, line); istringstream is2(line); is2 >> iDum >> iDum >> iDum >> nfMx >> mxVal >> iDum; if (mxVal > 4) mxVal = 3; getline( pdfgrid, line); getline( pdfgrid, line); istringstream is3(line); is3 >> nX >> nT >> iDum >> nG >> iDum; for (int i = 0; i < nG + 2; ++i) getline( pdfgrid, line); getline( pdfgrid, line); istringstream is4(line); is4 >> qIni >> qMax; for (int iT = 0; iT <= nT; ++iT) { getline( pdfgrid, line); istringstream is5(line); is5 >> qTmp; tv[iT] = log( log( qTmp/lambda)); } getline( pdfgrid, line); getline( pdfgrid, line); istringstream is6(line); is6 >> xMin >> rDum; int nPackX = 6; xv[0] = 0.; for (int iXrng = 0; iXrng < int( (nX + nPackX - 1) / nPackX); ++iXrng) { getline( pdfgrid, line); istringstream is7(line); for (int iX = nPackX * iXrng + 1; iX <= nPackX * (iXrng + 1); ++iX) if (iX <= nX) is7 >> xv[iX]; } } // Read in information for the .tbl grid format. else { mxVal = 2; getline( pdfgrid, line); istringstream is2(line); is2 >> nX >> nT >> nfMx; getline( pdfgrid, line); getline( pdfgrid, line); istringstream is3(line); is3 >> qIni >> qMax; int nPackT = 6; for (int iTrng = 0; iTrng < int( (nT + nPackT) / nPackT); ++iTrng) { getline( pdfgrid, line); istringstream is4(line); for (int iT = nPackT * iTrng; iT < nPackT * (iTrng + 1); ++iT) if (iT <= nT) { is4 >> qTmp; tv[iT] = log( log( qTmp / lambda) ); } } getline( pdfgrid, line); getline( pdfgrid, line); istringstream is5(line); is5 >> xMin; int nPackX = 6; for (int iXrng = 0; iXrng < int( (nX + nPackX) / nPackX); ++iXrng) { getline( pdfgrid, line); istringstream is6(line); for (int iX = nPackX * iXrng; iX < nPackX * (iXrng + 1); ++iX) if (iX <= nX) is6 >> xv[iX]; } } // Read in the grid proper. getline( pdfgrid, line); int nBlk = (nX + 1) * (nT + 1); int nPts = nBlk * (nfMx + 1 + mxVal); int nPack = (isPdsGrid) ? 6 : 5; for (int iRng = 0; iRng < int( (nPts + nPack - 1) / nPack); ++iRng) { getline( pdfgrid, line); istringstream is8(line); for (int i = nPack * iRng + 1; i <= nPack * (iRng + 1); ++i) if (i <= nPts) is8 >> upd[i]; } // Initialize x grid mapped to x^0.3. xvpow[0] = 0.; for (int iX = 1; iX <= nX; ++iX) xvpow[iX] = pow(xv[iX], XPOWER); // Set x and Q borders with some margin. xMinEps = xMin * (1. + EPSILON); xMaxEps = 1. - EPSILON; qMinEps = qIni * (1. + EPSILON); qMaxEps = qMax * (1. - EPSILON); // Initialize (x, Q) values of previous call. xLast = 0.; qLast = 0.; } //-------------------------------------------------------------------------- // Update PDF values. void CTEQ6pdf::xfUpdate(int , double x, double Q2) { // Update using CTEQ6 routine, within allowed (x, q) range. double xEps = max( xMinEps, x); double qEps = max( qMinEps, min( qMaxEps, sqrtpos(Q2) ) ); // Gluon: double glu = xEps * parton6( 0, xEps, qEps); // Sea quarks (note wrong order u, d): double bot = xEps * parton6( 5, xEps, qEps); double chm = xEps * parton6( 4, xEps, qEps); double str = xEps * parton6( 3, xEps, qEps); double usea = xEps * parton6(-1, xEps, qEps); double dsea = xEps * parton6(-2, xEps, qEps); // Valence quarks: double upv = xEps * parton6( 1, xEps, qEps) - usea; double dnv = xEps * parton6( 2, xEps, qEps) - dsea; // Transfer to Pythia notation. xg = glu; xu = upv + usea; xd = dnv + dsea; xubar = usea; xdbar = dsea; xs = str; xsbar = str; xc = chm; xb = bot; xgamma = 0.; // Subdivision of valence and sea. xuVal = upv; xuSea = usea; xdVal = dnv; xdSea = dsea; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //-------------------------------------------------------------------------- // Returns the PDF value for parton of flavour iParton at x, q. double CTEQ6pdf::parton6(int iParton, double x, double q) { // Put zero for large x. Parton table and interpolation variables. if (x > xMaxEps) return 0.; int iP = (iParton > mxVal) ? -iParton : iParton; double ss = pow( x, XPOWER); double tt = log( log(q / lambda) ); // Find location in grid.Skip if same as in latest call. if (x != xLast || q != qLast) { // Binary search in x grid. iGridX = 0; iGridLX = -1; int ju = nX + 1; int jm = 0; while (ju - iGridLX > 1 && jm >= 0) { jm = (ju + iGridLX) / 2; if (x >= xv[jm]) iGridLX = jm; else ju = jm; } // Separate acceptable from unacceptable grid points. if (iGridLX <= -1) return 0.; else if (iGridLX == 0) iGridX = 0; else if (iGridLX <= nX - 2) iGridX = iGridLX - 1; else if (iGridLX == nX - 1) iGridX = iGridLX - 2; else return 0.; // Expressions for interpolation in x Grid. if (iGridLX > 1 && iGridLX < nX - 1) { double svec1 = xvpow[iGridX]; double svec2 = xvpow[iGridX+1]; double svec3 = xvpow[iGridX+2]; double svec4 = xvpow[iGridX+3]; double s12 = svec1 - svec2; double s13 = svec1 - svec3; xConst[8] = svec2 - svec3; double s24 = svec2 - svec4; double s34 = svec3 - svec4; xConst[6] = ss - svec2; xConst[7] = ss - svec3; xConst[0] = s13 / xConst[8]; xConst[1] = s12 / xConst[8]; xConst[2] = s34 / xConst[8]; xConst[3] = s24 / xConst[8]; double s1213 = s12 + s13; double s2434 = s24 + s34; double sdet = s12 * s34 - s1213 * s2434; double tmp = xConst[6] * xConst[7] / sdet; xConst[4] = (s34 * xConst[6] - s2434 * xConst[7]) * tmp / s12; xConst[5] = (s1213 * xConst[6] - s12 * xConst[7]) * tmp / s34; } // Binary search in Q grid. iGridQ = 0; iGridLQ = -1; ju = nT + 1; jm = 0; while (ju - iGridLQ > 1 && jm >= 0) { jm = (ju + iGridLQ) / 2; if (tt >= tv[jm]) iGridLQ = jm; else ju = jm; } if (iGridLQ == 0) iGridQ = 0; else if (iGridLQ <= nT - 2) iGridQ = iGridLQ - 1; else iGridQ = nT - 3; // Expressions for interpolation in Q Grid. if (iGridLQ > 0 && iGridLQ < nT - 1) { double tvec1 = tv[iGridQ]; double tvec2 = tv[iGridQ+1]; double tvec3 = tv[iGridQ+2]; double tvec4 = tv[iGridQ+3]; double t12 = tvec1 - tvec2; double t13 = tvec1 - tvec3; tConst[8] = tvec2 - tvec3; double t24 = tvec2 - tvec4; double t34 = tvec3 - tvec4; tConst[6] = tt - tvec2; tConst[7] = tt - tvec3; double tmp1 = t12 + t13; double tmp2 = t24 + t34; double tdet = t12 * t34 - tmp1 * tmp2; tConst[0] = t13 / tConst[8]; tConst[1] = t12 / tConst[8]; tConst[2] = t34 / tConst[8]; tConst[3] = t24 / tConst[8]; tConst[4] = (t34 * tConst[6] - tmp2 * tConst[7]) / t12 * tConst[6] * tConst[7] / tdet; tConst[5] = (tmp1 * tConst[6] - t12 * tConst[7]) / t34 * tConst[6] * tConst[7] / tdet; } // Save x and q values so do not have to redo same again. xLast = x; qLast = q; } // Jump to here if x and q are the same as for the last call. int jtmp = ( (iP + nfMx) * (nT + 1) + (iGridQ - 1) ) * (nX + 1) + iGridX + 1; // Interpolate in x space for four different q values. for(int it = 1; it <= 4; ++it) { int j1 = jtmp + it * (nX + 1); if (iGridX == 0) { double fij[5]; fij[1] = 0.; fij[2] = upd[j1+1] * pow2(xv[1]); fij[3] = upd[j1+2] * pow2(xv[2]); fij[4] = upd[j1+3] * pow2(xv[3]); double fX = polint4F( &xvpow[0], &fij[1], ss); fVec[it] = (x > 0.) ? fX / pow2(x) : 0.; } else if (iGridLX==nX-1) { fVec[it] = polint4F( &xvpow[nX-3], &upd[j1], ss); } else { double sf2 = upd[j1+1]; double sf3 = upd[j1+2]; double g1 = sf2 * xConst[0] - sf3 * xConst[1]; double g4 = -sf2 * xConst[2] + sf3 * xConst[3]; fVec[it] = (xConst[4] * (upd[j1] - g1) + xConst[5] * (upd[j1+3] - g4) + sf2 * xConst[7] - sf3 * xConst[6]) / xConst[8]; } } // Interpolate in q space for x-interpolated values found above. double ff; if( iGridLQ <= 0 ) { ff = polint4F( &tv[0], &fVec[1], tt); } else if (iGridLQ >= nT - 1) { ff=polint4F( &tv[nT-3], &fVec[1], tt); } else { double tf2 = fVec[2]; double tf3 = fVec[3]; double g1 = tf2 * tConst[0] - tf3 * tConst[1]; double g4 = -tf2 * tConst[2] + tf3 * tConst[3]; ff = (tConst[4] * (fVec[1] - g1) + tConst[5] * (fVec[4] - g4) + tf2 * tConst[7] - tf3 * tConst[6]) / tConst[8]; } // Done. return ff; } //-------------------------------------------------------------------------- // The POLINT4 routine is based on the POLINT routine from "Numerical Recipes", // but assuming N=4, and ignoring the error estimation. // Suggested by Z. Sullivan. double CTEQ6pdf::polint4F(double xa[],double ya[],double x) { double y, h1, h2, h3, h4, w, den, d1, c1, d2, c2, d3, c3, cd1, cc1, cd2, cc2, dd1, dc1; h1 = xa[0] - x; h2 = xa[1] - x; h3 = xa[2] - x; h4 = xa[3] - x; w = ya[1] - ya[0]; den = w / (h1 - h2); d1 = h2 * den; c1 = h1 * den; w = ya[2] - ya[1]; den = w / (h2 - h3); d2 = h3 * den; c2 = h2 * den; w = ya[3] - ya[2]; den = w / (h3 - h4); d3 = h4 * den; c3 = h3 * den; w = c2 - d1; den = w / (h1 - h3); cd1 = h3 * den; cc1 = h1 * den; w = c3 - d2; den = w / (h2 - h4); cd2 = h4 * den; cc2 = h2 * den; w = cc2 - cd1; den = w / (h1 - h4); dd1 = h4 * den; dc1 = h1 * den; if (h3 + h4 < 0.) y = ya[3] + d3 + cd2 + dd1; else if (h2 + h3 < 0.) y = ya[2] + d2 + cd1 + dc1; else if (h1 + h2 < 0.) y = ya[1] + c2 + cd1 + dc1; else y = ya[0] + c1 + cc1 + dc1; return y; } //========================================================================== // SA Unresolved proton: equivalent photon spectrum from // V.M. Budnev, I.F. Ginzburg, G.V. Meledin and V.G. Serbo, // Phys. Rept. 15 (1974/1975) 181. // Constants: const double ProtonPoint::ALPHAEM = 0.00729735; const double ProtonPoint::Q2MAX = 2.0; const double ProtonPoint::Q20 = 0.71; const double ProtonPoint::A = 7.16; const double ProtonPoint::B = -3.96; const double ProtonPoint::C = 0.028; //-------------------------------------------------------------------------- // Gives a generic Q2-independent equivalent photon spectrum. void ProtonPoint::xfUpdate(int , double x, double /*Q2*/ ) { // Photon spectrum double tmpQ2Min = 0.88 * pow2(x); double phiMax = phiFunc(x, Q2MAX / Q20); double phiMin = phiFunc(x, tmpQ2Min / Q20); double fgm = 0; if (phiMax < phiMin && m_infoPtr != 0) { m_infoPtr->errorMsg("Error from ProtonPoint::xfUpdate: " "phiMax - phiMin < 0!"); } else { // Corresponds to: x*f(x) fgm = (ALPHAEM / M_PI) * (1 - x) * (phiMax - phiMin); } // Update values xg = 0.; xu = 0.; xd = 0.; xubar = 0.; xdbar = 0.; xs = 0.; xsbar = 0.; xc = 0.; xb = 0.; xgamma = fgm; // Subdivision of valence and sea. xuVal = 0.; xuSea = 0; xdVal = 0.; xdSea = 0; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //-------------------------------------------------------------------------- // Function related to Q2 integration. double ProtonPoint::phiFunc(double x, double Q) { double tmpV = 1. + Q; double tmpSum1 = 0; double tmpSum2 = 0; for (int k=1; k<4; ++k) { tmpSum1 += 1. / (k * pow(tmpV, k)); tmpSum2 += pow(B, k) / (k * pow(tmpV, k)); } double tmpY = pow2(x) / (1 - x); double funVal = (1 + A * tmpY) * (-1.*log(tmpV / Q) + tmpSum1) + (1 - B) * tmpY / (4 * Q * pow(tmpV, 3)) + C * (1 + tmpY/4.)* (log((tmpV - B)/tmpV) + tmpSum2); return funVal; } //========================================================================== // Gives the GRV 1992 pi+ (leading order) parton distribution function set // in parametrized form. Authors: Glueck, Reya and Vogt. // Ref: M. Glueck, E. Reya and A. Vogt, Z. Phys. C53 (1992) 651. // Allowed variable range: 0.25 GeV^2 < Q^2 < 10^8 GeV^2 and 10^-5 < x < 1. void GRVpiL::xfUpdate(int , double x, double Q2) { // Common expressions. Constrain Q2 for which parametrization is valid. double mu2 = 0.25; double lam2 = 0.232 * 0.232; double s = (Q2 > mu2) ? log( log(Q2/lam2) / log(mu2/lam2) ) : 0.; double s2 = s * s; double x1 = 1. - x; double xL = -log(x); double xS = sqrt(x); // uv, dbarv. double uv = (0.519 + 0.180 * s - 0.011 * s2) * pow(x, 0.499 - 0.027 * s) * (1. + (0.381 - 0.419 * s) * xS) * pow(x1, 0.367 + 0.563 * s); // g. double gl = ( pow(x, 0.482 + 0.341 * sqrt(s)) * ( (0.678 + 0.877 * s - 0.175 * s2) + (0.338 - 1.597 * s) * xS + (-0.233 * s + 0.406 * s2) * x) + pow(s, 0.599) * exp(-(0.618 + 2.070 * s) + sqrt(3.676 * pow(s, 1.263) * xL) ) ) * pow(x1, 0.390 + 1.053 * s); // sea: u, d, s. double ub = pow(s, 0.55) * (1. - 0.748 * xS + (0.313 + 0.935 * s) * x) * pow(x1, 3.359) * exp(-(4.433 + 1.301 * s) + sqrt((9.30 - 0.887 * s) * pow(s, 0.56) * xL) ) / pow(xL, 2.538 - 0.763 * s); // c. double chm = (s < 0.888) ? 0. : pow(s - 0.888, 1.02) * (1. + 1.008 * x) * pow(x1, 1.208 + 0.771 * s) * exp(-(4.40 + 1.493 * s) + sqrt( (2.032 + 1.901 * s) * pow(s, 0.39) * xL) ); // b. double bot = (s < 1.351) ? 0. : pow(s - 1.351, 1.03) * pow(x1, 0.697 + 0.855 * s) * exp(-(4.51 + 1.490 * s) + sqrt( (3.056 + 1.694 * s) * pow(s, 0.39) * xL) ); // Update values. xg = gl; xu = uv + ub; xd = ub; xubar = ub; xdbar = uv + ub; xs = ub; xsbar = ub; xc = chm; xb = bot; // Subdivision of valence and sea. xuVal = uv; xuSea = ub; xdVal = uv; xdSea = ub; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //========================================================================== // Pomeron PDF: simple Q2-independent parametrizations N x^a (1 - x)^b. //-------------------------------------------------------------------------- // Calculate normalization factors once and for all. void PomFix::init() { normGluon = GammaReal(PomGluonA + PomGluonB + 2.) / (GammaReal(PomGluonA + 1.) * GammaReal(PomGluonB + 1.)); normQuark = GammaReal(PomQuarkA + PomQuarkB + 2.) / (GammaReal(PomQuarkA + 1.) * GammaReal(PomQuarkB + 1.)); } //-------------------------------------------------------------------------- // Gives a generic Q2-independent Pomeron PDF. void PomFix::xfUpdate(int , double x, double) { // Gluon and quark distributions. double gl = normGluon * pow(x, PomGluonA) * pow( (1. - x), PomGluonB); double qu = normQuark * pow(x, PomQuarkA) * pow( (1. - x), PomQuarkB); // Update values xg = (1. - PomQuarkFrac) * gl; xu = (PomQuarkFrac / (4. + 2. * PomStrangeSupp) ) * qu; xd = xu; xubar = xu; xdbar = xu; xs = PomStrangeSupp * xu; xsbar = xs; xc = 0.; xb = 0.; // Subdivision of valence and sea. xuVal = 0.; xuSea = xu; xdVal = 0.; xdSea = xd; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //========================================================================== // Pomeron PDF: the H1 2006 Fit A and Fit B Q2-dependent parametrizations. //-------------------------------------------------------------------------- void PomH1FitAB::init( int iFit, string xmlPath, Info* infoPtr) { // Open files from which grids should be read in. if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; string dataFile = "pomH1FitBlo.data"; if (iFit == 1) dataFile = "pomH1FitA.data"; if (iFit == 2) dataFile = "pomH1FitB.data"; ifstream is( (xmlPath + dataFile).c_str() ); if (!is.good()) { if (infoPtr != 0) infoPtr->errorMsg("Error from PomH1FitAB::init: " "the H1 Pomeron parametrization file was not found"); else cout << " Error from PomH1FitAB::init: " << "the H1 Pomeron parametrization file was not found" << endl; isSet = false; return; } // Lower and upper bounds. Bin widths for logarithmic spacing. nx = 100; xlow = 0.001; xupp = 0.99; dx = log(xupp / xlow) / (nx - 1.); nQ2 = 30; Q2low = 1.0; Q2upp = 30000.; dQ2 = log(Q2upp / Q2low) / (nQ2 - 1.); // Read in quark data grid. for (int i = 0; i < nx; ++i) for (int j = 0; j < nQ2; ++j) is >> quarkGrid[i][j]; // Read in gluon data grid. for (int i = 0; i < nx; ++i) for (int j = 0; j < nQ2; ++j) is >> gluonGrid[i][j]; // Check for errors during read-in of file. if (!is) { if (infoPtr != 0) infoPtr->errorMsg("Error from PomH1FitAB::init: " "the H1 Pomeron parametrization files could not be read"); else cout << " Error from PomH1FitAB::init: " << "the H1 Pomeron parametrization files could not be read" << endl; isSet = false; return; } // Done. isSet = true; return; } //-------------------------------------------------------------------------- void PomH1FitAB::xfUpdate(int , double x, double Q2) { // Retrict input to validity range. double xt = min( xupp, max( xlow, x) ); double Q2t = min( Q2upp, max( Q2low, Q2) ); // Lower grid point and distance above it. double dlx = log( xt / xlow) / dx; int i = min( nx - 2, int(dlx) ); dlx -= i; double dlQ2 = log( Q2t / Q2low) / dQ2; int j = min( nQ2 - 2, int(dlQ2) ); dlQ2 -= j; // Interpolate to derive quark PDF. double qu = (1. - dlx) * (1. - dlQ2) * quarkGrid[i][j] + dlx * (1. - dlQ2) * quarkGrid[i + 1][j] + (1. - dlx) * dlQ2 * quarkGrid[i][j + 1] + dlx * dlQ2 * quarkGrid[i + 1][j + 1]; // Interpolate to derive gluon PDF. double gl = (1. - dlx) * (1. - dlQ2) * gluonGrid[i][j] + dlx * (1. - dlQ2) * gluonGrid[i + 1][j] + (1. - dlx) * dlQ2 * gluonGrid[i][j + 1] + dlx * dlQ2 * gluonGrid[i + 1][j + 1]; // Update values. xg = rescale * gl; xu = rescale * qu; xd = xu; xubar = xu; xdbar = xu; xs = xu; xsbar = xu; xc = 0.; xb = 0.; // Subdivision of valence and sea. xuVal = 0.; xuSea = xu; xdVal = 0.; xdSea = xu; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //========================================================================== // Pomeron PDF: the H1 2007 Jets Q2-dependent parametrization. //-------------------------------------------------------------------------- void PomH1Jets::init( string xmlPath, Info* infoPtr) { // Open files from which grids should be read in. if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; ifstream isg( (xmlPath + "pomH1JetsGluon.data").c_str() ); ifstream isq( (xmlPath + "pomH1JetsSinglet.data").c_str() ); ifstream isc( (xmlPath + "pomH1JetsCharm.data").c_str() ); if (!isg.good() || !isq.good() || !isc.good()) { if (infoPtr != 0) infoPtr->errorMsg("Error from PomH1Jets::init: " "the H1 Pomeron parametrization files were not found"); else cout << " Error from PomH1Jets::init: " << "the H1 Pomeron parametrization files were not found" << endl; isSet = false; return; } // Read in x and Q grids. Do interpolation logarithmically in Q2. for (int i = 0; i < 100; ++i) { isg >> setw(13) >> xGrid[i]; } for (int j = 0; j < 88; ++j) { isg >> setw(13) >> Q2Grid[j]; Q2Grid[j] = log( Q2Grid[j] ); } // Read in gluon data grid. for (int j = 0; j < 88; ++j) { for (int i = 0; i < 100; ++i) { isg >> setw(13) >> gluonGrid[i][j]; } } // Identical x and Q2 grid for singlet, so skip ahead. double dummy; for (int i = 0; i < 188; ++i) isq >> setw(13) >> dummy; // Read in singlet data grid. for (int j = 0; j < 88; ++j) { for (int i = 0; i < 100; ++i) { isq >> setw(13) >> singletGrid[i][j]; } } // Identical x and Q2 grid for charm, so skip ahead. for (int i = 0; i < 188; ++i) isc >> setw(13) >> dummy; // Read in charm data grid. for (int j = 0; j < 88; ++j) { for (int i = 0; i < 100; ++i) { isc >> setw(13) >> charmGrid[i][j]; } } // Check for errors during read-in of files. if (!isg || !isq || !isc) { if (infoPtr != 0) infoPtr->errorMsg("Error from PomH1Jets::init: " "the H1 Pomeron parametrization files could not be read"); else cout << " Error from PomH1Jets::init: " << "the H1 Pomeron parametrization files could not be read" << endl; isSet = false; return; } // Done. isSet = true; return; } //-------------------------------------------------------------------------- void PomH1Jets::xfUpdate(int , double x, double Q2) { // Find position in x array. double xLog = log(x); int i = 0; double dx = 0.; if (xLog <= xGrid[0]); else if (xLog >= xGrid[99]) { i = 98; dx = 1.; } else { while (xLog > xGrid[i]) ++i; --i; dx = (xLog - xGrid[i]) / (xGrid[i + 1] - xGrid[i]); } // Find position in y array. double Q2Log = log(Q2); int j = 0; double dQ2 = 0.; if (Q2Log <= Q2Grid[0]); else if (Q2Log >= Q2Grid[87]) { j = 86; dQ2 = 1.; } else { while (Q2Log > Q2Grid[j]) ++j; --j; dQ2 = (Q2Log - Q2Grid[j]) / (Q2Grid[j + 1] - Q2Grid[j]); } // Interpolate to derive gluon PDF. double gl = (1. - dx) * (1. - dQ2) * gluonGrid[i][j] + dx * (1. - dQ2) * gluonGrid[i + 1][j] + (1. - dx) * dQ2 * gluonGrid[i][j + 1] + dx * dQ2 * gluonGrid[i + 1][j + 1]; // Interpolate to derive singlet PDF. (Sum of u, d, s, ubar, dbar, sbar.) double sn = (1. - dx) * (1. - dQ2) * singletGrid[i][j] + dx * (1. - dQ2) * singletGrid[i + 1][j] + (1. - dx) * dQ2 * singletGrid[i][j + 1] + dx * dQ2 * singletGrid[i + 1][j + 1]; // Interpolate to derive charm PDF. (Charge-square times c and cbar.) double ch = (1. - dx) * (1. - dQ2) * charmGrid[i][j] + dx * (1. - dQ2) * charmGrid[i + 1][j] + (1. - dx) * dQ2 * charmGrid[i][j + 1] + dx * dQ2 * charmGrid[i + 1][j + 1]; // Update values. xg = rescale * gl; xu = rescale * sn / 6.; xd = xu; xubar = xu; xdbar = xu; xs = xu; xsbar = xu; xc = rescale * ch * 9./8.; xb = 0.; // Subdivision of valence and sea. xuVal = 0.; xuSea = xu; xdVal = 0.; xdSea = xd; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //========================================================================== // Gives electron (or muon, or tau) parton distribution. // Constants: alphaEM(0), m_e, m_mu, m_tau. const double Lepton::ALPHAEM = 0.00729735; const double Lepton::ME = 0.0005109989; const double Lepton::MMU = 0.10566; const double Lepton::MTAU = 1.77699; void Lepton::xfUpdate(int id, double x, double Q2) { // Squared mass of lepton species: electron, muon, tau. if (!isInit) { double mLep = ME; if (abs(id) == 13) mLep = MMU; if (abs(id) == 15) mLep = MTAU; m2Lep = pow2( mLep ); isInit = true; } // Electron inside electron, see R. Kleiss et al., in Z physics at // LEP 1, CERN 89-08, p. 34 double xLog = log(max(1e-10,x)); double xMinusLog = log( max(1e-10, 1. - x) ); double Q2Log = log( max(3., Q2/m2Lep) ); double beta = (ALPHAEM / M_PI) * (Q2Log - 1.); double delta = 1. + (ALPHAEM / M_PI) * (1.5 * Q2Log + 1.289868) + pow2(ALPHAEM / M_PI) * (-2.164868 * Q2Log*Q2Log + 9.840808 * Q2Log - 10.130464); double fPrel = beta * pow(1. - x, beta - 1.) * sqrtpos( delta ) - 0.5 * beta * (1. + x) + 0.125 * beta*beta * ( (1. + x) * (-4. * xMinusLog + 3. * xLog) - 4. * xLog / (1. - x) - 5. - x); // Zero distribution for very large x and rescale it for intermediate. if (x > 1. - 1e-10) fPrel = 0.; else if (x > 1. - 1e-7) fPrel *= pow(1000.,beta) / (pow(1000.,beta) - 1.); xlepton = x * fPrel; // Photon inside electron (one possible scheme - primitive). xgamma = (0.5 * ALPHAEM / M_PI) * Q2Log * (1. + pow2(1. - x)); // idSav = 9 to indicate that all flavours reset. idSav = 9; } //========================================================================== // The NNPDF class. // Code for handling NNPDF2.3 QCD+QED LO // Code provided by Juan Rojo and Stefano Carrazza. //-------------------------------------------------------------------------- // Freeze PDFs below XMINGRID const double NNPDF::fXMINGRID = 1e-7; //-------------------------------------------------------------------------- // Initialize PDF: read in data grid from file. void NNPDF::init(int iFitIn, string xmlPath, Info* infoPtr) { // Choice of fit among possibilities. iFit = iFitIn; // Select which data file to read for current fit. if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; string fileName = " "; // NNPDF2.3 LO QCD+QED, for two values of alphas if (iFit == 1) fileName = "NNPDF23_lo_as_0130_qed.grid"; if (iFit == 2) fileName = "NNPDF23_lo_as_0119_qed.grid"; // NNPDF2.3 NLO QCD+QED if (iFit == 3) fileName = "NNPDF23_nlo_as_0119_qed.grid"; // NNPDF2.4 NLO QCD+QED if (iFit == 4) fileName = "NNPDF23_nnlo_as_0119_qed.grid"; // Open data file. fstream f; f.open( (xmlPath + fileName).c_str(),ios::in); if (f.fail()) { if (infoPtr != 0) infoPtr->errorMsg("Error from NNPDF::init: " "did not find data file ", fileName); else cout << "Error: cannot open file " << (xmlPath + fileName) << endl; isSet = false; return; } // Reading grid: removing header. string tmp; for (;;) { getline(f,tmp); if (tmp.find("NNPDF20intqed") != string::npos) { getline(f,tmp); break; } } // Get nx and x grid. f >> fNX; fXGrid = new double[fNX]; for (int ix = 0; ix < fNX; ix++) f >> fXGrid[ix]; fLogXGrid = new double[fNX]; for (int ix = 0; ix < fNX; ix++) fLogXGrid[ix] = log(fXGrid[ix]); // Get nQ2 and Q2 grid (ignorming first value). f >> fNQ2; f >> tmp; fQ2Grid = new double[fNQ2]; for (int iq = 0; iq < fNQ2; iq++) f >> fQ2Grid[iq]; fLogQ2Grid = new double[fNQ2]; for (int iq = 0; iq < fNQ2; iq++) fLogQ2Grid[iq] = log(fQ2Grid[iq]); // Prepare grid array. fPDFGrid = new double**[fNFL]; for (int i = 0; i < fNFL; i++) { fPDFGrid[i] = new double*[fNX]; for (int j = 0; j < fNX; j++) { fPDFGrid[i][j] = new double[fNQ2]; for (int z = 0; z < fNQ2; z++) fPDFGrid[i][j][z] = 0.0; } } // Check values of number of grid entries. if (fNX<= 0 || fNX>100 || fNQ2<=0 || fNQ2>50) { cout << "Error in NNPDF::init, Invalid grid values" << endl << "fNX = " << fNX << endl << "fNQ2 = " << fNQ2 << endl << "fNFL = " <> tmp; for (int ix = 0; ix < fNX; ix++) for (int iq = 0; iq < fNQ2; iq++) for (int fl = 0; fl < fNFL; fl++) f >> fPDFGrid[fl][ix][iq]; f.close(); // Other vectors. fRes = new double[fNFL]; } //-------------------------------------------------------------------------- void NNPDF::xfUpdate(int , double x, double Q2) { // Update using NNPDF routine, within allowed (x, q) range. xfxevolve(x,Q2); // Then transfer to Pythia8 notation. xg = fRes[6]; xu = fRes[8]; xd = fRes[7]; xubar = fRes[4]; xdbar = fRes[5]; xs = fRes[9]; xsbar = fRes[3]; xc = fRes[10]; xb = fRes[11]; xgamma = fRes[13]; // Subdivision of valence and sea. xuVal = xu - xubar; xuSea = xubar; xdVal = xd - xdbar; xdSea = xdbar; // idSav = 9 to indicate that all flavours reset. idSav = 9; } //-------------------------------------------------------------------------- void NNPDF::xfxevolve(double x, double Q2) { // Freeze outside x-Q2 grid. if (x < fXMINGRID || x > fXGrid[fNX-1]) { if (x < fXMINGRID) x = fXMINGRID; if (x > fXGrid[fNX-1]) x = fXGrid[fNX-1]; } if (Q2 < fQ2Grid[0] || Q2 > fQ2Grid[fNQ2-1]) { if (Q2 < fQ2Grid[0]) Q2 = fQ2Grid[0]; if (Q2 > fQ2Grid[fNQ2-1]) Q2 = fQ2Grid[fNQ2-1]; } // Find nearest points in the x-Q2 grid. int minx = 0; int maxx = fNX; while (maxx-minx > 1) { int midx = (minx+maxx)/2; if (x < fXGrid[midx]) maxx = midx; else minx = midx; } int ix = minx; int minq = 0; int maxq = fNQ2; while (maxq-minq > 1) { int midq = (minq+maxq)/2; if (Q2 < fQ2Grid[midq]) maxq = midq; else minq = midq; } int iq2 = minq; // Assign grid for interpolation. M,N -> order of polyN interpolation. int ix1a[fM], ix2a[fN]; double x1a[fM], x2a[fN]; double ya[fM][fN]; for (int i = 0; i < fM; i++) { if (ix+1 >= fM/2 && ix+1 <= (fNX-fM/2)) ix1a[i] = ix+1 - fM/2 + i; if (ix+1 < fM/2) ix1a[i] = i; if (ix+1 > (fNX-fM/2)) ix1a[i] = (fNX-fM) + i; // Check grids. if (ix1a[i] < 0 || ix1a[i] >= fNX) { cout << "Error in grids! i, ixia[i] = " << i << "\t" << ix1a[i] << endl; return; } } for (int j = 0; j < fN; j++) { if (iq2+1 >= fN/2 && iq2+1 <= (fNQ2-fN/2)) ix2a[j] = iq2+1 - fN/2 + j; if (iq2+1 < fN/2) ix2a[j] = j; if (iq2+1 > (fNQ2-fN/2)) ix2a[j] = (fNQ2-fN) + j; // Check grids. if (ix2a[j] < 0 || ix2a[j] >= fNQ2) { cout << "Error in grids! j, ix2a[j] = " << j << "\t" << ix2a[j] << endl; return; } } const double xch = 1e-1; double x1; if (x < xch) x1 = log(x); else x1 = x; double x2 = log(Q2); for (int ipdf = 0; ipdf < fNFL; ipdf++) { fRes[ipdf] = 0.0; for (int i = 0; i < fM; i++) { if (x < xch) x1a[i] = fLogXGrid[ix1a[i]]; else x1a[i] = fXGrid[ix1a[i]]; for (int j = 0; j < fN; j++) { x2a[j] = fLogQ2Grid[ix2a[j]]; ya[i][j] = fPDFGrid[ipdf][ix1a[i]][ix2a[j]]; } } // 2D polynomial interpolation. double y = 0, dy = 0; polin2(x1a,x2a,ya,x1,x2,y,dy); fRes[ipdf] = y; } } //-------------------------------------------------------------------------- // 1D polynomial interpolation. void NNPDF::polint(double xa[], double yal[], int n, double x, double& y, double& dy) { int ns = 0; double dif = abs(x-xa[0]); double c[fM > fN ? fM : fN]; double d[fM > fN ? fM : fN]; for (int i = 0; i < n; i++) { double dift = abs(x-xa[i]); if (dift < dif) { ns = i; dif = dift; } c[i] = yal[i]; d[i] = yal[i]; } y = yal[ns]; ns--; for (int m = 1; m < n; m++) { for (int i = 0; i < n-m; i++) { double ho = xa[i]-x; double hp = xa[i+m]-x; double w = c[i+1]-d[i]; double den = ho-hp; if (den == 0) { cout << "NNPDF::polint, failure" << endl; return; } den = w/den; d[i] = hp*den; c[i] = ho*den; } if (2*(ns+1) < n-m) dy = c[ns+1]; else { dy = d[ns]; ns--; } y+=dy; } } //-------------------------------------------------------------------------- // 2D polynomial interpolation. void NNPDF::polin2(double x1al[], double x2al[], double yal[][fN], double x1, double x2, double& y, double& dy) { double yntmp[fN]; double ymtmp[fM]; for (int j = 0; j < fM; j++) { for (int k = 0; k < fN; k++) yntmp[k] = yal[j][k]; polint(x2al,yntmp,fN,x2,ymtmp[j],dy); } polint(x1al,ymtmp,fM,x1,y,dy); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/ResonanceWidths.cc0000644000175000017500000022522112217346247016543 0ustar sunsun// ResonanceWidths.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for // the ResonanceWidths class and classes derived from it. #include "Pythia8/ParticleData.h" #include "Pythia8/ResonanceWidths.h" #include "Pythia8/PythiaComplex.h" namespace Pythia8 { //========================================================================== // The ResonanceWidths class. // Base class for the various resonances. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of points in integration direction for numInt routines. const int ResonanceWidths::NPOINT = 100; // The sum of product masses must not be too close to the resonance mass. const double ResonanceWidths::MASSMARGIN = 0.1; //-------------------------------------------------------------------------- // Initialize data members. // Calculate and store partial and total widths at the nominal mass. bool ResonanceWidths::init(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Couplings* couplingsPtrIn) { // Save pointers. infoPtr = infoPtrIn; settingsPtr = settingsPtrIn; particleDataPtr = particleDataPtrIn; couplingsPtr = couplingsPtrIn; // Perform any model dependent initialisations (pure dummy in base class). bool isInit = initBSM(); // Minimal decaying-resonance width. Minimal phase space for meMode = 103. minWidth = settingsPtr->parm("ResonanceWidths:minWidth"); minThreshold = settingsPtr->parm("ResonanceWidths:minThreshold"); // Pointer to particle species. particlePtr = particleDataPtr->particleDataEntryPtr(idRes); if (particlePtr == 0) { infoPtr->errorMsg("Error in ResonanceWidths::init:" " unknown resonance identity code"); return false; } // Generic particles should not have meMode < 100, but allow // some exceptions: not used Higgses and not used Technicolor. if (idRes == 35 || idRes == 36 || idRes == 37 || idRes/1000000 == 3) isGeneric = false; // Resonance properties: antiparticle, mass, width hasAntiRes = particlePtr->hasAnti(); mRes = particlePtr->m0(); GammaRes = particlePtr->mWidth(); m2Res = mRes*mRes; // For very narrow resonances assign fictitious small width. if (GammaRes < minWidth) GammaRes = 0.1 * minWidth; GamMRat = (mRes == 0.) ? 0. : GammaRes / mRes; // Secondary decay chains by default all on. openPos = 1.; openNeg = 1.; // Allow option where on-shell width is forced to current value. doForceWidth = particlePtr->doForceWidth(); forceFactor = 1.; // Check that resonance OK. if (particlePtr == 0) infoPtr->errorMsg("Error in ResonanceWidths::init:" " unknown resonance identity code"); // Check if we are supposed to do the width calculation // (can be false e.g. if SLHA decay table should take precedence instead). allowCalcWidth = isInit && allowCalc(); if ( allowCalcWidth ) { // Initialize constants used for a resonance. initConstants(); // Calculate various common prefactors for the current mass. mHat = mRes; calcPreFac(true); } // Reset quantities to sum. Declare variables inside loop. double widTot = 0.; double widPos = 0.; double widNeg = 0.; int idNow, idAnti; double openSecPos, openSecNeg; // Loop over all decay channels. Basic properties of channel. for (int i = 0; i < particlePtr->sizeChannels(); ++i) { iChannel = i; onMode = particlePtr->channel(i).onMode(); meMode = particlePtr->channel(i).meMode(); mult = particlePtr->channel(i).multiplicity(); widNow = 0.; // Warn if not relevant meMode. if ( meMode < 0 || meMode > 103 || (isGeneric && meMode < 100) ) { infoPtr->errorMsg("Error in ResonanceWidths::init:" " resonance meMode not acceptable"); } // Channels with meMode < 100 must be implemented in derived classes. if (meMode < 100 || (meMode == 103 && allowCalcWidth)) { // Read out information on channel: primarily use first two. id1 = particlePtr->channel(i).product(0); id2 = particlePtr->channel(i).product(1); id1Abs = abs(id1); id2Abs = abs(id2); // Order first two in descending order of absolute values. if (id2Abs > id1Abs) {swap( id1, id2); swap( id1Abs, id2Abs);} // Allow for third product to be treated in derived classes. if (mult > 2) { id3 = particlePtr->channel(i).product(2); id3Abs = abs(id3); // Also order third into descending order of absolute values. if (id3Abs > id2Abs) {swap( id2, id3); swap( id2Abs, id3Abs);} if (id2Abs > id1Abs) {swap( id1, id2); swap( id1Abs, id2Abs);} } // Read out masses. Calculate two-body phase space. mf1 = particleDataPtr->m0(id1Abs); mf2 = particleDataPtr->m0(id2Abs); mr1 = pow2(mf1 / mHat); mr2 = pow2(mf2 / mHat); ps = (mHat < mf1 + mf2 + MASSMARGIN) ? 0. : sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2 ); if (mult > 2) { mf3 = particleDataPtr->m0(id3Abs); mr3 = pow2(mf3 / mHat); } // Let derived class calculate width for channel provided. calcWidth(true); } // Channels with meMode >= 100 are calculated based on stored values. else widNow = GammaRes * particlePtr->channel(i).bRatio(); // Find secondary open fractions of partial width. openSecPos = 1.; openSecNeg = 1.; if (widNow > 0.) for (int j = 0; j < mult; ++j) { idNow = particlePtr->channel(i).product(j); idAnti = (particleDataPtr->hasAnti(idNow)) ? -idNow : idNow; // Secondary widths not yet initialized for heavier states, // so have to assume unit open fraction there. if (idNow == 23 || abs(idNow) == 24 || idNow == 93 || abs(idNow) == 94 || particleDataPtr->m0(abs(idNow)) < mRes) { openSecPos *= particleDataPtr->resOpenFrac(idNow); openSecNeg *= particleDataPtr->resOpenFrac(idAnti); } } // Store partial widths and secondary open fractions. particlePtr->channel(i).onShellWidth(widNow); particlePtr->channel(i).openSec( idRes, openSecPos); particlePtr->channel(i).openSec(-idRes, openSecNeg); // Update sum over all channnels and over open channels only. widTot += widNow; if (onMode == 1 || onMode == 2) widPos += widNow * openSecPos; if (onMode == 1 || onMode == 3) widNeg += widNow * openSecNeg; } // If no decay channels are open then set particle stable and done. if (widTot < minWidth) { particlePtr->setMayDecay(false, false); particlePtr->setMWidth(0., false); for (int i = 0; i < particlePtr->sizeChannels(); ++i) particlePtr->channel(i).bRatio( 0., false); return true; } // Normalize branching ratios to unity. double bRatio; for (int i = 0; i < particlePtr->sizeChannels(); ++i) { bRatio = particlePtr->channel(i).onShellWidth() / widTot; particlePtr->channel(i).bRatio( bRatio, false); } // Optionally force total width by rescaling of all partial ones. if (doForceWidth) { forceFactor = GammaRes / widTot; for (int i = 0; i < particlePtr->sizeChannels(); ++i) particlePtr->channel(i).onShellWidthFactor( forceFactor); } // Else update newly calculated partial width. else { particlePtr->setMWidth(widTot, false); GammaRes = widTot; } // Updated width-to-mass ratio. Secondary widths for open. GamMRat = GammaRes / mRes; openPos = widPos / widTot; openNeg = widNeg / widTot; // Clip wings of Higgses. bool isHiggs = (idRes == 25 || idRes == 35 ||idRes == 36 ||idRes == 37); bool clipHiggsWings = settingsPtr->flag("Higgs:clipWings"); if (isHiggs && clipHiggsWings) { double mMinNow = particlePtr->mMin(); double mMaxNow = particlePtr->mMax(); double wingsFac = settingsPtr->parm("Higgs:wingsFac"); double mMinWing = mRes - wingsFac * GammaRes; double mMaxWing = mRes + wingsFac * GammaRes; if (mMinWing > mMinNow) particlePtr->setMMinNoChange(mMinWing); if (mMaxWing < mMaxNow || mMaxNow < mMinNow) particlePtr->setMMaxNoChange(mMaxWing); } // Done. return true; } //-------------------------------------------------------------------------- // Calculate the total width and store phase-space-weighted coupling sums. double ResonanceWidths::width(int idSgn, double mHatIn, int idInFlavIn, bool openOnly, bool setBR, int idOutFlav1, int idOutFlav2) { // Calculate various prefactors for the current mass. mHat = mHatIn; idInFlav = idInFlavIn; if (allowCalcWidth) calcPreFac(false); // Reset quantities to sum. Declare variables inside loop. double widSum = 0.; double mfSum, psOnShell; // Loop over all decay channels. Basic properties of channel. for (int i = 0; i < particlePtr->sizeChannels(); ++i) { iChannel = i; onMode = particlePtr->channel(i).onMode(); meMode = particlePtr->channel(i).meMode(); mult = particlePtr->channel(i).multiplicity(); // Initially assume vanishing branching ratio. widNow = 0.; if (setBR) particlePtr->channel(i).currentBR(widNow); // Optionally only consider specific (two-body) decay channel. // Currently only used for Higgs -> q qbar, g g or gamma gamma. if (idOutFlav1 > 0 || idOutFlav2 > 0) { if (mult > 2) continue; if (particlePtr->channel(i).product(0) != idOutFlav1) continue; if (particlePtr->channel(i).product(1) != idOutFlav2) continue; } // Optionally only consider open channels. if (openOnly) { if (idSgn > 0 && onMode !=1 && onMode != 2) continue; if (idSgn < 0 && onMode !=1 && onMode != 3) continue; } // Channels with meMode < 100 must be implemented in derived classes. if (meMode < 100) { // Read out information on channel: primarily use first two. id1 = particlePtr->channel(i).product(0); id2 = particlePtr->channel(i).product(1); id1Abs = abs(id1); id2Abs = abs(id2); // Order first two in descending order of absolute values. if (id2Abs > id1Abs) {swap( id1, id2); swap( id1Abs, id2Abs);} // Allow for third product to be treated in derived classes. if (mult > 2) { id3 = particlePtr->channel(i).product(2); id3Abs = abs(id3); // Also order third into descending order of absolute values. if (id3Abs > id2Abs) {swap( id2, id3); swap( id2Abs, id3Abs);} if (id2Abs > id1Abs) {swap( id1, id2); swap( id1Abs, id2Abs);} } // Read out masses. Calculate two-body phase space. mf1 = particleDataPtr->m0(id1Abs); mf2 = particleDataPtr->m0(id2Abs); mr1 = pow2(mf1 / mHat); mr2 = pow2(mf2 / mHat); ps = (mHat < mf1 + mf2 + MASSMARGIN) ? 0. : sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2 ); if (mult > 2) { mf3 = particleDataPtr->m0(id3Abs); mr3 = pow2(mf3 / mHat); } // Let derived class calculate width for channel provided. calcWidth(false); } // Now on to meMode >= 100. First case: no correction at all. else if (meMode == 100) widNow = GammaRes * particlePtr->channel(i).bRatio(); // Correction by step at threshold. else if (meMode == 101) { mfSum = 0.; for (int j = 0; j < mult; ++j) mfSum += particleDataPtr->m0( particlePtr->channel(i).product(j) ); if (mfSum + MASSMARGIN < mHat) widNow = GammaRes * particlePtr->channel(i).bRatio(); } // Correction by a phase space factor for two-body decays. else if ( (meMode == 102 || meMode == 103) && mult == 2) { mf1 = particleDataPtr->m0( particlePtr->channel(i).product(0) ); mf2 = particleDataPtr->m0( particlePtr->channel(i).product(1) ); mr1 = pow2(mf1 / mHat); mr2 = pow2(mf2 / mHat); ps = (mHat < mf1 + mf2 + MASSMARGIN) ? 0. : sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2 ); mr1 = pow2(mf1 / mRes); mr2 = pow2(mf2 / mRes); psOnShell = (meMode == 102) ? 1. : max( minThreshold, sqrtpos( pow2(1.- mr1 - mr2) - 4. * mr1 * mr2) ); widNow = GammaRes * particlePtr->channel(i).bRatio() * ps / psOnShell; } // Correction by simple threshold factor for multibody decay. else if (meMode == 102 || meMode == 103) { mfSum = 0.; for (int j = 0; j < mult; ++j) mfSum += particleDataPtr->m0( particlePtr->channel(i).product(j) ); ps = sqrtpos(1. - mfSum / mHat); psOnShell = (meMode == 102) ? 1. : max( minThreshold, sqrtpos(1. - mfSum / mRes) ); widNow = GammaRes * particlePtr->channel(i).bRatio() * ps / psOnShell; } // Optionally multiply by secondary widths. if (openOnly) widNow *= particlePtr->channel(i).openSec(idSgn); // Optionally include factor to force to fixed width?? // Optionally multiply by current/nominal resonance mass?? // Sum back up. widSum += widNow; // Optionally store partial widths for later decay channel choice. if (setBR) particlePtr->channel(i).currentBR(widNow); } // Done. return widSum; } //-------------------------------------------------------------------------- // Numerical integration of matrix-element in two-body decay, // where one particle is described by a Breit-Wigner mass distribution. // Normalization to unit integral if matrix element is unity // and there are no phase-space restrictions. double ResonanceWidths::numInt1BW(double mHatIn, double m1, double Gamma1, double mMin1, double m2, int psMode) { // Check that phase space is open for integration. if (mMin1 + m2 > mHatIn) return 0.; // Precalculate coefficients for Breit-Wigner selection. double s1 = m1 * m1; double mG1 = m1 * Gamma1; double mMax1 = mHatIn - m2; double atanMin1 = atan( (mMin1 * mMin1 - s1) / mG1 ); double atanMax1 = atan( (mMax1 * mMax1 - s1) / mG1 ); double atanDif1 = atanMax1 - atanMin1; double wtDif1 = atanDif1 / (M_PI * NPOINT); // Step size in atan-mapped variable. double xStep = 1. / NPOINT; // Variables used in loop over integration points. double sum = 0.; double mrNow2 = pow2(m2 / mHatIn); double xNow1, sNow1, mNow1, mrNow1, psNow, value; // Loop with first-particle mass selection. for (int ip1 = 0; ip1 < NPOINT; ++ip1) { xNow1 = xStep * (ip1 + 0.5); sNow1 = s1 + mG1 * tan(atanMin1 + xNow1 * atanDif1); mNow1 = min( mMax1, max( mMin1, sqrtpos(sNow1) ) ); mrNow1 = pow2(mNow1 / mHatIn); // Evaluate value and add to sum. Different matrix elements. psNow = sqrtpos( pow2(1. - mrNow1 - mrNow2) - 4. * mrNow1 * mrNow2); value = 1.; if (psMode == 1) value = psNow; else if (psMode == 2) value = psNow * psNow; else if (psMode == 3) value = pow3(psNow); else if (psMode == 5) value = psNow * (pow2(1. - mrNow1 - mrNow2) + 8. * mrNow1 * mrNow2); else if (psMode == 6) value = pow3(psNow); sum += value; // End of loop over integration points. Overall normalization. } sum *= wtDif1; // Done. return sum; } //-------------------------------------------------------------------------- // Numerical integration of matrix-element in two-body decay, // where both particles are described by Breit-Wigner mass distributions. // Normalization to unit integral if matrix element is unity // and there are no phase-space restrictions. double ResonanceWidths::numInt2BW(double mHatIn, double m1, double Gamma1, double mMin1, double m2, double Gamma2, double mMin2, int psMode) { // Check that phase space is open for integration. if (mMin1 + mMin2 >= mHatIn) return 0.; // Precalculate coefficients for Breit-Wigner selection. double s1 = m1 * m1; double mG1 = m1 * Gamma1; double mMax1 = mHatIn - mMin2; double atanMin1 = atan( (mMin1 * mMin1 - s1) / mG1 ); double atanMax1 = atan( (mMax1 * mMax1 - s1) / mG1 ); double atanDif1 = atanMax1 - atanMin1; double wtDif1 = atanDif1 / (M_PI * NPOINT); double s2 = m2 * m2; double mG2 = m2 * Gamma2; double mMax2 = mHatIn - mMin1; double atanMin2 = atan( (mMin2 * mMin2 - s2) / mG2 ); double atanMax2 = atan( (mMax2 * mMax2 - s2) / mG2 ); double atanDif2 = atanMax2 - atanMin2; double wtDif2 = atanDif2 / (M_PI * NPOINT); // If on-shell decay forbidden then split integration range // to ensure that low-mass region is not forgotten. bool mustDiv = false; double mDiv1 = 0.; double atanDiv1 = 0.; double atanDLo1 = 0.; double atanDHi1 = 0.; double wtDLo1 = 0.; double wtDHi1 = 0.; double mDiv2 = 0.; double atanDiv2 = 0.; double atanDLo2 = 0.; double atanDHi2 = 0.; double wtDLo2 = 0.; double wtDHi2 = 0.; if (m1 + m2 > mHatIn) { mustDiv = true; double tmpDiv = (mHatIn - m1 - m2) / (Gamma1 + Gamma2); mDiv1 = m1 + Gamma1 * tmpDiv; atanDiv1 = atan( (mDiv1 * mDiv1 - s1) / mG1 ); atanDLo1 = atanDiv1 - atanMin1; atanDHi1 = atanMax1 - atanDiv1; wtDLo1 = atanDLo1 / (M_PI * NPOINT); wtDHi1 = atanDHi1 / (M_PI * NPOINT); mDiv2 = m2 + Gamma2 * tmpDiv; atanDiv2 = atan( (mDiv2 * mDiv2 - s2) / mG2 ); atanDLo2 = atanDiv2 - atanMin2; atanDHi2 = atanMax2 - atanDiv2; wtDLo2 = atanDLo2 / (M_PI * NPOINT); wtDHi2 = atanDHi2 / (M_PI * NPOINT); } // Step size in atan-mapped variable. double xStep = 1. / NPOINT; int nIter = (mustDiv) ? 2 * NPOINT : NPOINT; // Variables used in loop over integration points. double sum = 0.; double xNow1, sNow1, mNow1, mrNow1, xNow2, sNow2, mNow2, mrNow2, psNow, value; double wtNow1 = wtDif1; double wtNow2 = wtDif2; // Outer loop with first-particle mass selection. for (int ip1 = 0; ip1 < nIter; ++ip1) { if (!mustDiv) { xNow1 = xStep * (ip1 + 0.5); sNow1 = s1 + mG1 * tan(atanMin1 + xNow1 * atanDif1); } else if (ip1 < NPOINT) { xNow1 = xStep * (ip1 + 0.5); sNow1 = s1 + mG1 * tan(atanMin1 + xNow1 * atanDLo1); wtNow1 = wtDLo1; } else { xNow1 = xStep * (ip1 - NPOINT + 0.5); sNow1 = s1 + mG1 * tan(atanDiv1 + xNow1 * atanDHi1); wtNow1 = wtDHi1; } mNow1 = min( mMax1, max( mMin1, sqrtpos(sNow1) ) ); mrNow1 = pow2(mNow1 / mHatIn); // Inner loop with second-particle mass selection. for (int ip2 = 0; ip2 < nIter; ++ip2) { if (!mustDiv) { xNow2 = xStep * (ip2 + 0.5); sNow2 = s2 + mG2 * tan(atanMin2 + xNow2 * atanDif2); } else if (ip2 < NPOINT) { xNow2 = xStep * (ip2 + 0.5); sNow2 = s2 + mG2 * tan(atanMin2 + xNow2 * atanDLo2); wtNow2 = wtDLo2; } else { xNow2 = xStep * (ip2 - NPOINT + 0.5); sNow2 = s2 + mG2 * tan(atanDiv2 + xNow2 * atanDHi2); wtNow2 = wtDHi2; } mNow2 = min( mMax2, max( mMin2, sqrtpos(sNow2) ) ); mrNow2 = pow2(mNow2 / mHatIn); // Check that point is inside phase space. if (mNow1 + mNow2 > mHatIn) break; // Evaluate value and add to sum. Different matrix elements. psNow = sqrtpos( pow2(1. - mrNow1 - mrNow2) - 4. * mrNow1 * mrNow2); value = 1.; if (psMode == 1) value = psNow; else if (psMode == 2) value = psNow * psNow; else if (psMode == 3) value = pow3(psNow); else if (psMode == 5) value = psNow * (pow2(1. - mrNow1 - mrNow2) + 8. * mrNow1 * mrNow2); else if (psMode == 6) value = pow3(psNow); sum += value * wtNow1 * wtNow2; // End of second and first loop over integration points. } } // Done. return sum; } //========================================================================== // The ResonanceGmZ class. // Derived class for gamma*/Z0 properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceGmZ::initConstants() { // Locally stored properties and couplings. gmZmode = settingsPtr->mode("WeakZ0:gmZmode"); thetaWRat = 1. / (16. * couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); // The Z0copy with id = 93 is a pure Z0. if (idRes == 93) gmZmode = 2; } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceGmZ::calcPreFac(bool calledFromInit) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = alpEM * thetaWRat * mHat / 3.; // When call for incoming flavour need to consider gamma*/Z0 mix. if (!calledFromInit) { // Couplings when an incoming fermion is specified; elso only pure Z0. ei2 = 0.; eivi = 0.; vi2ai2 = 1.; int idInFlavAbs = abs(idInFlav); if (idInFlavAbs > 0 && idInFlavAbs < 19) { ei2 = couplingsPtr->ef2(idInFlavAbs); eivi = couplingsPtr->efvf(idInFlavAbs); vi2ai2 = couplingsPtr->vf2af2(idInFlavAbs); } // Calculate prefactors for gamma/interference/Z0 terms. double sH = mHat * mHat; gamNorm = ei2; intNorm = 2. * eivi * thetaWRat * sH * (sH - m2Res) / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); resNorm = vi2ai2 * pow2(thetaWRat * sH) / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); // Rescale Z0 height normalization to compensate for a width one?? //if (doForceWidth) { // intNorm *= forceFactor; // resNorm *= forceFactor; //} // Optionally only keep gamma* or Z0 term. if (gmZmode == 1) {intNorm = 0.; resNorm = 0.;} if (gmZmode == 2) {gamNorm = 0.; intNorm = 0.;} } } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceGmZ::calcWidth(bool calledFromInit) { // Check that above threshold. if (ps == 0.) return; // Only contributions from three fermion generations, except top. if ( (id1Abs > 5 && id1Abs < 11) || id1Abs > 16 ) return; // At initialization only the pure Z0 should be considered. if (calledFromInit) { // Combine kinematics with colour factor and couplings. widNow = preFac * ps * (couplingsPtr->vf2(id1Abs) * (1. + 2. * mr1) + couplingsPtr->af2(id1Abs) * ps*ps); if (id1Abs < 6) widNow *= colQ; } // When call for incoming flavour need to consider gamma*/Z0 mix. else { // Kinematical factors and couplings. double kinFacV = ps * (1. + 2. * mr1); double ef2 = couplingsPtr->ef2(id1Abs) * kinFacV; double efvf = couplingsPtr->efvf(id1Abs) * kinFacV; double vf2af2 = couplingsPtr->vf2(id1Abs) * kinFacV + couplingsPtr->af2(id1Abs) * pow3(ps); // Relative outwidths: combine instate, propagator and outstate. widNow = gamNorm * ef2 + intNorm * efvf + resNorm * vf2af2; // Colour factor. if (id1Abs < 6) widNow *= colQ; } } //========================================================================== // The ResonanceW class. // Derived class for W+- properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceW::initConstants() { // Locally stored properties and couplings. thetaWRat = 1. / (12. * couplingsPtr->sin2thetaW()); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceW::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = alpEM * thetaWRat * mHat; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceW::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // Only contributions from three fermion generations, except top. if ( (id1Abs > 5 && id1Abs < 11) || id1Abs > 16 ) return; // Combine kinematics with colour factor and couplings. widNow = preFac * ps * (1. - 0.5 * (mr1 + mr2) - 0.5 * pow2(mr1 - mr2)); if (id1Abs < 6) widNow *= colQ * couplingsPtr->V2CKMid(id1Abs, id2Abs); } //========================================================================== // The ResonanceTop class. // Derived class for top/antitop properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceTop::initConstants() { // Locally stored properties and couplings. thetaWRat = 1. / (16. * couplingsPtr->sin2thetaW()); m2W = pow2(particleDataPtr->m0(24)); // Extra coupling factors for t -> H+ + b. tanBeta = settingsPtr->parm("HiggsHchg:tanBeta"); tan2Beta = tanBeta * tanBeta; mbRun = particleDataPtr->mRun( 5, particleDataPtr->m0(6) ); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceTop::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 1. - 2.5 * alpS / M_PI; preFac = alpEM * thetaWRat * pow3(mHat) / m2W; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceTop::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // Contributions from W + quark. if (id1Abs == 24 && id2Abs < 6) { widNow = preFac * ps * ( pow2(1. - mr2) + (1. + mr2) * mr1 - 2. * mr1 * mr1 ); // Combine with colour factor and CKM couplings. widNow *= colQ * couplingsPtr->V2CKMid(6, id2Abs); // Contributions from H+ + quark (so far only b). } else if (id1Abs == 37 && id2Abs == 5) { widNow = preFac * ps * ( (1. + mr2 - mr1) * (pow2(mbRun / mHat) * tan2Beta + 1. / tan2Beta) + 4. * mbRun * mf2 / pow2(mHat) ); } } //========================================================================== // The ResonanceFour class. // Derived class for fourth-generation properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceFour::initConstants() { // Locally stored properties and couplings. thetaWRat = 1. / (16. * couplingsPtr->sin2thetaW()); m2W = pow2(particleDataPtr->m0(24)); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceFour::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = (idRes < 9) ? 1. - 2.5 * alpS / M_PI : 1.; preFac = alpEM * thetaWRat * pow3(mHat) / m2W; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceFour::calcWidth(bool) { // Only contributions from W + fermion. if (id1Abs != 24 || id2Abs > 18) return; // Check that above threshold. Kinematical factor. if (ps == 0.) return; widNow = preFac * ps * ( pow2(1. - mr2) + (1. + mr2) * mr1 - 2. * mr1 * mr1 ); // Combine with colour factor and CKM couplings. if (idRes < 9) widNow *= colQ * couplingsPtr->V2CKMid(idRes, id2Abs); } //========================================================================== // The ResonanceH class. // Derived class for SM and BSM Higgs properties. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Minimal mass for W, Z, top in integration over respective Breit-Wigner. // Top constrainted by t -> W b decay, which is not seen in simple top BW. const double ResonanceH::MASSMINWZ = 10.; const double ResonanceH::MASSMINT = 100.; // Number of widths above threshold where B-W integration not needed. const double ResonanceH::GAMMAMARGIN = 10.; //-------------------------------------------------------------------------- // Initialize constants. void ResonanceH::initConstants() { // Locally stored properties and couplings. useCubicWidth = settingsPtr->flag("Higgs:cubicWidth"); useRunLoopMass = settingsPtr->flag("Higgs:runningLoopMass"); sin2tW = couplingsPtr->sin2thetaW(); cos2tW = 1. - sin2tW; mT = particleDataPtr->m0(6); mZ = particleDataPtr->m0(23); mW = particleDataPtr->m0(24); mHchg = particleDataPtr->m0(37); GammaT = particleDataPtr->mWidth(6); GammaZ = particleDataPtr->mWidth(23); GammaW = particleDataPtr->mWidth(24); // Couplings to fermions, Z and W, depending on Higgs type. coup2d = 1.; coup2u = 1.; coup2l = 1.; coup2Z = 1.; coup2W = 1.; coup2Hchg = 0.; coup2H1H1 = 0.; coup2A3A3 = 0.; coup2H1Z = 0.; coup2A3Z = 0.; coup2A3H1 = 0.; coup2HchgW = 0.; if (higgsType == 1) { coup2d = settingsPtr->parm("HiggsH1:coup2d"); coup2u = settingsPtr->parm("HiggsH1:coup2u"); coup2l = settingsPtr->parm("HiggsH1:coup2l"); coup2Z = settingsPtr->parm("HiggsH1:coup2Z"); coup2W = settingsPtr->parm("HiggsH1:coup2W"); coup2Hchg = settingsPtr->parm("HiggsH1:coup2Hchg"); } else if (higgsType == 2) { coup2d = settingsPtr->parm("HiggsH2:coup2d"); coup2u = settingsPtr->parm("HiggsH2:coup2u"); coup2l = settingsPtr->parm("HiggsH2:coup2l"); coup2Z = settingsPtr->parm("HiggsH2:coup2Z"); coup2W = settingsPtr->parm("HiggsH2:coup2W"); coup2Hchg = settingsPtr->parm("HiggsH2:coup2Hchg"); coup2H1H1 = settingsPtr->parm("HiggsH2:coup2H1H1"); coup2A3A3 = settingsPtr->parm("HiggsH2:coup2A3A3"); coup2H1Z = settingsPtr->parm("HiggsH2:coup2H1Z"); coup2A3Z = settingsPtr->parm("HiggsA3:coup2H2Z"); coup2A3H1 = settingsPtr->parm("HiggsH2:coup2A3H1"); coup2HchgW = settingsPtr->parm("HiggsH2:coup2HchgW"); } else if (higgsType == 3) { coup2d = settingsPtr->parm("HiggsA3:coup2d"); coup2u = settingsPtr->parm("HiggsA3:coup2u"); coup2l = settingsPtr->parm("HiggsA3:coup2l"); coup2Z = settingsPtr->parm("HiggsA3:coup2Z"); coup2W = settingsPtr->parm("HiggsA3:coup2W"); coup2Hchg = settingsPtr->parm("HiggsA3:coup2Hchg"); coup2H1H1 = settingsPtr->parm("HiggsA3:coup2H1H1"); coup2H1Z = settingsPtr->parm("HiggsA3:coup2H1Z"); coup2HchgW = settingsPtr->parm("HiggsA3:coup2Hchg"); } // Initialization of threshold kinematical factor by stepwise // numerical integration of H -> t tbar, Z0 Z0 and W+ W-. int psModeT = (higgsType < 3) ? 3 : 1; int psModeWZ = (higgsType < 3) ? 5 : 6; mLowT = max( 2.02 * MASSMINT, 0.5 * mT); mStepT = 0.01 * (3. * mT - mLowT); mLowZ = max( 2.02 * MASSMINWZ, 0.5 * mZ); mStepZ = 0.01 * (3. * mZ - mLowZ); mLowW = max( 2.02 * MASSMINWZ, 0.5 * mW); mStepW = 0.01 * (3. * mW - mLowW); for (int i = 0; i <= 100; ++i) { kinFacT[i] = numInt2BW( mLowT + i * mStepT, mT, GammaT, MASSMINT, mT, GammaT, MASSMINT, psModeT); kinFacZ[i] = numInt2BW( mLowZ + i * mStepZ, mZ, GammaZ, MASSMINWZ, mZ, GammaZ, MASSMINWZ, psModeWZ); kinFacW[i] = numInt2BW( mLowW + i * mStepW, mW, GammaW, MASSMINWZ, mW, GammaW, MASSMINWZ, psModeWZ); } } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceH::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = (alpEM / (8. * sin2tW)) * pow3(mHat) / pow2(mW); } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceH::calcWidth(bool) { // Widths of decays Higgs -> f + fbar. if ( id2Abs == id1Abs && ( (id1Abs > 0 && id1Abs < 7) || (id1Abs > 10 && id1Abs < 17) ) ) { kinFac = 0.; // Check that above threshold (well above for top). Kinematical factor. if ( (id1Abs != 6 && mHat > 2. * mf1 + MASSMARGIN) || (id1Abs == 6 && mHat > 3. * mT ) ) { // A0 behaves like beta, h0 and H0 like beta**3. kinFac = (higgsType < 3) ? pow3(ps) : ps; } // Top near or below threshold: interpolate in table. else if (id1Abs == 6 && mHat > mLowT) { double xTab = (mHat - mLowT) / mStepT; int iTab = max( 0, min( 99, int(xTab) ) ); kinFac = kinFacT[iTab] * pow( kinFacT[iTab + 1] / kinFacT[iTab], xTab - iTab); } // Coupling from mass and from BSM deviation from SM. double coupFac = pow2(particleDataPtr->mRun(id1Abs, mHat) / mHat); if (id1Abs < 7 && id1Abs%2 == 1) coupFac *= coup2d * coup2d; else if (id1Abs < 7) coupFac *= coup2u * coup2u; else coupFac *= coup2l * coup2l; // Combine couplings and phase space with colour factor. widNow = preFac * coupFac * kinFac; if (id1Abs < 7) widNow *= colQ; } // Widths of decays Higgs -> g + g. else if (id1Abs == 21 && id2Abs == 21) widNow = preFac * pow2(alpS / M_PI) * eta2gg(); // Widths of decays Higgs -> gamma + gamma. else if (id1Abs == 22 && id2Abs == 22) widNow = preFac * pow2(alpEM / M_PI) * 0.5 * eta2gaga(); // Widths of decays Higgs -> Z0 + gamma0. else if (id1Abs == 23 && id2Abs == 22) widNow = preFac * pow2(alpEM / M_PI) * pow3(ps) * eta2gaZ(); // Widths of decays Higgs (h0, H0) -> Z0 + Z0. else if (id1Abs == 23 && id2Abs == 23) { // If Higgs heavy use on-shell expression, else interpolation in table if (mHat > 3. * mZ) kinFac = (1. - 4. * mr1 + 12. * mr1 * mr1) * ps; else if (mHat > mLowZ) { double xTab = (mHat - mLowZ) / mStepZ; int iTab = max( 0, min( 99, int(xTab) ) ); kinFac = kinFacZ[iTab] * pow( kinFacZ[iTab + 1] / kinFacZ[iTab], xTab - iTab ); } else kinFac = 0.; // Prefactor, normally rescaled to mRes^2 * mHat rather than mHat^3. widNow = 0.25 * preFac * pow2(coup2Z) * kinFac; if (!useCubicWidth) widNow *= pow2(mRes / mHat); } // Widths of decays Higgs (h0, H0) -> W+ + W-. else if (id1Abs == 24 && id2Abs == 24) { // If Higgs heavy use on-shell expression, else interpolation in table. if (mHat > 3. * mW) kinFac = (1. - 4. * mr1 + 12. * mr1 * mr1) * ps; else if (mHat > mLowW) { double xTab = (mHat - mLowW) / mStepW; int iTab = max( 0, min( 99, int(xTab) ) ); kinFac = kinFacW[iTab] * pow( kinFacW[iTab + 1] / kinFacW[iTab], xTab - iTab); } else kinFac = 0.; // Prefactor, normally rescaled to mRes^2 * mHat rather than mHat^3. widNow = 0.5 * preFac * pow2(coup2W) * kinFac; if (!useCubicWidth) widNow *= pow2(mRes / mHat); } // Widths of decays Higgs (H0) -> h0 + h0. else if (id1Abs == 25 && id2Abs == 25) widNow = 0.25 * preFac * pow4(mZ / mHat) * ps * pow2(coup2H1H1); // Widths of decays Higgs (H0) -> A0 + A0. else if (id1Abs == 36 && id2Abs == 36) widNow = 0.5 * preFac * pow4(mZ / mHat) * ps * pow2(coup2A3A3); // Widths of decays Higgs (A0) -> h0 + Z0. else if (id1Abs == 25 && id2Abs == 23) widNow = 0.5 * preFac * pow3(ps) * pow2(coup2H1Z); // Widths of decays Higgs (H0) -> A0 + Z0. else if (id1Abs == 36 && id2Abs == 23) widNow = 0.5 * preFac * pow3(ps) * pow2(coup2A3Z); // Widths of decays Higgs (H0) -> A0 + h0. else if (id1Abs == 36 && id2Abs == 25) widNow = 0.25 * preFac * pow4(mZ / mHat) * ps * pow2(coup2A3H1); // Widths of decays Higgs -> H+- + W-+. else if (id1Abs == 37 && id2Abs == 24) widNow = 0.5 * preFac * pow3(ps) * pow2(coup2HchgW); } //-------------------------------------------------------------------------- // Sum up quark loop contributions in Higgs -> g + g. // Note: running quark masses are used, unlike Pythia6 (not negligible shift). double ResonanceH::eta2gg() { // Initial values. complex eta = complex(0., 0.); double mLoop, epsilon, root, rootLog; complex phi, etaNow; // Loop over s, c, b, t quark flavours. for (int idNow = 3; idNow < 7; ++idNow) { mLoop = (useRunLoopMass) ? particleDataPtr->mRun(idNow, mHat) : particleDataPtr->m0(idNow); epsilon = pow2(2. * mLoop / mHat); // Value of loop integral. if (epsilon <= 1.) { root = sqrt(1. - epsilon); rootLog = (epsilon < 1e-4) ? log(4. / epsilon - 2.) : log( (1. + root) / (1. - root) ); phi = complex( -0.25 * (pow2(rootLog) - pow2(M_PI)), 0.5 * M_PI * rootLog ); } else phi = complex( pow2( asin(1. / sqrt(epsilon)) ), 0.); // Factors that depend on Higgs and flavour type. if (higgsType < 3) etaNow = -0.5 * epsilon * (complex(1., 0.) + (1. - epsilon) * phi); else etaNow = -0.5 * epsilon * phi; if (idNow%2 == 1) etaNow *= coup2d; else etaNow *= coup2u; // Sum up contribution and return square of absolute value. eta += etaNow; } return (pow2(eta.real()) + pow2(eta.imag())); } //-------------------------------------------------------------------------- // Sum up quark, lepton, W+- and (for BSM) H+- loop contributions // in Higgs -> gamma + gamma. double ResonanceH::eta2gaga() { // Initial values. complex eta = complex(0., 0.); int idNow; double ef, mLoop, epsilon, root, rootLog; complex phi, etaNow; // Loop over s, c, b, t, mu, tau, W+-, H+- flavours. for (int idLoop = 0; idLoop < 8; ++idLoop) { if (idLoop < 4) idNow = idLoop + 3; else if (idLoop < 6) idNow = 2 * idLoop + 5; else if (idLoop < 7) idNow = 24; else idNow = 37; if (idNow == 37 && higgsType == 0) continue; // Charge and loop integral parameter. ef = (idNow < 20) ? couplingsPtr->ef(idNow) : 1.; mLoop = (useRunLoopMass) ? particleDataPtr->mRun(idNow, mHat) : particleDataPtr->m0(idNow); epsilon = pow2(2. * mLoop / mHat); // Value of loop integral. if (epsilon <= 1.) { root = sqrt(1. - epsilon); rootLog = (epsilon < 1e-4) ? log(4. / epsilon - 2.) : log( (1. + root) / (1. - root) ); phi = complex( -0.25 * (pow2(rootLog) - pow2(M_PI)), 0.5 * M_PI * rootLog ); } else phi = complex( pow2( asin(1. / sqrt(epsilon)) ), 0.); // Expressions for quarks and leptons that depend on Higgs type. if (idNow < 17) { if (higgsType < 3) etaNow = -0.5 * epsilon * (complex(1., 0.) + (1. - epsilon) * phi); else etaNow = -0.5 * epsilon * phi; if (idNow < 7 && idNow%2 == 1) etaNow *= 3. * pow2(ef) * coup2d; else if (idNow < 7 ) etaNow *= 3. * pow2(ef) * coup2u; else etaNow *= pow2(ef) * coup2l; } // Expression for W+-. else if (idNow == 24) etaNow = (complex(0.5 + 0.75 * epsilon, 0.) + 0.75 * epsilon * (2. - epsilon) * phi) * coup2W; // Expression for H+-. else etaNow = (complex(epsilon, 0.) - epsilon * epsilon * phi) * pow2(mW / mHchg) * coup2Hchg; // Sum up contribution and return square of absolute value. eta += etaNow; } return (pow2(eta.real()) + pow2(eta.imag())); } //-------------------------------------------------------------------------- // Sum up quark, lepton, W+- and (for BSM) H+- loop contributions // in Higgs -> gamma + Z0. double ResonanceH::eta2gaZ() { // Initial values. complex eta = complex(0., 0.); int idNow; double ef, vf, mLoop, epsilon, epsPrime, root, rootLog, asinEps; complex phi, psi, phiPrime, psiPrime, fXY, f1, etaNow; // Loop over s, c, b, t, mu , tau, W+-, H+- flavours. for (int idLoop = 0; idLoop < 7; ++idLoop) { if (idLoop < 4) idNow = idLoop + 3; else if (idLoop < 6) idNow = 2 * idLoop + 5; else if (idLoop < 7) idNow = 24; else idNow = 37; // Electroweak charges and loop integral parameters. ef = (idNow < 20) ? couplingsPtr->ef(idNow) : 1.; vf = (idNow < 20) ? couplingsPtr->vf(idNow) : 0.; mLoop = (useRunLoopMass) ? particleDataPtr->mRun(idNow, mHat) : particleDataPtr->m0(idNow); epsilon = pow2(2. * mLoop / mHat); epsPrime = pow2(2. * mLoop / mZ); // Value of loop integral for epsilon = 4 m^2 / sHat. if (epsilon <= 1.) { root = sqrt(1. - epsilon); rootLog = (epsilon < 1e-4) ? log(4. / epsilon - 2.) : log( (1. + root) / (1. - root) ); phi = complex( -0.25 * (pow2(rootLog) - pow2(M_PI)), 0.5 * M_PI * rootLog ); psi = 0.5 * root * complex( rootLog, -M_PI); } else { asinEps = asin(1. / sqrt(epsilon)); phi = complex( pow2(asinEps), 0.); psi = complex( sqrt(epsilon - 1.) * asinEps, 0.); } // Value of loop integral for epsilonPrime = 4 m^2 / m_Z^2. if (epsPrime <= 1.) { root = sqrt(1. - epsPrime); rootLog = (epsPrime < 1e-4) ? log(4. / epsPrime - 2.) : log( (1. + root) / (1. - root) ); phiPrime = complex( -0.25 * (pow2(rootLog) - pow2(M_PI)), 0.5 * M_PI * rootLog ); psiPrime = 0.5 * root * complex( rootLog, -M_PI); } else { asinEps = asin(1. / sqrt(epsPrime)); phiPrime = complex( pow2(asinEps), 0.); psiPrime = complex( sqrt(epsPrime - 1.) * asinEps, 0.); } // Combine the two loop integrals. fXY = (epsilon * epsPrime / (8. * pow2(epsilon - epsPrime))) * ( complex(epsilon - epsPrime, 0) + epsilon * epsPrime * (phi - phiPrime) + 2. * epsilon * (psi - psiPrime) ); f1 = - (epsilon * epsPrime / (2. * (epsilon - epsPrime))) * (phi - phiPrime); // Expressions for quarks and leptons that depend on Higgs type. if (idNow < 17) { etaNow = (higgsType < 3) ? -fXY + 0.25 * f1 : 0.25 * f1; if (idNow < 7 && idNow%2 == 1) etaNow *= 3. * ef * vf * coup2d; else if (idNow < 7) etaNow *= 3. * ef * vf * coup2u; else etaNow *= ef * vf * coup2l; // Expression for W+-. } else if (idNow == 24) { double coef1 = 3. - sin2tW / cos2tW; double coefXY = (1. + 2. / epsilon) * sin2tW / cos2tW - (5. + 2. / epsilon); etaNow = -cos2tW * (coef1 * f1 + coefXY * fXY) * coup2W; // Expression for H+-. } else etaNow = (1. - 2. * sin2tW) * fXY * pow2(mW / mHchg) * coup2Hchg; // Sum up contribution and return square of absolute value. eta += etaNow; } return ( (pow2(eta.real()) + pow2(eta.imag())) / (sin2tW * cos2tW) ); } //========================================================================== // The ResonanceHchg class. // Derived class for H+- properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceHchg::initConstants() { // Locally stored properties and couplings. useCubicWidth = settingsPtr->flag("Higgs:cubicWidth"); thetaWRat = 1. / (8. * couplingsPtr->sin2thetaW()); mW = particleDataPtr->m0(24); tanBeta = settingsPtr->parm("HiggsHchg:tanBeta"); tan2Beta = tanBeta * tanBeta; coup2H1W = settingsPtr->parm("HiggsHchg:coup2H1W"); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceHchg::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = alpEM * thetaWRat * pow3(mHat) / pow2(mW); } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceHchg::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // H+- decay to fermions involves running masses. if (id1Abs < 17 && (id1Abs < 7 || id1Abs > 10)) { double mRun1 = particleDataPtr->mRun(id1Abs, mHat); double mRun2 = particleDataPtr->mRun(id2Abs, mHat); double mrRunDn = pow2(mRun1 / mHat); double mrRunUp = pow2(mRun2 / mHat); if (id1Abs%2 == 0) swap( mrRunDn, mrRunUp); // Width to fermions: couplings, kinematics, colour factor. widNow = preFac * max( 0., (mrRunDn * tan2Beta + mrRunUp / tan2Beta) * (1. - mrRunDn - mrRunUp) - 4. *mrRunDn * mrRunUp ) * ps; if (id1Abs < 7) widNow *= colQ; } // H+- decay to h0 + W+-. else if (id1Abs == 25 && id2Abs == 24) widNow = 0.5 * preFac * pow3(ps) * pow2(coup2H1W); } //========================================================================== // The ResonanceZprime class. // Derived class for gamma*/Z0/Z'^0 properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceZprime::initConstants() { // Locally stored properties and couplings. gmZmode = settingsPtr->mode("Zprime:gmZmode"); sin2tW = couplingsPtr->sin2thetaW(); cos2tW = 1. - sin2tW; thetaWRat = 1. / (16. * sin2tW * cos2tW); // Properties of Z resonance. mZ = particleDataPtr->m0(23); GammaZ = particleDataPtr->mWidth(23); m2Z = mZ*mZ; GamMRatZ = GammaZ / mZ; // Ensure that arrays initially empty. for (int i = 0; i < 20; ++i) afZp[i] = 0.; for (int i = 0; i < 20; ++i) vfZp[i] = 0.; // Store first-generation axial and vector couplings. afZp[1] = settingsPtr->parm("Zprime:ad"); afZp[2] = settingsPtr->parm("Zprime:au"); afZp[11] = settingsPtr->parm("Zprime:ae"); afZp[12] = settingsPtr->parm("Zprime:anue"); vfZp[1] = settingsPtr->parm("Zprime:vd"); vfZp[2] = settingsPtr->parm("Zprime:vu"); vfZp[11] = settingsPtr->parm("Zprime:ve"); vfZp[12] = settingsPtr->parm("Zprime:vnue"); // Second and third generation could be carbon copy of this... if (settingsPtr->flag("Zprime:universality")) { for (int i = 3; i <= 6; ++i) { afZp[i] = afZp[i-2]; vfZp[i] = vfZp[i-2]; afZp[i+10] = afZp[i+8]; vfZp[i+10] = vfZp[i+8]; } // ... or could have different couplings. } else { afZp[3] = settingsPtr->parm("Zprime:as"); afZp[4] = settingsPtr->parm("Zprime:ac"); afZp[5] = settingsPtr->parm("Zprime:ab"); afZp[6] = settingsPtr->parm("Zprime:at"); afZp[13] = settingsPtr->parm("Zprime:amu"); afZp[14] = settingsPtr->parm("Zprime:anumu"); afZp[15] = settingsPtr->parm("Zprime:atau"); afZp[16] = settingsPtr->parm("Zprime:anutau"); vfZp[3] = settingsPtr->parm("Zprime:vs"); vfZp[4] = settingsPtr->parm("Zprime:vc"); vfZp[5] = settingsPtr->parm("Zprime:vb"); vfZp[6] = settingsPtr->parm("Zprime:vt"); vfZp[13] = settingsPtr->parm("Zprime:vmu"); vfZp[14] = settingsPtr->parm("Zprime:vnumu"); vfZp[15] = settingsPtr->parm("Zprime:vtau"); vfZp[16] = settingsPtr->parm("Zprime:vnutau"); } // Coupling for Z' -> W+ W-. coupZpWW = settingsPtr->parm("Zprime:coup2WW"); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceZprime::calcPreFac(bool calledFromInit) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = alpEM * thetaWRat * mHat / 3.; // When call for incoming flavour need to consider gamma*/Z0 mix. if (!calledFromInit) { // Couplings when an incoming fermion is specified; elso only pure Z'0. ei2 = 0.; eivi = 0.; vai2 = 0.; eivpi = 0.; vaivapi = 0., vapi2 = 1.; int idInFlavAbs = abs(idInFlav); if (idInFlavAbs > 0 && idInFlavAbs < 19) { double ei = couplingsPtr->ef(idInFlavAbs); double ai = couplingsPtr->af(idInFlavAbs); double vi = couplingsPtr->vf(idInFlavAbs); double api = afZp[idInFlavAbs]; double vpi = vfZp[idInFlavAbs]; ei2 = ei * ei; eivi = ei * vi; vai2 = vi * vi + ai * ai; eivpi = ei * vpi; vaivapi = vi * vpi + ai * api;; vapi2 = vpi * vpi + api * api; } // Calculate prefactors for gamma/interference/Z0 terms. double sH = mHat * mHat; double propZ = sH / ( pow2(sH - m2Z) + pow2(sH * GamMRatZ) ); double propZp = sH / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); gamNorm = ei2; gamZNorm = 2. * eivi * thetaWRat * (sH - m2Z) * propZ; ZNorm = vai2 * pow2(thetaWRat) * sH * propZ; gamZpNorm = 2. * eivpi * thetaWRat * (sH - m2Res) * propZp; ZZpNorm = 2. * vaivapi * pow2(thetaWRat) * ((sH - m2Res) * (sH - m2Z) + sH * GamMRat * sH * GamMRatZ) * propZ * propZp; ZpNorm = vapi2 * pow2(thetaWRat) * sH * propZp; // Rescale Z0 height normalization to compensate for a width one?? //if (doForceWidth) { // intNorm *= forceFactor; // resNorm *= forceFactor; //} // Optionally only keep some of gamma*, Z0 and Z' terms. if (gmZmode == 1) {gamZNorm = 0; ZNorm = 0.; gamZpNorm = 0.; ZZpNorm = 0.; ZpNorm = 0.;} if (gmZmode == 2) {gamNorm = 0.; gamZNorm = 0.; gamZpNorm = 0.; ZZpNorm = 0.; ZpNorm = 0.;} if (gmZmode == 3) {gamNorm = 0.; gamZNorm = 0.; ZNorm = 0.; gamZpNorm = 0.; ZZpNorm = 0.;} if (gmZmode == 4) {gamZpNorm = 0.; ZZpNorm = 0.; ZpNorm = 0.;} if (gmZmode == 5) {gamZNorm = 0.; ZNorm = 0.; ZZpNorm = 0.;} if (gmZmode == 6) {gamNorm = 0.; gamZNorm = 0.; gamZpNorm = 0.;} } } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceZprime::calcWidth(bool calledFromInit) { // Check that above threshold. if (ps == 0.) return; // At initialization only the pure Z'0 should be considered. if (calledFromInit) { // Contributions from three fermion generations. if ( id1Abs < 7 || (id1Abs > 10 && id1Abs < 17) ) { double apf = afZp[id1Abs]; double vpf = vfZp[id1Abs]; widNow = preFac * ps * (vpf*vpf * (1. + 2. * mr1) + apf*apf * ps*ps); if (id1Abs < 7) widNow *= colQ; // Contribution from Z'0 -> W^+ W^-. } else if (id1Abs == 24) { widNow = preFac * pow2(coupZpWW * cos2tW) * pow3(ps) * (1. + mr1*mr1 + mr2*mr2 + 10. * (mr1 + mr2 + mr1 * mr2)); } } // When call for incoming flavour need to consider full mix. else { // Contributions from three fermion generations. if ( id1Abs < 7 || (id1Abs > 10 && id1Abs < 17) ) { // Couplings of gamma^*/Z^0/Z'^0 to final flavour double ef = couplingsPtr->ef(id1Abs); double af = couplingsPtr->af(id1Abs); double vf = couplingsPtr->vf(id1Abs); double apf = afZp[id1Abs]; double vpf = vfZp[id1Abs]; // Combine couplings with kinematical factors. double kinFacA = pow3(ps); double kinFacV = ps * (1. + 2. * mr1); double ef2 = ef * ef * kinFacV; double efvf = ef * vf * kinFacV; double vaf2 = vf * vf * kinFacV + af * af * kinFacA; double efvpf = ef * vpf * kinFacV; double vafvapf = vf * vpf * kinFacV + af * apf * kinFacA; double vapf2 = vpf * vpf * kinFacV + apf * apf * kinFacA; // Relative outwidths: combine instate, propagator and outstate. widNow = gamNorm * ef2 + gamZNorm * efvf + ZNorm * vaf2 + gamZpNorm * efvpf + ZZpNorm * vafvapf + ZpNorm * vapf2; if (id1Abs < 7) widNow *= colQ; // Contribution from Z'0 -> W^+ W^-. } else if (id1Abs == 24) { widNow = ZpNorm * pow2(coupZpWW * cos2tW) * pow3(ps) * (1. + mr1*mr1 + mr2*mr2 + 10. * (mr1 + mr2 + mr1 * mr2)); } } } //========================================================================== // The ResonanceWprime class. // Derived class for W'+- properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceWprime::initConstants() { // Locally stored properties and couplings. thetaWRat = 1. / (12. * couplingsPtr->sin2thetaW()); cos2tW = couplingsPtr->cos2thetaW(); // Axial and vector couplings of fermions. aqWp = settingsPtr->parm("Wprime:aq"); vqWp = settingsPtr->parm("Wprime:vq"); alWp = settingsPtr->parm("Wprime:al"); vlWp = settingsPtr->parm("Wprime:vl"); // Coupling for W' -> W Z. coupWpWZ = settingsPtr->parm("Wprime:coup2WZ"); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceWprime::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = alpEM * thetaWRat * mHat; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceWprime::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // Decay to quarks involves colour factor and CKM matrix. if (id1Abs > 0 && id1Abs < 7) widNow = preFac * ps * 0.5 * ((vqWp*vqWp + aqWp * aqWp) + 6. * (vqWp*vqWp - aqWp * aqWp) * sqrt(mr1 *mr2)) * (1. - 0.5 * (mr1 + mr2) - 0.5 * pow2(mr1 - mr2)) * colQ * couplingsPtr->V2CKMid(id1Abs, id2Abs); // Decay to leptons simpler. else if (id1Abs > 10 && id1Abs < 17) widNow = preFac * ps * 0.5 * ((vlWp*vqWp + alWp * aqWp) + 6. * (vlWp*vqWp - alWp * aqWp) * sqrt(mr1 *mr2)) * (1. - 0.5 * (mr1 + mr2) - 0.5 * pow2(mr1 - mr2)); // Decay to W^+- Z^0. else if (id1Abs == 24 && id2Abs == 23) widNow = preFac * 0.25 * pow2(coupWpWZ) * cos2tW * (mr1 / mr2) * pow3(ps) * (1. + mr1*mr1 + mr2*mr2 + 10. * (mr1 + mr2 + mr1 * mr2)); } //========================================================================== // The ResonanceRhorizontal class. // Derived class for R^0 (horizontal gauge boson) properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceRhorizontal::initConstants() { // Locally stored properties and couplings. thetaWRat = 1. / (12. * couplingsPtr->sin2thetaW()); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceRhorizontal::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = alpEM * thetaWRat * mHat; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceRhorizontal::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // R -> f fbar. Colour factor for quarks. widNow = preFac * ps * (2. - mr1 - mr2 - pow2(mr1 - mr2)); if (id1Abs < 9) widNow *= colQ; } //========================================================================== // The ResonanceExcited class. // Derived class for excited-fermion properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceExcited::initConstants() { // Locally stored properties and couplings. Lambda = settingsPtr->parm("ExcitedFermion:Lambda"); coupF = settingsPtr->parm("ExcitedFermion:coupF"); coupFprime = settingsPtr->parm("ExcitedFermion:coupFprime"); coupFcol = settingsPtr->parm("ExcitedFermion:coupFcol"); sin2tW = couplingsPtr->sin2thetaW(); cos2tW = 1. - sin2tW; } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceExcited::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); preFac = pow3(mHat) / pow2(Lambda); } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceExcited::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // f^* -> f g. if (id1Abs == 21) widNow = preFac * alpS * pow2(coupFcol) / 3.; // f^* -> f gamma. else if (id1Abs == 22) { double chgI3 = (id2Abs%2 == 0) ? 0.5 : -0.5; double chgY = (id2Abs < 9) ? 1. / 6. : -0.5; double chg = chgI3 * coupF + chgY * coupFprime; widNow = preFac * alpEM * pow2(chg) / 4.; } // f^* -> f Z^0. else if (id1Abs == 23) { double chgI3 = (id2Abs%2 == 0) ? 0.5 : -0.5; double chgY = (id2Abs < 9) ? 1. / 6. : -0.5; double chg = chgI3 * cos2tW * coupF - chgY * sin2tW * coupFprime; widNow = preFac * (alpEM * pow2(chg) / (8. * sin2tW * cos2tW)) * ps*ps * (2. + mr1); } // f^* -> f' W^+-. else if (id1Abs == 24) widNow = preFac * (alpEM * pow2(coupF) / (16. * sin2tW)) * ps*ps * (2. + mr1); } //========================================================================== // The ResonanceGraviton class. // Derived class for excited Graviton properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceGraviton::initConstants() { // SMinBulk = off/on, use universal coupling (kappaMG) // or individual (Gxx) between graviton and SM particles. eDsmbulk = settingsPtr->flag("ExtraDimensionsG*:SMinBulk"); eDvlvl = false; if (eDsmbulk) eDvlvl = settingsPtr->flag("ExtraDimensionsG*:VLVL"); kappaMG = settingsPtr->parm("ExtraDimensionsG*:kappaMG"); for (int i = 0; i < 27; ++i) eDcoupling[i] = 0.; double tmp_coup = settingsPtr->parm("ExtraDimensionsG*:Gqq"); for (int i = 1; i <= 4; ++i) eDcoupling[i] = tmp_coup; eDcoupling[5] = settingsPtr->parm("ExtraDimensionsG*:Gbb"); eDcoupling[6] = settingsPtr->parm("ExtraDimensionsG*:Gtt"); tmp_coup = settingsPtr->parm("ExtraDimensionsG*:Gll"); for (int i = 11; i <= 16; ++i) eDcoupling[i] = tmp_coup; eDcoupling[21] = settingsPtr->parm("ExtraDimensionsG*:Ggg"); eDcoupling[22] = settingsPtr->parm("ExtraDimensionsG*:Ggmgm"); eDcoupling[23] = settingsPtr->parm("ExtraDimensionsG*:GZZ"); eDcoupling[24] = settingsPtr->parm("ExtraDimensionsG*:GWW"); eDcoupling[25] = settingsPtr->parm("ExtraDimensionsG*:Ghh"); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceGraviton::calcPreFac(bool) { // Common coupling factors. alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = mHat / M_PI; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceGraviton::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // Widths to fermion pairs. if (id1Abs < 19) { widNow = preFac * pow3(ps) * (1. + 8. * mr1 / 3.) / 320.; if (id1Abs < 9) widNow *= colQ; // Widths to gluon and photon pair. } else if (id1Abs == 21) { widNow = preFac / 20.; } else if (id1Abs == 22) { widNow = preFac / 160.; // Widths to Z0 Z0 and W+ W- pair. } else if (id1Abs == 23 || id1Abs == 24) { // Longitudinal W/Z only. if (eDvlvl) { widNow = preFac * pow(ps,5) / 480.; // Transverse W/Z contributions as well. } else { widNow = preFac * ps * (13. / 12. + 14. * mr1 / 3. + 4. * mr1 * mr1) / 80.; } if (id1Abs == 23) widNow *= 0.5; // Widths to h h pair. } else if (id1Abs == 25) { widNow = preFac * pow(ps,5) / 960.; } // RS graviton coupling if (eDsmbulk) widNow *= 2. * pow2(eDcoupling[min( id1Abs, 26)] * mHat); else widNow *= pow2(kappaMG); } //========================================================================== // The ResonanceKKgluon class. // Derived class for excited kk-gluon properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceKKgluon::initConstants() { // KK-gluon gv/ga couplings and interference. for (int i = 0; i < 10; ++i) { eDgv[i] = 0.; eDga[i] = 0.; } double tmp_gL = settingsPtr->parm("ExtraDimensionsG*:KKgqL"); double tmp_gR = settingsPtr->parm("ExtraDimensionsG*:KKgqR"); for (int i = 1; i <= 4; ++i) { eDgv[i] = 0.5 * (tmp_gL + tmp_gR); eDga[i] = 0.5 * (tmp_gL - tmp_gR); } tmp_gL = settingsPtr->parm("ExtraDimensionsG*:KKgbL"); tmp_gR = settingsPtr->parm("ExtraDimensionsG*:KKgbR"); eDgv[5] = 0.5 * (tmp_gL + tmp_gR); eDga[5] = 0.5 * (tmp_gL - tmp_gR); tmp_gL = settingsPtr->parm("ExtraDimensionsG*:KKgtL"); tmp_gR = settingsPtr->parm("ExtraDimensionsG*:KKgtR"); eDgv[6] = 0.5 * (tmp_gL + tmp_gR); eDga[6] = 0.5 * (tmp_gL - tmp_gR); interfMode = settingsPtr->mode("ExtraDimensionsG*:KKintMode"); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceKKgluon::calcPreFac(bool calledFromInit) { // Common coupling factors. alpS = couplingsPtr->alphaS(mHat * mHat); preFac = alpS * mHat / 6; // When call for incoming flavour need to consider g*/gKK mix. if (!calledFromInit) { // Calculate prefactors for g/interference/gKK terms. int idInFlavAbs = abs(idInFlav); double sH = mHat * mHat; normSM = 1; normInt = 2. * eDgv[min(idInFlavAbs, 9)] * sH * (sH - m2Res) / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); normKK = ( pow2(eDgv[min(idInFlavAbs, 9)]) + pow2(eDga[min(idInFlavAbs, 9)]) ) * sH * sH / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); // Optionally only keep g* or gKK term. if (interfMode == 1) {normInt = 0.; normKK = 0.;} if (interfMode == 2) {normSM = 0.; normInt = 0.; normKK = 1.;} } } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceKKgluon::calcWidth(bool calledFromInit) { // Check that above threshold. if (ps == 0.) return; // Widths to quark pairs. if (id1Abs > 9) return; if (calledFromInit) { widNow = preFac * ps * (pow2(eDgv[min(id1Abs, 9)]) * (1. + 2.*mr1) + pow2(eDga[min(id1Abs, 9)]) * (1. - 4.*mr1) ); } else { // Relative outwidths: combine instate, propagator and outstate. widNow = normSM * ps * (1. + 2. * mr1) + normInt * ps * eDgv[min(id1Abs, 9)] * (1. + 2. * mr1) + normKK * ps * (pow2(eDgv[min(id1Abs, 9)]) * (1. + 2.*mr1) + pow2(eDga[min(id1Abs, 9)]) * (1. - 4.*mr1) ); widNow *= preFac; } } //========================================================================== // The ResonanceLeptoquark class. // Derived class for leptoquark properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceLeptoquark::initConstants() { // Locally stored properties and couplings. kCoup = settingsPtr->parm("LeptoQuark:kCoup"); // Check that flavour info in decay channel is correctly set. int id1Now = particlePtr->channel(0).product(0); int id2Now = particlePtr->channel(0).product(1); if (id1Now < 1 || id1Now > 5) { infoPtr->errorMsg("Error in ResonanceLeptoquark::init:" " unallowed input quark flavour reset to u"); id1Now = 2; particlePtr->channel(0).product(0, id1Now); } if (abs(id2Now) < 11 || abs(id2Now) > 16) { infoPtr->errorMsg("Error in ResonanceLeptoquark::init:" " unallowed input lepton flavour reset to e-"); id2Now = 11; particlePtr->channel(0).product(1, id2Now); } // Set/overwrite charge and name of particle. bool changed = particlePtr->hasChanged(); int chargeLQ = particleDataPtr->chargeType(id1Now) + particleDataPtr->chargeType(id2Now); particlePtr->setChargeType(chargeLQ); string nameLQ = "LQ_" + particleDataPtr->name(id1Now) + "," + particleDataPtr->name(id2Now); particlePtr->setNames(nameLQ, nameLQ + "bar"); if (!changed) particlePtr->setHasChanged(false); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceLeptoquark::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); preFac = 0.25 * alpEM * kCoup * mHat; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceLeptoquark::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // Width into lepton plus quark. if (id1Abs > 10 && id1Abs < 17 && id2Abs < 7) widNow = preFac * pow3(ps); } //========================================================================== // The ResonanceNuRight class. // Derived class for righthanded Majorana neutrino properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceNuRight::initConstants() { // Locally stored properties and couplings: righthanded W mass. thetaWRat = 1. / (768. * M_PI * pow2(couplingsPtr->sin2thetaW())); mWR = particleDataPtr->m0(9900024); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceNuRight::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = pow2(alpEM) * thetaWRat * pow5(mHat) / pow4(max(mHat, mWR)); } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceNuRight::calcWidth(bool) { // Check that above threshold. if (mHat < mf1 + mf2 + mf3 + MASSMARGIN) return; // Coupling part of widths to l- q qbar', l- l'+ nu_lR' and c.c. widNow = (id2Abs < 9 && id3Abs < 9) ? preFac * colQ * couplingsPtr->V2CKMid(id2, id3) : preFac; // Phase space corrections in decay. Must have y < 1. double x = (mf1 + mf2 + mf3) / mHat; double x2 = x * x; double fx = 1. - 8. * x2 + 8. * pow3(x2) - pow4(x2) - 24. * pow2(x2) * log(x); double y = min( 0.999, pow2(mHat / mWR) ); double fy = ( 12. * (1. - y) * log(1. - y) + 12. * y - 6. * y*y - 2.* pow3(y) ) / pow4(y); widNow *= fx * fy; } //========================================================================== // The ResonanceZRight class. // Derived class for Z_R^0 properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceZRight::initConstants() { // Locally stored properties and couplings: righthanded W mass. sin2tW = couplingsPtr->sin2thetaW(); thetaWRat = 1. / (48. * sin2tW * (1. - sin2tW) * (1. - 2. * sin2tW) ); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceZRight::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = alpEM * thetaWRat * mHat; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceZRight::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // Couplings to q qbar and l+ l-. double vf = 0.; double af = 0.; double symMaj = 1.; if (id1Abs < 9 && id1Abs%2 == 1) { af = -1. + 2. * sin2tW; vf = -1. + 4. * sin2tW / 3.; } else if (id1Abs < 9) { af = 1. - 2. * sin2tW; vf = 1. - 8. * sin2tW / 3.; } else if (id1Abs < 19 && id1Abs%2 == 1) { af = -1. + 2. * sin2tW; vf = -1. + 4. * sin2tW; // Couplings to nu_L nu_Lbar and nu_R nu_Rbar, both assumed Majoranas. } else if (id1Abs < 19) { af = -2. * sin2tW; vf = 0.; symMaj = 0.5; } else { af = 2. * (1. - sin2tW); vf = 0.; symMaj = 0.5; } // Width expression, including phase space and colour factor. widNow = preFac * (vf*vf * (1. + 2. * mr1) + af*af * ps*ps) * ps * symMaj; if (id1Abs < 9) widNow *= colQ; } //========================================================================== // The ResonanceWRight class. // Derived class for W_R+- properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceWRight::initConstants() { // Locally stored properties and couplings. thetaWRat = 1. / (12. * couplingsPtr->sin2thetaW()); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceWRight::calcPreFac(bool) { // Common coupling factors. alpEM = couplingsPtr->alphaEM(mHat * mHat); alpS = couplingsPtr->alphaS(mHat * mHat); colQ = 3. * (1. + alpS / M_PI); preFac = alpEM * thetaWRat * mHat; } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceWRight::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // Combine kinematics with colour factor and CKM couplings. widNow = preFac * (1. - 0.5 * (mr1 + mr2) - 0.5 * pow2(mr1 - mr2)) * ps; if (id1Abs < 9) widNow *= colQ * couplingsPtr->V2CKMid(id1Abs, id2Abs); } //========================================================================== // The ResonanceHchgchgLeft class. // Derived class for H++/H-- (left) properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceHchgchgLeft::initConstants() { // Read in Yukawa matrix for couplings to a lepton pair. yukawa[1][1] = settingsPtr->parm("LeftRightSymmmetry:coupHee"); yukawa[2][1] = settingsPtr->parm("LeftRightSymmmetry:coupHmue"); yukawa[2][2] = settingsPtr->parm("LeftRightSymmmetry:coupHmumu"); yukawa[3][1] = settingsPtr->parm("LeftRightSymmmetry:coupHtaue"); yukawa[3][2] = settingsPtr->parm("LeftRightSymmmetry:coupHtaumu"); yukawa[3][3] = settingsPtr->parm("LeftRightSymmmetry:coupHtautau"); // Locally stored properties and couplings. gL = settingsPtr->parm("LeftRightSymmmetry:gL"); vL = settingsPtr->parm("LeftRightSymmmetry:vL"); mW = particleDataPtr->m0(24); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceHchgchgLeft::calcPreFac(bool) { // Common coupling factors. preFac = mHat / (8. * M_PI); } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceHchgchgLeft::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // H++-- width to a pair of leptons. Combinatorial factor of 2. if (id1Abs < 17 && id2Abs < 17) { widNow = preFac * pow2(yukawa[(id1Abs-9)/2][(id2Abs-9)/2]) * ps; if (id2Abs != id1Abs) widNow *= 2.; } // H++-- width to a pair of lefthanded W's. else if (id1Abs == 24 && id2Abs == 24) widNow = preFac * 0.5 * pow2(gL*gL * vL / mW) * (3. * mr1 + 0.25 / mr1 - 1.) * ps; } //========================================================================== // The ResonanceHchgchgRight class. // Derived class for H++/H-- (right) properties. //-------------------------------------------------------------------------- // Initialize constants. void ResonanceHchgchgRight::initConstants() { // Read in Yukawa matrix for couplings to a lepton pair. yukawa[1][1] = settingsPtr->parm("LeftRightSymmmetry:coupHee"); yukawa[2][1] = settingsPtr->parm("LeftRightSymmmetry:coupHmue"); yukawa[2][2] = settingsPtr->parm("LeftRightSymmmetry:coupHmumu"); yukawa[3][1] = settingsPtr->parm("LeftRightSymmmetry:coupHtaue"); yukawa[3][2] = settingsPtr->parm("LeftRightSymmmetry:coupHtaumu"); yukawa[3][3] = settingsPtr->parm("LeftRightSymmmetry:coupHtautau"); // Locally stored properties and couplings. idWR = 9000024; gR = settingsPtr->parm("LeftRightSymmmetry:gR"); } //-------------------------------------------------------------------------- // Calculate various common prefactors for the current mass. void ResonanceHchgchgRight::calcPreFac(bool) { // Common coupling factors. preFac = mHat / (8. * M_PI); } //-------------------------------------------------------------------------- // Calculate width for currently considered channel. void ResonanceHchgchgRight::calcWidth(bool) { // Check that above threshold. if (ps == 0.) return; // H++-- width to a pair of leptons. Combinatorial factor of 2. if (id1Abs < 17 && id2Abs < 17) { widNow = preFac * pow2(yukawa[(id1Abs-9)/2][(id2Abs-9)/2]) * ps; if (id2Abs != id1Abs) widNow *= 2.; } // H++-- width to a pair of lefthanded W's. else if (id1Abs == idWR && id2Abs == idWR) widNow = preFac * pow2(yukawa[(id1Abs-9)/2][(id2Abs-9)/2]) * ps; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/Pythia.cc0000644000175000017500000021760012217346247014703 0ustar sunsun// Pythia.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the Pythia class. #include "Pythia8/Pythia.h" // Access time information. #include // Allow string and character manipulation. #include namespace Pythia8 { //========================================================================== // The Pythia class. //-------------------------------------------------------------------------- // The current Pythia (sub)version number, to agree with XML version. const double Pythia::VERSIONNUMBERCODE = 8.180; //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Maximum number of tries to produce parton level from given input. const int Pythia::NTRY = 10; // Negative integer to denote that no subrun has been set. const int Pythia::SUBRUNDEFAULT = -999; //-------------------------------------------------------------------------- // Constructor. Pythia::Pythia(string xmlDir, bool printBanner) { // Initial values for pointers to PDF's. useNewPdfA = false; useNewPdfB = false; useNewPdfHard = false; useNewPdfPomA = false; useNewPdfPomB = false; pdfAPtr = 0; pdfBPtr = 0; pdfHardAPtr = 0; pdfHardBPtr = 0; pdfPomAPtr = 0; pdfPomBPtr = 0; // Initial values for pointers to Les Houches Event objects. doLHA = false; useNewLHA = false; lhaUpPtr = 0; //Initial value for couplings pointer couplingsPtr = &couplings; // Initial value for pointer to external decay handler. decayHandlePtr = 0; // Initial value for pointer to user hooks. userHooksPtr = 0; // Initial value for pointer to merging hooks. doMerging = false; hasMergingHooks = false; hasOwnMergingHooks = false; mergingHooksPtr = 0; // Initial value for pointer to beam shape. useNewBeamShape = false; beamShapePtr = 0; // Initial values for pointers to timelike and spacelike showers. useNewTimes = false; useNewSpace = false; timesDecPtr = 0; timesPtr = 0; spacePtr = 0; // Find path to data files, i.e. xmldoc directory location. // Environment variable takes precedence, else use constructor input. xmlPath = ""; const char* PYTHIA8DATA = "PYTHIA8DATA"; char* envPath = getenv(PYTHIA8DATA); if (envPath != 0 && *envPath != '\0') { int i = 0; while (*(envPath+i) != '\0') xmlPath += *(envPath+(i++)); } else xmlPath = xmlDir; if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; // Read in files with all flags, modes, parms and words. settings.initPtr( &info); string initFile = xmlPath + "Index.xml"; isConstructed = settings.init( initFile); if (!isConstructed) { info.errorMsg("Abort from Pythia::Pythia: settings unavailable"); return; } // Check that XML version number matches code version number. double versionNumberXML = parm("Pythia:versionNumber"); isConstructed = (abs(versionNumberXML - VERSIONNUMBERCODE) < 0.0005); if (!isConstructed) { ostringstream errCode; errCode << fixed << setprecision(3) << ": in code " << VERSIONNUMBERCODE << " but in XML " << versionNumberXML; info.errorMsg("Abort from Pythia::Pythia: unmatched version numbers", errCode.str()); return; } // Read in files with all particle data. particleData.initPtr( &info, &settings, &rndm, couplingsPtr); string dataFile = xmlPath + "ParticleData.xml"; isConstructed = particleData.init( dataFile); if (!isConstructed) { info.errorMsg("Abort from Pythia::Pythia: particle data unavailable"); return; } // Write the Pythia banner to output. if (printBanner) banner(); // Not initialized until at the end of the init() call. isInit = false; info.addCounter(0); } //-------------------------------------------------------------------------- // Destructor. Pythia::~Pythia() { // Delete the PDF's created with new. if (useNewPdfHard && pdfHardAPtr != pdfAPtr) delete pdfHardAPtr; if (useNewPdfHard && pdfHardBPtr != pdfBPtr) delete pdfHardBPtr; if (useNewPdfA) delete pdfAPtr; if (useNewPdfB) delete pdfBPtr; if (useNewPdfPomA) delete pdfPomAPtr; if (useNewPdfPomB) delete pdfPomBPtr; // Delete the Les Houches object created with new. if (useNewLHA) delete lhaUpPtr; // Delete the MergingHooks object created with new. if (hasOwnMergingHooks) delete mergingHooksPtr; // Delete the BeamShape object created with new. if (useNewBeamShape) delete beamShapePtr; // Delete the timelike and spacelike showers created with new. if (useNewTimes) delete timesPtr; if (useNewSpace) delete spacePtr; } //-------------------------------------------------------------------------- // Read in one update for a setting or particle data from a single line. bool Pythia::readString(string line, bool warn) { // Check that constructor worked. if (!isConstructed) return false; // If empty line then done. if (line.find_first_not_of(" \n\t\v\b\r\f\a") == string::npos) return true; // If first character is not a letter/digit, then taken to be a comment. int firstChar = line.find_first_not_of(" \n\t\v\b\r\f\a"); if (!isalnum(line[firstChar])) return true; // Send on particle data to the ParticleData database. if (isdigit(line[firstChar])) return particleData.readString(line, warn); // Everything else sent on to Settings. return settings.readString(line, warn); } //-------------------------------------------------------------------------- // Read in updates for settings or particle data from user-defined file. bool Pythia::readFile(string fileName, bool warn, int subrun) { // Check that constructor worked. if (!isConstructed) return false; // Open file for reading. const char* cstring = fileName.c_str(); ifstream is(cstring); if (!is.good()) { info.errorMsg("Error in Pythia::readFile: did not find file", fileName); return false; } // Hand over real work to next method. return readFile( is, warn, subrun); } //-------------------------------------------------------------------------- // Read in updates for settings or particle data // from user-defined stream (or file). bool Pythia::readFile(istream& is, bool warn, int subrun) { // Check that constructor worked. if (!isConstructed) return false; // Read in one line at a time. string line; bool accepted = true; int subrunNow = SUBRUNDEFAULT; while ( getline(is, line) ) { // Check whether entered new subrun. int subrunLine = readSubrun( line, warn); if (subrunLine >= 0) subrunNow = subrunLine; // Process the line if in correct subrun. if ( (subrunNow == subrun || subrunNow == SUBRUNDEFAULT) && !readString( line, warn) ) accepted = false; // Reached end of input file. }; return accepted; } //-------------------------------------------------------------------------- // Routine to pass in pointers to PDF's. Usage optional. bool Pythia::setPDFPtr( PDF* pdfAPtrIn, PDF* pdfBPtrIn, PDF* pdfHardAPtrIn, PDF* pdfHardBPtrIn, PDF* pdfPomAPtrIn, PDF* pdfPomBPtrIn) { // Delete any PDF's created in a previous init call. if (useNewPdfHard && pdfHardAPtr != pdfAPtr) delete pdfHardAPtr; if (useNewPdfHard && pdfHardBPtr != pdfBPtr) delete pdfHardBPtr; if (useNewPdfA) delete pdfAPtr; if (useNewPdfB) delete pdfBPtr; if (useNewPdfPomA) delete pdfPomAPtr; if (useNewPdfPomB) delete pdfPomBPtr; // Reset pointers to be empty. useNewPdfA = false; useNewPdfB = false; useNewPdfHard = false; useNewPdfPomA = false; useNewPdfPomB = false; pdfAPtr = 0; pdfBPtr = 0; pdfHardAPtr = 0; pdfHardBPtr = 0; pdfPomAPtr = 0; pdfPomBPtr = 0; // Switch off external PDF's by zero as input. if (pdfAPtrIn == 0 && pdfBPtrIn == 0) return true; // The two PDF objects cannot be one and the same. if (pdfAPtrIn == pdfBPtrIn) return false; // Save pointers. pdfAPtr = pdfAPtrIn; pdfBPtr = pdfBPtrIn; // By default same pointers for hard-process PDF's. pdfHardAPtr = pdfAPtrIn; pdfHardBPtr = pdfBPtrIn; // Optionally allow separate pointers for hard process. if (pdfHardAPtrIn != 0 && pdfHardBPtrIn != 0) { if (pdfHardAPtrIn == pdfHardBPtrIn) return false; pdfHardAPtr = pdfHardAPtrIn; pdfHardBPtr = pdfHardBPtrIn; } // Optionally allow pointers for Pomerons in the proton. if (pdfPomAPtrIn != 0 && pdfPomBPtrIn != 0) { if (pdfPomAPtrIn == pdfPomBPtrIn) return false; pdfPomAPtr = pdfPomAPtrIn; pdfPomBPtr = pdfPomBPtrIn; } // Done. return true; } //-------------------------------------------------------------------------- // Routine to initialize with the variable values of the Beams kind. bool Pythia::init() { // Check that constructor worked. isInit = false; if (!isConstructed) { info.errorMsg("Abort from Pythia::init: constructur " "initialization failed"); return false; } // Early readout to be safe in case of a return false. doProcessLevel = settings.flag("ProcessLevel:all"); // Check that changes in Settings and ParticleData have worked. if (settings.readingFailed()) { info.errorMsg("Abort from Pythia::init: some user settings " "did not make sense"); return false; } if (particleData.readingFailed()) { info.errorMsg("Abort from Pythia::init: some user particle data " "did not make sense"); return false; } // Begin initialization. Find which frame type to use. info.addCounter(1); frameType = mode("Beams:frameType"); // Initialization with internal processes: read in and set values. if (frameType < 4 ) { doLHA = false; boostType = frameType; idA = mode("Beams:idA"); idB = mode("Beams:idB"); eCM = parm("Beams:eCM"); eA = parm("Beams:eA"); eB = parm("Beams:eB"); pxA = parm("Beams:pxA"); pyA = parm("Beams:pyA"); pzA = parm("Beams:pzA"); pxB = parm("Beams:pxB"); pyB = parm("Beams:pyB"); pzB = parm("Beams:pzB"); // Initialization with a Les Houches Event File or an LHAup object. } else { doLHA = true; boostType = 2; string lhef = word("Beams:LHEF"); string lhefHeader = word("Beams:LHEFheader"); bool readHeaders = flag("Beams:readLHEFheaders"); bool skipInit = flag("Beams:newLHEFsameInit"); int nSkipAtInit = mode("Beams:nSkipLHEFatInit"); // For file input: renew file stream or (re)new Les Houches object. if (frameType == 4) { const char* cstring1 = lhef.c_str(); if (useNewLHA && skipInit) lhaUpPtr->newEventFile(cstring1); else { if (useNewLHA) delete lhaUpPtr; // Header is optional, so use NULL pointer to indicate no value. const char* cstring2 = (lhefHeader == "void") ? NULL : lhefHeader.c_str(); lhaUpPtr = new LHAupLHEF(cstring1, cstring2, readHeaders); useNewLHA = true; } // Check that file was properly opened. if (!lhaUpPtr->fileFound()) { info.errorMsg("Abort from Pythia::init: " "Les Houches Event File not found"); return false; } // For object input: at least check that not null pointer. } else { if (lhaUpPtr == 0) { info.errorMsg("Abort from Pythia::init: " "LHAup object not found"); return false; } // LHAup object generic abort using fileFound() routine if (!lhaUpPtr->fileFound()) { info.errorMsg("Abort from Pythia::init: " "LHAup initialisation error"); return false; } } // Send in pointer to info. Store or replace LHA pointer in other classes. lhaUpPtr->setPtr( &info); processLevel.setLHAPtr( lhaUpPtr); // If second time around, only with new file, then simplify. // Optionally skip ahead a number of events at beginning of file. if (skipInit) { isInit = true; info.addCounter(2); if (nSkipAtInit > 0) lhaUpPtr->skipEvent(nSkipAtInit); return true; } // Set up values related to merging hooks. if (frameType == 4 || frameType == 5) { // Set up values related to CKKW-L merging. bool doUserMerging = settings.flag("Merging:doUserMerging"); bool doMGMerging = settings.flag("Merging:doMGMerging"); bool doKTMerging = settings.flag("Merging:doKTMerging"); bool doPTLundMerging = settings.flag("Merging:doPTLundMerging"); bool doCutBasedMerging = settings.flag("Merging:doCutBasedMerging"); // Set up values related to unitarised CKKW merging bool doUMEPSTree = settings.flag("Merging:doUMEPSTree"); bool doUMEPSSubt = settings.flag("Merging:doUMEPSSubt"); // Set up values related to NL3 NLO merging bool doNL3Tree = settings.flag("Merging:doNL3Tree"); bool doNL3Loop = settings.flag("Merging:doNL3Loop"); bool doNL3Subt = settings.flag("Merging:doNL3Subt"); // Set up values related to unitarised NLO merging bool doUNLOPSTree = settings.flag("Merging:doUNLOPSTree"); bool doUNLOPSLoop = settings.flag("Merging:doUNLOPSLoop"); bool doUNLOPSSubt = settings.flag("Merging:doUNLOPSSubt"); bool doUNLOPSSubtNLO = settings.flag("Merging:doUNLOPSSubtNLO"); bool doXSectionEst = settings.flag("Merging:doXSectionEstimate"); doMerging = doUserMerging || doMGMerging || doKTMerging || doPTLundMerging || doCutBasedMerging || doUMEPSTree || doUMEPSSubt || doNL3Tree || doNL3Loop || doNL3Subt || doUNLOPSTree || doUNLOPSLoop || doUNLOPSSubt || doUNLOPSSubtNLO || doXSectionEst; // Set up MergingHooks object. bool inputMergingHooks = (mergingHooksPtr != 0); if (doMerging && !inputMergingHooks){ if (hasOwnMergingHooks && mergingHooksPtr) delete mergingHooksPtr; mergingHooksPtr = new MergingHooks(); hasOwnMergingHooks = true; } hasMergingHooks = (mergingHooksPtr != 0); // Merging hooks required for merging. If no merging hooks pointer is // available, exit. if (doMerging && !hasMergingHooks) { info.errorMsg("Abort from Pythia::init: " "no merging hooks object has been provided"); return false; } else if (doMerging) { string lhefIn = (frameType == 4) ? lhef : ""; mergingHooksPtr->setLHEInputFile( lhefIn); } // Initialise counting of Les Houches Events significantly above the // merging scale. info.setCounter(41,0); } // Set LHAinit information (in some external program). if (settings.flag("ProcessLevel:all") && !lhaUpPtr->setInit()) { info.errorMsg("Abort from Pythia::init: " "Les Houches initialization failed"); return false; } // Extract beams from values set in an LHAinit object. idA = lhaUpPtr->idBeamA(); idB = lhaUpPtr->idBeamB(); eA = lhaUpPtr->eBeamA(); eB = lhaUpPtr->eBeamB(); // Optionally skip ahead a number of events at beginning of file. if (nSkipAtInit > 0) lhaUpPtr->skipEvent(nSkipAtInit); } // Set up values related to user hooks. hasUserHooks = (userHooksPtr != 0); doVetoProcess = false; doVetoPartons = false; retryPartonLevel = false; if (hasUserHooks) { userHooksPtr->initPtr( &info, &settings, &particleData, &rndm, &beamA, &beamB, &beamPomA, &beamPomB, couplingsPtr, &partonSystems, &sigmaTot); if (!userHooksPtr->initAfterBeams()) { info.errorMsg("Abort from Pythia::init: could not initialise UserHooks"); return false; } doVetoProcess = userHooksPtr->canVetoProcessLevel(); doVetoPartons = userHooksPtr->canVetoPartonLevel(); retryPartonLevel = userHooksPtr->retryPartonLevel(); } // Back to common initialization. Reset error counters. nErrEvent = 0; info.setTooLowPTmin(false); info.sigmaReset(); // Initialize data members extracted from database. doProcessLevel = settings.flag("ProcessLevel:all"); doPartonLevel = settings.flag("PartonLevel:all"); doHadronLevel = settings.flag("HadronLevel:all"); doDiffraction = settings.flag("SoftQCD:all") || settings.flag("SoftQCD:singleDiffractive") || settings.flag("SoftQCD:doubleDiffractive") || settings.flag("SoftQCD:centralDiffractive") || settings.flag("SoftQCD:inelastic"); doResDec = settings.flag("Standalone:allowResDec"); doFSRinRes = doPartonLevel && settings.flag("PartonLevel:FSR") && settings.flag("PartonLevel:FSRinResonances"); decayRHadrons = settings.flag("RHadrons:allowDecay"); doMomentumSpread = settings.flag("Beams:allowMomentumSpread"); doVertexSpread = settings.flag("Beams:allowVertexSpread"); abortIfVeto = settings.flag("Check:abortIfVeto"); checkEvent = settings.flag("Check:event"); checkHistory = settings.flag("Check:history"); nErrList = settings.mode("Check:nErrList"); epTolErr = settings.parm("Check:epTolErr"); epTolWarn = settings.parm("Check:epTolWarn"); // Initialise merging hooks. if ( doMerging && (hasMergingHooks || hasOwnMergingHooks) ) mergingHooksPtr->init( settings, &info, &particleData, &partonSystems ); // Initialize the random number generator. if ( settings.flag("Random:setSeed") ) rndm.init( settings.mode("Random:seed") ); // Check that combinations of settings are allowed; change if not. checkSettings(); // Initialize the SM couplings (needed to initialize resonances). couplingsPtr->init( settings, &rndm ); // Initialize SLHA interface (including SLHA/BSM couplings). bool useSLHAcouplings = false; slhaInterface.setPtr( &info ); slhaInterface.init( settings, &rndm, couplingsPtr, &particleData, useSLHAcouplings ); if (useSLHAcouplings) couplingsPtr = slhaInterface.couplingsPtr; // Reset couplingsPtr to the correct memory address. particleData.initPtr( &info, &settings, &rndm, couplingsPtr); if (hasUserHooks) userHooksPtr->initPtr( &info, &settings, &particleData, &rndm, &beamA, &beamB, &beamPomA, &beamPomB, couplingsPtr, &partonSystems, &sigmaTot); // Set headers to distinguish the two event listing kinds. int startColTag = settings.mode("Event:startColTag"); process.init("(hard process)", &particleData, startColTag); event.init("(complete event)", &particleData, startColTag); // Final setup stage of particle data, notably resonance widths. particleData.initWidths( resonancePtrs); // Set up R-hadrons particle data, where relevant. rHadrons.init( &info, settings, &particleData, &rndm); // Set up objects for timelike and spacelike showers. if (timesDecPtr == 0 || timesPtr == 0) { TimeShower* timesNow = new TimeShower(); if (timesDecPtr == 0) timesDecPtr = timesNow; if (timesPtr == 0) timesPtr = timesNow; useNewTimes = true; } if (spacePtr == 0) { spacePtr = new SpaceShower(); useNewSpace = true; } // Initialize showers, especially for simple showers in decays. timesPtr->initPtr( &info, &settings, &particleData, &rndm, couplingsPtr, &partonSystems, userHooksPtr, mergingHooksPtr); timesDecPtr->initPtr( &info, &settings, &particleData, &rndm, couplingsPtr, &partonSystems, userHooksPtr, mergingHooksPtr); spacePtr->initPtr( &info, &settings, &particleData, &rndm, couplingsPtr, &partonSystems, userHooksPtr, mergingHooksPtr); timesDecPtr->init( 0, 0); // Set up values related to beam shape. if (beamShapePtr == 0) { beamShapePtr = new BeamShape(); useNewBeamShape = true; } beamShapePtr->init( settings, &rndm); // Check that beams and beam combination can be handled. if (!checkBeams()) { info.errorMsg("Abort from Pythia::init: " "checkBeams initialization failed"); return false; } // Do not set up beam kinematics when no process level. if (!doProcessLevel) boostType = 1; else { // Set up beam kinematics. if (!initKinematics()) { info.errorMsg("Abort from Pythia::init: " "kinematics initialization failed"); return false; } // Set up pointers to PDFs. if (!initPDFs()) { info.errorMsg("Abort from Pythia::init: PDF initialization failed"); return false; } // Set up the two beams and the common remnant system. StringFlav* flavSelPtr = hadronLevel.getStringFlavPtr(); beamA.init( idA, pzAcm, eA, mA, &info, settings, &particleData, &rndm, pdfAPtr, pdfHardAPtr, isUnresolvedA, flavSelPtr); beamB.init( idB, pzBcm, eB, mB, &info, settings, &particleData, &rndm, pdfBPtr, pdfHardBPtr, isUnresolvedB, flavSelPtr); // Optionally set up new alternative beams for these Pomerons. if ( doDiffraction) { beamPomA.init( 990, 0.5 * eCM, 0.5 * eCM, 0., &info, settings, &particleData, &rndm, pdfPomAPtr, pdfPomAPtr, false, flavSelPtr); beamPomB.init( 990, -0.5 * eCM, 0.5 * eCM, 0., &info, settings, &particleData, &rndm, pdfPomBPtr, pdfPomBPtr, false, flavSelPtr); } } // Send info/pointers to process level for initialization. if ( doProcessLevel && !processLevel.init( &info, settings, &particleData, &rndm, &beamA, &beamB, couplingsPtr, &sigmaTot, doLHA, &slhaInterface, userHooksPtr, sigmaPtrs) ) { info.errorMsg("Abort from Pythia::init: " "processLevel initialization failed"); return false; } // Optionally only initialize resonance decays. if ( !doProcessLevel && doResDec) processLevel.initDecays( &info, &particleData, &rndm, lhaUpPtr); // Send info/pointers to parton level for initialization. if ( doPartonLevel && doProcessLevel && !partonLevel.init( &info, settings, &particleData, &rndm, &beamA, &beamB, &beamPomA, &beamPomB, couplingsPtr, &partonSystems, &sigmaTot, timesDecPtr, timesPtr, spacePtr, &rHadrons, userHooksPtr, mergingHooksPtr, false) ) { info.errorMsg("Abort from Pythia::init: " "partonLevel initialization failed" ); return false; } // Optionally only initialize final-state showers in resonance decays. if ( (!doProcessLevel || !doPartonLevel) && doFSRinRes) partonLevel.init( &info, settings, &particleData, &rndm, 0, 0, 0, 0, couplingsPtr, &partonSystems, 0, timesDecPtr, 0, 0, &rHadrons, 0, 0, false); // Send info/pointers to parton level for trial shower initialization. if ( doMerging && !trialPartonLevel.init( &info, settings, &particleData, &rndm, &beamA, &beamB, &beamPomA, &beamPomB, couplingsPtr, &partonSystems, &sigmaTot, timesDecPtr, timesPtr, spacePtr, &rHadrons, NULL, mergingHooksPtr, true) ) { info.errorMsg("Abort from Pythia::init: " "trialPartonLevel initialization failed"); return false; } // Initialise the merging wrapper class. if (doMerging ) merging.init( &settings, &info, &particleData, &rndm, &beamA, &beamB, mergingHooksPtr, &trialPartonLevel ); // Send info/pointers to hadron level for initialization. // Note: forceHadronLevel() can come, so we must always initialize. if ( !hadronLevel.init( &info, settings, &particleData, &rndm, couplingsPtr, timesDecPtr, &rHadrons, decayHandlePtr, handledParticles) ) { info.errorMsg("Abort from Pythia::init: " "hadronLevel initialization failed"); return false; } // Optionally check particle data table for inconsistencies. if ( settings.flag("Check:particleData") ) particleData.checkTable( settings.mode("Check:levelParticleData") ); // Optionally show settings and particle data, changed or all. bool showCS = settings.flag("Init:showChangedSettings"); bool showAS = settings.flag("Init:showAllSettings"); bool showCPD = settings.flag("Init:showChangedParticleData"); bool showCRD = settings.flag("Init:showChangedResonanceData"); bool showAPD = settings.flag("Init:showAllParticleData"); int show1PD = settings.mode("Init:showOneParticleData"); bool showPro = settings.flag("Init:showProcesses"); if (showCS) settings.listChanged(); if (showAS) settings.listAll(); if (show1PD > 0) particleData.list(show1PD); if (showCPD) particleData.listChanged(showCRD); if (showAPD) particleData.listAll(); // Listing options for the next() routine. nCount = settings.mode("Next:numberCount"); nShowLHA = settings.mode("Next:numberShowLHA"); nShowInfo = settings.mode("Next:numberShowInfo"); nShowProc = settings.mode("Next:numberShowProcess"); nShowEvt = settings.mode("Next:numberShowEvent"); showSaV = settings.flag("Next:showScaleAndVertex"); showMaD = settings.flag("Next:showMothersAndDaughters"); // Succeeded. isInit = true; info.addCounter(2); if (useNewLHA && showPro) lhaUpPtr->listInit(); return true; } //-------------------------------------------------------------------------- // Routine to initialize with CM energy. bool Pythia::init( int idAin, int idBin, double eCMin) { // Set arguments in Settings database. settings.mode("Beams:idA", idAin); settings.mode("Beams:idB", idBin); settings.mode("Beams:frameType", 1); settings.parm("Beams:eCM", eCMin); // Send on to common initialization. return init(); } //-------------------------------------------------------------------------- // Routine to initialize with two collinear beams, energies specified. bool Pythia::init( int idAin, int idBin, double eAin, double eBin) { // Set arguments in Settings database. settings.mode("Beams:idA", idAin); settings.mode("Beams:idB", idBin); settings.mode("Beams:frameType", 2); settings.parm("Beams:eA", eAin); settings.parm("Beams:eB", eBin); // Send on to common initialization. return init(); } //-------------------------------------------------------------------------- // Routine to initialize with two beams specified by three-momenta. bool Pythia::init( int idAin, int idBin, double pxAin, double pyAin, double pzAin, double pxBin, double pyBin, double pzBin) { // Set arguments in Settings database. settings.mode("Beams:idA", idAin); settings.mode("Beams:idB", idBin); settings.mode("Beams:frameType", 3); settings.parm("Beams:pxA", pxAin); settings.parm("Beams:pyA", pyAin); settings.parm("Beams:pzA", pzAin); settings.parm("Beams:pxB", pxBin); settings.parm("Beams:pyB", pyBin); settings.parm("Beams:pzB", pzBin); // Send on to common initialization. return init(); } //-------------------------------------------------------------------------- // Routine to initialize when all info is given in a Les Houches Event File. bool Pythia::init( string LesHouchesEventFile, bool skipInit) { // Set arguments in Settings database. settings.mode("Beams:frameType", 4); settings.word("Beams:LHEF", LesHouchesEventFile); settings.flag("Beams:newLHEFsameInit", skipInit); // Send on to common initialization. return init(); } //-------------------------------------------------------------------------- // Routine to initialize when beam info is given in an LHAup object. bool Pythia::init( LHAup* lhaUpPtrIn) { // Store LHAup object and set arguments in Settings database. setLHAupPtr( lhaUpPtrIn); settings.mode("Beams:frameType", 5); // Send on to common initialization. return init(); } //-------------------------------------------------------------------------- // Check that combinations of settings are allowed; change if not. void Pythia::checkSettings() { // Double rescattering not allowed if ISR or FSR. if ((settings.flag("PartonLevel:ISR") || settings.flag("PartonLevel:FSR")) && settings.flag("MultipartonInteractions:allowDoubleRescatter")) { info.errorMsg("Warning in Pythia::checkSettings: " "double rescattering switched off since showering is on"); settings.flag("MultipartonInteractions:allowDoubleRescatter", false); } } //-------------------------------------------------------------------------- // Check that beams and beam combination can be handled. Set up unresolved. bool Pythia::checkBeams() { // Absolute flavours. If not to do process level then no check needed. int idAabs = abs(idA); int idBabs = abs(idB); if (!doProcessLevel) return true; // Neutrino beams always unresolved, charged lepton ones conditionally. bool isLeptonA = (idAabs > 10 && idAabs < 17); bool isLeptonB = (idBabs > 10 && idBabs < 17); bool isUnresLep = !settings.flag("PDF:lepton"); isUnresolvedA = isLeptonA && (idAabs%2 == 0 || isUnresLep); isUnresolvedB = isLeptonB && (idBabs%2 == 0 || isUnresLep); // Lepton-lepton collisions OK (including neutrinos) if both (un)resolved. if (isLeptonA && isLeptonB && isUnresolvedA == isUnresolvedB) return true; // MBR model only implemented for pp/ppbar/pbarp collisions. int PomFlux = settings.mode("Diffraction:PomFlux"); if (PomFlux == 5) { bool ispp = (idAabs == 2212 && idBabs == 2212); bool ispbarpbar = (idA == -2212 && idB == -2212); if (ispp && !ispbarpbar) return true; info.errorMsg("Error in Pythia::init: cannot handle this beam combination" " with PomFlux == 5"); return false; } // Hadron-hadron collisions OK, with Pomeron counted as hadron. bool isHadronA = (idAabs == 2212) || (idAabs == 2112) || (idA == 111) || (idAabs == 211) || (idA == 990); bool isHadronB = (idBabs == 2212) || (idBabs == 2112) || (idB == 111) || (idBabs == 211) || (idB == 990); if (isHadronA && isHadronB) return true; // If no case above then failed. info.errorMsg("Error in Pythia::init: cannot handle this beam combination"); return false; } //-------------------------------------------------------------------------- // Calculate kinematics at initialization. Store beam four-momenta. bool Pythia::initKinematics() { // Find masses. Initial guess that we are in CM frame. mA = particleData.m0(idA); mB = particleData.m0(idB); betaZ = 0.; gammaZ = 1.; // Collinear beams not in CM frame: find CM energy. if (boostType == 2) { eA = max(eA, mA); eB = max(eB, mB); pzA = sqrt(eA*eA - mA*mA); pzB = -sqrt(eB*eB - mB*mB); pAinit = Vec4( 0., 0., pzA, eA); pBinit = Vec4( 0., 0., pzB, eB); eCM = sqrt( pow2(eA + eB) - pow2(pzA + pzB) ); // Find boost to rest frame. betaZ = (pzA + pzB) / (eA + eB); gammaZ = (eA + eB) / eCM; if (abs(betaZ) < 1e-10) boostType = 1; } // Completely general beam directions: find CM energy. else if (boostType == 3) { eA = sqrt( pxA*pxA + pyA*pyA + pzA*pzA + mA*mA); eB = sqrt( pxB*pxB + pyB*pyB + pzB*pzB + mB*mB); pAinit = Vec4( pxA, pyA, pzA, eA); pBinit = Vec4( pxB, pyB, pzB, eB); eCM = (pAinit + pBinit).mCalc(); // Find boost+rotation needed to move from/to CM frame. MfromCM.reset(); MfromCM.fromCMframe( pAinit, pBinit); MtoCM = MfromCM; MtoCM.invert(); } // Fail if CM energy below beam masses. if (eCM < mA + mB) { info.errorMsg("Error in Pythia::initKinematics: too low energy"); return false; } // Set up CM-frame kinematics with beams along +-z axis. pzAcm = 0.5 * sqrtpos( (eCM + mA + mB) * (eCM - mA - mB) * (eCM - mA + mB) * (eCM + mA - mB) ) / eCM; pzBcm = -pzAcm; eA = sqrt(mA*mA + pzAcm*pzAcm); eB = sqrt(mB*mB + pzBcm*pzBcm); // If in CM frame then store beam four-vectors (else already done above). if (boostType != 2 && boostType != 3) { pAinit = Vec4( 0., 0., pzAcm, eA); pBinit = Vec4( 0., 0., pzBcm, eB); } // Store main info for access in process generation. info.setBeamA( idA, pzAcm, eA, mA); info.setBeamB( idB, pzBcm, eB, mB); info.setECM( eCM); // Must allow for generic boost+rotation when beam momentum spread. if (doMomentumSpread) boostType = 3; // Done. return true; } //-------------------------------------------------------------------------- // Set up pointers to PDFs. bool Pythia::initPDFs() { // Delete any PDF's created in a previous init call. if (useNewPdfHard) { if (pdfHardAPtr != pdfAPtr) { delete pdfHardAPtr; pdfHardAPtr = 0; } if (pdfHardBPtr != pdfBPtr) { delete pdfHardBPtr; pdfHardBPtr = 0; } useNewPdfHard = false; } if (useNewPdfA) { delete pdfAPtr; useNewPdfA = false; pdfAPtr = 0; } if (useNewPdfB) { delete pdfBPtr; useNewPdfB = false; pdfBPtr = 0; } if (useNewPdfPomA) { delete pdfPomAPtr; useNewPdfPomA = false; pdfPomAPtr = 0; } if (useNewPdfPomB) { delete pdfPomBPtr; useNewPdfPomB = false; pdfPomBPtr = 0; } // Set up the PDF's, if not already done. if (pdfAPtr == 0) { pdfAPtr = getPDFPtr(idA); if (pdfAPtr == 0 || !pdfAPtr->isSetup()) { info.errorMsg("Error in Pythia::init: " "could not set up PDF for beam A"); return false; } pdfHardAPtr = pdfAPtr; useNewPdfA = true; } if (pdfBPtr == 0) { pdfBPtr = getPDFPtr(idB); if (pdfBPtr == 0 || !pdfBPtr->isSetup()) { info.errorMsg("Error in Pythia::init: " "could not set up PDF for beam B"); return false; } pdfHardBPtr = pdfBPtr; useNewPdfB = true; } // Optionally set up separate PDF's for hard process. if (settings.flag("PDF:useHard") && useNewPdfA && useNewPdfB) { pdfHardAPtr = getPDFPtr(idA, 2); if (!pdfHardAPtr->isSetup()) return false; pdfHardBPtr = getPDFPtr(idB, 2); if (!pdfHardBPtr->isSetup()) return false; useNewPdfHard = true; } // Optionally set up Pomeron PDF's for diffractive physics. if ( doDiffraction) { if (pdfPomAPtr == 0) { pdfPomAPtr = getPDFPtr(990); useNewPdfPomA = true; } if (pdfPomBPtr == 0) { pdfPomBPtr = getPDFPtr(990); useNewPdfPomB = true; } } // Done. return true; } //-------------------------------------------------------------------------- // Main routine to generate the next event, using internal machinery. bool Pythia::next() { // Check that constructor worked. if (!isConstructed) return false; // Regularly print how many events have been generated. int nPrevious = info.getCounter(3); if (nCount > 0 && nPrevious > 0 && nPrevious%nCount == 0) cout << "\n Pythia::next(): " << nPrevious << " events have been generated " << endl; // Set/reset info counters specific to each event. info.addCounter(3); for (int i = 10; i < 13; ++i) info.setCounter(i); // Simpler option when no hard process, i.e. mainly hadron level. if (!doProcessLevel) { // Optionally fetch in resonance decays from LHA interface. if (doLHA && !processLevel.nextLHAdec( event)) { if (info.atEndOfFile()) info.errorMsg("Abort from Pythia::next:" " reached end of Les Houches Events File"); return false; } // Reset info array (while event record contains data). info.clear(); // Set correct energy for system. Vec4 pSum = 0.; for (int i = 1; i < event.size(); ++i) if (event[i].isFinal()) pSum += event[i].p(); event[0].p( pSum ); event[0].m( pSum.mCalc() ); // Generate hadronization and decays. bool status = forceHadronLevel(); if (status) info.addCounter(4); if (status && nPrevious < nShowEvt) event.list(showSaV, showMaD); return status; } // Reset arrays. info.clear(); process.clear(); event.clear(); partonSystems.clear(); beamA.clear(); beamB.clear(); beamPomA.clear(); beamPomB.clear(); // Can only generate event if initialization worked. if (!isInit) { info.errorMsg("Abort from Pythia::next: " "not properly initialized so cannot generate events"); return false; } // Pick beam momentum spread and beam vertex. if (doMomentumSpread || doVertexSpread) beamShapePtr->pick(); // Recalculate kinematics when beam momentum spread. if (doMomentumSpread) nextKinematics(); // Outer loop over hard processes; only relevant for user-set vetoes. for ( ; ; ) { info.addCounter(10); bool hasVetoed = false; // Provide the hard process that starts it off. Only one try. info.clear(); process.clear(); if ( !processLevel.next( process) ) { if (doLHA && info.atEndOfFile()) info.errorMsg("Abort from " "Pythia::next: reached end of Les Houches Events File"); else info.errorMsg("Abort from Pythia::next: " "processLevel failed; giving up"); return false; } info.addCounter(11); // Possibility for a user veto of the process-level event. if (doVetoProcess) { hasVetoed = userHooksPtr->doVetoProcessLevel( process); if (hasVetoed) { if (abortIfVeto) return false; continue; } } // Possibility to perform matrix element merging for this event. if (doMerging) { int veto = merging.mergeProcess( process ); // Apply possible merging scale cut. if ( veto == -1 ) { hasVetoed = true; if (abortIfVeto) return false; continue; // Exit because of vanishing no-emission probability. } else if ( veto == 0 ) break; // Redo resonance decays after the merging, in case the resonance // structure has been changed because of reclusterings. if (veto == 2 ) processLevel.nextDecays( process); } // Possibility to stop the generation at this stage. if (!doPartonLevel) { boostAndVertex( true, true); processLevel.accumulate(); info.addCounter(4); if (doLHA && nPrevious < nShowLHA) lhaUpPtr->listEvent(); if (nPrevious < nShowInfo) info.list(); if (nPrevious < nShowProc) process.list(showSaV, showMaD); return true; } // Save spare copy of process record in case of problems. Event processSave = process; int sizeMPI = info.sizeMPIarrays(); info.addCounter(12); for (int i = 14; i < 19; ++i) info.setCounter(i); // Allow up to ten tries for parton- and hadron-level processing. bool physical = true; for (int iTry = 0; iTry < NTRY; ++ iTry) { info.addCounter(14); physical = true; // Restore original process record if problems. if (iTry > 0) process = processSave; if (iTry > 0) info.resizeMPIarrays( sizeMPI); // Reset event record and (extracted partons from) beam remnants. event.clear(); beamA.clear(); beamB.clear(); beamPomA.clear(); beamPomB.clear(); partonSystems.clear(); // Parton-level evolution: ISR, FSR, MPI. if ( !partonLevel.next( process, event) ) { // Skip to next hard process for failure owing to deliberate veto, // or alternatively retry for the same hard process. hasVetoed = partonLevel.hasVetoed(); if (hasVetoed) { if (retryPartonLevel) { --iTry; continue; } if (abortIfVeto) return false; break; } // Else make a new try for other failures. info.errorMsg("Error in Pythia::next: " "partonLevel failed; try again"); physical = false; continue; } info.addCounter(15); // Possibility for a user veto of the parton-level event. if (doVetoPartons) { hasVetoed = userHooksPtr->doVetoPartonLevel( event); if (hasVetoed) { if (abortIfVeto) return false; break; } } // Boost to lab frame (before decays, for vertices). boostAndVertex( true, true); // Possibility to stop the generation at this stage. if (!doHadronLevel) { processLevel.accumulate(); partonLevel.accumulate(); // Optionally check final event for problems. if (checkEvent && !check()) { info.errorMsg("Abort from Pythia::next: " "check of event revealed problems"); return false; } info.addCounter(4); if (doLHA && nPrevious < nShowLHA) lhaUpPtr->listEvent(); if (nPrevious < nShowInfo) info.list(); if (nPrevious < nShowProc) process.list(showSaV, showMaD); if (nPrevious < nShowEvt) event.list(showSaV, showMaD); return true; } // Hadron-level: hadronization, decays. info.addCounter(16); if ( !hadronLevel.next( event) ) { info.errorMsg("Error in Pythia::next: " "hadronLevel failed; try again"); physical = false; continue; } // If R-hadrons have been formed, then (optionally) let them decay. if (decayRHadrons && rHadrons.exist() && !doRHadronDecays()) { info.errorMsg("Error in Pythia::next: " "decayRHadrons failed; try again"); physical = false; continue; } info.addCounter(17); // Optionally check final event for problems. if (checkEvent && !check()) { info.errorMsg("Error in Pythia::next: " "check of event revealed problems"); physical = false; continue; } // Stop parton- and hadron-level looping if you got this far. info.addCounter(18); break; } // If event vetoed then to make a new try. if (hasVetoed) { if (abortIfVeto) return false; continue; } // If event failed any other way (after ten tries) then give up. if (!physical) { info.errorMsg("Abort from Pythia::next: " "parton+hadronLevel failed; giving up"); return false; } // Process- and parton-level statistics. Event scale. processLevel.accumulate(); partonLevel.accumulate(); event.scale( process.scale() ); // End of outer loop over hard processes. Done with normal option. info.addCounter(13); break; } // List events. if (doLHA && nPrevious < nShowLHA) lhaUpPtr->listEvent(); if (nPrevious < nShowInfo) info.list(); if (nPrevious < nShowProc) process.list(showSaV,showMaD); if (nPrevious < nShowEvt) event.list(showSaV, showMaD); // Done. info.addCounter(4); return true; } //-------------------------------------------------------------------------- // Generate only the hadronization/decay stage, using internal machinery. // The "event" instance should already contain a parton-level configuration. bool Pythia::forceHadronLevel(bool findJunctions) { // Can only generate event if initialization worked. if (!isInit) { info.errorMsg("Abort from Pythia::forceHadronLevel: " "not properly initialized so cannot generate events"); return false; } // Check whether any junctions in system. (Normally done in ProcessLevel.) // Avoid it if there are no final-state coloured partons. if (findJunctions) { event.clearJunctions(); for (int i = 0; i < event.size(); ++i) if (event[i].isFinal() && (event[i].col() != 0 || event[i].acol() != 0)) { processLevel.findJunctions( event); break; } } // Save spare copy of event in case of failure. Event spareEvent = event; // Allow up to ten tries for hadron-level processing. bool physical = true; for (int iTry = 0; iTry < NTRY; ++ iTry) { physical = true; // Check whether any resonances need to be handled at process level. if (doResDec) { process = event; processLevel.nextDecays( process); bool hasDecays = false; for (int i = 1; i < process.size(); ++i) if (process[i].status() < 0) hasDecays = true; // Allow for showers if decays happened at process level. if (hasDecays) { if (doFSRinRes) { partonLevel.setupShowerSys( process, event); partonLevel.resonanceShowers( process, event, false); } else event = process; } } // Hadron-level: hadronization, decays. if (hadronLevel.next( event)) break; // If failure then warn, restore original configuration and try again. info.errorMsg("Error in Pythia::forceHadronLevel: " "hadronLevel failed; try again"); physical = false; event = spareEvent; } // Done for simpler option. if (!physical) { info.errorMsg("Abort from Pythia::forceHadronLevel: " "hadronLevel failed; giving up"); return false; } // Optionally check final event for problems. if (checkEvent && !check()) { info.errorMsg("Abort from Pythia::forceHadronLevel: " "check of event revealed problems"); return false; } // Done. return true; } //-------------------------------------------------------------------------- // Recalculate kinematics for each event when beam momentum has a spread. void Pythia::nextKinematics() { // Read out momentum shift to give current beam momenta. pAnow = pAinit + beamShapePtr->deltaPA(); pAnow.e( sqrt(pAnow.pAbs2() + mA * mA) ); pBnow = pBinit + beamShapePtr->deltaPB(); pBnow.e( sqrt(pBnow.pAbs2() + mB * mB) ); // Construct CM frame kinematics. eCM = (pAnow + pBnow).mCalc(); pzAcm = 0.5 * sqrtpos( (eCM + mA + mB) * (eCM - mA - mB) * (eCM - mA + mB) * (eCM + mA - mB) ) / eCM; pzBcm = -pzAcm; eA = sqrt(mA*mA + pzAcm*pzAcm); eB = sqrt(mB*mB + pzBcm*pzBcm); // Set relevant info for other classes to use. info.setBeamA( idA, pzAcm, eA, mA); info.setBeamB( idB, pzBcm, eB, mB); info.setECM( eCM); beamA.newPzE( pzAcm, eA); beamB.newPzE( pzBcm, eB); // Set boost/rotation matrices from/to CM frame. MfromCM.reset(); MfromCM.fromCMframe( pAnow, pBnow); MtoCM = MfromCM; MtoCM.invert(); } //-------------------------------------------------------------------------- // Boost from CM frame to lab frame, or inverse. Set production vertex. void Pythia::boostAndVertex( bool toLab, bool setVertex) { // Boost process from CM frame to lab frame. if (toLab) { if (boostType == 2) process.bst(0., 0., betaZ, gammaZ); else if (boostType == 3) process.rotbst(MfromCM); // Boost nonempty event from CM frame to lab frame. if (event.size() > 0) { if (boostType == 2) event.bst(0., 0., betaZ, gammaZ); else if (boostType == 3) event.rotbst(MfromCM); } // Boost process from lab frame to CM frame. } else { if (boostType == 2) process.bst(0., 0., -betaZ, gammaZ); else if (boostType == 3) process.rotbst(MtoCM); // Boost nonempty event from lab frame to CM frame. if (event.size() > 0) { if (boostType == 2) event.bst(0., 0., -betaZ, gammaZ); else if (boostType == 3) event.rotbst(MtoCM); } } // Set production vertex; assumes particles are in lab frame and at origin. if (setVertex && doVertexSpread) { Vec4 vertex = beamShapePtr->vertex(); for (int i = 0; i < process.size(); ++i) process[i].vProd( vertex); for (int i = 0; i < event.size(); ++i) event[i].vProd( vertex); } } //-------------------------------------------------------------------------- // Perform R-hadron decays, either as part of normal evolution or forced. bool Pythia::doRHadronDecays( ) { // Check if R-hadrons exist to be processed. if ( !rHadrons.exist() ) return true; // Do the R-hadron decay itself. if ( !rHadrons.decay( event) ) return false; // Perform showers in resonance decay chains. if ( !partonLevel.resonanceShowers( process, event, false) ) return false; // Subsequent hadronization and decays. if ( !hadronLevel.next( event) ) return false; // Done. return true; } //-------------------------------------------------------------------------- // Print statistics on event generation. void Pythia::stat() { // Read out settings for what to include. bool showPrL = settings.flag("Stat:showProcessLevel"); bool showPaL = settings.flag("Stat:showPartonLevel"); bool showErr = settings.flag("Stat:showErrors"); bool reset = settings.flag("Stat:reset"); // Statistics on cross section and number of events. if (doProcessLevel) { if (showPrL) processLevel.statistics(false); if (reset) processLevel.resetStatistics(); } // Statistics from other classes, currently multiparton interactions. if (showPaL) partonLevel.statistics(false); if (reset) partonLevel.resetStatistics(); // Merging statistics. if (doMerging) merging.statistics(); // Summary of which and how many warnings/errors encountered. if (showErr) info.errorStatistics(); if (reset) info.errorReset(); } //-------------------------------------------------------------------------- // Print statistics on event generation - deprecated version. void Pythia::statistics(bool all, bool reset) { // Statistics on cross section and number of events. if (doProcessLevel) processLevel.statistics(reset); // Statistics from other classes, e.g. multiparton interactions. if (all) partonLevel.statistics(reset); // Merging statistics. if (doMerging) merging.statistics(); // Summary of which and how many warnings/errors encountered. info.errorStatistics(); if (reset) info.errorReset(); } //-------------------------------------------------------------------------- // Write the Pythia banner, with symbol and version information. void Pythia::banner(ostream& os) { // Read in version number and last date of change. double versionNumber = settings.parm("Pythia:versionNumber"); int versionDate = settings.mode("Pythia:versionDate"); string month[12] = {"Jan", "Feb", "Mar", "Apr", "May", "Jun", "Jul", "Aug", "Sep", "Oct", "Nov", "Dec"}; // Get date and time. time_t t = time(0); char dateNow[12]; strftime(dateNow,12,"%d %b %Y",localtime(&t)); char timeNow[9]; strftime(timeNow,9,"%H:%M:%S",localtime(&t)); os << "\n" << " *-------------------------------------------" << "-----------------------------------------* \n" << " | " << " | \n" << " | *----------------------------------------" << "--------------------------------------* | \n" << " | | " << " | | \n" << " | | " << " | | \n" << " | | PPP Y Y TTTTT H H III A " << " Welcome to the Lund Monte Carlo! | | \n" << " | | P P Y Y T H H I A A " << " This is PYTHIA version " << fixed << setprecision(3) << setw(5) << versionNumber << " | | \n" << " | | PPP Y T HHHHH I AAAAA" << " Last date of change: " << setw(2) << versionDate%100 << " " << month[ (versionDate/100)%100 - 1 ] << " " << setw(4) << versionDate/10000 << " | | \n" << " | | P Y T H H I A A" << " | | \n" << " | | P Y T H H III A A" << " Now is " << dateNow << " at " << timeNow << " | | \n" << " | | " << " | | \n" << " | | Torbjorn Sjostrand; Department of As" << "tronomy and Theoretical Physics, | | \n" << " | | Lund University, Solvegatan 14A, S" << "E-223 62 Lund, Sweden; | | \n" << " | | phone: + 46 - 46 - 222 48 16; e-ma" << "il: torbjorn@thep.lu.se | | \n" << " | | Jesper Roy Christiansen; Department " << "of Astronomy and Theoretical Physics, | | \n" << " | | Lund University, Solvegatan 14A, S" << "E-223 62 Lund, Sweden; | | \n" << " | | e-mail: Jesper.Roy.Christiansen@th" << "ep.lu.se | | \n" << " | | Nishita Desai; Department of Physics" << " and Astronomy, University College | | \n" << " | | London, Gower Street, London, WC1E" << " 6BT, United Kingdom; | | \n" << " | | e-mail: Nishita.Desai@cern.ch " << " | | \n" << " | | Philip Ilten; School of Physics, Uni" << "iversity College Dublin, | | \n" << " | | Belfield, Dublin 4, Ireland; " << " | | \n" << " | | e-mail: philten@cern.ch " << " | | \n" << " | | Stephen Mrenna; Computing Division, " << "Simulations Group, | | \n" << " | | Fermi National Accelerator Laborat" << "ory, MS 234, Batavia, IL 60510, USA; | | \n" << " | | phone: + 1 - 630 - 840 - 2556; e-m" << "ail: mrenna@fnal.gov | | \n" << " | | Stefan Prestel; Theory Group, DESY, " << " | | \n" << " | | Notkestrasse 85, D-22607 Hamburg, " << "Germany; | | \n" << " | | phone: + 49 - 40 - 8998-4250; e-ma" << "il: stefan.prestel@thep.lu.se | | \n" << " | | Peter Skands; Theoretical Physics, C" << "ERN, CH-1211 Geneva 23, Switzerland; | | \n" << " | | phone: + 41 - 22 - 767 2447; e-mai" << "l: peter.skands@cern.ch | | \n" << " | | Stefan Ask; former author; e-mail: as" << "k.stefan@gmail.com | | \n" << " | | Richard Corke; former author; e-mail:" << " r.corke@errno.net | | \n" << " | | " << " | | \n" << " | | The main program reference is the 'Br" << "ief Introduction to PYTHIA 8.1', | | \n" << " | | T. Sjostrand, S. Mrenna and P. Skands" << ", Comput. Phys. Comm. 178 (2008) 85 | | \n" << " | | [arXiv:0710.3820] " << " | | \n" << " | | " << " | | \n" << " | | The main physics reference is the 'PY" << "THIA 6.4 Physics and Manual', | | \n" << " | | T. Sjostrand, S. Mrenna and P. Skands" << ", JHEP05 (2006) 026 [hep-ph/0603175]. | | \n" << " | | " << " | | \n" << " | | An archive of program versions and do" << "cumentation is found on the web: | | \n" << " | | http://www.thep.lu.se/~torbjorn/Pythi" << "a.html | | \n" << " | | " << " | | \n" << " | | This program is released under the GN" << "U General Public Licence version 2. | | \n" << " | | Please respect the MCnet Guidelines f" << "or Event Generator Authors and Users. | | \n" << " | | " << " | | \n" << " | | Disclaimer: this program comes withou" << "t any guarantees. | | \n" << " | | Beware of errors and use common sense" << " when interpreting results. | | \n" << " | | " << " | | \n" << " | | Copyright (C) 2013 Torbjorn Sjostrand" << " | | \n" << " | | " << " | | \n" << " | | " << " | | \n" << " | *----------------------------------------" << "--------------------------------------* | \n" << " | " << " | \n" << " *-------------------------------------------" << "-----------------------------------------* \n" << endl; } //-------------------------------------------------------------------------- // Check for lines in file that mark the beginning of new subrun. int Pythia::readSubrun(string line, bool warn, ostream& os) { // If empty line then done. int subrunLine = SUBRUNDEFAULT; if (line.find_first_not_of(" \n\t\v\b\r\f\a") == string::npos) return subrunLine; // If first character is not a letter, then done. string lineNow = line; int firstChar = lineNow.find_first_not_of(" \n\t\v\b\r\f\a"); if (!isalpha(lineNow[firstChar])) return subrunLine; // Replace an equal sign by a blank to make parsing simpler. while (lineNow.find("=") != string::npos) { int firstEqual = lineNow.find_first_of("="); lineNow.replace(firstEqual, 1, " "); } // Get first word of a line. istringstream splitLine(lineNow); string name; splitLine >> name; // Replace two colons by one (:: -> :) to allow for such mistakes. while (name.find("::") != string::npos) { int firstColonColon = name.find_first_of("::"); name.replace(firstColonColon, 2, ":"); } // Convert to lowercase. for (int i = 0; i < int(name.length()); ++i) name[i] = tolower(name[i]); // If no match then done. if (name != "main:subrun") return subrunLine; // Else find new subrun number and return it. splitLine >> subrunLine; if (!splitLine) { if (warn) os << "\n PYTHIA Warning: Main:subrun number not" << " recognized; skip:\n " << line << endl; subrunLine = SUBRUNDEFAULT; } return subrunLine; } //-------------------------------------------------------------------------- // Check that the final event makes sense: no unknown id codes; // charge and energy-momentum conserved. bool Pythia::check(ostream& os) { // Reset. bool physical = true; bool listVertices = false; bool listHistory = false; bool listSystems = false; bool listBeams = false; iErrId.resize(0); iErrCol.resize(0); iErrEpm.resize(0); iErrNan.resize(0); iErrNanVtx.resize(0); Vec4 pSum; double chargeSum = 0.; // Incoming beams counted with negative momentum and charge. if (doProcessLevel) { pSum = - (event[1].p() + event[2].p()); chargeSum = - (event[1].charge() + event[2].charge()); // If no ProcessLevel then sum final state of process record. } else if (process.size() > 0) { pSum = - process[0].p(); for (int i = 0; i < process.size(); ++i) if (process[i].isFinal()) chargeSum -= process[i].charge(); // If process not filled, then use outgoing primary in event. } else { pSum = - event[0].p(); for (int i = 1; i < event.size(); ++i) if (event[i].statusAbs() < 10 || event[i].statusAbs() == 23) chargeSum -= event[i].charge(); } double eLab = abs(pSum.e()); // Loop over particles in the event. for (int i = 0; i < event.size(); ++i) { // Look for any unrecognized particle codes. int id = event[i].id(); if (id == 0 || !particleData.isParticle(id)) { ostringstream errCode; errCode << ", i = " << i << ", id = " << id; info.errorMsg("Error in Pythia::check: " "unknown particle code", errCode.str()); physical = false; iErrId.push_back(i); // Check that colour assignments are the expected ones. } else { int colType = event[i].colType(); int col = event[i].col(); int acol = event[i].acol(); if ( (colType == 0 && (col > 0 || acol > 0)) || (colType == 1 && (col <= 0 || acol > 0)) || (colType == -1 && (col > 0 || acol <= 0)) || (colType == 2 && (col <= 0 || acol <= 0)) ) { ostringstream errCode; errCode << ", i = " << i << ", id = " << id << " cols = " << col << " " << acol; info.errorMsg("Error in Pythia::check: " "incorrect colours", errCode.str()); physical = false; iErrCol.push_back(i); } } // Look for particles with mismatched or not-a-number energy/momentum/mass. if (abs(event[i].px()) >= 0. && abs(event[i].py()) >= 0. && abs(event[i].pz()) >= 0. && abs(event[i].e()) >= 0. && abs(event[i].m()) >= 0.) { if (abs(event[i].mCalc() - event[i].m()) > epTolErr * event[i].e()) { info.errorMsg("Error in Pythia::check: " "unmatched particle energy/momentum/mass"); physical = false; iErrEpm.push_back(i); } } else { info.errorMsg("Error in Pythia::check: " "not-a-number energy/momentum/mass"); physical = false; iErrNan.push_back(i); } // Look for particles with not-a-number vertex/lifetime. if (abs(event[i].xProd()) >= 0. && abs(event[i].yProd()) >= 0. && abs(event[i].zProd()) >= 0. && abs(event[i].tProd()) >= 0. && abs(event[i].tau()) >= 0.) ; else { info.errorMsg("Error in Pythia::check: " "not-a-number vertex/lifetime"); physical = false; listVertices = true; iErrNanVtx.push_back(i); } // Add final-state four-momentum and charge. if (event[i].isFinal()) { pSum += event[i].p(); chargeSum += event[i].charge(); } // End of particle loop. } // Check energy-momentum/charge conservation. double epDev = abs(pSum.e()) + abs(pSum.px()) + abs(pSum.py()) + abs(pSum.pz()); if (epDev > epTolErr * eLab) { info.errorMsg("Error in Pythia::check: energy-momentum not conserved"); physical = false; } else if (epDev > epTolWarn * eLab) { info.errorMsg("Warning in Pythia::check: " "energy-momentum not quite conserved"); } if (abs(chargeSum) > 0.1) { info.errorMsg("Error in Pythia::check: charge not conserved"); physical = false; } // Check that beams and event records agree on incoming partons. // Only meaningful for resolved beams. if (info.isResolved()) for (int iSys = 0; iSys < beamA.sizeInit(); ++iSys) { int eventANw = partonSystems.getInA(iSys); int eventBNw = partonSystems.getInB(iSys); int beamANw = beamA[iSys].iPos(); int beamBNw = beamB[iSys].iPos(); if (eventANw != beamANw || eventBNw != beamBNw) { info.errorMsg("Error in Pythia::check: " "event and beams records disagree"); physical = false; listSystems = true; listBeams = true; } } // Check that mother and daughter information match for each particle. vector noMot; vector noDau; vector< pair > noMotDau; if (checkHistory) { // Loop through the event and check that there are beam particles. bool hasBeams = false; for (int i = 0; i < event.size(); ++i) { int status = event[i].status(); if (abs(status) == 12) hasBeams = true; // Check that mother and daughter lists not empty where not expected to. vector mList = event[i].motherList(); vector dList = event[i].daughterList(); if (mList.size() == 0 && abs(status) != 11 && abs(status) != 12) noMot.push_back(i); if (dList.size() == 0 && status < 0 && status != -11) noDau.push_back(i); // Check that the particle appears in the daughters list of each mother. for (int j = 0; j < int(mList.size()); ++j) { if ( event[mList[j]].daughter1() <= i && event[mList[j]].daughter2() >= i ) continue; vector dmList = event[mList[j]].daughterList(); bool foundMatch = false; for (int k = 0; k < int(dmList.size()); ++k) if (dmList[k] == i) { foundMatch = true; break; } if (!hasBeams && mList.size() == 1 && mList[0] == 0) foundMatch = true; if (!foundMatch) { bool oldPair = false; for (int k = 0; k < int(noMotDau.size()); ++k) if (noMotDau[k].first == mList[j] && noMotDau[k].second == i) { oldPair = true; break; } if (!oldPair) noMotDau.push_back( make_pair( mList[j], i) ); } } // Check that the particle appears in the mothers list of each daughter. for (int j = 0; j < int(dList.size()); ++j) { if ( event[dList[j]].statusAbs() > 80 && event[dList[j]].statusAbs() < 90 && event[dList[j]].mother1() <= i && event[dList[j]].mother2() >= i) continue; vector mdList = event[dList[j]].motherList(); bool foundMatch = false; for (int k = 0; k < int(mdList.size()); ++k) if (mdList[k] == i) { foundMatch = true; break; } if (!foundMatch) { bool oldPair = false; for (int k = 0; k < int(noMotDau.size()); ++k) if (noMotDau[k].first == i && noMotDau[k].second == dList[j]) { oldPair = true; break; } if (!oldPair) noMotDau.push_back( make_pair( i, dList[j]) ); } } } // Warn if any errors were found. if (noMot.size() > 0 || noDau.size() > 0 || noMotDau.size() > 0) { info.errorMsg("Error in Pythia::check: " "mismatch in daughter and mother lists"); physical = false; listHistory = true; } } // Done for sensible events. if (physical) return true; // Print (the first few) flawed events: local info. if (nErrEvent < nErrList) { os << "\n PYTHIA erroneous event info: \n"; if (iErrId.size() > 0) { os << " unknown particle codes in lines "; for (int i = 0; i < int(iErrId.size()); ++i) os << iErrId[i] << " "; os << "\n"; } if (iErrCol.size() > 0) { os << " incorrect colour assignments in lines "; for (int i = 0; i < int(iErrCol.size()); ++i) os << iErrCol[i] << " "; os << "\n"; } if (iErrEpm.size() > 0) { os << " mismatch between energy/momentum/mass in lines "; for (int i = 0; i < int(iErrEpm.size()); ++i) os << iErrEpm[i] << " "; os << "\n"; } if (iErrNan.size() > 0) { os << " not-a-number energy/momentum/mass in lines "; for (int i = 0; i < int(iErrNan.size()); ++i) os << iErrNan[i] << " "; os << "\n"; } if (iErrNanVtx.size() > 0) { os << " not-a-number vertex/lifetime in lines "; for (int i = 0; i < int(iErrNanVtx.size()); ++i) os << iErrNanVtx[i] << " "; os << "\n"; } if (epDev > epTolErr * eLab) os << scientific << setprecision(3) << " total energy-momentum non-conservation = " << epDev << "\n"; if (abs(chargeSum) > 0.1) os << fixed << setprecision(2) << " total charge non-conservation = " << chargeSum << "\n"; if (noMot.size() > 0) { os << " missing mothers for particles "; for (int i = 0; i < int(noMot.size()); ++i) os << noMot[i] << " "; os << "\n"; } if (noDau.size() > 0) { os << " missing daughters for particles "; for (int i = 0; i < int(noDau.size()); ++i) os << noDau[i] << " "; os << "\n"; } if (noMotDau.size() > 0) { os << " inconsistent history for (mother,daughter) pairs "; for (int i = 0; i < int(noMotDau.size()); ++i) os << "(" << noMotDau[i].first << "," << noMotDau[i].second << ") "; os << "\n"; } // Print (the first few) flawed events: standard listings. info.list(); event.list(listVertices, listHistory); if (listSystems) partonSystems.list(); if (listBeams) beamA.list(); if (listBeams) beamB.list(); } // Update error counter. Done also for flawed event. ++nErrEvent; return false; } //-------------------------------------------------------------------------- // Routine to set up a PDF pointer. PDF* Pythia::getPDFPtr(int idIn, int sequence) { // Temporary pointer to be returned. PDF* tempPDFPtr = 0; // One option is to treat a Pomeron like a pi0. if (idIn == 990 && settings.mode("PDF:PomSet") == 2) idIn = 111; // Proton beam, normal choice. Also used for neutron. if ((abs(idIn) == 2212 || abs(idIn) == 2112) && sequence == 1) { int pSet = settings.mode("PDF:pSet"); bool useLHAPDF = settings.flag("PDF:useLHAPDF"); // Use internal sets. if (!useLHAPDF) { if (pSet == 1) tempPDFPtr = new GRV94L(idIn); else if (pSet == 2) tempPDFPtr = new CTEQ5L(idIn); else if (pSet <= 6) tempPDFPtr = new MSTWpdf(idIn, pSet - 2, xmlPath, &info); else if (pSet <= 12) tempPDFPtr = new CTEQ6pdf(idIn, pSet - 6, xmlPath, &info); else tempPDFPtr = new NNPDF(idIn, pSet - 12, xmlPath, &info); } // Use sets from LHAPDF. else { string LHAPDFset = settings.word("PDF:LHAPDFset"); int LHAPDFmember = settings.mode("PDF:LHAPDFmember"); int nSet = LHAPDF::findNSet(LHAPDFset, LHAPDFmember); if (nSet == -1) nSet = LHAPDF::freeNSet(); tempPDFPtr = new LHAPDF(idIn, LHAPDFset, LHAPDFmember, nSet, &info); // Optionally allow extrapolation beyond x and Q2 limits. tempPDFPtr->setExtrapolate( settings.flag("PDF:extrapolateLHAPDF") ); } } // Proton beam, special choice for the hard process. Also neutron. else if (abs(idIn) == 2212 || abs(idIn) == 2112) { int pSet = settings.mode("PDF:pHardSet"); bool useLHAPDF = settings.flag("PDF:useHardLHAPDF"); // Use internal sets. if (!useLHAPDF) { if (pSet == 1) tempPDFPtr = new GRV94L(idIn); else if (pSet == 2) tempPDFPtr = new CTEQ5L(idIn); else if (pSet <= 6) tempPDFPtr = new MSTWpdf(idIn, pSet - 2, xmlPath, &info); else if (pSet <= 12) tempPDFPtr = new CTEQ6pdf(idIn, pSet - 6, xmlPath, &info); else tempPDFPtr = new NNPDF(idIn, pSet - 12, xmlPath, &info); } // Use sets from LHAPDF. else { string LHAPDFset = settings.word("PDF:hardLHAPDFset"); int LHAPDFmember = settings.mode("PDF:hardLHAPDFmember"); int nSet = LHAPDF::findNSet(LHAPDFset, LHAPDFmember); if (nSet == -1) nSet = LHAPDF::freeNSet(); tempPDFPtr = new LHAPDF(idIn, LHAPDFset, LHAPDFmember, nSet, &info); // Optionally allow extrapolation beyond x and Q2 limits. tempPDFPtr->setExtrapolate( settings.flag("PDF:extrapolateLHAPDF") ); } } // Pion beam (or, in one option, Pomeron beam). else if (abs(idIn) == 211 || idIn == 111) { bool useLHAPDF = settings.flag("PDF:piUseLHAPDF"); // Use internal sets. if (!useLHAPDF) { tempPDFPtr = new GRVpiL(idIn); } // Use sets from LHAPDF. else { string LHAPDFset = settings.word("PDF:piLHAPDFset"); int LHAPDFmember = settings.mode("PDF:piLHAPDFmember"); tempPDFPtr = new LHAPDF(idIn, LHAPDFset, LHAPDFmember, 1, &info); // Optionally allow extrapolation beyond x and Q2 limits. tempPDFPtr->setExtrapolate( settings.flag("PDF:extrapolateLHAPDF") ); } } // Pomeron beam, if not treated like a pi0 beam. else if (idIn == 990) { int pomSet = settings.mode("PDF:PomSet"); double rescale = settings.parm("PDF:PomRescale"); // A generic Q2-independent parametrization. if (pomSet == 1) { double gluonA = settings.parm("PDF:PomGluonA"); double gluonB = settings.parm("PDF:PomGluonB"); double quarkA = settings.parm("PDF:PomQuarkA"); double quarkB = settings.parm("PDF:PomQuarkB"); double quarkFrac = settings.parm("PDF:PomQuarkFrac"); double strangeSupp = settings.parm("PDF:PomStrangeSupp"); tempPDFPtr = new PomFix( 990, gluonA, gluonB, quarkA, quarkB, quarkFrac, strangeSupp); } // The H1 Q2-dependent parametrizations. Initialization requires files. else if (pomSet == 3 || pomSet == 4) tempPDFPtr = new PomH1FitAB( 990, pomSet - 2, rescale, xmlPath, &info); else if (pomSet == 5) tempPDFPtr = new PomH1Jets( 990, rescale, xmlPath, &info); else if (pomSet == 6) tempPDFPtr = new PomH1FitAB( 990, 3, rescale, xmlPath, &info); } // Lepton beam: neutrino, resolved charged lepton or unresolved ditto. else if (abs(idIn) > 10 && abs(idIn) < 17) { if (abs(idIn)%2 == 0) tempPDFPtr = new NeutrinoPoint(idIn); else if (settings.flag("PDF:lepton")) tempPDFPtr = new Lepton(idIn); else tempPDFPtr = new LeptonPoint(idIn); } // Failure for unrecognized particle. else tempPDFPtr = 0; // Done. return tempPDFPtr; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaProcess.cc0000644000175000017500000013404312217346251016036 0ustar sunsun// SigmaProcess.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // SigmaProcess class, and classes derived from it. #include "Pythia8/SigmaProcess.h" namespace Pythia8 { //========================================================================== // The SigmaProcess class. // Base class for cross sections. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Conversion of GeV^{-2} to mb for cross section. const double SigmaProcess::CONVERT2MB = 0.389380; // The sum of outgoing masses must not be too close to the cm energy. const double SigmaProcess::MASSMARGIN = 0.1; // Parameters of momentum rescaling procedure: maximally allowed // relative energy error and number of iterations. const double SigmaProcess::COMPRELERR = 1e-10; const int SigmaProcess::NCOMPSTEP = 10; //-------------------------------------------------------------------------- // Perform simple initialization and store pointers. void SigmaProcess::init(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, Couplings* couplingsPtrIn, SigmaTotal* sigmaTotPtrIn, SLHAinterface* slhaInterfacePtrIn) { // Store pointers. infoPtr = infoPtrIn; settingsPtr = settingsPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; couplingsPtr = couplingsPtrIn; sigmaTotPtr = sigmaTotPtrIn; // Pointer to SLHA object allows semi-internal processes to access // SLHA blocks via getEntry() methods, see arXiv:1109.5852 slhaPtr = (slhaInterfacePtrIn != 0) ? &slhaInterfacePtrIn->slha : 0; // Read out some properties of beams to allow shorthand. idA = (beamAPtr != 0) ? beamAPtr->id() : 0; idB = (beamBPtr != 0) ? beamBPtr->id() : 0; mA = (beamAPtr != 0) ? beamAPtr->m() : 0.; mB = (beamBPtr != 0) ? beamBPtr->m() : 0.; isLeptonA = (beamAPtr != 0) ? beamAPtr->isLepton() : false; isLeptonB = (beamBPtr != 0) ? beamBPtr->isLepton() : false; hasLeptonBeams = isLeptonA || isLeptonB; // K factor, multiplying resolved processes. (But not here for MPI.) Kfactor = settingsPtr->parm("SigmaProcess:Kfactor"); // Maximum incoming quark flavour. nQuarkIn = settingsPtr->mode("PDFinProcess:nQuarkIn"); // Medium heavy fermion masses set massless or not in ME expressions. mcME = (settingsPtr->flag("SigmaProcess:cMassiveME")) ? particleDataPtr->m0(4) : 0.; mbME = (settingsPtr->flag("SigmaProcess:bMassiveME")) ? particleDataPtr->m0(5) : 0.; mmuME = (settingsPtr->flag("SigmaProcess:muMassiveME")) ? particleDataPtr->m0(13) : 0.; mtauME = (settingsPtr->flag("SigmaProcess:tauMassiveME")) ? particleDataPtr->m0(15) : 0.; // Renormalization scale choice. renormScale1 = settingsPtr->mode("SigmaProcess:renormScale1"); renormScale2 = settingsPtr->mode("SigmaProcess:renormScale2"); renormScale3 = settingsPtr->mode("SigmaProcess:renormScale3"); renormScale3VV = settingsPtr->mode("SigmaProcess:renormScale3VV"); renormMultFac = settingsPtr->parm("SigmaProcess:renormMultFac"); renormFixScale = settingsPtr->parm("SigmaProcess:renormFixScale"); // Factorization scale choice. factorScale1 = settingsPtr->mode("SigmaProcess:factorScale1"); factorScale2 = settingsPtr->mode("SigmaProcess:factorScale2"); factorScale3 = settingsPtr->mode("SigmaProcess:factorScale3"); factorScale3VV = settingsPtr->mode("SigmaProcess:factorScale3VV"); factorMultFac = settingsPtr->parm("SigmaProcess:factorMultFac"); factorFixScale = settingsPtr->parm("SigmaProcess:factorFixScale"); // CP violation parameters for the BSM Higgs sector. higgsH1parity = settingsPtr->mode("HiggsH1:parity"); higgsH1eta = settingsPtr->parm("HiggsH1:etaParity"); higgsH2parity = settingsPtr->mode("HiggsH2:parity"); higgsH2eta = settingsPtr->parm("HiggsH2:etaParity"); higgsA3parity = settingsPtr->mode("HiggsA3:parity"); higgsA3eta = settingsPtr->parm("HiggsA3:etaParity"); // If BSM not switched on then H1 should have SM properties. if (!settingsPtr->flag("Higgs:useBSM")){ higgsH1parity = 1; higgsH1eta = 0.; } } //-------------------------------------------------------------------------- // Set up allowed flux of incoming partons. // addBeam: set up PDF's that need to be evaluated for the two beams. // addPair: set up pairs of incoming partons from the two beams. bool SigmaProcess::initFlux() { // Reset arrays (in case of several init's in same run). inBeamA.clear(); inBeamB.clear(); inPair.clear(); // Read in process-specific channel information. string fluxType = inFlux(); // Case with g g incoming state. if (fluxType == "gg") { addBeamA(21); addBeamB(21); addPair(21, 21); } // Case with q g incoming state. else if (fluxType == "qg") { for (int i = -nQuarkIn; i <= nQuarkIn; ++i) { int idNow = (i == 0) ? 21 : i; addBeamA(idNow); addBeamB(idNow); } for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addPair(idNow, 21); addPair(21, idNow); } } // Case with q q', q qbar' or qbar qbar' incoming state. else if (fluxType == "qq") { for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamA(idNow); addBeamB(idNow); } for (int id1Now = -nQuarkIn; id1Now <= nQuarkIn; ++id1Now) if (id1Now != 0) for (int id2Now = -nQuarkIn; id2Now <= nQuarkIn; ++id2Now) if (id2Now != 0) addPair(id1Now, id2Now); } // Case with q qbar' incoming state. else if (fluxType == "qqbar") { for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamA(idNow); addBeamB(idNow); } for (int id1Now = -nQuarkIn; id1Now <= nQuarkIn; ++id1Now) if (id1Now != 0) for (int id2Now = -nQuarkIn; id2Now <= nQuarkIn; ++id2Now) if (id2Now != 0 && id1Now * id2Now < 0) addPair(id1Now, id2Now); } // Case with q qbar incoming state. else if (fluxType == "qqbarSame") { for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamA(idNow); addBeamB(idNow); } for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) addPair(idNow, -idNow); } // Case with f f', f fbar', fbar fbar' incoming state. else if (fluxType == "ff") { // If beams are leptons then they are also the colliding partons. if ( isLeptonA && isLeptonB ) { addBeamA(idA); addBeamB(idB); addPair(idA, idB); // First beam is lepton and second is hadron. } else if ( isLeptonA ) { addBeamA(idA); for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamB(idNow); addPair(idA, idNow); } // First beam is hadron and second is lepton. } else if ( isLeptonB ) { addBeamB(idB); for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamA(idNow); addPair(idNow, idB); } // Hadron beams gives quarks. } else { for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamA(idNow); addBeamB(idNow); } for (int id1Now = -nQuarkIn; id1Now <= nQuarkIn; ++id1Now) if (id1Now != 0) for (int id2Now = -nQuarkIn; id2Now <= nQuarkIn; ++id2Now) if (id2Now != 0) addPair(id1Now, id2Now); } } // Case with f fbar' generic incoming state. else if (fluxType == "ffbar") { // If beams are leptons then also colliding partons. if (isLeptonA && isLeptonB && idA * idB < 0) { addBeamA(idA); addBeamB(idB); addPair(idA, idB); // Hadron beams gives quarks. } else { for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamA(idNow); addBeamB(idNow); } for (int id1Now = -nQuarkIn; id1Now <= nQuarkIn; ++id1Now) if (id1Now != 0) for (int id2Now = -nQuarkIn; id2Now <= nQuarkIn; ++id2Now) if (id2Now != 0 && id1Now * id2Now < 0) addPair(id1Now, id2Now); } } // Case with f fbar incoming state. else if (fluxType == "ffbarSame") { // If beams are antiparticle pair and leptons then also colliding partons. if ( idA + idB == 0 && isLeptonA ) { addBeamA(idA); addBeamB(idB); addPair(idA, idB); // Else assume both to be hadrons, for better or worse. } else { for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamA(idNow); addBeamB(idNow); } for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) addPair(idNow, -idNow); } } // Case with f fbar' charged(+-1) incoming state. else if (fluxType == "ffbarChg") { // If beams are leptons then also colliding partons. if ( isLeptonA && isLeptonB && abs( particleDataPtr->chargeType(idA) + particleDataPtr->chargeType(idB) ) == 3 ) { addBeamA(idA); addBeamB(idB); addPair(idA, idB); // Hadron beams gives quarks. } else { for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamA(idNow); addBeamB(idNow); } for (int id1Now = -nQuarkIn; id1Now <= nQuarkIn; ++id1Now) if (id1Now != 0) for (int id2Now = -nQuarkIn; id2Now <= nQuarkIn; ++id2Now) if (id2Now != 0 && id1Now * id2Now < 0 && (abs(id1Now) + abs(id2Now))%2 == 1) addPair(id1Now, id2Now); } } // Case with f gamma incoming state. else if (fluxType == "fgm") { // Fermion from incoming side A. if ( isLeptonA ) { addBeamA(idA); addPair(idA, 22); } else { for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamA(idNow); addPair(idNow, 22); } } // Fermion from incoming side B. if ( isLeptonB ) { addBeamB( idB); addPair(22, idB); } else { for (int idNow = -nQuarkIn; idNow <= nQuarkIn; ++idNow) if (idNow != 0) { addBeamB(idNow); addPair(22, idNow); } } // Photons in the beams. addBeamA(22); addBeamB(22); } // Case with gamma gamma incoming state. else if (fluxType == "ggm") { addBeamA(21); addBeamA(22); addBeamB(21); addBeamB(22); addPair(21, 22); addPair(22, 21); } // Case with gamma gamma incoming state. else if (fluxType == "gmgm") { addBeamA(22); addBeamB(22); addPair(22, 22); } // Unrecognized fluxType is bad sign. Else done. else { infoPtr->errorMsg("Error in SigmaProcess::initFlux: " "unrecognized inFlux type", fluxType); return false; } return true; } //-------------------------------------------------------------------------- // Convolute matrix-element expression(s) with parton flux and K factor. double SigmaProcess::sigmaPDF() { // Evaluate and store the required parton densities. for (int j = 0; j < sizeBeamA(); ++j) inBeamA[j].pdf = beamAPtr->xfHard( inBeamA[j].id, x1Save, Q2FacSave); for (int j = 0; j < sizeBeamB(); ++j) inBeamB[j].pdf = beamBPtr->xfHard( inBeamB[j].id, x2Save, Q2FacSave); // Loop over allowed incoming channels. sigmaSumSave = 0.; for (int i = 0; i < sizePair(); ++i) { // Evaluate hard-scattering cross section. Include K factor. inPair[i].pdfSigma = Kfactor * sigmaHatWrap(inPair[i].idA, inPair[i].idB); // Multiply by respective parton densities. for (int j = 0; j < sizeBeamA(); ++j) if (inPair[i].idA == inBeamA[j].id) { inPair[i].pdfA = inBeamA[j].pdf; inPair[i].pdfSigma *= inBeamA[j].pdf; break; } for (int j = 0; j < sizeBeamB(); ++j) if (inPair[i].idB == inBeamB[j].id) { inPair[i].pdfB = inBeamB[j].pdf; inPair[i].pdfSigma *= inBeamB[j].pdf; break; } // Sum for all channels. sigmaSumSave += inPair[i].pdfSigma; } // Done. return sigmaSumSave; } //-------------------------------------------------------------------------- // Select incoming parton channel and extract parton densities (resolved). void SigmaProcess::pickInState(int id1in, int id2in) { // Multiparton interactions: partons already selected. if (id1in != 0 && id2in != 0) { id1 = id1in; id2 = id2in; } // Pick channel. Extract channel flavours and pdf's. double sigmaRand = sigmaSumSave * rndmPtr->flat(); for (int i = 0; i < sizePair(); ++i) { sigmaRand -= inPair[i].pdfSigma; if (sigmaRand <= 0.) { id1 = inPair[i].idA; id2 = inPair[i].idB; pdf1Save = inPair[i].pdfA; pdf2Save = inPair[i].pdfB; break; } } } //-------------------------------------------------------------------------- // Calculate incoming modified masses and four-vectors for matrix elements. bool SigmaProcess::setupForMEin() { // Initially assume it will work out to set up modified kinematics. bool allowME = true; // Correct incoming c, b, mu and tau to be massive or not. mME[0] = 0.; int id1Tmp = abs(id1); if (id1Tmp == 4) mME[0] = mcME; if (id1Tmp == 5) mME[0] = mbME; if (id1Tmp == 13) mME[0] = mmuME; if (id1Tmp == 15) mME[0] = mtauME; mME[1] = 0.; int id2Tmp = abs(id2); if (id2Tmp == 4) mME[1] = mcME; if (id2Tmp == 5) mME[1] = mbME; if (id2Tmp == 13) mME[1] = mmuME; if (id2Tmp == 15) mME[1] = mtauME; // If kinematically impossible return to massless case, but set error. if (mME[0] + mME[1] >= mH) { mME[0] = 0.; mME[1] = 0.; allowME = false; } // Do incoming two-body kinematics for massless or massive cases. if (mME[0] == 0. && mME[1] == 0.) { pME[0] = 0.5 * mH * Vec4( 0., 0., 1., 1.); pME[1] = 0.5 * mH * Vec4( 0., 0., -1., 1.); } else { double e0 = 0.5 * (mH * mH + mME[0] * mME[0] - mME[1] * mME[1]) / mH; double pz0 = sqrtpos(e0 * e0 - mME[0] * mME[0]); pME[0] = Vec4( 0., 0., pz0, e0); pME[1] = Vec4( 0., 0., -pz0, mH - e0); } // Done. return allowME; } //-------------------------------------------------------------------------- // Evaluate weight for W decay distribution in t -> W b -> f fbar b. double SigmaProcess::weightTopDecay( Event& process, int iResBeg, int iResEnd) { // If not pair W d/s/b and mother t then return unit weight. if (iResEnd - iResBeg != 1) return 1.; int iW1 = iResBeg; int iB2 = iResBeg + 1; int idW1 = process[iW1].idAbs(); int idB2 = process[iB2].idAbs(); if (idW1 != 24) { swap(iW1, iB2); swap(idW1, idB2); } if (idW1 != 24 || (idB2 != 1 && idB2 != 3 && idB2 != 5)) return 1.; int iT = process[iW1].mother1(); if (iT <= 0 || process[iT].idAbs() != 6) return 1.; // Find sign-matched order of W decay products. int iF = process[iW1].daughter1(); int iFbar = process[iW1].daughter2(); if (iFbar - iF != 1) return 1.; if (process[iT].id() * process[iF].id() < 0) swap(iF, iFbar); // Weight and maximum weight. double wt = (process[iT].p() * process[iFbar].p()) * (process[iF].p() * process[iB2].p()); double wtMax = ( pow4(process[iT].m()) - pow4(process[iW1].m()) ) / 8.; // Done. return wt / wtMax; } //-------------------------------------------------------------------------- // Evaluate weight for Z0/W+- decay distributions in H -> Z0/W+ Z0/W- -> 4f // and H -> gamma Z0 -> gamma f fbar. double SigmaProcess::weightHiggsDecay( Event& process, int iResBeg, int iResEnd) { // If not pair Z0 Z0, W+ W- or gamma Z0 then return unit weight. if (iResEnd - iResBeg != 1) return 1.; int iZW1 = iResBeg; int iZW2 = iResBeg + 1; int idZW1 = process[iZW1].id(); int idZW2 = process[iZW2].id(); if (idZW1 < 0 || idZW2 == 22) { swap(iZW1, iZW2); swap(idZW1, idZW2); } if ( (idZW1 != 23 || idZW2 != 23) && (idZW1 != 24 || idZW2 != -24) && (idZW1 != 22 || idZW2 != 23) ) return 1.; // If mother is not Higgs then return unit weight. int iH = process[iZW1].mother1(); if (iH <= 0) return 1.; int idH = process[iH].id(); if (idH != 25 && idH != 35 && idH !=36) return 1.; // H -> gamma Z0 -> gamma f fbar is 1 + cos^2(theta) in Z rest frame. if (idZW1 == 22) { int i5 = process[iZW2].daughter1(); int i6 = process[iZW2].daughter2(); double pgmZ = process[iZW1].p() * process[iZW2].p(); double pgm5 = process[iZW1].p() * process[i5].p(); double pgm6 = process[iZW1].p() * process[i6].p(); return (pow2(pgm5) + pow2(pgm6)) / pow2(pgmZ); } // Parameters depend on Higgs type: H0(H_1), H^0(H_2) or A^0(H_3). int higgsParity = higgsH1parity; double higgsEta = higgsH1eta; if (idH == 35) { higgsParity = higgsH2parity; higgsEta = higgsH2eta; } else if (idH == 36) { higgsParity = higgsA3parity; higgsEta = higgsA3eta; } // Option with isotropic decays. if (higgsParity == 0) return 1.; // Maximum and initial weight. double wtMax = pow4(process[iH].m()); double wt = wtMax; // Find sign-matched order of Z0/W+- decay products. int i3 = process[iZW1].daughter1(); int i4 = process[iZW1].daughter2(); if (process[i3].id() < 0) swap( i3, i4); int i5 = process[iZW2].daughter1(); int i6 = process[iZW2].daughter2(); if (process[i5].id() < 0) swap( i5, i6); // Evaluate four-vector products and find masses.. double p35 = 2. * process[i3].p() * process[i5].p(); double p36 = 2. * process[i3].p() * process[i6].p(); double p45 = 2. * process[i4].p() * process[i5].p(); double p46 = 2. * process[i4].p() * process[i6].p(); double p34 = 2. * process[i3].p() * process[i4].p(); double p56 = 2. * process[i5].p() * process[i6].p(); double mZW1 = process[iZW1].m(); double mZW2 = process[iZW2].m(); // For mixed CP states need epsilon product and gauge boson masses. double epsilonProd = 0.; if (higgsParity == 3) { double p[4][4]; for (int i = 0; i < 4; ++i) { int ii = i3; if (i == 1) ii = i4; if (i == 2) ii = i5; if (i == 3) ii = i6; p[i][0] = process[ii].e(); p[i][1] = process[ii].px(); p[i][2] = process[ii].py(); p[i][3] = process[ii].pz(); } epsilonProd = p[0][0]*p[1][1]*p[2][2]*p[3][3] - p[0][0]*p[1][1]*p[2][3]*p[3][2] - p[0][0]*p[1][2]*p[2][1]*p[3][3] + p[0][0]*p[1][2]*p[2][3]*p[3][1] + p[0][0]*p[1][3]*p[2][1]*p[3][2] - p[0][0]*p[1][3]*p[2][2]*p[3][1] - p[0][1]*p[1][0]*p[2][2]*p[3][3] + p[0][1]*p[1][0]*p[2][3]*p[3][2] + p[0][1]*p[1][2]*p[2][0]*p[3][3] - p[0][1]*p[1][2]*p[2][3]*p[3][0] - p[0][1]*p[1][3]*p[2][0]*p[3][2] + p[0][1]*p[1][3]*p[2][2]*p[3][0] + p[0][2]*p[1][0]*p[2][1]*p[3][3] - p[0][2]*p[1][0]*p[2][3]*p[3][1] - p[0][2]*p[1][1]*p[2][0]*p[3][3] + p[0][2]*p[1][1]*p[2][3]*p[3][0] + p[0][2]*p[1][3]*p[2][0]*p[3][1] - p[0][2]*p[1][3]*p[2][1]*p[3][0] - p[0][3]*p[1][0]*p[2][1]*p[3][2] + p[0][3]*p[1][0]*p[2][2]*p[3][1] + p[0][3]*p[1][1]*p[2][0]*p[3][2] - p[0][3]*p[1][1]*p[2][2]*p[3][0] - p[0][3]*p[1][2]*p[2][0]*p[3][1] + p[0][3]*p[1][2]*p[2][1]*p[3][0]; } // Z0 Z0 decay: vector and axial couplings of two fermion pairs. if (idZW1 == 23) { double vf1 = couplingsPtr->vf(process[i3].idAbs()); double af1 = couplingsPtr->af(process[i3].idAbs()); double vf2 = couplingsPtr->vf(process[i5].idAbs()); double af2 = couplingsPtr->af(process[i5].idAbs()); double va12asym = 4. * vf1 * af1 * vf2 * af2 / ( (vf1*vf1 + af1*af1) * (vf2*vf2 + af2*af2) ); double etaMod = higgsEta / pow2( particleDataPtr->m0(23) ); // Normal CP-even decay. if (higgsParity == 1) wt = 8. * (1. + va12asym) * p35 * p46 + 8. * (1. - va12asym) * p36 * p45; // CP-odd decay (normal for A0(H_3)). else if (higgsParity == 2) wt = ( pow2(p35 + p46) + pow2(p36 + p45) - 2. * p34 * p56 - 2. * pow2(p35 * p46 - p36 * p45) / (p34 * p56) + va12asym * (p35 + p36 - p45 - p46) * (p35 + p45 - p36 - p46) ) / (1. + va12asym); // Mixed CP states. else wt = 32. * ( 0.25 * ( (1. + va12asym) * p35 * p46 + (1. - va12asym) * p36 * p45 ) - 0.5 * etaMod * epsilonProd * ( (1. + va12asym) * (p35 + p46) - (1. - va12asym) * (p36 + p45) ) + 0.0625 * etaMod * etaMod * (-2. * pow2(p34 * p56) - 2. * pow2(p35 * p46 - p36 * p45) + p34 * p56 * (pow2(p35 + p46) + pow2(p36 + p45)) + va12asym * p34 * p56 * (p35 + p36 - p45 - p46) * (p35 + p45 - p36 - p46) ) ) / ( 1. + 2. * etaMod * mZW1 * mZW2 + 2. * pow2(etaMod * mZW1 * mZW2) * (1. + va12asym) ); // W+ W- decay. } else if (idZW1 == 24) { double etaMod = higgsEta / pow2( particleDataPtr->m0(24) ); // Normal CP-even decay. if (higgsParity == 1) wt = 16. * p35 * p46; // CP-odd decay (normal for A0(H_3)). else if (higgsParity == 2) wt = 0.5 * ( pow2(p35 + p46) + pow2(p36 + p45) - 2. * p34 * p56 - 2. * pow2(p35 * p46 - p36 * p45) / (p34 * p56) + (p35 + p36 - p45 - p46) * (p35 + p45 - p36 - p46) ); // Mixed CP states. else wt = 32. * ( 0.25 * 2. * p35 * p46 - 0.5 * etaMod * epsilonProd * 2. * (p35 + p46) + 0.0625 * etaMod * etaMod * (-2. * pow2(p34 * p56) - 2. * pow2(p35 * p46 - p36 * p45) + p34 * p56 * (pow2(p35 + p46) + pow2(p36 + p45)) + p34 * p56 * (p35 + p36 - p45 - p46) * (p35 + p45 - p36 - p46) ) ) / ( 1. * 2. * etaMod * mZW1 * mZW2 + 2. * pow2(etaMod * mZW1 * mZW2) ); } // Done. return wt / wtMax; } //========================================================================== // The Sigma1Process class. // Base class for resolved 2 -> 1 cross sections; derived from SigmaProcess. //-------------------------------------------------------------------------- // Wrapper to sigmaHat, to (a) store current incoming flavours, // (b) convert from GeV^-2 to mb where required, and // (c) convert from |M|^2 to d(sigmaHat)/d(tHat) where required. double Sigma1Process::sigmaHatWrap(int id1in, int id2in) { id1 = id1in; id2 = id2in; double sigmaTmp = sigmaHat(); if (convertM2()) { sigmaTmp /= 2. * sH; // Convert 2 * pi * delta(p^2 - m^2) to Breit-Wigner with same area. int idTmp = resonanceA(); double mTmp = particleDataPtr->m0(idTmp); double GamTmp = particleDataPtr->mWidth(idTmp); sigmaTmp *= 2. * mTmp * GamTmp / ( pow2(sH - mTmp * mTmp) + pow2(mTmp * GamTmp) ); } if (convert2mb()) sigmaTmp *= CONVERT2MB; return sigmaTmp; } //-------------------------------------------------------------------------- // Input and complement kinematics for resolved 2 -> 1 process. void Sigma1Process::store1Kin( double x1in, double x2in, double sHin) { // Default value only sensible for these processes. swapTU = false; // Incoming parton momentum fractions and sHat. x1Save = x1in; x2Save = x2in; sH = sHin; mH = sqrt(sH); sH2 = sH * sH; // Different options for renormalization scale, but normally sHat. Q2RenSave = renormMultFac * sH; if (renormScale1 == 2) Q2RenSave = renormFixScale; // Different options for factorization scale, but normally sHat. Q2FacSave = factorMultFac * sH; if (factorScale1 == 2) Q2FacSave = factorFixScale; // Evaluate alpha_strong and alpha_EM. alpS = couplingsPtr->alphaS(Q2RenSave); alpEM = couplingsPtr->alphaEM(Q2RenSave); } //-------------------------------------------------------------------------- // Calculate modified masses and four-vectors for matrix elements. bool Sigma1Process::setupForME() { // Common initial-state handling. bool allowME = setupForMEin(); // Final state trivial here. mME[2] = mH; pME[2] = Vec4( 0., 0., 0., mH); // Done. return allowME; } //========================================================================== // The Sigma2Process class. // Base class for resolved 2 -> 2 cross sections; derived from SigmaProcess. //-------------------------------------------------------------------------- // Input and complement kinematics for resolved 2 -> 2 process. void Sigma2Process::store2Kin( double x1in, double x2in, double sHin, double tHin, double m3in, double m4in, double runBW3in, double runBW4in) { // Default ordering of particles 3 and 4. swapTU = false; // Incoming parton momentum fractions. x1Save = x1in; x2Save = x2in; // Incoming masses and their squares. bool masslessKin = (id3Mass() == 0) && (id4Mass() == 0); if (masslessKin) { m3 = 0.; m4 = 0.; } else { m3 = m3in; m4 = m4in; } mSave[3] = m3; mSave[4] = m4; s3 = m3 * m3; s4 = m4 * m4; // Standard Mandelstam variables and their squares. sH = sHin; tH = tHin; uH = (masslessKin) ? -(sH + tH) : s3 + s4 - (sH + tH); mH = sqrt(sH); sH2 = sH * sH; tH2 = tH * tH; uH2 = uH * uH; // The nominal Breit-Wigner factors with running width. runBW3 = runBW3in; runBW4 = runBW4in; // Calculate squared transverse momentum. pT2 = (masslessKin) ? tH * uH / sH : (tH * uH - s3 * s4) / sH; // Special case: pick scale as if 2 -> 1 process in disguise. if (isSChannel()) { // Different options for renormalization scale, but normally sHat. Q2RenSave = renormMultFac * sH; if (renormScale1 == 2) Q2RenSave = renormFixScale; // Different options for factorization scale, but normally sHat. Q2FacSave = factorMultFac * sH; if (factorScale1 == 2) Q2FacSave = factorFixScale; // Normal case with "true" 2 -> 2. } else { // Different options for renormalization scale. if (masslessKin) Q2RenSave = (renormScale2 < 4) ? pT2 : sH; else if (renormScale2 == 1) Q2RenSave = pT2 + min(s3, s4); else if (renormScale2 == 2) Q2RenSave = sqrt((pT2 + s3) * (pT2 + s4)); else if (renormScale2 == 3) Q2RenSave = pT2 + 0.5 * (s3 + s4); else Q2RenSave = sH; Q2RenSave *= renormMultFac; if (renormScale2 == 5) Q2RenSave = renormFixScale; // Different options for factorization scale. if (masslessKin) Q2FacSave = (factorScale2 < 4) ? pT2 : sH; else if (factorScale2 == 1) Q2FacSave = pT2 + min(s3, s4); else if (factorScale2 == 2) Q2FacSave = sqrt((pT2 + s3) * (pT2 + s4)); else if (factorScale2 == 3) Q2FacSave = pT2 + 0.5 * (s3 + s4); else Q2FacSave = sH; Q2FacSave *= factorMultFac; if (factorScale2 == 5) Q2FacSave = factorFixScale; } // Evaluate alpha_strong and alpha_EM. alpS = couplingsPtr->alphaS(Q2RenSave); alpEM = couplingsPtr->alphaEM(Q2RenSave); } //-------------------------------------------------------------------------- // As above, special kinematics for multiparton interactions. void Sigma2Process::store2KinMPI( double x1in, double x2in, double sHin, double tHin, double uHin, double alpSin, double alpEMin, bool needMasses, double m3in, double m4in) { // Default ordering of particles 3 and 4. swapTU = false; // Incoming x values. x1Save = x1in; x2Save = x2in; // Standard Mandelstam variables and their squares. sH = sHin; tH = tHin; uH = uHin; mH = sqrt(sH); sH2 = sH * sH; tH2 = tH * tH; uH2 = uH * uH; // Strong and electroweak couplings. alpS = alpSin; alpEM = alpEMin; // Assume vanishing masses. (Will be modified in final kinematics.) m3 = 0.; s3 = 0.; m4 = 0.; s4 = 0.; sHBeta = sH; // Scattering angle. cosTheta = (tH - uH) / sH; sinTheta = 2. * sqrtpos( tH * uH ) / sH; // In some cases must use masses and redefine meaning of tHat and uHat. if (needMasses) { m3 = m3in; s3 = m3 * m3; m4 = m4in; s4 = m4 * m4; sHMass = sH - s3 - s4; sHBeta = sqrtpos(sHMass*sHMass - 4. * s3 * s4); tH = -0.5 * (sHMass - sHBeta * cosTheta); uH = -0.5 * (sHMass + sHBeta * cosTheta); tH2 = tH * tH; uH2 = uH * uH; } // pT2 with masses (at this stage) included. pT2Mass = 0.25 * sHBeta * pow2(sinTheta); } //-------------------------------------------------------------------------- // Perform kinematics for a multiparton interaction, including a rescattering. bool Sigma2Process::final2KinMPI( int i1Res, int i2Res, Vec4 p1Res, Vec4 p2Res, double m1Res, double m2Res) { // Have to set flavours and colours. setIdColAcol(); // Check that masses of outgoing particles not too big. m3 = particleDataPtr->m0(idSave[3]); m4 = particleDataPtr->m0(idSave[4]); mH = sqrt(sH); if (m3 + m4 + MASSMARGIN > mH) return false; s3 = m3 * m3; s4 = m4 * m4; // Do kinematics of the production; without or with masses. double e1In = 0.5 * mH; double e2In = e1In; double pzIn = e1In; if (i1Res > 0 || i2Res > 0) { double s1 = m1Res * m1Res; double s2 = m2Res * m2Res; e1In = 0.5 * (sH + s1 - s2) / mH; e2In = 0.5 * (sH + s2 - s1) / mH; pzIn = sqrtpos( e1In*e1In - s1 ); } // Do kinematics of the decay. double e3 = 0.5 * (sH + s3 - s4) / mH; double e4 = 0.5 * (sH + s4 - s3) / mH; double pAbs = sqrtpos( e3*e3 - s3 ); phi = 2. * M_PI * rndmPtr->flat(); double pZ = pAbs * cosTheta; pTFin = pAbs * sinTheta; double pX = pTFin * sin(phi); double pY = pTFin * cos(phi); double scale = 0.5 * mH * sinTheta; // Fill particle info. int status1 = (i1Res == 0) ? -31 : -34; int status2 = (i2Res == 0) ? -31 : -34; parton[1] = Particle( idSave[1], status1, 0, 0, 3, 4, colSave[1], acolSave[1], 0., 0., pzIn, e1In, m1Res, scale); parton[2] = Particle( idSave[2], status2, 0, 0, 3, 4, colSave[2], acolSave[2], 0., 0., -pzIn, e2In, m2Res, scale); parton[3] = Particle( idSave[3], 33, 1, 2, 0, 0, colSave[3], acolSave[3], pX, pY, pZ, e3, m3, scale); parton[4] = Particle( idSave[4], 33, 1, 2, 0, 0, colSave[4], acolSave[4], -pX, -pY, -pZ, e4, m4, scale); // Boost particles from subprocess rest frame to event rest frame. // Normal multiparton interaction: only longitudinal boost. if (i1Res == 0 && i2Res == 0) { double betaZ = (x1Save - x2Save) / (x1Save + x2Save); for (int i = 1; i <= 4; ++i) parton[i].bst(0., 0., betaZ); // Rescattering: generic rotation and boost required. } else { RotBstMatrix M; M.fromCMframe( p1Res, p2Res); for (int i = 1; i <= 4; ++i) parton[i].rotbst(M); } // Done. return true; } //-------------------------------------------------------------------------- // Calculate modified masses and four-vectors for matrix elements. bool Sigma2Process::setupForME() { // Common initial-state handling. bool allowME = setupForMEin(); // Correct outgoing c, b, mu and tau to be massive or not. mME[2] = m3; int id3Tmp = abs(id3Mass()); if (id3Tmp == 4) mME[2] = mcME; if (id3Tmp == 5) mME[2] = mbME; if (id3Tmp == 13) mME[2] = mmuME; if (id3Tmp == 15) mME[2] = mtauME; mME[3] = m4; int id4Tmp = abs(id4Mass()); if (id4Tmp == 4) mME[3] = mcME; if (id4Tmp == 5) mME[3] = mbME; if (id4Tmp == 13) mME[3] = mmuME; if (id4Tmp == 15) mME[3] = mtauME; // If kinematically impossible turn to massless case, but set error. if (mME[2] + mME[3] >= mH) { mME[2] = 0.; mME[3] = 0.; allowME = false; } // Calculate scattering angle in subsystem rest frame. double sH34 = sqrtpos( pow2(sH - s3 - s4) - 4. * s3 * s4); double cThe = (tH - uH) / sH34; double sThe = sqrtpos(1. - cThe * cThe); // Setup massive kinematics with preserved scattering angle. double s3ME = pow2(mME[2]); double s4ME = pow2(mME[3]); double sH34ME = sqrtpos( pow2(sH - s3ME - s4ME) - 4. * s3ME * s4ME); double pAbsME = 0.5 * sH34ME / mH; // Normally allowed with unequal (or vanishing) masses. if (id3Tmp == 0 || id3Tmp != id4Tmp) { pME[2] = Vec4( pAbsME * sThe, 0., pAbsME * cThe, 0.5 * (sH + s3ME - s4ME) / mH); pME[3] = Vec4( -pAbsME * sThe, 0., -pAbsME * cThe, 0.5 * (sH + s4ME - s3ME) / mH); // For equal (anti)particles (e.g. W+ W-) use averaged mass. } else { mME[2] = sqrtpos(0.5 * (s3ME + s4ME) - 0.25 * pow2(s3ME - s4ME) / sH); mME[3] = mME[2]; pME[2] = Vec4( pAbsME * sThe, 0., pAbsME * cThe, 0.5 * mH); pME[3] = Vec4( -pAbsME * sThe, 0., -pAbsME * cThe, 0.5 * mH); } // Done. return allowME; } //========================================================================== // The Sigma3Process class. // Base class for resolved 2 -> 3 cross sections; derived from SigmaProcess. //-------------------------------------------------------------------------- // Input and complement kinematics for resolved 2 -> 3 process. void Sigma3Process::store3Kin( double x1in, double x2in, double sHin, Vec4 p3cmIn, Vec4 p4cmIn, Vec4 p5cmIn, double m3in, double m4in, double m5in, double runBW3in, double runBW4in, double runBW5in) { // Default ordering of particles 3 and 4 - not relevant here. swapTU = false; // Incoming parton momentum fractions. x1Save = x1in; x2Save = x2in; // Incoming masses and their squares. if (id3Mass() == 0 && id4Mass() == 0 && id5Mass() == 0) { m3 = 0.; m4 = 0.; m5 = 0.; } else { m3 = m3in; m4 = m4in; m5 = m5in; } mSave[3] = m3; mSave[4] = m4; mSave[5] = m5; s3 = m3 * m3; s4 = m4 * m4; s5 = m5 * m5; // Standard Mandelstam variables and four-momenta in rest frame. sH = sHin; mH = sqrt(sH); sH2 = sH * sH; p3cm = p3cmIn; p4cm = p4cmIn; p5cm = p5cmIn; // The nominal Breit-Wigner factors with running width. runBW3 = runBW3in; runBW4 = runBW4in; runBW5 = runBW5in; // Special case: pick scale as if 2 -> 1 process in disguise. if (isSChannel()) { // Different options for renormalization scale, but normally sHat. Q2RenSave = renormMultFac * sH; if (renormScale1 == 2) Q2RenSave = renormFixScale; // Different options for factorization scale, but normally sHat. Q2FacSave = factorMultFac * sH; if (factorScale1 == 2) Q2RenSave = factorFixScale; // "Normal" 2 -> 3 processes, i.e. not vector boson fusion. } else if ( idTchan1() != 23 && idTchan1() != 24 && idTchan2() != 23 && idTchan2() != 24 ) { double mT3S = s3 + p3cm.pT2(); double mT4S = s4 + p4cm.pT2(); double mT5S = s5 + p5cm.pT2(); // Different options for renormalization scale. if (renormScale3 == 1) Q2RenSave = min( mT3S, min(mT4S, mT5S) ); else if (renormScale3 == 2) Q2RenSave = sqrt( mT3S * mT4S * mT5S / max( mT3S, max(mT4S, mT5S) ) ); else if (renormScale3 == 3) Q2RenSave = pow( mT3S * mT4S * mT5S, 1./3. ); else if (renormScale3 == 4) Q2RenSave = (mT3S + mT4S + mT5S) / 3.; else Q2RenSave = sH; Q2RenSave *= renormMultFac; if (renormScale3 == 6) Q2RenSave = renormFixScale; // Different options for factorization scale. if (factorScale3 == 1) Q2FacSave = min( mT3S, min(mT4S, mT5S) ); else if (factorScale3 == 2) Q2FacSave = sqrt( mT3S * mT4S * mT5S / max( mT3S, max(mT4S, mT5S) ) ); else if (factorScale3 == 3) Q2FacSave = pow( mT3S * mT4S * mT5S, 1./3. ); else if (factorScale3 == 4) Q2FacSave = (mT3S + mT4S + mT5S) / 3.; else Q2FacSave = sH; Q2FacSave *= factorMultFac; if (factorScale3 == 6) Q2FacSave = factorFixScale; // Vector boson fusion 2 -> 3 processes; recoils in positions 4 and 5. } else { double sV4 = pow2( particleDataPtr->m0(idTchan1()) ); double sV5 = pow2( particleDataPtr->m0(idTchan2()) ); double mT3S = s3 + p3cm.pT2(); double mTV4S = sV4 + p4cm.pT2(); double mTV5S = sV5 + p5cm.pT2(); // Different options for renormalization scale. if (renormScale3VV == 1) Q2RenSave = max( sV4, sV5); else if (renormScale3VV == 2) Q2RenSave = sqrt( mTV4S * mTV5S ); else if (renormScale3VV == 3) Q2RenSave = pow( mT3S * mTV4S * mTV5S, 1./3. ); else if (renormScale3VV == 4) Q2RenSave = (mT3S * mTV4S * mTV5S) / 3.; else Q2RenSave = sH; Q2RenSave *= renormMultFac; if (renormScale3VV == 6) Q2RenSave = renormFixScale; // Different options for factorization scale. if (factorScale3VV == 1) Q2FacSave = max( sV4, sV5); else if (factorScale3VV == 2) Q2FacSave = sqrt( mTV4S * mTV5S ); else if (factorScale3VV == 3) Q2FacSave = pow( mT3S * mTV4S * mTV5S, 1./3. ); else if (factorScale3VV == 4) Q2FacSave = (mT3S * mTV4S * mTV5S) / 3.; else Q2FacSave = sH; Q2FacSave *= factorMultFac; if (factorScale3VV == 6) Q2FacSave = factorFixScale; } // Evaluate alpha_strong and alpha_EM. alpS = couplingsPtr->alphaS(Q2RenSave); alpEM = couplingsPtr->alphaEM(Q2RenSave); } //-------------------------------------------------------------------------- // Calculate modified masses and four-vectors for matrix elements. bool Sigma3Process::setupForME() { // Common initial-state handling. bool allowME = setupForMEin(); // Correct outgoing c, b, mu and tau to be massive or not. mME[2] = m3; int id3Tmp = abs(id3Mass()); if (id3Tmp == 4) mME[2] = mcME; if (id3Tmp == 5) mME[2] = mbME; if (id3Tmp == 13) mME[2] = mmuME; if (id3Tmp == 15) mME[2] = mtauME; mME[3] = m4; int id4Tmp = abs(id4Mass()); if (id4Tmp == 4) mME[3] = mcME; if (id4Tmp == 5) mME[3] = mbME; if (id4Tmp == 13) mME[3] = mmuME; if (id4Tmp == 15) mME[3] = mtauME; mME[4] = m5; int id5Tmp = abs(id5Mass()); if (id5Tmp == 4) mME[4] = mcME; if (id5Tmp == 5) mME[4] = mbME; if (id5Tmp == 13) mME[4] = mmuME; if (id5Tmp == 15) mME[4] = mtauME; // If kinematically impossible turn to massless case, but set error. if (mME[2] + mME[3] + mME[4] >= mH) { mME[2] = 0.; mME[3] = 0.; mME[4] = 0.; allowME = false; } // Form new average masses if identical particles. if (id3Tmp != 0 && id4Tmp == id3Tmp && id5Tmp == id3Tmp) { double mAvg = (mME[2] + mME[3] + mME[4]) / 3.; mME[2] = mAvg; mME[3] = mAvg; mME[4] = mAvg; } else if (id3Tmp != 0 && id4Tmp == id3Tmp) { mME[2] = sqrtpos(0.5 * (pow2(mME[2]) + pow2(mME[3])) - 0.25 * pow2(pow2(mME[2]) - pow2(mME[3])) / sH); mME[3] = mME[2]; } else if (id3Tmp != 0 && id5Tmp == id3Tmp) { mME[2] = sqrtpos(0.5 * (pow2(mME[2]) + pow2(mME[4])) - 0.25 * pow2(pow2(mME[2]) - pow2(mME[4])) / sH); mME[4] = mME[2]; } else if (id4Tmp != 0 && id5Tmp == id4Tmp) { mME[3] = sqrtpos(0.5 * (pow2(mME[3]) + pow2(mME[4])) - 0.25 * pow2(pow2(mME[3]) - pow2(mME[4])) / sH); mME[4] = mME[2]; } // Iterate rescaled three-momenta until convergence. double m2ME3 = pow2(mME[2]); double m2ME4 = pow2(mME[3]); double m2ME5 = pow2(mME[4]); double p2ME3 = p3cm.pAbs2(); double p2ME4 = p4cm.pAbs2(); double p2ME5 = p5cm.pAbs2(); double p2sum = p2ME3 + p2ME4 + p2ME5; double eME3 = sqrt(m2ME3 + p2ME3); double eME4 = sqrt(m2ME4 + p2ME4); double eME5 = sqrt(m2ME5 + p2ME5); double esum = eME3 + eME4 + eME5; double p2rat = p2ME3 / eME3 + p2ME4 / eME4 + p2ME5 / eME5; int iStep = 0; while ( abs(esum - mH) > COMPRELERR * mH && iStep < NCOMPSTEP ) { ++iStep; double compFac = 1. + 2. * (mH - esum) / p2rat; p2ME3 *= compFac; p2ME4 *= compFac; p2ME5 *= compFac; eME3 = sqrt(m2ME3 + p2ME3); eME4 = sqrt(m2ME4 + p2ME4); eME5 = sqrt(m2ME5 + p2ME5); esum = eME3 + eME4 + eME5; p2rat = p2ME3 / eME3 + p2ME4 / eME4 + p2ME5 / eME5; } // If failed convergence set error flag. if (abs(esum - mH) > COMPRELERR * mH) allowME = false; // Set up accepted kinematics. double totFac = sqrt( (p2ME3 + p2ME4 + p2ME5) / p2sum); pME[2] = totFac * p3cm; pME[2].e( eME3); pME[3] = totFac * p4cm; pME[3].e( eME4); pME[4] = totFac * p5cm; pME[4].e( eME5); // Done. return allowME; } //========================================================================== // The SigmaLHAProcess class. // Wrapper for Les Houches Accord external input; derived from SigmaProcess. // Note: arbitrary subdivision into PhaseSpaceLHA and SigmaLHAProcess tasks. //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double SigmaLHAProcess::weightDecay( Event& process, int iResBeg, int iResEnd) { // Do nothing if decays present already at input. if (iResBeg < process.savedSizeValue()) return 1.; // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //-------------------------------------------------------------------------- // Set scale, alpha_strong and alpha_EM when not set. void SigmaLHAProcess::setScale() { // If scale has not been set, then to set. double scaleLHA = lhaUpPtr->scale(); if (scaleLHA < 0.) { // Final-state partons and their invariant mass. vector iFin; Vec4 pFinSum; for (int i = 3; i < lhaUpPtr->sizePart(); ++i) if (lhaUpPtr->mother1(i) == 1) { iFin.push_back(i); pFinSum += Vec4( lhaUpPtr->px(i), lhaUpPtr->py(i), lhaUpPtr->pz(i), lhaUpPtr->e(i) ); } int nFin = iFin.size(); sH = pFinSum * pFinSum; mH = sqrt(sH); sH2 = sH * sH; // If 1 final-state particle then use Sigma1Process logic. if (nFin == 1) { Q2RenSave = renormMultFac * sH; if (renormScale1 == 2) Q2RenSave = renormFixScale; Q2FacSave = factorMultFac * sH; if (factorScale1 == 2) Q2FacSave = factorFixScale; // If 2 final-state particles then use Sigma2Process logic. } else if (nFin == 2) { double s3 = pow2(lhaUpPtr->m(iFin[0])); double s4 = pow2(lhaUpPtr->m(iFin[1])); double pT2 = pow2(lhaUpPtr->px(iFin[0])) + pow2(lhaUpPtr->py(iFin[0])); if (renormScale2 == 1) Q2RenSave = pT2 + min(s3, s4); else if (renormScale2 == 2) Q2RenSave = sqrt((pT2 + s3) * (pT2 + s4)); else if (renormScale2 == 3) Q2RenSave = pT2 + 0.5 * (s3 + s4); else Q2RenSave = sH; Q2RenSave *= renormMultFac; if (renormScale2 == 5) Q2RenSave = renormFixScale; if (factorScale2 == 1) Q2FacSave = pT2 + min(s3, s4); else if (factorScale2 == 2) Q2FacSave = sqrt((pT2 + s3) * (pT2 + s4)); else if (factorScale2 == 3) Q2FacSave = pT2 + 0.5 * (s3 + s4); else Q2FacSave = sH; Q2FacSave *= factorMultFac; if (factorScale2 == 5) Q2FacSave = factorFixScale; // If 3 or more final-state particles then use Sigma3Process logic. } else { double mTSlow = sH; double mTSmed = sH; double mTSprod = 1.; double mTSsum = 0.; for (int i = 0; i < nFin; ++i) { double mTSnow = pow2(lhaUpPtr->m(iFin[i])) + pow2(lhaUpPtr->px(iFin[i])) + pow2(lhaUpPtr->py(iFin[i])); if (mTSnow < mTSlow) {mTSmed = mTSlow; mTSlow = mTSnow;} else if (mTSnow < mTSmed) mTSmed = mTSnow; mTSprod *= mTSnow; mTSsum += mTSnow; } if (renormScale3 == 1) Q2RenSave = mTSlow; else if (renormScale3 == 2) Q2RenSave = sqrt(mTSlow * mTSmed); else if (renormScale3 == 3) Q2RenSave = pow(mTSprod, 1. / nFin); else if (renormScale3 == 4) Q2RenSave = mTSsum / nFin; else Q2RenSave = sH; Q2RenSave *= renormMultFac; if (renormScale3 == 6) Q2RenSave = renormFixScale; if (factorScale3 == 1) Q2FacSave = mTSlow; else if (factorScale3 == 2) Q2FacSave = sqrt(mTSlow * mTSmed); else if (factorScale3 == 3) Q2FacSave = pow(mTSprod, 1. / nFin); else if (factorScale3 == 4) Q2FacSave = mTSsum / nFin; else Q2FacSave = sH; Q2FacSave *= factorMultFac; if (factorScale3 == 6) Q2FacSave = factorFixScale; } } // If alpha_strong and alpha_EM have not been set, then set them. if (lhaUpPtr->alphaQCD() < 0.001) { double Q2RenNow = (scaleLHA < 0.) ? Q2RenSave : pow2(scaleLHA); alpS = couplingsPtr->alphaS(Q2RenNow); } if (lhaUpPtr->alphaQED() < 0.001) { double Q2RenNow = (scaleLHA < 0.) ? Q2RenSave : pow2(scaleLHA); alpEM = couplingsPtr->alphaEM(Q2RenNow); } } //-------------------------------------------------------------------------- // Obtain number of final-state partons from LHA object. int SigmaLHAProcess::nFinal() const { // At initialization size unknown, so return 0. if (lhaUpPtr->sizePart() <= 0) return 0; // Sum up all particles that has first mother = 1. int nFin = 0; for (int i = 3; i < lhaUpPtr->sizePart(); ++i) if (lhaUpPtr->mother1(i) == 1) ++nFin; return nFin; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/ProcessLevel.cc0000644000175000017500000013677312217346247016066 0ustar sunsun// ProcessLevel.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the ProcessLevel class. #include "Pythia8/ProcessLevel.h" namespace Pythia8 { //========================================================================== // The ProcessLevel class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Allow a few failures in final construction of events. const int ProcessLevel::MAXLOOP = 5; //-------------------------------------------------------------------------- // Destructor. ProcessLevel::~ProcessLevel() { // Run through list of first hard processes and delete them. for (int i = 0; i < int(containerPtrs.size()); ++i) delete containerPtrs[i]; // Run through list of second hard processes and delete them. for (int i = 0; i < int(container2Ptrs.size()); ++i) delete container2Ptrs[i]; } //-------------------------------------------------------------------------- // Main routine to initialize generation process. bool ProcessLevel::init( Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, Couplings* couplingsPtrIn, SigmaTotal* sigmaTotPtrIn, bool doLHA, SLHAinterface* slhaInterfacePtrIn, UserHooks* userHooksPtrIn, vector& sigmaPtrs, ostream& os) { // Store input pointers for future use. infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; couplingsPtr = couplingsPtrIn; sigmaTotPtr = sigmaTotPtrIn; userHooksPtr = userHooksPtrIn; slhaInterfacePtr = slhaInterfacePtrIn; // Send on some input pointers. resonanceDecays.init( infoPtr, particleDataPtr, rndmPtr); // Set up SigmaTotal. Store sigma_nondiffractive for future use. sigmaTotPtr->init( infoPtr, settings, particleDataPtr); int idA = infoPtr->idA(); int idB = infoPtr->idB(); double eCM = infoPtr->eCM(); sigmaTotPtr->calc( idA, idB, eCM); sigmaND = sigmaTotPtr->sigmaND(); // Options to allow second hard interaction and resonance decays. doSecondHard = settings.flag("SecondHard:generate"); doSameCuts = settings.flag("PhaseSpace:sameForSecond"); doResDecays = settings.flag("ProcessLevel:resonanceDecays"); startColTag = settings.mode("Event:startColTag"); // Second interaction not to be combined with biased phase space. if (doSecondHard && userHooksPtr != 0 && userHooksPtr->canBiasSelection()) { infoPtr->errorMsg("Error in ProcessLevel::init: " "cannot combine second interaction with biased phase space"); return false; } // Mass and pT cuts for two hard processes. mHatMin1 = settings.parm("PhaseSpace:mHatMin"); mHatMax1 = settings.parm("PhaseSpace:mHatMax"); if (mHatMax1 < mHatMin1) mHatMax1 = eCM; pTHatMin1 = settings.parm("PhaseSpace:pTHatMin"); pTHatMax1 = settings.parm("PhaseSpace:pTHatMax"); if (pTHatMax1 < pTHatMin1) pTHatMax1 = eCM; mHatMin2 = settings.parm("PhaseSpace:mHatMinSecond"); mHatMax2 = settings.parm("PhaseSpace:mHatMaxSecond"); if (mHatMax2 < mHatMin2) mHatMax2 = eCM; pTHatMin2 = settings.parm("PhaseSpace:pTHatMinSecond"); pTHatMax2 = settings.parm("PhaseSpace:pTHatMaxSecond"); if (pTHatMax2 < pTHatMin2) pTHatMax2 = eCM; // Check whether mass and pT ranges agree or overlap. cutsAgree = doSameCuts; if (mHatMin2 == mHatMin1 && mHatMax2 == mHatMax1 && pTHatMin2 == pTHatMin1 && pTHatMax2 == pTHatMax1) cutsAgree = true; cutsOverlap = cutsAgree; if (!cutsAgree) { bool mHatOverlap = (max( mHatMin1, mHatMin2) < min( mHatMax1, mHatMax2)); bool pTHatOverlap = (max( pTHatMin1, pTHatMin2) < min( pTHatMax1, pTHatMax2)); if (mHatOverlap && pTHatOverlap) cutsOverlap = true; } // Set up containers for all the internal hard processes. SetupContainers setupContainers; setupContainers.init(containerPtrs, settings, particleDataPtr, couplingsPtr); // Append containers for external hard processes, if any. if (sigmaPtrs.size() > 0) { for (int iSig = 0; iSig < int(sigmaPtrs.size()); ++iSig) containerPtrs.push_back( new ProcessContainer(sigmaPtrs[iSig], true) ); } // Append single container for Les Houches processes, if any. if (doLHA) { SigmaProcess* sigmaPtr = new SigmaLHAProcess(); containerPtrs.push_back( new ProcessContainer(sigmaPtr) ); // Store location of this container, and send in LHA pointer. iLHACont = containerPtrs.size() - 1; containerPtrs[iLHACont]->setLHAPtr(lhaUpPtr); } // If no processes found then refuse to do anything. if ( int(containerPtrs.size()) == 0) { infoPtr->errorMsg("Error in ProcessLevel::init: " "no process switched on"); return false; } // Check whether pT-based weighting in 2 -> 2 is requested. if (settings.flag("PhaseSpace:bias2Selection")) { bool bias2Sel = false; if (sigmaPtrs.size() == 0 && !doLHA && !doSecondHard) { bias2Sel = true; for (int i = 0; i < int(containerPtrs.size()); ++i) { if (containerPtrs[i]->nFinal() != 2) bias2Sel = false; int code = containerPtrs[i]->code(); if (code > 100 && code < 110) bias2Sel = false; } } if (!bias2Sel) { infoPtr->errorMsg("Error in ProcessLevel::init: " "requested event weighting not possible"); return false; } } // Check that SUSY couplings were indeed initialized where necessary. bool hasSUSY = false; for (int i = 0; i < int(containerPtrs.size()); ++i) if (containerPtrs[i]->isSUSY()) hasSUSY = true; // If SUSY processes requested but no SUSY couplings present if(hasSUSY && !couplingsPtr->isSUSY) { infoPtr->errorMsg("Error in ProcessLevel::init: " "SUSY process switched on but no SUSY couplings found"); return false; } // Fill SLHA blocks SMINPUTS and MASS from PYTHIA SM parameter values. slhaInterfacePtr->pythia2slha(particleDataPtr); // Initialize each process. int numberOn = 0; for (int i = 0; i < int(containerPtrs.size()); ++i) if (containerPtrs[i]->init(true, infoPtr, settings, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr, sigmaTotPtr, &resonanceDecays, slhaInterfacePtr, userHooksPtr)) ++numberOn; // Sum maxima for Monte Carlo choice. sigmaMaxSum = 0.; for (int i = 0; i < int(containerPtrs.size()); ++i) sigmaMaxSum += containerPtrs[i]->sigmaMax(); // Option to pick a second hard interaction: repeat as above. int number2On = 0; if (doSecondHard) { setupContainers.init2(container2Ptrs, settings); if ( int(container2Ptrs.size()) == 0) { infoPtr->errorMsg("Error in ProcessLevel::init: " "no second hard process switched on"); return false; } for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) if (container2Ptrs[i2]->init(false, infoPtr, settings, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr, sigmaTotPtr, &resonanceDecays, slhaInterfacePtr, userHooksPtr)) ++number2On; sigma2MaxSum = 0.; for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) sigma2MaxSum += container2Ptrs[i2]->sigmaMax(); } // Printout during initialization is optional. if (settings.flag("Init:showProcesses")) { // Construct string with incoming beams and for cm energy. string collision = "We collide " + particleDataPtr->name(idA) + " with " + particleDataPtr->name(idB) + " at a CM energy of "; string pad( 51 - collision.length(), ' '); // Print initialization information: header. os << "\n *------- PYTHIA Process Initialization ---------" << "-----------------*\n" << " | " << " |\n" << " | " << collision << scientific << setprecision(3) << setw(9) << eCM << " GeV" << pad << " |\n" << " | " << " |\n" << " |---------------------------------------------------" << "---------------|\n" << " | " << " | |\n" << " | Subprocess Code" << " | Estimated |\n" << " | " << " | max (mb) |\n" << " | " << " | |\n" << " |---------------------------------------------------" << "---------------|\n" << " | " << " | |\n"; // Loop over existing processes: print individual process info. for (int i = 0; i < int(containerPtrs.size()); ++i) os << " | " << left << setw(45) << containerPtrs[i]->name() << right << setw(5) << containerPtrs[i]->code() << " | " << scientific << setprecision(3) << setw(11) << containerPtrs[i]->sigmaMax() << " |\n"; // Loop over second hard processes, if any, and repeat as above. if (doSecondHard) { os << " | " << " | |\n" << " |---------------------------------------------------" <<"---------------|\n" << " | " <<" | |\n"; for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) os << " | " << left << setw(45) << container2Ptrs[i2]->name() << right << setw(5) << container2Ptrs[i2]->code() << " | " << scientific << setprecision(3) << setw(11) << container2Ptrs[i2]->sigmaMax() << " |\n"; } // Listing finished. os << " | " << " |\n" << " *------- End PYTHIA Process Initialization ----------" <<"-------------*" << endl; } // If sum of maxima vanishes then refuse to do anything. if ( numberOn == 0 || sigmaMaxSum <= 0.) { infoPtr->errorMsg("Error in ProcessLevel::init: " "all processes have vanishing cross sections"); return false; } if ( doSecondHard && (number2On == 0 || sigma2MaxSum <= 0.) ) { infoPtr->errorMsg("Error in ProcessLevel::init: " "all second hard processes have vanishing cross sections"); return false; } // If two hard processes then check whether some (but not all) agree. allHardSame = true; noneHardSame = true; if (doSecondHard) { bool foundMatch = false; // Check for each first process if matched in second. for (int i = 0; i < int(containerPtrs.size()); ++i) { foundMatch = false; if (cutsOverlap) for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) if (container2Ptrs[i2]->code() == containerPtrs[i]->code()) foundMatch = true; containerPtrs[i]->isSame( foundMatch ); if (!foundMatch) allHardSame = false; if ( foundMatch) noneHardSame = false; } // Check for each second process if matched in first. for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) { foundMatch = false; if (cutsOverlap) for (int i = 0; i < int(containerPtrs.size()); ++i) if (containerPtrs[i]->code() == container2Ptrs[i2]->code()) foundMatch = true; container2Ptrs[i2]->isSame( foundMatch ); if (!foundMatch) allHardSame = false; if ( foundMatch) noneHardSame = false; } } // Concluding classification, including cuts. if (!cutsAgree) allHardSame = false; someHardSame = !allHardSame && !noneHardSame; // Reset counters for average impact-parameter enhancement. nImpact = 0; sumImpactFac = 0.; sum2ImpactFac = 0.; // Done. return true; } //-------------------------------------------------------------------------- // Main routine to generate the hard process. bool ProcessLevel::next( Event& process) { // Generate the next event with two or one hard interactions. bool physical = (doSecondHard) ? nextTwo( process) : nextOne( process); // Check that colour assignments make sense. if (physical) physical = checkColours( process); // Done. return physical; } //-------------------------------------------------------------------------- // Generate (= read in) LHA input of resonance decay only. bool ProcessLevel::nextLHAdec( Event& process) { // Read resonance decays from LHA interface. infoPtr->setEndOfFile(false); if (!lhaUpPtr->setEvent()) { infoPtr->setEndOfFile(true); return false; } // Store LHA output in standard event record format. containerLHAdec.constructDecays( process); // Done. return true; } //-------------------------------------------------------------------------- // Accumulate and update statistics (after possible user veto). void ProcessLevel::accumulate() { // Increase number of accepted events. containerPtrs[iContainer]->accumulate(); // Provide current generated cross section estimate. long nTrySum = 0; long nSelSum = 0; long nAccSum = 0; double sigmaSum = 0.; double delta2Sum = 0.; double sigSelSum = 0.; double weightSum = 0.; int codeNow; long nTryNow, nSelNow, nAccNow; double sigmaNow, deltaNow, sigSelNow, weightNow; for (int i = 0; i < int(containerPtrs.size()); ++i) if (containerPtrs[i]->sigmaMax() != 0.) { codeNow = containerPtrs[i]->code(); nTryNow = containerPtrs[i]->nTried(); nSelNow = containerPtrs[i]->nSelected(); nAccNow = containerPtrs[i]->nAccepted(); sigmaNow = containerPtrs[i]->sigmaMC(); deltaNow = containerPtrs[i]->deltaMC(); sigSelNow = containerPtrs[i]->sigmaSelMC(); weightNow = containerPtrs[i]->weightSum(); nTrySum += nTryNow; nSelSum += nSelNow; nAccSum += nAccNow; sigmaSum += sigmaNow; delta2Sum += pow2(deltaNow); sigSelSum += sigSelNow; weightSum += weightNow; if (!doSecondHard) infoPtr->setSigma( codeNow, nTryNow, nSelNow, nAccNow, sigmaNow, deltaNow, weightNow); } // Normally only one hard interaction. Then store info and done. if (!doSecondHard) { double deltaSum = sqrtpos(delta2Sum); infoPtr->setSigma( 0, nTrySum, nSelSum, nAccSum, sigmaSum, deltaSum, weightSum); return; } // Increase counter for a second hard interaction. container2Ptrs[i2Container]->accumulate(); // Update statistics on average impact factor. ++nImpact; sumImpactFac += infoPtr->enhanceMPI(); sum2ImpactFac += pow2(infoPtr->enhanceMPI()); // Cross section estimate for second hard process. double sigma2Sum = 0.; double sig2SelSum = 0.; for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) if (container2Ptrs[i2]->sigmaMax() != 0.) { nTrySum += container2Ptrs[i2]->nTried(); sigma2Sum += container2Ptrs[i2]->sigmaMC(); sig2SelSum += container2Ptrs[i2]->sigmaSelMC(); } // Average impact-parameter factor and error. double invN = 1. / max(1, nImpact); double impactFac = max( 1., sumImpactFac * invN); double impactErr2 = ( sum2ImpactFac * invN / pow2(impactFac) - 1.) * invN; // Cross section estimate for combination of first and second process. // Combine two possible ways and take average. double sigmaComb = 0.5 * (sigmaSum * sig2SelSum + sigSelSum * sigma2Sum); sigmaComb *= impactFac / sigmaND; if (allHardSame) sigmaComb *= 0.5; double deltaComb = sqrtpos(2. / nAccSum + impactErr2) * sigmaComb; // Store info and done. infoPtr->setSigma( 0, nTrySum, nSelSum, nAccSum, sigmaComb, deltaComb, weightSum); } //-------------------------------------------------------------------------- // Print statistics on cross sections and number of events. void ProcessLevel::statistics(bool reset, ostream& os) { // Special processing if two hard interactions selected. if (doSecondHard) { statistics2(reset, os); return; } // Header. os << "\n *------- PYTHIA Event and Cross Section Statistics ------" << "-------------------------------------------------------*\n" << " | " << " |\n" << " | Subprocess Code | " << " Number of events | sigma +- delta |\n" << " | | " << "Tried Selected Accepted | (estimated) (mb) |\n" << " | | " << " | |\n" << " |------------------------------------------------------------" << "-----------------------------------------------------|\n" << " | | " << " | |\n"; // Reset sum counters. long nTrySum = 0; long nSelSum = 0; long nAccSum = 0; double sigmaSum = 0.; double delta2Sum = 0.; // Loop over existing processes. for (int i = 0; i < int(containerPtrs.size()); ++i) if (containerPtrs[i]->sigmaMax() != 0.) { // Read info for process. Sum counters. long nTry = containerPtrs[i]->nTried(); long nSel = containerPtrs[i]->nSelected(); long nAcc = containerPtrs[i]->nAccepted(); double sigma = containerPtrs[i]->sigmaMC(); double delta = containerPtrs[i]->deltaMC(); nTrySum += nTry; nSelSum += nSel; nAccSum += nAcc; sigmaSum += sigma; delta2Sum += pow2(delta); // Print individual process info. os << " | " << left << setw(45) << containerPtrs[i]->name() << right << setw(5) << containerPtrs[i]->code() << " | " << setw(11) << nTry << " " << setw(10) << nSel << " " << setw(10) << nAcc << " | " << scientific << setprecision(3) << setw(11) << sigma << setw(11) << delta << " |\n"; // Print subdivision by user code for Les Houches process. if (containerPtrs[i]->code() == 9999) for (int j = 0; j < containerPtrs[i]->codeLHASize(); ++j) os << " | ... whereof user classification code " << setw(10) << containerPtrs[i]->subCodeLHA(j) << " | " << setw(11) << containerPtrs[i]->nTriedLHA(j) << " " << setw(10) << containerPtrs[i]->nSelectedLHA(j) << " " << setw(10) << containerPtrs[i]->nAcceptedLHA(j) << " | | \n"; } // Print summed process info. os << " | | " << " | |\n" << " | " << left << setw(50) << "sum" << right << " | " << setw(11) << nTrySum << " " << setw(10) << nSelSum << " " << setw(10) << nAccSum << " | " << scientific << setprecision(3) << setw(11) << sigmaSum << setw(11) << sqrtpos(delta2Sum) << " |\n"; // Listing finished. os << " | " << " |\n" << " *------- End PYTHIA Event and Cross Section Statistics -----" << "-----------------------------------------------------*" << endl; // Optionally reset statistics contants. if (reset) resetStatistics(); } //-------------------------------------------------------------------------- // Reset statistics on cross sections and number of events. void ProcessLevel::resetStatistics() { for (int i = 0; i < int(containerPtrs.size()); ++i) containerPtrs[i]->reset(); if (doSecondHard) for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) container2Ptrs[i2]->reset(); } //-------------------------------------------------------------------------- // Generate the next event with one interaction. bool ProcessLevel::nextOne( Event& process) { // Update CM energy for phase space selection. double eCM = infoPtr->eCM(); for (int i = 0; i < int(containerPtrs.size()); ++i) containerPtrs[i]->newECM(eCM); // Outer loop in case of rare failures. bool physical = true; for (int loop = 0; loop < MAXLOOP; ++loop) { if (!physical) process.clear(); physical = true; // Loop over tries until trial event succeeds. for ( ; ; ) { // Pick one of the subprocesses. double sigmaMaxNow = sigmaMaxSum * rndmPtr->flat(); int iMax = containerPtrs.size() - 1; iContainer = -1; do sigmaMaxNow -= containerPtrs[++iContainer]->sigmaMax(); while (sigmaMaxNow > 0. && iContainer < iMax); // Do a trial event of this subprocess; accept or not. if (containerPtrs[iContainer]->trialProcess()) break; // Check for end-of-file condition for Les Houches events. if (infoPtr->atEndOfFile()) return false; } // Update sum of maxima if current maximum violated. if (containerPtrs[iContainer]->newSigmaMax()) { sigmaMaxSum = 0.; for (int i = 0; i < int(containerPtrs.size()); ++i) sigmaMaxSum += containerPtrs[i]->sigmaMax(); } // Construct kinematics of acceptable process. containerPtrs[iContainer]->constructState(); if ( !containerPtrs[iContainer]->constructProcess( process) ) physical = false; // Do all resonance decays. if ( physical && doResDecays && !containerPtrs[iContainer]->decayResonances( process) ) physical = false; // Add any junctions to the process event record list. if (physical) findJunctions( process); // Outer loop should normally work first time around. if (physical) break; } // Done. return physical; } //-------------------------------------------------------------------------- // Generate the next event with two hard interactions. bool ProcessLevel::nextTwo( Event& process) { // Update CM energy for phase space selection. double eCM = infoPtr->eCM(); for (int i = 0; i < int(containerPtrs.size()); ++i) containerPtrs[i]->newECM(eCM); for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) container2Ptrs[i2]->newECM(eCM); // Outer loop in case of rare failures. bool physical = true; for (int loop = 0; loop < MAXLOOP; ++loop) { if (!physical) process.clear(); physical = true; // Loop over both hard processes to find consistent common kinematics. for ( ; ; ) { // Loop internally over tries for hardest process until succeeds. for ( ; ; ) { // Pick one of the subprocesses. double sigmaMaxNow = sigmaMaxSum * rndmPtr->flat(); int iMax = containerPtrs.size() - 1; iContainer = -1; do sigmaMaxNow -= containerPtrs[++iContainer]->sigmaMax(); while (sigmaMaxNow > 0. && iContainer < iMax); // Do a trial event of this subprocess; accept or not. if (containerPtrs[iContainer]->trialProcess()) break; // Check for end-of-file condition for Les Houches events. if (infoPtr->atEndOfFile()) return false; } // Update sum of maxima if current maximum violated. if (containerPtrs[iContainer]->newSigmaMax()) { sigmaMaxSum = 0.; for (int i = 0; i < int(containerPtrs.size()); ++i) sigmaMaxSum += containerPtrs[i]->sigmaMax(); } // Loop internally over tries for second hardest process until succeeds. for ( ; ; ) { // Pick one of the subprocesses. double sigma2MaxNow = sigma2MaxSum * rndmPtr->flat(); int i2Max = container2Ptrs.size() - 1; i2Container = -1; do sigma2MaxNow -= container2Ptrs[++i2Container]->sigmaMax(); while (sigma2MaxNow > 0. && i2Container < i2Max); // Do a trial event of this subprocess; accept or not. if (container2Ptrs[i2Container]->trialProcess()) break; } // Update sum of maxima if current maximum violated. if (container2Ptrs[i2Container]->newSigmaMax()) { sigma2MaxSum = 0.; for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) sigma2MaxSum += container2Ptrs[i2]->sigmaMax(); } // Pick incoming flavours (etc), needed for PDF reweighting. containerPtrs[iContainer]->constructState(); container2Ptrs[i2Container]->constructState(); // Check whether common set of x values is kinematically possible. double xA1 = containerPtrs[iContainer]->x1(); double xB1 = containerPtrs[iContainer]->x2(); double xA2 = container2Ptrs[i2Container]->x1(); double xB2 = container2Ptrs[i2Container]->x2(); if (xA1 + xA2 >= 1. || xB1 + xB2 >= 1.) continue; // Reset beam contents. Naive parton densities for second interaction. // (Subsequent procedure could be symmetrized, but would be overkill.) beamAPtr->clear(); beamBPtr->clear(); int idA1 = containerPtrs[iContainer]->id1(); int idB1 = containerPtrs[iContainer]->id2(); int idA2 = container2Ptrs[i2Container]->id1(); int idB2 = container2Ptrs[i2Container]->id2(); double Q2Fac1 = containerPtrs[iContainer]->Q2Fac(); double Q2Fac2 = container2Ptrs[i2Container]->Q2Fac(); double pdfA2Raw = beamAPtr->xf( idA2, xA2,Q2Fac2); double pdfB2Raw = beamBPtr->xf( idB2, xB2,Q2Fac2); // Remove partons in first interaction from beams. beamAPtr->append( 3, idA1, xA1); beamAPtr->xfISR( 0, idA1, xA1, Q2Fac1); beamAPtr->pickValSeaComp(); beamBPtr->append( 4, idB1, xB1); beamBPtr->xfISR( 0, idB1, xB1, Q2Fac1); beamBPtr->pickValSeaComp(); // Reevaluate pdf's for second interaction and weight by reduction. double pdfA2Mod = beamAPtr->xfMPI( idA2, xA2,Q2Fac2); double pdfB2Mod = beamBPtr->xfMPI( idB2, xB2,Q2Fac2); double wtPdfMod = (pdfA2Mod * pdfB2Mod) / (pdfA2Raw * pdfB2Raw); if (wtPdfMod < rndmPtr->flat()) continue; // Reduce by a factor of 2 for identical processes when others not, // and when in same phase space region. bool toLoop = false; if ( someHardSame && containerPtrs[iContainer]->isSame() && container2Ptrs[i2Container]->isSame()) { if (cutsAgree) { if (rndmPtr->flat() > 0.5) toLoop = true; } else { double mHat1 = containerPtrs[iContainer]->mHat(); double pTHat1 = containerPtrs[iContainer]->pTHat(); double mHat2 = container2Ptrs[i2Container]->mHat(); double pTHat2 = container2Ptrs[i2Container]->pTHat(); if (mHat1 > mHatMin2 && mHat1 < mHatMax2 && pTHat1 > pTHatMin2 && pTHat1 < pTHatMax2 && mHat2 > mHatMin1 && mHat2 < mHatMax1 && pTHat2 > pTHatMin1 && pTHat2 < pTHatMax1 && rndmPtr->flat() > 0.5) toLoop = true; } } if (toLoop) continue; // If come this far then acceptable event. break; } // Construct kinematics of acceptable processes. Event process2; process2.init( "(second hard)", particleDataPtr, startColTag); process2.initColTag(); if ( !containerPtrs[iContainer]->constructProcess( process) ) physical = false; if (physical && !container2Ptrs[i2Container]->constructProcess( process2, false) ) physical = false; // Do all resonance decays. if ( physical && doResDecays && !containerPtrs[iContainer]->decayResonances( process) ) physical = false; if ( physical && doResDecays && !container2Ptrs[i2Container]->decayResonances( process2) ) physical = false; // Append second hard interaction to normal process object. if (physical) combineProcessRecords( process, process2); // Add any junctions to the process event record list. if (physical) findJunctions( process); // Outer loop should normally work first time around. if (physical) break; } // Done. return physical; } //-------------------------------------------------------------------------- // Append second hard interaction to normal process object. // Complication: all resonance decay chains must be put at the end. void ProcessLevel::combineProcessRecords( Event& process, Event& process2) { // Find first event record size, excluding resonances. int nSize = process.size(); int nHard = 5; while (nHard < nSize && process[nHard].mother1() == 3) ++nHard; // Save resonance products temporarily elsewhere. vector resProd; if (nSize > nHard) { for (int i = nHard; i < nSize; ++i) resProd.push_back( process[i] ); process.popBack(nSize - nHard); } // Find second event record size, excluding resonances. int nSize2 = process2.size(); int nHard2 = 5; while (nHard2 < nSize2 && process2[nHard2].mother1() == 3) ++nHard2; // Find amount of necessary position and colour offset for second process. int addPos = nHard - 3; int addCol = process.lastColTag() - startColTag; // Loop over all particles (except beams) from second process. for (int i = 3; i < nSize2; ++i) { // Offset mother and daughter pointers and colour tags of particle. process2[i].offsetHistory( 2, addPos, 2, addPos); process2[i].offsetCol( addCol); // Append hard-process particles from process2 to process. if (i < nHard2) process.append( process2[i] ); } // Reinsert resonance decay chains of first hard process. int addPos2 = nHard2 - 3; if (nHard < nSize) { // Offset daughter pointers of unmoved mothers. for (int i = 5; i < nHard; ++i) process[i].offsetHistory( 0, 0, nHard - 1, addPos2); // Modify history of resonance products when restoring. for (int i = 0; i < int(resProd.size()); ++i) { resProd[i].offsetHistory( nHard - 1, addPos2, nHard - 1, addPos2); process.append( resProd[i] ); } } // Insert resonance decay chains of second hard process. if (nHard2 < nSize2) { int nHard3 = nHard + nHard2 - 3; int addPos3 = nSize - nHard; // Offset daughter pointers of second-process mothers. for (int i = nHard + 2; i < nHard3; ++i) process[i].offsetHistory( 0, 0, nHard3 - 1, addPos3); // Modify history of second-process resonance products and insert. for (int i = nHard2; i < nSize2; ++i) { process2[i].offsetHistory( nHard3 - 1, addPos3, nHard3 - 1, addPos3); process.append( process2[i] ); } } // Store PDF scale for second interaction. process.scaleSecond( process2.scale() ); } //-------------------------------------------------------------------------- // Add any junctions to the process event record list. // Also check that do not doublebook if called repeatedly. void ProcessLevel::findJunctions( Event& junEvent) { // Check all hard vertices for BNV for (int i = 1; i motherList = junEvent.motherList(i); int iMot1 = motherList[0]; vector sisterList = junEvent.daughterList(iMot1); // Check baryon number of vertex. int barSum = 0; map colVertex, acolVertex; // Loop over mothers (enter with crossed colors and negative sign). for (unsigned int indx = 0; indx < motherList.size(); indx++) { int iMot = motherList[indx]; if ( abs(junEvent[iMot].colType()) == 1 ) barSum -= junEvent[iMot].colType(); else if ( abs(junEvent[iMot].colType()) == 3) barSum -= 2*junEvent[iMot].colType()/3; int col = junEvent[iMot].acol(); int acol = junEvent[iMot].col(); // If unmatched (so far), add end. Else erase matching parton. if (col > 0) { if (acolVertex.find(col) == acolVertex.end() ) colVertex[col] = iMot; else acolVertex.erase(col); } else if (col < 0) { if (colVertex.find(-col) == colVertex.end() ) acolVertex[-col] = iMot; else colVertex.erase(-col); } if (acol > 0) { if (colVertex.find(acol) == colVertex.end()) acolVertex[acol] = iMot; else colVertex.erase(acol); } else if (acol < 0) { if (acolVertex.find(-acol) == acolVertex.end()) colVertex[-acol] = iMot; else acolVertex.erase(-acol); } } // Loop over sisters. for (unsigned int indx = 0; indx < sisterList.size(); indx++) { int iDau = sisterList[indx]; if ( abs(junEvent[iDau].colType()) == 1 ) barSum += junEvent[iDau].colType(); else if ( abs(junEvent[iDau].colType()) == 3) barSum += 2*junEvent[iDau].colType()/3; int col = junEvent[iDau].col(); int acol = junEvent[iDau].acol(); // If unmatched (so far), add end. Else erase matching parton. if (col > 0) { if (acolVertex.find(col) == acolVertex.end() ) colVertex[col] = iDau; else acolVertex.erase(col); } else if (col < 0) { if (colVertex.find(-col) == colVertex.end() ) acolVertex[-col] = iDau; else colVertex.erase(-col); } if (acol > 0) { if (colVertex.find(acol) == colVertex.end()) acolVertex[acol] = iDau; else colVertex.erase(acol); } else if (acol < 0) { if (acolVertex.find(-acol) == acolVertex.end()) colVertex[-acol] = iDau; else acolVertex.erase(-acol); } } // Skip if baryon number conserved in this vertex. if (barSum == 0) continue; // Check and skip any junctions that have already been added. for (int iJun = 0; iJun < junEvent.sizeJunction(); ++iJun) { // Remove the tags corresponding to each of the 3 existing junction legs. for (int j = 0; j < 3; ++j) { int colNow = junEvent.colJunction(iJun, j); if (junEvent.kindJunction(iJun) % 2 == 1) colVertex.erase(colNow); else acolVertex.erase(colNow); } } // Skip if no junction colors remain. if (colVertex.size() == 0 && acolVertex.size() == 0) continue; // If baryon number violated, is B = +1 or -1 (larger values not handled). int kindJun = 0; if (colVertex.size() == 3 && acolVertex.size() == 0) kindJun = 1; else if (colVertex.size() == 0 && acolVertex.size() == 3) kindJun = 2; else { infoPtr->errorMsg("Error in ProcessLevel::findJunctions: " "N(unmatched (anti)colour tags) != 3"); return; } // From now on, use colJun as shorthand for colVertex or acolVertex. map colJun = (kindJun == 1) ? colVertex : acolVertex; // Order so incoming tags appear first in colVec, outgoing tags last. vector colVec; for (map::iterator it = colJun.begin(); it != colJun.end(); it++) { int col = it->first; int iCol = it->second; for (unsigned int indx = 0; indx < motherList.size(); indx++) { if (iCol == motherList[indx]) { kindJun += 2; colVec.insert(colVec.begin(),col); } } if (colVec.size() == 0 || colVec[0] != col) colVec.push_back(col); } // Add junction with these tags. junEvent.appendJunction( kindJun, colVec[0], colVec[1], colVec[2]); } } //-------------------------------------------------------------------------- // Check that colours match up. bool ProcessLevel::checkColours( Event& process) { // Variables and arrays for common usage. bool physical = true; bool match; int colType, col, acol, iPos, iNow, iNowA; vector colTags, colPos, acolPos; // Check that each particle has the kind of colours expected of it. for (int i = 0; i < process.size(); ++i) { colType = process[i].colType(); col = process[i].col(); acol = process[i].acol(); if (colType == 0 && (col != 0 || acol != 0)) physical = false; else if (colType == 1 && (col <= 0 || acol != 0)) physical = false; else if (colType == -1 && (col != 0 || acol <= 0)) physical = false; else if (colType == 2 && (col <= 0 || acol <= 0)) physical = false; // Preparations for colour-sextet assignments // (colour,colour) = (colour,negative anticolour) else if (colType == 3 && (col <= 0 || acol >= 0)) physical = false; else if (colType == -3 && (col >= 0 || acol <= 0)) physical = false; // All other cases else if (colType < -1 || colType > 3) physical = false; // Add to the list of colour tags. if (col > 0) { match = false; for (int ic = 0; ic < int(colTags.size()) ; ++ic) if (col == colTags[ic]) match = true; if (!match) colTags.push_back(col); } else if (acol > 0) { match = false; for (int ic = 0; ic < int(colTags.size()) ; ++ic) if (acol == colTags[ic]) match = true; if (!match) colTags.push_back(acol); } // Colour sextets : map negative colour -> anticolour and vice versa else if (col < 0) { match = false; for (int ic = 0; ic < int(colTags.size()) ; ++ic) if (-col == colTags[ic]) match = true; if (!match) colTags.push_back(-col); } else if (acol < 0) { match = false; for (int ic = 0; ic < int(colTags.size()) ; ++ic) if (-acol == colTags[ic]) match = true; if (!match) colTags.push_back(-acol); } } // Warn and give up if particles did not have the expected colours. if (!physical) { infoPtr->errorMsg("Error in ProcessLevel::checkColours: " "incorrect colour assignment"); return false; } // Remove (anti)colours coming from an (anti)junction. for (int iJun = 0; iJun < process.sizeJunction(); ++iJun) { for (int j = 0; j < 3; ++j) { int colJun = process.colJunction(iJun, j); for (int ic = 0; ic < int(colTags.size()) ; ++ic) if (colJun == colTags[ic]) { colTags[ic] = colTags[colTags.size() - 1]; colTags.pop_back(); break; } } } // Loop through all colour tags and find their positions (by sign). for (int ic = 0; ic < int(colTags.size()); ++ic) { col = colTags[ic]; colPos.resize(0); acolPos.resize(0); for (int i = 0; i < process.size(); ++i) { if (process[i].col() == col || process[i].acol() == -col) colPos.push_back(i); if (process[i].acol() == col || process[i].col() == -col) acolPos.push_back(i); } // Trace colours back through decays; remove daughters. while (colPos.size() > 1) { iPos = colPos.size() - 1; iNow = colPos[iPos]; if ( process[iNow].mother1() == colPos[iPos - 1] && process[iNow].mother2() == 0) colPos.pop_back(); else break; } while (acolPos.size() > 1) { iPos = acolPos.size() - 1; iNow = acolPos[iPos]; if ( process[iNow].mother1() == acolPos[iPos - 1] && process[iNow].mother2() == 0) acolPos.pop_back(); else break; } // Now colour should exist in only 2 copies. if (colPos.size() + acolPos.size() != 2) physical = false; // If both colours or both anticolours then one mother of the other. else if (colPos.size() == 2) { iNow = colPos[1]; if ( process[iNow].mother1() != colPos[0] && process[iNow].mother2() != colPos[0] ) physical = false; } else if (acolPos.size() == 2) { iNowA = acolPos[1]; if ( process[iNowA].mother1() != acolPos[0] && process[iNowA].mother2() != acolPos[0] ) physical = false; } // If one of each then should have same mother(s), or point to beams. else { iNow = colPos[0]; iNowA = acolPos[0]; if ( process[iNow].status() == -21 && process[iNowA].status() == -21 ); else if ( (process[iNow].mother1() != process[iNowA].mother1()) || (process[iNow].mother2() != process[iNowA].mother2()) ) physical = false; } } // Error message if problem found. Done. if (!physical) infoPtr->errorMsg("Error in ProcessLevel::checkColours: " "unphysical colour flow"); return physical; } //-------------------------------------------------------------------------- // Print statistics when two hard processes allowed. void ProcessLevel::statistics2(bool reset, ostream& os) { // Average impact-parameter factor and error. double invN = 1. / max(1, nImpact); double impactFac = max( 1., sumImpactFac * invN); double impactErr2 = ( sum2ImpactFac * invN / pow2(impactFac) - 1.) * invN; // Derive scaling factor to be applied to first set of processes. double sigma2SelSum = 0.; int n2SelSum = 0; for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) { sigma2SelSum += container2Ptrs[i2]->sigmaSelMC(); n2SelSum += container2Ptrs[i2]->nSelected(); } double factor1 = impactFac * sigma2SelSum / sigmaND; double rel1Err = sqrt(1. / max(1, n2SelSum) + impactErr2); if (allHardSame) factor1 *= 0.5; // Derive scaling factor to be applied to second set of processes. double sigma1SelSum = 0.; int n1SelSum = 0; for (int i = 0; i < int(containerPtrs.size()); ++i) { sigma1SelSum += containerPtrs[i]->sigmaSelMC(); n1SelSum += containerPtrs[i]->nSelected(); } double factor2 = impactFac * sigma1SelSum / sigmaND; if (allHardSame) factor2 *= 0.5; double rel2Err = sqrt(1. / max(1, n1SelSum) + impactErr2); // Header. os << "\n *------- PYTHIA Event and Cross Section Statistics ------" << "--------------------------------------------------*\n" << " | " << " |\n" << " | Subprocess Code | " << "Number of events | sigma +- delta |\n" << " | | Tried" << " Selected Accepted | (estimated) (mb) |\n" << " | | " << " | |\n" << " |------------------------------------------------------------" << "------------------------------------------------|\n" << " | | " << " | |\n" << " | First hard process: | " << " | |\n" << " | | " << " | |\n"; // Reset sum counters. long nTrySum = 0; long nSelSum = 0; long nAccSum = 0; double sigmaSum = 0.; double delta2Sum = 0.; // Loop over existing first processes. for (int i = 0; i < int(containerPtrs.size()); ++i) if (containerPtrs[i]->sigmaMax() != 0.) { // Read info for process. Sum counters. long nTry = containerPtrs[i]->nTried(); long nSel = containerPtrs[i]->nSelected(); long nAcc = containerPtrs[i]->nAccepted(); double sigma = containerPtrs[i]->sigmaMC() * factor1; double delta2 = pow2( containerPtrs[i]->deltaMC() * factor1 ); nTrySum += nTry; nSelSum += nSel; nAccSum += nAcc; sigmaSum += sigma; delta2Sum += delta2; delta2 += pow2( sigma * rel1Err ); // Print individual process info. os << " | " << left << setw(40) << containerPtrs[i]->name() << right << setw(5) << containerPtrs[i]->code() << " | " << setw(11) << nTry << " " << setw(10) << nSel << " " << setw(10) << nAcc << " | " << scientific << setprecision(3) << setw(11) << sigma << setw(11) << sqrtpos(delta2) << " |\n"; } // Print summed info for first processes. delta2Sum += pow2( sigmaSum * rel1Err ); os << " | | " << " | |\n" << " | " << left << setw(45) << "sum" << right << " | " << setw(11) << nTrySum << " " << setw(10) << nSelSum << " " << setw(10) << nAccSum << " | " << scientific << setprecision(3) << setw(11) << sigmaSum << setw(11) << sqrtpos(delta2Sum) << " |\n"; // Separation lines to second hard processes. os << " | | " << " | |\n" << " |------------------------------------------------------------" << "------------------------------------------------|\n" << " | | " << " | |\n" << " | Second hard process: | " << " | |\n" << " | | " << " | |\n"; // Reset sum counters. nTrySum = 0; nSelSum = 0; nAccSum = 0; sigmaSum = 0.; delta2Sum = 0.; // Loop over existing second processes. for (int i2 = 0; i2 < int(container2Ptrs.size()); ++i2) if (container2Ptrs[i2]->sigmaMax() != 0.) { // Read info for process. Sum counters. long nTry = container2Ptrs[i2]->nTried(); long nSel = container2Ptrs[i2]->nSelected(); long nAcc = container2Ptrs[i2]->nAccepted(); double sigma = container2Ptrs[i2]->sigmaMC() * factor2; double delta2 = pow2( container2Ptrs[i2]->deltaMC() * factor2 ); nTrySum += nTry; nSelSum += nSel; nAccSum += nAcc; sigmaSum += sigma; delta2Sum += delta2; delta2 += pow2( sigma * rel2Err ); // Print individual process info. os << " | " << left << setw(40) << container2Ptrs[i2]->name() << right << setw(5) << container2Ptrs[i2]->code() << " | " << setw(11) << nTry << " " << setw(10) << nSel << " " << setw(10) << nAcc << " | " << scientific << setprecision(3) << setw(11) << sigma << setw(11) << sqrtpos(delta2) << " |\n"; } // Print summed info for second processes. delta2Sum += pow2( sigmaSum * rel2Err ); os << " | | " << " | |\n" << " | " << left << setw(45) << "sum" << right << " | " << setw(11) << nTrySum << " " << setw(10) << nSelSum << " " << setw(10) << nAccSum << " | " << scientific << setprecision(3) << setw(11) << sigmaSum << setw(11) << sqrtpos(delta2Sum) << " |\n"; // Print information on how the two processes were combined. os << " | | " << " | |\n" << " |------------------------------------------------------------" << "------------------------------------------------|\n" << " | " << " |\n" << " | Uncombined cross sections for the two event sets were " << setw(10) << sigma1SelSum << " and " << sigma2SelSum << " mb, " << "respectively, combined |\n" << " | using a sigma(nonDiffractive) of " << setw(10) << sigmaND << " mb and an impact-parameter enhancement factor of " << setw(10) << impactFac << ". |\n"; // Listing finished. os << " | " << " |\n" << " *------- End PYTHIA Event and Cross Section Statistics -----" << "------------------------------------------------*" << endl; // Optionally reset statistics contants. if (reset) resetStatistics(); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/HiddenValleyFragmentation.cc0000644000175000017500000003474112217346245020535 0ustar sunsun// HiddenValleyFragmentation.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // HiddenValleyFragmentation class and its helper classes. #include "Pythia8/HiddenValleyFragmentation.h" namespace Pythia8 { //========================================================================== // The HVStringFlav class is used to select HV-quark and HV-hadron flavours. //-------------------------------------------------------------------------- // Initialize data members of the flavour generation. void HVStringFlav::init(Settings& settings, Rndm* rndmPtrIn) { // Save pointer. rndmPtr = rndmPtrIn; // Read in data from Settings. nFlav = settings.mode("HiddenValley:nFlav"); probVector = settings.parm("HiddenValley:probVector"); } //-------------------------------------------------------------------------- // Pick a new HV-flavour given an incoming one. FlavContainer HVStringFlav::pick(FlavContainer& flavOld) { // Initial values for new flavour. FlavContainer flavNew; flavNew.rank = flavOld.rank + 1; // Pick new HV-flavour at random; keep track of sign. flavNew.id = 4900100 + min( 1 + int(nFlav * rndmPtr->flat()), nFlav); if (flavOld.id > 0) flavNew.id = -flavNew.id; // Done. return flavNew; } //-------------------------------------------------------------------------- // Combine two HV-flavours to produce an HV-hadron. // This is simplified procedure, assuming only two HV mesons defined. int HVStringFlav::combine(FlavContainer& flav1, FlavContainer& flav2) { // Positive and negative flavour. Note that with kinetic mixing // the Fv are really intended to represent qv, so remap. int idMeson = 0; int idPos = max( flav1.id, flav2.id) - 4900000; int idNeg = -min( flav1.id, flav2.id) - 4900000; if (idPos < 20) idPos = 101; if (idNeg < 20) idNeg = 101; // Pick HV-meson code, spin either 0 or 1. if (idNeg == idPos) idMeson = 4900111; else if (idPos > idNeg) idMeson = 4900211; else idMeson = -4900211; if (rndmPtr->flat() < probVector) idMeson += ((idMeson > 0) ? 2 : -2); // Done. return idMeson; } //========================================================================== // The HVStringPT class is used to select pT in HV fragmentation. //-------------------------------------------------------------------------- // Initialize data members of the string pT selection. void HVStringPT::init(Settings& settings, ParticleData& particleData, Rndm* rndmPtrIn) { // Save pointer. rndmPtr = rndmPtrIn; // Parameter of the pT width. No enhancement, since this is finetuning. double sigmamqv = settings.parm("HiddenValley:sigmamqv"); double sigma = sigmamqv * particleData.m0( 4900101); sigmaQ = sigma / sqrt(2.); enhancedFraction = 0.; enhancedWidth = 0.; // Parameter for pT suppression in MiniStringFragmentation. sigma2Had = 2. * pow2( max( SIGMAMIN, sigma) ); } //========================================================================== // The HVStringZ class is used to select z in HV fragmentation. //-------------------------------------------------------------------------- // Initialize data members of the string z selection. void HVStringZ::init(Settings& settings, ParticleData& particleData, Rndm* rndmPtrIn) { // Save pointer. rndmPtr = rndmPtrIn; // Paramaters of Lund/Bowler symmetric fragmentation function. aLund = settings.parm("HiddenValley:aLund"); bmqv2 = settings.parm("HiddenValley:bmqv2"); rFactqv = settings.parm("HiddenValley:rFactqv"); // Use qv mass to set scale of bEff = b * m^2; mqv2 = pow2( particleData.m0( 4900101) ); bLund = bmqv2 / mqv2; // Mass of qv meson used to set stop scale for fragmentation iteration. mhvMeson = particleData.m0( 4900111); } //-------------------------------------------------------------------------- // Generate the fraction z that the next hadron will take using Lund/Bowler. double HVStringZ::zFrag( int , int , double mT2) { // Shape parameters of Lund symmetric fragmentation function. double bShape = bLund * mT2; double cShape = 1. + rFactqv * bmqv2; return zLund( aLund, bShape, cShape); } //========================================================================== // The HiddenValleyFragmentation class. //-------------------------------------------------------------------------- // Initialize and save pointers. bool HiddenValleyFragmentation::init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn) { // Save pointers. infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; // Check whether Hidden Valley fragmentation switched on, and SU(N). doHVfrag = settings.flag("HiddenValley:fragment"); if (settings.mode("HiddenValley:Ngauge") < 2) doHVfrag = false; if (!doHVfrag) return false; // Several copies of qv may be needed. Taken to have same mass. nFlav = settings.mode("HiddenValley:nFlav"); if (nFlav > 1) { int spinType = particleDataPtr->spinType(4900101); double m0 = particleDataPtr->m0(4900101); for (int iFlav = 2; iFlav <= nFlav; ++iFlav) particleDataPtr->addParticle( 4900100 + iFlav, "qv", "qvbar", spinType, 0, 0, m0); } // Hidden Valley meson mass used to choose hadronization mode. mhvMeson = particleDataPtr->m0(4900111); // Initialize the hvEvent instance of an event record. hvEvent.init( "(Hidden Valley fragmentation)", particleDataPtr); // Create HVStringFlav instance for HV-flavour selection. hvFlavSelPtr = new HVStringFlav(); hvFlavSelPtr->init( settings, rndmPtr); // Create HVStringPT instance for pT selection in HV fragmentation. hvPTSelPtr = new HVStringPT(); hvPTSelPtr->init( settings, *particleDataPtr, rndmPtr); // Create HVStringZ instance for z selection in HV fragmentation. hvZSelPtr = new HVStringZ(); hvZSelPtr->init( settings, *particleDataPtr, rndmPtr); // Initialize auxiliary administrative class. hvColConfig.init(infoPtr, settings, hvFlavSelPtr); // Initialize HV-string and HV-ministring fragmentation. hvStringFrag.init(infoPtr, settings, particleDataPtr, rndmPtr, hvFlavSelPtr, hvPTSelPtr, hvZSelPtr); hvMinistringFrag.init(infoPtr, settings, particleDataPtr, rndmPtr, hvFlavSelPtr, hvPTSelPtr, hvZSelPtr); // Done. return true; } //-------------------------------------------------------------------------- // Perform the fragmentation. bool HiddenValleyFragmentation::fragment(Event& event) { // Reset containers for next event. hvEvent.reset(); hvColConfig.clear(); ihvParton.resize(0); // Extract HV-particles from event to hvEvent. Assign HV-colours. // Done if no HV-particles found. if (!extractHVevent(event)) return true; // Store found string system. Analyze its properties. if (!hvColConfig.insert(ihvParton, hvEvent)) return false; // Collect sequentially all partons in the HV subsystem. // Copy also if already in order, or else history tracing may fail. hvColConfig.collect(0, hvEvent, false); // Mass used to decide how to fragment system. mSys = hvColConfig[0].mass; // HV-string fragmentation when enough mass to produce >= 3 HV-mesons. if (mSys > 3.5 * mhvMeson) { if (!hvStringFrag.fragment( 0, hvColConfig, hvEvent)) return false; // HV-ministring fragmentation when enough mass to produce 2 HV-mesons. } else if (mSys > 2.1 * mhvMeson) { if (!hvMinistringFrag.fragment( 0, hvColConfig, hvEvent, true)) return false; // If only enough mass for one HV-meson assume HV-glueballs emitted. } else if (!collapseToMeson()) return false; // Insert HV particles from hvEvent to event. insertHVevent(event); // Done. return true; } //-------------------------------------------------------------------------- // Extract HV-particles from event to hvEvent. Assign HV-colours. bool HiddenValleyFragmentation::extractHVevent(Event& event) { // Copy Hidden-Valley particles to special event record. for (int i = 0; i < event.size(); ++i) { int idAbs = event[i].idAbs(); bool isHV = (idAbs > 4900000 && idAbs < 4900007) || (idAbs > 4900010 && idAbs < 4900017) || idAbs == 4900021 || idAbs == 4900101; if (isHV) { int iHV = hvEvent.append( event[i]); // Convert HV-gluons into normal ones so as to use normal machinery. if (event[i].id() == 4900021) hvEvent[iHV].id(21); // Second mother points back to position in complete event; // otherwise construct the HV history inside hvEvent. hvEvent[iHV].mothers( 0, i); hvEvent[iHV].daughters( 0, 0); int iMother = event[i].mother1(); for (int iHVM = 1; iHVM < hvEvent.size(); ++iHVM) if (hvEvent[iHVM].mother2() == iMother) { hvEvent[iHV].mother1( iHVM); if (hvEvent[iHVM].daughter1() == 0) hvEvent[iHVM].daughter1(iHV); else hvEvent[iHVM].daughter2(iHV); } } } // Done if no HV particles found. hvOldSize = hvEvent.size(); if (hvOldSize == 1) return false; // Initial colour - anticolour parton pair. int colBeg = hvEvent.nextColTag(); for (int iHV = 1; iHV < hvOldSize; ++iHV) if (hvEvent[iHV].mother1() == 0) { if (hvEvent[iHV].id() > 0) hvEvent[iHV].col( colBeg); else hvEvent[iHV].acol( colBeg); } // Then trace colours down to daughters; new colour if two daughters. for (int iHV = 1; iHV < hvOldSize; ++iHV) { int dau1 = hvEvent[iHV].daughter1(); int dau2 = hvEvent[iHV].daughter2(); if (dau1 > 0 && dau2 == 0) hvEvent[dau1].cols( hvEvent[iHV].col(), hvEvent[iHV].acol()); else if (dau2 > 0) { int colHV = hvEvent[iHV].col(); int acolHV = hvEvent[iHV].acol(); int colNew = hvEvent.nextColTag(); if (acolHV == 0) { hvEvent[dau1].cols( colNew, 0); hvEvent[dau2].cols( colHV, colNew); } else if (colHV == 0) { hvEvent[dau1].cols( 0, colNew); hvEvent[dau2].cols( colNew, acolHV); // Temporary: should seek recoiling dipole end!?? } else if (rndmPtr->flat() > 0.5) { hvEvent[dau1].cols( colHV, colNew); hvEvent[dau2].cols( colNew, acolHV); } else { hvEvent[dau1].cols( colNew, acolHV); hvEvent[dau2].cols( colHV, colNew); } } } // Pick up the colour end. int colNow = 0; for (int iHV = 1; iHV < hvOldSize; ++iHV) if (hvEvent[iHV].isFinal() && hvEvent[iHV].acol() == 0) { ihvParton.push_back( iHV); colNow = hvEvent[iHV].col(); } // Trace colour by colour until reached anticolour end. while (colNow > 0) { for (int iHV = 1; iHV < hvOldSize; ++iHV) if (hvEvent[iHV].isFinal() && hvEvent[iHV].acol() == colNow) { ihvParton.push_back( iHV); colNow = hvEvent[iHV].col(); break; } } // Done. return true; } //-------------------------------------------------------------------------- // Collapse of light system to one HV-meson, by the emission of HV-glueballs. bool HiddenValleyFragmentation::collapseToMeson() { // If too low mass then cannot do anything. Should not happen. if (mSys < 1.001 * mhvMeson) { infoPtr->errorMsg("Error in HiddenValleyFragmentation::collapseToMeson:" " too low mass to do anything"); return false; } // Choose mass of collective HV-glueball states flat between limits. double mhvGlue = (0.001 + 0.998 * rndmPtr->flat()) * (mSys - mhvMeson); // Find momentum in rest frame, with isotropic "decay" angles. double pAbs = 0.5 * sqrtpos( pow2(mSys*mSys - mhvMeson*mhvMeson - mhvGlue*mhvGlue) - pow2(2. * mhvMeson * mhvGlue) ) / mSys; double pz = (2 * rndmPtr->flat() - 1.) * pAbs; double pT = sqrtpos( pAbs*pAbs - pz*pz); double phi = 2. * M_PI * rndmPtr->flat(); double px = pT * cos(phi); double py = pT * sin(phi); // Construct four-vectors and boost them to event frame. Vec4 phvMeson( px, py, pz, sqrt(mhvMeson*mhvMeson + pAbs*pAbs) ); Vec4 phvGlue( -px, -py, -pz, sqrt(mhvGlue*mhvGlue + pAbs*pAbs) ); phvMeson.bst( hvColConfig[0].pSum ); phvGlue.bst( hvColConfig[0].pSum ); // Add produced particles to the event record. vector iParton = hvColConfig[0].iParton; int iFirst = hvEvent.append( 4900111, 82, iParton.front(), iParton.back(), 0, 0, 0, 0, phvMeson, mhvMeson); int iLast = hvEvent.append( 4900991, 82, iParton.front(), iParton.back(), 0, 0, 0, 0, phvGlue, mhvGlue); // Mark original partons as hadronized and set their daughter range. for (int i = 0; i < int(iParton.size()); ++i) { hvEvent[ iParton[i] ].statusNeg(); hvEvent[ iParton[i] ].daughters(iFirst, iLast); } // Done. return true; } //-------------------------------------------------------------------------- // Insert HV-particles from hvEvent to event. bool HiddenValleyFragmentation::insertHVevent(Event& event) { // Offset for mother/daughter indices. hvNewSize = hvEvent.size(); int nOffset = event.size() - hvOldSize; // Copy back HV-particles. int iNew, iMot1, iMot2, iDau1, iDau2; for (int iHV = hvOldSize; iHV < hvNewSize; ++iHV) { iNew = event.append( hvEvent[iHV]); // Restore HV-gluon codes. Do not keep HV-colours, to avoid confusion. if (hvEvent[iHV].id() == 21) event[iNew].id(4900021); event[iNew].cols( 0, 0); // Begin history construction. iMot1 = hvEvent[iHV].mother1(); iMot2 = hvEvent[iHV].mother2(); iDau1 = hvEvent[iHV].daughter1(); iDau2 = hvEvent[iHV].daughter2(); // Special mother for partons copied from event, else simple offset. // Also set daughters of mothers in original record. if (iMot1 > 0 && iMot1 < hvOldSize) { iMot1 = hvEvent[iMot1].mother2(); event[iMot1].statusNeg(); event[iMot1].daughter1(iNew); } else if (iMot1 > 0) iMot1 += nOffset; if (iMot2 > 0 && iMot2 < hvOldSize) { iMot2 = hvEvent[iMot2].mother2(); event[iMot2].statusNeg(); if (event[iMot2].daughter1() == 0) event[iMot2].daughter1(iNew); else event[iMot2].daughter2(iNew); } else if (iMot2 > 0) iMot2 += nOffset; if (iDau1 > 0) iDau1 += nOffset; if (iDau2 > 0) iDau2 += nOffset; event[iNew].mothers( iMot1, iMot2); event[iNew].daughters( iDau1, iDau2); } // Done. return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/PythiaStdlib.cc0000644000175000017500000000250612217346247016042 0ustar sunsun// PythiaStdlib.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the Gamma function. #include "Pythia8/PythiaStdlib.h" namespace Pythia8 { //========================================================================== // The Gamma function for real arguments, using the Lanczos approximation. // Code based on http://en.wikipedia.org/wiki/Lanczos_approximation double GammaCoef[9] = { 0.99999999999980993, 676.5203681218851, -1259.1392167224028, 771.32342877765313, -176.61502916214059, 12.507343278686905, -0.13857109526572012, 9.9843695780195716e-6, 1.5056327351493116e-7}; double GammaReal(double x) { // Reflection formula (recursive!) for x < 0.5. if (x < 0.5) return M_PI / (sin(M_PI * x) * GammaReal(1 - x)); // Iterate through terms. double z = x - 1.; double gamma = GammaCoef[0]; for (int i = 1; i < 9; ++i) gamma += GammaCoef[i] / (z + i); // Answer. double t = z + 7.5; gamma *= sqrt(2. * M_PI) * pow(t, z + 0.5) * exp(-t); return gamma; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/MergingHooks.cc0000644000175000017500000037132112217616032016032 0ustar sunsun// MergingHooks.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // This file is written by Stefan Prestel. // Function definitions (not found in the header) for the HardProcess and // MergingHooks classes. #include "Pythia8/MergingHooks.h" namespace Pythia8 { //========================================================================== // The HardProcess class. //-------------------------------------------------------------------------- // Declaration of hard process class // This class holds information on the desired hard 2->2 process to be merged // This class is a container class for History class use. // Initialisation on the process string void HardProcess::initOnProcess( string process, ParticleData* particleData) { state.init("(hard process)", particleData); translateProcessString(process); } //-------------------------------------------------------------------------- // Initialisation on the path to LHE file void HardProcess::initOnLHEF( string LHEfile, ParticleData* particleData) { state.init("(hard process)", particleData); translateLHEFString(LHEfile); } //-------------------------------------------------------------------------- // Function to access the LHE file and read relevant information. // The merging scale will be read from the +1 jet sample, called // LHEpath_1.lhe // while the hard process will be read from // LHEpath_0.lhe // Currently, only read from MadEvent- or Sherpa-generated LHE files // is automatic, else the user is asked to supply the necessary // information. void HardProcess::translateLHEFString( string LHEpath){ // Open path to LHEF and extract merging scale ifstream infile; infile.open( (char*)( LHEpath +"_0.lhe").c_str()); // Check with ME generator has been used int iLine =0; int nLinesMax = 200; string lineGenerator; while( iLine < nLinesMax && lineGenerator.find("SHERPA", 0) == string::npos && lineGenerator.find("POWHEG-BOX", 0) == string::npos && lineGenerator.find("Pythia8", 0) == string::npos && lineGenerator.find("MadGraph", 0) == string::npos){ iLine++; lineGenerator = " "; getline(infile,lineGenerator); } infile.close(); vector incom; vector inter; vector outgo; // Particle identifiers, ordered in such a way that e.g. the "u" // in a mu is not mistaken for an u quark int inParticleNumbers[] = { // Leptons -11,11,-12,12,-13,13,-14,14,-15,15,-16,16, // Jet container 2212,2212,0,0,0,0, // Quarks -1,1,-2,2,-3,3,-4,4,-5,5,-6,6}; string inParticleNamesSH[] = { // Leptons "-11","11","-12","12","-13","13","-14","14","-15","15","-16","16", // Jet container "-93","93","-90","90","-91","91", // Quarks "-1","1","-2","2","-3","3","-4","4","-5","5","-6","6"}; string inParticleNamesMG[] = { // Leptons "e+","e-","ve~","ve","mu+","mu-","vm~","vm","ta+","ta-","vt~","vt", // Jet container "p~","p","l+","l-","vl~","vl", // Quarks "d~","d","u~","u","s~","s","c~","c","b~","b","t~","t"}; // Declare intermediate particle identifiers int interParticleNumbers[] = { // Electroweak gauge bosons 22,23,-24,24,25,2400, // Top quarks -6,6, // Dummy index as back-up 0, // All squarks -1000001,1000001,-1000002,1000002,-1000003,1000003,-1000004,1000004, -1000005,1000005,-1000006,1000006,-2000001,2000001,-2000002,2000002, -2000003,2000003,-2000004,2000004,-2000005,2000005,-2000006,2000006}; // Declare names of intermediate particles string interParticleNamesMG[] = { // Electroweak gauge bosons "a","z","w-","w+","h","W", // Top quarks "t~","t", // Dummy index as back-up "xx", // All squarks "dl~","dl","ul~","ul","sl~","sl","cl~","cl","b1~","b1","t1~","t1", "dr~","dr","ur~","ur","sr~","sr","cr~","cr","b2~","b2","t2~","t2"}; // Declare final state particle identifiers int outParticleNumbers[] = { // Leptons -11,11,-12,12,-13,13,-14,14,-15,15,-16,16, // Jet container and lepton containers 2212,2212,0,0,0,0,1200,1100,5000, // Quarks -1,1,-2,2,-3,3,-4,4,-5,5,-6,6, // SM uncoloured bosons 22,23,-24,24,25,2400, // Neutralino in SUSY 1000022, // All squarks -1000001,1000001,-1000002,1000002,-1000003,1000003,-1000004,1000004, -1000005,1000005,-1000006,1000006,-2000001,2000001,-2000002,2000002, -2000003,2000003,-2000004,2000004,-2000005,2000005,-2000006,2000006}; // Declare names of final state particles string outParticleNamesMG[] = { // Leptons "e+","e-","ve~","ve","mu+","mu-","vm~","vm","ta+","ta-","vt~","vt", // Jet container and lepton containers "j~","j","l+","l-","vl~","vl","NEUTRINOS","LEPTONS","BQUARKS", // Quarks "d~","d","u~","u","s~","s","c~","c","b~","b","t~","t", // SM uncoloured bosons "a","z","w-","w+","h","W", // Neutralino in SUSY "n1", // All squarks "dl~","dl","ul~","ul","sl~","sl","cl~","cl","b1~","b1","t1~","t1", "dr~","dr","ur~","ur","sr~","sr","cr~","cr","b2~","b2","t2~","t2"}; string outParticleNamesSH[] = { // Leptons "-11","11","-12","12","-13","13","-14","14","-15","15","-16","16", // Jet container and lepton containers "-93","93","-90","90","-91","91","0","0","0", // Quarks "-1","1","-2","2","-3","3","-4","4","-5","5","-6","6", // SM uncoloured bosons "22","23","-24","24","25","0", // Neutralino in SUSY "1000022", // All squarks "-1000001","1000001","-1000002","1000002","-1000003","1000003", "-1000004","1000004", "-1000005","1000005","-1000006","1000006","-2000001","2000001", "-2000002","2000002", "-2000003","2000003","-2000004","2000004","-2000005","2000005", "-2000006","2000006"}; // Declare size of particle name arrays int nIn = 30; int nInt = 33; int nOut = 64; // Save type of the generator, in order to be able to extract // the tms definition int meGenType = (lineGenerator.find("MadGraph", 0) != string::npos) ? -1 : (lineGenerator.find("SHERPA", 0) != string::npos) ? -2 : (lineGenerator.find("POWHEG-BOX", 0) != string::npos) ? -3 : (lineGenerator.find("Pythia8", 0) != string::npos) ? -4 : 0; if (meGenType == -2){ // Now read merging scale // Open path to LHEF and extract merging scale infile.open( (char*)( LHEpath +"_1.lhe").c_str()); string lineTMS; while(lineTMS.find("NJetFinder ", 0) == string::npos){ lineTMS = " "; getline(infile,lineTMS); } infile.close(); lineTMS = lineTMS.substr(0,lineTMS.find(" 0.0 ",0)); lineTMS = lineTMS.substr(lineTMS.find(" ", 0)+3,lineTMS.size()); // Remove whitespaces while(lineTMS.find(" ", 0) != string::npos) lineTMS.erase(lineTMS.begin()+lineTMS.find(" ",0)); // Replace d with e if ( lineTMS.find("d", 0) != string::npos) lineTMS.replace(lineTMS.find("d", 0),1,1,'e'); tms = atof((char*)lineTMS.c_str()); // Now read hard process // Open path to LHEF and extract hard process infile.open( (char*)( LHEpath +"_0.lhe").c_str()); string line; while(line.find("Process", 0) == string::npos){ line = " "; getline(infile,line); } infile.close(); line = line.substr(line.find(" ",0),line.size()); // Cut string into incoming and outgoing pieces vector pieces; pieces.push_back( line.substr(0,line.find("->", 0)) ); // Do not count additional final jets int end = (line.find("{", 0) != string::npos) ? line.find("{", 0)-2 : line.size(); pieces.push_back( line.substr(line.find("->", 0)+2, end) ); // Get incoming particles for(int i=0; i < nIn; ++i) { for(int n = pieces[0].find(inParticleNamesSH[i], 0); n != int(string::npos); n = pieces[0].find(inParticleNamesSH[i], n)) { incom.push_back(inParticleNumbers[i]); pieces[0].erase(pieces[0].begin()+n, pieces[0].begin()+n+inParticleNamesSH[i].size()); n=0; } } // Get intermediate particles // If intermediates are still empty, fill intermediate with default value inter.push_back(0); // Get final particles for(int i=0; i < nOut; ++i) { for(int n = pieces[1].find(outParticleNamesSH[i], 0); n != int(string::npos); n = pieces[1].find(outParticleNamesSH[i], n)) { outgo.push_back(outParticleNumbers[i]); pieces[1].erase(pieces[1].begin()+n, pieces[1].begin()+n+outParticleNamesSH[i].size()); n=0; } } } else if (meGenType == -1 || meGenType == -3 || meGenType == -4){ // Now read merging scale string lineTMS; if (meGenType == -1) { // Open path to LHEF and extract merging scale infile.open( (char*)( LHEpath +"_1.lhe").c_str()); while(lineTMS.find("ktdurham", 0) == string::npos){ lineTMS = " "; getline(infile,lineTMS); } lineTMS = lineTMS.substr(0,lineTMS.find("=",0)); infile.close(); } else { lineTMS = "30."; } // Remove whitespaces while(lineTMS.find(" ", 0) != string::npos) lineTMS.erase(lineTMS.begin()+lineTMS.find(" ",0)); // Replace d with e if ( lineTMS.find("d", 0) != string::npos) lineTMS.replace(lineTMS.find("d", 0),1,1,'e'); tms = atof((char*)lineTMS.c_str()); // Now read hard process // Open path to LHEF and extract hard process infile.open( (char*)( LHEpath +"_0.lhe").c_str()); string line; while(line.find("@1", 0) == string::npos){ line = " "; getline(infile,line); } infile.close(); line = line.substr(0,line.find("@",0)); // Count number of resonances int appearances = 0; for(int n = line.find("(", 0); n != int(string::npos); n = line.find("(", n)) { appearances++; n++; } // Cut string in incoming, resonance+decay and outgoing pieces vector pieces; for(int i =0; i < appearances;++i) { int n = line.find("(", 0); pieces.push_back(line.substr(0,n)); line = line.substr(n+1,line.size()); } // Cut last resonance from rest if (appearances > 0) { pieces.push_back( line.substr(0,line.find(")",0)) ); pieces.push_back( line.substr(line.find(")",0)+1,line.size()) ); } // If the string was not cut into pieces, i.e. no resonance was // required, cut string using '>' as delimiter if (pieces.empty() ){ appearances = 0; for(int n = line.find(">", 0); n != int(string::npos); n = line.find(">", n)) { appearances++; n++; } // Cut string in incoming and outgoing pieces for(int i =0; i < appearances;++i) { int n = line.find(">", 0); pieces.push_back(line.substr(0,n)); line = line.substr(n+1,line.size()); } if (appearances == 1) pieces.push_back(line); if (appearances > 1) { pieces.push_back( line.substr(0,line.find(">",0)) ); pieces.push_back( line.substr(line.find(">",0)+1,line.size()) ); } } // Get incoming particles for(int i=0; i < nIn; ++i) { for(int n = pieces[0].find(inParticleNamesMG[i], 0); n != int(string::npos); n = pieces[0].find(inParticleNamesMG[i], n)) { incom.push_back(inParticleNumbers[i]); pieces[0].erase(pieces[0].begin()+n, pieces[0].begin()+n+inParticleNamesMG[i].size()); n=0; } } // Check intermediate resonances and decay products for(int i =1; i < int(pieces.size()); ++i){ // Seperate strings into intermediate and outgoing, if not already done int k = pieces[i].find(">", 0); string intermediate = (pieces[i].find(">", 0) != string::npos) ? pieces[i].substr(0,k) : ""; string outgoing = (pieces[i].find(">", 0) != string::npos) ? pieces[i].substr(k+1,pieces[i].size()) : pieces[i]; // Get intermediate particles for(int j=0; j < nInt; ++j) { for(int n = intermediate.find(interParticleNamesMG[j], 0); n != int(string::npos); n = intermediate.find(interParticleNamesMG[j], n)) { inter.push_back(interParticleNumbers[j]); intermediate.erase(intermediate.begin()+n, intermediate.begin()+n+interParticleNamesMG[j].size()); n=0; } } // Get outgoing particles for(int j=0; j < nOut; ++j) { for(int n = outgoing.find(outParticleNamesMG[j], 0); n != int(string::npos); n = outgoing.find(outParticleNamesMG[j], n)) { outgo.push_back(outParticleNumbers[j]); outgoing.erase(outgoing.begin()+n, outgoing.begin()+n+outParticleNamesMG[j].size()); n=0; } } // For arbitrary or non-existing intermediate, remember zero for each // two outgoing particles, without bosons. if (inter.empty()) { // For final state bosons, bookkeep the final state boson as // intermediate as well. int nBosons = 0; for(int l=0; l < int(outgo.size()); ++l) if ( (abs(outgo[l]) > 20 && abs(outgo[l]) <= 25) || outgo[l] == 2400) nBosons++; int nZeros = (outgo.size() - nBosons)/2; for(int l=0; l < nZeros; ++l) inter.push_back(0); } // For final state bosons, bookkeep the final state boson as // intermediate as well. for(int l=0; l < int(outgo.size()); ++l) if ( (abs(outgo[l]) > 20 && abs(outgo[l]) <= 25) || outgo[l] == 2400) inter.push_back(outgo[l]); } } else { cout << "Reading of tms and hard process information from LHEF currently" << " only automated for MadEvent- or SHERPA-produced LHEF" << endl; int tempInt = 0; cout << "Use default process pp -> e+ve + jets? (0:no / 1:yes): "; cin >> tempInt; cout << endl; if (tempInt == 0){ tempInt = 0; double tempDouble = 0.0; cout << "Please specify merging scale (kT Durham, in GeV): "; cin >> tempDouble; tms = tempDouble; cout << endl; cout << "Please specify first incoming particle "; cout << "(p+/p- = 2212, e- = 11, e+ = -11): "; cin >> tempInt; incom.push_back(tempInt); tempInt = 0; cout << endl; cout << "Please specify second incoming particle "; cout << "(p+/p- = 2212, e- = 11, e+ = -11): "; cin >> tempInt; incom.push_back(tempInt); tempInt = 0; cout << endl; cout << "Please specify intermediate particle, if any "; cout << "(0 for none, else PDG code): "; cin >> tempInt; inter.push_back(tempInt); cout << endl; do { tempInt = 0; cout << "Please specify outgoing particle "; cout << "(jet=2212, else PDG code, exit with 99): "; cin >> tempInt; if (tempInt != 99) outgo.push_back(tempInt); } while(tempInt != 99); cout << endl; } else { cout << "LHE file not produced by SHERPA or MG/ME - "; cout << "Using default process and tms" << endl; incom.push_back(2212); incom.push_back(2212); inter.push_back(24); outgo.push_back(-11); outgo.push_back(12); tms = 10.; } } // Now store incoming, intermediate and outgoing // Set intermediate tags for(int i=0; i < int(inter.size()); ++i) hardIntermediate.push_back(inter[i]); // Set the incoming particle tags if (incom.size() != 2) cout << "Only two incoming particles allowed" << endl; else { hardIncoming1 = incom[0]; hardIncoming2 = incom[1]; } // Remember final state bosons int nBosons = 0; for(int i=0; i < int(outgo.size()); ++i) if ( (abs(outgo[i]) > 20 && abs(outgo[i]) <= 25) || outgo[i] == 2400) nBosons++; // Remember b-quark container int nBQuarks = 0; for(int i=0; i < int(outgo.size()); ++i) if ( outgo[i] == 5000) nBQuarks++; // Remember jet container int nJets = 0; for(int i=0; i < int(outgo.size()); ++i) if ( outgo[i] == 2212) nJets++; // Remember lepton container int nLeptons = 0; for(int i=0; i < int(outgo.size()); ++i) if ( outgo[i] == 1100) nLeptons++; // Remember lepton container int nNeutrinos = 0; for(int i=0; i < int(outgo.size()); ++i) if ( outgo[i] == 1200) nNeutrinos++; int nContainers = nLeptons + nNeutrinos + nJets + nBQuarks; // Set final particle identifiers if ( (outgo.size() - nBosons - nContainers)%2 == 1) { cout << "Only even number of outgoing particles allowed" << endl; for(int i=0; i < int(outgo.size()); ++i) cout << outgo[i] << endl; } else { // Push back particles / antiparticles for(int i=0; i < int(outgo.size()); ++i) if (outgo[i] > 0 && outgo[i] != 2212 && outgo[i] != 5000 && outgo[i] != 1100 && outgo[i] != 1200 && outgo[i] != 2400 && outgo[i] != 1000022) hardOutgoing2.push_back( outgo[i]); else if (outgo[i] < 0) hardOutgoing1.push_back( outgo[i]); // Save final state W-boson container as particle for(int i=0; i < int(outgo.size()); ++i) if ( outgo[i] == 2400) hardOutgoing2.push_back( outgo[i]); // Push back jets, distribute evenly amongst particles / antiparticles // Push back majorana particles, distribute evenly int iNow = 0; for(int i=0; i < int(outgo.size()); ++i) if ( (outgo[i] == 2212 || outgo[i] == 5000 || outgo[i] == 1200 || outgo[i] == 1000022) && iNow%2 == 0 ){ hardOutgoing2.push_back( outgo[i]); iNow++; } else if ( (outgo[i] == 2212 || outgo[i] == 5000 || outgo[i] == 1100 || outgo[i] == 1000022) && iNow%2 == 1 ){ hardOutgoing1.push_back( outgo[i]); iNow++; } } // Done } //-------------------------------------------------------------------------- // Function to translate a string specitying the core process into the // internal notation // Currently, the input string has to be in MadEvent notation void HardProcess::translateProcessString( string process){ vector incom; vector inter; vector outgo; // Particle identifiers, ordered in such a way that e.g. the "u" // in a mu is not mistaken for an u quark int inParticleNumbers[] = { // Leptons -11,11,-12,12,-13,13,-14,14,-15,15,-16,16, // Jet container 2212,2212,0,0,0,0, // Quarks -1,1,-2,2,-3,3,-4,4,-5,5,-6,6}; string inParticleNamesMG[] = { // Leptons "e+","e-","ve~","ve","mu+","mu-","vm~","vm","ta+","ta-","vt~","vt", // Jet container "p~","p","l+","l-","vl~","vl", // Quarks "d~","d","u~","u","s~","s","c~","c","b~","b","t~","t"}; // Declare intermediate particle identifiers int interParticleNumbers[] = { // Electroweak gauge bosons 22,23,-24,24,25,2400, // Top quarks -6,6, // Dummy index as back-up 0, // All squarks -1000001,1000001,-1000002,1000002,-1000003,1000003,-1000004,1000004, -1000005,1000005,-1000006,1000006,-2000001,2000001,-2000002,2000002, -2000003,2000003,-2000004,2000004,-2000005,2000005,-2000006,2000006}; // Declare names of intermediate particles string interParticleNamesMG[] = { // Electroweak gauge bosons "a","z","w-","w+","h","W", // Top quarks "t~","t", // Dummy index as back-up "xx", // All squarks "dl~","dl","ul~","ul","sl~","sl","cl~","cl","b1~","b1","t1~","t1", "dr~","dr","ur~","ur","sr~","sr","cr~","cr","b2~","b2","t2~","t2"}; // Declare final state particle identifiers int outParticleNumbers[] = { // Leptons -11,11,-12,12,-13,13,-14,14,-15,15,-16,16, // Jet container and lepton containers 2212,2212,0,0,0,0,1200,1100,5000, // Quarks -1,1,-2,2,-3,3,-4,4,-5,5,-6,6, // SM uncoloured bosons 22,23,-24,24,25,2400, // Neutralino in SUSY 1000022, // All squarks -1000001,1000001,-1000002,1000002,-1000003,1000003,-1000004,1000004, -1000005,1000005,-1000006,1000006,-2000001,2000001,-2000002,2000002, -2000003,2000003,-2000004,2000004,-2000005,2000005,-2000006,2000006}; // Declare names of final state particles string outParticleNamesMG[] = { // Leptons "e+","e-","ve~","ve","mu+","mu-","vm~","vm","ta+","ta-","vt~","vt", // Jet container and lepton containers "j~","j","l+","l-","vl~","vl","NEUTRINOS","LEPTONS","BQUARKS", // Quarks "d~","d","u~","u","s~","s","c~","c","b~","b","t~","t", // SM uncoloured bosons "a","z","w-","w+","h","W", // Neutralino in SUSY "n1", // All squarks "dl~","dl","ul~","ul","sl~","sl","cl~","cl","b1~","b1","t1~","t1", "dr~","dr","ur~","ur","sr~","sr","cr~","cr","b2~","b2","t2~","t2"}; // Declare size of particle name arrays int nIn = 30; int nInt = 33; int nOut = 64; // Start mapping user-defined particles onto particle ids. //string fullProc = "pp>{blaa,124}LEPTONS,NEUTRINOS"; string fullProc = process; // Find user-defined hard process content // Count number of user particles int nUserParticles = 0; for(int n = fullProc.find("{", 0); n != int(string::npos); n = fullProc.find("{", n)) { nUserParticles++; n++; } // Cut user-defined particles from remaining process vector userParticleStrings; for(int i =0; i < nUserParticles;++i) { int n = fullProc.find("{", 0); userParticleStrings.push_back(fullProc.substr(0,n)); fullProc = fullProc.substr(n+1,fullProc.size()); } // Cut remaining process string from rest if (nUserParticles > 0) userParticleStrings.push_back( fullProc.substr( 0, fullProc.find("}",0) ) ); // Remove curly brackets and whitespace for(int i =0; i < int(userParticleStrings.size());++i) { while(userParticleStrings[i].find("{", 0) != string::npos) userParticleStrings[i].erase(userParticleStrings[i].begin() +userParticleStrings[i].find("{", 0)); while(userParticleStrings[i].find("}", 0) != string::npos) userParticleStrings[i].erase(userParticleStrings[i].begin() +userParticleStrings[i].find("}", 0)); while(userParticleStrings[i].find(" ", 0) != string::npos) userParticleStrings[i].erase(userParticleStrings[i].begin() +userParticleStrings[i].find(" ", 0)); } // Convert particle numbers in user particle to integers vectoruserParticleNumbers; if ( int(userParticleStrings.size()) > 1) { for( int i = 1; i < int(userParticleStrings.size()); ++i) { userParticleNumbers.push_back( atoi((char*)userParticleStrings[i].substr( userParticleStrings[i].find(",",0)+1, userParticleStrings[i].size()).c_str() ) ); } } // Save remaining process string if (nUserParticles > 0) userParticleStrings.push_back( fullProc.substr( fullProc.find("}",0)+1, fullProc.size() ) ); // Remove curly brackets and whitespace for( int i = 0; i < int(userParticleStrings.size()); ++i) { while(userParticleStrings[i].find("{", 0) != string::npos) userParticleStrings[i].erase(userParticleStrings[i].begin() +userParticleStrings[i].find("{", 0)); while(userParticleStrings[i].find("}", 0) != string::npos) userParticleStrings[i].erase(userParticleStrings[i].begin() +userParticleStrings[i].find("}", 0)); while(userParticleStrings[i].find(" ", 0) != string::npos) userParticleStrings[i].erase(userParticleStrings[i].begin() +userParticleStrings[i].find(" ", 0)); } // Start mapping residual process string onto particle IDs. // Declare leftover process after user-defined particles have been converted string residualProc; if ( int(userParticleStrings.size()) > 1 ) residualProc = userParticleStrings.front() + userParticleStrings.back(); else residualProc = fullProc; // Remove comma separation while(residualProc.find(",", 0) != string::npos) residualProc.erase(residualProc.begin()+residualProc.find(",",0)); // Count number of resonances int appearances = 0; for(int n = residualProc.find("(", 0); n != int(string::npos); n = residualProc.find("(", n)) { appearances++; n++; } // Cut string in incoming, resonance+decay and outgoing pieces vector pieces; for(int i =0; i < appearances;++i) { int n = residualProc.find("(", 0); pieces.push_back(residualProc.substr(0,n)); residualProc = residualProc.substr(n+1,residualProc.size()); } // Cut last resonance from rest if (appearances > 0) { pieces.push_back( residualProc.substr(0,residualProc.find(")",0)) ); pieces.push_back( residualProc.substr( residualProc.find(")",0)+1, residualProc.size()) ); } // If the string was not cut into pieces, i.e. no resonance was // required, cut string using '>' as delimiter if (pieces.empty() ){ appearances = 0; for(int n = residualProc.find(">", 0); n != int(string::npos); n = residualProc.find(">", n)) { appearances++; n++; } // Cut string in incoming and outgoing pieces for(int i =0; i < appearances;++i) { int n = residualProc.find(">", 0); pieces.push_back(residualProc.substr(0,n)); residualProc = residualProc.substr(n+1,residualProc.size()); } if (appearances == 1) pieces.push_back(residualProc); if (appearances > 1) { pieces.push_back( residualProc.substr(0,residualProc.find(">",0)) ); pieces.push_back( residualProc.substr( residualProc.find(">",0)+1, residualProc.size()) ); } } // Get incoming particles for(int i=0; i < nIn; ++i) { for(int n = pieces[0].find(inParticleNamesMG[i], 0); n != int(string::npos); n = pieces[0].find(inParticleNamesMG[i], n)) { incom.push_back(inParticleNumbers[i]); pieces[0].erase(pieces[0].begin()+n, pieces[0].begin()+n+inParticleNamesMG[i].size()); n=0; } } // Check intermediate resonances and decay products for(int i =1; i < int(pieces.size()); ++i){ // Seperate strings into intermediate and outgoing, if not already done int k = pieces[i].find(">", 0); string intermediate = (pieces[i].find(">", 0) != string::npos) ? pieces[i].substr(0,k) : ""; string outgoing = (pieces[i].find(">", 0) != string::npos) ? pieces[i].substr(k+1,pieces[i].size()) : pieces[i]; // Get intermediate particles for(int j=0; j < nInt; ++j) { for(int n = intermediate.find(interParticleNamesMG[j], 0); n != int(string::npos); n = intermediate.find(interParticleNamesMG[j], n)) { inter.push_back(interParticleNumbers[j]); intermediate.erase(intermediate.begin()+n, intermediate.begin()+n+interParticleNamesMG[j].size()); n=0; } } // Get outgoing particles for(int j=0; j < nOut; ++j) { for(int n = outgoing.find(outParticleNamesMG[j], 0); n != int(string::npos); n = outgoing.find(outParticleNamesMG[j], n)) { outgo.push_back(outParticleNumbers[j]); outgoing.erase(outgoing.begin()+n, outgoing.begin()+n+outParticleNamesMG[j].size()); n=0; } } // For arbitrary or non-existing intermediate, remember zero for each // two outgoing particles, without bosons. if (inter.empty()) { // For final state bosons, bookkeep the final state boson as // intermediate as well. int nBosons = 0; for(int l=0; l < int(outgo.size()); ++l) if ( (abs(outgo[l]) > 20 && abs(outgo[l]) <= 25) || outgo[l] == 2400) nBosons++; int nZeros = (outgo.size() - nBosons)/2; for(int l=0; l < nZeros; ++l) inter.push_back(0); } // For final state bosons, bookkeep the final state boson as // intermediate as well. for(int l=0; l < int(outgo.size()); ++l) if ( (abs(outgo[l]) > 20 && abs(outgo[l]) <= 25) || outgo[l] == 2400) inter.push_back(outgo[l]); } // Now store incoming, intermediate and outgoing // Set intermediate tags for(int i=0; i < int(inter.size()); ++i) hardIntermediate.push_back(inter[i]); // Set the incoming particle tags if (incom.size() != 2) cout << "Only two incoming particles allowed" << endl; else { hardIncoming1 = incom[0]; hardIncoming2 = incom[1]; } // Now store final particle identifiers // Start with user-defined particles. for( int i = 0; i < int(userParticleNumbers.size()); ++i) if (userParticleNumbers[i] > 0) { hardOutgoing2.push_back( userParticleNumbers[i]); hardIntermediate.push_back(0); // For non-existing intermediate, remember zero. } else if (userParticleNumbers[i] < 0) { hardOutgoing1.push_back( userParticleNumbers[i]); // For non-existing intermediate, remember zero. hardIntermediate.push_back(0); } // Push back particles / antiparticles for(int i=0; i < int(outgo.size()); ++i) if (outgo[i] > 0 && outgo[i] != 2212 && outgo[i] != 5000 && outgo[i] != 1100 && outgo[i] != 1200 && outgo[i] != 2400 && outgo[i] != 1000022) hardOutgoing2.push_back( outgo[i]); else if (outgo[i] < 0) hardOutgoing1.push_back( outgo[i]); // Save final state W-boson container as particle for(int i=0; i < int(outgo.size()); ++i) if ( outgo[i] == 2400) hardOutgoing2.push_back( outgo[i]); // Push back jets, distribute evenly among particles / antiparticles // Push back majorana particles, distribute evenly int iNow = 0; for(int i=0; i < int(outgo.size()); ++i) if ( (outgo[i] == 2212 || outgo[i] == 5000 || outgo[i] == 1200 || outgo[i] == 1000022) && iNow%2 == 0 ){ hardOutgoing2.push_back( outgo[i]); iNow++; } else if ( (outgo[i] == 2212 || outgo[i] == 5000 || outgo[i] == 1100 || outgo[i] == 1000022) && iNow%2 == 1 ){ hardOutgoing1.push_back( outgo[i]); iNow++; } // Done } //-------------------------------------------------------------------------- // Function to check if the candidates stored in Pos1 and Pos2, together with // a proposed candidate iPos are allowed. bool HardProcess::allowCandidates(int iPos, vector Pos1, vector Pos2, const Event& event){ bool allowed = true; // Find colour-partner of new candidate int type = (event[iPos].col() > 0) ? 1 : (event[iPos].acol() > 0) ? -1 : 0; if (type == 0) return true; if (type == 1){ int col = event[iPos].col(); int iPartner = 0; for(int i=0; i < int(event.size()); ++i) if ( i != iPos && (( event[i].isFinal() && event[i].acol() == col) ||( event[i].status() == -21 && event[i].col() == col) )) iPartner = i; vector partners; for(int i=0; i < int(event.size()); ++i) for(int j=0; j < int(Pos1.size()); ++j) if ( Pos1[j] != 0 && i != Pos1[j] && event[Pos1[j]].colType() != 0 && (( event[i].isFinal() && event[i].col() == event[Pos1[j]].acol()) ||( event[i].status() == -21 && event[i].acol() == event[Pos1[j]].acol()) )) partners.push_back(i); // Never allow equal initial partners! if (event[iPartner].status() == -21){ for(int i=0; i < int(partners.size()); ++i) if ( partners[i] == iPartner) allowed = false; } } else { int col = event[iPos].acol(); int iPartner = 0; for(int i=0; i < int(event.size()); ++i) if ( i != iPos && (( event[i].isFinal() && event[i].col() == col) ||(!event[i].isFinal() && event[i].acol() == col) )) iPartner = i; vector partners; for(int i=0; i < int(event.size()); ++i) for(int j=0; j < int(Pos2.size()); ++j) if ( Pos2[j] != 0 && i != Pos2[j] && event[Pos2[j]].colType() != 0 && (( event[i].isFinal() && event[i].acol() == event[Pos2[j]].col()) ||( event[i].status() == -21 && event[i].col() == event[Pos2[j]].col()) )) partners.push_back(i); // Never allow equal initial partners! if (event[iPartner].status() == -21){ for(int i=0; i < int(partners.size()); ++i){ if ( partners[i] == iPartner) allowed = false; } } } return allowed; } //-------------------------------------------------------------------------- // Function to identify the hard subprocess in the current event void HardProcess::storeCandidates( const Event& event, string process){ // Store the reference event state.clear(); state = event; // Local copy of intermediate bosons vector intermediates; for(int i =0; i < int(hardIntermediate.size());++i) intermediates.push_back( hardIntermediate[i]); // Local copy of outpoing partons vector outgoing1; for(int i =0; i < int(hardOutgoing1.size());++i) outgoing1.push_back( hardOutgoing1[i]); vector outgoing2; for(int i =0; i < int(hardOutgoing2.size());++i) outgoing2.push_back( hardOutgoing2[i]); // Clear positions of intermediate and outgoing particles PosIntermediate.resize(0); PosOutgoing1.resize(0); PosOutgoing2.resize(0); for(int i =0; i < int(hardIntermediate.size());++i) PosIntermediate.push_back(0); for(int i =0; i < int(hardOutgoing1.size());++i) PosOutgoing1.push_back(0); for(int i =0; i < int(hardOutgoing2.size());++i) PosOutgoing2.push_back(0); // For QCD dijet or e+e- > jets hard process, do not store any candidates, // as to not discrimintate clusterings if ( process.compare("pp>jj") == 0 || process.compare("e+e->jj") == 0 || process.compare("e+e->(z>jj)") == 0 ){ for(int i =0; i < int(hardOutgoing1.size());++i) PosOutgoing1[i] = 0; for(int i =0; i < int(hardOutgoing2.size());++i) PosOutgoing2[i] = 0; // Done return; } // Initialise vector of particles that were already identified as // hard process particles vector iPosChecked; // If the hard process is specified only by containers, then add all // particles matching with the containers to the hard process. bool hasOnlyContainers = true; for(int i =0; i < int(hardOutgoing1.size());++i) if ( hardOutgoing1[i] != 1100 && hardOutgoing1[i] != 1200 && hardOutgoing1[i] != 5000) hasOnlyContainers = false; for(int i =0; i < int(hardOutgoing2.size());++i) if ( hardOutgoing2[i] != 1100 && hardOutgoing2[i] != 1200 && hardOutgoing2[i] != 5000) hasOnlyContainers = false; if (hasOnlyContainers){ PosOutgoing1.resize(0); PosOutgoing2.resize(0); // Try to find all unmatched hard process leptons. // Loop through event to find outgoing lepton for(int i=0; i < int(event.size()); ++i){ // Skip non-final particles if ( !event[i].isFinal() ) continue; // Skip all particles that have already been identified bool skip = false; for(int k=0; k < int(iPosChecked.size()); ++k){ if (i == iPosChecked[k]) skip = true; } if (skip) continue; for(int j=0; j < int(outgoing2.size()); ++j){ // If the particle matches an outgoing neutrino, save it if ( outgoing2[j] == 1100 && ( event[i].idAbs() == 11 || event[i].idAbs() == 13 || event[i].idAbs() == 15) ){ PosOutgoing2.push_back(i); iPosChecked.push_back(i); } // If the particle matches an outgoing lepton, save it if ( outgoing2[j] == 1200 && ( event[i].idAbs() == 12 || event[i].idAbs() == 14 || event[i].idAbs() == 16) ){ PosOutgoing2.push_back(i); iPosChecked.push_back(i); } // If the particle matches an outgoing b-quark, save it if ( outgoing2[j] == 5000 && event[i].idAbs() == 5 ){ PosOutgoing2.push_back(i); iPosChecked.push_back(i); } } // Skip all particles that have already been identified skip = false; for(int k=0; k < int(iPosChecked.size()); ++k){ if (i == iPosChecked[k]) skip = true; } if (skip) continue; for(int j=0; j < int(outgoing1.size()); ++j){ // If the particle matches an outgoing neutrino, save it if ( outgoing1[j] == 1100 && ( event[i].idAbs() == 11 || event[i].idAbs() == 13 || event[i].idAbs() == 15) ){ PosOutgoing1.push_back(i); iPosChecked.push_back(i); } // If the particle matches an outgoing lepton, save it if ( outgoing1[j] == 1200 && ( event[i].idAbs() == 12 || event[i].idAbs() == 14 || event[i].idAbs() == 16) ){ PosOutgoing1.push_back(i); iPosChecked.push_back(i); } // If the particle matches an outgoing b-quark, save it if ( outgoing1[j] == 5000 && event[i].idAbs() == 5 ){ PosOutgoing1.push_back(i); iPosChecked.push_back(i); } } } // Done return; } // Now begin finding candidates when not only containers are used. // First try to find final state bosons for(int i=0; i < int(intermediates.size()); ++i){ // Do nothing if the intermediate boson is absent if (intermediates[i] == 0) continue; // Do nothing if this boson does not match any final state boson bool matchesFinalBoson = false; for(int j =0; j< int(outgoing1.size()); ++j){ if ( intermediates[i] == outgoing1[j] ) matchesFinalBoson = true; } for(int j =0; j< int(outgoing2.size()); ++j){ if ( intermediates[i] == outgoing2[j] ) matchesFinalBoson = true; } if (!matchesFinalBoson) continue; // Loop through event for(int j=0; j < int(event.size()); ++j) { // Skip all particles that have already been identified bool skip = false; for(int m=0; m < int(iPosChecked.size()); ++m) if (j == iPosChecked[m]) skip = true; if (skip) continue; // If the particle has a requested intermediate id, check if // if is a final state boson if ( (event[j].id() == intermediates[i]) ||(event[j].idAbs() == 24 && intermediates[i] == 2400) ) { PosIntermediate[i] = j; intermediates[i] = 0; // Be careful only to replace one index at a time! bool indexSet = false; for(int k=0; k < int(outgoing1.size()); ++k) { if (event[j].id() == outgoing1[k] && !indexSet){ PosOutgoing1[k] = j; outgoing1[k] = 99; indexSet = true; } } for(int k=0; k < int(outgoing2.size()); ++k) { if (event[j].id() == outgoing2[k] && !indexSet){ PosOutgoing2[k] = j; outgoing2[k] = 99; indexSet = true; } } // Check for W-boson container for(int k=0; k < int(outgoing2.size()); ++k) { if (event[j].idAbs() == 24 && outgoing2[k] == 2400 && !indexSet ){ PosOutgoing2[k] = j; outgoing2[k] = 99; indexSet = true; } } iPosChecked.push_back(j); } } } // Second try to find particles coupled to intermediate bosons for(int i=0; i < int(intermediates.size()); ++i){ // Do nothing if the intermediate boson is absent if (intermediates[i] == 0) continue; // Loop through event for(int j=0; j < int(event.size()); ++j) { // If the particle has a requested intermediate id, check if // daughters are hard process particles if ( (event[j].id() == intermediates[i]) ||(event[j].idAbs() == 24 && intermediates[i] == 2400) ) { // If this particle is a potential intermediate PosIntermediate[i] = j; intermediates[i] = 0; // If id's of daughters are good, store position int iPos1 = event[j].daughter1(); int iPos2 = event[j].daughter2(); // Loop through daughters to check if these contain some hard // outgoing particles for( int k=iPos1; k <= iPos2; ++k){ int id = event[k].id(); // Skip all particles that have already been identified bool skip = false; for(int m=0; m < int(iPosChecked.size()); ++m) if (k == iPosChecked[m]) skip = true; if (skip) continue; // Check if daughter is hard outgoing particle for(int l=0; l < int(outgoing2.size()); ++l) if ( outgoing2[l] != 99 ){ // Found particle id if (id == outgoing2[l] // Found jet || (id > 0 && abs(id) < 10 && outgoing2[l] == 2212) ){ // Store position PosOutgoing2[l] = k; // Remove the matched particle from the list outgoing2[l] = 99; iPosChecked.push_back(k); break; } } // Check if daughter is hard outgoing antiparticle for(int l=0; l < int(outgoing1.size()); ++l) if ( outgoing1[l] != 99 ){ // Found particle id if (id == outgoing1[l] // Found jet || (id < 0 && abs(id) < 10 && outgoing1[l] == 2212) ){ // Store position PosOutgoing1[l] = k; // Remove the matched particle from the list outgoing1[l] = 99; iPosChecked.push_back(k); break; } } } // End loop through daughters } // End if ids match } // End loop through event } // End loop though requested intermediates // If all outgoing particles were found, done bool done = true; for(int i=0; i < int(outgoing1.size()); ++i) if (outgoing1[i] != 99) done = false; for(int i=0; i < int(outgoing2.size()); ++i) if (outgoing2[i] != 99) done = false; // Return if (done) return; // Leptons not associated with resonance are allowed. // Try to find all unmatched hard process leptons. // Loop through event to find outgoing lepton for(int i=0; i < int(event.size()); ++i){ // Skip non-final particles and final partons if ( !event[i].isFinal() || event[i].colType() != 0) continue; // Skip all particles that have already been identified bool skip = false; for(int k=0; k < int(iPosChecked.size()); ++k){ if (i == iPosChecked[k]) skip = true; } if (skip) continue; // Check if any hard outgoing leptons remain for(int j=0; j < int(outgoing2.size()); ++j){ // Do nothing if this particle has already be found, // or if this particle is a jet or quark if ( outgoing2[j] == 99 || outgoing2[j] == 2212 || abs(outgoing2[j]) < 10) continue; // If the particle matches an outgoing lepton, save it if ( event[i].id() == outgoing2[j] ){ PosOutgoing2[j] = i; outgoing2[j] = 99; iPosChecked.push_back(i); } } // Check if any hard outgoing antileptons remain for(int j=0; j < int(outgoing1.size()); ++j){ // Do nothing if this particle has already be found, // or if this particle is a jet or quark if ( outgoing1[j] == 99 || outgoing1[j] == 2212 || abs(outgoing1[j]) < 10) continue; // If the particle matches an outgoing lepton, save it if (event[i].id() == outgoing1[j] ){ PosOutgoing1[j] = i; outgoing1[j] = 99; iPosChecked.push_back(i); } } } multimap out2copy; for(int i=0; i < int(event.size()); ++i) for(int j=0; j < int(outgoing2.size()); ++j) // Do nothing if this particle has already be found, // or if this particle is a jet. if ( outgoing2[j] != 99 && outgoing2[j] != 2212 && ( abs(outgoing2[j]) < 10 || (abs(outgoing2[j]) > 1000000 && abs(outgoing2[j]) < 1000010) || (abs(outgoing2[j]) > 2000000 && abs(outgoing2[j]) < 2000010) ) && event[i].isFinal() && event[i].id() == outgoing2[j] ){ out2copy.insert(make_pair(j, i)); } multimap out1copy; for(int i=0; i < int(event.size()); ++i) for(int j=0; j < int(outgoing1.size()); ++j) // Do nothing if this particle has already be found, // or if this particle is a jet. if ( outgoing1[j] != 99 && outgoing1[j] != 2212 && ( abs(outgoing1[j]) < 10 || (abs(outgoing1[j]) > 1000000 && abs(outgoing1[j]) < 1000010) || (abs(outgoing1[j]) > 2000000 && abs(outgoing1[j]) < 2000010) ) && event[i].isFinal() && event[i].id() == outgoing1[j] ){ out1copy.insert(make_pair(j, i)); } if ( out1copy.size() > out2copy.size()){ // In case the index of the multimap is filled twice, make sure not to // arbitrarily overwrite set values. vector indexWasSet; for ( multimap::iterator it = out2copy.begin(); it != out2copy.end(); ++it ) { if ( allowCandidates(it->second, PosOutgoing1, PosOutgoing2, event) ){ // Skip all particles that have already been identified bool skip = false; for(int k=0; k < int(iPosChecked.size()); ++k) if (it->second == iPosChecked[k]) skip = true; // Skip all indices that have already been identified for(int k=0; k < int(indexWasSet.size()); ++k) if (it->first == indexWasSet[k]) skip = true; if (skip) continue; // Save parton PosOutgoing2[it->first] = it->second; // remove entry form lists outgoing2[it->first] = 99; iPosChecked.push_back(it->second); indexWasSet.push_back(it->first); } } indexWasSet.resize(0); for ( multimap::iterator it = out1copy.begin(); it != out1copy.end(); ++it ) { if ( allowCandidates(it->second, PosOutgoing1, PosOutgoing2, event) ){ // Skip all particles that have already been identified bool skip = false; for(int k=0; k < int(iPosChecked.size()); ++k) if (it->second == iPosChecked[k]) skip = true; // Skip all indices that have already been identified for(int k=0; k < int(indexWasSet.size()); ++k) if (it->first == indexWasSet[k]) skip = true; if (skip) continue; // Save parton PosOutgoing1[it->first] = it->second; // remove entry form lists outgoing1[it->first] = 99; iPosChecked.push_back(it->second); indexWasSet.push_back(it->first); } } } else { // In case the index of the multimap is filled twice, make sure not to // arbitraryly overwrite set values. vector indexWasSet; for ( multimap::iterator it = out1copy.begin(); it != out1copy.end(); ++it ) { if ( allowCandidates(it->second, PosOutgoing1, PosOutgoing2, event) ){ // Skip all particles that have already been identified bool skip = false; for(int k=0; k < int(iPosChecked.size()); ++k) if (it->second == iPosChecked[k]) skip = true; // Skip all indices that have already been identified for(int k=0; k < int(indexWasSet.size()); ++k) if (it->first == indexWasSet[k]) skip = true; if (skip) continue; // Save parton PosOutgoing1[it->first] = it->second; // remove entry form lists outgoing1[it->first] = 99; iPosChecked.push_back(it->second); indexWasSet.push_back(it->first); } } indexWasSet.resize(0); for ( multimap::iterator it = out2copy.begin(); it != out2copy.end(); ++it ) { if ( allowCandidates(it->second, PosOutgoing1, PosOutgoing2, event) ){ // Skip all particles that have already been identified bool skip = false; for(int k=0; k < int(iPosChecked.size()); ++k) if (it->second == iPosChecked[k]) skip = true; // Skip all indices that have already been identified for(int k=0; k < int(indexWasSet.size()); ++k) if (it->first == indexWasSet[k]) skip = true; if (skip) continue; // Save parton PosOutgoing2[it->first] = it->second; // remove entry form lists outgoing2[it->first] = 99; iPosChecked.push_back(it->second); indexWasSet.push_back(it->first); } } } // It sometimes happens that MadEvent does not put a // heavy coloured resonance into the LHE file, even if requested. // This means that the decay products of this resonance need to be // found separately. // Loop through event to find hard process (anti)quarks for(int i=0; i < int(event.size()); ++i){ // Skip non-final particles and final partons if ( !event[i].isFinal() || event[i].colType() == 0) continue; // Skip all particles that have already been identified bool skip = false; for(int k=0; k < int(iPosChecked.size()); ++k){ if (i == iPosChecked[k]) skip = true; } if (skip) continue; // Check if any hard outgoing quarks remain for(int j=0; j < int(outgoing2.size()); ++j){ // Do nothing if this particle has already be found, // or if this particle is a jet, lepton container or lepton if ( outgoing2[j] == 99 || outgoing2[j] == 2212 || abs(outgoing2[j]) > 10) continue; // If the particle matches an outgoing quark, save it if (event[i].id() == outgoing2[j]){ // Save parton PosOutgoing2[j] = i; // remove entry form lists outgoing2[j] = 99; iPosChecked.push_back(i); } } // Check if any hard outgoing antiquarks remain for(int j=0; j < int(outgoing1.size()); ++j){ // Do nothing if this particle has already be found, // or if this particle is a jet, lepton container or lepton if ( outgoing1[j] == 99 || outgoing1[j] == 2212 || abs(outgoing1[j]) > 10) continue; // If the particle matches an outgoing antiquark, save it if (event[i].id() == outgoing1[j]){ // Save parton PosOutgoing1[j] = i; // Remove parton from list outgoing1[j] = 99; iPosChecked.push_back(i); } } } // Done } //-------------------------------------------------------------------------- // Function to check if the particle event[iPos] matches any of // the stored outgoing particles of the hard subprocess bool HardProcess::matchesAnyOutgoing(int iPos, const Event& event){ // Match quantum numbers of any first outgoing candidate bool matchQN1 = false; // Match quantum numbers of any second outgoing candidate bool matchQN2 = false; // Match parton in the hard process, // or parton from decay of electroweak boson in hard process, // or parton from decay of electroweak boson from decay of top bool matchHP = false; // Check outgoing candidates for(int i=0; i < int(PosOutgoing1.size()); ++i) // Compare particle properties if ( event[iPos].id() == state[PosOutgoing1[i]].id() && event[iPos].colType() == state[PosOutgoing1[i]].colType() && event[iPos].chargeType() == state[PosOutgoing1[i]].chargeType() && event[iPos].col() == state[PosOutgoing1[i]].col() && event[iPos].acol() == state[PosOutgoing1[i]].acol() && event[iPos].charge() == state[PosOutgoing1[i]].charge() ) matchQN1 = true; // Check outgoing candidates for(int i=0; i < int(PosOutgoing2.size()); ++i) // Compare particle properties if ( event[iPos].id() == state[PosOutgoing2[i]].id() && event[iPos].colType() == state[PosOutgoing2[i]].colType() && event[iPos].chargeType() == state[PosOutgoing2[i]].chargeType() && event[iPos].col() == state[PosOutgoing2[i]].col() && event[iPos].acol() == state[PosOutgoing2[i]].acol() && event[iPos].charge() == state[PosOutgoing2[i]].charge() ) matchQN2 = true; // Check if maps to hard process: // Check that particle is in hard process if ( event[iPos].mother1()*event[iPos].mother2() == 12 // Or particle has taken recoil from first splitting || ( event[iPos].status() == 44 && event[event[iPos].mother1()].mother1() *event[event[iPos].mother1()].mother2() == 12 ) // Or particle has on-shell resonace as mother || ( event[iPos].status() == 23 && event[event[iPos].mother1()].mother1() *event[event[iPos].mother1()].mother2() == 12 ) // Or particle has on-shell resonace as mother, // which again has and on-shell resonance as mother || ( event[iPos].status() == 23 && event[event[iPos].mother1()].status() == -22 && event[event[event[iPos].mother1()].mother1()].status() == -22 && event[event[event[iPos].mother1()].mother1()].mother1() *event[event[event[iPos].mother1()].mother1()].mother2() == 12 ) ) matchHP = true; // Done return ( matchHP && (matchQN1 || matchQN2) ); } //-------------------------------------------------------------------------- // Function to check if instead of the particle event[iCandidate], another // particle could serve as part of the hard process. Assumes that iCandidate // is already stored as part of the hard process. bool HardProcess::findOtherCandidates(int iPos, const Event& event, bool doReplace){ // Return value bool foundCopy = false; // Save stored candidates' properties. int id = event[iPos].id(); int col = event[iPos].col(); int acl = event[iPos].acol(); // Find candidate amongst the already stored ME process candidates. vector candidates1; vector candidates2; // Check outgoing candidates for(int i=0; i < int(PosOutgoing1.size()); ++i) // Compare particle properties if ( id == state[PosOutgoing1[i]].id() && col == state[PosOutgoing1[i]].col() && acl == state[PosOutgoing1[i]].acol() ) candidates1.push_back(i); // Check outgoing candidates for(int i=0; i < int(PosOutgoing2.size()); ++i) // Compare particle properties if ( id == state[PosOutgoing2[i]].id() && col == state[PosOutgoing2[i]].col() && acl == state[PosOutgoing2[i]].acol() ) candidates2.push_back(i); // If more / less than one stored candidate for iPos has been found, exit. if ( candidates1.size() + candidates2.size() != 1 ) return false; // Now check for other allowed candidates. map further1; for(int i=0; i < int(state.size()); ++i) for(int j=0; j < int(PosOutgoing1.size()); ++j) // Do nothing if this particle has already be found, // or if this particle is a jet, lepton container or lepton if ( state[i].isFinal() && i != PosOutgoing1[j] && state[PosOutgoing1[j]].id() == id && state[i].id() == id ){ // Declare vector of already existing candiates. vector newPosOutgoing1; for(int k=0; k < int(PosOutgoing1.size()); ++k) if ( k != j ) newPosOutgoing1.push_back( PosOutgoing1[k] ); // If allowed, remember replacment parton. if ( allowCandidates(i, newPosOutgoing1, PosOutgoing2, state) ) further1.insert(make_pair(j, i)); } // Now check for other allowed candidates. map further2; for(int i=0; i < int(state.size()); ++i) for(int j=0; j < int(PosOutgoing2.size()); ++j) // Do nothing if this particle has already be found, // or if this particle is a jet, lepton container or lepton if ( state[i].isFinal() && i != PosOutgoing2[j] && state[PosOutgoing2[j]].id() == id && state[i].id() == id ){ // Declare vector of already existing candidates. vector newPosOutgoing2; for(int k=0; k < int(PosOutgoing2.size()); ++k) if ( k != j ) newPosOutgoing2.push_back( PosOutgoing2[k] ); // If allowed, remember replacment parton. if ( allowCandidates(i, PosOutgoing1, newPosOutgoing2, state) ) further2.insert(make_pair(j, i)); } // Decide of a replacment candidate has been found. foundCopy = (doReplace) ? exchangeCandidates(candidates1, candidates2, further1, further2) : (further1.size() + further2.size() > 0); // Done return foundCopy; } //-------------------------------------------------------------------------- // Function to exchange hard process candidates. bool HardProcess::exchangeCandidates( vector candidates1, vector candidates2, map further1, map further2) { int nOld1 = candidates1.size(); int nOld2 = candidates2.size(); int nNew1 = further1.size(); int nNew2 = further2.size(); bool exchanged = false; // Replace, if one-to-one correspondence exists. if ( nOld1 == 1 && nOld2 == 0 && nNew1 == 1 && nNew2 == 0){ PosOutgoing1[further1.begin()->first] = further1.begin()->second; exchanged = true; } else if ( nOld1 == 0 && nOld2 == 1 && nNew1 == 0 && nNew2 == 1){ PosOutgoing2[further2.begin()->first] = further2.begin()->second; exchanged = true; // Else simply swap with the first candidate. } else if ( nNew1 > 1 && nNew2 == 0 ) { PosOutgoing1[further1.begin()->first] = further1.begin()->second; exchanged = true; } else if ( nNew1 == 0 && nNew2 > 0 ) { PosOutgoing2[further2.begin()->first] = further2.begin()->second; exchanged = true; } // Done return exchanged; } //-------------------------------------------------------------------------- // Function to get the number of coloured final state partons in the // hard process int HardProcess::nQuarksOut(){ int nFin =0; for(int i =0; i< int(hardOutgoing1.size()); ++i){ if (hardOutgoing1[i] == 2212 || abs(hardOutgoing1[i]) < 10) nFin++; } for(int i =0; i< int(hardOutgoing2.size()); ++i){ if (hardOutgoing2[i] == 2212 || abs(hardOutgoing2[i]) < 10) nFin++; } // For very loose hard process definition, check number of hard process // b-quarks explicitly. for(int i =0; i< int(hardOutgoing1.size()); ++i) if (hardOutgoing1[i] == 5000) for(int j =0; j< int(PosOutgoing1.size()); ++j) if (state[PosOutgoing1[j]].idAbs() == 5) nFin++; for(int i =0; i< int(hardOutgoing2.size()); ++i) if (hardOutgoing2[i] == 5000) for(int j =0; j< int(PosOutgoing2.size()); ++j) if (state[PosOutgoing2[j]].idAbs() == 5) nFin++; return nFin; } //-------------------------------------------------------------------------- // Function to get the number of uncoloured final state particles in the // hard process int HardProcess::nLeptonOut(){ int nFin =0; for(int i =0; i< int(hardOutgoing1.size()); ++i){ if (abs(hardOutgoing1[i]) > 10 && abs(hardOutgoing1[i]) < 20) nFin++; // Bookkeep MSSM neutralinos as leptons if (abs(hardOutgoing1[i]) == 1000022) nFin++; // Bookkeep sleptons as leptons if ( abs(hardOutgoing1[i]) == 1000011 || abs(hardOutgoing1[i]) == 2000011 || abs(hardOutgoing1[i]) == 1000013 || abs(hardOutgoing1[i]) == 2000013 || abs(hardOutgoing1[i]) == 1000015 || abs(hardOutgoing1[i]) == 2000015) nFin++; } for(int i =0; i< int(hardOutgoing2.size()); ++i){ if (abs(hardOutgoing2[i]) > 10 && abs(hardOutgoing2[i]) < 20) nFin++; // Bookkeep MSSM neutralinos as leptons if (abs(hardOutgoing2[i]) == 1000022) nFin++; // Bookkeep sleptons as leptons if ( abs(hardOutgoing2[i]) == 1000011 || abs(hardOutgoing2[i]) == 2000011 || abs(hardOutgoing2[i]) == 1000013 || abs(hardOutgoing2[i]) == 2000013 || abs(hardOutgoing2[i]) == 1000015 || abs(hardOutgoing2[i]) == 2000015) nFin++; } // For very loose hard process definition, check number of hard process // lepton explicitly. // Check lepton / neutrino containers as leptons for(int i =0; i< int(hardOutgoing1.size()); ++i) if (hardOutgoing1[i] == 1100) for(int j =0; j< int(PosOutgoing1.size()); ++j) if ( abs(state[PosOutgoing1[j]].id()) == 11 || abs(state[PosOutgoing1[j]].id()) == 13 || abs(state[PosOutgoing1[j]].id()) == 15 ) nFin++; for(int i =0; i< int(hardOutgoing2.size()); ++i) if (hardOutgoing2[i] == 1200) for(int j =0; j< int(PosOutgoing2.size()); ++j) if ( abs(state[PosOutgoing2[j]].id()) == 12 || abs(state[PosOutgoing2[j]].id()) == 14 || abs(state[PosOutgoing2[j]].id()) == 16 ) nFin++; return nFin; } //-------------------------------------------------------------------------- // Function to get the number of uncoloured final state particles in the // hard process int HardProcess::nBosonsOut(){ int nFin =0; for(int i =0; i< int(hardOutgoing1.size()); ++i){ if (abs(hardOutgoing1[i]) > 20 && abs(hardOutgoing1[i]) <= 25) nFin++; } for(int i =0; i< int(hardOutgoing2.size()); ++i){ if (abs(hardOutgoing2[i]) > 20 && abs(hardOutgoing2[i]) <= 25) nFin++; if ( hardOutgoing2[i] == 2400) nFin++; } return nFin; } //-------------------------------------------------------------------------- // Function to get the number of coloured initial state partons in the // hard process int HardProcess::nQuarksIn(){ int nIn =0; if (hardIncoming1 == 2212 || abs(hardIncoming1) < 10) nIn++; if (hardIncoming2 == 2212 || abs(hardIncoming2) < 10) nIn++; return nIn; } //-------------------------------------------------------------------------- // Function to get the number of uncoloured initial state particles in the // hard process int HardProcess::nLeptonIn(){ int nIn =0; if (abs(hardIncoming1) > 10 && abs(hardIncoming1) < 20) nIn++; if (abs(hardIncoming2) > 10 && abs(hardIncoming2) < 20) nIn++; return nIn; } //-------------------------------------------------------------------------- // Function to report if a resonace decay was found in the // 2->2 hard sub-process in the current state int HardProcess::hasResInCurrent(){ for(int i =0; i< int(PosIntermediate.size()); ++i) if (PosIntermediate[i] == 0) return 0; // Do not count final state bosons as resonaces for(int i =0; i< int(PosIntermediate.size()); ++i){ for(int j =0; j< int(PosOutgoing1.size()); ++j){ if ( PosIntermediate[i] == PosOutgoing1[j] ) return 0; } for(int j =0; j< int(PosOutgoing2.size()); ++j){ if ( PosIntermediate[i] == PosOutgoing2[j] ) return 0; } } return 1; } //-------------------------------------------------------------------------- // Function to report the number of resonace decays in the 2->2 sub-process // of the current state int HardProcess::nResInCurrent(){ int nRes = 0; for(int i =0; i< int(PosIntermediate.size()); ++i){ if (PosIntermediate[i] != 0) { bool matchesFinalBoson = false; for(int j =0; j< int(PosOutgoing1.size()); ++j){ if ( PosIntermediate[i] == PosOutgoing1[j] ) matchesFinalBoson = true; } for(int j =0; j< int(PosOutgoing2.size()); ++j){ if ( PosIntermediate[i] == PosOutgoing2[j] ) matchesFinalBoson = true; } if (!matchesFinalBoson) nRes++; } } return nRes; } //-------------------------------------------------------------------------- // Function to report if a resonace decay was found in the // 2->2 hard core process bool HardProcess::hasResInProc(){ for(int i =0; i< int(hardIntermediate.size()); ++i) if (hardIntermediate[i] == 0) return false; // Do not count final state bosons as resonaces for(int i =0; i< int(hardIntermediate.size()); ++i){ for(int j =0; j< int(hardOutgoing1.size()); ++j){ if ( hardIntermediate[i] == hardOutgoing1[j] ) return false; } for(int j =0; j< int(hardOutgoing2.size()); ++j){ if ( hardIntermediate[i] == hardOutgoing2[j] ) return false; } } return true; } //-------------------------------------------------------------------------- // Function to print the hard process (for debug) void HardProcess::list() const { cout << " Hard Process: "; cout << " \t " << hardIncoming1 << " + " << hardIncoming2; cout << " \t -----> \t "; for(int i =0; i < int(hardIntermediate.size());++i) cout << hardIntermediate[i] << " "; cout << " \t -----> \t "; for(int i =0; i < int(hardOutgoing1.size());++i) cout << hardOutgoing1[i] << " "; for(int i =0; i < int(hardOutgoing2.size());++i) cout << hardOutgoing2[i] << " "; cout << endl; } //-------------------------------------------------------------------------- // Function to list the hard process candiates in the matrix element state // (for debug) void HardProcess::listCandidates() const { cout << " Hard Process candidates: "; cout << " \t " << hardIncoming1 << " + " << hardIncoming2; cout << " \t -----> \t "; for(int i =0; i < int(PosIntermediate.size());++i) cout << PosIntermediate[i] << " "; cout << " \t -----> \t "; for(int i =0; i < int(PosOutgoing1.size());++i) cout << PosOutgoing1[i] << " "; for(int i =0; i < int(PosOutgoing2.size());++i) cout << PosOutgoing2[i] << " "; cout << endl; } //-------------------------------------------------------------------------- // Function to clear hard process information void HardProcess::clear() { // Clear flavour of the first incoming particle hardIncoming1 = hardIncoming2 = 0; // Clear outgoing particles hardOutgoing1.resize(0); hardOutgoing2.resize(0); // Clear intermediate bosons in the hard 2->2 hardIntermediate.resize(0); // Clear reference event state.clear(); // Clear potential positions of outgoing particles in reference event PosOutgoing1.resize(0); PosOutgoing2.resize(0); // Clear potential positions of intermediate bosons in reference event PosIntermediate.resize(0); // Clear merging scale read from LHE file tms = 0.; } //========================================================================== // The MergingHooks class. //-------------------------------------------------------------------------- // Initialise MergingHooks class void MergingHooks::init( Settings settings, Info* infoPtrIn, ParticleData* particleDataPtrIn, PartonSystems* partonSystemsPtrIn, ostream& os){ // Save pointers infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; partonSystemsPtr = partonSystemsPtrIn; // Initialise AlphaS objects for reweighting double alphaSvalueFSR = settings.parm("TimeShower:alphaSvalue"); int alphaSorderFSR = settings.mode("TimeShower:alphaSorder"); int alphaSnfmax = settings.mode("StandardModel:alphaSnfmax"); int alphaSuseCMWFSR= settings.flag("TimeShower:alphaSuseCMW"); AlphaS_FSRSave.init(alphaSvalueFSR, alphaSorderFSR, alphaSnfmax, alphaSuseCMWFSR); double alphaSvalueISR = settings.parm("SpaceShower:alphaSvalue"); int alphaSorderISR = settings.mode("SpaceShower:alphaSorder"); int alphaSuseCMWISR= settings.flag("SpaceShower:alphaSuseCMW"); AlphaS_ISRSave.init(alphaSvalueISR, alphaSorderISR, alphaSnfmax, alphaSuseCMWISR); // Initialise AlphaEM objects for reweighting int alphaEMFSRorder = settings.mode("TimeShower:alphaEMorder"); AlphaEM_FSRSave.init(alphaEMFSRorder, &settings); // Initialise merging switches doUserMergingSave = settings.flag("Merging:doUserMerging"); // Initialise automated MadGraph kT merging doMGMergingSave = settings.flag("Merging:doMGMerging"); // Initialise kT merging doKTMergingSave = settings.flag("Merging:doKTMerging"); // Initialise evolution-pT merging doPTLundMergingSave = settings.flag("Merging:doPTLundMerging"); // Initialise \Delta_R_{ij}, pT_i Q_{ij} merging doCutBasedMergingSave = settings.flag("Merging:doCutBasedMerging"); // Initialise exact definition of kT ktTypeSave = settings.mode("Merging:ktType"); // Initialise NL3 switches. doNL3TreeSave = settings.flag("Merging:doNL3Tree"); doNL3LoopSave = settings.flag("Merging:doNL3Loop"); doNL3SubtSave = settings.flag("Merging:doNL3Subt"); bool doNL3 = doNL3TreeSave || doNL3LoopSave || doNL3SubtSave; // Initialise UNLOPS switches. doUNLOPSTreeSave = settings.flag("Merging:doUNLOPSTree"); doUNLOPSLoopSave = settings.flag("Merging:doUNLOPSLoop"); doUNLOPSSubtSave = settings.flag("Merging:doUNLOPSSubt"); doUNLOPSSubtNLOSave = settings.flag("Merging:doUNLOPSSubtNLO"); bool doUNLOPS = doUNLOPSTreeSave || doUNLOPSLoopSave || doUNLOPSSubtSave || doUNLOPSSubtNLOSave; // Initialise UMEPS switches doUMEPSTreeSave = settings.flag("Merging:doUMEPSTree"); doUMEPSSubtSave = settings.flag("Merging:doUMEPSSubt"); nReclusterSave = settings.mode("Merging:nRecluster"); nQuarksMergeSave = settings.mode("Merging:nQuarksMerge"); bool doUMEPS = doUMEPSTreeSave || doUMEPSSubtSave; // Flag to only do phase space cut. doEstimateXSection = settings.flag("Merging:doXSectionEstimate"); // Get core process from user input processSave = settings.word("Merging:Process"); // Clear hard process hardProcess.clear(); // Initialise input event. inputEvent.init("(hard process)", particleDataPtr); doRemoveDecayProducts = settings.flag("Merging:mayRemoveDecayProducts"); // Initialise the hard process if ( doMGMergingSave ) hardProcess.initOnLHEF(lheInputFile, particleDataPtr); else hardProcess.initOnProcess(processSave, particleDataPtr); // Parameters for reconstruction of evolution scales includeMassiveSave = settings.flag("Merging:includeMassive"); enforceStrongOrderingSave = settings.flag("Merging:enforceStrongOrdering"); scaleSeparationFactorSave = settings.parm("Merging:scaleSeparationFactor"); orderInRapiditySave = settings.flag("Merging:orderInRapidity"); // Parameters for choosing history probabilistically nonJoinedNormSave = settings.parm("Merging:nonJoinedNorm"); fsrInRecNormSave = settings.parm("Merging:fsrInRecNorm"); pickByFullPSave = settings.flag("Merging:pickByFullP"); pickByPoPT2Save = settings.flag("Merging:pickByPoPT2"); includeRedundantSave = settings.flag("Merging:includeRedundant"); // Parameters for scale choices unorderedScalePrescipSave = settings.mode("Merging:unorderedScalePrescrip"); unorderedASscalePrescipSave = settings.mode("Merging:unorderedASscalePrescrip"); unorderedPDFscalePrescipSave = settings.mode("Merging:unorderedPDFscalePrescrip"); incompleteScalePrescipSave = settings.mode("Merging:incompleteScalePrescrip"); // Parameter for allowing swapping of one colour index while reclustering allowColourShufflingSave = settings.flag("Merging:allowColourShuffling"); // Parameters to allow setting hard process scales to default (dynamical) // Pythia values. resetHardQRenSave = settings.flag("Merging:usePythiaQRenHard"); resetHardQFacSave = settings.flag("Merging:usePythiaQFacHard"); // Parameters for choosing history by sum(|pT|) pickBySumPTSave = settings.flag("Merging:pickBySumPT"); herwigAcollFSRSave = settings.parm("Merging:aCollFSR"); herwigAcollISRSave = settings.parm("Merging:aCollISR"); // Information on the shower cut-off scale pT0ISRSave = settings.parm("SpaceShower:pT0Ref"); pTcutSave = settings.parm("SpaceShower:pTmin"); pTcutSave = max(pTcutSave,pT0ISRSave); // Initialise CKKWL weight weightCKKWLSave = 1.; weightFIRSTSave = 0.; nMinMPISave = 100; muMISave = -1.; // Initialise merging scale tmsValueSave = 0.; tmsListSave.resize(0); kFactor0jSave = settings.parm("Merging:kFactor0j"); kFactor1jSave = settings.parm("Merging:kFactor1j"); kFactor2jSave = settings.parm("Merging:kFactor2j"); muFSave = settings.parm("Merging:muFac"); muRSave = settings.parm("Merging:muRen"); muFinMESave = settings.parm("Merging:muFacInME"); muRinMESave = settings.parm("Merging:muRenInME"); doWClusteringSave = settings.flag("Merging:allowWClustering"); doSQCDClusteringSave = settings.flag("Merging:allowSQCDClustering"); // Save merging scale on maximal number of jets if ( doKTMergingSave || doUserMergingSave || doPTLundMergingSave || doUMEPS ) { // Read merging scale (defined in kT) from input parameter. tmsValueSave = settings.parm("Merging:TMS"); nJetMaxSave = settings.mode("Merging:nJetMax"); nJetMaxNLOSave = -1; } else if (doMGMergingSave) { // Read merging scale (defined in kT) from LHE file. tmsValueSave = hardProcess.tms; nJetMaxSave = settings.mode("Merging:nJetMax"); nJetMaxNLOSave = -1; } else if (doCutBasedMergingSave) { // Save list of cuts defining the merging scale. nJetMaxSave = settings.mode("Merging:nJetMax"); nJetMaxNLOSave = -1; // Write tms cut values to list of cut values, // ordered by DeltaR_{ij}, pT_{i}, Q_{ij}. tmsListSave.resize(0); double drms = settings.parm("Merging:dRijMS"); double ptms = settings.parm("Merging:pTiMS"); double qms = settings.parm("Merging:QijMS"); tmsListSave.push_back(drms); tmsListSave.push_back(ptms); tmsListSave.push_back(qms); } if ( doNL3 || doUNLOPS || doEstimateXSection ) { tmsValueSave = settings.parm("Merging:TMS"); nJetMaxSave = settings.mode("Merging:nJetMax"); nJetMaxNLOSave = settings.mode("Merging:nJetMaxNLO"); } bool writeBanner = doKTMergingSave || doMGMergingSave || doUserMergingSave || doNL3 || doUNLOPS || doUMEPS || doPTLundMergingSave || doCutBasedMergingSave; if (!writeBanner) return; // Write banner os << "\n *------------------ MEPS Merging Initialization ---------------" << "---*"; os << "\n | " << " |\n"; if ( doKTMergingSave || doMGMergingSave || doUserMergingSave || doPTLundMergingSave || doCutBasedMergingSave ) os << " | CKKW-L merge " << " |\n" << " |"<< setw(34) << processSave << " with up to" << setw(3) << nJetMaxSave << " additional jets |\n"; else if ( doNL3 ) os << " | NL3 merge " << " |\n" << " |" << setw(31) << processSave << " with jets up to" << setw(3) << nJetMaxNLOSave << " correct to NLO |\n" << " | and up to" << setw(3) << nJetMaxSave << " additional jets included by CKKW-L merging at LO |\n"; else if ( doUNLOPS ) os << " | UNLOPS merge " << " |\n" << " |" << setw(31) << processSave << " with jets up to" << setw(3)<< nJetMaxNLOSave << " correct to NLO |\n" << " | and up to" << setw(3) << nJetMaxSave << " additional jets included by UMEPS merging at LO |\n"; else if ( doUMEPS ) os << " | UMEPS merge " << " |\n" << " |" << setw(34) << processSave << " with up to" << setw(3) << nJetMaxSave << " additional jets |\n"; if ( doKTMergingSave ) os << " | Merging scale is defined in kT, with value ktMS = " << tmsValueSave << " GeV"; else if ( doMGMergingSave ) os << " | Perform automanted MG/ME merging \n" << " | Merging scale is defined in kT, with value ktMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; else if ( doUserMergingSave ) os << " | Merging scale is defined by the user, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " |"; else if ( doPTLundMergingSave ) os << " | Merging scale is defined by Lund pT, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; else if ( doCutBasedMergingSave ) os << " | Merging scale is defined by combination of Delta R_{ij}, pT_i " << " |\n" << " | and Q_{ij} cut, with values " << " |\n" << " | Delta R_{ij,min} = " << setw(7) << scientific << setprecision(2) << tmsListSave[0] << " |\n" << " | pT_{i,min} = " << setw(6) << fixed << setprecision(1) << tmsListSave[1] << " GeV |\n" << " | Q_{ij,min} = " << setw(6) << fixed << setprecision(1) << tmsListSave[2] << " GeV |"; else if ( doNL3TreeSave ) os << " | Generate tree-level O(alpha_s)-subtracted events " << " |\n" << " | Merging scale is defined by Lund pT, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; else if ( doNL3LoopSave ) os << " | Generate virtual correction unit-weight events " << " |\n" << " | Merging scale is defined by Lund pT, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; else if ( doNL3SubtSave ) os << " | Generate reclustered tree-level events " << " |\n" << " | Merging scale is defined by Lund pT, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; else if ( doUNLOPSTreeSave ) os << " | Generate tree-level O(alpha_s)-subtracted events " << " |\n" << " | Merging scale is defined by Lund pT, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; else if ( doUNLOPSLoopSave ) os << " | Generate virtual correction unit-weight events " << " |\n" << " | Merging scale is defined by Lund pT, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; else if ( doUNLOPSSubtSave ) os << " | Generate reclustered tree-level events " << " |\n" << " | Merging scale is defined by Lund pT, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; else if ( doUNLOPSSubtNLOSave ) os << " | Generate reclustered loop-level events " << " |\n" << " | Merging scale is defined by Lund pT, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; else if ( doUMEPSTreeSave ) os << " | Generate tree-level events " << " |\n" << " | Merging scale is defined by Lund pT, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; else if ( doUMEPSSubtSave ) os << " | Generate reclustered tree-level events " << " |\n" << " | Merging scale is defined by Lund pT, with value tMS = " << setw(6) << fixed << setprecision(1) << tmsValueSave << " GeV |"; os << "\n | " << " |"; os << "\n *-------------- END MEPS Merging Initialization ---------------" << "---*\n\n"; } //-------------------------------------------------------------------------- // Function to check if emission should be rejected. bool MergingHooks::doVetoEmission( const Event& event) { // Do nothing in trial showers, or after first step. if ( doIgnoreEmissionsSave ) return false; // Do nothing in CKKW-L if ( doUserMerging() || doMGMerging() || doKTMerging() || doPTLundMerging() || doCutBasedMerging() ) return false; // For NLO merging, count and veto emissions above the merging scale bool veto = false; // Get number of clustering steps int nSteps = getNumberOfClusteringSteps(event); // Get merging scale in current event double tnow = rhoms( event, false); // Get maximal number of additional jets int nJetMax = nMaxJets(); // Always remove emissions above the merging scale for // samples containing reclusterings! if ( nRecluster() > 0 ) nSteps = max(1, min(nJetMax-2, 1)); // Check veto condition if ( nSteps - 1 < nJetMax && nSteps >= 1 && tnow > tms() ) veto = true; // Do not veto if state already includes MPI. if ( infoPtr->nMPI() > 1 ) veto = false; // When performing NL3 merging of tree-level events, reset the // CKKWL weight. if ( veto && doNL3Tree() ) setWeightCKKWL(0.); // If the emission is allowed, do not check any further emissions if ( !veto ) doIgnoreEmissionsSave = true; // Done return veto; } //-------------------------------------------------------------------------- // Function to check if emission should be rejected. bool MergingHooks::doVetoStep( const Event& process, const Event& event, bool doResonance ) { // Do nothing in trial showers, or after first step. if ( doIgnoreStepSave && !doResonance ) return false; // Do nothing in UMEPS or UNLOPS if ( doUMEPSTree() || doUMEPSSubt() || doUMEPSMerging() || doUNLOPSTree() || doUNLOPSLoop() || doUNLOPSSubt() || doUNLOPSSubtNLO() || doUNLOPSMerging() ) return false; // Get number of clustering steps. If necessary, remove resonance // decay products first. int nSteps = (doResonance) ? getNumberOfClusteringSteps(process) : getNumberOfClusteringSteps( bareEvent( process, false) ); // Get maximal number of additional jets. int nJetMax = nMaxJets(); // Get merging scale in current event. double tnow = tmsNow( event ); // For non-resonant showers, simply check veto. If event should indeed be // vetoed, save the current pT and weights in case the veto needs to be // revoked. if ( !doResonance ) { // Store pT to check if veto needs to be revoked later. pTsave = infoPtr->pTnow(); if ( nRecluster() == 1) nSteps--; // Check merging veto condition. bool veto = false; if ( nSteps > nMaxJetsNLO() && nSteps < nJetMax && tnow > tms() ) { // Set weight to zero if event should be vetoed. weightCKKWL1Save = 0.; // Save weight before veto, in case veto needs to be revoked. weightCKKWL2Save = getWeightCKKWL(); // Reset stored weights. setWeightCKKWL(0.); veto = true; } // Done return veto; // For resonant showers, check if any previous veto should be revoked. // This means we treat showers off resonance decay products identical to // MPI: If a hard resonance emission has been produced, the event should // have been kept. Following this reasoning, it might be necessary to revoke // any previous veto. } else { // Initialise switch to revoke vetoing. bool revokeVeto = false; // Nothing to check if pTsave was not stored, i.e. no emission to // possibly veto was recorded. // Only allow revoking the veto for diboson processes, with resonant // electroweak bosons bool check = (nHardInLeptons() == 0)&& (nHardOutLeptons() == 2) && (nHardOutPartons() == 2); // For current purpose only!!! check = false; // For hadronic resonance decays at hadron colliders, do not veto // events with a hard emission of the resonance decay products, // since such states are not included in the matrix element if ( pTsave > 0. && check ) { // Check how many resonance decay systems are allowed int nResNow = nResInCurrent(); // Find systems really containing only emission off a resonance // decay vectorgoodSys; // Resonance decay systems are considered last, thus at the end of // the list int sysSize = partonSystemsPtr->sizeSys(); for ( int i=0; i < nResNow; ++i ) { if ( partonSystemsPtr->sizeOut(sysSize - 1 - i) == 3 ) goodSys.push_back(sysSize - 1 - i); } // Check the members of the resonance decay systems for ( int i=0; i < int(goodSys.size()); ++i ) { // Save the (three) members of the resonance decay system int iMem1 = partonSystemsPtr->getOut(goodSys[i],0); int iMem2 = partonSystemsPtr->getOut(goodSys[i],1); int iMem3 = partonSystemsPtr->getOut(goodSys[i],2); // Now find emitted gluon or gamma int iEmtGlue = ((event[iMem1].id() == 21) ? iMem1 : ((event[iMem2].id() == 21) ? iMem2 : ((event[iMem3].id() == 21) ? iMem3: 0))); int iEmtGamm = ((event[iMem1].id() == 22) ? iMem1 : ((event[iMem2].id() == 22) ? iMem2 : ((event[iMem3].id() == 22) ? iMem3: 0))); // Per system, only one emission int iEmt = (iEmtGlue != 0) ? iEmtGlue : iEmtGamm; int iRad = 0; int iRec = 0; if ( iEmt == iMem1 ) { iRad = (event[iMem2].mother1() != event[iMem2].mother2()) ? iMem2 : iMem3; iRec = (event[iMem3].mother1() == event[iMem3].mother2()) ? iMem3 : iMem2; } else if ( iEmt == iMem2 ) { iRad = (event[iMem1].mother1() != event[iMem1].mother2()) ? iMem1 : iMem3; iRec = (event[iMem3].mother1() == event[iMem3].mother2()) ? iMem3 : iMem1; } else { iRad = (event[iMem1].mother1() != event[iMem1].mother2()) ? iMem1 : iMem2; iRec = (event[iMem2].mother1() == event[iMem2].mother2()) ? iMem2 : iMem1; } double pTres = rhoPythia(event[iRad], event[iEmt], event[iRec], 1); // Revoke previous veto of last emission if a splitting of the // resonance produced a harder parton, i.e. we are inside the // PS region if ( pTres > pTsave ) { revokeVeto = true; // Do nothing (i.e. allow other first emission veto) for soft // splitting } else { revokeVeto = false; } // Done with one system } // Done with all systems } // Check veto condition bool veto = false; if ( revokeVeto && check ) { setWeightCKKWL(weightCKKWL2Save); } else if ( check ) { setWeightCKKWL(weightCKKWL1Save); if ( weightCKKWL1Save == 0. ) veto = true; } // Check veto condition. if ( !check && nSteps > nMaxJetsNLO() && nSteps < nJetMax && tnow > tms()){ // Set stored weights to zero. setWeightCKKWL(0.); // Now allow veto. veto = true; } // If the emission is allowed, do not check any further emissions if ( !veto || !doIgnoreStepSave ) doIgnoreStepSave = true; // Done return veto; } // Done return false; } //-------------------------------------------------------------------------- // Return event stripped from decay products. Event MergingHooks::bareEvent(const Event& inputEventIn, bool storeInputEvent ) { // Find and detach decay products. Event newProcess = Event(); newProcess.init("(hard process-modified)", particleDataPtr); // If desired, store input event. if ( storeInputEvent ) { resonances.resize(0); inputEvent.clear(); for (int i = 0; i < inputEventIn.size(); ++i) inputEvent.append( inputEventIn[i] ); for (int i = 0; i < inputEventIn.sizeJunction(); ++i) inputEvent.appendJunction( inputEventIn.getJunction(i) ); inputEvent.saveSize(); inputEvent.saveJunctionSize(); } // Now remove decay products. if ( doRemoveDecayProducts ) { // Add the beam and initial partons to the event record. for (int i = 0; i < inputEventIn.size(); ++ i) { if ( inputEventIn[i].mother1() > 4 || inputEventIn[i].statusAbs() == 22 || inputEventIn[i].statusAbs() == 23) break; newProcess.append(inputEventIn[i]); } // Add the intermediate particles to the event record. for (int i = 0; i < inputEventIn.size(); ++ i) { if (inputEventIn[i].mother1() > 4) break; if ( inputEventIn[i].status() == -22) { int j = newProcess.append(inputEventIn[i]); newProcess[j].statusPos(); if ( storeInputEvent ) resonances.push_back( make_pair(j, i) ); newProcess[j].daughters(0, 0); } } // Add remaining outgoing particles to the event record. for (int i = 0; i < inputEventIn.size(); ++ i) { if (inputEventIn[i].mother1() > 4) break; if ( inputEventIn[i].statusAbs() != 11 && inputEventIn[i].statusAbs() != 12 && inputEventIn[i].statusAbs() != 21 && inputEventIn[i].statusAbs() != 22) newProcess.append(inputEventIn[i]); } // Update event colour tag to maximum in whole process. int maxColTag = 0; for (int i = 0; i < inputEventIn.size(); ++ i) { if ( inputEventIn[i].col() > maxColTag ) maxColTag = inputEventIn[i].col(); if ( inputEventIn[i].acol() > maxColTag ) maxColTag = inputEventIn[i].acol(); } newProcess.initColTag(maxColTag); // Copy junctions from process to newProcess. for (int i = 0; i < inputEventIn.sizeJunction(); ++i) newProcess.appendJunction( inputEventIn.getJunction(i)); newProcess.saveSize(); newProcess.saveJunctionSize(); } else { newProcess = inputEventIn; } // Remember scale newProcess.scale( inputEventIn.scale() ); // Done return newProcess; } //-------------------------------------------------------------------------- // Write event with decay products attached to argument. Only possible if an // input event with decay producs had been stored before. bool MergingHooks::reattachResonanceDecays(Event& process ) { // Now reattach the decay products. if ( doRemoveDecayProducts && inputEvent.size() > 0 ) { int sizeBef = process.size(); // Vector of resonances for which the decay products were already attached. vector iAftChecked; // Reset daughters and status of intermediate particles. for ( int i = 0; i < int(resonances.size()); ++i ) { for (int j = 0; j < sizeBef; ++j ) { if ( j != resonances[i].first ) continue; int iOldDaughter1 = inputEvent[resonances[i].second].daughter1(); int iOldDaughter2 = inputEvent[resonances[i].second].daughter2(); // Get momenta in case of reclustering. int iHardMother = resonances[i].second; Particle& hardMother = inputEvent[iHardMother]; // Find current mother copy (after clustering). int iAftMother = 0; for ( int k = 0; k < process.size(); ++k ) if ( process[k].id() == inputEvent[resonances[i].second].id() ) { // Only attempt if decays of this resonance were not attached. bool checked = false; for ( int l = 0; l < int(iAftChecked.size()); ++l ) if ( k == iAftChecked[l] ) checked = true; if ( !checked ) { iAftChecked.push_back(k); iAftMother = k; break; } } Particle& aftMother = process[iAftMother]; // Resonance can have been moved by clustering, // so prepare to update colour and momentum information for system. int colBef = hardMother.col(); int acolBef = hardMother.acol(); int colAft = aftMother.col(); int acolAft = aftMother.acol(); RotBstMatrix M; M.bst( hardMother.p(), aftMother.p()); // Attach resonance decay products. int iNewDaughter1 = 0; int iNewDaughter2 = 0; for ( int k = iOldDaughter1; k <= iOldDaughter2; ++k ) { if ( k == iOldDaughter1 ) iNewDaughter1 = process.append(inputEvent[k] ); else iNewDaughter2 = process.append(inputEvent[k] ); process.back().statusPos(); Particle& now = process.back(); // Update colour and momentum information. if (now.col() != 0 && now.col() == colBef ) now.col(colAft); if (now.acol() != 0 && now.acol() == acolBef) now.acol(acolAft); now.rotbst( M); // Update vertex information. if (now.hasVertex()) now.vProd( aftMother.vDec() ); // Update mothers. now.mothers(iAftMother,0); } process[iAftMother].daughters( iNewDaughter1, iNewDaughter2 ); process[iAftMother].statusNeg(); // Loop through event and attach remaining decays int iDec = 0; do { if ( process[iDec].isFinal() && process[iDec].canDecay() && process[iDec].mayDecay() && process[iDec].isResonance() ) { int iD1 = process[iDec].daughter1(); int iD2 = process[iDec].daughter2(); // Done if no daughters exist. if ( iD1 == 0 || iD2 == 0 ) continue; // Attach daughters. int iNewDaughter12 = 0; int iNewDaughter22 = 0; for ( int k = iD1; k <= iD2; ++k ) { if ( k == iD1 ) iNewDaughter12 = process.append(inputEvent[k] ); else iNewDaughter22 = process.append(inputEvent[k] ); process.back().statusPos(); Particle& now = process.back(); // Update colour and momentum information. if (now.col() != 0 && now.col() == colBef ) now.col(colAft); if (now.acol()!= 0 && now.acol()== acolBef) now.acol(acolAft); now.rotbst( M); // Update vertex information. if (now.hasVertex()) now.vProd( process[iDec].vDec() ); // Update mothers. now.mothers(iDec,0); } // Modify mother status and daughters. process[iDec].status(-22); process[iDec].daughters(iNewDaughter12, iNewDaughter22); // End of loop over all entries. } } while (++iDec < process.size()); } // End loop over process entries. } // End loop over resonances. // Update event colour tag to maximum in whole process. int maxColTag = 0; for (int i = 0; i < process.size(); ++ i) { if (process[i].col() > maxColTag) maxColTag = process[i].col(); if (process[i].acol() > maxColTag) maxColTag = process[i].acol(); } process.initColTag(maxColTag); } // Done. return (doRemoveDecayProducts) ? inputEvent.size() > 0 : true; } //-------------------------------------------------------------------------- bool MergingHooks::isInHard( int iPos, const Event& event){ // MPI not part of hard process if ( event[iPos].statusAbs() > 30 && event[iPos].statusAbs() < 40 ) return false; // Beam remnants and hadronisation not part of hard process if ( event[iPos].statusAbs() > 60 ) return false; // Still MPI: Check that the particle is not due to radiation off MPIs. // First get all intermediate MPI partons in the state. vector mpiParticlePos; mpiParticlePos.clear(); for ( int i=0; i < event.size(); ++i ) if ( event[i].statusAbs() > 30 && event[i].statusAbs() < 40 ) mpiParticlePos.push_back(i); // Disregard any parton iPos that has MPI ancestors. for ( int i=0; i < int(mpiParticlePos.size()); ++i) if ( event.isAncestor(iPos, mpiParticlePos[i]) ) return false; // Disallow other systems. // Get sub-system of particles for iPos int iSys = partonSystemsPtr->getSystemOf(iPos, !event[iPos].isFinal() ); if ( iSys > 0 ) { // Check all partons belonging to the same system as iPos. If any is // produced in MPI or has MPI ancestors, the whole system is not the // hard subprocess, i.e. iPos is not in the hard subprocess. int sysSize = partonSystemsPtr->sizeAll(iSys); for ( int i = 0; i < sysSize; ++i ) { int iPosNow = partonSystemsPtr->getAll( iSys, i ); // MPI not part of hard process if ( event[iPosNow].statusAbs() > 30 && event[iPosNow].statusAbs() < 40 ) return false; // Disregard any parton iPos that has MPI ancestors. for ( int j=0; j < int(mpiParticlePos.size()); ++j) if ( event.isAncestor(iPosNow, mpiParticlePos[j]) ) return false; // Beam remnants and hadronisation not part of hard process if ( event[iPosNow].statusAbs() > 60 ) return false; } } // Check if any ancestor contains the hard incoming partons as daughters. // Begin loop to trace upwards from the daughter. bool containsInitialParton = false; int iUp = iPos; for ( ; ; ) { // If out of range then failed to find match. if (iUp <= 0 || iUp > event.size()) break; // If positive match then done. if ( iUp == 3 || iUp == 4 ) { containsInitialParton = true; break; } if ( event[iUp].mother1() == 1 && (event[iUp].daughter1() == 3 || event[iUp].daughter2() == 3) ) { containsInitialParton = true; break; } if ( event[iUp].mother1() == 2 && (event[iUp].daughter1() == 4 || event[iUp].daughter2() == 4) ) { containsInitialParton = true; break; } // If unique mother then keep on moving up the chain. iUp = event[iUp].mother1(); } if ( !containsInitialParton ) return false; // Done return true; } //-------------------------------------------------------------------------- // Function to return the number of clustering steps for the current event int MergingHooks::getNumberOfClusteringSteps(const Event& event){ // Count the number of final state partons int nFinalPartons = 0; for ( int i=0; i < event.size(); ++i) if ( event[i].isFinal() && isInHard( i, event) && (event[i].isQuark() || event[i].isGluon()) ) nFinalPartons++; // Count the number of final state leptons int nFinalLeptons = 0; for( int i=0; i < event.size(); ++i) if ( event[i].isFinal() && isInHard( i, event) && event[i].isLepton()) nFinalLeptons++; // Add neutralinos to number of leptons for( int i=0; i < event.size(); ++i) if ( event[i].isFinal() && isInHard( i, event) && event[i].idAbs() == 1000022) nFinalLeptons++; // Add sleptons to number of leptons for( int i=0; i < event.size(); ++i) if ( event[i].isFinal() && isInHard( i, event) && (event[i].idAbs() == 1000011 || event[i].idAbs() == 2000011 || event[i].idAbs() == 1000013 || event[i].idAbs() == 2000013 || event[i].idAbs() == 1000015 || event[i].idAbs() == 2000015) ) nFinalLeptons++; // Count the number of final state electroweak bosons int nFinalBosons = 0; for( int i=0; i < event.size(); ++i) if ( event[i].isFinal() && isInHard( i, event) && ( event[i].idAbs() == 22 || event[i].idAbs() == 23 || event[i].idAbs() == 24 || event[i].idAbs() == 25 ) ) nFinalBosons++; // Save sum of all final state particles int nFinal = nFinalPartons + nFinalLeptons + 2*(nFinalBosons - nHardOutBosons() ); // Return the difference to the core process outgoing particles return (nFinal - nHardOutPartons() - nHardOutLeptons() ); } //-------------------------------------------------------------------------- // Function to check if event contains an emission not present in the hard // process. bool MergingHooks::isFirstEmission(const Event& event ) { // If the beam remnant treatment or hadronisation has already started, do // no veto. for ( int i=0; i < event.size(); ++i) if ( event[i].statusAbs() > 60 ) return false; // Count particle types int nFinalQuarks = 0; int nFinalGluons = 0; int nFinalLeptons = 0; int nFinalBosons = 0; int nFinalPhotons = 0; int nFinal = 0; for( int i=0; i < event.size(); ++i) { if (event[i].isFinal() && isInHard(i, event) ){ if ( event[i].spinType() == 2 && event[i].colType() == 0) nFinalLeptons++; if ( event[i].id() == 23 || event[i].idAbs() == 24 || event[i].id() == 25) nFinalBosons++; if ( event[i].id() == 22) nFinalPhotons++; if ( event[i].isQuark()) nFinalQuarks++; if ( event[i].isGluon()) nFinalGluons++; if ( !event[i].isDiquark() ) nFinal++; } } // Return highest value if the event does not contain any final state // coloured particles. if (nFinalQuarks + nFinalGluons == 0) return false; // Use MergingHooks functions to get information on the hard process. int nLeptons = nHardOutLeptons(); // The state is already in the PS region if the number of leptons had been // increased bt QED splittings. if (nFinalLeptons > nLeptons) return false; // If the mumber of photons if larger than in the hard process, QED // radiation has pushed the state into the PS region. int nPhotons = 0; for(int i =0; i< int(hardProcess.hardOutgoing1.size()); ++i) if (hardProcess.hardOutgoing1[i] == 22) nPhotons++; for(int i =0; i< int(hardProcess.hardOutgoing2.size()); ++i) if (hardProcess.hardOutgoing2[i] == 22) nPhotons++; if (nFinalPhotons > nPhotons) return false; // Done return true; } //-------------------------------------------------------------------------- // Function to set the correct starting scales of the shower // Set starting scales bool MergingHooks::setShowerStartingScales( bool isTrial, bool doMergeFirstEmm, double& pTscaleIn, const Event& event, double& pTmaxFSRIn, bool& limitPTmaxFSRIn, double& pTmaxISRIn, bool& limitPTmaxISRIn, double& pTmaxMPIIn, bool& limitPTmaxMPIIn ) { // MPI treated differently in case of qcd djiet merging, since hard MPI // can be misidentified as hard process. bool isPureQCD = ( getProcessString().compare("pp>jj") == 0 ); int nSteps = getNumberOfClusteringSteps( bareEvent(event, false) ); double scale = event.scale(); bool doRecluster = doUMEPSSubt() || doNL3Subt() || doUNLOPSSubt() || doUNLOPSSubtNLO(); // Set correct starting scales for trial showers. if ( isTrial ) { // Reset shower scales. pTmaxISRIn = pTmaxFSRIn = scale; if ( limitPTmaxISRIn ) pTmaxISRIn = min(scale,muF()); if ( limitPTmaxFSRIn ) pTmaxFSRIn = min(scale,muF()); // Reset MPI scale. if ( !isPureQCD ) pTmaxMPIIn = scale; else pTmaxMPIIn = infoPtr->eCM(); // Reset phase space limitation flags if ( pTscaleIn < infoPtr->eCM() ) { limitPTmaxISRIn = limitPTmaxFSRIn = true; if ( !isPureQCD ) limitPTmaxMPIIn = true; else limitPTmaxMPIIn = false; } } // Reset starting scales. if ( isPureQCD && doMergeFirstEmm ) { // Set correct shower starting scales. if ( nSteps == 0 && !doRecluster && pTscaleIn < infoPtr->eCM() ) { pTmaxMPIIn = infoPtr->eCM(); limitPTmaxMPIIn = false; } } // Reset starting scales. if ( !isPureQCD && doMergeFirstEmm ) { // Set correct shower starting scales. if ( nSteps == 0 && !doRecluster ) { pTscaleIn = infoPtr->eCM(); limitPTmaxMPIIn = false; } if ( limitPTmaxISRIn ) pTscaleIn = min(scale,muF()); if ( limitPTmaxFSRIn ) pTscaleIn = min(scale,muF()); pTmaxISRIn = pTmaxFSRIn = pTscaleIn; // Reset MPI starting scale. Standard treatment if ( pTscaleIn < infoPtr->eCM() && !(nSteps == 0 && !doRecluster && (limitPTmaxISRIn || limitPTmaxFSRIn)) ) { pTmaxMPIIn = pTscaleIn; limitPTmaxMPIIn = true; } if (doRecluster) { pTmaxMPIIn = muMI(); limitPTmaxMPIIn = true; } } // Done return true; } //-------------------------------------------------------------------------- // Function to return the value of the merging scale function in the current // event. double MergingHooks::tmsNow( const Event& event ) { // Get merging scale in current event. double tnow = 0.; // Use KT/Durham merging scale definition. if ( doKTMerging() || doMGMerging() ) tnow = kTms(event); // Use Lund PT merging scale definition. else if ( doPTLundMerging() ) tnow = rhoms(event, false); // Use DeltaR_{ij}, pT_i, Q_{ij} combination merging scale definition. else if ( doCutBasedMerging() ) tnow = cutbasedms(event); // Use NLO merging (Lund PT) merging scale definition. else if ( doNL3Merging() ) tnow = rhoms(event, false); // Use NLO merging (Lund PT) merging scale definition. else if ( doUNLOPSMerging() ) tnow = rhoms(event, false); // Use UMEPS (Lund PT) merging scale definition. else if ( doUMEPSMerging() ) tnow = rhoms(event, false); // Use user-defined merging scale. else tnow = tmsDefinition(event); // Return merging scale value. Done return tnow; } //-------------------------------------------------------------------------- // Function to check if the properties of the input particle should be // checked against the cut-based merging scale defintion. bool MergingHooks::checkAgainstCut( const Particle& particle){ // Do not check uncoloured particles. if (particle.colType() == 0) return false; // By default, use u-, d-, c-, s- and b-quarks. if ( particle.idAbs() != 21 && particle.idAbs() > nQuarksMergeSave ) return false; // Done return true; } //-------------------------------------------------------------------------- // Function to return the minimal kT in the event. If doKTMerging = true, this // function will be used as a merging scale definition. double MergingHooks::kTms(const Event& event) { // Only check first emission. if (!isFirstEmission(event)) return 0.; // Find all electroweak decayed bosons in the state. vector ewResonancePos; ewResonancePos.clear(); for (int i=0; i < event.size(); ++i) if ( abs(event[i].status()) == 22 && ( event[i].idAbs() == 22 || event[i].idAbs() == 23 || event[i].idAbs() == 24 || event[i].idAbs() == 25 || event[i].idAbs() == 6 ) ) ewResonancePos.push_back(i); // Declare final parton vectors vector FinalPartPos; FinalPartPos.clear(); // Search inEvent record for final state partons. // Exclude decay products of ew resonance. for (int i=0; i < event.size(); ++i){ if ( event[i].isFinal() && isInHard( i, event ) && event[i].colType() != 0 && checkAgainstCut(event[i]) ){ bool isDecayProduct = false; for(int j=0; j < int(ewResonancePos.size()); ++j) if ( event.isAncestor(i, ewResonancePos[j]) ) isDecayProduct = true; // Except for e+e- -> jets, do not check radiation in resonance decays. if ( !isDecayProduct || getProcessString().compare("e+e->jj") == 0 || getProcessString().compare("e+e->(z>jj)") == 0 ) FinalPartPos.push_back(i); } } // Declare kT algorithm parameters double Dparam = 0.4; // Find minimal Durham kT in event, using own function: Check // definition of separation int type = (event[3].colType() == 0 && event[4].colType() == 0) ? -1 : ktTypeSave; // Find minimal kT double ktmin = event[0].e(); for(int i=0; i < int(FinalPartPos.size()); ++i){ double kt12 = ktmin; // Compute separation to the beam axis for hadronic collisions if (type == 1 || type == 2) { double temp = event[FinalPartPos[i]].pT(); kt12 = min(kt12, temp); } // Compute separation to other final state jets for(int j=i+1; j < int(FinalPartPos.size()); ++j) { double temp = kTdurham( event[FinalPartPos[i]], event[FinalPartPos[j]], type, Dparam); kt12 = min(kt12, temp); } // Keep the minimal Durham separation ktmin = min(ktmin,kt12); } // Return minimal Durham kT return ktmin; } //-------------------------------------------------------------------------- // Function to compute durham y separation from Particle input. double MergingHooks::kTdurham(const Particle& RadAfterBranch, const Particle& EmtAfterBranch, int Type, double D ){ // Declare return variable double ktdur; // Save 4-momenta of final state particles Vec4 jet1 = RadAfterBranch.p(); Vec4 jet2 = EmtAfterBranch.p(); if ( Type == -1) { // Get angle between jets for e+e- collisions, make sure that // -1 <= cos(theta) <= 1 double costh; if (jet1.pAbs()*jet2.pAbs() <=0.) costh = 1.; else { costh = costheta(jet1,jet2); } // Calculate kt durham separation between jets for e+e- collisions ktdur = 2.0*min( pow(jet1.e(),2) , (pow(jet2.e(),2)) )*(1.0 - costh); } else if ( Type == 1 ){ // Get delta_y for hadronic collisions: // Get mT of first jet double mT1sq = jet1.m2Calc() + jet1.pT2(); double mT1 = 0.; if (mT1sq < 0) mT1 = - sqrt(-mT1sq); else mT1 = sqrt(mT1sq); // Get mT of second jet double mT2sq = jet2.m2Calc() + jet2.pT2(); double mT2 = 0.; if (mT2sq < 0) mT2 = - sqrt(-mT2sq); else mT2 = sqrt(mT2sq); // Get rapidity of first jet double y1 = log( ( jet1.e() + abs(jet1.pz()) ) / mT1 ); if (jet1.pz() < 0) y1 *= -1.; // Get rapidity of second jet double y2 = log( ( jet2.e() + abs(jet2.pz()) ) / mT2 ); if (jet2.pz() < 0) y2 *= -1.; // Get delta_phi for hadronic collisions double pt1 = sqrt( pow(jet1.px(),2) + pow(jet1.py(),2) ); double pt2 = sqrt( pow(jet2.px(),2) + pow(jet2.py(),2) ); double cosdPhi = ( jet1.px()*jet2.px() + jet1.py()*jet2.py() ) / (pt1*pt2); double dPhi = acos( cosdPhi ); // Calculate kT durham like fastjet, // but with rapidity instead of pseudo-rapidity ktdur = min( pow(pt1,2),pow(pt2,2) ) * ( pow(y1-y2,2) + pow(dPhi,2) ) / pow(D,2); } else if ( Type == 2 ){ // Get mT of first jet double mT1sq = jet1.m2Calc() + jet1.pT2(); double mT1 = 0.; if (mT1sq < 0) mT1 = - sqrt(-mT1sq); else mT1 = sqrt(mT1sq); // Get mT of second jet double mT2sq = jet2.m2Calc() + jet2.pT2(); double mT2 = 0.; if (mT2sq < 0) mT2 = - sqrt(-mT2sq); else mT2 = sqrt(mT2sq); // Get pseudo-rapidity of first jet double eta1 = log( ( sqrt(jet1.px()*jet1.px() + jet1.py()*jet1.py() + jet1.pz()*jet1.pz()) + abs(jet1.pz()) ) / mT1); if (jet1.pz() < 0) eta1 *= -1.; // Get pseudo-rapidity of second jet double eta2 = log( ( sqrt(jet2.px()*jet2.px() + jet2.py()*jet2.py() + jet2.pz()*jet2.pz()) + abs(jet2.pz()) ) / mT2); if (jet2.pz() < 0) eta2 *= -1.; // Get delta_phi and cos(Delta_phi) for hadronic collisions double pt1 = sqrt( pow(jet1.px(),2) + pow(jet1.py(),2) ); double pt2 = sqrt( pow(jet2.px(),2) + pow(jet2.py(),2) ); double cosdPhi = ( jet1.px()*jet2.px() + jet1.py()*jet2.py() ) / (pt1*pt2); double dPhi = acos( cosdPhi ); // Calculate kT durham like fastjet ktdur = min( pow(pt1,2),pow(pt2,2) ) * ( pow(eta1-eta2,2) + pow(dPhi,2) ) / pow(D,2); } else if ( Type == 3 ){ // Get cosh(Delta_eta) for hadronic collisions double eta1 = 0.5*log( (jet1.e() + jet1.pz()) / (jet1.e() - jet1.pz()) ); double eta2 = 0.5*log( (jet2.e() + jet2.pz()) / (jet2.e() - jet2.pz()) ); double coshdEta = cosh( eta1 - eta2 ); // Get delta_phi and cos(Delta_phi) for hadronic collisions double pt1 = sqrt( pow(jet1.px(),2) + pow(jet1.py(),2) ); double pt2 = sqrt( pow(jet2.px(),2) + pow(jet2.py(),2) ); double cosdPhi = ( jet1.px()*jet2.px() + jet1.py()*jet2.py() ) / (pt1*pt2); // Calculate kT durham separation "SHERPA-like" ktdur = 2.0*min( pow(pt1,2),pow(pt2,2) ) * ( coshdEta - cosdPhi ) / pow(D,2); } else { ktdur = 0.0; } // Return kT return sqrt(ktdur); } //-------------------------------------------------------------------------- // Find the minimal Lund pT between coloured partons in the input // event. If doPTLundMerging = true, this function will be used as a merging // scale definition. double MergingHooks::rhoms( const Event& event, bool withColour){ // Only check first emission. if (!isFirstEmission(event)) return 0.; // Find all electroweak decayed bosons in the state. vector ewResonancePos; ewResonancePos.clear(); for (int i=0; i < event.size(); ++i) if ( abs(event[i].status()) == 22 && ( event[i].idAbs() == 22 || event[i].idAbs() == 23 || event[i].idAbs() == 24 || event[i].idAbs() == 25 || event[i].idAbs() == 6 ) ) ewResonancePos.push_back(i); // Declare final parton vectors vector FinalPartPos; FinalPartPos.clear(); // Search inEvent record for final state partons. // Exclude decay products of ew resonance. for (int i=0; i < event.size(); ++i){ if ( event[i].isFinal() && isInHard( i, event ) && event[i].colType() != 0 && checkAgainstCut(event[i]) ){ bool isDecayProduct = false; for(int j=0; j < int(ewResonancePos.size()); ++j) if ( event.isAncestor(i, ewResonancePos[j]) ) isDecayProduct = true; // Except for e+e- -> jets, do not check radiation in resonance decays. if ( !isDecayProduct || getProcessString().compare("e+e->jj") == 0 || getProcessString().compare("e+e->(z>jj)") == 0 ) FinalPartPos.push_back(i); } } // Get index of first incoming int in1 = 0; for (int i=0; i < event.size(); ++i) if (abs(event[i].status()) == 41 ){ in1 = i; break; } // Get index of second incoming int in2 = 0; for (int i=0; i < event.size(); ++i) if (abs(event[i].status()) == 42 ){ in2 = i; break; } // If no incoming of the cascade are found, try incoming if (in1 == 0 || in2 == 0){ // Find current incoming partons for(int i=3; i < int(event.size()); ++i){ if ( !isInHard( i, event ) ) continue; if (event[i].mother1() == 1) in1 = i; if (event[i].mother1() == 2) in2 = i; } } // Find minimal pythia pt in event double ptmin = event[0].e(); for(int i=0; i < int(FinalPartPos.size()); ++i){ double pt12 = ptmin; // Compute pythia ISR separation i-jet and first incoming if (event[in1].colType() != 0) { double temp = rhoPythia( event[in1], event[FinalPartPos[i]], event[in2], -1 ); pt12 = min(pt12, temp); } // Compute pythia ISR separation i-jet and second incoming if ( event[in2].colType() != 0) { double temp = rhoPythia( event[in2], event[FinalPartPos[i]], event[in1], -1 ); pt12 = min(pt12, temp); } if (withColour) { // Compute pythia FSR separation between two jets, // with knowledge of colour connections for(int j=0; j < int(FinalPartPos.size()); ++j) { // Find recoiler in event if ( i!=j ){ bool isHard = false; int radAcl = event[FinalPartPos[i]].acol(); int radCol = event[FinalPartPos[i]].col(); int emtAcl = event[FinalPartPos[j]].acol(); int emtCol = event[FinalPartPos[j]].col(); int iRec = -1; // Check in final state if (iRec <= 0 && radAcl > 0 && radAcl != emtCol) iRec = findColour(radAcl, FinalPartPos[i], FinalPartPos[j], event,1, isHard); if (iRec <= 0 && radCol > 0 && radCol != emtAcl) iRec = findColour(radCol, FinalPartPos[i], FinalPartPos[j], event,1, isHard); if (iRec <= 0 && emtAcl > 0 && emtAcl != radCol) iRec = findColour(emtAcl, FinalPartPos[i], FinalPartPos[j], event,1, isHard); if (iRec <= 0 && emtCol > 0 && emtCol != radAcl) iRec = findColour(emtCol, FinalPartPos[i], FinalPartPos[j], event,1, isHard); // Check in initial state if (iRec <= 0 && radAcl > 0 && radAcl != emtCol) iRec = findColour(radAcl, FinalPartPos[i], FinalPartPos[j], event,2, isHard); if (iRec <= 0 && radCol > 0 && radCol != emtAcl) iRec = findColour(radCol, FinalPartPos[i], FinalPartPos[j], event,2, isHard); if (iRec <= 0 && emtAcl > 0 && emtAcl != radCol) iRec = findColour(emtAcl, FinalPartPos[i], FinalPartPos[j], event,2, isHard); if (iRec <= 0 && emtCol > 0 && emtCol != radAcl) iRec = findColour(emtCol, FinalPartPos[i], FinalPartPos[j], event,2, isHard); if (iRec > 0) { double temp = rhoPythia( event[FinalPartPos[i]], event[FinalPartPos[j]], event[iRec], 1 ); pt12 = min(pt12, temp); } } } } else { // Compute pythia FSR separation between two jets, // without any knowledge of colour connections for(int j=0; j < int(FinalPartPos.size()); ++j) { for(int k=0; k < int(FinalPartPos.size()); ++k) { // Allow any parton as recoiler if ( (i != j) && (i != k) && (j != k) ){ double temp = 0.; // Only check splittings allowed by flavour, e.g. // only q -> qg and g -> qqbar temp = rhoPythia( event[FinalPartPos[i]], event[FinalPartPos[j]], event[FinalPartPos[k]], 1 ); pt12 = min(pt12, temp); } } } // Compute pythia FSR separation between two jets, with initial recoiler // without any knowledge of colour connections if ( event[in1].colType() != 0 && event[in2].colType() != 0) { for(int j=0; j < int(FinalPartPos.size()); ++j) { // Allow both initial partons as recoiler if ( i != j ){ // Check with first initial as recoiler double temp = rhoPythia( event[FinalPartPos[i]], event[FinalPartPos[j]], event[in1], 1 ); pt12 = min(pt12, temp); // Check with second initial as recoiler temp = rhoPythia( event[FinalPartPos[i]], event[FinalPartPos[j]], event[in2], 1 ); pt12 = min(pt12, temp); } } } } // Reset minimal y separation ptmin = min(ptmin,pt12); } return ptmin; } //-------------------------------------------------------------------------- // Function to compute "pythia pT separation" from Particle input, as a helper // for rhoms(...). double MergingHooks::rhoPythia(const Particle& RadAfterBranch, const Particle& EmtAfterBranch, const Particle& RecAfterBranch, int ShowerType){ // Save type: 1 = FSR pT definition, else ISR definition int Type = ShowerType; // Calculate virtuality of splitting int sign = (Type==1) ? 1 : -1; Vec4 Q(RadAfterBranch.p() + sign*EmtAfterBranch.p()); double Qsq = sign * Q.m2Calc(); // Mass term of radiator double m2Rad = ( includeMassive() && abs(RadAfterBranch.id()) >= 4 && abs(RadAfterBranch.id()) < 7) ? pow(particleDataPtr->m0(RadAfterBranch.id()), 2) : 0.; // Construct 2->3 variables for FSR Vec4 sum = RadAfterBranch.p() + RecAfterBranch.p() + EmtAfterBranch.p(); double m2Dip = sum.m2Calc(); double x1 = 2. * (sum * RadAfterBranch.p()) / m2Dip; double x3 = 2. * (sum * EmtAfterBranch.p()) / m2Dip; // Construct momenta of dipole before/after splitting for ISR Vec4 qBR(RadAfterBranch.p() - EmtAfterBranch.p() + RecAfterBranch.p()); Vec4 qAR(RadAfterBranch.p() + RecAfterBranch.p()); // Calculate z of splitting, different for FSR and ISR double z = (Type==1) ? x1/(x1+x3) : (qBR.m2Calc())/( qAR.m2Calc()); // Separation of splitting, different for FSR and ISR double pTpyth = (Type==1) ? z*(1.-z) : (1.-z); // pT^2 = separation*virtuality pTpyth *= (Qsq - sign*m2Rad); if (pTpyth < 0.) pTpyth = 0.; // Return pT return sqrt(pTpyth); } //-------------------------------------------------------------------------- // Function to find a colour (anticolour) index in the input event. // Helper for rhoms // IN int col : Colour tag to be investigated // int iExclude1 : Identifier of first particle to be excluded // from search // int iExclude2 : Identifier of second particle to be excluded // from search // Event event : event to be searched for colour tag // int type : Tag to define if col should be counted as // colour (type = 1) [->find anti-colour index // contracted with col] // anticolour (type = 2) [->find colour index // contracted with col] // OUT int : Position of particle in event record // contraced with col [0 if col is free tag] int MergingHooks::findColour(int col, int iExclude1, int iExclude2, const Event& event, int type, bool isHardIn){ bool isHard = isHardIn; int index = 0; if (isHard){ // Search event record for matching colour & anticolour for(int n = 0; n < event.size(); ++n) { if ( n != iExclude1 && n != iExclude2 && event[n].colType() != 0 &&( event[n].status() > 0 // Check outgoing || event[n].status() == -21) ) { // Check incoming if ( event[n].acol() == col ) { index = -n; break; } if ( event[n].col() == col ){ index = n; break; } } } } else { // Search event record for matching colour & anticolour for(int n = 0; n < event.size(); ++n) { if ( n != iExclude1 && n != iExclude2 && event[n].colType() != 0 &&( event[n].status() == 43 // Check outgoing from ISR || event[n].status() == 51 // Check outgoing from FSR || event[n].status() == 52 // Check outgoing from FSR || event[n].status() == -41 // first initial || event[n].status() == -42) ) { // second initial if ( event[n].acol() == col ) { index = -n; break; } if ( event[n].col() == col ){ index = n; break; } } } } // if no matching colour / anticolour has been found, return false if ( type == 1 && index < 0) return abs(index); if ( type == 2 && index > 0) return abs(index); return 0; } //-------------------------------------------------------------------------- // Find the if the event passes the Delta R_{ij}, pT_{i} and Q_{ij} cuts on // the matrix element, as needed for cut-based merging scale definition. double MergingHooks::cutbasedms( const Event& event ){ // Only check first emission. if (!isFirstEmission(event)) return -1.; // Save allowed final state particles vector partons; for( int i=0; i < event.size(); ++i) { if ( event[i].isFinal() && isInHard( i, event ) && checkAgainstCut(event[i]) ) partons.push_back(i); } // Declare overall veto bool doVeto = false; // Declare vetoes bool vetoPT = false; bool vetoRjj = false; bool vetoMjj = false; // Declare cuts used in matrix element double pTjmin = pTiMS(); double mjjmin = QijMS(); double rjjmin = dRijMS(); // Declare minimum values double minPT = event[0].e(); double minRJJ = 10.; double minMJJ = event[0].e(); // Check matrix element cuts for( int i=0; i < int(partons.size()); ++i){ // Save pT value minPT = min(minPT,event[partons[i]].pT()); // Check two-parton cuts for( int j=0; j < int(partons.size()); ++j){ if (i!=j){ // Save delta R value minRJJ = min(minRJJ, deltaRij( event[partons[i]].p(), event[partons[j]].p()) ); // Save delta R value minMJJ = min(minMJJ, ( event[partons[i]].p() +event[partons[j]].p() ).mCalc() ); } } // Done with cut evaluation } // Check if all partons are in the matrix element region if (minPT > pTjmin) vetoPT = true; if (minRJJ > rjjmin) vetoRjj = true; if (minMJJ > mjjmin) vetoMjj = true; // In the matrix element calculation, we have rejected the events if any of // the cuts had not been fulfilled, // i.e. we are in the matrix element domain if all cuts are fulfilled. // We veto any emission in the ME region. // Disregard the two-parton cuts if only one parton in the final state if (int(partons.size() == 1)) doVeto = vetoPT; else // Veto if the combination of cuts would be in the ME region doVeto = vetoPT && vetoRjj && vetoMjj; // If event is above merging scale, veto if (doVeto) return 1.; // Else, do nothing return -1.; } //-------------------------------------------------------------------------- // Function to compute Delta R separation from 4-vector input. double MergingHooks::deltaRij(Vec4 jet1, Vec4 jet2){ // Declare return variable double deltaR = 0.; // Get delta_eta and cosh(Delta_eta) for hadronic collisions double eta1 = 0.5*log( (jet1.e() + jet1.pz()) / (jet1.e() - jet1.pz()) ); double eta2 = 0.5*log( (jet2.e() + jet2.pz()) / (jet2.e() - jet2.pz()) ); // Get delta_phi and cos(Delta_phi) for hadronic collisions double pt1 = sqrt( pow(jet1.px(),2) + pow(jet1.py(),2) ); double pt2 = sqrt( pow(jet2.px(),2) + pow(jet2.py(),2) ); double cosdPhi = ( jet1.px()*jet2.px() + jet1.py()*jet2.py() ) / (pt1*pt2); double dPhi = acos( cosdPhi ); // Calculate kT durham like fastjet deltaR = sqrt(pow(eta1-eta2,2) + pow(dPhi,2)); // Return kT return deltaR; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaLeptoquark.cc0000644000175000017500000002163712217346251016553 0ustar sunsun// SigmaLeptoquark.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // leptoquark simulation classes. #include "Pythia8/SigmaLeptoquark.h" namespace Pythia8 { //========================================================================== // Sigma1ql2LeptoQuark class. // Cross section for q l -> LQ (leptoquark state). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ql2LeptoQuark::initProc() { // Store LQ mass and width for propagator. mRes = particleDataPtr->m0(42); GammaRes = particleDataPtr->mWidth(42); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Yukawa coupling strength. kCoup = settingsPtr->parm("LeptoQuark:kCoup"); // Set pointer to particle properties and decay table. LQPtr = particleDataPtr->particleDataEntryPtr(42); // Read out quark and lepton the LQ couples to. idQuark = LQPtr->channel(0).product(0); idLepton = LQPtr->channel(0).product(1); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1ql2LeptoQuark::sigmaKin() { // Incoming width for correct quark-lepton pair. widthIn = 0.25 * alpEM * kCoup * mH; // Set up Breit-Wigner. sigBW = 4. * M_PI/ ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat) for specific incoming flavours. double Sigma1ql2LeptoQuark::sigmaHat() { // Identify whether correct incoming flavours. int idLQ = 0; if (id1 == idQuark && id2 == idLepton) idLQ = 42; else if (id2 == idQuark && id1 == idLepton) idLQ = 42; else if (id1 == -idQuark && id2 == -idLepton) idLQ = -42; else if (id2 == -idQuark && id1 == -idLepton) idLQ = -42; if (idLQ == 0) return 0.; // Outgoing width and total sigma. Done. return widthIn * sigBW * LQPtr->resWidthOpen(idLQ, mH); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ql2LeptoQuark::setIdColAcol() { // Flavours. int idq = (abs(id1) < 9) ? id1 : id2; int idLQ = (idq > 0) ? 42 : -42; setId( id1, id2, idLQ); // Colour flow topology. if (id1 == idq) setColAcol( 1, 0, 0, 0, 1, 0); else setColAcol( 0, 0, 1, 0, 1, 0); if (idq < 0) swapColAcol(); } //========================================================================== // Sigma2qg2LeptoQuarkl class. // Cross section for q g -> LQ l (leptoquark state). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2LeptoQuarkl::initProc() { // Store LQ mass and width for propagator. mRes = particleDataPtr->m0(42); GammaRes = particleDataPtr->mWidth(42); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Yukawa coupling strength. kCoup = settingsPtr->parm("LeptoQuark:kCoup"); // Read out quark and lepton the LQ couples to. ParticleDataEntry* LQPtr = particleDataPtr->particleDataEntryPtr(42); idQuark = LQPtr->channel(0).product(0); idLepton = LQPtr->channel(0).product(1); // Secondary open width fraction. openFracPos = LQPtr->resOpenFrac( 42); openFracNeg = LQPtr->resOpenFrac(-42); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2qg2LeptoQuarkl::sigmaKin() { // Evaluate cross section. sigma0 = (M_PI / sH2) * kCoup * (alpS * alpEM / 6.) * (-tH / sH) * (uH2 + s3 * s3) / pow2(uH - s3); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat) for specific incoming flavours. double Sigma2qg2LeptoQuarkl::sigmaHat() { // Check that correct incoming flavour. if (abs(id1) != idQuark && abs(id2) != idQuark) return 0.; // Answer, with secondary width correction. double sigma = sigma0; sigma *= (id1 == idQuark || id2 == idQuark) ? openFracPos : openFracNeg; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2LeptoQuarkl::setIdColAcol() { // Flavour set up for q g -> H q. int idq = (id2 == 21) ? id1 : id2; int idLQ = (idq > 0) ? 42 : -42; int idlp = (idq > 0) ? -idLepton : idLepton; setId( id1, id2, idLQ, idlp); // tH defined between f and f': must swap tHat <-> uHat if q g in. swapTU = (id2 == 21); // Colour flow topologies. Swap when antiquarks. if (id2 == 21) setColAcol( 1, 0, 2, 1, 2, 0, 0, 0); else setColAcol( 2, 1, 1, 0, 2, 0, 0, 0); if (idq < 0) swapColAcol(); } //========================================================================== // Sigma2gg2LQLQbar class. // Cross section for g g -> LQ LQbar (leptoquark state). //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2LQLQbar::initProc() { // Store LQ mass and width for propagator. mRes = particleDataPtr->m0(42); GammaRes = particleDataPtr->mWidth(42); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(42, -42); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2gg2LQLQbar::sigmaKin() { // Average outgoing masses and adjust kinematics accordingly. double delta = 0.25 * pow2(s3 - s4) / sH; double m2avg = 0.5 * (s3 + s4) - delta; double tHavg = tH - delta; double uHavg = uH - delta; // Evaluate cross section. Secondary width for G*. sigma = (M_PI / sH2) * 0.5 * pow2(alpS) * ( 7. / 48. + 3. * pow2(uHavg - tHavg) / (16. * sH2) ) * ( 1. + 2. * m2avg * tHavg / pow2(tHavg - m2avg) + 2. * m2avg * uHavg / pow2(uHavg - m2avg) + 4. * m2avg * m2avg / ((tHavg - m2avg) * (uHavg - m2avg)) ); sigma *= openFrac; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2LQLQbar::setIdColAcol() { // Flavours trivial. setId( 21, 21, 42, -42); // Colour flow topologies: random choice between two mirrors. if (rndmPtr->flat() < 0.5) setColAcol( 1, 2, 2, 3, 1, 0, 0, 3); else setColAcol( 1, 2, 3, 1, 3, 0, 0, 2); } //========================================================================== // Sigma2qqbar2LQLQbar class. // Cross section for q qbar -> LQ LQbar (leptoquark state). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2LQLQbar::initProc() { // Store LQ mass and width for propagator. mRes = particleDataPtr->m0(42); GammaRes = particleDataPtr->mWidth(42); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Yukawa coupling strength. kCoup = settingsPtr->parm("LeptoQuark:kCoup"); // Read out quark and lepton the LQ couples to. ParticleDataEntry* LQPtr = particleDataPtr->particleDataEntryPtr(42); idQuark = LQPtr->channel(0).product(0); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(42, -42); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2qqbar2LQLQbar::sigmaKin() { // Average outgoing masses and adjust kinematics accordingly. double delta = 0.25 * pow2(s3 - s4) / sH; double m2avg = 0.5 * (s3 + s4) - delta; double tHavg = tH - delta; double uHavg = uH - delta; // Evaluate cross section for quark of different flavour than LQ. sigmaDiff = (M_PI / sH2) * (pow2(alpS) / 9.) * ( sH * (sH - 4. * m2avg) - pow2(uHavg - tHavg) ) / sH2; // Evaluate cross section for quark of same flavour as LQ. sigmaSame = sigmaDiff + (M_PI / sH2) * (pow2(kCoup * alpEM) / 8.) * (-sH * tHavg - pow2(m2avg-tHavg)) / pow2(tHavg) + (M_PI / sH2) * (kCoup * alpEM * alpS / 18.) * ( (m2avg - tHavg) * (uHavg - tHavg) + sH * (m2avg + tHavg) ) / (sH * tHavg); // Open fraction. sigmaDiff *= openFrac; sigmaSame *= openFrac; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2LQLQbar::setIdColAcol() { // Flavours trivial. setId( id1, id2, 42, -42); // tH defined between f and LQ: must swap tHat <-> uHat if qbar q in. swapTU = (id1 < 0); // Colour flow topologies. if (id1 > 0) setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); else setColAcol( 0, 2, 1, 0, 1, 0, 0, 2); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/ParticleDecays.cc0000644000175000017500000012772112217346246016344 0ustar sunsun// ParticleDecays.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // ParticleDecays class. #include "Pythia8/ParticleDecays.h" namespace Pythia8 { //========================================================================== // The ParticleDecays class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of times one tries to let decay happen (for 2 nested loops). const int ParticleDecays::NTRYDECAY = 10; // Number of times one tries to pick valid hadronic content in decay. const int ParticleDecays::NTRYPICK = 100; // Number of times one tries to pick decay topology. const int ParticleDecays::NTRYMEWT = 1000; // Maximal loop count in Dalitz decay treatment. const int ParticleDecays::NTRYDALITZ = 1000; // Minimal Dalitz pair mass this factor above threshold. const double ParticleDecays::MSAFEDALITZ = 1.000001; // These numbers are hardwired empirical parameters, // intended to speed up the M-generator. const double ParticleDecays::WTCORRECTION[11] = { 1., 1., 1., 2., 5., 15., 60., 250., 1250., 7000., 50000. }; //-------------------------------------------------------------------------- // Initialize and save pointers. void ParticleDecays::init(Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, Couplings* couplingsPtrIn, TimeShower* timesDecPtrIn, StringFlav* flavSelPtrIn, DecayHandler* decayHandlePtrIn, vector handledParticles) { // Save pointers to error messages handling and flavour generation. infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; couplingsPtr = couplingsPtrIn; flavSelPtr = flavSelPtrIn; // Save pointer to timelike shower, as needed in some few decays. timesDecPtr = timesDecPtrIn; // Save pointer for external handling of some decays. decayHandlePtr = decayHandlePtrIn; // Set which particles should be handled externally. if (decayHandlePtr != 0) for (int i = 0; i < int(handledParticles.size()); ++i) particleDataPtr->doExternalDecay(handledParticles[i], true); // Safety margin in mass to avoid troubles. mSafety = settings.parm("ParticleDecays:mSafety"); // Lifetime and vertex rules for determining whether decay allowed. limitTau0 = settings.flag("ParticleDecays:limitTau0"); tau0Max = settings.parm("ParticleDecays:tau0Max"); limitTau = settings.flag("ParticleDecays:limitTau"); tauMax = settings.parm("ParticleDecays:tauMax"); limitRadius = settings.flag("ParticleDecays:limitRadius"); rMax = settings.parm("ParticleDecays:rMax"); limitCylinder = settings.flag("ParticleDecays:limitCylinder"); xyMax = settings.parm("ParticleDecays:xyMax"); zMax = settings.parm("ParticleDecays:zMax"); limitDecay = limitTau0 || limitTau || limitRadius || limitCylinder; // B-Bbar mixing parameters. mixB = settings.flag("ParticleDecays:mixB"); xBdMix = settings.parm("ParticleDecays:xBdMix"); xBsMix = settings.parm("ParticleDecays:xBsMix"); // Suppression of extra-hadron momenta in semileptonic decays. sigmaSoft = settings.parm("ParticleDecays:sigmaSoft"); // Selection of multiplicity and colours in "phase space" model. multIncrease = settings.parm("ParticleDecays:multIncrease"); multIncreaseWeak = settings.parm("ParticleDecays:multIncreaseWeak"); multRefMass = settings.parm("ParticleDecays:multRefMass"); multGoffset = settings.parm("ParticleDecays:multGoffset"); colRearrange = settings.parm("ParticleDecays:colRearrange"); // Minimum energy in system (+ m_q) from StringFragmentation. stopMass = settings.parm("StringFragmentation:stopMass"); // Parameters for Dalitz decay virtual gamma mass spectrum. sRhoDal = pow2(particleDataPtr->m0(113)); wRhoDal = pow2(particleDataPtr->mWidth(113)); // Allow showers in decays to qqbar/gg/ggg/gammagg. doFSRinDecays = settings.flag("ParticleDecays:FSRinDecays"); doGammaRad = settings.flag("ParticleDecays:allowPhotonRadiation"); // Use standard decays or dedicated tau decay package sophisticatedTau = settings.mode("ParticleDecays:sophisticatedTau"); // Initialize the dedicated tau decay handler. if (sophisticatedTau) tauDecayer.init(infoPtr, &settings, particleDataPtr, rndmPtr, couplingsPtr); } //-------------------------------------------------------------------------- // Decay a particle; main method. bool ParticleDecays::decay( int iDec, Event& event) { // Check whether a decay is allowed, given the upcoming decay vertex. Particle& decayer = event[iDec]; hasPartons = false; keepPartons = false; if (limitDecay && !checkVertex(decayer)) return true; // Do not allow resonance decays (beyond handling capability). if (decayer.isResonance()) { infoPtr->errorMsg("Warning in ParticleDecays::decay: " "resonance left undecayed"); return true; } // Fill the decaying particle in slot 0 of arrays. idDec = decayer.id(); iProd.resize(0); idProd.resize(0); mProd.resize(0); iProd.push_back( iDec ); idProd.push_back( idDec ); mProd.push_back( decayer.m() ); // Check for oscillations B0 <-> B0bar or B_s0 <-> B_s0bar. bool hasOscillated = (abs(idDec) == 511 || abs(idDec) == 531) ? oscillateB(decayer) : false; if (hasOscillated) {idDec = - idDec; idProd[0] = idDec;} // Particle data for decaying particle. decDataPtr = &decayer.particleDataEntry(); // Optionally send on to external decay program. bool doneExternally = false; if (decDataPtr->doExternalDecay()) { pProd.resize(0); pProd.push_back(decayer.p()); doneExternally = decayHandlePtr->decay(idProd, mProd, pProd, iDec, event); // If it worked, then store the decay products in the event record. if (doneExternally) { mult = idProd.size() - 1; int status = (hasOscillated) ? 94 : 93; for (int i = 1; i <= mult; ++i) { int iPos = event.append( idProd[i], status, iDec, 0, 0, 0, 0, 0, pProd[i], mProd[i]); iProd.push_back( iPos); } // Also mark mother decayed and store daughters. event[iDec].statusNeg(); event[iDec].daughters( iProd[1], iProd[mult]); } } // Check if the particle is tau and let the special tau decayer handle it. if (decayer.idAbs() == 15 && !doneExternally && sophisticatedTau) { doneExternally = tauDecayer.decay(iDec, event); if (doneExternally) return true; } // Now begin normal internal decay treatment. if (!doneExternally) { // Allow up to ten tries to pick a channel. if (!decDataPtr->preparePick(idDec, decayer.m())) return false; bool foundChannel = false; bool hasStored = false; for (int iTryChannel = 0; iTryChannel < NTRYDECAY; ++iTryChannel) { // Remove previous failed channel. if (hasStored) event.popBack(mult); hasStored = false; // Pick new channel. Read out basics. DecayChannel& channel = decDataPtr->pickChannel(); meMode = channel.meMode(); keepPartons = (meMode > 90 && meMode <= 100); mult = channel.multiplicity(); // Allow up to ten tries for each channel (e.g with different masses). bool foundMode = false; for (int iTryMode = 0; iTryMode < NTRYDECAY; ++iTryMode) { idProd.resize(1); mProd.resize(1); scale = 0.; // Extract and store the decay products in local arrays. hasPartons = false; for (int i = 0; i < mult; ++i) { int idNow = channel.product(i); int idAbs = abs(idNow); if ( idAbs < 10 || idAbs == 21 || idAbs == 81 || idAbs == 82 || idAbs == 83 || (idAbs > 1000 && idAbs < 10000 && (idAbs/10)%10 == 0) ) hasPartons = true; if (idDec < 0 && particleDataPtr->hasAnti(idNow)) idNow = -idNow; double mNow = particleDataPtr->mSel(idNow); idProd.push_back( idNow); mProd.push_back( mNow); } // Decays into partons usually translate into hadrons. if (hasPartons && !keepPartons && !pickHadrons()) continue; // Need to set colour flow if explicit decay to partons. cols.resize(0); acols.resize(0); for (int i = 0; i <= mult; ++i) { cols.push_back(0); acols.push_back(0); } if (hasPartons && keepPartons && !setColours(event)) continue; // Check that enough phase space for decay. if (mult > 1) { double mDiff = mProd[0]; for (int i = 1; i <= mult; ++i) mDiff -= mProd[i]; if (mDiff < mSafety) continue; } // End of inner trial loops. Check if succeeded or not. foundMode = true; break; } if (!foundMode) continue; // Store decay products in the event record. int status = (hasOscillated) ? 92 : 91; for (int i = 1; i <= mult; ++i) { int iPos = event.append( idProd[i], status, iDec, 0, 0, 0, cols[i], acols[i], Vec4(0., 0., 0., 0.), mProd[i], scale); iProd.push_back( iPos); } hasStored = true; // Pick mass of Dalitz decay. Temporarily change multiplicity. if ( (meMode == 11 || meMode == 12 || meMode == 13) && !dalitzMass() ) continue; // Do a decay, split by multiplicity. bool decayed = false; if (mult == 1) decayed = oneBody(event); else if (mult == 2) decayed = twoBody(event); else if (mult == 3) decayed = threeBody(event); else decayed = mGenerator(event); if (!decayed) continue; // Kinematics of gamma* -> l- l+ in Dalitz decay. Restore multiplicity. if (meMode == 11 || meMode == 12 || meMode == 13) dalitzKinematics(event); // End of outer trial loops. foundChannel = true; break; } // If the decay worked, then mark mother decayed and store daughters. if (foundChannel) { event[iDec].statusNeg(); event[iDec].daughters( iProd[1], iProd[mult]); // Else remove unused daughters and return failure. } else { if (hasStored) event.popBack(mult); infoPtr->errorMsg("Error in ParticleDecays::decay: " "failed to find workable decay channel"); return false; } // Now finished normal internal decay treatment. } // Set decay vertex when this is displaced. if (event[iDec].hasVertex() || event[iDec].tau() > 0.) { Vec4 vDec = event[iDec].vDec(); for (int i = 1; i <= mult; ++i) event[iProd[i]].vProd( vDec ); } // Set lifetime of daughters. for (int i = 1; i <= mult; ++i) event[iProd[i]].tau( event[iProd[i]].tau0() * rndmPtr->exp() ); // In a decay explicitly to partons then optionally do a shower, // and always flag that partonic system should be fragmented. if (hasPartons && keepPartons && doFSRinDecays) timesDecPtr->shower( iProd[1], iProd.back(), event, mProd[0]); // Photon radiation implemented only for two-body decay to leptons. else if (doGammaRad && mult == 2 && event[iProd[1]].isLepton() && event[iProd[2]].isLepton()) timesDecPtr->showerQED( iProd[1], iProd[2], event, mProd[0]); // For Hidden Valley particles also allow leptons to shower. else if (event[iDec].idAbs() > 4900000 && event[iDec].idAbs() < 5000000 && doFSRinDecays && mult == 2 && event[iProd[1]].isLepton()) { event[iProd[1]].scale(mProd[0]); event[iProd[2]].scale(mProd[0]); timesDecPtr->shower( iProd[1], iProd.back(), event, mProd[0]); } // Done. return true; } //-------------------------------------------------------------------------- // Check whether a decay is allowed, given the upcoming decay vertex. bool ParticleDecays::checkVertex(Particle& decayer) { // Check whether any of the conditions are not fulfilled. if (limitTau0 && decayer.tau0() > tau0Max) return false; if (limitTau && decayer.tau() > tauMax) return false; if (limitRadius && pow2(decayer.xDec()) + pow2(decayer.yDec()) + pow2(decayer.zDec()) > pow2(rMax)) return false; if (limitCylinder && (pow2(decayer.xDec()) + pow2(decayer.yDec()) > pow2(xyMax) || abs(decayer.zDec()) > zMax) ) return false; // Done. return true; } //-------------------------------------------------------------------------- // Check for oscillations B0 <-> B0bar or B_s0 <-> B_s0bar. bool ParticleDecays::oscillateB(Particle& decayer) { // Extract relevant information and decide. if (!mixB) return false; double xBmix = (abs(decayer.id()) == 511) ? xBdMix : xBsMix; double tau = decayer.tau(); double tau0 = decayer.tau0(); double probosc = pow2(sin(0.5 * xBmix * tau / tau0)); return (probosc > rndmPtr->flat()); } //-------------------------------------------------------------------------- // Do a one-body decay. (Rare; e.g. for K0 -> K0_short.) bool ParticleDecays::oneBody(Event& event) { // References to the particles involved. Particle& decayer = event[iProd[0]]; Particle& prod = event[iProd[1]]; // Set momentum and expand mother information. prod.p( decayer.p() ); prod.m( decayer.m() ); prod.mother2( iProd[0] ); // Done. return true; } //-------------------------------------------------------------------------- // Do a two-body decay. bool ParticleDecays::twoBody(Event& event) { // References to the particles involved. Particle& decayer = event[iProd[0]]; Particle& prod1 = event[iProd[1]]; Particle& prod2 = event[iProd[2]]; // Masses. double m0 = mProd[0]; double m1 = mProd[1]; double m2 = mProd[2]; // Energies and absolute momentum in the rest frame. if (m1 + m2 + mSafety > m0) return false; double e1 = 0.5 * (m0*m0 + m1*m1 - m2*m2) / m0; double e2 = 0.5 * (m0*m0 + m2*m2 - m1*m1) / m0; double pAbs = 0.5 * sqrtpos( (m0 - m1 - m2) * (m0 + m1 + m2) * (m0 + m1 - m2) * (m0 - m1 + m2) ) / m0; // When meMode = 2, for V -> PS2 + PS3 (V = vector, pseudoscalar), // need to check if production is PS0 -> PS1/gamma + V. int iMother = event[iProd[0]].mother1(); int idSister = 0; if (meMode == 2) { if (iMother <= 0 || iMother >= iProd[0]) meMode = 0; else { int iDaughter1 = event[iMother].daughter1(); int iDaughter2 = event[iMother].daughter2(); if (iDaughter2 != iDaughter1 + 1) meMode = 0; else { int idMother = abs( event[iMother].id() ); if (idMother <= 100 || idMother%10 !=1 || (idMother/1000)%10 != 0) meMode = 0; else { int iSister = (iProd[0] == iDaughter1) ? iDaughter2 : iDaughter1; idSister = abs( event[iSister].id() ); if ( (idSister <= 100 || idSister%10 !=1 || (idSister/1000)%10 != 0) && idSister != 22) meMode = 0; } } } } // Begin loop over matrix-element corrections. double wtME, wtMEmax; int loop = 0; do { wtME = 1.; wtMEmax = 1.; ++loop; // Isotropic angles give three-momentum. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(1. - cosTheta*cosTheta); double phi = 2. * M_PI * rndmPtr->flat(); double pX = pAbs * sinTheta * cos(phi); double pY = pAbs * sinTheta * sin(phi); double pZ = pAbs * cosTheta; // Fill four-momenta and boost them away from mother rest frame. prod1.p( pX, pY, pZ, e1); prod2.p( -pX, -pY, -pZ, e2); prod1.bst( decayer.p(), decayer.m() ); prod2.bst( decayer.p(), decayer.m() ); // Matrix element for PS0 -> PS1 + V1 -> PS1 + PS2 + PS3 of form // cos**2(theta02) in V1 rest frame, and for PS0 -> gamma + V1 // -> gamma + PS2 + PS3 of form sin**2(theta02). if (meMode == 2) { double p10 = decayer.p() * event[iMother].p(); double p12 = decayer.p() * prod1.p(); double p02 = event[iMother].p() * prod1.p(); double s0 = pow2(event[iMother].m()); double s1 = pow2(decayer.m()); double s2 = pow2(prod1.m()); if (idSister != 22) wtME = pow2(p10 * p12 - s1 * p02); else wtME = s1 * (2. * p10 * p12 * p02 - s1 * p02*p02 - s0 * p12*p12 - s2 * p10*p10 + s1 * s0 * s2); wtME = max( wtME, 1e-6 * s1*s1 * s0 * s2); wtMEmax = (p10*p10 - s1 * s0) * (p12*p12 - s1 * s2); } // Break out of loop if no sensible ME weight. if(loop > NTRYMEWT) { infoPtr->errorMsg("ParticleDecays::twoBody: " "caught in infinite ME weight loop"); wtME = abs(wtMEmax); } // If rejected, try again with new invariant masses. } while ( wtME < rndmPtr->flat() * wtMEmax ); // Done. return true; } //-------------------------------------------------------------------------- // Do a three-body decay (except Dalitz decays). bool ParticleDecays::threeBody(Event& event) { // References to the particles involved. Particle& decayer = event[iProd[0]]; Particle& prod1 = event[iProd[1]]; Particle& prod2 = event[iProd[2]]; Particle& prod3 = event[iProd[3]]; // Mother and sum daughter masses. Fail if too close. double m0 = mProd[0]; double m1 = mProd[1]; double m2 = mProd[2]; double m3 = mProd[3]; double mSum = m1 + m2 + m3; double mDiff = m0 - mSum; if (mDiff < mSafety) return false; // Kinematical limits for 2+3 mass. Maximum phase-space weight. double m23Min = m2 + m3; double m23Max = m0 - m1; double p1Max = 0.5 * sqrtpos( (m0 - m1 - m23Min) * (m0 + m1 + m23Min) * (m0 + m1 - m23Min) * (m0 - m1 + m23Min) ) / m0; double p23Max = 0.5 * sqrtpos( (m23Max - m2 - m3) * (m23Max + m2 + m3) * (m23Max + m2 - m3) * (m23Max - m2 + m3) ) / m23Max; double wtPSmax = 0.5 * p1Max * p23Max; // Begin loop over matrix-element corrections. double wtME, wtMEmax, wtPS, m23, p1Abs, p23Abs; do { wtME = 1.; wtMEmax = 1.; // Pick an intermediate mass m23 flat in the allowed range. do { m23 = m23Min + rndmPtr->flat() * mDiff; // Translate into relative momenta and find phase-space weight. p1Abs = 0.5 * sqrtpos( (m0 - m1 - m23) * (m0 + m1 + m23) * (m0 + m1 - m23) * (m0 - m1 + m23) ) / m0; p23Abs = 0.5 * sqrtpos( (m23 - m2 - m3) * (m23 + m2 + m3) * (m23 + m2 - m3) * (m23 - m2 + m3) ) / m23; wtPS = p1Abs * p23Abs; // If rejected, try again with new invariant masses. } while ( wtPS < rndmPtr->flat() * wtPSmax ); // Set up m23 -> m2 + m3 isotropic in its rest frame. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(1. - cosTheta*cosTheta); double phi = 2. * M_PI * rndmPtr->flat(); double pX = p23Abs * sinTheta * cos(phi); double pY = p23Abs * sinTheta * sin(phi); double pZ = p23Abs * cosTheta; double e2 = sqrt( m2*m2 + p23Abs*p23Abs); double e3 = sqrt( m3*m3 + p23Abs*p23Abs); prod2.p( pX, pY, pZ, e2); prod3.p( -pX, -pY, -pZ, e3); // Set up m0 -> m1 + m23 isotropic in its rest frame. cosTheta = 2. * rndmPtr->flat() - 1.; sinTheta = sqrt(1. - cosTheta*cosTheta); phi = 2. * M_PI * rndmPtr->flat(); pX = p1Abs * sinTheta * cos(phi); pY = p1Abs * sinTheta * sin(phi); pZ = p1Abs * cosTheta; double e1 = sqrt( m1*m1 + p1Abs*p1Abs); double e23 = sqrt( m23*m23 + p1Abs*p1Abs); prod1.p( pX, pY, pZ, e1); // Boost 2 + 3 to the 0 rest frame. Vec4 p23( -pX, -pY, -pZ, e23); prod2.bst( p23, m23 ); prod3.bst( p23, m23 ); // Matrix-element weight for omega/phi -> pi+ pi- pi0. if (meMode == 1) { double p1p2 = prod1.p() * prod2.p(); double p1p3 = prod1.p() * prod3.p(); double p2p3 = prod2.p() * prod3.p(); wtME = pow2(m1 * m2 * m3) - pow2(m1 * p2p3) - pow2(m2 * p1p3) - pow2(m3 * p1p2) + 2. * p1p2 * p1p3 * p2p3; wtMEmax = pow3(m0 * m0) / 150.; // Effective matrix element for nu spectrum in tau -> nu + hadrons. } else if (meMode == 21) { double x1 = 2. * prod1.e() / m0; wtME = x1 * (3. - 2. * x1); double xMax = min( 0.75, 2. * (1. - mSum / m0) ); wtMEmax = xMax * (3. - 2. * xMax); // Matrix element for weak decay (only semileptonic for c and b). } else if ((meMode == 22 || meMode == 23) && prod1.isLepton()) { wtME = m0 * prod1.e() * (prod2.p() * prod3.p()); wtMEmax = min( pow4(m0) / 16., m0 * (m0 - m1 - m2) * (m0 - m1 - m3) * (m0 - m2 - m3) ); // Effective matrix element for weak decay to hadrons (B -> D, D -> K). } else if (meMode == 22 || meMode == 23) { double x1 = 2. * prod1.pAbs() / m0; wtME = x1 * (3. - 2. * x1); double xMax = min( 0.75, 2. * (1. - mSum / m0) ); wtMEmax = xMax * (3. - 2. * xMax); // Effective matrix element for gamma spectrum in B -> gamma + hadrons. } else if (meMode == 31) { double x1 = 2. * prod1.e() / m0; wtME = pow3(x1); double x1Max = 1. - pow2(mSum / m0); wtMEmax = pow3(x1Max); // Matrix-element weight for "onium" -> g + g + g or gamma + g + g. } else if (meMode == 92) { double x1 = 2. * prod1.e() / m0; double x2 = 2. * prod2.e() / m0; double x3 = 2. * prod3.e() / m0; wtME = pow2( (1. - x1) / (x2 * x3) ) + pow2( (1. - x2) / (x1 * x3) ) + pow2( (1. - x3) / (x1 * x2) ); wtMEmax = 2.; // For gamma + g + g require minimum mass for g + g system. if (prod1.id() == 22 && sqrt(1. - x1) * m0 < 2. * stopMass) wtME = 0.; if (prod2.id() == 22 && sqrt(1. - x2) * m0 < 2. * stopMass) wtME = 0.; if (prod3.id() == 22 && sqrt(1. - x3) * m0 < 2. * stopMass) wtME = 0.; } // If rejected, try again with new invariant masses. } while ( wtME < rndmPtr->flat() * wtMEmax ); // Boost 1 + 2 + 3 to the current frame. prod1.bst( decayer.p(), decayer.m() ); prod2.bst( decayer.p(), decayer.m() ); prod3.bst( decayer.p(), decayer.m() ); // Done. return true; } //-------------------------------------------------------------------------- // Do a multibody decay using the M-generator algorithm. bool ParticleDecays::mGenerator(Event& event) { // Mother and sum daughter masses. Fail if too close or inconsistent. double m0 = mProd[0]; double mSum = mProd[1]; for (int i = 2; i <= mult; ++i) mSum += mProd[i]; double mDiff = m0 - mSum; if (mDiff < mSafety) return false; // Begin setup of intermediate invariant masses. mInv.resize(0); for (int i = 0; i <= mult; ++i) mInv.push_back( mProd[i]); // Calculate the maximum weight in the decay. double wtPS, wtME, wtMEmax; double wtPSmax = 1. / WTCORRECTION[mult]; double mMax = mDiff + mProd[mult]; double mMin = 0.; for (int i = mult - 1; i > 0; --i) { mMax += mProd[i]; mMin += mProd[i+1]; double mNow = mProd[i]; wtPSmax *= 0.5 * sqrtpos( (mMax - mMin - mNow) * (mMax + mMin + mNow) * (mMax + mMin - mNow) * (mMax - mMin + mNow) ) / mMax; } // Begin loop over matrix-element corrections. do { wtME = 1.; wtMEmax = 1.; // Begin loop to find the set of intermediate invariant masses. do { wtPS = 1.; // Find and order random numbers in descending order. rndmOrd.resize(0); rndmOrd.push_back(1.); for (int i = 1; i < mult - 1; ++i) { double rndm = rndmPtr->flat(); rndmOrd.push_back(rndm); for (int j = i - 1; j > 0; --j) { if (rndm > rndmOrd[j]) swap( rndmOrd[j], rndmOrd[j+1] ); else break; } } rndmOrd.push_back(0.); // Translate into intermediate masses and find weight. for (int i = mult - 1; i > 0; --i) { mInv[i] = mInv[i+1] + mProd[i] + (rndmOrd[i-1] - rndmOrd[i]) * mDiff; wtPS *= 0.5 * sqrtpos( (mInv[i] - mInv[i+1] - mProd[i]) * (mInv[i] + mInv[i+1] + mProd[i]) * (mInv[i] + mInv[i+1] - mProd[i]) * (mInv[i] - mInv[i+1] + mProd[i]) ) / mInv[i]; } // If rejected, try again with new invariant masses. } while ( wtPS < rndmPtr->flat() * wtPSmax ); // Perform two-particle decays in the respective rest frame. pInv.resize(mult + 1); for (int i = 1; i < mult; ++i) { double pAbs = 0.5 * sqrtpos( (mInv[i] - mInv[i+1] - mProd[i]) * (mInv[i] + mInv[i+1] + mProd[i]) * (mInv[i] + mInv[i+1] - mProd[i]) * (mInv[i] - mInv[i+1] + mProd[i]) ) / mInv[i]; // Isotropic angles give three-momentum. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(1. - cosTheta*cosTheta); double phi = 2. * M_PI * rndmPtr->flat(); double pX = pAbs * sinTheta * cos(phi); double pY = pAbs * sinTheta * sin(phi); double pZ = pAbs * cosTheta; // Calculate energies, fill four-momenta. double eHad = sqrt( mProd[i]*mProd[i] + pAbs*pAbs); double eInv = sqrt( mInv[i+1]*mInv[i+1] + pAbs*pAbs); event[iProd[i]].p( pX, pY, pZ, eHad); pInv[i+1].p( -pX, -pY, -pZ, eInv); } // Boost decay products to the mother rest frame. event[iProd[mult]].p( pInv[mult] ); for (int iFrame = mult - 1; iFrame > 1; --iFrame) for (int i = iFrame; i <= mult; ++i) event[iProd[i]].bst( pInv[iFrame], mInv[iFrame]); // Effective matrix element for nu spectrum in tau -> nu + hadrons. if (meMode == 21 && event[iProd[1]].isLepton()) { double x1 = 2. * event[iProd[1]].e() / m0; wtME = x1 * (3. - 2. * x1); double xMax = min( 0.75, 2. * (1. - mSum / m0) ); wtMEmax = xMax * (3. - 2. * xMax); // Effective matrix element for weak decay (only semileptonic for c and b). // Particles 4 onwards should be made softer explicitly? } else if ((meMode == 22 || meMode == 23) && event[iProd[1]].isLepton()) { Vec4 pRest = event[iProd[3]].p(); for (int i = 4; i <= mult; ++i) pRest += event[iProd[i]].p(); wtME = m0 * event[iProd[1]].e() * (event[iProd[2]].p() * pRest); for (int i = 4; i <= mult; ++i) wtME *= exp(- event[iProd[i]].pAbs2() / pow2(sigmaSoft) ); wtMEmax = pow4(m0) / 16.; // Effective matrix element for weak decay to hadrons (B -> D, D -> K). } else if (meMode == 22 || meMode == 23) { double x1 = 2. * event[iProd[1]].pAbs() / m0; wtME = x1 * (3. - 2. * x1); double xMax = min( 0.75, 2. * (1. - mSum / m0) ); wtMEmax = xMax * (3. - 2. * xMax); // Effective matrix element for gamma spectrum in B -> gamma + hadrons. } else if (meMode == 31) { double x1 = 2. * event[iProd[1]].e() / m0; wtME = pow3(x1); double x1Max = 1. - pow2(mSum / m0); wtMEmax = pow3(x1Max); } // If rejected, try again with new invariant masses. } while ( wtME < rndmPtr->flat() * wtMEmax ); // Boost decay products to the current frame. pInv[1].p( event[iProd[0]].p() ); for (int i = 1; i <= mult; ++i) event[iProd[i]].bst( pInv[1], mInv[1] ); // Done. return true; } //-------------------------------------------------------------------------- // Select mass of lepton pair in a Dalitz decay. bool ParticleDecays::dalitzMass() { // Mother and sum daughter masses. double mSum1 = 0; for (int i = 1; i <= mult - 2; ++i) mSum1 += mProd[i]; if (meMode == 13) mSum1 *= MSAFEDALITZ; double mSum2 = MSAFEDALITZ * (mProd[mult -1] + mProd[mult]); double mDiff = mProd[0] - mSum1 - mSum2; // Fail if too close or inconsistent. if (mDiff < mSafety) return false; if (idProd[mult - 1] + idProd[mult] != 0 || mProd[mult - 1] != mProd[mult]) { infoPtr->errorMsg("Error in ParticleDecays::dalitzMass:" " inconsistent flavour/mass assignments"); return false; } if ( meMode == 13 && (idProd[1] + idProd[2] != 0 || mProd[1] != mProd[2]) ) { infoPtr->errorMsg("Error in ParticleDecays::dalitzMass:" " inconsistent flavour/mass assignments"); return false; } // Case 1: one Dalitz pair. if (meMode == 11 || meMode == 12) { // Kinematical limits for gamma* squared mass. double sGamMin = pow2(mSum2); double sGamMax = pow2(mProd[0] - mSum1); // Select virtual gamma squared mass. Guessed form for meMode == 12. double sGam, wtGam; int loop = 0; do { if (++loop > NTRYDALITZ) return false; sGam = sGamMin * pow( sGamMax / sGamMin, rndmPtr->flat() ); wtGam = (1. + 0.5 * sGamMin / sGam) * sqrt(1. - sGamMin / sGam) * pow3(1. - sGam / sGamMax) * sRhoDal * (sRhoDal + wRhoDal) / ( pow2(sGam - sRhoDal) + sRhoDal * wRhoDal ); } while ( wtGam < rndmPtr->flat() ); // Store results in preparation for doing a one-less-body decay. --mult; mProd[mult] = sqrt(sGam); // Case 2: two Dalitz pairs. } else { // Kinematical limits for 1 + 2 and 3 + 4 gamma* masses. double s0 = pow2(mProd[0]); double s12Min = pow2(mSum1); double s12Max = pow2(mProd[0] - mSum2); double s34Min = pow2(mSum2); double s34Max = pow2(mProd[0] - mSum1); // Select virtual gamma squared masses. Guessed form for meMode == 13. double s12, s34, wt12, wt34, wtPAbs, wtAll; int loop = 0; do { if (++loop > NTRYDALITZ) return false; s12 = s12Min * pow( s12Max / s12Min, rndmPtr->flat() ); wt12 = (1. + 0.5 * s12Min / s12) * sqrt(1. - s12Min / s12) * sRhoDal * (sRhoDal + wRhoDal) / ( pow2(s12 - sRhoDal) + sRhoDal * wRhoDal ); s34 = s34Min * pow( s34Max / s34Min, rndmPtr->flat() ); wt34 = (1. + 0.5 * s34Min / s34) * sqrt(1. - s34Min / s34) * sRhoDal * (sRhoDal + wRhoDal) / ( pow2(s34 - sRhoDal) + sRhoDal * wRhoDal ); wtPAbs = sqrtpos( pow2(1. - (s12 + s34)/ s0) - 4. * s12 * s34 / (s0 * s0) ); wtAll = wt12 * wt34 * pow3(wtPAbs); if (wtAll > 1.) infoPtr->errorMsg( "Error in ParticleDecays::dalitzMass: weight > 1"); } while (wtAll < rndmPtr->flat()); // Store results in preparation for doing a two-body decay. mult = 2; mProd[1] = sqrt(s12); mProd[2] = sqrt(s34); } // Done. return true; } //-------------------------------------------------------------------------- // Do kinematics of gamma* -> l- l+ in Dalitz decay. bool ParticleDecays::dalitzKinematics(Event& event) { // Restore multiplicity. int nDal = (meMode < 13) ? 1 : 2; mult += nDal; // Loop over one or two lepton pairs. for (int iDal = 0; iDal < nDal; ++iDal) { // References to the particles involved. Particle& decayer = event[iProd[0]]; Particle& prodA = (iDal == 0) ? event[iProd[mult - 1]] : event[iProd[1]]; Particle& prodB = (iDal == 0) ? event[iProd[mult]] : event[iProd[2]]; // Reconstruct required rotations and boosts backwards. Vec4 pDec = decayer.p(); int iGam = (meMode < 13) ? mult - 1 : 2 - iDal; Vec4 pGam = event[iProd[iGam]].p(); pGam.bstback( pDec, decayer.m() ); double phiGam = pGam.phi(); pGam.rot( 0., -phiGam); double thetaGam = pGam.theta(); pGam.rot( -thetaGam, 0.); // Masses and phase space in gamma* rest frame. double mGam = (meMode < 13) ? mProd[mult - 1] : mProd[2 - iDal]; double mA = prodA.m(); double mB = prodB.m(); double mGamMin = MSAFEDALITZ * (mA + mB); double mGamRat = pow2(mGamMin / mGam); double pGamAbs = 0.5 * sqrtpos( (mGam - mA - mB) * (mGam + mA + mB) ); // Set up decay in gamma* rest frame, reference along +z axis. double cosTheta, cos2Theta; do { cosTheta = 2. * rndmPtr->flat() - 1.; cos2Theta = cosTheta * cosTheta; } while ( 1. + cos2Theta + mGamRat * (1. - cos2Theta) < 2. * rndmPtr->flat() ); double sinTheta = sqrt(1. - cosTheta*cosTheta); double phi = 2. * M_PI * rndmPtr->flat(); double pX = pGamAbs * sinTheta * cos(phi); double pY = pGamAbs * sinTheta * sin(phi); double pZ = pGamAbs * cosTheta; double eA = sqrt( mA*mA + pGamAbs*pGamAbs); double eB = sqrt( mB*mB + pGamAbs*pGamAbs); prodA.p( pX, pY, pZ, eA); prodB.p( -pX, -pY, -pZ, eB); // Boost to lab frame. prodA.bst( pGam, mGam); prodB.bst( pGam, mGam); prodA.rot( thetaGam, phiGam); prodB.rot( thetaGam, phiGam); prodA.bst( pDec, decayer.m() ); prodB.bst( pDec, decayer.m() ); } // Done. return true; } //-------------------------------------------------------------------------- // Translate a partonic content into a set of actual hadrons. bool ParticleDecays::pickHadrons() { // Find partonic decay products. Rest are known id's, mainly hadrons, // when necessary shuffled to beginning of idProd list. idPartons.resize(0); int nPartons = 0; int nKnown = 0; bool closedGLoop = false; for (int i = 1; i <= mult; ++i) { int idAbs = abs(idProd[i]); if ( idAbs < 9 || (idAbs > 1000 && idAbs < 10000 && (idAbs/10)%10 == 0) || idAbs == 81 || idAbs == 82 || idAbs == 83) { ++nPartons; idPartons.push_back(idProd[i]); if (idAbs == 83) closedGLoop = true; } else { ++nKnown; if (nPartons > 0) { idProd[nKnown] = idProd[i]; mProd[nKnown] = mProd[i]; } } } // Replace generic spectator flavour code by the actual one. for (int i = 0; i < nPartons; ++i) { int idPart = idPartons[i]; int idNew = idPart; if (idPart == 81) { int idAbs = abs(idDec); if ( (idAbs/1000)%10 == 0 ) { idNew = -(idAbs/10)%10; if ((idAbs/100)%2 == 1) idNew = -idNew; } else if ( (idAbs/100)%10 >= (idAbs/10)%10 ) idNew = 100 * ((idAbs/10)%100) + 3; else idNew = 1000 * ((idAbs/10)%10) + 100 * ((idAbs/100)%10) + 1; if (idDec < 0) idNew = -idNew; // Replace generic random flavour by a randomly selected one. } else if (idPart == 82 || idPart == 83) { double mFlav; do { int idDummy = -flavSelPtr->pickLightQ(); FlavContainer flavDummy(idDummy, idPart - 82); do idNew = flavSelPtr->pick(flavDummy).id; while (idNew == 0); mFlav = particleDataPtr->constituentMass(idNew); } while (2. * mFlav + stopMass > mProd[0]); } else if (idPart == -82 || idPart == -83) { idNew = -idPartons[i-1]; } idPartons[i] = idNew; } // Determine whether fixed multiplicity or to be selected at random. int nMin = max( 2, nKnown + nPartons / 2); if (meMode == 23) nMin = 3; if (meMode > 41 && meMode <= 50) nMin = meMode - 40; if (meMode > 51 && meMode <= 60) nMin = meMode - 50; int nFix = 0; if (meMode == 0) nFix = nMin; if (meMode == 11) nFix = 3; if (meMode == 12) nFix = 4; if (meMode > 61 && meMode <= 70) nFix = meMode - 60; if (meMode > 71 && meMode <= 80) nFix = meMode - 70; if (nFix > 0 && nKnown + nPartons/2 > nFix) return false; // Initial values for loop to set new hadronic content. int nFilled, nTotal, nNew, nSpec, nLeft; double mDiff; int nTry = 0; bool diquarkClash = false; bool usedChannel = false; // Begin loop; interrupt if multiple tries fail. do { ++nTry; if (nTry > NTRYPICK) return false; // Initialize variables inside new try. nFilled = nKnown + 1; idProd.resize(nFilled); mProd.resize(nFilled); nTotal = nKnown; nSpec = 0; nLeft = nPartons; mDiff = mProd[0]; for (int i = 1; i < nFilled; ++i) mDiff -= mProd[i]; diquarkClash = false; usedChannel = false; // For weak decays collapse spectators to one particle. if ( (meMode == 22 || meMode == 23) && nLeft > 1) { FlavContainer flav1( idPartons[nPartons - 2] ); FlavContainer flav2( idPartons[nPartons - 1] ); int idHad; do idHad = flavSelPtr->combine( flav1, flav2); while (idHad == 0); double mHad = particleDataPtr->mSel(idHad); mDiff -= mHad; idProd.push_back( idHad); mProd.push_back( mHad); ++nFilled; nSpec = 1; nLeft -= 2; } // If there are partons left, then determine how many hadrons to pick. if (nLeft > 0) { // For B -> gamma + X use geometrical distribution. if (meMode == 31) { double geom = rndmPtr->flat(); nTotal = 1; do { ++nTotal; geom *= 2.; } while (geom < 1. && nTotal < 10); // Calculate mass excess and from there average multiplicity. } else if (nFix == 0) { double multIncreaseNow = (meMode == 23) ? multIncreaseWeak : multIncrease; double mDiffPS = mDiff; for (int i = 0; i < nLeft; ++i) mDiffPS -= particleDataPtr->constituentMass( idPartons[i] ); double average = 0.5 * (nKnown + nSpec) + 0.25 * nPartons + multIncreaseNow * log( max( 1.1, mDiffPS / multRefMass ) ); if (closedGLoop) average += multGoffset; // Pick multiplicity according to Poissonian. double value = 1.; double sum = 1.; for (int nNow = nMin + 1; nNow <= 10; ++nNow) { value *= average / nNow; sum += value; } nTotal = nMin; value = 1.; sum *= rndmPtr->flat(); sum -= value; if (sum > 0.) do { ++nTotal; value *= average / nTotal; sum -= value; } while (sum > 0. && nTotal < 10); // Alternatively predetermined multiplicity. } else { nTotal = nFix; } nNew = nTotal - nKnown - nSpec; // Set up ends of fragmented system, as copy of idPartons. flavEnds.resize(0); for (int i = 0; i < nLeft; ++i) { flavEnds.push_back( FlavContainer(idPartons[i]) ); if (abs(idPartons[i]) > 100) flavSelPtr->assignPopQ( flavEnds[i] ); } // Fragment off at random, but save nLeft/2 for final recombination. if (nNew > nLeft/2) { FlavContainer flavNew; int idHad; for (int i = 0; i < nNew - nLeft/2; ++i) { // When four quarks consider last one to be spectator. int iEnd = int( (nLeft - 1.) * rndmPtr->flat() ); // Pick new flavour and form a new hadron. do { flavNew = flavSelPtr->pick( flavEnds[iEnd] ); idHad = flavSelPtr->combine( flavEnds[iEnd], flavNew); } while (idHad == 0); // Store new hadron and endpoint flavour. idProd.push_back( idHad); flavEnds[iEnd].anti(flavNew); } } // When only two quarks left, combine to form final hadron. if (nLeft == 2) { int idHad; if ( abs(flavEnds[0].id) > 8 && abs(flavEnds[1].id) > 8) diquarkClash = true; else { do idHad = flavSelPtr->combine( flavEnds[0], flavEnds[1]); while (idHad == 0); idProd.push_back( idHad); } // If four quarks, decide how to pair them up. } else { int iEnd1 = 0; int iEnd2 = 1; int iEnd3 = 2; int iEnd4 = 3; if ( rndmPtr->flat() < colRearrange) iEnd2 = 3; int relColSign = ( (flavEnds[iEnd1].id > 0 && flavEnds[iEnd1].id < 9) || flavEnds[iEnd1].id < -10 ) ? 1 : -1; if ( (flavEnds[iEnd2].id < 0 && flavEnds[iEnd2].id > -9) || flavEnds[iEnd2].id > 10 ) relColSign *= -1; if (relColSign == 1) iEnd2 = 2; if (iEnd2 == 2) iEnd3 = 1; if (iEnd2 == 3) iEnd4 = 1; // Then combine to get final two hadrons. int idHad; if ( abs(flavEnds[iEnd1].id) > 8 && abs(flavEnds[iEnd2].id) > 8) diquarkClash = true; else { do idHad = flavSelPtr->combine( flavEnds[iEnd1], flavEnds[iEnd2]); while (idHad == 0); idProd.push_back( idHad); } if ( abs(flavEnds[iEnd3].id) > 8 && abs(flavEnds[iEnd4].id) > 8) diquarkClash = true; else { do idHad = flavSelPtr->combine( flavEnds[iEnd3], flavEnds[iEnd4]); while (idHad == 0); idProd.push_back( idHad); } } // Find masses of the new hadrons. for (int i = nFilled; i < int(idProd.size()) ; ++i) { double mHad = particleDataPtr->mSel(idProd[i]); mProd.push_back( mHad); mDiff -= mHad; } } // Optional: check that this decay mode is not explicitly defined. if ( (meMode > 61 && meMode <= 80) && mDiff > mSafety && !diquarkClash ) { int idMatch[10], idPNow; usedChannel = false; bool matched = false; // Loop through all channels. Done if not same multiplicity. for (int i = 0; i < decDataPtr->sizeChannels(); ++i) { DecayChannel& channel = decDataPtr->channel(i); if (channel.multiplicity() != nTotal) continue; for (int k = 0; k < nTotal; ++k) idMatch[k] = channel.product(k); // Match particles one by one until fail. // Do not distinguish K0/K0bar/K0short/K0long at this stage. for (int j = 0; j < nTotal; ++j) { matched = false; idPNow = idProd[j + 1]; if (idPNow == -311 || idPNow == 130 || idPNow == 310) idPNow = 311; for (int k = 0; k < nTotal - j; ++k) if (idMatch[k] == idPNow || (idMatch[k] == -311 && idPNow == 311)) { // Compress list of unmatched when matching worked. idMatch[k] = idMatch[nTotal - 1 - j]; matched = true; break; } if (!matched) break; } // If matching worked, then chosen channel to be rejected. if (matched) {usedChannel = true; break;} } } // Keep on trying until enough phase space and no clash. } while (mDiff < mSafety || diquarkClash || usedChannel); // Update particle multiplicity. mult = idProd.size() - 1; // For Dalitz decays shuffle Dalitz pair to the end of the list. if (meMode == 11 || meMode == 12) { int iL1 = 0; int iL2 = 0; for (int i = 1; i <= mult; ++i) { if (idProd[i] == 11 || idProd[i] == 13 || idProd[i] == 15) iL1 = i; if (idProd[i] == -11 || idProd[i] == -13 || idProd[i] == -15) iL2 = i; } if (iL1 > 0 && iL2 > 0) { int idL1 = idProd[iL1]; int idL2 = idProd[iL2]; double mL1 = mProd[iL1]; double mL2 = mProd[iL2]; int iMove = 0; for (int i = 1; i <= mult; ++i) if (i != iL1 && i != iL2) { ++iMove; idProd[iMove] = idProd[i]; mProd[iMove] = mProd[i]; } idProd[mult - 1] = idL1; idProd[mult] = idL2; mProd[mult - 1] = mL1; mProd[mult] = mL2; } } // Done. return true; } //-------------------------------------------------------------------------- // Set colour flow and scale in a decay explicitly to partons. bool ParticleDecays::setColours(Event& event) { // Decay to q qbar (or qbar q). if (meMode == 91 && idProd[1] > 0 && idProd[1] < 9) { int newCol = event.nextColTag(); cols[1] = newCol; acols[2] = newCol; } else if (meMode == 91 && idProd[1] < 0 && idProd[1] > -9) { int newCol = event.nextColTag(); cols[2] = newCol; acols[1] = newCol; // Decay to g g. } else if (meMode == 91 && idProd[1] == 21) { int newCol1 = event.nextColTag(); int newCol2 = event.nextColTag(); cols[1] = newCol1; acols[1] = newCol2; cols[2] = newCol2; acols[2] = newCol1; // Decay to g g g. } else if (meMode == 92 && idProd[1] == 21 && idProd[2] == 21 && idProd[3] == 21) { int newCol1 = event.nextColTag(); int newCol2 = event.nextColTag(); int newCol3 = event.nextColTag(); cols[1] = newCol1; acols[1] = newCol2; cols[2] = newCol2; acols[2] = newCol3; cols[3] = newCol3; acols[3] = newCol1; // Decay to g g gamma: locate which is gamma. } else if (meMode == 92) { int iGlu1 = (idProd[1] == 21) ? 1 : 3; int iGlu2 = (idProd[2] == 21) ? 2 : 3; int newCol1 = event.nextColTag(); int newCol2 = event.nextColTag(); cols[iGlu1] = newCol1; acols[iGlu1] = newCol2; cols[iGlu2] = newCol2; acols[iGlu2] = newCol1; // Unknown decay mode means failure. } else return false; // Set maximum scale to be mass of decaying particle. scale = mProd[0]; // Done. return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/RHadrons.cc0000644000175000017500000014255112217346250015161 0ustar sunsun// RHadrons.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the RHadrons class. #include "Pythia8/RHadrons.h" namespace Pythia8 { //========================================================================== // The RHadrons class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. const int RHadrons::IDRHADSB[14] = { 1000512, 1000522, 1000532, 1000542, 1000552, 1005113, 1005211, 1005213, 1005223, 1005311, 1005313, 1005321, 1005323, 1005333 }; const int RHadrons::IDRHADST[14] = { 1000612, 1000622, 1000632, 1000642, 1000652, 1006113, 1006211, 1006213, 1006223, 1006311, 1006313, 1006321, 1006323, 1006333 }; // Gluino code and list of gluino R-hadron codes. const int RHadrons::IDRHADGO[38] = { 1000993, 1009113, 1009213, 1009223, 1009313, 1009323, 1009333, 1009413, 1009423, 1009433, 1009443, 1009513, 1009523, 1009533, 1009543, 1009553, 1091114, 1092114, 1092214, 1092224, 1093114, 1093214, 1093224, 1093314, 1093324, 1093334, 1094114, 1094214, 1094224, 1094314, 1094324, 1094334, 1095114, 1095214, 1095224, 1095314, 1095324, 1095334 }; // Allow a few tries for flavour selection since failure is allowed. const int RHadrons::NTRYMAX = 10; // Safety margin (in GeV) when constructing kinematics of system. const double RHadrons::MSAFETY = 0.1; // Maximal energy to borrow for gluon to insert on leg in to junction. const double RHadrons::EGBORROWMAX = 4.; //-------------------------------------------------------------------------- // Main routine to initialize R-hadron handling. bool RHadrons::init( Info* infoPtrIn, Settings& settings, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn) { // Store input pointers for future use. infoPtr = infoPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; // Flags and parameters related to R-hadron formation and decay. allowRH = settings.flag("RHadrons:allow"); maxWidthRH = settings.parm("RHadrons:maxWidth"); idRSb = settings.mode("RHadrons:idSbottom"); idRSt = settings.mode("RHadrons:idStop"); idRGo = settings.mode("RHadrons:idGluino"); setMassesRH = settings.flag("RHadrons:setMasses"); probGluinoballRH = settings.parm("RHadrons:probGluinoball"); mOffsetCloudRH = settings.parm("RHadrons:mOffsetCloud"); mCollapseRH = settings.parm("RHadrons:mCollapse"); diquarkSpin1RH = settings.parm("RHadrons:diquarkSpin1"); // Check whether sbottom, stop or gluino should form R-hadrons. allowRSb = allowRH && idRSb > 0 && (particleDataPtr->mWidth(idRSb) < maxWidthRH); allowRSt = allowRH && idRSt > 0 && (particleDataPtr->mWidth(idRSt) < maxWidthRH); allowRGo = allowRH && idRGo > 0 && (particleDataPtr->mWidth(idRGo) < maxWidthRH); allowSomeR = allowRSb || allowRSt || allowRGo; // Set nominal masses of sbottom R-mesons and R-baryons. if (allowRSb) { m0Sb = particleDataPtr->m0(idRSb); if (setMassesRH) { for (int i = 0; i < 14; ++i) { int idR = IDRHADSB[i]; double m0RHad = m0Sb + mOffsetCloudRH; m0RHad += particleDataPtr->constituentMass( (idR%100)/10); if (i > 4) m0RHad += particleDataPtr->constituentMass( (idR%1000)/100 ); particleDataPtr->m0( idR, m0RHad); } } // Set widths and lifetimes of sbottom R-hadrons. double mWidthRHad = particleDataPtr->mWidth(idRSb); double tau0RHad = particleDataPtr->tau0( idRSb); for (int i = 0; i < 14; ++i) { particleDataPtr->mWidth( IDRHADSB[i], mWidthRHad); particleDataPtr->tau0( IDRHADSB[i], tau0RHad); } } // Set nominal masses of stop R-mesons and R-baryons. if (allowRSt) { m0St = particleDataPtr->m0(idRSt); if (setMassesRH) { for (int i = 0; i < 14; ++i) { int idR = IDRHADST[i]; double m0RHad = m0St + mOffsetCloudRH; m0RHad += particleDataPtr->constituentMass( (idR%100)/10); if (i > 4) m0RHad += particleDataPtr->constituentMass( (idR%1000)/100 ); particleDataPtr->m0( idR, m0RHad); } } // Set widths and lifetimes of stop R-hadrons. double mWidthRHad = particleDataPtr->mWidth(idRSt); double tau0RHad = particleDataPtr->tau0( idRSt); for (int i = 0; i < 14; ++i) { particleDataPtr->mWidth( IDRHADST[i], mWidthRHad); particleDataPtr->tau0( IDRHADST[i], tau0RHad); } } // Set nominal masses of gluino R-glueballs, R-mesons and R-baryons. if (allowRGo) { m0Go = particleDataPtr->m0(idRGo); if (setMassesRH) { particleDataPtr->m0( IDRHADGO[0], m0Go + 2. * mOffsetCloudRH + particleDataPtr->constituentMass(21) ); for (int i = 1; i < 38; ++i) { int idR = IDRHADGO[i]; double m0RHad = m0Go + 2. * mOffsetCloudRH; m0RHad += particleDataPtr->constituentMass( (idR%1000)/100 ); m0RHad += particleDataPtr->constituentMass( (idR%100)/10); if (i > 15) m0RHad += particleDataPtr->constituentMass( (idR%10000)/1000 ); particleDataPtr->m0( idR, m0RHad); } } // Set widths and lifetimes of gluino R-hadrons. double mWidthRHad = particleDataPtr->mWidth(idRGo); double tau0RHad = particleDataPtr->tau0( idRGo); for (int i = 0; i < 38; ++i) { particleDataPtr->mWidth( IDRHADGO[i], mWidthRHad); particleDataPtr->tau0( IDRHADGO[i], tau0RHad); } } // Done. return true; } //-------------------------------------------------------------------------- // Check if a given particle can produce R-hadrons. bool RHadrons::givesRHadron( int id) { if (allowRSb && abs(id) == idRSb) return true; if (allowRSt && abs(id) == idRSt) return true; if (allowRGo && id == idRGo) return true; return false; } //-------------------------------------------------------------------------- // Produce R-hadrons by fragmenting them off from existing strings. bool RHadrons::produce( ColConfig& colConfig, Event& event) { // Check whether some sparticles are allowed to hadronize. if (!allowSomeR) return true; // Reset arrays and values. iBefRHad.resize(0); iCreRHad.resize(0); iRHadron.resize(0); iAftRHad.resize(0); isTriplet.resize(0); nRHad = 0; // Loop over event and identify hadronizing sparticles. for (int i = 0; i < event.size(); ++i) if (event[i].isFinal() && givesRHadron(event[i].id())) { iBefRHad.push_back(i); iCreRHad.push_back(i); iRHadron.push_back(0); iAftRHad.push_back(0); isTriplet.push_back(true); } nRHad = iRHadron.size(); // Done if no hadronizing sparticles. if (nRHad == 0) return true; // Max two R-hadrons. Randomize order of processing. if (nRHad > 2) { infoPtr->errorMsg("Error in RHadrons::produce: " "cannot handle more than two R-hadrons"); return false; } if (nRHad > 1 && rndmPtr->flat() > 0.5) swap( iBefRHad[0], iBefRHad[1]); // Split a system with both a sparticle and a junction. iBef = iBefRHad[0]; iSys = colConfig.findSinglet( iBef); systemPtr = &colConfig[iSys]; if (systemPtr->hasJunction && !splitOffJunction( colConfig, event)) { infoPtr->errorMsg("Error in RHadrons::produce: " "cannot handle system with junction"); return false; } if (nRHad == 2) { iBef = iBefRHad[1]; iSys = colConfig.findSinglet( iBefRHad[1]); systemPtr = &colConfig[iSys]; if (systemPtr->hasJunction && !splitOffJunction( colConfig, event)) { infoPtr->errorMsg("Error in RHadrons::produce: " "cannot handle system with junction"); return false; } } // Open up a closed gluon/gluino loop. iBef = iBefRHad[0]; iSys = colConfig.findSinglet( iBef); systemPtr = &colConfig[iSys]; if (systemPtr->isClosed && !openClosedLoop( colConfig, event)) { infoPtr->errorMsg("Error in RHadrons::produce: " "cannot open up closed gluon/gluino loop"); return false; } if (nRHad == 2) { iBef = iBefRHad[1]; iSys = colConfig.findSinglet( iBefRHad[1]); systemPtr = &colConfig[iSys]; if (systemPtr->isClosed && !openClosedLoop( colConfig, event)) { infoPtr->errorMsg("Error in RHadrons::produce: " "cannot open up closed gluon/gluino loop"); return false; } } // Split up a colour singlet system that should give two R-hadrons. if (nRHad == 2) { int iSys1 = colConfig.findSinglet( iBefRHad[0]); int iSys2 = colConfig.findSinglet( iBefRHad[1]); if (iSys2 == iSys1) { iSys = iSys1; systemPtr = &colConfig[iSys]; if ( !splitSystem( colConfig, event) ) { infoPtr->errorMsg("Error in RHadrons::produce: " "failed to handle two sparticles in same system"); return false; } } } // Loop over R-hadrons to be formed. Find its colour singlet system. for (iRHad = 0; iRHad < nRHad; ++iRHad) { iBef = iBefRHad[iRHad]; iSys = colConfig.findSinglet( iBef); if (iSys < 0) { infoPtr->errorMsg("Error in RHadrons::produce: " "sparticle not in any colour singlet"); return false; } systemPtr = &colConfig[iSys]; // For now don't handle systems involving junctions or loops. if (systemPtr->hasJunction) { infoPtr->errorMsg("Error in RHadrons::produce: " "cannot handle system with junction"); return false; } if (systemPtr->isClosed) { infoPtr->errorMsg("Error in RHadrons::produce: " "cannot handle closed colour loop"); return false; } // Handle formation of R-hadron separately for gluino and squark. if (event[iBef].id() == idRGo) isTriplet[iRHad] = false; bool formed = (isTriplet[iRHad]) ? produceSquark( colConfig, event) : produceGluino( colConfig, event); if (!formed) return false; // End of loop over R-hadrons. Done. } return true; } //-------------------------------------------------------------------------- // Decay R-hadrons by resolving them into string systems and letting the // heavy unstable particle decay as normal. bool RHadrons::decay( Event& event) { // Loop over R-hadrons to decay. for (iRHad = 0; iRHad < nRHad; ++iRHad) { int iRNow = iRHadron[iRHad]; int iRBef = iBefRHad[iRHad]; int idRHad = event[iRNow].id(); double mRHad = event[iRNow].m(); double mRBef = event[iRBef].m(); int iR0 = 0; int iR2 = 0; // Find flavour content of squark or gluino R-hadron. pair idPair = (isTriplet[iRHad]) ? fromIdWithSquark( idRHad) : fromIdWithGluino( idRHad); int id1 = idPair.first; int id2 = idPair.second; // Sharing of momentum: the squark/gluino should be restored // to original mass, but error if negative-mass spectators. double fracR = mRBef / mRHad; if (fracR >= 1.) { infoPtr->errorMsg("Error in RHadrons::decay: " "too low R-hadron mass for decay"); return false; } // Squark: new colour needed in the breakup. if (isTriplet[iRHad]) { int colNew = event.nextColTag(); int col = (event[iRBef].col() != 0) ? colNew : 0; int acol = (col == 0) ? colNew : 0; // Store the constituents of a squark R-hadron. iR0 = event.append( id1, 106, iRNow, 0, 0, 0, col, acol, fracR * event[iRNow].p(), fracR * mRHad, 0.); iR2 = event.append( id2, 106, iRNow, 0, 0, 0, acol, col, (1. - fracR) * event[iRNow].p(), (1. - fracR) * mRHad, 0.); // Gluino: set mass sharing between two spectators. } else { double m1Eff = particleDataPtr->constituentMass(id1) + mOffsetCloudRH; double m2Eff = particleDataPtr->constituentMass(id2) + mOffsetCloudRH; double frac1 = (1. - fracR) * m1Eff / ( m1Eff + m2Eff); double frac2 = (1. - fracR) * m2Eff / ( m1Eff + m2Eff); // Two new colours needed in the breakups. int col1 = event.nextColTag(); int col2 = event.nextColTag(); // Store the constituents of a gluino R-hadron. iR0 = event.append( idRGo, 106, iRNow, 0, 0, 0, col2, col1, fracR * event[iRNow].p(), fracR * mRHad, 0.); event.append( id1, 106, iRNow, 0, 0, 0, col1, 0, frac1 * event[iRNow].p(), frac1 * mRHad, 0.); iR2 = event.append( id2, 106, iRNow, 0, 0, 0, 0, col2, frac2 * event[iRNow].p(), frac2 * mRHad, 0.); } // Mark R-hadron as decayed and update history. event[iRNow].statusNeg(); event[iRNow].daughters( iR0, iR2); iAftRHad[iRHad] = iR0; // Set secondary vertex for decay products, but no lifetime. Vec4 vDec = event[iRNow].vProd() + event[iRNow].tau() * event[iR0].p() / event[iR0].m(); for (int iRd = iR0; iRd <= iR2; ++iRd) event[iRd].vProd( vDec); // End loop over R-hadron decays, based on velocity of squark. } // Done. return true; } //-------------------------------------------------------------------------- // Split a system that contains both a sparticle and a junction. bool RHadrons::splitOffJunction( ColConfig& colConfig, Event& event) { // Classify system into three legs, and find sparticle location. vector leg1, leg2, leg3; int iLegSP = 0; int iPosSP = 0; int iLeg = 0; int iPos = 0; for (int i = 0; i < systemPtr->size(); ++i) { ++iPos; int iP = systemPtr->iParton[i]; if (iP < 0) { ++iLeg; iPos = -1; } else if (iLeg == 1) leg1.push_back( iP); else if (iLeg == 2) leg2.push_back( iP); else if (iLeg == 3) leg3.push_back( iP); if (iP == iBef) { iLegSP = iLeg; iPosSP = iPos; } } if (iLegSP == 0) return false; // Swap so leg 1 contains sparticle. If not innermost sparticle then // skip for now, and wait for this other (gluino!) to be split off. if (iLegSP == 2) swap(leg2, leg1); else if (iLegSP == 3) swap(leg3, leg1); for (int i = 0; i < iPosSP; ++i) if (event[leg1[i]].id() != 21) return true; // No gluon between sparticle and junction: find kinetic energy of system. if (iPosSP == 0) { Vec4 pSP = event[iBef].p(); Vec4 pRec = 0.; for (int i = 0; i < int(leg2.size()); ++i) pRec += event[leg2[i]].p(); for (int i = 0; i < int(leg3.size()); ++i) pRec += event[leg3[i]].p(); double mSys = (pSP + pRec).mCalc(); double mSP = pSP.mCalc(); double mRec = pRec.mCalc(); double eKin = mSys - mSP - mRec; // Insert new gluon that borrows part of kinetic energy. double mNewG = EGBORROWMAX * eKin / (EGBORROWMAX + eKin) ; Vec4 pNewG = (mNewG / mSys) * (pSP + pRec); int newCol = event.nextColTag(); bool isCol = (event[leg1.back()].col() > 0); int colNG = (isCol)? newCol : event[iBef].acol(); int acolNG = (isCol) ? event[iBef].col() : newCol; int iNewG = event.append( 21, 101, iBef, 0, 0, 0, colNG, acolNG, pNewG, mNewG, 0.); leg1.insert( leg1.begin(), iNewG); ++iPosSP; // Boosts for remainder systems that gave up energy. double mNewSys = mSys - mNewG; double pAbsOld = 0.5 * sqrtpos( pow2(mSys*mSys - mSP*mSP - mRec*mRec) - pow2(2. * mSP * mRec) ) / mSys; double pAbsNew = 0.5 * sqrtpos( pow2(mNewSys*mNewSys - mSP*mSP - mRec*mRec) - pow2(2. * mSP * mRec) ) / mNewSys; RotBstMatrix MtoCM, MfromCM, MSP, MRec; MtoCM.toCMframe( pSP, pRec); MfromCM = MtoCM; MfromCM.invert(); MSP = MtoCM; MSP.bst( 0., 0., -pAbsOld / sqrt(mSP * mSP + pAbsOld * pAbsOld)); MSP.bst( 0., 0., pAbsNew / sqrt(mSP * mSP + pAbsNew * pAbsNew)); MSP.rotbst( MfromCM); MRec = MtoCM; MRec.bst( 0., 0., pAbsOld / sqrt(mRec * mRec + pAbsOld * pAbsOld)); MRec.bst( 0., 0., -pAbsNew / sqrt(mRec * mRec + pAbsNew * pAbsNew)); MRec.rotbst( MfromCM); // Copy down recoling partons and boost their momenta. int iNewSP = event.copy( iBef, 101); event[iNewSP].mother2(0); event[iBef].daughter1(iNewG); event[iNewSP].rotbst( MSP); leg1[iPosSP] = iNewSP; if (iBefRHad[0] == iBef) iBefRHad[0] = iNewSP; else if (nRHad > 1 && iBefRHad[1] == iBef) iBefRHad[1] = iNewSP; iBef = iNewSP; for (int i = 0; i < int(leg2.size()); ++i) { int iCopy = event.copy( leg2[i], 101); event[iCopy].rotbst( MRec); if (iBefRHad[0] == leg2[i]) iBefRHad[0] = iCopy; else if (nRHad > 1 && iBefRHad[1] == leg2[i]) iBefRHad[1] = iCopy; leg2[i] = iCopy; } for (int i = 0; i < int(leg3.size()); ++i) { int iCopy = event.copy( leg3[i], 101); event[iCopy].rotbst( MRec); if (iBefRHad[0] == leg3[i]) iBefRHad[0] = iCopy; else if (nRHad > 1 && iBefRHad[1] == leg3[i]) iBefRHad[1] = iCopy; leg3[i] = iCopy; } // Now always at least one gluon between sparticle and junction. } // Find gluon with largest energy in sparticle rest frame. int iGspl = 0; double eGspl = event[leg1[0]].p() * event[iBef].p(); for (int i = 1; i < iPosSP; ++i) { double eGnow = event[leg1[i]].p() * event[iBef].p(); if (eGnow > eGspl) { iGspl = i; eGspl = eGnow; } } int iG = leg1[iGspl]; // Split this gluon into a collinear quark.antiquark pair. int idNewQ = flavSelPtr->pickLightQ(); int iNewQ = event.append( idNewQ, 101, iG, 0, 0, 0, event[iG].col(), 0, 0.5 * event[iG].p(), 0.5 * event[iG].m(), 0.); int iNewQb = event.append( -idNewQ, 101, iG, 0, 0, 0, 0, event[iG].acol(), 0.5 * event[iG].p(), 0.5 * event[iG].m(), 0.); event[iG].statusNeg(); event[iG].daughters( iNewQ, iNewQb); if (event[leg1.back()].col() == 0) swap( iNewQ, iNewQb); // Collect two new systems after split. vector iNewSys1, iNewSys2; iNewSys1.push_back( iNewQb); for (int i = iGspl + 1; i < int(leg1.size()); ++i) iNewSys1.push_back( leg1[i]); iNewSys2.push_back( -10); for (int i = 0; i < iGspl; ++i) iNewSys2.push_back( leg1[i]); iNewSys2.push_back( iNewQ); iNewSys2.push_back( -11); for (int i = 0; i < int(leg2.size()); ++i) iNewSys2.push_back( leg2[i]); iNewSys2.push_back( -12); for (int i = 0; i < int(leg3.size()); ++i) iNewSys2.push_back( leg3[i]); // Remove old system and insert two new ones. colConfig.erase(iSys); colConfig.insert( iNewSys1, event); colConfig.insert( iNewSys2, event); // Done. return true; } //-------------------------------------------------------------------------- // Open up a closed gluon/gluino loop. bool RHadrons::openClosedLoop( ColConfig& colConfig, Event& event) { // Find gluon with largest energy in gluino rest frame. int iGspl = -1; double eGspl = 0.; for (int i = 0; i < systemPtr->size(); ++i) { int iGNow = systemPtr->iParton[i]; if (event[iGNow].id() == 21) { double eGnow = event[iGNow].p() * event[iBef].p(); if (eGnow > eGspl) { iGspl = i; eGspl = eGnow; } } } if (iGspl == -1) return false; // Split this gluon into a collinear quark.antiquark pair. int iG = systemPtr->iParton[iGspl]; int idNewQ = flavSelPtr->pickLightQ(); int iNewQ = event.append( idNewQ, 101, iG, 0, 0, 0, event[iG].col(), 0, 0.5 * event[iG].p(), 0.5 * event[iG].m(), 0.); int iNewQb = event.append( -idNewQ, 101, iG, 0, 0, 0, 0, event[iG].acol(), 0.5 * event[iG].p(), 0.5 * event[iG].m(), 0.); event[iG].statusNeg(); event[iG].daughters( iNewQ, iNewQb); // Order partons in new system. Note order of colour flow. int iNext = iGspl + 1; if (iNext == systemPtr->size()) iNext = 0; if (event[ systemPtr->iParton[iNext]].acol() != event[iNewQ].col()) swap( iNewQ, iNewQb); vector iNewSys; iNewSys.push_back( iNewQ); for (int i = iGspl + 1; i < systemPtr->size(); ++i) iNewSys.push_back( systemPtr->iParton[i]); for (int i = 0; i < iGspl; ++i) iNewSys.push_back( systemPtr->iParton[i]); iNewSys.push_back( iNewQb); // Erase the old system and insert the new one instead. colConfig.erase(iSys); colConfig.insert( iNewSys, event); // Done. return true; } //-------------------------------------------------------------------------- // Split a single colour singlet that contains two sparticles. // To fix : if nLeg >= 3 && mMin large handle as in nLeg == 1?? bool RHadrons::splitSystem( ColConfig& colConfig, Event& event) { // First and second R-hadron mother. Number of legs in between. int iFirst = -1; int iSecond = -1; for (int i = 0; i < int(systemPtr->size()); ++i) { int iTmp = systemPtr->iParton[i]; if ( givesRHadron( event[iTmp].id()) ) { if (iFirst == -1) iFirst = i; else iSecond = i; } } int nLeg = iSecond - iFirst; // New flavour pair for breaking the string, and its mass. int idNewQ = flavSelPtr->pickLightQ(); double mNewQ = particleDataPtr->constituentMass( idNewQ); vector iNewSys1, iNewSys2; // If sparticles are neighbours then need new q-qbar pair in between. if (nLeg == 1) { // The location of the two sparticles. int i1Old = systemPtr->iParton[iFirst]; int i2Old = systemPtr->iParton[iSecond]; // Take a fraction of momentum to give breakup quark pair. double mHat = (event[i1Old].p() + event[i2Old].p()).mCalc(); double mMax = mHat - event[i1Old].m() - event[i2Old].m(); if (mMax < 2. * (mNewQ + MSAFETY)) return false; double mEff = min( 2. * (mNewQ + mOffsetCloudRH), mMax - 2. * MSAFETY); double frac = mEff / mHat; Vec4 pEff = frac * (event[i1Old].p() + event[i2Old].p()); // New kinematics by (1) go to same mHat with bigger masses, and // (2) rescale back down to original masses and reduced mHat. Vec4 p1New, p2New; if ( !newKin( event[i1Old].p(), event[i2Old].p(), event[i1Old].m() / (1. - frac), event[i2Old].m() / (1. - frac), p1New, p2New) ) return false; p1New *= 1. - frac; p2New *= 1. - frac; // Fill in new partons after branching, with correct colour/flavour sign. int i1New, i2New, i3New, i4New; int newCol = event.nextColTag(); i1New = event.copy( i1Old, 101); if (event[i2Old].acol() == event[i1Old].col()) { i3New = event.append( -idNewQ, 101, i1Old, 0, 0, 0, 0, event[i2Old].acol(), 0.5 * pEff, 0.5 * mEff, 0.); i2New = event.copy( i2Old, 101); event[i2New].acol( newCol); i4New = event.append( idNewQ, 101, i2Old, 0, 0, 0, newCol, 0, 0.5 * pEff, 0.5 * mEff, 0.); } else { i3New = event.append( idNewQ, 101, i1Old, 0, 0, 0, event[i2Old].col(), 0, 0.5 * pEff, 0.5 * mEff, 0.); i2New = event.copy( i2Old, 101); event[i2New].col( newCol); i4New = event.append( -idNewQ, 101, i2Old, 0, 0, 0, 0, newCol, 0.5 * pEff, 0.5 * mEff, 0.); } // Modify momenta and history. For iBotCopyId tracing asymmetric // bookkeeping where one sparticle is radiator and the other recoiler. event[i1New].p( p1New); event[i2New].p( p2New); event[i1Old].daughters( i1New, i3New); event[i1New].mother2( 0); event[i2Old].daughters( i2New, i4New); event[i2New].mother2( 0); iBefRHad[0] = i1New; iBefRHad[1] = i2New; // Partons in the two new systems. for (int i = 0; i < iFirst; ++i) iNewSys1.push_back( systemPtr->iParton[i]); iNewSys1.push_back( i1New); iNewSys1.push_back( i3New); iNewSys2.push_back( i4New); iNewSys2.push_back( i2New); for (int i = iSecond + 1; i < int(systemPtr->size()); ++i) iNewSys2.push_back( systemPtr->iParton[i]); // If one gluon between sparticles then split it into a // collinear q-qbar pair. } else if (nLeg == 2) { // Gluon to be split and its two daughters. int iOld = systemPtr->iParton[iFirst + 1]; int i1New = event.append( idNewQ, 101, iOld, 0, 0, 0, event[iOld].col(), 0, 0.5 * event[iOld].p(), 0.5 * event[iOld].m(), 0.); int i2New = event.append( -idNewQ, 101, iOld, 0, 0, 0, 0, event[iOld].acol(), 0.5 * event[iOld].p(), 0.5 * event[iOld].m(), 0.); event[iOld].statusNeg(); event[iOld].daughters( i1New, i2New); // Partons in the two new systems. if (event[systemPtr->iParton[iFirst]].col() == event[i2New].acol()) swap( i1New, i2New); for (int i = 0; i <= iFirst; ++i) iNewSys1.push_back( systemPtr->iParton[i]); iNewSys1.push_back( i1New); iNewSys2.push_back( i2New); for (int i = iSecond; i < int(systemPtr->size()); ++i) iNewSys2.push_back( systemPtr->iParton[i]); // If several gluons between sparticles then find lowest-mass gluon pair // and replace it by a q-qbar pair. } else { // Find lowest-mass gluon pair and adjust effective quark mass. int iMin = 0; int i1Old = 0; int i2Old = 0; double mMin = 1e20; for (int i = iFirst + 1; i < iSecond - 1; ++i) { int i1Tmp = systemPtr->iParton[i]; int i2Tmp = systemPtr->iParton[i + 1]; double mTmp = (event[i1Tmp].p() + event[i2Tmp].p()).mCalc(); if (mTmp < mMin) { iMin = i; i1Old = i1Tmp; i2Old = i2Tmp; mMin = mTmp; } } double mEff = min( mNewQ + mOffsetCloudRH, 0.4 * mMin); // New kinematics by sharing mHat appropriately. Vec4 p1New, p2New; if ( !newKin( event[i1Old].p(), event[i2Old].p(), mEff, mEff, p1New, p2New, false) ) return false; // Insert new partons and update history. int i1New, i2New; if (event[systemPtr->iParton[0]].acol() == 0) { i1New = event.append( -idNewQ, 101, i1Old, 0, 0, 0, 0, event[i1Old].acol(), p1New, mEff, 0.); i2New = event.append( idNewQ, 101, i2Old, 0, 0, 0, event[i2Old].col(), 0, p2New, mEff, 0.); } else { i1New = event.append( idNewQ, 101, i1Old, 0, 0, 0, event[i1Old].col(), 0, p1New, mEff, 0.); i2New = event.append( -idNewQ, 101, i2Old, 0, 0, 0, 0, event[i2Old].acol(), p2New, mEff, 0.); } event[i1Old].statusNeg(); event[i2Old].statusNeg(); event[i1Old].daughters( i1New, 0); event[i2Old].daughters( i2New, 0); // Partons in the two new systems. for (int i = 0; i < iMin; ++i) iNewSys1.push_back( systemPtr->iParton[i]); iNewSys1.push_back( i1New); iNewSys2.push_back( i2New); for (int i = iMin + 2; i < int(systemPtr->size()); ++i) iNewSys2.push_back( systemPtr->iParton[i]); } // Erase the old system and insert the two new ones instead. colConfig.erase(iSys); colConfig.insert( iNewSys1, event); colConfig.insert( iNewSys2, event); // Done. return true; } //-------------------------------------------------------------------------- // Produce a R-hadron from a squark and another string end. bool RHadrons::produceSquark( ColConfig& colConfig, Event& event) { // Initial values. int nBody = 0; int iRNow = 0; int iNewQ = 0; int iNewL = 0; // Check at which end of the string the squark is located. int idAbsTop = event[ systemPtr->iParton[0] ].idAbs(); bool sqAtTop = (allowRSb && idAbsTop == idRSb) || (allowRSt && idAbsTop == idRSt); // Copy down system consecutively from squark end. int iBeg = event.size(); iCreRHad[iRHad] = iBeg; if (sqAtTop) for (int i = 0; i < systemPtr->size(); ++i) event.copy( systemPtr->iParton[i], 102); else for (int i = systemPtr->size() - 1; i >= 0; --i) event.copy( systemPtr->iParton[i], 102); int iEnd = event.size() - 1; // Input flavours. From now on H = heavy and L = light string ends. int idOldH = event[iBeg].id(); int idOldL = event[iEnd].id(); // Pick new flavour to form R-hadron. FlavContainer flavOld( idOldH%10); int idNewQ = flavSelPtr->pick(flavOld).id; int idRHad = toIdWithSquark( idOldH, idNewQ); if (idRHad == 0) { infoPtr->errorMsg("Error in RHadrons::produceSquark: " "cannot form R-hadron code"); return false; } // Target mass of R-hadron and z value of fragmentation function. double mRHad = particleDataPtr->m0(idRHad) + event[iBeg].m() - ( (abs(idOldH) == idRSb) ? m0Sb : m0St ); double z = zSelPtr->zFrag( idOldH, idNewQ, mRHad*mRHad); // Basic kinematics of string piece where break is to occur. Vec4 pOldH = event[iBeg].p(); int iOldL = iBeg + 1; Vec4 pOldL = event[iOldL].p(); double mOldL = event[iOldL].m(); double mNewH = mRHad / z; double sSys = (pOldH + pOldL).m2Calc(); double sRem = (1. - z) * (sSys - mNewH*mNewH); double sMin = pow2(mOldL + mCollapseRH); // If too low remaining mass in system then add one more parton to it. while ( ( sRem < sMin || sSys < pow2(mNewH + mOldL + MSAFETY) ) && iOldL < iEnd ) { ++iOldL; pOldL += event[iOldL].p(); mOldL = event[iOldL].m(); sSys = (pOldH + pOldL).m2Calc(); sRem = (1. - z) * (sSys - mNewH*mNewH); sMin = pow2(mOldL + mCollapseRH); } // If enough mass then split off R-hadron and reduced system. if ( sRem > sMin && sSys > pow2(mNewH + mOldL + MSAFETY) ) { Vec4 pNewH, pNewL; if ( !newKin( pOldH, pOldL, mNewH, mOldL, pNewH, pNewL) ) { infoPtr->errorMsg("Error in RHadrons::produceSquark: " "failed to construct kinematics with reduced system"); return false; } // Insert R-hadron with new momentum. iRNow = event.append( idRHad, 104, iBeg, iOldL, 0, 0, 0, 0, z * pNewH, mRHad, 0.); // Reduced system with new string endpoint and modified recoiler. idNewQ = -idNewQ; bool hasCol = (idNewQ > 0 && idNewQ < 10) || idNewQ < -10; int col = (hasCol) ? event[iOldL].acol() : 0; int acol = (hasCol) ? 0 : event[iOldL].col(); iNewQ = event.append( idNewQ, 105, iBeg, iOldL, 0, 0, col, acol, (1. - z) * pNewH, (1. - z) * mNewH, 0.); iNewL = event.copy( iOldL, 105); event[iNewL].mothers( iBeg, iOldL); event[iNewL].p( pNewL); // Done with processing of split to R-hadron and reduced system. nBody = 3; } // Two-body final state: form light hadron from endpoint and new flavour. if (nBody == 0) { FlavContainer flav1( idOldL); FlavContainer flav2( -idNewQ); int iTry = 0; int idNewL = flavSelPtr->combine( flav1, flav2); while (++iTry < NTRYMAX && idNewL == 0) idNewL = flavSelPtr->combine( flav1, flav2); if (idNewL == 0) { infoPtr->errorMsg("Error in RHadrons::produceSquark: " "cannot form light hadron code"); return false; } double mNewL = particleDataPtr->mSel( idNewL); // Check that energy enough for light hadron and R-hadron. if ( sSys > pow2(mRHad + mNewL + MSAFETY) ) { Vec4 pRHad, pNewL; if ( !newKin( pOldH, pOldL, mRHad, mNewL, pRHad, pNewL) ) { infoPtr->errorMsg("Error in RHadrons::produceSquark: " "failed to construct kinematics for two-hadron decay"); return false; } // Insert R-hadron and light hadron. iRNow = event.append( idRHad, 104, iBeg, iOldL, 0, 0, 0, 0, pRHad, mRHad, 0.); event.append( idNewL, 105, iBeg, iOldL, 0, 0, 0, 0, pNewL, mNewL, 0.); // Done for two-body case. nBody = 2; } } // Final case: for very low mass collapse to one single R-hadron. if (nBody == 0) { idRHad = toIdWithSquark( idOldH, idOldL); if (idRHad == 0) { infoPtr->errorMsg("Error in RHadrons::produceSquark: " "cannot form R-hadron code"); return false; } // Insert R-hadron with new momentum. iRNow = event.append( idRHad, 104, iBeg, iOldL, 0, 0, 0, 0, systemPtr->pSum, systemPtr->mass, 0.); // Done with one-body case. nBody = 1; } // History bookkeeping: the R-hadron and processed partons. iRHadron[iRHad] = iRNow; int iLast = event.size() - 1; for (int i = iBeg; i <= iOldL; ++i) { event[i].statusNeg(); event[i].daughters( iRNow, iLast); } // Remove old string system and, if needed, insert a new one. colConfig.erase(iSys); if (nBody == 3) { vector iNewSys; iNewSys.push_back( iNewQ); iNewSys.push_back( iNewL); for ( int i = iOldL + 1; i <= iEnd; ++i) iNewSys.push_back( i); colConfig.insert( iNewSys, event); } // Copy lifetime and vertex from sparticle to R-hadron. event[iRNow].tau( event[iBef].tau() ); if (event[iBef].hasVertex()) event[iRNow].vProd( event[iBef].vProd() ); // Done with production of a R-hadron from a squark. return true; } //-------------------------------------------------------------------------- // Produce a R-hadron from a gluino and two string ends (or a gluon). bool RHadrons::produceGluino( ColConfig& colConfig, Event& event) { // Initial values. int iGlui = 0; int idSave = 0; int idQLeap = 0; bool isDiq1 = false; vector iSide1, iSide2, iSideTmp, iNewSys1, iNewSys2; Vec4 pGlui, pSide1, pSide2; // Decide whether to produce a gluinoball or not. bool isGBall = (rndmPtr->flat() < probGluinoballRH); // Extract one string system on either side of the gluino. for (int i = 0; i < systemPtr->size(); ++i) { int iTmp = systemPtr->iParton[i]; if (iGlui == 0 && event[ iTmp ].id() == idRGo) { iGlui = iTmp; pGlui = event[ iTmp ].p(); } else if (iGlui == 0) { iSideTmp.push_back( iTmp); pSide1 += event[ iTmp ].p(); } else { iSide2.push_back( iTmp); pSide2 += event[ iTmp ].p(); } } // Order sides from gluino outwards and with lowest relative mass first. for (int i = int(iSideTmp.size()) - 1; i >= 0; --i) iSide1.push_back( iSideTmp[i]); double m1H = (pGlui + pSide1).mCalc() - event[ iSide1.back() ].m(); double m2H = (pGlui + pSide2).mCalc() - event[ iSide2.back() ].m(); if (m2H < m1H) { swap( iSide1, iSide2); swap( pSide1, pSide2); } // Begin loop over two sides of gluino, with lowest relative mass first. for (int iSide = 1; iSide < 3; ++iSide) { // Begin processing of lower-mass string side. int idRHad = 0; double mRHad = 0.; int nBody = 0; int iRNow = 0; int iNewQ = 0; int iNewL = 0; int statusRHad = 0; // Copy down system consecutively from gluino end. int iBeg = event.size(); if (iSide == 1) { iCreRHad[iRHad] = iBeg; event.copy( iGlui, 102); for (int i = 0; i < int(iSide1.size()); ++i) event.copy( iSide1[i], 102); } else { event.copy( iGlui, 102); for (int i = 0; i < int(iSide2.size()); ++i) event.copy( iSide2[i], 102); } int iEnd = event.size() - 1; // Pick new flavour to help form R-hadron. Initial colour values. int idOldL = event[iEnd].id(); int idNewQ = 21; if (!isGBall) { do { FlavContainer flavOld( idOldL); idNewQ = -flavSelPtr->pick(flavOld).id; } while (iSide == 2 && isDiq1 && abs(idNewQ) > 10); if (iSide == 1) isDiq1 = (abs(idNewQ) > 10); } bool hasCol = (event[iEnd].col() > 0); int colR = 0; int acolR = 0; // Target intermediary mass or R-hadron mass. if (iSide == 1) { idSave = idNewQ; idRHad = (hasCol) ? 1009002 : -1009002; if (hasCol) colR = event[iBeg].col(); else acolR = event[iBeg].acol(); statusRHad = 103; double mNewQ = particleDataPtr->constituentMass( idNewQ); if (isGBall) mNewQ *= 0.5; mRHad = event[iBeg].m() + mOffsetCloudRH + mNewQ; } else { idRHad = toIdWithGluino( idSave, idNewQ); if (idRHad == 0) { infoPtr->errorMsg("Error in RHadrons::produceGluino: " "cannot form R-hadron code"); return false; } statusRHad = 104; mRHad = particleDataPtr->m0(idRHad) + event[iBeg].m() - m0Go; } // z value of fragmentation function. double z = zSelPtr->zFrag( idRGo, idNewQ, mRHad*mRHad); // Basic kinematics of string piece where break is to occur. Vec4 pOldH = event[iBeg].p(); int iOldL = iBeg + 1; Vec4 pOldL = event[iOldL].p(); double mOldL = event[iOldL].m(); double mNewH = mRHad / z; double sSys = (pOldH + pOldL).m2Calc(); double sRem = (1. - z) * (sSys - mNewH*mNewH); double sMin = pow2(mOldL + mCollapseRH); // If too low remaining mass in system then add one more parton to it. while ( ( sRem < sMin || sSys < pow2(mNewH + mOldL + MSAFETY) ) && iOldL < iEnd ) { ++iOldL; pOldL += event[iOldL].p(); mOldL = event[iOldL].m(); sSys = (pOldH + pOldL).m2Calc(); sRem = (1. - z) * (sSys - mNewH*mNewH); sMin = pow2(mOldL + mCollapseRH); } // If enough mass then split off R-hadron and reduced system. if ( sRem > sMin && sSys > pow2(mNewH + mOldL + MSAFETY) ) { Vec4 pNewH, pNewL; if ( !newKin( pOldH, pOldL, mNewH, mOldL, pNewH, pNewL) ) { infoPtr->errorMsg("Error in RHadrons::produceGluino: " "failed to construct kinematics with reduced system"); return false; } // Insert intermediary or R-hadron with new momentum, less colour. iRNow = event.append( idRHad, statusRHad, iBeg, iOldL, 0, 0, colR, acolR, z * pNewH, mRHad, 0.); // Reduced system with new string endpoint and modified recoiler. if (!isGBall) idNewQ = -idNewQ; int colN = (hasCol) ? 0 : event[iOldL].acol(); int acolN = (hasCol) ? event[iOldL].col() : 0; iNewQ = event.append( idNewQ, 105, iBeg, iOldL, 0, 0, colN, acolN, (1. - z) * pNewH, (1. - z) * mNewH, 0.); iNewL = event.copy( iOldL, 105); event[iNewL].mothers( iBeg, iOldL); event[iNewL].p( pNewL); // Collect partons of new string system. if (iSide == 1) { iNewSys1.push_back( iNewQ); iNewSys1.push_back( iNewL); for ( int i = iOldL + 1; i <= iEnd; ++i) iNewSys1.push_back( i); } else { iNewSys2.push_back( iNewQ); iNewSys2.push_back( iNewL); for ( int i = iOldL + 1; i <= iEnd; ++i) iNewSys2.push_back( i); } // Done with processing of split to R-hadron and reduced system. nBody = 3; } // For side-1 low-mass glueball system reabsorb full momentum. if (nBody == 0 && isGBall && iSide == 1) { idQLeap = event[iOldL].id(); Vec4 pNewH = event[iBeg].p() + pOldL; // Insert intermediary R-hadron with new momentum, less colour. iRNow = event.append( idRHad, statusRHad, iBeg, iEnd, 0, 0, colR, acolR, pNewH, pNewH.mCalc(), 0.); nBody = 1; } // Two-body final state: form light hadron from endpoint and new flavour. // Also for side 2 if gluinoball formation gives quark from side 1. if (nBody == 0 && (!isGBall || (iSide == 2 && idQLeap != 0) )) { if (isGBall) idNewQ = -idQLeap; FlavContainer flav1( idOldL); FlavContainer flav2( -idNewQ); int iTry = 0; int idNewL = flavSelPtr->combine( flav1, flav2); while (++iTry < NTRYMAX && idNewL == 0) idNewL = flavSelPtr->combine( flav1, flav2); if (idNewL == 0) { infoPtr->errorMsg("Error in RHadrons::produceGluino: " "cannot form light hadron code"); return false; } double mNewL = particleDataPtr->mSel( idNewL); // Check that energy enough for light hadron and R-hadron. if ( sSys > pow2(mRHad + mNewL + MSAFETY) ) { Vec4 pRHad, pNewL; if ( !newKin( pOldH, pOldL, mRHad, mNewL, pRHad, pNewL) ) { infoPtr->errorMsg("Error in RHadrons::produceGluino: " "failed to construct kinematics for two-hadron decay"); return false; } // Insert intermediary or R-hadron and light hadron. iRNow = event.append( idRHad, statusRHad, iBeg, iOldL, 0, 0, colR, acolR, pRHad, mRHad, 0.); event.append( idNewL, 105, iBeg, iOldL, 0, 0, 0, 0, pNewL, mNewL, 0.); // Done for two-body case. nBody = 2; // For this case gluinoball should be handled as normal flavour. isGBall = false; } } // Final case: for very low mass collapse to one single R-hadron. if (nBody == 0 && (!isGBall || (iSide == 2 && idQLeap != 0) )) { if (isGBall) idSave = idQLeap; if (iSide == 1) idSave = idOldL; else idRHad = toIdWithGluino( idSave, idOldL); if (idRHad == 0) { infoPtr->errorMsg("Error in RHadrons::produceGluino: " "cannot form R-hadron code"); return false; } // Insert R-hadron with new momentum. iRNow = event.append( idRHad, statusRHad, iBeg, iOldL, 0, 0, colR, acolR, pOldH + pOldL, (pOldH + pOldL).mCalc(), 0.); // Done with one-body case. // Even if hoped-for, it was not possible to create a gluinoball. isGBall = false; } // History bookkeeping: the processed partons. int iLast = event.size() - 1; for (int i = iBeg; i <= iOldL; ++i) { event[i].statusNeg(); event[i].daughters( iRNow, iLast); } // End of loop over two sides of the gluino. iGlui = iRNow; } // History bookkeeping: insert R-hadron; delete old string system. if (iGlui == 0) { infoPtr->errorMsg("Error in RHadrons::produceGluino: " "could not handle gluinoball kinematics"); return false; } iRHadron[iRHad] = iGlui; colConfig.erase(iSys); // Non-gluinoball: insert (up to) two new string systems. if (!isGBall) { if (iNewSys1.size() > 0) colConfig.insert( iNewSys1, event); if (iNewSys2.size() > 0) colConfig.insert( iNewSys2, event); // Gluinoball with enough energy in first string: // join two temporary gluons into one. } else if (idQLeap == 0) { int iG1 = iNewSys1[0]; int iG2 = iNewSys2[0]; int colG = event[iG1].col() + event[iG2].col(); int acolG = event[iG1].acol() + event[iG2].acol(); Vec4 pG = event[iG1].p() + event[iG2].p(); int iG12 = event.append( 21, 107, iG1, iG2, 0, 0, colG, acolG, pG, pG.mCalc(), 0.); // Temporary gluons no longer needed, but new colour to avoid warnings. event[iG1].id( 21); event[iG2].id( 21); event[iG1].statusNeg(); event[iG2].statusNeg(); event[iG1].daughter1( iG12); event[iG2].daughter1( iG12); int colBridge = event.nextColTag(); if (event[iG1].col() == 0) { event[iG1].col( colBridge); event[iG2].acol( colBridge); } else { event[iG1].acol( colBridge); event[iG2].col( colBridge); } // Form the remnant system from which the R-hadron has been split off. vector iNewSys12; for (int i = int(iNewSys1.size()) - 1; i > 0; --i) iNewSys12.push_back( iNewSys1[i]); iNewSys12.push_back( iG12); for (int i = 1; i < int(iNewSys2.size()); ++i) iNewSys12.push_back( iNewSys2[i]); colConfig.insert( iNewSys12, event); // Gluinoball where side 1 was fully eaten, and its flavour content // should leap over to the other side, to a gluon there. } else { int iG2 = iNewSys2[0]; event[iG2].id( idQLeap); colConfig.insert( iNewSys2, event); } // Copy lifetime and vertex from sparticle to R-hadron. event[iGlui].tau( event[iBef].tau() ); if (event[iBef].hasVertex()) event[iGlui].vProd( event[iBef].vProd() ); // Done with production of a R-hadron from a gluino. return true; } //-------------------------------------------------------------------------- // Form a R-hadron code from a squark and a (di)quark code. // First argument is the (anti)squark, second the (anti)(di)quark. int RHadrons::toIdWithSquark( int id1, int id2) { // Check that physical combination; return 0 if not. int id1Abs = abs(id1); int id2Abs = abs(id2); if (id2Abs < 10 && id1 > 0 && id2 > 0) return 0; if (id2Abs < 10 && id1 < 0 && id2 < 0) return 0; if (id2Abs > 10 && id1 > 0 && id2 < 0) return 0; if (id2Abs > 10 && id1 < 0 && id2 > 0) return 0; // Form R-hadron code. Flip sign for antisquark. bool isSt = (id1Abs == idRSt); int idRHad = 1000000; if (id2Abs < 10) idRHad += ((isSt) ? 600 : 500) + 10 * id2Abs + 2; else idRHad += ((isSt) ? 6000 : 5000) + 10 * (id2Abs/100) + id2Abs%10; if (id1 < 0) idRHad = -idRHad; // Done. return idRHad; } //-------------------------------------------------------------------------- // Resolve a R-hadron code into a squark and a (di)quark. // Return a pair, where first is the squark and the second the (di)quark. pair RHadrons::fromIdWithSquark( int idRHad) { // Find squark flavour content. int idLight = (abs(idRHad) - 1000000) / 10; int idSq = (idLight < 100) ? idLight/10 : idLight/100; int id1 = (idSq == 6) ? idRSt : idRSb; if (idRHad < 0) id1 = -id1; // Find light (di)quark flavour content. int id2 = (idLight < 100) ? idLight%10 : idLight%100; if (id2 > 10) id2 = 100 * id2 + abs(idRHad)%10; if ((id2 < 10 && idRHad > 0) || (id2 > 10 && idRHad < 0)) id2 = -id2; // Done. return make_pair( id1, id2); } //-------------------------------------------------------------------------- // Form a R-hadron code from two quark/diquark endpoints and a gluino. int RHadrons::toIdWithGluino( int id1, int id2) { // Check that physical combination; return 0 if not. Handle gluinoball. int id1Abs = abs(id1); int id2Abs = abs(id2); if (id1Abs == 21 && id2Abs == 21) return 1000993; int idMax = max( id1Abs, id2Abs); int idMin = min( id1Abs, id2Abs); if (idMin > 10) return 0; if (idMax > 10 && id1 > 0 && id2 < 0) return 0; if (idMax > 10 && id1 < 0 && id2 > 0) return 0; if (idMax < 10 && id1 > 0 && id2 > 0) return 0; if (idMax < 10 && id1 < 0 && id2 < 0) return 0; // Form R-meson code. Flip sign for antiparticle. int idRHad = 0; if (idMax < 10) { idRHad = 1009003 + 100 * idMax + 10 * idMin; if (idMin != idMax && idMax%2 == 1) { if (id1Abs == idMax && id1 > 0) idRHad = -idRHad; if (id2Abs == idMax && id2 > 0) idRHad = -idRHad; } if (idMin != idMax && idMax%2 == 0) { if (id1Abs == idMax && id1 < 0) idRHad = -idRHad; if (id2Abs == idMax && id2 < 0) idRHad = -idRHad; } // Form R-baryon code. Flip sign for antiparticle. } else { int idA = idMax/1000; int idB = (idMax/100)%10; int idC = idMin; if (idC > idB) swap( idB, idC); if (idB > idA) swap( idA, idB); if (idC > idB) swap( idB, idC); idRHad = 1090004 + 1000 * idA + 100 * idB + 10 * idC; if (id1 < 0) idRHad = -idRHad; } // Done. return idRHad; } //-------------------------------------------------------------------------- // Resolve a R-hadron code into two quark/diquark endpoints (and a gluino). // Return a pair, where first carries colour and second anticolour. pair RHadrons::fromIdWithGluino( int idRHad) { // Find light flavour content of R-hadron. int idLight = (abs(idRHad) - 1000000) / 10; int id1, id2, idTmp, idA, idB, idC; // Gluinoballs: split g into d dbar or u ubar. if (idLight < 100) { id1 = (rndmPtr->flat() < 0.5) ? 1 : 2; id2 = -id1; // Gluino-meson: split into q + qbar. } else if (idLight < 1000) { id1 = (idLight / 10) % 10; id2 = -(idLight % 10); // Flip signs when first quark of down-type. if (id1%2 == 1) { idTmp = id1; id1 = -id2; id2 = -idTmp; } // Gluino-baryon: split to q + qq (diquark). // Pick diquark at random, except if c or b involved. } else { idA = (idLight / 100) % 10; idB = (idLight / 10) % 10; idC = idLight % 10; double rndmQ = 3. * rndmPtr->flat(); if (idA > 3) rndmQ = 0.5; if (rndmQ < 1.) { id1 = idA; id2 = 1000 * idB + 100 * idC + 3; if (idB != idC && rndmPtr->flat() > diquarkSpin1RH) id2 -= 2; } else if (rndmQ < 2.) { id1 = idB; id2 = 1000 * idA + 100 * idC + 3; if (idA != idC && rndmPtr->flat() > diquarkSpin1RH) id2 -= 2; } else { id1 = idC; id2 = 1000 * idA + 100 * idB +3; if (idA != idB && rndmPtr->flat() > diquarkSpin1RH) id2 -= 2; } } // Flip signs for anti-R-hadron. if (idRHad < 0) { idTmp = id1; id1 = -id2; id2 = -idTmp; } // Done. return make_pair( id1, id2); } //-------------------------------------------------------------------------- // Construct modified four-vectors to match modified masses: // minimal reshuffling of momentum along common axis. // Note that last two arguments are used to provide output! bool RHadrons::newKin( Vec4 pOld1, Vec4 pOld2, double mNew1, double mNew2, Vec4& pNew1, Vec4& pNew2, bool checkMargin) { // Squared masses in initial and final kinematics. double sSum = (pOld1 + pOld2).m2Calc(); double sOld1 = pOld1.m2Calc(); double sOld2 = pOld2.m2Calc(); double sNew1 = mNew1 * mNew1; double sNew2 = mNew2 * mNew2; // Check that kinematically possible. if (checkMargin && pow2(mNew1 + mNew2 + MSAFETY) > sSum) return false; // Transfer coefficients to give four-vectors with the new masses. double lamOld = sqrt( pow2(sSum - sOld1 - sOld2) - 4. * sOld1 * sOld2 ); double lamNew = sqrt( pow2(sSum - sNew1 - sNew2) - 4. * sNew1 * sNew2 ); double move1 = (lamNew * (sSum - sOld1 + sOld2) - lamOld * (sSum - sNew1 + sNew2)) / (2. * sSum * lamOld); double move2 = (lamNew * (sSum + sOld1 - sOld2) - lamOld * (sSum + sNew1 - sNew2)) / (2. * sSum * lamOld); // Construct final vectors. Done. pNew1 = (1. + move1) * pOld1 - move2 * pOld2; pNew2 = (1. + move2) * pOld2 - move1 * pOld1; return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SusyLesHouches.cc0000644000175000017500000017017212217346252016371 0ustar sunsun// SusyLesHouches.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // Main authors of this file: N. Desai, P. Skands // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. #include "Pythia8/SusyLesHouches.h" // GZIP support. #ifdef GZIPSUPPORT // For GCC versions >= 4.6, can switch off shadow warnings. #if (defined GZIPSUPPORT && ((__GNUC__ * 100) + __GNUC_MINOR__) >= 406) #pragma GCC diagnostic ignored "-Wshadow" #endif // Boost includes. #include "boost/iostreams/filtering_stream.hpp" #include "boost/iostreams/filter/gzip.hpp" // Switch shadow warnings back on. #if (defined GZIPSUPPORT && ((__GNUC__ * 100) + __GNUC_MINOR__) >= 406) #pragma GCC diagnostic warning "-Wshadow" #endif #endif // GZIPSUPPORT namespace Pythia8 { //========================================================================== // The SusyLesHouches class. //========================================================================== // Main routine to read in SLHA and LHEF+SLHA files int SusyLesHouches::readFile(string slhaFileIn, int verboseIn, bool useDecayIn) { // Copy inputs to local slhaFile = slhaFileIn; verbose = verboseIn; useDecay = useDecayIn; // Check that input file is OK. int iFailFile=0; const char* cstring = slhaFile.c_str(); // Construct istream without gzip support. #ifndef GZIPSUPPORT ifstream file(cstring); // Construct istream with gzip support. #else boost::iostreams::filtering_istream file; ifstream fileBase(cstring); // Pass along the 'good()' flag, so code elsewhere works unmodified. if (!fileBase.good()) file.setstate(ios_base::badbit); // Check filename ending to decide which filters to apply. else { const char *last = strrchr(cstring, '.'); if (last && strncmp(last, ".gz", 3) == 0) file.push(boost::iostreams::gzip_decompressor()); file.push(fileBase); } #endif // Exit if input file not found. Else print file name. if (!file.good()) { message(2,"readFile",slhaFile+" not found",0); return -1; slhaRead=false; } if (verbose >= 3) { message(0,"readFile","parsing "+slhaFile,0); filePrinted = true; } // Array of particles read in. vector idRead; //Initial values for read-in variables. slhaRead=true; lhefRead=false; lhefSlha=false; bool foundSlhaTag = false; bool xmlComment = false; bool decayPrinted = false; string line=""; string blockIn=""; string decay=""; string comment=""; string blockName=""; string nameNow=""; int idNow=0; double width=0.0; //Initialize line counter int iLine=0; // Read in one line at a time. while ( getline(file, line) ) { iLine++; //Rewrite string in lowercase for (unsigned int i=0;i") != string::npos) { xmlComment = false; } else if (xmlComment) continue; else if (line.find(" SLHA2 interoperability //Note: the mass basis is NOT mass-ordered in SLHA1, so be careful! //Here, the mass basis is hence by PDG code, not by mass-ordered value. if (stopmix.exists() && ! usqmix.exists() ) { //1000002 = ~uL, 1000004 = ~cL, 2000002 = ~uR, 2000004 = ~cR usqmix.set(1,1, 1.0); usqmix.set(2,2, 1.0); usqmix.set(4,4, 1.0); usqmix.set(5,5, 1.0); //Fill (1000006,2000006) sector from stopmix usqmix.set(3,3, stopmix(1,1)); usqmix.set(3,6, stopmix(1,2)); usqmix.set(6,3, stopmix(2,1)); usqmix.set(6,6, stopmix(2,2)); }; if (sbotmix.exists() && ! dsqmix.exists() ) { //1000001 = ~dL, 1000003 = ~sL, 2000001 = ~dR, 2000003 = ~sR dsqmix.set(1,1, 1.0); dsqmix.set(2,2, 1.0); dsqmix.set(4,4, 1.0); dsqmix.set(5,5, 1.0); //Fill (1000005,2000005) sector from sbotmix dsqmix.set(3,3, sbotmix(1,1)); dsqmix.set(3,6, sbotmix(1,2)); dsqmix.set(6,3, sbotmix(2,1)); dsqmix.set(6,6, sbotmix(2,2)); }; if (staumix.exists() && ! selmix.exists() ) { //1000011 = ~eL, 1000013 = ~muL, 2000011 = ~eR, 2000013 = ~muR selmix.set(1,1, 1.0); selmix.set(2,2, 1.0); selmix.set(4,4, 1.0); selmix.set(5,5, 1.0); //Fill (1000015,2000015) sector from staumix selmix.set(3,3, staumix(1,1)); selmix.set(3,6, staumix(1,2)); selmix.set(6,3, staumix(2,1)); selmix.set(6,6, staumix(2,2)); }; if (! snumix.exists() && ! snsmix.exists()) { //1000012 = ~nu_e, 1000014 = ~nu_mu, 1000016 = ~nu_tau snumix.set(1,1, 1.0); snumix.set(2,2, 1.0); snumix.set(3,3, 1.0); }; // Step 4) Check mass ordering and unitarity/orthogonality of mixing matrices // Check expected mass orderings if (mass.exists()) { // CP-even Higgs if (abs(mass(25)) > abs(mass(35)) || (modsel(3) == 1 && abs(mass(35)) > abs(mass(45))) ) message(0,"checkSpectrum","Note: Higgs sector is not mass-ordered",0); // CP-odd Higgs if (modsel(3) == 1 && abs(mass(36)) > abs(mass(46))) message(0,"checkSpectrum", "Note: CP-odd Higgs sector is not mass-ordered",0); // Neutralinos if (abs(mass(1000022)) > abs(mass(1000023)) || abs(mass(1000023)) > abs(mass(1000025)) || abs(mass(1000025)) > abs(mass(1000035)) || (modsel(3) == 1 && abs(mass(1000035)) > abs(mass(1000045))) ) message(0,"checkSpectrum","Note: Neutralino sector is not mass-ordered" ,0); // Charginos if (abs(mass(1000024)) > abs(mass(1000037)) || (modsel(3) == 1 && abs(mass(1000037)) > abs(mass(1000047))) ) message(0,"checkSpectrum","Note: Chargino sector is not mass-ordered",0); } //NMIX if (nmix.exists()) { for (int i=1;i<=4;i++) { double cn1=0.0; double cn2=0.0; for (int j=1;j<=4;j++) { cn1 += pow(nmix(i,j),2); cn2 += pow(nmix(j,i),2); } if (abs(1.0-cn1) > 1e-3 || abs(1.0-cn2) > 1e-3) { ifail=2; message(2,"checkSpectrum","NMIX is not unitary (wrong format?)",0); break; } } } //VMIX, UMIX if (vmix.exists() && umix.exists()) { // First check for non-standard "madgraph" convention // (2,2) entry not given explicitly for (int i=1;i<=2;i++) { double cu1=0.0; double cu2=0.0; double cv1=0.0; double cv2=0.0; for (int j=1;j<=2;j++) { cu1 += pow(umix(i,j),2); cu2 += pow(umix(j,i),2); cv1 += pow(vmix(i,j),2); cv2 += pow(vmix(j,i),2); } if (abs(1.0-cu1) > 1e-3 || abs(1.0-cu2) > 1e-3) { cu1 += pow(umix(1,1),2); cu2 += pow(umix(1,1),2); if (abs(1.0-cu1) > 1e-3 || abs(1.0-cu2) > 1e-3) { ifail=max(1,ifail); message(2,"checkSpectrum","UMIX is not unitary (wrong format?)",0); break; } else { // Fix madgraph non-standard convention problem message(1,"checkSpectrum","UMIX is not unitary (repaired)",0); umix.set(2,2,umix(1,1)); } } if (abs(1.0-cv1) > 1e-3 || abs(1.0-cv2) > 1e-3) { cv1 += pow(vmix(1,1),2); cv2 += pow(vmix(1,1),2); if (abs(1.0-cv1) > 1e-3 || abs(1.0-cv2) > 1e-3) { ifail=max(1,ifail); message(2,"checkSpectrum","VMIX is not unitary (wrong format?)",0); break; } else { // Fix madgraph non-standard convention problem message(1,"checkSpectrum","VMIX is not unitary (repaired)",0); vmix.set(2,2,vmix(1,1)); } } } } //STOPMIX, SBOTMIX if (stopmix.exists() && sbotmix.exists()) { for (int i=1;i<=2;i++) { double ct1=0.0; double ct2=0.0; double cb1=0.0; double cb2=0.0; for (int j=1;j<=2;j++) { ct1 += pow(stopmix(i,j),2); ct2 += pow(stopmix(j,i),2); cb1 += pow(sbotmix(i,j),2); cb2 += pow(sbotmix(j,i),2); } if (abs(1.0-ct1) > 1e-3 || abs(1.0-ct2) > 1e-3) { ifail=-1; message(2,"checkSpectrum","STOPMIX is not unitary (wrong format?)",0); break; } if (abs(1.0-cb1) > 1e-3 || abs(1.0-cb2) > 1e-3) { ifail=-1; message(2,"checkSpectrum","SBOTMIX is not unitary (wrong format?)",0); break; } } } //STAUMIX if (staumix.exists()) { for (int i=1;i<=2;i++) { double ct1=0.0; double ct2=0.0; for (int j=1;j<=2;j++) { ct1 += pow(staumix(i,j),2); ct2 += pow(staumix(j,i),2); } if (abs(1.0-ct1) > 1e-3 || abs(1.0-ct2) > 1e-3) { ifail=-1; message(2,"checkSpectrum","STAUMIX is not unitary (wrong format?)",0); break; } } } //DSQMIX if (dsqmix.exists()) { for (int i=1;i<=6;i++) { double sr=0.0; double sc=0.0; for (int j=1;j<=6;j++) { sr += pow(dsqmix(i,j),2); sc += pow(dsqmix(j,i),2); } if (abs(1.0-sr) > 1e-3 || abs(1.0-sc) > 1e-3) { ifail=-1; message(2,"checkSpectrum","DSQMIX is not unitary (wrong format?)",0); break; } } } //USQMIX if (usqmix.exists()) { for (int i=1;i<=6;i++) { double sr=0.0; double sc=0.0; for (int j=1;j<=6;j++) { sr += pow(usqmix(i,j),2); sc += pow(usqmix(j,i),2); } if (abs(1.0-sr) > 1e-3 || abs(1.0-sc) > 1e-3) { ifail=-1; message(2,"checkSpectrum","USQMIX is not unitary (wrong format?)",0); break; } } } //SELMIX if (selmix.exists()) { for (int i=1;i<=6;i++) { double sr=0.0; double sc=0.0; for (int j=1;j<=6;j++) { sr += pow(selmix(i,j),2); sc += pow(selmix(j,i),2); } if (abs(1.0-sr) > 1e-3 || abs(1.0-sc) > 1e-3) { ifail=-1; message(2,"checkSpectrum","SELMIX is not unitary (wrong format?)",0); break; } } } //NMSSM: if (modsel(3) == 1) { //NMNMIX if ( nmnmix.exists() ) { for (int i=1;i<=5;i++) { double cn1=0.0; double cn2=0.0; for (int j=1;j<=5;j++) { cn1 += pow(nmnmix(i,j),2); cn2 += pow(nmnmix(j,i),2); } if (abs(1.0-cn1) > 1e-3 || abs(1.0-cn2) > 1e-3) { ifail=-1; message(2,"checkSpectrum","NMNMIX is not unitary (wrong format?)",0); break; } } } else { ifail=-1; message(1,"checkSpectrum","MODSEL 3 = 1 (NMSSM) but no NMNMIX found",0); } //NMAMIX if ( nmamix.exists() ) { for (int i=1;i<=2;i++) { double cn1=0.0; for (int j=1;j<=3;j++) { cn1 += pow(nmamix(i,j),2); } if (abs(1.0-cn1) > 1e-3) { ifail=-1; message(2,"checkSpectrum","NMAMIX is not unitary (wrong format?)",0); } } } else { ifail=-1; message(1,"checkSpectrum","MODSEL 3 = 1 (NMSSM) but no NMAMIX found",0); } //NMHMIX if ( nmhmix.exists() ) { for (int i=1;i<=3;i++) { double cn1=0.0; double cn2=0.0; for (int j=1;j<=3;j++) { cn1 += pow(nmhmix(i,j),2); cn2 += pow(nmhmix(j,i),2); } if (abs(1.0-cn1) > 1e-3 || abs(1.0-cn2) > 1e-3) { ifail=-1; message(2,"checkSpectrum","NMHMIX is not unitary (wrong format?)",0); } } } else { ifail=-1; message(1,"checkSpectrum","MODSEL 3 = 1 (NMSSM) but no NMHMIX found",0); } //NMSSMRUN if (! nmssmrun.exists() ) { ifail=-1; message(2,"checkSpectrum","MODSEL 3 = 1 (NMSSM) but no NMSSMRUN found", 0); } } //Check for documentation if (slhaRead && ! spinfo.exists(1)) spinfo.set(1,"unknown"); if (slhaRead && ! spinfo.exists(2)) spinfo.set(2,"unknown"); if (! slhaRead && ! spinfo.exists(1)) { spinfo.set(1,"DEFAULT"); spinfo.set(2,"n/a"); } //Give status if (ifail >= 2) message(0,"checkSpectrum","one or more serious problems were found"); //Print Footer printFooter(); //Return return ifail; } //-------------------------------------------------------------------------- // Check consistency of decay tables int SusyLesHouches::checkDecays() { if (! headerPrinted) printHeader(); int iFailDecays=0; // Loop over all particles read in for (int i = 0; i < int(decays.size()); ++i) { // Shorthand LHdecayTable decTab = decays[i]; int idRes = decTab.getId(); double width = decTab.getWidth(); if (width <= 0.0 || decTab.size() == 0) continue; // Check sum of branching ratios and phase spaces double sum = 0.0; double absSum = 0.0; int decSize = decTab.size(); for (int j = 0; j < decSize; ++j) { double brat = decTab.getBrat(j); // Check phase space if (abs(brat) > 0.0) { vector idDa = decTab.getIdDa(j); double massSum=abs(mass(idRes)); for (int k=0; k"; for (int jDa=0; jDa 1e-6) { message(1,"checkDecays","sum(BR) != 1"); cout << " | offending particle: "< infoPtr->eCM()) doDiffraction = false; // Need MPI initialization for soft QCD processes, even if only first MPI. // But no need to initialize MPI if never going to use it. doMPI = settings.flag("PartonLevel:MPI"); doMPIMB = doMPI; doMPISDA = doMPI; doMPISDB = doMPI; doMPICD = doMPI; doMPIinit = doMPI; if (doNonDiff || doDiffraction) doMPIinit = true; if (!settings.flag("PartonLevel:all")) doMPIinit = false; // Initialise trial shower switch doTrial = useAsTrial; // Merging initialization. bool hasMergingHooks = (mergingHooksPtr != 0); canRemoveEvent = !doTrial && hasMergingHooks && ( mergingHooksPtr->doCKKWLMerging() || mergingHooksPtr->doNL3Merging()); canRemoveEmission = !doTrial && hasMergingHooks && ( mergingHooksPtr->doUMEPSMerging() || mergingHooksPtr->doNL3Merging() || mergingHooksPtr->doUNLOPSMerging() ); nTrialEmissions = 1; pTLastBranch = 0.0; typeLastBranch = 0; // Flags for showers: ISR and FSR. doISR = settings.flag("PartonLevel:ISR"); bool FSR = settings.flag("PartonLevel:FSR"); bool FSRinProcess = settings.flag("PartonLevel:FSRinProcess"); bool interleaveFSR = settings.flag("TimeShower:interleave"); doFSRduringProcess = FSR && FSRinProcess && interleaveFSR; doFSRafterProcess = FSR && FSRinProcess && !interleaveFSR; doFSRinResonances = FSR && settings.flag("PartonLevel:FSRinResonances"); // Some other flags. doRemnants = settings.flag("PartonLevel:Remnants"); doSecondHard = settings.flag("SecondHard:generate"); earlyResDec = settings.flag("PartonLevel:earlyResDec"); // Allow R-hadron formation. allowRH = settings.flag("RHadrons:allow"); // Possibility to allow user veto during evolution. canVetoPT = (userHooksPtr != 0) ? userHooksPtr->canVetoPT() : false; pTvetoPT = (canVetoPT) ? userHooksPtr->scaleVetoPT() : -1.; canVetoStep = (userHooksPtr != 0) ? userHooksPtr->canVetoStep() : false; nVetoStep = (canVetoStep) ? userHooksPtr->numberVetoStep() : -1; canVetoMPIStep = (userHooksPtr != 0) ? userHooksPtr->canVetoMPIStep() : false; nVetoMPIStep = (canVetoMPIStep) ? userHooksPtr->numberVetoMPIStep() : -1; canVetoEarly = (userHooksPtr != 0) ? userHooksPtr->canVetoPartonLevelEarly() : false; // Possibility to set maximal shower scale in resonance decays. canSetScale = (userHooksPtr != 0) ? userHooksPtr->canSetResonanceScale() : false; // Done with initialization only for FSR in resonance decays. if (beamAPtr == 0 || beamBPtr == 0) return true; // Flag if lepton beams, and if non-resolved ones. May change main flags. hasLeptonBeams = ( beamAPtr->isLepton() || beamBPtr->isLepton() ); hasPointLeptons = ( hasLeptonBeams && (beamAPtr->isUnresolved() || beamBPtr->isUnresolved() ) ); if (hasLeptonBeams) { doMPIMB = false; doMPISDA = false; doMPISDB = false; doMPICD = false; doMPIinit = false; } if (hasPointLeptons) { doISR = false; doRemnants = false; } // Set info and initialize the respective program elements. timesPtr->init( beamAPtr, beamBPtr); if (doISR) spacePtr->init( beamAPtr, beamBPtr); doMPIMB = multiMB.init( doMPIinit, 0, infoPtr, settings, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr, partonSystemsPtr, sigmaTotPtr, userHooksPtr); if (doSD || doDD || doSQ) doMPISDA = multiSDA.init( doMPIinit, 1, infoPtr, settings, particleDataPtr, rndmPtr, beamAPtr, beamPomBPtr, couplingsPtr, partonSystemsPtr, sigmaTotPtr, userHooksPtr); if (doSD || doDD || doSQ) doMPISDB = multiSDB.init( doMPIinit, 2, infoPtr, settings, particleDataPtr, rndmPtr, beamPomAPtr, beamBPtr, couplingsPtr, partonSystemsPtr, sigmaTotPtr, userHooksPtr); if (doCD || doSQ) doMPICD = multiCD.init( doMPIinit, 3, infoPtr, settings, particleDataPtr, rndmPtr, beamPomAPtr, beamPomBPtr, couplingsPtr, partonSystemsPtr, sigmaTotPtr, userHooksPtr); remnants.init( infoPtr, settings, rndmPtr, beamAPtr, beamBPtr, partonSystemsPtr); resonanceDecays.init( infoPtr, particleDataPtr, rndmPtr); // Succeeded, or not. multiPtr = &multiMB; if (doMPIinit && !doMPIMB) return false; if (doMPIinit && (doSD || doDD || doSQ) && (!doMPISDA || !doMPISDB)) return false; if (doMPIinit && (doCD || doSQ) && !doMPICD) return false; if (!doMPIMB || !doMPISDA || !doMPISDB || !doMPICD) doMPI = false; return true; } //-------------------------------------------------------------------------- // Function to reset PartonLevel object for trial shower usage. void PartonLevel::resetTrial() { // Clear input pointers. partonSystemsPtr->clear(); beamAPtr->clear(); beamBPtr->clear(); beamHadAPtr->clear(); beamHadBPtr->clear(); beamPomAPtr->clear(); beamPomBPtr->clear(); // Clear last branching return values. pTLastBranch = 0.0; typeLastBranch = 0; } //-------------------------------------------------------------------------- // Main routine to do the parton-level evolution. bool PartonLevel::next( Event& process, Event& event) { // Current event classification. isResolved = infoPtr->isResolved(); isResolvedA = isResolved; isResolvedB = isResolved; isResolvedC = isResolved; isDiffA = infoPtr->isDiffractiveA(); isDiffB = infoPtr->isDiffractiveB(); isDiffC = infoPtr->isDiffractiveC(); isDiff = isDiffA || isDiffB || isDiffC; isCentralDiff = isDiffC; isDoubleDiff = isDiffA && isDiffB; isSingleDiff = isDiff && !isDoubleDiff && !isCentralDiff; isNonDiff = infoPtr->isNonDiffractive(); // nHardLoop counts how many hard-scattering subsystems are to be processed. // Almost always 1, but elastic and low-mass diffraction gives 0, while // double diffraction can give up to 2. Not to be confused with SecondHard. int nHardLoop = 1; if (!isResolved) nHardLoop = (isDiff) ? decideResolvedDiff( process) : 0; // Handle unresolved subsystems. Done if no resolved ones. sizeProcess = 0; sizeEvent = 0; if (!isResolvedA || !isResolvedB || !isResolvedC) { bool physical = setupUnresolvedSys( process, event); if (!physical || nHardLoop == 0) return physical; sizeProcess = process.size(); sizeEvent = event.size(); } // Number of actual branchings. int nBranch = 0; // Number of desired branchings, negative value means no restriction. int nBranchMax = (doTrial) ? nTrialEmissions : -1; // Store merging weight. bool hasMergingHooks = (mergingHooksPtr != 0); if ( hasMergingHooks && canRemoveEvent ) mergingHooksPtr->storeWeights(infoPtr->getWeightCKKWL()); // Big outer loop to handle up to two systems (in double diffraction), // but normally one. (Not indented in following, but end clearly marked.) for (int iHardLoop = 1; iHardLoop <= nHardLoop; ++iHardLoop) { infoPtr->setCounter(20, iHardLoop); infoPtr->setCounter(21); // Classification of diffractive system: 1 = A, 2 = B, 3 = central. iDS = 0; if (isDiffA || isDiffB) iDS = (iHardLoop == 2 || !isResolvedA) ? 2 : 1; if (isDiffC) iDS = 3; // Process and event records can be out of step for diffraction. if (iHardLoop == 2) { sizeProcess = process.size(); sizeEvent = event.size(); partonSystemsPtr->clear(); } // If you need to restore then do not throw existing diffractive system. if (isDiff) { event.saveSize(); event.saveJunctionSize(); // Allow special treatment of diffractive systems. setupResolvedDiff( process); } // Prepare to do multiparton interactions; at new mass for diffraction. if (doMPIinit) multiPtr->reset(); // Special case if nondiffractive: do hardest interaction. if (isNonDiff || isDiff) { multiPtr->pTfirst(); multiPtr->setupFirstSys( process); } // Allow up to ten tries; failure possible for beam remnants. // Main cause: inconsistent colour flow at the end of the day. bool physical = true; int nRad = 0; for (int iTry = 0; iTry < NTRY; ++ iTry) { infoPtr->addCounter(21); for (int i = 22; i < 32; ++i) infoPtr->setCounter(i); // Reset flag, counters and max scales. physical = true; nMPI = (doSecondHard) ? 2 : 1; nISR = 0; nFSRinProc = 0; nFSRinRes = 0; nISRhard = 0; nFSRhard = 0; pTsaveMPI = 0.; pTsaveISR = 0.; pTsaveFSR = 0.; // Identify hard interaction system for showers. setupHardSys( process, event); // Optionally check for a veto after the hardest interaction. if (canVetoMPIStep) { doVeto = userHooksPtr->doVetoMPIStep( 1, event); // Abort event if vetoed. if (doVeto) { if (isDiff) leaveResolvedDiff( iHardLoop, process, event); return false; } } // Check matching of process scale to maximum ISR/FSR/MPI scales. double Q2Fac = infoPtr->Q2Fac(); double Q2Ren = infoPtr->Q2Ren(); bool limitPTmaxISR = (doISR) ? spacePtr->limitPTmax( event, Q2Fac, Q2Ren) : false; bool limitPTmaxFSR = (doFSRduringProcess) ? timesPtr->limitPTmax( event, Q2Fac, Q2Ren) : false; bool limitPTmaxMPI = (doMPI) ? multiPtr->limitPTmax( event) : false; // Global recoil: reset counters and store locations of outgoing partons. timesPtr->prepareGlobal( event); // Set hard scale, maximum for showers and multiparton interactions. double pTscaleRad = process.scale(); double pTscaleMPI = pTscaleRad; if (doSecondHard) { pTscaleRad = max( pTscaleRad, process.scaleSecond() ); pTscaleMPI = min( pTscaleMPI, process.scaleSecond() ); } double pTmaxMPI = (limitPTmaxMPI) ? pTscaleMPI : infoPtr->eCM(); double pTmaxISR = (limitPTmaxISR) ? spacePtr->enhancePTmax() * pTscaleRad : infoPtr->eCM(); double pTmaxFSR = (limitPTmaxFSR) ? timesPtr->enhancePTmax() * pTscaleRad : infoPtr->eCM(); // Potentially reset up starting scales for matrix element merging. if ( hasMergingHooks && (doTrial || canRemoveEvent || canRemoveEmission) ) mergingHooksPtr->setShowerStartingScales( doTrial, (canRemoveEvent || canRemoveEmission), pTscaleRad, process, pTmaxFSR, limitPTmaxFSR, pTmaxISR, limitPTmaxISR, pTmaxMPI, limitPTmaxMPI ); double pTmax = max( pTmaxMPI, max( pTmaxISR, pTmaxFSR) ); pTsaveMPI = pTmaxMPI; pTsaveISR = pTmaxISR; pTsaveFSR = pTmaxFSR; // Prepare the classes to begin the generation. if (doMPI) multiPtr->prepare( event, pTmaxMPI); if (doISR) spacePtr->prepare( 0, event, limitPTmaxISR); if (doFSRduringProcess) timesPtr->prepare( 0, event, limitPTmaxFSR); if (doSecondHard && doISR) spacePtr->prepare( 1, event, limitPTmaxISR); if (doSecondHard && doFSRduringProcess) timesPtr->prepare( 1, event, limitPTmaxFSR); // Impact parameter has now been chosen, except for diffraction. if (!isDiff) infoPtr->setImpact( multiPtr->bMPI(), multiPtr->enhanceMPI(), true); // Set up initial veto scale. doVeto = false; double pTveto = pTvetoPT; typeLatest = 0; // Need to know if first emission to allow for weak shower // to go to the scale pT2 + mW2 (mZ2) instead of just pT2. bool isFirstTrial = true; // Begin evolution down in pT from hard pT scale. do { infoPtr->addCounter(22); typeVetoStep = 0; nRad = nISR + nFSRinProc; // Find next pT value for FSR, MPI and ISR. // Order calls to minimize time expenditure. double pTgen = 0.; double pTtimes = (doFSRduringProcess) ? timesPtr->pTnext( event, pTmaxFSR, pTgen, isFirstTrial) : -1.; pTgen = max( pTgen, pTtimes); double pTmulti = (doMPI) ? multiPtr->pTnext( pTmaxMPI, pTgen, event) : -1.; pTgen = max( pTgen, pTmulti); double pTspace = (doISR) ? spacePtr->pTnext( event, pTmaxISR, pTgen, nRad, isFirstTrial) : -1.; double pTnow = max( pTtimes, max( pTmulti, pTspace)); infoPtr->setPTnow( pTnow); isFirstTrial = false; // Allow a user veto. Only do it once, so remember to change pTveto. if (pTveto > 0. && pTveto > pTnow) { pTveto = -1.; doVeto = userHooksPtr->doVetoPT( typeLatest, event); // Abort event if vetoed. if (doVeto) { if (isDiff) leaveResolvedDiff( iHardLoop, process, event); return false; } } // Do a multiparton interaction (if allowed). if (pTmulti > 0. && pTmulti > pTspace && pTmulti > pTtimes) { infoPtr->addCounter(23); if (multiPtr->scatter( event)) { typeLatest = 1; ++nMPI; if (canVetoMPIStep && nMPI <= nVetoMPIStep) typeVetoStep = 1; // Update ISR and FSR dipoles. if (doISR) spacePtr->prepare( nMPI - 1, event); if (doFSRduringProcess) timesPtr->prepare( nMPI - 1, event); } // Set maximal scales for next pT to pick. pTmaxMPI = pTmulti; pTmaxISR = min( pTmulti, pTmaxISR); pTmaxFSR = min( pTmulti, pTmaxFSR); pTmax = pTmulti; nBranch++; pTLastBranch = pTmulti; typeLastBranch = 1; } // Do an initial-state emission (if allowed). else if (pTspace > 0. && pTspace > pTtimes) { infoPtr->addCounter(24); if (spacePtr->branch( event)) { typeLatest = 2; iSysNow = spacePtr->system(); ++nISR; if (iSysNow == 0) ++nISRhard; if (canVetoStep && iSysNow == 0 && nISRhard <= nVetoStep) typeVetoStep = 2; // Update FSR dipoles. if (doFSRduringProcess) timesPtr->update( iSysNow, event); nBranch++; pTLastBranch = pTspace; typeLastBranch = 2; // Rescatter: it is possible for kinematics to fail, in which // case we need to restart the parton level processing. } else if (spacePtr->doRestart()) { physical = false; break; } // Set maximal scales for next pT to pick. pTmaxMPI = min( pTspace, pTmaxMPI); pTmaxISR = pTspace; pTmaxFSR = min( pTspace, pTmaxFSR); pTmax = pTspace; } // Do a final-state emission (if allowed). else if (pTtimes > 0.) { infoPtr->addCounter(25); if (timesPtr->branch( event, true)) { typeLatest = 3; iSysNow = timesPtr->system(); ++nFSRinProc; if (iSysNow == 0) ++nFSRhard; if (canVetoStep && iSysNow == 0 && nFSRhard <= nVetoStep) typeVetoStep = 3; // Update ISR dipoles. if (doISR) spacePtr->update( iSysNow, event); nBranch++; pTLastBranch = pTtimes; typeLastBranch = 3; } // Set maximal scales for next pT to pick. pTmaxMPI = min( pTtimes, pTmaxMPI); pTmaxISR = min( pTtimes, pTmaxISR); pTmaxFSR = pTtimes; pTmax = pTtimes; } // If no pT scales above zero then nothing to be done. else pTmax = 0.; // Optionally check for a veto after the first few interactions, // or after the first few emissions, ISR or FSR, in the hardest system. if (typeVetoStep == 1) { doVeto = userHooksPtr->doVetoMPIStep( nMPI, event); } else if (typeVetoStep > 1) { doVeto = userHooksPtr->doVetoStep( typeVetoStep, nISRhard, nFSRhard, event); } // Abort event if vetoed. if (doVeto) { if (isDiff) leaveResolvedDiff( iHardLoop, process, event); return false; } // Keep on evolving until nothing is left to be done. if (typeLatest > 0 && typeLatest < 4) infoPtr->addCounter(25 + typeLatest); if (!isDiff) infoPtr->setPartEvolved( nMPI, nISR); // Handle potential merging veto. if ( canRemoveEvent && nISRhard + nFSRhard == 1 ){ // Simply check, and possibly reset weights. mergingHooksPtr->doVetoStep( process, event ); } // End loop evolution down in pT from hard pT scale. } while (pTmax > 0. && (nBranchMax <= 0 || nBranch < nBranchMax) ); // Do all final-state emissions if not already considered above. if (doFSRafterProcess && (nBranchMax <= 0 || nBranch < nBranchMax) ) { // Find largest scale for final partons. pTmax = 0.; for (int i = 0; i < event.size(); ++i) if (event[i].isFinal() && event[i].scale() > pTmax) pTmax = event[i].scale(); pTsaveFSR = pTmax; // Prepare all subsystems for evolution. for (int iSys = 0; iSys < partonSystemsPtr->sizeSys(); ++iSys) timesPtr->prepare( iSys, event); // Set up initial veto scale. doVeto = false; pTveto = pTvetoPT; // Begin evolution down in pT from hard pT scale. do { infoPtr->addCounter(29); typeVetoStep = 0; double pTtimes = timesPtr->pTnext( event, pTmax, 0.); infoPtr->setPTnow( pTtimes); // Allow a user veto. Only do it once, so remember to change pTveto. if (pTveto > 0. && pTveto > pTtimes) { pTveto = -1.; doVeto = userHooksPtr->doVetoPT( 4, event); // Abort event if vetoed. if (doVeto) { if (isDiff) leaveResolvedDiff( iHardLoop, process, event); return false; } } // Do a final-state emission (if allowed). if (pTtimes > 0.) { infoPtr->addCounter(30); if (timesPtr->branch( event, true)) { iSysNow = timesPtr->system(); ++nFSRinProc; if (iSysNow == 0) ++nFSRhard; if (canVetoStep && iSysNow == 0 && nFSRhard <= nVetoStep) typeVetoStep = 4; nBranch++; pTLastBranch = pTtimes; typeLastBranch = 4; } pTmax = pTtimes; } // If no pT scales above zero then nothing to be done. else pTmax = 0.; // Optionally check for a veto after the first few emissions. if (typeVetoStep > 0) { doVeto = userHooksPtr->doVetoStep( typeVetoStep, nISRhard, nFSRhard, event); // Abort event if vetoed. if (doVeto) { if (isDiff) leaveResolvedDiff( iHardLoop, process, event); return false; } } // Handle potential merging veto. if ( canRemoveEvent && nISRhard + nFSRhard == 1 ){ // Simply check, and possibly reset weights. mergingHooksPtr->doVetoStep( process, event ); } // Keep on evolving until nothing is left to be done. infoPtr->addCounter(31); } while (pTmax > 0. && (nBranchMax <= 0 || nBranch < nBranchMax) ); } // Handle veto after ISR + FSR + MPI, but before beam remnants // and resonance decays, e.g. for MLM matching. if (canVetoEarly && userHooksPtr->doVetoPartonLevelEarly( event)) { doVeto = true; if (isDiff) leaveResolvedDiff( iHardLoop, process, event); return false; } if (earlyResDec) { int oldSizeSys = partonSystemsPtr->sizeSys(); // Perform showers in resonance decay chains. if(nBranchMax <= 0 || nBranch < nBranchMax) doVeto = !resonanceShowers( process, event, true); // Abort event if vetoed. if (doVeto) return false; // Reassign new decay products to original system. for (int iSys = oldSizeSys; iSys < partonSystemsPtr->sizeSys(); ++iSys) for (int iOut = 0; iOut < partonSystemsPtr->sizeOut(iSys); ++iOut) partonSystemsPtr->addOut(0, partonSystemsPtr->getOut( iSys, iOut) ); partonSystemsPtr->setSizeSys( oldSizeSys); // Perform decays and showers of W and Z emitted in shower. // To do:check if W/Z emission is on in ISR or FSR?? if (!wzDecayShowers( event)) return false; } // Add beam remnants, including primordial kT kick and colour tracing. if (!doTrial && physical && doRemnants && !remnants.add( event)) physical = false; // If no problems then done. if (physical) break; // Else restore and loop, but do not throw existing diffractive system. if (!isDiff) event.clear(); else { event.restoreSize(); event.restoreJunctionSize(); } beamAPtr->clear(); beamBPtr->clear(); partonSystemsPtr->clear(); // End loop over ten tries. Restore from diffraction. Hopefully it worked. } if (isDiff) leaveResolvedDiff( iHardLoop, process, event); if (!physical) return false; // End big outer loop to handle two systems in double diffraction. } if (!earlyResDec) { // Perform showers in resonance decay chains. if(nBranchMax <= 0 || nBranch < nBranchMax) doVeto = !resonanceShowers( process, event, true); // Abort event if vetoed. if (doVeto) return false; // Perform decays and showers of W and Z emitted in shower. // To do:check if W/Z emission is on in ISR or FSR?? if (!wzDecayShowers( event)) return false; } // Store event properties. Not available for diffraction. if (!isDiff) infoPtr->setEvolution( pTsaveMPI, pTsaveISR, pTsaveFSR, nMPI, nISR, nFSRinProc, nFSRinRes); if (isDiff) { multiPtr->setEmpty(); infoPtr->setImpact( multiPtr->bMPI(), multiPtr->enhanceMPI(), false); } // Done. return true; } //-------------------------------------------------------------------------- // Decide which diffractive subsystems are resolved (= perturbative). int PartonLevel::decideResolvedDiff( Event& process) { // Loop over two systems. int nHighMass = 0; int iDSmin = (isDiffC) ? 3 : 1; int iDSmax = (isDiffC) ? 3 : 2; for (int iDSnow = iDSmin; iDSnow <= iDSmax; ++iDSnow) { int iDiffMot = iDSnow + 2; // Only high-mass diffractive systems should be resolved. double mDiff = process[iDiffMot].m(); bool isHighMass = ( mDiff > mMinDiff && rndmPtr->flat() < pMaxDiff * ( 1. - exp( -(mDiff - mMinDiff) / mWidthDiff ) ) ); // Set outcome and done. if (isHighMass) ++nHighMass; if (iDSnow == 1) isResolvedA = isHighMass; if (iDSnow == 2) isResolvedB = isHighMass; if (iDSnow == 3) isResolvedC = isHighMass; } return nHighMass; } //-------------------------------------------------------------------------- // Set up an unresolved process, i.e. elastic or diffractive. bool PartonLevel::setupUnresolvedSys( Event& process, Event& event) { // No hard scale in event. process.scale( 0.); // Copy particles from process to event. for (int i = 0; i < process.size(); ++ i) event.append( process[i]); // Loop to find diffractively excited beams. for (iDS = 1; iDS < 4; ++iDS) if ( (iDS == 1 && isDiffA && !isResolvedA) || (iDS == 2 && isDiffB && !isResolvedB) || (iDS == 3 && isDiffC && !isResolvedC) ) { int iBeam = iDS + 2; // Diffractive mass. Boost and rotation from diffractive system // rest frame, aligned along z axis, to event cm frame. double mDiff = process[iBeam].m(); double m2Diff = mDiff * mDiff; Vec4 pDiffA = (iDS == 1) ? process[1].p() : process[1].p() - process[3].p(); Vec4 pDiffB = (iDS == 2) ? process[2].p() : process[2].p() - process[4].p(); RotBstMatrix MtoCM; MtoCM.fromCMframe( pDiffA, pDiffB); // Beam Particle used for flavour content kicked out by Pomeron. // Randomize for central diffraction; misses closed gluon loop case. bool beamSideA = (iDS == 1 || (iDS == 3 && rndmPtr->flat() < 0.5)); BeamParticle* beamPtr = (beamSideA) ? beamAPtr : beamBPtr; if (iDS == 3) beamPtr = (beamSideA) ? beamPomAPtr : beamPomBPtr; // Pick quark or gluon kicked out and flavour subdivision. beamPtr->newValenceContent(); bool gluonIsKicked = beamPtr->pickGluon(mDiff); int id1 = beamPtr->pickValence(); int id2 = beamPtr->pickRemnant(); // Find flavour masses. Scale them down if too big. double m1 = particleDataPtr->constituentMass(id1); double m2 = particleDataPtr->constituentMass(id2); if (m1 + m2 > 0.5 * mDiff) { double reduce = 0.5 * mDiff / (m1 + m2); m1 *= reduce; m2 *= reduce; } // If quark is kicked out, then trivial kinematics in rest frame. if (!gluonIsKicked) { double pAbs = sqrt( pow2(m2Diff - m1*m1 - m2*m2) - pow2(2. * m1 * m2) ) / (2. * mDiff); if (!beamSideA) pAbs = -pAbs; double e1 = (m2Diff + m1*m1 - m2*m2) / (2. * mDiff); double e2 = (m2Diff + m2*m2 - m1*m1) / (2. * mDiff); Vec4 p1( 0., 0., -pAbs, e1); Vec4 p2( 0., 0., pAbs, e2); // Boost and rotate to event cm frame. p1.rotbst( MtoCM); p2.rotbst( MtoCM); // Set colours. int col1, acol1, col2, acol2; if (particleDataPtr->colType(id1) == 1) { col1 = event.nextColTag(); acol1 = 0; col2 = 0; acol2 = col1; } else { col1 = 0; acol1 = event.nextColTag(); col2 = acol1; acol2 = 0; } // Update process colours to stay in step. process.nextColTag(); // Store partons of diffractive system and mark system decayed. int iDauBeg = event.append( id1, 23, iBeam, 0, 0, 0, col1, acol1, p1, m1); int iDauEnd = event.append( id2, 63, iBeam, 0, 0, 0, col2, acol2, p2, m2); event[iBeam].statusNeg(); event[iBeam].daughters(iDauBeg, iDauEnd); // If gluon is kicked out: share momentum between two remnants. } else { double m2Sys, zSys, pxSys, pySys, mTS1, mTS2; zSys = beamPtr->zShare(mDiff, m1, m2); // Provide relative pT kick in remnant. Construct (transverse) masses. pxSys = beamPtr->pxShare(); pySys = beamPtr->pyShare(); mTS1 = m1*m1 + pxSys*pxSys + pySys*pySys; mTS2 = m2*m2 + pxSys*pxSys + pySys*pySys; m2Sys = mTS1 / zSys + mTS2 / (1. - zSys); // Momentum of kicked-out massless gluon in diffractive rest frame. double pAbs = (m2Diff - m2Sys) / (2. * mDiff); double pLRem = (beamSideA) ? pAbs : -pAbs; Vec4 pG( 0., 0., -pLRem, pAbs); Vec4 pRem(0., 0., pLRem, mDiff - pAbs); // Momenta of the two beam remnant flavours. (Lightcone p+ = m_diff!) double e1 = 0.5 * (zSys * mDiff + mTS1 / (zSys * mDiff)); double pL1 = 0.5 * (zSys * mDiff - mTS1 / (zSys * mDiff)); if (!beamSideA) pL1 = -pL1; Vec4 p1(pxSys, pySys, pL1, e1); Vec4 p2 = pRem - p1; // Boost and rotate to event cm frame. Improve precision. pG.rotbst( MtoCM); p1.rotbst( MtoCM); p2.rotbst( MtoCM); pG.e( pG.pAbs()); // Set colours. int colG, acolG, col1, acol1, col2, acol2; if (particleDataPtr->colType(id1) == 1) { col1 = event.nextColTag(); acol1 = 0; colG = event.nextColTag(); acolG = col1; col2 = 0; acol2 = colG; } else { col1 = 0; acol1 = event.nextColTag(); colG = acol1; acolG = event.nextColTag(); col2 = acolG; acol2 = 0; } // Update process colours to stay in step. process.nextColTag(); process.nextColTag(); // Store partons of diffractive system and mark system decayed. int iDauBeg = event.append( 21, 23, iBeam, 0, 0, 0, colG, acolG, pG, 0.); event.append( id1, 63, iBeam, 0, 0, 0, col1, acol1, p1, m1); int iDauEnd = event.append( id2, 63, iBeam, 0, 0, 0, col2, acol2, p2, m2); event[iBeam].statusNeg(); event[iBeam].daughters(iDauBeg, iDauEnd); } // End loop over beams. Done. } return true; } //-------------------------------------------------------------------------- // Set up the hard process(es), excluding subsequent resonance decays. void PartonLevel::setupHardSys( Event& process, Event& event) { // Incoming partons to hard process are stored in slots 3 and 4. int inS = 0; int inP = 3; int inM = 4; // Mother and last entry of diffractive system. Offset. int iDiffMot = iDS + 2; int iDiffDau = process.size() - 1; int nOffset = sizeEvent - sizeProcess; // Resolved diffraction means more entries. if (isDiff) { inS = iDiffMot; inP = iDiffDau - 3; inM = iDiffDau - 2; // Diffractively excited particle described as Pomeron-hadron beams. event[inS].statusNeg(); event[inS].daughters( inP - 2 + nOffset, inM - 2 + nOffset); } // If two hard interactions then find where second begins. int iBeginSecond = process.size(); if (doSecondHard) { iBeginSecond = 5; while (process[iBeginSecond].status() != -21) ++iBeginSecond; } // If incoming partons are massive then recalculate to put them massless. if (process[inP].m() != 0. || process[inM].m() != 0.) { double pPos = process[inP].pPos() + process[inM].pPos(); double pNeg = process[inP].pNeg() + process[inM].pNeg(); process[inP].pz( 0.5 * pPos); process[inP].e( 0.5 * pPos); process[inP].m( 0.); process[inM].pz(-0.5 * pNeg); process[inM].e( 0.5 * pNeg); process[inM].m( 0.); } // Add incoming hard-scattering partons to list in beam remnants. double x1 = process[inP].pPos() / process[inS].m(); beamAPtr->append( inP + nOffset, process[inP].id(), x1); double x2 = process[inM].pNeg() / process[inS].m(); beamBPtr->append( inM + nOffset, process[inM].id(), x2); // Scale. Find whether incoming partons are valence or sea. Store. // When an x-dependent matter profile is used with nonDiffractive, // trial interactions mean that the valence/sea choice has already // been made and should be restored here. double scale = process.scale(); int vsc1, vsc2; beamAPtr->xfISR( 0, process[inP].id(), x1, scale*scale); if (isNonDiff && (vsc1 = multiPtr->getVSC1()) != 0) (*beamAPtr)[0].companion(vsc1); else vsc1 = beamAPtr->pickValSeaComp(); beamBPtr->xfISR( 0, process[inM].id(), x2, scale*scale); if (isNonDiff && (vsc2 = multiPtr->getVSC2()) != 0) (*beamBPtr)[0].companion(vsc2); else vsc2 = beamBPtr->pickValSeaComp(); bool isVal1 = (vsc1 == -3); bool isVal2 = (vsc2 == -3); infoPtr->setValence( isVal1, isVal2); // Initialize info needed for subsequent sequential decays + showers. nHardDone = sizeProcess; iPosBefShow.resize( process.size() ); fill( iPosBefShow.begin(), iPosBefShow.end(), 0); // Add the beam and hard subprocess partons to the event record. for (int i = sizeProcess; i < iBeginSecond; ++i) { if (process[i].mother1() > inM) break; int j = event.append(process[i]); iPosBefShow[i] = i; // Offset history if process and event not in step. if (nOffset != 0) { int iOrd = i - iBeginSecond + 7; if (iOrd == 1 || iOrd == 2) event[j].offsetHistory( 0, 0, 0, nOffset); else if (iOrd == 3 || iOrd == 4) event[j].offsetHistory( 0, nOffset, 0, nOffset); else if (iOrd == 5 || iOrd == 6) event[j].offsetHistory( 0, nOffset, 0, 0); } // Currently outgoing ones should not count as decayed. if (event[j].status() == -22) { event[j].statusPos(); event[j].daughters(0, 0); } // Complete task of copying hard subsystem into event record. ++nHardDone; } // Store participating partons as first set in list of all systems. partonSystemsPtr->addSys(); partonSystemsPtr->setInA(0, inP + nOffset); partonSystemsPtr->setInB(0, inM + nOffset); for (int i = inM + 1; i < nHardDone; ++i) partonSystemsPtr->addOut(0, i + nOffset); partonSystemsPtr->setSHat( 0, (event[inP + nOffset].p() + event[inM + nOffset].p()).m2Calc() ); partonSystemsPtr->setPTHat( 0, scale); // Identify second hard process where applicable. // Since internally generated incoming partons are guaranteed massless. if (doSecondHard) { int inP2 = iBeginSecond; int inM2 = iBeginSecond + 1; // Add incoming hard-scattering partons to list in beam remnants. // Not valid if not in rest frame?? x1 = process[inP2].pPos() / process[0].e(); beamAPtr->append( inP2, process[inP2].id(), x1); x2 = process[inM2].pNeg() / process[0].e(); beamBPtr->append( inM2, process[inM2].id(), x2); // Find whether incoming partons are valence or sea. scale = process.scaleSecond(); beamAPtr->xfISR( 1, process[inP2].id(), x1, scale*scale); beamAPtr->pickValSeaComp(); beamBPtr->xfISR( 1, process[inM2].id(), x2, scale*scale); beamBPtr->pickValSeaComp(); // Add the beam and hard subprocess partons to the event record. for (int i = inP2; i < process.size(); ++ i) { int mother = process[i].mother1(); if ( (mother > 2 && mother < inP2) || mother > inM2 ) break; event.append(process[i]); iPosBefShow[i] = i; // Currently outgoing ones should not count as decayed. if (event[i].status() == -22) { event[i].statusPos(); event[i].daughters(0, 0); } // Complete task of copying hard subsystem into event record. ++nHardDone; } // Store participating partons as second set in list of all systems. partonSystemsPtr->addSys(); partonSystemsPtr->setInA(1, inP2); partonSystemsPtr->setInB(1, inM2); for (int i = inM2 + 1; i < nHardDone; ++i) partonSystemsPtr->addOut(1, i); partonSystemsPtr->setSHat( 1, (event[inP2].p() + event[inM2].p()).m2Calc() ); partonSystemsPtr->setPTHat( 1, scale); // End code for second hard process. } // Update event colour tag to maximum in whole process. int maxColTag = 0; for (int i = 0; i < process.size(); ++ i) { if (process[i].col() > maxColTag) maxColTag = process[i].col(); if (process[i].acol() > maxColTag) maxColTag = process[i].acol(); } event.initColTag(maxColTag); // Copy junctions from process to event. for (int iJun = 0; iJun < process.sizeJunction(); ++iJun) { // Resonance decay products may not have been copied from process to // event yet. If so, do not add junctions associated with decays yet. int kindJunction = process.kindJunction(iJun); bool doCopy = true; // For junction types <= 4, check if final-state legs were copied. if (kindJunction <= 4) { int iLegF1 = (kindJunction - 1) / 2; for (int iLeg = iLegF1; iLeg <= 2; ++iLeg) { bool colFound = false; for (int i = inM + 1; i < event.size(); ++i) { int col = (kindJunction % 2 == 1) ? event[i].col() : event[i].acol(); if (col == process.colJunction(iJun,iLeg)) colFound = true; } if (!colFound) doCopy = false; } } if (doCopy) event.appendJunction( process.getJunction(iJun)); } // Done. } //-------------------------------------------------------------------------- // Set up the event for subsequent resonance decays and showers. void PartonLevel::setupShowerSys( Event& process, Event& event) { // Reset event record to only contain line 0. event.clear(); event.append( process[0]); // Initialize info needed for subsequent sequential decays + showers. nHardDone = 1; iPosBefShow.resize( process.size()); fill( iPosBefShow.begin(), iPosBefShow.end(), 0); // Add the hard subprocess partons to the event record. for (int i = 1; i < process.size(); ++i) { if (process[i].mother1() > 0) break; int j = event.append(process[i]); iPosBefShow[i] = i; // Currently outgoing ones should not count as decayed. if (event[j].status() == -22) { event[j].statusPos(); event[j].daughters(0, 0); } // Complete task of copying hard subsystem into event record. ++nHardDone; } // Store participating partons as first set in list of all systems. partonSystemsPtr->clear(); partonSystemsPtr->addSys(); for (int i = 1; i < nHardDone; ++i) partonSystemsPtr->addOut(0, i); partonSystemsPtr->setSHat( 0, pow2(process[0].m()) ); partonSystemsPtr->setPTHat( 0, 0.5 * process[0].m() ); // Copy junctions from process to event. for (int iJun = 0; iJun < process.sizeJunction(); ++iJun) { // Resonance decay products may not have been copied from process to // event yet. If so, do not add junctions associated with decays yet. int kindJunction = process.kindJunction(iJun); bool doCopy = true; // For junction types <= 4, check if final-state legs were copied. if (kindJunction <= 4) { int iLegF1 = (kindJunction - 1) / 2; for (int iLeg = iLegF1; iLeg <= 2; ++iLeg) { bool colFound = false; for (int i = 1; i < event.size(); ++i) { int col = (kindJunction % 2 == 1) ? event[i].col() : event[i].acol(); if (col == process.colJunction(iJun,iLeg)) colFound = true; } if (!colFound) doCopy = false; } } if (doCopy) event.appendJunction( process.getJunction(iJun)); } // Done. } //-------------------------------------------------------------------------- // Resolved diffraction: replace full event with diffractive subsystem. void PartonLevel::setupResolvedDiff( Event& process) { // Mother and last entry of diffractive system. int iDiffMot = iDS + 2; int iDiffDau = process.size() - 1; // Diffractively excited particle to be replaced by Pomeron-hadron beams // (or Pomeron-Pomeron beams for central diffraction). process[iDiffMot].statusNeg(); process[iDiffMot].daughters( iDiffDau + 1, iDiffDau + 2); // Diffractive system mass. double mDiff = process[iDiffMot].m(); double m2Diff = mDiff * mDiff; // Set up Pomeron-proton or Pomeron-Pomeron system as if it were // the complete collision. Set Pomeron "beam particle" massless. int idDiffA = (iDS == 1) ? process[1].id() : 990; int idDiffB = (iDS == 2) ? process[2].id() : 990; double mDiffA = (iDS == 1) ? process[1].m() : 0.; double mDiffB = (iDS == 2) ? process[2].m() : 0.; double m2DiffA = mDiffA * mDiffA; double m2DiffB = mDiffB * mDiffB; double eDiffA = 0.5 * (m2Diff + m2DiffA - m2DiffB) / mDiff; double eDiffB = 0.5 * (m2Diff + m2DiffB - m2DiffA) / mDiff; double pzDiff = 0.5 * sqrtpos( pow2(m2Diff - m2DiffA - m2DiffB) - 4. * m2DiffA * m2DiffB ) / mDiff; process.append( idDiffA, 13, iDiffMot, 0, 0, 0, 0, 0, 0., 0., pzDiff, eDiffA, mDiffA); process.append( idDiffB, 13, iDiffMot, 0, 0, 0, 0, 0, 0., 0., -pzDiff, eDiffB, mDiffB); // Reassign beam pointers to refer to subsystem effective beams. beamAPtr = (iDS == 1) ? beamHadAPtr : beamPomAPtr; beamBPtr = (iDS == 2) ? beamHadBPtr : beamPomBPtr; // Pretend that the diffractive system is the whole collision. eCMsave = infoPtr->eCM(); infoPtr->setECM( mDiff); beamAPtr->newPzE( pzDiff, eDiffA); beamBPtr->newPzE( -pzDiff, eDiffB); // Beams not found in normal slots 1 and 2. int beamOffset = (sizeEvent > 0) ? sizeEvent - 1 : 4; // Reassign beam pointers in other classes. timesPtr->reassignBeamPtrs( beamAPtr, beamBPtr, beamOffset); spacePtr->reassignBeamPtrs( beamAPtr, beamBPtr, beamOffset); remnants.reassignBeamPtrs( beamAPtr, beamBPtr, iDS); // Reassign multiparton interactions pointer to right object. if (iDS == 1) multiPtr = &multiSDA; else if (iDS == 2) multiPtr = &multiSDB; else multiPtr = &multiCD; } //-------------------------------------------------------------------------- // Resolved diffraction: restore to original behaviour. void PartonLevel::leaveResolvedDiff( int iHardLoop, Event& process, Event& event) { // Reconstruct boost and rotation to event cm frame. Vec4 pDiffA = (iDS == 1) ? process[1].p() : process[1].p() - process[3].p(); Vec4 pDiffB = (iDS == 2) ? process[2].p() : process[2].p() - process[4].p(); RotBstMatrix MtoCM; MtoCM.fromCMframe( pDiffA, pDiffB); // Perform rotation and boost on diffractive system. for (int i = sizeProcess; i < process.size(); ++i) process[i].rotbst( MtoCM); int iFirst = (iHardLoop == 1) ? 5 + sizeEvent - sizeProcess : sizeEvent; if(isDiffC) iFirst = 6 + sizeEvent - sizeProcess; for (int i = iFirst; i < event.size(); ++i) event[i].rotbst( MtoCM); // Restore cm energy. infoPtr->setECM( eCMsave); beamAPtr->newPzE( event[1].pz(), event[1].e()); beamBPtr->newPzE( event[2].pz(), event[2].e()); // Restore beam pointers to incoming hadrons. beamAPtr = beamHadAPtr; beamBPtr = beamHadBPtr; // Reassign beam pointers in other classes. timesPtr->reassignBeamPtrs( beamAPtr, beamBPtr, 0); spacePtr->reassignBeamPtrs( beamAPtr, beamBPtr, 0); remnants.reassignBeamPtrs( beamAPtr, beamBPtr, 0); // Restore multiparton interactions pointer to default object. multiPtr = &multiMB; } //-------------------------------------------------------------------------- // Handle showers in successive resonance decays. bool PartonLevel::resonanceShowers( Event& process, Event& event, bool skipForR) { // Prepare to start over from beginning for R-hadron decays. if (allowRH) { if (skipForR) { nHardDoneRHad = nHardDone; inRHadDecay.resize(0); for (int i = 0; i < process.size(); ++i) inRHadDecay.push_back( false); } else nHardDone = nHardDoneRHad; } // Isolate next system to be processed, if anything remains. int nRes = 0; int nFSRres = 0; // Number of desired branchings, negative value means no restriction. int nBranchMax = (doTrial) ? nTrialEmissions : -1; // Vector to tell which junctions have already been copied vector iJunCopied; while (nHardDone < process.size()) { ++nRes; int iBegin = nHardDone; // In first call (skipForR = true) skip over resonances // that should form R-hadrons, and their daughters. if (allowRH) { if (skipForR) { bool comesFromR = false; int iTraceUp = iBegin; do { if ( rHadronsPtr->givesRHadron(process[iTraceUp].id()) ) comesFromR = true; iTraceUp = process[iTraceUp].mother1(); } while (iTraceUp > 0 && !comesFromR); if (comesFromR) { inRHadDecay[iBegin] = true; ++nHardDone; continue; } // In optional second call (skipForR = false) process decay chains // inside R-hadrons. } else if (!inRHadDecay[iBegin]) { ++nHardDone; continue; } } // Mother in hard process and in complete event (after shower). int iHardMother = process[iBegin].mother1(); Particle& hardMother = process[iHardMother]; int iBefMother = iPosBefShow[iHardMother]; int iAftMother = event.iBotCopyId(iBefMother); // Possibly trace across intermediate R-hadron state. if (allowRH) { int iTraceRHadron = rHadronsPtr->trace( iAftMother); if (iTraceRHadron > 0) iAftMother = iTraceRHadron; } Particle& aftMother = event[iAftMother]; // From now on mother counts as decayed. aftMother.statusNeg(); // Mother can have been moved by showering (in any of previous steps), // so prepare to update colour and momentum information for system. int colBef = hardMother.col(); int acolBef = hardMother.acol(); int colAft = aftMother.col(); int acolAft = aftMother.acol(); RotBstMatrix M; M.bst( hardMother.p(), aftMother.p()); // Extract next partons from hard event into normal event record. vector doCopyJun; for (int i = iBegin; i < process.size(); ++i) { if (process[i].mother1() != iHardMother) break; int iNow = event.append( process[i] ); iPosBefShow[i] = iNow; Particle& now = event.back(); // Currently outgoing ones should not count as decayed. if (now.status() == -22) { now.statusPos(); now.daughters(0, 0); } // Update daughter and mother information. if (i == iBegin) event[iAftMother].daughter1( iNow); else event[iAftMother].daughter2( iNow); now.mother1(iAftMother); // Check if this parton carries a junction color in hard event. for (int iJun = 0; iJun < process.sizeJunction(); ++iJun) { if (iJun >= int(doCopyJun.size())) doCopyJun.push_back(false); // Only consider junctions that can appear in decays. int kindJunction = process.kindJunction(iJun); if (kindJunction >= 5) continue; int col = (kindJunction % 2 == 1) ? now.col() : now.acol(); int iLegF1 = (kindJunction - 1) / 2; for (int iLeg = iLegF1; iLeg <= 2; ++iLeg) if (col == process.colJunction(iJun,iLeg)) doCopyJun[iJun] = true; } // Update colour and momentum information. if (now.col() == colBef) now.col( colAft); if (now.acol() == acolBef) now.acol( acolAft); now.rotbst( M); // Update vertex information. if (now.hasVertex()) now.vProd( aftMother.vDec() ); // Complete task of copying next subsystem into event record. ++nHardDone; } int iEnd = nHardDone - 1; // Copy down junctions from hard event into normal event record. for (int iJun = 0; iJun < int(doCopyJun.size()); ++iJun) { // Check if this junction was already copied for (int jJun = 0; jJun < int(iJunCopied.size()); ++jJun) if (iJunCopied[jJun] == iJun) doCopyJun[iJun] = false; // Skip if not doing anything if (!doCopyJun[iJun]) continue; // Check for changed colors and update as necessary. Junction junCopy = process.getJunction(iJun); for (int iLeg = 0; iLeg <= 2; ++iLeg) { int colLeg = junCopy.col(iLeg); if (colLeg == colBef) junCopy.col(iLeg, colAft); if (colLeg == acolBef) junCopy.col(iLeg, acolAft); } event.appendJunction(junCopy); // Mark junction as copied (to avoid later recopying) iJunCopied.push_back(iJun); } // Reset pT of last branching pTLastBranch = 0.0; // Do parton showers inside subsystem: maximum scale by mother mass. if (doFSRinResonances) { double pTmax = 0.5 * hardMother.m(); if (canSetScale) pTmax = userHooksPtr->scaleResonance( iAftMother, event); nFSRhard = 0; // Set correct scale for trial showers. if (doTrial) pTmax = process.scale(); // Add new system, automatically with two empty beam slots. int iSys = partonSystemsPtr->addSys(); partonSystemsPtr->setSHat(iSys, pow2(hardMother.m()) ); partonSystemsPtr->setPTHat(iSys, 0.5 * hardMother.m() ); // Loop over allowed range to find all final-state particles. for (int i = iPosBefShow[iBegin]; i <= iPosBefShow[iEnd]; ++i) if (event[i].isFinal()) partonSystemsPtr->addOut( iSys, i); // Let prepare routine do the setup. timesDecPtr->prepare( iSys, event); // Number of actual branchings int nBranch = 0; // Set up initial veto scale. doVeto = false; double pTveto = pTvetoPT; // Begin evolution down in pT from hard pT scale. do { typeVetoStep = 0; double pTtimes = timesDecPtr->pTnext( event, pTmax, 0.); // Allow a user veto. Only do it once, so remember to change pTveto. if (pTveto > 0. && pTveto > pTtimes) { pTveto = -1.; doVeto = userHooksPtr->doVetoPT( 5, event); // Abort event if vetoed. if (doVeto) return false; } // Do a final-state emission (if allowed). if (pTtimes > 0.) { if (timesDecPtr->branch( event)) { ++nFSRres; ++nFSRhard; if (canVetoStep && nFSRhard <= nVetoStep) typeVetoStep = 5; nBranch++; pTLastBranch = pTtimes; typeLastBranch = 5; } pTmax = pTtimes; } // If no pT scales above zero then nothing to be done. else pTmax = 0.; // Optionally check for a veto after the first few emissions. if (typeVetoStep > 0) { doVeto = userHooksPtr->doVetoStep( typeVetoStep, 0, nFSRhard, event); // Abort event if vetoed. if (doVeto) return false; } // Handle potential merging veto. if ( canRemoveEvent && nFSRhard == 1 ) { // Simply check, and possibly reset weights. mergingHooksPtr->doVetoStep( process, event, true ); } // Keep on evolving until nothing is left to be done. } while (pTmax > 0. && (nBranchMax <= 0 || nBranch < nBranchMax) ); } // No more systems to be processed. Set total number of emissions. } if (skipForR) nFSRinRes = nFSRres; return true; } //-------------------------------------------------------------------------- // Perform decays and showers of W and Z emitted in shower. bool PartonLevel::wzDecayShowers( Event& event) { // Identify W/Z produced by a parton shower. for (int iWZ = 0; iWZ < event.size(); ++iWZ) if (event[iWZ].isFinal() && (event[iWZ].id() == 23 || event[iWZ].idAbs() == 24) ) { int iWZtop = event[iWZ].iTopCopy(); int typeWZ = 0; if (event[iWZtop].statusAbs() == 56) typeWZ = 1; if (event[iWZtop].statusAbs() == 47) typeWZ = 2; int sizeSave = event.size(); // Map id_Z = 23 -> 93 and id_W = 24 -> 94, for separate decay settings. // Let W/Z resonance decay. Restore correct identity and status codes. if (typeWZ > 0) { int idSave = event[iWZ].id(); event[iWZ].id( (idSave > 0) ? idSave + 70 : idSave - 70); int statusSave = event[iWZ].status(); resonanceDecays.next( event, iWZ); event[iWZ].id( idSave); event[iWZ].status( -statusSave); if (event.size() - sizeSave != 2) { infoPtr->errorMsg("Error in PartonLevel::wzDecayShowers: " "not two decay products"); return false; } } // FSR decays. if (typeWZ == 1) { // Identify fermion after W/Z emission. vector iSisters = event[iWZtop].sisterList(); if (iSisters.size() != 1) { infoPtr->errorMsg("Error in PartonLevel::wzDecayShowers: " "Not able to find a single sister particle"); return false; } int iEmitter = iSisters[0]; // Boosts to study decay in W/Z rest frame. RotBstMatrix MtoNew, MtoRest, MtoCM; MtoNew.bst( event[iWZtop].p(), event[iWZ].p()); MtoRest.bstback( event[iWZ].p()); MtoCM.bst( event[iWZ].p()); // Emitter and recoiler in W/Z rest frame. Vec4 pEmitter = event[iEmitter].p(); pEmitter.rotbst( MtoNew); pEmitter.rotbst( MtoRest); if (event[iWZtop + 1].statusAbs() != 52) { infoPtr->errorMsg("Error in PartonLevel::wzDecayShowers: " "Found wrong recoiler"); return false; } Vec4 pRecoiler = event[iWZtop + 1].p(); pRecoiler.rotbst( MtoNew); pRecoiler.rotbst( MtoRest); Vec4 pWZRest = event[iWZ].p(); pWZRest.rotbst( MtoRest); // Always choose p4 as the particle and p5 as the anti-particle. Vec4 p4 = pEmitter; Vec4 p5 = pRecoiler; if (event[iEmitter].id() < 0) swap( p4, p5); // Decay daughters in W/Z rest frame. // Always choose pDec1 as the particle and p2Dec as the anti-particle. Vec4 pDec1 = event[sizeSave].p(); Vec4 pDec2 = event[sizeSave + 1].p(); if (event[sizeSave].id() < 0) swap( pDec1, pDec2); pDec1.rotbst( MtoRest); pDec2.rotbst( MtoRest); // Couplings. double li2, ri2, lf2, rf2; // Z couplings: make use of initial fermion polarization if set. if (event[iWZ].id() == 23) { li2 = pow2(couplingsPtr->lf( event[iEmitter].idAbs() )); ri2 = pow2(couplingsPtr->rf( event[iEmitter].idAbs() )); lf2 = pow2(couplingsPtr->lf( event[sizeSave].idAbs() )); rf2 = pow2(couplingsPtr->rf( event[sizeSave].idAbs() )); if ( abs( event[iEmitter].pol() + 1.) < 0.1) ri2 = 0.; if ( abs( event[iEmitter].pol() - 1.) < 0.1) li2 = 0.; // W couplings. } else { li2 = 1.; ri2 = 0.; lf2 = 1.; rf2 = 0.; } // Different needed kinematic variables. double sWZER = (p4 + pWZRest + p5).m2Calc(); double x1 = 2. * p4 * (p4 + pWZRest + p5) / sWZER; double x2 = 2. * p5 * (p4 + pWZRest + p5) / sWZER; double x1s = x1 * x1; double x2s = x2 * x2; double m2Sel = pWZRest.m2Calc(); double rWZER = m2Sel / sWZER; // Calculate constants needed in correction. double con[9]; con[0] = 2. * m2Sel * (1.-x1) * ((x2s+1.-x1-x2) - rWZER * (1.-x2)) * (li2 * lf2 + ri2 * rf2); con[1] = 2. * m2Sel * (1.-x2) * ((x1s+1.-x1-x2) - rWZER * (1.-x1)) * (li2 * rf2 + ri2 * lf2); con[2] = 2. * m2Sel * (1.-x1) * ((x2s+1.-x1-x2) - rWZER * (1.-x2)) * (li2 * rf2 + ri2 * lf2); con[3] = 2. * m2Sel * (1.-x2) * ((x1s+1.-x1-x2) - rWZER * (1.-x1)) * (li2 * lf2 + ri2 * rf2); con[4] = m2Sel * sWZER * (1.-x1) * (1.-x2) * ((x1+x2-1.) + rWZER) * (li2 + ri2) * (lf2 + rf2); con[5] = -4. * (1.-x1) * (1.-x2) * (li2 + ri2) * (lf2 + rf2); con[6] = -4. * (1.-x1) * (1.-x2) * (li2 + ri2) * (lf2 + rf2); con[7] = 4. * (1.-x1) * ((1.-x1) - rWZER * (1.-x2)) * (li2 + ri2) * (lf2 + rf2); con[8] = 4. * (1.-x2) * ((1.-x2) - rWZER * (1.-x1)) * (li2 + ri2) * (lf2 + rf2); // Find maximum value: try pDec1 and pDec2 = -pDec1 along +-x, +-y, +-z. double wtMax = 0.; double pAbs12 = pDec1.pAbs(); for (int j = 0; j < 6; ++j) { Vec4 pDec1Test( 0., 0., 0., pDec1.e()); Vec4 pDec2Test( 0., 0., 0., pDec2.e()); if (j == 0) { pDec1Test.px( pAbs12); pDec1Test.px( -pAbs12);} else if (j == 1) { pDec1Test.px( -pAbs12); pDec1Test.px( pAbs12);} else if (j == 2) { pDec1Test.py( pAbs12); pDec1Test.py( -pAbs12);} else if (j == 3) { pDec1Test.py( -pAbs12); pDec1Test.py( pAbs12);} else if (j == 4) { pDec1Test.pz( pAbs12); pDec1Test.pz( -pAbs12);} else if (j == 5) { pDec1Test.pz( -pAbs12); pDec1Test.pz( pAbs12);} // Evaluate matrix element and compare with current maximum. double p2p4Test = p4 * pDec1Test; double p3p4Test = p4 * pDec2Test; double p2p5Test = p5 * pDec1Test; double p3p5Test = p5 * pDec2Test; double testValues[9] = { p2p4Test, p2p5Test, p3p4Test, p3p5Test, 1., p2p5Test * p3p4Test, p2p4Test * p3p5Test, p2p4Test * p3p4Test, p2p5Test * p3p5Test}; double wtTest = 0.; for (int i = 0; i < 9; ++i) wtTest += con[i] * testValues[i]; if (wtTest > wtMax) wtMax = wtTest; } // Multiply by four to ensure maximum is an overestimate. wtMax *= 4.; // Iterate with new angles until weighting succeeds. int nRot = -1; double wt = 0.; do { ++nRot; if (nRot > 0) { RotBstMatrix MrndmRot; MrndmRot.rot( acos(2. * rndmPtr->flat() - 1.), 2. * M_PI * rndmPtr->flat()); pDec1.rotbst(MrndmRot); pDec2.rotbst(MrndmRot); } // p2 is decay product, p3 is anti decay product, // p4 is dipole particle, p5 is dipole anti particle. // So far assumed that we always have qQ-dipole. double p2p4 = p4 * pDec1; double p3p4 = p4 * pDec2; double p2p5 = p5 * pDec1; double p3p5 = p5 * pDec2; // Calculate weight and compare with maximum weight. double wtValues[9] = { p2p4, p2p5, p3p4, p3p5, 1., p2p5 * p3p4, p2p4 * p3p5, p2p4 * p3p4, p2p5 * p3p5}; wt = 0.; for (int i = 0; i < 9; ++i) wt += con[i] * wtValues[i]; if (wt > wtMax || wt < 0.) { infoPtr->errorMsg("Error in PartonLevel::wzDecayShowers: " "wt bigger than wtMax or less than zero"); return false; } } while (wt < wtMax * rndmPtr->flat()); // If momenta rotated then store new ones. if (nRot > 0) { pDec1.rotbst( MtoCM); pDec2.rotbst( MtoCM); if(event[sizeSave].id() > 0) { event[sizeSave].p( pDec1); event[sizeSave + 1].p( pDec2); } else { event[sizeSave].p( pDec2); event[sizeSave + 1].p( pDec1); } } } // ISR decays. if (typeWZ == 2) { // Identify mother of W/Z emission. double iMother = event[iWZtop].mother1(); // Boosts to study decay in W/Z rest frame. RotBstMatrix MtoNew, MtoRest, MtoCM; MtoNew.bst( event[iWZtop].p(), event[iWZ].p()); MtoRest.bstback( event[iWZ].p()); MtoCM.bst( event[iWZ].p()); // Find recoiler. int iRecoiler; if (event[iMother + 1].statusAbs() == 42) iRecoiler = iMother + 1; else if(event[iMother - 1].statusAbs() == 42) iRecoiler = iMother - 1; else { infoPtr->errorMsg("Error in PartonLevel::wzDecayShowers: " "Found wrong recoiler"); return false; } // Emitter and recoiler in W/Z rest frame. Vec4 pMother = event[iMother].p(); pMother.rotbst( MtoNew); pMother.rotbst( MtoRest); Vec4 pRecoiler = event[iRecoiler].p(); pRecoiler.rotbst( MtoNew); pRecoiler.rotbst( MtoRest); Vec4 pWZRest = event[iWZ].p(); pWZRest.rotbst( MtoRest); // Always choose p1 as the particle and p2 as the anti-particle. // If no anti-particles just continue. Vec4 p1 = pMother; Vec4 p2 = pRecoiler; if (event[iMother].id() < 0) swap( p1, p2); // Decay daughters in W/Z rest frame. // Always choose pDec1 as the particle and p2Dec as the anti-particle. Vec4 pDec1 = event[sizeSave].p(); Vec4 pDec2 = event[sizeSave + 1].p(); if (event[sizeSave].id() < 0) swap( pDec1, pDec2); pDec1.rotbst( MtoRest); pDec2.rotbst( MtoRest); // Couplings. double li2, ri2, lf2, rf2; // Z couplings: make use of initial fermion polarization if set. if (event[iWZ].id() == 23) { li2 = pow2(couplingsPtr->lf( event[iMother].idAbs() )); ri2 = pow2(couplingsPtr->rf( event[iMother].idAbs() )); lf2 = pow2(couplingsPtr->lf( event[sizeSave].idAbs() )); rf2 = pow2(couplingsPtr->rf( event[sizeSave].idAbs() )); if ( abs( event[iMother].pol() + 1.) < 0.1) ri2 = 0.; if ( abs( event[iMother].pol() - 1.) < 0.1) li2 = 0.; // W couplings. } else { li2 = 1.; ri2 = 0.; lf2 = 1.; rf2 = 0.; } // Different needed kinematic variables. double s = (p1 + p2).m2Calc(); double t = (p1-pWZRest).m2Calc(); double u = (p2-pWZRest).m2Calc(); double m2Sel = pWZRest.m2Calc(); double m2Final = t + u + s - m2Sel; // Calculate constants needed in correction. double con[9]; con[0] = 2. * m2Sel * (u * (1. - m2Final / t) + s) * (li2 * rf2 + ri2 * lf2); con[1] = 2. * m2Sel * (u * (1. - m2Final / t) + s) * (li2 * lf2 + ri2 * rf2); con[2] = 2. * m2Sel * (t * (1. - m2Final / u) + s) * (li2 * lf2 + ri2 * rf2); con[3] = 2. * m2Sel * (t * (1. - m2Final / u) + s) * (li2 * rf2 + ri2 * lf2); con[4] = m2Sel * m2Final * s * (li2 + ri2) * (lf2 + rf2); con[5] = -4. * m2Final * (li2 + ri2) * (lf2 + rf2); con[6] = -4. * m2Final * (li2 + ri2) * (lf2 + rf2); con[7] = 4. * (m2Final * u / t - m2Sel) * (li2 + ri2) * (lf2 + rf2); con[8] = 4. * (m2Final * t / u - m2Sel) * (li2 + ri2) * (lf2 + rf2); // Find maximum value: try pDec1 and pDec2 = -pDec1 along +-x, +-y, +-z. double wtMax = 0.; double pAbs12 = pDec1.pAbs(); for (int j = 0; j < 6; ++j) { Vec4 pDec1Test( 0., 0., 0., pDec1.e()); Vec4 pDec2Test( 0., 0., 0., pDec2.e()); if (j == 0) { pDec1Test.px( pAbs12); pDec1Test.px( -pAbs12);} else if (j == 1) { pDec1Test.px( -pAbs12); pDec1Test.px( pAbs12);} else if (j == 2) { pDec1Test.py( pAbs12); pDec1Test.py( -pAbs12);} else if (j == 3) { pDec1Test.py( -pAbs12); pDec1Test.py( pAbs12);} else if (j == 4) { pDec1Test.pz( pAbs12); pDec1Test.pz( -pAbs12);} else if (j == 5) { pDec1Test.pz( -pAbs12); pDec1Test.pz( pAbs12);} // Evaluate matrix element and compare with current maximum. double p1p4Test = p1 * pDec1Test; double p1p5Test = p1 * pDec2Test; double p2p4Test = p2 * pDec1Test; double p2p5Test = p2 * pDec2Test; double testValues[9] = { p1p4Test, p1p5Test, p2p4Test, p2p5Test, 1., p1p4Test * p2p5Test, p1p5Test * p2p4Test, p1p4Test * p1p5Test, p2p4Test * p2p5Test}; double wtTest = 0.; for (int i = 0; i < 9; ++i) wtTest += con[i] * testValues[i]; if (wtTest > wtMax) wtMax = wtTest; } // Multiply by four to ensure maximum is an overestimate. wtMax *= 4.; // Iterate with new angles until weighting succeeds. int nRot = -1; double wt = 0.; do { ++nRot; if (nRot > 0) { RotBstMatrix MrndmRot; MrndmRot.rot( acos(2. * rndmPtr->flat() - 1.), 2. * M_PI * rndmPtr->flat()); pDec1.rotbst(MrndmRot); pDec2.rotbst(MrndmRot); } // p2 is decay product, p3 is anti decay product, // p4 is dipole particle, p5 is dipole anti particle. // So far assumed that we always have qQ-dipole. double p1p4 = p1 * pDec1; double p1p5 = p1 * pDec2; double p2p4 = p2 * pDec1; double p2p5 = p2 * pDec2; // Calculate weight and compare with maximum weight. double wtValues[9] = { p1p4, p1p5, p2p4, p2p5, 1., p1p4 * p2p5, p1p5 * p2p4, p1p4 * p1p5, p2p4 * p2p5}; wt = 0.; for (int i = 0; i < 9; ++i) wt += con[i] * wtValues[i]; if (wt > wtMax || wt < 0.) { infoPtr->errorMsg("Error in PartonLevel::wzDecayShowers: " "wt bigger than wtMax or less than zero"); return false; } } while (wt < wtMax * rndmPtr->flat()); // If momenta rotated then store new ones. if (nRot > 0) { pDec1.rotbst( MtoCM); pDec2.rotbst( MtoCM); if(event[sizeSave].id() > 0) { event[sizeSave].p( pDec1); event[sizeSave + 1].p( pDec2); } else { event[sizeSave].p( pDec2); event[sizeSave + 1].p( pDec1); } } } // Do parton showers inside subsystem: maximum scale by mother mass. if (typeWZ > 0 && doFSRinResonances) { double pTmax = 0.5 * event[iWZ].m(); // Add new system, automatically with two empty beam slots. int iSys = partonSystemsPtr->addSys(); partonSystemsPtr->setSHat(iSys, pow2(event[iWZ].m()) ); partonSystemsPtr->setPTHat(iSys, pTmax ); for (int i = sizeSave; i < event.size(); ++i) partonSystemsPtr->addOut( iSys, i); // Let prepare routine do the setup. timesDecPtr->prepare( iSys, event); // Begin evolution down in pT from hard pT scale. do { double pTtimes = timesDecPtr->pTnext( event, pTmax, 0.); // Do a final-state emission (if allowed). if (pTtimes > 0.) { timesDecPtr->branch( event); pTmax = pTtimes; } // If no pT scales above zero then nothing to be done. else pTmax = 0.; // Keep on evolving until nothing is left to be done. } while (pTmax > 0.); } // End loop over event to find W/Z gauge bosons. } // Done. return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/StandardModel.cc0000644000175000017500000005076012217346252016164 0ustar sunsun// StandardModel.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the AlphaStrong class. #include "Pythia8/StandardModel.h" namespace Pythia8 { //========================================================================== // The AlphaStrong class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of iterations to determine Lambda from given alpha_s. const int AlphaStrong::NITER = 10; // Masses: m_c, m_b, m_t, m_Z. // Used for flavour thresholds and normalization scale. const double AlphaStrong::MC = 1.5; const double AlphaStrong::MB = 4.8; const double AlphaStrong::MT = 171.0; const double AlphaStrong::MZ = 91.188; // Always evaluate running alpha_s above Lambda3 to avoid disaster. // Safety margin picked to freeze roughly for alpha_s = 10. const double AlphaStrong::SAFETYMARGIN1 = 1.07; const double AlphaStrong::SAFETYMARGIN2 = 1.33; // CMW factor for 3, 4, 5, and 6 flavours. const double AlphaStrong::FACCMW3 = 1.661; const double AlphaStrong::FACCMW4 = 1.618; const double AlphaStrong::FACCMW5 = 1.569; const double AlphaStrong::FACCMW6 = 1.513; //-------------------------------------------------------------------------- // Initialize alpha_strong calculation by finding Lambda values etc. void AlphaStrong::init( double valueIn, int orderIn, int nfmaxIn, bool useCMWIn) { // Order of alpha_s evaluation.Default values. valueRef = valueIn; order = max( 0, min( 2, orderIn ) ); nfmax = max(5,min(6,nfmaxIn)); useCMW = useCMWIn; lastCallToFull = false; Lambda3Save = Lambda4Save = Lambda5Save = Lambda6Save = scale2Min = 0.; // Fix alpha_s. if (order == 0) { // First order alpha_s: match at flavour thresholds. } else if (order == 1) { Lambda5Save = MZ * exp( -6. * M_PI / (23. * valueRef) ); Lambda6Save = Lambda5Save * pow(Lambda5Save/MT, 2./21.); Lambda4Save = Lambda5Save * pow(MB/Lambda5Save, 2./25.); Lambda3Save = Lambda4Save * pow(MC/Lambda4Save, 2./27.); // Second order alpha_s: iterative match at flavour thresholds. } else { // The one-loop coefficients: b1 / b0^2 double b16 = 234. / 441.; double b15 = 348. / 529.; double b14 = 462. / 625.; double b13 = 576. / 729.; // The two-loop coefficients: b2 * b0 / b1^2 double b26 = -36855. / 109512.; double b25 = 224687. / 242208.; double b24 = 548575. / 426888.; double b23 = 938709. / 663552.; double logScale, loglogScale, correction, valueIter; // Find Lambda_5 at m_Z. Lambda5Save = MZ * exp( -6. * M_PI / (23. * valueRef) ); for (int iter = 0; iter < NITER; ++iter) { logScale = 2. * log(MZ/Lambda5Save); loglogScale = log(logScale); correction = 1. - b15 * loglogScale / logScale + pow2(b15 / logScale) * (pow2(loglogScale - 0.5) + b25 - 1.25); valueIter = valueRef / correction; Lambda5Save = MZ * exp( -6. * M_PI / (23. * valueIter) ); } // Find Lambda_6 at m_t. double logScaleT = 2. * log(MT/Lambda5Save); double loglogScaleT = log(logScaleT); double valueT = 12. * M_PI / (21. * logScaleT) * (1. - b16 * loglogScaleT / logScaleT + pow2(b16 / logScaleT) * (pow2(loglogScaleT - 0.5) + b26 - 1.25) ); Lambda6Save = Lambda5Save; for (int iter = 0; iter < NITER; ++iter) { logScale = 2. * log(MT/Lambda6Save); loglogScale = log(logScale); correction = 1. - b15 * loglogScale / logScale + pow2(b15 / logScale) * (pow2(loglogScale - 0.5) + b25 - 1.25); valueIter = valueT / correction; Lambda6Save = MT * exp( -6. * M_PI / (21. * valueIter) ); } // Find Lambda_4 at m_b. double logScaleB = 2. * log(MB/Lambda5Save); double loglogScaleB = log(logScaleB); double valueB = 12. * M_PI / (23. * logScaleB) * (1. - b15 * loglogScaleB / logScaleB + pow2(b15 / logScaleB) * (pow2(loglogScaleB - 0.5) + b25- 1.25) ); Lambda4Save = Lambda5Save; for (int iter = 0; iter < NITER; ++iter) { logScale = 2. * log(MB/Lambda4Save); loglogScale = log(logScale); correction = 1. - b14 * loglogScale / logScale + pow2(b14 / logScale) * (pow2(loglogScale - 0.5) + b24 - 1.25); valueIter = valueB / correction; Lambda4Save = MB * exp( -6. * M_PI / (25. * valueIter) ); } // Find Lambda_3 at m_c. double logScaleC = 2. * log(MC/Lambda4Save); double loglogScaleC = log(logScaleC); double valueC = 12. * M_PI / (25. * logScaleC) * (1. - b14 * loglogScaleC / logScaleC + pow2(b14 / logScaleC) * (pow2(loglogScaleC - 0.5) + b24 - 1.25) ); Lambda3Save = Lambda4Save; for (int iter = 0; iter < NITER; ++iter) { logScale = 2. * log(MC/Lambda3Save); loglogScale = log(logScale); correction = 1. - b13 * loglogScale / logScale + pow2(b13 / logScale) * (pow2(loglogScale - 0.5) + b23 - 1.25); valueIter = valueC / correction; Lambda3Save = MC * exp( -6. * M_PI / (27. * valueIter) ); } } // Optionally rescale Lambda values by CMW factor. if (useCMW) { Lambda3Save *= FACCMW3; Lambda4Save *= FACCMW4; Lambda5Save *= FACCMW5; Lambda6Save *= FACCMW6; } // Impose SAFETYMARGINs to prevent getting too close to LambdaQCD. if (order == 1) scale2Min = pow2(SAFETYMARGIN1 * Lambda3Save); else if (order == 2) scale2Min = pow2(SAFETYMARGIN2 * Lambda3Save); // Save squares of mass and Lambda values as well. Lambda3Save2 = pow2(Lambda3Save); Lambda4Save2 = pow2(Lambda4Save); Lambda5Save2 = pow2(Lambda5Save); Lambda6Save2 = pow2(Lambda6Save); mc2 = pow2(MC); mb2 = pow2(MB); mt2 = pow2(MT); valueNow = valueIn; scale2Now = MZ * MZ; isInit = true; } //-------------------------------------------------------------------------- // Calculate alpha_s value. double AlphaStrong::alphaS( double scale2) { // Check for initialization and ensure minimal scale2 value. if (!isInit) return 0.; if (scale2 < scale2Min) scale2 = scale2Min; // If equal to old scale then same answer. if (scale2 == scale2Now && (order < 2 || lastCallToFull)) return valueNow; scale2Now = scale2; lastCallToFull = true; // Fix alpha_s. if (order == 0) { valueNow = valueRef; // First order alpha_s: differs by mass region. } else if (order == 1) { if (scale2 > mt2 && nfmax >= 6) valueNow = 12. * M_PI / (21. * log(scale2/Lambda6Save2)); else if (scale2 > mb2) valueNow = 12. * M_PI / (23. * log(scale2/Lambda5Save2)); else if (scale2 > mc2) valueNow = 12. * M_PI / (25. * log(scale2/Lambda4Save2)); else valueNow = 12. * M_PI / (27. * log(scale2/Lambda3Save2)); // Second order alpha_s: differs by mass region. } else { double Lambda2, b0, b1, b2; if (scale2 > mt2 && nfmax >= 6) { Lambda2 = Lambda6Save2; b0 = 21.; b1 = 234. / 441.; b2 = -36855. / 109512.; } else if (scale2 > mb2) { Lambda2 = Lambda5Save2; b0 = 23.; b1 = 348. / 529.; b2 = 224687. / 242208.; } else if (scale2 > mc2) { Lambda2 = Lambda4Save2; b0 = 25.; b1 = 462. / 625.; b2 = 548575. / 426888.; } else { Lambda2 = Lambda3Save2; b0 = 27.; b1 = 64. / 81.; b2 = 938709. / 663552.; } double logScale = log(scale2/Lambda2); double loglogScale = log(logScale); valueNow = 12. * M_PI / (b0 * logScale) * ( 1. - b1 * loglogScale / logScale + pow2(b1 / logScale) * (pow2(loglogScale - 0.5) + b2 - 1.25) ); } // Done. return valueNow; } //-------------------------------------------------------------------------- // Calculate alpha_s value, but only use up to first-order piece. // (To be combined with alphaS2OrdCorr.) double AlphaStrong::alphaS1Ord( double scale2) { // Check for initialization and ensure minimal scale2 value. if (!isInit) return 0.; if (scale2 < scale2Min) scale2 = scale2Min; // If equal to old scale then same answer. if (scale2 == scale2Now && (order < 2 || !lastCallToFull)) return valueNow; scale2Now = scale2; lastCallToFull = false; // Fix alpha_S. if (order == 0) { valueNow = valueRef; // First/second order alpha_s: differs by mass region. } else { if (scale2 > mt2 && nfmax >= 6) valueNow = 12. * M_PI / (21. * log(scale2/Lambda6Save2)); else if (scale2 > mb2) valueNow = 12. * M_PI / (23. * log(scale2/Lambda5Save2)); else if (scale2 > mc2) valueNow = 12. * M_PI / (25. * log(scale2/Lambda4Save2)); else valueNow = 12. * M_PI / (27. * log(scale2/Lambda3Save2)); } // Done. return valueNow; } //-------------------------------------------------------------------------- // Calculates the second-order extra factor in alpha_s. // (To be combined with alphaS1Ord.) double AlphaStrong::alphaS2OrdCorr( double scale2) { // Check for initialization and ensure minimal scale2 value. if (!isInit) return 1.; if (scale2 < scale2Min) scale2 = scale2Min; // Only meaningful for second-order calculations. if (order < 2) return 1.; // Second order correction term: differs by mass region. double Lambda2, b1, b2; if (scale2 > mt2 && nfmax >= 6) { Lambda2 = Lambda6Save2; b1 = 234. / 441.; b2 = -36855. / 109512.; } else if (scale2 > mb2) { Lambda2 = Lambda5Save2; b1 = 348. / 529.; b2 = 224687. / 242208.; } else if (scale2 > mc2) { Lambda2 = Lambda4Save2; b1 = 462. / 625.; b2 = 548575. / 426888.; } else { Lambda2 = Lambda3Save2; b1 = 64. / 81.; b2 = 938709. / 663552.; } double logScale = log(scale2/Lambda2); double loglogScale = log(logScale); return ( 1. - b1 * loglogScale / logScale + pow2(b1 / logScale) * (pow2(loglogScale - 0.5) + b2 - 1.25) ); } //-------------------------------------------------------------------------- // muThres(2): tell what values of flavour thresholds are being used. double AlphaStrong::muThres( int idQ) { int idAbs = abs(idQ); // Return the scale of each flavour threshold included in running. if (idAbs == 4) return MC; else if (idAbs == 5) return MB; else if (idAbs == 6 && nfmax >= 6) return MT; // Else return -1 (indicates no such threshold is included in running). return -1.; } double AlphaStrong::muThres2( int idQ) { int idAbs = abs(idQ); // Return the scale of each flavour threshold included in running. if (idAbs == 4) return mc2; else if (idAbs == 5) return mb2; else if (idAbs == 6 && nfmax >=6) return mt2; // Else return -1 (indicates no such threshold is included in running). return -1.; } //-------------------------------------------------------------------------- // facCMW: tells what values of the CMW factors are being used (if any). double AlphaStrong::facCMW( int NFIn) { // Return unity if we are not doing CMW rescaling.. if (!isInit || !useCMW) return 1.0; // Else return the NF-dependent value of the CMW rescaling factor. else if (NFIn <= 3) return FACCMW3; else if (NFIn == 4) return FACCMW4; else if (NFIn == 5) return FACCMW5; else return FACCMW6; } //========================================================================== // The AlphaEM class. //-------------------------------------------------------------------------- // Definitions of static variables. // Z0 mass. Used for normalization scale. const double AlphaEM::MZ = 91.188; // Effective thresholds for electron, muon, light quarks, tau+c, b. const double AlphaEM::Q2STEP[5] = {0.26e-6, 0.011, 0.25, 3.5, 90.}; // Running coefficients are sum charge2 / 3 pi in pure QED, here slightly // enhanced for quarks to approximately account for QCD corrections. const double AlphaEM::BRUNDEF[5] = {0.1061, 0.2122, 0.460, 0.700, 0.725}; //-------------------------------------------------------------------------- // Initialize alpha_EM calculation. void AlphaEM::init(int orderIn, Settings* settingsPtr) { // Order. Read in alpha_EM value at 0 and m_Z, and mass of Z. order = orderIn; alpEM0 = settingsPtr->parm("StandardModel:alphaEM0"); alpEMmZ = settingsPtr->parm("StandardModel:alphaEMmZ"); mZ2 = MZ * MZ; // AlphaEM values at matching scales and matching b value. if (order <= 0) return; for (int i = 0; i < 5; ++i) bRun[i] = BRUNDEF[i]; // Step down from mZ to tau/charm threshold. alpEMstep[4] = alpEMmZ / ( 1. + alpEMmZ * bRun[4] * log(mZ2 / Q2STEP[4]) ); alpEMstep[3] = alpEMstep[4] / ( 1. - alpEMstep[4] * bRun[3] * log(Q2STEP[3] / Q2STEP[4]) ); // Step up from me to light-quark threshold. alpEMstep[0] = alpEM0; alpEMstep[1] = alpEMstep[0] / ( 1. - alpEMstep[0] * bRun[0] * log(Q2STEP[1] / Q2STEP[0]) ); alpEMstep[2] = alpEMstep[1] / ( 1. - alpEMstep[1] * bRun[1] * log(Q2STEP[2] / Q2STEP[1]) ); // Fit b in range between light-quark and tau/charm to join smoothly. bRun[2] = (1./alpEMstep[3] - 1./alpEMstep[2]) / log(Q2STEP[2] / Q2STEP[3]); } //-------------------------------------------------------------------------- // Calculate alpha_EM value double AlphaEM::alphaEM( double scale2) { // Fix alphaEM; for order = -1 fixed at m_Z. if (order == 0) return alpEM0; if (order < 0) return alpEMmZ; // Running alphaEM. for (int i = 4; i >= 0; --i) if (scale2 > Q2STEP[i]) return alpEMstep[i] / (1. - bRun[i] * alpEMstep[i] * log(scale2 / Q2STEP[i]) ); return alpEM0; } //========================================================================== // The CoupSM class. //-------------------------------------------------------------------------- // Definitions of static variables: charges and axial couplings. const double CoupSM::efSave[20] = { 0., -1./3., 2./3., -1./3., 2./3., -1./3., 2./3., -1./3., 2./3., 0., 0., -1., 0., -1., 0., -1., 0., -1., 0., 0.}; const double CoupSM::afSave[20] = { 0., -1., 1., -1., 1., -1., 1., -1., 1., 0., 0., -1., 1., -1., 1., -1., 1., -1., 1., 0.}; //-------------------------------------------------------------------------- // Initialize electroweak mixing angle and couplings, and CKM matrix elements. void CoupSM::init(Settings& settings, Rndm* rndmPtrIn) { // Store input pointer; rndmPtr = rndmPtrIn; // Initialize the local AlphaStrong instance. double alphaSvalue = settings.parm("SigmaProcess:alphaSvalue"); int alphaSorder = settings.mode("SigmaProcess:alphaSorder"); int alphaSnfmax = settings.mode("StandardModel:alphaSnfmax"); alphaSlocal.init( alphaSvalue, alphaSorder, alphaSnfmax, false); // Initialize the local AlphaEM instance. int order = settings.mode("SigmaProcess:alphaEMorder"); alphaEMlocal.init( order, &settings); // Read in electroweak mixing angle and the Fermi constant. s2tW = settings.parm("StandardModel:sin2thetaW"); c2tW = 1. - s2tW; s2tWbar = settings.parm("StandardModel:sin2thetaWbar"); GFermi = settings.parm("StandardModel:GF"); // Initialize electroweak couplings. for (int i = 0; i < 20; ++i) { vfSave[i] = afSave[i] - 4. * s2tWbar * efSave[i]; lfSave[i] = afSave[i] - 2. * s2tWbar * efSave[i]; rfSave[i] = - 2. * s2tWbar * efSave[i]; ef2Save[i] = pow2(efSave[i]); vf2Save[i] = pow2(vfSave[i]); af2Save[i] = pow2(afSave[i]); efvfSave[i] = efSave[i] * vfSave[i]; vf2af2Save[i] = vf2Save[i] + af2Save[i]; } // Read in CKM matrix element values and store them. VCKMsave[1][1] = settings.parm("StandardModel:Vud"); VCKMsave[1][2] = settings.parm("StandardModel:Vus"); VCKMsave[1][3] = settings.parm("StandardModel:Vub"); VCKMsave[2][1] = settings.parm("StandardModel:Vcd"); VCKMsave[2][2] = settings.parm("StandardModel:Vcs"); VCKMsave[2][3] = settings.parm("StandardModel:Vcb"); VCKMsave[3][1] = settings.parm("StandardModel:Vtd"); VCKMsave[3][2] = settings.parm("StandardModel:Vts"); VCKMsave[3][3] = settings.parm("StandardModel:Vtb"); // Also allow for the potential existence of a fourth generation. VCKMsave[1][4] = settings.parm("FourthGeneration:VubPrime"); VCKMsave[2][4] = settings.parm("FourthGeneration:VcbPrime"); VCKMsave[3][4] = settings.parm("FourthGeneration:VtbPrime"); VCKMsave[4][1] = settings.parm("FourthGeneration:VtPrimed"); VCKMsave[4][2] = settings.parm("FourthGeneration:VtPrimes"); VCKMsave[4][3] = settings.parm("FourthGeneration:VtPrimeb"); VCKMsave[4][4] = settings.parm("FourthGeneration:VtPrimebPrime"); // Calculate squares of matrix elements. for(int i = 1; i < 5; ++i) for(int j = 1; j < 5; ++j) V2CKMsave[i][j] = pow2(VCKMsave[i][j]); // Sum VCKM^2_out sum for given incoming flavour, excluding top as partner. V2CKMout[1] = V2CKMsave[1][1] + V2CKMsave[2][1]; V2CKMout[2] = V2CKMsave[1][1] + V2CKMsave[1][2] + V2CKMsave[1][3]; V2CKMout[3] = V2CKMsave[1][2] + V2CKMsave[2][2]; V2CKMout[4] = V2CKMsave[2][1] + V2CKMsave[2][2] + V2CKMsave[2][3]; V2CKMout[5] = V2CKMsave[1][3] + V2CKMsave[2][3]; V2CKMout[6] = V2CKMsave[3][1] + V2CKMsave[3][2] + V2CKMsave[3][3]; V2CKMout[7] = V2CKMsave[1][4] + V2CKMsave[2][4]; V2CKMout[8] = V2CKMsave[4][1] + V2CKMsave[4][2] + V2CKMsave[4][3]; for (int i = 11; i <= 18; ++i) V2CKMout[i] = 1.; } //-------------------------------------------------------------------------- // Return CKM value for incoming flavours (sign irrelevant). double CoupSM::VCKMid(int id1, int id2) { // Use absolute sign (want to cover both f -> f' W and f fbar' -> W). int id1Abs = abs(id1); int id2Abs = abs(id2); if (id1Abs == 0 || id2Abs == 0 || (id1Abs + id2Abs)%2 != 1) return 0.; // Ensure proper order before reading out from VCKMsave or lepton match. if (id1Abs%2 == 1) swap(id1Abs, id2Abs); if (id1Abs <= 8 && id2Abs <= 8) return VCKMsave[id1Abs/2][(id2Abs + 1)/2]; if ( (id1Abs == 12 || id1Abs == 14 || id1Abs == 16 || id1Abs == 18) && id2Abs == id1Abs - 1 ) return 1.; // No more valid cases. return 0.; } //-------------------------------------------------------------------------- // Return squared CKM value for incoming flavours (sign irrelevant). double CoupSM::V2CKMid(int id1, int id2) { // Use absolute sign (want to cover both f -> f' W and f fbar' -> W). int id1Abs = abs(id1); int id2Abs = abs(id2); if (id1Abs == 0 || id2Abs == 0 || (id1Abs + id2Abs)%2 != 1) return 0.; // Ensure proper order before reading out from V2CKMsave or lepton match. if (id1Abs%2 == 1) swap(id1Abs, id2Abs); if (id1Abs <= 8 && id2Abs <= 8) return V2CKMsave[id1Abs/2][(id2Abs + 1)/2]; if ( (id1Abs == 12 || id1Abs == 14 || id1Abs == 16 || id1Abs == 18) && id2Abs == id1Abs - 1 ) return 1.; // No more valid cases. return 0.; } //-------------------------------------------------------------------------- // Pick an outgoing flavour for given incoming one, given CKM mixing. int CoupSM::V2CKMpick(int id) { // Initial values. int idIn = abs(id); int idOut = 0; // Quarks: need to make random choice. if (idIn >= 1 && idIn <= 8) { double V2CKMrndm = rndmPtr->flat() * V2CKMout[idIn]; if (idIn == 1) idOut = (V2CKMrndm < V2CKMsave[1][1]) ? 2 : 4; else if (idIn == 2) idOut = (V2CKMrndm < V2CKMsave[1][1]) ? 1 : ( (V2CKMrndm < V2CKMsave[1][1] + V2CKMsave[1][2]) ? 3 : 5 ); else if (idIn == 3) idOut = (V2CKMrndm < V2CKMsave[1][2]) ? 2 : 4; else if (idIn == 4) idOut = (V2CKMrndm < V2CKMsave[2][1]) ? 1 : ( (V2CKMrndm < V2CKMsave[2][1] + V2CKMsave[2][2]) ? 3 : 5 ); else if (idIn == 5) idOut = (V2CKMrndm < V2CKMsave[1][3]) ? 2 : 4; else if (idIn == 6) idOut = (V2CKMrndm < V2CKMsave[3][1]) ? 1 : ( (V2CKMrndm < V2CKMsave[3][1] + V2CKMsave[3][2]) ? 3 : 5 ); else if (idIn == 7) idOut = (V2CKMrndm < V2CKMsave[1][4]) ? 2 : 4; else if (idIn == 8) idOut = (V2CKMrndm < V2CKMsave[4][1]) ? 1 : ( (V2CKMrndm < V2CKMsave[4][1] + V2CKMsave[4][2]) ? 3 : 5 ); // Leptons: unambiguous. } else if (idIn >= 11 && idIn <= 18) { if (idIn%2 == 1) idOut = idIn + 1; else idOut = idIn - 1; } // Done. Return with sign. return ( (id > 0) ? idOut : -idOut ); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/ParticleData.cc0000644000175000017500000022004412217346246015775 0ustar sunsun// ParticleData.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // DecayChannel, ParticleDataEntry and ParticleData classes. #include "Pythia8/ParticleData.h" #include "Pythia8/ResonanceWidths.h" #include "Pythia8/StandardModel.h" #include "Pythia8/SusyResonanceWidths.h" // Allow string and character manipulation. #include namespace Pythia8 { //========================================================================== // DecayChannel class. // This class holds info on a single decay channel. //-------------------------------------------------------------------------- // Check whether id1 occurs anywhere in product list. bool DecayChannel::contains(int id1) const { bool found1 = false; for (int i = 0; i < nProd; ++i) if (prod[i] == id1) found1 = true; return found1; } //-------------------------------------------------------------------------- // Check whether id1 and id2 occur anywhere in product list. // iF ID1 == ID2 then two copies of this particle must be present. bool DecayChannel::contains(int id1, int id2) const { bool found1 = false; bool found2 = false; for (int i = 0; i < nProd; ++i) { if (!found1 && prod[i] == id1) {found1 = true; continue;} if (!found2 && prod[i] == id2) {found2 = true; continue;} } return found1 && found2; } //-------------------------------------------------------------------------- // Check whether id1, id2 and id3 occur anywhere in product list. // iF ID1 == ID2 then two copies of this particle must be present, etc. bool DecayChannel::contains(int id1, int id2, int id3) const { bool found1 = false; bool found2 = false; bool found3 = false; for (int i = 0; i < nProd; ++i) { if (!found1 && prod[i] == id1) {found1 = true; continue;} if (!found2 && prod[i] == id2) {found2 = true; continue;} if (!found3 && prod[i] == id3) {found3 = true; continue;} } return found1 && found2 && found3; } //========================================================================== // ParticleDataEntry class. // This class holds info on a single particle species. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // A particle is invisible if it has neither strong nor electric charge, // and is not made up of constituents that have it. Only relevant for // long-lived particles. This list may need to be extended. const int ParticleDataEntry::INVISIBLENUMBER = 50; const int ParticleDataEntry::INVISIBLETABLE[50] = { 12, 14, 16, 18, 23, 25, 32, 33, 35, 36, 39, 41, 1000012, 1000014, 1000016, 1000018, 1000022, 1000023, 1000025, 1000035, 1000045, 1000039, 2000012, 2000014, 2000016, 2000018, 4900012, 4900014, 4900016, 4900021, 4900022, 4900101, 4900102, 4900103, 4900104, 4900105, 4900106, 4900107, 4900108, 4900111, 4900113, 4900211, 4900213, 4900991, 5000039, 5100039, 9900012, 9900014, 9900016, 9900023 }; // For some particles we know it is necessary to switch off width, // although they do have one, so do not warn. const int ParticleDataEntry::KNOWNNOWIDTH[3] = {10313, 10323, 10333}; // Particles with a read-in tau0 (in mm/c) below this mayDecay by default. const double ParticleDataEntry::MAXTAU0FORDECAY = 1000.; // Particles with a read-in m0 above this isResonance by default. const double ParticleDataEntry::MINMASSRESONANCE = 20.; // Narrow states are assigned nominal mass. const double ParticleDataEntry::NARROWMASS = 1e-6; // Constituent quark masses (d, u, s, c, b, -, -, -, g). const double ParticleDataEntry::CONSTITUENTMASSTABLE[10] = {0., 0.325, 0.325, 0.50, 1.60, 5.00, 0., 0., 0., 0.7}; //-------------------------------------------------------------------------- // Destructor: delete any ResonanceWidths object. ParticleDataEntry::~ParticleDataEntry() { if (resonancePtr != 0) delete resonancePtr; } //-------------------------------------------------------------------------- // Set initial default values for some quantities. void ParticleDataEntry::setDefaults() { // A particle is a resonance if it is heavy enough. isResonanceSave = (m0Save > MINMASSRESONANCE); // A particle may decay if it is shortlived enough. mayDecaySave = (tau0Save < MAXTAU0FORDECAY); // A particle by default has no external decays. doExternalDecaySave = false; // A particle is invisible if in current table of such. isVisibleSave = true; for (int i = 0; i < INVISIBLENUMBER; ++i) if (idSave == INVISIBLETABLE[i]) isVisibleSave = false; // Normally a resonance should not have width forced to fixed value. doForceWidthSave = false; // Set up constituent masses. setConstituentMass(); // No Breit-Wigner mass selection before initialized. modeBWnow = 0; } //-------------------------------------------------------------------------- // Find out if a particle is a hadron. // Only covers normal hadrons, not e.g. R-hadrons. bool ParticleDataEntry::isHadron() const { if (idSave <= 100 || (idSave >= 1000000 && idSave <= 9000000) || idSave >= 9900000) return false; if (idSave == 130 || idSave == 310) return true; if (idSave%10 == 0 || (idSave/10)%10 == 0 || (idSave/100)%10 == 0) return false; return true; } //-------------------------------------------------------------------------- // Find out if a particle is a meson. // Only covers normal hadrons, not e.g. R-hadrons. bool ParticleDataEntry::isMeson() const { if (idSave <= 100 || (idSave >= 1000000 && idSave <= 9000000) || idSave >= 9900000) return false; if (idSave == 130 || idSave == 310) return true; if (idSave%10 == 0 || (idSave/10)%10 == 0 || (idSave/100)%10 == 0 || (idSave/1000)%10 != 0) return false; return true; } //-------------------------------------------------------------------------- // Find out if a particle is a baryon. // Only covers normal hadrons, not e.g. R-hadrons. bool ParticleDataEntry::isBaryon() const { if (idSave <= 1000 || (idSave >= 1000000 && idSave <= 9000000) || idSave >= 9900000) return false; if (idSave%10 == 0 || (idSave/10)%10 == 0 || (idSave/100)%10 == 0 || (idSave/1000)%10 == 0) return false; return true; } //-------------------------------------------------------------------------- // Extract the heaviest (= largest id) quark in a hadron. int ParticleDataEntry::heaviestQuark(int idIn) const { if (!isHadron()) return 0; int hQ = 0; // Meson. if ( (idSave/1000)%10 == 0 ) { hQ = (idSave/100)%10; if (idSave == 130) hQ = 3; if (hQ%2 == 1) hQ = -hQ; // Baryon. } else hQ = (idSave/1000)%10; // Done. return (idIn > 0) ? hQ : -hQ; } //-------------------------------------------------------------------------- // Calculate three times baryon number, i.e. net quark - antiquark number. int ParticleDataEntry::baryonNumberType(int idIn) const { // Quarks. if (isQuark()) return (idIn > 0) ? 1 : -1; // Diquarks if (isDiquark()) return (idIn > 0) ? 2 : -2; // Baryons. if (isBaryon()) return (idIn > 0) ? 3 : -3; // Done. return 0; } //-------------------------------------------------------------------------- // Prepare the Breit-Wigner mass selection by precalculating // frequently-used expressions. void ParticleDataEntry::initBWmass() { // Find Breit-Wigner mode for current particle. modeBWnow = particleDataPtr->modeBreitWigner; if ( m0Save < NARROWMASS ) mWidthSave = 0.; if ( mWidthSave < NARROWMASS || (mMaxSave > mMinSave && mMaxSave - mMinSave < NARROWMASS) ) modeBWnow = 0; if (modeBWnow == 0) return; // Find atan expressions to be used in random mass selection. if (modeBWnow < 3) { atanLow = atan( 2. * (mMinSave - m0Save) / mWidthSave ); double atanHigh = (mMaxSave > mMinSave) ? atan( 2. * (mMaxSave - m0Save) / mWidthSave ) : 0.5 * M_PI; atanDif = atanHigh - atanLow; } else { atanLow = atan( (pow2(mMinSave) - pow2(m0Save)) / (m0Save * mWidthSave) ); double atanHigh = (mMaxSave > mMinSave) ? atan( (pow2(mMaxSave) - pow2(m0Save)) / (m0Save * mWidthSave) ) : 0.5 * M_PI; atanDif = atanHigh - atanLow; } // Done if no threshold factor. if (modeBWnow%2 == 1) return; // Find average mass threshold for threshold-factor correction. double bRatSum = 0.; double mThrSum = 0; for (int i = 0; i < int(channels.size()); ++i) if (channels[i].onMode() >= 0) { bRatSum += channels[i].bRatio(); double mChannelSum = 0.; for (int j = 0; j < channels[i].multiplicity(); ++j) mChannelSum += particleDataPtr->m0( channels[i].product(j) ); mThrSum += channels[i].bRatio() * mChannelSum; } mThr = (bRatSum == 0.) ? 0. : mThrSum / bRatSum; // Switch off Breit-Wigner if very close to threshold. if (mThr + NARROWMASS > m0Save) { modeBWnow = 0; bool knownProblem = false; for (int i = 0; i < 3; ++i) if (idSave == KNOWNNOWIDTH[i]) knownProblem = true; if (!knownProblem) { ostringstream osWarn; osWarn << "for id = " << idSave; particleDataPtr->infoPtr->errorMsg("Warning in ParticleDataEntry::" "initBWmass: switching off width", osWarn.str(), true); } } } //-------------------------------------------------------------------------- // Function to give mass of a particle, either at the nominal value // or picked according to a (linear or quadratic) Breit-Wigner. double ParticleDataEntry::mSel() { // Nominal value. (Width check should not be needed, but just in case.) if (modeBWnow == 0 || mWidthSave < NARROWMASS) return m0Save; double mNow, m2Now; // Mass according to a Breit-Wigner linear in m. if (modeBWnow == 1) { mNow = m0Save + 0.5 * mWidthSave * tan( atanLow + atanDif * particleDataPtr->rndmPtr->flat() ); // Ditto, but make Gamma proportional to sqrt(m^2 - m_threshold^2). } else if (modeBWnow == 2) { double mWidthNow, fixBW, runBW; double m0ThrS = m0Save*m0Save - mThr*mThr; do { mNow = m0Save + 0.5 * mWidthSave * tan( atanLow + atanDif * particleDataPtr->rndmPtr->flat() ); mWidthNow = mWidthSave * sqrtpos( (mNow*mNow - mThr*mThr) / m0ThrS ); fixBW = mWidthSave / (pow2(mNow - m0Save) + pow2(0.5 * mWidthSave)); runBW = mWidthNow / (pow2(mNow - m0Save) + pow2(0.5 * mWidthNow)); } while (runBW < particleDataPtr->rndmPtr->flat() * particleDataPtr->maxEnhanceBW * fixBW); // Mass according to a Breit-Wigner quadratic in m. } else if (modeBWnow == 3) { m2Now = m0Save*m0Save + m0Save * mWidthSave * tan( atanLow + atanDif * particleDataPtr->rndmPtr->flat() ); mNow = sqrtpos( m2Now); // Ditto, but m_0 Gamma_0 -> m Gamma(m) with threshold factor as above. } else { double mwNow, fixBW, runBW; double m2Ref = m0Save * m0Save; double mwRef = m0Save * mWidthSave; double m2Thr = mThr * mThr; do { m2Now = m2Ref + mwRef * tan( atanLow + atanDif * particleDataPtr->rndmPtr->flat() ); mNow = sqrtpos( m2Now); mwNow = mNow * mWidthSave * sqrtpos( (m2Now - m2Thr) / (m2Ref - m2Thr) ); fixBW = mwRef / (pow2(m2Now - m2Ref) + pow2(mwRef)); runBW = mwNow / (pow2(m2Now - m2Ref) + pow2(mwNow)); } while (runBW < particleDataPtr->rndmPtr->flat() * particleDataPtr->maxEnhanceBW * fixBW); } // Done. return mNow; } //-------------------------------------------------------------------------- // Function to calculate running mass at given mass scale. double ParticleDataEntry::mRun(double mHat) { // Except for six quarks return nominal mass. if (idSave > 6) return m0Save; double mQRun = particleDataPtr->mQRun[idSave]; double Lam5 = particleDataPtr->Lambda5Run; // For d, u, s quarks start running at 2 GeV (RPP 2006 p. 505). if (idSave < 4) return mQRun * pow ( log(2. / Lam5) / log(max(2., mHat) / Lam5), 12./23.); // For c, b and t quarks start running at respective mass. return mQRun * pow ( log(mQRun / Lam5) / log(max(mQRun, mHat) / Lam5), 12./23.); } //-------------------------------------------------------------------------- // Rescale all branching ratios to assure normalization to unity. void ParticleDataEntry::rescaleBR(double newSumBR) { // Sum up branching ratios. Find rescaling factor. Rescale. double oldSumBR = 0.; for ( int i = 0; i < int(channels.size()); ++ i) oldSumBR += channels[i].bRatio(); double rescaleFactor = newSumBR / oldSumBR; for ( int i = 0; i < int(channels.size()); ++ i) channels[i].rescaleBR(rescaleFactor); } //-------------------------------------------------------------------------- // Prepare to pick a decay channel. bool ParticleDataEntry::preparePick(int idSgn, double mHat, int idInFlav) { // Reset sum of allowed widths/branching ratios. currentBRSum = 0.; // For resonances the widths are calculated dynamically. if (isResonanceSave && resonancePtr != 0) { resonancePtr->widthStore(idSgn, mHat, idInFlav); for (int i = 0; i < int(channels.size()); ++i) currentBRSum += channels[i].currentBR(); // Else use normal fixed branching ratios. } else { int onMode; double currentBRNow; for (int i = 0; i < int(channels.size()); ++i) { onMode = channels[i].onMode(); currentBRNow = 0.; if ( idSgn > 0 && (onMode == 1 || onMode == 2) ) currentBRNow = channels[i].bRatio(); else if ( idSgn < 0 && (onMode == 1 || onMode == 3) ) currentBRNow = channels[i].bRatio(); channels[i].currentBR(currentBRNow); currentBRSum += currentBRNow; } } // Failure if no channels found with positive branching ratios. return (currentBRSum > 0.); } //-------------------------------------------------------------------------- // Pick a decay channel according to branching ratios from preparePick. DecayChannel& ParticleDataEntry::pickChannel() { // Find channel in table. int size = channels.size(); double rndmBR = currentBRSum * particleDataPtr->rndmPtr->flat(); int i = -1; do rndmBR -= channels[++i].currentBR(); while (rndmBR > 0. && i < size); // Emergency if no channel found. Done. if (i == size) i = 0; return channels[i]; } //-------------------------------------------------------------------------- // Access methods stored in ResonanceWidths. Could have been // inline in .h, except for problems with forward declarations. void ParticleDataEntry::setResonancePtr( ResonanceWidths* resonancePtrIn) { if (resonancePtr == resonancePtrIn) return; if (resonancePtr != 0) delete resonancePtr; resonancePtr = resonancePtrIn; } void ParticleDataEntry::resInit(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Couplings* couplingsPtrIn) { if (resonancePtr != 0) resonancePtr->init(infoPtrIn, settingsPtrIn, particleDataPtrIn, couplingsPtrIn); } double ParticleDataEntry::resWidth(int idSgn, double mHat, int idIn, bool openOnly, bool setBR) { return (resonancePtr != 0) ? resonancePtr->width( idSgn, mHat, idIn, openOnly, setBR) : 0.; } double ParticleDataEntry::resWidthOpen(int idSgn, double mHat, int idIn) { return (resonancePtr != 0) ? resonancePtr->widthOpen( idSgn, mHat, idIn) : 0.; } double ParticleDataEntry::resWidthStore(int idSgn, double mHat, int idIn) { return (resonancePtr != 0) ? resonancePtr->widthStore( idSgn, mHat, idIn) : 0.; } double ParticleDataEntry::resOpenFrac(int idSgn) { return (resonancePtr != 0) ? resonancePtr->openFrac(idSgn) : 1.; } double ParticleDataEntry::resWidthRescaleFactor() { return (resonancePtr != 0) ? resonancePtr->widthRescaleFactor() : 1.; } double ParticleDataEntry::resWidthChan(double mHat, int idAbs1, int idAbs2) { return (resonancePtr != 0) ? resonancePtr->widthChan( mHat, idAbs1, idAbs2) : 0.; } //-------------------------------------------------------------------------- // Constituent masses for (d, u, s, c, b) quarks and diquarks. // Hardcoded in CONSTITUENTMASSTABLE so that they are not overwritten // by mistake, and separated from the "normal" masses. // Called both by setDefaults and setM0 so kept as separate method. void ParticleDataEntry::setConstituentMass() { // Equate with the normal masses as default guess. constituentMassSave = m0Save; // Quark masses trivial. Also gluon mass. if (idSave < 6) constituentMassSave = CONSTITUENTMASSTABLE[idSave]; if (idSave == 21) constituentMassSave = CONSTITUENTMASSTABLE[9]; // Diquarks as simple sum of constituent quarks. if (idSave > 1000 && idSave < 10000 && (idSave/10)%10 == 0) { int id1 = idSave/1000; int id2 = (idSave/100)%10; if (id1 <6 && id2 < 6) constituentMassSave = CONSTITUENTMASSTABLE[id1] + CONSTITUENTMASSTABLE[id2]; } } //========================================================================== // ParticleData class. // This class holds a map of all ParticleDataEntries, // each entry containing info on a particle species. //-------------------------------------------------------------------------- // Get data to be distributed among particles during setup. // Note: this routine is called twice. Firstly from init(...), but // the data should not be used at that point, so is likely overkill. // Secondly, from initWidths, after user has had time to change. void ParticleData::initCommon() { // Mass generation: fixed mass or linear/quadratic Breit-Wigner. modeBreitWigner = settingsPtr->mode("ParticleData:modeBreitWigner"); // Maximum tail enhancement when adding threshold factor to Breit-Wigner. maxEnhanceBW = settingsPtr->parm("ParticleData:maxEnhanceBW"); // Find initial MSbar masses for five light flavours. mQRun[1] = settingsPtr->parm("ParticleData:mdRun"); mQRun[2] = settingsPtr->parm("ParticleData:muRun"); mQRun[3] = settingsPtr->parm("ParticleData:msRun"); mQRun[4] = settingsPtr->parm("ParticleData:mcRun"); mQRun[5] = settingsPtr->parm("ParticleData:mbRun"); mQRun[6] = settingsPtr->parm("ParticleData:mtRun"); // Find Lambda5 value to use in running of MSbar masses. double alphaSvalue = settingsPtr->parm("ParticleData:alphaSvalueMRun"); AlphaStrong alphaS; alphaS.init( alphaSvalue, 1, 5, false); Lambda5Run = alphaS.Lambda5(); } //-------------------------------------------------------------------------- // Initialize pointer for particles to the full database, the Breit-Wigners // of normal hadrons and the ResonanceWidths of resonances. For the latter // the order of initialization is essential to get secondary widths right. void ParticleData::initWidths( vector resonancePtrs) { // Initialize some common data. initCommon(); // Pointer to database and Breit-Wigner mass initialization for each // particle. ResonanceWidths* resonancePtr = 0; for (map::iterator pdtEntry = pdt.begin(); pdtEntry != pdt.end(); ++pdtEntry) { ParticleDataEntry& pdtNow = pdtEntry->second; pdtNow.initPtr( this); pdtNow.initBWmass(); // Remove any existing resonances. resonancePtr = pdtNow.getResonancePtr(); if (resonancePtr != 0) pdtNow.setResonancePtr(0); } // Begin set up new resonance objects. // Z0, W+- and top are almost always needed. resonancePtr = new ResonanceGmZ(23); setResonancePtr( 23, resonancePtr); resonancePtr = new ResonanceW(24); setResonancePtr( 24, resonancePtr); resonancePtr = new ResonanceTop(6); setResonancePtr( 6, resonancePtr); // Higgs in SM. if (!settingsPtr->flag("Higgs:useBSM")) { resonancePtr = new ResonanceH(0, 25); setResonancePtr( 25, resonancePtr); // Higgses in BSM. } else { resonancePtr = new ResonanceH(1, 25); setResonancePtr( 25, resonancePtr); resonancePtr = new ResonanceH(2, 35); setResonancePtr( 35, resonancePtr); resonancePtr = new ResonanceH(3, 36); setResonancePtr( 36, resonancePtr); resonancePtr = new ResonanceHchg(37); setResonancePtr( 37, resonancePtr); } // A fourth generation: b', t', tau', nu'_tau. resonancePtr = new ResonanceFour(7); setResonancePtr( 7, resonancePtr); resonancePtr = new ResonanceFour(8); setResonancePtr( 8, resonancePtr); resonancePtr = new ResonanceFour(17); setResonancePtr( 17, resonancePtr); resonancePtr = new ResonanceFour(18); setResonancePtr( 18, resonancePtr); // New gauge bosons: Z', W', R. resonancePtr = new ResonanceZprime(32); setResonancePtr( 32, resonancePtr); resonancePtr = new ResonanceWprime(34); setResonancePtr( 34, resonancePtr); resonancePtr = new ResonanceRhorizontal(41); setResonancePtr( 41, resonancePtr); // A leptoquark. resonancePtr = new ResonanceLeptoquark(42); setResonancePtr( 42, resonancePtr); // 93 = Z0copy and 94 = W+-copy used to pick decay channels // for W/Z production in parton showers. resonancePtr = new ResonanceGmZ(93); setResonancePtr( 93, resonancePtr); resonancePtr = new ResonanceW(94); setResonancePtr( 94, resonancePtr); // Supersymmetry // - Squarks for(int i = 1; i < 7; i++){ resonancePtr = new ResonanceSquark(1000000 + i); setResonancePtr( 1000000 + i, resonancePtr); resonancePtr = new ResonanceSquark(2000000 + i); setResonancePtr( 2000000 + i, resonancePtr); } // - Sleptons and sneutrinos for(int i = 1; i < 7; i++){ resonancePtr = new ResonanceSlepton(1000010 + i); setResonancePtr( 1000010 + i, resonancePtr); resonancePtr = new ResonanceSlepton(2000010 + i); setResonancePtr( 2000010 + i, resonancePtr); } // - Gluino resonancePtr = new ResonanceGluino(1000021); setResonancePtr( 1000021, resonancePtr); // - Charginos resonancePtr = new ResonanceChar(1000024); setResonancePtr( 1000024, resonancePtr); resonancePtr = new ResonanceChar(1000037); setResonancePtr( 1000037, resonancePtr); // - Neutralinos resonancePtr = new ResonanceNeut(1000022); setResonancePtr( 1000022, resonancePtr); resonancePtr = new ResonanceNeut(1000023); setResonancePtr( 1000023, resonancePtr); resonancePtr = new ResonanceNeut(1000025); setResonancePtr( 1000025, resonancePtr); resonancePtr = new ResonanceNeut(1000035); setResonancePtr( 1000035, resonancePtr); resonancePtr = new ResonanceNeut(1000045); setResonancePtr( 1000045, resonancePtr); // Excited quarks and leptons. for (int i = 1; i < 7; ++i) { resonancePtr = new ResonanceExcited(4000000 + i); setResonancePtr( 4000000 + i, resonancePtr); } for (int i = 11; i < 17; ++i) { resonancePtr = new ResonanceExcited(4000000 + i); setResonancePtr( 4000000 + i, resonancePtr); } // An excited graviton/gluon in extra-dimensional scenarios. resonancePtr = new ResonanceGraviton(5100039); setResonancePtr( 5100039, resonancePtr); resonancePtr = new ResonanceKKgluon(5100021); setResonancePtr( 5100021, resonancePtr); // A left-right-symmetric scenario with new righthanded neutrinos, // righthanded gauge bosons and doubly charged Higgses. resonancePtr = new ResonanceNuRight(9900012); setResonancePtr( 9900012, resonancePtr); resonancePtr = new ResonanceNuRight(9900014); setResonancePtr( 9900014, resonancePtr); resonancePtr = new ResonanceNuRight(9900016); setResonancePtr( 9900016, resonancePtr); resonancePtr = new ResonanceZRight(9900023); setResonancePtr( 9900023, resonancePtr); resonancePtr = new ResonanceWRight(9900024); setResonancePtr( 9900024, resonancePtr); resonancePtr = new ResonanceHchgchgLeft(9900041); setResonancePtr( 9900041, resonancePtr); resonancePtr = new ResonanceHchgchgRight(9900042); setResonancePtr( 9900042, resonancePtr); // Attach user-defined external resonances and do basic initialization. for (int i = 0; i < int(resonancePtrs.size()); ++i) { int idNow = resonancePtrs[i]->id(); resonancePtrs[i]->initBasic(idNow); setResonancePtr( idNow, resonancePtrs[i]); } // Set up lists to order resonances in ascending mass. vector idOrdered; vector m0Ordered; // Put Z0 and W+- first, since known to be SM and often off-shell. idOrdered.push_back(23); m0Ordered.push_back(m0(23)); idOrdered.push_back(24); m0Ordered.push_back(m0(24)); // Loop through particle table to find resonances. for (map::iterator pdtEntry = pdt.begin(); pdtEntry != pdt.end(); ++pdtEntry) { ParticleDataEntry& pdtNow = pdtEntry->second; int idNow = pdtNow.id(); // Set up a simple default object for uninitialized resonances. if (pdtNow.isResonance() && pdtNow.getResonancePtr() == 0) { resonancePtr = new ResonanceGeneric(idNow); setResonancePtr( idNow, resonancePtr); } // Insert resonances in ascending mass, to respect decay hierarchies. if (pdtNow.getResonancePtr() != 0 && idNow != 23 && idNow != 24) { double m0Now = pdtNow.m0(); idOrdered.push_back(idNow); m0Ordered.push_back(m0Now); for (int i = int(idOrdered.size()) - 2; i > 1; --i) { if (m0Ordered[i] < m0Now) break; swap( idOrdered[i], idOrdered[i + 1]); swap( m0Ordered[i], m0Ordered[i + 1]); } } } // Initialize the resonances in ascending mass order. Reset mass generation. for (int i = 0; i < int(idOrdered.size()); ++i) { resInit( idOrdered[i]); ParticleDataEntry* pdtPtrNow = particleDataEntryPtr( idOrdered[i]); pdtPtrNow->initBWmass(); } } //-------------------------------------------------------------------------- // Read in database from specific XML file (which may refer to others). bool ParticleData::readXML(string inFile, bool reset) { // Normally reset whole database before beginning. if (reset) {pdt.clear(); isInit = false;} // List of files to be checked. vector files; files.push_back(inFile); // Loop over files. Open them for read. for (int i = 0; i < int(files.size()); ++i) { const char* cstring = files[i].c_str(); ifstream is(cstring); // Check that instream is OK. if (!is.good()) { infoPtr->errorMsg("Error in ParticleData::readXML:" " did not find file", files[i]); return false; } // Read in one line at a time. particlePtr = 0; string line; while ( getline(is, line) ) { // Get first word of a line. istringstream getfirst(line); string word1; getfirst >> word1; // Check for occurence of a particle. Add any continuation lines. if (word1 == "") == string::npos) { string addLine; getline(is, addLine); line += addLine; } // Read in particle properties. int idTmp = intAttributeValue( line, "id"); string nameTmp = attributeValue( line, "name"); string antiNameTmp = attributeValue( line, "antiName"); if (antiNameTmp == "") antiNameTmp = "void"; int spinTypeTmp = intAttributeValue( line, "spinType"); int chargeTypeTmp = intAttributeValue( line, "chargeType"); int colTypeTmp = intAttributeValue( line, "colType"); double m0Tmp = doubleAttributeValue( line, "m0"); double mWidthTmp = doubleAttributeValue( line, "mWidth"); double mMinTmp = doubleAttributeValue( line, "mMin"); double mMaxTmp = doubleAttributeValue( line, "mMax"); double tau0Tmp = doubleAttributeValue( line, "tau0"); // Erase if particle already exists. if (isParticle(idTmp)) pdt.erase(idTmp); // Store new particle. Save pointer, to be used for decay channels. addParticle( idTmp, nameTmp, antiNameTmp, spinTypeTmp, chargeTypeTmp, colTypeTmp, m0Tmp, mWidthTmp, mMinTmp, mMaxTmp, tau0Tmp); particlePtr = particleDataEntryPtr(idTmp); // Check for occurence of a decay channel. Add any continuation lines. } else if (word1 == "") == string::npos) { string addLine; getline(is, addLine); line += addLine; } // Read in channel properties - products so far only as a string. int onMode = intAttributeValue( line, "onMode"); double bRatio = doubleAttributeValue( line, "bRatio"); int meMode = intAttributeValue( line, "meMode"); string products = attributeValue( line, "products"); // Read in decay products from stream. Must have at least one. istringstream prodStream(products); int prod0 = 0; int prod1 = 0; int prod2 = 0; int prod3 = 0; int prod4 = 0; int prod5 = 0; int prod6 = 0; int prod7 = 0; prodStream >> prod0 >> prod1 >> prod2 >> prod3 >> prod4 >> prod5 >> prod6 >> prod7; if (prod0 == 0) { infoPtr->errorMsg("Error in ParticleData::readXML:" " incomplete decay channel", line); return false; } // Store new channel (if particle already known). if (particlePtr == 0) { infoPtr->errorMsg("Error in ParticleData::readXML:" " orphan decay channel", line); return false; } particlePtr->addChannel(onMode, bRatio, meMode, prod0, prod1, prod2, prod3, prod4, prod5, prod6, prod7); // Check for occurence of a file also to be read. } else if (word1 == "errorMsg("Error in ParticleData::readXML:" " skip unrecognized file name", line); } else files.push_back(file); } // End of loop over lines in input file and loop over files. }; }; // All particle data at this stage defines baseline original. if (reset) for (map::iterator pdtEntry = pdt.begin(); pdtEntry != pdt.end(); ++pdtEntry) { particlePtr = &pdtEntry->second; particlePtr->setHasChanged(false); } // Done. isInit = true; return true; } //-------------------------------------------------------------------------- // Print out complete database in numerical order as an XML file. void ParticleData::listXML(string outFile) { // Convert file name to ofstream. const char* cstring = outFile.c_str(); ofstream os(cstring); // Iterate through the particle data table. for (map::iterator pdtEntry = pdt.begin(); pdtEntry != pdt.end(); ++pdtEntry) { particlePtr = &pdtEntry->second; // Print particle properties. os << "id() << "\"" << " name=\"" << particlePtr->name() << "\""; if (particlePtr->hasAnti()) os << " antiName=\"" << particlePtr->name(-1) << "\""; os << " spinType=\"" << particlePtr->spinType() << "\"" << " chargeType=\"" << particlePtr->chargeType() << "\"" << " colType=\"" << particlePtr->colType() << "\"\n"; // Pick format for mass and width based on mass value. double m0Now = particlePtr->m0(); if (m0Now == 0 || (m0Now > 0.1 && m0Now < 1000.)) os << fixed << setprecision(5); else os << scientific << setprecision(3); os << " m0=\"" << m0Now << "\""; if (particlePtr->mWidth() > 0.) os << " mWidth=\"" << particlePtr->mWidth() << "\"" << " mMin=\"" << particlePtr->mMin() << "\"" << " mMax=\"" << particlePtr->mMax() << "\""; if (particlePtr->tau0() > 0.) os << scientific << setprecision(5) << " tau0=\"" << particlePtr->tau0() << "\""; os << ">\n"; // Loop through the decay channel table for each particle. if (particlePtr->sizeChannels() > 0) { for (int i = 0; i < particlePtr->sizeChannels(); ++i) { const DecayChannel& channel = particlePtr->channel(i); int mult = channel.multiplicity(); // Print decay channel properties. os << " 0) os << " meMode=\"" << channel.meMode() << "\""; os << " products=\""; for (int j = 0; j < mult; ++j) { os << channel.product(j); if (j < mult - 1) os << " "; } // Finish off line and loop over allowed decay channels. os << "\"/>\n"; } } // Finish off existing particle. os << "\n\n"; } } //-------------------------------------------------------------------------- // Read in database from specific free format file. bool ParticleData::readFF(string inFile, bool reset) { // Normally reset whole database before beginning. if (reset) {pdt.clear(); isInit = false;} // Open file for read and check that instream is OK. const char* cstring = inFile.c_str(); ifstream is(cstring); if (!is.good()) { infoPtr->errorMsg("Error in ParticleData::readFF:" " did not find file", inFile); return false; } // Read in one line at a time. particlePtr = 0; string line; bool readParticle = false; while ( getline(is, line) ) { // Empty lines begins new particle. if (line.find_first_not_of(" \n\t\v\b\r\f\a") == string::npos) { readParticle = true; continue; } // Prepare to use standard read from line. istringstream readLine(line); // Read in a line with particle information. if (readParticle) { // Properties to be read. int idTmp; string nameTmp, antiNameTmp; int spinTypeTmp, chargeTypeTmp, colTypeTmp; double m0Tmp, mWidthTmp, mMinTmp, mMaxTmp, tau0Tmp; string mayTmp; // Do the reading. readLine >> idTmp >> nameTmp >> antiNameTmp >> spinTypeTmp >> chargeTypeTmp >> colTypeTmp >> m0Tmp >> mWidthTmp >> mMinTmp >> mMaxTmp >> tau0Tmp; // Error printout if something went wrong. if (!readLine) { infoPtr->errorMsg("Error in ParticleData::readFF:" " incomplete particle", line); return false; } // Erase if particle already exists. if (isParticle(idTmp)) pdt.erase(idTmp); // Store new particle. Save pointer, to be used for decay channels. addParticle( idTmp, nameTmp, antiNameTmp, spinTypeTmp, chargeTypeTmp, colTypeTmp, m0Tmp, mWidthTmp, mMinTmp, mMaxTmp, tau0Tmp); particlePtr = particleDataEntryPtr(idTmp); readParticle = false; // Read in a line with decay channel information. } else { // Properties to be read. int onMode = 0; double bRatio = 0.; int meMode = 0; int prod0 = 0; int prod1 = 0; int prod2 = 0; int prod3 = 0; int prod4 = 0; int prod5 = 0; int prod6 = 0; int prod7 = 0; // Read in data from stream. Need at least one decay product. readLine >> onMode >> bRatio >> meMode >> prod0; if (!readLine) { infoPtr->errorMsg("Error in ParticleData::readFF:" " incomplete decay channel", line); return false; } readLine >> prod1 >> prod2 >> prod3 >> prod4 >> prod5 >> prod6 >> prod7; // Store new channel. if (particlePtr == 0) { infoPtr->errorMsg("Error in ParticleData::readFF:" " orphan decay channel", line); return false; } particlePtr->addChannel(onMode, bRatio, meMode, prod0, prod1, prod2, prod3, prod4, prod5, prod6, prod7); } // End of while loop over lines in the file. } // Done. isInit = true; return true; } //-------------------------------------------------------------------------- // Print out complete database in numerical order as a free format file. void ParticleData::listFF(string outFile) { // Convert file name to ofstream. const char* cstring = outFile.c_str(); ofstream os(cstring); // Iterate through the particle data table. for (map::iterator pdtEntry = pdt.begin(); pdtEntry != pdt.end(); ++pdtEntry) { particlePtr = &pdtEntry->second; // Pick format for mass and width based on mass value. double m0Now = particlePtr->m0(); if (m0Now == 0 || (m0Now > 0.1 && m0Now < 1000.)) os << fixed << setprecision(5); else os << scientific << setprecision(3); // Print particle properties. os << "\n" << setw(8) << particlePtr->id() << " " << left << setw(16) << particlePtr->name() << " " << setw(16) << particlePtr->name(-1) << " " << right << setw(2) << particlePtr->spinType() << " " << setw(2) << particlePtr->chargeType() << " " << setw(2) << particlePtr->colType() << " " << setw(10) << particlePtr->m0() << " " << setw(10) << particlePtr->mWidth() << " " << setw(10) << particlePtr->mMin() << " " << setw(10) << particlePtr->mMax() << " " << scientific << setprecision(5) << setw(12) << particlePtr->tau0() << "\n"; // Loop through the decay channel table for each particle. if (particlePtr->sizeChannels() > 0) { for (int i = 0; i < particlePtr->sizeChannels(); ++i) { const DecayChannel& channel = particlePtr->channel(i); os << " " << setw(6) << channel.onMode() << " " << fixed << setprecision(7) << setw(10) << channel.bRatio() << " " << setw(3) << channel.meMode() << " "; for (int j = 0; j < channel.multiplicity(); ++j) os << setw(8) << channel.product(j) << " "; os << "\n"; } } } } //-------------------------------------------------------------------------- // Read in updates from a character string, like a line of a file. // Is used by readString (and readFile) in Pythia. bool ParticleData::readString(string lineIn, bool warn, ostream& os) { // If empty line then done. if (lineIn.find_first_not_of(" \n\t\v\b\r\f\a") == string::npos) return true; // Take copy that will be modified. string line = lineIn; // If first character is not a digit then taken to be a comment. int firstChar = line.find_first_not_of(" \n\t\v\b\r\f\a"); if (!isdigit(line[firstChar])) return true; // Replace colons and equal signs by blanks to make parsing simpler. for ( int j = 0; j < int(line.size()); ++ j) if (line[j] == ':' || line[j] == '=') line[j] = ' '; // Get particle id and property name. int idTmp; string property; istringstream getWord(line); getWord >> idTmp >> property; property = toLower(property); // Check that valid particle. if ( (!isParticle(idTmp) && property != "all" && property != "new") || idTmp <= 0) { if (warn) os << "\n PYTHIA Error: input particle not found in Particle" << " Data Table:\n " << lineIn << "\n"; readingFailedSave = true; return false; } // Identify particle property and read + set its value, case by case. if (property == "name") { string nameTmp; getWord >> nameTmp; pdt[idTmp].setName(nameTmp); return true; } if (property == "antiname") { string antiNameTmp; getWord >> antiNameTmp; pdt[idTmp].setAntiName(antiNameTmp); return true; } if (property == "names") { string nameTmp, antiNameTmp; getWord >> nameTmp >> antiNameTmp; pdt[idTmp].setNames(nameTmp, antiNameTmp); return true; } if (property == "spintype") { int spinTypeTmp; getWord >> spinTypeTmp; pdt[idTmp].setSpinType(spinTypeTmp); return true; } if (property == "chargetype") { int chargeTypeTmp; getWord >> chargeTypeTmp; pdt[idTmp].setChargeType(chargeTypeTmp); return true; } if (property == "coltype") { int colTypeTmp; getWord >> colTypeTmp; pdt[idTmp].setColType(colTypeTmp); return true; } if (property == "m0") { double m0Tmp; getWord >> m0Tmp; pdt[idTmp].setM0(m0Tmp); return true; } if (property == "mwidth") { double mWidthTmp; getWord >> mWidthTmp; pdt[idTmp].setMWidth(mWidthTmp); return true; } if (property == "mmin") { double mMinTmp; getWord >> mMinTmp; pdt[idTmp].setMMin(mMinTmp); return true; } if (property == "mmax") { double mMaxTmp; getWord >> mMaxTmp; pdt[idTmp].setMMax(mMaxTmp); return true; } if (property == "tau0") { double tau0Tmp; getWord >> tau0Tmp; pdt[idTmp].setTau0(tau0Tmp); return true; } if (property == "isresonance") { string isresTmp; getWord >> isresTmp; bool isResonanceTmp = boolString(isresTmp); pdt[idTmp].setIsResonance(isResonanceTmp); return true; } if (property == "maydecay") { string mayTmp; getWord >> mayTmp; bool mayDecayTmp = boolString(mayTmp); pdt[idTmp].setMayDecay(mayDecayTmp); return true; } if (property == "doexternaldecay") { string extdecTmp; getWord >> extdecTmp; bool doExternalDecayTmp = boolString(extdecTmp); pdt[idTmp].setDoExternalDecay(doExternalDecayTmp); return true; } if (property == "isvisible") { string isvisTmp; getWord >> isvisTmp; bool isVisibleTmp = boolString(isvisTmp); pdt[idTmp].setIsVisible(isVisibleTmp); return true; } if (property == "doforcewidth") { string doforceTmp; getWord >> doforceTmp; bool doForceWidthTmp = boolString(doforceTmp); pdt[idTmp].setDoForceWidth(doForceWidthTmp); return true; } // Addition or complete replacement of a particle. if (property == "all" || property == "new") { // Default values for properties to be read. string nameTmp = "void"; string antiNameTmp = "void"; int spinTypeTmp = 0; int chargeTypeTmp = 0; int colTypeTmp = 0; double m0Tmp = 0.; double mWidthTmp = 0.; double mMinTmp = 0.; double mMaxTmp = 0.; double tau0Tmp = 0.; // Read in data from stream. getWord >> nameTmp >> antiNameTmp >> spinTypeTmp >> chargeTypeTmp >> colTypeTmp >> m0Tmp >> mWidthTmp >> mMinTmp >> mMaxTmp >> tau0Tmp; // To keep existing decay channels, only overwrite particle data. if (property == "all" && isParticle(idTmp)) { setAll( idTmp, nameTmp, antiNameTmp, spinTypeTmp, chargeTypeTmp, colTypeTmp, m0Tmp, mWidthTmp, mMinTmp, mMaxTmp, tau0Tmp); // Else start over completely from scratch. } else { if (isParticle(idTmp)) pdt.erase(idTmp); addParticle( idTmp, nameTmp, antiNameTmp, spinTypeTmp, chargeTypeTmp, colTypeTmp, m0Tmp, mWidthTmp, mMinTmp, mMaxTmp, tau0Tmp); } return true; } // Set onMode of all decay channels in one go. if (property == "onmode") { int onMode = 0; string onModeIn; getWord >> onModeIn; // For onMode allow the optional possibility of Bool input. if (isdigit(onModeIn[0])) { istringstream getOnMode(onModeIn); getOnMode >> onMode; } else onMode = (boolString(onModeIn)) ? 1 : 0; for (int i = 0; i < pdt[idTmp].sizeChannels(); ++i) pdt[idTmp].channel(i).onMode(onMode); return true; } // Selective search for matching decay channels. int matchKind = 0; if (property == "offifany" || property == "onifany" || property == "onposifany" || property == "onnegifany") matchKind = 1; if (property == "offifall" || property == "onifall" || property == "onposifall" || property == "onnegifall") matchKind = 2; if (property == "offifmatch" || property == "onifmatch" || property == "onposifmatch" || property == "onnegifmatch") matchKind = 3; if (matchKind > 0) { int onMode = 0; if (property == "onifany" || property == "onifall" || property == "onifmatch") onMode = 1; if (property == "onposifany" || property == "onposifall" || property == "onposifmatch") onMode = 2; if (property == "onnegifany" || property == "onnegifall" || property == "onnegifmatch") onMode = 3; // Read in particles to match. vector idToMatch; int idRead; for ( ; ; ) { getWord >> idRead; if (!getWord) break; idToMatch.push_back(abs(idRead)); } int nToMatch = idToMatch.size(); // Loop over all decay channels. for (int i = 0; i < pdt[idTmp].sizeChannels(); ++i) { int multi = pdt[idTmp].channel(i).multiplicity(); // Look for any match at all. if (matchKind == 1) { bool foundMatch = false; for (int j = 0; j < multi; ++j) { int idNow = abs(pdt[idTmp].channel(i).product(j)); for (int k = 0; k < nToMatch; ++k) if (idNow == idToMatch[k]) {foundMatch = true; break;} if (foundMatch) break; } if (foundMatch) pdt[idTmp].channel(i).onMode(onMode); // Look for match of all products provided. } else { int nUnmatched = nToMatch; if (multi < nToMatch); else if (multi > nToMatch && matchKind == 3); else { vector idUnmatched; for (int k = 0; k < nToMatch; ++k) idUnmatched.push_back(idToMatch[k]); for (int j = 0; j < multi; ++j) { int idNow = abs(pdt[idTmp].channel(i).product(j)); for (int k = 0; k < nUnmatched; ++k) if (idNow == idUnmatched[k]) { idUnmatched[k] = idUnmatched[--nUnmatched]; break; } if (nUnmatched == 0) break; } } if (nUnmatched == 0) pdt[idTmp].channel(i).onMode(onMode); } } return true; } // Rescale all branching ratios by common factor. if (property == "rescalebr") { double factor; getWord >> factor; pdt[idTmp].rescaleBR(factor); return true; } // Reset decay table in preparation for new input. if (property == "onechannel") pdt[idTmp].clearChannels(); // Add or change a decay channel: get channel number and new property. if (property == "addchannel" || property == "onechannel" || isdigit(property[0])) { int channel; if (property == "addchannel" || property == "onechannel") { pdt[idTmp].addChannel(); channel = pdt[idTmp].sizeChannels() - 1; property = "all"; } else{ istringstream getChannel(property); getChannel >> channel; getWord >> property; property = toLower(property); } // Check that channel exists. if (channel < 0 || channel >= pdt[idTmp].sizeChannels()) return false; // Find decay channel property and value, case by case. // At same time also do case where all should be replaced. if (property == "onmode" || property == "all") { int onMode = 0; string onModeIn; getWord >> onModeIn; // For onMode allow the optional possibility of Bool input. if (isdigit(onModeIn[0])) { istringstream getOnMode(onModeIn); getOnMode >> onMode; } else onMode = (boolString(onModeIn)) ? 1 : 0; pdt[idTmp].channel(channel).onMode(onMode); if (property == "onmode") return true; } if (property == "bratio" || property == "all") { double bRatio; getWord >> bRatio; pdt[idTmp].channel(channel).bRatio(bRatio); if (property == "bratio") return true; } if (property == "memode" || property == "all") { int meMode; getWord >> meMode; pdt[idTmp].channel(channel).meMode(meMode); if (property == "memode") return true; } // Scan for products until end of line. if (property == "products" || property == "all") { int nProd = 0; for (int iProd = 0; iProd < 8; ++iProd) { int idProd; getWord >> idProd; if (!getWord) break; pdt[idTmp].channel(channel).product(iProd, idProd); ++nProd; } for (int iProd = nProd; iProd < 8; ++iProd) pdt[idTmp].channel(channel).product(iProd, 0); pdt[idTmp].channel(channel).multiplicity(nProd); return true; } // Rescale an existing branching ratio. if (property == "rescalebr") { double factor; getWord >> factor; pdt[idTmp].channel(channel).rescaleBR(factor); return true; } } // Return false if failed to recognize property. if (warn) os << "\n PYTHIA Error: input property not found in Particle" << " Data Table:\n " << lineIn << "\n"; readingFailedSave = true; return false; } //-------------------------------------------------------------------------- // Print out complete or changed table of database in numerical order. void ParticleData::list(bool changedOnly, bool changedRes, ostream& os) { // Table header; output for bool as off/on. if (!changedOnly) { os << "\n -------- PYTHIA Particle Data Table (complete) --------" << "------------------------------------------------------------" << "--------------\n \n"; } else { os << "\n -------- PYTHIA Particle Data Table (changed only) ----" << "------------------------------------------------------------" << "--------------\n \n"; } os << " id name antiName spn chg col m0" << " mWidth mMin mMax tau0 res dec ext " << "vis wid\n no onMode bRatio meMode products \n"; // Iterate through the particle data table. Option to skip unchanged. int nList = 0; for (map::iterator pdtEntry = pdt.begin(); pdtEntry != pdt.end(); ++pdtEntry) { particlePtr = &pdtEntry->second; if ( !changedOnly || particlePtr->hasChanged() || ( changedRes && particlePtr->getResonancePtr() != 0 ) ) { // Pick format for mass and width based on mass value. double m0Now = particlePtr->m0(); if (m0Now == 0 || (m0Now > 0.1 && m0Now < 1000.)) os << fixed << setprecision(5); else os << scientific << setprecision(3); // Print particle properties. ++nList; string antiNameTmp = particlePtr->name(-1); if (antiNameTmp == "void") antiNameTmp = " "; os << "\n" << setw(8) << particlePtr->id() << " " << left << setw(16) << particlePtr->name() << " " << setw(16) << antiNameTmp << " " << right << setw(2) << particlePtr->spinType() << " " << setw(2) << particlePtr->chargeType() << " " << setw(2) << particlePtr->colType() << " " << setw(10) << particlePtr->m0() << " " << setw(10) << particlePtr->mWidth() << " " << setw(10) << particlePtr->mMin() << " " << setw(10) << particlePtr->mMax() << " " << scientific << setprecision(5) << setw(12) << particlePtr->tau0() << " " << setw(2) << particlePtr->isResonance() << " " << setw(2) << (particlePtr->mayDecay() && particlePtr->canDecay()) << " " << setw(2) << particlePtr->doExternalDecay() << " " << setw(2) << particlePtr->isVisible()<< " " << setw(2) << particlePtr->doForceWidth() << "\n"; // Loop through the decay channel table for each particle. if (particlePtr->sizeChannels() > 0) { for (int i = 0; i < int(particlePtr->sizeChannels()); ++i) { const DecayChannel& channel = particlePtr->channel(i); os << " " << setprecision(7) << setw(5) << i << setw(6) << channel.onMode() << fixed<< setw(12) << channel.bRatio() << setw(5) << channel.meMode() << " "; for (int j = 0; j < channel.multiplicity(); ++j) os << setw(8) << channel.product(j) << " "; os << "\n"; } } } } // End of loop over database contents. if (changedOnly && nList == 0) os << "\n no particle data has been " << "changed from its default value \n"; os << "\n -------- End PYTHIA Particle Data Table -----------------" << "--------------------------------------------------------------" << "----------\n" << endl; } //-------------------------------------------------------------------------- // Print out partial table of database in input order. void ParticleData::list(vector idList, ostream& os) { // Table header; output for bool as off/on. os << "\n -------- PYTHIA Particle Data Table (partial) ---------" << "------------------------------------------------------------" << "--------------\n \n"; os << " id name antiName spn chg col m0" << " mWidth mMin mMax tau0 res dec ext " << "vis wid\n no onMode bRatio meMode products \n"; // Iterate through the given list of input particles. for (int i = 0; i < int(idList.size()); ++i) { particlePtr = particleDataEntryPtr(idList[i]); // Pick format for mass and width based on mass value. double m0Now = particlePtr->m0(); if (m0Now == 0 || (m0Now > 0.1 && m0Now < 1000.)) os << fixed << setprecision(5); else os << scientific << setprecision(3); // Print particle properties. string antiNameTmp = particlePtr->name(-1); if (antiNameTmp == "void") antiNameTmp = " "; os << "\n" << setw(8) << particlePtr->id() << " " << left << setw(16) << particlePtr->name() << " " << setw(16) << antiNameTmp << " " << right << setw(2) << particlePtr->spinType() << " " << setw(2) << particlePtr->chargeType() << " " << setw(2) << particlePtr->colType() << " " << setw(10) << particlePtr->m0() << " " << setw(10) << particlePtr->mWidth() << " " << setw(10) << particlePtr->mMin() << " " << setw(10) << particlePtr->mMax() << " " << scientific << setprecision(5) << setw(12) << particlePtr->tau0() << " " << setw(2) << particlePtr->isResonance() << " " << setw(2) << (particlePtr->mayDecay() && particlePtr->canDecay()) << " " << setw(2) << particlePtr->doExternalDecay() << " " << setw(2) << particlePtr->isVisible() << " " << setw(2) << particlePtr->doForceWidth() << "\n"; // Loop through the decay channel table for each particle. if (particlePtr->sizeChannels() > 0) { for (int j = 0; j < int(particlePtr->sizeChannels()); ++j) { const DecayChannel& channel = particlePtr->channel(j); os << " " << setprecision(7) << setw(5) << j << setw(6) << channel.onMode() << fixed<< setw(12) << channel.bRatio() << setw(5) << channel.meMode() << " "; for (int k = 0; k < channel.multiplicity(); ++k) os << setw(8) << channel.product(k) << " "; os << "\n"; } } } // End of loop over database contents. os << "\n -------- End PYTHIA Particle Data Table -----------------" << "--------------------------------------------------------------" << "----------\n" << endl; } //-------------------------------------------------------------------------- // Check that table makes sense: e.g. consistent names and mass ranges, // that branching ratios sum to unity, that charge is conserved and // that phase space is open in each channel. // verbosity = 0: mimimal amount of checks, e.g. that no channels open. // = 1: further warning if individual channels closed // (except for resonances). // = 2: also print branching-ratio-averaged threshold mass. // = 11, 12: as 1, 2, but include resonances in detailed checks. void ParticleData::checkTable(int verbosity, ostream& os) { // Header. os << "\n -------- PYTHIA Check of Particle Data Table ------------" <<"------\n\n"; int nErr = 0; // Loop through all particles. for (map::iterator pdtEntry = pdt.begin(); pdtEntry != pdt.end(); ++pdtEntry) { particlePtr = &pdtEntry->second; // Extract some particle properties. Set some flags. int idNow = particlePtr->id(); bool hasAntiNow = particlePtr->hasAnti(); int spinTypeNow = particlePtr->spinType(); int chargeTypeNow = particlePtr->chargeType(); int baryonTypeNow = particlePtr->baryonNumberType(); double m0Now = particlePtr->m0(); double mMinNow = particlePtr->mMin(); double mMaxNow = particlePtr->mMax(); double mWidthNow = particlePtr->mWidth(); double tau0Now = particlePtr->tau0(); bool isResonanceNow = particlePtr->isResonance(); bool hasPrinted = false; bool studyCloser = verbosity > 10 || !isResonanceNow; // Check that particle name consistent with charge information. string particleName = particlePtr->name(1); if (particleName.size() > 16) { os << " Warning: particle " << idNow << " has name " << particleName << " of length " << particleName.size() << "\n"; hasPrinted = true; ++nErr; } int nPos = 0; int nNeg = 0; for (int i = 0; i < int(particleName.size()); ++i) { if (particleName[i] == '+') ++nPos; if (particleName[i] == '-') ++nNeg; } if ( (nPos > 0 && nNeg > 0) || ( nPos + nNeg > 0 && 3 * (nPos - nNeg) != chargeTypeNow )) { os << " Warning: particle " << idNow << " has name " << particleName << " inconsistent with charge type " << chargeTypeNow << "\n"; hasPrinted = true; ++nErr; } // Check that antiparticle name consistent with charge information. if (hasAntiNow) { particleName = particlePtr->name(-1); if (particleName.size() > 16) { os << " Warning: particle " << idNow << " has name " << particleName << " of length " << particleName.size() << "\n"; hasPrinted = true; ++nErr; } nPos = 0; nNeg = 0; for (int i = 0; i < int(particleName.size()); ++i) { if (particleName[i] == '+') ++nPos; if (particleName[i] == '-') ++nNeg; } if ( (nPos > 0 && nNeg > 0) || ( nPos + nNeg > 0 && 3 * (nPos - nNeg) != -chargeTypeNow )) { os << " Warning: particle " << -idNow << " has name " << particleName << " inconsistent with charge type " << -chargeTypeNow << "\n"; hasPrinted = true; ++nErr; } } // Check that mass, mass range and width are consistent. if (particlePtr->useBreitWigner()) { if (mMinNow > m0Now) { os << " Error: particle " << idNow << " has mMin " << fixed << setprecision(5) << mMinNow << " larger than m0 " << m0Now << "\n"; hasPrinted = true; ++nErr; } if (mMaxNow > mMinNow && mMaxNow < m0Now) { os << " Error: particle " << idNow << " has mMax " << fixed << setprecision(5) << mMaxNow << " smaller than m0 " << m0Now << "\n"; hasPrinted = true; ++nErr; } if (mMaxNow > mMinNow && mMaxNow - mMinNow < mWidthNow) { os << " Warning: particle " << idNow << " has mMax - mMin " << fixed << setprecision(5) << mMaxNow - mMinNow << " smaller than mWidth " << mWidthNow << "\n"; hasPrinted = true; ++nErr; } } // Check that particle does not both have width and lifetime. if (mWidthNow > 0. && tau0Now > 0.) { os << " Warning: particle " << idNow << " has both nonvanishing width " << scientific << setprecision(5) << mWidthNow << " and lifetime " << tau0Now << "\n"; hasPrinted = true; ++nErr; } // Begin study decay channels. if (particlePtr->sizeChannels() > 0) { // Loop through all decay channels. double bRatioSum = 0.; double bRatioPos = 0.; double bRatioNeg = 0.; bool hasPosBR = false; bool hasNegBR = false; double threshMass = 0.; bool openChannel = false; for (int i = 0; i < particlePtr->sizeChannels(); ++i) { // Extract channel properties. int onMode = particlePtr->channel(i).onMode(); double bRatio = particlePtr->channel(i).bRatio(); int meMode = particlePtr->channel(i).meMode(); int mult = particlePtr->channel(i).multiplicity(); int prod[8]; for (int j = 0; j < 8; ++j) prod[j] = particlePtr->channel(i).product(j); // Sum branching ratios. Include off-channels. if (onMode == 0 || onMode == 1) bRatioSum += bRatio; else if (onMode == 2) {bRatioPos += bRatio; hasPosBR = true;} else if (onMode == 3) {bRatioNeg += bRatio; hasNegBR = true;} // Error printout when unknown decay product code. for (int j = 0; j < 8; ++j) { if ( prod[j] != 0 && !isParticle(prod[j]) ) { os << " Error: unknown decay product for " << idNow << " -> " << prod[j] << "\n"; hasPrinted = true; ++nErr; continue; } } // Error printout when no decay products or 0 interspersed. int nLast = 0; for (int j = 0; j < 8; ++j) if (prod[j] != 0) nLast = j + 1; if (mult == 0 || mult != nLast) { os << " Error: corrupted decay product list for " << particlePtr->id() << " -> "; for (int j = 0; j < 8; ++j) os << prod[j] << " "; os << "\n"; hasPrinted = true; ++nErr; continue; } // Check charge conservation and open phase space in decay channel. int chargeTypeSum = -chargeTypeNow; int baryonTypeSum = -baryonTypeNow; double avgFinalMass = 0.; double minFinalMass = 0.; bool canHandle = true; for (int j = 0; j < mult; ++j) { chargeTypeSum += chargeType( prod[j] ); baryonTypeSum += baryonNumberType( prod[j] ); avgFinalMass += m0( prod[j] ); minFinalMass += m0Min( prod[j] ); if (prod[j] == 81 || prod[j] == 82 || prod[j] == 83) canHandle = false; } threshMass += bRatio * avgFinalMass; // Error printout when charge or baryon number not conserved. if (chargeTypeSum != 0 && canHandle) { os << " Error: 3*charge changed by " << chargeTypeSum << " in " << idNow << " -> "; for (int j = 0; j < mult; ++j) os << prod[j] << " "; os << "\n"; hasPrinted = true; ++nErr; continue; } if ( baryonTypeSum != 0 && canHandle && particlePtr->isHadron() ) { os << " Error: 3*baryon number changed by " << baryonTypeSum << " in " << idNow << " -> "; for (int j = 0; j < mult; ++j) os << prod[j] << " "; os << "\n"; hasPrinted = true; ++nErr; continue; } // Begin check that some matrix elements are used correctly. bool correctME = true; // Check matrix element mode 0: recommended not into partons. if (meMode == 0 && !isResonanceNow) { bool hasPartons = false; for (int j = 0; j < mult; ++j) { int idAbs = abs(prod[j]); if ( idAbs < 10 || idAbs == 21 || idAbs == 81 || idAbs == 82 || idAbs == 83 || (idAbs > 1000 && idAbs < 10000 && (idAbs/10)%10 == 0) ) hasPartons = true; } if (hasPartons) correctME = false; } // Check matrix element mode 1: rho/omega -> pi+ pi- pi0. bool useME1 = ( mult == 3 && spinTypeNow == 3 && idNow > 100 && idNow < 1000 && particlePtr->channel(i).contains(211, -211, 111) ); if ( meMode == 1 && !useME1 ) correctME = false; if ( meMode != 1 && useME1 ) correctME = false; // Check matrix element mode 2: polarization in V -> PS + PS. bool useME2 = ( mult == 2 && spinTypeNow == 3 && idNow > 100 && idNow < 1000 && spinType(prod[0]) == 1 && spinType(prod[1]) == 1 ); if ( meMode == 2 && !useME2 ) correctME = false; if ( meMode != 2 && useME2 ) correctME = false; // Check matrix element mode 11, 12 and 13: Dalitz decay with // one or more particles in addition to the lepton pair, // or double Dalitz decay. bool useME11 = ( mult == 3 && !isResonanceNow && (prod[1] == 11 || prod[1] == 13 || prod[1] == 15) && prod[2] == -prod[1] ); bool useME12 = ( mult > 3 && !isResonanceNow && (prod[mult - 2] == 11 || prod[mult - 2] == 13 || prod[mult - 2] == 15) && prod[mult - 1] == -prod[mult - 2] ); bool useME13 = ( mult == 4 && !isResonanceNow && (prod[0] == 11 || prod[0] == 13) && prod[1] == -prod[0] && (prod[2] == 11 || prod[2] == 13) && prod[3] == -prod[2] ); if (useME13) useME12 = false; if ( meMode == 11 && !useME11 ) correctME = false; if ( meMode != 11 && useME11 ) correctME = false; if ( meMode == 12 && !useME12 ) correctME = false; if ( meMode != 12 && useME12 ) correctME = false; if ( meMode == 13 && !useME13 ) correctME = false; if ( meMode != 13 && useME13 ) correctME = false; // Check matrix element mode 21: tau -> nu_tau hadrons. bool useME21 = (idNow == 15 && mult > 2 && prod[0] == 16 && abs(prod[1]) > 100); if ( meMode == 21 && !useME21 ) correctME = false; if ( meMode != 21 && useME21 ) correctME = false; // Check matrix element mode 22, but only for semileptonic decay. // For a -> b c d require types u = 2, ubar = -2, d = 1, dbar = -1. if ( isLepton(prod[0]) && isLepton(prod[1]) ) { bool useME22 = false; int typeA = 0; int typeB = 0; int typeC = 0; if (particlePtr->isLepton()) { typeA = (idNow > 0) ? 1 + (idNow-1)%2 : -1 - (1-idNow)%2; } else if (particlePtr->isHadron()) { int hQ = particlePtr->heaviestQuark(); // Special case: for B_c either bbar or c decays. if (idNow == 541 && heaviestQuark(prod[2]) == -5) hQ = 4; typeA = (hQ > 0) ? 1 + (hQ-1)%2 : -1 - (1-hQ)%2; } typeB = (prod[0] > 0) ? 1 + (prod[0]-1)%2 : -1 - (1-prod[0])%2; typeC = (prod[1] > 0) ? 1 + (prod[1]-1)%2 : -1 - (1-prod[1])%2; // Special cases. if ( (idNow == 130 || idNow == 310) && typeC * typeA < 0) typeA = -typeA; if (mult == 3 && idNow == 2112 && prod[2] == 2212) typeA = 3 - typeA; if (mult == 3 && idNow == 3222 && prod[2] == 3122) typeA = 3 - typeA; if (mult > 2 && typeC == typeA && typeB * typeC < 0 && (typeB + typeC)%2 != 0) useME22 = true; if ( meMode == 22 && !useME22 ) correctME = false; if ( meMode != 22 && useME22 ) correctME = false; } // Check for matrix element mode 31. if (meMode == 31) { int nGamma = 0; for (int j = 0; j < mult; ++j) if (prod[j] == 22) ++nGamma; if (nGamma != 1) correctME = false; } // Check for unknown mode, or resonance-only mode. if ( !isResonanceNow && (meMode < 0 || (meMode > 2 && meMode <= 10) || (meMode > 13 && meMode <= 20) || (meMode > 23 && meMode <= 30) || (meMode > 31 && meMode <= 41) || meMode == 51 || meMode == 61 || meMode == 71 || (meMode > 80 && meMode <= 90) || (!particlePtr->isOctetHadron() && meMode > 92) ) ) correctME = false; // Print if incorrect matrix element mode. if ( !correctME ) { os << " Warning: meMode " << meMode << " used for " << idNow << " -> "; for (int j = 0; j < mult; ++j) os << prod[j] << " "; os << "\n"; hasPrinted = true; ++nErr; } // Warning printout when no phase space for decay. if ( studyCloser && verbosity > 0 && canHandle && onMode > 0 && particlePtr->m0Min() - minFinalMass < 0. ) { if (particlePtr->m0Max() - minFinalMass < 0.) os << " Error: decay never possible for "; else os << " Warning: decay sometimes not possible for "; os << idNow << " -> "; for (int j = 0; j < mult; ++j) os << prod[j] << " "; os << "\n"; hasPrinted = true; ++nErr; } // End loop over decay channels. if (onMode > 0 && bRatio > 0.) openChannel = true; } // Optional printout of threshold. if (verbosity%10 > 1 && particlePtr->useBreitWigner()) { threshMass /= bRatioSum; os << " Info: particle " << idNow << fixed << setprecision(5) << " has average mass threshold " << threshMass << " while mMin is " << mMinNow << "\n"; hasPrinted = true; } // Error printout when no acceptable decay channels found. if (studyCloser && !openChannel) { os << " Error: no acceptable decay channel found for particle " << idNow << "\n"; hasPrinted = true; ++nErr; } // Warning printout when branching ratios do not sum to unity. if (studyCloser && (!hasAntiNow || (!hasPosBR && !hasNegBR)) && abs(bRatioSum + bRatioPos - 1.) > 1e-8) { os << " Warning: particle " << idNow << fixed << setprecision(8) << " has branching ratio sum " << bRatioSum << "\n"; hasPrinted = true; ++nErr; } else if (studyCloser && hasAntiNow && (abs(bRatioSum + bRatioPos - 1.) > 1e-8 || abs(bRatioSum + bRatioNeg - 1.) > 1e-8)) { os << " Warning: particle " << idNow << fixed << setprecision(8) << " has branching ratio sum " << bRatioSum + bRatioPos << " while its antiparticle has " << bRatioSum + bRatioNeg << "\n"; hasPrinted = true; ++nErr; } // End study of decay channels and loop over particles. } if (hasPrinted) os << "\n"; } // Final output. Done. os << " Total number of errors and warnings is " << nErr << "\n"; os << "\n -------- End PYTHIA Check of Particle Data Table --------" << "------\n" << endl; } //-------------------------------------------------------------------------- // Return the id of the sequentially next particle stored in table. int ParticleData::nextId(int idIn) { // Return 0 for negative or unknown codes. Return first for 0. if (idIn < 0 || (idIn > 0 && !isParticle(idIn))) return 0; if (idIn == 0) return pdt.begin()->first; // Find pointer to current particle and step up. Return 0 if impossible. map::const_iterator pdtIn = pdt.find(idIn); if (pdtIn == pdt.end()) return 0; ++pdtIn; if (pdtIn == pdt.end()) return 0; return pdtIn->first; } //-------------------------------------------------------------------------- // Fractional width associated with open channels of one or two resonances. double ParticleData::resOpenFrac(int id1In, int id2In, int id3In) { // Default value. double answer = 1.; // First resonance. if (isParticle(id1In)) answer = pdt[abs(id1In)].resOpenFrac(id1In); // Possibly second resonance. if (isParticle(id2In)) answer *= pdt[abs(id2In)].resOpenFrac(id2In); // Possibly third resonance. if (isParticle(id3In)) answer *= pdt[abs(id2In)].resOpenFrac(id3In); // Done. return answer; } //-------------------------------------------------------------------------- // Extract XML value string following XML attribute. string ParticleData::attributeValue(string line, string attribute) { if (line.find(attribute) == string::npos) return ""; int iBegAttri = line.find(attribute); int iBegQuote = line.find("\"", iBegAttri + 1); int iEndQuote = line.find("\"", iBegQuote + 1); return line.substr(iBegQuote + 1, iEndQuote - iBegQuote - 1); } //-------------------------------------------------------------------------- // Extract XML bool value following XML attribute. bool ParticleData::boolAttributeValue(string line, string attribute) { string valString = attributeValue(line, attribute); if (valString == "") return false; return boolString(valString); } //-------------------------------------------------------------------------- // Extract XML int value following XML attribute. int ParticleData::intAttributeValue(string line, string attribute) { string valString = attributeValue(line, attribute); if (valString == "") return 0; istringstream valStream(valString); int intVal; valStream >> intVal; return intVal; } //-------------------------------------------------------------------------- // Extract XML double value following XML attribute. double ParticleData::doubleAttributeValue(string line, string attribute) { string valString = attributeValue(line, attribute); if (valString == "") return 0.; istringstream valStream(valString); double doubleVal; valStream >> doubleVal; return doubleVal; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaEW.cc0000644000175000017500000026303412217346250014735 0ustar sunsun// SigmaEW.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // electroweak simulation classes (including photon processes). #include "Pythia8/SigmaEW.h" namespace Pythia8 { //========================================================================== // Sigma2qg2qgamma class. // Cross section for q g -> q gamma. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qg2qgamma::sigmaKin() { // Calculate kinematics dependence. sigUS = (1./3.) * (sH2 + uH2) / (-sH * uH); // Answer. sigma0 = (M_PI/sH2) * alpS * alpEM * sigUS; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qg2qgamma::sigmaHat() { // Incoming flavour gives charge factor. int idNow = (id2 == 21) ? id1 : id2; double eNow = couplingsPtr->ef( abs(idNow) ); return sigma0 * pow2(eNow); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2qgamma::setIdColAcol() { // Construct outgoing flavours. id3 = (id1 == 21) ? 22 : id1; id4 = (id2 == 21) ? 22 : id2; setId( id1, id2, id3, id4); // Colour flow topology. Swap if first is gluon, or when antiquark. setColAcol( 1, 0, 2, 1, 2, 0, 0, 0); if (id1 == 21) swapCol1234(); if (id1 < 0 || id2 < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2ggamma class. // Cross section for q qbar -> g gamma. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2ggamma::sigmaKin() { // Calculate kinematics dependence. double sigTU = (8./9.) * (tH2 + uH2) / (tH * uH); // Answer. sigma0 = (M_PI/sH2) * alpS * alpEM * sigTU; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2ggamma::sigmaHat() { // Incoming flavour gives charge factor. double eNow = couplingsPtr->ef( abs(id1) ); return sigma0 * pow2(eNow); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2ggamma::setIdColAcol() { // Outgoing flavours trivial. setId( id1, id2, 21, 22); // One colour flow topology. Swap if first is antiquark. setColAcol( 1, 0, 0, 2, 1, 2, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2gg2ggamma class. // Cross section for g g -> g gamma. // Proceeds through a quark box, by default using 5 massless quarks. //-------------------------------------------------------------------------- // Initialize process, especially parton-flux object. void Sigma2gg2ggamma::initProc() { // Maximum quark flavour in loop. int nQuarkLoop = settingsPtr->mode("PromptPhoton:nQuarkLoop"); // Calculate charge factor from the allowed quarks in the box. chargeSum = - 1./3. + 2./3. - 1./3.; if (nQuarkLoop >= 4) chargeSum += 2./3.; if (nQuarkLoop >= 5) chargeSum -= 1./3.; if (nQuarkLoop >= 6) chargeSum += 2./3.; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat). void Sigma2gg2ggamma::sigmaKin() { // Logarithms of Mandelstam variable ratios. double logST = log( -sH / tH ); double logSU = log( -sH / uH ); double logTU = log( tH / uH ); // Real and imaginary parts of separate amplitudes. double b0stuRe = 1. + (tH - uH) / sH * logTU + 0.5 * (tH2 + uH2) / sH2 * (pow2(logTU) + pow2(M_PI)); double b0stuIm = 0.; double b0tsuRe = 1. + (sH - uH) / tH * logSU + 0.5 * (sH2 + uH2) / tH2 * pow2(logSU); double b0tsuIm = -M_PI * ( (sH - uH) / tH + (sH2 + uH2) / tH2 * logSU); double b0utsRe = 1. + (sH - tH) / uH * logST + 0.5 * (sH2 + tH2) / uH2 * pow2(logST); double b0utsIm = -M_PI * ( (sH - tH) / uH + (sH2 + tH2) / uH2 * logST); double b1stuRe = -1.; double b1stuIm = 0.; double b2stuRe = -1.; double b2stuIm = 0.; // Calculate kinematics dependence. double sigBox = pow2(b0stuRe) + pow2(b0stuIm) + pow2(b0tsuRe) + pow2(b0tsuIm) + pow2(b0utsRe) + pow2(b0utsIm) + 4. * pow2(b1stuRe) + 4. * pow2(b1stuIm) + pow2(b2stuRe) + pow2(b2stuIm); // Answer. sigma = (5. / (192. * M_PI * sH2)) * pow2(chargeSum) * pow3(alpS) * alpEM * sigBox; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2ggamma::setIdColAcol() { // Flavours and colours are trivial. setId( id1, id2, 21, 22); setColAcol( 1, 2, 2, 3, 1, 3, 0, 0); if (rndmPtr->flat() > 0.5) swapColAcol(); } //========================================================================== // Sigma2ffbar2gammagamma class. // Cross section for q qbar -> gamma gamma. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2gammagamma::sigmaKin() { // Calculate kinematics dependence. sigTU = 2. * (tH2 + uH2) / (tH * uH); // Answer contains factor 1/2 from identical photons. sigma0 = (M_PI/sH2) * pow2(alpEM) * 0.5 * sigTU; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2gammagamma::sigmaHat() { // Incoming flavour gives charge and colour factors. double eNow = couplingsPtr->ef( abs(id1) ); double colFac = (abs(id1) < 9) ? 1. / 3. : 1.; return sigma0 * pow4(eNow) * colFac; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2gammagamma::setIdColAcol() { // Outgoing flavours trivial. setId( id1, id2, 22, 22); // No colours at all or one flow topology. Swap if first is antiquark. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2gg2gammagamma class. // Cross section for g g -> gamma gamma. // Proceeds through a quark box, by default using 5 massless quarks. //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2gammagamma::initProc() { // Maximum quark flavour in loop. int nQuarkLoop = settingsPtr->mode("PromptPhoton:nQuarkLoop"); // Calculate charge factor from the allowed quarks in the box. charge2Sum = 1./9. + 4./9. + 1./9.; if (nQuarkLoop >= 4) charge2Sum += 4./9.; if (nQuarkLoop >= 5) charge2Sum += 1./9.; if (nQuarkLoop >= 6) charge2Sum += 4./9.; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat). void Sigma2gg2gammagamma::sigmaKin() { // Logarithms of Mandelstam variable ratios. double logST = log( -sH / tH ); double logSU = log( -sH / uH ); double logTU = log( tH / uH ); // Real and imaginary parts of separate amplitudes. double b0stuRe = 1. + (tH - uH) / sH * logTU + 0.5 * (tH2 + uH2) / sH2 * (pow2(logTU) + pow2(M_PI)); double b0stuIm = 0.; double b0tsuRe = 1. + (sH - uH) / tH * logSU + 0.5 * (sH2 + uH2) / tH2 * pow2(logSU); double b0tsuIm = -M_PI * ( (sH - uH) / tH + (sH2 + uH2) / tH2 * logSU); double b0utsRe = 1. + (sH - tH) / uH * logST + 0.5 * (sH2 + tH2) / uH2 * pow2(logST); double b0utsIm = -M_PI * ( (sH - tH) / uH + (sH2 + tH2) / uH2 * logST); double b1stuRe = -1.; double b1stuIm = 0.; double b2stuRe = -1.; double b2stuIm = 0.; // Calculate kinematics dependence. double sigBox = pow2(b0stuRe) + pow2(b0stuIm) + pow2(b0tsuRe) + pow2(b0tsuIm) + pow2(b0utsRe) + pow2(b0utsIm) + 4. * pow2(b1stuRe) + 4. * pow2(b1stuIm) + pow2(b2stuRe) + pow2(b2stuIm); // Answer contains factor 1/2 from identical photons. sigma = (0.5 / (16. * M_PI * sH2)) * pow2(charge2Sum) * pow2(alpS) * pow2(alpEM) * sigBox; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2gammagamma::setIdColAcol() { // Flavours and colours are trivial. setId( id1, id2, 22, 22); setColAcol( 1, 2, 2, 1, 0, 0, 0, 0); } //========================================================================== // Sigma2ff2fftgmZ class. // Cross section for f f' -> f f' via t-channel gamma*/Z0 exchange // (f is quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma2ff2fftgmZ::initProc() { // Store Z0 mass for propagator. Common coupling factor. gmZmode = settingsPtr->mode("WeakZ0:gmZmode"); mZ = particleDataPtr->m0(23); mZS = mZ*mZ; thetaWRat = 1. / (16. * couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ff2fftgmZ::sigmaKin() { // Cross section part common for all incoming flavours. double sigma0 = (M_PI / sH2) * pow2(alpEM); // Kinematical functions for gamma-gamma, gamma-Z and Z-Z parts. sigmagmgm = sigma0 * 2. * (sH2 + uH2) / tH2; sigmagmZ = sigma0 * 4. * thetaWRat * sH2 / (tH * (tH - mZS)); sigmaZZ = sigma0 * 2. * pow2(thetaWRat) * sH2 / pow2(tH - mZS); if (gmZmode == 1) {sigmagmZ = 0.; sigmaZZ = 0.;} if (gmZmode == 2) {sigmagmgm = 0.; sigmagmZ = 0.;} } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ff2fftgmZ::sigmaHat() { // Couplings for current flavour combination. int id1Abs = abs(id1); double e1 = couplingsPtr->ef(id1Abs); double v1 = couplingsPtr->vf(id1Abs); double a1 = couplingsPtr->af(id1Abs); int id2Abs = abs(id2); double e2 = couplingsPtr->ef(id2Abs); double v2 = couplingsPtr->vf(id2Abs); double a2 = couplingsPtr->af(id2Abs); // Distinguish same-sign and opposite-sign fermions. double epsi = (id1 * id2 > 0) ? 1. : -1.; // Flavour-dependent cross section. double sigma = sigmagmgm * pow2(e1 * e2) + sigmagmZ * e1 * e2 * (v1 * v2 * (1. + uH2 / sH2) + a1 * a2 * epsi * (1. - uH2 / sH2)) + sigmaZZ * ((v1*v1 + a1*a1) * (v2*v2 + a2*a2) * (1. + uH2 / sH2) + 4. * v1 * a1 * v2 * a2 * epsi * (1. - uH2 / sH2)); // Spin-state extra factor 2 per incoming neutrino. if (id1Abs == 12 || id1Abs == 14 || id1Abs == 16) sigma *= 2.; if (id2Abs == 12 || id2Abs == 14 || id2Abs == 16) sigma *= 2.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ff2fftgmZ::setIdColAcol() { // Trivial flavours: out = in. setId( id1, id2, id1, id2); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9 && abs(id2) < 9 && id1*id2 > 0) setColAcol( 1, 0, 2, 0, 1, 0, 2, 0); else if (abs(id1) < 9 && abs(id2) < 9) setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); else if (abs(id1) < 9) setColAcol( 1, 0, 0, 0, 1, 0, 0, 0); else if (abs(id2) < 9) setColAcol( 0, 0, 1, 0, 0, 0, 1, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if ( (abs(id1) < 9 && id1 < 0) || (abs(id1) > 10 && id2 < 0) ) swapColAcol(); } //========================================================================== // Sigma2ff2fftW class. // Cross section for f_1 f_2 -> f_3 f_4 via t-channel W+- exchange // (f is quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma2ff2fftW::initProc() { // Store W+- mass for propagator. Common coupling factor. mW = particleDataPtr->m0(24); mWS = mW*mW; thetaWRat = 1. / (4. * couplingsPtr->sin2thetaW()); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ff2fftW::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * pow2(alpEM * thetaWRat) * 4. * sH2 / pow2(tH - mWS); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ff2fftW::sigmaHat() { // Some flavour combinations not possible. int id1Abs = abs(id1); int id2Abs = abs(id2); if ( (id1Abs%2 == id2Abs%2 && id1 * id2 > 0) || (id1Abs%2 != id2Abs%2 && id1 * id2 < 0) ) return 0.; // Basic cross section. double sigma = sigma0; if (id1 * id2 < 0) sigma *= uH2 / sH2; // CKM factors for final states. sigma *= couplingsPtr->V2CKMsum(id1Abs) * couplingsPtr->V2CKMsum(id2Abs); // Spin-state extra factor 2 per incoming neutrino. if (id1Abs == 12 || id1Abs == 14 || id1Abs == 16) sigma *= 2.; if (id2Abs == 12 || id2Abs == 14 || id2Abs == 16) sigma *= 2.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ff2fftW::setIdColAcol() { // Pick out-flavours by relative CKM weights. id3 = couplingsPtr->V2CKMpick(id1); id4 = couplingsPtr->V2CKMpick(id2); setId( id1, id2, id3, id4); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9 && abs(id2) < 9 && id1*id2 > 0) setColAcol( 1, 0, 2, 0, 1, 0, 2, 0); else if (abs(id1) < 9 && abs(id2) < 9) setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); else if (abs(id1) < 9) setColAcol( 1, 0, 0, 0, 1, 0, 0, 0); else if (abs(id2) < 9) setColAcol( 0, 0, 1, 0, 0, 0, 1, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if ( (abs(id1) < 9 && id1 < 0) || (abs(id1) > 10 && id2 < 0) ) swapColAcol(); } //========================================================================== // Sigma2qq2QqtW class. // Cross section for q q' -> Q q" via t-channel W+- exchange. // Related to Sigma2ff2ffViaW class, but with massive matrix elements. //-------------------------------------------------------------------------- // Initialize process. void Sigma2qq2QqtW::initProc() { // Process name. nameSave = "q q -> Q q (t-channel W+-)"; if (idNew == 4) nameSave = "q q -> c q (t-channel W+-)"; if (idNew == 5) nameSave = "q q -> b q (t-channel W+-)"; if (idNew == 6) nameSave = "q q -> t q (t-channel W+-)"; if (idNew == 7) nameSave = "q q -> b' q (t-channel W+-)"; if (idNew == 8) nameSave = "q q -> t' q (t-channel W+-)"; // Store W+- mass for propagator. Common coupling factor. mW = particleDataPtr->m0(24); mWS = mW*mW; thetaWRat = 1. / (4. * couplingsPtr->sin2thetaW()); // Secondary open width fractions, relevant for top (or heavier). openFracPos = particleDataPtr->resOpenFrac(idNew); openFracNeg = particleDataPtr->resOpenFrac(-idNew); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qq2QqtW::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * pow2(alpEM * thetaWRat) * 4. / pow2(tH - mWS); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qq2QqtW::sigmaHat() { // Some flavour combinations not possible. int id1Abs = abs(id1); int id2Abs = abs(id2); bool diff12 = (id1Abs%2 != id2Abs%2); if ( (!diff12 && id1 * id2 > 0) || ( diff12 && id1 * id2 < 0) ) return 0.; // Basic cross section. double sigma = sigma0; sigma *= (id1 * id2 > 0) ? sH * (sH - s3) : uH * (uH - s3); // Secondary width if t or tbar produced on either side. double openFrac1 = (id1 > 0) ? openFracPos : openFracNeg; double openFrac2 = (id2 > 0) ? openFracPos : openFracNeg; // CKM factors for final states; further impossible case. bool diff1N = (id1Abs%2 != idNew%2); bool diff2N = (id2Abs%2 != idNew%2); if (diff1N && diff2N) sigma *= ( couplingsPtr->V2CKMid(id1Abs, idNew) * openFrac1 * couplingsPtr->V2CKMsum(id2Abs) + couplingsPtr->V2CKMsum(id1Abs) * couplingsPtr->V2CKMid(id2Abs, idNew) * openFrac2 ); else if (diff1N) sigma *= couplingsPtr->V2CKMid(id1Abs, idNew) * openFrac1 * couplingsPtr->V2CKMsum(id2Abs); else if (diff2N) sigma *= couplingsPtr->V2CKMsum(id1Abs) * couplingsPtr->V2CKMid(id2Abs, idNew) * openFrac2; else sigma = 0.; // Spin-state extra factor 2 per incoming neutrino. if (id1Abs == 12 || id1Abs == 14 || id1Abs == 16) sigma *= 2.; if (id2Abs == 12 || id2Abs == 14 || id2Abs == 16) sigma *= 2.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qq2QqtW::setIdColAcol() { // For topologies like d dbar -> (t/c/u) (t/c/u)bar pick side. int id1Abs = abs(id1); int id2Abs = abs(id2); int side = 1; if ( (id1Abs + idNew)%2 == 1 && (id2Abs + idNew)%2 == 1 ) { double prob1 = couplingsPtr->V2CKMid(id1Abs, idNew) * couplingsPtr->V2CKMsum(id2Abs); prob1 *= (id1 > 0) ? openFracPos : openFracNeg; double prob2 = couplingsPtr->V2CKMid(id2Abs, idNew) * couplingsPtr->V2CKMsum(id1Abs); prob2 *= (id2 > 0) ? openFracPos : openFracNeg; if (prob2 > rndmPtr->flat() * (prob1 + prob2)) side = 2; } else if ((id2Abs + idNew)%2 == 1) side = 2; // Pick out-flavours by relative CKM weights. if (side == 1) { // q q' -> t q" : correct order from start. id3 = (id1 > 0) ? idNew : -idNew; id4 = couplingsPtr->V2CKMpick(id2); setId( id1, id2, id3, id4); } else { // q q' -> q" t : stored as t q" so swap tHat <-> uHat. swapTU = true; id3 = couplingsPtr->V2CKMpick(id1); id4 = (id2 > 0) ? idNew : -idNew; setId( id1, id2, id4, id3); } // Colour flow topologies. Swap when antiquarks on side 1. if (side == 1 && id1 * id2 > 0) setColAcol( 1, 0, 2, 0, 1, 0, 2, 0); else if (id1 * id2 > 0) setColAcol( 1, 0, 2, 0, 2, 0, 1, 0); else if (side == 1) setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); else setColAcol( 1, 0, 0, 2, 0, 2, 1, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles of W in top decay. double Sigma2qq2QqtW::weightDecay( Event& process, int iResBeg, int iResEnd) { // For top decay hand over to standard routine, else done. if (idNew == 6 && process[process[iResBeg].mother1()].idAbs() == 6) return weightTopDecay( process, iResBeg, iResEnd); else return 1.; } //========================================================================== // Sigma1ffbar2gmZ class. // Cross section for f fbar -> gamma*/Z0 (f is quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2gmZ::initProc() { // Allow to pick only gamma* or Z0 part of full gamma*/Z0 expression. gmZmode = settingsPtr->mode("WeakZ0:gmZmode"); // Store Z0 mass and width for propagator. mRes = particleDataPtr->m0(23); GammaRes = particleDataPtr->mWidth(23); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; thetaWRat = 1. / (16. * couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(23); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1ffbar2gmZ::sigmaKin() { // Common coupling factors. double colQ = 3. * (1. + alpS / M_PI); // Reset quantities to sum. Declare variables in loop. gamSum = 0.; intSum = 0.; resSum = 0.; int idAbs, onMode; double mf, mr, psvec, psaxi, betaf, ef2, efvf, vf2af2, colf; // Loop over all Z0 decay channels. for (int i = 0; i < particlePtr->sizeChannels(); ++i) { idAbs = abs( particlePtr->channel(i).product(0) ); // Only contributions from three fermion generations, except top. if ( (idAbs > 0 && idAbs < 6) || ( idAbs > 10 && idAbs < 17)) { mf = particleDataPtr->m0(idAbs); // Check that above threshold. Phase space. if (mH > 2. * mf + MASSMARGIN) { mr = pow2(mf / mH); betaf = sqrtpos(1. - 4. * mr); psvec = betaf * (1. + 2. * mr); psaxi = pow3(betaf); // Combine phase space with couplings. ef2 = couplingsPtr->ef2(idAbs) * psvec; efvf = couplingsPtr->efvf(idAbs) * psvec; vf2af2 = couplingsPtr->vf2(idAbs) * psvec + couplingsPtr->af2(idAbs) * psaxi; colf = (idAbs < 6) ? colQ : 1.; // Store sum of combinations. For outstate only open channels. onMode = particlePtr->channel(i).onMode(); if (onMode == 1 || onMode == 2) { gamSum += colf * ef2; intSum += colf * efvf; resSum += colf * vf2af2; } // End loop over fermions. } } } // Calculate prefactors for gamma/interference/Z0 cross section terms. gamProp = 4. * M_PI * pow2(alpEM) / (3. * sH); intProp = gamProp * 2. * thetaWRat * sH * (sH - m2Res) / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); resProp = gamProp * pow2(thetaWRat * sH) / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); // Optionally only keep gamma* or Z0 term. if (gmZmode == 1) {intProp = 0.; resProp = 0.;} if (gmZmode == 2) {gamProp = 0.; intProp = 0.;} } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma1ffbar2gmZ::sigmaHat() { // Combine gamma, interference and Z0 parts. int idAbs = abs(id1); double sigma = couplingsPtr->ef2(idAbs) * gamProp * gamSum + couplingsPtr->efvf(idAbs) * intProp * intSum + couplingsPtr->vf2af2(idAbs) * resProp * resSum; // Colour factor. Answer. if (idAbs < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2gmZ::setIdColAcol() { // Flavours trivial. setId( id1, id2, 23); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for gamma*/Z0 decay angle. double Sigma1ffbar2gmZ::weightDecay( Event& process, int iResBeg, int iResEnd) { // Z should sit in entry 5. if (iResBeg != 5 || iResEnd != 5) return 1.; // Couplings for in- and out-flavours. int idInAbs = process[3].idAbs(); double ei = couplingsPtr->ef(idInAbs); double vi = couplingsPtr->vf(idInAbs); double ai = couplingsPtr->af(idInAbs); int idOutAbs = process[6].idAbs(); double ef = couplingsPtr->ef(idOutAbs); double vf = couplingsPtr->vf(idOutAbs); double af = couplingsPtr->af(idOutAbs); // Phase space factors. (One power of beta left out in formulae.) double mf = process[6].m(); double mr = mf*mf / sH; double betaf = sqrtpos(1. - 4. * mr); // Coefficients of angular expression. double coefTran = ei*ei * gamProp * ef*ef + ei * vi * intProp * ef * vf + (vi*vi + ai*ai) * resProp * (vf*vf + pow2(betaf) * af*af); double coefLong = 4. * mr * ( ei*ei * gamProp * ef*ef + ei * vi * intProp * ef * vf + (vi*vi + ai*ai) * resProp * vf*vf ); double coefAsym = betaf * ( ei * ai * intProp * ef * af + 4. * vi * ai * resProp * vf * af ); // Flip asymmetry for in-fermion + out-antifermion. if (process[3].id() * process[6].id() < 0) coefAsym = -coefAsym; // Reconstruct decay angle and weight for it. double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * betaf); double wtMax = 2. * (coefTran + abs(coefAsym)); double wt = coefTran * (1. + pow2(cosThe)) + coefLong * (1. - pow2(cosThe)) + 2. * coefAsym * cosThe; // Done. return (wt / wtMax); } //========================================================================== // Sigma1ffbar2W class. // Cross section for f fbar' -> W+- (f is quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2W::initProc() { // Store W+- mass and width for propagator. mRes = particleDataPtr->m0(24); GammaRes = particleDataPtr->mWidth(24); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; thetaWRat = 1. / (12. * couplingsPtr->sin2thetaW()); // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(24); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1ffbar2W::sigmaKin() { // Set up Breit-Wigner. Cross section for W+ and W- separately. double sigBW = 12. * M_PI / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); double preFac = alpEM * thetaWRat * mH; sigma0Pos = preFac * sigBW * particlePtr->resWidthOpen(24, mH); sigma0Neg = preFac * sigBW * particlePtr->resWidthOpen(-24, mH); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma1ffbar2W::sigmaHat() { // Secondary width for W+ or W-. CKM and colour factors. int idUp = (abs(id1)%2 == 0) ? id1 : id2; double sigma = (idUp > 0) ? sigma0Pos : sigma0Neg; if (abs(id1) < 9) sigma *= couplingsPtr->V2CKMid(abs(id1), abs(id2)) / 3.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2W::setIdColAcol() { // Sign of outgoing W. int sign = 1 - 2 * (abs(id1)%2); if (id1 < 0) sign = -sign; setId( id1, id2, 24 * sign); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for W decay angle. double Sigma1ffbar2W::weightDecay( Event& process, int iResBeg, int iResEnd) { // W should sit in entry 5. if (iResBeg != 5 || iResEnd != 5) return 1.; // Phase space factors. double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double betaf = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); // Sign of asymmetry. double eps = (process[3].id() * process[6].id() > 0) ? 1. : -1.; // Reconstruct decay angle and weight for it. double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * betaf); double wtMax = 4.; double wt = pow2(1. + betaf * eps * cosThe) - pow2(mr1 - mr2); // Done. return (wt / wtMax); } //========================================================================== // Sigma2ffbar2ffbarsgm class. // Cross section f fbar -> gamma* -> f' fbar', for multiparton interactions. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2ffbarsgm::sigmaKin() { // Pick new flavour. Allow three leptons and five quarks. double colQ = 1. + (alpS / M_PI); double flavWt = 3. + colQ * 11. / 3.; double flavRndm = rndmPtr->flat() * flavWt; if (flavRndm < 3.) { if (flavRndm < 1.) idNew = 11; else if (flavRndm < 2.) idNew = 13; else idNew = 15; } else { flavRndm = 3. * (flavRndm - 3.) / colQ; if (flavRndm < 4.) idNew = 2; else if (flavRndm < 8.) idNew = 4; else if (flavRndm < 9.) idNew = 1; else if (flavRndm < 10.) idNew = 3; else idNew = 5; } double mNew = particleDataPtr->m0(idNew); double m2New = mNew*mNew; // Calculate kinematics dependence. Give correct mass factors for // tHat, uHat defined as if massless kinematics, d(sigma)/d(Omega) // = beta (1 + cos^2(theta) + (1 - beta^2) sin^2(theta)). // Special case related to phase space form in multiparton interactions. double sigS = 0.; if (sH > 4. * m2New) { double beta = sqrt(1. - 4. * m2New / sH); sigS = beta * (2.* (tH2 + uH2) + 4. * (1. - beta * beta) * tH * uH) / sH2; } // Answer is proportional to number of outgoing flavours. sigma0 = (M_PI/sH2) * pow2(alpEM) * sigS * flavWt; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2ffbarsgm::sigmaHat() { // Charge and colour factors. double eNow = couplingsPtr->ef( abs(id1) ); double sigma = sigma0 * pow2(eNow); if (abs(id1) < 9) sigma /= 3.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2ffbarsgm::setIdColAcol() { // Set outgoing flavours. id3 = (id1 > 0) ? idNew : -idNew; setId( id1, id2, id3, -id3); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9 && idNew < 9) setColAcol( 1, 0, 0, 1, 2, 0, 0, 2); else if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else if (idNew < 9) setColAcol( 0, 0, 0, 0, 1, 0, 0, 1); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2ffbar2FFbarsgmZ class. // Cross section f fbar -> gamma*/Z0 -> F Fbar. //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2FFbarsgmZ::initProc() { // Process name. nameSave = "f fbar -> F Fbar (s-channel gamma*/Z0)"; if (idNew == 4) nameSave = "f fbar -> c cbar (s-channel gamma*/Z0)"; if (idNew == 5) nameSave = "f fbar -> b bbar (s-channel gamma*/Z0)"; if (idNew == 6) nameSave = "f fbar -> t tbar (s-channel gamma*/Z0)"; if (idNew == 7) nameSave = "f fbar -> b' b'bar (s-channel gamma*/Z0)"; if (idNew == 8) nameSave = "f fbar -> t' t'bar (s-channel gamma*/Z0)"; if (idNew == 15) nameSave = "f fbar -> tau+ tau- (s-channel gamma*/Z0)"; if (idNew == 17) nameSave = "f fbar -> tau'+ tau'- (s-channel gamma*/Z0)"; if (idNew == 18) nameSave = "f fbar -> nu'_tau nu'bar_tau (s-channel gamma*/Z0)"; // Allow to pick only gamma* or Z0 part of full gamma*/Z0 expression. gmZmode = settingsPtr->mode("WeakZ0:gmZmode"); // Store Z0 mass and width for propagator. mRes = particleDataPtr->m0(23); GammaRes = particleDataPtr->mWidth(23); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; thetaWRat = 1. / (16. * couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); // Store couplings of F. ef = couplingsPtr->ef(idNew); vf = couplingsPtr->vf(idNew); af = couplingsPtr->af(idNew); // Secondary open width fraction, relevant for top (or heavier). openFracPair = particleDataPtr->resOpenFrac(idNew, -idNew); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2FFbarsgmZ::sigmaKin() { // Check that above threshold. isPhysical = true; if (mH < m3 + m4 + MASSMARGIN) { isPhysical = false; return; } // Define average F, Fbar mass so same beta. Phase space. double s34Avg = 0.5 * (s3 + s4) - 0.25 * pow2(s3 - s4) / sH; mr = s34Avg / sH; betaf = sqrtpos(1. - 4. * mr); // Final-state colour factor. double colF = (idNew < 9) ? 3. * (1. + alpS / M_PI) : 1.; // Reconstruct decay angle so can reuse 2 -> 1 cross section. cosThe = (tH - uH) / (betaf * sH); // Calculate prefactors for gamma/interference/Z0 cross section terms. gamProp = colF * M_PI * pow2(alpEM) / sH2; intProp = gamProp * 2. * thetaWRat * sH * (sH - m2Res) / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); resProp = gamProp * pow2(thetaWRat * sH) / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); // Optionally only keep gamma* or Z0 term. if (gmZmode == 1) {intProp = 0.; resProp = 0.;} if (gmZmode == 2) {gamProp = 0.; intProp = 0.;} } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2FFbarsgmZ::sigmaHat() { // Fail if below threshold. if (!isPhysical) return 0.; // Couplings for in-flavours. int idAbs = abs(id1); double ei = couplingsPtr->ef(idAbs); double vi = couplingsPtr->vf(idAbs); double ai = couplingsPtr->af(idAbs); // Coefficients of angular expression. double coefTran = ei*ei * gamProp * ef*ef + ei * vi * intProp * ef * vf + (vi*vi + ai*ai) * resProp * (vf*vf + pow2(betaf) * af*af); double coefLong = 4. * mr * ( ei*ei * gamProp * ef*ef + ei * vi * intProp * ef * vf + (vi*vi + ai*ai) * resProp * vf*vf ); double coefAsym = betaf * ( ei * ai * intProp * ef * af + 4. * vi * ai * resProp * vf * af ); // Combine gamma, interference and Z0 parts. double sigma = coefTran * (1. + pow2(cosThe)) + coefLong * (1. - pow2(cosThe)) + 2. * coefAsym * cosThe; // Top: corrections for closed decay channels. sigma *= openFracPair; // Initial-state colour factor. Answer. if (idAbs < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2FFbarsgmZ::setIdColAcol() { // Set outgoing flavours. id3 = (id1 > 0) ? idNew : -idNew; setId( id1, id2, id3, -id3); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9 && idNew < 9) setColAcol( 1, 0, 0, 1, 2, 0, 0, 2); else if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else if (idNew < 9) setColAcol( 0, 0, 0, 0, 1, 0, 0, 1); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles of W in top decay. double Sigma2ffbar2FFbarsgmZ::weightDecay( Event& process, int iResBeg, int iResEnd) { // For top decay hand over to standard routine, else done. if (idNew == 6 && process[process[iResBeg].mother1()].idAbs() == 6) return weightTopDecay( process, iResBeg, iResEnd); else return 1.; } //========================================================================== // Sigma2ffbar2FfbarsW class. // Cross section f fbar' -> W+- -> F fbar". //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2FfbarsW::initProc() { // Process name. nameSave = "f fbar -> F fbar (s-channel W+-)"; if (idNew == 4) nameSave = "f fbar -> c qbar (s-channel W+-)"; if (idNew == 5) nameSave = "f fbar -> b qbar (s-channel W+-)"; if (idNew == 6) nameSave = "f fbar -> t qbar (s-channel W+-)"; if (idNew == 7) nameSave = "f fbar -> b' qbar (s-channel W+-)"; if (idNew == 8) nameSave = "f fbar -> t' qbar (s-channel W+-)"; if (idNew == 7 && idNew2 == 6) nameSave = "f fbar -> b' tbar (s-channel W+-)"; if (idNew == 8 && idNew2 == 7) nameSave = "f fbar -> t' b'bar (s-channel W+-)"; if (idNew == 15 || idNew == 16) nameSave = "f fbar -> tau nu_taubar (s-channel W+-)"; if (idNew == 17 || idNew == 18) nameSave = "f fbar -> tau' nu'_taubar (s-channel W+-)"; // Store W+- mass and width for propagator. mRes = particleDataPtr->m0(24); GammaRes = particleDataPtr->mWidth(24); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; thetaWRat = 1. / (12. * couplingsPtr->sin2thetaW()); // For t/t' want to use at least b mass. idPartner = idNew2; if ( (idNew == 6 || idNew == 8) && idNew2 == 0 ) idPartner = 5; // Sum of CKM weights for quarks. V2New = (idNew < 9) ? couplingsPtr->V2CKMsum(idNew) : 1.; if (idNew2 != 0) V2New = couplingsPtr->V2CKMid(idNew, idNew2); // Secondary open width fractions, relevant for top or heavier. openFracPos = particleDataPtr->resOpenFrac( idNew, -idNew2); openFracNeg = particleDataPtr->resOpenFrac(-idNew, idNew2); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2FfbarsW::sigmaKin() { // Check that above threshold. isPhysical = true; if (mH < m3 + m4 + MASSMARGIN) { isPhysical = false; return; } // Phase space factors. double mr1 = s3 / sH; double mr2 = s4 / sH; double betaf = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); // Reconstruct decay angle so can reuse 2 -> 1 cross section. double cosThe = (tH - uH) / (betaf * sH); // Set up Breit-Wigner and in- and out-widths. double sigBW = 9. * M_PI * pow2(alpEM * thetaWRat) / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); // Initial-state colour factor. double colF = (idNew < 9) ? 3. * (1. + alpS / M_PI) * V2New : 1.; // Angular dependence. double wt = pow2(1. + betaf * cosThe) - pow2(mr1 - mr2); // Temporary answer. sigma0 = sigBW * colF * wt; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2FfbarsW::sigmaHat() { // Fail if below threshold. if (!isPhysical) return 0.; // CKM and colour factors. double sigma = sigma0; if (abs(id1) < 9) sigma *= couplingsPtr->V2CKMid(abs(id1), abs(id2)) / 3.; // Correction for secondary width in top (or heavier) decay. int idSame = ((abs(id1) + idNew)%2 == 0) ? id1 : id2; sigma *= (idSame > 0) ? openFracPos : openFracNeg; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2FfbarsW::setIdColAcol() { // Set outgoing flavours. id3 = idNew; id4 = (idNew2 != 0) ? idNew2 : couplingsPtr->V2CKMpick(idNew); if (idNew%2 == 0) { int idInUp = (abs(id1)%2 == 0) ? id1 : id2; if (idInUp > 0) id4 = -id4; else id3 = -id3; } else { int idInDn = (abs(id1)%2 == 1) ? id1 : id2; if (idInDn > 0) id4 = -id4; else id3 = -id3; } setId( id1, id2, id3, id4); // Swap tHat and uHat for fbar' f -> F f". if (id1 * id3 < 0) swapTU = true; // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9 && idNew < 9) setColAcol( 1, 0, 0, 1, 2, 0, 0, 2); else if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else if (idNew < 9) setColAcol( 0, 0, 0, 0, 1, 0, 0, 1); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapCol12(); if (id3 < 0) swapCol34(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles of W in top decay. double Sigma2ffbar2FfbarsW::weightDecay( Event& process, int iResBeg, int iResEnd) { // For top decay hand over to standard routine, else done. if (idNew == 6 && process[process[iResBeg].mother1()].idAbs() == 6) return weightTopDecay( process, iResBeg, iResEnd); else return 1.; } //========================================================================== // Sigma2ffbargmZWgmZW class. // Collects common methods for f fbar -> gamma*/Z0/W+- gamma*/Z0/W-+. //-------------------------------------------------------------------------- // Calculate and store internal products. void Sigma2ffbargmZWgmZW::setupProd( Event& process, int i1, int i2, int i3, int i4, int i5, int i6) { // Store incoming and outgoing momenta, pRot[1] = process[i1].p(); pRot[2] = process[i2].p(); pRot[3] = process[i3].p(); pRot[4] = process[i4].p(); pRot[5] = process[i5].p(); pRot[6] = process[i6].p(); // Do random rotation to avoid accidental zeroes in HA expressions. bool smallPT = false; do { smallPT = false; double thetaNow = acos(2. * rndmPtr->flat() - 1.); double phiNow = 2. * M_PI * rndmPtr->flat(); for (int i = 1; i <= 6; ++i) { pRot[i].rot( thetaNow, phiNow); if (pRot[i].pT2() < 1e-4 * pRot[i].pAbs2()) smallPT = true; } } while (smallPT); // Calculate internal products. for (int i = 1; i < 6; ++i) { for (int j = i + 1; j <= 6; ++j) { hA[i][j] = sqrt( (pRot[i].e() - pRot[i].pz()) * (pRot[j].e() + pRot[j].pz()) / pRot[i].pT2() ) * complex( pRot[i].px(), pRot[i].py() ) - sqrt( (pRot[i].e() + pRot[i].pz()) * (pRot[j].e() - pRot[j].pz()) / pRot[j].pT2() ) * complex( pRot[j].px(), pRot[j].py() ); hC[i][j] = conj( hA[i][j] ); if (i <= 2) { hA[i][j] *= complex( 0., 1.); hC[i][j] *= complex( 0., 1.); } hA[j][i] = - hA[i][j]; hC[j][i] = - hC[i][j]; } } } //-------------------------------------------------------------------------- // Evaluate the F function of Gunion and Kunszt. complex Sigma2ffbargmZWgmZW::fGK(int j1, int j2, int j3, int j4, int j5, int j6) { return 4. * hA[j1][j3] * hC[j2][j6] * ( hA[j1][j5] * hC[j1][j4] + hA[j3][j5] * hC[j3][j4] ); } //-------------------------------------------------------------------------- // Evaluate the Xi function of Gunion and Kunszt. double Sigma2ffbargmZWgmZW::xiGK( double tHnow, double uHnow) { return - 4. * s3 * s4 + tHnow * (3. * tHnow + 4. * uHnow) + tHnow * tHnow * ( tHnow * uHnow / (s3 * s4) - 2. * (1. / s3 + 1./s4) * (tHnow + uHnow) + 2. * (s3 / s4 + s4 / s3) ); } //-------------------------------------------------------------------------- // Evaluate the Xj function of Gunion and Kunszt. double Sigma2ffbargmZWgmZW::xjGK( double tHnow, double uHnow) { return 8. * pow2(s3 + s4) - 8. * (s3 + s4) * (tHnow + uHnow) - 6. * tHnow * uHnow - 2. * tHnow * uHnow * ( tHnow * uHnow / (s3 * s4) - 2. * (1. / s3 + 1. / s4) * (tHnow + uHnow) + 2. * (s3 / s4 + s4 / s3) ); } //========================================================================== // Sigma2ffbar2gmZgmZ class. // Cross section for f fbar -> gamma*/Z0 gamma*/Z0 (f is quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2gmZgmZ::initProc() { // Allow to pick only gamma* or Z0 part of full gamma*/Z0 expression. gmZmode = settingsPtr->mode("WeakZ0:gmZmode"); // Store Z0 mass and width for propagator. mRes = particleDataPtr->m0(23); GammaRes = particleDataPtr->mWidth(23); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; thetaWRat = 1. / (16. * couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(23); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2gmZgmZ::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * pow2(alpEM) * 0.5 * ( (tH2 + uH2 + 2. * (s3 + s4) * sH) / (tH * uH) - s3 * s4 * (1./tH2 + 1./uH2) ); // Common coupling factors at the resonance masses double alpEM3 = couplingsPtr->alphaEM(s3); double alpS3 = couplingsPtr->alphaS(s3); double colQ3 = 3. * (1. + alpS3 / M_PI); double alpEM4 = couplingsPtr->alphaEM(s4); double alpS4 = couplingsPtr->alphaS(s4); double colQ4 = 3. * (1. + alpS4 / M_PI); // Reset quantities to sum. Declare variables in loop. gamSum3 = 0.; intSum3 = 0.; resSum3 = 0.; gamSum4 = 0.; intSum4 = 0.; resSum4 = 0.; int onMode; double mf, mr, psvec, psaxi, betaf, ef2, efvf, vf2af2, colf; // Loop over all Z0 decay channels. for (int i = 0; i < particlePtr->sizeChannels(); ++i) { int idAbs = abs( particlePtr->channel(i).product(0) ); // Only contributions from three fermion generations, except top. if ( (idAbs > 0 && idAbs < 6) || ( idAbs > 10 && idAbs < 17)) { mf = particleDataPtr->m0(idAbs); onMode = particlePtr->channel(i).onMode(); // First Z0: check that above threshold. Phase space. if (m3 > 2. * mf + MASSMARGIN) { mr = pow2(mf / m3); betaf = sqrtpos(1. - 4. * mr); psvec = betaf * (1. + 2. * mr); psaxi = pow3(betaf); // First Z0: combine phase space with couplings. ef2 = couplingsPtr->ef2(idAbs) * psvec; efvf = couplingsPtr->efvf(idAbs) * psvec; vf2af2 = couplingsPtr->vf2(idAbs) * psvec + couplingsPtr->af2(idAbs) * psaxi; colf = (idAbs < 6) ? colQ3 : 1.; // First Z0: store sum of combinations for open outstate channels. if (onMode == 1 || onMode == 2) { gamSum3 += colf * ef2; intSum3 += colf * efvf; resSum3 += colf * vf2af2; } } // Second Z0: check that above threshold. Phase space. if (m4 > 2. * mf + MASSMARGIN) { mr = pow2(mf / m4); betaf = sqrtpos(1. - 4. * mr); psvec = betaf * (1. + 2. * mr); psaxi = pow3(betaf); // Second Z0: combine phase space with couplings. ef2 = couplingsPtr->ef2(idAbs) * psvec; efvf = couplingsPtr->efvf(idAbs) * psvec; vf2af2 = couplingsPtr->vf2(idAbs) * psvec + couplingsPtr->af2(idAbs) * psaxi; colf = (idAbs < 6) ? colQ4 : 1.; // Second Z0: store sum of combinations for open outstate channels. if (onMode == 1 || onMode == 2) { gamSum4 += colf * ef2; intSum4 += colf * efvf; resSum4 += colf * vf2af2; } } // End loop over fermions. } } // First Z0: calculate prefactors for gamma/interference/Z0 terms. gamProp3 = 4. * alpEM3 / (3. * M_PI * s3); intProp3 = gamProp3 * 2. * thetaWRat * s3 * (s3 - m2Res) / ( pow2(s3 - m2Res) + pow2(s3 * GamMRat) ); resProp3 = gamProp3 * pow2(thetaWRat * s3) / ( pow2(s3 - m2Res) + pow2(s3 * GamMRat) ); // First Z0: optionally only keep gamma* or Z0 term. if (gmZmode == 1) {intProp3 = 0.; resProp3 = 0.;} if (gmZmode == 2) {gamProp3 = 0.; intProp3 = 0.;} // Second Z0: calculate prefactors for gamma/interference/Z0 terms. gamProp4 = 4. * alpEM4 / (3. * M_PI * s4); intProp4 = gamProp4 * 2. * thetaWRat * s4 * (s4 - m2Res) / ( pow2(s4 - m2Res) + pow2(s4 * GamMRat) ); resProp4 = gamProp4 * pow2(thetaWRat * s4) / ( pow2(s4 - m2Res) + pow2(s4 * GamMRat) ); // Second Z0: optionally only keep gamma* or Z0 term. if (gmZmode == 1) {intProp4 = 0.; resProp4 = 0.;} if (gmZmode == 2) {gamProp4 = 0.; intProp4 = 0.;} } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2gmZgmZ::sigmaHat() { // Charge/2, left- and righthanded couplings for in-fermion. int idAbs = abs(id1); double ei = 0.5 * couplingsPtr->ef(idAbs); double li = couplingsPtr->lf(idAbs); double ri = couplingsPtr->rf(idAbs); // Combine left/right gamma, interference and Z0 parts for each Z0. double left3 = ei * ei * gamProp3 * gamSum3 + ei * li * intProp3 * intSum3 + li * li * resProp3 * resSum3; double right3 = ei * ei * gamProp3 * gamSum3 + ei * ri * intProp3 * intSum3 + ri * ri * resProp3 * resSum3; double left4 = ei * ei * gamProp4 * gamSum4 + ei * li * intProp4 * intSum4 + li * li * resProp4 * resSum4; double right4 = ei * ei * gamProp4 * gamSum4 + ei * ri * intProp4 * intSum4 + ri * ri * resProp4 * resSum4; // Combine left- and right-handed couplings for the two Z0's. double sigma = sigma0 * (left3 * left4 + right3 * right4); // Correct for the running-width Z0 propagators weight in PhaseSpace. sigma /= (runBW3 * runBW4); // Initial-state colour factor. Answer. if (idAbs < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2gmZgmZ::setIdColAcol() { // Flavours trivial. setId( id1, id2, 23, 23); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate correlated decay flavours of the two gamma*/Z0. // Unique complication, caused by gamma*/Z0 mix different left/right. double Sigma2ffbar2gmZgmZ::weightDecayFlav( Event& process) { // Order so that fbar(1) f(2) -> f'(3) fbar'(4) f"(5) fbar"(6). i1 = (process[3].id() < 0) ? 3 : 4; i2 = 7 - i1; i3 = (process[7].id() > 0) ? 7 : 8; i4 = 15 - i3; i5 = (process[9].id() > 0) ? 9 : 10; i6 = 19 - i5; // Charge/2, left- and righthanded couplings for in- and out-fermions. int idAbs = process[i1].idAbs(); double ei = 0.5 * couplingsPtr->ef(idAbs); double li = couplingsPtr->lf(idAbs); double ri = couplingsPtr->rf(idAbs); idAbs = process[i3].idAbs(); double e3 = 0.5 * couplingsPtr->ef(idAbs); double l3 = couplingsPtr->lf(idAbs); double r3 = couplingsPtr->rf(idAbs); idAbs = process[i5].idAbs(); double e4 = 0.5 * couplingsPtr->ef(idAbs); double l4 = couplingsPtr->lf(idAbs); double r4 = couplingsPtr->rf(idAbs); // Left- and righthanded couplings combined with propagators. c3LL = ei * ei * gamProp3 * e3 * e3 + ei * li * intProp3 * e3 * l3 + li * li * resProp3 * l3 * l3; c3LR = ei * ei * gamProp3 * e3 * e3 + ei * li * intProp3 * e3 * r3 + li * li * resProp3 * r3 * r3; c3RL = ei * ei * gamProp3 * e3 * e3 + ei * ri * intProp3 * e3 * l3 + ri * ri * resProp3 * l3 * l3; c3RR = ei * ei * gamProp3 * e3 * e3 + ei * ri * intProp3 * e3 * r3 + ri * ri * resProp3 * r3 * r3; c4LL = ei * ei * gamProp4 * e4 * e4 + ei * li * intProp4 * e4 * l4 + li * li * resProp4 * l4 * l4; c4LR = ei * ei * gamProp4 * e4 * e4 + ei * li * intProp4 * e4 * r4 + li * li * resProp4 * r4 * r4; c4RL = ei * ei * gamProp4 * e4 * e4 + ei * ri * intProp4 * e4 * l4 + ri * ri * resProp4 * l4 * l4; c4RR = ei * ei * gamProp4 * e4 * e4 + ei * ri * intProp4 * e4 * r4 + ri * ri * resProp4 * r4 * r4; // Flavour weight and maximum. flavWt = (c3LL + c3LR) * (c4LL + c4LR) + (c3RL + c3RR) * (c4RL + c4RR); double flavWtMax = (c3LL + c3LR + c3RL + c3RR) * (c4LL + c4LR + c4RL + c4RR); // Done. return flavWt / flavWtMax; } //-------------------------------------------------------------------------- // Evaluate weight for decay angles of the two gamma*/Z0. double Sigma2ffbar2gmZgmZ::weightDecay( Event& process, int iResBeg, int iResEnd) { // Two resonance decays, but with common weight. if (iResBeg != 5 || iResEnd != 6) return 1.; // Set up four-products and internal products. setupProd( process, i1, i2, i3, i4, i5, i6); // Flip tHat and uHat if first incoming is fermion. double tHres = tH; double uHres = uH; if (process[3].id() > 0) swap( tHres, uHres); // Kinematics factors (norm(x) = |x|^2). double fGK135 = norm( fGK( 1, 2, 3, 4, 5, 6) / tHres + fGK( 1, 2, 5, 6, 3, 4) / uHres ); double fGK145 = norm( fGK( 1, 2, 4, 3, 5, 6) / tHres + fGK( 1, 2, 5, 6, 4, 3) / uHres ); double fGK136 = norm( fGK( 1, 2, 3, 4, 6, 5) / tHres + fGK( 1, 2, 6, 5, 3, 4) / uHres ); double fGK146 = norm( fGK( 1, 2, 4, 3, 6, 5) / tHres + fGK( 1, 2, 6, 5, 4, 3) / uHres ); double fGK253 = norm( fGK( 2, 1, 5, 6, 3, 4) / tHres + fGK( 2, 1, 3, 4, 5, 6) / uHres ); double fGK263 = norm( fGK( 2, 1, 6, 5, 3, 4) / tHres + fGK( 2, 1, 3, 4, 6, 5) / uHres ); double fGK254 = norm( fGK( 2, 1, 5, 6, 4, 3) / tHres + fGK( 2, 1, 4, 3, 5, 6) / uHres ); double fGK264 = norm( fGK( 2, 1, 6, 5, 4, 3) / tHres + fGK( 2, 1, 4, 3, 6, 5) / uHres ); // Weight and maximum. double wt = c3LL * c4LL * fGK135 + c3LR * c4LL * fGK145 + c3LL * c4LR * fGK136 + c3LR * c4LR * fGK146 + c3RL * c4RL * fGK253 + c3RR * c4RL * fGK263 + c3RL * c4RR * fGK254 + c3RR * c4RR * fGK264; double wtMax = 16. * s3 * s4 * flavWt * ( (tHres*tHres + uHres*uHres + 2. * sH * (s3 + s4)) / (tHres * uHres) - s3 * s4 * (1. / (tHres*tHres) + 1. / (uHres*uHres)) ); // Done. return wt / wtMax; } //========================================================================== // Sigma2ffbar2ZW class. // Cross section for f fbar' -> Z0 W+- (f is quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2ZW::initProc() { // Store W+- mass and width for propagator. mW = particleDataPtr->m0(24); widW = particleDataPtr->mWidth(24); mWS = mW*mW; mwWS = pow2(mW * widW); // Left-handed couplings for up/nu- and down/e-type quarks. lun = (hasLeptonBeams) ? couplingsPtr->lf(12) : couplingsPtr->lf(2); lde = (hasLeptonBeams) ? couplingsPtr->lf(11) : couplingsPtr->lf(1); // Common weak coupling factor. sin2thetaW = couplingsPtr->sin2thetaW(); cos2thetaW = couplingsPtr->cos2thetaW(); thetaWRat = 1. / (4. * cos2thetaW); cotT = sqrt(cos2thetaW / sin2thetaW); thetaWpt = (9. - 8. * sin2thetaW) / 4.; thetaWmm = (8. * sin2thetaW - 6.) / 4.; // Secondary open width fractions. openFracPos = particleDataPtr->resOpenFrac(23, 24); openFracNeg = particleDataPtr->resOpenFrac(23, -24); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2ffbar2ZW::sigmaKin() { // Evaluate cross section, as programmed by Merlin Kole (after tidying), // based on Brown, Sahdev, Mikaelian, Phys Rev. D20 (1979) 1069. /* double resBW = 1. / (pow2(sH - mWS) + mwWS); double prefac = 12.0 * M_PI * pow2(alpEM) / (sH2 * 8. * sin2thetaW); double temp1 = tH * uH - s3 * s4; double temp2 = temp1 / (s3 * s4); double temp3 = (s3 + s4) / sH; double temp4 = s3 * s4 / sH; double partA = temp2 * (0.25 - 0.5 * temp3 + (pow2(s3 + s4) + 8. * s3 * s4)/(4. * sH2) ) + (s3 + s4)/(s3 * s4) * (sH/2. - s3 - s4 + pow2(s3 - s4)/(2. * sH)); double partB1 = lun * (0.25 * temp2 * (1. - temp3 - 4. * temp4 / tH) + ((s3 + s4)/(2. * s3 * s4)) * (sH - s3 - s4 + 2. * s3 * s4 / tH) ); double partB2 = lde * ( 0.25 * temp2 * (1.- temp3 - 4. * temp4 / uH) + ((s3 + s4)/(2. * s3 * s4)) * (sH - s3 - s4 + 2. * s3 * s4 / uH) ); double partE = 0.25 * temp2 + 0.5 *(s3 + s4) / temp4; sigma0 = prefac * (pow2(cotT) * sH2 * resBW * partA + 2.* sH * cotT * resBW * (sH - mWS) * (partB2 - partB1) + pow2(lun - lde) * partE + pow2(lde) * temp1/uH2 + pow2(lun) * temp1/tH2 + 2. * lun * lde * sH * (s3 + s4) / (uH * tH)); */ // Evaluate cross section. Expression from EHLQ, with bug fix, // but can still give negative cross section so suspect. double resBW = 1. / (pow2(sH - mWS) + mwWS); sigma0 = (M_PI / sH2) * 0.5 * pow2(alpEM / sin2thetaW); sigma0 *= sH * resBW * (thetaWpt * pT2 + thetaWmm * (s3 + s4)) + (sH - mWS) * resBW * sH * (pT2 - s3 - s4) * (lun / tH - lde / uH) + thetaWRat * sH * pT2 * ( lun*lun / tH2 + lde*lde / uH2 ) + 2. * thetaWRat * sH * (s3 + s4) * lun * lde / (tH * uH); // Need to protect against negative cross sections at times. sigma0 = max(0., sigma0); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2ZW::sigmaHat() { // CKM and colour factors. double sigma = sigma0; if (abs(id1) < 9) sigma *= couplingsPtr->V2CKMid(abs(id1), abs(id2)) / 3.; // Corrections for secondary widths in Z0 and W+- decays. int idUp = (abs(id1)%2 == 0) ? id1 : id2; sigma *= (idUp > 0) ? openFracPos : openFracNeg; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2ZW::setIdColAcol() { // Sign of outgoing W. int sign = 1 - 2 * (abs(id1)%2); if (id1 < 0) sign = -sign; setId( id1, id2, 23, 24 * sign); // tHat is defined between (f, W-) or (fbar, W+), // so OK for u/ubar on side 1, but must swap tHat <-> uHat if d/dbar. if (abs(id1)%2 == 1) swapTU = true; // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for Z0 and W+- decay angles. double Sigma2ffbar2ZW::weightDecay( Event& process, int iResBeg, int iResEnd) { // Two resonance decays, but with common weight. if (iResBeg != 5 || iResEnd != 6) return 1.; // Order so that fbar(1) f(2) -> f'(3) fbar'(4) f"(5) fbar"(6) // with f' fbar' from W+- and f" fbar" from Z0 (note flip Z0 <-> W+-). int i1 = (process[3].id() < 0) ? 3 : 4; int i2 = 7 - i1; int i3 = (process[9].id() > 0) ? 9 : 10; int i4 = 19 - i3; int i5 = (process[7].id() > 0) ? 7 : 8; int i6 = 15 - i5; // Set up four-products and internal products. setupProd( process, i1, i2, i3, i4, i5, i6); // Swap tHat and uHat if incoming fermion is downtype. double tHres = tH; double uHres = uH; if (process[i2].id()%2 == 1) swap( tHres, uHres); // Couplings of incoming (anti)fermions and outgoing from Z0. int idAbs = process[i1].idAbs(); double ai = couplingsPtr->af(idAbs); double li1 = couplingsPtr->lf(idAbs); idAbs = process[i2].idAbs(); double li2 = couplingsPtr->lf(idAbs); idAbs = process[i5].idAbs(); double l4 = couplingsPtr->lf(idAbs); double r4 = couplingsPtr->rf(idAbs); // W propagator/interference factor. double Wint = cos2thetaW * (sH - mWS) / (pow2(sH - mWS) + mwWS); // Combinations of couplings and kinematics (norm(x) = |x|^2). double aWZ = li2 / tHres - 2. * Wint * ai; double bWZ = li1 / uHres + 2. * Wint * ai; double fGK135 = norm( aWZ * fGK( 1, 2, 3, 4, 5, 6) + bWZ * fGK( 1, 2, 5, 6, 3, 4) ); double fGK136 = norm( aWZ * fGK( 1, 2, 3, 4, 6, 5) + bWZ * fGK( 1, 2, 6, 5, 3, 4) ); double xiT = xiGK( tHres, uHres); double xiU = xiGK( uHres, tHres); double xjTU = xjGK( tHres, uHres); // Weight and maximum weight. double wt = l4*l4 * fGK135 + r4*r4 * fGK136; double wtMax = 4. * s3 * s4 * (l4*l4 + r4*r4) * (aWZ * aWZ * xiT + bWZ * bWZ * xiU + aWZ * bWZ * xjTU); // Done. return wt / wtMax; } //========================================================================== // Sigma2ffbar2WW class. // Cross section for f fbar -> W- W+ (f is quark or lepton). //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2WW::initProc() { // Store Z0 mass and width for propagator. Common coupling factor. mZ = particleDataPtr->m0(23); widZ = particleDataPtr->mWidth(23); mZS = mZ*mZ; mwZS = pow2(mZ * widZ); thetaWRat = 1. / (4. * couplingsPtr->sin2thetaW()); // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(24, -24); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2ffbar2WW::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * pow2(alpEM); // Z0 propagator and gamma*/Z0 interference. double Zprop = sH2 / (pow2(sH - mZS) + mwZS); double Zint = Zprop * (1. - mZS / sH); // Common coupling factors (g = gamma*, Z = Z0, f = t-channel fermion). cgg = 0.5; cgZ = thetaWRat * Zint; cZZ = 0.5 * pow2(thetaWRat) * Zprop; cfg = thetaWRat; cfZ = pow2(thetaWRat) * Zint; cff = pow2(thetaWRat); // Kinematical functions. double rat34 = sH * (2. * (s3 + s4) + pT2) / (s3 * s4); double lambdaS = pow2(sH - s3 - s4) - 4. * s3 * s4; double intA = (sH - s3 - s4) * rat34 / sH; double intB = 4. * (s3 + s4 - pT2); gSS = (lambdaS * rat34 + 12. * sH * pT2) / sH2; gTT = rat34 + 4. * sH * pT2 / tH2; gST = intA + intB / tH; gUU = rat34 + 4. * sH * pT2 / uH2; gSU = intA + intB / uH; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2WW::sigmaHat() { // Flavour-specific couplings. int idAbs = abs(id1); double ei = couplingsPtr->ef(idAbs); double vi = couplingsPtr->vf(idAbs); double ai = couplingsPtr->af(idAbs); // Combine, with different cases for up- and down-type in-flavours. double sigma = sigma0; sigma *= (idAbs%2 == 1) ? (cgg * ei*ei + cgZ * ei * vi + cZZ * (vi*vi + ai*ai)) * gSS + (cfg * ei + cfZ * (vi + ai)) * gST + cff * gTT : (cgg * ei*ei + cgZ * ei * vi + cZZ * (vi*vi + ai*ai)) * gSS - (cfg * ei + cfZ * (vi + ai)) * gSU + cff * gUU; // Initial-state colour factor. Correction for secondary widths. Answer. if (idAbs < 9) sigma /= 3.; sigma *= openFracPair; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2WW::setIdColAcol() { // Always order W- W+, i.e. W- first. setId( id1, id2, -24, 24); // tHat is defined between (f, W-) or (fbar, W+), if (id1 < 0) swapTU = true; // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for W+ and W- decay angles. double Sigma2ffbar2WW::weightDecay( Event& process, int iResBeg, int iResEnd) { // Two resonance decays, but with common weight. if (iResBeg != 5 || iResEnd != 6) return 1.; // Order so that fbar(1) f(2) -> f'(3) fbar'(4) f"(5) fbar"(6). // with f' fbar' from W- and f" fbar" from W+. int i1 = (process[3].id() < 0) ? 3 : 4; int i2 = 7 - i1; int i3 = (process[7].id() > 0) ? 7 : 8; int i4 = 15 - i3; int i5 = (process[9].id() > 0) ? 9 : 10; int i6 = 19 - i5; // Set up four-products and internal products. setupProd( process, i1, i2, i3, i4, i5, i6); // tHat and uHat of fbar f -> W- W+ opposite to previous convention. double tHres = uH; double uHres = tH; // Couplings of incoming (anti)fermion. int idAbs = process[i1].idAbs(); double ai = couplingsPtr->af(idAbs); double li = couplingsPtr->lf(idAbs); double ri = couplingsPtr->rf(idAbs); // gamma*/Z0 propagator/interference factor. double Zint = mZS * (sH - mZS) / (pow2(sH - mZS) + mwZS); // Combinations of couplings and kinematics (norm(x) = |x|^2). double dWW = (li * Zint + ai) / sH; double aWW = dWW + 0.5 * (ai + 1.) / tHres; double bWW = dWW + 0.5 * (ai - 1.) / uHres; double cWW = ri * Zint / sH; double fGK135 = norm( aWW * fGK( 1, 2, 3, 4, 5, 6) - bWW * fGK( 1, 2, 5, 6, 3, 4) ); double fGK253 = norm( cWW * ( fGK( 2, 1, 5, 6, 3, 4) - fGK( 2, 1, 3, 4, 5, 6) ) ); double xiT = xiGK( tHres, uHres); double xiU = xiGK( uHres, tHres); double xjTU = xjGK( tHres, uHres); // Weight and maximum weight. double wt = fGK135 + fGK253; double wtMax = 4. * s3 * s4 * ( aWW * aWW * xiT + bWW * bWW * xiU - aWW * bWW * xjTU + cWW * cWW * (xiT + xiU - xjTU) ); // Done. return wt / wtMax; } //========================================================================== // Sigma2ffbargmZggm class. // Collects common methods for f fbar -> gamma*/Z0 g/gamma and permutations. //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbargmZggm::initProc() { // Allow to pick only gamma* or Z0 part of full gamma*/Z0 expression. gmZmode = settingsPtr->mode("WeakZ0:gmZmode"); // Store Z0 mass and width for propagator. mRes = particleDataPtr->m0(23); GammaRes = particleDataPtr->mWidth(23); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; thetaWRat = 1. / (16. * couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(23); } //-------------------------------------------------------------------------- // Evaluate sum of flavour couplings times phase space. void Sigma2ffbargmZggm::flavSum() { // Coupling factors for Z0 subsystem. double alpSZ = couplingsPtr->alphaS(s3); double colQZ = 3. * (1. + alpSZ / M_PI); // Reset quantities to sum. Declare variables in loop. gamSum = 0.; intSum = 0.; resSum = 0.; int onMode; double mf, mr, psvec, psaxi, betaf, ef2, efvf, vf2af2, colf; // Loop over all Z0 decay channels. for (int i = 0; i < particlePtr->sizeChannels(); ++i) { int idAbs = abs( particlePtr->channel(i).product(0) ); // Only contributions from three fermion generations, except top. if ( (idAbs > 0 && idAbs < 6) || ( idAbs > 10 && idAbs < 17)) { mf = particleDataPtr->m0(idAbs); // Check that above threshold. Phase space. if (m3 > 2. * mf + MASSMARGIN) { mr = pow2(mf / m3); betaf = sqrtpos(1. - 4. * mr); psvec = betaf * (1. + 2. * mr); psaxi = pow3(betaf); // Combine phase space with couplings. ef2 = couplingsPtr->ef2(idAbs) * psvec; efvf = couplingsPtr->efvf(idAbs) * psvec; vf2af2 = couplingsPtr->vf2(idAbs) * psvec + couplingsPtr->af2(idAbs) * psaxi; colf = (idAbs < 6) ? colQZ : 1.; // Store sum of combinations. For outstate only open channels. onMode = particlePtr->channel(i).onMode(); if (onMode == 1 || onMode == 2) { gamSum += colf * ef2; intSum += colf * efvf; resSum += colf * vf2af2; } // End loop over fermions. } } } // Done. Return values in gamSum, intSum and resSum. } //-------------------------------------------------------------------------- // Calculate common parts of gamma/interference/Z0 propagator terms. void Sigma2ffbargmZggm::propTerm() { // Calculate prefactors for gamma/interference/Z0 cross section terms. gamProp = 4. * alpEM / (3. * M_PI * s3); intProp = gamProp * 2. * thetaWRat * s3 * (s3 - m2Res) / ( pow2(s3 - m2Res) + pow2(s3 * GamMRat) ); resProp = gamProp * pow2(thetaWRat * s3) / ( pow2(s3 - m2Res) + pow2(s3 * GamMRat) ); // Optionally only keep gamma* or Z0 term. if (gmZmode == 1) {intProp = 0.; resProp = 0.;} if (gmZmode == 2) {gamProp = 0.; intProp = 0.;} } //-------------------------------------------------------------------------- // Evaluate weight for gamma*/Z0 decay angle. double Sigma2ffbargmZggm::weightDecay( Event& process, int iResBeg, int iResEnd) { // Z should sit in entry 5 and one more parton in entry 6. if (iResBeg != 5 || iResEnd != 6) return 1.; // In an outgoing sense fermions are labelled f(1) fbar(2) f'(3) fbar'(4) // where f' fbar' come from gamma*/Z0 decay. int i1, i2; int i3 = (process[7].id() > 0) ? 7 : 8; int i4 = 15 - i3; // Order so that fbar(1) f(2) -> gamma*/Z0 g/gamma. if (process[3].idAbs() < 20 && process[4].idAbs() < 20) { i1 = (process[3].id() < 0) ? 3 : 4; i2 = 7 - i1; // Order so that f(2)/fbar(1) g/gamma -> f(1)/fbar(2) f'(3) gamma*/Z0. } else if (process[3].idAbs() < 20) { i1 = (process[3].id() < 0) ? 3 : 6; i2 = 9 - i1; } else { i1 = (process[4].id() < 0) ? 4 : 6; i2 = 10 - i1; } // Charge/2, left- and righthanded couplings for in- and out-fermion. int id1Abs = process[i1].idAbs(); double ei = 0.5 * couplingsPtr->ef(id1Abs); double li = couplingsPtr->lf(id1Abs); double ri = couplingsPtr->rf(id1Abs); int id3Abs = process[i3].idAbs(); double ef = 0.5 * couplingsPtr->ef(id3Abs); double lf = couplingsPtr->lf(id3Abs); double rf = couplingsPtr->rf(id3Abs); // Combinations of left/right for in/out, gamma*/interference/Z0. double clilf = ei*ei * gamProp * ef*ef + ei*li * intProp * ef*lf + li*li * resProp * lf*lf; double clirf = ei*ei * gamProp * ef*ef + ei*li * intProp * ef*rf + li*li * resProp * rf*rf; double crilf = ei*ei * gamProp * ef*ef + ei*ri * intProp * ef*lf + ri*ri * resProp * lf*lf; double crirf = ei*ei * gamProp * ef*ef + ei*ri * intProp * ef*rf + ri*ri * resProp * rf*rf; // Evaluate four-vector products. double p13 = process[i1].p() * process[i3].p(); double p14 = process[i1].p() * process[i4].p(); double p23 = process[i2].p() * process[i3].p(); double p24 = process[i2].p() * process[i4].p(); // Calculate weight and its maximum. double wt = (clilf + crirf) * (p13*p13 + p24*p24) + (clirf + crilf) * (p14*p14 + p23*p23) ; double wtMax = (clilf + clirf + crilf + crirf) * (pow2(p13 + p14) + pow2(p23 + p24)); // Done. return (wt / wtMax); } //========================================================================== // Sigma2qqbar2gmZg class. // Cross section for q qbar -> gamma*/Z0 g. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2gmZg::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * (alpEM * alpS) * (2./9.) * (tH2 + uH2 + 2. * sH * s3) / (tH * uH); // Calculate flavour sums for final state. flavSum(); // Calculate prefactors for gamma/interference/Z0 cross section terms. propTerm(); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2gmZg::sigmaHat() { // Combine gamma, interference and Z0 parts. int idAbs = abs(id1); double sigma = sigma0 * ( couplingsPtr->ef2(idAbs) * gamProp * gamSum + couplingsPtr->efvf(idAbs) * intProp * intSum + couplingsPtr->vf2af2(idAbs) * resProp * resSum); // Correct for the running-width Z0 propagater weight in PhaseSpace. sigma /= runBW3; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2gmZg::setIdColAcol() { // Flavours trivial. setId( id1, id2, 23, 21); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 0, 0, 1, 2); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2qg2gmZq class. // Cross section for q g -> gamma*/Z0 q. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qg2gmZq::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * (alpEM * alpS) * (1./12.) * (sH2 + uH2 + 2. * tH * s3) / (-sH * uH); // Calculate flavour sums for final state. flavSum(); // Calculate prefactors for gamma/interference/Z0 cross section terms. propTerm(); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qg2gmZq::sigmaHat() { // Combine gamma, interference and Z0 parts. int idAbs = (id2 == 21) ? abs(id1) : abs(id2); double sigma = sigma0 * ( couplingsPtr->ef2(idAbs) * gamProp * gamSum + couplingsPtr->efvf(idAbs) * intProp * intSum + couplingsPtr->vf2af2(idAbs) * resProp * resSum); // Correct for the running-width Z0 propagater weight in PhaseSpace. sigma /= runBW3; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2gmZq::setIdColAcol() { // Flavour set up for q g -> gamma*/Z0 q. int idq = (id2 == 21) ? id1 : id2; setId( id1, id2, 23, idq); // tH defined between f and f': must swap tHat <-> uHat if q g in. swapTU = (id2 == 21); // Colour flow topologies. Swap when antiquarks. if (id2 == 21) setColAcol( 1, 0, 2, 1, 0, 0, 2, 0); else setColAcol( 2, 1, 1, 0, 0, 0, 2, 0); if (idq < 0) swapColAcol(); } //========================================================================== // Sigma2ffbar2gmZgm class. // Cross section for f fbar -> gamma*/Z0 gamma. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2gmZgm::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * (alpEM*alpEM) * 0.5 * (tH2 + uH2 + 2. * sH * s3) / (tH * uH); // Calculate flavour sums for final state. flavSum(); // Calculate prefactors for gamma/interference/Z0 cross section terms. propTerm(); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2gmZgm::sigmaHat() { // Combine gamma, interference and Z0 parts. int idAbs = abs(id1); double sigma = sigma0 * couplingsPtr->ef2(idAbs) * ( couplingsPtr->ef2(idAbs) * gamProp * gamSum + couplingsPtr->efvf(idAbs) * intProp * intSum + couplingsPtr->vf2af2(idAbs) * resProp * resSum); // Correct for the running-width Z0 propagater weight in PhaseSpace. sigma /= runBW3; // Colour factor. Answer. if (idAbs < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2gmZgm::setIdColAcol() { // Flavours trivial. setId( id1, id2, 23, 22); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2fgm2gmZf class. // Cross section for f gamma -> gamma*/Z0 f'. //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2fgm2gmZf::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * (alpEM*alpEM) * 0.5 * (sH2 + uH2 + 2. * tH * s3) / (- sH * uH); // Calculate flavour sums for final state. flavSum(); // Calculate prefactors for gamma/interference/Z0 cross section terms. propTerm(); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2fgm2gmZf::sigmaHat() { // Combine gamma, interference and Z0 parts. int idAbs = (id2 == 22) ? abs(id1) : abs(id2); double sigma = sigma0 * couplingsPtr->ef2(idAbs) * ( couplingsPtr->ef2(idAbs) * gamProp * gamSum + couplingsPtr->efvf(idAbs) * intProp * intSum + couplingsPtr->vf2af2(idAbs) * resProp * resSum); // Correct for the running-width Z0 propagater weight in PhaseSpace. sigma /= runBW3; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2fgm2gmZf::setIdColAcol() { // Flavour set up for q gamma -> gamma*/Z0 q. int idq = (id2 == 22) ? id1 : id2; setId( id1, id2, 23, idq); // tH defined between f and f': must swap tHat <-> uHat if q gamma in. swapTU = (id2 == 22); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 0, 0, 0, 1, 0); else if (abs(id2) < 9) setColAcol( 0, 0, 1, 0, 0, 0, 1, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (idq < 0) swapColAcol(); } //========================================================================== // Sigma2ffbarWggm class. // Collects common methods for f fbar -> W+- g/gamma and permutations. //-------------------------------------------------------------------------- // Evaluate weight for W+- decay angle. double Sigma2ffbarWggm::weightDecay( Event& process, int iResBeg, int iResEnd) { // W should sit in entry 5 and one more parton in entry 6. if (iResBeg != 5 || iResEnd != 6) return 1.; // In an outgoing sense fermions are labelled f(1) fbar(2) f'(3) fbar'(4) // where f' fbar' come from W+- decay. int i1, i2; int i3 = (process[7].id() > 0) ? 7 : 8; int i4 = 15 - i3; // Order so that fbar(1) f(2) -> W+- g/gamma. if (process[3].idAbs() < 20 && process[4].idAbs() < 20) { i1 = (process[3].id() < 0) ? 3 : 4; i2 = 7 - i1; // Order so that f(2)/fbar(1) g/gamma -> f(1)/fbar(2) f'(3) W+-. } else if (process[3].idAbs() < 20) { i1 = (process[3].id() < 0) ? 3 : 6; i2 = 9 - i1; } else { i1 = (process[4].id() < 0) ? 4 : 6; i2 = 10 - i1; } // Evaluate four-vector products. double p13 = process[i1].p() * process[i3].p(); double p14 = process[i1].p() * process[i4].p(); double p23 = process[i2].p() * process[i3].p(); double p24 = process[i2].p() * process[i4].p(); // Calculate weight and its maximum. double wt = pow2(p13) + pow2(p24); double wtMax = pow2(p13 + p14) + pow2(p23 + p24); // Done. return (wt / wtMax); } //========================================================================== // Sigma2qqbar2Wg class. // Cross section for q qbar' -> W+- g. //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2Wg::initProc() { // Secondary open width fractions, relevant for top (or heavier). openFracPos = particleDataPtr->resOpenFrac(24); openFracNeg = particleDataPtr->resOpenFrac(-24); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2Wg::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * (alpEM * alpS / couplingsPtr->sin2thetaW()) * (2./9.) * (tH2 + uH2 + 2. * sH * s3) / (tH * uH); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2Wg::sigmaHat() { // CKM factor. Secondary width for W+ or W-. double sigma = sigma0 * couplingsPtr->V2CKMid(abs(id1), abs(id2)); int idUp = (abs(id1)%2 == 0) ? id1 : id2; sigma *= (idUp > 0) ? openFracPos : openFracNeg; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2Wg::setIdColAcol() { // Sign of outgoing W. int sign = 1 - 2 * (abs(id1)%2); if (id1 < 0) sign = -sign; setId( id1, id2, 24 * sign, 21); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 0, 0, 1, 2); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2qg2Wq class. // Cross section for q g -> W+- q'. //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2Wq::initProc() { // Secondary open width fractions, relevant for top (or heavier). openFracPos = particleDataPtr->resOpenFrac(24); openFracNeg = particleDataPtr->resOpenFrac(-24); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qg2Wq::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * (alpEM * alpS / couplingsPtr->sin2thetaW()) * (1./12.) * (sH2 + uH2 + 2. * tH * s3) / (-sH * uH); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qg2Wq::sigmaHat() { // CKM factor. Secondary width for W+ or W-. int idAbs = (id2 == 21) ? abs(id1) : abs(id2); double sigma = sigma0 * couplingsPtr->V2CKMsum(idAbs); int idUp = (id2 == 21) ? id1 : id2; if (idAbs%2 == 1) idUp = -idUp; sigma *= (idUp > 0) ? openFracPos : openFracNeg; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2Wq::setIdColAcol() { // Sign of outgoing W. Flavour of outgoing quark. int idq = (id2 == 21) ? id1 : id2; int sign = 1 - 2 * (abs(idq)%2); if (idq < 0) sign = -sign; id4 = couplingsPtr->V2CKMpick(idq); // Flavour set up for q g -> W q. setId( id1, id2, 24 * sign, id4); // tH defined between f and f': must swap tHat <-> uHat if q g in. swapTU = (id2 == 21); // Colour flow topologies. Swap when antiquarks. if (id2 == 21) setColAcol( 1, 0, 2, 1, 0, 0, 2, 0); else setColAcol( 2, 1, 1, 0, 0, 0, 2, 0); if (idq < 0) swapColAcol(); } //========================================================================== // Sigma2ffbar2Wgm class. // Cross section for f fbar' -> W+- gamma. //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2Wgm::initProc() { // Secondary open width fractions, relevant for top (or heavier). openFracPos = particleDataPtr->resOpenFrac(24); openFracNeg = particleDataPtr->resOpenFrac(-24); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2Wgm::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * (alpEM*alpEM / couplingsPtr->sin2thetaW()) * 0.5 * (tH2 + uH2 + 2. * sH * s3) / (tH * uH); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2Wgm::sigmaHat() { // Extrafactor different for e nu and q qbar' instate. int id1Abs = abs(id1); int id2Abs = abs(id2); double chgUp = (id1Abs > 10) ? 0. : 2./3.; double sigma = sigma0 * pow2( chgUp - tH / (tH + uH) ); // CKM and colour factors. Secondary width for W+ or W-. if (id1Abs < 9) sigma *= couplingsPtr->V2CKMid(id1Abs, id2Abs) / 3.; int idUp = (abs(id1)%2 == 0) ? id1 : id2; sigma *= (idUp > 0) ? openFracPos : openFracNeg; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2Wgm::setIdColAcol() { // Sign of outgoing W. int sign = 1 - 2 * (abs(id1)%2); if (id1 < 0) sign = -sign; setId( id1, id2, 24 * sign, 22); // tH defined between (f,W-) or (fbar',W+). swapTU = (sign * id1 > 0); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2fgm2Wf class. // Cross section for f gamma -> W+- f'. //-------------------------------------------------------------------------- // Initialize process. void Sigma2fgm2Wf::initProc() { // Secondary open width fractions, relevant for top (or heavier). openFracPos = particleDataPtr->resOpenFrac(24); openFracNeg = particleDataPtr->resOpenFrac(-24); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2fgm2Wf::sigmaKin() { // Cross section part common for all incoming flavours. sigma0 = (M_PI / sH2) * (alpEM*alpEM / couplingsPtr->sin2thetaW()) * 0.5 * (sH2 + uH2 + 2. * tH * s3) / (pT2 * s3 - sH * uH); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2fgm2Wf::sigmaHat() { // Extrafactor dependent on charge of incoming fermion. int idAbs = (id2 == 22) ? abs(id1) : abs(id2); double charge = (idAbs > 10) ? 1. : ( (idAbs%2 == 1) ? 1./3. : 2./3. ); double sigma = sigma0 * pow2( charge - sH / (sH + uH) ); // CKM factor. Secondary width for W+ or W-. sigma *= couplingsPtr->V2CKMsum(idAbs); int idUp = (id2 == 22) ? id1 : id2; if (idAbs%2 == 1) idUp = -idUp; sigma *= (idUp > 0) ? openFracPos : openFracNeg; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2fgm2Wf::setIdColAcol() { // Sign of outgoing W. Flavour of outgoing fermion. int idq = (id2 == 22) ? id1 : id2; int sign = 1 - 2 * (abs(idq)%2); if (idq < 0) sign = -sign; id4 = couplingsPtr->V2CKMpick(idq); // Flavour set up for q gamma -> W q. setId( id1, id2, 24 * sign, id4); // tH defined between f and f': must swap tHat <-> uHat if q gamma in. swapTU = (id2 == 22); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 0, 0, 0, 1, 0); else if (abs(id2) < 9) setColAcol( 0, 0, 1, 0, 0, 0, 1, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (idq < 0) swapColAcol(); } //========================================================================== // Sigma2gmgm2ffbar class. // Cross section for gamma gamma -> l lbar. //-------------------------------------------------------------------------- // Initialize process wrt flavour. void Sigma2gmgm2ffbar::initProc() { // Process name. nameSave = "gamma gamma -> f fbar"; if (idNew == 1) nameSave = "gamma gamma -> q qbar (uds)"; if (idNew == 4) nameSave = "gamma gamma -> c cbar"; if (idNew == 5) nameSave = "gamma gamma -> b bbar"; if (idNew == 6) nameSave = "gamma gamma -> t tbar"; if (idNew == 11) nameSave = "gamma gamma -> e+ e-"; if (idNew == 13) nameSave = "gamma gamma -> mu+ mu-"; if (idNew == 15) nameSave = "gamma gamma -> tau+ tau-"; // Generate massive phase space, except for u+d+s. idMass = 0; if (idNew > 3) idMass = idNew; // Charge and colour factor. ef4 = 1.; if (idNew == 1) ef4 = 3. * (pow4(2./3.) + 2. * pow4(1./3.)); if (idNew == 4 || idNew == 6) ef4 = 3. * pow4(2./3.); if (idNew == 5) ef4 = 3. * pow4(1./3.); // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(idNew, -idNew); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2gmgm2ffbar::sigmaKin() { // Pick current flavour for u+d+s mix by e_q^4 weights. if (idNew == 1) { double rId = 18. * rndmPtr->flat(); idNow = 1; if (rId > 1.) idNow = 2; if (rId > 17.) idNow = 3; s34Avg = pow2(particleDataPtr->m0(idNow)); } else { idNow = idNew; s34Avg = 0.5 * (s3 + s4) - 0.25 * pow2(s3 - s4) / sH; } // Modified Mandelstam variables for massive kinematics with m3 = m4. double tHQ = -0.5 * (sH - tH + uH); double uHQ = -0.5 * (sH + tH - uH); double tHQ2 = tHQ * tHQ; double uHQ2 = uHQ * uHQ; // Calculate kinematics dependence. if (sH < 4. * s34Avg) sigTU = 0.; else sigTU = 2. * (tHQ * uHQ - s34Avg * sH) * (tHQ2 + uHQ2 + 2. * s34Avg * sH) / (tHQ2 * uHQ2); // Answer. sigma = (M_PI / sH2) * pow2(alpEM) * ef4 * sigTU * openFracPair; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gmgm2ffbar::setIdColAcol() { // Flavours are trivial. setId( id1, id2, idNow, -idNow); // Colour flow in singlet state. if (idNow < 10) setColAcol( 0, 0, 0, 0, 1, 0, 0, 1); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SpaceShower.cc0000644000175000017500000026005012217346252015661 0ustar sunsun// SpaceShower.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // SpaceShower class. #include "Pythia8/SpaceShower.h" namespace Pythia8 { //========================================================================== // The SpaceShower class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Leftover companion can give PDF > 0 at small Q2 where other PDF's = 0, // and then one can end in infinite loop of impossible kinematics. const int SpaceShower::MAXLOOPTINYPDF = 10; // Switch to alternative (but equivalent) backwards evolution for // g -> Q Qbar (Q = c or b) when below QTHRESHOLD * mQ2. const double SpaceShower::CTHRESHOLD = 2.0; const double SpaceShower::BTHRESHOLD = 2.0; // Renew evaluation of PDF's when the pT2 step is bigger than this // (in addition to initial scale and c and b thresholds.) const double SpaceShower::EVALPDFSTEP = 0.1; // Lower limit on PDF value in order to avoid division by zero. const double SpaceShower::TINYPDF = 1e-10; // Lower limit on estimated evolution rate, below which stop. const double SpaceShower::TINYKERNELPDF = 1e-6; // Lower limit on pT2, below which branching is rejected. const double SpaceShower::TINYPT2 = 0.25e-6; // No attempt to do backwards evolution of a heavy (c or b) quark // if evolution starts at a scale pT2 < HEAVYPT2EVOL * mQ2. const double SpaceShower::HEAVYPT2EVOL = 1.1; // No attempt to do backwards evolution of a heavy (c or b) quark // if evolution starts at a x > HEAVYXEVOL * x_max, where // x_max is the largest possible x value for a g -> Q Qbar branching. const double SpaceShower::HEAVYXEVOL = 0.9; // When backwards evolution Q -> g + Q creates a heavy quark Q, // an earlier branching g -> Q + Qbar will restrict kinematics // to M_{Q Qbar}^2 > EXTRASPACEQ * 4 m_Q^2. (Smarter to be found??) const double SpaceShower::EXTRASPACEQ = 2.0; // Never pick pT so low that alphaS is evaluated too close to Lambda_3. const double SpaceShower::LAMBDA3MARGIN = 1.1; // Do not warn for large PDF ratios at small pT2 scales. const double SpaceShower::PT2MINWARN = 1.; // Cutoff for f_e^e at x < 1 - 10^{-10} to be used in z selection. // Note: the x_min quantity come from 1 - x_max. const double SpaceShower::LEPTONXMIN = 1e-10; const double SpaceShower::LEPTONXMAX = 1. - 1e-10; // Stop l -> l gamma evolution slightly above m2l. const double SpaceShower::LEPTONPT2MIN = 1.2; // Enhancement of l -> l gamma trial rate to compensate imperfect modelling. const double SpaceShower::LEPTONFUDGE = 10.; //-------------------------------------------------------------------------- // Initialize alphaStrong, alphaEM and related pTmin parameters. void SpaceShower::init( BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn) { // Store input pointers for future use. beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; // Main flags to switch on and off branchings. doQCDshower = settingsPtr->flag("SpaceShower:QCDshower"); doQEDshowerByQ = settingsPtr->flag("SpaceShower:QEDshowerByQ"); doQEDshowerByL = settingsPtr->flag("SpaceShower:QEDshowerByL"); doWeakShower = settingsPtr->flag("SpaceShower:WeakShower"); // Matching in pT of hard interaction to shower evolution. pTmaxMatch = settingsPtr->mode("SpaceShower:pTmaxMatch"); pTdampMatch = settingsPtr->mode("SpaceShower:pTdampMatch"); pTmaxFudge = settingsPtr->parm("SpaceShower:pTmaxFudge"); pTmaxFudgeMPI = settingsPtr->parm("SpaceShower:pTmaxFudgeMPI"); pTdampFudge = settingsPtr->parm("SpaceShower:pTdampFudge"); // Optionally force emissions to be ordered in rapidity/angle. doRapidityOrder = settingsPtr->flag("SpaceShower:rapidityOrder"); // Charm, bottom and lepton mass thresholds. mc = particleDataPtr->m0(4); mb = particleDataPtr->m0(5); m2c = pow2(mc); m2b = pow2(mb); // Parameters of scale choices. renormMultFac = settingsPtr->parm("SpaceShower:renormMultFac"); factorMultFac = settingsPtr->parm("SpaceShower:factorMultFac"); // Parameters of alphaStrong generation. alphaSvalue = settingsPtr->parm("SpaceShower:alphaSvalue"); alphaSorder = settingsPtr->mode("SpaceShower:alphaSorder"); alphaSnfmax = settingsPtr->mode("StandardModel:alphaSnfmax"); alphaSuseCMW = settingsPtr->flag("SpaceShower:alphaSuseCMW"); alphaS2pi = 0.5 * alphaSvalue / M_PI; // Initialize alpha_strong generation. alphaS.init( alphaSvalue, alphaSorder, alphaSnfmax, alphaSuseCMW); // Lambda for 5, 4 and 3 flavours. Lambda5flav = alphaS.Lambda5(); Lambda4flav = alphaS.Lambda4(); Lambda3flav = alphaS.Lambda3(); Lambda5flav2 = pow2(Lambda5flav); Lambda4flav2 = pow2(Lambda4flav); Lambda3flav2 = pow2(Lambda3flav); // Regularization of QCD evolution for pT -> 0. Can be taken // same as for multiparton interactions, or be set separately. useSamePTasMPI = settingsPtr->flag("SpaceShower:samePTasMPI"); if (useSamePTasMPI) { pT0Ref = settingsPtr->parm("MultipartonInteractions:pT0Ref"); ecmRef = settingsPtr->parm("MultipartonInteractions:ecmRef"); ecmPow = settingsPtr->parm("MultipartonInteractions:ecmPow"); pTmin = settingsPtr->parm("MultipartonInteractions:pTmin"); } else { pT0Ref = settingsPtr->parm("SpaceShower:pT0Ref"); ecmRef = settingsPtr->parm("SpaceShower:ecmRef"); ecmPow = settingsPtr->parm("SpaceShower:ecmPow"); pTmin = settingsPtr->parm("SpaceShower:pTmin"); } // Calculate nominal invariant mass of events. Set current pT0 scale. sCM = m2( beamAPtr->p(), beamBPtr->p()); eCM = sqrt(sCM); pT0 = pT0Ref * pow(eCM / ecmRef, ecmPow); // Restrict pTmin to ensure that alpha_s(pTmin^2 + pT_0^2) does not blow up. double pTminAbs = sqrtpos(pow2(LAMBDA3MARGIN) * Lambda3flav2 / renormMultFac - pT0*pT0); if (pTmin < pTminAbs) { pTmin = pTminAbs; ostringstream newPTmin; newPTmin << fixed << setprecision(3) << pTmin; infoPtr->errorMsg("Warning in SpaceShower::init: pTmin too low", ", raised to " + newPTmin.str() ); infoPtr->setTooLowPTmin(true); } // Parameters of alphaEM generation. alphaEMorder = settingsPtr->mode("SpaceShower:alphaEMorder"); // Initialize alphaEM generation. alphaEM.init( alphaEMorder, settingsPtr); // Parameters of QED evolution. pTminChgQ = settingsPtr->parm("SpaceShower:pTminchgQ"); pTminChgL = settingsPtr->parm("SpaceShower:pTminchgL"); // Derived parameters of QCD evolution. pT20 = pow2(pT0); pT2min = pow2(pTmin); pT2minChgQ = pow2(pTminChgQ); pT2minChgL = pow2(pTminChgL); // Parameters of weak evolution. weakMode = settingsPtr->mode("SpaceShower:weakShowerMode"); pTweakCut = settingsPtr->parm("SpaceShower:pTminWeak"); pT2weakCut = pow2(pTweakCut); weakEnhancement = settingsPtr->parm("SpaceShower:weakShowerEnhancement"); singleWeakEmission = settingsPtr->flag("SpaceShower:singleWeakEmission"); extraScaleTerm = settingsPtr->parm("SpaceShower:extraScaleTerm"); dopTdampMass = settingsPtr->flag("SpaceShower:dopTdampMass"); vetoWeakJets = settingsPtr->flag("SpaceShower:vetoWeakJets"); vetoWeakJetspTcut = settingsPtr->parm("SpaceShower:vetoWeakJetspTcut"); // Z0 and W+- properties needed for weak showers. mZ = particleDataPtr->m0(23); gammaZ = particleDataPtr->mWidth(23); thetaWRat = 1. / (16. * coupSMPtr->sin2thetaW() * coupSMPtr->cos2thetaW()); mW = particleDataPtr->m0(24); gammaW = particleDataPtr->mWidth(24); // Various other parameters. doMEcorrections = settingsPtr->flag("SpaceShower:MEcorrections"); doMEafterFirst = settingsPtr->flag("SpaceShower:MEafterFirst"); doPhiPolAsym = settingsPtr->flag("SpaceShower:phiPolAsym"); doPhiIntAsym = settingsPtr->flag("SpaceShower:phiIntAsym"); strengthIntAsym = settingsPtr->parm("SpaceShower:strengthIntAsym"); nQuarkIn = settingsPtr->mode("SpaceShower:nQuarkIn"); // Possibility of two predetermined hard emissions in event. doSecondHard = settingsPtr->flag("SecondHard:generate"); // Optional dampening at small pT's when large multiplicities. enhanceScreening = settingsPtr->mode("MultipartonInteractions:enhanceScreening"); if (!useSamePTasMPI) enhanceScreening = 0; // Possibility to allow user veto of emission step. canVetoEmission = (userHooksPtr != 0) ? userHooksPtr->canVetoISREmission() : false; } //-------------------------------------------------------------------------- // Find whether to limit maximum scale of emissions. // Also allow for dampening at factorization or renormalization scale. bool SpaceShower::limitPTmax( Event& event, double Q2Fac, double Q2Ren) { // Find whether to limit pT. Begin by user-set cases. bool dopTlimit = false; dopTlimit1 = dopTlimit2 = false; if (pTmaxMatch == 1) dopTlimit = dopTlimit1 = dopTlimit2 = true; else if (pTmaxMatch == 2) dopTlimit = dopTlimit1 = dopTlimit2 = false; // Look if any quark (u, d, s, c, b), gluon or photon in final state. else { int n21 = 0; for (int i = 5; i < event.size(); ++i) { if (event[i].status() == -21) ++n21; else if (n21 == 0) { int idAbs = event[i].idAbs(); if (idAbs <= 5 || idAbs == 21 || idAbs == 22) dopTlimit1 = true; } else if (n21 == 2) { int idAbs = event[i].idAbs(); if (idAbs <= 5 || idAbs == 21 || idAbs == 22) dopTlimit2 = true; } } dopTlimit = (doSecondHard) ? (dopTlimit1 && dopTlimit2) : dopTlimit1; } // Dampening at factorization or renormalization scale; only for hardest. dopTdamp = false; pT2damp = 0.; if ( !dopTlimit1 && (pTdampMatch == 1 || pTdampMatch == 2) ) { dopTdamp = true; pT2damp = pow2(pTdampFudge) * ((pTdampMatch == 1) ? Q2Fac : Q2Ren); } // Done. return dopTlimit; } //-------------------------------------------------------------------------- // Prepare system for evolution; identify ME. // Routine may be called after multiparton interactions, for a new subystem. void SpaceShower::prepare( int iSys, Event& event, bool limitPTmaxIn, double pTfirstTrialIn) { // Reset W/Z radiation flag and counters at first call for new event. if (iSys == 0) { hasWeaklyRadiated = false; nRadA.clear(); nRadB.clear(); } // Find positions of incoming colliding partons. int in1 = partonSystemsPtr->getInA(iSys); int in2 = partonSystemsPtr->getInB(iSys); // Rescattered partons cannot radiate. bool canRadiate1 = !(event[in1].isRescatteredIncoming()); bool canRadiate2 = !(event[in2].isRescatteredIncoming()); // Reset dipole-ends list for first interaction. Also resonances. if (iSys == 0) dipEnd.resize(0); if (iSys == 0) idResFirst = 0; if (iSys == 1) idResSecond = 0; // Find matrix element corrections for system. int MEtype = findMEtype( iSys, event); // In case of DPS overwrite limitPTmaxIn by saved value. if (doSecondHard && iSys == 0) limitPTmaxIn = dopTlimit1; if (doSecondHard && iSys == 1) limitPTmaxIn = dopTlimit2; // Maximum pT scale for dipole ends. double pTmax1 = (limitPTmaxIn) ? event[in1].scale() : eCM; double pTmax2 = (limitPTmaxIn) ? event[in2].scale() : eCM; if ( limitPTmaxIn && (iSys == 0 || (iSys == 1 && doSecondHard)) ) { pTmax1 *= pTmaxFudge; pTmax2 *= pTmaxFudge; } else if (limitPTmaxIn && iSys > 0) { pTmax1 *= pTmaxFudgeMPI; pTmax2 *= pTmaxFudgeMPI; } // Find dipole ends for QCD radiation. // Note: colour type can change during evolution, so book also if zero. if (doQCDshower) { int colType1 = event[in1].colType(); if (canRadiate1) dipEnd.push_back( SpaceDipoleEnd( iSys, 1, in1, in2, pTmax1, colType1, 0, 0, MEtype, canRadiate2) ); int colType2 = event[in2].colType(); if (canRadiate2) dipEnd.push_back( SpaceDipoleEnd( iSys, 2, in2, in1, pTmax2, colType2, 0, 0, MEtype, canRadiate1) ); } // Find dipole ends for QED radiation. // Note: charge type can change during evolution, so book also if zero. if (doQEDshowerByQ || doQEDshowerByL) { int chgType1 = ( (event[in1].isQuark() && doQEDshowerByQ) || (event[in1].isLepton() && doQEDshowerByL) ) ? event[in1].chargeType() : 0; // Special: photons have charge zero, but can evolve (only off Q for now) if (event[in1].id() == 22 && doQEDshowerByQ) chgType1 = 22 ; if (canRadiate1) dipEnd.push_back( SpaceDipoleEnd( iSys, -1, in1, in2, pTmax1, 0, chgType1, 0, MEtype, canRadiate2) ); int chgType2 = ( (event[in2].isQuark() && doQEDshowerByQ) || (event[in2].isLepton() && doQEDshowerByL) ) ? event[in2].chargeType() : 0; // Special: photons have charge zero, but can evolve (only off Q for now) if (event[in2].id() == 22 && doQEDshowerByQ) chgType2 = 22 ; if (canRadiate2) dipEnd.push_back( SpaceDipoleEnd( iSys, -2, in2, in1, pTmax2, 0, chgType2, 0, MEtype, canRadiate1) ); } // Find dipole ends for Weak radiation. No right-handed W emission. // Currently leptons are not allow to emit W bosons. if (doWeakShower) { int weakPol = (rndmPtr->flat() > 0.5) ? -1 : 1; if (canRadiate1) { if ((weakMode == 0 || weakMode == 1) && weakPol == -1 && event[in1].isQuark()) dipEnd.push_back( SpaceDipoleEnd( iSys, 1, in1, in2, pTmax1, 0, 0, 1, 4, canRadiate2, weakPol) ); if ( (weakMode == 0 || weakMode == 2) && (event[in1].isQuark() || event[in1].isLepton()) ) dipEnd.push_back( SpaceDipoleEnd( iSys, 1, in1, in2, pTmax1, 0, 0, 2, 4, canRadiate2, weakPol) ); } weakPol = (rndmPtr->flat() > 0.5) ? -1 : 1; if (canRadiate2) { if ((weakMode == 0 || weakMode == 1) && weakPol == -1 && event[in2].isQuark()) dipEnd.push_back( SpaceDipoleEnd( iSys, 2, in2, in1, pTmax2, 0, 0, 1, 4, canRadiate1, weakPol)); if ((weakMode == 0 || weakMode == 2) && (event[in2].isQuark() || event[in2].isLepton())) dipEnd.push_back( SpaceDipoleEnd( iSys, 2, in2, in1, pTmax2, 0, 0, 2, 4, canRadiate1, weakPol) ); } } // Store the z and pT2 values of the last previous splitting // when an event history has already been constructed. if (iSys == 0 && infoPtr->hasHistory()) { double zNow = infoPtr->zNowISR(); double pT2Now = infoPtr->pT2NowISR(); for (int iDipEnd = 0; iDipEnd < int(dipEnd.size()); ++iDipEnd) { dipEnd[iDipEnd].zOld = zNow; dipEnd[iDipEnd].pT2Old = pT2Now; ++dipEnd[iDipEnd].nBranch; } } // Set the maximum first trial emission's pT. pTfirstTrial = pTfirstTrialIn; } //-------------------------------------------------------------------------- // Select next pT in downwards evolution of the existing dipoles. double SpaceShower::pTnext( Event& event, double pTbegAll, double pTendAll, int nRadIn, bool isFirstTrial) { // Current cm energy, in case it varies between events. sCM = m2( beamAPtr->p(), beamBPtr->p()); eCM = sqrt(sCM); pTbegRef = pTbegAll; // Starting values: no radiating dipole found. nRad = nRadIn; double pT2sel = pow2(pTendAll); iDipSel = 0; iSysSel = 0; dipEndSel = 0; // Loop over all possible dipole ends. for (int iDipEnd = 0; iDipEnd < int(dipEnd.size()); ++iDipEnd) { iDipNow = iDipEnd; dipEndNow = &dipEnd[iDipEnd]; iSysNow = dipEndNow->system; dipEndNow->pT2 = 0.; // Calculate the weak corrections needed for the different // ordering used for weak showers. double weakCorrection = 0.; if (dipEndNow->weakType == 1) weakCorrection = extraScaleTerm * pow2(mW); else if (dipEndNow->weakType == 2) weakCorrection = extraScaleTerm * pow2(mZ); // If first trial, allow weak showers to start at higher scale. if (isFirstTrial) pTbegAll = sqrt(pow2(pTbegAll) + weakCorrection); // If the scale got above the initial max scale for QCD/QED, // set it back to the initial max scale. // This can happen if first emission is a high pT W/Z particle, // because W/Z emissions are allowed to start at the scale pT2 + mW2(mZ2). double pTbegDip = 0; if (dipEndNow->weakType == 0) { if (pTbegAll > pTfirstTrial) pTbegDip = min( pTfirstTrial, dipEndNow->pTmax ); else pTbegDip = min( pTbegAll, dipEndNow->pTmax ); } // Special scales for weak (for different competition). else { pTbegDip = min(sqrt(pow2(pTbegAll) - weakCorrection), dipEndNow->pTmax); pT2sel -= weakCorrection; } // Check whether dipole end should be allowed to shower. double pT2begDip = pow2(pTbegDip); if (pT2begDip > pT2sel && ( dipEndNow->colType != 0 || dipEndNow->chgType != 0 || dipEndNow->weakType != 0) ) { double pT2endDip = 0.; // Determine lower cut for evolution, for QCD or QED (q or l). if (dipEndNow->colType != 0) pT2endDip = max( pT2sel, pT2min ); else if (abs(dipEndNow->weakType) != 0) pT2endDip = max( pT2sel, pT2weakCut); else if (abs(dipEndNow->chgType) != 3 && dipEndNow->chgType != 0) pT2endDip = max( pT2sel, pT2minChgQ ); else pT2endDip = max( pT2sel, pT2minChgL ); // Find properties of dipole and radiating dipole end. sideA = ( abs(dipEndNow->side) == 1 ); BeamParticle& beamNow = (sideA) ? *beamAPtr : *beamBPtr; BeamParticle& beamRec = (sideA) ? *beamBPtr : *beamAPtr; iNow = beamNow[iSysNow].iPos(); iRec = beamRec[iSysNow].iPos(); idDaughter = beamNow[iSysNow].id(); xDaughter = beamNow[iSysNow].x(); x1Now = (sideA) ? xDaughter : beamRec[iSysNow].x(); x2Now = (sideA) ? beamRec[iSysNow].x() : xDaughter; // Note dipole mass correction when recoiler is a rescatter. m2Rec = (dipEndNow->normalRecoil) ? 0. : event[iRec].m2(); m2Dip = x1Now * x2Now * sCM + m2Rec; // Now do evolution in pT2, for QCD, QED or weak. if (pT2begDip > pT2endDip) { if (dipEndNow->colType != 0) pT2nextQCD( pT2begDip, pT2endDip); else if (dipEndNow->chgType != 0 || idDaughter == 22) pT2nextQED( pT2begDip, pT2endDip); else if (dipEndNow->weakType != 0) pT2nextWeak( pT2begDip, pT2endDip); // Update if found larger pT than current maximum. if (dipEndNow->pT2 > pT2sel && dipEndNow->weakType == 0) { pT2sel = dipEndNow->pT2; iDipSel = iDipNow; iSysSel = iSysNow; dipEndSel = dipEndNow; } if (dipEndNow->weakType != 0 && dipEndNow->pT2 > pT2weakCut / 2. && dipEndNow->pT2 + weakCorrection > pT2sel) { pT2sel = dipEndNow->pT2; iDipSel = iDipNow; iSysSel = iSysNow; dipEndSel = dipEndNow; } } } // Cleanup for weak corrections. if (dipEndNow->weakType != 0) { pT2sel += weakCorrection; if (isFirstTrial) pTbegAll = sqrt(pow2(pTbegAll) - weakCorrection); } // End loop over dipole ends. } // Return nonvanishing value if found pT is bigger than already found. return (dipEndSel == 0) ? 0. : sqrt(pT2sel); } //-------------------------------------------------------------------------- // Evolve a QCD dipole end. void SpaceShower::pT2nextQCD( double pT2begDip, double pT2endDip) { // Some properties and kinematical starting values. BeamParticle& beam = (sideA) ? *beamAPtr : *beamBPtr; bool isGluon = (idDaughter == 21); bool isValence = beam[iSysNow].isValence(); int MEtype = dipEndNow->MEtype; double pT2 = pT2begDip; double xMaxAbs = beam.xMax(iSysNow); double zMinAbs = xDaughter / xMaxAbs; if (xMaxAbs < 0.) { infoPtr->errorMsg("Warning in SpaceShower::pT2nextQCD: " "xMaxAbs negative"); return; } // Starting values for handling of massive quarks (c/b), if any. double idMassive = 0; if ( abs(idDaughter) == 4 ) idMassive = 4; if ( abs(idDaughter) == 5 ) idMassive = 5; bool isMassive = (idMassive > 0); double m2Massive = 0.; double mRatio = 0.; double zMaxMassive = 1.; double m2Threshold = pT2; // Evolution below scale of massive quark or at large x is impossible. if (isMassive) { m2Massive = (idMassive == 4) ? m2c : m2b; if (pT2 < HEAVYPT2EVOL * m2Massive) return; mRatio = sqrt( m2Massive / m2Dip ); zMaxMassive = (1. - mRatio) / ( 1. + mRatio * (1. - mRatio) ); if (xDaughter > HEAVYXEVOL * zMaxMassive * xMaxAbs) return; // Find threshold scale below which only g -> Q + Qbar will be allowed. m2Threshold = (idMassive == 4) ? min( pT2, CTHRESHOLD * m2c) : min( pT2, BTHRESHOLD * m2b); } // Variables used inside evolution loop. (Mainly dummy starting values.) int nFlavour = 3; double b0 = 4.5; double Lambda2 = Lambda3flav2; double pT2minNow = pT2endDip; int idMother = 0; int idSister = 0; double z = 0.; double zMaxAbs = 0.; double zRootMax = 0.; double zRootMin = 0.; double g2gInt = 0.; double q2gInt = 0.; double q2qInt = 0.; double g2qInt = 0.; double g2Qenhance = 0.; double xPDFdaughter = 0.; double xPDFmother[21] = {0.}; double xPDFgMother = 0.; double xPDFmotherSum = 0.; double kernelPDF = 0.; double xMother = 0.; double wt = 0.; double Q2 = 0.; double mSister = 0.; double m2Sister = 0.; double pT2corr = 0.; double pT2PDF = pT2; bool needNewPDF = true; // Begin evolution loop towards smaller pT values. int loopTinyPDFdau = 0; bool hasTinyPDFdau = false; do { wt = 0.; // Bad sign if repeated looping with small daughter PDF, so fail. // (Example: if all PDF's = 0 below Q_0, except for c/b companion.) if (hasTinyPDFdau) ++loopTinyPDFdau; if (loopTinyPDFdau > MAXLOOPTINYPDF) { infoPtr->errorMsg("Warning in SpaceShower::pT2nextQCD: " "small daughter PDF"); return; } // Initialize integrals of splitting kernels and evaluate parton // densities at the beginning. Reinitialize after long evolution // in pT2 or when crossing c and b flavour thresholds. if (needNewPDF || pT2 < EVALPDFSTEP * pT2PDF) { pT2PDF = pT2; hasTinyPDFdau = false; // Determine overestimated z range; switch at c and b masses. if (pT2 > m2b) { nFlavour = 5; pT2minNow = max( m2b, pT2endDip); b0 = 23./6.; Lambda2 = Lambda5flav2; } else if (pT2 > m2c) { nFlavour = 4; pT2minNow = max( m2c, pT2endDip); b0 = 25./6.; Lambda2 = Lambda4flav2; } else { nFlavour = 3; pT2minNow = pT2endDip; b0 = 27./6.; Lambda2 = Lambda3flav2; } // A change of renormalization scale expressed by a change of Lambda. Lambda2 /= renormMultFac; zMaxAbs = 1. - 0.5 * (pT2minNow / m2Dip) * ( sqrt( 1. + 4. * m2Dip / pT2minNow ) - 1. ); if (isMassive) zMaxAbs = min( zMaxAbs, zMaxMassive); // Go to another z range with lower mass scale if current is closed. if (zMinAbs > zMaxAbs) { if (nFlavour == 3 || (idMassive == 4 && nFlavour == 4) || idMassive == 5) return; pT2 = (nFlavour == 4) ? m2c : m2b; continue; } // Parton density of daughter at current scale. xPDFdaughter = beam.xfISR(iSysNow, idDaughter, xDaughter, factorMultFac * pT2); if (xPDFdaughter < TINYPDF) { xPDFdaughter = TINYPDF; hasTinyPDFdau = true; } // Integrals of splitting kernels for gluons: g -> g, q -> g. if (isGluon) { g2gInt = 6. * log(zMaxAbs * (1.-zMinAbs) / (zMinAbs * (1.-zMaxAbs))); if (doMEcorrections) g2gInt *= calcMEmax(MEtype, 21, 21); q2gInt = (16./3.) * (1./sqrt(zMinAbs) - 1./sqrt(zMaxAbs)); if (doMEcorrections) q2gInt *= calcMEmax(MEtype, 1, 21); // Parton density of potential quark mothers to a g. xPDFmotherSum = 0.; for (int i = -nQuarkIn; i <= nQuarkIn; ++i) { if (i == 0) { xPDFmother[10] = 0.; } else { xPDFmother[i+10] = beam.xfISR(iSysNow, i, xDaughter, factorMultFac * pT2); xPDFmotherSum += xPDFmother[i+10]; } } // Total QCD evolution coefficient for a gluon. kernelPDF = g2gInt + q2gInt * xPDFmotherSum / xPDFdaughter; // For valence quark only need consider q -> q g branchings. // Introduce an extra factor sqrt(z) to smooth bumps. } else if (isValence) { zRootMin = (1. + sqrt(zMinAbs)) / (1. - sqrt(zMinAbs)); zRootMax = (1. + sqrt(zMaxAbs)) / (1. - sqrt(zMaxAbs)); q2qInt = (8./3.) * log( zRootMax / zRootMin ); if (doMEcorrections) q2qInt *= calcMEmax(MEtype, 1, 1); kernelPDF = q2qInt; // Integrals of splitting kernels for quarks: q -> q, g -> q. } else { q2qInt = (8./3.) * log( (1. - zMinAbs) / (1. - zMaxAbs) ); if (doMEcorrections) q2qInt *= calcMEmax(MEtype, 1, 1); g2qInt = 0.5 * (zMaxAbs - zMinAbs); if (doMEcorrections) g2qInt *= calcMEmax(MEtype, 21, 1); // Increase estimated upper weight for g -> Q + Qbar. if (isMassive) { if (alphaSorder == 0) g2Qenhance = log(pT2/m2Massive) / log(m2Threshold/m2Massive); else { double m2log = log( m2Massive / Lambda2); g2Qenhance = log( log(pT2/Lambda2) / m2log ) / log( log(m2Threshold/Lambda2) / m2log ); } g2qInt *= g2Qenhance; } // Parton density of a potential gluon mother to a q. xPDFgMother = beam.xfISR(iSysNow, 21, xDaughter, factorMultFac * pT2); // Total QCD evolution coefficient for a quark. kernelPDF = q2qInt + g2qInt * xPDFgMother / xPDFdaughter; } // End evaluation of splitting kernels and parton densities. needNewPDF = false; } if (kernelPDF < TINYKERNELPDF) return; // Pick pT2 (in overestimated z range), for one of three different cases. // Assume form alphas(pT0^2 + pT^2) * dpT^2/(pT0^2 + pT^2). double Q2alphaS; // Fixed alpha_strong. if (alphaSorder == 0) { pT2 = (pT2 + pT20) * pow( rndmPtr->flat(), 1. / (alphaS2pi * kernelPDF)) - pT20; // First-order alpha_strong. } else if (alphaSorder == 1) { pT2 = Lambda2 * pow( (pT2 + pT20) / Lambda2, pow(rndmPtr->flat(), b0 / kernelPDF) ) - pT20; // For second order reject by second term in alpha_strong expression. } else { do { pT2 = Lambda2 * pow( (pT2 + pT20) / Lambda2, pow(rndmPtr->flat(), b0 / kernelPDF) ) - pT20; Q2alphaS = renormMultFac * max( pT2 + pT20, pow2(LAMBDA3MARGIN) * Lambda3flav2); } while (alphaS.alphaS2OrdCorr(Q2alphaS) < rndmPtr->flat() && pT2 > pT2minNow); } // Check for pT2 values that prompt special action. // If fallen into b threshold region, force g -> b + bbar. if (idMassive == 5 && pT2 < m2Threshold) { pT2nearQCDthreshold( beam, m2Massive, m2Threshold, xMaxAbs, zMinAbs, zMaxMassive ); return; // If crossed b threshold, continue evolution from this threshold. } else if (nFlavour == 5 && pT2 < m2b) { needNewPDF = true; pT2 = m2b; continue; // If fallen into c threshold region, force g -> c + cbar. } else if (idMassive == 4 && pT2 < m2Threshold) { pT2nearQCDthreshold( beam, m2Massive, m2Threshold, xMaxAbs, zMinAbs, zMaxMassive ); return; // If crossed c threshold, continue evolution from this threshold. } else if (nFlavour == 4 && pT2 < m2c) { needNewPDF = true; pT2 = m2c; continue; // Abort evolution if below cutoff scale, or below another branching. } else if (pT2 < pT2endDip) return; // Select z value of branching to g, and corrective weight. if (isGluon) { // g -> g (+ g). if (rndmPtr->flat() * kernelPDF < g2gInt) { idMother = 21; idSister = 21; z = 1. / ( 1. + ((1. - zMinAbs) / zMinAbs) * pow( (zMinAbs * (1. - zMaxAbs)) / (zMaxAbs * (1. - zMinAbs)), rndmPtr->flat() ) ); wt = pow2( 1. - z * (1. - z)); } else { // q -> g (+ q): also select flavour. double temp = xPDFmotherSum * rndmPtr->flat(); idMother = -nQuarkIn - 1; do { temp -= xPDFmother[(++idMother) + 10]; } while (temp > 0. && idMother < nQuarkIn); idSister = idMother; z = (zMinAbs * zMaxAbs) / pow2( sqrt(zMinAbs) + rndmPtr->flat() * ( sqrt(zMaxAbs)- sqrt(zMinAbs) )); wt = 0.5 * (1. + pow2(1. - z)) * sqrt(z) * xPDFdaughter / xPDFmother[idMother + 10]; } // Select z value of branching to q, and corrective weight. // Include massive kernel corrections for c and b quarks. } else { // q -> q (+ g). if (isValence || rndmPtr->flat() * kernelPDF < q2qInt) { idMother = idDaughter; idSister = 21; // Valence more peaked at large z. if (isValence) { double zTmp = zRootMin * pow(zRootMax / zRootMin, rndmPtr->flat() ); z = pow2( (1. - zTmp) / (1. + zTmp) ); } else { z = 1. - (1. - zMinAbs) * pow( (1. - zMaxAbs) / (1. - zMinAbs), rndmPtr->flat() ); } if (!isMassive) { wt = 0.5 * (1. + pow2(z)); } else { //?? Bug?? should be 2 more for massive part?? // wt = 0.5 * (1. + pow2(z) - z * pow2(1.-z) * m2Massive / pT2); wt = 0.5 * (1. + pow2(z)) - z * pow2(1.-z) * m2Massive / pT2; } if (isValence) wt *= sqrt(z); // g -> q (+ qbar). } else { idMother = 21; idSister = - idDaughter; z = zMinAbs + rndmPtr->flat() * (zMaxAbs - zMinAbs); if (!isMassive) { wt = (pow2(z) + pow2(1.-z)) * xPDFdaughter / xPDFgMother ; } else { wt = (pow2(z) + pow2(1.-z) + 2. * z * (1.-z) * m2Massive / pT2) * xPDFdaughter / (xPDFgMother * g2Qenhance) ; } } } // Derive Q2 and x of mother from pT2 and z. Q2 = pT2 / (1. - z); xMother = xDaughter / z; // Correction to x for massive recoiler from rescattering. if (!dipEndNow->normalRecoil) { if (sideA) xMother += (m2Rec / (x2Now * sCM)) * (1. / z - 1.); else xMother += (m2Rec / (x1Now * sCM)) * (1. / z - 1.); } if (xMother > xMaxAbs) { wt = 0.; continue; } // Forbidden emission if outside allowed z range for given pT2. mSister = particleDataPtr->m0(idSister); m2Sister = pow2(mSister); pT2corr = Q2 - z * (m2Dip + Q2) * (Q2 + m2Sister) / m2Dip; if (pT2corr < TINYPT2) { wt = 0.; continue; } // Optionally veto emissions not ordered in rapidity (= angle). if ( doRapidityOrder && dipEndNow->nBranch > 0 && pT2 > pow2( (1. - z) / (z * (1. - dipEndNow->zOld)) ) * dipEndNow->pT2Old ) { wt = 0.; continue; } // If creating heavy quark by Q -> g + Q then next need g -> Q + Qbar. // So minimum total mass2 is 4 * m2Sister, but use more to be safe. if ( isGluon && ( abs(idMother) == 4 || abs(idMother) == 5 )) { double m2QQsister = EXTRASPACEQ * 4. * m2Sister; double pT2QQcorr = Q2 - z * (m2Dip + Q2) * (Q2 + m2QQsister) / m2Dip; if (pT2QQcorr < TINYPT2) { wt = 0.; continue; } } // Evaluation of ME correction. if (doMEcorrections) wt *= calcMEcorr(MEtype, idMother, idDaughter, m2Dip, z, Q2, m2Sister) / calcMEmax(MEtype, idMother, idDaughter); // Optional dampening of large pT values in first radiation. if (dopTdamp && iSysNow == 0 && MEtype == 0 && nRad == 0) wt *= pT2damp / (pT2 + pT2damp); // Idea suggested by Gosta Gustafson: increased screening in events // with large activity can be simulated by pT0_eff = sqrt(n) * pT0. if (enhanceScreening == 2) { int nSysNow = infoPtr->nMPI() + infoPtr->nISR() + 1; double WTscreen = pow2( (pT2 + pT20) / (pT2 + nSysNow * pT20) ); wt *= WTscreen; } // Evaluation of new daughter and mother PDF's. double xPDFdaughterNew = max ( TINYPDF, beam.xfISR(iSysNow, idDaughter, xDaughter, factorMultFac * pT2) ); double xPDFmotherNew = beam.xfISR(iSysNow, idMother, xMother, factorMultFac * pT2); wt *= xPDFmotherNew / xPDFdaughterNew; // Check that valence step does not cause problem. if (wt > 1. && pT2 > PT2MINWARN) infoPtr->errorMsg("Warning in " "SpaceShower::pT2nextQCD: weight above unity"); // Iterate until acceptable pT (or have fallen below pTmin). } while (wt < rndmPtr->flat()) ; // Save values for (so far) acceptable branching. dipEndNow->store( idDaughter,idMother, idSister, x1Now, x2Now, m2Dip, pT2, z, xMother, Q2, mSister, m2Sister, pT2corr); } //-------------------------------------------------------------------------- // Evolve a QCD dipole end near threshold, with g -> Q + Qbar enforced. // Note: No explicit Sudakov factor formalism here. Instead use that // df_Q(x, pT2) = (alpha_s/2pi) * (dT2/pT2) * ((gluon) * (splitting)). // This implies that effects of Q -> Q + g are neglected in this range. void SpaceShower::pT2nearQCDthreshold( BeamParticle& beam, double m2Massive, double m2Threshold, double xMaxAbs, double zMinAbs, double zMaxMassive) { // Initial values, to be used in kinematics and weighting. double Lambda2 = (abs(idDaughter) == 4) ? Lambda4flav2 : Lambda5flav2; Lambda2 /= renormMultFac; double logM2Lambda2 = (alphaSorder > 0) ? log( m2Massive / Lambda2 ) : 1.; double xPDFmotherOld = beam.xfISR(iSysNow, 21, xDaughter, factorMultFac * m2Threshold); // Variables used inside evolution loop. (Mainly dummy start values.) int loop = 0; double wt = 0.; double pT2 = 0.; double z = 0.; double Q2 = 0.; double pT2corr = 0.; double xMother = 0.; // Begin loop over tries to find acceptable g -> Q + Qbar branching. do { wt = 0.; // Check that not caught in infinite loop with impossible kinematics. if (++loop > 100) { infoPtr->errorMsg("Error in SpaceShower::pT2nearQCDthreshold: " "stuck in loop"); return; } // Pick dpT2/pT2 in range [m2Massive,thresholdRatio * m2Massive]. pT2 = m2Massive * pow( m2Threshold / m2Massive, rndmPtr->flat() ); // Pick z flat in allowed range. z = zMinAbs + rndmPtr->flat() * (zMaxMassive - zMinAbs); // Check that kinematically possible choice. Q2 = pT2 / (1.-z) - m2Massive; pT2corr = Q2 - z * (m2Dip + Q2) * (Q2 + m2Massive) / m2Dip; if (pT2corr < TINYPT2) continue; // Correction factor for running alpha_s. (Only first order for now.) wt = (alphaSorder > 0) ? logM2Lambda2 / log( pT2 / Lambda2 ) : 1.; // Correction factor for splitting kernel. wt *= pow2(z) + pow2(1.-z) + 2. * z * (1.-z) * m2Massive / pT2; // x, including correction for massive recoiler from rescattering. xMother = xDaughter / z; if (!dipEndNow->normalRecoil) { if (sideA) xMother += (m2Rec / (x2Now * sCM)) * (1. / z - 1.); else xMother += (m2Rec / (x1Now * sCM)) * (1. / z - 1.); } if (xMother > xMaxAbs) { wt = 0.; continue; } // Correction factor for gluon density. double xPDFmotherNew = beam.xfISR(iSysNow, 21, xMother, factorMultFac * pT2); wt *= xPDFmotherNew / xPDFmotherOld; // Iterate until acceptable pT and z. } while (wt < rndmPtr->flat()) ; // Save values for (so far) acceptable branching. double mSister = (abs(idDaughter) == 4) ? mc : mb; dipEndNow->store( idDaughter, 21, -idDaughter, x1Now, x2Now, m2Dip, pT2, z, xMother, Q2, mSister, pow2(mSister), pT2corr); } //-------------------------------------------------------------------------- // Evolve a QED dipole end. void SpaceShower::pT2nextQED( double pT2begDip, double pT2endDip) { // Type of dipole and starting values. BeamParticle& beam = (sideA) ? *beamAPtr : *beamBPtr; bool isLeptonBeam = beam.isLepton(); int MEtype = dipEndNow->MEtype; bool isPhoton = (idDaughter == 22); double pT2 = pT2begDip; double m2Lepton = (isLeptonBeam) ? pow2(beam.m()) : 0.; if (isLeptonBeam && pT2begDip < m2Lepton) return; // Currently no f -> gamma branching implemented for lepton beams if (isPhoton && isLeptonBeam) return; // alpha_em at maximum scale provides upper estimate. double alphaEMmax = alphaEM.alphaEM(renormMultFac * pT2begDip); double alphaEM2pi = alphaEMmax / (2. * M_PI); // Maximum x of mother implies minimum z = xDaughter / xMother. double xMaxAbs = (isLeptonBeam) ? LEPTONXMAX : beam.xMax(iSysNow); double zMinAbs = xDaughter / xMaxAbs; if (xMaxAbs < 0.) { infoPtr->errorMsg("Warning in SpaceShower::pT2nextQED: " "xMaxAbs negative"); return; } // Maximum z from minimum pT and, for lepton, from minimum x_gamma. double zMaxAbs = 1. - 0.5 * (pT2endDip / m2Dip) * ( sqrt( 1. + 4. * m2Dip / pT2endDip ) - 1. ); if (isLeptonBeam) { double zMaxLepton = xDaughter / (xDaughter + LEPTONXMIN); if (zMaxLepton < zMaxAbs) zMaxAbs = zMaxLepton; } if (zMaxAbs < zMinAbs) return; // Variables used inside evolution loop. (Mainly dummy start values.) int idMother = 0; int idSister = 22; double z = 0.; double xMother = 0.; double wt = 0.; double Q2 = 0.; double mSister = 0.; double m2Sister = 0.; double pT2corr = 0.; // QED evolution of fermions if (!isPhoton) { // Integrals of splitting kernels for fermions: f -> f. Use 1 + z^2 < 2. // Ansatz f(z) = 2 / (1 - z), with + 2 / (z - xDaughter) for lepton. double f2fInt = 0.; double f2fIntA = 2. * log( (1. - zMinAbs) / (1. - zMaxAbs) ); double f2fIntB = 0.; if (isLeptonBeam) { f2fIntB = 2. * log( (zMaxAbs - xDaughter) / (zMinAbs - xDaughter) ); f2fInt = f2fIntA + f2fIntB; } else f2fInt = pow2(dipEndNow->chgType / 3.) * f2fIntA; // Upper estimate for evolution equation, including fudge factor. if (doMEcorrections) f2fInt *= calcMEmax(MEtype, 1, 1); double kernelPDF = alphaEM2pi * f2fInt; double fudge = (isLeptonBeam) ? LEPTONFUDGE * log(m2Dip/m2Lepton) : 1.; kernelPDF *= fudge; if (kernelPDF < TINYKERNELPDF) return; // Begin evolution loop towards smaller pT values. do { // Pick pT2 (in overestimated z range). // For l -> l gamma include extrafactor 1 / ln(pT2 / m2l) in evolution. double shift = pow(rndmPtr->flat(), 1. / kernelPDF); if (isLeptonBeam) pT2 = m2Lepton * pow( pT2 / m2Lepton, shift); else pT2 = pT2 * shift; // Abort evolution if below cutoff scale, or below another branching. if (pT2 < pT2endDip) return; if (isLeptonBeam && pT2 < LEPTONPT2MIN * m2Lepton) return; // Select z value of branching f -> f + gamma, and corrective weight. idMother = idDaughter; wt = 1.; if (isLeptonBeam) { if (f2fIntA > rndmPtr->flat() * (f2fIntA + f2fIntB)) { z = 1. - (1. - zMinAbs) * pow( (1. - zMaxAbs) / (1. - zMinAbs), rndmPtr->flat() ); } else { z = xDaughter + (zMinAbs - xDaughter) * pow( (zMaxAbs - xDaughter) / (zMinAbs - xDaughter), rndmPtr->flat() ); } wt *= (z - xDaughter) / (1. - xDaughter); } else { z = 1. - (1. - zMinAbs) * pow( (1. - zMaxAbs) / (1. - zMinAbs), rndmPtr->flat() ); } wt *= 0.5 * (1. + pow2(z)); // Derive Q2 and x of mother from pT2 and z. Q2 = pT2 / (1. - z); xMother = xDaughter / z; // Correction to x for massive recoiler from rescattering. if (!dipEndNow->normalRecoil) { if (sideA) xMother += (m2Rec / (x2Now * sCM)) * (1. / z - 1.); else xMother += (m2Rec / (x1Now * sCM)) * (1. / z - 1.); } if (xMother > xMaxAbs) { wt = 0.; continue; } // Forbidden emission if outside allowed z range for given pT2. mSister = 0.; m2Sister = 0.; pT2corr = Q2 - z * (m2Dip + Q2) * (Q2 + m2Sister) / m2Dip; if (pT2corr < TINYPT2) { wt = 0.; continue; } // Correct by ln(pT2 / m2l) and fudge factor. if (isLeptonBeam) wt *= log(pT2 / m2Lepton) / fudge; // Evaluation of ME correction. if (doMEcorrections) wt *= calcMEcorr(MEtype, idMother, idDaughter, m2Dip, z, Q2, m2Sister) / calcMEmax(MEtype, idMother, idDaughter); // Extra QED correction for f fbar -> W+- gamma. Debug?? if (doMEcorrections && MEtype == 1 && idDaughter == idMother && ( (iSysNow == 0 && idResFirst == 24) || (iSysNow == 1 && idResSecond == 24) ) ) { double tHe = -Q2; double uHe = Q2 - m2Dip * (1. - z) / z; double chg1 = abs(dipEndNow->chgType / 3.); double chg2 = 1. - chg1; wt *= pow2(chg1 * uHe - chg2 * tHe) / ( (tHe + uHe) * (pow2(chg1) * uHe + pow2(chg2) * tHe) ); } // Optional dampening of large pT values in first radiation. if (dopTdamp && iSysNow == 0 && MEtype == 0 && nRad == 0) wt *= pT2damp / (pT2 + pT2damp); // Correct to current value of alpha_EM. double alphaEMnow = alphaEM.alphaEM(renormMultFac * pT2); wt *= (alphaEMnow / alphaEMmax); // Evaluation of new daughter and mother PDF's. double xPDFdaughterNew = max ( TINYPDF, beam.xfISR(iSysNow, idDaughter, xDaughter, factorMultFac * pT2) ); double xPDFmotherNew = beam.xfISR(iSysNow, idMother, xMother, factorMultFac * pT2); wt *= xPDFmotherNew / xPDFdaughterNew; // Iterate until acceptable pT (or have fallen below pTmin). } while (wt < rndmPtr->flat()) ; } // QED evolution of photons (so far only for hadron beams). else { // Initial values int nFlavour = 3; double kernelPDF = 0.0; double xPDFdaughter = 0.; double xPDFmother[21] = {0.}; double xPDFmotherSum = 0.0; double pT2PDF = pT2; double pT2minNow = pT2endDip; bool needNewPDF = true; // Begin evolution loop towards smaller pT values. int loopTinyPDFdau = 0; bool hasTinyPDFdau = false; do { wt = 0.; // Bad sign if repeated looping with small daughter PDF, so fail. if (hasTinyPDFdau) ++loopTinyPDFdau; if (loopTinyPDFdau > MAXLOOPTINYPDF) { infoPtr->errorMsg("Warning in SpaceShower::pT2nextQED: " "small daughter PDF"); return; } // Initialize integrals of splitting kernels and evaluate parton // densities at the beginning. Reinitialize after long evolution // in pT2 or when crossing c and b flavour thresholds. if (needNewPDF || pT2 < EVALPDFSTEP * pT2PDF) { pT2PDF = pT2; hasTinyPDFdau = false; // Determine overestimated z range; switch at c and b masses. if (pT2 > m2b && nQuarkIn >= 5) { nFlavour = 5; pT2minNow = max( m2b, pT2endDip); } else if (pT2 > m2c && nQuarkIn >= 4) { nFlavour = 4; pT2minNow = max( m2c, pT2endDip); } else { nFlavour = 3; pT2minNow = pT2endDip; } // Compute upper z limit zMaxAbs = 1. - 0.5 * (pT2minNow / m2Dip) * ( sqrt( 1. + 4. * m2Dip / pT2minNow ) - 1. ); // Parton density of daughter at current scale. xPDFdaughter = beam.xfISR(iSysNow, idDaughter, xDaughter, factorMultFac * pT2); if (xPDFdaughter < TINYPDF) { xPDFdaughter = TINYPDF; hasTinyPDFdau = true; } // Integral over f -> gamma f splitting kernel. // Normalized so: 4/3 aS/2pi P(z) -> eq^2 * aEM/2pi P(z). // (Charge-weighting happens below.) double q2gInt = 4. * (1./sqrt(zMinAbs) - 1./sqrt(zMaxAbs)); // Charge-weighted Parton density of potential quark mothers. xPDFmotherSum = 0.; for (int i = -nFlavour; i <= nFlavour; ++i) { if (i == 0) { xPDFmother[10] = 0.; } else { xPDFmother[i+10] = pow2((abs(i+1) % 2 + 1)/3.0) * beam.xfISR(iSysNow, i, xDaughter, factorMultFac * pT2); xPDFmotherSum += xPDFmother[i+10]; } } // Total QED evolution coefficient for a photon. kernelPDF = q2gInt * xPDFmotherSum / xPDFdaughter; // End evaluation of splitting kernels and parton densities. needNewPDF = false; } if (kernelPDF < TINYKERNELPDF) return; // Select pT2 for next trial branching pT2 *= pow( rndmPtr->flat(), 1. / (alphaEM2pi * kernelPDF)); // If crossed b threshold, continue evolution from this threshold. if (nFlavour == 5 && pT2 < m2b) { needNewPDF = true; pT2 = m2b; continue; } // If crossed c threshold, continue evolution from this threshold. else if (nFlavour == 4 && pT2 < m2c) { needNewPDF = true; pT2 = m2c; continue; } // Abort evolution if below cutoff scale, or below another branching. else if (pT2 < pT2endDip) return; // Select flavour for trial branching double temp = xPDFmotherSum * rndmPtr->flat(); idMother = -nQuarkIn - 1; do { temp -= xPDFmother[(++idMother) + 10]; } while (temp > 0. && idMother < nQuarkIn); // Sister is same as mother, but can have m2 > 0 idSister = idMother; mSister = particleDataPtr->m0(idSister); m2Sister = pow2(mSister); // Select z for trial branching z = (zMinAbs * zMaxAbs) / pow2( sqrt(zMinAbs) + rndmPtr->flat() * ( sqrt(zMaxAbs)- sqrt(zMinAbs) )); // Trial weight: splitting kernel wt = 0.5 * (1. + pow2(1. - z)) * sqrt(z); // Trial weight: running alpha_EM double alphaEMnow = alphaEM.alphaEM(renormMultFac * pT2); wt *= (alphaEMnow / alphaEMmax); // Derive Q2 and x of mother from pT2 and z Q2 = pT2 / (1. - z); xMother = xDaughter / z; // Correction to x for massive recoiler from rescattering. if (!dipEndNow->normalRecoil) { if (sideA) xMother += (m2Rec / (x2Now * sCM)) * (1. / z - 1.); else xMother += (m2Rec / (x1Now * sCM)) * (1. / z - 1.); } // Compute pT2corr pT2corr = Q2 - z * (m2Dip + Q2) * (Q2 + m2Sister) / m2Dip; if (pT2corr < TINYPT2) { wt = 0.; continue; } // If creating heavy quark by Q -> gamma + Q then next g -> Q + Qbar. // So minimum total mass2 is 4 * m2Sister, but use more to be safe. if ( abs(idMother) == 4 || abs(idMother) == 5 ) { double m2QQsister = EXTRASPACEQ * 4. * m2Sister; double pT2QQcorr = Q2 - z * (m2Dip + Q2) * (Q2 + m2QQsister) / m2Dip; if (pT2QQcorr < TINYPT2) { wt = 0.; continue; } } // Optional dampening of large pT values in first radiation. if (dopTdamp && iSysNow == 0 && MEtype == 0 && nRad == 0) wt *= pT2damp / (pT2 + pT2damp); // Evaluation of new daughter PDF double xPDFdaughterNew = beam.xfISR(iSysNow, idDaughter, xDaughter, factorMultFac * pT2); if (xPDFdaughterNew < TINYPDF) { xPDFdaughterNew = TINYPDF; } // Evaluation of new charge-weighted mother PDF double xPDFmotherNew = pow2( (abs(idMother+1) % 2 + 1)/3.0 ) * beam.xfISR(iSysNow, idMother, xMother, factorMultFac * pT2); // Trial weight: divide out old pdf ratio wt *= xPDFdaughter / xPDFmother[idMother + 10]; // Trial weight: new pdf ratio wt *= xPDFmotherNew / xPDFdaughterNew; // Iterate until acceptable pT (or have fallen below pTmin). } while (wt < rndmPtr->flat()) ; } // Save values for (so far) acceptable branching. dipEndNow->store( idDaughter, idMother, idSister, x1Now, x2Now, m2Dip, pT2, z, xMother, Q2, mSister, m2Sister, pT2corr); } //-------------------------------------------------------------------------- void SpaceShower::pT2nextWeak( double pT2begDip, double pT2endDip) { // Type of dipole and starting values. BeamParticle& beam = (sideA) ? *beamAPtr : *beamBPtr; bool isLeptonBeam = beam.isLepton(); bool isValence = beam[iSysNow].isValence(); int MEtype = dipEndNow->MEtype; double pT2 = pT2begDip; double m2Lepton = (isLeptonBeam) ? pow2(beam.m()) : 0.; if (isLeptonBeam && pT2begDip < m2Lepton) return; // alpha_em at maximum scale provides upper estimate. double alphaEMmax = alphaEM.alphaEM(pT2begDip); double alphaEM2pi = alphaEMmax / (2. * M_PI); // Maximum x of mother implies minimum z = xDaughter / xMother. double xMaxAbs = (isLeptonBeam) ? LEPTONXMAX : beam.xMax(iSysNow); double zMinAbs = xDaughter / xMaxAbs; if (xMaxAbs < 0.) { infoPtr->errorMsg("Warning in SpaceShower::pT2nextWeak: " "xMaxAbs negative"); return; } // Maximum z from minimum pT and, for lepton, from minimum x_gamma. double zMaxAbs = 1. - 0.5 * (pT2endDip / m2Dip) * ( sqrt( 1. + 4. * m2Dip / pT2endDip ) - 1. ); if (isLeptonBeam) { double zMaxLepton = xDaughter / (xDaughter + LEPTONXMIN); if (zMaxLepton < zMaxAbs) zMaxAbs = zMaxLepton; } if (zMaxAbs < zMinAbs) return; // Variables used inside evolution loop. (Mainly dummy start values.) int idMother = 0; int idSister = 0; // Check whether emission of W+, W- or Z0. if (dipEndNow->weakType == 1) { idSister = (idDaughter > 0) ? -24 : 24; if (abs(idDaughter) % 2 == 1) idSister = -idSister; } else if (dipEndNow->weakType == 2) idSister = 23; double z = 0.; double xMother = 0.; double wt = 0.; double Q2 = 0.; double mSister = particleDataPtr->mSel(idSister); double m2Sister = pow2(mSister); double pT2corr = 0.; // Maximum z due to massive sister. double mRatio = mSister/ sqrt(m2Dip); double zMaxMassive = 1. / pow2(1. + mRatio); if (zMaxMassive < zMaxAbs) zMaxAbs = zMaxMassive; if (zMaxAbs < zMinAbs) return; // Weak evolution of fermions. // Integrals of splitting kernels for fermions: f -> f. Use 1 + z^2 < 2. // Ansatz f(z) = 2 / (1 - z), with + 2 / (z - xDaughter) for lepton. double f2fInt = 0.; double f2fIntA = 2. * log( (1. - zMinAbs) / (1. - zMaxAbs) ); double f2fIntB = 0.; double zRootMin = (1. + sqrt(zMinAbs)) / (1. - sqrt(zMinAbs)); double zRootMax = (1. + sqrt(zMaxAbs)) / (1. - sqrt(zMaxAbs)); if (isLeptonBeam) { f2fIntB = 2. * log( (zMaxAbs - xDaughter) / (zMinAbs - xDaughter) ); f2fInt = f2fIntA + f2fIntB; } else if (isValence) f2fInt = 2 * log( zRootMax / zRootMin ); else f2fInt = f2fIntA; // Calculating the weak coupling. double weakCoupling = 0; if (dipEndNow->weakType == 1) weakCoupling = 2. * alphaEM2pi / (4. * coupSMPtr->sin2thetaW()); else if (dipEndNow->weakType == 2 && dipEndNow->weakPol == -1) weakCoupling = alphaEM2pi * thetaWRat * pow2(2. * coupSMPtr->lf( abs(idDaughter) )); else weakCoupling = alphaEM2pi * thetaWRat * pow2(2. * coupSMPtr->rf(abs(idDaughter) )); // Find the possible mothers for a W emission. vector possibleMothers; if (abs(idDaughter) % 2 == 0) { possibleMothers.push_back(1); possibleMothers.push_back(3); possibleMothers.push_back(5); } else { possibleMothers.push_back(2); possibleMothers.push_back(4); } if (idDaughter < 0) for (unsigned int i = 0; i < possibleMothers.size(); i++) possibleMothers[i] = - possibleMothers[i]; // Check if daughter estimate is 0, return in that case. // Only write warning if u, d or g is the daughter. if (beam.xfISR(iSysNow, idDaughter, xDaughter, pT2begDip) < TINYPDF) { if (abs(idDaughter) == 1 || abs(idDaughter) == 2 || abs(idDaughter) == 21) infoPtr->errorMsg("Warning in SpaceShower::pT2nextWeak: " "very small PDF"); return; } // PDF and CKM upper estimate needed for W emission. double PDFCKMoverEstimate = 0; if (dipEndNow->weakType == 2) PDFCKMoverEstimate = 1; else if (dipEndNow->weakType == 1) { for (unsigned int i = 0; i < possibleMothers.size(); i++) PDFCKMoverEstimate += coupSMPtr->V2CKMid(idDaughter,possibleMothers[i]) * beam.xfISR(iSysNow, possibleMothers[i], xDaughter, pT2begDip) / beam.xfISR(iSysNow, idDaughter, xDaughter, pT2begDip); } // Upper estimate for evolution equation, including fudge factor. if (doMEcorrections) f2fInt *= calcMEmax(MEtype, 1, 1); double kernelPDF = weakCoupling * f2fInt * weakEnhancement; // PDF and CKM overestimate. kernelPDF *= PDFCKMoverEstimate; double fudge = (isLeptonBeam) ? LEPTONFUDGE * log(m2Dip/m2Lepton) : 1.; kernelPDF *= fudge; if (kernelPDF < TINYKERNELPDF) return; // Begin evolution loop towards smaller pT values. do { // Pick pT2 (in overestimated z range). // For l -> l gamma include extrafactor 1 / ln(pT2 / m2l) in evolution. double shift = pow(rndmPtr->flat(), 1. / kernelPDF); if (isLeptonBeam) pT2 = m2Lepton * pow( pT2 / m2Lepton, shift); else pT2 = pT2 * shift; // Abort evolution if below cutoff scale, or below another branching. if (pT2 < pT2endDip) return; if (isLeptonBeam && pT2 < LEPTONPT2MIN * m2Lepton) return; // Abort evolution if below mass treshold. if (pT2 < HEAVYPT2EVOL * pow2(particleDataPtr->m0(idDaughter))) return; // Set the id for the mother particle to be equal to the daughter // particle. This is correct for Z, and it will later be changed for W. idMother = idDaughter; // Select z value of branching f -> f + Z/W, and corrective weight. wt = 1.0; if (isLeptonBeam) { if (f2fIntA > rndmPtr->flat() * (f2fIntA + f2fIntB)) { z = 1. - (1. - zMinAbs) * pow( (1. - zMaxAbs) / (1. - zMinAbs), rndmPtr->flat() ); } else { z = xDaughter + (zMinAbs - xDaughter) * pow( (zMaxAbs - xDaughter) / (zMinAbs - xDaughter), rndmPtr->flat() ); } wt *= (z - xDaughter) / (1. - xDaughter); } else if (isValence) { // Valence more peaked at large z. double zTmp = zRootMin * pow(zRootMax / zRootMin, rndmPtr->flat() ); z = pow2( (1. - zTmp) / (1. + zTmp) ); wt *= sqrt(z); } else { z = 1. - (1. - zMinAbs) * pow( (1. - zMaxAbs) / (1. - zMinAbs), rndmPtr->flat() ); } wt *= 0.5 * (1. + pow2(z)); // Derive Q2 and x of mother from pT2 and z. Q2 = pT2 / (1. - z); xMother = xDaughter / z; // Correction to x for massive recoiler from rescattering. if (!dipEndNow->normalRecoil) { if (sideA) xMother += (m2Rec / (x2Now * sCM)) * (1. / z - 1.); else xMother += (m2Rec / (x1Now * sCM)) * (1. / z - 1.); } if (xMother > xMaxAbs) { wt = 0.; continue; } // Forbidden emission if outside allowed z range for given pT2. pT2corr = Q2 - z * (m2Dip + Q2) * (Q2 + m2Sister) / m2Dip; if (pT2corr < TINYPT2) { wt = 0.; continue; } // Correct by ln(pT2 / m2l) and fudge factor. if (isLeptonBeam) wt *= log(pT2 / m2Lepton) / fudge; // Evaluation of ME correction. if (doMEcorrections) wt *= calcMEcorr(MEtype, idMother, idDaughter, m2Dip, z, Q2, m2Sister) / calcMEmax(MEtype, idMother, idDaughter); // Optional dampening of large pT values in first radiation. // Allow damping also for corrected matrix elements if (dopTdamp && iSysNow == 0 && nRad == 0) wt *= pT2damp / (pT2 + pT2damp); // Extra dampening of low pT values. if (dopTdampMass) wt *= (pT2 + 0.25 * m2Sister) / (pT2 + 1. * m2Sister); // Correct to current value of alpha_EM. double alphaEMnow = alphaEM.alphaEM(pT2); wt *= (alphaEMnow / alphaEMmax); // Evaluation of new daughter and mother PDF's for Z. if (dipEndNow->weakType == 2) { double xPDFdaughterNew = max ( TINYPDF, beam.xfISR(iSysNow, idDaughter, xDaughter, pT2) ); double xPDFmotherNew = beam.xfISR(iSysNow, idMother, xMother, pT2); wt *= xPDFmotherNew / xPDFdaughterNew; } // Evaluation of daughter and mother PDF's for W. if (dipEndNow->weakType == 1) { double PDFCKMcurrent = 0; for(unsigned int i = 0;i < possibleMothers.size();i++) { PDFCKMcurrent += coupSMPtr->V2CKMid(idDaughter,possibleMothers[i]) * beam.xfISR(iSysNow, possibleMothers[i], xMother, pT2) / beam.xfISR(iSysNow, idDaughter, xDaughter, pT2); } wt *= PDFCKMcurrent / PDFCKMoverEstimate; // Choose id for mother in case of W. double pickIdRndm = PDFCKMcurrent * rndmPtr->flat(); double pickIdSum = 0; for (unsigned int i = 0;i < possibleMothers.size();i++) { pickIdSum += coupSMPtr->V2CKMid(idDaughter,possibleMothers[i]) * beam.xfISR(iSysNow, possibleMothers[i], xMother, pT2) / beam.xfISR(iSysNow, idDaughter, xDaughter, pT2); if (pickIdRndm < pickIdSum) { idMother = possibleMothers[i]; break; } } } if (wt > 1.) { infoPtr->errorMsg("Warning in SpaceShower::pT2nextWeak: " "weight is above unity."); } // Iterate until acceptable pT (or have fallen below pTmin). } while (wt < rndmPtr->flat()) ; // Save values for (so far) acceptable branching. dipEndNow->store( idDaughter, idMother, idSister, x1Now, x2Now, m2Dip, pT2, z, xMother, Q2, mSister, m2Sister, pT2corr); } //-------------------------------------------------------------------------- // Kinematics of branching. // Construct mother -> daughter + sister, with recoiler on other side. bool SpaceShower::branch( Event& event) { // Side on which branching occured. int side = abs(dipEndSel->side); double sideSign = (side == 1) ? 1. : -1.; // Read in flavour and colour variables. int iDaughter = partonSystemsPtr->getInA(iSysSel); int iRecoiler = partonSystemsPtr->getInB(iSysSel); if (side == 2) swap(iDaughter, iRecoiler); int idDaughterNow = dipEndSel->idDaughter; int idMother = dipEndSel->idMother; int idSister = dipEndSel->idSister; int colDaughter = event[iDaughter].col(); int acolDaughter = event[iDaughter].acol(); // Recoil parton may be rescatterer, requiring special processing. bool normalRecoil = dipEndSel->normalRecoil; int iRecoilMother = event[iRecoiler].mother1(); // Read in kinematical variables. double x1 = dipEndSel->x1; double x2 = dipEndSel->x2; double xMo = dipEndSel->xMo; double m2 = dipEndSel->m2Dip; double m = sqrt(m2); double pT2 = dipEndSel->pT2; double z = dipEndSel->z; double Q2 = dipEndSel->Q2; double mSister = dipEndSel->mSister; double m2Sister = dipEndSel->m2Sister; double pT2corr = dipEndSel->pT2corr; double x1New = (side == 1) ? xMo : x1; double x2New = (side == 2) ? xMo : x2; // Rescatter: kinematics may fail; use the rescatterFail flag to tell // parton level to try again. rescatterFail = false; // Construct kinematics of mother, sister and recoiler in old rest frame. // Normally both mother and recoiler are taken massless. double eNewRec, pzNewRec, pTbranch, pzMother; if (normalRecoil) { eNewRec = 0.5 * (m2 + Q2) / m; pzNewRec = -sideSign * eNewRec; pTbranch = sqrt(pT2corr) * m2 / ( z * (m2 + Q2) ); pzMother = sideSign * 0.5 * m * ( (m2 - Q2) / ( z * (m2 + Q2) ) + (Q2 + m2Sister) / m2 ); // More complicated kinematics when recoiler not massless. May fail. } else { m2Rec = event[iRecoiler].m2(); double s1Tmp = m2 + Q2 - m2Rec; double s3Tmp = m2 / z - m2Rec; double r1Tmp = sqrt(s1Tmp * s1Tmp + 4. * Q2 * m2Rec); eNewRec = 0.5 * (m2 + m2Rec + Q2) / m; pzNewRec = -sideSign * 0.5 * r1Tmp / m; double pT2br = Q2 * s3Tmp * (m2 / z - m2 - Q2) - m2Sister * s1Tmp * s3Tmp - m2Rec * pow2(Q2 + m2Sister); if (pT2br <= 0.) return false; pTbranch = sqrt(pT2br) / r1Tmp; pzMother = sideSign * (m * s3Tmp - eNewRec * (m2 / z - Q2 - m2Rec - m2Sister)) / r1Tmp; } // Common final kinematics steps for both normal and rescattering. double eMother = sqrt( pow2(pTbranch) + pow2(pzMother) ); double pzSister = pzMother + pzNewRec; double eSister = sqrt( pow2(pTbranch) + pow2(pzSister) + m2Sister ); Vec4 pMother( pTbranch, 0., pzMother, eMother ); Vec4 pSister( pTbranch, 0., pzSister, eSister ); Vec4 pNewRec( 0., 0., pzNewRec, eNewRec ); // Current event and subsystem size. int eventSizeOld = event.size(); int systemSizeOld = partonSystemsPtr->sizeAll(iSysSel); // Save properties to be restored in case of user-hook veto of emission. int beamOff1 = 1 + beamOffset; int beamOff2 = 2 + beamOffset; int ev1Dau1V = event[beamOff1].daughter1(); int ev2Dau1V = event[beamOff2].daughter1(); vector statusV, mother1V, mother2V, daughter1V, daughter2V; // Check if the first emission shoild be checked for removal bool canMergeFirst = (mergingHooksPtr != 0) ? mergingHooksPtr->canVetoEmission() : false; if (canVetoEmission || canMergeFirst || vetoWeakJets) { for ( int iCopy = 0; iCopy < systemSizeOld; ++iCopy) { int iOldCopy = partonSystemsPtr->getAll(iSysSel, iCopy); statusV.push_back( event[iOldCopy].status()); mother1V.push_back( event[iOldCopy].mother1()); mother2V.push_back( event[iOldCopy].mother2()); daughter1V.push_back( event[iOldCopy].daughter1()); daughter2V.push_back( event[iOldCopy].daughter2()); } } // Take copy of existing system, to be given modified kinematics. // Incoming negative status. Rescattered also negative, but after copy. for ( int iCopy = 0; iCopy < systemSizeOld; ++iCopy) { int iOldCopy = partonSystemsPtr->getAll(iSysSel, iCopy); int statusOld = event[iOldCopy].status(); int statusNew = (iOldCopy == iDaughter || iOldCopy == iRecoiler) ? statusOld : 44; int iNewCopy = event.copy(iOldCopy, statusNew); if (statusOld < 0) event[iNewCopy].statusNeg(); } // Define colour flow in branching. // Default corresponds to f -> f + gamma. int colMother = colDaughter; int acolMother = acolDaughter; int colSister = 0; int acolSister = 0; if (idSister == 22 || idSister == 23 || abs(idSister) == 24) ; // q -> q + g and 50% of g -> g + g; need new colour. else if (idSister == 21 && ( (idMother > 0 && idMother < 9) || (idMother == 21 && rndmPtr->flat() < 0.5) ) ) { colMother = event.nextColTag(); colSister = colMother; acolSister = colDaughter; // qbar -> qbar + g and other 50% of g -> g + g; need new colour. } else if (idSister == 21) { acolMother = event.nextColTag(); acolSister = acolMother; colSister = acolDaughter; // q -> g + q. } else if (idDaughterNow == 21 && idMother > 0) { colMother = colDaughter; acolMother = 0; colSister = acolDaughter; // qbar -> g + qbar } else if (idDaughterNow == 21) { acolMother = acolDaughter; colMother = 0; acolSister = colDaughter; // g -> q + qbar. } else if (idDaughterNow > 0 && idDaughterNow < 9) { acolMother = event.nextColTag(); acolSister = acolMother; // g -> qbar + q. } else if (idDaughterNow < 0 && idDaughterNow > -9) { colMother = event.nextColTag(); colSister = colMother; // q -> gamma + q. } else if (idDaughterNow == 22 && idMother > 0) { colMother = event.nextColTag(); colSister = colMother; // qbar -> gamma + qbar. } else if (idDaughterNow == 22) { acolMother = event.nextColTag(); acolSister = acolMother; } // Indices of partons involved. Add new sister. int iMother = eventSizeOld + side - 1; int iNewRecoiler = eventSizeOld + 2 - side; int iSister = event.append( idSister, 43, iMother, 0, 0, 0, colSister, acolSister, pSister, mSister, sqrt(pT2) ); // References to the partons involved. Particle& daughter = event[iDaughter]; Particle& mother = event[iMother]; Particle& newRecoiler = event[iNewRecoiler]; Particle& sister = event.back(); // Replace old by new mother; update new recoiler. mother.id( idMother ); mother.status( -41); mother.cols( colMother, acolMother); mother.p( pMother); newRecoiler.status( (normalRecoil) ? -42 : -46 ); newRecoiler.p( pNewRec); if (!normalRecoil) newRecoiler.m( event[iRecoiler].m() ); // Update mother and daughter pointers; also for beams. daughter.mothers( iMother, 0); mother.daughters( iSister, iDaughter); if (iSysSel == 0) { event[beamOff1].daughter1( (side == 1) ? iMother : iNewRecoiler ); event[beamOff2].daughter1( (side == 2) ? iMother : iNewRecoiler ); } // Special checks to set weak particles status equal to 47. if (sister.idAbs() == 23 || sister.idAbs() == 24) sister.status(47); // Find boost to old rest frame. RotBstMatrix Mtot; if (normalRecoil) Mtot.bst(0., 0., (x2 - x1) / (x1 + x2) ); else if (side == 1) Mtot.toCMframe( event[iDaughter].p(), event[iRecoiler].p() ); else Mtot.toCMframe( event[iRecoiler].p(), event[iDaughter].p() ); // Initially select phi angle of branching at random. double phi = 2. * M_PI * rndmPtr->flat(); // Evaluate coefficient of azimuthal asymmetry from gluon polarization. findAsymPol( event, dipEndSel); int iFinPol = dipEndSel->iFinPol; double cPol = dipEndSel->asymPol; double phiPol = (iFinPol == 0) ? 0. : event[iFinPol].phi(); // If interference: try to match sister (anti)colour to final state. int iFinInt = 0; double cInt = 0.; double phiInt = 0.; if (doPhiIntAsym) { for (int i = 0; i < partonSystemsPtr->sizeOut(iSysSel); ++ i) { int iOut = partonSystemsPtr->getOut(iSysSel, i); if ( (acolSister != 0 && event[iOut].col() == acolSister) || (colSister != 0 && event[iOut].acol() == colSister) ) iFinInt = iOut; } if (iFinInt != 0) { // Boost final-state parton to current frame of new kinematics. Vec4 pFinTmp = event[iFinInt].p(); pFinTmp.rotbst(Mtot); double theFin = pFinTmp.theta(); if (side == 2) theFin = M_PI - theFin; double theSis = pSister.theta(); if (side == 2) theSis = M_PI - theSis; cInt = strengthIntAsym * 2. * theSis * theFin / (pow2(theSis) + pow2(theFin)); phiInt = event[iFinInt].phi(); } } // Bias phi distribution for polarization and interference. if (iFinPol != 0 || iFinInt != 0) { double cPhiPol, cPhiInt, weight; do { phi = 2. * M_PI * rndmPtr->flat(); weight = 1.; if (iFinPol !=0 ) { cPhiPol = cos(phi - phiPol); weight *= ( 1. + cPol * (2. * pow2(cPhiPol) - 1.) ) / ( 1. + abs(cPol) ); } if (iFinInt !=0 ) { cPhiInt = cos(phi - phiInt); weight *= (1. - cInt) * (1. - cInt * cPhiInt) / (1. + pow2(cInt) - 2. * cInt * cPhiInt); } } while (weight < rndmPtr->flat()); } // Include rotation -phi on boost to old rest frame. Mtot.rot(0., -phi); // Find boost from old rest frame to event cm frame. RotBstMatrix MfromRest; // The boost to the new rest frame. Vec4 sumNew = pMother + pNewRec; double betaX = sumNew.px() / sumNew.e(); double betaZ = sumNew.pz() / sumNew.e(); MfromRest.bst( -betaX, 0., -betaZ); // Alignment of radiator + recoiler to +- z axis, and rotation +phi. // Note: with spacelike (E < 0) recoiler p'_x_mother < 0 can happen! pMother.rotbst(MfromRest); double theta = pMother.theta(); if (pMother.px() < 0.) theta = -theta; if (side == 2) theta += M_PI; MfromRest.rot(-theta, phi); // Boost to radiator + recoiler in event cm frame. if (normalRecoil) { MfromRest.bst( 0., 0., (x1New - x2New) / (x1New + x2New) ); } else if (side == 1) { Vec4 pMotherWanted( 0., 0., 0.5 * eCM * x1New, 0.5 * eCM * x1New); MfromRest.fromCMframe( pMotherWanted, event[iRecoiler].p() ); } else { Vec4 pMotherWanted( 0., 0., -0.5 * eCM * x2New, 0.5 * eCM * x2New); MfromRest.fromCMframe( event[iRecoiler].p(), pMotherWanted ); } Mtot.rotbst(MfromRest); // Perform cumulative rotation/boost operation. // Mother, recoiler and sister from old rest frame to event cm frame. mother.rotbst(MfromRest); newRecoiler.rotbst(MfromRest); sister.rotbst(MfromRest); // The rest from (and to) event cm frame. for ( int i = eventSizeOld + 2; i < eventSizeOld + systemSizeOld; ++i) event[i].rotbst(Mtot); // Check for veto of jets in W/Z production. // (Not applicable for diffractive events; info not set there.) bool isNotDiff = !infoPtr->isDiffractiveA() && !infoPtr->isDiffractiveB() && !infoPtr->isDiffractiveC(); if (vetoWeakJets && isNotDiff && (infoPtr->codeMPI(iSysSel) == 221 || infoPtr->codeMPI(iSysSel) == 222 || infoPtr->codeMPI(iSysSel) == 223)) { if ( (side == 1 && iSysSel < int(nRadA.size()) && nRadA[iSysSel] > 0) || (side == 2 && iSysSel < int(nRadB.size()) && nRadB[iSysSel] > 0) ) { // Find relevant particles to calculate momentum. Vec4 p1 = event[iSister].p(); Vec4 p2; Vec4 p0 = event[iMother].p(); // Find first daughter. int i2 = iDaughter; while (event[i2].statusAbs() == 53 || event[i2].statusAbs() == 42) i2 = event[i2].daughter1(); if (event[event[i2].daughter1()].statusAbs() == 43) p2 = event[event[i2].daughter1()].p(); if (event[event[i2].daughter2()].statusAbs() == 43) p2 = event[event[i2].daughter2()].p(); // Boost to CM frame. Vec4 pSum = p1+p2; p1.bstback(pSum); p2.bstback(pSum); p0.bstback(pSum); // Rotate such that p0 is along z axis. double phiRot = atan2(p0.py(),p0.px()); p0.rot(0, - phiRot); double thetaRot = atan2(p0.px(),p0.pz()); p0.rot(-thetaRot, 0); p1.rot(0, -phiRot); p1.rot(-thetaRot,0); // Do veto if pT above cut-off. if (p1.pT() > vetoWeakJetspTcut) { event.popBack( event.size() - eventSizeOld); event[beamOff1].daughter1( ev1Dau1V); event[beamOff2].daughter1( ev2Dau1V); for ( int iCopy = 0; iCopy < systemSizeOld; ++iCopy) { int iOldCopy = partonSystemsPtr->getAll(iSysSel, iCopy); event[iOldCopy].status( statusV[iCopy]); event[iOldCopy].mothers( mother1V[iCopy], mother2V[iCopy]); event[iOldCopy].daughters( daughter1V[iCopy], daughter2V[iCopy]); } return false; } } } // Allow veto of branching. If so restore event record to before emission. if ( (canVetoEmission && userHooksPtr->doVetoISREmission(eventSizeOld, event, iSysSel)) || (canMergeFirst && mergingHooksPtr->doVetoEmission( event )) ) { event.popBack( event.size() - eventSizeOld); event[beamOff1].daughter1( ev1Dau1V); event[beamOff2].daughter1( ev2Dau1V); for ( int iCopy = 0; iCopy < systemSizeOld; ++iCopy) { int iOldCopy = partonSystemsPtr->getAll(iSysSel, iCopy); event[iOldCopy].status( statusV[iCopy]); event[iOldCopy].mothers( mother1V[iCopy], mother2V[iCopy]); event[iOldCopy].daughters( daughter1V[iCopy], daughter2V[iCopy]); } return false; } // Update list of partons in system; adding newly produced one. partonSystemsPtr->setInA(iSysSel, eventSizeOld); partonSystemsPtr->setInB(iSysSel, eventSizeOld + 1); for (int iCopy = 2; iCopy < systemSizeOld; ++iCopy) partonSystemsPtr->setOut(iSysSel, iCopy - 2, eventSizeOld + iCopy); partonSystemsPtr->addOut(iSysSel, eventSizeOld + systemSizeOld); partonSystemsPtr->setSHat(iSysSel, m2 / z); // Add dipoles for the case that q -> g q, where the daughter is a gluon. if (idDaughter == 21 && idMother != 21) { if (doWeakShower) { int weakPol = (rndmPtr->flat() > 0.5) ? -1 : 1; if ((weakMode == 0 || weakMode == 1) && weakPol == -1) dipEnd.push_back( SpaceDipoleEnd( iSysSel, side, iMother, iNewRecoiler, pT2, 0, 0, 1, 4, normalRecoil, weakPol) ); if (weakMode == 0 || weakMode == 2) dipEnd.push_back( SpaceDipoleEnd( iSysSel, side, iMother, iNewRecoiler, pT2, 0, 0, 2, 4, normalRecoil, weakPol) ); } if (doQEDshowerByQ) dipEnd.push_back( SpaceDipoleEnd( iSysSel, side, iMother, iNewRecoiler, pT2, 0, mother.chargeType(), 0, 4, normalRecoil) ); } // Add dipoles for the case that q -> g gamma, where the daughter is a gamma. if (idDaughter == 22 && idMother != 22) { if (doWeakShower) { int weakPol = (rndmPtr->flat() > 0.5) ? -1 : 1; if ((weakMode == 0 || weakMode == 1) && weakPol == -1) dipEnd.push_back( SpaceDipoleEnd( iSysSel, side, iMother, iNewRecoiler, pT2, 0, 0, 1, 4, normalRecoil, weakPol) ); if (weakMode == 0 || weakMode == 2) dipEnd.push_back( SpaceDipoleEnd( iSysSel, side, iMother, iNewRecoiler, pT2, 0, 0, 2, 4, normalRecoil, weakPol) ); } if (doQCDshower && mother.colType() != 0) dipEnd.push_back( SpaceDipoleEnd( iSysSel, side, iMother, iNewRecoiler, pT2, mother.colType(), 0, 0, 4, normalRecoil) ); if (doQEDshowerByQ && mother.chargeType() != 3) dipEnd.push_back( SpaceDipoleEnd( iSysSel, side, iMother, iNewRecoiler, pT2, 0, mother.chargeType(), 0, 4, normalRecoil) ); if (doQEDshowerByL && mother.chargeType() == 3) dipEnd.push_back( SpaceDipoleEnd( iSysSel, side, iMother, iNewRecoiler, pT2, 0, mother.chargeType(), 0, 4, normalRecoil) ); } // dipEnd array may have expanded and been moved, so regenerate dipEndSel. dipEndSel = &dipEnd[iDipSel]; // Set flag to tell that a weak emission has happened. if (dipEndSel->weakType != 0) hasWeaklyRadiated = true; // Update list of QCD emissions in side A and B in given iSysSel // This is used to veto jets in W/z events. while (iSysSel >= int(nRadA.size()) || iSysSel >= int(nRadB.size())) { nRadA.push_back(0); nRadB.push_back(0); } if (dipEndSel->colType != 0 && side == 1) ++nRadA[iSysSel]; else if (dipEndSel->colType != 0) ++nRadB[iSysSel]; // Update info on radiating dipole ends (QCD, QED or weak). for (int iDip = 0; iDip < int(dipEnd.size()); ++iDip) if ( dipEnd[iDip].system == iSysSel) { if (abs(dipEnd[iDip].side) == side) { dipEnd[iDip].iRadiator = iMother; dipEnd[iDip].iRecoiler = iNewRecoiler; if (dipEnd[iDip].colType != 0) dipEnd[iDip].colType = mother.colType(); else if(dipEnd[iDip].chgType != 0) { dipEnd[iDip].chgType = 0; if ( (mother.isQuark() && doQEDshowerByQ) || (mother.isLepton() && doQEDshowerByL) ) dipEnd[iDip].chgType = mother.chargeType(); } else if(dipEnd[iDip].weakType != 0) { // Kill weak dipole if mother becomes gluon / photon. if (!(mother.isLepton() || mother.isQuark())) dipEnd[iDip].weakType = 0; if (singleWeakEmission && hasWeaklyRadiated) dipEnd[iDip].weakType = 0; } // Kill ME corrections after first emission for everything // but weak showers. if(dipEnd[iDip].weakType == 0) dipEnd[iDip].MEtype = 0; // Update info on recoiling dipole ends (QCD or QED). } else { dipEnd[iDip].iRadiator = iNewRecoiler; dipEnd[iDip].iRecoiler = iMother; // Optionally also kill recoiler ME corrections after first emission. if (!doMEafterFirst && dipEnd[iDip].weakType == 0) dipEnd[iDip].MEtype = 0; // Remove weak dipoles if we only want a single emission. if (dipEnd[iDip].weakType != 0 && singleWeakEmission && hasWeaklyRadiated) dipEnd[iDip].weakType = 0; } } // Set polarisation of mother for weak emissions. if (dipEndSel->weakType != 0) mother.pol(dipEndSel->weakPol); // Update info on beam remnants. BeamParticle& beamNow = (side == 1) ? *beamAPtr : *beamBPtr; double xNew = (side == 1) ? x1New : x2New; beamNow[iSysSel].update( iMother, idMother, xNew); // Redo choice of companion kind whenever new flavour. if (idMother != idDaughterNow) { beamNow.xfISR( iSysSel, idMother, xNew, factorMultFac * pT2); beamNow.pickValSeaComp(); } BeamParticle& beamRec = (side == 1) ? *beamBPtr : *beamAPtr; beamRec[iSysSel].iPos( iNewRecoiler); // Store branching values of current dipole. (For rapidity ordering.) ++dipEndSel->nBranch; dipEndSel->pT2Old = pT2; dipEndSel->zOld = z; // Update history if recoiler rescatters. if (!normalRecoil) event[iRecoilMother].daughters( iNewRecoiler, iNewRecoiler); // Start list of rescatterers that force changed kinematics. vector iRescatterer; for ( int i = 0; i < systemSizeOld - 2; ++i) { int iOutNew = partonSystemsPtr->getOut( iSysSel, i); if (!event[iOutNew].isFinal()) iRescatterer.push_back(iOutNew); } // Start iterate over list of such rescatterers. int iRescNow = -1; while (++iRescNow < int(iRescatterer.size())) { // Identify partons that induce or are affected by rescatter shift. // In following Old is before change of kinematics, New after, // Out scatterer in outstate and In in instate of another system. // Daughter sequence is (iOutOld ->) iOutNew -> iInNew -> iInOld. int iOutNew = iRescatterer[iRescNow]; int iInOld = event[iOutNew].daughter1(); int iSysResc = partonSystemsPtr->getSystemOf(iInOld, true); // Copy incoming partons of rescattered system and hook them up. int iOldA = partonSystemsPtr->getInA(iSysResc); int iOldB = partonSystemsPtr->getInB(iSysResc); bool rescSideA = event[iOldA].isRescatteredIncoming(); int statusNewA = (rescSideA) ? -45 : -42; int statusNewB = (rescSideA) ? -42 : -45; int iNewA = event.copy(iOldA, statusNewA); int iNewB = event.copy(iOldB, statusNewB); // Copy outgoing partons of rescattered system and hook them up. int eventSize = event.size(); int sizeOutAB = partonSystemsPtr->sizeOut(iSysResc); int iOldAB, statusOldAB, iNewAB; for (int iOutAB = 0; iOutAB < sizeOutAB; ++iOutAB) { iOldAB = partonSystemsPtr->getOut(iSysResc, iOutAB); statusOldAB = event[iOldAB].status(); iNewAB = event.copy(iOldAB, 44); // Status could be negative for parton that rescatters in its turn. if (statusOldAB < 0) { event[iNewAB].statusNeg(); iRescatterer.push_back(iNewAB); } } // Hook up new outgoing with new incoming parton. int iInNew = (rescSideA) ? iNewA : iNewB; event[iOutNew].daughters( iInNew, iInNew); event[iInNew].mothers( iOutNew, iOutNew); // Rescale recoiling incoming parton for correct invariant mass. event[iInNew].p( event[iOutNew].p() ); double momFac = (rescSideA) ? event[iInOld].pPos() / event[iInNew].pPos() : event[iInOld].pNeg() / event[iInNew].pNeg(); int iInRec = (rescSideA) ? iNewB : iNewA; // Rescatter: A previous boost may cause the light cone momentum of a // rescattered parton to change sign. If this happens, tell // parton level to try again. if (momFac < 0.0) { infoPtr->errorMsg("Warning in SpaceShower::branch: " "change in lightcone momentum sign; retrying parton level"); rescatterFail = true; return false; } event[iInRec].rescale4( momFac); // Boost outgoing partons to new frame of incoming. RotBstMatrix MmodResc; MmodResc.toCMframe( event[iOldA].p(), event[iOldB].p()); MmodResc.fromCMframe(event[iNewA].p(), event[iNewB].p()); for (int iOutAB = 0; iOutAB < sizeOutAB; ++iOutAB) event[eventSize + iOutAB].rotbst(MmodResc); // Update list of partons in system. partonSystemsPtr->setInA(iSysResc, iNewA); partonSystemsPtr->setInB(iSysResc, iNewB); for (int iCopy = 0; iCopy < sizeOutAB; ++iCopy) partonSystemsPtr->setOut(iSysResc, iCopy, eventSize + iCopy); // Update info on radiating dipole ends (QCD or QED). for (int iDip = 0; iDip < int(dipEnd.size()); ++iDip) if ( dipEnd[iDip].system == iSysResc) { bool sideAnow = (abs(dipEnd[iDip].side) == 1); dipEnd[iDip].iRadiator = (sideAnow) ? iNewA : iNewB; dipEnd[iDip].iRecoiler = (sideAnow) ? iNewB : iNewA; } // Update info on beam remnants. BeamParticle& beamResc = (rescSideA) ? *beamAPtr : *beamBPtr; beamResc[iSysResc].iPos( iInNew); beamResc[iSysResc].p( event[iInNew].p() ); beamResc[iSysResc].scaleX( 1. / momFac ); BeamParticle& beamReco = (rescSideA) ? *beamBPtr : *beamAPtr; beamReco[iSysResc].iPos( iInRec); beamReco[iSysResc].scaleX( momFac); // End iterate over list of rescatterers. } // Check that beam momentum not used up by rescattered-system boosts. if (beamAPtr->xMax(-1) < 0.0 || beamBPtr->xMax(-1) < 0.0) { infoPtr->errorMsg("Warning in SpaceShower::branch: " "used up beam momentum; retrying parton level"); rescatterFail = true; return false; } // Done without any errors. return true; } //-------------------------------------------------------------------------- // Find class of ME correction. int SpaceShower::findMEtype( int iSys, Event& event) { // Default values and no action. int MEtype = 0; if (!doMEcorrections) ; // Identify systems producing a single resonance. else if (partonSystemsPtr->sizeOut( iSys) == 1) { int idIn1 = event[partonSystemsPtr->getInA(iSys)].id(); int idIn2 = event[partonSystemsPtr->getInA(iSys)].id(); int idRes = event[partonSystemsPtr->getOut(iSys, 0)].id(); if (iSys == 0) idResFirst = abs(idRes); if (iSys == 1) idResSecond = abs(idRes); // f + fbar -> vector boson. if ( (idRes == 23 || abs(idRes) == 24 || idRes == 32 || idRes == 33 || abs(idRes) == 34 || abs(idRes) == 41) && abs(idIn1) < 20 && abs(idIn2) < 20 ) MEtype = 1; // g + g, gamma + gamma -> Higgs boson. if ( (idRes == 25 || idRes == 35 || idRes == 36) && ( ( idIn1 == 21 && idIn2 == 21 ) || ( idIn1 == 22 && idIn2 == 22 ) ) ) MEtype = 2; // f + fbar -> Higgs boson. if ( (idRes == 25 || idRes == 35 || idRes == 36) && abs(idIn1) < 20 && abs(idIn2) < 20 ) MEtype = 3; } // Done. return MEtype; } //-------------------------------------------------------------------------- // Provide maximum of expected ME weight; for preweighting of evolution. double SpaceShower::calcMEmax( int MEtype, int idMother, int idDaughterIn) { // Currently only one non-unity case: g(gamma) f -> V f'. if (MEtype == 1 && idMother > 20 && idDaughterIn < 20) return 3.; return 1.; } //-------------------------------------------------------------------------- // Provide actual ME weight for current branching. // Note: currently ME corrections are only allowed for first branching // on each side, so idDaughter is essentially known and checks overkill. double SpaceShower::calcMEcorr(int MEtype, int idMother, int idDaughterIn, double M2, double z, double Q2, double m2Sister) { // Convert to Mandelstam variables. Sometimes may need to swap later. double sH = M2 / z; double tH = -Q2; double uH = Q2 - M2 * (1. - z) / z; int idMabs = abs(idMother); int idDabs = abs(idDaughterIn); // Corrections for f + fbar -> s-channel vector boson. if (MEtype == 1) { if (idMabs < 20 && idDabs < 20) { return (tH*tH + uH*uH + 2. * M2 * sH) / (sH*sH + M2*M2); } else if (idDabs < 20) { // g(gamma) f -> V f': -Q2 = (p_g - p_f')^2 in PS while // tHat = (p_f - p_f')^2 in ME so need to swap tHat <-> uHat. swap( tH, uH); return (sH*sH + uH*uH + 2. * M2 * tH) / (pow2(sH - M2) + M2*M2); } // Corrections for g + g -> Higgs boson. } else if (MEtype == 2) { if (idMabs < 20 && idDabs > 20) { return (sH*sH + uH*uH) / (sH*sH + pow2(sH - M2)); } else if (idDabs > 20) { return 0.5 * (pow4(sH) + pow4(tH) + pow4(uH) + pow4(M2)) / pow2(sH*sH - M2 * (sH - M2)); } // Corrections for f + fbar -> Higgs boson (f = b mainly). } else if (MEtype == 3) { if (idMabs < 20 && idDabs < 20) { // The PS and ME answers agree for f fbar -> H g/gamma. return 1.; } else if (idDabs < 20) { // Need to swap tHat <-> uHat, cf. vector-boson production above. swap( tH, uH); return (sH*sH + uH*uH + 2. * (M2 - uH) * (M2 - sH)) / (pow2(sH - M2) + M2*M2); } // Corrections for f -> f' + W/Z. } else if (MEtype == 4) { // Need to redo calculations of uH since we now emit a massive particle. uH += m2Sister; double wtME = (uH*uH+ tH*tH+ 2* sH * (m2Sister + M2)) / (uH*tH) - M2*m2Sister * (1/(tH*tH) + 1/(uH*uH)); double wtPS = (sH*sH + M2*M2)/(tH*uH) * (tH+uH)/(tH+uH-m2Sister); return wtME / wtPS; } // Default, when no ME correction. return 1.; } //-------------------------------------------------------------------------- // Find coefficient of azimuthal asymmetry from gluon polarization. void SpaceShower::findAsymPol( Event& event, SpaceDipoleEnd* dip) { // Default is no asymmetry. Only gluons are studied. dip->iFinPol = 0; dip->asymPol = 0.; int iRad = dip->iRadiator; if (!doPhiPolAsym || dip->idDaughter != 21) return; // At least two particles in final state, whereof at least one coloured. int systemSizeOut = partonSystemsPtr->sizeOut( iSysSel); if (systemSizeOut < 2) return; bool foundColOut = false; for (int ii = 0; ii < systemSizeOut; ++ii) { int i = partonSystemsPtr->getOut( iSysSel, ii); if (event[i].col() != 0 || event[i].acol() != 0) foundColOut = true; } if (!foundColOut) return; // Check if granddaughter in final state of hard scattering. // (May need to trace across carbon copies to find granddaughters.) // If so, only accept 2 -> 2 scatterings with gg or qq in final state. int iGrandD1 = event[iRad].daughter1(); int iGrandD2 = event[iRad].daughter2(); bool traceCopy = false; do { traceCopy = false; if (iGrandD1 > 0 && iGrandD2 == iGrandD1) { iGrandD1 = event[iGrandD2].daughter1(); iGrandD2 = event[iGrandD2].daughter2(); traceCopy = true; } } while (traceCopy); int statusGrandD1 = event[ iGrandD1 ].statusAbs(); bool isHardProc = (statusGrandD1 == 23 || statusGrandD1 == 33); if (isHardProc) { if (iGrandD2 != iGrandD1 + 1) return; if (event[iGrandD1].isGluon() && event[iGrandD2].isGluon()); else if (event[iGrandD1].isQuark() && event[iGrandD2].isQuark()); else return; } dip->iFinPol = iGrandD1; // Coefficient from gluon production. if (dip->idMother == 21) dip->asymPol = pow2( (1. - dip->z) / (1. - dip->z * (1. - dip->z) ) ); else dip->asymPol = 2. * (1. - dip->z) / (1. + pow2(1. - dip->z) ); // Coefficients from gluon decay. Put z = 1/2 for hard process. double zDau = (isHardProc) ? 0.5 : dip->zOld; if (event[iGrandD1].isGluon()) dip->asymPol *= pow2( (1. - zDau) / (1. - zDau * (1. - zDau) ) ); else dip->asymPol *= -2. * zDau *( 1. - zDau ) / (1. - 2. * zDau * (1. - zDau) ); } //-------------------------------------------------------------------------- // Print the list of dipoles. void SpaceShower::list(ostream& os) const { // Header. os << "\n -------- PYTHIA SpaceShower Dipole Listing -------------- \n" << "\n i syst side rad rec pTmax col chg ME rec \n" << fixed << setprecision(3); // Loop over dipole list and print it. for (int i = 0; i < int(dipEnd.size()); ++i) os << setw(5) << i << setw(6) << dipEnd[i].system << setw(6) << dipEnd[i].side << setw(6) << dipEnd[i].iRadiator << setw(6) << dipEnd[i].iRecoiler << setw(12) << dipEnd[i].pTmax << setw(5) << dipEnd[i].colType << setw(5) << dipEnd[i].chgType << setw(5) << dipEnd[i].MEtype << setw(4) << dipEnd[i].normalRecoil << "\n"; // Done. os << "\n -------- End PYTHIA SpaceShower Dipole Listing ----------" << endl; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaExtraDim.cc0000644000175000017500000032313512217346250016136 0ustar sunsun// SigmaExtraDim.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Author: Stefan Ask for the *LED* routines. // Function definitions (not found in the header) for the // extra-dimensional simulation classes. #include "Pythia8/SigmaExtraDim.h" namespace Pythia8 { //========================================================================== // ampLedS (amplitude) method for LED graviton tree level exchange. // Based on Eq. (8) in JHEP 1105 (2011) 092, arXiv:1101.4919. complex ampLedS(double x, double n, double L, double M) { complex cS(0., 0.); if (n <= 0) return cS; // Constants. double exp1 = n - 2; double exp2 = n + 2; double rC = sqrt(pow(M_PI,n)) * pow(L,exp1) / (GammaReal(n/2.) * pow(M,exp2)); // Base functions, F1 and F2. complex I(0., 1.); if (x < 0) { double sqrX = sqrt(-x); if (int(n) % 2 == 0) { cS = -log(fabs(1 - 1/x)); } else { cS = (2.*atan(sqrX) - M_PI)/sqrX; } } else if ((x > 0) && (x < 1)) { double sqrX = sqrt(x); if (int(n) % 2 == 0) { cS = -log(fabs(1 - 1/x)) - M_PI*I; } else { double rat = (sqrX + 1)/(sqrX - 1); cS = log(fabs(rat))/sqrX - M_PI*I/sqrX; } } else if (x > 1){ double sqrX = sqrt(x); if (int(n) % 2 == 0) { cS = -log(fabs(1 - 1/x)); } else { double rat = (sqrX + 1)/(sqrX - 1); cS = log(fabs(rat))/sqrX; } } // Recursive part. int nL; int nD; if (int(n) % 2 == 0) { nL = int(n/2.); nD = 2; } else { nL = int((n + 1)/2.); nD = 1; } for (int i=1; i G* (excited graviton state). //-------------------------------------------------------------------------- // Initialize process. void Sigma1gg2GravitonStar::initProc() { // Store G* mass and width for propagator. idGstar = 5100039; mRes = particleDataPtr->m0(idGstar); GammaRes = particleDataPtr->mWidth(idGstar); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // SMinBulk = off/on, use universal coupling (kappaMG) // or individual (Gxx) between graviton and SM particles. eDsmbulk = settingsPtr->flag("ExtraDimensionsG*:SMinBulk"); eDvlvl = false; if (eDsmbulk) eDvlvl = settingsPtr->flag("ExtraDimensionsG*:VLVL"); kappaMG = settingsPtr->parm("ExtraDimensionsG*:kappaMG"); for (int i = 0; i < 27; ++i) eDcoupling[i] = 0.; double tmPcoup = settingsPtr->parm("ExtraDimensionsG*:Gqq"); for (int i = 1; i <= 4; ++i) eDcoupling[i] = tmPcoup; eDcoupling[5] = settingsPtr->parm("ExtraDimensionsG*:Gbb"); eDcoupling[6] = settingsPtr->parm("ExtraDimensionsG*:Gtt"); tmPcoup = settingsPtr->parm("ExtraDimensionsG*:Gll"); for (int i = 11; i <= 16; ++i) eDcoupling[i] = tmPcoup; eDcoupling[21] = settingsPtr->parm("ExtraDimensionsG*:Ggg"); eDcoupling[22] = settingsPtr->parm("ExtraDimensionsG*:Ggmgm"); eDcoupling[23] = settingsPtr->parm("ExtraDimensionsG*:GZZ"); eDcoupling[24] = settingsPtr->parm("ExtraDimensionsG*:GWW"); eDcoupling[25] = settingsPtr->parm("ExtraDimensionsG*:Ghh"); // Set pointer to particle properties and decay table. gStarPtr = particleDataPtr->particleDataEntryPtr(idGstar); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1gg2GravitonStar::sigmaKin() { // Incoming width for gluons. double widthIn = mH / (160. * M_PI); // RS graviton coupling if (eDsmbulk) widthIn *= 2. * pow2(eDcoupling[21] * mH); else widthIn *= pow2(kappaMG); // Set up Breit-Wigner. Width out only includes open channels. double sigBW = 5. * M_PI/ ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); double widthOut = gStarPtr->resWidthOpen(idGstar, mH); // Modify cross section in wings of peak. Done. sigma = widthIn * sigBW * widthOut * pow2(sH / m2Res); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1gg2GravitonStar::setIdColAcol() { // Flavours trivial. setId( 21, 21, idGstar); // Colour flow topology. setColAcol( 1, 2, 2, 1, 0, 0); } //-------------------------------------------------------------------------- // Evaluate weight for G* decay angle. // SA: Angle dist. for decay G* -> W/Z/h, based on // Phys.Rev. D65 (2002) 075008, [arXiv:hep-ph/0103308v3] double Sigma1gg2GravitonStar::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // G* should sit in entry 5. if (iResBeg != 5 || iResEnd != 5) return 1.; // Phase space factors. Reconstruct decay angle. double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double betaf = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * betaf); // Default is isotropic decay. double wt = 1.; // Angular weight for g + g -> G* -> f + fbar. if (process[6].idAbs() < 19) { wt = 1. - pow4(cosThe); // Angular weight for g + g -> G* -> g + g or gamma + gamma. } else if (process[6].id() == 21 || process[6].id() == 22) { wt = (1. + 6. * pow2(cosThe) + pow4(cosThe)) / 8.; // Angular weight for g + g -> G* -> Z + Z or W + W. } else if (process[6].id() == 23 || process[6].id() == 24) { double beta2 = pow2(betaf); double cost2 = pow2(cosThe); double cost4 = pow2(cost2); wt = pow2(beta2 - 2.)*(1. - 2.*cost2 + cost4); // Longitudinal W/Z only. if(eDvlvl) { wt /= 4.; // Transverse W/Z contributions as well. } else { double beta4 = pow2(beta2); double beta8 = pow2(beta4); wt += 2.*pow2(beta4 - 1.)*beta4*cost4; wt += 2.*pow2(beta2 - 1.)*(1. - 2.*beta4*cost2 + beta8*cost4); wt += 2.*(1. + 6.*beta4*cost2 + beta8*cost4); wt += 8.*(1. - beta2)*(1. - cost4); wt /= 18.; } // Angular weight for g + g -> G* -> h + h } else if (process[6].id() == 25) { double beta2 = pow2(betaf); double cost2 = pow2(cosThe); double cost4 = pow2(cost2); wt = pow2(beta2 - 2.)*(1. - 2.*cost2 + cost4); wt /= 4.; } // Done. return wt; } //========================================================================== // Sigma1ffbar2GravitonStar class. // Cross section for f fbar -> G* (excited graviton state). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2GravitonStar::initProc() { // Store G* mass and width for propagator. idGstar = 5100039; mRes = particleDataPtr->m0(idGstar); GammaRes = particleDataPtr->mWidth(idGstar); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // SMinBulk = off/on, use universal coupling (kappaMG) // or individual (Gxx) between graviton and SM particles. eDsmbulk = settingsPtr->flag("ExtraDimensionsG*:SMinBulk"); eDvlvl = false; if (eDsmbulk) eDvlvl = settingsPtr->flag("ExtraDimensionsG*:VLVL"); kappaMG = settingsPtr->parm("ExtraDimensionsG*:kappaMG"); for (int i = 0; i < 27; ++i) eDcoupling[i] = 0.; double tmPcoup = settingsPtr->parm("ExtraDimensionsG*:Gqq"); for (int i = 1; i <= 4; ++i) eDcoupling[i] = tmPcoup; eDcoupling[5] = settingsPtr->parm("ExtraDimensionsG*:Gbb"); eDcoupling[6] = settingsPtr->parm("ExtraDimensionsG*:Gtt"); tmPcoup = settingsPtr->parm("ExtraDimensionsG*:Gll"); for (int i = 11; i <= 16; ++i) eDcoupling[i] = tmPcoup; eDcoupling[21] = settingsPtr->parm("ExtraDimensionsG*:Ggg"); eDcoupling[22] = settingsPtr->parm("ExtraDimensionsG*:Ggmgm"); eDcoupling[23] = settingsPtr->parm("ExtraDimensionsG*:GZZ"); eDcoupling[24] = settingsPtr->parm("ExtraDimensionsG*:GWW"); eDcoupling[25] = settingsPtr->parm("ExtraDimensionsG*:Ghh"); // Set pointer to particle properties and decay table. gStarPtr = particleDataPtr->particleDataEntryPtr(idGstar); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1ffbar2GravitonStar::sigmaKin() { // Incoming width for fermions, disregarding colour factor. double widthIn = mH / (80. * M_PI); // Set up Breit-Wigner. Width out only includes open channels. double sigBW = 5. * M_PI/ ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); double widthOut = gStarPtr->resWidthOpen(idGstar, mH); // Modify cross section in wings of peak. Done. sigma0 = widthIn * sigBW * widthOut * pow2(sH / m2Res); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part dependent of incoming flavour. double Sigma1ffbar2GravitonStar::sigmaHat() { double sigma = sigma0; // RS graviton coupling if (eDsmbulk) sigma *= 2. * pow2(eDcoupling[min( abs(id1), 26)] * mH); else sigma *= pow2(kappaMG); // If initial quarks, 1/N_C if (abs(id1) < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2GravitonStar::setIdColAcol() { // Flavours trivial. setId( id1, id2, idGstar); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for G* decay angle. // SA: Angle dist. for decay G* -> W/Z/h, based on // Phys.Rev. D65 (2002) 075008, [arXiv:hep-ph/0103308v3] double Sigma1ffbar2GravitonStar::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // G* should sit in entry 5. if (iResBeg != 5 || iResEnd != 5) return 1.; // Phase space factors. Reconstruct decay angle. double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double betaf = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * betaf); // Default is isotropic decay. double wt = 1.; // Angular weight for f + fbar -> G* -> f + fbar. if (process[6].idAbs() < 19) { wt = (1. - 3. * pow2(cosThe) + 4. * pow4(cosThe)) / 2.; // Angular weight for f + fbar -> G* -> g + g or gamma + gamma. } else if (process[6].id() == 21 || process[6].id() == 22) { wt = 1. - pow4(cosThe); // Angular weight for f + fbar -> G* -> Z + Z or W + W. } else if (process[6].id() == 23 || process[6].id() == 24) { double beta2 = pow2(betaf); double cost2 = pow2(cosThe); double cost4 = pow2(cost2); wt = pow2(beta2 - 2.)*cost2*(1. - cost2); // Longitudinal W/Z only. if (eDvlvl) { wt /= 4.; // Transverse W/Z contributions as well. } else { wt += pow2(beta2 - 1.)*cost2*(1. - cost2); wt += 2.*(1. - cost4); wt += (1. - beta2)*(1. - 3.*cost2 + 4.*cost4); wt /= 8.; } // Angular weight for f + fbar -> G* -> h + h } else if (process[6].id() == 25) { double beta2 = pow2(betaf); double cost2 = pow2(cosThe); wt = pow2(beta2 - 2.)*cost2*(1. - cost2); wt /= 4.; } // Done. return wt; } //========================================================================== // Sigma1qqbar2KKgluonStar class. // Cross section for q qbar -> g^*/KK-gluon^* (excited KK-gluon state). //-------------------------------------------------------------------------- // Initialize process. void Sigma1qqbar2KKgluonStar::initProc() { // Store kk-gluon* mass and width for propagator. idKKgluon = 5100021; mRes = particleDataPtr->m0(idKKgluon); GammaRes = particleDataPtr->mWidth(idKKgluon); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // KK-gluon gv/ga couplings and interference. for (int i = 0; i < 10; ++i) { eDgv[i] = 0.; eDga[i] = 0.; } double tmPgL = settingsPtr->parm("ExtraDimensionsG*:KKgqL"); double tmPgR = settingsPtr->parm("ExtraDimensionsG*:KKgqR"); for (int i = 1; i <= 4; ++i) { eDgv[i] = 0.5 * (tmPgL + tmPgR); eDga[i] = 0.5 * (tmPgL - tmPgR); } tmPgL = settingsPtr->parm("ExtraDimensionsG*:KKgbL"); tmPgR = settingsPtr->parm("ExtraDimensionsG*:KKgbR"); eDgv[5] = 0.5 * (tmPgL + tmPgR); eDga[5] = 0.5 * (tmPgL - tmPgR); tmPgL = settingsPtr->parm("ExtraDimensionsG*:KKgtL"); tmPgR = settingsPtr->parm("ExtraDimensionsG*:KKgtR"); eDgv[6] = 0.5 * (tmPgL + tmPgR); eDga[6] = 0.5 * (tmPgL - tmPgR); interfMode = settingsPtr->mode("ExtraDimensionsG*:KKintMode"); // Set pointer to particle properties and decay table. gStarPtr = particleDataPtr->particleDataEntryPtr(idKKgluon); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1qqbar2KKgluonStar::sigmaKin() { // Incoming width for fermions. double widthIn = alpS * mH * 4 / 27; double widthOut = alpS * mH / 6; // Loop over all decay channels. sumSM = 0.; sumInt = 0.; sumKK = 0.; for (int i = 0; i < gStarPtr->sizeChannels(); ++i) { int idAbs = abs( gStarPtr->channel(i).product(0) ); // Only contributions quarks. if ( idAbs > 0 && idAbs <= 6 ) { double mf = particleDataPtr->m0(idAbs); // Check that above threshold. Phase space. if (mH > 2. * mf + MASSMARGIN) { double mr = pow2(mf / mH); double beta = sqrtpos(1. - 4. * mr); // Store sum of combinations. For outstate only open channels. int onMode = gStarPtr->channel(i).onMode(); if (onMode == 1 || onMode == 2) { sumSM += beta * (1. + 2. * mr); sumInt += beta * eDgv[min(idAbs, 9)] * (1. + 2. * mr); sumKK += beta * (pow2(eDgv[min(idAbs, 9)]) * (1. + 2.*mr) + pow2(eDga[min(idAbs, 9)]) * (1. - 4.*mr)); } } } } // Set up Breit-Wigner. Width out only includes open channels. sigSM = widthIn * 12. * M_PI * widthOut / sH2; sigInt = 2. * sigSM * sH * (sH - m2Res) / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); sigKK = sigSM * sH2 / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); // Optionally only keep g* or gKK term. if (interfMode == 1) {sigInt = 0.; sigKK = 0.;} if (interfMode == 2) {sigSM = 0.; sigInt = 0.;} } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part dependent of incoming flavour. double Sigma1qqbar2KKgluonStar::sigmaHat() { // RS graviton coupling. double sigma = sigSM * sumSM + eDgv[min(abs(id1), 9)] * sigInt * sumInt + ( pow2(eDgv[min(abs(id1), 9)]) + pow2(eDga[min(abs(id1), 9)]) ) * sigKK * sumKK; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1qqbar2KKgluonStar::setIdColAcol() { // Flavours trivial. setId( id1, id2, idKKgluon); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 1, 2); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for KK-gluon* decay angle (based on ffbar2gmZ). double Sigma1qqbar2KKgluonStar::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // g* should sit in entry 5. if (iResBeg != 5 || iResEnd != 5) return 1.; // Couplings for in- and out-flavours (alpS already included). int idInAbs = process[3].idAbs(); double vi = eDgv[min(idInAbs, 9)]; double ai = eDga[min(idInAbs, 9)]; int idOutAbs = process[6].idAbs(); double vf = eDgv[min(idOutAbs, 9)]; double af = eDga[min(idOutAbs, 9)]; // Phase space factors. (One power of beta left out in formulae.) double mf = process[6].m(); double mr = mf*mf / sH; double betaf = sqrtpos(1. - 4. * mr); // Coefficients of angular expression. double coefTran = sigSM + vi * sigInt * vf + (vi*vi + ai*ai) * sigKK * (vf*vf + pow2(betaf) * af*af); double coefLong = 4. * mr * ( sigSM + vi * sigInt * vf + (vi*vi + ai*ai) * sigKK * vf*vf ); double coefAsym = betaf * ( ai * sigInt * af + 4. * vi * ai * sigKK * vf * af ); // Flip asymmetry for in-fermion + out-antifermion. if (process[3].id() * process[6].id() < 0) coefAsym = -coefAsym; // Reconstruct decay angle and weight for it. double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * betaf); double wtMax = 2. * (coefTran + abs(coefAsym)); double wt = coefTran * (1. + pow2(cosThe)) + coefLong * (1. - pow2(cosThe)) + 2. * coefAsym * cosThe; // Done. return (wt / wtMax); } //========================================================================== // Sigma2gg2GravitonStarg class. // Cross section for g g -> G* g (excited graviton state). //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2GravitonStarg::initProc() { // Store G* mass and width for propagator. idGstar = 5100039; mRes = particleDataPtr->m0(idGstar); GammaRes = particleDataPtr->mWidth(idGstar); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Overall coupling strength kappa * m_G*. kappaMG = settingsPtr->parm("ExtraDimensionsG*:kappaMG"); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(idGstar); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2gg2GravitonStarg::sigmaKin() { // Evaluate cross section. Secondary width for G*. sigma = (3. * pow2(kappaMG) * alpS) / (32. * sH * s3) * ( pow2(tH2 + tH * uH + uH2) / (sH2 * tH * uH) + 2. * (tH2 / uH + uH2 / tH) / sH + 3. * (tH / uH + uH / tH) + 2. * (sH / uH + sH/tH) + sH2 / (tH * uH) ); sigma *= openFrac; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2GravitonStarg::setIdColAcol() { // Flavours trivial. setId( 21, 21, idGstar, 21); // Colour flow topologies: random choice between two mirrors. if (rndmPtr->flat() < 0.5) setColAcol( 1, 2, 2, 3, 0, 0, 1, 3); else setColAcol( 1, 2, 3, 1, 0, 0, 3, 2); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles: currently G* assumed isotropic. double Sigma2gg2GravitonStarg::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // No equations for G* decay so assume isotropic. return 1.; } //========================================================================== // Sigma2qg2GravitonStarq class. // Cross section for q g -> G* q (excited graviton state). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2GravitonStarq::initProc() { // Store G* mass and width for propagator. idGstar = 5100039; mRes = particleDataPtr->m0(idGstar); GammaRes = particleDataPtr->mWidth(idGstar); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Overall coupling strength kappa * m_G*. kappaMG = settingsPtr->parm("ExtraDimensionsG*:kappaMG"); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(idGstar); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2qg2GravitonStarq::sigmaKin() { // Evaluate cross section. Secondary width for G*. sigma = -(pow2(kappaMG) * alpS) / (192. * sH * s3) * ( 4. * (sH2 + uH2) / (tH * sH) + 9. * (sH + uH) / sH + sH / uH + uH2 / sH2 + 3. * tH * (4. + sH / uH + uH / sH) / sH + 4. * tH2 * (1. / uH + 1. / sH) / sH + 2. * tH2 * tH / (uH * sH2) ); sigma *= openFrac; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2GravitonStarq::setIdColAcol() { // Flavour set up for q g -> H q. int idq = (id2 == 21) ? id1 : id2; setId( id1, id2, idGstar, idq); // tH defined between f and f': must swap tHat <-> uHat if q g in. swapTU = (id2 == 21); // Colour flow topologies. Swap when antiquarks. if (id2 == 21) setColAcol( 1, 0, 2, 1, 0, 0, 2, 0); else setColAcol( 2, 1, 1, 0, 0, 0, 2, 0); if (idq < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles: currently G* assumed isotropic. double Sigma2qg2GravitonStarq::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // No equations for G* decay so assume isotropic. return 1.; } //========================================================================== // Sigma2qqbar2GravitonStarg class. // Cross section for q qbar -> G* g (excited graviton state). //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2GravitonStarg::initProc() { // Store G* mass and width for propagator. idGstar = 5100039; mRes = particleDataPtr->m0(idGstar); GammaRes = particleDataPtr->mWidth(idGstar); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Overall coupling strength kappa * m_G*. kappaMG = settingsPtr->parm("ExtraDimensionsG*:kappaMG"); // Secondary open width fraction. openFrac = particleDataPtr->resOpenFrac(idGstar); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma2qqbar2GravitonStarg::sigmaKin() { // Evaluate cross section. Secondary width for G*. sigma = (pow2(kappaMG) * alpS) / (72. * sH * s3) * ( 4. * (tH2 + uH2) / sH2 + 9. * (tH + uH) / sH + (tH2 / uH + uH2 / tH) / sH + 3. * (4. + tH / uH + uH/ tH) + 4. * (sH / uH + sH / tH) + 2. * sH2 / (tH * uH) ); sigma *= openFrac; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2GravitonStarg::setIdColAcol() { // Flavours trivial. setId( id1, id2, idGstar, 21); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 0, 0, 1, 2); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles: currently G* assumed isotropic. double Sigma2qqbar2GravitonStarg::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // No equations for G* decay so assume isotropic. return 1.; } //========================================================================== // NOAM: Sigma2ffbar2TEVffbar class. // Cross section for, f fbar -> gammaKK/ZKK -> F Fbar. // Process provided by N. Hod et al. and is described in arXiv:XXXX.YYYY //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2TEVffbar::initProc() { // Process name. if (idNew == 1) nameSave = "f fbar -> d dbar (s-channel gamma_KK/Z_KK)"; if (idNew == 2) nameSave = "f fbar -> u ubar (s-channel gamma_KK/Z_KK)"; if (idNew == 3) nameSave = "f fbar -> s sbar (s-channel gamma_KK/Z_KK)"; if (idNew == 4) nameSave = "f fbar -> c cbar (s-channel gamma_KK/Z_KK)"; if (idNew == 5) nameSave = "f fbar -> b bbar (s-channel gamma_KK/Z_KK)"; if (idNew == 6) nameSave = "f fbar -> t tbar (s-channel gamma_KK/Z_KK)"; if (idNew == 11) nameSave = "f fbar -> e+ e- (s-channel gamma_KK/Z_KK)"; if (idNew == 12) nameSave = "f fbar -> nue nuebar (s-channel gamma_KK/Z_KK)"; if (idNew == 13) nameSave = "f fbar -> mu+ mu- (s-channel gamma_KK/Z_KK)"; if (idNew == 14) nameSave = "f fbar -> numu numubar (s-channel gamma_KK/Z_KK)"; if (idNew == 15) nameSave = "f fbar -> tau+ tau- (s-channel gamma_KK/Z_KK)"; if (idNew == 16) nameSave = "f fbar -> nutau nutaubar (s-channel gamma_KK/Z_KK)"; // Allow to pick only gamma* or Z0 part of full gamma*/Z0 expression. gmZmode = settingsPtr->mode("ExtraDimensionsTEV:gmZmode"); // Pick number of KK excitations nexcitationmax = (int)settingsPtr->parm("ExtraDimensionsTEV:nMax"); // Initialize the widths of the KK propogators. // partial width of the KK photon wgmKKFactor = 0.; // total width of the KK photon wgmKKn = 0.; // will be proportional to "wZ0" + ttbar addition wZKKn = 0.; // Store Z0 mass and width for propagator. wZ0 = particleDataPtr->mWidth(23); mRes = particleDataPtr->m0(23); m2Res = mRes*mRes; // Store the top mass for the ttbar width calculations mTop = particleDataPtr->m0(6); m2Top = mTop*mTop; // Store the KK mass parameter, equivalent to the mass of the first KK // excitation: particleDataPtr->m0(5000023); mStar = (double)settingsPtr->parm("ExtraDimensionsTEV:mStar"); // Get alphaEM - relevant for the calculation of the widths alphaemfixed = settingsPtr->parm("StandardModel:alphaEM0"); // initialize imaginari number mI = complex(0.,1.); // Sum all partial widths of the KK photon except for the ttbar channel // which is handeled afterwards seperately if (gmZmode>=0 && gmZmode<=5) { for (int i=1 ; i<17 ; i++) { if (i==7) { i=11; } // skip the ttbar decay and add its contribution later if (i==6) { continue; } if (i<9) { wgmKKFactor += ( (alphaemfixed / 6.) * 4. * couplingsPtr->ef(i) * couplingsPtr->ef(i) * 3. ); } else { wgmKKFactor += (alphaemfixed / 6.) * 4. * couplingsPtr->ef(i) * couplingsPtr->ef(i); } } } // Get the helicity-couplings of the Z0 to all the fermions except top gMinusF = ( couplingsPtr->t3f(idNew) - couplingsPtr->ef(idNew) * couplingsPtr->sin2thetaW() ) / sqrt( couplingsPtr->sin2thetaW()*couplingsPtr->cos2thetaW() ); gPlusF = -1. * couplingsPtr->ef(idNew) * couplingsPtr->sin2thetaW() / sqrt( couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW() ); // Get the helicity-couplings of the Z0 to the top quark gMinusTop = ( couplingsPtr->t3f(6) - couplingsPtr->ef(6) * couplingsPtr->sin2thetaW() ) / sqrt( couplingsPtr->sin2thetaW()*couplingsPtr->cos2thetaW() ); gPlusTop = -1. * couplingsPtr->ef(6) * couplingsPtr->sin2thetaW() / sqrt( couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW() ); // calculate the constant factor of the unique ttbar decay width ttbarwFactorA = pow2(gMinusTop) + pow2(gPlusTop); ttbarwFactorB = 6.*gMinusTop*gPlusTop - pow2(gMinusTop) - pow2(gPlusTop); // Secondary open width fraction, relevant for top (or heavier). openFracPair = 1.; if ((idNew >=6 && idNew <=8) || idNew == 17 || idNew == 18) openFracPair = particleDataPtr->resOpenFrac(idNew, -idNew); } //-------------------------------------------------------------------------- // For improving the phase-space sampling (there can be 2 resonances) int Sigma2ffbar2TEVffbar::resonanceB() { return 23; } //-------------------------------------------------------------------------- // For improving the phase-space sampling (there can be 2 resonances) int Sigma2ffbar2TEVffbar::resonanceA() { if (gmZmode>=3) { phaseSpacemHatMin = settingsPtr->parm("PhaseSpace:mHatMin"); phaseSpacemHatMax = settingsPtr->parm("PhaseSpace:mHatMax"); double mResFirstKKMode = sqrt(pow2(particleDataPtr->m0(23)) + pow2(mStar)); if (mResFirstKKMode/2. <= phaseSpacemHatMax || 3*mResFirstKKMode/2. >= phaseSpacemHatMin) { return 5000023; } else { return 23; } // no KK terms at all } else { return 23; } } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2ffbar2TEVffbar::sigmaKin() { // Check that above threshold. isPhysical = true; if (mH < m3 + m4 + MASSMARGIN) { isPhysical = false; return; } // Define average F, Fbar mass so same beta. Phase space. double s34Avg = 0.5 * (s3 + s4) - 0.25 * pow2(s3 - s4) / sH; mr = s34Avg / sH; betaf = sqrtpos(1. - 4. * mr); // Reconstruct decay angle so can reuse 2 -> 1 cross section. cosThe = (tH - uH) / (betaf * sH); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2ffbar2TEVffbar::sigmaHat() { // Fail if below threshold. if (!isPhysical) return 0.; // Couplings for in/out-flavours. int idAbs = abs(id1); // The couplings of the Z0 to the fermions for in/out flavors gMinusf = ( couplingsPtr->t3f(idAbs) - couplingsPtr->ef(idAbs) * couplingsPtr->sin2thetaW() ) / sqrt( couplingsPtr->sin2thetaW()*couplingsPtr->cos2thetaW() ); gPlusf = -1. * couplingsPtr->ef(idAbs)*couplingsPtr->sin2thetaW() / sqrt( couplingsPtr->sin2thetaW()*couplingsPtr->cos2thetaW() ); // Initialize the some values helicityME2 = 0.; coefAngular = 0.; gf=0.; gF=0.; gammaProp = complex(0.,0.); resProp = complex(0.,0.); gmPropKK = complex(0.,0.); ZPropKK = complex(0.,0.); totalProp = complex(0.,0.); // Sum all initial and final helicity states this corresponds to an // unpolarized beams and unmeasured polarization final-state for (double helicityf=-0.5 ; helicityf<=0.5 ; helicityf++) { for (double helicityF=-0.5 ; helicityF<=0.5 ; helicityF++) { // the couplings for the initial-final helicity configuration gF = (helicityF == +0.5) ? gMinusF : gPlusF; gf = (helicityf == +0.5) ? gMinusf : gPlusf; // 0=SM gmZ, 1=SM gm, 2=SM Z, 3=SM+KK gmZ, 4=KK gm, 5=KK Z switch(gmZmode) { // SM photon and Z0 only case 0: gammaProp = couplingsPtr->ef(idAbs)*couplingsPtr->ef(idNew)/sH; resProp = gf*gF/( sH - m2Res + mI*sH*(wZ0/mRes) ); break; // SM photon only case 1: gammaProp = couplingsPtr->ef(idAbs)*couplingsPtr->ef(idNew)/sH; break; // SM Z0 only case 2: resProp = gf*gF/( sH - m2Res + mI*sH*(wZ0/mRes) ); break; // KK photon and Z case 3: gammaProp = couplingsPtr->ef(idAbs)*couplingsPtr->ef(idNew)/sH; resProp = gf*gF/( sH - m2Res + mI*sH*(wZ0/mRes) ); ZPropKK = complex(0.,0.); gmPropKK = complex(0.,0.); // Sum all KK excitations contributions for(int nexcitation = 1; nexcitation <= nexcitationmax; nexcitation++) { mZKKn = sqrt(m2Res + pow2(mStar * nexcitation)); m2ZKKn = m2Res + pow2(mStar * nexcitation); mgmKKn = mStar * nexcitation; m2gmKKn = (mStar*nexcitation)*(mStar*nexcitation); // calculate the width of the n'th excitation of the KK Z // (proportional to the Z0 width + ttbar partial width) ttbarwZKKn = 2.*(alphaemfixed*3./6.)*mZKKn * sqrt(1.-4.*m2Top/m2ZKKn) * (ttbarwFactorA+(m2Top/m2ZKKn)*ttbarwFactorB); wZKKn = 2.*wZ0*mZKKn/mRes+ttbarwZKKn; // calculate the width of the n'th excitation of the // KK photon ttbarwgmKKn = 2.*(alphaemfixed*3./6.)*mgmKKn * sqrt(1.-4.*m2Top/m2gmKKn) * 2.*pow2(couplingsPtr->ef(6))*(1.+2.*(m2Top/m2gmKKn)); wgmKKn = wgmKKFactor*mgmKKn+ttbarwgmKKn; // the propogators gmPropKK += (2.*couplingsPtr->ef(idAbs)*couplingsPtr->ef(idNew)) / (sH-m2gmKKn+mI*sH*wgmKKn/mgmKKn); ZPropKK += (2.*gf*gF)/(sH-m2ZKKn+mI*sH*wZKKn/mZKKn ); } break; // SM photon and Z0 with KK photon only case 4: gammaProp = couplingsPtr->ef(idAbs)*couplingsPtr->ef(idNew)/sH; resProp = gf*gF/( sH - m2Res + mI*sH*(wZ0/mRes) ); gmPropKK = complex(0.,0.); for (int nexcitation = 1; nexcitation <= nexcitationmax; nexcitation++ ) { mgmKKn = mStar * nexcitation; m2gmKKn = (mStar*nexcitation)*(mStar*nexcitation); ttbarwgmKKn = 2.*(alphaemfixed*3./6.)*mgmKKn * sqrt(1.-4.*m2Top/m2gmKKn) * 2.*pow2(couplingsPtr->ef(6)) * (1.+2.*(m2Top/m2gmKKn)); wgmKKn = wgmKKFactor*mgmKKn+ttbarwgmKKn; gmPropKK += (2.*couplingsPtr->ef(idAbs)*couplingsPtr->ef(idNew)) / (sH-m2gmKKn+mI*sH*wgmKKn/mgmKKn); } break; // SM photon and Z0 with KK Z only case 5: gammaProp = couplingsPtr->ef(idAbs)*couplingsPtr->ef(idNew)/sH; resProp = gf*gF/( sH - m2Res + mI*sH*(wZ0/mRes) ); ZPropKK = complex(0.,0.); for (int nexcitation = 1; nexcitation <= nexcitationmax; nexcitation++ ) { mZKKn = sqrt(m2Res + pow2(mStar * nexcitation)); m2ZKKn = m2Res + pow2(mStar * nexcitation); ttbarwZKKn = 2.*(alphaemfixed*3./6.)*mZKKn * sqrt(1.-4.*m2Top/m2ZKKn) * (ttbarwFactorA+(m2Top/m2ZKKn)*ttbarwFactorB); wZKKn = 2.*wZ0*mZKKn/mRes+ttbarwZKKn; ZPropKK += (2.*gf*gF)/(sH-m2ZKKn+mI*sH*wZKKn/mZKKn ); } break; default: break; // end run over initial and final helicity states } // sum all contributing amplitudes totalProp = gammaProp + resProp + ZPropKK + gmPropKK; // angular distribution for the helicity configuration coefAngular = 1. + 4. * helicityF * helicityf * cosThe; // the squared helicity matrix element helicityME2 += real(totalProp*conj(totalProp))*pow2(coefAngular); } } // calculate the coefficient of the squared helicity matrix element. coefTot = (2./sH) * 2*M_PI * pow2(alpEM)/(4.*sH) * pow2(sH)/4.; // the full squared helicity matrix element. double sigma = helicityME2 * coefTot; // Top: corrections for closed decay channels. sigma *= openFracPair; // Initial-state colour factor. Answer. if (idAbs < 9) sigma /= 3.; // Final-state colour factor. Answer. if (idNew < 9) sigma *= 3.*(1.+alpS/M_PI); return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2TEVffbar::setIdColAcol() { // Set outgoing flavours. id3 = (id1 > 0) ? idNew : -idNew; setId( id1, id2, id3, -id3); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9 && idNew < 9) setColAcol( 1, 0, 0, 1, 2, 0, 0, 2); else if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else if (idNew < 9) setColAcol( 0, 0, 0, 0, 1, 0, 0, 1); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles of W in top decay. double Sigma2ffbar2TEVffbar::weightDecay( Event& process, int iResBeg, int iResEnd) { // For top decay hand over to standard routine, else done. if (idNew == 6 && process[process[iResBeg].mother1()].idAbs() == 6) return weightTopDecay( process, iResBeg, iResEnd); else return 1.; } //========================================================================== // Sigma2gg2LEDUnparticleg class. // Cross section for g g -> U/G g (real graviton emission in // large extra dimensions or unparticle emission). //-------------------------------------------------------------------------- void Sigma2gg2LEDUnparticleg::initProc() { // Init model parameters. eDidG = 5000039; if (eDgraviton) { eDspin = (settingsPtr->flag("ExtraDimensionsLED:GravScalar")) ? 0 : 2; eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDdU = 0.5 * eDnGrav + 1; eDLambdaU = settingsPtr->parm("ExtraDimensionsLED:MD"); eDlambda = 1; eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); eDcf = settingsPtr->parm("ExtraDimensionsLED:c"); } else { eDspin = settingsPtr->mode("ExtraDimensionsUnpart:spinU"); eDdU = settingsPtr->parm("ExtraDimensionsUnpart:dU"); eDLambdaU = settingsPtr->parm("ExtraDimensionsUnpart:LambdaU"); eDlambda = settingsPtr->parm("ExtraDimensionsUnpart:lambda"); eDcutoff = settingsPtr->mode("ExtraDimensionsUnpart:CutOffMode"); } // The A(dU) or S'(n) value. double tmpAdU = 0; if (eDgraviton) { tmpAdU = 2 * M_PI * sqrt( pow(M_PI, double(eDnGrav)) ) / GammaReal(0.5 * eDnGrav); if (eDspin == 0) { // Scalar graviton tmpAdU *= sqrt( pow(2., double(eDnGrav)) ); eDcf *= eDcf; } } else { tmpAdU = 16 * pow2(M_PI) * sqrt(M_PI) / pow(2. * M_PI, 2. * eDdU) * GammaReal(eDdU + 0.5) / (GammaReal(eDdU - 1.) * GammaReal(2. * eDdU)); } // Cross section related constants // and ME dependent powers of lambda / LambdaU. double tmpExp = eDdU - 2; double tmpLS = pow2(eDLambdaU); eDconstantTerm = tmpAdU / (2 * 16 * pow2(M_PI) * tmpLS * pow(tmpLS,tmpExp)); if (eDgraviton) { eDconstantTerm /= tmpLS; } else if (eDspin == 0) { eDconstantTerm *= pow2(eDlambda) / tmpLS; } else { eDconstantTerm = 0; infoPtr->errorMsg("Error in Sigma2gg2LEDUnparticleg::initProc: " "Incorrect spin value (turn process off)!"); } } //-------------------------------------------------------------------------- void Sigma2gg2LEDUnparticleg::sigmaKin() { // Set graviton mass. mG = m3; mGS = mG*mG; // Set mandelstam variables and ME expressions. if (eDgraviton) { double A0 = 1/sH; if (eDspin == 0) { // Scalar graviton double tmpTerm1 = uH + tH; double tmpTerm2 = uH + sH; double tmpTerm3 = tH + sH; double T0 = pow(tmpTerm1,4) + pow(tmpTerm2,4) + pow(tmpTerm3,4) + 12. * sH * tH * uH * mGS; eDsigma0 = eDcf * A0 * T0 / (sH2 * tH * uH); } else { double xH = tH/sH; double yH = mGS/sH; double xHS = pow2(xH); double yHS = pow2(yH); double xHC = pow(xH,3); double yHC = pow(yH,3); double xHQ = pow(xH,4); double yHQ = pow(yH,4); double T0 = 1/(xH*(yH-1-xH)); double T1 = 1 + 2*xH + 3*xHS + 2*xHC + xHQ; double T2 = -2*yH*(1 + xHC); double T3 = 3*yHS*(1 + xHS); double T4 = -2*yHC*(1 + xH); double T5 = yHQ; eDsigma0 = A0 * T0 *( T1 + T2 + T3 + T4 + T5 ); } } else if (eDspin == 0) { double A0 = 1/pow2(sH); double sHQ = pow(sH,4); double tHQ = pow(tH,4); double uHQ = pow(uH,4); eDsigma0 = A0 * (pow(mGS,4) + sHQ + tHQ + uHQ) / (sH * tH * uH); } // Mass measure, (m^2)^(d-2). double tmpExp = eDdU - 2; eDsigma0 *= pow(mGS, tmpExp); // Constants. eDsigma0 *= eDconstantTerm; } //-------------------------------------------------------------------------- double Sigma2gg2LEDUnparticleg::sigmaHat() { // Mass spectrum weighting. double sigma = eDsigma0 / runBW3; // SM couplings... if (eDgraviton) { sigma *= 16 * M_PI * alpS * 3 / 16; } else if (eDspin == 0) { sigma *= 6 * M_PI * alpS; } // Truncate sH region or use form factor. // Form factor uses either pythia8 renormScale2 // or E_jet in cms. if (eDcutoff == 1) { if (sH > pow2(eDLambdaU) ) { sigma *= pow(eDLambdaU,4)/pow2(sH); } } else if ( (eDgraviton && (eDspin == 2)) && ((eDcutoff == 2) || (eDcutoff == 3)) ) { double tmPmu = sqrt(Q2RenSave); if (eDcutoff == 3) tmPmu = (sH + s4 - s3) / (2 * mH); double tmPformfact = tmPmu / (eDtff * eDLambdaU); double tmPexp = double(eDnGrav) + 2; sigma *= 1 / (1 + pow(tmPformfact, tmPexp)); } return sigma; } //-------------------------------------------------------------------------- void Sigma2gg2LEDUnparticleg::setIdColAcol() { // Flavours trivial. setId( 21, 21, eDidG, 21); // Colour flow topologies: random choice between two mirrors. if (rndmPtr->flat() < 0.5) setColAcol( 1, 2, 2, 3, 0, 0, 1, 3); else setColAcol( 1, 2, 3, 1, 0, 0, 3, 2); } //========================================================================== // Sigma2qg2LEDUnparticleq class. // Cross section for q g -> U/G q (real graviton emission in // large extra dimensions or unparticle emission). //-------------------------------------------------------------------------- void Sigma2qg2LEDUnparticleq::initProc() { // Init model parameters. eDidG = 5000039; if (eDgraviton) { eDspin = (settingsPtr->flag("ExtraDimensionsLED:GravScalar")) ? 0 : 2; eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDdU = 0.5 * eDnGrav + 1; eDLambdaU = settingsPtr->parm("ExtraDimensionsLED:MD"); eDlambda = 1; eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); eDgf = settingsPtr->parm("ExtraDimensionsLED:g"); eDcf = settingsPtr->parm("ExtraDimensionsLED:c"); } else { eDspin = settingsPtr->mode("ExtraDimensionsUnpart:spinU"); eDdU = settingsPtr->parm("ExtraDimensionsUnpart:dU"); eDLambdaU = settingsPtr->parm("ExtraDimensionsUnpart:LambdaU"); eDlambda = settingsPtr->parm("ExtraDimensionsUnpart:lambda"); eDcutoff = settingsPtr->mode("ExtraDimensionsUnpart:CutOffMode"); } // The A(dU) or S'(n) value. double tmpAdU = 0; if (eDgraviton) { tmpAdU = 2 * M_PI * sqrt( pow(M_PI, double(eDnGrav)) ) / GammaReal(0.5 * eDnGrav); // Scalar graviton if (eDspin == 0) { tmpAdU *= 2. * sqrt( pow(2., double(eDnGrav)) ); eDcf *= 4. * eDcf / pow2(eDLambdaU); double tmpExp = 2. * double(eDnGrav) / (double(eDnGrav) + 2.); eDgf *= eDgf / pow(2. * M_PI, tmpExp); } } else { tmpAdU = 16 * pow2(M_PI) * sqrt(M_PI) / pow(2. * M_PI, 2. * eDdU) * GammaReal(eDdU + 0.5) / (GammaReal(eDdU - 1.) * GammaReal(2. * eDdU)); } // Cross section related constants // and ME dependent powers of lambda / LambdaU. double tmpExp = eDdU - 2; double tmpLS = pow2(eDLambdaU); eDconstantTerm = tmpAdU / (2 * 16 * pow2(M_PI) * tmpLS * pow(tmpLS,tmpExp)); if (eDgraviton && (eDspin == 2)) { eDconstantTerm /= tmpLS; } else if (eDspin == 1) { eDconstantTerm *= pow2(eDlambda); } else if (eDspin == 0) { eDconstantTerm *= pow2(eDlambda); } else { eDconstantTerm = 0; infoPtr->errorMsg("Error in Sigma2qg2LEDUnparticleq::initProc: " "Incorrect spin value (turn process off)!"); } } //-------------------------------------------------------------------------- void Sigma2qg2LEDUnparticleq::sigmaKin() { // Set graviton mass. mG = m3; mGS = mG*mG; // Set mandelstam variables and ME expressions. if (eDgraviton) { double A0 = 1/sH; // Scalar graviton if (eDspin == 0) { A0 /= sH; double T0 = -(uH2 + pow2(mGS)) / (sH * tH); double T1 = -(tH2 + sH2)/ uH; eDsigma0 = A0 * (eDgf * T0 + eDcf * T1); } else { double xH = tH/sH; double yH = mGS/sH; double x2H = xH/(yH - 1 - xH); double y2H = yH/(yH - 1 - xH); double x2HS = pow2(x2H); double y2HS = pow2(y2H); double x2HC = pow(x2H,3); double y2HC = pow(y2H,3); double T0 = -(yH - 1 - xH); double T20 = 1/(x2H*(y2H-1-x2H)); double T21 = -4*x2H*(1 + x2H)*(1 + 2*x2H + 2*x2HS); double T22 = y2H*(1 + 6*x2H + 18*x2HS + 16*x2HC); double T23 = -6*y2HS*x2H*(1+2*x2H); double T24 = y2HC*(1 + 4*x2H); eDsigma0 = A0 * T0 * T20 * ( T21 + T22 + T23 + T24 ); } } else if (eDspin == 1) { double A0 = 1/pow2(sH); double tmpTerm1 = tH - mGS; double tmpTerm2 = sH - mGS; eDsigma0 = A0 * (pow2(tmpTerm1) + pow2(tmpTerm2)) / (sH*tH); } else if (eDspin == 0) { double A0 = 1/pow2(sH); // Sign correction by Tom eDsigma0 = A0 * (pow2(tH) + pow2(mGS)) / (sH*uH); } // Mass measure, (m^2)^(d-2). double tmpExp = eDdU - 2; eDsigma0 *= pow(mGS, tmpExp); // Constants. eDsigma0 *= eDconstantTerm; } //-------------------------------------------------------------------------- double Sigma2qg2LEDUnparticleq::sigmaHat() { // Mass spactrum weighting. double sigma = eDsigma0 /runBW3; // SM couplings... if (eDgraviton) { sigma *= 16 * M_PI * alpS / 96; } else if (eDspin == 1) { sigma *= - 4 * M_PI * alpS / 3; } else if (eDspin == 0) { sigma *= - 2 * M_PI * alpS / 3; } // Truncate sH region or use form factor. // Form factor uses either pythia8 renormScale2 // or E_jet in cms. if (eDcutoff == 1) { if (sH > pow2(eDLambdaU) ) { sigma *= pow(eDLambdaU,4)/pow2(sH); } } else if ( (eDgraviton && (eDspin == 2)) && ((eDcutoff == 2) || (eDcutoff == 3)) ) { double tmPmu = sqrt(Q2RenSave); if (eDcutoff == 3) tmPmu = (sH + s4 - s3) / (2 * mH); double tmPformfact = tmPmu / (eDtff * eDLambdaU); double tmPexp = double(eDnGrav) + 2; sigma *= 1 / (1 + pow(tmPformfact, tmPexp)); } return sigma; } //-------------------------------------------------------------------------- void Sigma2qg2LEDUnparticleq::setIdColAcol() { // Flavour set up for q g -> G* q. int idq = (id2 == 21) ? id1 : id2; setId( id1, id2, eDidG, idq); // tH defined between f and f': must swap tHat <-> uHat if q g in. swapTU = (id2 == 21); // Colour flow topologies. Swap when antiquarks. if (id2 == 21) setColAcol( 1, 0, 2, 1, 0, 0, 2, 0); else setColAcol( 2, 1, 1, 0, 0, 0, 2, 0); if (idq < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2LEDUnparticleg class. // Cross section for q qbar -> U/G g (real graviton emission in // large extra dimensions or unparticle emission). //-------------------------------------------------------------------------- void Sigma2qqbar2LEDUnparticleg::initProc() { // Init model parameters. eDidG = 5000039; if (eDgraviton) { eDspin = (settingsPtr->flag("ExtraDimensionsLED:GravScalar")) ? 0 : 2; eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDdU = 0.5 * eDnGrav + 1; eDLambdaU = settingsPtr->parm("ExtraDimensionsLED:MD"); eDlambda = 1; eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); eDgf = settingsPtr->parm("ExtraDimensionsLED:g"); eDcf = settingsPtr->parm("ExtraDimensionsLED:c"); } else { eDspin = settingsPtr->mode("ExtraDimensionsUnpart:spinU"); eDdU = settingsPtr->parm("ExtraDimensionsUnpart:dU"); eDLambdaU = settingsPtr->parm("ExtraDimensionsUnpart:LambdaU"); eDlambda = settingsPtr->parm("ExtraDimensionsUnpart:lambda"); eDcutoff = settingsPtr->mode("ExtraDimensionsUnpart:CutOffMode"); } // The A(dU) or S'(n) value. double tmpAdU = 0; if (eDgraviton) { tmpAdU = 2 * M_PI * sqrt( pow(M_PI, double(eDnGrav)) ) / GammaReal(0.5 * eDnGrav); // Scalar graviton if (eDspin == 0) { tmpAdU *= 2. * sqrt( pow(2., double(eDnGrav)) ); eDcf *= 4. * eDcf / pow2(eDLambdaU); double tmpExp = 2. * double(eDnGrav) / (double(eDnGrav) + 2.); eDgf *= eDgf / pow(2. * M_PI, tmpExp); } } else { tmpAdU = 16 * pow2(M_PI) * sqrt(M_PI) / pow(2. * M_PI, 2. * eDdU) * GammaReal(eDdU + 0.5) / (GammaReal(eDdU - 1.) * GammaReal(2. * eDdU)); } // Cross section related constants // and ME dependent powers of lambda / LambdaU. double tmpExp = eDdU - 2; double tmpLS = pow2(eDLambdaU); eDconstantTerm = tmpAdU / (2 * 16 * pow2(M_PI) * tmpLS * pow(tmpLS,tmpExp)); if (eDgraviton && (eDspin == 2)) { eDconstantTerm /= tmpLS; } else if (eDspin == 1) { eDconstantTerm *= pow2(eDlambda); } else if (eDspin == 0) { eDconstantTerm *= pow2(eDlambda); } else { eDconstantTerm = 0; infoPtr->errorMsg("Error in Sigma2qqbar2LEDUnparticleg::initProc: " "Incorrect spin value (turn process off)!"); } } //-------------------------------------------------------------------------- void Sigma2qqbar2LEDUnparticleg::sigmaKin() { // Set graviton mass. mG = m3; mGS = mG*mG; // Set mandelstam variables and ME expressions. if (eDgraviton) { double A0 = 1/sH; // Scalar graviton if (eDspin == 0) { A0 /= sH; double tmpTerm1 = uH + tH; double T0 = (2. * mGS * sH + pow2(tmpTerm1)) / (uH * tH); double T1 = (tH2 + uH2) / sH; eDsigma0 = A0 * (eDgf * T0 + eDcf * T1); } else { double xH = tH/sH; double yH = mGS/sH; double xHS = pow2(xH); double yHS = pow2(yH); double xHC = pow(xH,3); double yHC = pow(yH,3); double T0 = 1/(xH*(yH-1-xH)); double T1 = -4*xH*(1 + xH)*(1 + 2*xH + 2*xHS); double T2 = yH*(1 + 6*xH + 18*xHS + 16*xHC); double T3 = -6*yHS*xH*(1+2*xH); double T4 = yHC*(1 + 4*xH); eDsigma0 = A0 * T0 *( T1 + T2 + T3 + T4 ); } } else if (eDspin == 1) { double A0 = 1/pow2(sH); double tmpTerm1 = tH - mGS; double tmpTerm2 = uH - mGS; eDsigma0 = A0 * (pow2(tmpTerm1) + pow2(tmpTerm2)) / (tH * uH); } else if (eDspin == 0) { double A0 = 1/pow2(sH); eDsigma0 = A0 * (pow2(sH) - pow2(mGS)) / (tH * uH); } // Mass measure, (m^2)^(d-2). double tmpExp = eDdU - 2; eDsigma0 *= pow(mGS, tmpExp); // Constants. eDsigma0 *= eDconstantTerm; } //-------------------------------------------------------------------------- double Sigma2qqbar2LEDUnparticleg::sigmaHat() { // Mass spactrum weighting. double sigma = eDsigma0 /runBW3; // SM couplings... if (eDgraviton) { sigma *= 16 * M_PI * alpS / 36; } else if (eDspin == 1) { sigma *= 4 * M_PI * 8 * alpS / 9; } else if (eDspin == 0) { sigma *= 4 * M_PI * 4 * alpS / 9; } // Truncate sH region or use form factor. // Form factor uses either pythia8 renormScale2 // or E_jet in cms. if (eDcutoff == 1) { if (sH > pow2(eDLambdaU) ) { sigma *= pow(eDLambdaU,4)/pow2(sH); } } else if ( (eDgraviton && (eDspin == 2)) && ((eDcutoff == 2) || (eDcutoff == 3)) ) { double tmPmu = sqrt(Q2RenSave); if (eDcutoff == 3) tmPmu = (sH + s4 - s3) / (2 * mH); double tmPformfact = tmPmu / (eDtff * eDLambdaU); double tmPexp = double(eDnGrav) + 2; sigma *= 1 / (1 + pow(tmPformfact, tmPexp)); } return sigma; } //-------------------------------------------------------------------------- void Sigma2qqbar2LEDUnparticleg::setIdColAcol() { // Flavours trivial. setId( id1, id2, eDidG, 21); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 2, 0, 0, 1, 2); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2ffbar2LEDUnparticleZ class. // Cross section for f fbar -> U/G Z (real LED graviton or unparticle // emission). //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // FIXRATIO: // Ratio between the two possible coupling constants of the spin-2 ME. // A value different from one give rise to an IR divergence which makes // the event generation very slow, so this values is fixed to 1 until // investigated further. const double Sigma2ffbar2LEDUnparticleZ::FIXRATIO = 1.; //-------------------------------------------------------------------------- void Sigma2ffbar2LEDUnparticleZ::initProc() { // Init model parameters. eDidG = 5000039; if (eDgraviton) { eDspin = 2; eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDdU = 0.5 * eDnGrav + 1; eDLambdaU = settingsPtr->parm("ExtraDimensionsLED:MD"); eDlambda = 1; eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } else { eDspin = settingsPtr->mode("ExtraDimensionsUnpart:spinU"); eDdU = settingsPtr->parm("ExtraDimensionsUnpart:dU"); eDLambdaU = settingsPtr->parm("ExtraDimensionsUnpart:LambdaU"); eDlambda = settingsPtr->parm("ExtraDimensionsUnpart:lambda"); eDratio = FIXRATIO; // = settingsPtr->parm("ExtraDimensionsUnpart:ratio"); eDcutoff = settingsPtr->mode("ExtraDimensionsUnpart:CutOffMode"); } // Store Z0 mass and width for propagator. mZ = particleDataPtr->m0(23); widZ = particleDataPtr->mWidth(23); mZS = mZ*mZ; mwZS = pow2(mZ * widZ); // Init spin-2 parameters if ( eDspin != 2 ){ eDgraviton = false; eDlambdaPrime = 0; } else if (eDgraviton) { eDlambda = 1; eDratio = 1; eDlambdaPrime = eDlambda; } else { eDlambdaPrime = eDratio * eDlambda; } // The A(dU) or S'(n) value double tmpAdU = 16 * pow2(M_PI) * sqrt(M_PI) / pow(2. * M_PI, 2. * eDdU) * GammaReal(eDdU + 0.5) / (GammaReal(eDdU - 1.) * GammaReal(2. * eDdU)); if (eDgraviton) { tmpAdU = 2 * M_PI * sqrt( pow(M_PI, double(eDnGrav)) ) / GammaReal(0.5 * eDnGrav); } // Standard 2 to 2 cross section related constants double tmpTerm1 = 1/(2 * 16 * pow2(M_PI)); double tmpLS = pow2(eDLambdaU); // Spin dependent constants from ME. double tmpTerm2 = 0; if ( eDspin == 0 ) { tmpTerm2 = 2 * pow2(eDlambda); } else if (eDspin == 1) { tmpTerm2 = 4 * pow2(eDlambda); } else if (eDspin == 2) { tmpTerm2 = pow2(eDlambda)/(4 * 3 * tmpLS); } // Unparticle phase space related double tmpExp2 = eDdU - 2; double tmpTerm3 = tmpAdU / (tmpLS * pow(tmpLS, tmpExp2)); // All in total eDconstantTerm = tmpTerm1 * tmpTerm2 * tmpTerm3; } //-------------------------------------------------------------------------- void Sigma2ffbar2LEDUnparticleZ::sigmaKin() { // Set graviton mass and some powers of mandelstam variables mU = m3; mUS = mU*mU; sHS = pow2(sH); tHS = pow2(tH); uHS = pow2(uH); tHC = pow(tH,3); uHC = pow(uH,3); tHQ = pow(tH,4); uHQ = pow(uH,4); tHuH = tH+uH; // Evaluate (m**2, t, u) part of differential cross section. // Extra 1/sHS comes from standard 2 to 2 cross section // phase space factors. if ( eDspin == 0 ) { double A0 = 1/sHS; double T1 = - sH/tH - sH/uH; double T2 = - (1 - mZS/tH)*(1 - mUS/tH); double T3 = - (1 - mZS/uH)*(1 - mUS/uH); double T4 = 2*(1 - mUS/tH)*(1 - mUS/uH); eDsigma0 = A0 * ( T1 + T2 + T3 + T4); } else if ( eDspin == 1 ) { double A0 = 1/sHS; double T1 = 0.5 * (tH/uH + uH/tH); double T2 = pow2(mZS + mUS)/(tH * uH); double T3 = - 0.5 * mUS * (mZS/tHS + mZS/uHS) ; double T4 = - (mZS+mUS)*(1/tH + 1/uH); eDsigma0 = A0 * ( T1 + T2 + T3 + T4 ); } else if ( eDspin == 2 ) { double A0 = 1 / ( sHS * uHS * tHS * pow2(sH-mZS) ); double F0 = 2*tHS*uHS*( 16*pow(mZS,3) + mUS*(7*tHS + 12*tH*uH + 7*uHS) - 3*(3*tHC + 11*tHS*uH + 11*tH*uHS + 3*uHC) + 6*pow(mZS,2)*(7*mUS - 2*tHuH) + mZS*(14*pow(mUS,2) - 15*tHS - 44*tH*uH - 15*uHS + 2*mUS*tHuH) ); double F2 = 2*tHS*uHS*tHuH*( -8*pow(mZS,2)*tHuH + 4*mZS*(tHS + 3*tH*uH + uHS) + 3*(tHC + 5*tHS*uH + 5*tH*uHS + uHC) ); double F4 = -2*tHS*uHS*pow(tHuH,3)*(tHS + uHS - mZS*tHuH); double G0 = 4*tH*uH*( 6*pow(mZS,3)*(mUS - tH - uH)*tHuH + pow(mZS,2)*( 9*tHC + 7*tHS*uH + 7*tH*uHS + 9*uHC + 15*pow2(mUS)*tHuH - 2*mUS*(12*tHS + 19*tH*uH + 12*uHS) ) + tH*uH*( 6*pow(mUS,3) - 9*pow(mUS,2)*tHuH - mUS*(tHS + 12*tH*uH + uHS) + 6*(tHC + 6*tHS*uH + 6*tH*uHS + uHC) ) + mZS*(-3*tHQ + 25*tHC*uH + 58*tHS*uHS + 25*tH*uHC - 3*uHQ + 6*pow(mUS,3)*tHuH - pow(mUS,2)*(15*tHS + 2*tH*uH + 15*uHS) + 2*mUS*(6*tHC - 11*tHS*uH - 11*tH*uHS + 6*uHC)) ); double G2 = -4*tHS*uHS*tHuH*( -10*pow2(mZS)*tHuH + 2*mZS*(3*tHS + 7*tH*uH + 3*uHS) + 3*(tHC + 5*tHS*uH + 5*tH*uHS + uHC) ); double G4 = -2*F4; double H0 = 24*pow(mZS,3)*tH*uH*pow2(-mUS + tHuH) - 6*pow(mZS,2)*tH*uH*( -9*pow(mUS,3) + 24*pow(mUS,2)*tHuH - mUS*(21*tHS + 38*tH*uH + 21*uHS) + 2*(3*tHC + 5*tHS*uH + 5*tH*uHS + 3*uHC) ) - mZS*( 3*pow(mUS,4)*(tHS - 12*tH*uH + uHS) - 2*tH*uH*pow2(tHuH)*(6*tHS - 29*tH*uH + 6*uHS) - 6*pow(mUS,3)*(tHC - 16*tHS*uH - 16*tH*uHS + uHC) + 54*mUS*tH*uH*(tHC + tHS*uH + tH*uHS + uHC) + pow2(mUS)*(3*tHQ - 102*tHC*uH - 166*tHS*uHS - 102*tH*uHC + 3*uHQ) ) + tH*uH*( 6*pow(mUS,5) - 18*pow(mUS,4)*tHuH - 12*pow(mUS,2)*pow(tHuH,3) + 3*pow(mUS,3)*(7*tHS + 12*tH*uH + 7*uHS) - 18*tH*uH*(tHC + 5*tHS*uH + 5*tH*uHS + uHC) + mUS*(3*tHQ + 32*tHC*uH + 78*tHS*uHS + 32*tH*uHC + 3*uHQ) ); double H2 = 2*tHS*uHS*pow2(tHuH)*( -12*pow2(mZS) + 8*mZS*tHuH + 3*(tHS + 4*tH*uH + uHS) ); double H4 = F4; eDsigma0 = A0*( F0 + 1/mUS*F2 + 1/pow2(mUS)*F4 + eDratio*(G0 + 1/mUS*G2 + 1/pow2(mUS)*G4) + pow2(eDratio)*(H0 + 1/mUS*H2 + 1/pow2(mUS)*H4) ); } else { eDsigma0 = 0; } } //-------------------------------------------------------------------------- double Sigma2ffbar2LEDUnparticleZ::sigmaHat() { // Electroweak couplings. int idAbs = abs(id1); // Note: 1/2 * (g_L^2 + g_R^2) = (g_v^2 + g_a^2) double facEWS = 4 * M_PI * alpEM / (couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()) * ( 0.25 * 0.25 * couplingsPtr->vf2af2(idAbs) ); // Mass Spectrum, (m^2)^(d-2) double tmpExp = eDdU - 2; double facSpect = pow(mUS, tmpExp); // Total cross section double sigma = eDconstantTerm * facEWS * facSpect * eDsigma0; // If f fbar are quarks (1/N_c) if (idAbs < 9) sigma /= 3.; // Related to mass spactrum weighting. sigma /= runBW3; // Truncate sH region or use form factor. // Form factor uses either pythia8 renormScale2 // or E_jet in cms. if (eDcutoff == 1) { if (sH > pow2(eDLambdaU) ) { sigma *= pow(eDLambdaU,4)/pow2(sH); } } else if (eDgraviton && ((eDcutoff == 2) || (eDcutoff == 3))) { double tmPmu = sqrt(Q2RenSave); if (eDcutoff == 3) tmPmu = (sH + s4 - s3) / (2 * mH); double tmPformfact = tmPmu / (eDtff * eDLambdaU); double tmPexp = double(eDnGrav) + 2; sigma *= 1 / (1 + pow(tmPformfact, tmPexp)); } return sigma; } //-------------------------------------------------------------------------- void Sigma2ffbar2LEDUnparticleZ::setIdColAcol() { // Flavours trivial. setId( id1, id2, eDidG, 23); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2ffbar2LEDUnparticlegamma class. // Cross section for f fbar -> U/G gamma (real LED graviton or unparticle // emission). //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // FIXRATIO: // Ratio between the two possible coupling constants of the spin-2 ME. // A value different from one give rise to an IR divergence which makes // the event generation very slow, so this values is fixed to 1 until // investigated further. const double Sigma2ffbar2LEDUnparticlegamma::FIXRATIO = 1.; //-------------------------------------------------------------------------- void Sigma2ffbar2LEDUnparticlegamma::initProc() { // WARNING: Keep in mind that this class uses the photon limit // of the Z+G/U ME code. This might give rise to some // confusing things, e.g. mZ = particleDataPtr->m0(22); // Init model parameters. eDidG = 5000039; if (eDgraviton) { eDspin = 2; eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDdU = 0.5 * eDnGrav + 1; eDLambdaU = settingsPtr->parm("ExtraDimensionsLED:MD"); eDlambda = 1; eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } else { eDspin = settingsPtr->mode("ExtraDimensionsUnpart:spinU"); eDdU = settingsPtr->parm("ExtraDimensionsUnpart:dU"); eDLambdaU = settingsPtr->parm("ExtraDimensionsUnpart:LambdaU"); eDlambda = settingsPtr->parm("ExtraDimensionsUnpart:lambda"); eDratio = FIXRATIO; // = settingsPtr->parm("ExtraDimensionsUnpart:ratio"); eDcutoff = settingsPtr->mode("ExtraDimensionsUnpart:CutOffMode"); } // Store Z0 mass. mZ = particleDataPtr->m0(22); mZS = mZ*mZ; // Init spin-2 parameters if ( eDspin != 2 ){ eDgraviton = false; eDlambdaPrime = 0; } else if (eDgraviton) { eDlambda = 1; eDratio = 1; eDlambdaPrime = eDlambda; } else { eDlambdaPrime = eDratio * eDlambda; } // The A(dU) or S'(n) value double tmpAdU = 16 * pow2(M_PI) * sqrt(M_PI) / pow(2. * M_PI, 2. * eDdU) * GammaReal(eDdU + 0.5) / (GammaReal(eDdU - 1.) * GammaReal(2. * eDdU)); if (eDgraviton) { tmpAdU = 2 * M_PI * sqrt( pow(M_PI, double(eDnGrav)) ) / GammaReal(0.5 * eDnGrav); } // Standard 2 to 2 cross section related constants double tmpTerm1 = 1/(2 * 16 * pow2(M_PI)); double tmpLS = pow2(eDLambdaU); // Spin dependent constants from ME. double tmpTerm2 = 0; if ( eDspin == 0 ) { tmpTerm2 = 2 * pow2(eDlambda); } else if (eDspin == 1) { tmpTerm2 = 4 * pow2(eDlambda); } else if (eDspin == 2) { tmpTerm2 = pow2(eDlambda)/(4 * 3 * tmpLS); } // Unparticle phase space related double tmpExp2 = eDdU - 2; double tmpTerm3 = tmpAdU / (tmpLS * pow(tmpLS, tmpExp2)); // All in total eDconstantTerm = tmpTerm1 * tmpTerm2 * tmpTerm3; } //-------------------------------------------------------------------------- void Sigma2ffbar2LEDUnparticlegamma::sigmaKin() { // Set graviton mass and some powers of mandelstam variables mU = m3; mUS = mU*mU; sHS = pow2(sH); tHS = pow2(tH); uHS = pow2(uH); tHC = pow(tH,3); uHC = pow(uH,3); tHQ = pow(tH,4); uHQ = pow(uH,4); tHuH = tH+uH; // Evaluate (m**2, t, u) part of differential cross section. // Extra 1/sHS comes from standard 2 to 2 cross section // phase space factors. if ( eDspin == 0 ) { double A0 = 1/sHS; double T1 = - sH/tH - sH/uH; double T2 = - (1 - mZS/tH)*(1 - mUS/tH); double T3 = - (1 - mZS/uH)*(1 - mUS/uH); double T4 = 2*(1 - mUS/tH)*(1 - mUS/uH); eDsigma0 = A0 * ( T1 + T2 + T3 + T4); } else if ( eDspin == 1 ) { double A0 = 1/sHS; double T1 = 0.5 * (tH/uH + uH/tH); double T2 = pow2(mZS + mUS)/(tH * uH); double T3 = - 0.5 * mUS * (mZS/tHS + mZS/uHS) ; double T4 = - (mZS+mUS)*(1/tH + 1/uH); eDsigma0 = A0 * ( T1 + T2 + T3 + T4 ); } else if ( eDspin == 2 ) { double A0 = 1 / ( sHS * uHS * tHS * pow2(sH-mZS) ); double F0 = 2*tHS*uHS*( 16*pow(mZS,3) + mUS*(7*tHS + 12*tH*uH + 7*uHS) - 3*(3*tHC + 11*tHS*uH + 11*tH*uHS + 3*uHC) + 6*pow(mZS,2)*(7*mUS - 2*tHuH) + mZS*(14*pow(mUS,2) - 15*tHS - 44*tH*uH - 15*uHS + 2*mUS*tHuH) ); double F2 = 2*tHS*uHS*tHuH*( -8*pow(mZS,2)*tHuH + 4*mZS*(tHS + 3*tH*uH + uHS) + 3*(tHC + 5*tHS*uH + 5*tH*uHS + uHC) ); double F4 = -2*tHS*uHS*pow(tHuH,3)*(tHS + uHS - mZS*tHuH); double G0 = 4*tH*uH*( 6*pow(mZS,3)*(mUS - tH - uH)*tHuH + pow(mZS,2)*( 9*tHC + 7*tHS*uH + 7*tH*uHS + 9*uHC + 15*pow2(mUS)*tHuH - 2*mUS*(12*tHS + 19*tH*uH + 12*uHS) ) + tH*uH*( 6*pow(mUS,3) - 9*pow(mUS,2)*tHuH - mUS*(tHS + 12*tH*uH + uHS) + 6*(tHC + 6*tHS*uH + 6*tH*uHS + uHC) ) + mZS*(-3*tHQ + 25*tHC*uH + 58*tHS*uHS + 25*tH*uHC - 3*uHQ + 6*pow(mUS,3)*tHuH - pow(mUS,2)*(15*tHS + 2*tH*uH + 15*uHS) + 2*mUS*(6*tHC - 11*tHS*uH - 11*tH*uHS + 6*uHC)) ); double G2 = -4*tHS*uHS*tHuH*( -10*pow2(mZS)*tHuH + 2*mZS*(3*tHS + 7*tH*uH + 3*uHS) + 3*(tHC + 5*tHS*uH + 5*tH*uHS + uHC) ); double G4 = -2*F4; double H0 = 24*pow(mZS,3)*tH*uH*pow2(-mUS + tHuH) - 6*pow(mZS,2)*tH*uH*( -9*pow(mUS,3) + 24*pow(mUS,2)*tHuH - mUS*(21*tHS + 38*tH*uH + 21*uHS) + 2*(3*tHC + 5*tHS*uH + 5*tH*uHS + 3*uHC) ) - mZS*( 3*pow(mUS,4)*(tHS - 12*tH*uH + uHS) - 2*tH*uH*pow2(tHuH)*(6*tHS - 29*tH*uH + 6*uHS) - 6*pow(mUS,3)*(tHC - 16*tHS*uH - 16*tH*uHS + uHC) + 54*mUS*tH*uH*(tHC + tHS*uH + tH*uHS + uHC) + pow2(mUS)*(3*tHQ - 102*tHC*uH - 166*tHS*uHS - 102*tH*uHC + 3*uHQ) ) + tH*uH*( 6*pow(mUS,5) - 18*pow(mUS,4)*tHuH - 12*pow(mUS,2)*pow(tHuH,3) + 3*pow(mUS,3)*(7*tHS + 12*tH*uH + 7*uHS) - 18*tH*uH*(tHC + 5*tHS*uH + 5*tH*uHS + uHC) + mUS*(3*tHQ + 32*tHC*uH + 78*tHS*uHS + 32*tH*uHC + 3*uHQ) ); double H2 = 2*tHS*uHS*pow2(tHuH)*( -12*pow2(mZS) + 8*mZS*tHuH + 3*(tHS + 4*tH*uH + uHS) ); double H4 = F4; eDsigma0 = A0*( F0 + 1/mUS*F2 + 1/pow2(mUS)*F4 + eDratio*(G0 + 1/mUS*G2 + 1/pow2(mUS)*G4) + pow2(eDratio)*(H0 + 1/mUS*H2 + 1/pow2(mUS)*H4) ); } else { eDsigma0 = 0; } } //-------------------------------------------------------------------------- double Sigma2ffbar2LEDUnparticlegamma::sigmaHat() { // Electroweak couplings.. int idAbs = abs(id1); double facEWS = 4 * M_PI * alpEM * couplingsPtr->ef2(idAbs); // Mass Spectrum, (m^2)^(d-2) double tmpExp = eDdU - 2; double facSpect = pow(mUS, tmpExp); // Total cross section double sigma = eDconstantTerm * facEWS * facSpect * eDsigma0; // If f fbar are quarks if (idAbs < 9) sigma /= 3.; // Related to mass spactrum weighting. sigma /= runBW3; // Truncate sH region or use form factor. // Form factor uses either pythia8 renormScale2 // or E_jet in cms. if (eDcutoff == 1) { if (sH > pow2(eDLambdaU) ) { sigma *= pow(eDLambdaU,4)/pow2(sH); } } else if (eDgraviton && ((eDcutoff == 2) || (eDcutoff == 3))) { double tmPmu = sqrt(Q2RenSave); if (eDcutoff == 3) tmPmu = (sH + s4 - s3) / (2 * mH); double tmPformfact = tmPmu / (eDtff * eDLambdaU); double tmPexp = double(eDnGrav) + 2; sigma *= 1 / (1 + pow(tmPformfact, tmPexp)); } return sigma; } //-------------------------------------------------------------------------- void Sigma2ffbar2LEDUnparticlegamma::setIdColAcol() { // Flavours trivial. setId( id1, id2, eDidG, 22); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2ffbar2LEDgammagamma class. // Cross section for f fbar -> (LED G*/U*) -> gamma gamma // (virtual graviton/unparticle exchange). //-------------------------------------------------------------------------- void Sigma2ffbar2LEDgammagamma::initProc() { // Init model parameters. if (eDgraviton) { eDspin = 2; eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDdU = 2; eDLambdaU = settingsPtr->parm("ExtraDimensionsLED:LambdaT"); eDlambda = 1; eDnegInt = settingsPtr->mode("ExtraDimensionsLED:NegInt"); eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } else { eDspin = settingsPtr->mode("ExtraDimensionsUnpart:spinU"); eDdU = settingsPtr->parm("ExtraDimensionsUnpart:dU"); eDLambdaU = settingsPtr->parm("ExtraDimensionsUnpart:LambdaU"); eDlambda = settingsPtr->parm("ExtraDimensionsUnpart:lambda"); eDnegInt = 0; } // Model dependent constants. if (eDgraviton) { eDlambda2chi = 4*M_PI; if (eDnegInt == 1) eDlambda2chi *= -1.; } else { double tmPAdU = 16 * pow2(M_PI) * sqrt(M_PI) / pow(2. * M_PI, 2. * eDdU) * GammaReal(eDdU + 0.5) / (GammaReal(eDdU - 1.) * GammaReal(2. * eDdU)); double tmPdUpi = eDdU * M_PI; eDlambda2chi = pow2(eDlambda) * tmPAdU / (2 * sin(tmPdUpi)); } // Model parameter check (if not applicable, sigma = 0). // Note: SM contribution still generated. if ( !(eDspin==0 || eDspin==2) ) { eDlambda2chi = 0; infoPtr->errorMsg("Error in Sigma2ffbar2LEDgammagamma::initProc: " "Incorrect spin value (turn process off)!"); } else if ( !eDgraviton && (eDdU >= 2)) { eDlambda2chi = 0; infoPtr->errorMsg("Error in Sigma2ffbar2LEDgammagamma::initProc: " "This process requires dU < 2 (turn process off)!"); } } //-------------------------------------------------------------------------- void Sigma2ffbar2LEDgammagamma::sigmaKin() { // Mandelstam variables. double sHS = pow2(sH); double sHQ = pow(sH, 4); double tHS = pow2(tH); double uHS = pow2(uH); // Form factor. double tmPeffLambdaU = eDLambdaU; if (eDgraviton && ((eDcutoff == 2) || (eDcutoff == 3))) { double tmPffterm = sqrt(Q2RenSave) / (eDtff * eDLambdaU); double tmPexp = double(eDnGrav) + 2; double tmPformfact = 1 + pow(tmPffterm, tmPexp); tmPeffLambdaU *= pow(tmPformfact,0.25); } // ME from spin-0 and spin-2 unparticles // including extra 1/sHS from 2-to-2 phase space. if (eDspin == 0) { double tmPsLambda2 = sH / pow2(tmPeffLambdaU); double tmPexp = 2 * eDdU - 1; eDterm1 = pow(tmPsLambda2,tmPexp); eDterm1 /= sHS; } else { eDterm1 = (uH / tH + tH / uH); eDterm1 /= sHS; double tmPsLambda2 = sH / pow2(tmPeffLambdaU); double tmPexp = eDdU; eDterm2 = pow(tmPsLambda2,tmPexp) * (uHS + tHS) / sHS; eDterm2 /= sHS; tmPexp = 2 * eDdU; eDterm3 = pow(tmPsLambda2,tmPexp) * tH * uH * (uHS + tHS) / sHQ; eDterm3 /= sHS; } } //-------------------------------------------------------------------------- double Sigma2ffbar2LEDgammagamma::sigmaHat() { // Incoming fermion flavor. int idAbs = abs(id1); // Couplings and constants. // Note: ME already contain 1/2 for identical // particles in the final state. double sigma = 0; if (eDspin == 0) { sigma = pow2(eDlambda2chi) * eDterm1 / 8; } else { double tmPe2Q2 = 4 * M_PI * alpEM * couplingsPtr->ef2(idAbs); double tmPdUpi = eDdU * M_PI; sigma = pow2(tmPe2Q2) * eDterm1 - tmPe2Q2 * eDlambda2chi * cos(tmPdUpi) * eDterm2 + pow2(eDlambda2chi) * eDterm3 / 4; } // dsigma/dt, 2-to-2 phase space factors. sigma /= 16 * M_PI; // If f fbar are quarks. if (idAbs < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- void Sigma2ffbar2LEDgammagamma::setIdColAcol() { // Flavours trivial. setId( id1, id2, 22, 22); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2gg2LEDgammagamma class. // Cross section for g g -> (LED G*/U*) -> gamma gamma // (virtual graviton/unparticle exchange). //-------------------------------------------------------------------------- void Sigma2gg2LEDgammagamma::initProc() { // Init model parameters. if (eDgraviton) { eDspin = 2; eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDdU = 2; eDLambdaU = settingsPtr->parm("ExtraDimensionsLED:LambdaT"); eDlambda = 1; eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } else { eDspin = settingsPtr->mode("ExtraDimensionsUnpart:spinU"); eDdU = settingsPtr->parm("ExtraDimensionsUnpart:dU"); eDLambdaU = settingsPtr->parm("ExtraDimensionsUnpart:LambdaU"); eDlambda = settingsPtr->parm("ExtraDimensionsUnpart:lambda"); } // Model dependent constants. if (eDgraviton) { eDlambda2chi = 4 * M_PI; } else { double tmPAdU = 16 * pow2(M_PI) * sqrt(M_PI) / pow(2. * M_PI, 2. * eDdU) * GammaReal(eDdU + 0.5) / (GammaReal(eDdU - 1.) * GammaReal(2. * eDdU)); double tmPdUpi = eDdU * M_PI; eDlambda2chi = pow2(eDlambda) * tmPAdU / (2 * sin(tmPdUpi)); } // Model parameter check (if not applicable, sigma = 0). if ( !(eDspin==0 || eDspin==2) ) { eDlambda2chi = 0; infoPtr->errorMsg("Error in Sigma2gg2LEDgammagamma::initProc: " "Incorrect spin value (turn process off)!"); } else if ( !eDgraviton && (eDdU >= 2)) { eDlambda2chi = 0; infoPtr->errorMsg("Error in Sigma2gg2LEDgammagamma::initProc: " "This process requires dU < 2 (turn process off)!"); } } //-------------------------------------------------------------------------- void Sigma2gg2LEDgammagamma::sigmaKin() { // Mandelstam variables. double sHS = pow2(sH); double sHQ = pow(sH, 4); double tHQ = pow(tH, 4); double uHQ = pow(uH, 4); // Form factor. double tmPeffLambdaU = eDLambdaU; if (eDgraviton && ((eDcutoff == 2) || (eDcutoff == 3))) { double tmPffterm = sqrt(Q2RenSave) / (eDtff * eDLambdaU); double tmPexp = double(eDnGrav) + 2; double tmPformfact = 1 + pow(tmPffterm, tmPexp); tmPeffLambdaU *= pow(tmPformfact,0.25); } // ME from spin-0 and spin-2 unparticles. if (eDspin == 0) { double tmPsLambda2 = sH / pow2(tmPeffLambdaU); double tmPexp = 2 * eDdU; eDsigma0 = pow(tmPsLambda2,tmPexp); } else { double tmPsLambda2 = sH / pow2(tmPeffLambdaU); double tmPexp = 2 * eDdU; eDsigma0 = pow(tmPsLambda2,tmPexp) * (uHQ + tHQ) / sHQ; } // extra 1/sHS from 2-to-2 phase space. eDsigma0 /= sHS; } //-------------------------------------------------------------------------- double Sigma2gg2LEDgammagamma::sigmaHat() { // Couplings and constants. // Note: ME already contain 1/2 for identical // particles in the final state. double sigma = eDsigma0; if (eDspin == 0) { sigma *= pow2(eDlambda2chi) / 256; } else { sigma *= pow2(eDlambda2chi) / 32; } // dsigma/dt, 2-to-2 phase space factors. sigma /= 16 * M_PI; return sigma; } //-------------------------------------------------------------------------- void Sigma2gg2LEDgammagamma::setIdColAcol() { // Flavours trivial. setId( 21, 21, 22, 22); // Colour flow topologies. setColAcol( 1, 2, 2, 1, 0, 0, 0, 0); } //========================================================================== // Sigma2ffbar2LEDllbar class. // Cross section for f fbar -> (LED G*/U*) -> l lbar // (virtual graviton/unparticle exchange). // Does not include t-channel contributions relevant for e^+e^- to e^+e^- //-------------------------------------------------------------------------- void Sigma2ffbar2LEDllbar::initProc() { // Init model parameters. if (eDgraviton) { eDspin = 2; eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDdU = 2; eDLambdaU = settingsPtr->parm("ExtraDimensionsLED:LambdaT"); eDlambda = 1; eDnegInt = settingsPtr->mode("ExtraDimensionsLED:NegInt"); eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } else { eDspin = settingsPtr->mode("ExtraDimensionsUnpart:spinU"); eDdU = settingsPtr->parm("ExtraDimensionsUnpart:dU"); eDLambdaU = settingsPtr->parm("ExtraDimensionsUnpart:LambdaU"); eDlambda = settingsPtr->parm("ExtraDimensionsUnpart:lambda"); eDnxx = settingsPtr->mode("ExtraDimensionsUnpart:gXX"); eDnxy = settingsPtr->mode("ExtraDimensionsUnpart:gXY"); eDnegInt = 0; } eDmZ = particleDataPtr->m0(23); eDmZS = eDmZ * eDmZ; eDGZ = particleDataPtr->mWidth(23); eDGZS = eDGZ * eDGZ; // Model dependent constants. if (eDgraviton) { eDlambda2chi = 4*M_PI; if (eDnegInt == 1) eDlambda2chi *= -1.; } else { double tmPAdU = 16 * pow2(M_PI) * sqrt(M_PI) / pow(2. * M_PI, 2. * eDdU) * GammaReal(eDdU + 0.5) / (GammaReal(eDdU - 1.) * GammaReal(2. * eDdU)); double tmPdUpi = eDdU * M_PI; eDlambda2chi = pow2(eDlambda) * tmPAdU / (2 * sin(tmPdUpi)); } // Model parameter check (if not applicable, sigma = 0). // Note: SM contribution still generated. if ( !(eDspin==1 || eDspin==2) ) { eDlambda2chi = 0; infoPtr->errorMsg("Error in Sigma2ffbar2LEDllbar::initProc: " "Incorrect spin value (turn process off)!"); } else if ( !eDgraviton && (eDdU >= 2)) { eDlambda2chi = 0; infoPtr->errorMsg("Error in Sigma2ffbar2LEDllbar::initProc: " "This process requires dU < 2 (turn process off)!"); } } //-------------------------------------------------------------------------- void Sigma2ffbar2LEDllbar::sigmaKin() { // Mandelstam variables. double tHS = pow2(tH); double uHS = pow2(uH); double tHC = pow(tH,3); double uHC = pow(uH,3); double tHQ = pow(tH,4); double uHQ = pow(uH,4); // Form factor. double tmPeffLambdaU = eDLambdaU; if (eDgraviton && ((eDcutoff == 2) || (eDcutoff == 3))) { double tmPffterm = sqrt(Q2RenSave) / (eDtff * eDLambdaU); double tmPexp = double(eDnGrav) + 2; double tmPformfact = 1 + pow(tmPffterm, tmPexp); tmPeffLambdaU *= pow(tmPformfact,0.25); } // ME from spin-1 and spin-2 unparticles eDdenomPropZ = pow2(sH - eDmZS) + eDmZS * eDGZS; eDrePropZ = (sH - eDmZS) / eDdenomPropZ; eDimPropZ = -eDmZ * eDGZ / eDdenomPropZ; eDrePropGamma = 1 / sH; if (eDspin == 1) { double tmPsLambda2 = sH / pow2(tmPeffLambdaU); double tmPexp = eDdU - 2; eDabsMeU = eDlambda2chi * pow(tmPsLambda2,tmPexp) / pow2(tmPeffLambdaU); } else { double tmPsLambda2 = sH / pow2(tmPeffLambdaU); double tmPexp = eDdU - 2; double tmPA = -eDlambda2chi * pow(tmPsLambda2,tmPexp) / (8 * pow(tmPeffLambdaU,4)); eDabsAS = pow2(tmPA); eDreA = tmPA * cos(M_PI * eDdU); eDreABW = tmPA * ((sH - eDmZS) * cos(M_PI * eDdU) + eDmZ * eDGZ * sin(M_PI * eDdU)) / eDdenomPropZ; eDpoly1 = tHQ + uHQ - 6*tHC*uH - 6*tH*uHC + 18*tHS*uHS; double tmPdiffUT = uH - tH; eDpoly2 = pow(tmPdiffUT,3); eDpoly3 = tHC - 3*tHS*uH - 3*tH*uHS + uHC; } } //-------------------------------------------------------------------------- double Sigma2ffbar2LEDllbar::sigmaHat() { // Incoming fermion flavor. int idAbs = abs(id1); // Couplings and constants. // Qq = couplingsPtr->ef(idAbs), quark, i.e. id > 0. // Ql = couplingsPtr->ef(11), electron. double tmPe2QfQl = 4 * M_PI * alpEM * couplingsPtr->ef(idAbs) * couplingsPtr->ef(11); double tmPgvq = 0.25 * couplingsPtr->vf(idAbs); double tmPgaq = 0.25 * couplingsPtr->af(idAbs); double tmPgLq = tmPgvq + tmPgaq; double tmPgRq = tmPgvq - tmPgaq; double tmPgvl = 0.25 * couplingsPtr->vf(11); double tmPgal = 0.25 * couplingsPtr->af(11); double tmPgLl = tmPgvl + tmPgal; double tmPgRl = tmPgvl - tmPgal; double tmPe2s2c2 = 4 * M_PI * alpEM / (couplingsPtr->sin2thetaW() * couplingsPtr->cos2thetaW()); // LL, RR, LR, RL couplings. vector tmPcoupZ; tmPcoupZ.push_back(tmPe2s2c2 * tmPgLq * tmPgLl); tmPcoupZ.push_back(tmPe2s2c2 * tmPgRq * tmPgRl); tmPcoupZ.push_back(tmPe2s2c2 * tmPgRq * tmPgLl); tmPcoupZ.push_back(tmPe2s2c2 * tmPgLq * tmPgRl); vector tmPcoupU; if (eDnxx == 1) { // LL tmPcoupU.push_back(-1); // RR tmPcoupU.push_back(-1); } else if (eDnxx == 2) { // LL tmPcoupU.push_back(0); // RR tmPcoupU.push_back(0); } else { // LL tmPcoupU.push_back(1); // RR tmPcoupU.push_back(1); } if (eDnxy == 1) { // RL tmPcoupU.push_back(-1); // LR tmPcoupU.push_back(-1); } else if (eDnxy == 2) { // RL tmPcoupU.push_back(0); // LR tmPcoupU.push_back(0); } else { // RL tmPcoupU.push_back(1); // LR tmPcoupU.push_back(1); } // Matrix elements double tmPMES = 0; if (eDspin == 1) { for (unsigned int i = 0; illbar) = 3 * sigma(ffbar->eebar) sigma *= 3.; return sigma; } //-------------------------------------------------------------------------- void Sigma2ffbar2LEDllbar::setIdColAcol() { double tmPrand = rndmPtr->flat(); // Flavours trivial. if (tmPrand < 0.33333333) { setId( id1, id2, 11, -11); } else if (tmPrand < 0.66666667) { setId( id1, id2, 13, -13); } else { setId( id1, id2, 15, -15); } // tH defined between f and f': must swap tHat <-> uHat if id1 is fbar. swapTU = (id2 > 0); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2gg2LEDllbar class. // Cross section for g g -> (LED G*/U*) -> l lbar // (virtual graviton/unparticle exchange). //-------------------------------------------------------------------------- void Sigma2gg2LEDllbar::initProc() { // Init model parameters. if (eDgraviton) { eDspin = 2; eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDdU = 2; eDLambdaU = settingsPtr->parm("ExtraDimensionsLED:LambdaT"); eDlambda = 1; eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } else { eDspin = settingsPtr->mode("ExtraDimensionsUnpart:spinU"); eDdU = settingsPtr->parm("ExtraDimensionsUnpart:dU"); eDLambdaU = settingsPtr->parm("ExtraDimensionsUnpart:LambdaU"); eDlambda = settingsPtr->parm("ExtraDimensionsUnpart:lambda"); } // Model dependent constants. if (eDgraviton) { eDlambda2chi = 4 * M_PI; } else { double tmPAdU = 16 * pow2(M_PI) * sqrt(M_PI) / pow(2. * M_PI, 2. * eDdU) * GammaReal(eDdU + 0.5) / (GammaReal(eDdU - 1.) * GammaReal(2. * eDdU)); double tmPdUpi = eDdU * M_PI; eDlambda2chi = pow2(eDlambda) * tmPAdU / (2 * sin(tmPdUpi)); } // Model parameter check (if not applicable, sigma = 0). if ( !(eDspin==2) ) { eDlambda2chi = 0; infoPtr->errorMsg("Error in Sigma2gg2LEDllbar::initProc: " "Incorrect spin value (turn process off)!"); } else if ( !eDgraviton && (eDdU >= 2)) { eDlambda2chi = 0; infoPtr->errorMsg("Error in Sigma2gg2LEDllbar::initProc: " "This process requires dU < 2 (turn process off)!"); } } //-------------------------------------------------------------------------- void Sigma2gg2LEDllbar::sigmaKin() { // Form factor. double tmPeffLambdaU = eDLambdaU; if (eDgraviton && ((eDcutoff == 2) || (eDcutoff == 3))) { double tmPffterm = sqrt(Q2RenSave) / (eDtff * eDLambdaU); double tmPexp = double(eDnGrav) + 2; double tmPformfact = 1 + pow(tmPffterm, tmPexp); tmPeffLambdaU *= pow(tmPformfact,0.25); } // ME from spin-2 unparticle. double tmPsLambda2 = sH / pow2(tmPeffLambdaU); double tmPexp = eDdU - 2; double tmPA = -eDlambda2chi * pow(tmPsLambda2,tmPexp) / (8 * pow(tmPeffLambdaU,4)); eDsigma0 = 4 * pow2(tmPA) * uH * tH * (pow2(uH) + pow2(tH)); // extra 1/sHS from 2-to-2 phase space. eDsigma0 /= 16 * M_PI * pow2(sH); // sigma(ffbar->llbar) = 3 * sigma(ffbar->eebar) eDsigma0 *= 3.; } //-------------------------------------------------------------------------- void Sigma2gg2LEDllbar::setIdColAcol() { double tmPrand = rndmPtr->flat(); // Flavours trivial. if (tmPrand < 0.33333333) { setId( 21, 21, 11, -11); } else if (tmPrand < 0.66666667) { setId( 21, 21, 13, -13); } else { setId( 21, 21, 15, -15); } // Colour flow topologies. setColAcol( 1, 2, 2, 1, 0, 0, 0, 0); } //========================================================================== // Sigma2gg2LEDgg class. // Cross section for g g -> (LED G*) -> g g. //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2LEDgg::initProc() { // Read model parameters. eDopMode = settingsPtr->mode("ExtraDimensionsLED:opMode"); eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDMD = settingsPtr->parm("ExtraDimensionsLED:MD"); eDLambdaT = settingsPtr->parm("ExtraDimensionsLED:LambdaT"); eDnegInt = settingsPtr->mode("ExtraDimensionsLED:NegInt"); eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2gg2LEDgg::sigmaKin() { // Get S(x) values for G amplitude. complex sS(0., 0.); complex sT(0., 0.); complex sU(0., 0.); if (eDopMode == 0) { sS = ampLedS( sH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sT = ampLedS( tH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sU = ampLedS( uH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); } else { // Form factor. double effLambda = eDLambdaT; if ((eDcutoff == 2) || (eDcutoff == 3)) { double ffterm = sqrt(Q2RenSave) / (eDtff * eDLambdaT); double exp = double(eDnGrav) + 2.; double formfa = 1. + pow(ffterm, exp); effLambda *= pow(formfa,0.25); } sS = 4.*M_PI/pow(effLambda,4); sT = 4.*M_PI/pow(effLambda,4); sU = 4.*M_PI/pow(effLambda,4); if (eDnegInt == 1) { sS *= -1.; sT *= -1.; sU *= -1.; } } // Calculate kinematics dependence. double sH3 = sH*sH2; double tH3 = tH*tH2; double uH3 = uH*uH2; sigTS = (128. * pow2(M_PI) * pow2(alpS)) * (9./4.) * (tH2 / sH2 + 2. * tH / sH + 3. + 2. * sH / tH + sH2 / tH2) + 24.*M_PI*alpS*( (sH3/tH + tH2 + 3.*(sH*tH + sH2))*sS.real() + (tH3/sH + sH2 + 3.*(tH*sH + tH2))*sT.real()) + pow2(uH2)*( 4.*real(sS*conj(sS)) + sS.real()*sT.real() + sS.imag()*sT.imag() + 4.*real(sT*conj(sT))); sigUS = (128. * pow2(M_PI) * pow2(alpS)) * (9./4.) * (uH2 / sH2 + 2. * uH / sH + 3. + 2. * sH / uH + sH2 / uH2) + 24.*M_PI*alpS*( (sH3/uH + uH2 + 3.*(sH*uH + sH2))*sS.real() + (uH3/sH + sH2 + 3.*(uH*sH + uH2))*sU.real()) + pow2(tH2)*( 4.*real(sS*conj(sS)) + sS.real()*sU.real() + sS.imag()*sU.imag() + 4.*real(sU*conj(sU))); sigTU = (128. * pow2(M_PI) * pow2(alpS)) * (9./4.) * (tH2 / uH2 + 2. * tH / uH + 3. + 2. * uH / tH + uH2 / tH2) + 24.*M_PI*alpS*( (tH3/uH + uH2 + 3.*(tH*uH + tH2))*sT.real() + (uH3/tH + tH2 + 3.*(uH*tH + uH2))*sU.real()) + pow2(sH2)*( 4.*real(sT*conj(sT)) + sT.real()*sU.real() + sT.imag()*sU.imag() + 4.*real(sU*conj(sU))); sigSum = sigTS + sigUS + sigTU; // Answer contains factor 1/2 from identical gluons. sigma = 0.5 * sigSum / (128. * M_PI * sH2); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2LEDgg::setIdColAcol() { // Flavours are trivial. setId( id1, id2, 21, 21); // Three colour flow topologies, each with two orientations. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 2, 2, 3, 1, 4, 4, 3); else if (sigRand < sigTS + sigUS) setColAcol( 1, 2, 3, 1, 3, 4, 4, 2); else setColAcol( 1, 2, 3, 4, 1, 4, 3, 2); if (rndmPtr->flat() > 0.5) swapColAcol(); } //========================================================================== // Sigma2gg2LEDqqbar class. // Cross section for g g -> (LED G*) -> q qbar. //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2LEDqqbar::initProc() { // Read number of quarks to be considered in massless approximation // as well as model parameters. nQuarkNew = settingsPtr->mode("ExtraDimensionsLED:nQuarkNew"); eDopMode = settingsPtr->mode("ExtraDimensionsLED:opMode"); eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDMD = settingsPtr->parm("ExtraDimensionsLED:MD"); eDLambdaT = settingsPtr->parm("ExtraDimensionsLED:LambdaT"); eDnegInt = settingsPtr->mode("ExtraDimensionsLED:NegInt"); eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2gg2LEDqqbar::sigmaKin() { // Get S(x) values for G amplitude. complex sS(0., 0.); complex sT(0., 0.); complex sU(0., 0.); if (eDopMode == 0) { sS = ampLedS( sH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sT = ampLedS( tH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sU = ampLedS( uH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); } else { // Form factor. double effLambda = eDLambdaT; if ((eDcutoff == 2) || (eDcutoff == 3)) { double ffterm = sqrt(Q2RenSave) / (eDtff * eDLambdaT); double exp = double(eDnGrav) + 2.; double formfa = 1. + pow(ffterm, exp); effLambda *= pow(formfa,0.25); } sS = 4.*M_PI/pow(effLambda,4); sT = 4.*M_PI/pow(effLambda,4); sU = 4.*M_PI/pow(effLambda,4); if (eDnegInt == 1) { sS *= -1.; sT *= -1.; sU *= -1.; } } // Pick new flavour. idNew = 1 + int( nQuarkNew * rndmPtr->flat() ); mNew = particleDataPtr->m0(idNew); m2New = mNew*mNew; // Calculate kinematics dependence. sigTS = 0.; sigUS = 0.; if (sH > 4. * m2New) { double tH3 = tH*tH2; double uH3 = uH*uH2; sigTS = (16. * pow2(M_PI) * pow2(alpS)) * ((1./6.) * uH / tH - (3./8.) * uH2 / sH2) - 0.5 * M_PI * alpS * uH2 * sS.real() + (3./16.) * uH3 * tH * real(sS*conj(sS)); sigUS = (16. * pow2(M_PI) * pow2(alpS)) * ((1./6.) * tH / uH - (3./8.) * tH2 / sH2) - 0.5 * M_PI * alpS * tH2 * sS.real() + (3./16.) * tH3 * uH * real(sS*conj(sS)); } sigSum = sigTS + sigUS; // Answer is proportional to number of outgoing flavours. sigma = nQuarkNew * sigSum / (16. * M_PI * sH2); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2LEDqqbar::setIdColAcol() { // Flavours are trivial. setId( id1, id2, idNew, -idNew); // Two colour flow topologies. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 2, 2, 3, 1, 0, 0, 3); else setColAcol( 1, 2, 3, 1, 3, 0, 0, 2); } //========================================================================== // Sigma2qg2LEDqg class. // Cross section for q g -> (LED G*) -> q g. //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2LEDqg::initProc() { // Read model parameters. eDopMode = settingsPtr->mode("ExtraDimensionsLED:opMode"); eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDMD = settingsPtr->parm("ExtraDimensionsLED:MD"); eDLambdaT = settingsPtr->parm("ExtraDimensionsLED:LambdaT"); eDnegInt = settingsPtr->mode("ExtraDimensionsLED:NegInt"); eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2qg2LEDqg::sigmaKin() { // Get S(x) values for G amplitude. complex sS(0., 0.); complex sT(0., 0.); complex sU(0., 0.); if (eDopMode == 0) { sS = ampLedS( sH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sT = ampLedS( tH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sU = ampLedS( uH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); } else { // Form factor. double effLambda = eDLambdaT; if ((eDcutoff == 2) || (eDcutoff == 3)) { double ffterm = sqrt(Q2RenSave) / (eDtff * eDLambdaT); double exp = double(eDnGrav) + 2.; double formfa = 1. + pow(ffterm, exp); effLambda *= pow(formfa,0.25); } sS = 4.*M_PI/pow(effLambda,4); sT = 4.*M_PI/pow(effLambda,4); sU = 4.*M_PI/pow(effLambda,4); if (eDnegInt == 1) { sS *= -1.; sT *= -1.; sU *= -1.; } } // Calculate kinematics dependence. double sH3 = sH*sH2; double uH3 = uH*uH2; sigTS = (16. * pow2(M_PI) * pow2(alpS)) * (uH2 / tH2 - (4./9.) * uH / sH) + (4./3.) * M_PI * alpS * uH2 * sT.real() - 0.5 * uH3 * sH * real(sT*conj(sT)); sigTU = (16. * pow2(M_PI) * pow2(alpS)) * (sH2 / tH2 - (4./9.) * sH / uH) + (4./3.) * M_PI * alpS * sH2 * sT.real() - 0.5 * sH3 * uH * real(sT*conj(sT)); sigSum = sigTS + sigTU; // Answer. sigma = sigSum / (16. * M_PI * sH2); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2LEDqg::setIdColAcol() { // Outgoing = incoming flavours. setId( id1, id2, id1, id2); // Two colour flow topologies. Swap if first is gluon, or when antiquark. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 0, 2, 1, 3, 0, 2, 3); else setColAcol( 1, 0, 2, 3, 2, 0, 1, 3); if (id1 == 21) swapCol1234(); if (id1 < 0 || id2 < 0) swapColAcol(); } //========================================================================== // Sigma2qq2LEDqq class. // Cross section for q q(bar)' -> (LED G*) -> q q(bar)' //-------------------------------------------------------------------------- // Initialize process. void Sigma2qq2LEDqq::initProc() { // Read model parameters. eDopMode = settingsPtr->mode("ExtraDimensionsLED:opMode"); eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDMD = settingsPtr->parm("ExtraDimensionsLED:MD"); eDLambdaT = settingsPtr->parm("ExtraDimensionsLED:LambdaT"); eDnegInt = settingsPtr->mode("ExtraDimensionsLED:NegInt"); eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qq2LEDqq::sigmaKin() { // Get S(x) values for G amplitude. complex sS(0., 0.); complex sT(0., 0.); complex sU(0., 0.); if (eDopMode == 0) { sS = ampLedS( sH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sT = ampLedS( tH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sU = ampLedS( uH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); } else { // Form factor. double effLambda = eDLambdaT; if ((eDcutoff == 2) || (eDcutoff == 3)) { double ffterm = sqrt(Q2RenSave) / (eDtff * eDLambdaT); double exp = double(eDnGrav) + 2.; double formfa = 1. + pow(ffterm, exp); effLambda *= pow(formfa,0.25); } sS = 4.*M_PI/pow(effLambda,4); sT = 4.*M_PI/pow(effLambda,4); sU = 4.*M_PI/pow(effLambda,4); if (eDnegInt == 1) { sS *= -1.; sT *= -1.; sU *= -1.; } } // Calculate kinematics dependence for different terms. sigT = (4./9.) * (sH2 + uH2) / tH2; sigU = (4./9.) * (sH2 + tH2) / uH2; sigTU = - (8./27.) * sH2 / (tH * uH); sigST = - (8./27.) * uH2 / (sH * tH); // Graviton terms. sigGrT1 = funLedG(tH, uH) * real(sT*conj(sT)) / 8.; sigGrT2 = funLedG(tH, sH) * real(sT*conj(sT)) / 8.; sigGrU = funLedG(uH, tH) * real(sU*conj(sU)) / 8.; sigGrTU = (8./9.) * M_PI * alpS * sH2 * ((4.*uH + tH)*sT.real()/uH + (4.*tH + uH)*sU.real()/tH) + (sT.real()*sU.real() + sT.imag()*sU.imag()) * (4.*tH + uH)*(4.*uH + tH) * sH2 / 48.; sigGrST = (8./9.) * M_PI * alpS * uH2 * ((4.*tH + sH)*sS.real()/tH + (4.*sH + tH)*sT.real()/sH) + (sS.real()*sT.real() + sS.imag()*sT.imag()) * (4.*sH + tH)*(4.*tH + sH) * uH2 / 48.; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qq2LEDqq::sigmaHat() { // Combine cross section terms; factor 1/2 when identical quarks. if (id2 == id1) { sigSum = (16. * pow2(M_PI) * pow2(alpS)) * (sigT + sigU + sigTU) + sigGrT1 + sigGrU + sigGrTU; sigSum *= 0.5; } else if (id2 == -id1) { sigSum = (16. * pow2(M_PI) * pow2(alpS)) * (sigT + sigST) + sigGrT2 + sigGrST; } else { sigSum = 16. * pow2(M_PI) * pow2(alpS) * sigT + sigGrT1; } // Answer. return sigSum / (16. * M_PI * sH2); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qq2LEDqq::setIdColAcol() { // Outgoing = incoming flavours. setId( id1, id2, id1, id2); // Colour flow topologies. Swap when antiquarks. double sigTtot = sigT + sigGrT2; double sigUtot = sigU + sigGrU; if (id1 * id2 > 0) setColAcol( 1, 0, 2, 0, 2, 0, 1, 0); else setColAcol( 1, 0, 0, 1, 2, 0, 0, 2); if (id2 == id1 && (sigTtot + sigUtot) * rndmPtr->flat() > sigTtot) setColAcol( 1, 0, 2, 0, 1, 0, 2, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2LEDgg class. // Cross section for q qbar -> (LED G*) -> g g. //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2LEDgg::initProc() { // Read model parameters. eDopMode = settingsPtr->mode("ExtraDimensionsLED:opMode"); eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDMD = settingsPtr->parm("ExtraDimensionsLED:MD"); eDLambdaT = settingsPtr->parm("ExtraDimensionsLED:LambdaT"); eDnegInt = settingsPtr->mode("ExtraDimensionsLED:NegInt"); eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2qqbar2LEDgg::sigmaKin() { // Get S(x) values for G amplitude. complex sS(0., 0.); complex sT(0., 0.); complex sU(0., 0.); if (eDopMode == 0) { sS = ampLedS( sH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sT = ampLedS( tH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sU = ampLedS( uH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); } else { // Form factor. double effLambda = eDLambdaT; if ((eDcutoff == 2) || (eDcutoff == 3)) { double ffterm = sqrt(Q2RenSave) / (eDtff * eDLambdaT); double exp = double(eDnGrav) + 2.; double formfa = 1. + pow(ffterm, exp); effLambda *= pow(formfa,0.25); } sS = 4.*M_PI/pow(effLambda,4); sT = 4.*M_PI/pow(effLambda,4); sU = 4.*M_PI/pow(effLambda,4); if (eDnegInt == 1) { sS *= -1.; sT *= -1.; sU *= -1.; } } // Calculate kinematics dependence. double tH3 = tH*tH2; double uH3 = uH*uH2; sigTS = (16. * pow2(M_PI) * pow2(alpS)) * ((1./6.) * uH / tH - (3./8.) * uH2 / sH2) - 0.5 * M_PI * alpS * uH2 * sS.real() + (3./16.) * uH3 * tH * real(sS*conj(sS)); sigUS = (16. * pow2(M_PI) * pow2(alpS)) * ((1./6.) * tH / uH - (3./8.) * tH2 / sH2) - 0.5 * M_PI * alpS * tH2 * sS.real() + (3./16.) * tH3 * uH * real(sS*conj(sS)); sigSum = sigTS + sigUS; // Answer contains factor 1/2 from identical gluons. sigma = (64./9.) * 0.5 * sigSum / (16. * M_PI * sH2); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2LEDgg::setIdColAcol() { // Outgoing flavours trivial. setId( id1, id2, 21, 21); // Two colour flow topologies. Swap if first is antiquark. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 0, 0, 2, 1, 3, 3, 2); else setColAcol( 1, 0, 0, 2, 3, 2, 1, 3); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2LEDqqbarNew class. // Cross section q qbar -> (LED G*) -> q' qbar'. //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2LEDqqbarNew::initProc() { // Read number of quarks to be considered in massless approximation // as well as model parameters. nQuarkNew = settingsPtr->mode("ExtraDimensionsLED:nQuarkNew"); eDopMode = settingsPtr->mode("ExtraDimensionsLED:opMode"); eDnGrav = settingsPtr->mode("ExtraDimensionsLED:n"); eDMD = settingsPtr->parm("ExtraDimensionsLED:MD"); eDLambdaT = settingsPtr->parm("ExtraDimensionsLED:LambdaT"); eDcutoff = settingsPtr->mode("ExtraDimensionsLED:CutOffMode"); eDtff = settingsPtr->parm("ExtraDimensionsLED:t"); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2qqbar2LEDqqbarNew::sigmaKin() { // Get S(x) values for G amplitude. complex sS(0., 0.); complex sT(0., 0.); complex sU(0., 0.); if (eDopMode == 0) { sS = ampLedS( sH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sT = ampLedS( tH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); sU = ampLedS( uH/pow2(eDLambdaT), eDnGrav, eDLambdaT, eDMD); } else { // Form factor. double effLambda = eDLambdaT; if ((eDcutoff == 2) || (eDcutoff == 3)) { double ffterm = sqrt(Q2RenSave) / (eDtff * eDLambdaT); double exp = double(eDnGrav) + 2.; double formfa = 1. + pow(ffterm, exp); effLambda *= pow(formfa,0.25); } sS = 4.*M_PI/pow(effLambda,4); sT = 4.*M_PI/pow(effLambda,4); sU = 4.*M_PI/pow(effLambda,4); } // Pick new flavour. idNew = 1 + int( nQuarkNew * rndmPtr->flat() ); mNew = particleDataPtr->m0(idNew); m2New = mNew*mNew; // Calculate kinematics dependence. sigS = 0.; if (sH > 4. * m2New) { sigS = (16. * pow2(M_PI) * pow2(alpS)) * (4./9.) * (tH2 + uH2) / sH2 + funLedG(sH, tH) * real(sS*conj(sS)) / 8.; } // Answer is proportional to number of outgoing flavours. sigma = nQuarkNew * sigS / (16. * M_PI * sH2); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2LEDqqbarNew::setIdColAcol() { // Set outgoing flavours ones. id3 = (id1 > 0) ? idNew : -idNew; setId( id1, id2, id3, -id3); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); if (id1 < 0) swapColAcol(); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/PhaseSpace.cc0000644000175000017500000042167712217346247015474 0ustar sunsun// PhaseSpace.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // PhaseSpace and PhaseSpace2to2tauyz classes. #include "Pythia8/PhaseSpace.h" namespace Pythia8 { //========================================================================== // The PhaseSpace class. // Base class for phase space generators. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of trial maxima around which maximum search is performed. const int PhaseSpace::NMAXTRY = 2; // Number of three-body trials in phase space optimization. const int PhaseSpace::NTRY3BODY = 20; // Maximum cross section increase, just in case true maximum not found. const double PhaseSpace::SAFETYMARGIN = 1.05; // Small number to avoid division by zero. const double PhaseSpace::TINY = 1e-20; // Fraction of total weight that is shared evenly between all shapes. const double PhaseSpace::EVENFRAC = 0.4; // Two cross sections with a small relative error are assumed same. const double PhaseSpace::SAMESIGMA = 1e-6; // Do not include resonances peaked too far outside allowed mass region. const double PhaseSpace::WIDTHMARGIN = 20.; // Special optimization treatment when two resonances at almost same mass. const double PhaseSpace::SAMEMASS = 0.01; // Minimum phase space left when kinematics constraints are combined. const double PhaseSpace::MASSMARGIN = 0.01; // When using Breit-Wigners in 2 -> 2 raise maximum weight estimate. const double PhaseSpace::EXTRABWWTMAX = 1.25; // Size of Breit-Wigner threshold region, for mass selection biasing. const double PhaseSpace::THRESHOLDSIZE = 3.; // Step size in optimal-mass search, for mass selection biasing. const double PhaseSpace::THRESHOLDSTEP = 0.2; // Minimal rapidity range for allowed open range (in 2 -> 3). const double PhaseSpace::YRANGEMARGIN = 1e-6; // Cutoff for f_e^e at x < 1 - 10^{-10} to be used in phase space selection. // Note: the ...MIN quantities come from 1 - x_max or 1 - tau_max. const double PhaseSpace::LEPTONXMIN = 1e-10; const double PhaseSpace::LEPTONXMAX = 1. - 1e-10; const double PhaseSpace::LEPTONXLOGMIN = log(1e-10); const double PhaseSpace::LEPTONXLOGMAX = log(1. - 1e-10); const double PhaseSpace::LEPTONTAUMIN = 2e-10; // Safety to avoid division with unreasonably small value for z selection. const double PhaseSpace::SHATMINZ = 1.; // Regularization for small pT2min in z = cos(theta) selection. const double PhaseSpace::PT2RATMINZ = 0.0001; // These numbers are hardwired empirical parameters, // intended to speed up the M-generator. const double PhaseSpace::WTCORRECTION[11] = { 1., 1., 1., 2., 5., 15., 60., 250., 1250., 7000., 50000. }; // MBR: form factor appoximation with two exponents, [FFB1,FFB2] = GeV-2. const double PhaseSpace::FFA1 = 0.9; const double PhaseSpace::FFA2 = 0.1; const double PhaseSpace::FFB1 = 4.6; const double PhaseSpace::FFB2 = 0.6; //-------------------------------------------------------------------------- // Perform simple initialization and store pointers. void PhaseSpace::init(bool isFirst, SigmaProcess* sigmaProcessPtrIn, Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn, Couplings* couplingsPtrIn, SigmaTotal* sigmaTotPtrIn, UserHooks* userHooksPtrIn) { // Store input pointers for future use. sigmaProcessPtr = sigmaProcessPtrIn; infoPtr = infoPtrIn; settingsPtr = settingsPtrIn; particleDataPtr = particleDataPtrIn; rndmPtr = rndmPtrIn; beamAPtr = beamAPtrIn; beamBPtr = beamBPtrIn; couplingsPtr = couplingsPtrIn; sigmaTotPtr = sigmaTotPtrIn; userHooksPtr = userHooksPtrIn; // Some commonly used beam information. idA = beamAPtr->id(); idB = beamBPtr->id(); mA = beamAPtr->m(); mB = beamBPtr->m(); eCM = infoPtr->eCM(); s = eCM * eCM; // Flag if lepton beams, and if non-resolved ones. hasLeptonBeams = ( beamAPtr->isLepton() || beamBPtr->isLepton() ); hasPointLeptons = ( hasLeptonBeams && (beamAPtr->isUnresolved() || beamBPtr->isUnresolved() ) ); // Standard phase space cuts. if (isFirst || settingsPtr->flag("PhaseSpace:sameForSecond")) { mHatGlobalMin = settingsPtr->parm("PhaseSpace:mHatMin"); mHatGlobalMax = settingsPtr->parm("PhaseSpace:mHatMax"); pTHatGlobalMin = settingsPtr->parm("PhaseSpace:pTHatMin"); pTHatGlobalMax = settingsPtr->parm("PhaseSpace:pTHatMax"); // Optionally separate phase space cuts for second hard process. } else { mHatGlobalMin = settingsPtr->parm("PhaseSpace:mHatMinSecond"); mHatGlobalMax = settingsPtr->parm("PhaseSpace:mHatMaxSecond"); pTHatGlobalMin = settingsPtr->parm("PhaseSpace:pTHatMinSecond"); pTHatGlobalMax = settingsPtr->parm("PhaseSpace:pTHatMaxSecond"); } // Cutoff against divergences at pT -> 0. pTHatMinDiverge = settingsPtr->parm("PhaseSpace:pTHatMinDiverge"); // When to use Breit-Wigners. useBreitWigners = settingsPtr->flag("PhaseSpace:useBreitWigners"); minWidthBreitWigners = settingsPtr->parm("PhaseSpace:minWidthBreitWigners"); // Whether generation is with variable energy. doEnergySpread = settingsPtr->flag("Beams:allowMomentumSpread"); // Flags for maximization information and violation handling. showSearch = settingsPtr->flag("PhaseSpace:showSearch"); showViolation = settingsPtr->flag("PhaseSpace:showViolation"); increaseMaximum = settingsPtr->flag("PhaseSpace:increaseMaximum"); // Know whether a Z0 is pure Z0 or admixed with gamma*. gmZmodeGlobal = settingsPtr->mode("WeakZ0:gmZmode"); // Flags if user should be allowed to reweight cross section. canModifySigma = (userHooksPtr != 0) ? userHooksPtr->canModifySigma() : false; canBiasSelection = (userHooksPtr != 0) ? userHooksPtr->canBiasSelection() : false; // Parameters for simplified reweighting of 2 -> 2 processes. canBias2Sel = settingsPtr->flag("PhaseSpace:bias2Selection"); bias2SelPow = settingsPtr->parm("PhaseSpace:bias2SelectionPow"); bias2SelRef = settingsPtr->parm("PhaseSpace:bias2SelectionRef"); // Possibility to recalculate mass for Les Houches input. mRecalculate = settingsPtr->parm("LesHouches:mRecalculate"); // Default event-specific kinematics properties. x1H = 1.; x2H = 1.; m3 = 0.; m4 = 0.; m5 = 0.; s3 = m3 * m3; s4 = m4 * m4; s5 = m5 * m5; mHat = eCM; sH = s; tH = 0.; uH = 0.; pTH = 0.; theta = 0.; phi = 0.; runBW3H = 1.; runBW4H = 1.; runBW5H = 1.; // Default cross section information. sigmaNw = 0.; sigmaMx = 0.; sigmaPos = 0.; sigmaNeg = 0.; newSigmaMx = false; biasWt = 1.; } //-------------------------------------------------------------------------- // Allow for nonisotropic decays when ME's available. void PhaseSpace::decayKinematics( Event& process) { // Identify sets of sister partons. int iResEnd = 4; for (int iResBeg = 5; iResBeg < process.size(); ++iResBeg) { if (iResBeg <= iResEnd) continue; iResEnd = iResBeg; while ( iResEnd < process.size() - 1 && process[iResEnd + 1].mother1() == process[iResBeg].mother1() && process[iResEnd + 1].mother2() == process[iResBeg].mother2() ) ++iResEnd; // Check that at least one of them is a resonance. bool hasRes = false; for (int iRes = iResBeg; iRes <= iResEnd; ++iRes) if ( !process[iRes].isFinal() ) hasRes = true; if ( !hasRes ) continue; // Evaluate matrix element and decide whether to keep kinematics. double decWt = sigmaProcessPtr->weightDecay( process, iResBeg, iResEnd); if (decWt < 0.) infoPtr->errorMsg("Warning in PhaseSpace::decay" "Kinematics: negative angular weight"); if (decWt > 1.) infoPtr->errorMsg("Warning in PhaseSpace::decay" "Kinematics: angular weight above unity"); while (decWt < rndmPtr->flat() ) { // Find resonances for which to redo decay angles. for (int iRes = iResBeg; iRes < process.size(); ++iRes) { if ( process[iRes].isFinal() ) continue; int iResMother = iRes; while (iResMother > iResEnd) iResMother = process[iResMother].mother1(); if (iResMother < iResBeg) continue; // Do decay of this mother isotropically in phase space. decayKinematicsStep( process, iRes); // End loop over resonance decay chains. } // Ready to allow new test of matrix element. decWt = sigmaProcessPtr->weightDecay( process, iResBeg, iResEnd); if (decWt < 0.) infoPtr->errorMsg("Warning in PhaseSpace::decay" "Kinematics: negative angular weight"); if (decWt > 1.) infoPtr->errorMsg("Warning in PhaseSpace::decay" "Kinematics: angular weight above unity"); } // End loop over sets of sister resonances/partons. } } //-------------------------------------------------------------------------- // Reselect decay products momenta isotropically in phase space. // Does not redo secondary vertex position! void PhaseSpace::decayKinematicsStep( Event& process, int iRes) { // Multiplicity and mother mass and four-momentum. int i1 = process[iRes].daughter1(); int mult = process[iRes].daughter2() + 1 - i1; double m0 = process[iRes].m(); Vec4 pRes = process[iRes].p(); // Description of two-body decays as simple special case. if (mult == 2) { // Products and product masses. int i2 = i1 + 1; double m1t = process[i1].m(); double m2t = process[i2].m(); // Energies and absolute momentum in the rest frame. double e1 = 0.5 * (m0*m0 + m1t*m1t - m2t*m2t) / m0; double e2 = 0.5 * (m0*m0 + m2t*m2t - m1t*m1t) / m0; double p12 = 0.5 * sqrtpos( (m0 - m1t - m2t) * (m0 + m1t + m2t) * (m0 + m1t - m2t) * (m0 - m1t + m2t) ) / m0; // Pick isotropic angles to give three-momentum. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(1. - cosTheta*cosTheta); double phi12 = 2. * M_PI * rndmPtr->flat(); double pX = p12 * sinTheta * cos(phi12); double pY = p12 * sinTheta * sin(phi12); double pZ = p12 * cosTheta; // Fill four-momenta in mother rest frame and then boost to lab frame. Vec4 p1( pX, pY, pZ, e1); Vec4 p2( -pX, -pY, -pZ, e2); p1.bst( pRes ); p2.bst( pRes ); // Done for two-body decay. process[i1].p( p1 ); process[i2].p( p2 ); return; } // Description of three-body decays as semi-simple special case. if (mult == 3) { // Products and product masses. int i2 = i1 + 1; int i3 = i2 + 1; double m1t = process[i1].m(); double m2t = process[i2].m(); double m3t = process[i3].m(); double mDiff = m0 - (m1t + m2t + m3t); // Kinematical limits for 2+3 mass. Maximum phase-space weight. double m23Min = m2t + m3t; double m23Max = m0 - m1t; double p1Max = 0.5 * sqrtpos( (m0 - m1t - m23Min) * (m0 + m1t + m23Min) * (m0 + m1t - m23Min) * (m0 - m1t + m23Min) ) / m0; double p23Max = 0.5 * sqrtpos( (m23Max - m2t - m3t) * (m23Max + m2t + m3t) * (m23Max + m2t - m3t) * (m23Max - m2t + m3t) ) / m23Max; double wtPSmax = 0.5 * p1Max * p23Max; // Pick an intermediate mass m23 flat in the allowed range. double wtPS, m23, p1Abs, p23Abs; do { m23 = m23Min + rndmPtr->flat() * mDiff; // Translate into relative momenta and find phase-space weight. p1Abs = 0.5 * sqrtpos( (m0 - m1t - m23) * (m0 + m1t + m23) * (m0 + m1t - m23) * (m0 - m1t + m23) ) / m0; p23Abs = 0.5 * sqrtpos( (m23 - m2t - m3t) * (m23 + m2t + m3t) * (m23 + m2t - m3t) * (m23 - m2t + m3t) ) / m23; wtPS = p1Abs * p23Abs; // If rejected, try again with new invariant masses. } while ( wtPS < rndmPtr->flat() * wtPSmax ); // Set up m23 -> m2 + m3 isotropic in its rest frame. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(1. - cosTheta*cosTheta); double phi23 = 2. * M_PI * rndmPtr->flat(); double pX = p23Abs * sinTheta * cos(phi23); double pY = p23Abs * sinTheta * sin(phi23); double pZ = p23Abs * cosTheta; double e2 = sqrt( m2t*m2t + p23Abs*p23Abs); double e3 = sqrt( m3t*m3t + p23Abs*p23Abs); Vec4 p2( pX, pY, pZ, e2); Vec4 p3( -pX, -pY, -pZ, e3); // Set up 0 -> 1 + 23 isotropic in its rest frame. cosTheta = 2. * rndmPtr->flat() - 1.; sinTheta = sqrt(1. - cosTheta*cosTheta); phi23 = 2. * M_PI * rndmPtr->flat(); pX = p1Abs * sinTheta * cos(phi23); pY = p1Abs * sinTheta * sin(phi23); pZ = p1Abs * cosTheta; double e1 = sqrt( m1t*m1t + p1Abs*p1Abs); double e23 = sqrt( m23*m23 + p1Abs*p1Abs); Vec4 p1( pX, pY, pZ, e1); // Boost 2 + 3 to the 0 rest frame and then boost to lab frame. Vec4 p23( -pX, -pY, -pZ, e23); p2.bst( p23 ); p3.bst( p23 ); p1.bst( pRes ); p2.bst( pRes ); p3.bst( pRes ); // Done for three-body decay. process[i1].p( p1 ); process[i2].p( p2 ); process[i3].p( p3 ); return; } // Do a multibody decay using the M-generator algorithm. // Set up masses and four-momenta in a vector, with mother in slot 0. vector mProd; mProd.push_back( m0); for (int i = i1; i <= process[iRes].daughter2(); ++i) mProd.push_back( process[i].m() ); vector pProd; pProd.push_back( pRes); // Sum of daughter masses. double mSum = mProd[1]; for (int i = 2; i <= mult; ++i) mSum += mProd[i]; double mDiff = m0 - mSum; // Begin setup of intermediate invariant masses. vector mInv; for (int i = 0; i <= mult; ++i) mInv.push_back( mProd[i]); // Calculate the maximum weight in the decay. double wtPSmax = 1. / WTCORRECTION[mult]; double mMaxWT = mDiff + mProd[mult]; double mMinWT = 0.; for (int i = mult - 1; i > 0; --i) { mMaxWT += mProd[i]; mMinWT += mProd[i+1]; double mNow = mProd[i]; wtPSmax *= 0.5 * sqrtpos( (mMaxWT - mMinWT - mNow) * (mMaxWT + mMinWT + mNow) * (mMaxWT + mMinWT - mNow) * (mMaxWT - mMinWT + mNow) ) / mMaxWT; } // Begin loop to find the set of intermediate invariant masses. vector rndmOrd; double wtPS; do { wtPS = 1.; // Find and order random numbers in descending order. rndmOrd.resize(0); rndmOrd.push_back(1.); for (int i = 1; i < mult - 1; ++i) { double rndm = rndmPtr->flat(); rndmOrd.push_back(rndm); for (int j = i - 1; j > 0; --j) { if (rndm > rndmOrd[j]) swap( rndmOrd[j], rndmOrd[j+1] ); else break; } } rndmOrd.push_back(0.); // Translate into intermediate masses and find weight. for (int i = mult - 1; i > 0; --i) { mInv[i] = mInv[i+1] + mProd[i] + (rndmOrd[i-1] - rndmOrd[i]) * mDiff; wtPS *= 0.5 * sqrtpos( (mInv[i] - mInv[i+1] - mProd[i]) * (mInv[i] + mInv[i+1] + mProd[i]) * (mInv[i] + mInv[i+1] - mProd[i]) * (mInv[i] - mInv[i+1] + mProd[i]) ) / mInv[i]; } // If rejected, try again with new invariant masses. } while ( wtPS < rndmPtr->flat() * wtPSmax ); // Perform two-particle decays in the respective rest frame. vector pInv; pInv.resize(mult + 1); for (int i = 1; i < mult; ++i) { double p12 = 0.5 * sqrtpos( (mInv[i] - mInv[i+1] - mProd[i]) * (mInv[i] + mInv[i+1] + mProd[i]) * (mInv[i] + mInv[i+1] - mProd[i]) * (mInv[i] - mInv[i+1] + mProd[i]) ) / mInv[i]; // Isotropic angles give three-momentum. double cosTheta = 2. * rndmPtr->flat() - 1.; double sinTheta = sqrt(1. - cosTheta*cosTheta); double phiLoc = 2. * M_PI * rndmPtr->flat(); double pX = p12 * sinTheta * cos(phiLoc); double pY = p12 * sinTheta * sin(phiLoc); double pZ = p12 * cosTheta; // Calculate energies, fill four-momenta. double eHad = sqrt( mProd[i]*mProd[i] + p12*p12); double eInv = sqrt( mInv[i+1]*mInv[i+1] + p12*p12); pProd.push_back( Vec4( pX, pY, pZ, eHad) ); pInv[i+1].p( -pX, -pY, -pZ, eInv); } pProd.push_back( pInv[mult] ); // Boost decay products to the mother rest frame and on to lab frame. pInv[1] = pProd[0]; for (int iFrame = mult - 1; iFrame > 0; --iFrame) for (int i = iFrame; i <= mult; ++i) pProd[i].bst(pInv[iFrame]); // Done for multibody decay. for (int i = 1; i < mult; ++i) process[i1 + i - 1].p( pProd[i] ); return; } //-------------------------------------------------------------------------- // Determine how 3-body phase space should be sampled. void PhaseSpace::setup3Body() { // Check for massive t-channel propagator particles. int idTchan1 = abs( sigmaProcessPtr->idTchan1() ); int idTchan2 = abs( sigmaProcessPtr->idTchan2() ); mTchan1 = (idTchan1 == 0) ? pTHatMinDiverge : particleDataPtr->m0(idTchan1); mTchan2 = (idTchan2 == 0) ? pTHatMinDiverge : particleDataPtr->m0(idTchan2); sTchan1 = mTchan1 * mTchan1; sTchan2 = mTchan2 * mTchan2; // Find coefficients of different pT2 selection terms. Mirror choice. frac3Pow1 = sigmaProcessPtr->tChanFracPow1(); frac3Pow2 = sigmaProcessPtr->tChanFracPow2(); frac3Flat = 1. - frac3Pow1 - frac3Pow2; useMirrorWeight = sigmaProcessPtr->useMirrorWeight(); } //-------------------------------------------------------------------------- // Determine how phase space should be sampled. bool PhaseSpace::setupSampling123(bool is2, bool is3, ostream& os) { // Optional printout. if (showSearch) os << "\n PYTHIA Optimization printout for " << sigmaProcessPtr->name() << "\n \n" << scientific << setprecision(3); // Check that open range in tau (+ set tauMin, tauMax). if (!limitTau(is2, is3)) return false; // Reset coefficients and matrices of equation system to solve. int binTau[8], binY[8], binZ[8]; double vecTau[8], matTau[8][8], vecY[8], matY[8][8], vecZ[8], matZ[8][8]; for (int i = 0; i < 8; ++i) { tauCoef[i] = 0.; yCoef[i] = 0.; zCoef[i] = 0.; binTau[i] = 0; binY[i] = 0; binZ[i] = 0; vecTau[i] = 0.; vecY[i] = 0.; vecZ[i] = 0.; for (int j = 0; j < 8; ++j) { matTau[i][j] = 0.; matY[i][j] = 0.; matZ[i][j] = 0.; } } sigmaMx = 0.; sigmaNeg = 0.; // Number of used coefficients/points for each dimension: tau, y, c. nTau = (hasPointLeptons) ? 1 : 2; nY = (hasPointLeptons) ? 1 : 5; nZ = (is2) ? 5 : 1; // Identify if any resonances contribute in s-channel. idResA = sigmaProcessPtr->resonanceA(); if (idResA != 0) { mResA = particleDataPtr->m0(idResA); GammaResA = particleDataPtr->mWidth(idResA); if (mHatMin > mResA + WIDTHMARGIN * GammaResA || (mHatMax > 0. && mHatMax < mResA - WIDTHMARGIN * GammaResA) ) idResA = 0; } idResB = sigmaProcessPtr->resonanceB(); if (idResB != 0) { mResB = particleDataPtr->m0(idResB); GammaResB = particleDataPtr->mWidth(idResB); if (mHatMin > mResB + WIDTHMARGIN * GammaResB || (mHatMax > 0. && mHatMax < mResB - WIDTHMARGIN * GammaResB) ) idResB = 0; } if (idResA == 0 && idResB != 0) { idResA = idResB; mResA = mResB; GammaResA = GammaResB; idResB = 0; } // More sampling in tau if resonances in s-channel. if (idResA !=0 && !hasPointLeptons) { nTau += 2; tauResA = mResA * mResA / s; widResA = mResA * GammaResA / s; } if (idResB != 0 && !hasPointLeptons) { nTau += 2; tauResB = mResB * mResB / s; widResB = mResB * GammaResB / s; } // More sampling in tau (and different in y) if incoming lepton beams. if (hasLeptonBeams && !hasPointLeptons) ++nTau; // Special case when both resonances have same mass. sameResMass = false; if (idResB != 0 && abs(mResA - mResB) < SAMEMASS * (GammaResA + GammaResB)) sameResMass = true; // Default z value and weight required for 2 -> 1. Number of dimensions. z = 0.; wtZ = 1.; int nVar = (is2) ? 3 : 2; // Initial values, to be modified later. tauCoef[0] = 1.; yCoef[1] = 0.5; yCoef[2] = 0.5; zCoef[0] = 1.; // Step through grid in tau. Set limits on y and z generation. for (int iTau = 0; iTau < nTau; ++iTau) { double posTau = 0.5; if (sameResMass && iTau > 1 && iTau < 6) posTau = (iTau < 4) ? 0.4 : 0.6; selectTau( iTau, posTau, is2); if (!limitY()) continue; if (is2 && !limitZ()) continue; // Step through grids in y and z. for (int iY = 0; iY < nY; ++iY) { selectY( iY, 0.5); for (int iZ = 0; iZ < nZ; ++iZ) { if (is2) selectZ( iZ, 0.5); double sigmaTmp = 0.; // 2 -> 1: calculate cross section, weighted by phase-space volume. if (!is2 && !is3) { sigmaProcessPtr->set1Kin( x1H, x2H, sH); sigmaTmp = sigmaProcessPtr->sigmaPDF(); sigmaTmp *= wtTau * wtY; // 2 -> 2: calculate cross section, weighted by phase-space volume // and Breit-Wigners for masses } else if (is2) { sigmaProcessPtr->set2Kin( x1H, x2H, sH, tH, m3, m4, runBW3H, runBW4H); sigmaTmp = sigmaProcessPtr->sigmaPDF(); sigmaTmp *= wtTau * wtY * wtZ * wtBW; // 2 -> 3: repeat internal 3-body phase space several times and // keep maximal cross section, weighted by phase-space volume // and Breit-Wigners for masses } else if (is3) { for (int iTry3 = 0; iTry3 < NTRY3BODY; ++iTry3) { if (!select3Body()) continue; sigmaProcessPtr->set3Kin( x1H, x2H, sH, p3cm, p4cm, p5cm, m3, m4, m5, runBW3H, runBW4H, runBW5H); double sigmaTry = sigmaProcessPtr->sigmaPDF(); sigmaTry *= wtTau * wtY * wt3Body * wtBW; if (sigmaTry > sigmaTmp) sigmaTmp = sigmaTry; } } // Allow possibility for user to modify cross section. (3body??) if (canModifySigma) sigmaTmp *= userHooksPtr->multiplySigmaBy( sigmaProcessPtr, this, false); if (canBiasSelection) sigmaTmp *= userHooksPtr->biasSelectionBy( sigmaProcessPtr, this, false); if (canBias2Sel) sigmaTmp *= pow( pTH / bias2SelRef, bias2SelPow); // Check if current maximum exceeded. if (sigmaTmp > sigmaMx) sigmaMx = sigmaTmp; // Optional printout. Protect against negative cross sections. if (showSearch) os << " tau =" << setw(11) << tau << " y =" << setw(11) << y << " z =" << setw(11) << z << " sigma =" << setw(11) << sigmaTmp << "\n"; if (sigmaTmp < 0.) sigmaTmp = 0.; // Sum up tau cross-section pieces in points used. if (!hasPointLeptons) { binTau[iTau] += 1; vecTau[iTau] += sigmaTmp; matTau[iTau][0] += 1. / intTau0; matTau[iTau][1] += (1. / intTau1) / tau; if (idResA != 0) { matTau[iTau][2] += (1. / intTau2) / (tau + tauResA); matTau[iTau][3] += (1. / intTau3) * tau / ( pow2(tau - tauResA) + pow2(widResA) ); } if (idResB != 0) { matTau[iTau][4] += (1. / intTau4) / (tau + tauResB); matTau[iTau][5] += (1. / intTau5) * tau / ( pow2(tau - tauResB) + pow2(widResB) ); } if (hasLeptonBeams) matTau[iTau][nTau - 1] += (1. / intTau6) * tau / max( LEPTONTAUMIN, 1. - tau); } // Sum up y cross-section pieces in points used. if (!hasPointLeptons) { binY[iY] += 1; vecY[iY] += sigmaTmp; matY[iY][0] += (yMax / intY0) / cosh(y); matY[iY][1] += (yMax / intY12) * (y + yMax); matY[iY][2] += (yMax / intY12) * (yMax - y); if (!hasLeptonBeams) { matY[iY][3] += (yMax / intY34) * exp(y); matY[iY][4] += (yMax / intY34) * exp(-y); } else { matY[iY][3] += (yMax / intY56) / max( LEPTONXMIN, 1. - exp( y - yMax) ); matY[iY][4] += (yMax / intY56) / max( LEPTONXMIN, 1. - exp(-y - yMax) ); } } // Integrals over z expressions at tauMax, to be used below. if (is2) { double p2AbsMax = 0.25 * (pow2(tauMax * s - s3 - s4) - 4. * s3 * s4) / (tauMax * s); double zMaxMax = sqrtpos( 1. - pT2HatMin / p2AbsMax ); double zPosMaxMax = max(ratio34, unity34 + zMaxMax); double zNegMaxMax = max(ratio34, unity34 - zMaxMax); double intZ0Max = 2. * zMaxMax; double intZ12Max = log( zPosMaxMax / zNegMaxMax); double intZ34Max = 1. / zNegMaxMax - 1. / zPosMaxMax; // Sum up z cross-section pieces in points used. binZ[iZ] += 1; vecZ[iZ] += sigmaTmp; matZ[iZ][0] += 1.; matZ[iZ][1] += (intZ0Max / intZ12Max) / zNeg; matZ[iZ][2] += (intZ0Max / intZ12Max) / zPos; matZ[iZ][3] += (intZ0Max / intZ34Max) / pow2(zNeg); matZ[iZ][4] += (intZ0Max / intZ34Max) / pow2(zPos); } // End of loops over phase space points. } } } // Fail if no non-vanishing cross sections. if (sigmaMx <= 0.) { sigmaMx = 0.; return false; } // Solve respective equation system for better phase space coefficients. if (!hasPointLeptons) solveSys( nTau, binTau, vecTau, matTau, tauCoef); if (!hasPointLeptons) solveSys( nY, binY, vecY, matY, yCoef); if (is2) solveSys( nZ, binZ, vecZ, matZ, zCoef); if (showSearch) os << "\n"; // Provide cumulative sum of coefficients. tauCoefSum[0] = tauCoef[0]; yCoefSum[0] = yCoef[0]; zCoefSum[0] = zCoef[0]; for (int i = 1; i < 8; ++ i) { tauCoefSum[i] = tauCoefSum[i - 1] + tauCoef[i]; yCoefSum[i] = yCoefSum[i - 1] + yCoef[i]; zCoefSum[i] = zCoefSum[i - 1] + zCoef[i]; } // The last element should be > 1 to be on safe side in selection below. tauCoefSum[nTau - 1] = 2.; yCoefSum[nY - 1] = 2.; zCoefSum[nZ - 1] = 2.; // Begin find two most promising maxima among same points as before. int iMaxTau[NMAXTRY + 2], iMaxY[NMAXTRY + 2], iMaxZ[NMAXTRY + 2]; double sigMax[NMAXTRY + 2]; int nMax = 0; // Scan same grid as before in tau, y, z. for (int iTau = 0; iTau < nTau; ++iTau) { double posTau = 0.5; if (sameResMass && iTau > 1 && iTau < 6) posTau = (iTau < 4) ? 0.4 : 0.6; selectTau( iTau, posTau, is2); if (!limitY()) continue; if (is2 && !limitZ()) continue; for (int iY = 0; iY < nY; ++iY) { selectY( iY, 0.5); for (int iZ = 0; iZ < nZ; ++iZ) { if (is2) selectZ( iZ, 0.5); double sigmaTmp = 0.; // 2 -> 1: calculate cross section, weighted by phase-space volume. if (!is2 && !is3) { sigmaProcessPtr->set1Kin( x1H, x2H, sH); sigmaTmp = sigmaProcessPtr->sigmaPDF(); sigmaTmp *= wtTau * wtY; // 2 -> 2: calculate cross section, weighted by phase-space volume // and Breit-Wigners for masses } else if (is2) { sigmaProcessPtr->set2Kin( x1H, x2H, sH, tH, m3, m4, runBW3H, runBW4H); sigmaTmp = sigmaProcessPtr->sigmaPDF(); sigmaTmp *= wtTau * wtY * wtZ * wtBW; // 2 -> 3: repeat internal 3-body phase space several times and // keep maximal cross section, weighted by phase-space volume // and Breit-Wigners for masses } else if (is3) { for (int iTry3 = 0; iTry3 < NTRY3BODY; ++iTry3) { if (!select3Body()) continue; sigmaProcessPtr->set3Kin( x1H, x2H, sH, p3cm, p4cm, p5cm, m3, m4, m5, runBW3H, runBW4H, runBW5H); double sigmaTry = sigmaProcessPtr->sigmaPDF(); sigmaTry *= wtTau * wtY * wt3Body * wtBW; if (sigmaTry > sigmaTmp) sigmaTmp = sigmaTry; } } // Allow possibility for user to modify cross section. (3body??) if (canModifySigma) sigmaTmp *= userHooksPtr->multiplySigmaBy( sigmaProcessPtr, this, false); if (canBiasSelection) sigmaTmp *= userHooksPtr->biasSelectionBy( sigmaProcessPtr, this, false); if (canBias2Sel) sigmaTmp *= pow( pTH / bias2SelRef, bias2SelPow); // Optional printout. Protect against negative cross section. if (showSearch) os << " tau =" << setw(11) << tau << " y =" << setw(11) << y << " z =" << setw(11) << z << " sigma =" << setw(11) << sigmaTmp << "\n"; if (sigmaTmp < 0.) sigmaTmp = 0.; // Check that point is not simply mirror of already found one. bool mirrorPoint = false; for (int iMove = 0; iMove < nMax; ++iMove) if (abs(sigmaTmp - sigMax[iMove]) < SAMESIGMA * (sigmaTmp + sigMax[iMove])) mirrorPoint = true; // Add to or insert in maximum list. Only first two count. if (!mirrorPoint) { int iInsert = 0; for (int iMove = nMax - 1; iMove >= -1; --iMove) { iInsert = iMove + 1; if (iInsert == 0 || sigmaTmp < sigMax[iMove]) break; iMaxTau[iMove + 1] = iMaxTau[iMove]; iMaxY[iMove + 1] = iMaxY[iMove]; iMaxZ[iMove + 1] = iMaxZ[iMove]; sigMax[iMove + 1] = sigMax[iMove]; } iMaxTau[iInsert] = iTau; iMaxY[iInsert] = iY; iMaxZ[iInsert] = iZ; sigMax[iInsert] = sigmaTmp; if (nMax < NMAXTRY) ++nMax; } // Found two most promising maxima. } } } if (showSearch) os << "\n"; // Read out starting position for search. sigmaMx = sigMax[0]; int beginVar = (hasPointLeptons) ? 2 : 0; for (int iMax = 0; iMax < nMax; ++iMax) { int iTau = iMaxTau[iMax]; int iY = iMaxY[iMax]; int iZ = iMaxZ[iMax]; double tauVal = 0.5; double yVal = 0.5; double zVal = 0.5; int iGrid; double varVal, varNew, deltaVar, marginVar, sigGrid[3]; // Starting point and step size in parameter space. for (int iRepeat = 0; iRepeat < 2; ++iRepeat) { // Run through (possibly a subset of) tau, y and z. for (int iVar = beginVar; iVar < nVar; ++iVar) { if (iVar == 0) varVal = tauVal; else if (iVar == 1) varVal = yVal; else varVal = zVal; deltaVar = (iRepeat == 0) ? 0.1 : max( 0.01, min( 0.05, min( varVal - 0.02, 0.98 - varVal) ) ); marginVar = (iRepeat == 0) ? 0.02 : 0.002; int moveStart = (iRepeat == 0 && iVar == 0) ? 0 : 1; for (int move = moveStart; move < 9; ++move) { // Define new parameter-space point by step in one dimension. if (move == 0) { iGrid = 1; varNew = varVal; } else if (move == 1) { iGrid = 2; varNew = varVal + deltaVar; } else if (move == 2) { iGrid = 0; varNew = varVal - deltaVar; } else if (sigGrid[2] >= max( sigGrid[0], sigGrid[1]) && varVal + 2. * deltaVar < 1. - marginVar) { varVal += deltaVar; sigGrid[0] = sigGrid[1]; sigGrid[1] = sigGrid[2]; iGrid = 2; varNew = varVal + deltaVar; } else if (sigGrid[0] >= max( sigGrid[1], sigGrid[2]) && varVal - 2. * deltaVar > marginVar) { varVal -= deltaVar; sigGrid[2] = sigGrid[1]; sigGrid[1] = sigGrid[0]; iGrid = 0; varNew = varVal - deltaVar; } else if (sigGrid[2] >= sigGrid[0]) { deltaVar *= 0.5; varVal += deltaVar; sigGrid[0] = sigGrid[1]; iGrid = 1; varNew = varVal; } else { deltaVar *= 0.5; varVal -= deltaVar; sigGrid[2] = sigGrid[1]; iGrid = 1; varNew = varVal; } // Convert to relevant variables and find derived new limits. bool insideLimits = true; if (iVar == 0) { tauVal = varNew; selectTau( iTau, tauVal, is2); if (!limitY()) insideLimits = false; if (is2 && !limitZ()) insideLimits = false; if (insideLimits) { selectY( iY, yVal); if (is2) selectZ( iZ, zVal); } } else if (iVar == 1) { yVal = varNew; selectY( iY, yVal); } else if (iVar == 2) { zVal = varNew; selectZ( iZ, zVal); } // Evaluate cross-section. double sigmaTmp = 0.; if (insideLimits) { // 2 -> 1: calculate cross section, weighted by phase-space volume. if (!is2 && !is3) { sigmaProcessPtr->set1Kin( x1H, x2H, sH); sigmaTmp = sigmaProcessPtr->sigmaPDF(); sigmaTmp *= wtTau * wtY; // 2 -> 2: calculate cross section, weighted by phase-space volume // and Breit-Wigners for masses } else if (is2) { sigmaProcessPtr->set2Kin( x1H, x2H, sH, tH, m3, m4, runBW3H, runBW4H); sigmaTmp = sigmaProcessPtr->sigmaPDF(); sigmaTmp *= wtTau * wtY * wtZ * wtBW; // 2 -> 3: repeat internal 3-body phase space several times and // keep maximal cross section, weighted by phase-space volume // and Breit-Wigners for masses } else if (is3) { for (int iTry3 = 0; iTry3 < NTRY3BODY; ++iTry3) { if (!select3Body()) continue; sigmaProcessPtr->set3Kin( x1H, x2H, sH, p3cm, p4cm, p5cm, m3, m4, m5, runBW3H, runBW4H, runBW5H); double sigmaTry = sigmaProcessPtr->sigmaPDF(); sigmaTry *= wtTau * wtY * wt3Body * wtBW; if (sigmaTry > sigmaTmp) sigmaTmp = sigmaTry; } } // Allow possibility for user to modify cross section. if (canModifySigma) sigmaTmp *= userHooksPtr->multiplySigmaBy( sigmaProcessPtr, this, false); if (canBiasSelection) sigmaTmp *= userHooksPtr->biasSelectionBy( sigmaProcessPtr, this, false); if (canBias2Sel) sigmaTmp *= pow( pTH / bias2SelRef, bias2SelPow); // Optional printout. Protect against negative cross section. if (showSearch) os << " tau =" << setw(11) << tau << " y =" << setw(11) << y << " z =" << setw(11) << z << " sigma =" << setw(11) << sigmaTmp << "\n"; if (sigmaTmp < 0.) sigmaTmp = 0.; } // Save new maximum. Final maximum. sigGrid[iGrid] = sigmaTmp; if (sigmaTmp > sigmaMx) sigmaMx = sigmaTmp; } } } } sigmaMx *= SAFETYMARGIN; sigmaPos = sigmaMx; // Optional printout. if (showSearch) os << "\n Final maximum = " << setw(11) << sigmaMx << endl; // Done. return true; } //-------------------------------------------------------------------------- // Select a trial kinematics phase space point. // Note: by In is meant the integral over the quantity multiplying // coefficient cn. The sum of cn is normalized to unity. bool PhaseSpace::trialKin123(bool is2, bool is3, bool inEvent, ostream& os) { // Allow for possibility that energy varies from event to event. if (doEnergySpread) { eCM = infoPtr->eCM(); s = eCM * eCM; // Find shifted tauRes values. if (idResA !=0 && !hasPointLeptons) { tauResA = mResA * mResA / s; widResA = mResA * GammaResA / s; } if (idResB != 0 && !hasPointLeptons) { tauResB = mResB * mResB / s; widResB = mResB * GammaResB / s; } } // Choose tau according to h1(tau)/tau, where // h1(tau) = c0/I0 + (c1/I1) * 1/tau // + (c2/I2) / (tau + tauResA) // + (c3/I3) * tau / ((tau - tauResA)^2 + widResA^2) // + (c4/I4) / (tau + tauResB) // + (c5/I5) * tau / ((tau - tauResB)^2 + widResB^2) // + (c6/I6) * tau / (1 - tau). if (!limitTau(is2, is3)) return false; int iTau = 0; if (!hasPointLeptons) { double rTau = rndmPtr->flat(); while (rTau > tauCoefSum[iTau]) ++iTau; } selectTau( iTau, rndmPtr->flat(), is2); // Choose y according to h2(y), where // h2(y) = (c0/I0) * 1/cosh(y) // + (c1/I1) * (y-ymin) + (c2/I2) * (ymax-y) // + (c3/I3) * exp(y) + (c4/i4) * exp(-y) (for hadron; for lepton instead) // + (c5/I5) * 1 / (1 - exp(y-ymax)) + (c6/I6) * 1 / (1 - exp(ymin-y)). if (!limitY()) return false; int iY = 0; if (!hasPointLeptons) { double rY = rndmPtr->flat(); while (rY > yCoefSum[iY]) ++iY; } selectY( iY, rndmPtr->flat()); // Choose z = cos(thetaHat) according to h3(z), where // h3(z) = c0/I0 + (c1/I1) * 1/(A - z) + (c2/I2) * 1/(A + z) // + (c3/I3) * 1/(A - z)^2 + (c4/I4) * 1/(A + z)^2, // where A = 1 + 2*(m3*m4/sH)^2 (= 1 for massless products). if (is2) { if (!limitZ()) return false; int iZ = 0; double rZ = rndmPtr->flat(); while (rZ > zCoefSum[iZ]) ++iZ; selectZ( iZ, rndmPtr->flat()); } // 2 -> 1: calculate cross section, weighted by phase-space volume. if (!is2 && !is3) { sigmaProcessPtr->set1Kin( x1H, x2H, sH); sigmaNw = sigmaProcessPtr->sigmaPDF(); sigmaNw *= wtTau * wtY; // 2 -> 2: calculate cross section, weighted by phase-space volume // and Breit-Wigners for masses } else if (is2) { sigmaProcessPtr->set2Kin( x1H, x2H, sH, tH, m3, m4, runBW3H, runBW4H); sigmaNw = sigmaProcessPtr->sigmaPDF(); sigmaNw *= wtTau * wtY * wtZ * wtBW; // 2 -> 3: also sample internal 3-body phase, weighted by // 2 -> 1 phase-space volume and Breit-Wigners for masses } else if (is3) { if (!select3Body()) sigmaNw = 0.; else { sigmaProcessPtr->set3Kin( x1H, x2H, sH, p3cm, p4cm, p5cm, m3, m4, m5, runBW3H, runBW4H, runBW5H); sigmaNw = sigmaProcessPtr->sigmaPDF(); sigmaNw *= wtTau * wtY * wt3Body * wtBW; } } // Allow possibility for user to modify cross section. if (canModifySigma) sigmaNw *= userHooksPtr->multiplySigmaBy( sigmaProcessPtr, this, inEvent); if (canBiasSelection) sigmaNw *= userHooksPtr->biasSelectionBy( sigmaProcessPtr, this, inEvent); if (canBias2Sel) sigmaNw *= pow( pTH / bias2SelRef, bias2SelPow); // Check if maximum violated. newSigmaMx = false; if (sigmaNw > sigmaMx) { infoPtr->errorMsg("Warning in PhaseSpace2to2tauyz::trialKin: " "maximum for cross section violated"); // Violation strategy 1: increase maximum (always during initialization). if (increaseMaximum || !inEvent) { double violFact = SAFETYMARGIN * sigmaNw / sigmaMx; sigmaMx = SAFETYMARGIN * sigmaNw; newSigmaMx = true; if (showViolation) { if (violFact < 9.99) os << fixed; else os << scientific; os << " PYTHIA Maximum for " << sigmaProcessPtr->name() << " increased by factor " << setprecision(3) << violFact << " to " << scientific << sigmaMx << endl; } // Violation strategy 2: weight event (done in ProcessContainer). } else if (showViolation && sigmaNw > sigmaPos) { double violFact = sigmaNw / sigmaMx; if (violFact < 9.99) os << fixed; else os << scientific; os << " PYTHIA Maximum for " << sigmaProcessPtr->name() << " exceeded by factor " << setprecision(3) << violFact << endl; sigmaPos = sigmaNw; } } // Check if negative cross section. if (sigmaNw < sigmaNeg) { infoPtr->errorMsg("Warning in PhaseSpace2to2tauyz::trialKin:" " negative cross section set 0", "for " + sigmaProcessPtr->name() ); sigmaNeg = sigmaNw; // Optional printout of (all) violations. if (showViolation) os << " PYTHIA Negative minimum for " << sigmaProcessPtr->name() << " changed to " << scientific << setprecision(3) << sigmaNeg << endl; } if (sigmaNw < 0.) sigmaNw = 0.; // Set event weight, where relevant. biasWt = (canBiasSelection) ? userHooksPtr->biasedSelectionWeight() : 1.; if (canBias2Sel) biasWt /= pow( pTH / bias2SelRef, bias2SelPow); // Done. return true; } //-------------------------------------------------------------------------- // Find range of allowed tau values. bool PhaseSpace::limitTau(bool is2, bool is3) { // Trivial reply for unresolved lepton beams. if (hasPointLeptons) { tauMin = 1.; tauMax = 1.; return true; } // Requirements from allowed mHat range. tauMin = sHatMin / s; tauMax = (mHatMax < mHatMin) ? 1. : min( 1., sHatMax / s); // Requirements from allowed pT range and masses. if (is2 || is3) { double mT3Min = sqrt(s3 + pT2HatMin); double mT4Min = sqrt(s4 + pT2HatMin); double mT5Min = (is3) ? sqrt(s5 + pT2HatMin) : 0.; tauMin = max( tauMin, pow2(mT3Min + mT4Min + mT5Min) / s); } // Check that there is an open range. return (tauMax > tauMin); } //-------------------------------------------------------------------------- // Find range of allowed y values. bool PhaseSpace::limitY() { // Trivial reply for unresolved lepton beams. if (hasPointLeptons) { yMax = 1.; return true; } // Requirements from selected tau value. yMax = -0.5 * log(tau); // For lepton beams requirements from cutoff for f_e^e. double yMaxMargin = (hasLeptonBeams) ? yMax + LEPTONXLOGMAX : yMax; // Check that there is an open range. return (yMaxMargin > 0.); } //-------------------------------------------------------------------------- // Find range of allowed z = cos(theta) values. bool PhaseSpace::limitZ() { // Default limits. zMin = 0.; zMax = 1.; // Requirements from pTHat limits. zMax = sqrtpos( 1. - pT2HatMin / p2Abs ); if (pTHatMax > pTHatMin) zMin = sqrtpos( 1. - pT2HatMax / p2Abs ); // Check that there is an open range. return (zMax > zMin); } //-------------------------------------------------------------------------- // Select tau according to a choice of shapes. void PhaseSpace::selectTau(int iTau, double tauVal, bool is2) { // Trivial reply for unresolved lepton beams. if (hasPointLeptons) { tau = 1.; wtTau = 1.; sH = s; mHat = sqrt(sH); if (is2) { p2Abs = 0.25 * (pow2(sH - s3 - s4) - 4. * s3 * s4) / sH; pAbs = sqrtpos( p2Abs ); } return; } // Contributions from s-channel resonances. double tRatA = 0.; double aLowA = 0.; double aUppA = 0.; if (idResA !=0) { tRatA = ((tauResA + tauMax) / (tauResA + tauMin)) * (tauMin / tauMax); aLowA = atan( (tauMin - tauResA) / widResA); aUppA = atan( (tauMax - tauResA) / widResA); } double tRatB = 0.; double aLowB = 0.; double aUppB = 0.; if (idResB != 0) { tRatB = ((tauResB + tauMax) / (tauResB + tauMin)) * (tauMin / tauMax); aLowB = atan( (tauMin - tauResB) / widResB); aUppB = atan( (tauMax - tauResB) / widResB); } // Contributions from 1 / (1 - tau) for lepton beams. double aLowT = 0.; double aUppT = 0.; if (hasLeptonBeams) { aLowT = log( max( LEPTONTAUMIN, 1. - tauMin) ); aUppT = log( max( LEPTONTAUMIN, 1. - tauMax) ); intTau6 = aLowT - aUppT; } // Select according to 1/tau or 1/tau^2. if (iTau == 0) tau = tauMin * pow( tauMax / tauMin, tauVal); else if (iTau == 1) tau = tauMax * tauMin / (tauMin + (tauMax - tauMin) * tauVal); // Select according to 1 / (1 - tau) for lepton beams. else if (hasLeptonBeams && iTau == nTau - 1) tau = 1. - exp( aUppT + intTau6 * tauVal ); // Select according to 1 / (tau * (tau + tauRes)) or // 1 / ((tau - tauRes)^2 + widRes^2) for resonances A and B. else if (iTau == 2) tau = tauResA * tauMin / ((tauResA + tauMin) * pow( tRatA, tauVal) - tauMin); else if (iTau == 3) tau = tauResA + widResA * tan( aLowA + (aUppA - aLowA) * tauVal); else if (iTau == 4) tau = tauResB * tauMin / ((tauResB + tauMin) * pow( tRatB, tauVal) - tauMin); else if (iTau == 5) tau = tauResB + widResB * tan( aLowB + (aUppB - aLowB) * tauVal); // Phase space weight in tau. intTau0 = log( tauMax / tauMin); intTau1 = (tauMax - tauMin) / (tauMax * tauMin); double invWtTau = (tauCoef[0] / intTau0) + (tauCoef[1] / intTau1) / tau; if (idResA != 0) { intTau2 = -log(tRatA) / tauResA; intTau3 = (aUppA - aLowA) / widResA; invWtTau += (tauCoef[2] / intTau2) / (tau + tauResA) + (tauCoef[3] / intTau3) * tau / ( pow2(tau - tauResA) + pow2(widResA) ); } if (idResB != 0) { intTau4 = -log(tRatB) / tauResB; intTau5 = (aUppB - aLowB) / widResB; invWtTau += (tauCoef[4] / intTau4) / (tau + tauResB) + (tauCoef[5] / intTau5) * tau / ( pow2(tau - tauResB) + pow2(widResB) ); } if (hasLeptonBeams) invWtTau += (tauCoef[nTau - 1] / intTau6) * tau / max( LEPTONTAUMIN, 1. - tau); wtTau = 1. / invWtTau; // Calculate sHat and absolute momentum of outgoing partons. sH = tau * s; mHat = sqrt(sH); if (is2) { p2Abs = 0.25 * (pow2(sH - s3 - s4) - 4. * s3 * s4) / sH; pAbs = sqrtpos( p2Abs ); } } //-------------------------------------------------------------------------- // Select y according to a choice of shapes. void PhaseSpace::selectY(int iY, double yVal) { // Trivial reply for unresolved lepton beams. if (hasPointLeptons) { y = 0.; wtY = 1.; x1H = 1.; x2H = 1.; return; } // For lepton beams skip options 3&4 and go straight to 5&6. if (hasLeptonBeams && iY > 2) iY += 2; // Standard expressions used below. double expYMax = exp( yMax ); double expYMin = exp(-yMax ); double atanMax = atan( expYMax ); double atanMin = atan( expYMin ); double aUppY = (hasLeptonBeams) ? log( max( LEPTONXMIN, LEPTONXMAX / tau - 1. ) ) : 0.; double aLowY = LEPTONXLOGMIN; // 1 / cosh(y). if (iY == 0) y = log( tan( atanMin + (atanMax - atanMin) * yVal ) ); // y - y_min or mirrored y_max - y. else if (iY <= 2) y = yMax * (2. * sqrt(yVal) - 1.); // exp(y) or mirrored exp(-y). else if (iY <= 4) y = log( expYMin + (expYMax - expYMin) * yVal ); // 1 / (1 - exp(y - y_max)) or mirrored 1 / (1 - exp(y_min - y)). else y = yMax - log( 1. + exp(aLowY + (aUppY - aLowY) * yVal) ); // Mirror two cases. if (iY == 2 || iY == 4 || iY == 6) y = -y; // Phase space integral in y. intY0 = 2. * (atanMax - atanMin); intY12 = 0.5 * pow2(2. * yMax); intY34 = expYMax - expYMin; intY56 = aUppY - aLowY; double invWtY = (yCoef[0] / intY0) / cosh(y) + (yCoef[1] / intY12) * (y + yMax) + (yCoef[2] / intY12) * (yMax - y); if (!hasLeptonBeams) invWtY += (yCoef[3] / intY34) * exp(y) + (yCoef[4] / intY34) * exp(-y); else invWtY += (yCoef[3] / intY56) / max( LEPTONXMIN, 1. - exp( y - yMax) ) + (yCoef[4] / intY56) / max( LEPTONXMIN, 1. - exp(-y - yMax) ); wtY = 1. / invWtY; // Calculate x1 and x2. x1H = sqrt(tau) * exp(y); x2H = sqrt(tau) * exp(-y); } //-------------------------------------------------------------------------- // Select z = cos(theta) according to a choice of shapes. // The selection is split in the positive- and negative-z regions, // since a pTmax cut can remove the region around z = 0. void PhaseSpace::selectZ(int iZ, double zVal) { // Mass-dependent dampening of pT -> 0 limit. ratio34 = max(TINY, 2. * s3 * s4 / pow2(sH)); unity34 = 1. + ratio34; double ratiopT2 = 2. * pT2HatMin / max( SHATMINZ, sH); if (ratiopT2 < PT2RATMINZ) ratio34 = max( ratio34, ratiopT2); // Common expressions in z limits. double zPosMax = max(ratio34, unity34 + zMax); double zNegMax = max(ratio34, unity34 - zMax); double zPosMin = max(ratio34, unity34 + zMin); double zNegMin = max(ratio34, unity34 - zMin); // Flat in z. if (iZ == 0) { if (zVal < 0.5) z = -(zMax + (zMin - zMax) * 2. * zVal); else z = zMin + (zMax - zMin) * (2. * zVal - 1.); // 1 / (unity34 - z). } else if (iZ == 1) { double areaNeg = log(zPosMax / zPosMin); double areaPos = log(zNegMin / zNegMax); double area = areaNeg + areaPos; if (zVal * area < areaNeg) { double zValMod = zVal * area / areaNeg; z = unity34 - zPosMax * pow(zPosMin / zPosMax, zValMod); } else { double zValMod = (zVal * area - areaNeg)/ areaPos; z = unity34 - zNegMin * pow(zNegMax / zNegMin, zValMod); } // 1 / (unity34 + z). } else if (iZ == 2) { double areaNeg = log(zNegMin / zNegMax); double areaPos = log(zPosMax / zPosMin); double area = areaNeg + areaPos; if (zVal * area < areaNeg) { double zValMod = zVal * area / areaNeg; z = zNegMax * pow(zNegMin / zNegMax, zValMod) - unity34; } else { double zValMod = (zVal * area - areaNeg)/ areaPos; z = zPosMin * pow(zPosMax / zPosMin, zValMod) - unity34; } // 1 / (unity34 - z)^2. } else if (iZ == 3) { double areaNeg = 1. / zPosMin - 1. / zPosMax; double areaPos = 1. / zNegMax - 1. / zNegMin; double area = areaNeg + areaPos; if (zVal * area < areaNeg) { double zValMod = zVal * area / areaNeg; z = unity34 - 1. / (1./zPosMax + areaNeg * zValMod); } else { double zValMod = (zVal * area - areaNeg)/ areaPos; z = unity34 - 1. / (1./zNegMin + areaPos * zValMod); } // 1 / (unity34 + z)^2. } else if (iZ == 4) { double areaNeg = 1. / zNegMax - 1. / zNegMin; double areaPos = 1. / zPosMin - 1. / zPosMax; double area = areaNeg + areaPos; if (zVal * area < areaNeg) { double zValMod = zVal * area / areaNeg; z = 1. / (1./zNegMax - areaNeg * zValMod) - unity34; } else { double zValMod = (zVal * area - areaNeg)/ areaPos; z = 1. / (1./zPosMin - areaPos * zValMod) - unity34; } } // Safety check for roundoff errors. Combinations with z. if (z < 0.) z = min(-zMin, max(-zMax, z)); else z = min(zMax, max(zMin, z)); zNeg = max(ratio34, unity34 - z); zPos = max(ratio34, unity34 + z); // Phase space integral in z. double intZ0 = 2. * (zMax - zMin); double intZ12 = log( (zPosMax * zNegMin) / (zPosMin * zNegMax) ); double intZ34 = 1. / zPosMin - 1. / zPosMax + 1. / zNegMax - 1. / zNegMin; wtZ = mHat * pAbs / ( (zCoef[0] / intZ0) + (zCoef[1] / intZ12) / zNeg + (zCoef[2] / intZ12) / zPos + (zCoef[3] / intZ34) / pow2(zNeg) + (zCoef[4] / intZ34) / pow2(zPos) ); // Calculate tHat and uHat. Also gives pTHat. double sH34 = -0.5 * (sH - s3 - s4); tH = sH34 + mHat * pAbs * z; uH = sH34 - mHat * pAbs * z; pTH = sqrtpos( (tH * uH - s3 * s4) / sH); } //-------------------------------------------------------------------------- // Select three-body phase space according to a cylindrically based form // that can be chosen to favour low pT based on the form of propagators. bool PhaseSpace::select3Body() { // Upper and lower limits of pT choice for 4 and 5. double m35S = pow2(m3 + m5); double pT4Smax = 0.25 * ( pow2(sH - s4 - m35S) - 4. * s4 * m35S ) / sH; if (pTHatMax > pTHatMin) pT4Smax = min( pT2HatMax, pT4Smax); double pT4Smin = pT2HatMin; double m34S = pow2(m3 + m4); double pT5Smax = 0.25 * ( pow2(sH - s5 - m34S) - 4. * s5 * m34S ) / sH; if (pTHatMax > pTHatMin) pT5Smax = min( pT2HatMax, pT5Smax); double pT5Smin = pT2HatMin; // Check that pT ranges not closed. if ( pT4Smax < pow2(pTHatMin + MASSMARGIN) ) return false; if ( pT5Smax < pow2(pTHatMin + MASSMARGIN) ) return false; // Select pT4S according to c0 + c1/(M^2 + pT^2) + c2/(M^2 + pT^2)^2. double pTSmaxProp = pT4Smax + sTchan1; double pTSminProp = pT4Smin + sTchan1; double pTSratProp = pTSmaxProp / pTSminProp; double pTSdiff = pT4Smax - pT4Smin; double rShape = rndmPtr->flat(); double pT4S = 0.; if (rShape < frac3Flat) pT4S = pT4Smin + rndmPtr->flat() * pTSdiff; else if (rShape < frac3Flat + frac3Pow1) pT4S = max( pT2HatMin, pTSminProp * pow( pTSratProp, rndmPtr->flat() ) - sTchan1 ); else pT4S = max( pT2HatMin, pTSminProp * pTSmaxProp / (pTSminProp + rndmPtr->flat()* pTSdiff) - sTchan1 ); double wt4 = pTSdiff / ( frac3Flat + frac3Pow1 * pTSdiff / (log(pTSratProp) * (pT4S + sTchan1)) + frac3Pow2 * pTSminProp * pTSmaxProp / pow2(pT4S + sTchan1) ); // Select pT5S according to c0 + c1/(M^2 + pT^2) + c2/(M^2 + pT^2)^2. pTSmaxProp = pT5Smax + sTchan2; pTSminProp = pT5Smin + sTchan2; pTSratProp = pTSmaxProp / pTSminProp; pTSdiff = pT5Smax - pT5Smin; rShape = rndmPtr->flat(); double pT5S = 0.; if (rShape < frac3Flat) pT5S = pT5Smin + rndmPtr->flat() * pTSdiff; else if (rShape < frac3Flat + frac3Pow1) pT5S = max( pT2HatMin, pTSminProp * pow( pTSratProp, rndmPtr->flat() ) - sTchan2 ); else pT5S = max( pT2HatMin, pTSminProp * pTSmaxProp / (pTSminProp + rndmPtr->flat()* pTSdiff) - sTchan2 ); double wt5 = pTSdiff / ( frac3Flat + frac3Pow1 * pTSdiff / (log(pTSratProp) * (pT5S + sTchan2)) + frac3Pow2 * pTSminProp * pTSmaxProp / pow2(pT5S + sTchan2) ); // Select azimuthal angles and check that third pT in range. double phi4 = 2. * M_PI * rndmPtr->flat(); double phi5 = 2. * M_PI * rndmPtr->flat(); double pT3S = max( 0., pT4S + pT5S + 2. * sqrt(pT4S * pT5S) * cos(phi4 - phi5) ); if ( pT3S < pT2HatMin || (pTHatMax > pTHatMin && pT3S > pT2HatMax) ) return false; // Calculate transverse masses and check that phase space not closed. double sT3 = s3 + pT3S; double sT4 = s4 + pT4S; double sT5 = s5 + pT5S; double mT3 = sqrt(sT3); double mT4 = sqrt(sT4); double mT5 = sqrt(sT5); if ( mT3 + mT4 + mT5 + MASSMARGIN > mHat ) return false; // Select rapidity for particle 3 and check that phase space not closed. double m45S = pow2(mT4 + mT5); double y3max = log( ( sH + sT3 - m45S + sqrtpos( pow2(sH - sT3 - m45S) - 4 * sT3 * m45S ) ) / (2. * mHat * mT3) ); if (y3max < YRANGEMARGIN) return false; double y3 = (2. * rndmPtr->flat() - 1.) * (1. - YRANGEMARGIN) * y3max; double pz3 = mT3 * sinh(y3); double e3 = mT3 * cosh(y3); // Find momentum transfers in the two mirror solutions (in 4-5 frame). double pz45 = -pz3; double e45 = mHat - e3; double sT45 = e45 * e45 - pz45 * pz45; double lam45 = sqrtpos( pow2(sT45 - sT4 - sT5) - 4. * sT4 * sT5 ); if (lam45 < YRANGEMARGIN * sH) return false; double lam4e = sT45 + sT4 - sT5; double lam5e = sT45 + sT5 - sT4; double tFac = -0.5 * mHat / sT45; double t1Pos = tFac * (e45 - pz45) * (lam4e - lam45); double t1Neg = tFac * (e45 - pz45) * (lam4e + lam45); double t2Pos = tFac * (e45 + pz45) * (lam5e - lam45); double t2Neg = tFac * (e45 + pz45) * (lam5e + lam45); // Construct relative mirror weights and make choice. double wtPosUnnorm = 1.; double wtNegUnnorm = 1.; if (useMirrorWeight) { wtPosUnnorm = 1./ pow2( (t1Pos - sTchan1) * (t2Pos - sTchan2) ); wtNegUnnorm = 1./ pow2( (t1Neg - sTchan1) * (t2Neg - sTchan2) ); } double wtPos = wtPosUnnorm / (wtPosUnnorm + wtNegUnnorm); double wtNeg = wtNegUnnorm / (wtPosUnnorm + wtNegUnnorm); double epsilon = (rndmPtr->flat() < wtPos) ? 1. : -1.; // Construct four-vectors in rest frame of subprocess. double px4 = sqrt(pT4S) * cos(phi4); double py4 = sqrt(pT4S) * sin(phi4); double px5 = sqrt(pT5S) * cos(phi5); double py5 = sqrt(pT5S) * sin(phi5); double pz4 = 0.5 * (pz45 * lam4e + epsilon * e45 * lam45) / sT45; double pz5 = pz45 - pz4; double e4 = sqrt(sT4 + pz4 * pz4); double e5 = sqrt(sT5 + pz5 * pz5); p3cm = Vec4( -(px4 + px5), -(py4 + py5), pz3, e3); p4cm = Vec4( px4, py4, pz4, e4); p5cm = Vec4( px5, py5, pz5, e5); // Total weight to associate with kinematics choice. wt3Body = wt4 * wt5 * (2. * y3max) / (128. * pow3(M_PI) * lam45); wt3Body *= (epsilon > 0.) ? 1. / wtPos : 1. / wtNeg; // Cross section of form |M|^2/(2 sHat) dPS_3 so need 1/(2 sHat). wt3Body /= (2. * sH); // Done. return true; } //-------------------------------------------------------------------------- // Solve linear equation system for better phase space coefficients. void PhaseSpace::solveSys( int n, int bin[8], double vec[8], double mat[8][8], double coef[8], ostream& os) { // Optional printout. if (showSearch) { os << "\n Equation system: " << setw(5) << bin[0]; for (int j = 0; j < n; ++j) os << setw(12) << mat[0][j]; os << setw(12) << vec[0] << "\n"; for (int i = 1; i < n; ++i) { os << " " << setw(5) << bin[i]; for (int j = 0; j < n; ++j) os << setw(12) << mat[i][j]; os << setw(12) << vec[i] << "\n"; } } // Local variables. double vecNor[8], coefTmp[8]; for (int i = 0; i < n; ++i) coefTmp[i] = 0.; // Check if equation system solvable. bool canSolve = true; for (int i = 0; i < n; ++i) if (bin[i] == 0) canSolve = false; double vecSum = 0.; for (int i = 0; i < n; ++i) vecSum += vec[i]; if (abs(vecSum) < TINY) canSolve = false; // Solve to find relative importance of cross-section pieces. if (canSolve) { for (int i = 0; i < n; ++i) vecNor[i] = max( 0.1, vec[i] / vecSum); for (int k = 0; k < n - 1; ++k) { for (int i = k + 1; i < n; ++i) { if (abs(mat[k][k]) < TINY) {canSolve = false; break;} double ratio = mat[i][k] / mat[k][k]; vec[i] -= ratio * vec[k]; for (int j = k; j < n; ++j) mat[i][j] -= ratio * mat[k][j]; } if (!canSolve) break; } if (canSolve) { for (int k = n - 1; k >= 0; --k) { for (int j = k + 1; j < n; ++j) vec[k] -= mat[k][j] * coefTmp[j]; coefTmp[k] = vec[k] / mat[k][k]; } } } // Share evenly if failure. if (!canSolve) for (int i = 0; i < n; ++i) { coefTmp[i] = 1.; vecNor[i] = 0.1; if (vecSum > TINY) vecNor[i] = max(0.1, vec[i] / vecSum); } // Normalize coefficients, with piece shared democratically. double coefSum = 0.; vecSum = 0.; for (int i = 0; i < n; ++i) { coefTmp[i] = max( 0., coefTmp[i]); coefSum += coefTmp[i]; vecSum += vecNor[i]; } if (coefSum > 0.) for (int i = 0; i < n; ++i) coef[i] = EVENFRAC / n + (1. - EVENFRAC) * 0.5 * (coefTmp[i] / coefSum + vecNor[i] / vecSum); else for (int i = 0; i < n; ++i) coef[i] = 1. / n; // Optional printout. if (showSearch) { os << " Solution: "; for (int i = 0; i < n; ++i) os << setw(12) << coef[i]; os << "\n"; } } //-------------------------------------------------------------------------- // Setup mass selection for one resonance at a time - part 1. void PhaseSpace::setupMass1(int iM) { // Identity for mass seletion; is 0 also for light quarks (not yet selected). if (iM == 3) idMass[iM] = abs(sigmaProcessPtr->id3Mass()); if (iM == 4) idMass[iM] = abs(sigmaProcessPtr->id4Mass()); if (iM == 5) idMass[iM] = abs(sigmaProcessPtr->id5Mass()); // Masses and widths of resonances. if (idMass[iM] == 0) { mPeak[iM] = 0.; mWidth[iM] = 0.; mMin[iM] = 0.; mMax[iM] = 0.; } else { mPeak[iM] = particleDataPtr->m0(idMass[iM]); mWidth[iM] = particleDataPtr->mWidth(idMass[iM]); mMin[iM] = particleDataPtr->mMin(idMass[iM]); mMax[iM] = particleDataPtr->mMax(idMass[iM]); // gmZmode == 1 means pure photon propagator; set at lower mass limit. if (idMass[iM] == 23 && gmZmode == 1) mPeak[iM] = mMin[iM]; } // Mass and width combinations for Breit-Wigners. sPeak[iM] = mPeak[iM] * mPeak[iM]; useBW[iM] = useBreitWigners && (mWidth[iM] > minWidthBreitWigners); if (!useBW[iM]) mWidth[iM] = 0.; mw[iM] = mPeak[iM] * mWidth[iM]; wmRat[iM] = (idMass[iM] == 0 || mPeak[iM] == 0.) ? 0. : mWidth[iM] / mPeak[iM]; // Simple Breit-Wigner range, upper edge to be corrected subsequently. if (useBW[iM]) { mLower[iM] = mMin[iM]; mUpper[iM] = mHatMax; } } //-------------------------------------------------------------------------- // Setup mass selection for one resonance at a time - part 2. void PhaseSpace::setupMass2(int iM, double distToThresh) { // Store reduced Breit-Wigner range. if (mMax[iM] > mMin[iM]) mUpper[iM] = min( mUpper[iM], mMax[iM]); sLower[iM] = mLower[iM] * mLower[iM]; sUpper[iM] = mUpper[iM] * mUpper[iM]; // Prepare to select m3 by BW + flat + 1/s_3. // Determine relative coefficients by allowed mass range. if (distToThresh > THRESHOLDSIZE) { fracFlat[iM] = 0.1; fracInv[iM] = 0.1; } else if (distToThresh > - THRESHOLDSIZE) { fracFlat[iM] = 0.25 - 0.15 * distToThresh / THRESHOLDSIZE; fracInv [iM] = 0.15 - 0.05 * distToThresh / THRESHOLDSIZE; } else { fracFlat[iM] = 0.4; fracInv[iM] = 0.2; } // For gamma*/Z0: increase 1/s_i part and introduce 1/s_i^2 part. fracInv2[iM] = 0.; if (idMass[iM] == 23 && gmZmode == 0) { fracFlat[iM] *= 0.5; fracInv[iM] = 0.5 * fracInv[iM] + 0.25; fracInv2[iM] = 0.25; } else if (idMass[iM] == 23 && gmZmode == 1) { fracFlat[iM] = 0.1; fracInv[iM] = 0.4; fracInv2[iM] = 0.4; } // Normalization integrals for the respective contribution. atanLower[iM] = atan( (sLower[iM] - sPeak[iM])/ mw[iM] ); atanUpper[iM] = atan( (sUpper[iM] - sPeak[iM])/ mw[iM] ); intBW[iM] = atanUpper[iM] - atanLower[iM]; intFlat[iM] = sUpper[iM] - sLower[iM]; intInv[iM] = log( sUpper[iM] / sLower[iM] ); intInv2[iM] = 1./sLower[iM] - 1./sUpper[iM]; } //-------------------------------------------------------------------------- // Select Breit-Wigner-distributed or fixed masses. void PhaseSpace::trialMass(int iM) { // References to masses to be set. double& mSet = (iM == 3) ? m3 : ( (iM == 4) ? m4 : m5 ); double& sSet = (iM == 3) ? s3 : ( (iM == 4) ? s4 : s5 ); // Distribution for m_i is BW + flat + 1/s_i + 1/s_i^2. if (useBW[iM]) { double pickForm = rndmPtr->flat(); if (pickForm > fracFlat[iM] + fracInv[iM] + fracInv2[iM]) sSet = sPeak[iM] + mw[iM] * tan( atanLower[iM] + rndmPtr->flat() * intBW[iM] ); else if (pickForm > fracInv[iM] + fracInv2[iM]) sSet = sLower[iM] + rndmPtr->flat() * (sUpper[iM] - sLower[iM]); else if (pickForm > fracInv2[iM]) sSet = sLower[iM] * pow( sUpper[iM] / sLower[iM], rndmPtr->flat() ); else sSet = sLower[iM] * sUpper[iM] / (sLower[iM] + rndmPtr->flat() * (sUpper[iM] - sLower[iM])); mSet = sqrt(sSet); // Else m_i is fixed at peak value. } else { mSet = mPeak[iM]; sSet = sPeak[iM]; } } //-------------------------------------------------------------------------- // Naively a fixed-width Breit-Wigner is used to pick the mass. // Here come the correction factors for // (i) preselection according to BW + flat in s_i + 1/s_i + 1/s_i^2, // (ii) reduced allowed mass range, // (iii) running width, i.e. m0*Gamma0 -> s*Gamma0/m0. // In the end, the weighted distribution is a running-width BW. double PhaseSpace::weightMass(int iM) { // Reference to mass and to Breit-Wigner weight to be set. double& sSet = (iM == 3) ? s3 : ( (iM == 4) ? s4 : s5 ); double& runBWH = (iM == 3) ? runBW3H : ( (iM == 4) ? runBW4H : runBW5H ); // Default weight if no Breit-Wigner. runBWH = 1.; if (!useBW[iM]) return 1.; // Weight of generated distribution. double genBW = (1. - fracFlat[iM] - fracInv[iM] - fracInv2[iM]) * mw[iM] / ( (pow2(sSet - sPeak[iM]) + pow2(mw[iM])) * intBW[iM]) + fracFlat[iM] / intFlat[iM] + fracInv[iM] / (sSet * intInv[iM]) + fracInv2[iM] / (sSet*sSet * intInv2[iM]); // Weight of distribution with running width in Breit-Wigner. double mwRun = sSet * wmRat[iM]; runBWH = mwRun / (pow2(sSet - sPeak[iM]) + pow2(mwRun)) / M_PI; // Done. return (runBWH / genBW); } //========================================================================== // PhaseSpace2to1tauy class. // 2 -> 1 kinematics for normal subprocesses. //-------------------------------------------------------------------------- // Set limits for resonance mass selection. bool PhaseSpace2to1tauy::setupMass() { // Treat Z0 as such or as gamma*/Z0 gmZmode = gmZmodeGlobal; int gmZmodeProc = sigmaProcessPtr->gmZmode(); if (gmZmodeProc >= 0) gmZmode = gmZmodeProc; // Mass limits for current resonance. int idRes = abs(sigmaProcessPtr->resonanceA()); int idTmp = abs(sigmaProcessPtr->resonanceB()); if (idTmp > 0) idRes = idTmp; double mResMin = (idRes == 0) ? 0. : particleDataPtr->mMin(idRes); double mResMax = (idRes == 0) ? 0. : particleDataPtr->mMax(idRes); // Compare with global mass limits and pick tighter of them. mHatMin = max( mResMin, mHatGlobalMin); sHatMin = mHatMin*mHatMin; mHatMax = eCM; if (mResMax > mResMin) mHatMax = min( mHatMax, mResMax); if (mHatGlobalMax > mHatGlobalMin) mHatMax = min( mHatMax, mHatGlobalMax); sHatMax = mHatMax*mHatMax; // Default Breit-Wigner weight. wtBW = 1.; // Fail if mass window (almost) closed. return (mHatMax > mHatMin + MASSMARGIN); } //-------------------------------------------------------------------------- // Construct the four-vector kinematics from the trial values. bool PhaseSpace2to1tauy::finalKin() { // Particle masses; incoming always on mass shell. mH[1] = 0.; mH[2] = 0.; mH[3] = mHat; // Incoming partons along beam axes. Outgoing has sum of momenta. pH[1] = Vec4( 0., 0., 0.5 * eCM * x1H, 0.5 * eCM * x1H); pH[2] = Vec4( 0., 0., -0.5 * eCM * x2H, 0.5 * eCM * x2H); pH[3] = pH[1] + pH[2]; // Done. return true; } //========================================================================== // PhaseSpace2to2tauyz class. // 2 -> 2 kinematics for normal subprocesses. //-------------------------------------------------------------------------- // Set up for fixed or Breit-Wigner mass selection. bool PhaseSpace2to2tauyz::setupMasses() { // Treat Z0 as such or as gamma*/Z0 gmZmode = gmZmodeGlobal; int gmZmodeProc = sigmaProcessPtr->gmZmode(); if (gmZmodeProc >= 0) gmZmode = gmZmodeProc; // Set sHat limits - based on global limits only. mHatMin = mHatGlobalMin; sHatMin = mHatMin*mHatMin; mHatMax = eCM; if (mHatGlobalMax > mHatGlobalMin) mHatMax = min( eCM, mHatGlobalMax); sHatMax = mHatMax*mHatMax; // Masses and widths of resonances. setupMass1(3); setupMass1(4); // Reduced mass range when two massive particles. if (useBW[3]) mUpper[3] -= (useBW[4]) ? mMin[4] : mPeak[4]; if (useBW[4]) mUpper[4] -= (useBW[3]) ? mMin[3] : mPeak[3]; // If closed phase space then unallowed process. bool physical = true; if (useBW[3] && mUpper[3] < mLower[3] + MASSMARGIN) physical = false; if (useBW[4] && mUpper[4] < mLower[4] + MASSMARGIN) physical = false; if (!useBW[3] && !useBW[4] && mHatMax < mPeak[3] + mPeak[4] + MASSMARGIN) physical = false; if (!physical) return false; // If either particle is massless then need extra pTHat cut. pTHatMin = pTHatGlobalMin; if (mPeak[3] < pTHatMinDiverge || mPeak[4] < pTHatMinDiverge) pTHatMin = max( pTHatMin, pTHatMinDiverge); pT2HatMin = pTHatMin * pTHatMin; pTHatMax = pTHatGlobalMax; pT2HatMax = pTHatMax * pTHatMax; // Prepare to select m3 by BW + flat + 1/s_3. if (useBW[3]) { double distToThreshA = (mHatMax - mPeak[3] - mPeak[4]) * mWidth[3] / (pow2(mWidth[3]) + pow2(mWidth[4])); double distToThreshB = (mHatMax - mPeak[3] - mMin[4]) / mWidth[3]; double distToThresh = min( distToThreshA, distToThreshB); setupMass2(3, distToThresh); } // Prepare to select m4 by BW + flat + 1/s_4. if (useBW[4]) { double distToThreshA = (mHatMax - mPeak[3] - mPeak[4]) * mWidth[4] / (pow2(mWidth[3]) + pow2(mWidth[4])); double distToThreshB = (mHatMax - mMin[3] - mPeak[4]) / mWidth[4]; double distToThresh = min( distToThreshA, distToThreshB); setupMass2(4, distToThresh); } // Initialization masses. Special cases when constrained phase space. m3 = (useBW[3]) ? min(mPeak[3], mUpper[3]) : mPeak[3]; m4 = (useBW[4]) ? min(mPeak[4], mUpper[4]) : mPeak[4]; if (m3 + m4 + THRESHOLDSIZE * (mWidth[3] + mWidth[4]) + MASSMARGIN > mHatMax) { if (useBW[3] && useBW[4]) physical = constrainedM3M4(); else if (useBW[3]) physical = constrainedM3(); else if (useBW[4]) physical = constrainedM4(); } s3 = m3*m3; s4 = m4*m4; // Correct selected mass-spectrum to running-width Breit-Wigner. // Extra safety margin for maximum search. wtBW = 1.; if (useBW[3]) wtBW *= weightMass(3) * EXTRABWWTMAX; if (useBW[4]) wtBW *= weightMass(4) * EXTRABWWTMAX; // Done. return physical; } //-------------------------------------------------------------------------- // Select Breit-Wigner-distributed or fixed masses. bool PhaseSpace2to2tauyz::trialMasses() { // By default vanishing cross section. sigmaNw = 0.; wtBW = 1.; // Pick m3 and m4 independently. trialMass(3); trialMass(4); // If outside phase space then reject event. if (m3 + m4 + MASSMARGIN > mHatMax) return false; // Correct selected mass-spectrum to running-width Breit-Wigner. if (useBW[3]) wtBW *= weightMass(3); if (useBW[4]) wtBW *= weightMass(4); // Done. return true; } //-------------------------------------------------------------------------- // Construct the four-vector kinematics from the trial values. bool PhaseSpace2to2tauyz::finalKin() { // Assign masses to particles assumed massless in matrix elements. int id3 = sigmaProcessPtr->id(3); int id4 = sigmaProcessPtr->id(4); if (idMass[3] == 0) { m3 = particleDataPtr->m0(id3); s3 = m3*m3; } if (idMass[4] == 0) { m4 = particleDataPtr->m0(id4); s4 = m4*m4; } // Sometimes swap tHat <-> uHat to reflect chosen final-state order. if (sigmaProcessPtr->swappedTU()) { swap(tH, uH); z = -z; } // Check that phase space still open after new mass assignment. if (m3 + m4 + MASSMARGIN > mHat) { infoPtr->errorMsg("Warning in PhaseSpace2to2tauyz::finalKin: " "failed after mass assignment"); return false; } p2Abs = 0.25 * (pow2(sH - s3 - s4) - 4. * s3 * s4) / sH; pAbs = sqrtpos( p2Abs ); // Particle masses; incoming always on mass shell. mH[1] = 0.; mH[2] = 0.; mH[3] = m3; mH[4] = m4; // Incoming partons along beam axes. pH[1] = Vec4( 0., 0., 0.5 * eCM * x1H, 0.5 * eCM * x1H); pH[2] = Vec4( 0., 0., -0.5 * eCM * x2H, 0.5 * eCM * x2H); // Outgoing partons initially in collision CM frame along beam axes. pH[3] = Vec4( 0., 0., pAbs, 0.5 * (sH + s3 - s4) / mHat); pH[4] = Vec4( 0., 0., -pAbs, 0.5 * (sH + s4 - s3) / mHat); // Then rotate and boost them to overall CM frame. theta = acos(z); phi = 2. * M_PI * rndmPtr->flat(); betaZ = (x1H - x2H)/(x1H + x2H); pH[3].rot( theta, phi); pH[4].rot( theta, phi); pH[3].bst( 0., 0., betaZ); pH[4].bst( 0., 0., betaZ); pTH = pAbs * sin(theta); // Done. return true; } //-------------------------------------------------------------------------- // Special choice of m3 and m4 when mHatMax push them off mass shell. // Vary x in expression m3 + m4 = mHatMax - x * (Gamma3 + Gamma4). // For each x try to put either 3 or 4 as close to mass shell as possible. // Maximize BW_3 * BW_4 * beta_34, where latter approximate phase space. bool PhaseSpace2to2tauyz::constrainedM3M4() { // Initial values. bool foundNonZero = false; double wtMassMax = 0.; double m3WtMax = 0.; double m4WtMax = 0.; double xMax = (mHatMax - mLower[3] - mLower[4]) / (mWidth[3] + mWidth[4]); double xStep = THRESHOLDSTEP * min(1., xMax); double xNow = 0.; double wtMassXbin, wtMassMaxOld, m34, mT34Min, wtMassNow, wtBW3Now, wtBW4Now, beta34Now; // Step through increasing x values. do { xNow += xStep; wtMassXbin = 0.; wtMassMaxOld = wtMassMax; m34 = mHatMax - xNow * (mWidth[3] + mWidth[4]); // Study point where m3 as close as possible to on-shell. m3 = min( mUpper[3], m34 - mLower[4]); if (m3 > mPeak[3]) m3 = max( mLower[3], mPeak[3]); m4 = m34 - m3; if (m4 < mLower[4]) {m4 = mLower[4]; m3 = m34 - m4;} // Check that inside phase space limit set by pTmin. mT34Min = sqrt(m3*m3 + pT2HatMin) + sqrt(m4*m4 + pT2HatMin); if (mT34Min < mHatMax) { // Breit-Wigners and beta factor give total weight. wtMassNow = 0.; if (m3 > mLower[3] && m3 < mUpper[3] && m4 > mLower[4] && m4 < mUpper[4]) { wtBW3Now = mw[3] / ( pow2(m3*m3 - sPeak[3]) + pow2(mw[3]) ); wtBW4Now = mw[4] / ( pow2(m4*m4 - sPeak[4]) + pow2(mw[4]) ); beta34Now = sqrt( pow2(mHatMax*mHatMax - m3*m3 - m4*m4) - pow2(2. * m3 * m4) ) / (mHatMax*mHatMax); wtMassNow = wtBW3Now * wtBW4Now * beta34Now; } // Store new maximum, if any. if (wtMassNow > wtMassXbin) wtMassXbin = wtMassNow; if (wtMassNow > wtMassMax) { foundNonZero = true; wtMassMax = wtMassNow; m3WtMax = m3; m4WtMax = m4; } } // Study point where m4 as close as possible to on-shell. m4 = min( mUpper[4], m34 - mLower[3]); if (m4 > mPeak[4]) m4 = max( mLower[4], mPeak[4]); m3 = m34 - m4; if (m3 < mLower[3]) {m3 = mLower[3]; m4 = m34 - m3;} // Check that inside phase space limit set by pTmin. mT34Min = sqrt(m3*m3 + pT2HatMin) + sqrt(m4*m4 + pT2HatMin); if (mT34Min < mHatMax) { // Breit-Wigners and beta factor give total weight. wtMassNow = 0.; if (m3 > mLower[3] && m3 < mUpper[3] && m4 > mLower[4] && m4 < mUpper[4]) { wtBW3Now = mw[3] / ( pow2(m3*m3 - sPeak[3]) + pow2(mw[3]) ); wtBW4Now = mw[4] / ( pow2(m4*m4 - sPeak[4]) + pow2(mw[4]) ); beta34Now = sqrt( pow2(mHatMax*mHatMax - m3*m3 - m4*m4) - pow2(2. * m3 * m4) ) / (mHatMax*mHatMax); wtMassNow = wtBW3Now * wtBW4Now * beta34Now; } // Store new maximum, if any. if (wtMassNow > wtMassXbin) wtMassXbin = wtMassNow; if (wtMassNow > wtMassMax) { foundNonZero = true; wtMassMax = wtMassNow; m3WtMax = m3; m4WtMax = m4; } } // Continue stepping if increasing trend and more x range available. } while ( (!foundNonZero || wtMassXbin > wtMassMaxOld) && xNow < xMax - xStep); // Restore best values for subsequent maximization. Return. m3 = m3WtMax; m4 = m4WtMax; return foundNonZero; } //-------------------------------------------------------------------------- // Special choice of m3 when mHatMax pushes it off mass shell. // Vary x in expression m3 = mHatMax - m4 - x * Gamma3. // Maximize BW_3 * beta_34, where latter approximate phase space. bool PhaseSpace2to2tauyz::constrainedM3() { // Initial values. bool foundNonZero = false; double wtMassMax = 0.; double m3WtMax = 0.; double mT4Min = sqrt(m4*m4 + pT2HatMin); double xMax = (mHatMax - mLower[3] - m4) / mWidth[3]; double xStep = THRESHOLDSTEP * min(1., xMax); double xNow = 0.; double wtMassNow, mT34Min, wtBW3Now, beta34Now; // Step through increasing x values; gives m3 unambiguously. do { xNow += xStep; wtMassNow = 0.; m3 = mHatMax - m4 - xNow * mWidth[3]; // Check that inside phase space limit set by pTmin. mT34Min = sqrt(m3*m3 + pT2HatMin) + mT4Min; if (mT34Min < mHatMax) { // Breit-Wigner and beta factor give total weight. wtBW3Now = mw[3] / ( pow2(m3*m3 - sPeak[3]) + pow2(mw[3]) ); beta34Now = sqrt( pow2(mHatMax*mHatMax - m3*m3 - m4*m4) - pow2(2. * m3 * m4) ) / (mHatMax*mHatMax); wtMassNow = wtBW3Now * beta34Now; // Store new maximum, if any. if (wtMassNow > wtMassMax) { foundNonZero = true; wtMassMax = wtMassNow; m3WtMax = m3; } } // Continue stepping if increasing trend and more x range available. } while ( (!foundNonZero || wtMassNow > wtMassMax) && xNow < xMax - xStep); // Restore best value for subsequent maximization. Return. m3 = m3WtMax; return foundNonZero; } //-------------------------------------------------------------------------- // Special choice of m4 when mHatMax pushes it off mass shell. // Vary x in expression m4 = mHatMax - m3 - x * Gamma4. // Maximize BW_4 * beta_34, where latter approximate phase space. bool PhaseSpace2to2tauyz::constrainedM4() { // Initial values. bool foundNonZero = false; double wtMassMax = 0.; double m4WtMax = 0.; double mT3Min = sqrt(m3*m3 + pT2HatMin); double xMax = (mHatMax - mLower[4] - m3) / mWidth[4]; double xStep = THRESHOLDSTEP * min(1., xMax); double xNow = 0.; double wtMassNow, mT34Min, wtBW4Now, beta34Now; // Step through increasing x values; gives m4 unambiguously. do { xNow += xStep; wtMassNow = 0.; m4 = mHatMax - m3 - xNow * mWidth[4]; // Check that inside phase space limit set by pTmin. mT34Min = mT3Min + sqrt(m4*m4 + pT2HatMin); if (mT34Min < mHatMax) { // Breit-Wigner and beta factor give total weight. wtBW4Now = mw[4] / ( pow2(m4*m4 - sPeak[4]) + pow2(mw[4]) ); beta34Now = sqrt( pow2(mHatMax*mHatMax - m3*m3 - m4*m4) - pow2(2. * m3 * m4) ) / (mHatMax*mHatMax); wtMassNow = wtBW4Now * beta34Now; // Store new maximum, if any. if (wtMassNow > wtMassMax) { foundNonZero = true; wtMassMax = wtMassNow; m4WtMax = m4; } } // Continue stepping if increasing trend and more x range available. } while ( (!foundNonZero || wtMassNow > wtMassMax) && xNow < xMax - xStep); // Restore best value for subsequent maximization. m4 = m4WtMax; return foundNonZero; } //========================================================================== // PhaseSpace2to2elastic class. // 2 -> 2 kinematics set up for elastic scattering. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Maximum positive/negative argument for exponentiation. const double PhaseSpace2to2elastic::EXPMAX = 50.; // Conversion coefficients = 1/(16pi) * (mb <-> GeV^2). const double PhaseSpace2to2elastic::CONVERTEL = 0.0510925; //-------------------------------------------------------------------------- // Form of phase space sampling already fixed, so no optimization. // However, need to read out relevant parameters from SigmaTotal. bool PhaseSpace2to2elastic::setupSampling() { // Find maximum = value of cross section. sigmaNw = sigmaProcessPtr->sigmaHatWrap(); sigmaMx = sigmaNw; // Squared and outgoing masses of particles. s1 = mA * mA; s2 = mB * mB; m3 = mA; m4 = mB; // Elastic slope. bSlope = sigmaTotPtr->bSlopeEl(); // Determine maximum possible t range. lambda12S = pow2(s - s1 - s2) - 4. * s1 * s2 ; tLow = - lambda12S / s; tUpp = 0.; // Production model with Coulomb corrections need more parameters. useCoulomb = settingsPtr->flag("SigmaTotal:setOwn") && settingsPtr->flag("SigmaElastic:setOwn"); if (useCoulomb) { sigmaTot = sigmaTotPtr->sigmaTot(); rho = settingsPtr->parm("SigmaElastic:rho"); lambda = settingsPtr->parm("SigmaElastic:lambda"); tAbsMin = settingsPtr->parm("SigmaElastic:tAbsMin"); phaseCst = settingsPtr->parm("SigmaElastic:phaseConst"); alphaEM0 = settingsPtr->parm("StandardModel:alphaEM0"); // Relative rate of nuclear and Coulombic parts in trials. tUpp = -tAbsMin; sigmaNuc = CONVERTEL * pow2(sigmaTot) * (1. + rho*rho) / bSlope * exp(-bSlope * tAbsMin); sigmaCou = (useCoulomb) ? pow2(alphaEM0) / (4. * CONVERTEL * tAbsMin) : 0.; signCou = (idA == idB) ? 1. : -1.; // Dummy values. } else { sigmaNuc = sigmaNw; sigmaCou = 0.; } // Calculate coefficient of generation. tAux = exp( max(-EXPMAX, bSlope * (tLow - tUpp)) ) - 1.; return true; } //-------------------------------------------------------------------------- // Select a trial kinematics phase space point. Perform full // Monte Carlo acceptance/rejection at this stage. bool PhaseSpace2to2elastic::trialKin( bool, bool ) { // Allow for possibility that energy varies from event to event. if (doEnergySpread) { eCM = infoPtr->eCM(); s = eCM * eCM; lambda12S = pow2(s - s1 - s2) - 4. * s1 * s2 ; tLow = - lambda12S / s; tAux = exp( max(-EXPMAX, bSlope * (tLow - tUpp)) ) - 1.; } // Select t according to exp(bSlope*t). if (!useCoulomb || sigmaNuc > rndmPtr->flat() * (sigmaNuc + sigmaCou)) tH = tUpp + log(1. + tAux * rndmPtr->flat()) / bSlope; // Select t according to 1/t^2. else tH = tLow * tUpp / (tUpp + rndmPtr->flat() * (tLow - tUpp)); // Correction factor for ratio full/simulated. if (useCoulomb) { double sigmaN = CONVERTEL * pow2(sigmaTot) * (1. + rho*rho) * exp(bSlope * tH); double alpEM = couplingsPtr->alphaEM(-tH); double sigmaC = pow2(alpEM) / (4. * CONVERTEL * tH*tH); double sigmaGen = 2. * (sigmaN + sigmaC); double form2 = pow4(lambda/(lambda - tH)); double phase = signCou * alpEM * (-phaseCst - log(-0.5 * bSlope * tH)); double sigmaCor = sigmaN + pow2(form2) * sigmaC - signCou * alpEM * sigmaTot * (form2 / (-tH)) * exp(0.5 * bSlope * tH) * (rho * cos(phase) + sin(phase)); sigmaNw = sigmaMx * sigmaCor / sigmaGen; } // Careful reconstruction of scattering angle. double tRat = s * tH / lambda12S; double cosTheta = min(1., max(-1., 1. + 2. * tRat ) ); double sinTheta = 2. * sqrtpos( -tRat * (1. + tRat) ); theta = asin( min(1., sinTheta)); if (cosTheta < 0.) theta = M_PI - theta; return true; } //-------------------------------------------------------------------------- // Construct the four-vector kinematics from the trial values. bool PhaseSpace2to2elastic::finalKin() { // Particle masses. mH[1] = mA; mH[2] = mB; mH[3] = m3; mH[4] = m4; // Incoming particles along beam axes. pAbs = 0.5 * sqrtpos(lambda12S) / eCM; pH[1] = Vec4( 0., 0., pAbs, 0.5 * (s + s1 - s2) / eCM); pH[2] = Vec4( 0., 0., -pAbs, 0.5 * (s + s2 - s1) / eCM); // Outgoing particles initially along beam axes. pH[3] = Vec4( 0., 0., pAbs, 0.5 * (s + s1 - s2) / eCM); pH[4] = Vec4( 0., 0., -pAbs, 0.5 * (s + s2 - s1) / eCM); // Then rotate them phi = 2. * M_PI * rndmPtr->flat(); pH[3].rot( theta, phi); pH[4].rot( theta, phi); // Set some further info for completeness. x1H = 1.; x2H = 1.; sH = s; uH = 2. * (s1 + s2) - sH - tH; mHat = eCM; p2Abs = pAbs * pAbs; betaZ = 0.; pTH = pAbs * sin(theta); // Done. return true; } //========================================================================== // PhaseSpace2to2diffractive class. // 2 -> 2 kinematics set up for diffractive scattering. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of tries to find acceptable (m^2, t) set. const int PhaseSpace2to2diffractive::NTRY = 500; // Maximum positive/negative argument for exponentiation. const double PhaseSpace2to2diffractive::EXPMAX = 50.; // Safety margin so sum of diffractive masses not too close to eCM. const double PhaseSpace2to2diffractive::DIFFMASSMARGIN = 0.2; //-------------------------------------------------------------------------- // Form of phase space sampling already fixed, so no optimization. // However, need to read out relevant parameters from SigmaTotal. bool PhaseSpace2to2diffractive::setupSampling() { // Pomeron flux parametrization, and parameters of some options. PomFlux = settingsPtr->mode("Diffraction:PomFlux"); epsilonPF = settingsPtr->parm("Diffraction:PomFluxEpsilon"); alphaPrimePF = settingsPtr->parm("Diffraction:PomFluxAlphaPrime"); // Find maximum = value of cross section. sigmaNw = sigmaProcessPtr->sigmaHatWrap(); sigmaMx = sigmaNw; // Masses of particles and minimal masses of diffractive states. m3ElDiff = (isDiffA) ? sigmaTotPtr->mMinXB() : mA; m4ElDiff = (isDiffB) ? sigmaTotPtr->mMinAX() : mB; s1 = mA * mA; s2 = mB * mB; s3 = pow2( m3ElDiff); s4 = pow2( m4ElDiff); // Determine maximum possible t range and coefficient of generation. lambda12 = sqrtpos( pow2( s - s1 - s2) - 4. * s1 * s2 ); lambda34 = sqrtpos( pow2( s - s3 - s4) - 4. * s3 * s4 ); double tempA = s - (s1 + s2 + s3 + s4) + (s1 - s2) * (s3 - s4) / s; double tempB = lambda12 * lambda34 / s; double tempC = (s3 - s1) * (s4 - s2) + (s1 + s4 - s2 - s3) * (s1 * s4 - s2 * s3) / s; tLow = -0.5 * (tempA + tempB); tUpp = tempC / tLow; // Default for all parametrization-specific parameters. cRes = sResXB = sResAX = sProton = bMin = bSlope = bSlope1 = bSlope2 = probSlope1 = xIntPF = xtCorPF = mp24DL = coefDL = tAux = tAux1 = tAux2 = 0.; // Schuler&Sjostrand: parameters of low-mass-resonance enhancement. if (PomFlux == 1) { cRes = sigmaTotPtr->cRes(); sResXB = pow2( sigmaTotPtr->mResXB()); sResAX = pow2( sigmaTotPtr->mResAX()); sProton = sigmaTotPtr->sProton(); // Schuler&Sjostrand: lower limit diffractive slope. if (!isDiffB) bMin = sigmaTotPtr->bMinSlopeXB(); else if (!isDiffA) bMin = sigmaTotPtr->bMinSlopeAX(); else bMin = sigmaTotPtr->bMinSlopeXX(); tAux = exp( max(-EXPMAX, bMin * (tLow - tUpp)) ) - 1.; // Bruni&Ingelman: relative weight of two diffractive slopes. } else if (PomFlux == 2) { bSlope1 = 8.0; probSlope1 = 6.38 * ( exp(max(-EXPMAX, bSlope1 * tUpp)) - exp(max(-EXPMAX, bSlope1 * tLow)) ) / bSlope1; bSlope2 = 3.0; double pS2 = 0.424 * ( exp(max(-EXPMAX, bSlope2 * tUpp)) - exp(max(-EXPMAX, bSlope2 * tLow)) ) / bSlope2; probSlope1 /= probSlope1 + pS2; tAux1 = exp( max(-EXPMAX, bSlope1 * (tLow - tUpp)) ) - 1.; tAux2 = exp( max(-EXPMAX, bSlope2 * (tLow - tUpp)) ) - 1.; // Streng&Berger (RapGap): diffractive slope, power of mass spectrum. } else if (PomFlux == 3) { bSlope = 4.7; double xPowPF = 1. - 2. * (1. + epsilonPF); xIntPF = 2. * (1. + xPowPF); xtCorPF = 2. * alphaPrimePF; tAux = exp( max(-EXPMAX, bSlope * (tLow - tUpp)) ) - 1.; // Donnachie&Landshoff (RapGap): power of mass spectrum. } else if (PomFlux == 4) { mp24DL = 4. * pow2(particleDataPtr->m0(2212)); double xPowPF = 1. - 2. * (1. + epsilonPF); xIntPF = 2. * (1. + xPowPF); xtCorPF = 2. * alphaPrimePF; // Upper estimate of t dependence, for preliminary choice. coefDL = 0.85; tAux1 = 1. / pow3(1. - coefDL * tLow); tAux2 = 1. / pow3(1. - coefDL * tUpp); // MBR model. } else if (PomFlux == 5) { eps = settingsPtr->parm("Diffraction:MBRepsilon"); alph = settingsPtr->parm("Diffraction:MBRalpha"); alph2 = alph * alph; m2min = settingsPtr->parm("Diffraction:MBRm2Min"); dyminSD = settingsPtr->parm("Diffraction:MBRdyminSD"); dyminDD = settingsPtr->parm("Diffraction:MBRdyminDD"); dyminSigSD = settingsPtr->parm("Diffraction:MBRdyminSigSD"); dyminSigDD = settingsPtr->parm("Diffraction:MBRdyminSigDD"); // Max f(dy) for Von Neumann method, from SigmaTot. sdpmax= sigmaTotPtr->sdpMax(); ddpmax= sigmaTotPtr->ddpMax(); } // Done. return true; } //-------------------------------------------------------------------------- // Select a trial kinematics phase space point. Perform full // Monte Carlo acceptance/rejection at this stage. bool PhaseSpace2to2diffractive::trialKin( bool, bool ) { // Allow for possibility that energy varies from event to event. if (doEnergySpread) { eCM = infoPtr->eCM(); s = eCM * eCM; lambda12 = sqrtpos( pow2( s - s1 - s2) - 4. * s1 * s2 ); lambda34 = sqrtpos( pow2( s - s3 - s4) - 4. * s3 * s4 ); double tempA = s - (s1 + s2 + s3 + s4) + (s1 - s2) * (s3 - s4) / s; double tempB = lambda12 * lambda34 / s; double tempC = (s3 - s1) * (s4 - s2) + (s1 + s4 - s2 - s3) * (s1 * s4 - s2 * s3) / s; tLow = -0.5 * (tempA + tempB); tUpp = tempC / tLow; if (PomFlux == 1) { tAux = exp( max(-EXPMAX, bMin * (tLow - tUpp)) ) - 1.; } else if (PomFlux == 2) { tAux1 = exp( max(-EXPMAX, bSlope1 * (tLow - tUpp)) ) - 1.; tAux2 = exp( max(-EXPMAX, bSlope2 * (tLow - tUpp)) ) - 1.; } else if (PomFlux == 3) { tAux = exp( max(-EXPMAX, bSlope * (tLow - tUpp)) ) - 1.; } else if (PomFlux == 4) { tAux1 = 1. / pow3(1. - coefDL * tLow); tAux2 = 1. / pow3(1. - coefDL * tUpp); } } // Loop over attempts to set up masses and t consistently. for (int loop = 0; ; ++loop) { if (loop == NTRY) { infoPtr->errorMsg("Error in PhaseSpace2to2diffractive::trialKin: " " quit after repeated tries"); return false; } // Schuler and Sjostrand: if (PomFlux == 1) { // Select diffractive mass(es) according to dm^2/m^2. m3 = (isDiffA) ? m3ElDiff * pow( max(mA, eCM - m4ElDiff) / m3ElDiff, rndmPtr->flat()) : m3ElDiff; m4 = (isDiffB) ? m4ElDiff * pow( max(mB, eCM - m3ElDiff) / m4ElDiff, rndmPtr->flat()) : m4ElDiff; if (m3 + m4 + DIFFMASSMARGIN >= eCM) continue; s3 = m3 * m3; s4 = m4 * m4; // Additional mass factors, including resonance enhancement. if (isDiffA && !isDiffB) { double facXB = (1. - s3 / s) * (1. + cRes * sResXB / (sResXB + s3)); if (facXB < rndmPtr->flat() * (1. + cRes)) continue; } else if (isDiffB && !isDiffA) { double facAX = (1. - s4 / s) * (1. + cRes * sResAX / (sResAX + s4)); if (facAX < rndmPtr->flat() * (1. + cRes)) continue; } else { double facXX = (1. - pow2(m3 + m4) / s) * (s * sProton / (s * sProton + s3 * s4)) * (1. + cRes * sResXB / (sResXB + s3)) * (1. + cRes * sResAX / (sResAX + s4)); if (facXX < rndmPtr->flat() * pow2(1. + cRes)) continue; } // Select t according to exp(bMin*t) and correct to right slope. tH = tUpp + log(1. + tAux * rndmPtr->flat()) / bMin; double bDiff = 0.; if (isDiffA && !isDiffB) bDiff = sigmaTotPtr->bSlopeXB(s3) - bMin; else if (!isDiffA) bDiff = sigmaTotPtr->bSlopeAX(s4) - bMin; else bDiff = sigmaTotPtr->bSlopeXX(s3, s4) - bMin; bDiff = max(0., bDiff); if (exp( max(-EXPMAX, bDiff * (tH - tUpp)) ) < rndmPtr->flat()) continue; // Bruni and Ingelman: } else if (PomFlux == 2) { // Select diffractive mass(es) according to dm^2/m^2. m3 = (isDiffA) ? m3ElDiff * pow( max(mA, eCM - m4ElDiff) / m3ElDiff, rndmPtr->flat()) : m3ElDiff; m4 = (isDiffB) ? m4ElDiff * pow( max(mB, eCM - m3ElDiff) / m4ElDiff, rndmPtr->flat()) : m4ElDiff; if (m3 + m4 + DIFFMASSMARGIN >= eCM) continue; s3 = m3 * m3; s4 = m4 * m4; // Select t according to exp(bSlope*t) with two possible slopes. tH = (rndmPtr->flat() < probSlope1) ? tUpp + log(1. + tAux1 * rndmPtr->flat()) / bSlope1 : tUpp + log(1. + tAux2 * rndmPtr->flat()) / bSlope2; // Streng and Berger et al. (RapGap): } else if (PomFlux == 3) { // Select diffractive mass(es) according to dm^2/(m^2)^(1 + 2 epsilon). m3 = m3ElDiff; m4 = m4ElDiff; if (isDiffA) { double s3MinPow = pow( m3ElDiff, xIntPF ); double s3MaxPow = pow( max(mA, eCM - m4ElDiff), xIntPF ); m3 = pow( s3MinPow + rndmPtr->flat() * (s3MaxPow - s3MinPow), 1. / xIntPF ); } if (isDiffB) { double s4MinPow = pow( m4ElDiff, xIntPF ); double s4MaxPow = pow( max(mB, eCM - m3ElDiff), xIntPF ); m4 = pow( s4MinPow + rndmPtr->flat() * (s4MaxPow - s4MinPow), 1. / xIntPF ); } if (m3 + m4 + DIFFMASSMARGIN >= eCM) continue; s3 = m3 * m3; s4 = m4 * m4; // Select t according to exponential and weigh by x_P^(2 alpha' |t|). tH = tUpp + log(1. + tAux * rndmPtr->flat()) / bSlope; if ( isDiffA && pow( s3 / s, xtCorPF * abs(tH) ) < rndmPtr->flat() ) continue; if ( isDiffB && pow( s4 / s, xtCorPF * abs(tH) ) < rndmPtr->flat() ) continue; // Donnachie and Landshoff (RapGap): } else if (PomFlux == 4) { // Select diffractive mass(es) according to dm^2/(m^2)^(1 + 2 epsilon). m3 = m3ElDiff; m4 = m4ElDiff; if (isDiffA) { double s3MinPow = pow( m3ElDiff, xIntPF ); double s3MaxPow = pow( max(mA, eCM - m4ElDiff), xIntPF ); m3 = pow( s3MinPow + rndmPtr->flat() * (s3MaxPow - s3MinPow), 1. / xIntPF ); } if (isDiffB) { double s4MinPow = pow( m4ElDiff, xIntPF ); double s4MaxPow = pow( max(mB, eCM - m3ElDiff), xIntPF ); m4 = pow( s4MinPow + rndmPtr->flat() * (s4MaxPow - s4MinPow), 1. / xIntPF ); } if (m3 + m4 + DIFFMASSMARGIN >= eCM) continue; s3 = m3 * m3; s4 = m4 * m4; // Select t according to power and weigh by x_P^(2 alpha' |t|). tH = - (1. / pow( tAux1 + rndmPtr->flat() * (tAux2 - tAux1), 1./3.) - 1.) / coefDL; double wDL = pow2( (mp24DL - 2.8 * tH) / (mp24DL - tH) ) / pow4( 1. - tH / 0.7); double wMX = 1. / pow4( 1. - coefDL * tH); if (wDL < rndmPtr->flat() * wMX) continue; if ( isDiffA && pow( s3 / s, xtCorPF * abs(tH) ) < rndmPtr->flat() ) continue; if ( isDiffB && pow( s4 / s, xtCorPF * abs(tH) ) < rndmPtr->flat() ) continue; // MBR model: } else if (PomFlux == 5) { m3 = mA; m4 = mB; double xi, P, yRnd, dy; // MBR double diffractive. if (isDiffA && isDiffB) { dymin0 = 0.; dymax = log(s/pow2(m2min)); // Von Neumann method to generate dy, uses ddpmax from SigmaTot. do { dy = dymin0 + (dymax - dymin0) * rndmPtr->flat(); P = (dymax - dy) * exp(eps*dy) * ( exp(-2. * alph * dy * exp(-dy)) - exp(-2. * alph * dy * exp(dy)) ) / dy; // Suppress smaller gap, smooth transition to non-diffractive. P *= 0.5 * (1 + erf( ( dy - dyminDD) / dyminSigDD ) ); if (P > ddpmax) { ostringstream osWarn; osWarn << "ddpmax = " << scientific << setprecision(3) << ddpmax << " " << P << " " << dy << endl; infoPtr->errorMsg("Warning in PhaseSpace2to2diffractive::" "trialKin for double diffraction:", osWarn.str()); } yRnd = ddpmax * rndmPtr->flat(); } while (yRnd > P); double y0max = (dymax - dy)/2.; double y0min = -y0max; double y0 = y0min + (y0max - y0min) * rndmPtr->flat(); am1 = sqrt( eCM * exp( -y0 - dy/2. ) ); am2 = sqrt( eCM * exp( y0 - dy/2. ) ); // Generate 4-momentum transfer, t from exp. double b = 2. * alph * dy; tUpp = -exp( -dy ); tLow = -exp( dy ); tAux = exp( b * (tLow - tUpp) ) - 1.; t = tUpp + log(1. + tAux * rndmPtr->flat()) / b; m3 = am1; m4 = am2; tH = t; // MBR single diffractive. } else if (isDiffA || isDiffB) { dymin0 = 0.; dymax = log(s/m2min); // Von Neumann method to generate dy, uses sdpmax from SigmaTot. do { dy = dymin0 + (dymax - dymin0) * rndmPtr->flat(); P = exp(eps * dy) * ( (FFA1 / (FFB1 + 2. * alph * dy) ) + (FFA2 / (FFB2 + 2. * alph * dy) ) ); // Suppress smaller gap. P *= 0.5 * (1. + erf( (dy - dyminSD) / dyminSigSD) ); if (P > sdpmax) { ostringstream osWarn; osWarn << "sdpmax = " << scientific << setprecision(3) << sdpmax << " " << P << " " << dy << endl; infoPtr->errorMsg("Warning in PhaseSpace2to2diffractive::" "trialKin for single diffraction:", osWarn.str()); } yRnd = sdpmax * rndmPtr->flat(); } while (yRnd > P); xi = exp( -dy ); amx = sqrt( xi * s ); // Generate 4-momentum transfer, t. First exponent, then FF*exp. double tmin = -s1 * xi * xi / (1 - xi); do { t = tmin + log(1. - rndmPtr->flat()); double pFF = (4. * s1 - 2.8 * t) / ( (4. * s1 - t) * pow2(1. - t / 0.71) ); P = pow2(pFF) * exp(2. * alph * dy * t); yRnd = exp(t) * rndmPtr->flat(); } while (yRnd > P); if(isDiffA) m3 = amx; if(isDiffB) m4 = amx; tH = t; } // End of MBR model code. s3 = m3 * m3; s4 = m4 * m4; } // Check whether m^2 and t choices are consistent. lambda34 = sqrtpos( pow2( s - s3 - s4) - 4. * s3 * s4 ); double tempA = s - (s1 + s2 + s3 + s4) + (s1 - s2) * (s3 - s4) / s; double tempB = lambda12 * lambda34 / s; double tempC = (s3 - s1) * (s4 - s2) + (s1 + s4 - s2 - s3) * (s1 * s4 - s2 * s3) / s; double tLowNow = -0.5 * (tempA + tempB); double tUppNow = tempC / tLowNow; if (tH < tLowNow || tH > tUppNow) continue; // Careful reconstruction of scattering angle. double cosTheta = min(1., max(-1., (tempA + 2. * tH) / tempB)); double sinTheta = 2. * sqrtpos( -(tempC + tempA * tH + tH * tH) ) / tempB; theta = asin( min(1., sinTheta)); if (cosTheta < 0.) theta = M_PI - theta; // Found acceptable kinematics, so no more looping. Done break; } return true; } //-------------------------------------------------------------------------- // Construct the four-vector kinematics from the trial values. bool PhaseSpace2to2diffractive::finalKin() { // Particle masses; incoming always on mass shell. mH[1] = mA; mH[2] = mB; mH[3] = m3; mH[4] = m4; // Incoming particles along beam axes. pAbs = 0.5 * lambda12 / eCM; pH[1] = Vec4( 0., 0., pAbs, 0.5 * (s + s1 - s2) / eCM); pH[2] = Vec4( 0., 0., -pAbs, 0.5 * (s + s2 - s1) / eCM); // Outgoing particles initially along beam axes. pAbs = 0.5 * lambda34 / eCM; pH[3] = Vec4( 0., 0., pAbs, 0.5 * (s + s3 - s4) / eCM); pH[4] = Vec4( 0., 0., -pAbs, 0.5 * (s + s4 - s3) / eCM); // Then rotate them phi = 2. * M_PI * rndmPtr->flat(); pH[3].rot( theta, phi); pH[4].rot( theta, phi); // Set some further info for completeness (but Info can be for subprocess). x1H = 1.; x2H = 1.; sH = s; uH = s1 + s2 + s3 + s4 - sH - tH; mHat = eCM; p2Abs = pAbs * pAbs; betaZ = 0.; pTH = pAbs * sin(theta); // Done. return true; } //========================================================================== // PhaseSpace2to3diffractive class. // 2 -> 3 kinematics set up for central diffractive scattering. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of tries to find acceptable (m^2, t1, t2) set. const int PhaseSpace2to3diffractive::NTRY = 500; const int PhaseSpace2to3diffractive::NINTEG2 = 40; // Maximum positive/negative argument for exponentiation. const double PhaseSpace2to3diffractive::EXPMAX = 50.; // Minimal mass of central diffractive system. const double PhaseSpace2to3diffractive::DIFFMASSMIN = 0.8; // Safety margin so sum of diffractive masses not too close to eCM. const double PhaseSpace2to3diffractive::DIFFMASSMARGIN = 0.2; //-------------------------------------------------------------------------- // Set up for phase space sampling. bool PhaseSpace2to3diffractive::setupSampling() { // Pomeron flux parametrization, and parameters of some options. PomFlux = settingsPtr->mode("Diffraction:PomFlux"); epsilonPF = settingsPtr->parm("Diffraction:PomFluxEpsilon"); alphaPrimePF = settingsPtr->parm("Diffraction:PomFluxAlphaPrime"); // Find maximum = value of cross section. sigmaNw = sigmaProcessPtr->sigmaHatWrap(); sigmaMx = sigmaNw; // Squared masses of particles and minimal mass of diffractive states. s1 = mA * mA; s2 = mB * mB; m5min = sigmaTotPtr->mMinAXB(); s5min = m5min * m5min; // Loop over two cases: s4 = (X + B)^2 and s3 = (A + X)^2. for (int i = 0; i < 2; ++i) { s3 = (i == 0) ? s1 : pow2(mA + m5min); s4 = (i == 0) ? pow2(mB + m5min) : s2; // Determine maximum possible t range and coefficient of generation. double lambda12 = sqrtpos( pow2( s - s1 - s2) - 4. * s1 * s2 ); double lambda34 = sqrtpos( pow2( s - s3 - s4) - 4. * s3 * s4 ); double tempA = s - (s1 + s2 + s3 + s4) + (s1 - s2) * (s3 - s4) / s; double tempB = lambda12 * lambda34 / s; double tempC = (s3 - s1) * (s4 - s2) + (s1 + s4 - s2 - s3) * (s1 * s4 - s2 * s3) / s; tLow[i] = -0.5 * (tempA + tempB); tUpp[i] = tempC / tLow[i]; } s3 = s1; s4 = s2; // Default for all parametrization-specific parameters. bSlope1 = bSlope2 = bSlope = xIntPF = xIntInvPF = xtCorPF = mp24DL = coefDL = 0.; for (int i = 0; i < 2; ++i) bMin[i] = tAux[i] = probSlope1[i] = tAux1[i] = tAux2[i] = 0.; // Schuler&Sjostrand: lower limit diffractive slope. if (PomFlux == 1) { bMin[0] = sigmaTotPtr->bMinSlopeAX(); tAux[0] = exp( max(-EXPMAX, bMin[0] * (tLow[0] - tUpp[0])) ) - 1.; bMin[1] = sigmaTotPtr->bMinSlopeXB(); tAux[1] = exp( max(-EXPMAX, bMin[1] * (tLow[1] - tUpp[1])) ) - 1.; // Bruni&Ingelman: relative weight of two diffractive slopes. } else if (PomFlux == 2) { bSlope1 = 8.0; bSlope2 = 3.0; for (int i = 0; i < 2; ++i) { probSlope1[i] = 6.38 * ( exp(max(-EXPMAX, bSlope1 * tUpp[i])) - exp(max(-EXPMAX, bSlope1 * tLow[i])) ) / bSlope1; double pS2 = 0.424 * ( exp(max(-EXPMAX, bSlope2 * tUpp[i])) - exp(max(-EXPMAX, bSlope2 * tLow[i])) ) / bSlope2; probSlope1[i] /= probSlope1[i] + pS2; tAux1[i] = exp( max(-EXPMAX, bSlope1 * (tLow[i] - tUpp[i])) ) - 1.; tAux2[i] = exp( max(-EXPMAX, bSlope2 * (tLow[i] - tUpp[i])) ) - 1.; } // Streng&Berger (RapGap): diffractive slope, power of mass spectrum. } else if (PomFlux == 3) { bSlope = 4.7; double xPowPF = 1. - 2. * (1. + epsilonPF); xIntPF = 1. + xPowPF; xIntInvPF = 1. / xIntPF; xtCorPF = 2. * alphaPrimePF; tAux[0] = exp( max(-EXPMAX, bSlope * (tLow[0] - tUpp[0])) ) - 1.; tAux[1] = exp( max(-EXPMAX, bSlope * (tLow[1] - tUpp[1])) ) - 1.; // Donnachie&Landshoff (RapGap): power of mass spectrum. } else if (PomFlux == 4) { mp24DL = 4. * pow2(particleDataPtr->m0(2212)); double xPowPF = 1. - 2. * (1. + epsilonPF); xIntPF = 1. + xPowPF; xIntInvPF = 1. / xIntPF; xtCorPF = 2. * alphaPrimePF; // Upper estimate of t dependence, for preliminary choice. coefDL = 0.85; tAux1[0] = 1. / pow3(1. - coefDL * tLow[0]); tAux2[0] = 1. / pow3(1. - coefDL * tUpp[0]); tAux1[1] = 1. / pow3(1. - coefDL * tLow[1]); tAux2[1] = 1. / pow3(1. - coefDL * tUpp[1]); // Setup for the MBR model. } else if (PomFlux == 5) { epsMBR = settingsPtr->parm("Diffraction:MBRepsilon"); alphMBR = settingsPtr->parm("Diffraction:MBRalpha"); m2minMBR = settingsPtr->parm("Diffraction:MBRm2Min"); dyminMBR = settingsPtr->parm("Diffraction:MBRdyminCD"); dyminSigMBR = settingsPtr->parm("Diffraction:MBRdyminSigCD"); dyminInvMBR = sqrt(2.) / dyminSigMBR; // Max f(dy) for Von Neumann method, dpepmax from SigmaTot. dpepmax = sigmaTotPtr->dpepMax(); } // Done. return true; } //-------------------------------------------------------------------------- // Select a trial kinematics phase space point. Perform full // Monte Carlo acceptance/rejection at this stage. bool PhaseSpace2to3diffractive::trialKin( bool, bool ) { // Allow for possibility that energy varies from event to event. if (doEnergySpread) { eCM = infoPtr->eCM(); s = eCM * eCM; for (int i = 0; i < 2; ++i) { s3 = (i == 0) ? s1 : pow2(mA + m5min); s4 = (i == 0) ? pow2(mB + m5min) : s2; double lambda12 = sqrtpos( pow2( s - s1 - s2) - 4. * s1 * s2 ); double lambda34 = sqrtpos( pow2( s - s3 - s4) - 4. * s3 * s4 ); double tempA = s - (s1 + s2 + s3 + s4) + (s1 - s2) * (s3 - s4) / s; double tempB = lambda12 * lambda34 / s; double tempC = (s3 - s1) * (s4 - s2) + (s1 + s4 - s2 - s3) * (s1 * s4 - s2 * s3) / s; tLow[i] = -0.5 * (tempA + tempB); tUpp[i] = tempC / tLow[i]; } s3 = s1; s4 = s2; if (PomFlux == 1) { tAux[0] = exp( max(-EXPMAX, bMin[0] * (tLow[0] - tUpp[0])) ) - 1.; tAux[1] = exp( max(-EXPMAX, bMin[1] * (tLow[1] - tUpp[1])) ) - 1.; } else if (PomFlux == 2) { for (int i = 0; i < 2; ++i) { tAux1[i] = exp( max(-EXPMAX, bSlope1 * (tLow[i] - tUpp[i])) ) - 1.; tAux2[i] = exp( max(-EXPMAX, bSlope2 * (tLow[i] - tUpp[i])) ) - 1.; } } else if (PomFlux == 3) { tAux[0] = exp( max(-EXPMAX, bSlope * (tLow[0] - tUpp[0])) ) - 1.; tAux[1] = exp( max(-EXPMAX, bSlope * (tLow[1] - tUpp[1])) ) - 1.; } else if (PomFlux == 4) { tAux1[0] = 1. / pow3(1. - coefDL * tLow[0]); tAux2[0] = 1. / pow3(1. - coefDL * tUpp[0]); tAux1[1] = 1. / pow3(1. - coefDL * tLow[1]); tAux2[1] = 1. / pow3(1. - coefDL * tUpp[1]); } } // Trivial kinematics of incoming hadrons. double lambda12 = sqrtpos( pow2( s - s1 - s2) - 4. * s1 * s2 ); pAbs = 0.5 * lambda12 / eCM; p1.p( 0., 0., pAbs, 0.5 * (s + s1 - s2) / eCM); p2.p( 0., 0., -pAbs, 0.5 * (s + s2 - s1) / eCM); // Loop over attempts to set up mass, t1, t2 consistently. for (int loop = 0; ; ++loop) { if (loop == NTRY) { infoPtr->errorMsg("Error in PhaseSpace2to3diffractive::trialKin: " " quit after repeated tries"); return false; } double xi1 = 0.; double xi2 = 0.; double tVal[2] = { 0., 0.}; // Schuler and Sjostrand: if (PomFlux == 1) { // Select mass according to dxi_1/xi_1 * dxi_2/xi_2 * (1 - m^2/s). do { xi1 = pow( s5min / s, rndmPtr->flat()); xi2 = pow( s5min / s, rndmPtr->flat()); s5 = xi1 * xi2 * s; } while (s5 < s5min || xi1 * xi2 > rndmPtr->flat()); if (mA + mB + sqrt(s5) + DIFFMASSMARGIN >= eCM) continue; // Select t according to exp(bMin*t) and correct to right slope. bool tryAgain = false; for (int i = 0; i < 2; ++i) { tVal[i] = tUpp[i] + log(1. + tAux[i] * rndmPtr->flat()) / bMin[i]; double bDiff = (i == 0) ? sigmaTotPtr->bSlopeAX(s2 + xi1 * s) : sigmaTotPtr->bSlopeXB(s1 + xi2 * s); bDiff = max(0., bDiff - bMin[i]); if (exp( max(-EXPMAX, bDiff * (tVal[i] - tUpp[i])) ) < rndmPtr->flat()) tryAgain = true; } if (tryAgain) continue; // Bruni and Ingelman: } else if (PomFlux == 2) { // Select mass according to dxi_1/xi_1 * dxi_2/xi_2. do { xi1 = pow( s5min / s, rndmPtr->flat()); xi2 = pow( s5min / s, rndmPtr->flat()); s5 = xi1 * xi2 * s; } while (s5 < s5min); if (mA + mB + sqrt(s5) + DIFFMASSMARGIN >= eCM) continue; // Select t according to exp(bSlope*t) with two possible slopes. for (int i = 0; i < 2; ++i) tVal[i] = (rndmPtr->flat() < probSlope1[i]) ? tUpp[i] + log(1. + tAux1[i] * rndmPtr->flat()) / bSlope1 : tUpp[i] + log(1. + tAux2[i] * rndmPtr->flat()) / bSlope2; // Streng and Berger et al. (RapGap): } else if (PomFlux == 3) { // Select mass by dxi_1 * dxi_2 / (xi_1 * xi_2)^(1 + 2 epsilon). double sMinPow = pow( s5min / s, xIntPF); do { xi1 = pow( sMinPow + rndmPtr->flat() * (1. - sMinPow), xIntInvPF ); xi2 = pow( sMinPow + rndmPtr->flat() * (1. - sMinPow), xIntInvPF ); s5 = xi1 * xi2 * s; } while (s5 < s5min); if (mA + mB + sqrt(s5) + DIFFMASSMARGIN >= eCM) continue; // Select t according to exponential and weigh by x_P^(2 alpha' |t|). bool tryAgain = false; for (int i = 0; i < 2; ++i) { tVal[i] = tUpp[i] + log(1. + tAux[i] * rndmPtr->flat()) / bSlope; double xi = (i == 0) ? xi1 : xi2; if ( pow( xi, xtCorPF * abs(tVal[i]) ) < rndmPtr->flat() ) tryAgain = true; } if (tryAgain) continue; // Donnachie and Landshoff (RapGap): } else if (PomFlux == 4) { // Select mass by dxi_1 * dxi_2 / (xi_1 * xi_2)^(1 + 2 epsilon). double sMinPow = pow( s5min / s, xIntPF); do { xi1 = pow( sMinPow + rndmPtr->flat() * (1. - sMinPow), xIntInvPF ); xi2 = pow( sMinPow + rndmPtr->flat() * (1. - sMinPow), xIntInvPF ); s5 = xi1 * xi2 * s; } while (s5 < s5min); if (mA + mB + sqrt(s5) + DIFFMASSMARGIN >= eCM) continue; // Select t according to power and weigh by x_P^(2 alpha' |t|). bool tryAgain = false; for (int i = 0; i < 2; ++i) { tVal[i] = - (1. / pow( tAux1[i] + rndmPtr->flat() * (tAux2[i] - tAux1[i]), 1./3.) - 1.) / coefDL; double wDL = pow2( (mp24DL - 2.8 * tVal[i]) / (mp24DL - tVal[i]) ) / pow4( 1. - tVal[i] / 0.7); double wMX = 1. / pow4( 1. - coefDL * tVal[i]); if (wDL < rndmPtr->flat() * wMX) tryAgain = true; double xi = (i == 0) ? xi1 : xi2; if ( pow( xi, xtCorPF * abs(tVal[i]) ) < rndmPtr->flat() ) tryAgain = true; } if (tryAgain) continue; // The MBR model (PomFlux == 5). } else { double dymin0 = 0.; double dymax = log(s/m2minMBR); double f1, f2, step2, dy, yc, ycmin, ycmax, dy1, dy2, P, P1, P2, yRnd, yRnd1, yRnd2; // Von Neumann method to generate dy, uses dpepmax from SigmaTot. do { dy = dymin0 + (dymax - dymin0) * rndmPtr->flat(); P = 0.; step2 = (dy - dymin0) / NINTEG2; for (int j = 0; j < NINTEG2 ; ++j) { yc = -(dy - dymin0) / 2. + (j + 0.5) * step2; dy1 = 0.5 * dy - yc; dy2 = 0.5 * dy + yc; f1 = exp(epsMBR * dy1) * ( (FFA1 / (FFB1 + 2. * alphMBR * dy1) ) + (FFA2 / (FFB2 + 2. * alphMBR * dy1) ) ); f2 = exp(epsMBR * dy2) * ( (FFA1 / (FFB1 + 2. * alphMBR * dy2) ) + (FFA2 / (FFB2 + 2. * alphMBR * dy2) ) ); f1 *= 0.5 * (1. + erf( (dy1 - 0.5 * dyminMBR) * dyminInvMBR )); f2 *= 0.5 * (1. + erf( (dy2 - 0.5 * dyminMBR) * dyminInvMBR )); P += f1 * f2 * step2; } if (P > dpepmax) { ostringstream osWarn; osWarn << "dpepmax = " << scientific << setprecision(3) << dpepmax << " " << P << " " << dy << endl; infoPtr->errorMsg("Warning in PhaseSpace2to2diffractive::" "trialKin for central diffraction:", osWarn.str()); } yRnd = dpepmax * rndmPtr->flat(); // Generate dyc. ycmax = (dy - dymin0) / 2.; ycmin = -ycmax; yc = ycmin + (ycmax - ycmin) * rndmPtr->flat(); // xi1, xi2 from dy and dy0. dy1 = 0.5 * dy + yc; dy2 = 0.5 * dy - yc; P1 = 0.5 * (1. + erf( (dy1 - 0.5 * dyminMBR) * dyminInvMBR )); P2 = 0.5 * (1. + erf( (dy2 - 0.5 * dyminMBR) * dyminInvMBR )); yRnd1 = rndmPtr->flat(); yRnd2 = rndmPtr->flat(); } while( !(yRnd < P && yRnd1 < P1 && yRnd2 < P2) ); xi1 = exp( -dy1 ); xi2 = exp( -dy2 ); // Generate t1 at vertex1. First exponent, then FF*exp. double tmin = -s1 * xi1 * xi1 / (1. - xi1); do { t1 = tmin + log(1. - rndmPtr->flat()); double pFF = (4. * s1 - 2.8 * t1) / ( (4. * s1 - t1) * pow2(1. - t1 / 0.71)); P = pow2(pFF) * exp(2. * alphMBR * dy1 * t1); yRnd = exp(t1) * rndmPtr->flat(); } while (yRnd > P); // Generate t2 at vertex2. First exponent, then FF*exp. tmin = -s2 * xi2 * xi2 / (1. - xi2); do { t2 = tmin + log(1. - rndmPtr->flat()); double pFF = (4. * s2 - 2.8 * t2) / ((4. * s2 - t2) * pow2(1. - t2 / 0.71)); P = pow2(pFF) * exp(2. * alphMBR * dy2 * t2); yRnd = exp(t2) * rndmPtr->flat(); } while (yRnd > P); } // Checks and kinematics construction four first options. double pz3 = 0.; double pz4 = 0.; double pT3 = 0.; double pT4 = 0.; if (PomFlux < 5) { // Check whether m^2 (i.e. xi) and t choices are consistent. bool tryAgain = false; for (int i = 0; i < 2; ++i) { double sx1 = (i == 0) ? s1 : s2; double sx2 = (i == 0) ? s2 : s1; double sx3 = sx1; double sx4 = (i == 0) ? s2 + xi1 * s : s1 + xi2 * s; if (sqrt(sx3) + sqrt(sx4) + DIFFMASSMARGIN > eCM) tryAgain = true; double lambda34 = sqrtpos( pow2( s - sx3 - sx4) - 4. * sx3 * sx4 ); double tempA = s - (sx1 + sx2 + sx3 + sx4) + (sx1 - sx2) * (sx3 - sx4) / s; double tempB = lambda12 * lambda34 / s; double tempC = (sx3 - sx1) * (sx4 - sx2) + (sx1 + sx4 - sx2 - sx3) * (sx1 * sx4 - sx2 * sx3) / s; double tLowNow = -0.5 * (tempA + tempB); double tUppNow = tempC / tLowNow; if (tVal[i] < tLowNow || tVal[i] > tUppNow) tryAgain = true; if (tryAgain) break; // Careful reconstruction of scattering angle. double cosTheta = min(1., max(-1., (tempA + 2. * tVal[i]) / tempB)); double sinTheta = 2. * sqrtpos( -(tempC + tempA * tVal[i] + tVal[i] * tVal[i]) ) / tempB; theta = asin( min(1., sinTheta)); if (cosTheta < 0.) theta = M_PI - theta; double pAbs34 = 0.5 * lambda34 / eCM; if (i == 0) { pz3 = pAbs34 * cos(theta); pT3 = pAbs34 * sin(theta); } else { pz4 = -pAbs34 * cos(theta); pT4 = pAbs34 * sin(theta); } } if (tryAgain) continue; t1 = tVal[0]; t2 = tVal[1]; // Kinematics construction in the MBR model. } else { pz3 = pAbs * (1. - xi1); pz4 = -pAbs * (1. - xi2); pT3 = sqrt( (1. - xi1) * abs(t1) - s1 * pow2(xi1) ); pT4 = sqrt( (1. - xi2) * abs(t2) - s2 * pow2(xi2) ); } // Common final steps of kinematics. double phi3 = 2. * M_PI * rndmPtr->flat(); double phi4 = 2. * M_PI * rndmPtr->flat(); p3.p( pT3 * cos(phi3), pT3 * sin(phi3), pz3, sqrt(pz3 * pz3 + pT3 * pT3 + s1) ); p4.p( pT4 * cos(phi4), pT4 * sin(phi4), pz4, sqrt(pz4 * pz4 + pT4 * pT4 + s2) ); // Central dissociated system, from Pomeron-Pomeron 4 vectors. p5 = (p1 - p3) + (p2 - p4); mHat = p5.mCalc(); // If acceptable diffractive mass then no more looping. if (mHat > DIFFMASSMIN) break; } return true; } //-------------------------------------------------------------------------- // Construct the four-vector kinematics from the trial values. bool PhaseSpace2to3diffractive::finalKin() { // Particle four-momenta and masses. pH[1] = p1; pH[2] = p2; pH[3] = p3; pH[4] = p4; pH[5] = p5; mH[1] = mA; mH[2] = mB; mH[3] = mA; mH[4] = mB; mH[5] = mHat; // Set some further info for completeness (but Info can be for subprocess). x1H = 1.; x2H = 1.; sH = s; tH = (p1 - p3).m2Calc(); uH = (p2 - p4).m2Calc(); mHat = eCM; p2Abs = pAbs * pAbs; betaZ = 0.; // Store average pT of three final particles for documentation. pTH = (p3.pT() + p4.pT() + p5.pT()) / 3.; // Done. return true; } //========================================================================== // PhaseSpace2to3tauycyl class. // 2 -> 3 kinematics for normal subprocesses. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Number of Newton-Raphson iterations of kinematics when masses introduced. const int PhaseSpace2to3tauycyl::NITERNR = 5; //-------------------------------------------------------------------------- // Set up for fixed or Breit-Wigner mass selection. bool PhaseSpace2to3tauycyl::setupMasses() { // Treat Z0 as such or as gamma*/Z0 gmZmode = gmZmodeGlobal; int gmZmodeProc = sigmaProcessPtr->gmZmode(); if (gmZmodeProc >= 0) gmZmode = gmZmodeProc; // Set sHat limits - based on global limits only. mHatMin = mHatGlobalMin; sHatMin = mHatMin*mHatMin; mHatMax = eCM; if (mHatGlobalMax > mHatGlobalMin) mHatMax = min( eCM, mHatGlobalMax); sHatMax = mHatMax*mHatMax; // Masses and widths of resonances. setupMass1(3); setupMass1(4); setupMass1(5); // Reduced mass range - do not make it as fancy as in two-body case. if (useBW[3]) mUpper[3] -= (mPeak[4] + mPeak[5]); if (useBW[4]) mUpper[4] -= (mPeak[3] + mPeak[5]); if (useBW[5]) mUpper[5] -= (mPeak[3] + mPeak[4]); // If closed phase space then unallowed process. bool physical = true; if (useBW[3] && mUpper[3] < mLower[3] + MASSMARGIN) physical = false; if (useBW[4] && mUpper[4] < mLower[4] + MASSMARGIN) physical = false; if (useBW[5] && mUpper[5] < mLower[5] + MASSMARGIN) physical = false; if (!useBW[3] && !useBW[4] && !useBW[5] && mHatMax < mPeak[3] + mPeak[4] + mPeak[5] + MASSMARGIN) physical = false; if (!physical) return false; // No extra pT precautions in massless limit - assumed fixed by ME's. pTHatMin = pTHatGlobalMin; pT2HatMin = pTHatMin * pTHatMin; pTHatMax = pTHatGlobalMax; pT2HatMax = pTHatMax * pTHatMax; // Prepare to select m3 by BW + flat + 1/s_3. if (useBW[3]) { double distToThreshA = (mHatMax - mPeak[3] - mPeak[4] - mPeak[5]) * mWidth[3] / (pow2(mWidth[3]) + pow2(mWidth[4]) + pow2(mWidth[5])); double distToThreshB = (mHatMax - mPeak[3] - mMin[4] - mMin[5]) / mWidth[3]; double distToThresh = min( distToThreshA, distToThreshB); setupMass2(3, distToThresh); } // Prepare to select m4 by BW + flat + 1/s_3. if (useBW[4]) { double distToThreshA = (mHatMax - mPeak[3] - mPeak[4] - mPeak[5]) * mWidth[4] / (pow2(mWidth[3]) + pow2(mWidth[4]) + pow2(mWidth[5])); double distToThreshB = (mHatMax - mPeak[4] - mMin[3] - mMin[5]) / mWidth[4]; double distToThresh = min( distToThreshA, distToThreshB); setupMass2(4, distToThresh); } // Prepare to select m5 by BW + flat + 1/s_3. if (useBW[5]) { double distToThreshA = (mHatMax - mPeak[3] - mPeak[4] - mPeak[5]) * mWidth[5] / (pow2(mWidth[3]) + pow2(mWidth[4]) + pow2(mWidth[5])); double distToThreshB = (mHatMax - mPeak[5] - mMin[3] - mMin[4]) / mWidth[5]; double distToThresh = min( distToThreshA, distToThreshB); setupMass2(5, distToThresh); } // Initialization masses. For now give up when constrained phase space. m3 = (useBW[3]) ? min(mPeak[3], mUpper[3]) : mPeak[3]; m4 = (useBW[4]) ? min(mPeak[4], mUpper[4]) : mPeak[4]; m5 = (useBW[5]) ? min(mPeak[5], mUpper[5]) : mPeak[5]; if (m3 + m4 + m5 + MASSMARGIN > mHatMax) physical = false; s3 = m3*m3; s4 = m4*m4; s5 = m5*m5; // Correct selected mass-spectrum to running-width Breit-Wigner. // Extra safety margin for maximum search. wtBW = 1.; if (useBW[3]) wtBW *= weightMass(3) * EXTRABWWTMAX; if (useBW[4]) wtBW *= weightMass(4) * EXTRABWWTMAX; if (useBW[5]) wtBW *= weightMass(5) * EXTRABWWTMAX; // Done. return physical; } //-------------------------------------------------------------------------- // Select Breit-Wigner-distributed or fixed masses. bool PhaseSpace2to3tauycyl::trialMasses() { // By default vanishing cross section. sigmaNw = 0.; wtBW = 1.; // Pick m3, m4 and m5 independently. trialMass(3); trialMass(4); trialMass(5); // If outside phase space then reject event. if (m3 + m4 + m5 + MASSMARGIN > mHatMax) return false; // Correct selected mass-spectrum to running-width Breit-Wigner. if (useBW[3]) wtBW *= weightMass(3); if (useBW[4]) wtBW *= weightMass(4); if (useBW[5]) wtBW *= weightMass(5); // Done. return true; } //-------------------------------------------------------------------------- // Construct the four-vector kinematics from the trial values. bool PhaseSpace2to3tauycyl::finalKin() { // Assign masses to particles assumed massless in matrix elements. int id3 = sigmaProcessPtr->id(3); int id4 = sigmaProcessPtr->id(4); int id5 = sigmaProcessPtr->id(5); if (idMass[3] == 0) { m3 = particleDataPtr->m0(id3); s3 = m3*m3; } if (idMass[4] == 0) { m4 = particleDataPtr->m0(id4); s4 = m4*m4; } if (idMass[5] == 0) { m5 = particleDataPtr->m0(id5); s5 = m5*m5; } // Check that phase space still open after new mass assignment. if (m3 + m4 + m5 + MASSMARGIN > mHat) { infoPtr->errorMsg("Warning in PhaseSpace2to3tauycyl::finalKin: " "failed after mass assignment"); return false; } // Particle masses; incoming always on mass shell. mH[1] = 0.; mH[2] = 0.; mH[3] = m3; mH[4] = m4; mH[5] = m5; // Incoming partons along beam axes. pH[1] = Vec4( 0., 0., 0.5 * eCM * x1H, 0.5 * eCM * x1H); pH[2] = Vec4( 0., 0., -0.5 * eCM * x2H, 0.5 * eCM * x2H); // Begin three-momentum rescaling to compensate for masses. if (idMass[3] == 0 || idMass[4] == 0 || idMass[5] == 0) { double p3S = p3cm.pAbs2(); double p4S = p4cm.pAbs2(); double p5S = p5cm.pAbs2(); double fac = 1.; double e3, e4, e5, value, deriv; // Iterate rescaling solution five times, using Newton-Raphson. for (int i = 0; i < NITERNR; ++i) { e3 = sqrt(s3 + fac * p3S); e4 = sqrt(s4 + fac * p4S); e5 = sqrt(s5 + fac * p5S); value = e3 + e4 + e5 - mHat; deriv = 0.5 * (p3S / e3 + p4S / e4 + p5S / e5); fac -= value / deriv; } // Rescale momenta appropriately. double facRoot = sqrt(fac); p3cm.rescale3( facRoot ); p4cm.rescale3( facRoot ); p5cm.rescale3( facRoot ); p3cm.e( sqrt(s3 + fac * p3S) ); p4cm.e( sqrt(s4 + fac * p4S) ); p5cm.e( sqrt(s5 + fac * p5S) ); } // Outgoing partons initially in collision CM frame along beam axes. pH[3] = p3cm; pH[4] = p4cm; pH[5] = p5cm; // Then boost them to overall CM frame betaZ = (x1H - x2H)/(x1H + x2H); pH[3].rot( theta, phi); pH[4].rot( theta, phi); pH[3].bst( 0., 0., betaZ); pH[4].bst( 0., 0., betaZ); pH[5].bst( 0., 0., betaZ); // Store average pT of three final particles for documentation. pTH = (p3cm.pT() + p4cm.pT() + p5cm.pT()) / 3.; // Done. return true; } //========================================================================== // The PhaseSpace2to3yyycyl class. // Phase space for 2 -> 3 QCD processes, 1 + 2 -> 3 + 4 + 5 set up in // y3, y4, y5, pT2_3, pT2_5, phi_3 and phi_5, and with R separation cut. // Note: here cout is used for output, not os. Change?? //-------------------------------------------------------------------------- // Sample the phase space of the process. bool PhaseSpace2to3yyycyl::setupSampling() { // Phase space cuts specifically for 2 -> 3 QCD processes. pTHat3Min = settingsPtr->parm("PhaseSpace:pTHat3Min"); pTHat3Max = settingsPtr->parm("PhaseSpace:pTHat3Max"); pTHat5Min = settingsPtr->parm("PhaseSpace:pTHat5Min"); pTHat5Max = settingsPtr->parm("PhaseSpace:pTHat5Max"); RsepMin = settingsPtr->parm("PhaseSpace:RsepMin"); R2sepMin = pow2(RsepMin); // If both beams are baryons then softer PDF's than for mesons/Pomerons. hasBaryonBeams = ( beamAPtr->isBaryon() && beamBPtr->isBaryon() ); // Work with massless partons. for (int i = 0; i < 6; ++i) mH[i] = 0.; // Constrain to possible cuts at current CM energy and check consistency. pT3Min = pTHat3Min; pT3Max = pTHat3Max; if (pT3Max < pT3Min) pT3Max = 0.5 * eCM; pT5Min = pTHat5Min; pT5Max = pTHat5Max; if (pT5Max < pT5Min) pT5Max = 0.5 * eCM; if (pT5Max > pT3Max || pT5Min > pT3Min || pT3Min + 2. * pT5Min > eCM) { infoPtr->errorMsg("Error in PhaseSpace2to3yyycyl::setupSampling: " "inconsistent pT limits in 3-body phase space"); return false; } // Loop over some configurations where cross section could be maximal. // In all cases all sum p_z = 0, for maximal PDF weights. // Also pT3 and R45 are minimal, while pT5 may vary. sigmaMx = 0.; double pT5EffMax = min( pT5Max, 0.5 * pT3Min / cos(0.5 * RsepMin) ); double pT3EffMin = max( pT3Min, 2.0 * pT5Min * cos(0.5 * RsepMin) ) ; double sinhR = sinh(0.5 * RsepMin); double coshR = cosh(0.5 * RsepMin); for (int iStep = 0; iStep < 120; ++iStep) { // First kind: |phi4 - phi5| = R, all p_z = 0, i.e. separation in phi. if (iStep < 10) { pT3 = pT3EffMin; pT5 = pT5Min * pow( pT5EffMax / pT5Min, iStep / 9.); double pTRat = pT5 / pT3; double sin2Rsep = pow2( sin(RsepMin) ); double cosPhi35 = - cos(RsepMin) * sqrtpos(1. - sin2Rsep * pow2(pTRat)) - sin2Rsep * pTRat; cosPhi35 = max( cosPhi35, cos(M_PI - 0.5 * RsepMin) ); double sinPhi35 = sqrt(1. - pow2(cosPhi35)); pT4 = sqrt( pow2(pT3) + pow2(pT5) + 2. * pT3 * pT5 * cosPhi35); p3cm = pT3 * Vec4( 1., 0., 0., 1.); p4cm = Vec4(-pT3 - pT5 * cosPhi35, -pT5 * sinPhi35, 0., pT4); p5cm = pT5 * Vec4( cosPhi35, sinPhi35, 0., 1.); // Second kind: |y4 - y5| = R, phi4 = phi5, i.e. separation in y. } else { pT5 = pT5Min * pow( pT5Max / pT5Min, iStep%10 / 9. ); pT3 = max( pT3Min, 2. * pT5); pT4 = pT3 - pT5; p4cm = pT4 * Vec4( -1., 0., sinhR, coshR ); p5cm = pT5 * Vec4( -1., 0., -sinhR, coshR ); y3 = -1.2 + 0.2 * (iStep/10); p3cm = pT3 * Vec4( 1., 0., sinh(y3), cosh(y3)); betaZ = (p3cm.pz() + p4cm.pz() + p5cm.pz()) / (p3cm.e() + p4cm.e() + p5cm.e()); p3cm.bst( 0., 0., -betaZ); p4cm.bst( 0., 0., -betaZ); p5cm.bst( 0., 0., -betaZ); } // Find cross section in chosen phase space point. pInSum = p3cm + p4cm + p5cm; x1H = pInSum.e() / eCM; x2H = x1H; sH = pInSum.m2Calc(); sigmaProcessPtr->set3Kin( x1H, x2H, sH, p3cm, p4cm, p5cm, 0., 0., 0., 1., 1., 1.); sigmaNw = sigmaProcessPtr->sigmaPDF(); // Multiply by Jacobian. double flux = 1. /(8. * pow2(sH) * pow5(2. * M_PI)); double pTRng = pow2(M_PI) * pow4(pT3) * (1./pow2(pT3Min) - 1./pow2(pT3Max)) * pow2(pT5) * 2.* log(pT5Max/pT5Min); double yRng = 8. * log(eCM / pT3) * log(eCM / pT4) * log(eCM / pT5); sigmaNw *= SAFETYMARGIN * flux * pTRng * yRng; // Update to largest maximum. if (showSearch && sigmaNw > sigmaMx) cout << "\n New sigmamax is " << scientific << setprecision(3) << sigmaNw << " for x1 = " << x1H << " x2 = " << x2H << " sH = " << sH << endl << " p3 = " << p3cm << " p4 = " << p4cm << " p5 = " << p5cm; if (sigmaNw > sigmaMx) sigmaMx = sigmaNw; } sigmaPos = sigmaMx; // Done. return true; } //-------------------------------------------------------------------------- // Sample the phase space of the process. bool PhaseSpace2to3yyycyl::trialKin(bool inEvent, bool) { // Allow for possibility that energy varies from event to event. if (doEnergySpread) { eCM = infoPtr->eCM(); s = eCM * eCM; } sigmaNw = 0.; // Constrain to possible cuts at current CM energy and check consistency. pT3Min = pTHat3Min; pT3Max = pTHat3Max; if (pT3Max < pT3Min) pT3Max = 0.5 * eCM; pT5Min = pTHat5Min; pT5Max = pTHat5Max; if (pT5Max < pT5Min) pT5Max = 0.5 * eCM; if (pT5Max > pT3Max || pT5Min > pT3Min || pT3Min + 2. * pT5Min > eCM) { infoPtr->errorMsg("Error in PhaseSpace2to3yyycyl::trialKin: " "inconsistent pT limits in 3-body phase space"); return false; } // Pick pT3 according to d^2(pT3)/pT3^4 and pT5 to d^2(pT5)/pT5^2. pT3 = pT3Min * pT3Max / sqrt( pow2(pT3Min) + rndmPtr->flat() * (pow2(pT3Max) - pow2(pT3Min)) ); pT5Max = min(pT5Max, pT3); if (pT5Max < pT5Min) return false; pT5 = pT5Min * pow( pT5Max / pT5Min, rndmPtr->flat() ); // Pick azimuthal angles flat and reconstruct pT4, between pT3 and pT5. phi3 = 2. * M_PI * rndmPtr->flat(); phi5 = 2. * M_PI * rndmPtr->flat(); pT4 = sqrt( pow2(pT3) + pow2(pT5) + 2. * pT3 * pT5 * cos(phi3 - phi5) ); if (pT4 > pT3 || pT4 < pT5) return false; phi4 = atan2( -(pT3 * sin(phi3) + pT5 * sin(phi5)), -(pT3 * cos(phi3) + pT5 * cos(phi5)) ); // Pick rapidities flat in allowed ranges. y3Max = log(eCM / pT3); y4Max = log(eCM / pT4); y5Max = log(eCM / pT5); y3 = y3Max * (2. * rndmPtr->flat() - 1.); y4 = y4Max * (2. * rndmPtr->flat() - 1.); y5 = y5Max * (2. * rndmPtr->flat() - 1.); // Reject some events at large rapidities to improve efficiency. // (Works for baryons, not pions or Pomerons if they have hard PDF's.) double WTy = (hasBaryonBeams) ? (1. - pow2(y3/y3Max)) * (1. - pow2(y4/y4Max)) * (1. - pow2(y5/y5Max)) : 1.; if (WTy < rndmPtr->flat()) return false; // Check that any pair separated more then RsepMin in (y, phi) space. dphi = abs(phi3 - phi4); if (dphi > M_PI) dphi = 2. * M_PI - dphi; if (pow2(y3 - y4) + pow2(dphi) < R2sepMin) return false; dphi = abs(phi3 - phi5); if (dphi > M_PI) dphi = 2. * M_PI - dphi; if (pow2(y3 - y5) + pow2(dphi) < R2sepMin) return false; dphi = abs(phi4 - phi5); if (dphi > M_PI) dphi = 2. * M_PI - dphi; if (pow2(y4 - y5) + pow2(dphi) < R2sepMin) return false; // Reconstruct all four-vectors. pH[3] = pT3 * Vec4( cos(phi3), sin(phi3), sinh(y3), cosh(y3) ); pH[4] = pT4 * Vec4( cos(phi4), sin(phi4), sinh(y4), cosh(y4) ); pH[5] = pT5 * Vec4( cos(phi5), sin(phi5), sinh(y5), cosh(y5) ); pInSum = pH[3] + pH[4] + pH[5]; // Check that x values physical and sHat in allowed range. x1H = (pInSum.e() + pInSum.pz()) / eCM; x2H = (pInSum.e() - pInSum.pz()) / eCM; if (x1H >= 1. || x2H >= 1.) return false; sH = pInSum.m2Calc(); if ( sH < pow2(mHatGlobalMin) || (mHatGlobalMax > mHatGlobalMin && sH > pow2(mHatGlobalMax)) ) return false; // Boost four-vectors to rest frame of collision. betaZ = (x1H - x2H)/(x1H + x2H); p3cm = pH[3]; p3cm.bst( 0., 0., -betaZ); p4cm = pH[4]; p4cm.bst( 0., 0., -betaZ); p5cm = pH[5]; p5cm.bst( 0., 0., -betaZ); // Find cross section in chosen phase space point. sigmaProcessPtr->set3Kin( x1H, x2H, sH, p3cm, p4cm, p5cm, 0., 0., 0., 1., 1., 1.); sigmaNw = sigmaProcessPtr->sigmaPDF(); // Multiply by Jacobian. Correct for rejection of large rapidities. double flux = 1. /(8. * pow2(sH) * pow5(2. * M_PI)); double yRng = 8. * y3Max * y4Max * y5Max; double pTRng = pow2(M_PI) * pow4(pT3) * (1./pow2(pT3Min) - 1./pow2(pT3Max)) * pow2(pT5) * 2.* log(pT5Max/pT5Min); sigmaNw *= flux * yRng * pTRng / WTy; // Allow possibility for user to modify cross section. if (canModifySigma) sigmaNw *= userHooksPtr->multiplySigmaBy( sigmaProcessPtr, this, inEvent); if (canBiasSelection) sigmaNw *= userHooksPtr->biasSelectionBy( sigmaProcessPtr, this, inEvent); if (canBias2Sel) sigmaNw *= pow( pTH / bias2SelRef, bias2SelPow); // Check if maximum violated. newSigmaMx = false; if (sigmaNw > sigmaMx) { infoPtr->errorMsg("Warning in PhaseSpace2to3yyycyl::trialKin: " "maximum for cross section violated"); // Violation strategy 1: increase maximum (always during initialization). if (increaseMaximum || !inEvent) { double violFact = SAFETYMARGIN * sigmaNw / sigmaMx; sigmaMx = SAFETYMARGIN * sigmaNw; newSigmaMx = true; if (showViolation) { if (violFact < 9.99) cout << fixed; else cout << scientific; cout << " PYTHIA Maximum for " << sigmaProcessPtr->name() << " increased by factor " << setprecision(3) << violFact << " to " << scientific << sigmaMx << endl; } // Violation strategy 2: weight event (done in ProcessContainer). } else if (showViolation && sigmaNw > sigmaPos) { double violFact = sigmaNw / sigmaMx; if (violFact < 9.99) cout << fixed; else cout << scientific; cout << " PYTHIA Maximum for " << sigmaProcessPtr->name() << " exceeded by factor " << setprecision(3) << violFact << endl; sigmaPos = sigmaNw; } } // Check if negative cross section. if (sigmaNw < sigmaNeg) { infoPtr->errorMsg("Warning in PhaseSpace2to3yyycyl::trialKin:" " negative cross section set 0", "for " + sigmaProcessPtr->name() ); sigmaNeg = sigmaNw; // Optional printout of (all) violations. if (showViolation) cout << " PYTHIA Negative minimum for " << sigmaProcessPtr->name() << " changed to " << scientific << setprecision(3) << sigmaNeg << endl; } if (sigmaNw < 0.) sigmaNw = 0.; // Done. return true; } //-------------------------------------------------------------------------- // Construct the final kinematics of the process: not much left bool PhaseSpace2to3yyycyl::finalKin() { // Work with massless partons. for (int i = 0; i < 6; ++i) mH[i] = 0.; // Ibncoming partons to collision. pH[1] = 0.5 * (pInSum.e() + pInSum.pz()) * Vec4( 0., 0., 1., 1.); pH[2] = 0.5 * (pInSum.e() - pInSum.pz()) * Vec4( 0., 0., -1., 1.); // Some quantities meaningless for 2 -> 3. pT devined as average value. tH = 0.; uH = 0.; pTH = (pH[3].pT() + pH[4].pT() + pH[5].pT()) / 3.; theta = 0.; phi = 0.; return true; } //========================================================================== // The PhaseSpaceLHA class. // A derived class for Les Houches events. // Note: arbitrary subdivision into PhaseSpaceLHA and SigmaLHAProcess tasks. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // LHA convention with cross section in pb forces conversion to mb. const double PhaseSpaceLHA::CONVERTPB2MB = 1e-9; //-------------------------------------------------------------------------- // Find maximal cross section for comparison with internal processes. bool PhaseSpaceLHA::setupSampling() { // Find which strategy Les Houches events are produced with. strategy = lhaUpPtr->strategy(); stratAbs = abs(strategy); if (strategy == 0 || stratAbs > 4) { ostringstream stratCode; stratCode << strategy; infoPtr->errorMsg("Error in PhaseSpaceLHA::setupSampling: unknown " "Les Houches Accord weighting stategy", stratCode.str()); return false; } // Number of contributing processes. nProc = lhaUpPtr->sizeProc(); // Loop over all processes. Read out maximum and cross section. xMaxAbsSum = 0.; xSecSgnSum = 0.; int idPr; double xMax, xSec, xMaxAbs; for (int iProc = 0 ; iProc < nProc; ++iProc) { idPr = lhaUpPtr->idProcess(iProc); xMax = lhaUpPtr->xMax(iProc); xSec = lhaUpPtr->xSec(iProc); // Check for inconsistencies between strategy and stored values. if ( (strategy == 1 || strategy == 2) && xMax < 0.) { infoPtr->errorMsg("Error in PhaseSpaceLHA::setupSampling: " "negative maximum not allowed"); return false; } if ( ( strategy == 2 || strategy == 3) && xSec < 0.) { infoPtr->errorMsg("Error in PhaseSpaceLHA::setupSampling: " "negative cross section not allowed"); return false; } // Store maximal cross sections for later choice. if (stratAbs == 1) xMaxAbs = abs(xMax); else if (stratAbs < 4) xMaxAbs = abs(xSec); else xMaxAbs = 1.; idProc.push_back( idPr ); xMaxAbsProc.push_back( xMaxAbs ); // Find sum and convert to mb. xMaxAbsSum += xMaxAbs; xSecSgnSum += xSec; } sigmaMx = xMaxAbsSum * CONVERTPB2MB; sigmaSgn = xSecSgnSum * CONVERTPB2MB; // Done. return true; } //-------------------------------------------------------------------------- // Construct the next process, by interface to Les Houches class. bool PhaseSpaceLHA::trialKin( bool, bool repeatSame ) { // Must select process type in some cases. int idProcNow = 0; if (repeatSame) idProcNow = idProcSave; else if (stratAbs <= 2) { double xMaxAbsRndm = xMaxAbsSum * rndmPtr->flat(); int iProc = -1; do xMaxAbsRndm -= xMaxAbsProc[++iProc]; while (xMaxAbsRndm > 0. && iProc < nProc - 1); idProcNow = idProc[iProc]; } // Generate Les Houches event. Return if fail (= end of file). bool physical = lhaUpPtr->setEvent(idProcNow, mRecalculate); if (!physical) return false; // Find which process was generated. int idPr = lhaUpPtr->idProcess(); int iProc = 0; for (int iP = 0; iP < int(idProc.size()); ++iP) if (idProc[iP] == idPr) iProc = iP; idProcSave = idPr; // Extract cross section and rescale according to strategy. double wtPr = lhaUpPtr->weight(); if (stratAbs == 1) sigmaNw = wtPr * CONVERTPB2MB * xMaxAbsSum / xMaxAbsProc[iProc]; else if (stratAbs == 2) sigmaNw = (wtPr / abs(lhaUpPtr->xMax(iProc))) * sigmaMx; else if (strategy == 3) sigmaNw = sigmaMx; else if (strategy == -3 && wtPr > 0.) sigmaNw = sigmaMx; else if (strategy == -3) sigmaNw = -sigmaMx; else if (stratAbs == 4) sigmaNw = wtPr * CONVERTPB2MB; // Set x scales. x1H = lhaUpPtr->x1(); x2H = lhaUpPtr->x2(); // Done. return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/Analysis.cc0000644000175000017500000011720312217346244015223 0ustar sunsun// Analysis.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // Sphericity, Thrust, ClusJet, CellJet and SlowJet classes. #include "Pythia8/Analysis.h" #include "Pythia8/FJcore.h" namespace Pythia8 { //========================================================================== // Sphericity class. // This class finds sphericity-related properties of an event. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Minimum number of particles to perform study. const int Sphericity::NSTUDYMIN = 2; // Maximum number of times that an error warning will be printed. const int Sphericity::TIMESTOPRINT = 1; // Assign mimimum squared momentum in weight to avoid division by zero. const double Sphericity::P2MIN = 1e-20; // Second eigenvalue not too low or not possible to find eigenvectors. const double Sphericity::EIGENVALUEMIN = 1e-10; //-------------------------------------------------------------------------- // Analyze event. bool Sphericity::analyze(const Event& event, ostream& os) { // Initial values, tensor and counters zero. eVal1 = eVal2 = eVal3 = 0.; eVec1 = eVec2 = eVec3 = 0.; double tt[4][4]; for (int j = 1; j < 4; ++j) for (int k = j; k < 4; ++k) tt[j][k] = 0.; int nStudy = 0; double denom = 0.; // Loop over desired particles in the event. for (int i = 0; i < event.size(); ++i) if (event[i].isFinal()) { if (select > 2 && event[i].isNeutral() ) continue; if (select == 2 && !event[i].isVisible() ) continue; ++nStudy; // Calculate matrix to be diagonalized. Special cases for speed. double pNow[4]; pNow[1] = event[i].px(); pNow[2] = event[i].py(); pNow[3] = event[i].pz(); double p2Now = pNow[1]*pNow[1] + pNow[2]*pNow[2] + pNow[3]*pNow[3]; double pWeight = 1.; if (powerInt == 1) pWeight = 1. / sqrt(max(P2MIN, p2Now)); else if (powerInt == 0) pWeight = pow( max(P2MIN, p2Now), powerMod); for (int j = 1; j < 4; ++j) for (int k = j; k < 4; ++k) tt[j][k] += pWeight * pNow[j] * pNow[k]; denom += pWeight * p2Now; } // Very low multiplicities (0 or 1) not considered. if (nStudy < NSTUDYMIN) { if (nFew < TIMESTOPRINT) os << " PYTHIA Error in " << "Sphericity::analyze: too few particles" << endl; ++nFew; return false; } // Normalize tensor to trace = 1. for (int j = 1; j < 4; ++j) for (int k = j; k < 4; ++k) tt[j][k] /= denom; // Find eigenvalues to matrix (third degree equation). double qCoef = ( tt[1][1] * tt[2][2] + tt[1][1] * tt[3][3] + tt[2][2] * tt[3][3] - pow2(tt[1][2]) - pow2(tt[1][3]) - pow2(tt[2][3]) ) / 3. - 1./9.; double qCoefRt = sqrt( -qCoef); double rCoef = -0.5 * ( qCoef + 1./9. + tt[1][1] * pow2(tt[2][3]) + tt[2][2] * pow2(tt[1][3]) + tt[3][3] * pow2(tt[1][2]) - tt[1][1] * tt[2][2] * tt[3][3] ) + tt[1][2] * tt[1][3] * tt[2][3] + 1./27.; double pTemp = max( min( rCoef / pow3(qCoefRt), 1.), -1.); double pCoef = cos( acos(pTemp) / 3.); double pCoefRt = sqrt( 3. * (1. - pow2(pCoef)) ); eVal1 = 1./3. + qCoefRt * max( 2. * pCoef, pCoefRt - pCoef); eVal3 = 1./3. + qCoefRt * min( 2. * pCoef, -pCoefRt - pCoef); eVal2 = 1. - eVal1 - eVal3; // Begin find first and last eigenvector. for (int iVal = 0; iVal < 2; ++iVal) { double eVal = (iVal == 0) ? eVal1 : eVal3; // If all particles are back-to-back then simpleminded third axis. if (iVal > 0 && eVal2 < EIGENVALUEMIN) { if ( abs(eVec1.pz()) > 0.5) eVec3 = Vec4( 1., 0., 0., 0.); else eVec3 = Vec4( 0., 0., 1., 0.); eVec3 -= dot3( eVec1, eVec3) * eVec1; eVec3 /= eVec3.pAbs(); eVec2 = cross3( eVec1, eVec3); return true; } // Set up matrix to diagonalize. double dd[4][4]; for (int j = 1; j < 4; ++j) { dd[j][j] = tt[j][j] - eVal; for (int k = j + 1; k < 4; ++k) { dd[j][k] = tt[j][k]; dd[k][j] = tt[j][k]; } } // Find largest = pivotal element in matrix. int jMax = 0; int kMax = 0; double ddMax = 0.; for (int j = 1; j < 4; ++j) for (int k = 1; k < 4; ++k) if (abs(dd[j][k]) > ddMax) { jMax = j; kMax = k; ddMax = abs(dd[j][k]); } // Subtract one row from the other two; find new largest element. int jMax2 = 0; ddMax = 0.; for (int j = 1; j < 4; ++j) if ( j != jMax) { double pivot = dd[j][kMax] / dd[jMax][kMax]; for (int k = 1; k < 4; ++k) { dd[j][k] -= pivot * dd[jMax][k]; if (abs(dd[j][k]) > ddMax) { jMax2 = j; ddMax = abs(dd[j][k]); } } } // Construct eigenvector. Normalize to unit length; sign irrelevant. int k1 = kMax + 1; if (k1 > 3) k1 -= 3; int k2 = kMax + 2; if (k2 > 3) k2 -= 3; double eVec[4]; eVec[k1] = -dd[jMax2][k2]; eVec[k2] = dd[jMax2][k1]; eVec[kMax] = (dd[jMax][k1] * dd[jMax2][k2] - dd[jMax][k2] * dd[jMax2][k1]) / dd[jMax][kMax]; double length = sqrt( pow2(eVec[1]) + pow2(eVec[2]) + pow2(eVec[3]) ); // Store eigenvectors. if (iVal == 0) eVec1 = Vec4( eVec[1] / length, eVec[2] / length, eVec[3] / length, 0.); else eVec3 = Vec4( eVec[1] / length, eVec[2] / length, eVec[3] / length, 0.); } // Middle eigenvector is orthogonal to the other two; sign irrelevant. eVec2 = cross3( eVec1, eVec3); // Done. return true; } //-------------------------------------------------------------------------- // Provide a listing of the info. void Sphericity::list(ostream& os) const { // Header. os << "\n -------- PYTHIA Sphericity Listing -------- \n"; if (powerInt !=2) os << " Nonstandard momentum power = " << fixed << setprecision(3) << setw(6) << power << "\n"; os << "\n no lambda e_x e_y e_z \n"; // The three eigenvalues and eigenvectors. os << setprecision(5); os << " 1" << setw(11) << eVal1 << setw(11) << eVec1.px() << setw(10) << eVec1.py() << setw(10) << eVec1.pz() << "\n"; os << " 2" << setw(11) << eVal2 << setw(11) << eVec2.px() << setw(10) << eVec2.py() << setw(10) << eVec2.pz() << "\n"; os << " 3" << setw(11) << eVal3 << setw(11) << eVec3.px() << setw(10) << eVec3.py() << setw(10) << eVec3.pz() << "\n"; // Listing finished. os << "\n -------- End PYTHIA Sphericity Listing ----" << endl; } //========================================================================== // Thrust class. // This class finds thrust-related properties of an event. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Minimum number of particles to perform study. const int Thrust::NSTUDYMIN = 2; // Maximum number of times that an error warning will be printed. const int Thrust::TIMESTOPRINT = 1; // Major not too low or not possible to find major axis. const double Thrust::MAJORMIN = 1e-10; //-------------------------------------------------------------------------- // Analyze event. bool Thrust::analyze(const Event& event, ostream& os) { // Initial values and counters zero. eVal1 = eVal2 = eVal3 = 0.; eVec1 = eVec2 = eVec3 = 0.; int nStudy = 0; vector pOrder; Vec4 pSum, nRef, pPart, pFull, pMax; // Loop over desired particles in the event. for (int i = 0; i < event.size(); ++i) if (event[i].isFinal()) { if (select > 2 && event[i].isNeutral() ) continue; if (select == 2 && !event[i].isVisible() ) continue; ++nStudy; // Store momenta. Use energy component for absolute momentum. Vec4 pNow = event[i].p(); pNow.e(pNow.pAbs()); pSum += pNow; pOrder.push_back(pNow); } // Very low multiplicities (0 or 1) not considered. if (nStudy < NSTUDYMIN) { if (nFew < TIMESTOPRINT) os << " PYTHIA Error in " << "Thrust::analyze: too few particles" << endl; ++nFew; return false; } // Try all combinations of reference vector orthogonal to two particles. for (int i1 = 0; i1 < nStudy - 1; ++i1) for (int i2 = i1 + 1; i2 < nStudy; ++i2) { nRef = cross3( pOrder[i1], pOrder[i2]); nRef /= nRef.pAbs(); pPart = 0.; // Add all momenta with sign; two choices for each reference particle. for (int i = 0; i < nStudy; ++i) if (i != i1 && i != i2) { if (dot3(pOrder[i], nRef) > 0.) pPart += pOrder[i]; else pPart -= pOrder[i]; } for (int j = 0; j < 4; ++j) { if (j == 0) pFull = pPart + pOrder[i1] + pOrder[i2]; else if (j == 1) pFull = pPart + pOrder[i1] - pOrder[i2]; else if (j == 2) pFull = pPart - pOrder[i1] + pOrder[i2]; else pFull = pPart - pOrder[i1] - pOrder[i2]; pFull.e(pFull.pAbs()); if (pFull.e() > pMax.e()) pMax = pFull; } } // Maximum gives thrust axis and value. eVal1 = pMax.e() / pSum.e(); eVec1 = pMax / pMax.e(); eVec1.e(0.); // Subtract momentum along thrust axis. double pAbsSum = 0.; for (int i = 0; i < nStudy; ++i) { pOrder[i] -= dot3( eVec1, pOrder[i]) * eVec1; pOrder[i].e(pOrder[i].pAbs()); pAbsSum += pOrder[i].e(); } // Simpleminded major and minor axes if too little transverse left. if (pAbsSum < MAJORMIN * pSum.e()) { if ( abs(eVec1.pz()) > 0.5) eVec2 = Vec4( 1., 0., 0., 0.); else eVec2 = Vec4( 0., 0., 1., 0.); eVec2 -= dot3( eVec1, eVec2) * eVec1; eVec2 /= eVec2.pAbs(); eVec3 = cross3( eVec1, eVec2); return true; } // Try all reference vectors orthogonal to one particles. pMax = 0.; for (int i1 = 0; i1 < nStudy; ++i1) { nRef = cross3( pOrder[i1], eVec1); nRef /= nRef.pAbs(); pPart = 0.; // Add all momenta with sign; two choices for each reference particle. for (int i = 0; i < nStudy; ++i) if (i != i1) { if (dot3(pOrder[i], nRef) > 0.) pPart += pOrder[i]; else pPart -= pOrder[i]; } pFull = pPart + pOrder[i1]; pFull.e(pFull.pAbs()); if (pFull.e() > pMax.e()) pMax = pFull; pFull = pPart - pOrder[i1]; pFull.e(pFull.pAbs()); if (pFull.e() > pMax.e()) pMax = pFull; } // Maximum gives major axis and value. eVal2 = pMax.e() / pSum.e(); eVec2 = pMax / pMax.e(); eVec2.e(0.); // Orthogonal direction gives minor axis, and from there value. eVec3 = cross3( eVec1, eVec2); pAbsSum = 0.; for (int i = 0; i < nStudy; ++i) pAbsSum += abs( dot3(eVec3, pOrder[i]) ); eVal3 = pAbsSum / pSum.e(); // Done. return true; } //-------------------------------------------------------------------------- // Provide a listing of the info. void Thrust::list(ostream& os) const { // Header. os << "\n -------- PYTHIA Thrust Listing ------------ \n" << "\n value e_x e_y e_z \n"; // The thrust, major and minor values and related event axes. os << setprecision(5); os << " Thr" << setw(11) << eVal1 << setw(11) << eVec1.px() << setw(10) << eVec1.py() << setw(10) << eVec1.pz() << "\n"; os << " Maj" << setw(11) << eVal2 << setw(11) << eVec2.px() << setw(10) << eVec2.py() << setw(10) << eVec2.pz() << "\n"; os << " Min" << setw(11) << eVal3 << setw(11) << eVec3.px() << setw(10) << eVec3.py() << setw(10) << eVec3.pz() << "\n"; // Listing finished. os << "\n -------- End PYTHIA Thrust Listing --------" << endl; } //========================================================================== // SingleClusterJet class. // Simple helper class to ClusterJet for a jet and its contents. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Assign minimal pAbs to avoid division by zero. const double SingleClusterJet::PABSMIN = 1e-10; //-------------------------------------------------------------------------- // Distance measures between two SingleClusterJet objects. double dist2Fun(int measure, const SingleClusterJet& j1, const SingleClusterJet& j2) { // JADE distance. if (measure == 2) return 2. * j1.pJet.e() * j2.pJet.e() * (1. - dot3( j1.pJet, j2.pJet) / (j1.pAbs * j2.pAbs) ); // Durham distance. if (measure == 3) return 2. * pow2( min( j1.pJet.e(), j2.pJet.e() ) ) * (1. - dot3( j1.pJet, j2.pJet) / (j1.pAbs * j2.pAbs) ); // Lund distance; "default". return (j1.pAbs * j2.pAbs - dot3( j1.pJet, j2.pJet)) * 2. * j1.pAbs * j2.pAbs / pow2(j1.pAbs + j2.pAbs); } //========================================================================== // ClusterJet class. // This class performs a jet clustering according to different // distance measures: Lund, JADE or Durham. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Maximum number of times that an error warning will be printed. const int ClusterJet::TIMESTOPRINT = 1; // Assume the pi+- mass for all particles, except the photon, in one option. const double ClusterJet::PIMASS = 0.13957; // Assign minimal pAbs to avoid division by zero. const double ClusterJet::PABSMIN = 1e-10; // Initial pT/m preclustering scale as fraction of clustering one. const double ClusterJet::PRECLUSTERFRAC = 0.1; // Step with which pT/m is reduced if preclustering gives too few jets. const double ClusterJet::PRECLUSTERSTEP = 0.8; //-------------------------------------------------------------------------- // Analyze event. bool ClusterJet::analyze(const Event& event, double yScaleIn, double pTscaleIn, int nJetMinIn, int nJetMaxIn, ostream& os) { // Input values. Initial values zero. yScale = yScaleIn; pTscale = pTscaleIn; nJetMin = nJetMinIn; nJetMax = nJetMaxIn; particles.resize(0); jets.resize(0); Vec4 pSum; distances.clear(); // Loop over desired particles in the event. for (int i = 0; i < event.size(); ++i) if (event[i].isFinal()) { if (select > 2 && event[i].isNeutral() ) continue; if (select == 2 && !event[i].isVisible() ) continue; // Store them, possibly with modified mass => new energy. Vec4 pTemp = event[i].p(); if (massSet == 0 || massSet == 1) { double mTemp = (massSet == 0 || event[i].id() == 22) ? 0. : PIMASS; double eTemp = sqrt(pTemp.pAbs2() + pow2(mTemp)); pTemp.e(eTemp); } particles.push_back( SingleClusterJet(pTemp, i) ); pSum += pTemp; } // Very low multiplicities not considered. nParticles = particles.size(); if (nParticles < nJetMin) { if (nFew < TIMESTOPRINT) os << " PYTHIA Error in " << "ClusterJet::analyze: too few particles" << endl; ++nFew; return false; } // Squared maximum distance in GeV^2 for joining. double p2Sum = pSum.m2Calc(); dist2Join = max( yScale * p2Sum, pow2(pTscale)); dist2BigMin = 2. * max( dist2Join, p2Sum); // Do preclustering if desired and possible. if (doPrecluster && nParticles > nJetMin + 2) { precluster(); if (doReassign) reassign(); } // If no preclustering: each particle is a starting jet. else for (int i = 0; i < nParticles; ++i) { jets.push_back( SingleClusterJet(particles[i]) ); particles[i].daughter = i; } // Begin iteration towards fewer jets. for ( ; ; ) { // Find the two closest jets. double dist2Min = dist2BigMin; int jMin = 0; int kMin = 0; for (int j = 0; j < int(jets.size()) - 1; ++j) for (int k = j + 1; k < int(jets.size()); ++k) { double dist2 = dist2Fun( measure, jets[j], jets[k]); if (dist2 < dist2Min) { dist2Min = dist2; jMin = j; kMin = k; } } // Stop if no pair below cut and not more jets than allowed. if ( dist2Min > dist2Join && (nJetMax < nJetMin || int(jets.size()) <= nJetMax) ) break; // Stop if reached minimum allowed number of jets. Else continue. if (int(jets.size()) <= nJetMin) break; // Join two closest jets. jets[jMin].pJet += jets[kMin].pJet; jets[jMin].pAbs = max( PABSMIN, jets[jMin].pJet.pAbs()); jets[jMin].multiplicity += jets[kMin].multiplicity; for (int i = 0; i < nParticles; ++i) if (particles[i].daughter == kMin) particles[i].daughter = jMin; // Save the last 5 distances. distances.push_front(dist2Min); if (distances.size() > 5) distances.pop_back(); // Move up last jet to empty slot to shrink list. jets[kMin] = jets.back(); jets.pop_back(); int iEnd = jets.size(); for (int i = 0; i < nParticles; ++i) if (particles[i].daughter == iEnd) particles[i].daughter = kMin; // Do reassignments of particles to nearest jet if desired. if (doReassign) reassign(); } // Order jets in decreasing energy. for (int j = 0; j < int(jets.size()) - 1; ++j) for (int k = int(jets.size()) - 1; k > j; --k) if (jets[k].pJet.e() > jets[k-1].pJet.e()) { swap( jets[k], jets[k-1]); for (int i = 0; i < nParticles; ++i) { if (particles[i].daughter == k) particles[i].daughter = k-1; else if (particles[i].daughter == k-1) particles[i].daughter = k; } } // Done. return true; } //-------------------------------------------------------------------------- // Precluster nearby particles to save computer time. void ClusterJet::precluster() { // Begin iteration over preclustering scale. distPre = PRECLUSTERFRAC * sqrt(dist2Join) / PRECLUSTERSTEP; for ( ; ;) { distPre *= PRECLUSTERSTEP; dist2Pre = pow2(distPre); for (int i = 0; i < nParticles; ++i) { particles[i].daughter = -1; particles[i].isAssigned = false; } // Sum up low-momentum region. Jet if enough momentum. Vec4 pCentral; int multCentral = 0; for (int i = 0; i < nParticles; ++i) if (particles[i].pAbs < 2. * distPre) { pCentral += particles[i].pJet; multCentral += particles[i].multiplicity; particles[i].isAssigned = true; } if (pCentral.pAbs() > 2. * distPre) { jets.push_back( SingleClusterJet(pCentral) ); jets.back().multiplicity = multCentral; for (int i = 0; i < nParticles; ++i) if (particles[i].isAssigned) particles[i].daughter = 0; } // Find fastest remaining particle until none left. for ( ; ;) { int iMax = -1; double pMax = 0.; for (int i = 0; i < nParticles; ++i) if ( !particles[i].isAssigned && particles[i].pAbs > pMax) { iMax = i; pMax = particles[i].pAbs; } if (iMax == -1) break; // Sum up precluster around it according to distance function. Vec4 pPre; int multPre = 0; int nRemain = 0; for (int i = 0; i < nParticles; ++i) if ( !particles[i].isAssigned) { double dist2 = dist2Fun( measure, particles[iMax], particles[i]); if (dist2 < dist2Pre) { pPre += particles[i].pJet; ++multPre; particles[i].isAssigned = true; particles[i].daughter = jets.size(); } else ++nRemain; } jets.push_back( SingleClusterJet(pPre) ); jets.back().multiplicity = multPre; // Decide whether sensible starting configuration or iterate. if (int(jets.size()) + nRemain < nJetMin) break; } if (int(jets.size()) >= nJetMin) break; } } //-------------------------------------------------------------------------- // Reassign particles to nearest jet to correct misclustering. void ClusterJet::reassign() { // Reset clustered momenta. for (int j = 0; j < int(jets.size()); ++j) { jets[j].pTemp = 0.; jets[j].multiplicity = 0; } // Loop through particles to find closest jet. for (int i = 0; i < nParticles; ++i) { particles[i].daughter = -1; double dist2Min = dist2BigMin; int jMin = 0; for (int j = 0; j < int(jets.size()); ++j) { double dist2 = dist2Fun( measure, particles[i], jets[j]); if (dist2 < dist2Min) { dist2Min = dist2; jMin = j; } } jets[jMin].pTemp += particles[i].pJet; ++jets[jMin].multiplicity; particles[i].daughter = jMin; } // Replace old by new jet momenta. for (int j = 0; j < int(jets.size()); ++j) { jets[j].pJet = jets[j].pTemp; jets[j].pAbs = max( PABSMIN, jets[j].pJet.pAbs()); } // Check that no empty clusters after reassignments. for ( ; ; ) { // If no empty jets then done. int jEmpty = -1; for (int j = 0; j < int(jets.size()); ++j) if (jets[j].multiplicity == 0) jEmpty = j; if (jEmpty == -1) return; // Find particle assigned to jet with largest distance to it. int iSplit = -1; double dist2Max = 0.; for (int i = 0; i < nParticles; ++i) { int j = particles[i].daughter; double dist2 = dist2Fun( measure, particles[i], jets[j]); if (dist2 > dist2Max) { iSplit = i; dist2Max = dist2; } } // Let this particle form new jet and subtract off from existing. int jSplit = particles[iSplit].daughter; jets[jEmpty] = SingleClusterJet( particles[iSplit].pJet ); jets[jSplit].pJet -= particles[iSplit].pJet; jets[jSplit].pAbs = max( PABSMIN,jets[jSplit].pJet.pAbs()); particles[iSplit].daughter = jEmpty; --jets[jSplit].multiplicity; } } //-------------------------------------------------------------------------- // Provide a listing of the info. void ClusterJet::list(ostream& os) const { // Header. string method = (measure == 1) ? "Lund pT" : ( (measure == 2) ? "JADE m" : "Durham kT" ) ; os << "\n -------- PYTHIA ClusterJet Listing, " << setw(9) << method << " =" << fixed << setprecision(3) << setw(7) << sqrt(dist2Join) << " GeV --- \n \n no mult p_x p_y p_z " << " e m \n"; // The jets. for (int i = 0; i < int(jets.size()); ++i) { os << setw(4) << i << setw(6) << jets[i].multiplicity << setw(11) << jets[i].pJet.px() << setw(11) << jets[i].pJet.py() << setw(11) << jets[i].pJet.pz() << setw(11) << jets[i].pJet.e() << setw(11) << jets[i].pJet.mCalc() << "\n"; } // Listing finished. os << "\n -------- End PYTHIA ClusterJet Listing ---------------" << "--------" << endl; } //========================================================================== // CellJet class. // This class performs a cone jet search in (eta, phi, E_T) space. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Minimum number of particles to perform study. const int CellJet::TIMESTOPRINT = 1; //-------------------------------------------------------------------------- // Analyze event. bool CellJet::analyze(const Event& event, double eTjetMinIn, double coneRadiusIn, double eTseedIn, ostream& ) { // Input values. Initial values zero. eTjetMin = eTjetMinIn; coneRadius = coneRadiusIn; eTseed = eTseedIn; jets.resize(0); vector cells; // Loop over desired particles in the event. for (int i = 0; i < event.size(); ++i) if (event[i].isFinal()) { if (select > 2 && event[i].isNeutral() ) continue; if (select == 2 && !event[i].isVisible() ) continue; // Find particle position in (eta, phi, pT) space. double etaNow = event[i].eta(); if (abs(etaNow) > etaMax) continue; double phiNow = event[i].phi(); double pTnow = event[i].pT(); int iEtaNow = max(1, min( nEta, 1 + int(nEta * 0.5 * (1. + etaNow / etaMax) ) ) ); int iPhiNow = max(1, min( nPhi, 1 + int(nPhi * 0.5 * (1. + phiNow / M_PI) ) ) ); int iCell = nPhi * iEtaNow + iPhiNow; // Add pT to cell already hit or book a new cell. bool found = false; for (int j = 0; j < int(cells.size()); ++j) { if (iCell == cells[j].iCell) { found = true; ++cells[j].multiplicity; cells[j].eTcell += pTnow; continue; } } if (!found) { double etaCell = (etaMax / nEta) * (2 * iEtaNow - 1 - nEta); double phiCell = (M_PI / nPhi) * (2 * iPhiNow - 1 - nPhi); cells.push_back( SingleCell( iCell, etaCell, phiCell, pTnow, 1) ); } } // Smear true bin content by calorimeter resolution. if (smear > 0 && rndmPtr != 0) for (int j = 0; j < int(cells.size()); ++j) { double eTeConv = (smear < 2) ? 1. : cosh( cells[j].etaCell ); double eBef = cells[j].eTcell * eTeConv; double eAft = 0.; do eAft = eBef + resolution * sqrt(eBef) * rndmPtr->gauss(); while (eAft < 0 || eAft > upperCut * eBef); cells[j].eTcell = eAft / eTeConv; } // Remove cells below threshold for seed or for use at all. for (int j = 0; j < int(cells.size()); ++j) { if (cells[j].eTcell < eTseed) cells[j].canBeSeed = false; if (cells[j].eTcell < threshold) cells[j].isUsed = true; } // Find seed cell: the one with highest pT of not yet probed ones. for ( ; ; ) { int jMax = 0; double eTmax = 0.; for (int j = 0; j < int(cells.size()); ++j) if (cells[j].canBeSeed && cells[j].eTcell > eTmax) { jMax = j; eTmax = cells[j].eTcell; } // If too small cell eT then done, else start new trial jet. if (eTmax < eTseed) break; double etaCenterNow = cells[jMax].etaCell; double phiCenterNow = cells[jMax].phiCell; double eTjetNow = 0.; // Sum up unused cells within required distance of seed. for (int j = 0; j < int(cells.size()); ++j) { if (cells[j].isUsed) continue; double dEta = abs( cells[j].etaCell - etaCenterNow ); if (dEta > coneRadius) continue; double dPhi = abs( cells[j].phiCell - phiCenterNow ); if (dPhi > M_PI) dPhi = 2. * M_PI - dPhi; if (dPhi > coneRadius) continue; if (pow2(dEta) + pow2(dPhi) > pow2(coneRadius)) continue; cells[j].isAssigned = true; eTjetNow += cells[j].eTcell; } // Reject cluster below minimum ET. if (eTjetNow < eTjetMin) { cells[jMax].canBeSeed = false; for (int j = 0; j < int(cells.size()); ++j) cells[j].isAssigned = false; // Else find new jet properties. } else { double etaWeightedNow = 0.; double phiWeightedNow = 0.; int multiplicityNow = 0; Vec4 pMassiveNow; for (int j = 0; j < int(cells.size()); ++j) if (cells[j].isAssigned) { cells[j].canBeSeed = false; cells[j].isUsed = true; cells[j].isAssigned = false; etaWeightedNow += cells[j].eTcell * cells[j].etaCell; double phiCell = cells[j].phiCell; if (abs(phiCell - phiCenterNow) > M_PI) phiCell += (phiCenterNow > 0.) ? 2. * M_PI : -2. * M_PI; phiWeightedNow += cells[j].eTcell * phiCell; multiplicityNow += cells[j].multiplicity; pMassiveNow += cells[j].eTcell * Vec4( cos(cells[j].phiCell), sin(cells[j].phiCell), sinh(cells[j].etaCell), cosh(cells[j].etaCell) ); } etaWeightedNow /= eTjetNow; phiWeightedNow /= eTjetNow; // Bookkeep new jet, in decreasing ET order. jets.push_back( SingleCellJet( eTjetNow, etaCenterNow, phiCenterNow, etaWeightedNow, phiWeightedNow, multiplicityNow, pMassiveNow) ); for (int i = int(jets.size()) - 1; i > 0; --i) { if (jets[i-1].eTjet > jets[i].eTjet) break; swap( jets[i-1], jets[i]); } } } // Done. return true; } //-------------------------------------------------------------------------- // Provide a listing of the info. void CellJet::list(ostream& os) const { // Header. os << "\n -------- PYTHIA CellJet Listing, eTjetMin = " << fixed << setprecision(3) << setw(8) << eTjetMin << ", coneRadius = " << setw(5) << coneRadius << " ------------------------------ \n \n no " << " eTjet etaCtr phiCtr etaWt phiWt mult p_x" << " p_y p_z e m \n"; // The jets. for (int i = 0; i < int(jets.size()); ++i) { os << setw(4) << i << setw(10) << jets[i].eTjet << setw(8) << jets[i].etaCenter << setw(8) << jets[i].phiCenter << setw(8) << jets[i].etaWeighted << setw(8) << jets[i].phiWeighted << setw(5) << jets[i].multiplicity << setw(11) << jets[i].pMassive.px() << setw(11) << jets[i].pMassive.py() << setw(11) << jets[i].pMassive.pz() << setw(11) << jets[i].pMassive.e() << setw(11) << jets[i].pMassive.mCalc() << "\n"; } // Listing finished. os << "\n -------- End PYTHIA CellJet Listing ------------------" << "-------------------------------------------------" << endl; } //========================================================================== // SlowJet class. // This class performs clustering in (y, phi, pT) space. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Minimum number of particles to perform study. const int SlowJet::TIMESTOPRINT = 1; // Assume the pi+- mass for all particles, except the photon, in one option. const double SlowJet::PIMASS = 0.13957; // Small number to avoid division by zero. const double SlowJet::TINY = 1e-20; //-------------------------------------------------------------------------- // Set up list of particles to analyze, and initial distances. bool SlowJet::setup(const Event& event) { // Initial values zero. clusters.resize(0); jets.resize(0); jtSize = 0; // Loop over final particles in the event. Vec4 pTemp; double mTemp, pT2Temp, mTTemp, yTemp, phiTemp; for (int i = 0; i < event.size(); ++i) if (event[i].isFinal()) { // Always apply selection options for visible or charged particles. if (chargedOnly && event[i].isNeutral() ) continue; else if (visibleOnly && !event[i].isVisible() ) continue; // Normally use built-in selection machinery. if (noHook) { // Pseudorapidity cut to describe detector range. if (cutInEta && abs(event[i].eta()) > etaMax) continue; // Optionally modify mass and energy. pTemp = event[i].p(); mTemp = event[i].m(); if (modifyMass) { mTemp = (massSet == 0 || event[i].id() == 22) ? 0. : PIMASS; pTemp.e( sqrt(pTemp.pAbs2() + mTemp*mTemp) ); } // Alternatively pass info to SlowJetHook for decision. // User can also modify pTemp and mTemp. } else { pTemp = event[i].p(); mTemp = event[i].m(); if ( !sjHookPtr->include( i, event, pTemp, mTemp) ) continue; } // Store particle momentum, including some derived quantities. pT2Temp = max( TINY*TINY, pTemp.pT2()); mTTemp = sqrt( mTemp*mTemp + pT2Temp); yTemp = (pTemp.pz() > 0) ? log( max( TINY, pTemp.e() + pTemp.pz() ) / mTTemp ) : log( mTTemp / max( TINY, pTemp.e() - pTemp.pz() ) ); phiTemp = pTemp.phi(); clusters.push_back( SingleSlowJet(pTemp, pT2Temp, yTemp, phiTemp, i) ); } origSize = clusters.size(); // Done here for FJcore machinery. if (useFJcore) return true; // Resize arrays to store distances between clusters. clSize = origSize; clLast = clSize - 1; diB.resize(clSize); dij.resize(clSize * (clSize - 1) / 2); // Loop through particles and find distance to beams. for (int i = 0; i < clSize; ++i) { if (isAnti) diB[i] = 1. / clusters[i].pT2; else if (isKT) diB[i] = clusters[i].pT2; else diB[i] = 1.; // Loop through pairs and find relative distance. for (int j = 0; j < i; ++j) { dPhi = abs( clusters[i].phi - clusters[j].phi ); if (dPhi > M_PI) dPhi = 2. * M_PI - dPhi; dijTemp = (useStandardR) ? (pow2( clusters[i].y - clusters[j].y) + dPhi*dPhi) / R2 : 2. * (cosh( clusters[i].y - clusters[j].y) - cos(dPhi)) / R2 ; if (isAnti) dijTemp /= max(clusters[i].pT2, clusters[j].pT2); else if (isKT) dijTemp *= min(clusters[i].pT2, clusters[j].pT2); dij[i*(i-1)/2 + j] = dijTemp; // End of original-particle loops. } } // Find first particle pair to join. findNext(); // Done. return true; } //-------------------------------------------------------------------------- // Do one recombination step, possibly giving a jet. bool SlowJet::doStep() { // Fail if using FJcore or if no possibility to take a step. if (useFJcore) return false; if (clSize == 0) return false; // When distance to beam is smallest the cluster is promoted to jet. if (jMin == -1) { // Store new jet if its pT is above pTMin. if (clusters[iMin].pT2 > pT2jetMin) { jets.push_back( SingleSlowJet(clusters[iMin]) ); ++jtSize; // Order jets in decreasing pT. for (int i = jtSize - 1; i > 0; --i) { if (jets[i].pT2 < jets[i-1].pT2) break; swap( jets[i], jets[i-1]); } } } // When distance between two clusters is smallest they are joined. else { // Add iMin cluster to jMin. clusters[jMin].p += clusters[iMin].p; clusters[jMin].pT2 = max( TINY*TINY, clusters[jMin].p.pT2()); double mTTemp = sqrt(clusters[jMin].p.m2Calc() + clusters[jMin].pT2); clusters[jMin].y = (clusters[jMin].p.pz() > 0) ? log( max( TINY, clusters[jMin].p.e() + clusters[jMin].p.pz() ) / mTTemp ) : log( mTTemp / max( TINY, clusters[jMin].p.e() - clusters[jMin].p.pz() ) ); clusters[jMin].phi = clusters[jMin].p.phi(); clusters[jMin].mult += clusters[iMin].mult; clusters[jMin].idx.insert(clusters[iMin].idx.begin(), clusters[iMin].idx.end()); // Update distances for and to new jMin. if (isAnti) diB[jMin] = 1. / clusters[jMin].pT2; else if (isKT) diB[jMin] = clusters[jMin].pT2; else diB[jMin] = 1.; for (int i = 0; i < clSize; ++i) if (i != jMin && i != iMin) { dPhi = abs( clusters[i].phi - clusters[jMin].phi ); if (dPhi > M_PI) dPhi = 2. * M_PI - dPhi; dijTemp = (useStandardR) ? (pow2( clusters[i].y - clusters[jMin].y) + dPhi*dPhi) / R2 : 2. * (cosh( clusters[i].y - clusters[jMin].y) - cos(dPhi)) / R2 ; if (isAnti) dijTemp /= max(clusters[i].pT2, clusters[jMin].pT2); else if (isKT) dijTemp *= min(clusters[i].pT2, clusters[jMin].pT2); if (i < jMin) dij[jMin*(jMin-1)/2 + i] = dijTemp; else dij[i*(i-1)/2 + jMin] = dijTemp; } } // Move up last cluster and distances to vacated position iMin. if (iMin < clLast) { clusters[iMin] = clusters[clLast]; diB[iMin] = diB[clLast]; for (int j = 0; j < iMin; ++j) dij[iMin*(iMin-1)/2 + j] = dij[clLast*(clLast-1)/2 + j]; for (int j = iMin + 1; j < clLast; ++j) dij[j*(j-1)/2 + iMin] = dij[clLast*(clLast-1)/2 + j]; } // Shrink cluster list by one. clusters.pop_back(); --clSize; --clLast; // Find next cluster pair to join. findNext(); // Done. return true; } //-------------------------------------------------------------------------- // Provide a listing of the info. void SlowJet::list(bool listAll, ostream& os) const { // Header. if (useFJcore) os << "\n -- PYTHIA SlowJet(fjcore) Listing, p = "; else os << "\n -- PYTHIA SlowJet(native) Listing, p = "; os << setw(2) << power << ", R = " << fixed << setprecision(3) << setw(5) << R << ", pTjetMin =" << setw(8) << pTjetMin << ", etaMax = " << setw(6) << etaMax << " -- \n \n no pTjet y phi" << " mult p_x p_y p_z e m \n"; // The jets. for (int i = 0; i < jtSize; ++i) { os << setw(5) << i << setw(11) << sqrt(jets[i].pT2) << setw(9) << jets[i].y << setw(9) << jets[i].phi << setw(6) << jets[i].mult << setw(11) << jets[i].p.px() << setw(11) << jets[i].p.py() << setw(11) << jets[i].p.pz() << setw(11) << jets[i].p.e() << setw(11) << jets[i].p.mCalc() << "\n"; } // Optionally list also clusters not yet jets. if (listAll && clSize > 0) { os << " -------- Below this line follows remaining clusters," << " still pT-unordered -------------------\n"; for (int i = 0; i < clSize; ++i) { os << setw(5) << i + jtSize << setw(11) << sqrt(clusters[i].pT2) << setw(9) << clusters[i].y << setw(9) << clusters[i].phi << setw(6) << clusters[i].mult << setw(11) << clusters[i].p.px() << setw(11) << clusters[i].p.py() << setw(11) << clusters[i].p.pz() << setw(11) << clusters[i].p.e() << setw(11) << clusters[i].p.mCalc() << "\n"; } } // Listing finished. os << "\n -------- End PYTHIA SlowJet Listing ------------------" << "--------------------------------------" << endl; } //-------------------------------------------------------------------------- // Find next cluster pair to join. void SlowJet::findNext() { // Find smallest of diB, dij. if (clSize > 0) { iMin = 0; jMin = -1; dMin = diB[0]; for (int i = 1; i < clSize; ++i) { if (diB[i] < dMin) { iMin = i; jMin = -1; dMin = diB[i]; } for (int j = 0; j < i; ++j) { if (dij[i*(i-1)/2 + j] < dMin) { iMin = i; jMin = j; dMin = dij[i*(i-1)/2 + j]; } } } // If no clusters left then instead default values. } else { iMin = -1; jMin = -1; dMin = 0.; } } //-------------------------------------------------------------------------- // Use FJcore interface to perform clustering. bool SlowJet::clusterFJ() { // Read in input configuration of particles. vector inFJ; for (int i = 0; i < int(clusters.size()); ++i) { inFJ.push_back( fjcore::PseudoJet( clusters[i].p.px(), clusters[i].p.py(), clusters[i].p.pz(), clusters[i].p.e() ) ); set::iterator idxTmp = clusters[i].idx.begin(); inFJ[i].set_user_index( *idxTmp); } // Create a jet definition = jet algorithm + radius parameter. fjcore::JetAlgorithm jetAlg = fjcore::cambridge_algorithm; if (isAnti) jetAlg = fjcore::antikt_algorithm; if (isKT) jetAlg = fjcore::kt_algorithm; fjcore::JetDefinition jetDef( jetAlg, R); // Run the jet clustering with the above jet definition. fjcore::ClusterSequence clust_seq( inFJ, jetDef); // Get the resulting jets above pTmin, ordered in pT. vector outFJ = sorted_by_pt( clust_seq.inclusive_jets( pTjetMin) ); // Store the FJcore output in the standard SlowJet format. Vec4 pTemp; double pT2Temp, yTemp, phiTemp; for (int i = 0; i < int(outFJ.size()); ++i) { pTemp = Vec4( outFJ[i].px(), outFJ[i].py(), outFJ[i].pz(), outFJ[i].e() ); pT2Temp = outFJ[i].pt2(); yTemp = outFJ[i].rap(); phiTemp = outFJ[i].phi_std(); jets.push_back( SingleSlowJet(pTemp, pT2Temp, yTemp, phiTemp, 0) ); // Also find constituents of jet. jets[i].idx.clear(); vector constFJ = outFJ[i].constituents(); for (int j = 0; j < int(constFJ.size()); ++j) jets[i].idx.insert( constFJ[j].user_index() ); jets[i].mult = constFJ.size(); } // Set counters and some dummy (for FJcore) information. clSize = 0; clLast = 0; jtSize = outFJ.size(); iMin = -1; jMin = -1; dMin = 0.; // Done. return true; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaSUSY.cc0000644000175000017500000026634012217346251015231 0ustar sunsun// SigmaSUSY.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // Main authors of this file: N. Desai, P. Skands // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // supersymmetry simulation classes. #include "Pythia8/SigmaSUSY.h" namespace Pythia8 { //========================================================================== // Sigma2SUSY // An intermediate class for SUSY 2 -> 2 processes with nontrivial decay angles. //-------------------------------------------------------------------------- double Sigma2SUSY::weightDecay( Event& process, int iResBeg, int iResEnd) { // Do nothing if decays present already at input. // Identity of mother of decaying resonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For Higgs decay hand over to standard routine. if (idMother == 25 || idMother == 35 || idMother == 36) return weightHiggsDecay( process, iResBeg, iResEnd); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // For Neutralino(i) decay hand over to standard routine. if ( settingsPtr->flag("SUSYResonance:3BodyMatrixElement") && (idMother == 1000023 || idMother == 1000025 || idMother == 1000035) ) { // Nj -> Ni f fbar if (iResEnd - iResBeg != 2) return(1.0); int iW1 = iResBeg; int iF = iResBeg + 1; int iFbar= iResBeg + 2; int iT = process[iW1].mother1(); if( iT <= 0 ) return(1.0); int idDau= process[iW1].idAbs(); // Neutralino decays to charginos not yet implemented if (idDau == 1000024 || idDau == 1000037 ) return(1.0); if (idDau != 1000022 && idDau != 1000023 && idDau != 1000025 && idDau != 1000035 ) { return(1.0); } else { if( process[iF].idAbs() != process[iFbar].idAbs() ) return(1.0); int idmo = -1; int iddau = -1; switch (idMother) { case 1000023: idmo = 2; break; case 1000025: idmo = 3; break; case 1000035: idmo = 4; break; } switch (idDau) { case 1000022: iddau = 1; break; case 1000023: iddau = 2; break; case 1000025: iddau = 3; break; } if( idmo<0 || iddau<0 ) return(1.0); Sigma2qqbar2chi0chi0 localDecay(idmo,iddau,0); localDecay.init(infoPtr, settingsPtr, particleDataPtr,NULL,NULL, NULL,couplingsPtr); localDecay.initProc(); localDecay.alpEM = 1; localDecay.id1 = process[iF].id(); localDecay.id2 = process[iFbar].id(); double xm3 = process[iT].m(); double xm4 = process[iW1].m(); localDecay.m3 = xm3; localDecay.m4 = xm4; localDecay.s3 = xm3*xm3; localDecay.s4 = xm4*xm4; localDecay.sH = (process[iF].p()+process[iFbar].p()).m2Calc(); localDecay.sH2 = pow2(localDecay.sH); localDecay.tH = (process[iF].p()-process[iT].p()).m2Calc(); localDecay.uH = localDecay.s3+localDecay.s4-localDecay.tH-localDecay.sH; localDecay.sigmaKin(); double wt = -localDecay.sigmaHat(); // Estimate maximum weight by sampling kinematic extremes // Case I: neutralino(i) at rest localDecay.sH = pow2(xm4-xm3); localDecay.tH = 0.5*(localDecay.s3+localDecay.s4-localDecay.sH); localDecay.uH = localDecay.tH; localDecay.sigmaKin(); double wtmax = -localDecay.sigmaHat(); // Case II: fermion at rest localDecay.sH = 0; localDecay.tH = localDecay.s3; localDecay.uH = localDecay.s3+localDecay.s4-localDecay.tH-localDecay.sH; localDecay.sigmaKin(); wtmax += -localDecay.sigmaHat(); // Case III: antifermion at rest localDecay.uH = localDecay.s3; localDecay.tH = localDecay.s3+localDecay.s4-localDecay.tH-localDecay.sH; localDecay.sigmaKin(); wtmax += -localDecay.sigmaHat(); return(wt/wtmax); } } // Else done. return 1.; } //========================================================================== // Sigma2qqbar2chi0chi0 // Cross section for gaugino pair production: neutralino pair //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2chi0chi0::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Construct name of process. nameSave = "q qbar' -> " + particleDataPtr->name(id3) + " " + particleDataPtr->name(id4); // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(id3, id4); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2chi0chi0::sigmaKin() { // Common flavour-independent factor. sigma0 = M_PI /3.0/ sH2 / pow2(coupSUSYPtr->sin2W) * pow2(alpEM) * openFracPair; // Auxiliary factors for use below ui = uH - s3; uj = uH - s4; ti = tH - s3; tj = tH - s4; double sV= sH - pow2(coupSUSYPtr->mZpole); double d = pow2(sV) + pow2(coupSUSYPtr->mZpole * coupSUSYPtr->wZpole); propZ = complex( sV / d, coupSUSYPtr->mZpole * coupSUSYPtr->wZpole / d); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2chi0chi0::sigmaHat() { // Only allow quark-antiquark incoming states if (id1*id2 >= 0) { return 0.0; } // Only allow incoming states with sum(charge) = 0 if ((id1+id2) % 2 != 0) { return 0.0; } if(id1<0) swapTU = true; // Shorthands int idAbs1 = abs(id1); int idAbs2 = abs(id2); // Flavour-dependent kinematics-dependent couplings. complex QuLL(0.0),QtLL(0.0),QuRR(0.0),QtRR(0.0); complex QuLR(0.0),QtLR(0.0),QuRL(0.0),QtRL(0.0); double *LqqZloc; double *RqqZloc; int iAdd=0; if( idAbs1 > 10 && idAbs1 < 17 ) { LqqZloc = coupSUSYPtr->LllZ; RqqZloc = coupSUSYPtr->RllZ; iAdd+=10; } else { LqqZloc = coupSUSYPtr->LqqZ; RqqZloc = coupSUSYPtr->RqqZ; } // s-channel Z couplings if (idAbs1 == idAbs2) { QuLL = LqqZloc[idAbs1-iAdd] * coupSUSYPtr->OLpp[id3chi][id4chi] * propZ / 2.0; QtLL = LqqZloc[idAbs1-iAdd] * coupSUSYPtr->ORpp[id3chi][id4chi] * propZ / 2.0; QuRR = RqqZloc[idAbs1-iAdd] * coupSUSYPtr->ORpp[id3chi][id4chi] * propZ / 2.0; QtRR = RqqZloc[idAbs1-iAdd] * coupSUSYPtr->OLpp[id3chi][id4chi] * propZ / 2.0; } // Flavour indices int ifl1 = (idAbs1+1-iAdd) / 2; int ifl2 = (idAbs2+1-iAdd) / 2; complex (*LsddXloc)[4][6]; complex (*RsddXloc)[4][6]; complex (*LsuuXloc)[4][6]; complex (*RsuuXloc)[4][6]; if( idAbs1 > 10 && idAbs1 < 17 ) { LsddXloc = coupSUSYPtr->LsllX; RsddXloc = coupSUSYPtr->RsllX; LsuuXloc = coupSUSYPtr->LsvvX; RsuuXloc = coupSUSYPtr->RsvvX; } else { LsddXloc = coupSUSYPtr->LsddX; RsddXloc = coupSUSYPtr->RsddX; LsuuXloc = coupSUSYPtr->LsuuX; RsuuXloc = coupSUSYPtr->RsuuX; } // Add t-channel squark flavour sums to QmXY couplings for (int ksq=1; ksq<=6; ksq++) { // squark id and squark-subtracted u and t int idsq; idsq=((ksq+2)/3)*1000000 + 2*((ksq-1) % 3) + (idAbs1+1) % 2 + 1; idsq+=iAdd; double msq2 = pow(particleDataPtr->m0(idsq),2); double usq = uH - msq2; double tsq = tH - msq2; complex Lsqq1X3; complex Lsqq1X4; complex Lsqq2X3; complex Lsqq2X4; complex Rsqq1X3; complex Rsqq1X4; complex Rsqq2X3; complex Rsqq2X4; // Couplings Lsqq1X3 = LsuuXloc[ksq][ifl1][id3chi]; Lsqq1X4 = LsuuXloc[ksq][ifl1][id4chi]; Lsqq2X3 = LsuuXloc[ksq][ifl2][id3chi]; Lsqq2X4 = LsuuXloc[ksq][ifl2][id4chi]; Rsqq1X3 = RsuuXloc[ksq][ifl1][id3chi]; Rsqq1X4 = RsuuXloc[ksq][ifl1][id4chi]; Rsqq2X3 = RsuuXloc[ksq][ifl2][id3chi]; Rsqq2X4 = RsuuXloc[ksq][ifl2][id4chi]; if (idAbs1 % 2 != 0) { Lsqq1X3 = LsddXloc[ksq][ifl1][id3chi]; Lsqq1X4 = LsddXloc[ksq][ifl1][id4chi]; Lsqq2X3 = LsddXloc[ksq][ifl2][id3chi]; Lsqq2X4 = LsddXloc[ksq][ifl2][id4chi]; Rsqq1X3 = RsddXloc[ksq][ifl1][id3chi]; Rsqq1X4 = RsddXloc[ksq][ifl1][id4chi]; Rsqq2X3 = RsddXloc[ksq][ifl2][id3chi]; Rsqq2X4 = RsddXloc[ksq][ifl2][id4chi]; } // QuXY QuLL += conj(Lsqq1X4)*Lsqq2X3/usq; QuRR += conj(Rsqq1X4)*Rsqq2X3/usq; QuLR += conj(Lsqq1X4)*Rsqq2X3/usq; QuRL += conj(Rsqq1X4)*Lsqq2X3/usq; // QtXY QtLL -= conj(Lsqq1X3)*Lsqq2X4/tsq; QtRR -= conj(Rsqq1X3)*Rsqq2X4/tsq; QtLR += conj(Lsqq1X3)*Rsqq2X4/tsq; QtRL += conj(Rsqq1X3)*Lsqq2X4/tsq; } // Overall factor multiplying each coupling; multiplied at the end as fac^2 double fac = (1.0-coupSUSYPtr->sin2W); if(abs(id3)==abs(id4)) fac *= sqrt(2.); // for identical final particles // Compute matrix element weight double weight = 0; double facLR = uH*tH - s3*s4; double facMS = m3*m4*sH; // Average over separate helicity contributions // LL (ha = -1, hb = +1) (divided by 4 for average) weight += norm(QuLL) * ui * uj + norm(QtLL) * ti * tj + 2 * real(conj(QuLL) * QtLL) * facMS; // RR (ha = 1, hb = -1) (divided by 4 for average) weight += norm(QtRR) * ti * tj + norm(QuRR) * ui * uj + 2 * real(conj(QuRR) * QtRR) * facMS; // RL (ha = 1, hb = 1) (divided by 4 for average) weight += norm(QuRL) * ui * uj + norm(QtRL) * ti * tj + real(conj(QuRL) * QtRL) * facLR; // LR (ha = -1, hb = -1) (divided by 4 for average) weight += norm(QuLR) * ui * uj + norm(QtLR) * ti * tj + real(conj(QuLR) * QtLR) * facLR; double colorFactor = ( idAbs1 > 10 && idAbs1 < 17 ) ? 3.0 : 1.0; // Cross section, including colour factor. double sigma = sigma0 * weight / pow2(fac) * colorFactor; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2chi0chi0::setIdColAcol() { // Set flavours. setId( id1, id2, id3, id4); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2charchi0 // Cross section for gaugino pair production: neutralino-chargino //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2charchi0::sigmaKin() { // Common flavour-independent factor. sigma0 = M_PI / sH2 / 3.0 / pow2(coupSUSYPtr->sin2W) * pow2(alpEM) ; sigma0 /= 2.0 * (1 - coupSUSYPtr->sin2W) ; // Auxiliary factors for use below ui = uH - s3; uj = uH - s4; ti = tH - s3; tj = tH - s4; double sW = sH - pow2(coupSUSYPtr->mWpole); double d = pow2(sW) + pow2(coupSUSYPtr->mWpole * coupSUSYPtr->wWpole); propW = complex( sW / d, coupSUSYPtr->mWpole * coupSUSYPtr->wWpole / d); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2charchi0::sigmaHat() { // Only allow particle-antiparticle incoming states if (id1*id2 >= 0) { return 0.0; } // Only allow incoming states with sum(charge) = final state if (abs(id1) % 2 == abs(id2) % 2) return 0.0; int isPos = (id3chi > 0 ? 1 : 0); if (id1 < 0 && id1 > -19 && abs(id1) % 2 == 1-isPos ) return 0.0; else if (id1 > 0 && id1 < 19 && abs(id1) % 2 == isPos ) return 0.0; // Flavour-dependent kinematics-dependent couplings. int idAbs1 = abs(id1); int iChar = abs(id3chi); int iNeut = abs(id4chi); complex QuLL(0.0),QtLL(0.0),QuRR(0.0),QtRR(0.0); complex QuLR(0.0),QtLR(0.0),QuRL(0.0),QtRL(0.0); // Calculate everything from udbar -> ~chi+ ~chi0 template process int iAdd=0; complex (*LudWloc)[4]; complex (*LsddXloc)[4][6]; complex (*RsddXloc)[4][6]; complex (*LsuuXloc)[4][6]; complex (*RsuuXloc)[4][6]; complex (*LsduXloc)[4][3]; complex (*RsduXloc)[4][3]; complex (*LsudXloc)[4][3]; complex (*RsudXloc)[4][3]; if( idAbs1 > 10 && idAbs1 < 17 ) { iAdd+=10; LudWloc = coupSUSYPtr->LlvW; LsddXloc = coupSUSYPtr->LsllX; RsddXloc = coupSUSYPtr->RsllX; LsuuXloc = coupSUSYPtr->LsvvX; RsuuXloc = coupSUSYPtr->RsvvX; LsduXloc = coupSUSYPtr->LslvX; RsduXloc = coupSUSYPtr->RslvX; LsudXloc = coupSUSYPtr->LsvlX; RsudXloc = coupSUSYPtr->RsvlX; } else { LudWloc = coupSUSYPtr->LudW; LsddXloc = coupSUSYPtr->LsddX; RsddXloc = coupSUSYPtr->RsddX; LsuuXloc = coupSUSYPtr->LsuuX; RsuuXloc = coupSUSYPtr->RsuuX; LsduXloc = coupSUSYPtr->LsduX; RsduXloc = coupSUSYPtr->RsduX; LsudXloc = coupSUSYPtr->LsudX; RsudXloc = coupSUSYPtr->RsudX; } // u dbar , ubar d : do nothing // dbar u , d ubar : swap 1<->2 and t<->u int iGu = (abs(id1)-iAdd)/2; int iGd = (abs(id2)+1-iAdd)/2; if (idAbs1 % 2 != 0) { swapTU = true; iGu = (abs(id2)-iAdd)/2; iGd = (abs(id1)+1-iAdd)/2; } // s-channel W contribution QuLL = conj(LudWloc[iGu][iGd]) * conj(coupSUSYPtr->OL[iNeut][iChar]) * propW / sqrt(2.0); QtLL = conj(LudWloc[iGu][iGd]) * conj(coupSUSYPtr->OR[iNeut][iChar]) * propW / sqrt(2.0); // Add t-channel squark flavour sums to QmXY couplings for (int jsq=1; jsq<=6; jsq++) { int idsu=((jsq+2)/3)*1000000 + 2*((jsq-1) % 3) + 2 +iAdd; int idsd=((jsq+2)/3)*1000000 + 2*((jsq-1) % 3) + 1 +iAdd; double msd2 = pow(particleDataPtr->m0(idsd),2); double msu2 = pow(particleDataPtr->m0(idsu),2); double tsq = tH - msd2; double usq = uH - msu2; QuLL += conj(LsuuXloc[jsq][iGu][iNeut]) * conj(LsudXloc[jsq][iGd][iChar])/usq; QuLR += conj(LsuuXloc[jsq][iGu][iNeut]) * conj(RsudXloc[jsq][iGd][iChar])/usq; QuRR += conj(RsuuXloc[jsq][iGu][iNeut]) * conj(RsudXloc[jsq][iGd][iChar])/usq; QuRL += conj(RsuuXloc[jsq][iGu][iNeut]) * conj(LsudXloc[jsq][iGd][iChar])/usq; QtLL -= conj(LsduXloc[jsq][iGu][iChar]) * LsddXloc[jsq][iGd][iNeut]/tsq; QtRR -= conj(RsduXloc[jsq][iGu][iChar]) * RsddXloc[jsq][iGd][iNeut]/tsq; QtLR += conj(LsduXloc[jsq][iGu][iChar]) * RsddXloc[jsq][iGd][iNeut]/tsq; QtRL += conj(RsduXloc[jsq][iGu][iChar]) * LsddXloc[jsq][iGd][iNeut]/tsq; } // Compute matrix element weight double weight = 0; // Average over separate helicity contributions // (if swapped, swap ha, hb if computing polarized cross sections) // LL (ha = -1, hb = +1) (divided by 4 for average) weight += norm(QuLL) * ui * uj + norm(QtLL) * ti * tj + 2 * real(conj(QuLL) * QtLL) * m3 * m4 * sH; // RR (ha = 1, hb = -1) (divided by 4 for average) weight += norm(QtRR) * ti * tj + norm(QuRR) * ui * uj + 2 * real(conj(QuRR) * QtRR) * m3 * m4 * sH; // RL (ha = 1, hb = 1) (divided by 4 for average) weight += norm(QuRL) * ui * uj + norm(QtRL) * ti * tj + real(conj(QuRL) * QtRL) * (uH * tH - s3 * s4); // LR (ha = -1, hb = -1) (divided by 4 for average) weight += norm(QuLR) * ui * uj + norm(QtLR) * ti * tj + real(conj(QuLR) * QtLR) * (uH * tH - s3 * s4); double colorFactor = ( idAbs1 > 10 && idAbs1 < 17 ) ? 3.0 : 1.0; // Cross section, including colour factor. double sigma = sigma0 * weight * colorFactor; // Answer. return sigma; } //========================================================================== // Sigma2qqbar2charchar // Cross section for gaugino pair production: chargino-chargino //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2charchar::sigmaKin() { // Common flavour-independent factor. sigma0 = M_PI / 3.0 / sH2 / pow2(coupSUSYPtr->sin2W) * pow2(alpEM) ; // Auxiliary factors for use below ui = uH - s3; uj = uH - s4; ti = tH - s3; tj = tH - s4; double sV= sH - pow2(coupSUSYPtr->mZpole); double d = pow2(sV) + pow2(coupSUSYPtr->mZpole * coupSUSYPtr->wZpole); propZ = complex( sV / d, coupSUSYPtr->mZpole * coupSUSYPtr->wZpole / d); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2charchar::sigmaHat() { // Only allow quark-antiquark incoming states if (id1*id2 >= 0) return 0.0; // Only allow incoming states with sum(charge) = 0 if ((id1+id2) % 2 != 0) return 0.0; //if (id1 > 0 || id1==-1 || id1==-3 || id1==-5) return 0.0; //if (id1 < 0 || id1==1 || id1==3 || id1==5) return 0.0; swapTU = (id1 < 0 ? true : false); // Flavour-dependent kinematics-dependent couplings. int idAbs1 = abs(id1); int idAbs2 = abs(id2); int i3 = abs(id3chi); int i4 = abs(id4chi); // Flavour-dependent kinematics-dependent couplings. complex QuLL(0.0),QtLL(0.0),QuRR(0.0),QtRR(0.0); complex QuLR(0.0),QtLR(0.0),QuRL(0.0),QtRL(0.0); double *LqqZloc; double *RqqZloc; complex (*LsduXloc)[4][3]; complex (*RsduXloc)[4][3]; complex (*LsudXloc)[4][3]; complex (*RsudXloc)[4][3]; int iShift(0); if( idAbs1 > 10 && idAbs1 < 17 ) { iShift+=10; LqqZloc = coupSUSYPtr->LllZ; RqqZloc = coupSUSYPtr->RllZ; LsduXloc = coupSUSYPtr->LslvX; RsduXloc = coupSUSYPtr->RslvX; LsudXloc = coupSUSYPtr->LsvlX; RsudXloc = coupSUSYPtr->RsvlX; } else { LqqZloc = coupSUSYPtr->LqqZ; RqqZloc = coupSUSYPtr->RqqZ; LsduXloc = coupSUSYPtr->LsduX; RsduXloc = coupSUSYPtr->RsduX; LsudXloc = coupSUSYPtr->LsudX; RsudXloc = coupSUSYPtr->RsudX; } // Add Z/gamma* for same-flavour in-quarks if (idAbs1 == idAbs2) { QuLL = -LqqZloc[idAbs1-iShift]*conj(coupSUSYPtr->ORp[i3][i4]); QtLL = -LqqZloc[idAbs1-iShift]*conj(coupSUSYPtr->OLp[i3][i4]); QuRR = -RqqZloc[idAbs1-iShift]*conj(coupSUSYPtr->OLp[i3][i4]); QtRR = -RqqZloc[idAbs1-iShift]*conj(coupSUSYPtr->ORp[i3][i4]); QuLL *= propZ / 2.0 / (1.0-coupSUSYPtr->sin2W); QtLL *= propZ / 2.0 / (1.0-coupSUSYPtr->sin2W); QuRR *= propZ / 2.0 / (1.0-coupSUSYPtr->sin2W); QtRR *= propZ / 2.0 / (1.0-coupSUSYPtr->sin2W); // s-channel gamma* (only for same-type charginos) if (i3 == i4) { // Charge of in-particles double q = particleDataPtr->chargeType(idAbs1)/3.0; QuLL += q * coupSUSYPtr->sin2W / sH; QuRR += q * coupSUSYPtr->sin2W / sH; QtLL += q * coupSUSYPtr->sin2W / sH; QtRR += q * coupSUSYPtr->sin2W / sH; } } int iG1 = (abs(id1)+1-iShift)/2; int iG2 = (abs(id2)+1-iShift)/2; // Add t- or u-channel squark flavour sums to QmXY couplings for (int ksq=1; ksq<=6; ksq++) { if(id1 % 2 == 0) { // u-channel diagrams only // up-type incoming; u-channel ~d int idsd = ((ksq+2)/3)*1000000 + 2*((ksq-1) % 3) + 1; idsd +=iShift; double msq = particleDataPtr->m0(idsd); double ufac = 2.0 * (uH - pow2(msq)); //u-ubar -> chi-chi+ QuLL += LsduXloc[ksq][iG2][i3] * conj(LsduXloc[ksq][iG1][i4]) / ufac; QuRR += RsduXloc[ksq][iG2][i3] * conj(RsduXloc[ksq][iG1][i4]) / ufac; QuLR += RsduXloc[ksq][iG2][i3] * conj(LsduXloc[ksq][iG1][i4]) / ufac; QuRL += LsduXloc[ksq][iG2][i3] * conj(RsduXloc[ksq][iG1][i4]) / ufac; }else{ // t-channel diagrams only; // down-type incoming; t-channel ~u int idsu = ((ksq+2)/3)*1000000 + 2*((ksq-1) % 3) + 2; idsu += iShift; double msq = particleDataPtr->m0(idsu); double tfac = 2.0 * (tH - pow2(msq)); //d-dbar -> chi-chi+ QtLL -= LsudXloc[ksq][iG1][i3] * conj(LsudXloc[ksq][iG2][i4]) / tfac; QtRR -= RsudXloc[ksq][iG1][i3] * conj(RsudXloc[ksq][iG2][i4]) / tfac; QtLR += LsudXloc[ksq][iG1][i3] * conj(RsudXloc[ksq][iG2][i4]) / tfac; QtRL += RsudXloc[ksq][iG1][i3] * conj(LsudXloc[ksq][iG2][i4]) / tfac; } } // Compute matrix element weight double weight = 0; // Average over separate helicity contributions // LL (ha = -1, hb = +1) (divided by 4 for average) weight += norm(QuLL) * ui * uj + norm(QtLL) * ti * tj + 2 * real(conj(QuLL) * QtLL) * m3 * m4 * sH; // RR (ha = 1, hb = -1) (divided by 4 for average) weight += norm(QtRR) * ti * tj + norm(QuRR) * ui * uj + 2 * real(conj(QuRR) * QtRR) * m3 * m4 * sH; // RL (ha = 1, hb = 1) (divided by 4 for average) weight += norm(QuRL) * ui * uj + norm(QtRL) * ti * tj + real(conj(QuRL) * QtRL) * (uH * tH - s3 * s4); // LR (ha = -1, hb = -1) (divided by 4 for average) weight += norm(QuLR) * ui * uj + norm(QtLR) * ti * tj + real(conj(QuLR) * QtLR) * (uH * tH - s3 * s4); double colorFactor = ( idAbs1 > 10 && idAbs1 < 17 ) ? 3.0 : 1.0; // Cross section, including colour factor. double sigma = sigma0 * weight * colorFactor; // Answer. return sigma; } //========================================================================== // Sigma2qgchi0squark // Cross section for gaugino-squark production: neutralino-squark //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2chi0squark::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Construct name of process. if (id4 % 2 == 0) { nameSave = "q g -> " + particleDataPtr->name(id3) + " " + particleDataPtr->name(id4) + " + c.c. (q=u,c)"; } else { nameSave = "q g -> " + particleDataPtr->name(id3) + " " + particleDataPtr->name(id4) + " + c.c. (q=d,s,b)"; } // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(id3, id4); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qg2chi0squark::sigmaKin() { // Common flavour-independent factor. // tmp: alphaS = 0.1 for counter-checks sigma0 = M_PI / sH2 / coupSUSYPtr->sin2W * alpEM * alpS * openFracPair; // Auxiliary factors for use below ui = uH - s3; uj = uH - s4; ti = tH - s3; tj = tH - s4; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qg2chi0squark::sigmaHat() { // Antiquark -> antisquark int idq = id1; if (id1 == 21 || id1 == 22) idq = id2; if (idq < 0) { id4 = -abs(id4); } else { id4 = abs(id4); } // tmp: only allow incoming quarks on side 1 // if (id1 < 0 || id1 == 21) return 0.0; // Generation index int iGq = (abs(idq)+1)/2; // Only accept u(bar) -> ~u(bar) and d(bar) -> ~d(bar) if (particleDataPtr->chargeType(idq) != particleDataPtr->chargeType(id4)) return 0.0; // Couplings complex LsqqX, RsqqX; if (idq % 2 == 0) { LsqqX = coupSUSYPtr->LsuuX[id4sq][iGq][id3chi]; RsqqX = coupSUSYPtr->RsuuX[id4sq][iGq][id3chi]; } else { LsqqX = coupSUSYPtr->LsddX[id4sq][iGq][id3chi]; RsqqX = coupSUSYPtr->RsddX[id4sq][iGq][id3chi]; } // Prefactors : swap u and t if gq instead of qg double fac1, fac2; if (idq == id1) { fac1 = -ui/sH + 2.0 * ( uH*tH - s4*s3 )/sH/tj; fac2 = ti/tj * ( (tH + s4)/tj + (ti - uj)/sH ); } else { fac1 = -ti/sH + 2.0 * ( uH*tH - s4*s3 )/sH/uj; fac2 = ui/uj * ( (uH + s4)/uj + (ui - tj)/sH ); } // Compute matrix element weight double weight = 0.0; // Average over separate helicity contributions // (for qbar g : ha -> -ha ) // LL (ha = -1, hb = +1) (divided by 4 for average) weight += fac2 * norm(LsqqX) / 2.0; // RR (ha = 1, hb = -1) (divided by 4 for average) weight += fac2 * norm(RsqqX) / 2.0; // RL (ha = 1, hb = 1) (divided by 4 for average) weight += fac2 * norm(RsqqX) / 2.0 + fac1 * norm(RsqqX); // LR (ha = -1, hb = -1) (divided by 4 for average) weight += fac2 * norm(LsqqX) / 2.0 + fac1 * norm(LsqqX); double sigma = sigma0 * weight; if (abs(idq) < 9) sigma /= 3.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2chi0squark::setIdColAcol() { // Set flavours. setId( id1, id2, id3, (id1*id2 > 0 ? abs(id4) : -abs(id4))); // Colour flow topology. Swap if first is gluon, or when antiquark. if (id1 != 21) setColAcol( 1, 0, 2, 1, 0, 0, 2, 0); else setColAcol( 1, 2, 2, 0, 0, 0, 1, 0); if (id1*id2 < 0) swapColAcol(); } //========================================================================== // Sigma2qg2charsquark // Cross section for gaugino-squark production: chargino-squark //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2charsquark::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Construct name of process. if (id4 % 2 == 0) { nameSave = "q g -> " + particleDataPtr->name(id3) + " " + particleDataPtr->name(id4) + " + c.c. (q=d,s,b)"; } else { nameSave = "q g -> " + particleDataPtr->name(id3) + " " + particleDataPtr->name(id4) + " + c.c. (q=u,c)"; } // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(id3Sav, id4Sav); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qg2charsquark::sigmaHat() { // Antiquark -> antisquark int idq = (id1 == 21) ? id2 : id1; if (idq > 0) { id3 = id3Sav; id4 = id4Sav; } else { id3 = -id3Sav; id4 = -id4Sav; } // Only accept u(bar) -> ~d(bar) and d(bar) -> ~u(bar) if (particleDataPtr->chargeType(idq) == particleDataPtr->chargeType(id4)) return 0.0; // Generation index int iGq = (abs(idq)+1)/2; // Couplings complex LsqqX, RsqqX; if (idq % 2 == 0) { LsqqX = coupSUSYPtr->LsduX[id4sq][iGq][id3chi]; RsqqX = coupSUSYPtr->RsduX[id4sq][iGq][id3chi]; } else { LsqqX = coupSUSYPtr->LsduX[id4sq][iGq][id3chi]; RsqqX = coupSUSYPtr->RsduX[id4sq][iGq][id3chi]; } // Prefactors : swap u and t if gq instead of qg double fac1, fac2; if (idq == id1) { fac1 = -ui/sH + 2.0 * ( uH*tH - s4*s3 )/sH/tj; fac2 = ti/tj * ( (tH + s4)/tj + (ti - uj)/sH ); } else { fac1 = -ti/sH + 2.0 * ( uH*tH - s4*s3 )/sH/uj; fac2 = ui/uj * ( (uH + s4)/uj + (ui - tj)/sH ); } // Compute matrix element weight double weight = 0.0; // Average over separate helicity contributions // (a, b refers to qg configuration) // LL (ha = -1, hb = +1) (divided by 4 for average) weight += fac2 * norm(LsqqX) / 2.0; // RR (ha = 1, hb = -1) (divided by 4 for average) weight += fac2 * norm(RsqqX) / 2.0; // RL (ha = 1, hb = 1) (divided by 4 for average) weight += fac2 * norm(RsqqX) / 2.0 + fac1 * norm(RsqqX); // LR (ha = -1, hb = -1) (divided by 4 for average) weight += fac2 * norm(LsqqX) / 2.0 + fac1 * norm(LsqqX); double sigma = sigma0 * weight; if (abs(idq) < 9) sigma /= 3.; // Answer. return sigma * openFracPair; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2charsquark::setIdColAcol() { // Set flavours. if (id1 > 0 && id2 > 0) { setId( id1, id2, id3Sav, id4Sav); } else { setId( id1, id2,-id3Sav,-id4Sav); } // Colour flow topology. Swap if first is gluon, or when antiquark. if (id1 != 21) setColAcol( 1, 0, 2, 1, 0, 0, 2, 0); else setColAcol( 1, 2, 2, 0, 0, 0, 1, 0); if (id1 < 0 || id2 < 0) swapColAcol(); } //========================================================================== // Sigma2qq2squarksquark // Cross section for squark-squark production //-------------------------------------------------------------------------- // Initialize process. void Sigma2qq2squarksquark::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Extract mass-ordering indices iGen3 = 3*(abs(id3Sav)/2000000) + (abs(id3Sav)%10+1)/2; iGen4 = 3*(abs(id4Sav)/2000000) + (abs(id4Sav)%10+1)/2; // Is this a ~u_i ~d_j fial state or ~d_i ~d_j, ~u_i ~u_j if (abs(id3Sav) % 2 == abs(id4Sav) % 2) isUD = false; else isUD = true; // Derive name nameSave = "q q' -> "+particleDataPtr->name(abs(id3Sav))+" " +particleDataPtr->name(abs(id4Sav))+" + c.c."; // Count 5 neutralinos in NMSSM nNeut = (coupSUSYPtr->isNMSSM ? 5 : 4); // Store mass squares of all possible internal propagator lines m2Glu = pow2(particleDataPtr->m0(1000021)); m2Neut.resize(nNeut+1); for (int iNeut=1;iNeut<=nNeut;iNeut++) { m2Neut[iNeut] = pow2(particleDataPtr->m0(coupSUSYPtr->idNeut(iNeut))); } m2Char.resize(3); m2Char[1] = pow2(particleDataPtr->m0(coupSUSYPtr->idChar(1))); m2Char[2] = pow2(particleDataPtr->m0(coupSUSYPtr->idChar(2))); // Set sizes of some arrays to be used below tNeut.resize(nNeut+1); uNeut.resize(nNeut+1); tChar.resize(3); uChar.resize(3); // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(id3Sav, id4Sav); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qq2squarksquark::sigmaKin() { // Weak mixing double xW = coupSUSYPtr->sin2W; // pi/sH2 double comFacHat = M_PI/sH2 * openFracPair; // Channel-dependent but flavor-independent pre-factors sigmaNeut = comFacHat * pow2(alpEM) / pow2(xW) / pow2(1-xW); sigmaGlu = comFacHat * 2.0 * pow2(alpS) / 9.0; if (isUD) { sigmaChar = comFacHat * pow2(alpEM) / 4.0 / pow2(xW); sigmaCharNeut = comFacHat * pow2(alpEM) / 3.0 / pow2(xW) / (1-xW); sigmaCharGlu = comFacHat * 4.0 * alpEM * alpS / 9.0 / xW; sigmaNeutGlu = 0.0; } else { sigmaChar = 0.0; sigmaCharNeut = 0.0; sigmaCharGlu = 0.0; sigmaNeutGlu = comFacHat * 8.0 * alpEM * alpS / 9.0 / xW/(1-xW); } } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qq2squarksquark::sigmaHat() { // In-pair must be same-sign if (id1 * id2 < 0) return 0.0; // Check correct charge sum if (isUD && abs(id1) %2 == abs(id2) % 2) return 0.0; if (!isUD && abs(id1) % 2 != abs(id2) % 2) return 0.0; if (!isUD && abs(id1) % 2 != abs(id3Sav) % 2) return 0.0; // Coded sigma is for ud -> ~q~q'. Swap t and u for du -> ~q~q'. swapTU = (isUD && abs(id1) % 2 == 0); int idIn1A = (swapTU) ? abs(id2) : abs(id1); int idIn2A = (swapTU) ? abs(id1) : abs(id2); // Auxiliary factors for use below tGlu = tH - m2Glu; uGlu = uH - m2Glu; for (int i=1; i<= nNeut; i++) { tNeut[i] = tH - m2Neut[i]; uNeut[i] = uH - m2Neut[i]; if (isUD && i <= 2) { tChar[i] = tH - m2Char[i]; uChar[i] = uH - m2Char[i]; } } // Generation indices of incoming particles int iGen1 = (abs(idIn1A)+1)/2; int iGen2 = (abs(idIn2A)+1)/2; // Initial values for pieces used for color-flow selection below sumCt = 0.0; sumCu = 0.0; sumNt = 0.0; sumNu = 0.0; sumGt = 0.0; sumGu = 0.0; sumInterference = 0.0; // Common factor for LR and RL contributions double facTU = uH*tH-s3*s4; // Case A) Opposite-isospin: qq' -> ~d~u if ( isUD ) { // t-channel Charginos for (int k=1;k<=2;k++) { // Skip if only including gluinos if (settingsPtr->flag("SUSY:qq2squarksquark:onlyQCD")) continue; for (int l=1;l<=2;l++) { // kl-dependent factor for LL and RR contributions double facMS = sH*sqrt(m2Char[k]*m2Char[l]); // Note: Ckl defined as in [Boz07] with sigmaChar factored out // [1][1] = LL, [1][2] = LR, [2][1] = RL, [2][2] = RR complex Ckl[3][3]; Ckl[1][1] = facMS * coupSUSYPtr->LsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->LsduX[iGen3][iGen1][k]) * conj(coupSUSYPtr->LsudX[iGen4][iGen2][l]) * coupSUSYPtr->LsduX[iGen3][iGen1][l]; Ckl[1][2] = facTU * coupSUSYPtr->RsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->LsduX[iGen3][iGen1][k]) * conj(coupSUSYPtr->RsudX[iGen4][iGen2][l]) * coupSUSYPtr->LsduX[iGen3][iGen1][l]; Ckl[2][1] = facTU * coupSUSYPtr->LsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->RsduX[iGen3][iGen1][k]) * conj(coupSUSYPtr->LsudX[iGen4][iGen2][l]) * coupSUSYPtr->RsduX[iGen3][iGen1][l]; Ckl[2][2] = facMS * coupSUSYPtr->RsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->RsduX[iGen3][iGen1][k]) * conj(coupSUSYPtr->RsudX[iGen4][iGen2][l]) * coupSUSYPtr->RsduX[iGen3][iGen1][l]; // Add to sum of t-channel charginos sumCt += sigmaChar * real(Ckl[1][1] + Ckl[1][2] + Ckl[2][1] + Ckl[2][2]) / tChar[k] / tChar[l]; } } // u-channel Neutralinos for (int k=1;k<=nNeut;k++) { // Skip if only including gluinos if (settingsPtr->flag("SUSY:qq2squarksquark:onlyQCD")) continue; for (int l=1;l<=nNeut;l++) { // kl-dependent factor for LL, RR contributions double facMS = sH*sqrt(m2Neut[k]*m2Neut[l]); // Note: Nkl defined as in [Boz07] with sigmaNeut factored out // [1][1] = LL, [1][2] = LR, [2][1] = RL, [2][2] = RR complex Nkl[3][3]; Nkl[1][1] = facMS * conj(coupSUSYPtr->LsuuX[iGen4][iGen1][k]) * conj(coupSUSYPtr->LsddX[iGen3][iGen2][k]) * coupSUSYPtr->LsuuX[iGen4][iGen1][l] * coupSUSYPtr->LsddX[iGen3][iGen2][l]; Nkl[1][2] = facTU * conj(coupSUSYPtr->LsuuX[iGen4][iGen1][k]) * conj(coupSUSYPtr->RsddX[iGen3][iGen2][k]) * coupSUSYPtr->LsuuX[iGen4][iGen1][l] * coupSUSYPtr->RsddX[iGen3][iGen2][l]; Nkl[2][1] = facTU * conj(coupSUSYPtr->RsuuX[iGen4][iGen1][k]) * conj(coupSUSYPtr->LsddX[iGen3][iGen2][k]) * coupSUSYPtr->RsuuX[iGen4][iGen1][l] * coupSUSYPtr->LsddX[iGen3][iGen2][l]; Nkl[2][2] = facMS * conj(coupSUSYPtr->RsuuX[iGen4][iGen1][k]) * conj(coupSUSYPtr->RsddX[iGen3][iGen2][k]) * coupSUSYPtr->RsuuX[iGen4][iGen1][l] * coupSUSYPtr->RsddX[iGen3][iGen2][l]; // Add to sum of u-channel neutralinos sumNu += sigmaNeut / uNeut[k] / uNeut[l] * real(Nkl[1][1] + Nkl[1][2] + Nkl[2][1] + Nkl[2][2]); } } // u-channel gluino // Note: Gij defined as in [Boz07] with sigmaGlu factored out // [1][1] = LL, [1][2] = LR, [2][1] = RL, [2][2] = RR double Gij[3][3]; Gij[1][1] = norm(coupSUSYPtr->LsuuG[iGen4][iGen1] * coupSUSYPtr->LsddG[iGen3][iGen2]); Gij[1][2] = norm(coupSUSYPtr->LsuuG[iGen4][iGen1] * coupSUSYPtr->RsddG[iGen3][iGen2]); Gij[2][1] = norm(coupSUSYPtr->RsuuG[iGen4][iGen1] * coupSUSYPtr->LsddG[iGen3][iGen2]); Gij[2][2] = norm(coupSUSYPtr->RsuuG[iGen4][iGen1] * coupSUSYPtr->RsddG[iGen3][iGen2]); Gij[1][1] *= sH*m2Glu; Gij[1][2] *= facTU; Gij[2][1] *= facTU; Gij[2][2] *= sH*m2Glu; // Sum over polarizations sumGu += sigmaGlu * (Gij[1][1] + Gij[1][2] + Gij[2][1] + Gij[2][2]) / pow2(uGlu); // chargino-neutralino interference for (int k=1;k<=2;k++) { for (int l=1;l<=nNeut;l++) { // Skip if only including gluinos if (settingsPtr->flag("SUSY:qq2squarksquark:onlyQCD")) continue; // Note: CNkl defined as in [Boz07] with pi/sH2 factored out // [1][1] = LL, [1][2] = LR, [2][1] = RL, [2][2] = RR double CNkl[3][3]; CNkl[1][1] = real(coupSUSYPtr->LsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->LsduX[iGen3][iGen1][k]) * coupSUSYPtr->LsuuX[iGen4][iGen1][l] * coupSUSYPtr->LsddX[iGen3][iGen2][l]); CNkl[1][2] = real(coupSUSYPtr->RsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->LsduX[iGen3][iGen1][k]) * coupSUSYPtr->LsuuX[iGen4][iGen1][l] * coupSUSYPtr->RsddX[iGen3][iGen2][l]); CNkl[2][1] = real(coupSUSYPtr->LsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->RsduX[iGen3][iGen1][k]) * coupSUSYPtr->RsuuX[iGen4][iGen1][l] * coupSUSYPtr->LsddX[iGen3][iGen2][l]); CNkl[2][2] = real(coupSUSYPtr->RsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->RsduX[iGen3][iGen1][k]) * coupSUSYPtr->RsuuX[iGen4][iGen1][l] * coupSUSYPtr->RsddX[iGen3][iGen2][l]); CNkl[1][1] *= sH*sqrt(m2Char[k]*m2Neut[l]); CNkl[1][2] *= uH*tH-s3*s4; CNkl[2][1] *= uH*tH-s3*s4; CNkl[2][2] *= sH*sqrt(m2Char[k]*m2Neut[l]); // Sum over polarizations sumInterference += sigmaCharNeut * (CNkl[1][1] + CNkl[1][2] + CNkl[2][1] + CNkl[2][2]) / tChar[k] / uNeut[l]; } } // chargino-gluino interference for (int k=1;k<=2;k++) { // Skip if only including gluinos if (settingsPtr->flag("SUSY:qq2squarksquark:onlyQCD")) continue; // Note: CGk defined as in [Boz07] with sigmaCharGlu factored out // [1][1] = LL, [1][2] = LR, [2][1] = RL, [2][2] = RR double CGk[3][3]; CGk[1][1] = real(coupSUSYPtr->LsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->LsduX[iGen3][iGen1][k]) * conj(coupSUSYPtr->LsuuG[iGen4][iGen1]) * conj(coupSUSYPtr->LsddG[iGen3][iGen2])); CGk[1][2] = real(coupSUSYPtr->RsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->LsduX[iGen3][iGen1][k]) * conj(coupSUSYPtr->LsuuG[iGen4][iGen1]) * conj(coupSUSYPtr->RsddG[iGen3][iGen2])); CGk[2][1] = real(coupSUSYPtr->LsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->RsduX[iGen3][iGen1][k]) * conj(coupSUSYPtr->RsuuG[iGen4][iGen1]) * conj(coupSUSYPtr->LsddG[iGen3][iGen2])); CGk[2][2] = real(coupSUSYPtr->RsudX[iGen4][iGen2][k] * conj(coupSUSYPtr->RsduX[iGen3][iGen1][k]) * conj(coupSUSYPtr->RsuuG[iGen4][iGen1]) * conj(coupSUSYPtr->RsddG[iGen3][iGen2])); CGk[1][1] *= sH*sqrt(m2Glu*m2Char[k]); CGk[1][2] *= uH*tH-s3*s4; CGk[2][1] *= uH*tH-s3*s4; CGk[2][2] *= sH*sqrt(m2Glu*m2Char[k]); // Sum over polarizations sumInterference += sigmaGlu * (CGk[1][1] + CGk[1][2] + CGk[2][1] + CGk[2][2]) / uGlu / tChar[k]; } } // Case B) Same-isospin: qq' -> ~d~d , ~u~u else { // t-channel + u-channel Neutralinos + t/u interference for (int k=1;k<=nNeut;k++) { // Skip if only including gluinos if (settingsPtr->flag("SUSY:qq2squarksquark:onlyQCD")) continue; for (int l=1;l<=nNeut;l++) { // kl-dependent factor for LL and RR contributions double facMS = sH * particleDataPtr->m0(coupSUSYPtr->idNeut(k)) * particleDataPtr->m0(coupSUSYPtr->idNeut(l)); // Note: Nxkl defined as in [Boz07] with sigmaNeut factored out // [1][1] = LL, [1][2] = LR, [2][1] = RL, [2][2] = RR complex NTkl[3][3], NUkl[3][3], NTUkl[3][3]; NTkl[1][1] = facMS * conj(coupSUSYPtr->getLsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getLsqqX(iGen3,idIn1A,k)) * coupSUSYPtr->getLsqqX(iGen4,idIn2A,l) * coupSUSYPtr->getLsqqX(iGen3,idIn1A,l); NTkl[1][2] = facTU * conj(coupSUSYPtr->getRsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getLsqqX(iGen3,idIn1A,k)) * coupSUSYPtr->getRsqqX(iGen4,idIn2A,l) * coupSUSYPtr->getLsqqX(iGen3,idIn1A,l); NTkl[2][1] = facTU * conj(coupSUSYPtr->getLsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getRsqqX(iGen3,idIn1A,k)) * coupSUSYPtr->getLsqqX(iGen4,idIn2A,l) * coupSUSYPtr->getRsqqX(iGen3,idIn1A,l); NTkl[2][2] = facMS * conj(coupSUSYPtr->getRsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getRsqqX(iGen3,idIn1A,k)) * coupSUSYPtr->getRsqqX(iGen4,idIn2A,l) * coupSUSYPtr->getRsqqX(iGen3,idIn1A,l); NUkl[1][1] = facMS * conj(coupSUSYPtr->getLsqqX(iGen3,idIn2A,k)) * conj(coupSUSYPtr->getLsqqX(iGen4,idIn1A,k)) * coupSUSYPtr->getLsqqX(iGen3,idIn2A,l) * coupSUSYPtr->getLsqqX(iGen4,idIn1A,l); NUkl[1][2] = facTU * conj(coupSUSYPtr->getRsqqX(iGen3,idIn2A,k)) * conj(coupSUSYPtr->getLsqqX(iGen4,idIn1A,k)) * coupSUSYPtr->getRsqqX(iGen3,idIn2A,l) * coupSUSYPtr->getLsqqX(iGen4,idIn1A,l); NUkl[2][1] = facTU * conj(coupSUSYPtr->getLsqqX(iGen3,idIn2A,k)) * conj(coupSUSYPtr->getRsqqX(iGen4,idIn1A,k)) * coupSUSYPtr->getLsqqX(iGen3,idIn2A,l) * coupSUSYPtr->getRsqqX(iGen4,idIn1A,l); NUkl[2][2] = facMS * conj(coupSUSYPtr->getRsqqX(iGen3,idIn2A,k)) * conj(coupSUSYPtr->getRsqqX(iGen4,idIn1A,k)) * coupSUSYPtr->getRsqqX(iGen3,idIn2A,l) * coupSUSYPtr->getRsqqX(iGen4,idIn1A,l); NTUkl[1][1] = facMS * real( conj(coupSUSYPtr->getLsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getLsqqX(iGen3,idIn1A,k)) * coupSUSYPtr->getLsqqX(iGen3,idIn2A,l) * coupSUSYPtr->getLsqqX(iGen4,idIn1A,l) ); NTUkl[1][2] = facTU * real( conj(coupSUSYPtr->getRsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getLsqqX(iGen3,idIn1A,k)) * coupSUSYPtr->getRsqqX(iGen3,idIn2A,l) * coupSUSYPtr->getLsqqX(iGen4,idIn1A,l) ); NTUkl[2][1] = facTU * real( conj(coupSUSYPtr->getLsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getRsqqX(iGen3,idIn1A,k)) * coupSUSYPtr->getLsqqX(iGen3,idIn2A,l) * coupSUSYPtr->getRsqqX(iGen4,idIn1A,l) ); NTUkl[2][2] = facMS * real( conj(coupSUSYPtr->getRsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getRsqqX(iGen3,idIn1A,k)) * coupSUSYPtr->getRsqqX(iGen3,idIn2A,l) * coupSUSYPtr->getRsqqX(iGen4,idIn1A,l) ); // Add to sums sumNt += sigmaNeut / tNeut[k] / tNeut[l] * real(NTkl[1][1] + NTkl[1][2] + NTkl[2][1] + NTkl[2][2]); sumNu += sigmaNeut / uNeut[k] / uNeut[l] * real(NUkl[1][1] + NUkl[1][2] + NUkl[2][1] + NUkl[2][2]); sumInterference += 2.0 / 3.0 * sigmaNeut * real(NTUkl[1][1] + NTUkl[1][2] + NTUkl[2][1] + NTUkl[2][2]) / tNeut[k] / uNeut[l]; } // Neutralino / Gluino interference // k-dependent factor for LL and RR contributions double facMS = sH * particleDataPtr->m0(coupSUSYPtr->idNeut(k)) * particleDataPtr->m0(1000021); // Note: Nxkl defined as in [Boz07] with sigmaNeutGlu factored out // [1][1] = LL, [1][2] = LR, [2][1] = RL, [2][2] = RR complex NGA[3][3], NGB[3][3]; NGA[1][1] = facMS * real( conj(coupSUSYPtr->getLsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getLsqqX(iGen3,idIn1A,k)) * conj(coupSUSYPtr->getLsqqG(iGen3,idIn2A)) * conj(coupSUSYPtr->getLsqqG(iGen4,idIn1A)) ); NGA[1][2] = facTU * real( conj(coupSUSYPtr->getRsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getLsqqX(iGen3,idIn1A,k)) * conj(coupSUSYPtr->getLsqqG(iGen3,idIn2A)) * conj(coupSUSYPtr->getRsqqG(iGen4,idIn1A)) ); NGA[2][1] = facTU * real( conj(coupSUSYPtr->getLsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getRsqqX(iGen3,idIn1A,k)) * conj(coupSUSYPtr->getRsqqG(iGen3,idIn2A)) * conj(coupSUSYPtr->getLsqqG(iGen4,idIn1A)) ); NGA[2][2] = facMS * real( conj(coupSUSYPtr->getRsqqX(iGen4,idIn2A,k)) * conj(coupSUSYPtr->getRsqqX(iGen3,idIn1A,k)) * conj(coupSUSYPtr->getRsqqG(iGen3,idIn2A)) * conj(coupSUSYPtr->getRsqqG(iGen4,idIn1A)) ); NGB[1][1] = facMS * real( conj(coupSUSYPtr->getLsqqX(iGen3,idIn2A,k)) * conj(coupSUSYPtr->getLsqqX(iGen4,idIn1A,k)) * conj(coupSUSYPtr->getLsqqG(iGen4,idIn2A)) * conj(coupSUSYPtr->getLsqqG(iGen3,idIn1A)) ); NGB[1][2] = facMS * real( conj(coupSUSYPtr->getRsqqX(iGen3,idIn2A,k)) * conj(coupSUSYPtr->getLsqqX(iGen4,idIn1A,k)) * conj(coupSUSYPtr->getRsqqG(iGen4,idIn2A)) * conj(coupSUSYPtr->getLsqqG(iGen3,idIn1A)) ); NGB[2][1] = facMS * real( conj(coupSUSYPtr->getLsqqX(iGen3,idIn2A,k)) * conj(coupSUSYPtr->getRsqqX(iGen4,idIn1A,k)) * conj(coupSUSYPtr->getLsqqG(iGen4,idIn2A)) * conj(coupSUSYPtr->getRsqqG(iGen3,idIn1A)) ); NGB[2][2] = facMS * real( conj(coupSUSYPtr->getRsqqX(iGen3,idIn2A,k)) * conj(coupSUSYPtr->getRsqqX(iGen4,idIn1A,k)) * conj(coupSUSYPtr->getRsqqG(iGen4,idIn2A)) * conj(coupSUSYPtr->getRsqqG(iGen3,idIn1A)) ); // Add to sums sumInterference += sigmaNeutGlu * ( real(NGA[1][1] + NGA[1][2] + NGA[2][1] + NGA[2][2]) / tNeut[k] / uGlu + real(NGB[1][1] + NGB[1][2] + NGB[2][1] + NGB[2][2]) / uNeut[k] / tGlu ); } // t-channel + u-channel Gluinos + t/u interference // factor for LL and RR contributions double facMS = sH * m2Glu; // Note: GT, GU defined as in [Boz07] with sigmaGlu factored out // [1][1] = LL, [1][2] = LR, [2][1] = RL, [2][2] = RR complex GT[3][3], GU[3][3], GTU[3][3]; GT[1][1] = facMS * norm(coupSUSYPtr->getLsqqG(iGen4,idIn2A) * coupSUSYPtr->getLsqqG(iGen3,idIn1A)); GT[1][2] = facTU * norm(coupSUSYPtr->getRsqqG(iGen4,idIn2A) * coupSUSYPtr->getLsqqG(iGen3,idIn1A)); GT[2][1] = facTU * norm(coupSUSYPtr->getLsqqG(iGen4,idIn2A) * coupSUSYPtr->getRsqqG(iGen3,idIn1A)); GT[2][2] = facMS * norm(coupSUSYPtr->getRsqqG(iGen4,idIn2A) * coupSUSYPtr->getRsqqG(iGen3,idIn1A)); GU[1][1] = facMS * norm(coupSUSYPtr->getLsqqG(iGen3,idIn2A) * coupSUSYPtr->getLsqqG(iGen4,idIn1A)); GU[1][2] = facTU * norm(coupSUSYPtr->getLsqqG(iGen3,idIn2A) * coupSUSYPtr->getRsqqG(iGen4,idIn1A)); GU[2][1] = facTU * norm(coupSUSYPtr->getRsqqG(iGen3,idIn2A) * coupSUSYPtr->getLsqqG(iGen4,idIn1A)); GU[2][2] = facMS * norm(coupSUSYPtr->getRsqqG(iGen3,idIn2A) * coupSUSYPtr->getRsqqG(iGen4,idIn1A)); GTU[1][1] = facMS * real(coupSUSYPtr->getLsqqG(iGen3,idIn1A) * coupSUSYPtr->getLsqqG(iGen4,idIn2A) * conj(coupSUSYPtr->getLsqqG(iGen3,idIn2A)) * conj(coupSUSYPtr->getLsqqG(iGen4,idIn1A)) ); GTU[1][2] = facTU * real(coupSUSYPtr->getLsqqG(iGen3,idIn1A) * coupSUSYPtr->getRsqqG(iGen4,idIn2A) * conj(coupSUSYPtr->getRsqqG(iGen3,idIn2A)) * conj(coupSUSYPtr->getLsqqG(iGen4,idIn1A)) ); GTU[2][1] = facTU * real(coupSUSYPtr->getRsqqG(iGen3,idIn1A) * coupSUSYPtr->getLsqqG(iGen4,idIn2A) * conj(coupSUSYPtr->getLsqqG(iGen3,idIn2A)) * conj(coupSUSYPtr->getRsqqG(iGen4,idIn1A)) ); GTU[2][2] = facMS * real(coupSUSYPtr->getRsqqG(iGen3,idIn1A) * coupSUSYPtr->getRsqqG(iGen4,idIn2A) * conj(coupSUSYPtr->getRsqqG(iGen3,idIn2A)) * conj(coupSUSYPtr->getRsqqG(iGen4,idIn1A)) ); // Add to sums sumGt += sigmaGlu * real(GT[1][1] + GT[1][2] + GT[2][1] + GT[2][2]) / pow2(tGlu) ; sumGu += sigmaGlu * real(GU[1][1] + GU[1][2] + GU[2][1] + GU[2][2]) / pow2(uGlu) ; sumInterference += - 2.0 / 3.0 * sigmaGlu * real(GTU[1][1] + GTU[1][2] + GTU[2][1] + GTU[2][2]) / tGlu / uGlu; } // Cross section double sigma = sumNt + sumNu + sumCt + sumCu + sumGt + sumGu + sumInterference; // Identical particles? if (id3Sav == id4Sav) sigma /= 2.0; // Return answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qq2squarksquark::setIdColAcol() { // Set flavours. if (id1 > 0 && id2 > 0) { setId( id1, id2, id3Sav, id4Sav); } else { // 1,2 -> -3,-4 setId( id1, id2,-id3Sav,-id4Sav); } // Coded sigma is for ud -> ~q~q'. Swap t and u for du -> ~q~q'. swapTU = (isUD && abs(id1) % 2 == 0); // Select colour flow topology // Recompute contributions to this particular in- out- flavour combination sigmaHat(); // A: t-channel neutralino, t-channel chargino, or u-channel gluino double sumA = sumNt + sumCt + sumGu; double sumAB = sumNt + sumNu + sumCt + sumCu + sumGt + sumGu; if (swapTU) sumA = sumAB - sumA; setColAcol( 1, 0, 2, 0, 1, 0, 2, 0); // B: t-channel gluino or u-channel neutralino if (rndmPtr->flat()*sumAB > sumA) setColAcol( 1, 0, 2, 0, 2, 0, 1, 0); // Switch to anti-colors if antiquarks if (id1 < 0 || id2 < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2squarkantisquark // Cross section for qqbar-initiated squark-antisquark production //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2squarkantisquark::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Is this a ~u_i ~d*_j, ~d_i ~u*_j final state or ~d_i ~d*_j, ~u_i ~u*_j if (abs(id3Sav) % 2 == abs(id4Sav) % 2) isUD = false; else isUD = true; // Extract isospin and mass-ordering indices if(isUD && abs(id3Sav)%2 == 1){ iGen3 = 3*(abs(id4Sav)/2000000) + (abs(id3Sav)%10+1)/2; iGen4 = 3*(abs(id3Sav)/2000000) + (abs(id4Sav)%10+1)/2; } else { iGen3 = 3*(abs(id3Sav)/2000000) + (abs(id3Sav)%10+1)/2; iGen4 = 3*(abs(id4Sav)/2000000) + (abs(id4Sav)%10+1)/2; } // Derive name nameSave = "q qbar' -> "+particleDataPtr->name(abs(id3Sav))+" "+ particleDataPtr->name(-abs(id4Sav)); if (isUD && abs(id3Sav) != abs(id4Sav)) nameSave +=" + c.c."; // Count 5 neutralinos in NMSSM nNeut = (coupSUSYPtr->isNMSSM ? 5 : 4); // Store mass squares of all possible internal propagator lines m2Glu = pow2(particleDataPtr->m0(1000021)); m2Neut.resize(nNeut+1); for (int iNeut=1;iNeut<=nNeut;iNeut++) m2Neut[iNeut] = pow2(particleDataPtr->m0(coupSUSYPtr->idNeut(iNeut))); // Set sizes of some arrays to be used below tNeut.resize(nNeut+1); uNeut.resize(nNeut+1); // Shorthand for Weak mixing xW = coupSUSYPtr->sin2W; // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(id3Sav, id4Sav); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2squarkantisquark::sigmaKin() { // Z/W propagator if (! isUD) { double sV= sH - pow2(coupSUSYPtr->mZpole); double d = pow2(sV) + pow2(coupSUSYPtr->mZpole * coupSUSYPtr->wZpole); propZW = complex( sV / d, coupSUSYPtr->mZpole * coupSUSYPtr->wZpole / d); } else { double sV= sH - pow2(coupSUSYPtr->mWpole); double d = pow2(sV) + pow2(coupSUSYPtr->mWpole * coupSUSYPtr->wWpole); propZW = complex( sV / d, coupSUSYPtr->mWpole * coupSUSYPtr->wWpole / d); } // Flavor-independent pre-factors double comFacHat = M_PI/sH2 * openFracPair; sigmaEW = comFacHat * pow2(alpEM); sigmaGlu = comFacHat * 2.0 * pow2(alpS) / 9.0; sigmaEWG = comFacHat * 8.0 * alpEM * alpS / 9.0; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2squarkantisquark::sigmaHat() { // In-pair must be opposite-sign if (id1 * id2 > 0) return 0.0; // Check correct charge sum if (isUD && abs(id1) %2 == abs(id2) % 2) return 0.0; if (!isUD && abs(id1) % 2 != abs(id2) % 2) return 0.0; // Check if using QCD diagrams only bool onlyQCD = settingsPtr->flag("SUSY:qqbar2squarkantisquark:onlyQCD"); // Coded UD sigma is for udbar -> ~u~d'*. Swap t<->u for dbaru -> ~u~d'*. swapTU = (isUD && abs(id1) % 2 != 0); // Coded QQ sigma is for qqbar -> ~q~q*. Swap t<->u for qbarq -> ~q~q*. if (!isUD && id1 < 0) swapTU = true; // Generation indices of incoming particles int idIn1A = (swapTU) ? abs(id2) : abs(id1); int idIn2A = (swapTU) ? abs(id1) : abs(id2); int iGen1 = (idIn1A+1)/2; int iGen2 = (idIn2A+1)/2; // Auxiliary factors for use below tGlu = tH - m2Glu; uGlu = uH - m2Glu; for (int i=1; i<= nNeut; i++) { tNeut[i] = tH - m2Neut[i]; uNeut[i] = uH - m2Neut[i]; } // Initial values for pieces used for color-flow selection below sumColS = 0.0; sumColT = 0.0; sumInterference = 0.0; // Common factor for LR and RL contributions double facTU = uH*tH-s3*s4; // Case A) Opposite-isospin: udbar -> ~u~d* if ( isUD ) { // s-channel W contribution (only contributes to LL helicities) if ( !onlyQCD ) { sumColS += sigmaEW / 16.0 / pow2(xW) / pow2(1.0-xW) * norm(conj(coupSUSYPtr->LudW[iGen1][iGen2]) * coupSUSYPtr->LsusdW[iGen3][iGen4]) * facTU * norm(propZW); } // t-channel gluino contributions double GT[3][3]; double facLR = m2Glu * sH; // LL, LR, RL, RR GT[1][1] = facTU * norm(conj(coupSUSYPtr->LsddG[iGen4][iGen2]) *coupSUSYPtr->LsuuG[iGen3][iGen1]); GT[1][2] = facLR * norm(conj(coupSUSYPtr->RsddG[iGen4][iGen2]) *coupSUSYPtr->LsuuG[iGen3][iGen1]); GT[2][1] = facLR * norm(conj(coupSUSYPtr->LsddG[iGen4][iGen2]) *coupSUSYPtr->RsuuG[iGen3][iGen1]); GT[2][2] = facTU * norm(conj(coupSUSYPtr->RsddG[iGen4][iGen2]) *coupSUSYPtr->RsuuG[iGen3][iGen1]); // leading color flow for t-channel gluino is annihilation-like sumColS += sigmaGlu / pow2(tGlu) * (GT[1][1] + GT[1][2] + GT[2][1] + GT[2][2]); // W-Gluino interference (only contributes to LL helicities) if ( !onlyQCD ) { sumColS += sigmaEWG / 4.0 / xW / (1-xW) * real(conj(coupSUSYPtr->LsuuG[iGen3][iGen1]) * coupSUSYPtr->LsddG[iGen4][iGen2] * conj(coupSUSYPtr->LudW[iGen1][iGen2]) * coupSUSYPtr->LsusdW[iGen3][iGen4]) * facTU / tGlu * sqrt(norm(propZW)); } // t-channel neutralinos // NOT YET IMPLEMENTED ! } // Case B) Same-isospin: qqbar -> ~d~d* , ~u~u* else { double eQ = (idIn1A % 2 == 0) ? 2./3. : 1./3. ; double eSq = (abs(id3Sav) % 2 == 0) ? 2./3. : 1./3. ; // s-channel gluon (strictly flavor-diagonal) if (abs(id3Sav) == abs(id4Sav) && abs(id1) == abs(id2)) { // Factor 2 since contributes to both ha != hb helicities sumColT += 2. * sigmaGlu * facTU / pow2(sH); } // t-channel gluino (only for in-isospin = out-isospin). if (eQ == eSq) { // Sum over helicities. double GT[3][3]; double facLR = sH * m2Glu; GT[1][1] = facTU * norm(coupSUSYPtr->getLsqqG(iGen3,idIn1A) * conj(coupSUSYPtr->getLsqqG(iGen4,idIn2A))); GT[1][2] = facLR * norm(coupSUSYPtr->getLsqqG(iGen3,idIn1A) * conj(coupSUSYPtr->getRsqqG(iGen4,idIn2A))); GT[2][1] = facLR * norm(coupSUSYPtr->getRsqqG(iGen3,idIn1A) * conj(coupSUSYPtr->getLsqqG(iGen4,idIn2A))); GT[2][2] = facTU * norm(coupSUSYPtr->getRsqqG(iGen3,idIn1A) * conj(coupSUSYPtr->getRsqqG(iGen4,idIn2A))); // Add contribution to color topology: S sumColS += sigmaGlu / pow2(tGlu) * ( GT[1][1] + GT[1][2] + GT[2][1] + GT[2][2]); // gluon-gluino interference (strictly flavor-diagonal) if (abs(id3Sav) == abs(id4Sav) && abs(id1) == abs(id2)) { double GG11, GG22; GG11 = - facTU * 2./3. * real( conj(coupSUSYPtr->getLsqqG(iGen3,idIn1A)) * coupSUSYPtr->getLsqqG(iGen4,idIn2A)); GG22 = - facTU * 2./3. * real( conj(coupSUSYPtr->getRsqqG(iGen3,idIn1A)) * coupSUSYPtr->getRsqqG(iGen4,idIn2A)); // Sum over two contributing helicities sumInterference += sigmaGlu / sH / tGlu * ( GG11 + GG22 ); } } // Skip the rest if only including QCD diagrams if (onlyQCD) return sumColT+sumColS+sumInterference; // s-channel photon (strictly flavor-diagonal) and Z/gamma interference if (abs(id3Sav) == abs(id4Sav) && abs(id1) == abs(id2)) { // gamma // Factor 2 since contributes to both ha != hb helicities sumColS += 2. * pow2(eQ) * pow2(eSq) * sigmaEW * facTU / pow2(sH); // Z/gamma interference double CsqZ = real(coupSUSYPtr->LsusuZ[iGen3][iGen4] + coupSUSYPtr->RsusuZ[iGen3][iGen4]); if (abs(id3Sav)%2 != 0) CsqZ = real(coupSUSYPtr->LsdsdZ[iGen3][iGen4] + coupSUSYPtr->RsdsdZ[iGen3][iGen4]); sumColS += eQ * eSq * sigmaEW * facTU / 2.0 / xW / (1.-xW) * sqrt(norm(propZW)) / sH * CsqZ * (coupSUSYPtr->LqqZ[idIn1A] + coupSUSYPtr->LqqZ[idIn2A]); // Gluino/gamma interference (only for same-isospin) if (eQ == eSq) { double CsqG11 = real(conj(coupSUSYPtr->LsuuG[iGen3][iGen1]) *coupSUSYPtr->LsuuG[iGen4][iGen2]); double CsqG22 = real(conj(coupSUSYPtr->RsuuG[iGen3][iGen1]) *coupSUSYPtr->RsuuG[iGen4][iGen2]); if (id3Sav%2 != 0) { CsqG11 = real(conj(coupSUSYPtr->LsddG[iGen3][iGen1]) *coupSUSYPtr->LsddG[iGen4][iGen2]); CsqG22 = real(conj(coupSUSYPtr->RsddG[iGen3][iGen1]) *coupSUSYPtr->RsddG[iGen4][iGen2]); } sumColS += eQ * eSq * sigmaEWG * facTU * (CsqG11 + CsqG22) / sH / tGlu; } } // s-channel Z (only for q flavor = qbar flavor) if (abs(id1) == abs(id2)) { double CsqZ = norm(coupSUSYPtr->LsusuZ[iGen3][iGen4] + coupSUSYPtr->RsusuZ[iGen3][iGen4]); if (abs(id3Sav)%2 != 0) CsqZ = norm(coupSUSYPtr->LsdsdZ[iGen3][iGen4] + coupSUSYPtr->RsdsdZ[iGen3][iGen4]); sumColS += sigmaEW * facTU / 16.0 / pow2(xW) / pow2(1.0-xW) * norm(propZW) * CsqZ * ( pow2(coupSUSYPtr->LqqZ[idIn1A]) + pow2(coupSUSYPtr->RqqZ[idIn1A]) ); // Z/gluino interference (only for in-isospin = out-isospin) if (eQ == eSq) { double GZ11 = real(conj(coupSUSYPtr->getLsqqG(iGen3,idIn1A)) *coupSUSYPtr->getLsqqG(iGen4,idIn2A) *(coupSUSYPtr->getLsqsqZ(id3Sav,id4Sav) +coupSUSYPtr->getRsqsqZ(id3Sav,id4Sav))) *coupSUSYPtr->LqqZ[idIn1A]; double GZ22 = real(conj(coupSUSYPtr->getRsqqG(iGen3,idIn1A)) *coupSUSYPtr->getRsqqG(iGen4,idIn2A) *(coupSUSYPtr->getLsqsqZ(id3Sav,id4Sav) +coupSUSYPtr->getRsqsqZ(id3Sav,id4Sav))) *coupSUSYPtr->RqqZ[idIn1A]; sumColS += sigmaEWG * facTU / 4.0 / xW / (1.-xW) * ( GZ11 + GZ22 ) * sqrt(norm(propZW)) / tGlu; } } // t-channel neutralinos // NOT YET IMPLEMENTED ! } // Cross section double sigma = sumColS + sumColT + sumInterference; // Return answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2squarkantisquark::setIdColAcol() { // Check if charge conjugate final state? isCC = false; if (isUD && ( (id1-1)%2 < 0 || (id2-1)%2 < 0 )) isCC = true; //check if charge conjugate id3 = (isCC) ? -id3Sav : id3Sav; id4 = (isCC) ? -id4Sav : id4Sav; // Set flavours. setId( id1, id2, id3, id4); // Coded UD sigma is for udbar -> ~u~d'*. Swap t<->u for dbaru -> ~u~d'*. // Coded QQ sigma is for qqbar -> ~q~q*. Swap t<->u for qbarq -> ~q~q*. if (isUD) { swapTU = (abs(id1) % 2 != 0); } else { swapTU = (id1 < 0); } // Select colour flow topology // Recompute individual contributions to this in-out flavour combination sigmaHat(); double R = rndmPtr->flat(); double fracS = sumColS / (sumColS + sumColT) ; // S: color flow as in S-channel singlet if (R < fracS) { setColAcol( 1, 0, 0, 1, 2, 0, 0, 2); if (swapTU) setColAcol( 0, 1, 1, 0, 2, 0, 0, 2); } // T: color flow as in T-channel singlet else { setColAcol( 1, 0, 0, 2, 1, 0, 0, 2); if (swapTU) setColAcol( 0, 1, 2, 0, 2, 0, 0, 1); } if (isCC) swapColAcol(); } //========================================================================== // Sigma2gg2squarkantisquark // Cross section for gg-initiated squark-antisquark production //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2squarkantisquark::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Process Name nameSave = "g g -> "+particleDataPtr->name(abs(id3Sav))+" " +particleDataPtr->name(-abs(id4Sav)); // Squark pole mass m2Sq = pow2(particleDataPtr->m0(id3Sav)); // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(id3Sav, id4Sav); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2gg2squarkantisquark::sigmaKin() { // Modified Mandelstam variables for massive kinematics with m3 = m4. // tHSq = tHat - m_squark^2; uHSq = uHat - m_squark^2. // double s34Avg = 0.5 * (s3 + s4) - 0.25 * pow2(s3 - s4) / sH; double tHSq = -0.5 * (sH - tH + uH); double uHSq = -0.5 * (sH + tH - uH); // ! (NEED TO CHECK THAT THESE APPLIED CORRECTLY BELOW) ! // ! (PRELIMINARY CROSS-CHECKS WITH PYTHIA 6 COME OUT OK) ! // Helicity-independent prefactor double comFacHat = M_PI/sH2 * pow2(alpS) / 128.0 * ( 24.0 * (1.0 - 2*tHSq*uHSq/sH2) - 8.0/3.0 ); // Helicity-dependent factors sigma = 0.0; for (int ha=-1;ha<=1;ha += 2) { for (int hb=-1;hb<=1;hb += 2) { // Divide by 4 for helicity average sigma += comFacHat / 4.0 * ( (1.0-ha*hb) - 2.0 * sH*m2Sq/tHSq/uHSq * ( 1.0 - ha*hb - sH*m2Sq/tHSq/uHSq)); } } } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2squarkantisquark::setIdColAcol() { // Set flavours. setId( id1, id2, id3Sav, id4Sav); // Set color flow (random for now) double R = rndmPtr->flat(); if (R < 0.5) setColAcol( 1, 2, 2, 3, 1, 0, 0, 3); else setColAcol( 1, 2, 3, 1, 3, 0, 0, 2); } //========================================================================== // Sigma2qg2squarkgluino // Cross section for squark-gluino production //-------------------------------------------------------------------------- // Initialize process. void Sigma2qg2squarkgluino::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Derive name nameSave = "q g -> "+particleDataPtr->name(abs(id3Sav))+" gluino + c.c."; // Final-state mass squares m2Glu = pow2(particleDataPtr->m0(1000021)); m2Sq = pow2(particleDataPtr->m0(id3Sav)); // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(id3Sav, 1000021); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qg2squarkgluino::sigmaKin() { // Common pre-factor comFacHat = (M_PI / sH2) * pow2(alpS) * 0.5 * openFracPair; // Invariants (still with Pythia 6 sign convention) double tGlu = m2Glu-tH; double uGlu = m2Glu-uH; double tSq = m2Sq-tH; double uSq = m2Sq-uH; // Color flow A: quark color annihilates with anticolor of g sigmaA = 0.5*4./9.* tGlu/sH + (tGlu*sH+2.*m2Glu*tSq)/pow2(tGlu) - ( (sH-m2Sq+m2Glu)*(-tSq)-sH*m2Glu )/sH/(-tGlu) + 0.5*1./2.*( tSq*(tH+2.*uH+m2Glu)-tGlu*(sH-2.*tSq) + (-uGlu)*(tH+m2Glu+2.*m2Sq) )/2./tGlu/uSq; // Color flow B: quark and gluon colors iterchanged sigmaB = 4./9.*(-uGlu)*(uH+m2Sq)/pow2(uSq) + 1./18.* (sH*(uH+m2Glu) + 2.*(m2Sq-m2Glu)*uGlu)/sH/(-uSq) + 0.5*4./9.*tGlu/sH + 0.5*1./2.*(tSq*(tH+2.*uH+m2Glu)-tGlu*(sH-2.*tSq) + (-uGlu)*(tH+m2Glu+2.*m2Sq))/2./tGlu/uSq; } //-------------------------------------------------------------------------- double Sigma2qg2squarkgluino::sigmaHat() { // Check whether right incoming flavor int idQA = (id1 == 21) ? id2 : id1; int idSq = (abs(id3) == 10000021) ? id4 : id3; // Check for charge conservation if(idQA%2 != idSq%2) return 0.0; int idQ = (abs(idQA)+1)/2; idSq = 3 * (id3Sav / 2000000) + (id3Sav % 10 + 1)/2; double mixingFac; if(abs(idQA) % 2 == 1) mixingFac = norm(coupSUSYPtr->LsddG[idSq][idQ]) + norm(coupSUSYPtr->RsddG[idSq][idQ]); else mixingFac = norm(coupSUSYPtr->LsuuG[idSq][idQ]) + norm(coupSUSYPtr->RsuuG[idSq][idQ]); return mixingFac * comFacHat * (sigmaA + sigmaB); } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qg2squarkgluino::setIdColAcol() { // Check if charge conjugate final state? int idQ = (id1 == 21) ? id2 : id1; id3 = (idQ > 0) ? id3Sav : -id3Sav; id4 = 1000021; // Set flavors setId( id1, id2, id3, id4); // Select color flow A or B (see above) // Recompute individual contributions to this in-out flavour combination sigmaHat(); double R = rndmPtr->flat()*(sigmaA+sigmaB); if (idQ == id1) { setColAcol(1,0,2,1,3,0,2,3); if (R > sigmaA) setColAcol(1,0,2,3,2,0,1,3); } else { setColAcol(2,1,1,0,3,0,2,3); if (R > sigmaB) setColAcol(2,3,1,0,2,0,1,3); } if (idQ < 0) swapColAcol(); // Use reflected kinematics if gq initial state if (id1 == 21) swapTU = true; } //========================================================================== // Sigma2gg2gluinogluino // Cross section for gluino pair production from gg initial states // (validated against Pythia 6) //-------------------------------------------------------------------------- // Initialize process. void Sigma2gg2gluinogluino::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(1000021, 1000021); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat) - no incoming flavour dependence. void Sigma2gg2gluinogluino::sigmaKin() { // Modified Mandelstam variables for massive kinematics with m3 = m4. // tHG = tHat - m_gluino^2; uHG = uHat - m_gluino^2. double s34Avg = 0.5 * (s3 + s4) - 0.25 * pow2(s3 - s4) / sH; double tHG = -0.5 * (sH - tH + uH); double uHG = -0.5 * (sH + tH - uH); double tHG2 = tHG * tHG; double uHG2 = uHG * uHG; // Calculate kinematics dependence. sigTS = (tHG * uHG - 2. * s34Avg * (tHG + 2. * s34Avg)) / tHG2 + (tHG * uHG + s34Avg * (uHG - tHG)) / (sH * tHG); sigUS = (tHG * uHG - 2. * s34Avg * (uHG + 2. * s34Avg)) / uHG2 + (tHG * uHG + s34Avg * (tHG - uHG)) / (sH * uHG); sigTU = 2. * tHG * uHG / sH2 + s34Avg * (sH - 4. * s34Avg) / (tHG * uHG); sigSum = sigTS + sigUS + sigTU; // Answer contains factor 1/2 from identical gluinos. sigma = (M_PI / sH2) * pow2(alpS) * (9./4.) * 0.5 * sigSum * openFracPair; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2gg2gluinogluino::setIdColAcol() { // Flavours are trivial. setId( id1, id2, 1000021, 1000021); // Three colour flow topologies, each with two orientations. double sigRand = sigSum * rndmPtr->flat(); if (sigRand < sigTS) setColAcol( 1, 2, 2, 3, 1, 4, 4, 3); else if (sigRand < sigTS + sigUS) setColAcol( 1, 2, 3, 1, 3, 4, 4, 2); else setColAcol( 1, 2, 3, 4, 1, 4, 3, 2); if (rndmPtr->flat() > 0.5) swapColAcol(); } //========================================================================== // Sigma2qqbar2gluinogluino // Cross section for gluino pair production from qqbar initial states // (validated against Pythia 6 for SLHA1 case) //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2gluinogluino::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(1000021, 1000021); } //-------------------------------------------------------------------------- // Begin evaluate d(sigmaHat)/d(tHat); flavour-independent part. void Sigma2qqbar2gluinogluino::sigmaKin() { // Modified Mandelstam variables for massive kinematics with m3 = m4. // tHG = tHat - m_gluino^2; uHG = uHat - m_gluino^2. // (Note: tHG and uHG defined with opposite sign wrt Pythia 6) tHG = -0.5 * (sH - tH + uH); uHG = -0.5 * (sH + tH - uH); tHG2 = tHG * tHG; uHG2 = uHG * uHG; s34Avg = 0.5 * (s3 + s4) - 0.25 * pow2(s3 - s4) / sH; // s-channel gluon contribution (only used if id1 == -id2) // = Qss/s^2 in including 2N*(N^2-1)/N^2 color factor. sigS = 16./3. * (tHG2 + uHG2 + 2. * s34Avg * sH) / sH2; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2gluinogluino::sigmaHat() { // Only allow quark-antiquark incoming states if (id1 * id2 > 0) return 0.0; // In-pair must both be up-type or both down-type if ((id1+id2) % 2 != 0) return 0.0; // Flavor indices for the incoming quarks int iQA = (abs(id1)+1)/2; int iQB = (abs(id2)+1)/2; // Use up- or down-type squark-quark-gluino couplings complex LsqqG[7][4]; complex RsqqG[7][4]; for (int iSq=1; iSq<=6; ++iSq) { for (int iQ=1; iQ<=3; ++iQ) { if (abs(id1) % 2 == 1) { LsqqG[iSq][iQ] = coupSUSYPtr->LsddG[iSq][iQ]; RsqqG[iSq][iQ] = coupSUSYPtr->RsddG[iSq][iQ]; } else { LsqqG[iSq][iQ] = coupSUSYPtr->LsuuG[iSq][iQ]; RsqqG[iSq][iQ] = coupSUSYPtr->RsuuG[iSq][iQ]; } } } // sigHel contains (-1, 1), (1,-1), (-1,-1), ( 1, 1) // divided by 4 for helicity average vector sigHel; for (int iHel=0; iHel <4; ++iHel) sigHel.push_back(0.); // S-channel gluon contributions: only if id1 == -id2 (so iQA == iQB) if (abs(id1) == abs(id2)) { // S-channel squared sigHel[0] += sigS; sigHel[1] += sigS; } // T, U, and S/T/U interferences for (int iSq=1; iSq<=6; ++iSq) { int idSq = ((iSq+2)/3)*1000000 + 2*((iSq-1)%3) + abs(id1-1) % 2 + 1; double mSq2 = pow2(particleDataPtr->m0(idSq)); // Modified Mandelstam variables for massive kinematics with m3 = m4. // tHG = tHat - m_gluino^2; uHG = uHat - m_gluino^2. double tHsq = tHG + s34Avg - mSq2; double uHsq = uHG + s34Avg - mSq2; // ST and SU interferences: only if id1 == -id2 (so iQA == iQB) // incl 2N*(N^2 - 1)/N^2 color factor (note: original reference // was missing a factor 2 on the color factor here.) if ( abs(id1) == abs(id2) ) { double Qst1 = 16./3. * norm(LsqqG[iSq][iQA]) * (s34Avg * sH + tHG2); double Qsu1 = 16./3. * norm(LsqqG[iSq][iQA]) * (s34Avg * sH + uHG2); double Qst2 = 16./3. * norm(RsqqG[iSq][iQA]) * (s34Avg * sH + tHG2); double Qsu2 = 16./3. * norm(RsqqG[iSq][iQA]) * (s34Avg * sH + uHG2); double sigL = (Qst1 / tHsq + Qsu1 / uHsq) / sH; double sigR = (Qst2 / tHsq + Qsu2 / uHsq) / sH; sigHel[0] += sigL; sigHel[1] += sigR; } // T, U, and TU interferences for (int jSq=1; jSq<=6; ++jSq) { int idSqJ = ((jSq+2)/3)*1000000 + 2*((jSq-1)%3) + abs(id1-1) % 2 + 1; double mSqJ2 = pow2(particleDataPtr->m0(idSqJ)); // Modified Mandelstam variables for massive kinematics with m3 = m4. // tHG = tHat - m_gluino^2; uHG = uHat - m_gluino^2. double tHsqJ = tHG + s34Avg - mSqJ2; double uHsqJ = uHG + s34Avg - mSqJ2; double Q11 = real(LsqqG[iSq][iQA] * conj(LsqqG[iSq][iQB]) * conj(LsqqG[jSq][iQA]) * LsqqG[jSq][iQB]); double Q12 = real(LsqqG[iSq][iQA] * conj(RsqqG[iSq][iQB]) * conj(LsqqG[jSq][iQA]) * RsqqG[jSq][iQB]); double Q21 = real(RsqqG[iSq][iQA] * conj(LsqqG[iSq][iQB]) * conj(RsqqG[jSq][iQA]) * LsqqG[jSq][iQB]); double Q22 = real(RsqqG[iSq][iQA] * conj(RsqqG[iSq][iQB]) * conj(RsqqG[jSq][iQA]) * RsqqG[jSq][iQB]); double Qtt11 = 64./27. * Q11 * tHG2; double Qtt12 = 64./27. * Q12 * tHG2; double Qtt21 = 64./27. * Q21 * tHG2; double Qtt22 = 64./27. * Q22 * tHG2; double Quu11 = 64./27. * Q11 * uHG2; double Quu12 = 64./27. * Q12 * uHG2; double Quu21 = 64./27. * Q21 * uHG2; double Quu22 = 64./27. * Q22 * uHG2; double Qtu11 = 16./27. * Q11 * (s34Avg * sH); double Qtu12 = 16./27. * Q12 * (s34Avg * sH - tHG * uHG); double Qtu21 = 16./27. * Q21 * (s34Avg * sH - tHG * uHG); double Qtu22 = 16./27. * Q22 * (s34Avg * sH); // Cross sections for each helicity configuration (incl average fac 1/4) sigHel[0] += Qtt11 / tHsq / tHsqJ + Quu11 / uHsq / uHsqJ + Qtu11 / tHsq / uHsqJ; sigHel[1] += Qtt22 / tHsq / tHsqJ + Quu22 / uHsq / uHsqJ + Qtu22 / tHsq / uHsqJ; sigHel[2] += Qtt12 / tHsq / tHsqJ + Quu12 / uHsq / uHsqJ + Qtu12 / tHsq / uHsqJ; sigHel[3] += Qtt21 / tHsq / tHsqJ + Quu21 / uHsq / uHsqJ + Qtu21 / tHsq / uHsqJ; } } // Sum helicity contributions double sigSum = sigHel[0] + sigHel[1] + sigHel[2] + sigHel[3]; // Return 0 if all terms vanish, else compute and return cross section if ( sigSum <= 0. ) return 0.0; // Answer double sigma = (M_PI / 8. / sH2) * pow2(alpS) * sigSum * openFracPair; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2gluinogluino::setIdColAcol() { // Flavours are trivial. setId( id1, id2, 1000021, 1000021); // Two colour flow topologies. Swap if first is antiquark. if (rndmPtr->flat() < 0.5) setColAcol( 1, 0, 0, 2, 1, 3, 3, 2); else setColAcol( 1, 0, 0, 2, 3, 2, 1, 3); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma1qq2antisquark // R-parity violating squark production //-------------------------------------------------------------------------- // Initialise process void Sigma1qq2antisquark::initProc(){ //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; //Construct name of the process from lambda'' couplings nameSave = "q q' -> " + coupSUSYPtr->getName(idRes)+"* + c.c"; codeSave = 2000 + 10*abs(idRes)/1000000 + abs(idRes)%10; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma1qq2antisquark::sigmaKin() { // Check if at least one RPV coupling non-zero if(!coupSUSYPtr->isUDD) { sigBW = 0.0; return; } mRes = particleDataPtr->m0(abs(idRes)); GammaRes = particleDataPtr->mWidth(abs(idRes)); m2Res = pow2(mRes); sigBW = sH * GammaRes/ ( pow2(sH - m2Res) + pow2(mRes * GammaRes) ); sigBW *= 2.0/3.0/mRes; // Width out only includes open channels. widthOut = GammaRes * particleDataPtr->resOpenFrac(id3); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma1qq2antisquark::sigmaHat() { // Only allow (anti)quark-(anti)quark incoming states if (id1*id2 <= 0) return 0.0; // Generation indices int iA = (abs(id1)+1)/2; int iB = (abs(id2)+1)/2; //Covert from pdg-code to ~u_i/~d_i basis bool idown = (abs(idRes)%2 == 1) ? true : false; int iC = (abs(idRes)/1000000 == 2) ? (abs(idRes)%10+1)/2 + 3: (abs(idRes)%10+1)/2; // UDD structure if (abs(id1)%2 == 0 && abs(id2)%2 == 0) return 0.0; if (abs(id1)%2 == 1 && abs(id2)%2 == 1 && idown) return 0.0; if ((abs(id1) + abs(id2))%2 == 1 && !idown) return 0.0; double sigma = 0.0; if(!idown){ // d_i d_j --> ~u*_k for(int isq = 1; isq <=3; isq++){ // Loop over R-type squark contributions sigma += pow2(coupSUSYPtr->rvUDD[isq][iA][iB]) * norm(coupSUSYPtr->Rusq[iC][isq+3]); } }else{ // u_i d_j --> d*_k // Pick the correct coupling for d-u in-state if(abs(id1)%2==1){ iA = (abs(id2)+1)/2; iB = (abs(id1)+1)/2; } for(int isq = 1; isq <= 3; isq++){ // Loop over R-type squark contributions sigma += pow2(coupSUSYPtr->rvUDD[iA][iB][isq]) * norm(coupSUSYPtr->Rdsq[iC][isq+3]); } } sigma *= sigBW; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1qq2antisquark::setIdColAcol() { // Set flavours. if(id1 < 0 && id2 < 0 ) setId( id1, id2, idRes); else setId( id1, id2, -idRes); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 2, 0, 0, 3); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2chi0gluino // Cross section for gaugino pair production: neutralino-gluino //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2chi0gluino::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Construct name of process. nameSave = "q qbar' -> " + particleDataPtr->name(id3) + " " + particleDataPtr->name(id4); // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(id3, id4); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2chi0gluino::sigmaKin() { // Common flavour-independent factor. sigma0 = M_PI * 4.0 / 9.0/ sH2 / coupSUSYPtr->sin2W * alpEM * alpS * openFracPair; // Auxiliary factors for use below ui = uH - s3; uj = uH - s4; ti = tH - s3; tj = tH - s4; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2chi0gluino::sigmaHat() { // Only allow quark-antiquark incoming states if (id1*id2 >= 0) return 0.0; // In-pair must both be up-type or both down-type if ((id1+id2) % 2 != 0) return 0.0; // Swap T and U if antiquark-quark instead of quark-antiquark if (id1<0) swapTU = true; // Shorthands int idAbs1 = abs(id1); int idAbs2 = abs(id2); // Flavour-dependent kinematics-dependent couplings. complex QuLL(0.0),QtLL(0.0),QuRR(0.0),QtRR(0.0); complex QuLR(0.0),QtLR(0.0),QuRL(0.0),QtRL(0.0); // Flavour indices int ifl1 = (idAbs1+1) / 2; int ifl2 = (idAbs2+1) / 2; complex (*LsddXloc)[4][6]; complex (*RsddXloc)[4][6]; complex (*LsuuXloc)[4][6]; complex (*RsuuXloc)[4][6]; LsddXloc = coupSUSYPtr->LsddX; RsddXloc = coupSUSYPtr->RsddX; LsuuXloc = coupSUSYPtr->LsuuX; RsuuXloc = coupSUSYPtr->RsuuX; // Add t-channel squark flavour sums to QmXY couplings for (int ksq=1; ksq<=6; ksq++) { // squark id and squark-subtracted u and t int idsq; idsq=((ksq+2)/3)*1000000 + 2*((ksq-1) % 3) + (idAbs1+1) % 2 + 1; double msq2 = pow(particleDataPtr->m0(idsq),2); double usq = uH - msq2; double tsq = tH - msq2; complex Lsqq1X4; complex Lsqq2X4; complex Rsqq1X4; complex Rsqq2X4; complex Lsqq1G; complex Rsqq1G; complex Lsqq2G; complex Rsqq2G; // Couplings Lsqq1X4 = LsuuXloc[ksq][ifl1][id4chi]; Lsqq2X4 = LsuuXloc[ksq][ifl2][id4chi]; Rsqq1X4 = RsuuXloc[ksq][ifl1][id4chi]; Rsqq2X4 = RsuuXloc[ksq][ifl2][id4chi]; Lsqq1G = coupSUSYPtr->LsuuG[ksq][ifl1]; Rsqq1G = coupSUSYPtr->RsuuG[ksq][ifl1]; Lsqq2G = coupSUSYPtr->LsuuG[ksq][ifl2]; Rsqq2G = coupSUSYPtr->RsuuG[ksq][ifl2]; if (idAbs1 % 2 != 0) { Lsqq1X4 = LsddXloc[ksq][ifl1][id4chi]; Lsqq2X4 = LsddXloc[ksq][ifl2][id4chi]; Rsqq1X4 = RsddXloc[ksq][ifl1][id4chi]; Rsqq2X4 = RsddXloc[ksq][ifl2][id4chi]; Lsqq1G = coupSUSYPtr->LsddG[ksq][ifl1]; Rsqq1G = coupSUSYPtr->RsddG[ksq][ifl1]; Lsqq2G = coupSUSYPtr->LsddG[ksq][ifl2]; Rsqq2G = coupSUSYPtr->RsddG[ksq][ifl2]; } // QuXY QuLL += conj(Lsqq1X4)*Lsqq2G/usq; QuRR += conj(Rsqq1X4)*Rsqq2G/usq; QuLR += conj(Lsqq1X4)*Rsqq2G/usq; QuRL += conj(Rsqq1X4)*Lsqq2G/usq; // QtXY QtLL -= conj(Lsqq1G)*Lsqq2X4/tsq; QtRR -= conj(Rsqq1G)*Rsqq2X4/tsq; QtLR += conj(Lsqq1G)*Rsqq2X4/tsq; QtRL += conj(Rsqq1G)*Lsqq2X4/tsq; } // Overall factor multiplying coupling double fac = (1.0-coupSUSYPtr->sin2W); // Compute matrix element weight double weight = 0; double facLR = uH*tH - s3*s4; double facMS = m3*m4*sH; // Average over separate helicity contributions // LL (ha = -1, hb = +1) (divided by 4 for average) weight += norm(QuLL) * ui * uj + norm(QtLL) * ti * tj + 2 * real(conj(QuLL) * QtLL) * facMS; // RR (ha = 1, hb = -1) (divided by 4 for average) weight += norm(QtRR) * ti * tj + norm(QuRR) * ui * uj + 2 * real(conj(QuRR) * QtRR) * facMS; // RL (ha = 1, hb = 1) (divided by 4 for average) weight += norm(QuRL) * ui * uj + norm(QtRL) * ti * tj + real(conj(QuRL) * QtRL) * facLR; // LR (ha = -1, hb = -1) (divided by 4 for average) weight += norm(QuLR) * ui * uj + norm(QtLR) * ti * tj + real(conj(QuLR) * QtLR) * facLR; // Cross section, including colour factor. double sigma = sigma0 * weight / fac; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2chi0gluino::setIdColAcol() { // Set flavours. setId( id1, id2, id3, id4); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 1, 2, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2chargluino // Cross section for gaugino pair production: chargino-gluino //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2chargluino::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Construct name of process. nameSave = "q qbar' -> " + particleDataPtr->name(id3) + " " + particleDataPtr->name(id4) + " + c.c"; // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(id3, id4); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2chargluino::sigmaKin() { // Common flavour-independent factor. sigma0 = M_PI / sH2 * 4.0 / 9.0 / coupSUSYPtr->sin2W * alpEM * alpS ; sigma0 /= 2.0 * (1 - coupSUSYPtr->sin2W) ; // Auxiliary factors for use below ui = uH - s3; uj = uH - s4; ti = tH - s3; tj = tH - s4; } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2chargluino::sigmaHat() { // Only allow particle-antiparticle incoming states if (id1*id2 >= 0) return 0.0; // Only allow incoming states with sum(charge) = final state if (abs(id1) % 2 == abs(id2) % 2) return 0.0; int isPos = (id4chi > 0 ? 1 : 0); if (id1 < 0 && id1 > -19 && abs(id1) % 2 == 1-isPos ) return 0.0; else if (id1 > 0 && id1 < 19 && abs(id1) % 2 == isPos ) return 0.0; // Flavour-dependent kinematics-dependent couplings. int idAbs1 = abs(id1); int iChar = abs(id4chi); complex QuLL(0.0),QtLL(0.0),QuRR(0.0),QtRR(0.0); complex QuLR(0.0),QtLR(0.0),QuRL(0.0),QtRL(0.0); // Calculate everything from udbar -> ~chi+ ~chi0 template process complex LsddGl; complex RsddGl; complex LsuuGl; complex RsuuGl; complex (*LsduXloc)[4][3]; complex (*RsduXloc)[4][3]; complex (*LsudXloc)[4][3]; complex (*RsudXloc)[4][3]; LsduXloc = coupSUSYPtr->LsduX; RsduXloc = coupSUSYPtr->RsduX; LsudXloc = coupSUSYPtr->LsudX; RsudXloc = coupSUSYPtr->RsudX; // u dbar , ubar d : do nothing // dbar u , d ubar : swap 1<->2 and t<->u int iGu = abs(id1)/2; int iGd = (abs(id2)+1)/2; if (idAbs1 % 2 != 0) { swapTU = true; iGu = abs(id2)/2; iGd = (abs(id1)+1)/2; } // Add t-channel squark flavour sums to QmXY couplings for (int jsq=1; jsq<=6; jsq++) { int idsu=((jsq+2)/3)*1000000 + 2*((jsq-1) % 3) + 2 ; int idsd=((jsq+2)/3)*1000000 + 2*((jsq-1) % 3) + 1 ; LsddGl = coupSUSYPtr->LsddG[jsq][iGd]; RsddGl = coupSUSYPtr->RsddG[jsq][iGd]; LsuuGl = coupSUSYPtr->LsuuG[jsq][iGu]; RsuuGl = coupSUSYPtr->RsuuG[jsq][iGu]; double msd2 = pow(particleDataPtr->m0(idsd),2); double msu2 = pow(particleDataPtr->m0(idsu),2); double tsq = tH - msd2; double usq = uH - msu2; QuLL += conj(LsuuGl) * conj(LsudXloc[jsq][iGd][iChar])/usq; QuLR += conj(LsuuGl) * conj(RsudXloc[jsq][iGd][iChar])/usq; QuRR += conj(RsuuGl) * conj(RsudXloc[jsq][iGd][iChar])/usq; QuRL += conj(RsuuGl) * conj(LsudXloc[jsq][iGd][iChar])/usq; QtLL -= conj(LsduXloc[jsq][iGu][iChar]) * LsddGl/tsq; QtRR -= conj(RsduXloc[jsq][iGu][iChar]) * RsddGl/tsq; QtLR += conj(LsduXloc[jsq][iGu][iChar]) * RsddGl/tsq; QtRL += conj(RsduXloc[jsq][iGu][iChar]) * LsddGl/tsq; } // Compute matrix element weight double weight = 0; // Average over separate helicity contributions // (if swapped, swap ha, hb if computing polarized cross sections) // LL (ha = -1, hb = +1) (divided by 4 for average) weight += norm(QuLL) * ui * uj + norm(QtLL) * ti * tj + 2 * real(conj(QuLL) * QtLL) * m3 * m4 * sH; // RR (ha = 1, hb = -1) (divided by 4 for average) weight += norm(QtRR) * ti * tj + norm(QuRR) * ui * uj + 2 * real(conj(QuRR) * QtRR) * m3 * m4 * sH; // RL (ha = 1, hb = 1) (divided by 4 for average) weight += norm(QuRL) * ui * uj + norm(QtRL) * ti * tj + real(conj(QuRL) * QtRL) * (uH * tH - s3 * s4); // LR (ha = -1, hb = -1) (divided by 4 for average) weight += norm(QuLR) * ui * uj + norm(QtLR) * ti * tj + real(conj(QuLR) * QtLR) * (uH * tH - s3 * s4); // Cross section, including colour factor. double sigma = sigma0 * weight; // Answer. return sigma; } //-------------------------------------------------------------------------- void Sigma2qqbar2chargluino::setIdColAcol() { // Set flavours. setId( id1, id2, id3, id4); // Colour flow topologies. Swap when antiquarks. setColAcol( 1, 0, 0, 2, 1, 2, 0, 0); if (id1 < 0) swapColAcol(); } //========================================================================== // Sigma2qqbar2sleptonantislepton // Cross section for qqbar-initiated slepton-antislepton production //-------------------------------------------------------------------------- // Initialize process. void Sigma2qqbar2sleptonantislepton::initProc() { //Typecast to the correct couplings coupSUSYPtr = (CoupSUSY*) couplingsPtr; // Is this a ~u_i ~d*_j, ~d_i ~u*_j final state or ~d_i ~d*_j, ~u_i ~u*_j if (abs(id3Sav) % 2 == abs(id4Sav) % 2) isUD = false; else isUD = true; // Derive name nameSave = "q qbar' -> "+particleDataPtr->name(abs(id3Sav))+" "+ particleDataPtr->name(-abs(id4Sav)); if (isUD) nameSave +=" + c.c."; // Extract isospin and mass-ordering indices if(isUD && abs(id3Sav)%2 == 0) { // Make sure iGen3 is always slepton and iGen4 is always sneutrino iGen3 = 3*(abs(id4Sav)/2000000) + (abs(id4Sav)%10+1)/2; iGen4 = 3*(abs(id3Sav)/2000000) + (abs(id3Sav)%10+1)/2; } else { iGen3 = 3*(abs(id3Sav)/2000000) + (abs(id3Sav)%10+1)/2; iGen4 = 3*(abs(id4Sav)/2000000) + (abs(id4Sav)%10+1)/2; } // Count 5 neutralinos in NMSSM nNeut = (coupSUSYPtr->isNMSSM ? 5 : 4); // Store mass squares of all possible internal propagator lines; // retained for future extension to leptonic initial states m2Neut.resize(nNeut+1); for (int iNeut=1;iNeut<=nNeut;iNeut++) m2Neut[iNeut] = pow2(particleDataPtr->m0(coupSUSYPtr->idNeut(iNeut))); // Set sizes of some arrays to be used below tNeut.resize(nNeut+1); uNeut.resize(nNeut+1); // Shorthand for Weak mixing xW = coupSUSYPtr->sin2W; // Secondary open width fraction. openFracPair = particleDataPtr->resOpenFrac(id3Sav, id4Sav); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), part independent of incoming flavour. void Sigma2qqbar2sleptonantislepton::sigmaKin() { // Z/W propagator if (! isUD) { double sV= sH - pow2(coupSUSYPtr->mZpole); double d = pow2(sV) + pow2(coupSUSYPtr->mZpole * coupSUSYPtr->wZpole); propZW = complex( sV / d, coupSUSYPtr->mZpole * coupSUSYPtr->wZpole / d); } else { double sV= sH - pow2(coupSUSYPtr->mWpole); double d = pow2(sV) + pow2(coupSUSYPtr->mWpole * coupSUSYPtr->wWpole); propZW = complex( sV / d, coupSUSYPtr->mWpole * coupSUSYPtr->wWpole / d); } // Flavor-independent pre-factors double comFacHat = M_PI/sH2 * openFracPair; sigmaEW = comFacHat * pow2(alpEM); } //-------------------------------------------------------------------------- // Evaluate d(sigmaHat)/d(tHat), including incoming flavour dependence. double Sigma2qqbar2sleptonantislepton::sigmaHat() { // In-pair must be opposite-sign if (id1 * id2 > 0) return 0.0; // Check correct charge sum if (isUD && abs(id1) %2 == abs(id2) % 2) return 0.0; if (!isUD && abs(id1) % 2 != abs(id2) % 2) return 0.0; // No RH sneutrinos if ( (abs(id3)%2 == 0 && abs(id3) > 2000000) || (abs(id4)%2 == 0 && abs(id4) > 2000000) ) return 0.0; // Coded UD sigma is for udbar -> ~v~l'*. Swap t<->u for dbaru -> ~l~v*. swapTU = (isUD && abs(id1) % 2 != 0); // Coded QQ sigma is for qqbar -> ~l~l*. Swap t<->u for qbarq -> ~l~l*. if (!isUD && id1 < 0) swapTU = true; // Generation indices of incoming particles int idIn1A = (swapTU) ? abs(id2) : abs(id1); int idIn2A = (swapTU) ? abs(id1) : abs(id2); int iGen1 = (idIn1A+1)/2; int iGen2 = (idIn2A+1)/2; // Auxiliary factors for use below for (int i=1; i<= nNeut; i++) { tNeut[i] = tH - m2Neut[i]; uNeut[i] = uH - m2Neut[i]; } double eQ = (idIn1A % 2 == 0) ? 2./3. : -1./3. ; double eSl = (abs(id3Sav) % 2 == 0) ? 0. : -1. ; // Initial values for pieces used for color-flow selection below sumColS = 0.0; sumColT = 0.0; sumInterference = 0.0; // Common factor for LR and RL contributions double facTU = uH*tH-s3*s4; // Opposite-isospin: udbar -> ~l~v* if ( isUD ) { // s-channel W contribution (only contributes to LL helicities) sumColS = sigmaEW / 32.0 / pow2(xW) / pow2(1.0-xW) * norm(conj(coupSUSYPtr->LudW[iGen1][iGen2]) * coupSUSYPtr->LslsvW[iGen3][iGen4]) * facTU * norm(propZW); } double CslZ; // s-channel Z/photon and interference if (abs(id1) == abs(id2)) { CslZ = real(coupSUSYPtr->LslslZ[iGen3][iGen4] + coupSUSYPtr->RslslZ[iGen3][iGen4]); if (abs(id3)%2 == 0) CslZ = real(coupSUSYPtr->LsvsvZ[iGen3][iGen4] + coupSUSYPtr->RsvsvZ[iGen3][iGen4]); // gamma // Factor 2 since contributes to both ha != hb helicities sumColS += (abs(CslZ) > 0.0) ? 2. * pow2(eQ) * pow2(eSl) * sigmaEW * facTU / pow2(sH): 0.0; // Z/gamma interference sumInterference += eQ * eSl * sigmaEW * facTU / 2.0 / xW / (1.-xW) * sqrt(norm(propZW)) / sH * CslZ * (coupSUSYPtr->LqqZ[idIn1A] + coupSUSYPtr->RqqZ[idIn1A]); // s-channel Z CslZ = norm(coupSUSYPtr->LslslZ[iGen3][iGen4] + coupSUSYPtr->RslslZ[iGen3][iGen4]); if (abs(id3Sav)%2 == 0) CslZ = norm(coupSUSYPtr->LsvsvZ[iGen3][iGen4] + coupSUSYPtr->RsvsvZ[iGen3][iGen4]); sumColS += sigmaEW * facTU / 16.0 / pow2(xW) / pow2(1.0-xW) * norm(propZW) * CslZ * ( pow2(coupSUSYPtr->LqqZ[idIn1A]) + pow2(coupSUSYPtr->RqqZ[idIn1A]) ); } // Cross section double sigma = sumColS + sumColT + sumInterference; // Colour average if(abs(id1) < 10) sigma /= 3.0; // Add cc term if(isUD) sigma *= 2.0; // Return answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2qqbar2sleptonantislepton::setIdColAcol() { // Set flavours. int iSl, iSv; if( isUD ){ iSl = (abs(id3)%2 == 0) ? abs(id3) : abs(id4); iSv = (abs(id3)%2 == 0) ? abs(id4) : abs(id3); if ((id1%2 + id2%2 ) > 0) setId( id1, id2, -iSl, iSv); else setId( id1, id2, iSl, -iSv); } else setId( id1, id2, abs(id3), -abs(id4)); setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); if (id1 < 0 ) swapColAcol(); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SigmaLeftRightSym.cc0000644000175000017500000006415112217346251017003 0ustar sunsun// SigmaLeftRightSym.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // left-right-symmetry simulation classes. #include "Pythia8/SigmaLeftRightSym.h" namespace Pythia8 { //========================================================================== // Sigma1ffbar2ZRight class. // Cross section for f fbar -> Z_R^0 (righthanded gauge boson). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2ZRight::initProc() { // Store Z_R mass and width for propagator. idZR = 9900023; mRes = particleDataPtr->m0(idZR); GammaRes = particleDataPtr->mWidth(idZR); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; sin2tW = couplingsPtr->sin2thetaW(); // Set pointer to particle properties and decay table. ZRPtr = particleDataPtr->particleDataEntryPtr(idZR); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1ffbar2ZRight::sigmaKin() { // Set up Breit-Wigner. Width out only includes open channels. double sigBW = 12. * M_PI/ ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); double widthOut = ZRPtr->resWidthOpen(idZR, mH); // Prefactor for incoming widths. Combine. Done. double preFac = alpEM * mH / ( 48. * sin2tW * (1. - sin2tW) * (1. - 2. * sin2tW) ); sigma0 = preFac * sigBW * widthOut; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma1ffbar2ZRight::sigmaHat() { // Vector and axial couplings of incoming fermion pair. int idAbs = abs(id1); double af = 0.; double vf = 0.; if (idAbs < 9 && idAbs%2 == 1) { af = -1. + 2. * sin2tW; vf = -1. + 4. * sin2tW / 3.; } else if (idAbs < 9) { af = 1. - 2. * sin2tW; vf = 1. - 8. * sin2tW / 3.; } else if (idAbs < 19 && idAbs%2 == 1) { af = -1. + 2. * sin2tW; vf = -1. + 4. * sin2tW; } // Colour factor. Answer. double sigma = (vf*vf + af*af) * sigma0; if (idAbs < 9) sigma /= 3.; return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2ZRight::setIdColAcol() { // Flavours trivial. setId( id1, id2, idZR); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for Z_R decay angle. double Sigma1ffbar2ZRight::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Z_R should sit in entry 5. if (iResBeg != 5 || iResEnd != 5) return 1.; // Couplings for in- and out-flavours. double ai, vi, af, vf; int idInAbs = process[3].idAbs(); if (idInAbs < 9 && idInAbs%2 == 1) { ai = -1. + 2. * sin2tW; vi = -1. + 4. * sin2tW / 3.; } else if (idInAbs < 9) { ai = 1. - 2. * sin2tW; vi = 1. - 8. * sin2tW / 3.; } else { ai = -1. + 2. * sin2tW; vi = -1. + 4. * sin2tW; } int idOutAbs = process[6].idAbs(); if (idOutAbs < 9 && idOutAbs%2 == 1) { af = -1. + 2. * sin2tW; vf = -1. + 4. * sin2tW / 3.; } else if (idOutAbs < 9) { af = 1. - 2. * sin2tW; vf = 1. - 8. * sin2tW / 3.; } else { af = -1. + 2. * sin2tW; vf = -1. + 4. * sin2tW; } // Phase space factors. Reconstruct decay angle. double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double betaf = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * betaf); // Angular weight and its maximum. double wt1 = (vi*vi + ai*ai) * (vf*vf + af*af * betaf*betaf); double wt2 = (1. - betaf*betaf) * (vi*vi + ai*ai) * vf*vf; double wt3 = betaf * 4. * vi * ai * vf * af; if (process[3].id() * process[6].id() < 0) wt3 = -wt3; double wt = wt1 * (1. + cosThe*cosThe) + wt2 * (1. - cosThe*cosThe) + 2. * wt3 * cosThe; double wtMax = 2. * (wt1 + abs(wt3)); // Done. return wt / wtMax; } //========================================================================== // Sigma1ffbar2WRight class. // Cross section for f fbar' -> W_R^+- (righthanded gauge boson). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ffbar2WRight::initProc() { // Store W_R^+- mass and width for propagator. idWR = 9900024; mRes = particleDataPtr->m0(idWR); GammaRes = particleDataPtr->mWidth(idWR); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; thetaWRat = 1. / (12. * couplingsPtr->sin2thetaW()); // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(idWR); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma1ffbar2WRight::sigmaKin() { // Common coupling factors. double colQ = 3. * (1. + alpS / M_PI); // Reset quantities to sum. Declare variables inside loop. double widOutPos = 0.; double widOutNeg = 0.; int id1Now, id2Now, id1Abs, id2Abs, id1Neg, id2Neg, onMode; double widNow, widSecPos, widSecNeg, mf1, mf2, mr1, mr2, kinFac; // Loop over all W_R^+- decay channels. for (int i = 0; i < particlePtr->sizeChannels(); ++i) { id1Now = particlePtr->channel(i).product(0); id2Now = particlePtr->channel(i).product(1); id1Abs = abs(id1Now); id2Abs = abs(id2Now); // Check that above threshold. Phase space. mf1 = particleDataPtr->m0(id1Abs); mf2 = particleDataPtr->m0(id2Abs); if (mH > mf1 + mf2 + MASSMARGIN) { mr1 = pow2(mf1 / mH); mr2 = pow2(mf2 / mH); kinFac = (1. - 0.5 * (mr1 + mr2) - 0.5 * pow2(mr1 - mr2)) * sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2 ); // Combine kinematics with colour factor and CKM couplings. widNow = kinFac; if (id1Abs < 9) widNow *= colQ * couplingsPtr->V2CKMid(id1Abs, id2Abs); // Secondary width from top and righthanded neutrino decay. id1Neg = (id1Abs < 19) ? -id1Now : id1Abs; id2Neg = (id2Abs < 19) ? -id2Now : id2Abs; widSecPos = particleDataPtr->resOpenFrac(id1Now, id2Now); widSecNeg = particleDataPtr->resOpenFrac(id1Neg, id2Neg); // Add weight for channels on for all, W_R^+ and W_R^-, respectively. onMode = particlePtr->channel(i).onMode(); if (onMode == 1 || onMode == 2) widOutPos += widNow * widSecPos; if (onMode == 1 || onMode == 3) widOutNeg += widNow * widSecNeg; // End loop over fermions. } } // Set up Breit-Wigner. Cross section for W_R^+ and W_R^- separately. double sigBW = 12. * M_PI * pow2(alpEM * thetaWRat) * sH / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); sigma0Pos = sigBW * widOutPos; sigma0Neg = sigBW * widOutNeg; } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma1ffbar2WRight::sigmaHat() { // Secondary width for W_R^+ or W_R^-. CKM and colour factors. int idUp = (abs(id1)%2 == 0) ? id1 : id2; double sigma = (idUp > 0) ? sigma0Pos : sigma0Neg; if (abs(id1) < 9) sigma *= couplingsPtr->V2CKMid(abs(id1), abs(id2)) / 3.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ffbar2WRight::setIdColAcol() { // Sign of outgoing W_R. int sign = (abs(id1)%2 == 0) ? 1 : -1; if (id1 < 0) sign = -sign; setId( id1, id2, idWR * sign); // Colour flow topologies. Swap when antiquarks. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for W_R decay angle. double Sigma1ffbar2WRight::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // W_R should sit in entry 5. if (iResBeg != 5 || iResEnd != 5) return 1.; // Phase space factors. double mr1 = pow2(process[6].m()) / sH; double mr2 = pow2(process[7].m()) / sH; double betaf = sqrtpos( pow2(1. - mr1 - mr2) - 4. * mr1 * mr2); // Sign of asymmetry. double eps = (process[3].id() * process[6].id() > 0) ? 1. : -1.; // Reconstruct decay angle and weight for it. double cosThe = (process[3].p() - process[4].p()) * (process[7].p() - process[6].p()) / (sH * betaf); double wtMax = 4.; double wt = pow2(1. + betaf * eps * cosThe) - pow2(mr1 - mr2); // Done. return (wt / wtMax); } //========================================================================== // Sigma1ll2Hchgchg class. // Cross section for l l -> H_L^++-- or H_R^++-- (doubly charged Higgs). //-------------------------------------------------------------------------- // Initialize process. void Sigma1ll2Hchgchg::initProc() { // Set process properties: H_L^++-- or H_R^++--. if (leftRight == 1) { idHLR = 9900041; codeSave = 3121; nameSave = "l l -> H_L^++--"; } else { idHLR = 9900042; codeSave = 3141; nameSave = "l l -> H_R^++--"; } // Read in Yukawa matrix for couplings to a lepton pair. yukawa[1][1] = settingsPtr->parm("LeftRightSymmmetry:coupHee"); yukawa[2][1] = settingsPtr->parm("LeftRightSymmmetry:coupHmue"); yukawa[2][2] = settingsPtr->parm("LeftRightSymmmetry:coupHmumu"); yukawa[3][1] = settingsPtr->parm("LeftRightSymmmetry:coupHtaue"); yukawa[3][2] = settingsPtr->parm("LeftRightSymmmetry:coupHtaumu"); yukawa[3][3] = settingsPtr->parm("LeftRightSymmmetry:coupHtautau"); // Store H_L/R mass and width for propagator. mRes = particleDataPtr->m0(idHLR); GammaRes = particleDataPtr->mWidth(idHLR); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; // Set pointer to particle properties and decay table. particlePtr = particleDataPtr->particleDataEntryPtr(idHLR); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma1ll2Hchgchg::sigmaHat() { // Initial state must consist of two identical-sign leptons. if (id1 * id2 < 0) return 0.; int id1Abs = abs(id1); int id2Abs = abs(id2); if (id1Abs != 11 && id1Abs != 13 && id1Abs != 15) return 0.; if (id2Abs != 11 && id2Abs != 13 && id2Abs != 15) return 0.; // Set up Breit-Wigner, inwidth and outwidth. double sigBW = 8. * M_PI / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); double widIn = pow2(yukawa[(id1Abs-9)/2][(id2Abs-9)/2]) * mH / (8. * M_PI); int idSgn = (id1 < 0) ? idHLR : -idHLR; double widOut = particlePtr->resWidthOpen( idSgn, mH); // Answer. return widIn * sigBW * widOut; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma1ll2Hchgchg::setIdColAcol() { // Sign of outgoing H_L/R. int idSgn = (id1 < 0) ? idHLR : -idHLR; setId( id1, id2, idSgn); // No colours whatsoever. setColAcol( 0, 0, 0, 0, 0, 0); } //-------------------------------------------------------------------------- // Evaluate weight for H_L/R sequential decay angles. double Sigma1ll2Hchgchg::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else isotropic decay. return 1.; } //========================================================================== // Sigma2lgm2Hchgchgl class. // Cross section for l gamma -> H_L^++-- l or H_R^++-- l // (doubly charged Higgs). //-------------------------------------------------------------------------- // Initialize process. void Sigma2lgm2Hchgchgl::initProc() { // Set process properties: H_L^++-- or H_R^++-- and e/mu/tau. idHLR = (leftRight == 1) ? 9900041 : 9900042; codeSave = (leftRight == 1) ? 3122 : 3142; if (idLep == 13) codeSave += 2; if (idLep == 15) codeSave += 4; if (codeSave == 3122) nameSave = "l^+- gamma -> H_L^++-- e^-+"; else if (codeSave == 3123) nameSave = "l^+- gamma -> H_L^++-- mu^-+"; else if (codeSave == 3124) nameSave = "l^+- gamma -> H_L^++-- tau^-+"; else if (codeSave == 3142) nameSave = "l^+- gamma -> H_R^++-- e^-+"; else if (codeSave == 3143) nameSave = "l^+- gamma -> H_R^++-- mu^-+"; else nameSave = "l^+- gamma -> H_R^++-- tau^-+"; // Read in relevantYukawa matrix for couplings to a lepton pair. if (idLep == 11) { yukawa[1] = settingsPtr->parm("LeftRightSymmmetry:coupHee"); yukawa[2] = settingsPtr->parm("LeftRightSymmmetry:coupHmue"); yukawa[3] = settingsPtr->parm("LeftRightSymmmetry:coupHtaue"); } else if (idLep == 13) { yukawa[1] = settingsPtr->parm("LeftRightSymmmetry:coupHmue"); yukawa[2] = settingsPtr->parm("LeftRightSymmmetry:coupHmumu"); yukawa[3] = settingsPtr->parm("LeftRightSymmmetry:coupHtaumu"); } else { yukawa[1] = settingsPtr->parm("LeftRightSymmmetry:coupHtaue"); yukawa[2] = settingsPtr->parm("LeftRightSymmmetry:coupHtaumu"); yukawa[3] = settingsPtr->parm("LeftRightSymmmetry:coupHtautau"); } // Secondary open width fractions. openFracPos = particleDataPtr->resOpenFrac( idHLR); openFracNeg = particleDataPtr->resOpenFrac(-idHLR); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma2lgm2Hchgchgl::sigmaHat() { // Initial state must consist of a lepton and a photon. int idIn = (id2 == 22) ? id1 : id2; int idInAbs = abs(idIn); if (idInAbs != 11 && idInAbs != 13 && idInAbs != 15) return 0.; // Incoming squared lepton mass. double s1 = pow2( particleDataPtr->m0(idInAbs) ); // Kinematical expressions. double smm1 = 8. * (sH + tH - s3) * (sH + tH - 2. * s3 - s1 - s4) / pow2(uH - s3); double smm2 = 2. * ( (2. * s3 - 3. * s1) * s4 + (s1 - 2. * s4) * tH - (tH - s4) * sH ) / pow2(tH - s4); double smm3 = 2. * ( (2. * s3 - 3. * s4 + tH) * s1 - (2. * s1 - s4 + tH) * sH ) / pow2(sH - s1); double smm12 = 4. * ( (2. * s1 - s4 - 2. * s3 + tH) * sH + (tH - 3. * s3 - 3. * s4) * tH + (2. * s3 - 2. * s1 + 3. * s4) * s3 ) / ( (uH - s3) * (tH - s4) ); double smm13 = -4. * ( (tH + s1 - 2. * s4) * tH - (s3 + 3. * s1 - 2. * s4) * s3 + (s3 + 3. * s1 + tH) * sH - pow2(tH - s3 + sH) ) / ( (uH - s3) * (sH - s1) ); double smm23 = -4. * ( (s1 - s4 + s3) * tH - s3*s3 + s3 * (s1 + s4) - 3. * s1 * s4 - (s1 - s4 - s3 + tH) * sH) / ( (sH - s1) * (tH - s4) ); double sigma = alpEM * pow2(sH / (sH - s1) ) * (smm1 + smm2 + smm3 + smm12 + smm13 + smm23) / (4. * sH2); // Lepton Yukawa and secondary widths. sigma *= pow2(yukawa[(idInAbs-9)/2]); sigma *= (idIn < 0) ? openFracPos : openFracNeg; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2lgm2Hchgchgl::setIdColAcol() { // Sign of outgoing H_L/R. int idIn = (id2 == 22) ? id1 : id2; int idSgn = (idIn < 0) ? idHLR : -idHLR; int idOut = (idIn < 0) ? idLep : -idLep; setId( id1, id2, idSgn, idOut); // tHat is defined between incoming lepton and outgoing Higgs. if (id1 == 22) swapTU = true; // No colours whatsoever. setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); } //-------------------------------------------------------------------------- // Evaluate weight for H_L/R sequential decay angles. double Sigma2lgm2Hchgchgl::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else isotropic decay. return 1.; } //========================================================================== // Sigma3ff2HchgchgfftWW class. // Cross section for f_1 f_2 -> H_(L/R)^++-- f_3 f_4 (W+- W+- fusion). //-------------------------------------------------------------------------- // Initialize process. void Sigma3ff2HchgchgfftWW::initProc() { // Set process properties: H_L^++-- or H_R^++--. if (leftRight == 1) { idHLR = 9900041; codeSave = 3125; nameSave = "f_1 f_2 -> H_L^++-- f_3 f_4 (W+- W+- fusion)"; } else { idHLR = 9900042; codeSave = 3145; nameSave = "f_1 f_2 -> H_R^++-- f_3 f_4 (W+- W+- fusion)"; } // Common fixed mass and coupling factor. double mW = particleDataPtr->m0(24); double mWR = particleDataPtr->m0(9900024); mWS = (leftRight == 1) ? pow2(mW) : pow2(mWR); double gL = settingsPtr->parm("LeftRightSymmmetry:gL"); double gR = settingsPtr->parm("LeftRightSymmmetry:gR"); double vL = settingsPtr->parm("LeftRightSymmmetry:vL"); prefac = (leftRight == 1) ? pow2(pow4(gL) * vL) : 2. * pow2(pow3(gR) * mWR); // Secondary open width fractions. openFracPos = particleDataPtr->resOpenFrac( idHLR); openFracNeg = particleDataPtr->resOpenFrac(-idHLR); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), part independent of incoming flavour. void Sigma3ff2HchgchgfftWW::sigmaKin() { // Required four-vector products. double pp12 = 0.5 * sH; double pp14 = 0.5 * mH * p4cm.pNeg(); double pp15 = 0.5 * mH * p5cm.pNeg(); double pp24 = 0.5 * mH * p4cm.pPos(); double pp25 = 0.5 * mH * p5cm.pPos(); double pp45 = p4cm * p5cm; // Cross section: kinematics part. Combine with couplings. double propT = 1. / ( (2. * pp14 + mWS) * (2. * pp25 + mWS) ); double propU = 1. / ( (2. * pp24 + mWS) * (2. * pp15 + mWS) ); sigma0TU = prefac * pp12 * pp45 * pow2(propT + propU); sigma0T = prefac * pp12 * pp45 * 2. * pow2(propT); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma3ff2HchgchgfftWW::sigmaHat() { // Do not allow creation of righthanded neutrinos for H_R. int id1Abs = abs(id1); int id2Abs = abs(id2); if ( leftRight == 2 && (id1Abs > 10 || id2Abs > 10) ) return 0.; // Many flavour combinations not possible because of charge. int chg1 = (( id1Abs%2 == 0 && id1 > 0) || (id1Abs%2 == 1 && id1 < 0) ) ? 1 : -1; int chg2 = (( id2Abs%2 == 0 && id2 > 0) || (id2Abs%2 == 1 && id2 < 0) ) ? 1 : -1; if (abs(chg1 + chg2) != 2) return 0.; // Basic cross section. CKM factors for final states. double sigma = (id2 == id1 && id1Abs > 10) ? sigma0TU : sigma0T; sigma *= couplingsPtr->V2CKMsum(id1Abs) * couplingsPtr->V2CKMsum(id2Abs); // Secondary width for H0. sigma *= (chg1 + chg2 == 2) ? openFracPos : openFracNeg; // Spin-state extra factor 2 per incoming neutrino. if (id1Abs == 12 || id1Abs == 14 || id1Abs == 16) sigma *= 2.; if (id2Abs == 12 || id2Abs == 14 || id2Abs == 16) sigma *= 2.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma3ff2HchgchgfftWW::setIdColAcol() { // Pick out-flavours by relative CKM weights. int id1Abs = abs(id1); int id2Abs = abs(id2); id4 = couplingsPtr->V2CKMpick(id1); id5 = couplingsPtr->V2CKMpick(id2); // Find charge of Higgs . id3 = (( id1Abs%2 == 0 && id1 > 0) || (id1Abs%2 == 1 && id1 < 0) ) ? idHLR : -idHLR; setId( id1, id2, id3, id4, id5); // Colour flow topologies. Swap when antiquarks. if (id1Abs < 9 && id2Abs < 9 && id1*id2 > 0) setColAcol( 1, 0, 2, 0, 0, 0, 1, 0, 2, 0); else if (id1Abs < 9 && id2Abs < 9) setColAcol( 1, 0, 0, 2, 0, 0, 1, 0, 0, 2); else if (id1Abs < 9) setColAcol( 1, 0, 0, 0, 0, 0, 1, 0, 0, 0); else if (id2Abs < 9) setColAcol( 0, 0, 1, 0, 0, 0, 0, 0, 1, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0, 0, 0); if ( (id1Abs < 9 && id1 < 0) || (id1Abs > 10 && id2 < 0) ) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for decay angles. double Sigma3ff2HchgchgfftWW::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else done. return 1.; } //========================================================================== // Sigma2ffbar2HchgchgHchgchg class. // Cross section for f fbar -> H_(L/R)^++ H_(L/R)^-- (doubly charged Higgs). //-------------------------------------------------------------------------- // Initialize process. void Sigma2ffbar2HchgchgHchgchg::initProc() { // Set process properties: H_L^++ H_L^-- or H_R^++ H_R^--. if (leftRight == 1) { idHLR = 9900041; codeSave = 3126; nameSave = "f fbar -> H_L^++ H_L^--"; } else { idHLR = 9900042; codeSave = 3146; nameSave = "f fbar -> H_R^++ H_R^--"; } // Read in Yukawa matrix for couplings to a lepton pair. yukawa[1][1] = settingsPtr->parm("LeftRightSymmmetry:coupHee"); yukawa[2][1] = settingsPtr->parm("LeftRightSymmmetry:coupHmue"); yukawa[2][2] = settingsPtr->parm("LeftRightSymmmetry:coupHmumu"); yukawa[3][1] = settingsPtr->parm("LeftRightSymmmetry:coupHtaue"); yukawa[3][2] = settingsPtr->parm("LeftRightSymmmetry:coupHtaumu"); yukawa[3][3] = settingsPtr->parm("LeftRightSymmmetry:coupHtautau"); // Electroweak parameters. mRes = particleDataPtr->m0(23); GammaRes = particleDataPtr->mWidth(23); m2Res = mRes*mRes; GamMRat = GammaRes / mRes; sin2tW = couplingsPtr->sin2thetaW(); preFac = (1. - 2. * sin2tW) / ( 8. * sin2tW * (1. - sin2tW) ); // Open fraction from secondary widths. openFrac = particleDataPtr->resOpenFrac( idHLR, -idHLR); } //-------------------------------------------------------------------------- // Evaluate sigmaHat(sHat), including incoming flavour dependence. double Sigma2ffbar2HchgchgHchgchg::sigmaHat() { // Electroweak couplings to gamma^*/Z^0. int idAbs = abs(id1); double ei = couplingsPtr->ef(idAbs); double vi = couplingsPtr->vf(idAbs); double ai = couplingsPtr->af(idAbs); // Part via gamma^*/Z^0 propagator. No Z^0 coupling to H_R. double resProp = 1. / ( pow2(sH - m2Res) + pow2(sH * GamMRat) ); double sigma = 8. * pow2(alpEM) * ei*ei / sH2; if (leftRight == 1) sigma += 8. * pow2(alpEM) * (2. * ei * vi * preFac * (sH - m2Res) * resProp / sH + (vi * vi + ai * ai) * pow2(preFac) * resProp); // Part via t-channel lepton + interference; sum over possibilities. if (idAbs == 11 || idAbs == 13 || idAbs == 15) { double yuk2Sum; if (idAbs == 11) yuk2Sum = pow2(yukawa[1][1]) + pow2(yukawa[2][1]) + pow2(yukawa[3][1]); else if (idAbs == 13) yuk2Sum = pow2(yukawa[2][1]) + pow2(yukawa[2][2]) + pow2(yukawa[3][2]); else yuk2Sum = pow2(yukawa[3][1]) + pow2(yukawa[3][2]) + pow2(yukawa[3][3]); yuk2Sum /= 4. * M_PI; sigma += 8. * alpEM * ei * yuk2Sum / (sH * tH) + 4. * pow2(yuk2Sum) / tH2; if (leftRight == 1) sigma += 8. * alpEM * (vi + ai) * yuk2Sum * preFac * (sH - m2Res) * resProp / tH; } // Common kinematical factor. Colour factor. sigma *= M_PI * (tH * uH - s3 * s4) / sH2; if (idAbs < 9) sigma /= 3.; // Answer. return sigma; } //-------------------------------------------------------------------------- // Select identity, colour and anticolour. void Sigma2ffbar2HchgchgHchgchg::setIdColAcol() { // Outgoing flavours trivial. setId( id1, id2, idHLR, -idHLR); // tHat is defined between incoming fermion and outgoing H--. if (id1 > 0) swapTU = true; // No colours at all or one flow topology. Swap if first is antiquark. if (abs(id1) < 9) setColAcol( 1, 0, 0, 1, 0, 0, 0, 0); else setColAcol( 0, 0, 0, 0, 0, 0, 0, 0); if (id1 < 0) swapColAcol(); } //-------------------------------------------------------------------------- // Evaluate weight for H_L/R sequential decay angles. double Sigma2ffbar2HchgchgHchgchg::weightDecay( Event& process, int iResBeg, int iResEnd) { // Identity of mother of decaying reseonance(s). int idMother = process[process[iResBeg].mother1()].idAbs(); // For top decay hand over to standard routine. if (idMother == 6) return weightTopDecay( process, iResBeg, iResEnd); // Else isotropic decay. return 1.; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/FragmentationFlavZpT.cc0000644000175000017500000007275712217346245017524 0ustar sunsun// FragmentationFlavZpT.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // StringFlav, StringZ and StringPT classes. #include "Pythia8/FragmentationFlavZpT.h" namespace Pythia8 { //========================================================================== // The StringFlav class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Offset for different meson multiplet id values. const int StringFlav::mesonMultipletCode[6] = { 1, 3, 10003, 10001, 20003, 5}; // Clebsch-Gordan coefficients for baryon octet and decuplet are // fixed once and for all, so only weighted sum needs to be edited. // Order: ud0 + u, ud0 + s, uu1 + u, uu1 + d, ud1 + u, ud1 + s. const double StringFlav::baryonCGOct[6] = { 0.75, 0.5, 0., 0.1667, 0.0833, 0.1667}; const double StringFlav::baryonCGDec[6] = { 0., 0., 1., 0.3333, 0.6667, 0.3333}; //-------------------------------------------------------------------------- // Initialize data members of the flavour generation. void StringFlav::init(Settings& settings, Rndm* rndmPtrIn) { // Save pointer. rndmPtr = rndmPtrIn; // Basic parameters for generation of new flavour. probQQtoQ = settings.parm("StringFlav:probQQtoQ"); probStoUD = settings.parm("StringFlav:probStoUD"); probSQtoQQ = settings.parm("StringFlav:probSQtoQQ"); probQQ1toQQ0 = settings.parm("StringFlav:probQQ1toQQ0"); // Parameters derived from above. probQandQQ = 1. + probQQtoQ; probQandS = 2. + probStoUD; probQandSinQQ = 2. + probSQtoQQ * probStoUD; probQQ1corr = 3. * probQQ1toQQ0; probQQ1corrInv = 1. / probQQ1corr; probQQ1norm = probQQ1corr / (1. + probQQ1corr); // Parameters for normal meson production. for (int i = 0; i < 4; ++i) mesonRate[i][0] = 1.; mesonRate[0][1] = settings.parm("StringFlav:mesonUDvector"); mesonRate[1][1] = settings.parm("StringFlav:mesonSvector"); mesonRate[2][1] = settings.parm("StringFlav:mesonCvector"); mesonRate[3][1] = settings.parm("StringFlav:mesonBvector"); // Parameters for L=1 excited-meson production. mesonRate[0][2] = settings.parm("StringFlav:mesonUDL1S0J1"); mesonRate[1][2] = settings.parm("StringFlav:mesonSL1S0J1"); mesonRate[2][2] = settings.parm("StringFlav:mesonCL1S0J1"); mesonRate[3][2] = settings.parm("StringFlav:mesonBL1S0J1"); mesonRate[0][3] = settings.parm("StringFlav:mesonUDL1S1J0"); mesonRate[1][3] = settings.parm("StringFlav:mesonSL1S1J0"); mesonRate[2][3] = settings.parm("StringFlav:mesonCL1S1J0"); mesonRate[3][3] = settings.parm("StringFlav:mesonBL1S1J0"); mesonRate[0][4] = settings.parm("StringFlav:mesonUDL1S1J1"); mesonRate[1][4] = settings.parm("StringFlav:mesonSL1S1J1"); mesonRate[2][4] = settings.parm("StringFlav:mesonCL1S1J1"); mesonRate[3][4] = settings.parm("StringFlav:mesonBL1S1J1"); mesonRate[0][5] = settings.parm("StringFlav:mesonUDL1S1J2"); mesonRate[1][5] = settings.parm("StringFlav:mesonSL1S1J2"); mesonRate[2][5] = settings.parm("StringFlav:mesonCL1S1J2"); mesonRate[3][5] = settings.parm("StringFlav:mesonBL1S1J2"); // Store sum over multiplets for Monte Carlo generation. for (int i = 0; i < 4; ++i) mesonRateSum[i] = mesonRate[i][0] + mesonRate[i][1] + mesonRate[i][2] + mesonRate[i][3] + mesonRate[i][4] + mesonRate[i][5]; // Parameters for uubar - ddbar - ssbar meson mixing. for (int spin = 0; spin < 6; ++spin) { double theta; if (spin == 0) theta = settings.parm("StringFlav:thetaPS"); else if (spin == 1) theta = settings.parm("StringFlav:thetaV"); else if (spin == 2) theta = settings.parm("StringFlav:thetaL1S0J1"); else if (spin == 3) theta = settings.parm("StringFlav:thetaL1S1J0"); else if (spin == 4) theta = settings.parm("StringFlav:thetaL1S1J1"); else theta = settings.parm("StringFlav:thetaL1S1J2"); double alpha = (spin == 0) ? 90. - (theta + 54.7) : theta + 54.7; alpha *= M_PI / 180.; // Fill in (flavour, spin)-dependent probability of producing // the lightest or the lightest two mesons of the nonet. mesonMix1[0][spin] = 0.5; mesonMix2[0][spin] = 0.5 * (1. + pow2(sin(alpha))); mesonMix1[1][spin] = 0.; mesonMix2[1][spin] = pow2(cos(alpha)); } // Additional suppression of eta and etaPrime. etaSup = settings.parm("StringFlav:etaSup"); etaPrimeSup = settings.parm("StringFlav:etaPrimeSup"); // Sum of baryon octet and decuplet weights. decupletSup = settings.parm("StringFlav:decupletSup"); for (int i = 0; i < 6; ++i) baryonCGSum[i] = baryonCGOct[i] + decupletSup * baryonCGDec[i]; // Maximum SU(6) weight for ud0, ud1, uu1 types. baryonCGMax[0] = max( baryonCGSum[0], baryonCGSum[1]); baryonCGMax[1] = baryonCGMax[0]; baryonCGMax[2] = max( baryonCGSum[2], baryonCGSum[3]); baryonCGMax[3] = baryonCGMax[2]; baryonCGMax[4] = max( baryonCGSum[4], baryonCGSum[5]); baryonCGMax[5] = baryonCGMax[4]; // Popcorn baryon parameters. popcornRate = settings.parm("StringFlav:popcornRate"); popcornSpair = settings.parm("StringFlav:popcornSpair"); popcornSmeson = settings.parm("StringFlav:popcornSmeson"); // Suppression of leading (= first-rank) baryons. suppressLeadingB = settings.flag("StringFlav:suppressLeadingB"); lightLeadingBSup = settings.parm("StringFlav:lightLeadingBSup"); heavyLeadingBSup = settings.parm("StringFlav:heavyLeadingBSup"); // Begin calculation of derived parameters for baryon production. // Enumerate distinguishable diquark types (in diquark first is popcorn q). enum Diquark {ud0, ud1, uu1, us0, su0, us1, su1, ss1}; // Maximum SU(6) weight by diquark type. double barCGMax[8]; barCGMax[ud0] = baryonCGMax[0]; barCGMax[ud1] = baryonCGMax[4]; barCGMax[uu1] = baryonCGMax[2]; barCGMax[us0] = baryonCGMax[0]; barCGMax[su0] = baryonCGMax[0]; barCGMax[us1] = baryonCGMax[4]; barCGMax[su1] = baryonCGMax[4]; barCGMax[ss1] = baryonCGMax[2]; // Diquark SU(6) survival = Sum_quark (quark tunnel weight) * SU(6). double dMB[8]; dMB[ud0] = 2. * baryonCGSum[0] + probStoUD * baryonCGSum[1]; dMB[ud1] = 2. * baryonCGSum[4] + probStoUD * baryonCGSum[5]; dMB[uu1] = baryonCGSum[2] + (1. + probStoUD) * baryonCGSum[3]; dMB[us0] = (1. + probStoUD) * baryonCGSum[0] + baryonCGSum[1]; dMB[su0] = dMB[us0]; dMB[us1] = (1. + probStoUD) * baryonCGSum[4] + baryonCGSum[5]; dMB[su1] = dMB[us1]; dMB[ss1] = probStoUD * baryonCGSum[2] + 2. * baryonCGSum[3]; for (int i = 1; i < 8; ++i) dMB[i] = dMB[i] / dMB[0]; // Tunneling factors for diquark production; only half a pair = sqrt. double probStoUDroot = sqrt(probStoUD); double probSQtoQQroot = sqrt(probSQtoQQ); double probQQ1toQQ0root = sqrt(probQQ1toQQ0); double qBB[8]; qBB[ud1] = probQQ1toQQ0root; qBB[uu1] = probQQ1toQQ0root; qBB[us0] = probSQtoQQroot; qBB[su0] = probStoUDroot * probSQtoQQroot; qBB[us1] = probQQ1toQQ0root * qBB[us0]; qBB[su1] = probQQ1toQQ0root * qBB[su0]; qBB[ss1] = probStoUDroot * pow2(probSQtoQQroot) * probQQ1toQQ0root; // spin * (vertex factor) * (half-tunneling factor above). double qBM[8]; qBM[ud1] = 3. * qBB[ud1]; qBM[uu1] = 6. * qBB[uu1]; qBM[us0] = probStoUD * qBB[us0]; qBM[su0] = qBB[su0]; qBM[us1] = probStoUD * 3. * qBB[us1]; qBM[su1] = 3. * qBB[su1]; qBM[ss1] = probStoUD * 6. * qBB[ss1]; // Combine above two into total diquark weight for q -> B Bbar. for (int i = 1; i < 8; ++i) qBB[i] = qBB[i] * qBM[i]; // Suppression from having strange popcorn meson. qBM[us0] *= popcornSmeson; qBM[us1] *= popcornSmeson; qBM[ss1] *= popcornSmeson; // Suppression for a heavy quark of a diquark to fit into a baryon // on the other side of popcorn meson: (0) s/u for q -> B M; // (1) s/u for rank 0 diquark su -> M B; (2) ditto for s -> c/b. double uNorm = 1. + qBM[ud1] + qBM[uu1] + qBM[us0] + qBM[us1]; scbBM[0] = (2. * (qBM[su0] + qBM[su1]) + qBM[ss1]) / uNorm; scbBM[1] = scbBM[0] * popcornSpair * qBM[su0] / qBM[us0]; scbBM[2] = (1. + qBM[ud1]) * (2. + qBM[us0]) / uNorm; // Include maximum of Clebsch-Gordan coefficients. for (int i = 1; i < 8; ++i) dMB[i] *= qBM[i]; for (int i = 1; i < 8; ++i) qBM[i] *= barCGMax[i] / barCGMax[0]; for (int i = 1; i < 8; ++i) qBB[i] *= barCGMax[i] / barCGMax[0]; // Popcorn fraction for normal diquark production. double qNorm = uNorm * popcornRate / 3.; double sNorm = scbBM[0] * popcornSpair; popFrac = qNorm * (1. + qBM[ud1] + qBM[uu1] + qBM[us0] + qBM[us1] + sNorm * (qBM[su0] + qBM[su1] + 0.5 * qBM[ss1])) / (1. + qBB[ud1] + qBB[uu1] + 2. * (qBB[us0] + qBB[us1]) + 0.5 * qBB[ss1]); // Popcorn fraction for rank 0 diquarks, depending on number of s quarks. popS[0] = qNorm * qBM[ud1] / qBB[ud1]; popS[1] = qNorm * 0.5 * (qBM[us1] / qBB[us1] + sNorm * qBM[su1] / qBB[su1]); popS[2] = qNorm * sNorm * qBM[ss1] / qBB[ss1]; // Recombine diquark weights to flavour and spin ratios. Second index: // 0 = s/u popcorn quark ratio. // 1, 2 = s/u ratio for vertex quark if popcorn quark is u/d or s. // 3 = q/q' vertex quark ratio if popcorn quark is light and = q. // 4, 5, 6 = (spin 1)/(spin 0) ratio for su, us and ud. // Case 0: q -> B B. dWT[0][0] = (2. * (qBB[su0] + qBB[su1]) + qBB[ss1]) / (1. + qBB[ud1] + qBB[uu1] + qBB[us0] + qBB[us1]); dWT[0][1] = 2. * (qBB[us0] + qBB[us1]) / (1. + qBB[ud1] + qBB[uu1]); dWT[0][2] = qBB[ss1] / (qBB[su0] + qBB[su1]); dWT[0][3] = qBB[uu1] / (1. + qBB[ud1] + qBB[uu1]); dWT[0][4] = qBB[su1] / qBB[su0]; dWT[0][5] = qBB[us1] / qBB[us0]; dWT[0][6] = qBB[ud1]; // Case 1: q -> B M B. dWT[1][0] = (2. * (qBM[su0] + qBM[su1]) + qBM[ss1]) / (1. + qBM[ud1] + qBM[uu1] + qBM[us0] + qBM[us1]); dWT[1][1] = 2. * (qBM[us0] + qBM[us1]) / (1. + qBM[ud1] + qBM[uu1]); dWT[1][2] = qBM[ss1] / (qBM[su0] + qBM[su1]); dWT[1][3] = qBM[uu1] / (1. + qBM[ud1] + qBM[uu1]); dWT[1][4] = qBM[su1] / qBM[su0]; dWT[1][5] = qBM[us1] / qBM[us0]; dWT[1][6] = qBM[ud1]; // Case 2: qq -> M B; diquark inside chain. dWT[2][0] = (2. * (dMB[su0] + dMB[su1]) + dMB[ss1]) / (1. + dMB[ud1] + dMB[uu1] + dMB[us0] + dMB[us1]); dWT[2][1] = 2. * (dMB[us0] + dMB[us1]) / (1. + dMB[ud1] + dMB[uu1]); dWT[2][2] = dMB[ss1] / (dMB[su0] + dMB[su1]); dWT[2][3] = dMB[uu1] / (1. + dMB[ud1] + dMB[uu1]); dWT[2][4] = dMB[su1] / dMB[su0]; dWT[2][5] = dMB[us1] / dMB[us0]; dWT[2][6] = dMB[ud1]; } //-------------------------------------------------------------------------- // Pick a new flavour (including diquarks) given an incoming one. FlavContainer StringFlav::pick(FlavContainer& flavOld) { // Initial values for new flavour. FlavContainer flavNew; flavNew.rank = flavOld.rank + 1; // For original diquark assign popcorn quark and whether popcorn meson. int idOld = abs(flavOld.id); if (flavOld.rank == 0 && idOld > 1000) assignPopQ(flavOld); // Diquark exists, to be forced into baryon now. bool doOldBaryon = (idOld > 1000 && flavOld.nPop == 0); // Diquark exists, but do meson now. bool doPopcornMeson = flavOld.nPop > 0; // Newly created diquark gives baryon now, antibaryon later. bool doNewBaryon = false; // Choose whether to generate a new meson or a new baryon. if (!doOldBaryon && !doPopcornMeson && probQandQQ * rndmPtr->flat() > 1.) { doNewBaryon = true; if ((1. + popFrac) * rndmPtr->flat() > 1.) flavNew.nPop = 1; } // Optional suppression of first-rank baryon. if (flavOld.rank == 0 && doNewBaryon && suppressLeadingB) { double leadingBSup = (idOld < 4) ? lightLeadingBSup : heavyLeadingBSup; if (rndmPtr->flat() > leadingBSup) { doNewBaryon = false; flavNew.nPop = 0; } } // Single quark for new meson or for baryon where diquark already exists. if (!doPopcornMeson && !doNewBaryon) { flavNew.id = pickLightQ(); if ( (flavOld.id > 0 && flavOld.id < 9) || flavOld.id < -1000 ) flavNew.id = -flavNew.id; // Done for simple-quark case. return flavNew; } // Case: 0 = q -> B B, 1 = q -> B M B, 2 = qq -> M B. int iCase = flavNew.nPop; if (flavOld.nPop == 1) iCase = 2; // Flavour of popcorn quark (= q shared between B and Bbar). if (doNewBaryon) { double sPopWT = dWT[iCase][0]; if (iCase == 1) sPopWT *= scbBM[0] * popcornSpair; double rndmFlav = (2. + sPopWT) * rndmPtr->flat(); flavNew.idPop = 1; if (rndmFlav > 1.) flavNew.idPop = 2; if (rndmFlav > 2.) flavNew.idPop = 3; } else flavNew.idPop = flavOld.idPop; // Flavour of vertex quark. double sVtxWT = dWT[iCase][1]; if (flavNew.idPop >= 3) sVtxWT = dWT[iCase][2]; if (flavNew.idPop > 3) sVtxWT *= 0.5 * (1. + 1./dWT[iCase][4]); double rndmFlav = (2. + sVtxWT) * rndmPtr->flat(); flavNew.idVtx = 1; if (rndmFlav > 1.) flavNew.idVtx = 2; if (rndmFlav > 2.) flavNew.idVtx = 3; // Special case for light flavours, possibly identical. if (flavNew.idPop < 3 && flavNew.idVtx < 3) { flavNew.idVtx = flavNew.idPop; if (rndmPtr->flat() > dWT[iCase][3]) flavNew.idVtx = 3 - flavNew.idPop; } // Pick 2 * spin + 1. int spin = 3; if (flavNew.idVtx != flavNew.idPop) { double spinWT = dWT[iCase][6]; if (flavNew.idVtx == 3) spinWT = dWT[iCase][5]; if (flavNew.idPop >= 3) spinWT = dWT[iCase][4]; if ((1. + spinWT) * rndmPtr->flat() < 1.) spin = 1; } // Form outgoing diquark. Done. flavNew.id = 1000 * max(flavNew.idVtx, flavNew.idPop) + 100 * min(flavNew.idVtx, flavNew.idPop) + spin; if ( (flavOld.id < 0 && flavOld.id > -9) || flavOld.id > 1000 ) flavNew.id = -flavNew.id; return flavNew; } //-------------------------------------------------------------------------- // Combine two flavours (including diquarks) to produce a hadron. // The weighting of the combination may fail, giving output 0. int StringFlav::combine(FlavContainer& flav1, FlavContainer& flav2) { // Recognize largest and smallest flavour. int id1Abs = abs(flav1.id); int id2Abs = abs(flav2.id); int idMax = max(id1Abs, id2Abs); int idMin = min(id1Abs, id2Abs); // Construct a meson. if (idMax < 9 || idMin > 1000) { // Popcorn meson: use only vertex quarks. Fail if none. if (idMin > 1000) { id1Abs = flav1.idVtx; id2Abs = flav2.idVtx; idMax = max(id1Abs, id2Abs); idMin = min(id1Abs, id2Abs); if (idMin == 0) return 0; } // Pick spin state and preliminary code. int flav = (idMax < 3) ? 0 : idMax - 2; double rndmSpin = mesonRateSum[flav] * rndmPtr->flat(); int spin = -1; do rndmSpin -= mesonRate[flav][++spin]; while (rndmSpin > 0.); int idMeson = 100 * idMax + 10 * idMin + mesonMultipletCode[spin]; // For nondiagonal mesons distinguish particle/antiparticle. if (idMax != idMin) { int sign = (idMax%2 == 0) ? 1 : -1; if ( (idMax == id1Abs && flav1.id < 0) || (idMax == id2Abs && flav2.id < 0) ) sign = -sign; idMeson *= sign; // For light diagonal mesons include uubar - ddbar - ssbar mixing. } else if (flav < 2) { double rMix = rndmPtr->flat(); if (rMix < mesonMix1[flav][spin]) idMeson = 110; else if (rMix < mesonMix2[flav][spin]) idMeson = 220; else idMeson = 330; idMeson += mesonMultipletCode[spin]; // Additional suppression of eta and eta' may give failure. if (idMeson == 221 && etaSup < rndmPtr->flat()) return 0; if (idMeson == 331 && etaPrimeSup < rndmPtr->flat()) return 0; } // Finished for mesons. return idMeson; } // SU(6) factors for baryon production may give failure. int idQQ1 = idMax / 1000; int idQQ2 = (idMax / 100) % 10; int spinQQ = idMax % 10; int spinFlav = spinQQ - 1; if (spinFlav == 2 && idQQ1 != idQQ2) spinFlav = 4; if (idMin != idQQ1 && idMin != idQQ2) spinFlav++; if (baryonCGSum[spinFlav] < rndmPtr->flat() * baryonCGMax[spinFlav]) return 0; // Order quarks to form baryon. Pick spin. int idOrd1 = max( idMin, max( idQQ1, idQQ2) ); int idOrd3 = min( idMin, min( idQQ1, idQQ2) ); int idOrd2 = idMin + idQQ1 + idQQ2 - idOrd1 - idOrd3; int spinBar = (baryonCGSum[spinFlav] * rndmPtr->flat() < baryonCGOct[spinFlav]) ? 2 : 4; // Distinguish Lambda- and Sigma-like. bool LambdaLike = false; if (spinBar == 2 && idOrd1 > idOrd2 && idOrd2 > idOrd3) { LambdaLike = (spinQQ == 1); if (idOrd1 != idMin && spinQQ == 1) LambdaLike = (rndmPtr->flat() < 0.25); else if (idOrd1 != idMin) LambdaLike = (rndmPtr->flat() < 0.75); } // Form baryon code and return with sign. int idBaryon = (LambdaLike) ? 1000 * idOrd1 + 100 * idOrd3 + 10 * idOrd2 + spinBar : 1000 * idOrd1 + 100 * idOrd2 + 10 * idOrd3 + spinBar; return (flav1.id > 0) ? idBaryon : -idBaryon; } //-------------------------------------------------------------------------- // Assign popcorn quark inside an original (= rank 0) diquark. void StringFlav::assignPopQ(FlavContainer& flav) { // Safety check that intended to do something. int idAbs = abs(flav.id); if (flav.rank > 0 || idAbs < 1000) return; // Make choice of popcorn quark. int id1 = (idAbs/1000)%10; int id2 = (idAbs/100)%10; double pop2WT = 1.; if (id1 == 3) pop2WT = scbBM[1]; else if (id1 > 3) pop2WT = scbBM[2]; if (id2 == 3) pop2WT /= scbBM[1]; else if (id2 > 3) pop2WT /= scbBM[2]; // Agrees with Patrik code, but opposite to intention?? flav.idPop = ((1. + pop2WT) * rndmPtr->flat() > 1.) ? id2 : id1; flav.idVtx = id1 + id2 - flav.idPop; // Also determine if to produce popcorn meson. flav.nPop = 0; double popWT = popS[0]; if (id1 == 3) popWT = popS[1]; if (id2 == 3) popWT = popS[2]; if (idAbs%10 == 1) popWT *= sqrt(probQQ1toQQ0); if ((1. + popWT) * rndmPtr->flat() > 1.) flav.nPop = 1; } //-------------------------------------------------------------------------- // Combine two quarks to produce a diquark. // Normally according to production composition, but nonvanishing idHad // means diquark from known hadron content, so use SU(6) wave fucntion. int StringFlav::makeDiquark(int id1, int id2, int idHad) { // Initial values. int idMin = min( abs(id1), abs(id2)); int idMax = max( abs(id1), abs(id2)); int spin = 1; // Select spin of diquark formed from two valence quarks in proton. // (More hadron cases??) if (abs(idHad) == 2212 || abs(idHad) == 2112) { if (idMin == 1 && idMax == 2 && rndmPtr->flat() < 0.75) spin = 0; // Else select spin of diquark according to production composition. } else { if (idMin != idMax && rndmPtr->flat() > probQQ1norm) spin = 0; } // Combined diquark code. int idNewAbs = 1000 * idMax + 100 * idMin + 2 * spin + 1; return (id1 > 0) ? idNewAbs : -idNewAbs; } //========================================================================== // The StringZ class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // When a or c are close to special cases, default to these. const double StringZ::CFROMUNITY = 0.01; const double StringZ::AFROMZERO = 0.02; const double StringZ::AFROMC = 0.01; // Do not take exponent of too large or small number. const double StringZ::EXPMAX = 50.; //-------------------------------------------------------------------------- // Initialize data members of the string z selection. void StringZ::init(Settings& settings, ParticleData& particleData, Rndm* rndmPtrIn) { // Save pointer. rndmPtr = rndmPtrIn; // c and b quark masses. mc2 = pow2( particleData.m0(4)); mb2 = pow2( particleData.m0(5)); // Paramaters of Lund/Bowler symmetric fragmentation function. aLund = settings.parm("StringZ:aLund"); bLund = settings.parm("StringZ:bLund"); aExtraDiquark = settings.parm("StringZ:aExtraDiquark"); rFactC = settings.parm("StringZ:rFactC"); rFactB = settings.parm("StringZ:rFactB"); rFactH = settings.parm("StringZ:rFactH"); // Flags and parameters of nonstandard Lund fragmentation functions. useNonStandC = settings.flag("StringZ:useNonstandardC"); useNonStandB = settings.flag("StringZ:useNonstandardB"); useNonStandH = settings.flag("StringZ:useNonstandardH"); aNonC = settings.parm("StringZ:aNonstandardC"); aNonB = settings.parm("StringZ:aNonstandardB"); aNonH = settings.parm("StringZ:aNonstandardH"); bNonC = settings.parm("StringZ:bNonstandardC"); bNonB = settings.parm("StringZ:bNonstandardB"); bNonH = settings.parm("StringZ:bNonstandardH"); // Flags and parameters of Peterson/SLAC fragmentation function. usePetersonC = settings.flag("StringZ:usePetersonC"); usePetersonB = settings.flag("StringZ:usePetersonB"); usePetersonH = settings.flag("StringZ:usePetersonH"); epsilonC = settings.parm("StringZ:epsilonC"); epsilonB = settings.parm("StringZ:epsilonB"); epsilonH = settings.parm("StringZ:epsilonH"); // Parameters for joining procedure. stopM = settings.parm("StringFragmentation:stopMass"); stopNF = settings.parm("StringFragmentation:stopNewFlav"); stopS = settings.parm("StringFragmentation:stopSmear"); } //-------------------------------------------------------------------------- // Generate the fraction z that the next hadron will take, // using either Lund/Bowler or, for heavy, Peterson/SLAC functions. // Note: for a heavy new coloured particle we assume pT negligible. double StringZ::zFrag( int idOld, int idNew, double mT2) { // Find if old or new flavours correspond to diquarks. int idOldAbs = abs(idOld); int idNewAbs = abs(idNew); bool isOldDiquark = (idOldAbs > 1000 && idOldAbs < 10000); bool isNewDiquark = (idNewAbs > 1000 && idNewAbs < 10000); // Find heaviest quark in fragmenting parton/diquark. int idFrag = idOldAbs; if (isOldDiquark) idFrag = max( idOldAbs / 1000, (idOldAbs / 100) % 10); // Use Peterson where explicitly requested for heavy flavours. if (idFrag == 4 && usePetersonC) return zPeterson( epsilonC); if (idFrag == 5 && usePetersonB) return zPeterson( epsilonB); if (idFrag > 5 && usePetersonH) { double epsilon = epsilonH * mb2 / mT2; return zPeterson( epsilon); } // Nonstandard a and b values implemented for heavy flavours. double aNow = aLund; double bNow = bLund; if (idFrag == 4 && useNonStandC) { aNow = aNonC; bNow = bNonC; } else if (idFrag == 5 && useNonStandB) { aNow = aNonB; bNow = bNonB; } else if (idFrag > 5 && useNonStandH) { aNow = aNonH; bNow = bNonH; } // Shape parameters of Lund symmetric fragmentation function. double aShape = aNow; if (isOldDiquark) aShape += aExtraDiquark; double bShape = bNow * mT2; double cShape = 1.; if (isOldDiquark) cShape -= aExtraDiquark; if (isNewDiquark) cShape += aExtraDiquark; if (idFrag == 4) cShape += rFactC * bNow * mc2; if (idFrag == 5) cShape += rFactB * bNow * mb2; if (idFrag > 5) cShape += rFactH * bNow * mT2; return zLund( aShape, bShape, cShape); } //-------------------------------------------------------------------------- // Generate a random z according to the Lund/Bowler symmetric // fragmentation function f(z) = (1 -z)^a * exp(-b/z) / z^c. // Normalized so that f(z_max) = 1 it can also be written as // f(z) = exp( a * ln( (1 - z) / (1 - z_max) ) + b * (1/z_max - 1/z) // + c * ln(z_max/z) ). double StringZ::zLund( double a, double b, double c) { // Special cases for c = 1, a = 0 and a = c. bool cIsUnity = (abs( c - 1.) < CFROMUNITY); bool aIsZero = (a < AFROMZERO); bool aIsC = (abs(a - c) < AFROMC); // Determine position of maximum. double zMax; if (aIsZero) zMax = (c > b) ? b / c : 1.; else if (aIsC) zMax = b / (b + c); else { zMax = 0.5 * (b + c - sqrt( pow2(b - c) + 4. * a * b)) / (c - a); if (zMax > 0.9999 && b > 100.) zMax = min(zMax, 1. - a / b); } // Subdivide z range if distribution very peaked near either endpoint. bool peakedNearZero = (zMax < 0.1); bool peakedNearUnity = (zMax > 0.85 && b > 1.); // Find integral of trial function everywhere bigger than f. // (Dummy start values.) double fIntLow = 1.; double fIntHigh = 1.; double fInt = 2.; double zDiv = 0.5; double zDivC = 0.5; // When z_max is small use that f(z) // < 1 for z < z_div = 2.75 * z_max, // < (z_div/z)^c for z > z_div (=> logarithm for c = 1, else power). if (peakedNearZero) { zDiv = 2.75 * zMax; fIntLow = zDiv; if (cIsUnity) fIntHigh = -zDiv * log(zDiv); else { zDivC = pow( zDiv, 1. - c); fIntHigh = zDiv * (1. - 1./zDivC) / (c - 1.);} fInt = fIntLow + fIntHigh; // When z_max large use that f(z) // < exp( b * (z - z_div) ) for z < z_div with z_div messy expression, // < 1 for z > z_div. // To simplify expressions the integral is extended to z = -infinity. } else if (peakedNearUnity) { double rcb = sqrt(4. + pow2(c / b)); zDiv = rcb - 1./zMax - (c / b) * log( zMax * 0.5 * (rcb + c / b) ); if (!aIsZero) zDiv += (a/b) * log(1. - zMax); zDiv = min( zMax, max(0., zDiv)); fIntLow = 1. / b; fIntHigh = 1. - zDiv; fInt = fIntLow + fIntHigh; } // Choice of z, preweighted for peaks at low or high z. (Dummy start values.) double z = 0.5; double fPrel = 1.; double fVal = 1.; do { // Choice of z flat good enough for distribution peaked in the middle; // if not this z can be reused as a random number in general. z = rndmPtr->flat(); fPrel = 1.; // When z_max small use flat below z_div and 1/z^c above z_div. if (peakedNearZero) { if (fInt * rndmPtr->flat() < fIntLow) z = zDiv * z; else if (cIsUnity) {z = pow( zDiv, z); fPrel = zDiv / z;} else { z = pow( zDivC + (1. - zDivC) * z, 1. / (1. - c) ); fPrel = pow( zDiv / z, c); } // When z_max large use exp( b * (z -z_div) ) below z_div // and flat above it. } else if (peakedNearUnity) { if (fInt * rndmPtr->flat() < fIntLow) { z = zDiv + log(z) / b; fPrel = exp( b * (z - zDiv) ); } else z = zDiv + (1. - zDiv) * z; } // Evaluate actual f(z) (if in physical range) and correct. if (z > 0 && z < 1) { double fExp = b * (1. / zMax - 1. / z)+ c * log(zMax / z); if (!aIsZero) fExp += a * log( (1. - z) / (1. - zMax) ); fVal = exp( max( -EXPMAX, min( EXPMAX, fExp) ) ) ; } else fVal = 0.; } while (fVal < rndmPtr->flat() * fPrel); // Done. return z; } //-------------------------------------------------------------------------- // Generate a random z according to the Peterson/SLAC formula // f(z) = 1 / ( z * (1 - 1/z - epsilon/(1-z))^2 ) // = z * (1-z)^2 / ((1-z)^2 + epsilon * z)^2. double StringZ::zPeterson( double epsilon) { double z, fVal; // For large epsilon pick z flat and reject, // knowing that 4 * epsilon * f(z) < 1 everywhere. if (epsilon > 0.01) { do { z = rndmPtr->flat(); fVal = 4. * epsilon * z * pow2(1. - z) / pow2( pow2(1. - z) + epsilon * z); } while (fVal < rndmPtr->flat()); return z; } // Else split range, using that 4 * epsilon * f(z) // < 4 * epsilon / (1 - z)^2 for 0 < z < 1 - 2 * sqrt(epsilon) // < 1 for 1 - 2 * sqrt(epsilon) < z < 1 double epsRoot = sqrt(epsilon); double epsComb = 0.5 / epsRoot - 1.; double fIntLow = 4. * epsilon * epsComb; double fInt = fIntLow + 2. * epsRoot; do { if (rndmPtr->flat() * fInt < fIntLow) { z = 1. - 1. / (1. + rndmPtr->flat() * epsComb); fVal = z * pow2( pow2(1. - z) / (pow2(1. - z) + epsilon * z) ); } else { z = 1. - 2. * epsRoot * rndmPtr->flat(); fVal = 4. * epsilon * z * pow2(1. - z) / pow2( pow2(1. - z) + epsilon * z); } } while (fVal < rndmPtr->flat()); return z; } //========================================================================== // The StringPT class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // To avoid division by zero one must have sigma > 0. const double StringPT::SIGMAMIN = 0.2; //-------------------------------------------------------------------------- // Initialize data members of the string pT selection. void StringPT::init(Settings& settings, ParticleData& , Rndm* rndmPtrIn) { // Save pointer. rndmPtr = rndmPtrIn; // Parameters of the pT width and enhancement. double sigma = settings.parm("StringPT:sigma"); sigmaQ = sigma / sqrt(2.); enhancedFraction = settings.parm("StringPT:enhancedFraction"); enhancedWidth = settings.parm("StringPT:enhancedWidth"); // Parameter for pT suppression in MiniStringFragmentation. sigma2Had = 2. * pow2( max( SIGMAMIN, sigma) ); } //-------------------------------------------------------------------------- // Generate Gaussian pT such that = = sigma^2 = width^2/2, // but with small fraction multiplied up to a broader spectrum. pair StringPT::pxy() { double sigma = sigmaQ; if (rndmPtr->flat() < enhancedFraction) sigma *= enhancedWidth; pair gauss2 = rndmPtr->gauss2(); return pair(sigma * gauss2.first, sigma * gauss2.second); } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/src/SusyCouplings.cc0000644000175000017500000011706412217346252016273 0ustar sunsun// SusyCouplings.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // Main authors of this file: N. Desai, P. Skands // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Function definitions (not found in the header) for the // supersymmetric couplings class. #include "Pythia8/ParticleData.h" #include "Pythia8/SusyCouplings.h" namespace Pythia8 { //========================================================================== // The CoupSUSY class. //-------------------------------------------------------------------------- // Constants: could be changed here if desired, but normally should not. // These are of technical nature, as described for each. // Allow verbose printout for debug purposes. const bool CoupSUSY::DBSUSY = false; //-------------------------------------------------------------------------- // Initialize SM+SUSY couplings (only performed once). void CoupSUSY::initSUSY (SusyLesHouches* slhaPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn) { // Save pointers. slhaPtr = slhaPtrIn; settingsPtr = settingsPtrIn; particleDataPtr = particleDataPtrIn; // Only initialize SUSY parts if SUSY is actually switched on if (!slhaPtr->modsel.exists()) return; // Is NMSSM switched on? isNMSSM = (slhaPtr->modsel(3) != 1 ? false : true); settingsPtr->flag("SLHA:NMSSM",isNMSSM); int nNeut = (isNMSSM ? 5 : 4); int nChar = 2; // Initialize pole masses mZpole = particleDataPtr->m0(23); wZpole = particleDataPtr->mWidth(23); mWpole = particleDataPtr->m0(24); wWpole = particleDataPtr->mWidth(24); // Running masses and weak mixing angle // (default to pole values if no running available) mW = mWpole; mZ = mZpole; sin2W = sin2thetaW(); if (settingsPtr->mode("SUSY:sin2thetaWMode") == 3) { // Possibility to force on-shell sin2W definition, mostly intended for // cross-checks sin2W = 1.0 - pow(mW/mZ,2); } else if (settingsPtr->mode("SUSY:sin2thetaWMode") == 2){ // Possibility to use running sin2W definition, derived from gauge // couplings in running SLHA blocks (normally defined at SUSY scale) if(slhaPtr->gauge.exists(1) && slhaPtr->gauge.exists(2) && slhaPtr->hmix.exists(3)) { double gp=slhaPtr->gauge(1); double g =slhaPtr->gauge(2); double v =slhaPtr->hmix(3); mW = g * v / 2.0; mZ = sqrt(pow(gp,2)+pow(g,2)) * v / 2.0; //double tan2W = pow2(gp)/pow2(g); //if (DBSUSY) cout << " tan2W = " << tan2W << endl; sin2W = pow2(gp)/(pow2(g)+pow2(gp)); } else { slhaPtr->message(1,"initSUSY", "Block GAUGE not found or incomplete; using sin(thetaW) at mZ"); } } // Overload the SM value of sin2thetaW s2tW = sin2W; sinW = sqrt(sin2W); cosW = sqrt(1.0-sin2W); // Tan(beta) // By default, use the running one in HMIX (if not found, use MINPAR) if(slhaPtr->hmix.exists(2)) tanb = slhaPtr->hmix(2); else{ tanb = slhaPtr->minpar(3); slhaPtr->message(1,"initSUSY", "Block HMIX not found or incomplete; using MINPAR tan(beta)"); } cosb = sqrt( 1.0 / (1.0 + tanb*tanb) ); sinb = sqrt( max(0.0, 1.0 - cosb*cosb)); double beta = acos(cosb); // Verbose output if (DBSUSY) { cout << " sin2W(Q) = " << sin2W << " mW(Q) = " << mW << " mZ(Q) = " << mZ << endl; cout << " vev(Q) = " << slhaPtr->hmix(3) << " tanb(Q) = " << tanb << endl; for (int i=1;i<=3;i++) { for (int j=1;j<=3;j++) { cout << " VCKM [" << i << "][" << j << "] = " << scientific << setw(10) << VCKMgen(i,j) << endl; } } } // Higgs sector if(slhaPtr->alpha.exists()) { alphaHiggs = slhaPtr->alpha(); } // If RPV, assume alpha = asin(RVHMIX(1,2)) (ignore Higgs-Sneutrino mixing) else if (slhaPtr->modsel(4) == 1) { alphaHiggs = asin(slhaPtr->rvhmix(1,2)); slhaPtr->message(0,"initSUSY","Extracting angle alpha from RVHMIX"); } else { slhaPtr->message(1,"initSUSY","Block ALPHA not found; using alpha = beta."); // Define approximate alpha by simple SM limit alphaHiggs = atan(tanb); } if(slhaPtr->hmix.exists(1) && slhaPtr->hmix.exists(4)){ muHiggs = slhaPtr->hmix(1); mAHiggs = sqrt(slhaPtr->hmix(4)); } else if (slhaPtr->rvamix.exists()){ mAHiggs = particleDataPtr->m0(36); muHiggs = 0.0; slhaPtr->message(1,"initSUSY", "Block HMIX not found or incomplete; setting mu = 0."); } else{ slhaPtr->message(1,"initSUSY", "Block HMIX not found or incomplete; setting mu = mA = 0."); muHiggs = 0.0; mAHiggs = 0.0; } // Pass SLHA input to 2HDM sector double sba = sin(beta-alphaHiggs); double cba = cos(beta-alphaHiggs); double cosa = cos(alphaHiggs); double sina = sin(alphaHiggs); // h0 settingsPtr->parm("HiggsH1:coup2d", -sina/cosb); settingsPtr->parm("HiggsH1:coup2u", cosa/sinb); settingsPtr->parm("HiggsH1:coup2l", cosa/sinb); settingsPtr->parm("HiggsH1:coup2Z", sba); settingsPtr->parm("HiggsH1:coup2W", sba); // H0 settingsPtr->parm("HiggsH2:coup2d", cosa/cosb); settingsPtr->parm("HiggsH2:coup2u", sina/sinb); settingsPtr->parm("HiggsH2:coup2l", sina/sinb); settingsPtr->parm("HiggsH2:coup2Z", cba); settingsPtr->parm("HiggsH2:coup2W", cba); settingsPtr->parm("HiggsH2:coup2H1Z", 0.0); settingsPtr->parm("HiggsH2:coup2HchgW", sba); // A0 settingsPtr->parm("HiggsA3:coup2d", tanb); settingsPtr->parm("HiggsA3:coup2u", cosb/sinb); settingsPtr->parm("HiggsA3:coup2l", cosb/sinb); settingsPtr->parm("HiggsA3:coup2Z", 0.0); settingsPtr->parm("HiggsA3:coup2W", 0.0); settingsPtr->parm("HiggsA3:coup2H1Z", cba); settingsPtr->parm("HiggsA3:coup2H2Z", sba); settingsPtr->parm("HiggsA3:coup2HchgW", 1.0); // H^+ settingsPtr->parm("HiggsHchg:tanBeta", tanb); settingsPtr->parm("HiggsHchg:coup2H1W", cba); settingsPtr->parm("HiggsHchg:coup2H2W", sba); // Triple higgs couplings double cbpa = cos(beta+alphaHiggs); double sbpa = sin(beta+alphaHiggs); settingsPtr->parm("HiggsH1:coup2Hchg", cos(2*beta)*sbpa + 2*pow2(cosW)*sba); settingsPtr->parm("HiggsH2:coup2Hchg", -cos(2*beta)*cbpa + 2*pow2(cosW)*cba); settingsPtr->parm("HiggsH2:coup2H1H1", 2*sin(2*alphaHiggs)*sbpa - cos(2*alphaHiggs)*cbpa); settingsPtr->parm("HiggsH2:coup2A3A3", -cos(2*beta)*cbpa); settingsPtr->parm("HiggsH2:coup2A3H1", 0.0); settingsPtr->parm("HiggsA3:coup2H1H1", 0.0); settingsPtr->parm("HiggsA3:coup2Hchg", 0.0); // Shorthand for squark mixing matrices LHmatrixBlock<6> Ru(slhaPtr->usqmix); LHmatrixBlock<6> Rd(slhaPtr->dsqmix); LHmatrixBlock<6> imRu(slhaPtr->imusqmix); LHmatrixBlock<6> imRd(slhaPtr->imdsqmix); // Construct ~g couplings for (int i=1; i<=6; i++) { for (int j=1; j<=3; j++) { LsddG[i][j] = complex( Rd(i,j) , imRd(i,j)); RsddG[i][j] = complex(-Rd(i,j+3), -imRd(i,j+3)); LsuuG[i][j] = complex( Ru(i,j) , imRu(i,j)); RsuuG[i][j] = complex(-Ru(i,j+3), -imRu(i,j+3)); if (DBSUSY) { cout << " Lsddg [" << i << "][" << j << "] = " << scientific << setw(10) << LsddG[i][j] << " RsddG [" << i << "][" << j << "] = " << scientific << setw(10) << RsddG[i][j] << endl; cout << " Lsuug [" << i << "][" << j << "] = " << scientific << setw(10) << LsuuG[i][j] << " RsuuG [" << i << "][" << j << "] = " << scientific << setw(10) << RsuuG[i][j] << endl; } } } // Construct qqZ couplings for (int i=1 ; i<=6 ; i++) { // q[i] q[i] Z (def with extra factor 2 compared to [Okun]) LqqZ[i] = af(i) - 2.0*ef(i)*sin2W ; RqqZ[i] = - 2.0*ef(i)*sin2W ; // tmp: verbose output if (DBSUSY) { cout << " LqqZ [" << i << "][" << i << "] = " << scientific << setw(10) << LqqZ[i] << " RqqZ [" << i << "][" << i << "] = " << scientific << setw(10) << RqqZ[i] << endl; } } // Construct ~q~qZ couplings for (int i=1 ; i<=6 ; i++) { // Squarks can have off-diagonal couplings as well for (int j=1 ; j<=6 ; j++) { // ~d[i] ~d[j] Z LsdsdZ[i][j] = 0.0; RsdsdZ[i][j] = 0.0; for (int k=1;k<=3;k++) { complex Rdik = complex(Rd(i,k), imRd(i,k) ); complex Rdjk = complex(Rd(j,k), imRd(j,k) ); complex Rdik3 = complex(Rd(i,k+3),imRd(i,k+3)); complex Rdjk3 = complex(Rd(j,k+3),imRd(j,k+3)); LsdsdZ[i][j] += LqqZ[1] * (Rdik*conj(Rdjk)); RsdsdZ[i][j] += RqqZ[1] * (Rdik3*conj(Rdjk3)); } // ~u[i] ~u[j] Z LsusuZ[i][j] = 0.0; RsusuZ[i][j] = 0.0; for (int k=1;k<=3;k++) { complex Ruik = complex(Ru(i,k) ,imRu(i,k) ); complex Rujk = complex(Ru(j,k) ,imRu(j,k) ); complex Ruik3 = complex(Ru(i,k+3),imRu(i,k+3)); complex Rujk3 = complex(Ru(j,k+3),imRu(j,k+3)); LsusuZ[i][j] += LqqZ[2] * (Ruik*conj(Rujk)); RsusuZ[i][j] += RqqZ[2] * (Ruik3*conj(Rujk3)); } // tmp: verbose output if (DBSUSY) { if (max(abs(LsdsdZ[i][j]),abs(RsdsdZ[i][j])) > 1e-6) { cout << " LsdsdZ[" << i << "][" << j << "] = " << scientific << setw(10) << LsdsdZ[i][j] << " RsdsdZ[" << i << "][" << j << "] = " << scientific << setw(10) << RsdsdZ[i][j] << endl; } if (max(abs(LsusuZ[i][j]),abs(RsusuZ[i][j]))> 1e-6) { cout << " LsusuZ[" << i << "][" << j << "] = " << scientific << setw(10) << LsusuZ[i][j] << " RsusuZ[" << i << "][" << j << "] = " << scientific << setw(10) << RsusuZ[i][j] << endl; } } } } LHmatrixBlock<6> Rsl(slhaPtr->selmix); LHmatrixBlock<3> Rsv(slhaPtr->snumix); // In RPV, the slepton mixing matrices include Higgs bosons // Here we just extract the entries corresponding to the slepton PDG codes // I.e., slepton-Higgs mixing is not supported. // Charged sleptons if (slhaPtr->modsel(4) >= 1 && slhaPtr->rvlmix.exists()) { for (int i=1; i<=6; ++i) for (int j=1; j<=6; ++j) Rsl.set(i,j,slhaPtr->rvlmix(i+1,j+2)); // Check for Higgs-slepton mixing in RVLMIX bool hasCrossTerms = false; for (int i=2; i<=7; ++i) for (int j=1; j<=2; ++j) if (abs(slhaPtr->rvlmix(i,j)) > 1e-5) { hasCrossTerms = true; break; } if (hasCrossTerms) slhaPtr->message(0,"initSUSY", "Note: slepton-Higgs mixing not supported in PYTHIA"); } // Neutral sleptons if (slhaPtr->modsel(4) >= 1 && slhaPtr->rvhmix.exists()) { for (int i=1; i<=3; ++i) for (int j=1; j<=3; ++j) Rsv.set(i,j,slhaPtr->rvhmix(i+2,j+2)); // Check for Higgs-sneutrino mixing in RVHMIX bool hasCrossTerms = false; for (int i=3; i<=7; ++i) for (int j=1; j<=2; ++j) if (abs(slhaPtr->rvhmix(i,j)) > 1e-5) { hasCrossTerms = true; break; } if (hasCrossTerms) slhaPtr->message(0,"initSUSY", "Note: sneutrino-Higgs mixing not supported in PYTHIA"); } if(DBSUSY){ cout<<"Rsl"<modsel(4) >= 1 && slhaPtr->rvnmix.exists()) { ni1=complex( slhaPtr->rvnmix(i+3,4), 0.0 ); ni2=complex( slhaPtr->rvnmix(i+3,5), 0.0 ); ni3=complex( slhaPtr->rvnmix(i+3,6), 0.0 ); ni4=complex( slhaPtr->rvnmix(i+3,7), 0.0 ); ni5=complex( 0.0, 0.0); } else if (!isNMSSM) { ni1=complex( slhaPtr->nmix(i,1), slhaPtr->imnmix(i,1) ); ni2=complex( slhaPtr->nmix(i,2), slhaPtr->imnmix(i,2) ); ni3=complex( slhaPtr->nmix(i,3), slhaPtr->imnmix(i,3) ); ni4=complex( slhaPtr->nmix(i,4), slhaPtr->imnmix(i,4) ); ni5=complex( 0.0, 0.0); } else { ni1=complex( slhaPtr->nmnmix(i,1), slhaPtr->imnmnmix(i,1) ); ni2=complex( slhaPtr->nmnmix(i,2), slhaPtr->imnmnmix(i,2) ); ni3=complex( slhaPtr->nmnmix(i,3), slhaPtr->imnmnmix(i,3) ); ni4=complex( slhaPtr->nmnmix(i,4), slhaPtr->imnmnmix(i,4) ); ni5=complex( slhaPtr->nmnmix(i,5), slhaPtr->imnmnmix(i,5) ); } // Change to positive mass convention complex iRot( 0., 1.); if (slhaPtr->mass(idNeut(i)) < 0.) { ni1 *= iRot; ni2 *= iRot; ni3 *= iRot; ni4 *= iRot; ni5 *= iRot; } // ~chi0 [i] ~chi0 [j] Z : loop over [j] for (int j=1; j<=nNeut; j++) { // neutralino [j] higgsino components complex nj3, nj4; if (slhaPtr->modsel(4) >= 1 && slhaPtr->rvnmix.exists()) { nj3=complex( slhaPtr->rvnmix(i+3,6), 0.0 ); nj4=complex( slhaPtr->rvnmix(i+3,7), 0.0 ); } else if (!isNMSSM) { nj3=complex( slhaPtr->nmix(j,3), slhaPtr->imnmix(j,3) ); nj4=complex( slhaPtr->nmix(j,4), slhaPtr->imnmix(j,4) ); } else { nj3=complex( slhaPtr->nmnmix(j,3), slhaPtr->imnmnmix(j,3) ); nj4=complex( slhaPtr->nmnmix(j,4), slhaPtr->imnmnmix(j,4) ); } // Change to positive mass convention if (slhaPtr->mass(idNeut(j)) < 0.) { nj3 *= iRot; nj4 *= iRot; } // ~chi0 [i] ~chi0 [j] Z : couplings OLpp[i][j] = -0.5 * ni3 * conj(nj3) + 0.5 * ni4 * conj(nj4); ORpp[i][j] = 0.5 * conj(ni3) * nj3 - 0.5 * conj(ni4) * nj4; // tmp: verbose output if (DBSUSY) { cout << " OL'' [" << i << "][" << j << "] = " << scientific << setw(10) << OLpp[i][j] << " OR'' [" << i << "][" << j << "] = " << scientific << setw(10) << ORpp[i][j] << endl; } } // ~chi0 [i] ~chi+ [j] W : loop over [j] for (int j=1; j<=nChar; j++) { // Chargino mixing complex uj1, uj2, vj1, vj2; if (slhaPtr->modsel(4)<1 || !slhaPtr->rvumix.exists()) { uj1=complex( slhaPtr->umix(j,1), slhaPtr->imumix(j,1) ); uj2=complex( slhaPtr->umix(j,2), slhaPtr->imumix(j,2) ); vj1=complex( slhaPtr->vmix(j,1), slhaPtr->imvmix(j,1) ); vj2=complex( slhaPtr->vmix(j,2), slhaPtr->imvmix(j,2) ); } // RPV: ignore lepton-chargino mixing else { uj1=complex( slhaPtr->rvumix(j+3,4), 0.0 ); uj2=complex( slhaPtr->rvumix(j+3,5), 0.0 ); vj1=complex( slhaPtr->rvvmix(j+3,4), 0.0 ); vj2=complex( slhaPtr->rvvmix(j+3,5), 0.0 ); } // ~chi0 [i] ~chi+ [j] W : couplings OL[i][j] = -1.0/sqrt(2.0)*ni4*conj(vj2)+ni2*conj(vj1); OR[i][j] = 1.0/sqrt(2.0)*conj(ni3)*uj2+conj(ni2)*uj1; // tmp: verbose output if (DBSUSY) { cout << " OL [" << i << "][" << j << "] = " << scientific << setw(10) << OL[i][j] << " OR [" << i << "][" << j << "] = " << scientific << setw(10) << OR[i][j] << endl; } } // ~qqX couplings // Quark Charges double ed = -1.0/3.0; double T3d = -0.5; double eu = 2.0/3.0; double T3u = 0.5; // Loop over quark [k] generation for (int k=1;k<=3;k++) { // Set quark masses // Initial guess 0,0,0,mc,mb,mt with the latter from the PDT double mu = particleDataPtr->m0(2*k); double md = particleDataPtr->m0(2*k-1); if (k == 1) { mu=0.0 ; md=0.0; } if (k == 2) { md=0.0 ; mu=0.0; } // Compute running mass from Yukawas and vevs if possible. if (slhaPtr->yd.exists() && slhaPtr->hmix.exists(3)) { double ykk=slhaPtr->yd(k,k); double v1=slhaPtr->hmix(3)/sqrt(1+pow(tanb,2)); if (ykk > 0.0) md = ykk * v1 / sqrt(2.0) ; } if (slhaPtr->yu.exists() && slhaPtr->hmix.exists(3)) { double ykk=slhaPtr->yu(k,k); double v2=slhaPtr->hmix(3)/sqrt(1.0+1.0/pow(tanb,2)); if (ykk > 0.0) mu = ykk * v2 / sqrt(2.0) ; } // tmp: verbose output if (DBSUSY) { cout << " Gen = " << k << " mu = " << mu << " md = " << md << " yUU,DD = " << slhaPtr->yu(k,k) << "," << slhaPtr->yd(k,k) << endl; } // Loop over squark [j] flavour for (int j=1;j<=6;j++) { // Squark mixing complex Rdjk = complex(Rd(j,k), imRd(j,k) ); complex Rdjk3 = complex(Rd(j,k+3),imRd(j,k+3)); complex Rujk = complex(Ru(j,k), imRu(j,k) ); complex Rujk3 = complex(Ru(j,k+3),imRu(j,k+3)); // ~d[j] d[k] ~chi0[i] // Changed according to new notation LsddX[j][k][i] = ((ed-T3d)*sinW*ni1 + T3d*cosW*ni2)*conj(Rdjk) + md*cosW*ni3*conj(Rdjk3)/2.0/mW/cosb; RsddX[j][k][i] = -ed*sinW*conj(ni1)*conj(Rdjk3) + md*cosW*conj(ni3)*conj(Rdjk)/2.0/mW/cosb; // ~u[j] u[k] ~chi0[i] LsuuX[j][k][i] = ((eu-T3u)*sinW*ni1 + T3u*cosW*ni2)*conj(Rujk) + mu*cosW*ni4*conj(Rujk3)/2.0/mW/sinb; RsuuX[j][k][i] = -eu*sinW*conj(ni1)*conj(Rujk3) + mu*cosW*conj(ni4)*conj(Rujk)/2.0/mW/sinb; if (DBSUSY) { if (abs(LsddX[j][k][i]) > 1e-6) { // tmp: verbose output cout << " LsddX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << LsddX[j][k][i] << endl; } if (abs(RsddX[j][k][i]) > 1e-6) { // tmp: verbose output cout << " RsddX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << RsddX[j][k][i] << endl; } if (abs(LsuuX[j][k][i]) > 1e-6) { // tmp: verbose output cout << " LsuuX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << LsuuX[j][k][i] << endl; } if (abs(RsuuX[j][k][i]) > 1e-6) { // tmp: verbose output cout << " RsuuX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << RsuuX[j][k][i] << endl; } } } } // Start slepton couplings // Lepton Charges double el = -1.0; double T3l = -0.5; double ev = 0.0; double T3v = 0.5; // Need to define lepton mass for (int k=1;k<=3;k++) { // Set lepton masses double ml(0.0); if(k==3) ml = particleDataPtr->m0(15); for(int j=1;j<=6;j++){ LsllX[j][k][i] = 0; RsllX[j][k][i] = 0; LsvvX[j][k][i] = 0; RsvvX[j][k][i] = 0; // ~l[j] l[k] ~chi0[i] // Changed according to new notation LsllX[j][k][i] = ((el-T3l)*sinW*ni1 + T3l*cosW*ni2)*Rsl(j,k) + ml*cosW*ni3/2.0/mW/cosb*Rsl(j,k+3); RsllX[j][k][i] = -el*sinW*conj(ni1)*Rsl(j,k+3) + ml*cosW*conj(ni3)/2.0/mW/cosb*Rsl(j,k); if(j<3 && j==k){ // No sneutrino mixing; only left handed // ~v[j] v[k] ~chi0[i] LsvvX[j][k][i] = ((ev-T3v)*sinW*ni1 + T3v*cosW*ni2); } if (DBSUSY) { if (abs(LsllX[j][k][i]) > 1e-6) { // tmp: verbose output cout << " LsllX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << LsllX[j][k][i] << endl; } if (abs(RsllX[j][k][i]) > 1e-6) { // tmp: verbose output cout << " RsllX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << RsllX[j][k][i] << endl; } if (abs(LsvvX[j][k][i]) > 1e-6) { // tmp: verbose output cout << " LsvvX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << LsvvX[j][k][i] << endl; } } } } } // RPV: check for lepton-chargino mixing (not supported) if (slhaPtr->modsel(4) >= 1 && slhaPtr->rvumix.exists()) { bool hasCrossTerms = false; for (int i=1; i<=3; ++i) for (int j=4; j<=5; ++j) if (abs(slhaPtr->rvumix(i,j)) > 1e-5 || abs(slhaPtr->rvvmix(i,j)) > 1e-5) { hasCrossTerms = true; break; } if (hasCrossTerms) slhaPtr->message(1,"initSUSY", "Lepton-Chargino mixing not supported!"); } // Construct ~chi+ couplings // sqrt(2) double rt2 = sqrt(2.0); for (int i=1;i<=nChar;i++) { // Ui1, Ui2, Vi1, Vi2 complex ui1,ui2,vi1,vi2; ui1=complex( slhaPtr->umix(i,1), slhaPtr->imumix(i,1) ); ui2=complex( slhaPtr->umix(i,2), slhaPtr->imumix(i,2) ); vi1=complex( slhaPtr->vmix(i,1), slhaPtr->imvmix(i,1) ); vi2=complex( slhaPtr->vmix(i,2), slhaPtr->imvmix(i,2) ); // ~chi+ [i] ~chi- [j] Z : loop over [j] for (int j=1; j<=nChar; j++) { // Chargino mixing complex uj1, uj2, vj1, vj2; uj1=complex( slhaPtr->umix(j,1), slhaPtr->imumix(j,1) ); uj2=complex( slhaPtr->umix(j,2), slhaPtr->imumix(j,2) ); vj1=complex( slhaPtr->vmix(j,1), slhaPtr->imvmix(j,1) ); vj2=complex( slhaPtr->vmix(j,2), slhaPtr->imvmix(j,2) ); // ~chi+ [i] ~chi- [j] Z : couplings OLp[i][j] = -vi1*conj(vj1) - 0.5*vi2*conj(vj2) + ( (i == j) ? sin2W : 0.0); ORp[i][j] = -conj(ui1)*uj1 - 0.5*conj(ui2)*uj2 + ( (i == j) ? sin2W : 0.0); if (DBSUSY) { // tmp: verbose output cout << " OL' [" << i << "][" << j << "] = " << scientific << setw(10) << OLp[i][j] << " OR' [" << i << "][" << j << "] = " << scientific << setw(10) << ORp[i][j] << endl; } } // Loop over quark [l] flavour for (int l=1;l<=3;l++) { // Set quark [l] masses // Initial guess 0,0,0,mc,mb,mt with the latter from the PDT double mul = particleDataPtr->m0(2*l); double mdl = particleDataPtr->m0(2*l-1); if (l == 1 || l == 2) { mul=0.0 ; mdl=0.0; } // Compute running mass from Yukawas and vevs if possible. if (slhaPtr->yd.exists() && slhaPtr->hmix.exists(3)) { double yll=slhaPtr->yd(l,l); double v1=slhaPtr->hmix(3)/sqrt(1+pow(tanb,2)); if (yll > 0.0) mdl = yll * v1 / sqrt(2.0) ; } if (slhaPtr->yu.exists() && slhaPtr->hmix.exists(3)) { double yll=slhaPtr->yu(l,l); double v2=slhaPtr->hmix(3)/sqrt(1.0+1.0/pow(tanb,2)); if (yll > 0.0) mul = yll * v2 / sqrt(2.0) ; } // Loop over squark [j] flavour for (int j=1;j<=6;j++) { // Loop over off-diagonal quark [k] generation for (int k=1;k<=3;k++) { // Set quark [k] masses // Initial guess 0,0,0,0,mb,mt with the latter from the PDT double muk = particleDataPtr->m0(2*k); double mdk = particleDataPtr->m0(2*k-1); if (k == 1) { muk=0.0 ; mdk=0.0; } if (k == 2) { mdk=0.0 ; muk=0.0; } // Compute running mass from Yukawas and vevs if possible. if (slhaPtr->yd.exists() && slhaPtr->hmix.exists(3)) { double ykk=slhaPtr->yd(k,k); double v1=slhaPtr->hmix(3)/sqrt(1+pow(tanb,2)); if (ykk > 0.0) mdk = ykk * v1 / sqrt(2.0) ; } if (slhaPtr->yu.exists() && slhaPtr->hmix.exists(3)) { double ykk=slhaPtr->yu(k,k); double v2=slhaPtr->hmix(3)/sqrt(1.0+1.0/pow(tanb,2)); if (ykk > 0.0) muk = ykk * v2 / sqrt(2.0) ; } // CKM matrix (use Pythia one if no SLHA) // (NB: could also try input one if no running one found, but // would then need to compute from Wolfenstein) complex Vlk=VCKMgen(l,k); complex Vkl=VCKMgen(k,l); if (slhaPtr->vckm.exists()) { Vlk=complex(slhaPtr->vckm(l,k),slhaPtr->imvckm(l,k)); Vkl=complex(slhaPtr->vckm(k,l),slhaPtr->imvckm(k,l)); } // Squark mixing complex Rdjk = complex(Rd(j,k), imRd(j,k) ); complex Rdjk3 = complex(Rd(j,k+3),imRd(j,k+3)); complex Rujk = complex(Ru(j,k), imRu(j,k) ); complex Rujk3 = complex(Ru(j,k+3),imRu(j,k+3)); // ~d[j] u[l] ~chi+[i] LsduX[j][l][i] += (ui1*conj(Rdjk) - mdk*ui2*conj(Rdjk3)/rt2/mW/cosb)*Vlk; RsduX[j][l][i] -= mul*conj(vi2)*Vlk*conj(Rdjk)/rt2/mW/sinb; // ~u[j] d[l] ~chi+[i] LsudX[j][l][i] += (conj(vi1)*Rujk - muk*conj(vi2)*Rujk3/rt2/mW/sinb)*Vkl; RsudX[j][l][i] -= mdl*ui2*Vkl*Rujk/rt2/mW/cosb; } if (DBSUSY) { if (max(abs(LsduX[j][l][i]),abs(RsduX[j][l][i])) > 1e-6) { // tmp: verbose output cout << " LsduX[" << j << "][" << l << "][" << i << "] = " << scientific << setw(10) << LsduX[j][l][i]; cout << " RsduX[" << j << "][" << l << "][" << i << "] = " << scientific << setw(10) << RsduX[j][l][i] << endl; } if (max(abs(LsudX[j][l][i]),abs(RsudX[j][l][i])) > 1e-6) { // tmp: verbose output cout << " LsudX[" << j << "][" << l << "][" << i << "] = " << scientific << setw(10) << LsudX[j][l][i]; cout << " RsudX[" << j << "][" << l << "][" << i << "] = " << scientific << setw(10) << RsudX[j][l][i] << endl; } } } } // Loop over slepton [j] flavour for (int j=1;j<=6;j++) { for (int k=1;k<=3;k++) { LslvX[j][k][i] = 0.0; RslvX[j][k][i] = 0.0; LsvlX[j][k][i] = 0.0; RsvlX[j][k][i] = 0.0; // Set lepton [k] masses double ml = 0.0; if (k == 3) ml = particleDataPtr->m0(15); if(j==k || j==k+3){ // No lepton mixing // ~l[j] v[l] ~chi+[i] LslvX[j][k][i] += ui1- ml*ui2/rt2/mW/cosb; RslvX[j][k][i] -= ml*conj(vi2)/rt2/mW/sinb; // ~v[j] l[l] ~chi+[i] if(j<=3){ // No right handed sneutrinos LsvlX[j][k][i] += conj(vi1) - ml*conj(vi2)/rt2/mW/sinb; } } if (DBSUSY) { if (max(abs(LslvX[j][k][i]),abs(RslvX[j][k][i])) > 1e-6) { // tmp: verbose output cout << " LslvX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << LslvX[j][k][i]; cout << " RslvX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << RslvX[j][k][i] << endl; } if (max(abs(LsvlX[j][k][i]),abs(RsvlX[j][k][i])) > 1e-6) { // tmp: verbose output cout << " LsvlX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << LsvlX[j][k][i]; cout << " RsvlX[" << j << "][" << k << "][" << i << "] = " << scientific << setw(10) << RsvlX[j][k][i] << endl; } } } } } // SLHA2 compatibility // Check whether scalar particle masses are ordered bool orderedQ = true; bool orderedL = true; for (int j=1;j<=5;j++) { if (particleDataPtr->m0(idSlep(j+1)) < particleDataPtr->m0(idSlep(j))) orderedL = false; if (particleDataPtr->m0(idSup(j+1)) < particleDataPtr->m0(idSup(j))) orderedQ = false; if (particleDataPtr->m0(idSdown(j+1)) m0(idSdown(j))) orderedQ = false; } // If ordered, change sparticle labels to mass-ordered enumeration for (int i=1;i<=6;i++) { ostringstream indx; indx << i; string uName = "~u_"+indx.str(); string dName = "~d_"+indx.str(); string lName = "~e_"+indx.str(); ParticleDataEntry* pdePtr; if (orderedQ) { pdePtr = particleDataPtr->particleDataEntryPtr(idSup(i)); pdePtr->setNames(uName,uName+"bar"); pdePtr = particleDataPtr->particleDataEntryPtr(idSdown(i)); pdePtr->setNames(dName,dName+"bar"); } if (orderedL) { pdePtr = particleDataPtr->particleDataEntryPtr(idSlep(i)); pdePtr->setNames(lName,lName+"bar"); } } // Shorthand for RPV couplings // The input LNV lambda couplings LHtensor3Block<3> rvlle(slhaPtr->rvlamlle); // The input LNV lambda' couplings LHtensor3Block<3> rvlqd(slhaPtr->rvlamlqd); // The input BNV lambda'' couplings LHtensor3Block<3> rvudd(slhaPtr->rvlamudd); isLLE = false; isLQD = false; isUDD = false; // Symmetry properties if(rvlle.exists()){ isLLE = true; for(int i=1;i<=3;i++){ for(int j=i;j<=3;j++){ //lambda(i,j,k)=-lambda(j,i,k) for(int k=1;k<=3;k++){ if(i==j){ rvLLE[i][j][k] = 0.0; }else{ rvLLE[i][j][k] = rvlle(i,j,k); rvLLE[j][i][k] = -rvlle(i,j,k); } } } } } if(rvlqd.exists()){ isLQD=true; for(int i=1;i<=3;i++){ for(int j=1;j<=3;j++){ for(int k=1;k<=3;k++){ rvLQD[i][j][k] = rvlqd(i,j,k); } } } } //lambda''(k,j,i)=-lambda''(k,i,j) if(rvudd.exists()){ isUDD = true; for(int i=1;i<=3;i++){ for(int j=i;j<=3;j++){ for(int k=1;k<=3;k++){ if(i==j){ rvUDD[k][i][j] = 0.0; }else{ rvUDD[k][i][j] = rvudd(k,i,j); rvUDD[k][j][i] = -rvudd(k,i,j); } } } } } if(DBSUSY){ for(int i=1;i<=3;i++){ for(int j=1;j<=3;j++){ for(int k=1;k<=3;k++){ if(rvlle.exists()) cout<<"LambdaLLE["< 0 ) ? 1 : -1; iSup = abs(iSup); if (iSup == 1) id = 1000002; else if (iSup == 2) id = 1000004; else if (iSup == 3) id = 1000006; else if (iSup == 4) id = 2000002; else if (iSup == 5) id = 2000004; else if (iSup == 6) id = 2000006; return sgn*id; } //-------------------------------------------------------------------------- // Return sdown flavour codes int CoupSUSY::idSdown(int iSdown) { int id = 0; int sgn = ( iSdown > 0 ) ? 1 : -1; iSdown = abs(iSdown); if (iSdown == 1) id = 1000001; else if (iSdown == 2) id = 1000003; else if (iSdown == 3) id = 1000005; else if (iSdown == 4) id = 2000001; else if (iSdown == 5) id = 2000003; else if (iSdown == 6) id = 2000005; return sgn*id; } //-------------------------------------------------------------------------- // Function to return slepton flavour codes int CoupSUSY::idSlep(int iSlep) { int id = 0; int sgn = ( iSlep > 0 ) ? 1 : -1; iSlep = abs(iSlep); if (iSlep == 1) id = 1000011; else if (iSlep == 2) id = 1000013; else if (iSlep == 3) id = 1000015; else if (iSlep == 4) id = 2000011; else if (iSlep == 5) id = 2000013; else if (iSlep == 6) id = 2000015; return sgn*id; } //-------------------------------------------------------------------------- // Return a particle name, given the PDG code. string CoupSUSY::getName(int pdgCode) { // Absolute value and corresponding SM code int codeA = abs(pdgCode); int idSM = codeA % 1000000; // Name string name; // Flag to indicate whether SLHA1 or SLHA2 bool slha1 = false; // SM particles if (codeA == idSM) { // Neutrinos if (!slhaPtr->upmns.exists()) slha1=true; if (codeA == 12) name = (slha1) ? "nu_e" : "nu_1"; if (codeA == 14) name = (slha1) ? "nu_mu" : "nu_2"; if (codeA == 16) name = (slha1) ? "nu_tau" : "nu_3"; } // Squarks else if ( idSM <= 6) { // up squarks if (idSM % 2 == 0) { // If SLHA1, return old PDG names if (slhaPtr->stopmix.exists()) slha1 = true; if (codeA == 1000002) name = (slha1) ? "~u_L" : "~u_1"; if (codeA == 1000004) name = (slha1) ? "~c_L" : "~u_2"; if (codeA == 1000006) name = (slha1) ? "~t_1" : "~u_3"; if (codeA == 2000002) name = (slha1) ? "~u_R" : "~u_4"; if (codeA == 2000004) name = (slha1) ? "~c_R" : "~u_5"; if (codeA == 2000006) name = (slha1) ? "~t_2" : "~u_6"; } // down squarks else { // If SLHA1, return old PDG names if (slhaPtr->sbotmix.exists()) slha1 = true; if (codeA == 1000001) name = (slha1) ? "~d_L" : "~d_1"; if (codeA == 1000003) name = (slha1) ? "~s_L" : "~d_2"; if (codeA == 1000005) name = (slha1) ? "~b_1" : "~d_3"; if (codeA == 2000001) name = (slha1) ? "~d_R" : "~d_4"; if (codeA == 2000003) name = (slha1) ? "~s_R" : "~d_5"; if (codeA == 2000005) name = (slha1) ? "~b_2" : "~d_6"; } if (pdgCode < 0) name += "bar"; } // Sleptons else if ( idSM <= 19 ) { // Sneutrinos if (idSM % 2 == 0) { // If SLHA1, return old PDG names if (slhaPtr->staumix.exists()) slha1 = true; if (codeA == 1000012) name = (slha1) ? "~nu_eL" : "~nu_1"; if (codeA == 1000014) name = (slha1) ? "~nu_muL" : "~nu_2"; if (codeA == 1000016) name = (slha1) ? "~nu_tauL" : "~nu_3"; if (codeA == 2000012) name = (slha1) ? "~nu_eR" : "~nu_4"; if (codeA == 2000014) name = (slha1) ? "~nu_muR" : "~nu_5"; if (codeA == 2000016) name = (slha1) ? "~nu_tauR" : "~nu_6"; if (pdgCode < 0) name += "bar"; } // charged sleptons else { // If SLHA1, return old PDG names if (slhaPtr->staumix.exists()) slha1 = true; if (codeA == 1000011) name = (slha1) ? "~e_L" : "~e_1"; if (codeA == 1000013) name = (slha1) ? "~mu_L" : "~e_2"; if (codeA == 1000015) name = (slha1) ? "~tau_1" : "~e_3"; if (codeA == 2000011) name = (slha1) ? "~e_R" : "~e_4"; if (codeA == 2000013) name = (slha1) ? "~mu_R" : "~e_5"; if (codeA == 2000015) name = (slha1) ? "~tau_2" : "~e_6"; if (pdgCode < 0) name += "-"; else name += "+"; } } else if (codeA == 1000021) name = "~g"; else if (codeA == 1000022) name = "~chi_10"; else if (codeA == 1000023) name = "~chi_20"; else if (codeA == 1000024) name = (pdgCode > 0) ? "~chi_1+" : "~chi_1-"; else if (codeA == 1000025) name = "~chi_30"; else if (codeA == 1000035) name = "~chi_40"; else if (codeA == 1000037) name = (pdgCode > 0) ? "~chi_2+" : "~chi_2-"; return name; } //-------------------------------------------------------------------------- // Return neutralino code; zero if not a neutralino int CoupSUSY::typeNeut(int idPDG) { int type = 0; int idAbs = abs(idPDG); if(idAbs == 1000022) type = 1; else if(idAbs == 1000023) type = 2; else if(idAbs == 1000025) type = 3; else if(idAbs == 1000035) type = 4; else if(isNMSSM && idAbs == 1000045) type = 5; return type; } //-------------------------------------------------------------------------- // Check whether particle is a Chargino int CoupSUSY::typeChar(int idPDG) { int type = 0; if(abs(idPDG) == 1000024) type = 1; else if (abs(idPDG) == 1000037)type = 2; return type; } //========================================================================== } // end namespace Pythia8 pythia8-8.1.80.orig/GUIDELINES0000644000175000017500000001105212217346211013702 0ustar sunsun MCNET GUIDELINES for Event Generator Authors and Users PREAMBLE This generator has been developed as part of an academic research project and is the result of many years of work by the authors. Proper academic recognition is a requirement for its continued development. The components of the program have been developed to work together as a coherent physics framework. We believe that the creation of separately maintained forks or piecewise distribution of individual parts would diminish their scientific value. The authors are convinced that software development in a scientific context requires full availability of all source code, to further progress and to allow local modifications to meet the specific requirements of the individual user. Therefore we have decided to release this program under the GNU General Public License (GPL) version 2. This ensures that the source code will be available to you and grants you the freedom to use and modify the program. You can redistribute your modified versions as long as you retain the GPL and respect existing copyright notices (see the file 'COPYING' for details). By using the GPL, we entrust you with considerable freedom and expect you to use it wisely, since the GPL does not address the issues in the first two paragraphs. To remedy this shortcoming, we have formulated the following guidelines relevant for the distribution and usage of event generator software in an academic setting. GUIDELINES 1) The integrity of the program should be respected. ------------------------------------------------- 1.1) Suspected bugs and proposed fixes should be reported back to the original authors to be considered for inclusion in the standard distribution. No independently developed and maintained forks should be created as long as the original authors actively work on the program. 1.2) The program should normally be redistributed in its entirety. When there are special reasons, an agreement should be sought with the original authors to redistribute only specific parts. This should be arranged such that the redistributed parts remain updated in step with the standard distribution. 1.3) Any changes in the code must be clearly marked in the source (reason, author, date) and documented. If any modified version is redistributed it should be stated at the point of distribution (download link) that it has been modified and why. 1.4) If a significant part of the code is used by another program, this should be clearly specified in that program's documentation and stated at its point of distribution. 1.5) Copyright information and references may not be removed. Copyright-related program messages may not be altered and must be printed even if only a part of the program is used. Adding further messages specifying any modifications is encouraged. 2) The program and its physics should be properly cited when used for academic publications ------------------------------------------------------------------ 2.1) The main software reference as designated by the program authors should always be cited. 2.2) In addition, the original literature on which the program is based should be cited to the extent that it is of relevance for a study, applying the same threshold criteria as for other literature. 2.3) When several programs are combined, they should all be mentioned, commensurate with their importance for the physics study at hand. 2.4) To make published results reproducible, the exact versions of the codes that were used and any relevant program and parameter modifications should be spelled out. POSTSCRIPT The copyright license of the software is the GPL v2 alone, therefore the above guidelines are not legally binding. However, we reserve the right to criticize offenders. The guidelines should always be combined with common sense, for interpretation and for issues not covered. Enquiries regarding the guidelines and related issues are encouraged and should be directed to the authors of the program. Please note that the program, including all its code and documentation, is intended for academic use and is delivered "as is" to be used at your own risk, without any guarantees. ---------------------------------------------------------------------- These guidelines were edited by Nils Lavesson and David Grellscheid for the MCnet collaboration, which has approved and agreed to respect them. MCnet is a Marie Curie Research Training Network funded under Framework Programme 6 contract MRTN-CT-2006-035606. pythia8-8.1.80.orig/COPYING0000644000175000017500000004310312217346162013371 0ustar sunsun GNU GENERAL PUBLIC LICENSE Version 2, June 1991 Copyright (C) 1989, 1991 Free Software Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA Everyone is permitted to copy and distribute verbatim copies of this license document, but changing it is not allowed. Preamble The licenses for most software are designed to take away your freedom to share and change it. By contrast, the GNU General Public License is intended to guarantee your freedom to share and change free software--to make sure the software is free for all its users. This General Public License applies to most of the Free Software Foundation's software and to any other program whose authors commit to using it. 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It is safest to attach them to the start of each source file to most effectively convey the exclusion of warranty; and each file should have at least the "copyright" line and a pointer to where the full notice is found. Copyright (C) This program is free software; you can redistribute it and/or modify it under the terms of the GNU General Public License as published by the Free Software Foundation; either version 2 of the License, or (at your option) any later version. This program is distributed in the hope that it will be useful, but WITHOUT ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public License for more details. You should have received a copy of the GNU General Public License along with this program; if not, write to the Free Software Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA. Also add information on how to contact you by electronic and paper mail. If the program is interactive, make it output a short notice like this when it starts in an interactive mode: Gnomovision version 69, Copyright (C) year name of author Gnomovision comes with ABSOLUTELY NO WARRANTY; for details type `show w'. This is free software, and you are welcome to redistribute it under certain conditions; type `show c' for details. The hypothetical commands `show w' and `show c' should show the appropriate parts of the General Public License. Of course, the commands you use may be called something other than `show w' and `show c'; they could even be mouse-clicks or menu items--whatever suits your program. You should also get your employer (if you work as a programmer) or your school, if any, to sign a "copyright disclaimer" for the program, if necessary. Here is a sample; alter the names: Yoyodyne, Inc., hereby disclaims all copyright interest in the program `Gnomovision' (which makes passes at compilers) written by James Hacker. , 1 April 1989 Ty Coon, President of Vice This General Public License does not permit incorporating your program into proprietary programs. If your program is a subroutine library, you may consider it more useful to permit linking proprietary applications with the library. If this is what you want to do, use the GNU Lesser General Public License instead of this License. pythia8-8.1.80.orig/README0000644000175000017500000002546012217346243013224 0ustar sunsun BASIC INSTALLATION 1) Once you have unpacked your tarball into a new (sub)directory, the first step is to run the "configure" script. If you accept the default compiler options, and plan to run PYTHIA 8 standalone, you only have to type "./configure". This will create the file config.mk. Actually, running this script by hand is optional since "make" will run "configure" anyway, but possible errors in the paths will be less clearly visible. 2) Type "gmake" or "make". This will create an archive library. On Linux systems gmake and make are usually equivalent. For others, in case of doubt, use gmake. This applies below as well. 3) The library should now be ready for use. To study some examples, go to the "examples" subdirectory. The README file in that subdirectory contain further instructions how executables can be built and run. 4) At any time, typing "gmake clean" will remove all files related to the library compilation, including the library itself, but it will not reset the configure selections. With "gmake distclean" additionally the configure selection is reset, and many other temporary files are removed. Output files you may have created during your test runs are not affected. (A "gmake clean" is also available in the examples subdirectory, see the README there.) ---------------------------------------------------------------------- ADVANCED INSTALLATION 1) If you want to set various compilation options, or prepare the linking to the HepMC external library then the "configure" script will have to do more work. There are two different ways to accomplish this. 1.1) You can use command-line arguments to set up the desired library links. The possible options are: --help : prints a brief summary of the options described here. --enable-debug : turns on debugging flags and turns off optimization. (This makes program execution much slower. If you later want to switch optimization back on you have to rerun configure without this option, since default is to allow optimization.) --enable-shared : turns on shared-library creation, in addition to the archive libraries always built. --enable-64bits : turns on 64 bits compilation flag (is automatic on many 64-bit installations, but just in case). --lcgplatform=name : allows you to specify the platform assumed for compilation, which also affects the assumed location of the libraries below; default is x86_64-slc5-gcc43-opt while other supported values for name include slc4_ia32_gcc34, slc4_amd64_gcc34 and slc3_ia32_gcc323 (deprecated). --installdir=name : absolute path to a directory where the compiled library and header file directories will be copied, by a "gmake install" command subsequent to the "gmake" one. Note that the files in the current working directory are kept. --prefix=name : equivalent alternative to --installdir=name. --datadir=name : absolute path to a directory where the xmldoc data directory will be copied, by a "gmake install" command subsequent to the "gmake" one. Defaults to the same as --installdir=name if not set separately. --with-hepmc=path : the path to your local copy of the HepMC library. You must use version 2.06 (or later). If the path does not contain the version number you will be warned about it. --with-hepmcversion=v : a simpler alternative to the above, valid if you are using the CERN AFS LCG external area. --enable-gzip : enable support for gzipped LHE file reading --with-boost=path see GZIP SUPPORT section below for --with-zlib=path further details There also are a few environment variables that you can set to force the configuration process or add flags: USRCXXFLAGS : to add flags. Use this variable to add -fPIC to the compilation flags for the static libraries USRLDFLAGSSHARED : to add flags to the shared library build command USRSHAREDSUFFIX : to force shared libraries suffix to be like this (default on MacOSX is dylib). 1.2) If you want to use the external HepMC from some different location, or it is more convenient to put the paths directly into the script, then you have to edit the "configure" file by hand before you run it. Search in the "configure" file for HEPMCLOCATION and provide the paths where you have the respective libraries installed on your local platform. Information on the selected paths is stored in the files config.mk, examples/config.sh and examples/config.csh when you run "./configure". 1.3) The CC and FC global environment variables can be set to specify the C++ and Fortran 77/90 compilers, otherwise set in configure and examples/configure. 2) If you want to change the version of HepMC, you have to rerun the script "configure" with relevant options, then type "make" to recompile the library hepmcinterface. If you tried already to run examples with previous versions, pay attention to the environment variable LD_LIBRARY_PATH (see README in examples). Hints on how to install HepMC from scratch can be found in the separate README.HepMC file. 3) If you have two CPUs or cores on your computer then using the -j2 option on make/gmake may speed up compilation. 4) Necessary data are automatically loaded when you use the default PYTHIA installation directory structure and run the main programs in the examples subdirectory. However, in the general case, you must provide the path to the .xml files, originally stored in the xmldoc directory, where default settings and particle data are found. This can be done in two ways. 4.1) You can set the environment variable PYTHIA8DATA to contain the location of the xmldoc directory. In the csh and tcsh shells this could e.g. be setenv PYTHIA8DATA /home/myname/pythia81xx/xmldoc while in other shells it could be export PYTHIA8DATA=/home/myname/pythia81xx/xmldoc where xx is the subversion number. Recall that environment variables set locally are only defined in the current instance of the shell. The above lines should go into your .cshrc and .bashrc files, respectively, if you want a more permanent assignment. 4.2) You can provide the path as argument to the Pythia constructor in your main program, e.g. Pythia pythia("/home/myname/pythia81xx/xmldoc"); where again xx is the subversion number. When PYTHIA8DATA is set it takes precedence, else the path in the constructor is used, else one defaults to the ../xmldoc directory. ---------------------------------------------------------------------- COMPILING PROGRAMS AGAINST PYTHIA 8 Generally compiling programs against the PYTHIA 8 libraries requires that the PYTHIA 8 header and library directories be specified via the usual -I and -L compiler flags, and that at least the -lpythia8 option be provided to link against the main Pythia8 library. Extra compiler flags will be needed if you are making use of PYTHIA 8's HepMC, LHAPDF, FastJet, and gzipped LHEF features. To make this simpler, and so that an identical compilation recipe can be used with different builds of PYTHIA (e.g. for inclusion in shared Makefiles), a pythia8-config script will be installed into $prefix/bin by the "make install" build target. A typical usage of this script is as follows: g++ myprog.cc -o myprog `pythia8-config --cppflags --libs` The --cppflags option to this script makes pythia8-config write out the necessary -I flags corresponding to the installed headers, and --libs adds the required -L and -l flags. If gzip support is enabled, flags for its extra Boost/zlib dependencies will be automatically included. Adding an extra --hepmc flag will additionally include the required flags for building with HepMC support. Adding --lhapdf will _disable_ the inclusion of the lhapdfdummy library to avoid link-time clashing with LHAPDF itself. FastJet and LHAPDF provide their own *-config scripts, so compiling a complex program which uses PYTHIA 8 with HepMC and LHAPDF support, and which makes use of FastJet, can use a compilation command similar to this: g++ myprog.cc -o myprog `pythia8-config --cppflags --libs --hepmc --lhapdf` \ `lhapdf-config --cppflags --ldflags` `fastjet-config --cxxflags --libs` The pythia8-config script may also be used at runtime to generate the data directory environment variable if needed, e.g.: PYTHIA8DATA=`pythia8-config --xmldoc` ./myprog ---------------------------------------------------------------------- GZIP SUPPORT (experimental) The '--enable-gzip' options turns on support for the reading of gzipped LHE files. It relies upon Boost and zlib to function, and the locations of these must be set with the '--with-boost=boost_path' and '--with-zlib=zlib_path' options. Specifically, it requires (note that .so should be replaced with .dylib for Mac OS X): boost_path/include/boost/iostreams/ (with the appropriate files in this directory) boost_path/lib/libboost_iostreams.so (or boost_path/lib64/...) zlib_path/libz.so The zlib library may not be necessary when linking against PYTHIA using shared libraries. Note that when compiling a final PYTHIA executable, these libraries must also be included, e.g.: -Lboost_path/lib -lboost_iostreams -Lzlib_path -lz This is done automatically for the examples in the 'examples' and 'rootexamples' directories when gzip support is enabled. When running the executable, if the Boost and zlib libraries are in a non-standard directory, the LD_LIBRARY_PATH (DYLD_LIBRARY_PATH for Mac OS X) must be set to include these directories, e.g. in a bash-type shell: export LD_LIBRARY_PATH=$LD_LIBRARY_PATH:boost_path/lib:zlib_path Gzip support currently switches off the '-Wshadow' compiler option to avoid the possibility of a large number of warning messages. ---------------------------------------------------------------------- FOR WINDOWS USERS The Makefile.msc file is intended for use on Win32/NMAKE systems with the Microsoft Visual C/C++ compiler. This alternative installation is not the development platform, however, and therefore not as well tested. Not all parts of the above installation procedure are the same, so some experimentation may be required. A few suggestions are found in the the separate README.Win32 file. ---------------------------------------------------------------------- LEARN MORE To learn more about the current program: A) A brief self-contained introduction is found in the htmldoc/pythia8100.pdf file. B) Details can be found by opening a web browser on the htmldoc/Welcome.html file, and then navigating among the pages in the index there. ---------------------------------------------------------------------- pythia8-8.1.80.orig/CODINGSTYLE0000644000175000017500000003650712217346162014057 0ustar sunsunCoding Style This file is only intended for contributors of code to Pythia 8. As a normal user you need not read it. A reasonably consistent coding style enhances readability and understanding of code, so do take the time to make new code blend smoothly with the existing structure. That said, complete consistency is impossible, and style must always come second to content. So any rules should be applied with common sense. Remember to update the xmldoc documentation in parallel with the code updates. The xml rules are provided after the coding rules. ----------------------------------------------------------------------- For the Pythia8 code some principles have been used, some by deliberate decision, while others evolved organically. An incomplete list is as follows. 1. Use existing files to get a feel for the general outlay. (Especially the "core" files that have set the standard for later writing, e.g. Pythia, Event, or Basics.) 2. Use standard C++, in a clear and consistent manner. Do not show off by using special tricks that only experts will appreciate. Do not use any experimental language features. 3. English is the only allowed language (for comments, variable names, etc.). 4. Lines should be at most 79 characters long, so that they do not overflow when opened in an 80 characters wide text editor window. This number includes any trailing blanks, another "feature" that should be avoided. 5. Never make code dependent on the presence of external libraries. Some libraries, like LHAPDF and HepMC are already interfaced, but only in well-defined non-critical manners. If you want to include interfaces to new libraries, or modify the existing ones, you should bring it up for open discussion beforehand. 6. The underscore "character" should be avoided as far as possible; it makes code difficult to read. See also point 24. Currently it is only used in headers, for #ifndef Pythia8_filename_H. 7. Extra code used for debugging purposes, or left behind from the development process, even if commented out, should be removed from the public version. Feel free to save your own private versions where such code is available. 8. Begin each code file with // (filename) is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. to establish the legal structure. Follow that with specific information on authorship of the particular file, where relevant, and a very brief summary of the contents. After that follow with #include and other preprocessor commands and namespace Pythia8 {, before the actual code. 9. Use lines //========================================================================== to separate classes from each other, and from top and bottom material of a file, that does not belong to a class. 10. Use lines //-------------------------------------------------------------------------- for smaller subdivisions than above. Specifically, in .cc files, insert it between the different methods that belong to the same class. 11. Blank lines should be used to separate the code into suitable chunks of statements that belong together. Never use two or more blank lines consecutively, however. 12. Begin each code chunk with one or more comment lines that explains the purpose of this chunk. Do not overdo documentation, however: the purpose is to provide overview, not clutter. 13. Comment lines may also precede a particularly crucial statement inside a code chunk, without the need for a blank line before. 14. Do not add comments on the same line as a statement: a = b + c; // No comment here! 15. Write comments in terms of (cryptic but) correct English, with relevant punctuation. 16. Do not use /* .... */ : not for code because all such code should have been removed in the first place (point 7), and not for comments since intent is more obvious if all comment lines begin with //. 17. Indent two further steps for each new logical substructure (loops, conditional statements, etc.). The namespace {, public: and private: are exceptions to this rule, requiring no extra indentation. 18. Do not use tabs for formatting; it may give a mess when read by another user. 19. Use exactly one space to separate logical structures and operators: if (a == b) then { If readibility can be improved by lining up nearby statements then this is allowed to take precedence, however: int iNew = 0; double pm = 0.; 20. One area of inconsistency is whether a blank is used after ( or not: void status(int statusIn) {statusSave = statusIn;} virtual void set1Kin( double x1in, double x2in, double sHin); If there is a thought, it is that for short constructions a blank tends to unnecessarily break up the structure, while for longer ones such breaks are necessary to gain overview. Similarly ( ( may often be used to give better structure than ((. 21. Allow several statements on the same line in header files, since operations here should be simple and short. Avoid it in .cc files, where one may want to more carefully study the logical structure, and could more easily miss statements that way. 22. Do not use pointers more than you absolutely need to. For most usage a reference is much nicer, but unfortunetely it cannot be saved. If you need a pointer, have its name end with Ptr, so it is easily recognized. In declarations the * goes with the pointer type: Info* infoPtr; rather than e.g. Info *infoPtr. 23. Class names should begin with a capital letter, whereas instances of this class begin lowercase. Also methods and local variable names should begin lowercase. Only static const VARIABLENAME are given in uppercase throughout. 24. Use capitalization inside a word to help reading, e.g. pAbs, toCMframe, useNewBeamShape, skipInit. Descriptive names are helpful, but don't make them longer than they have to (thisVariableSumsAllDiagonalMatrixElements is better replaced by sumDiag). 25. It is useful if index names begin with an i (or j, k if several are needed) and sizes with an n. 26. Pick ++i instead of i++, unless the latter is intentional. Recall that ++i is updated at the point it is encountered, while i++ implies it need only be updated after other operations have taken place, which can be confusing. 27. Use int for all integers, except where potential overflow warrants long, and avoid unsigned integers. 28. Use double for all real variables. 29. Use the Pythia complex type for all complex variables, defined by typedef std::complex complex; in PythiaComplex.h 30. Use the Pythia Vec4 class for four-vectors. 31. Use string for all text, except when C++ leaves you no option but to use char or char*, e.g. for the name of a file to be opened. 32. Use the Boolean operators &&, || and !, not the alternative old cleartext "and", "or" and "not". 33. Do not use cast notation where function style is possible, i.e. int i = int(r); rather than int i = (int)r;. 34. Do not use typedef (except in point 29 above). 35. Units of GeV for energies and mm for distances are implicit, with c = 1 so the same units can be used for momentum, mass and time. 36. If an expression needs to be split over lines, let the new line begin with an operator, so that the reason for several lines is apparent: double sum = a + b + c + d + e + f + g; alternatively double sum = a + b + c + d + e + f + g; (i.e. lined-up or indented-two-steps, whatever is most convenient). 37. Be very restrictive with output from your methods. Some limited initialization info may be relevant, but desist if you can. During running printing should either be located in special methods that the user has to call explicitly (with ostream& os = cout as last argument) or, for error messages, make use of the Info::errorMsg(..) method. 38. No global variables. It should be possible to have several instances of Pythia running without any risk of interference between them. 39. Do not have a { on a line of its own, but allow a lone } at the very end of the conditions/loops (or, for longer pieces of code, at the end of each conditions case): if (isCharged) { statements; } else { more statements; } 40. Use the standard constant M_PI for the value of pi = 3.141592... 41. Use pow2(double), pow3(double), pow4(double), pow5(double) and pow6(double) for small positive integer powers, since the standard pow(double, double) can be very slow for such operations. 42. The event record, both the process and event ones, are always passed as references rather than pointers. This allows notation like event[i].p() rather than (*eventPtr)[i].p(); note that eventPtr[i]->p() is not allowed C++ notation. 43. Use standard names for some of the other class instances, like infoPtr, particleDataPtr, rndmPtr, beamAPtr, beamBPtr, couplingsPtr, partonSystemsPtr, userHooksPtr, etc..The Settings database is normally only interrogated during initializations, so is usually passad as reference settings rather than pointer settingsPtr. 44. Only use == and != for comparisons between two pointers, or a pointer and 0. Thus comparisons like (Xptr > 0) are forbidden. ----------------------------------------------------------------------- Remember to update the xmldoc documentation in parallel with the code updates. All the details should make it directly into the respective webpage, with UpdateHistory.xml only giving a very brief summary. (This is different from Pythia 6, where the update notes had to be complete.) The xml notes are not intended to be read by users, who instead will access the html and php equivalents. The translation from xml to html and php is done with a specially written conversion program. This program is not distributed with the code, to avoid abuse by users, but will be run from time to time. The program handles a set of new tags, and additionally you can use many standard html ones, which are passed on without any action. Outlined below is the set of xml tags in current use, that are covered by a translation program. Also a few other open issues. We try to stick with xml rules, e.g. ... for pair and for single (=combined begin+end). Note that the parsing of the conversion program assumes a "sensible" layout of the text. A) Standard html concepts:

      a top-level header;

      a subheader;

      a subsubheader;

      a subsubsubheader;
      a new line;

      a new paragraph;

        an ordered list, with
      1. items;
          a bulleted list, with
        • items;
        • an item in an ordered or bulleted list;
          a definition list (used for references);
          a definition term in a definition list;
          a definition text in a definition list; boldface; italics - will be used for typesetting formulae so avoid for text; inline computer code (teletype font);
           a piece of code, with linebreaks as formatted (teletype font); 
           anchor;
           : only used in Welcome.xml;
           : only used in Welcome.xml;
          ... only used in Index.xml;
           and  around SaveSettings dialog box.
          
          B) New concepts for simple markup (no interactivity):
           a large chunk of text, 
              stored as one single xml file;
           text to be displayed on a separate line, centered if possible 
              (a poor man's equation), maybe typeset in italics ();
           inline variant of above;
           text begun on new line, in boldface;
           text begun, no linebreak, in boldface;
           name of a program file (new paragraph, boldface);
           information on a specific class,
              specifically the class creation command form;
           explanation of a class method;
           a class method to be listed closely
              together with the previous one, since they belong together;
           an argument of 
              the class creation or another method in the class, optionally 
              with a default value:
           further explanation of an 
              allowed option of an argument.   
          
          C) New concepts for user interaction in php files (but no interactivity 
          in html):
           
              reference to an article; replaced by [...] and anchor;
           
              anchor among local pages; automatically fills with file type and
              target="page";
           
              anchor from Index.xml to other files; automatically fills with 
              file type and target="page";
           
              a switch to be used in the event generation; in php shown with 
              radio buttons to pick on (= yes, true) or off (= no, false), 
              written to file as a line with name = value; 
          
              ditto but no interactivity;
          
              an integer value to be used in the event generation; in php
              shown as a dialogue box where an integer can be typed in, and
              written to file as a line with name = value; the min and max values 
              are optional; 
          
              an integer value to be used in the event generation; unlike modeopen 
              above there is a fixed set of 
              a discrete set of options for a , see above;
          
              ditto but no interactivity;
          
              a double-precision value to be used in the event generation; in php
              shown as a dialogue box where a real number can be typed in, and
              written to file as a line with name = value; the min and max values 
              are optional; 
          
              ditto but no interactivity;
          
              a character string, without blanks, to be used in the event generation
              mainly for file names; in php shown as a dialogue box where text can be 
              typed in, and written to file as a line with name = value;
          
              ditto but no interactivity;
          
          D) New concepts that could one day be made interactive, but currently 
          are not:
          
              the properties of a particle, most of which are optional;
          
              the properties of a decay channel; this tag can only appear inside a
              ... block; the meMode field is optional; the
              products appear as a blank-separated list.
          pythia8-8.1.80.orig/phpdoc/0000755000175000017500000000000012217346243013612 5ustar  sunsunpythia8-8.1.80.orig/phpdoc/BeamShape.php0000644000175000017500000001052612217615312016150 0ustar  sunsun
          
          Beam Shape
          
          
          
          
          
          
          SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Beam Shape

          The ";?>Beam Parameters page explains how you can set a momentum spread of the two incoming beams, and a spread and offset for the location of the interaction vertex. The spread is based on a simple parametrization in terms of independent Gaussians, however, which is likely to be too primitive for realistic applications.

          It is therefore possible to define your own class, derived from the BeamShape base class, and hand it in to Pythia with the ";?> pythia.setBeamShapePtr( BeamShape*) method. Below we describe what such a class has to do. An explicit toy example is shown in main23.cc.

          The BeamShape base class has a very simple structure. It only has two main virtual methods. The first, init(), is used for initialization. The second, pick(), selects beam momentum and production vertex in the current event.

          BeamShape::BeamShape()  
          virtual BeamShape::~BeamShape()  
          the constructor and destructor do not need to do anything.

          virtual void BeamShape::init( Settings& settings, Rndm* rndmPtrIn)  
          the base-class method simply reads in the relevant values stored in the Settings data base, and saves a pointer to the random-number generator. You are free to write your own derived initialization routine, or use the existing one. In the latter case you can then give your own modified interpretation to the beam spread parameters defined there.
          The two flags Beams:allowMomentumSpread and Beams:allowVertexSpread should not be tampered with, however. These are checked elsewhere to determine whether the beam shape should be set or not, whereas the other momentum-spread and vertex-spread parameters are local to this class.

          virtual void BeamShape::pick()  
          this method is the key one to supply in the derived class. Here you are free to pick whatever parametrization you desire for beam momenta and vertex position, including correlations between the two. At the end of the day, you should set a few protected double numbers:
          deltaPxA, deltaPyA, deltaPzA for the three-momentum shift of the first incoming beam, relative to the nominal values;
          deltaPxB, deltaPyB, deltaPzB for the three-momentum shift of the second incoming beam, relative to the nominal values;
          vertexX, vertexY, vertexZ, vertexT for the production-vertex position and time.
          As usual, momentum is given in GeV, and space and time in mm, with c = 1.

          Vec4 BeamShape::deltaPA()  
          Vec4 BeamShape::deltaPB()  
          read out the three-momentum shifts for beams A and B that were set by pick(). The energy components are put to zero at this stage, since they are most conveniently calculated after the original and the shift three-momenta have been added.

          Vec4 BeamShape::vertex()  
          read out the production-vertex position and time that were set by pick(). pythia8-8.1.80.orig/phpdoc/ASecondHardProcess.php0000644000175000017500000005731412217615312020003 0ustar sunsun A Second Hard Process SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          A Second Hard Process

          When you have selected a set of hard processes for hadron beams, the ";?>multiparton interactions framework can add further interactions to build up a realistic underlying event. These further interactions can come from a wide variety of processes, and will occasionally be quite hard. They do represent a realistic random mix, however, which means one cannot predetermine what will happen. Occasionally there may be cases where one wants to specify also the second hard interaction rather precisely. The options on this page allow you to do precisely that.

          SecondHard:generate On Off   (default = off)
          Generate two hard scatterings in a collision between hadron beams. The hardest process can be any combination of internal processes, available in the normal ";?>process selection machinery, or external input. Here you must further specify which set of processes to allow for the second hard one, see the following.

          Process Selection

          In principle the whole ";?>process selection allowed for the first process could be repeated for the second one. However, this would probably be overkill. Therefore here a more limited set of prepackaged process collections are made available, that can then be further combined at will. Since the description is almost completely symmetric between the first and the second process, you always have the possibility to pick one of the two processes according to the complete list of possibilities.

          Here comes the list of allowed sets of processes, to combine at will:

          SecondHard:TwoJets On Off   (default = off)
          Standard QCD 2 -> 2 processes involving gluons and d, u, s, c, b quarks.

          SecondHard:PhotonAndJet On Off   (default = off)
          A prompt photon recoiling against a quark or gluon jet.

          SecondHard:TwoPhotons On Off   (default = off)
          Two prompt photons recoiling against each other.

          SecondHard:Charmonium On Off   (default = off)
          Production of charmonium via colour singlet and colour octet channels.

          SecondHard:Bottomonium On Off   (default = off)
          Production of bottomonium via colour singlet and colour octet channels.

          SecondHard:SingleGmZ On Off   (default = off)
          Scattering q qbar -> gamma^*/Z^0, with full interference between the gamma^* and Z^0.

          SecondHard:SingleW On Off   (default = off)
          Scattering q qbar' -> W^+-.

          SecondHard:GmZAndJet On Off   (default = off)
          Scattering q qbar -> gamma^*/Z^0 g and q g -> gamma^*/Z^0 q.

          SecondHard:WAndJet On Off   (default = off)
          Scattering q qbar' -> W^+- g and q g -> W^+- q'.

          SecondHard:TopPair On Off   (default = off)
          Production of a top pair, either via QCD processes or via an intermediate gamma^*/Z^0 resonance.

          SecondHard:SingleTop On Off   (default = off)
          Production of a single top, either via a t- or an s-channel W^+- resonance.

          A further process collection comes with a warning flag:

          SecondHard:TwoBJets On Off   (default = off)
          The q qbar -> b bbar and g g -> b bbar processes. These are already included in the TwoJets sample above, so it would be double-counting to include both, but we assume there may be cases where the b subsample will be of special interest. This subsample does not include flavour-excitation or gluon-splitting contributions to the b rate, however, so, depending on the topology if interest, it may or may not be a good approximation.

          Cuts and scales

          The second hard process obeys exactly the same selection rules for ";?>phase space cuts and ";?>couplings and scales as the first one does. Specifically, a pTmin cut for 2 -> 2 processes would apply to the first and the second hard process alike, and ballpark half of the time the second could be generated with a larger pT than the first. (Exact numbers depending on the relative shape of the two cross sections.) That is, first and second is only used as an administrative distinction between the two, not as a physics ordering one.

          Optionally it is possible to pick the mass and pT ";?>phase space cuts separately for the second hard interaction. The main application presumably would be to allow a second process that is softer than the first, but still hard. But one is also free to make the second process harder than the first, if desired. So long as the two pT (or mass) ranges overlap the ordering will not be the same in all events, however.

          Cross-section calculation

          As an introduction, a brief reminder of Poissonian statistics. Assume a stochastic process in time, for now not necessarily a high-energy physics one, where the probability for an event to occur at any given time is independent of what happens at other times. Then the probability for n events to occur in a finite time interval is
          P_n = <n>^n exp(-<n>) / n!
          where <n> is the average number of events. If this number is small we can approximate exp(-<n>) = 1 , so that P_1 = <n> and P_2 = <n>^2 / 2 = P_1^2 / 2.

          Now further assume that the events actually are of two different kinds a and b, occurring independently of each other, such that <n> = <n_a> + <n_b>. It then follows that the probability of having one event of type a (or b) and nothing else is P_1a = <n_a> (or P_1b = <n_b>). From
          P_2 = (<n_a> + <n_b>)^2 / 2 = (P_1a + P_1b)^2 / 2 = (P_1a^2 + 2 P_1a P_1b + P_1b^2) / 2
          it is easy to read off that the probability to have exactly two events of kind a and none of b is P_2aa = P_1a^2 / 2 whereas that of having one a and one b is P_2ab = P_1a P_1b. Note that the former, with two identical events, contains a factor 1/2 while the latter, with two different ones, does not. If viewed in a time-ordered sense, the difference is that the latter can be obtained two ways, either first an a and then a b or else first a b and then an a.

          To translate this language into cross-sections for high-energy events, we assume that interactions can occur at different pT values independently of each other inside inelastic nondiffractive (sometimes equated with "minbias") events. Then the above probabilities translate into P_n = sigma_n / sigma_ND where sigma_ND is the total nondiffractive cross section. Again we want to assume that exp(-<n>) is close to unity, i.e. that the total hard cross section above pTmin is much smaller than sigma_ND. The hard cross section is dominated by QCD jet production, and a reasonable precaution is to require a pTmin of at least 20 GeV at LHC energies. (For 2 -> 1 processes such as q qbar -> gamma^*/Z^0 (-> f fbar) one can instead make a similar cut on mass.) Then the generic equation P_2 = P_1^2 / 2 translates into sigma_2/sigma_ND = (sigma_1 / sigma_ND)^2 / 2 or sigma_2 = sigma_1^2 / (2 sigma_ND).

          Again different processes a, b, c, ... contribute, and by the same reasoning we obtain sigma_2aa = sigma_1a^2 / (2 sigma_ND), sigma_2ab = sigma_1a sigma_1b / sigma_ND, and so on.

          There is one important correction to this picture: all collisions do no occur under equal conditions. Some are more central in impact parameter, others more peripheral. This leads to a further element of variability: central collisions are likely to have more activity than the average, peripheral less. Integrated over impact parameter standard cross sections are recovered, but correlations are affected by a "trigger bias" effect: if you select for events with a hard process you favour events at small impact parameter which have above-average activity, and therefore also increased chance for further interactions. (In PYTHIA this is the origin of the "pedestal effect", i.e. that events with a hard interaction have more underlying activity than the level found in minimum-bias events.) When you specify a matter overlap profile in the multiparton-interactions scenario, such an enhancement/depletion factor f_impact is chosen event-by-event and can be averaged during the course of the run. As an example, the double Gaussian form used in Tune A gives approximately <f_impact> = 2.5. The above equations therefore have to be modified to sigma_2aa = <f_impact> sigma_1a^2 / (2 sigma_ND), sigma_2ab = <f_impact> sigma_1a sigma_1b / sigma_ND. Experimentalists often instead use the notation sigma_2ab = sigma_1a sigma_1b / sigma_eff, from which we see that PYTHIA "predicts" sigma_eff = sigma_ND / <f_impact>. When the generation of multiparton interactions is switched off it is not possible to calculate <f_impact> and therefore it is set to unity.

          When this recipe is to be applied to calculate actual cross sections, it is useful to distinguish three cases, depending on which set of processes are selected to study for the first and second interaction.

          (1) The processes a for the first interaction and b for the second one have no overlap at all. For instance, the first could be TwoJets and the second TwoPhotons. In that case, the two interactions can be selected independently, and cross sections tabulated for each separate subprocess in the two above classes. At the end of the run, the cross sections in a should be multiplied by <f_impact> sigma_1b / sigma_ND to bring them to the correct overall level, and those in b by <f_impact> sigma_1a / sigma_ND.

          (2) Exactly the same processes a are selected for the first and second interaction. In that case it works as above, with a = b, and it is only necessary to multiply by an additional factor 1/2. A compensating factor of 2 is automatically obtained for picking two different subprocesses, e.g. if TwoJets is selected for both interactions, then the combination of the two subprocesses q qbar -> g g and g g -> g g can trivially be obtained two ways.

          (3) The list of subprocesses partly but not completely overlap. For instance, the first process is allowed to contain a or c and the second b or c, where there is no overlap between a and b. Then, when an independent selection for the first and second interaction both pick one of the subprocesses in c, half of those events have to be thrown, and the stored cross section reduced accordingly. Considering the four possible combinations of first and second process, this gives a
          sigma'_1 = sigma_1a + sigma_1c * (sigma_2b + sigma_2c/2) / (sigma_2b + sigma_2c)
          with the factor 1/2 for the sigma_1c sigma_2c term. At the end of the day, this sigma'_1 should be multiplied by the normalization factor
          f_1norm = <f_impact> (sigma_2b + sigma_2c) / sigma_ND
          here without a factor 1/2 (or else it would have been double-counted). This gives the correct
          (sigma_2b + sigma_2c) * sigma'_1 = sigma_1a * sigma_2b + sigma_1a * sigma_2c + sigma_1c * sigma_2b + sigma_1c * sigma_2c/2
          The second interaction can be handled in exact analogy.

          For the considerations above it is assumed that the phase space cuts are the same for the two processes. It is possible to set the mass and transverse momentum cuts differently, however. This changes nothing for processes that already are different. For two collisions of the same type it is partly a matter of interpretation what is intended. If we consider the case of the same process in two non-overlapping phase space regions, most likely we want to consider them as separate processes, in the sense that we expect a factor 2 relative to Poissonian statistics from either of the two hardest processes populating either of the two phase space regions. In total we are therefore lead to adopt the same strategy as in case (3) above: only in the overlapping part of the two allowed phase space regions could two processes be identical and thus appear with a 1/2 factor, elsewhere the two processes are never identical and do not include the 1/2 factor. We reiterate, however, that the case of partly but not completely overlapping phase space regions for one and the same process is tricky, and not to be used without prior deliberation.

          The listing obtained with the pythia.statistics() already contain these corrections factors, i.e. cross sections are for the occurrence of two interactions of the specified kinds. There is not a full tabulation of the matrix of all the possible combinations of a specific first process together with a specific second one (but the information is there for the user to do that, if desired). Instead pythia.statistics() shows this matrix projected onto the set of processes and associated cross sections for the first and the second interaction, respectively. Up to statistical fluctuations, these two sections of the pythia.statistics() listing both add up to the same total cross section for the event sample.

          There is a further special feature to be noted for this listing, and that is the difference between the number of "selected" events and the number of "accepted" ones. Here is how that comes about. Originally the first and second process are selected completely independently. The generation (in)efficiency is reflected in the different number of initially tried events for the first and second process, leading to the same number of selected events. While acceptable on their own, the combination of the two processes may be unacceptable, however. It may be that the two processes added together use more energy-momentum than kinematically allowed, or, even if not, are disfavoured when the PYTHIA approach to provide correlated parton densities is applied. Alternatively, referring to case (3) above, it may be because half of the events should be thrown for identical processes. Taken together, it is these effects that reduced the event number from "selected" to "accepted". (A further reduction may occur if a ";?>user hook rejects some events.)

          It is allowed to use external Les Houches Accord input for the hardest process, and then pick an internal one for the second hardest. In this case PYTHIA does not have access to your thinking concerning the external process, and cannot know whether it overlaps with the internal or not. (External events q qbar' -> e+ nu_e could agree with the internal W ones, or be a W' resonance in a BSM scenario, to give one example.) Therefore the combined cross section is always based on the scenario (1) above. Corrections for correlated parton densities are included also in this case, however. That is, an external event that takes a large fraction of the incoming beam momenta stands a fair chance of being rejected when it has to be combined with another hard process. For this reason the "selected" and "accepted" event numbers are likely to disagree.

          In the cross section calculation above, the sigma'_1 cross sections are based on the number of accepted events, while the f_1norm factor is evaluated based on the cross sections for selected events. That way the suppression by correlations between the two processes does not get to be double-counted.

          The pythia.statistics() listing contains two final lines, indicating the summed cross sections sigma_1sum and sigma_2sum for the first and second set of processes, at the "selected" stage above, plus information on the sigma_ND and <f_impact> used. The total cross section generated is related to this by
          <f_impact> * (sigma_1sum * sigma_2sum / sigma_ND) * (n_accepted / n_selected)
          with an additional factor of 1/2 for case 2 above.

          The error quoted for the cross section of a process is a combination in quadrature of the error on this process alone with the error on the normalization factor, including the error on <f_impact>. As always it is a purely statistical one and of course hides considerably bigger systematic uncertainties.

          Event information

          Normally the process event record only contains the hardest interaction, but in this case also the second hardest is stored there. If both of them are 2 -> 2 ones, the first would be stored in lines 3 - 6 and the second in 7 - 10. For both, status codes 21 - 29 would be used, as for a hardest process. Any resonance decay chains would occur after the two main processes, to allow normal parsing. The beams in 1 and 2 only appear in one copy. This structure is echoed in the full event event record.

          Most of the properties accessible by the ";?>pythia.info methods refer to the first process, whether that happens to be the hardest or not. The code and pT scale of the second process are accessible by the info.codeMPI(1) and info.pTMPI(1), however.

          The sigmaGen() and sigmaErr() methods provide the cross section and its error for the event sample as a whole, combining the information from the two hard processes as described above. In particular, the former should be used to give the weight of the generated event sample. The statistical error estimate is somewhat cruder and gives a larger value than the subprocess-by-subprocess one employed in pythia.statistics(), but this number is anyway less relevant, since systematical errors are likely to dominate. "?>

          pythia8-8.1.80.orig/phpdoc/ElectroweakProcesses.php0000644000175000017500000005122412217615312020457 0ustar sunsun Electroweak Processes SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Electroweak Processes

          This page contains processes involving Prompt-photon, gamma^*/Z^0 and W^+- production, plus a few with t-channel boson exchange.

          Prompt photon processes

          This group collects the processes where one or two photons are produced by the hard process. Additional sources of photons include parton showers and hadron decays. A pT cut is required to stay away from the unphysical low-pT region. An eikonalized description, intended to be valid at all pT, is included as part of the multiparton-interactions framework.

          PromptPhoton:all On Off   (default = off)
          Common switch for the group of all prompt photon processes, as listed separately in the following.

          PromptPhoton:qg2qgamma On Off   (default = off)
          Scattering q g -> q gamma. Code 201.

          PromptPhoton:qqbar2ggamma On Off   (default = off)
          Scattering q qbar -> g gamma. Code 202.

          PromptPhoton:gg2ggamma On Off   (default = off)
          Scattering g g -> g gamma.
          Note: This is a box graph. The full quark-mass dependence in the loop leads to very complicated expressions. The current implementation is based on assuming five massless quarks (see below), and thus is questionable at small (pT < m_b) or large (pT > m_t) transverse momenta. Code 203.

          PromptPhoton:ffbar2gammagamma On Off   (default = off)
          Scattering q qbar -> gamma gamma. Code 204.

          PromptPhoton:gg2gammagamma On Off   (default = off)
          Scattering g g -> gamma gamma.
          Note: This is a box graph. The full quark-mass dependence in the loop leads to very complicated expressions. The current implementation is based on assuming five massless quarks (see below), and thus is questionable at small (pT < m_b) or large (pT > m_t) transverse momenta. Code 205.

          PromptPhoton:nQuarkLoop   (default = 5; minimum = 3; maximum = 6)
          Number of quark flavours included in the box graphs responsible for g g -> g gamma and g g-> gamma gamma processes. Owing to the complexity if the massive expressions, quarks are treated as massless. The default value should be applicable in the range of transverse momenta above the b mass but below the t one.

          Weak boson processes

          Under this heading we group processes involving the production of a single electroweak gauge boson, i.e. a gamma^*/Z^0 or a W^+-, or a pair of them, or one of them in combination with a parton. Since the three sets are partly conflicting, each is associated with its own group flag. In addition, t-channel exchange of such a boson between two fermions form a separate group.

          There is one flag that can be used to influence the gamma^*/Z^0 structure in all the processes below where it is produced, unless otherwise stated.

          WeakZ0:gmZmode   (default = 0; minimum = 0; maximum = 2)
          Choice of full gamma^*/Z^0 structure or not in relevant processes.
          0 : full gamma^*/Z^0 structure, with interference included.
          1 : only pure gamma^* contribution.
          2 : only pure Z^0 contribution.

          Note: irrespective of the option used, the particle produced will always be assigned code 23 for Z^0, and open decay channels is purely dictated by what is set for the Z^0.

          Boson exchange

          The two processes in this subgroup is included as part of the multiparton-interactions framework.

          WeakBosonExchange:all On Off   (default = off)
          Common switch for the group of gamma^*/Z^0 or W^+- exchange between two fermions.

          WeakBosonExchange:ff2ff(t:gmZ) On Off   (default = off)
          Scattering f f' -> f f' via
          gamma^*/Z^0
          t-channel exchange, with full interference between the gamma^* and Z^0. Code 211.

          WeakBosonExchange:ff2ff(t:W) On Off   (default = off)
          Scattering f_1 f_2 -> f_3 f_4 via
          W^+-
          t-channel exchange. Code 212.

          Single boson



          WeakSingleBoson:all On Off   (default = off)
          Common switch for the group of a single gamma^*/Z^0 or W^+- production.

          WeakSingleBoson:ffbar2gmZ On Off   (default = off)
          Scattering f fbar -> gamma^*/Z^0, with full interference between the gamma^* and Z^0. Code 221.

          WeakSingleBoson:ffbar2W On Off   (default = off)
          Scattering f fbar' -> W^+-. Code 222.

          WeakSingleBoson:ffbar2ffbar(s:gm) On Off   (default = off)
          Scattering f fbar -> gamma^* -> f' fbar'. Subset of process 221, but written as a 2 -> 2 process, so that pT can be used as ordering variable, e.g. in multiparton interactions. Hardcoded for the final state being either of the five quark flavours or three lepton ones. Not included in the WeakSingleBoson:all set, but included in the multiparton-interactions framework. Code 223.

          Boson pair

          Note that, in the decay of the two vector bosons produced by an f fbar -> V V process, the full four-fermion correlations from the leading-order f fbar -> V V -> 4f matrix elements are included [Gun86] (with some extensions by the authors). The matrix elements are provided in the double-resonant approach, i.e. excludes graph like f fbar -> V -> f fbar -> f fbar V -> 4f.

          WeakDoubleBoson:all On Off   (default = off)
          Common switch for the group of pair production of gamma^*/Z^0 and W^+-.

          WeakDoubleBoson:ffbar2gmZgmZ On Off   (default = off)
          Scattering f fbar' -> gamma^*/Z^0 gamma^*/Z^0. Code 231.

          WeakDoubleBoson:ffbar2ZW On Off   (default = off)
          Scattering f fbar' -> Z^0 W^+-. Note that here the gamma^* contribution is not (currently) included. Code 232.

          WeakDoubleBoson:ffbar2WW On Off   (default = off)
          Scattering f fbar -> W^+ W^-. Code 233.

          Boson and parton



          WeakBosonAndParton:all On Off   (default = off)
          Common switch for the group of production of a single electroweak gauge boson, i.e. a gamma^*/Z^0 or a W^+-, in association with a parton, i.e. a quark, gluon, photon or lepton. These processes give first-order corrections to the ones in the WeakSingleBoson class, and both sets cannot be used simultaneously without unphysical double-counting. The current class should only be used to study the high-pT tail of the gauge-boson production processes (for LHC applications at least pT > 20 GeV), while the ones in WeakSingleBoson should be used for inclusive production.

          WeakBosonAndParton:qqbar2gmZg On Off   (default = off)
          Scattering q qbar -> gamma^*/Z^0 g. Code 241.

          WeakBosonAndParton:qg2gmZq On Off   (default = off)
          Scattering q g -> gamma^*/Z^0 q . Code 242.

          WeakBosonAndParton:ffbar2gmZgm On Off   (default = off)
          Scattering f fbar -> gamma^*/Z^0 gamma. Code 243.

          WeakBosonAndParton:fgm2gmZf On Off   (default = off)
          Scattering f gamma -> gamma^*/Z^0 f. Code 244.

          WeakBosonAndParton:qqbar2Wg On Off   (default = off)
          Scattering q qbar -> W^+- g. Code 251.

          WeakBosonAndParton:qg2Wq On Off   (default = off)
          Scattering q g -> W^+- q. Code 252.

          WeakBosonAndParton:ffbar2Wgm On Off   (default = off)
          Scattering f fbar -> W^+- gamma. Code 253.

          WeakBosonAndParton:fgm2Wf On Off   (default = off)
          Scattering f gamma -> W^+- f. Code 254.

          Photon Collision Processes

          A few electroweak two-photon production processes are available. To use them, photon PDFs have to be defined for the incoming beam particles. For proton beams an appropriate set would be MRST QED 2004 [Mar05], available in the LHAPDF library.

          PhotonCollision:all On Off   (default = off)
          Common switch for the group of six processes presented below.

          PhotonCollision:gmgm2qqbar On Off   (default = off)
          Scatterings gamma gamma -> q qbar, where q is a light quark (u, d, s) . Code 261.

          PhotonCollision:gmgm2ccbar On Off   (default = off)
          Scattering gamma gamma -> c cbar. Code 262.

          PhotonCollision:gmgm2bbbar On Off   (default = off)
          Scattering gamma gamma -> b bbar. Code 263.

          PhotonCollision:gmgm2ee On Off   (default = off)
          Scattering gamma gamma -> e+ e-. Code 264.

          PhotonCollision:gmgm2mumu On Off   (default = off)
          Scattering gamma gamma -> mu+ mu-. Code 265.

          PhotonCollision:gmgm2tautau On Off   (default = off)
          Scattering gamma gamma -> tau+ tau-. Code 266. "?>
          pythia8-8.1.80.orig/phpdoc/EventRecord.php0000644000175000017500000006557512217615312016561 0ustar sunsun The Event Record SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          The Event Record

          A Pythia instance contains two members of the Event class. The one called process provides a brief summary of the main steps of the hard process, while the one called event contains the full history. The user would normally interact mainly with the second one, so we will exemplify primarily with that one.

          The Event class to first approximation is a vector of Particles, so that it can expand to fit the current event size. The index operator is overloaded, so that e.g. event[i] corresponds to the i'th particle of the object event. Thus event[i].id() returns the identity of the i'th particle, and so on. Therefore the methods of the ";?>Particle class are at least as essential as those of the Event class itself.

          As used inside PYTHIA, some conventions are imposed on the structure of the event record. Entry 0 of the vector<Particle> is used to represent the event as a whole, with its total four-momentum and invariant mass, but does not form part of the event history. Lines 1 and 2 contains the two incoming beams, and only from here on history tracing works as could be expected. That way unassigned mother and daughter indices can be put 0 without ambiguity. Depending on the task at hand, a loop may therefore start at index 1 rather than 0 without any loss. Specifically, for translation to other event record formats such as HepMC [Dob01], where the first index is 1, the Pythia entry 0 definitely ought to be skipped in order to minimize the danger of indexing errors.

          In the following we will list the methods available. Only a few of them have a function to fill in normal user code.

          Basic output methods

          Some methods are available to read out information on the current event record:

          Particle& Event::operator[](int i)  
          const Particle& Event::operator[](int i)  
          returns a (const) reference to the i'th particle in the event record, which can be used to get (or set) all the ";?>properties of this particle.

          Particle& Event::front()  
          Particle& Event::at(int i)  
          Particle& Event::back()  
          returns a reference to the zeroth, i'th or last particle in the event record, as an alternative to the methods above.

          int Event::size()  
          The event size, i.e. the size of the vector<Particle>. Thus valid particles, to be accessed by the above indexing operator, are stored in the range 0 <= i < size(). See comment above about the (ir)relevance of entry 0.

          void Event::list()  
          void Event::list(ostream& os)  
          void Event::list(bool showScaleAndVertex, bool showMothersAndDaughters = false)  
          void Event::list(bool showScaleAndVertex, bool showMothersAndDaughters, ostream& os)  
          Provide a listing of the whole event, i.e. of the vector<Particle>. The methods with fewer arguments call the final one with the respective default values, and are non-inlined so they can be used in a debugger. The basic identity code, status, mother, daughter, colour, four-momentum and mass data are always given, but the methods can also be called with a few optional arguments for further information:
          argument showScaleAndVertex (default = false) : optionally give a second line for each particle, with the production scale (in GeV), the particle polarization (dimensionless), the production vertex (in mm or mm/c) and the invariant lifetime (also in mm/c).
          argument showMothersAndDaughters (default = false) : gives a list of all daughters and mothers of a particle, as defined by the motherList(i) and daughterList(i) methods described below. It is mainly intended for debug purposes.
          argument os (default = cout) : a reference to the ostream object to which the event listing will be directed.

          Each Particle has two mother and two daughter indices. These may be used to encode zero, one, two or more mothers/daughters, depending on the combination of values and status code, according to well-defined ";?>rules. The two methods below can do this job easier for you.

          vector<int> Event::motherList(int i)  
          returns a vector of all the mother indices of the particle at index i. This list is empty for entries 0, 1 and 2, i.e. the "system" in line 0 is not counted as part of the history. Normally the list contains one or two mothers, but it can also be more, e.g. in string fragmentation the whole fragmenting system is counted as mothers to the primary hadrons. Many particles may have the same motherList. Mothers are listed in ascending order.

          vector<int> Event::daughterList(int i)  
          returns a vector of all the daughter indices of the particle at index i. This list is empty for a particle that did not decay (or, if the evolution is stopped early enough, a parton that did not branch), while otherwise it can contain a list of varying length, from one to many. For the two incoming beam particles, all shower initiators and beam remnants are counted as daughters, with the one in slot 0 being the one leading up to the hardest interaction. The "system" in line 0 does not have any daughters, i.e. is not counted as part of the history. Many partons may have the same daughterList. Daughters are listed in ascending order.

          int Event::statusHepMC(int i)  
          returns the status code according to the HepMC conventions agreed in February 2009. This convention does not preserve the full information provided by the internal PYTHIA status code, as obtained by Particle::status(), but comes reasonably close. The allowed output values are:

          • 0 : an empty entry, with no meaningful information and therefore to be skipped unconditionally (should not occur in PYTHIA);
          • 1 : a final-state particle, i.e. a particle that is not decayed further by the generator (may also include unstable particles that are to be decayed later, as part of the detector simulation);
          • 2 : a decayed Standard Model hadron or tau or mu lepton, excepting virtual intermediate states thereof (i.e. the particle must undergo a normal decay, not e.g. a shower branching);
          • 3 : a documentation entry (not used in PYTHIA);
          • 4 : an incoming beam particle;
          • 11 - 200 : an intermediate (decayed/branched/...) particle that does not fulfill the criteria of status code 2, with a generator-dependent classification of its nature; in PYTHIA the absolute value of the normal status code is used.

          Further output methods

          The above methods are the main ones that a normal user would make frequent use of. There are some further methods that also could come in handy, in the exploration of the history of an event, but where the outcome is not always obvious if one is not familiar with the detailed structure of an event record.

          int Event::iTopCopy(int i)  
          int Event::iBotCopy(int i)  
          are used to trace carbon copies of the particle at index i up to its top mother or down to its bottom daughter. If there are no such carbon copies, i itself will be returned. A carbon copy is when the "same" particle appears several times in the event record, but with changed momentum owing to recoil effects.

          int Event::iTopCopyId(int i)  
          int Event::iBotCopyId(int i)  
          also trace top mother and bottom daughter, but do not require carbon copies, only that one can find an unbroken chain, of mothers or daughters, with the same flavour id code. When it encounters ambiguities, say a g -> g g branching or a u u -> u u hard scattering, it will stop the tracing and return the current position. It can be confused by nontrivial flavour changes, e.g. a hard process u d -> d u by W^+- exchange will give the wrong answer. These methods therefore are of limited use for common particles, in particular for the gluon, but should work well for "rare" particles.

          vector<int> Event::sisterList(int i)  
          returns a vector of all the sister indices of the particle at index i, i.e. all the daughters of the first mother, except the particle itself.

          vector<int> Event::sisterListTopBot(int i,bool widenSearch = true)  
          returns a vector of all the sister indices of the particle at index i, tracking up and back down through carbon copies if required. That is, the particle is first traced up with iTopCopy() before its mother is found, and then all the particles in the daughterList() of this mother are traced down with iBotCopy(), omitting the original particle itself. Any non-final particles are removed from the list. Should this make the list empty the search criterion is widened so that all final daughters are allowed, not only carbon-copy ones. That is, starting from the top mother, all its daughters are found, except for the traced-up one, and then all their daughters, and so on. This can produce quite extensive and rather useless output, notably when tracing parton showers. A second argument false inhibits the second step, and increases the risk that an empty list is returned. A typical example of this is for ISR cascades, e.g. e -> e gamma where the photon may not have any obvious sister in the final state if the bottom copy of the photon is an electron that annihilates and thus is not part of the final state.

          bool Event::isAncestor(int i, int iAncestor)  
          traces the particle i upwards through mother, grandmother, and so on, until either iAncestor is found or the top of the record is reached. Normally one unique mother is required, as is the case e.g. in decay chains or in parton showers, so that e.g. the tracing through a hard scattering would not work. For hadronization, first-rank hadrons are identified with the respective string endpoint quark, which may be useful e.g. for b physics, while higher-rank hadrons give false. Currently also ministrings that collapsed to one single hadron and junction topologies give false.

          One data member in an Event object is used to keep track of the largest col() or acol() colour tag set so far, so that new ones do not clash.

          Event:startColTag   (default = 100; minimum = 0; maximum = 1000)
          This sets the initial colour tag value used, so that the first one assigned is startColTag + 1, etc. The Les Houches accord [Boo01] suggests this number to be 500, but 100 works equally well.

          void Event::initColTag(int colTag = 0)  
          forces the current colour tag value to be the larger of the input colTag and the above Event:startColTag values.

          int Event::lastColTag()  
          returns the current maximum colour tag.

          int Event::nextColTag()  
          increases the current maximum colour tag by one and returns this new value. This method is used whenever a new colour tag is needed.

          Many event properties are accessible via the Info class, ";?>see here. Since they are used directly in the event generation, a few are stored directly in the Event class, however.

          void Event::scale( double scaleIn)  
          double Event::scale()  
          set or get the scale (in GeV) of the hardest process in the event. Matches the function of the scale variable in the ";?>Les Houches Accord.

          void Event::scaleSecond( double scaleSecondIn)  
          double Event::scaleSecond()  
          set or get the scale (in GeV) of a second hard process in the event, in those cases where such a one ";?>has been requested.

          Constructors and modifications of the event record

          Although you would not normally need to create your own Event instance, there may be times where that could be convenient. The typical example would be if you want to create a new event record that is the sum of a few different ones, e.g. if you want to simulate pileup events. There may also be cases where you want to add one or a few particles to an existing event record.

          Event::Event(int capacity = 100)  
          creates an empty event record, but with a reserved size capacity for the Particle vector.

          Event& Event::operator=(const Event& oldEvent)  
          copies the input event record.

          Event& Event::operator+=(const Event& addEvent)  
          appends an event to an existing one. For the appended particles mother, daughter and colour tags are shifted to make a consistent record. The zeroth particle of the appended event is not copied, but the zeroth particle of the combined event is updated to the full energy-momentum content.

          void Event::init(string headerIn = "", ParticleData* particleDataPtrIn = 0, int startColTagIn = 100)  
          initializes colour, the pointer to the particle database, and the header specification used for the event listing. We remind that a Pythia object contains two event records process and event. Thus one may e.g. call either pythia.process.list() or pythia.event.list(). To distinguish those two rapidly at visual inspection, the "Pythia Event Listing" header is printed out differently, in one case adding "(hard process)" and in the other "(complete event)". When += is used to append an event, the modified event is printed with "(combination of several events)" as a reminder.

          void Event::clear()  
          empties event record. Specifically the Particle vector size is reset to zero.

          void Event::reset()  
          empties the event record, as clear() above, but then fills the zero entry of the Particle vector with the pseudoparticle used to represent the event as a whole. At this point the pseudoparticle is not assigned any momentum or mass.

          void Event::popBack(int n = 1)  
          removes the last n particle entries; must be a positive number. History (and other) information of remaning entries is untouched, and so may be internally inconsistent.

          void Event::remove(int iFirst, int iLast)  
          removes particles in the range between indices iFirst and iLast, including the endpoints. History (and other) information of remaning entries is untouched, and so may be internally inconsistent.

          bool Event::undoDecay(int i)  
          removes the decay chain of the particle i and thus restores it to its undecayed state. It is only intended for "normal" particle decay chains, and will return false in other cases, notably if the particle is coloured. The procedure would not work if non-local momentum shifts have been performed, such as with a Bose-Einstein shift procedure (or for a dipole shower recoiler). The history information of the remaining particles, many of which may have new indices, is updated to be internally consistent.

          int Event::append(Particle entryIn)  
          appends a particle to the bottom of the event record and returns the index of this position.

          int Event::append(int id, int status, int mother1, int mother2, int daughter1, int daughter2, int col, int acol, double px, double py, double pz, double e, double m = 0., double scale = 0., double pol = 9.)  
          appends a particle to the bottom of the event record and returns the index of this position; ";?>see here for the meaning of the various particle properties.

          int Event::append(int id, int status, int mother1, int mother2, int daughter1, int daughter2, int col, int acol, Vec4 p, double m = 0., double scale = 0., double pol = 9.)  
          appends a particle to the bottom of the event record and returns the index of this position, as above but with four-momentum as a Vec4.

          int Event::append(int id, int status, int col, int acol, double px, double py, double pz, double e, double m = 0., double scale = 0., double pol = 9.)  
          int Event::append(int id, int status, int col, int acol, Vec4 p, double m = 0., double scale = 0., double pol = 9.)  
          appends a particle to the bottom of the event record and returns the index of this position, as above but with vanishing (i.e. zero) mother and daughter indices.

          int Event::setEvtPtr(int iSet = -1)  
          send in the this pointer of the current Event itself to the particle iSet, by default the most recently appended particle. Also generates a pointer to the ParticleDataEntry object of the identity code of the particle.

          int Event::copy(int iCopy, int newStatus = 0)  
          copies the existing particle in entry iCopy to the bottom of the event record and returns the index of this position. By default, i.e. with newStatus = 0, everything is copied precisely as it is, which means that history information has to be modified further by hand to make sense. With a positive newStatus, the new copy is set up to be the daughter of the old, with status code newStatus, while the status code of iCopy is negated. With a negative newStatus, the new copy is instead set up to be the mother of iCopy. An attempt to copy an out-of-range entry will return -1.

          void Event::restorePtrs()  
          each particle in the event record has a pointer to the event itself and another to the particle species it belongs to. The latter pointer is automatically set/changed whenever the particle identity is set/changed by one of the normal methods. Of course the pointer values are specific to the memory locations of the current run, and so it has no sense to save them if events are written to file. Should you use some persistency scheme that bypasses the normal methods when the event is read back in, you can use restorePtrs() afterwards to set these pointers appropriately.

          A few methods exist to rotate and boost events. These derive from the ";?>Vec4 methods, and affect both the momentum and the vertex (position) components of all particles.

          void Event::rot(double theta, double phi)  
          rotate all particles in the event by this polar and azimuthal angle (expressed in radians).

          void Event::bst(double betaX, double betaY, double betaZ)  
          void Event::bst(double betaX, double betaY, double betaZ, double gamma)  
          void Event::bst(const Vec4& vec)  
          boost all particles in the event by this three-vector. Optionally you may provide the gamma value as a fourth argument, which may help avoid roundoff errors for big boosts. You may alternatively supply a Vec4 four-vector, in which case the boost vector becomes beta = p/E.

          void Event::rotbst(const RotBstMatrix& M)  
          rotate and boost by the combined action encoded in the ";?>RotBstMatrix M.

          The Junction Class

          The event record also contains a vector of junctions, which often is empty or else contains only a very few per event. Methods are available to add further junctions or query the current junction list. This is only for the expert user, however, and is not discussed further here, but only the main points.

          A junction stores the properties associated with a baryon number that is fully resolved, i.e. where three different colour indices are involved. There are two main applications,

          1. baryon beams, where at least two valence quarks are kicked out, and so the motion of the baryon number is nontrivial;
          2. baryon-number violating processes, e.g. in SUSY with broken R-parity.
          Information on junctions is set, partly in the process generation, partly in the beam remnants machinery, and used by the fragmentation routines, but the normal user does not have to know the details.

          For each junction, information is stored on the kind of junction, and on the three (anti)colour indices that are involved in the junction. The possibilities foreseen are:

          • kind = 1 : incoming colourless particle to three outgoing colours (e.g. baryon beam remnant or neutralino -> q q q);
          • kind = 2 : incoming colourless particle to three outgoing anticolours;
          • kind = 3 : one incoming anticolour (stored first) and two outgoing colours (e.g. antisquark decaying to two quarks, or gluino decay to three quarks);
          • kind = 4 : one incoming colour (stored first) and two outgoing anticolours (e.g. squark decaying to two antiquarks, or gluino decaying to three antiquarks);
          • kind = 5 : two incoming anticolours (stored first) and one outgoing colour (e.g. resonant squark production through RPV);
          • kind = 6 : two incoming colours (stored first) and one outgoing anticolour (e.g. resonant antisquark production through RPV);
          The odd (even) kind codes corresponds to a +1 (-1) change in baryon number across the junction.

          The kind and colour information in the list of junctions can be set or read with methods of the Event class, but are not of common interest and so not described here.

          A listing of current junctions can be obtained with the listJunctions() method.

          Subsystems

          Separate from the event record as such, but closely tied to it is the ";?>PartonSystems class, which mainly stores the parton indices of incoming and outgoing partons, classified by collision subsystem. Such information is needed to interleave multiparton interactions, initial-state showers and final-state showers, and append beam remnants. It could also be used in other places. It is intended to be accessed only by experts, such as implementors of ";?>new showering models. "?>
          pythia8-8.1.80.orig/phpdoc/SemiInternalResonances.php0000644000175000017500000003154312217615312020740 0ustar sunsun Semi-Internal Resonances SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Semi-Internal Resonances

          The introduction of a new ";?> semi-internal process may also involve a new particle, not currently implemented in PYTHIA. Often it is then enough to use the ";?>standard machinery to introduce a new particle (id:all = ...) and new decay channels (id:addChannel = ...). By default this only allows you to define a fixed total width and fixed branching ratios. Using ";?>meMode values 100 or bigger provides the possibility of a very simple threshold behaviour.

          If you want to have complete freedom, however, there are two ways to go. One is that you make the resonance decay part of the hard process itself, either using the ";?>Les Houches interface or a semi-internal process. The other is for you to create a new ResonanceWidths object, where you write the code needed for a calculation of the partial width of a particular channel.

          Here we will explain what is involved in setting up a resonance. Should you actually go ahead with this, it is strongly recommended to use an existing resonance as a template, to get the correct structure. There also exists a sample main program, main22.cc, that illustrates how you could combine a new process and a new resonance.

          There are three steps involved in implementing a new resonance:
          1) providing the standard particle information, as already outlined above (id:all = ..., id:addChannel = ...), except that now branching ratios need not be specified, since they anyway will be overwritten by the dynamically calculated values.
          2) writing the class that calculates the partial widths.
          3) handing in a pointer to an instance of this class to PYTHIA.
          We consider the latter two aspects in turn.

          The ResonanceWidths Class

          The resonance-width calculation has to be encoded in a new class. The relevant code could either be put before the main program in the same file, or be stored separately, e.g. in a matched pair of .h and .cc files. The latter may be more convenient, in particular if the calculations are lengthy, or likely to be used in many different runs, but of course requires that these additional files are correctly compiled and linked.

          The class has to be derived from the ResonanceWidths base class. It can implement a number of methods. The constructor and the calcWidth ones are always needed, while others are for convenience. Much of the administrative machinery is handled by methods in the base class.

          Thus, in particular, you must implement expressions for all possible final states, whether switched on in the current run or not, since all contribute to the total width needed in the denominator of the Breit-Wigner expression. Then the methods in the base class take care of selecting only allowed channels where that is required, and also of including effects of closed channels in secondary decays. These methods can be accessed indirectly via the ";?>res... methods of the normal ";?>particle database.

          A constructor for the derived class obviously must be available. Here you are quite free to allow a list of arguments, to set the parameters of your model. The constructor must call the base-class initBasic(idResIn) method, where the argument idResIn is the PDG-style identity code you have chosen for the new resonance. When you create several related resonances as instances of the same class you would naturally make idResIn an argument of the constructor; for the PYTHIA classes this convention is used also in cases when it is not needed.
          The initBasic(...) method will hook up the ResonanceWidths object with the corresponding entry in the generic particle database, i.e. with the normal particle information you set up in point 1) above. It will store, in base-class member variables, a number of quantities that you later may find useful:
          idRes : the identity code you provide;
          hasAntiRes : whether there is an antiparticle;
          mRes : resonance mass;
          GammaRes resonance width;
          m2Res : the squared mass;
          GamMRat : the ratio of width to mass.

          A destructor is only needed if you plan to delete the resonance before the natural end of the run, and require some special behaviour at that point. If you call such a destructor you will leave a pointer dangling inside the Pythia object you gave it in to, if that still exists.

          void ResonanceWidths::initConstants()  
          is called once during initialization, and can then be used to set up further parameters specific to this particle species, such as couplings, and perform calculations that need not be repeated for each new event, thereby saving time. This method needs not be implemented.

          void ResonanceWidths::calcPreFac(bool calledFromInit = false)  
          is called once a mass has been chosen for the resonance, but before a specific final state is considered. This routine can therefore be used to perform calculations that otherwise might have to be repeated over and over again in calcWidth below. It is optional whether you want to use this method, however, or put everything in calcWidth().
          The optional argument will have the value true when the resonance is initialized, and then be false throughout the event generation, should you wish to make a distinction. In PYTHIA such a distinction is made for gamma^*/Z^0 and gamma^*/Z^0/Z'^0, owing to the necessity of a special description of interference effects, but not for other resonances.
          In addition to the base-class member variables already described above, mHat contains the current mass of the resonance. At initialization this agrees with the nominal mass mRes, but during the run it will not (in general).

          void ResonanceWidths::calcWidth(bool calledFromInit = false)  
          is the key method for width calculations and returns a partial width value, as further described below. It is called for a specific final state, typically in a loop over all allowed final states, subsequent to the calcPreFac(...) call above. Information on the final state is stored in a number of base-class variables, for you to use in your calculations:
          iChannel : the channel number in the list of possible decay channels;
          mult : the number of decay products;
          id1, id2, id3 : the identity code of up to the first three decay products, arranged in descending order of the absolute value of the identity code;
          id1Abs, id2Abs, id3Abs : the absolute value of the above three identity codes;
          mHat : the current resonance mass, which is the same as in the latest calcPreFac(...) call;
          mf1, mf2, mf3 : masses of the above decay products;
          mr1, mr2, mr3 : squared ratio of the product masses to the resonance mass;
          ps : is only meaningful for two-body decays, where it gives the phase-space factor ps = sqrt( (1. - mr1 - mr2)^2 - 4. * mr1 * mr2 );
          In two-body decays the third slot is zero for the above properties. Should there be more than three particles in the decay, you would have to take care of the subsequent products yourself, e.g. using
          particlePtr->decay[iChannel].product(j);
          to extract the j'th decay products (with j = 0 for the first, etc.). Currently we are not aware of any such examples.
          The base class also contains methods for alpha_em and alpha_strong evaluation, and can access many standard-model couplings; see the existing code for examples.
          The result of your calculation should be stored in
          widNow : the partial width of the current channel, expressed in GeV.

          double ResonanceWidths::widthChan( double mHat, int idAbs1, int idAbs2)  
          is not normally used. In PYTHIA the only exception is Higgs decays, where it is used to define the width (except for colour factors) associated with a specific incoming/outgoing state. It allows the results of some loop expressions to be pretabulated.

          bool ResonanceWidths::allowCalc()  
          can normally be left dummy (and then always returns true) but can optionally be used to determine whether to force dynamical width calculation to be switched off (return false). An example is provided by the SUSYResonanceWidths class, in which the implementation of this method checks for the existence of SLHA decay tables for the particular resonance in question, and checks if those tables should be given precedence over the internal width calculation.

          bool ResonanceWidths::initBSM()  
          can normally be left dummy, but for advanced implementations it provides a possibility to initialize data members of the derived class at a very early stage during initialization, before any of the other members are called. An example is provided by the SUSYResonanceWidths class, in which an internal pointer to a derived Couplings class must be (re)set before any of the other methods are used. A return value of false can be used to signal that this initialization step failed.

          Access to resonance widths

          Once you have implemented a class, it is straightforward to make use of it in a run. Assume you have written a new class MyResonance, which inherits from ResonanceWidths. You then create an instance of this class and hand it in to a pythia object with
                ResonanceWidths* myResonance = new MyResonance();
                pythia.setResonancePtr( myResonance); 
          
          If you have several resonances you can repeat the procedure any number of times. When pythia.init(...) is called these resonances are initialized along with all the internal resonances, and treated in exactly the same manner. See also the ";?>Program Flow description.

          If the code should be of good quality and general usefulness, it would be simple to include it as a permanently available process in the standard program distribution. The final step of that integration ought to be left for the PYTHIA authors, but basically all that is needed is to add one line in ParticleData::initResonances, where one creates an instance of the resonance in the same way as for the resonances already there. In addition, the particle data and decay table for the new resonance has to be added to the permanent ";?>particle database, and the code itself to include/ResonanceWidths.h and src/ResonanceWidths.cc. pythia8-8.1.80.orig/phpdoc/LesHouchesAccord.php0000644000175000017500000012124212217615312017477 0ustar sunsun Les Houches Accord SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Les Houches Accord

          The Les Houches Accord (LHA) for user processes [Boo01] is the standard way to input parton-level information from a matrix-elements-based generator into PYTHIA. The conventions for which information should be stored has been defined in a Fortran context, as two commonblocks. Here a C++ equivalent is defined, as a single class.

          The LHAup class is a base class, containing reading and printout functions, plus two pure virtual functions, one to set initialization information and one to set information on each new event. Derived classes have to provide these two virtual functions to do the actual work. The existing derived classes are for reading information from a Les Houches Event File (LHEF), from the respective Fortran commonblocks, or from PYTHIA 8 itself.

          You are free to write your own derived classes, using the rules and methods to be described below. Normally, pointers to objects of such derived classes should be handed in with the ";?>Pythia::init( LHAup*) method. However, with the LHEF format a filename can replace the pointer, see further below.

          Let us now describe the methods at your disposal to do the job.

          LHAup::LHAup( int strategy = 3)  
          the base class constructor takes the choice of mixing/weighting strategy as optional input argument, and calls setStrategy, see below. It also reserves some space for processes and particles.

          virtual LHAup::~LHAup()  
          the destructor does not need to do anything.

          void LHAup::setPtr(Info* infoPtr)  
          this method only sets the pointer that allows some information to be accessed, and is automatically called by Pythia::init(...).

          Initialization

          The LHAup class stores information equivalent to the /HEPRUP/ commonblock, as required to initialize the event generation chain. The main difference is that the vector container now allows a flexible number of subprocesses to be defined. For the rest, names have been modified, since the 6-character-limit does not apply, and variables have been regrouped for clarity, but nothing fundamental is changed.

          virtual bool LHAup::setInit()  
          this pure virtual method has to be implemented in the derived class, to set relevant information when called. It should return false if it fails to set the info.

          Inside setInit(), such information can be set by the following methods:

          void LHAup::setBeamA( int identity, double energy, int pdfGroup, int pdfSet)  
          void LHAup::setBeamB( int identity, double energy, int pdfGroup, int pdfSet)  
          sets the properties of the first and second incoming beam, respectively (cf. the Fortran IDBMUP(1), EBMUP(i), PDFGUP(i), PDFSUP(i), with i 1 or 2). The parton distribution information defaults to zero. These numbers can be used to tell which PDF sets were used when the hard process was generated, while the normal ";?>PDF Selection is used for the further event generation in PYTHIA.

          void LHAup::setStrategy( int strategy)  
          sets the event weighting and cross section strategy. The default, provided in the class constructor, is 3, which is the natural value e.g. for an LHEF.
          argument strategy : chosen strategy (cf. IDWTUP; see [Sjo06] section 9.9.1 for extensive comments).
          argumentoption 1 : events come with non-negative weight, given in units of pb, with an average that converges towards the cross section of the process. PYTHIA is in charge of the event mixing, i.e. for each new try decides which process should be generated, and then decides whether is should be kept, based on a comparison with xMax. Accepted events therefore have unit weight.
          argumentoption -1 : as option 1, except that cross sections can now be negative and events after unweighting have weight +-1. You can use ";?>Info::weight() to find the weight of the current event. A correct event mixing requires that a process that can take both signs should be split in two, one limited to positive or zero and the other to negative or zero values, with xMax chosen appropriately for the two.
          argumentoption 2 : events come with non-negative weight, in unspecified units, but such that xMax can be used to unweight the events to unit weight. Again PYTHIA is in charge of the event mixing. The total cross section of a process is stored in xSec.
          argumentoption -2 : as option 2, except that cross sections can now be negative and events after unweighting have weight +-1. As for option -1 processes with indeterminate sign should be split in two.
          argumentoption 3 : events come with unit weight, and are thus accepted as is. The total cross section of the process is stored in xSec.
          argumentoption -3 : as option 3, except that events now come with weight +-1. Unlike options -1 and -2 processes with indeterminate sign need not be split in two, unless you intend to mix with internal PYTHIA processes (see below).
          argumentoption 4 : events come with non-negative weight, given in units of pb, with an average that converges towards the cross section of the process, like for option 1. No attempt is made to unweight the events, however, but all are generated in full, and retain their original weight. For consistency with normal PYTHIA units, the weight stored in Info::weight() has been converted to mb, however.
          argumentoption -4 : as option 4, except that events now can come either with positive or negative weights.
          Note 1: if several processes have already been mixed and stored in a common event file, either LHEF or some private format, it would be problematical to read back events in a different order. Since it is then not feasible to let PYTHIA pick the next process type, strategies +-1 and +-2 would not work. Instead strategy 3 would be the recommended choice, or -3 if negative-weight events are required.
          Note 2: it is possible to switch on internally implemented processes and have PYTHIA mix these with LHA ones according to their relative cross sections for strategies +-1, +-2 and 3. It does not work for strategy -3 unless the positive and negative sectors of the cross sections are in separate subprocesses (as must always be the case for -1 and -2), since otherwise the overall mixture of PYTHIA and LHA processes will be off. Mixing is not possible for strategies +-4, since the weighting procedure is not specified by the standard. (For instance, the intention may be to have events biased towards larger pT values in some particular functional form.)

          void LHAup::addProcess( int idProcess, double xSec, double xErr, double xMax)  
          sets info on an allowed process (cf. LPRUP, XSECUP, XERRUP, XMAXUP). Each new call will append one more entry to the list of processes. The choice of strategy determines which quantities are mandatory: xSec for strategies +-2 and +-3, xErr never, and xMax for strategies +-1 and +-2.
          Note: PYTHIA does not make active use of the (optional) xErr values, but calculates a statistical cross section error based on the spread of event-to-event weights. This should work fine for strategy options +-1, but not for the others. Specifically, for options +-2 and +-3 the weight spread may well vanish, and anyway is likely to be an underestimate of the true error. If the author of the LHA input information does provide error information you may use that - this information is displayed at initialization. If not, then a relative error decreasing like 1/sqrt(n_acc), where n_acc is the number of accepted events, should offer a reasonable estimate.

          void LHAup::setXSec( int i, double xSec)  
          update the xSec value of the i'th process added with addProcess method (i.e. i runs from 0 through sizeProc() - 1, see below).

          void LHAup::setXErr( int i, double xErr)  
          update the xErr value of the i'th process added with addProcess method.

          void LHAup::setXMax( int i, double xMax)  
          update the xMax value of the i'th process added with addProcess method.

          void LHAup::setInfoHeader(string &key, string &val)  
          set the header key to have value val. This is a wrapper function to the ";?>Info::setHeader function that should be used in any classes derived from LHAup.

          Information is handed back by the following methods (that normally you would not need to touch):

          int LHAup::idBeamA()  
          int LHAup::idBeamB()  
          double LHAup::eBeamA()  
          double LHAup::eBeamB()  
          int LHAup::pdfGroupBeamA()  
          int LHAup::pdfGroupBeamB()  
          int LHAup::pdfSetBeamA()  
          int LHAup::pdfSetBeamB()  
          for the beam properties.

          int LHAup::strategy()  
          for the strategy choice.

          int LHAup::sizeProc()  
          for the number of subprocesses.

          int LHAup::idProcess(i)  
          double LHAup::xSec(i)  
          double LHAup::xErr(i)  
          double LHAup::xMax(i)  
          for process i in the range 0 <= i < sizeProc().

          double LHAup::xSecSum()  
          double LHAup::xErrSum()  
          the sum of the cross sections and errors (the latter added quadratically). Note that cross section errors are only meaningful for strategies +-3.

          void LHAup::listInit(ostream& os = cout)  
          prints the above initialization information. This method is automatically called from Pythia::init(...), so would normally not need to be called directly by the user.

          Event input

          The LHAup class also stores information equivalent to the /HEPEUP/ commonblock, as required to hand in the next parton-level configuration for complete event generation. The main difference is that the vector container now allows a flexible number of partons to be defined. For the rest, names have been modified, since the 6-character-limit does not apply, and variables have been regrouped for clarity, but nothing fundamental is changed.

          The LHA standard is based on Fortran arrays beginning with index 1, and mother information is defined accordingly. In order to be compatible with this convention, the zeroth line of the C++ particle array is kept empty, so that index 1 also here corresponds to the first particle. One small incompatibility is that the sizePart() method returns the full size of the particle array, including the empty zeroth line, and thus is one larger than the true number of particles (NUP).

          virtual bool LHAup::setEvent(int idProcess = 0, double mRecalculate = -1.)  
          this pure virtual method has to be implemented in the derived class, to set relevant information when called. For strategy options +-1 and +-2 the input idProcess value specifies which process that should be generated, while idProcess is irrelevant for strategies +-3 and +-4. The mRecalculate input alllows an optional recalculation of the mass from the four-momentum, see LesHouches::mRecalculate below. The method should return false if it fails to set the info, i.e. normally that the supply of events in a file is exhausted. If so, no event is generated, and Pythia::next() returns false. You can then interrogate ";?>Info::atEndOfFile() to confirm that indeed the failure is caused in this method, and decide to break out of the event generation loop.

          Inside a normal setEvent(...) call, information can be set by the following methods:

          void LHAup::setProcess( int idProcess, double weight, double scale, double alphaQED, double alphaQCD)  
          tells which kind of process occurred, with what weight, at what scale, and which alpha_EM and alpha_strong were used (cf. IDPRUP, XWTGUP, SCALUP, AQEDUP, AQCDUP). This method also resets the size of the particle list, and adds the empty zeroth line, so it has to be called before the addParticle method below.

          void LHAup::addParticle( int id, int status, int mother1, int mother2, int colourTag1, int colourTag2, double p_x, double p_y, double p_z, double e, double m, double tau, double spin, double scale)  
          gives the properties of the next particle handed in (cf. IDUP, ISTUP, MOTHUP(1,..), MOTHUP(2,..), ICOLUP(1,..), ICOLUP(2,..), PUP(J,..), VTIMUP, SPINUP; while scale is a new optional property, see further below) .

          Information is handed back by the following methods:

          int LHAup::idProcess()  
          process number.

          double LHAup::weight()  
          Note that the weight stored in Info::weight() as a rule is not the same as the above weight(): the method here gives the value before unweighting while the one in info gives the one after unweighting and thus normally is 1 or -1. Only with strategy options +-3 and +-4 would the value in info be the same as here, except for a conversion from pb to mb for +-4.

          double LHAup::scale()  
          double LHAup::alphaQED()  
          double LHAup::alphaQCD()  
          scale and couplings at that scale.

          int LHAup::sizePart()  
          the size of the particle array, which is one larger than the number of particles in the event, since the zeroth entry is kept empty (see above).

          int LHAup::id(int i)  
          int LHAup::status(int i)  
          int LHAup::mother1(int i)  
          int LHAup::mother2(int i)  
          int LHAup::col1(int i)  
          int LHAup::col2(int i)  
          double LHAup::px(int i)  
          double LHAup::py(int i)  
          double LHAup::pz(int i)  
          double LHAup::e(int i)  
          double LHAup::m(int i)  
          double LHAup::tau(int i)  
          double LHAup::spin(int i)  
          double LHAup::scale(int i)  
          for particle i in the range 0 <= i < sizePart(). (But again note that i = 0 is an empty line, so the true range begins at 1.)

          From the information in the event record it is possible to set the flavour and x values of the initiators

          void LHAup::setIdX(int id1, int id2, double x1, double x2)  

          This information is returned by the methods

          int LHAup::id1()  
          int LHAup::id2()  
          double LHAup::x1()  
          double LHAup::x2()  

          In the LHEF description [Alw06] an extension to include information on the parton densities of the colliding partons is suggested. This optional further information can be set by

          void LHAup::setPdf( int id1pdf, int id2pdf, double x1pdf, double x2pdf, double scalePDF, double pdf1, double pdf2, bool pdfIsSet)  
          which gives the flavours , the x and the Q scale (in GeV) at which the parton densities x*f_i(x, Q) have been evaluated. The last argument is normally true.

          This information is returned by the methods

          bool LHAup::pdfIsSet()  
          int LHAup::id1pdf()  
          int LHAup::id2pdf()  
          double LHAup::x1pdf()  
          double LHAup::x2pdf()  
          double LHAup::scalePDF()  
          double LHAup::pdf1()  
          double LHAup::pdf2()  
          where the first one tells whether this optional information has been set for the current event. (setPdf(...) must be called after the setProcess(...) call of the event for this to work.) Note that the flavour and x values usually but not always agree with those obtained by the same methods without pdf in their names, see explanation in the ";?>Event Information description.

          As a further, currently completely non-standard feature, it is also possible to read in the separate scale values of all final particles. Currently such information should appear as a line begun by a single hashtag character (#) and then sequentially the scale value of all particles with status 1. Such scale values could be used e.g. to restrict the maximum scale for shower evolutions for each parton separately. This information is returned by the method double LHAup::scale(int i). When no such information has been read from the LHEF, the scale defaults to -1.

          void LHAup::listEvent(ostream& os = cout)  
          prints the above information for the current event. In cases where the LHAup object is not available to the user, the Pythia::LHAeventList(ostream& os = cout) method can be used, which is a wrapper for the above.

          virtual bool LHAup::skipEvent(int nSkip)  
          skip ahead nSkip events in the Les Houches generation sequence, without doing anything further with them. Mainly intended for debug purposes, e.g. when an event at a known location in a Les Houches Event File is causing problems. Will return false if operation fails, specifically if the end of an LHEF has been reached. The implementation in the base class simply executes setEvent() the requested number of times. The derived LHAupLHEF class (see below) only uses the setNewEventLHEF(...) part of its setEvent() method, and other derived classes could choose other shortcuts.

          The LHA expects the decay of resonances to be included as part of the hard process, i.e. if unstable particles are produced in a process then their decays are also described. This includes Z^0, W^+-, H^0 and other short-lived particles in models beyond the Standard Model. Should this not be the case then PYTHIA will perform the decays of all resonances it knows how to do, in the same way as for internal processes. Note that you will be on slippery ground if you then restrict the decay of these resonances to specific allowed channels since, if this is not what was intended, you will obtain the wrong cross section and potentially the wrong mix of different event types. (Since the original intention is unknown, the cross section will not be corrected for the fraction of open channels, i.e. the procedure used for internal processes is not applied in this case.)

          Even if PYTHIA can select resonance decay modes according to its internal tables, there is normally no way for it to know which decay angular correlations should exist in the simulated process. Therefore almost all decays are isotropic. The exceptions are Higgs and top decays, in the decay chains H -> WW/ZZ -> f fbar f' fbar' and t -> b W -> b f fbar, where the process-independent correlations implemented for internal processes are used. If part of the decay chain has already been set, however (e.g. H -> WW/ZZ or t -> b W), then decay is still isotropic.

          There is one setting available for event input.

          LesHouches:setLifetime   (default = 1; minimum = 0; maximum = 2)
          handling of the decay time information stored in VTIMUP when the Les Houches event record is stored into the PYTHIA process one. The reason is that some matrix-element generators (like POWHEG) do not set decay times, so that it is up to PYTHIA to make that selection. This is particularly important for the tau lepton.
          0 : all decay times are taken from the Les Houches input.
          1 : the decay time of tau leptons is generated like for internal PYTHIA taus, whereas all other decay times are taken from the Les Houches input.
          2 : all decay times are generated by PYTHIA, thus completely disregarding the Les Houches values. This option could go wrong in BSM scenarios with long-lived particles, if PYTHIA has not been provided with the information to select those lifetimes correctly.

          There is also one parameter that can be used to modify the setting of event information, if implemented in the derived class. It is prompted by an unforeseen choice made in some programs (like CalcHEP) of storing the nominal mass of a particle species rather than the mass of the current member of that species. This is likely to induce energy-momentum nonconservation when the event is further processed.

          LesHouches:mRecalculate   (default = -1.)
          Does not have any effect by default, or more generally when it is negative. If it is positive then all particles with an input mass above this value will have the mass recalculated and reset from the four-momentum, m^2 = E^2 - p^2. Obviously such a step is problematic numerically for light particles, so it should only be used for the programs and particles where it is needed. Thus the value ought to be at least 10 GeV, so that only massive particles like W^+-, Z^0 and t are affected.

          An interface to Les Houches Event Files

          The LHEF standard [Alw06] specifies a format where a single file packs initialization and event information. This has become the most frequently used procedure to process external parton-level events in Pythia. Therefore a special ";?>Pythia::init(fileName) initialization option exists, where the LHEF name is provided as input. Internally this name is then used to create an instance of the derived class LHAupLHEF, which can do the job of reading an LHEF.

          The LHEF reader can also read in and store header blocks. By default this option is switched on, but may be controlled through the ";?>Beams:readLHEFheaders flag if necessary. The information can later be read out through the ";?>Info class for further processing. Due to the non-standard nature of the information in these blocks they are stored whole, and PYTHIA itself makes no further attempt to process their meaning.

          Because Les Houches Event files tend not to adhere strictly to XML conventions, to consistently read in header information, certain choices must be made. The primary goal is to make as much information available as possible. First, information sitting directly in the <header> block is stored under the key "base". Second, the tags starting and ending each sub block must be on their own line. Finally, the contents of comment blocks, <!-- -->, are still stored. The header keys are formed hierarchically from the names of the header blocks. This behaviour is illustrated in the following example:

            <header>
              BaseA
              <hblock1>
                1A
                <hblock11>
                  11A <hblock111>
                  </hblock111> 11B
                </hblock11>
                1B
              </hblock1>
              <hblock2>
                2A
                <!-- 2B -->
              </hblock2>
              BaseB
            </header>
          
          which would lead to the following information being stored in the ";?>Info class:
          Key Value
          base BaseA
          BaseB
          hblock1 1A
          1B
          hblock1.hblock11 11A <hblock111>
          </hblock111> 11B
          hblock2 2A
          <!-- 2B -->

          Normally the LHEF would be in uncompressed format, and thus human-readable if opened in a text editor. A possibility to read gzipped files has been added, based on the Boost and zlib libraries, which therefore have to be linked appropriately in order for this option to work. See the README file in the main directory for details on how to do this.

          An example how to generate events from an LHEF is found in main11.cc. Note the use of Info::atEndOfFile() to find out when the whole LHEF has been processed.

          To allow the sequential use of several event files the Pythia::init(...) method has an optional second argument: Pythia::init(fileName, bool skipInit = false). If called with this argument true then there will be no initialization, except that the existing LHAupLHEF class instance will be deleted and replaced by ones pointing to the new file. It is assumed (but never checked) that the initialization information is identical, and that the new file simply contains further events of exactly the same kind as the previous one. An example of this possibility, and the option to mix with internal processes, is found in main12.cc. A variant, based on input in a command file, is given in main13.cc.

          In C++, real numbers are printed with an 'E' to denote the exponent part, e.g. 1.23E+04, and are read in accordingly. Other languages may use other letters, e.g. Fortran allows either 'E' or 'D'. A file using the latter convention would not be readable by the standard routines. In case you have such an "incorrectly formatted" file, a conversion to a new corrected file could be done e.g. using sed, as a one-line command

            sed -e 's/\([0-9]\.\{0,1\}\)[dD]\([+-]\{0,1\}[0-9]\)/\1E\2/g' old.lhe > new.lhe
          
          This replaces a 'd' or 'D' with an 'E' only when it occurs in the combination
          (digit) ('.' or absent) ('d' or 'D') ('+', '-' or absent) (digit)
          It will work on all parts of the file, also inside a <header>...</header> block. For conversion only inside the <init>...</init> and <event>...</event> blocks, create a file convert.sed containing
            /<init>/,/<\/init>/bconv
            /<event>/,/<\/event>/bconv
            b
            :conv
            s/\([0-9]\.\{0,1\}\)[dD]\([+-]\{0,1\}[0-9]\)/\1E\2/g
          
          and run it with
            sed -f convert.sed old.lhe > new.lhe
          

          The workhorses of the LHAupLHEF class are three methods found in the base class, so as to allow them to be reused in other contexts. Specifically, it allows derived classes where one parton-level configuration can be reused several times, e.g. in the context of matrix-element-to-parton-shower matching (example in preparation). Also two small utility routines.

          bool LHAup::setInitLHEF(ifstream& is, bool readHeaders = false)  
          read in and set all required initialization information from the specified stream. With second argument true it will also read and store header information, as described above. Return false if it fails.

          bool LHAup::setNewEventLHEF(ifstream& is)  
          read in event information from the specified stream into a staging area where it can be reused by setOldEventLHEF.

          bool LHAup::setOldEventLHEF()  
          store the event information from the staging area into the normal location. Thus a single setNewEventLHEF call can be followed by several setOldEventLHEF ones, so as to process the same configuration several times. This method currently only returns true, i.e. any errors should be caught by the preceding setNewEventLHEF call.

          bool LHAup::fileFound()  
          always returns true in the base class, but in LHAupLHEF it returns false if the LHEF provided in the constructor is not found and opened correctly.

          void LHAup::setInfoHeader(const string &key, const string &val)  
          is used to send header information on to the Info class.

          A few other methods, most of them derived from the base class, streamlines file opening and closing, e.g. if several LHE files are to be read consecutively, without the need for a complete reinitialization. This presupposes that the events are of the same kind, only split e.g. to limit file sizes.

          bool LHAup::newEventFile(const char* fileIn)  
          close current event input file/stream and open a new one, to continue reading events of the same kind as before.

          istream* LHAup::openFile(const char *fn, ifstream &ifs)  
          void LHAup::closeFile(istream *&is, ifstream &ifs)  
          open and close a file, also gzip files, where an intermediate decompression layer is needed.

          void LHAupLHEF::closeAllFiles()  
          close main event file (LHEF) and, if present, separate header file.

          A runtime Fortran interface

          The runtime Fortran interface requires linking to an external Fortran code. In order to avoid problems with unresolved external references when this interface is not used, the code has been put in a separate LHAFortran.h file, that is not included in any of the other library files. Instead it should be included in the user-supplied main program, together with the implementation of two methods below that call the Fortran program to do its part of the job.

          The LHAupFortran class derives from LHAup. It reads initialization and event information from the LHA standard Fortran commonblocks, assuming these commonblocks behave like two extern "C" struct named heprup_ and hepeup_. (Note the final underscore, to match how the gcc compiler internally names Fortran files.)

          The instantiation does not require any arguments.

          The user has to supply implementations of the fillHepRup() and fillHepEup() methods, that is to do the actual calling of the external Fortran routines that fill the HEPRUP and HEPEUP commonblocks. The translation of this information to the C++ structure is provided by the existing setInit() and setEvent() code.

          Up to and including version 8.125 the LHAupFortran class was used to construct a runtime interface to PYTHIA 6.4. This was convenient in the early days of PYTHIA 8 evolution, when this program did not yet contain hard-process generation, and the LHEF standard did not yet exist. Nowadays it is more of a bother, since a full cross-platform support leads to many possible combinations. Therefore this support has been removed, but can still be recuperated from previous code versions, in a reduced form up to version 8.176.

          Methods for LHEF output

          The main objective of the LHAup class is to feed information from an external program into PYTHIA. It can be used to export information as well, however. Specifically, there are four routines in the base class that can be called to write a Les Houches Event File. These should be called in sequence in order to build up the proper file structure.

          bool LHAup::openLHEF(string filename)  
          Opens a file with the filename indicated, and writes a header plus a brief comment with date and time information.

          bool LHAup::initLHEF()  
          Writes initialization information to the file above. Such information should already have been set with the methods described in the "Initialization" section above.

          bool LHAup::eventLHEF(bool verbose = true)  
          Writes event information to the file above. Such information should already have been set with the methods described in the "Event input" section above. This call should be repeated once for each event to be stored. By default the event information is lined up in columns. To save space, the alternative verbose = false only leaves a single blank between the information fields.

          bool LHAup::closeLHEF(bool updateInit = false)  
          Writes the closing tag and closes the file. Optionally, if updateInit = true, this routine will reopen the file from the beginning, rewrite the same header as openLHEF() did, and then call initLHEF() again to overwrite the old information. This is especially geared towards programs, such as PYTHIA itself, where the cross section information is not available at the beginning of the run, but only is obtained by Monte Carlo integration in parallel with the event generation itself. Then the setXSec( i, xSec), setXErr( i, xSec) and setXMax( i, xSec) can be used to update the relevant information before closeLHEF is called.
          Warning: overwriting the beginning of a file without upsetting anything is a delicate operation. It only works when the new lines require exactly as much space as the old ones did. Thus, if you add another process in between, the file will be corrupted.

          PYTHIA 8 output to an LHEF

          The above methods could be used by any program to write an LHEF. For PYTHIA 8 to do this, a derived class already exists, LHAupFromPYTHIA8. In order for it to do its job, it must gain access to the information produced by PYTHIA, specifically the process event record and the generic information stored in info. Therefore, if you are working with an instance pythia of the Pythia class, you have to instantiate LHAupFromPYTHIA8 with pointers to the process and info objects of pythia:
          LHAupFromPYTHIA8 myLHA(&pythia.process, &pythia.info);

          The method setInit() should be called to store the pythia initialization information in the LHA object, and setEvent() to store event information. Furthermore, updateSigma() can be used at the end of the run to update cross-section information, cf. closeLHEF(true) above. An example how the generation, translation and writing methods should be ordered is found in main20.cc.

          Currently there are some limitations, that could be overcome if necessary. Firstly, you may mix many processes in the same run, but the cross-section information stored in info only refers to the sum of them all, and therefore they are all classified as a common process 9999. Secondly, you should generate your events in the CM frame of the collision, since this is the assumed frame of stored Les Houches events, and no boosts have been implemented for the case that Pythia::process is not in this frame.

          The LHEF standard is the agreed format to store the particles of a hard process, as input to generators, whereas output of final states is normally handled using the ";?>HepMC standard. It is possible to use LHEF also here, however. It requires that the above initialization is replaced by
          LHAupFromPYTHIA8 myLHA(&pythia.event, &pythia.info);
          i.e. that process is replaced by event. In addition, the PartonLevel:all = off command found in main20.cc obviously must be removed if one wants to obtain complete events. "?>

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Ϙ=&OCW*#oa&rl 'ᔖrk5Ǡ5{CW4٢_ kk)WPnmZWW9<`'!?Ah MW@e./P, T‚A4~9fsBNd9Ṵ")&Y[5H 8N+}M)݁0*&oZ-Ӻ}P :N^*Fmqf`sR>@95]qҨ 6,Çh;l4 @_LYՆ Vo3qa>=`\ej@2 p^${_;6Aj$dԠ>ѨzSMwiP}W/nM Տlbw+;U)˔siQ:P*G|VWTC 7iw$mJr(+WUR\pv%@1#ȗ-%\Y|?NE׷AĪ7k]Q)d^Eݏ ?gՓ.LC!C`'/ݲhcXQ0Y葶ɚ JX-s6#G zhjIΙ&t]ow5G3X,b4kR *dIU>(fh` bs1U|,1' )ThH5߿s\}xmcAJ? b ^\[EyӋj;niOe#qfCX79ߏ8{9-] tl:M1/8dl0 lԫZ2C  7=g ֻ|%R~O oj> endobj 20 0 obj <>stream xcd`ab`ddv44f!CyПڳ%L1wfFF7hʢ gMCKKsԢ<Ē 'G!8?93RO1'G!X!(8,5bs~nAiIjo~JjQ5/##F~.B=g6d/\3}Fr}=====]YY ݝ-'L};_Ÿ /6mi쫸.sq\2d endstream endobj 187 0 obj 283 endobj 18 0 obj <> endobj 17 0 obj <>stream xR HTHPLJ+CMR10c=4.FKZCopyright (C) 1997 American Mathematical Society. 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          Higgs Processes

          This page documents Higgs production within and beyond the Standard Model (SM and BSM for short). This includes several different processes and, for the BSM scenarios, a large set of parameters that would only be fixed within a more specific framework such as MSSM. Three choices can be made irrespective of the particular model:

          Higgs:cubicWidth On Off   (default = off)
          The partial width of a Higgs particle to a pair of gauge bosons, W^+ W^- or Z^0 Z^0, depends cubically on the Higgs mass. When selecting the Higgs according to a Breit-Wigner, so that the actual mass mHat does not agree with the nominal m_Higgs one, an ambiguity arises which of the two to use [Sey95]. The default is to use a linear dependence on mHat, i.e. a width proportional to m_Higgs^2 * mHat, while on gives a mHat^3 dependence. This does not affect the widths to fermions, which only depend linearly on mHat. This flag is used both for SM and BSM Higgs bosons.

          Higgs:runningLoopMass On Off   (default = on)
          The partial width of a Higgs particle to a pair of gluons or photons, or a gamma Z^0 pair, proceeds in part through quark loops, mainly b and t. There is some ambiguity what kind of masses to use. Default is running MSbar ones, but alternatively fixed pole masses are allowed (as was standard in PYTHIA 6), which typically gives a noticeably higher cross section for these channels. (For a decay to a pair of fermions, such as top, the running mass is used for couplings and the fixed one for phase space.)

          Higgs:clipWings On Off   (default = on)
          The Breit-Wigner shape of a Higgs is nontrivial, owing to the rapid width variation with the mass of a Higgs. This implies that a Higgs of low nominal mass may still acquire a non-negligible high-end tail. The validity of the calculation may be questioned in these wings. With this option on, the Higgs:wingsFac value is used to cut away the wings.
          Warning: with this option on, the allowed mass range is shrunk, but never widened. This can lead to inconsistencies if a run consists of several subruns with different Higgs masses. The id:mMin and id:mMax values should therefore be reset (e.g. to the defaults 50. and 0.) when id:m0 is changed.

          Higgs:wingsFac   (default = 50.; minimum = 0.)
          With Higgs:clipWings on, all Higgs masses which deviate from the nominal one by more than Higgs:wingsFac times the nominal width are forbidden. This is achieved by setting the mMin and mMax values of the Higgs states at initialization. These changes never allow a wider range than already set by the user, alternatively by the current default values, see warning above.

          Standard-Model Higgs, basic processes

          This section provides the standard set of processes that can be run together to provide a reasonably complete overview of possible production channels for a single SM Higgs. The main parameter is the choice of Higgs mass, which can be set in the normal ParticleData database; thereafter the properties within the SM are essentially fixed.

          HiggsSM:all On Off   (default = off)
          Common switch for the group of Higgs production within the Standard Model.

          HiggsSM:ffbar2H On Off   (default = off)
          Scattering f fbar -> H^0, where f sums over available flavours except top. Related to the mass-dependent Higgs point coupling to fermions, so at hadron colliders the bottom contribution will dominate. Code 901.

          HiggsSM:gg2H On Off   (default = off)
          Scattering g g -> H^0 via loop contributions primarily from top. Code 902.

          HiggsSM:gmgm2H On Off   (default = off)
          Scattering gamma gamma -> H^0 via loop contributions primarily from top and W. Code 903.

          HiggsSM:ffbar2HZ On Off   (default = off)
          Scattering f fbar -> H^0 Z^0 via s-channel Z^0 exchange. Code 904.

          HiggsSM:ffbar2HW On Off   (default = off)
          Scattering f fbar -> H^0 W^+- via s-channel W^+- exchange. Code 905.

          HiggsSM:ff2Hff(t:ZZ) On Off   (default = off)
          Scattering f f' -> H^0 f f' via Z^0 Z^0 fusion. Code 906.

          HiggsSM:ff2Hff(t:WW) On Off   (default = off)
          Scattering f_1 f_2 -> H^0 f_3 f_4 via W^+ W^- fusion. Code 907.

          HiggsSM:gg2Httbar On Off   (default = off)
          Scattering g g -> H^0 t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 908.

          HiggsSM:qqbar2Httbar On Off   (default = off)
          Scattering q qbar -> H^0 t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 909.

          Standard-Model Higgs, further processes

          A number of further production processes has been implemented, that are specializations of some of the above ones to the high-pT region. The sets therefore could not be used simultaneously without unphysical double-counting, as further explained below. They are not switched on by the HiggsSM:all flag, but have to be switched on for each separate process after due consideration.

          The first three processes in this section are related to the Higgs point coupling to fermions, and so primarily are of interest for b quarks. It is here useful to begin by reminding that a process like b bbar -> H^0 implies that a b/bbar is taken from each incoming hadron, leaving behind its respective antiparticle. The initial-state showers will then add one g -> b bbar branching on either side, so that effectively the process becomes g g -> H0 b bbar. This would be the same basic process as the g g -> H^0 t tbar one used for top. The difference is that (a) no PDF's are defined for top and (b) the shower approach would not be good enough to provide sensible kinematics for the H^0 t tbar subsystem. By contrast, owing to the b being much lighter than the Higgs, multiple gluon emissions must be resummed for b, as is done by PDF's and showers, in order to obtain a sensible description of the total production rate, when the b quarks predominantly are produced at small pT values.

          HiggsSM:qg2Hq On Off   (default = off)
          Scattering q g -> H^0 q. This process gives first-order corrections to the f fbar -> H^0 one above, and should only be used to study the high-pT tail, while f fbar -> H^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> H^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 911.

          HiggsSM:gg2Hbbbar On Off   (default = off)
          Scattering g g -> H^0 b bbar. This process is yet one order higher of the b bbar -> H^0 and b g -> H^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 912.

          HiggsSM:qqbar2Hbbbar On Off   (default = off)
          Scattering q qbar -> H^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 913.

          The second set of processes are predominantly first-order corrections to the g g -> H^0 process, again dominated by the top loop. We here only provide the kinematical expressions obtained in the limit that the top quark goes to infinity, but scaled to the finite-top-mass coupling in g g -> H^0. (Complete loop expressions are available e.g. in PYTHIA 6.4 but are very lengthy.) This provides a reasonably accurate description for "intermediate" pT values, but fails when the pT scale approaches the top mass.

          HiggsSM:gg2Hg(l:t) On Off   (default = off)
          Scattering g g -> H^0 g via loop contributions primarily from top. Code 914.

          HiggsSM:qg2Hq(l:t) On Off   (default = off)
          Scattering q g -> H^0 q via loop contributions primarily from top. Not to be confused with the HiggsSM:qg2Hq process above, with its direct fermion-to-Higgs coupling. Code 915.

          HiggsSM:qqbar2Hg(l:t) On Off   (default = off)
          Scattering q qbar -> H^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> H^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 916.

          Beyond-the-Standard-Model Higgs, introduction

          Further Higgs multiplets arise in a number of scenarios. We here concentrate on the MSSM scenario with two Higgs doublets, but with flexibility enough that also other two-Higgs-doublet scenarios could be represented by a suitable choice of parameters. Conventionally the Higgs states are labeled h^0, H^0, A^0 and H^+-. If the scalar and pseudocalar states mix the resulting states are labeled H_1^0, H_2^0, H_3^0. In process names and parameter explanations both notations will be used, but for settings labels we have adapted the shorthand hybrid notation H1 for h^0(H_1^0), H2 for H^0(H_2^0) and A3 for A^0(H_3^0). (Recall that the Settings database does not distinguish upper- and lowercase characters, so that the user has one thing less to worry about, but here it causes problems with h^0 vs. H^0.) We leave the issue of mass ordering between H^0 and A^0 open, and thereby also that of H_2^0 and H_3^0.

          Higgs:useBSM On Off   (default = off)
          Master switch to initialize and use the two-Higgs-doublet states. If off, only the above SM Higgs processes can be used, with couplings as predicted in the SM. If on, only the below BSM Higgs processes can be used, with couplings that can be set freely, also found further down on this page.

          Beyond-the-Standard-Model Higgs, basic processes

          This section provides the standard set of processes that can be run together to provide a reasonably complete overview of possible production channels for a single neutral Higgs state in a two-doublet scenarios such as MSSM. The list of processes for neutral states closely mimics the one found for the SM Higgs. Some of the processes vanish for a pure pseudoscalar A^0, but are kept for flexibility in cases of mixing with the scalar h^0 and H^0 states, or for use in the context of non-MSSM models. This should work well to represent e.g. that a small admixture of the "wrong" parity would allow a process such as q qbar -> A^0 Z^0, which otherwise is forbidden. However, note that the loop integrals e.g. for g g -> h^0/H^0/A^0 are hardcoded to be for scalars for the former two particles and for a pseudoscalar for the latter one, so absolute rates would not be correctly represented in the case of large scalar/pseudoscalar mixing.

          HiggsBSM:all On Off   (default = off)
          Common switch for the group of Higgs production beyond the Standard Model, as listed below.

          1) h^0(H_1^0) processes



          HiggsBSM:allH1 On Off   (default = off)
          Common switch for the group of h^0(H_1^0) production processes.

          HiggsBSM:ffbar2H1 On Off   (default = off)
          Scattering f fbar -> h^0(H_1^0), where f sums over available flavours except top. Code 1001.

          HiggsBSM:gg2H1 On Off   (default = off)
          Scattering g g -> h^0(H_1^0) via loop contributions primarily from top. Code 1002.

          HiggsBSM:gmgm2H1 On Off   (default = off)
          Scattering gamma gamma -> h^0(H_1^0) via loop contributions primarily from top and W. Code 1003.

          HiggsBSM:ffbar2H1Z On Off   (default = off)
          Scattering f fbar -> h^0(H_1^0) Z^0 via s-channel Z^0 exchange. Code 1004.

          HiggsBSM:ffbar2H1W On Off   (default = off)
          Scattering f fbar -> h^0(H_1^0) W^+- via s-channel W^+- exchange. Code 1005.

          HiggsBSM:ff2H1ff(t:ZZ) On Off   (default = off)
          Scattering f f' -> h^0(H_1^0) f f' via Z^0 Z^0 fusion. Code 1006.

          HiggsBSM:ff2H1ff(t:WW) On Off   (default = off)
          Scattering f_1 f_2 -> h^0(H_1^0) f_3 f_4 via W^+ W^- fusion. Code 1007.

          HiggsBSM:gg2H1ttbar On Off   (default = off)
          Scattering g g -> h^0(H_1^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1008.

          HiggsBSM:qqbar2H1ttbar On Off   (default = off)
          Scattering q qbar -> h^0(H_1^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1009.

          2) H^0(H_2^0) processes



          HiggsBSM:allH2 On Off   (default = off)
          Common switch for the group of H^0(H_2^0) production processes.

          HiggsBSM:ffbar2H2 On Off   (default = off)
          Scattering f fbar -> H^0(H_2^0), where f sums over available flavours except top. Code 1021.

          HiggsBSM:gg2H2 On Off   (default = off)
          Scattering g g -> H^0(H_2^0) via loop contributions primarily from top. Code 1022.

          HiggsBSM:gmgm2H2 On Off   (default = off)
          Scattering gamma gamma -> H^0(H_2^0) via loop contributions primarily from top and W. Code 1023.

          HiggsBSM:ffbar2H2Z On Off   (default = off)
          Scattering f fbar -> H^0(H_2^0) Z^0 via s-channel Z^0 exchange. Code 1024.

          HiggsBSM:ffbar2H2W On Off   (default = off)
          Scattering f fbar -> H^0(H_2^0) W^+- via s-channel W^+- exchange. Code 1025.

          HiggsBSM:ff2H2ff(t:ZZ) On Off   (default = off)
          Scattering f f' -> H^0(H_2^0) f f' via Z^0 Z^0 fusion. Code 1026.

          HiggsBSM:ff2H2ff(t:WW) On Off   (default = off)
          Scattering f_1 f_2 -> H^0(H_2^0) f_3 f_4 via W^+ W^- fusion. Code 1027.

          HiggsBSM:gg2H2ttbar On Off   (default = off)
          Scattering g g -> H^0(H_2^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1028.

          HiggsBSM:qqbar2H2ttbar On Off   (default = off)
          Scattering q qbar -> H^0(H_2^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1029.

          3) A^0(H_3^0) processes



          HiggsBSM:allA3 On Off   (default = off)
          Common switch for the group of A^0(H_3^0) production processes.

          HiggsBSM:ffbar2A3 On Off   (default = off)
          Scattering f fbar -> A^0(H_3^0), where f sums over available flavours except top. Code 1041.

          HiggsBSM:gg2A3 On Off   (default = off)
          Scattering g g -> A^0(A_3^0) via loop contributions primarily from top. Code 1042.

          HiggsBSM:gmgm2A3 On Off   (default = off)
          Scattering gamma gamma -> A^0(A_3^0) via loop contributions primarily from top and W. Code 1043.

          HiggsBSM:ffbar2A3Z On Off   (default = off)
          Scattering f fbar -> A^0(A_3^0) Z^0 via s-channel Z^0 exchange. Code 1044.

          HiggsBSM:ffbar2A3W On Off   (default = off)
          Scattering f fbar -> A^0(A_3^0) W^+- via s-channel W^+- exchange. Code 1045.

          HiggsBSM:ff2A3ff(t:ZZ) On Off   (default = off)
          Scattering f f' -> A^0(A_3^0) f f' via Z^0 Z^0 fusion. Code 1046.

          HiggsBSM:ff2A3ff(t:WW) On Off   (default = off)
          Scattering f_1 f_2 -> A^0(A_3^0) f_3 f_4 via W^+ W^- fusion. Code 1047.

          HiggsBSM:gg2A3ttbar On Off   (default = off)
          Scattering g g -> A^0(A_3^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1048.

          HiggsBSM:qqbar2A3ttbar On Off   (default = off)
          Scattering q qbar -> A^0(A_3^0) t tbar via t tbar fusion (or, alternatively put, Higgs radiation off a top line). Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1049.

          4) H+- processes



          HiggsBSM:allH+- On Off   (default = off)
          Common switch for the group of H^+- production processes.

          HiggsBSM:ffbar2H+- On Off   (default = off)
          Scattering f fbar' -> H^+-, where f, fbar' sums over available incoming flavours. Since couplings are assumed generation-diagonal, in practice this means c sbar -> H^+ and s cbar -> H^-. Code 1061.

          HiggsBSM:bg2H+-t On Off   (default = off)
          Scattering b g -> H^+ tbar. At hadron colliders this is the dominant process for single-charged-Higgs production. Code 1062.

          5) Higgs-pair processes



          HiggsBSM:allHpair On Off   (default = off)
          Common switch for the group of Higgs pair-production processes.

          HiggsBSM:ffbar2A3H1 On Off   (default = off)
          Scattering f fbar -> A^0(H_3) h^0(H_1). Code 1081.

          HiggsBSM:ffbar2A3H2 On Off   (default = off)
          Scattering f fbar -> A^0(H_3) H^0(H_2). Code 1082.

          HiggsBSM:ffbar2H+-H1 On Off   (default = off)
          Scattering f fbar -> H^+- h^0(H_1). Code 1083.

          HiggsBSM:ffbar2H+-H2 On Off   (default = off)
          Scattering f fbar -> H^+- H^0(H_2). Code 1084.

          HiggsBSM:ffbar2H+H- On Off   (default = off)
          Scattering f fbar -> H+ H-. Code 1085.

          Beyond-the-Standard-Model Higgs, further processes

          This section mimics the above section on "Standard-Model Higgs, further processes", i.e. it contains higher-order corrections to the processes already listed. The two sets therefore could not be used simultaneously without unphysical double-counting. They are not controlled by any group flag, but have to be switched on for each separate process after due consideration. We refer to the standard-model description for a set of further comments on the processes.

          1) h^0(H_1^0) processes



          HiggsBSM:qg2H1q On Off   (default = off)
          Scattering q g -> h^0 q. This process gives first-order corrections to the f fbar -> h^0 one above, and should only be used to study the high-pT tail, while f fbar -> h^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> h^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 1011.

          HiggsBSM:gg2H1bbbar On Off   (default = off)
          Scattering g g -> h^0 b bbar. This process is yet one order higher of the b bbar -> h^0 and b g -> h^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1012.

          HiggsBSM:qqbar2H1bbbar On Off   (default = off)
          Scattering q qbar -> h^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1013.

          HiggsBSM:gg2H1g(l:t) On Off   (default = off)
          Scattering g g -> h^0 g via loop contributions primarily from top. Code 1014.

          HiggsBSM:qg2H1q(l:t) On Off   (default = off)
          Scattering q g -> h^0 q via loop contributions primarily from top. Not to be confused with the HiggsBSM:qg2H1q process above, with its direct fermion-to-Higgs coupling. Code 1015.

          HiggsBSM:qqbar2H1g(l:t) On Off   (default = off)
          Scattering q qbar -> h^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> h^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 1016.

          2) H^0(H_2^0) processes



          HiggsBSM:qg2H2q On Off   (default = off)
          Scattering q g -> H^0 q. This process gives first-order corrections to the f fbar -> H^0 one above, and should only be used to study the high-pT tail, while f fbar -> H^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> H^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 1031.

          HiggsBSM:gg2H2bbbar On Off   (default = off)
          Scattering g g -> H^0 b bbar. This process is yet one order higher of the b bbar -> H^0 and b g -> H^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1032.

          HiggsBSM:qqbar2H2bbbar On Off   (default = off)
          Scattering q qbar -> H^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1033.

          HiggsBSM:gg2H2g(l:t) On Off   (default = off)
          Scattering g g -> H^0 g via loop contributions primarily from top. Code 1034.

          HiggsBSM:qg2H2q(l:t) On Off   (default = off)
          Scattering q g -> H^0 q via loop contributions primarily from top. Not to be confused with the HiggsBSM:qg2H1q process above, with its direct fermion-to-Higgs coupling. Code 1035.

          HiggsBSM:qqbar2H2g(l:t) On Off   (default = off)
          Scattering q qbar -> H^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> H^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 1036.

          3) A^0(H_3^0) processes



          HiggsBSM:qg2A3q On Off   (default = off)
          Scattering q g -> A^0 q. This process gives first-order corrections to the f fbar -> A^0 one above, and should only be used to study the high-pT tail, while f fbar -> A^0 should be used for inclusive production. Only the dominant c and b contributions are included, and generated separately for technical reasons. Note that another first-order process would be q qbar -> A^0 g, which is not explicitly implemented here, but is obtained from showering off the lowest-order process. It does not contain any b at large pT, however, so is less interesting for many applications. Code 1051.

          HiggsBSM:gg2A3bbbar On Off   (default = off)
          Scattering g g -> A^0 b bbar. This process is yet one order higher of the b bbar -> A^0 and b g -> A^0 b chain, where now two quarks should be required above some large pT threshold. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1052.

          HiggsBSM:qqbar2A3bbbar On Off   (default = off)
          Scattering q qbar -> A^0 b bbar via an s-channel gluon, so closely related to the previous one, but typically less important owing to the smaller rate of (anti)quarks relative to gluons. Warning: unfortunately this process is rather slow, owing to a lengthy cross-section expression and inefficient phase-space selection. Code 1053.

          HiggsBSM:gg2A3g(l:t) On Off   (default = off)
          Scattering g g -> A^0 g via loop contributions primarily from top. Code 1054.

          HiggsBSM:qg2A3q(l:t) On Off   (default = off)
          Scattering q g -> A^0 q via loop contributions primarily from top. Not to be confused with the HiggsBSM:qg2H1q process above, with its direct fermion-to-Higgs coupling. Code 1055.

          HiggsBSM:qqbar2A3g(l:t) On Off   (default = off)
          Scattering q qbar -> A^0 g via an s-channel gluon and loop contributions primarily from top. Is strictly speaking a "new" process, not directly derived from g g -> A^0, and could therefore be included in the standard mix without double-counting, but is numerically negligible. Code 1056.

          Parameters for Beyond-the-Standard-Model Higgs production and decay

          This section offers a big flexibility to set couplings of the various Higgs states to fermions and gauge bosons, and also to each other. The intention is that, for scenarios like MSSM, you should use standard input from the ";?>SUSY Les Houches Accord, rather than having to set it all yourself. In other cases, however, the freedom is there for you to use. Kindly note that some of the internal calculations of partial widths from the parameters provided do not include mixing between the scalar and pseudoscalar states.

          Masses would be set in the ParticleData database, while couplings are set below. When possible, the couplings of the Higgs states are normalized to the corresponding coupling within the SM. When not, their values within the MSSM are indicated, from which it should be straightforward to understand what to use instead. The exception is some couplings that vanish also in the MSSM, where the normalization has been defined in close analogy with nonvanishing ones. Some parameter names are asymmetric but crossing can always be used, i.e. the coupling for A^0 -> H^0 Z^0 obviously is also valid for H^0 -> A^0 Z^0 and Z^0 -> H^0 A^0. Note that couplings usually appear quadratically in matrix elements.

          HiggsH1:coup2d   (default = 1.)
          The h^0(H_1^0) coupling to down-type quarks.

          HiggsH1:coup2u   (default = 1.)
          The h^0(H_1^0) coupling to up-type quarks.

          HiggsH1:coup2l   (default = 1.)
          The h^0(H_1^0) coupling to (charged) leptons.

          HiggsH1:coup2Z   (default = 1.)
          The h^0(H_1^0) coupling to Z^0.

          HiggsH1:coup2W   (default = 1.)
          The h^0(H_1^0) coupling to W^+-.

          HiggsH1:coup2Hchg   (default = 0.)
          The h^0(H_1^0) coupling to H^+- (in loops). Is sin(beta - alpha) + cos(2 beta) sin(beta + alpha) / (2 cos^2theta_W) in the MSSM.

          HiggsH2:coup2d   (default = 1.)
          The H^0(H_2^0) coupling to down-type quarks.

          HiggsH2:coup2u   (default = 1.)
          The H^0(H_2^0) coupling to up-type quarks.

          HiggsH2:coup2l   (default = 1.)
          The H^0(H_2^0) coupling to (charged) leptons.

          HiggsH2:coup2Z   (default = 1.)
          The H^0(H_2^0) coupling to Z^0.

          HiggsH2:coup2W   (default = 1.)
          The H^0(H_2^0) coupling to W^+-.

          HiggsH2:coup2Hchg   (default = 0.)
          The H^0(H_2^0) coupling to H^+- (in loops). Is cos(beta - alpha) + cos(2 beta) cos(beta + alpha) / (2 cos^2theta_W) in the MSSM.

          HiggsH2:coup2H1H1   (default = 1.)
          The H^0(H_2^0) coupling to a h^0(H_1^0) pair. Is cos(2 alpha) cos(beta + alpha) - 2 sin(2 alpha) sin(beta + alpha) in the MSSM.

          HiggsH2:coup2A3A3   (default = 1.)
          The H^0(H_2^0) coupling to an A^0(H_3^0) pair. Is cos(2 beta) cos(beta + alpha) in the MSSM.

          HiggsH2:coup2H1Z   (default = 0.)
          The H^0(H_2^0) coupling to a h^0(H_1^0) Z^0 pair. Vanishes in the MSSM.

          HiggsH2:coup2A3H1   (default = 0.)
          The H^0(H_2^0) coupling to an A^0(H_3^0) h^0(H_1^0) pair. Vanishes in the MSSM.

          HiggsH2:coup2HchgW   (default = 0.)
          The H^0(H_2^0) coupling to a H^+- W-+ pair. Is sin(beta - alpha) in the MSSM.

          HiggsA3:coup2d   (default = 1.)
          The A^0(H_3^0) coupling to down-type quarks.

          HiggsA3:coup2u   (default = 1.)
          The A^0(H_3^0) coupling to up-type quarks.

          HiggsA3:coup2l   (default = 1.)
          The A^0(H_3^0) coupling to (charged) leptons.

          HiggsA3:coup2H1Z   (default = 1.)
          The A^0(H_3^0) coupling to a h^0(H_1^0) Z^0 pair. Is cos(beta - alpha) in the MSSM.

          HiggsA3:coup2H2Z   (default = 1.)
          The A^0(H_3^0) coupling to a H^0(H_2^0) Z^0 pair. Is sin(beta - alpha) in the MSSM.

          HiggsA3:coup2Z   (default = 0.)
          The A^0(H_3^0) coupling to Z^0. Vanishes in the MSSM.

          HiggsA3:coup2W   (default = 0.)
          The A^0(H_3^0) coupling to W^+-. Vanishes in the MSSM.

          HiggsA3:coup2H1H1   (default = 0.)
          The A^0(H_3^0) coupling to a h^0(H_1^0) pair. Vanishes in the MSSM.

          HiggsA3:coup2Hchg   (default = 0.)
          The A^0(H_3^0) coupling to H^+-. Vanishes in the MSSM.

          HiggsA3:coup2HchgW   (default = 1.)
          The A^0(H_3^0) coupling to a H^+- W-+ pair. Is 1 in the MSSM.

          HiggsHchg:tanBeta   (default = 5.)
          The tan(beta) value, which leads to an enhancement of the H^+- coupling to down-type fermions and suppression to up-type ones. The same angle also appears in many other places, but this particular parameter is only used for the charged-Higgs case.

          HiggsHchg:coup2H1W   (default = 1.)
          The H^+- coupling to a h^0(H_1^0) W^+- pair. Is cos(beta - alpha) in the MSSM.

          HiggsHchg:coup2H2W   (default = 0.)
          The H^+- coupling to a H^0(H_2^0) W^+- pair. Is sin(beta - alpha) in the MSSM.

          Another set of parameters are not used in the production stage but exclusively for the description of angular distributions in decays.

          HiggsH1:parity   (default = 1; minimum = 0; maximum = 3)
          possibility to modify angular decay correlations in the decay of a h^0(H_1) decay Z^0 Z^0 or W^+ W^- to four fermions. Currently it does not affect the partial width of the channels, which is only based on the above parameters.
          0 : isotropic decays.
          1 : assuming the h^0(H_1) is a pure scalar (CP-even), as in the MSSM.
          2 : assuming the h^0(H_1) is a pure pseudoscalar (CP-odd).
          3 : assuming the h^0(H_1) is a mixture of the two, including the CP-violating interference term. The parameter eta, see below, sets the strength of the CP-odd admixture, with the interference term being proportional to eta and the CP-odd one to eta^2.


          HiggsH1:etaParity   (default = 0.)
          The eta value of CP-violation in the HiggsSM:parity = 3 option.

          HiggsH2:parity   (default = 1; minimum = 0; maximum = 3)
          possibility to modify angular decay correlations in the decay of a H^0(H_2) decay Z^0 Z^0 or W^+ W^- to four fermions. Currently it does not affect the partial width of the channels, which is only based on the above parameters.
          0 : isotropic decays.
          1 : assuming the H^0(H_2) is a pure scalar (CP-even), as in the MSSM.
          2 : assuming the H^0(H_2) is a pure pseudoscalar (CP-odd).
          3 : assuming the H^0(H_2) is a mixture of the two, including the CP-violating interference term. The parameter eta, see below, sets the strength of the CP-odd admixture, with the interference term being proportional to eta and the CP-odd one to eta^2.


          HiggsH2:etaParity   (default = 0.)
          The eta value of CP-violation in the HiggsSM:parity = 3 option.

          HiggsA3:parity   (default = 2; minimum = 0; maximum = 3)
          possibility to modify angular decay correlations in the decay of a A^0(H_3) decay Z^0 Z^0 or W^+ W^- to four fermions. Currently it does not affect the partial width of the channels, which is only based on the above parameters.
          0 : isotropic decays.
          1 : assuming the A^0(H_3) is a pure scalar (CP-even).
          2 : assuming the A^0(H_3) is a pure pseudoscalar (CP-odd), as in the MSSM.
          3 : assuming the A^0(H_3) is a mixture of the two, including the CP-violating interference term. The parameter eta, see below, sets the strength of the CP-odd admixture, with the interference term being proportional to eta and the CP-odd one to eta^2.


          HiggsA3:etaParity   (default = 0.)
          The eta value of CP-violation in the HiggsSM:parity = 3 option. "?>

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          Left-Right-Symmetry Processes

          At current energies, the world is left-handed, i.e. the Standard Model contains an SU(2)_L group. Left-right symmetry at some larger scale implies the need for an SU(2)_R group. Thus the particle content is expanded by right-handed Z_R^0 and W_R^+- and right-handed neutrinos. The Higgs fields have to be in a triplet representation, leading to doubly-charged Higgs particles, one set for each of the two SU(2) groups. Also the number of neutral and singly-charged Higgs states is increased relative to the Standard Model, but a search for the lowest-lying states of this kind is no different from e.g. the freedom already accorded by the MSSM Higgs scenarios.

          PYTHIA implements the scenario of [Hui97].

          The W_R^+- has been implemented as a simple copy of the ordinary W^+-, with the exception that it couples to right-handed neutrinos instead of the ordinary left-handed ones. Thus the standard CKM matrix is used in the quark sector, and the same vector and axial coupling strengths, leaving only the mass as free parameter. The Z_R^0 implementation (without interference with the photon or the ordinary Z^0) allows decays both to left- and right-handed neutrinos, as well as other fermions, according to one specific model ansatz. Obviously both the W_R^+- and the Z_R^0 descriptions are likely to be simplifications, but provide a starting point.

          For the doubly-charged Higgs bosons, the main decay modes implemented are H_L^++ -> W_L^+ W_L^+, l_i^+ l_j^+ (i, j generation indices) and H_R^++ -> W_R^+ W_R^+, l_i^+ l_j^+.

          The right-handed neutrinos can be allowed to decay further. Assuming them to have a mass below that of W_R^+-, they decay to three-body states via a virtual W_R^+-, nu_Rl -> l+- f fbar', where both lepton charges are allowed owing to the Majorana character of the neutrinos. If there is a significant mass splitting, also sequential decays nu_Rl -> l+- l'-+ nu'_Rl are allowed. Currently the decays are isotropic in phase space. If the neutrino masses are close to or above the W_R^ ones, this description has to be substituted by a sequential decay via a real W_R^ (not implemented, but actually simpler to do than the one here).

          Production processes

          A few different production processes have been implemented, which normally would not overlap and therefore could be run together.

          LeftRightSymmmetry:all On Off   (default = off)
          Common switch for the group of implemented processes within a left-right-symmetric scenario.

          LeftRightSymmmetry:ffbar2ZR On Off   (default = off)
          Scatterings f fbar -> Z_R^0. Code 3101.

          LeftRightSymmmetry:ffbar2WR On Off   (default = off)
          Scatterings W_R^+. Code 3102.

          LeftRightSymmmetry:ll2HL On Off   (default = off)
          Scatterings l_i l_j -> H_L^--. Code 3121.

          LeftRightSymmmetry:lgm2HLe On Off   (default = off)
          Scatterings l_i gamma -> H_L^-- e^+. Code 3122.

          LeftRightSymmmetry:lgm2HLmu On Off   (default = off)
          Scatterings l_i gamma -> H_L^-- mu^+. Code 3123.

          LeftRightSymmmetry:lgm2HLtau On Off   (default = off)
          Scatterings l_i gamma -> H_L^-- tau^+. Code 3124.

          LeftRightSymmmetry:ff2HLff On Off   (default = off)
          Scatterings f_1 f_2 -> H_L^-- f_3 f_4 via WW fusion. Code 3125.

          LeftRightSymmmetry:ffbar2HLHL On Off   (default = off)
          Scatterings f fbar -> H_L^++ H_L^--. Code 3126.

          LeftRightSymmmetry:ll2HR On Off   (default = off)
          Scatterings l_i l_j -> H_R^--. Code 3141.

          LeftRightSymmmetry:lgm2HRe On Off   (default = off)
          Scatterings l_i gamma -> H_R^-- e^+. Code 3142.

          LeftRightSymmmetry:lgm2HRmu On Off   (default = off)
          Scatterings l_i gamma -> H_R^-- mu^+. Code 3143.

          LeftRightSymmmetry:lgm2HRtau On Off   (default = off)
          Scatterings l_i gamma -> H_R^-- tau^+. Code 3144.

          LeftRightSymmmetry:ff2HRff On Off   (default = off)
          Scatterings f_1 f_2 -> H_R^-- f_3 f_4 via WW fusion. Code 3145.

          LeftRightSymmmetry:ffbar2HRHR On Off   (default = off)
          Scatterings f fbar -> H_R^++ H_L^--. Code 3146.

          Parameters

          The basic couplings of the model are

          LeftRightSymmmetry:gL   (default = 0.64; minimum = 0.0)
          lefthanded coupling g_L = e / sin(theta).

          LeftRightSymmmetry:gR   (default = 0.64; minimum = 0.0)
          righthanded coupling g_R, assumed the same as g_L.

          LeftRightSymmmetry:vL   (default = 5.; minimum = 0.0)
          vacuum expectation value v_L (in GeV) for the left-triplet.

          The corresponding vacuum expectation value v_R is assumed given by v_R = sqrt(2) M_WR / g_R and is not stored explicitly.

          The Yukawa couplings of a lepton pair to a H^--, assumed the same for H_L^-- and H_R^--, is described by a symmetric 3-by-3 matrix. The default matrix is dominated by the diagonal elements and especially by the tau tau one.

          LeftRightSymmmetry:coupHee   (default = 0.1; minimum = 0.0)
          Yukawa coupling for H^-- -> e- e-.

          LeftRightSymmmetry:coupHmue   (default = 0.01; minimum = 0.0)
          Yukawa coupling for H^-- -> mu- e-.

          LeftRightSymmmetry:coupHmumu   (default = 0.1; minimum = 0.0)
          Yukawa coupling for H^-- -> mu- mu-.

          LeftRightSymmmetry:coupHtaue   (default = 0.01; minimum = 0.0)
          Yukawa coupling for H^-- -> tau- e-.

          LeftRightSymmmetry:coupHtaumu   (default = 0.01; minimum = 0.0)
          Yukawa coupling for H^-- -> tau- mu-.

          LeftRightSymmmetry:coupHtautau   (default = 0.3; minimum = 0.0)
          Yukawa coupling for H^-- -> tau- tau-. "?>

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          New-Gauge-Boson Processes

          This page contains the production of new Z'^0 and W'^+- gauge bosons, e.g. within the context of a new U(1) or SU(2) gauge group, and also a (rather speculative) horizontal gauge boson R^0. Left-right-symmetry scenarios also contain new gauge bosons, but are described ";?>separately.

          Z'^0

          This group only contains one subprocess, with the full gamma^*/Z^0/Z'^0 interference structure for couplings to fermion pairs. It is possible to pick only a subset, e.g, only the pure Z'^0 piece. No higher-order processes are available explicitly, but the ISR showers contain automatic matching to the Z'^0 + 1 jet matrix elements, as for the corresponding gamma^*/Z^0 process.

          NewGaugeBoson:ffbar2gmZZprime On Off   (default = off)
          Scattering f fbar ->Z'^0. Code 3001.

          Zprime:gmZmode   (default = 0; minimum = 0; maximum = 6)
          Choice of full gamma^*/Z^0/Z'^0 structure or not in the above process. Note that, with the Z'^0 part switched off, this process is reduced to what already exists among electroweak processes, so those options are here only for crosschecks.
          0 : full gamma^*/Z^0/Z'^0 structure, with interference included.
          1 : only pure gamma^* contribution.
          2 : only pure Z^0 contribution.
          3 : only pure Z'^0 contribution.
          4 : only the gamma^*/Z^0 contribution, including interference.
          5 : only the gamma^*/Z'^0 contribution, including interference.
          6 : only the Z^0/Z'^0 contribution, including interference.

          Note: irrespective of the option used, the particle produced will always be assigned code 32 for Z'^0, and open decay channels is purely dictated by what is set for the Z'^0.

          The couplings of the Z'^0 to quarks and leptons can either be assumed universal, i.e. generation-independent, or not. In the former case eight numbers parametrize the vector and axial couplings of down-type quarks, up-type quarks, leptons and neutrinos, respectively. Depending on your assumed neutrino nature you may want to restrict your freedom in that sector, but no limitations are enforced by the program. The default corresponds to the same couplings as that of the Standard Model Z^0, with axial couplings a_f = +-1 and vector couplings v_f = a_f - 4 e_f sin^2(theta_W), with sin^2(theta_W) = 0.23. Without universality the same eight numbers have to be set separately also for the second and the third generation. The choice of fixed axial and vector couplings implies a resonance width that increases linearly with the Z'^0 mass.

          By a suitable choice of the parameters, it is possible to simulate just about any imaginable Z'^0 scenario, with full interference effects in cross sections and decay angular distributions and generation-dependent couplings; the default values should mainly be viewed as placeholders. The conversion from the coupling conventions in a set of different Z'^0 models in the literature to those used in PYTHIA is described by C. Ciobanu et al.

          Zprime:universality On Off   (default = on)
          If on then you need only set the first-generation couplings below, and these are automatically also used for the second and third generation. If off, then couplings can be chosen separately for each generation.

          Here are the couplings always valid for the first generation, and normally also for the second and third by trivial analogy:

          Zprime:vd   (default = -0.693)
          vector coupling of d quarks.

          Zprime:ad   (default = -1.)
          axial coupling of d quarks.

          Zprime:vu   (default = 0.387)
          vector coupling of u quarks.

          Zprime:au   (default = 1.)
          axial coupling of u quarks.

          Zprime:ve   (default = -0.08)
          vector coupling of e leptons.

          Zprime:ae   (default = -1.)
          axial coupling of e leptons.

          Zprime:vnue   (default = 1.)
          vector coupling of nu_e neutrinos.

          Zprime:anue   (default = 1.)
          axial coupling of nu_e neutrinos.

          Here are the further couplings that are specific for a scenario with Zprime:universality switched off:

          Zprime:vs   (default = -0.693)
          vector coupling of s quarks.

          Zprime:as   (default = -1.)
          axial coupling of s quarks.

          Zprime:vc   (default = 0.387)
          vector coupling of c quarks.

          Zprime:ac   (default = 1.)
          axial coupling of c quarks.

          Zprime:vmu   (default = -0.08)
          vector coupling of mu leptons.

          Zprime:amu   (default = -1.)
          axial coupling of mu leptons.

          Zprime:vnumu   (default = 1.)
          vector coupling of nu_mu neutrinos.

          Zprime:anumu   (default = 1.)
          axial coupling of nu_mu neutrinos.

          Zprime:vb   (default = -0.693)
          vector coupling of b quarks.

          Zprime:ab   (default = -1.)
          axial coupling of b quarks.

          Zprime:vt   (default = 0.387)
          vector coupling of t quarks.

          Zprime:at   (default = 1.)
          axial coupling of t quarks.

          Zprime:vtau   (default = -0.08)
          vector coupling of tau leptons.

          Zprime:atau   (default = -1.)
          axial coupling of tau leptons.

          Zprime:vnutau   (default = 1.)
          vector coupling of nu_tau neutrinos.

          Zprime:anutau   (default = 1.)
          axial coupling of nu_tau neutrinos.

          The coupling to the decay channel Z'^0 -> W^+ W^- is more model-dependent. By default it is therefore off, but can be switched on as follows. Furthermore, we have left some amount of freedom in the choice of decay angular correlations in this channel, but obviously alternative shapes could be imagined.

          Zprime:coup2WW   (default = 0.; minimum = 0.)
          the coupling Z'^0 -> W^+ W^- is taken to be this number times m_W^2 / m_Z'^2 times the Z^0 -> W^+ W^- coupling. Thus a unit value corresponds to the Z^0 -> W^+ W^- coupling, scaled down by a factor m_W^2 / m_Z'^2, and gives a Z'^0 partial width into this channel that again increases linearly. If you cancel this behaviour, by letting Zprime:coup2WW be proportional to m_Z'^2 / m_W^2, you instead obtain a partial width that goes like the fifth power of the Z'^0 mass. These two extremes correspond to the "extended gauge model" and the "reference model", respectively, of [Alt89]. Note that this channel only includes the pure Z' part, while f fbar -> gamma^*/Z^*0 -> W^+ W^- is available as a separate electroweak process.

          Zprime:anglesWW   (default = 0.; minimum = 0.; maximum = 1.)
          in the decay chain Z'^0 -> W^+ W^- ->f_1 fbar_2 f_3 fbar_4 the decay angular distributions is taken to be a mixture of two possible shapes. This parameter gives the fraction that is distributed as in Higgs h^0 -> W^+ W^- (longitudinal bosons), with the remainder (by default all) is taken to be the same as for Z^0 -> W^+ W^- (a mixture of transverse and longitudinal bosons).

          A massive Z'^0 is also likely to decay into Higgs bosons and potentially into other now unknown particles. Such possibilities clearly are quite model-dependent, and have not been included for now.

          W'^+-

          The W'^+- implementation is less ambitious than the Z'^0. Specifically, while indirect detection of a Z'^0 through its interference contribution is a possible discovery channel in lepton colliders, there is no equally compelling case for W^+-/W'^+- interference effects being of importance for discovery, and such interference has therefore not been implemented for now. Related to this, a Z'^0 could appear on its own in a new U(1) group, while W'^+- would have to sit in a SU(2) group and thus have a Z'^0 partner that is likely to be found first. Only one process is implemented but, like for the W^+-, the ISR showers contain automatic matching to the W'^+- + 1 jet matrix elements.

          NewGaugeBoson:ffbar2Wprime On Off   (default = off)
          Scattering f fbar' -> W'^+-. Code 3021.

          The couplings of the W'^+- are here assumed universal, i.e. the same for all generations. One may set vector and axial couplings freely, separately for the q qbar' and the l nu_l decay channels. The defaults correspond to the V - A structure and normalization of the Standard Model W^+-, but can be changed to simulate a wide selection of models. One limitation is that, for simplicity, the same Cabibbo--Kobayashi--Maskawa quark mixing matrix is assumed as for the standard W^+-. Depending on your assumed neutrino nature you may want to restrict your freedom in the lepton sector, but no limitations are enforced by the program.

          Wprime:vq   (default = 1.)
          vector coupling of quarks.

          Wprime:aq   (default = -1.)
          axial coupling of quarks.

          Wprime:vl   (default = 1.)
          vector coupling of leptons.

          Wprime:al   (default = -1.)
          axial coupling of leptons.

          The coupling to the decay channel W'^+- -> W^+- Z^0 is more model-dependent, like for Z'^0 -> W^+ W^- described above. By default it is therefore off, but can be switched on as follows. Furthermore, we have left some amount of freedom in the choice of decay angular correlations in this channel, but obviously alternative shapes could be imagined.

          Wprime:coup2WZ   (default = 0.; minimum = 0.)
          the coupling W'^0 -> W^+- Z^0 is taken to be this number times m_W^2 / m_W'^2 times the W^+- -> W^+- Z^0 coupling. Thus a unit value corresponds to the W^+- -> W^+- Z^0 coupling, scaled down by a factor m_W^2 / m_W'^2, and gives a W'^+- partial width into this channel that increases linearly with the W'^+- mass. If you cancel this behaviour, by letting Wprime:coup2WZ be proportional to m_W'^2 / m_W^2, you instead obtain a partial width that goes like the fifth power of the W'^+- mass. These two extremes correspond to the "extended gauge model" and the "reference model", respectively, of [Alt89].

          Wprime:anglesWZ   (default = 0.; minimum = 0.; maximum = 1.)
          in the decay chain W'^+- -> W^+- Z^0 ->f_1 fbar_2 f_3 fbar_4 the decay angular distributions is taken to be a mixture of two possible shapes. This parameter gives the fraction that is distributed as in Higgs H^+- -> W^+- Z^0 (longitudinal bosons), with the remainder (by default all) is taken to be the same as for W^+- -> W^+- Z^0 (a mixture of transverse and longitudinal bosons).

          A massive W'^+- is also likely to decay into Higgs bosons and potentially into other now unknown particles. Such possibilities clearly are quite model-dependent, and have not been included for now.

          R^0

          The R^0 boson (particle code 41) represents one possible scenario for a horizontal gauge boson, i.e. a gauge boson that couples between the generations, inducing processes like s dbar -> R^0 -> mu^- e^+. Experimental limits on flavour-changing neutral currents forces such a boson to be fairly heavy. In spite of being neutral the antiparticle is distinct from the particle: one carries a net positive generation number and the other a negative one. This particular model has no new parameters beyond the R^0 mass. Decays are assumed isotropic. For further details see [Ben85].

          NewGaugeBoson:ffbar2R0 On Off   (default = off)
          Scattering f_1 fbar_2 -> R^0 -> f_3 fbar_4, where f_1 and fbar_2 are separated by +- one generation and similarly for f_3 and fbar_4. Thus possible final states are e.g. d sbar, u cbar s bbar, c tbar, e- mu+ and mu- tau+. Code 3041. "?>
          pythia8-8.1.80.orig/phpdoc/Glossary.php0000644000175000017500000000717212217615312016131 0ustar sunsun Glossary SETTINGS SAVED TO FILE

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          Glossary

          BR
          Beam Remnants; not much used since it may be confused with Branching Ratio
          BSM
          Beyond-the-Standard-Model physics, as a generic term for anything not contained within the SM
          FSR
          Final-State Radiation, implemented in terms of timelike showers
          LHA
          Les Houches Accord for user processes, describing which process-level information should be stored to allow further showering and hadronization of "skeleton" hard processes
          LHAPDF
          Les Houches Accord Parton Distribution Functions, originally a standard format for defining PDF's and later a library with such PDF's
          LHEF
          Les Houches Event File(s), a file format for storing LHA process and event information
          ISR
          Initial-State Radiation, implemented in terms of spacelike showers
          MPI
          Multiparton Interactions, i.e. several (more or less) independent parton-parton subcollisions as part of a hadron-hadron event (previously called MI for multiple interactions)
          MSSM
          Minimal Supersymmetric extension of the Standard Model
          PDF
          Parton Distribution Function (alternatively Parton Density Function)
          PDG code
          a scheme for assigning unique integers, particle identity codes, to known and hypothetical particles; code rules and tables are published in the RPP (see below).
          pileup
          several hadron-hadron collisions in a bunch crossing; not to be confused with MPI
          RPP
          Review of Particle Physics, the biannual review by the ParticleData Group (PDG) from which many Standard-Model parameter values and much particle data has been taken (but, given the poor data on many hadron resonances, a lot of extra (guess)work is needed)
          setting
          collectively used to denote all the boolean flag, integer mode, double-precision parm and string word variables that can be set by the user to steer the behaviour of a run; normally particle data are considered separately but clearly are closely related
          SLHA
          SUSY Les Houches Accord for interchange of mass and coupling information in SUSY scenarios, via a well-defined file format
          SM
          the Standard Model of particle physics
          SUSY
          SUperSYmmetry
          units
          Normal PYTHIA input, internal operations and output is based on a set of standard units, such as:
          GeV for all energies, momenta and masses, always with c = 1;
          mm for all distances and mm/c for all times, so that again they match for c = 1;
          mb for all cross sections (but input or output via the Les Houches Accord takes into account that the unit there is pb)
          pythia8-8.1.80.orig/phpdoc/Tunes.php0000644000175000017500000004171012217615312015420 0ustar sunsun Tunes SETTINGS SAVED TO FILE

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          Tunes

          Since some physics aspects cannot be derived from first principles, this program contains many parameters that represent a true uncertainty in our understanding of nature. Particularly afflicted are the areas of hadronization and multiparton interactions, which both involve nonperturbative QCD physics.

          Technically, PYTHIA parameters can be varied independently of each other, but the physical requirement of a sensible description of a set of data leads to correlations and anticorrelations between the parameters. Hence the need to produce tunes, not of one parameter at a time, but simultaneously for a group of them. A well-known (separate) such example is parton densities, where combined tunes to a wide range of data have been produced, that can then be obtained prepackaged.

          Given the many PYTHIA parameters to be tuned, it is convenient to divide the task into subtasks. Firstly, if we assume jet universality, hadronization and final-state parton showers should be tuned to e^+e^- annihilation data, notably from LEP1, since this offers the cleanest environment. Secondly, with such parameters fixed, hadron collider data should be studied to pin down multiparton interactions and other further aspects, such as initial-state radiation. Ideally this would be done separately for diffractive and non-diffractive events, although it is not possible to have a clean separation. (Thirdly would come anything else, such as physics with photon beams, which involve further parameters, but that is beyond the current scope.)

          The first step in this program has now been taken, with a tune to LEP1 data by Hendrik Hoeth, using the Rivet + Professor framework. Starting with version 8.125 it defines the default values for hadronization parameters and timelike showers.

          The situation is more complicated for hadronic interactions in general and multiparton interactions in particular, where PYTHIA 8 is more different from PYTHIA 6, and therefore more work is needed. Specifically, it is not possible to "port" a PYTHIA 6 tune to PYTHIA 8.

          A first simple tune, appropriately called "Tune 1", became default starting with version 8.127. It was noted, in particular by Hendrik Hoeth, that this tune had a tension between parameters needed to describe minimum-bias and underlying-event activity. Therefore some further physics features were introduced in the code itself [Cor10a], which were made default as of 8.140. This version also included two new tunes, 2C and 2M, based on the CTEQ 6L1 and the MRST LO** PDF sets, respectively. These have been made by hand, as a prequel to complete Professor-style tunings.

          The very first data to come out of the LHC showed a higher rapidity plateau than predicted for current PYTHIA 6 tunes, also for the lower energies. This may suggest some tension in the data. Two alternatives, 3C and 3M, were produced by a few brute-force changes of 2C and 2M. These were introduced in 8.140, but discontinued in 8.145 in favour of the new 4C tune, that is based on a more serious study of some early LHC data, see [Cor10a]. Following the comparative studies in [Buc11], which independently confirmed a reasonable agreement with LHC data, tune 4C was made the default as of 8.150. A variant is tune 4Cx, where the Gaussian matter profile has an x-dependent width [Cor11].

          Several ATLAS tunes have now been included, obtained with different PDFs and with different emphasis on minimum-bias and underlying-event data [ATL12]. These typically require LHAPDF to be linked, but this can be avoided in cases where the same PDF set is implemented internally.

          Central diffraction is a recent addition to the "soft QCD" process palette, and is thus not yet included in tunes; indeed its cross section is actively zeroed. You can switch it back on after you have selected your tune, with SigmaTotal:zeroAXB = off. But note that, since the total cross section is assumed unchanged, the nondiffractive cross section is reduced and thus also the MPI machinery affected, even if effects should not be big (for a small central diffractive cross section).

          Note that comparisons with data also require that other aspects agree, such as that decay chains are stopped at an agreed-on level. For instance, in the ATLAS tunes all particles with a lifetime above 10 mm are considered stable, ParticleDecays:limitTau0 = on, ParticleDecays:tau0Max = 10. We have chosen not to include this as part of the tune settings itself, since the tune as such could still be used with any other choice of stable and unstable particles.

          Further comparisons have been posted on the MCPLOTS pages. They have been produced with help of the Rivet package [Buc10].

          In the future we hope to see further PYTHIA 8 tunes appear. Like with parton distributions, there is likely to be several tunes, because different sets of data will pull in different directions, by imperfections in the model or in the data, and by differences in the chosen tuning strategies. We therefore propose to collect some of these tunes here, in a prepackaged form. Of course, in all cases it is a matter of setting values for parameters already defined elsewhere, so the tunes offer no new functionality, only a more convenient setup.

          You should be aware that the evolution of the program will not guarantee complete backwards compatibility between versions. Most obviously this concerns bug fixes. But also for some other major changes, like the introduction of the new diffractive machinery, the default behaviour of old tunes has been changed retroactively. (Which should be fine for diffraction, since previous tunes were not based on data strongly influenced by diffraction.)

          The setup of the tunes is special, in that the choice of a tune forces the change of several different flags, modes and parameters. Furthermore a design principle has been that it should be possible to start out from a tune and then change a few of its settings. This gives power and flexibility at the expense of requiring a more careful ordering of commands. We therefore here sketch the order in which operations are carried out.

          1. The constructor of a Pythia instance will read in all settings, and initialize them with their default values.
          2. At the end of this operation, the Tune:ee and Tune:pp modes (see further below) are checked. If either of them are positive the methods Settings::initTuneEE(...) and Settings::initTunePP(...), respectively, are called to overwrite the whole collection of settings in the relevant tune. Zero (or negative) means that nothing will be done.
          3. After the Pythia constructor all the relevant values for the default tune(s) have thus been set up.
          4. You as a user can now start to overwrite the values at will, using Pythia::readFile(...) to read a configuration file, or a list of Pythia::readString(...) commands, or the lower-level Settings methods. All changes are made in the order in which the commands are encountered during the execution. A given variable can be changed multiparton times, but it is the latest change that sets the current value.
          5. The two Tune:ee and Tune:pp modes can also be changed in exactly the same way as described for all other settings above. Unique for them, however, is that when one of them is encountered it also initiates a call to the initTuneEE(...) or initTunePP(...) method, respectively. In such cases all settings affected by the e^+e^- or pp/ppbar tune are first reset to the default values (the -1 options) and thereafter the relevant tune is set up.
          6. It is possible to mix commands of type 4 and 5 in any order; it is always the last change that counts. That is, any changes you have made to variables of a tune before a Tune:ee or Tune:pp command are overwritten by it, while variables you set after will overwrite the tune values. As a rule, therefore, you want to begin with the tune choice, and thereafter modify only a small part of its settings.
          7. Needless to say, the flexibility can lead to unwanted setups if you do not exercise some discipline. It is therefore recommended that you always check the listing obtained with Pythia::settings.listChanged() to confirm that the final set of changes is the intended one.


          Tune:ee   (default = 0; minimum = -1; maximum = 3)
          Choice of tune to e^+e^- data, mainly for the hadronization and timelike-showering aspects of PYTHIA. You should study the Settings::initTuneEE(...) method to find exactly which are the settings for the respective tune.
          -1 : reset all values that are affected by any of the e^+e^- tunes to the default values. This option can be used on its own, but is also automatically used as a first step for either of the positive tune values below, to undo the effect of previous tune settings.
          0 : no values are overwritten during the initial setup, step 2 above. Note that changing to 0 in the user code has no effect; if you want to restore the individual settings you should instead use -1.
          1 : the original PYTHIA 8 parameter set, based on some very old flavour studies (with JETSET around 1990) and a simple tune of alpha_strong to three-jet shapes to the new pT-ordered shower. These were the default values before version 8.125.
          2 : a tune by Marc Montull to the LEP 1 particle composition, as published in the RPP (August 2007). No related (re)tune to event shapes has been performed, however.
          3 : a tune to a wide selection of LEP1 data by Hendrik Hoeth within the Rivet + Professor framework, both to hadronization and timelike-shower parameters (June 2009). These are the default values starting from version 8.125, so currently there is no need for this option.


          Tune:preferLHAPDF On Off   (default = on)
          Tunes made by experimental collaborations typically use the LHAPDF package to obtain their PDF values, and so PYTHIA has to be linked accordingly. For PDFs implemented natively in PYTHIA it is possible to use the respective tunes, without having to link to LHAPDF, if you set Tune:preferLHAPDF = off before the Tune:pp choice.

          Tune:pp   (default = 5; minimum = -1; maximum = 13)
          Choice of tune to pp/ppbar data, mainly for the initial-state-radiation, multiparton-interactions and beam-remnants aspects of PYTHIA. Note that the previous crude (non-)tunes 3C and 3M are removed as of 8.145, superseded by the 4C tune. You should study the Settings::initTunePP(...) method to find exactly which are the settings for the respective tune.
          -1 : reset all values that are affected by any of the pp/ppbar tunes to the default values. This option can be used on its own, but is also automatically used as a first step for either of the positive tune values below, to undo the effect of previous tune settings.
          0 : no values are overwritten during the initial setup, step 2 above. Note that changing to 0 in the user code has no effect; if you want to restore the individual settings you should instead use -1.
          1 : default used up to version 8.126, based on some early and primitive comparisons with data.
          2 : "Tune 1", default in 8.127 - 8.139, based on some data comparisons by Peter Skands. Largely but not wholly overlaps with the default option 0.
          3 : "Tune 2C", introduced with 8.140 Cor10a. It uses the CTEQ 6L1 PDF, and is intended to give good agreement with much of the published CDF data.
          4 : "Tune 2M", introduced with 8.140 Cor10a. It is uses the MRST LO** PDF, which has a momentum sum somewhat above unity, which is compensated by a smaller alpha_s than in the previous tune. Again it is intended to give good agreement with much of the published CDF data.
          5 : "Tune 4C", new tune, introduced with 8.145 Cor10a. Starts out from tune 2C, but with a reduced cross section for diffraction, plus modified multiparton interactions parameters to give a higher and more rapidly increasing charged pseudorapidity plateau, for better agreement with some early key LHC numbers. See also the comparative study in Buc11.
          6 : "Tune 4Cx", based on tune 4C, but using the x-dependent matter profile, MultipartonInteractions:bProfile = 4 and an increased MultipartonInteractions:pT0Ref Cor11.
          7 : "ATLAS MB Tune A2-CTEQ6L1", a minimum-bias tune based on tune 4Cx, but without rapidity-ordered spacelike emissions ATL12. Uses CTEQ 6L1, by default from LHAPDF.
          8 : "ATLAS MB Tune A2-MSTW2008LO", as above, but uses MSTW 2008 LO, by default from LHAPDF.
          9 : "ATLAS UE Tune AU2-CTEQ6L1", an underlying-event tune based on tune 4Cx, but without rapidity-ordered spacelike emissions ATL12. Uses CTEQ 6L1, by default from LHAPDF.
          10 : "ATLAS UE Tune AU2-MSTW2008LO", as above, but uses MSTW 2008 LO, by default from LHAPDF.
          11 : "ATLAS UE Tune AU2-CT10", as above, but uses CT 10, which is not currently implemented in PYTHIA, so you must link LHAPDF.
          12 : "ATLAS UE Tune AU2-MRST2007LO*", as above, but uses MRST 2007 LO*, by default from LHAPDF.
          13 : "ATLAS UE Tune AU2-MRST2007LO**", as above, but uses MRST 2007 LO**, by default from LHAPDF.
          "?>
          pythia8-8.1.80.orig/phpdoc/EventInformation.php0000644000175000017500000007761712217615312017630 0ustar sunsun Event Information SETTINGS SAVED TO FILE

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          Event Information

          The Info class collects various one-of-a-kind information, some relevant for all events and others for the current event. An object info is a public member of the Pythia class, so if you e.g. have declared Pythia pythia, the Info methods can be accessed by pythia.info.method(). Most of this is information that could also be obtained e.g. from the event record, but is here more directly available. It is primarily intended for processes generated internally in PYTHIA, but many of the methods would work also for events fed in via the Les Houches Accord.

          List information

          void Info::list()  
          a listing of most of the information set for the current event.

          The beams

          int Info::idA()  
          int Info::idB()  
          the identities of the two beam particles.

          double Info::pzA()  
          double Info::pzB()  
          the longitudinal momenta of the two beam particles.

          double Info::eA()  
          double Info::eB()  
          the energies of the two beam particles.

          double Info::mA()  
          double Info::mB()  
          the masses of the two beam particles.

          double Info::eCM()  
          double Info::s()  
          the CM energy and its square for the two beams.

          Initialization

          bool Info::tooLowPTmin()  
          normally false, but true if the proposed pTmin scale was too low in timelike or spacelike showers, or in multiparton interactions. In the former case the pTmin is raised to some minimal value, in the latter the initialization fails (it is impossible to obtain a minijet cross section bigger than the nondiffractive one by reducing pTmin).

          The event type

          string Info::name()  
          int Info::code()  
          the name and code of the process that occurred.

          int Info::nFinal()  
          the number of final-state partons in the hard process.

          bool Info::isResolved()  
          are beam particles resolved, i.e. were PDF's used for the process?

          bool Info::isDiffractiveA()  
          bool Info::isDiffractiveB()  
          is either beam diffractively excited?

          bool Info::isDiffractiveC()  
          is there central diffraction (a.k.a. double Pomeron exchange)?

          bool Info::isNonDiffractive()  
          is the process the SoftQCD:nonDiffractive one, i.e. corresponding to the full inelastic nondiffractive part of the total cross section. (Note that a hard process, say Z^0 production, normally is nondiffractive, but this is not what we aim at here, and so the method would return false, unless the Z^0 had been generated as part of the MPI machinery for the SoftQCD:nonDiffractive component.)

          bool Info::isMinBias()  
          the same as above, retained for backwards compatibility, but to be removed in PYTHIA 8.2.

          bool Info::isLHA()  
          has the process been generated from external Les Houches Accord information?

          bool Info::atEndOfFile()  
          true if a linked Les Houches class refuses to return any further events, presumably because it has reached the end of the file from which events have been read in.

          bool Info::hasSub()  
          does the process have a subprocess classification? Currently only true for nondiffractive and Les Houches events, where it allows the hardest collision to be identified.

          string Info::nameSub()  
          int Info::codeSub()  
          int Info::nFinalSub()  
          the name, code and number of final-state partons in the subprocess that occurred when hasSub() is true. For a minimum-bias event the code would always be 101, while codeSub() would vary depending on the actual hardest interaction, e.g. 111 for g g -> g g. For a Les Houches event the code would always be 9999, while codeSub() would be the external user-defined classification code. The methods below would also provide information for such particular subcollisions.

          Hard process initiators

          The methods in this sections refer to the two initial partons of the hard 2 -> n process (diffraction excluded; see below).

          int Info::id1()  
          int Info::id2()  
          the identities of the two partons coming in to the hard process.

          double Info::x1()  
          double Info::x2()  
          x fractions of the two partons coming in to the hard process.

          double Info::y()  
          double Info::tau()  
          rapidity and scaled mass-squared of the hard-process subsystem, as defined by the above x values.

          bool Info::isValence1()  
          bool Info::isValence2()  
          true if the two hard incoming partons have been picked to belong to the valence piece of the parton-density distribution, else false. Should be interpreted with caution. Information is not set if you switch off parton-level processing.

          Hard process parton densities and scales

          The methods in this section refer to the partons for which parton densities have been defined, in order to calculate the cross section of the hard process (diffraction excluded; see below).

          These partons would normally agree with the ones above, the initiators of the 2 -> n process, but it does not have to be so. Currently the one counterexample is POWHEG events [Ali10]. Here the original hard process could be 2 -> (n-1). The NLO machinery at times would add an initial-state branching to give a 2 -> n process with a changed initial state. In that case the values in this section refer to the original 2 -> (n-1) state and the initiator ones above to the complete2 -> n process. The Info::list() printout will contain a warning in such cases.

          For external events in the Les Houches format, the pdf information is obtained from the optional #pdf line. When this information is absent, the parton identities and x values agree with the initiator ones above, while the pdf values are unknown and therefore set to vanish. The alpha_s and alpha_em values are part of the compulsory information. The factorization and renormalization scales are both equated with the one compulsory scale value in the Les Houches standard, except when a #pdf line provides the factorization scale separately. If alpha_s, alpha_em or the compulsory scale value are negative at input then new values are defined as for internal processes.

          int Info::id1pdf()  
          int Info::id2pdf()  
          the identities of the two partons for which parton density values are defined.

          double Info::x1pdf()  
          double Info::x2pdf()  
          x fractions of the two partons for which parton density values are defined.

          double Info::pdf1()  
          double Info::pdf2()  
          parton densities x*f(x,Q^2) evaluated for the two incoming partons; could be used e.g. for reweighting purposes in conjunction with the idpdf, xpdf and QFac methods. Events obtained from external programs or files may not contain this information and, if so, 0 is returned.

          double Info::QFac()  
          double Info::Q2Fac()  
          the Q or Q^2 factorization scale at which the densities were evaluated.

          double Info::alphaS()  
          double Info::alphaEM()  
          the alpha_strong and alpha_electromagnetic values used for the hard process.

          double Info::QRen()  
          double Info::Q2Ren()  
          the Q or Q^2 renormalization scale at which alpha_strong and alpha_electromagnetic were evaluated.

          double Info::scalup()  
          returns the stored SCALUP value for Les Houches events, and else zero. It may agree with both the QFac() and QRen() values, as explained above. However, to repeat, should the input SCALUP scale be negative, separate positive factorization and renormalization scales are calculated and set as for internally generated events. Furthermore, when PDF info is supplied for the Les Houches event, the factorization scale is set by this PDF info (scalePDF), which can disagree with SCALUP.

          Hard process kinematics

          The methods in this section provide info on the kinematics of the hard processes, with special emphasis on 2 -> 2 (diffraction excluded; see below).

          double Info::mHat()  
          double Info::sHat()  
          the invariant mass and its square for the hard process.

          double Info::tHat()  
          double Info::uHat()  
          the remaining two Mandelstam variables; only defined for 2 -> 2 processes.

          double Info::pTHat()  
          double Info::pT2Hat()  
          transverse momentum and its square in the rest frame of a 2 -> 2 processes.

          double Info::m3Hat()  
          double Info::m4Hat()  
          the masses of the two outgoing particles in a 2 -> 2 processes.

          double Info::thetaHat()  
          double Info::phiHat()  
          the polar and azimuthal scattering angles in the rest frame of a 2 -> 2 process.

          Diffraction

          Information on the primary elastic or ";?>diffractive process (A B -> A B, X1 B, A X2, X1 X2, A X B) can be obtained with the methods in the "Hard process kinematics" section above. The variables here obviously are s, t, u, ... rather than sHat, tHat, uHat, ..., but the method names remain to avoid unnecessary duplication. Most other methods are irrelevant for a primary elastic/diffractive process.

          Central diffraction A B -> A X B is a 2 -> 3 process, and therefore most of the 2 -> 2 variables are no longer relevant. The tHat() and uHat() methods instead return the two t values at the A -> A and B -> B vertices, and pTHat() the average transverse momentum of the three outgoing "particles", while thetaHat() and phiHat() are undefined.

          While the primary interaction does not contain a hard process, the diffractive subsystems can contain them, but need not. Specifically, double diffraction can contain two separate hard subprocesses, which breaks the methods above. Most of them have been expanded with an optional argument to address properties of diffractive subsystems. This argument can take four values:

          • 0 : default argument, used for normal nondiffractive events or the primary elastic/diffractive process (see above);
          • 1 : the X1 system in single diffraction A B -> X1 B or double diffraction A B -> X1 X2;
          • 2 : the X2 system in single diffraction A B -> A X2 or double diffraction A B -> X1 X2;
          • 3 : the X system in central diffraction A B -> A X B.
          The argument is defined for all of the methods in the three sections above, "Hard process initiators", "Hard process parton densities and scales" and "Hard process kinematics", with the exception of the isValence methods. Also the four final methods of "The event type" section, the ...Sub() methods, take this argument. But recall that they will only provide meaningful answers, firstly if there is a system of the requested type, and secondly if there is a hard subprocess in this system. A simple check for this is that id1() has to be nonvanishing. The methods below this section do not currently provide information specific to diffractive subsystems, e.g. the MPI information is not bookkept in such cases.

          Event weight and activity

          double Info::weight()  
          weight assigned to the current event. Is normally 1 and thus uninteresting. However, there are several cases where one may have nontrivial event weights. These weights must the be used e.g. when filling histograms.
          (i) In the ";?> PhaseSpace:increaseMaximum = off default strategy, an event with a differential cross-section above the assumed one (in a given phase-space point) is assigned a weight correspondingly above unity. This should happen only very rarely, if at all, and so could normally be disregarded.
          (ii) The ";?>User Hooks class offers the possibility to bias the selection of phase space points, which means that events come with a compensating weight, stored here.
          (iii) For Les Houches events some strategies allow negative weights, which then after unweighting lead to events with weight -1. There are also Les Houches strategies where no unweighting is done, so events come with a weight. Specifically, for strategies +4 and -4, the event weight is in units of pb. (Internally in mb, but converted at output.)

          double Info::weightSum()  
          Sum of weights accumulated during the run. For unweighted events this agrees with the number of generated events. In order to obtain histograms normalized "per event", at the end of a run, histogram contents should be divided by this weight. (And additionally divided by the bin width.) Normalization to cross section also required multiplication by sigmaGen() below.

          int Info::lhaStrategy()  
          normally 0, but if Les Houches events are input then it gives the event weighting strategy, see ";?>Les Houches Accord.

          int Info::nISR()  
          int Info::nFSRinProc()  
          int Info::nFSRinRes()  
          the number of emissions in the initial-state showering, in the final-state showering excluding resonance decays, and in the final-state showering inside resonance decays, respectively.

          double Info::pTmaxMPI()  
          double Info::pTmaxISR()  
          double Info::pTmaxFSR()  
          Maximum pT scales set for MPI, ISR and FSR, given the process type and scale choice for the hard interactions. The actual evolution will run down from these scales.

          double Info::pTnow()  
          The current pT scale in the combined MPI, ISR and FSR evolution. Useful for classification in ";?>user hooks, but not once the event has been evolved.

          double Info::mergingWeight()  
          combined leading-order merging weight assigned to the current event, if tree-level multi-jet merging (i.e. CKKW-L or UMEPS merging) is attempted. If tree-level multi-jet merging is performed, all histograms should be filled with this weight, as discussed in CKKW-L Merging and UMEPS Merging.

          double Info::mergingWeightNLO()  
          combined NLO merging weight assigned to the current event, if NLO multi-jet merging (i.e. NL3 or UNLOPS merging) is attempted. If NLO multi-jet merging is performed, all histograms should be filled with this weight, as discussed in NLO Merging .

          Multiparton interactions

          As already noted, these methods do not make sense for diffractive topologies, and should not be used there. Partly this is physics, but mainly it is for technical reasons, e.g. that double diffraction involves two separate systems that would have to be bookkept as such.

          double Info::a0MPI()  
          The value of a0 when an x-dependent matter profile is used, MultipartonInteractions:bProfile = 4.

          double Info::bMPI()  
          The impact parameter b assumed for the current collision when multiparton interactions are simulated. Is not expressed in any physical size (like fm), but only rescaled so that the average should be unity for minimum-bias events (meaning less than that for events with hard processes).

          double Info::enhanceMPI()  
          The choice of impact parameter implies an enhancement or depletion of the rate of subsequent interactions, as given by this number. Again the average is normalized be unity for minimum-bias events (meaning more than that for events with hard processes).

          int Info::nMPI()  
          The number of hard interactions in the current event. Is 0 for elastic and diffractive events, and else at least 1, with more possible from multiparton interactions.

          int Info::codeMPI(int i)  
          double Info::pTMPI(int i)  
          the process code and transverse momentum of the i'th subprocess, with i in the range from 0 to nMPI() - 1. The values for subprocess 0 is redundant with information already provided above.

          int Info::iAMPI(int i)  
          int Info::iBMPI(int i)  
          are normally zero. However, if the i'th subprocess is a rescattering, i.e. either or both incoming partons come from the outgoing state of previous scatterings, they give the position in the event record of the outgoing-state parton that rescatters. iAMPI and iBMPI then denote partons coming from the first or second beam, respectively.

          double Info::eMPI(int i)  
          The enhancement or depletion of the rate of the i'th subprocess. Is primarily of interest for the MultipartonInteractions:bProfile = 4 option, where the size of the proton depends on the x values of the colliding partons. Note that eMPI(0) = enhanceMPI().

          Cross sections

          Here are the currently available methods related to the event sample as a whole, for the default value i = 0, and otherwise for the specific process code provided as argument. This is the number obtained with Info::code(), while the further subdivision given by Info::codeSub() is not bookkept. While continuously updated during the run, it is recommended only to study these properties at the end of the event generation, when the full statistics is available. The individual process results are not available if ";?>a second hard process has been chosen, but can be gleaned from the pythia.stat() output.

          long Info::nTried(int i = 0)  
          long Info::nSelected(int i = 0)  
          long Info::nAccepted(int i = 0)  
          the total number of tried phase-space points, selected hard processes and finally accepted events, summed over all allowed processes (i = 0) or for the given process. The first number is only intended for a study of the phase-space selection efficiency. The last two numbers usually only disagree if the user introduces some veto during the event-generation process; then the former is the number of acceptable events found by PYTHIA and the latter the number that also were approved by the user. If you set ";?>a second hard process there may also be a mismatch.

          double Info::sigmaGen(int i = 0)  
          double Info::sigmaErr(int i = 0)  
          the estimated cross section and its estimated error, summed over all allowed processes (i = 0) or for the given process, in units of mb. The numbers refer to the accepted event sample above, i.e. after any user veto.

          Loop counters

          Mainly for internal/debug purposes, a number of loop counters from various parts of the program are stored in the Info class, so that one can keep track of how the event generation is progressing. This may be especially useful in the context of the ";?>User Hooks facility.

          int Info::getCounter(int i)  
          the method that gives you access to the value of the various loop counters.
          argument i : the counter number you want to access:
          argumentoption 0 - 9 : counters that refer to the run as a whole, i.e. are set 0 at the beginning of the run and then only can increase.
          argumentoption 0 : the number of successful constructor calls for the Pythia class (can only be 0 or 1).
          argumentoption 1 : the number of times a Pythia::init(...) call has been begun.
          argumentoption 2 : the number of times a Pythia::init(...) call has been completed successfully.
          argumentoption 3 : the number of times a Pythia::next() call has been begun.
          argumentoption 4 : the number of times a Pythia::next() call has been completed successfully.
          argumentoption 10 - 19 : counters that refer to each individual event, and are reset and updated in the top-level Pythia::next() method.
          argumentoption 10 : the number of times the selection of a new hard process has been begun. Normally this should only happen once, unless a user veto is set to abort the current process and try a new one.
          argumentoption 11 : the number of times the selection of a new hard process has been completed successfully.
          argumentoption 12 : as 11, but additionally the process should survive any user veto and go on to the parton- and hadron-level stages.
          argumentoption 13 : as 11, but additionally the process should survive the parton- and hadron-level stage and any user cuts.
          argumentoption 14 : the number of times the loop over parton- and hadron-level processing has begun for a hard process. Is reset each time counter 12 above is reached.
          argumentoption 15 : the number of times the above loop has successfully completed the parton-level step.
          argumentoption 16 : the number of times the above loop has successfully completed the checks and user vetoes after the parton-level step.
          argumentoption 17 : the number of times the above loop has successfully completed the hadron-level step.
          argumentoption 18 : the number of times the above loop has successfully completed the checks and user vetoes after the hadron-level step.
          argumentoption 20 - 39 : counters that refer to a local part of the individual event, and are reset at the beginning of this part.
          argumentoption 20 : the current system being processed in PartonLevel::next(). Is almost always 1, but for double diffraction the two diffractive systems are 1 and 2, respectively.
          argumentoption 21 : the number of times the processing of the current system (see above) has begun.
          argumentoption 22 : the number of times a step has begun in the combined MPI/ISR/FSR evolution downwards in pT for the current system.
          argumentoption 23 : the number of times MPI has been selected for the downwards step above.
          argumentoption 24 : the number of times ISR has been selected for the downwards step above.
          argumentoption 25 : the number of times FSR has been selected for the downwards step above.
          argumentoption 26 : the number of times MPI has been accepted as the downwards step above, after the vetoes.
          argumentoption 27 : the number of times ISR has been accepted as the downwards step above, after the vetoes.
          argumentoption 28 : the number of times FSR has been accepted as the downwards step above, after the vetoes.
          argumentoption 29 : the number of times a step has begun in the separate (optional) FSR evolution downwards in pT for the current system.
          argumentoption 30 : the number of times FSR has been selected for the downwards step above.
          argumentoption 31 : the number of times FSR has been accepted as the downwards step above, after the vetoes.
          argumentoption 40 - 49 : counters that are unused (currently), and that therefore are free to use, with the help of the two methods below.

          void Info::setCounter(int i, int value = 0)  
          set the above counters to a given value. Only to be used by you for the unassigned counters 40 - 49.
          argument i : the counter number, see above.
          argument value (default = 0) : set the counter to this number; normally the default value is what you want.

          void Info::addCounter(int i, int value = 0)  
          increase the above counters by a given amount. Only to be used by you for the unassigned counters 40 - 49.
          argument i : the counter number, see above.
          argument value (default = 1) : increase the counter by this amount; normally the default value is what you want.

          Parton shower history

          The following methods are mainly intended for internal use, e.g. for matrix-element matching.

          void Info::hasHistory(bool hasHistoryIn)  
          bool Info::hasHistory()  
          set/get knowledge whether the likely shower history of an event has been traced.

          void Info::zNowISR(bool zNowIn)  
          double Info::zNowISR()  
          set/get value of z in latest ISR branching.

          void Info::pT2NowISR(bool pT2NowIn)  
          double Info::pT2NowISR()  
          set/get value of pT^2 in latest ISR branching.

          Header information

          A simple string key/value store, mainly intended for accessing information that is stored in the header block of Les Houches Event (LHE) files. In principle, any LHAup derived class can set this header information, which can then be read out later. Although the naming convention is arbitrary, in practice, it is dictated by the XML-like format of LHE files, see ";?> Les Houches Accord for more details.

          string Info::header(string key)  
          return the header named key

          vector <string> Info::headerKeys()  
          return a vector of all header key names

          void Info::setHeader(string key, string val)  
          set the header named key with the contents of val pythia8-8.1.80.orig/phpdoc/MatchingAndMerging.php0000644000175000017500000002262112217615312020010 0ustar sunsun Matching and Merging SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Matching and Merging

          Starting from a Born-level leading-order (LO) process, higher orders can be included in various ways. The three basic approaches would be
          • A formal order-by-order perturbative calculation, in each order higher including graphs both with one particle more in the final state and with one loop more in the intermediate state. This is accurate to the order of the calculation, but gives no hint of event structures beyond that, with more particles in the final state. Today next-to-leading order (NLO) is standard, while next-to-next-to-leading order (NNLO) is coming. This approach thus is limited to few orders, and also breaks down in soft and collinear regions, which makes it unsuitable for matching to hadronization.
          • Real emissions to several higher orders, but neglecting the virtual/loop corrections that should go with it at any given order. Thereby it is possible to allow for topologies with a large and varying number of partons, at the prize of not being accurate to any particular order. The approach also opens up for doublecounting, and as above breaks down in soft and colliner regions.
          • The parton shower provides an approximation to higher orders, both real and virtual contributions for the emission of arbitrarily many particles. As such it is less accurate than either of the two above, at least for topologies of well separated partons, but it contains a physically sensible behaviour in the soft and collinear limits, and therefore matches well onto the hadronization stage.
          Given the pros and cons, much of the effort in recent years has involved the development of different prescriptions to combine the methods above in various ways.

          The common traits of all combination methods are that matrix elements are used to describe the production of hard and well separated particles, and parton showers for the production of soft or collinear particles. What differs between the various approaches that have been proposed are which matrix elements are being used, how doublecounting is avoided, and how the transition from the hard to the soft regime is handled. These combination methods are typically referred to as "matching" or "merging" algorithms. There is some confusion about the distinction between the two terms, and so we leave it to the inventor/implementor of a particular scheme to choose and motivate the name given to that scheme.

          PYTHIA comes with methods, to be described next, that implement or support several different kind of algorithms. The field is open-ended, however: any external program can feed in ";?>Les Houches events that PYTHIA subsequently showers, adds multiparton interactions to, and hadronizes. These events afterwards can be reweighted and combined in any desired way. The maximum pT of the shower evolution is set by the Les Houches scale, on the one hand, and by the values of the SpaceShower:pTmaxMatch, TimeShower:pTmaxMatch and other parton-shower settings, on the other. Typically it is not possible to achieve perfect matching this way, given that the PYTHIA pT evolution variables are not likely to agree with the variables used for cuts in the external program. Often one can get close enough with simple means but, for an improved matching, ";?>User Hooks can be inserted to control the steps taken on the way, e.g. to veto those parton shower branchings that would doublecount emissions included in the matrix elements.

          Zooming in from the "anything goes" perspective, the list of relevent approaches actively supported is as follows.

          • For many/most resonance decays the first branching in the shower is merged with first-order matrix elements [Ben87, Nor01]. This means that the emission rate is accurate to NLO, similarly to the POWHEG strategy (see below), but built into the ";?>timelike showers. The angular orientation of the event after the first emission is only handled by the parton shower kinematics, however. Needless to say, this formalism is precisely what is tested by Z^0 decays at LEP1, and it is known to do a pretty good job there.
          • Also the ";?>spacelike showers contain a correction to first-order matrix elements, but only for the one-body-final-state processes q qbar -> gamma^*/Z^0/W^+-/h^0/H^0/A0/Z'0/W'+-/R0 [Miu99] and g g -> h^0/H^0/A0, and only to leading order. That is, it is equivalent to the POWHEG formalism for the real emission, but the prefactor "cross section normalization" is LO rather than NLO. Therefore this framework is less relevant, and has been superseded the following ones.
          • The POWHEG strategy [Nas04] provides a cross section accurate to NLO. The hardest emission is constructed with unit probability, based on the ratio of the real-emission matrix element to the Born-level cross section, and with a Sudakov factor derived from this ratio, i.e. the philosophy introduced in [Ben87].
            While POWHEG is a generic strategy, the POWHEG BOX [Ali] is an explicit framework, within which several processes are available. Potential emissions are ordered in a transverse-momentum-related variable. The LHA scale variable encodes this value for each event, and thereby sets the upper limit for subsequent shower emissions. There is a mismatch between the POWHEG BOX and the PYTHIA pT variables, however, which gives imperfections in the transition region [Cor10]. The proposed solution is to allow showers to cover the full phase space, but then veto emissions in the region already covered by the POWHEG BOX evolution. The code required for this can be found in examples/main31. While fairly general, the code would have to be modified to accommodate a different pT scale definition in the POWHEG BOX.
          • The other traditional approach for NLO calculations is the MC@NLO one [Fri02]. In it the shower emission probability, without its Sudakov factor, is subtracted from the real-emission matrix element to regularize divergences. It therefore requires a analytic knowledge of the way the shower populates phase space. Currently there is no MC@NLO implementation for PYTHIA 8, but one is in preparation by Paolo Torrielli and Stefano Frixione, for the aMC@NLO program [Fre11]. The global-recoil option of the PYTHIA final-state shower has been constructed in anticipation of its use for the above-mentioned subtraction.
          • Multi-jet merging in the CKKW-L approach [Lon01] is directly available. Its implementation, relevant parameters and test programs are documented on a ";?>separate page.
          • Multi-jet matching in the MLM approach [Man02, Man07] is also available, either based on the ALPGEN or on the Madgraph variant, and with input events either from ALPGEN or from Madgraph. For details see ";?>separate page.
          • Unitarised matrix element + parton shower merging (UMEPS) is directly available. Its implementation, relevant parameters and test programs are documented on a ";?>separate page.
          • Next-to-leading order multi-jet merging (in the NL3 and UNLOPS approaches) is directly available. Its implementation, relevant parameters and test programs are documented on a ";?>separate page.
          pythia8-8.1.80.orig/phpdoc/ProcessSelection.php0000644000175000017500000001660612217615312017614 0ustar sunsun Process Selection SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

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          Process Selection

          There is no way PYTHIA could contain all processes of interest, neither in terms of potential physics topics nor in terms of high-multiplicity final states. What exists is a reasonably complete setup of all 2 -> 1 and 2 -> 2 processes within the Standard Model, plus some examples of processes beyond that, again for low multiplicities. Combined with the PYTHIA parton showers, this should be enough to get a flying start in the study of many physics scenarios. Other processes could be fed in via the ";?>Les Houches Accord or be implemented as a ";?>Semi-Internal Process. In the latter case the existing processes would act as obvious templates.

          By default all processes are switched off. You should switch on those you want to simulate. This may be done at two (occasionally three) levels, either for each individual process or for a group of processes. That is, a process is going to be generated either if its own flag or its group flag is on. There is no built-in construction to switch on a group and then switch off a few of its members.

          Each process is assigned an integer code. This code is not used in the internal administration of events (so having the same code for two completely different processes would not be a problem), but only intended to allow a simpler user separation of different processes. Also the process name is available, as a string.

          To ease navigation, the list of processes has been split into several separate pages, by main topic. The classification is hopefully intuitive, but by no means unambiguous. For instance, essentially all processes involve QCD, so the "QCD processes" are the ones that only involve QCD. (And also that is not completely true, once one includes all that may happen in multiparton interactions.) On these separate pages also appear the settings that are completely local to that particular process class, but not the ones that have a broader usage.

          ";?>QCD Processes

          QCD processes fall in two main categories: soft and hard. The soft ones contain elastic, diffractive and "minimum-bias" events, together covering the total cross section. Hard processes are the normal 2 -> 2 ones, including charm and bottom production.
          Reserved code range: 101 - 199.

          ";?>Electroweak Processes

          Prompt-photon, gamma^*/Z^0 and W^+- production, plus a few processes with t-channel boson exchange.
          Reserved code range: 201 - 299.

          ";?>Onia Processes

          Colour singlet and octet production of charmonium and bottomonium.
          Reserved code range: 401 - 499 for charmonium and 501 - 599 for bottomonium.

          ";?>Top Processes

          Top production, singly or doubly.
          Reserved code range: 601 - 699.

          ";?>Fourth-Generation Processes

          Production of hypothetical fourth-generation fermions.
          Reserved code range: 801 - 899.

          ";?>Higgs Processes

          Higgs production, within or beyond the Standard Model. See section on Left-Right-Symmetry processes for doubly charged Higgs bosons.
          Reserved code range: 901 - 999 for a Standard Model Higgs and 1001 - 1199 for MSSM Higgs bosons.

          ";?>SUSY Processes

          Production of supersymmetric particles, currently barely begun.
          Reserved code range: 1001 - 2999. (Whereof 1001 - 1199 for Higgs bosons; see above.)

          ";?>New-Gauge-Boson Processes

          Production of new gauge bosons such as Z' and W'.
          Reserved code range: 3001 - 3099.

          ";?>Left-Right-Symmetry Processes

          Production of righthanded Z_R and W_R bosons and of doubly charged Higgs bosons.
          Reserved code range: 3101 - 3199.

          ";?>Leptoquark Processes

          Production of a simple scalar leptoquark state.
          Reserved code range: 3201 - 3299.

          ";?>Compositeness Processes

          Production of excited fermion states and contact-interaction modification to interactions between fermions (excluding technicolor; see below).
          Reserved code range: 4001 - 4099.

          Technicolor Processes

          Production of technicolor particles and modifications of QCD processes by technicolor interactions. Does not exist yet.
          Reserved code range: 4101 - 4199.

          ";?>Hidden Valley Processes

          A scenario for the pair production of new particles with couplings under a new gauge group, with invisible gauge bosons. Radiation of these gauge bosons is included in the standard final-state parton shower.
          Reserved code range: 4901 - 4999.

          ";?>Extra-Dimensional Processes

          A vast area, here represented by the production of a Randall-Sundrum excited graviton state and a Kaluza-Klein gluon, a Kaluza-Klein tower of gamma/Z^0 excitations in one TeV^- sized extra dimension, several Large Extra Dimension processes, and a few related Unparticle processes.
          Reserved code range: 5001 - 5099. pythia8-8.1.80.orig/phpdoc/Frontpage.php0000644000175000017500000001656212217615312016256 0ustar sunsun Front SETTINGS SAVED TO FILE

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          PYTHIA 8

          Welcome to PYTHIA - The Lund Monte Carlo!

          PYTHIA 8 is the successor to PYTHIA 6, rewritten from scratch in C++. With the release of PYTHIA 8.1 it now becomes the official "current" PYTHIA version, although PYTHIA 6.4 will be supported in parallel with it for some time to come. Specifically, the new version has not yet been enough tested and tuned for it to have reached the same level of reliability as the older one. This testing will only happen if people begin to work with the program, however, which is why we encourage a gradual transition to the new version, starting now. There are some new physics features in PYTHIA 8.1, that would make use of it more attractive, but also some topics still missing, where 6.4 would have to be used. Further, many obsolete features will not be carried over, so for some backwards compatibility studies again 6.4 would be the choice.

          Documentation

          On these webpages you will find the up-to-date manual for PYTHIA 8.1. Use the left-hand index to navigate this documentation of program elements, especially of all possible program settings. All parameters are provided with sensible default values, however, so you need only change those of relevance to your particular study, such as choice of beams, processes and phase space cuts. The pages also contain a fairly extensive survey of all methods available to the user, e.g. to study the produced events. What is lacking on these webpages is an overview, on the one hand, and an in-depth physics description, on the other.

          The overview can be found in the attached PDF file
          A Brief Introduction to PYTHIA 8.1
          T. Sjöstrand, S. Mrenna and P. Skands, Comput. Phys. Comm. 178 (2008) 852 [arXiv:0710.3820].
          You are strongly recommended to read this summary when you start out to learn how to use PYTHIA 8.1. Note that some details have changed since the 8.100 version described there.

          For the physics description we refer to the complete
          PYTHIA 6.4 Physics and Manual
          T. Sjöstrand, S. Mrenna and P. Skands, JHEP05 (2006) 026,
          which in detail describes the physics (largely) implemented also in PYTHIA 8, and also provides a more extensive bibliography than found here.

          When you use PYTHIA 8.1, you should therefore cite both, e.g. like
          T. Sjöstrand, S. Mrenna and P. Skands, JHEP05 (2006) 026, Comput. Phys. Comm. 178 (2008) 852.

          Furthermore, a separate
          PYTHIA 8 Worksheet,
          also an attached PDF file, offers a practical introduction to using the generator. It has been developed for and used at a few summer schools, with minor variations, but is also suited for self-study.

          Authors

          Torbjörn Sjöstrand
          Department of Astronomy and Theoretical Physics, Lund University, Sölvegatan 14A, SE-223 62 Lund, Sweden
          phone: + 46 - 46 - 222 48 16, e-mail: torbjorn@thep.lu.se

          Jesper Roy Christiansen
          Department of Astronomy and Theoretical Physics, Lund University, Sölvegatan 14A, SE-223 62 Lund, Sweden
          e-mail: Jesper.Roy.Christiansen@thep.lu.se

          Nishita Desai
          Department of Physics and Astronomy, University College London, Gower Street, London, WC1E 6BT, United Kingdom
          e-mail: Nishita.Desai@cern.ch

          Philip Ilten
          School of Physics, University College Dublin, Belfield, Dublin 4, Ireland
          e-mail: philten@cern.ch

          Stephen Mrenna
          Computing Division, Simulations Group, Fermi National Accelerator Laboratory, MS 234, Batavia, IL 60510, USA
          phone: + 1 - 630 - 840 - 2556, e-mail: mrenna@fnal.gov

          Stefan Prestel
          Theory Group, DESY, Notkestrasse 85, D-22607 Hamburg, Germany
          phone: + 49 - 40 - 8998-4250, e-mail: stefan.prestel@thep.lu.se

          Peter Skands
          Theoretical Physics, CERN, CH-1211 Geneva 23, Switzerland
          phone: + 41 - 22 - 767 2447, e-mail: peter.skands@cern.ch

          Former authors

          Stefan Ask, e-mail: ask.stefan@gmail.com

          Richard Corke, e-mail: r.corke@errno.net

          Further contributions

          Makefiles, configure scripts and HepMC interface by Mikhail Kirsanov.
          Conversion of XML files to PHP ones by Ben Lloyd.
          Simple Makefile for Win32/NMAKE by Bertrand Bellenot.
          Extended Higgs sector partly implemented by Marc Montull.
          Parts of charm and bottom decay tables courtesy DELPHI and LHCb collaborations.
          Tunes and comparisons with data, based on Rivet and Professor, by Hendrik Hoeth.
          Text and code on the use of ROOT in conjunction with PYTHIA by Rene Brun, Andreas Morsch and Axel Naumann.
          Code and data for MRST/MSTW PDFs by Robert Thorne and Graeme Watt.
          Code and data for the CTEQ/CT PDFs by Joey Huston and colleagues.
          Help with implementing new proton PDFs by Tomas Kasemets.
          Code and data for Pomeron PDFs by H1 collaboration and especially Paul Newman.
          Help with implementing new Pomeron fluxes and PDFs by Sparsh Navin.
          The new Hidden Valley code developed together with Lisa Carloni.
          Code for a Kaluza-Klein electroweak gauge boson provided by Noam Hod and Mark Sutton.
          Code for equivalent photon flux around an unresolved proton by Oystein Alvestad.
          The MBR diffractive model and central diffraction by Robert Ciesielski.
          2012 branching ratios for most light hadrons, and the tau lepton, by Anil Pratap Singh.
          The pythia8-config script has been contributed by Andy Buckley, along with many other helpful suggestions.
          Code and data for several of the NNPDF2.3 QCD+QED sets provided by Juan Rojo and Stefano Carrazza.
          The fjcore code from FastJet provided by Matteo Cacciari, Gavin Salam and Gregory Soyez.
          Note: in several cases modifications have been made to the original code, in order to integrate it with PYTHIA. In these cases the blame for any mistakes has to rest with the regular authors.

          Licence

          PYTHIA 8 is licensed under the GNU General Public Licence version 2.
          Please respect the MCnet Guidelines for Event Generator Authors and Users.

          The program and the documentation is Copyright © 2013 Torbjörn Sjöstrand pythia8-8.1.80.orig/phpdoc/ResonanceDecays.php0000644000175000017500000005010312217615312017364 0ustar sunsun Resonance Decays SETTINGS SAVED TO FILE

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          Resonance Decays

          The ResonanceDecays class performs the sequential decays of all resonances formed in the hard process. Note the important distinction between "resonances" and other "particles" made in PYTHIA.
          • The list of resonances contains gamma^*/Z^0, W^+-, top, the Higgs, and essentially all new particles of Beyond-the-Standard-Model physics: further Higgs bosons, sfermions, gauginos, techniparticles, and so on. The partial widths to different decay channels are perturbatively calculable, given the parameters of the respective model, and branching ratios may be allowed to vary across a (reasonably broad) resonance peak. Usually resonances are short-lived, and therefore it makes sense to consider their decays immediately after the primary hard process has been set up. Furthermore, in several cases the decay angular distributions are encoded as part of the specific process, e.g. the W decays differently in f fbar -> W^+-, f fbar -> W^+ W^- and h^0 -> W^+ W^- . All of these particles are (in PYTHIA) only produced as part of the hard process itself, i.e. they are not produced in showers or hadronization processes. Therefore the restriction to specific decay channels can be consistently taken into account as a corresponding reduction in the cross section of a process. Finally, note that all of these resonances have an on-shell mass above 20 GeV, with the exception of some hypothetical weakly interacting and stable particles such as the gravitino.
          • The other particles include normal hadrons and the Standard-Model leptons, including the tau^+-. These can be produced in the normal hadronization and decay description, which involve unknown nonperturbative parameters and multistep chains that cannot be predicted beforehand: a hard process like g g -> g g can develop a shower with a g -> b bbar branching, where the b hadronizes to a B^0bar that oscillates to a B^0 that decays to a tau^+. Therefore any change of branching ratios - most of which are determined from data rather than from first principles anyway - will not be taken into account in the cross section of a process. Exceptions exist, but most particles in this class are made to decay isotropically. Finally, note that all of these particles have a mass below 20 GeV.
          There is one ambiguous case in this classification, namely the photon. The gamma^*/Z^0 combination contains a low-mass peak when produced in a hard process. On the other hand, photons can participate in shower evolution, and therefore a photon originally assumed massless can be assigned an arbitrarily high mass when it is allowed to branch into a fermion pair. In some cases this could lead to double-counting, e.g. between processes such as f fbar -> (gamma^*/Z^0) (gamma^*/Z^0), f fbar -> (gamma^*/Z^0) gamma and f fbar -> gamma gamma. Here it make sense to limit the lower mass allowed for the gamma^*/Z^0 combination, in 23:mMin, to be the same as the upper limit allowed for an off-shell photon in the shower evolution, in TimeShower:mMaxGamma. By default this matching is done at 10 GeV.

          In spite of the above-mentioned differences, the resonances and the other particles are all stored in one common ";?>particle data table, so as to offer a uniform interface to ";?>setting and getting properties such as name, mass, charge and decay modes, also for the ";?>particle properties in the event record. Some methods are specific to resonances, however, in particular for the calculation of partial widths and thereby of branching ratio. For resonances these can be calculated dynamically, set up at initialization for the nominal mass and then updated to the current mass when these are picked according to a Breit-Wigner resonance shape.

          Resonance Decays and Cross Sections

          As already hinted above, you have the possibility to set the allowed decay channels of resonances, see ";?>Particle Data Scheme description. For instance, if you study the process q qbar -> H^0 Z^0 you could specify that the Z^0 should decay only to lepton pairs, the H^0 only to W^+ W^-, the W^+ only to a muon and a neutrino, while the W^- can decay to anything. Unfortunately there are limits to the flexibility: you cannot set a resonance to have different properties in different places of a process, e.g. if instead H^0 -> Z^0 Z^0 in the above process then the three Z^0's would all obey the same rules.

          The restrictions on the allowed final states of a process is directly reflected in the cross section of it. That is, if some final states are excluded then the cross section is reduced accordingly. Such restrictions are built up recursively in cases of sequential decay chains. The restrictions are also reflected in the compositions of those events that actually do get to be generated. For instance, the relative rates of H^0 -> W^+ W^- and H^0 -> Z^0 Z^0 are shifted when the allowed sets of W^+- and Z^0 decay channels are changed.

          We remind that only those particles that Pythia treat as resonances enjoy this property, and only those that are considered as part of the hard process and its associated resonance decays.

          There is one key restriction on resonances:

          ResonanceWidths:minWidth   (default = 1e-20; minimum = 1e-30)
          Minimal allowed width of a resonance, in GeV. If the width falls below this number the resonance is considered stable and will not be allowed to decay. This is mainly intended as a technical parameter, to avoid disasters in cases where no open decay channels exists at all. It could be used for real-life decisions as well, however, but then typically would have to be much bigger than the default value. Special caution would be needed if coloured resonance particles were made stable, since the program would not necessarily know how to hadronize them, and therefore fail at that stage.

          In spite of this technical parameter choice, it is possible to set a lifetime for a resonance, and thereby to obtain displaced vertices. If a resonance is allowed to decay it will do so, irrespective of the location of the decay vertex. This is unlike ";?>normal particle decays, where it is possible to define some region around the primary vertex within which all decays should happen, with particles leaving that region considered stable. The logic is that resonances as a rule are too short-lived for secondary vertices, so if you pick a scenario with a long-lived but unstable resonance it is because you want to study secondary vertices. How to interface those decays to a detector simulation program then is another story, to be solved separately. Do note that a special treatment is needed for coloured long-lived resonances, that form ";?>R-hadrons, and where charge and flavour may change between the production and decay vertices.

          Special properties and methods for resonances

          The method ParticleData::isResonance(id) allows you to query whether a given particle species is considered a resonance or not. You can also change the default value of this flag in the normal way, e.g. pythia.readString("id:isResonance = true").

          An option with a forced width can be set with the id:doForceWidth flag as above, and queried with ParticleData::doForceWidth(id). It is by default off, and should normally so remain. If switched on then the width stored in id:mWidth is strictly used to describe the Breit-Wigner of the resonance. This is unlike the normal behaviour of standard resonances such as the Z^0, W^+-, t or h^0, which have explicit decay-widths formulae encoded, in classes derived from the ";?>ResonanceWidths base class. These formulae are used, e.g., to derive all the Higgs partial widths as a function of the Higgs mass you choose, and at initialization overwrites the existing total width value. The reason for forcing the width to another value specified by you would normally more have to do with experimental issues than with physics ones, e.g. how sensitive your detector would be to changes in the Higgs width by a factor of two. A warning is that such a rescaling could modify the cross section of a process correspondingly for some processes, while leaving it (essentially) unchanged for others (as would seem most logical), depending on how these were encoded. A further warning is that, if you use this facility for Z^0 or Z'^0 with gamma^*/Z^0 or gamma^*/Z^0/Z'^0 interference on, then also the handling of this interference is questionable. So, if you need to use the width-rescaling option, be extremely cautious.

          If a resonance does not have a class of its own, with hardcoded equations for all relevant partial widths, then a simpler object will be created at initialization. This object will take the total width and branching ratios as is (with the optional variations explained in the next section), and thus the rescaling approach brings no further freedom.

          Mainly for internal usage, the ";?>ParticleData contain some special methods that are only meaningful for resonances:

          • resInit(...) to initialize a resonance, possibly including a recalculation of the nominal width to match the nominal mass;
          • resWidth(...) to calculate the partial and total widths at the currently selected mass;
          • resWidthOpen(...) to calculate the partial and total widths of those channels left open by user switches, at the currently selected mass;
          • resWidthStore(...) to calculate the partial and total widths of those channels left open by user switches, at the currently selected mass, and store those as input for a subsequent selection of decay channel;
          • resOpenFrac(...) to return the fraction of the total width that is open by the decay channel selection made by users (based on the choice of ";?>onMode for the various decay channels, recursively calculated for sequential decays);
          • resWidthRescaleFactor(...) returns the factor by which the internally calculated PYTHIA width has to be rescaled to give the user-enforced width;
          • resWidthChan(...) to return the width for one particular channel (currently only used for Higgs decays, to obtain instate coupling from outstate width).
          These methods actually provide an interface to the classes derived from the ResonanceWidths base class, to describe various resonances.

          Modes for Matrix Element Processing

          The meMode() value for a decay mode is used to specify ";?>nonisotropic decays or the conversion of a parton list into a set of hadrons in some channels of normal particles. For resonances it can also take a third function, namely to describe how the branching ratios and widths of a resonance should be rescaled as a function of the current mass of the decaying resonance. The rules are especially useful when new channels are added to an existing particle, or a completely new resonance added.
          • 0 : channels for which hardcoded partial-width expressions are expected to exist in the derived class of the respective resonance. Should no such code exist then the partial width defaults to zero.
          • 1 - 99 : same as 0, but normally not used for resonances.
          • 100 : calculate the partial width of the channel from its stored branching ratio times the stored total width. This value remains unchanged when the resonance fluctuates in mass. Specifically there are no threshold corrections. That is, if the resonance fluctuates down in mass, to below the nominal threshold, it is assumed that one of the daughters could also fluctuate down to keep the channel open. (If not, there may be problems later on.)
          • 101 : calculate the partial width of the channel from its stored branching ratio times the stored total width. Multiply by a step threshold, i.e. the channel is switched off when the sum of the daughter on-shell masses is above the current mother mass.
          • 102 : calculate the partial width of the channel from its stored branching ratio times the stored total width. Multiply by a smooth threshold factor beta = sqrt( (1 - m_1^2/m_2 - m_2^2/m^2)^2 - 4 m_1^2 m_2^2/m^4) for two-body decays and sqrt(1 - Sum_i m_i / m) for multibody ones. The former correctly encodes the size of the phase space but misses out on any nontrivial matrix-element behaviour, while the latter obviously is a very crude simplification of the correct phase-space expression. Specifically, it is thereby assumed that the stored branching ratio and total width did not take into account such a factor.
          • 103 : use the same kind of behaviour and threshold factor as for 102 above, but assume that such a threshold factor has been used when the default branching ratio and total width were calculated, so that one should additionally divide by the on-shell threshold factor. Specifically, this will give back the stored branching ratios for on-shell mass, unlike the 102 option. To avoid division by zero, or in general unreasonably big rescaling factors, a lower limit minThreshold (see below) on the value of the on-shell threshold factor is imposed. (In cases where a big rescaling is intentional, code 102 would be more appropriate.)


          ResonanceWidths:minThreshold   (default = 0.1; minimum = 0.01)
          Used uniquely for meMode = 103 to set the minimal value assumed for the threshold factor, sqrt( (1 - m_1^2/m_2 - m_2^2/m^2)^2 - 4 m_1^2 m_2^2/m^4) for two-body decays and sqrt(1 - Sum_i m_i / m) for multibody ones. Thus the inverse of this number sets an upper limit for how much the partial width of a channel can increase from the on-shell value to the value for asymptotically large resonance masses. Is mainly intended as a safety measure, to avoid unintentionally large rescalings.

          All of these meMode's may coexist for the same resonance. This would be the case e.g. if you want to add a few new channels to an already existing resonance, where the old partial widths come hardcoded while the new ones are read in from an external file. The typical example would be an MSSM Higgs sector, where partial widths to SM particles are already encoded, meMode = 0, while decay rates to sparticles are read in from some external calculation and maybe would be best approximated by using meMode = 103. Indeed the default particle table in PYTHIA uses 103 for all channels that are expected to be provided by external input.

          Some further clarification may be useful. At initialization the existing total width and on-shell branching ratios will be updated. For channels with meMode < 100 the originally stored branching ratios are irrelevant, since the existing code will anyway be used to calculate the partial widths from scratch. For channels with meMode = 100 or bigger, instead the stored branching ratio is used together with the originally stored total width to define the correct on-shell partial width. The sum of partial widths then gives the new total width, and from there new branching ratios are defined.

          In these operations the original sum of branching ratios need not be normalized to unity. For instance, you may at input have a stored total width of 1 GeV and a sum of branching ratios of 2. After initialization the width will then have been changed to 2 GeV and the sum of branching ratios rescaled to unity. This might happen e.g. if you add a few channels to an existing resonance, without changing the branching ratios of the existing channels or the total width of the resonance.

          In order to simulate the Breit-Wigner shape correctly, it is important that all channels that contribute to the total width are included in the above operations. This must be kept separate from the issue of which channels you want to have switched on for a particular study, to be considered next.

          In the event-generation process, when an off-shell resonance mass has been selected, the width and branching ratios are re-evaluated for this new mass. At this stage also the effects of restrictions on allowed decay modes are taken into account, as set by the onMode switch for each separate decay channel. Thus a channel may be on or off, with different choices of open channels between the particle and its antiparticle. In addition, even when a channel is on, the decay may be into another resonance with its selection of allowed channels. It is these kinds of restrictions that lead to the Gamma_out possibly being smaller than Gamma_tot. As a reminder, the Breit-Wigner for decays behaves like Gamma_out / ((s - m^2)^2 + s * Gamma_tot^2), where the width in the numerator is only to those channels being studied, but the one in the denominator to all channels of the particle. These ever-changing numbers are not directly visible to the user, but are only stored in a work area. "?>

          pythia8-8.1.80.orig/phpdoc/StandardModelParameters.php0000644000175000017500000004656112217615312021100 0ustar sunsun Standard-Model Parameters SETTINGS SAVED TO FILE

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          Standard-Model Parameters

          The strong coupling

          The AlphaStrong class is used to provide a first- or second-order running alpha_strong (or, trivially, a zeroth-order fixed one). Formulae are the standard ones found in [Yao06]. The second-order expression used, eq. (9.5), may be somewhat different in other approaches (with differences formally of higher order), so do not necessarily expect perfect agreement, especially not at small Q^2 scales. The starting alpha_strong value is defined at the M_Z mass scale. The Lambda values are matched at the c, b and t flavour thresholds, such that alpha_strong is continuous. For second-order matching an approximate iterative method is used.

          For backwards compatibility, the following global switch determines whether 5- or 6-flavour running will be used above the t threshold:

          StandardModel:alphaSnfmax   (default = 6; minimum = 5; maximum = 6)

          5 : Use 5-flavour running for all scales above the b flavour threshold (old default).
          6 : Use 6-flavour running above the t threshold (new default).

          Since we allow alpha_strong to vary separately for hard processes, timelike showers, spacelike showers and multiparton interactions, all other relevant values are set in each of these classes. The default behaviour is everywhere first-order running.

          The alpha_strong calculation is initialized by init( value, order, nfmax), where value is the alpha_strong value at M_Z, order is the order of the running, 0, 1 or 2, and nfmax is the highest number of flavours to include in the running. Thereafter the value can be calculated by alphaS(scale2), where scale2 is the Q^2 scale in GeV^2.

          For applications inside shower programs, a second-order alpha_s value can be obtained as the product of the two functions alphaS1Ord(scale2) and alphaS2OrdCorr(scale2), where the first gives a simple first-order running (but with the second-order Lambda) and the second the correction factor, below unity, for the second-order terms. This allows a compact handling of evolution equations.

          Resummation arguments [Cat91] show that a set of universal QCD corrections can be absorbed in coherent parton showers by applying the so-called CMW rescaling of the MSbar value of Lambda_QCD. This can be accomplished via a fourth (optional) boolean argument to init( value, order, nfmax, useCMW), with default value useCMW = false. When set to true, the translation amounts to an N_F-dependent rescaling of Lambda_QCD, relative to its MSbar value, by a factor 1.661 for NF=3, 1.618 for NF=4, 1.569 for NF=5, and 1.513 for NF=6. When using this option, be aware that the original CMW arguments were derived using two-loop running and that the CMW rescaling may need be taken into account in the context of matrix-element matching. Note also that this option has only been made available for timelike and spacelike showers, not for hard processes.

          The electromagnetic coupling

          The AlphaEM class is used to generate a running alpha_em. The input StandardModel:alphaEMmZ value at the M_Z mass is matched to a low-energy behaviour with running starting at the electron mass threshold. The matching is done by fitting an effective running coefficient in the region between the light-quark threshold and the charm/tau threshold. This procedure is approximate, but good enough for our purposes.

          Since we allow alpha_em to vary separately for hard processes, timelike showers, spacelike showers and multiparton interactions, the choice between using a fixed or a running alpha_em can be made in each of these classes. The default behaviour is everywhere first-order running. The actual values assumed at zero momentum transfer and at M_Z are only set here, however.

          StandardModel:alphaEM0   (default = 0.00729735; minimum = 0.0072973; maximum = 0.0072974)
          The alpha_em value at vanishing momentum transfer (and also below m_e).

          StandardModel:alphaEMmZ   (default = 0.00781751; minimum = 0.00780; maximum = 0.00783)
          The alpha_em value at the M_Z mass scale. Default is taken from [Yao06].

          The alpha_em calculation is initialized by init(order), where order is the order of the running, 0 or 1, with -1 a special option to use the fix value provided at M_Z. Thereafter the value can be calculated by alphaEM(scale2), where scale2 is the Q^2 scale in GeV^2.

          The electroweak couplings

          There are two degrees of freedom that can be set, related to the electroweak mixing angle:

          StandardModel:sin2thetaW   (default = 0.2312; minimum = 0.225; maximum = 0.240)
          The sine-squared of the weak mixing angle, as used in all Z^0 and W^+- masses and couplings, except for the vector couplings of fermions to the Z^0, see below. Default is the MSbar value from [Yao06].

          StandardModel:sin2thetaWbar   (default = 0.2315; minimum = 0.225; maximum = 0.240)
          The sine-squared of the weak mixing angle, as used to derive the vector couplings of fermions to the Z^0, in the relation v_f = a_f - 4 e_f sin^2(theta_W)bar. Default is the effective-angle value from [Yao06].

          The Fermi constant is not much used in the currently coded matrix elements, since it is redundant, but it is available:

          StandardModel:GF   (default = 1.16637e-5; minimum = 1.0e-5; maximum = 1.3e-5)
          The Fermi coupling constant, in units of GeV^-2.

          The quark weak-mixing matrix

          The absolute values of the Cabibbo-Kobayashi-Maskawa matrix elements are set by the following nine real values taken from [Yao06] - currently the CP-violating phase is not taken into account in this parametrization. It is up to the user to pick a consistent unitary set of new values whenever changes are made.

          StandardModel:Vud   (default = 0.97383; minimum = 0.973; maximum = 0.975)
          The V_ud CKM matrix element.

          StandardModel:Vus   (default = 0.2272; minimum = 0.224; maximum = 0.230)
          The V_us CKM matrix element.

          StandardModel:Vub   (default = 0.00396; minimum = 0.0037; maximum = 0.0042)
          The V_ub CKM matrix element.

          StandardModel:Vcd   (default = 0.2271; minimum = 0.224; maximum = 0.230)
          The V_cd CKM matrix element.

          StandardModel:Vcs   (default = 0.97296; minimum = 0.972; maximum = 0.974)
          The V_cs CKM matrix element.

          StandardModel:Vcb   (default = 0.04221; minimum = 0.0418; maximum = 0.0426)
          The V_cb CKM matrix element.

          StandardModel:Vtd   (default = 0.00814; minimum = 0.006; maximum = 0.010)
          The V_td CKM matrix element.

          StandardModel:Vts   (default = 0.04161; minimum = 0.039; maximum = 0.043)
          The V_ts CKM matrix element.

          StandardModel:Vtb   (default = 0.9991; minimum = 0.99907; maximum = 0.9992)
          The V_tb CKM matrix element.

          The CoupSM class

          The ";?>Pythia class contains a public instance coupSM of the CoupSM class. This class contains one instance each of the AlphaStrong and AlphaEM classes, and additionally stores the weak couplings and the quark mixing matrix mentioned above. This class is used especially in the calculation of cross sections and resonance widths, but could also be used elsewhere. Specifically, as already mentioned, there are separate AlphaStrong and AlphaEM instances for timelike and spacelike showers and for multiparton interactions, while weak couplings and the quark mixing matrix are only stored here. With the exception of the first two methods below, which are for internal use, the subsequent ones could also be used externally.

          CoupSM::CoupSM()  
          the constructor does nothing. Internal.

          void CoupSM::init(Settings& settings, Rndm* rndmPtr)  
          this is where the AlphaStrong and AlphaEM instances are initialized, and weak couplings and the quark mixing matrix are read in and set. This is based on the values stored on this page and among the ";?>Couplings and Scales. Internal.

          double CoupSM::alphaS(double scale2)  
          the alpha_strong value at the quadratic scale scale2.

          double CoupSM::alphaS1Ord(double scale2)  
          a first-order overestimate of the full second-order alpha_strong value at the quadratic scale scale2.

          double CoupSM::alphaS2OrdCorr(double scale2)  
          a multiplicative correction factor, below unity, that brings the first-order overestimate above into agreement with the full second-order alpha_strong value at the quadratic scale scale2.

          double CoupSM::Lambda3()  
          double CoupSM::Lambda4()  
          double CoupSM::Lambda5()  
          the three-, four-, and five-flavour Lambda scale.

          double CoupSM::alphaEM(double scale2)  
          the alpha_em value at the quadratic scale scale2.

          double CoupSM::sin2thetaW()  
          double CoupSM::cos2thetaW()  
          the sine-squared and cosine-squared of the weak mixing angle, as used in the gauge-boson sector.

          double CoupSM::sin2thetaWbar()  
          the sine-squared of the weak mixing angle, as used to derive the vector couplings of fermions to the Z^0.

          double CoupSM::GF()  
          the Fermi constant of weak decays, in GeV^-2.

          double CoupSM::ef(int idAbs)  
          the electrical charge of a fermion, by the absolute sign of the PDF code, i.e. idAbs must be in the range between 1 and 18.

          double CoupSM::vf(int idAbs)  
          double CoupSM::af(int idAbs)  
          the vector and axial charges of a fermion, by the absolute sign of the PDF code (a_f = +-1, v_f = a_f - 4. * sin2thetaWbar * e_f).

          double CoupSM::t3f(int idAbs)  
          double CoupSM::lf(int idAbs)  
          double CoupSM::rf(int idAbs)  
          the weak isospin, left- and righthanded charges of a fermion, by the absolute sign of the PDF code (t^3_f = a_f/2, l_f = (v_f + a_f)/2, r_f = (v_f - a_f)/2; you may find other conventions in the literature that differ by a factor of 2).

          double CoupSM::ef2(int idAbs)  
          double CoupSM::vf2(int idAbs)  
          double CoupSM::af2(int idAbs)  
          double CoupSM::efvf(int idAbs)  
          double CoupSM::vf2af2(int idAbs)  
          common quadratic combinations of the above couplings: e_f^2, v_f^2, a_f^2, e_f * v_f, v_f^2 + a_f^2.

          double CoupSM::VCKMgen(int genU, int genD)  
          double CoupSM::V2CKMgen(int genU, int genD)  
          the CKM mixing element,or the square of it, for up-type generation index genU (1 = u, 2 = c, 3 = t, 4 = t') and down-type generation index genD (1 = d, 2 = s, 3 = b, 4 = b').

          double CoupSM::VCKMid(int id1, int id2)  
          double CoupSM::V2CKMid(int id1, int id2)  
          the CKM mixing element,or the square of it, for flavours id1 and id2, both in the range from -18 to +18. The sign is here not checked (so it can be used both for u + dbar -> W+ and u -> d + W+, say), but impossible flavour combinations evaluate to zero. The neutrino sector is numbered by flavor eigenstates, so there is no mixing in the lepton-neutrino system.

          double CoupSM::V2CKMsum(int id)  
          the sum of squared CKM mixing element that a given flavour can couple to, excluding the top quark and fourth generation. Is close to unity for the first two generations. Returns unity for the lepton-neutrino sector.

          int CoupSM::V2CKMpick(int id)  
          picks a random CKM partner quark or lepton (with the same sign as id) according to the respective squared elements, again excluding the top quark and fourth generation from the list of possibilities. Unambiguous choice for the lepton-neutrino sector. "?>

          pythia8-8.1.80.orig/phpdoc/ExtraDimensionalProcesses.php0000644000175000017500000014127312217615312021464 0ustar sunsun Extra-Dimensional Processes SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Extra-Dimensional Processes

          Scenarios with extra dimensions (ED) allow a multitude of processes. Currently three different categories of processes are implemented. The first involves the production of excited Kaluza Klein states within so-called Randall-Sundrum (RS) scenarios, the second is related to resonance production in TeV-1 sized extra dimensions and the third relates to phenomena from large extra dimensions (LED). Due to the close relation between the LED model and a so-called unparticle model, similar unparticle processes are also kept in this section.

          Randall-Sundrum Resonances, production processes

          The graviton (G*) and gluon (KKgluon*) resonance states are assigned PDG code 5100039 and 5100021 respectively. The G* processes are described in [Bij01] and the KKgluon* process in [Ask11]. Decays into fermion and boson pairs are handled with the correct angular distributions, while subsequent decays are handled isotropically.

          There are two lowest-order processes that together normally should be sufficient for a simulation of G^* production.

          ExtraDimensionsG*:all On Off   (default = off)
          Common switch for the group of lowest-order G^* production processes, i.e. the two ones below.

          ExtraDimensionsG*:gg2G* On Off   (default = off)
          Scatterings g g -> G^*. Code 5001.

          ExtraDimensionsG*:ffbar2G* On Off   (default = off)
          Scatterings f fbar -> G^*. Code 5002.

          In addition there are three first-order processes included. These are of less interest, but can be used for dedicated studies of the high-pT tail of G^* production. As usual, it would be double counting to include the lowest-order and first-order processes simultaneously. Therefore the latter ones are not included with the ExtraDimensionsG*:all = on option. In this set of processes all decay angles are assumed isotropic.

          ExtraDimensionsG*:gg2G*g On Off   (default = off)
          Scatterings g g -> G^* g. Code 5003.

          ExtraDimensionsG*:qg2G*q On Off   (default = off)
          Scatterings q g -> G^* q. Code 5004.

          ExtraDimensionsG*:qqbar2G*g On Off   (default = off)
          Scatterings q qbar -> G^* g. Code 5005.

          There is also one process for the production of a gluon resonance.

          ExtraDimensionsG*:qqbar2KKgluon* On Off   (default = off)
          Scatterings q qbar -> g^*/KKgluon^*. Code 5006.

          Randall-Sundrum Resonances, parameters

          In the above scenario the main free parameters are the masses, which are set as usual. In addition there are the following coupling parameters. The coupling kappaMG follows the conventions in [Bij01], where as the flavour dependent couplings follow the conventions used in [Dav01].

          ExtraDimensionsG*:SMinBulk On Off   (default = off)
          Parameter to choose between the two scenarios: off, SM on the TeV brane (common kappaMG coupling); on, SM in the ED bulk (flavour dependent couplings). This parameter is only relevant for the lowest-order graviton (G*) processes, where as the first-order processes corresponds to the off scenario.

          ExtraDimensionsG*:VLVL On Off   (default = on)
          Parameter to specify Z/W coupling scenario: off, usual Z/W boson couplings; on, coupling only to longitudinal Z/W bosons. In both cases the GZZ and GWW values are used and this parameter is only relevant when SMinBulk = on. The formulas for longitudinal bosons should be appropriate up to O(m_V/E_V) corrections.

          ExtraDimensionsG*:kappaMG   (default = 0.054; minimum = 0.0)
          dimensionless coupling, which enters quadratically in all partial widths of the G^*. Is kappa m_G* = sqrt(2) x_1 k / Mbar_Pl, where x_1 = 3.83 is the first zero of the J_1 Bessel function and Mbar_Pl is the modified Planck mass.

          ExtraDimensionsG*:Gll   (default = 0.0; minimum = 0.0)
          Coupling between graviton and leptons.

          ExtraDimensionsG*:Gqq   (default = 0.0; minimum = 0.0)
          Coupling between graviton and light quarks.

          ExtraDimensionsG*:Gbb   (default = 0.0; minimum = 0.0)
          Coupling between graviton and bottom quark.

          ExtraDimensionsG*:Gtt   (default = 0.001; minimum = 0.0)
          Coupling between graviton and top quark.

          ExtraDimensionsG*:Ggg   (default = 0.000013; minimum = 0.0)
          Coupling between graviton and gluon.

          ExtraDimensionsG*:Ggmgm   (default = 0.000013; minimum = 0.0)
          Coupling between graviton and gamma.

          ExtraDimensionsG*:GZZ   (default = 0.001; minimum = 0.0)
          Coupling between graviton and Z boson.

          ExtraDimensionsG*:GWW   (default = 0.001; minimum = 0.0)
          Coupling between graviton and W boson.

          ExtraDimensionsG*:Ghh   (default = 0.001; minimum = 0.0)
          Coupling between graviton and Higgs bosons.

          ExtraDimensionsG*:KKgqR   (default = -0.2)
          Coupling between KK-gluon and a right-handed light quark.

          ExtraDimensionsG*:KKgqL   (default = -0.2)
          Coupling between KK-gluon and a left-handed light quark.

          ExtraDimensionsG*:KKgbR   (default = -0.2)
          Coupling between KK-gluon and a right-handed bottom quark.

          ExtraDimensionsG*:KKgbL   (default = 1.0)
          Coupling between KK-gluon and a left-handed bottom quark.

          ExtraDimensionsG*:KKgtR   (default = 4.0)
          Coupling between KK-gluon and a right-handed top quark.

          ExtraDimensionsG*:KKgtL   (default = 1.0)
          Coupling between KK-gluon and a left-handed top quark.

          ExtraDimensionsG*:KKintMode   (default = 0; minimum = 0; maximum = 2)
          Choice of full g^*/KK-gluon^* structure or not in relevant processes.
          0 : full g^*/KK-gluon^* structure, with interference included.
          1 : only pure gluon_{SM} contribution.
          2 : only pure gluon_{KK} contribution.

          TeV^-1 Sized Extra Dimension, production processes

          This section contains a processes involving the production of electroweak KK gauge bosons, i.e. gamma_{KK}/Z_{KK}, in one TeV^-1 sized extra dimension. The process is described in [Bel10] and allows for individual final states to be specified.

          ExtraDimensionsTEV:ffbar2ddbar On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> d dbar , Code 5061.

          ExtraDimensionsTEV:ffbar2uubar On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> u ubar , Code 5062.

          ExtraDimensionsTEV:ffbar2ssbar On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> s sbar , Code 5063.

          ExtraDimensionsTEV:ffbar2ccbar On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> c cbar , Code 5064.

          ExtraDimensionsTEV:ffbar2bbbar On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> b bbar , Code 5065.

          ExtraDimensionsTEV:ffbar2ttbar On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> t tbar , Code 5066.

          ExtraDimensionsTEV:ffbar2e+e- On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> e+ e- , Code 5071.

          ExtraDimensionsTEV:ffbar2nuenuebar On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> nue nuebar , Code 5072.

          ExtraDimensionsTEV:ffbar2mu+mu- On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> mu+ mu- , Code 5073.

          ExtraDimensionsTEV:ffbar2numunumubar On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> numu numubar , Code 5074.

          ExtraDimensionsTEV:ffbar2tau+tau- On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> tau+ tau- , Code 5075.

          ExtraDimensionsTEV:ffbar2nutaunutaubar On Off   (default = off)
          Scatterings f fbar -> (gamma_{KK}/Z_{KK}) -> nutau nutaubar , Code 5076.

          TeV^-1 Sized Extra Dimension, parameters

          Irrespective of the parameter options used, the particle produced, gamma_{KK}/Z_{KK}, will always be assigned code 5000023.

          ExtraDimensionsTEV:gmZmode   (default = 3; minimum = 0; maximum = 5)
          Choice of full gamma_{KK}/Z_{KK} structure or not in relevant processes.
          0 : full gamma_{SM}/Z_{SM} structure, with interference included.
          1 : only pure gamma_{SM} contribution.
          2 : only pure Z_{SM} contribution.
          3 : full gamma_{KK}/Z_{KK} structure, with interference included.
          4 : only pure gamma_{KK} contribution, with SM interference included.
          5 : only pure Z_{KK} contribution, with SM interference included.


          ExtraDimensionsTEV:nMax   (default = 10; minimum = 1; maximum = 100)
          The number of included KK excitations.

          ExtraDimensionsTEV:mStar   (default = 4000.0; minimum = 1000.0)
          The KK mass m^*, given by the inverse of the single extra dimension radius.

          Large Extra Dimensions, production processes

          The LED graviton, where the KK-modes normally are summed and do not give rise to phenomena individually, is assigned PDG code 5000039. The graviton emission and virtual graviton exchange processes use the same implementation as the corresponding unparticle processes, which are all described in [Ask10]. It is also possible to generate monojet events from scalar graviton emission as described in [Azu05], by turning on the option GravScalar.

          Note: As discussed in [Ask09], for the graviton or unparticle emission processes the underlying Breit-Wigner mass distribution should be matched to the graviton mass spectrum in order to achieve an optimal MC efficiency.

          The following lowest order graviton emission processes are available.

          ExtraDimensionsLED:monojet On Off   (default = off)
          Common switch for the group of lowest-order G jet emission processes, i.e. the three ones below.

          ExtraDimensionsLED:gg2Gg On Off   (default = off)
          Scatterings g g -> G g. Code 5021.

          ExtraDimensionsLED:qg2Gq On Off   (default = off)
          Scatterings q g -> G q. Code 5022.

          ExtraDimensionsLED:qqbar2Gg On Off   (default = off)
          Scatterings q qbar -> G g. Code 5023.

          ExtraDimensionsLED:ffbar2GZ On Off   (default = off)
          Scatterings f fbar -> G Z. Code 5024.

          ExtraDimensionsLED:ffbar2Ggamma On Off   (default = off)
          Scatterings f fbar -> G gamma. This process corresponds to the photon limit of the G Z process, as described in [Ask09]. Code 5025.

          The following LED processes with virtual graviton exchange are available.

          ExtraDimensionsLED:ffbar2gammagamma On Off   (default = off)
          Scatterings f fbar -> (LED G*) -> gamma gamma. If the graviton contribution is zero, the results corresponds to the SM contribution, i.e. equivalent to PromptPhoton:ffbar2gammagamma. Code 5026.

          ExtraDimensionsLED:gg2gammagamma On Off   (default = off)
          Scatterings g g -> (LED G*) -> gamma gamma. Code 5027.

          ExtraDimensionsLED:ffbar2llbar On Off   (default = off)
          Scatterings f fbar -> (LED G*) -> l l , where l is a charged lepton. If the graviton contribution is zero, the results corresponds to the SM contribution, i.e. similar to WeakSingleBoson:ffbar2gmZ. Does not include t-channel amplitude relevant for e^+e^- to e^+e^- and no K-factor is used. Code 5028.

          ExtraDimensionsLED:gg2llbar On Off   (default = off)
          Scatterings g g -> (LED G*) -> l l. Code 5029.

          Dijet production including graviton exchange is also available, using the same effective theory approach as the LED G exchange processes above or including more detailed amplitudes in accordance with [Fra11]. In case of the latter, the value of LambdaT is used as the value of the cut-off scale Lambda. For this reason the dijet processes only relates to the LED model and no unparticle versions are available. The processes are grouped together like their HardQCD equivalents and should therefore converge to the same results in the limit of an insignificant graviton contribution.

          Warning: These LED dijets processes are still being validated.

          ExtraDimensionsLED:dijets On Off   (default = off)
          Common switch for the group of lowest-order jet jet production processes with graviton exchange, i.e. the six ones below.

          ExtraDimensionsLED:gg2DJgg On Off   (default = off)
          Scatterings g g -> (LED G*) -> g g. Code 5030.

          ExtraDimensionsLED:gg2DJqqbar On Off   (default = off)
          Scatterings g g -> (LED G*) -> q qbar. Number of outgoing flavours specified by nQuarkNew parameter below. Code 5031.

          ExtraDimensionsLED:qg2DJqg On Off   (default = off)
          Scatterings q g -> (LED G*) -> q g and qbar g -> (LED G*) -> qbar g. Code 5032.

          ExtraDimensionsLED:qq2DJqq On Off   (default = off)
          Scatterings q q(bar)' -> (LED G*) -> q q(bar)'. Including q and qbar of same or different flavours, but the outgoing flavours equals the incoming ones. Code 5033.

          ExtraDimensionsLED:qqbar2DJgg On Off   (default = off)
          Scatterings q qbar -> (LED G*) -> g g. Code 5034.

          ExtraDimensionsLED:qqbar2DJqqbarNew On Off   (default = off)
          Scatterings q qbar -> (LED G*) -> q' qbar'. Number of outgoing flavours specified by nQuarkNew parameter below. Code 5035.

          Large Extra Dimensions, parameters



          ExtraDimensionsLED:GravScalar On Off   (default = off)
          Allow the monojet processes to produce scalar graviton emission instead of the default tensor one. The scalar option is according to the processes described in [Azu05] and includes two coupling constants below.

          ExtraDimensionsLED:n   (default = 2; minimum = 1)
          Number of extra dimensions.

          ExtraDimensionsLED:MD   (default = 2000.; minimum = 100.0)
          Fundamental scale of gravity in D = 4 + n dimensions.

          ExtraDimensionsLED:LambdaT   (default = 2000.; minimum = 100.0)
          Ultraviolet cutoff parameter for the virtual graviton exchange processes.

          ExtraDimensionsLED:NegInt   (default = 0; minimum = 0; maximum = 1)
          Allows to change sign of the interference terms in the graviton exchange processes, common in connection to using the Hewett convention Hew99.
          0 : 1
          1 : -1


          ExtraDimensionsLED:CutOffMode   (default = 0; minimum = 0; maximum = 3)
          Options for when the hard scale of the process (e.g. sHat) approaches or exceed the scale of validity of the low energy effective theory (e.g. M_D). Note: Option 1 only concerns the graviton emission processes and the form factor is currently not available for the scalar graviton processes.
          0 : Do nothing, i.e. all values of sHat contribute.
          1 : Truncate contributing sHat region (Ask09).
          2 : Form factor, using mu = renormScale2 .
          3 : Form factor, using mu = E_jet.


          ExtraDimensionsLED:t   (default = 1.; minimum = 0.001)
          Form factor parameter.

          ExtraDimensionsLED:g   (default = 1.0; minimum = 0.0)
          Coupling related to scalar graviton emission.

          ExtraDimensionsLED:c   (default = 1.0; minimum = 0.0)
          Coupling related to scalar graviton emission.

          ExtraDimensionsLED:nQuarkNew   (default = 3; minimum = 0; maximum = 5)
          Number of allowed outgoing new quark flavours in the above q qbar -> (LED G*) -> q' qbar' and g g -> (LED G*) -> q' qbar' processes. Similar to HardQCD:nQuarkNew for the QCD processes.

          ExtraDimensionsLED:opMode   (default = 0; minimum = 0; maximum = 1)
          Options to specify S function for LED dijet amplitudes.
          option 0 : Use detailed amplitude, as described in [Fra11].
          option 1 : Use conventional LambdaT parametrization, like the other LED processes.

          Unparticles, production processes

          As mentioned above, the similar unparticle and graviton processes share the same implementations. The unparticle processes, however, only use the dedicated unparticle parameters below. The unparticle is also assigned the PDG code 5000039 and is therefore called Graviton in the event record. The graviton and unparticle emission as well as virtual graviton and unparticle exchange processes are described in [Ask10].

          Note: As discussed in [Ask09], for the graviton or unparticle emission processes the underlying Breit-Wigner mass distribution should be matched to the graviton mass spectrum in order to achieve an optimal MC efficiency.

          The following unparticle emission processes are available.

          ExtraDimensionsUnpart:monojet On Off   (default = off)
          Common switch for the group of lowest-order U jet emission processes, i.e. the three ones below.

          ExtraDimensionsUnpart:gg2Ug On Off   (default = off)
          Scatterings g g -> U g. Code 5045.

          ExtraDimensionsUnpart:qg2Uq On Off   (default = off)
          Scatterings q g -> U q. Code 5046.

          ExtraDimensionsUnpart:qqbar2Ug On Off   (default = off)
          Scatterings q qbar -> U g. Code 5047.

          ExtraDimensionsUnpart:ffbar2UZ On Off   (default = off)
          Scatterings f fbar -> U Z. Code 5041.

          ExtraDimensionsUnpart:ffbar2Ugamma On Off   (default = off)
          Scatterings f fbar -> U gamma. This process corresponds to the photon limit of the U Z process, as described in [Ask09]. Code 5042.

          The following processes with virtual unparticle exchange are available.

          ExtraDimensionsUnpart:ffbar2gammagamma On Off   (default = off)
          Scatterings f fbar -> (U*) -> gamma gamma. If the unparticle contribution is zero in the spin-2 case, the results corresponds to the SM contribution, i.e. equivalent to PromptPhoton:ffbar2gammagamma. Code 5043.

          ExtraDimensionsUnpart:gg2gammagamma On Off   (default = off)
          Scatterings g g -> (U*) -> gamma gamma. Code 5044.

          ExtraDimensionsUnpart:ffbar2llbar On Off   (default = off)
          Scatterings f fbar -> (U*) -> l lbar , where l is a charged lepton. If the unparticle contribution is zero, the results corresponds to the SM contribution, i.e. similar to WeakSingleBoson:ffbar2gmZ. Does not include t-channel amplitude relevant for e^+e^- to e^+e^- and no K-factor is used. Code 5048.

          ExtraDimensionsUnpart:gg2llbar On Off   (default = off)
          Scatterings g g -> (U*) -> l lbar. Code 5049.

          Unparticles, parameters



          ExtraDimensionsUnpart:spinU   (default = 2; minimum = 0; maximum = 2)
          Unparticle spin.

          ExtraDimensionsUnpart:dU   (default = 1.4; minimum = 1.0)
          Scale dimension parameter.

          ExtraDimensionsUnpart:LambdaU   (default = 2000.; minimum = 100.0)
          Unparticle renormalization scale.

          ExtraDimensionsUnpart:lambda   (default = 1.0; minimum = 0.0)
          Unparticle coupling to the SM fields.

          ExtraDimensionsUnpart:ratio   (default = 1.0; minimum = 1.0; maximum = 1.0)
          Ratio, lambda'/lambda, between the two possible coupling constants of the spin-2 ME. Warning: A ratio value different from one give rise to an IR divergence which makes the event generation very slow, so this values is fixed to ratio = 1 for the moment.

          ExtraDimensionsUnpart:CutOffMode   (default = 0; minimum = 0; maximum = 1)
          Options for when the hard scale of the process (e.g. sHat) approaches or exceed the scale of validity of the low energy effective theory (Lambda_U). This mode only concerns the unparticle emission processes.
          0 : Do nothing, i.e. all values of sHat contribute.
          1 : Truncate contributing sHat region (Ask09).


          ExtraDimensionsUnpart:gXX   (default = 0; minimum = 0; maximum = 2)
          Chiral unparticle couplings, gXX = gLL = gRR. Only relevant for lepton production from spin-1 unparticle exchange.
          0 : 1
          1 : -1
          2 : 0


          ExtraDimensionsUnpart:gXY   (default = 0; minimum = 0; maximum = 2)
          Chiral unparticle couplings, gXY = gLR = gRL. Only relevant for lepton production from spin-1 unparticle exchange.
          0 : 1
          1 : -1
          2 : 0
          "?>
          pythia8-8.1.80.orig/phpdoc/Diffraction.php0000644000175000017500000007012612217615312016555 0ustar sunsun Diffraction SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Diffraction

          Introduction

          Diffraction is not well understood, and several alternative approaches have been proposed. Here we follow a fairly conventional Pomeron-based one, in the Ingelman-Schlein spirit [Ing85], but integrated to make full use of the standard PYTHIA machinery for multiparton interactions, parton showers and hadronization [Nav10,Cor10a]. This is the approach pioneered in the PomPyt program by Ingelman and collaborators [Ing97].

          For ease of use (and of modelling), the Pomeron-specific parts of the generation are subdivided into three sets of parameters that are rather independent of each other:
          (i) the total, elastic and diffractive cross sections are parametrized as functions of the CM energy, or can be set by the user to the desired values, see the ";?>Total Cross Sections page;
          (ii) once it has been decided to have a diffractive process, a Pomeron flux parametrization is used to pick the mass of the diffractive system(s) and the t of the exchanged Pomeron, see below;
          (iii) a diffractive system of a given mass is classified either as low-mass unresolved, which gives a simple low-pT string topology, or as high-mass resolved, for which the full machinery of multiparton interactions and parton showers are applied, making use of ";?>Pomeron PDFs.
          The parameters related to multiparton interactions, parton showers and hadronization are kept the same as for normal nondiffractive events, with only one exception. This may be questioned, especially for the multiparton interactions, but we do not believe that there are currently enough good diffractive data that would allow detailed separate tunes.

          The above subdivision may not represent the way "physics comes about". For instance, the total diffractive cross section can be viewed as a convolution of a Pomeron flux with a Pomeron-proton total cross section. Since neither of the two is known from first principles there will be a significant amount of ambiguity in the flux factor. The picture is further complicated by the fact that the possibility of simultaneous further multiparton interactions ("cut Pomerons") will screen the rate of diffractive systems. In the end, our set of parameters refers to the effective description that emerges out of these effects, rather than to the underlying "bare" parameters.

          In the event record the diffractive system in the case of an excited proton is denoted p_diffr, code 9902210, whereas a central diffractive system is denoted rho_diffr, code 9900110. Apart from representing the correct charge and baryon numbers, no deeper meaning should be attributed to the names.

          Pomeron flux

          As already mentioned above, the total diffractive cross section is fixed by a default energy-dependent parametrization or by the user, see the ";?>Total Cross Sections page. Therefore we do not attribute any significance to the absolute normalization of the Pomeron flux. The choice of Pomeron flux model still will decide on the mass spectrum of diffractive states and the t spectrum of the Pomeron exchange.

          Diffraction:PomFlux   (default = 1; minimum = 1; maximum = 5)
          Parametrization of the Pomeron flux f_Pom/p( x_Pom, t).
          1 : Schuler and Sjöstrand Sch94: based on a critical Pomeron, giving a mass spectrum roughly like dm^2/m^2; a mass-dependent exponential t slope that reduces the rate of low-mass states; partly compensated by a very-low-mass (resonance region) enhancement. Is currently the only one that contains a separate t spectrum for double diffraction (along with MBR) and separate parameters for pion beams.
          2 : Bruni and Ingelman Bru93: also a critical Pomeron giving close to dm^2/m^2, with a t distribution the sum of two exponentials. The original model only covers single diffraction, but is here expanded by analogy to double and central diffraction.
          3 : a conventional Pomeron description, in the RapGap manual Jun95 attributed to Berger et al. and Streng Ber87a, but there (and here) with values updated to a supercritical Pomeron with epsilon > 0 (see below), which gives a stronger peaking towards low-mass diffractive states, and with a mass-dependent (the alpha' below) exponential t slope. The original model only covers single diffraction, but is here expanded by analogy to double and central diffraction.
          4 : a conventional Pomeron description, attributed to Donnachie and Landshoff Don84, again with supercritical Pomeron, with the same two parameters as option 3 above, but this time with a power-law t distribution. The original model only covers single diffraction, but is here expanded by analogy to double and central diffraction.
          5 : the MBR (Minimum Bias Rockefeller) simulation of (anti)proton-proton interactions Cie12. The event generation follows a renormalized-Regge-theory model, successfully tested using CDF data. The simulation includes single and double diffraction, as well as the central diffractive (double-Pomeron exchange) process (106). Only p p, pbar p and p pbar beam combinations are allowed for this option. Several parameters of this model are listed below.

          In options 3 and 4 above, the Pomeron Regge trajectory is parametrized as
          alpha(t) = 1 + epsilon + alpha' t
          The epsilon and alpha' parameters can be set separately:

          Diffraction:PomFluxEpsilon   (default = 0.085; minimum = 0.02; maximum = 0.15)
          The Pomeron trajectory intercept epsilon above. For technical reasons epsilon > 0 is necessary in the current implementation.

          Diffraction:PomFluxAlphaPrime   (default = 0.25; minimum = 0.1; maximum = 0.4)
          The Pomeron trajectory slope alpha' above.

          When option 5 is selected, the following parameters of the MBR model [Cie12] are used:

          Diffraction:MBRepsilon   (default = 0.104; minimum = 0.02; maximum = 0.15)


          Diffraction:MBRalpha   (default = 0.25; minimum = 0.1; maximum = 0.4)
          the parameters of the Pomeron trajectory.

          Diffraction:MBRbeta0   (default = 6.566; minimum = 0.0; maximum = 10.0)


          Diffraction:MBRsigma0   (default = 2.82; minimum = 0.0; maximum = 5.0)
          the Pomeron-proton coupling, and the total Pomeron-proton cross section.

          Diffraction:MBRm2Min   (default = 1.5; minimum = 0.0; maximum = 3.0)
          the lowest value of the mass squared of the dissociated system.

          Diffraction:MBRdyminSDflux   (default = 2.3; minimum = 0.0; maximum = 5.0)


          Diffraction:MBRdyminDDflux   (default = 2.3; minimum = 0.0; maximum = 5.0)


          Diffraction:MBRdyminCDflux   (default = 2.3; minimum = 0.0; maximum = 5.0)
          the minimum width of the rapidity gap used in the calculation of Ngap(s) (flux renormalization).

          Diffraction:MBRdyminSD   (default = 2.0; minimum = 0.0; maximum = 5.0)


          Diffraction:MBRdyminDD   (default = 2.0; minimum = 0.0; maximum = 5.0)


          Diffraction:MBRdyminCD   (default = 2.0; minimum = 0.0; maximum = 5.0)
          the minimum width of the rapidity gap used in the calculation of cross sections, i.e. the parameter dy_S, which suppresses the cross section at low dy (non-diffractive region).

          Diffraction:MBRdyminSigSD   (default = 0.5; minimum = 0.001; maximum = 5.0)


          Diffraction:MBRdyminSigDD   (default = 0.5; minimum = 0.001; maximum = 5.0)


          Diffraction:MBRdyminSigCD   (default = 0.5; minimum = 0.001; maximum = 5.0)
          the parameter sigma_S, used for the cross section suppression at low dy (non-diffractive region).

          Separation into low and high masses

          Preferably one would want to have a perturbative picture of the dynamics of Pomeron-proton collisions, like multiparton interactions provide for proton-proton ones. However, while PYTHIA by default will only allow collisions with a CM energy above 10 GeV, the mass spectrum of diffractive systems will stretch to down to the order of 1.2 GeV. It would not be feasible to attempt a perturbative description there. Therefore we do offer a simpler low-mass description, with only longitudinally stretched strings, with a gradual switch-over to the perturbative picture for higher masses. The probability for the latter picture is parametrized as
          P_pert = P_max ( 1 - exp( (m_diffr - m_min) / m_width ) )
          which vanishes for the diffractive system mass m_diffr < m_min, and is 1 - 1/e = 0.632 for m_diffr = m_min + m_width, assuming P_max = 1.

          Diffraction:mMinPert   (default = 10.; minimum = 5.)
          The abovementioned threshold mass m_min for phasing in a perturbative treatment. If you put this parameter to be bigger than the CM energy then there will be no perturbative description at all, but only the older low-pt description.

          Diffraction:mWidthPert   (default = 10.; minimum = 0.)
          The abovementioned threshold width m_width.

          Diffraction:probMaxPert   (default = 1.; minimum = 0.; maximum = 1.)
          The abovementioned maximum probability P_max.. Would normally be assumed to be unity, but a somewhat lower value could be used to represent a small nonperturbative component also at high diffractive masses.

          Low-mass diffraction

          When an incoming hadron beam is diffractively excited, it is modeled as if either a valence quark or a gluon is kicked out from the hadron. In the former case this produces a simple string to the leftover remnant, in the latter it gives a hairpin arrangement where a string is stretched from one quark in the remnant, via the gluon, back to the rest of the remnant. The latter ought to dominate at higher mass of the diffractive system. Therefore an approximate behaviour like
          P_q / P_g = N / m^p
          is assumed.

          Diffraction:pickQuarkNorm   (default = 5.0; minimum = 0.)
          The abovementioned normalization N for the relative quark rate in diffractive systems.

          Diffraction:pickQuarkPower   (default = 1.0)
          The abovementioned mass-dependence power p for the relative quark rate in diffractive systems.

          When a gluon is kicked out from the hadron, the longitudinal momentum sharing between the the two remnant partons is determined by the same parameters as above. It is plausible that the primordial kT may be lower than in perturbative processes, however:

          Diffraction:primKTwidth   (default = 0.5; minimum = 0.)
          The width of Gaussian distributions in p_x and p_y separately that is assigned as a primordial kT to the two beam remnants when a gluon is kicked out of a diffractive system.

          Diffraction:largeMassSuppress   (default = 2.; minimum = 0.)
          The choice of longitudinal and transverse structure of a diffractive beam remnant for a kicked-out gluon implies a remnant mass m_rem distribution (i.e. quark plus diquark invariant mass for a baryon beam) that knows no bounds. A suppression like (1 - m_rem^2 / m_diff^2)^p is therefore introduced, where p is the diffLargeMassSuppress parameter.

          High-mass diffraction

          The perturbative description need to use parton densities of the Pomeron. The options are described in the page on ";?>PDF Selection. The standard perturbative multiparton interactions framework then provides cross sections for parton-parton interactions. In order to turn these cross section into probabilities one also needs an ansatz for the Pomeron-proton total cross section. In the literature one often finds low numbers for this, of the order of 2 mb. These, if taken at face value, would give way too much activity per event. There are ways to tame this, e.g. by a larger pT0 than in the normal pp framework. Actually, there are many reasons to use a completely different set of parameters for MPI in diffraction than in pp collisions, especially with respect to the impact-parameter picture, see below. A lower number in some frameworks could alternatively be regarded as a consequence of screening, with a larger "bare" number.

          For now, however, an attempt at the most general solution would carry too far, and instead we patch up the problem by using a larger Pomeron-proton total cross section, such that average activity makes more sense. This should be viewed as the main tunable parameter in the description of high-mass diffraction. It is to be fitted to diffractive event-shape data such as the average charged multiplicity. It would be very closely tied to the choice of Pomeron PDF; we remind that some of these add up to less than unit momentum sum in the Pomeron, a choice that also affect the value one ends up with. Furthermore, like with hadronic cross sections, it is quite plausible that the Pomeron-proton cross section increases with energy, so we have allowed for a power-like dependence on the diffractive mass.

          Diffraction:sigmaRefPomP   (default = 10.; minimum = 2.; maximum = 40.)
          The assumed Pomeron-proton effective cross section, as used for multiparton interactions in diffractive systems. If this cross section is made to depend on the mass of the diffractive system then the above value refers to the cross section at the reference scale, and
          sigma_PomP(m) = sigma_PomP(m_ref) * (m / m_ref)^p
          where m is the mass of the diffractive system, m_ref is the reference mass scale Diffraction:mRefPomP below and p is the mass-dependence power Diffraction:mPowPomP. Note that a larger cross section value gives less MPI activity per event. There is no point in making the cross section too big, however, since then pT0 will be adjusted downwards to ensure that the integrated perturbative cross section stays above this assumed total cross section. (The requirement of at least one perturbative interaction per event.)

          Diffraction:mRefPomP   (default = 100.0; minimum = 1.)
          The mRef reference mass scale introduced above.

          Diffraction:mPowPomP   (default = 0.0; minimum = 0.0; maximum = 0.5)
          The p mass rescaling pace introduced above.

          Also note that, even for a fixed CM energy of events, the diffractive subsystem will range from the abovementioned threshold mass m_min to the full CM energy, with a variation of parameters such as pT0 along this mass range. Therefore multiparton interactions are initialized for a few different diffractive masses, currently five, and all relevant parameters are interpolated between them to obtain the behaviour at a specific diffractive mass. Furthermore, A B ->X B and A B ->A X are initialized separately, to allow for different beams or PDF's on the two sides. These two aspects mean that initialization of MPI is appreciably slower when perturbative high-mass diffraction is allowed.

          Diffraction tends to be peripheral, i.e. occur at intermediate impact parameter for the two protons. That aspect is implicit in the selection of diffractive cross section. For the simulation of the Pomeron-proton subcollision it is the impact-parameter distribution of that particular subsystem that should rather be modeled. That is, it also involves the transverse coordinate space of a Pomeron wavefunction. The outcome of the convolution therefore could be a different shape than for nondiffractive events. For simplicity we allow the same kind of options as for nondiffractive events, except that the bProfile = 4 option for now is not implemented.

          Diffraction:bProfile   (default = 1; minimum = 0; maximum = 3)
          Choice of impact parameter profile for the incoming hadron beams.
          0 : no impact parameter dependence at all.
          1 : a simple Gaussian matter distribution; no free parameters.
          2 : a double Gaussian matter distribution, with the two free parameters coreRadius and coreFraction.
          3 : an overlap function, i.e. the convolution of the matter distributions of the two incoming hadrons, of the form exp(- b^expPow), where expPow is a free parameter.


          Diffraction:coreRadius   (default = 0.4; minimum = 0.1; maximum = 1.)
          When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a radius that is a factor coreRadius smaller than the rest.

          Diffraction:coreFraction   (default = 0.5; minimum = 0.; maximum = 1.)
          When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a fraction coreFraction of the matter content of the hadron.

          Diffraction:expPow   (default = 1.; minimum = 0.4; maximum = 10.)
          When bProfile = 3 it gives the power of the assumed overlap shape exp(- b^expPow). Default corresponds to a simple exponential drop, which is not too dissimilar from the overlap obtained with the standard double Gaussian parameters. For expPow = 2 we reduce to the simple Gaussian, bProfile = 1, and for expPow -> infinity to no impact parameter dependence at all, bProfile = 0. For small expPow the program becomes slow and unstable, so the min limit must be respected. "?>

          pythia8-8.1.80.orig/phpdoc/UMEPSMerging.php0000644000175000017500000002643512217615312016533 0ustar sunsun UMEPS Merging SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Unitarised Matrix Element + Parton Shower Merging

          Pythia offers the possibility to use the unitarised matrix element + parton shower merging scheme, as presented in [Lon12]. Unitarised ME+PS merging (UMEPS) allows for a consistent inclusion of tree-level multi-parton matrix elements into Pythia, and prevents potential changes in the inclusive production cross section. This makes it theoretically more appealing than CKKW-L merging. As in CKKW-L, UMEPS merging requires the user to supply Les Houches Event File input.

          UMEPS is different from other tree-level merging schemes in that it contains events with negative weights. These are generated by constructing parts of no-emission probabilities by reweighted higher-multiplicity samples [Lon12]. The main philosophy of UMEPS is "subtract what you add", meaning that in order to ensure the stability of the inclusive cross section, one has to counter the inclusion of additional tree-level matrix elements by "subtraction terms".

          The scheme closely reflects how unitarity is achieved in a non-merged shower, and indeed explicitly enforces the cancellations that are implicitly happening in a non-merged shower. This makes very low merging scale values possible.

          The usage of UMEPS is illustrated in the sample main program main86.cc, together with the input file main86.cmnd.

          Unitarised merging is heavily indebted to CKKW-L merging, and shares many settings with CKKW-L. In particular,

                   The hard process (Merging:Process)needs to be defined exactly as in CKKW-L (see Defining the hard process in the ";?>CKKW-L documentation).

                   The merging scale value (Merging:TMS) has to be set.

                   The maximal number of additional partons Merging:nJetMax has to be set.

          UMEPS further shares the switches listed under the sections "Matrix element merging and HepMC output for RIVET" and "Further variables" in the ";?>CKKW-L documentation with CKKW-L merging. Also, all MergingHooks routines that allow for user interference in CKKW-L merging are also usable for UMEPS -- with the exception of a user-defined merging scale. Currently, UMEPS is only implemented for a merging scale defined by the minimal Pythia evolution pT value between sets of radiator, emitted and recoiler partons. This is no fundamental limitation of the method, and will possibly be lifted in the future. Since this merging scale definition is not completely obvious, UMEPS also shares the Merging:enforceCutOnLHE switch with CKKW-L. In this way, it is possible to use LHE files that are regularised only with weak cuts as input, while the merging machinery imposes the stronger merging scale cut automatically. This means that no merging scale implementation is required from the user side, but also means that it is the user's responsibility to ensure that the cuts used for generating input LHE files are always looser than the cut given by the merging scale value Merging:TMS.


          UMEPS merging with main86.cc

          The UMEPS procedure is illustrated in the sample main program main86.cc (with the input card main86.cmnd). This program produces HepMC events [Dob01], that can be histogrammed (e.g. using RIVET [Buc10]), or used as input for a detector simulation. If the user is not familiar with HepMC analysis tools, it is possible to instead use Pythia's histogramming routines. For this, remove the lines referring to HepMC, and histogram events as illustrated (for CKKW-L) for the histogram histPTFirstSum in main84.cc, i.e. using weight*normhepmc as weight.

          In principle, no changes to main86.cc are necessary. Instead, all settings can be transferred to main86.cc through an input file. The input LHE files are also part of the (command line) input of main86.cc. Note that the sample program assumes that LHE file names are of the form name_tree_#nAdditionalJets.lhe. If you want to e.g. use the LHE files that are shipped with the Pythia distribution, you can execute main86.exe with the command

          ./main86.exe ./main86.cmnd ./w_production ./myhepmc.hepmc

          Since main86.cc is currently the "front-end" for UMEPS merging, we will briefly discuss this sample program in the following.

          Inputs

          In its current form, main86.cc uses separate tree-level LHE files for different numbers of additional partons as input. If e.g. UMEPS merging for W-boson + up to two additional partons is to be performed, three LHE files (for W+zero, W+one, W+two partons) are required. The configurations in the input files should be regularised with inclusive (i.e. weak) cuts. The actual "merging scale cut" will be handled internally. If e.g. Merging:TMS = 15 is the desired merging scale value, it is acceptable to regularise the matrix element calculation for Higgs+jets events at the LHC with the loose cuts pTjet = 5 GeV, ΔRjetA jetB = 0.01 and QjetA jetB = 5 GeV.

          All input settings are handed to main86.cc in the form of an input file. This input file has to contain

                   The number of desired events (Main:numberOfEvents)

                   The hard process (Merging:Process)

                   The merging scale value (Merging:TMS)

                   The maximal number of additional partons (Merging:nJetMax).

          Other settings are of course allowed. However, please refrain from adding switches that are used to invoke other merging schemes (e.g. Merging:doKTMerging) into the input file, since this can cause problems.

          Program flow

          The sample program starts by estimating the cross section for samples with different jet multiplicities. For this, the switch Merging:doXSectionEstimate is invoked together with the merging scale definition of Merging:doUMEPSTree, which corresponds to the minimal Pythia evolution pT value. We will come back to the latter switch below. All showering, multiparton interactions and hadronisation is, for speed reasons, switched off when estimating the cross section, since the hard cross section estimate would not be influenced by the event evolution anyway.

          After the hard cross sections are known (including the application of the merging scale cut), the first part of the UMEPS events is generated by using the following switch.

          Merging:doUMEPSTree On Off   (default = off)
          Reweight events according to the UMEPS prescription for tree-level configurations.

          The weight generated by the UMEPS procedure can be accessed by using the function double Info::mergingWeight(). When printing (or histogramming) merged events, this weight, multiplied with the estimated cross section for the current sample, should be used as event weight (or to fill histogram bins).

          After this first part is complete, the outcome is an addition of reweighted tree-level samples. To restore the inclusive cross section (i.e. that the cross section after merging corresponds to the cross section of the hard process, without any additional jets), it is necessary to subtract samples. Parton shower unitarity leads to the conclusion that "resolved" and "unresolved" corrections always cancel between states that contain an additional resolved jet, and states in which we "integrate over" the phase space of the additional jet. main86.cc makes this cancellation explicit by producing (correctly weighted) counter events by switching on

          Merging:doUMEPSSubt On Off   (default = off)
          Reweight events according to the UMEPS prescription of reweighted, integrated configurations. Please note that, in order for this to work smoothly, the switch Merging:doUMEPSTree has to be turned off.

          The integration is achieved internally, and the number of desired integrations (which is always one for UMEPS counter events) is set by

          Merging:nRecluster   (default = 0; minimum = 0)
          Number of hard partons to integrate out in the UMEPS procedure.

          Again, the weight generated by the UMEPS procedure can be accessed by using the function double Info::mergingWeight(). This weight, multiplied with the cross section of the current sample, and multiplied by -1, should then be used as event weight (or to fill histogram bins).

          Before returning, main86.cc prints the merged cross section after UMEPS merging. "?>

          pythia8-8.1.80.orig/phpdoc/files/0000755000175000017500000000000012217346234014714 5ustar sunsunpythia8-8.1.80.orig/phpdoc/PhaseSpaceCuts.php0000644000175000017500000006002412217615312017174 0ustar sunsun Phase Space Cuts SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Phase Space Cuts

          PhaseSpace is base class for all hard-process phase-space generators, either generic 2 -> 1 or 2 -> 2 ones, or specialized ones like for elastic and diffractive scattering.

          In it, it is possible to constrain the kinematics of most processes. (Exceptions are "soft physics", i.e. minimum bias, elastic and diffractive processes. The Coulomb singularity for elastic scatterings, if simulated, is ";?>handled separately.) These constraints apply in the rest frame of the hard subprocess, and topologies normally would be changed e.g. by subsequent showering activity. The cross section of a process is adjusted to only correspond to the allowed phase space.

          The more particles in the final state, the more cuts could be applied. Here we have tried to remain with the useful minimum, however. More generic possibilities could be handled by the ";?>user hooks facility.

          Cuts in all processes



          PhaseSpace:mHatMin   (default = 4.; minimum = 0.)
          The minimum invariant mass.

          PhaseSpace:mHatMax   (default = -1.)
          The maximum invariant mass. A value below mHatMin means there is no upper limit.

          Cuts in 2 -> 1 processes

          When a resonance id is produced, the ";?>mMin(id) and ";?>mMax(id) methods restrict the allowed mass range of this resonance. Therefore the allowed range is chosen to be the overlap of this range and the mHatMin to mHatMax range above. Most resonances by default have no upper mass limit, so effects mainly concern the lower limit. Should there be no overlap between the two ranges then the process will be switched off.

          Cuts in 2 -> 2 processes



          PhaseSpace:pTHatMin   (default = 0.; minimum = 0.)
          The minimum invariant pT.

          PhaseSpace:pTHatMax   (default = -1.)
          The maximum invariant pT. A value below pTHatMin means there is no upper limit.

          PhaseSpace:pTHatMinDiverge   (default = 1.; minimum = 0.5)
          Extra pT cut to avoid the divergences of some processes in the limit pT -> 0. Specifically, if either or both produced particles have a mass below pTHatMinDiverge then pT is limited from below by the larger of pTHatMin and pTHatMinDiverge.

          PhaseSpace:useBreitWigners On Off   (default = on)
          Allows masses to be selected according to Breit-Wigner shapes in 2 -> 2 processes, whenever particles have been declared with a nonvanishing width above the threshold below. In those cases also the limits below will be used for the mass selection. For 2 -> 1 processes the Breit-Wigner shape is part of the cross section itself, and therefore always included.

          PhaseSpace:minWidthBreitWigners   (default = 0.01; minimum = 1e-6)
          The minimum width a resonance must have for the mass to be dynamically selected according to a Breit-Wigner shape, within the limits set below. Only applies when useBreitWigners is on; else the nominal mass value is always used.

          For a particle with a Breit-Wigner shape selected, according to the rules above and to the rules of the particle species itself, the ";?>mMin(id) and ";?>mMax(id) methods restrict the allowed mass range of the particle, just like for the 2 -> 1 processes.

          Cuts in 2 -> 3 processes

          There are two main classes of 2 -> 3 processes. One is the processes such as WW/ZZ-fusion Higgs production, i.e. q q -> q q H, where there are no special singularities associated with two partons in the final state being collinear, or even for pT -> 0. For this class, no further cuts have been introduced than those already available for 2 -> 2 processes. Specifically, for now all three are restricted exactly the same way by pTHatMin and pTHatMax. As above, Breit-Wigner mass ranges can be restricted.

          The other 2 -> 3 event class is QCD processes, such as g g -> g g g. Here the soft and collinear singularities play a major role, and the phase space generation and cuts have been adapted to this. For this class, an alternative set of cuts is used, as outlined in the following. First of all the three outgoing partons are ordered in falling pT, i.e. pT_3 > pT_4 > pT_5 (where the labeling 3, 4, 5 of the outgoing partons is random, i.e. unrelated to the order specified in the process name). The allowed ranges of pT_3 and pT_5 can be specified, but obviously pT_3max >= pT_5max and pT_3min >= pT_5min. The pT_4 is not constrained explicitly, but is constructed from the vector sum of pT_3 and pT_5, subject to the constraint that it has to lie between the two in magnitude. While the pT cuts take care of singularities collinear with the incoming beams, it is also necessary to handle final-state singularities, when two outgoing partons become collinear. This is done by requiring a minimal separation in R, where R^2 = (Delta eta)^2 + (Delta phi)^2. Finally, a note about efficiency. The QCD 2 -> 3 phase space is not set up to explicitly include mHat as one of the basic variables. Such a cut is only done after a phase space point is already selected, which means that a narrow mass choice will slow down the program appreciably. Also narrow pT_3 and pT_5 bins are likely to give inefficient generation, if it gives rise to significant indirect restrictions on pT_4.

          PhaseSpace:pTHat3Min   (default = 10.; minimum = 0.)
          The minimum invariant pT of the highest-pT parton in QCD 2 -> 3 processes.

          PhaseSpace:pTHat3Max   (default = -1.)
          The maximum invariant pT of the highest-pT parton in QCD 2 -> 3 processes A value below pTHat3Min means there is no upper limit.

          PhaseSpace:pTHat5Min   (default = 10.; minimum = 0.)
          The minimum invariant pT of the lowest-pT parton in QCD 2 -> 3 processes.

          PhaseSpace:pTHat5Max   (default = -1.)
          The maximum invariant pT of the lowest-pT parton in QCD 2 -> 3 processes A value below pTHat5Min means there is no upper limit.

          PhaseSpace:RsepMin   (default = 1.)
          The minimum separation R in (eta, phi) space between any two outgoing partons in QCD 2 -> 3 processes.

          Cuts for a second hard process

          If you use the machinery that allows the generation of a specified ";?>second hard process then, by default, the same phase space cuts will be used for it as listed above. Optionally, however, you may use a second set of cuts, as described here. In this context "first" and "second" is merely a technical distinction; you are welcome e.g. to pick pT ranges such that the second interaction always has a larger pT than the first.

          PhaseSpace:sameForSecond On Off   (default = on)
          By default use the same cuts for a second hard process as for the first. If off then instead use the mass and pT cuts below, where relevant. (The other cuts above still remain the same.)

          PhaseSpace:mHatMinSecond   (default = 4.; minimum = 0.)
          The minimum invariant mass for a second interaction, if separate.

          PhaseSpace:mHatMaxSecond   (default = -1.)
          The maximum invariant mass for a second interaction, if separate. A value below mHatMin means there is no upper limit.

          PhaseSpace:pTHatMinSecond   (default = 0.; minimum = 0.)
          The minimum invariant pT for a second interaction, if separate.

          PhaseSpace:pTHatMaxSecond   (default = -1.)
          The maximum invariant pT for a second interaction, if separate. A value below pTHatMin means there is no upper limit.

          Generation strategy and documentation

          During the initialization stage a simplified function is found, that is intended to be above the true cross-section behaviour over the whole of phase space. It is chosen to be easily integrable and invertible. That way a trial phase space point can be selected according this simple function, and then be accepted by the ratio of true to the simple function. For a good efficiency the ratio should be close to unity, yet never above it. This constrains the absolute normalization of the simple function. The initial search may fail to find the phase space point where the true-to-simple ratio is maximal, however. This then can lead to subsequent maximum violations, where the ratio is above unity. Two alternative strategies are implemented to handle such situations, see below.

          PhaseSpace:showSearch On Off   (default = off)
          Possibility to print information on the search for phase-space coefficients that (in a multichannel approach) provides an analytical upper envelope of the differential cross section, and the corresponding upper estimate of the cross section. Of interest for crosschecks by expert users only.

          PhaseSpace:showViolation On Off   (default = off)
          Possibility to print information whenever the assumed maximum differential cross section of a process is violated, i.e. when the initial maximization procedure did not find the true maximum. Also, should negative cross sections occur, print whenever a more negative value is encountered.

          PhaseSpace:increaseMaximum On Off   (default = off)
          Strategy for handling cases where a larger cross section is obtained during the event generation than was assumed at initialization, i.e. when a violation occurs.
          off:each event comes with a weight, which normally is unity (as a consequence of the acceptance/rejection step), and is found in ";?>Info::weight(). For events which exceed the maximum instead the true-to-simple ratio is stored as event weight, which then is above unity. If the user so wishes this weight can then be carried along when event properties are histogrammed. Since normally such violations should be rare and not too much above unity one could expect most users to ignore such issues be default. Should maximum violations turn out to be frequent (visible in the ";?>Pythia::statistics() output) the option exists to use the information.
          on:the maximum is increased whenever it is exceeded. Thus events generated after this point will be "correctly" distributed, while ones generated previously obviously then have had too high a relative weight. If violations occur early on and/or are small this strategy should do a good job of correcting to the desired phase-space distribution. This strategy may be more convenient for the normal user, who would not wish to worry about event weights. It does have the disadvantage that the raised maximum introduces an extra amount of "history memory" to the generation sequence, so that it becomes less easy to save-and-restore the ";?>random-number state for debugging purposes.

          Reweighting of 2 -> 2 processes

          Events normally come with unit weight, i.e. are distributed across the allowed phase space region according to the appropriate differential cross sections. Sometimes it may be convenient to have an uneven distribution of events. The classical example here is that many cross sections drop off with transverse momentum pT, such that few events are generated at large pT scales. If one wants to plot the pT cross section, and all that comes with it, the statistical error will then degrade with increasing pT where fewer events end up.

          One solution is to split the full pT range into several separate subranges, where the events of each subsample obtains a different overall normalization. Specifically, if you generate a comparable number of events in each pT bin, such that larger pT bins are oversampled, these bins come with a correspondingly reduced overall weight, that needs to be taken into account when the bins are combined. The other is to have a continuously increasing oversampling of events at larger pT scales, which is compensated by a continuously decreasing weight for the event.

          Both of these solutions are supported. Specifically, for 2 -> 2 processes, the pTHat scale offers a convenient classification of the event. (Of course, two events starting out from the same pTHat scale will experience different parton shower evolutions, etc., and may therefore look quite different at the end.) The two cuts PhaseSpace:pTHatMin and PhaseSpace:pTHatMax therefore offers a way to slice a pT range into subranges, see e.g. main08.cc. Alternatively the ";?>User Hooks machinery offers the possibility for you to define your own reweighting of phase space sampling, with a corresponding event weight, with UserHooks::canBiasSelection and related methods.

          As a simplified option, we here offer the possibility to bias the 2 -> 2 sampling by a power of pTHat, then with events having a weight the inverse of this. This fast track will only work under a number of strict conditions, implemented to reduce the risk of abuse. (Whereas a UserHooks setup can be more flexible.) Specifically it will work if only high-pT 2 -> 2 processes already implemented in PYTHIA are requested, notably the HardQCD ones. That is, you cannot mix with 2 -> 1 or 2 -> 3 processes, nor with external processes (notably Les Houches input) or SoftQCD ones, and you cannot use the option to define a ";?>second hard process in the same event. Furthermore you have to be careful about the choice of PhaseSpace:pTHatMin, since a pTHat = 0 event would come with an infinite weight.

          PhaseSpace:bias2Selection On Off   (default = off)
          Possibility to switch on a biased phase space sampling, with compensatingly weighted events, for 2 -> 2 processes. Can only be used under the specific conditions explained in the paragraph above; under other conditions the initialization will abort.

          PhaseSpace:bias2SelectionPow   (default = 4.; minimum = 0.; maximum = 10.)
          If the above flag is on, then a 2 -> 2 process at a scale pTHat will be oversampled in phase space by an amount (pTHat/pTRef)^pow, where you set the power pow here. Events are assigned a compensating ";?>weight the inverse of this, i.e. Info::weight() will return (pTRef/pTHat)^pow. This weight should then be used in the histogramming of event properties. The final overall normalization also involves the Info::weightSum() value.

          PhaseSpace:bias2SelectionRef   (default = 10.; minimum = 1.)
          The reference scale pTRef introduced above, such that events with this pTHat obtain unit weight in the reweighting procedure. The value of this parameter has no impact on the final result of the reweighting procedure, but is only there for convenience, i.e. to give "reasonably-sized" weights. "?>

          pythia8-8.1.80.orig/phpdoc/HiddenValleyProcesses.php0000644000175000017500000010604212217615312020561 0ustar sunsun Hidden Valley Processes SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Hidden Valley Processes

          This Hidden Valley (HV) scenario has been developed specifically to allow the study of visible consequences of radiation in a hidden sector, by recoil effect. A key aspect is therefore that the normal timelike showering machinery has been expanded with a third kind of radiation, in addition to the QCD and QED ones. These three kinds of radiation are fully interleaved, i.e. evolution occurs in a common pT-ordered sequence. The scenario is described in [Car10]. Furthermore hadronization in the hidden sector has been implemented. Three main scenarios for production into and decay out of the hidden sector can be compared, in each case either for an Abelian or a non-Abelian gauge group in the HV. For further details see [Car11].

          Particle content and properties

          For simplicity we assume that the HV contains an unbroken SU(N) gauge symmetry. This is used in the calculation of production cross sections. These could be rescaled by hand for other gauge groups.

          HiddenValley:Ngauge   (default = 3; minimum = 1)
          is U(1) for Ngauge = 1, is SU(N) if Ngauge > 1. Note that pair production cross sections contains a factor of Ngauge for new particles in the fundamental representation of this group.

          A minimal HV particle content has been introduced. Firstly, there is a set of 12 particles that mirrors the Standard Model flavour structure, and is charged under both the SM and the HV symmetry groups. Each new particle couples flavour-diagonally to a corresponding SM state, and has the same SM charge and colour, but in addition is in the fundamental representation of the HV colour, as follows:
          Dv, identity 4900001, partner to the normal d quark;
          Uv, identity 4900002, partner to the normal u quark;
          Sv, identity 4900003, partner to the normal s quark;
          Cv, identity 4900004, partner to the normal c quark;
          Bv, identity 4900005, partner to the normal b quark;
          Tv, identity 4900006, partner to the normal t quark;
          Ev, identity 4900011, partner to the normal e lepton;
          nuEv, identity 4900012, partner to the normal nue neutrino;
          MUv, identity 4900013, partner to the normal mu lepton;
          nuMUv, identity 4900014, partner to the normal numu neutrino;
          TAUv, identity 4900015, partner to the normal tau lepton;
          nuTAUv, identity 4900016, partner to the normal nutau neutrino.
          Collectively we will refer to these states as Fv; note, however, that they need not be fermions themselves.

          In addition the model contains the HV gauge particle, either a HV-gluon or a HV-photon, but not both; see Ngauge above:
          gv, identity 4900021, is the massless gauge boson of the HV SU(N) group;
          gammav, identity 4900022, is the massless gauge boson of the HV U(1) group.

          Finally, for the basic HV scenario, there is a new massive particle with only HV charge sitting in the fundamental representation of the HV gauge group:
          qv, identity 4900101.

          The typical scenario would be for pair production of one of the states presented first above, e.g. g g -> Dv Dvbar. Such a Dv can radiate gluons and photons like an SM quark, but in addition HV-gluons or HV-photons in a similar fashion. Eventually the Dv will decay like Dv -> d + qv. The strength of this decay is not set as such, but is implicit in your choice of width for the Dv state. Thereafter the d and qv can radiate further within their respective sectors. The qv, gv or gammav are invisible, so their fate need not be considered further.

          While not part of the standard scenario, as an alternative there is also a kind of Z' resonance:
          Zv, identity 4900023, a boson that can couple both to pairs of Standard Model fermions and to qv qvbar pairs. Mass, total width and branching ratios can be set as convenient.
          This opens up for alternative processes l^+l^-, q qbar -> Zv -> qv qvbar.

          The possibility of a leakage back from the hidden sector will be considered in the Hadronization section below. For the U(1) case the gammav acquires a mass and can decay back to a Standard-Model fermion pair, while the qv remains invisible. The SU(N) alternative remains unbroken, so confinement holds and the gv is massless. A string like qv - gv - ... - gv - qvbar can break by the production of new qv - qvbar pairs, which will produce qv-qvbar mesons. It would be possible to build a rather sophisticated hidden sector by trivial extensions of the HV flavour content. For now, however, the qv can be duplicated in up to eight copies with the same properties except for the flavour charge. These are assigned codes 4900101 - 4900108. This gives a total of 64 possible lowest-lying mesons. We also include a duplication of that, into two multiplets, corresponding to the pseudoscalar and vector mesons of QCD. For now, again, these are assumed to have the same mass and other properties. Only the flavour-diagonal ones can decay back into the Standard-Model sector, however, while the rest remains in the hidden sector. It is therefore only necessary to distinguish a few states:
          pivDiag, identity 4900111, a flavour-diagonal HV-meson with spin 0 that can decay back into the Standard-Model sector;
          rhovDiag, identity 4900113, a flavour-diagonal HV-meson with spin 1 that can decay back into the Standard-Model sector;
          pivUp, identity 4900211, an off-diagonal HV-meson with spin 0 that is stable and invisible, with an antiparticle pivDn with identity -4900211; the particle is the one where the code of the flavour is larger than that of the antiflavour;
          rhovUp, identity 4900213, an off-diagonal HV-meson with spin 1 that is stable and invisible, with an antiparticle rhovDn with identity -4900213; again the particle is the one where the code of the flavour is larger than that of the antiflavour;
          ggv, identity 4900991, is only rarely used, to handle cases where it is kinematically impossible to produce an HV-meson on shell, and it therefore is assumed to de-excite by the emission of invisible gv-gv v-glueball bound states.

          Only the spin of the HV-gluon or HV-photon is determined unambiguously to be unity, for the others you can make your choice.

          HiddenValley:spinFv   (default = 1; minimum = 0; maximum = 2)
          The spin of the HV partners of the SM fermions, e.g. Dv, Uv, Ev and nuEv.
          0 : spin 0.
          1 : spin 1/2.
          2 : spin 1/2.


          HiddenValley:spinqv   (default = 0; minimum = 0; maximum = 1)
          The spin of qv when the Fv (the HV partners of the SM fermions) have spin 1/2. (While, if they have spin 0 or 1, the qv spin is fixed at 1/2.)
          0 : spin 0.
          1 : spin 0.


          HiddenValley:kappa   (default = 1.)
          If the Fv have spin 1 then their production cross section depends on the presence of anomalous magnetic dipole moment, i.e. of a kappa different from unity. For other spins this parameter is not used.

          HiddenValley:doKinMix On Off   (default = off)
          allow kinematic mixing or not.

          HiddenValley:kinMix   (default = 1.)
          strength of kinetic mixing.

          You should set the Fv and qv masses appropriately, with the latter smaller than the former two to allow decays. When U(1) hadronization is switched on, you need to set the gammav mass and decay modes. For SU(N) hadronization the HV-meson masses should be set to match the qv ones. The simplest is to assume that m_qv defines a constituent mass, so that m_HVmeson = 2 m_qv. The hvMesonDiag decay modes also need to be set.

          Production processes



          HiddenValley:all On Off   (default = off)
          Common switch for the group of all hard Hidden Valley processes, as listed separately in the following.

          HiddenValley:gg2DvDvbar On Off   (default = off)
          Pair production g g -> Dv Dvbar. Code 4901.

          HiddenValley:gg2UvUvbar On Off   (default = off)
          Pair production g g -> Uv Uvbar. Code 4902.

          HiddenValley:gg2SvSvbar On Off   (default = off)
          Pair production g g -> Sv Svbar. Code 4903.

          HiddenValley:gg2CvCvbar On Off   (default = off)
          Pair production g g -> Cv Cvbar. Code 4904.

          HiddenValley:gg2BvBvbar On Off   (default = off)
          Pair production g g -> Bv Bvbar. Code 4905.

          HiddenValley:gg2TvTvbar On Off   (default = off)
          Pair production g g -> Tv Tvbar. Code 4906.

          HiddenValley:qqbar2DvDvbar On Off   (default = off)
          Pair production q qbar -> Dv Dvbar via intermediate gluon. Code 4911.

          HiddenValley:qqbar2UvUvbar On Off   (default = off)
          Pair production q qbar -> Uv Uvbar via intermediate gluon. Code 4912.

          HiddenValley:qqbar2SvSvbar On Off   (default = off)
          Pair production q qbar -> Sv Svbar via intermediate gluon. Code 4913.

          HiddenValley:qqbar2CvCvbar On Off   (default = off)
          Pair production q qbar -> Cv Cvbar via intermediate gluon. Code 4914.

          HiddenValley:qqbar2BvBvbar On Off   (default = off)
          Pair production q qbar -> Bv Bvbar via intermediate gluon. Code 4915.

          HiddenValley:qqbar2TvTvbar On Off   (default = off)
          Pair production q qbar -> Tv Tvbar via intermediate gluon. Code 4916.

          HiddenValley:ffbar2DvDvbar On Off   (default = off)
          Pair production f fbar -> Dv Dvbar via intermediate gamma*/Z^*. Code 4921.

          HiddenValley:ffbar2UvUvbar On Off   (default = off)
          Pair production f fbar -> Uv Uvbar via intermediate gamma*/Z^*. Code 4922.

          HiddenValley:ffbar2SvSvbar On Off   (default = off)
          Pair production f fbar -> Sv Svbar via intermediate gamma*/Z^*. Code 4923.

          HiddenValley:ffbar2CvCvbar On Off   (default = off)
          Pair production f fbar -> Cv Cvbar via intermediate gamma*/Z^*. Code 4924.

          HiddenValley:ffbar2BvBvbar On Off   (default = off)
          Pair production f fbar -> Bv Bvbar via intermediate gamma*/Z^*. Code 4925.

          HiddenValley:ffbar2TvTvbar On Off   (default = off)
          Pair production f fbar -> Tv Tvbar via intermediate gamma*/Z^*. Code 4926.

          HiddenValley:ffbar2EvEvbar On Off   (default = off)
          Pair production f fbar -> Ev Evbar via intermediate gamma*/Z^*. Code 4931.

          HiddenValley:ffbar2nuEvnuEvbar On Off   (default = off)
          Pair production f fbar -> nuEv nuEvbar via intermediate gamma*/Z^*. Code 4932.

          HiddenValley:ffbar2MUvMUvbar On Off   (default = off)
          Pair production f fbar -> MUv MUvbar via intermediate gamma*/Z^*. Code 4933.

          HiddenValley:ffbar2nuMUvnuMUvbar On Off   (default = off)
          Pair production f fbar -> nuMUv nuMUvbar via intermediate gamma*/Z^*. Code 4934.

          HiddenValley:ffbar2TAUvTAUvbar On Off   (default = off)
          Pair production f fbar -> TAUv TAUvbar via intermediate gamma*/Z^*. Code 4935.

          HiddenValley:ffbar2nuTAUvnuTAUvbar On Off   (default = off)
          Pair production f fbar -> nuTAUv nuTAUvbar via intermediate gamma*/Z^*. Code 4936.

          HiddenValley:ffbar2Zv On Off   (default = off)
          Production f fbar -> Zv where Zv is a generic resonance that couples both SM fermion pairs and a qv qvbar pair. Not part of the framework of the above processes, but as an alternative. Code 4941.

          Timelike showers

          One key point of this HV scenario is that radiation off the HV-charged particles is allowed. This is done by the standard final-state showering machinery. (HV particles are not produced in initial-state radiation.) All the (anti)particles Fv and qv have one (negative) unit of HV charge. That is, radiation closely mimics the one in QCD. Both QCD, QED and HV radiation are interleaved in one common sequence of decreasing emission pT scales. Each radiation kind defines a set of dipoles, usually spanned between a radiating parton and its recoil partner, such that the invariant mass of the pair is not changed when a radiation occurs. This need not follow from trivial colour assignments, but is often obvious. For instance, in a decay Qv -> q + qv the QCD dipole is between the q and the hole after Qv, but qv becomes the recoiler should a radiation occur, while the role of q and qv is reversed for HV radiation.

          This also includes matrix-element corrections for a number of decay processes, with colour, spin and mass effects included [Nor01]. They were calculated within the context of the particle content of the MSSM, however, which does not include spin 1 particles with unit colour charge. In such cases spin 0 is assumed instead. By experience, the main effects come from mass and colour flow anyway, so this is not a bad approximation. (Furthermore the MSSM formulae allow for gamma_5 factors from wave functions or vertices; these are even less important.)

          An emitted gv can branch in its turn, gv -> gv + gv. This radiation may affect momenta in the visible sector by recoil effect, but this is a minor effect relative to the primary emission of the gv.

          HiddenValley:FSR On Off   (default = off)
          switch on final-state shower of gv or gammav in a HV production process.

          HiddenValley:alphaFSR   (default = 0.1; minimum = 0.0)
          fixed alpha scale of gv/gammav emission; corresponds to alpha_strong of QCD or alpha_em of QED. For shower branchings such as Dv -> Dv + gv the coupling is multiplied by C_F = (N^2 - 1) / (2 * N) for an SU(N) group and for gv -> gv + gv by N.

          HiddenValley:pTminFSR   (default = 0.4; minimum = 0.1)
          lowest allowed pT of emission. Chosen with same default as in normal QCD showers.

          Hadronization

          By default the HV particles with no Standard Model couplings are not visible. Their presence can only be deduced by the observation of missing (transverse) momentum in the event as a whole. In the current implementation it is possible to simulate two different scenarios where activity can leak back from the hidden sector.

          The first possibility is relevant for the U(1) scenario. The U(1) group may be broken, so that the gammav acquires a mass. Furthermore, the gammav may have a small mixing angle with the normal photon, or with some Z' state or other mediator, and may thus decay back into Standard Model particles. The qv still escapes undetected; recall that there is no confinement in the U(1) option.

          In order to enable this machinery two commands are necessary, 4900022:m0 = ... to set the gammav mass to the desired value, and 4900022:onMode = on to enable gammav decays. The default gammav decay table contains all Standard Model fermion-antifermion pairs, except top, with branching ratios in proportion to their coupling to the photon, whenever the production channel is allowed by kinematics. This table could easily be tailored to more specific models and needs. For instance, for a mass below 1 - 2 GeV, it would make sense to construct a table of exclusive hadronic decay channels rather than go the way via a hadronizing quark pair.

          The gammav are expected to decay so rapidly that no secondary vertex will be detectable. However, it is possible to set 4900022:tau0 to a finite lifetime (in mm) that will be used to create separated secondary vertices.

          The second, more interesting, possibility is relevant for the SU(N) scenarios. Here the gauge group remains unbroken, i.e. gv is massless, and the partons are confined. Like in QCD, the HV-partons can therefore be arranged in one single HV-colour-ordered chain, with a qv in one end, a qvbar in the other, and a varying number of gv in between. Each event will only contain (at most) one such string, (i) since perturbative branchings gv -> qv qvbar have been neglected, as is a reasonable approximation for QCD, and (ii) since HV-colours are assigned in the N_C -> infinity limit, just like in the handling of string fragmentation in QCD. The HV-string can then fragment by the nonperturbative creation of qv qvbar pairs, leading to the formation of HV-mesons along the string, each with its qv from one vertex and its qvbar from the neighbouring one.

          Since, so far, we have only assumed there to be one qv species, all produced qv qvbar HV-mesons are of the same flavour-diagonal species. Such an HV-meson can decay back to the normal sector, typically by whatever mediator particle allowed production in the first place. In this framework the full energy put into the HV sector will leak back to the normal one. To allow more flexibility, an ad hoc possibility of n_Flav different qv species is introduced. For now they are all assumed to have the same mass and other properties, but distinguished by some flavour-like property. Only the flavour-diagonal ones can decay, meaning that only a fraction (approximately) 1/n_Flav of the HV-energy leaks back, while the rest remains in the hidden sector.

          This scenario contains more parameters than the first one, for the U(1) group. They can be subdivided into two sets. One is related to particle properties, both for qv and for the two different kinds of HV-mesons, here labeled 4900111 and 4900113 for the diagonal ones, and +-4900211 and +-4900213 for the off-diagonal ones. It makes sense to set the HV-meson masses to be twice the qv one, as in a simple constituent mass context. Furthermore the hvMesonDiag decay modes need to be set up. Like with the gammav in the U(1) option, the default decay table is based on the branching ratios of an off-shell photon.

          The second set are fragmentation parameters that extend or replace the ones used in normal string fragmentation. Some of them are not encoded in the same way as normally, however, but rather scale as the qv mass is changed, so as to keep a sensible default behaviour. This does not mean that deviations from this set should not be explored, or that other scaling rules could be preferred within alternative scenarios. These parameters are as follows.

          HiddenValley:fragment On Off   (default = off)
          switch on string fragmentation of the HV partonic system. Only relevant for SU(N) scenarios.

          HiddenValley:nFlav   (default = 1; minimum = 1; maximum = 8)
          number of different flavours assumed to exist in the hadronization description, leading to approximately 1/n_Flav of the produced HV-mesons being flavour-diagonal and capable to decay back to Standard Model particles.

          HiddenValley:probVector   (default = 0.75; minimum = 0.; maximum = 1.)
          fraction of HV-mesons that are assigned spin 1 (vector), with the remainder spin 0 (pseudoscalar). Assuming the qv have spin 1/2 and the mass splitting is small, spin counting predicts that 3/4 of the mesons should have spin 1.

          HiddenValley:aLund   (default = 0.3; minimum = 0.0; maximum = 2.0)
          The a parameter of the Lund symmetric fragmentation function. See the normal ";?>fragmentation function description for the shape of this function.

          HiddenValley:bmqv2   (default = 0.8; minimum = 0.2; maximum = 2.0)
          The b parameter of the Lund symmetric fragmentation function, multiplied by the square of the qv mass. This scaling ensures that the fragmentation function keeps the same shape when the qv mass is changed (neglecting transverse momenta).

          HiddenValley:rFactqv   (default = 1.0; minimum = 0.0; maximum = 2.0)
          r_qv, i.e. the Bowler correction factor to the Lund symmetric fragmentation function, which could be made weaker or stronger than its natural value.

          HiddenValley:sigmamqv   (default = 0.5; minimum = 0.0)
          the width sigma of transverse momenta in the HV fragmentation process, normalized to the qv mass. This ensures that sigma scales proportionately to m_qv. See the normal ";?>fragmentation pT description for conventions for factors of 2. "?>

          pythia8-8.1.80.orig/phpdoc/HepMCInterface.php0000644000175000017500000002137012217615312017077 0ustar sunsun HepMC Interface SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          HepMC Interface

          An interface to the HepMC [Dob01] standard event record format has been provided by M. Kirsanov. To use it, the relevant libraries need to be linked, as explained in the README and README.HepMC files. Only version 2.06 (or later) of HepMC is supported as of 1 January 2013, by agreement with the LHC experimental community.

          The (simple) procedure to translate PYTHIA 8 events into HepMC ones is illustrated in the main41.cc, main42.cc main61.cc and main62.cc main programs. At the core is a call to the

          HepMC::Pythia8ToHepMC::fill_next_event( pythia, hepmcevt, ievnum = -1) 
          
          which takes a reference of the generator object and uses it, on the one hand, to read out and convert the event record in pythia.event and, on the other hand, to extract and store parton-density (PDF), cross section and other information for the hard subprocess from pythia.info. There is also an alternative form that does not requires access to the full pythia object, but only the event record, at the expense of a reduced information storage, see below.

          While PYTHIA always stores momenta in units of GeV, with c = 1, HepMC nowadays can be built either for MeV or GeV as default, a choice that can then be overridden on an event-by-event basis, see e.g. the main41.cc code. When filling the HepMC event record, PYTHIA will convert to the unit specified for the current HepMC event record.

          Also for length units there are choices, and again the PYTHIA interface will convert to the units set for the HepMC event record. Here the mm choice of PYTHIA seems to be shared by most other programs, and is HepMC default.

          The status code is now based on the new standard introduced for HepMC 2.05, see the ";?>Event::statusHepMC(...) conversion routine for details.

          The current values from pythia.info.sigmaGen() and pythia.info.sigmaErr() are stored for each event, multiplied by 10^9 to convert from mb to pb. Note that PYTHIA improves its accuracy by Monte Carlo integration in the course of the run, so the values associated with the last generated event should be the most accurate ones. If events also come with a dimensional weight, like in some Les Houches strategies, this weight is in units of pb.

          The public methods

          Here comes a complete list of all public methods of the Pythia8ToHepMC class in the HepMC (not Pythia8!) namespace.

          Pythia8ToHepMC::Pythia8ToHepMC()  
          virtual Pythia8ToHepMC::~Pythia8ToHepMC()  
          the constructor and destructor take no arguments.

          bool Pythia8ToHepMC::fill_next_event( Pythia8::Pythia& pythia, GenEvent* evt, int ievnum = -1)  
          convert a Pythia event to a HepMC one. Will return true if succeeded.
          argument pythia : the input Pythia generator object, from which both the event and other information can be obtained.
          argument evt : the output GenEvt event, in its standard form.
          argument iev : set the event number of the current event. If negative then the internal event number is used, which is incremented by one for each new event.

          bool Pythia8ToHepMC::fill_next_event( Pythia8::Event& pyev, GenEvent* evt, int ievnum = -1, Pythia8::Info* pyinfo = 0, Pythia8::Settings* pyset = 0)  
          convert a Pythia event to a HepMC one. Will return true if succeeded.
          argument pyev : the input Pythia event that is to be converted to HepMC format.
          argument evt : the output GenEvt event, in its standard form.
          argument iev : set the event number of the current event. If negative then the internal event number is used, which is incremented by one for each new event.
          argument pyinfo : pointer to the Pythia Info object, which is used to extract PFD values, and process and cross section information. Without such a pointer this information therefore cannot be stored, i.e. it is equivalent to the three set_store methods below being set false.
          argument pyset : pointer to the Pythia Settings object, which is used to decide whether hadronization is carried out, and therefore whether to warn about unhadronized partons. Without such a pointer the set_free_parton_warnings method below uniquely controls the behaviour.

          The following paired methods can be used to set and get the status of some switches that modify the behaviour of the conversion routine. The set methods have the same default input values as the internal initialization ones, so that a call without an argument (re)stores the default.

          void Pythia8ToHepMC::set_print_inconsistency(bool b = true)  
          bool Pythia8ToHepMC::print_inconsistency()  
          print a warning line, on cerr, when inconsistent mother and daughter information is encountered.

          void Pythia8ToHepMC::set_free_parton_warnings(bool b = true)  
          bool Pythia8ToHepMC::free_parton_warnings()  
          check and print a warning line when unhadronized gluons or quarks are encountered in the event record. Does not apply when Pythia hadronization is switched off. Default is to do this check.

          void Pythia8ToHepMC::set_crash_on_problem(bool b = false)  
          bool Pythia8ToHepMC::crash_on_problem()  
          if problems (like the free partons above) are encountered then the run is interrupted by an exit(1) command. Default is not to crash.

          void Pythia8ToHepMC::set_convert_gluon_to_0(bool b = false)  
          bool Pythia8ToHepMC::convert_gluon_to_0()  
          the normal gluon identity code 21 is used also when parton density information is stored, unless this optional argument is set true to have gluons represented by a 0. This choice does not affect the normal event record, where a gluon is always 21.

          void Pythia8ToHepMC::set_store_pdf(bool b = true)  
          bool Pythia8ToHepMC::store_pdf()  
          for each event store information on the two incoming flavours, their x values and common factorization scale, and the values of the two parton distributions, xf(x,Q).

          void Pythia8ToHepMC::set_store_proc(bool b = true)  
          bool Pythia8ToHepMC::store_proc()  
          for each event store information on the Pythia process code, the renormalization scale, and alpha_em and alpha_s values used for the hard process.

          void Pythia8ToHepMC::set_store_xsec(bool b = true)  
          bool Pythia8ToHepMC::store_xsec()  
          for each event store information on the Pythia cross section and its error, in pb, and the event weight. If events also come with a dimensional weight, like in some Les Houches strategies, this weight is in units of pb. pythia8-8.1.80.orig/phpdoc/UserHooks.php0000644000175000017500000014154712217615312016255 0ustar sunsun User Hooks SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          User Hooks

          Sometimes it may be convenient to step in during the generation process: to modify the built-in cross sections, to veto undesirable events or simply to collect statistics at various stages of the evolution. There is a base class UserHooks that gives you this access at a few selected places. This class in itself does nothing; the idea is that you should write your own derived class for your task. One simple derived class (SuppressSmallPT) comes with the program, mainly as illustration, and the main10.cc program provides a complete (toy) example how a derived class could be set up and used.

          There are six sets of routines, that give you different kinds of freedom. They are, in no particular order:
          (i) Ones that give you access to the event record in between the process-level and parton-level steps, or in between the parton-level and hadron-level ones. You can study the event record and decide whether to veto this event.
          (ii) Ones that allow you to set a scale at which the combined parton-level MPI+ISR+FSR downwards evolution in pT is temporarily interrupted, so the event can be studied and either vetoed or allowed to continue the evolution.
          (iii) Ones that allow you to to study the event after the first few ISR/FSR emissions, or first few MPI, so the event can be vetoed or allowed to continue the evolution.
          (iv) Ones that allow you to study the latest initial- or final-state emission and veto that emission, without vetoing the event as a whole.
          (v) Ones that give you access to the properties of the trial hard process, so that you can modify the internal Pythia cross section, alternatively the phase space sampling, by your own correction factors.
          (vi) Ones that allow you to reject the decay sequence of resonances at the process level.
          (vii) Ones that let you set the scale of shower evolution, specifically for matching in resonance decays.
          They are described further in the following numbered subsections.

          All the possibilities above can be combined freely and also be combined with the standard flags. An event would then survive only if it survived each of the possible veto methods. There are no hidden interdependencies in this game, but of course some combinations may not be particularly meaningful. For instance, if you set PartonLevel:all = off then the doVetoPT(...) and doVetoPartonLevel(...) locations in the code are not even reached, so they would never be called.

          The effect of the vetoes of types (i), (ii) and (iii) can be studied in the output of the ";?>Pythia::statistics() method. The "Selected" column represents the number of events that were found acceptable by the internal Pythia machinery, whereas the "Accepted" one are the events that also survived the user cuts. The cross section is based on the latter number, and so is reduced by the amount associated by the vetoed events. Also type (v) modifies the cross section, while types (iv), (vi) and (vii) do not.

          A warning. When you program your own derived class, do remember that you must exactly match the arguments of the base-class methods you overload. If not, your methods will be considered as completely new ones, and compile without any warnings, but not be used inside Pythia. So, at the debug stage, do insert some suitable print statements to check that the new methods are called (and do what they should).

          The basic components

          For a derived UserHooks class to be called during the execution, a pointer to an object of this class should be handed in with the
          ";?> Pythia::setUserHooksPtr( UserHooks*)
          method. The first step therefore is to construct your own derived class, of course. This must contain a constructor and a destructor. The initPtr method comes "for free", and is set up without any intervention from you.

          UserHooks::UserHooks()  
          virtual UserHooks::~UserHooks()  
          The constructor and destructor do not need to do anything.

          void UserHooks::initPtr( Info* infoPtr, Settings* settingsPtr, ParticleData* particleDataPtr, Rndm* rndmPtr, BeamParticle* beamAPtr, BeamParticle* beamBPtr, BeamParticle* beamPomAPtr, BeamParticle* beamPomBPtr, CoupSM* coupSMPtr, PartonSystems* partonSystemsPtr, SigmaTotal* sigmaTotPtr)  
          this (non-virtual) method is automatically called during the initialization stage to set several useful pointers, and to set up the workEvent below. The corresponding objects can later be used to extract some useful information.
          ";?>Info: general event and run information, including some loop counters.
          ";?>Settings: the settings used to determine the character of the run.
          ";?>ParticleData: the particle data used in the event record (including workEvent below).
          ";?>Rndm: the random number generator, that you could also use in your code.
          ";?>BeamParticle: the beamAPtr and beamBPtr beam particles contain info on partons extracted from the two incoming beams, on the PDFs used, and more. In cases when diffraction is simulated, also special Pomeron beams beamPomAPtr and beamPomBPtr are introduced, for the Pomerons residing inside the respective proton.
          ";?>CoupSM: Standard Model couplings.
          ";?>PartonSystems: the list of partons that belong to each individual subcollision system.
          ";?>SigmaTotal: total/elastic/diffractive cross section parametrizations.

          Next you overload the desired methods listed in the sections below. These often come in pairs or triplets, where the first must return true for the last method to be called. This latter method typically hands you a reference to the event record, which you then can use to decide whether or not to veto. Often the event record can be quite lengthy and difficult to overview. The following methods and data member can then come in handy.

          void UserHooks::omitResonanceDecays(const Event& process, bool finalOnly = false)  
          is a protected method that you can make use of in your own methods to extract a simplified list of the hard process, where all resonance decay chains are omitted. Intended for the can/doVetoProcessLevel routines. Note that the normal process-level generation does include resonance decays. That is, if a top quark is produced in the hard process, then also decays such as t -> b W+, W+ -> u dbar will be generated and stored in process. The omitResonanceDecays routine will take the input process and copy it to workEvent (see below), minus the resonance decay chains. All particles produced in the hard process, such as the top, will be considered final-state ones, with positive status and no daughters, just as it is before resonances are allowed to decay.
          (In the PartonLevel routines, these decay chains will initially not be copied from process to event. Instead the combined MPI, ISR and FSR evolution is done with the top above as final particle. Only afterwards will the resonance decay chains be copied over, with kinematics changes reflecting those of the top, and showers in the decays carried out.)
          For the default finalOnly = false the beam particles and incoming partons are retained, so the event looks like a normal event record up to the point of resonance decays, with a normal history setup.
          With finalOnly = true only the final-state partons are retained in the list. It therefore becomes similar in functionality to the subEvent method below, with the difference that subEvent counts the decay products of the resonances as the final state, whereas here the resonances themselves are the final state. Since the history has been removed in this option, mother1() and mother2() return 0, while daughter1() and daughter2() both return the index of the same parton in the original event record.

          void UserHooks::subEvent(const Event& event, bool isHardest = true)  
          is a protected method that you can make use of in your own methods to extract a brief list of the current partons of interest, with all irrelevant ones omitted. It is primarily intended to track the evolution at the parton level, notably the shower evolution of the hardest (i.e. first) interaction.
          For the default isHardest = true only the outgoing partons from the hardest interaction (including the partons added to it by ISR and FSR) are extracted, as relevant e.g. for doVetoPT( iPos, event) with iPos = 0 - 4. With isHardest = false instead the outgoing partons of the latest "subprocess" are extracted, as relevant when iPos = 5, where it corresponds to the outgoing partons in the currently considered decay.
          The method also works at the process level, but there simply extracts all final-state partons in the event, and thus offers no extra functionality.
          The result is stored in workEvent below. Since the history has been removed, mother1() and mother2() return 0, while daughter1() and daughter2() both return the index of the same parton in the original event record (event; possibly process), so that you can trace the full history, if of interest.

          Event UserHooks::workEvent  
          This protected class member contains the outcome of the above omitResonanceDecays(...) and subEvent(...) methods. Alternatively you can use it for whatever temporary purposes you wish. You are free to use standard operations, e.g. to boost the event to its rest frame before analysis, or remove particles that should not be analyzed. The workEvent can also be sent on to a ";?>jet clustering algorithm.

          (i) Interrupt between the main generation levels

          virtual bool UserHooks::initAfterBeams()  
          This routine is called by Pythia::init(), after the beams have been set up, but before any other initialisation. Therefore, at this stage, it is still possible to modify settings (apart from Beams:*) and particle data. This is mainly intended to be used in conjunction with Les Houches Event files, where headers are read in during beam initialisation, see the header functions in the ";?>Info class. In the base class this method returns true. By returning false, PYTHIA initialisation will be aborted.

          virtual bool UserHooks::canVetoProcessLevel()  
          In the base class this method returns false. If you redefine it to return true then the method doVetoProcessLevel(...) will be called immediately after a hard process (and associated resonance decays) has been selected and stored in the ";?>process event record.
          At this stage, the process record typically contains the two beams in slots 1 and 2, the two incoming partons to the hard process in slots 3 and 4, the N (usually 1, 2 or 3) primary produced particles in slots 5 through 4 + N, and thereafter recursively the resonance decay chains, if any. Use the method omitResonanceDecays(...) if you want to skip these decay chains. There are exceptions to this structure, for ";?>soft QCD processes (where the partonic process may not yet have been selected at this stage), and when ";?>a second hard process has been requested (where two hard processes are bookkept). In general it is useful to begin the development work by listing a few process records, to clarify what the structure is for the cases of interest.

          virtual bool UserHooks::doVetoProcessLevel(Event& process)  
          can optionally be called, as described above. You can study the process event record of the hard process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next().
          Warning: Normally you should not modify the process event record. However, for some matrix-element-matching procedures it may become unavoidable. If so, be very careful, since there are many pitfalls. Only to give one example: if you modify the incoming partons then also the information stored in the beam particles may need to be modified.
          Note: the above veto is different from setting the flag ";?>PartonLevel:all = off. Also in the latter case the event generation will stop after the process level, but an event generated up to this point is considered perfectly acceptable. It can be studied and it contributes to the cross section. That is, PartonLevel:all = off is intended for simple studies of hard processes, where one can save a lot of time by not generating the rest of the story. By contrast, the doVetoProcessLevel() method allows you to throw away uninteresting events at an early stage to save time, but those events that do survive the veto are allowed to develop into complete final states (unless flags have been set otherwise).

          virtual bool UserHooks::canVetoPartonLevel()  
          In the base class this method returns false. If you redefine it to return true then the method doVetoPartonLevel(...) will be called immediately after the parton level has been generated and stored in the ";?>event event record. Thus showers, multiparton interactions and beam remnants have been set up, but hadronization and decays have not yet been performed. This is already a fairly complete event, possibly with quite a complex parton-level history. Therefore it is usually only meaningful to study the hardest interaction, e.g. using subEvent(...) introduced above, or fairly generic properties, such as the parton-level jet structure.

          virtual bool UserHooks::doVetoPartonLevel(const Event& event)  
          can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next().
          Note: the above veto is different from setting the flag ";?>HadronLevel:all = off. Also in the latter case the event generation will stop after the parton level, but an event generated up to this point is considered perfectly acceptable. It can be studied and it contributes to the cross section. That is, HadronLevel:all = off is intended for simple studies of complete partonic states, where one can save time by not generating the complete hadronic final state. By contrast, the doVetoPartonLevel() method allows you to throw away uninteresting events to save time that way, but those events that do survive the veto are allowed to develop into complete final states (unless flags have been set otherwise).

          virtual bool UserHooks::canVetoPartonLevelEarly()  
          is very similar to canVetoPartonLevel() above, except that the chance to veto appears somewhat earlier in the generation chain, after showers and multiparton interactions, but before the beam remnants and resonance decays have been added. It is therefore somewhat more convenient for many matrix element strategies, where the primordial kT added along with the beam remnants should not be included.

          virtual bool UserHooks::doVetoPartonLevelEarly(const Event& event)  
          is very similar to doVetoPartonLevel(...) above, but the veto can be done earlier, as described for canVetoPartonLevelEarly().

          (ii) Interrupt during the parton-level evolution, at a pT scale

          During the parton-level evolution, multiparton interactions (MPI), initial-state radiation (ISR) and final-state radiation (FSR) are normally evolved downwards in one interleaved evolution sequence of decreasing pT values. For some applications, e.g matrix-element-matching approaches, it may be convenient to stop the evolution temporarily when the "hard" emissions have been considered, but before continuing with the more time-consuming soft activity. Based on these hard partons one can make a decision whether the event at all falls in the intended event class, e.g. has the "right" number of parton-level jets. If yes then, as for the methods above, the evolution will continue all the way up to a complete event. Also as above, if no, then the event will not be considered in the final cross section.

          Recall that the new or modified partons resulting from a MPI, ISR or FSR step are always appended to the end of the then-current event record. Previously existing partons are not touched, except for the ";?>status, mother and daughter values, which are updated to reflect the modified history. It is therefore straightforward to find the partons associated with the most recent occurrence.
          An MPI results in four new partons being appended, two incoming and two outgoing ones.
          An ISR results in the whole affected system being copied down, with one of the two incoming partons being replaced by a new one, and one more outgoing parton.
          An FSR results in three new partons, two that come from the branching and one that takes the recoil.
          The story becomes more messy when rescattering is allowed as part of the MPI machinery. Then there will not only be a new system, as outlined above, but additionally some existing systems will undergo cascade effects, and be copied down with changed kinematics.

          In this subsection we outline the possibility to interrupt at a given pT scale, in the next to interrupt after a given number of emissions.

          virtual bool UserHooks::canVetoPT()  
          In the base class this method returns false. If you redefine it to return true then the method doVetoPT(...) will interrupt the downward evolution at scaleVetoPT().

          virtual double UserHooks::scaleVetoPT()  
          In the base class this method returns 0. You should redefine it to return the pT scale at which you want to study the event.

          virtual bool UserHooks::doVetoPT(int iPos, const Event& event)  
          can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next().
          argument iPos : is the position/status when the routine is called, information that can help you decide your course of action:
          argumentoption 0 : when no MPI, ISR or FSR occurred above the veto scale;
          argumentoption 1 : when inside the interleaved MPI + ISR + FSR evolution, after an MPI process;
          argumentoption 2 : when inside the interleaved MPI + ISR + FSR evolution, after an ISR emission;
          argumentoption 3 : when inside the interleaved MPI + ISR + FSR evolution, after an FSR emission;
          argumentoption 4 : for the optional case where FSR is deferred from the interleaved evolution and only considered separately afterward (then alternative 3 would never occur);
          argumentoption 5 : is for subsequent resonance decays, and is called once for each decaying resonance in a chain such as t -> b W, W -> u dbar.
          argument event : the event record contains a list of all partons generated so far, also including intermediate ones not part of the "current final state", and also those from further multiparton interactions. This may not be desirable for comparisons with matrix-element calculations. You may want to make use of the subEvent(...) method below to obtain a simplified event record workEvent.

          (iii) Interrupt during the parton-level evolution, after a step

          These options are closely related to the ones above in section (ii), so we do not repeat the introduction, nor the possibilities to study the event record, also by using subEvent(...) and workEvent. What is different is that the methods in this section give access to the event as it looks like after each of the first few steps in the downwards evolution, irrespective of the pT scales of these branchings. Furthermore, it is here assumed that the focus normally is on the hardest subprocess, so that ISR/FSR emissions associated with additional MPI's are not considered. For MPI studies, however, a separate simpler alternative is offered to consider the event after a given number of interactions.

          virtual bool UserHooks::canVetoStep()  
          In the base class this method returns false. If you redefine it to return true then the method doVetoStep(...) will interrupt the downward ISR and FSR evolution the first numberVetoStep() times.

          virtual int UserHooks::numberVetoStep()  
          Returns the number of steps n each of ISR and FSR, for the hardest interaction, that you want to be able to study. That is, the method will be called after the first n ISR emissions, irrespective of the number of FSR ones at the time, and after the first n FSR emissions, irrespective of the number of ISR ones. The number of steps defaults to the first one only, but you are free to pick another value. Note that double diffraction is handled as two separate Pomeron-proton collisions, and thus has two sequences of emissions.

          virtual bool UserHooks::doVetoStep(int iPos, int nISR, int nFSR, const Event& event)  
          can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next().
          argument iPos : is the position/status when the routine is called, information that can help you decide your course of action. Agrees with options 2 - 5 of the doVetoPT(...) routine above, while options 0 and 1 are not relevant here.
          argument nISR : is the number of ISR emissions in the hardest process so far. For resonance decays, iPos = 5, it is 0.
          argument nFSR : is the number of FSR emissions in the hardest process so far. For resonance decays, iPos = 5, it is the number of emissions in the currently studied system.
          argument event : the event record contains a list of all partons generated so far, also including intermediate ones not part of the "current final state", and also those from further multiparton interactions. This may not be desirable for comparisons with matrix-element calculations. You may want to make use of the subEvent(...) method above to obtain a simplified event record.

          virtual bool UserHooks::canVetoMPIStep()  
          In the base class this method returns false. If you redefine it to return true then the method doVetoMPIStep(...) will interrupt the downward MPI evolution the first numberVetoMPIStep() times.

          virtual int UserHooks::numberVetoMPIStep()  
          Returns the number of steps in the MPI evolution that you want to be able to study, right after each new step has been taken and the subcollision has been added to the event record. The number of steps defaults to the first one only, but you are free to pick another value. Note that the hardest interaction of an events counts as the first multiparton interaction. For most hard processes it thus at the first step offers nothing not available with the VetoProcessLevel functionality above. For the minimum-bias and diffractive systems the hardest interaction is not selected at the process level, however, so there a check after the first multiparton interaction offers new functionality. Note that double diffraction is handled as two separate Pomeron-proton collisions, and thus has two sequences of interactions. Also, if you have set up a second hard process then a check is made after these first two, and the first interaction coming from the MPI machinery would have sequence number 3.

          virtual bool UserHooks::doVetoMPIStep(int nMPI,const Event& event)  
          can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the event, true, or let it continue to evolve, false. If you veto, then this event is not counted among the accepted ones, and does not contribute to the estimated cross section. The Pytha::next() method will begin a completely new event, so the vetoed event will not appear in the output of Pythia::next().
          argument nMPI : is the number of MPI subprocesses has occurred so far.
          argument event : the event record contains a list of all partons generated so far, also including intermediate ones not part of the "current final state", e.g. leftovers from the ISR and FSR evolution of previously generated systems. The most recently added one has not had time to radiate, of course.

          (iv) Veto emissions

          The methods in this group are intended to allow the veto of an emission in ISR, FSR or MPI, without affecting the evolution in any other way. If an emission is vetoed, the event record is "rolled back" to the way it was before the emission occurred, and the evolution in pT is continued downwards from the rejected value. The decision can be based on full knowledge of the kinematics of the shower branching or MPI.

          To identify where shower emissions originated, the ISR/FSR veto routines are passed the system from which the radiation occurred, according to the Parton Systems class (see ";?>Advanced Usage). Note, however, that inside the veto routines only the event record has been updated; all other information, including the Parton Systems, reflects the event before the shower branching or MPI has taken place.

          virtual bool UserHooks::canVetoISREmission()  
          In the base class this method returns false. If you redefine it to return true then the method doVetoISREmission(...) will interrupt the initial-state shower immediately after each emission and allow that emission to be vetoed.

          virtual bool UserHooks::doVetoISREmission( int sizeOld, const Event& event, int iSys)  
          can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the emission, true, or not, false. If you veto, then the latest emission is removed from the event record. In either case the evolution of the shower will continue from the point where it was left off.
          argument sizeOld : is the size of the event record before the latest emission was added to it. It will also become the new size if the emission is vetoed.
          argument event : the event record contains a list of all partons generated so far. Of special interest are the ones associated with the most recent emission, which are stored in entries from sizeOld through event.size() - 1 inclusive. If you veto the emission these entries will be removed, and the history info in the remaining partons will be restored to a state as if the emission had never occurred.
          argument iSys : the system where the radiation occurs, according to Parton Systems.

          virtual bool UserHooks::canVetoFSREmission()  
          In the base class this method returns false. If you redefine it to return true then the method doVetoFSREmission(...) will interrupt the final-state shower immediately after each emission and allow that emission to be vetoed.

          virtual bool UserHooks::doVetoFSREmission( int sizeOld, const Event& event, int iSys, bool inResonance = false)  
          can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the emission, true, or not, false. If you veto, then the latest emission is removed from the event record. In either case the evolution of the shower will continue from the point where it was left off.
          argument sizeOld : is the size of the event record before the latest emission was added to it. It will also become the new size if the emission is vetoed.
          argument event : the event record contains a list of all partons generated so far. Of special interest are the ones associated with the most recent emission, which are stored in entries from sizeOld through event.size() - 1 inclusive. If you veto the emission these entries will be removed, and the history info in the remaining partons will be restored to a state as if the emission had never occurred.
          argument iSys : the system where the radiation occurs, according to Parton Systems.
          argument inResonance : true if the emission takes place in a resonance decay, subsequent to the hard process.

          virtual bool UserHooks::canVetoMPIEmission()  
          In the base class this method returns false. If you redefine it to return true then the method doVetoMPIEmission(...) will interrupt the MPI machinery immediately after each multiparton interaction and allow it to be vetoed.

          virtual bool UserHooks::doVetoMPIEmission( int sizeOld, const Event& event)  
          can optionally be called, as described above. You can study, but not modify, the event event record of the partonic process. Based on that you can decide whether to veto the MPI, true, or not, false. If you veto, then the latest MPI is removed from the event record. In either case the interleaved evolution will continue from the point where it was left off.
          argument sizeOld : is the size of the event record before the latest MPI was added to it. It will also become the new size if the MPI is vetoed.
          argument event : the event record contains a list of all partons generated so far. Of special interest are the ones associated with the most recent MPI, which are stored in entries from sizeOld through event.size() - 1 inclusive. If you veto the MPI these entries will be removed.

          (v) Modify cross-sections or phase space sampling

          This section addresses two related but different topics. In both cases the sampling of events in phase space is modified, so that some regions are more populated while others are depleted. In the first case, this is assumed to be because the physical cross section should be modified relative to the built-in Pythia form. Therefore not only the relative population of phase space is changed, but also the integrated cross section of the process. In the second case the repopulation is only to be viewed as a technical trick to sample some phase-space regions better, so as to reduce the statistical error. There each event instead obtains a compensating weight, the inverse of the differential cross section reweighting factor, in such a way that the integrated cross section is unchanged. Below these two cases are considered separately, but note that they share many points.

          virtual bool UserHooks::canModifySigma()  
          In the base class this method returns false. If you redefine it to return true then the method multiplySigmaBy(...) will allow you to modify the cross section weight assigned to the current event.

          virtual double UserHooks::multiplySigmaBy(const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool inEvent)  
          when called this method should provide the factor by which you want to see the cross section weight of the current event modified. If you return unity then the normal cross section is obtained. Note that, unlike the methods above, these modifications do not lead to a difference between the number of "selected" events and the number of "accepted" ones, since the modifications occur already before the "selected" level. The integrated cross section of a process is modified, of course. Note that the cross section is only modifiable for normal hard processes. It does not affect the cross section in further multiparton interactions, nor in elastic/diffractive/minimum-bias events.
          argument sigmaProcessPtr, phaseSpacePtr : : what makes this routine somewhat tricky to write is that the hard-process event has not yet been constructed, so one is restricted to use the information available in the phase-space and cross-section objects currently being accessed. Which of their methods are applicable depends on the process, in particular the number of final-state particles. The multiplySigmaBy code in UserHooks.cc contains explicit instructions about which methods provide meaningful information, and so offers a convenient starting point.
          argument inEvent : : this flag is true when the method is called from within the event-generation machinery and false when it is called at the initialization stage of the run, when the cross section is explored to find a maximum for later Monte Carlo usage. Cross-section modifications should be independent of this flag, for consistency, but if multiplySigmaBy(...) is used to collect statistics on the original kinematics distributions before cuts, then it is important to be able to exclude the initialization stage from comparisons.

          One derived class is supplied as an example how this facility can be used to reweight cross sections in the same spirit as is done with QCD cross sections for the minimum-bias/underlying-event description:

          class  SuppressSmallPT : public UserHooks  
          suppress small-pT production for 2 -> 2 processes only, while leaving other processes unaffected. The basic suppression factor is pT^4 / ((k*pT0)^2 + pT^2)^2, where pT refers to the current hard subprocess and pT0 is the same energy-dependent dampening scale as used for ";?>multiparton interactions. This class contains canModifySigma() and multiplySigmaBy() methods that overload the base class ones.

          SuppressSmallPT::SuppressSmallPT( double pT0timesMPI = 1., int numberAlphaS = 0, bool useSameAlphaSasMPI = true)  
          The optional arguments of the constructor provides further variability.
          argument pT0timesMPI : corresponds to the additional factor k in the above formula. It is by default equal to 1 but can be used to explore deviations from the expected value.
          argument numberAlphaS : if this number n is bigger than the default 0, the corresponding number of alpha_strong factors is also reweighted from the normal renormalization scale to a modified one, i.e. a further suppression factor ( alpha_s((k*pT0)^2 + Q^2_ren) / alpha_s(Q^2_ren) )^n is introduced.
          argument useSameAlphaSasMPI : regulates which kind of new alpha_strong value is evaluated for the numerator in the above expression. It is by default the same as set for multiparton interactions (i.e. same starting value at M_Z and same order of running), but if false instead the one for hard subprocesses. The denominator alpha_s(Q^2_ren) is always the value used for the "original", unweighted cross section.

          The second main case of the current section involves three methods, as follows.

          virtual bool UserHooks::canBiasSelection()  
          In the base class this method returns false. If you redefine it to return true then the method biasSelectionBy(...) will allow you to modify the phase space sampling, with a compensating event weight, such that the cross section is unchanged. You cannot combine this kind of reweighting with the selection of ";?>a second hard process.

          virtual double UserHooks::biasSelectionBy(const SigmaProcess* sigmaProcessPtr, const PhaseSpace* phaseSpacePtr, bool inEvent)  
          when called this method should provide the factor by which you want to see the phase space sampling of the current event modified. Events are assigned a weight being the inverse of this, such that the integrated cross section of a process is unchanged. Note that the selection is only modifiable for normal hard processes. It does not affect the selection in further multiparton interactions, nor in elastic/diffractive/minimum-bias events.
          argument sigmaProcessPtr, phaseSpacePtr : : what makes this routine somewhat tricky to write is that the hard-process event has not yet been constructed, so one is restricted to use the information available in the phase-space and cross-section objects currently being accessed. Which of their methods are applicable depends on the process, in particular the number of final-state particles. The biasSelectionBy code in UserHooks.cc contains explicit instructions about which methods provide meaningful information, and so offers a convenient starting point.
          argument inEvent : : this flag is true when the method is called from within the event-generation machinery and false when it is called at the initialization stage of the run, when the cross section is explored to find a maximum for later Monte Carlo usage. Cross-section modifications should be independent of this flag, for consistency, but if biasSelectionBy(...) is used to collect statistics on the original kinematics distributions before cuts, then it is important to be able to exclude the initialization stage from comparisons.

          virtual double UserHooks::biasedSelectionWeight()  
          Returns the weight you should assign to the event, to use e.g. when you histogram results. It is the exact inverse of the weight you used to modify the phase-space sampling, a weight that must be stored in the selBias member variable, such that this routine can return 1/selBias. The weight is also returned by the Info::weight() method, which may be more convenient to use.

          (vi) Reject the decay sequence of resonances

          Resonance decays are performed already at the process level, as an integrated second step of the hard process itself. One reason is that the matrix element of many processes encode nontrivial decay angular distributions. Another is to have equivalence with Les Houches input, where resonance decays typically are provided from the onset. The methods in this section allow you to veto that decay sequence and try a new one. Unlike the veto of the whole process-level step, in point (i), the first step of the hard process is retained, i.e. where the resonances are produced. For this reason the cross section is not affected here but, depending on context, you may want to introduce your own counters to check how often a new set of decay modes and kinematics is selected, and correct accordingly.

          The main method below is applied after all decays. For the production of a t tbar pair this typically means after four decays, namely those of the t, the tbar, the W+ and the W-. If Les Houches events are processed, the rollback is to the level of the originally read events. For top, that might mean either to the tops, or to the W bosons, or no rollback at all, depending on how the process generation was set up.

          virtual bool UserHooks::canVetoResonanceDecays()  
          In the base class this method returns false. If you redefine it to return true then the method doVetoResonanceDecays(...) will be called immediately after the resonance decays have been selected and stored in the process event record, as described above for canVetoProcessLevel().

          virtual bool UserHooks::doVetoResonanceDecays(Event& process)  
          can optionally be called, as described above. You can study the process event record of the hard process. Based on that you can decide whether to reject the sequence of resonance decays that was not already fixed by the production step of the hard process (which can vary depending on how a process has been set up, see above). If you veto, then a new resonance decay sequence is selected, but the production step remains unchanged. The cross section remains unaffected by this veto, for better or worse.
          Warning: Normally you should not modify the process event record. However, as an extreme measure, parts or the complete decay chain could be overwritten. If so, be very careful.

          (vii) Modify scale in shower evolution

          The choice of maximum shower scale in resonance decays is normally not a big issue, since the shower here is expected to cover the full phase space. In some special cases a matching scheme is intended, where hard radiation is covered by matrix elements, and only softer by showers. The below two methods support such an approach. Note that the two methods are not used in the TimeShower class itself, but when showers are called from the PartonLevel generation. Thus user calls directly to TimeShower are not affected.

          virtual bool UserHooks::canSetResonanceScale()  
          In the base class this method returns false. If you redefine it to return true then the method scaleResonance(...) will set the initial scale of downwards shower evolution.

          virtual double UserHooks::scaleResonance( int iRes, const Event& event)  
          can optionally be called, as described above. You should return the maximum scale, in GeV, from which the shower evolution will begin. The base class method returns 0, i.e. gives no shower evolution at all. You can study, but not modify, the event event record of the partonic process to check which resonance is decaying, and into what.
          argument iRes : is the location in the event record of the resonance that decayed to the particles that now will shower.
          argument event : the event record contains a list of all partons generated so far, specifically the decaying resonance and its immediate decay products. pythia8-8.1.80.orig/phpdoc/ParticleDataScheme.php0000644000175000017500000021277212217615312020014 0ustar sunsun The Particle Data Scheme SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          The Particle Data Scheme

          The particle data scheme may take somewhat longer to understand than the settings one. In particular the set of methods to access information is rather more varied, to allow better functionality for advanced usage. However, PYTHIA does come with a sensible default set of particle properties and decay tables. Thus there is no need to learn any of the methods on this page to get going. Only when you perceive a specific need does it make sense to learn the basics.

          The central section on this page is the Operation one. The preceding sections are there mainly to introduce the basic structure and the set of properties that can be accessed. The subsequent sections provide a complete listing of the existing public methods, which most users probably will have little interaction with.

          Databases

          The management of particle data is based on three classes:
          • ParticleData, which is the top-level class, with methods that can be used to interrogate all particle data. It contains a map of PDG particle identity numbers [Yao06] onto the relevant ParticleDataEntry objects,
          • ParticleDataEntry, which stores the relevant information on an individual particle species, and
          • DecayChannel, which stores info on one particular decay mode of a particle.
          The objects of these classes together form a database that is continuously being used as the program has to assign particle masses, select decay modes, etc.

          Each Pythia object has a public member particleData of the ParticleData class. Therefore you access the particle data methods as pythia.particleData.command(argument), assuming that pythia is an instance of the Pythia class. Further, for some of the most frequent user tasks, Pythia methods have been defined, so that pythia.command(argument) would work, see further below.

          A fundamental difference between the particle data classes and the settings ones is that the former are accessed regularly during the event generation process, as a new particle is produced and its mass need to be set, e.g., while the latter are mainly/only used at the initialization stage. Nevertheless, it is not a good idea to change data in either of them in mid-run, since this may lead to inconsistencies.

          Stored properties for particles

          The main properties stored for each particle are as follows. Different ways to set and get these properties will be described further down.
          • name: a character string with the name of the particle. Particle and antiparticle names are stored separately, with void returned when no antiparticle exists.
          • spinType: the spin type, of the form 2 s + 1, with special code 0 for entries of unknown or indeterminate spin.
          • chargeType: three times the charge (to make it an integer).
          • colType: the colour type, with 0 uncoloured, 1 triplet, -1 antitriplet and 2 octet. (A preliminary implementation of colour sextets, available since version 8.150, further uses 3 for a sextet and -3 for an antisextet.)
          • m0: the nominal mass m_0 (in GeV).
          • mWidth: the width Gamma of the Breit-Wigner distribution (in GeV).
          • mMin: the lower limit of the allowed mass range generated by the Breit-Wigner (in GeV). Has no meaning for particles without width, and would typically be 0 there.
          • mMax: the upper limit of the allowed mass range generated by the Breit-Wigner (in GeV). If mMax < mMin then no upper limit is imposed. Has no meaning for particles without width, and would typically be 0 there.
          • tau0: the nominal proper lifetime tau_0 (in mm/c).
          • isResonance: a flag telling whether a particle species is considered as a resonance or not. Here ";?>"resonance" is used as shorthand for any massive particle where the decay process should be counted as part of the hard process itself, and thus be performed before showers and other event aspects are added. Restrictions on allowed decay channels is also directly reflected in the cross section of simulated processes, while those of normal hadrons and other light particles are not. In practice, it is reserved for states above the b bbar bound systems in mass, i.e. for W, Z, t, Higgs states, supersymmetric states and (most?) other states in any new theory. All particles with m0 above 20 GeV are by default initialized to be considered as resonances.
          • mayDecay: a flag telling whether a particle species may decay or not, offering the main user switch. Whether a given particle of this kind then actually will decay also depends on it having allowed decay channels, and on other flags for ";?>particle decays (or ";?>resonance decays). All particles with tau0 below 1000 mm are by default initialized to allow decays.
          • doExternalDecays: a flag telling whether a particle should be handled by an external decay package or not, with the latter default. Can be manipulated as described on this page, but should normally not be. Instead the ";?>Pythia::decayPtr(...) method should be provided with the list of relevant particles.
          • isVisible: a flag telling whether a particle species is to be considered as visible in a detector or not, as used e.g. in analysis routines. By default this includes neutrinos and a few BSM particles (gravitino, sneutrinos, neutralinos) that have neither strong nor electromagnetic charge, and are not made up of constituents that have it. The value of this flag is only relevant if a particle is long-lived enough actually to make it to a detector.
          • doForceWidth: a flag valid only for resonances where PYTHIA contains code to calculate the width of the resonance from encoded matrix-element expressions, i.e. the Z^0, W^+-, t, h^0, and a few more. The normal behaviour (false) is then that the width is calculated from the mass, but it is possible to ";?>force the resonance to retain the nominal width. Branching ratios and the running of the total width are unaffected.

          Stored properties for decays

          An unstable particle has a decay table consisting of one or more decay channel. The following properties are stored for each such channel. Again different ways to set and get these properties will be described further down.
          • onMode: integer code for use or not of channel,
            0 if a channel is off,
            1 if on,
            2 if on for a particle but off for an antiparticle,
            3 if on for an antiparticle but off for a particle.
            If a particle is its own antiparticle then 2 is on and 3 off but, of course, for such particles it is much simpler and safer to use only 1 and 0.
            The 2 and 3 options can be used e.g. to encode CP violation in B decays, or to let the W's in a q qbar -> W^+ W^- process decay in different channels.
          • bRatio: the branching ratio of the channel (with some reservations for resonances, see meMode below).
          • meMode: the mode of processing this channel, possibly with matrix elements; see the ";?>particle decays and ";?>resonance decays descriptions for the list of possibilities. Notably the default code 0 for a particle means pure phase space decays according to the given branching ratios, while for a resonance it means that code exists for the dynamic calculations of partial widths and thereby branching ratios as a function of the resonance mass (which is done e.g. at initialization based on the mass set by the user). Then codes 1 - 99 are reserved for various matrix-element-improved ordinary particle decays, and 100 - 103 for resonances where the partial width of a given channel is calculated from the total width and the stored branching ratio. Thus, to enforce a new branching ratio for a resonance channel (with its own partial-width calculation code) it is not sufficient only to change the bRatio but also to set e.g. meMode = 100.
          • multiplicity: the number of decay products of the channel. Can be at most 8.
          • product(i): the identity code of the decay products, where i runs between 0 and multiplicity - 1. Trailing positions are filled with 0.

          Operation

          The normal flow of the particle data operations is:
          1. When a Pythia object pythia is created, the pythia.particleData member is asked to scan the ParticleData.xml file.

            All lines beginning with <particle are scanned for information on a particle species, and all lines beginning with <channel are assumed to contain a decay channel of the enclosing particle. In both cases XML syntax is used, with attributes used to identify the stored properties, and with omitted properties defaulting back to 0 where meaningful. The particle and channel information may be split over several lines, up to the > endtoken. The format of a <particle tag is:

                <particle id="..." name="..." antiName="..." spinType="..." chargeType="..." colType="..." 
                   m0="..." mWidth="..." mMin="..." mMax="..." tau0="...">
                </particle>
            
            where the fields are the properties already introduced above. Note that isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth are not set here, but are provided with default values by the rules described above. Once initialized, also these latter properties can be changed, see below.
            The format of a <channel> tag is:
                <channel onMode="..." bRatio="..." meMode="..." products="..." />
            
            again see properties above. The products are given as a blank-separated list of id codes.
            Important: the values in the .xml file should not be changed, except by the PYTHIA authors. Any changes should be done with the help of the methods described below.
          2. Between the creation of the Pythia object and the init call for it, you may use the methods of the ParticleData class to modify some of the default values. Several different approaches can be chosen for this.

            a) Inside your main program you can directly set values with

                pythia.readString(string);
            
            where both the variable name and the value are contained inside the character string, separated by blanks and/or a =, e.g.
                pythia.readString("111:mayDecay = off"); 
            
            switches off the decays of the pi^0.
            The particle id (> 0) and the property to be changed must be given, separated by a colon.
            The allowed properties are: name, antiName, spinType, chargeType, colType, m0, mWidth, mMin, mMax, tau0, isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth. All of these names are case-insensitive. Names that do not match an existing variable are ignored.
            Strings beginning with a non-alphanumeric character, like # or !, are assumed to be comments and are not processed at all. For bool values, the following notation may be used interchangeably: true = on = yes = ok = 1, while everything else gives false (including but not limited to false, off, no and 0).

            Particle data often comes in sets of closely related information. Therefore some properties expect the value to consist of several numbers. These can then be separated by blanks (or by commas). A simple example is names, which expects both the name and antiname to be given. A more interesting one is the all property,

              
                id:all = name antiName spinType chargeType colType m0 mWidth mMin mMax tau0
            
            where all the current information on the particle itself is replaced, but any decay channels are kept unchanged. Using new instead of all also removes any previous decay channels. If the string contains fewer fields than expected the trailing properties are set to vanish ("void", 0 or 0.). Note that such a truncated string should not be followed by a comment, since this comment would then be read in as if it contained the missing properties. The truncation can be done anywhere, specifically a string with only id:new defines a new "empty" particle. As before, isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth are (re)set to their default values, and would have to be changed separately if required.

            A further command is rescaleBR, which rescales each of the existing branching ratios with a common factor, such that their new sum is the provided value. This may be a first step towards adding new decay channels, see further below.

            Alternatively the id code may be followed by another integer, which then gives the decay channel number. This then has to be followed by the property specific to this channel, either onMode, bRatio, meMode or products. In the latter case all the products of the channel should be given:

                id:channel:products =  product1 product2 ....  
            
            The line will be scanned until the end of the line, or until a non-number word is encountered, or until the maximum allowed number of eight products is encountered, whichever happens first. (Thus the multiplicity of a decay channel need not be input; it is automatically calculated from the products list.) It is also possible to replace all the properties of a channel in a similar way:
                id:channel:all = onMode bRatio meMode product1 product2 ....  
            
            To add a new channel at the end, use
                id:addChannel = onMode bRatio meMode product1 product2 ....
            

            It is currently not possible to remove a channel selectively, but setting its branching ratio vanishing is as effective. If you want to remove all existing channels and force decays into one new channel you can use

                id:oneChannel = onMode bRatio meMode product1 product2 ....
            
            A first oneChannel command could be followed by several subsequent addChannel ones, to build up a completely new decay table for an existing particle.

            When adding new channels or changing branching ratios in general, note that, once a particle is to be decayed, the sum of branching ratios is always rescaled to unity. Beforehand, rescaleBR may be used to rescale an existing branching ratio by the given factor.

            There are a few commands that will study all the decay channels of the given particle, to switch them on or off as desired. The

                id:onMode = onMode
            
            will set the onMode property of all channels to the desired value. The
             
                id:offIfAny   = product1 product2 .... 
                id:onIfAny    = product1 product2 .... 
                id:onPosIfAny = product1 product2 .... 
                id:onNegIfAny = product1 product2 .... 
            
            will set the onMode 0, 1, 2 or 3, respectively, for all channels which contain any of the enumerated products, where the matching to these products is done without distinction of particles and antiparticles. Note that "Pos" and "Neg" are slightly misleading since it refers to the particle and antiparticle of the id species rather than charge, but should still be simpler to remember and understand than alternative notations. Correspondingly
             
                id:offIfAll   = product1 product2 .... 
                id:onIfAll    = product1 product2 .... 
                id:onPosIfAll = product1 product2 .... 
                id:onNegIfAll = product1 product2 .... 
            
            will set the onMode 0, 1, 2 or 3, respectively, for all channels which contain all of the enumerated products, again without distinction of particles and antiparticles. If the same product appears twice in the list it must also appear twice in the decay channel, and so on. The decay channel is allowed to contain further particles, beyond the product list. By contrast,
             
                id:offIfMatch   = product1 product2 .... 
                id:onIfMatch    = product1 product2 .... 
                id:onPosIfMatch = product1 product2 .... 
                id:onPosIfMatch = product1 product2 .... 
            
            requires the decay-channel multiplicity to agree with that of the product list, but otherwise works as the onIfAll/offIfAll methods.

            Note that the action of several of the commands depends on the order in which they are executed, as one would logically expect. For instance, id:oneChannel removes all decay channels of id and thus all previous changes in this decay table, while subsequent additions or changes would still take effect. Another example would be that 23:onMode = off followed by 23:onIfAny = 1 2 3 4 5 would let the Z^0 decay to quarks, while no decays would be allowed if the order were to be reversed.

            b) The Pythia readString(string) method actually does not do changes itself, but sends on the string either to the ParticleData class or to the Settings one, depending on whether the string begins with a digit or a letter. If desired, it is possible to communicate directly with the corresponding ParticleData method:

                pythia.particleData.readString("111:mayDecay = off"); 
                pythia.particleData.readString("15:2:products = 16 -211"); 
            
            In this case, changes intended for Settings would not be understood.

            c) Underlying this are commands for all the individual properties in the ParticleData class, one for each. These are further described below. Thus, an example now reads

                pythia.particleData.mayDecay(111, false);
            
            Boolean values should here be given as true or false.

            d) A simpler and more useful way is to collect all your changes in a separate file, with one line per change, e.g.

                111:mayDecay = off
            
            The file can be read by the
                pythia.readFile(fileName); 
            
            method, where fileName is a string, e.g. pythia.readFile("main.cmnd") (or an istream instead of a fileName). Each line is processed as described for the string in 2a). This file can freely mix commands to the Settings and ParticleData classes.
          3. A routine reInit(fileName) is provided, and can be used to zero the particle data table and reinitialize it from scratch. Such a call might be useful if several subruns are to be made with widely different particle data - normally the maps are only built from scratch once, namely when the Pythia() object is created. Also, there is no other possibility to restore the default values, unlike for the settings.

          4. You may at any time obtain a listing of all the particle data by calling

                pythia.particleData.listAll();
            
            The listing is by increasing id number. It shows the basic quantities introduced above. Some are abbreviated in the header to fit on the lines: spn = spinType, chg = chargeType, col = colType, res = isResonance, dec = mayDecay && canDecay (the latter checks that decay channels have been defined), ext = doExternalDecay, vis = isVisible and wid = doForceWidth.
            To list only those particles that were changed (one way or another, the listing will not tell what property or decay channel was changed), instead use
                pythia.particleData.listChanged();
            
            (This info is based on a further hasChanged flag of a particle or a channel, set true whenever any of the changing methods are used. It is possible to manipulate this value, but this is not recommended.) By default the internal initialization of the widths of resonances such as gamma^*/Z^0, W^+-, t/tbar, H^0 do not count as changes; if you want to list also those changes instead call listChanged(true).
            To list only one particle, give its id code as argument to the list(...) function.. To list a restricted set of particles, give in their id codes to list(...) as a vector<int>.
          5. For wholesale changes of particle properties all available data can be written out, edited, and then read back in again. These methods are mainly intended for expert users. You can choose between two alternative syntaxes.

            a) XML syntax, using the <particle and <channel lines already described. You use the method particleData.listXML(fileName) to produce such an XML file and particleData.readXML(fileName) to read it back in after editing.

            b) Fixed/free format, using exactly the same information as illustrated for the <particle and <channel lines above, but now without any tags. This means that all information fields must be provided (if there is no antiparticle then write void), in the correct order (while the order is irrelevant with XML syntax), and all on one line. Information is written out in properly lined-up columns, but the reading is done using free format, so fields need only be separated by at least one blank. Each new particle is supposed to be separated by (at least) one blank line, whereas no blank lines are allowed between the particle line and the subsequent decay channel lines, if any. You use the method particleData.listFF(fileName) to produce such a fixed/free file and particleData.readFF(fileName) to read it back in after editing.

            As an alternative to the readXML and readFF methods you can also use the particleData.reInit(fileName, xmlFormat) method, where xmlFormat = true (default) corresponds to reading an XML file and xmlFormat = false to a fixed/free format one.

            To check that the new particle and decay tables makes sense, you can use the particleData.checkTable() method, either directly or by switching it on among the standard ";?>error checks.

          The public methods

          In the following we present briefly the public methods in the three classes used to build up the particle database. The order is top-down, i.e from the full table of all particles to a single particle to a single channel. Note that these methods usually are less elegant and safe than the input methods outlined above. If you use any of these methods, it is likely to be the ones in the full database, i.e. the first ones to be covered in the following.

          For convenience, we have grouped related input and output methods together. It should be obvious from the context which is which: the input is of type void and has an extra last argument, namely is the input value, while the output method returns a quantity of the expected type.

          The ParticleData methods

          ParticleData::ParticleData()  
          the constructor has no arguments and does not do anything. Internal.

          void ParticleData::initPtr(Info* infoPtr,Settings* settingsPtrIn, Rndm* rndmPtrIn, CoupSM* coupSMPtrIn)  
          initialize pointers to a few other classes. Internal.

          bool ParticleData::init(string startFile = "../xmldoc/ParticleData.xml")  
          read in an XML-style file with particle data and initialize the particle data tables accordingly. This command is executed in the Pythia constructor, i.e. is mainly for internal use.
          argument startFile (default = ../xmldoc/ParticleData.xml) : the name of the data file to be read. When called from the Pythia constructor the directory is provided by the ";?>PYTHIA8DATA environment variable, if set, else by the argument of this constructor, which has the default value "../xmldoc".

          bool ParticleData::reInit(string startFile,bool xmlFormat = true)  
          overwrite the existing database by reading from the specified file. Unlike init above this method is not called by the Pythia constructor, but is entirely intended for users who want to replace the existing particle data with their own.
          argument startFile : the path and name of file to be read.
          argument xmlFormat : if true read the same kind of XML-style file as used by init, if not use an alternative "free format" file (i.e. without any XML tags, but with well-defined rules specifying in which order properties are stored).

          void ParticleData::initWidths(vector<ResonanceWidths*> resonancePtrs)  
          initialize Breit-Wigner shape parameters for all particles, and the detailed handling of resonances, i.e. particles with perturbatively calculable partial widths, which can be used to obtain a mass-dependent Breit-Wigner and a dynamic choice of decay channels. Called from Pythia::init().

          bool ParticleData::readXML(string inFile, bool reset = true)  
          void ParticleData::listXML(string outFile)  
          read in XML-style data from a file or write it out to a file. For the former one can also decide whether to reset all particles to scratch, or only overwrite those particles in the file. The former method is used by init and reInit above.

          bool ParticleData::readFF(string inFile, bool reset = true)  
          void ParticleData::listFF(string outFile)  
          read in free-format-style data from a file or write it out to a file. For the former one can also decide whether to reset all particles to scratch, or only overwrite those particles in the file. The former method is used by reInit above.

          bool ParticleData::readString(string line, bool warn = true, ostream& os = cout)  
          read in a string and interpret is as a new or changed particle data. The possibilities are extensively described above. It is normally used indirectly, via Pythia::readString(...) and Pythia::readFile(...).
          argument line : the string to be interpreted as an instruction.
          argument warn (default = true) : write a warning message or not whenever the instruction does not make sense, e.g. if the particle does not exist in the database.
          argument os (default = cout) : stream for error printout.
          Note: the method returns false if it fails to make sense out of the input string.

          void ParticleData::listAll(ostream& os = cout)  
          void ParticleData::listChanged(ostream& os = cout)  
          void ParticleData::listChangedAndRes(ostream& os = cout)  
          void ParticleData::list(bool changedOnly = false, bool changedRes = true, ostream& os = cout)  
          methods intended to present a listing of particle data in a readable format. The first three are special cases of the fourth. The first lists all particle data, the second only data for those particles that were changed after the original creation of the particle data table. Resonances are a special case since they can get their data changed by being linked to an object that does the calculation of branching ratios. The second method does not count such resonances as changed, whereas the third does and thus lists all resonances.

          void ParticleData::list(int idList, ostream& os = cout)  
          void ParticleData::list(vector<int> idList, ostream& os = cout)  
          list particle data for one single particle, with the identity code as input, or for a set of particles, with an input vector of identity codes.

          void ParticleData::checkTable(ostream& os = cout)  
          void ParticleData::checkTable(int verbosity,ostream& os = cout)  
          check that the particle decay table makes sense, especially for decays.
          argument verbosity : level of checks. 0 is only minimal, e.g. if a particle has no open decay channels. 1, which is the level of the first method, provides warning if any individual channel is closed, except for resonances. 2 also prints the branching-ratio-averaged threshold mass. 11 and 12 are like 1 and 2, but also include resonances in the detailed checks.

          void ParticleData::addParticle(int id, string name = " ", int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0., double tau0 = 0.)  
          void ParticleData::addParticle(int id, string name, string antiName, int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0., double tau0 = 0.)  
          add a particle to the decay table; in the first form a particle which is its own antiparticle, in the second where a separate antiparticle exists.

          void ParticleData::setAll(int id, string name, string antiName, int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0.,double tau0 = 0.)  
          change all the properties of the particle associated with a given identity code.

          bool ParticleData::isParticle(int id)  
          query whether the particle data table contains the particle of the identity code.

          int ParticleData::nextId(int id)  
          return the identity code of the sequentially next particle stored in table.

          bool ParticleData::hasAnti(int id)  
          bool whether a distinct antiparticle exists or not. Is true if an antiparticle name has been set (and is different from void).

          void ParticleData::name(int id, string name)  
          void ParticleData::antiName(int id, string antiName)  
          void ParticleData::names(int id, string name, string antiName)  
          string ParticleData::name(int id)  
          particle and antiparticle names are stored separately, the sign of id determines which of the two is returned, with void used to indicate the absence of an antiparticle.

          void ParticleData::spinType(int id, int spinType)  
          int ParticleData::spinType(int id)  
          the spin type, of the form 2 s + 1, with special code 0 for entries of unknown or indeterminate spin.

          void ParticleData::chargeType(int id, int chargeType)  
          int ParticleData::chargeType(int id)  
          three times the charge (to make it an integer), taking into account the sign of id.

          double ParticleData::charge(int id)  
          the electrical charge of a particle, equal to chargeType(id)/3.

          void ParticleData::colType(int id, int colType)  
          int ParticleData::colType(int id)  
          the colour type, with 0 uncoloured, 1 triplet, -1 antitriplet and 2 octet, taking into account the sign of id.

          void ParticleData::m0(int id, double m0)  
          double ParticleData::m0(int id)  
          the nominal mass m_0 (in GeV).

          void ParticleData::mWidth(int id, double mWidth)  
          double ParticleData::mWidth(int id)  
          the width Gamma of the Breit-Wigner distribution (in GeV).

          void ParticleData::mMin(int id, double mMin)  
          double ParticleData::mMin(int id)  
          the lower limit of the allowed mass range generated by the Breit-Wigner (in GeV). Has no meaning for particles without width, and would typically be 0 there.

          void ParticleData::mMax(int id, double mMax)  
          double ParticleData::mMax(int id)  
          the upper limit of the allowed mass range generated by the Breit-Wigner (in GeV). If mMax < mMin then no upper limit is imposed. Has no meaning for particles without width, and would typically be 0 there.

          double ParticleData::m0Min(int id)  
          similar to mMin() above, except that for particles with no width the m0(id) value is returned.

          double ParticleData::m0Max(int id)  
          similar to mMax() above, except that for particles with no width the m0(id) value is returned.

          void ParticleData::tau0(int id, double tau0)  
          double ParticleData::tau0(int id)  
          the nominal proper lifetime tau_0 (in mm/c).

          void ParticleData::isResonance(int id, bool isResonance)  
          bool ParticleData::isResonance(int id)  
          a flag telling whether a particle species are considered as a resonance or not. Here ";?>"resonance" is used as shorthand for any massive particle where the decay process should be counted as part of the hard process itself, and thus be performed before showers and other event aspects are added. Restrictions on allowed decay channels is also directly reflected in the cross section of simulated processes, while those of normal hadrons and other light particles are not. In practice, it is reserved for states above the b bbar bound systems in mass, i.e. for W, Z, t, Higgs states, supersymmetric states and (most?) other states in any new theory. All particles with m0 above 20 GeV are by default initialized to be considered as resonances.

          void ParticleData::mayDecay(int id, bool mayDecay)  
          bool ParticleData::mayDecay(int id)  
          a flag telling whether a particle species may decay or not, offering the main user switch. Whether a given particle of this kind then actually will decay also depends on it having allowed decay channels, and on other flags for ";?>particle decays (or ";?>resonance decays). All particles with tau0 below 1000 mm are by default initialized to allow decays.

          void ParticleData::doExternalDecays(int id, bool doExternalDecays)  
          bool ParticleData::doExternalDecay(int id)  
          a flag telling whether a particle should be handled by an external decay package or not, with the latter default. Can be manipulated as described on this page, but should normally not be. Instead the ";?>pythia.decayPtr method should be provided with the list of relevant particles.

          void ParticleData::isVisible(int id, bool isVisible)  
          bool ParticleData::isVisible(int id)  
          a flag telling whether a particle species is to be considered as visible in a detector or not, as used e.g. in analysis routines. By default this includes neutrinos and a few BSM particles (gravitino, sneutrinos, neutralinos) that have neither strong nor electromagnetic charge, and are not made up of constituents that have it. The value of this flag is only relevant if a particle is long-lived enough actually to make it to a detector.

          void ParticleData::doForceWidth(int id, bool doForceWidth)  
          bool ParticleData::doForceWidth(int id)  
          a flag valid only for resonances where PYTHIA contains code to calculate the width of the resonance from encoded matrix-element expressions, i.e. the Z^0, W^+-, t, h^0, and a few more. The normal behaviour (false) is then that the width is calculated from the mass, but it is possible to ";?>force the resonance to retain the nominal width. Branching ratios and the running of the total width are unaffected.

          void ParticleData::hasChanged(int id, bool hasChanged)  
          bool ParticleData::hasChanged(int id)  
          keep track of whether the data for a particle has been changed in any respect between initialization and the current status. Is used e.g. by the listChanged method to determine which particles to list.

          bool ParticleData::useBreitWigner(int id)  
          tells whether a particle will have a Breit-Wigner mass distribution or not. Is determined by an internal logic based on the particle width and on the value of the ";?>ParticleData:modeBreitWigner switch.

          double ParticleData::constituentMass(int id)  
          is the constituent mass for a quark, hardcoded as m_u = m_d = 0.325, m_s = 0.50, m_c = 1.60 and m_b = 5.0 GeV, for a diquark the sum of quark constituent masses, and for everything else the same as the ordinary mass.

          double ParticleData::mSel(int id)  
          returns a mass distributed according to a truncated Breit-Wigner, with parameters as described here. Is equal to m0(id) for particles without width.

          double ParticleData::mRun(int id, double mH)  
          calculate the running mass of species id when probed at a hard mass scale of mH. Only applied to obtain the running quark masses; for all other particle the normal fixed mass is used.

          bool ParticleData::canDecay(int id)  
          true for a particle with at least one decay channel defined.

          bool ParticleData::isLepton(int id)  
          true for a lepton or an antilepton (including neutrinos).

          bool ParticleData::isQuark(int id)  
          true for a quark or an antiquark.

          bool ParticleData::isGluon(int id)  
          true for a gluon.

          bool ParticleData::isDiquark(int id)  
          true for a diquark or antidiquark.

          bool ParticleData::isParton()  
          true for a gluon, a quark or antiquark up to the b (but excluding top), and a diquark or antidiquark consisting of quarks up to the b.

          bool ParticleData::isHadron(int id)  
          true for a hadron (made up out of normal quarks and gluons, i.e. not for R-hadrons and other exotic states).

          bool ParticleData::isMeson(int id)  
          true for a meson.

          bool ParticleData::isBaryon(int id)  
          true for a baryon or antibaryon.

          bool ParticleData::isOctetHadron(int id)  
          true for an intermediate hadron-like state with a colour octet charge as used in the colour octet model for ";?>onia production.

          int ParticleData::heaviestQuark(int id)  
          extracts the heaviest quark or antiquark, i.e. one with largest id number, for a hadron.

          int ParticleData::baryonNumberType(int id)  
          is 1 for a quark, 2 for a diquark, 3 for a baryon, the same with a minus sign for antiparticles, and else zero.

          void ParticleData::rescaleBR(int id, double newSumBR = 1.)  
          rescales all partial branching ratios by a common factor, such that the sum afterward becomes newSumBR.

          void setResonancePtr(int id, ResonanceWidths* resonancePtr)  
          set a pointer for a particle kind to a ResonanceWidths object. This is done, from inside ParticleData::initWidths, only for resonances, i.e. for particles such as Z^0, W^+-, top, Higgs, and new unstable states beyond the Standard Model. The presence of such an object will allow a more dynamic calculation of partial and total widths, as illustrated by the following methods.

          void ParticleData::resInit(int id)  
          initialize the treatment of a resonance.

          double ParticleData::resWidth(int id, double mHat, int idInFlav = 0, bool openOnly = false, bool setBR = false)  
          calculate the total with for a resonance of a given current mass, optionally including coupling to incoming flavour state (consider the gamma*/Z^0 combination), optionally excluding decay channels that have been closed by the user, and optionally storing the results in the normal decay table.

          double ParticleData::resWidthOpen(int id, double mHat, int idInFlav = 0)  
          special case of resWidth, where only open channels are included, but results are not stored in the normal decay table.

          double ParticleData::resWidthStore(int id, double mHat, int idInFlav = 0)  
          special case of resWidth, where only open channels are included, and results are stored in the normal decay table.

          double ParticleData::resOpenFrac(int id1, int id2 = 0, int id3 = 0)  
          calculate the fraction of the full branching ratio that is left open by the user choice of allowed decay channels. Can be applied to a final state with up to three resonances. Since the procedure is multiplicative, it would be easy to generalize also to more.

          double ParticleData::resWidthRescaleFactor(int id)  
          the factor used to rescale all partial widths in case the total width is being forced to a specific value by the user.

          double ParticleData::resWidthChan(int id,double mHat, int idAbs1 = 0, int idAbs2 = 0)  
          special case to calculate one final-state width; currently only used for Higgs decay to q qbar, g g or gamma gamma.

          ParticleDataEntry* ParticleData::particleDataEntryPtr(int id)  
          returns a pointer to the ParticleDataEntry object. The methods in the next section can then be used to manipulate this object.

          The ParticleDataEntry methods

          Most of the methods that can be applied to a single ParticleDataEntry object are almost identical with those used above for the ParticleData, except that the id argument is no longer needed to find the right entry in the table. By and large, this makes direct access to the ParticleDataEntry methods superfluous. There are a few methods that are unique to each class, however. Furthermore, to avoid some naming ambiguities, many methods that set values begin with set.

          ParticleDataEntry::ParticleDataEntry(int id = 0, string name = " ", int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0., double tau0 = 0.)  
          ParticleDataEntry::ParticleDataEntry(int id, string name, string antiName, int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0., double tau0 = 0.)  
          there are two alternative constructors, that both expect the properties of a particle as input. The first assumes that there is only one particle, the latter that there is a particle-antiparticle pair (but if the antiparticle name is void one reverts back to the particle-only case).

          ParticleDataEntry::~ParticleDataEntry  
          the destructor is needed to delete any ResonanceWidths objects that have been created and linked to the respective particle.

          void ParticleDataEntry::setDefaults()  
          initialize some particle flags with default values, e.g. whether a particle is a resonance, may decay, or is visible. Is called from the constructors and from setAll.

          void ParticleDataEntry::initPtr(ParticleData* particleDataPtrIn)  
          initialize pointer back to the whole database (so that masses of decay products can be accessed, e.g.).

          void ParticleDataEntry::setAll( string name, string antiName, int spinType = 0, int chargeType = 0, int colType = 0, double m0 = 0., double mWidth = 0., double mMin = 0., double mMax = 0.,double tau0 = 0.)  
          change all the properties of the particle associated with a given identity code.

          int ParticleDataEntry::id()  
          the PDG identity code.

          bool ParticleDataEntry::hasAnti()  
          tell whether a separate antiparticle exists.

          void ParticleDataEntry::setName(string name)  
          void ParticleDataEntry::setAntiName(string antiName)  
          void ParticleDataEntry::setNames(string name,string antiName)  
          string ParticleDataEntry::name(int id = 1)  
          set or get the particle or antiparticle name. Only the sign of id is needed to distinguish particle/antiparticle.

          void ParticleDataEntry::setSpinType(int spinType)  
          int ParticleDataEntry::spinType()  
          set or get the particle spin type, i.e. 2 s + 1, or 0 in some special cases.

          void ParticleDataEntry::setChargeType(int chargeType)  
          int ParticleDataEntry::chargeType(int id = 1)  
          double ParticleDataEntry::charge(int id = 1)  
          set or get the particle charge type, i.e. three times the charge, or the charge itself. Only the sign of id is needed to distinguish particle/antiparticle.

          void ParticleDataEntry::setColType(int colType)  
          int ParticleDataEntry::colType(int id = 1)  
          set or get the particle colour type, 0 for singlet, 1 for triplet, -1 for antitriplet, 2 for octet. Only the sign of id is needed to distinguish particle/antiparticle.

          void ParticleDataEntry::setM0(double m0)  
          double ParticleDataEntry::m0()  
          the nominal mass m_0 (in GeV).

          void ParticleDataEntry::setMWidth(double mWidth)  
          double ParticleDataEntry::mWidth()  
          the width Gamma of the Breit-Wigner distribution (in GeV).

          void ParticleDataEntry::setMMin(double mMin)  
          double ParticleDataEntry::mMin()  
          the lower limit of the allowed mass range generated by the Breit-Wigner (in GeV). Has no meaning for particles without width, and would typically be 0 there.

          void ParticleDataEntry::setMMax(double mMax)  
          double ParticleDataEntry::mMax()  
          the upper limit of the allowed mass range generated by the Breit-Wigner (in GeV). If mMax < mMin then no upper limit is imposed. Has no meaning for particles without width, and would typically be 0 there.

          double ParticleDataEntry::m0Min()  
          similar to mMin() above, except that for particles with no width the m0(id) value is returned.

          double ParticleDataEntry::m0Max()  
          similar to mMax() above, except that for particles with no width the m0(id) value is returned.

          void ParticleDataEntry::setTau0(double tau0)  
          double ParticleDataEntry::tau0()  
          the nominal proper lifetime tau_0 (in mm/c).

          void ParticleDataEntry::setIsResonance(bool isResonance)  
          bool ParticleDataEntry::isResonance()  
          a flag telling whether a particle species are considered as a resonance or not. Here ";?>"resonance" is used as shorthand for any massive particle where the decay process should be counted as part of the hard process itself, and thus be performed before showers and other event aspects are added. Restrictions on allowed decay channels is also directly reflected in the cross section of simulated processes, while those of normal hadrons and other light particles are not. In practice, it is reserved for states above the b bbar bound systems in mass, i.e. for W, Z, t, Higgs states, supersymmetric states and (most?) other states in any new theory. All particles with m0 above 20 GeV are by default initialized to be considered as resonances.

          void ParticleDataEntry::setMayDecay(bool mayDecay)  
          bool ParticleDataEntry::mayDecay()  
          a flag telling whether a particle species may decay or not, offering the main user switch. Whether a given particle of this kind then actually will decay also depends on it having allowed decay channels, and on other flags for ";?>particle decays (or ";?>resonance decays). All particles with tau0 below 1000 mm are by default initialized to allow decays.

          void ParticleDataEntry::setDoExternalDecays(bool doExternalDecays)  
          bool ParticleDataEntry::doExternalDecay()  
          a flag telling whether a particle should be handled by an external decay package or not, with the latter default. Can be manipulated as described on this page, but should normally not be. Instead the ";?>pythia.decayPtr method should be provided with the list of relevant particles.

          void ParticleDataEntry::setIsVisible(bool isVisible)  
          bool ParticleDataEntry::isVisible()  
          a flag telling whether a particle species is to be considered as visible in a detector or not, as used e.g. in analysis routines. By default this includes neutrinos and a few BSM particles (gravitino, sneutrinos, neutralinos) that have neither strong nor electromagnetic charge, and are not made up of constituents that have it. The value of this flag is only relevant if a particle is long-lived enough actually to make it to a detector.

          void ParticleDataEntry::setDoForceWidth(bool doForceWidth)  
          bool ParticleDataEntry::doForceWidth()  
          a flag valid only for resonances where PYTHIA contains code to calculate the width of the resonance from encoded matrix-element expressions, i.e. the Z^0, W^+-, t, h^0, and a few more. The normal behaviour (false) is then that the width is calculated from the mass, but it is possible to ";?>force the resonance to retain the nominal width. Branching ratios and the running of the total width are unaffected.

          void ParticleDataEntry::setHasChanged(bool hasChanged)  

          void ParticleDataEntry::hasChanged(bool hasChanged)  
          keep track of whether the data for a particle has been changed in any respect between initialization and the current status. Is used e.g. by the ParticleData::listChanged method to determine which particles to list.

          void ParticleDataEntry::initBWmass()  
          Prepare the Breit-Wigner mass selection by precalculating frequently-used expressions.

          double ParticleDataEntry::constituentMass()  
          is the constituent mass for a quark, hardcoded as m_u = m_d = 0.325, m_s = 0.50, m_c = 1.60 and m_b = 5.0 GeV, for a diquark the sum of quark constituent masses, and for everything else the same as the ordinary mass.

          double ParticleDataEntry::mSel()  
          give the mass of a particle, either at the nominal value or picked according to a (linear or quadratic) Breit-Wigner.

          double ParticleDataEntry::mRun(double mH)  
          calculate the running quark mass at a hard scale mH. For other particles the on-shell mass is given.

          bool ParticleDataEntry::useBreitWigner()  
          tells whether a particle will have a Breit-Wigner mass distribution or not. Is determined by an internal logic based on the particle width and on the value of the ";?> ParticleData:modeBreitWigner switch.

          bool ParticleDataEntry::canDecay(int id)  
          true for a particle with at least one decay channel defined.

          bool ParticleDataEntry::isLepton()  
          true for a lepton or an antilepton (including neutrinos).

          bool ParticleDataEntry::isQuark()  
          true for a quark or an antiquark.

          bool ParticleDataEntry::isGluon()  
          true for a gluon.

          bool ParticleDataEntry::isDiquark()  
          true for a diquark or antidiquark.

          bool ParticleDataEntry::isParton()  
          true for a gluon, a quark or antiquark up to the b (but excluding top), and a diquark or antidiquark consisting of quarks up to the b.

          bool ParticleDataEntry::isHadron()  
          true for a hadron (made up out of normal quarks and gluons, i.e. not for R-hadrons and other exotic states).

          bool ParticleDataEntry::isMeson()  
          true for a meson.

          bool ParticleDataEntry::isBaryon()  
          true for a baryon or antibaryon.

          bool ParticleDataEntry::isOctetHadron()  
          true for an intermediate hadron-like state with a colour octet charge as used in the colour octet model for ";?>onia production.

          int ParticleDataEntry::heaviestQuark(int id)  
          extracts the heaviest quark or antiquark, i.e. one with largest id number, for a hadron. Only the sign of the input argument is relevant.

          int ParticleDataEntry::baryonNumberType(int id)  
          is 1 for a quark, 2 for a diquark, 3 for a baryon, the same with a minus sign for antiparticles, and else zero. Only the sign of the input argument is relevant.

          void ParticleDataEntry::clearChannels()  
          resets to an empty decay table.

          void ParticleDataEntry::addChannel(int onMode = 0, double bRatio = 0., int meMode = 0, int prod0 = 0, int prod1 = 0,int prod2 = 0, int prod3 = 0, int prod4 = 0, int prod5 = 0, int prod6 = 0, int prod7 = 0,)  
          adds a decay channel with up to 8 products.

          int ParticleDataEntry::sizeChannels()  
          returns the number of decay channels for a particle.

          DecayChannel& ParticleDataEntry::channel(int i)  
          const DecayChannel& ParticleDataEntry::channel(int i)  
          gain access to a specified channel in the decay table.

          void ParticleDataEntry::rescaleBR(double newSumBR = 1.)  
          rescales all partial branching ratios by a common factor, such that the sum afterward becomes newSumBR.

          bool ParticleDataEntry::preparePick(int idSgn, double mHat = 0., int idInFlav = 0)  
          prepare to pick a decay channel.

          DecayChannel& ParticleDataEntry::pickChannel()  
          pick a decay channel according to branching ratios from preparePick.

          void ParticleDataEntry::setResonancePtr(ResonanceWidths* resonancePtr)  
          ResonanceWidths* ParticleDataEntry::getResonancePtr()  
          set or get a pointer to an object that can be used for dynamic calculation of partial and total resonance widths. Here a resonance is a particle such as top, Z^0, W^+-, Higgs, and new unstable states beyond the Standard Model.

          void ParticleDataEntry::resInit(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, CoupSM* coupSMPtrIn)  
          initialize the treatment of a resonance.

          double ParticleDataEntry::resWidth(int idSgn,double mHat, int idInFlav = 0, bool openOnly = false, bool setBR = false)  
          calculate the total with for a resonance of a given current mass, optionally including coupling to incoming flavour state (consider the gamma*/Z^0 combination), optionally excluding decay channels that have been closed by the user, and optionally storing the results in the normal decay table. For the first argument only the sign is relevant.

          double ParticleDataEntry::resWidthOpen(int idSgn,double mHat, int idInFlav = 0)  
          special case of resWidth, where only open channels are included, but results are not stored in the normal decay table.

          double ParticleDataEntry::resWidthStore(int idSgn,double mHat, int idInFlav = 0)  
          special case of resWidth, where only open channels are included, and results are stored in the normal decay table.

          double ParticleDataEntry::resOpenFrac(int idSgn)  
          calculate the fraction of the full branching ratio that is left open by the user choice of allowed decay channels.

          double ParticleDataEntry::resWidthRescaleFactor()  
          the factor used to rescale all partial widths in case the total width is being forced to a specific value by the user.

          double ParticleDataEntry::resWidthChan(double mHat, int idAbs1 = 0, int idAbs2 = 0)  
          special case to calculate one final-state width; currently only used for Higgs decay to q qbar, g g or gamma gamma.

          The DecayChannel methods

          The properties stored in an individual decay channel can be set or get by the methods in this section.

          DecayChannel::DecayChannel(int onMode = 0, double bRatio = 0., int meMode = 0, int prod0 = 0, int prod1 = 0, int prod2 = 0, int prod3 = 0, int prod4 = 0, int prod5 = 0, int prod6 = 0, int prod7 = 0)  
          the constructor for a decay channel. Internal.

          void DecayChannel::onMode(int onMode)  
          int DecayChannel::onMode()  
          set or get the onMode of a decay channel,
          0 if a channel is off,
          1 if on,
          2 if on for a particle but off for an antiparticle,
          3 if on for an antiparticle but off for a particle.
          If a particle is its own antiparticle then 2 is on and 3 off but, of course, for such particles it is much simpler and safer to use only 1 and 0.
          The 2 and 3 options can be used e.g. to encode CP violation in B decays, or to let the W's in a q qbar -> W^+ W^- process decay in different channels.

          void DecayChannel::bRatio(double bRatio, bool countAsChanged = true)  
          double DecayChannel::bRatio()  
          set or get the branching ratio of the channel. Second argument only for internal use.

          void DecayChannel::rescaleBR(double fac)  
          multiply the current branching ratio by fac.

          void DecayChannel::meMode(int meMode)  
          int DecayChannel::meMode()  
          set or get the mode of processing this channel, possibly with matrix elements (see the ";?>particle decays and ";?>resonance decays descriptions).

          void DecayChannel::multiplicity(int multiplicity)  
          int DecayChannel::multiplicity()  
          set or get the number of decay products in a channel, at most 8. (Is normally not to be set by hand, since it is automatically updated whenever the products list is changed.)

          void DecayChannel::product(int i, int product)  
          int DecayChannel::product(int i)  
          set or get a list of the decay products, 8 products 0 <= i < 8, with trailing unused ones set to 0.

          void DecayChannel::setHasChanged(bool hasChanged)  
          bool DecayChannel::hasChanged()  
          used for internal purposes, to know which decay modes have been changed.

          bool DecayChannel::contains(int id1)  
          bool DecayChannel::contains(int id1, int id2)  
          bool DecayChannel::contains(int id1, int id2, int id3)  
          find if the decay product list contains the one, two or three particle identities provided. If the same code is repeated then so must it be in the products list. Matching also requires correct sign.

          void DecayChannel::currentBR(double currentBR)  
          double DecayChannel::currentBR()  
          set or get the current branching ratio, taking into account on/off switches and dynamic width for resonances. For internal use.

          void DecayChannel::onShellWidth(double onShellWidth)  
          double DecayChannel::onShellWidth()  
          set or get the current partial width of the channel; intended for resonances where the widths are recalculated based on the current resonance mass. For internal use.

          void DecayChannel::onShellWidthFactor(double factor)  
          multiply the current partial width by factor.

          void DecayChannel::openSec(int idSgn, double openSecIn)  
          double DecayChannel::openSec(nt idSgn)  
          set or get the fraction of secondary open widths, separately for positive and negative particles. For internal use. pythia8-8.1.80.orig/phpdoc/ProgramClasses.php0000644000175000017500000002271612217615312017254 0ustar sunsun Program Classes SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Program Classes

          The complete PYTHIA 8 package contains ";?>a multitude of classes. There is no reason to describe all of them, with all of their methods, since most should not be touched by a normal user. Nevertheless some of the crucial ones are described in detail, as a help not only to advanced users but also to developers. We here provide a quick reference (still incomplete) which classes you can find described where on these pages. Normally you have to scroll down to find the details, since the top of the page contains information of more general interest.

          Class Reference Comment
          BeamShape ";?>Beam Shape vertex and beam momentum spread
          CellJet ";?>Event Analysis jet cone clustering analysis, intended for hadron collider topologies
          ClusterJet ";?>Event Analysis jet clustering analysis, intended for e^+e^- collider topologies
          CoupSM ";?>Standard Model Parameters couplings and mixing matrices
          CoupSUSY ";?>SUSY Les Houches Accord compute and store SUSY couplings, using input from SusyLesHouches
          DecayChannel ";?>Particle Data Scheme the properties of a single decay channel of particle species
          Event ";?>Event Record the complete event record
          HepMC::Pythia8ToHepMC ";?>HepMC Interface convert a PYTHIA event record to the HepMC format
          Hist ";?>Histograms a primitive built-in histogramming package
          Info ";?>Event Information various one-of-a-kind information on the current event
          LHAPDFInterface ";?>Parton Distributions use PDF sets from the LHAPDF library
          LHAup ";?>Les Houches Accord base class for Les Houches external hard-event input
          Particle ";?>Particle Properties the properties of a particle in the event record
          ParticleData ";?>Particle Data Scheme the database of particle species properties
          ParticleDataEntry ";?>Particle Data Scheme the properties of a particle species
          PDF ";?>Parton Distributions base class for all PDFs
          Pythia ";?>Program Flow the top-level class, that drives the generation process
          ResonanceWidths ";?>Semi-Internal Resonances base class for all resonance-width treatment
          Rndm ";?>RandomNumbers a primitive built-in histogramming package
          RotBstMatrix ";?>Four-Vectors rotation and boosts of four-vectors
          Settings ";?>Settings Scheme the database that regulates the behaviour of the program
          SigmaProcess ";?>Semi-Internal Processes base class for all hard-process cross sections
          SlowJet ";?>Event Analysis simple jet clustering using the kT, anti-kT or Cambridge/Aachen algorithms.
          SpaceShower ";?>Implement New Showers spacelike, i..e. initial-state showers
          Sphericity ";?>Event Analysis sphericity analysis of events
          SusyLesHouches ";?>SUSY Les Houches Accord reading in of SLHA information
          Thrust ";?>Event Analysis thrust analysis of events
          TimeShower ";?>Implement New Showers timelike, i..e. final-state showers
          UserHooks ";?>User Hooks get access to some steps of the generation process
          Vec4 ";?>Four-Vectors four-vectors
          ";?>
          ";?>

          You can also access an extensive list of the public ";?>methods in these classes, which compensates for the brevity of the current page. pythia8-8.1.80.orig/phpdoc/CompositenessProcesses.php0000644000175000017500000004437612217615312021057 0ustar sunsun Compositeness Processes SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Compositeness Processes

          Compositeness scenarios may give rise to sharp resonances of excited quarks and leptons. An excited copy of the first generation is implemented, consisting of spin 1/2 particles. The possibility of contact interactions between SM fermions is also implemented in the context of 2 -> 2 quark or fermion-lepton scattering.

          Related to excited fermions, the current implementation contains gauge interaction production by quark-gluon fusion or lepton-photon fusion and contact interaction production by quark-quark or quark-antiquark scattering. For both the 2 -> 1 and 2 -> 2 processes a non-trivial angular dependence is included in the decay, however, only decays into gauge bosons are supported, i.e. not decays through contact interactions. In additions to the compositeness scale and couplings listed below, you are expected to change the excited-fermion masses in accordance with what is desired. See [Bau90] for conventions.

          The contact interactions are implemented according to [Eic83]. The processes include the SM contributions as well as interference. For this reason the processes below converge toward the SM equivalents when the contact interaction contributions are close to zero, e.g. HardQCD:qq2qq and HardQCD:qqbar2qqbarNew in the case of quark scattering.

          Excited fermions, production processes

          A few different production processes have been implemented, which normally would not overlap and therefore could be run together.

          ExcitedFermion:all On Off   (default = off)
          Common switch for the group of implemented processes that produce an excited fermion.

          ExcitedFermion:dg2dStar On Off   (default = off)
          Scatterings d g -> d^*. Code 4001.

          ExcitedFermion:ug2uStar On Off   (default = off)
          Scatterings u g -> u^*. Code 4002.

          ExcitedFermion:sg2sStar On Off   (default = off)
          Scatterings s g -> s^*. Code 4003.

          ExcitedFermion:cg2cStar On Off   (default = off)
          Scatterings c g -> c^*. Code 4004.

          ExcitedFermion:bg2bStar On Off   (default = off)
          Scatterings b g -> b^*. Code 4005.

          ExcitedFermion:egm2eStar On Off   (default = off)
          Scatterings e gamma -> e^*. Code 4011.

          ExcitedFermion:mugm2muStar On Off   (default = off)
          Scatterings mu gamma -> mu^*. Code 4013.

          ExcitedFermion:taugm2tauStar On Off   (default = off)
          Scatterings tau gamma -> tau^*. Code 4015.

          ExcitedFermion:qq2dStarq On Off   (default = off)
          Scatterings q q(bar) -> d^* q(bar). Code 4021.

          ExcitedFermion:qq2uStarq On Off   (default = off)
          Scatterings q q(bar) -> u^* q(bar). Code 4022.

          ExcitedFermion:qq2sStarq On Off   (default = off)
          Scatterings q q(bar) -> s^* q(bar). Code 4023.

          ExcitedFermion:qq2cStarq On Off   (default = off)
          Scatterings q q(bar) -> c^* q(bar). Code 4024.

          ExcitedFermion:qq2bStarq On Off   (default = off)
          Scatterings q q(bar) -> b^* q(bar). Code 4025.

          ExcitedFermion:qqbar2eStare On Off   (default = off)
          Scatterings q qbar -> e^*+- e^-+. Code 4031.

          ExcitedFermion:qqbar2nueStarnue On Off   (default = off)
          Scatterings q qbar -> nu_e^* nu_ebar. Code 4032.

          ExcitedFermion:qqbar2muStarmu On Off   (default = off)
          Scatterings q qbar -> mu^*+- mu^-+. Code 4033.

          ExcitedFermion:qqbar2numuStarnumu On Off   (default = off)
          Scatterings q qbar -> nu_mu^* nu_mubar. Code 4034.

          ExcitedFermion:qqbar2tauStartau On Off   (default = off)
          Scatterings q qbar -> tau^*+- tau^-+. Code 4035.

          ExcitedFermion:qqbar2nutauStarnutau On Off   (default = off)
          Scatterings q qbar -> nu_tau^* nu_taubar. Code 4036.

          Excited fermions, parameters

          The basic couplings of the model are

          ExcitedFermion:Lambda   (default = 1000.; minimum = 100.)
          Compositeness scale Lambda in GeV.

          ExcitedFermion:coupF   (default = 1.0; minimum = 0.0)
          Strength f of the SU(2) coupling.

          ExcitedFermion:coupFprime   (default = 1.0; minimum = 0.0)
          Strength f' of the U(1) coupling.

          ExcitedFermion:coupFcol   (default = 1.0; minimum = 0.0)
          Strength f_c of the SU(3) coupling.

          Contact interactions, production processes

          The processes including contact interactions are

          ContactInteractions:QCqq2qq On Off   (default = off)
          Scatterings q q -> q q including contact interactions. Code 4201.

          ContactInteractions:QCqqbar2qqbar On Off   (default = off)
          Scatterings q qbar -> q' qbar' including contact interactions. Code 4202.

          ContactInteractions:QCffbar2eebar On Off   (default = off)
          Scatterings f fbar -> e- e+ including contact interactions. Code 4203.

          ContactInteractions:QCffbar2mumubar On Off   (default = off)
          Scatterings f fbar -> mu- mu+ including contact interactions. Code 4204.

          ContactInteractions:QCffbar2tautaubar On Off   (default = off)
          Scatterings f fbar -> tau- tau+ including contact interactions. Code 4205.

          Contact interactions, parameters



          ContactInteractions:nQuarkNew   (default = 3; minimum = 0; maximum = 5)
          Number of allowed outgoing new quark flavours in the above q qbar -> q' qbar' process. Similar to HardQCD:nQuarkNew for the QCD processes.

          ContactInteractions:Lambda   (default = 1000.; minimum = 100.)
          Compositeness scale Lambda in GeV. Its overall normalization is largely a matter of convention. The choice made here for the q qbar -> l- l+ processes is such that the pure contact interaction part of the left-left interactions (i.e. disregarding gamma^*, Z^0 and interference terms) has the form d(sigmaHat)/d(tHat) = pi * uHat^2 / (3 * sHat^2 * Lambda^4). The corresponding part of the q qbar -> q' qbar' cross section is a factor 3 larger from colour.

          ContactInteractions:etaLL   (default = 0; minimum = -1; maximum = 1)
          Helicity parameter.
          1 :
          0 :
          -1 :


          ContactInteractions:etaRR   (default = 0; minimum = -1; maximum = 1)
          Helicity parameter.
          1 :
          0 :
          -1 :


          ContactInteractions:etaLR   (default = 0; minimum = -1; maximum = 1)
          Helicity parameter.
          1 :
          0 :
          -1 :
          "?>
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          Particle Decays

          The ParticleDecays class performs the sequential decays of all unstable hadrons produced in the string fragmentation stage, i.e. up to and including b hadrons and their decay products, such as the tau lepton. It is not to be used for the decay of more massive ";?>resonances, such as top, Z^0 or SUSY, where decays must be performed already at the ProcessLevel of the event generation.

          The decay description essentially copies the one present in PYTHIA since many years, but with some improvements, e.g. in the decay tables and the number of decay models available. Recently a more sophisticated handling of tau decays has also been introduced. Some issues may need further polishing.

          Variables determining whether a particle decays

          Before a particle is actually decayed, a number of checks are made.

          (i) Decay modes must have been defined for the particle kind; tested by the canDecay() method of Event (and ParticleData).

          (ii) The main switch for allowing this particle kind to decay must be on; tested by the mayDecay() method of Event (and ParticleData).

          (iii) Particles may be requested to have a nominal proper lifetime tau0 below a threshold.

          ParticleDecays:limitTau0 On Off   (default = off)
          When on, only particles with tau0 < tau0Max are decayed.

          ParticleDecays:tau0Max   (default = 10.; minimum = 0.)
          The above tau0Max, expressed in mm/c.

          (iv) Particles may be requested to have an actual proper lifetime tau below a threshold.

          ParticleDecays:limitTau On Off   (default = off)
          When on, only particles with tau < tauMax are decayed.

          ParticleDecays:tauMax   (default = 10.; minimum = 0.)
          The above tauMax, expressed in mm/c.
          In order for this and the subsequent tests to work, a tau is selected and stored for each particle, whether in the end it decays or not. (If each test would use a different temporary tau it would lead to inconsistencies.)

          (v) Particles may be requested to decay within a given distance of the origin.

          ParticleDecays:limitRadius On Off   (default = off)
          When on, only particles with a decay within a radius r < rMax are decayed. There is assumed to be no magnetic field or other detector effects.

          ParticleDecays:rMax   (default = 10.; minimum = 0.)
          The above rMax, expressed in mm.

          (vi) Particles may be requested to decay within a given cylindrical volume around the origin.

          ParticleDecays:limitCylinder On Off   (default = off)
          When on, only particles with a decay within a volume limited by rho = sqrt(x^2 + y^2) < xyMax and |z| < zMax are decayed. There is assumed to be no magnetic field or other detector effects.

          ParticleDecays:xyMax   (default = 10.; minimum = 0.)
          The above xyMax, expressed in mm.

          ParticleDecays:zMax   (default = 10.; minimum = 0.)
          The above zMax, expressed in mm.

          Mixing



          ParticleDecays:mixB On Off   (default = on)
          Allow or not B^0 - B^0bar and B_s^0 - B_s^0bar mixing.

          ParticleDecays:xBdMix   (default = 0.776; minimum = 0.74; maximum = 0.81)
          The mixing parameter x_d = Delta(m_B^0)/Gamma_B^0 in the B^0 - B^0bar system. (Default from RPP2006.)

          ParticleDecays:xBsMix   (default = 26.05; minimum = 22.0; maximum = 30.0)
          The mixing parameter x_s = Delta(m_B_s^0)/Gamma_B_s^0 in the B_s^0 - B_s^0bar system. (Delta-m from CDF hep-ex-0609040, Gamma from RPP2006.)

          Tau decays

          A new machinery has been introduced to handle tau lepton decays, with helicity information related to the production process and with the form of the hadronic current fitted to data. It is largely based on the corresponding Herwig++ implementation [Gre07], with some input from Tauola [Jad90]. A complete writeup is in preparation, but meanwhile a short summary can be found at [Ilt12].

          For taus in external processes, interfaced with Les Houches Accord information available, e.g. via Les Houches Event Files (LHEF), the new machinery interprets the SPINUP number for tau leptons as giving their helicity, and decays them accordingly. The only exceptions are when a specific polarization is forced by the user (see below), which then overrides the SPINUP value, or when SPINUP has the special value 9 (unpolarized). In the latter case, PYTHIA defaults back to attempting to determine the helicity structure from the production process, in the same way as for internal processes.

          This new machinery is on by default, but it is possible to revert to the simpler old decay handling, e.g. to study differences. Furthermore the spin tracing framework does not yet cover all possibilities; notably it cannot handle taus coming from SUSY decay chains (except via LHEF), so it makes sense to switch off the new machinery in such instances, for speed reasons if nothing else. In case only one tau mother species is undefined, the polarization involved can be set by hand.

          ParticleDecays:sophisticatedTau   (default = 1; minimum = 0; maximum = 3)
          Choice of tau decay model.
          0 : old decay model, with isotropic decays. When reading LHEF files, the SPINUP digit will be ignored.
          1 : sophisticated decays where tau polarization is calculated from the tau production mechanism. When reading LHEF files, the SPINUP digit will be used.
          2 : sophisticated decays as above, but additionally tau polarization is set to ParticleDecaus:tauPolarization for taus produced from ParticleDecays:tauMother. When reading LHEF files, this overrides the SPINUP digit.
          3 : sophisticated decays where tau polarization is set to ParticleDecaus:tauPolarization for all tau decays. When reading LHEF files, this overrides the SPINUP digit.

          Note: options 2 and 3, to force a specific tau polarization, only affect the decay of the tau. The angular distribution of the tau itself, given by its production, is not modified by these options. If you want, e.g., a righthanded W, or a SUSY decay chain, the kinematics should be handled by the corresponding cross section class(es), supplemented by the resonance decay one(s). The options here could then still be used to ensure the correct polarization at the tau decay stage.

          ParticleDecays:tauPolarization   (default = 0; minimum = -1.; maximum = 1.)
          Polarization of the tau when mode 2 or 3 of ParticleDecays:sophisticatedTau is selected.

          ParticleDecays:tauMother   (default = 0; minimum = 0)
          Mother of the tau for forced polarization when mode 2 of ParticleDecays:sophisticatedTau is selected. You should give the positive identity code; to the extent an antiparticle exists it will automatically obtain the inverse polarization.

          QED radiation

          So far PYTHIA does not have any generic machinery for handling QED radiation in normal particle decays. In order to include this, a program like Photos [Bar94, Dav10] could be used as an afterburner. In a few cases, however, the existing shower machinery can be used also here: for two-body decays to a lepton pair (l^+ l^- or l^+- nu_l). Such decays are mediated by gamma^*/Z^0/W^+- exchange, for which PYTHIA does have an existing machinery that can be applied, including first-order matrix-element corrections for the first (hardest) photon emission.

          ParticleDecays:allowPhotonRadiation On Off   (default = off)
          Allow or not photon radiations in decays to a lepton pair, see above.
          Note: The current default is to have radiation switched off, in order to avoid double-counting of emissions if you link to an external QED-radiation program, as is the norm in many collaborations.

          Other variables



          ParticleDecays:mSafety   (default = 0.0005; minimum = 0.; maximum = 0.01)
          Minimum mass difference required between the decaying mother mass and the sum of the daughter masses, kept as a safety margin to avoid numerical problems in the decay generation.

          ParticleDecays:sigmaSoft   (default = 0.5; minimum = 0.2; maximum = 2.)
          In semileptonic decays to more than one hadron, such as B -> nu l D pi, decay products after the first three are dampened in momentum by an explicit weight factor exp(-p^2/sigmaSoft^2), where p is the three-momentum in the rest frame of the decaying particle. This takes into account that such further particles come from the fragmentation of the spectator parton and thus should be soft.

          When a decay mode is defined in terms of a partonic content, a random multiplicity (and a random flavour set) of hadrons is to be picked, especially for some charm and bottom decays. This is done according to a Poissonian distribution, for n_p normal particles and n_q quarks the average value is chosen as
          n_p/ 2 + n_q/4 + multIncrease * ln ( mDiff / multRefMass)
          with mDiff the difference between the decaying particle mass and the sum of the normal-particle masses and the constituent quark masses. For gluon systems multGoffset offers and optional additional term to the multiplicity. The lowest possible multiplicity is n_p + n_q/2 (but at least 2) and the highest possible 10. If the picked hadrons have a summed mass above that of the mother a new try is made, including a new multiplicity. These constraints imply that the actual average multiplicity does not quite agree with the formula above.

          ParticleDecays:multIncrease   (default = 4.; minimum = 2.; maximum = 6.)
          The above multIncrease parameter, except for meMode = 23.

          ParticleDecays:multIncreaseWeak   (default = 2.5; minimum = 1.; maximum = 4.)
          The above multIncrease parameter, specifically for meMode = 23. Here the weak decay implies that only the virtual W mass should contribute to the production of new particles, rather than the full meson mass.

          ParticleDecays:multRefMass   (default = 0.7; minimum = 0.2; maximum = 2.0)
          The above multRefMass parameter.

          ParticleDecays:multGoffset   (default = 0.5; minimum = 0.0; maximum = 2.0)
          The above multGoffset parameter.

          ParticleDecays:colRearrange   (default = 0.5; minimum = 0.; maximum = 1.0)
          When a decay is given as a list of four partons to be turned into hadrons (primarily for modes 41 - 80) it is assumed that they are listed in pairs, as a first and a second colour singlet, which could give rise to separate sets of hadrons. Here colRearrange is the probability that this original assignment is not respected, and default corresponds to no memory of this original colour topology.

          ParticleDecays:FSRinDecays On Off   (default = true)
          When a particle decays to q qbar, g g, g g g or gamma g g, with meMode > 90, allow or not a shower to develop from it, before the partonic system is hadronized. (The typical example is Upsilon decay.) In addition, some variables defined for string fragmentation and for flavour production are used also here.

          Modes for Matrix Element Processing

          Some decays can be treated better than what pure phase space allows, by reweighting with appropriate matrix elements. In others a partonic content has to be converted to a set of hadrons. The presence of such corrections is signaled by a nonvanishing meMode() value for a decay mode in the ";?>particle data table. The list of allowed possibilities almost agrees with the PYTHIA 6 ones, but several obsolete choices have been removed, a few new introduced, and most have been moved for better consistency. Here is the list of currently allowed meMode() codes:
          • 0 : pure phase space of produced particles ("default"); input of partons is allowed and then the partonic content is converted into the minimal number of hadrons (i.e. one per parton pair, but at least two particles in total)
          • 1 : omega and phi -> pi+ pi- pi0
          • 2 : polarization in V -> PS + PS (V = vector, PS = pseudoscalar), when V is produced by PS -> PS + V or PS -> gamma + V
          • 11 : Dalitz decay into one particle, in addition to the lepton pair (also allowed to specify a quark-antiquark pair that should collapse to a single hadron)
          • 12 : Dalitz decay into two or more particles in addition to the lepton pair
          • 13 : double Dalitz decay into two lepton pairs
          • 21 : decay to phase space, but weight up neutrino_tau spectrum in tau decay
          • 22 : weak decay; if there is a quark spectator system it collapses to one hadron; for leptonic/semileptonic decays the V-A matrix element is used, for hadronic decays simple phase space
          • 23 : as 22, but require at least three particles in decay
          • 31 : decays of type B -> gamma X, very primitive simulation where X is given in terms of its flavour content, the X multiplicity is picked according to a geometrical distribution with average number 2, and the photon energy spectrum is weighted up relative to pure phase space
          • 42 - 50 : turn partons into a random number of hadrons, picked according to a Poissonian with average value as described above, but at least code - 40 and at most 10, and then distribute then in pure phase space; make a new try with another multiplicity if the sum of daughter masses exceed the mother one
          • 52 - 60 : as 42 - 50, with multiplicity between code - 50 and 10, but avoid already explicitly listed non-partonic channels
          • 62 - 70 : as 42 - 50, but fixed multiplicity code - 60
          • 72 - 80 : as 42 - 50, but fixed multiplicity code - 70, and avoid already explicitly listed non-partonic channels
          • 91 : decay to q qbar or g g, which should shower and hadronize
          • 92 : decay onium to g g g or g g gamma (with matrix element), which should shower and hadronize
          • 100 - : reserved for the description of partial widths of ";?>resonances
          Three special decay product identity codes are defined.
          • 81: remnant flavour. Used for weak decays of c and b hadrons, where the c or b quark decays and the other quarks are considered as a spectator remnant in this decay. In practice only used for baryons with multiple c and b quarks, which presumably would never be used, but have simple (copied) just-in-case decay tables. Assumed to be last decay product.
          • 82: random flavour, picked by the standard fragmentation flavour machinery, used to start a sequence of hadrons, for matrix element codes in 41 - 80. Assumed to be first decay product, with -82 as second and last. Where multiplicity is free to be picked it is selected as for normal quarkonic systems. Currently unused.
          • 83: as for 82, with matched pair 83, -83 of decay products. The difference is that here the pair is supposed to come from a closed gluon loop (e.g. eta_c -> g g) and so have a somewhat higher average multiplicity than the simple string assumed for 82, see the ParticleDecays:multGoffset parameter above.
          "?>
          pythia8-8.1.80.orig/phpdoc/Bibliography.php0000644000175000017500000003060212217615312016733 0ustar sunsun Bibliography SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

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          pythia8-8.1.80.orig/phpdoc/MadGraph5Processes.php0000644000175000017500000001475712217615312017774 0ustar sunsun MadGraph 5 Processes SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          MadGraph 5 Processes

          By far the easiest way to implement new processes into PYTHIA 8 is by using the matrix-element generator MadGraph 5. This program has an option to output the results of a matrix-element calculation as a set of PYTHIA 8 C++ classes (plus further auxiliary code), that can then be linked and used as ";?>semi-internal processes, meaning they are handled identically with normal internal ones. This way, MadGraph 5 can be used to implement processes from any model that can be written in terms of a Lagrangian. Any 2 -> 1, 2 -> 2 and 2 -> 3 processes can be implemented, the limit being set by the absence of efficient phase space generator algorithms for higher multiplicities in PYTHIA. Features such as s-channel resonances are automatically implemented in the process classes. Besides the process library and necessary model files, also an example main program is generated for each set of processes, which can be easily modified to perform the desired analyses.

          In order to create a PYTHIA 8 process library with MadGraph 5, first download the MadGraph 5 package from https://launchpad.net/madgraph5, and untar the package. You can then specify the location of your pythia81xx directory in the file input/mg5_configuration.txt:
          pythia8_path = ./pythia81xx
          The location can be either relative (to the directory MadGraph5_v_x_x_x/.) or absolute.

          For any model that is already implemented in the MadGraph 5 package, you can directly use the model. Start the MadGraph 5 interface bin/mg5, and do:

          import model model_name  
          generate your_process_in_mg5_syntax 
          add process your_next_process_in_mg5_syntax 
          ...  
          output pythia8 [path_to_pythia81xx_directory]
          

          For examples of MG5 process syntax, please see http://madgraph.phys.ucl.ac.be/EXAMPLES/example_mg5.html or type help generate. If you specified the path to the pythia81xx directory in the mg5_configuration file, you do not need to enter it in the output command.

          If your preferred model is found on the FeynRules model wiki page, http://feynrules.irmp.ucl.ac.be/wiki/ModelDatabaseMainPage, download the UFO (Universal FeynRules Output) tar file for the model, untar in the models/ directory, and use as above.

          If you want to implement a new model which has not yet been implemented, you can do this either using the Mathematica package FeynRules (see http://feynrules.irmp.ucl.ac.be/) or directly edit the UFO model files of the most similar model in the models/ directory.

          The resulting output from the output pythia8 command is:

          • A process directory Processes_modelname with the model information and the files needed for all processes defined for this model, placed in the pythia81xx main directory. The model files are Parameters_modelname.h/cc and HelAmps_modelname.h/cc, and the process files for each process class (with the same mass, spin and color of the initial/final state particles) are called Sigma_modelname_processname.h/cc. The directory also contains a makefile and a model parameter file param_card_modelname.dat.
          • An example main program in the directory examples/ (in the pythia81xx main directory) called main_modelname_N.cc and a corresponding makefile Makefile_modelname_N. This main program links in the process classes in the process directory described above. To run the example main program, just go to the examples/ directory and run
            make -f Makefile_modelname_N
            or run launch directly inside the MadGraph 5 command line interface.

          Note that in order for PYTHIA 8 to be able to automatically decay any new particles, it is necessary to specify the branching ratios of the particles in the param_card file, see [Ska04,Alw07] for details.

          For further technical details, please see the MadGraph 5 release paper [Alw11] and the ";?>semi-internal processes page.

          Of course, as with MadGraph 4, MadGraph 5 can also output files of parton-level events according to the ";?>LHEF standard, that can be read in and processed further by PYTHIA 8. The advantage is that then the MadGraph 5 phase space generator can be used, which opens up for processes with more than three particles in the final state. The disadvantages are that it is less easy to mix and match with existing PYTHIA processes, and that one needs to regenerate and store large LHEF files for different kinematics cuts or parameter values.

          Please cite the MadGraph 5 release paper [Alw11] if you use MadGraph 5 to generate process libraries for PYTHIA 8. pythia8-8.1.80.orig/phpdoc/SUSYLesHouchesAccord.php0000644000175000017500000004723112217615312020230 0ustar sunsun SUSY Les Houches Accord SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          SUSY Les Houches Accord

          The PYTHIA 8 program does not contain an internal spectrum calculator (a.k.a. RGE package) to provide supersymmetric couplings, mixing angles, masses and branching ratios. Thus the SUSY Les Houches Accord (SLHA) [Ska04][All08] is the only way of inputting SUSY models, and SUSY processes (see the ";?>SUSYProcesses page) cannot be run unless such an input has taken place.

          The SLHA input format can also be extended for use with more general BSM models, beyond SUSY. Information specific to how to use the SLHA interface for generic BSM models is collected below, under Using SLHA for generic BSM Models, with more elaborate explanations and examples in [Des11].

          Most of the SUSY implementation in PYTHIA 8 is compatible with both the SLHA1 [Ska04] and SLHA2 [All08] conventions (with some limitations for the NMSSM in the latter case). Internally, PYTHIA 8 uses the SLHA2 conventions and translates SLHA1 input to these when necessary. See the section on SUSY Processes and [Des11] for more information. Note that PYTHIA assumes that a spectrum is either fully SHLA1 or fully SLHA2 compliant. Mixing of the two standards is discouraged, as this can lead to ambiguities and inconsistencies.

          When reading LHEF files, Pythia automatically looks for SLHA information between <slha>...</slha> tags in the header of such files. When running Pythia without LHEF input (or if reading an LHEF file that does not contain SLHA information in the header), a separate file containing SLHA information may be specified using SLHA:file (see below).

          Normally the LHEF would be in uncompressed format, and thus human-readable if opened in a text editor. A possibility to read gzipped files has been added, based on the Boost and zlib libraries, which therefore have to be linked appropriately in order for this option to work. See the README file in the main directory for details on how to do this.

          Finally, the SLHA input capability can of course also be used to input SLHA-formatted MASS and DECAY tables for other particles, such as the Higgs boson, furnishing a less sophisticated but more universal complement to the standard PYTHIA 8-specific methods for inputting such information (for the latter, see the section on ";?>Particle Data and the ";?>scheme to modify it). This may at times not be desirable, so a few options can be used to curb the right of SLHA to overwrite particle data. Conversely, it is sometimes useful to allow the user to modify eg a mass parameter relative to its value in the SLHA spectrum. This is normally not permitted (the SLHA spectrum is normally self-consistent and should not be modified), but an option for allowing it is provided.

          The reading-in of information from SLHA or LHEF files is handled by the SusyLesHouches class, while the subsequent calculation of derived quantities of direct application to SUSY processes is done in the CoupSUSY, SigmaSUSY, and SUSYResonanceWidths classes.

          Sanity Checks

          As an aid for basic validation, some checks and ranges are imposed on SLHA input during initialization, as follows:
          • Several parameters (SLHA:keepSM, minMassSM, and SLHA:allowUserOverride) provide some safety against unintentionally overwriting PYTHIA's Standard-Model information. These parameters can be altered to hand over more or less control to the SLHA interface. In particular, a lot of mass and decay-table information may be included by default in some SLHA files, without it being the explicit intention of the user to overwrite the corresponding PYTHIA information. The default values of the SLHA safety parameters have been chosen so as to eliminate at least the most obvious causes of Garbage In Garbage Out. (E.g., there is usually no reason to modify the masses of well-measured SM particles, like the W and Z bosons, nor to replace their sophisticated internal decay treatments by the simplified isotropic treatment used for SLHA DECAY tables.)
          • For SLHA SUSY spectra, the interface checks the mass-ordering of the Higgs, Neutralino, and Chargino sectors, and the unitarity/orthogonality of the mixing matrices. It also performs some additional self-consistency checks on whether the correct SLHA BLOCKs for the given SUSY model have been included, and whether all required entries have been defined.
          • If MASS or DECAY information for a particle has been changed by SLHA input, the following sanity checks will be carried out. The particle will be declared stable unless there is at least one on-shell decay channel open (regardless of the presence of any DECAY information). In particular, massless particles will always be declared stable. A lower cutoff is imposed on the Breit-Wigner shape of the particle, requiring its mass to remain above the sum of masses for the lightest decay channel. Subject to that constraint, the lower cutoff will normally be placed at 5 times the width (so that the default gives a decent sampling of the shape), but the user is allowed to use the mMin parameter to choose a larger sampling range if so desired (still subject to the on-shell constraint).
          • For each decay channel in an SLHA DECAY table, PYTHIA will checks the available phase space. If the channel is on shell (sum of daughter masses is less than mass of decaying particle), then the threshold dependence is given by SLHA:meMode. If the channel is off shell, then an meMode of 100 is always used. As a further protection against GIGO, if the channel appears to be physically impossible (defined as requiring fluctuations of more than more than 100 times the effective combined widths), it is switched of and a warning message is printed.
          • DECAY table branching fractions are always interpreted as positive. However, a negative sign for one or more channels can be given, and will then be interpreted to mean that the corresponding channel(s) should be switched off for the current run. This furnishes a simple way to switch SLHA DECAY channels on and off while preserving the sum of branching fractions equal to unity.
          Note that these sanity checks will not catch all possible cases of Garbage In Garbage Out, so human verification of the input files is always a good idea, as is taking a look at any warnings or error messages printed by the SLHA interface during initialization. It is ultimately up to the user to ensure that sensible input is being given.

          SLHA Switches and Parameters

          mode  SLHA:readFrom   (default = 1; minimum = 0; maximum = 2)
          Controls from where SLHA information is read.
          option 0 : is not read at all. Useful when SUSY is not simulated and normal particle properties should not be overwritten.
          option 1 : read in from the <slha>...</slha> block of a LHEF, if such a file is read during initialization, and else from the SLHA:file below.
          option 2 : read in from the SLHA:file below.

          SLHA:file   (default = void)
          Name of an SLHA (or LHEF) file containing the SUSY/BSM model definition, spectra, and (optionally) decay tables. Default void signals that no such file has been assigned.

          SLHA:keepSM On Off   (default = on)
          Some programs write SLHA output also for SM particles where normally one would not want to have masses and decay modes changed unwittingly. Therefore, by default, known SM particles are ignored in SLHA files. To be more specific, particle data for identity codes in the ranges 1 - 24 and 81 - 999,999 are ignored. Notably this includes Z^0, W^+- and t. The SM Higgs is modified by the SLHA input, as is other codes in the range 25 - 80 and 1,000,000 - . If you switch off this flag then also SM particles are modified by SLHA input.

          SLHA:minMassSM   (default = 100.0)
          This parameter provides an alternative possibility to ignore SLHA input for all particles with identity codes below 1,000,000 (which mainly means SM particle, but also includes e.g. the Higgs bosons in two-Higgs-doublet scenarios) whose default masses in PYTHIA lie below some threshold value, given by this parameter. The default value of 100.0 allows SLHA input to modify the top quark, but not, e.g., the Z^0 and W^+- bosons.

          SLHA:allowUserOverride On Off   (default = off)
          Flag to set whether the user is allowed to modify the parameters read from an SLHA spectrum. Is normally kept off to preserve the internal self-consistency of SLHA spectra. If this flag is switched on, the mass values read from the SLHA block MASS are allowed to be modified by the user, using PYTHIA's standard readString and related methods.

          SLHA DECAY Tables

          In addition to SUSY spectra, the SLHA also defines a set of conventions for decay tables. These are not restricted to SUSY models, but can be used for arbitrary particles, either in combination with or independently of the SUSY parts of the Accord. The settings in this section control whether and how PYTHIA will make use of such tables. See also the comments under sanity checks above.
          Note: the PYTHIA SLHA interface is limited to at most 1→8 decays.

          SLHA:useDecayTable On Off   (default = on)
          Switch to choose whether to read in SLHA DECAY tables or not. If this switch is set to off, PYTHIA will ignore any decay tables found in the SLHA file, and all decay widths will be calculated internally by PYTHIA. If switched on, SLHA decay tables will be read in, and will then supersede PYTHIA's internal calculations, with PYTHIA only computing the decays for particles for which no SLHA decay table is found. (To set a particle stable, you may either omit an SLHA DECAY table for it and then use PYTHIA's internal id:MayDecay switch for that particle, or you may include an SLHA DECAY table for it, with the width set explicitly to zero.)

          mode  SLHA:meMode   (default = 100; minimum = 100; maximum = 103)
          This value specifies how threshold, off-shell, and phase-space weighting effects for SLHA decay channels should be treated, using the same numbering scheme as for ";?>resonances. The default (100) is to use the branching fraction given in the SLHA DECAY tables without any modifications. The corresponding partial widths remain unchanged when the resonance fluctuates in mass. Specifically there are no threshold corrections. That is, if the resonance fluctuates down in mass, to below the nominal threshold for some decay mode, it is assumed that one of the daughters could also fluctuate down to keep the channel open. (If not, there may be problems later on.) Alternative options (with values 101+) documented under ";?>resonances allow for some flexibility to apply threshold factors expressing the closing of the on-shell phase space when the daughter masses approach or exceed the parent one. Note that modes that are extremely far off shell (defined as needing a fluctuation of more than 100 times the root-sum-square of the widths of the mother and daughter particles) will always be assigned meMode = 100 and should be switched off by hand if so desired. It is up to the user to ensure that the final behaviour is consistent with what is desired (and/or to apply suitable post facto reweightings). Plotting the generator-level resonance and decay-product mass distributions (and e.g., mass differences), effective branching fractions, etc, may be of assistance to validate the behaviour of the program.

          Internal SLHA Variables

          mode  SLHA:verbose   (default = 1; minimum = 0; maximum = 3)
          Controls amount of text output written by the SLHA interface, with a value of 0 corresponding to the most quiet mode. The following variables are used internally by PYTHIA as local copies of SLHA information. User changes will generally have no effect, since these variables will be reset by the SLHA reader during initialization.

          SLHA:NMSSM On Off   (default = off)
          Corresponds to SLHA block MODSEL entry 3.

          Using SLHA for generic BSM Models

          Using the QNUMBERS extension [Alw07], the SLHA can also be used to define new particles, with arbitrary quantum numbers. This already serves as a useful way to introduce new particles and can be combined with MASS and DECAY tables in the usual way, to generate isotropically distributed decays or even chains of such decays. (If you want something better than isotropic, sorry, you'll have to do some actual work ...)

          A more advanced further option is to make use of the possibility in the SLHA to include user-defined blocks with arbitrary names and contents. Obviously, standalone PYTHIA 8 does not know what to do with such information. However, it does not throw it away either, but instead stores the contents of user blocks as strings, which can be read back later, with the user having full control over the format used to read the individual entries.

          The contents of both standard and user-defined SLHA blocks can be accessed in any class inheriting from PYTHIA 8's SigmaProcess class (i.e., in particular, from any semi-internal process written by a user), through its SLHA pointer, slhaPtr, by using the following methods:
          bool slhaPtr->getEntry(string blockName, double& val);
          bool slhaPtr->getEntry(string blockName, int indx, double& val);
          bool slhaPtr->getEntry(string blockName, int indx, int jndx, double& val);
          bool slhaPtr->getEntry(string blockName, int indx, int jndx, int kndx, double& val);

          This particular example assumes that the user wants to read the entries (without index, indexed, matrix-indexed, or 3-tensor-indexed, respectively) in the user-defined block blockName, and that it should be interpreted as a double. The last argument is templated, and hence if anything other than a double is desired to be read, the user has only to give the last argument a different type. If anything went wrong (i.e., the block doesn't exist, or it doesn't have an entry with that index, or that entry can't be read as a double), the method returns false; true otherwise. This effectively allows to input completely arbitrary parameters using the SLHA machinery, with the user having full control over names and conventions. Of course, it is then the user's responsibility to ensure complete consistency between the names and conventions used in the SLHA input, and those assumed in any user-written semi-internal process code.

          Note that PYTHIA 8 always initializes at least the SLHA blocks MASS and SMINPUTS, starting from its internal SM parameters and particle data table values (updated to take into account user modifications). These blocks can therefore be accessed using the slhaPtr->getEntry() methods even in the absence of SLHA input. Note: in the SMINPUTS block, PYTHIA outputs physically correct (i.e., measured) values of GF, m_Z, and alpha_EM(m_Z). However, if one attempts to compute, e.g., the W mass, at one loop from these quantities, a value of 79 GeV results, with a corresponding value for the weak mixing angle. We advise to instead take the physically measured W mass from block MASS, and recompute the EW parameters as best suited for the application at hand.

          "?>
          pythia8-8.1.80.orig/phpdoc/TimelikeShowers.php0000644000175000017500000015152712217615312017450 0ustar sunsun Timelike Showers SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Timelike Showers

          The PYTHIA algorithm for timelike final-state showers is based on the article [Sjo05], where a transverse-momentum-ordered evolution scheme is introduced, with the extension to fully interleaved evolution covered in [Cor10a]. This algorithm is influenced by the previous mass-ordered algorithm in PYTHIA [Ben87] and by the dipole-emission formulation in Ariadne [Gus86]. From the mass-ordered algorithm it inherits a merging procedure for first-order gluon-emission matrix elements in essentially all two-body decays in the standard model and its minimal supersymmetric extension [Nor01].

          The normal user is not expected to call TimeShower directly, but only have it called from Pythia. Some of the parameters below, in particular TimeShower:alphaSvalue, would be of interest for a tuning exercise, however.

          Main variables

          Often the maximum scale of the FSR shower evolution is understood from the context. For instance, in a resonance decay half the resonance mass sets an absolute upper limit. For a hard process in a hadronic collision the choice is not as unique. Here the ";?>factorization scale has been chosen as the maximum evolution scale. This would be the pT for a 2 -> 2 process, supplemented by mass terms for massive outgoing particles. For some special applications we do allow an alternative.

          TimeShower:pTmaxMatch   (default = 1; minimum = 0; maximum = 2)
          Way in which the maximum shower evolution scale is set to match the scale of the hard process itself.
          0 : (i) if the final state of the hard process (not counting subsequent resonance decays) contains at least one quark (u, d, s, c ,b), gluon or photon then pT_max is chosen to be the factorization scale for internal processes and the scale value for Les Houches input; (ii) if not, emissions are allowed to go all the way up to the kinematical limit (i.e. to half the dipole mass). This option agrees with the corresponding one for spacelike showers. There the reasoning is that in the former set of processes the ISR emission of yet another quark, gluon or photon could lead to double-counting, while no such danger exists in the latter case. The argument is less compelling for timelike showers, but could be a reasonable starting point.
          1 : always use the factorization scale for an internal process and the scale value for Les Houches input, i.e. the lower value. This should avoid double-counting, but may leave out some emissions that ought to have been simulated. (Also known as wimpy showers.)
          2 : always allow emissions up to the kinematical limit (i.e. to half the dipole mass). This will simulate all possible event topologies, but may lead to double-counting. (Also known as power showers.)

          Note 1: as enumerated in the text, these options take effect both for internal and external processes. Whether a particular option makes sense depends on the context. For instance, if events for the same basic process to different orders are to be matched, then option 1 would be a reasonable first guess. But in more sophisticated descriptions option 2 could be combined with UserHook vetoes on emissions that would lead to double-counting, using more flexible phase space boundaries. Option 0, finally, may be most realistic when only Born-level processes are involved, possibly in combination with a nonzero TimeShower:pTdampMatch.
          Note 2: These options only apply to the hard interaction. If a "second hard" process is present, the two are analyzed and set separately for the default 0 option, while both are affected the same way for non-default options 1 and 2. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of each process itself. The options also assume that you use interleaved evolution, so that FSR is in direct competition with ISR for the hardest emission. If you already generated a number of ISR partons at low pT, it would not make sense to have a later FSR shower up to the kinematical limit for all of them.
          Note 3: Recall that resonance decays are not affected by this mode, but that showers there are always set to fill the full phase space, often with built-in matrix-element-matching that give a NLO accuracy. A modification of this behaviour would require you to work with UserHooks.

          TimeShower:pTmaxFudge   (default = 1.0; minimum = 0.25; maximum = 2.0)
          In cases where the above pTmaxMatch rules would imply that pT_max = pT_factorization, pTmaxFudge introduces a multiplicative factor f such that instead pT_max = f * pT_factorization. Only applies to the hardest interaction in an event, and a "second hard" if there is such a one, cf. below. It is strongly suggested that f = 1, but variations around this default can be useful to test this assumption.
          Note:Scales for resonance decays are not affected, but can be set separately by ";?>user hooks.

          TimeShower:pTmaxFudgeMPI   (default = 1.0; minimum = 0.25; maximum = 2.0)
          A multiplicative factor f such that pT_max = f * pT_factorization, as above, but here for the non-hardest interactions (when multiparton interactions are allowed).

          TimeShower:pTdampMatch   (default = 0; minimum = 0; maximum = 2)
          These options only take effect when a process is allowed to radiate up to the kinematical limit by the above pTmaxMatch choice, and no matrix-element corrections are available. Then, in many processes, the fall-off in pT will be too slow by one factor of pT^2. That is, while showers have an approximate dpT^2/pT^2 shape, often it should become more like dpT^2/pT^4 at pT values above the scale of the hard process. This argument is more obvious and relevant for ISR, where emissions could go the the kinematical limit, whereas they are constrained by the respective dipole mass for FSR. Nevertheless this matching option is offered for FSR to have a (semi-)symmetric description. Note that a dampening factor is applied to all dipoles in the final state of the hard process, which is somewhat different from the ISR implementation.
          0 : emissions go up to the kinematical limit, with no special dampening.
          1 : emissions go up to the kinematical limit, but dampened by a factor k^2 Q^2_fac/(pT^2 + k^2 Q^2_fac), where Q_fac is the factorization scale and k is a multiplicative fudge factor stored in pTdampFudge below.
          2 : emissions go up to the kinematical limit, but dampened by a factor k^2 Q^2_ren/(pT^2 + k^2 Q^2_ren), where Q_ren is the renormalization scale and k is a multiplicative fudge factor stored in pTdampFudge below.

          Note: These options only apply to the hard interaction. Specifically, a "second hard" interaction would not be affected. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of the process itself.

          TimeShower:pTdampFudge   (default = 1.0; minimum = 0.25; maximum = 4.0)
          In cases 1 and 2 above, where a dampening is imposed at around the factorization or renormalization scale, respectively, this allows the pT scale of dampening of radiation by a half to be shifted by this factor relative to the default Q_fac or Q_ren. This number ought to be in the neighbourhood of unity, but variations away from this value could do better in some processes.

          The amount of QCD radiation in the shower is determined by

          TimeShower:alphaSvalue   (default = 0.1383; minimum = 0.06; maximum = 0.25)
          The alpha_strong value at scale M_Z^2. The default value corresponds to a crude tuning to LEP data, to be improved.

          The actual value is then regulated by the running to the scale pT^2, at which the shower evaluates alpha_strong.

          TimeShower:alphaSorder   (default = 1; minimum = 0; maximum = 2)
          Order at which alpha_strong runs,
          0 : zeroth order, i.e. alpha_strong is kept fixed.
          1 : first order, which is the normal value.
          2 : second order. Since other parts of the code do not go to second order there is no strong reason to use this option, but there is also nothing wrong with it.

          The CMW rescaling of Lambda_QCD (see the section on ";?>StandardModelParameters) can be applied to the alpha_strong values used for timelike showers. Note that tunes using this option need lower values of alpha_strong(m_Z^2) than tunes that do not.

          TimeShower:alphaSuseCMW On Off   (default = false)

          option false : Do not apply the CMW rescaling.
          option true : Apply the CMW rescaling, increasing Lambda_QCD for timelike showers by a factor roughly 1.6.

          QED radiation is regulated by the alpha_electromagnetic value at the pT^2 scale of a branching.

          TimeShower:alphaEMorder   (default = 1; minimum = -1; maximum = 1)
          The running of alpha_em.
          1 : first-order running, constrained to agree with StandardModel:alphaEMmZ at the Z^0 mass.
          0 : zeroth order, i.e. alpha_em is kept fixed at its value at vanishing momentum transfer.
          -1 : zeroth order, i.e. alpha_em is kept fixed, but at StandardModel:alphaEMmZ, i.e. its value at the Z^0 mass.

          The natural scale for couplings, and PDFs for dipoles stretching out to the beam remnants, is pT^2. To explore uncertainties it is possibly to vary around this value, however, in analogy with what can be done for ";?>hard processes.

          TimeShower:renormMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
          The default pT^2 renormalization scale is multiplied by this prefactor. For QCD this is equivalent to a change of Lambda^2 in the opposite direction, i.e. to a change of alpha_strong(M_Z^2) (except that flavour thresholds remain at fixed scales).

          TimeShower:factorMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
          The default pT^2 factorization scale is multiplied by this prefactor.

          The rate of radiation if divergent in the pT -> 0 limit. Here, however, perturbation theory is expected to break down. Therefore an effective pT_min cutoff parameter is introduced, below which no emissions are allowed. The cutoff may be different for QCD and QED radiation off quarks, and is mainly a technical parameter for QED radiation off leptons.

          TimeShower:pTmin   (default = 0.4; minimum = 0.1; maximum = 2.0)
          Parton shower cut-off pT for QCD emissions.

          TimeShower:pTminChgQ   (default = 0.4; minimum = 0.1; maximum = 2.0)
          Parton shower cut-off pT for photon coupling to coloured particle.

          TimeShower:pTminChgL   (default = 1e-6; minimum = 1e-10; maximum = 2.0)
          Parton shower cut-off pT for pure QED branchings. Assumed smaller than (or equal to) pTminChgQ.

          Shower branchings gamma -> f fbar, where f is a quark or lepton, in part compete with the hard processes involving gamma^*/Z^0 production. In order to avoid overlap it makes sense to correlate the maximum gamma mass allowed in showers with the minimum gamma^*/Z^0 mass allowed in hard processes. In addition, the shower contribution only contains the pure gamma^* contribution, i.e. not the Z^0 part, so the mass spectrum above 50 GeV or so would not be well described.

          TimeShower:mMaxGamma   (default = 10.0; minimum = 0.001; maximum = 5000.0)
          Maximum invariant mass allowed for the created fermion pair in a gamma -> f fbar branching in the shower.

          Interleaved evolution

          Multiparton interactions (MPI) and initial-state showers (ISR) are always interleaved, as follows. Starting from the hard interaction, the complete event is constructed by a set of steps. In each step the pT scale of the previous step is used as starting scale for a downwards evolution. The MPI and ISR components each make their respective Monte Carlo choices for the next lower pT value. The one with larger pT is allowed to carry out its proposed action, thereby modifying the conditions for the next steps. This is relevant since the two components compete for the energy contained in the beam remnants: both an interaction and an emission take away some of the energy, leaving less for the future. The end result is a combined chain of decreasing pT values, where ones associated with new interactions and ones with new emissions are interleaved.

          There is no corresponding requirement for final-state radiation (FSR) to be interleaved. Such an FSR emission does not compete directly for beam energy (but see below), and also can be viewed as occurring after the other two components in some kind of time sense. Interleaving is allowed, however, since it can be argued that a high-pT FSR occurs on shorter time scales than a low-pT MPI, say. Backwards evolution of ISR is also an example that physical time is not the only possible ordering principle, but that one can work with conditional probabilities: given the partonic picture at a specific pT resolution scale, what possibilities are open for a modified picture at a slightly lower pT scale, either by MPI, ISR or FSR? Complete interleaving of the three components also offers advantages if one aims at matching to higher-order matrix elements above some given scale.

          TimeShower:interleave On Off   (default = on)
          If on, final-state emissions are interleaved in the same decreasing-pT chain as multiparton interactions and initial-state emissions. If off, final-state emissions are only addressed after the multiparton interactions and initial-state radiation have been considered.

          As an aside, it should be noted that such interleaving does not affect showering in resonance decays, such as a Z^0. These decays are only introduced after the production process has been considered in full, and the subsequent FSR is carried out inside the resonance, with preserved resonance mass.

          One aspect of FSR for a hard process in hadron collisions is that often colour dipoles are formed between a scattered parton and a beam remnant, or rather the hole left behind by an incoming partons. If such holes are allowed as dipole ends and take the recoil when the scattered parton undergoes a branching then this translates into the need to take some amount of remnant energy also in the case of FSR, i.e. the roles of ISR and FSR are not completely decoupled. The energy taken away is bookkept by increasing the x value assigned to the incoming scattering parton, and a reweighting factor x_new f(x_new, pT^2) / x_old f(x_old, pT^2) in the emission probability ensures that not unphysically large x_new values are reached. Usually such x changes are small, and they can be viewed as a higher-order effect beyond the accuracy of the leading-log initial-state showers.

          This choice is not unique, however. As an alternative, if nothing else useful for cross-checks, one could imagine that the FSR is completely decoupled from the ISR and beam remnants.

          TimeShower:allowBeamRecoil On Off   (default = on)
          If on, the final-state shower is allowed to borrow energy from the beam remnants as described above, thereby changing the mass of the scattering subsystem. If off, the partons in the scattering subsystem are constrained to borrow energy from each other, such that the total four-momentum of the system is preserved. This flag has no effect on resonance decays, where the shower always preserves the resonance mass, cf. the comment above about showers for resonances never being interleaved.

          TimeShower:dampenBeamRecoil On Off   (default = on)
          When beam recoil is allowed there is still some ambiguity how far into the beam end of the dipole that emission should be allowed. It is dampened in the beam region, but probably not enough. When on an additional suppression factor 4 pT2_hard / (4 pT2_hard + m2) is multiplied on to the emission probability. Here pT_hard is the transverse momentum of the radiating parton and m the off-shell mass it acquires by the branching, m2 = pT2/(z(1-z)). Note that m2 = 4 pT2_hard is the kinematical limit for a scattering at 90 degrees without beam recoil.

          Global recoil

          The final-state algorithm is based on dipole-style recoils, where one single parton takes the full recoil of a branching. This is unlike the initial-state algorithm, where the complete already-existing final state shares the recoil of each new emission. As an alternative, also the final-state algorithm contains an option where the recoil is shared between all partons in the final state. Thus the radiation pattern is unrelated to colour correlations. This is especially convenient for some matching algorithms, like MC@NLO, where a full analytic knowledge of the shower radiation pattern is needed to avoid double-counting. (The pT-ordered shower is described in [Sjo05], and the corrections for massive radiator and recoiler in [Nor01].)

          Technically, the radiation pattern is most conveniently represented in the rest frame of the final state of the hard subprocess. Then, for each parton at a time, the rest of the final state can be viewed as a single effective parton. This "parton" has a fixed invariant mass during the emission process, and takes the recoil without any changed direction of motion. The momenta of the individual new recoilers are then obtained by a simple common boost of the original ones.

          This alternative approach will miss out on the colour coherence phenomena. Specifically, with the whole subcollision mass as "dipole" mass, the phase space for subsequent emissions is larger than for the normal dipole algorithm. The phase space difference grows as more and more gluons are created, and thus leads to a way too steep multiplication of soft gluons. Therefore the main application is for the first one or few emissions of the shower, where a potential overestimate of the emission rate is to be corrected for anyway, by matching to the relevant matrix elements. Thereafter, subsequent emissions should be handled as before, i.e. with dipoles spanned between nearby partons. Furthermore, only the first (hardest) subcollision is handled with global recoils, since subsequent MPI's would not be subject to matrix element corrections anyway.

          In order for the mid-shower switch from global to local recoils to work, colours are traced and bookkept just as for normal showers; it is only that this information is not used in those steps where a global recoil is requested. (Thus, e.g., a gluon is still bookkept as one colour and one anticolour dipole end, with half the charge each, but with global recoil those two ends radiate identically.)

          TimeShower:globalRecoil On Off   (default = off)
          Alternative approach as above, where all final-state particles share the recoil of an emission.
          If off, then use the standard dipole-recoil approach.
          If on, use the alternative global recoil, but only for the first interaction, and only while the number of particles in the final state is at most TimeShower:nMaxGlobalRecoil before the branching.

          TimeShower:nMaxGlobalRecoil   (default = 2; minimum = 1)
          Represents the maximum number of particles in the final state for which the next final-state emission can be performed with the global recoil strategy. This number counts all particles, whether they are allowed to radiate or not, e.g. also Z^0. Also partons created by initial-state radiation emissions counts towards this sum, as part of the interleaved evolution. Without interleaved evolution this option would not make sense, since then a varying and large number of partons could already have been created by the initial-state radiation before the first final-state one, and then there is not likely to be any matrix elements available for matching.

          Two variations of the scheme outlined above are also available, (motivated by comparative studies within aMC@NLO). These studies indicate that global recoils should be used as sparsely as possible, in order to retain desirable features of the radiation pattern produced with the local recoil prescription.

          TimeShower:globalRecoilMode   (default = 0; minimum = 0; maximum = 2)
          Choice which splittings are produced with the global recoil approach.
          0 : Global recoil mode as outlined above, i.e. using global recoils until the number of final state particles exceeds TimeShower:nMaxGlobalRecoil.
          1 : Global recoil only for the first branching of final state legs that have an ancestor in the hard process, and if the maximal number of branchings generated according to the global recoil scheme (see TimeShower:nMaxGlobalBranch below) has not yet been reached.
          2 : Global recoil only if the first branching in the whole evolution is a timelike splitting of a parton in an event with Born-like kinematics (i.e.\ an S-event). The impact of global recoils should be minimal in this case. This option is only sensible for interleaved evolution.


          TimeShower:nMaxGlobalBranch   (default = -1)
          The maximum number of splittings in the final state for which the next final-state emission can be performed with the global recoil strategy. This number has to be set if TimeShower:globalRecoilMode = 1 or TimeShower:globalRecoilMode = 2

          TimeShower:nPartonsInBorn   (default = -1)
          The number of partons for Born-like phase space points. This number needs to be set if a different treatment of S-events (with Born-like kinematics) and H-events (with real-emission kinematics) is desired. This number has to be set if TimeShower:globalRecoilMode = 2.

          TimeShower:limitPTmaxGlobal On Off   (default = off)
          If on, limit the maximal pT produced in branchings in the global recoil scheme exactly as in the default (local) scheme. This means that the mass of the splitting dipole will set an upper bound for the pT of an emission. To be more explicit, this disallows emissions with pT larger than min{μstart 2, mD2/4}, with mD 2 = (√ (pr +ps)2 -m0,s)2 - m0,r2 , where the shower starting scale is μstart (i.e. SCALUP when reading LHE files, and Info.QFac() otherwise), r the radiating parton, and s the recoiling particle that would have been used in the local recoil scheme. This option is only used if wimpy showers are enabled.

          The global-recoil machinery does not work well with rescattering in the MPI machinery, since then the recoiling system is not uniquely defined. MultipartonInteractions:allowRescatter = off by default, so this is not a main issue. If both options are switched on, rescattering will only be allowed to kick in after the global recoil has ceased to be active, i.e. once the nMaxGlobalRecoil limit has been exceeded. This should not be a major conflict, since rescattering is mainly of interest at later stages of the downwards pT evolution.

          Further, it is strongly recommended to set TimeShower:MEcorrections = off (not default!), i.e. not to correct the emission probability to the internal matrix elements. The internal ME options do not cover any cases relevant for a multibody recoiler anyway, so no guarantees are given what prescription would come to be used. Instead, without ME corrections, a process-independent emission rate is obtained, and ";?>user hooks can provide the desired process-specific rejection factors.

          Radiation off octet onium states

          In the current implementation, charmonium and bottomonium production can proceed either through colour singlet or colour octet mechanisms, both of them implemented in terms of 2 -> 2 hard processes such as g g -> (onium) g. In the former case the state does not radiate and the onium therefore is produced in isolation, up to normal underlying-event activity. In the latter case the situation is not so clear, but it is sensible to assume that a shower can evolve. (Assuming, of course, that the transverse momentum of the onium state is sufficiently high that radiation is of relevance.)

          There could be two parts to such a shower. Firstly a gluon (or even a quark, though less likely) produced in a hard 2 -> 2 process can undergo showering into many gluons, whereof one branches into the heavy-quark pair. Secondly, once the pair has been produced, each quark can radiate further gluons. This latter kind of emission could easily break up a semibound quark pair, but might also create a new semibound state where before an unbound pair existed, and to some approximation these two effects should balance in the onium production rate. The showering "off an onium state" as implemented here therefore should not be viewed as an accurate description of the emission history step by step, but rather as an effective approach to ensure that the octet onium produced "in the hard process" is embedded in a realistic amount of jet activity. Of course both the isolated singlet and embedded octet are likely to be extremes, but hopefully the mix of the two will strike a reasonable balance. However, it is possible that some part of the octet production occurs in channels where it should not be accompanied by (hard) radiation. Therefore reducing the fraction of octet onium states allowed to radiate is a valid variation to explore uncertainties.

          If an octet onium state is chosen to radiate, the simulation of branchings is based on the assumption that the full radiation is provided by an incoherent sum of radiation off the quark and off the antiquark of the onium state. Thus the splitting kernel is taken to be the normal q -> q g one, multiplied by a factor of two. Obviously this is a simplification of a more complex picture, averaging over factors pulling in different directions. Firstly, radiation off a gluon ought to be enhanced by a factor 9/4 relative to a quark rather than the 2 now used, but this is a minor difference. Secondly, our use of the q -> q g branching kernel is roughly equivalent to always following the harder gluon in a g -> g g branching. This could give us a bias towards producing too hard onia. A soft gluon would have little phase space to branch into a heavy-quark pair however, so the bias may not be as big as it would seem at first glance. Thirdly, once the gluon has branched into a quark pair, each quark carries roughly only half of the onium energy. The maximum energy per emitted gluon should then be roughly half the onium energy rather than the full, as it is now. Thereby the energy of radiated gluons is exaggerated, i.e. onia become too soft. So the second and the third points tend to cancel each other.

          Finally, note that the lower cutoff scale of the shower evolution depends on the onium mass rather than on the quark mass, as it should be. Gluons below the octet-onium scale should only be part of the octet-to-singlet transition.

          TimeShower:octetOniumFraction   (default = 1.; minimum = 0.; maximum = 1.)
          Allow colour-octet charmonium and bottomonium states to radiate gluons. 0 means that no octet-onium states radiate, 1 that all do, with possibility to interpolate between these two extremes.

          TimeShower:octetOniumColFac   (default = 2.; minimum = 0.; maximum = 4.)
          The colour factor used used in the splitting kernel for those octet onium states that are allowed to radiate, normalized to the q -> q g splitting kernel. Thus the default corresponds to twice the radiation off a quark. The physically preferred range would be between 1 and 9/4.

          Weak showers

          The emission of W^+- and Z^0 gauge bosons off fermions is intended to become an integrated part of the initial- and final-state radiation frameworks, and is fully interleaved with QCD and QED emissions. Currently it is under development, and off by default. Another restriction is that there is no simulation of the full gamma^*/Z^0 interference: at low masses the QED shower involves a pure gamma^* component, whereas the weak shower generates a pure Z^0.

          Most events will not contain a W^+-/Z^0 emission at all, and in a shower framework it is not straightforward to force such emissions to happen without biasing the event sample in some respect. An option is available to enhance the emission rate artificially, but it is then the responsibility of the user to correct the cross section accordingly, and not to pick an enhancement so big that the probability for more than one emission is non-negligible. (It is not enough to assign an event weight 1/e^n where e is the enhancement factor and n is the number of emitted gauge bosons. This still misses to account for the change in phase space for late emissions by the effect of earlier ones, or equivalently for the unwanted change in the Sudakov form factor. See [Lon12a] for a detailed discussion and possible solutions.)

          Another enhancement probability is to only allow some specific W^+-/Z^0 decay modes. By default the shower is inclusive, since it should describe all that can happen with unit probability. This also holds even if the W^+- and Z^0 produced in the hard process have been restricted to specific decay channels. The trick that allows this is that two new "aliases" have been produced, a Zcopy with identity code 93 and a Wcopy with code 94. These copies are used specifically to bookkeep decay channels open for W^+-/Z^0 bosons produced in the shower. For the rest they are invisible, i.e. you will not find them in event listings. The separation into two sets of gauge bosons then also allows the selection of specific decay modes for 93 and 94, i.e. for only the gauge bosons produced in the shower. As above it is here up to the user to reweight the event to compensate for the bias introduced, and to watch out for possible complications. In this case there is no kinematics bias, but one would miss out on topologies where a not-selected decay channel could be part of the background to the selected one, notably when more than one gauge boson is produced.

          Note that the common theme is that a bias leads to an event-specific weight, since each event is unique. It also means that the cross-section information obtained e.g. by Pythia::stat() is misleading, since it has not been corrected for such weights. This is different from biases in a predetermined hard process, where the net reduction in cross section can be calculated once and for all at initialization, and events generated with unit weight thereafter.

          Special for the weak showers is that couplings are different for left- and righthanded fermions. With incoming unpolarized beams this should average out, at least so long as only one weak emission occurs. In the case of several weak emissions off the same fermion the correlation between them will carry a memory of the fermion helicity. Such a memory is retained for the affected dipole end, and is reflected in the Particle::pol() property, it being +1 (-1) for fermions considered righthanded (lefthanded), and 0 for the bulk where no choice has been made.

          The FSR shower emission is always matched to the matrix element for emission off a f fbar weak dipole. (Emission rates are normalized to the invariant mass of the dipole at the time of the weak emission, i.e. discounting the energy lost by previous QCD/QED emissions.) Also the angular distribution in the subsequent V = W^+-/Z^0 decay is matched to the matrix element expression for f fbar -> f fbar V -> f fbar f' fbar'. Afterwards the f' fbar' system undergoes showers and hadronization just like any W^+-/Z^0 decay products would.

          A few special switches are available for the weak framework, several mainly intended for tryout purposes, as follows.

          TimeShower:weakShower On Off   (default = off)
          Allow a weak shower, yes or no.

          TimeShower:weakShowerMode   (default = 0; minimum = 0; maximum = 2)
          Determine which branchings are allowed.
          option 0 : both W^+- and Z^0 branchings.
          option 1 : only W^+- branchings.
          option 2 : only Z^0 branchings.

            (default = 1.0; minimum = 0.1; maximum = 2.0)
          Parton shower cut-off pT for weak branchings.

          TimeShower:weakShowerEnhancement   (default = 1.; minimum = 1.; maximum = 1000.)
          Enhancement factor for the weak shower. This is used to increase the statistics of weak shower emissions. Remember afterwards to correct for the additional weak emissions (i.e. divide the rate of weak emissions by the same factor).

          TimeShower:singleWeakEmission On Off   (default = off)
          This parameter allows to stop the weak shower after a single emission.
          If on, only a single weak emission is allowed.
          If off, an unlimited number of weak emissions possible.

          TimeShower:extraScaleTerm   (default = 0.; minimum = 0.; maximum = 2.)
          The normal showers uses pT^2 as ordering variable, but for massive particles it could be preferred to use pT^2 + M^2 instead. This parameter allows to use pT^2 + k * M^2 for weak showers, thus k = 0 is the standard ordering and is used as default.

          TimeShower:dopTDampMass On Off   (default = on)
          Add an extra dampening to the weak shower to lower the production of low-pT W/Z's. The dampening is given by (pT^2 + 0.25 M^2)/ (pT^2 + M^2), where M^2 is the squared mass of the W/Z.

          Further variables

          There are several possibilities you can use to switch on or off selected branching types in the shower, or in other respects simplify the shower. These should normally not be touched. Their main function is for cross-checks.

          TimeShower:QCDshower On Off   (default = on)
          Allow a QCD shower, i.e. branchings q -> q g, g -> g g and g -> q qbar; on/off = true/false.

          TimeShower:nGluonToQuark   (default = 5; minimum = 0; maximum = 5)
          Number of allowed quark flavours in g -> q qbar branchings (phase space permitting). A change to 4 would exclude g -> b bbar, etc.

          TimeShower:QEDshowerByQ On Off   (default = on)
          Allow quarks to radiate photons, i.e. branchings q -> q gamma; on/off = true/false.

          TimeShower:QEDshowerByL On Off   (default = on)
          Allow leptons to radiate photons, i.e. branchings l -> l gamma; on/off = true/false.

          TimeShower:QEDshowerByGamma On Off   (default = on)
          Allow photons to branch into lepton or quark pairs, i.e. branchings gamma -> l+ l- and gamma -> q qbar; on/off = true/false.

          TimeShower:nGammaToQuark   (default = 5; minimum = 0; maximum = 5)
          Number of allowed quark flavours in gamma -> q qbar branchings (phase space permitting). A change to 4 would exclude g -> b bbar, etc.

          TimeShower:nGammaToLepton   (default = 3; minimum = 0; maximum = 3)
          Number of allowed lepton flavours in gamma -> l+ l- branchings (phase space permitting). A change to 2 would exclude gamma -> tau+ tau-, and a change to 1 also gamma -> mu+ mu-.

          TimeShower:MEcorrections On Off   (default = on)
          Use of matrix element corrections where available; on/off = true/false.

          TimeShower:MEafterFirst On Off   (default = on)
          Use of matrix element corrections also after the first emission, for dipole ends of the same system that did not yet radiate. Only has a meaning if MEcorrections above is switched on.

          TimeShower:phiPolAsym On Off   (default = on)
          Azimuthal asymmetry induced by gluon polarization; on/off = true/false.

          TimeShower:recoilToColoured On Off   (default = on)
          In the decays of coloured resonances, say t -> b W, it is not possible to set up dipoles with matched colours. Originally the b radiator therefore has W as recoiler, and that choice is unique. Once a gluon has been radiated, however, it is possible either to have the unmatched colour (inherited by the gluon) still recoiling against the W (off), or else let it recoil against the b also for this dipole (on). Before version 8.160 the former was the only possibility, which could give unphysical radiation patterns. It is kept as an option to check backwards compatibility. The same issue exists for QED radiation, but obviously is less significant. Consider the example W -> e nu, where originally the nu takes the recoil. In the old (off) scheme the nu would remain recoiler, while in the new (on) instead each newly emitted photon becomes the new recoiler. "?>
          pythia8-8.1.80.orig/phpdoc/EventAnalysis.php0000644000175000017500000013022012217615312017102 0ustar sunsun Event Analysis SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Event Analysis

          Introduction

          The routines in this section are intended to be used to analyze event properties. As such they are not part of the main event generation chain, but can be used in comparisons between Monte Carlo events and real data. They are rather free-standing, but assume that input is provided in the PYTHIA 8 Event format, and use a few basic facilities such as four-vectors. Their ordering is mainly by history; for current LHC applications the final one, SlowJet, is of special interest.

          In addition to the methods presented here, there is also the possibility to make use of ";?>external jet finders .

          Sphericity

          The standard sphericity tensor is
          S^{ab} = (sum_i p_i^a p_i^b) / (sum_i p_i^2)
          where the sum i runs over the particles in the event, a, b = x, y, z, and p without such an index is the absolute size of the three-momentum . This tensor can be diagonalized to find eigenvalues and eigenvectors.

          The above tensor can be generalized by introducing a power r, such that
          S^{ab} = (sum_i p_i^a p_i^b p_i^{r-2}) / (sum_i p_i^r)
          In particular, r = 1 gives a linear dependence on momenta and thus a collinear safe definition, unlike sphericity.

          To do sphericity analyses you have to set up a Sphericity instance, and then feed in events to it, one at a time. The results for the latest event are available as output from a few methods.

          Sphericity::Sphericity(double power = 2., int select = 2)  
          create a sphericity analysis object, where
          argument power (default = 2.) : is the power r defined above, i.e.
          argumentoption 2. : gives Sphericity, and
          argumentoption 1. : gives the linear form.
          argument select (default = 2) : tells which particles are analyzed,
          argumentoption 1 : all final-state particles,
          argumentoption 2 : all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and
          argumentoption 3 : only charged final-state particles.

          bool Sphericity::analyze( const Event& event, ostream& os = cout)  
          perform a sphericity analysis, where
          argument event : is an object of the Event class, most likely the pythia.event one.
          argument os (default = cout) : is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
          If the routine returns false the analysis failed, e.g. if too few particles are present to analyze.

          After the analysis has been performed, a few methods are available to return the result of the analysis of the latest event:

          double Sphericity::sphericity()  
          gives the sphericity (or equivalent if r is not 2),

          double Sphericity::aplanarity()  
          gives the aplanarity (with the same comment),

          double Sphericity::eigenValue(int i)  
          gives one of the three eigenvalues for i = 1, 2 or 3, in descending order,

          Vec4 Sphericity::eventAxis(i)  
          gives the matching normalized eigenvector, as a Vec4 with vanishing time/energy component.

          void Sphericity::list(ostream& os = cout)  
          provides a listing of the above information.

          There is also one method that returns information accumulated for all the events analyzed so far.

          int Sphericity::nError()  
          tells the number of times analyze(...) failed to analyze events, i.e. returned false.

          Thrust

          Thrust is obtained by varying the thrust axis so that the longitudinal momentum component projected onto it is maximized, and thrust itself is then defined as the sum of absolute longitudinal momenta divided by the sum of absolute momenta. The major axis is found correspondingly in the plane transverse to thrust, and the minor one is then defined to be transverse to both. Oblateness is the difference between the major and the minor values.

          The calculation of thrust is more computer-time-intensive than e.g. linear sphericity, introduced above, and has no specific advantages except historical precedent. In the PYTHIA 6 implementation the search was sped up at the price of then not being guaranteed to hit the absolute maximum. The current implementation studies all possibilities, but at the price of being slower, with time consumption for an event with n particles growing like n^3.

          To do thrust analyses you have to set up a Thrust instance, and then feed in events to it, one at a time. The results for the latest event are available as output from a few methods.

          Thrust::Thrust(int select = 2)  
          create a thrust analysis object, where
          argument select (default = 2) : tells which particles are analyzed,
          argumentoption 1 : all final-state particles,
          argumentoption 2 : all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and
          argumentoption 3 : only charged final-state particles.

          bool Thrust::analyze( const Event& event, ostream& os = cout)  
          perform a thrust analysis, where
          argument event : is an object of the Event class, most likely the pythia.event one.
          argument os (default = cout) : is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
          If the routine returns false the analysis failed, e.g. if too few particles are present to analyze.

          After the analysis has been performed, a few methods are available to return the result of the analysis of the latest event:

          double Thrust::thrust()  
          double Thrust::tMajor()  
          double Thrust::tMinor()  
          double Thrust::oblateness()  
          gives the thrust, major, minor and oblateness values, respectively,

          Vec4 Thrust::eventAxis(int i)  
          gives the matching normalized event-axis vectors, for i = 1, 2 or 3 corresponding to thrust, major or minor, as a Vec4 with vanishing time/energy component.

          void Thrust::list(ostream& os = cout)  
          provides a listing of the above information.

          There is also one method that returns information accumulated for all the events analyzed so far.

          int Thrust::nError()  
          tells the number of times analyze(...) failed to analyze events, i.e. returned false.

          ClusterJet

          ClusterJet (a.k.a. LUCLUS and PYCLUS) is a clustering algorithm of the type used for analyses of e^+e^- events, see the PYTHIA 6 manual. All visible particles in the events are clustered into jets. A few options are available for some well-known distance measures. Cutoff distances can either be given in terms of a scaled quadratic quantity like y = pT^2/E^2 or an unscaled linear one like pT.

          Note that we have deliberately chosen not to include the e^+e^- equivalents of the Cambridge/Aachen and anti-kRT algorithms. These tend to be good at clustering the densely populated (in angle) cores of jets, but less successful for the sparsely populated transverse regions, where many jets may come to consist of a single low-momentum particle. In hadron collisions such jets could easily be disregarded, while in e^+e^- annihilation all particles derive back from the hard process.

          To do jet finding analyses you have to set up a ClusterJet instance, and then feed in events to it, one at a time. The results for the latest event are available as output from a few methods.

          ClusterJet::ClusterJet(string measure = "Lund", int select = 2, int massSet = 2, bool precluster = false, bool reassign = false)  
          create a ClusterJet instance, where
          argument measure (default = "Lund") : distance measure, to be provided as a character string (actually, only the first character is necessary)
          argumentoption "Lund" : the Lund pT distance,
          argumentoption "JADE" : the JADE mass distance, and
          argumentoption "Durham" : the Durham kT measure.
          argument select (default = 2) : tells which particles are analyzed,
          argumentoption 1 : all final-state particles,
          argumentoption 2 : all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and
          argumentoption 3 : only charged final-state particles.
          argument massSet (default = 2) : masses assumed for the particles used in the analysis
          argumentoption 0 : all massless,
          argumentoption 1 : photons are massless while all others are assigned the pi+- mass, and
          argumentoption 2 : all given their correct masses.
          argument precluster (default = false) : perform or not a early preclustering step, where nearby particles are lumped together so as to speed up the subsequent normal clustering.
          argument reassign (default = false) : reassign all particles to the nearest jet each time after two jets have been joined.

          ClusterJet::analyze( const Event& event, double yScale, double pTscale, int nJetMin = 1, int nJetMax = 0, ostream& os = cout)  
          performs a jet finding analysis, where
          argument event : is an object of the Event class, most likely the pythia.event one.
          argument yScale : is the cutoff joining scale, below which jets are joined. Is given in quadratic dimensionless quantities. Either yScale or pTscale must be set nonvanishing, and the larger of the two dictates the actual value.
          argument pTscale : is the cutoff joining scale, below which jets are joined. Is given in linear quantities, such as pT or m depending on the measure used, but always in units of GeV. Either yScale or pTscale must be set nonvanishing, and the larger of the two dictates the actual value.
          argument nJetMin (default = 1) : the minimum number of jets to be reconstructed. If used, it can override the yScale and pTscale values.
          argument nJetMax (default = 0) : the maximum number of jets to be reconstructed. Is not used if below nJetMin. If used, it can override the yScale and pTscale values. Thus e.g. nJetMin = nJetMax = 3 can be used to reconstruct exactly 3 jets.
          argument os (default = cout) : is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
          If the routine returns false the analysis failed, e.g. because the number of particles was smaller than the minimum number of jets requested.

          After the analysis has been performed, a few ClusterJet class methods are available to return the result of the analysis:

          int ClusterJet::size()  
          gives the number of jets found, with jets numbered 0 through size() - 1.

          Vec4 ClusterJet::p(int i)  
          gives a Vec4 corresponding to the four-momentum defined by the sum of all the contributing particles to the i'th jet.

          int ClusterJet::mult(int i)  
          the number of particles that have been clustered into the i'th jet.

          int ClusterJet::jetAssignment(int i)  
          gives the index of the jet that the particle i of the event record belongs to,

          void ClusterJet::list(ostream& os = cout)  
          provides a listing of the reconstructed jets.

          int ClusterJet::distanceSize()  
          the number of most recent clustering scales that have been stored for readout with the next method. Normally this would be five, but less if fewer clustering steps occurred.

          double ClusterJet::distance(int i)  
          clustering scales, with distance(0) being the most recent one, i.e. normally the highest, up to distance(4) being the fifth most recent. That is, with n being the final number of jets, ClusterJet::size(), the scales at which n+1 jets become n, n+2 become n+1, and so on till n+5 become n+4. Nonexisting clustering scales are returned as zero. The physical interpretation of a scale is as provided by the respective distance measure (Lund, JADE, Durham).

          There is also one method that returns information accumulated for all the events analyzed so far.

          int ClusterJet::nError()  
          tells the number of times analyze(...) failed to analyze events, i.e. returned false.

          CellJet

          CellJet (a.k.a. PYCELL) is a simple cone jet finder in the UA1 spirit, see the PYTHIA 6 manual. It works in an (eta, phi, eT) space, where eta is pseudorapidity, phi azimuthal angle and eT transverse energy. It will draw cones in R = sqrt(Delta-eta^2 + Delta-phi^2) around seed cells. If the total eT inside the cone exceeds the threshold, a jet is formed, and the cells are removed from further analysis. There are no split or merge procedures, so later-found jets may be missing some of the edge regions already used up by previous ones. Not all particles in the event are assigned to jets; leftovers may be viewed as belonging to beam remnants or the underlying event. It is not used by any experimental collaboration, but is closely related to the more recent and better theoretically motivated anti-kT algorithm [Cac08].

          To do jet finding analyses you have to set up a CellJet instance, and then feed in events to it, one at a time. Especially note that, if you want to use the options where energies are smeared in order so emulate detector imperfections, you must hand in an external random number generator, preferably the one residing in the Pythia class. The results for the latest event are available as output from a few methods.

          CellJet::CellJet(double etaMax = 5., int nEta = 50, int nPhi = 32, int select = 2, int smear = 0, double resolution = 0.5, double upperCut = 2., double threshold = 0., Rndm* rndmPtr = 0)  
          create a CellJet instance, where
          argument etaMax (default = 5.) : the maximum +-pseudorapidity that the detector is assumed to cover.
          argument nEta (default = 50) : the number of equal-sized bins that the +-etaMax range is assumed to be divided into.
          argument nPhi (default = 32) : the number of equal-sized bins that the phi range +-pi is assumed to be divided into.
          argument select (default = 2) : tells which particles are analyzed,
          argumentoption 1 : all final-state particles,
          argumentoption 2 : all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and
          argumentoption 3 : only charged final-state particles.
          argument smear (default = 0) : strategy to smear the actual eT bin by bin,
          argumentoption 0 : no smearing,
          argumentoption 1 : smear the eT according to a Gaussian with width resolution * sqrt(eT), with the Gaussian truncated at 0 and upperCut * eT,
          argumentoption 2 : smear the e = eT * cosh(eta) according to a Gaussian with width resolution * sqrt(e), with the Gaussian truncated at 0 and upperCut * e.
          argument resolution (default = 0.5) : see above.
          argument upperCut (default = 2.) : see above.
          argument threshold (default = 0 GeV) : completely neglect all bins with an eT < threshold.
          argument rndmPtr (default = 0) : the random-number generator used to select the smearing described above. Must be handed in for smearing to be possible. If your Pythia class instance is named pythia, then &pythia.rndm would be the logical choice.

          bool CellJet::analyze( const Event& event, double eTjetMin = 20., double coneRadius = 0.7, double eTseed = 1.5, ostream& os = cout)  
          performs a jet finding analysis, where
          argument event : is an object of the Event class, most likely the pythia.event one.
          argument eTjetMin (default = 20. GeV) : is the minimum transverse energy inside a cone for this to be accepted as a jet.
          argument coneRadius (default = 0.7) : is the size of the cone in (eta, phi) space drawn around the geometric center of the jet.
          argument eTseed (default = 1.5 GeV) : the minimum eT in a cell for this to be acceptable as the trial center of a jet.
          argument os (default = cout) : is the output stream for error messages. (The method does not rely on the Info machinery for error messages.)
          If the routine returns false the analysis failed, but currently this is not foreseen ever to happen.

          After the analysis has been performed, a few CellJet class methods are available to return the result of the analysis:

          int CellJet::size()  
          gives the number of jets found, with jets numbered 0 through size() - 1,

          double CellJet::eT(i)  
          gives the eT of the i'th jet, where jets have been ordered with decreasing eT values,

          double CellJet::etaCenter(int i)  
          double CellJet::phiCenter(int i)  
          gives the eta and phi coordinates of the geometrical center of the i'th jet,

          double CellJet::etaWeighted(int i)  
          double CellJet::phiWeighted(int i)  
          gives the eta and phi coordinates of the eT-weighted center of the i'th jet,

          int CellJet::multiplicity(int i)  
          gives the number of particles clustered into the i'th jet,

          Vec4 CellJet::pMassless(int i)  
          gives a Vec4 corresponding to the four-momentum defined by the eT and the weighted center of the i'th jet,

          Vec4 CellJet::pMassive(int i)  
          gives a Vec4 corresponding to the four-momentum defined by the sum of all the contributing cells to the i'th jet, where each cell contributes a four-momentum as if all the eT is deposited in the center of the cell,

          double CellJet::m(int i)  
          gives the invariant mass of the i'th jet, defined by the pMassive above,

          void CellJet::list()  
          provides a listing of the above information (except pMassless, for reasons of space).

          There is also one method that returns information accumulated for all the events analyzed so far.

          int CellJet::nError()  
          tells the number of times analyze(...) failed to analyze events, i.e. returned false.

          SlowJet

          SlowJet is a simple program for doing jet finding according to either of the kT, anti-kT, and Cambridge/Aachen algorithms, in a cylindrical coordinate frame. The name is obviously an homage to the FastJet program [Cac06, Cac12]. That package contains many more algorithms, with many more options, and, above all, is much faster. Therefore SlowJet is not so much intended for massive processing of data or Monte Carlo files as for simple first tests. Nevertheless, within the advertised capabilities of SlowJet, it has been checked to find identically the same jets as FastJet. The time consumption typically is around or below that to generate an LHC pp event in the first place, so is not prohibitive. But the time rises rapidly for large multiplicities, so obviously SlowJet can not be used for tricks like distributing a dense grid of pseudoparticles to be able to define jet areas, like FastJet can, and also not for events with much pileup or other noise.

          The recent introduction of fjcore, containing the core functionality of FastJet in a very much smaller package, has changed the conditions. It now is possible (even encouraged by the authors) to distribute the two fjcore files as part of the PYTHIA package. Therefore the SlowJet class doubles as a convenient front end to fjcore, managing the conversion back and forth between PYTHIA and FastJet variables. Some applications may still benefit from using the native codes, but the default now is to let SlowJet call on fjcore for the jet finding.

          The first step is to decide which particles should be included in the analysis, and with what four-momenta. The SlowJet constructor allows to pick a maximum pseudorapidity defined by the extent of the assumed detector, to pick among some standard options of which particles to analyze, and to allow for some standard mass assumptions, like that all charged particles have the pion mass. Obviously this is only a restricted set of possibilities.

          Full flexibility can be obtained by deriving from the base class SlowJetHook to write your own include method. This will be presented with one final-state particle at a time, and should return true for those particles that should be analyzed. It is also possible to return modified four-momenta and masses, to take into account detector smearing effects or particle identity misassignments, but you must respect E^2 - p^2 = m^2.

          Alternatively you can modify the event record itself, or a copy of it (if you want to keep the original intact). For instance, only final particles are considered in the analysis, i.e. particles with positive status code, so negative status code should then be assigned to those particles that you do not want to see analyzed. Again four-momenta and masses can be modified, subject to E^2 - p^2 = m^2.

          The jet reconstructions is then based on sequential recombination with progressive removal, using the E recombination scheme. To be more specific, the algorithm works as follows.

          1. Each particle to be analyzed defines an original cluster. It has a well-defined four-momentum and mass at input. From this information the triplet (pT, y, phi) is calculated, i.e. the transverse momentum, rapidity and azimuthal angle of the cluster.
          2. Define distance measures of all clusters i to the beam
            d_iB = pT_i^2p
            and of all pairs (i,j) relative to each other
            d_ij = min( pT_i^2p, pT_j^2p) DeltaR_ij^2 / R^2
            where
            DeltaR_ij^2 = (y_i - y_j)^2 + (phi_i - phi_j)^2.
            The jet algorithm is determined by the user-selected p value, where p = -1 corresponds to the anti-kT one, p = 0 to the Cambridge/Aachen one and p = 1 to the kT one. Also R is chosen by the user, to give an approximate measure of the size of jets. However, note that jets need not have a circular shape in (y, phi) space, so R can not straight off be interpreted as a jet radius.
          3. Find the smallest of all d_iB and d_ij.
          4. If this is a d_iB then cluster i is removed from the clusters list and instead added to the jets list. Optionally, a pTjetMin requirement is imposed, where only clusters with pT > pTjetMin are added to the jets list. If so, some of the analyzed particles will not be part of any final jet.
          5. If instead the smallest measure is a d_ij then the four-momenta of the i and j clusters are added to define a single new cluster. Convert this four-momentum to a new (pT, y, phi) triplet and update the list of d_iB and d_ij.
          6. Return to step 3 until no clusters remain.

          To do jet finding analyses you first have to set up a SlowJet instance, where the arguments of the constructor specifies the details of the subsequent analyses. Thereafter you can feed in events to it, one at a time, and have them analyzed by the analyze method. Information on the resulting jets can be extracted by a few different methods. The minimal procedure only requires one call per event to do the analysis. We will begin by presenting it, and only afterwards some extensions.

          SlowJet::SlowJet(int power, double R, double pTjetMin = 0.,double etaMax = 25., int select = 2, int massSet = 2, SlowJetHook* sjHookPtr = 0, bool useFJcore = true, bool useStandardR = true)  
          create a SlowJet instance, where
          argument power : tells (half) the power of the transverse-momentum dependence of the distance measure,
          argumentoption -1 : the anti-kT algorithm,
          argumentoption 0 : the Cambridge/Aachen algorithm, and
          argumentoption 1 : the kT algorithm.
          argument R : the R size parameter, which is crudely related to the radius of the jet cone in (y, phi) space around the center of the jet.
          argument pTjetMin (default = 0.0 GeV) : the minimum transverse momentum required for a cluster to become a jet. By default all clusters become jets, and therefore all analyzed particles are assigned to a jet. For comparisons with perturbative QCD, however, it is only meaningful to consider jets with a significant pT.
          argument etaMax (default = 25.) : the maximum +-pseudorapidity that the detector is assumed to cover. If you pick a value above 20 there is assumed to be full coverage (obviously only meaningful for theoretical studies).
          argument select (default = 2) : tells which particles are analyzed,
          argumentoption 1 : all final-state particles,
          argumentoption 2 : all observable final-state particles, i.e. excluding neutrinos and other particles without strong or electromagnetic interactions (the isVisible() particle method), and
          argumentoption 3 : only charged final-state particles.
          argument massSet (default = 2) : masses assumed for the particles used in the analysis
          argumentoption 0 : all massless,
          argumentoption 1 : photons are massless while all others are assigned the pi+- mass, and
          argumentoption 2 : all given their correct masses.
          argument sjHookPtr (default = 0) : gives the possibility to send in your own selection routine for which particles should be part of the analysis; see further below on the SlowJetHook class. If this pointer is sent in nonzero, etaMax and massSet are disregarded, and select only gives the basic selection, to which the user can add further requirements.
          argument useFJcore (default = true) : choice of code used for finding the jets. Does not affect the outcome of the analysis, but only the speed, and some more specialized options.
          argumentoption true : use the fjcore package of FastJet 3.0.5.
          argumentoption false : use the native SlowJet implementation, which gives a slower jet finding, but allows some extra options of step-by-step jet joining.
          argument useStandardR (default = true) : definition of R distance between two jets. This switch is only meaningful for useFJcore = false; within the fjcore package the standard option below is always used.
          argumentoption true : standard, as described above, DeltaR_ij^2 = (y_i - y_j)^2 + (phi_i - phi_j)^2.
          argumentoption false : alternative, DeltaR_ij^2 = 2 (cosh(y_i - y_j) - cos(phi_i - phi_j)), which corresponds to the rim of the "deformed cone" giving a constant invariant mass between the two partons considered (for fixed masses and transverse momenta).

          bool SlowJet::analyze( const Event& event)  
          performs a jet finding analysis, where
          argument event : is an object of the Event class, most likely the pythia.event one.
          If the routine returns false the analysis failed, but currently this is not foreseen ever to happen.

          After the analysis has been performed, a few SlowJet class methods are available to return the result of the analysis:

          int SlowJet::sizeOrig()  
          gives the original number of particles (and thus clusters) that the analysis starts with.

          int SlowJet::sizeJet()  
          gives the number of jets found, with jets numbered 0 through sizeJet() - 1, and ordered in terms of decreasing transverse momentum values w.r.t. the beam axis,

          double SlowJet::pT(i)  
          gives the transverse momentum pT of the i'th jet,

          double SlowJet::y(int i)  
          double SlowJet::phi(int i)  
          gives the rapidity y and azimuthal angle phi of the center of the i'th jet (defined by the vector sum of constituent four-momenta),

          Vec4 SlowJet::p(int i)  
          double SlowJet::m(int i)  
          gives a Vec4 corresponding to the four-momentum sum of the particles assigned to the i'th jet, and the invariant mass of this four-vector,

          int SlowJet::multiplicity(int i)  
          gives the number of particles clustered into the i'th jet,

          vector<int> SlowJet::constituents(int i)  
          gives a list of the indices of the particles that have been clustered into the i'th jet,

          int SlowJet::jetAssignment(int i)  
          gives the index of the jet that the particle i of the event record belongs to, or -1 if there is no jet containing particle i,

          void SlowJet::removeJet(int i)  
          removes the i'th jet,

          void SlowJet::list()  
          provides a listing of the basic jet information from above.

          These are the basic methods. For more sophisticated usage it is possible to trace the clustering, one step at a time. It requires the native jet finding code, useFJcore = false in the constructor. If so, the setup method should be used to read in the event and find the initial smallest distance. Each subsequent doStep will then do one cluster joining and find the new smallest distance. You can therefore interrogate which clusters will be joined next before the joining actually is performed. Alternatively you can take several steps in one go, or take steps down to a predetermined number of jets plus remaining clusters.

          bool SlowJet::setup( const Event& event)  
          selects the particles to be analyzed, calculates initial distances, and finds the initial smallest distance.
          argument event : is an object of the Event class, most likely the pythia.event one.
          If the routine returns false the setup failed, but currently this is not foreseen ever to happen.

          bool SlowJet::doStep()  
          do the next step of the clustering. This can either be that two clusters are joined to one, or that a cluster is promoted to a jet (which is discarded if its pT value is below pTjetMin).
          The routine will only return false if there are no clusters left, or if useFJcore = true.

          bool SlowJet::doNSteps(int nStep)  
          calls the doStep() method nStep times, if possible. Will return false if the list of clusters is emptied before then. The stored jet information is still perfectly fine; it is only the number of steps that is wrong. Will also return false if useFJcore = true.

          bool SlowJet::stopAtN(int nStop)  
          calls the doStep() method until a total of nStop jet and cluster objects remain. Will return false if this is not possible, specifically if the number of objects already is smaller than nStop when the method is called. The stored jet and cluster information is still perfectly fine; it only does not have the expected multiplicity. Will also return false if useFJcore = true.

          int SlowJet::sizeAll()  
          gives the total current number of jets and clusters. The jets are numbered 0 through sizeJet() - 1, while the clusters are numbered sizeJet() through sizeAll() - 1. (Internally jets and clusters are represented by two separate arrays, but are here presented in one flat range.) Note that the jets are ordered in decreasing pT, while the clusters are not ordered. When useFJcore = true there are no intermediate steps, and thus the number of clusters is zero (after jet finding).

          With this extension, the methods double pT(int i), double y(int i), double phi(int i), Vec4 p(int i), double m(int i) and int multiplicity(int i) can be used as before. Furthermore, list() generalizes

          void SlowJet::list(bool listAll = false, ostream& os = cout)  
          provides a listing of the above information.
          argument listAll : lists both jets and clusters if true, else only jets.

          Three further methods can be used to check what will happen next.

          int SlowJet::iNext()  
          int SlowJet::jNext()  
          double SlowJet::dNext()  
          if the next step is to join two clusters, then the methods give the (i,j, d_ij) values, if instead to promote a cluster to a jet then (i, -1, d_iB). If no clusters remain then (-1, -1, 0.). Note that the cluster numbers are offset as described above, i.e. they begin at sizeJet(), which of course easily could be subtracted off. Also note that the jet and cluster lists are (moderately) reshuffled in each new step. When useFJcore = true there are no intermediate steps, and thus these methods do not return meaningul information.

          Finally, and separately, the SlowJetHook class can be used for a more smart selection of which particles to include in the analysis. For instance, isolated and/or high-pT muons, electrons and photons should presumably be identified separately at an early stage, and then not clustered to jets.

          Technically, it works like with ";?>User Hooks. That is, PYTHIA contains the base class. You write a derived class. In the main program you create an instance of this class, and hand it in to SlowJet; in this case already as part of the constructor.

          The following methods should be defined in your derived class.

          SlowJetHook::SlowJetHook()  
          virtual SlowJetHook::~SlowJetHook()  
          the constructor and destructor need not do anything, and if so you need not write your own destructor.

          virtual bool SlowJetHook::include(int iSel, const Event& event, Vec4& pSel, double& mSel)  
          is the main method that you will need to write. It will be called once for each final-state particle in an event, subject to the value of the select switch in the SlowJet constructor. The value select = 2 may be convenient since then you do not need to remove e.g. neutrinos yourself, but use select = 1 for full control. The method should then return true if you want to see particle included in the jet clustering, and false if not.
          argument iSel : is the index in the event record of the currently studied particle.
          argument event : is an object of the Event class, most likely the pythia.event one, where the currently studied particle is found.
          argument pSel : is at input the four-momentum of the currently studied particle. You can change the values, e.g. to take into account energy smearing in the detector, to define the initial cluster value, without corrupting the event record itself.
          argument mSel : is at input the mass of the currently studied particle. You can change the value, e.g. to take into account particle misidentification, to define the initial cluster value, without corrupting the event record itself. Note that the changes of pSel and mSel must be coordinated such that E^2 - p^2 = m^2 holds.

          It is also possible to define further methods of your own. One such could e.g. be called directly in the main program before the analyze method is called, to identify and bookkeep some event properties you may not want to reanalyze for each individual particle. pythia8-8.1.80.orig/phpdoc/PartonDistributions.php0000644000175000017500000001624312217615312020353 0ustar sunsun Parton Distributions SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Parton Distributions

          The parton distributions file contains the PDF class. PDF is the base class, from which specific PDF classes are derived.

          The choice of which PDF to use is made by settings in the Pythia class, see ";?>here. These settings also allow to access all the proton PDF's available in the LHAPDF library [Wha05]. Thus there is no need for a normal user to study the PDF class. The structure must only be understood when interfacing new PDF's, e.g. ones not yet found in LHAPDF.

          The PDF base class

          PDF defines the interface that all PDF classes should respect. The constructor requires the incoming beam species to be given: even if used for a proton PDF, one needs to know whether the beam is actually an antiproton. This is one of the reasons why Pythia always defines two PDF objects in an event, one for each beam.

          Once a PDF object has been constructed, call it pdf, the main method is pdf.xf( id, x, Q2), which returns x*f_id(x, Q2), properly taking into account whether the beam is an antiparticle or not.

          Whenever the xf member is called with a new flavour, x or Q^2, the xfUpdate member is called to do the actual updating. This routine may either update that particular flavour or all flavours at this (x, Q^2) point. (In the latter case the saved id value idSav should be set to 9.) The choice is to be made by the producer of a given set, based on what he/she deems most effective, given that sometimes only one flavour need be evaluated, and about equally often all flavours are needed at the same x and Q^2. Anyway, the latest value is always kept in memory. This is the other reason why Pythia has one separate PDF object for each beam, so that values at different x can be kept in memory.

          Two further public methods are xfVal( id, x, Q2) and xfSea( id, x, Q2). These are simple variants whereby the quark distributions can be subdivided into a valence and a sea part. If these are not directly accessible in the parametrization, one can make the simplified choices u_sea = ubar_sea, u_val = u_tot - u_sea, and correspondingly for d. (Positivity will always be guaranteed at output.) The xfUpdate method should also take care of updating this information.

          A method setExtrapolate(bool) allows you to switch between freezing parametrizations at the x and Q^2 boundaries (false) or extrapolating them outside the boundaries (true). This method is only implemented for the LHAPDF class below. If you implement a new PDF you are free to use this method, but it would be smarter to hardcode the desired limiting behaviour.

          Derived classes

          There is only one pure virtual method, xfUpdate, that therefore must be implemented in any derived class. A reasonable number of such classes come with the program:

          For protons:

          • LHAPDFinterface provides an interface to the LHAPDF library[Wha05].
          • GRV94L gives the GRV 94 L parametrization [Glu95].
          • CTEQ5L gives the CTEQ 5 L parametrization [Lai00].
          • MSTWpdf gives the four distributions of the MRST/MSTW group that have been implemented.
          • CTEQ6pdf gives the six distributions of the CTEQ/CT group that have been implemented.
          • NNPDF gives four distributions from the NNPDF 2.3 QCD+QED sets that have been implemented.
          The current default is CTEQ 5L, which has been used in most studies to date.

          For charged pions:

          • GRVpiL gives the GRV 1992 pi+ parametrization.

          For Pomerons (used to describe diffraction):

          • PomFix gives a simple but flexible Q2-independent parametrization.
          • PomH1FitAB gives the H1 2006 Fit A and Fit B parametrizations.
          • PomH1Jets gives the H1 2007 Jets parametrization.

          For charged leptons (e, mu, tau):

          • Lepton gives a QED parametrization [Kle89]. In QED there are not so many ambiguities, so here one set should be enough. On the other hand, there is the problem that the lepton-inside-lepton pdf is integrably divergent for x -> 1, which gives numerical problems. Like in PYTHIA 6, the pdf is therefore made to vanish for x > 1 - 10^{-10}, and scaled up in the range 1 - 10^{-7} < x < 1 - 10^{-10} in such a way that the total area under the pdf is preserved.
          • LeptonPoint gives the trivial distribution of a pointlike (i.e. unresolved) charged lepton.

          For neutrinos:

          • NeutrinoPoint is the only method, so there is no choice. Analogously to LeptonPoint it gives the distribution of a pointlike (i.e. unresolved) neutrino. A difference, however, is that neutrinos always are lefthanded, so there is no need to average over incoming spin states. Since the PYTHIA formalism assumes unpolarized beams, and thus implicitly includes a 1/2 for incoming fermions, the NeutrinoPoint PDF is normalized to 2 rather than 1 to compensate for this.

          There is another method, isSetup(), that returns the base-class boolean variable isSet. This variable is initially true, but could be set false if the setup procedure of a PDF failed, e.g. if the user has chosen an unknown PDF set.

          The MRST/MSTW, CTEQ/CT, NNPDF and H1 PDF routines are based on the interpolation in (x, Q) grids. The grid files are stored in the xmldoc subdirectory, like settings and particle data. Only PDF sets that will be used are read in during the initialization stage. pythia8-8.1.80.orig/phpdoc/SUSYProcesses.php0000644000175000017500000005743612217615312017030 0ustar sunsun SUSY Processes SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          SUSY

          Here is collected processes involving supersymmetric particle production, with the exception of the (extended) Higgs sector. Since the number of separate but closely related processes is so big, there will not be switches for each separate process but only for a reasonable set of subgroups. However, the general switches SUSY:idA and SUSY:idB,valternatively vectors SUSY:idVecA and SUSY:idVecB, may be used in conjunction with any of these groups to provide some additional flexibility to concentrate on processes involving only specific (s)particle final states, see below.

          Most of the SUSY implementation in PYTHIA 8 has been written by N. Desai and is documented in [Des11]. Please give due credit to external contributions to PYTHIA 8, such as this one, by including the original work in your list of references when using this implementation. The cross section formulae are mostly taken from [Boz07] and [Fuk11].

          Since the implementation of SUSY processes was only recently completed [Des11], case-by-case validations against other codes are still recommended. A set of default validations have already been carried out by the authors, comparing to the PYTHIA 6 SUSY implementation and to the XSUSY code, using an sps1a spectrum. Explicit validations of the non-trivial SLHA2-specific extensions have generally not been carried out yet, with the exception of the R-parity violating single-sparticle production cross sections. Please report the results of any user validations you may carry out to the authors.


          Important Note on SLHA: In order to simulate SUSY processes it is required to read in the couplings and masses relevant for the scenario to be studied. This is done with the help of the SUSY Les Houches Accord (SLHA), including the SLHA2 extensions and generalizations. (Internally, the SLHA2 conventions are used. SLHA1 spectra are automatically translated into SLHA2 notation during initialization.) The reading of a relevant SLHA file must be set up, as described on ";?>the SLHA page. Attempting to generate SUSY processes without a properly initialized SLHA spectrum is strongly discouraged and may lead to unexpected results. Always check for warnings and errors reported by the SLHA reader during the initialization stage.

          SUSY Processes


          Note 1: Decays of SUSY particles are described separately below.
          Note 2: One special possibility is that the gluino or some squark(s) are sufficiently long-lived to hadronize. See ";?>the R-hadrons page for further details.
          Note 3: lepton- and photon-initial states are not yet available. Only quark/gluon-initiated 2 -> 2 and 2 -> 1 (RPV) processes have been implemented.
          Note 4: cross sections will be correctly folded with open branching fractions of cascade decays, but at present any difference between particle and antiparticle decay tables is not taken into account. This possibility will be included in a future update.

          SUSY:all On Off   (default = off)
          Common switch for production of supersymmetric particles, i.e. particles with R-parity -1.

          SUSY:idA   (default = 0; minimum = 0)
          Option to limit the sum over possible outgoing states in SUSY 2 -> 2 processes to ones including a specific particle identity code. The default corresponds to summing over all possible indices. A non-zero value of SUSY:idA selects only processes that contain the state corresponding to that particular particle identity code in the fundamental 2 -> 2 scattering process (summed over particle/antiparticle). It is the user's responsibility to ensure that (a subset of) the processes to be simulated actually include this particle at the 2 -> 2 level; thus, asking for the lightest neutralino (code 1000021) to be present in a squark-squark production process will give no match.

          SUSY:idB   (default = 0; minimum = 0)
          As for SUSY:idA, but requires an additional particle with PDG code SUSY:idB to be present in the 2 -> 2 process. Thus, using SUSY:idA and SUSY:idB a specific subprocess can be selected. Again only the absolute sign is used, i.e. the summation over particle and antiparticle is retained. Also the order of SUSY:idA and SUSY:idB is irrelevant; since both possible orderings are checked for a match with the two outgoing particles. (Although not recommended, should SUSY:idA be zero and SUSY:idB nonzero a match is searched for just like in the normal case with SUSY:idA nonzero and SUSY:idB zero.)

          SUSY:idVecA   (default = 0; minimum = 0)
          As for SUSY:idA, but as a vector of PDG codes. (Character-string input of such vectors should be as a comma-separated list, without any blanks.) Thus, it selects only processes that have a final-state particle corresponding to one of the identity codes in this vector. Note that, to activate this, SUSY:idA must be equal to zero; if not then the match to SUSY:idA takes precedence.

          SUSY:idVecB   (default = 0; minimum = 0)
          As for SUSY:idB, but as a vector of PDG codes. (Character-string input of such vectors should be as a comma-separated list, without any blanks.) As above, to activate this, SUSY:idB must be equal to zero; if not then the match to SUSY:idB takes precedence. For the matching, either of SUSY:idA and SUSY:idVecA may be combined with either of SUSY:idB and SUSY:idVecB. As above one of the two outgoing SUSY particles must match one of the particles in SUSY:id(Vec)A and the other one of the particles in SUSY:id(Vec)B when both are nonzero.

          SUSY:sin2thetaWMode   (default = 2; minimum = 1; maximum = 3)
          The value of sin2(thetaW) should be taken from
          1 : SM value, defined at M_Z, taken from PYTHIA's StandardModel:sin2thetaW parameter.
          2 : SUSY value, defined at M_SUSY, derived from the running gauge couplings in BLOCK GAUGE in the SLHA file. Note: if no such block is present in the input file, this option will default back to option 1 above, i.e., the SM value.
          3 : Pole value, defined by 1 - M_W^2/M_Z^2, using the pole masses stored in the SLHA BLOCK MASS, or, alternatively, PYTHIA's internal pole masses if no such block is present.

          Gluino Pair Production



          SUSY:gg2gluinogluino On Off   (default = off)
          Pair production of gluinos by gluon-gluon initial states.

          SUSY:qqbar2gluinogluino On Off   (default = off)
          Pair production of gluinos by quark-antiquark annihilation and t-channel squark exchange. The cross section expression follows [Fuk11] and include the possibility of non-minimal flavour violation through misalignment of quarks with squarks. Only the MFV case has been explicitly validated.

          Associated Squark-Gluino Production



          SUSY:qg2squarkgluino On Off   (default = off)
          Associated production of a squark with a gluino. The cross section expression follows [Fuk11] and include the possibility of non-minimal flavour violation through misalignment of quarks with squarks. Only the MFV case has been explicitly validated.

          Squark Pair Production



          SUSY:gg2squarkantisquark On Off   (default = off)
          Pair production of a scalar quark together with a scalar antiquark by gluon annihilation via s-channel gluon exchange, t- and u-channel squark exchange, and the direct 4-point coupling. The cross section expression follows [Boz07]. Only the MFV case has been explicitly validated.

          SUSY:qqbar2squarkantisquark On Off   (default = off)
          Pair production of a scalar quark together with a scalar antiquark by quark-antiquark annihilation. For same-isospin ~q~q* production (i.e., ~u~u*, ~u~c*, ...), the s-channel gluon, photon, and Z and t-channel gluino contributions have so far been implemented (i.e., the t-channel neutralino contributions are neglected). For opposite-isospin ~q~q* production (~u~d*, ~u~s*, ...), the s-channel W and t-channel gluino contributions have been implemented (i.e., the t-channel neutralino contributions are neglected). The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated. (Note to PYTHIA 6 users: in older PYTHIA 6 versions, a bug caused the ~t1~t2* cross to be overcounted by a factor of 2. Starting from version 6.4.24, that generator now agrees with the implementation here.)

          SUSY:qqbar2squarkantisquark:onlyQCD On Off   (default = off)
          When switched on this flag switches off all but the s-channel gluon contribution in the calculation of same-isospin squark-antisquark production cross sections. Intended for reference only. For the most accurate physics simulation, leave this flag in the off position.

          SUSY:qq2squarksquark On Off   (default = off)
          Pair production of scalar quarks (squark-squark and its charge conjugate process; for squark-antisquark production see above) by t- and u-channel gluino, neutralino, and chargino exchange. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated. (Note to PYTHIA 6 users: PYTHIA 6 only included the gluino exchange contribution, which typically dominates due to the size of the strong coupling; for counterchecks, the flag SUSY:qq2squarksquark:onlyQCD below can be switched on to eliminate the chargino and neutralino contributions.)

          SUSY:qq2squarksquark:onlyQCD On Off   (default = off)
          When switched on this flag causes the t- or u-channel neutralino and chargino contributions to be ignored in the calculation of squark pair production cross sections. Intended for reference only. For the most accurate physics simulation, leave this flag in the off position.

          Neutralino and Chargino Pair Production



          SUSY:qqbar2chi0chi0 On Off   (default = off)
          Pair production of neutralinos by quark-antiquark annihilation. With four neutralino species this gives ten separate processes, codes 1201 - 1210. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated.

          SUSY:qqbar2chi+-chi0 On Off   (default = off)
          Associated chargino-neutralino production by quark-antiquark annihilation. With four neutralino species, two chargino ones, and maintaining charge conjugate processes separate, this gives 16 separate processes, codes 1221 - 1236. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated.

          SUSY:qqbar2chi+chi- On Off   (default = off)
          Pair production of charginos by quark-antiquark annihilation. With two chargino species and maintaining mutually charge conjugate processes separate, this gives four separate processes, codes 1241 - 1244. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated.

          Associated Neutralino/Chargino + Squark/Gluino Production



          SUSY:qg2chi0squark On Off   (default = off)
          Pair production of neutralinos from quark-gluon initial states. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated.

          SUSY:qg2chi+-squark On Off   (default = off)
          Associated chargino-squark production from quark-gluon initial states. annihilation. The cross section expressions follow [Boz07]. Only the MFV case has been explicitly validated.

          SUSY:qqbar2chi0gluino On Off   (default = off)
          Associated neutralino-gluino production by quark-antiquark annihilation. The cross section expressions follow [Fuk11]. Only the MFV case has been explicitly validated.

          SUSY:qqbar2chi+-gluino On Off   (default = off)
          Associated chargino-gluino production by quark-antiquark annihilation. The cross section expressions follow [Fuk11]. Only the MFV case has been explicitly validated. (Note to PYTHIA 6 users: small differences between this implementation and PYTHIA 6 arise due to slightly different treatments of the weak mixing angle, which is fixed in PYTHIA 6, while it is computed from the SLHA input in PYTHIA 8; see SUSY:sin2thetaWMode above.)

          Slepton Production



          SUSY:qqbar2sleptonantislepton On Off   (default = off)
          Pair production of slepton-antislepton via s-channel W, Z and gamma exchange. Includes both charged sleptons and sneutrinos but right handed sneutrinos currently not supported.

          R-parity violating squark production



          SUSY:qq2antisquark On Off   (default = off)
          Resonant squark production via R-parity violating UDD couplings. The couplings must be input using the SLHA2 structure.

          Decays of SUSY Particles

          Based on the parameters read in from the SLHA, PYTHIA 8 will normally compute the decay modes of SUSY particles automatically, using the SusyResonanceDecays class(es). Essentially all tree-level 2-body decays in the MSSM have been implemented this way, excepting so far only those involving Higgs bosons (either in the in- or out-state) or gravitinos. Available channels so far include:
          • ~q → q + ~chi
          • ~q → ~q + W/Z
          • ~q → q + q (RPV UDD)
          • ~q → l + q (RPV LQD)
          • ~g → ~q + q
          • ~chi → ~chi + Z/W
          • ~chi → ~q + q
          • ~chi → ~l/~nu + l/nu
          • ~chi0 → q + q + q (RPV UDD)
          • ~l/~nu → l/nu + ~chi
          • ~l/~nu → ~l/~nu + W/Z
          All channels are still undergoing validation, so this implementation should be considered preliminary. Still missing but to be included in a forthcoming update are: 3-body decays of charginos (via RPV), and 2-body decays of squarks and gauginos with Higgs as one of the decay products. Some 3-body decays have been implemented with Matrix Element weighting. In particular, those for a neutralino to a lighter neutralino and a fermion pair can be enabled.

          SUSYResonance:3BodyMatrixElement On Off   (default = off)
          When "on", the spin-averaged, squared matrix element is used to sample the phase space for resonance decay. Currently, only possible for a heavy neutralino decay to a light neutralino and a fermion-antifermion pair. "?>
          pythia8-8.1.80.orig/phpdoc/HadronLevelStandalone.php0000644000175000017500000003242312217615312020537 0ustar sunsun Hadron-Level Standalone SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Hadron-Level Standalone

          The Les Houches Accord allows external process-level configurations to be fed in, for subsequent parton-level and hadron-level generation to be handled internally by PYTHIA. There is no correspondingly standardized interface if you have external events that have also been generated through the parton-level stage, so that only the hadron-level remains to be handled. A non-standard way to achieve this exists, however, and can be useful both for real applications and for various tests of the hadronization model on its own.

          The key trick is to set the flag ProcessLevel:all = off. When pythia.next() is called it then does not try to generate a hard process. Since there are no beams, it is also not possible to perform the normal PartonLevel step. (It is still possible to generate final-state radiation, but this is not automatic. It would have to be done by hand, using the pythia.forceTimeShower(...) method, before pythia.next() is called.) Thus only the HadronLevel methods are called, to take the current content of the event record stored in pythia.event as a starting point for any hadronization and decays that are allowed by the normal parameters of this step. Often the input would consist solely of partons grouped into colour singlets, but also (colour-singlet) particles are allowed.

          To set up all the parameters, a pythia.init() call has to be used, without any arguments. In brief, the structure of the main program therefore should be something like

            Pythia pythia;                               // Declare generator.
            Event& event = pythia.event                  // Convenient shorthand.
            pythia.readString("ProcessLevel:all = off"); // The trick!
            pythia.init();                               // Initialization.
            for (int iEvent = 0; iEvent < nEvent; ++iEvent) {
              // Insert filling of event here!
              pythia.next();                             // Do the hadron level.
            }
          
          Of course this should be supplemented by analysis of events, error checks, and so on, as for a normal PYTHIA run. The unique aspect is how to fill the event inside the loop, before pythia.next() is called.

          Input configuration

          To set up a new configuration the first step is to throw away the current one, with event.reset(). This routine will also reserve the zeroth entry in the even record to represent the event as a whole.

          With the event.append(...) methods a new entry is added at the bottom of the current record, i.e. the first time it is called entry number 1 is filled, and so on. The append method basically exists in four variants, either without or with history information, and with four-momentum provided either as a Vec4 four-vector or as four individual components:

            append( id, status, col, acol, p, m)
            append( id, status, col, acol, px, py, pz, e, m)
            append( id, status, mother1, mother2, daughter1, daughter2, col, acol, p, m)
            append( id, status, mother1, mother2, daughter1, daughter2, col, acol, px, py, pz, e, m)
          
          The methods return the index at which the entry has been stored, but normally you would not use this feature.

          You can find descriptions of the input variables ";?>here. The PDG particle code id and the Les Houches Accord colour col and anticolour acol tags must be set correctly. The four-momentum and mass have to be provided in units of GeV; if you omit the mass it defaults to 0.

          Outgoing particles that should hadronize should be given status code 23. Often this is the only status code you need. You could e.g. also fill in incoming partons with -21 and intermediate ones with -22, if you so wish. Usually the choice of status codes is not crucial, so long as you recall that positive numbers correspond to particles that are still around, while negative numbers denote ones that already hadronized or decayed. However, so as not to run into contradictions with the internal PYTHIA checks (when Check:event = on), or with external formats such as HepMC, we do recommend the above codes. When pythia.next() is called the positive-status particles that hadronize/decay get the sign of the status code flipped to negative but the absolute value is retained. The new particles are added with normal PYTHIA status codes.

          For normal hadronization/decays in pythia.next() the history encoded in the mother and daughter indices is not used. Therefore the first two append methods, which set all these indices vanishing, should suffice. The subsequent hadronization/decays will still be properly documented.

          The exception is when you want to include junctions in your string topology, i.e. have three string pieces meet. Then you must insert in your event record the (decayed) particle that is the reason for the presence of a junction, e.g. a baryon beam remnant from which several valence quarks have been kicked out, or a neutralino that underwent a baryon-number-violating decay. This particle must have as daughters the three partons that together carry the baryon number.

          The sample program in main21.cc illustrates how you can work with this facility, both for simple parton configurations and for more complicated ones with junctions.

          As an alternative to setting up a topology with the methods above, a ";?>Les Houches Event File (LHEF) can also provide the configurations. Since no beams or processes are defined, only the <event>....</event> blocks need to be present, one for each event, so strictly it is not a true LHEF. You need to select Beams:frameType = 4, provide the file name in Beams:LHEF and, as above, set ProcessLevel:all = off. Needless to say, an externally linked LHAup class works as well as an LHEF, with Beams:frameType = 5.

          The event information to store in the LHEF, or provide by the LHAup, is essentially the same as above. The only difference is in status codes: outgoing particles should have 1 instead of 23, and intermediate resonances 2 instead of -22. Incoming partons, if any, are -1 instead of -21.

          Extensions to resonance decays

          With the above scheme, pythia.next() will generate hadronization, i.e. string fragmentation and subsequent decays of normal unstable particles. It will not decay ";?>resonances, i.e. W, Z, top, Higgs, SUSY and other massive particles.

          If the decay products are already provided, of course those products will be hadronized, but without any of the showers that one would expect in Z^0 -> q qbar, say. That is, the presence of a decayed resonance in the event record can be nice for documentation purposes, but otherwise it plays no role. It is possible to change this behaviour with the following flag.

          Standalone:allowResDec On Off   (default = off)
          If off, then resonances are stable if final-state particles, and irrelevant if intermediate particles. If on, then resonances are decayed, sequentially if necessary. After each decay step a parton shower is applied, and subsequent decay kinematics is shifted by the recoil of such branchings. If the decay chain and kinematics of the resonance is provided at input, this information is used, otherwise it is generated internally according to built-in branching ratios etc.

          The input configuration has to follow the rules described above, with ProcessLevel:all = off. (Terminology not quite consistent, since resonance decays normally is part of the process-level step.) It is possible to combine several resonances, and other coloured or uncoloured particles into the same event.

          Final-state radiation is applied to each step of the decay sequence by default, but can be switched off with PartonLevel:FSR = off or PartonLevel:FSRinResonances.

          Repeated hadronization or decay

          An alternative approach is possible with the pythia.forceHadronLevel() routine. This method does a call to the HadronLevel methods, irrespective of the value of the HadronLevel:all flag. If you hadronize externally generated events it is equivalent to a pythia.next() call with ProcessLevel:all = off.

          This method truly sticks to the hadron level, and thus cannot handle resonance decays. You therefore must not mix it with the Standalone:allowResDec = on framework.

          The similarity of names indicates that pythia.forceTimeShower( int iBeg, int iEnd, double pTmax, int nBranchMax = 0) is intended to belong to the same set of work-by-hand methods. Here iBeg and iEnd give the range of partons that should be allowed to shower, pTmax the maximum pT scale of emissions, and a nonzero nBranchMax a maximum number of allowed branchings. Additionally, a scale has to be set for each parton that should shower, which requires an additional final argument to the append methods above. This scale limits the maximum pT allowed for each parton, in addition to the global pTmax. When not set the scale defaults to 0, meaning no radiation for that parton.

          The real application instead is for repeated hadronization of the same PYTHIA process- and parton-level event. This may for some studies help to save time, given that these two first step are more time-consuming than the hadronization one.

          For repeated hadronization you should first generate an event as usual, but with HadronLevel:all = off. This event you can save in a temporary copy, e.g. Event savedEvent = pythia.event. Inside a loop you copy back with pythia.event = savedEvent, and call pythia.forceHadronLevel() to obtain a new hadronization history.

          A more limited form of repetition is if you want to decay a given kind of particle repeatedly, without having to generate the rest of the event anew. This could be the case e.g. in B physics applications. Then you can use the pythia.moreDecays() method, which decays all particles in the event record that have not been decayed but should have been done so. The pythia.particleData.mayDecay( id, false/true) method may be used to switch off/on the decays of a particle species id, so that it is not decayed in the pythia.next() call but only inside a loop over a number of tries.

          Between each loop the newly produced decay products must be removed and the decayed particle status restored to undecayed. The former is simple, since the new products are appended to the end of the event record: event.saveSize() saves the initial size of the event record, and event.restoreSize() can later be used repeatedly to restore this original size, which means that the new particles at the end are thrown away. The latter is more complicated, and requires the user to identify the positions of all particles of the species and restore a positive status code with event[i].statusPos().

          The main15.cc program illustrates both these methods, i.e. either repeated hadronization or repeated decay of PYTHIA events. "?>

          pythia8-8.1.80.orig/phpdoc/SaveSettings.php0000644000175000017500000002102012217615312016731 0ustar sunsun Save Settings SETTINGS SAVED TO FILE

          "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

          "; } } ?>

          Save Settings

          The information on this webpage is only valid if you access the PHP dynamic webpages via a web browser, and does not apply to the static HTML equivalents. With PHP, all of the settings in the PYTHIA program are represented by radio buttons or fill-in boxes, that makes it easy for you to construct a file with your desired changes. This file can then be read into PYTHIA by your main program to steer the whole run.

          Basic instructions

          The functionality of the PHP option is described in the following.

          "; if($_POST["resetval"] == 1) { //DELETE OLD FILE ON RESET unlink($_POST["rmfile"]); } if (!$_POST["filename"]) { echo "Please choose a (temporary) file name:
          "; echo ""; echo ""; echo ""; echo ""; } else if ($_POST["filename"] != "") { $filename = $_POST["filename"]; $filepath = "files/".$_POST["filename"]; $filecheck = file_exists($filepath); if(($_POST["finish"] == 1) || ($_GET["returning"] == 1)) { $filecheck = 0; $fileopen = 1; } if ($filecheck == 1) { echo "File in use.. choose again:
          "; echo "
          "; echo ""; echo ""; echo "
          "; } else { if(!$_POST["finish"]) { echo "Filename chosen: "; echo $_POST["filename"]; echo "
          "; echo ""; echo "
          "; echo ""; echo ""; echo ""; echo "
          "; echo ""; echo ""; echo ""; echo ""; echo "
          "; } if($fileopen != 1) { //CREATE & OPEN FILE & CHANGE PERMISSIONS TO 666 $handle = fopen($filepath, 'w'); chmod($filepath, 0666); fclose($handle); } if ($_POST["finish"]) { echo "
        • Right Click to Save Target: ".$filename."
          "; echo "
          "; echo ""; echo ""; echo ""; echo ""; echo "
          "; } } } echo "
        • "; ?>

          • To begin with, you must specify a (temporary) file name in the box above. If the filename already exists on the server, you will be requested to pick a new name.
          • Once you have Submitted your filename, you can browse through the pages and make your selections. The values currently selected when you load the page are the default values.
          • When you have finished making your changes to a particular page, you must click on Save Settings at the bottom of the page. This will write the changes to your temporary file. If you make a mistake, just repeat the procedure for that category again.

          • When you have finished all the changes you need, return to this page and click Finish File.
          • You will then get up a link, that you are asked to right-click with your mouse (or equivalent).
          • In the menu that appears, pick the option Save Link As (or equivalent).
          • You will now get up a file browser, for you to pick and Save the location and file name (the latter by default the same as the temporary file name).
          • At any time, if you click the RESET button, your temporary file will be erased and you can start anew.
          • Before you use a file, be sure to check it visually to confirm that you saved what you intended to. Minor corrections are easily made in a text editor.

          Supplementary notes

          The documentation files exist in three versions.

          1. As a set of .xml files, in the xmldoc/ subdirectory. These are the master copies that no user ever should touch, but that are used to generate the variants below.
          2. As a set of .html files, in the htmldoc/ subdirectory. You can open your own locally installed copy of the Welcome.html file in your web browser and thereafter navigate among all the pages. You can learn which parameters are free to be changed, but not change anything, except by brute-force cut-and-paste to a file of your own.
          3. As a set of .php files, in the phpdoc/ subdirectory. For these files to provide the functionality described above they have to accessed via a webserver. The one where you have your homepage should work fine. Alternatively you can use pages already available on another server.

          A few further comments about the operation of the PHP option:

          • To set up the PHP files on your webserver, you have to install the whole phpdoc/ subdirectory there. In addition to the .php code this includes a few more files, plus a subdirectory named files where the temporary files are stored. This subdirectory must have public write access to work (chmod a+w files if not).
          • The "temporary" files stored in files actually remain unless the RESET button is used. The good news is that this makes it possible to recover a file that otherwise might be lost. The bad news is that the files directory may need to be cleaned up from time to time. (But typically the files are pretty small, so this should not be a major problem.)
          • When you click the Save Settings button on the bottom of a page all changed settings are written on the temporary file in the format
            name-of-flag/mode/parameter/word = value
            
            with one variable per line. Thereafter all the settings on the page are restored to their default values.
          • You can return to a page to do some further changes and save those. If you change the same parameter twice, it is the last value that counts. (Both values are stored in the file, with the more recent lower down, and then PYTHIA does the changes sequentially.) However remember that unchanged values are not stored, so if you want to restore some default value it may be simpler to edit the file afterwards.
          • The changeable flags/modes/parameters/words are mainly in the "Setup Run Tasks" section of the index, but a few (less frequently used ones) can also be found lower down, in the "Study Output" and "Link to Other Programs" pages.

          • It is not (yet) possible to modify particle data within the PHP-based setup approach. This is a more difficult task, since e.g. the modifications one may want to do in a decay table can be quite interrelated. pythia8-8.1.80.orig/phpdoc/BeamRemnants.php0000644000175000017500000005074012217615312016701 0ustar sunsun Beam Remnants SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Beam Remnants

            Introduction

            The BeamParticle class contains information on all partons extracted from a beam (so far). As each consecutive multiparton interaction defines its respective incoming parton to the hard scattering a new slot is added to the list. This information is modified when the backwards evolution of the spacelike shower defines a new initiator parton. It is used, both for the multiparton interactions and the spacelike showers, to define rescaled parton densities based on the x and flavours already extracted, and to distinguish between valence, sea and companion quarks. Once the perturbative evolution is finished, further beam remnants are added to obtain a consistent set of flavours. The current physics framework is further described in [Sjo04].

            The introduction of ";?>rescattering in the multiparton interactions framework further complicates the processing of events. Specifically, when combined with showers, the momentum of an individual parton is no longer uniquely associated with one single subcollision. Nevertheless the parton is classified with one system, owing to the technical and administrative complications of more complete classifications. Therefore the addition of primordial kT to the subsystem initiator partons does not automatically guarantee overall pT conservation. Various tricks are used to minimize the mismatch, with a brute force shift of all parton pT's as a final step.

            Much of the above information is stored in a vector of ResolvedParton objects, which each contains flavour and momentum information, as well as valence/companion information and more. The BeamParticle method list() shows the contents of this vector, mainly for debug purposes.

            The BeamRemnants class takes over for the final step of adding primordial kT to the initiators and remnants, assigning the relative longitudinal momentum sharing among the remnants, and constructing the overall kinematics and colour flow. This step couples the two sides of an event, and could therefore not be covered in the BeamParticle class, which only considers one beam at a time.

            The methods of these classes are not intended for general use, and so are not described here.

            In addition to the parameters described on this page, note that the choice of ";?>parton densities is made in the Pythia class. Then pointers to the pdf's are handed on to BeamParticle at initialization, for all subsequent usage.

            Primordial kT

            The primordial kT of initiators of hard-scattering subsystems are selected according to Gaussian distributions in p_x and p_y separately. The widths of these distributions are chosen to be dependent on the hard scale of the central process and on the mass of the whole subsystem defined by the two initiators:
            sigma = (sigma_soft * Q_half + sigma_hard * Q) / (Q_half + Q) * m / (m_half + m)
            Here Q is the hard-process renormalization scale for the hardest process and the pT scale for subsequent multiparton interactions, m the mass of the system, and sigma_soft, sigma_hard, Q_half and m_half parameters defined below. Furthermore each separately defined beam remnant has a distribution of width sigma_remn, independently of kinematical variables.

            BeamRemnants:primordialKT On Off   (default = on)
            Allow or not selection of primordial kT according to the parameter values below.

            BeamRemnants:primordialKTsoft   (default = 0.5; minimum = 0.)
            The width sigma_soft in the above equation, assigned as a primordial kT to initiators in the soft-interaction limit.

            BeamRemnants:primordialKThard   (default = 2.0; minimum = 0.)
            The width sigma_hard in the above equation, assigned as a primordial kT to initiators in the hard-interaction limit.

            BeamRemnants:halfScaleForKT   (default = 1.; minimum = 0.)
            The scale Q_half in the equation above, defining the half-way point between hard and soft interactions.

            BeamRemnants:halfMassForKT   (default = 1.; minimum = 0.)
            The scale m_half in the equation above, defining the half-way point between low-mass and high-mass subsystems. (Kinematics construction can easily fail if a system is assigned a primordial kT value higher than its mass, so the mass-dampening is intended to reduce some troubles later on.)

            BeamRemnants:primordialKTremnant   (default = 0.4; minimum = 0.)
            The width sigma_remn, assigned as a primordial kT to beam-remnant partons.

            A net kT imbalance is obtained from the vector sum of the primordial kT values of all initiators and all beam remnants. This quantity is compensated by a shift shared equally between all partons, except that the dampening factor m / (m_half + m) is again used to suppress the role of small-mass systems.

            Note that the current sigma definition implies that <pT^2> = <p_x^2>+ <p_y^2> = 2 sigma^2. It thus cannot be compared directly with the sigma of nonperturbative hadronization, where each quark-antiquark breakup corresponds to <pT^2> = sigma^2 and only for hadrons it holds that <pT^2> = 2 sigma^2. The comparison is further complicated by the reduction of primordial kT values by the overall compensation mechanism.

            BeamRemnants:rescatterRestoreY On Off   (default = off)
            Is only relevant when ";?>rescattering is switched on in the multiparton interactions scenario. For a normal interaction the rapidity and mass of a system is preserved when primordial kT is introduced, by appropriate modification of the incoming parton momenta. Kinematics construction is more complicated for a rescattering, and two options are offered. Differences between these can be used to explore systematic uncertainties in the rescattering framework.
            The default behaviour is to keep the incoming rescattered parton as is, but to modify the unrescattered incoming parton so as to preserve the invariant mass of the system. Thereby the rapidity of the rescattering is modified.
            The alternative is to retain the rapidity (and mass) of the rescattered system when primordial kT is introduced. This is made at the expense of a modified longitudinal momentum of the incoming rescattered parton, so that it does not agree with the momentum it ought to have had by the kinematics of the previous interaction.
            For a double rescattering, when both incoming partons have already scattered, there is no obvious way to retain the invariant mass of the system in the first approach, so the second is always used.

            Colour flow

            The colour flows in the separate subprocesses defined in the multiparton-interactions scenario are tied together via the assignment of colour flow in the beam remnant. This is not an unambiguous procedure, but currently no parameters are directly associated with it. However, a simple "minimal" procedure of colour flow only via the beam remnants does not result in a scenario in agreement with data, notably not a sufficiently steep rise of <pT>(n_ch). The true origin of this behaviour and the correct mechanism to reproduce it remains one of the big unsolved issues at the borderline between perturbative and nonperturbative QCD. As a simple attempt, an additional step is introduced, wherein the gluons of a lower-pT system are merged with the ones in a higher-pT one.

            BeamRemnants:reconnectColours On Off   (default = on)
            Allow or not a system to be merged with another one.

            BeamRemnants:reconnectRange   (default = 10.0; minimum = 0.; maximum = 10.)
            A system with a hard scale pT can be merged with one of a harder scale with a probability that is pT0_Rec^2 / (pT0_Rec^2 + pT^2), where pT0_Rec is reconnectRange times pT0, the latter being the same energy-dependent dampening parameter as used for multiparton interactions. Thus it is easy to merge a low-pT system with any other, but difficult to merge two high-pT ones with each other.

            The procedure is used iteratively. Thus first the reconnection probability P = pT0_Rec^2 / (pT0_Rec^2 + pT^2) of the lowest-pT system is found, and gives the probability for merger with the second-lowest one. If not merged, it is tested with the third-lowest one, and so on. For the m'th higher system the reconnection probability thus becomes (1 - P)^(m-1) P. That is, there is no explicit dependence on the higher pT scale, but implicitly there is via the survival probability of not already having been merged with a lower-pT system. Also note that the total reconnection probability for the lowest-pT system in an event with n systems becomes 1 - (1 - P)^(n-1). Once the fate of the lowest-pT system has been decided, the second-lowest is considered with respect to the ones above it, then the third-lowest, and so on.

            Once it has been decided which systems should be joined, the actual merging is carried out in the opposite direction. That is, first the hardest system is studied, and all colour dipoles in it are found (including to the beam remnants, as defined by the holes of the incoming partons). Next each softer system to be merged is studied in turn. Its gluons are, in decreasing pT order, inserted on the colour dipole i,j that gives the smallest (p_g p_i)(p_g p_j)/(p_i p_j), i.e. minimizes the "disturbance" on the existing dipole, in terms of pT^2 or Lambda measure (string length). The insertion of the gluon means that the old dipole is replaced by two new ones. Also the (rather few) quark-antiquark pairs that can be traced back to a gluon splitting are treated in close analogy with the gluon case. Quark lines that attach directly to the beam remnants cannot be merged but are left behind.

            The joining procedure can be viewed as a more sophisticated variant of the one introduced already in [Sjo87]. Clearly it is ad hoc. It hopefully captures some elements of truth. The lower pT scale a system has the larger its spatial extent and therefore the larger its overlap with other systems. It could be argued that one should classify individual initial-state partons by pT rather than the system as a whole. However, for final-state radiation, a soft gluon radiated off a hard parton is actually produced at late times and therefore probably less likely to reconnect. In the balance, a classification by system pT scale appears sensible as a first try.

            Note that the reconnection is carried out before resonance decays are considered. Colour inside a resonance therefore is not reconnected. This is a deliberate choice, but certainly open to discussion and extensions at a later stage, as is the rest of this procedure.

            Further variables



            BeamRemnants:maxValQuark   (default = 3; minimum = 0; maximum = 5)
            The maximum valence quark kind allowed in acceptable incoming beams, for which multiparton interactions are simulated. Default is that hadrons may contain u, d and s quarks, but not c and b ones, since sensible kinematics has not really been worked out for the latter.

            BeamRemnants:companionPower   (default = 4; minimum = 0; maximum = 4)
            When a sea quark has been found, a companion antisea quark ought to be nearby in x. The shape of this distribution can be derived from the gluon mother distribution convoluted with the g -> q qbar splitting kernel. In practice, simple solutions are only feasible if the gluon shape is assumed to be of the form g(x) ~ (1 - x)^p / x, where p is an integer power, the parameter above. Allowed values correspond to the cases programmed.
            Since the whole framework is approximate anyway, this should be good enough. Note that companions typically are found at small Q^2, if at all, so the form is supposed to represent g(x) at small Q^2 scales, close to the lower cutoff for multiparton interactions.

            When assigning relative momentum fractions to beam-remnant partons, valence quarks are chosen according to a distribution like (1 - x)^power / sqrt(x). This power is given below for quarks in mesons, and separately for u and d quarks in the proton, based on the approximate shape of low-Q^2 parton densities. The power for other baryons is derived from the proton ones, by an appropriate mixing. The x of a diquark is chosen as the sum of its two constituent x values, and can thus be above unity. (A common rescaling of all remnant partons and particles will fix that.) An additional enhancement of the diquark momentum is obtained by its x value being rescaled by the valenceDiqEnhance factor.

            BeamRemnants:valencePowerMeson   (default = 0.8; minimum = 0.)
            The abovementioned power for valence quarks in mesons.

            BeamRemnants:valencePowerUinP   (default = 3.5; minimum = 0.)
            The abovementioned power for valence u quarks in protons.

            BeamRemnants:valencePowerDinP   (default = 2.0; minimum = 0.)
            The abovementioned power for valence d quarks in protons.

            BeamRemnants:valenceDiqEnhance   (default = 2.0; minimum = 0.5; maximum = 10.)
            Enhancement factor for valence diquarks in baryons, relative to the simple sum of the two constituent quarks.

            BeamRemnants:allowJunction On Off   (default = on)
            The off option is intended for debug purposes only, as follows. When more than one valence quark is kicked out of a baryon beam, as part of the multiparton interactions scenario, the subsequent hadronization is described in terms of a junction string topology. This description involves a number of technical complications that may make the program more unstable. As an alternative, by switching this option off, junction configurations are rejected (which gives an error message that the remnant flavour setup failed), and the multiparton interactions and showers are redone until a junction-free topology is found. "?>

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            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            PDF Selection

            This page contains five subsections. The first deals with how to pick the parton distribution set for protons, including from LHAPDF, to be used for all proton and antiproton beams. The second is a special option that allows a separate PDF set to be used for the hard process only, while the first choice would still apply to everything else. The third and fourth give access to pion and Pomeron PDF's, respectively, the latter being used to describe diffractive systems. The fifth gives the possibility to switch off the lepton "parton density". More information on PDF classes is found ";?>here.

            Parton densities for protons

            The selection of parton densities is made once and then is propagated through the program. It is essential to make an informed choice, for several reasons [Kas10]:
            Warning 1: the choice of PDF set affects a number of properties of events. A change of PDF therefore requires a complete retuning e.g. of the multiparton-interactions model for minimum-bias and underlying events.
            Warning 2: People often underestimate the differences between different sets on the market. The sets for the same order are constructed to behave more or less similarly at large x and Q^2, while the multiparton interactions are dominated by the behaviour in the region of small x and Q^2. A good PDF parametrization ought to be sensible down to x = 10^-6 (x = 10^-7) and Q^2 = 1 GeV^2 for Tevatron (LHC) applications. Unfortunately there are distributions on the market that completely derail in that region. The main51.cc and main52.cc programs in the examples subdirectory provide some examples of absolutely minimal sanity checks before a new PDF set is put in production.
            Warning 3: NLO and LO sets tend to have quite different behaviours, e.g. NLO ones have less gluons at small x, which then is compensated by positive corrections in the NLO matrix elements. Therefore do not blindly assume that an NLO tune has to be better than an LO one when combined with the LO matrix elements in PYTHIA. There are explicit examples where such thinking can lead you down the wrong alley, especially if you study low-pT physics. In the list below you should therefore be extra cautious when using set 6 or set 9.

            The simplest option is to pick one of the distributions available internally:

            PDF:pSet   (default = 2; minimum = 1; maximum = 16)
            Parton densities to be used for proton beams (and, by implication, antiproton ones):
            1 : GRV 94L, LO alpha_s(M_Z) = 0.128 (this set is out of date, but retained for historical comparisons).
            2 : CTEQ 5L, LO alpha_s(M_Z) = 0.127 (this set is also out of date, but not badly so, and many tunes are based on it).
            3 : MRST LO* (2007), NLO alpha_s(M_Z) = 0.12032.
            4 : MRST LO** (2008), NLO alpha_s(M_Z) = 0.11517.
            5 : MSTW 2008 LO (central member), LO alpha_s(M_Z) = 0.13939.
            6 : MSTW 2008 NLO (central member), NLO alpha_s(M_Z) = 0.12018 (NLO, see Warning 3 above).
            7 : CTEQ6L, NLO alpha_s(M_Z) = 0.1180.
            8 : CTEQ6L1, LO alpha_s(M_Z) = 0.1298.
            9 : CTEQ66.00 (NLO, central member), NLO alpha_s(M_Z) = 0.1180 (NLO, see Warning 3 above).
            10 : CT09MC1, LO alpha_s(M_Z) = 0.1300.
            11 : CT09MC2, NLO alpha_s(M_Z) = 0.1180.
            12 : CT09MCS, NLO alpha_s(M_Z) = 0.1180.
            13 : NNPDF2.3 QCD+QED LO alpha_s(M_Z) = 0.130.
            14 : NNPDF2.3 QCD+QED LO alpha_s(M_Z) = 0.119.
            15 : NNPDF2.3 QCD+QED NLO alpha_s(M_Z) = 0.119.
            16 : NNPDF2.3 QCD+QED NNLO alpha_s(M_Z) = 0.119.

            Note: the alpha_s(M_Z) values and the order of the running in the description above is purely informative, and does not affect any other parts of the program. Instead you have the freedom to set alpha_s(M_Z) value and running separately for ";?>hard processes (including resonance decays), ";?>multiparton interactions, ";?>initial-state radiation, and ";?>final-state radiation.

            This is a reasonably complete list of recent LO fits, both ones within the normal LO context and ones with modifications for better matching to event generators. In addition two older sets are included for backwards reference (most studies to date are based on CTEQ 5L). If you link to the LHAPDF library [Wha05] you get access to a much wider selection.
            Warning 1: owing to previous problems with the behaviour of PDF's beyond the x and Q^2 boundaries of a set, you should only use LHAPDF version 5.3.0 or later.
            Warning 2: the behaviour of the LHAPDF sets need not be identical with the implementation found in PYTHIA. Specifically we are aware of the following points that may influence a comparison.
            (a) CTEQ 5L in PYTHIA is the parametrization, in LHAPDF the grid interpolation.
            (b) MRST LO* and LO** in PYTHIA is based on an updated edition, where one makes use of the expanded MSTW grid format, while LHAPDF is based on the original smaller grid.
            (c) The CTEQ 6 and CT09MC sets in PYTHIA are frozen at the boundaries of the grid, by recommendation of the authors, while LHAPDF also offers an option with a smooth extrapolation outside the grid boundaries.

            PDF:useLHAPDF On Off   (default = off)
            If off then the choice of proton PDF is based on PDF:pSet above. If on then it is instead based on the choice of PDF:LHAPDFset and PDF:LHAPDFmember below.
            Note: in order for this option to work you must have compiled PYTHIA appropriately and have set the LHAPATH environment variable to provide the data-files directory of your local LHAPDF installation. See the README file in the examples directory for further instructions.

            PDF:LHAPDFset   (default = MRST2004FF4lo.LHgrid)
            Name of proton PDF set from LHAPDF to be used. You have to choose from the list of available sets. Examples of some fairly recent ones (but still less recent than found above) would be cteq61.LHpdf, cteq61.LHgrid, cteq6l.LHpdf, cteq6ll.LHpdf, MRST2004nlo.LHpdf, MRST2004nlo.LHgrid, MRST2004nnlo.LHgrid and MRST2004FF3lo.LHgrid. If you pick a LHpdf set it will require some calculation the first time it is called.
            Technical note: if you provide a name beginning with a slash (/) it is assumed you want to provide the full file path and then initPDFsetM(name) is called, else the correct path is assumed already set and initPDFsetByNameM(name) is called.

            PDF:LHAPDFmember   (default = 0; minimum = 0)
            Further choice of a specific member from the set picked above. Member 0 should normally correspond to the central value, with higher values corresponding to different error PDF's somewhat off in different directions. You have to check from set to set which options are open.
            Note: you can only use one member in a run, so if you want to sweep over many members you either have to do many separate runs or, as a simplification, save the ";?>pdf weights at the hard scattering and do an offline reweighting of events.

            PDF:extrapolateLHAPDF On Off   (default = off)
            Parton densities have a guaranteed range of validity in x and Q^2, and what should be done beyond that range usually is not explained by the authors of PDF sets. Nevertheless these boundaries very often are exceeded, e.g. minimum-bias studies at LHC may sample x values down to 10^-8, while many PDF sets stop already at 10^-5. The default behaviour is then that the PDF's are frozen at the boundary, i.e. xf(x,Q^2) is fixed at its value at x_min for all values x < x_min, and so on. This is a conservative approach. Alternatively, if you switch on extrapolation, then parametrizations will be extended beyond the boundaries, by some prescription. In some cases this will provide a more realistic answer, in others complete rubbish. Another problem is that some of the PDF-set codes will write a warning message anytime the limits are exceeded, thus swamping your output file. Therefore you should study a set seriously before you run it with this switch on.

            If you want to use PDF's not found in LHAPDF, or you want to interface LHAPDF another way, you have full freedom to use the more generic ";?>interface options.

            Parton densities for protons in the hard process

            The above options provides a PDF set that will be used everywhere: for the hard process, the parton showers and the multiparton interactions alike. As already mentioned, therefore a change of PDF should be accompanied by a complete retuning of the whole MPI framework, and maybe more. There are cases where one may want to explore different PDF options for the hard process, but would not want to touch the rest. If several different sets are to be compared, a simple reweighting based on the ";?>originally used flavour, x, Q^2 and PDF values may offer the best route. The options in this section allow a choice of the PDF set for the hard process alone, while the choice made in the previous section would still be used for everything else. The hardest interaction of the minimum-bias process is part of the multiparton-interactions framework and so does not count as a hard process here.

            Of course it is inconsistent to use different PDF's in different parts of an event, but if the x and Q^2 ranges mainly accessed by the components are rather different then the contradiction would not be too glaring. Furthermore, since standard PDF's are one-particle-inclusive we anyway have to 'invent' our own PDF modifications to handle configurations where more than one parton is kicked out of the proton [Sjo04].

            The PDF choices that can be made are the same as above, so we do not repeat the detailed discussion.

            PDF:useHard On Off   (default = off)
            If on then select a separate PDF set for the hard process, using the variables below. If off then use the same PDF set for everything, as already chosen above.

            PDF:pHardSet   (default = 2; minimum = 1; maximum = 16)
            Parton densities to be used for proton beams (and, by implication, antiproton ones):
            1 : GRV 94L, LO alpha_s(M_Z) = 0.128 (out of date).
            2 : CTEQ 5L, LO alpha_s(M_Z) = 0.127 (slightly out of date; many tunes are based on it).
            3 : MRST LO* (2007), NLO alpha_s(M_Z) = 0.12032.
            4 : MRST LO** (2008), NLO alpha_s(M_Z) = 0.11517.
            5 : MSTW 2008 LO (central member), LO alpha_s(M_Z) = 0.13939.
            6 : MSTW 2008 NLO (central member), LO alpha_s(M_Z) = 0.12018.
            7 : CTEQ6L, NLO alpha_s(M_Z) = 0.1180.
            8 : CTEQ6L1, LO alpha_s(M_Z) = 0.1298.
            9 : CTEQ66.00 (NLO, central member), NLO alpha_s(M_Z) = 0.1180.
            10 : CT09MC1, LO alpha_s(M_Z) = 0.1300.
            11 : CT09MC2, NLO alpha_s(M_Z) = 0.1180.
            12 : CT09MCS, NLO alpha_s(M_Z) = 0.1180.
            13 : NNPDF2.3 QCD+QED LO alpha_s(M_Z) = 0.130.
            14 : NNPDF2.3 QCD+QED LO alpha_s(M_Z) = 0.119.
            15 : NNPDF2.3 QCD+QED NLO alpha_s(M_Z) = 0.119.
            16 : NNPDF2.3 QCD+QED NNLO alpha_s(M_Z) = 0.119.


            PDF:useHardLHAPDF On Off   (default = off)
            If off then the choice of proton PDF is based on hardpPDFset above. If on then it is instead based on the choice of hardLHAPDFset and hardLHAPDFmember below. Note that if you want to use LHAPDF here, and you also use LHAPDF for the "normal" PDF set, then LHAPDF must have been compiled so as to handle (at least) two concurrent sets, with the configure statement --with-max-num-pdfsets=2.

            PDF:hardLHAPDFset   (default = MRST2004FF4lo.LHgrid)
            Name of proton PDF set from LHAPDF to be used.

            PDF:hardLHAPDFmember   (default = 0; minimum = 0)
            Further choice of a specific member from the set picked above.

            Note that there is no separate equivalent of the PDF:extrapolateLHAPDF flag specifically for the hard PDF. Since LHAPDF only has one global flag for extrapolation or not, the choice for the normal PDF's also applies to the hard ones.

            Parton densities for pions

            The parton densities of the pion are considerably less well known than those of the proton. There are only rather few sets on the market, and none particularly recent. Only one comes built-in, but others can be accessed from LHAPDF. Input parametrizations are for the pi+. >From this the pi- is obtained by charge conjugation and the pi0 from averaging (half the pions have d dbar valence quark content, half u ubar.

            Much of the switches are taken over from the proton case, with obvious modifications; therefore the description is briefer. Currently we have not seen the need to allow separate parton densities for hard processes. When using LHAPDF the PDF:extrapolateLHAPDF switch of the proton also applies to pions.

            PDF:piSet   (default = 1; minimum = 1; maximum = 1)
            Internal parton densities that can be used for pion beams, currently with only one choice.
            1 : GRV 92 L.


            PDF:piUseLHAPDF On Off   (default = off)
            If off then the choice of proton PDF is based on PDF:piSet above. If on then it is instead based on the choice of PDF:piLHAPDFset and PDF:piLHAPDFmember below.

            PDF:piLHAPDFset   (default = OWPI.LHgrid)
            Name of pion PDF set from LHAPDF to be used. You have to choose from the list of available sets.

            PDF:piLHAPDFmember   (default = 0; minimum = 0)
            Further choice of a specific member from the set picked above.

            Parton densities for Pomerons

            The Pomeron is introduced in the description of diffractive events, i.e. a diffractive system is viewed as a Pomeron-proton collision at a reduced CM energy. Here the PDF's are even less well known. Most experimental parametrizations are NLO, which makes them less well suited for Monte Carlo applications. Furthermore note that the momentum sum is arbitrarily normalized to a non-unity value.

            PDF:PomSet   (default = 6; minimum = 1; maximum = 6)
            Parton densities that can be used for Pomeron beams.
            1 : Q^2-independent parametrizations xf(x) = N_ab x^a (1 - x)^b, where N_ab ensures unit momentum sum. The a and b parameters can be set separately for the gluon and the quark distributions. The momentum fraction of gluons and quarks can be freely mixed, and production of s quarks can be suppressed relative to that of d and u ones, with antiquarks as likely as quarks. See further below how to set the six parameters of this approach.
            2 : pi0 distributions, as specified in the section above.
            3 : the H1 2006 Fit A NLO Q^2-dependent parametrization, based on a tune to their data H1P06, rescaled by the factor PomRescale below.
            4 : the H1 2006 Fit B NLO Q^2-dependent parametrization, based on a tune to their data H1P06, rescaled by the factor PomRescale below.
            5 : the H1 2007 Jets NLO Q^2-dependent parametrization, based on a tune to their data H1P07, rescaled by the factor PomRescale below.
            6 : the H1 2006 Fit B LO Q^2-dependent parametrization, based on a tune to their data H1P06, rescaled by the factor PomRescale below.


            PDF:PomGluonA   (default = 0.; minimum = -0.5; maximum = 2.)
            the parameter a in the ansatz xg(x) = N_ab x^a (1 - x)^b for option 1 above.

            PDF:PomGluonB   (default = 3.; minimum = 0.; maximum = 10.)
            the parameter b in the ansatz xg(x) = N_ab x^a (1 - x)^b for option 1 above.

            PDF:PomQuarkA   (default = 0.; minimum = -0.5; maximum = 2.)
            the parameter a in the ansatz xq(x) = N_ab x^a (1 - x)^b for option 1 above.

            PDF:PomQuarkB   (default = 3.; minimum = 0.; maximum = 10.)
            the parameter b in the ansatz xq(x) = N_ab x^a (1 - x)^b for option 1 above.

            PDF:PomQuarkFrac   (default = 0.2; minimum = 0.; maximum = 1.)
            the fraction of the Pomeron momentum carried by quarks for option 1 above, with the rest carried by gluons.

            PDF:PomStrangeSupp   (default = 0.5; minimum = 0.; maximum = 1.)
            the suppression of the s quark density relative to that of the d and u ones for option 1 above.

            PDF:PomRescale   (default = 1.0; minimum = 0.5; maximum = 5.0)
            Rescale the four H1 fits above by this uniform factor, e.g. to bring up their momentum sum to around unity. By default all three have a momentum sum of order 0.5, suggesting that a factor around 2.0 should be used. You can use examples/main51.cc to get a more precise value. Note that also other parameters in the ";?>diffraction framework may need to be retuned when this parameter is changed.

            Parton densities for leptons

            For electrons/muons/taus there is no need to choose between different parametrizations, since only one implementation is available, and should be rather uncontroversial (apart from some technical details). However, insofar as e.g. e^+ e^- data often are corrected back to a world without any initial-state photon radiation, it is useful to have a corresponding option available here.

            PDF:lepton On Off   (default = on)
            Use parton densities for lepton beams or not. If off the colliding leptons carry the full beam energy, if on part of the energy is radiated away by initial-state photons. In the latter case the initial-state showers will generate the angles and energies of the set of photons that go with the collision. In addition one collinear photon per beam carries any leftover amount of energy not described by shower emissions. If the initial-state showers are switched off these collinear photons will carry the full radiated energy.

            Neutrinos are always taken pointlike. Do note that the phase space selection machinery currently does not allow one resolved and one unresolved beam. For lepton-neutrino collisions to work you must therefore set PDF:lepton = off.

            Incoming parton selection

            There is one useful degree of freedom to restrict the set of incoming quark flavours for hard processes. It does not change the PDF's as such, only which quarks are allowed to contribute to the hard-process cross sections. Note that separate but similarly named modes are available for multiparton interactions and spacelike showers.

            PDFinProcess:nQuarkIn   (default = 5; minimum = 0; maximum = 5)
            Number of allowed incoming quark flavours in the beams; a change to 4 would thus exclude b and bbar as incoming partons, etc. "?>
            pythia8-8.1.80.orig/phpdoc/ProgramMethods.php0000644000175000017500000043467212217615312017272 0ustar sunsun Program Methods

            Program Methods

            This is an alphabetical index of all methods that are documented elsewhere on these pages, beginning with the few methods that do not belong to a class. Many of them are only intended for experts, while undocumented ones are only for code authors.

            Return type Method name Documentation page
            AlpgenHooks(...) Alpgen Event Interface
            friend double cosphi(...) Four-Vectors
            friend double cosphi(...) Four-Vectors
            friend double costheta(...) Four-Vectors
            friend double cross3(...) Four-Vectors
            friend double dot3(...) Four-Vectors
            PDF* getPDFPtr(...) Program Flow
            bool initAfterBeams() Alpgen Event Interface
            friend double m(...) Four-Vectors
            double m(...) Particle Properties
            friend double m2(...) Four-Vectors
            double m2(...) Particle Properties
            friend ostream& operator<<(...) Four-Vectors
            friend ostream& operator<<(...) Four-Vectors
            friend Vec4 operator*(...) Four-Vectors
            friend Vec4 operator*(...) Four-Vectors
            friend double operator*(...) Four-Vectors
            friend Hist operator*(...) Histograms
            friend Hist operator*(...) Histograms
            friend Hist operator*(...) Histograms
            friend Vec4 operator+(...) Four-Vectors
            friend Hist operator+(...) Histograms
            friend Hist operator+(...) Histograms
            friend Hist operator+(...) Histograms
            friend Vec4 operator-(...) Four-Vectors
            friend Hist operator-(...) Histograms
            friend Hist operator-(...) Histograms
            friend Hist operator-(...) Histograms
            friend Vec4 operator/(...) Four-Vectors
            friend Hist operator/(...) Histograms
            friend Hist operator/(...) Histograms
            friend Hist operator/(...) Histograms
            friend ostream& operator<<(...) Histograms
            ParticleDataEntry& particleDataEntry() Particle Properties
            friend double phi(...) Four-Vectors
            friend double phi(...) Four-Vectors
            friend double REtaPhi(...) Four-Vectors
            friend double RRapPhi(...) Four-Vectors
            void setResonancePtr(...) Particle Data Scheme
            friend void table(...) Histograms
            friend void table(...) Histograms
            friend double theta(...) Four-Vectors
            AlpgenPar::AlpgenPar(...) Alpgen Event Interface
            double AlpgenPar::getParam(...) Alpgen Event Interface
            int AlpgenPar::getParamAsInt(...) Alpgen Event Interface
            bool AlpgenPar::haveParam(...) Alpgen Event Interface
            bool AlpgenPar::parse(...) Alpgen Event Interface
            BeamShape::BeamShape() Beam Shape
            Vec4 BeamShape::deltaPA() Beam Shape
            Vec4 BeamShape::deltaPB() Beam Shape
            virtual void BeamShape::init(...) Beam Shape
            virtual void BeamShape::pick() Beam Shape
            Vec4 BeamShape::vertex() Beam Shape
            virtual BeamShape::~BeamShape() Beam Shape
            bool CellJet::analyze(...) Event Analysis
            CellJet::CellJet(...) Event Analysis
            double CellJet::eT(...) Event Analysis
            double CellJet::etaCenter(...) Event Analysis
            double CellJet::etaWeighted(...) Event Analysis
            void CellJet::list() Event Analysis
            double CellJet::m(...) Event Analysis
            int CellJet::multiplicity(...) Event Analysis
            int CellJet::nError() Event Analysis
            double CellJet::phiCenter(...) Event Analysis
            double CellJet::phiWeighted(...) Event Analysis
            Vec4 CellJet::pMassive(...) Event Analysis
            Vec4 CellJet::pMassless(...) Event Analysis
            int CellJet::size() Event Analysis
            ClusterJet::analyze(...) Event Analysis
            ClusterJet::ClusterJet(...) Event Analysis
            double ClusterJet::distance(...) Event Analysis
            int ClusterJet::distanceSize() Event Analysis
            int ClusterJet::jetAssignment(...) Event Analysis
            void ClusterJet::list(...) Event Analysis
            int ClusterJet::mult(...) Event Analysis
            int ClusterJet::nError() Event Analysis
            Vec4 ClusterJet::p(...) Event Analysis
            int ClusterJet::size() Event Analysis
            double CoupSM::af(...) Standard Model Parameters
            double CoupSM::af2(...) Standard Model Parameters
            double CoupSM::alphaEM(...) Standard Model Parameters
            double CoupSM::alphaS(...) Standard Model Parameters
            double CoupSM::alphaS1Ord(...) Standard Model Parameters
            double CoupSM::alphaS2OrdCorr(...) Standard Model Parameters
            double CoupSM::cos2thetaW() Standard Model Parameters
            CoupSM::CoupSM() Standard Model Parameters
            double CoupSM::ef(...) Standard Model Parameters
            double CoupSM::ef2(...) Standard Model Parameters
            double CoupSM::efvf(...) Standard Model Parameters
            double CoupSM::GF() Standard Model Parameters
            void CoupSM::init(...) Standard Model Parameters
            double CoupSM::Lambda3() Standard Model Parameters
            double CoupSM::Lambda4() Standard Model Parameters
            double CoupSM::Lambda5() Standard Model Parameters
            double CoupSM::lf(...) Standard Model Parameters
            double CoupSM::rf(...) Standard Model Parameters
            double CoupSM::sin2thetaW() Standard Model Parameters
            double CoupSM::sin2thetaWbar() Standard Model Parameters
            double CoupSM::t3f(...) Standard Model Parameters
            double CoupSM::V2CKMgen(...) Standard Model Parameters
            double CoupSM::V2CKMid(...) Standard Model Parameters
            int CoupSM::V2CKMpick(...) Standard Model Parameters
            double CoupSM::V2CKMsum(...) Standard Model Parameters
            double CoupSM::VCKMgen(...) Standard Model Parameters
            double CoupSM::VCKMid(...) Standard Model Parameters
            double CoupSM::vf(...) Standard Model Parameters
            double CoupSM::vf2(...) Standard Model Parameters
            double CoupSM::vf2af2(...) Standard Model Parameters
            double DecayChannel::bRatio() Particle Data Scheme
            void DecayChannel::bRatio(...) Particle Data Scheme
            bool DecayChannel::contains(...) Particle Data Scheme
            bool DecayChannel::contains(...) Particle Data Scheme
            bool DecayChannel::contains(...) Particle Data Scheme
            double DecayChannel::currentBR() Particle Data Scheme
            void DecayChannel::currentBR(...) Particle Data Scheme
            DecayChannel::DecayChannel(...) Particle Data Scheme
            bool DecayChannel::hasChanged() Particle Data Scheme
            int DecayChannel::meMode() Particle Data Scheme
            void DecayChannel::meMode(...) Particle Data Scheme
            int DecayChannel::multiplicity() Particle Data Scheme
            void DecayChannel::multiplicity(...) Particle Data Scheme
            int DecayChannel::onMode() Particle Data Scheme
            void DecayChannel::onMode(...) Particle Data Scheme
            double DecayChannel::onShellWidth() Particle Data Scheme
            void DecayChannel::onShellWidth(...) Particle Data Scheme
            void DecayChannel::onShellWidthFactor(...) Particle Data Scheme
            void DecayChannel::openSec(...) Particle Data Scheme
            double DecayChannel::openSec(...) Particle Data Scheme
            void DecayChannel::product(...) Particle Data Scheme
            int DecayChannel::product(...) Particle Data Scheme
            void DecayChannel::rescaleBR(...) Particle Data Scheme
            void DecayChannel::setHasChanged(...) Particle Data Scheme
            virtual bool DecayHandler::decay(...) External Decays
            int Event::append(...) Event Record
            int Event::append(...) Event Record
            int Event::append(...) Event Record
            int Event::append(...) Event Record
            int Event::append(...) Event Record
            Particle& Event::at(...) Event Record
            Particle& Event::back() Event Record
            void Event::bst(...) Event Record
            void Event::bst(...) Event Record
            void Event::bst(...) Event Record
            void Event::clear() Event Record
            int Event::copy(...) Event Record
            vector<int> Event::daughterList(...) Event Record
            Event::Event(...) Event Record
            Particle& Event::front() Event Record
            int Event::iBotCopy(...) Event Record
            int Event::iBotCopyId(...) Event Record
            void Event::init(...) Event Record
            void Event::initColTag(...) Event Record
            bool Event::isAncestor(...) Event Record
            int Event::iTopCopy(...) Event Record
            int Event::iTopCopyId(...) Event Record
            int Event::lastColTag() Event Record
            void Event::list() Event Record
            void Event::list(...) Event Record
            void Event::list(...) Event Record
            void Event::list(...) Event Record
            vector<int> Event::motherList(...) Event Record
            int Event::nextColTag() Event Record
            Event& Event::operator+=(...) Event Record
            Event& Event::operator=(...) Event Record
            Particle& Event::operator[](...) Event Record
            const Particle& Event::operator[](...) Event Record
            void Event::popBack(...) Event Record
            void Event::remove(...) Event Record
            void Event::reset() Event Record
            void Event::restorePtrs() Event Record
            void Event::rot(...) Event Record
            void Event::rotbst(...) Event Record
            double Event::scale() Event Record
            void Event::scale(...) Event Record
            double Event::scaleSecond() Event Record
            void Event::scaleSecond(...) Event Record
            int Event::setEvtPtr(...) Event Record
            vector<int> Event::sisterList(...) Event Record
            vector<int> Event::sisterListTopBot(...) Event Record
            int Event::size() Event Record
            int Event::statusHepMC(...) Event Record
            bool Event::undoDecay(...) Event Record
            void Hist::book(...) Histograms
            void Hist::fill(...) Histograms
            double Hist::getBinContent(...) Histograms
            int Hist::getEntries() Histograms
            Hist::Hist() Histograms
            Hist::Hist(...) Histograms
            Hist::Hist(...) Histograms
            Hist::Hist(...) Histograms
            void Hist::name(...) Histograms
            void Hist::null() Histograms
            Hist& Hist::operator*=(...) Histograms
            Hist& Hist::operator*=(...) Histograms
            Hist& Hist::operator*=(...) Histograms
            Hist& Hist::operator+=(...) Histograms
            Hist& Hist::operator+=(...) Histograms
            Hist& Hist::operator-=(...) Histograms
            Hist& Hist::operator-=(...) Histograms
            Hist& Hist::operator/=(...) Histograms
            Hist& Hist::operator=(...) Histograms
            bool Hist::sameSize(...) Histograms
            void Hist::table(...) Histograms
            void Hist::table(...) Histograms
            void Hist::takeLog(...) Histograms
            void Hist::takeSqrt() Histograms
            double Info::a0MPI() Event Information
            void Info::addCounter(...) Event Information
            double Info::alphaEM() Event Information
            double Info::alphaS() Event Information
            bool Info::atEndOfFile() Event Information
            double Info::bMPI() Event Information
            int Info::code() Event Information
            int Info::codeMPI(...) Event Information
            int Info::codeSub() Event Information
            double Info::eA() Event Information
            double Info::eB() Event Information
            double Info::eCM() Event Information
            double Info::eMPI(...) Event Information
            double Info::enhanceMPI() Event Information
            int Info::getCounter(...) Event Information
            bool Info::hasHistory() Event Information
            void Info::hasHistory(...) Event Information
            bool Info::hasSub() Event Information
            string Info::header(...) Event Information
            vector <string> Info::headerKeys() Event Information
            int Info::iAMPI(...) Event Information
            int Info::iBMPI(...) Event Information
            int Info::id1() Event Information
            int Info::id1pdf() Event Information
            int Info::id2() Event Information
            int Info::id2pdf() Event Information
            int Info::idA() Event Information
            int Info::idB() Event Information
            bool Info::isDiffractiveA() Event Information
            bool Info::isDiffractiveB() Event Information
            bool Info::isDiffractiveC() Event Information
            bool Info::isLHA() Event Information
            bool Info::isMinBias() Event Information
            bool Info::isNonDiffractive() Event Information
            bool Info::isResolved() Event Information
            bool Info::isValence1() Event Information
            bool Info::isValence2() Event Information
            int Info::lhaStrategy() Event Information
            void Info::list() Event Information
            double Info::m3Hat() Event Information
            double Info::m4Hat() Event Information
            double Info::mA() Event Information
            double Info::mB() Event Information
            double Info::mergingWeight() Event Information
            double Info::mergingWeightNLO() Event Information
            double Info::mHat() Event Information
            long Info::nAccepted(...) Event Information
            string Info::name() Event Information
            string Info::nameSub() Event Information
            int Info::nFinal() Event Information
            int Info::nFinalSub() Event Information
            int Info::nFSRinProc() Event Information
            int Info::nFSRinRes() Event Information
            int Info::nISR() Event Information
            int Info::nMPI() Event Information
            long Info::nSelected(...) Event Information
            long Info::nTried(...) Event Information
            double Info::pdf1() Event Information
            double Info::pdf2() Event Information
            double Info::phiHat() Event Information
            double Info::pT2Hat() Event Information
            double Info::pT2NowISR() Event Information
            void Info::pT2NowISR(...) Event Information
            double Info::pTHat() Event Information
            double Info::pTmaxFSR() Event Information
            double Info::pTmaxISR() Event Information
            double Info::pTmaxMPI() Event Information
            double Info::pTMPI(...) Event Information
            double Info::pTnow() Event Information
            double Info::pzA() Event Information
            double Info::pzB() Event Information
            double Info::Q2Fac() Event Information
            double Info::Q2Ren() Event Information
            double Info::QFac() Event Information
            double Info::QRen() Event Information
            double Info::s() Event Information
            double Info::scalup() Event Information
            void Info::setCounter(...) Event Information
            void Info::setHeader(...) Event Information
            double Info::sHat() Event Information
            double Info::sigmaErr(...) Event Information
            double Info::sigmaGen(...) Event Information
            double Info::tau() Event Information
            double Info::tHat() Event Information
            double Info::thetaHat() Event Information
            bool Info::tooLowPTmin() Event Information
            double Info::uHat() Event Information
            double Info::weight() Event Information
            double Info::weightSum() Event Information
            double Info::x1() Event Information
            double Info::x1pdf() Event Information
            double Info::x2() Event Information
            double Info::x2pdf() Event Information
            double Info::y() Event Information
            double Info::zNowISR() Event Information
            void Info::zNowISR(...) Event Information
            void LHAup::addParticle(...) Les Houches Accord
            void LHAup::addProcess(...) Les Houches Accord
            double LHAup::alphaQCD() Les Houches Accord
            double LHAup::alphaQED() Les Houches Accord
            void LHAup::closeFile(...) Les Houches Accord
            bool LHAup::closeLHEF(...) Les Houches Accord
            int LHAup::col1(...) Les Houches Accord
            int LHAup::col2(...) Les Houches Accord
            double LHAup::e(...) Les Houches Accord
            double LHAup::eBeamA() Les Houches Accord
            double LHAup::eBeamB() Les Houches Accord
            bool LHAup::eventLHEF(...) Les Houches Accord
            bool LHAup::fileFound() Les Houches Accord
            int LHAup::id(...) Les Houches Accord
            int LHAup::id1() Les Houches Accord
            int LHAup::id1pdf() Les Houches Accord
            int LHAup::id2() Les Houches Accord
            int LHAup::id2pdf() Les Houches Accord
            int LHAup::idBeamA() Les Houches Accord
            int LHAup::idBeamB() Les Houches Accord
            int LHAup::idProcess() Les Houches Accord
            int LHAup::idProcess(...) Les Houches Accord
            bool LHAup::initLHEF() Les Houches Accord
            LHAup::LHAup(...) Les Houches Accord
            void LHAup::listEvent(...) Les Houches Accord
            void LHAup::listInit(...) Les Houches Accord
            double LHAup::m(...) Les Houches Accord
            int LHAup::mother1(...) Les Houches Accord
            int LHAup::mother2(...) Les Houches Accord
            bool LHAup::newEventFile(...) Les Houches Accord
            istream* LHAup::openFile(...) Les Houches Accord
            bool LHAup::openLHEF(...) Les Houches Accord
            double LHAup::pdf1() Les Houches Accord
            double LHAup::pdf2() Les Houches Accord
            int LHAup::pdfGroupBeamA() Les Houches Accord
            int LHAup::pdfGroupBeamB() Les Houches Accord
            bool LHAup::pdfIsSet() Les Houches Accord
            int LHAup::pdfSetBeamA() Les Houches Accord
            int LHAup::pdfSetBeamB() Les Houches Accord
            double LHAup::px(...) Les Houches Accord
            double LHAup::py(...) Les Houches Accord
            double LHAup::pz(...) Les Houches Accord
            double LHAup::scale() Les Houches Accord
            double LHAup::scale(...) Les Houches Accord
            double LHAup::scalePDF() Les Houches Accord
            void LHAup::setBeamA(...) Les Houches Accord
            void LHAup::setBeamB(...) Les Houches Accord
            virtual bool LHAup::setEvent(...) Les Houches Accord
            void LHAup::setIdX(...) Les Houches Accord
            void LHAup::setInfoHeader(...) Les Houches Accord
            void LHAup::setInfoHeader(...) Les Houches Accord
            virtual bool LHAup::setInit() Les Houches Accord
            bool LHAup::setInitLHEF(...) Les Houches Accord
            bool LHAup::setNewEventLHEF(...) Les Houches Accord
            bool LHAup::setOldEventLHEF() Les Houches Accord
            void LHAup::setPdf(...) Les Houches Accord
            void LHAup::setProcess(...) Les Houches Accord
            void LHAup::setPtr(...) Les Houches Accord
            void LHAup::setStrategy(...) Les Houches Accord
            void LHAup::setXErr(...) Les Houches Accord
            void LHAup::setXMax(...) Les Houches Accord
            void LHAup::setXSec(...) Les Houches Accord
            int LHAup::sizePart() Les Houches Accord
            int LHAup::sizeProc() Les Houches Accord
            virtual bool LHAup::skipEvent(...) Les Houches Accord
            double LHAup::spin(...) Les Houches Accord
            int LHAup::status(...) Les Houches Accord
            int LHAup::strategy() Les Houches Accord
            double LHAup::tau(...) Les Houches Accord
            double LHAup::weight() Les Houches Accord
            double LHAup::x1() Les Houches Accord
            double LHAup::x1pdf() Les Houches Accord
            double LHAup::x2() Les Houches Accord
            double LHAup::x2pdf() Les Houches Accord
            double LHAup::xErr(...) Les Houches Accord
            double LHAup::xErrSum() Les Houches Accord
            double LHAup::xMax(...) Les Houches Accord
            double LHAup::xSec(...) Les Houches Accord
            double LHAup::xSecSum() Les Houches Accord
            virtual LHAup::~LHAup() Les Houches Accord
            bool LHAupAlpgen::addResonances() Alpgen Event Interface
            LHAupAlpgen::LHAupAlpgen(...) Alpgen Event Interface
            bool LHAupAlpgen::rescaleMomenta() Alpgen Event Interface
            void LHAupLHEF::closeAllFiles() Les Houches Accord
            virtual bool MergingHooks::canCutOnRecState() C K K W L Merging
            virtual double MergingHooks::dampenIfFailCuts(...) C K K W L Merging
            virtual bool MergingHooks::doCutOnRecState(...) C K K W L Merging
            virtual double MergingHooks::hardProcessME(...) C K K W L Merging
            MergingHooks::MergingHooks() C K K W L Merging
            int MergingHooks::nHardInLeptons() C K K W L Merging
            int MergingHooks::nHardInPartons() C K K W L Merging
            int MergingHooks::nHardOutLeptons() C K K W L Merging
            int MergingHooks::nHardOutPartons() C K K W L Merging
            int MergingHooks::nMaxJets() C K K W L Merging
            int MergingHooks::nResInCurrent() C K K W L Merging
            double MergingHooks::tms() C K K W L Merging
            virtual double MergingHooks::tmsDefinition(...) C K K W L Merging
            virtual MergingHooks::~MergingHooks() C K K W L Merging
            int Particle::acol() Particle Properties
            void Particle::bst(...) Particle Properties
            void Particle::bst(...) Particle Properties
            void Particle::bst(...) Particle Properties
            void Particle::bst(...) Particle Properties
            void Particle::bstback(...) Particle Properties
            void Particle::bstback(...) Particle Properties
            bool Particle::canDecay() Particle Properties
            double Particle::charge() Particle Properties
            int Particle::chargeType() Particle Properties
            int Particle::col() Particle Properties
            void Particle::cols(...) Particle Properties
            int Particle::colType() Particle Properties
            double Particle::constituentMass() Particle Properties
            int Particle::daughter1() Particle Properties
            int Particle::daughter2() Particle Properties
            void Particle::daughters(...) Particle Properties
            bool Particle::doExternalDecay() Particle Properties
            double Particle::e() Particle Properties
            double Particle::eCalc() Particle Properties
            double Particle::eT() Particle Properties
            double Particle::eT2() Particle Properties
            double Particle::eta() Particle Properties
            bool Particle::hasVertex() Particle Properties
            int Particle::iBotCopy() Particle Properties
            int Particle::iBotCopyId() Particle Properties
            int Particle::id() Particle Properties
            int Particle::idAbs() Particle Properties
            void Particle::index() Particle Properties
            bool Particle::isAncestor(...) Particle Properties
            bool Particle::isCharged() Particle Properties
            bool Particle::isDiquark() Particle Properties
            bool Particle::isFinal() Particle Properties
            bool Particle::isGluon() Particle Properties
            bool Particle::isHadron() Particle Properties
            bool Particle::isLepton() Particle Properties
            bool Particle::isNeutral() Particle Properties
            bool Particle::isParton() Particle Properties
            bool Particle::isQuark() Particle Properties
            bool Particle::isRescatteredIncoming() Particle Properties
            bool Particle::isResonance() Particle Properties
            bool Particle::isVisible() Particle Properties
            int Particle::iTopCopy() Particle Properties
            int Particle::iTopCopyId() Particle Properties
            double Particle::m() Particle Properties
            double Particle::m0() Particle Properties
            double Particle::m2() Particle Properties
            double Particle::m2Calc() Particle Properties
            bool Particle::mayDecay() Particle Properties
            double Particle::mCalc() Particle Properties
            double Particle::mMax() Particle Properties
            double Particle::mMin() Particle Properties
            int Particle::mother1() Particle Properties
            int Particle::mother2() Particle Properties
            void Particle::mothers(...) Particle Properties
            double Particle::mSel() Particle Properties
            double Particle::mT() Particle Properties
            double Particle::mT2() Particle Properties
            double Particle::mWidth() Particle Properties
            string Particle::name() Particle Properties
            string Particle::nameWithStatus() Particle Properties
            void Particle::offsetCol(...) Particle Properties
            void Particle::offsetHistory(...)) Particle Properties
            Particle& Particle::operator=(...) Particle Properties
            Vec4 Particle::p() Particle Properties
            void Particle::p(...) Particle Properties
            double Particle::pAbs() Particle Properties
            double Particle::pAbs2() Particle Properties
            Particle::Particle() Particle Properties
            Particle::Particle(...) Particle Properties
            Particle::Particle(...) Particle Properties
            Particle::Particle(...) Particle Properties
            double Particle::phi() Particle Properties
            double Particle::pNeg() Particle Properties
            double Particle::pol() Particle Properties
            double Particle::pPos() Particle Properties
            double Particle::pT() Particle Properties
            double Particle::pT2() Particle Properties
            double Particle::px() Particle Properties
            double Particle::py() Particle Properties
            double Particle::pz() Particle Properties
            void Particle::rescale3(...) Particle Properties
            void Particle::rescale4(...) Particle Properties
            void Particle::rescale5(...) Particle Properties
            void Particle::rot(...) Particle Properties
            void Particle::rotbst(...) Particle Properties
            double Particle::scale() Particle Properties
            void Particle::setEvtPtr(...) Particle Properties
            void Particle::setPDEPtr(...) Particle Properties
            vector<int> Particle::sisterList(...) Particle Properties
            int Particle::spinType() Particle Properties
            int Particle::status() Particle Properties
            int Particle::statusAbs() Particle Properties
            void Particle::statusCode(...) Particle Properties
            int Particle::statusHepMC() Particle Properties
            void Particle::statusNeg() Particle Properties
            void Particle::statusPos() Particle Properties
            double Particle::tau() Particle Properties
            double Particle::tau0() Particle Properties
            double Particle::tDec() Particle Properties
            double Particle::theta() Particle Properties
            double Particle::thetaXZ() Particle Properties
            double Particle::tProd() Particle Properties
            bool Particle::undoDecay() Particle Properties
            Vec4 Particle::vDec() Particle Properties
            Vec4 Particle::vProd() Particle Properties
            void Particle::vProd(...) Particle Properties
            double Particle::xDec() Particle Properties
            double Particle::xProd() Particle Properties
            double Particle::y() Particle Properties
            double Particle::yDec() Particle Properties
            double Particle::yProd() Particle Properties
            double Particle::zDec() Particle Properties
            double Particle::zProd() Particle Properties
            void ParticleData::addParticle(...) Particle Data Scheme
            void ParticleData::addParticle(...) Particle Data Scheme
            void ParticleData::antiName(...) Particle Data Scheme
            int ParticleData::baryonNumberType(...) Particle Data Scheme
            bool ParticleData::canDecay(...) Particle Data Scheme
            double ParticleData::charge(...) Particle Data Scheme
            void ParticleData::chargeType(...) Particle Data Scheme
            int ParticleData::chargeType(...) Particle Data Scheme
            void ParticleData::checkTable(...) Particle Data Scheme
            void ParticleData::checkTable(...) Particle Data Scheme
            void ParticleData::colType(...) Particle Data Scheme
            int ParticleData::colType(...) Particle Data Scheme
            double ParticleData::constituentMass(...) Particle Data Scheme
            bool ParticleData::doExternalDecay(...) Particle Data Scheme
            void ParticleData::doExternalDecays(...) Particle Data Scheme
            void ParticleData::doForceWidth(...) Particle Data Scheme
            bool ParticleData::doForceWidth(...) Particle Data Scheme
            bool ParticleData::hasAnti(...) Particle Data Scheme
            void ParticleData::hasChanged(...) Particle Data Scheme
            bool ParticleData::hasChanged(...) Particle Data Scheme
            int ParticleData::heaviestQuark(...) Particle Data Scheme
            bool ParticleData::init(...) Particle Data Scheme
            void ParticleData::initPtr(...) Particle Data Scheme
            void ParticleData::initWidths(...) Particle Data Scheme
            bool ParticleData::isBaryon(...) Particle Data Scheme
            bool ParticleData::isDiquark(...) Particle Data Scheme
            bool ParticleData::isGluon(...) Particle Data Scheme
            bool ParticleData::isHadron(...) Particle Data Scheme
            bool ParticleData::isLepton(...) Particle Data Scheme
            bool ParticleData::isMeson(...) Particle Data Scheme
            bool ParticleData::isOctetHadron(...) Particle Data Scheme
            bool ParticleData::isParticle(...) Particle Data Scheme
            bool ParticleData::isParton() Particle Data Scheme
            bool ParticleData::isQuark(...) Particle Data Scheme
            void ParticleData::isResonance(...) Particle Data Scheme
            bool ParticleData::isResonance(...) Particle Data Scheme
            void ParticleData::isVisible(...) Particle Data Scheme
            bool ParticleData::isVisible(...) Particle Data Scheme
            void ParticleData::list(...) Particle Data Scheme
            void ParticleData::list(...) Particle Data Scheme
            void ParticleData::list(...) Particle Data Scheme
            void ParticleData::listAll(...) Particle Data Scheme
            void ParticleData::listChanged(...) Particle Data Scheme
            void ParticleData::listChangedAndRes(...) Particle Data Scheme
            void ParticleData::listFF(...) Particle Data Scheme
            void ParticleData::listXML(...) Particle Data Scheme
            void ParticleData::m0(...) Particle Data Scheme
            double ParticleData::m0(...) Particle Data Scheme
            double ParticleData::m0Max(...) Particle Data Scheme
            double ParticleData::m0Min(...) Particle Data Scheme
            void ParticleData::mayDecay(...) Particle Data Scheme
            bool ParticleData::mayDecay(...) Particle Data Scheme
            void ParticleData::mMax(...) Particle Data Scheme
            double ParticleData::mMax(...) Particle Data Scheme
            void ParticleData::mMin(...) Particle Data Scheme
            double ParticleData::mMin(...) Particle Data Scheme
            double ParticleData::mRun(...) Particle Data Scheme
            double ParticleData::mSel(...) Particle Data Scheme
            void ParticleData::mWidth(...) Particle Data Scheme
            double ParticleData::mWidth(...) Particle Data Scheme
            void ParticleData::name(...) Particle Data Scheme
            string ParticleData::name(...) Particle Data Scheme
            void ParticleData::names(...) Particle Data Scheme
            int ParticleData::nextId(...) Particle Data Scheme
            ParticleData::ParticleData() Particle Data Scheme
            ParticleDataEntry* ParticleData::particleDataEntryPtr(...) Particle Data Scheme
            bool ParticleData::readFF(...) Particle Data Scheme
            bool ParticleData::readString(...) Particle Data Scheme
            bool ParticleData::readXML(...) Particle Data Scheme
            bool ParticleData::reInit(...) Particle Data Scheme
            void ParticleData::rescaleBR(...) Particle Data Scheme
            void ParticleData::resInit(...) Particle Data Scheme
            double ParticleData::resOpenFrac(...) Particle Data Scheme
            double ParticleData::resWidth(...) Particle Data Scheme
            double ParticleData::resWidthChan(...) Particle Data Scheme
            double ParticleData::resWidthOpen(...) Particle Data Scheme
            double ParticleData::resWidthRescaleFactor(...) Particle Data Scheme
            double ParticleData::resWidthStore(...) Particle Data Scheme
            void ParticleData::setAll(...) Particle Data Scheme
            void ParticleData::spinType(...) Particle Data Scheme
            int ParticleData::spinType(...) Particle Data Scheme
            void ParticleData::tau0(...) Particle Data Scheme
            double ParticleData::tau0(...) Particle Data Scheme
            bool ParticleData::useBreitWigner(...) Particle Data Scheme
            void ParticleDataEntry::addChannel(...) Particle Data Scheme
            int ParticleDataEntry::baryonNumberType(...) Particle Data Scheme
            bool ParticleDataEntry::canDecay(...) Particle Data Scheme
            DecayChannel& ParticleDataEntry::channel(...) Particle Data Scheme
            const DecayChannel& ParticleDataEntry::channel(...) Particle Data Scheme
            double ParticleDataEntry::charge(...) Particle Data Scheme
            int ParticleDataEntry::chargeType(...) Particle Data Scheme
            void ParticleDataEntry::clearChannels() Particle Data Scheme
            int ParticleDataEntry::colType(...) Particle Data Scheme
            double ParticleDataEntry::constituentMass() Particle Data Scheme
            bool ParticleDataEntry::doExternalDecay() Particle Data Scheme
            bool ParticleDataEntry::doForceWidth() Particle Data Scheme
            ResonanceWidths* ParticleDataEntry::getResonancePtr() Particle Data Scheme
            bool ParticleDataEntry::hasAnti() Particle Data Scheme
            void ParticleDataEntry::hasChanged(...) Particle Data Scheme
            int ParticleDataEntry::heaviestQuark(...) Particle Data Scheme
            int ParticleDataEntry::id() Particle Data Scheme
            void ParticleDataEntry::initBWmass() Particle Data Scheme
            void ParticleDataEntry::initPtr(...) Particle Data Scheme
            bool ParticleDataEntry::isBaryon() Particle Data Scheme
            bool ParticleDataEntry::isDiquark() Particle Data Scheme
            bool ParticleDataEntry::isGluon() Particle Data Scheme
            bool ParticleDataEntry::isHadron() Particle Data Scheme
            bool ParticleDataEntry::isLepton() Particle Data Scheme
            bool ParticleDataEntry::isMeson() Particle Data Scheme
            bool ParticleDataEntry::isOctetHadron() Particle Data Scheme
            bool ParticleDataEntry::isParton() Particle Data Scheme
            bool ParticleDataEntry::isQuark() Particle Data Scheme
            bool ParticleDataEntry::isResonance() Particle Data Scheme
            bool ParticleDataEntry::isVisible() Particle Data Scheme
            double ParticleDataEntry::m0() Particle Data Scheme
            double ParticleDataEntry::m0Max() Particle Data Scheme
            double ParticleDataEntry::m0Min() Particle Data Scheme
            bool ParticleDataEntry::mayDecay() Particle Data Scheme
            double ParticleDataEntry::mMax() Particle Data Scheme
            double ParticleDataEntry::mMin() Particle Data Scheme
            double ParticleDataEntry::mRun(...) Particle Data Scheme
            double ParticleDataEntry::mSel() Particle Data Scheme
            double ParticleDataEntry::mWidth() Particle Data Scheme
            string ParticleDataEntry::name(...) Particle Data Scheme
            ParticleDataEntry::ParticleDataEntry(...) Particle Data Scheme
            ParticleDataEntry::ParticleDataEntry(...) Particle Data Scheme
            DecayChannel& ParticleDataEntry::pickChannel() Particle Data Scheme
            bool ParticleDataEntry::preparePick(...) Particle Data Scheme
            void ParticleDataEntry::rescaleBR(...) Particle Data Scheme
            void ParticleDataEntry::resInit(...) Particle Data Scheme
            double ParticleDataEntry::resOpenFrac(...) Particle Data Scheme
            double ParticleDataEntry::resWidth(...) Particle Data Scheme
            double ParticleDataEntry::resWidthChan(...) Particle Data Scheme
            double ParticleDataEntry::resWidthOpen(...) Particle Data Scheme
            double ParticleDataEntry::resWidthRescaleFactor() Particle Data Scheme
            double ParticleDataEntry::resWidthStore(...) Particle Data Scheme
            void ParticleDataEntry::setAll(...) Particle Data Scheme
            void ParticleDataEntry::setAntiName(...) Particle Data Scheme
            void ParticleDataEntry::setChargeType(...) Particle Data Scheme
            void ParticleDataEntry::setColType(...) Particle Data Scheme
            void ParticleDataEntry::setDefaults() Particle Data Scheme
            void ParticleDataEntry::setDoExternalDecays(...) Particle Data Scheme
            void ParticleDataEntry::setDoForceWidth(...) Particle Data Scheme
            void ParticleDataEntry::setHasChanged(...) Particle Data Scheme
            void ParticleDataEntry::setIsResonance(...) Particle Data Scheme
            void ParticleDataEntry::setIsVisible(...) Particle Data Scheme
            void ParticleDataEntry::setM0(...) Particle Data Scheme
            void ParticleDataEntry::setMayDecay(...) Particle Data Scheme
            void ParticleDataEntry::setMMax(...) Particle Data Scheme
            void ParticleDataEntry::setMMin(...) Particle Data Scheme
            void ParticleDataEntry::setMWidth(...) Particle Data Scheme
            void ParticleDataEntry::setName(...) Particle Data Scheme
            void ParticleDataEntry::setNames(...) Particle Data Scheme
            void ParticleDataEntry::setResonancePtr(...) Particle Data Scheme
            void ParticleDataEntry::setSpinType(...) Particle Data Scheme
            void ParticleDataEntry::setTau0(...) Particle Data Scheme
            int ParticleDataEntry::sizeChannels() Particle Data Scheme
            int ParticleDataEntry::spinType() Particle Data Scheme
            double ParticleDataEntry::tau0() Particle Data Scheme
            bool ParticleDataEntry::useBreitWigner() Particle Data Scheme
            ParticleDataEntry::~ParticleDataEntry Particle Data Scheme
            void AlpgenPar::void printParams() Alpgen Event Interface
            bool Pythia8ToHepMC::convert_gluon_to_0() HepMC Interface
            bool Pythia8ToHepMC::crash_on_problem() HepMC Interface
            bool Pythia8ToHepMC::fill_next_event(...) HepMC Interface
            bool Pythia8ToHepMC::fill_next_event(...) HepMC Interface
            bool Pythia8ToHepMC::free_parton_warnings() HepMC Interface
            bool Pythia8ToHepMC::print_inconsistency() HepMC Interface
            Pythia8ToHepMC::Pythia8ToHepMC() HepMC Interface
            void Pythia8ToHepMC::set_convert_gluon_to_0(...) HepMC Interface
            void Pythia8ToHepMC::set_crash_on_problem(...) HepMC Interface
            void Pythia8ToHepMC::set_free_parton_warnings(...) HepMC Interface
            void Pythia8ToHepMC::set_print_inconsistency(...) HepMC Interface
            void Pythia8ToHepMC::set_store_pdf(...) HepMC Interface
            void Pythia8ToHepMC::set_store_proc(...) HepMC Interface
            void Pythia8ToHepMC::set_store_xsec(...) HepMC Interface
            bool Pythia8ToHepMC::store_pdf() HepMC Interface
            bool Pythia8ToHepMC::store_proc() HepMC Interface
            bool Pythia8ToHepMC::store_xsec() HepMC Interface
            virtual Pythia8ToHepMC::~Pythia8ToHepMC() HepMC Interface
            CoupSM Pythia::coupSM Program Flow
            Event Pythia::event Program Flow
            bool Pythia::flag(...) Program Flow
            bool Pythia::forceHadronLevel(...) Program Flow
            bool Pythia::forceRHadronDecays() Program Flow
            int Pythia::forceTimeShower(...) Program Flow
            Info Pythia::info Program Flow
            bool Pythia::init() Program Flow
            bool Pythia::init(...) Program Flow
            bool Pythia::init(...) Program Flow
            bool Pythia::init(...) Program Flow
            bool Pythia::init(...) Program Flow
            bool Pythia::init(...) Program Flow
            void Pythia::LHAeventList(...) Program Flow
            bool Pythia::LHAeventSkip(...) Program Flow
            int Pythia::mode(...) Program Flow
            bool Pythia::moreDecays() Program Flow
            bool Pythia::next() Program Flow
            double Pythia::parm(...) Program Flow
            ParticleData Pythia::particleData Program Flow
            PartonSystems Pythia::partonSystems Program Flow
            Event Pythia::process Program Flow
            Pythia::Pythia(...) Program Flow
            bool Pythia::readFile(...) Program Flow
            bool Pythia::readFile(...) Program Flow
            bool Pythia::readFile(...) Program Flow
            bool Pythia::readFile(...) Program Flow
            bool Pythia::readString(...) Program Flow
            Rndm Pythia::rndm Program Flow
            bool Pythia::setBeamShapePtr(...) Program Flow
            bool Pythia::setDecayPtr(...) Program Flow
            bool Pythia::setLHAupPtr(...) Program Flow
            bool Pythia::setPDFPtr(...) Program Flow
            bool Pythia::setResonancePtr(...) Program Flow
            bool Pythia::setRndmEnginePtr(...) Program Flow
            bool Pythia::setShowerPtr(...) Program Flow
            bool Pythia::setSigmaPtr(...) Program Flow
            Settings Pythia::settings Program Flow
            bool Pythia::setUserHooksPtr(...) Program Flow
            SusyLesHouches Pythia::slha Program Flow
            void Pythia::stat() Program Flow
            void Pythia::statistics(...) Program Flow
            void Pythia::statistics(...) Event Statistics
            string Pythia::word(...) Program Flow
            Pythia::~Pythia Program Flow
            bool ResonanceWidths::allowCalc() Semi Internal Resonances
            void ResonanceWidths::calcPreFac(...) Semi Internal Resonances
            void ResonanceWidths::calcWidth(...) Semi Internal Resonances
            bool ResonanceWidths::initBSM() Semi Internal Resonances
            void ResonanceWidths::initConstants() Semi Internal Resonances
            double ResonanceWidths::widthChan(...) Semi Internal Resonances
            bool Rndm::dumpState(...) Random Numbers
            double Rndm::exp() Random Numbers
            double Rndm::flat() Random Numbers
            double Rndm::gauss() Random Numbers
            pair<double, double> Rndm::gauss2() Random Numbers
            void Rndm::init(...) Random Numbers
            int Rndm::pick(...) Random Numbers
            bool Rndm::readState(...) Random Numbers
            Rndm::Rndm() Random Numbers
            Rndm::Rndm(...) Random Numbers
            bool Rndm::rndmEnginePtr(...) Random Numbers
            double Rndm::xexp() Random Numbers
            virtual double RndmEngine::flat() Random Numbers
            void RotBstMatrix::bst(...) Four-Vectors
            void RotBstMatrix::bst(...) Four-Vectors
            void RotBstMatrix::bst(...) Four-Vectors
            void RotBstMatrix::bstback(...) Four-Vectors
            double RotBstMatrix::deviation() Four-Vectors
            void RotBstMatrix::fromCMframe(...) Four-Vectors
            void RotBstMatrix::invert() Four-Vectors
            RotBstMatrix& RotBstMatrix::operator=(...) Four-Vectors
            void RotBstMatrix::reset() Four-Vectors
            void RotBstMatrix::rot(...) Four-Vectors
            void RotBstMatrix::rot(...) Four-Vectors
            void RotBstMatrix::rotbst(...); Four-Vectors
            RotBstMatrix::RotBstMatrix() Four-Vectors
            RotBstMatrix::RotBstMatrix(...) Four-Vectors
            void RotBstMatrix::toCMframe(...) Four-Vectors
            void Settings::addFlag(...) Settings Scheme
            void Settings::addMode(...) Settings Scheme
            void Settings::addMVec(...) Settings Scheme
            void Settings::addParm(...) Settings Scheme
            void Settings::addPVec(...) Settings Scheme
            void Settings::addWord(...) Settings Scheme
            bool Settings::flag(...) Settings Scheme
            void Settings::flag(...) Settings Scheme
            bool Settings::flagDefault(...) Settings Scheme
            void Settings::forceMode(...) Settings Scheme
            void Settings::forceMVec(...) Settings Scheme
            void Settings::forceParm(...) Settings Scheme
            void Settings::forcePVec(...) Settings Scheme
            map Settings::getFlagMap(...) Settings Scheme
            map Settings::getModeMap(...) Settings Scheme
            map Settings::getMVecMap(...) Settings Scheme
            map Settings::getParmMap(...) Settings Scheme
            map Settings::getPVecMap(...) Settings Scheme
            map Settings::getWordMap(...) Settings Scheme
            bool Settings::init(...) Settings Scheme
            bool Settings::initPtr(...) Settings Scheme
            bool Settings::isFlag(...) Settings Scheme
            bool Settings::isMode(...) Settings Scheme
            bool Settings::isMVec(...) Settings Scheme
            bool Settings::isParm(...) Settings Scheme
            bool Settings::isPVec(...) Settings Scheme
            bool Settings::isWord(...) Settings Scheme
            void Settings::list(...) Settings Scheme
            void Settings::listAll(...) Settings Scheme
            void Settings::listChanged(...) Settings Scheme
            int Settings::mode(...) Settings Scheme
            void Settings::mode(...) Settings Scheme
            int Settings::modeDefault(...) Settings Scheme
            vector<int> Settings::mvec(...) Settings Scheme
            void Settings::mvec(...) Settings Scheme
            vector<int> Settings::mvecDefault(...) Settings Scheme
            double Settings::parm(...) Settings Scheme
            void Settings::parm(...) Settings Scheme
            double Settings::parmDefault(...) Settings Scheme
            vector<double> Settings::pvec(...) Settings Scheme
            void Settings::pvec(...) Settings Scheme
            vector<double> Settings::pvecDefault(...) Settings Scheme
            bool Settings::readString(...) Settings Scheme
            bool Settings::reInit(...) Settings Scheme
            void Settings::resetAll() Settings Scheme
            void Settings::resetFlag(...) Settings Scheme
            void Settings::resetMode(...) Settings Scheme
            void Settings::resetMVec(...) Settings Scheme
            void Settings::resetParm(...) Settings Scheme
            void Settings::resetPVec(...) Settings Scheme
            void Settings::resetWord(...) Settings Scheme
            Settings::Settings() Settings Scheme
            string Settings::word(...) Settings Scheme
            void Settings::word(...) Settings Scheme
            string Settings::wordDefault(...) Settings Scheme
            bool Settings::writeFile(...) Settings Scheme
            bool Settings::writeFile(...) Settings Scheme
            int SigmaProcess::code() Semi Internal Processes
            bool SigmaProcess::convert2mb() Semi Internal Processes
            bool SigmaProcess::convertM2() Semi Internal Processes
            int SigmaProcess::gmZmode() Semi Internal Processes
            int SigmaProcess::id3Mass() Semi Internal Processes
            int SigmaProcess::id4Mass() Semi Internal Processes
            int SigmaProcess::id5Mass() Semi Internal Processes
            int SigmaProcess::idSChannel() Semi Internal Processes
            int SigmaProcess::idTchan1() Semi Internal Processes
            int SigmaProcess::idTchan2() Semi Internal Processes
            string SigmaProcess::inFlux() Semi Internal Processes
            void SigmaProcess::initProc() Semi Internal Processes
            int SigmaProcess::isQCD3body() Semi Internal Processes
            bool SigmaProcess::isSChannel() Semi Internal Processes
            string SigmaProcess::name() Semi Internal Processes
            int SigmaProcess::resonanceA() Semi Internal Processes
            int SigmaProcess::resonanceB() Semi Internal Processes
            void SigmaProcess::setIdColAcol() Semi Internal Processes
            bool SigmaProcess::setupForME() Semi Internal Processes
            double SigmaProcess::sigmaHat() Semi Internal Processes
            void SigmaProcess::sigmaKin() Semi Internal Processes
            double SigmaProcess::tChanFracPow1() Semi Internal Processes
            double SigmaProcess::tChanFracPow2() Semi Internal Processes
            bool SigmaProcess::useMirrorWeight() Semi Internal Processes
            double SigmaProcess::weightDecay(...) Semi Internal Processes
            double SigmaProcess::weightDecayFlav(...) Semi Internal Processes
            bool SlowJet::analyze(...) Event Analysis
            vector<int> SlowJet::constituents(...) Event Analysis
            double SlowJet::dNext() Event Analysis
            bool SlowJet::doNSteps(...) Event Analysis
            bool SlowJet::doStep() Event Analysis
            int SlowJet::iNext() Event Analysis
            int SlowJet::jetAssignment(...) Event Analysis
            int SlowJet::jNext() Event Analysis
            void SlowJet::list() Event Analysis
            void SlowJet::list(...) Event Analysis
            double SlowJet::m(...) Event Analysis
            int SlowJet::multiplicity(...) Event Analysis
            Vec4 SlowJet::p(...) Event Analysis
            double SlowJet::phi(...) Event Analysis
            double SlowJet::pT(...) Event Analysis
            void SlowJet::removeJet(...) Event Analysis
            bool SlowJet::setup(...) Event Analysis
            int SlowJet::sizeAll() Event Analysis
            int SlowJet::sizeJet() Event Analysis
            int SlowJet::sizeOrig() Event Analysis
            SlowJet::SlowJet(...) Event Analysis
            bool SlowJet::stopAtN(...) Event Analysis
            double SlowJet::y(...) Event Analysis
            virtual bool SlowJetHook::include(...) Event Analysis
            SlowJetHook::SlowJetHook() Event Analysis
            virtual SlowJetHook::~SlowJetHook() Event Analysis
            virtual bool SpaceShower::branch(...) Implement New Showers
            bool SpaceShower::doRestart() Implement New Showers
            virtual double SpaceShower::enhancePTmax() Implement New Showers
            virtual void SpaceShower::init(...) Implement New Showers
            void SpaceShower::initPtr(...) Implement New Showers
            virtual bool SpaceShower::limitPTmax(...) Implement New Showers
            virtual void SpaceShower::list(...) Implement New Showers
            virtual void SpaceShower::prepare(...) Implement New Showers
            virtual double SpaceShower::pTnext(...) Implement New Showers
            SpaceShower::SpaceShower() Implement New Showers
            int SpaceShower::system() Implement New Showers
            virtual void SpaceShower::update(...) Implement New Showers
            virtual SpaceShower::~SpaceShower() Implement New Showers
            bool Sphericity::analyze(...) Event Analysis
            double Sphericity::aplanarity() Event Analysis
            double Sphericity::eigenValue(...) Event Analysis
            Vec4 Sphericity::eventAxis(...) Event Analysis
            void Sphericity::list(...) Event Analysis
            int Sphericity::nError() Event Analysis
            double Sphericity::sphericity() Event Analysis
            Sphericity::Sphericity(...) Event Analysis
            SuppressSmallPT::SuppressSmallPT(...) User Hooks
            bool Thrust::analyze(...) Event Analysis
            Vec4 Thrust::eventAxis(...) Event Analysis
            void Thrust::list(...) Event Analysis
            int Thrust::nError() Event Analysis
            double Thrust::oblateness() Event Analysis
            double Thrust::thrust() Event Analysis
            Thrust::Thrust(...) Event Analysis
            double Thrust::tMajor() Event Analysis
            double Thrust::tMinor() Event Analysis
            virtual bool TimeShower::branch(...) Implement New Showers
            double TimeShower::enhancePTmax() Implement New Showers
            virtual void TimeShower::init(...) Implement New Showers
            void TimeShower::initPtr(...) Implement New Showers
            virtual bool TimeShower::limitPTmax(...) Implement New Showers
            virtual void TimeShower::list(...) Implement New Showers
            virtual void TimeShower::prepare(...) Implement New Showers
            virtual void TimeShower::prepareGlobal(...) Implement New Showers
            double TimeShower::pTLastInShower() Implement New Showers
            virtual double TimeShower::pTnext(...) Implement New Showers
            virtual bool TimeShower::rescatterPropogateRecoil(...) Implement New Showers
            virtual void TimeShower::rescatterUpdate(...) Implement New Showers
            virtual int TimeShower::shower(...) Implement New Showers
            virtual int TimeShower::showerQED(...) Implement New Showers
            int TimeShower::system() Implement New Showers
            TimeShower::TimeShower() Implement New Showers
            virtual void TimeShower::update(...) Implement New Showers
            virtual TimeShower::~TimeShower() Implement New Showers
            virtual double UserHooks::biasedSelectionWeight() User Hooks
            virtual double UserHooks::biasSelectionBy(...) User Hooks
            virtual bool UserHooks::canBiasSelection() User Hooks
            virtual bool UserHooks::canModifySigma() User Hooks
            virtual bool UserHooks::canSetResonanceScale() User Hooks
            virtual bool UserHooks::canVetoFSREmission() User Hooks
            virtual bool UserHooks::canVetoISREmission() User Hooks
            virtual bool UserHooks::canVetoMPIEmission() User Hooks
            virtual bool UserHooks::canVetoMPIStep() User Hooks
            virtual bool UserHooks::canVetoPartonLevel() User Hooks
            virtual bool UserHooks::canVetoPartonLevelEarly() User Hooks
            virtual bool UserHooks::canVetoProcessLevel() User Hooks
            virtual bool UserHooks::canVetoPT() User Hooks
            virtual bool UserHooks::canVetoResonanceDecays() User Hooks
            virtual bool UserHooks::canVetoStep() User Hooks
            virtual bool UserHooks::doVetoFSREmission(...) User Hooks
            virtual bool UserHooks::doVetoISREmission(...) User Hooks
            virtual bool UserHooks::doVetoMPIEmission(...) User Hooks
            virtual bool UserHooks::doVetoMPIStep(...) User Hooks
            virtual bool UserHooks::doVetoPartonLevel(...) User Hooks
            virtual bool UserHooks::doVetoPartonLevelEarly(...) User Hooks
            virtual bool UserHooks::doVetoProcessLevel(...) User Hooks
            virtual bool UserHooks::doVetoPT(...) User Hooks
            virtual bool UserHooks::doVetoResonanceDecays(...) User Hooks
            virtual bool UserHooks::doVetoStep(...) User Hooks
            virtual bool UserHooks::initAfterBeams() User Hooks
            void UserHooks::initPtr(...) User Hooks
            virtual double UserHooks::multiplySigmaBy(...) User Hooks
            virtual int UserHooks::numberVetoMPIStep() User Hooks
            virtual int UserHooks::numberVetoStep() User Hooks
            void UserHooks::omitResonanceDecays(...) User Hooks
            virtual double UserHooks::scaleResonance(...) User Hooks
            virtual double UserHooks::scaleVetoPT() User Hooks
            void UserHooks::subEvent(...) User Hooks
            UserHooks::UserHooks() User Hooks
            Event UserHooks::workEvent User Hooks
            virtual UserHooks::~UserHooks() User Hooks
            void Vec4::bst(...) Four-Vectors
            void Vec4::bst(...) Four-Vectors
            void Vec4::bst(...) Four-Vectors
            void Vec4::bst(...) Four-Vectors
            void Vec4::bstback(...) Four-Vectors
            void Vec4::bstback(...) Four-Vectors
            double Vec4::e() Four-Vectors
            void Vec4::e(...) Four-Vectors
            double Vec4::eT() Four-Vectors
            double Vec4::eT2() Four-Vectors
            double Vec4::eta() Four-Vectors
            void Vec4::flip3() Four-Vectors
            void Vec4::flip4() Four-Vectors
            double Vec4::m2Calc() Four-Vectors
            double Vec4::mCalc() Four-Vectors
            Vec4& Vec4::operator*=(...) Four-Vectors
            Vec4& Vec4::operator+=(...) Four-Vectors
            Vec4 Vec4::operator-() Four-Vectors
            Vec4& Vec4::operator-=(...) Four-Vectors
            Vec4& Vec4::operator/=(...) Four-Vectors
            Vec4& Vec4::operator=(...) Four-Vectors
            Vec4& Vec4::operator=(...) Four-Vectors
            void Vec4::p(...) Four-Vectors
            void Vec4::p(...) Four-Vectors
            double Vec4::pAbs() Four-Vectors
            double Vec4::pAbs2() Four-Vectors
            double Vec4::phi() Four-Vectors
            double Vec4::pNeg() Four-Vectors
            double Vec4::pPos() Four-Vectors
            double Vec4::pT() Four-Vectors
            double Vec4::pT2() Four-Vectors
            double Vec4::px() Four-Vectors
            void Vec4::px(...) Four-Vectors
            double Vec4::py() Four-Vectors
            void Vec4::py(...) Four-Vectors
            double Vec4::pz() Four-Vectors
            void Vec4::pz(...) Four-Vectors
            double Vec4::rap() Four-Vectors
            void Vec4::rescale3(...) Four-Vectors
            void Vec4::rescale4(...) Four-Vectors
            void Vec4::reset() Four-Vectors
            void Vec4::rot(...) Four-Vectors
            void Vec4::rotaxis(...) Four-Vectors
            void Vec4::rotaxis(...) Four-Vectors
            void Vec4::rotbst(...) Four-Vectors
            double Vec4::theta() Four-Vectors
            double Vec4::thetaXZ() Four-Vectors
            Vec4::Vec4(...) Four-Vectors
            Vec4::Vec4(...) Four-Vectors
            pythia8-8.1.80.orig/phpdoc/ParticleData.php0000644000175000017500000245153012217615312016666 0ustar sunsun Particle Data SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Particle Data

            The structure and operation of the particle data table is described ";?>here. That page also describes how default data properties can be changed. The current page provides the actual default values.

            Main settings

            Apart from the data itself, the particle data table only contains a few aspects that are available to change:

            ParticleData:modeBreitWigner   (default = 4; minimum = 0; maximum = 4)
            Selection of particle masses when the mSel(id) is called to provide a new mass:
            0 : mass is fixed at the nominal m_0 value.
            1 : particles registered as having a mass width are given a mass in the range m_min < m < m_max, according to a truncated nonrelativistic Breit-Wigner, i.e. linear in m.
            2 : as above, except that the width is made mass-dependent: Gamma = Gamma_0 * sqrt( (m^2 - m_thr^2) / (m_0^2 - m_thr^2) ) where m is the current mass, m_0 the nominal one and m_thr is the mass threshold, given by the sum of the nominal masses of the decay products. In order to decouple production and decay the threshold is defined as the branching-ratio-weighted average over all allowed decay channels.
            3 : particles registered as having a mass width are given a mass in the range m_min < m < m_max, according to a truncated relativistic Breit-Wigner, i.e. quadratic in m.
            4 : as 3, but the width is modified as for 2, and the current mass is used for its phase-space prefactor, i.e. m_0 Gamma_0 -> m Gamma(m).

            Note: this mode only applies to normal hadronic resonances like the rho. The more massive states of the isResonance() type, like Z^0 or top, are considered separately.

            ParticleData:maxEnhanceBW   (default = 2.5; minimum = 1.; maximum = 5.)
            The modifications in options 2 and 4 above enhance the large-mass tail of the Breit-Wigner distributions (the mass spectrum develops a dm/m divergence). However, we expect form factors to dampen this tail at masses some distance above the nominal one, so cut off the rise by requiring the actual Breit-Wigner weight not to be more than a factor maxEnhanceBW above the one obtained with options 1 or 3, respectively. This also opens up for a simpler technical handling of mass selection in options 2 and 4, by using standard hit-and-miss Monte Carlo.

            Since running masses are only calculated for the six quark flavours, e.g. to obtain couplings to the Higgs boson(s), there is not an entry in the normal tables for each particles, but only the six MSbar mass values below, used as starting point for the running. In addition you can pick an alpha_s(M_Z), which is converted into a first-order five-flavour Lambda that is used to determine the rate of the running. (Without any match to four flavours below m_b; if desired, this can be fixed by slightly shifted default mass values, since the routines never should be called below the m_b scale anyway.)

            ParticleData:mdRun   (default = 0.006; minimum = 0.003; maximum = 0.008)
            the d quark MSbar mass at 2 GeV scale.

            ParticleData:muRun   (default = 0.003; minimum = 0.001; maximum = 0.006)
            the u quark MSbar mass at 2 GeV scale.

            ParticleData:msRun   (default = 0.095; minimum = 0.060; maximum = 0.150)
            the s quark MSbar mass at 2 GeV scale.

            ParticleData:mcRun   (default = 1.25; minimum = 1.00; maximum = 1.50)
            the c quark MSbar mass at the mass scale itself.

            ParticleData:mbRun   (default = 4.20; minimum = 4.00; maximum = 4.50)
            the b quark MSbar mass at the mass scale itself.

            ParticleData:mtRun   (default = 165.0; minimum = 150.0; maximum = 175.0)
            the t quark MSbar mass at the mass scale itself.

            ParticleData:alphaSvalueMRun   (default = 0.125; minimum = 0.10; maximum = 0.20)
            the alpha_s(M_Z) value used to define the rate at which MSbar masses run.

            Comments on the data

            Much of the current data has been updated based on the 2012 Review of Particle Physics [Ber12], while some is still based on the 2006 RPP [Yao06]. All known particle masses, widths and lifetimes have been set accordingly, while most not-yet-measured particles are kept at their values from PYTHIA 6. Decay channels and their branching ratios remain a major worry: many particles do not have one single solidly measured branching ratio, and many further do not have known branching ratios that add up to (the neighbourhood of) unity.

            Uncertainties are especially big for the scalar, pseudovector and tensor L = 1 multiplets available in PYTHIA. We note that some distributions become better described when these multiplets are included in the generation, while others become worse. It is tempting to associate this lackluster performance with the primitive knowledge. Not even the multiplets themselves are particularly well known. It used to be that the a_0(980) and f_0(980) were considered to be members of the scalar multiplet. Nowadays they are commonly assumed to be either four-quark states or of some other exotic character. This means that the PYTHIA 8 PDG particle codes have been changed for these particles, relative to what was used in PYTHIA 6 based on previous PDG editions. Specifically their numbers are now in the 9000000 series, and they have been replaced in the scalar multiplet by a_0(1450) and f_0(1370).

            For charm and bottom mesons the jungle of partial measurements makes it very difficult to construct fully consistent sets of decay channels. This part of the program has not yet been brought up to date to the 2006 RPP. Instead the LHCb decay tables (for EvtGen, but without using the EvtGen matrix-element machinery) and the DELPHI tune for PYTHIA 6 is being used. (This also includes a few non-c/b hadrons that only occur in the c/b decay tables.) This has the advantage that many tests have been made for consistency, but the disadvantage that it is not always in agreement with the latest measurements of some specific decay channels. The decays based on the LHCb tables (with some modifications) are 411, 421, 431, 441, 445, 511, 521, 531, 541, 3124, 4122, 4124, 5122, 10441, 10443, 13122, 14122, 20443, 23122, 30313, 30323, 30443, 33122, 100113, 100213, 100441, 100443, 100553, 9000111, 9000211. Correspondingly the decays based on the DELPHI tables are 415, 425, 435, 515, 525, 535, 4132, 4232, 4332, 5132, 5232 and 5332.

            The data itself

            Here comes the default particle data used in the program. Do not touch. The meaning of the various properties and the format used are explained ";?>here and the meMode codes ";?>here.

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            pythia8-8.1.80.orig/phpdoc/UpdateHistory.php0000644000175000017500000036417612217615312017144 0ustar sunsun Update History SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Update History

            These update notes describe major updates relative to the baseline PYTHIA 8.100 version. However, they are less extensive than the corresponding update notes for PYTHIA 6. On the other hand, whereas the PYTHIA 6 manual is a static document, the PYTHIA 8 html/php pages are kept up to date for each subversion.

            Important note:version 8.160 does introduce some elements of backwards incompatibility. Specifically, "multiple interactions", abbreviated MI, has been renamed "multiparton interactions", MPI. This affects many parts of the code and documentation. Also some features are deprecated, although remaining until the end of the 8.1xx version series.

            Main news by version

            • 8.105: 24 February 2008
              • New option to initialize with arbitrary beam directions
                pythia.init( idA, idB, pxA, pyA, pzA, pxB, pyB, pzB)
              • Added capability to set ";?>beam energy spread and beam vertex.
                Warning: as a consequence, the old Beams group of settings has been moved to BeamRemnants, and Beams is now instead used for machine beam parameters. Therefore also some Main settings of this character have been regrouped, as follows:
                8.100 setting has been moved to
                Main:idA Beams:idA
                Main:idB Beams:idB
                Main:inCMframe (Beams:frameType)
                Main:eCM Beams:eCM
                Main:eA Beams:eA
                Main:eB Beams:eB
                Main:LHEF Beams:LHEF
              • The forceHadronLevel() method introduced for standalone hadronization.
              • main15.cc illustrated how either full hadronization or only decays of some particles can be looped over for the rest of the event retained.
              • The LHAevnt and LHAinit classes have been joined into a new LHAup one, with new options that allow the writing of a Les Houches Event File.
              • The SusyLesHouches class updated to handle SLHA version 2.
              • Updated HepMC conversion routine.
              • The static ErrorMsg class has been removed and its functionality moved into the non-static Info class, in the renamed Info file.
              • Further reduction of the use of static, with related code changes. This should allow to have several almost independent Pythia instances. Some static classes still remain, however, notably for random number generation and particle properties.
              • Limited capability to use two different Pythia instances for signal + pileup event generation, see main19.cc for an example.
              • In the Event class the = and =+ methods have been overloaded to allow the copying or appending of event records. Illustrated in main19.cc.
              • The html and php page formatting improved with cascading style sheets.
              • Several minor improvements and new options, including updated configure scripts.
            • 8.108: 1 May 2008
              • Correction in the event record, so that the beam particles in line 1 and 2 do not have any mother according to the motherList method. Previously the "system" entry in line 0 was counted as their mother, which gave rise to an unexpected extra vertex in the conversion to the HepMC format.
              • Support for HepMC version 1 is removed, to simplify the code and reflect the evolution of the field.
              • Status codes are stored in HepMC only as 1 for existing and 2 for decayed or fragmented particles (whereas previously the original PYTHIA codes were used for the latter).
              • Parton densities are stored in HepMC as xf(x,Q^2) rather than the f(x,Q^2) used in (some) previous versions.
              • The SusyLesHouches class has been updated so that reading is fully compatible with the SLHA2 standard.
              • Improved handling of the Higgs width, relevant for massive and thereby broad resonance shapes.
              • The matrix elements for neutralino pair production have now been completed and checked.
              • Ensure that alpha_strong does not blow up, by introducing a minimal scale somewhat above Lambda_3 (roughly where alpha_strong = 10).
              • New methods isValence1() and isValence2() in the Info class.
              • Protection against division by zero in calculation of decay vertex (for zero-mass gluons with zero lifetime, where there should be no displacement).
              • A new compilation option -Wshadow is introduced and code is rewritten at all places where this option gave warnings.
              • Minor library correction to allow compilation with gcc 4.3.0.
            • 8.114: 22 October 2008
              • New rescattering description operational (but still experimental) for the case that FSR is not interleaved, but saved until after MPI, ISR and beam remnants have been handled. This involves much new code in several classes.
              • A new class PartonSystems is introduced to keep track of which partons in the event record belong to which subcollision system, plus some further information on each subsystem. It takes over functionality previously found as part of the Event class, but leaves room for future growth.
              • Add optional model, wherein an increased pT0 turnoff scale for MPI and ISR is used for above-average active events, i.e. events that already have several MPI's or ISR emissions.
              • Freeze GRV 94L distribution at small Q^2 to avoid blowup.
              • The pythia.readFile(...) method can now alternatively take an istream as argument instead of a filename.
              • Minor bug correction in PartonLevel.cc; the bug could (rarely) give a segmentation fault.
            • 8.120: 10 March 2009
              • New rescattering description further developed, but not yet recommended for normal usage.
              • Include new processes for Large Extra Dimensions and Unparticles, contributed by Stefan Ask. New test program main28.cc illustrates.
              • Include further SUSY processes: neutralino-chargino and chargino-chargino pairs. The processes should be valid also in the case of non-minimal flavour violation and/or CP violation. Expanded machinery to keep track of SUSY parameters.
              • Include backwards evolution of incoming photon as part of the SpaceShower initial-state radiation description. This allows you to simulate hard collisions where one of the incoming partons is a photon. New test program main43.cc illustrates.
              • Allow separate mass and transverse momentum cuts when two hard subprocesses are generated in the same event.
              • The default value for the border between short- and long-lived particles has been changed from 1 mm to 10 mm, to better conform with LHC standards, see ";?>here. The default is still to let all unstable particles decay.
              • New ISR matrix-element correction to f -> f gamma in single W production.
              • New method Event::statusHepMC returns the status code according to the HepMC conventions agreed in February 2009. The interface to HepMC now writes out status according to this convention.
              • Add capability to link to FastJet, with expanded configure script and Makefile, and with main61.cc as new example.
              • Update of Makefile.msc, with added support for latest Visual C++ Express edition and use of regexp to check nmake version.
              • Update of LHAFortran.h and Pythia6Interface.h, to make the interface to Fortran routines work also under Windows. (Thanks to Anton Karneyeu.)
              • Updated and expanded worksheet.
              • The manual pages in the xmldoc directory, and thereby also those of the htmldoc and phpdoc directories, have been significantly updated and expanded. In particular, in many places the class of each method is explicitly shown, as well as the type of the return value and of the arguments. This upgrade is not yet completed, but already covers the more relevant sections.
              • The unary minus operator in the Vec4() returns a reference to a four-vector with all components negated, but leaves the original four-vector unchanged. Previously the four-vector itself was flipped.
              • The pPlus() and pMinus() methods of a four-vector and an event-record particle are renamed pPos() and pNeg(), respectively.
              • Include a further loop in ProcessLevel, so that a new process is generated in case of failures of a less severe nature.
              • Introduce warning message for unexpected meMode in ResonanceWidths.
              • Les Houches event reading framework has been rearranged for more flexibility. Some bugs corrected. Specifically, when scale is not set (scale = -1. in the Les Houches standard), PYTHIA did not attempt to set this scale itself, which typically lead to there not being any ISR or FSR. Now the ";?>rules for normal 1-, 2- and 3-body final states are applied, with a trivial extension of the 3-body rules for higher multiplicities.
              • Correct bug in the handling of parton densities, whereby it was not possible to switch to a new set, once a first initialization had been done.
              • Correct bugs when several Pythia::init initialization calls are made in the same run, specifically in the case that pointers to external processes have been handed in.
              • Changes in main03.cmnd and main04.cmnd so that some nonstandard options are commented out rather than active. Related comments inserted also in some other .cmnd files, but there without any change in program execution.
              • A few further minor bug fixes.
              • Update year to 2009.
            • 8.125: 16 June 2009
              • Hadronization and timelike-shower parameter default values updated according to a tune to LEP1 data by Hendrik Hoeth, using the Rivet + Professor framework.
              • Many further SUSY production processes. SLHA readin expanded to cover also masses and decay modes. Example main22.cc updated, while main33.cc now superfluous and removed.
              • Also further processes for extra dimensions.
              • Stefan Ask joins as coauthor.
              • The TimeShower::shower(...) method has gained a new argument, that forces the shower evolution to stop after a given number of branchings. A new method TimeShower::pTLastInShower() permits the last evolution pT to be read out. These extensions can be useful for matching studies.
              • New optional argument isInterleaved added to TimeShower::branch(...). Is false by default, but true when called from the parton level for interleaved evolution of several parton systems, optionally also with ISR and MPI.
              • New methods UserHooks::canSetResonanceScale() and UserHooks:scaleResonance(...) allows an optional user choice of the maximum shower scale in resonance decays.
              • A new method SpaceShower::doRestart() has been added, to help distinguish cases when a SpaceShower::branch(...) failure forces a complete restart of the evolution from ones where only the intended current branching has been vetoed.
              • When multiparton interactions are initialized, it is now possible to reduce both pT0 and pTmin if necessary to find a valid solution where sigma_jet > sigma_nondiffractive. Previously only the former would be reduced, which could lead to infinite loops if too large a pTmin was used. Thanks to Sami Kama for pointing out the problem.
              • The rescattering machinery is now essentially completed, and can be used also by others than the authors. For now, however, it can only be recommended for dedicated studies, not e.g. for generic tunes.
              • Timelike and spacelike showers, and beam remnant handling, are modified to handle rescattering partons. Specifically, a new machinery is introduced to trace the recoils from the combination of rescattering with showers and primordial kT. Can assign space- or timelike virtualities to intermediate particles to have energy and momentum conserved locally. This affects the PartonLevel, MultipartonInteractions, TimeShower, SpaceShower and BeamRemnants classes. Further details to appear in the upcoming article on rescattering. (Another change is a reversal to pre-8.114 order for non-interleaved FSR, wherein also FSR is treated before beam remnants are attached.)
              • Four new status codes introduced, as part of the rescattering description:
                45 : incoming rescattered parton, with changed kinematics owing to ISR in the mother system (cf. status 34);
                46 : incoming copy of recoiler when this is a rescattered parton (cf. status 42);
                54 : copy of a recoiler, when in the initial state of a different system from the radiator;
                55 : copy of a recoiler, when in the final state of a different system from the radiator.
              • New method Info::tooLowPTmin() can tell whether the pTmin scales for showers or multiparton interactions are too low.
              • Pion beams allowed, both pi^+, pi^- and pi^0. New machinery for the latter, where the valence flavour content is chosen to be either d dbar or u ubar for each new event. One internal pion PDF implemented, with others from LHAPDF.
              • Treatment of Pomeron-proton collisions begun.
              • Phase-space handling of hard processes and multiparton interactions slightly expanded to better allow for harder PDF's than proton ones, e.g. for Pomerons.
              • The program documentation has been expanded with an alphabetical index of all methods that are described on the webpages, see the ";?>Program Methods page. Also other sections of the documentation have been updated and expanded, including the worksheet.
              • Several list methods have been made const. For the listing of events two new methods have been added, Event::list() and Event::list(bool showScaleAndVertex, bool showMothersAndDaughters = false), that correspond to special cases of the general method.
              • A new method Pythia::LHAeventSkip(int nSkip) permits a skip-ahead of the reading of external Les Houches Events, without the necessity to generate the intervening nSkip events in full. Makes use of the new LHAup::skipEvent(int nSkip) method to perform the operations. Mainly intended for debug purposes.
              • The ClusterJet jet finder now saves the last five clustering scales. Also a minor bug fix. Thanks to Nils Lavesson for this contribution.
              • The Particle::m2() method now returns a negative number when the stored mass m is negative, as used to indicate spacelike virtualities. Also the Particle::eCalc(), Particle::mT() and Particle::mT2() methods have been modified.
              • The << method to print our a four-vector has been expanded with a fifth number, the invariant length, with a minus sign for spacelike vectors, and provided within brackets to allow a simple visual distinction.
              • New methods Rndm::dumpState(string fileName) and Rndm::readState(string fileName) allows to write or read the state of the random number generator to or from a binary file.
              • New method double GammaReal(double x) returns the value of the Gamma function for arbitrary real argument. Some cross sections for extra-dimensional processes rewritten to make use of it.
              • New example program main29.cc shows how to set up a fictitious process of a heavy system decaying to two particles or partons, with decays traced to stable particles, as relevant for astroparticle applications.
              • Main programs that illustrate the HepMC interface have been updated to use version 2.04, including units and excluding deprecated output formats.
              • The main32.cc example extended also to handle Les Houches Event Files.
              • The Makefile has been modified so that "make clean" only removes the current compilation and library files, while "make distclean" gives a more extensive reset and cleanup. Thanks to Nils Lavesson for this contribution. Some other minor Makefile corrections.
              • Several main programs that use the Main:timesToShow mode have been corrected so as not to crash if this is set to zero. Also some other cosmetics changes in main programs that do not affect the running.
              • Bug correction, in that previously a veto with user hooks was not propagated from parton showers inside resonance decays.
              • Minor bug fix in TimeShower for kinematics with unequal beam-particle masses.
              • Bug fix so that PartonLevel:MPI = off also works for minimum-bias events.
              • Minor bug fix in the impact-parameter selection of multiparton interactions. Thanks to Sami Kama for pointing it out.
              • String fragmentation for junction topology protected against numerical instability in boost.
              • Bug correction in the handling of particle decays to partons, where the scale of the partons was set before the partons had been added to some arrays, leading to indexation out of bounds. Thanks to Vladislav Burylov for discovering this bug.
              • Bug correction in the handling of particles with inhibited decay, where the decay vertex would be too far displaced, which could lead to infinite loop. Thanks to Sami Kama for debugging this.
              • Check to avoid infinite loop in matrix-element handling of two-body decays.
              • Bug correction to avoid infinite loops in Dalitz decay treatment. Some changes in the decay handling logic to allow a new try when the decay of a particle fails.
              • Minor correction, so the pointer to the Info class is set also for user-written classes derived from LHAup.
              • Correction for typo in the matrix element of the Sigma3ff2HchgchgfftWW class, for doubly charged Higgs production. Thanks to Merlin Kole for spotting it.
              • Updated colour bookkeeping in junction-antijunction annihilation avoids later problems in Pythia::check().
              • Minor updates of the Makefile.msc file to work with Visual Studio 2008. Thanks to David Bailey for these modifications.
              • Ensure that nInit in the BeamParticle class is set also for unresolved lepton beams.
              • The VetoEvolution class, derived from UserHooks, is obsolete and has been removed.
            • 8.130: 15 September 2009
              • New machinery that allows multiparton interactions inside diffractive systems. Also new optional Pomeron flux factors and Pomeron PDFs. New page on ";?>diffraction added, where further details are collected. Still not tuned, so to be used with caution.
              • Make Peter Skands' "Tune 1" parameters for ISR and MPI default. The older simpler tune is still available as an option, see ";?>Tune:pp.
              • New possible choices for a second hard process: charmonium, bottomonium, top pair and single top.
              • New code for pair production of generic colour-triplet scalar, fermion or vector. Largely written by Johan Bijnens, partly recycling existing code.
              • Add user hooks possibility to veto event after a given number of multiparton interactions.
              • Add instructions how PYTHIA 8 can be used from inside ROOT. Thanks to Andreas Morsch for providing the text and Rene Brun for a simple example.
              • The main21.cc example extended with an option for a single-particle gun.
              • Improvements and bug fixes in rescattering framework.
              • New method Hist::table(string fileName) provides a more direct way to print a two-column table of histogram contents into a file than the current Hist::table(ostream& os = cout).
              • Modify reading of external files so that a line only consisting of control characters counts as empty, the same way as a line only consisting of blanks already did. This includes carriage return, tabs and a few more, the ones represented by \n \t \v \b \r \f \a. Applies to Les Houches Event files, settings files and particle data files.
              • Fix it so that the read-in of a Les Houches Event File for the hardest process can be combined with the facility to select a specified second hard process.
              • New empty base class method LHAup::fileFound() allows the derived class LHAupLHEF to signal more clearly that a failed initialization is caused by a failure to open the desired file.
              • Check that a pointer to an LHAup object has been set in Pythia::LHAeventList() and Pythia::LHAeventSkip(...) calls.
              • Updated configure and Makefile, e.g. to build shared libraries on Mac OS X.
              • The options with a direct link to hard-process generation in PYTHIA 6 has been removed. It is hardly ever used but complicates the build structure. (Owing to its usefulness for some debug work, it was reinstated in a limited form in version 8.135. Thus main51.cc now contains the complete interface, previously in separate files, and commented-out lines in examples/Makefile suggest how PYTHIA 6 could be linked.)
              • New argument to Info::errorMsg(...) allows to show all error messages of a specific kind rather than only the first one, e.g. for initialization.
              • Correction in decay table of righthanded Majorana neutrinos. Thanks to Arnaud Ferrari and Vladimir Savinov.
              • Correction in expressions in the manual for H^+- couplings to an h^0, H^0 or A^0 and a W^+-. Thanks to Rikard Enberg.
              • Fix for accessing uninitialized memory, caused by accessing the daughters of the incoming beams before these daughters actually existed. Thanks to David Bailey and Sami Kama.
              • Uninitialized photon PDF inside the proton could give crazy results for processes with incoming photons. Thanks to Adam Davison.
              • Bug fix such that finite lifetimes can be set also for particles produced in the hard process. To exemplify, the bug affected tau leptons produced in Z^0 and W^+- decays. Thanks to Troels Petersen.
              • Bug fix in TimeShower, that beamOffset could remain uninitialized. Thanks to Sami Kama.
              • Minor correction to resonance decays: fail if the allowed mass range of a Breit-Wigner resonance is a small fraction of the total area under the resonance curve.
              • Correction when all three valence quarks were kicked out from a proton and could give false messages that beam momentum had been used up.
              • Clarify status codes needed for hadron-level standalone runs in order to avoid error messages, and modify the main21.cc example accordingly.
              • Minor corrections in the processes for extra dimensions.
              • Some other minor additions to existing facilities and minor bug fixes.
            • 8.135: 10 January 2010
              • All usage of static member methods inside Pythia8 has now been eliminated. This simplifies for you to have several simultaneous Pythia instances that are run with different conditions. The three main classes affected by this are the Settings and ParticleData databases and the Rndm random-number generator. You can no longer address the methods of these classes directly, but have to address them via the settings, particleData and rndm instances in the respective Pythia object. Also some other smaller pieces of code are affected, e.g. Standard Model and SUSY couplings (the latter in new files).
                Note 1: The documentation has been updated accordingly on these webpages, but the "A Brief Introduction to PYTHIA 8.1" still refers to the old behaviour of version 8.100.
                Note 2: the interface to the external LHAPDF library remains static, since LHAPDF is written in Fortran and thus by definition static.
                Note 3: if you want to have momentum smearing in CellJet you now need to send in a pointer to a random-number generator.
              • Ten new proton PDF sets are made available internally: MRST LO* (2007), MRST LO** (2008), MSTW 2008 LO (central member), MSTW 2008 NLO (central member), CTEQ6L, CTEQ6L1, CTEQ6.6 (NLO, central member), CT09MC1, CT09MC2, and CT09MCS, see ";?>PDF Selection. The Pomeron PDF data files have been renamed for consistency. Thanks to Tomas Kasemets for help with this [Kas10].
              • New parameters TimeShower:pTmaxFudgeMPI and SpaceShower:pTmaxFudgeMPI introduced, to give the same functionality for multiparton interactions that TimeShower:pTmaxFudge and SpaceShower:pTmaxFudge do for the hardest.
              • A few extensions of the UserHooks framework. New methods UserHooks:canVetoISREmission() and UserHooks::doVetoISREmission(...) allows the latest initial-state emission to be studied before being finalized, with the possibility to veto it. Similarly Userhooks:canVetoFSREmission() and UserHooks::doVetoFSREmission(...) can be used to veto the latest final-state emission.
              • A number of loop counters have been introduced in the Info class, that offers some further information on the progress of the event generation, for use e.g. in conjunction with the UserHooks facility.
              • The Pythia::initTunes(...) method is made public, so that it can be called before the normal call from Pythia::init(...). That way it is possible to start out from a given tune and change a few of the parameters.
              • Bug corrected in LHAFortran.h for hard-process input from Fortran commonblock. This did not work properly when the input was used in combination with a second hard process generated internally. Thanks to Mikhail Kirsanov and Roberto Chierici.
              • Insertion of missing initialization of isInit in the Settings and ParticleData constructors, and nInit for BeamParticle. Thanks to Leif Lönnblad.
              • Updated Makefile.msc for Windows users.
              • Fix of some non-optimal use of booleans, that give warnings on a Windows compiler. Thanks to Anton Karneyeu.
              • New options for the ";?> SUSY Les Houches Accord such that, by default, particle and decay data are not overwritten for known Standard Model particles (including Z^0, W^+- and t, but excluding the Higgs).
              • Bug fix in SusyLesHouches, where the reading of SLHA information embedded in an LHEF would not stop at the end of the header section.
              • Bug correction for undefined secondary widths where decay products together are heavier than the mother. Also unit default secondary width values in the DecayChannel constructor.
              • Documentation updated, including change of current year to 2010.
            • 8.140: 16 July 2010
              • Four new draft ";?>tunes available.
              • Introduction of a new scenario for production of Hidden-Valley particles, and interleaved showering in the QCD and HV sectors, see the new ";?>Hidden Valleys description. A longer physics writeup is available [Car10].
              • Implementation of 2 -> 3 phase space selection intended for QCD processes with massless partons. A new set of matching ";?>phase space cut parameters. The ";?>ten different QCD 2 -> 3 processes have been implemented making use of this new possibility, so far without a complete handling of possible colour flows, however.
              • New processes have been added for ";?>contact interactions in q q -> q q and q qbar -> q qbar scattering.
              • A process has been added for TeV^-1 Sized ";?>Extra Dimensions, which involves the electroweak KK gauge bosons, i.e. gamma_{KK}/Z_{KK}, in one TeV^-1 sized extra dimension; see main30.cc for an example. This scenario is described in [Bel10]. Thanks to Noam Hod and coworkers for contributing this code.
              • In the Randall-Sundrum extra-dimensional scenario a new option has been added where SM fields can exist in the bulk rather than only on a brane. (Still under development.) Furthermore production of a Kaluza-Klein gluon state has been added, and the main28.cc test program extended.
              • The scenario for monojets in Large Extra Dimensions has been expanded with an alternative for scalar graviton exchange instead of tensor one.
              • New parameters for maximum scale of ";?>timelike showers, TimeShower:pTmaxMatch, and the dampening of hard radiation, TimeShower:pTdampMatch and TimeShower:pTdampFudge, by analogy with corresponding ones for spacelike showers. Also new method TimeShower:limitPTmax(...) to implement alternative procedures. For dipoles stretched to the beam the new switch TimeShower:dampenBeamRecoil allows to dampen radiation close to the beam direction, with a changed default behaviour.
              • Azimuthal anisotropies from coherence arguments have been introduced for the spacelike parton showers, see SpaceShower:phiIntAsym and SpaceShower:strengthIntAsym. Also azimuthal anisotropies from gluon polarization have been introduced for the spacelike parton showers, see SpaceShower:phiPolAsym, and updated for timelike parton showers, see TimeShower:phiPolAsym.
              • Improvements for the matching to POWHEG LHEF-style input illustrated by the new main71.cc example. See also [Cor10].
              • A set of new processes gamma gamma -> f fbar, with f quarks or leptons. Code for equivalent photon flux around an unresolved proton, with more to come. Thanks to Oystein Alvestad.
              • A new option has been included to dampen the growth of the diffractive cross sections, see ";?>Total Cross Sections.
              • A new method virtual int SigmaProcess::idSChannel() has been introduced. If overloaded to return a nonzero value then a 2 -> n process will appear listed as a 2 -> 1 -> n one. That is, an intermediate resonance with the requested identity will be inserted in the event record, even without appearing in the calculation of the matrix element proper. Thanks to Noam Hod for idea and code.
              • A new method SigmaProcess::convertM2() has been introduced to optionally allow the SigmaProcess::sigmaHat() to return the squared matrix element rather than d(sigmaHat)/d(tHat) for 2 -> 2 processes. Furthermore kinematics is stored in the new mME and pME vectors for alternative cross section encodings.
              • Different encoding of the f fbar -> Z W cross section, contributed by Merlin Kole, based on the cross section of Brown, Sahdev and Mikaelian. Gives a distinctly different cross section than the previous based on EHLQ (including their bug fix). In particular the problem with negative cross sections is now fixed.
              • Minor updates: pass xmlPath to new MSTW and CTEQ PDFs; reset beams earlier to give cleaner documentation.
              • The H1 Fit B LO parametrization to the Pomeron PDF has been included, and made new default for Pomerons. Thanks to Paul Newman for providing the data files.
              • Three changes, in principle unrelated, but with the common objective to make the generation of a given event depend only on the values determined during the initialization stage and on the state of the random-number generator when the event is begun. The new default should ensure a reproducible stop-and-restart behaviour, convenient for debug purposes. Thanks to Michael Schmelling for stressing the desire for such a behaviour.
                (i) Introduction of a new option ";?> PhaseSpace:increaseMaximum that allows to switch between two strategies for handling the (hopefully rare) cases when the assumed maximum of the cross section function is exceeded during the event generation, with a changed default behaviour. In the old default the maximum could be increased if it was exceeded during the run, thereby introducing a memory of the previously generated events.
                (ii) Updated handling of random numbers with Gaussian distributions. The gauss() method now only generates one value at a time. Instead the new gauss2() method returns a pair of Gauss numbers, with related time savings. In the old approach one Gaussian number could be buffered, which introduced a memory.
                (iii) Minor bug fix in MiniStringFragmentation, where the popcorn baryon state was not reset for each new system, again giving a (flawed) memory.
              • New directory rootexample with a simple code example how to use ROOT for histogramming in PYTHIA runs. See ";?>ROOT Usage for details. Thanks to Rene Brun.
              • In the HepMCinterface the checks for unhadronized quarks and gluons are not performed if hadronization has been switched off.
              • The UserHooks::initPtr(...) has been expanded so that pointers to more classes (beam particles, random number, couplings, etc.) are sent in, thereby increasing the scope of possible user-written code. Also, the UserHooks::doVetoProcessLevel(Event& process) now allows the process event record to be modified, even if it is not recommended. The new Info::pTnow() method returns the current pT scale of the combined MPI, ISR and FSR evolution, which can be useful for some user hooks decisions.
              • Histograms of the Hist class can now be booked with up to 1000 bins, instead of the previous maximum 100. All bins can be written to file, but the line-printer style printing will join nearby bins so at most 100 are printed, as before.
              • Updated configure and Makefile to allow 64-bit compilation and more options. Thanks to Mikhail Kirsanov, Rene Brun and Fons Rademakers.
              • Bug fix in ProcessLevel for colour flow checks of junctions. Enables the decay of a neutralino to three quarks, e.g. Thanks to Nils-Erik Bomark.
              • Bug fixes in TimeShower, where recoil partners in resonance decays of coloured particles, and recoil partners in QED dipoles when beams are not allowed to take a recoil, might not be correctly identified.
              • Bug fix in SpaceShower: when used with a fixed alpha_strong, the threshold enhancement factor of g -> Q Qbar became undefined. Thanks to Stefan Prestel.
              • Bug fix in initialization of resonance widths, where the minWidth parameter could be used uninitialized, occasionally resulting in strange initialization problems when kinematics needs to force at least one resonance to be off-shell.
              • Minor updates of main06.cc, main10.cc and main23.cc.
              • Bug fix in mother pointer of multiparton interactions in diffractive systems.
            • 8.142: 15 August 2010
              • The strategy for setting up tune values has been changed. Previously the Tune:ee and Tune:pp settings were only interpreted during the Pythia::init(...) stage. Now they are interpreted as soon as they are read. Specifically this means that it is possible to override any of the tune parameters by putting new commands below Tune:ee and Tune:pp in the Pythia::readFile(...) configuration file or in the list of Pythia::readString(...) commands.
                As a consequence of this change, the public Pythia::initTunes(...) method has been replaced by two private Settings::initTuneEE(...) and Settings::initTunePP(...) methods.
                If Tune:ee or Tune:pp are nonvanishing by default, then the corresponding tune variables are set also from the Pythia constructor, before any user changes are possible. Currently this is not relevant.
              • Bug fix in the setup of the Tune:pp = 5 and = 6 options, which meant that diffractive cross sections were not reduced as advertised.
              • The default value of MultipartonInteractions:pT0Ref has been slightly reduced so as to give a somewhat improved default description. It is not intended as a replacement for the specific tunes, however.
              • Some comparisons between tunes and data, obtained with the Rivet package, have been posted on http://home.thep.lu.se/~richard/pythia81/. Further improvements can be expected from future Professor-based tunes. The current set of 2C, 2M, 3C and 3M "draft tunes" have deliberately been chosen different also to explore a range of possibilities. One not visible in the plots is the fraction of single and double diffractive events in the inelastic cross section. This is 32% in 2C and 2M, while it was reduced to 21% in 3C and 3M, and a recent ATLAS study (ATLAS-CONF-2010-048) would suggest 28+-4%.
              • Minor changes in TimeShower and SpaceShower, as protection if the c or b masses are set small.
              • Bug fix in SpaceShower, for case when phi angle selection is biased to take into account interference effects.
              • The SigmaProcess::convertM2() method now has been implemented also for 2 -> 1 processes, so that it is possible to provide the squared matrix element instead of sigmaHat for semi-internal processes. A fixed-width Breit-Wigner is also inserted, since the matrix element is supposed not to include it.
              • New method SigmaProcess::setupForME() does an extended conversion from the internal kinematics to an almost equivalent one, better adapted to the mass conventions of matrix-element calculation programs, such as massive incoming b quarks. New flags allow to determine whether the c, b, mu and tau should be considered massless or not in the calculations.
              • Two new friend methods table of the Hist class allow to print a table with three columns, the first for the (common!) x values and the other two for the respective histogram values. A new method takeSqrt for the square root of histogram bin contents.
            • 8.145: 10 November 2010
              • Couplings is defined in StandardModel.h as a derived class of coupSM and has only one extra flag: isSUSY to check presence of extra couplings.Changed all pointers CoupSM* to Couplings* and removed explicit references to CoupSUSY*. The coupSUSY object is only initialised if SUSY couplings are present. The new pointer couplingsPtr points either to only SM couplings or SM+SUSY couplings based on SLHA data.
              • New files SusyResonanceWidths.h/cc contains the SusyResonanceWidths class, which inherits from ResonanceWidths but typecasts the couplingsPtr to (CoupSUSY*) coupSUSYPtr. This is the base class for all SUSY resonances. It contains the ResonanceSquark class for all squark decays. A new flag SLHA:useDecayTable to check if internal widths should be overwritten by those read in via SLHA.
              • Added new functionality to SusyLesHouches for read-in of generic user blocks in the SLHA format, along with methods to extract parameters from them with typecasting controlled by the user. Intended for use with user-written semi-internal processes.
              • Added Sigma1qq2antisquark cross section.
              • Some new flags and modes in the SUSY and SLHA series offer further functionality.
              • Several further changes as a consequence of the upgrade of the SUSY machinery.
              • Bug/typo fixes in rotation matrices for SUSY couplings and for the processes qqbar2squarkantisquark, qq2squarksquark and more.
              • Improved handling of colour junctions. Added new example program main72.cc, to illustrate read-in of color junction structures via LHEF (main72.lhe). The example used is SUSY with RPV.
              • New Tune 4C introduced as Tune:pp = 5. The more crude (non-)tunes 3C and 3M are removed.
              • New methods Settings::getFlagMap(...), Settings::getModeMap(...), Settings::getParmMap(...) and Settings::getWordMap(...) allows to return a map of all settings of the respective type that contain a specific string in its name.
              • Improved description of excited g^*/KK-gluon^* production in the Sigma1qqbar2KKgluonStar and ResonanceKKgluon classes.
              • Possibility added to let Hidden-Valley gamma_v have a nonzero mass and decay by mixing with the ordinary photon. Still experimental.
              • Minor bug fix in handling of three-body phase space.
              • Minor correction in Sigma2ffbar2TEVffbar class.
              • Bug fix for decays of W' to a pair of heavy fermions when gV != gA. Thanks to M. Chizhov, see arXiv:0705.3944.
              • Restore the older EHLQ-based encoding of the f fbar -> Z W cross section, which was changed in version 8.140, since comparisons with Madgraph gives much better agreement with it than with the expression of Brown, Sahdev and Mikaelian.
              • The HepMCInterface now also stores colour flow information for coloured particles.
              • Pointer to Couplings made available for particle decays.
              • Minor update in main61.cc for more elegant usage of FastJet, as suggested by Gregory Soyez.
            • 8.150: 20 April 2011
              • Tune 4C is made default. It is based on first comparisons with LHC data [Cor10a], and has also been checked independently [Buc11] to give reasonable agreement with many distributions.
              • The description of tau lepton decays has been significantly enhanced, to include helicity information related to the production process and hadronic currents fitted to data. A complete writeup is in preparation, while a summary can be found in [Ilt12]. A new flag is introduced to revert to the old behaviour, for cross-checks, see ";?>Particle Decays. The new tau decay machinery is on by default.
              • A new option MultipartonInteractions:bProfile = 4 has been introduced for the impact-parameter profile of protons in the ";?>Multiparton Interactions framework, wherein low-x partons are spread over a larger area than high-x ones, see [Cor11]. A new method Info::eMPI(i) gives back the enhancement factor related to the i'th interaction. The impact-parameter profile can now be selected separately for ";?>diffraction, but without a bProfile = 4 option.
              • The possibility of "hadronization" in the ";?>Hidden Valley sector has been added as a new option HiddenValley:fragment = on. This is based on a copy of the standard string fragmentation framework, but with the option of a completely separate "flavour" sector, and separately tunable longitudinal fragmentation functions and transverse momenta. For now only a simple flavour scenario is provided, where flavour-diagonal mesons can decay back into the normal visible sector while off-diagonal ones remain hidden. A writeup of the model is in preparation [Car11]. Also some further Hidden Valley options have been added.
              • Included possibility in TimeShower for QCD dipoles to have an adjustable normalization factor, via the new bool isFlexible and double flexFactor properties of class TimeDipoleEnd. This flexibility is used to treat radiation off colour topologies with epsilon tensors, in particular colour junctions which have all their partons in the final state. (An example is the BNV-SUSY decay ~chi0→uds.) For such topologies, the new treatment in PYTHIA 8 is that a half-strength dipole is spanned between all combinations of final-state quarks. For junctions with an incoming (anti)colour line (such as in the BNV-SUSY decay ~t*→cb), a full-strength dipole is instead spanned between the two daughters, with no radiation from the decaying object (in its CM). As will be described in a forthcoming paper with N. Desai, this should give the closest possible correspondence to the radiation patterns exhibited by higher-order matrix elements for this type of process.
              • Corrected harmless bugs in ProcessLevel::findJunctions which caused junctions of types 3 and 4 (i.e., junctions with 1 incoming color tag) to sometimes be incorrectly classified as types 1 and 2 (with all color tags outgoing), respectively. Since the parity (even/odd) of the junction kind was still correct, however, this did not cause any problems at the hadronization stage.
              • The junction-finder in ProcessLevel::findJunctions has been made more stable, and the following ordering of the color tags returned by Event::endColJunction(iJun, iLeg) is now enforced: for junction kinds 3 and 4 (one tag incoming), iLeg = 0 will return the incoming tag, while for kinds 5 and 6 (two tags incoming), iLeg = 0 and iLeg = 1 will return the incoming tags. Apart from this ordering, the color tags are ordered in ascending color tag number.
              • Declarations of friend functions moved to sit outside the class it befriends. Thanks to Axel Naumann for pointing out the incorrect previous construction.
              • The rootexample subdirectory becomes rootexamples as the old example is split into two, with improved documentation to clarify usage. Thanks to Axel Naumann and Bernhard Meirose for the new code.
              • In the Les Houches Event File machinery, input type has been changed from ifstream to istream for more flexibility.
              • R-hadron handling is largely implemented, see the ";?>R-hadrons page, although some aspects still need polishing. A new class RHadrons takes care of the hadronization and decay. Particle data have been added for R-hadrons containing a gluino, stop or sbottom, but could alternatively be used for other long-lived coloured particles. Thanks to Bernhard Meirose for support.
              • Calculations of SUSY decay widths included by N. Desai, contained in the new source files SusyResonanceWidth.cc and .h. Validation and addition of more modes is still in progress, so this implementation should be considered preliminary for now. For a list of available modes, see the ";?>SUSY Processes page.
              • A first implementation of the SLHA-based QNUMBERS interface for defining new exotic particles has been included. See [Alw07] and the ";?>SUSY Les Houches Accord page.
              • Read-in of LHEF events containing Baryon Number Violating vertices has been included, using colour junctions, see the ";?>Event Record page. The advanced shower model taking into account the full colour structure of such events, developed by N. Desai and described above, is turned on by default in such events. Several test cases were used to validate this implementation, but it is possible that problems could still exist for some cases. Feedback is welcome. Thanks to the MadGraph authors for providing several test cases.
              • Some first steps taken to allow events containing colour sextets, e.g., from semi-internal processes or LHEF interfaces, and/or from SLHA DECAY tables. New colType codes 3 and -3 are introduced to describe sextets and antisextets, respectively. The state of the current implementation is that hard processes containing such states can be read in and decays generated (via DECAY tables). Parton showers can be added, but the sextets themselves do not, as yet, shower, and any undecayed sextets remaining at the hadronization stage would lead to unpredictable problems if hadronization is switched on. Thanks to J. Alwall for help with testing this implementation.
              • The functionality of the SLHA SUSY/BSM interface (see the ";?>SUSY Les Houches page) has been extended so that copies of all BLOCKs are now stored internally as strings, regardless of whether they correspond to "official" SLHA blocks or not. Their contents can subsequently be queried by a set of new templated member functions of the class SusyLesHouches. Available query functions so far include
                template <class T> bool getEntry(string, T&);,
                template <class T> bool getEntry(string, int, T&);,
                template <class T> bool getEntry(string, int, int, T&); , and
                template <class T> bool getEntry(string, int, int, int, T&);,
                where the type of the argument used in the call determines how to read the block entries. Thus, if an LHEF, SLHA, or other card file is read in by PYTHIA, the contents of any BLOCK in that file can subsequently be queried run-time using these functions. This is used, e.g., in the new interface between MADGRAPH 5 and PYTHIA 8. Thanks to the MADGRAPH team, and to J. Alwall in particular, for help and debug on this new implementation.
            • 8.153: 10 August 2011
              • The setup of tunes has been modified, see the ";?>Tunes page for details. Specifically the Tune:ee and Tune:pp modes have acquired a new option -1 for a forced restore to the default values of all settings used in the respective kind of tunes.
              • The code for handling multiparton interactions in the scenario with an x-dependent width of the Gaussian matter profile [Cor11], has been improved and updated. Tune 4Cx, which is based on this option, has been added as a further tune option.
              • A possibility to bias the phase-space selection has been added, whereby some phase space regions can be oversampled, which is compensated by assigning a weight to each event. A new set of methods have been added to the UserHooks class to allow users to program how to bias the selection.
              • New options added so that matrix-element corrections can be switched off after the first branching in ISR or FSR.
              • Some new Info methods have been added to store information on latest ISR branching. The SpaceShower class has also been corrected so that the latest z = 1/2 when not defined by history. This avoids undefined values for azimuthal asymmetries. Thanks to Stefan Prestel for finding and sorting out this problem.
              • The Pythia::forceHadronLevel() method now takes an argument that optionally means that existing junction information is not overwritten. Thanks to Leif Lönnblad for pointing out the usefulness of this.
              • For particle decays to a varying number of hadrons the multiplicity increase with mass has been somewhat reduced, and especially for meMode = 23 a separate even slower increase has been introduced.
              • New possibility to force the tau polarization.
              • Bug fix for the special case in which events containing SUSY particles are generated without proper initialization of SUSY decays. This can happen, e.g., if events containing SUSY particles are read in via external LHEF files, if those files do not contain readable SLHA spectra in their headers. In this case, a failed attempt to generate sparticle decays with ill-defined couplings previously led to crashes. The program now reverts to the old behaviour, based on static decay tables, in such cases, with the default being to decay all sparticles to gravitino + particle. An error message stating that the full SUSY treatment has been switched off and why is also issued. Thanks to N. Desai for this fix.
              • The R-hadron machinery has been completed.
              • Minor change in timelike showers: gluons which fall below the pTmin cutoff by the correction for mass effects are now eliminated, while previously they were kept. This reduces the number of gluons somewhat, but has no significant effects on the hadronic final state. (Prompted by R-hadron studies, where big mass effects else give bothersome low-energy gluons.)
              • Corrected typos in two of the Upsilon wave function matrix elements, Bottomonium:OUpsilon3P08 and Bottomonium:Ochib03P01. Thanks to Beate Heinemann for pointing it out.
              • Implemented f* decay angle in f f -> f f* processes, and fixed some bugs for the same process. Thanks to Piyali Banerjee for tests.
              • Introduce possibility to separate production channels for TeV-sized extra dimensions, and a small code correction. Thanks to Noam Hod for code contribution.
              • Bug fix for neutrino beams: since neutrinos are always lefthanded there should be a factor 2 in the cross section, relative to charged leptons, from the non-need to average over incoming spin states. This is now fixed by introducing a new PDF class NeutrinoPoint for (unresolved) neutrinos, with normalization 2 rather than 1 for charged leptons. Thanks to Ryosuke Sato.
              • Bug fix for some (rarely used) particle settings, which could not be changed by users because they were read too early. Thanks to Andrew Altheimer and Gustaaf Brooijmans.
              • Bug fix in handling of tau decays, where setting of decay vertices could write outside memory. Thanks to Steven Schramm.
              • Minor expansion of the BeamParticle constructor.
              • Minor bug fix in CTEQ 6L for uninitialized variables.
              • Minor bug fix in fragmentation flavour combination to hadron.
              • Some updates of the documentation, including new pages on MadGraph 5 as a generator for semi-internal processes (thanks to Johan Alwall) and on RIVET interfacing.
              • Minor improvements of ROOT- and HepMC-related code and documentation.
              • Some cleanup of code.
            • 8.157: 10 November 2011
                Stefan Prestel joins as new member of the PYTHIA author team. He is mainly working on matching/merging issues, and has contributed the CKKW-L machinery mentioned below.
              • Merging capabilities according to the CKKW-L scheme [Lon11] have been added, see the new ";?>Matrix Element Merging page. It involves new classes to reconstruct and select how a matrix-element-generated partonic configuration could have been obtained by the PYTHIA evolution, and to perform trial showers (using a new copy of the normal parton-level machinery) that introduce the appropriate Sudakov suppression factors. New examples to illustrate various common tasks are found in main81.cc, main82.cc, main83.cc and main84.cc.
              • The main71.cc program is now generalised for reading in arbitrary POWHEG LHE files, to implement a smooth matching between NLO matrix elements and the PYTHIA parton showers. Cuts are made on both ISR and FSR emissions, while previously only ISR was covered. The key assumptions are the pT definitions used for ISR and FSR, but several further options are available, as documented in the main71.cmnd file. Work is still ongoing to pick the best default options.
              • Several expansions of the UserHooks class. For both doVetoFSREmission and doVetoISREmission a new argument iSys labels the system within which the radiation occurs. For doVetoFSREmission a further argument inResonance distinguishes FSR in resonance decays from that in the hard process itself. New methods canVetoMPIEmission and doVetoMPIEmission have been added to veto multiparton interactions in the same way as FSR and ISR. In biasSelectionBy at times incorrect values for inEvent has been corrected. Also some systematization of the use of const.
              • A new model for hadron scattering is introduced, still at an early stage and therefore more intended for internal development than for the normal user. The basic idea is that a high-energy pp collision involves the fragmentation of multiparton strings that overlap in space (and time). Also the produced hadrons therefore initially overlap, and there is a strong likelihood that hadrons can scatter against each other until the system has expanded sufficiently. This can e.g. increase the transverse momentum of heavier hadrons at the expense of lighter ones.
              • A new jet finder SlowJet offers simple access to the inclusive kT, anti-kT, and Cambridge/Aachen algorithms in a cylindrical coordinate frame. The jet reconstruction is then based on sequential recombination with progressive removal, using the E recombination scheme. The minimalistic SlowJet code is much slower than FastJet [Cac06], and contains less options, but reconstructs the same jets if run under identical conditions. For details see the ";?>Event Analysis page.
              • Starting in gcc 4.6, it is possible to switch off specific warnings around specific blocks of code. Although version 4.6 is some way off from being commonly found, this option has now been introduced to switch off -Wshadow warnings in HepMCInterface.cc. For other compilers, or earlier versions of gcc, the old behaviour is retained.
              • Support for reading in gzipped LHEFs has been added in the LesHouches and SusyLesHouches classes. This also affects configure and Makefiles. Unless explicitly enabled, it should not affect anything. If enabled, it relies on the Boost and zlib libraries to function, so paths to these must be set appropriately, see the README file for details. The Boost header files can give very many shadow warnings, so -Wshadow is disabled if gzip support is enabled, as described above.
              • Introduce use of the HEPMC_HAS_UNITS environment variable in the HepMCInterface.cc and main32.cc codes to automatically check whether GeV and mm can be set as relevant units. If yes, then it is set in main32.cc. If no, a conversion from GeV to MeV is done explicitly in HepMCInterface.cc. Note that, for early HepMC versions, this means a change of behaviour. Thanks to Andy Buckley.
              • A new method Info::lhaStrategy() returns the Les Houches event weighting strategy where relevant, and 0 where not. For the strategies +-4 the event weight and sum, Info::weight() and Info::weightSum(), is now in units of pb at output, as it should be at input. (While internally mb is used.)
              • New flag Check:abortIfVeto allows the user to resume control over execution in case of a veto in the event generation process.
              • New method Event::at(i) returns reference to i'th particle in the event record.
              • Introduce the Fermi constant as one of the Standard Model parameters.
              • Included automatic pre-initialization of SLHA blocks MASS and SMINPUTS using PYTHIA's SM parameters and particle data table values.
              • SUSY: added sleptons (and sneutrinos) as resonances. Corrected 2-body decay widths of gluinos, squarks and gauginos. Added sleptonic decay modes to gaugino decays. Implemented 2-body decays of sleptons (and sneutrinos) into sleptons/leptons/gauginos. Corrected slepton couplings (they now look exactly like squark couplings, using a 6x6 slepton mixing matrix).
              • New parameter Diffraction:probMaxPert introduce to give more flexibility in transition from a nonperturbative to a perturbative description of a diffractive system.
              • Bug corrected in SigmaEW.cc, for the process WeakSingleBoson:ffbar2ffbar(s:gm). Previously, all outgoing quark flavours in this process were erroneously assigned ID code 5 (b quarks). This has now been corrected so the proper ratios are obtained, with u : c : d : s : b = 4 : 4 : 1 : 1 : 1, according to the squared quark charges.
              • Changes in FragmentationSystems and StringFragmentation to reject systems with three or more interconnected junctions. This may happen in baryon-number-violating scenarios in pp collisions, if both of the beam baryon junctions are resolved and get connected via an antijunction created by a hard-process BNV vertex. In principle, this could be addressed by an extension of the existing junction fragmentation framework. However, since it happens rarely, for the time being an error message is printed and the fragmentation restarted.
              • Change in Event::copy to safeguard against attempting to copy out-of-range entries. An attempt to copy a non-existing entry will now return -1.
              • Bug fix in the machinery for the user to force the setting of tau polarization.
              • Bug fix in the initial search for a maximum of the process cross section (only affecting rare cases).
              • Corrected angular decay distributions for two compositeness processes, Sigma2qq2qStarq and Sigma2qqbar2lStarlbar.
              • Extra check in HiddenValleyFragmentation to make sure that pointers which have not been assigned with new are not deleted.
              • Some further minor changes.
            • 8.160: 23 January 2012
              • The older term "multiple interactions" has been replaced by the new standard "multiparton interactions" one, and correspondingly the abbreviation MI by MPI. This affects everything: settings, class and method names, documentation, etc. It therefore becomes necessary to rewrite user code. However, so as to keep the immediate effort at a reasonable level, the old settings names are kept as aliases. Thus PartonLevel:MI and PartonLevel:MPI are equivalent, and similarly MultipleInteractions:pT0Ref and MultipartonInteractions:pT0Ref. Should you be using methods such as double Info::pTMI(int i) you need to edit the code, however. All the example/main* files have been updated accordingly.
              • A new option Beams:frameType = 5 has been added for the case where an external generator should provide LHA process information. The new Pythia::setLHAupPtr(...) method should then be used to link in this generator. The new switch Beams:newLHEFsameInit can be used to tell that a new LHEF should be used, but without the need for a new initialization. With these two changes, all the different ways of initializing can be covered by the Pythia::init() call with no arguments. The various init(...)options with arguments are deprecated and will be removed for PYTHIA 8.2.
              • The Pythia::stat() method, with no arguments, replaces Pythia::statistics(...), although the latter remains as a deprecated alternative.
              • New settings Init:..., Next:..., and Stat:... can be used to steer some details of the operation of the Pythia::init(), Pythia::next() and Pythia::stat(), respectively. In particular it affects the amount of printout at the various stages of operation. See ";?>here for further details. This change involves several code changes, but in documentation rather than physics. Most of the Main:... settings are deprecated as a consequence.
              • The sample main programs in the examples subdirectory have been updated. This includes a change to the new favoured methods and settings outlined above, plus some update of the physics contents. Some of the examples have been combined, some others have been added (e.g. for R-hadrons), and as a consequence some renumbering has been made. See the modified list of ";?>sample main programs for the new status. In particular note that (the new) main61.cc allows streamlined input and output in HepMC, like main42.cc (previously main32.cc), but additionally links to LHAPDF.
              • The examples/configure script has new optional argument --with-pythia8. It can be used to set the new PYTHIA8LOCATION environment variable, which then is used in examples/Makefile to give the path to the PYTHIA library. Thereby it becomes possible to relocate (parts of) the examples directory and still obtain the correct path. Thanks to Mikhail Kirsanov.
              • Polarization information has been included as a new Particle property, that can be set by void pol(double polIn) and obtained by double pol(). Default value is 9., in agreement with the Les Houches standard. Event listings have been expanded to optionally display this information. Currently polarization is not used internally.
              • The matrix element merging machinery has been modified as follows.
                - Improved handling of the hard process, so that MadGraph5-produced LHE files do not produce problems (sometimes, the choices of MG4 on what to put into a LHEF have changed in MG5).
                - Improved handling of colour for easier handling of states with many quarks (the code has been tested for states with up to 5 q qbar pairs and some gluons).
                - Improved checking which clusterings are allowed. Now, clusterings should immediately be rejected if they lead to unphysical states, without the need to explicitly construct these states. This was needed to get t tbar production, VBF and some simple SUSY processes running with reasonable generality.
                - Improved handling of incomplete histories. Now there is an additional switch allowing code to try to swap some colours when fewer clusterings than requested have been found.
              • Updates in the handling of graviton resonances in scenarios with extra dimensions.
                - Now all G decays have correct angular distribution, which was not the case before for W/Z decays.
                - Added the possibility for G to only couple to longitudinal W/Z bosons, which affects both the width and angular distributions.
                - Added decays to Higgs pairs, G -> hh.
              • Bug fix in the findJunctions() function in ProcessLevel.cc. Changes introduced in version 8.145 (to allow for junctions in baryon-number-violating processes) did not correctly handle the remapping of color tags that can be applied when adding beam remnants to events with multiparton interactions. A simpler and more stable algorithm is now applied for the simplest cases, with the more complex one only invoked for cases such as BNV, which are normally considered before remnants are added, hence avoiding this particular problem. Also some other changes in the handling of junction, including a safeguard to reject systems with three or more interconnected junctions.
              • Bug fix and updates to the SLHA interface. Possibility of infinite loop during ProcessLevel::initSLHA corrected. Modifications to SusyLesHouches to allow interpretation of SLHA1 spectra with R-parity violation. Rather than reject spectra that do not conform fully to the SLHA2 standard for RPV, the interface will now first look for SLHA1 mixing matrices and attempt to translate those into SLHA2 ones if possible. In this case, warnings that the expected SLHA2 blocks were not found will be printed. It is up to the user to check that the derived SLHA2 information is correct. Corresponding additions to SusyCouplings.cc to extract mixing-matrix information from the relevant SLHA2 RPV blocks when RPV is switched on.
              • Updated SLHA example main24.cmnd to use new example spectrum, cmssm.spc, corresponding to CMSSM point 10.1.1, obtained with SOFTSUSY 3.3.0. Thanks to B. Allanach for providing the new spectrum file.
              • A new include/FastJet3.h header file simplifies interfacing of FastJet to Pythia. For details see documentation in the file itself. Thanks to Gavin Salam for this contribution.
              • The handling of diffraction has been made more flexible. Specifically the "total" Pomeron-proton cross section can now be made to depend on the mass of the diffractive system. This does not affect the diffractive cross section in pp collisions, which is set separately, but is used in the MPI machinery to affect the average number of interactions per Pomeron-proton collision. Furthermore, the allowed range for some parameters has been expanded. Thanks to Robert Ciesielski.
              • New method Pythia::forceTimeShower(...) can be used to generate a single final-state cascade from a set of partons, without any knowledge of prior history. This is mainly intended for toy studies. The meaning of the ProcessLevel:all switch has been modified so that this parton-level function is available, but not any others at this level.
              • ATLAS tune A2 now included. Thanks to Deepak Kar for providing it.
              • Change in the handling of recoils of timelike showers in resonance decays, in cases of coloured resonances such as t -> b W. In the first step the W always acts as recoiler to the b, but in subsequent step previously the W remained as recoiler to one dipole, while now all QCD-radiating partons recoil against another coloured parton. The old behaviour could give a (small) unphysical spike of radiation collinear with the colourless recoiler in the subsequent emissions (while the pattern of the first was and remains correct). The old behaviour can be recovered for checks, see TimeShower:recoilToColoured. Thanks to Yevgeny Kats for pointing out this issue (previously noted for Pythia 6 by several persons).
              • Bug fixes for rootexamples/Makefile and restoration of some deleted information in rootexamples/README. Thanks to Axel Naumann and Bernhard Meirose.
              • Bug fix, so that displaced vertices are possible in resonance decay chains. Thanks to Daniel Blackburn and Andy Buckley for pointing this out.
              • Bug fix for Info counter 2.
              • Bug fix so that sextet quarks now are read in correctly from Les Houches Event files; previously the (anti)colours were set to 0.
              • Year updated to 2012 in copyright statements etc.
              • Reformatting to reduce the number of code lines with more than 79 characters.
              • Pythia::initSLHA() moved from public to private.
              • Remove warning message when tau polarization is set by hand.
              • Several minor changes to reduce the number of warnings issued by the clang compiler. The origin of some warnings remains unclear so those remain to track down (could also be compiler bugs; note that we discuss warnings, not errors). Thanks to Randy MacLeod for bringing this up.
              • The worksheet has been updated to be in step with Pythia 8.160.
              • Several other minor corrections in the code and documentation.
            • 8.162: 12 March 2012
              • A new option allows for several partons to share the recoil in final-state radiation, see";?>Timelike Showers. It is mainly intended to be used in the context of matching to matrix elements, and so only to be used in the first few branchings.
              • Several new processes for LED dijet production, see ";?>Extra Dimensions.
              • Small update of the Sigma2ffbar2LEDllbar and Sigma2ffbar2LEDgammagamma LED processes.
              • New Sigma2QCffbar2llbar ";?>contact interaction process.
              • Inclusion of a new method in the ";?>matrix-element merging framework to influence the construction of histories, e.g. to already in the construction of histories disallow paths that fail the 2 -> 2 cuts.
              • Further minor updates of the matrix-element merging code, mainly for improved clarity.
              • Minor bug fix in the handling of beam and event information fed in from an LHAup instance.
              • Minor bug fix for potential crashes from uninitialized variables for the merging machinery when merging is not used.
              • Updated History class for matrix element merging, also avoiding some compiler warnings.
              • Bug fixes in the handling of correlated mass choices in resonance decays, such as H -> Z^*0 Z^*0.
              • Bug fix when the process-level execution is switched off, where Info::isResolved() could be called before its value was initialized. Thanks to Christian Pulvermacher for finding this.
              • Corrected matrix-element expression for mass selection in A^0 -> Z^*0 Z^*0 and A^0 -> W^*+ W^*-.
              • SM Higgs mass updated to 125 GeV and default width and branching ratios modified accordingly. Minor technical improvements of width calculation.
              • The usage of nested classes has been removed from SusyLesHouches, since it could give compilation errors on some platforms. The new class names begin with LH and all classes have been put inside the Pythia8 namespace.
              • Minor Makefile updates. Thanks to Mikhail Kirsanov.
              • Minor changes to avoid some clang compiler warnings on the Mac OS X platform.
            • 8.163: 27 March 2012
              • New methods in the ";?>Info class, id1pdf(), id2pdf(), x1pdf() and x2pdf(), to denote the partons for which parton distribution values have been defined. Previously this was assumed to agree with the incoming partons to the hard process, the same methods without the pdf qualifier. However, now the POWHEG approach offers a counterexample. Also the reading and handling of Les Houches (and other) events, and the interface to HepMC, has been modified accordingly.
              • The decay of Higgs and top resonances read in from Les Houches Event files is now performed with angular correlations as for internal processes. LHE files should normally contain all process-specific resonance decay chains and, if not, decays are made isotropic. The H -> WW/ZZ -> f fbar f' fbar' and t -> b W -> b f fbar correlations are process-independent, however, and thus can be handled internally. If part of the decay chain has already been set, e.g. H -> WW/Z> or t -> b W, then the subsequent decays are still isotropic.
              • Updated instructions how to link to HepMC, in README.HepMC.
              • Bug fix in the turn-on of resolved diffraction for low CM energies. Thanks to Erwin Visser.
              • Bug fix in the handling of string junctions at very high energies, caused by numerical errors. Thanks to Erwin Visser.
              • Some other small changes, mainly aesthetics.
            • 8.165: 8 May 2012
              • The MBR (Minimum Bias Rockefeller) model for single, double and central diffraction [Cie12] is included as new option ";?>Diffraction:PomFlux = 5. It is specifically intended for p p and pbar p interactions, and is currently the only option that also supports central diffraction. Thus the basic machinery for Central Diffraction (a.k.a. Double Pomeron Exchange) has now been implemented. See examples/main04.cc for an example. Thanks to Robert Ciesielski for contributing the new code.
              • For a tau lepton in an external process, by default the SPINUP number in the Les Houches Accord now is interpreted as giving the tau helicity, and is used for its decay.
              • A tau coming from a W now defaults to being purely lefthanded when neither of the existing matrix elements apply.
              • Decay mode t -> H+ b included as an option.
              • Four ATLAS tunes have been implemented as options for Tune:pp: A2-minbias-mstw2008lo, AU2-cteq6l1, AU2-mstw2008lo, and AU2-ct10. The new flag Tune:preferLHAPDF can be used to switch between the LHAPDF and the internal implementation of a PDF set, in cases where both are available.
              • Reorder libraries in examples/Makefile, specifically move LIBGZIP so that it is properly linked when used. Thanks to Erik Schnetter.
              • Minor modification so that LHAPDF can be used for PDFs in the hard process, with one of the built-in PDFs for the rest, even if LHAPDF is compiled so as to handle only one concurrent PDF set.
              • Bug fix, that ParticleDecays:mixB = off did not switch off B0 - B0bar and Bs0 - Bs0bar mixing. Thanks to James Catmore.
              • Bug fix for the handling of gluon polarization of initial-state radiation, where an anisotropic azimuthal distribution was inadvertently generated in some 2 -> 1 processes. The update also includes always setting the second daughter zero for the two partons coming in to a hard 2 -> 1 process. Thanks to Antonio Policicchio.
              • Bug fix, that the setting of the number of user hooks MPI steps did not use UserHooks::canVetoMPIStep() properly.
              • Some other small changes, mainly documentation and aesthetics.
            • 8.170: 21 September 2012
              • Streamline default behaviour and options for choice of GeV or MeV for output to the HepMC event format, see ";?>HepMC Interface. Also set the mass of HepMC particles explicitly, rather than having it calculated implicitly. Thanks to James Monk and Andy Buckley.
              • The tau decay machinery has been further augmented with matrix elements and form factors for a variety of decay modes, such that all modes with a branching ratio above 0.1% are fully modeled. Several new classes and methods have been added to this end, Also, a tau pair coming from a Z^0 decay is now handled by assuming the Z^0 to be unpolarized when neither of the existing matrix elements apply. Taus coming from B baryons are handed as for B mesons.
              • Flavour violating decays have been added to the squark, gluino, neutralino and chargino decay tables.
              • Extend the UserHooks::subEvent(...) method so that it also works passably at the process level. Also new option for UserHooks::omitResonanceDecays(...).
              • New methods UserHooks::canVetoPartonLevelEarly() and UserHooks::doVetoPartonLevelEarly( const Event&) are intended to be used the same way as the existing ones without Early in their names, but allow veto right after the ISR + FSR + MPI evolution, before beam remnants are added and resonance decays are considered.
              • Central diffraction now available for all ";?>PomFlux options, not only the MBR model. This has been constructed by analogy with the respective assumptions made for single diffraction, but includes some arbitrariness. Therefore the cross section is left easily rescaleable and, for backwards compatibility with tunes that does not contain it, easily possible to switch off, see the ";?>relevant section.
              • Reading of ALPGEN parameter and event files has been added, see ";?>ALPGEN and MLM Merging.
              • MLM matching has been added, as a first step for ALPGEN events, see ";?>ALPGEN and MLM Merging.
              • The CKKW-L merging machinery has been upgraded in a number of respects.
                - More thorough treatment of pp>bb~e+e-veve~ with additional b-jets.
                - Corrected hard mu_r and mu_f choices for dijet and prompt photon.
                - More ways to define a hard process, e.g. with the LEPTONS and NEUTRINO tags. The merging will understand LHE files for mixed processes (e.g. W+ and W- production together).
                - More merging scale definitions.
                - More freedom to generate all possible histories.
                - Internal check (and cut) on Les Houches events in Pythia::mergeProcess if merging scale value of the events is below the value given to Pythia by setting Merging::TMS.
              • It now works to have R-parity violating decays of R-hadrons, i.e. baryon number violation in a vertex displaced from the primary one.
              • The documentation of diffractive processes by the ";?>Info methods has been expanded and corrected. This also include the list() method.
              • Particle masses and widths have been updated to agree with the 2012 RPP values [Ber12]. Thanks to Piotr Zyla for data file and James Catmore for program to update the PYTHIA tables from this input.
              • New methods jetAssignment and removeJet added to the SlowJet class.
              • Introduce angular correlation in decay chain H -> gamma Z0 -> gamma f fbar. Thanks to Tim Barklow and Michael Peskin.
              • Introduce simple way to bias the selection of 2 -> 2 processes towards larger pT values, with a compensatingly decreasing event weight, see ";?>Phase Space Cuts. Only offers a subset of the possibilities allowed by UserHooks, but simpler to use. The main08.cc program has been expanded to illustrate this possibility, and also expanded to include low-pT subsamples.
              • The two remaining non-NLO tunes from [ATL12] are now included.
              • The ";?>Info methods nTried, nSelected, nAccepted, sigmaGen and SigmaErr now takes the code of an individual process as an optional argument.
              • It is now possible to generate resonance decays, followed by showers and hadronization, without having them associated with any specific process. This is part of an expanded ";?>Hadron-Level Standalone machinery, as before triggered by ProcessLevel = off, but additionally requiring Standalone:allowResDec = on. Input can either be directly into the event event record or via a (simplified) Les Houches Event File.
              • New configure script options --installdir, --prefix and --datadir can be used to set the location(s) to which the library, header and data directories will be copied by a make install subsequent to the make. Thanks to Mikhail Kirsanov.
              • Fix charge in antiparticle name when particle read in from SLHA file. Thanks to Johan Alwall.
              • Pointers now only compared with == and != (not e.g. > 0), to avoid warnings in gcc 4.7.
              • New check that version number of the code matches that of the XML files. If not, no events can be generated. Thanks to James Monk for suggestion.
              • New check that mother and daughter indices have been set to give a consistent event history. Can be switched on/off with the new Check:history flag.
              • A new method LHAup::newEventFile has been added to switch to reading in events from another LHE file without having to reinitialize the whole class. Lower-level routines like openFile and closeFile have been added to handle correct order of operations also when an intermediate gzip decompression step is involved.
              • LHAup::eventLHEF() can now be called with an optional argument false, to make event files somewhat smaller by reducing the amount of blanks.
              • A new mode Beams:nSkipLHEFatInit introduced to skip ahead the first few events in a Les Houches Event File (cf. the LHAup::skipEvent(nSkip) method).
              • Introduce a new pair of user hooks that can be used to reject the sequence of hard-process resonance decays, without rejecting the production of the primary resonances.
              • The possibility of separate multiplicative prefactors to the renormalization and factorization default pT^2 scale has been introduced for both timelike and spacelike showers.
              • Bug fixes in history information for R-hadron production, which also fixes HepMC conversion in this case.
              • Bug corrected in SigmaSusy.cc, for chargino+neutralino production. Indexing error for incoming quark states in the process Sigma2qqbar2charchi0, resulted in incorrect CKM factors.
              • Corrected a bug in SusyLesHouches.cc, for NMSSM spectra. The unitarity check on the neutralino mixing matrix was faulty, leading to erroneous messages about unitarity violations and SUSY being switched off.
              • Bug fixes in the handling of resolved and unresolved diffractive events. Thanks to Robert Ciesielski for debug.
              • Do not set up FSR dipoles for 2 -> 1 processes.
              • Check that some channel open for resonance decays. Also further check whether resonance decay treatment should be invoked.
              • Bug fix in reading of particle names from SLHA input.
              • Change mass, width and decay mode(s) of D*_s(10431). Thanks to Michal Petran.
              • Bug fix in leptoquark production (lepton sign in q g -> LQ l).
              • New argument added to SpaceShower::reassignBeamPtrs for diffractive event processing, as already available for TimeShower.
              • Do not write warnings in SpaceShower for weights above unity if the evolution scale is below 1 GeV^2.
              • Add default values for member variables in some constructors, and some related changes for AlphaStrong code.
              • Warn if negative-energy parton in hadronization.
              • The MPI pT values assumed in the beam remnant setting of primordial kT and colour reconnection probability were incorrect for diffractive events.
              • The arrays with MPI information were not reset when parton or hadron level fails and a new try is made. Only affected few events.
              • MPI statistics can not yet be accumulated for diffractive events, and therefore the relevant routine is no longer called.
              • Bug fix in the double parton scattering suppression from energy-momentum conservation.
              • Outgoing proton masses were not set in the event record for elastic scattering (but kinematics handling was correct).
              • Bug fixes in the identification and documentation of junctions, previously leading to some unnecessarily rejected events. Also other improvements leading to fewer errors.
              • Slightly increased values for FragmentationSystems:mJoin and StringFragmentation::FACSTOPMASS to reduce failure rate, without noticeably affecting event properties.
              • The Les Houches cross section error is now taken into account in the final Pythia error for strategies +-3. New methods LHAup::xSecSum() and LHAup::xErrSum() provide the necessary information.
              • When a tau pair comes from a massless photon, in dipole shower evolution, for the decay description the mother photon is reassigned to have the sum of the tau momenta.
              • Minor change in initialization sequence for user hooks, to allow for more flexibility.
              • Do not print warnings when multiparton interaction weights are only slightly above unity.
              • Do not write warnings for three known particles that are so close to threshold that widths are switched off to avoid trouble.
              • Some minor typographical changes.
            • 8.175: 18 February 2013
              • Richard Corke and Stefan Ask leave as active authors, and have new e-mail addresses.
              • Jesper Roy Christiansen and Philip Ilten join as new authors.
              • A severe bug found and corrected in the handling of junction fragmentation. For some string topologies it could lead to parts of partonic systems mainly aligned along the beam axis to obtain an effective tilt, thereby giving rise to a pair of opposing jets that should not be there. The bug was an unfortunate side consequence of the improvement of junction handling introduced in version 8.170, and do not affect versions prior to that. To the largest extent possible, it is recommended to avoid this version. Potential errors are likely to be most relevant for processes at low pT, whereas processes that already have a large scale proportionately are less affected. Sincere apologies, and thanks to Hannes Jung for discovering it.
              • The initialization is aborted when the user tries to change the value of a non-existing variable in the Settings or ParticleData databases, and it becomes impossible to generate events. This may be rather brutal, as opposed to the former policy of ignoring such commands (except for a warning), but avoids that the user wastes time on a run that is likely not to give the wanted results. Thanks to Gavin Salam for stressing this point.
              • Major updates of the merging code. CKKW-L code is made more flexible, and now includes additional options to facilitate merging of additional jets in MSSM processes. Unitarised ME+PS merging (UMEPS) is introduced as a new merging scheme for tree-level input. An example main program for UMEPS is added. UMEPS is documented in the new section ";?>UMEPS Merging. NLO merging methods are now functional. Two NLO merging schemes are implemented: NL3 and unitarised NLO+PS merging (UNLOPS), both of which are illustrated with example main programs. NLO merging is documented in ";?>NLO Merging.
              • The machinery for the MLM-style matching of jets has been expanded to cover input either from ALPGEN, as before, or from Madgraph (or other LHEF input), and expanded to cover either a matching algorithm based on the one in ALPGEN or the one in Madgraph. See ";?>Jet Matching for details.
              • Neutrons and antineutrons are now allowed as incoming beam particles. The neutron PDF is derived from the chosen proton PDF by simple isospin conjugation, and total/elastic/diffractive cross sections are assumed the same as for protons.
              • Update in Pythia.cc, to allow user to override SLHA mass values by hand, controlled by the new flag SLHA:allowUserOverride. This was motivated by people wanting to be able to read in a base SLHA spectrum and then quickly scan over particular mass values manually. Corresponding documentation update in SUSYLesHouchesAccord.xml.
              • Updates to the ResonanceWidths and SUSYResonanceWidths classes, to merge common initialization steps into the base class. Corresponding documentation update in SemiInternalResonances.xml. Also some cosmetic changes in SUSYResonanceWidths to improve conformity with CODINGSTYLE rules.
              • The SlowJet jet finder is updated with an option for an alternative R separation based on cosh(Delta y)-cos(Delta phi).
              • Statistics information on the separate subprocesses among the Les Houches external input is improved.
              • The sophisticated tau decay machinery has been expanded so that it can also handle production of taus in hypothetical lepton-number-violating processes, such as H0 -> tau+ mu-.
              • Branching ratios for most light hadrons, and the tau lepton, have been updated to agree with the 2012 Review of Particle Physics [Ber12], by Anil Pratap Singh.
              • Photon radiation can now be included in leptonic two-body decays of hadrons by setting the new switch ParticleDecays:allowPhotonRadiation = on. The lower shower cutoff TimeShower:pTminChgL has been reduced so as to let the simulated photon spectrum extend to lower energies.
              • A new switch MultipartonInteractions:bSelScale has been introduced, to determine the relevant mass or pT scale of an event for the selection of impact parameter in the MPI framework. In spite of a changed default behaviour (the old being option 3), practical consequences are small for most processes.
              • The new UserHooks::retryPartonLevel() method can be overloaded, so that the same hard process is reused for a new try on the parton level, rather than being rejected completely. Thanks to Christian Bauer for suggestion.
              • A new method Event::undoDecay(int i) can be used to remove the daughters of a particle, and further descendents. Does not work for removing the daughters of a parton.
              • The interface to HepMC has been updated. In particular the support for old version has been removed, thereby allowing significant simplifications. The list of methods to set and get the behaviour of the conversion routine has also been updated. The set_event_scale method now stores the renormalization scale (rather than the pT stored previously). The examples main41, main42, main61, main62 and main84 have been updated accordingly.
              • Four new methods to interrogate the default values of the four different kinds of settings.
              • The Vec4 class has been expanded with methods to return true rapidity or pseudorapidity, and the R distance in (y, phi) or (eta, phi) cylindrical coordinates. Thanks to Andy Buckley.
              • The copy and = constructors of the Pythia class are made private so that compilers will block use of them. Thanks to Andy Buckley.
              • New option of the Pythia constructor, to omit the banner printout where necessary. Also new master switch Print:quiet to switch off most runtime program messages. Thanks to Andy Buckley.
              • Updates in the machinery that restores all affected values to their defaults before setting a new tune.
              • A new Vect class has been introduced for the ";?>Settings database. It can be used to store a vector of double-precision real values.
              • Three new groupings of existing QCD processes: SoftQCD:inelastic, HardQCD:hardccbar and HardQCD:hardbbbar.
              • New possibility to set the a and b parameters of the Lund fragmentation function separately for heavy flavour. Especially the b is expected to be universal, but Aurelien Martens and Eli Ben-Haim have found improved fits by relaxing this condition, so we formalize this possibility without recommeding it.
              • Method Pythia::getPDFPtr is made public so it can be used also outside the Pythia class to access PDF sets. Internally the PDF bookkeeping is modified to allow for the simultaneous handling of several PDF sets. Thanks to Mathias Ritzmann for providing code changes.
              • It is now possible to read the separate scale values of all outgoing particles, if this info is stored as a single line in an LHEF, begun by a single hashtag character. This is currently nonstandard and may evolve.
              • Some improvements to the install targets code in the Makefile and error detection in examples/configure. Thanks to Mikhail Kirsanov.
              • The CC and FC global environment variables can be set to specify the C++ and Fortran 77/90 compilers, otherwise set in configure and examples/configure. Thanks to Mikhail Kirsanov.
              • Check of shell choice in configure removed. Thanks to Andy Buckley.
              • Minor modifications in the Makefile and text for Root examples, relevant if shared libraries are used.
              • Previously the whole std namespace has been made available in PythiaStdlib.h. Now this behaviour has been replaced by the already-existing alternative, where only a part of std is made available, and only inside the Pythia8 namespace. Thus user code does not become reliant on the choices in PYTHIA. Some related smaller code rearrangements. Thanks to Andy Buckley.
              • When the "second hard" machinery is used to set two hard processes, the old behaviour for the SpaceShower:pTmaxMatch = 0 and TimeShower:pTmaxMatch = 0 options was to use the combined final state of the two processes to decide what pT_max scale to use. This could have unexpected consequences. Now each process is analyzed separately, and therefore has a separate scale. Also for MultipartonInteractions:pTmaxMatch = 0 the two interactions now are analyzed separately. It is then enough that one of them should limit pT_max of subsequent MPI's for such a restriction to be imposed. Thanks to Monika Jindal for discovering this bug.
              • The TimeShower:pTdampMatch option had no effect if switched on, since some code was missing. The manual description of it and the more relevant SpaceShower:pTdampMatch has been updated.
              • One minor bug fix and some corrections to make the code compile on Windows/VisualC++-2010. A simple error function parametrization has been added to PhaseSpace.h and SigmaTotal.h, to be uncommented in case erf(x) is not available by default. Thanks to Guy Barrand for providing the information.
              • Break a closed dependency loop between ParticleData.h and ResonanceWidths.h. Thanks to Andreas Schaelicke and Andy Buckley.
              • In the examples/mainXX.cc programs, class instances that have been created with a new are explicitly deleted at the end of the run. Useful if trying to track memory leaks.
              • Bug fix for R-parity violating decays of R-hadrons, to treat the special case of sequential resonance decays after the RPV one. Thanks to Mariangela Lisanti for pointing out this bug.
              • Changed the maximum allowed value for Tune:pp. Thanks to Yevgeny Kats.
              • Bug fix in the z-value weight for QED ISR emissions.
              • Some destructors moved for improved consistency.
              • Constants DEBUG renamed DBSUSY in the SusyCouplings and SusyResonanceWidths classes to avoid confusion. Thanks to Guy Barrand.
              • Many typos corrected and some other minor improvements of the online documentation.
              • The year has been updated to 2013 in files.
            • 8.176: 18 April 2013
              • Introduce weak shower, whereby W^+- and Z^0 gauge bosons can be produced interleaved with ordinary QCD and QED emissions. Currently only available for final-state radiation, and off by default, see ";?>Timelike Showers. A new status code 56 denotes W^+- and Z^0 gauge bosons produced by the FSR parton showers.
              • The gauge bosons produced by showers decay at the end of the parton-level step. New identity codes 93 for a Zcopy and 94 for a Wcopy can be used to set the decay modes of shower-produced gauge bosons separately from hard-process ones, but do not appear in event listings.
              • The Particle class has been updated with a pointer to the mother Event class, replacing the previous pointer to the ParticleData class. Thereby several old methods in the Event class can obtain new equivalents for the Particle one. That is, a call event.method(i) instead can be written event[i].method(). The duplicated methods are statusHepMC, iTopCopy, iBotCopy, iTopCopyId, iBotCopyId, motherList, daughterList, sisterList, isAncestor and undoDecay. Omitted is sisterListTopBot, while sisterList obtains an optional argument. A new method index is introduced. The now redundant Event class methods will be removed in PYTHIA version 8.2. Thanks to Andy Buckley for suggestion.
              • The initialization of SUSY couplings and particle data has been moved from the Pythia and ProcessLevel classes to a new dedicated SLHAinterface class.
              • Some SUSY 3-body decays have been implemented with Matrix Element weighting.
              • New method Info::scalup() returns the Les Houches SCALUP variable. This method is now used instead of QFac() in main31.cc, to set maximal scale for shower radiation in case that the event contains no POWHEG emission, and thereby sidesteps a potential bug when PDF information is provided in the Les Houches Event File. Also some default values have been changed in main31.cmnd. Thanks to James Monk.
              • New parameter LesHouches:mRecalculate can be used to prompt the recalculation of a particle mass from its four-momentum. This may be required for Les Houches input events where the nominal mass of the particle species is stored in the mass slot, rather than the actual mass of the current particle, as foreseen.
              • Extra checks that tracing of junctions in particular and partonic colour singlets in general are only performed when the event record contains coloured unhadronized partons. Thanks to James Catmore.
              • Minor correction related to GZIP support. Thanks to James Monk.
              • Recalculate the phase space of diffractive processes for each event when variable beam energies are allowed. Thanks to Oldrich Kepka for finding the bug.
              • Fix a bug whereby a gluon in diffractive systems would obtain a light-quark mass.
              • The Pythia::check() method can also check that each particle obeys E^2 - p^2 = m^2 (within numerical precision). Speed up the checks on mother-daughter history by streamlining the handling of simple cases.
            • 8.180: 22 September 2013
              • Nishita Desai joins as new author.
              • All the header files include/*.h have been moved to include/Pythia8/*.h to better comply with conventions in other libraries (* = generic name). Thus also all code lines #include "*.h" that refer to PYTHIA files have been changed to #include "Pythia8/*.h". Thanks to Andy Buckley for suggestion.
              • The class that converts PYTHIA events to the HepMC format is renamed from I_Pythia8 to Pythia8ToHepMC, the files where the class resides from HepMCInterface.h/.cc to Pythia8ToHepMC.h/.cc, and the subdirectory of the .cc file from hepmcinterface to pythia8tohepmc. This clarifies the role of the class and avoids potential future name clashes with other interfaces. Makefiles and example main runs have been modified accordingly. Thanks to Andy Buckley.
              • The configure/Makefile step has been extended such that a bin/pythia8-config script is constructed, to simplify subsequent linking of PYTHIA 8 and other libraries to your main program. See the README file for further instructions, the new "Compling programs against PYTHIA 8" section. Thanks to Andy Buckley for code and text.
              • The "minbias" event class has been renamed into the (inelastic) "nondiffractive" one, since the "minbias" denomination should be reserved for an experimental procedure. Needless to say, also the separation into diffraction or not could be made by experimental procedures, but here it is more generally accepted that there is an underlying theoretical description that takes precedence in cases of conflict. Thus the SoftQCD:minBias flag has been remaned SoftQCD:nonDiffractive, and the Info::isMinBias() method has been renamed Info::isNonDiffractive(). The old names have been retained as alternatives for now. Thanks to Andy Buckley.
              • Four PDF sets have been added from the NNPDF2.3 QCD+QED family: the central sets for LO with alpha_s(M_Z) = 0.130, LO with alpha_s(M_Z) = 0.119, NLO with alpha_s(M_Z) = 0.119, and NNLO with alpha_s(M_Z) = 0.119. Thanks to Juan Rojo and Stefano Carrazza for providing the code.
              • The fjcore version 3.0.5 code from FastJet has been included with the PYTHIA distribution. SlowJet now by default becomes a front end to fjcore, but the old behaviour is retained as an option. The new approach is faster, but the older one still offers a few extra possibilities. Note that the new useFJcore argument to the SlowJet constructor has been included as a new last-but-one argument, since the last one is likely to be used much more infrequently and logically depends on the value set for useFJcore. Thanks to Matteo Cacciari, Gavin Salam and Gregory Soyez for making the fjcore code freely distributable.
              • New method constituents(i) in FastJet returns a vector with the indices of the particles belonging to the i'th jet.
              • The global recoil option for final-state showers has been extended with a few more options to improve possibility for matching to output from other programs, such as aMC@NLO.
              • Further extensions of the weak-showering machinery, but still experimental. Now also includes W/Z emission in the initial state.
              • Introduce new qqbar option for SigmaProcess::inFlux() and update documentation.
              • Improve the description of meMode for resonances and illustrate how to force specific Higgs branching ratios in main16.cmnd.
              • Added two previously missing SUSY processes for associated production of a gluino with a neutralino or chargino: SUSY:qqbar2chi0gluino and SUSY:qqbar2chi+-gluino, using the cross section expressions in [Fuk11]. Validated against PYTHIA 6 and XSUSY.
              • Added direct slepton production from q qbar annihilation, SUSY:qqbar2sleptonantislepton. Validated against PYTHIA 6.
              • Corrected some slepton and squark EW couplings in SusyCouplings.
              • Generalized the cross section formulae for SUSY:qg2squarkgluino to the case of non-minimal flavor violation, using the expressions in [Fuk11]. Validated against PYTHIA 6 and XSUSY. The new implementation is compatible with both SLHA2 and SLHA1, whereas the older was only compatible with SLHA1.
              • Generalized the cross section formulae for SUSY:qqbar2gluinogluino to the case of non-minimal flavour violation, using the expressions in [Fuk11]. (Also corrected a factor 2 in that paper on the color factor for st and su interference terms.) The new implementation is compatible with both SLHA2 and SLHA1, whereas the older was only compatible with SLHA1.
              • Changed the default meMode for SLHA DECAY modes to 100, to allow off-shell decays. Enabled the user to choose a different meMode if desired, via a new mode, SLHA:meMode. If values different from 100 are selected (e.g., 103), modes that are extremely far off shell (defined as needing a fluctuation of more than 100 times the root-sum-square of the widths of the mother and daughter particles) will still default back to 100, though the user may of course still switch them off if so desired. Added documentation about this in SusyLesHouchesAccord.xml. Deleted the parameter SLHA:minDecayDeltaM, which would prevent the possibility of off-shell decays unless set to a large negative value.
              • Added calculation of decay lengths to SLHA DECAY modes.
              • Updated documentation of SUSY processes and SLHA-related parameters. Additional reference to the new cross sections included in the bibliography.
              • Allow six-flavour running of alpha_s above the top threshold, and implement option with CMW rescaling of the Lambda values, for use in coherent showers.
              • The merging code has been updated, with corrected handling of massive partons. This amends problems in tt̄, and makes clusterings of massive emissions W, Z, ~g possible. The bookkeeping for the hard process has been upgraded to accommodate more general BSM processes. The treatment of incomplete histories has been upgraded, so that histories which allow for at least one clustering will be used in the unitarisation. Also, states that do not allow for any clustering will not be subject to the (internal, optional) cut on the input events any longer, to guarantee full phase space coverage. This is important for processes for which a non-negligible fraction of states lead to incomplete histories, e.g. tt̄W production. Further, functionality for reclustering FSR off SUSY particles has been added. A new setting allows more easily to switch between 4-flavour and 5-flavour merging schemes.
              • The main85.cc - main88.cc have obtained support for zipped LHE input files, and have nicer printing of the inclusive cross section at the end.
              • Introduced new mode LesHouches:setLifetime so that the lifetime information in Les Houches input can be replaced by the standard PYTHIA selection procedure. By default this is applied to tau leptons, since some matrix-element generators do not set this lifetime. Thanks to James Monk and Thorsten Kuhl.
              • A new examples/main46.cc illustrates how to write a ProMC file with PYTHIA events. Thanks to Sergei Chekanov.
              • The Vect class has been renamed PVec and a new MVec class has been introduced along the same lines, see the ";?>Settings database. They can be used to store a vector of double-precision real or integer values, respectively, i.e. of parms or modes, hence the names. Thanks to Abram Krislock.
              • Two new vectors of integers SUSY:idVecA and SUSY:idVecB have been introduced to allow a more flexible selection of final states in SUSY processes, see the ";?>SUSY process selection page. The selection machinery has been expanded to cope. Thanks to Abram Krislock.
              • New switch PartonLevel:earlyResDec to give first simple option where resonances are allowed ro decay before colour reconnection and beam remnants are added.
              • Renamed the mass(...) methods to mSel(...) in the Particle, ParticleData and ParticleDataEntry classes, to avoid users mistaking Particle::mass() for Particle::m().
              • Fixed a missing (unused) argument in some derived classes when the mRecalculate parameter was introduced in Les Houches code in version 8.176.
              • Removed several unused class variables from header files, based on new compiler information.
              • Fixed a bug in Sigma2ffbar2HposHneg, where int(...) was used instead of abs.(...). Thanks to Vittorio Zecca.
              • Fixed missing re-initialization of Breit-Wigner mass generation parameters for externally set new resonance widths. Thanks to Vittorio Zecca.
              • Fixed several places where division by zero or adressing of arrays out-of-bounds could occur. While some were trivial, others revealed underlying errors, notably in the handling of some SUSY processes and resonances. New checks against unphysical SLHA input have been implemented. Also some bug fixes in the new weak-shower ISR component, the sphericity analysis, the event undo-decay option, and more. Thanks to Vittorio Zecca.
              • Bug fix in the tau decay description for decay chains like H0 -> A0 A0 -> 4 tau, caused by an erroneous assignment of the number of spin states. Thanks to Brock Tweedie.
              • Add setting of some TimeShower variables that might remain uninitialized. Thanks to Christian Pulvermacher.
              • Extra check in TimeShower for incoming massive particles, where a recalculation of kinematics to an equivalent massless case could give a slightly negative effective dipole mass (with endpoint masses subtracted). Thanks to Paolo Torrielli.
              • Updated manual on how to implement new showers, mainly detailing new optional method arguments. Thanks to Mathias Ritzmann.
              • Corrected bug in SigmaSUSY which caused flavour violating slepton production (for R-parity conserving cases too).
              • Corrected bug in SusyCouplings where tan(beta) was not read from LHA file for RPV spectrum.
              • Modified the contact interaction term normalization of the f fbar -> l lbar process to agree with the one used in PYTHIA 6. Documentation of the ContactInteractions:Lambda updated to reflect this. Thanks to Daniel Hayden.
              • Introduced copy constroctor for the Event class.
              • Reset the Higgs mass range when its mass is changed in examples/main14.cc.
              • Remove obsolete examples/main91.cc and associated Makefile code.
              • Catch cases where junction topologies are sent to the ministring machinery, which is not set up to handle it, and therefore could give segmentation faults. Very rare.
            pythia8-8.1.80.orig/phpdoc/RIVETusage.php0000644000175000017500000000703612217615312016243 0ustar sunsun RIVET usage SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

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            RIVET usage

            RIVET is a toolkit for the validation of Monte Carlo event generators [Buc10]. It contains the results of many experimental analyses, so that generator output can easily be compared to data, as well as providing a framework to implement your own analyses. Although using PYTHIA with RIVET is not officially supported, some helpful hints are given below. The full RIVET manual is available online.

            Using PYTHIA with RIVET

            The following assumes that you already have RIVET installed. Instructions for this may be found here.

            Events are passed from PYTHIA to RIVET using the HepMC format. PYTHIA must be compiled with HepMC support, using the same version of HepMC used when compiling RIVET. This is setup through the PYTHIA configure script e.g.
              ./configure --with-hepmc=/path/to/HepMC --with-hepmcversion=HepMC.version.number
            
            The PYTHIA library itself does not need to be recompiled.

            The examples/main42.cc sample program can then be used to generate events in HepMC format (which examples/main61.cc and examples/main62.cc extends by allowing LHAPDF usage and subruns). When in the examples directory, the main program can be built and used as follows
              make main42
              ./main42 main42.cmnd main42.hepmc
            
            The first argument is the input file which provides the options for event generation, while the second is the output file where the HepMC events should be written.

            This HepMC file may now be read and processed by RIVET
              rivet --analysis=ANALYSIS_NAME main42.hepmc
            
            where ANALYSIS_NAME is a built-in RIVET analysis, or one you have created yourself. The output of RIVET is in the form of .aida files, containing the histograms for the analysis, which can be processed further with RIVET (see the RIVET documentation for more details).

            The above examples requires that (potentially large) HepMC events are stored to disk before being read by RIVET. It is possible, instead, to pass the events directly to RIVET as they are produced by using a FIFO pipe. This is done with the mkfifo command
              mkfifo my_fifo
              ./main42.exe main42.cmnd my_fifo &
              rivet --analysis=ANALYSIS_NAME my_fifo
            
            Note that main42 is run in the background. pythia8-8.1.80.orig/phpdoc/pythia32.gif0000644000175000017500000000337512217346241015752 0ustar sunsunGIF89a         #!($,#)+* 4 10 8 6! 1%6"=#A!C" =& <&@)>, A*I(G* F.I,M0K2I5 F7O5L7S4^3X8]7V<X=[;f9a;V@[?Z?]@_>b@`?g?g@aDhD gDfE!mDfHmEpFmHhJrDkHtEfMsItJqLrMEzJyJJ!vQ~MyO!xRI"vQ!|PsT"NQT SL"{V&R&VWU'V!ST(U#ZZ#T$UZV'\&X,Y [&ZV)Z$_\*a$e] _ ]&['_&Y(aZ#`-]"e!`^[*cc$a$a1c0g`,d+ia&e&f d h&^)a*f"f)f/k#b1e+j$gg&m,k2g3l-o&m'i(k5l/m"p#t)n*p0u#j2i-n3o'p3p s-m.u u(s(q/p*s*u,v&yt/y.z(|/0v,y,|%{'%~..|2z2Ʉ*͂+̂2Ӂ-|1߀)Ӈ0ׅ14ޅ4ԍ,܉4ފ.03234.//1.2214-5-./003!Created with The GIMP!,  Hp Bbl}UÂQc*S>Np?,qكYdGQ're9pO֗:^0l@]m@={Ny색#b| `n*0DF=<QN p!` -*9Q28fń `*MpB><Խ2 H43O#07xb?Î=c*)xQc:0 I0~D093.DP-k4;ُ4@,HL0~rs;鼃9=0spHqd1D7s=x (B=fۉ3@ZX*@M9픣9J% Bc>DC SNTFP9m Advanced Usage SETTINGS SAVED TO FILE

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            Advanced Usage

            On this page we collect information on a number of classes that the normal user would not encounter. There are cases where the information is essential, however, for instance to ";?>implement your own showers.

            The subsystems

            One aspect that complicates administration is that an event can contain several subsystems, each consisting of one MPI and its associated ISR and FSR. To first approximation these systems are assumed to evolve independently, but to second they are connected by the interleaved evolution, and potentially by rescattering effects. The partons of a given subsystem therefore do not have to be stored consecutively.

            The PartonSystems class is primarily used to keep track of the current positions of all partons belonging to each system, represented by the index iPos for a parton stored in the event-record slot event[iPos]. With "all" we mean the currently defined two incoming partons, or none for a resonance decay, and the current set of outgoing partons, but with all ISR and FSR intermediate-state partons omitted. That is, it stores all partons that could be subject to some action in the next step of the combined MPI/ISR/FSR/BR description. As a special case, an outgoing parton is stored even if it undergoes a rescattering, and thus no longer belongs to the final state proper.

            The partonSystems instance of PartonSystems class is a public member of the Pythia top-level class, but is also available as a pointer partonSystemsPtr in various PartonLevel classes, e.g. inside the current instances of the TimeShower and SpaceShower classes.

            A number of PartonSystems methods can be used to set or get information on the subsystems:

            • clear() resets all the contents in preparation for the next event.
            • addSys() add a new (initially empty) subsystem to the current list and return its index iSys in the list, where index 0 is the hardest subcollision and so on.
            • sizeSys() the number of separate subsystems.
            • setInA(iSys, iPos), setInB(iSys, iPos) store position iPos of the incoming parton from beam A or beam B to the iSys'th subcollision. These values are 0 initially, and should so remain if there are no beams, such as in resonance decays.
            • addOut(iSys, iPos) store position iPos of a new outgoing parton in the iSys'th subcollision, by appending it at the end of the current vector, with beginning in slot 0.
            • setOut(iSys, iMem, iPos) store position iPos in the iMem'th slot in the vector of outgoing partons in the iSys'th subcollision. Here iMem must be in the range already constructed by addOut calls.
            • replace(iSys, iPosOld, iPosNew) replace the existing incoming or outgoing parton position iPosOld by iPosNew in the iSys'th subcollision.
            • setSHat(iSys, sHat) set the invariant squared mass sHat of the iSys'th subcollision.
            • hasInAB(iSys) true if an incoming parton has been set for beam A or beam B (and hence should have been set for both) in the iSys'th subcollision, else false.
            • getInA(iSys), getInB(iSys) the position iPos of the incoming parton from beam A or beam B to the iSys'th subcollision.
            • sizeOut(iSys) the number of outgoing partons in the iSys'th subcollision.
            • getOut(iSys, iMem) the position iPos of an outgoing parton in the iSys'th subcollision, with the iMem range limited by sizeOut(iSys). These partons are not guaranteed to appear in any particular order.
            • sizeAll(iSys) the total number of incoming and outgoing partons in the iSys'th subcollision.
            • getAll(iSys, iMem) the position iPos of an incoming or outgoing parton in the iSys'th subcollision. In case there are beams it gives same as getInA(iSys) and getInB(iSys) for indices 0 and 1, and thereafter agrees with getOut(iSys, iMem) offset two positions. If there are no beams it is identical with getOut(iSys, iMem).
            • getSHat(iSys) the invariant squared mass sHat of the iSys'th subcollision.
            • list() print a listing of all the system information, except for the sHat values.

            New systems are created from the hard process and by the MPI, not from any of the other components. Both FSR and ISR modify the position of partons, however. Since an FSR or ISR branching typically implies a new state with one more parton than before, an outgoing parton must be added to the system. Furthermore, in a branching, several existing partons may also be moved to new slots, including the incoming beam ones. In a FSR 1 -> 2 branching it is irrelevant which parton position you let overwrite the existing slot and which is added to the end of the system.

            The system information must be kept up-to-date. Both the MPI, ISR, FSR and BR descriptions make extensive use of the existing information. As an example, the introduction of primordial kT in the beam remnants will fail if the information on which final-state partons belong to which system is out-of-date. The introduction of rescattering as part of the MPI framework adds further complications, where an outgoing parton of one subsystem may be the incoming one of another system. This part of the code is still under development.

            Currently the system information is kept throughout the continued history of the event. Specifically, resonance decays create new systems, appended to the existing ones. This could be useful during the hadronization stage, to collect the partons that belong to a resonance with preserved mass when a small string collapses to one particle, but is not yet used for that.

            The beams

            The different subsystems are tied together by them sharing the same initial beam particles, and thereby being restricted by energy-momentum and flavour conservation issues. The information stored in the two beam particles, here called beamA and beamB, is therefore as crucial to keep correct as the above subsystem list.

            Both beam objects are of the BeamParticle class. Each such object contains a vector with the partons extracted from it. The number of such partons, beamX.size() (X = A or B), of course is the same as the above number of subsystems in the event record. (The two diverge at the BR step, where further beam remnants are added to the beams without corresponding to new subsystems.) The individual partons are accessed by an overloaded indexing operator to a vector of ResolvedParton objects. The iPos() property corresponds to the iPos one above, i.e. providing the position in the main event record of a parton. In particular, beamA[iSys].iPos() = partonSystemsPtr->getInA(iSys) and beamB[iSys].iPos() = partonSystemsPtr->getInB(iSys). Whereas thus the indices of the two incoming partons to a subsystem are stored in two places, the ones of the outgoing partons only appear in the system part of the PartonSystems class.

            Just as the subsystems in PartonSystems must be updated, so must the information in the two BeamParticle's, e.g. with methodsbeamX[iSys].iPos( iPosIn) when an incoming parton is replaced by a new one in line iPosIn. Furthermore the new parton identity should be set by beamX[iSys].id( idIn) and the new x energy-momentum fraction by beamX[iSys].x( xIn). The three can be combined in one go by beamX[iSys].update( iPosIn, idIn, xIn).

            To be specific, it is assumed that, at each step, the two incoming partons are moving along the +-z axis and are massless. Since the event is constructed in the c.m. frame of the incoming beams this implies that x = 2 E / E_cm. If the x values are not defined accordingly or not kept up-to-date the BR treatment will not conserve energy-momentum.

            In return, the BeamParticle objects give access to some useful methods. The beamX.xf( id, x, Q2) returns the standard PDF weight x f_id(x, Q^2). More interestingly, beamX.xfISR( iSys, id, x, Q2) returns the modified weight required when several subsystems have to share the energy and flavours. Thus iSys is added as an extra argument, and the momentum already assigned to the other subsystems is not available for evolution, i.e. the maximal x is correspondingly smaller than unity. Also flavour issues are handled in a similar spirit.

            An additional complication is that a parton can be either valence or sea, and in the latter case the BR treatment also distinguishes companion quarks, i.e. quark-antiquark pairs that are assumed to come from the same original g -> q qbar branching, whether perturbative or not. This can be queried either with the beamX[iSys].companion() method, for detailed information, or with the beamX[iSys].isValence(), beamX[iSys].isUnmatched() and beamX[iSys].isCompanion() methods for yes/no answers whether a parton is valence, unmatched sea or matched sea. This choice should affect the ISR evolution; e.g., a valence quark cannot be constructed back to come from a gluon.

            To keep this info up-to-date, the beamX.pickValSeaComp() method should be called whenever a parton of a new flavour has been picked in the ISR backwards evolution, but not if the flavour has not been changed, since then one should not be allowed to switch back and forth between the same quark being considered as valence or as sea. Since the pickValSeaComp() method makes use of the current parton-density values, it should be preceded by a call to beamX.xfISR( iSys, id, x, Q2), where the values in the call are the now finally accepted ones for the newly-found mother. (Such a call is likely to have been made before, during the evolution, but is not likely to be the most recent one, i.e. still in memory, and therefore had better be redone.) pythia8-8.1.80.orig/phpdoc/CouplingsAndScales.php0000644000175000017500000004612212217615312020045 0ustar sunsun Couplings and Scales SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

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            Couplings and Scales

            Here is collected some possibilities to modify the scale choices of couplings and parton densities for all internally implemented hard processes. This is based on them all being derived from the SigmaProcess base class. The matrix-element coding is also used by the multiparton-interactions machinery, but there with a separate choice of alpha_strong(M_Z^2) value and running, and separate PDF scale choices. Also, in 2 -> 2 and 2 -> 3 processes where resonances are produced, their couplings and thereby their Breit-Wigner shapes are always evaluated with the resonance mass as scale, irrespective of the choices below.

            Couplings and K factor

            The size of QCD cross sections is mainly determined by

            SigmaProcess:alphaSvalue   (default = 0.1265; minimum = 0.06; maximum = 0.25)
            The alpha_strong value at scale M_Z^2.

            The actual value is then regulated by the running to the Q^2 renormalization scale, at which alpha_strong is evaluated

            SigmaProcess:alphaSorder   (default = 1; minimum = 0; maximum = 2)
            Order at which alpha_strong runs,
            0 : zeroth order, i.e. alpha_strong is kept fixed.
            1 : first order, which is the normal value.
            2 : second order. Since other parts of the code do not go to second order there is no strong reason to use this option, but there is also nothing wrong with it.

            QED interactions are regulated by the alpha_electromagnetic value at the Q^2 renormalization scale of an interaction.

            SigmaProcess:alphaEMorder   (default = 1; minimum = -1; maximum = 1)
            The running of alpha_em used in hard processes.
            1 : first-order running, constrained to agree with StandardModel:alphaEMmZ at the Z^0 mass.
            0 : zeroth order, i.e. alpha_em is kept fixed at its value at vanishing momentum transfer.
            -1 : zeroth order, i.e. alpha_em is kept fixed, but at StandardModel:alphaEMmZ, i.e. its value at the Z^0 mass.

            In addition there is the possibility of a global rescaling of cross sections (which could not easily be accommodated by a changed alpha_strong, since alpha_strong runs)

            SigmaProcess:Kfactor   (default = 1.0; minimum = 0.5; maximum = 4.0)
            Multiply almost all cross sections by this common fix factor. Excluded are only unresolved processes, where cross sections are better ";?>set directly, and multiparton interactions, which have a separate K factor ";?>of their own. This degree of freedom is primarily intended for hadron colliders, and should not normally be used for e^+e^- annihilation processes.

            Renormalization scales

            The Q^2 renormalization scale can be chosen among a few different alternatives, separately for 2 -> 1, 2 -> 2 and two different kinds of 2 -> 3 processes. In addition a common multiplicative factor may be imposed.

            SigmaProcess:renormScale1   (default = 1; minimum = 1; maximum = 2)
            The Q^2 renormalization scale for 2 -> 1 processes. The same options also apply for those 2 -> 2 and 2 -> 3 processes that have been specially marked as proceeding only through an s-channel resonance, by the isSChannel() virtual method of SigmaProcess.
            1 : the squared invariant mass, i.e. sHat.
            2 : fix scale set in SigmaProcess:renormFixScale below.


            SigmaProcess:renormScale2   (default = 2; minimum = 1; maximum = 5)
            The Q^2 renormalization scale for 2 -> 2 processes.
            1 : the smaller of the squared transverse masses of the two outgoing particles, i.e. min(mT_3^2, mT_4^2) = pT^2 + min(m_3^2, m_4^2).
            2 : the geometric mean of the squared transverse masses of the two outgoing particles, i.e. mT_3 * mT_4 = sqrt((pT^2 + m_3^2) * (pT^2 + m_4^2)).
            3 : the arithmetic mean of the squared transverse masses of the two outgoing particles, i.e. (mT_3^2 + mT_4^2) / 2 = pT^2 + 0.5 * (m_3^2 + m_4^2). Useful for comparisons with PYTHIA 6, where this is the default.
            4 : squared invariant mass of the system, i.e. sHat. Useful for processes dominated by s-channel exchange.
            5 : fix scale set in SigmaProcess:renormFixScale below.


            SigmaProcess:renormScale3   (default = 3; minimum = 1; maximum = 6)
            The Q^2 renormalization scale for "normal" 2 -> 3 processes, i.e excepting the vector-boson-fusion processes below. Here it is assumed that particle masses in the final state either match or are heavier than that of any t-channel propagator particle. (Currently only g g / q qbar -> H^0 Q Qbar processes are implemented, where the "match" criterion holds.)
            1 : the smaller of the squared transverse masses of the three outgoing particles, i.e. min(mT_3^2, mT_4^2, mT_5^2).
            2 : the geometric mean of the two smallest squared transverse masses of the three outgoing particles, i.e. sqrt( mT_3^2 * mT_4^2 * mT_5^2 / max(mT_3^2, mT_4^2, mT_5^2) ).
            3 : the geometric mean of the squared transverse masses of the three outgoing particles, i.e. (mT_3^2 * mT_4^2 * mT_5^2)^(1/3).
            4 : the arithmetic mean of the squared transverse masses of the three outgoing particles, i.e. (mT_3^2 + mT_4^2 + mT_5^2)/3.
            5 : squared invariant mass of the system, i.e. sHat.
            6 : fix scale set in SigmaProcess:renormFixScale below.


            SigmaProcess:renormScale3VV   (default = 3; minimum = 1; maximum = 6)
            The Q^2 renormalization scale for 2 -> 3 vector-boson-fusion processes, i.e. f_1 f_2 -> H^0 f_3 f_4 with Z^0 or W^+- t-channel propagators. Here the transverse masses of the outgoing fermions do not reflect the virtualities of the exchanged bosons. A better estimate is obtained by replacing the final-state fermion masses by the vector-boson ones in the definition of transverse masses. We denote these combinations mT_Vi^2 = m_V^2 + pT_i^2.
            1 : the squared mass m_V^2 of the exchanged vector boson.
            2 : the geometric mean of the two propagator virtuality estimates, i.e. sqrt(mT_V3^2 * mT_V4^2).
            3 : the geometric mean of the three relevant squared transverse masses, i.e. (mT_V3^2 * mT_V4^2 * mT_H^2)^(1/3).
            4 : the arithmetic mean of the three relevant squared transverse masses, i.e. (mT_V3^2 + mT_V4^2 + mT_H^2)/3.
            5 : squared invariant mass of the system, i.e. sHat.
            6 : fix scale set in SigmaProcess:renormFixScale below.


            SigmaProcess:renormMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
            The Q^2 renormalization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes is multiplied by this factor relative to the scale described above (except for the options with a fix scale). Should be use sparingly for 2 -> 1 processes.

            SigmaProcess:renormFixScale   (default = 10000.; minimum = 1.)
            A fix Q^2 value used as renormalization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes in some of the options above.

            Factorization scales

            Corresponding options exist for the Q^2 factorization scale used as argument in PDF's. Again there is a choice of form for 2 -> 1, 2 -> 2 and 2 -> 3 processes separately. For simplicity we have let the numbering of options agree, for each event class separately, between normalization and factorization scales, and the description has therefore been slightly shortened. The default values are not necessarily the same, however.

            SigmaProcess:factorScale1   (default = 1; minimum = 1; maximum = 2)
            The Q^2 factorization scale for 2 -> 1 processes. The same options also apply for those 2 -> 2 and 2 -> 3 processes that have been specially marked as proceeding only through an s-channel resonance.
            1 : the squared invariant mass, i.e. sHat.
            2 : fix scale set in SigmaProcess:factorFixScale below.


            SigmaProcess:factorScale2   (default = 1; minimum = 1; maximum = 5)
            The Q^2 factorization scale for 2 -> 2 processes.
            1 : the smaller of the squared transverse masses of the two outgoing particles.
            2 : the geometric mean of the squared transverse masses of the two outgoing particles.
            3 : the arithmetic mean of the squared transverse masses of the two outgoing particles. Useful for comparisons with PYTHIA 6, where this is the default.
            4 : squared invariant mass of the system, i.e. sHat. Useful for processes dominated by s-channel exchange.
            5 : fix scale set in SigmaProcess:factorFixScale below.


            SigmaProcess:factorScale3   (default = 2; minimum = 1; maximum = 6)
            The Q^2 factorization scale for "normal" 2 -> 3 processes, i.e excepting the vector-boson-fusion processes below.
            1 : the smaller of the squared transverse masses of the three outgoing particles.
            2 : the geometric mean of the two smallest squared transverse masses of the three outgoing particles.
            3 : the geometric mean of the squared transverse masses of the three outgoing particles.
            4 : the arithmetic mean of the squared transverse masses of the three outgoing particles.
            5 : squared invariant mass of the system, i.e. sHat.
            6 : fix scale set in SigmaProcess:factorFixScale below.


            SigmaProcess:factorScale3VV   (default = 2; minimum = 1; maximum = 6)
            The Q^2 factorization scale for 2 -> 3 vector-boson-fusion processes, i.e. f_1 f_2 -> H^0 f_3 f_4 with Z^0 or W^+- t-channel propagators. Here we again introduce the combinations mT_Vi^2 = m_V^2 + pT_i^2 as replacements for the normal squared transverse masses of the two outgoing quarks.
            1 : the squared mass m_V^2 of the exchanged vector boson.
            2 : the geometric mean of the two propagator virtuality estimates.
            3 : the geometric mean of the three relevant squared transverse masses.
            4 : the arithmetic mean of the three relevant squared transverse masses.
            5 : squared invariant mass of the system, i.e. sHat.
            6 : fix scale set in SigmaProcess:factorFixScale below.


            SigmaProcess:factorMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
            The Q^2 factorization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes is multiplied by this factor relative to the scale described above (except for the options with a fix scale). Should be use sparingly for 2 -> 1 processes.

            SigmaProcess:factorFixScale   (default = 10000.; minimum = 1.)
            A fix Q^2 value used as factorization scale for 2 -> 1, 2 -> 2 and 2 -> 3 processes in some of the options above. "?>
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            Random-Number Seed

            The seed of the random number generator can be set as follows:

            Random:setSeed On Off   (default = off)
            Indicates whether a user-set seed should be used every time the Pythia::init routine is called. If off, the random number generator is initialized with its default seed at the beginning of the run, and never again. If on, each new Pythia::init call (should several be made in the same run) results in the random number being re-initialized, thereby possibly starting over with the same sequence, if you do not watch out.

            Random:seed   (default = -1; maximum = 900000000)
            The seed to be used, if setSeed is on.
            A negative value gives the default seed,
            a value 0 gives a random seed based on the time, and
            a value between 1 and 900,000,000 a unique different random number sequence.

            For more on random numbers see ";?>here. This includes methods to save and restore the state of the generator, and some preprogrammed methods to generate non-uniform random numbers. "?>

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            CKKW-L Merging

            CKKW-L merging [Lon01] allows for a consistent merging of parton showers with matrix elements to include multiple well-separated partons. The algorithm implemented in PYTHIA is described in [Lon11]. To perform matrix element merging, the user has to supply LHE files [Alw07] for the hard process and the corresponding process with up to N additional jets.

            The usage of the merging procedure is illustrated in a few example main programs (main81.cc, main82.cc, main83.cc, main84.cc and main85.cc, together with the input files main81.cmnd, main82.cmnd, main84.cmnd and main85.cmnd). These examples should of course only serve as an illustration, and as such will not make use of the merging in all possible ways. For full generality, the example programs link to LHAPDF, FastJet and HepMC. Of course the user is welcome to remove these dependencies. To remove the FastJet dependence, the functions calculating example observables have to be deleted. Removing the LHAPDF dependence requires changing the cmnd input files to choose an inbuilt PDF, as outlined in the PDF documentation. The HepMC dependence can be removed by erasing the code allowing for HepMC output.

            Please note that a detailed tutorial on merging in Pythia is available from http://home.thep.lu.se/~torbjorn/pythia8/mergingworksheet8160.pdf.

            Three very short LHE files (w+_production_lhc_0.lhe, w+_production_lhc_1.lhe, w+_production_lhc_2.lhe) are included in the distribution. These files are not intended for physics studies, but only serve as input for the example main programs. For realistic studies, the user has to supply LHE files.

            In the generation of LHE files, the value of the factorisation scale used in the PDFs is not important, since the cross section will be multiplied by ratios of PDFs to adjust to the PYTHIA starting scales. The same is true for the renormalisation scale (and starting value αs(MZ)) used to evaluate αs. Coupling and scale choices by the user will be transferred to the merging routines.

            Multi-jet events can suffer from infrared divergences in the calculation. Sensible matrix element generator (MEG) outputs should not contain phase space points in which the calculation is ill-defined, meaning infrared regions need to be removed by cuts. This is most conveniently done by disallowing the MEG to produce partons below a minimal parton-parton separation in a certain jet algorithm. Using dedicated cuts to regularise MEG output is of course possible as well. Any regularisation criterion defines the matrix element region: The parts of phase space in which the fixed order calculation is considered valid and preferable to the parton shower. Matrix element merging is combining MEG events in the matrix element region with parton shower events in regions outside the regularisation cut (often called parton shower region). Because the regularisation cut defines a boundary between the matrix element and parton shower regions, i.e. the regions to be merged into one inclusive sample, it is usually called merging scale . Since many different cut choices may regularise the MEG calculation, many different merging scale definitions are possible. A few standard choices are listed below, as well as documentation on how to use a user-defined cut criterion. In combining matrix element and parton shower regions, the CKKW-L prescription tries to minimise the dependence on the merging scale. This can only be achieved if the combination of MEG events and parton shower populates the whole phase space. Additional cuts on the partons in the LHEF generation should hence be avoided as much as possible, meaning that the merging scale cut should always pose a more stringent cut than all other cuts on the partons. Of course, if the hard process itself is divergent, cuts need to be made. However, this should be chosen in such a way as to not exclude regions that will be available to the matrix elements with additional jets. An example is QCD di-jet production with additional jets: Say the 2 -> 2 process is regularised with a pTmin cut of pTminCut = 100 GeV, and the 2 - >3 sample is regularised with a kTmin-cut of kTminCut = 50 GeV. This would mean that when reclustering the emission in the 2 -> 3 sample, we could end up with a pT value pTminNow of the 2 -> 2 configuration with pTminCut > pTminNow, which is excluded in the 2 -> 2 sample. Thus, the 2 -> 3 sample will include a Sudakov factor not included in the 2 -> 2 sample, resulting in merging scale dependencies. Such dependencies can be avoided if the additional cuts on the hard process are minimal.

            Of course, additional cuts on electroweak particles are allowed. These should be the same for all samples with 0 <= n <= N additional partons.

            If it is not possible to generate LHE files with minimal cuts, the user can choose to use the MergingHooks structures in order to decide how much influence to attribute to parton shower histories in which the reclustered lowest multiplicity process does not pass the matrix element cuts. This is described below.

            When generating LHE files, we advise against putting unstable particles (e.g. massive gauge bosons) in the final state. Rather, specify a resonance by its decay products, e.g. if Les Houches events for the pp → Z + jets → e+e- + jets process are desired, generate the matrix element events with the Z decay included. From a physical point of view, on-shell final massive gauge bosons should not be considered part of a hard process, since only the boson decay products will be detectable. Furthermore, non-narrow-width approximation contributions are not present if the ME generator only produces on-shell bosons. Interference effects between different production channels for the decay products would also be neglected. These points seem an unnecessary restriction on the accuracy of the ME calculation. In addition, there is a technical reason for this strategy. Since some matrix element generators choose to put additional information on intermediate bosons into Les Houches events, depending on if they pass a certain criterion (e.g. being close to the mass shell), without exact knowledge of this criterion, the only feasible way of bookkeeping the hard process is by identifying outgoing decay products.

            Despite these considerations, (massive) gauge bosons in the final state are allowed in the hard process definition. This is useful particularly for Higgs physics, when different decays of the Higgs boson need to be simulated after the LHEF generation.

            For all merging purposes, processes with different charge of outgoing leptons are considered different processes. That means e.g. that e+νe+ jets and e-ν̄e + jets are considered independent processes. If the user wishes to generate distributions including effects of more than one process, merged samples for all independent processes should be generated separately and added afterwards. Alternatively, to combine simple processes, combined LHE files can be used in conjunction with flexible containers (see below).

            When the matrix element merging is used to produce HepMC [Dob01] files to be analysed with RIVET [Buc10], special care needs to taken in how the cross section is read by RIVET (see below).

            To specify the merging conditions, additionally information on the merging scale value and the functional definition of the merging scale is needed. A few standard definitions of merging scales are available. We hope this makes the user interface less cumbersome.

            Different choices intrinsic to the CKKW-L merging procedure might be relevant for the user as well. The base class MergingHooks gives the user the opportunity to define the functional form of the merging scale. In the following, the usage of the merging machinery to consistently include LHE files with additional jets into PYTHIA will be discussed.


            Merging scale definitions

            The quickest way to include processes with additional jets is to produce LHE files with one of the standard ways to define the merging scale. Three standard ways to define a merging scale (minimal kT, minimal evolution pT and by three cuts) are implemented. All of these prescriptions are equivalent - different definitions have only been introduced for the convenience of users, who might be limited by which cuts can be used in the generation of LHE files. Below, we describe how to switch on and use these different merging scale definitions.

            Merging with merging scale defined in kT:



            Merging:doKTMerging On Off   (default = off)
            If the additional jets in the LHE files have been regulated by a kT cut, the user can supply the merging scale definition by setting this flag to on. kT here and below means cutting on Durham kT for e+e- collisions, and cutting on longitudinally invariant kT for hadronic collisions. Please note that this particular merging scale definition will check kT between all pairs of u,d,c,s,b,g partons.

            Currently, the name longitudinally invariant kT is used for a few jet recombination algorithms with slightly different jet measures. A specific form can be chosen by setting the switch

            Merging:ktType   (default = 1; minimum = 1; maximum = 3)
            Precise functional definition of longitudinally invariant kT. For e+e- collisions, Durham kT is always defined by the square root of min{ 2*min[ Ei2, Ej2] * [ 1 - cosθij] }, so that this switch will have no effect.
            1 : Longitudinally invariant kT is defined by the square root of the minimum of minimal jet kinematic pT (pTkin,min2 = min{ pT,i2 } ) and pTlon,min2 = min{ min[ pT,i2, pT,j2] * [ (Δyij)2 + (Δφij)2 ] / D2 } , i.e. kT = min{ √pTkin,min2, √pTlon,min2 } for hadronic collisions. Note that the true rapidity of partons is used.
            2 : Longitudinally invariant kT is defined by the square root of the minimum of minimal jet kinematic pT (pTkin,min2 = min{ pT,i2 } ) and pTlon,min2 = min{ min[ pT,i2, pT,j2] * [ (Δηij)2 + (Δφij)2 ] / D2 }, i.e. kT = min{ √pTkin,min2, √pTlon,min2 } for hadronic collisions. Note that the pseudorapidity of partons is used.
            3 : Longitudinally invariant kT is defined by the square root of the minimum of minimal jet kinematic pT (pTkin,min2 = min{ pT,i2 } ) and pTlon,min2 = min{ min[ pT,i2, pT,j2] * [ cosh(Δηij) - cos(Δφij) ] / D2 } , i.e. kT = min{ √pTkin,min2 , √pTlon,min2 } for hadronic collisions.


            Merging:nJetMax   (default = 0; minimum = 0)
            Maximal number of additional jets in the matrix element

            Merging:TMS   (default = 0.0)
            The value of the merging scale. The name is inspired by the scale in evolution equations, which is often called 't', and the suffix 'MS' stands for merging scale. In the particular case of kT-merging, this would be the value of the kT-cut in GeV. For any merging scale definition, this input is considered the actual value of the merging scale.

            Merging:Process   (default = void)
            The string specifying the hard core process, in MG4/ME notation.

            If e.g. W + jets merging should be performed, set this to pp>e+ve (without white spaces or quotation marks). This string may contain resonances in the MG/ME notation, e.g. for merging pp→Z W+→q q̄ e+νe + jets, the string pp>(z>jj)(w+>e+ve) would be applicable.

            A lot more flexible hard process definitions are possible. To not dwell too much on these details here, we will come back to the process string at the end of this section.

            Merging:doMGMerging On Off   (default = off)
            Even easier, but highly non-general, is to perform the merging with MadGraph/MadEvent-produced LHE files, with a merging scale defined by a kT cut. For this, set this switch to on. The merging scale value will be read from the +1 jet LHE file by searching for the string ktdurham, and extracting the value from value = ktdurham. Also, the hard process will be read from the +0 jet LHE file, from the line containing the string @1 (the tag specifying the first process in the MadGraph process card). For this to work, PYTHIA should be initialised on LHE files called NameOfYourLesHouchesFile_0.lhe (+0 jet sample) and NameOfYourLesHouchesFile_1.lhe (+1 jet sample) and the same naming convention for LHE files with two or more additional jets. Since for this option, the merging scale value is read from the LHEF, no merging scale value needs to be supplied by setting Merging:TMS . Also, the hard process is read from LHEF, the input Merging::Process does not have to be defined. However, the maximal number of merged jets still has to be supplied by setting Merging:nJetMax.

            Merging with merging scale defined in Pythia evolution pT:

            If the LHE file has been regularised by cutting on the minimal Pythia evolution pT in the state, this can also be used as a merging scale right away. For this, change the switch

            Merging:doPTLundMerging On Off   (default = off)
            The merging scale is then defined by finding the minimal Pythia evolution pT between sets of radiator, emitted and recoiler partons. For this particular merging scale definition, u,d,c,s,b,g are considered partons. The Pythia evolution pT of a single three-parton set is defined by

            pTevol = zijk(1-zijk) Qij2 for FSR, where i is the radiating parton, j is the emitted parton and k is the recoiler, and Qij2 = (pi + pj)2 , and zijk = xi,jk / (xi,jk + xj,ik) with xi,jk = 2 pi (pi + pj + pk) / (pi + pj + pk)2

            pTevol = (1-zijk) Qij2 for ISR, where i is the radiating parton, j is the emitted parton and k is the second initial state parton, and Qij2 = -(pi - pj)2 , and zijk = (pi - pj + pk)2 / (pi + pk)2 .

            When using this option, the merging scale is defined by the minimum pTevol for all combinations of three partons in the event, irrespective of flavour or colour-connections. The merging scale value will be read from the Merging:TMS parameter, so that this needs to be set just as in the case of the kT-merging prescription. Of course you will also need to set Merging:Process and the maximal number of additional matrix element jets Merging:nJetMax.

            Merging with merging scale defined by a combination of cuts:

            It is possible to regularise QCD divergences in a LHE file by applying cuts to the kinematical pT of jets (pTi), combined with a cut on ΔRij between jets and a cut on invariant mass Qij of jet pairs. The combination of these standard cuts can also serve as a merging scale. For this, use this setting

            Merging:doCutBasedMerging On Off   (default = off)
            This switch will use cuts on (pTi), ΔRij and Qij to define when parton shower emissions are allowed. Please note for this particular merging scale definition, only light jets (u,d,c,s,g) are checked.

            The values of the cuts will then be read from

            Merging:QijMS   (default = 0.0)
            The value of the invariant mass cut Qij of pairs of final state partons used in the matrix element generation.

            Merging:pTiMS   (default = 0.0)
            The value of the minimal transverse momentum cut pTi on final state partons, as used in the matrix element generation.

            Merging:dRijMS   (default = 0.0)
            The value of the minimal ΔRij separation between pairs of final state partons used in the matrix element generation, where ΔRij2 = (Δyij)2 + (Δφij)2.

            With knowledge of these values, and Merging:doCutBasedMerging, Pythia will use these cuts as a separation between matrix element phase space and parton shower region. If e.g. the Les Houches Events have been generated with the cuts ΔRij = 0.1 , pTi= 20 GeV and Qij = 40 GeV, set Merging:QijMS=40., Merging:pTjMS=20., Merging:dRijMS=0.1 to perform a cut-based merging. Of course you will also need to set Merging:Process and the maximal number of additional matrix element jets Merging:nJetMax.

            Les Houches events outside the matrix element region

            Before continuing, we would like to point out that in general, the user should make sure that the events in the Les Houches file are actually calculated using the regularisation cut definition and value(s) supplied to Pythia as merging scale definition and value(s). However, if LH files with a large number of events and loose merging scale cuts are available, it might be useful to choose a higher merging scale value, e.g. for merging scale variations as part of uncertainty assessments. If CKKW-L merging is enabled, Pythia will by default check if events read from Les Houches file are in the matrix element region as defined by the merging scale definition and merging scale value. Events outside the matrix element region will be discarded. This will lead to warnings of the form "Les Houches Event fails merging scale cut. Cut by rejecting event". These warnings should, in this case, rather be regarded as information. To change the default behaviour, use the flag

            Merging:enforceCutOnLHE On Off   (default = on)
            This will check if the events read from LHE file are in the matrix element region as defined by the merging scale definition and value(s). If on, LHE input outside the matrix element region will be rejected. If off, every event is assumed to pass the merging scale cut.

            Defining the hard process

            To perform CKKW-L matrix element merging, the user has to decide on a hard process, and communicate this choice to Pythia. This is done by setting the input Merging:Process

            For single processes in the Standard Model or the MSSM, MG4/ME notation is applicable. However, for some purposes, using a single simple process string is not satisfactory. Mixed W+ and W- events in a single LHE file is a common example. For this case, it would of course be perfectly allowed to perform twice, once for W+ production and once for W- production, and then add the results. Nevertheless, it seems reasonable to alleviate difficulties by allowing for less restrictive hard process definitions. Two generalisations of the process tag are available: Containers and user-defined particle tags. The syntax of these settings is described below.

            In case you want multiple processes in a LHE file to be treated on equal footing (e.g. W+ + jets and W- + jets), you should use flexible containers do specify the hard process. So far, we allow the use of the containers LEPTONS, NEUTRINOS, BQUARKS. If you use these containers, the hard process definition is relatively flexible, meaning that Pythia will attempt a merging of QCD jets for each event in the LHE file, and assume that all particles matching one of the containers are products of the hard process. This is best explained by examples. If you want to have both pp → e+ νe + jets and pp → e- ν̄e + jets events in a single file, you can set Merging:Process=pp>LEPTONS,NEUTRINOS as hard process (note that for readability, you are allowed to use commata to separate container names). Combining e.g. the processes pp → e+ νe and pp → μ+ νμ is possible with the hard process definition pp>LEPTONS,NEUTRINOS.

            For maximal flexibility, the definition of the hard process by these containers does not mean that each Les Houches event needs to contain particles to match each container. It is enough if one container is matched. This means that with the string pp>LEPTONS,NEUTRINOS, you can immediately process pp → e+ e- events mixed with pp → e+ νe events, since particles matching at least one container can be found in both cases. Another example for the usage of containers is mixing pp → e+ νe and pp → tt̄ → e+ νe e- ν̄e bb̄. This can be accommodated by the hard process string Merging:Process=pp>LEPTONS,NEUTRINOS,BQUARKS.

            There is however a conceptual limitation to containers: The hard process definition is necessary to ensure that when constructing lower multiplicity states (that will be used to calculate the correct merging weight), the structure of the hard process will be preserved. If e.g. we want the hard process to be pp → Z → bb̄ , we should ensure that the lowest multiplicity state contains a colour-singlet bb̄-pair. When reconstructing intermediate lower multiplicity states from multi-jet matrix elements, we should thus always be able to find at least one bb̄-pair. By mixing different processes in a LHE file, this requirement might already be violated at the level of Les Houches events. Flexible containers cannot give strong conditions which flavours should be preserved in the construction of the hard process. In order to avoid non-sensible results, it is hence assumed that all particles matching any of the containers will be part of the lowest multiplicity process. This implies that if you decide to use the BQUARKS container, all b-quarks in the LHE file will be interpreted as hard process particles, and never as additional radiation.

            Another way to specify the hard process particles is to explicitly define the particle names and identifiers. This is necessary if the matrix element merging in Pythia does not contain the particles of interest. To make sure that the hard process is still treated correctly, it is possible to define particles in the process string. If you e.g. want the hard process to contain a particle "zeta~" with PDG identifier "12345", produced in proton collisions, you have to include a user-defined particle tag by setting the process string to pp>{zeta~,12345}. The user-defined particle is enclosed in curly brackets, with syntax {particle_name,particle_identifier}, where "particle_name" and "particle_identifier" are the particle name and particle identifier used for this particle in the input LHE file. User-defined particles are only allowed in the final state. You are free to fix user-defined particles with more common ones, as long as user-defined particles are put before more common particles in the process string. This means that if you e.g. wanted the hard process to contain a graviton in association with a positron and an electron-neutrino, you have to define the hard process as pp>{G,39}e+ve.

            Below you can find a list of particles predefined in the merging. If you wish to include a hard process with different final state particles, you may use the "curly bracket notation" outlined above.

            The set of incoming particles us limited to: e- (electron), e+ (positron), mu- (muon), mu+ (antimuon), p (proton, container to hold all initial state coloured particles), p~ (identical to p container).

            The following intermediate particles are allowed: a (photon), z (Z boson), w- (W- boson), w+ (W+ boson), h (scalar Higgs boson), W (container to hold both W- and W+ boson), t (top quark), t~ (anti-top), dl, dl~, ul, ul~, sl, sl~, cl, cl~, b1, b1~, t1, t1~, dr, dr~, ur, ur~, sr, sr~, cr, cr~, b2, b2~, t2, t2~ (all MSSM squarks).

            We have pre-defined the outgoing particles: e+, e-, ve~, ve, mu+, mu-, vm~, vm, ta+, ta-, vt~, vt (all SM leptons and neutrinos), j~ (container to hold all final state coloured particles), j (container to hold all final state coloured particles), NEUTRINOS (container to hold all final state neutrinos and anti-neutrinos), LEPTONS (container to hold all final state leptons and anti-leptons), BQUARKS (container to hold final state b-quarks), d~, d, u~, u, s~, s, c~, c, b~, b, t~, t (all SM quarks), a, z, w-, w+ (all SM electro-weak bosons), h (scalar Higgs boson), W (container to hold both W- and W+ boson), n1 (MSSM neutralino), dl~, dl, ul~, ul, sl~, sl, cl~, cl, b1~, b1, t1~, t1, dr~, dr, ur~, ur, sr~, sr, cr~, cr, b2~, b2, t2~, t2 (all MSSM squarks). Other outgoing particles are possible if you use the "curly bracket notation" described earlier.


            Histogramming the events

            After the event has been processed, histograms for observables of interest need to be filled. In order to achieve good statistical accuracy for all jet multiplicities and all subprocesses contributing to one jet multiplicity, generally a fixed number of unit-weighted events is read from each Les Houches Event file. To then arrive at the correct prediction, for each of these events, histogram bins should be filled with the corresponding cross section, or weighted with unit weight and normalised at the end to the generated cross section for each jet multiplicity separately.

            Still another, even more important, event weight that has to applied on an event-by-event basis is the CKKW-L-weight. This corrective weight is the main outcome of the merging procedure and includes the correct no-emission probabilities, PDF weights and αs factors. This means that the merging implementation will generate weighted events. The CKKW-L-weight can be accessed by the following function:

            double Info::mergingWeight()  
            Returns the CKKW-L weight for the current event.

            Note that to avoid confusion, this function does not include the the weight of a phase space point (given by Info::weight()). This weight will differ from unity when reading in weighted Les Houches events. In this case, the full weight with which to fill histogram bins is Info::mergingWeight() * Info::weight().

            Finally, to arrive at a correct relative normalisation of the contributions from different number of additional jets in the matrix element, each histogram should be rescaled with the accepted cross section given by Info::sigmaGen(). The accepted cross section includes the effect of vetoes generating Sudakov form factors for the matrix elements, and is in general only known after the run.

            This final step can of course be skipped if the accepted cross section had been estimated before the histogramming run, and histogram bins had instead been filled with the weight Info::mergingWeight() * σest(number of additional jets in current ME sample). This is the way HepMC events should be weighted to produce correct relative weights of events (see below, and particularly examine the example programs main84.cc and main85.cc).

            Examples how to use these options are given in main81.cc (kT merging), main84.cc (automatic MG/ME merging for RIVET usage), and main85.cc (HepMC output for RIVET usage).


            Merging with user-defined merging scale function

            For all other merging scale definitions, the procedure is slightly more complicated, since the user has to write a small piece of code defining the merging scale. To allow for a user defined procedure, set the input

            Merging:doUserMerging On Off   (default = off)
            General user defined merging on/off.

            Then, set the Merging:nJetMax, Merging:TMS and Merging:Process input as before.

            Since during execution, PYTHIA needs to evaluate the merging scale with the definition of the user, the user interface is designed in a way similar to the UserHooks strategy. The class controlling the merging scale definition is called MergingHooks.

            Initialisation

            To initialise the merging with user-defined merging scale, we should construct a class derived from MergingHooks, with a constructor and destructor

            MergingHooks::MergingHooks()  

            virtual MergingHooks::~MergingHooks()  
            The constructor and destructor do not need to do anything.

            For the class to be called during execution, a pointer to an object of the class should be handed in with the
            Pythia::setMergingHooksPtr( MergingHooks*) method. An examples of this procedure are given in main82.cc.

            Defining a merging scale

            Then, in the spirit of the UserHooks class, the user needs to supply the process to be merged by defining a methods to evaluate the merging scale variable.

            virtual double MergingHooks::tmsDefinition(const Event& event)  
            This method will have to calculate the value of the merging scale defined in some variable from the input event record. An example of such a function is given in main82.cc.

            The base class MergingHooks contains many functions giving information on the hard process, to make the definition of the merging scale as easy as possible:

            int MergingHooks::nMaxJets()  
            Return the maximum number of additional jets to be merged.

            int MergingHooks::nHardOutPartons()  
            Returns the number of outgoing partons in the hard core process.

            int MergingHooks::nHardOutLeptons()  
            Returns the number of outgoing leptons in the hard core process.

            int MergingHooks::nHardInPartons()  
            Returns the number of incoming partons in the hard core process.

            int MergingHooks::nHardInLeptons()  
            Returns the number of incoming leptons in the hard core process.

            int MergingHooks::nResInCurrent()  
            The number of resonances in the hard process reconstructed from the current event. If e.g. the ME configuration was pp -> (w+->e+ve)(z -> mu+mu-)jj, and the ME generator put both intermediate bosons into the LHE file, this will return 2.

            double MergingHooks::tms()  
            Returns the value used as the merging scale.

            Filling output histograms for the event then proceeds along the lines described above in "Histogramming the events".

            The full procedure is outlined in main82.cc. Special care needs to be taken when the output is stored in the form of HepMC files for RIVET usage.

            Defining a cut on lowest jet multiplicity events

            It can sometimes happen that when generating LHE files, a fairly restrictive cut has been used when generating the lowest multiplicity matrix element configurations. Then, it can happen that states that are (in the generation of a parton shower history) constructed by reclustering from higher multiplicity configurations, do not pass this matrix element cut.

            Consider as an example pure QCD dijet merging, when up to one additional jet should be merged. Three-jet matrix element configurations for which the reclustered two-jet state does not pass the cuts applied to the two-jet matrix element would never have been produced by showering the two-jet matrix element. This means that the three-jet matrix element includes regions of phase space that would never have been populated by the parton shower. Thus, since the matrix element phase space is larger than the shower phase space, merging scale dependencies are expected. A priori, this is not troublesome, since the aim of matrix element merging is to include regions of phase space outside the range of the parton shower approximation into the shower. An example is the inclusion of configurations with only unordered histories.

            Clearly, if the parton shower phase space is very constrained by applying stringent cuts to the two-jet matrix element, merging scale dependencies can become sizable, as was e.g. seen in [Lon11] when forcing shower emissions to be ordered both in the evolution variable and in rapidity. To influence the effect of large phase space differences for shower emissions and matrix element configurations due to LHEF generation cuts, the user has to write a small piece of code overwriting method

            virtual double MergingHooks::dampenIfFailCuts(const Event&event)  
            multiplicity reclustered state as an input Event. From this input event, the user can then check if matrix element cuts are fulfilled. The return value will be internally multiplied to the CKKW-L weight of the current event. Thus, if the user wishes to suppress contributions not passing particular cuts, a number smaller than unity can be returned.

            Note that this method gives the user access to the lowest multiplicity state, which ( e.g. in the case of incomplete histories) does not have to be a 2 → 2 configuration. Also, changing the weight of the current event by hand is of course a major intervention in the algorithm, and should be considered very carefully. Generally, if this facility would have to be used extensively, it is certainly preferable to be less restrictive when applying additional, non-merging-scale-related cuts to the matrix element.

            An example how to force a cut on lowest multiplicity reclustered states for pure QCD matrix element configurations is given by main83.cc (to be used with e.g. main82.cmnd).

            Influencing the construction of all possible histories

            Even more powerful - and dangerous - is influencing the construction of histories directly. This should only be attempted by expert users. If you believe manipulations completely unavoidable, we advise you to take great care when redefining the following functions.

            virtual bool MergingHooks::canCutOnRecState()  
            In the base class this method returns false. If you redefine it to return true then the method doCutOnRecState(...) will be called for each reclustered state encountered in the generation of all possible histories of the matrix element state.

            virtual bool MergingHooks::doCutOnRecState(const Event&event)  
            This routine will be supplied internally with every possible reclustered event that can be reached by reclustering any number of partons in the matrix element input state. The new, reclustered, states can then be analysed. If the method returns false, the history to which the state belongs will be treated as if it were unordered, i.e. this path will only be chosen if no other histories are available. In this way, the number of histories not fulfilling the user criterion will be minimised.

            Clearly, these methods are highly intrusive. It could e.g. happen that no history is allowed, which would make merging impossible. One example where this method could be useful is if cuts on the core 2 -> 2 processes have to be checked, and the method MergingHooks::dampenIfFailCuts(const Event& event) is not sufficiently effective.

            Defining the hard process matrix element

            The MergingHooks class also allows the expert user to define the matrix element of the hard process, by defining the method

            virtual double MergingHooks::hardProcessME(const Event&inEvent)  
            This routine will be supplied internally with the reconstructed lowest-multiplicity event. From this, it is possible to calculate the squared matrix element of the hard process, by using the information stored in the event record. The function should return a double value that corresponds to the matrix element at the phase space point given by the input event record. This number will then be multiplied to the product of splitting functions that define the probability of the current path of the parton shower history. In this way, the hard process configuration can be taken into account when choosing the parton shower history, which is, internally, used to generate the "merging weight".

            The inclusion of the hard process matrix element into the choice of histories becomes relevant when the hard process matrix element has very strong phase space dependencies. QCD dijet cross sections for example strongly depend on the transverse momentum of the jets. So far, the authors have not encountered any changes upon inclusion of the full hard process matrix element, even for the QCD dijet case.


            Matrix element merging and HepMC output for RIVET

            Examples how to produce matrix element merged events to be analysed with RIVET are given by main84.cc and main85.cc.

            The main issue is that the output of separate RIVET runs can not in general be combined. To perform a matrix element merging, we however need to runs over different LHE files. The solution to this problem (so far) is to only perform one RIVET run for all matrix elements, i.e. print the events for all ME parton multiplicities, with the correct weights, to a single HepMC file. Since the correct weight includes the cross section of the different samples after Sudakov vetoes --- which is not a priori known --- the cross sections have to be estimated in a test run, before the actual production run is performed. Finally, the cross section of the last event in the HepMC file has to be taken as the full merged cross section sigma_merge = Sum_{i=0}^N Sum_{j=0}*^{nEvents} sigma_est(i)*wckkwl(j).

            This procedure is outlined in main84.cc. Input LHE files with only very inclusive cuts pose further difficulties. For such files (which were already addressed under the heading Les Houches events outside the matrix element region), the cross section after the merging scale cut is not known before the cut is performed. Using Pythia's UserHooks facilities, it is possible to produce a valid estimate of the cross section after cuts. This however entails a careful cut definition by the user, which might become cumbersome for some in-built merging scale definitions. A reasonable alternative is using the switch

            Merging:doXSectionEstimate On Off   (default = off)
            If on, estimate cross section after merging scale cut. This switch has to be used in conjunction with a merging scale definition (e.g. Merging:doPTLundMerging = on). Then, this merging scale definition will be used as a cut on the input events. After the requested number of Monte Carlo events, the cross section after the cut can be extracted by inferring the Info::sigmaGen() method, and the number of accepted events by using Info::nAccepted()

            This switch also relies on knowledge on how many partons a LHE file should contain. This is important for real-emission kinematics in the case of NLO merging. The number of (additional) partons in a LHE file can be set with

            Merging:nRequested   (default = -1; minimum = -1)
            Exact number of additional jets requested for a particular LHE file. If a file should for example only contain W+ g g events, this switch should be set to "2" for this LHE file. For NLO merging schemes (see ";?>NLO Merging), this number has to be set.

            The usage of these switches to obtain the necessary cross section estimate is illustrated in main85.cc. The example main85.cc program is intended as a "front-end" for CKKW-L merging in Pythia8, so we will discuss the program briefly. main85.cc should be used together with an input file (like main85.cmnd). The executable should be invoked with three arguments: the input file, the "name" of the input LHE files, and the name of the output HepMC event file. To use the LHE files that are shipped with the Pythia distribution, a valid usage would be

            ./main85.exe ./main85.cmnd ./w_production ./myhepmc.hepmc

            If you want to use other input LHE files, note that main85.cc assumes the naming convention name_tree_#nAdditionalJets.lhe. All settings can be included though the input file, so that main85.cc does not have to be changed explicitly. main85.cc first switches off showers, multiparton interactions and hadronisation, and estimates the cross sections (after enforcing the merging scale cut) of samples for different numbers of additional jets. Then, showers, MPI and hadronisation are switched on again, and the CKKW-L merging procedure is performed. Events will be read in a decreasing sequence of jet multiplicities, which also means that e.g. events with two additional partons in the LHE file will be printed to the HepMC file before events with one additional parton.


            Further variables

            For more advanced manipulations of the merging machinery, all parameter changes that were investigated in [Lon11] are supplied. Please check [Lon11] for a detailed discussion of the switches.

            These switches allow enthusiastic users to perform a systematic assessment of the merging prescription. Apart from this, we advise the non-expert user to keep the default values.

            Merging:nQuarksMerge   (default = 5; minimum = 2; maximum = 5)
            This switch controls which quarks flavours (labelled by PDG id's) are considered additional partons. If e.g. set to 4, then u-, d-, c- and s-quarks will be merged, while b-quarks will not be considered in the merging (corresponding to a 4-flavour merging scheme). We advise caution when changing this number. In particular, please ensure that the allowed flavour for additional partons in the input LHE file does not exceed this value, since unnecessary double-counting might occur otherwise.

            Merging:includeMassive On Off   (default = on)
            If on, use the correct massive evolution variable and massive splitting kernels in the reconstruction and picking of parton shower histories of the matrix element. If off, reconstruct evolution scales, kinematics and splitting kernels as if all partons were massless.

            Merging:enforceStrongOrdering On Off   (default = off)
            If on, preferably pick parton shower histories of the matrix element which have strongly ordered consecutive splittings, i.e. paths in which consecutive reclustered evolution scales are separated by a user-defined factor.

            Merging:scaleSeparationFactor   (default = 1.0; minimum = 1.0; maximum = 10.0)
            The factor by which scales should differ to be classified as strongly ordered.

            Merging:orderInRapidity On Off   (default = off)
            If on, preferably pick parton shower histories of the matrix element with consecutive splittings ordered in rapidity and pT.

            Merging:pickByFullP On Off   (default = on)
            If on, pick parton shower histories of the matrix element by the full shower splitting kernels, including potential ME corrections and Jacobians from joined evolution measures.

            Merging:pickByPoPT2 On Off   (default = off)
            If on, pick parton shower histories of the matrix element by the shower splitting kernels divided by the evolution pT.

            Merging:pickBySumPT On Off   (default = off)
            If on, exclusively pick parton shower histories of the matrix element for which have the smallest sum of scalar evolution pT for consecutive splittings has been calculated.

            Merging:includeRedundant On Off   (default = off)
            If on, then also include PDF ratios and αs factors in the splitting probabilities used for picking a parton shower history of the matrix element, when picking histories by the full shower splitting probability. As argued in [Lon11], this should not be done since a reweighting with PDF ratios and αs factors will be performed. However, it can give useful insight in how sensitive the results are to the prescription on how to choose PS histories.

            Merging:nonJoinedNorm   (default = 1.0; minimum = 0.0; maximum = 10.0)
            Normalisation factor with which to multiply splitting probability for splittings without joined evolution equation.

            Merging:fsrInRecNorm   (default = 1.0; minimum = 0.0; maximum = 10.0)
            Normalisation factor with which to multiply splitting probability for final state splittings with an initial state recoiler.

            Merging:aCollFSR   (default = 1.0; minimum = 0.0; maximum = 10.0)
            Factor with which to multiply the scalar pT of a final state splitting, when choosing the history by the smallest sum of scalar pT. Default value taken from Herwig++ [Tul09].

            Merging:aCollISR   (default = 0.9; minimum = 0.0; maximum = 10.0)
            Factor with which to multiply the scalar pT of an initial state splitting, when choosing the history by the smallest sum of scalar pT. Default value taken from Herwig++ [Tul09].

            Merging:unorderedScalePrescrip   (default = 0; minimum = 0; maximum = 1)
            When the parton shower history of the matrix element contains a sequence of splittings which are not ordered in evolution pT (called an unordered history), this sequence is interpreted as a combined emission. Then, a decision on which starting scale for trial emissions off reconstructed states in this sequence of unordered splittings has to be made. Two options are available:
            0 : Use larger of the two reconstructed (unordered) scales as starting scale.
            1 : Use smaller of the two reconstructed (unordered) scales as starting scale.


            Merging:unorderedASscalePrescrip   (default = 1; minimum = 0; maximum = 1)
            Prescription which scale to use to evaluate αs weight for splittings in a sequence of splittings which are not ordered in evolution pT.
            0 : Use the combined splitting scale as argument in αs, for both splittings.
            1 : Use the true reconstructed scale as as argument in αs, for each splitting separately.


            Merging:unorderedPDFscalePrescrip   (default = 0; minimum = 0; maximum = 1)
            Prescription which scale to use to evaluate ratios of parton distributions for splittings in a sequence of splittings which are not ordered in evolution pT.
            0 : Use the combined splitting scale as argument in PDF ratios, for both splittings.
            1 : Use the true reconstructed scale as argument in PDF ratios, for each splitting separately.


            Merging:incompleteScalePrescrip   (default = 0; minimum = 0; maximum = 2)
            When no complete parton shower history (i.e. starting from a 2 → 2 process) for a matrix element with additional jets can be found, such a configuration is said to have an incomplete history. Since in incomplete histories, not all shower starting scales are determined by clusterings, a prescription for setting the starting scale of trial showers in incomplete histories is needed. Three options are provided.
            0 : Use factorisation scale as shower starting scale for incomplete histories.
            1 : Use sHat as shower starting scale for incomplete histories.
            2 : Use s as shower starting scale for incomplete histories.


            Merging:allowColourShuffling On Off   (default = off)
            If on, this will allow the algorithm to swap one colour index in the state, when trying to find all possible clusterings, if no clustering has been found, but more clusterings had been requested. In this way, some incomplete histories can be avoided. Generally, we advise the non-expert user to not touch this switch, because a slight change in the colour structure can change the radiation pattern. To however study the sensitivity of the predictions on these effects, allowing for colour reshuffling can be useful.

            Merging:usePythiaQRenHard On Off   (default = on)
            If on, this will allow the algorithm to use a dynamical renormalisation scale to evaluate the strong couplings of the core hard process in dijet and prompt photon events. This means that the value of αs used as coupling of the hard process in the matrix element generation will be replaced with a running coupling evaluated at the geometric mean of the squared transverse masses of the two outgoing particles, as is the default prescription in Pythia.

            Merging:usePythiaQFacHard On Off   (default = on)
            If on, this will allow the algorithm to use a dynamical factorisation scale to evaluate parton distributions associated with the hadronic cross section of the core hard process in dijet and prompt photon events. In the calculation of PDF ratios as part of the CKKW-L weight of an event, parton distributions that should be evaluated at the scale of the core 2 - >2 process will be evaluated using the dynamical factorisation scale Pythia would attribute to this process. This means that the hard process factorisation scale is set to the smaller of the squared transverse masses of the two outgoing particles.

            Merging:mayRemoveDecayProducts On Off   (default = off)
            Remove products of resonances in the hard process, in case Pythia generates decay products before merging. This makes merging possible even for an indeterminate final state, if Pythia itself has produced the decay products. The merging methods will instead be invoked on the "non-decayed" event, thus removing the limitation to only one decay channel when performing the merging. This switch is necessary e.g. for slepton pair production in association with additional QCD jets, if the input LHE file contains the resonant sleptons, and Pythia decides on a decay according to the branching fractions read from SLHA input.

            Merging:allowSQCDClustering On Off   (default = off)
            Allow clustering of gluon emission off squarks.

            Merging:allowWClustering On Off   (default = off)
            Allow clustering of W boson, if interpreted as a final state emission. This switch should not be used until electro-weak showers become available. "?>

            pythia8-8.1.80.orig/phpdoc/Index.php0000644000175000017500000002242312217615312015371 0ustar sunsun Index SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>
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            PYTHIA 8 Index

            Program Overview

            Frontpage
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              --   QCD
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              --   Compositeness
              --   Hidden Valleys
              --   Extra Dimensions
            A Second Hard Process
            Phase Space Cuts
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            Study Output

            Four-Vectors
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            Link to Other Programs

            Les Houches Accord
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            Matching and Merging
              --   CKKW-L Merging
              --   Jet Matching
              --   UMEPS Merging
              --   NLO Merging
            User Hooks
            Hadron-Level Standalone
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            Brief Introduction
            Worksheet pythia8-8.1.80.orig/phpdoc/SettingsScheme.php0000644000175000017500000005317012217615312017252 0ustar sunsun The Settings Scheme SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            The Settings Scheme

            The Settings class keeps track of all the flags, modes, parameters and words used during the event generation. As such, it serves all the Pythia program elements from one central repository. Accessing it allows the user to modify the generator behaviour.

            Each Pythia object has a public member settings of the Settings class. Therefore you access the settings methods as pythia.settings.command(argument), assuming that pythia is an instance of the Pythia class. Further, for the most frequent user tasks, Pythia methods have been defined, so that pythia.command(argument) would work, see further below.

            The central section on this page is the Operation one. The preceding concepts section is there mainly to introduce the basic structure and the set of properties that can be accessed. The subsequent sections provide a complete listing of the existing public methods, which most users probably will have little interaction with.

            Concepts

            We distinguish six kinds of user-modifiable variables, by the way they have to be stored:
            1. Flags are on/off switches, and are stored as bool.
            2. Modes corresponds to a finite enumeration of separate options, and are stored as int.
            3. Parameters take a continuum of values, and are stored as double. The shorthand notation parm is used in the C++ code and XML tags.
            4. Words are simple character strings and are stored as string. No blanks or double quotation marks (") may appear inside a word, the former to simplify parsing of an input file and the latter not to cause conflicts with XML attribute delimiters. Currently the main application is to store file names.
            5. Vectors of modes take a variable length, and are stored as vector<int>. The shorthand notation mvec is used in the C++ code and XML tags. When the vector is input as a string, all the values have to be given as a comma-separated list with no blanks, to simplify parsing.
            6. Vectors of parameters take a variable length and for each element a continuum of values, and are stored as vector<double>. The shorthand notation pvec is used in the C++ code and XML tag. When the vector is input as a string, all the values have to be given as a comma-separated list with no blanks, to simplify parsing.
            Note that all shorthands have been chosen four letters long.

            In general, each variable stored in Settings is associated with four kinds of information:

            • The variable name, of the form class:name (or file:name, usually these agree), e.g. TimeShower:pTmin. The class/file part usually identifies the .xml file where the variable is defined, and the part of the program where it is used, but such a connection cannot be strictly upheld, since e.g. the same variable may be used in a few different cases (even if most of them are not).
            • The default value, set in the original declaration, and intended to represent a reasonable choice.
            • The current value, which differs from the default when the user so requests.
            • An allowed range of values, represented by meaningful minimum and maximum values. This has no sense for a flag or a word (and is not used there), is usually rather well-defined for a mode or mvec, but less so for a parm or pvec. Often the allowed range exaggerates the degree of our current knowledge, so as not to restrict too much what the user can do. One may choose not to set the lower or upper limit, in which case the range is open-ended.

            Technically, the Settings class is implemented with the help of six separate maps, one for each kind of variable, with the variable name used as key.

            Operation

            The normal flow of setting values is:

            1. When a Pythia object pythia is created, the member pythia.settings is asked to scan the files listed in the Index.xml file in the xmldoc subdirectory.

              In all of the files scanned, lines beginning with <flag, <mode, <parm, <word, <mvec or <pvec are identified, and the information on such a line is used to define a new flag, mode, parameter, word, or vector of modes or parameters. To exemplify, consider a line

              <parm name="TimeShower:pTmin" default="0.5" min="0.1" max="2.0">
              
              which appears in the TimeShower.xml file, and there defines a parameter TimeShower:pTmin with default value 0.5 GeV and allowed variation in the range 0.1 - 2.0 GeV. The min and max values are optional.
              Important: the values in the .xml files should not be changed, except by the PYTHIA authors. Any changes should be done with the help of the methods described below.
            2. Between the creation of the Pythia object and the init call for it, you may use several alternative methods to modify some of the default values. The same variable can be changed several times. If so, it is the last read value that counts. The two special ";?>Tune:ee and ";?>Tune:pp modes and the ";?>Print:quiet flag are expanded to change several settings in one go, but these obey the same ordering rules.

              a) Inside your main program you can directly set values with

                  pythia.readString(string) 
              
              where both the variable name and the value are contained inside the character string, separated by blanks and/or a =, e.g.
                  pythia.readString("TimeShower:pTmin = 1.0"); 
              
              The match of the name to the database is case-insensitive. Names that do not match an existing variable are ignored. A warning is printed, however. Strings beginning with a non-alphanumeric character, like # or !, are assumed to be comments and are not processed at all. Values below the minimum or above the maximum are set at the respective border. For bool values, the following notation may be used interchangeably: true = on = yes = ok = 1, while everything else gives false (including but not limited to false, off, no and 0).

              b) The Pythia readString(string) method actually does not do changes itself, but sends on the string either to the Settings class or to ParticleData. The former holds if the string begins with a letter, the latter if it begins with a digit. If desired, it is possible to communicate directly with the corresponding Settings method:

                  pythia.settings.readString("TimeShower:pTmin = 1.0"); 
              
              In this case, changes intended for ParticleData would not be understood.

              c) Underlying the settings.readString(string) method are the settings-type-sensitive commands in the Settings, that are split by names containing flag, mode, parm or word. Thus, the example now reads

                  pythia.settings.parm("TimeShower:pTmin", 1.0); 
              
              Such a form could be convenient e.g. if a parameter is calculated at the beginning of the main program, and thus is available as a variable rather than as a character string. Note that Boolean values must here be given as true or false i.e. there is less flexibility than with the previous methods.

              At the same level, there are several different methods available. These are included in the full description below, but normally the user should have no need for them.

              d) A simpler and more useful way is to collect all your changes in a separate file, with one line per change, e.g.

                  TimeShower:pTmin = 1.0
              
              Each line is read in as a string and processed with the methods already introduced. The file can be read by the
                  pythia.readFile(fileName); 
              
              method (or an istream instead of a fileName). The file can freely mix commands to the Settings and ParticleData classes, and so is preferable. Lines with settings are handled by calls to the pythia.settings.readString(string) method.
            3. In the pythia.init(...) call, many of the various other program elements are initialized, making use of the current values in the database. Once initialized, the common Settings database is likely not consulted again by these routines. It is therefore not productive to do further changes in mid-run: at best nothing changes, at worst you may set up inconsistencies.

              A routine reInit(fileName) is provided, and can be used to zero all the maps and reinitialize them from scratch. Such a call might be useful if several subruns are to be made with widely different parameter sets - normally the maps are only built from scratch once, namely when the Pythia() object is created. A more economical alternative is offered by resetAll(), however, which sets all variables back to their default values.

            4. You may at any time obtain a listing of all variables in the database by calling
                  pythia.settings.listAll();
              
              The listing is strictly alphabetical, which at least means that names from the same file are kept together, but otherwise may not be so well-structured: important and unimportant ones will appear mixed. A more relevant alternative is
                  pythia.settings.listChanged();
              
              where you will only get those variables that differ from their defaults. Or you can use
                  pythia.settings.list("string");
              
              where only those variables with names that contain the string (case-insensitive match) are listed. Thus, with a string shower, the shower-related variables would be shown.
            5. The above listings are in a tabular form that cannot be read back in. Assuming you want to save all changed settings (maybe because you read in changes from several files), you can do that by calling
                  pythia.settings.writeFile(fileName);
              
              This file could then directly be read in by readFile(fileName) in a subsequent (identical) run. Some variants of this command are listed below.

            Methods

            The complete list of methods and arguments is as follows. Most of the ones of interest to the user have already been mentioned above. Others can be used, but the same functionality is better achieved by higher-level routines. Some are part of the internal machinery, and should not be touched by user.

            Note that there is no Settings::readFile(...) method. The intention is that you should use Pythia::readFile(...). It parses and decides which individual lines should be sent on to Settings::readString(...).

            Settings::Settings()  
            the constructor, which takes no arguments. Internal.

            bool Settings::initPtr(Info* infoPtrIn)  
            initialize pointer to error-message database. Internal.

            bool Settings::init(string startFile = "../xmldoc/Index.xml", bool append = false, ostream& os = cout)  
            read in the settings database.
            argument startFile (default = "../xmldoc/Index.xml") : read in the settings from all the files listed in this file, and assumed to be located in the same subdirectory.
            argument append (default = false) : By default nothing is done if the method has already been called once. If true the further settings read in are added to the current database.
            argument os (default = cout) : stream for error printout.
            Note: The method returns false if it fails.

            bool Settings::reInit(string startFile = "../xmldoc/Index.xml", ostream& os = cout)  
            overwrite the existing database.
            argument startFile (default = "../xmldoc/Index.xml") : read in the settings from all the files listed in this file, and assumed to be located in the same subdirectory.
            argument os (default = cout) : stream for error printout.
            Note: The method returns false if it fails.

            bool Settings::readString(string line, bool warn = true, ostream& os = cout)  
            read in a string, and change the relevant quantity in the database. It is normally used indirectly, via Pythia::readString(...) and Pythia::readFile(...).
            argument line : the string to be interpreted as an instruction.
            argument warn (default = true) : write a warning message or not whenever the instruction does not make sense, e.g. if the variable does not exist in the databases.
            argument os (default = cout) : stream for error printout.
            Note: the method returns false if it fails to make sense out of the input string.

            bool Settings::writeFile(string toFile, bool writeAll = false)  
            bool Settings::writeFile(ostream& os = cout, bool writeAll = false)  
            write current settings to a file or to an ostream.
            argument toFile, os : file or stream on which settings are written.
            argument writeAll (default = false) : normally only settings that have been changed are written, but if true then all settings are output.
            Note: the method returns false if it fails.

            void Settings::listAll(ostream& os = cout)  
            void Settings::listChanged(ostream& os = cout)  
            void Settings::list(string match, ostream& os = cout)  
            list all or changed settings, or a group of them.
            argument match : list all those settings where the name contains the match (sub)string (case-insensitive).
            argument os (default = cout) : output stream for the listing.

            void Settings::resetAll()  
            reset all current values to their defaults.

            bool Settings::isFlag(string key)  
            bool Settings::isMode(string key)  
            bool Settings::isParm(string key)  
            bool Settings::isWord(string key)  
            bool Settings::isMVec(string key)  
            bool Settings::isPVec(string key)  
            return true if an entry of the given name and kind exists, else false.

            void Settings::addFlag(string key, bool default)  
            void Settings::addMode(string key, int default, bool hasMin, bool hasMax, int min, int max)  
            void Settings::addParm(string key, double default, bool hasMin, bool hasMax, double min, double max)  
            void Settings::addWord(string key, string default)  
            void Settings::addMVec(string key, vector<int> default, bool hasMin, bool hasMax, int min, int max)  
            void Settings::addPVec(string key, vector<double> default, bool hasMin, bool hasMax, double min, double max)  
            add an entry of the respective kind to the database. The name and default value(s) always has to be supplied, for Mode, Parm, MVec and PVec additionally if lower and/or upper limits are to be imposed and, if so, what those limit are.

            bool Settings::flag(string key)  
            int Settings::mode(string key)  
            double Settings::parm(string key)  
            string Settings::word(string key)  
            vector<int> Settings::mvec(string key)  
            vector<double> Settings::pvec(string key)  
            return the current value(s) of the respective setting. If the name does not exist in the database, a value false, 0, 0., " ", or a vector of length 1 and value 0 or 0., respectively, is returned.

            bool Settings::flagDefault(string key)  
            int Settings::modeDefault(string key)  
            double Settings::parmDefault(string key)  
            string Settings::wordDefault(string key)  
            vector<int> Settings::mvecDefault(string key)  
            vector<double> Settings::pvecDefault(string key)  
            return the default value(s) of the respective setting. If the name does not exist in the database, a value false, 0, 0., " ", or a vector of length 1 and value 0 or 0., respectively, is returned.

            map Settings::getFlagMap(string match)  
            map Settings::getModeMap(string match)  
            map Settings::getParmMap(string match)  
            map Settings::getWordMap(string match)  
            map Settings::getMVecMap(string match)  
            map Settings::getPVecMap(string match)  
            return a map of all settings of the respective type that contain the string "match" in its name.

            void Settings::flag(string key, bool now)  
            void Settings::mode(string key, int now)  
            void Settings::parm(string key, double now)  
            void Settings::word(string key, string now)  
            void Settings::mvec(string key, vector<int> now)  
            void Settings::pvec(string key, vector<double> now)  
            change the current value(s) of the respective setting to the provided new value(s). If lower or upper limits have been set, input values outside the allowed range are reinterpreted as being a the nearest limit.

            void Settings::forceMode(string key, int now)  
            void Settings::forceParm(string key, double now)  
            void Settings::forceMVec(string key, vector<int> now)  
            void Settings::forcePVec(string key, vector<double> now)  
            as above, but do not check lower and upper limits, so that the current value(s) can be put outside the intended borders.

            void Settings::resetFlag(string key)  
            void Settings::resetMode(string key)  
            void Settings::resetParm(string key)  
            void Settings::resetWord(string key)  
            void Settings::resetMVec(string key)  
            void Settings::resetPVec(string key)  
            reset the current value to the default one. pythia8-8.1.80.orig/phpdoc/AlpgenEventInterface.php0000644000175000017500000003505012217615312020353 0ustar sunsun ALPGEN Event Interface SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            ALPGEN Event Interface

            This manual page describes the ALPGEN [Man03] event interface for PYTHIA8. While future versions of ALPGEN will be able to write out events in LHEF format, previous versions always output events in an ALPGEN native format (a combination of a ".unw" and a "_unw.par" file). The ALPGEN component of this code contains a reader for this native format (for unweighted events), as well as parameter reading for both ALPGEN native and LHE file formats. The reader was designed to work together with an implementation of the ALPGEN-style parton-jet matching JetMatchingAlpgen described on the ";?>Jet Matching page. However, it will also work with a implementation of the Madgraph-style [Alw11] parton-jet matching JetMatchingMadgraph also described on the ";?>Jet Matching page. A sensible choice of JetMatching parameters is needed when using ALPGEN files with Madgraph-style matching and vice versa.

            It should be noted that all the functionality described here is provided through external routines, and therefore the presence of these features is dependent on the main program being used. This structure allows for the easy extensibility of the merging scheme. The files of interest are located in the examples/ subdirectory:

            • GeneratorInput.h : provides three classes for the reading of ALPGEN event and parameter files. LHAupAlpgen is an ";?>LHAup derived class for reading in ALPGEN native format event files. AlpgenPar is a class for the parsing of ALPGEN parameter files, making the information available through a simple interface. AlpgenHooks is a ";?>UserHooks derived class that provides the Alpgen:* options, described below. Further technical details of these classes are given at the end of this manual page.
            • main32.cc, main32.cmnd : a sample main program and card file showing the usage of previous file and an MLM UserHooks class. In combination, it reads in a sample ALPGEN (or Madgraph) event file while performing the MLM merging procedure as implemented in ALPGEN (or as in Madgraph). Some commented-out sets of options are provided in the card file, which can be activated to try different merging setups.
            • main32.unw, main32_unw.par : an ALPGEN format event and parameter file containing 100 W + 3 jet events. It is not feasible to package large event files with the PYTHIA distribution, but this sample is enough to show the different components in action.

            ALPGEN main options

            These following options are provided by the AlpgenHooks class, which must be loaded for this functionality to be present

            ALPGEN event files that have been written out in LHEF format should be read in through the normal LHEF machinery (see ";?>Beam Parameters). Files in ALPGEN's native format, instead, may be processed using the Alpgen:file option below. When using this option, the ALPGEN parameter file is stored in the PYTHIA Info object under the key AlpgenPar, see the "Header information" section of the ";?>Event Information manual page for more details. Processes not implemented by the PYTHIA 6 interface supplied with ALPGEN are also not implemented here.

            When reading in ALPGEN native event files, some momenta are shifted by the file reader to ensure energy-momentum conservation. The magnitude of these shifts should be small (around the MeV level in the worst case) and warnings will be produced if they are above a set threshold. A large number of warnings may signify unexpected behaviour and should potentially be investigated. It is also known that certain event classes, for example an event with both light and heavy b quarks may give rise to these warnings.

            The ALPGEN file reader supports the reading of the event and parameter files in gzip format with file extensions ".unw.gz" and "_unw.par.gz" respectively. This requires the use of external libraries, however, and the README file in the main directory contains instructions on how to enable this.

            All other Alpgen:* options apply to both LHE and native file formats, and include options to guide the MLM merging procedure based on the parameters that are read in with the events file.

            Alpgen:file   (default = void)
            This option is used to read in ALPGEN format event files. Using this option overrides any previously set beam options inside PYTHIA. The path to the files, not including any file extension, should be provided e.g. for input files input_unw.par and input.unw, the value input should be used.

            Alpgen:setMasses On Off   (default = on)
            When switched on, any particle masses provided by ALPGEN are set in the PYTHIA ";?>particle database.

            Alpgen:setMLM On Off   (default = on)
            When switched on, the merging parameters (see below) are set according to the ALPGEN hard process cuts:

            • JetMatching:eTjetMin = min(ptjmin + 5., 1.2 * ptjmin),
            • JetMatching:coneRadius = drjmin,
            • JetMatching:etaJetMax = etajmax.
            where the ptjmin, drjmin and etajmax are the incoming ALPGEN parameters. Note that any existing values of these parameters are overwritten.

            Alpgen:setNjet On Off   (default = on)
            When switched on, the JetMatching:nJet parameter (see below) is set to the incoming njet ALPGEN parameter. Note that any existing value of this parameter is overwritten.

            Class information

            Some more technical information about the different classes is given below. For clarity, some limited information on certain private methods is provided.

            LHAupAlpgen

            This class is derived from the ";?>LHAup base class, and uses the standard machinery to pass initialisation and event data to PYTHIA. These standard functions are not documented here. The complete parameter file is stored in the PYTHIA Info object, if given, under the key AlpgenPar.

            LHAupAlpgen::LHAupAlpgen(const char *baseFNin, Info *infoPtrIn = NULL)  
            The constructor for the class takes the base filename for the ALPGEN format files (without file extensions) and optionally a pointer to a PYTHIA Info class, used for warning/error message printing and for storing the ALPGEN parameter file. The event and parameter files are opened immediately, with the AlpgenPar class, described below, used to parse the parameter file.

            bool LHAupAlpgen::addResonances()  
            This is a private method used when an event is read in. The information read from the event file does not always contain a complete listing of all particles and four-momenta, and so various details must be reconstructed. Exactly which details are filled in can vary based on the ALPGEN process in question.

            bool LHAupAlpgen::rescaleMomenta()  
            This is another private method used when an event is read in. It shuffles and rescales momenta in an event to ensure energy-momentum conservation. First, pT is made to balance by splitting any imbalance between all outgoing particles with their energies also scaled. Second, the e/pZ of the two incoming particles are scaled to balance the outgoing particles. Finally, any intermediate resonances are recalculated from their decay products.

            AlpgenPar

            This class parses an ALPGEN parameter file and makes the information available through a simple interface. The information is stored internally in key/value (string/double) format. All lines prior to:
              ************** run parameters 
            are ignored, and in the general case, a line e.g.
              10   3.00000000000000        ! njets
            would be stored with key "njets" and value "3.0". The following lines are special cases where the line may be split or the key translated:
              3 ! hard process code
              0.000   4.700 174.300  80.419  91.188 120.000 ! mc,mb,mt,mw,mz,mh
              912.905 0.0914176   ! Crosssection +- error (pb)
              100 29787.4  ! unwtd events, lum (pb-1) Njob= 2
            
            In the first line, the key "hard process code" is translated to "hpc". In the second, the mass values are split and each given an entry in the internal store. In the third, the cross section and cross section error are stored under the keys "xsecup" and "xerrup" respectively. Finally, the number of events and luminosity are stored under the keys "nevent" and "lum" respectively. In the event that a duplicate key is present, with differing values, the stored value is overwritten and a warning given.

            AlpgenPar::AlpgenPar(Info *infoPtrIn = NULL)  
            The constructor does nothing except for store the PYTHIA Info pointer, if given. This is used for warning/error message printing.

            bool AlpgenPar::parse(const string paramStr)  
            This method parses an ALPGEN parameter file. The parameter file is passed as a single string, mainly intended to be read out from the PYTHIA Info object using the header information methods.

            bool AlpgenPar::haveParam(const string &paramIn)  
            Method to check if a parameter with key paramIn is present. Returns true if present, else false.

            double AlpgenPar::getParam(const string &paramIn)  
            int AlpgenPar::getParamAsInt(const string &paramIn)  
            Return the parameter with key paramIn as a double or integer. The presence of a parameter should have already been checked using the haveParam() function above. If the parameter is not present, 0 is returned.

            void AlpgenPar::void printParams()  
            Method to print a list of stored parameters.

            AlpgenHooks

            This ";?>UserHooks derived class provides all the Alpgen:* options. It is provided as a UserHooks class such that the code works regardless of whether ALPGEN native or LHE file formats are used. It is declared with virtual inheritance so that it may be combine with other UserHooks classes, see the "Combining UserHooks" section below.

            AlpgenHooks(Pythia &pythia)  
            The constructor takes a PYTHIA object as input, so that the beam parameter settings can be overridden if the Alpgen:file option is given. If this is the case, an LHAupAlpgen instance is automatically created and passed to PYTHIA.

            bool initAfterBeams()  
            This is the only UserHooks method that is overridden. It is called directly after PYTHIA has initialised the beams, and therefore the header information should be present in the PYTHIA Info object. The AlpgenPar class is used to parse ALPGEN parameters, if present, which are then used to set further PYTHIA settings. "?>

            pythia8-8.1.80.orig/phpdoc/GUIDELINES0000644000175000017500000001105212217346234015164 0ustar sunsun MCNET GUIDELINES for Event Generator Authors and Users PREAMBLE This generator has been developed as part of an academic research project and is the result of many years of work by the authors. Proper academic recognition is a requirement for its continued development. The components of the program have been developed to work together as a coherent physics framework. We believe that the creation of separately maintained forks or piecewise distribution of individual parts would diminish their scientific value. The authors are convinced that software development in a scientific context requires full availability of all source code, to further progress and to allow local modifications to meet the specific requirements of the individual user. Therefore we have decided to release this program under the GNU General Public License (GPL) version 2. This ensures that the source code will be available to you and grants you the freedom to use and modify the program. You can redistribute your modified versions as long as you retain the GPL and respect existing copyright notices (see the file 'COPYING' for details). By using the GPL, we entrust you with considerable freedom and expect you to use it wisely, since the GPL does not address the issues in the first two paragraphs. To remedy this shortcoming, we have formulated the following guidelines relevant for the distribution and usage of event generator software in an academic setting. GUIDELINES 1) The integrity of the program should be respected. ------------------------------------------------- 1.1) Suspected bugs and proposed fixes should be reported back to the original authors to be considered for inclusion in the standard distribution. No independently developed and maintained forks should be created as long as the original authors actively work on the program. 1.2) The program should normally be redistributed in its entirety. When there are special reasons, an agreement should be sought with the original authors to redistribute only specific parts. This should be arranged such that the redistributed parts remain updated in step with the standard distribution. 1.3) Any changes in the code must be clearly marked in the source (reason, author, date) and documented. If any modified version is redistributed it should be stated at the point of distribution (download link) that it has been modified and why. 1.4) If a significant part of the code is used by another program, this should be clearly specified in that program's documentation and stated at its point of distribution. 1.5) Copyright information and references may not be removed. Copyright-related program messages may not be altered and must be printed even if only a part of the program is used. Adding further messages specifying any modifications is encouraged. 2) The program and its physics should be properly cited when used for academic publications ------------------------------------------------------------------ 2.1) The main software reference as designated by the program authors should always be cited. 2.2) In addition, the original literature on which the program is based should be cited to the extent that it is of relevance for a study, applying the same threshold criteria as for other literature. 2.3) When several programs are combined, they should all be mentioned, commensurate with their importance for the physics study at hand. 2.4) To make published results reproducible, the exact versions of the codes that were used and any relevant program and parameter modifications should be spelled out. POSTSCRIPT The copyright license of the software is the GPL v2 alone, therefore the above guidelines are not legally binding. However, we reserve the right to criticize offenders. The guidelines should always be combined with common sense, for interpretation and for issues not covered. Enquiries regarding the guidelines and related issues are encouraged and should be directed to the authors of the program. Please note that the program, including all its code and documentation, is intended for academic use and is delivered "as is" to be used at your own risk, without any guarantees. ---------------------------------------------------------------------- These guidelines were edited by Nils Lavesson and David Grellscheid for the MCnet collaboration, which has approved and agreed to respect them. MCnet is a Marie Curie Research Training Network funded under Framework Programme 6 contract MRTN-CT-2006-035606. pythia8-8.1.80.orig/phpdoc/NLOMerging.php0000644000175000017500000013330612217615312016266 0ustar sunsun NLO Merging SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            NLO Merging

            Pythia offers two NLO merging approaches. Both of these methods have been presented in [Lon13]. The goal of NLO merging is to extend tree-level multi-jet merging methods to next-to-leading order accuracy in QCD, for every available jet multiplicity. If for example NLO calculations for Higgs + 0 jet, Higgs + 1 jet and Higgs + 2 jets were available, NLO merging allows to simultaneously describe 0-, 1- and 2-jet observables with NLO accuracy. Further jets can, depending on additional tree-level input, be described by additional tree-level matrix elements. In the example, it would be possible to achieve NLO accuracy for 0-, 1- and 2-jet observables, tree-level accuracy for 3-, 4- and 5-jet configurations, and use the parton shower approximation for events with more than five jets.

            The two NLO merging methods implemented in Pythia are called NL3 (for Nils Lavesson + Leif Lönnblad) and UNLOPS (for unitarised NLO+PS merging). Both of these schemes require Les Houches Event File input that is generated by tree-level or NLO matrix element generators. Currently, Pythia requires NLO input generated within the POWHEG framework. The generation of sensible input will be discussed below. The two NLO merging methods are illustrated in the sample main programs main87.cc (introducing NL3 ) and main88.cc (introducing UNLOPS). Before describing these programs, we would like to outline the differences between the two approaches.

            NL3 is a generalisation of ";?>CKKW-L tree-level merging. The main idea of NL3 is to start from CKKW-L-reweighted multi-jet merging, and replace the αsn+0- and αsn+1-terms by the NLO result of POWHEG. This "replacement" means that we subtract the αsn+0- and αsn+1-terms from the CKKW-L-reweighted tree-level samples, and add another sample -- the POWHEG input. All "higher orders" are unchanged w.r.t. CKKW-L. We have implemented the "inclusive" scheme of [Lon13] in Pythia. This means that the POWHEG input will contain contributions for hard, resolved real emission jets, which are already taken care of by higher-multiplicity samples in CKKW-L. Thus, explicit phase space subtractions are also included. The sample program main87.cc, together with the input file main87.cmnd, illustrates the procedure.

            UNLOPS is a generalisation of the ";?>UMEPS multi-jet merging scheme. Since UMEPS is already slightly more complicated than CKKW-L, this makes UNLOPS more complicated than NL3. The basic idea however remains the same: Start from a tree-level merging scheme (in this case UMEPS), remove all undesirable αsn+0- and αsn+1-terms from this result, and add back the "correct" description via POWHEG input samples. Again, since the "inclusive" scheme of [Lon13] was implemented in Pythia, it is necessary to handle explicit phase space subtractions. Similar to UMEPS, UNLOPS further ensures that the lowest-multiplicity cross section is given by the NLO result. This means that the UMEPS philosophy of "subtract what you add" needs to be extended to multi-leg NLO inputs.

            UNLOPS is a theoretically more appealing definition of NLO merging than NL3, and should thus be considered the preferred choice. However, we believe it valuable to include both methods into Pythia, so that the variation of NLO merged results due to different NLO merging schemes can be studied in situ. Furthermore, NLO merging can be outlined more pedagogically when starting from NL3. The two NLO merging methods share parts of code with CKKW-L and UMEPS, and correspondingly share many input settings with these schemes. In particular,

                     The hard process (Merging:Process) needs to be defined exactly as in CKKW-L (see Defining the hard process in the ";?>CKKW-L documentation).

                     The merging scale value (Merging:TMS) has to be set.

                     The maximal number of additional partons in tree-level events (Merging:nJetMax) has to be set.

            All settings listed under the sections "Matrix element merging and HepMC output for RIVET" and "Further variables" in the ";?>CKKW-L documentation can be accessed in NLO merging as well. Furthermore, the Merging:nRecluster switch (see the ";?>UMEPS documentation) is important. Also, all MergingHooks routines that allow for user interference in CKKW-L merging are also usable for NLO merging -- with the exception of a user-defined merging scale. The NLO merging schemes currently implemented in Pythia do not allow for a merging scale definition that differs from the parton shower evolution variable. Since this merging scale definition is not completely obvious, the NLO merging schemes also share the Merging:enforceCutOnLHE switch with CKKW-L. In this way, it is possible to use LHE files that are regularised only with weak cuts as input, while the merging machinery imposes the stronger merging scale cut automatically. This means that no merging scale implementation is required from the user side, but also means that it is the user's responsibility to ensure that the cuts used for generating input LHE files are always looser than the cut given by the merging scale value Merging:TMS. This will lead to warnings of the form "Les Houches Event fails merging scale cut. Cut by rejecting event". These warning should rather be regarded as information. An example of inclusive matrix element generation cuts would be pTjet = 5 GeV, ΔRjetA jetB = 0.01 and QjetA jetB = 5 GeV, if NLO merging with a desired merging scale value of Merging:TMS = 15 is attempted for Higgs + jets events at the LHC.

            In the following, we will first describe the generation of NLO input samples, and list input settings for NLO merging in Pythia. Then, we will examine the sample main programs main87.cc and main88.cc, which implement NL3 and UNLOPS merging, respectively.


            Inputs for NLO merging

            The NLO merging schemes in Pythia currently require Les Houches Event File input. To perform a merging with up to M additional partons described by tree-level matrix elements, and with up to N ≤ M-1 additional partons at NLO accuracy, the user needs to supply

                     LHE files for 0... M additional partons, taken from a tree-level matrix element generator, and

                     LHE files for 0... N additional partons, taken from a POWHEG NLO generator.

            All input files need to be regularised, if they contain additional partons. Large files with fairly inclusive (i.e. loose) cuts are recommended. The input LHE files should further be generated with fixed renormalisation and factorisation scales. (In the POWHEG-BOX program, this means using the settings runningscales 0, btlscalereal 1, btlscalect 1, ckkwscalup 0. Some older processes in the POWHEG-BOX program need the input runningscale 0 instead of runningscales 0.)

            When attempting NLO merging, the following Pythia settings are relevant.

            Merging:nJetMaxNLO   (default = 0; minimum = 0)
            The maximal number of additional jets for which NLO event samples are supplied by the user.

            Merging:muFac   (default = -1.0)
            The fixed factorisation scale used in the hard process cross section, as needed to generate the leading-order weight, in case the factorisation scale cannot be inferred from Les Houches event input. (This is the case for files that have been generated with the POWHEG-BOX program, since this program prints the transverse momentum scale of the real emission into the LH events.). If the value is not set, the SCALUP variable of the current LH event will be used instead. If wimpy showers (see ";?>Timelike Showers and ";?>Spacelike Showers) are used together with multi-jet merging, then this scale further sets the parton shower starting scale (μQ) for the core hard process.

            Merging:muRen   (default = -1.0)
            The fixed renormalisation scale used in the hard process cross section, as needed to generate the leading-order weight, in case the renormalisation scale cannot be inferred from Les Houches event input. (As mentioned above, this is the case for files generated with the POWHEG-BOX program.) If the value is not set, the SCALUP variable of the current LH event will be used instead.

            Merging:muFacInME   (default = -1.0)
            The fixed factorisation scale used in the matrix element calculation. This information is needed if factorisation scale variations in NLO merged results are attempted. Depending on the matrix element generator, it might not be possible to infer the factorisation scale from Les Houches event input, and thus, setting an explicit value is required. (As mentioned above, this is the case for files generated with the POWHEG-BOX program.) If the value is not set, the SCALUP variable of the current LH event will be used instead.

            Merging:muRenInME   (default = -1.0)
            The fixed renormalisation scale used in the matrix element calculation. This information is needed if renormalisation scale variations in NLO merged results are attempted, for the same reason as factorisation scales might be required. (As mentioned above, this is the case for files generated with the POWHEG-BOX program.) If the value is not set, the SCALUP variable of the current LH event will be used instead.

            All further settings will be discussed while examining the sample main programs.


            NL3 merging with main87.cc

            NL3-style NLO merging in Pythia is illustrated by the sample main program main87.cc. This program works together with an input file (e.g. main87.cmnd) for Pythia settings, and requires LHE input files that follow the naming convention name_tree_#nAdditionalJets.lhe (tree-level samples) and name_powheg_#nAdditionalJets.lhe (POWHEG NLO samples). main87.cc produces HepMC event output [Dob01], which can be used for analysis (e.g. using RIVET [Buc10]), or as input for detector simulations. For users not familiar with HepMC output, it is of course possible remove the HepMC code in the sample program, and use Pythia's histogramming routines instead. Histograms should then be filled as indicated for the histPTFirstSum histograms in main84.cc, i.e. using weightNLO*normhepmc.

            If the user only wants to change the number of requested events (Main:numberOfEvents), the hard process (Merging:Process), the merging scale value (Merging:TMS) and the maximal number of additional tree-level or NLO-accuracte jets (Merging:nJetMax and Merging:nJetMaxNLO, respectively), and HepMC output is desired, then there is no need to change the main87.cc code. The input LHE files are also part of the (command line) input for main87.exe. The default settings in main87.cmnd are intended to work with the (very short) sample LHEF inputs (w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and w_production_powheg_0.lhe, w_production_powheg_1.lhe). For these input files, the main87.exe executable can be run with the command

            ./main87.exe main87.cmnd w_production myhepmc.hepmc

            to produce a file myhepmc.hepmc of NLO merged HepMC event output. All mandatory Pythia input settngs have been outlined earlier. Please refrain from adding input switches than invoke any other merging scheme (e.g. e.g. Merging:doKTMerging) into the input file that you want to use in conjunction with main87.cc.

            In the following, we will explain main87.cc in depth. Users who are willing to accept the default choices do not need to know all details, but are still encouraged to read further.

            Program flow

            main87.cc can be divided into four steps:

                     1. Estimate the cross section for tree-level and NLO samples after the merging scale cut.

                     2. Produce reweighted tree-level events, which do not contain αs0- and αs1-terms.

                     3. Add POWHEG NLO events.

                     4. Subtract phase space points with an extra (real-emission) jet above the merging scale from the POWHEG result, since such configurations have already been taken into account by processing other samples.

            The first step is necessary to produce the correct weights for HepMC output events. The estimation of tree-level cross sections after the merging scale cut is generated by invoking the switch Merging:doXSectionEstimate together with Merging:doNL3Tree. In this configuration, the latter switch will only act to define the merging scale. After the tree-level cross sections have been estimated, main87.cc estimates the NLO cross sections after application of the merging scale cut, by inferring Merging:doXSectionEstimate together with Merging:doNL3Loop. Again, in this configuration, the latter switch only acts as the merging scale definition. When generating the estimates, all showering, multiparton interactions and hadronisation is turned off to not unnecessarily waste processor time. For all estimates, is further mandatory to set the value of Merging:nRequested to the jet multiplicity of the current event sample (e.g. to "2" for a sample containing W + 2 jet events). This is necessary in order to correctly apply the merging scale cut. POWHEG NLO input files for W + 1 jet e.g. contain W + 1 jet and W + 2 jet (i.e. real emission) kinematics. However, the merging scale cut aims at regularising the "underlying Born" configuration (i.e. the W + 1 states in our example). Setting Merging:nRequested = 1 for the W + 1 jet POWHEG sample ensures that even for real-emission (W + 2 jet) kinematics, the merging scale cut is applied to W + 1 jet states.

            After the cross section estimation step, main87.cc proceeds to perform the actual merging. Before explaining this part, we would like to make some comments about K-factors.

            main87.cc is prepared to use fixed K-factors to rescale the weight of tree-level events. This rescaling does not affect the NLO accuracy of the method, and was investigated in [Lon13]. By default, main87.cc does not use K-factors. However, if the user wants to include K-factors, this can be done by using the following input settings.

            Merging:kFactor0j   (default = 1.0)
            The k-Factor used to rescale the tree-level (i.e. CKKW-L or UMEPS) part of zero-jet tree-level events.

            Merging:kFactor1j   (default = 1.0)
            The k-Factor used to rescale the tree-level (i.e. CKKW-L or UMEPS) part of one-jet tree-level events.

            Merging:kFactor2j   (default = 1.0)
            The k-Factor used to rescale the tree-level (i.e. CKKW-L or UMEPS) part of two-jet tree-level events.

            If the variables k0, k1, k2 in main87.cc are set to non-unity values, K-factors will be applied. The K-factor of highest jet multiplicity will then be used to also rescale tree-level samples with a number of additional jets beyond the number of the highest-multiplicity real-emission sample. If we, for example, attempt an NLO merging of W+0 jet and W+1 jet at NLO accuracy, and with W+≤4 jets at tree-level accuracy, then Merging:kFactor2j is used to rescale the W+2 jet, W+3 jets and W+4 jets tree-level samples. We recommend to not include a K-factor rescaling of the tree-level samples.

            Let us turn to the production of NLO merged events. The first step in the procedure is to generate reweighted tree-level samples. This is implemented by using the following switch.

            Merging:doNL3Tree On Off   (default = off)
            This switch will allow the generation of the weight that should be applied to tree-level events in the NL3 merging scheme. Please note that, in order for this to work smoothly, the switch Merging:doNL3Loop and the switch Merging:doNL3Subt have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

            The weight of tree-level events can be accessed by calling the function double Info::mergingWeightNLO(). When printing (or histogramming) NLO merged events, this weight, multiplied with the estimated cross section of the current event sample, should be used as event weight (or weight of histogram bins). For Merging:doNL3Tree = on, the weight double Info::mergingWeightNLO() contains the CKKW-L weight, subtracted, if necessary, by αs0- and αs1-terms. This weight can become negative. As an example, imagine we attempt an NLO merging of W + 0 jet and W + 1 jet at NLO accuracy, and with W + 2 jets at tree-level accuracy. This weight will then be

              Info::mergingWeightNLO() = CKKW-L-weight for zero jets - αs0-terms - αs1-terms for events in the zero-jet sample,

              Info::mergingWeightNLO() = CKKW-L-weight for one jet - αs0-terms - αs1-terms for events in the one-jet sample, and

              Info::mergingWeightNLO() = CKKW-L-weight for two jets for events in the two-jet sample.

            After the tree-level events have been reweighted, main87.cc will move on to process the POWHEG NLO input. This is done by switching to the following flag.

            Merging:doNL3Loop On Off   (default = off)
            This switch will allow the processing of POWHEG NLO events in the NL3 merging scheme. Please note that, in order for this to work smoothly, the switch Merging:doNL3Tree and the switch Merging:doNL3Subt have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

            Also in this case, the NLO merging weight of the events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doNL3Loop = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in [Lon13]). After the processing of POWHEG NLO events, main87.cc continues by generating explicit phase space subtractions. This is facilitated by the following switch.

            Merging:doNL3Subt On Off   (default = off)
            This switch will allow the processing of tree-level events, to produce explicit phase space subtractions in the NL3 merging scheme. Please note that, in order for this to work smoothly, the switch Merging:doNL3Tree and the switch Merging:doNL3Loop have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested. Furthermore, it is necessary to set the value of Merging:nRecluster to one.

            These contributions are necessary because we have implemented the "inclusive scheme" of [Lon13] in Pythia. The benefit of this scheme is the user does not have to intrusively change the POWHEG-BOX program to implement very particular cuts. Let us explain this comment with an example (a more detailed explanation of the idea is given in Appendix A.2 of [Lon13]). When generating W + 0 jet events with the POWHEG-BOX program, the output LHE files will contain W + 1 jet real emission events. Some of these events will contain a jet above the merging scale. However, in NLO merging methods, such configurations have already been included by a separate W + 1 jet sample. Thus, to avoid counting such events twice, we have to remove the configurations from the POWHEG-BOX output. We choose to remove such events by explicit subtraction.

            As always, the NLO merging weight of the events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doNL3Subt = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in [Lon13]).

            After these steps, all necessary events for NL3 merging have been produced. main87.cc finishes by returning the NL3-merged total cross section.


            UNLOPS merging with main88.cc

            UNLOPS-style NLO merging in Pythia is illustrated by the sample main program main88.cc, which relies on an input file (e.g. main88.cmnd) for Pythia settings. As for all merging methods in Pythia, main88.cc requires LHE input files. To use main88.cc without any changes, these input files should follow the naming convention name_tree_#nAdditionalJets.lhe (for tree-level samples) and name_powheg_#nAdditionalJets.lhe (for POWHEG NLO samples). main88.cc produces HepMC event output, which can e.g. be analysed with RIVET, or used as input for detector simulations. For users not familiar with HepMC output, it is of course possible remove the HepMC code in the sample program, and use Pythia's histogramming routines instead. Histograms should then be filled as indicated for the histPTFirstSum histograms in main84.cc, i.e. using weightNLO*normhepmc.

            As for NL3, it is not necessary to change main88.cc if the user is only interested in changing standard settings. Thus, if the user only wants to change the number of requested events (Main:numberOfEvents), the hard process (Merging:Process), the merging scale value (Merging:TMS) and the maximal number of additional tree-level or NLO-accuracte jets (Merging:nJetMax and Merging:nJetMaxNLO, respectively), and HepMC output is desired, then there is no need to change the main88.cc code. The input LHE files are also part of the (command line) input for main88.exe. The default settings in main88.cmnd are intended to work with the (very short) sample LHEF inputs (w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and w_production_powheg_0.lhe, w_production_powheg_1.lhe). For these input files, the main88.exe executable can be run with the command

            ./main88.exe main88.cmnd w_production myhepmc.hepmc

            to produce a file myhepmc.hepmc of UNLOPS merged HepMC event output. Please refrain from adding input switches than invoke any other merging scheme (e.g. Merging:doKTMerging) into the input file that you want to use in conjunction with main88.cc.

            In the following, we will explain main88.cc in depth. To not be overly repetitive, we will at times refer to the relevant parts in the discussion of main87.cc. Users who are willing to accept the default choices do not need to know all details, but are still encouraged to read further.

            Program flow

            main88.cc can be divided into five steps:

                     1. Estimate the cross section for tree-level and NLO samples after the merging scale cut.

                     2. Produce reweighted tree-level events, which do not contain αs0- and αs1-terms.

                     3. Add POWHEG NLO events.

                     4. Subtract integrated, reweighted tree-level events, to ensure that the inclusive NLO cross section remains intact upon inclusion of multi-jet tree-level events.

                     5. Subtract integrated POWHEG NLO events, to ensure that the inclusive NLO cross section remains intact upon inclusion of multi-jet tree-level events.

            The estimation of cross sections after the application of the merging scale cut is nearly identical to the first step in main87.cc, and we refer to the first paragraph of the "Program flow" discussion for main87.cc for details. For main88.cc, the flags Merging:doUNLOPSTree or Merging:doUNLOPSLoop supply the merging scale definition used in the cross section estimation.

            After the cross section estimation step, main88.cc proceeds to perform the actual NLO merging. The discussion of K-factors given in the NL3 section (i.e. of Merging:kFactor0j, Merging:kFactor1j and Merging:kFactor2j) also applies to main88.cc. Although UNLOPS is considerably more stable than NL3 upon changing the K-factors, we do not recommend the use of K-factors.

            The production of UNLOPS-merged events with main88.cc starts by generating reweighted tree-level events. The processing of tree-level events can be invoked by setting the following flag.

            Merging:doUNLOPSTree On Off   (default = off)
            This switch will allow the generation of the weight that should be applied to tree-level events in the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSLoop, Merging:doUNLOPSSubt and Merging:doUNLOPSSubtNLO have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

            The weight of tree-level events is returned by the function double Info::mergingWeightNLO(). When printing (or histogramming) NLO merged events, this weight, multiplied with the estimated cross section of the current event sample, should be used as event weight (or weight of histogram bins). For Merging:doUNLOPSTree = on, the weight double Info::mergingWeightNLO() contains the UMEPS weight, subtracted, if necessary, by αs0- and αs1-terms. This weight can become negative. As an example, assume that we attempt an UNLOPS merging of W + 0 jet and W + 1 jet at NLO accuracy, and with W + 2 jets at tree-level accuracy. This weight will then be

              Info::mergingWeightNLO() = UMEPS-weight for one jet - αs0-terms - αs1-terms for events in the one-jet sample, and

              Info::mergingWeightNLO() = UMEPS-weight for two jets for events in the two-jet sample.

            After reweighted tree-level events have been generated, main88.cc processes the POWHEG NLO input files. This is facilitated by the following switch.

            Merging:doUNLOPSLoop On Off   (default = off)
            This switch will allow the processing of POWHEG NLO events in the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSTree, Merging:doUNLOPSSubt and Merging:doUNLOPSSubtNLO have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested.

            The NLO merging weight of the events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doUNLOPSLoop = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in [Lon13]).

            After processing the POWHEG NLO events, main88.cc continues by generating the reweighted subtraction terms of UMEPS. This part is implemented by setting the following flag.

            Merging:doUNLOPSSubt On Off   (default = off)
            This switch will allow the processing of tree-level events, to produce UMEPS subtraction terms for the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSTree, Merging:doUNLOPSLoop and Merging:doUNLOPSSubtNLO have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested. Furthermore, it is necessary to set the value of Merging:nRecluster to one.

            By using this switch, main88.cc ensures that the inclusive cross section is preserved. At variance with UMEPS however, the event weight contains the UMEPS weight, subtracted, if necessary, by αs+0- and αs1-terms. Otherwise, αsn+0- and αsn+1-terms of the UMEPS procedure would be introduced, although our goal is to describe all αsn+0- and αsn+1-terms by n-jet POWHEG input. The weight of these integrated, subtractive tree-level events is, as always, returned by the function double Info::mergingWeightNLO(). When printing (or histogramming) NLO merged events, this weight, multiplied with the estimated cross section of the current event sample, and with -1, should be used as event weight (or weight of histogram bins). As for the case of tree-level events in UNLOPS, this weight can become negative. For the example given before, i.e. attempting an UNLOPS merging of W + 0 jet and W + 1 jet at NLO accuracy, and with W + 2 jets at tree-level accuracy, this weight will be

              Info::mergingWeightNLO() = UMEPS-weight for the integrated one-jet sample - αs0-terms - αs1-terms for events in the integrated one-jet sample, and

              Info::mergingWeightNLO() = UMEPS-weight for the integrated two-jet sample for events in the integrated two-jet sample.

            This choice of weights already incorporates the fact that we have implemented the "inclusive scheme" of [Lon13], meaning that the "explicit phase space subtractions" of NL3 are (partially) included though these weights.

            To ensure that the NLO inclusive cross section is unchanged, UNLOPS further requires the introduction of another sample. If POWHEG NLO events with one or more jets are included, it is necessary to subtract these samples in an integrated form. In main88.cc, this is done by setting the following flag.

            Merging:doUNLOPSSubtNLO On Off   (default = off)
            This switch will allow the processing of POWHEG NLO events, to produce NLO subtraction terms for the UNLOPS merging scheme. Please note that, in order for this to work smoothly, the switches Merging:doUNLOPSTree, Merging:doUNLOPSLoop and Merging:doUNLOPSSubt have to be turned off. As for the estimation of cross sections, it is mandatory to set the correct value of Merging:nRequested. Furthermore, it is necessary to set the value of Merging:nRecluster to one.

            This sample also provides some "explicit phase space subtractions" of NL3, which are necessary because we implemented the "inclusive scheme" of [Lon13]. Let us again look at the example of UNLOPS merging of W + 0 jet and W + 1 jet at NLO accuracy. The integrated W + 1 jet NLO events, which are produced by the setting Merging:doUNLOPSSubtNLO = on, contain a tree-level part. This part will exactly cancel the real-emission events with one jet above the merging scale in the W + 0 jet NLO events.

            The NLO merging weight of these "integrated" events can be accessed by calling the function double Info::mergingWeightNLO(). This weight should also be used when printing (or histogramming) events. For Merging:doUNLOPSSubtNLO = on, the weight double Info::mergingWeightNLO() is either one or zero (see Appendix E in [Lon13]).

            After these five steps (estimation of cross sections, tree-level processing, POWHEG processing, integrated tree-level processing, integrated POWHEG processing) we have produced a UNLOPS-merged HepMC event file. main88.cc finishes by returning the UNLOPS-merged total cross section.


            NLO merging and "exclusive" NLO inputs

            Currently, both sample main programs for NLO merging (main87.cc and main88.cc) are intended for "inclusive" POWHEG input. Inclusive input means that all real emission phase space points are included in the POWHEG output files. In order to avoid double counting with higher-multiplicity matrix elements, it is then necessary remove phase space points with too many jets from the real-emission configurations. This can be done by introducing explicit phase space subtractions. Another way of removing the undesired configurations is by implementing a cut in the NLO generator. This is not a completely trivial task, since it is necessary to ensure numerical stability and the correct cancellation of (finite) dipole regularisation terms. One way of producing such exclusive NLO output is by setting the (tree-level) real-emission matrix element in the NLO generator to zero if the real-emission phase space point contains too many jets above the merging scale. This will however not be numerically stable for too low merging scale values.

            We should be very clear that using exclusive NLO input is not recommended, since it requires hacking the NLO generator. Only for the expert user, we briefly summarise the necessary changes for using exclusive NLO input.

            For the moment, assume that the NLO input has been produced in an "exclusive" way. This input can then be processed by some trivial changes in main87.cc: estimate the cross section for tree-level and NLO samples after the merging scale cut, still using inclusive NLO samples, remove the last part of main87.cc, i.e. the part that produces explicit phase space subtractions, and use the exclusive NLO files as input files for the processing of "POWHEG NLO files".

            The changes to main88.cc (implementing UNLOPS) are slightly more complicated. This is the case because the weights of integrated tree-level samples change when using exclusive input, as can be seen in Appendix D in [Lon13]. The correct weights can be produced by Pythia by using the following flag.

            Merging:doUNLOPSTilde On Off   (default = off)
            This flag allows the UNLOPS machinery to produce the event weights if exclusive NLO input is used for the merging. This flag should be set to "on" directly after the cross section estimates have been produced.

            Then, it is necessary to add code for processing another sample to main88.cc, since when using exclusive inputs, it is also necessary to enforce two integrations on tree-level events (the "↑"-contributions in Appendix D of [Lon13]). This can be achieved by adding the following code at the end of main88.cc.

              cout << endl << endl << endl;
              cout << "Shower subtractive events" << endl;
            
              // Switch on processing of counter-events.
              pythia.settings.flag("Merging:doUNLOPSTree",false);
              pythia.settings.flag("Merging:doUNLOPSLoop",false);
              pythia.settings.flag("Merging:doUNLOPSSubt",true);
              pythia.settings.flag("Merging:doUNLOPSSubtNLO",false);
              pythia.settings.mode("Merging:nRecluster",2);
            
              nMaxCT         = nMaxNLO+1;
              njetcounterCT  = nMaxCT;
              iPathSubt      = iPath + "_tree";
            
              while(njetcounterCT >= 2){
            
                // From njet, choose LHE file
                stringstream in;
                in   << "_" << njetcounterCT << ".lhe";
                string LHEfile = iPathSubt + in.str();
            
                cout << endl << endl << endl
                     << "Start subtractive treatment for " << njetcounterCT << " jets\n"
                     << "Recluster at least 2 times" << endl;
            
                pythia.readString("Beams:frameType = 4"); 
                pythia.settings.word("Beams:LHEF", LHEfile);  
                pythia.settings.mode("Merging:nRequested", njetcounterCT);
                pythia.init();
                // Remember position in vector of cross section estimates.
                int iNow = sizeLO-1-njetcounterCT;
            
                // Start generation loop
                for( int iEvent=0; iEvent < nEvent; ++iEvent ){
            
                  // Generate next event
                  if( !pythia.next() ) {
                    if( pythia.info.atEndOfFile() ) break;
                    else continue;
                  }
            
                  // Get event weight(s).
                  double weightNLO  = pythia.info.mergingWeightNLO();
                  double evtweight  = pythia.info.weight();
                  weightNLO        *= evtweight;
                  // Do not print zero-weight events.
                  if ( weightNLO == 0. ) continue; 
            
                  // Construct new empty HepMC event.
                  HepMC::GenEvent* hepmcevt = new HepMC::GenEvent();
                  // Get correct cross section from previous estimate.
                  double normhepmc = -1*xsecLO[iNow] / nAcceptLO[iNow];
                  // Set hepmc event weight.
                  hepmcevt->weights().push_back(weightNLO*normhepmc);
                  // Fill HepMC event.
                  ToHepMC.fill_next_event( pythia, hepmcevt );
                  // Add the weight of the current event to the cross section.
                  sigmaTotal += weightNLO*normhepmc;
                  errorTotal += pow2(weightNLO*normhepmc);
                  // Report cross section to hepmc.
                  HepMC::GenCrossSection xsec;
                  xsec.set_cross_section( sigmaTotal*1e9, pythia.info.sigmaErr()*1e9 );
                  hepmcevt->set_cross_section( xsec );
                  // Write the HepMC event to file. Done with it.
                  ascii_io << hepmcevt;
                  delete hepmcevt;
            
                } // end loop over events to generate
            
                // print cross section, errors
                pythia.stat();
            
                // Restart with ME of a reduced the number of jets
                if( njetcounterCT > 2 )
                  njetcounterCT--;
                else
                  break;
            
              }
            
            "?>
            pythia8-8.1.80.orig/phpdoc/ImplementNewShowers.php0000644000175000017500000007062012217615312020303 0ustar sunsun Implement New Showers SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Implement New Showers

            In case you want to replace the PYTHIA initial- and final-state showers by your own, it is possible but not trivial. The point is that multiparton interactions (MPI), initial-state radiation (ISR) and final-state radiation (FSR) in general appear in one single interleaved sequence of decreasing pT values. Therefore shower replacements would have to be able to play the game by such rules, as we will outline further below. Of course, this still leaves the field open exactly how to define what to mean by pT, how to handle recoil effects, how the colour flow is affected, and so on, so there is certainly room for alternative showers. A first example of a shower implemented within the PYTHIA context is VINCIA, which however so far only handles FSR.

            For the moment we assume you want to keep the MPI part of the story unchanged, and make use of the existing beam-remnants (BR) machinery. If you want to replace both MPI, ISR, FSR and BR then you had better replace the whole PartonLevel module of the code. If, in addition, you want to produce your own hard processes, then you only need the ";?>hadron-level standalone part of the machinery.

            In order to write replacement codes for ISR and/or FSR it is useful to be aware of which information has to be shared between the different components, and which input/output structure is required of the relevant methods. For details, nothing beats studying the existing code. However, here we provide an overview, that should serve as a useful introduction.

            It should be noted that we here primarily address the problem in its full generality, with interleaved MPI, ISR and FSR. There exists an option TimeShower:interleave = off where only MPI and ISR would be interleaved and FSR be considered after these two, but still before BR. Most of the aspects described here would apply also for that case. By contrast, resonance decays are only considered after all the four above components, and timelike showers in those decays would never be interleaved with anything else, so are much simpler to administrate.

            Therefore the ";?> pythia.setShowerPtr( timesDecPtr, timesPtr, spacePtr) method allows two separate pointers to be set to instances of derived TimeShower classes. The first is only required to handle decays, say of Z^0 or Upsilon, with no dependence on beam remnants or ISR. The second, as well as spacePtr, has to handle the interleaved evolution of MPI, ISR and FSR. Therefore you are free to implement only the first, and let the PYTHIA default showers take care of the latter two. But, if you wanted to, you could also set timesDecPtr = 0 and only provide a timesPtr, or only a spacePtr. If your timelike shower does both cases, the first two pointers can agree. The only tiny point to take into account then is that init( beamAPtr, beamBPtr) is called twice, a first time to timesDecPtr with beam pointers 0, and a second time to timesPtr with nonvanishing beam pointers.

            The event record and associated information

            Obviously the main place for sharing information is the event record, specifically the Event event member of Pythia, passed around as a reference. It is assumed you already studied how it works, so here we only draw attention to a few aspects of special relevance.

            One basic principle is that existing partons should not be overwritten. Instead new partons should be created, even when a parton only receives a slightly shifted momentum and for the rest stays the same. Such "carbon copies" by final-state branchings should be denoted by both daughter indices of the original parton pointing to the copy, and both mother indices of the copy to the original. If the copy instead is intended to represent an earlier step, e.g. in ISR backwards evolution, the role of mothers and daughters is interchanged. The event.copy( iCopy, newStatus) routine can take care of this tedious task; the sign of newStatus tells the program which case to assume.

            To make the event record legible it is essential that the ";?>status codes are selected appropriately to represent the reason why each new parton is added to the record. Also remember to change the status of a parton to be negative whenever an existing parton is replaced by a set of new daughter partons.

            Another important parton property is scale(), which does not appear in the normal event listing, but only if you use the extended Event:listScaleAndVertex = on option. This property is supposed to represent the production scale (in GeV) of a parton. In the current FSR and ISR algorithms it is used to restrict from above the allowed pT values for branchings of this particular parton. Beam remnants and other partons that should not radiate are assigned scale 0.

            Auxiliary to the event record proper is the ";?>PartonSystems class, that keep track of which partons belong together in the same scattering subsystem. This information must be kept up-to-date during the shower evolution.

            For initial-state showers it is also necessary to keep track of the partonic content extracted from the beams. This information is stored in the ";?>BeamParticle class.

            The TimeShower interface

            If you want to replace the TimeShower class this would involve replacing the virtual methods among the following ones.

            TimeShower::TimeShower()  
            The constructor does not need to do anything.

            virtual TimeShower::~TimeShower()  
            The destructor does not need to do anything.

            void TimeShower::initPtr(Info* infoPtr, Settings* settingsPtr, ParticleData* particleDataPtr, Rndm* rndmPtr, CoupSM* coupSMPtr, PartonSystems* partonSystemsPtr, UserHooks* userHooksPtr)  
            This method only imports pointers to standard facilities, and is not virtual.

            virtual void TimeShower::init( BeamParticle* beamAPtrIn = 0, BeamParticle* beamBPtrIn = 0)  
            You have to store your local copy of the pointers to these objects, since they have to be used during the generation, as explained above. The pointers could be zero; e.g. a local copy of TimeShower is created to handle showers in decays such as Upsilon -> q qbar from inside the ParticleDecays class. This is also the place to do initialization of whatever parameters you plan to use, e.g. by reading in them from a user-accessible database like the Settings one.

            virtual bool TimeShower::limitPTmax( Event& event, double Q2Fac = 0., double Q2Ren = 0.)  
            The question is whether the FSR should be allowed to occur at larger scales than the hard process it surrounds. This is process-dependent, as illustrated below for the the analogous SpaeShower::limitPTmax(...) method, although the two kinds of radiation need not have to be modeled identically. The TimeShower:pTmaxMatch switch allows you to force the behaviour among three options, but you may replace by your own logic.
            The internal PYTHIA implementation also allows intermediate options, where emissions can go up to the kinematical limit but be dampened above the factorization or renormalization scale. Therefore the (square of the) latter two are provided as optional input parameters.

            double TimeShower::enhancePTmax()  
            Relative to the default pT_max evolution scale of the process, it may still be convenient to vary the matching slightly for the hardest interaction in an event, to probe the sensitivity to such details. The base-class implementation returns the value of the TimeShower:pTmaxFudge parameter.

            virtual int TimeShower::shower( int iBeg, int iEnd, Event& event, double pTmax, int nBranchMax = 0)  
            This is an all-in-one call for shower evolution, and as such cannot be used for the normal interleaved evolution, where only the routines below are used. It also cannot be used in resonance decays that form part of the hard process, since there the ";?>user hooks insert a potential veto step. Currently this routine is therefore only used in the hadron-level decays, e.g. Upsilon -> g g g.
            iBeg and iEnd is the position of the first and last parton of a separate system, typically produced by a resonance decay. Such a system only evolves in isolation, and in particular does not relate to the beams.
            The pTmax value sets the maximum scale for evolution, but normally you would restrict that further for each individual parton based on its respective scale value.
            The nBranchMax value, if positive, gives the maximum number of allowed branchings in the call, as useful for matching studies.
            The routine is expected to return the number of FSR branchings that were generated, but only for non-critical statistics purposes.
            Since the real action typically is delegated to the routines below, it may well be that the existing code need not be replaced.

            virtual int TimeShower::showerQED( int iBeg, int iEnd, Event& event, double pTmax)  
            This is a further simplified version of the shower method above. Currently it only handles the emission of photons in the decay of a hadron into a pair of leptons, either a charged lepton-antilepton or a lepton-neutrino pair. It is properly matched to the matrix element in the decay via a virtual photon or W^+-, respectively. It is called as part of such decays if ParticleDecays:allowPhotonRadiation = on, which is not the default value.

            double TimeShower::pTLastInShower()  
            Can be used to return the pT evolution scale of the last branching in the cascade generated with the above shower(...) method. Is to be set in the internal pTLastInShower variable, and should be 0 if there were no branchings. Can be useful for matching studies.

            virtual void TimeShower::prepareGlobal( Event& event)  
            This method resets some counters and extracts the locations of outgoing partons, in preparation of using the optional global recoil scheme. Unlike prepare(...) below it is only called once during the parton-level evolution, since it only relates to the hardest interaction. Is probably of no use to most people.

            virtual void TimeShower::prepare( int iSys, Event& event, bool limitPTmaxIn = true, double pTfirstTrialIn = 1e9)  
            This method is called immediately after a new interaction (or the products of a resonance decay) has been added, and should then be used to prepare the subsystem of partons for subsequent evolution. In the current code this involves identifying all colour and charge dipole ends: the position of radiating and recoiling partons, maximum pT scales, possible higher-order matrix elements matchings to apply, and so on.
            The iSys parameter specifies which parton system is to be prepared. It is used to extract the set of partons to be treated, with rules as described in the above section on subsystems. Specifically, the first two partons represent the incoming state, or are 0 for resonance decays unrelated to the beams, while the rest are not required to be in any particular order.
            The limitPTmaxIn switch conveys the choice made on maximum scale for the dipole-ends evolution associated with the hard interaction of the event (while scales for subsequent MPIs by default are set to respect pT ordering). If true then this scale is set by the user choice options, see the TimeShower::limitPTmax method above, while if false emissions are allowed to go up to the kinematical limit. For the two-hard-interactions scenario, the two class variables dopTlimit1 and dopTlimit2 instead convey the choice made.
            The pTfirstTrialIn parameter is tentatively used in the new weak-shower part of the code. It is related to the option to shift the weak-shower evolution scale up by (some factor times) the gauge boson mass, without this backfiring on the QCD/QED evolution. Still under evolution, and normally not used.

            virtual void TimeShower::rescatterUpdate( int iSys, Event& event)  
            This method is called immediately after rescattering in the description of multiparton interactions. Thus the information on one or several systems is out-of-date, while that of the others is unchanged. We do not provide the details here, since we presume few implementors of new showers will want to touch the technicalities involved in obtaining a description of rescattering.

            virtual void TimeShower::update( int iSys, Event& event)  
            This method is called immediately after a spacelike branching in the iSys'th subsystem. Thus the information for that system is out-of-date, while that of the others is unchanged. If you want, you are free to throw away all information for the affected subsystem and call prepare( iSys, event) to create new one. Alternatively you may choose only to update the information that has changed.

            virtual double TimeShower::pTnext( Event& event, double pTbegAll, double pTendAll, bool isFirstTrialIn = false)  
            This is the main driver routine for the downwards evolution. A new pT is to be selected based on the current information set up by the routines above, and along with that a branching parton or dipole. The pTbegAll scale is the maximum scale allowed, from which the downwards evolution should be begun (usually respecting the maximum scale of each individual parton). If no emission is found above pTendAll (and above the respective shower cutoff scales) then 0. should be returned and no emissions will be allowed. Both scales can vary from one event to the next: if a scale has already been selected for MPI or ISR it makes no sense to look for a scale smaller than that from FSR, since it would not be able to compete, so pTendAll is set correspondingly. As it happens, FSR is tried before ISR and MPI in the interleaved evolution, but this is an implementation detail that could well change.
            Typically the implementation of this routine would be to set up a loop over all possible radiating objects (dipoles, dipole ends, ...), for each pick its possible branching scale and then pick the one with largest scale as possible winner. At this stage no branching should actually be carried out, since MPI, ISR and FSR still have to be compared to assign the winner.
            The isFirstTrialIn is true only for the very first emission, and can then optionally be used to switch the weak-shower evolution scale up by (some factor times) the gauge boson mass.

            virtual bool TimeShower::branch( Event& event, bool isInterleaved = false)  
            This method will be called once FSR has won the competition with MPI and ISR to do the next branching. The candidate branching found in the previous step should here be carried out in full. The pre-branching partons should get a negative status code and new replacement ones added to the end of the event record. Also the subsystem information should be updated, and possibly also the beams.
            Should some problem be encountered in this procedure, e.g. if some not-previously-considered kinematics requirement fails, it is allowed to return false to indicate that no branching could be carried out.
            Normally the optional isInterleaved argument would not be of interest. It can be used to separate resonance decays, false, from the interleaved evolution together with MPI and ISR, true. More precisely, it separates calls to the timesDecPtr and the timesPtr instances.

            virtual bool TimeShower::rescatterPropogateRecoil( Event& event, Vec4& pNew)  
            This method is only called if rescattering is switched on in the description of multiparton interactions. It then propagates a recoil from a timelike branching to internal lines that connect systems. As for rescatterUpdate above, this is not likely to be of interest to most implementors of new showers.

            int TimeShower::system()  
            This method is not virtual. If a branching is constructed by the previous routine this tiny method should be able to return the number of the selected subsystem iSysSel where it occurred, so that the spacelike shower can be told which system to update, if necessary. Therefore iSysSel must be set in branch (or already in pTnext).

            virtual void TimeShower::list( ostream& os = cout)  
            This method is not at all required. In the current implementation it outputs a list of all the dipole ends, with information on the respective dipole. The routine is not called anywhere in the public code, but has been inserted at various places during the development/debug phase.

            The SpaceShower interface

            If you want to replace the SpaceShower class this would involve replacing the virtual methods in the following. You will find that much of the story reminds of TimeShower above, and actually some cut-and-paste of text is involved. In some respects the description is simpler, since there are no special cases for resonance decays and non-interleaved evolution. Thus there is no correspondence to the TimeShower::shower(...) routine.

            SpaceShower::SpaceShower()  
            The constructor does not need to do anything.

            virtual SpaceShower::~SpaceShower()  
            Also the destructor does not need to do anything.

            void SpaceShower::initPtr(Info* infoPtrIn, Settings* settingsPtrIn, ParticleData* particleDataPtrIn, Rndm* rndmPtrIn, CoupSM* coupSMPtrIn, PartonSystems* partonSystemsPtrIn, UserHooks* userHooksPtrIn, MergingHooks* mergingHooksPtrIn = 0)  
            This method only imports pointers to standard facilities, and is not virtual.

            virtual void SpaceShower::init(BeamParticle* beamAPtrIn, BeamParticle* beamBPtrIn)  
            You have to store your local copy of the pointers to these objects, since they have to be used during the generation, as explained above. This is also the place to do initialization of whatever parameters you plan to use, e.g. by reading in them from a user-accessible database like the Settings one.

            virtual bool SpaceShower::limitPTmax( Event& event, double Q2Fac = 0., double Q2Ren = 0.)  
            The question is whether the ISR should be allowed to occur at larger scales than the hard process it surrounds. This is process-dependent. For instance, if the hard process is Z^0 production we know that ISR should be allowed to go right up to the kinematical limit. If it is a 2 -> 2 QCD process the ISR should not exceed the scale of the hard process, since if so one would double-count. The SpaceShower:pTmaxMatch switch allows you to force the behaviour, or else to program your own logic. The current default implementation limits pT whenever the final state contains a quark (except top), gluon or photon, since then the danger of double-counting is there. You may replace by your own logic, or leave as is.
            The internal PYTHIA implementation also allows intermediate options, where emissions can go up to the kinematical limit but be dampened above the factorization or renormalization scale. Therefore the (square of the) latter two are provided as optional input parameters.

            virtual double SpaceShower::enhancePTmax()  
            When the above method limits pT_max to the scale of the process, it may still be convenient to vary the matching slightly for the hardest interaction in an event, to probe the sensitivity to such details. The base-class implementation returns the value of the SpaceShower:pTmaxFudge parameter.

            virtual void SpaceShower::prepare( int iSys, Event& event, bool limitPTmaxIn = true, double pTfirstTrialIn = 1e9)  
            This method is called immediately after a new interaction has been added, and should then be used to prepare the subsystem of partons for subsequent evolution. In the current code this involves identifying the colour and charge dipole ends: the position of radiating and recoiling partons, maximum pT scales, and possible higher-order matrix elements matchings to apply. Depending on what you have in mind you may choose to store slightly different quantities. You have to use the subsystem information described above to find the positions of the two incoming partons (and the outgoing ones) of the system, and from there the scales at which they were produced.
            The limitPTmax input agrees with the output of the previous method for the hardest process, and is always true for subsequent MPI, since there an unlimited pT for sure would lead to double-counting.
            The pTfirstTrialIn parameter is tentatively used in the new weak-shower part of the code. It is related to the option to shift the weak-shower evolution scale up by (some factor times) the gauge boson mass, without this backfiring on the QCD/QED evolution. Still under evolution, and normally not used.

            virtual void SpaceShower::update( int iSys, Event& event)  
            This method is called immediately after a timelike branching in the iSys'th subsystem. Thus the information for that system may be out-of-date, and to be updated. For the standard PYTHIA showers this routine does not need to do anything, but that may be different in another implementation.

            virtual double SpaceShower::pTnext( Event& event, double pTbegAll, double pTendAll, int nRadIn = -1, bool isFirstTrial = false)  
            This is the main driver routine for the downwards evolution. A new pT is to be selected based on the current information set up by the routines above, and along with that a branching parton or dipole. The pTbegAll scale is the maximum scale allowed, from which the downwards evolution should be begun (usually respecting the maximum scale of each individual parton). If no emission is found above pTendAll (and above the respective shower cutoff scales) then 0. should be returned and no emissions will be allowed. Both scales can vary from one event to the next: if a scale has already been selected for MPI or ISR it makes no sense to look for a scale smaller than that from FSR, since it would not be able to compete, so pTendAll is set correspondingly. As it happens, FSR is tried before ISR and MPI in the interleaved evolution, but this is an implementation detail that could well change.
            Typically the implementation of this routine would be to set up a loop over all possible radiating objects (dipoles, dipole ends, ...), for each pick its possible branching scale and then pick the one with largest scale as possible winner. At this stage no branching should actually be carried out, since MPI, ISR and FSR still have to be compared to assign the winner.
            The input nRadIn provides the total number of ISR and FSR emissions already generated in the event, and so allows a special treatment for the very first emission, if desired.
            The isFirstTrialIn is true only for the very first emission, and can then optionally be used to switch the weak-shower evolution scale up by (some factor times) the gauge boson mass.

            virtual bool SpaceShower::branch( Event& event)  
            This method will be called once ISR has won the competition with MPI and FSR to do the next branching. The candidate branching found in the previous step should here be carried out in full. The pre-branching partons should get a negative status code and new replacement ones added to the end of the event record. Also the subsystem information should be updated, and possibly also the beams.
            Should some problem be encountered in this procedure, e.g. if some not-previously-considered kinematics requirement fails, it is allowed to return false to indicate that no branching could be carried out. Also a complete restart of the parton-level description may be necessary, see doRestart() below.

            int SpaceShower::system()  
            This method is not virtual. If a branching is constructed by the previous routine this tiny method should be able to return the number of the selected subsystem iSysSel where it occurred, so that the spacelike shower can be told which system to update, if necessary. Therefore iSysSel must be set in branch (or already in pTnext).

            bool SpaceShower::doRestart()  
            This method is not virtual. If branch(...) above fails to construct a branching, and the conditions are such that the whole parton-level description should be restarted, then it should return true, else not. Currently only the rescattering description can give this kind of failures, and so the internal rescatterFail boolean must be set true when this should happen, and else false.

            virtual void SpaceShower::list( ostream& os = cout)  
            This method is not at all required. In the current implementation it outputs a list of all the dipole ends, with information on the respective dipole. The routine is not called anywhere in the public code, but has been inserted at various places during the development/debug phase. pythia8-8.1.80.orig/phpdoc/Version.php0000644000175000017500000000267112217615312015752 0ustar sunsun Version SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Version

            The settings on this page should not be changed by the ordinary user, but appear here for documentation purposes, and so that they can form part of the standard databases and be queried accordingly.

            parm  Pythia:versionNumber   (default = 8.180)
            Version and subversion number, with three significant decimals.

            mode  Pythia:versionDate   (default = 20130922)
            Last date of change of current (sub)version, in format yyyymmdd. pythia8-8.1.80.orig/phpdoc/pythia99.gif0000644000175000017500000000535312217346241015765 0ustar sunsunGIF89acd3̙3f33f333!,cdI8E^ aa@blrEN;0D;UB9OIr+2(s8tGNT@BB='}t^\B{=yZWDWDi9=e){5Vn'WQ=,,iq_6*Ƅ,NĔ:a|uTXҚ w-*1VTNזn> ! RC2Rk? AX6qJL)woU?Ҙ`J Ґ2>[EUCApCDME Ϊg""ةXrYZW.|H72 RE+@w2F!mh*Z],Z7ǰ݇dIjBs@j8׃=FEZ3tődZ`((-Q &A7 X"bo^vFr#PꅖIdOi ":_VK\ ~uLj?.,N|n8T-h̀%S ^B 80L.cF7ǼdGY guD[<^:OQZ&ICKLE!0^q(fυF!Pdɋ3$0wJsDk o)/-dz0:%~R2XT,VY藆6Ox*b+YbKcAdw1˼!i`%,699mhG#"[NM-@dyCjLqO`&'|5IY̫M{,@ҷ"8B*لd%d jwG @'͚(̕H\v3a/YDS"\L.ƌW"wxՒwYUN>Bs 9iQަǪv` &c>W`mG]5c ^%p Ɲ$+z9e(MjҰ_ 2:qpƩ}^bS`0NRqFoVEa #K[@kMTz_RW2j dkAL$r;qd4pr+1W$?@ v)M>2'ҵUHTSAaѸ.I9b7[Y \~8<=Gy4!ռ!.xP/)X0Qzk'8׎ Y'RJ蔤Yroߤx%8lf몥r7@(Yv2ݖ#0A&Qi(,e/y3 ժR>Ba  @^'s^X` w[m&&ԼO Kds_ +$Á]C`SB@9;a&aPL }E1Gwv.ƪi)p1c,^Nk?]0&.mE!&b)^B>+-E'&f*;?YE$8C0·FY!t炢 #%.mUSpAӘ֙"C~{BQia|E144|cH`ڈBn}SD 1zѡc8+A7~~-0VgpFO=`,wytpx 2V p9SP*QbC]Vxp6|G``u&A1Q́-hc9($NE8C3FXOX[cuQHkWx.YYY; pythia8-8.1.80.orig/phpdoc/COPYING0000644000175000017500000004310312217346233014645 0ustar sunsun GNU GENERAL PUBLIC LICENSE Version 2, June 1991 Copyright (C) 1989, 1991 Free Software Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA Everyone is permitted to copy and distribute verbatim copies of this license document, but changing it is not allowed. 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            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Histograms

            The Hist class gives a simple implementation of one-dimensional histograms, useful for quick-and-dirty testing, without the need to link to more sophisticated packages. For this reason it is used in many of the ";?>sample main programs found in the examples subdirectory.

            Basic principles

            We here provide a simple overview of what is involved. As a first step you need to declare a histogram, with name, title, number of bins and x range (from, to).
               Hist ZpT( "Z0 pT spectrum", 100, 0., 100.);
            
            Alternatively you can first declare it and later define it:
               Hist ZpT;
               ZpT.book( "Z0 pT spectrum", 100, 0., 100.);
            
            Once declared, its contents can be added by repeated calls to fill,
               ZpT.fill( 22.7, 1.); 
            
            where the first argument is the x value and the second the weight. Since the weight defaults to 1 the last argument could have been omitted in this case.

            A set of overloaded operators have been defined, so that histograms can be added, subtracted, divided or multiplied by each other. Then the contents are modified accordingly bin by bin. Thus the relative deviation between two histograms data and theory can be found as

              diff = (data - theory) / (data + theory);
            
            assuming that diff, data and theory have been booked with the same number of bins and x range. That responsibility rests on the user; some checks are made for compatibility, but not enough to catch all possible mistakes.

            Also overloaded operations with double real numbers are available. Again these four operations are defined bin by bin, i.e. the corresponding amount is added to, subtracted from, multiplied by or divided by each bin. The double number can come before or after the histograms, with obvious results. Thus the inverse of a histogram result is given by 1. / result. The two kind of operations can be combined, e.g.

              allpT = ZpT + 2. * WpT
            
            Finally, also the +=, -+, *=, /= are overloaded, with the right-hand side being either a histogram or a real number.

            Output format

            A histogram can be printed by making use of the overloaded << operator, e.g.:

               cout << ZpT;
            
            The printout format is inspired by the old HBOOK one. To understand how to read this format, consider the simplified example
                                                
                    3.50*10^ 2  9                     
                    3.00*10^ 2  X   7               
                    2.50*10^ 2  X  1X               
                    2.00*10^ 2  X6 XX                
                    1.50*10^ 2  XX5XX                 
                    1.00*10^ 2  XXXXX                
                    0.50*10^ 2  XXXXX        
            
                      Contents 
                        *10^ 2  31122
                        *10^ 1  47208
                        *10^ 0  79373
            
                      Low edge  -- 
                        *10^ 1  10001 
                        *10^ 0  05050
            
            The key feature is that the Contents and Low edge have to be read vertically. For instance, the first bin has the contents 3 * 10^2 + 4 * 10^1 + 7 * 10^0 = 347. Correspondingly, the other bins have contents 179, 123, 207 and 283. The first bin stretches from -(1 * 10^1 + 0 * 10^0) = -10 to the beginning of the second bin, at -(0 * 10^1 + 5 * 10^0) = -5.

            The visual representation above the contents give a simple impression of the shape. An X means that the contents are filled up to this level, a digit in the topmost row the fraction to which the last level is filled. So the 9 of the first column indicates this bin is filled 9/10 of the way from 3.00*10^2 = 300 to 3.50*10^2 = 350, i.e. somewhere close to 345, or more precisely in the range 342.5 to 347.5.

            The printout also provides some other information, such as the number of entries, i.e. how many times the histogram has been filled, the total weight inside the histogram, the total weight in underflow and overflow, and the mean value and root-mean-square width (disregarding underflow and overflow). The mean and width assumes that all the contents is in the middle of the respective bin. This is especially relevant when you plot a integer quantity, such as a multiplicity. Then it makes sense to book with limits that are half-integers, e.g.

               Hist multMPI( "number of multiparton interactions", 20, -0.5, 19.5);
            
            so that the bins are centered at 0, 1, 2, ..., respectively. This also avoids ambiguities which bin gets to be filled if entries are exactly at the border between two bins. Also note that the fill( xValue) method automatically performs a cast to double precision where necessary, i.e. xValue can be an integer.

            The methods

            We here collect a more complete and formal overview of the methods.

            Hist::Hist()  
            declare a histogram, but does not define it.

            Hist::Hist(string title, int numberOfBins, double xMin, double xMax)  
            declare and define a histogram, where
            argument title : is a string with the title of the histogram at output,
            argument numberOfBins : is the number of bin the x range will be subdivided into, limited to be at most 1000,
            argument xMin : is the lower edge of the histogram,
            argument xMax : is the upper edge of the histogram.

            Hist::Hist(const Hist& h)  
            creates an identical copy of the histogram in the argument, including bin contents.

            Hist::Hist(string title, const Hist& h)  
            creates an identical copy of the histogram in the argument, including bin contents, except that a new title is provided as first argument.

            Hist& Hist::operator=(const Hist& h)  
            copies all properties of the histogram in the argument, except that the original histogram title is retained.

            void Hist::book(string title, int numberOfBins, double xMin, double xMax)  
            define a histogram that previously was only declared; see above for the meaning of the arguments.

            void Hist::name(string title)  
            change the title of a histogram, but keep other properties unchanged.

            void Hist::null()  
            reset bin contents, but keep other histogram properties unchanged.

            void Hist::fill(double xValue, double weight)  
            fill the histogram, where
            argument xValue : is the x position where the filling should occur, and
            argument weight (default = 1.) : is the amount of weight to be added at this x value.

            friend ostream& operator<<(ostream& os, const Hist& h)  
            appends a simple histogram printout (see above for format) to the ostream, while leaving the histogram object itself unchanged. At most 100 columns are allowed to be displayed. If the number of bins is larger than 100 then the contents of adjacent bins are added to give the value in each column. (Two by two up to 200 bins, three by three up to 300, and so on, with the very last column possibly summing fewer rows than the others.)

            void Hist::table(ostream& os = cout)  
            void Hist::table(string fileName)  
            print a two-column table, where the first column gives the center of each bin and the second one the corresponding bin contents. The desired output stream or file name can be provided as argument. The former is more flexible (e.g., it allows easy append to an existing file), whereas the latter is simpler for the case that each histogram should be a file of its own. The table may be useful for plotting e.g. with Gnuplot.

            friend void table(const Hist& h1, const Hist& h2, ostream& os = cout)  
            friend void table(const Hist& h1, const Hist& h2, string fileName)  
            print a three-column table, where the first column gives the center of each bin and the second and third ones the corresponding bin contents of the two histograms. Only works if the two histograms have the same x axis (within a tiny tolerance), else nothing will be done.

            double Hist::getBinContent(int iBin)  
            return the value in bin iBin, ranging from 1 through numberOfBins, with 0 for underflow and numberOfBins + 1 for overflow.

            int Hist::getEntries()  
            return the number of entries, i.e. the number of time that fill(...) has been called.

            bool Hist::sameSize(const Hist& h)  
            checks that the number of bins and upper and lower limits are the same as in the histogram in the argument.

            void Hist::takeLog(bool tenLog = true)  
            by default take 10-logarithm of current contents bin by bin. With optional argument false instead take e-logarithm of contents bin by bin. If to be used, then right before the histogram is output.

            void Hist::takeSqrt()  
            take square root of current contents bin by bin, with negative contents set to zero.

            Hist& Hist::operator+=(const Hist& h)  
            Hist& Hist::operator-=(const Hist& h)  
            adds or subtracts the current histogram by the contents of the histogram in the argument if sameSize(...) is true, else does nothing.

            Hist& Hist::operator*=(const Hist& h)  
            Hist& Hist::operator/=(const Hist& h)  
            multiplies or divides the current histogram by the contents of the histogram in the argument if sameSize(...) is true, else does nothing.

            Hist& Hist::operator+=(double f)  
            Hist& Hist::operator-=(double f)  
            adds or subtracts each bin content by the common offset f.

            Hist& Hist::operator*=(double f)  
            Hist& Hist::operator*=(double f)  
            multiplies or divides each bin content by the common factor f.

            friend Hist operator+(double f, const Hist& h1)  
            friend Hist operator+(const Hist& h1, double f)  
            friend Hist operator+(const Hist& h1, const Hist h2)  
            add a constant to a histogram or two histograms to each other, bin by bin.

            friend Hist operator-(double f, const Hist& h1)  
            friend Hist operator-(const Hist& h1, double f)  
            friend Hist operator-(const Hist& h1, const Hist h2)  
            subtract a histogram from a constant, a constant from a histogram, or two histograms from each other, bin by bin.

            friend Hist operator*(double f, const Hist& h1)  
            friend Hist operator*(const Hist& h1, double f)  
            friend Hist operator*(const Hist& h1, const Hist h2)  
            multiply a constant by a histogram or two histograms by each other, bin by bin.

            friend Hist operator/(double f, const Hist& h1)  
            friend Hist operator/(const Hist& h1, double f)  
            friend Hist operator/(const Hist& h1, const Hist h2)  
            divide a constant by a histogram, a histogram by a constant, or two histograms by each other, bin by bin. pythia8-8.1.80.orig/phpdoc/JetMatching.php0000644000175000017500000007752212217615312016531 0ustar sunsun Jet Matching SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Jet Matching

            This manual page describes the parton-jet matching interfaces for PYTHIA8. In this approach, usually referred to as MLM matching [Man02, Man07], the final jets after parton-shower evolution and jet clustering are matched to the original partons. The event is accepted if a reasonable match is found, and rejected if not. The rejection step in an approximate way introduces a Sudakov form factor on to the hard processes. Notably the parton shower should not generate an emission that would doublecount hard activity already included in the matrix-element description. Within this general ansatz, different technical solutions can be adopted. We provide two alternatives, one based on the algorithm used in ALPGEN [Man03], and another on the one used in Madgraph [Alw11], both reimplemented from scratch here. The main points of these two algorithms are outlined further down on this page.

            We also allow for two alternative sources of external events, one in the ALPGEN native format and one in the Madgraph LHEF-based one. All four combinations of input format and matching style are implemented. In the following it is therefore important to keep the two aspects apart, whenever the ALPGEN and Madgraph labels are used.

            Currently all the files of interest are located in the examples/ subdirectory:

            • JetMatching.h contains the machinery for the parton-jet matching, in the two JetMatchingAlpgen and JetMatchingMadgraph classes.
            • GeneratorInput.h contains three classes for the reading of ALPGEN event and parameter files, and one for the reading of Madgraph parameters.
            • CombineMatchingInput.h contains three classes that combine the reading of events with the matching of them.
            • main32.cc, main32.cmnd : a sample main program and card file showing the usage of the previous files/classes.

            Event input source

            External sources of partons are used in the parton-jet matching process. The source of the partons has been separated from the implementation of the matching algorithm. By default, PYTHIA8 contains a machinery to process Les Houches Event Files (LHEFs) as described on the ";?>Les Houches Accord and ";?>Beam Parameters pages. Madgraph5 adheres to this format, but also contains some further non-standardized information that can be used. The parsing of the native ALPGEN file format is described on the ";?>Alpgen Event Interface page.

            Commonly, the source of external partons also contains information about how a particular type of matching algorithm should be employed. This information is handled by the AlpgenPar class for ALPGEN files, and MadgraphPar for LHEFs. The user can choose to set default matching parameters using the ";?>Alpgen:setMLM flag for ALPGEN files. For LHEFs, instead, the setting of default parameters is controlled with the JetMatching:setMad flag:

            JetMatching:setMad On Off   (default = on)
            When enabled, the merging parameters are set according to the values in the LHEF header. Specifically, the header must set the ickkw, xqcut, maxjetflavor and alpsfact values, and ickkw must be nonzero. Note that these labels are Madgraph-specific. For other programs with LHEF output, or for Madgraph files lacking this information, these parameters should be set by the user (or one can rely on the default values). The following parameters (described below) must then be specified:

            • JetMatching:doMerge = ickkw,
            • JetMatching:qCut = xqcut,
            • JetMatching:nQmatch = maxjetflavor,
            • JetMatching:clFact = alpsfact.
            With this flag on, the values from the LHEF for these parameters take precedence over other values.

            Jet Matching parameters

            A class JetMatching, derived from UserHooks, is used to define the basic structure of a parton-jet matching algorithm. Two versions are implemented here, based on the FORTRAN code provided by the ALPGEN and Madgraph packages, respectively: JetMatchingAlpgen and JetMatchingMadgraph. The matching parameters are defined with the JetMatching:* keyword.

            Scheme and Usage



            JetMatching:merge On Off   (default = off)
            Master switch to activate parton-jet matching. When off, all external events are accepted (unless they are rejected due to weighting or event processing problems).

            JetMatching:scheme   (default = 1; minimum = 1; maximum = 2)
            The parton-jet MLM-style matching scheme.
            1 : The one inspired by the Madgraph matching code, here implemented in the JetMatchingMadgraph class.
            2 : The one inspired by the ALPGEN matching code, here implemented in the JetMatchingAlpgen class.

            Jet algorithm

            The choice of jet algorithm and associated parameters can be adjusted with the settings below. The PYTHIA8 internal CellJet and SlowJet routines are used for jet finding. See the ";?>Event Analysis page for more details.

            JetMatching:jetAlgorithm   (default = 1; minimum = 1; maximum = 2)
            The choice of jet algorithm to use when merging against hard partons. Currently, only SlowJet with the kT algorithm (and useStandardR = false) is supported for Madgraph-style matching, while there is full freedom for the ALPGEN-style matching.
            1 : The CellJet cone algorithm.
            2 : The SlowJet clustering algorithm.


            JetMatching:slowJetPower   (default = -1; minimum = -1; maximum = 1)
            The power to use in the SlowJet algorithm.
            -1 : The anti-kT algorithm.
            0 : The Cambridge/Aachen algorithm.
            1 : The kT algorithm.


            JetMatching:nEta   (default = 100; minimum = 50)
            Specific to the CellJet algorithm, the number of bins in pseudorapidity. Specific to the CellJet algorithm, the number of bins in phi. Specific to the CellJet algorithm, the minimum eT for a cell to be acceptable as the trial center of a jet. Specific to the CellJet algorithm, cells with eT < eTthreshold are completely neglected by the jet algorithm.

            Merging parameters

            The following options are the three main parameters for the merging procedure. Although here they are in principle free parameters, they should be heavily influenced by the hard process generation cuts. These values can be set automatically based on the information in the ALPGEN file or LHEF. For the CellJet algorithm, this gives the minimum transverse energy inside a cone for a jet to be accepted. For the SlowJet algorithm, this is instead the minimum transverse momentum required for a cluster to be accepted as a jet. For Madgraph-style matching, this parameter should match the qCut parameter described later. For the CellJet algorithm, this gives the size of the cone in (eta, phi) space drawn around the geometric center of the jet. For the SlowJet algorithm, this gives the R parameter. For both jet algorithms, this defines the maximum pseudorapidity that the detector is assumed to cover. In this context, however, it is tied to the phase space region in which partons have been generated. For the Alpgen-style matching, particles within etaJetMax + coneRadius are passed to the jet algorithm, with only jets within etaJetMax retained in the merging. For the Madgraph-style matching, only particles within etaJetMax are used.

            Exclusive mode

            The following settings determine whether clustered jets which do not match an original hard parton are allowed. They are typically permitted in the highest jet multiplicity sample, where the parton shower may produce extra hard jets, without risk of double counting. Any extra jet produced by the shower must be softer than any matched light jet, or else the event is vetoed. Exclusive or inclusive merging.
            0 : The merging is run in inclusive mode. All partons must match jets, but additional jets are allowed, provided they are not harder than the matched jets.
            1 : The merging is run in exclusive mode. All partons must match jets, and no additional jets are allowed.
            2 : If nJet < nJetMax, then the merging is run in exclusive mode, otherwise it is run in inclusive mode. For Madgraph-style matching, this is checked on an event-by-event basis, which is useful when an LHEF contains a "soup" of partonic multiplicities. If nJetMax < 0 or nJet < 0, then the algorithm defaults to exclusive mode.


            JetMatching:nJet   (default = -1; minimum = -1)
            When JetMatching:exclusive = 2, nJet indicates the minimum number of additional light jets in the incoming process. This value may be set automatically.
            When JetMatching:exclusive = 2, nJetMax is used to indicate the maximum number of jets that will be matched.

            Jet matching

            The following parameters control the criteria for matching a clustered jet to a hard parton. Controls which particles are clustered by the jet algorithm.
            1 : This option explicitly disallows top quarks, leptons and photons. All other particle types are passed to the jet algorithm.
            2 : No extra particles are disallowed.

            Alpgen-specific parameters



            JetMatching:jetMatch   (default = 1; minimum = 1; maximum = 2)
            Criteria for matching a clustered jet to a parton.
            1 : This option can be used with both the CellJet and SlowJet algorithms. The delta R between each parton and jet is taken, and the minimal value compared against coneMatchLight * coneRadius for light jets or coneMatchHeavy * coneRadiusHeavy for heavy jets. Note that by default coneRadiusHeavy = coneRadius, see below. If below this value, the parton and jet are considered to match. With CellJet, the delta R measure is in (eta, phi), while with SlowJet it is in (y, phi).
            2 : This option can only be used with the SlowJet algorithm. The hard partons are inserted into the parton level event as "ghost" particles, but at the correct (y, phi) position. If this particle is then clustered into a jet, it is considered a match.


            JetMatching:coneMatchLight   (default = 1.5; minimum = 0.1)
            The coneMatchLight parameter used when JetMatching:jetMatch = 1.

            JetMatching:coneRadiusHeavy   (default = -1.0)
            The coneRadiusHeavy parameter used when JetMatching:jetMatch = 1. When assigned a negative value, the value of JetMatching:coneRadius is used.

            JetMatching:coneMatchHeavy   (default = 1.0; minimum = 0.1)
            The coneMatchHeavy parameter used when JetMatching:jetMatch = 1.

            Madgraph-specific parameters



            JetMatching:qCut   (default = 10.0; minimum = 0.0)
            kT scale for merging shower products into jets.

            JetMatching:nQmatch   (default = 5; minimum = 3; maximum = 6)
            Controls the treatment of heavy quarks.
            5 : All quarks (except top) are treated as light quarks for matching.
            4 : Bottom quarks are treated separately. Currently, they are unmatched.


            JetMatching:clFact   (default = 1.0)
            The clFact parameter determines how jet-to parton matching is done. A match is defined as a squared cluster scale that equals:
            |clFact| * qCut for inclusive mode,
            |clFact| * max(qCut,min(pT(parton))) for exclusive mode, clFact ≥ 0, or
            |clFact| * min(kT(parton)) for exclusive mode, clFact < 0.

            Alpgen-style parton-jet matching and merging

            This section describes the Alpgen-style MLM merging algorithm for PYTHIA8. The most common reference to the algorithm is [Man02]. In many respects, however, the implementation provided in the ALPGEN package should be considered the official description of the MLM merging procedure. Although designed primarily to work with events generated with ALPGEN, it can in principle also be used with events from a different source. This should not be done without thought, however, and it is up to the user to understand the details of the algorithm and the implications of using a different hard process generator.

            First, either the CellJet or SlowJet jet algorithm is chosen. Both of these algorithms have an R and an etaMax parameter. In addition, CellJet has an eTmin and SlowJet has a pTmin parameter. These are the primary three parameters of the merging procedure, and in practice are set dependent on the cuts applied to the matrix element (ME) generation. We stress that the merging procedure is not tied to the geometry of a specific physical detector, but only to the match between the original partons and the resulting jets, using standard jet algorithms in the phase space region where partons have been generated.

            ME samples with different jet multiplicities are run through the event generator, and the generation interrupted after parton showers have been applied, but before resonance decays and beam remnants have been processed. Note in particular that top quarks will not yet be decayed, which may lead to slight differences with the PYTHIA 6 interface included with the ALPGEN package. In what follows, the hardness measure of jets/partons is taken to be eT when CellJet is used and pT when SlowJet is used. The hard system (ignoring all MPI systems) is then analysed:

            • The particles in the original matrix element process are sorted into light partons, heavy partons and other particles. For backwards compatibility, a light parton is defined as the set (d, u, s, c, b, g) with zero mass. A heavy parton is defined as the set (c, b, t) with non-zero mass.
            • All particles not originating from the heavy partons or other particles are passed to the jet algorithm and clustered.
            • Clustered jets are matched to the light partons in the original ME process. There are two different methods which can be used:
              • Method 1: The following is done for each parton, in order of decreasing hardness. The delta R between the parton and all jets is calculated and the smallest value taken. If this is less than the jet R parameter, possibly multiplied by a constant, the jet and parton are considered to match, and the jet is removed from further consideration. Note that for CellJet the delta R measure is in (eta, phi), while for SlowJet, it is in (y, phi).
              • Method 2: This method is only possible when using the SlowJet algorithm. Before the clustering is performed, extremely soft "ghost" particles are added to the event at the (y, phi) coordinates of the original matrix element partons. If such a particle is clustered into a jet, the parton and jet are considered to match. The idea of "ghost" particles was originally introduced by FastJet as a way to measure jet areas [Cac06] and should not affect clustering with an infrared-safe jet algorithm.
            • If there is a light ME parton remaining which has not been matched to a jet, then the event is vetoed. If all ME partons have been matched to a jet, but there are still some extra jets remaining, then two options are possible:
              • Exclusive mode: the event is vetoed. This is typically used when there are ME samples with higher jet multiplicities, which would fill in the extra jets.
              • Inclusive mode: the event is retained if the extra jets are softer than the softest matched jet. This is typically used when there is no ME sample with higher jet multiplicity, so the parton shower should be allowed to give extra jets.
            • All particles originating from the heavy partons are passed to the jet algorithm and clustered.
            • The clustered jets are again matched to the original partons, but there is no requirement for a match to be present; all matched jets are immediately discarded. The matching procedure is much the same as for light partons, but with two differences when delta R matching is used. First, a different R parameter than that used by the jet algorithm may optionally be given. Second, all jets that are within the given radius of the parton are matched, not just the one with the smallest delta R measure. If there are still extra jets remaining then in exclusive mode the event is immediately vetoed, while in inclusive mode the event is retained if the extra jets are softer than the softest light matched jet.

            Some different options are provided, specified further above in the parameters section. These are set so that, by default, the algorithm closely follows the official MLM interface provided in the ALPGEN package.

            All vetoing of events is done through the usual ";?>User Hooks machinery, and is therefore already taken into account in the cross section. In the output from ";?>Pythia::stat(), the difference between the "Selected" and "Accepted" columns gives the number of events that have not survived the vetoing procedure. It is still the responsibility of the user to add together the results from runs with different jet multiplicities. In the simplest case, when ALPGEN input is used and the hard process parameters are used to guide the merging procedure, it is enough to set the JetMatching:nJetMax parameter.

            Madgraph-style parton-jet Merging and Matching

            This section describes the Madgraph-style parton-jet matching algorithm for PYTHIA8.

            First, the kT jet algorithm is applied using the PYTHIA8 SlowJet implementation. The useStandardR = false is used, ie. the (delta R)^2 separation is defined as 2 (cosh(delta y) - cos(delta phi)) rather than the more common (delta y)^2 + delta phi)^2. The R, etaMax, and a pTmin parameters are specified. By default, R = 1 and pTmin = qCut . It is not recommended to change these. These should match the algorithm parameters used in the Madgraph Matrix Element (ME) generation.

            ME samples with different jet multiplicities are run through the event generator, and the generation is interrupted after parton showers have been applied, but before resonance decays and beam remnants have been processed. In what follows, the hardness measure of jets/partons is taken to be kT relative to qCut. The hard system (ignoring all MPI systems) is analyzed:

            • The hard partons in the original matrix element process, provided by the LHEF, are sorted into light partons, heavy partons and other particles. A heavy parton is defined by the JetMatching:nQmatch or by the maxjetflavor value in the LHEF. nQmatch refers to the absolute value of the quark PDG identity code.
            • All partons arising from the parton shower are sorted based on their motherhood. A showered parton arising from a heavy parton or "other" parton classified in the previous step is not passed to the jet algorithm. All other partons are clustered into light jets.
            • It is checked whether there are "too few" or "too many" light jets. If the number of light jets is less than the number of light partons defined by nQmatch, the event is vetoed. If the number is larger, the event is vetoed only in exclusive mode (defined below).
            • In exclusive mode, the number of jets matches the number of light partons. In inclusive mode, the jets are re-clustered until the number of jets equals the number of light partons. Next, each light hard parton is clustered, one at a time, with the jets until a match is found. A match is defined as a squared cluster scale that equals:
              • |clFact| * qCut for inclusive mode,
              • |clFact| * max(qCut,min(pT(parton))) for exclusive mode, clFact ≥ 0, or
              • |clFact| * min(kT(parton)) for exclusive mode, clFact < 0.
              If no match is found, the event is vetoed. When a parton matches a jet, the jet is removed from the collection, and the process continues. The process terminates when all partons are matched to a jet, or a parton is unmatched.
            • All particles originating from the heavy partons are not used.
            In exclusive mode, it is expected that ME samples with higher parton multiplicity are available to fill the phase space above qCut. The inclusive mode is when there are no such samples, and the parton shower is used to fill the phase space.

            Some different options are provided, specified further above. These are set so that, by default, the algorithm closely follows the FORTRAN interface ME2Pythia provided in the Madgraph package.

            All vetoing of events is done through the usual ";?>User Hooks machinery, and is therefore already taken into account in the cross section. In the output from ";?>Pythia::stat(), the difference between the "Selected" and "Accepted" columns gives the number of events that have not survived the vetoing procedure. It is still the responsibility of the user to add together the results from runs with different jet multiplicities. In the simplest case, when the hard process parameters are used to guide the merging procedure, events will be matched in the exclusive mode.

            A note on combining UserHooks

            As have been noted above, the matching is implemented using classes derived from the ";?>UserHooks class, thereby gaining access to the event generation process at the relevant locations. For native ALPGEN files, which do not adhere to the Les Houches standards, it is also necessary to intervene with a UserHooks-derived AlpgenHooks to handle the extraction and setting of relevant extra information.

            One must then combine multiple UserHooks classes, such that the functionality of both is present. A prerequisite is that the different UserHooks classes should be declared with virtual inheritance, e.g.

              class JetMatching : virtual public UserHooks
            
            Without this option, when combining two UserHooks-derived classes, two copies of the base UserHooks class would be created, leading to ambiguities.

            The two first classes in CombineMatchingInput.h combine ALPGEN input with the two different matching schemes, e.g. for the first

            class JetMatchingAlpgenInputAlpgen : public AlpgenHooks, 
              public JetMatchingAlpgen {
            public:
              // Constructor and destructor.
              JetMatchingAlpgenInputAlpgen(Pythia& pythia) : AlpgenHooks(pythia), 
                JetMatchingAlpgen() { }
              ~JetMatchingAlpgenInputAlpgen() {}
              // Initialisation.
              virtual bool initAfterBeams() {
                if (!AlpgenHooks::initAfterBeams()) return false;
                if (!JetMatchingAlpgen::initAfterBeams()) return false;
                return true;
              }
              // Process level vetos.
              virtual bool canVetoProcessLevel() { 
                return JetMatchingAlpgen::canVetoProcessLevel();    
              }
              ....
            };
            
            This class inherits from both AlpgenHooks and JetMatchingAlpgen. Any functions which are present in both classes should be overridden with a function that calls the different parent methods in the desired order. In the above example, the only shared methods are the constructor and initAfterBeams(). "?>
            pythia8-8.1.80.orig/phpdoc/MasterSwitches.php0000644000175000017500000003465712217615312017303 0ustar sunsun Master Switches SETTINGS SAVED TO FILE

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            Master Switches

            Sometimes it may be convenient to omit certain aspects of the event generation chain. This cannot be motivated in a full-blown production run, but can often be convenient for own understanding and for debug purposes. The flags on this page allow just that.

            The event generation is subdivided into three levels: the process level, the parton level and the hadron level, and flags are grouped accordingly.

            Process Level

            The ProcessLevel class administrates the initial step of the event generation, wherein the basic process is selected. Currently this is done either using some of the internal processes, or with Les Houches Accord input.

            There could not be a complete event without an initial process, so it would not be a normal action to switch off this step. Furthermore, without a process set, it is also not possible to carry out the tasks on the parton level. It is still possible, however, to hadronize a parton-level configuration provided by some external program.

            ProcessLevel:all On Off   (default = on)
            If off, do not attempt to carry out any generation at all on the process level. For the parton level only final-state radiation is possible, using the Pythia::forceTimeShower(...) method. Do allow parton configurations stored in the event record to hadronize and hadrons to decay, however, as set by the HadronLevel switches. Further details are found ";?>here.

            For ProcessLevel:all = on one part of the event generation on this level may be switched off individually:

            ProcessLevel:resonanceDecays On Off   (default = on)
            Master switch to allow resonance decays; on/off = true/false. Normal hadrons and leptons do not count as resonances, so this is aimed specifically towards Z^0, W^+-, t, h^0 and similar objects beyond the Standard Model. Do not use this option if you may produce coloured resonances and intend to allow hadronization, since currently the program would not know how to handle this.

            It is possible to stop the generation immediately after the basic process has been selected, see PartonLevel:all below.

            PartonLevel

            The PartonLevel class administrates the middle step of the event generation, i.e. the evolution from an input (hard) process from ProcessLevel, containing a few partons only, to a complete parton-level configuration to be handed on to HadronLevel. This step involves the application of initial- and final-state radiation, multiparton interactions and the structure of beam remnants.

            PartonLevel:all On Off   (default = on)
            If off then stop the generation after the hard process has been generated, but before the parton-level and hadron-level steps. The process record is filled, but the event one is then not.

            For PartonLevel:all = on some parts of the event generation on this level may be switched off individually:

            PartonLevel:MPI On Off   (default = on)
            Master switch for multiparton interactions; on/off = true/false. Further options are found ";?>here.

            PartonLevel:ISR On Off   (default = on)
            Master switch for initial-state radiation; on/off = true/false. Further options are found ";?>here.

            PartonLevel:FSR On Off   (default = on)
            Master switch for final-state radiation; on/off = true/false. Further options are found ";?>here. If you leave this switch on, the following two switches allow more detailed control to switch off only parts of the showers.

            PartonLevel:FSRinProcess On Off   (default = on)
            Switch for final-state radiation in association with the hard process itself; on/off = true/false. In addition PartonLevel:FSR must be on for these emissions to occur.

            PartonLevel:FSRinResonances On Off   (default = on)
            Master switch for final-state radiation in any resonance decays subsequent to the hard process itself; on/off = true/false. In addition PartonLevel:FSR must be on for these emissions to occur.

            PartonLevel:earlyResDec On Off   (default = off)
            If on then do resonance decays early, before beam handling including colour reconnection. If off then decays are done afterwards, and so are unaffected by colour reconnection. The early-decay option is still primitive, for some first studies. Eventually the choice should be made individually for each resonance based on lifetime (and the environment).

            Switching off all the above MPI/ISR/FSR switches is not equivalent to setting PartonLevel:all = off. In the former case a minimal skeleton of parton-level operations are carried out, such as tying together the scattered partons with the beam remnants into colour singlets, and storing this information in the event record. It is therefore possible to go on and hadronize the event, if desired. In the latter case no operations at all are carried out on the parton level, and therefore it is also not possible to go on to the hadron level.

            PartonLevel:Remnants On Off   (default = on)
            Master switch for addition of beam remnants; on/off = true/false. Only intended for very special applications, and cannot be used to generate complete events. Specifically, unlike the other switches above, the program will complain and possibly crash unlike you also set HadronLevel:all = off and Check:event = off.

            It is possible to stop the generation immediately after the parton level has been set up, see HadronLevel:all below.

            HadronLevel

            The HadronLevel class administrates the final step of the event generation, wherein the partonic configuration from PartonLevel is hadronized, including string fragmentation and secondary decays.

            Most of the code in this class itself deals with subdividing the partonic content of the event into separate colour singlets, that can be treated individually by the string fragmentation machinery. When a junction and an antijunction are directly connected, it also breaks the string between the two, so that the topology can be reduced back to two separate one-junction systems, while still preserving the expected particle flow in the junction-junction string region(s).

            HadronLevel:all On Off   (default = on)
            If off then stop the generation after the hard process and parton-level activity has been generated, but before the hadron-level steps.

            For HadronLevel:all = on some parts of the event generation on this level may be switched off individually:

            HadronLevel:Hadronize On Off   (default = on)
            Master switch for hadronization; on/off = true/false. Further options are found ";?>here.

            HadronLevel:Decay On Off   (default = on)
            Master switch for decays; on/off = true/false. Further options are found ";?>here.

            HadronLevel:BoseEinstein On Off   (default = off)
            Master switch for the simulation of Bose-Einstein effects; on/off = true/false. Further options are found ";?>here.

            Printing



            Print:quiet On Off   (default = off)
            Can be set on to avoid the printing during program execution, to the largest extent possible. This flag acts by setting the relevant values for Init:showProcesses, Init:showMultipartonInteractions, Init:showChangedSettings, Init:showAllSettings, Init:showChangedParticleData, Init:showChangedResonanceData, Init:showAllParticleData, Init:showOneParticleData, Next:numberCount, Next:numberShowLHA, Next:numberShowInfo, Next:numberShowProcess, and Next:numberShowEvent. The change is to off or 0 for Print:quiet = off, and restores to the respective default value for = on. Those changes take effect immediately, so individual settings can be changed afterwards. "?>
            pythia8-8.1.80.orig/phpdoc/QCDProcesses.php0000644000175000017500000005415212217615312016624 0ustar sunsun QCD Processes SETTINGS SAVED TO FILE

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            QCD Processes

            This section is subdivided into soft and hard QCD processes, with open charm and bottom production set aside as a special part of the latter, and three-jet topologies as a special subset. Kindly note that there is a considerable amount of overlap between the soft and hard process classes, so that you are likely to double-count if you include both in a run.

            Soft QCD processes

            As a rule, the processes in this class should not be mixed with the simulation of other processes. All by themselves, they are intended to represent the total cross section of hadron collisions, with the exception of the "rare processes" that one wishes to study separately. In particular, jet physics at all scales occurs as part of the minimum-bias description.

            We here use the "minimum bias" expression as a shorthand for inelastic, nondiffractive events. Strictly speaking, "minimum bias" represents an experimental procedure of accepting "everything", with some non-universal cuts to exclude elastic and diffractive topologies. In practice, the experimental minimum-bias sample may then contain some contamination of what is in PYTHIA classified as diffractive, especially (high-mass) double diffractive.

            Some options to modify these cross sections are found on the ";?>Total Cross Sections page.

            SoftQCD:all On Off   (default = off)
            Common switch for the group of all soft QCD processes, as listed separately in the following.

            SoftQCD:nonDiffractive On Off   (default = off)
            The inelastic nondiffrative part of the total cross section, i.e. what would often be called the "minimum-bias component". The formalism is based on an ";?> eikonalized description of all the hard QCD processes, so includes them in combination with low-pT events. Code 101.
            Since the current description is handled by the multiparton-interactions machinery as part of the parton-level processing, no hard process at all is defined at the process-level part of the event generation. Fortunately, in this case a special ";?>codeSub() method provides information on the first, i.e. hardest, subprocess selected by the multiparton-interactions machinery.
            Note: this flag was precviously named SoftQCD:minBias, since it is almost equivalent to the minimum-bias component of the total cross section. It has invited some confusion, however, since "minimum-bias" usually refers to the experimental procedure, while "(inelastic) non-diffractive" better relates to the way events are generated in the program code. (Although also what separates diffractive from nondiffractive physics can be a matter of definition.) For backwards compatibility the SoftQCD:minBias name can be used as an alternative to SoftQCD:nonDiffractive for some time yet.

            SoftQCD:elastic On Off   (default = off)
            Elastic scattering A B -> A B. Code 102. It is possible to include ";?> Coulomb corrections, but by default this is off.

            SoftQCD:singleDiffractive On Off   (default = off)
            Single diffractive scattering A B -> X B and A B -> A X. See page on ";?> Diffraction for details. Codes 103 and 104.

            SoftQCD:doubleDiffractive On Off   (default = off)
            Double diffractive scattering A B -> X_1 X_2. See page on ";?>Diffraction for details. Code 105.

            SoftQCD:centralDiffractive On Off   (default = off)
            Central diffractive scattering A B -> A X B (a.k.a. double-Pomeron exchange, DPE). See pages on ";?>Total Cross Sections and on ";?>Diffraction for details. In particular note the SigmaTotal:zeroAXB flag, which is off in most tunes, and that therefore would need to be reset to on after the selection of a tune (even the default one). Code 106.

            SoftQCD:inelastic On Off   (default = off)
            All of the above processes, except for elastic. Codes 101, 103, 104, 105 and 106.

            Hard QCD processes

            This group contains the processes for QCD jet production above some minimum pT threshold. The pT_min cut cannot be put too low, or else unreasonably large jet cross sections will be obtained. This is because the divergent perturbative QCD cross section is used in this process group, without any regularization modifications. An eikonalized description, intended to be valid at all pT, is instead included as part of the multiparton-interactions framework, specifically in SoftQCD:nonDiffractive above.
            Warning 1: you must remember to set the PhaseSpace:pTHatMin value if you use any of these processes; there is no sensible default.
            Warning 2: you must not mix processes from the SoftQCD and HardQCD process groups, since this is likely to lead to double-counting.

            HardQCD:all On Off   (default = off)
            Common switch for the group of all hard QCD processes, as listed separately in the following.

            HardQCD:gg2gg On Off   (default = off)
            Scatterings g g -> g g. Code 111.

            HardQCD:gg2qqbar On Off   (default = off)
            Scatterings g g -> q qbar, where q by default is a light quark (u, d, s) (see below). Code 112.

            HardQCD:qg2qg On Off   (default = off)
            Scatterings q g -> q g and qbar g -> qbar g. Code 113.

            HardQCD:qq2qq On Off   (default = off)
            Scatterings q q' -> q q', q qbar' -> q qbar', qbar qbar' -> qbar qbar', where q' and q may agree, but the outgoing flavours equals the incoming ones Code 114.

            HardQCD:qqbar2gg On Off   (default = off)
            Scatterings q qbar -> g g. Code 115.

            HardQCD:qqbar2qqbarNew On Off   (default = off)
            Scatterings q qbar -> q' qbar', where q' by default is a light quark (u, d, s) (see below). Code 116.

            HardQCD:nQuarkNew   (default = 3; minimum = 0; maximum = 5)
            Number of allowed outgoing new quark flavours in the above g g -> q qbar and q qbar -> q' qbar' processes, where quarks are treated as massless in the matrix-element expressions (but correctly in the phase space). It is thus assumed that c cbar and b bbar are added separately with masses taken into account, using the processes below. A change to 4 would also include c cbar in the massless approximation, etc. In order to avoid double-counting the processes below should then not be used simultaneously.

            Hard QCD processes: heavy-flavour subset

            These processes form a natural part of the above class, but can also be generated separately. Formally the heavy-quark mass makes these matrix elements finite in the pT -> 0 limit, but at high energies one may still question the validity of the expressions at low pT values, like for the other hard-QCD processes. Also as above, an eikonalized description, intended to be valid at all pT, is included as part of the multiparton-interactions framework.
            Note that the processes below only represent the "tip of the iceberg" of charm and bottom production at high energies, where flavour excitation and shower branchings provide major additional sources. All these sources come together in the descriptions offered by SoftQCD:nonDiffractive and HardQCD:all.

            HardQCD:gg2ccbar On Off   (default = off)
            Scatterings g g -> c cbar. Code 121.

            HardQCD:qqbar2ccbar On Off   (default = off)
            Scatterings q qbar -> c cbar. Code 122.

            HardQCD:hardccbar On Off   (default = off)
            Sum of the previous two event types. Codes 121 and 122.

            HardQCD:gg2bbbar On Off   (default = off)
            Scatterings g g -> b bbar. Code 123.

            HardQCD:qqbar2bbbar On Off   (default = off)
            Scatterings q qbar -> b bbar. Code 124.

            HardQCD:hardbbbar On Off   (default = off)
            Sum of the previous two event types. Codes 123 and 124.

            Hard QCD three-parton processes

            Three-parton final states are generated by showers off two-parton processes. Topologies then cannot be specified beforehand, beyond what is provided by the two-parton hard process. For some checks it may be convenient to have access to the dedicated three-parton final states, which is what this set of processes allows. Cross sections have been taken from [Ber81].
            Note that the processes in this section are not affected by the HardQCD:all switch. In fact, it would be double-counting to include both the HardQCD:all and the HardQCD:3parton processes in a run or study.
            Warning: this section is still incomplete, e.g. the selection of colour flow is very simple, and so it should only be used with caution.

            HardQCD:3parton On Off   (default = off)
            Common switch for the group of all hard QCD processes with three partons in the final state, as listed separately in the following.

            HardQCD:gg2ggg On Off   (default = off)
            Scatterings g g -> g g g. Code 131.

            HardQCD:qqbar2ggg On Off   (default = off)
            Scatterings q qbar -> g g g. Code 132.

            HardQCD:qg2qgg On Off   (default = off)
            Scatterings q g -> q g g and qbar g -> qbar g g. Code 133.

            HardQCD:qq2qqgDiff On Off   (default = off)
            Scatterings q q' -> q q' g, q qbar' -> q qbar' g, and qbar qbar' -> qbar qbar' g. Code 134.

            HardQCD:qq2qqgSame On Off   (default = off)
            Scatterings q q -> q q g and qbar qbar -> qbar qbar g (q qbar -> q qbar g scatterings are considered separately below, see HardQCD:qqbar2qqbargSame). Code 135.

            HardQCD:qqbar2qqbargDiff On Off   (default = off)
            Scatterings q qbar -> q' qbar' g, where q' by default is a light quark (u, d, s) (see HardQCD:nQuarkNew above). Code 136.

            HardQCD:qqbar2qqbargSame On Off   (default = off)
            Scatterings q qbar -> q qbar g. Code 137.

            HardQCD:gg2qqbarg On Off   (default = off)
            Scatterings g g -> q qbar g, where q by default is a light quark (u, d, s) (see HardQCD:nQuarkNew above). Code 138.

            HardQCD:qg2qqqbarDiff On Off   (default = off)
            Scatterings q g -> q q' qbar' and qbar g -> qbar qbar' q', where q' by default is a light quark (u, d, s) (see HardQCD:nQuarkNew above). Code 139.

            HardQCD:qg2qqqbarSame On Off   (default = off)
            Scatterings q g -> q q qbar and qbar g -> qbar qbar q. Code 140. "?>
            pythia8-8.1.80.orig/phpdoc/SpacelikeShowers.php0000644000175000017500000010200212217615312017565 0ustar sunsun Spacelike Showers SETTINGS SAVED TO FILE

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            Spacelike Showers

            The PYTHIA algorithm for spacelike initial-state showers is based on the article [Sjo05], where a transverse-momentum-ordered backwards evolution scheme is introduced, with the extension to fully interleaved evolution covered in [Cor10a]. This algorithm is a further development of the virtuality-ordered one presented in [Sj085], with matching to first-order matrix element for Z^0, W^+- and Higgs (in the m_t -> infinity limit) production as introduced in [Miu99].

            The normal user is not expected to call SpaceShower directly, but only have it called from Pythia, via PartonLevel. Some of the parameters below, in particular SpaceShower:alphaSvalue, would be of interest for a tuning exercise, however.

            Main variables

            The maximum pT to be allowed in the shower evolution is related to the nature of the hard process itself. It involves a delicate balance between not double-counting and not leaving any gaps in the coverage. The best procedure may depend on information only the user has: how the events were generated and mixed (e.g. with Les Houches Accord external input), and how they are intended to be used. Therefore a few options are available, with a sensible default behaviour.

            SpaceShower:pTmaxMatch   (default = 0; minimum = 0; maximum = 2)
            Way in which the maximum shower evolution scale is set to match the scale of the hard process itself.
            0 : (i) if the final state of the hard process (not counting subsequent resonance decays) contains at least one quark (u, d, s, c ,b), gluon or photon then pT_max is chosen to be the factorization scale for internal processes and the scale value for Les Houches input; (ii) if not, emissions are allowed to go all the way up to the kinematical limit. The reasoning is that in the former set of processes the ISR emission of yet another quark, gluon or photon could lead to double-counting, while no such danger exists in the latter case.
            1 : always use the factorization scale for an internal process and the scale value for Les Houches input, i.e. the lower value. This should avoid double-counting, but may leave out some emissions that ought to have been simulated. (Also known as wimpy showers.)
            2 : always allow emissions up to the kinematical limit. This will simulate all possible event topologies, but may lead to double-counting. (Also known as power showers.)

            Note 1: Some processes contain matrix-element matching to the first emission; this is the case notably for single gamma^*/Z^0, W^+- and H^0 production. Then default and option 2 give the correct result, while option 1 should never be used.
            Note 2: as enumerated in the text, these options take effect both for internal and external processes. Whether a particular option makes sense depends on the context. For instance, if events for the same basic process to different orders are to be matched, then option 1 would be a reasonable first guess. But in more sophisticated descriptions option 2 could be combined with UserHooks vetoes on emissions that would lead to double-counting, using more flexible phase space boundaries. Option 0, finally, may be most realistic when only Born-level processes are involved, possibly in combination with a nonzero SpaceShower:pTdampMatch. The rules used for avoiding double-counting are not foolproof, however. As an example, for the t-channel process gamma gamma -> e^+ e^- its pT scale is the plausible upper shower limit, with only dampened emissions above it. But the initial state is not checked and, had only incoming quarks and gluons been taken into account, only the s-channel process q qbar -> gamma^*/Z^0 -> e^+ e^- would have been possible, where indeed the whole phase space should be populated. So this is erroneously used, giving too much emissions.
            Note 3: These options only apply to the hard interaction. If a "second hard" process is present, the two are analyzed and set separately for the default 0 option, while both are affected the same way for non-default options 1 and 2. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of each process itself.

            SpaceShower:pTmaxFudge   (default = 1.0; minimum = 0.25; maximum = 2.0)
            In cases where the above pTmaxMatch rules would imply that pT_max = pT_factorization, pTmaxFudge introduces a multiplicative factor f such that instead pT_max = f * pT_factorization. Only applies to the hardest interaction in an event, and a "second hard" if there is such a one, cf. below. It is strongly suggested that f = 1, but variations around this default can be useful to test this assumption.

            SpaceShower:pTmaxFudgeMPI   (default = 1.0; minimum = 0.25; maximum = 2.0)
            A multiplicative factor f such that pT_max = f * pT_factorization, as above, but here for the non-hardest interactions (when multiparton interactions are allowed).

            SpaceShower:pTdampMatch   (default = 0; minimum = 0; maximum = 2)
            These options only take effect when a process is allowed to radiate up to the kinematical limit by the above pTmaxMatch choice, and no matrix-element corrections are available. Then, in many processes, the fall-off in pT will be too slow by one factor of pT^2. That is, while showers have an approximate dpT^2/pT^2 shape, often it should become more like dpT^2/pT^4 at pT values above the scale of the hard process. Whether this actually is the case depends on the particular process studied, e.g. if t-channel gluon exchange is likely to dominate. If so, the options below could provide a reasonable high-pT behaviour without requiring higher-order calculations.
            0 : emissions go up to the kinematical limit, with no special dampening.
            1 : emissions go up to the kinematical limit, but dampened by a factor k^2 Q^2_fac/(pT^2 + k^2 Q^2_fac), where Q_fac is the factorization scale and k is a multiplicative fudge factor stored in pTdampFudge below.
            2 : emissions go up to the kinematical limit, but dampened by a factor k^2 Q^2_ren/(pT^2 + k^2 Q^2_ren), where Q_ren is the renormalization scale and k is a multiplicative fudge factor stored in pTdampFudge below.

            Note: These options only apply to the hard interaction. Specifically, a "second hard" interaction would not be affected. Emissions off subsequent multiparton interactions are always constrained to be below the factorization scale of the process itself.

            SpaceShower:pTdampFudge   (default = 1.0; minimum = 0.25; maximum = 4.0)
            In cases 1 and 2 above, where a dampening is imposed at around the factorization or renormalization scale, respectively, this allows the pT scale of dampening of radiation by a half to be shifted by this factor relative to the default Q_fac or Q_ren. This number ought to be in the neighbourhood of unity, but variations away from this value could do better in some processes.

            The amount of QCD radiation in the shower is determined by

            SpaceShower:alphaSvalue   (default = 0.137; minimum = 0.06; maximum = 0.25)
            The alpha_strong value at scale M_Z^2. Default value is picked equal to the one used in CTEQ 5L.

            The actual value is then regulated by the running to the scale pT^2, at which it is evaluated

            SpaceShower:alphaSorder   (default = 1; minimum = 0; maximum = 2)
            Order at which alpha_strong runs,
            0 : zeroth order, i.e. alpha_strong is kept fixed.
            1 : first order, which is the normal value.
            2 : second order. Since other parts of the code do not go to second order there is no strong reason to use this option, but there is also nothing wrong with it.

            The CMW rescaling of Lambda_QCD (see the section on ";?>StandardModelParameters) can be applied to the alpha_strong values used for spacelike showers. Note that tunes using this option need lower values of alpha_strong(m_Z^2) than tunes that do not.

            SpaceShower:alphaSuseCMW On Off   (default = false)

            option false : Do not apply the CMW rescaling.
            option true : Apply the CMW rescaling, increasing Lambda_QCD for spacelike showers by a factor roughly 1.6.

            QED radiation is regulated by the alpha_electromagnetic value at the pT^2 scale of a branching.

            SpaceShower:alphaEMorder   (default = 1; minimum = -1; maximum = 1)
            The running of alpha_em.
            1 : first-order running, constrained to agree with StandardModel:alphaEMmZ at the Z^0 mass.
            0 : zeroth order, i.e. alpha_em is kept fixed at its value at vanishing momentum transfer.
            -1 : zeroth order, i.e. alpha_em is kept fixed, but at StandardModel:alphaEMmZ, i.e. its value at the Z^0 mass.

            The natural scale for couplings and PDFs is pT^2. To explore uncertainties it is possibly to vary around this value, however, in analogy with what can be done for ";?>hard processes.

            SpaceShower:renormMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
            The default pT^2 renormalization scale is multiplied by this prefactor. For QCD this is equivalent to a change of Lambda^2 in the opposite direction, i.e. to a change of alpha_strong(M_Z^2) (except that flavour thresholds remain at fixed scales). Below, when pT^2 + pT_0^2 is used as scale, it is this whole expression that is multiplied by the prefactor.

            SpaceShower:factorMultFac   (default = 1.; minimum = 0.1; maximum = 10.)
            The default pT^2 factorization scale is multiplied by this prefactor.

            There are two complementary ways of regularizing the small-pT divergence, a sharp cutoff and a smooth dampening. These can be combined as desired but it makes sense to coordinate with how the same issue is handled in multiparton interactions.

            SpaceShower:samePTasMPI On Off   (default = off)
            Regularize the pT -> 0 divergence using the same sharp cutoff and smooth dampening parameters as used to describe multiparton interactions. That is, the MultipartonInteractions:pT0Ref, MultipartonInteractions:ecmRef, MultipartonInteractions:ecmPow and MultipartonInteractions:pTmin parameters are used to regularize all ISR QCD radiation, rather than the corresponding parameters below. This is a sensible physics ansatz, based on the assumption that colour screening effects influence both MPI and ISR in the same way. Photon radiation is regularized separately in either case.
            Warning: if a large pT0 is picked for multiparton interactions, such that the integrated interaction cross section is below the nondiffractive inelastic one, this pT0 will automatically be scaled down to cope. Information on such a rescaling does NOT propagate to SpaceShower, however.

            The actual pT0 parameter used at a given CM energy scale, ecmNow, is obtained as
            pT0 = pT0(ecmNow) = pT0Ref * (ecmNow / ecmRef)^ecmPow
            where pT0Ref, ecmRef and ecmPow are the three parameters below.

            SpaceShower:pT0Ref   (default = 2.0; minimum = 0.5; maximum = 10.0)
            Regularization of the divergence of the QCD emission probability for pT -> 0 is obtained by a factor pT^2 / (pT0^2 + pT^2), and by using an alpha_s(pT0^2 + pT^2). An energy dependence of the pT0 choice is introduced by the next two parameters, so that pT0Ref is the pT0 value for the reference cm energy, pT0Ref = pT0(ecmRef).

            SpaceShower:ecmRef   (default = 1800.0; minimum = 1.)
            The ecmRef reference energy scale introduced above.

            SpaceShower:ecmPow   (default = 0.0; minimum = 0.; maximum = 0.5)
            The ecmPow energy rescaling pace introduced above.

            SpaceShower:pTmin   (default = 0.2; minimum = 0.1; maximum = 10.0)
            Lower cutoff in pT, below which no further ISR branchings are allowed. Normally the pT0 above would be used to provide the main regularization of the branching rate for pT -> 0, in which case pTmin is used mainly for technical reasons. It is possible, however, to set pT0Ref = 0 and use pTmin to provide a step-function regularization, or to combine them in intermediate approaches. Currently pTmin is taken to be energy-independent.

            SpaceShower:pTminChgQ   (default = 0.5; minimum = 0.01)
            Parton shower cut-off pT for photon coupling to a coloured particle.

            SpaceShower:pTminChgL   (default = 0.0005; minimum = 0.0001)
            Parton shower cut-off mass for pure QED branchings. Assumed smaller than (or equal to) pTminChgQ.

            SpaceShower:rapidityOrder On Off   (default = off)
            Force emissions, after the first, to be ordered in rapidity, i.e. in terms of decreasing angles in a backwards-evolution sense. Could be used to probe sensitivity to unordered emissions. Only affects QCD emissions.

            Weak showers

            The description of W^+- and Z^0 gauge boson emission in ISR closely parallels that of such emissions in ";?>FSR. We therefore will not repeat the discussion here, but only report on the settings names, which again are similar to the FSR ones.

            SpaceShower:weakShower On Off   (default = off)
            Allow a weak shower, yes or no.

            SpaceShower:weakShowerMode   (default = 0; minimum = 0; maximum = 2)
            Determine which branchings are allowed.
            option 0 : both W^+- and Z^0 branchings.
            option 1 : only W^+- branchings.
            option 2 : only Z^0 branchings.

              (; minimum = 0.1; maximum = 2.0)
            Parton shower cut-off pT for weak branchings.

            SpaceShower:weakShowerEnhancement   (default = 1.; minimum = 1.; maximum = 1000.)
            Enhancement factor for the weak shower. This is used to increase the statistics of weak shower emissions. Remember afterwards to correct for the additional weak emissions (i.e. divide the weak emissions by the same factor).

            SpaceShower:singleWeakEmission On Off   (default = off)
            This parameter allows to stop the weak shower after a single emission.
            on = only a single weak emission is allowed.
            off = unlimited number of weak emissions possible.

            SpaceShower:extraScaleTerm   (default = 0.; minimum = 0.; maximum = 200.)
            The normal showers uses pT^2 as ordering variable, but for massive particles it could be preferred to use pT^2 + M^2 instead. This parameter allows to use pT^2 + k * M^2 for weak showers, thus k = 0 is the standard ordering and is used as default.

            SpaceShower:dopTDampMass On Off   (default = on)
            Add an extra dampening to the weak shower to lower the production of low-pT W/Z's. The dampening is given by (pT^2 + 0.25 M^2)/ (pT^2 + M^2), where M^2 is the squared mass of the W/Z.

            SpaceShower:vetoWeakJets On Off   (default = on)
            This flag will veto the 2nd emission on the same side of the process if it has too high "pT" if the primary process was weak production (code 221, 222, 223). This is too avoid doubling counting with dijet production followed by an emission of a W/Z boson. The pT definition used is the pT in the rest frame of the two emitted partons with respect to the incoming parton. This pT definition should be close to the pT definition of a dijet event.

            SpaceShower:vetoWeakJetspTcut   (default = 20.0; minimum = 1.0; maximum = 1e9)
            This parameter determines the cut-off pT used for the veto of emissions for weak production. For more information see vetoWeakJets.

            Further variables

            These should normally not be touched. Their only function is for cross-checks.

            There are three flags you can use to switch on or off selected branchings in the shower:

            SpaceShower:QCDshower On Off   (default = on)
            Allow a QCD shower; on/off = true/false.

            SpaceShower:QEDshowerByQ On Off   (default = on)
            Allow quarks to radiate photons; on/off = true/false.

            SpaceShower:QEDshowerByL On Off   (default = on)
            Allow leptons to radiate photons; on/off = true/false.

            There are some further possibilities to modify the shower:

            SpaceShower:MEcorrections On Off   (default = on)
            Use of matrix element corrections; on/off = true/false.

            SpaceShower:MEafterFirst On Off   (default = on)
            Use of matrix element corrections also after the first emission, for dipole ends of the same system that did not yet radiate. Only has a meaning if MEcorrections above is switched on.

            SpaceShower:phiPolAsym On Off   (default = on)
            Azimuthal asymmetry induced by gluon polarization; on/off = true/false.

            SpaceShower:phiIntAsym On Off   (default = on)
            Azimuthal asymmetry induced by interference; on/off = true/false.

            SpaceShower:strengthIntAsym   (default = 0.7; minimum = 0.; maximum = 0.9)
            Size of asymmetry induced by interference. Natural value of order 0.5; expression would blow up for a value of 1.

            SpaceShower:nQuarkIn   (default = 5; minimum = 0; maximum = 5)
            Number of allowed quark flavours in g -> q qbar branchings, when kinematically allowed, and thereby also in incoming beams. Changing it to 4 would forbid g -> b bbar, etc.

            Technical notes

            Almost everything is equivalent to the algorithm in [1]. Minor changes are as follows.
            • It is now possible to have a second-order running alpha_s, in addition to fixed or first-order running.
            • The description of heavy flavour production in the threshold region has been modified, so as to be more forgiving about mismatches between the c/b masses used in Pythia relative to those used in a respective PDF parametrization. The basic idea is that, in the threshold region of a heavy quark Q, Q = c/b, the effect of subsequent Q -> Q g branchings is negligible. If so, then
              f_Q(x, pT2) = integral_mQ2^pT2 dpT'2/pT'2 * alpha_s(pT'2)/2pi * integral P(z) g(x', pT'2) delta(x - z x')
              so use this to select the pT2 of the g -> Q Qbar branching. In the old formalism the same kind of behaviour should be obtained, but by a cancellation of a 1/f_Q that diverges at the threshold and a Sudakov that vanishes.
              The strategy therefore is that, once pT2 < f * mQ2, with f a parameter of the order of 2, a pT2 is chosen like dpT2/pT2 between mQ2 and f * mQ2, a nd a z flat in the allowed range. Thereafter acceptance is based on the product of three factors, representing the running of alpha_strong, the splitting kernel (including the mass term) and the gluon density weight. At failure, a new pT2 is chosen in the same range, i.e. is not required to be lower since no Sudakov is involved.
            • The QED algorithm now allows for hadron beams with non-zero photon content. The backwards-evolution of a photon in a hadron is identical to that of a gluon, with CF -> eq^2 and CA -> 0. Note that this will only work in conjunction with parton distribution that explicitly include photons as part of the hadron structure (such as the MRST2004qed set). Since Pythia's internal sets do not allow for photon content in hadrons, it is thus necessary to use the LHAPDF interface to make use of this feature. The possibility of a fermion backwards-evolving to a photon has not yet been included, nor has photon backwards-evolution in lepton beams.
            "?>
            pythia8-8.1.80.orig/phpdoc/FlavourSelection.php0000644000175000017500000006471112217615312017614 0ustar sunsun Flavour Selection SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Flavour Selection

            The StringFlav class handles the choice of a new flavour in the fragmentation process, and the production of a new hadron from a set of input flavours. It is mainly used by the string fragmentation machinery (including ministrings), but also e.g. in some particle decays and for some beam-remnant cases. The basic concepts are in agreement with [And83]. The baryon-sector implementation is based on the MSTJ(12)=3 option of PYTHIA 6, i.e. new SU(6) weights scheme with at most one popcorn meson.

            The relative production rates of different particle species is influenced by the parameters below. Some have only an impact on one specific quantity, but most directly or indirectly have consequences for many observables. Therefore the values to use have to be viewed in the context of a complete ";?>tune.

            New flavours

            The main parameters of the selection of a new flavour are

            StringFlav:probStoUD   (default = 0.19; minimum = 0.0; maximum = 1.0)
            the suppression of s quark production relative to ordinary u or d one.

            StringFlav:probQQtoQ   (default = 0.09; minimum = 0.0; maximum = 1.0)
            the suppression of diquark production relative to quark production, i.e. of baryon relative to meson production.

            StringFlav:probSQtoQQ   (default = 1.00; minimum = 0.0; maximum = 1.0)
            the suppression of strange diquark production relative to light diquark production, over and above the one already given by probStoU.

            StringFlav:probQQ1toQQ0   (default = 0.027; minimum = 0.0; maximum = 1.0)
            the suppression of spin 1 diquark production relative to spin 0 one, apart from the factor of 3 enhancement of spin 1 from counting the number of states.

            Standard-meson production

            The bulk of the particle production corresponds to the lowest-lying pseudoscalar and vector multiplets. Their production rates are determined by the parameters in this section.

            For a given set of flavours, produced according to the probabilities outlined above, the ratio of vector-to-pseudocalar meson production is described by the parameters below. The maximum allowed rate for each case has been set according to spin-counting rules, but we expect the real rates to be lower, especially for lighter mesons, owing to the vector-pseudoscalar mass splitting.

            StringFlav:mesonUDvector   (default = 0.62; minimum = 0.; maximum = 3.)
            the relative production ratio vector/pseudoscalar for light (u, d) mesons.

            StringFlav:mesonSvector   (default = 0.725; minimum = 0.; maximum = 3.)
            the relative production ratio vector/pseudoscalar for strange mesons.

            StringFlav:mesonCvector   (default = 1.06; minimum = 0.; maximum = 3.)
            the relative production ratio vector/pseudoscalar for charm mesons.

            StringFlav:mesonBvector   (default = 3.0; minimum = 0.; maximum = 3.)
            the relative production ratio vector/pseudoscalar for bottom mesons.

            Inside each light-quark meson nonet, an octet-singlet mixing angle describes the mixing of the two flavour-diagonal isoscalar = 0 states. (For terminology and details see [Yao06], chapter 14 on the quark model.) This angle is needed to specify the probability for such a q qbar state to project onto a specific meson. More transparent formulae are obtained by introducing the angle alpha = theta + 54.7 degrees:
            f = (uubar + ddbar)/sqrt(2) * sin(alpha) + ssbar * cos(alpha)
            f' = (uubar + ddbar)/sqrt(2) * cos(alpha) - ssbar * sin(alpha)



            StringFlav:thetaPS   (default = -15.; minimum = -90.; maximum = 90.)
            gives the mixing angle theta_PS in the pseudoscalar meson sector (which is rather poorly determined), expressed in degrees. Here f is associated with eta' and f' with eta. (This standard but counterintuitive choice is fixed up in the code by replacing alpha -> 90^0 - alpha so that eta <-> eta'; relative signs do not matter since we are interested in probabilities only.)

            StringFlav:thetaV   (default = 36.; minimum = -90.; maximum = 90.)
            gives the mixing angle theta_V in the vector meson sector (which is somewhat better determined), expressed in degrees. Here f is associated with omega and f' with phi.

            Further, the simple model overestimates the production of eta and, in particular, eta' mesons, which can be rectified by

            StringFlav:etaSup   (default = 0.63; minimum = 0.; maximum = 1.)
            the additional suppression of eta production, multiplying the normal production probability. Thus 0 means no eta at all are produced, while 1 means full rate.

            StringFlav:etaPrimeSup   (default = 0.12; minimum = 0.; maximum = 1.)
            the additional suppression of eta' production, multiplying the normal production probability. Thus 0 means no eta' at all are produced, while 1 means full rate.

            Excited-meson production

            Several excited mesons, ie. with radial or orbital excitations, have been observed at non-negligible production rates. Extrapolated to all states a fair fraction of all particle production might proceed through such states. There are big uncertainties, however, since these excited mesons in many cases are extremely poorly known. This also means that the modeling of their production and decay is very primitive, and even that the inclusion of the production of such states may lead to a degraded agreement with data. Currently the default is that all such production is switched off.

            Parameters are provided to switch them on. By demand, this machinery has been made more flexible than in the past. Therefore one parameter is provided for each combination of heaviest flavour (u/d, s, c or b) and multiplet produced. In each case the production rate is normalized to that of the lowest-lying pseudoscalar of the same flavour content, as for the vector-meson rates introduced above. The multiplets available are the four obtained for one unit of orbital angular momentum, in the nonrelativistic classification. Using J to denote the sum of quark spin S and orbital angular momentum L, i.e. what would normally be called the spin of the meson, one has:

            • a pseudovector multiplet with L=1, S=0, J=1;
            • a scalar multiplet with L=1, S=1, J=0;
            • a pseudovector multiplet with L=1, S=1, J=1;
            • a tensor multiplet with L=1, S=1, J=2.
            The maximum allowed rate for each case has been set according to spin-counting rules, but we expect the real rates to be significantly lower, owing to mass suppression.

            StringFlav:mesonUDL1S0J1   (default = 0.0; minimum = 0.; maximum = 3.)
            the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for light (u, d) mesons.

            StringFlav:mesonUDL1S1J0   (default = 0.0; minimum = 0.; maximum = 1.)
            the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for light (u, d) mesons.

            StringFlav:mesonUDL1S1J1   (default = 0.0; minimum = 0.; maximum = 3.)
            the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for light (u, d) mesons.

            StringFlav:mesonUDL1S1J2   (default = 0.0; minimum = 0.; maximum = 5.)
            the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for light (u, d) mesons.

            StringFlav:mesonSL1S0J1   (default = 0.0; minimum = 0.; maximum = 3.)
            the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for strange mesons.

            StringFlav:mesonSL1S1J0   (default = 0.0; minimum = 0.; maximum = 1.)
            the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for strange mesons.

            StringFlav:mesonSL1S1J1   (default = 0.0; minimum = 0.; maximum = 3.)
            the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for strange mesons.

            StringFlav:mesonSL1S1J2   (default = 0.0; minimum = 0.; maximum = 5.)
            the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for strange mesons.

            StringFlav:mesonCL1S0J1   (default = 0.0; minimum = 0.; maximum = 3.)
            the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for charm mesons.

            StringFlav:mesonCL1S1J0   (default = 0.0; minimum = 0.; maximum = 1.)
            the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for charm mesons.

            StringFlav:mesonCL1S1J1   (default = 0.0; minimum = 0.; maximum = 3.)
            the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for charm mesons.

            StringFlav:mesonCL1S1J2   (default = 0.0; minimum = 0.; maximum = 5.)
            the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for charm mesons.

            StringFlav:mesonBL1S0J1   (default = 0.0; minimum = 0.; maximum = 3.)
            the relative pseudovector production ratio (L=1,S=0,J=1)/pseudoscalar for bottom mesons.

            StringFlav:mesonBL1S1J0   (default = 0.0; minimum = 0.; maximum = 1.)
            the relative scalar production ratio (L=1,S=1,J=0)/pseudoscalar for bottom mesons.

            StringFlav:mesonBL1S1J1   (default = 0.0; minimum = 0.; maximum = 3.)
            the relative pseudovector production ratio (L=1,S=1,J=1)/pseudoscalar for bottom mesons.

            StringFlav:mesonBL1S1J2   (default = 0.0; minimum = 0.; maximum = 5.)
            the relative tensor production ratio (L=1,S=1,J=2)/pseudoscalar for bottom mesons.

            In addition, an octet-singlet mixing angle is needed for each multiplet, as for the pseudoscalar and vector multiplets above. Only for the tensor multiplet does any determination exist; for the other multiplets default has been chose so that ssbar does not mix with the light quarks, and so that the ssbar state is the heavier of the two.

            StringFlav:thetaL1S0J1   (default = 35.3; minimum = -90.; maximum = 90.)
            gives the mixing angle theta in the (L=1,S=0,J=1) pseudovector meson sector, expressed in degrees.

            StringFlav:thetaL1S1J0   (default = 35.3; minimum = -90.; maximum = 90.)
            gives the mixing angle theta in the (L=1,S=1,J=0) scalar meson sector, expressed in degrees.

            StringFlav:thetaL1S1J1   (default = 35.3; minimum = -90.; maximum = 90.)
            gives the mixing angle theta in the (L=1,S=1,J=1) pseudovector meson sector, expressed in degrees.

            StringFlav:thetaL1S1J2   (default = 28.0; minimum = -90.; maximum = 90.)
            gives the mixing angle theta in the (L=1,S=1,J=2) tensor meson sector, expressed in degrees.

            Baryon production

            The relative rate of baryon production is mainly given by the quark and diquark production parameters above, plus SU(6) Clebsch-Gordans. The one modifiable parameter related to these coefficients is

            StringFlav:decupletSup   (default = 1.0; minimum = 0.0; maximum = 1.0)
            the suppression, relative to default SU(6) factors, of decuplet baryon production. Default corresponds to no suppression, while 0 corresponds to no decuplet production at all.

            In addition, if popcorn production is allowed, wherein a set of mesons (M) may be produced in between the baryon (B) and the antibaryon (Bbar), a set of further parameters is introduced. Currently only the simplest scenario is implemented, wherein at most one intermediate meson may be produced.

            StringFlav:popcornRate   (default = 0.5; minimum = 0.; maximum = 2.0)
            gives the relative rates of B Bbar and B M Bbar production, roughly as
            Prob(B M Bbar) / (Prob(B Bbar) + Prob(B M Bbar)) = popcornRate / (0.5 + popcornRate)
            (the complete expression depends on all the quark and diquark production parameters and is therefore not so useful).

            StringFlav:popcornSpair   (default = 0.5; minimum = 0.; maximum = 1.0)
            extra suppression for having an s sbar pair shared between the B and Bbar in a B M Bbar configuration.

            StringFlav:popcornSmeson   (default = 0.5; minimum = 0.; maximum = 1.0)
            extra suppression for having a strange meson M in a B M Bbar configuration.

            Finally, there are some indications that leading-baryon production may be further suppressed. A proper description should probably be based on a suppression of early production times [Ede97], but we here only implement a simpler version where production near the end of a string, as defined by rank, is suppressed. The more detailed studies suggest that leading c and b baryon production will be less suppressed, so we leave it open to set light- and heavy-baryon suppression separately.

            StringFlav:suppressLeadingB On Off   (default = off)
            Suppress leading-baryon production.
            option off : No suppression.
            option on : Suppress the production of a diquark in the string breaking closest to a quark end of a string, by either of the factors below. This suppresses the production of first-rank baryons by the same amount. Indirectly also the second-rank and, if popcorn production is switched on, third-rank (anti)baryon production is affected.

            StringFlav:lightLeadingBSup   (default = 0.5; minimum = 0.; maximum = 1.0)
            extra suppression of leading-baryon production for a light-quark jet, i.e. d, u or s, when suppressLeadingB = on. Thus 0 means no leading-baryon production at all, while 1 means full rate.

            StringFlav:heavyLeadingBSup   (default = 0.9; minimum = 0.; maximum = 1.0)
            extra suppression of leading-baryon production for a heavy-quark jet, i.e. c or b, when suppressLeadingB = on. Thus 0 means no leading-baryon production at all, while 1 means full rate. "?>

            pythia8-8.1.80.orig/phpdoc/TotalCrossSections.php0000644000175000017500000003731212217615312020132 0ustar sunsun Total Cross Sections SETTINGS SAVED TO FILE

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            "; } } ?>

            Total Cross Sections

            The SigmaTotal class returns the total, elastic, diffractive and nondiffractive cross sections in hadronic collisions, and also the slopes of the d(sigma)/dt distributions. Most of the parametrizations used are from [Sch94, Sch97] which borrows some of the total cross sections from [Don92]. If you use the MBR (Minimum Bias Rockefeller) model [Cie12], Diffraction:PomFlux = 5, this model contains its own parametrizations of all cross sections in p p and pbar p collisions.

            There are strong indications that the currently implemented diffractive cross section parametrizations, which should be in reasonable agreement with data at lower energies, overestimate the diffractive rate at larger values. If you wish to explore this (or other) aspect, it is possible to override the cross section values in two different ways. The first offers (almost) complete freedom, but needs to be defined separately for each CM energy, while the second introduces a simpler parametrized damping. The two cannot be combined. Furthermore the Coulomb term for elastic scattering, which by default is off, can be switched on.

            The allowed combinations of incoming particles are p + p, pbar + p, pi+ + p, pi- + p, pi0/rho0 + p, phi + p, J/psi + p, rho + rho, rho + phi, rho + J/psi, phi + phi, phi + J/psi, J/psi + J/psi. The strong emphasis on vector mesons is related to the description of gamma + p and gamma + gamma interactions in a Vector Dominance Model framework (which will not be available for some time to come, so this is a bit of overkill). Nevertheless, the sections below, with allowed variations, are mainly intended to make sense for p + p.

            Central diffraction

            Central diffraction (CD), a.k.a. double Pomeron exchange (DPE), was not part of the framework in [Sch94]. It has now been added for multiparticle states, i.e. excluding the resonance region below 1 GeV mass, as well as other exclusive states, but only for p p or pbar p. It uses the same proton-Pomeron vertex as in single diffraction, twice, to describe x_Pomeron and t spectra. This fixes the energy dependence, which has been integrated and parametrized. The absolute normalization has been left open, however. Furthermore, since CD has not been included in previous tunes to data, a special flag is available to reproduce the old behaviour (with due complications when one does not want to do this).

            SigmaTotal:sigmaAXB2TeV   (default = 1.5; minimum = 0.)
            The CD cross section for p p and pbar p collisions, normalized to its value at 2 TeV CM energy, expressed in mb. The energy dependence is then parametrized, and behaves roughly like ln^1.5(s). Is used for the options Diffraction:PomFlux = 1 - 4, while the MBR model (= 5) has its own parametrization.

            SigmaTotal:zeroAXB On Off   (default = off)
            several existing ";?>tunes do not include CD. An inclusion of a nonvanishing CD cross section directly affects the nondiffractive phenomenology (even if not dramatically), and so this flag is used to switch off the CD cross section in such tunes. You can switch it back on after the selection of a tune, if you so wish. This option has no effect for the MBR model (Diffraction:PomFlux = 5), where the CD cross section has been included from the onset.

            Set cross sections



            SigmaTotal:setOwn On Off   (default = off)
            Allow a user to set own cross sections by hand; on/off = true/false.

            When SigmaTotal:setOwn = on, the user is expected to set values for the corresponding cross sections:

            SigmaTotal:sigmaTot   (default = 80.; minimum = 0.)
            Total cross section in mb.

            SigmaTotal:sigmaEl   (default = 20.; minimum = 0.)
            Elastic cross section in mb.

            SigmaTotal:sigmaXB   (default = 8.; minimum = 0.)
            Single Diffractive cross section A + B -> X + B in mb.

            SigmaTotal:sigmaAX   (default = 8.; minimum = 0.)
            Single Diffractive cross section A + B -> A + X in mb.

            SigmaTotal:sigmaXX   (default = 4.; minimum = 0.)
            Double Diffractive cross section A + B -> X_1 + X_2 in mb.

            SigmaTotal:sigmaAXB   (default = 1.; minimum = 0.)
            Central Diffractive cross section A + B -> A + X + B in mb.

            Note that the total cross section subtracted by the elastic and various diffractive ones gives the inelastic nondiffractive cross section, which therefore is not set separately. If this cross section evaluates to be negative the internal parametrizations are used instead of the ones here. However, since the nondiffractive inelastic cross section is what makes up the minimum-bias event class, and plays a major role in the description of multiparton interactions, it is important that a consistent set is used.

            Dampen diffractive cross sections

            As already noted, unitarization effects may dampen the rise of diffractive cross sections relative to the default parametrizations. The settings here allows one way to introduce a dampening, which is used in some of the existing ";?>tunes.

            SigmaDiffractive:dampen On Off   (default = no)
            Allow a user to dampen diffractive cross sections; on/off = true/false.

            When SigmaDiffractive:dampen = on, the three diffractive cross sections are damped so that they never can exceed the respective values below. Specifically, if the standard parametrization gives the cross section sigma_old(s) and a fixed sigma_max is set, the actual cross section becomes sigma_new(s) = sigma_old(s) * sigma_max / (sigma_old(s) + sigma_max). This reduces to sigma_old(s) at low energies and to sigma_max at high ones. Note that the asymptotic value is approached quite slowly, however.

            SigmaDiffractive:maxXB   (default = 15.; minimum = 0.)
            The above sigma_max for A + B -> X + B in mb.

            SigmaDiffractive:maxAX   (default = 15.; minimum = 0.)
            The above sigma_max for A + B -> A + X in mb.

            SigmaDiffractive:maxXX   (default = 15.; minimum = 0.)
            The above sigma_max for A + B -> X_1 + X_2 in mb.

            SigmaDiffractive:maxAXB   (default = 3.; minimum = 0.)
            The above sigma_max for A + B -> A + X + B in mb.

            As above, a reduced diffractive cross section automatically translates into an increased nondiffractive one, such that the total (and elastic) cross section remains fixed.

            Set elastic cross section

            In the above option the t slopes are based on the internal parametrizations. In addition there is no Coulomb-term contribution to the elastic (or total) cross section, which of course becomes infinite if this contribution is included. If you have switched on SigmaTotal:setOwn you can further switch on a machinery to include the Coulomb term, including interference with the conventional strong-interaction Pomeron one [Ber87]. Then the elastic cross section is no longer taken from SigmaTotal:sigmaEl but derived from the parameters below and SigmaTotal:sigmaTot, using the optical theorem. The machinery is only intended to be used for p p and pbar p collisions. The description of diffractive events, and especially their slopes, remains unchanged.

            SigmaElastic:setOwn On Off   (default = no)
            Allow a user to set parameters for the normalization and shape of the elastic cross section the by hand; yes/no = true/false.

            SigmaElastic:bSlope   (default = 18.; minimum = 0.)
            the slope b of the strong-interaction term exp(bt), in units of GeV^-2.

            SigmaElastic:rho   (default = 0.13; minimum = -1.; maximum = 1.)
            the ratio of the real to the imaginary parts of the nuclear scattering amplitude.

            SigmaElastic:lambda   (default = 0.71; minimum = 0.1; maximum = 2.)
            the main parameter of the electric form factor G(t) = lambda^2 / (lambda + |t|)^2, in units of GeV^2.

            SigmaElastic:tAbsMin   (default = 5e-5; minimum = 1e-10)
            since the Coulomb contribution is infinite a lower limit on |t| must be set to regularize the divergence, in units of GeV^2.

            SigmaElastic:phaseConst   (default = 0.577)
            The Coulomb term is taken to contain a phase factor exp(+- i alpha phi(t)), with + for p p and - for pbar p, where phi(t) = - phaseConst - ln(-B t/2). This constant is model dependent [Cah82]. "?>

            pythia8-8.1.80.orig/phpdoc/MainProgramSettings.php0000644000175000017500000006535412217615312020271 0ustar sunsun Main-Program and Related Settings SETTINGS SAVED TO FILE

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            "; } } ?>

            Main-Program and Related Settings

            Introduction

            The main program is up to the user to write. However, ";?>sample main programs are provided. In one such class of programs, key settings of the run are read in from a "cards file". For experimental collaborations this is actually the most common way to run a program like PYTHIA. The commands in such a file may be of two types
            (a) instructions directly to Pythia, like which processes to generate, and
            (b) instructions to the main program for what it should do, like how many events to generate, and how many events should be listed.
            In principle these two kinds could be kept completely separate. However, to make life simpler, a number of useful main-program settings are defined on this page, so that they are recognized by the Settings machinery. They can thus be put among the other cards without distinction. It is up to you to decide which ones, if any, you actually want to use when you write your main program.

            To further reduce the necessary amount of main-program code, some of the tasks that you can steer from your main program can also be done internally. This in particular relates to some information printing. To give an example, the Main:numberToList mode can be used by you in your main program to decide to list a few of the generated events, whereas Next:numberListEvent is used internally in a pythia.next() call to do such a listing automatically. Ultimately, in both cases, a pythia.event.list() call is the one that generates the listing, explicitly in the main program in the former case, implicitly called from pythia.next() in the latter.

            The settings names on this page thus fall into four main groups

            • Init:... denote actions that automatically may be taken during the pythia.init() call.
            • Next:... denote actions that automatically may be taken during the pythia.next() call.
            • Stat:... denote actions that automatically may be taken during the pythia.stat() call.
            • Main:... denote actions that you yourself have the freedom to make use of in your main program.
            The use of several of the Main:... options is deprecated in favour of the other possibilities.

            The Main:... options works like this. Once you have used the pythia.readFile(fileName) method to read in the cards file, where the values have been set, you can interrogate the Settings database to make the values available in your main program. A slight complication is that you need to use a different Settings method for each of the four possible return types that you want to extract. To save some typing the same method names are found directly in the Pythia class, and just send on to the Settings ones to do the job, e.g.

              bool   showCS = pythia.flag("Main:showChangedSettings");
              int    nEvent = pythia.mode("Main:numberOfEvents");
              double spare1 = pythia.parm("Main:spareParm1");
              string file   = pythia.word("Main:allSettingsFile"); 
            

            Main-program settings

            The settings in this section must be under the control of the user, i.e. there are no internal equivalents.

            Main:numberOfEvents   (default = 1000; minimum = 0)
            The number of events to be generated.

            Main:timesAllowErrors   (default = 10)
            Allow this many times that pythia.next() returns false, i.e. that an event is flawed, before aborting the run.

            Initialization settings



            Init:showProcesses On Off   (default = on)
            Print a list of all processes that will be simulated, with their estimated cross section maxima, as used for the subsequent Monte Carlo selection. Also print corresponding Les Houches initialization data, where relevant.

            Init:showMultipartonInteractions On Off   (default = on)
            Print initialization information for the multiparton interactions machinery.

            Init:showChangedSettings On Off   (default = on)
            Print a list of the changed flag/mode/parameter/word settings.

            Init:showAllSettings On Off   (default = off)
            Print a list of all flag/mode/parameter/word settings. Warning: this will be a long list.

            Init:showChangedParticleData On Off   (default = on)
            Print a list of particle and decay data for those particles that were changed (one way or another).

            Init:showChangedResonanceData On Off   (default = off)
            In the previous listing also include the resonances that are initialized at the beginning of a run and thus get new particle data, even if these may well agree with the default ones. Warning: this will be a rather long list.

            Init:showAllParticleData On Off   (default = off)
            Print a list of all particle and decay data. Warning: this will be a long list.

            Init:showOneParticleData   (default = 0; minimum = 0)
            Print particle and decay data for the particle with this particular identity code. Default means that no particle is printed.

            Main:showChangedSettings On Off   (default = on)
            Deprecated. Print a list of the changed flag/mode/parameter/word settings.

            Main:showAllSettings On Off   (default = off)
            Deprecated. Print a list of all flag/mode/parameter/word settings. Warning: this will be a long list.

            Main:showChangedParticleData On Off   (default = off)
            Deprecated. Print a list of particle and decay data for those particles that were changed (one way or another).

            Main:showChangedResonanceData On Off   (default = off)
            Deprecated. In the previous listing also include the resonances that are initialized at the beginning of a run and thus get new particle data, even if these may well agree with the default ones. Warning: this will be a rather long list.

            Main:showAllParticleData On Off   (default = off)
            Deprecated. Print a list of all particle and decay data. Warning: this will be a long list.

            Main:showOneParticleData   (default = 0; minimum = 0)
            Deprecated. Print particle and decay data for the particle with this particular identity code. Default means that no particle is printed.

            Main:writeChangedSettings On Off   (default = off)
            Write a file with the changed flag/mode/parameter/word settings, in a format appropriate to be read in at the beginning of a new run, using the pythia.readFile(fileName) method.

            Main:changedSettingsFile   (default = currentSettings.cmnd)
            The name of the file to which the changed flag/mode/parameter/word settings are written if Main:writeChangedSettings is on.

            Main:writeAllSettings On Off   (default = off)
            Write a file with all flag/mode/parameter/word settings, in a format appropriate to be read in at the beginning of a new run, using the pythia.readFile(fileName) method.

            Main:allSettingsFile   (default = allSettings.cmnd)
            The name of the file to which a flag/mode/parameter/word settings are written if Main:writeAllSettings is on.

            Event-generation settings



            Next:numberCount   (default = 1000; minimum = 0)
            Print a line telling how many events have been generated so far, once every numberCount events. If set zero then no lines are ever printed.

            Next:numberShowLHA   (default = 1; minimum = 0)
            The number of events to list the Les Houches input information for, where relevant.

            Next:numberShowInfo   (default = 1; minimum = 0)
            The number of events to list the Info information for, where relevant.

            Next:numberShowProcess   (default = 1; minimum = 0)
            The number of events to list the process record for, where relevant.

            Next:numberShowEvent   (default = 1; minimum = 0)
            The number of events to list the event record for, where relevant.

            Next:showScaleAndVertex On Off   (default = off)
            In addition to the normal information in the listing of the process and event records, a second line per particle provides information on the production scale, particle polarization and production vertex.

            Next:showMothersAndDaughters On Off   (default = off)
            In addition to the normal information in the listing of the process and event records, further lines list all the mothers and daughters of each particle.

            Main:numberToList   (default = 2; minimum = 0)
            Deprecated. The number of events to list.

            Main:timesToShow   (default = 50; minimum = 0)
            Deprecated. Print the number of events generated so far, this many times, i.e. once every numberOfEvents/numberToShow events.

            Statistics



            Stat:showProcessLevel On Off   (default = on)
            Print the available statistics on number of generated events and cross sections, where relevant.

            Stat:showPartonLevel On Off   (default = off)
            Print the available statistics on number and types of multiparton interactions, where relevant.

            Stat:showErrors On Off   (default = on)
            Print the available statistics on number and types of aborts, errors and warnings.

            Stat:reset On Off   (default = off)
            Reset the statistics of the above three kinds. The default is that all stored statistics information is unaffected by the pythia.stat() call. Counters are automatically reset in each new pythia.init() call, however, so the only time the reset option makes a difference is if stat() is called several times in a (sub)run.

            Main:showAllStatistics On Off   (default = off)
            Print all available statistics or only the minimal set at the end of the run.

            Subruns

            You can use ";?>subruns to carry out several tasks in the same run. In that case you will need repeated instances of the first setting below in your command file, and could additionally use the second and third as well.

            Main:subrun   (default = -999; minimum = 0)
            The number of the current subrun, a non-negative integer, put as first line in a section of lines to be read for this particular subrun.

            Main:LHEFskipInit On Off   (default = off)
            If you read several Les Houches Event Files that you want to see considered as one single combined event sample you can set this flag on after the first subrun to skip (most of) the (re-)initialization step.

            Main:numberOfSubruns   (default = 0)
            The number of subruns you intend to use in your current run. Unlike the two settings above, Pythia itself will not interpret this number, but you could e.g. have a loop in your main program to loop over subruns from 0 through numberOfSubruns - 1.

            Spares

            For currently unforeseen purposes, a few dummy settings are made available here. The user can set the desired value in a "cards file" and then use that value in the main program as desired.

            Main:spareFlag1 On Off   (default = off)


            Main:spareFlag2 On Off   (default = off)


            Main:spareFlag3 On Off   (default = off)


            Main:spareMode1   (default = 0)


            Main:spareMode2   (default = 0)


            Main:spareMode3   (default = 0)


            Main:spareParm1   (default = 0.)


            Main:spareParm2   (default = 0.)


            Main:spareParm3   (default = 0.)


            Main:spareWord1   (default = void)


            Main:spareWord2   (default = void)


            Main:spareWord3   (default = void)
            "?>
            pythia8-8.1.80.orig/phpdoc/ProgramFiles.php0000644000175000017500000004024412217615312016715 0ustar sunsun Program Files SETTINGS SAVED TO FILE

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            "; } } ?>

            Program Files

            The code is subdivided into a set of files, mainly by physics task. Each file typically contains one main class, but often with a few related helper classes that are not used elsewhere in the program. Normally the files come in pairs.
            • A header file, .h in the include subdirectory, where the public interface of the class is declared, and inline methods are defined.
            • A source code file, .cc in the src subdirectory, where most of the methods are implemented.
            During compilation, related dependency files, .d, and compiled code, .o are created in the tmp subdirectory.

            In part the .xml documentation files in the xmldoc subdirectory have matching names, but the match is broken by the desire to group topics more by user interaction than internal operation. On these pages the function of the different code files is summarized. Currently, each .xml file is also translated into an .html one in the htmldoc subdirectory, to allow easy viewing of the contents in a web browser, and an .php one in phpdoc, for more sophisticated interactivity if that subdirectory is installed on a web server.

            Here is the current list of files, ordered alphabetically, with a brief description of contents.

            file  Analysis  
            contains routines to analyze events. Currently it can do sphericity, thrust, Lund/Jade/Durham jet clustering, cone-jet finding, and the kT, anti-kT and Cambridge/Aachen algorithms for hadron colliders.

            file  Basics  
            contains some basic facilities of general use: a random number generator Rndm, a four-vector class Vec4, and a histogram class Hist.

            file  BeamParticle  
            contains information on all partons extracted from one of the two beams. Defines modified parton distributions accordingly during the showering and multiparton interactions processing, thereby extending on the one-particle-inclusive distributions defined by the previous class. Finds the internal structure for a beam remnant.

            file  BeamRemnants  
            adds primordial kT to the set of hard subsystems, and combines these subsystems with the two beam remnants to provide the overall energy-momentum picture. Also ties together all the colour lines into consistent singlets.

            file  BeamShape  
            generates momentum spread of beams, and spread of collision vertex position.

            file  BoseEinstein  
            provides a simple method to impose Bose-Einstein correlations on pairs of identical mesons.

            file  Event  
            contains the event record, which basically is a vector of particles. This file also contains the Particle class, used by Event. Pythia uses two Event objects, one for the process-level record (process) and one for the complete event (event).

            file  FragmentationFlavZpT  
            contains the classes for describing the fragmentation steps in flavour and in longitudinal and transverse momentum.

            file  FragmentationSystems  
            defines some containers of parton systems, for use in the fragmentation routines.

            file  HadronLevel  
            turns the parton-level event above into a set of outgoing particles, by applying string fragmentation (with special treatment for low-mass systems) and secondary decays, and optionally Bose-Einstein corrections.

            file  HelicityBasics  
            basic classes for the handling of helicities in tau lepton decays.

            file  HelicityMatrixElements  
            helicity-dependent decay matrix elements for the tau lepton.

            file  HiddenValleyFragmentation  
            hadronization in models with a hidden sector that contains an unbroken SU(N), which gives confinement. The model and code is largely derived from the normal fragmentation classes.

            file  History  
            methods to reconstruct the imagined shower history of a matrix-element-generated multiparton configuration, as part of the CKKW-L matrix element merging.

            file  Info  
            is a simple container that gives access to some information on the nature of the current process, such as Mandelstam variables. Also contains a small database for errors and warnings encountered during program execution.

            file  LesHouches  
            gives the possibility to feed in parton configurations for the subsequent event generation. One base class is defined, with containers for initialization and event information, that can be read from Pythia. Derived classes allow for a few different cases.

            file  LHAFortran  
            is a header file only, for a class derived from the above LesHouches one, to be used for runtime interfacing to Fortran programs, such as PYTHIA 6.

            file  LHAPDFInterface  
            is a header file only, with interfaces to the key LHAPDF routines, as needed for a runtime interface. There is a file lhapdfdummy/LHAPDFdummy.cc with matching dummy implementations, however. This file is used to build a separate liblhapdfdummy library, to be linked when the LHAPDF library is not used, so as to avoid problems with undefined references.

            file  MergingHooks  
            intercede in the normal shower evolution to construct the relevant Sudakov form factor suppressions as part of the CKKW-L matrix element merging.

            file  MiniStringFragmentation  
            performs string fragmentation in cases where the colour singlet subsystem mass is so small that one or at most two primary hadrons should be produced from it.

            file  MultipartonInteractions  
            performs multiparton interactions.

            file  ParticleData  
            contains a database of all necessary particle data (masses, names, ..) and decay channels.

            file  ParticleDecays  
            performs the decays of all normal unstable hadrons and leptons, i.e. in mass up to and including b bbar systems. It is not intended for decays of electroweak resonances, like Z^0.

            file  PartonDistributions  
            contains parton distribution functions for the proton and electron. Currently very simple, with only two p parametrizations and one e ditto available, but it is possible to link in external sets.

            file  PartonLevel  
            turns the (hard) process above into a complete set of partons, by adding initial- and final-state radiation, multiparton interactions, and beam remnants.

            file  PartonSystems  
            keeps track of which partons belong to which partonic subsystem, i.e. one of the multiparton (semi)hard interactions with associated showers.

            file  PhaseSpace  
            selects a point in phase space for the hard-process generation, optimized separately for each process to give improved Monte Carlo efficiency.

            file  ProcessContainer  
            packages the information on a given subprocess, combining the phase-space selection and cross-section evaluation machineries with some statistics information. Also sets up the list of processes to be studied in a run.

            file  ProcessLevel  
            handles the generation of the (hard) process that sets the character of the event. This involves either using internally implemented processes or linking to Les Houches information. The latter can be by runtime interfaces or by reading in a file. This step also includes resonance decays.

            file  Pythia  
            is the main class, that administrates the whole event generation process by making use of all the others classes. Objects of most other classes reside (directly or indirectly) inside Pythia, so only a Pythia object needs to be explicitly instantiated and addressed by the user.

            file  Pythia8ToHepMC  
            contains an interface to convert the PYTHIA 8 event record into the HepMC format. The Pythia8ToHepMC.cc file is located in the subdirectory pythia8tohepmc and is used to build a separate libpythia8tohepmc library.

            file  PythiaComplex  
            is only a .h file, containing a typedef for double precision complex numbers.

            file  PythiaStdlib  
            contains most of the Stdlib headers used in PYTHIA 8, with using directives. It defines M_PI if this is not already done. Also a few simple inline methods: pow2(x), pow3(x), pow4(x), pow5(x) and pow6(x) for small integer powers, and sqrtpos(x) where a max(0., x) ensures that one does not take the square root of a negative number. Also non-inlined GammaReal(x) for the Gamma function value of a real argument.

            file  ResonanceDecays  
            decays resonances as part of the hard-process stage, in many cases (but not all) including angular correlations between the decay products.

            file  ResonanceWidths  
            encodes some properties of resonances, in particular the dynamic calculation of widths.

            file  RHadrons  
            handles the production and decay of hadrons formed by long-lived gluinos, stops or sbottoms.

            file  Settings  
            contains a database of all flags, modes, parameters and words that determine the performance of the generator. Initial values are obtained from the contents of the .xml files, but these values can then be changed by the user.

            file  SigmaCompositeness  
            contains the cross sections and matrix elements for production of some particles in compositeness scenarios, specifically excited fermions.

            file  SigmaEW  
            contains the cross sections and matrix elements for electroweak processes involving photons, Z^0's and W^+-'s.

            file  SigmaExtraDim  
            contains the cross sections and matrix elements for processes in scenarios involving extra dimensions.

            file  SigmaGeneric  
            contains the cross sections and matrix elements for some generic processes, to be used as building blocks for a few BSM scenarios.

            file  SigmaHiggs  
            contains the cross sections and matrix elements for Higgs production.

            file  SigmaLeftRightSym  
            contains the cross sections and matrix elements for particle production in left-right-symmetry scenarios, specifically righthanded Z and W bosons and doubly-charged Higgs bosons.

            file  SigmaLeptoquark  
            contains the cross sections and matrix elements for leptoquark production.

            file  SigmaNewGaugeBosons  
            contains the cross sections and matrix elements for a Z'^0, a W^+- and a horizontal gauge boson R^0.

            file  SigmaOnia  
            contains the cross sections and matrix elements for charmonium and bottomonium production.

            file  SigmaProcess  
            contains the base class and derived classes for the evaluation of different matrix elements. Also keeps track of allowed incoming parton configurations and their cross sections, including parton densities. In order to keep this file from becoming too big, actual cross sections are found in several separate files of derived classes: SigmaQCD, SigmaEW, SigmaOnia, SigmaHiggs, SigmaSUSY, SigmaNewGaugeBosons, SigmaLeftRightSym, SigmaLeptoquark, SigmaCompositeness, SigmaExtraDim and SigmaGeneric.

            file  SigmaQCD  
            contains the cross sections and matrix elements for soft and hard QCD processes.

            file  SigmaSUSY  
            contains the cross sections and matrix elements for Supersymmetric processes.

            file  SigmaTotal  
            contains parametrizations of total, elastic and diffractive hadronic cross sections.

            file  SpaceShower  
            performs spacelike initial-state transverse-momentum-ordered shower evolution.

            file  StandardModel  
            contains the running alpha_strong, with Lambda matching at flavour thresholds, the running alpha_em, CKM mixing matrices, and a few other parameters such as sin^2(theta_W).

            file  StringFragmentation  
            performs string fragmentation of a given set of partons.

            file  SusyCouplings  
            stores the various couplings used for SUSY cross sections and decays, as calculated from input e.g. based on the SUSY Les Houches Accord.

            file  SusyLesHouches  
            contains information on SUSY parameters and particle data as specified by the SUSY Les Houches Accord.

            file  TauDecays  
            the main routines for handling tau lepton decays with helicity information.

            file  TimeShower  
            performs timelike final-state transverse-momentum-ordered shower evolution.

            file  UserHooks  
            Provides a way for a user to study the event at a few intermediate stages of evolution, to reject the event as a whole or to modify its cross-section weight. pythia8-8.1.80.orig/phpdoc/HadronScattering.php0000644000175000017500000002002412217615312017554 0ustar sunsun Hadron Scattering SETTINGS SAVED TO FILE

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            Hadron Scattering

            A simple hadron scattering model. It is intended to take into account that the overlap of multiple strings at low transverse dimensions is likely to lead to some collective effects, not unlike those observed in heavy-ion collisions, even if not quite as pronounced. Specifically, it is assumed that the hadrons produced can scatter against each other on the way out, before the fragmenting system has had time to expand enough that the hadrons get free. Thereby heavier particles are shifted to higher transverse momenta, at the expense of the lighter ones.
            Warning: This is still at an experimental level, and should not be used unless you know what you are doing.

            HadronScatter:scatter On Off   (default = off)
            Master flag for hadron scattering.

            HadronScatter:afterDecay On Off   (default = off)
            Perform hadron scattering before or after first round of decays, involving very short-lived particles like the rho. The default is to perform scattering directly after the string fragmentation, before any decays.

            HadronScatter:allowDecayProd On Off   (default = off)
            Allow two hadrons with same parent hadron to scatter.

            HadronScatter:scatterRepeat On Off   (default = off)
            Allow hadrons which have already scattered to scatter again. Even if switched on, the same pair can not scatter off each other twice.

            Hadron selection



            HadronScatter:hadronSelect   (default = 0; minimum = 0; maximum = 0)
            Probability that a hadron is soft enough to scatter. (A high-pT hadron presumably being part of a jet, and thus produced away from the high-particle-density region at small transverse dimensions.)
            0 : P = N exp(-pT^2 / 2 / sigma^2) / ( (1 - k) exp(-pT^2 / 2 / sigma^2) + k pT0^p / (pT0^2 + pT^2)^(p/2), with sigma = 2 StringPT:sigma and pT0 the same as that used in MultipartonInteractions.


            HadronScatter:N   (default = 1.0; minimum = 0.01; maximum = 1.0)
            N parameter as above.

            HadronScatter:k   (default = 1.0; minimum = 0.01; maximum = 1.0)
            k parameter as above.

            HadronScatter:p   (default = 6; minimum = 2; maximum = 30)
            p parameter as above.

            Scattering probability



            HadronScatter:scatterProb   (default = 0; minimum = 0; maximum = 2)
            Probability for a pair of hadrons to scatter.
            0 : All hadrons scatter with probability j max(0, 1 - dR^2 / rMax^2). Angular distribution is picked flat in cos(theta).
            1 : As option 0, above, but only pi-pi, pi-K and pi-p scatterings are considered.
            2 : Only pi-pi, pi-K and pi-p scatterings are considered, with probability given by (1 - exp(-j sigEl)) max(0, 1 - dR^2 / rMax^2). The elastic cross sections and angular distributions are taken from the partial-wave distributions.


            HadronScatter:j   (default = 0.5; minimum = 0.0; maximum = 10.0)
            j parameter as above.

            HadronScatter:rMax   (default = 0.5; minimum = 0.1; maximum = 2.0)
            rMax parameter as above.

            HadronScatter:tile On Off   (default = off)
            Use tiling in (eta, phi) to reduce number of pairwise tests. "?>
            pythia8-8.1.80.orig/phpdoc/RandomNumbers.php0000644000175000017500000001435412217615312017102 0ustar sunsun Random Numbers SETTINGS SAVED TO FILE

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            Random Numbers

            This page describes the random-number generator in PYTHIA and how it can be replaced by an external one.

            Internal random numbers

            The Rndm class generates random numbers, using the Marsaglia-Zaman-Tsang algorithm [Mar90].

            Random numbers R uniformly distributed in 0 < R < 1 are obtained with

               Rndm::flat();
            
            There are also methods to generate according to an exponential, to x * exp(-x), to a Gaussian, or picked among a set of possibilities, which make use of flat().

            If the random number generator is not initialized before, it will be so the first time it is asked to generate a random number, and then with the default seed, 19780503. This means that, by default, all runs will use identically the same random number sequence. This is convenient for debugging purposes, but dangerous if you intend to run several "identical" jobs to boost statistics. You can initialize, or reinitialize, with your own choice of seed with a

               Rndm::init(seed);
            
            Here values 0 < seed < 900 000 000 gives so many different random number sequences, while seed = 0 will call the Stdlib time(0) function to provide a "random" seed, and seed < 0 will revert back to the default seed.

            The Pythia class defines ";?>a flag and a mode, that allows the seed to be set in the Pythia::init call. That would be the standard way for a user to pick the random number sequence in a run.

            External random numbers

            RndmEngine is a base class for the external handling of random-number generation. The user-written derived class is called if a pointer to it has been handed in with the pythia.rndmEnginePtr() method. Since the default Marsaglia-Zaman-Tsang algorithm is quite good, chances are that any replacement would be a step down, but this may still be required by consistency with other program elements in big experimental frameworks.

            There is only one pure virtual method in RndmEngine, to generate one random number flat in the range between 0 and 1:

              virtual double flat() = 0;
            
            Note that methods for initialization are not provided in the base class, in part since input parameters may be specific to the generator used, in part since initialization can as well be taken care of externally to the Pythia code.

            An example illustrating how to run with an external random number generator is provided in main23.cc.

            The methods

            We here collect a more complete and formal overview of the methods.

            Rndm::Rndm()  
            construct a random number generator, but does not initialize it.

            Rndm::Rndm(int seed)  
            construct a random number generator, and initialize it for the given seed number.

            bool Rndm::rndmEnginePtr( RndmEngine* rndmPtr)  
            pass in pointer for external random number generation.

            void Rndm::init(int seed = 0)  
            initialize, or reinitialize, the random number generator for the given seed number. Not necessary if the seed was already set in the constructor.

            double Rndm::flat()  
            generate next random number uniformly between 0 and 1.

            double Rndm::exp()  
            generate random numbers according to exp(-x).

            double Rndm::xexp()  
            generate random numbers according to x exp(-x).

            double Rndm::gauss()  
            generate random numbers according to exp(-x^2/2).

            pair<double, double> Rndm::gauss2()  
            generate a pair of random numbers according to exp( -(x^2 + y^2) / 2). Is faster than two calls to gauss().

            int Rndm::pick(const vector& prob)  
            pick one option among vector of (positive) probabilities.

            bool Rndm::dumpState(string fileName)  
            save the current state of the random number generator to a binary file. This involves two integers and 100 double-precision numbers. Intended for debug purposes. Note that binary files may be platform-dependent and thus not transportable.

            bool Rndm::readState(string fileName)  
            set the state of the random number generator by reading in a binary file saved by the above command. Comments as above.

            virtual double RndmEngine::flat()  
            if you want to construct an external random number generator (or generator interface) then you must implement this method in your class derived from the RndmEningen base class, to give a random number between 0 and 1. pythia8-8.1.80.orig/phpdoc/TopProcesses.php0000644000175000017500000001112512217615312016750 0ustar sunsun Top Processes SETTINGS SAVED TO FILE

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            Top Processes

            Different ways to produce top quarks, singly or in pairs.

            Top:all On Off   (default = off)
            Common switch for the group of top production.

            Top:gg2ttbar On Off   (default = off)
            Scatterings g g -> t tbar. Code 601.

            Top:qqbar2ttbar On Off   (default = off)
            Scatterings q qbar -> t tbar by gluon exchange. Code 602.

            Top:qq2tq(t:W) On Off   (default = off)
            Scatterings q q' -> t q'' by t-channel exchange of a W^+- boson. Code 603.

            Top:ffbar2ttbar(s:gmZ) On Off   (default = off)
            Scatterings f fbar -> t tbar by s-channel exchange of a gamma^*/Z^0 boson. Code 604.

            Top:ffbar2tqbar(s:W) On Off   (default = off)
            Scatterings f fbar' -> t q'' by s-channel exchange of a W^+- boson. Code 605.

            Top:gmgm2ttbar On Off   (default = off)
            Scatterings gamma gamma -> t tbar. Code 606.

            By default top always decays to a W and a down-type quark. It is possible to switch on the t -> H+ b decay mode. Note that its partial width is calculated using the tan(beta) value stored in HiggsHchg:tanBeta, so that it can be used without having to read in a SUSY parameter file. For the H+ to decay also Higgs:useBSM = on is necessary. "?>

            pythia8-8.1.80.orig/phpdoc/FourVectors.php0000644000175000017500000004226512217615312016611 0ustar sunsun Four-Vectors SETTINGS SAVED TO FILE

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            Four-Vectors

            The Vec4 class gives a simple implementation of four-vectors. The member function names are based on the assumption that these represent four-momentum vectors. Thus one can get or set p_x, p_y, p_z and e, but not x, y, z or t. This is only a matter of naming, however; a Vec4 can equally well be used to store a space-time four-vector.

            The Particle object contains a Vec4 p that stores the particle four-momentum, and another Vec4 vProd for the production vertex. For the latter the input/output method names are adapted to the space-time character rather than the normal energy-momentum one. Thus a user would not normally access the Vec4 classes directly, but only via the methods of the Particle class, see ";?>Particle Properties.

            Nevertheless you are free to use the PYTHIA four-vectors, e.g. as part of some simple analysis code based directly on the PYTHIA output, say to define the four-vector sum of a set of particles. But note that this class was never set up to allow complete generality, only to provide the operations that are of use inside PYTHIA. There is no separate class for three-vectors, since such can easily be represented by four-vectors where the fourth component is not used.

            Four-vectors have the expected functionality: they can be created, copied, added, multiplied, rotated, boosted, and manipulated in other ways. Operator overloading is implemented where reasonable. Properties can be read out, not only the components themselves but also for derived quantities such as absolute momentum and direction angles.

            Constructors and basic operators

            A few methods are available to create or copy a four-vector:

            Vec4::Vec4(double x = 0., double y = 0., double z = 0., double t = 0.)  
            creates a four-vector, by default with all components set to 0.

            Vec4::Vec4(const Vec4& v)  
            creates a four-vector copy of the input four-vector.

            Vec4& Vec4::operator=(const Vec4& v)  
            copies the input four-vector.

            Vec4& Vec4::operator=(double value)  
            gives a four-vector with all components set to value.

            Member methods for input

            The values stored in a four-vector can be modified in a few different ways:

            void Vec4::reset()  
            sets all components to 0.

            void Vec4::p(double pxIn, double pyIn, double pzIn, double eIn)  
            sets all components to their input values.

            void Vec4::p(Vec4 pIn)  
            sets all components equal to those of the input four-vector.

            void Vec4::px(double pxIn)  
            void Vec4::py(double pyIn)  
            void Vec4::pz(double pzIn)  
            void Vec4::e(double eIn)  
            sets the respective component to the input value.

            Member methods for output

            A number of methods provides output of basic or derived quantities:

            double Vec4::px()  
            double Vec4::py()  
            double Vec4::pz()  
            double Vec4::e()  
            gets the respective component.

            double Vec4::mCalc()  
            double Vec4::m2Calc()  
            the (squared) mass, calculated from the four-vectors. If m^2 < 0 the mass is given with a minus sign, -sqrt(-m^2). Note the possible loss of precision in the calculation of E^2 - p^2; for particles the correct mass is stored separately to avoid such problems.

            double Vec4::pT()  
            double Vec4::pT2()  
            the (squared) transverse momentum.

            double Vec4::pAbs()  
            double Vec4::pAbs2()  
            the (squared) absolute momentum.

            double Vec4::eT()  
            double Vec4::eT2()  
            the (squared) transverse energy, eT = e * sin(theta) = e * pT / pAbs.

            double Vec4::theta()  
            the polar angle, in the range 0 through pi.

            double Vec4::phi()  
            the azimuthal angle, in the range -pi through pi.

            double Vec4::thetaXZ()  
            the angle in the xz plane, in the range -pi through pi, with 0 along the +z axis.

            double Vec4::pPos()  
            double Vec4::pNeg()  
            the combinations E+-p_z.

            double Vec4::rap()  
            double Vec4::eta()  
            true rapidity y and pseudorapidity eta.

            Friend methods for output

            There are also some friend methods that take one, two or three four-vectors as argument. Several of them only use the three-vector part of the four-vector.

            friend ostream& operator<<(ostream&, const Vec4& v)  
            writes out the values of the four components of a Vec4 and, within brackets, a fifth component being the invariant length of the four-vector, as provided by mCalc() above, and it all ended with a newline.

            friend double m(const Vec4& v1, const Vec4& v2)  
            friend double m2(const Vec4& v1, const Vec4& v2)  
            the (squared) invariant mass.

            friend double dot3(const Vec4& v1, const Vec4& v2)  
            the three-product.

            friend double cross3(const Vec4& v1, const Vec4& v2)  
            the cross-product.

            friend double theta(const Vec4& v1, const Vec4& v2)  
            friend double costheta(const Vec4& v1, const Vec4& v2)  
            the (cosine) of the opening angle between the vectors, in the range 0 through pi.

            friend double phi(const Vec4& v1, const Vec4& v2)  
            friend double cosphi(const Vec4& v1, const Vec4& v2)  
            the (cosine) of the azimuthal angle between the vectors around the z axis, in the range 0 through pi.

            friend double phi(const Vec4& v1, const Vec4& v2, const Vec4& v3)  
            friend double cosphi(const Vec4& v1, const Vec4& v2, const Vec4& v3)  
            the (cosine) of the azimuthal angle between the first two vectors around the direction of the third, in the range 0 through pi.

            friend double RRapPhi(const Vec4& v1, const Vec4& v2)  
            friend double REtaPhi(const Vec4& v1, const Vec4& v2)  
            the R distance measure, in (y, phi) or (eta, phi) cylindrical coordinates, i.e. R^2 = (y_1 - y_2)^2 + (phi_1 - phi_2)^2 and equivalent.

            Operations with four-vectors

            Of course one should be able to add, subtract and scale four-vectors, and more:

            Vec4 Vec4::operator-()  
            return a vector with flipped sign for all components, while leaving the original vector unchanged.

            Vec4& Vec4::operator+=(const Vec4& v)  
            add a four-vector to an existing one.

            Vec4& Vec4::operator-=(const Vec4& v)  
            subtract a four-vector from an existing one.

            Vec4& Vec4::operator*=(double f)  
            multiply all four-vector components by a real number.

            Vec4& Vec4::operator/=(double f)  
            divide all four-vector components by a real number.

            friend Vec4 operator+(const Vec4& v1, const Vec4& v2)  
            add two four-vectors.

            friend Vec4 operator-(const Vec4& v1, const Vec4& v2)  
            subtract two four-vectors.

            friend Vec4 operator*(double f, const Vec4& v)  
            friend Vec4 operator*(const Vec4& v, double f)  
            multiply a four-vector by a real number.

            friend Vec4 operator/(const Vec4& v, double f)  
            divide a four-vector by a real number.

            friend double operator*(const Vec4& v1, const Vec4 v2)  
            four-vector product.

            There are also a few related operations that are normal member methods:

            void Vec4::rescale3(double f)  
            multiply the three-vector components by f, but keep the fourth component unchanged.

            void Vec4::rescale4(double f)  
            multiply all four-vector components by f.

            void Vec4::flip3()  
            flip the sign of the three-vector components, but keep the fourth component unchanged.

            void Vec4::flip4()  
            flip the sign of all four-vector components.

            Rotations and boosts

            A common task is to rotate or boost four-vectors. In case only one four-vector is affected the operation may be performed directly on it. However, in case many particles are affected, the helper class RotBstMatrix can be used to speed up operations.

            void Vec4::rot(double theta, double phi)  
            rotate the three-momentum with the polar angle theta and the azimuthal angle phi.

            void Vec4::rotaxis(double phi, double nx, double ny, double nz)  
            rotate the three-momentum with the azimuthal angle phi around the direction defined by the (n_x, n_y, n_z) three-vector.

            void Vec4::rotaxis(double phi, Vec4& n)  
            rotate the three-momentum with the azimuthal angle phi around the direction defined by the three-vector part of n.

            void Vec4::bst(double betaX, double betaY, double betaZ)  
            boost the four-momentum by beta = (beta_x, beta_y, beta_z).

            void Vec4::bst(double betaX, double betaY, double betaZ,double gamma)  
            boost the four-momentum by beta = (beta_x, beta_y, beta_z), where the gamma = 1/sqrt(1 - beta^2) is also input to allow better precision when beta is close to unity.

            void Vec4::bst(const Vec4& p)  
            boost the four-momentum by beta = (p_x/E, p_y/E, p_z/E).

            void Vec4::bst(const Vec4& p, double m)  
            boost the four-momentum by beta = (p_x/E, p_y/E, p_z/E), where the gamma = E/m is also calculated from input to allow better precision when beta is close to unity.

            void Vec4::bstback(const Vec4& p)  
            boost the four-momentum by beta = (-p_x/E, -p_y/E, -p_z/E).

            void Vec4::bstback(const Vec4& p, double m)  
            boost the four-momentum by beta = (-p_x/E, -p_y/E, -p_z/E), where the gamma = E/m is also calculated from input to allow better precision when beta is close to unity.

            void Vec4::rotbst(const RotBstMatrix& M)  
            perform a combined rotation and boost; see below for a description of the RotBstMatrix.

            For a longer sequence of rotations and boosts, and where several Vec4 are to be rotated and boosted in the same way, a more efficient approach is to define a RotBstMatrix, which forms a separate auxiliary class. You can build up this 4-by-4 matrix by successive calls to the methods of the class, such that the matrix encodes the full sequence of operations. The order in which you do these calls must agree with the imagined order in which the rotations/boosts should be applied to a four-momentum, since in general the operations do not commute.

            RotBstMatrix::RotBstMatrix()  
            creates a diagonal unit matrix, i.e. one that leaves a four-vector unchanged.

            RotBstMatrix::RotBstMatrix(const RotBstMatrix& Min)  
            creates a copy of the input matrix.

            RotBstMatrix& RotBstMatrix::operator=(const RotBstMatrix4& Min)  
            copies the input matrix.

            void RotBstMatrix::rot(double theta = 0., double phi = 0.)  
            rotate by this polar and azimuthal angle.

            void RotBstMatrix::rot(const Vec4& p)  
            rotate so that a vector originally along the +z axis becomes parallel with p. More specifically, rotate by -phi, theta and phi, with angles defined by p.

            void RotBstMatrix::bst(double betaX = 0., double betaY = 0., double betaZ = 0.)  
            boost by this beta vector.

            void RotBstMatrix::bst(const Vec4&)  
            void RotBstMatrix::bstback(const Vec4&)  
            boost with a beta = p/E or beta = -p/E, respectively.

            void RotBstMatrix::bst(const Vec4& p1, const Vec4& p2)  
            boost so that p_1 is transformed to p_2. It is assumed that the two vectors obey p_1^2 = p_2^2.

            void RotBstMatrix::toCMframe(const Vec4& p1, const Vec4& p2)  
            boost and rotate to the rest frame of p_1 and p_2, with p_1 along the +z axis.

            void RotBstMatrix::fromCMframe(const Vec4& p1, const Vec4& p2)  
            rotate and boost from the rest frame of p_1 and p_2, with p_1 along the +z axis, to the actual frame of p_1 and p_2, i.e. the inverse of the above.

            void RotBstMatrix::rotbst(const RotBstMatrix& Min);  
            combine the current matrix with another one.

            void RotBstMatrix::invert()  
            invert the matrix, which corresponds to an opposite sequence and sign of rotations and boosts.

            void RotBstMatrix::reset()  
            reset to no rotation/boost; i.e. the default at creation.

            double RotBstMatrix::deviation()  
            crude estimate how much a matrix deviates from the unit matrix: the sum of the absolute values of all non-diagonal matrix elements plus the sum of the absolute deviation of the diagonal matrix elements from unity.

            friend ostream& operator<<(ostream&, const RotBstMatrix& M)  
            writes out the values of the sixteen components of a RotBstMatrix, on four consecutive lines and ended with a newline. pythia8-8.1.80.orig/phpdoc/ExternalDecays.php0000644000175000017500000001003012217615312017224 0ustar sunsun External Decays SETTINGS SAVED TO FILE

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            External Decays

            DecayHandler is a base class for the external handling of decays. It is intended for normal particle decays, primarily B mesons and tau, and cannot be used to redirect decays of heavy resonances like t or Z^0. The user-written derived class is called if a pointer to it has been given with the ";?>pythia.decayPtr() method, where it also is specified which particles it will be called for. This particle information is accessible with the ";?>doExternalDecay() method.

            There is only one pure virtual method in DecayHandler, to do the decay:

            virtual bool DecayHandler::decay(vector<int>& idProd, vector<double>& mProd, vector<Vec4>& pProd, int iDec, const Event& event)  
            where
            argument idProd : is a list of particle PDG identity codes,
            argument mProd : is a list of their respective masses (in GeV), and
            argument pProd : is a list of their respective four-momenta.

            At input, these vectors each have size one, so that idProd[0], mProd[0] and pProd[0] contain information on the particle that is to be decayed. At output, the vectors should have increased by the addition of all the decay products. Even if initially defined in the rest frame of the mother, the products should have been boosted so that their four-momenta add up to the pProd[0] of the decaying particle.

            Should it be of interest to know the prehistory of the decaying particle, e.g. to set some helicity information affecting the decay angular distribution, the full event record is available read-only, with info in which slot iDec the decaying particle is stored.

            The routine should return true if it managed the decay and false otherwise, in which case Pythia will try to do the decay itself. This e.g. means you can choose to do some decay channels yourself, and leave others to Pythia. To avoid double-counting, the channels you want to handle should be switched off in the Pythia particle database. In the beginning of the external decay method you should then return false with a probability given by the sum of the branching ratios for those channels you do not want to handle yourself.

            Note that the decay vertex is always set by Pythia, and that B-Bbar oscillations have already been taken into account, if they were switched on. Thus idProd[0] may be the opposite of event[iDec].id(), where the latter provides the code at production.

            A sample test program is available in main17.cc, providing a simple example of how to use this facility. pythia8-8.1.80.orig/phpdoc/EventStatistics.php0000644000175000017500000001565612217615312017470 0ustar sunsun Event Statistics SETTINGS SAVED TO FILE

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            Event Statistics

            At the end of the run you will want to write out the final statistics on number of events generated, the corresponding cross sections and the number of errors encountered. This is done either with the pythia.stat() method or the pythia.statistics() one, assuming pythia is an instance of the Pythia class.The former method is steered entirely by settings values, see ";?>here. The latter, deprecated one instead takes two arguments:

            void Pythia::statistics(bool all = false, bool reset = false)  
            write out statistics on cross sections and errors. This is based on calls to the methods below, for the two kinds of information.
            argument all : if true it allows a more extensive listing than the default one, see multiparton-interactions statistics below.
            argument reset : if true it implies that all counters, e.g on events generated and errors experienced, are reset to zero whenever the routine is called. The default instead is that all stored statistics information is unaffected by the call. Counters are automatically reset in each new Pythia::init() call, however, so the only time the reset option makes a difference is if statistics(...) is called several times in a (sub)run.

            Cross-section statistics

            The ProcessLevel::statistics() method cannot be accessed directly, but only via the Pythia::stat() and Pythia::statistics(...) calls above. When called it will loop over the list of existing processes, and for each write out name, code, the number of tried, selected and accepted events, the cross section and the estimated error on the latter. The three different event numbers are related to the Monte Carlo method used, whereby an initial upper estimate of the cross section is used to select a large number of trial phase-space points, whereof then not all survive. Rejections are normally done by the internal machinery, but can also be obtained by ";?>user hooks. Therefore:
            • tried events reflect the original number of phase-space points probed, as part of the upper estimate;
            • selected events correspond to those that survive the internal Monte-Carlo selection procedure;
            • accepted events are those that also survive the additional user cuts.
            In most runs there would be no user hooks implemented, and then the numbers of selected and of accepted events will agree. Aborted events (see below) usually appear in the selected statistics but not in the accepted one.

            For Les Houches events the total cross section will be correctly displayed; however the (optional) error value will not be used, so that the reported error will be smaller than the correct statistical ones, and often vanish completely. Furthermore, while the number of events is shown for each user process, the cross section is only for the sum of them.

            Error messages

            When Pythia is run, errors may occur, and give rise to warning messages. These may be of varying severity, as follows:
            • Abort means things went seriously wrong, and the initialization or event generation failed. In the former case it is not possible to generate events at all, in the latter the current event is flawed and should be skipped. In either case the respective method, Pythia::init() or Pythia::next(), then also returns the value false. There are occasions where an abort may be deliberate, such as when a file of Les Houches Events is read and the end of the file is reached.
            • Error normally is less severe. Typically the program will back up one step and try again. There are cases where this is not possible, in particular during the initialization and the generation of a hard process, and then the error may be followed by an abort as a direct consequence (with two separate messages).
            • Warning is even less severe. In some cases the program will try again, with good chances of success, in others no measure at all need to be taken.

            The error messages is handled by a small part of the Info class. It is handed any abort, error or warning messages during the event generation phase, and will store each distinct message, with a counter for how many times it is issued. Thus it is possible to limit the number of identical messages issued, currently hardcoded so that each kind of error message is only printed once (static const int TIMESTOPRINT = 1). This can be overridden by the calling routine, so that all messages of this kind are shown, which is particularly relevant for the initialization stage. The summary table printed by Pythia::statistics() provides a table with all the different messages issued, in alphabetical order, with the total number of times each was generated.

            Multiparton-interactions statistics

            If you call Pythia::statistics(true), i.e. with the first optional argument true, also statistics on multiparton interactions is printed, comprising a list of all allowed subprocesses with how many times each of them has been generated. For the nondiffractive process this also includes the hardest interaction, while else the hardest process is excluded from the statistics. (This is because the hardest process is of the same character and generated by the same machinery in the former case but not in the latter. Also, for the former case only, the standard statistics listing only lists nondiffractive as one single process, i.e. does not further specify the character of the hardest subprocess, so there is not any overlap between the two.) pythia8-8.1.80.orig/phpdoc/ParticleProperties.php0000644000175000017500000011105212217615312020137 0ustar sunsun Particle Properties SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Particle Properties

            A Particle corresponds to one entry/slot in the event record. Its properties therefore is a mix of ones belonging to a particle-as-such, like its identity code or four-momentum, and ones related to the event-as-a-whole, like which mother it has.

            What is stored for each particle is

            • the identity code,
            • the status code,
            • two mother indices,
            • two daughter indices,
            • a colour and an anticolour index,
            • the four-momentum and mass,
            • the scale at which the particle was produced (optional),
            • the polarization/spin/helicity of the particle (optional),
            • the production vertex and proper lifetime (optional),
            • a pointer to the particle kind in the particle data table, and
            • a pointer to the event the particle belongs to.
            From these, a number of further quantities may be derived.

            Basic output methods

            The following member functions can be used to extract the most important information:

            int Particle::id()  
            the identity of a particle, according to the PDG particle codes [Yao06].

            int Particle::status()  
            status code. The status code includes information on how a particle was produced, i.e. where in the program execution it was inserted into the event record, and why. It also tells whether the particle is still present or not. It does not tell how a particle disappeared, whether by a decay, a shower branching, a hadronization process, or whatever, but this is implicit in the status code of its daughter(s). The basic scheme is:

            • status = +- (10 * i + j)
            • + : still remaining particles
            • - : decayed/branched/fragmented/... and not remaining
            • i = 1 - 9 : stage of event generation inside PYTHIA
            • i = 10 -19 : reserved for future expansion
            • i >= 20 : free for add-on programs
            • j = 1 - 9 : further specification
            In detail, the list of used or foreseen status codes is:
            • 11 - 19 : beam particles
              • 11 : the event as a whole
              • 12 : incoming beam
              • 13 : incoming beam-inside-beam (e.g. gamma inside e)
              • 14 : outgoing elastically scattered
              • 15 : outgoing diffractively scattered
            • 21 - 29 : particles of the hardest subprocess
              • 21 : incoming
              • 22 : intermediate (intended to have preserved mass)
              • 23 : outgoing
            • 31 - 39 : particles of subsequent subprocesses
              • 31 : incoming
              • 32 : intermediate (intended to have preserved mass)
              • 33 : outgoing
              • 34 : incoming that has already scattered
            • 41 - 49 : particles produced by initial-state-showers
              • 41 : incoming on spacelike main branch
              • 42 : incoming copy of recoiler
              • 43 : outgoing produced by a branching
              • 44 : outgoing shifted by a branching
              • 45 : incoming rescattered parton, with changed kinematics owing to ISR in the mother system (cf. status 34)
              • 46 : incoming copy of recoiler when this is a rescattered parton (cf. status 42)
              • 47 : a W or Z gauge boson produced in the shower evolution
            • 51 - 59 : particles produced by final-state-showers
              • 51 : outgoing produced by parton branching
              • 52 : outgoing copy of recoiler, with changed momentum
              • 53 : copy of recoiler when this is incoming parton, with changed momentum
              • 54 : copy of a recoiler, when in the initial state of a different system from the radiator
              • 55 : copy of a recoiler, when in the final state of a different system from the radiator
              • 56 : a W or Z gauge boson produced in the shower evolution
            • 61 - 69 : particles produced by beam-remnant treatment
              • 61 : incoming subprocess particle with primordial kT included
              • 62 : outgoing subprocess particle with primordial kT included
              • 63 : outgoing beam remnant
            • 71 - 79 : partons in preparation of hadronization process
              • 71 : copied partons to collect into contiguous colour singlet
              • 72 : copied recoiling singlet when ministring collapses to one hadron and momentum has to be reshuffled
              • 73 : combination of very nearby partons into one
              • 74 : combination of two junction quarks (+ nearby gluons) to a diquark
              • 75 : gluons split to decouple a junction-antijunction pair
              • 76 : partons with momentum shuffled to decouple a junction-antijunction pair
              • 77 : temporary opposing parton when fragmenting first two strings in to junction (should disappear again)
              • 78 : temporary combined diquark end when fragmenting last string in to junction (should disappear again)
            • 81 - 89 : primary hadrons produced by hadronization process
              • 81 : from ministring into one hadron
              • 82 : from ministring into two hadrons
              • 83, 84 : from normal string (the difference between the two is technical, whether fragmented off from the top of the string system or from the bottom, useful for debug only)
              • 85, 86 : primary produced hadrons in junction fragmentation of the first two string legs in to the junction, in order of treatment
            • 91 - 99 : particles produced in decay process, or by Bose-Einstein effects
              • 91 : normal decay products
              • 92 : decay products after oscillation B0 <-> B0bar or B_s0 <-> B_s0bar
              • 93, 94 : decay handled by external program, normally or with oscillation
              • 99 : particles with momenta shifted by Bose-Einstein effects (not a proper decay, but bookkept as an 1 -> 1 such, happening after decays of short-lived resonances but before decays of longer-lived particles)
            • 101 - 109 : particles in the handling of R-hadron production and decay, i.e. long-lived (or stable) particles containing a very heavy flavour
              • 101 : when a string system contains two such long-lived particles, the system is split up by the production of a new q-qbar pair (bookkept as decay chains that seemingly need not conserve flavour etc., but do when considered together)
              • 102 : partons rearranged from the long-lived particle end to prepare for fragmentation from this end
              • 103 : intermediate "half-R-hadron" formed when a colour octet particle (like the gluino) has been fragmented on one side, but not yet on the other
              • 104 : an R-hadron
              • 105 : partons or particles formed together with the R-hadron during the fragmentation treatment
              • 106 : subdivision of an R-hadron into its flavour content, with momentum split accordingly, in preparation of the decay of the heavy new particle, if it is unstable
              • 107 : two temporary leftover gluons joined into one in the formation of a gluino-gluon R-hadron.
            • 111 - 199 : reserved for future expansion
            • 201 - : free to be used by anybody

            int Particle::mother1()  
            int Particle::mother2()  
            the indices in the event record where the first and last mothers are stored, if any. There are five allowed combinations of mother1 and mother2:

            1. mother1 = mother2 = 0: for lines 0 - 2, where line 0 represents the event as a whole, and 1 and 2 the two incoming beam particles;
            2. mother1 = mother2 > 0: the particle is a "carbon copy" of its mother, but with changed momentum as a "recoil" effect, e.g. in a shower;
            3. mother1 > 0, mother2 = 0: the "normal" mother case, where it is meaningful to speak of one single mother to several products, in a shower or decay;
            4. mother1 < mother2, both > 0, for abs(status) = 81 - 86: primary hadrons produced from the fragmentation of a string spanning the range from mother1 to mother2, so that all partons in this range should be considered mothers; and analogously for abs(status) = 101 - 106, the formation of R-hadrons;
            5. mother1 < mother2, both > 0, except case 4: particles with two truly different mothers, in particular the particles emerging from a hard 2 -> n interaction.

            Note 1: in backwards evolution of initial-state showers, the mother may well appear below the daughter in the event record.
            Note 2: the motherList() method below returns a vector of all the mothers, providing a uniform representation for all five cases.

            int Particle::daughter1()  
            int Particle::daughter2()  
            the indices in the event record where the first and last daughters are stored, if any. There are five allowed combinations of daughter1 and daughter2:

            1. daughter1 = daughter2 = 0: there are no daughters (so far);
            2. daughter1 = daughter2 > 0: the particle has a "carbon copy" as its sole daughter, but with changed momentum as a "recoil" effect, e.g. in a shower;
            3. daughter1 > 0, daughter2 = 0: each of the incoming beams has only (at most) one daughter, namely the initiator parton of the hardest interaction; further, in a 2 -> 1 hard interaction, like q qbar -> Z^0, or in a clustering of two nearby partons, the initial partons only have this one daughter;
            4. daughter1 < daughter2, both > 0: the particle has a range of decay products from daughter1 to daughter2;
            5. daughter2 < daughter1, both > 0: the particle has two separately stored decay products (e.g. in backwards evolution of initial-state showers).

            Note 1: in backwards evolution of initial-state showers, the daughters may well appear below the mother in the event record.
            Note 2: the mother-daughter relation normally is reciprocal, but not always. An example is hadron beams (indices 1 and 2), where each beam remnant and the initiator of each multiparton interaction has the respective beam as mother, but the beam itself only has the initiator of the hardest interaction as daughter.
            Note 3: the daughterList() method below returns a vector of all the daughters, providing a uniform representation for all five cases. With this method, also all the daughters of the beams are caught, with the initiators of the basic process given first, while the rest are in no guaranteed order (since they are found by a scanning of the event record for particles with the beam as mother, with no further information).

            int Particle::col()  
            int Particle::acol()  
            the colour and anticolour tags, Les Houches Accord [Boo01] style (starting from tag 101 by default, see below).
            Note: in the preliminary implementation of colour sextets (exotic BSM particles) that exists since PYTHIA 8.150, a negative anticolour tag is interpreted as an additional positive colour tag, and vice versa.

            double Particle::px()  
            double Particle::py()  
            double Particle::pz()  
            double Particle::e()  
            the particle four-momentum components.

            Vec4 Particle::p()  
            the particle four-momentum vector, with components as above.

            double Particle::m()  
            the particle mass, stored with a minus sign (times the absolute value) for spacelike virtual particles.

            double Particle::scale()  
            the scale at which a parton was produced, which can be used to restrict its radiation to lower scales in subsequent steps of the shower evolution. Note that scale is linear in momenta, not quadratic (i.e. Q, not Q^2).

            double Particle::pol()  
            the polarization/spin/helicity of a particle. Currently Pythia does not use this variable for any internal operations, so its meaning is not uniquely defined. The LHA standard sets SPINUP to be the cosine of the angle between the spin vector and the 3-momentum of the decaying particle in the lab frame, i.e. restricted to be between +1 and -1. A more convenient choice could be the same quantity in the rest frame of the particle production, either the hard subprocess or the mother particle of a decay. Unknown or unpolarized particles should be assigned the value 9.

            double Particle::xProd()  
            double Particle::yProd()  
            double Particle::zProd()  
            double Particle::tProd()  
            the production vertex coordinates, in mm or mm/c.

            Vec4 Particle::vProd()  
            The production vertex four-vector. Note that the components of a Vec4 are named px(), py(), pz() and e() which of course then should be reinterpreted as above.

            double Particle::tau()  
            the proper lifetime, in mm/c. It is assigned for all hadrons with positive nominal tau, tau_0 > 0, because it can be used by PYTHIA to decide whether a particle should or should not be allowed to decay, e.g. based on the decay vertex distance to the primary interaction vertex.

            Input methods

            The same method names as above are also overloaded in versions that set values. These have an input argument of the same type as the respective output above, and are of type void.

            There are also a few alternative methods for input:

            void Particle::statusPos()  
            void Particle::statusNeg()  
            sets the status sign positive or negative, without changing the absolute value.

            void Particle::statusCode(int code)  
            changes the absolute value but retains the original sign.

            void Particle::mothers(int mother1, int mother2)  
            sets both mothers in one go.

            void Particle::daughters(int daughter1, int daughter2)  
            sets both daughters in one go.

            void Particle::cols(int col, int acol)  
            sets both colour and anticolour in one go.

            void Particle::p(double px, double py, double pz, double e)  
            sets the four-momentum components in one go.

            void Particle::vProd(double xProd, double yProd, double zProd, double tProd)  
            sets the production vertex components in one go.

            Further output methods

            In addition, a number of derived quantities can easily be obtained, but cannot be set, such as:

            int Particle::idAbs()  
            the absolute value of the particle identity code.

            int Particle::statusAbs()  
            the absolute value of the status code.

            bool Particle::isFinal()  
            true for a remaining particle, i.e. one with positive status code, else false. Thus, after an event has been fully generated, it separates the final-state particles from intermediate-stage ones. (If used earlier in the generation process, a particle then considered final may well decay later.)

            bool Particle::isRescatteredIncoming()  
            true for particles with a status code -34, -45, -46 or -54, else false. This singles out partons that have been created in a previous scattering but here are bookkept as belonging to the incoming state of another scattering.

            bool Particle::hasVertex()  
            production vertex has been set; if false then production at the origin is assumed.

            double Particle::m2()  
            squared mass, which can be negative for spacelike partons.

            double Particle::mCalc()  
            double Particle::m2Calc()  
            (squared) mass calculated from the four-momentum; should agree with m(), m2() up to roundoff. Negative for spacelike virtualities.

            double Particle::eCalc()  
            energy calculated from the mass and three-momentum; should agree with e() up to roundoff. For spacelike partons a positive-energy solution is picked. This need not be the correct one, so it is recommended not to use the method in such cases.

            double Particle::pT()  
            double Particle::pT2()  
            (squared) transverse momentum.

            double Particle::mT()  
            double Particle::mT2()  
            (squared) transverse mass. If m_T^2 is negative, which can happen for a spacelike parton, then mT() returns -sqrt(-m_T^2), by analogy with the negative sign used to store spacelike masses.

            double Particle::pAbs()  
            double Particle::pAbs2()  
            (squared) three-momentum size.

            double Particle::eT()  
            double Particle::eT2()  
            (squared) transverse energy, eT = e * sin(theta) = e * pT / pAbs.

            double Particle::theta()  
            double Particle::phi()  
            polar and azimuthal angle.

            double Particle::thetaXZ()  
            angle in the (p_x, p_z) plane, between -pi and +pi, with 0 along the +z axis

            double Particle::pPos()  
            double Particle::pNeg()  
            E +- p_z.

            double Particle::y()  
            double Particle::eta()  
            rapidity and pseudorapidity.

            double Particle::xDec()  
            double Particle::yDec()  
            double Particle::zDec()  
            double Particle::tDec()  
            Vec4 Particle::vDec()  
            the decay vertex coordinates, in mm or mm/c. This decay vertex is calculated from the production vertex, the proper lifetime and the four-momentum assuming no magnetic field or other detector interference. It can be used to decide whether a decay should be performed or not, and thus is defined also for particles which PYTHIA did not let decay.

            Not part of the Particle class proper, but obviously tightly linked, are the two methods

            double m(const Particle& pp1, const Particle& pp2)  
            double m2(const Particle& pp1, const Particle& pp2)  
            the (squared) invariant mass of two particles.

            Properties of the particle species

            Each Particle contains a pointer to the respective ParticleDataEntry object in the ";?>particle data tables. This gives access to properties of the particle species as such. It is there mainly for convenience, and should be thrown if an event is written to disk, to avoid any problems of object persistency. Should an event later be read back in, the pointer will be recreated from the id code if the normal input methods are used. (Use the ";?>Event::restorePtrs() method if your persistency scheme bypasses the normal methods.) This pointer is used by the following member functions:

            string Particle::name()  
            the name of the particle.

            string Particle::nameWithStatus()  
            as above, but for negative-status particles the name is given in brackets to emphasize that they are intermediaries.

            int Particle::spinType()  
            2 *spin + 1 when defined, else 0.

            double Particle::charge()  
            int Particle::chargeType()  
            charge, and three times it to make an integer.

            bool Particle::isCharged()  
            bool Particle::isNeutral()  
            charge different from or equal to 0.

            int Particle::colType()  
            0 for colour singlets, 1 for triplets, -1 for antitriplets and 2 for octets. (A preliminary implementation of colour sextets also exists, using 3 for sextets and -3 for antisextets.)

            double Particle::m0()  
            the nominal mass of the particle, according to the data tables.

            double Particle::mWidth()  
            double Particle::mMin()  
            double Particle::mMax()  
            the width of the particle, and the minimum and maximum allowed mass value for particles with a width, according to the data tables.

            double Particle::mSel()  
            the mass of the particle, picked according to a Breit-Wigner distribution for particles with width. It is different each time called, and is therefore only used once per particle to set its mass m().

            double Particle::constituentMass()  
            will give the constituent masses for quarks and diquarks, else the same masses as with m0().

            double Particle::tau0()  
            the nominal lifetime tau_0 > 0, in mm/c, of the particle species. It is used to assign the actual lifetime tau.

            bool Particle::mayDecay()  
            flag whether particle has been declared unstable or not, offering the main user switch to select which particle species to decay.

            bool Particle::canDecay()  
            flag whether decay modes have been declared for a particle, so that it could be decayed, should that be requested.

            bool Particle::doExternalDecay()  
            particles that are decayed by an external program.

            bool Particle::isResonance()  
            particles where the decay is to be treated as part of the hard process, typically with nominal mass above 20 GeV (W^+-, Z^0, t, ...).

            bool Particle::isVisible()  
            particles with strong or electric charge, or composed of ones having it, which thereby should be considered visible in a normal detector.

            bool Particle::isLepton()  
            true for a lepton or an antilepton (including neutrinos).

            bool Particle::isQuark()  
            true for a quark or an antiquark.

            bool Particle::isGluon()  
            true for a gluon.

            bool Particle::isDiquark()  
            true for a diquark or an antidiquark.

            bool Particle::isParton()  
            true for a gluon, a quark or antiquark up to the b (but excluding top), and a diquark or antidiquark consisting of quarks up to the b.

            bool Particle::isHadron()  
            true for a hadron (made up out of normal quarks and gluons, i.e. not for R-hadrons and other exotic states).

            ParticleDataEntry& particleDataEntry()  
            a reference to the ParticleDataEntry.

            Methods that may access the event the particle belongs to

            A particle can be created on its own. When inserted into an event record, it obtains a pointer to that event-as-a-whole. It is then possible to use methods that do not make sense for a particle in isolation. These methods are listed below. Whenever the pointer to the event is not defined, these will return an appropriate "null" value, this being -1 for an integer, false for a bool, and empty for a vector, unless otherwise specified.

            void Particle::index()  
            the index of the particle itself in the event record.

            int Particle::statusHepMC()  
            returns the status code according to the HepMC conventions agreed in February 2009. This convention does not preserve the full information provided by the internal PYTHIA status code, as obtained by Particle::status(), but comes reasonably close. The allowed output values are:

            • 0 : an empty entry, with no meaningful information and therefore to be skipped unconditionally;
            • 1 : a final-state particle, i.e. a particle that is not decayed further by the generator (may also include unstable particles that are to be decayed later, as part of the detector simulation);
            • 2 : a decayed Standard Model hadron or tau or mu lepton, excepting virtual intermediate states thereof (i.e. the particle must undergo a normal decay, not e.g. a shower branching);
            • 3 : a documentation entry (not used in PYTHIA);
            • 4 : an incoming beam particle;
            • 11 - 200 : an intermediate (decayed/branched/...) particle that does not fulfill the criteria of status code 2, with a generator-dependent classification of its nature; in PYTHIA the absolute value of the normal status code is used.

            Note: for a particle without a properly set pointer to its event, codes 1 and 4 can still be inferred from its status code, while everythg else is assigned code 0.

            int Particle::iTopCopy()  
            int Particle::iBotCopy()  
            are used to trace carbon copies of the particle up to its top mother or down to its bottom daughter. If there are no such carbon copies, the index of the particle itself will be returned. A carbon copy is when the "same" particle appears several times in the event record, but with changed momentum owing to recoil effects.

            int Particle::iTopCopyId()  
            int Particle::iBotCopyId()  
            also trace top mother and bottom daughter, but do not require carbon copies, only that one can find an unbroken chain, of mothers or daughters, with the same flavour id code. When it encounters ambiguities, say a g -> g g branching or a u u -> u u hard scattering, it will stop the tracing and return the current position. It can be confused by nontrivial flavour changes, e.g. a hard process u d -> d u by W^+- exchange will give the wrong answer. These methods therefore are of limited use for common particles, in particular for the gluon, but should work well for "rare" particles.

            vector<int> Particle::sisterList(bool traceTopBot = false)  
            returns a vector of all the sister indices of the particle, i.e. all the daughters of the first mother, except the particle itself. If the argument traceTopBot = true the particle is first traced up with iTopCopy() before its mother is found, and then all the particles in the daughterList() of this mother are traced down with iBotCopy(), omitting the original particle itself. The method is not meaningful for the 0 entry, with status code -11, and there returns an empty list.

            bool Particle::isAncestor(int iAncestor)  
            traces the particle upwards through mother, grandmother, and so on, until either iAncestor is found or the top of the record is reached. Normally one unique mother is required, as is the case e.g. in decay chains or in parton showers, so that e.g. the tracing through a hard scattering would not work. For hadronization, first-rank hadrons are identified with the respective string endpoint quark, which may be useful e.g. for b physics, while higher-rank hadrons give false. Currently also ministrings that collapsed to one single hadron and junction topologies give false.

            bool Particle::undoDecay()  
            removes the decay chain of the particle and thus restores it to its undecayed state. It is only intended for "normal" particle decay chains, and will return false in other cases, notably if the particle is coloured. The procedure would not work if non-local momentum shifts have been performed, such as with a Bose-Einstein shift procedure (or for a dipole shower recoiler). As the decay products are erased from the event record, mother and daughter indices are updated to retain a correct history for the remaining particles.

            Methods that perform operations

            There are some further methods, some of them inherited from Vec4, to modify the properties of a particle. They are of little interest to the normal user.

            void Particle::rescale3(double fac)  
            multiply the three-momentum components by fac.

            void Particle::rescale4(double fac)  
            multiply the four-momentum components by fac.

            void Particle::rescale5(double fac)  
            multiply the four-momentum components and the mass by fac.

            void Particle::rot(double theta, double phi)  
            rotate three-momentum and production vertex by these polar and azimuthal angles.

            void Particle::bst(double betaX, double betaY, double betaZ)  
            boost four-momentum and production vertex by this three-vector.

            void Particle::bst(double betaX, double betaY, double betaZ, double gamma)  
            as above, but also input the gamma value, to reduce roundoff errors.

            void Particle::bst(const Vec4& pBst)  
            boost four-momentum and production vertex by beta = (px/e, py/e, pz/e).

            void Particle::bst(const Vec4& pBst, double mBst)  
            as above, but also use gamma> = e/m to reduce roundoff errors.

            void Particle::bstback(const Vec4& pBst)  
            void Particle::bstback(const Vec4& pBst, double mBst)  
            as above, but with sign of boost flipped.

            void Particle::rotbst(const RotBstMatrix& M)  
            combined rotation and boost of the four-momentum and production vertex.

            void Particle::offsetHistory( int minMother, int addMother, int minDaughter, int addDaughter))  
            add a positive offset to the mother and daughter indices, i.e. if mother1 is above minMother then addMother is added to it, same with mother2, if daughter1 is above minDaughter then addDaughter is added to it, same with daughter2.

            void Particle::offsetCol( int addCol)  
            add a positive offset to colour indices, i.e. if col is positive then addCol is added to it, same with acol.

            Constructors and operators

            Normally a user would not need to create new particles. However, if necessary, the following constructors and methods may be of interest.

            Particle::Particle()  
            constructs an empty particle, i.e. where all properties have been set 0 or equivalent.

            Particle::Particle(int id, int status = 0, int mother1 = 0, int mother2 = 0, int daughter1 = 0, int daughter2 = 0, int col = 0, int acol = 0, double px = 0., double py = 0., double pz = 0., double e = 0., double m = 0., double scale = 0., double pol = 9.)  
            constructs a particle with the input properties provided, and non-provided ones set 0 (9 for pol).

            Particle::Particle(int id, int status, int mother1, int mother2, int daughter1, int daughter2, int col, int acol, Vec4 p, double m = 0., double scale = 0., double pol = 9.)  
            constructs a particle with the input properties provided, and non-provided ones set 0 (9 for pol).

            Particle::Particle(const Particle& pt)  
            constructs an particle that is a copy of the input one.

            Particle& Particle::operator=(const Particle& pt)  
            copies the input particle.

            void Particle::setEvtPtr(Event* evtPtr)  
            sets the pointer to the Event object the particle belongs to. This method is automatically called when a particle is appended to an event record. Also calls setPDEPtr below.

            void Particle::setPDEPtr(ParticleDataEntry* pdePtr = 0)  
            sets the pointer to the ParticleDataEntry object of the particle, based on its current id code. If the particle belongs to an event there is no need to provide the input argument. As explained above, a valid ParticleDataEntry pointer is needed for the methods that provide information generic to the particle species. pythia8-8.1.80.orig/phpdoc/SemiInternalProcesses.php0000644000175000017500000010273312217615312020606 0ustar sunsun Semi-Internal Processes SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Semi-Internal Processes

            Normally users are expected to implement new processes via the ";?>Les Houches Accord. Then you do all flavour, colour and phase-space selection externally, before your process-level events are input for further processing by PYTHIA. However, it is also possible to implement a new process in exactly the same way as the internal PYTHIA ones, thus making use of the internal phase space selection machinery to sample an externally provided cross-section expression. The MadGraph 5 program [Alw11] allows you to do exactly that, i.e. it can be used to generate C++ code that can be linked into the existing PYTHIA framework, see ";?>here.

            Should you decide to go ahead on your own, this page gives a brief summary how to do that. If you additionally want to introduce a new resonance species, with its own internal width calculations, you will find further instructions ";?>here. It is strongly recommended to shop around for a similar process that has already been implemented, and to use that existing code as a template. Look for processes with the same combinations of incoming flavours and colour flows, rather than the shape of the cross section itself. With a reasonable such match the task should be of medium difficulty, without it more demanding.

            PYTHIA is rather good at handling the phase space of 2 -> 1 and 2 -> 2 processes, is more primitive for 2 -> 3 ones and does not at all address higher multiplicities. This limits the set of processes that you can implement in this framework. The produced particles may be resonances, however, so it is possible to end up with bigger "final" multiplicities through sequential decays, and to include further matrix-element weighting in those decays.

            There are three steps involved in implementing a process:

            1. making use of the PYTHIA-provided kinematics information to calculate the relevant cross section,
            2. writing a new class, where the matrix elements are implemented, including information on incoming and outgoing flavours and colours, and
            3. making the process available.
            We consider these aspects in turn. An example where it all comes together is found in main22.cc.

            The Cross Section Calculation

            The key method for the cross section calculation is SigmaProcess::sigmaHat(), described below. At the point when it is called, the kinematics has already been set up, and from these phase space variables the differential cross section is to be calculated.

            For a 2 -> 1 process, the returned value should be sigmaHat(sHat), where mH (= mHat), sH (= sHat) and sH2 (= sHat^2) are available to be used. Incoming partons are massless. Overload the convertM2() method below if you instead plan to return |M|^2.

            For a 2 -> 2 process, instead d(sigmaHat)/d(tHat) should be returned, based on provided mH, sH, sH2, tH, tH2, uH, uH2, m3, s3, m4, s4 and pT2 values (s3 = m3*m3 etc.). Incoming partons are massless. Overload the convertM2() method below if you instead plan to return |M|^2.

            For a 2 -> 3 process, instead |M|^2 should be returned, with normalization such that |M|^2 / (2 sHat) integrated over the three-body phase space gives the cross section. Here no standard set of Mandelstam-style variables exists. Instead the obvious ones, mH, sH, m3, s3, m4, s4, m5, s5, are complemented by the four-vectors p3cm, p4cm, p5cm, from which further invariants may be calculated. The four-vectors are defined in the CM frame of the subcollision, with massless incoming partons along the +-z axis.

            In either case, alpha_s and alpha_em have already been calculated, and are stored in alpS and alpEM. Also other standard variables may be used, like CoupEW::sin2thetaW(), and related flavour-dependent vector and axial couplings in CoupEW and CKM combinations in VCKM.

            In case some of the final-state particles are resonances, their squared masses have already been selected according to a Breit-Wigner with a linearly running width Gamma(m) = Gamma(m_0) * m / m_0. More precisely, the mass spectrum is weighted according to w_BW(m^2) d(m^2), where
            w_BW(m^2) = (1/pi) * (m * Gamma(m)) / ( (m^2 - m_0^2)^2 + (m * Gamma(m))^2 ) .
            If you would like to have another expression, the above weights are stored in runBW3, runBW4 and runBW5, respectively. If you divide out one of these factors, you just remain with a phase space selection d(m^2) for this particle, and can multiply on your desired shape factor instead. Unfortunately, the Monte Carlo efficiency will drop if your new mass distribution differs dramatically from the input one. Therefore it does make sense to adjust the database value of the width to be slightly (but not too much) broader than the distribution you have in mind. Also note that, already by default, the wings of the Breit-Wigner are oversampled (with a compensating lower internal weight) by partly sampling like (a + b/m^2 + c/m^4) d(m^2), where the last term is only used for gamma^*/Z^0.

            As alternative to the kinematics variables defined above, also the two arrays mME[5] and pME[5], for masses and four-momenta, respectively, can be used for cross-section calculations. Here indices 0 and 1 are the two incoming beams, and 2 and onwards the outgoing particles. Note that this differs by one step from the normal internal labeling, where slot 0 is left empty. The four-momenta are defined in the rest frame of the subcollision, with the incoming partons along the +-z direction. The kinematics need not agree with the "correct" one stored in the event record, for three reasons.
            1) Gauge invariance forces matrix-element calculations to use the same masses for incoming as outgoing legs of a particle species, say b quarks. Therefore the kinematics of the two incoming partons is recalculated, relative to the normal event record, to put the partons on the mass shell. (Note that initial masses is a technical issue, not the correct physics picture: the incoming partons are likely to be spacelike virtual rather than on the mass shell.)
            2) In principle each fermion flavour has to be treated separately, owing to a different mass. However, in many cases fermions can be assumed massless, which speeds up the calculations, and further gains occur if then different flavours can use the same cross-section expression. In MadGraph the default is that fermions up to and including the c quark and the mu lepton are considered massless, while the b quark and the tau lepton are considered massive. This can be modified however, and below we provide four flags that can be used to consider the "borderline" fermions either as massless or as massive when matrix elements are evaluated, to match the assumptions made for the matrix elements themselves.
            3) For 2 -> 2 and 2 -> 3 processes of massive identical particles (or antiparticles) in the final state, such as t tbar or W^+ W^-, the kinematics is here adjusted so that the two or three particles have the same mass, formed as a suitable average of the actual Breit-Wigner-distributed masses. This allows the evaluation of matrix-element expressions that only have meaning if the two/three have the same mass.
            Thus the mass array mME[5] and the four-momentum array pME[5] present values both for initial- and final-state particles based on these mass principles suited for matrix-element input. Note that these variables therefore differ from the kinematics stored in the event record proper, where incoming fermions are always massless and outgoing resonances have independent Breit-Wigner mass distributions.
            The conversion from the normal to the special kinematics is done by calling the setupForME() method. This you have to do yourself in the SigmaHat() member of your derived class. Alternatively it could be done in SigmaKin(), i.e. before the loop over incoming flavours, but then these would be considered massless. The identity of final-state particles is obtained from the id3Mass(), id4Mass() and id5Mass() methods. Should the conversion to mME[5] and pME[5] not work, setupForME() will return false, and then the cross section should be put zero.

            SigmaProcess:cMassiveME On Off   (default = off)
            Let the c quark be massive or not in the kinematics set up for external matrix-element evaluation.

            SigmaProcess:bMassiveME On Off   (default = on)
            Let the b quark be massive or not in the kinematics set up for external matrix-element evaluation.

            SigmaProcess:muMassiveME On Off   (default = off)
            Let the mu lepton be massive or not in the kinematics set up for external matrix-element evaluation.

            SigmaProcess:tauMassiveME On Off   (default = on)
            Let the tau lepton be massive or not in the kinematics set up for external matrix-element evaluation.

            The Cross Section Class

            The matrix-element information has to be encoded in a new class. The relevant code could either be put before the main program in the same file, or be stored separately, e.g. in a matched pair of .h and .cc files. The latter may be more convenient, in particular if the cross sections are lengthy, or if you intend to build up your own little process library, but of course requires that these additional files are correctly compiled and linked.

            The class has to be derived either from Sigma1Process, for 2 -> 1 processes, from Sigma2Process, for 2 -> 2 ones, or from Sigma3Process, for 2 -> 3 ones. (The Sigma0Process class is used for elastic, diffractive and minimum-bias events, and is not recommended for use beyond that.) These are in their turn derived from the SigmaProcess base class.

            The class can implement a number of methods. Some of these are compulsory, others strongly recommended, and the rest are to be used only when the need arises to override the default behaviour. The methods are:

            A constructor for the derived class obviously must be available. Here you are quite free to allow a list of arguments, to set the parameters of your model, or even to create a set of closely related but distinct processes. For instance, g g -> Q Qbar, Q = c or b, is only coded once, and then the constructor takes the quark code (4 or 5) as argument, to allow the proper amount of differentiation.

            A destructor is only needed if you plan to delete the process before the natural end of the run, and require some special behaviour at that point. If you call such a destructor you will leave a pointer dangling inside the Pythia object you gave it in to, if that still exists.

            void SigmaProcess::initProc()  
            is called once during initialization, and can then be used to set up parameters, such as masses and couplings, and perform calculations that need not be repeated for each new event, thereby saving time. This method needs not be implemented, since in principle all calculations can be done in sigmaHat below.

            void SigmaProcess::sigmaKin()  
            is called once a kinematical configuration has been determined, but before the two incoming flavours are known. This routine can therefore be used to perform calculations that otherwise might have to be repeated over and over again in sigmaHat below. For instance a flavour-independent cross section calculation for a q g initial state would be repeated 20 times in sigmaHat, five times for the five quark flavours allowed in the incoming beams, times twice to include antiquarks, times twice since the (anti)quark could be in either of the two beams. You could therefore calculate the result once only and store it as a private data member of the class. It is optional whether you want to use this method, however, or put everything in sigmaHat.

            double SigmaProcess::sigmaHat()  
            is the key method for cross section calculations and returns a cross section value, as described in the previous section. It is called when also a preliminary set of incoming flavours has been picked, in addition to the kinematical ones already available for sigmaKin. Typically sigmaHat is called inside a loop over all allowed incoming flavour combinations, stored in id1 and id2, with fixed kinematics, as already illustrated above. The sum over the different flavour combinations provides the total cross section, while their relative size is used to make a selection of a specific incoming state.

            bool SigmaProcess::setupForME()  
            to be called by the user from inside sigmaHat() (or possibly sigmaKin()) to setup alternative kinematics in the mME[5] and pME[5] arrays, better suited for matrix-element calculations. See the end of the previous section for a more detailed description. Should the method return false then the conversion did not work, and sigmaHat() (or sigmaKin()) should be set to vanish.

            void SigmaProcess::setIdColAcol()  
            is called only once an initial state and a kinematical configuration has been picked. This routine must set the complete flavour information and the colour flow of the process. This may involve further random choices, between different possible final-state flavours or between possible competing colour flows. Private data members of the class may be used to retain some information from the previous steps above.
            When this routine is called the two incoming flavours have already been selected and are available in id1 and id2, whereas the one, two or three outgoing ones either are fixed for a given process or can be determined from the instate (e.g. whether a W^+ or W^- was produced). There is also a standard method in VCKM to pick a final flavour from an initial one with CKM mixing. Once you have figured out the value of id3 and, the case being, id4 and id5, you store these values permanently by a call setId( id1, id2, id3, id4, id5), where the last two may be omitted if irrelevant.
            Correspondingly, the colours are stored with setColAcol( col1, acol1, col2, acol2, col3, acol3, col4, acol4, col5, acol5), where the final ones may be omitted if irrelevant. Les Houches style colour tags are used, but starting with number 1 (and later shifted by the currently requested offset). The input is grouped particle by particle, with the colour index before the anticolour one. You may need to select colour flow dynamically, depending on the kinematics, when several distinct possibilities exist. Trivial operations, like swapping colours and anticolours, can be done with existing methods.
            When the id3Mass() and id4Mass() methods have been used, the order of the outgoing particles may be inconsistent with the way the tHat and uHat variables have been defined. A typical example would be a process like q g -> q' W with tHat defined between incoming and outgoing quark, but where id3Mass() = 24 and so the process is to be stored as q g -> W q'. One should then put the variable swapTU = true in setIdColAcol() for each event where the tHat and uHat variables should be swapped before the event kinematics is reconstructed. This variable is automatically restored to false for each new event.

            double SigmaProcess::weightDecayFlav( Event& process)  
            is called to allow a reweighting of the simultaneous flavour choices of resonance decay products. Is currently only used for the q qbar -> gamma*/Z^0 gamma*/Z^0 process, and will likely not be of interest for you.

            double SigmaProcess::weightDecay( Event& process, int iResBeg, int iResEnd)  
            is called when the basic process has one or several resonances, after each set of related resonances in process[i], iResBeg <= i <= iResEnd, has been allowed to decay. The calculated weight, to be normalized to the range between 0 and 1, is used to decide whether to accept the decay(s) or try for a new decay configuration. The base-class version of this method returns unity, i.e. gives isotropic decays by default. This method may be called repeatedly for a single event. For instance, in q qbar -> H^0 Z^0 with H^0 -> W^+ W^-, a first call would be made after the H^0 and Z^0 decays, and then depend only on the Z^0 decay angles since the H^0 decays isotropically. The second call would be after the W^+ W^- decays and then involve correlations between the four daughter fermions.

            string SigmaProcess::name()  
            returns the name of the process, as you want it to be shown in listings.

            int SigmaProcess::code()  
            returns an integer identifier of the process. This has no internal function, but is only intended as a service for the user to rapidly (and hopefully uniquely) identify which process occurred in a given event. Numbers below 10000 are reserved for internal PYTHIA use.

            string SigmaProcess::inFlux()  
            this string specifies the combinations of incoming partons that are allowed for the process under consideration, and thereby which incoming flavours id1 and id2 the sigmaHat() calls will be looped over. It is always possible to pick a wider flavour selection than strictly required and then put to zero cross sections in the superfluous channels, but of course this may cost some extra execution time. Currently allowed options are:
            * gg: two gluons.
            * qg: one (anti)quark and one gluon.
            * qq: any combination of two quarks, two antiquarks or a quark and an antiquark.
            * qqbar: any combination of a quark and an antiquark; a subset of the qq option.
            * qqbarSame: a quark and its antiquark; a subset of the qqbar option.
            * ff: any combination of two fermions, two antifermions or a fermion and an antifermion; is the same as qq for hadron beams but also allows processes to work with lepton beams.
            * ffbar: any combination of a fermion and an antifermion; is the same as qqbar for hadron beams but also allows processes to work with lepton beams.
            * ffbarSame: a fermion and its antifermion; is the same as qqbarSame for hadron beams but also allows processes to work with lepton beams.
            * ffbarChg: a fermion and an antifermion that combine to give charge +-1.
            * fgm: a fermion and a photon (gamma).
            * ggm: a gluon and a photon.
            * gmgm: two photons.

            bool SigmaProcess::convert2mb()  
            it is assumed that cross sections normally come in dimensions such that they, when integrated over the relevant phase space, obtain the dimension GeV^-2, and therefore need to be converted to mb. If the cross section is already encoded as mb then convert2mb() should be overloaded to instead return false.

            bool SigmaProcess::convertM2()  
            it is assumed that 2 -> 1 cross sections are encoded as sigmaHat(sHat), and 2 -> 2 ones as d(sigmaHat)/d(tHat) in the SigmaProcess::sigmaHat() methods. If convertM2() is overloaded to instead return true then the return value is instead assumed to be the squared matrix element |M|^2, and SigmaProcess::sigmaHatWrap(...) converts to sigmaHat(sHat) or d(sigmaHat)/d(tHat), respectively. This switch has no effect on 2 -> 3 processes, where |M|^2 is the only allowed input anyway.

            int SigmaProcess::id3Mass()  
            int SigmaProcess::id4Mass()  
            int SigmaProcess::id5Mass()  
            are the one, two or three final-state flavours, where masses are to be selected before the matrix elements are evaluated. Only the absolute value should be given. For massless particles, like gluons and photons, one need not give anything, i.e. one defaults to 0. The same goes for normal light quarks, where masses presumably are not implemented in the matrix elements. Later on, these quarks can still (automatically) obtain constituent masses, once a u, d or s flavour has been selected.

            int SigmaProcess::resonanceA()  
            int SigmaProcess::resonanceB()  
            are the codes of up to two s-channel resonances contributing to the matrix elements. These are used by the program to improve the phase-space selection efficiency, by partly sampling according to the relevant Breit-Wigner distributions. Massless resonances (the gluon and photon) need not be specified.

            bool SigmaProcess::isSChannel()  
            normally the choice of renormalization and factorization scales in 2 -> 2 and 2 -> 3 processes is based on the assumption that t- and u-channel exchanges dominates the cross section. In cases such as f fbar -> gamma* -> f' fbar' a 2 -> 2 process actually ought to be given scales as a 2 -> 1 one, in the sense that it proceeds entirely through an s-channel resonance. This can be achieved if you override the default false to return true. See further the page on ";?>couplings and scales.

            int SigmaProcess::idSChannel()  
            normally no intermediate state is shown in the event record for 2 -> 2 and 2 -> 3 processes. However, in case that idSChannel is overloaded to return a nonzero value, an intermediate particle with that identity code is inserted into the event record, to make it a 2 -> 1 -> 2 or 2 -> 1 -> 3 process. Thus if both isSChannel and idSChannel are overloaded, a process will behave and look like it proceeded through a resonance. The one difference is that the implementation of the matrix element is not based on the division into a production and a decay of an intermediate resonance, but is directly describing the transition from the initial to the final state.

            int SigmaProcess::isQCD3body()  
            there are two different 3-body phase-space selection machineries, of which the non-QCD one is default. If you overload this method instead the QCD-inspired machinery will be used. The differences between these two is related to which ";?>phase space cuts can be set, and also that the QCD machinery assumes (almost) massless outgoing partons.

            int SigmaProcess::idTchan1()  
            int SigmaProcess::idTchan2()  
            the non-QCD 2 -> 3 phase space selection machinery is rather primitive, as already mentioned. The efficiency can be improved in processes that proceed though t-channel exchanges, such as q qbar' -> H^0 q qbar' via Z^0 Z^0 fusion, if the identity of the t-channel-exchanged particles on the two side of the event are provided. Only the absolute value is of interest.

            double SigmaProcess::tChanFracPow1()  
            double SigmaProcess::tChanFracPow2()  
            in the above kind of 2 -> 3 phase-space selection, the sampling of pT^2 is done with one part flat, one part weighted like 1 / (pT^2 + m_R^2) and one part like 1 / (pT^2 + m_R^2)^2. The above values provide the relative amount put in the latter two channels, respectively, with the first obtaining the rest. Thus the sum of tChanFracPow1() and tChanFracPow2() must be below unity. The final results should be independent of these numbers, but the Monte Carlo efficiency may be quite low for a bad choice. Here m_R is the mass of the exchanged resonance specified by idTchan1() or idTchan2(). Note that the order of the final-state listing is important in the above q qbar' -> H^0 q qbar' example, i.e. the H^0 must be returned by id3Mass(), since it is actually the pT^2 of the latter two that are selected independently, with the first pT then fixed by transverse-momentum conservation.

            bool SigmaProcess::useMirrorWeight()  
            in 2 -> 3 processes the phase space selection used here involves a twofold ambiguity basically corresponding to a flipping of the positions of last two outgoing particles. These are assumed equally likely by default, false, but for processes proceeding entirely through t-channel exchange the Monte Carlo efficiency can be improved by making a preselection based on the relative propagator weights, true.

            int SigmaProcess::gmZmode()  
            allows a possibility to override the global mode ";?>WeakZ0:gmZmode for a specific process. The global mode normally is used to switch off parts of the gamma^*/Z^0 propagator for test purposes. The above local mode is useful for processes where a Z^0 really is that and nothing more, such as q qbar -> H^0 Z^0. The default value -1 returned by gmZmode() ensures that the global mode is used, while 0 gives full gamma^*/Z^0 interference, 1 gamma^* only and 2 Z^0 only.

            Access to a process

            Once you have implemented a class, it is straightforward to make use of it in a run. Assume you have written a new class MySigma, which inherits from Sigma1Process, Sigma2Process or Sigma3Process, which in their turn inherit from SigmaProcess. You then create an instance of this class and hand it in to a pythia object with
                  SigmaProcess* mySigma = new MySigma();
                  pythia.setSigmaPtr( mySigma); 
            
            If you have several processes you can repeat the procedure any number of times. When pythia.init(...) is called these processes are initialized along with any internal processes you may have switched on, and treated in exactly the same manner. The pythia.next() will therefore generate a mix of the different kinds of processes without distinction. See also the ";?>Program Flow description.

            If the code should be of good quality and general usefulness, it would be simple to include it as a permanently available process in the standard program distribution. The final step of that integration ought to be left for the PYTHIA authors, but here is a description of what is required.

            A flag has to be defined, that allows the process to be switched on; by default it should always be off. The name of the flag should be chosen of the type model:process. Here the model would be related to the general scenario considered, e.g. Compositeness, while process would specify instate and outstate, separated by a 2 (= to), e.g. ug2u*g. When several processes are implemented and "belong together" it is also useful to define a model:all switch that affects all the separate processes.

            The flags should normally be stored in the ProcessSelection.xml file or one of its daughters for a specific kind of processes. This is to make them easily found by users. You could create and use your own .xml file, so long as you then add that name to the list of files in the Index.xml file. (If not, the flags would never be created and the program would not work.)

            In the ProcessContainer.c file, the SetupContainers::init() method needs to be expanded to create instances of the processes switched on. This code is fairly repetitive, and should be easy to copy and modify from the code already there. The basic structure is
            (i) check whether a process is requested by the user and, if so,
            (ii) create an instance of the matrix-element class,
            (iii)create a container for the matrix element and its associated phase-space handling, and
            (iv) add the container to the existing process list.

            Two minor variations are possible. One is that a set of related processes are lumped inside the the same initial check, i.e. are switched on all together. The second is that the matrix-element constructor may take arguments, as specified by you (see above). If so, the same basic matrix element may be recycled for a set of related processes, e.g. one for a composite u and one for a composite d. Obviously these variations may be combined. "?>

            pythia8-8.1.80.orig/phpdoc/FourthGenerationProcesses.php0000644000175000017500000003336412217615312021502 0ustar sunsun Fourth-Generation Processes SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Fourth-Generation Processes

            A fourth generation can be accommodated within the Standard Model, without the introduction of any new concepts. Many experimental constraints exist, but it has not been fully excluded. Therefore we offer a simple implementation, along the lines of the top. It could also be useful as a template for studies of other new particles with similar characteristics.

            The fourth generation are given names as in the third, but with a prime, i.e. b' with PDG code 7, t' with code 8, tau' with code 17, and nu'_tau with code 18. Most important for you is to assign a mass hierarchy, to decide which fermions can decay into which. The current implementation assumes that mass splittings are big enough that fourth-generation fermions can decay to third-generation ones by the emission of an on-shell W. To this end, the standard three-generation CKM mixing matrix has been extended to include a fourth generation, see below. Since no mixing has been implemented in the neutrino sector it would be assumed that the lighter of tau' and nu'_tau is stable. No decay modes have been implemented that go beyond the Standard Model, so modifications would be needed if e.g. also SUSY is included in the game.

            Production processes

            1) b' processes

            Different ways to produce b' quarks, singly or in pairs. For a b' t' pair see section 3 below.

            FourthBottom:all On Off   (default = off)
            Common switch for the group of b' production. Also includes the process f fbar' -> t' b'bar in section 3 below.

            FourthBottom:gg2bPrimebPrimebar On Off   (default = off)
            Scatterings g g -> b' b'bar. Code 801.

            FourthBottom:qqbar2bPrimebPrimebar On Off   (default = off)
            Scatterings q qbar -> b' b'bar by gluon exchange. Code 802.

            FourthBottom:qq2bPrimeq(t:W) On Off   (default = off)
            Scatterings q q' -> b' q'' by t-channel exchange of a W^+- boson. Code 803.

            FourthBottom:ffbar2bPrimebPrimebar(s:gmZ) On Off   (default = off)
            Scatterings f fbar -> b' b'bar by s-channel exchange of a gamma^*/Z^0 boson. Code 804.

            FourthBottom:ffbar2bPrimeqbar(s:W) On Off   (default = off)
            Scatterings f fbar' -> b' qbar'' by s-channel exchange of a W^+- boson. Here q'' is either u or c. Code 805.

            FourthBottom:ffbar2bPrimetbar(s:W) On Off   (default = off)
            Scatterings f fbar' -> b' tbar by s-channel exchange of a W^+- boson. Code 806.

            2) t' processes

            Different ways to produce t' quarks, singly or in pairs. For a b' t' pair see section 3 below.

            FourthTop:all On Off   (default = off)
            Common switch for the group of t' production. Also includes the process f fbar' -> t' b'bar in section 3 below.

            FourthTop:gg2tPrimetPrimebar On Off   (default = off)
            Scatterings g g -> t' t'bar. Code 821.

            FourthTop:qqbar2tPrimetPrimebar On Off   (default = off)
            Scatterings q qbar -> t' t'bar by gluon exchange. Code 822.

            FourthTop:qq2tPrimeq(t:W) On Off   (default = off)
            Scatterings q q' -> t' q'' by t-channel exchange of a W^+- boson. Code 823.

            FourthTop:ffbar2tPrimetPrimebar(s:gmZ) On Off   (default = off)
            Scatterings f fbar -> t' t'bar by s-channel exchange of a gamma^*/Z^0 boson. Code 824.

            FourthTop:ffbar2tPrimeqbar(s:W) On Off   (default = off)
            Scatterings f fbar' -> t' qbar'' by s-channel exchange of a W^+- boson. Code 825.

            3) Pair-processes with different flavours

            Different ways to produce two different fourth-generation fermions.

            FourthPair:ffbar2tPrimebPrimebar(s:W) On Off   (default = off)
            Scatterings f fbar' -> t' b'bar by s-channel exchange of a W^+- boson. Code 841.

            FourthPair:ffbar2tauPrimenuPrimebar(s:W) On Off   (default = off)
            Scatterings f fbar' -> tau' nu'_taubar by s-channel exchange of a W^+- boson. Code 842.

            Missing in this list is scatterings q q' -> t' b' by t-channel exchange of a W^+- boson, since currently the matrix element for such processes have not been implemented for two massive particles in the final state. Since this process would involve two CKM-suppressed vertices it ought to be small.

            Parameters

            The Cabibbo-Kobayashi-Maskawa matrix is extended by seven further values. So as not to mess up the Standard Model, the normal 3 * 3 matrix is kept unitary, and so the new off-diagonal elements lead to a slight breaking of this. For exploratory studies this should be good enough; more detailed 4 * 4 tunes to data would only make sense the day there are evidence for the existence of a fourth generation.

            FourthGeneration:VubPrime   (default = 0.001; minimum = 0.0; maximum = 1.0)
            The V_ub' matrix element in the 4 * 4 CKM matrix.

            FourthGeneration:VcbPrime   (default = 0.01; minimum = 0.0; maximum = 1.0)
            The V_cb' matrix element in the 4 * 4 CKM matrix.

            FourthGeneration:VtbPrime   (default = 0.1; minimum = 0.0; maximum = 1.0)
            The V_tb' matrix element in the 4 * 4 CKM matrix.

            FourthGeneration:VtPrimed   (default = 0.001; minimum = 0.0; maximum = 1.0)
            The V_t'd matrix element in the 4 * 4 CKM matrix.

            FourthGeneration:VtPrimes   (default = 0.01; minimum = 0.0; maximum = 1.0)
            The V_t's matrix element in the 4 * 4 CKM matrix.

            FourthGeneration:VtPrimeb   (default = 0.1; minimum = 0.0; maximum = 1.0)
            The V_t'b matrix element in the 4 * 4 CKM matrix.

            FourthGeneration:VtPrimebPrime   (default = 0.99; minimum = 0.0; maximum = 1.0)
            The V_t'b' matrix element in the 4 * 4 CKM matrix. "?>
            pythia8-8.1.80.orig/phpdoc/LeptoquarkProcesses.php0000644000175000017500000001373512217615312020346 0ustar sunsun Leptoquark Processes SETTINGS SAVED TO FILE

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            Leptoquark Processes

            Leptoquarks arise in many scenarios, and can have widely different characteristics, with respect to spin, isospin am d flavour. The current implementation in no sense attempts to exhaust these possibilities, but only to encode one of the simplest possibilities, with a single scalar leptoquark, denoted LQ and assigned PDG code 42. The leptoquark is assumed to carry specific quark and lepton quantum numbers, by default u quark plus electron. These flavour numbers are conserved, i.e. a process such as u e^- -> LQ -> d nu_e is not allowed.

            Although only one leptoquark is implemented, its flavours may be changed arbitrarily to study the different possibilities. The flavours of the leptoquark are defined by the quark and lepton flavours in the decay mode list. Therefore, to change from the current u e^- to c mu^+, say, you only need a line
            pythia.readString("42:0:products = 4 -13");
            in your main program, or the equivalent in a command file. The former must always be a quark, while the latter could be a lepton or an antilepton; a charge-conjugate partner is automatically defined by the program. At initialization, the charge is recalculated as a function of the flavours defined; also the leptoquark name is redefined to be of the type LQ_q,l, where actual quark and lepton flavours are displayed.

            The leptoquark is likely to be fairly long-lived, in which case it could have time to fragment into a mesonic- or baryonic-type state, which would decay later on. Currently this possibility is not handled; therefore the leptoquark is always assumed to decay before fragmentation. For that reason the leptoquark can also not be put stable.

            Production processes

            Four production processes have been implemented, which normally would not overlap and therefore could be run together.

            LeptoQuark:all On Off   (default = off)
            Common switch for the group of lowest-order LQ production processes, i.e. the four ones below.

            LeptoQuark:ql2LQ On Off   (default = off)
            Scatterings q l -> LQ. Code 3201.

            LeptoQuark:qg2LQl On Off   (default = off)
            Scatterings q g -> LQ l. Code 3202.

            LeptoQuark:gg2LQLQbar On Off   (default = off)
            Scatterings g g -> LQ LQbar. Code 3203.

            LeptoQuark:qqbar2LQLQbar On Off   (default = off)
            Scatterings q qbar -> LQ LQbar. Code 3204.

            Parameters

            In the above scenario the main free parameters are the leptoquark flavour content, set as already described, and the LQ mass, set as usual. In addition there is one further parameter.

            LeptoQuark:kCoup   (default = 1.0; minimum = 0.0)
            multiplicative factor in the LQ -> q l squared Yukawa coupling, and thereby in the LQ width and the q l -> LQ and other cross sections. Specifically, lambda^2/(4 pi) = k alpha_em, i.e. it corresponds to the $k$ factor of [Hew88]. "?>
            pythia8-8.1.80.orig/phpdoc/ErrorChecks.php0000644000175000017500000001672512217615312016544 0ustar sunsun Error Checks SETTINGS SAVED TO FILE

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            Error Checks

            There is a few settings related to error checking during program execution. Many other checks are performed as well, but do not have any specific setting related to themselves.

            Check:abortIfVeto On Off   (default = off)
            There are a few ways in which an event can be vetoed, the most common being a ";?>User Hooks test. Normally this will simply mean that the next parton-level configuration is selected inside the Pythia::next() routine, without any need for a user intervention. With this option switched on, however, Pythia::next() will return false. It is then up to the user to decide what to do next.

            Check:particleData On Off   (default = off)
            Check the particle data tables for potential problems during initialization. This includes inconsistent use of charge in particle names, inconsistent setup of mass, mass range, width and lifetime, sum of branching ratios not unity (allowed but discouraged) or charge not conserved in a decay channel. Warnings should be viewed as reasons to check further, but need not indicate a true problem, and also not all problems may be caught. The pythia.particleData.checkTable(level) method, used for these checks, may also be called directly.

            Check:levelParticleData   (default = 1)
            The level of verbosity and checks of particle data, if switched on.
            0 : minimal amount of checks, e.g. that no channels open.
            1 : further warning if individual channels closed, except for resonances.
            2 : also print branching-ratio-averaged threshold mass except for resonances.
            11 : as 1, but include resonances in detailed checks.
            12 : as 2, but include resonances in detailed checks.


            Check:event On Off   (default = on)
            When an event has been successfully generated, check that the final event record in event does not contain any unphysical particles, or nonconserved charge or energy-momentum. If this check fails, then pythia.next() obtains the value false, i.e. the event is counted as aborted.

            Check:history On Off   (default = on)
            When Check:event = on and the event is checked as above, further checks are made that all mother and daughter pointers are consistently set. Specifically that all daughters in the daughterlist (or motherList) have the particle in their respective motherList (or daughterlist). This operation takes a bit more time than the other error tests (of the order of 10% of what it takes to generate the event in the first place), and so could be switched off to save time.

            Check:nErrList   (default = 0)
            The number of erroneous events, in the above check, for which event listing and other detailed information will be printed. After that, only the normal error messages will be issued. Error counters are always updated, and accumulated numbers can be shown with pythia.statistics() at the end of the run.

            Check:epTolErr   (default = 1e-4)
            Maximum allowed summed deviation of E, p_x, p_y and p_z between the incoming beams and the final state, as a fraction of the initial energy, above which the event is counted as aborted. (Unfortunately roundoff errors do not scale linearly with the energy, and also have a very long tail. So while most events at lower energies may be correct to better than 1e-10, at LHC it does not have to signal any fundamental bug if also the default tolerance above is violated occasionally.)

            Check:epTolWarn   (default = 1e-6)
            A check on the same summed deviation as above, but counted as a warning rather than an error, and not leading to the event being classified as aborted. "?>
            pythia8-8.1.80.orig/phpdoc/php.txt0000644000175000017500000000463712217346240015151 0ustar sunsun"; if($_POST["resetval"] == 1) { //DELETE OLD FILE ON RESET unlink($_POST["rmfile"]); } if (!$_POST["filename"]) { echo "Please choose a (temporary) file name:
            "; echo "
            "; echo ""; echo ""; echo "
            "; } else if ($_POST["filename"] != "") { $filename = $_POST["filename"]; $filepath = "files/".$_POST["filename"]; $filecheck = file_exists($filepath); if(($_POST["finish"] == 1) || ($_GET["returning"] == 1)) { $filecheck = 0; $fileopen = 1; } if ($filecheck == 1) { echo "File in use.. choose again:
            "; echo "
            "; echo ""; echo ""; echo "
            "; } else { if(!$_POST["finish"]) { echo "Filename chosen: "; echo $_POST["filename"]; echo "
            "; echo ""; echo "
            "; echo ""; echo ""; echo ""; echo "
            "; echo ""; echo ""; echo ""; echo ""; echo "
            "; } if($fileopen != 1) { //CREATE & OPEN FILE & CHANGE PERMISSIONS TO 666 $handle = fopen($filepath, 'w'); chmod($filepath, 0666); fclose($handle); } if ($_POST["finish"]) { echo "
          • Right Click to Save Target: ".$filename."
            "; echo "
            "; echo ""; echo ""; echo ""; echo ""; echo "
            "; } } } echo ""; ?> pythia8-8.1.80.orig/phpdoc/BoseEinsteinEffects.php0000644000175000017500000002032312217615312020206 0ustar sunsun Bose-Einstein Effects SETTINGS SAVED TO FILE

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            "; } } ?>

            Bose-Einstein Effects

            The BoseEinstein class performs shifts of momenta of identical particles to provide a crude estimate of Bose-Einstein effects. The algorithm is the BE_32 one described in [Lon95], with a Gaussian parametrization of the enhancement. We emphasize that this approach is not based on any first-principles quantum mechanical description of interference phenomena; such approaches anyway have many problems to contend with. Instead a cruder but more robust approach is adopted, wherein BE effects are introduced after the event has already been generated, with the exception of the decays of long-lived particles. The trick is that momenta of identical particles are shifted relative to each other so as to provide an enhancement of pairs closely separated, which is compensated by a depletion of pairs in an intermediate region of separation.

            More precisely, the intended target form of the BE correlations in BE_32 is
            f_2(Q) = (1 + lambda * exp(-Q^2 R^2)) * (1 + alpha * lambda * exp(-Q^2 R^2/9) * (1 - exp(-Q^2 R^2/4)))
            where Q^2 = (p_1 + p_2)^2 - (m_1 + m_2)^2. Here the strength lambda and effective radius R are the two main parameters. The first factor of the equation is implemented by pulling pairs of identical hadrons closer to each other. This is done in such a way that three-momentum is conserved, but at the price of a small but non-negligible negative shift in the energy of the event. The second factor compensates this by pushing particles apart. The negative alpha parameter is determined iteratively, separately for each event, so as to restore energy conservation. The effective radius parameter is here R/3, i.e. effects extend further out in Q. Without the dampening (1 - exp(-Q^2 R^2/4)) in the second factor the value at the origin would become f_2(0) = (1 + lambda) * (1 + alpha * lambda), with it the desired value f_2(0) = (1 + lambda) is restored. The end result can be viewed as a poor man's rendering of a rapidly dampened oscillatory behaviour in Q.

            Further details can be found in [Lon95]. For instance, the target is implemented under the assumption that the initial distribution in Q can be well approximated by pure phase space at small values, and implicitly generates higher-order effects by the way the algorithm is implemented. The algorithm is applied after the decay of short-lived resonances such as the rho, but before the decay of longer-lived particles.

            This algorithm is known to do a reasonable job of describing BE phenomena at LEP. It has not been tested against data for hadron colliders, to the best of our knowledge, so one should exercise some judgment before using it. Therefore by default the master switch ";?>HadronLevel:BoseEinstein is off. Furthermore, the implementation found here is not (yet) as sophisticated as the one used at LEP2, in that no provision is made for particles from separate colour singlet systems, such as W's and Z's, interfering only at a reduced rate.

            Warning: The algorithm will create a new copy of each particle with shifted momentum by BE effects, with status code 99, while the original particle with the original momentum at the same time will be marked as decayed. This means that if you e.g. search for all pi+- in an event you will often obtain the same particle twice. One way to protect yourself from unwanted doublecounting is to use only particles with a positive status code, i.e. ones for which event[i].isFinal() is true.

            Main parameters



            BoseEinstein:Pion On Off   (default = on)
            Include effects or not for identical pi^+, pi^- and pi^0.

            BoseEinstein:Kaon On Off   (default = on)
            Include effects or not for identical K^+, K^-, K_S^0 and K_L^0.

            BoseEinstein:Eta On Off   (default = on)
            Include effects or not for identical eta and eta'.

            BoseEinstein:lambda   (default = 1.; minimum = 0.; maximum = 2.)
            The strength parameter for Bose-Einstein effects. On physical grounds it should not be above unity, but imperfections in the formalism used may require that nevertheless.

            BoseEinstein:QRef   (default = 0.2; minimum = 0.05; maximum = 1.)
            The size parameter of the region in Q space over which Bose-Einstein effects are significant. Can be thought of as the inverse of an effective distance in normal space, R = hbar / QRef, with R as used in the above equation. That is, f_2(Q) = (1 + lambda * exp(-(Q/QRef)^2)) * (...).

            BoseEinstein:widthSep   (default = 0.02; minimum = 0.001; maximum = 1.)
            Particle species with a width above this value (in GeV) are assumed to be so short-lived that they decay before Bose-Einstein effects are considered, while otherwise they do not. In the former case the decay products thus can obtain shifted momenta, in the latter not. The default has been picked such that both rho and K^* decay products would be modified. "?>
            pythia8-8.1.80.orig/phpdoc/MultipartonInteractions.php0000644000175000017500000010641012217615312021222 0ustar sunsun Multiparton Interactions SETTINGS SAVED TO FILE

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            Multiparton Interactions

            The starting point for the multiparton interactions physics scenario in PYTHIA is provided by [Sjo87]. Recent developments have included a more careful study of flavour and colour correlations, junction topologies and the relationship to beam remnants [Sjo04], interleaving with initial-state radiation [Sjo05], making use of transverse-momentum-ordered initial- and final-state showers, with the extension to fully interleaved evolution covered in [Cor10a]. A framework to handle rescattering is described in [Cor09].

            A big unsolved issue is how the colour of all these subsystems is correlated. For sure there is a correlation coming from the colour singlet nature of the incoming beams, but in addition final-state colour rearrangements may change the picture. Indeed such extra effects appear necessary to describe data, e.g. on <pT>(n_ch). A simple implementation of colour rearrangement is found as part of the ";?>beam remnants description.

            Main variables

            Matching to hard process

            The maximum pT to be allowed for multiparton interactions is related to the nature of the hard process itself. It involves a delicate balance between not double-counting and not leaving any gaps in the coverage. The best procedure may depend on information only the user has: how the events were generated and mixed (e.g. with Les Houches Accord external input), and how they are intended to be used. Therefore a few options are available, with a sensible default behaviour.

            MultipartonInteractions:pTmaxMatch   (default = 0; minimum = 0; maximum = 2)
            Way in which the maximum scale for multiparton interactions is set to match the scale of the hard process itself.
            0 : (i) if the final state of the hard process (not counting subsequent resonance decays) contains only quarks (u, d, s, c, b), gluons and photons then pT_max is chosen to be the factorization scale for internal processes and the scale value for Les Houches input; (ii) if not, interactions are allowed to go all the way up to the kinematical limit. The reasoning is that the former kind of processes are generated by the multiparton-interactions machinery and so would double-count hard processes if allowed to overlap the same pT range, while no such danger exists in the latter case.
            1 : always use the factorization scale for an internal process and the scale value for Les Houches input, i.e. the lower value. This should avoid double-counting, but may leave out some interactions that ought to have been simulated.
            2 : always allow multiparton interactions up to the kinematical limit. This will simulate all possible event topologies, but may lead to double-counting.

            Note: If a "second hard" process is present, the two are analyzed separately for the default 0 option. It is enough that one of them only consists of quarks, gluons and photons to restrict the pT range. The maximum for MPI is then set by the hard interaction with lowest scale.

            Cross-section parameters

            The rate of interactions is determined by

            MultipartonInteractions:alphaSvalue   (default = 0.127; minimum = 0.06; maximum = 0.25)
            The value of alpha_strong at m_Z. Default value is picked equal to the one used in CTEQ 5L.

            The actual value is then regulated by the running to the scale pT^2, at which it is evaluated

            MultipartonInteractions:alphaSorder   (default = 1; minimum = 0; maximum = 2)
            The order at which alpha_strong runs at scales away from m_Z.
            0 : zeroth order, i.e. alpha_strong is kept fixed.
            1 : first order, which is the normal value.
            2 : second order. Since other parts of the code do not go to second order there is no strong reason to use this option, but there is also nothing wrong with it.

            QED interactions are regulated by the alpha_electromagnetic value at the pT^2 scale of an interaction.

            MultipartonInteractions:alphaEMorder   (default = 1; minimum = -1; maximum = 1)
            The running of alpha_em used in hard processes.
            1 : first-order running, constrained to agree with StandardModel:alphaEMmZ at the Z^0 mass.
            0 : zeroth order, i.e. alpha_em is kept fixed at its value at vanishing momentum transfer.
            -1 : zeroth order, i.e. alpha_em is kept fixed, but at StandardModel:alphaEMmZ, i.e. its value at the Z^0 mass.

            Note that the choices of alpha_strong and alpha_em made here override the ones implemented in the normal process machinery, but only for the interactions generated by the MultipartonInteractions class.

            In addition there is the possibility of a global rescaling of cross sections (which could not easily be accommodated by a changed alpha_strong, since alpha_strong runs)

            MultipartonInteractions:Kfactor   (default = 1.0; minimum = 0.5; maximum = 4.0)
            Multiply all cross sections by this fix factor.

            The processes used to generate multiparton interactions form a subset of the standard library of hard processes. The input is slightly different from the standard hard-process machinery, however, since incoming flavours, the alpha_strong value and most of the kinematics are already fixed when the process is called. It is possible to regulate the set of processes that are included in the multiparton-interactions framework.

            MultipartonInteractions:processLevel   (default = 3; minimum = 0; maximum = 3)
            Set of processes included in the machinery.
            0 : only the simplest 2 -> 2 QCD processes between quarks and gluons, giving no new flavours, i.e. dominated by t-channel gluon exchange.
            1 : also 2 -> 2 QCD processes giving new flavours (including charm and bottom), i.e. proceeding through s-channel gluon exchange.
            2 : also 2 -> 2 processes involving one or two photons in the final state, s-channel gamma boson exchange and t-channel gamma/Z^0/W^+- boson exchange.
            3 : also charmonium and bottomonium production, via colour singlet and colour octet channels.

            Cross-section regularization

            There are two complementary ways of regularizing the small-pT divergence, a sharp cutoff and a smooth dampening. These can be combined as desired, but it makes sense to coordinate with how the same issue is handled in ";?>spacelike showers. Actually, by default, the parameters defined here are used also for the spacelike showers, but this can be overridden.

            Regularization of the divergence of the QCD cross section for pT -> 0 is obtained by a factor pT^4 / (pT0^2 + pT^2)^2, and by using an alpha_s(pT0^2 + pT^2). An energy dependence of the pT0 choice is introduced by two further parameters, so that pT0Ref is the pT0 value for the reference CM energy, pT0Ref = pT0(ecmRef).
            Warning: if a large pT0 is picked for multiparton interactions, such that the integrated interaction cross section is below the nondiffractive inelastic one, this pT0 will automatically be scaled down to cope.

            The actual pT0 parameter used at a given CM energy scale, ecmNow, is obtained as
            pT0 = pT0(ecmNow) = pT0Ref * (ecmNow / ecmRef)^ecmPow
            where pT0Ref, ecmRef and ecmPow are the three parameters below.

            MultipartonInteractions:pT0Ref   (default = 2.15; minimum = 0.5; maximum = 10.0)
            The pT0Ref scale in the above formula.
            Note: pT0Ref is one of the key parameters in a complete PYTHIA tune. Its value is intimately tied to a number of other choices, such as that of colour flow description, so unfortunately it is difficult to give an independent meaning to pT0Ref.

            MultipartonInteractions:ecmRef   (default = 1800.0; minimum = 1.)
            The ecmRef reference energy scale introduced above.

            MultipartonInteractions:ecmPow   (default = 0.24; minimum = 0.0; maximum = 0.5)
            The ecmPow energy rescaling pace introduced above.

            Alternatively, or in combination, a sharp cut can be used.

            MultipartonInteractions:pTmin   (default = 0.2; minimum = 0.1; maximum = 10.0)
            Lower cutoff in pT, below which no further interactions are allowed. Normally pT0 above would be used to provide the main regularization of the cross section for pT -> 0, in which case pTmin is used mainly for technical reasons. It is possible, however, to set pT0Ref = 0 and use pTmin to provide a step-function regularization, or to combine them in intermediate approaches. Currently pTmin is taken to be energy-independent.

            Gösta Gustafson has proposed (private communication, unpublished) that the amount of screening, as encapsulated in the pT0 parameter, fluctuates from one event to the next. Specifically, high-activity event are more likely to lead to interactions at large pT scales, but the high activity simultaneously leads to a larger screening of interactions at smaller pT. Such a scenario can approximately be simulated by scaling up the pT0 by a factor sqrt(n), where n is the number of interactions considered so far, including the current one. That is, for the first interaction the dampening factor is pT^4 / (pT0^2 + pT^2)^2, for the second pT^4 / (2 pT0^2 + pT^2)^2, for the third pT^4 / (3 pT0^2 + pT^2)^2, and so on. Optionally the scheme may also be applied to ISR emissions. For simplicity the same alpha_s(pT0^2 + pT^2) is used throughout. Note that, in this scenario the pT0 scale must be lower than in the normal case to begin with, since it later is increased back up. Also note that the idea with this scenario is to propose an alternative to colour reconnection to understand the rise of <pT>(n_ch), so that the amount of colour reconnection should be reduced.

            MultipartonInteractions:enhanceScreening   (default = 0; minimum = 0; maximum = 2)
            Choice to activate the above screening scenario, i.e. an increasing effective pT0 for consecutive interactions.
            0 : No activity-dependent screening, i.e. pT0 is fixed.
            1 : The pT0 scale is increased as a function of the number of MPI's, as explained above. ISR is not affected, but note that, if SpaceShower:samePTasMPI is on, then MultipartonInteractions:pT0Ref is used also for ISR, which may or may not be desirable.
            2 : Both MPI and ISR influence and are influenced by the screening. That is, the dampening is reduced based on the total number of MPI and ISR steps considered so far, including the current one. This dampening is implemented both for MPI and for ISR emissions, for the latter provided that SpaceShower:samePTasMPI is on (default).

            Impact-parameter dependence

            The choice of impact-parameter dependence is regulated by several parameters. The ones listed here refer to nondiffractive topologies only, while their equivalents for diffractive events are put in the ";?>Diffraction description. Note that there is currently no bProfile = 4 option for diffraction. Other parameters are assumed to agree between diffractive and nondiffractive topologies.

            MultipartonInteractions:bProfile   (default = 1; minimum = 0; maximum = 4)
            Choice of impact parameter profile for the incoming hadron beams.
            0 : no impact parameter dependence at all.
            1 : a simple Gaussian matter distribution; no free parameters.
            2 : a double Gaussian matter distribution, with the two free parameters coreRadius and coreFraction.
            3 : an overlap function, i.e. the convolution of the matter distributions of the two incoming hadrons, of the form exp(- b^expPow), where expPow is a free parameter.
            4 : a Gaussian matter distribution with a width that varies according to the selected x value of an interaction, 1. + a1 log (1 / x), where a1 is a free parameter. Note that once b has been selected for the hard process, it remains fixed for the remainder of the evolution.


            MultipartonInteractions:coreRadius   (default = 0.4; minimum = 0.1; maximum = 1.)
            When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a radius that is a factor coreRadius smaller than the rest.

            MultipartonInteractions:coreFraction   (default = 0.5; minimum = 0.; maximum = 1.)
            When assuming a double Gaussian matter profile, bProfile = 2, the inner core is assumed to have a fraction coreFraction of the matter content of the hadron.

            MultipartonInteractions:expPow   (default = 1.; minimum = 0.4; maximum = 10.)
            When bProfile = 3 it gives the power of the assumed overlap shape exp(- b^expPow). Default corresponds to a simple exponential drop, which is not too dissimilar from the overlap obtained with the standard double Gaussian parameters. For expPow = 2 we reduce to the simple Gaussian, bProfile = 1, and for expPow -> infinity to no impact parameter dependence at all, bProfile = 0. For small expPow the program becomes slow and unstable, so the min limit must be respected.

            MultipartonInteractions:a1   (default = 0.15; minimum = 0.; maximum = 2.)
            When bProfile = 4, this gives the a1 constant in the Gaussian width. When a1 = 0., this reduces back to the single Gaussian case.

            MultipartonInteractions:bSelScale   (default = 1; minimum = 1; maximum = 3)
            The selection of impact parameter is related to the scale of the hard process: the harder this scale is, the more central the collision. In practice this centrality saturates quickly, however, and beyond a scale of roughly 20 GeV very little changes. (The relevant quantity is that the QCD jet cross section above the scale should be a tiny fraction of the total cross section.) In 2 -> 1 and 2 -> 2 processes traditional scale choices work fine, but ambiguities arise for higher multiplicities, in particular when the scale is used for matching between the multiparton matrix elements and parton showers. Then the event scale may be chosen as that of a very low-pT parton, i.e. suggesting a peripheral collision, while the much harder other partons instead would favour a central collision. Therefore the default here is to override whatever scale value have been read in from an LHEF, say. Notice that the scale used here is decoupled from the maximum scale for MPIs (MultipartonInteractions:pTmaxMatch).
            1 : Use the mass for a 2 -> 1 process. For 2 -> n, n > 1 processes order the particles in falling mmT = m + mT and then let the scale be (mmT_1 + mmT_2)/2 + mmT_3/3 + mmT_4/4 + ... + mmT_n/n. This is constructed always to be above m1, and to assign decreasing importance to softer particles that are less likely to be associated with the hard process.
            2 : Use the scale parameter of the event.
            3 : use the same scale as chosen by the rules for MultipartonInteractions:pTmaxMatch.

            Rescattering

            It is possible that a parton may rescatter, i.e. undergo a further interaction subsequent to the first one. The machinery to model this kind of physics has only recently become fully operational [Cor09], and is therefore not yet so well explored.

            The rescattering framework has ties with other parts of the program, notably with the ";?>beam remnants.

            MultipartonInteractions:allowRescatter On Off   (default = off)
            Switch to allow rescattering of partons; on/off = true/false.
            Note: the rescattering framework has not yet been implemented for the MultipartonInteractions:bProfile = 4 option, and can therefore not be switched on in that case. Warning: use with caution since machinery is still not so well tested.

            MultipartonInteractions:allowDoubleRescatter On Off   (default = off)
            Switch to allow rescattering of partons, where both incoming partons have already rescattered; on/off = true/false. Is only used if MultipartonInteractions:allowRescatter is switched on.
            Warning: currently there is no complete implementation that combines it with shower evolution, so you must use PartonLevel:ISR = off and PartonLevel:FSR = off. If not, a warning will be issued and double rescattering will not be simulated. The rate also comes out to be much lower than for single rescattering, so to first approximation it can be neglected.

            MultipartonInteractions:rescatterMode   (default = 0; minimum = 0; maximum = 4)
            Selection of which partons rescatter against unscattered partons from the incoming beams A and B, based on their rapidity value y in the collision rest frame. Here ySep is shorthand for MultipartonInteractions:ySepRescatter and deltaY for MultipartonInteractions:deltaYRescatter, defined below. The description is symmetric between the two beams, so only one case is described below.
            0 : only scattered partons with y > 0 can collide with unscattered partons from beam B.
            1 : only scattered partons with y > ySep can collide with unscattered partons from beam B.
            2 : the probability for a scattered parton to be considered as a potential rescatterer against unscattered partons in beam B increases linearly from zero at y = ySep - deltaY to unity at y = ySep + deltaY.
            3 : the probability for a scattered parton to be considered as a potential rescatterer against unscattered partons in beam B increases with y according to (1/2) * (1 + tanh( (y - ySep) / deltaY)).
            4 : all partons are potential rescatterers against both beams.


            MultipartonInteractions:ySepRescatter   (default = 0.)
            used for some of the MultipartonInteractions:rescatterMode options above, as the rapidity for which a scattered parton has a 50% probability to be considered as a potential rescatterer. A ySep > 0 generally implies that some central partons cannot rescatter at all, while a ySep < 0 instead allows central partons to scatter against either beam.

            MultipartonInteractions:deltaYRescatter   (default = 1.; minimum = 0.1)
            used for some of the MultipartonInteractions:rescatterMode options above, as the width of the rapidity transition region, where the probability rises from zero to unity that a scattered parton is considered as a potential rescatterer.

            Further variables

            These should normally not be touched. Their only function is for cross-checks.

            MultipartonInteractions:nQuarkIn   (default = 5; minimum = 0; maximum = 5)
            Number of allowed incoming quark flavours in the beams; a change to 4 would thus exclude b and bbar as incoming partons, etc.

            MultipartonInteractions:nSample   (default = 1000; minimum = 100)
            The allowed pT range is split (unevenly) into 100 bins, and in each of these the interaction cross section is evaluated in nSample random phase space points. The full integral is used at initialization, and the differential one during the run as a "Sudakov form factor" for the choice of the hardest interaction. A larger number implies increased accuracy of the calculations.

            Technical notes

            Relative to the articles mentioned above, not much has happened. The main news is a technical one, that the phase space of the 2 -> 2 (massless) QCD processes is now sampled in dy_3 dy_4 dpT^2, where y_3 and y_4 are the rapidities of the two produced partons. One can show that
            (dx_1 / x_1) * (dx_2 / x_2) * d(tHat) = dy_3 * dy_4 * dpT^2
            Furthermore, since cross sections are dominated by the "Rutherford" one of t-channel gluon exchange, which is enhanced by a factor of 9/4 for each incoming gluon, effective structure functions are defined as
            F(x, pT2) = (9/4) * xg(x, pT2) + sum_i xq_i(x, pT2)
            With this technical shift of factors 9/4 from cross sections to parton densities, a common upper estimate of
            d(sigmaHat)/d(pT2) < pi * alpha_strong^2 / pT^4
            is obtained.

            In fact this estimate can be reduced by a factor of 1/2 for the following reason: for any configuration (y_3, y_4, pT2) also one with (y_4, y_3, pT2) lies in the phase space. Not both of those can enjoy being enhanced by the tHat -> 0 singularity of
            d(sigmaHat) propto 1/tHat^2.
            Or if they are, which is possible with identical partons like q q -> q q and g g -> g g, each singularity comes with half the strength. So, when integrating/averaging over the two configurations, the estimated d(sigmaHat)/d(pT2) drops. Actually, it drops even further, since the naive estimate above is based on
            (4 /9) * (1 + (uHat/sHat)^2) < 8/9 < 1
            The 8/9 value would be approached for tHat -> 0, which implies sHat >> pT2 and thus a heavy parton-distribution penalty, while parton distributions are largest for tHat = uHat = -sHat/2, where the above expression evaluates to 5/9. A fudge factor is therefore introduced to go the final step, so it can easily be modified when further non-Rutherford processes are added, or should parton distributions change significantly.

            At initialization, it is assumed that
            d(sigma)/d(pT2) < d(sigmaHat)/d(pT2) * F(x_T, pT2) * F(x_T, pT2) * (2 y_max(pT))^2
            where the first factor is the upper estimate as above, the second two the parton density sum evaluated at y_3 = y_ 4 = 0 so that x_1 = x_2 = x_T = 2 pT / E_cm, where the product is expected to be maximal, and the final is the phase space for -y_max < y_{3,4} < y_max. The right-hand side expression is scanned logarithmically in y, and a N is determined such that it always is below N/pT^4.

            To describe the dampening of the cross section at pT -> 0 by colour screening, the actual cross section is multiplied by a regularization factor (pT^2 / (pT^2 + pT0^2))^2, and the alpha_s is evaluated at a scale pT^2 + pT0^2, where pT0 is a free parameter of the order of 2 - 4 GeV. Since pT0 can be energy-dependent, an ansatz
            pT0(ecm) = pT0Ref * (ecm/ecmRef)^ecmPow
            is used, where ecm is the current CM frame energy, ecmRef is an arbitrary reference energy where pT0Ref is defined, and ecmPow gives the energy rescaling pace. For technical reasons, also an absolute lower pT scale pTmin, by default 0.2 GeV, is introduced. In principle, it is possible to recover older scenarios with a sharp pT cutoff by setting pT0 = 0 and letting pTmin be a larger number.

            The above scanning strategy is then slightly modified: instead of an upper estimate N/pT^4 one of the form N/(pT^2 + r * pT0^2)^2 is used. At first glance, r = 1 would seem to be fixed by the form of the regularization procedure, but this does not take into account the nontrivial dependence on alpha_s, parton distributions and phase space. A better Monte Carlo efficiency is obtained for r somewhat below unity, and currently r = 0.25 is hardcoded. In the generation a trial pT2 is then selected according to
            d(Prob)/d(pT2) = (1/sigma_ND) * N/(pT^2 + r * pT0^2)^2 * ("Sudakov")
            For the trial pT2, a y_3 and a y_4 are then selected, and incoming flavours according to the respective F(x_i, pT2), and then the cross section is evaluated for this flavour combination. The ratio of trial/upper estimate gives the probability of survival.

            Actually, to profit from the factor 1/2 mentioned above, the cross section for the combination with y_3 and y_4 interchanged is also tried, which corresponds to exchanging tHat and uHat, and the average formed, while the final kinematics is given by the relative importance of the two.

            Furthermore, since large y values are disfavoured by dropping PDF's, a factor
            WT_y = (1 - (y_3/y_max)^2) * (1 - (y_4/y_max)^2)
            is evaluated, and used as a survival probability before the more time-consuming PDF+ME evaluation, with surviving events given a compensating weight 1/WT_y.

            An impact-parameter dependence is also allowed. Based on the hard pT scale of the first interaction, and enhancement/depletion factor is picked, which multiplies the rate of subsequent interactions.

            Parton densities are rescaled and modified to take into account the energy-momentum and flavours kicked out by already-considered interactions. "?>

            pythia8-8.1.80.orig/phpdoc/BeamParameters.php0000644000175000017500000005436412217615312017223 0ustar sunsun Beam Parameters SETTINGS SAVED TO FILE

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            Beam Parameters

            The settings on this page relate to the beam identities and energies, to a beam momentum spread and to a beam interaction spot. As always, momenta and energies are to be given in units of GeV, and of space and time in mm.

            Incoming beams

            There are two ways to set the identities and energies of the two incoming beam particles. One is to use the init() method with no arguments. Then the settings variables below will be read and used. The alternative is to call ";?>init(...) with arguments that provide this information. Then you need not use the variables below (although it would still be possible). Note that, if nothing is done, you will default to LHC at 14 TeV.

            Currently the beam particles must be either a hadron pair or a lepton pair. In the former category p p and pbar p combinations dominate, but it is also possible to combine with pi^+, pi^- and pi^0. In the latter e^+ e^- and mu^+ mu^- would be the most useful combinations, but also others should work if combined with an appropriate hard process.

            Beams:idA   (default = 2212)
            The PDG id code for the first incoming particle. Allowed codes include
            2212 = p, -2212 = pbar,
            2112 = n, -2112 = nbar,
            211 = pi^+, -211 = pi^-, 111 = pi^0,
            990 = Pomeron (used in diffractive machinery; here mainly for debug purposes),
            11 = e^-, -11 = e^+,
            13 = mu^-, -13 = mu^+,
            and a few more leptons/neutrinos in a few combinations.

            Beams:idB   (default = 2212)
            The PDG id code for the second incoming particle.

            Beams:frameType   (default = 1; minimum = 1; maximum = 5)
            Choice of frame for the two colliding particles. For options 1 - 3 the beam identities are specified above, while they are obtained by the Les Houches information for options 4 and 5.
            1 : the beams are colliding in their CM frame, and therefore only the CM energy needs to be provided, see Beams:eCM below.
            2 : the beams are back-to-back, but with different energies, see Beams:eA and Beams:eB below. This option could also be used for fixed-target configurations.
            3 : the beams are not back-to-back, and therefore the three-momentum of each incoming particle needs to be specified, see Beams:pxA through Beams:pzB below.
            4 : the beam and event information is stored in a Les Houches Event File, see Beams:LHEF below.
            5 : the beam and event information is obtained by a pointer to an LHAup class instance.


            Beams:eCM   (default = 14000.; minimum = 10.)
            Collision CM energy, to be set if Beams:frameType = 1.

            Beams:eA   (default = 7000.; minimum = 0.)
            The energy of the first incoming particle, moving in the +z direction, to be set if Beams:frameType = 2. If the particle energy is smaller than its mass it is assumed to be at rest.

            Beams:eB   (default = 7000.; minimum = 0.)
            The energy of the second incoming particle, moving in the -z direction, to be set if Beams:frameType = 2. If the particle energy is smaller than its mass it is assumed to be at rest.

            Beams:pxA   (default = 0.)
            The p_x component of the first incoming particle, to be set if Beams:frameType = 3.

            Beams:pyA   (default = 0.)
            The p_y component of the first incoming particle, to be set if Beams:frameType = 3.

            Beams:pzA   (default = 7000.)
            The p_z component of the first incoming particle, to be set if Beams:frameType = 3.

            Beams:pxB   (default = 0.)
            The p_x component of the second incoming particle, to be set if Beams:frameType = 3.

            Beams:pyB   (default = 0.)
            The p_y component of the second incoming particle, to be set if Beams:frameType = 3.

            Beams:pzB   (default = -7000.)
            The p_z component of the second incoming particle, to be set if Beams:frameType = 3.

            Beams:LHEF   (default = void)
            The name of a Les Houches Event File, to be set if Beams:frameType = 4.

            Beams:LHEFheader   (default = void)
            As some information in a Les Houches Event File init block is only known at the end of generation, some programs choose to output this as a separate file. If Beams:LHEFheader is given, information up till the end of the init block is read from this file, with the events themselves read as usual from the file given in Beams:LHEF.

            Beams:newLHEFsameInit On Off   (default = off)
            Allow to begin reading events from a new LHEF or or a new LHAup instance without a completely new initialization. Only useful when Beams:frameType = 4 or 5.

            Beams:readLHEFheaders On Off   (default = on)
            Read in LHEF header blocks and store them in the ";?>Info class. See also ";?>LHAupLHEF for more information.

            mode  Beams:nSkipLHEFatInit   (default = 0)
            Skip the first nSkip events of the input stream (cf. the LHAup::skipEvent(nSkip) method). Only used when Beams:frameType = 4 or 5.

            Beam momentum spread

            This framework currently is intended for a modest beam spread, such as experienced at hadron colliders. Thus it can be safely assumed that the physics does not change over the CM energy range probed, so that the parameters of the physics initialization at the nominal energy can be used as is. Currently it can not be used for the more extensive energy spread expected at linear e^+ e^- colliders. Also, any attempt to combine it with external Les Houches input of parton-level events is at own risk.

            On this page you can set the momentum spread according to a simple Gaussian distribution. If you instead want a more sophisticated parametrization, you can write and link your own ";?>BeamShape class.

            Beams:allowMomentumSpread On Off   (default = off)
            Allow the beam momenta to be smeared around their initialization nominal values.

            Beams:sigmaPxA   (default = 0.; minimum = 0.)
            The width of a Gaussian distribution of the p_x spread of the first incoming particle.

            Beams:sigmaPyA   (default = 0.; minimum = 0.)
            The width of a Gaussian distribution of the p_y spread of the first incoming particle.

            Beams:sigmaPzA   (default = 0.; minimum = 0.)
            The width of a Gaussian distribution of the p_z spread of the first incoming particle.

            Beams:maxDevA   (default = 5.; minimum = 0.)
            The triply Gaussian distribution (p_x, p_y, p_z) is restricted to a maximal total deviation from the nominal values (p_x0, p_y0, p_z0) for the first incoming particle, like
            (p_x - p_x0)^2/sigma_px^2 + (p_y - p_y0)^2/sigma_py^2 + (p_z - p_z0)^2/sigma_pz^2 < maxDev^2
            (Note the absence of a factor 2 in the denominator, unlike the Gaussians used to pick (p_x, p_y, p_z).)

            Beams:sigmaPxB   (default = 0.; minimum = 0.)
            The width of a Gaussian distribution of the p_x spread of the second incoming particle.

            Beams:sigmaPyB   (default = 0.; minimum = 0.)
            The width of a Gaussian distribution of the p_y spread of the second incoming particle.

            Beams:sigmaPzB   (default = 0.; minimum = 0.)
            The width of a Gaussian distribution of the p_z spread of the second incoming particle.

            Beams:maxDevB   (default = 5.; minimum = 0.)
            The triply Gaussian distribution (p_x, p_y, p_z) is restricted to a maximal total deviation from the nominal values (p_x0, p_y0, p_z0), for the second incoming particle, like
            (p_x - p_x0)^2/sigma_px^2 + (p_y - p_y0)^2/sigma_py^2 + (p_z - p_z0)^2/sigma_pz^2 < maxDev^2
            (Note the absence of a factor 2 in the denominator, unlike the Gaussians used to pick (p_x, p_y, p_z).)

            Beam interaction vertex

            On this page you can set the spread of the interaction vertex according to a simple Gaussian distribution. If you instead want a more sophisticated parametrization, you can write and link your own ";?>BeamShape class.

            Beams:allowVertexSpread On Off   (default = off)
            Allow the interaction vertex of the two colliding beams to be smeared. If off, then the vertex is set to be the origin.

            Beams:sigmaVertexX   (default = 0.; minimum = 0.)
            The width of a Gaussian distribution of the x location of the interaction vertex.

            Beams:sigmaVertexY   (default = 0.; minimum = 0.)
            The width of a Gaussian distribution of the y location of the interaction vertex.

            Beams:sigmaVertexZ   (default = 0.; minimum = 0.)
            The width of a Gaussian distribution of the z location of the interaction vertex.

            Beams:maxDevVertex   (default = 5.; minimum = 0.)
            The triply Gaussian distribution of interaction vertex position (x, y, z) is restricted to a maximal total deviation from the origin, like
            x^2/sigma_x^2 + y^2/sigma_y^2 + z^2/sigma_z^2 < maxDevVertex^2
            (Note the absence of a factor 2 in the denominator, unlike the Gaussians used to pick (x, y, z).)

            Beams:sigmaTime   (default = 0.; minimum = 0.)
            The width of a Gaussian distribution of the collision time (in units of mm/c). Note that, if the above space parametrization is viewed as the effect of two incoming beams along the +-z axis, with each beam having a Gaussian spread, then the spread of the time would also become a Gaussian with the same width as the z one (times the velocity of the beams, which we expect is close to unity). For flexibility we have not enforced any such relation, however.

            Beams:maxDevTime   (default = 5.; minimum = 0.)
            The collision time is restricted to be in the range |t| < sigma_t * maxDevTime.

            The distributions above are all centered at the origin. It is also possible to shift the above distributions to be centered around another nominal position. You must have Beams:allowVertexSpread = on to use this possibility.

            Beams:offsetVertexX   (default = 0.)
            The x location of the interaction vertex is centered at this value.

            Beams:offsetVertexY   (default = 0.)
            The y location of the interaction vertex is centered at this value.

            Beams:offsetVertexZ   (default = 0.)
            The z location of the interaction vertex is centered at this value.

            Beams:offsetTime   (default = 0.)
            The time t of the interaction vertex is centered at this value. "?>

            pythia8-8.1.80.orig/phpdoc/RHadrons.php0000644000175000017500000002514012217615312016041 0ustar sunsun R-hadrons SETTINGS SAVED TO FILE

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            R-hadrons

            When a coloured SUSY particle is longer-lived than typical hadronization scales, i.e. around c*tau > 1 fm, or equivalently width Gamma < 0.2 GeV, it will have time to hadronize into a colour singlet hadronic state, a R-hadron. Currently a set of such R-hadrons have been implemented for the case of a long-lived gluino, stop or sbottom. Needless to say, the normal case would be that only one of them will be long-lived enough to form R-hadrons.

            For simplicity all gluino-mesons are assumed to have light-flavour spin 1, since those are the lightest and favoured by spin-state counting. Further, all gluino-baryons are bookkept as having light-flavour spin 3/2, and flavours are listed in descending order. This is more for convenience of notation, however, since the normal baryon octet e.g. has no uuu = "p++" state. When a diquark is extracted, a mixture of spin 0 and spin 1 is allowed. Names and codes are essentially in agreement with the PDG conventions, e.g.
            1000993 R0(~g g) (or gluinoball)
            1009213 R+(~g u dbar) (or gluino-rho+)
            1092214 R+(~g uud) (or gluino-Delta+)
            For internal bookkeeping of momenta, the code 1009002, Rtemp(~g q), is used to denote the intermediate state formed when only one of the two string pieces attached to the gluino has broken.

            For the stop- and sbottom-hadrons the spin counting is simpler, since it is entirely given by the constituent quark or diquark spin. Again names and codes follow PDG conventions, e.g.
            1000612 R+(~t dbar)
            1006211 R+(~t ud0)

            The spin and electromagnetic charge of the new particle plays only a minor role in the hadronization process, that can be neglected to first approximation. Therefore it is possible to use the same R-hadrons framework instead for other BSM scenarios with long-lived coloured particles, e.g. with massive extra-dimensions copies of gluons and quarks, or with leptoquarks. This can be regulated by the switches below. Note that the codes and names of the R-hadrons is not changed when the heavy particle involved is switched, for reasons of administrative simplicity. R-hadron mass spectra and other relevant particle data is automatically updated to reflect the change, however.

            RHadrons:allow On Off   (default = off)
            Allows the gluino, stop and sbottom to hadronize if their respective widths are below the limit RHadrons:maxWidth.

            RHadrons:maxWidth   (default = 0.2; minimum = 0.0; maximum = 1.0)
            The maximum width of the gluino for which it is possible to form R-hadrons, provided that RHadrons:allow is on.

            mode  RHadrons:idGluino   (default = 1000021)
            The gluino identity code. For other scenarios than SUSY this code could be changed to represent another long-lived uncharged colour octet particle, that then would be treated in the same spirit. Could be set to 0 to forbid any gluino R-hadron formation even when the above two criteria, RHadrons:allow and RHadrons:maxWidth, are met.

            mode  RHadrons:idStop   (default = 1000006)
            The lightest stop identity code. For other scenarios than SUSY this code could be changed to represent another long-lived charge 2/3 colour triplet particle, that then would be treated in the same spirit. As above it could be set to 0 to forbid any stop R-hadron formation.

            mode  RHadrons:idSbottom   (default = 1000005)
            The lightest sbottom identity code. For other scenarios than SUSY this code could be changed to represent another long-lived charge -1/3 colour triplet particle, that then would be treated in the same spirit. As above it could be set to 0 to forbid any sbottom R-hadron formation.

            RHadrons:allowDecay On Off   (default = on)
            Allows the R-hadrons to decay or not. If the gluino/stop/sbottom is stable or too long-lived to decay inside the detector this switch has no real function, since then no decays will be performed anyway. If the sparticle is so short-lived that it decays before reaching the beam pipe then having the decay on is the logical choice. So the interesting region is when the decays happens after the R-hadron has passed through part of the detector, and changed its momentum and quite possibly its flavour content before it is to decay. Then normal decays should be switched off, and the R-hadron tracked through matter by a program like GEANT [Kra04,Mac07]. After that, the new R-hadron info can be overwritten into the event record and the Pythia::forceRHadronDecay() method can be called to force this modified R-hadron to decay.

            RHadrons:setMasses On Off   (default = on)
            Use simple mass formulae to construct all available R-hadron masses based on the currently initialized gluino/squark masses and the constituent masses of the other partons in the hadron. If you switch this off, it is your responsibility to set each of the R-hadron masses on your own, and set them in an internally consistent way. If you mess up on this you may generate accordingly crazy results. Specifically, it is to be assumed that none of the R-hadrons has a mass below its constituent sparticle, i.e. that the light degrees of freedom and the additional confinement gluon field gives a net positive contribution to the R-hadron mass.

            RHadrons:probGluinoball   (default = 0.1; minimum = 0.0; maximum = 1.0)
            The fraction of produced gluino R-hadrons that are contain a "valence" gluon, with the rest containing a meson or baryon quark flavour content.

            RHadrons:mOffsetCloud   (default = 0.2; minimum = 0.0)
            Extra mass (in GeV) added to each of the one or two extra constituent masses in an R-hadron, to calculate the mass of a R-hadron. The same offset is also used when the R-hadron momentum and mass is split between the squark or gluino and the one or two light (di)quarks, one for a squark and two for a gluino. Thus once or twice this amount represents a part of the nominal squark or gluino mass that will not decay weakly, since it is taken to correspond to the cloud of gluons that surround the squark or gluino.

            RHadrons:mCollapse   (default = 1.0; minimum = 0.0)
            A colour singlet system with an invariant mass less than this amount, above the R-hadron mass with the given flavour content, is assumed to collapse to this single R-hadron, whereas a full fragmentation handling is applied above this mass.

            RHadrons:diquarkSpin1   (default = 0.5; minimum = 0.0; maximum = 1.0)
            Probability that a diquark extracted from the flavour code of a gluino R-hadron should be assigned spin 1, with the rest being spin 0. Does not apply for two identical quarks, where spin 1 is only possibility. Note that gluino R-hadron codes for simplicity are assigned as if spin is 1 always, and so give no guidance. For stop and sbottom the diquark spin is preserved in the particle code, so there is no corresponding issue. "?>

            pythia8-8.1.80.orig/phpdoc/Fragmentation.php0000644000175000017500000006313612217615312017126 0ustar sunsun Fragmentation SETTINGS SAVED TO FILE

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            Fragmentation

            Fragmentation in PYTHIA is based on the Lund string model [And83, Sjo84]. Several different aspects are involved in the physics description, which here therefore is split accordingly. This also, at least partly, reflect the set of classes involved in the fragmentation machinery.

            The variables collected here have a very wide span of usefulness. Some would be central in any hadronization tuning exercise, others should not be touched except by experts.

            The fragmentation flavour-choice machinery is also used in a few other places of the program, notably particle decays, and is thus described on the separate ";?>Flavour Selection page.

            Fragmentation functions

            The StringZ class handles the choice of longitudinal lightcone fraction z according to one of two possible shape sets.

            The Lund symmetric fragmentation function [And83] is the only alternative for light quarks. It is of the form
            f(z) = (1/z) * (1-z)^a * exp(-b m_T^2 / z)
            with the two main free parameters a and b to be tuned to data. They are stored in

            StringZ:aLund   (default = 0.3; minimum = 0.0; maximum = 2.0)
            The a parameter of the Lund symmetric fragmentation function.

            StringZ:bLund   (default = 0.8; minimum = 0.2; maximum = 2.0)
            The b parameter of the Lund symmetric fragmentation function.

            In principle, each flavour can have a different a. Then, for going from an old flavour i to a new j one the shape is
            f(z) = (1/z) * z^{a_i} * ((1-z)/z)^{a_j} * exp(-b * m_T^2 / z)
            This is only implemented for diquarks relative to normal quarks:

            StringZ:aExtraDiquark   (default = 0.5; minimum = 0.0; maximum = 2.0)
            allows a larger a for diquarks, with total a = aLund + aExtraDiquark.

            Finally, the Bowler modification [Bow81] introduces an extra factor
            1/z^{r_Q * b * m_Q^2}
            for heavy quarks. To keep some flexibility, a multiplicative factor r_Q is introduced, which ought to be unity (provided that quark masses were uniquely defined) but can be set in

            StringZ:rFactC   (default = 1.0; minimum = 0.0; maximum = 2.0)
            r_c, i.e. the above parameter for c quarks.

            StringZ:rFactB   (default = 0.67; minimum = 0.0; maximum = 2.0)
            r_b, i.e. the above parameter for b quarks.

            StringZ:rFactH   (default = 1.0; minimum = 0.0; maximum = 2.0)
            r_h, i.e. the above parameter for heavier hypothetical quarks, or in general any new coloured particle long-lived enough to hadronize.

            Within the string framework, the b parameter is universal, i.e. common for all flavours. Nevertheless, for fits to experimental data, better agreement can be obtained if both a_Q and b_Q can be set freely in a general expression
            f(z) = 1/z^{1 + r_Q * b_Q * m_Q^2} * (1-z)^a_Q * exp(-b_Q m_T^2 / z)
            The below switches and values can be used to achieve this. They should be used with caution and constitute clear deviations from the Lund philosophy.

            StringZ:useNonstandardC On Off   (default = off)
            use the above nonstandard Lund ansatz for c quarks.

            StringZ:useNonstandardB On Off   (default = off)
            use the above nonstandard Lund ansatz for b quarks.

            StringZ:useNonstandardH On Off   (default = off)
            use the above nonstandard Lund ansatz for hypothetical heavier quarks.

            StringZ:aNonstandardC   (default = 0.3; minimum = 0.0; maximum = 2.0)
            The a parameter in the nonstandard Lund ansatz for c quarks.

            StringZ:aNonstandardB   (default = 0.3; minimum = 0.0; maximum = 2.0)
            The a parameter in the nonstandard Lund ansatz for b quarks.

            StringZ:aNonstandardH   (default = 0.3; minimum = 0.0; maximum = 2.0)
            The a parameter in the nonstandard Lund ansatz for hypothetical heavier quarks.

            StringZ:bNonstandardC   (default = 0.8; minimum = 0.2; maximum = 2.0)
            The b parameter in the nonstandard Lund ansatz for c quarks.

            StringZ:bNonstandardB   (default = 0.8; minimum = 0.2; maximum = 2.0)
            The b parameter in the nonstandard Lund ansatz for b quarks.

            StringZ:bNonstandardH   (default = 0.8; minimum = 0.2; maximum = 2.0)
            The b parameter in the nonstandard Lund ansatz for hypothetical heavier quarks.

            As another nonstandard alternative, it is possible to switch over to the Peterson/SLAC formula [Pet83]
            f(z) = 1 / ( z * (1 - 1/z - epsilon/(1-z))^2 )
            for charm, bottom and heavier (defined as above) by the three flags

            StringZ:usePetersonC On Off   (default = off)
            use Peterson for c quarks.

            StringZ:usePetersonB On Off   (default = off)
            use Peterson for b quarks.

            StringZ:usePetersonH On Off   (default = off)
            use Peterson for hypothetical heavier quarks.

            When switched on, the corresponding epsilon values are chosen to be

            StringZ:epsilonC   (default = 0.05; minimum = 0.01; maximum = 0.25)
            epsilon_c, i.e. the above parameter for c quarks.

            StringZ:epsilonB   (default = 0.005; minimum = 0.001; maximum = 0.025)
            epsilon_b, i.e. the above parameter for b quarks.

            StringZ:epsilonH   (default = 0.005; minimum = 0.0001; maximum = 0.25)
            epsilon_h, i.e. the above parameter for hypothetical heavier quarks, normalized to the case where m_h = m_b. The actually used parameter is then epsilon = epsilon_h * (m_b^2 / m_h^2). This allows a sensible scaling to a particle with an unknown higher mass without the need for a user intervention.

            Fragmentation pT

            The StringPT class handles the choice of fragmentation pT. At each string breaking the quark and antiquark of the pair are supposed to receive opposite and compensating pT kicks according to a Gaussian distribution in p_x and p_y separately. Call sigma_q the width of the p_x and p_y distributions separately, i.e.
            d(Prob) = exp( -(p_x^2 + p_y^2) / 2 sigma_q^2).
            Then the total squared width is
            <pT^2> = <p_x^2> + <p_y^2> = 2 sigma_q^2 = sigma^2.
            It is this latter number that is stored in

            StringPT:sigma   (default = 0.304; minimum = 0.0; maximum = 1.0)
            the width sigma in the fragmentation process.

            Since a normal hadron receives pT contributions for two string breakings, it has a <p_x^2>_had = <p_y^2>_had = sigma^2, and thus <pT^2>_had = 2 sigma^2.

            Some studies on isolated particles at LEP has indicated the need for a slightly enhanced rate in the high-pT tail of the above distribution. This would have to be reviewed in the context of a complete retune of parton showers and hadronization, but for the moment we stay with the current recipe, to boost the above pT by a factor enhancedWidth for a small fraction enhancedFraction of the breakups, where

            StringPT:enhancedFraction   (default = 0.01; minimum = 0.0; maximum = 1.)
            enhancedFraction,the fraction of string breaks with enhanced width.

            StringPT:enhancedWidth   (default = 2.0; minimum = 1.0; maximum = 10.0)
            enhancedWidth,the enhancement of the width in this fraction.

            Jet joining procedure

            String fragmentation is carried out iteratively from both string ends inwards, which means that the two chains of hadrons have to be joined up somewhere in the middle of the event. This joining is described by parameters that in principle follows from the standard fragmentation parameters, but in a way too complicated to parametrize. The dependence is rather mild, however, so for a sensible range of variation the parameters in this section should not be touched.

            StringFragmentation:stopMass   (default = 1.0; minimum = 0.0; maximum = 2.0)
            Is used to define a W_min = m_q1 + m_q2 + stopMass, where m_q1 and m_q2 are the masses of the two current endpoint quarks or diquarks.

            StringFragmentation:stopNewFlav   (default = 2.0; minimum = 0.0; maximum = 2.0)
            Add to W_min an amount stopNewFlav * m_q_last, where q_last is the last q qbar pair produced between the final two hadrons.

            StringFragmentation:stopSmear   (default = 0.2; minimum = 0.0; maximum = 0.5)
            The W_min above is then smeared uniformly in the range W_min_smeared = W_min * [ 1 - stopSmear, 1 + stopSmear ].

            This W_min_smeared is then compared with the current remaining W_transverse to determine if there is energy left for further particle production. If not, i.e. if W_transverse < W_min_smeared, the final two particles are produced from what is currently left, if possible. (If not, the fragmentation process is started over.)

            Simplifying systems

            There are a few situations when it is meaningful to simplify the original task, one way or another.

            HadronLevel:mStringMin   (default = 1.; minimum = 0.5; maximum = 1.5)
            Decides whether a partonic system should be considered as a normal string or a ministring, the latter only producing one or two primary hadrons. The system mass should be above mStringMin plus the sum of quark/diquark constituent masses for a normal string description, else the ministring scenario is used.

            FragmentationSystems:mJoin   (default = 0.3; minimum = 0.2; maximum = 1.)
            When two colour-connected partons are very nearby, with at least one being a gluon, they can be joined into one, to avoid technical problems of very small string regions. The requirement for joining is that the invariant mass of the pair is below mJoin, where a gluon only counts with half its momentum, i.e. with its contribution to the string region under consideration. (Note that, for technical reasons, the 0.2 GeV lower limit is de facto hardcoded.)

            FragmentationSystems:mJoinJunction   (default = 1.0; minimum = 0.5; maximum = 2.)
            When the invariant mass of two of the quarks in a three-quark junction string system becomes too small, the system is simplified to a quark-diquark simple string. The requirement for this simplification is that the diquark mass, minus the two quark masses, falls below mJoinJunction. Gluons on the string between the junction and the respective quark, if any, are counted as part of the quark four-momentum. Those on the two combined legs are clustered with the diquark when it is formed.

            Ministrings

            The MiniStringFragmentation machinery is only used when a string system has so small invariant mass that normal string fragmentation is difficult/impossible. Instead one or two particles are produced, in the former case shuffling energy-momentum relative to another colour singlet system in the event, while preserving the invariant mass of that system. With one exception parameters are the same as defined for normal string fragmentation, to the extent that they are at all applicable in this case. A discussion of the relevant physics is found in [Nor00]. The current implementation does not completely abide to the scheme presented there, however, but has in part been simplified. (In part for greater clarity, in part since the class is not quite finished yet.)

            MiniStringFragmentation:nTry   (default = 2; minimum = 1; maximum = 10)
            Whenever the machinery is called, first this many attempts are made to pick two hadrons that the system fragments to. If the hadrons are too massive the attempt will fail, but a new subsequent try could involve other flavour and hadrons and thus still succeed. After nTry attempts, instead an attempt is made to produce a single hadron from the system. Should also this fail, some further attempts at obtaining two hadrons will be made before eventually giving up.

            Junction treatment

            A junction topology corresponds to an Y arrangement of strings i.e. where three string pieces have to be joined up in a junction. Such topologies can arise if several valence quarks are kicked out from a proton beam, or in baryon-number-violating SUSY decays. Special attention is necessary to handle the region just around the junction, where the baryon number topologically is located. The junction fragmentation scheme is described in [Sjo03]. The parameters in this section should not be touched except by experts.

            StringFragmentation:eNormJunction   (default = 2.0; minimum = 0.5; maximum = 10)
            Used to find the effective rest frame of the junction, which is complicated when the three string legs may contain additional gluons between the junction and the endpoint. To this end, a pull is defined as a weighed sum of the momenta on each leg, where the weight is exp(- eSum / eNormJunction), with eSum the summed energy of all partons closer to the junction than the currently considered one (in the junction rest frame). Should in principle be (close to) sqrt((1 + a) / b), with a and b the parameters of the Lund symmetric fragmentation function.

            StringFragmentation:eBothLeftJunction   (default = 1.0; minimum = 0.5)
            Retry (up to 10 times) when the first two considered strings in to a junction both have a remaining energy (in the junction rest frame) above this number.

            StringFragmentation:eMaxLeftJunction   (default = 10.0; minimum = 0.)
            Retry (up to 10 times) when the first two considered strings in to a junction has a highest remaining energy (in the junction rest frame) above a random energy evenly distributed between eBothLeftJunction and eBothLeftJunction + eMaxLeftJunction (drawn anew for each test).

            StringFragmentation:eMinLeftJunction   (default = 0.2; minimum = 0.)
            Retry (up to 10 times) when the invariant mass-squared of the final leg and the leftover momentum of the first two treated legs falls below eMinLeftJunction times the energy of the final leg (in the junction rest frame). "?>
            pythia8-8.1.80.orig/phpdoc/JetFinders.php0000644000175000017500000000642112217615312016357 0ustar sunsun Jet Finders SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Jet Finders

            Pythia comes with three ";?>built-in jet finders, ClusterJet for e^+e^- events and SlowJet and CellJetfor hadron collider ones. Especially the latter is not so well matched to the standards of its field, however. (But it is closely related to the anti-kT algorithm, so is also not completely disconnected [Cac08].)

            SlowJet can do jet finding according to the current-day kT, Cambridge/Aachen and anti-kT algorithms. It can be run in two modes. The original one is a native implementation which, as the name indicates, is rather slow. However, with the release of the fjcore code from FastJet [Cac06, Cac12], the default mode has become to use the fjcore methods. This is transparent to the user.

            FastJet

            SlowJet does not exhaust all the posssibilities of the fjcore code, so users are welcome to extend on the existing functionality by a direct usage of the fjcore methods.

            Missing from fjcore is a number of aspects, such as jet areas functionality, background estimation, access to other algorithms via plugins, interface to CGAL and tools such as filters and taggers. Therefore, for more sophisticated jet studies the complete FastJet package needs to be linked. This is foreseen in the configure file in the examples subdirectory, and the main71.cc and main72.cc programs contain examples how it can be used with Pythia events. (Even if these examples do not go beyond the functionality that SlowJet can offer.)

            The latter program makes use of the include/Pythia8/FastJet3.h header file, contributed by Gavin Salam. This allows simple input of a Pythia particle into a FastJet one, either retaining only the four-momentum or the full particle information. Thereby more sophisticated selectors become possible at the FastJet level. This code could be duplicated, with trivial modifications, to augment the fjcore package functionality in an identical manner, should the need arise. pythia8-8.1.80.orig/phpdoc/ROOTusage.php0000644000175000017500000002404512217615312016134 0ustar sunsun ROOT usage SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            ROOT usage

            Many PYTHIA users wish to use ROOT to produce histograms, or even to run PYTHIA as a plugin to ROOT. This is possible. It is not a task supported by the PYTHIA team, however. All issues involving ROOT usage should be directed to the ROOT team, or to the local support team of your collaboration. Below some helpful hints have been collected. The text is based on contributions by Rene Brun, Andreas Morsch and Axel Naumann. Another example may be found in the VINCIA add-on program for parton showers, but this should also work for a PYTHIA standalone run.

            Note that in all that follows, a Linux-type system with a Bash shell and GNU Make is assumed. In particular, for Mac OS X, the LD_LIBRARY_PATH should be replaced with DYLD_LIBRARY_PATH and the extension for shared libraries .so should be replaced with .dylib.


            Standalone usage

            One can perform the generation and analysis of events in a completely standalone fashion, and only use ROOT to process the completed events. Some example programs are provided in the rootexamples directory, with details provided below and in the README file. The examples assume that you have already compiled the PYTHIA library, ROOT is installed, and that all paths have been setup correctly (e.g. PATH and LD_LIBRARY_PATH). If these paths are not already set, ROOT typically comes with a shell script to set these paths, which can be run with
                source /path_to_ROOT_installation/bin/thisroot.sh
            

            Histogramming with ROOT

            An example of histogramming with ROOT is provided in rootexamples/hist.cc. It may be compiled and run with the following commands
                make hist
                ./hist.exe
            
            After PYTHIA has run, a ROOT histogram of the charged multiplicity in the events will be shown. This is now stored in the hist.root file.

            Storing PYTHIA events in ROOT trees

            Instead of only generating histograms, it is possible to store entire PYTHIA events in ROOT trees. The tree example in the rootexamples subdirectory provides an example of this and is comprised of the following files
            • tree.cc is the main example program showing how PYTHIA events can be stored in ROOT trees.
            • pythiaLinkdef.h is used by Makefile to generate the dictionary for all PYTHIA classes involved in the IO, as needed for the example.
            • pythiaROOT.h is a small include declaring the Pythia8 namespace as default.

            The example may be compiled and run with
                make tree
                ./tree.exe
            
            After the example has run, the pytree.root file will now be present containing the PYTHIA events. Note that files can become quite large when many events are generated.


            PYTHIA as a plugin to ROOT

            In more ROOT-centric applications, PYTHIA can be run as a ROOT plug-in. This requires a version of ROOT that has been installed from source. The reason is that the interfaces depend on PYTHIA header files that are not distributed with ROOT. Installing ROOT is not more difficult than the PYTHIA installation, and some guidelines are provided below.

            Installation

            To be run as a plugin, PYTHIA must be compiled as a shared library. This is achieved by running the PYTHIA configure script with the --enable-shared option before make is run.

            Define an environment variable for the path to your PYTHIA installation directory
                export PYTHIA8=path_to_PYTHIA8_installation
            
            Before compiling ROOT, configure ROOT by running the configure command including the following options
                --enable-pythia8
                --with-pythia8-incdir=$PYTHIA8/include
                --with-pythia8-libdir=$PYTHIA8/lib
            
            In case ROOT has already been compiled before, it will only recompile the PYTHIA module and build the library libEGPythia8.

            Interfaces

            When running PYTHIA as a plugin, the exact interface structure becomes very relevant. ROOT provides two simple interfaces (wrappers) for PYTHIA 8. The code for these interfaces are located in
                path_to_ROOT_source/montecarlo/pythia8
            

            The two interfaces are
            • TPythia8 is an implementation of the TGenerator interface for PYTHIA 8.
              It allows you to use PYTHIA within a ROOT macro or as a plug-in for a general-purpose particle generator based on this interface. The main methods of the interface are
              • GenerateEvent() which triggers the generation of the next event, and
              • ImportParticles(TClonesArray* particles) which copies the native PYTHIA stack into a TClonesArray of TParticles.
              In addition, some methods that are directly related to corresponding PYTHIA methods are implemented
              • ReadString(const char* string) -> readString(...)
              • ReadConfigFile(const char* string) -> readFile(...)
              • Initialize(int idAin, int idBin, double ecms) -> init(...)
              • EventListing() -> event.list()
              • PrintStatistic() -> statistics()
              These methods provide already the basic PYTHIA functionality interactively from the ROOT command line. However, this does not mean that the usage of PYTHIA from within ROOT is restricted to these methods. In compiled code, one can always obtain a pointer to the Pythia instance e.g.
                  TPythia8        *tp = new TPythia8();
                  Pythia8::Pythia *p  = tp->Pythia8();
              giving access to the full PYTHIA functionality. To access this functionality in the CINT interpreter see the "Advanced usage" section below.
            • TPythia8Decayer is an implementation of the TVirtualMCDecayer interface.
              It allows you to use PYTHIA as a plug-in decayer for simulation frameworks based on the Virtual Monte Carlo (VMC) interface classes. The main methods of the interface are
              • TPythia8Decayer::Init() for initialisation,
              • TPythia8Decayer::Decay(Int_t pdg, TLorentzVector* p) to decay a particle with PDG code pdg and 4-momentum p, and
              • ImportParticles(TClonesArray* particles) to retrieve the decay products as TParticles in the TClonesArray particles.

            An example

            A basic example for generating minimum-bias events with PYTHIA 8 inside a ROOT macro, and filling some histograms with the kinematics of the final-state particles is provided in either of the locations below
                /path_to_ROOT_source/tutorials/pythia/pythia8.C
                /path_to_ROOT_installation/share/doc/root/tutorials/pythia/pythia8.C
            

            Note that before executing this script
            • the environment variables PYTHIA8 and PYTHIA8DATA must be setup correctly e.g.
                  export PYTHIA8=/path_to_PYTHIA_installation
                  export PYTHIA8DATA=$PYTHIA8/xmldoc
                
            • your LD_LIBRARY_PATH must contain the location of the PYTHIA 8 shared library, e.g.
                  export LD_LIBRARY_PATH=$LD_LIBRARY_PATH:path_to_PYTHIA8_installation/lib
                
            The script can then be run with ROOT
                root pythia8.C
            
            After execution, ROOT will display some histograms from the event generation.

            Advanced usage

            To access the full PYTHIA functionality from the CINT interpreter, a ROOT dictionary must be created. An example of creating this dictionary is contained in the rootexamples directory. The pythiaDict.so library may be created by running
                make dict
            
            This may then be loaded in ROOT giving full access to the full PYTHIA 8 functionality, e.g. in an interactive session
                gSystem->Load("path_to_PYTHIA8_installation/rootexamples/pythiaDict");
                Pythia8::Pythia *p = new Pythia8::Pythia();
                p->readString("SoftQCD:nonDiffractive = on");
            
            pythia8-8.1.80.orig/phpdoc/Welcome.php0000644000175000017500000000106512217615312015714 0ustar sunsun PYTHIA 8 online manual pythia8-8.1.80.orig/phpdoc/SampleMainPrograms.php0000644000175000017500000004112012217615312020056 0ustar sunsun Sample Main Programs SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Sample Main Programs

            Descriptions of available classes, methods and settings are all very good and useful. Ultimately they are necessary for you to be able to fine-tune your runs to the task at hand. To get going, however, nothing helps like having explicit examples to study. This is what is provided in the examples subdirectory, along with instructions how they should be run:
            • main00.cc : does not exist, but it has been defined in the Makefile, so this name could be used for a simple first test run.
            • main01.cc : a simple study of the charged multiplicity for jet events at the LHC. (Brief example fitting on one slide.)
            • main02.cc : a simple study of the pT spectrum of Z bosons at the Tevatron. (Brief example fitting on one slide.)
            • main03.cc : a simple study of several different kinds of events, with the choice to be made in the main03.cmnd "cards file".
            • main04.cc : tests of cross sections, multiplicities and average transverse momenta for elastic, diffractive and nondiffractive topologies, using main04.cmnd to pick processes.
            • main05.cc : generation of QCD jet events at the LHC, with jet analysis using the SlowJet inclusive anti-kT sequential-recombination finder and the CellJet cone-jet finder.
            • main06.cc : generation of LEP1 hadronic events, i.e. e^+e^- -> gamma*/Z^0 -> q qbar, with charged multiplicity, sphericity, thrust and jet analysis.
            • main07.cc : set up a fictitious production process to a generic resonance, where you easily can compose your own list of (two-body) decay modes to a variety of final states. Also traces decay chains down to truly stable particles: gamma, e+-, p/pbar and neutrinos. Suitable for astroparticle applications, like neutralino pair annihilation, where cross sections are calculated separately in another program.
            • main08.cc : generation of the QCD jet cross section biased towards higher pT values, by two different techniques. Firstly, by splitting the run into subruns, each in its own pT bin, and adding the results properly reweighted. Two suboptions, with limits set either in the main program or by subrun specification in the main08.cmnd file. Secondly, by a continuous reweighting with a pT^4 bias in the selection, compensated by a 1/pT^4 event weight. Also inclusion of soft processes is illustrated, with subruns and weighted events.
            • main09.cc : generation of two predetermined hard interactions in each event.
            • main10.cc : illustration how userHooks can be used interact directly with the event-generation process.
            • main11.cc : a study of top events, fed in from the Les Houches Event File ttbar.lhe, here generated by PYTHIA 6.4. This file currently only contains 100 events so as not to make the distributed PYTHIA package too big, and so serves mainly as a demonstration of the principles involved.
            • main12.cc : a more sophisticated variant of main11.cc, where two Les Houches Event Files (ttbar.lhe and ttbar2.lhe) successively are used as input. Also illustrating some other aspects, like the capability to mix in internally generated events.
            • main13.cc : a streamlined version of main12.cc, where two Les Houches Event Files (ttbar.lhe and ttbar2.lhe) successively are used as input in main13.cmnd file.
            • main14.cc : a systematic comparison of several cross section values with their corresponding values in PYTHIA 6.4, the latter available as a table in the code.
            • main15.cc : loop over several tries, either to redo B decays only or to redo the complete hadronization chain of an event. Since much of the generation process is only made once this is a way to increase efficiency.
            • main16.cc : put all user analysis code into a class of its own, separate from the main program; provide the "cards file" name as a command-line argument. Also exemplifies how Higgs mass, width and branching ratios can be set by hand.
            • main17.cc : shows (a) how to use UserHooks to regularize onium cross section for pT -> 0, and (b) how decays could be handled externally.
            • main18.cc : shows how to write an event filter class, where you keep a vector of pointers to the subset of particles you want to study further. The event record itself remains unchanged.
            • main19.cc : use several instances of Pythia, one for signal events and others for a variable number of pileup and "beam-gas" events, combined into one common event record.
            • main20.cc : shows how PYTHIA 8 can write a Les Houches Event File, using facilities potentially useful also for other programs to write an LHEF.
            • main21.cc : an example how a single particle or various parton-level configurations can be input directly for hadronization, without being tied to the full process-generation machinery, e.g. to study the hadronization of junction topologies. Can also be used for single-resonance decays, with showers.
            • main22.cc : shows how an external resonance can be implemented as a new class derived from a PYTHIA base class, and be used in an external process, both of them handed in for generation as with normal internal classes.
            • main23.cc : shows how an external beam momentum spread and vertex location generator can be implemented as a new class derived from a PYTHIA base class, and then handed in for internal use. Also how to use an external random-number generator and an external parton distribution set.
            • main24.cc : tests of internally implemented cross sections for Supersymmetric particle production, with SUSY spectrum defined in cmssm.spc and settings in main24.cmnd. For illustration, an alternative example spectrum is also available, sps1aWithDecays.spc, which contains a decay table in SLHA format.
            • main25.cc : input RPV-SUSY events from an LHEF file that contains an SLHA spectrum inside its header. The event file, main25.lhe, contains a sample events that illustrate how to arrange color tags in the presence of the color-space epsilon tensors that accompany baryon number violating event topologies.
            • main26.cc : test program for processes in scenarios with large extra dimensions or unparticles.
            • main27.cc : production of Kaluza-Klein gamma/Z states in TeV-sized extra dimensions.
            • main28.cc : production of long-lived R-hadrons, that are forced to decay at a separate vertices and possibly with changed momenta.
            • main31.cc : exemplifies an improved matching of parton showers to LHEF-style input based on the POWHEG approach. The main31.cmnd allows to switch between several different matching options. It also allows to select input process, in this case either for the POWHEG-hvq program applied to top pair production [Cor10] or for QCD 2+3-jet events. The small samples of input events are stored in the powheg-hvq.lhe and powheg-dijets.lhe files, respectively.
            • main32.cc : exemplifies MLM merging, either in the ALPGEN variant or in the Madgraph one, and with input events either from ALPGEN or from Madgraph, with relevant control cards stored in main32.cmnd. See ";?>Jet Matching for further details. Traditionally the ALPGEN output is split into one file with events and another with parameters and cross sections (unlike in LHEF). Here a sample of W + 3 jets events is stored in main32.unw and the parameters to go with it in main32_unw.par. Madgraph events are taken from the w+_production_lhc_2.lhe file in this case.
            • main41.cc : similar to main01, except that the event record is output in the HepMC event record format. Requires that HepMC is properly linked. Note that the hepmcout41.dat output file can become quite big; so no example is included in this distribution.
            • main42.cc : a streamlined version for the generation of events that are then stored in HepMC format, without any event analysis. That is, all physics studies will have to be done afterwards. The name of the input "cards file" (e.g. main42.cmnd) and output HepMC event file (e.g. hepmcout42.dat) are to be provided as command-line arguments. Requires that HepMC is properly linked. Note that the HepMC output file can become quite big; so no example is included in this distribution.
            • main46.cc : illustrates how to write a ProMC file with PYTHIA events. Note that this example cannot (yet) be built by the PYTHIA Makefile, but a relevant Makefile is available on the ProMC webpage http://atlaswww.hep.anl.gov/asc/promc/.
            • main51.cc : a test of the shape of parton densities, as a check prior to using a given PDF set in a generator. Requires that LHAPDF is properly linked.
            • main52.cc : compares the charged multiplicity distribution, and a few other minimum-bias physics aspects, between default PYTHIA PDF and another one. Requires that LHAPDF is properly linked.
            • main53.cc : tests the possibility to do backwards evolution from an incoming photon at the hard interaction. Requires that you link to a LHAPDF set that includes the photon PDF.
            • main61.cc : a streamlined version for the generation of events that are then stored in HepMC format, without any event analysis. That is, just like main42.cc, with the difference that main61.cc can be used in conjunction with LHAPDF. The name of the input "cards file" (e.g. main61.cmnd) and output HepMC event file (e.g. hepmcout61.dat) are to be provided as command-line arguments. Requires that HepMC and LHAPDF are properly linked. Note that the HepMC output file can become quite big; so no example is included in this distribution.
            • main62.cc : a further extension of main61.cc, where subruns are used to process several consecutive LHEF, as in main13.cc, with information stored e.g in main62.cmnd. Other comments as for main61.cc.
            • main71.cc : an example how the FastJet jet finding package can be linked to allow an analysis of the final state, in this case for a study of W + jet production.
            • main72.cc : a comparison of SlowJet and FastJet jet finding, showing that they find the same jets if run under identical conditions, in this case for QCD jets.
            • main81.cc : do CKKW-L merging with a merging scale defined in kT. Input is provided by the main81.cmnd file and the three data files w+_production_lhc_0.lhe, w+_production_lhc_1.lhe and w+_production_lhc_2.lhe.
            • main82.cc : do CKKW-L merging with a user-defined merging scale function. Input is provided by the main82.cmnd file and the three data files w+_production_lhc_0.lhe, w+_production_lhc_1.lhe and w+_production_lhc_2.lhe.
            • main83.cc : as main82.cc but with an additional cut on the lowest multiplicity allowed for the reclustered state. The same input as for main82.cc can be used.
            • main84.cc : do CKKW-L merging with output in such a way that it can be used in subsequent RIVET analyses. Input is provided by the main84.cmnd file and the three data files w+_production_lhc_0.lhe, w+_production_lhc_1.lhe and w+_production_lhc_2.lhe.
            • main85.cc : do CKKW-L merging, with HepMC event output. Input settings are provided by the main85.cmnd file. This example program allows the use of input Les Houches events that are regularised with only very minimal cuts, and on which Pythia itself should enforce the more restrictive merging scale cut. The example program can be used with the input files w_production_tree_0.lhe, w_production_tree_1.lhe and w_production_tree_2.lhe.
            • main86.cc : do unitarised ME+PS (UMEPS) merging, with HepMC event output. Input settings are provided by the main86.cmnd file. This example program allows the consistent use of input Les Houches events that are regularised with only very minimal cuts, similar to main85.cc. The example program can be used with the input files w_production_tree_0.lhe, w_production_tree_1.lhe and w_production_tree_2.lhe. The program will produce positively and negatively weighted events. See ";?>UMEPS Merging for further details.
            • main87.cc : do NL3 NLO merging, with inclusive NLO input, and with HepMC event output. Input settings are provided by the main87.cmnd file. This example program allows the consistent use of input Les Houches events that are regularised with only very minimal cuts, similar to main85.cc. The example program can be used with the tree-level input files w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and the inclusive POWHEG input files w_production_powheg_0.lhe, w_production_powheg_1.lhe. The program will produce positively and negatively weighted events. See ";?>NLO Merging (NL3 section) for further details.
            • main88.cc : do unitarised NLO+PS (UNLOPS) merging, with inclusive NLO input, and with HepMC event output. Input settings are provided by the main88.cmnd file. This example program allows the consistent use of input Les Houches events that are regularised with only very minimal cuts, similar to main85.cc. The example program can be used with the tree-level input files w_production_tree_0.lhe, w_production_tree_1.lhe, w_production_tree_2.lhe and the inclusive POWHEG input files w_production_powheg_0.lhe, w_production_powheg_1.lhe. The program will produce positively and negatively weighted events. See ";?>NLO Merging (UNLOPS section) for further details.
            In addition two main program illustrating the use of ROOT are available in the rootexamples subdirectory:
            • hist.cc : shows how ROOT can be used for histogramming in a program that for the rest is structured like a normal PYTHIA run.
            • tree.cc : shows how PYTHIA events can be stored as ROOT trees.
            This subdirectory also contains a special Makefile and related documentation. pythia8-8.1.80.orig/phpdoc/ProgramFlow.php0000644000175000017500000015752012217615312016570 0ustar sunsun Program Flow SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Program Flow

            Recall that, to first order, the event generation process can be subdivided into three stages:
            1. Initializaion.
            2. The event loop.
            3. Finishing.
            This is reflected in how the top-level Pythia class should be used in the user-supplied main program, further outlined in the following. Since the nature of the run is defined at the initialization stage, this is where most of the PYTHIA user code has to be written. So as not to confuse the reader unduly, the description of initialization options has been subdivided into what would normally be used and what is intended for more special applications.

            At the bottom of this webpage is a complete survey of all public Pythia methods and data members, in a more formal style than the task-oriented descriptions found in the preceding sections. This offers complementary information.

            Initialization - normal usage

            1. Already at the top of the main program file, you need to include the proper header file
                  #include "Pythia8/Pythia.h"
              
              To simplify typing, it also makes sense to declare
                  using namespace Pythia8; 
              
            2. The first step is to create a generator object, e.g. with
                   Pythia pythia;
              
              It is this object that we will use from now on. Normally a run will only contain one Pythia object. (But you can use several Pythia objects, which then will be independent of each other.)
              By default all output from Pythia will be on the cout stream, but the list methods below do allow output to alternative streams or files.
            3. You next want to set up the character of the run. The pages under the "Setup Run Tasks" heading in the index describe all the options available (with some very few exceptions, found on the other pages). The default values and your modifications are stored in two databases, one for ";?>generic settings and one for ";?>particle data. Both of these are initialized with their default values by the Pythia constructor. The default values can then be changed, primarily by one of the two ways below, or by a combination of them.

              a) You can use the

                  pythia.readString(string);
              
              method repeatedly to do a change of a property at a time. The information in the string is case-insensitive, but upper- and lowercase can be combined for clarity. The rules are that
              (i) if the first nonblank character of the string is a letter it is assumed to contain a setting, and is sent on to pythia.settings.readString(string);
              (ii) if instead the string begins with a digit it is assumed to contain particle data updates, and so sent on to pythia.particleData.readString(string);
              (iii) if none of the above, the string is assumed to be a comment, i.e. nothing will be done.
              In the former two cases, a warning is issued whenever a string cannot be recognized (maybe because of a spelling mistake).
              Some examples would be
                  pythia.readString("TimeShower:pTmin = 1.0");
                  pythia.readString("111:mayDecay = false");
              
              The readString(string) method is intended primarily for a few changes. It can also be useful if you want to construct a parser for input files that contain commands both to PYTHIA and to other libraries.

              b) You can read in a file containing a list of those variables you want to see changed, with a

                  pythia.readFile(fileName);
              
              Each line in this file with be processes by the readString(string) method introduced above. You can thus freely mix comment lines and lines handed on to Settings or to ParticleData.
              This approach is better suited for more extensive changes than a direct usage of readString(string), and can also avoid having to recompile and relink your main program between runs.
              It is also possible to read input from an istream, by default cin, rather than from a file. This may be convenient if information is generated on-the-fly, within the same run.

              Changes are made sequentially in the order the commands are encountered during execution, meaning that if a parameter is changed several times it is the last one that counts. The two special ";?>Tune:ee and ";?>Tune:pp modes are expanded to change several settings in one go, but these obey the same ordering rules.

            4. Next comes the initialization stage, where all remaining details of the generation are to be specified. There is one standard method to use for this

              pythia.init();
              with no arguments will read all relevant information from the ";?>Settings and ";?>ParticleData databases. Specifically the setup of incoming beams and energies is governed by the the beam parameters from the ";?>Beams group of variables. If you don't change any of those you will default to proton-proton collisions at 14 TeV, i.e. the nominal LHC values.

              A few alternative forms are available, where the arguments of the init(...) call can be used to set the beam parameters. These alternatives are now deprecated, and will be removed for PYTHIA 8.2.

              a) pythia.init( idA, idB, eCM);
              lets you specify the identities and the CM energy of the two incoming beam particles, with A (B) assumed moving in the +z (-z) direction.

              b) pythia.init( idA, idB, eA, eB);
              is similar, but the two beam energies can be different, so the collisions do not occur in the CM frame. If one of the beam energies is below the particle mass you obtain a fixed-target topology.

              c) pythia.init( idA, idB, pxA, pyA, pzA, pxB, pyB, pzB);
              is similar, but here you provide the three-momenta (p_x, p_y, p_z) of the two incoming particles, to allow for arbitrary beam directions.

              d) pythia.init(fileName);
              assumes a file in the ";?>Les Houches Event File format is provided.

              e) pythia.init( LHAup*);
              assumes ";?>Les Houches Accord initialization and event information is available in an LHAup class object, and that a pointer to this object is handed in.

            5. If you want to have a list of the generator and particle data used, either only what has been changed or everything, you can use
                  pythia.settings.listChanged();
                  pythia.settings.listAll();
                  pythia.particleData.listChanged(); 
                  pythia.particleData.listAll(); 
              

            The event loop

            1. Inside the event generation loop you generate the next event using the next() method,
                  pythia.next();
              
              This method takes no arguments; everything has already been specified. It does return a bool value, however, false when the generation failed. This can be a "programmed death" when the supply of input parton-level configurations on file is exhausted. It can alternatively signal a failure of Pythia to generate an event, or unphysical features in the event record at the end of the generation step. It makes sense to allow a few false values before a run is aborted, so long as the related faulty events are skipped.
            2. The generated event is now stored in the event object, of type ";?>Event, which is a public member of pythia. You therefore have access to all the tools described on the pages under the "Study Output" header in the index. For instance, an event can be listed with pythia.event.list(), the identity of the i'th ";?>particle is given by pythia.event[i].id(), and so on.
              The hard process - roughly the information normally stored in the Les Houches Accord event record - is available as a second object, process, also of type Event.
              A third useful public object is ";?>info, which offers a set of one-of-a kind pieces of information about the most recent event.

            Finishing

            1. At the end of the generation process, you can call
                  pythia.stat(); 
              
              to get some run statistics, on cross sections and the number of errors and warnings encountered. The alternative pythia.statistics(...); is equivalent but deprecated.

            Advanced usage, mainly for initialization

            A) Necessary data are automatically loaded when you use the default PYTHIA installation directory structure and run the main programs in the examples subdirectory. However, in the general case, you must provide the path of the xmldoc directory, where default settings and particle data are found. This can be done in two ways.
            1. You can set the environment variable PYTHIA8DATA to contain the location of the xmldoc directory. In the csh and tcsh shells this could e.g. be
                   setenv PYTHIA8DATA /home/myname/pythia81xx/xmldoc
              
              while in other shells it could be
                   export PYTHIA8DATA=/home/myname/pythia81xx/xmldoc
              
              where xx is the subversion number.
              Recall that environment variables set locally are only defined in the current instance of the shell. The above lines should go into your .cshrc and .bashrc files, respectively, if you want a more permanent assignment.
            2. You can provide the path as argument to the Pythia constructor, e.g.
                   Pythia pythia("/home/myname/pythia81xx/xmldoc");
              
            where again xx is the subversion number.
            When PYTHIA8DATA is set it takes precedence, else the path in the constructor is used, else one defaults to the ../xmldoc directory.

            B) You can override the default behaviour of PYTHIA not only by the settings and particle data, but also by replacing some of the PYTHIA standard routines by ones of your own. Of course, this is only possible if your routines fit into the general PYTHIA framework. Therefore they must be coded according to the the rules relevant in each case, as a derived class of a PYTHIA base class, and a pointer to such an object must be handed in by one of the methods below. These calls must be made before the pythia.init(...) call.

            1. If you are not satisfied with the list of parton density functions that are implemented internally or available via the LHAPDF interface (see the ";?>PDF Selection page), you can supply your own by a call to the setPDFPtr(...) method
                    pythia.setPDFptr( pdfAPtr, pdfBPtr); 
              
              where pdfAPtr and pdfBPtr are pointers to two Pythia ";?>PDF objects. Note that pdfAPtr and pdfBPtr cannot point to the same object; even if the PDF set is the same, two copies are needed to keep track of two separate sets of x and density values.
              If you further wish to use separate PDF's for the hard process of an event than the ones being used for everything else, the extended form
                    pythia.setPDFptr( pdfAPtr, pdfBPtr, pdfHardAPtr, pdfHardBPtr); 
              
              allows you to specify those separately, and then the first two sets would only be used for the showers and for multiparton interactions.
            2. If you want to link to an external generator that feeds in events in the LHA format, you can call the setLHAupPtr(...) method
                    pythia.setLHAupPtr( lhaUpPtr);
              
              where the lhaUpPtr derives from the ";?>LHAup base class.
            3. If you want to perform some particle decays with an external generator, you can call the setDecayPtr(...) method
                    pythia.setDecayPtr( decayHandlePtr, particles);
              
              where the decayHandlePtr derives from the ";?>DecayHandler base class and particles is a vector of particle codes to be handled.
            4. If you want to use an external random number generator, you can call the setRndmEnginePtr(...) method
                    pythia.setRndmEnginePtr( rndmEnginePtr); 
              
              where rndmEnginePtr derives from the ";?>RndmEngine base class. The Pythia default random number generator is perfectly good, so this is only intended for consistency in bigger frameworks.
            5. If you want to interrupt the evolution at various stages, to interrogate the event and possibly veto it, or you want to reweight the cross section, you can use
                    pythia.setUserHooksPtr( userHooksPtr); 
              
              where userHooksPtr derives from the ";?>UserHooks base class.
            6. If you want to use your own merging scale definition for matrix element + parton shower merging, you can call
                    pythia.setMergingHooksPtr( mergingHooksPtr); 
              
              where mergingHooksPtr derives from the ";?>MergingHooks base class.
            7. If you want to use your own parametrization of beam momentum spread and interaction vertex, rather than the provided simple Gaussian parametrization (off by default), you can call
                    pythia.setBeamShapePtr( beamShapePtr); 
              
              where beamShapePtr derives from the ";?>BeamShape base class.
            8. If you want to implement a cross section of your own, but still make use of the built-in phase space selection machinery, you can use
                    pythia.setSigmaPtr( sigmaPtr);
              
              where sigmaPtr of type SigmaProcess* is an instance of a class derived from one of the Sigma1Process, Sigma2Process and Sigma3Process base classes in their turn derived from ";?>SigmaProcess. This call can be used repeatedly to hand in several different processes.
            9. If your cross section contains the production of a new resonance with known analytical expression for all the relevant partial widths, you can make this resonance available to the program with
                    pythia.setResonancePtr( resonancePtr);
              
              where resonancePtr of type ResonanceWidths* is an instance of a class derived from the ";?>ResonanceWidths base class. In addition you need to add the particle to the normal ";?>particle and decay database. This procedure can be used repeatedly to hand in several different resonances.
            10. If you are a real expert and want to ";?>replace the PYTHIA initial- and final-state showers, you can use
                    pythia.setShowerPtr( timesDecPtr, timesPtr, spacePtr);
              
              where timesDecPtr and timesPtr derive from the TimeShower base class, and spacePtr from SpaceShower.

            C) Some comments on collecting several tasks in the same run.

            1. PYTHIA has not been written for threadsafe execution on multicore processors. If you want to use all cores, the most efficient way presumably is to start correspondingly many jobs, with different random number seeds, and add the statistics at the end. However, note that several instances can be set up in the same main program, since instances are completely independent of each other, so each instance could be run inside a separate thread.
            2. In some cases it is convenient to use more than one Pythia object. The key example would be the simultaneous generation of signal and pileup events, see main19.cc. The two objects are then set up and initialized separately, and generate events completely independently of each other. It is only afterwards that the event records are combined into one single super-event per beam crossing.
            3. When time is not an issue, it may be that you want to perform several separate subruns sequentially inside a run, e.g. to combine results for several kinematical regions or to compare results for some different tunes of the underlying event. One way to go is to create (and destroy) one pythia object for each subrun, in which case they are completely separate. You can also use the same pythia object, only doing a new init(...) call for each subrun. In that case, the settings and particle databases remain as they were in the previous subrun, only affected by the specific changes you introduced in the meantime. You can put those changes in the main program, with pythia.readString(string), using your own logic to decide which ones to execute in which subrun. A corresponding possibility exists with pythia.readFile(fileName, subrun) (or an istream instead of a fileName), which as second argument can take a non-negative subrun number. Then only those sections of the file before any Main:subrun = ... line or with matching subrun number will be read. That is, the file could have a structure like
                  ( lines always read, i.e. "default values" always (re)set )
                  Main:subrun = 1
                  ( lines only read with readFile(fileName, 1) )
                  Main:subrun = 2
                  ( lines only read with readFile(fileName, 2) )
              
              Both of these possibilities are illustrated in main08.cc.
            4. When working with Les Houches Event Files, it may well be that your intended input event sample is spread over several files, that you all want to turn into complete events in one and the same run. There is no problem with looping over several subruns, where each new subrun is initialized with a new file, with name set in Beams:LHEF. However, in that case you will do a complete re-initialization each time around. If you want to avoid this, note that the flag Beams:newLHEFsameInit = true can be set for the second and subsequent subruns. Then the new file will be simulated with the same initialization data as already set in a previous pythia.init() call. The burden rests on you to ensure that this is indeed correct, e.g. that the two event samples have not been generated for different beam energies. Also note that cross sections for processes will be based on the information in the first-read file, when the full initialization is performed.

            The Pythia Class

            Here follows the complete survey of all public Pythia methods and data members.

            Constructor and destructor

            Pythia::Pythia(string xmlDir = "../xmldoc",bool printBanner = true)  
            creates an instance of the Pythia event generators, and sets initial default values, notably for all settings and particle data. You may use several Pythia instances in the same run; only when you want to access external static libraries could this cause problems. (This includes in particular Fortran libraries such as ";?>LHAPDF.)
            argument xmlDir (default = ../xmldoc) : allows you to choose from which directory the default settings and particle data values are read in. If the PYTHIA8DATA environment variable has been set it takes precedence. Else this optional argument allows you to choose another directory location than the default one. Note that it is only the directory location you can change, its contents must be the ones of the xmldoc directory in the standard distribution.
            argument printBanner (default = true) : can be set false to stop the program from printing a banner. The banner contains useful information, so this option is only intended for runs with multiple Pythia instances, where output needs to be restricted.

            Pythia::~Pythia  
            the destructor deletes the objects created by the constructor.

            Set up run

            bool Pythia::readString(string line, bool warn = true)  
            reads in a single string, that is interpreted as an instruction to modify the value of a ";?>setting or ";?>particle data, as already described above.
            argument line : the string to be interpreted as an instruction.
            argument warn (default = true) : write a warning message or not whenever the instruction does not make sense, e.g. if the variable does not exist in the databases.
            Note: the method returns false if it fails to make sense out of the string.

            bool Pythia::readFile(string fileName, bool warn = true, int subrun = SUBRUNDEFAULT)  
            bool Pythia::readFile(string fileName, int subrun = SUBRUNDEFAULT)  
            bool Pythia::readFile(istream& inStream = cin, bool warn = true, int subrun = SUBRUNDEFAULT)  
            bool Pythia::readFile(istream& inStream = cin, int subrun = SUBRUNDEFAULT)  
            reads in a whole file, where each line is interpreted as an instruction to modify the value of a ";?>setting or ";?>particle data, cf. the above readString method. All four forms of the readFile command share code for actually reading a file.
            argument fileName : the file from which instructions are read.
            argument inStream : an istream from which instructions are read.
            argument warn (default = true) : write a warning message or not whenever the instruction does not make sense, e.g. if the variable does not exist in the databases. In the command forms where warn is omitted it is true.
            argument subrun : allows you have several optional sets of commands within the same file. Only those sections of the file before any Main:subrun = ... line or following such a line with matching subrun number will be read. The subrun number should not be negative; negative codes like SUBRUNDEFAULT corresponds to no specific subrun.
            Note: the method returns false if it fails to make sense out of any one line.

            bool Pythia::setPDFPtr( PDF* pdfAPtr, PDF* pdfBPtr, PDF* pdfHardAPtr = 0, PDF* pdfHardBPtr = 0)  
            offers the possibility to link in external PDF sets for usage inside the program. The rules for constructing your own class from the PDF base class are described ";?>here.
            argument pdfAPtr, pdfBPtr : pointers to two PDF-derived objects, one for each of the incoming beams. The two objects have to be instantiated by you in your program. Even if the two beam particles are the same (protons, say) two separate instances are required, since current information is cached in the objects. If both arguments are zero then any previous linkage to external PDF's is disconnected, see further Note 2 below.
            argument pdfHardAPtr, pdfHardBPtr (default = 0) : pointers to two further PDF-derived objects, one for each of the incoming beams. Normally only the first two arguments above would be used, and then the same PDF sets would be invoked everywhere. If you provide these two further pointers then two different sets of PDF's are used. This second set is then exclusively for the generation of the hard process from the process matrix elements library. The first set above is for everything else, notably parton showers and multiparton interactions.
            Note 1: The method returns false if the input is obviously incorrect, e.g. if two (nonzero) pointers agree.
            Note 2: If you want to combine several subruns you can call setPDFPtr with new arguments before each Pythia::init(...) call. To revert from external PDF's to the normal internal PDF selection you must call setPDFPtr(0, 0) before Pythia::init(...).

            bool Pythia::setLHAupPtr( LHAup* lhaUpPtrIn)  
            offers linkage to an external generator that feeds in events in the LHA format, see ";?>Les Houches Accord, assuming that ";?>Beams:frameType = 5 has been set.
            argument lhaUpPtrIn : pointer to a LHAup-derived object.
            Note: The method currently always returns true.

            bool Pythia::setDecayPtr( DecayHandler* decayHandlePtr, vector<int> handledParticles)  
            offers the possibility to link to an external program that can do some of the particle decays, instead of using the internal decay machinery. With particles we here mean the normal hadrons and leptons, not top quarks, electroweak bosons or new particles in BSM scenarios. The rules for constructing your own class from the DecayHandler base class are described ";?>here. Note that you can only provide one external object, but this object in its turn could very well hand on different particles to separate decay libraries.
            argument decayHandlePtr : pointer to a DecayHandler-derived object. This object must be instantiated by you in your program.
            argument handledParticles : vector with the PDG identity codes of the particles that should be handled by the external decay package. You should only give the particle (positive) codes; the respective antiparticle is always included as well.
            Note: The method currently always returns true.

            bool Pythia::setRndmEnginePtr( RndmEngine* rndmEnginePtr)  
            offers the possibility to link to an external random number generator. The rules for constructing your own class from the RndmEngine base class are described ";?>here.
            argument rndmEnginePtr : pointer to a RndmEngine-derived object. This object must be instantiated by you in your program.
            Note: The method returns true if the pointer is different from 0.

            bool Pythia::setUserHooksPtr( UserHooks* userHooksPtr)  
            offers the possibility to interact with the generation process at a few different specified points, e.g. to reject undesirable events at an early stage to save computer time. The rules for constructing your own class from the UserHooks base class are described ";?>here. You can only hand in one such pointer, but this may be to a class that implements several of the different allowed possibilities.
            argument userHooksPtr : pointer to a userHooks-derived object. This object must be instantiated by you in your program.
            Note: The method currently always returns true.

            bool Pythia::setBeamShapePtr( BeamShape* beamShapePtr)  
            offers the possibility to provide your own shape of the momentum and space-time spread of the incoming beams. The rules for constructing your own class from the BeamShape base class are described ";?>here.
            argument BeamShapePtr : pointer to a BeamShape-derived object. This object must be instantiated by you in your program.
            Note: The method currently always returns true.

            bool Pythia::setSigmaPtr( SigmaProcess* sigmaPtr)  
            offers the possibility to link your own implementation of a process and its cross section, to make it a part of the normal process generation machinery, without having to recompile the Pythia library itself. The rules for constructing your own class from the SigmaProcess base class are described ";?>here. You may call this routine repeatedly, to add as many new processes as you wish.
            argument sigmaPtr : pointer to a SigmaProcess-derived object. This object must be instantiated by you in your program.
            Note: The method currently always returns true.

            bool Pythia::setResonancePtr( ResonanceWidths* resonancePtr)  
            offers the possibility to link your own implementation of the calculation of partial resonance widths, to make it a part of the normal process generation machinery, without having to recompile the Pythia library itself. This allows the decay of new resonances to be handled internally, when combined with new particle data. Note that the decay of normal hadrons cannot be modeled here; this is for New Physics resonances. The rules for constructing your own class from the ResonanceWidths base class are described ";?>here. You may call this routine repeatedly, to add as many new resonances as you wish.
            argument resonancePtr : pointer to a ResonanceWidths-derived object. This object must be instantiated by you in your program.
            Note: The method currently always returns true.

            bool Pythia::setShowerPtr( TimeShower* timesDecPtr, TimeShower* timesPtr = 0, SpaceShower* spacePtr = 0)  
            offers the possibility to link your own parton shower routines as replacements for the default ones. This is much more complicated since the showers are so central and are so interlinked with other parts of the program. Therefore it is also possible to do the replacement in stages, from the more independent to the more intertwined. The rules for constructing your own classes from the TimeShower and SpaceShowerbase classes are described ";?>here. These objects must be instantiated by you in your program.
            argument timesDecPtr : pointer to a TimeShower-derived object for doing timelike shower evolution in resonance decays, e.g. of a Z^0. This is decoupled from beam remnants and parton distributions, and is therefore the simplest kind of shower to write. If you provide a value 0 then the internal shower routine will be used.
            argument timesPtr (default = 0) : pointer to a TimeShower-derived object for doing all other timelike shower evolution, which is normally interleaved with multiparton interactions and spacelike showers, introducing both further physics and further technical issues. If you retain the default value 0 then the internal shower routine will be used. You are allowed to use the same pointer as above for the timesDecPtr if the same shower can fulfill both tasks.
            argument spacePtr (default = 0) : pointer to a SpaceShower-derived object for doing all spacelike shower evolution, which is normally interleaved with multiparton interactions and timelike showers. If you retain the default value 0 then the internal shower routine will be used.
            Note: The method currently always returns true.

            Initialize

            At the initialization stage all the information provided above is processed, and the stage is set up for the subsequent generation of events. Currently several alternative forms of the init method are available for this stage, but only the first one is recommended.

            bool Pythia::init()  
            initialize for collisions, in any of the five separate possibilities below. In this option the beams are not specified by input arguments, but instead by the settings in the ";?>Beam Parameters section. This allows the beams to be specified in the same file as other run instructions. The default settings give pp collisions at 14 TeV.
            Note: The method returns false if the initialization fails. It is then not possible to generate any events.

            bool Pythia::init( int idA, int idB, double eCM)  
            initialize for collisions in the center-of-mass frame, with the beams moving in the +-z directions.
            argument idA, idB : particle identity code for the two incoming beams.
            argument eCM : the CM energy of the collisions.
            Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

            bool Pythia::init( int idA, int idB, double eA, double eB)  
            initialize for collisions with back-to-back beams, moving in the +-z directions, but with different energies.
            argument idA, idB : particle identity code for the two incoming beams.
            argument eA, eB : the energies of the two beams. If an energy is set to be below the mass of the respective beam particle that particle is taken to be at rest. This offers a simple possibility to simulate fixed-target collisions.
            Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

            bool Pythia::init( int idA, int idB, double pxA, double pyA, double pzA, double pxB, double pyB, double pzB)  
            initialize for collisions with arbitrary beam directions.
            argument idA, idB : particle identity code for the two incoming beams.
            argument pxA, pyA, pzA : the three-momentum vector (p_x, p_y, p_z) of the first incoming beam.
            argument pxB, pyB, pzB : the three-momentum vector (p_x, p_y, p_z) of the second incoming beam.
            Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

            bool Pythia::init( string LesHouchesEventFile, bool skipInit = false)  
            initialize for hard-process collisions fed in from an external file with events, written according to the ";?>Les Houches Event File standard.
            argument LesHouchesEventFile : the file name (including path, where required) where the events are stored, including relevant information on beam identities and energies.
            argument skipInit (default = false) : By default this method does a complete reinitialization of the generation process. If you set this argument to true then no reinitialization will occur, only the pointer to the event file is updated. This may come in handy if the full event sample is split across several files generated under the same conditions (except random numbers, of course). You then do the first initialization with the default, and all subsequent ones with true. Note that things may go wrong if the files are not created under the same conditions.
            Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

            bool Pythia::init( LHAup* lhaUpPtr)  
            initialize for hard-process collisions fed in from an external source of events, consistent with the Les Houches Accord standard. The rules for constructing your own class from the LHAup base class are described ";?>here. This class is also required to provide the beam parameters.
            argument lhaUpPtr : pointer to a LHAup-derived object. This object must be instantiated by you in your program.
            Notes: Deprecated. The method returns false if the initialization fails. It is then not possible to generate any events.

            Generate events

            The next() method is the main one to generate events. In this section we also put a few other specialized methods that may be useful in some circumstances.

            bool Pythia::next()  
            generate the next event. No input parameters are required; all instructions have already been set up in the initialization stage.
            Note: The method returns false if the event generation fails. The event record is then not consistent and should not be studied. When reading in hard collisions from a Les Houches Event File the problem may be that the end of the file has been reached. This can be checked with the ";?>Info::atEndOfFile() method.

            int Pythia::forceTimeShower( int iBeg, int iEnd, double pTmax, int nBranchMax = 0)  
            perform a final-state shower evolution on partons in the event event record. This could be used for externally provided simple events, or even parts of events, for which a complete generation is not foreseen. Since the mother source of the parton system is not known, one cannot expect as good accuracy as in a normal generation. When two different timelike shower instances are set up, it is the one used for showering in resonance decays that is used here. The forceTimeShower method can be used in conjunction with the forceHadronLevel one below. Further comments are found ";?>here.
            argument iBeg, iEnd : the first and last entry of the event record to be affected by the call.
            argument pTmax : the maximum pT scale of emissions. Additionally, as always, the scale variable of each parton sets the maximum pT scale of branchings of this parton. Recall that this scale defaults to 0 if not set, so that no radiation can occur.
            argument nBranchMax (default = 0) : when positive, it sets the maximum number of branchings that are allowed to occur in the shower, i.e. the shower may stop evolving before reaching the lower cutoff. The argument has no effect when zero or negative, i.e. then the shower will continue to the lower cutoff.
            Note: The method returns the number of branchings that has been generated.

            bool Pythia::forceHadronLevel(bool findJunctions = true)  
            hadronize the existing event record, i.e. perform string fragmentation and particle decays. There are two main applications. Firstly, you can use the same parton-level content as a basis for repeated hadronization attempts, in schemes intended to save computer time. Secondly, you may have an external program that can simulate the full partonic level of the event - hard process, parton showers, multiparton interactions, beam remnants, colour flow, and so on - but not hadronization. Further details are found ";?>here.
            argument findJunctions (default = true) : normally this routine will search through the event record and try to figure out if any colour junctions are present. If so, the colour topology of such junctions must be sorted out. In tricky cases this might fail, and then hadronization will not work. A user who is aware of this and knows the intended colour flow can set up the junction information (if any) in the event record, and then call forceHadronLevel(false) so as not to have this information overwritten. (If the event record contains no unhadronized partons then no junction search will be performed in any case.)
            Note: The method returns false if the hadronization fails. The event record is then not consistent and should not be studied.

            bool Pythia::moreDecays()  
            perform decays of all particles in the event record that have not been decayed but should have been done so. This can be used e.g. for repeated decay attempts, in schemes intended to save computer time. Further details are found ";?>here.
            Note: The method returns false if the decays fail. The event record is then not consistent and should not be studied.

            bool Pythia::forceRHadronDecays()  
            perform decays of R-hadrons that were previously considered stable. This could be if an R-hadron is sufficiently long-lived that it may interact in the detector between production and decay, so that its four-momentum is changed. Further details are found ";?>here.
            Note: The method returns false if the decays fail. The event record is then not consistent and should not be studied.

            void Pythia::LHAeventList(ostream& os = cout)  
            list the Les Houches Accord information on the current event, see ";?>LHAup::listEvent(...). (Other listings are available via the class members below, so this listing is a special case that would not fit elsewhere.)
            argument os (default = cout) : output stream where the listing occurs.

            bool Pythia::LHAeventSkip(int nSkip)  
            skip ahead a number of events in the Les Houches generation sequence, without doing anything further with them, see ";?>LHAup::skipEvent(nSkip). Mainly intended for debug purposes, e.g. when an event at a known location in a Les Houches Event File is causing problems.
            argument nSkip : number of events to skip.
            Note: The method returns false if the operation fails, specifically if the end of a LHEF has been reached, cf. next() above.

            Finalize

            There is no required finalization step; you can stop generating events when and how you want. It is still recommended that you make it a routine to call the following method at the end. A second method provides a deprecated alternative.

            void Pythia::stat()  
            list statistics on the event generation, specifically total and partial cross sections and the number of different errors. For more details see ";?>here and for available options ";?>here.

            void Pythia::statistics(bool all = false, bool reset = false)  
            list statistics on the event generation, specifically total and partial cross sections and the number of different errors. For more details see ";?>here.
            argument all (default = false) : if true also statistics on multiparton interactions is shown, by default not.
            argument reset (default = false) : if true then all counters, e.g on events generated and errors experienced, are reset to zero whenever the routine is called. The default instead is that all stored statistics information is unaffected by the call. Counters are automatically reset in each new Pythia::init(...) call, however, so the only time the reset option makes a difference is if statistics(...) is called several times in a (sub)run.
            Note: Deprecated.

            Interrogate settings

            Normally settings are used in the setup and initialization stages to determine the character of a run, e.g. read from a file with the above-described Pythia::readFile(...) method. There is no strict need for a user to interact with the Settings database in any other way. However, as an option, some settings variables have been left free for the user to set in such a file, and then use in the main program to directly affect the performance of that program, see ";?>here. A typical example would be the number of events to generate. For such applications the following shortcuts to some Settings methods may be convenient.

            bool Pythia::flag(string key)  
            read in a boolean variable from the Settings database.
            argument key : the name of the variable to be read.

            int Pythia::mode(string key)  
            read in an integer variable from the Settings database.
            argument key : the name of the variable to be read.

            double Pythia::parm(string key)  
            read in a double-precision variable from the Settings database.
            argument key : the name of the variable to be read.

            string Pythia::word(string key)  
            read in a string variable from the Settings database.
            argument key : the name of the variable to be read.

            Get a PDF set

            Pythia contains an number of parton density sets internally, plus an interface to LHAPDF. With the method below, this machinery is also made available for external usage.

            PDF* getPDFPtr(int id, int sequence = 1)  
            get a pointer to a PDF object. Which PDF is returned depends on the ";?>PDF Selection settings.
            argument id : the identity code of the incoming particle.
            argument sequence : should normally be 1, but 2 can be used for protons to let the PDF selection be determined by the special settings for hard processes (PDF:useHard etc.).

            Data members

            The Pythia class contains a few public data members, several of which play a central role. We list them here, with links to the places where they are further described.

            Event Pythia::process  
            the hard-process event record, see ";?>here for further details.

            Event Pythia::event  
            the complete event record, see ";?>here for further details.

            Info Pythia::info  
            further information on the event-generation process, see ";?>here for further details.

            Settings Pythia::settings  
            the settings database, see ";?>here for further details.

            ParticleData Pythia::particleData  
            the particle properties and decay tables database, see ";?>here for further details.

            Rndm Pythia::rndm  
            the random number generator, see ";?>here and ";?>here for further details.

            CoupSM Pythia::coupSM  
            Standard Model couplings and mixing matrices, see ";?>here for further details.

            SusyLesHouches Pythia::slha  
            parameters and particle data in the context of supersymmetric models, see ";?>here for further details.

            PartonSystems Pythia::partonSystems  
            a grouping of the partons in the event record by subsystem, see ";?>here for further details. pythia8-8.1.80.orig/phpdoc/OniaProcesses.php0000644000175000017500000006011212217615312017074 0ustar sunsun Onia Processes SETTINGS SAVED TO FILE

            "; } else { echo "NO FILE SELECTED YET.. PLEASE DO SO HERE

            "; } } ?>

            Onia Processes

            Production of J/psi or Upsilon, directly and via chi states and the colour-octet mechanism. In each process the square-bracketed expression specifies the state in spectroscopic notation, (2S+1) L J, followed by (1) for colour-singlet states and (8) for colour-octet ditto.

            The original Fortran code for these processes has been contributed by Stefan Wolf [unpublished]. For the C++ version only the unpolarized expressions are retained, since the theoretical predictions of the colour-octet model anyway do not agree with the experimental observations. Furthermore, the polarization effects are modest, so isotropic decay is not a bad starting point. Such an event sample can afterwards be reweighted at will by the user, to test various assumptions.

            The description of ";?>final-state radiation is in this case based on some further model assumptions.

            Most of the processes below are divergent in the limit pT -> 0, and therefore a pTmin scale should be set. Comparisons with data indicate that this divergence can be tamed the same way as for the normal QCD 2 -> 2 cross sections [Bar06,Kra08], which makes sense, since they are all dominated by the same kind of t-channel gluon exchange. It is therefore possible to use the ";?>SuppressSmallPT user hook to impose a reweighting that cancels the low-pT divergence.

            An eikonalized description of these processes is included in the multiparton-interactions framework. Here the low-pT dampening is automatic, and additionally the framework is more consistent (e.g. with respect to energy-momentum constraints and the impact-parameter description) for events where the onium production is not the hardest subprocess, as would often be the case in the low-pT limit.

            Charmonium



            Charmonium:all On Off   (default = off)
            Common switch for the group of charmonium production.

            Charmonium:gg2QQbar[3S1(1)]g On Off   (default = off)
            g g -> ccbar[3S1(1)] g. Code 401.

            Charmonium:gg2QQbar[3P0(1)]g On Off   (default = off)
            g g -> ccbar[3P0(1)] g. Code 402.

            Charmonium:gg2QQbar[3P1(1)]g On Off   (default = off)
            g g -> ccbar[3P1(1)] g. Code 403.

            Charmonium:gg2QQbar[3P2(1)]g On Off   (default = off)
            g g -> ccbar[3P2(1)] g. Code 404.

            Charmonium:qg2QQbar[3P0(1)]q On Off   (default = off)
            q g -> ccbar[3P0(1)] q. Code 405.

            Charmonium:qg2QQbar[3P1(1)]q On Off   (default = off)
            q g -> ccbar[3P1(1)] q. Code 406.

            Charmonium:qg2QQbar[3P2(1)]q On Off   (default = off)
            q g -> ccbar[3P2(1)] q. Code 407.

            Charmonium:qqbar2QQbar[3P0(1)]g On Off   (default = off)
            q qbar -> ccbar[3P0(1)] g. Code 408.

            Charmonium:qqbar2QQbar[3P1(1)]g On Off   (default = off)
            q qbar -> ccbar[3P1(1)] g. Code 409.

            Charmonium:qqbar2QQbar[3P2(1)]g On Off   (default = off)
            q qbar -> ccbar[3P2(1)] g. Code 410.

            Charmonium:gg2QQbar[3S1(8)]g On Off   (default = off)
            g g -> ccbar[3S1(8)] g. Code 411.

            Charmonium:gg2QQbar[1S0(8)]g On Off   (default = off)
            g g -> ccbar[3S1(8)] g. Code 412.

            Charmonium:gg2QQbar[3PJ(8)]g On Off   (default = off)
            g g -> ccbar[3S1(8)] g. Code 413.

            Charmonium:qg2QQbar[3S1(8)]q On Off   (default = off)
            q g -> ccbar[3S1(8)] q. Code 414.

            Charmonium:qg2QQbar[1S0(8)]q On Off   (default = off)
            q g -> ccbar[3S1(8)] q. Code 415.

            Charmonium:qg2QQbar[3PJ(8)]q On Off   (default = off)
            q g -> ccbar[3S1(8)] q. Code 416.

            Charmonium:qqbar2QQbar[3S1(8)]g On Off   (default = off)
            q qbar -> ccbar[3S1(8)] g. Code 417.

            Charmonium:qqbar2QQbar[1S0(8)]g On Off   (default = off)
            q qbar -> ccbar[3S1(8)] g. Code 418.

            Charmonium:qqbar2QQbar[3PJ(8)]g On Off   (default = off)
            q qbar -> ccbar[3S1(8)] g. Code 419.

            Bottomonium



            Bottomonium:all On Off   (default = off)
            Common switch for the group of charmonium production.

            Bottomonium:gg2QQbar[3S1(1)]g On Off   (default = off)
            g g -> bbbar[3S1(1)] g. Code 501.

            Bottomonium:gg2QQbar[3P0(1)]g On Off   (default = off)
            g g -> bbbar[3P0(1)] g. Code 502.

            Bottomonium:gg2QQbar[3P1(1)]g On Off   (default = off)
            g g -> bbbar[3P1(1)] g. Code 503.

            Bottomonium:gg2QQbar[3P2(1)]g On Off   (default = off)
            g g -> bbbar[3P2(1)] g. Code 504.

            Bottomonium:qg2QQbar[3P0(1)]q On Off   (default = off)
            q g -> bbbar[3P0(1)] q. Code 505.

            Bottomonium:qg2QQbar[3P1(1)]q On Off   (default = off)
            q g -> bbbar[3P1(1)] q. Code 506.

            Bottomonium:qg2QQbar[3P2(1)]q On Off   (default = off)
            q g -> bbbar[3P2(1)] q. Code 507.

            Bottomonium:qqbar2QQbar[3P0(1)]g On Off   (default = off)
            q qbar -> bbbar[3P0(1)] g. Code 508.

            Bottomonium:qqbar2QQbar[3P1(1)]g On Off   (default = off)
            q qbar -> bbbar[3P1(1)] g. Code 509.

            Bottomonium:qqbar2QQbar[3P2(1)]g On Off   (default = off)
            q qbar -> bbbar[3P2(1)] g. Code 510.

            Bottomonium:gg2QQbar[3S1(8)]g On Off   (default = off)
            g g -> bbbar[3S1(8)] g. Code 511.

            Bottomonium:gg2QQbar[1S0(8)]g On Off   (default = off)
            g g -> bbbar[3S1(8)] g. Code 512.

            Bottomonium:gg2QQbar[3PJ(8)]g On Off   (default = off)
            g g -> bbbar[3S1(8)] g. Code 513.

            Bottomonium:qg2QQbar[3S1(8)]q On Off   (default = off)
            q g -> bbbar[3S1(8)] q. Code 514.

            Bottomonium:qg2QQbar[1S0(8)]q On Off   (default = off)
            q g -> bbbar[3S1(8)] q. Code 515.

            Bottomonium:qg2QQbar[3PJ(8)]q On Off   (default = off)
            q g -> bbbar[3S1(8)] q. Code 516.

            Bottomonium:qqbar2QQbar[3S1(8)]g On Off   (default = off)
            q qbar -> bbbar[3S1(8)] g. Code 517.

            Bottomonium:qqbar2QQbar[1S0(8)]g On Off   (default = off)
            q qbar -> bbbar[3S1(8)] g. Code 518.

            Bottomonium:qqbar2QQbar[3PJ(8)]g On Off   (default = off)
            q qbar -> bbbar[3S1(8)] g. Code 519.

            Onium matrix elements

            The implementation of charmonium and bottomonium production, including the colour-octet production mechanism, requires information on NRQCD matrix elements for the various wavefunctions involved. Default values for these are encoded in the following ten variables. They are taken from [Nas00]; see also [Bar06].

            Charmonium:OJpsi3S11   (default = 1.16; minimum = 0.0)
            <O(J/psi)[3S1(1)]>.

            Charmonium:OJpsi3S18   (default = 0.0119; minimum = 0.0)
            <O(J/psi)[3S1(8)]>.

            Charmonium:OJpsi1S08   (default = 0.01; minimum = 0.0)
            <O(J/psi)[1S0(8)]>.

            Charmonium:OJpsi3P08   (default = 0.01; minimum = 0.0)
            <O(J/psi)[3P0(8)]>/m_c^2.

            Charmonium:Ochic03P01   (default = 0.05; minimum = 0.0)
            <O(chi_c0)[3P0(8)]>/m_c^2.

            Bottomonium:OUpsilon3S11   (default = 9.28; minimum = 0.0)
            <O(Upsilon)[3S1(1)]>.

            Bottomonium:OUpsilon3S18   (default = 0.15; minimum = 0.0)
            <O(Upsilon)[3S1(8)]>.

            Bottomonium:OUpsilon1S08   (default = 0.02; minimum = 0.0)
            <O(Upsilon)[1S0(8)]>.

            Bottomonium:OUpsilon3P08   (default = 0.02; minimum = 0.0)
            <O(Upsilon)[3P0(8)]>/m_b^2.

            Bottomonium:Ochib03P01   (default = 0.085; minimum = 0.0)
            <O(chi_b0)[3P0(8)]>/m_b^2. "?>
            pythia8-8.1.80.orig/pythia8tohepmc/0000755000175000017500000000000012217346243015303 5ustar sunsunpythia8-8.1.80.orig/pythia8tohepmc/Pythia8ToHepMC.cc0000644000175000017500000001765212217346243020333 0ustar sunsun// Pythia8ToHepMC.cc is a part of the PYTHIA event generator. // Copyright (C) 2013 Torbjorn Sjostrand. // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. // Please respect the MCnet Guidelines, see GUIDELINES for details. // Author: Mikhail Kirsanov, Mikhail.Kirsanov@cern.ch // Function definitions (not found in the header) for the Pythia8ToHepMC class, // which converts a PYTHIA event record to the standard HepMC format. #include "Pythia8/Pythia8ToHepMC.h" #include "HepMC/GenEvent.h" namespace HepMC { //========================================================================== // Main method for conversion from PYTHIA event to HepMC event. // Read one event from Pythia8 and fill GenEvent, // and return T/F = success/failure. bool Pythia8ToHepMC::fill_next_event( Pythia8::Event& pyev, GenEvent* evt, int ievnum, Pythia8::Info* pyinfo, Pythia8::Settings* pyset) { // 1. Error if no event passed. if (!evt) { std::cerr << "Pythia8ToHepMC::fill_next_event error - passed null event." << std::endl; return 0; } // Event number counter. if ( ievnum >= 0 ) { evt->set_event_number(ievnum); m_internal_event_number = ievnum; } else { evt->set_event_number(m_internal_event_number); ++m_internal_event_number; } // Conversion factors from Pythia units GeV and mm to HepMC ones. double momFac = HepMC::Units::conversion_factor(HepMC::Units::GEV, evt->momentum_unit()); double lenFac = HepMC::Units::conversion_factor(HepMC::Units::MM, evt->length_unit()); // 2. Create a particle instance for each entry and fill a map, and // a vector which maps from the particle index to the GenParticle address. std::vector hepevt_particles( pyev.size() ); for (int i = 1; i < pyev.size(); ++i) { // Fill the particle. hepevt_particles[i] = new GenParticle( FourVector( momFac * pyev[i].px(), momFac * pyev[i].py(), momFac * pyev[i].pz(), momFac * pyev[i].e() ), pyev[i].id(), pyev.statusHepMC(i) ); hepevt_particles[i]->suggest_barcode(i); hepevt_particles[i]->set_generated_mass( momFac * pyev[i].m() ); // Colour flow uses index 1 and 2. int colType = pyev[i].colType(); if (colType == 1 || colType == 2) hepevt_particles[i]->set_flow(1, pyev[i].col()); if (colType == -1 || colType == 2) hepevt_particles[i]->set_flow(2, pyev[i].acol()); } // Here we assume that the first two particles in the list // are the incoming beam particles. evt->set_beam_particles( hepevt_particles[1], hepevt_particles[2] ); // 3. Loop over particles AGAIN, this time creating vertices. // We build the production vertex for each entry in hepevt. // The HEPEVT pointers are bi-directional, so gives decay vertices as well. for (int i = 1; i < pyev.size(); ++i) { GenParticle *p = hepevt_particles[i]; // 3a. Search to see if a production vertex already exists. std::vector mothers = pyev.motherList(i); unsigned int imother = 0; int mother = -1; // note that in Pythia8 there is a particle number 0! if ( !mothers.empty() ) mother = mothers[imother]; GenVertex* prod_vtx = p->production_vertex(); while ( !prod_vtx && mother > 0 ) { prod_vtx = hepevt_particles[mother]->end_vertex(); if ( prod_vtx ) prod_vtx->add_particle_out( p ); mother = ( ++imother < mothers.size() ) ? mothers[imother] : -1; } // 3b. If no suitable production vertex exists - and the particle has // at least one mother or position information to store - make one. FourVector prod_pos( lenFac * pyev[i].xProd(), lenFac * pyev[i].yProd(), lenFac * pyev[i].zProd(), lenFac * pyev[i].tProd() ); if ( !prod_vtx && ( mothers.size() > 0 || prod_pos != FourVector() ) ) { prod_vtx = new GenVertex(); prod_vtx->add_particle_out( p ); evt->add_vertex( prod_vtx ); } // 3c. If prod_vtx doesn't already have position specified, fill it. if ( prod_vtx && prod_vtx->position() == FourVector() ) prod_vtx->set_position( prod_pos ); // 3d. loop over mothers to make sure their end_vertices are consistent. imother = 0; mother = -1; if ( !mothers.empty() ) mother = mothers[imother]; while ( prod_vtx && mother > 0 ) { // If end vertex of the mother isn't specified, do it now. if ( !hepevt_particles[mother]->end_vertex() ) { prod_vtx->add_particle_in( hepevt_particles[mother] ); // Problem scenario: the mother already has a decay vertex which // differs from the daughter's production vertex. This means there is // internal inconsistency in the HEPEVT event record. Print an error. // Note: we could provide a fix by joining the two vertices with a // dummy particle if the problem arises often. } else if (hepevt_particles[mother]->end_vertex() != prod_vtx ) { if ( m_print_inconsistency ) std::cerr << "HepMC::Pythia8ToHepMC: inconsistent mother/daugher " << "information in Pythia8 event " << std::endl << "i = " << i << " mother = " << mother << "\n This warning can be turned off with the " << "Pythia8ToHepMC::print_inconsistency switch." << std::endl; } // End of vertex-setting loops. mother = ( ++imother < mothers.size() ) ? mothers[imother] : -1; } } // If hadronization switched on then no final coloured particles. bool doHadr = (pyset == 0) ? m_free_parton_warnings : pyset->flag("HadronLevel:all") && pyset->flag("HadronLevel:Hadronize"); // 4. Check for particles which come from nowhere, i.e. are without // mothers or daughters. These need to be attached to a vertex, or else // they will never become part of the event. for (int i = 1; i < pyev.size(); ++i) { if ( !hepevt_particles[i]->end_vertex() && !hepevt_particles[i]->production_vertex() ) { std::cerr << "hanging particle " << i << std::endl; GenVertex* prod_vtx = new GenVertex(); prod_vtx->add_particle_out( hepevt_particles[i] ); evt->add_vertex( prod_vtx ); } // Also check for free partons (= gluons and quarks; not diquarks?). if ( doHadr && m_free_parton_warnings ) { if ( hepevt_particles[i]->pdg_id() == 21 && !hepevt_particles[i]->end_vertex() ) { std::cerr << "gluon without end vertex " << i << std::endl; if ( m_crash_on_problem ) exit(1); } if ( abs(hepevt_particles[i]->pdg_id()) <= 6 && !hepevt_particles[i]->end_vertex() ) { std::cerr << "quark without end vertex " << i << std::endl; if ( m_crash_on_problem ) exit(1); } } } // 5. Store PDF, weight, cross section and other event information. // Flavours of incoming partons. if (m_store_pdf && pyinfo != 0) { int id1pdf = pyinfo->id1pdf(); int id2pdf = pyinfo->id2pdf(); if ( m_convert_gluon_to_0 ) { if (id1pdf == 21) id1pdf = 0; if (id2pdf == 21) id2pdf = 0; } // Store PDF information. evt->set_pdf_info( PdfInfo( id1pdf, id2pdf, pyinfo->x1pdf(), pyinfo->x2pdf(), pyinfo->QFac(), pyinfo->pdf1(), pyinfo->pdf2() ) ); } // Store process code, scale, alpha_em, alpha_s. if (m_store_proc && pyinfo != 0) { evt->set_signal_process_id( pyinfo->code() ); evt->set_event_scale( pyinfo->QRen() ); if (evt->alphaQED() <= 0) evt->set_alphaQED( pyinfo->alphaEM() ); if (evt->alphaQCD() <= 0) evt->set_alphaQCD( pyinfo->alphaS() ); } // Store cross-section information in pb and event weight. The latter is // usually dimensionless, but in units of pb for Les Houches strategies +-4. if (m_store_xsec && pyinfo != 0) { HepMC::GenCrossSection xsec; xsec.set_cross_section( pyinfo->sigmaGen() * 1e9, pyinfo->sigmaErr() * 1e9); evt->set_cross_section(xsec); evt->weights().push_back( pyinfo->weight() ); } // Done. return true; } //========================================================================== } // end namespace HepMC pythia8-8.1.80.orig/README.Win320000644000175000017500000000252612217346244014124 0ustar sunsun==================================== INSTRUCTIONS FOR WINDOWS USERS ==================================== I) How to build II) How to clean III) Further notes Note: this is a first version, and does not (yet) have the full functionality offered for the Linux case. I) How to build =============== To build Pythia8 on windows, open a command prompt, cd to the location where Pythia has been extracted, then type nmake with any of these options : to build in debug mode : nmake -f Makefile.msc CFG="Win32 Debug" in optimized mode : nmake -f Makefile.msc CFG="Win32 Release" libPythia8.lib will be located in $PYTHIADIR\lib directory II) How to clean ================ To clean intermediate (obj) files : nmake -f Makefile.msc clean CFG="Win32 Debug" or nmake -f Makefile.msc clean CFG="Win32 Release" To clean all binaries (obj, idb, pdb, ilk, lib and exe) : nmake -f Makefile.msc distclean CFG="Win32 Debug" or nmake -f Makefile.msc distclean CFG="Win32 Release" III) Further notes ================== Some C++ distributions do not implement the error function erf(x). Should you encounter such a compilation problem, the PhaseSpace.h and SigmaTotal.h files do contain commented-out erf(x) code, that then should be uncommented. The approximation used is not of high precision, but fully sufficient for the task at hand.